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801.1773
Hans Christian Krahl
H. C. Krahl, J. A. M\"uller, C. Wetterich
Generation of d-wave coupling in the two-dimensional Hubbard model from functional renormalization
11 pages, 13 figures, equivalent to published version
Phys. Rev. B 79, 094526 (2009)
10.1103/PhysRevB.79.094526
null
cond-mat.str-el hep-th
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Within the two-dimensional repulsive t-t'-Hubbard model, an attractive coupling in the d-wave pairing channel is induced by antiferromagnetic fluctuations. We investigate this coupling using functional renormalization group equations. The momentum dependent d-wave coupling can be bosonized by the use of scale dependent field transformations. We propose an effective coarse grained model for the Hubbard model which is based on the exchange of antiferromagnetic and d-wave collective bosons.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 12:55:01 GMT" }, { "version": "v2", "created": "Mon, 13 Apr 2009 13:14:33 GMT" } ]
2009-11-13T00:00:00
[ [ "Krahl", "H. C.", "" ], [ "Müller", "J. A.", "" ], [ "Wetterich", "C.", "" ] ]
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801.1774
Dirk Lorenz
Dirk A. Lorenz
Convergence rates and source conditions for Tikhonov regularization with sparsity constraints
null
Journal of Inverse and Ill-Posed Problems, 16(5):463-478, 2008
10.1515/JIIP.2008.025
null
math.FA
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
This paper addresses the regularization by sparsity constraints by means of weighted $\ell^p$ penalties for $0\leq p\leq 2$. For $1\leq p\leq 2$ special attention is payed to convergence rates in norm and to source conditions. As main result it is proven that one gets a convergence rate in norm of $\sqrt{\delta}$ for $1\leq p\leq 2$ as soon as the unknown solution is sparse. The case $p=1$ needs a special technique where not only Bregman distances but also a so-called Bregman-Taylor distance has to be employed. For $p<1$ only preliminary results are shown. These results indicate that, different from $p\geq 1$, the regularizing properties depend on the interplay of the operator and the basis of sparsity. A counterexample for $p=0$ shows that regularization need not to happen.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:01:22 GMT" }, { "version": "v2", "created": "Fri, 18 Jul 2008 11:07:38 GMT" } ]
2011-03-16T00:00:00
[ [ "Lorenz", "Dirk A.", "" ] ]
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801.1775
X.R. Wang
X. R. Wang
Giant dynamical Zeeman split in inverse spin valves
null
null
null
null
cond-mat.mes-hall cond-mat.mtrl-sci
null
The inversion of a spin valve device is proposed. Opposite to a conventional spin valve of a non-magnetic spacer sandwiched between two ferromagnetic metals, an inverse spin valve is a ferromagnet sandwiched between two non-magnetic metals. It is predicted that, under a bias, the chemical potentials of spin-up and spin-down electrons in the metals split at metal-ferromagnet interfaces, a dynamical Zeeman effect. This split is of the order of an applied bias. Thus, there should be no problem of generating an $eV$ split that is not possible to be realized on the earth by the usual Zeeman effect.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:05:30 GMT" } ]
2008-01-14T00:00:00
[ [ "Wang", "X. R.", "" ] ]
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801.1776
Peter Morgan
Peter Morgan
Violation of Bell inequalities through the coincidence-time loophole
4 pages
null
null
null
quant-ph
null
The coincidence-time loophole was identified by Larsson & Gill (Europhys. Lett. 67, 707 (2004)); a concrete model that exploits this loophole has recently been described by De Raedt et al. (Found. Phys., to appear). It is emphasized here that De Raedt et al.'s model is experimentally testable. De Raedt et al.'s model also introduces contextuality in a novel and classically more natural way than the use of contextual particle properties, by introducing a probabilistic model of a limited set of degrees of freedom of the measurement apparatus, so that it can also be seen as a random field model. Even though De Raedt et al.'s model may well contradict detailed Physics, it nonetheless provides a way to simulate the logical operation of elements of a quantum computer, and may provide a way forward for more detailed random field models.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:11:03 GMT" } ]
2008-01-14T00:00:00
[ [ "Morgan", "Peter", "" ] ]
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801.1777
Vincent Tatischeff
V. Tatischeff, J.-P. Thibaud and I. Ribas
Nucleosynthesis in stellar flares
12 pages, 3 figures, contribution to the Proceedings of the XIXemes Rencontres de Blois, Matter and energy in the Universe, Blois, France, May 2007
null
null
null
astro-ph
null
Nuclear interactions of ions accelerated at the surface of flaring stars can produce fresh isotopes in stellar atmospheres. Although this nucleosynthesis is not significant for the chemical evolution of the Galaxy, it can be important for a number of measurements of "anomalously" high 6-Li and 7-Li abundances. We discuss the possible role of stellar flares to explain the recent report of high 6-Li abundances in metal-poor halo stars and the well-established correlation between Li abundance and stellar activity in young open clusters. We then study the possibility of observing directly Li production during flares of nearby and active dwarfs of spectral type M.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:28:46 GMT" } ]
2008-01-14T00:00:00
[ [ "Tatischeff", "V.", "" ], [ "Thibaud", "J. -P.", "" ], [ "Ribas", "I.", "" ] ]
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801.1778
Henrik Beuther
H. Beuther, A.J. Walsh, S. Thorwirth, Q. Zhang, T.R. Hunter, S.T. Megeath, K.M. Menten
ATCA 3mm observations of NGC6334I and I(N): dense cores, outflows and an UCHII region
14 pages, 14 figures, accepted for A&A
null
10.1051/0004-6361:20079014
null
astro-ph
null
Aims: Investigation of the dense gas, the outflows and the continuum emission from the massive twin cores NGC6334I and I(N) at high spatial resolution. Methods: We imaged the region with the Australia Telescope Compact Array (ATCA) at 3.4mm wavelength in continuum as well as CH3CN(5_K-4_K) and HCN(1-0) spectral line emission. Results: While the continuum emission in NGC6334I mainly traces the UCHII region, toward NGC6334I(N) we detect line emission from four of the previously identified dust continuum condensations that are of protostellar or pre-stellar nature. The CH3CN(5_K-4_K) lines are detected in all K-components up to energies of 128K above ground toward two protostellar condensations in both regions. We find line-width increasing with increasing K for all sources, which indicates a higher degree of internal motions closer to the central protostars. Toward the main mm and CH3CN source in NGC6334I we identify a velocity gradient approximately perpendicular to the large-scale molecular outflow. This may be interpreted as a signature of an accretion disk, although other scenarios, e.g., an unresolved double source, could produce a similar signature as well. No comparable signature is found toward any of the other sources. HCN does not trace the dense gas well but it is dominated by the molecular outflows. While the outflow in NGC6334I exhibits a normal Hubble-law like velocity structure, the data indicate a precessing outflow close to the plane of the sky for NGC6334I(N). Furthermore, we observe a wide (~15.4km/s) HCN absorption line, much broader than the previously observed CH3OH and NH3 absorption lines. Several explanations for the difference are discussed.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:25:25 GMT" } ]
2009-11-13T00:00:00
[ [ "Beuther", "H.", "" ], [ "Walsh", "A. J.", "" ], [ "Thorwirth", "S.", "" ], [ "Zhang", "Q.", "" ], [ "Hunter", "T. R.", "" ], [ "Megeath", "S. T.", "" ], [ "Menten", "K. M.", "" ] ]
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801.1779
Jiang Xiao
Jiang Xiao, Gerrit E. W. Bauer, Arne Brataas
Charge pumping in magnetic tunnel junctions: Scattering theory
4 pages, 3 figures. to be published on Physical Review B Rapid Communication
Physical Review B 77, 180407(R) (2008)
10.1103/PhysRevB.77.180407
null
cond-mat.mtrl-sci
null
We study theoretically the charge transport pumped by magnetization dynamics through epitaxial FIF and FNIF magnetic tunnel junctions (F: Ferromagnet, I: Insulator, N: Normal metal). We predict a small but measurable DC pumping voltage under ferromagnetic resonance conditions for collinear magnetization configurations, which may change sign as function of barrier parameters. A much larger AC pumping voltage is expected when the magnetizations are at right angles. Quantum size effects are predicted for an FNIF structure as a function of the normal layer thickness.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:26:01 GMT" }, { "version": "v2", "created": "Sat, 12 Jan 2008 15:55:57 GMT" }, { "version": "v3", "created": "Wed, 21 May 2008 09:53:16 GMT" } ]
2009-11-13T00:00:00
[ [ "Xiao", "Jiang", "" ], [ "Bauer", "Gerrit E. W.", "" ], [ "Brataas", "Arne", "" ] ]
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801.178
J\'er\^ome Bolte
Hedy Attouch, Jerome Bolte, Patrick Redont, Antoine Soubeyran
Proximal alternating minimization and projection methods for nonconvex problems. An approach based on the Kurdyka-Lojasiewicz inequality
null
null
null
null
math.OC
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We study the convergence properties of an alternating proximal minimization algorithm for nonconvex structured functions of the type: $L(x,y)=f(x)+Q(x,y)+g(y)$, where $f:\R^n\rightarrow\R\cup{+\infty}$ and $g:\R^m\rightarrow\R\cup{+\infty}$ are proper lower semicontinuous functions, and $Q:\R^n\times\R^m\rightarrow \R$ is a smooth $C^1$ function which couples the variables $x$ and $y$. The algorithm can be viewed as a proximal regularization of the usual Gauss-Seidel method to minimize $L$. We work in a nonconvex setting, just assuming that the function $L$ satisfies the Kurdyka-\L ojasiewicz inequality. An entire section illustrates the relevancy of such an assumption by giving examples ranging from semialgebraic geometry to "metrically regular" problems. Our main result can be stated as follows: If L has the Kurdyka-\L ojasiewicz property, then each bounded sequence generated by the algorithm converges to a critical point of $L$. This result is completed by the study of the convergence rate of the algorithm, which depends on the geometrical properties of the function $L$ around its critical points. When specialized to $Q(x,y)=|x-y|^2$ and to $f$, $g$ indicator functions, the algorithm is an alternating projection mehod (a variant of Von Neumann's) that converges for a wide class of sets including semialgebraic and tame sets, transverse smooth manifolds or sets with "regular" intersection. In order to illustrate our results with concrete problems, we provide a convergent proximal reweighted $\ell^1$ algorithm for compressive sensing and an application to rank reduction problems.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:54:05 GMT" }, { "version": "v2", "created": "Thu, 17 Jan 2008 09:34:35 GMT" }, { "version": "v3", "created": "Tue, 22 Jan 2013 20:19:54 GMT" } ]
2013-01-23T00:00:00
[ [ "Attouch", "Hedy", "" ], [ "Bolte", "Jerome", "" ], [ "Redont", "Patrick", "" ], [ "Soubeyran", "Antoine", "" ] ]
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801.1781
Erhu Zhang
Shengli Zhang, Qi Wang, Erhu Zhang
The Geometrical Effects on Electronic Spectrum and Persistent Currents in Mesoscopic Polygon
10 pages, 6 figures
Modern Physics Letters B, Vol. 23, No. 2 (2009) 191-201
10.1142/S0217984909017959
null
cond-mat.mes-hall
null
In this paper, a new mesoscopic polygon which possesses smooth transition at its corners is proposed. Because of the particularity of structure, this kind of mesoscopic polygon can also be a geometrical supperlattice. The geometrical effects on the electron states and persistent current are investigated comprehensively in the presence of magnetic flux. We find that the particular geometric structure of the polygon induces an effective periodic potential which results in gaps in the energy spectrum. The changes of gaps show the consistency with the geometrical twoness of this new polygon. This electronic structure and the corresponding physical properties are found to be periodic with period $\phi_{0}$ in the magnetic flux $\phi $ and can be controlled by the geometric method. We also consider the Rahsba spin-orbit interaction which make the energy levels splitting newly to double and leads to an additional small zigzag in one period of the persistent current. These new phenomena may be useful for the applications in quantum device design in the future.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 13:44:25 GMT" }, { "version": "v2", "created": "Wed, 9 Apr 2008 05:06:04 GMT" } ]
2009-03-03T00:00:00
[ [ "Zhang", "Shengli", "" ], [ "Wang", "Qi", "" ], [ "Zhang", "Erhu", "" ] ]
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801.1782
Xavier Artru
X. Artru (IPNL), J.-M. Richard (LPSC), J. Soffer
Positivity domains for pairs of triples of spin observables
Talk given by Xavier Artru at "DSPIN-07", XII Workshop on High-Energy Spin Physics, Dubna, Sept. 3-7, 2007, to appear in the Proceedings
Dans High-Energy Spin Physics - Proceeding of the XII Workshop on High-Energy Spin Physics, Dubna (2007)
null
null
nucl-th hep-ph
null
Positivity restrains the allowed domains for pairs or triples of spin observables in polarised reactions. Various domain shapes in ${1\over2}+{1\over2}\to{1\over2}+{1\over2}$ reactions are displayed. Some methods to determine these domains are mentioned and a new one based on the anticommutation between two observables is presented.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:03:50 GMT" } ]
2008-01-17T00:00:00
[ [ "Artru", "X.", "", "IPNL" ], [ "Richard", "J. -M.", "", "LPSC" ], [ "Soffer", "J.", "" ] ]
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801.1783
Olivier Finkel
Jacques Duparc (UNIL), Olivier Finkel (LIP)
An omega-power of a context-free language which is Borel above Delta^0_omega
To appear in the Proceedings of the International Conference Foundations of the Formal Sciences V : Infinite Games, November 26th to 29th, 2004, Bonn, Germany, Stefan Bold, Benedikt L\"owe, Thoralf R\"asch, Johan van Benthem (eds.), College Publications at King's College (Studies in Logic), 2007
Dans Proceedings of the International Conference on Foundations of the Formal Sciences V : Infinite Games - Foundations of the Formal Sciences V : Infinite Games, November 26-29, 2004, Bonn : Allemagne
null
null
cs.CC cs.GT cs.LO math.LO
null
We use erasers-like basic operations on words to construct a set that is both Borel and above Delta^0_omega, built as a set V^\omega where V is a language of finite words accepted by a pushdown automaton. In particular, this gives a first example of an omega-power of a context free language which is a Borel set of infinite rank.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:20:30 GMT" } ]
2008-09-10T00:00:00
[ [ "Duparc", "Jacques", "", "UNIL" ], [ "Finkel", "Olivier", "", "LIP" ] ]
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801.1784
Sergei Vyshenski
S. V. Vyshenski, P. V. Grigoriev, Yu. Yu. Dubenskaya
Ideal synchronizer for marked pairs in fork-join network
18 pages, 3 figures, in Russian, typos fixed
null
null
null
cs.DM
null
We introduce a new functional element (synchronizer for marked pairs) meant to join results of parallel processing in two-branch fork-join queueing network. Approximations for distribution of sojourn time at the synchronizer are derived along with a validity domain. Calculations are performed assuming that: arrivals to the network form a Poisson process, each branch operates like an M/M/N queueing system. It is shown that mean sojourn time at a real synchronizer node is bounded below by the value, defined by parameters of the network (which contains the synchronizer) and does not depend upon performance and particular properties of the synchronizer.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:00:59 GMT" }, { "version": "v2", "created": "Mon, 14 Jan 2008 20:57:32 GMT" } ]
2009-09-29T00:00:00
[ [ "Vyshenski", "S. V.", "" ], [ "Grigoriev", "P. V.", "" ], [ "Dubenskaya", "Yu. Yu.", "" ] ]
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801.1785
Troost Jan
Raphael Benichou, Giuseppe Policastro, Jan Troost
T-duality in Ramond-Ramond backgrounds
7 pages, accepted for publication in PLB
Phys.Lett.B661:192-195,2008
10.1016/j.physletb.2008.01.059
LPTENS-08/03
hep-th
null
Using the pure spinor formalism on the world-sheet, we derive the T-duality rules for all target space couplings in an efficient manner. The world-sheet path integral derivation is a proof of the equivalence of the T-dual Ramond-Ramond backgrounds which is valid non-perturbatively in the string length over the curvature radius and to all orders in perturbation theory in the string coupling.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:34:46 GMT" } ]
2008-11-26T00:00:00
[ [ "Benichou", "Raphael", "" ], [ "Policastro", "Giuseppe", "" ], [ "Troost", "Jan", "" ] ]
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801.1786
Roberto Raimondi
M. Milletari', R. Raimondi and P. Schwab
Magneto-spin Hall conductivity of a two-dimensional electron gas
5 pages, 1 figure
null
10.1209/0295-5075/82/67005
null
cond-mat.mes-hall cond-mat.dis-nn
null
It is shown that the interplay of long-range disorder and in-plane magnetic field gives rise to an out-of-plane spin polarization and a finite spin Hall conductivity of the two-dimensional electron gas in the presence of Rashba spin-orbit coupling. A key aspect is provided by the electric-field induced in-plane spin polarization. Our results are obtained first in the \textit{clean} limit where the spin-orbit splitting is much larger than the disorder broadening of the energy levels via the diagrammatic evaluation of the Kubo-formula. Then the results are shown to hold in the full range of the disorder parameter $\alpha p_F \tau$ by means of the quasiclassical Green function technique.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:37:36 GMT" } ]
2009-11-13T00:00:00
[ [ "Milletari'", "M.", "" ], [ "Raimondi", "R.", "" ], [ "Schwab", "P.", "" ] ]
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801.1787
Daniel Senff
D. Senff, O. Schumann, M. Benomar, M. Kriener, T. Lorenz, Y. Sidis, K. Habicht, P. Link, and M. Braden
Melting of magnetic correlations in charge-orbital ordered La(0.5)Sr(1.5)MnO(4) : competition of ferro and antiferromagnetic states
14 pages, 11 figures
null
10.1103/PhysRevB.77.184413
null
cond-mat.str-el
null
The magnetic correlations in the charge- and orbital-ordered manganite La(0.5)Sr(1.5)MnO(4) have been studied by elastic and inelastic neutron scattering techniques. Out of the well-defined CE-type magnetic structure with the corresponding magnons a competition between CE-type and ferromagnetic fluctuations develops. Whereas ferromagnetic correlations are fully suppressed by the static CE-type order at low temperature, elastic and inelastic CE-type correlations disappear with the melting of the charge-orbital order at high temperature. In its charge-orbital disordered phase, La(0.5)Sr(1.5)MnO(4) exhibits a dispersion of ferromagnetic correlations which remarkably resembles the magnon dispersion in ferromagnetically ordered metallic perovskite manganites.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:50:09 GMT" } ]
2009-11-13T00:00:00
[ [ "Senff", "D.", "" ], [ "Schumann", "O.", "" ], [ "Benomar", "M.", "" ], [ "Kriener", "M.", "" ], [ "Lorenz", "T.", "" ], [ "Sidis", "Y.", "" ], [ "Habicht", "K.", "" ], [ "Link", "P.", "" ], [ "Braden", "M.", "" ] ]
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801.1788
Dong Ye
Dong Ye and Heping Zhang
Extremal fullerene graphs with the maximum Clar number
35 pages, 43 figures
Discrete Appl. Math. 157 (2009) 3152-3173
10.1016/j.dam.2009.06.007
null
math.CO
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
A fullerene graph is a cubic 3-connected plane graph with (exactly 12) pentagonal faces and hexagonal faces. Let $F_n$ be a fullerene graph with $n$ vertices. A set $\mathcal H$ of mutually disjoint hexagons of $F_n$ is a sextet pattern if $F_n$ has a perfect matching which alternates on and off each hexagon in $\mathcal H$. The maximum cardinality of sextet patterns of $F_n$ is the Clar number of $F_n$. It was shown that the Clar number is no more than $\lfloor\frac {n-12} 6\rfloor$. Many fullerenes with experimental evidence attain the upper bound, for instance, $\text{C}_{60}$ and $\text{C}_{70}$. In this paper, we characterize extremal fullerene graphs whose Clar numbers equal $\frac{n-12} 6$. By the characterization, we show that there are precisely 18 fullerene graphs with 60 vertices, including $\text{C}_{60}$, achieving the maximum Clar number 8 and we construct all these extremal fullerene graphs.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:30:43 GMT" }, { "version": "v2", "created": "Tue, 11 Aug 2009 12:19:53 GMT" } ]
2009-08-11T00:00:00
[ [ "Ye", "Dong", "" ], [ "Zhang", "Heping", "" ] ]
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801.1789
Ekaterina Christova
Ekaterina Christova and Elliot Leader
About S-\bar s, \Delta S-\Delta\bar s and D_d^{K+ - K-} in K^\pm Production in Sidis
this is a talk given at the XII Workshop On High Energy Spin Physics (DSPIN-07), September 3--7, 2007 at JINR, Dubna, Russia, 4 pages. to appear in the proceedings of the workshop
null
null
null
hep-ph
null
We consider semi-inclusive unpolarized DIS for the production of charged Kaons and the different possibilities, both in LO and NLO, to test the conventionally used assumptions s-\bar s=0, \Delta s-\Delta \bar s=0 and D_d^{K+ - K-}=0. The considered tests have the advantage that they do not require any knowledge of the fragmentation functions.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 14:54:27 GMT" } ]
2008-01-14T00:00:00
[ [ "Christova", "Ekaterina", "" ], [ "Leader", "Elliot", "" ] ]
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801.179
Ian Appelbaum
Biqin Huang and Ian Appelbaum
Spin Dephasing in Drift-Dominated Semiconductor Spintronics Devices
null
Phys. Rev. B 77, 165331 (2008)
10.1103/PhysRevB.77.165331
null
cond-mat.mtrl-sci cond-mat.other
null
A spin transport model is employed to study the effects of spin dephasing induced by diffusion-driven transit-time uncertainty through semiconductor spintronic devices where drift is the dominant transport mechanism. It is found that in the ohmic regime, dephasing is independent of transit length, and determined primarily by voltage drop across the spin transport region. The effects of voltage and temperature predicted by the model are compared to experimental results from a 350-micron-thick silicon spin-transport device using derived mathematical expressions of spin dephasing.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:40:04 GMT" } ]
2009-11-13T00:00:00
[ [ "Huang", "Biqin", "" ], [ "Appelbaum", "Ian", "" ] ]
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801.1791
Christos Efthymiopoulos
Christos Efthymiopoulos, Tassos Bountis and Thanos Manos
Explicit Construction of First Integrals with Quasi-monomial Terms from the Painlev\'{e} Series
16 pages, 0 figures
null
10.1070/RD2004v009n03ABEH000286
null
nlin.SI
null
The Painlev\'{e} and weak Painlev\'{e} conjectures have been used widely to identify new integrable nonlinear dynamical systems. For a system which passes the Painlev\'{e} test, the calculation of the integrals relies on a variety of methods which are independent from Painlev\'{e} analysis. The present paper proposes an explicit algorithm to build first integrals of a dynamical system, expressed as `quasi-polynomial' functions, from the information provided solely by the Painlev\'{e} - Laurent series solutions of a system of ODEs. Restrictions on the number and form of quasi-monomial terms appearing in a quasi-polynomial integral are obtained by an application of a theorem by Yoshida (1983). The integrals are obtained by a proper balancing of the coefficients in a quasi-polynomial function selected as initial ansatz for the integral, so that all dependence on powers of the time $\tau=t-t_0$ is eliminated. Both right and left Painlev\'{e} series are useful in the method. Alternatively, the method can be used to show the non-existence of a quasi-polynomial first integral. Examples from specific dynamical systems are given.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:36:57 GMT" } ]
2015-05-13T00:00:00
[ [ "Efthymiopoulos", "Christos", "" ], [ "Bountis", "Tassos", "" ], [ "Manos", "Thanos", "" ] ]
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801.1792
Dmitry Beliaev
D. Beliaev and S. Smirnov
Harmonic measure and SLE
null
null
10.1007/s00220-009-0864-7
null
math.CV math.PR
null
In this paper we rigorously compute the average multifractal spectrum of harmonic measure on the boundary of SLE clusters.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:50:33 GMT" } ]
2015-05-13T00:00:00
[ [ "Beliaev", "D.", "" ], [ "Smirnov", "S.", "" ] ]
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801.1793
Giuseppe Falzetta doc
Giuseppe Falzetta
Realizzazione di un esperimento innovativo con doppia fenditura utilizzando coppie correlate di fotoni
My master thesis in italian
null
null
null
quant-ph
null
In this Thesis I present a double slit experiment where two undistinguishable photons produced by type I PDC are sent each to a well defined slit. Data about the diffraction and interference patterns for coincidences are presented and discussed. An analysis of these data allows a first test of standard quantum mechanics against de Broglie-Bohm theory.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:43:20 GMT" } ]
2008-01-14T00:00:00
[ [ "Falzetta", "Giuseppe", "" ] ]
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801.1794
Partha Konar
Kaoru Hagiwara, Partha Konar, Qiang Li, Kentarou Mawatari, Dieter Zeppenfeld
Graviton production with 2 jets at the LHC in large extra dimensions
8 pages, 10 figures, 1 table; Version to be printed in JHEP
JHEP 0804:019,2008
10.1088/1126-6708/2008/04/019
KA-TP-01-2008, KEK-TH-1217, KIAS-P08006, SFB/CPP-08-01, UFIFT-HEP-08-01
hep-ph
null
We study Kaluza-Klein (KK) graviton production in the large extra dimensions model via 2 jets plus missing transverse momentum signatures at the LHC. We make predictions for both the signal and the dominant Zjj and Wjj backgrounds, where we introduce missing P_T-dependent jet selection cuts that ensure the smallness of the 2-jet rate over the 1-jet rate. With the same jet selection cuts, the distributions of the two jets and their correlation with the missing transverse momentum provide additional evidence for the production of an invisible massive object.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:44:27 GMT" }, { "version": "v2", "created": "Fri, 28 Mar 2008 20:00:37 GMT" } ]
2009-01-06T00:00:00
[ [ "Hagiwara", "Kaoru", "" ], [ "Konar", "Partha", "" ], [ "Li", "Qiang", "" ], [ "Mawatari", "Kentarou", "" ], [ "Zeppenfeld", "Dieter", "" ] ]
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801.1795
Aleksi Halkola
A. Halkola, H. Hildebrandt, T. Schrabback, M. Lombardi, M. Bradac, T. Erben, P. Schneider, D. Wuttke
The mass distribution of RX J1347-1145 from strong lensing
Accepted for publication in the A&A
null
10.1051/0004-6361:20078877
null
astro-ph
null
High resolution HST/ACS images of the galaxy cluster RX J1347-1145 have enabled us to identify several new multiple image candidates in the cluster, including a 5 image system with a central image. The multiple images allow us to construct an accurate 2-dimensional mass map of the central part of the cluster. The modelling of the cluster mass includes the most prominent cluster galaxies modelled as truncated isothermal spheres and a smooth halo component that is described with 2 parametric profiles. The mass reconstruction is done using a Markov chain Monte Carlo method that provides us with a total projected mass density as well as estimates for the parameters of interest and their respective errors. The mass profile is in reasonable agreement with previous mass estimates based on the X-ray emission from the hot intra-cluster gas, however the X-ray mass estimates are systematically lower than what we obtain with gravitational lensing.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:54:04 GMT" } ]
2009-11-13T00:00:00
[ [ "Halkola", "A.", "" ], [ "Hildebrandt", "H.", "" ], [ "Schrabback", "T.", "" ], [ "Lombardi", "M.", "" ], [ "Bradac", "M.", "" ], [ "Erben", "T.", "" ], [ "Schneider", "P.", "" ], [ "Wuttke", "D.", "" ] ]
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801.1796
Alexander Khodjamirian
G.Duplancic, A.Khodjamirian, Th.Mannel, B.Melic, N.Offen
Light-cone sum rules for $B \to \pi$ form factors revisited
33 pages, 7 figures, one figure and a few comments added, version to appear in JHEP
JHEP 0804:014,2008
10.1088/1126-6708/2008/04/014
SI-HEP-2007-15
hep-ph
null
We reconsider and update the QCD light-cone sum rules for $B\to \pi$ form factors. The gluon radiative corrections to the twist-2 and twist-3 terms in the correlation functions are calculated. The $\bar{MS}$ $b$-quark mass is employed, instead of the one-loop pole mass used in the previous analyses. The light-cone sum rule for $f^+_{B\pi}(q^2)$ is fitted to the measured $q^2$-distribution in $B\to \pi l \nu_l$, fixing the input parameters with the largest uncertainty: the Gegenbauer moments of the pion distribution amplitude. For the $B\to \pi$ vector form factor at zero momentum transfer we predict $f^+_{B\pi}(0)= 0.26^{+0.04}_{-0.03}$. Combining it with the value of the product $|V_{ub}f^+_{B\pi}(0)|$ extracted from experiment, we obtain $|V_{ub}|=(3.5\pm 0.4\pm 0.2\pm 0.1) \times 10^{-3}$. In addition, the scalar and penguin $B\to \pi$ form factors $f^0_{B\pi}(q^2)$ and $f^T_{B\pi}(q^2)$ are calculated.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:59:02 GMT" }, { "version": "v2", "created": "Thu, 3 Apr 2008 12:47:31 GMT" } ]
2009-01-06T00:00:00
[ [ "Duplancic", "G.", "" ], [ "Khodjamirian", "A.", "" ], [ "Mannel", "Th.", "" ], [ "Melic", "B.", "" ], [ "Offen", "N.", "" ] ]
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801.1797
Makoto Natsuume
Makoto Natsuume and Takashi Okamura
A note on causal hydrodynamics for M-theory branes
6 pages, ReVTeX4
Prog.Theor.Phys.120:1217-1222,2008
10.1143/PTP.120.1217
KEK-TH-1221
hep-th hep-ph nucl-th
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We obtain new transport coefficients of causal hydrodynamics for the M2 and the M5-brane using a Kubo-like formula proposed by Baier, Romatschke, Son, Starinets, and Stephanov (arXiv:0712.2451 [hep-th]). The relaxation times agree with the ones obtained from the "sound mode" in our paper (arXiv:0712.2916 [hep-th]).
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:40:11 GMT" }, { "version": "v2", "created": "Mon, 14 Jan 2008 19:46:28 GMT" }, { "version": "v3", "created": "Wed, 10 Dec 2008 09:12:52 GMT" } ]
2008-12-25T00:00:00
[ [ "Natsuume", "Makoto", "" ], [ "Okamura", "Takashi", "" ] ]
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801.1798
Tobias Reichenbach
Tobias Reichenbach, Mauro Mobilia, and Erwin Frey
Self-Organization of Mobile Populations in Cyclic Competition
21 pages, 10 figures. To appear in J. Theor. Biol
J. Theor. Biol. 254, 368-383 (2008)
10.1016/j.jtbi.2008.05.014
LMU-ASC 04/08
q-bio.PE cond-mat.stat-mech nlin.AO physics.bio-ph
null
The formation of out-of-equilibrium patterns is a characteristic feature of spatially-extended, biodiverse, ecological systems. Intriguing examples are provided by cyclic competition of species, as metaphorically described by the `rock-paper-scissors' game. Both experimentally and theoretically, such non-transitive interactions have been found to induce self-organization of static individuals into noisy, irregular clusters. However, a profound understanding and characterization of such patterns is still lacking. Here, we theoretically investigate the influence of individuals' mobility on the spatial structures emerging in rock-paper-scissors games. We devise a quantitative approach to analyze the spatial patterns self-forming in the course of the stochastic time evolution. For a paradigmatic model originally introduced by May and Leonard, within an interacting particle approach, we demonstrate that the system's behavior - in the proper continuum limit - is aptly captured by a set of stochastic partial differential equations. The system's stochastic dynamics is shown to lead to the emergence of entangled rotating spiral waves. While the spirals' wavelength and spreading velocity is demonstrated to be accurately predicted by a (deterministic) complex Ginzburg-Landau equation, their entanglement results from the inherent stochastic nature of the system.These findings and our methods have important applications for understanding the formation of noisy patterns, e.g., in ecological and evolutionary contexts, and are also of relevance for the kinetics of (bio)-chemical reactions.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:08:56 GMT" }, { "version": "v2", "created": "Wed, 28 May 2008 11:23:18 GMT" } ]
2008-08-31T00:00:00
[ [ "Reichenbach", "Tobias", "" ], [ "Mobilia", "Mauro", "" ], [ "Frey", "Erwin", "" ] ]
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801.1799
Ivana Petkovi\'c
R. Latempa, M. Aprili and I. Petkovic
Quasiparticle Trapping In Three Terminal Ferromagnetic Tunneling Devices
null
null
10.1063/1.3260237
null
cond-mat.supr-con cond-mat.mes-hall
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Hybrid Superconductor/Ferromagnet structures have been investigated recently to address the interplay between ferromagnetism and superconductivity. They also open up new routes for the investigation of out of equilibrium superconductivity. Here, we show how it is possible for out of equilibrium excitations produced in a superconducting thin film (S) to be localized in a ferromagnetic trap (F). Specifically, a ferromagnetic nano-volume in good contact with S represents a potential well for the quasiparticles (QPs) at the gap edge. As the superconducting proximity effect is highly suppressed in F, QPs get efficiently trapped and they share their energy with the free electrons in the trap. The electronic temperature Te in the trap can be increased by up to 60% from the bath temperature at 320 mK as measured by tunneling spectroscopy using a second junction.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:07:36 GMT" }, { "version": "v2", "created": "Thu, 24 Jan 2008 12:27:28 GMT" }, { "version": "v3", "created": "Tue, 13 Jan 2009 13:30:35 GMT" } ]
2015-05-13T00:00:00
[ [ "Latempa", "R.", "" ], [ "Aprili", "M.", "" ], [ "Petkovic", "I.", "" ] ]
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801.18
Michelangelo Mangano
T. Lari, L. Pape, W. Porod, J.A. Aguilar-Saavedra, F. del Aguila, B.C. Allanach, J. Alwall, Yu. Andreev, D. Aristizabal Sierra, A. Bartl, M. Beccaria, S. Bejar, L. Benucci, S. Bityukov, I. Borjanovic, G. Bozzi, G. Burdman, J. Carvalho, N. Castro, B. Clerbaux, F. de Campos, A. de Gouvea, C. Dennis, A. Djouadi, O.J.P. Eboli, U. Ellwanger, D. Fassouliotis, P.M. Ferreira, R. Frederix, B. Fuks, J.-M. Gerard, A. Giammanco, S. Gopalakrishna, T. Goto, B. Grzadkowski, J. Guasch, T. Hahn, S. Heinemeyer, A. Hektor, M. Herquet, B. Herrmann, K. Hidaka, M. K. Hirsch, K. Hohenwarter-Sodek, W. Hollik, G. W. S. Hou, T. Hurth, A. Ibarra, J. Illana, M. Kadastik, S. Kalinin, C. Karafasoulis, M. Karagoz Unel, T. Kernreiter, M. M. Kirsanov, M. Klasen, E. Kou, C. Kourkoumelis, S. Kraml, N. Krasnikov, F. Krauss, A. Kyriakis, V. Lemaitre, G. Macorini, M.B. Magro, W. Majerotto, F. Maltoni, R. Mehdiyev, M. Misiak, F. Moortgat, G. Moreau, M. M\"uhlleitner, M. Muntel, A. Onofre, E. Ozcan, F. Palla, L. Panizzi, L. Pape, S. Penaranda, R. Pittau, G. Polesello, A. Pukhov, M. Raidal, A.R. Raklev, L. Rebane, F. M. Renard, D. Restrepo, Z. Roupas, R. Santos, S. Schumann, G. Servant, F. Siegert, P. Skands, P. Slavich, J. Sola, M. Spira, S. Sultansoy, A. Toropin, A. Tricomi, J. Tseng, G. Unel, J.W.F. Valle, F. Veloso, A. Ventura, G. Vermisoglou, C. Verzegnassi, A. Villanova del Moral, G. Weiglein, M. Yilmaz
Collider aspects of flavour physics at high Q
Report of Working Group 1 of the CERN Workshop ``Flavour in the era of the LHC'', Geneva, Switzerland, November 2005 -- March 2007
Eur.Phys.J.C57:183-308,2008
10.1140/epjc/s10052-008-0713-4
null
hep-ph hep-ex
null
This review presents flavour related issues in the production and decays of heavy states at LHC, both from the experimental side and from the theoretical side. We review top quark physics and discuss flavour aspects of several extensions of the Standard Model, such as supersymmetry, little Higgs model or models with extra dimensions. This includes discovery aspects as well as measurement of several properties of these heavy states. We also present public available computational tools related to this topic.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 15:34:00 GMT" } ]
2008-12-18T00:00:00
[ [ "Lari", "T.", "" ], [ "Pape", "L.", "" ], [ "Porod", "W.", "" ], [ "Aguilar-Saavedra", "J. A.", "" ], [ "del Aguila", "F.", "" ], [ "Allanach", "B. C.", "" ], [ "Alwall", "J.", "" ], [ "Andreev", "Yu.", "" ], [ "Sierra", "D. Aristizabal", "" ], [ "Bartl", "A.", "" ], [ "Beccaria", "M.", "" ], [ "Bejar", "S.", "" ], [ "Benucci", "L.", "" ], [ "Bityukov", "S.", "" ], [ "Borjanovic", "I.", "" ], [ "Bozzi", "G.", "" ], [ "Burdman", "G.", "" ], [ "Carvalho", "J.", "" ], [ "Castro", "N.", "" ], [ "Clerbaux", "B.", "" ], [ "de Campos", "F.", "" ], [ "de Gouvea", "A.", "" ], [ "Dennis", "C.", "" ], [ "Djouadi", "A.", "" ], [ "Eboli", "O. J. P.", "" ], [ "Ellwanger", "U.", "" ], [ "Fassouliotis", "D.", "" ], [ "Ferreira", "P. M.", "" ], [ "Frederix", "R.", "" ], [ "Fuks", "B.", "" ], [ "Gerard", "J. -M.", "" ], [ "Giammanco", "A.", "" ], [ "Gopalakrishna", "S.", "" ], [ "Goto", "T.", "" ], [ "Grzadkowski", "B.", "" ], [ "Guasch", "J.", "" ], [ "Hahn", "T.", "" ], [ "Heinemeyer", "S.", "" ], [ "Hektor", "A.", "" ], [ "Herquet", "M.", "" ], [ "Herrmann", "B.", "" ], [ "Hidaka", "K.", "" ], [ "Hirsch", "M. K.", "" ], [ "Hohenwarter-Sodek", "K.", "" ], [ "Hollik", "W.", "" ], [ "Hou", "G. W. S.", "" ], [ "Hurth", "T.", "" ], [ "Ibarra", "A.", "" ], [ "Illana", "J.", "" ], [ "Kadastik", "M.", "" ], [ "Kalinin", "S.", "" ], [ "Karafasoulis", "C.", "" ], [ "Unel", "M. Karagoz", "" ], [ "Kernreiter", "T.", "" ], [ "Kirsanov", "M. M.", "" ], [ "Klasen", "M.", "" ], [ "Kou", "E.", "" ], [ "Kourkoumelis", "C.", "" ], [ "Kraml", "S.", "" ], [ "Krasnikov", "N.", "" ], [ "Krauss", "F.", "" ], [ "Kyriakis", "A.", "" ], [ "Lemaitre", "V.", "" ], [ "Macorini", "G.", "" ], [ "Magro", "M. B.", "" ], [ "Majerotto", "W.", "" ], [ "Maltoni", "F.", "" ], [ "Mehdiyev", "R.", "" ], [ "Misiak", "M.", "" ], [ "Moortgat", "F.", "" ], [ "Moreau", "G.", "" ], [ "Mühlleitner", "M.", "" ], [ "Muntel", "M.", "" ], [ "Onofre", "A.", "" ], [ "Ozcan", "E.", "" ], [ "Palla", "F.", "" ], [ "Panizzi", "L.", "" ], [ "Pape", "L.", "" ], [ "Penaranda", "S.", "" ], [ "Pittau", "R.", "" ], [ "Polesello", "G.", "" ], [ "Pukhov", "A.", "" ], [ "Raidal", "M.", "" ], [ "Raklev", "A. R.", "" ], [ "Rebane", "L.", "" ], [ "Renard", "F. M.", "" ], [ "Restrepo", "D.", "" ], [ "Roupas", "Z.", "" ], [ "Santos", "R.", "" ], [ "Schumann", "S.", "" ], [ "Servant", "G.", "" ], [ "Siegert", "F.", "" ], [ "Skands", "P.", "" ], [ "Slavich", "P.", "" ], [ "Sola", "J.", "" ], [ "Spira", "M.", "" ], [ "Sultansoy", "S.", "" ], [ "Toropin", "A.", "" ], [ "Tricomi", "A.", "" ], [ "Tseng", "J.", "" ], [ "Unel", "G.", "" ], [ "Valle", "J. W. F.", "" ], [ "Veloso", "F.", "" ], [ "Ventura", "A.", "" ], [ "Vermisoglou", "G.", "" ], [ "Verzegnassi", "C.", "" ], [ "del Moral", "A. Villanova", "" ], [ "Weiglein", "G.", "" ], [ "Yilmaz", "M.", "" ] ]
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801.1801
Henri Gouin
Henri Gouin (LMMT, MSNMGP)
The wetting problem of fluids on solid surfaces. Part 1: the dynamics of contact lines
Fichier preprint 28 pages
Continuum Mechanics and Thermodynamics 15, 6 (2003) 581-596
10.1007/s00161-003-0136-2
null
physics.class-ph
null
The understanding of the spreading of liquids on solid surfaces is an important challenge for contemporary physics. Today, the motion of the contact line formed at the intersection of two immiscible fluids and a solid is still subject to dispute. In this paper, a new picture of the dynamics of wetting is offered through an example of non-Newtonian slow liquid movements. The kinematics of liquids at the contact line and equations of motion are revisited. Adherence conditions are required except at the contact line. Consequently, for each fluid, the velocity field is multivalued at the contact line and generates an equivalent concept of line friction but stresses and viscous dissipation remain bounded. A Young-Dupr\'e equation for the apparent dynamic contact angle between the interface and solid surface depending on the movements of the fluid near the contact line is proposed.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:22:02 GMT" } ]
2009-11-13T00:00:00
[ [ "Gouin", "Henri", "", "LMMT, MSNMGP" ] ]
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801.1802
Thorsten Feldmann
Thorsten Feldmann (TU Munich and Univ. Siegen), Thomas Mannel (Univ. Siegen)
Large Top Mass and Non-Linear Representation of Flavour Symmetry
4 pages, no figures, uses revtex4
Phys.Rev.Lett.100:171601,2008
10.1103/PhysRevLett.100.171601
SI-HEP-2008-01, TUM-HEP-680/08
hep-ph hep-th
null
We consider an effective theory (ET) approach to flavour-violating processes beyond the Standard Model (SM), where the breaking of flavour symmetry is described by spurion fields whose low-energy vacuum expectation values are identified with the SM Yukawa couplings. Insisting on canonical mass dimensions for the spurion fields, the large top-quark Yukawa coupling also implies a large expectation value for the associated spurion, which breaks part of the flavour symmetry already at the UV scale Lambda of the ET. Below that scale, flavour symmetry in the ET is represented in a non-linear way by introducing Goldstone modes for the partly broken flavour symmetry and spurion fields transforming under the residual symmetry. As a result, the dominance of certain flavour structures in rare quark decays can be understood in terms of the 1/Lambda expansion in the ET. We also discuss the generalization to 2-Higgs-doublet models with large tan(beta).
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:30:17 GMT" } ]
2008-11-26T00:00:00
[ [ "Feldmann", "Thorsten", "", "TU Munich and Univ. Siegen" ], [ "Mannel", "Thomas", "", "Univ.\n Siegen" ] ]
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801.1803
Huang Jing
M. Amenomori, et al (for the Tibet ASgamma Collaboration)
The all-particle spectrum of primary cosmic rays in the wide energy range from 10^14 eV to 10^17 eV observed with the Tibet-III air-shower array
19 pages, 20 figures, accepted by ApJ
Astrophys.J.678:1165-1179,2008
10.1086/529514
null
hep-ex astro-ph
null
We present an updated all-particle energy spectrum of primary cosmic rays in a wide range from 10^14 eV to 10^17 eV using 5.5 times 10^7 events collected in the period from 2000 November through 2004 October by the Tibet-III air-shower array located at 4300 m above sea level (atmospheric depth of 606 g/cm^2). The size spectrum exhibits a sharp knee at a corresponding primary energy around 4 PeV. This work uses increased statistics and new simulation calculations for the analysis. We performed extensive Monte Carlo calculations and discuss the model dependences involved in the final result assuming interaction models of QGSJET01c and SIBYLL2.1 and primary composition models of heavy dominant (HD) and proton dominant (PD) ones. Pure proton and pure iron primary models are also examined as extreme cases. The detector simulation was also made to improve the accuracy of determining the size of the air showers and the energy of the primary particle. We confirmed that the all-particle energy spectra obtained under various plausible model parameters are not significantly different from each other as expected from the characteristics of the experiment at the high altitude, where the air showers of the primary energy around the knee reaches near maximum development and their features are dominated by electromagnetic components leading to the weak dependence on the interaction model or the primary mass. This is the highest-statistical and the best systematics-controlled measurement covering the widest energy range around the knee energy region.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:40:39 GMT" }, { "version": "v2", "created": "Thu, 17 Jan 2008 12:14:46 GMT" } ]
2019-08-13T00:00:00
[ [ "Amenomori", "M.", "" ] ]
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801.1804
Bernhard Heim
Bernhard Heim
On the Spezialschar of Maass
null
null
null
null
math.NT math.CV
null
Let $M_k^{(n)}$ be the space of Siegel modular forms of degree $n$ and even weight $k$. In this paper firstly a certain subspace $\mathsf{Spez}(M_k^{(2n)})$ the Spezialschar of $M_k^{(2n)}$ is introduced. In the setting of the Siegel three-fold it is proven that this Spezialschar is the Maass Spezialschar. Secondly an embedding of $M_k^{(2)}$ into a direct sum $\oplus_{\nu = 0}^{\lfloor \frac{k}{10} \rfloor} \text{Sym}^2 M_{k + 2 \nu}$ is given. This leads to a basic characterization of the Spezialschar property. The results of this paper are directly related to the non-vanishing of certain special values of L-functions related to the Gross-Prasad conjecture. This is illustrated by a significant example in the paper.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 16:55:34 GMT" } ]
2008-01-14T00:00:00
[ [ "Heim", "Bernhard", "" ] ]
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801.1805
Leonardo Vanni
R. Laura, L. Vanni
Conditional probabilities and collapse in quantum measurements
15 pages
International Journal of Theoretical Physics, Volume 47, Issue 9, (2008), pp. 2382-2392
10.1007/s10773-008-9672-7
null
quant-ph
null
We show that including both the system and the apparatus in the quantum description of the measurement process, and using the concept of conditional probabilities, it is possible to deduce the statistical operator of the system after a measurement with a given result, which gives the probability distribution for all possible consecutive measurements on the system. This statistical operator, representing the state of the system after the first measurement, is in general not the same that would be obtained using the postulate of collapse.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:07:36 GMT" } ]
2008-11-29T00:00:00
[ [ "Laura", "R.", "" ], [ "Vanni", "L.", "" ] ]
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801.1806
Philip Massey
Philip Massey, Emily M. Levesque, Bertrand Plez, K. A. G. Olsen
The Physical Properties of Red Supergiants: Comparing Theory and Observations
Invited review; to appear in Massive Stars as Cosmic Engines, IAU Symp. 250, ed. F. Bresolin, P. A. Crowther, and J. Puls (Cambridge University Press)
null
10.1017/S1743921308020383
null
astro-ph
null
Red supergiants (RSGs) are an evolved stage in the life of intermediate massive stars (than than 25 solar masses). For many years, their location in the H-R diagram was at variance with the evolutionary models. Using the MARCS stellar atmospheres, we have determined new effective temperatures and bolometric luminosities for RSGs in the Milky Way, LMC, and SMC, and our work has resulted in much better agreement with the evolutionary models. We have also found evidence of significant visual extinction due to circumstellar dust. Although in the Milky Way the RSGs contribute only a small fraction (than than 1 percent) of the dust to the interstellar medium (ISM), in starburst galaxies or galaxies at large look-back times, we expect that RSGs may be the main dust source. We are in the process of extending this work now to RSGs of higher and lower metallicities using the galaxies M31 and WLM.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:30:41 GMT" }, { "version": "v2", "created": "Fri, 11 Jan 2008 23:28:22 GMT" } ]
2009-11-13T00:00:00
[ [ "Massey", "Philip", "" ], [ "Levesque", "Emily M.", "" ], [ "Plez", "Bertrand", "" ], [ "Olsen", "K. A. G.", "" ] ]
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801.1807
Sergei Urazhdin
Weng L. Lim, Nicholas Anthony, Andrew Higgins, Sergei Urazhdin
Thermal Dynamics in Symmetric Magnetic Nanopillars Driven by Spin Transfer
3 pages, 3 figures
null
10.1063/1.2918012
null
cond-mat.mtrl-sci
null
We study the effects of spin transfer on thermally activated dynamics of magnetic nanopillars with identical thicknesses of the magnetic layers. The symmetric nanopillars exhibit anomalous dependencies of switching statistics on magnetic field and current. We interpret our data in terms of simultaneous current-induced excitation of both layers. We also find evidence for coupling between the fluctuations of the layers due to the spin transfer.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:19:32 GMT" } ]
2009-11-13T00:00:00
[ [ "Lim", "Weng L.", "" ], [ "Anthony", "Nicholas", "" ], [ "Higgins", "Andrew", "" ], [ "Urazhdin", "Sergei", "" ] ]
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801.1808
Pablo I. Tamborenea
C. L. Romano, P. I. Tamborenea, and S. E. Ulloa
Spin-orbit effects on two-electron states in nanowhisker double quantum dots
5 pages, 6 figures
null
10.1016/j.physe.2009.04.039
null
cond-mat.mes-hall
null
We investigate theoretically the combined effects of the electron-electron and the Rashba spin-orbit interactions on two electrons confined in quasi-one-dimensional AlInSb-based double quantum dots. We calculate the two-electron wave functions and explore the interplay between these two interactions on the energy levels and the spin of the states. The energy spectrum as a function of an applied magnetic field shows crossings and anticrossings between triplet and singlet states, associated with level mixing induced by the spin-orbit coupling. We find that the fields at which these crossings occur can be naturally controlled by the interdot barrier width, which controls the exchange integral in the structure.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:26:35 GMT" } ]
2015-05-13T00:00:00
[ [ "Romano", "C. L.", "" ], [ "Tamborenea", "P. I.", "" ], [ "Ulloa", "S. E.", "" ] ]
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801.1809
Reinhard Laubenbacher
Reinhard Laubenbacher and David Pengelley
"Voici ce que j'ai trouve": Sophie Germain's grand plan to prove Fermat's Last Theorem
to appear in Historia Mathematica
Historia Mathematica 37 (2010) 641-692
10.1016/j.hm.2009.12.002
null
math.HO
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
A study of Sophie Germain's extensive manuscripts on Fermat's Last Theorem calls for a reassessment of her work in number theory. There is much in these manuscripts beyond the single theorem for Case 1 for which she is known from a published footnote by Legendre. Germain had a fully-fledged, highly developed, sophisticated plan of attack on Fermat's Last Theorem. The supporting algorithms she invented for this plan are based on ideas and results discovered independently only much later by others, and her methods are quite different from any of Legendre's. In addition to her program for proving Fermat's Last Theorem in its entirety, Germain also made major efforts at proofs for particular families of exponents. The isolation Germain worked in, due in substantial part to her difficult position as a woman, was perhaps sufficient that much of this extensive and impressive work may never have been studied and understood by anyone.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:32:03 GMT" }, { "version": "v2", "created": "Sat, 23 Jan 2010 17:08:48 GMT" }, { "version": "v3", "created": "Fri, 9 Jul 2010 06:47:35 GMT" } ]
2019-12-20T00:00:00
[ [ "Laubenbacher", "Reinhard", "" ], [ "Pengelley", "David", "" ] ]
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801.181
Bernhard Heim
Bernhard Heim
A Strong Symmetry Property Of Eisenstein Series
To appear in the conference volume "Modular forms" Schiermonnikoog 2006, by B. Edixhoven, G.van der Geer, and B. Moonen
null
null
null
math.NT
null
In this paper we present a new method to study Fourier coefficients of holomorphic and non-holomorphic Eisenstein series simultaneously.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:34:02 GMT" } ]
2008-01-14T00:00:00
[ [ "Heim", "Bernhard", "" ] ]
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801.1811
Abhay Ashtekar
Abhay Ashtekar, Victor Taveras, Madhavan Varadarajan
Information is Not Lost in the Evaporation of 2-dimensional Black Holes
4 pages, 2 figures
Phys.Rev.Lett.100:211302,2008
10.1103/PhysRevLett.100.211302
IGC-08/01-02
gr-qc hep-th
null
We analyze Hawking evaporation of the Callen-Giddings-Harvey-Strominger (CGHS) black holes from a quantum geometry perspective and show that information is not lost, primarily because the quantum space-time is sufficiently larger than the classical. Using suitable approximations to extract physics from quantum space-times we establish that: i)future null infinity of the quantum space-time is sufficiently long for the the past vacuum to evolve to a pure state in the future; ii) this state has a finite norm in the future Fock space; and iii) all the information comes out at future infinity; there are no remnants.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:36:26 GMT" }, { "version": "v2", "created": "Thu, 22 May 2008 13:39:24 GMT" } ]
2015-01-30T00:00:00
[ [ "Ashtekar", "Abhay", "" ], [ "Taveras", "Victor", "" ], [ "Varadarajan", "Madhavan", "" ] ]
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801.1812
Daniel M. Pellegrino
G. Botelho, M. C. Matos and D. Pellegrino
Lineability of summing sets of homogeneous polynomials
15 pages
null
null
null
math.FA
null
Given a continuous $n$-homogeneous polynomial $P\colon E\longrightarrow F$ between Banach spaces and $1\leq q\leq p<\infty$, in this paper we investigate some properties concerning lineability and spaceability of the $(p;q)$-summing set of $P$, defined by $S_{p;q}(P)=\{a\in E:P\mathrm{is}% (p;q)\mathrm{summing at}a\}$.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:24:22 GMT" } ]
2008-01-14T00:00:00
[ [ "Botelho", "G.", "" ], [ "Matos", "M. C.", "" ], [ "Pellegrino", "D.", "" ] ]
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801.1813
David Tong
Chris Pedder, Julian Sonner and David Tong
The Berry Phase of D0-Branes
14 pages, 1 figure. v3: references added
JHEP 0803:065,2008
10.1088/1126-6708/2008/03/065
null
hep-th
null
We study SU(2) Yang-Mills quantum mechanics with N=2,4,8 and 16 supercharges. This describes the non-relativistic dynamics of a pair of D0-branes moving in d=3,4,6 and 10 spacetime dimensions respectively. We show that as the D0-branes orbit, states undergo a Berry holonomy described by the four Hopf maps. For the N=2 theory, the associated Hopf map is the Mobius bundle and its effect is to turn the D0-branes into anyons with exchange statistics +i and -i. For the N=4,8 and 16 theories, the Hopf maps give rise to Berry connections that are familiar to physicists: the U(1) Dirac monopole; the SU(2) Yang monopole; and the SO(8) octonionic monopole.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:43:21 GMT" }, { "version": "v2", "created": "Sun, 13 Jan 2008 12:42:44 GMT" }, { "version": "v3", "created": "Mon, 4 Feb 2008 17:18:09 GMT" } ]
2014-11-18T00:00:00
[ [ "Pedder", "Chris", "" ], [ "Sonner", "Julian", "" ], [ "Tong", "David", "" ] ]
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801.1814
Antonio Di Lorenzo
Antonio Di Lorenzo and J. Carlos Egues
Weak measurement: Effect of the detector dynamics
5 pages, 3 figures. References added. Minor revisions
Phys. Rev. A 77, 042108 (2008) (5 pages)
10.1103/PhysRevA.77.042108
null
quant-ph cond-mat.other
null
A general approach to the measurement of an observable with pre- and post-selection is presented. The limit of weak measurement is studied in detail, and it is shown that the phase of the probe, including a Hamiltonian contribution to it, gives rise to observable effects, since the coherence of the probe is essential for the concept of complex weak value to be meaningful. As a particular example, the measurement of a spin component is considered. We find that the contribution of the imaginary part of the weak value is sizeable in this case.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 17:59:45 GMT" }, { "version": "v2", "created": "Fri, 18 Apr 2008 21:22:35 GMT" } ]
2008-04-19T00:00:00
[ [ "Di Lorenzo", "Antonio", "" ], [ "Egues", "J. Carlos", "" ] ]
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801.1815
M. A. Baranov
M.A. Baranov, C. Lobo, and G.V. Shlyapnikov
Superfluid pairing between fermions with unequal masses
21 pages, 9 figures, 1 table, discussions added
Phys.Rev.A78:033620,2008
10.1103/PhysRevA.78.033620
null
cond-mat.other cond-mat.supr-con
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We consider a superfluid state in a two-component gas of fermionic atoms with equal densities and unequal masses in the BCS limit. We develop a perturbation theory along the lines proposed by Gorkov and Melik-Barkhudarov and find that for a large difference in the masses of heavy ($M$) and light ($m$) atoms one has to take into account both the second-order and third-order contributions. The result for the critical temperature and order parameter is then quite different from the prediction of the simple BCS approach. Moreover, the small parameter of the theory turns out to be $(p_{F}|a|)/\hbar)\sqrt{M/m}\ll1$, where $p_{F}$ is the Fermi momentum, and $a$ the scattering length. Thus, for a large mass ratio $M/m$ the conventional perturbation theory requires significantly smaller Fermi momenta (densities) or scattering lengths than in the case of $M\sim m$, where the small parameter is $(p_{F}|a|)/\hbar)\ll1$. We show that 3-body scattering resonances appearing at a large mass ratio due to the presence of 3-body bound Efimov states do not influence the result, which in this sense becomes universal.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:06:13 GMT" }, { "version": "v2", "created": "Wed, 11 Jun 2008 13:18:49 GMT" } ]
2008-12-18T00:00:00
[ [ "Baranov", "M. A.", "" ], [ "Lobo", "C.", "" ], [ "Shlyapnikov", "G. V.", "" ] ]
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801.1816
Georgios Mountrichas
G. Mountrichas, T. Shanks, S. M. Croom, U. Sawangwit, D. P. Schneider, A. D. Myers, K. Pimbblet
QSO-LRG 2-Point Cross-Correlation Function and Redshift-Space Distorions
22 pages, 25 figures, 8 tables
null
10.1111/j.1365-2966.2009.14456.x
null
astro-ph
null
We have measured the bias of QSOs as a function of QSO luminosity at fixed redshift (z<1) by cross-correlating them with LRGs in the same spatial volume, hence breaking the degeneracy between QSO luminosity and redshift. We use three QSO samples from 2SLAQ, 2QZ and SDSS covering a QSO absolute magnitude range, -24.5<M_{b_J}<-21.5, and cross-correlate them with 2SLAQ (z~0.5) and AAOmega (z~0.7) photometric and spectroscopic LRGs in the same redshift ranges. The 2-D and 3-D cross-clustering measurements are generally in good agreement. Our (2SLAQ) QSO-LRG clustering amplitude (r_0=6.8_{-0.3}^{+0.1}h^{-1}Mpc) as measured from the semi-projected cross-correlation function appears similar to the (2SLAQ) LRG-LRG auto-correlation amplitude (r_0=7.45\pm0.35h^{-1}Mpc) and both are higher than the (2QZ+2SLAQ) QSO-QSO amplitude (r_0\simeq5.0h^{-1}Mpc). Our measurements show remarkably little QSO-LRG cross-clustering dependence on QSO luminosity. If anything, the results imply that brighter QSOs may be less highly biased than faint QSOs, the opposite direction expected from simple high peaks biasing models. Assuming a standard LCDM model and values for b_{LRG} measured from LRG autocorrelation analyses, we find b_Q=1.45\pm0.11 at M_{b_J}\approx-24 and b_Q=1.90\pm0.16 at M_{b_J}~-22. We also find consistent results for the QSO bias from a z-space distortion analysis of the QSO-LRG cross-clustering at z~0.55. The dynamical infall results give \beta _Q=0.55\pm0.10, implying b_Q=1.4\pm0.2. Thus both the z-space distortion and the amplitude analyses yield b_Q~1.5 at M_{b_J}~-23. The implied DM halo mass inhabited by QSOs at z~0.55 is \sim10^{13}h^{-1}M_{\sun}, again approximately independent of QSO luminosity.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:16:50 GMT" } ]
2009-11-13T00:00:00
[ [ "Mountrichas", "G.", "" ], [ "Shanks", "T.", "" ], [ "Croom", "S. M.", "" ], [ "Sawangwit", "U.", "" ], [ "Schneider", "D. P.", "" ], [ "Myers", "A. D.", "" ], [ "Pimbblet", "K.", "" ] ]
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801.1817
Federico Mescia DR
FlaviaNet Working Group on Kaon Decays, M. Antonelli, V. Cirigliano, P. Franzini, S. Glazov, R. Hill, G. Isidori, F. Mescia, M. Moulson, M. Palutan, E. Passemar, M. Piccini, M. Veltri, O. Yushchenko, R.Wanke
Precision tests of the Standard Model with leptonic and semileptonic kaon decays
null
Nucl.Phys.Proc.Suppl.181-182:83-88,2008
10.1016/j.nuclphysbps.2008.09.008
null
hep-ph
null
We present a global analysis of leptonic and semileptonic kaon decays data, including all recent results by BNL-E865, KLOE, KTeV, ISTRA+, and NA48. Experimental results are critically reviewed and combined, taking into account theoretical (both analytical and numerical) constraints on the semileptonic kaon form factors. This analysis leads to a very accurate determination of Vus and allows us to perform several stringent tests of the Standard Model.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:57:43 GMT" } ]
2012-08-27T00:00:00
[ [ "FlaviaNet Working Group", "", "" ], [ "Antonelli", "M.", "" ], [ "Cirigliano", "V.", "" ], [ "Franzini", "P.", "" ], [ "Glazov", "S.", "" ], [ "Hill", "R.", "" ], [ "Isidori", "G.", "" ], [ "Mescia", "F.", "" ], [ "Moulson", "M.", "" ], [ "Palutan", "M.", "" ], [ "Passemar", "E.", "" ], [ "Piccini", "M.", "" ], [ "Veltri", "M.", "" ], [ "Yushchenko", "O.", "" ], [ "Wanke", "R.", "" ] ]
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801.1818
Antonio De Nicola
Beniamino Cappelletti Montano, Antonio De Nicola, Giulia Dileo
The geometry of 3-quasi-Sasakian manifolds
22 pages, LaTeX, to appear in Internat. J. Math
Internat. J. Math. 20 (2009), 1081-1105.
10.1142/S0129167X09005662
DMUC 07-38
math.DG
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
3-quasi-Sasakian manifolds were studied systematically by the authors in a recent paper as a suitable setting unifying 3-Sasakian and 3-cosymplectic geometries. This paper throws new light on their geometric structure which reveals to be generally richer compared to the 3-Sasakian subclass. In fact, it turns out that they are multiply foliated by four distinct fundamental foliations. The study of the transversal geometries with respect to these foliations allows us to link the 3-quasi-Sasakian manifolds to the more famous hyper-Kaehler and quaternionic-Kaehler geometries. Furthermore, we strongly improve the splitting results previously found; we prove that any 3-quasi-Sasakian manifold of rank 4l+1 is 3-cosymplectic and any 3-quasi-Sasakian manifold of maximal rank is 3-alpha-Sasakian.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:43:29 GMT" }, { "version": "v2", "created": "Sun, 13 Jul 2008 19:04:55 GMT" } ]
2009-10-27T00:00:00
[ [ "Montano", "Beniamino Cappelletti", "" ], [ "De Nicola", "Antonio", "" ], [ "Dileo", "Giulia", "" ] ]
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801.1819
Abraham Jalbout
Abraham F. Jalbout and Thomas H. Seligman
Electron Localization on Molecular Surfaces by Metal Adsorption
This manuscript was accepted for publication on January 3, 2008 to the Journal of Computational and Theoretical Nanoscience (JCTN)
null
null
null
cond-mat.mtrl-sci
null
The ability of metal adsorption to transfer charge to the surface of single molecular carbon sheets is explored in this paper. Though other metals are considered we basically will deal with Lithium We concentrate on fairly small sheets and examined the minimum threshold size of a molecular surface needed to separate metals. From our quantum chemical calculations we deduce that a molecular surface of six benzene rings is needed for Lithium dimers to be separated. We further observe symmetry breaking, when two lithium atoms are adsorbed right opposite to each other on the two sides of the sheet.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:45:36 GMT" } ]
2008-01-14T00:00:00
[ [ "Jalbout", "Abraham F.", "" ], [ "Seligman", "Thomas H.", "" ] ]
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801.182
I. V. Zozoulenko
I. V. Zozoulenko, S. Ihnatsenko
Magnetoconductance of interacting electrons in quantum wires: Spin density functional theory study
null
Physical Review B 78, 78, 035340 (2008)
10.1103/PhysRevB.78.035340
null
cond-mat.mes-hall
null
We present systematic quantitative description of the magnetoconductance of the split-gate quantum wires. Accounting for the exchange and correlation interactions within the spin density function theory (DFT) leads to the lifting of the spin degeneracy and formation of the spin-resolved plateaus at odd values of $e^{2}/h$. We show that the width of the odd conductance steps in the spin DFT calculations is equal to the width of the transition intervals between the conductance steps for the spinless electrons in the Hartree approximation. A detailed analysis of the structure of compressible/incompressible strips and the evolution of the Hartree and the spin-DFT subband structure provides an explanation of this finding. Our spin-DFT calculations reproduce not only qualitatively, but rather quantitatively all the features in the magnetoconductance observed in the recent experiment (I. P. Radu, J. B. Miller, S. Amasha, E. Levenson-Falk, D. M. Zumbuhl, M. A. Kastner, C. M. Marcus, L. N. Pfeiffer, and K. W. West, to be published) including the unexpected effect of the collapse of the odd conductance plateaus at lower fields.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:49:56 GMT" } ]
2009-05-26T00:00:00
[ [ "Zozoulenko", "I. V.", "" ], [ "Ihnatsenko", "S.", "" ] ]
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801.1821
Konstantin Chetyrkin G.
P.A. Baikov, K.G. Chetyrkin and J.H. K\"uhn
Hadronic Z- and tau-Decays in Order alpha_s^4
few citations added, final published version
Phys.Rev.Lett.101:012002,2008
10.1103/PhysRevLett.101.012002
SFB/CPP-08-04, TTP08-01
hep-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Using recently developed methods for the evaluation of five-loop amplitudes in perturbative QCD, corrections of order alpha_s^4 for the cross section of electron-positron annihilation into hadrons and for the decay rates of the Z-boson and the tau-lepton into hadrons are evaluated. The new terms lead to a significant stabilization of the perturbative series, to a reduction of the theory uncertainly in the strong coupling constant alpha_s, as extracted from these measurements, and to a small shift of the central value, moving two central values closer together. The agreement between two values of alpha_s measured at vastly different energies constitutes a striking test of asymptotic freedom. Combining the results from Z and tau decays we find alpha_s(M_Z)=0.1198 \pm 0.0015 as one of the most precise and presently only result for the strong coupling constant in order alpha_s^4.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:11:37 GMT" }, { "version": "v2", "created": "Fri, 4 Jul 2008 15:09:36 GMT" } ]
2008-11-26T00:00:00
[ [ "Baikov", "P. A.", "" ], [ "Chetyrkin", "K. G.", "" ], [ "Kühn", "J. H.", "" ] ]
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801.1822
Gerald Hoehn
Gerald Hoehn
Self-Dual Vertex Operator Superalgebras of Large Minimal Weight
18 pages with 1 table, LaTeX
null
null
null
math.QA math-ph math.MP
null
The new general upper bound mu <= [c/24] + 1 for the minimal weight mu of a self-dual vertex operator superalgebra of central charge c different from 47/2 is proven. For central charges c <= 48, further improved estimates are given and examples of with large minimal weight are discussed. We also study the case of vertex operator superalgebras with N=1 supersymmetry which was first considered by Witten in connection with three-dimensional quantum gravity. The upper bound mu^* <= (1/2)[c/12]+1/2 for the minimal superconformal weight is obtained for c different from 47/2. In addition, we show that it is impossible that the monster sporadic group acts on an extremal self-dual N=1 supersymmetric vertex operator superalgebra of central charge 48 in a way proposed by Witten if certain standard assumptions about orbifold constructions hold. The same statement holds for extremal self-dual vertex operator algebras of central charge 48.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:17:38 GMT" } ]
2008-01-14T00:00:00
[ [ "Hoehn", "Gerald", "" ] ]
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801.1823
Manuel Tiglio
Oleg Korobkin, Burak Aksoylu, Michael Holst, Enrique Pazos, Manuel Tiglio
Solving the Einstein constraint equations on multi-block triangulations using finite element methods
Changes made to match the version to appear in Classical and Quantum Gravity
Class. Quantum Grav. 26, 145007 (2009)
10.1088/0264-9381/26/14/145007
null
gr-qc
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
In order to generate initial data for nonlinear relativistic simulations, one needs to solve the Einstein constraints, which can be cast into a coupled set of nonlinear elliptic equations. Here we present an approach for solving these equations on three-dimensional multi-block domains using finite element methods. We illustrate our approach on a simple example of Brill wave initial data, with the constraints reducing to a single linear elliptic equation for the conformal factor $\psi$. We use quadratic Lagrange elements on semi-structured simplicial meshes, obtained by triangulation of multi-block grids. In the case of uniform refinement the scheme is superconvergent at most mesh vertices, due to local symmetry of the finite element basis with respect to local spatial inversions. We show that in the superconvergent case subsequent unstructured mesh refinements do not improve the quality of our initial data. As proof of concept that this approach is feasible for generating multi-block initial data in three dimensions, after constructing the initial data we evolve them in time using a high order finite-differencing multi-block approach and extract the gravitational waves from the numerical solution.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:20:08 GMT" }, { "version": "v2", "created": "Fri, 11 Jan 2008 21:33:19 GMT" }, { "version": "v3", "created": "Wed, 3 Jun 2009 07:05:21 GMT" } ]
2015-05-13T00:00:00
[ [ "Korobkin", "Oleg", "" ], [ "Aksoylu", "Burak", "" ], [ "Holst", "Michael", "" ], [ "Pazos", "Enrique", "" ], [ "Tiglio", "Manuel", "" ] ]
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801.1824
Jaime Julve
J. Julve and F. J. de Urries
Tunnelling of plane waves through a square barrier
16 pages
null
10.1088/1751-8113/41/30/304010
null
quant-ph
null
The time evolution of plane waves in the presence of a 1-dimensional square quantum barrier is considered. Comparison is made between the cases of an infinite and a cut-off (shutter) initial plane wave. The difference is relevant when the results are applied to the analysis of the tunnelling regime. This work is focused on the analytical calculation of the time-evolved solution and highlights the contribution of the resonant (Gamow) states. PACS numbers: 11.10.Ef, 11.10.Lm, 04.60
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:27:20 GMT" } ]
2009-11-13T00:00:00
[ [ "Julve", "J.", "" ], [ "de Urries", "F. J.", "" ] ]
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801.1825
Steven Diehl
Steven Diehl (T-6, LANL), Hui Li (T-6, LANL), Chris Fryer (CCS-2, LANL), David Rafferty (Penn State)
Constraining the Nature of X-ray Cavities in Clusters and Galaxies
21 pages, 12 figures, emulateapj, accepted for publication in ApJ, responded to referee's comments and added a new model, conclusions unchanged
null
10.1086/591310
LA-UR-07-7698
astro-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We present results from an extensive survey of 64 cavities in the X-ray halos of clusters, groups and normal elliptical galaxies. We show that the evolution of the size of the cavities as they rise in the X-ray atmosphere is inconsistent with the standard model of adiabatic expansion of purely hydrodynamic models. We also note that the majority of the observed bubbles should have already been shredded apart by Rayleigh-Taylor and Richtmyer-Meshkov instabilities if they were of purely hydrodynamic nature. Instead we find that the data agrees much better with a model where the cavities are magnetically dominated and inflated by a current-dominated magneto-hydrodynamic jet model, recently developed by Li et al. (2006) and Nakamura et al. (2006). We conduct complex Monte-Carlo simulations of the cavity detection process including incompleteness effects to reproduce the cavity sample's characteristics. We find that the current-dominated model agrees within 1sigma, whereas the other models can be excluded at >5sigma confidence. To bring hydrodynamic models into better agreement, cavities would have to be continuously inflated. However, these assessments are dependent on our correct understanding of the detectability of cavities in X-ray atmospheres, and will await confirmation when automated cavity detection tools become available in the future. Our results have considerable impact on the energy budget associated with active galactic nucleus feedback.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:34:46 GMT" }, { "version": "v2", "created": "Tue, 8 Jul 2008 17:56:07 GMT" } ]
2009-11-13T00:00:00
[ [ "Diehl", "Steven", "", "T-6, LANL" ], [ "Li", "Hui", "", "T-6, LANL" ], [ "Fryer", "Chris", "", "CCS-2,\n LANL" ], [ "Rafferty", "David", "", "Penn State" ] ]
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801.1826
Michelangelo Mangano
M. Raidal, A. van der Schaaf, I. Bigi, M.L. Mangano, Y. Semertzidis, S. Abel, S. Albino, S. Antusch, E. Arganda, B. Bajc, S. Banerjee, C. Biggio, M. Blanke, W. Bonivento, G.C. Branco, D. Bryman, A.J. Buras, L. Calibbi, A. Ceccucci, P.H. Chankowski, S. Davidson, A. Deandrea, D.P. DeMille, F. Deppisch, M. Diaz, B. Duling, M. Felcini, W. Fetscher, D.K. Ghosh, M. Giffels, G. Giudice, E. Goudzovskij, T. Han, P.G. Harris, M.J. Herrero, J. Hisano, R.J. Holt, K. Huitu, A. Ibarra, O. Igonkina, A. Ilakovac, J. Imazato, G. Isidori, F.R. Joaquim, M. Kadastik, Y. Kajiyama, S.F. King, K. Kirch, M.G. Kozlov, M. Krawczyk, T. Kress, O. Lebedev, A. Lusiani, E. Ma, G. Marchiori, I. Masina, G. Moreau, T. Mori, M. Muntel, F. Nesti, C.J.G. Onderwater, P. Paradisi, S.T. Petcov, M. Picariello, V. Porretti, A. Poschenrieder, M. Pospelov, L. Rebane, M.N. Rebelo, A. Ritz, L. Roberts, A. Romanino, A. Rossi, R. Rueckl, G. Senjanovic, N. Serra, T. Shindou, Y. Takanishi, C. Tarantino, A.M. Teixeira, E. Torrente-Lujan, K.J. Turzynski, T.E.J. Underwood, S.K. Vempati, O. Vives
Flavour physics of leptons and dipole moments
Report of Working Group 3 of the CERN Workshop ``Flavour in the era of the LHC'', Geneva, Switzerland, November 2005 -- March 2007
Eur.Phys.J.C57:13-182,2008
10.1140/epjc/s10052-008-0715-2
null
hep-ph hep-ex
null
This chapter of the report of the ``Flavour in the era of the LHC'' Workshop discusses the theoretical, phenomenological and experimental issues related to flavour phenomena in the charged lepton sector and in flavour-conserving CP-violating processes. We review the current experimental limits and the main theoretical models for the flavour structure of fundamental particles. We analyze the phenomenological consequences of the available data, setting constraints on explicit models beyond the Standard Model, presenting benchmarks for the discovery potential of forthcoming measurements both at the LHC and at low energy, and exploring options for possible future experiments.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:25:25 GMT" } ]
2008-12-18T00:00:00
[ [ "Raidal", "M.", "" ], [ "van der Schaaf", "A.", "" ], [ "Bigi", "I.", "" ], [ "Mangano", "M. L.", "" ], [ "Semertzidis", "Y.", "" ], [ "Abel", "S.", "" ], [ "Albino", "S.", "" ], [ "Antusch", "S.", "" ], [ "Arganda", "E.", "" ], [ "Bajc", "B.", "" ], [ "Banerjee", "S.", "" ], [ "Biggio", "C.", "" ], [ "Blanke", "M.", "" ], [ "Bonivento", "W.", "" ], [ "Branco", "G. C.", "" ], [ "Bryman", "D.", "" ], [ "Buras", "A. J.", "" ], [ "Calibbi", "L.", "" ], [ "Ceccucci", "A.", "" ], [ "Chankowski", "P. H.", "" ], [ "Davidson", "S.", "" ], [ "Deandrea", "A.", "" ], [ "DeMille", "D. P.", "" ], [ "Deppisch", "F.", "" ], [ "Diaz", "M.", "" ], [ "Duling", "B.", "" ], [ "Felcini", "M.", "" ], [ "Fetscher", "W.", "" ], [ "Ghosh", "D. K.", "" ], [ "Giffels", "M.", "" ], [ "Giudice", "G.", "" ], [ "Goudzovskij", "E.", "" ], [ "Han", "T.", "" ], [ "Harris", "P. G.", "" ], [ "Herrero", "M. J.", "" ], [ "Hisano", "J.", "" ], [ "Holt", "R. J.", "" ], [ "Huitu", "K.", "" ], [ "Ibarra", "A.", "" ], [ "Igonkina", "O.", "" ], [ "Ilakovac", "A.", "" ], [ "Imazato", "J.", "" ], [ "Isidori", "G.", "" ], [ "Joaquim", "F. R.", "" ], [ "Kadastik", "M.", "" ], [ "Kajiyama", "Y.", "" ], [ "King", "S. F.", "" ], [ "Kirch", "K.", "" ], [ "Kozlov", "M. G.", "" ], [ "Krawczyk", "M.", "" ], [ "Kress", "T.", "" ], [ "Lebedev", "O.", "" ], [ "Lusiani", "A.", "" ], [ "Ma", "E.", "" ], [ "Marchiori", "G.", "" ], [ "Masina", "I.", "" ], [ "Moreau", "G.", "" ], [ "Mori", "T.", "" ], [ "Muntel", "M.", "" ], [ "Nesti", "F.", "" ], [ "Onderwater", "C. J. G.", "" ], [ "Paradisi", "P.", "" ], [ "Petcov", "S. T.", "" ], [ "Picariello", "M.", "" ], [ "Porretti", "V.", "" ], [ "Poschenrieder", "A.", "" ], [ "Pospelov", "M.", "" ], [ "Rebane", "L.", "" ], [ "Rebelo", "M. N.", "" ], [ "Ritz", "A.", "" ], [ "Roberts", "L.", "" ], [ "Romanino", "A.", "" ], [ "Rossi", "A.", "" ], [ "Rueckl", "R.", "" ], [ "Senjanovic", "G.", "" ], [ "Serra", "N.", "" ], [ "Shindou", "T.", "" ], [ "Takanishi", "Y.", "" ], [ "Tarantino", "C.", "" ], [ "Teixeira", "A. M.", "" ], [ "Torrente-Lujan", "E.", "" ], [ "Turzynski", "K. J.", "" ], [ "Underwood", "T. E. J.", "" ], [ "Vempati", "S. K.", "" ], [ "Vives", "O.", "" ] ]
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801.1827
Cindy Regal
C. A. Regal, J. D. Teufel, and K. W. Lehnert
Measuring nanomechanical motion with a microwave cavity interferometer
Minor changes and corrections to text and figures; 7 pages, 6 figures
Nature Physics 4, 555 (2008)
null
null
quant-ph cond-mat.other
null
In recent years microfabricated microwave cavities have been extremely successful in a wide variety of detector applications. In this article we focus this technology on the challenge of quantum-limited displacement detection of a macroscopic object. We measure the displacement of a nanomechanical beam by capacitively coupling its position to the resonant frequency of a superconducting transmission-line microwave cavity. With our device we realize near state-of-the-art mechanical force sensitivity (3 $\rm{aN/\sqrt{Hz}}$) and thus add to only a handful of techniques able to measure thermomechanical motion at 10's of milliKelvin temperatures. Our measurement imprecision reaches a promising 30 times the expected imprecision at the standard quantum limit, and we quantify our ability to extract measurement backaction from our results as well as elucidate the important steps that will be required to progress towards the full quantum limit with this new detector.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:40:13 GMT" }, { "version": "v2", "created": "Mon, 7 Apr 2008 17:37:41 GMT" } ]
2009-09-29T00:00:00
[ [ "Regal", "C. A.", "" ], [ "Teufel", "J. D.", "" ], [ "Lehnert", "K. W.", "" ] ]
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801.1828
Jacob Lund Fisker
R.D. Hoffman, J.L. Fisker, J. Pruet, S.E. Woosley, H.-T. Janka, R. Buras
Nucleosynthesis in Early Neutrino Driven Winds
4 pages, 4 figures, proceedings for CNR 2007 Compound-Nuclear Reactions and Related Topics Workshop
AIP Conf.Proc.1005:225-228,2008
10.1063/1.2920736
null
astro-ph
null
Nucleosynthesis in early neutrino winds is investigated. Presented is a brief overview of two recent problems of supernova nucleosynthesis. In the first part we investigate the effect of nuclear parameters on the synthesis of Mo92 and Mo94. Based on recent experimental results, we find that the proton rich winds of the model investigated here can not be the source of solar Mo92 and Mo94. In the second part we investigate the nucleosynthesis from neutron rich bubbles and show that they do not contribute to the overall nucleosynthesis.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:32:25 GMT" } ]
2010-12-13T00:00:00
[ [ "Hoffman", "R. D.", "" ], [ "Fisker", "J. L.", "" ], [ "Pruet", "J.", "" ], [ "Woosley", "S. E.", "" ], [ "Janka", "H. -T.", "" ], [ "Buras", "R.", "" ] ]
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801.1829
Thomas Creutzig
Thomas Creutzig, Alexander Klauer, Nils R. Scheithauer
Natural constructions of some generalized Kac-Moody algebras as bosonic strings
22 pages; published in Comm. Number Theory Phys. 1 (2007), 453-477
Commun.Num.Theor.Phys.1:453-477,2007
null
null
math.NT math-ph math.MP
null
There are 10 generalized Kac-Moody algebras whose denominator identities are completely reflective automorphic products of singular weight on lattices of squarefree level. Under the assumption that the meromorphic vertex operator algebra of central charge 24 and spin-1 algebra $\hat{A}_{p-1,p}^r$ exists we show that four of them can be constructed in a uniform way from bosonic strings moving on suitable target spaces.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:44:13 GMT" } ]
2009-03-24T00:00:00
[ [ "Creutzig", "Thomas", "" ], [ "Klauer", "Alexander", "" ], [ "Scheithauer", "Nils R.", "" ] ]
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801.183
Xicheng Zhang
Jiagang Ren, Xicheng Zhang
Freidlin-Wentzell's Large Deviations for Stochastic Evolution Equations
17Pages
null
null
null
math.PR math.DS
null
We prove a Freidlin-Wentzell large deviation principle for general stochastic evolution equations with small perturbation multiplicative noises. In particular, our general result can be used to deal with a large class of quasi linear stochastic partial differential equations, such as stochastic porous medium equations and stochastic reaction diffusion equations with polynomial growth zero order term and $p$-Laplacian second order term.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 19:50:12 GMT" } ]
2008-01-14T00:00:00
[ [ "Ren", "Jiagang", "" ], [ "Zhang", "Xicheng", "" ] ]
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801.1831
Howard Baer
Howard Baer, Sabine Kraml, Sezen Sekmen and Heaya Summy
Dark matter allowed scenarios for Yukawa-unified SO(10) SUSY GUTs
35 pages with 21 eps figures
JHEP0803:056,2008
10.1088/1126-6708/2008/03/056
FSU-HEP-071225, LPSC 07-195
hep-ph
null
Simple supersymmetric grand unified models based on the gauge group SO(10) require --in addition to gauge and matter unification-- the unification of t-b-\tau Yukawa couplings. Yukawa unification, however, only occurs for very special values of the soft SUSY breaking parameters. We perform a search using a Markov Chain Monte Carlo (MCMC) technique to investigate model parameters and sparticle mass spectra which occur in Yukawa-unified SUSY models, where we also require the relic density of neutralino dark matter to saturate the WMAP-measured abundance. We find the spectrum is characterizd by three mass scales: first/second generation scalars in the multi-TeV range, third generation scalars in the TeV range, and gauginos in the \sim 100 GeV range. Most solutions give far too high a relic abundance of neutralino dark matter. The dark matter discrepancy can be rectified by 1. allowing for neutralino decay to axino plus photon, 2. imposing gaugino mass non-universality or 3. imposing generational non-universality. In addition, the MCMC approach finds 4. a compromise solution where scalar masses are not too heavy, and where neutralino annihilation occurs via the light Higgs h resonance. By imposing weak scale Higgs soft term boundary conditions, we are also able to generate 5. low \mu, m_A solutions with neutralino annihilation via a light A resonance, though these solutions seem to be excluded by CDF/D0 measurements of the B_s\to \mu^+\mu^- branching fraction. Based on the dual requirements of Yukawa coupling unification and dark matter relic density, we predict new physics signals at the LHC from pair production of 350--450 GeV gluinos. The events are characterized by very high b-jet multiplicity and a dilepton mass edge around mz2-mz1 \sim 50-75 GeV.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 18:15:02 GMT" }, { "version": "v2", "created": "Wed, 5 Mar 2008 20:23:50 GMT" } ]
2008-11-26T00:00:00
[ [ "Baer", "Howard", "" ], [ "Kraml", "Sabine", "" ], [ "Sekmen", "Sezen", "" ], [ "Summy", "Heaya", "" ] ]
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801.1832
Greg Bell
Gregory C. Bell and Alexander Dranishnikov
Mapping class groups have finite asymptotic dimension
Withdrawn due to a critical error in Theorem 3 of [5] on which the main result relied
null
null
null
math.GR math.GT
null
By recognizing them as fundamental groups of developable complexes of groups we prove that mapping class groups of compact orientable surfaces have finite asymptotic dimension.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:10:10 GMT" }, { "version": "v2", "created": "Tue, 22 Jan 2008 19:13:53 GMT" } ]
2008-01-22T00:00:00
[ [ "Bell", "Gregory C.", "" ], [ "Dranishnikov", "Alexander", "" ] ]
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801.1833
Michelangelo Mangano
G. Buchalla, T.K. Komatsubara, F. Muheim, L. Silvestrini, M. Artuso, D.M. Asner, P. Ball, E. Baracchini, G. Bell, M. Beneke, J. Berryhill, A. Bevan, I.I. Bigi, M. Blanke, Ch. Bobeth, M. Bona, F. Borzumati, T. Browder, T. Buanes, O. Buchmuller, A.J. Buras, S. Burdin, D.G. Cassel, R. Cavanaugh, M. Ciuchini, P. Colangelo, G. Crosetti, A. Dedes, F. De Fazio, S. Descotes-Genon, J. Dickens, Z. Dolezal, S. Durr, U. Egede, C. Eggel, G. Eigen, S. Fajfer, Th. Feldmann, R. Ferrandes, P. Gambino, T. Gershon, V. Gibson, M. Giorgi, V.V. Gligorov, B. Golob, A. Golutvin, Y. Grossman, D. Guadagnoli, U. Haisch, M. Hazumi, S. Heinemeyer, G. Hiller, D. Hitlin, T. Huber, T. Hurth, T. Iijima, A. Ishikawa, G. Isidori, S. Jager, A. Khodjamirian, P. Koppenburg, T. Lagouri, U. Langenegger, C. Lazzeroni, A. Lenz, V. Lubicz, W. Lucha, H. Mahlke, D. Melikhov, F. Mescia, M. Misiak, M. Nakao, J. Napolitano, N. Nikitin, U. Nierste, K. Oide, Y. Okada, P. Paradisi, F. Parodi, M. Patel, A.A. Petrov, T.N. Pham, M. Pierini, S. Playfer, G. Polesello, A. Policicchio, A. Poschenrieder, P. Raimondi, S. Recksiegel, P. Reznicek, A. Robert, S. Robertson, J.L. Rosner, G. Ruggiero, A. Sarti, O. Schneider, F. Schwab, S. Simula, S. Sivoklokov, P. Slavich, C. Smith, M. Smizanska, A. Soni, T. Speer, P. Spradlin, M. Spranger, A. Starodumov, B. Stech, A. Stocchi, S. Stone, C. Tarantino, F. Teubert, S. T'Jampens, K. Toms, K. Trabelsi, S. Trine, S. Uhlig, V. Vagnoni, J.J. van Hunen, G. Weiglein, A. Weiler, G. Wilkinson, Y. Xie, M. Yamauchi, G. Zhu, J. Zupan, R. Zwicky
B, D and K decays
Report of Working Group 2 of the CERN Workshop ``Flavour in the era of the LHC'', Geneva, Switzerland, November 2005 -- March 2007
Eur.Phys.J.C57:309-492,2008
10.1140/epjc/s10052-008-0716-1
null
hep-ph hep-ex
null
With the advent of the LHC, we will be able to probe New Physics (NP) up to energy scales almost one order of magnitude larger than it has been possible with present accelerator facilities. While direct detection of new particles will be the main avenue to establish the presence of NP at the LHC, indirect searches will provide precious complementary information, since most probably it will not be possible to measure the full spectrum of new particles and their couplings through direct production. In particular, precision measurements and computations in the realm of flavour physics are expected to play a key role in constraining the unknown parameters of the Lagrangian of any NP model emerging from direct searches at the LHC. The aim of Working Group 2 was twofold: on one hand, to provide a coherent, up-to-date picture of the status of flavour physics before the start of the LHC; on the other hand, to initiate activities on the path towards integrating information on NP from high-pT and flavour data.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:14:51 GMT" } ]
2010-05-27T00:00:00
[ [ "Buchalla", "G.", "" ], [ "Komatsubara", "T. K.", "" ], [ "Muheim", "F.", "" ], [ "Silvestrini", "L.", "" ], [ "Artuso", "M.", "" ], [ "Asner", "D. M.", "" ], [ "Ball", "P.", "" ], [ "Baracchini", "E.", "" ], [ "Bell", "G.", "" ], [ "Beneke", "M.", "" ], [ "Berryhill", "J.", "" ], [ "Bevan", "A.", "" ], [ "Bigi", "I. I.", "" ], [ "Blanke", "M.", "" ], [ "Bobeth", "Ch.", "" ], [ "Bona", "M.", "" ], [ "Borzumati", "F.", "" ], [ "Browder", "T.", "" ], [ "Buanes", "T.", "" ], [ "Buchmuller", "O.", "" ], [ "Buras", "A. J.", "" ], [ "Burdin", "S.", "" ], [ "Cassel", "D. G.", "" ], [ "Cavanaugh", "R.", "" ], [ "Ciuchini", "M.", "" ], [ "Colangelo", "P.", "" ], [ "Crosetti", "G.", "" ], [ "Dedes", "A.", "" ], [ "De Fazio", "F.", "" ], [ "Descotes-Genon", "S.", "" ], [ "Dickens", "J.", "" ], [ "Dolezal", "Z.", "" ], [ "Durr", "S.", "" ], [ "Egede", "U.", "" ], [ "Eggel", "C.", "" ], [ "Eigen", "G.", "" ], [ "Fajfer", "S.", "" ], [ "Feldmann", "Th.", "" ], [ "Ferrandes", "R.", "" ], [ "Gambino", "P.", "" ], [ "Gershon", "T.", "" ], [ "Gibson", "V.", "" ], [ "Giorgi", "M.", "" ], [ "Gligorov", "V. V.", "" ], [ "Golob", "B.", "" ], [ "Golutvin", "A.", "" ], [ "Grossman", "Y.", "" ], [ "Guadagnoli", "D.", "" ], [ "Haisch", "U.", "" ], [ "Hazumi", "M.", "" ], [ "Heinemeyer", "S.", "" ], [ "Hiller", "G.", "" ], [ "Hitlin", "D.", "" ], [ "Huber", "T.", "" ], [ "Hurth", "T.", "" ], [ "Iijima", "T.", "" ], [ "Ishikawa", "A.", "" ], [ "Isidori", "G.", "" ], [ "Jager", "S.", "" ], [ "Khodjamirian", "A.", "" ], [ "Koppenburg", "P.", "" ], [ "Lagouri", "T.", "" ], [ "Langenegger", "U.", "" ], [ "Lazzeroni", "C.", "" ], [ "Lenz", "A.", "" ], [ "Lubicz", "V.", "" ], [ "Lucha", "W.", "" ], [ "Mahlke", "H.", "" ], [ "Melikhov", "D.", "" ], [ "Mescia", "F.", "" ], [ "Misiak", "M.", "" ], [ "Nakao", "M.", "" ], [ "Napolitano", "J.", "" ], [ "Nikitin", "N.", "" ], [ "Nierste", "U.", "" ], [ "Oide", "K.", "" ], [ "Okada", "Y.", "" ], [ "Paradisi", "P.", "" ], [ "Parodi", "F.", "" ], [ "Patel", "M.", "" ], [ "Petrov", "A. A.", "" ], [ "Pham", "T. N.", "" ], [ "Pierini", "M.", "" ], [ "Playfer", "S.", "" ], [ "Polesello", "G.", "" ], [ "Policicchio", "A.", "" ], [ "Poschenrieder", "A.", "" ], [ "Raimondi", "P.", "" ], [ "Recksiegel", "S.", "" ], [ "Reznicek", "P.", "" ], [ "Robert", "A.", "" ], [ "Robertson", "S.", "" ], [ "Rosner", "J. L.", "" ], [ "Ruggiero", "G.", "" ], [ "Sarti", "A.", "" ], [ "Schneider", "O.", "" ], [ "Schwab", "F.", "" ], [ "Simula", "S.", "" ], [ "Sivoklokov", "S.", "" ], [ "Slavich", "P.", "" ], [ "Smith", "C.", "" ], [ "Smizanska", "M.", "" ], [ "Soni", "A.", "" ], [ "Speer", "T.", "" ], [ "Spradlin", "P.", "" ], [ "Spranger", "M.", "" ], [ "Starodumov", "A.", "" ], [ "Stech", "B.", "" ], [ "Stocchi", "A.", "" ], [ "Stone", "S.", "" ], [ "Tarantino", "C.", "" ], [ "Teubert", "F.", "" ], [ "T'Jampens", "S.", "" ], [ "Toms", "K.", "" ], [ "Trabelsi", "K.", "" ], [ "Trine", "S.", "" ], [ "Uhlig", "S.", "" ], [ "Vagnoni", "V.", "" ], [ "van Hunen", "J. J.", "" ], [ "Weiglein", "G.", "" ], [ "Weiler", "A.", "" ], [ "Wilkinson", "G.", "" ], [ "Xie", "Y.", "" ], [ "Yamauchi", "M.", "" ], [ "Zhu", "G.", "" ], [ "Zupan", "J.", "" ], [ "Zwicky", "R.", "" ] ]
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801.1834
Shaun Mosley
Shaun N. Mosley
Non-dispersive wavepacket solutions of the Schrodinger equation
12 pages, parameters amended to yield correct dimension and new section added on relativistic extension
null
10.1088/1751-8113/41/26/265305
null
quant-ph
null
The free Schrodinger equation has constant velocity wavepacket solutions \psi_{\bf v} of the form \psi= f({\bf r} - {\bf v}t) e^{- i m c^2 t / 2}. These solutions are eigenvectors of a momentum operator {\bf \tilde p} which is symmetric in a positive definite scalar product space. We discuss whether these \psi_{\bf v} can act as basis states rather than the usual plane wave solutions.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:30:48 GMT" }, { "version": "v2", "created": "Wed, 16 Jan 2008 20:42:15 GMT" }, { "version": "v3", "created": "Mon, 21 Jan 2008 19:49:58 GMT" }, { "version": "v4", "created": "Wed, 23 Jan 2008 20:52:08 GMT" }, { "version": "v5", "created": "Fri, 1 Feb 2008 20:43:37 GMT" } ]
2009-11-13T00:00:00
[ [ "Mosley", "Shaun N.", "" ] ]
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801.1835
Ricardo Paszko
Ricardo Paszko
Semiclassical and Effective Theories of Gravitation
58 pages, 3 figures, Ph.D. Thesis (Advisor: Antonio Accioly), in portuguese, uses axodraw
null
null
IFT-T.003/06
gr-qc
null
First and second order corrections for the scattering of different types of particles by a weak gravitational field, treated as an external field, are calculated. These computations indicate a violation of the Equivalence Principle: to first order, the cross-sections are spin dependent; if the calculations are pushed to the next order, they become dependent upon energy as well. Interesting enough, the aforementioned results are equivalent to those obtained by means of the so-called Effective Theory of Gravitation, in the limit in which one of the masses is much greater than all the other energies involved. We discuss also some applications of our research, such as the determination of an upper bound for the photon mass, and the possible detection, in the foreseeable future, of these violations of the Equivalence Principle.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:47:28 GMT" }, { "version": "v2", "created": "Tue, 15 Jan 2008 19:21:10 GMT" } ]
2008-01-15T00:00:00
[ [ "Paszko", "Ricardo", "" ] ]
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801.1836
Elisabeth Nicol
E.J. Nicol and J.P. Carbotte
Optical conductivity of bilayer graphene with and without an asymmetry gap
final accepted version for PRB, added discussion and typos fixed
Phys. Rev. B vol. 77, 155409 (2008)
10.1103/PhysRevB.77.155409
null
cond-mat.mes-hall cond-mat.str-el
null
When a bilayer of graphene is placed in a suitably configured field effect device, an asymmetry gap can be generated and the carrier concentration made different in each layer. This provides a tunable semiconducting gap, and the valence and the conductance band no longer meet at the two Dirac points of the graphene Brillouin zone. We calculate the optical conductivity of such a semiconductor with particular emphasis on the optical spectral weight redistribution brought about by changes in gap and chemical potential due to charging. We derive an algebraic formula for arbitrary value of the chemical potential for the case of the bilayer conductivity without a gap.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:52:48 GMT" }, { "version": "v2", "created": "Mon, 17 Mar 2008 18:58:29 GMT" } ]
2009-11-13T00:00:00
[ [ "Nicol", "E. J.", "" ], [ "Carbotte", "J. P.", "" ] ]
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801.1837
Andrey Chubukov
Andrey V. Chubukov, Dmitrii L. Maslov, and Fabian H.L. Essler
A test of the g-ology model for one-dimensional interacting Fermi systems
4 pp, 1 fig, submitted to PRB RC
null
10.1103/PhysRevB.77.161102
null
cond-mat.str-el
null
Bosonization predicts that the specific heat, C(T), of a one-dimensional interacting Fermi system is a sum of the specific heats of free collective charge and spin excitations, plus the term with the running backscattering amplitude which flows to zero logarithmically with decreasing T. We verify whether this result is reproduced in the g-ology model. Of specific interest are the anomalous terms in C(T) that depend on the bare backscattering amplitude. We show that these terms can be incorporated into a renormalized spin velocity. We do this by proving the equivalence of the results for C(T) obtained within the g-ology model and by bosonization with velocities obtained by the numerical solution of the Bethe-ansatz equations for the Hubbard model.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:53:44 GMT" } ]
2009-11-13T00:00:00
[ [ "Chubukov", "Andrey V.", "" ], [ "Maslov", "Dmitrii L.", "" ], [ "Essler", "Fabian H. L.", "" ] ]
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801.1838
Inanc Sahin
I. Sahin
Rare decay Z \to \nu\bar{\nu}\gamma\gamma via tensor unparticle mediation
10 pages, 2 figures
Chinese Jour. of Phys. 47, 20-26 (2009)
null
null
hep-ph
null
The decay width of the rare decay Z \to \nu\bar{\nu}\gamma\gamma is strictly constrained from the LEP data. Tensor unparticles provide a tree-level contribution to this rare decay. We have calculated the tensor unparticle contribution to the rare decay Z\to \nu\bar{\nu}\gamma\gamma. The current experimental limit have been used to constrain unparticle couplings \nu\bar{\nu}Z {U}^{\mu\nu} and \gamma\gamma {U}^{\mu\nu}.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:55:52 GMT" }, { "version": "v2", "created": "Mon, 14 Jan 2008 21:40:14 GMT" } ]
2012-12-19T00:00:00
[ [ "Sahin", "I.", "" ] ]
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801.1839
Shabnam Safaei
Shabnam Safaei, Simone Montangero, Fabio Taddei and Rosario Fazio
Optimized Cooper pair pumps
9 pages, 10 figures
Phys. Rev. B 77, 144522 (2008)
10.1103/PhysRevB.77.144522
null
cond-mat.mes-hall cond-mat.other
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
In adiabatic Cooper pair pumps, operated by means of gate voltage modulation only, the quantization of the pumped charge during a cycle is limited due to the quantum coherence of the macroscopic superconducting wave function. In this work we show that it is possible to obtain very accurate pumps in the non-adiabatic regime by a suitable choice of the shape of the gate voltage pulses. We determine the shape of these pulses by applying quantum optimal control theory to this problem. In the optimal case the error, with respect to the quantized value, can be as small as of the order of (10E-6)e: the error is reduced by up to five orders of magnitude with respect to the adiabatic pumping. In order to test the experimental feasibility of this approach we consider the effect of charge noise and the deformations of the optimal pulse shapes on the accuracy of the pump. Charge noise is assumed to be induced by random background charges in the substrate, responsible for the observed 1/f noise. Inaccuracies in the pulse shaping are described by assuming a finite bandwidth for the pulse generator. In realistic cases the error increases at most of one order of magnitude as compared to the optimal case. Our results are promising for the realization of accurate and fast superconducting pumps.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:59:12 GMT" }, { "version": "v2", "created": "Mon, 24 Nov 2008 14:35:33 GMT" } ]
2010-09-08T00:00:00
[ [ "Safaei", "Shabnam", "" ], [ "Montangero", "Simone", "" ], [ "Taddei", "Fabio", "" ], [ "Fazio", "Rosario", "" ] ]
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801.184
Louis-Francois Arsenault
Louis-Francois Arsenault, B. Movaghar, P. Desjardins and A. Yelon
Transport in the metallic regime of Mn doped III-V Semiconductors
submitted to Phys. Rev. B
Phys. Rev. B 77, 115211 (2008)
10.1103/PhysRevB.77.115211
null
cond-mat.mtrl-sci
null
The standard model of Mn doping in GaAs is subjected to a coherent potential approximation (CPA) treatment. Transport coefficients are evaluated within the linear response Kubo formalism. Both normal (NHE) and anomalous contributions (AHE) to the Hall effect are examined. We use a simple model density of states to describe the undoped valence band. The CPA bandstructure evolves into a spin split band caused by the $p-d$ exchange scattering with Mn dopants. This gives rise to a strong magnetoresistance, which decreases sharply with temperature. The temperature ($T$) dependence of the resistance is due to spin disorder scattering (increasing with $T$), CPA bandstructure renormalization and charged impurity scattering (decreasing with $T$). The calculated transport coefficients are discussed in relation to experiment, with a view of assessing the overall trends and deciding whether the model describes the right physics. This does indeed appear to be case, bearing in mind that the hopping limit needs to be treated separately, as it cannot be described within the band CPA.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:59:23 GMT" } ]
2009-11-13T00:00:00
[ [ "Arsenault", "Louis-Francois", "" ], [ "Movaghar", "B.", "" ], [ "Desjardins", "P.", "" ], [ "Yelon", "A.", "" ] ]
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801.1841
Guillermo Torres
G. Torres (CfA), J. N. Winn (MIT), M. J. Holman (CfA)
Improved parameters for extrasolar transiting planets
To appear in The Astrophysical Journal. 23 pages in emulateapj format, including figures and tables. Figures 7, 8, and 9 are low resolution; higher resolution versions will be available from the journal when published. Acknowledgement added, and minor changes made to TrES-3 and TrES-4 in the Appendix
null
10.1086/529429
null
astro-ph
null
We present refined values for the physical parameters of transiting exoplanets, based on a self-consistent and uniform analysis of transit light curves and the observable properties of the host stars. Previously it has been difficult to interpret the ensemble properties of transiting exoplanets, because of the widely different methodologies that have been applied in individual cases. Furthermore, previous studies often ignored an important constraint on the mean stellar density that can be derived directly from the light curve. The main contributions of this work are 1) a critical compilation and error assessment of all reported values for the effective temperature and metallicity of the host stars; 2) the application of a consistent methodology and treatment of errors in modeling the transit light curves; and 3) more accurate estimates of the stellar mass and radius based on stellar evolution models, incorporating the photometric constraint on the stellar density. We use our results to revisit some previously proposed patterns and correlations within the ensemble. We confirm the mass-period correlation, and we find evidence for a new pattern within the scatter about this correlation: planets around metal-poor stars are more massive than those around metal-rich stars at a given orbital period. Likewise, we confirm the proposed dichotomy of planets according to their Safronov number, and we find evidence that the systems with small Safronov numbers are more metal-rich on average. Finally, we confirm the trend that led to the suggestion that higher-metallicity stars harbor planets with a greater heavy-element content.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 20:59:55 GMT" }, { "version": "v2", "created": "Fri, 11 Jan 2008 21:06:38 GMT" }, { "version": "v3", "created": "Wed, 16 Jan 2008 18:20:42 GMT" } ]
2009-11-13T00:00:00
[ [ "Torres", "G.", "", "CfA" ], [ "Winn", "J. N.", "", "MIT" ], [ "Holman", "M. J.", "", "CfA" ] ]
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801.1842
Duncan Farrah
D. Farrah (Cornell), C. Lonsdale (Virginia), D. Weedman (Cornell), H. Spoon (Cornell), M. Rowan-Robinson (Imperial College), M. Polletta (Institut d'Astrophysique de Paris), S. Oliver (Sussex), J. R. Houck (Cornell), H. E. Smith (UCSD)
The nature of star formation in distant ultraluminous infrared galaxies selected in a remarkably narrow redshift range
ApJ accepted. Higher quality figures available on request
null
10.1086/529485
null
astro-ph
null
We present mid-infrared spectra of thirty two high redshift ultraluminous infrared galaxies, selected via the stellar photospheric feature at rest-frame 1.6um, and an observed-frame 24um flux of >500muJy. Nearly all the sample reside in a redshift range of <z>=1.71+/-0.15, and have rest-frame 1-1000um luminosities of 10^12.9 - 10^13.8 Lsun. Most of the spectra exhibit prominent polycyclic aromatic hydrocarbon emission features, and weak silicate absorption, consistent with a starburst origin for the IR emission. Our selection method appears to be a straightforward and efficient way of finding distant, IR-luminous, star-forming galaxies in narrow redshift ranges. There is however evidence that the mid-IR spectra of our sample differ systematically from those of local ULIRGs; our sample have comparable PAH equivalent widths but weaker apparent silicate absorption, and (possibly) enhanced PAH 6.2um/7.7um and 6.2um/11.2um flux ratios. Furthermore, the composite mid-IR spectrum of our sample is almost identical to that of local starbursts with IR luminosities of 10^10-10^11 Lsun rather than that of local ULIRGs. These differences are consistent with a reduced dust column, which can plausibly be obtained via some combination of (1) star formation that is extended over spatial scales of 1-4Kpc, and (2) star formation in unusually gas-rich regions.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:00:04 GMT" } ]
2009-11-13T00:00:00
[ [ "Farrah", "D.", "", "Cornell" ], [ "Lonsdale", "C.", "", "Virginia" ], [ "Weedman", "D.", "", "Cornell" ], [ "Spoon", "H.", "", "Cornell" ], [ "Rowan-Robinson", "M.", "", "Imperial College" ], [ "Polletta", "M.", "", "Institut\n d'Astrophysique de Paris" ], [ "Oliver", "S.", "", "Sussex" ], [ "Houck", "J. R.", "", "Cornell" ], [ "Smith", "H. E.", "", "UCSD" ] ]
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801.1843
Xi Kang
X. Kang, Frank C. van den Bosch
New Constraints on the Efficiencies of Ram-Pressure Stripping and the Tidal Disruption of Satellite Galaxies
A few discussions added, updated to match the accepted version to ApJ Letters
Astrophys.J.676:L101-L104,2008
10.1086/587620
null
astro-ph
null
Using data from the Sloan Digital Sky Survey (SDSS) it has recently been shown that the red fraction of satellite galaxies increases with stellar mass. Semi-analytical models, however, predict red satellite fractions that are independent of stellar mass, and much higher than observed. It has been argued that this discrepancy owes to the fact that the models assume that satellite galaxies are instantaneously stripped of their hot gas reservoirs at the moment they are accreted into a bigger halo. In this letter we show that the fraction of red satellites can be brought in better agreement with the data by simply decreasing this stripping efficiency. However, this also results in a red fraction of massive centrals that is much too low. This owes to the fact that the massive centrals now accrete satellite galaxies that are bluer and more gas-rich. However, if a significant fraction of low mass satellite galaxies is tidally disrupted before being accreted by their central host galaxy, as suggested by recent studies, the red fractions of both centrals and satellites can be reproduced reasonably well. A problem remains with the red fraction of centrals of intermediate mass, which is likely to reflect an oversimplified treatment of AGN feedback.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:10:16 GMT" }, { "version": "v2", "created": "Fri, 22 Feb 2008 18:44:13 GMT" } ]
2010-05-25T00:00:00
[ [ "Kang", "X.", "" ], [ "Bosch", "Frank C. van den", "" ] ]
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801.1844
Paul Bourdon
Paul S. Bourdon and Joel H. Shapiro
Adjoints of rationally induced composition operators
21 pages, Published Version
J. Functional Analysis 255 (2008), 1995-2012
null
null
math.FA math.CV
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We give an elementary proof of a formula recently obtained by Hammond, Moorhouse, and Robbins for the adjoint of a rationally induced composition operator on the Hardy space H^2. We discuss some variants and implications of this formula, and use it to provide a sufficient condition for a rationally induced composition operator adjoint to be a compact perturbation of a weighted composition operator.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:01:01 GMT" }, { "version": "v2", "created": "Fri, 20 Mar 2009 19:47:42 GMT" } ]
2009-03-20T00:00:00
[ [ "Bourdon", "Paul S.", "" ], [ "Shapiro", "Joel H.", "" ] ]
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801.1845
Martin Snoager Sloth
Antonio Riotto and Martin S. Sloth
On Resumming Inflationary Perturbations beyond One-loop
17 pages, v2: minor corrections, to appear in jcap
JCAP0804:030,2008
10.1088/1475-7516/2008/04/030
CERN-PH-TH/2008-006
hep-ph astro-ph hep-th
null
It is well known that the correlation functions of a scalar field in a quasi-de Sitter space exhibit at the loop level cumulative infra-red effects proportional to the total number of e-foldings of inflation. Using the in-in formalism, we explore the behavior of these infra-red effects in the large N limit of an O(N) invariant scalar field theory with quartic self-interactions. By resumming all higher-order loop diagrams non-perturbatively, we show that the connected four-point correlation function, which is a signal of non-Gaussianity, is non-perturbatively enhanced with respect to its tree-level value.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:19:58 GMT" }, { "version": "v2", "created": "Tue, 8 Apr 2008 11:13:34 GMT" } ]
2008-11-26T00:00:00
[ [ "Riotto", "Antonio", "" ], [ "Sloth", "Martin S.", "" ] ]
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801.1846
Alain Barrat
Aurelien Gautreau (LPT), Alain Barrat (LPT), Marc Barthelemy (CEA DIF/DPTA)
Global disease spread: statistics and estimation of arrival times
J. Theor. Biol., in press
Journal of Theoretical Biology 251 (2008) 509-522
10.1016/j.jtbi.2007.12.001
null
q-bio.PE cond-mat.stat-mech
null
We study metapopulation models for the spread of epidemics in which different subpopulations (cities) are connected by fluxes of individuals (travelers). This framework allows to describe the spread of a disease on a large scale and we focus here on the computation of the arrival time of a disease as a function of the properties of the seed of the epidemics and of the characteristics of the network connecting the various subpopulations. Using analytical and numerical arguments, we introduce an easily computable quantity which approximates this average arrival time. We show on the example of a disease spread on the world-wide airport network that this quantity predicts with a good accuracy the order of arrival of the disease in the various subpopulations in each realization of epidemic scenario, and not only for an average over realizations. Finally, this quantity might be useful in the identification of the dominant paths of the disease spread.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:05:18 GMT" } ]
2008-03-20T00:00:00
[ [ "Gautreau", "Aurelien", "", "LPT" ], [ "Barrat", "Alain", "", "LPT" ], [ "Barthelemy", "Marc", "", "CEA\n DIF/DPTA" ] ]
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801.1847
Stephen D. H. Hsu
Paul Frampton, Stephen D.H. Hsu, Thomas W. Kephart, David Reeb
What is the entropy of the universe?
5 pages, 3 figures, 1 table, revtex; v3: revised and expanded version, to appear in Class. Quant. Grav
Class.Quant.Grav.26:145005,2009
10.1088/0264-9381/26/14/145005
null
hep-th astro-ph gr-qc hep-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Standard calculations suggest that the entropy of our universe is dominated by black holes, whose entropy is of order their area in Planck units, although they comprise only a tiny fraction of its total energy. Statistical entropy is the logarithm of the number of microstates consistent with the observed macroscopic properties of a system, hence a measure of uncertainty about its precise state. Therefore, assuming unitarity in black hole evaporation, the standard results suggest that the largest uncertainty in the future quantum state of the universe is due to the Hawking radiation from evaporating black holes. However, the entropy of the matter precursors to astrophysical black holes is enormously less than that given by area entropy. If unitarity relates the future radiation states to the black hole precursor states, then the standard results are highly misleading, at least for an observer that can differentiate the individual states of the Hawking radiation.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:43:43 GMT" }, { "version": "v2", "created": "Thu, 15 May 2008 20:24:47 GMT" }, { "version": "v3", "created": "Fri, 29 May 2009 20:02:41 GMT" } ]
2009-09-17T00:00:00
[ [ "Frampton", "Paul", "" ], [ "Hsu", "Stephen D. H.", "" ], [ "Kephart", "Thomas W.", "" ], [ "Reeb", "David", "" ] ]
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801.1848
Gerald Seidler
T. T. Fister, G. T. Seidler, E. L. Shirley, F. D. Vila, J. J. Rehr, K. P. Nagle, J. C. Linehan, J. O. Cross
The local electronic structure of alpha-Li3N
34 pages, 7 figures, 1 table
null
10.1063/1.2949550
null
cond-mat.mtrl-sci
null
New theoretical and experimental investigation of the occupied and unoccupied local electronic density of states (DOS) are reported for alpha-Li3N. Band structure and density functional theory calculations confirm the absence of covalent bonding character. However, real-space full-multiple-scattering (RSFMS) calculations of the occupied local DOS finds less extreme nominal valences than have previously been proposed. Nonresonant inelastic x-ray scattering (NRIXS), RSFMS calculations, and calculations based on the Bethe-Salpeter equation are used to characterize the unoccupied electronic final states local to both the Li and N sites. There is good agreement between experiment and theory. Throughout the Li 1s near-edge region, both experiment and theory find strong similarities in the s- and p-type components of the unoccupied local final density of states projected onto an orbital angular momentum basis (l-DOS). An unexpected, significant correspondence exists between the near-edge spectra for the Li 1s and N 1s initial states. We argue that both spectra are sampling essentially the same final density of states due to the combination of long core-hole lifetimes, long photoelectron lifetimes, and the fact that orbital angular momentum is the same for all relevant initial states. Such considerations may be generically applicable for low atomic number compounds.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:07:01 GMT" } ]
2009-11-13T00:00:00
[ [ "Fister", "T. T.", "" ], [ "Seidler", "G. T.", "" ], [ "Shirley", "E. L.", "" ], [ "Vila", "F. D.", "" ], [ "Rehr", "J. J.", "" ], [ "Nagle", "K. P.", "" ], [ "Linehan", "J. C.", "" ], [ "Cross", "J. O.", "" ] ]
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801.1849
Lisa J. Kewley
Lisa J. Kewley (1), Sara L. Ellison (2) ((1) University of Hawaii, (2) University of Victoria)
Metallicity Calibrations and the Mass-Metallicity Relation for Star-Forming Galaxies
26 pages, 5 tables, 11 figures (reduced resolution); accepted for publication in the Astrophysical Journal. . A full resolution version can be downloaded in pdf form (1 Mb) from http://www.ifa.hawaii.edu/~kewley/Metallicity/ms.pdf
Astrophys.J.681:1183-1204,2008
10.1086/587500
null
astro-ph
null
(Abridged) We investigate the effect of metallicity calibrations, AGN classification, and aperture covering fraction on the local mass-metallicity (MZ) relation using 27,730 star-forming galaxies from the Sloan Digital Sky Survey (SDSS) Data Release 4. We analyse the SDSS MZ relation with 10 metallicity calibrations, including theoretical and empirical methods. We show that the choice of metallicity calibration has a significant effect on the shape and y-intercept(12+log(O/H)) of the MZ relation. The absolute metallicity scale (y-int) varies up to 0.7 dex, depending on the calibration used, and the change in shape is substantial. These results indicate that it is critical to use the same metallicity calibration when comparing different luminosity-metallicity or mass-metallicity relations. We present new metallicity conversions that allow metallicities that have been derived using different strong-line calibrations to be converted to the same base calibration. These conversions facilitate comparisons between different samples, particularly comparisons between galaxies at different redshifts for which different suites of emission-lines are available.Our new conversions successfully remove the large 0.7 dex discrepancies between the metallicity calibrations, and we reach agreement in the MZ relation to within 0.03 dex on average. We find that different AGN classification methods have negligible effect on the SDSS MZ relation. We compare the SDSS MZ relation with nuclear and global relations from the Nearby Field Galaxy Survey (NFGS). The turn over of the MZ relation depends on aperture covering fraction. We find that a lower redshift limit of z<0.04 is insufficient for avoiding aperture effects in fiber spectra of the highest stellar mass galaxies.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:07:04 GMT" } ]
2014-11-18T00:00:00
[ [ "Kewley", "Lisa J.", "" ], [ "Ellison", "Sara L.", "" ] ]
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801.185
Voisin Christophe
Christophe Voisin (LGIT), Jean-Robert Grasso (LGIT), Eric Larose (LGIT), Fran\c{c}ois Renard (LGIT)
Evolution of seismic signals and slip patterns along subduction zones: insights from a friction lab scale experiment
null
null
10.1029/2008GL033356
null
physics.geo-ph
null
Continuous GPS and broadband seismic monitoring have revealed a variety of disparate slip patterns especially in shallow dipping subduction zones, among which regular earthquakes, slow slip events and silent quakes1,2. Slow slip events are sometimes accompanied by Non Volcanic Tremors (NVT), which origin remains unclear3, either related to fluid migration or to friction. The present understanding of the whole menagerie of slip patterns is based upon numerical simulations imposing ad hoc values of the rate and state parameters a and b4-6 derived from the temperature dependence of a and b of a wet granite gouge7. Here we investigate the influence of the cumulative slip on the frictional and acoustic patterns of a lab scale subduction zone. Shallow loud earthquakes (stick-slip events), medium depth slow, deeper silent quakes (smooth sliding oscillations) and deepest steady-state creep (continuous sliding) are reproduced by the ageing of contact interface with cumulative displacement8. The Acoustic Emission evolves with cumulative displacement and interface ageing, following a trend from strong impulsive events, similar to earthquake seismic signals, to a collection of smaller amplitude and longer duration signals, similar to Non Volcanic Tremors. NVT emerge as the recollection of the local unstable behaviour of the contact interface globally evolving towards the stable sliding regime.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:08:14 GMT" } ]
2015-05-13T00:00:00
[ [ "Voisin", "Christophe", "", "LGIT" ], [ "Grasso", "Jean-Robert", "", "LGIT" ], [ "Larose", "Eric", "", "LGIT" ], [ "Renard", "François", "", "LGIT" ] ]
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801.1851
Steffen Knollmann
Steffen R. Knollmann, Chris Power and Alexander Knebe
Dark Matter Halo Profiles in Scale-Free Cosmologies
9 pages, 4 figures. Accepted for publication in MNRAS
null
10.1111/j.1365-2966.2008.12857.x
null
astro-ph
null
We explore the dependence of the central logarithmic slope of dark matter halo density profiles $\alpha$ on the spectral index $n$ of the linear matter power spectrum $P(k)$ using cosmological $N$-body simulations of scale-free models (i.e. $P(k) \propto k^n$). For each of our simulations we identify samples of well resolved haloes in dynamical equilibrium and we analyse their mass profiles. By parameterising the mass profile using a ``generalised'' Navarro, Frenk & White profile in which the central logarithmic slope $\alpha$ is allowed to vary while preserving the $r^{-3}$ asymptotic form at large radii, we obtain preferred central slopes for haloes in each of our models. There is a strong correlation between $\alpha$ and $n$, such that $\alpha$ becomes shallower as $n$ becomes steeper. However, if we normalise our mass profiles by $r_{-2}$, the radius at which the logarithmic slope of the density profile is -2, we find that these differences are no longer present. We conclude that there is no evidence for convergence to a unique central asymptotic slope, at least on the scales that we can resolve.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:09:41 GMT" } ]
2009-11-13T00:00:00
[ [ "Knollmann", "Steffen R.", "" ], [ "Power", "Chris", "" ], [ "Knebe", "Alexander", "" ] ]
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801.1852
Darren Williams
D.M. Williams, E. Gaidos
Detecting the Glint of Starlight on the Oceans of Distant Planets
41 pages, 7 figures. Icarus in press
null
10.1016/j.icarus.2008.01.002
null
astro-ph
null
We propose that astronomers will be eventually be able to discriminate between extrasolar Earth-like planets with surface oceans and those without using the shape of phase light curves in the visible and near-IR spectrum. We model the visible light curves of planets having Earth-like surfaces, seasons, and optically-thin atmospheres with idealized diffuse-scattering clouds. We show that planets partially covered by water will appear measurably brighter near crescent phase (relative to Lambertian planets) because of the efficient specular reflection (i.e., glint) of starlight incident on their surfaces at a highly oblique angle. Planets on orbits within 30 degrees of edge-on orientation (half of all planets) will show pronounced glint over a sizeable range of orbital longitudes, from quadrature to crescent, all outside the glare of their parent stars. Also, water-covered planets will appear darker than a Lambertian disk near full illumination. Finally, we show that planets with a mixed land/water surface will polarize the reflected signal by as much as 30-70 percent. These results suggest several new ways of directly identifying water on distant planets.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:10:05 GMT" } ]
2009-11-13T00:00:00
[ [ "Williams", "D. M.", "" ], [ "Gaidos", "E.", "" ] ]
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801.1853
Gerald Seidler
T.T. Fister, K.P. Nagle, F.D. Vila, G.T. Seidler, C. Hamner, J.O. Cross, J.J. Rehr
Intermediate-Range Order in Water Ices
20 page, 4 figure. Submitted PRB
null
null
null
cond-mat.mtrl-sci
null
We report measurements of the non-resonant inelastic x-ray scattering (NRIXS) from the O 1s orbitals in ice Ih, and also report calculations of the corresponding spectra for ice Ih and several other phases of water ice. We find that the intermediate-energy fine structure may be calculated well using an ab initio real-space full multiple scattering approach, and that it provides a strong fingerprint of the intermediate-range order for some ice phases. These results have important consequences for future NRIXS measurements of high-pressure phases of ice and also may call into question the assumption that the wavefunctions for final states within a few eV of the absorption edge are strongly localized.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:12:26 GMT" } ]
2008-01-15T00:00:00
[ [ "Fister", "T. T.", "" ], [ "Nagle", "K. P.", "" ], [ "Vila", "F. D.", "" ], [ "Seidler", "G. T.", "" ], [ "Hamner", "C.", "" ], [ "Cross", "J. O.", "" ], [ "Rehr", "J. J.", "" ] ]
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801.1854
Andrew Tolley
Andrew J. Tolley, Mark Wyman
Stochastic Inflation Revisited: Non-Slow Roll Statistics and DBI Inflation
38 pages, 2 figures. v3: minor revisions; version accepted into JCAP
JCAP0804:028,2008
10.1088/1475-7516/2008/04/028
PI-COSMO-58
hep-th astro-ph gr-qc
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Stochastic inflation describes the global structure of the inflationary universe by modeling the super-Hubble dynamics as a system of matter fields coupled to gravity where the sub-Hubble field fluctuations induce a stochastic force into the equations of motion. The super-Hubble dynamics are ultralocal, allowing us to neglect spatial derivatives and treat each Hubble patch as a separate universe. This provides a natural framework in which to discuss probabilities on the space of solutions and initial conditions. In this article we derive an evolution equation for this probability for an arbitrary class of matter systems, including DBI and k-inflationary models, and discover equilibrium solutions that satisfy detailed balance. Our results are more general than those derived assuming slow roll or a quasi-de Sitter geometry, and so are directly applicable to models that do not satisfy the usual slow roll conditions. We discuss in general terms the conditions for eternal inflation to set in, and we give explicit numerical solutions of highly stochastic, quasi-stationary trajectories in the relativistic DBI regime. Finally, we show that the probability for stochastic/thermal tunneling can be significantly enhanced relative to the Hawking-Moss instanton result due to relativistic DBI effects.
[ { "version": "v1", "created": "Mon, 14 Jan 2008 20:16:52 GMT" }, { "version": "v2", "created": "Wed, 30 Jan 2008 00:18:11 GMT" }, { "version": "v3", "created": "Thu, 19 Jun 2008 14:52:43 GMT" } ]
2008-11-26T00:00:00
[ [ "Tolley", "Andrew J.", "" ], [ "Wyman", "Mark", "" ] ]
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801.1855
Alexander Volberg L
V. Eiderman, F. Nazarov, A. Volberg
Vector-valued Riesz potentials: Cartan type estimates and related capacities
33 pages
null
null
null
math.AP
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
There are many interesting problems about the electrostatic potential of finitely many charges. We consider one of them concerning the intensity of the field, in other words, about the magnitude of the gradient of this potential. We want to give a sharp estimate of the size of the set of points where this gradient is large. Of course we want the estimate to be sharp in number $N$ of charges. The size will be measured by the Hausdorff content with various gauge functions. Such a setting allows us to consider a wide class of measures (not necessarily with finitely many charges). The main technique will be Calder\'on-Zygmund capacities and nonhomogeneous Calder\'on-Zygmund operators. Here we establish a relationship between various types of capacities with singular kernels (e. g. analytic capacity, lipschitz harmonic capacity, etc) and non-linear capacity from the theory of potential \'a la Adams, Hedberg, Havin, Maz'ya, Wolff. "Capacitary" part of the paper extends the theorem of Mateu, Prat and Verdera [J. reine und angew. Math., 578 (2005), 201--223]. "Size estimates" part of the paper extends the theorem of M. Anderson and V. Eiderman [Annals of Math., 163 (2005), 1057--1076]. The difficulty lies in the fact that we cannot use Menger's curvature anymore because we are working in spaces of dimension bigger than two.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:20:49 GMT" }, { "version": "v2", "created": "Sat, 1 Nov 2008 17:29:37 GMT" } ]
2008-11-01T00:00:00
[ [ "Eiderman", "V.", "" ], [ "Nazarov", "F.", "" ], [ "Volberg", "A.", "" ] ]
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801.1856
Grenville Croll
David A. Banks, Ann Monday
Interpretation as a factor in understanding flawed spreadsheets
9 pages incuding references
Proc. European Spreadsheet Risks Int. Grp. 2002 13 21 ISBN 1 86166 182 7
null
null
cs.CY cs.HC
null
The spreadsheet has been used by the business community for many years and yet still raises a number of significant concerns. As educators our concern is to try to develop the students skills in both the development of spreadsheets and in taking a critical view of their potential defects. In this paper we consider both the problems of mechanical production and the problems of translation of problem to spreadsheet representation.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:47:01 GMT" } ]
2008-03-10T00:00:00
[ [ "Banks", "David A.", "" ], [ "Monday", "Ann", "" ] ]
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801.1857
Shailesh Chandrasekharan
D. J. Cecile and Shailesh Chandrasekharan
Absence of vortex condensation in a two dimensional fermionic XY model
5 pages, 5 figures
Phys.Rev.D77:054502,2008
10.1103/PhysRevD.77.054502
null
hep-lat
null
Motivated by a puzzle in the study of two dimensional lattice Quantum Electrodynamics with staggered fermions, we construct a two dimensional fermionic model with a global U(1) symmetry. Our model can be mapped into a model of closed packed dimers and plaquettes. Although the model has the same symmetries as the XY model, we show numerically that the model lacks the well known Kosterlitz-Thouless phase transition. The model is always in the gapless phase showing the absence of a phase with vortex condensation. In other words the low energy physics is described by a non-compact U(1) field theory. We show that by introducing an even number of layers one can introduce vortex condensation within the model and thus also induce a KT transition.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:50:21 GMT" } ]
2008-11-26T00:00:00
[ [ "Cecile", "D. J.", "" ], [ "Chandrasekharan", "Shailesh", "" ] ]
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801.1858
Pavel Bleher
Pavel M. Bleher
Lectures on random matrix models. The Riemann-Hilbert approach
84 pages, 23 figures, to appear in the CRM volume on "Random Matrices", Springer, 2008
null
null
null
math-ph math.MP
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
This is a review of the Riemann-Hilbert approach to the large $N$ asymptotics in random matrix models and its applications. We discuss the following topics: random matrix models and orthogonal polynomials, the Riemann-Hilbert approach to the large $N$ asymptotics of orthogonal polynomials and its applications to the problem of universality in random matrix models, the double scaling limits, the large $N$ asymptotics of the partition function, and random matrix models with external source.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 21:56:55 GMT" }, { "version": "v2", "created": "Thu, 26 Jun 2008 15:52:29 GMT" } ]
2008-06-26T00:00:00
[ [ "Bleher", "Pavel M.", "" ] ]
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801.1859
Maciej Nowak A.
Jean-Paul Blaizot and Maciej A. Nowak
Large N_c confinement and turbulence
4 pages, no figures- Some rewriting - Typos corrected - References completed and some corrected
Phys.Rev.Lett.101:102001,2008
10.1103/PhysRevLett.101.102001
null
hep-th hep-lat hep-ph
null
We suggest that the transition that occurs at large $N_c$ in the eigenvalue distribution of a Wilson loop may have a turbulent origin. We arrived at this conclusion by studying the complex-valued inviscid Burgers-Hopf equation that corresponds to the Makeenko-Migdal loop equation, and we demonstrate the appearance of a shock in the spectral flow of the Wilson loop eigenvalues. This picture supplements that of the Durhuus-Olesen transition with a particular realization of disorder. The critical behavior at the formation of the shock allows us to infer exponents that have been measured recently in lattice simulations by Narayanan and Neuberger in $d=2$ and $d=3$. Our analysis leads us to speculate that the universal behavior observed in these lattice simulations might be a generic feature of confinement, also in $d=4$ Yang-Mills theory.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:00:39 GMT" }, { "version": "v2", "created": "Sun, 24 Feb 2008 20:51:08 GMT" } ]
2008-11-26T00:00:00
[ [ "Blaizot", "Jean-Paul", "" ], [ "Nowak", "Maciej A.", "" ] ]
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801.186
Arjun Dey
Arjun Dey (1), B. T. Soifer (2), Vandana Desai (2), Kate Brand (3), Emeric LeFloc'h (4), Michael J. Brown (5), Buell T. Jannuzi (1), Lee Armus (2), Shane Bussmann (6), Mark Brodwin (1), Chao Bian (2), Peter Eisenhardt (7), Sarah Higdon (8), Daniel Weedman (9), Steve Willner (10) ((1) NOAO, (2) Caltech, (3) STScI, (4) U of Hawaii, (5) Monash, (6) U of Arizona, (7) JPL, (8) Georgia Southern U, (9) Cornell, (10) Harvard/CfA)
A Significant Population of Very Luminous Dust-Obscured Galaxies at Redshift z ~ 2
Accepted for publication in the Astrophysical Journal
null
10.1086/529516
null
astro-ph
null
Observations with Spitzer Space Telescope have recently revealed a significant population of high-redshift z~2 dust-obscured galaxies (DOGs) with large mid-IR to UV luminosity ratios. These galaxies have been missed in traditional optical studies of the distant universe. We present a simple method for selecting this high-z population based solely on the ratio of the observed mid-IR 24um to optical R-band flux density. In the 8.6 sq.deg Bootes NDWFS Field, we uncover ~2,600 DOG candidates (= 0.089/sq.arcmin) with 24um flux densities F24>0.3mJy and (R-[24])>14 (i.e., F[24]/F[R] > 1000). These galaxies have no counterparts in the local universe, and become a larger fraction of the population at fainter F24, representing 13% of the sources at 0.3~mJy. DOGs exhibit evidence of both star-formation and AGN activity, with the brighter 24um sources being more AGN- dominated. We have measured spectroscopic redshifts for 86 DOGs, and find a broad z distribution centered at <z>~2.0. Their space density is 2.82E-5 per cubic Mpc, similar to that of bright sub-mm-selected galaxies at z~2. These redshifts imply very large luminosities LIR>~1E12-14 Lsun. DOGs contribute ~45-100% of the IR luminosity density contributed by all z~2 ULIRGs, suggesting that our simple selection criterion identifies the bulk of z~2 ULIRGs. DOGs may be the progenitors of ~4L* present-day galaxies seen undergoing a luminous,short- lived phase of bulge and black hole growth. They may represent a brief evolution phase between SMGs and less obscured quasars or galaxies. [Abridged]
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:05:54 GMT" } ]
2009-11-13T00:00:00
[ [ "Dey", "Arjun", "" ], [ "Soifer", "B. T.", "" ], [ "Desai", "Vandana", "" ], [ "Brand", "Kate", "" ], [ "LeFloc'h", "Emeric", "" ], [ "Brown", "Michael J.", "" ], [ "Jannuzi", "Buell T.", "" ], [ "Armus", "Lee", "" ], [ "Bussmann", "Shane", "" ], [ "Brodwin", "Mark", "" ], [ "Bian", "Chao", "" ], [ "Eisenhardt", "Peter", "" ], [ "Higdon", "Sarah", "" ], [ "Weedman", "Daniel", "" ], [ "Willner", "Steve", "" ] ]
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801.1861
Erik Henriksen
E.A. Henriksen, Z. Jiang, L.-C. Tung, M.E. Schwartz, M. Takita, Y.-J. Wang, P. Kim, H.L. Stormer
Cyclotron resonance in bilayer graphene
to appear in Phys. Rev. Lett. Updated version with two added references and minor text editing
Phys. Rev. Lett. 100, 087403 (2008)
10.1103/PhysRevLett.100.087403
null
cond-mat.mes-hall
null
We present the first measurements of cyclotron resonance of electrons and holes in bilayer graphene. In magnetic fields up to B = 18 T we observe four distinct intraband transitions in both the conduction and valence bands. The transition energies are roughly linear in B between the lowest Landau levels, whereas they follow \sqrt{B} for the higher transitions. This highly unusual behavior represents a change from a parabolic to a linear energy dispersion. The density of states derived from our data generally agrees with the existing lowest order tight binding calculation for bilayer graphene. However in comparing data to theory, a single set of fitting parameters fails to describe the experimental results.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:18:37 GMT" }, { "version": "v2", "created": "Sat, 23 Feb 2008 23:32:46 GMT" } ]
2008-05-21T00:00:00
[ [ "Henriksen", "E. A.", "" ], [ "Jiang", "Z.", "" ], [ "Tung", "L. -C.", "" ], [ "Schwartz", "M. E.", "" ], [ "Takita", "M.", "" ], [ "Wang", "Y. -J.", "" ], [ "Kim", "P.", "" ], [ "Stormer", "H. L.", "" ] ]
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801.1862
Matthew Horak
Matthew Horak, Melanie Stein, Jennifer Taback
Convexity properties of Thompson's group F
11 pages, 3 figures
J. Group Theory 15 (2012): 37-45
10.1515/JGT.2010.093
null
math.GR
null
We prove that Thompson's group F is not minimally almost convex with respect to any generating set which is a subset of the standard infinite generating set for F and which contains x_1. We use this to show that F is not almost convex with respect to any generating set which is a subset of the standard infinite generating set.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:24:19 GMT" } ]
2021-09-24T00:00:00
[ [ "Horak", "Matthew", "" ], [ "Stein", "Melanie", "" ], [ "Taback", "Jennifer", "" ] ]
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801.1863
Joshua Davis
Alejandra Castro, Joshua L. Davis, Per Kraus, Finn Larsen
String Theory Effects on Five-Dimensional Black Hole Physics
85 pages; uses ws-ijmpa-mod.cls article class; Invited review for IJMPA
null
10.1142/S0217751X08039724
null
hep-th
null
We review recent developments in understanding quantum/string corrections to BPS black holes and strings in five-dimensional supergravity. These objects are solutions to the effective action obtained from M-theory compactified on a Calabi-Yau threefold, including the one-loop corrections determined by anomaly cancellation and supersymmetry. We introduce the off-shell formulation of this theory obtained through the conformal supergravity method and review the methods for investigating supersymmetric solutions. This leads to quantum/string corrected attractor geometries, as well as asymptotically flat black strings and spinning black holes. With these solutions in hand, we compare our results with analogous studies in four-dimensional string-corrected supergravity, emphasizing the distinctions between the four and five dimensional theories.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 23:00:32 GMT" } ]
2009-11-13T00:00:00
[ [ "Castro", "Alejandra", "" ], [ "Davis", "Joshua L.", "" ], [ "Kraus", "Per", "" ], [ "Larsen", "Finn", "" ] ]
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801.1864
Robert Kohn
P. Giordani and R. Kohn
Adaptive Independent Metropolis-Hastings by Fast Estimation of Mixtures of Normals
35 pages and 6 figures
null
null
null
stat.CO stat.AP stat.ME
null
We construct an adaptive independent Metropolis-Hastings sampler that uses a mixture of normals as a proposal distribution. To take full advantage of the potential of adaptive sampling our algorithm updates the mixture of normals frequently, starting early in the chain. The algorithm is built for speed and reliability and its sampling performance is evaluated with real and simulated examples. Our article outlines conditions for adaptive sampling to hold and gives a readily accessible proof that under these conditions the sampling scheme generates iterates that converge to the target distribution.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 22:53:12 GMT" } ]
2008-01-15T00:00:00
[ [ "Giordani", "P.", "" ], [ "Kohn", "R.", "" ] ]
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801.1865
Delfim F. M. Torres
Moulay Rchid Sidi Ammi, Delfim F. M. Torres
Combined dynamic Gruss inequalities on time scales
9 pages
Journal of Mathematical Sciences, Vol. 161, No. 6, 2009, 792--802
10.1007/s10958-009-9600-2
null
math.CA
null
We prove a more general version of the Gruss inequality by using the recent theory of combined dynamic derivatives on time scales and the more general notions of diamond-alpha derivative and integral. For the particular case when alpha = 1, one gets a delta-integral Gruss inequality on time scales; for alpha = 0 a nabla-integral Gruss inequality. If we further restrict ourselves by fixing the time scale to the real (or integer) numbers, then the standard continuous (discrete) inequalities are obtained.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 23:39:13 GMT" } ]
2009-09-18T00:00:00
[ [ "Ammi", "Moulay Rchid Sidi", "" ], [ "Torres", "Delfim F. M.", "" ] ]
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801.1866
William Krekelberg
William P. Krekelberg, Jeetain Mittal, Venkat Ganesan, Thomas M. Truskett
Structural anomalies of fluids: Origins in second and higher coordination shells
Submitted to The Journal of Chemical Physics
Phys. Rev. E 77, 041201 (2008)
10.1103/PhysRevE.77.041201
null
cond-mat.soft
null
Compressing or cooling a fluid typically enhances its static interparticle correlations. However, there are notable exceptions. Isothermal compression can reduce the translational order of fluids that exhibit anomalous waterlike trends in their thermodynamic and transport properties, while isochoric cooling (or strengthening of attractive interactions) can have a similar effect on fluids of particles with short-range attractions. Recent simulation studies by Yan et al. [Phys. Rev. E 76, 051201 (2007)] on the former type of system and Krekelberg et al. [J. Chem. Phys. 127, 044502 (2007)] on the latter provide examples where such structural anomalies can be related to specific changes in second and more distant coordination shells of the radial distribution function. Here, we confirm the generality of this microscopic picture through analysis, via molecular simulation and integral equation theory, of coordination shell contributions to the two-body excess entropy for several related model fluids which incorporate different levels of molecular resolution. The results suggest that integral equation theory can be an effective and computationally inexpensive first-pass tool for assessing, based on the pair potential alone, whether new model systems are good candidates for exhibiting structural (and hence thermodynamic and transport) anomalies.
[ { "version": "v1", "created": "Fri, 11 Jan 2008 23:59:26 GMT" } ]
2008-04-11T00:00:00
[ [ "Krekelberg", "William P.", "" ], [ "Mittal", "Jeetain", "" ], [ "Ganesan", "Venkat", "" ], [ "Truskett", "Thomas M.", "" ] ]
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801.1867
Artour Mouftakhov V
A. M. Akhtymov, A. V. Mouftakhov, M. Teicher
Identification of Boundary Conditions Using Natural Frequencies in Case of a Ring Membrane
null
null
null
null
math.SP
null
The problem of finding boundary conditions for fastening of a ring membrane, which are inaccessible for direct observation from the natural frequencies of its flexural oscillations, is considered. Two theorems on the uniqueness of this problem are proved, and a method for establishing the unknown conditions for fastening of the membrane to the walls is indicated. An approximate formula for determining the unknown conditions is obtained, using first three natural frequencies. The method of approximate calculation of unknown boundary conditions, is explained with the help of an example. Keywords: Boundary conditions, inverse spectral problem, membrane, natural frequencies, Plucker coordinates, Plucker relation.
[ { "version": "v1", "created": "Sat, 12 Jan 2008 00:03:37 GMT" } ]
2008-01-15T00:00:00
[ [ "Akhtymov", "A. M.", "" ], [ "Mouftakhov", "A. V.", "" ], [ "Teicher", "M.", "" ] ]
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801.1868
Luis Dorado
Luis A. Dorado and Ricardo A. Depine
Optical response of a self-standing monolayer of dielectric spheres
22 pages, 7 figures
null
null
null
physics.optics physics.class-ph
null
An analysis of the optical response of periodically arrayed monolayers composed of dielectric spheres with low refractive index is herein presented. The reflectance spectra of two-dimensional square and triangular lattices are obtained by means of the vector Korringa-Kohn-Rostoker method, both spectra showing very similar qualitative features for photon energies below the onset of diffraction spots. In this energy region, the same number of peaks of unitary amplitude in the reflectance spectra are predicted for both kinds of monolayers, suggesting that this must be a universal feature independent of the particular geometry of the lattice. The origin of these high reflectance peaks is investigated. It is found that the resonances of TM and TE modes due to dipolar, quadrupolar and octupolar interaction inside the monolayer are largely responsible for the peak structure observed in the reflectance spectra.
[ { "version": "v1", "created": "Sat, 12 Jan 2008 00:03:49 GMT" } ]
2008-01-15T00:00:00
[ [ "Dorado", "Luis A.", "" ], [ "Depine", "Ricardo A.", "" ] ]
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801.1869
Yuki Kaneko
Y. Kaneko, M.M. Gonzalez, R. Preece, B.L. Dingus, M.S. Briggs
Broadband Spectral Properties of Bright High-Energy Gamma-Ray Bursts Observed with BATSE and EGRET
18 pages (emulateapj) including 7 figures & 2 tables. Accepted for publication in ApJ
null
10.1086/529486
null
astro-ph
null
We present the spectral analysis of duration-integrated broadband spectra (in $\sim30 $keV$-200 $MeV) of 15 bright BATSE gamma-ray bursts (GRBs). Some GRB spectra are very hard, with their spectral peak energies being above the BATSE LAD passband limit of $\sim$2 MeV. In such cases, their high-energy spectral parameters (peak energy and high-energy power-law indices) cannot be adequately constrained by BATSE LAD data alone. A few dozen bright BATSE GRBs were also observed with EGRET's calorimeter, TASC, in multi-MeV energy band, with a large effective area and fine energy resolution. Combining the BATSE and TASC data, therefore, affords spectra that span four decades of energy ($30 $keV$-200 $MeV), allowing for a broadband spectral analysis with good statistics. Studying such broadband high-energy spectra of GRB prompt emission is crucial, as they provide key clues to understanding its gamma-ray emission mechanism. Among the 15 GRB spectra, we found two cases with a significant high-energy excess, and another case with a extremely high peak energy (\epeak $\gtrsim$ 170 MeV). There have been very limited number of GRBs observed at MeV energies and above, and only a few instruments have been capable of observing GRBs in this energy band with such high sensitivity. Thus, our analysis results presented here should also help predict GRB observations with current and future high-energy instruments such as AGILE and GLAST, as well as with ground-based very-high-energy telescopes.
[ { "version": "v1", "created": "Sat, 12 Jan 2008 00:12:51 GMT" } ]
2009-11-13T00:00:00
[ [ "Kaneko", "Y.", "" ], [ "Gonzalez", "M. M.", "" ], [ "Preece", "R.", "" ], [ "Dingus", "B. L.", "" ], [ "Briggs", "M. S.", "" ] ]
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801.187
Gerhard Kramm
Gerhard Kramm
Comment to "Recent Climate Observations Compared to Projections" by Rahmstorf et al
5 pages, 4 figures. Submitted for publication to Science
null
null
null
physics.ao-ph physics.ed-ph
null
It is shown in this comment that considering the Mauna Loa observation of the atmospheric carbon dioxide concentration and the mean near surface temperature anomalies for the period from the beginning of the seventies to recent years only is, clearly, a source of misinterpretation. If we consider the whole period of available data (1958 - 2004), we obtain results which differ from those presented by Rahmstorf et al. It is also shown that in 1988 when the Intergovernmental Panel of Climate Change (IPCC) of the United Nations and the World Meteorological Organization (WMO) was established there was certainly no correlation between the atmospheric carbon dioxide concentration and the mean near surface temperature anomalies, neither on the annual time scale nor on the monthly time scale.
[ { "version": "v1", "created": "Sat, 12 Jan 2008 00:43:45 GMT" } ]
2008-01-15T00:00:00
[ [ "Kramm", "Gerhard", "" ] ]
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801.1871
Toshihide Takagahara
Toshihide Takagahara and Ozgur Cakir
Theoretical aspects of quantum state transfer, correlation measurement and electron-nuclei coupled dynamics in quantum dots
null
J. Nanophotonics Vol. 1, 011593 (2007)
null
null
cond-mat.mes-hall
null
Photons and electrons are the key quantum media for the quantum information processing based on solid state devices. The essential ingredients to accomplish the quantum repeater were investigated and their underlying physics were revealed. The relevant elementary processes of the quantum state transfer between a single photon and a single electron were analyzed, to clarify the conditions to be satisfied to achieve the high fidelity of the quantum state transfer. An optical method based on the Faraday rotation was proposed to carry out the Bell measurement of two electrons which is a key operation in the entanglement swapping for the quantum repeater and its feasibility was confirmed. Also investigated was the quantum dynamics in the electron-nuclei coupled spin system in quantum dots and a couple of new phenomena were predicted related to the correlations induced by the hyperfine interaction, namely, bunching and revival in the electron spin measurements. These findings will pave the way to accomplish the efficient and robust quantum repeater and nuclear spin quantum memory.
[ { "version": "v1", "created": "Sat, 12 Jan 2008 00:37:26 GMT" } ]
2008-01-15T00:00:00
[ [ "Takagahara", "Toshihide", "" ], [ "Cakir", "Ozgur", "" ] ]
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801.1872
Artour Mouftakhov V
A. M. Akhtyamov, A. V. Mouftakhov, M. Teicher, L. S. Yamilova
Can One Hear Fastening of a Rod?
null
null
null
null
math.SP
null
Rods are parts of various devices. If it is impossible to observe the rod directly, the only source of information about possible defects of its fastening can be the natural frequencies of its flexural vibrations. The question arises whether one would be able to detect damage in rod fastening by the natural frequencies of its flexural vibrations. This paper gives and substantiates a positive answer to this question.
[ { "version": "v1", "created": "Sat, 12 Jan 2008 00:38:38 GMT" } ]
2008-01-15T00:00:00
[ [ "Akhtyamov", "A. M.", "" ], [ "Mouftakhov", "A. V.", "" ], [ "Teicher", "M.", "" ], [ "Yamilova", "L. S.", "" ] ]
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