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801.0673 | Kevin Edmonds | A.A. Freeman, K.W. Edmonds, G. van der Laan, R.P. Campion, N.R.S.
Farley, A.W. Rushforth, T.K. Johal, C.T. Foxon, B.L. Gallagher, A. Rogalev,
and F. Wilhelm | Valence band orbital polarization in III-V ferromagnetic semiconductors | 5 pages, 2 figures | null | 10.1103/PhysRevB.77.073304 | null | cond-mat.mtrl-sci cond-mat.mes-hall | null | The element-specific technique of x-ray magnetic circular dichroism (XMCD) is
used to directly determine the magnitude and character of the valence band
orbital magnetic moments in (III,Mn)As ferromagnetic semiconductors. A distinct
dichroism is observed at the As K absorption edge, yielding an As 4p orbital
magnetic moment of around -0.1 Bohr magnetons per valence band hole. This is
strongly influenced by strain, indicating its crucial influence on the magnetic
anisotropy. The dichroism at the Ga K edge is much weaker. The K edge XMCD
signals for Mn and As both have positive sign, which indicates the important
contribution of Mn 4p states to the Mn K edge spectra.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 12:49:43 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Freeman",
"A. A.",
""
],
[
"Edmonds",
"K. W.",
""
],
[
"van der Laan",
"G.",
""
],
[
"Campion",
"R. P.",
""
],
[
"Farley",
"N. R. S.",
""
],
[
"Rushforth",
"A. W.",
""
],
[
"Johal",
"T. K.",
""
],
[
"Foxon",
"C. T.",
""
],
[
"Gallagher",
"B. L.",
""
],
[
"Rogalev",
"A.",
""
],
[
"Wilhelm",
"F.",
""
]
] | [
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801.0674 | Griet C. Van de Steene | G.C. Van de Steene, T. Ueta, P.A.M.van Hoof, M. Reyniers, A.G.
Ginsburg | Kinematics and H_2 morphology of the multipolar Post-AGB star IRAS
16594-4656 | 11 pages and 8 figures; A&A in press; the paper includig high
resolution figures can be downloaded from
http://homepage.oma.be/gsteene/publications.html | null | 10.1051/0004-6361:20078880 | null | astro-ph | null | context: The spectrum of IRAS 16594-4656 shows shock excited H_2 emission and
collisionally excited emission lines such as[O I],[C I],and [Fe II]. aim: The
goal is to determine the location of the H_2 and [Fe II] shock emission, to
determine the shock velocities,and constrain the physical properties in the
shock. methods: High resolution spectra of the H_2 1-0 S(1),H_2 2-1 S(1), [Fe
II], and Pa$\beta$ emission lines were obtained with the near infrared
spectrograph Phoenix on Gemini South. results: The position-velocity diagrams
of H_2 1-0 S(1), H_2 2-1 S(1), and [Fe II] are presented. The H_2 and [Fe II]
emission is spatially extended. The collisionally excited [O I] and [C I]
optical emission lines have a similar double peaked profile compared to the
extracted H_2 profile and appear to be produced in the same shock. They all
indicate an expansion velocity of ~8 km/s and the presence of a neutral, very
high density region with $n_{\rm e}$ about 3 x 10^6 to 5 x10^7 cm$^{-3}$. The
[Fe II] emission however is single peaked. It has a gaussian FWHM of 30 km/s
and a total width of 62 km/s at 1% of the peak. The Pa$\beta$ profile is even
wider with a gaussian FWHM of 48 km/s and a total width of 75 km/s at 1% of the
peak. conclusions: The H$_2$ emission is excited in a slow 5 to 20 km/s shock
into dense material at the edge of the lobes, caused by the interaction of the
AGB ejecta and the post-AGB wind. The 3D representation of the H_2 data shows a
hollow structure with less H_2 emission in the equatorial region. The [Fe II]
emission is not present in the lobes, but originates close to the central star
in fast shocks in the post-AGB wind or in a disk. The Pa$\beta$ emission also
appears to originate close to the star.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:00:35 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Van de Steene",
"G. C.",
""
],
[
"Ueta",
"T.",
""
],
[
"van Hoof",
"P. A. M.",
""
],
[
"Reyniers",
"M.",
""
],
[
"Ginsburg",
"A. G.",
""
]
] | [
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] |
801.0675 | Matthias Neubert | Matthias Neubert (Univ. Mainz) | QCD Calculations of Decays of Heavy Flavor Hadrons | Invited plenary talk delivered at the 23rd International Symposium on
Lepton and Photon Interactions at High Energy (Daegu, Korea, 13-18 August
2007) | null | null | MZ-TH/08-2 | hep-ph | null | Precision tests of the Standard Model and searches for New Physics in the
quark flavor sector depend on accurate theoretical calculations of decay rates
and spectra for rare, flavor-changing processes. The theoretical status and
recent developments of techniques allowing such calculations are reviewed.
Special attention is paid to the calculation of the B->Xs+gamma branching
ratio, the extraction of the b-quark mass from a fit to B->Xc+l+nu moments, and
the determination of |V(ub)| from spectra in the inclusive decay B->Xu+l+nu.
From a reanalysis of different inclusive distributions the updated average
value |V(ub)|=(3.98+-0.15+-0.30)*10^{-3} is derived. Using only the
theoretically cleanest channels, we obtain |V(ub)|=(3.70+-0.15+-0.28)*10^{-3}.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:18:18 GMT"
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] | 2008-01-07T00:00:00 | [
[
"Neubert",
"Matthias",
"",
"Univ. Mainz"
]
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] |
801.0676 | Gleb Oshanin | G. Oshanin | Fractional Brownian motion in presence of two fixed adsorbing boundaries | 13 pages, submitted to J.Phys.A | null | null | null | cond-mat.stat-mech math.PR | null | We study the long-time asymptotics of the probability P_t that the
Riemann-Liouville fractional Brownian motion with Hurst index H does not escape
from a fixed interval [-L,L] up to time t. We show that for any H \in ]0,1],
for both subdiffusion and superdiffusion regimes, this probability obeys
\ln(P_t) \sim - t^{2 H}/L^2, i.e. may decay slower than exponential
(subdiffusion) or faster than exponential (superdiffusion). This implies that
survival probability S_t of particles undergoing fractional Brownian motion in
a one-dimensional system with randomly placed traps follows \ln(S_t) \sim -
n^{2/3} t^{2H/3} as t \to \infty, where n is the mean density of traps.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:07:07 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Oshanin",
"G.",
""
]
] | [
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] |
801.0677 | Jad Saklawi | Paul C. Attie | Finite-state concurrent programs can be expressed pairwise | 14 pages | null | null | null | cs.LO | null | We present a \emph{pairwise normal form} for finite-state shared memory
concurrent programs: all variables are shared between exactly two processes,
and the guards on transitions are conjunctions of conditions over this pairwise
shared state. This representation has been used to efficiently (in polynomial
time) synthesize and model-check correctness properties of concurrent programs.
Our main result is that any finite state concurrent program can be transformed
into pairwise normal form. Specifically, if $Q$ is an arbitrary finite-state
shared memory concurrent program, then there exists a finite-state shared
memory concurrent program $P$ expressed in pairwise normal form such that $P$
is strongly bisimilar to $Q$. Our result is constructive: we give an algorithm
for producing $P$, given $Q$.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:14:31 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Attie",
"Paul C.",
""
]
] | [
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] |
801.0678 | Joel Chevrier | Sylvain Marli\`ere (ICA), Jean Loup Florens (ICA), Florence Marchi
(ESRF, NEEL), Annie Luciani (ICA), Joel Chevrier (ESRF, NEEL) | Implementation of perception and action at nanoscale | Proceedings of ENACTIVE/07 4th International Conference on Enactive
Interfaces Grenoble, France, November 19th-22nd, 2007 | null | null | null | cs.RO cs.HC | null | Real time combination of nanosensors and nanoactuators with virtual reality
environment and multisensorial interfaces enable us to efficiently act and
perceive at nanoscale. Advanced manipulation of nanoobjects and new strategies
for scientific education are the key motivations. We have no existing intuitive
representation of the nanoworld ruled by laws foreign to our experience. A
central challenge is then the construction of nanoworld simulacrum that we can
start to visit and to explore. In this nanoworld simulacrum, object
identifications will be based on probed entity physical and chemical intrinsic
properties, on their interactions with sensors and on the final choices made in
building a multisensorial interface so that these objects become coherent
elements of the human sphere of action and perception. Here we describe a 1D
virtual nanomanipulator, part of the Cit\'e des Sciences EXPO NANO in Paris,
that is the first realization based on this program.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:38:39 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Marlière",
"Sylvain",
"",
"ICA"
],
[
"Florens",
"Jean Loup",
"",
"ICA"
],
[
"Marchi",
"Florence",
"",
"ESRF, NEEL"
],
[
"Luciani",
"Annie",
"",
"ICA"
],
[
"Chevrier",
"Joel",
"",
"ESRF, NEEL"
]
] | [
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801.0679 | Olivier Ramar\'e | Olivier Ramar\'e | A stronger model for peg solitaire, II | 27 pages, 31 figures | null | null | null | math.CO math.AG | null | The main problem addressed here is to decide whether it is possible or not to
go from a given position on a peg-solitaire board to another one. No
non-trivial sufficient conditions are known, but tests have been devised to
show impossibility. We expose the way these tests work in a unified formalism
and provide a new test which is strictly stronger than all previous ones.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:39:55 GMT"
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] | 2008-01-07T00:00:00 | [
[
"Ramaré",
"Olivier",
""
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801.068 | Pamela Morehouse | CLEO Collaboration: J. Alexander, et al | Absolute Measurement of Hadronic Branching Fractions of the D_s^+ Meson | 6 pages, postscript also available through
http://www.lns.cornell.edu/public/CLNS/2007/, revised | Phys.Rev.Lett.100:161804,2008 | 10.1103/PhysRevLett.100.161804 | CLNS 07/2016, CLEO 07-20 | hep-ex | null | The branching fractions of D_s meson decays serve to normalize many
measurements of processes involving charm quarks. Using 298 /pb of e+ e-
collisions recorded at a center of mass energy of 4.17 GeV, we determine
absolute branching fractions for eight D_s decays with a double tag technique.
In particular we determine the branching fraction B(D_s -> K- K+ pi+) = (5.50
+- 0.23 +- 0.16)%, where the uncertainties are statistical and systematic
respectively. We also provide partial branching fractions for kinematic subsets
of the K- K+ pi+ decay mode.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:44:16 GMT"
},
{
"version": "v2",
"created": "Thu, 24 Apr 2008 14:48:04 GMT"
}
] | 2010-04-08T00:00:00 | [
[
"CLEO Collaboration",
"",
""
],
[
"Alexander",
"J.",
""
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801.0681 | Zaninetti Lorenzo | Michele Rossi, Lorenzo Zaninetti | Linear and Non Linear Effects on the Newtonian Gravitational Constant as
deduced from the Torsion Balance | 11 pages, 2 figures | International Journal of Modern Physics A, Volume 29, pp.
5391-5400 (2007) | 10.1142/S0217751X07037329 | null | physics.class-ph physics.data-an | null | The Newtonian gravitational constant has still 150 parts per million of
uncertainty. This paper examines the linear and nonlinear equations governing
the rotational dynamics of the torsion gravitational balance. A nonlinear
effect modifying the oscillation period of the torsion gravitational balance is
carefully explored.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 13:44:26 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Rossi",
"Michele",
""
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[
"Zaninetti",
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] |
801.0682 | Ryusuke Ikeda | Yuichi Matsunaga, Norihito Hiasa, and Ryusuke Ikeda | Modulated vortex states in Rashba non-centrosymmetric superconductors | Final version accepted for publication in Phys.Rev.B (Rapid Commmun.) | null | 10.1103/PhysRevB.78.220508 | null | cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Vortex lattice structures to occur in Rashba non-centrosymmetric
superconductors under a magnetic field parallel to the basal plane are studied
by assuming a singlet Cooper pairing and taking account of both the
paramagnetic and orbital depairings. A vortex lattice of
Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) type with modulation perpendicular to
the field is expected to occur in the limit of vanishing ${\tilde \eta}$, where
${\tilde \eta}$ is the spin-orbit coupling {\it normalized} by Fermi energy. As
${\tilde \eta}$ increases, however, this state tends to be replaced by another
new vortex lattice with a modulation of the gap amplitude parallel to the
helical phase modulation induced by the absence of inversion symmetry.
Differences of the present results from those in the Pauli limit and a
correlation of a structural transition with the $H_{c2}(T)$-curve are discussed
in relation to possible experimental realization.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:16:08 GMT"
},
{
"version": "v2",
"created": "Mon, 17 Mar 2008 07:40:59 GMT"
},
{
"version": "v3",
"created": "Thu, 16 Oct 2008 09:37:28 GMT"
},
{
"version": "v4",
"created": "Wed, 3 Dec 2008 03:01:32 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Matsunaga",
"Yuichi",
""
],
[
"Hiasa",
"Norihito",
""
],
[
"Ikeda",
"Ryusuke",
""
]
] | [
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] |
801.0683 | Thomas Kallinger | T. Kallinger, P. Reegen, W. W. Weiss | A heuristic derivation of the uncertainty of the frequency determination
in time series data | null | null | 10.1051/0004-6361:20077559 | null | astro-ph | null | Context: Several approaches to estimate frequency, phase and amplitude errors
in time series analyses were reported in the literature, but they are either
time consuming to compute, grossly overestimating the error, or are based on
empirically determined criteria. Aims: A simple, but realistic estimate of the
frequency uncertainty in time series analyses. Methods: Synthetic data sets
with mono- and multi-periodic harmonic signals and with randomly distributed
amplitude, frequency and phase were generated and white noise added. We tried
to recover the input parameters with classical Fourier techniques and
investigated the error as a function of the relative level of noise, signal and
frequency difference. Results: We present simple formulas for the upper limit
of the amplitude, frequency and phase uncertainties in time-series analyses. We
also demonstrate the possibility to detect frequencies which are separated by
less than the classical frequency resolution and that the realistic frequency
error is at least 4 times smaller than the classical frequency resolution.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 14:16:50 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Kallinger",
"T.",
""
],
[
"Reegen",
"P.",
""
],
[
"Weiss",
"W. W.",
""
]
] | [
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] |
801.0684 | Norman G\"urlebeck | Norman G\"urlebeck | On Appell Sets and the Fueter-Sce Mapping | 10 pages | Advances in Applied Clifford Algebras, Volume 19 (2009), Number 1,
51-61 | 10.1007/s00006-008-0126-3 | null | math.CV | null | It is proved, that the recently discussed Appell polynomials in Clifford
algebras are the Fueter-Sce extension of the complex monomials z^k.
Furthermore, it is shown, for which complex functions the Fueter-Sce extension
and the extension method using Appell polynomials coincide.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 14:34:37 GMT"
}
] | 2011-06-13T00:00:00 | [
[
"Gürlebeck",
"Norman",
""
]
] | [
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] |
801.0685 | Irena Swanson | William Heinzer and Irena Swanson | The Goto numbers of parameter ideals | 21 pages; the project started in a working group at AIM in December
2006 | null | null | null | math.AC | null | Let Q be a parameter ideal of a Noetherian local ring (R,m). The Goto number
g(Q) of Q is the largest integer g such that Q:m^g is integral over Q. We
examine the values of g(Q) as Q varies over the parameter ideals of R. We
concentrate mainly on the case where dim R = 1, and many of our results concern
parameter ideals of a numerical semigroup ring.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 18:36:22 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Heinzer",
"William",
""
],
[
"Swanson",
"Irena",
""
]
] | [
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] |
801.0686 | Florian Lenz Mr | Florian Lenz, Fotis K. Diakonos, Peter Schmelcher | Classical Dynamics of the Time-Dependent Elliptical Billiard | null | Phys. Rev. E, {\bf 76}, 066213 (2007) | 10.1103/PhysRevE.76.066213 | null | nlin.CD | null | In this work we study the nonlinear dynamics of the static and the driven
ellipse. In the static case, we find numerically an asymptotical algebraic
decay for the escape of an ensemble of non-interacting particles through a
small hole due to the integrable structure of the phase space of the system.
Furthermore, for a certain hole position a saturation value in the decay that
can be tuned arbitrarily by varying the eccentricity of the ellipse is observed
and explained. When applying harmonic boundary oscillations this saturation
value caused by librator type orbits is gradually destroyed via two fundamental
processes which are discussed in detail. As a result, an amplitude dependent
emission rate is obtained in the long time behavior of the decay, suggesting
that the driven elliptical billiard can be used as a controllable source of
particles.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 14:47:29 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Lenz",
"Florian",
""
],
[
"Diakonos",
"Fotis K.",
""
],
[
"Schmelcher",
"Peter",
""
]
] | [
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] |
801.0687 | Evgeny Korotyaev | Evgeny Korotyaev, Anton Kutsenko | Borg type uniqueness Theorems for periodic Jacobi operators with matrix
valued coefficients | null | null | null | null | math.SP math-ph math.MP | null | We give a simple proof of Borg type uniqueness Theorems for periodic Jacobi
operators with matrix valued coefficients.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 14:54:43 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Korotyaev",
"Evgeny",
""
],
[
"Kutsenko",
"Anton",
""
]
] | [
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] |
801.0688 | James B. Hartle | James B. Hartle | Quantum Mechanics with Extended Probabilities | 15 pages, 2 figures, revtex4, minor corrections, add'l references | Phys. Rev. A, 78, 012108 (2008) | 10.1103/PhysRevA.78.012108 | null | quant-ph gr-qc hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The quantum mechanics of closed systems such as the universe is formulated
using an extension of familiar probability theory that incorporates negative
probabilities. Probabilities must be positive for sets of alternative histories
that are the basis of fair settleable bets. However, in quantum mechanics there
are sets of alternative histories that can be described but which cannot be the
basis for fair settleable bets. Members of such sets can be assigned extended
probabilities that are sometimes negative. A prescription for extended
probabilities is introduced that assigns extended probabilities to all
histories that can be described, fine grained or coarse grained, members of
decoherent sets or not. All probability sum rules are satisfied exactly. Sets
of histories that are recorded to sufficient precision are the basis of
settleable bets. This formulation is compared with the decoherent (consistent)
histories formulation of quantum theory. Prospects are discussed for using this
formulation to provide testable alternatives to quantum theory or further
generalizations of it.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:23:45 GMT"
},
{
"version": "v2",
"created": "Fri, 4 Jan 2008 22:32:29 GMT"
},
{
"version": "v3",
"created": "Thu, 17 Jul 2008 18:42:42 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Hartle",
"James B.",
""
]
] | [
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801.0689 | Mikhail Fedorov V. | Yu.M. Mikhailova, P.A. Volkov, and M.V. Fedorov | Frequency and temporal entanglement of biphoton states in spontaneous
parametric down conversion with a short-pulse pump | Contents is extended | null | null | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Spectral and temporal coincidence and single-particle photon wave packets are
described and their widths and durations are found. The degree of entanglement
is characterized by the experimentally measurable parameter R defined as the
ratio of the coincidence and single-particle spectral widths. In the frequency
representation, this parameter is found as a function of the pump-pulse
duration. This function is shown to have a minimum and even in the minimum, at
rather natural conditions, the parameter R is found to be very high (R=73>>1).
The Schmidt number K is found for both short and long pump pulses and
interpolated for arbitrary pulse durations. All functional dependences of R and
K are found to be identical and numerical difference between them is shown to
be not exceeding 20%. Two-time temporal wave function of a biphoton state is
investigated in details, and a rather significant difference between the cases
of short and long pump pulses is found to occur. In the case of long pulses,
the temporal parameter R is defined as the ratio of durations of the
single-particle and coincidence signals, and the defined in such a way
parameter R is shown to be very close to the Schmidt number K.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:31:57 GMT"
},
{
"version": "v2",
"created": "Sat, 12 Jul 2008 07:04:33 GMT"
}
] | 2009-09-29T00:00:00 | [
[
"Mikhailova",
"Yu. M.",
""
],
[
"Volkov",
"P. A.",
""
],
[
"Fedorov",
"M. V.",
""
]
] | [
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] |
801.069 | Rubens Ramos Viana | Rubens Viana Ramos and Fabio Alencar Mendonca | Quantum bit commitment protocol without quantum memory | 12 pages, 2 figures | null | null | null | quant-ph | null | Quantum protocols for bit commitment have been proposed and it is largely
accepted that unconditionally secure quantum bit commitment is not possible;
however, it can be more secure than classical bit commitment. In despite of its
usefulness, quantum bit commitment protocols have not been experimentally
implemented. The main reason is the fact that all proposed quantum bit
commitment protocols require quantum memory. In this work, we show a quantum
bit commitment protocol that does not require quantum memory and can be
implemented with present technology.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:33:07 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Ramos",
"Rubens Viana",
""
],
[
"Mendonca",
"Fabio Alencar",
""
]
] | [
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] |
801.0691 | George Tsibidis | George D. Tsibidis | A FRAP model to investigate reaction-diffusion of proteins within a
bounded domain: a theoretical approach | 25 pages. Abstracts Proceedings, The American Society for Cell
Biology, 46th Annual Meeting, December 9-13, 2006, San Diego | Journal of Theoretical Biology 253 (2008) 755-768 | 10.1016/j.jtbi.2008.04.010 | null | q-bio.SC physics.bio-ph q-bio.BM q-bio.QM | null | Temporally and spatially resolved measurements of protein transport inside
cells provide important clues to the functional architecture and dynamics of
biological systems. Fluorescence Recovery After Photobleaching (FRAP) technique
has been used over the past three decades to measure the mobility of
macromolecules and protein transport and interaction with immobile structures
inside the cell nucleus. A theoretical model is presented that aims to describe
protein transport inside the nucleus, a process which is influenced by the
presence of a boundary (i.e. membrane). A set of reaction-diffusion equations
is employed to model both the diffusion of proteins and their interaction with
immobile binding sites. The proposed model has been designed to be applied to
biological samples with a Confocal Laser Scanning Microscope (CLSM) equipped
with the feature to bleach regions characterised by a scanning beam that has a
radially Gaussian distributed profile. The proposed model leads to FRAP curves
that depend on the on- and off-rates. Semi-analytical expressions are used to
define the boundaries of on- (off-) rate parameter space in simplified cases
when molecules move within a bounded domain. The theoretical model can be used
in conjunction to experimental data acquired by CLSM to investigate the
biophysical properties of proteins in living cells.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:33:28 GMT"
}
] | 2009-03-04T00:00:00 | [
[
"Tsibidis",
"George D.",
""
]
] | [
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] |
801.0692 | Alexandre Eremenko | A. Eremenko and J. K. Langley | Meromorphic functions of one complex variable. A survey | 33 pages | null | null | null | math.CV | null | This is an appendix to the English translation of the book by A. A. Goldberg
and I. V. Ostrovskii, Distribution of values of meromorphic functions, Moscow,
Nauka, 1970. An English translation of this book is to be published soon by the
AMS. In this appendix we survey the results obtained on the topics of the book
after 1970.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:45:29 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Eremenko",
"A.",
""
],
[
"Langley",
"J. K.",
""
]
] | [
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] |
801.0693 | Annalisa Calamida | A. Calamida, C.E. Corsi, G. Bono (OAR/INAF), P. B. Stetson (HIA/NRC),
L. M. Freyhammer (Univ. Lancashire), R. Buonanno (Univ. Rome) | Relative and absolute calibration for multi-band data collected with the
2.2m ESO/MPI and 1.54m Danish Telescopes | 4 pages, 3 figures, to be published in the Springer-Verlag series
"ESO Astrophysics Symposia" | null | 10.1007/978-3-540-76963-7_80 | null | astro-ph | null | We present the strategies adopted in the relative and absolute calibration of
two different data sets: U,B,V,I-band images collected with the Wide Field
Imager (WFI) mosaic camera mounted on the 2.2m ESO/MPI Telescope and u,v,b,y
Stroemgren images collected with the 1.54m Danish Telescope (ESO, La Silla). In
the case of the WFI camera we adopted two methods for the calibration, one for
images collected before 2002, with the ESO filters U/38_ESO841 and B/99_ESO842,
and a different one for data secured after 2002, with the filters U/50_ESO877
and B/123_ESO878. The positional and color effects turned out to be stronger
for images collected with the old filters. The eight WFI chips of these images
were corrected one by one, while in the case of images secured with the new
filters, we corrected the entire mosaic in a single step. In the case of the
Danish data set, we compared point-spread function (PSF) and aperture
photometry for each frame, finding a trend in both the X and Y directions of
the chip. The corrections resulted in a set of first and second order
polynomials to be applied to the instrumental magnitudes of each individual
frame as a function of the star position.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:47:01 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Calamida",
"A.",
"",
"OAR/INAF"
],
[
"Corsi",
"C. E.",
"",
"OAR/INAF"
],
[
"Bono",
"G.",
"",
"OAR/INAF"
],
[
"Stetson",
"P. B.",
"",
"HIA/NRC"
],
[
"Freyhammer",
"L. M.",
"",
"Univ. Lancashire"
],
[
"Buonanno",
"R.",
"",
"Univ. Rome"
]
] | [
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] |
801.0694 | Valery Koryukin | V. M. Koryukin | On the Higgs mechanism and the gauge field theory | null | null | null | null | physics.gen-ph hep-ph | null | As laboratory experiments for the detection of particles with non-zero rest
masses forming the dark matter do not give positive results we offer once more
to turn the attention upon the neutrinos background of the Universe. If the
neutrinos background has the temperature 2 K, then direct observations of
particles are impossible ones and only their high density allows hope for the
success indirect observations. In consequence of this the field theory is
constructed as the maximum plausible reduction of the Feynman formulation of
the quantum theory displaying experiment data adequately.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:48:41 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Koryukin",
"V. M.",
""
]
] | [
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] |
801.0695 | Mark Veraar | Sonja Cox, Mark Veraar | Some remarks on tangent martingale difference sequences in $L^1$-spaces | null | Electron. Commun. Probab. 12, 421-433, (2007) | null | null | math.PR math.FA | null | Let X be a Banach space. Suppose that for all $p\in (1, \infty)$ a constant
$C_{p,X}$ depending only on X and p exists such that for any two X-valued
martingales f and g with tangent martingale difference sequences one has
\[\E\|f\|^p \leq C_{p,X} \E\|g\|^p (*).\] This property is equivalent to the
UMD condition. In fact, it is still equivalent to the UMD condition if in
addition one demands that either f or g satisfy the so-called (CI) condition.
However, for some applications it suffices to assume that (*) holds whenever g
satisfies the (CI) condition. We show that the class of Banach spaces for which
(*) holds whenever only g satisfies the (CI) condition is more general than the
class of UMD spaces, in particular it includes the space L^1. We state several
problems related to (*) and other decoupling inequalities.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:09:55 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Cox",
"Sonja",
""
],
[
"Veraar",
"Mark",
""
]
] | [
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] |
801.0696 | Rubens Ramos Viana | Rubens Viana Ramos and Jose Claudio do Nascimento | Quantum Zero-Knowledge Protocol Using Quantum Bit Commitment without
Quantum Memory | 4 pages and 1 figure | null | null | null | quant-ph | null | Zero-knowledge proof system is an important protocol that can be used as a
basic block for construction of other more complex cryptographic protocols.
Quantum zero-knowledge protocols have been proposed but, since their
implementation requires advanced quantum technology devices, experimental
implementation of zero-knowledge protocols have not being reported. In this
work, we present a quantum zero-knowledge protocol based on a quantum bit
commitment protocol that can be implemented with today technology. Hence, our
quantum zero-knowledge protocol can be readily implemented.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:59:42 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Ramos",
"Rubens Viana",
""
],
[
"Nascimento",
"Jose Claudio do",
""
]
] | [
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] |
801.0697 | Miika Klemetti | The BABAR Collaboration, B. Aubert, et al | Searches for the decays B0 -> l+ tau- and B+ -> l+ nu (l=e,mu) using
hadronic tag reconstruction | 8 pages, 2 postscript figures, submitted to PRD-RC | Phys.Rev.D77:091104,2008 | 10.1103/PhysRevD.77.091104 | BABAR-PUB-07/069, SLAC-PUB-13066 | hep-ex | null | We present searches for the leptonic decays B+ -> l+ nu and the lepton flavor
violating decays B0 -> l+ tau-, where l=e,mu, with data collected by the BaBar
experiment at SLAC. This search demonstrates a novel technique in which we
fully reconstruct the accompanying Bbar in Upsilon(4S)->BBbar events, and look
for a monoenergetic lepton from the signal B decay. The signal yield is
extracted from a fit to the signal lepton candidate momentum distribution in
the signal B rest frame. Using a data sample of approximately 378 million BBbar
pairs (342fb-1), we find no evidence of signal in any of the decay modes.
Branching fraction upper limits of B(B+ -> e+ nu)<5.2x10^-6, B(B+ -> mu+
nu)<5.6x10^-6, B(B0 -> e+ tau-)<2.8x10^-5 and B(B0 -> mu+ tau-)<2.2x10^-5, are
obtained at 90% confidence level.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:07:00 GMT"
}
] | 2010-04-12T00:00:00 | [
[
"The BABAR Collaboration",
"",
""
],
[
"Aubert",
"B.",
""
]
] | [
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] |
801.0698 | Matthias H. Hettler | Jasmin Aghassi, Matthias H. Hettler, and Gerd Sch\"on | Co-tunneling assisted sequential tunneling in multi-level quantum dots | 10 pages including 3 color figures | Applied Physics Letters, Vol. 92, 202101 (2008) | 10.1063/1.2927379 | null | cond-mat.mes-hall | null | We investigate the conductance and zero-frequency shot noise of interacting,
multi-level quantum dots coupled to leads. We observe that co-tunneling
assisted sequential tunneling (CAST) processes play a dominant role in the
transition region from Coulomb blockade to sequential tunneling. We analyze for
intermediate coupling strength the dependence of the conductance due to CAST
processes on temperature, coupling constant, and gate voltage. Remarkably, the
width of the CAST transport feature scales only with temperature, but not with
the coupling constant. While the onset of inelastic co-tunneling is associated
with a super-Poissonian noise, the noise is even stronger above the threshold
for CAST processes
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:08:35 GMT"
}
] | 2008-05-30T00:00:00 | [
[
"Aghassi",
"Jasmin",
""
],
[
"Hettler",
"Matthias H.",
""
],
[
"Schön",
"Gerd",
""
]
] | [
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] |
801.0699 | Orkan Umurhan | Oded Regev | Hydrodynamical activity in thin accretion disks | To appear in New Astronomy Review, Proc. of "J-P. Lasota, X-ray
binaries, accretion disks and compact stars" (October 2007); Abramowicz, M.
Ed | New Astron.Rev.51:819-827,2008 | 10.1016/j.newar.2008.03.011 | null | astro-ph | null | An asymptotic treatment of thin accretion disks, introduced by Klu\'zniak &
Kita (2000) for a steady-state disk flow, is extended to a time-dependent
problem. Transient growth of axisymmetric disturbances is analytically shown to
occur on the global disk scale. The implications of this result on the theory
of hydrodynamical thin accretion disks, as well as future prospects, are
discussed.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 18:28:38 GMT"
},
{
"version": "v2",
"created": "Thu, 10 Jan 2008 17:48:01 GMT"
}
] | 2009-06-23T00:00:00 | [
[
"Regev",
"Oded",
""
]
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801.07 | Anna Kowalczyk | Anna Kowalczyk | Proton induced spallation reactions in the energy range 0.1 - 10 GeV | null | null | null | null | nucl-th | null | One of considered nowadays scenarios of proton - nucleus reaction is
spallation. Its motivation is based on experimental final-state observations of
one heavy nucleus, a small number of light fragments and numerous individual
nucleons. It is theoretically described as two step process involving energy
deposition in the target nucleus and subsequent evaporation. Several models,
based on different assumptions, have been constructed in order to describe the
spallation process. The main subject of this work is description of global
average properties of proton induced spallation reactions in wide range of
projectile energy (0.1 - 10 GeV) and mass of target nuclei. This is
investigated within Hadron String Dynamics (HSD) model, based on Boltzmann -
Uehling - Uhlenbeck (BUU) equation, supplemented by a statistical evaporation
model for the second stage of the reaction. It has been shown that spallation
is the most probable scenario of proton - nucleus reaction. Proton induced
reactions, in considered here incident energy range, are visibly non-invasive
processes. Properties of residual nuclei after the first stage of the reaction
are weakly dependent on incident energy, but strongly dependent on mass of
target. The second stage of the reaction is a competition of evaporation and
fission. Results obtained from the HSD model vary smoothly as function of
proton incident energy and mass of target, so interpolation of the results is
quite feasible.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 15:55:21 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Kowalczyk",
"Anna",
""
]
] | [
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] |
801.0701 | Leah Nutman | Leah Nutman and Michael Langberg | Adversarial Models and Resilient Schemes for Network Coding | Second version includes minor editing | null | null | null | cs.IT cs.DC cs.NI math.IT | null | In a recent paper, Jaggi et al. (INFOCOM 2007), presented a distributed
polynomial-time rate-optimal network-coding scheme that works in the presence
of Byzantine faults. We revisit their adversarial models and augment them with
three, arguably realistic, models. In each of the models, we present a
distributed scheme that demonstrates the usefulness of the model. In
particular, all of the schemes obtain optimal rate $C-z$, where $C$ is the
network capacity and $z$ is a bound on the number of links controlled by the
adversary.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:17:49 GMT"
},
{
"version": "v2",
"created": "Wed, 6 Feb 2008 16:49:31 GMT"
}
] | 2008-02-06T00:00:00 | [
[
"Nutman",
"Leah",
""
],
[
"Langberg",
"Michael",
""
]
] | [
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] |
801.0702 | Sonia Schirmer | Xiaoting Wang and Sonia G. Schirmer | Analysis of Lyapunov Method for Control of Quantum Systems | 20 pages, 1 figure, draft version | null | 10.1109/TAC.2010.2043292 10.1109/TAC.2010.204276 | null | quant-ph | null | We present a detailed analysis of the convergence properties of Lyapunov
control for finite-dimensional quantum systems based on the application of the
LaSalle invariance principle and stability analysis from dynamical systems and
control theory. For a certain class of ideal Hamiltonians, convergence results
are derived both pure-state and mixed-state control, and the effectiveness of
the method for more realistic Hamiltonians is discussed.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:26:59 GMT"
},
{
"version": "v2",
"created": "Mon, 19 May 2008 15:02:07 GMT"
}
] | 2012-02-14T00:00:00 | [
[
"Wang",
"Xiaoting",
""
],
[
"Schirmer",
"Sonia G.",
""
]
] | [
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] |
801.0703 | Silvia Dalla | S. Dalla, L. Fletcher and N.A. Walton | Invisible sunspots and rate of solar magnetic flux emergence | A&A Lett, in press, 2008 | A&A 479, L1-L4 (2008) | 10.1051/0004-6361:20078800 | null | astro-ph | null | We study the visibility of sunspots and its influence on observed values of
sunspot region parameters. We use Virtual Observatory tools provided by
AstroGrid to analyse a sample of 6862 sunspot regions. By studying the
distributions of locations where sunspots were first and last observed on the
solar disk, we derive the visibility function of sunspots, the rate of magnetic
flux emergence and the ratio between the durations of growth and decay phases
of solar active regions. We demonstrate that the visibility of small sunspots
has a strong center-to-limb variation, far larger than would be expected from
geometrical (projection) effects. This results in a large number of young spots
being invisible: 44% of new regions emerging in the West of the Sun go
undetected. For sunspot regions that are detected, large differences exist
between actual locations and times of flux emergence, and the apparent ones
derived from sunspot data. The duration of the growth phase of solar regions
has been up to now underestimated.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:24:20 GMT"
}
] | 2008-02-12T00:00:00 | [
[
"Dalla",
"S.",
""
],
[
"Fletcher",
"L.",
""
],
[
"Walton",
"N. A.",
""
]
] | [
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] |
801.0704 | Albert Linnell | Albert P. Linnell, Patrick Godon, Ivan Hubeny, Edward M. Sion, Paula
Szkody, and Paul E. Barrett | Synthetic Spectrum Constraints on a Model of the Cataclysmic Variable QU
Carinae | 52 pages, 19 Figures | null | 10.1086/529118 | null | astro-ph | null | Neither standard model SEDs nor truncated standard model SEDs fit observed
spectra of QU Carinae with acceptable accuracy over the range 900\AA to
3000\AA. Non-standard model SEDs fit the observation set accurately. The
non-standard accretion disk models have a hot region extending from the white
dwarf to $R=1.36R_{\rm wd}$,a narrow intermediate temperature annulus, and an
isothermal remainder to the tidal cutoff boundary. The models include a range
of $\dot{M}$ values between $1.0{\times}10^{-7}M_{\odot} {\rm yr}^{-1}$ and
$1.0{\times}10^{-6}M_{\odot} {\rm yr}^{-1}$ and limiting values of $M_{\rm wd}$
between $0.6M_{\odot}$ and $1.2M_{\odot}$. A solution with $M_{\rm
wd}=1.2M_{\odot}$ is consistent with an empirical mass-period relation. The set
of models agree on a limited range of possible isothermal region $T_{\rm eff}$
values between 14,000K and 18,000K. The model-to-model residuals are so similar
that it is not possible to choose a best model. The Hipparcos distance, 610 pc,
is representative of the model results. The orbital inclination is between
$40\arcdeg$ and $60\arcdeg$.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:45:03 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Linnell",
"Albert P.",
""
],
[
"Godon",
"Patrick",
""
],
[
"Hubeny",
"Ivan",
""
],
[
"Sion",
"Edward M.",
""
],
[
"Szkody",
"Paula",
""
],
[
"Barrett",
"Paul E.",
""
]
] | [
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801.0705 | Leo Medeiros Gouvea | R. Aldrovandi, R.R. Cuzinatto, L. G. Medeiros | Realistic Equations of State for the Primeval Universe | 32 pages, 5 figures. Citations added in this version. Accepted EPJC | Eur.Phys.J.C58:483-497,2008 | 10.1140/epjc/s10052-008-0780-6 | null | astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Early universe equations of state including realistic interactions between
constituents are built up. Under certain reasonable assumptions, these
equations are able to generate an inflationary regime prior to the
nucleosynthesis period. The resulting accelerated expansion is intense enough
to solve the flatness and horizon problems. In the cases of curvature parameter
\kappa equal to 0 or +1, the model is able to avoid the initial singularity and
offers a natural explanation for why the universe is in expansion.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 18:18:24 GMT"
},
{
"version": "v2",
"created": "Tue, 21 Oct 2008 21:03:30 GMT"
}
] | 2008-12-18T00:00:00 | [
[
"Aldrovandi",
"R.",
""
],
[
"Cuzinatto",
"R. R.",
""
],
[
"Medeiros",
"L. G.",
""
]
] | [
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] |
801.0706 | Rhaana L. C. Starling | R.L.C. Starling (University of Leicester, UK) | Strong spectral evolution during the prompt emission of GRB 070616 | 4 pages, 2 figures (Fig 1 in colour), contributed talk, submitted to
the proceedings of Gamma Ray Bursts 2007, Santa Fe, New Mexico, November 5-9
2007 | AIP Conf.Proc.1000:113-116,2008 | 10.1063/1.2943421 | null | astro-ph | null | Swift has revealed features in GRB early light curves, such as steep decays
and X-ray flares, whose properties are consistent with an internal origin
though they are far from understood. The steep X-ray decay is often explained
using the curvature effect; however a significant number of GRBs display strong
spectral evolution during this phase, and a new mechanism must be invoked to
explain this. Of particular interest are the longest duration GRBs in which the
early emission can be studied in most detail. Here we present data for GRB
070616, in which the prompt emission shows a complex multipeaked structure,
leading to one of the longest prompt emission durations ever recorded. We take
advantage of extensive coverage of such a long burst by all Swift instruments.
Combining data from Swift and Suzaku we study the evolution of the prompt
emission spectrum, following the temporal variability of the peak energy and
spectral slope.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 16:51:45 GMT"
}
] | 2009-06-23T00:00:00 | [
[
"Starling",
"R. L. C.",
"",
"University of Leicester, UK"
]
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801.0707 | Morten Bache | M. Bache, O. Bang, W. Krolikowski, J. Moses, and F. W. Wise | Limits to compression with cascaded quadratic soliton compressors | 16 pages, 5 figures, submitted to Optics Express | Optics Express, Vol. 16, Issue 5, pp. 3273-3287 (2008),
http://www.opticsexpress.org/abstract.cfm?id=154644 | 10.1364/OE.16.003273 | null | physics.optics | null | We study cascaded quadratic soliton compressors and address the physical
mechanisms that limit the compression. A nonlocal model is derived, and the
nonlocal response is shown to have an additional oscillatory component in the
nonstationary regime when the group-velocity mismatch (GVM) is strong. This
inhibits efficient compression. Raman-like perturbations from the cascaded
nonlinearity, competing cubic nonlinearities, higher-order dispersion, and
soliton energy may also limit compression, and through realistic numerical
simulations we point out when each factor becomes important. We find that it is
theoretically possible to reach the single-cycle regime by compressing
high-energy fs pulses for wavelengths $\lambda=1.0-1.3 \mu{\rm m}$ in a
$\beta$-barium-borate crystal, and it requires that the system is in the
stationary regime, where the phase mismatch is large enough to overcome the
detrimental GVM effects. However, the simulations show that reaching
single-cycle duration is ultimately inhibited by competing cubic nonlinearities
as well as dispersive waves, that only show up when taking higher-order
dispersion into account.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:22:13 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Bache",
"M.",
""
],
[
"Bang",
"O.",
""
],
[
"Krolikowski",
"W.",
""
],
[
"Moses",
"J.",
""
],
[
"Wise",
"F. W.",
""
]
] | [
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] |
801.0708 | Igor Shovkovy | V. P. Gusynin, V. A. Miransky, S. G. Sharapov, I. A. Shovkovy and C.M.
Wyenberg | Edge states on graphene ribbon in magnetic field: interplay between
Dirac and ferromagnetic-like gaps | 13 pages, 7 figures. v2: analysis for ribbons with armchair edges
added, to appear in Phys. Rev. B | Phys. Rev. B 79, 115431 (2009) | 10.1103/PhysRevB.79.115431 | UWO-TH-08/1 | cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By combining analytic and numerical methods, edge states on a finite width
graphene ribbon in a magnetic field are studied in the framework of low-energy
effective theory that takes into account the possibility of quantum Hall
ferromagnetism (QHF) gaps and dynamically generated Dirac-like masses. The
analysis is done for graphene ribbons with both zigzag and armchair edges. The
characteristic features of the spectrum of the edge states in both these cases
are described. In particular, the conditions for the existence of the gapless
edge states are established. Implications of these results for the
interpretation of recent experiments are discussed.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:09:45 GMT"
},
{
"version": "v2",
"created": "Tue, 27 Jan 2009 16:07:07 GMT"
}
] | 2009-03-25T00:00:00 | [
[
"Gusynin",
"V. P.",
""
],
[
"Miransky",
"V. A.",
""
],
[
"Sharapov",
"S. G.",
""
],
[
"Shovkovy",
"I. A.",
""
],
[
"Wyenberg",
"C. M.",
""
]
] | [
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] |
801.0709 | Arun Ram | James Parkinson, Arun Ram, Christoph Schwer | Combinatorics in affine flag varieties | 21 pages, | null | null | null | math.RT math.CO | null | The Littelmann path moel gives a realization of the crystals of integrable
representations of symmetrizable Kac-Moody Lie algebras. Recent work of
Gaussent-Littelmann and others has demonstrated a connection between this model
and the geometry of the loop Grassmannian. The alcove walk model is a version
of the path model which is intimately connected to the combinatorics of the
affine Hecke algebra. In this paper we define a refined alcove walk model which
encodes the points of the affine flag variety. We show that this combinatorial
indexing naturally indexes the "cells" in generalized Mirkovic-Vilonen
intersections.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:16:07 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Parkinson",
"James",
""
],
[
"Ram",
"Arun",
""
],
[
"Schwer",
"Christoph",
""
]
] | [
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] |
801.071 | Mats Andersson | Mats Andersson, H{\aa}kan Samuelsson | Koppelman formulas and the $\dbar$-equation on an analytic space | null | null | null | null | math.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Let $X$ be an analytic space of pure dimension. We introduce a formalism to
generate intrinsic weighted Koppelman formulas on $X$ that provide solutions to
the $\dbar$-equation. We prove that if $\phi$ is a smooth $(0,q+1)$-form on a
Stein space $X$ with $\dbar\phi=0$, then there is a smooth $(0,q)$-form $\psi$
on $X_{reg}$ with at most polynomial growth at $X_{sing}$ such that
$\dbar\psi=\phi$. The integral formulas also give other new existence results
for the $\dbar$-equation and Hartogs theorems, as well as new proofs of various
known results.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:19:07 GMT"
},
{
"version": "v2",
"created": "Mon, 11 Feb 2008 16:49:10 GMT"
},
{
"version": "v3",
"created": "Tue, 23 Sep 2008 07:39:42 GMT"
}
] | 2016-08-14T00:00:00 | [
[
"Andersson",
"Mats",
""
],
[
"Samuelsson",
"Håkan",
""
]
] | [
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] |
801.0711 | Joseph Fu | Andreas Bernig and Joseph H.G. Fu | Hermitian integral geometry | To appear in Ann. of Math. Version for publication | Ann. of Math. 173 (2011), 907-945 | null | null | math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give in explicit form the principal kinematic formula for the action of
the affine unitary group on $\C^n$, together with a straightforward algebraic
method for computing the full array of unitary kinematic formulas, expressed in
terms of certain convex valuations introduced, essentially, by H. Tasaki. We
introduce also several other canonical bases for the algebra of
unitary-invariant valuations, explore their interrelations, and characterize in
these terms the cones of positive and monotone elements.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:23:24 GMT"
},
{
"version": "v2",
"created": "Sat, 5 Jan 2008 19:06:50 GMT"
},
{
"version": "v3",
"created": "Fri, 11 Jan 2008 15:34:09 GMT"
},
{
"version": "v4",
"created": "Sun, 13 Jan 2008 11:52:09 GMT"
},
{
"version": "v5",
"created": "Tue, 25 Mar 2008 15:53:07 GMT"
},
{
"version": "v6",
"created": "Thu, 19 Feb 2009 14:39:41 GMT"
},
{
"version": "v7",
"created": "Thu, 2 Jul 2009 19:40:10 GMT"
},
{
"version": "v8",
"created": "Tue, 1 Sep 2009 15:30:40 GMT"
},
{
"version": "v9",
"created": "Tue, 12 Jan 2010 16:37:07 GMT"
}
] | 2011-04-19T00:00:00 | [
[
"Bernig",
"Andreas",
""
],
[
"Fu",
"Joseph H. G.",
""
]
] | [
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801.0712 | Hanna Jankowski | Hanna K. Jankowski, Jon A. Wellner | Nonparametric estimation of a convex bathtub-shaped hazard function | Published in at http://dx.doi.org/10.3150/09-BEJ202 the Bernoulli
(http://isi.cbs.nl/bernoulli/) by the International Statistical
Institute/Bernoulli Society (http://isi.cbs.nl/BS/bshome.htm) | Bernoulli 2009, Vol. 15, No. 4, 1010-1035 | 10.3150/09-BEJ202 | IMS-BEJ-BEJ202 | math.ST stat.TH | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the nonparametric maximum likelihood estimator (MLE)
of a convex hazard function. We show that the MLE is consistent and converges
at a local rate of $n^{2/5}$ at points $x_0$ where the true hazard function is
positive and strictly convex. Moreover, we establish the pointwise asymptotic
distribution theory of our estimator under these same assumptions. One notable
feature of the nonparametric MLE studied here is that no arbitrary choice of
tuning parameter (or complicated data-adaptive selection of the tuning
parameter) is required.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:55:06 GMT"
},
{
"version": "v2",
"created": "Thu, 14 Jan 2010 08:46:23 GMT"
}
] | 2010-01-14T00:00:00 | [
[
"Jankowski",
"Hanna K.",
""
],
[
"Wellner",
"Jon A.",
""
]
] | [
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] |
801.0713 | Letian Ding | Letian Ding, Noah Bray-Ali, Rong Yu and Stephan Haas | Subarea law of entanglement in nodal fermionic systems | 4 pages,4 figures; published version | Phys. Rev. Lett. 100, 215701 (2008) | 10.1103/PhysRevLett.100.215701 | null | cond-mat.str-el cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the subarea law scaling properties of the block entropy in
bipartite fermionic systems which do not have a finite Fermi surface. It is
found that in gapped regimes the leading subarea term is a negative constant,
whereas in critical regimes with point nodes the leading subarea law is a
logarithmic additive term. At the phase boundary that separates the critical
and non-critical regimes, the subarea scaling shows power-law behavior.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 17:48:33 GMT"
},
{
"version": "v2",
"created": "Wed, 24 Sep 2008 18:00:35 GMT"
}
] | 2008-09-24T00:00:00 | [
[
"Ding",
"Letian",
""
],
[
"Bray-Ali",
"Noah",
""
],
[
"Yu",
"Rong",
""
],
[
"Haas",
"Stephan",
""
]
] | [
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] |
801.0714 | James Cheney | James Cheney | Regular Expression Subtyping for XML Query and Update Languages | ESOP 2008. Companion technical report with proofs | null | null | null | cs.PL cs.DB | null | XML database query languages such as XQuery employ regular expression types
with structural subtyping. Subtyping systems typically have two presentations,
which should be equivalent: a declarative version in which the subsumption rule
may be used anywhere, and an algorithmic version in which the use of
subsumption is limited in order to make typechecking syntax-directed and
decidable. However, the XQuery standard type system circumvents this issue by
using imprecise typing rules for iteration constructs and defining only
algorithmic typechecking, and another extant proposal provides more precise
types for iteration constructs but ignores subtyping. In this paper, we
consider a core XQuery-like language with a subsumption rule and prove the
completeness of algorithmic typechecking; this is straightforward for XQuery
proper but requires some care in the presence of more precise iteration typing
disciplines. We extend this result to an XML update language we have introduced
in earlier work.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 18:13:48 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Cheney",
"James",
""
]
] | [
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] |
801.0715 | Grenville Croll | Stephen G. Powell, Barry Lawson, and Kenneth R. Baker | Impact of Errors in Operational Spreadsheets | 12 pages including references | Proc. European Spreadsheet Risks Int. Grp. 2007 57-68 ISBN
978-905617-58-6 | null | null | cs.CY | null | All users of spreadsheets struggle with the problem of errors. Errors are
thought to be prevalent in spreadsheets, and in some instances they have cost
organizations millions of dollars. In a previous study of 50 operational
spreadsheets we found errors in 0.8% to 1.8% of all formula cells, depending on
how errors are defined. In the current study we estimate the quantitative
impacts of errors in 25 operational spreadsheets from five different
organizations. We find that many errors have no quantitative impact on the
spreadsheet. Those that have an impact often affect unimportant portions of the
spreadsheet. The remaining errors do sometimes have substantial impacts on key
aspects of the spreadsheet. This paper provides the first fully-documented
evidence on the quantitative impact of errors in operational spreadsheets.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 18:26:10 GMT"
}
] | 2008-03-10T00:00:00 | [
[
"Powell",
"Stephen G.",
""
],
[
"Lawson",
"Barry",
""
],
[
"Baker",
"Kenneth R.",
""
]
] | [
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801.0716 | Brian Jackson | Brian Jackson, Richard Greenberg, Rory Barnes | Tidal Evolution of Close-in Extra-Solar Planets | accepted to ApJ | null | null | null | astro-ph | null | The distribution of eccentricities e of extra-solar planets with semi-major
axes a > 0.2 AU is very uniform, and values for e are relatively large,
averaging 0.3 and broadly distributed up to near 1. For a < 0.2 AU,
eccentricities are much smaller (most e < 0.2), a characteristic widely
attributed to damping by tides after the planets formed and the protoplanetary
gas disk dissipated. Most previous estimates of the tidal damping considered
the tides raised on the planets, but ignored the tides raised on the stars.
Most also assumed specific values for the planets' poorly constrained tidal
dissipation parameter Qp. Perhaps most important, in many studies, the strongly
coupled evolution between e and a was ignored. We have now integrated the
coupled tidal evolution equations for e and a over the estimated age of each
planet, and confirmed that the distribution of initial e values of close-in
planets matches that of the general population for reasonable Q values, with
the best fits for stellar and planetary Q being ~10^5.5 and ~10^6.5,
respectively. The accompanying evolution of a values shows most close-in
planets had significantly larger a at the start of tidal migration. The earlier
gas disk migration did not bring all planets to their current orbits. The
current small values of a were only reached gradually due to tides over the
lifetimes of the planets. These results may have important implications for
planet formation models, atmospheric models of "hot Jupiters", and the success
of transit surveys.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:05:18 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Jackson",
"Brian",
""
],
[
"Greenberg",
"Richard",
""
],
[
"Barnes",
"Rory",
""
]
] | [
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] |
801.0717 | Anirban Pathak | Amit Verma and Anirban Pathak | Reduction of Quantum Phase Fluctuations in Intermediate States | 10 pages, 5 figures | Phys. Lett A 373 (2009) 1421 | 10.1016/j.physleta.2009.02.038 | null | quant-ph | null | Recently we have shown that the reduction of the Carruthers-Nieto symmetric
quantum phase fluctuation parameter (U) with respect to its coherent state
value corresponds to an antibunched state, but the converse is not true.
Consequently reduction of U is a stronger criterion of nonclassicality than the
lowest order antibunching. Here we have studied the possibilities of reduction
of $U$ in intermediate states by using the Barnett Pegg formalism. We have
shown that the reduction of phase fluctuation parameter U can be seen in
different intermediate states, such as binomial state, generalized binomial
state, hypergeometric state, negative binomial state, and photon added coherent
state. It is also shown that the depth of nonclassicality can be controlled by
various parameters related to intermediate states. Further, we have provided
specific examples of antibunched states, for which $U$ is greater than its
poissonian state value.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:08:02 GMT"
}
] | 2022-06-07T00:00:00 | [
[
"Verma",
"Amit",
""
],
[
"Pathak",
"Anirban",
""
]
] | [
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] |
801.0718 | Erhan Bayraktar | Erhan Bayraktar, Hasanjan Sayit | On the Stickiness Property | Key words: Transaction costs. No Arbitrage. Sticky processes. Time
change | null | null | null | q-fin.PR math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In [2] the notion of stickiness for stochastic processes was introduced. It
was also shown that stickiness implies absense of arbitrage in a market with
proportional transaction costs. In this paper, we investigate the notion of
stickiness further. In particular, we give examples of processes that are not
semimartingales but are sticky.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:41:05 GMT"
},
{
"version": "v2",
"created": "Tue, 15 Jan 2008 17:53:21 GMT"
},
{
"version": "v3",
"created": "Sat, 27 Sep 2008 22:07:57 GMT"
},
{
"version": "v4",
"created": "Mon, 14 Sep 2009 18:04:53 GMT"
}
] | 2009-09-14T00:00:00 | [
[
"Bayraktar",
"Erhan",
""
],
[
"Sayit",
"Hasanjan",
""
]
] | [
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801.0719 | Michael Macy | Arnout Van de Rijt, David Siegel, Michael Macy | Neighborhood Chance and Neighborhood Change | Forthcoming in American Journal of Sociology | null | null | null | nlin.AO physics.soc-ph | null | WITHDRAWAL NOTICE
This paper has been withdrawn by the authors as required by the American
Journal of Sociology, which has accepted the paper for publication. AJS will
not publish papers if the preprint remains posted on arXiv.
| [
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},
{
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"created": "Sun, 27 Jan 2008 22:13:00 GMT"
}
] | 2008-01-28T00:00:00 | [
[
"Van de Rijt",
"Arnout",
""
],
[
"Siegel",
"David",
""
],
[
"Macy",
"Michael",
""
]
] | [
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801.072 | Marco Aurelio Cattacin Kneipp | Marco A. C. Kneipp | Hitchin's equations and integrability of BPS Z(N) strings in Yang-Mills
theories | 13 pages. Some comments and references added; change of a convention
(Eq. (9)); version to appear in JHEP | JHEP 0811:049,2008 | 10.1088/1126-6708/2008/11/049 | null | hep-th hep-lat nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that Z(N) string's BPS equations are equivalent to the Hitchin's
equations (or self-duality equation) and also to the zero curvature condition.
We construct a general form for BPS Z(N) string solutions for arbitrary simple
gauge groups with non-trivial center. Depending on the vacuum solutions
considered, the Z(N) string's BPS equations reduce to different two dimensional
integrable field equations. For a particular vacuum we obtain the equation of
affine Toda field theory.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:25:49 GMT"
},
{
"version": "v2",
"created": "Wed, 19 Nov 2008 01:45:11 GMT"
}
] | 2009-12-15T00:00:00 | [
[
"Kneipp",
"Marco A. C.",
""
]
] | [
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801.0721 | Sonia Schirmer | Sonia G. Schirmer, Ivan C. H. Pullen, Peter J. Pemberton-Ross | Global controllability with a single local actuator | 7 pages, 1 table, no figures | Phys. Rev. A 78, 062339 (2008) | 10.1103/PhysRevA.78.062339 | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that we can achieve global density-operator controllability for most
N-dimensional bilinear Hamiltonian control systems with general fixed couplings
using a single, locally-acting actuator that modulates one energy-level
transition. Controllability depends upon the position of the actuator and
relies on the absence of either decompositions into non-interacting subgroups
or symmetries restricting the dynamics to a subgroup of SU(N). These results
are applied to spin-chain systems and used to explicitly construct control
sequences for a single binary-valued switch actuator.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:27:05 GMT"
},
{
"version": "v2",
"created": "Fri, 6 Jun 2008 10:57:15 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Schirmer",
"Sonia G.",
""
],
[
"Pullen",
"Ivan C. H.",
""
],
[
"Pemberton-Ross",
"Peter J.",
""
]
] | [
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801.0722 | Jeremy Clark | Jeremy Clark | An infinite-temperature limit for a quantum scattering process | 18 pages | Rep. Math. Phys. 63 (2009) 131-152. | 10.1016/S0034-4877(09)90009-X | null | math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a quantum dynamical semigroup driven by a Lindblad generator with a
deterministic Schr\"odinger part and a noisy Poission-timed scattering part.
The dynamics describes the evolution of a test particle in $\R^{n}$, $n=1,2,3$,
immersed in a gas, and the noisy scattering part is defined by the reduced
effect of an individual interaction, where the interaction between the test
particle and a single gas particle is via a repulsive point potential. In the
limit that the mass ratio $\lambda=\frac{m}{M}$ tends to zero and the
collisions become more frequent as $\frac{1}{\lambda}$, we show that our
dynamics $\Phi_{t,\lambda}$ approaches a limiting dynamics
$\Phi_{t,\lambda}^{\diamond}$ with second order error. Working in the
Heisenberg representation, for $G\in \Bi(L^{2}(\R^{n}))$ $n=1,3$ we bound the
difference between $\Phi_{t,\lambda}(G)$ and $\Phi_{t,\lambda}^{\diamond}(G)$
in operator norm proportional to $\lambda^{2}$.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:49:07 GMT"
},
{
"version": "v2",
"created": "Thu, 31 Jul 2008 17:40:22 GMT"
},
{
"version": "v3",
"created": "Fri, 12 Dec 2008 14:38:57 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Clark",
"Jeremy",
""
]
] | [
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801.0723 | Ribhu Krishna Kaul | Ribhu K. Kaul and Subir Sachdev | Quantum criticality of U(1) gauge theories with fermionic and bosonic
matter in two spatial dimensions | 30 pages, 8 figures | Phys. Rev. B 77, 155105 (2008) | 10.1103/PhysRevB.77.155105 | null | cond-mat.str-el | null | We consider relativistic U(1) gauge theories in 2+1 dimensions, with N_b
species of complex bosons and N_f species of Dirac fermions at finite
temperature. The quantum phase transition between the Higgs and Coulomb phases
is described by a conformal field theory (CFT). At large N_b and N_f, but for
arbitrary values of the ratio N_b/N_f, we present computations of various
critical exponents and universal amplitudes for these CFTs. We make contact
with the different spin-liquids, charge-liquids and deconfined critical points
of quantum magnets that these field theories describe. We compute physical
observables that may be measured in experiments or numerical simulations of
insulating and doped quantum magnets.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:45:45 GMT"
},
{
"version": "v2",
"created": "Sun, 6 Jan 2008 20:47:52 GMT"
}
] | 2008-04-07T00:00:00 | [
[
"Kaul",
"Ribhu K.",
""
],
[
"Sachdev",
"Subir",
""
]
] | [
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] |
801.0724 | Grigory Volovik | G.E. Volovik | Emergent physics: Fermi point scenario | 16 pages, 8 figures, submitted to proceedings of Royal Society
scientific discussion meeting "Cosmology meets condensed matter" held on 28
January 2008 in London, references added | Phil.Trans.Roy.Soc.Lond.A366:2935-2951,2008 | 10.1098/rsta.2008.0070 | null | gr-qc cond-mat.str-el hep-ph | null | The Fermi-point scenario of emergent gravity has the following consequences:
gravity emerges together with fermionic and bosonic matter; emergent fermionic
matter consists of massless Weyl fermions; emergent bosonic matter consists of
gauge fields; Lorentz symmetry persists well above the Planck energy;
space-time is naturally 4-dimensional; Universe is naturally flat; cosmological
constant is naturally small or zero; underlying physics is based on discrete
symmetries; `quantum gravity' cannot be obtained by quantization of Einstein
equations; there is no contradiction between quantum mechanics and gravity;
etc.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:40:01 GMT"
},
{
"version": "v2",
"created": "Tue, 8 Jan 2008 11:11:04 GMT"
},
{
"version": "v3",
"created": "Thu, 10 Jan 2008 10:54:19 GMT"
},
{
"version": "v4",
"created": "Tue, 22 Jan 2008 14:31:55 GMT"
},
{
"version": "v5",
"created": "Thu, 31 Jan 2008 15:19:42 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Volovik",
"G. E.",
""
]
] | [
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801.0725 | Francois Renard | Sergei Zubtsov (LGIT), Fran\c{c}ois Renard (LGIT, PGP), Jean-Pierre
Gratier (LGIT), Dag Dysthe (PGP), Vladimir Traskine | Single-contact pressure solution creep on calcite monocrystals | null | Deformation Mechanisms, Rheology and Tectonics: from Minerals to
the Lithosphere, Geological Society of London (Ed.) (2005) 67_79 | null | null | physics.geo-ph | null | Pressure solution creep rates and interface structures have been measured by
two methods on calcite single crystals. In the first kind of experiments,
calcite monocrystals were indented at 40 degrees C for six weeks using ceramic
indenters under stresses in the 50-200 MPa range in a saturated solution of
calcite and in a calcite-saturated aqueous solution of NH4Cl. The deformation
(depth of the hole below the indenter) is measured ex-situ at the end of the
experiment. In the second type of experiment, calcite monocrystals were
indented by spherical glass indenters for 200 hours under stresses in the 0-100
MPa range at room temperature in a saturated aqueous solution of calcite. The
displacement of the indenter was continuously recorded using a specially
constructed differential dilatometer. The experiments conducted in a
calcite-saturated aqueous solution of NH4Cl show an enhanced indentation rate
owing to the fairly high solubility of calcite in this solution. In contrast,
the experiments conducted in a calcite-saturated aqueous solution show moderate
indentation rate and the dry control experiments did not show any measurable
deformation. The rate of calcite indentation is found to be inversely
proportional to the indenter diameter, thus indicating that the process is
diffusion-controlled. The microcracks in the dissolution region under the
indenter dramatically enhance the rate of calcite indentation by a significant
reduction of the distance of solute transport in the trapped fluid phase. This
result indicates that care should be taken in extrapolating the kinetic data of
pressure solution creep from one mineral to another.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:44:44 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Zubtsov",
"Sergei",
"",
"LGIT"
],
[
"Renard",
"François",
"",
"LGIT, PGP"
],
[
"Gratier",
"Jean-Pierre",
"",
"LGIT"
],
[
"Dysthe",
"Dag",
"",
"PGP"
],
[
"Traskine",
"Vladimir",
""
]
] | [
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801.0726 | Gilles Pages | Gilles Pag\`es (PMA), Afef Sellami (PMA) | Convergence of multi-dimensional quantized $SDE$'s | 43 pages | S\'eminaire de Probabilit\'es 2006 (Lecture Notes in Math.) (2011)
269-307 | 10.1007/978-3-642-15217-7_11 | null | math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We quantize a multidimensional $SDE$ (in the Stratonovich sense) by solving
the related system of $ODE$'s in which the $d$-dimensional Brownian motion has
been replaced by the components of functional stationary quantizers. We make a
connection with rough path theory to show that the solutions of the quantized
solutions of the $ODE$ converge toward the solution of the $SDE$. On our way to
this result we provide convergence rates of optimal quantizations toward the
Brownian motion for $\frac 1q$-H\" older distance, $q>2$, in $L^p(\P)$.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:47:33 GMT"
},
{
"version": "v2",
"created": "Tue, 6 Jul 2010 08:06:26 GMT"
}
] | 2013-04-03T00:00:00 | [
[
"Pagès",
"Gilles",
"",
"PMA"
],
[
"Sellami",
"Afef",
"",
"PMA"
]
] | [
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] |
801.0727 | Marc Bellon | Marc Bellon (LPTHE, Cefimas), Fidel A. Schaposnik (CEFIMAS) | Renormalization group functions for the Wess-Zumino model: up to 200
loops through Hopf algebras | Changed title, match the version to be published in Nucl. Phys. B 12
pages, 2 tables, | Nucl.Phys.A800:517-526,2008 | 10.1016/j.nuclphysb.2008.02.005 | null | hep-th math-ph math.MP | null | We obtain the contributions to the renormalization group functions of all the
diagrams containing the unique one-loop primitive divergence of a simple
supersymmetric Wess--Zumino model, up to more than 200 loops. The asymptotic
behavior of the coefficients in the expansion of the anomalous dimension is
analyzed.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:48:32 GMT"
},
{
"version": "v2",
"created": "Thu, 28 Feb 2008 07:22:00 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Bellon",
"Marc",
"",
"LPTHE, Cefimas"
],
[
"Schaposnik",
"Fidel A.",
"",
"CEFIMAS"
]
] | [
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] |
801.0728 | Derrick Hart | David Covert, Derrick Hart, Alex Iosevich, Doowon Koh, Misha Rudnev | Generalized incidence theorems, homogeneous forms, and sum-product
estimates in finite fields | null | null | null | null | math.CO math.CA | null | In recent years, sum-product estimates in Euclidean space and finite fields
have been studied using a variety of combinatorial, number theoretic and
analytic methods. Erdos type problems involving the distribution of distances,
areas and volumes have also received much attention. In this paper we prove a
relatively straightforward function version of an incidence results for points
and planes previously established in \cite{HI07} and \cite{HIKR07}. As a
consequence of our methods, we obtain sharp or near sharp results on the
distribution of volumes determined by subsets of vector spaces over finite
fields and the associated arithmetic expressions.
In particular, our machinery enables us to prove that if $E \subset {\Bbb
F}_q^d$, $d \ge 4$, the $d$-dimensional vector space over a finite field ${\Bbb
F}_q$, of size much greater than $q^{\frac{d}{2}}$, and if $E$ is a product
set, then the set of volumes of $d$-dimensional parallelepipeds determined by
$E$ covers ${\Bbb F}_q$. This result is sharp as can be seen by taking $E$ to
equal to $A \times A \times ... \times A$, where $A$ is a sub-field of ${\Bbb
F}_q$ of size $\sqrt{q}$. In three dimensions we establish the same result if
$|E| \gtrsim q^{{15/8}}$. We prove in three dimensions that the set of volumes
covers a positive proportion of ${\Bbb F}_q$ if $|E| \ge Cq^{{3/2}}$. Finally
we show that in three dimensions the set of volumes covers a positive
proportion of ${\Bbb F}_q$ if $|E| \ge Cq^2$, without any further assumptions
on $E$, which is again sharp as taking $E$ to be a 2-plane through the origin
shows.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:48:43 GMT"
},
{
"version": "v2",
"created": "Mon, 31 Mar 2008 12:57:11 GMT"
}
] | 2008-03-31T00:00:00 | [
[
"Covert",
"David",
""
],
[
"Hart",
"Derrick",
""
],
[
"Iosevich",
"Alex",
""
],
[
"Koh",
"Doowon",
""
],
[
"Rudnev",
"Misha",
""
]
] | [
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] |
801.0729 | Richard J. Furnstahl | R.J. Furnstahl, G. Rupak, T. Schaefer | Effective Field Theory and Finite Density Systems | 27 pages, 5 figures | Ann.Rev.Nucl.Part.Sci.58:1-25,2008 | 10.1146/annurev.nucl.58.110707.171142 | null | nucl-th | null | This review gives an overview of effective field theory (EFT) as applied at
finite density, with a focus on nuclear many-body systems. Uniform systems with
short-range interactions illustrate the ingredients and virtues of many-body
EFT and then the varied frontiers of EFT for finite nuclei and nuclear matter
are surveyed.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 19:53:47 GMT"
}
] | 2009-11-19T00:00:00 | [
[
"Furnstahl",
"R. J.",
""
],
[
"Rupak",
"G.",
""
],
[
"Schaefer",
"T.",
""
]
] | [
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] |
801.073 | Paul R. Anderson | Paul R. Anderson, Carmen Molina-Paris, David Evanich, and Gregory B.
Cook | Study of the preheating phase of chaotic inflation | PRD version, some changes and corrections, 37 pages, 10 figures | Phys.Rev.D78:083514,2008 | 10.1103/PhysRevD.78.083514 | null | hep-ph gr-qc hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Particle production and its effects on the inflaton field are investigated
during the preheating phase of chaotic inflation using a model consisting of a
massive scalar inflaton field coupled to N massless quantum scalar fields. The
effects of spacetime curvature and interactions between the quantum fields are
ignored. A large N expansion is used to obtain a coupled set of equations
including a backreaction equation for the classical inflaton field. Previous
studies of preheating using these equations have been done. Here the first
numerical solutions to the full set of equations are obtained for various
values of the coupling constant and the initial amplitude of the inflaton
field. States are chosen so that initially the backreaction effects on the
inflaton field are small and the mode equations for the quantum fields take the
form of Mathieu equations. Potential problems relating to the parametric
amplification of certain modes of the quantum fields are identified and
resolved. A detailed study of the damping of the inflaton field is undertaken.
Some predictions of previous studies are verified and some new results are
obtained.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:41:10 GMT"
},
{
"version": "v2",
"created": "Wed, 9 Jan 2008 18:59:37 GMT"
},
{
"version": "v3",
"created": "Tue, 14 Oct 2008 16:00:50 GMT"
}
] | 2008-11-07T00:00:00 | [
[
"Anderson",
"Paul R.",
""
],
[
"Molina-Paris",
"Carmen",
""
],
[
"Evanich",
"David",
""
],
[
"Cook",
"Gregory B.",
""
]
] | [
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] |
801.0731 | Nico Spronk | Ebrahim Samei, Nico Spronk, Ross Stokke | Biflatness and Pseudo-Amenability of Segal algebras | 26 pages | Can. J. Math.-J. Can. Math. 62 (2010) 845-869 | 10.4153/CJM-2010-044-4 | null | math.FA | null | We investigate generalized amenability and biflatness properties of various
(operator) Segal algebras in both the group algebra, L1(G), and the Fourier
algebra, A(G), of a locally compact group, G.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:05:36 GMT"
}
] | 2019-08-15T00:00:00 | [
[
"Samei",
"Ebrahim",
""
],
[
"Spronk",
"Nico",
""
],
[
"Stokke",
"Ross",
""
]
] | [
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] |
801.0732 | Yan V. Fyodorov | Yan V Fyodorov | On statistical mechanics of a single particle in high-dimensional random
landscapes | This is mainly a conference presentation summarizing results of
arXiv:0706.3776; arXiv:0711.4006 and arXiv:cond-mat/0610035. The work in
progress and some new results are briefly discussed in the last part | ACTA PHYSICA POLONICA B, vol. 38 (2007), pp. 4055-4066 | null | null | cond-mat.dis-nn cond-mat.stat-mech | null | We discuss recent results of the replica approach to statistical mechanics of
a single classical particle placed in a random N(>>1)-dimensional Gaussian
landscape. The particular attention is paid to the case of landscapes with
logarithmically growing correlations and to its recent generalisations. Those
landscapes give rise to a rich multifractal spatial structure of the associated
Boltzmann-Gibbs measure. We also briefly mention related results on counting
stationary points of random Gaussian surfaces, as well as ongoing research on
statistical mechanics in a random landscape constructed locally by adding many
squared Gaussian-distributed terms.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:07:09 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Fyodorov",
"Yan V",
""
]
] | [
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] |
801.0733 | Oded Hod | Noa Marom, Oded Hod, Gustavo E. Scuseria, and Leeor Kronik | Electronic Structure of Copper Phthalocyanine: a Comparative Density
Functional Theory Study | 18 pages, 4 Figure, 1 Table | null | 10.1063/1.2898540 | null | cond-mat.mtrl-sci | null | We present a systematic density functional theory study of the electronic
structure of copper phthalocyanine (CuPc), using several different (semi)-local
and hybrid functionals, and compare the results to experimental photoemission
data. We show that semi-local functionals fail qualitatively for CuPc,
primarily because of under-binding of localized orbitals due to
self-interaction errors. We discuss an appropriate choice of functional for
studies of CuPc/metal interfaces and suggest the Heyd-Scuseria-Ernzerhof
screened hybrid functional as a suitable compromise functional.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:15:05 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Marom",
"Noa",
""
],
[
"Hod",
"Oded",
""
],
[
"Scuseria",
"Gustavo E.",
""
],
[
"Kronik",
"Leeor",
""
]
] | [
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] |
801.0734 | Kevin Tucker | Kevin Tucker | Jumping Numbers on Algebraic Surfaces with Rational Singularities | Replaced Introduction, Includes Minor Revisions | null | null | null | math.AG | null | In this article, we study the jumping numbers of an ideal in the local ring
at rational singularity on a complex algebraic surface. By understanding the
contributions of reduced divisors on a fixed resolution, we are able to present
an algorithm for finding of the jumping numbers of the ideal. This shows, in
particular, how to compute the jumping numbers of a plane curve from the
numerical data of its minimal resolution. In addition, the jumping numbers of
the maximal ideal at the singular point in a Du Val or toric surface
singularity are computed, and applications to the smooth case are explored.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:35:42 GMT"
},
{
"version": "v2",
"created": "Sun, 17 Feb 2008 19:10:40 GMT"
}
] | 2008-02-17T00:00:00 | [
[
"Tucker",
"Kevin",
""
]
] | [
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] |
801.0735 | John Friedman | John L. Friedman and Atsushi Higuchi | Topological censorship and chronology protection | Dedicated to Rafael Sorkin, whose tutoring and friendship from third
grade on is responsible for one of us (JF) having spent his adult life in
physics and whose work has inspired both of us. In v.2, some references are
updated, and references are added to early work on 2+1 spacetimes and to work
on event-horizon topology | AnnalenPhys.15:109-128,2006 | 10.1002/andp.200510172 | null | gr-qc | null | Over the past two decades, substantial efforts have been made to understand
the way in which physics enforces the ordinary topology and causal structure
that we observe, from subnuclear to cosmological scales. We review the status
of topological censorship and the topology of event horizons; chronology
protection in classical and semiclassical gravity; and related progress in
establishing quantum energy inequalities.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:40:15 GMT"
},
{
"version": "v2",
"created": "Tue, 3 Jun 2008 19:39:17 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Friedman",
"John L.",
""
],
[
"Higuchi",
"Atsushi",
""
]
] | [
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] |
801.0736 | John Franks | John Franks and Michael Handel | Global fixed points for centralizers and Morita's Theorem | null | Geom. Topol. 13 (2009) 87-98 | 10.2140/gt.2009.13.87 | null | math.DS math.GT | null | We prove a global fixed point theorem for the centralizer of a homeomorphism
of the two dimensional disk $D$ that has attractor-repeller dynamics on the
boundary with at least two attractors and two repellers. As one application, we
show that there is a finite index subgroup of the centralizer of a
pseudo-Anosov homeomorphism with infinitely many global fixed points. As
another application we give an elementary proof of Morita's Theorem, that the
mapping class group of a closed surface $S$ of genus $g$ does not lift to the
group of diffeormorphisms of $S$ and we improve the lower bound for $g$ from 5
to 3.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:47:27 GMT"
}
] | 2014-11-11T00:00:00 | [
[
"Franks",
"John",
""
],
[
"Handel",
"Michael",
""
]
] | [
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] |
801.0737 | Alexander Katz | Alexander A. Katz and Oleg Friedman | On Existence and Uniqueness of Universal Enveloping Locally C*-Algebra
for a Locally JB-Algebra | 3 pages | null | null | null | math.OA math.FA | null | A theorem is presented on existence and uniqueness up to the topological
*-isomorphism of universal locally C*-algebra for an arbitrary locally
JB-algebra.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 20:47:44 GMT"
}
] | 2008-01-07T00:00:00 | [
[
"Katz",
"Alexander A.",
""
],
[
"Friedman",
"Oleg",
""
]
] | [
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] |
801.0738 | Helen Wong | Helen Wong | Quantum invariants can provide sharp Heegaard genus bounds | 8 pages | null | null | null | math.GT | null | Using Seifert fibered three-manifold examples of Boileau and Zieschang, we
demonstrate that the Reshetikhin-Turaev quantum invariants may be used to
provide a sharp lower bound on the Heegaard genus which is strictly larger than
the rank of the fundamental group.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 22:41:22 GMT"
},
{
"version": "v2",
"created": "Tue, 15 Jan 2008 22:54:28 GMT"
}
] | 2008-01-16T00:00:00 | [
[
"Wong",
"Helen",
""
]
] | [
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] |
801.0739 | Zsolt Frei | Zoltan Lippai (1), Zsolt Frei (1), and Zoltan Haiman (2) ((1) Inst. of
Physics, Eotvos University, Budapest, Hungary, (2) Dept. of Astronomy,
Columbia University, New York, NY) | Prompt Shocks in the Gas Disk Around a Recoiling Supermassive Black Hole
Binary | 4 pages, 3 figures, submitted to ApJL | null | 10.1086/587034 | null | astro-ph gr-qc | null | Supermassive black hole binaries (BHBs) produced in galaxy mergers recoil at
the time of their coalescence due to the emission of gravitational waves (GWs).
We simulate the response of a thin, 2D disk of collisionless particles,
initially on circular orbits around a 10^6 M_sun BHB, to kicks that are either
parallel or perpendicular to the initial orbital plane. Typical kick velocities
(v_k) can exceed the sound speed in a circumbinary gas disk. While the inner
disk is strongly bound to the recoiling binary, the outer disk is only weakly
bound or unbound. This leads to differential motions in the disturbed disk that
increase with radius and can become supersonic at ~700 Schwarzschild radii for
v_k ~500 km/s, implying that shocks form beyond this radius. We indeed find
that kicks in the disk plane lead to immediate strong density enhancements
(within weeks) in a tightly wound spiral caustic, propagating outward at the
speed v_k. Concentric density enhancements are also observed for kicks
perpendicular to the disk, but are weaker and develop into caustics only after
a long delay (>1 year). Unless both BH spins are low or precisely aligned with
the orbital angular momentum, a significant fraction (> several %) of kicks are
sufficiently large and well aligned with the orbital plane for strong shocks to
be produced. The shocks could result in an afterglow whose characteristic
photon energy increases with time, from the UV (~10eV) to the soft X-ray
(~100eV) range, between one month and one year after the merger. This could
help identify EM counterparts to GW sources discovered by LISA.
| [
{
"version": "v1",
"created": "Mon, 7 Jan 2008 15:28:28 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Lippai",
"Zoltan",
""
],
[
"Frei",
"Zsolt",
""
],
[
"Haiman",
"Zoltan",
""
]
] | [
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] |
801.074 | Stefano Profumo | Stefano Profumo (UC Santa Cruz) | Non-thermal X-rays from the Ophiuchus galaxy cluster and dark matter
annihilation | 6 pages, 4 figures, matches published version | Phys.Rev.D77:103510,2008 | 10.1103/PhysRevD.77.103510 | null | astro-ph hep-ph | null | We investigate a scenario where the recently discovered non-thermal hard
X-ray emission from the Ophiuchus cluster originates from inverse Compton
scattering of energetic electrons and positrons produced in weakly interacting
dark matter pair annihilations. We show that this scenario can account for both
the X-ray and the radio emission, provided the average magnetic field is of the
order of 0.1 microGauss. We demonstrate that GLAST will conclusively test the
dark matter annihilation hypothesis. Depending on the particle dark matter
model, GLAST might even detect the monochromatic line produced by dark matter
pair annihilation into two photons.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 21:00:07 GMT"
},
{
"version": "v2",
"created": "Wed, 14 May 2008 19:39:24 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Profumo",
"Stefano",
"",
"UC Santa Cruz"
]
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-0.0139729865,
0.0457410552,
0.008035088,
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] |
801.0741 | Saskia Hekker | S. Hekker, I.A.G. Snellen, C. Aerts, A. Quirrenbach, S. Reffert, D.S.
Mitchell | Precise radial velocities of giant stars. IV. A correlation between
surface gravity and radial velocity variation and a statistical investigation
of companion properties | 10 pages, accepted by A&A | null | 10.1051/0004-6361:20078321 | null | astro-ph | null | Since 1999, we have been conducting a radial velocity survey of 179 K giants
using the CAT at UCO/Lick observatory. At present ~20-100 measurements have
been collected per star with a precision of 5 to 8 m/s. Of the stars monitored,
145 (80%) show radial velocity (RV) variations at a level >20 m/s, of which 43
exhibit significant periodicities. Our aim is to investigate possible
mechanism(s) that cause these observed RV variations. We intend to test whether
these variations are intrinsic in nature, or possibly induced by companions, or
both. In addition, we aim to characterise the parameters of these companions. A
relation between log g and the amplitude of the RV variations is investigated
for all stars in the sample. Furthermore, the hypothesis that all periodic RV
variations are caused by companions is investigated by comparing their inferred
orbital statistics with the statistics of companions around main sequence
stars. A strong relation is found between the amplitude of the RV variations
and log g in K giant stars, as suggested earlier by Hatzes & Cochran (1998).
However, most of the stars exhibiting periodic variations are located above
this relation. These RV variations can be split in a periodic component which
is not correlated with log g and a random residual part which does correlate
with log g. Compared to main-sequence stars, K giants frequently exhibit
periodic RV variations. Interpreting these RV variations as being caused by
companions, the orbital param eters are different from the companions orbiting
dwarfs. Intrinsic mechanisms play an important role in producing RV variations
in K giants stars, as suggested by their dependence on log g. However, it
appears that periodic RV variations are additional to these intrinsic
variations, consistent with them being caused by companions.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 21:09:00 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Hekker",
"S.",
""
],
[
"Snellen",
"I. A. G.",
""
],
[
"Aerts",
"C.",
""
],
[
"Quirrenbach",
"A.",
""
],
[
"Reffert",
"S.",
""
],
[
"Mitchell",
"D. S.",
""
]
] | [
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] |
801.0742 | Rachel Bean | Rachel Bean, Daniel J.H. Chung, and Ghazal Geshnizjani | Reconstructing a general inflationary action | 16 pages, 1 figure, References added, typos corrected | Phys.Rev.D78:023517,2008 | 10.1103/PhysRevD.78.023517 | null | astro-ph hep-ph hep-th | null | If inflation is to be considered in an unbiased way, as possibly originating
from one of a wide range of underlying theories, then observations need not be
simply applied to reconstructing the inflaton potential, V(\phi), or a specific
kinetic term, as in DBI inflation, but rather to reconstruct the inflationary
action in its entirety. We discuss the constraints that can be placed on a
general single field action from measurements of the primordial scalar and
tensor fluctuation power spectra and non-Gaussianities. We also present the
flow equation formalism for reconstructing a general inflationary Lagrangian,
L(X,\phi), with X={1/2}\partial_\mu\phi\partial^\mu\phi, in a general gauge,
that reduces to canonical and DBI inflation in the specific gauge \partial
L/\partial X = c_s^{-1}.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 23:44:15 GMT"
},
{
"version": "v2",
"created": "Tue, 8 Jan 2008 20:35:13 GMT"
},
{
"version": "v3",
"created": "Wed, 2 Apr 2008 22:35:53 GMT"
}
] | 2008-12-18T00:00:00 | [
[
"Bean",
"Rachel",
""
],
[
"Chung",
"Daniel J. H.",
""
],
[
"Geshnizjani",
"Ghazal",
""
]
] | [
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] |
801.0743 | Iain W. Stewart | Ambar Jain, Ignazio Scimemi, Iain W. Stewart | Two-loop Jet-Function and Jet-Mass for Top Quarks | 25 pages, some typos corrected in text and references; 1 figure
replaced | Phys.Rev.D77:094008,2008 | 10.1103/PhysRevD.77.094008 | MIT-CTP 3916 | hep-ph hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the two-loop heavy quark jet-function in the heavy quark limit.
This is one of the key ingredients in next-to-next-to-leading order (NNLO) and
next-to-next-to-leading-log order (NNLL) computations of the invariant mass
distribution of top-jets at a future e+e- collider. The shape of the top
invariant mass distribution is affected by large logs which we compute at NNLL
order. Exploiting the non-abelian exponentiation theorem, a definition of the
top jet-mass is given which is transitive and whose renormalization group
evolution is determined by the cusp-anomalous dimension to all orders in
perturbation theory. Relations of the jet-mass to the pole, MSbar, and 1S
masses are presented at two-loop order.
| [
{
"version": "v1",
"created": "Mon, 7 Jan 2008 20:43:32 GMT"
},
{
"version": "v2",
"created": "Mon, 16 Jun 2008 15:11:03 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Jain",
"Ambar",
""
],
[
"Scimemi",
"Ignazio",
""
],
[
"Stewart",
"Iain W.",
""
]
] | [
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] |
801.0744 | Cenke Xu | Cenke Xu and Congjun Wu | Resonating plaquette phases in large spin cold atom systems | 6 pages, 3 figures | Phys. Rev. B 77, 134449 (2008) | 10.1103/PhysRevB.77.134449 | null | cond-mat.str-el cond-mat.stat-mech | null | Large spin cold atom systems can exhibit novel magnetic properties which do
not appear in usual spin-1/2 systems. We investigate the SU(4) resonating
plaquette state in the three dimensional cubic optical lattice with spin-3/2
cold fermions. A novel gauge field formalism is constructed to describe the
Rokhsar-Kivelson type of Hamiltonian and a duality transformation is used to
study the phase diagram. Due to the proliferation of topological defects, the
system is generally gapped for the whole phase diagram of the quantum model,
which agrees with the recent numerical studies. A critical line is found for
the classical plaquette system, which also corresponds to a quantum many-body
wavefunction in a "plaquette liquid phase".
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 21:04:42 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Xu",
"Cenke",
""
],
[
"Wu",
"Congjun",
""
]
] | [
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] |
801.0745 | Anders Basboll | Anders Basboll | SUSY Flat Direction Decay - the prospect of particle production and
preheating investigated in the unitary gauge | v2: particle production also possible with 1 flat direction,
$QLQLQLE^c$ v3: 2 papers added to references and included in the discussion
v4: typos corrected - in line with publication | Phys.Rev.D78:023528,2008 | 10.1103/PhysRevD.78.023528 | null | hep-th astro-ph hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We look at the possibility of non-perturbative particle production after
inflation from SUSY flat directions produced by rotating eigenstates thereby
avoiding the standard adiabaticity conditions. This might lead to preheating
and prevent the delay of thermalisation of the universe. We investigate the
flat directions $LLE^c$ and $U^cD^cD^c$ and find no particle production. These
2 directions are very important, since they have been named as possible
candidates for being the inflaton. We investigate $QLQLQLE^c$ and find particle
production and therefore the possibility of preheating. We investigate the
$LLE^c$ and $U^cD^cD^c$ directions appearing simultaneously, and find no
production. Finally, we investigate $LLE^c$ and $QLD^c$ simultaneously - with
one L-field in common. Here we do find particle production and therefore the
possibility of preheating. This means that if SUSY flat directions are to delay
thermalisation and thus explain the (lack of) gravitino production, it is
necessary to explain why complicated directions as $QLQLQLE^c$ are not exited,
and why combinations like $LLE^c$ and $QLD^c$ are not both exited.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 21:09:14 GMT"
},
{
"version": "v2",
"created": "Tue, 11 Mar 2008 19:09:58 GMT"
},
{
"version": "v3",
"created": "Thu, 8 May 2008 08:32:26 GMT"
},
{
"version": "v4",
"created": "Tue, 19 Aug 2008 09:18:51 GMT"
},
{
"version": "v5",
"created": "Thu, 22 Apr 2010 11:31:54 GMT"
}
] | 2010-04-23T00:00:00 | [
[
"Basboll",
"Anders",
""
]
] | [
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] |
801.0746 | Sonia Schirmer | Sonia G Schirmer and Peter J Pemberton-Ross and Xiaoting Wang | Comparative Analysis of Control Strategies | This work is part of a more comprehensive analysis of control
strategies, which has prompted further work such as our recent analysis of
the Lyapunov method. It was originally presented at PhysCon2007 and has
appeared in the Proceedings. Some figures are poor quality but the arXiv
robot wouldn't accept the original figures. Online at:
http://lib.physcon.ru/?item=1207 | Proceedings of PhysCon2007, IPACS Electronic Library | null | null | quant-ph | null | Different ways of modelling quantum control systems, formulating control
problems and solving the resulting problems are considered and compared. In
particular, we compare the performance of geometric and optimal control, as
well as iterative techniques for optimal control design versus local gradient
optimization using a Lyapunov-type potential function for two problems of
general interest: global control of qubits and entanglement generation in the
form of Bell state preparation.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 21:36:17 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Schirmer",
"Sonia G",
""
],
[
"Pemberton-Ross",
"Peter J",
""
],
[
"Wang",
"Xiaoting",
""
]
] | [
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] |
801.0747 | Ryo Suzuki | Yasuyuki Hatsuda, Ryo Suzuki | Finite-Size Effects for Dyonic Giant Magnons | 1+45 pages, 10 figures, v2: references added, discussion in section
3.2 corrected, v3: references added, minor corrections, v4: published
version, v5: Revised subsection 2.3, section 3 and some appendices to correct
mistakes. Added the case 1 < Q << g | Nucl.Phys.B800:349-383,2008 | 10.1016/j.nuclphysb.2008.04.007 | UT-07-41 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute finite-size corrections to dyonic giant magnons in two ways. One
is by examining the asymptotic behavior of helical strings of hep-th/0609026 as
elliptic modulus k goes to unity, and the other is by applying the generalized
Luscher formula for mu-term of arXiv:0708.2208 to the situation in which
incoming particles are boundstates. By careful choice of poles in the
su(2|2)^2-invariant S-matrix, we find agreement of the two results, which makes
possible to predict the (leading) finite-size correction for dyonic giant
magnons to all orders in the 't Hooft coupling.
| [
{
"version": "v1",
"created": "Sun, 6 Jan 2008 12:58:17 GMT"
},
{
"version": "v2",
"created": "Wed, 16 Jan 2008 19:10:54 GMT"
},
{
"version": "v3",
"created": "Wed, 30 Jan 2008 14:24:45 GMT"
},
{
"version": "v4",
"created": "Sun, 11 May 2008 13:54:00 GMT"
},
{
"version": "v5",
"created": "Wed, 15 Oct 2008 14:25:46 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Hatsuda",
"Yasuyuki",
""
],
[
"Suzuki",
"Ryo",
""
]
] | [
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] |
801.0748 | Ester Pantaleo Dr. | N. Basalto, R. Bellotti, F. De Carlo, P. Facchi, E. Pantaleo, S.
Pascazio | Hausdorff clustering | 12 pages, 13 figures | Phys. Rev. E 78, 046112 (2008) | 10.1103/PhysRevE.78.046112 | null | q-fin.ST cond-mat.stat-mech physics.data-an physics.soc-ph | null | A clustering algorithm based on the Hausdorff distance is introduced and
compared to the single and complete linkage. The three clustering procedures
are applied to a toy example and to the time series of financial data. The
dendrograms are scrutinized and their features confronted. The Hausdorff
linkage relies of firm mathematical grounds and turns out to be very effective
when one has to discriminate among complex structures.
| [
{
"version": "v1",
"created": "Mon, 7 Jan 2008 16:14:38 GMT"
}
] | 2010-01-30T00:00:00 | [
[
"Basalto",
"N.",
""
],
[
"Bellotti",
"R.",
""
],
[
"De Carlo",
"F.",
""
],
[
"Facchi",
"P.",
""
],
[
"Pantaleo",
"E.",
""
],
[
"Pascazio",
"S.",
""
]
] | [
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] |
801.0749 | Michael Scalora | D. de Ceglia, M.A. Vincenti, M.G. Cappeddu, M. Centini, N. Akozbek, A.
DOrazio, J.W. Haus, M.J. Bloemer, M. Scalora | Tailoring Metallodielectric Structures for Super Resolution and
Superguiding Applications in the Visible and Near IR Ranges | null | null | 10.1103/PhysRevA.77.033848 | null | physics.optics | null | We discuss propagation effects in realistic, transparent, metallo-dielectric
photonic band gap structures in the context of negative refraction and
super-resolution in the visible and near infrared ranges. In the resonance
tunneling regime, we find that for transverse-magnetic incident polarization,
field localization effects contribute to a waveguiding phenomenon that makes it
possible for the light to remain confined within a small fraction of a
wavelength, without any transverse boundaries, due to the suppression of
diffraction. This effect is related to negative refraction of the Poynting
vector inside each metal layer, balanced by normal refraction inside the
adjacent dielectric layer: The degree of field localization and material
dispersion together determine the total momentum that resides within any given
layer, and thus the direction of energy flow. We find that the transport of
evanescent wave vectors is mediated by the excitation of quasi-stationary, low
group velocity surface waves responsible for relatively large losses. As
representative examples we consider transparent metallo-dielectric stacks such
as Ag/TiO2 and Ag/GaP and show in detail how to obtain the optimum conditions
for high transmittance of both propagating and evanescent modes for
super-guiding and super resolution applications across the visible and near IR
ranges. Finally, we study the influence of gain on super-resolution. We find
that the introduction of gain can compensate the losses caused by the
excitation of surface plasmons, improves the resolving characteristics of the
lens, and leads to gain-tunable super-resolution.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 21:57:43 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"de Ceglia",
"D.",
""
],
[
"Vincenti",
"M. A.",
""
],
[
"Cappeddu",
"M. G.",
""
],
[
"Centini",
"M.",
""
],
[
"Akozbek",
"N.",
""
],
[
"DOrazio",
"A.",
""
],
[
"Haus",
"J. W.",
""
],
[
"Bloemer",
"M. J.",
""
],
[
"Scalora",
"M.",
""
]
] | [
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801.075 | EDA Publishing Association | P. Furjes, P. Csikvari, I. B\'arsony, Cs. Ducso | Micro-Hotplates for Thermal Characterisation of Structural Materials of
Mems | Submitted on behalf of TIMA Editions
(http://irevues.inist.fr/tima-editions) | Dans 13th International Worshop on THERMal INvestigations of ICs
and Systems - THERMINIC 2007, Budapest : Hongrie (2007) | null | null | physics.gen-ph | null | Accurate knowledge of mechanical and thermal properties of structural
materials used in MEMS is essential for optimum geometric and functional
design. The extraction of precise physical properties is rather complicated due
to the size effects, the complexity of the structures and the variations of
formation processes. This work is intended to determine the thermal properties
of silicon-nitride and diamond layers applied in thermal sensor structures by
analyzing thermal responses of a multilayer micro-heater structure.
| [
{
"version": "v1",
"created": "Mon, 7 Jan 2008 16:15:31 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Furjes",
"P.",
""
],
[
"Csikvari",
"P.",
""
],
[
"Bársony",
"I.",
""
],
[
"Ducso",
"Cs.",
""
]
] | [
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] |
801.0751 | George M. Bergman | George M. Bergman | On lattices and their ideal lattices, and posets and their ideal posets | 8 pages. Copy at http://math.berkeley.edu/~gbergman/papers may be
updated more frequently than arXiv copy. After publication, updates, errata,
etc. may be noted at that page | Tbilisi Math. J. 1 (2008) 89-103 | null | null | math.RA math.CO | null | For P a poset or lattice, let Id(P) denote the poset, respectively, lattice,
of upward directed downsets in P, including the empty set, and let
id(P)=Id(P)-\{\emptyset\}. This note obtains various results to the effect that
Id(P) is always, and id(P) often, "essentially larger" than P. In the first
vein, we find that a poset P admits no "<"-respecting map (and so in
particular, no one-to-one isotone map) from Id(P) into P, and, going the other
way, that an upper semilattice S admits no semilattice homomorphism from any
subsemilattice of itself onto Id(S).
The slightly smaller object id(P) is known to be isomorphic to P if and only
if P has ascending chain condition. This result is strengthened to say that the
only posets P_0 such that for every natural number n there exists a poset P_n
with id^n(P_n)\cong P_0 are those having ascending chain condition. On the
other hand, a wide class of cases is noted here where id(P) is embeddable in P.
Counterexamples are given to many variants of the results proved.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 22:08:52 GMT"
},
{
"version": "v2",
"created": "Fri, 9 May 2008 16:25:42 GMT"
}
] | 2013-05-10T00:00:00 | [
[
"Bergman",
"George M.",
""
]
] | [
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] |
801.0752 | Kim A. Venn | K.A. Venn, D.L. Lambert | Could the Ultra Metal-poor Stars be Chemically Peculiar and Not Related
to the First Stars? | Accepted for ApJ. 17 pages, 10 figures | null | 10.1086/529069 | null | astro-ph | null | Chemically peculiar stars define a class of stars that show unusual elemental
abundances due to stellar photospheric effects and not due to natal variations.
In this paper, we compare the elemental abundance patterns of the ultra
metal-poor stars with metallicities [Fe/H] $\sim -5 $ to those of a subclass of
chemically peculiar stars. These include post-AGB stars, RV Tauri variable
stars, and the Lambda Bootis stars, which range in mass, age, binarity, and
evolutionary status, yet can have iron abundance determinations as low as
[Fe/H] $\sim -5$. These chemical peculiarities are interpreted as due to the
separation of gas and dust beyond the stellar surface, followed by the
accretion of dust depleted-gas. Contrary to this, the elemental abundances in
the ultra metal-poor stars are thought to represent yields of the most
metal-poor supernova and, therefore, observationally constrain the earliest
stages of chemical evolution in the Universe. The abundance of the elements in
the photospheres of the ultra metal-poor stars appear to be related to the
condensation temperature of that element; if so, then their CNO abundances
suggest true metallicities of [X/H]~ -2 to -4, rather than their present
metallicities of [Fe/H] < -5.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 22:14:50 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Venn",
"K. A.",
""
],
[
"Lambert",
"D. L.",
""
]
] | [
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] |
801.0753 | Przemyslaw Biecek | Przemyslaw Biecek, Stanislaw Cebrat | Why Y chromosome is shorter and women live longer? | 8 pages, 5 figures | Eur. Phys. J. B 65, 149-153 (2008) | 10.1140/epjb/e2008-00325-4 | null | q-bio.PE | null | We have used the Penna ageing model to analyze how the differences in
evolution of sex chromosomes depend on the strategy of reproduction. In
panmictic populations, when females (XX) can freely choose the male partner
(XY) for reproduction from the whole population, the Y chromosome accumulates
defects and eventually the only information it brings is a male sex
determination. As a result of shrinking Y chromosome the males become
hemizygous in respect to the X chromosome content and are characterized by
higher mortality, observed also in the human populations. If it is assumed in
the model that the presence of the male is indispensable at least during the
pregnancy of his female partner and he cannot be seduced by another female at
least during the one reproduction cycle - the Y chromosome preserves its
content, does not shrink and the lifespan of females and males is the same.
Thus, Y chromosome shrinks not because of existing in one copy, without the
possibility of recombination, but because it stays under weaker selection
pressure; in panmictic populations without the necessity of being faithful, a
considerable fraction of males is dispensable and they can be eliminated from
the population without reducing its reproduction potential.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 22:27:20 GMT"
}
] | 2008-11-03T00:00:00 | [
[
"Biecek",
"Przemyslaw",
""
],
[
"Cebrat",
"Stanislaw",
""
]
] | [
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] |
801.0754 | Michael Bonitz | M. Bonitz, P. Ludwig, H. Baumgartner, C. Henning, A. Filinov, D.
Block, O. Arp, A. Piel, S. Kading, Y. Ivanov, A. Melzer, H. Fehske, V.
Filinov | Classical and quantum Coulomb crystals | 19 pages, 6 figures | Physics of Plasmas 15, 055704 (2008) | 10.1063/1.2839297 | null | physics.plasm-ph | null | Strong correlation effects in classical and quantum plasmas are discussed. In
particular, Coulomb (Wigner) crystallization phenomena are reviewed focusing on
one-component non-neutral plasmas in traps and on macroscopic two-component
neutral plasmas. The conditions for crystal formation in terms of critical
values of the coupling parameters and the distance fluctuations and the phase
diagram of Coulomb crystals are discussed.
| [
{
"version": "v1",
"created": "Mon, 7 Jan 2008 10:39:48 GMT"
}
] | 2009-09-29T00:00:00 | [
[
"Bonitz",
"M.",
""
],
[
"Ludwig",
"P.",
""
],
[
"Baumgartner",
"H.",
""
],
[
"Henning",
"C.",
""
],
[
"Filinov",
"A.",
""
],
[
"Block",
"D.",
""
],
[
"Arp",
"O.",
""
],
[
"Piel",
"A.",
""
],
[
"Kading",
"S.",
""
],
[
"Ivanov",
"Y.",
""
],
[
"Melzer",
"A.",
""
],
[
"Fehske",
"H.",
""
],
[
"Filinov",
"V.",
""
]
] | [
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] |
801.0755 | Alexander Retakh | Victor G. Kac, Alexander Retakh | Simple Jordan conformal superalgebras | null | null | null | null | math.QA math.RA | null | We classify simple finite Jordan conformal superalgebras and establish
preliminary results for the classification of simple finite Jordan
pseudoalgebras.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 22:29:29 GMT"
},
{
"version": "v2",
"created": "Tue, 6 May 2008 18:07:31 GMT"
}
] | 2008-05-06T00:00:00 | [
[
"Kac",
"Victor G.",
""
],
[
"Retakh",
"Alexander",
""
]
] | [
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] |
801.0756 | Nan Ma | Nan Ma, Prakash Ishwar | Distributed Source Coding for Interactive Function Computation | 30 pages, 6 figures. This work has been submitted to the IEEE for
possible publication. Parts of this work were presented at 2008 IEEE
International Symposium on Information Theory (ISIT'08) | null | null | null | cs.IT math.IT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A two-terminal interactive distributed source coding problem with alternating
messages for function computation at both locations is studied. For any number
of messages, a computable characterization of the rate region is provided in
terms of single-letter information measures. While interaction is useless in
terms of the minimum sum-rate for lossless source reproduction at one or both
locations, the gains can be arbitrarily large for function computation even
when the sources are independent. For a class of sources and functions,
interaction is shown to be useless, even with infinite messages, when a
function has to be computed at only one location, but is shown to be useful, if
functions have to be computed at both locations. For computing the Boolean AND
function of two independent Bernoulli sources at both locations, an achievable
infinite-message sum-rate with infinitesimal-rate messages is derived in terms
of a two-dimensional definite integral and a rate-allocation curve. A general
framework for multiterminal interactive function computation based on an
information exchange protocol which successively switches among different
distributed source coding configurations is developed. For networks with a star
topology, multiple rounds of interactive coding is shown to decrease the
scaling law of the total network rate by an order of magnitude as the network
grows.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 22:37:47 GMT"
},
{
"version": "v2",
"created": "Sun, 17 Feb 2008 22:59:24 GMT"
},
{
"version": "v3",
"created": "Tue, 19 Feb 2008 22:31:24 GMT"
},
{
"version": "v4",
"created": "Wed, 12 Nov 2008 22:20:42 GMT"
}
] | 2008-11-13T00:00:00 | [
[
"Ma",
"Nan",
""
],
[
"Ishwar",
"Prakash",
""
]
] | [
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] |
801.0757 | Jeetain Mittal | Jeetain Mittal, Thomas M. Truskett, Jeffrey R. Errington, Gerhard
Hummer | Layering and position-dependent diffusive dynamics of confined fluids | null | Phys. Rev. Lett. 100, 145901 (2008) | 10.1103/PhysRevLett.100.145901 | null | cond-mat.soft cond-mat.stat-mech | null | We study the diffusive dynamics of a hard-sphere fluid confined between
parallel smooth hard walls. The position-dependent diffusion coefficient normal
to the walls is larger in regions of high local packing density. High density
regions also have the largest available volume, consistent with the fast local
diffusivity. Indeed, local and global diffusivities as a function of the Widom
insertion probability approximately collapse onto a master curve. Parallel and
average normal diffusivities are strongly coupled at high densities and deviate
from bulk fluid behavior.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 22:57:05 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Mittal",
"Jeetain",
""
],
[
"Truskett",
"Thomas M.",
""
],
[
"Errington",
"Jeffrey R.",
""
],
[
"Hummer",
"Gerhard",
""
]
] | [
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] |
801.0758 | Juan Pablo Paz | Ariel Bendersky, Fernando Pastawski and Juan Pablo Paz | Selective Efficient Quantum Process Tomography | 4 pages | null | null | null | quant-ph | null | We present a new method for quantum process tomography. The method enables us
to efficiently estimate, with fixed precision, any of the parameters
characterizing a quantum channel. It is selective since one can choose to
estimate the value of any specific set of matrix elements of the super-operator
describing the channel. Also, we show how to efficiently estimate all the
average survival probabilities associated with the channel (i.e., all the
diagonal elements of its $\chi$--matrix.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 23:07:24 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Bendersky",
"Ariel",
""
],
[
"Pastawski",
"Fernando",
""
],
[
"Paz",
"Juan Pablo",
""
]
] | [
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] |
801.0759 | Thomas M. Truskett | Gaurav Goel, William P. Krekelberg, Jeffrey R. Errington, and Thomas
M. Truskett | Tuning density profiles and mobility of inhomogeneous fluids | 5 pages, 3 figures | Physical Review Letters 100, 106001 (2008) | 10.1103/PhysRevLett.100.106001 | null | cond-mat.stat-mech cond-mat.soft | null | Density profiles are the most common measure of inhomogeneous structure in
confined fluids, but their connection to transport coefficients is poorly
understood. We explore via simulation how tuning particle-wall interactions to
flatten or enhance the particle layering of a model confined fluid impacts its
self-diffusivity, viscosity, and entropy. Interestingly, interactions that
eliminate particle layering significantly reduce confined fluid mobility,
whereas those that enhance layering can have the opposite effect. Excess
entropy helps to understand and predict these trends.
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 23:28:55 GMT"
}
] | 2008-03-14T00:00:00 | [
[
"Goel",
"Gaurav",
""
],
[
"Krekelberg",
"William P.",
""
],
[
"Errington",
"Jeffrey R.",
""
],
[
"Truskett",
"Thomas M.",
""
]
] | [
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] |
801.076 | Fernando C. Lombardo | C. D. Fosco, F. C. Lombardo, and F. D. Mazzitelli | Casimir energies with finite-width mirrors | 18 pages, no figures. Version to appear in Phys. Rev. D | Phys.Rev.D77:085018,2008 | 10.1103/PhysRevD.77.085018 | null | hep-th hep-ph quant-ph | null | We use a functional approach to the Casimir effect in order to evaluate the
exact vacuum energy for a real scalar field in $d+1$ dimensions, in the
presence of backgrounds that, in a particular limit, impose Dirichlet boundary
conditions on one or two parallel surfaces. Outside of that limit, the
background may be thought of as describing finite-width mirrors with
frequency-dependent transmission and reflection coefficients. We provide new
explicit results for the Casimir energy in some particular backgrounds
| [
{
"version": "v1",
"created": "Fri, 4 Jan 2008 23:34:21 GMT"
},
{
"version": "v2",
"created": "Thu, 13 Mar 2008 13:42:49 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Fosco",
"C. D.",
""
],
[
"Lombardo",
"F. C.",
""
],
[
"Mazzitelli",
"F. D.",
""
]
] | [
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] |
801.0761 | Andrew Kerman | Andrew J. Kerman and William D. Oliver | High-fidelity quantum operations on superconducting qubits in the
presence of noise | null | Phys. Rev. Lett. 101, 070501 (2008) | 10.1103/PhysRevLett.101.070501 | null | quant-ph cond-mat.supr-con physics.atom-ph | null | We present a scheme for implementing quantum operations with superconducting
qubits. Our approach uses a "coupler" qubit to mediate a controllable, secular
interaction between "data" qubits, pulse sequences which strongly mitigate the
effects of 1/f flux noise, and a high-Q resonator-based local memory. We
develop a Monte-Carlo simulation technique capable of describing arbitrary
noise-induced dephasing and decay, and demonstrate in this system a set of
universal gate operations with O(10^-5) error probabilities in the presence of
experimentally measured levels of 1/f noise. We then add relaxation and
quantify the decay times required to maintain this error level.
| [
{
"version": "v1",
"created": "Sun, 6 Jan 2008 16:05:40 GMT"
},
{
"version": "v2",
"created": "Wed, 19 Mar 2008 18:04:22 GMT"
}
] | 2013-10-22T00:00:00 | [
[
"Kerman",
"Andrew J.",
""
],
[
"Oliver",
"William D.",
""
]
] | [
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] |
801.0762 | Vasilis Niarchos | Adi Armoni, Dan Israel, Gregory Moraitis, Vasilis Niarchos | Non-Supersymmetric Seiberg Duality, Orientifold QCD and Non-Critical
Strings | 45 pages, 1 figure | Phys.Rev.D77:105009,2008 | 10.1103/PhysRevD.77.105009 | null | hep-th | null | We propose an electric-magnetic duality and conjecture an exact conformal
window for a class of non-supersymmetric U(N_c) gauge theories with fermions in
the (anti)symmetric representation of the gauge group and N_f additional scalar
and fermion flavors. The duality exchanges N_c with N_f -N_c \mp 4 leaving N_f
invariant, and has common features with Seiberg duality in N=1 SQCD with SU or
SO/Sp gauge group. At large N the duality holds due to planar equivalence with
N=1 SQCD. At finite N we embed these gauge theories in a setup with D-branes
and orientifolds in a non-supersymmetric, but tachyon-free, non-critical type
0B string theory and argue in favor of the duality in terms of boundary and
crosscap state monodromies as in analogous supersymmetric situations. One can
verify explicitly that the resulting duals have matching global anomalies.
Finally, we comment on the moduli space of these gauge theories and discuss
other potential non-supersymmetric examples that could exhibit similar
dualities.
| [
{
"version": "v1",
"created": "Mon, 7 Jan 2008 18:16:42 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Armoni",
"Adi",
""
],
[
"Israel",
"Dan",
""
],
[
"Moraitis",
"Gregory",
""
],
[
"Niarchos",
"Vasilis",
""
]
] | [
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] |
801.0763 | William Detmold | William Detmold and Martin J. Savage | The Energy of n Identical Bosons in a Finite Volume at O(L^{-7}) | 3 pages | Phys.Rev.D77:057502,2008 | 10.1103/PhysRevD.77.057502 | NT@UW-08-01 | hep-lat cond-mat.stat-mech nucl-th | null | The volume dependence of the ground-state energy of n identical bosons with
short-range interactions in a periodic spatial volume with sides of length L is
calculated at order L^{-7} in the large volume expansion. This result will
enable a refined determination of the pi^+ pi^+ pi^+ interaction from lattice
QCD calculations.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 00:05:20 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Detmold",
"William",
""
],
[
"Savage",
"Martin J.",
""
]
] | [
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] |
801.0764 | Nour-Eddine Raouafi | N.-E. Raouafi, J. W. Harvey and C. J. Henney | On the Polar Field Distribution as Observed by SOLIS | 8 pages, 3 figures | null | null | null | astro-ph | null | We use Vector Spectromagnetograph (VSM) chromospheric full-disk magnetograms,
from the Synoptic Optical Long-term Investigations of the Sun (SOLIS) project,
to study the distribution of magnetic field flux concentrations within the
polar caps. We find that magnetic flux elements preferentially appear toward
lower latitudes within the polar caps away from the poles. This has
implications on numerous solar phenomena such as the formation and evolution of
fine polar coronal structures (i.e., polar plumes). Our results also have
implications for the processes carrying the magnetic flux from low to high
latitudes (e.g., meridional circulation).
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 00:38:12 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Raouafi",
"N. -E.",
""
],
[
"Harvey",
"J. W.",
""
],
[
"Henney",
"C. J.",
""
]
] | [
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] |
801.0765 | Joel Berry | Joel Berry, K. R. Elder, and Martin Grant | Melting at dislocations and grain boundaries: A Phase Field Crystal
study | 4 pages, 3 figures | null | 10.1103/PhysRevB.77.224114 | null | cond-mat.mtrl-sci | null | Dislocation and grain boundary melting are studied in three dimensions using
the Phase Field Crystal method. Isolated dislocations are found to melt
radially outward from their core, as the localized excess elastic energy drives
a power law divergence in the melt radius. Dislocations within low-to-mid angle
grain boundaries melt similarly until an angle-dependent first order wetting
transition occurs when neighboring melted regions coalesce. High angle
boundaries are treated within a screening approximation, and issues related to
ensembles, metastability, and grain size are discussed.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 01:18:13 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Berry",
"Joel",
""
],
[
"Elder",
"K. R.",
""
],
[
"Grant",
"Martin",
""
]
] | [
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] |
801.0766 | Nour-Eddine Raouafi | N.-E. Raouafi and D. Tripathi | On the Relationship Between a CME Associated Waves Observed on 5 March
2000 | 8 pages, 4 figures | null | null | null | astro-ph | null | We study the relationship between different wave phenomena associated with a
coronal mass ejection (CME) observed on 05 Mar. 2000. EIT waves were observed
in the images recorded by EIT at 195 {\AA}. The white-light LASCO/C2 images
show clear deflection and propagation of a kink along with the CME.
Spectroscopic observations recorded by the UVCS reveals excessive line
broadening in the two O {\sc{vi}} lines (1032 and 1037 {\AA}). Moreover very
hot lines such as Si {\sc{xii}} and Mg {\sc{x}} were observed. Interestingly,
the EIT wave, the streamer deflection and the intensity modulation along the
slit were all propagating North-East. Spatial and temporal correlations show
that the streamer deflection and spectral line broadening are highly likely to
be due to a CME-driven shock wave and that the EIT wave is the signature of a
CME-driven shock wave in the lower corona.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 01:26:35 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Raouafi",
"N. -E.",
""
],
[
"Tripathi",
"D.",
""
]
] | [
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] |
801.0767 | Wolfgang Ziller | Karsten Grove and Wolfgang Ziller | Lifting Group Actions and Nonnegative Curvature | 27 pages | null | null | null | math.DG | null | We show that all vector bundles over CP^2 which are not spin admit a complete
metric with nonnegative sectional curvature. In the proof we construct a
nonnegatively curved metric on the corresponding principle bundle by showing
that it admits a cohomogeneity one action with singular orbits of codimension
2. This is closely related to the problem of when an action of G on the base of
an L principle bundle lifts to the total space, such that the lift commutes
with L. We solve this lifting problem for all SO(k) principle bundles over a
4-dimensional simply connected base B with G a cohomogeneity one action on B.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 01:43:09 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Grove",
"Karsten",
""
],
[
"Ziller",
"Wolfgang",
""
]
] | [
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] |
801.0768 | Chang Qing Sun Dr | Chang Q. Sun | The strongest size in the inverse Hall-Petch relationship | null | null | null | null | cond-mat.mtrl-sci | null | Incorporating the bond-order-length-strength correlation mechanism [Sun CQ,
Prog Solid State Chem 35, 1 -159 (2007)] and Borns criterion for melting [J.
Chem. Phys. 7, 591(1939)] into the conventional Hall-Petch relationship has
turned out an analytical expression for the size and temperature dependence of
the mechanical strength of nanograins, known as the inverse Hall-Petch
relationship (IHPR), that has long been a topic under debate regarding the
possible mechanisms. Reproduction of the measured IHPR of Ni, NiP and TiO2
nanocrystals revealed that: (i) the size induced energy densification and
cohesive energy loss of nanograins originates the IHPR that could be activated
in the contact mode of plastic deformation detection; (ii) the competition
between the inhibition of atomic dislocations, via the surface energy density
gain and the strain work hardening, and the activation for dislocations through
cohesive energy loss determine the entire IHPR profile of a specimen; (iii) the
presence of a soft quasisolid phase is responsible for the size-induced
softening and the superplasticity as well of nanostructures; (iv) the bond
nature involved and the T/Tm ratio between the temperature of operating and the
temperature of melting dictate the measured strongest sizes of a given
specimen.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 02:04:44 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Sun",
"Chang Q.",
""
]
] | [
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801.0769 | Chang Qing Sun Dr | Chang Q. Sun | Thermally driven elastic weakening of crystals | null | null | null | null | cond-mat.mtrl-sci | null | An analytical solution has been developed clarifying that the thermally
driven elastic softening of crystals can be directly related to the length and
strength of the representative bonds of the crystal and to the response of the
bonding identities to the change of temperature. Reproduction of the
experimental results Ag, Au, MgO, Mg2SO4, Al2O3, and KCl derived mean atomic
cohesive energy of the specimen may evidence the validity of the proposed
approach without involving parameters using in classical thermodynamics.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 02:09:42 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Sun",
"Chang Q.",
""
]
] | [
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801.077 | Chang Qing Sun Dr | Chang Q. Sun | Pressure-stiffened Raman Phonons in Group III Nitrides | null | null | null | null | cond-mat.mtrl-sci | null | It has long been puzzling regarding the atomistic origin of the
pressure-induced Raman phonon stiffening that generally follows a polynomial
expression with coefficients needing physical indication. Here we show that an
extension of the bond-order-length-strength (BOLS) correlation mechanism to the
pressure domain has led to an analytical solution to connect the
pressure-induced Raman phonon stiffening directly to the bonding identities of
the specimen and the response of the bonding identities to the applied
stimulus. It is found that the pressure-induced blue-shift of Raman phonons
arises from the bond compression and energy storage exerted by the compressive
stress. Agreement between predictions and experimental measurement leads to the
detailed form for the polynomial coefficients, which offer an atomic
understanding of the physical mechanism of the external pressure induced energy
gain, thermally induced bond expansion as well as means of determining the mode
atomic cohesive energy in a specimen.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 02:17:21 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Sun",
"Chang Q.",
""
]
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] |
801.0771 | Chang Qing Sun Dr | Chang Q. Sun | An approach to local band average for the temperature dependence of
lattice thermal expansion | null | null | null | null | cond-mat.mtrl-sci | null | It has long been puzzling regarding the mechanism behind the nonlinearity of
lattice thermal expansion at low temperatures despite modeling considerations
from various perspectives in classical or quantum approximations. An analytical
solution in terms of local bond average is presented herewith showing that the
thermal expansion coefficient follows closely the specific heat of Debye
approximation without the involvement of mode Gruneisen constant or the bulk
modulus. Matching predictions to experimental observations using the Debye
temperature and the atomic cohesive energy as input evidences that the current
approach may represent the true situation of temperature induced lattice
expansion though the exact form of phonon density of states need to be
considered for further refinement.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 02:26:19 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Sun",
"Chang Q.",
""
]
] | [
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] |
801.0772 | Chang Qing Sun Dr | Chang Q. Sun | Nanocavity hardening: impact of broken bonds at the negatively curved
surfaces | null | null | null | null | cond-mat.mes-hall | null | It is expected that atomic vacancies or nanometric cavities reduce the number
of chemical bonds of nearby atoms and hence the strength of a voided solid.
However, the hardness of a porous specimen does not always follow this simple
picture of coordination counting. An introduction of a certain amount of atomic
vacancies or nanocavities could, instead, enhance the mechanical strength of
the porous specimen. Understanding the mechanism behind the intriguing
observations remains yet a high challenge. Here we show with analytical
expressions that the shortened and strengthened bonds between the
under-coordinated atoms and the associated local strain and energy trapping
[Sun, Prog Solid State Chem 35, 1-159 (2007)] in the negatively curved surface
skins dominate the observed nanocavity hardening. Agreement between predictions
and the experimentally observed size-dependence of mechanical strength of some
nanoporous materials evidences for the proposed mechanism.
| [
{
"version": "v1",
"created": "Sat, 5 Jan 2008 02:31:03 GMT"
}
] | 2008-01-08T00:00:00 | [
[
"Sun",
"Chang Q.",
""
]
] | [
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