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801.1873 | Marius Junge | Marius Junge, Tao Mei | Noncommutative Riesz transforms -- a probabilistic approach | null | null | null | null | math.OA math.FA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For $2\le p<\infty$ we show the lower estimates
\[ \|A^{\frac 12}x\|_p \kl c(p)\max\{\pl \|\Gamma(x,x)^{{1/2}}\|_p,\pl
\|\Gamma(x^*,x^*)^{{1/2}}\|_p\} \] for the Riesz transform associated to a
semigroup $(T_t)$ of completely positive maps on a von Neumann algebra with
negative generator $T_t=e^{-tA}$, and gradient form \[ 2\Gamma(x,y)\lel
Ax^*y+x^*Ay-A(x^*y)\pl .\] As additional hypothesis we assume that $\Gamma^2\gl
0$ and the existence of a Markov dilation for $(T_t)$. We give applications to
quantum metric spaces and show the equivalence of semigroup Hardy norms and
martingale Hardy norms derived from the Markov dilation. In the limiting case
we obtain a viable definition of BMO spaces for general semigroups of
completely positive maps which can be used as an endpoint for interpolation.
For torsion free ordered groups we construct a connection between Riesz
transforms and the Hilbert transform induced by the order.
| [
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801.1874 | Sebastian Blatt | S. Blatt, A. D. Ludlow, G. K. Campbell, J. W. Thomsen, T. Zelevinsky,
M. M. Boyd, J. Ye, X. Baillard, M. Fouch\'e, R. Le Targat, A. Brusch, P.
Lemonde, M. Takamoto, F.-L. Hong, H. Katori, V. V. Flambaum | New Limits on Coupling of Fundamental Constants to Gravity Using
$^{87}$Sr Optical Lattice Clocks | Published version. 4 pages, 4 figures | Phys.Rev.Lett.100:140801,2008 | 10.1103/PhysRevLett.100.140801 | null | physics.atom-ph physics.gen-ph | null | The $^1\mathrm{S}_0$-$^3\mathrm{P}_0$ clock transition frequency
$\nu_\text{Sr}$ in neutral $^{87}$Sr has been measured relative to the Cs
standard by three independent laboratories in Boulder, Paris, and Tokyo over
the last three years. The agreement on the $1\times 10^{-15}$ level makes
$\nu_\text{Sr}$ the best agreed-upon optical atomic frequency. We combine
periodic variations in the $^{87}$Sr clock frequency with $^{199}$Hg$^+$ and
H-maser data to test Local Position Invariance by obtaining the strongest
limits to date on gravitational-coupling coefficients for the fine-structure
constant $\alpha$, electron-proton mass ratio $\mu$ and light quark mass.
Furthermore, after $^{199}$Hg$^+$, $^{171}$Yb$^+$ and H, we add $^{87}$Sr as
the fourth optical atomic clock species to enhance constraints on yearly drifts
of $\alpha$ and $\mu$.
| [
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"created": "Wed, 6 Feb 2008 22:18:19 GMT"
},
{
"version": "v3",
"created": "Tue, 29 Apr 2008 05:17:41 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Blatt",
"S.",
""
],
[
"Ludlow",
"A. D.",
""
],
[
"Campbell",
"G. K.",
""
],
[
"Thomsen",
"J. W.",
""
],
[
"Zelevinsky",
"T.",
""
],
[
"Boyd",
"M. M.",
""
],
[
"Ye",
"J.",
""
],
[
"Baillard",
"X.",
""
],
[
"Fouché",
"M.",
""
],
[
"Targat",
"R. Le",
""
],
[
"Brusch",
"A.",
""
],
[
"Lemonde",
"P.",
""
],
[
"Takamoto",
"M.",
""
],
[
"Hong",
"F. -L.",
""
],
[
"Katori",
"H.",
""
],
[
"Flambaum",
"V. V.",
""
]
] | [
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801.1875 | Rennan Barkana | Tom Broadhurst (1), Rennan Barkana (1 and 2) ((1) Tel Aviv University
(2) ICRR, University of Tokyo) | Large Einstein Radii: A Problem for LambdaCDM | 9 pages, 5 figures, accepted by MNRAS | null | 10.1111/j.1365-2966.2008.13852.x | null | astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Einstein radius of a cluster provides a relatively model-independent
measure of the mass density of a cluster within a projected radius of ~ 150
kpc, large enough to be relatively unaffected by gas physics. We show that the
observed Einstein radii of four well-studied massive clusters, for which
reliable virial masses are measured, lie well beyond the predicted distribution
of Einstein radii in the standard LambdaCDM model. Based on large samples of
numerically simulated cluster-sized objects with virial masses ~ 1e15 solar,
the predicted Einstein radii are only 15-25'', a factor of two below the
observed Einstein radii of these four clusters. This is because the predicted
mass profile is too shallow to exceed the critical surface density for lensing
at a sizable projected radius. After carefully accounting for measurement
errors as well as the biases inherent in the selection of clusters and the
projection of mass measured by lensing, we find that the theoretical
predictions are excluded at a 4-sigma significance. Since most of the free
parameters of the LambdaCDM model now rest on firm empirical ground, this
discrepancy may point to an additional mechanism that promotes the collapse of
clusters at an earlier time thereby enhancing their central mass density.
| [
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"created": "Sat, 12 Jan 2008 06:12:59 GMT"
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"version": "v2",
"created": "Mon, 18 Feb 2008 12:36:58 GMT"
},
{
"version": "v3",
"created": "Tue, 19 Aug 2008 19:03:03 GMT"
}
] | 2009-11-13T00:00:00 | [
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"Tom",
"",
"1 and 2"
],
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] |
801.1876 | Anant Godbole | Torey Burton, Anant P. Godbole, Brett M. Kindle | The Lexicographic First Occurrence of a I-II-III pattern | null | Lecture Notes of the London Mathematical Society 376, 213-219,
2010 | null | null | math.PR math.CO | null | Consider a random permutation $\pi\in{\cal S}_n$. In this paper, perhaps best
classified as a contribution to discrete probability distribution theory, we
study the {\it first} occurrence $X=X_n$ of a I-II-III-pattern, where "first"
is interpreted in the lexicographic order induced by the 3-subsets of
$[n]=\{1,2,...,n\}$. Of course if the permutation is I-II-III-avoiding then the
first I-II-III-pattern never occurs, and thus $\e(X)=\infty$ for each $n$; to
avoid this case, we also study the first occurrence of a I-II-III-pattern given
a bijection $f:{\bf Z}^+\to{\bf Z}^+$.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 02:40:27 GMT"
}
] | 2012-04-12T00:00:00 | [
[
"Burton",
"Torey",
""
],
[
"Godbole",
"Anant P.",
""
],
[
"Kindle",
"Brett M.",
""
]
] | [
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] |
801.1877 | Dong-Hee Kim | Dong-Hee Kim and Adilson E. Motter | Resource allocation pattern in infrastructure networks | null | J. Phys. A: Math. Theor. 41 (2008) 224019 | 10.1088/1751-8113/41/22/224019 | null | physics.soc-ph | null | Most infrastructure networks evolve and operate in a decentralized fashion,
which may adversely impact the allocation of resources across the system. Here
we investigate this question by focusing on the relation between capacity and
load in various such networks. We find that, due to network traffic
fluctuations, real systems tend to have larger unoccupied portions of the
capacities--smaller load-to-capacity ratios--on network elements with smaller
capacities, which contrasts with key assumptions involved in previous studies.
This finding suggests that infrastructure networks have evolved to minimize
local failures but not necessarily large-scale failures that can be caused by
the cascading spread of local damage.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 03:14:46 GMT"
},
{
"version": "v2",
"created": "Wed, 21 May 2008 20:44:17 GMT"
}
] | 2008-05-21T00:00:00 | [
[
"Kim",
"Dong-Hee",
""
],
[
"Motter",
"Adilson E.",
""
]
] | [
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] |
801.1878 | Marco Salluzzo | M. Salluzzo, G. Ghiringhelli, J. C. Cezar, N. B. Brookes, G. M. De
Luca, F. Fracassi and R. Vaglio | Indirect electric field doping of the CuO2 planes of the cuprate
NdBa2Cu3O7 superconductor | 4 pages, 4 figures, Phys. Rev. Lett. accepted January (2008) | Phys. Rev. Lett. 100, 056810 (2008) | 10.1103/PhysRevLett.100.056810 | null | cond-mat.str-el cond-mat.supr-con | null | The mechanism of field-effect doping in the "123" high critical temperature
superconductors (HTS) has been investigated by x-ray absorption spectroscopy in
the presence of an electric field. We demonstrate that holes are created at the
CuO chains of the charge reservoir and that field-effect doping of the CuO2
planes occurs by charge transfer, from the chains to the planes, of a fraction
of the overall induced holes. The electronic properties of the charge reservoir
and of the dielectric/HTS interface determine the electric field doping of the
CuO2 planes
| [
{
"version": "v1",
"created": "Mon, 14 Jan 2008 15:06:57 GMT"
}
] | 2008-12-07T00:00:00 | [
[
"Salluzzo",
"M.",
""
],
[
"Ghiringhelli",
"G.",
""
],
[
"Cezar",
"J. C.",
""
],
[
"Brookes",
"N. B.",
""
],
[
"De Luca",
"G. M.",
""
],
[
"Fracassi",
"F.",
""
],
[
"Vaglio",
"R.",
""
]
] | [
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] |
801.1879 | Yan Jing | Jing Yan, Lei Shan, Qiang Luo, Weihua Wang, Hai-Hu Wen | $S$-wave pairing symmetry in non-centrosymmetric superconductor Re$_3$W | 12 pages, 5 figures | null | null | null | cond-mat.supr-con | null | The alloys of non-centrosymmetric superconductor, Re$_3$W, which were
reported to have an $\alpha$-Mn structure [P. Greenfield and P. A. Beck, J.
Metals, N. Y. \textbf{8}, 265 (1959)] with $T_\mathrm{c}=9 $K were prepared by
arc melting. The ac susceptibility and low-temperature specific heat were
measured on these alloys. It is found that there are two superconducting phases
coexisting in the samples with $T_\mathrm{c1}\sim9 $K and $T_\mathrm{c2}\sim7
$K, both of which have a non-centrosymmetric structure as reported previously.
By analyzing the specific heat data measured in various magnetic fields, we
found that the absence of the inversion symmetry does not lead to the deviation
from a s-wave pairing symmetry in Re$_3$W.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 04:56:45 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Yan",
"Jing",
""
],
[
"Shan",
"Lei",
""
],
[
"Luo",
"Qiang",
""
],
[
"Wang",
"Weihua",
""
],
[
"Wen",
"Hai-Hu",
""
]
] | [
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] |
801.188 | Yue Chongxing | Li Ding and Chong-Xing Yue | Top quark chromomagnetic dipole moment in the littlest Higgs model with
T-parity | latex files, 12 pages, 3 figures | Commun.Theor.Phys.50:441-444,2008 | 10.1088/0253-6102/50/2/32 | null | hep-ph | null | The littlest Higgs model with T-parity, which is called $LHT$ model, predicts
the existence of the new particles, such as heavy top quark, heavy gauge
bosons, and mirror fermions. We calculate the one-loop contributions of these
new particles to the top quark chromomagnetic dipole moment $(CMDM)$ $\Delta
K$. We find that the contribution of the $LHT$ model is one order of magnitude
smaller than the standard model prediction value.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 06:45:47 GMT"
}
] | 2008-12-18T00:00:00 | [
[
"Ding",
"Li",
""
],
[
"Yue",
"Chong-Xing",
""
]
] | [
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801.1881 | Iosif Khriplovich | I.B. Khriplovich | Spinning Relativistic Particles in External Fields | 14 pages | Acta Physica Polonica B, Proceedigs Supplement, 1 (2008) 197 | null | 0801.1881v1 | gr-qc hep-ph physics.acc-ph | null | The motion of spinning relativistic particles in external electromagnetic and
gravitational fields is considered. A simple derivation of the spin interaction
with gravitational field is presented. The self-consistent description of the
spin corrections to the equations of motion is built with the noncovariant
description of spin and with the usual, ``naive'' definition of the coordinate
of a relativistic particle.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 07:20:03 GMT"
}
] | 2008-08-12T00:00:00 | [
[
"Khriplovich",
"I. B.",
""
]
] | [
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] |
801.1882 | Muhammad Sharif | M. Sharif and Kanwal Nazir | Energy-Momentum Problem of Bell-Szekeres Metric in General Relativity
and Teleparallel Gravity | 21 pages, accepted for publication in Braz. J. Phys | Braz.J.Phys.38:156-166,2008 | 10.1590/S0103-97332008000100028 | null | gr-qc | null | This paper is devoted to the investigation of the energy-momentum problem in
two theories, i.e., General Relativity and teleparallel gravity. We use
Einstein, Landau-Lifshitz, Bergmann-Thomson and M\"{o}ller's prescriptions to
evaluate energy-momentum distribution of Bell-Szekeres metric in both the
theories. It is shown that these prescriptions give the same energy-momentum
density components in both General Relativity and teleparallel theory.
M\"{o}ller's prescription yields constant energy in both the theories.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 07:45:57 GMT"
}
] | 2011-08-31T00:00:00 | [
[
"Sharif",
"M.",
""
],
[
"Nazir",
"Kanwal",
""
]
] | [
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] |
801.1883 | Andras Lorincz | Barnabas Poczos and Andras Lorincz | D-optimal Bayesian Interrogation for Parameter and Noise Identification
of Recurrent Neural Networks | null | null | null | null | cs.NE cs.IT math.IT | null | We introduce a novel online Bayesian method for the identification of a
family of noisy recurrent neural networks (RNNs). We develop Bayesian active
learning technique in order to optimize the interrogating stimuli given past
experiences. In particular, we consider the unknown parameters as stochastic
variables and use the D-optimality principle, also known as `\emph{infomax
method}', to choose optimal stimuli. We apply a greedy technique to maximize
the information gain concerning network parameters at each time step. We also
derive the D-optimal estimation of the additive noise that perturbs the
dynamical system of the RNN. Our analytical results are approximation-free. The
analytic derivation gives rise to attractive quadratic update rules.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 08:02:12 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Poczos",
"Barnabas",
""
],
[
"Lorincz",
"Andras",
""
]
] | [
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] |
801.1884 | Lorenzo Brandolese | Lorenzo Brandolese (ICJ), Grzegorz Karch | Far field asymptotics of solutions to convection equation with anomalous
diffusion | 16 pages | J. Evol. Equation 8 (2008) 307--326 | null | null | math.AP math.PR | null | The initial value problem for the conservation law $\partial_t
u+(-\Delta)^{\alpha/2}u+\nabla \cdot f(u)=0$ is studied for $\alpha\in (1,2)$
and under natural polynomial growth conditions imposed on the nonlinearity. We
find the asymptotic expansion as $|x|\to \infty$ of solutions to this equation
corresponding to initial conditions, decaying sufficiently fast at infinity.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 08:14:55 GMT"
}
] | 2009-07-17T00:00:00 | [
[
"Brandolese",
"Lorenzo",
"",
"ICJ"
],
[
"Karch",
"Grzegorz",
""
]
] | [
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] |
801.1885 | Takuma Tanaka | Takuma Tanaka, Takeshi Kaneko, Toshio Aoyagi | Recurrent infomax generates cell assemblies, avalanches, and simple
cell-like selectivity | 16 pages, 4 figures | null | null | null | q-bio.NC cond-mat.dis-nn | null | Through evolution, animals have acquired central nervous systems (CNSs),
which are extremely efficient information processing devices that improve an
animal's adaptability to various environments. It has been proposed that the
process of information maximization (infomax), which maximizes the information
transmission from the input to the output of a feedforward network, may provide
an explanation of the stimulus selectivity of neurons in CNSs. However, CNSs
contain not only feedforward but also recurrent synaptic connections, and
little is known about information retention over time in such recurrent
networks. Here, we propose a learning algorithm based on infomax in a recurrent
network, which we call "recurrent infomax" (RI). RI maximizes information
retention and thereby minimizes information loss in a network. We find that
feeding in external inputs consisting of information obtained from photographs
of natural scenes into an RI-based model of a recurrent network results in the
appearance of Gabor-like selectivity quite similar tothat existing in simple
cells of the primary visual cortex (V1). More importantly, we find that without
external input, this network exhibits cell assembly-like and synfire chain-like
spontaneous activity and a critical neuronal avalanche. RI provides a simple
framework to explain a wide range of phenomena observed in in vivo and in vitro
neuronal networks, and it should provide a novel understanding of experimental
results for multineuronal activity and plasticity from an information-theoretic
point of view.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 08:16:23 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Tanaka",
"Takuma",
""
],
[
"Kaneko",
"Takeshi",
""
],
[
"Aoyagi",
"Toshio",
""
]
] | [
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] |
801.1886 | Vadzim Piatrou | V.I. Kuvshinov, A.V. Kuzmin and V.A. Piatrou | Chaotic instantons in periodically perturbed double-well system | 8 pages, 5 figures | null | null | null | nlin.CD | null | Kicked double-well system is investigated both analytically and numerically.
Phenomenological formula for ground quasienergy splitting is obtained using
resonances overlap criterion in the framework of chaotic instanton approach.
Results of numerical calculations of quasienergy spectrum are in good agreement
with the phenomenological formula.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 09:11:43 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Kuvshinov",
"V. I.",
""
],
[
"Kuzmin",
"A. V.",
""
],
[
"Piatrou",
"V. A.",
""
]
] | [
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] |
801.1887 | Lode Pollet | Lode Pollet, Corinna Kollath, Kris Van Houcke, Matthias Troyer | Temperature changes when adiabatically ramping up an optical lattice | 18 pages, 24 figure | null | 10.1088/1367-2630/10/6/065001 | null | cond-mat.stat-mech | null | When atoms are loaded into an optical lattice, the process of gradually
turning on the lattice is almost adiabatic. In this paper we investigate how
the temperature changes when going from the gapless superfluid phase to the
gapped Mott phase along isentropic lines. To do so we calculate the entropy in
the single-band Bose-Hubbard model for various densities, interaction strengths
and temperatures in one and two dimensions for homogeneous and trapped systems.
Our theory is able to reproduce the experimentally observed visibilities and
therefore strongly supports that current experiments remain in the quantum
regime for all considered lattice depths with low temperatures and minimal
heating.
| [
{
"version": "v1",
"created": "Mon, 14 Jan 2008 19:25:48 GMT"
}
] | 2010-09-10T00:00:00 | [
[
"Pollet",
"Lode",
""
],
[
"Kollath",
"Corinna",
""
],
[
"Van Houcke",
"Kris",
""
],
[
"Troyer",
"Matthias",
""
]
] | [
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] |
801.1888 | Angelo Tartaglia | A. Tartaglia and N. Radicella | Effect of a possible cosmological time dependence of the gravitational
parameter G on the peak luminosity of type Ia supernovae | 9 pages | null | null | null | astro-ph | null | The cosmological expansion of the universe affects the behaviour of all
physical systems and, in the case of gravitationally bound ones, could
correspond to or mimic a time dependent Newton's constant. Here we discuss the
case of a locally spherical mass distribution embedded in a generic Robertson
Walker universe. Choosing the most appropriate metric tensor for the problem
and assuming that the local time scale is much much lower than the cosmic one,
we show that G is practically unaffected thus leaving the absolute magnitude of
type Ia supernovae unaltered at all epochs.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 10:15:10 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Tartaglia",
"A.",
""
],
[
"Radicella",
"N.",
""
]
] | [
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] |
801.1889 | Masahisa Tsuchiizu | Y. Omori, M. Tsuchiizu, and Y. Suzumura | Possible Metastable State Triggered by Competition of Peierls State and
Charge Ordered State | 8 pages, 9 figures | J. Phys. Soc. Jpn. 76 (2007) 114709 | 10.1143/JPSJ.76.114709 | null | cond-mat.str-el | null | We examine a Peierls ground state and its competing metastable state in the
one-dimensional quarter-filled Peierls-Hubbard model with the nearest-neighbor
repulsive interaction V and the electron-phonon interaction (\propto 1/K with K
being the elastic constant). From the mean-field approach, we obtain the phase
diagram for the ground state on the plane of parameters V and K. The coexistent
state of the spin-density wave and the charge ordering is realized for large V
and K. With decreasing K, it exhibits a first-order phase transition to the
unconventional Peierls state which is described by the bond-centered
charge-density-wave state. In the large region of the Peierls ground state in
the phase diagram, there exists the metastable state where the energy takes a
local minimum with respect to the lattice distortion. On the basis of the
present calculation, we discuss the photoinduced phase observed in the
(EDO-TTF)_{2}PF_{6} compound.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 19:06:40 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Omori",
"Y.",
""
],
[
"Tsuchiizu",
"M.",
""
],
[
"Suzumura",
"Y.",
""
]
] | [
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] |
801.189 | Jose Antonio Martins Simoes | Helder Chavez S. and J. A. Martins Simoes | A left-right SU(7) symmetric model with D-parity cosmic strings | 9 pages | null | null | null | hep-th | null | Cosmic strings with the property of D-parity symmetry are studied in this
paper. They are of a Z-2 type of strings that could appear in the spontaneous
breaking of SU(7) and would present extraordinary properties in a background of
ordinary and mirror neutrinos. Through the special embedding of the left-right
symmetry in SU(7), with a minimal content of Higgs fields, based on two
singlets and two doublets, it is possible to assure the topological stability
of this type of cosmic strings. In their presence we could have a neutral
flavor changing interaction between ordinary and mirror neutrinos as well as
the formation of superconducting currents in the form of zero modes of neutrino
mirrors that would show interesting effects.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 10:24:57 GMT"
},
{
"version": "v2",
"created": "Fri, 22 Feb 2008 17:39:51 GMT"
}
] | 2008-02-22T00:00:00 | [
[
"S.",
"Helder Chavez",
""
],
[
"Simoes",
"J. A. Martins",
""
]
] | [
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801.1891 | Masahisa Tsuchiizu | M. Tsuchiizu and Y. Suzumura | Peierls ground state and excitations in the electron-lattice correlated
system (EDO-TTF)_{2}X | 11 pages, 10 figures, to be published in Phys. Rev. B | Phys. Rev. B 77, 195128 (2008) | 10.1103/PhysRevB.77.195128 | null | cond-mat.str-el | null | We investigate the exotic Peierls state in the one-dimensional organic
compound (EDO-TTF)_{2}X, wherein the Peierls transition is accompanied by the
bending of molecules and also by a fourfold periodic array of charge
disproportionation along the one-dimensional chain. Such a Peierls state,
wherein the interplay between the electron correlation and the electron-phonon
interaction takes an important role, is examined based on an extended
Peierls-Holstein-Hubbard model that includes the alternation of the elastic
energies for both the lattice distortion and the molecular deformation. The
model reproduces the experimentally observed pattern of the charge
disproportionation and there exists a metastable state wherein the energy takes
a local minimum with respect to the lattice distortion and/or molecular
deformation. Furthermore, we investigate the excited states for both the
Peierls ground state and the metastable state by considering the soliton
formation of electrons. It is shown that the soliton excitation from the
metastable state costs energy that is much smaller than that of the Peierls
state, where the former is followed only by the charge degree of freedom and
the latter is followed by that of spin and charge. Based on these results, we
discuss the exotic photoinduced phase found in (EDO-TTF)_{2}PF_{6}.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 18:09:43 GMT"
},
{
"version": "v2",
"created": "Tue, 20 May 2008 00:50:14 GMT"
}
] | 2008-06-26T00:00:00 | [
[
"Tsuchiizu",
"M.",
""
],
[
"Suzumura",
"Y.",
""
]
] | [
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] |
801.1892 | Juha Pohjanpelto | Juha Pohjanpelto and Stephen C. Anco | Generalized Symmetries of Massless Free Fields on Minkowski Space | This is a contribution to the Proc. of the Seventh International
Conference ''Symmetry in Nonlinear Mathematical Physics'' (June 24-30, 2007,
Kyiv, Ukraine), published in SIGMA (Symmetry, Integrability and Geometry:
Methods and Applications) at http://www.emis.de/journals/SIGMA/ | SIGMA 4:004,2008 | 10.3842/SIGMA.2008.004 | null | math-ph gr-qc hep-th math.MP | null | A complete and explicit classification of generalized, or local, symmetries
of massless free fields of spin $s \geq 1/2$ is carried out. Up to equivalence,
these are found to consists of the conformal symmetries and their duals, new
chiral symmetries of order $2s$, and their higher-order extensions obtained by
Lie differentiation with respect to conformal Killing vectors. In particular,
the results yield a complete classification of generalized symmetries of the
Dirac-Weyl neutrino equation, Maxwell's equations, and the linearized gravity
equations.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 10:28:03 GMT"
}
] | 2008-12-19T00:00:00 | [
[
"Pohjanpelto",
"Juha",
""
],
[
"Anco",
"Stephen C.",
""
]
] | [
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] |
801.1893 | Mioara Mugur-Schachter | Mioara Mugur-Schachter | Infra-Mecanique Quantique | 67 pages double spaced | null | null | null | quant-ph | null | A qualitative representation of what is called 'microstates' is constructed
quite independently from the mathematical formalism of fundamental Quantum
Mechanics, by taking into accont exclusively the constraints imposed by (a) the
cognitive situation in which a human being places himself if he decides to
construct knowledge concerning microstates; (b) the general requirements of
human conceptualisation. The result, called infra quantum mechanics, offers a
semantic structure of reference that will permit to develop a unified coherent
treatment of all the interpretation problems raised by the formalism of
fundamental Quantum Mechanics.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 10:35:16 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Mugur-Schachter",
"Mioara",
""
]
] | [
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] |
801.1894 | Eugene Terentjev | G. Feio, J. L. Figueirinhas, A. R. Tajbakhsh, E. M. Terentjev | Critical fluctuations and random-anisotropy glass transition in nematic
elastomers | null | null | 10.1103/PhysRevB.78.020201 | null | cond-mat.dis-nn cond-mat.soft | null | We carry out a detailed deuterium NMR study of local nematic ordering in
polydomain nematic elastomers. This system has a close analogy to the
random-anisotropy spin glass. We find that, in spite of the quadrupolar nematic
symmetry in 3-dimensions requiring a first-order transition, the order
parameter in the quenched ``nematic glass'' emerges via a continuous phase
transition. In addition, by a careful analysis of the NMR line shape, we deduce
that the local director fluctuations grow in a critical manner around the
transition point. This could be the experimental evidence for the Aizenman-Wehr
theorem about the quenched impurities changing the order of discontinuous
transition.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 10:39:08 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Feio",
"G.",
""
],
[
"Figueirinhas",
"J. L.",
""
],
[
"Tajbakhsh",
"A. R.",
""
],
[
"Terentjev",
"E. M.",
""
]
] | [
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] |
801.1895 | Celestino Creatore | C. Creatore and A. L. Ivanov | Strong and weak coupling limits in optics of quantum well excitons | Published in Physical Review B. 29 pages, 12 figures | Phys. Rev. B 77, 075324 (2008) | 10.1103/PhysRevB.77.075324 | null | cond-mat.mes-hall cond-mat.other | null | A transition between the strong (coherent) and weak (incoherent) coupling
limits of resonant interaction between quantum well (QW) excitons and bulk
photons is analyzed and quantified as a function of the incoherent damping rate
caused by exciton-phonon and exciton-exciton scattering. For confined QW
polaritons, a second, anomalous, damping-induced dispersion branch arises and
develops with increasing damping. In this case, the strong-weak coupling
transition is attributed to a critical damping rate, when the intersection of
the normal and damping-induced dispersion branches occurs. For the radiative
states of QW excitons, i.e., for radiative QW polaritons, the transition is
described as a qualitative change of the photoluminescence spectrum at grazing
angles along the QW structure. Furthermore, we show that the radiative
corrections to the QW exciton states with in-plane wavevector approaching the
photon cone are universally scaled by an energy parameter rather than diverge.
The strong-weak coupling transition rates are also proportional to the same
energy parameter. The numerical evaluations are given for a GaAs single quantum
well with realistic parameters.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 11:23:00 GMT"
},
{
"version": "v2",
"created": "Tue, 4 Mar 2008 11:40:45 GMT"
}
] | 2008-03-04T00:00:00 | [
[
"Creatore",
"C.",
""
],
[
"Ivanov",
"A. L.",
""
]
] | [
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] |
801.1896 | Tao Zhou | Luo-Luo Jiang, Da-Yin Hua, Jun-Fang Zhu, Bing-Hong Wang, and Tao Zhou | Opinion dynamics on directed small-world networks | 6 pages, 5 figures | null | 10.1140/epjb/e2008-00342-3 | null | physics.soc-ph | null | In this paper, we investigate the self-affirmation effect on formation of
public opinion in a directed small-world social network. The system presents a
non-equilibrium phase transition from a consensus state to a disordered state
with coexistence of opinions. The dynamical behaviors are very sensitive to the
density of long-range interactions and the strength of self-affirmation. When
the long-range interactions are sparse and individual generally does not insist
on his/her opinion, the system will display a continuous phase transition, in
the opposite case with high self-affirmation strength and dense long-range
interactions, the system does not display a phase transition. Between those two
extreme cases, the system undergoes a discontinuous phase transition.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 11:22:36 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Jiang",
"Luo-Luo",
""
],
[
"Hua",
"Da-Yin",
""
],
[
"Zhu",
"Jun-Fang",
""
],
[
"Wang",
"Bing-Hong",
""
],
[
"Zhou",
"Tao",
""
]
] | [
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801.1897 | Fardin Kheirandish | Fardin Kheirandish, S. Javad Akhtarshenas and Hamidreza Mohammadi | The effect of spin-orbit interaction on entanglement of two-qubit
Heisenberg XYZ systems in an inhomogeneous magnetic field | Two columns, 9 pages, 8 Figs | Phys. Rev. A 042309 (2008) | 10.1103/PhysRevA.77.042309 | null | quant-ph | null | The role of spin-orbit interaction on the ground state and thermal
entanglement of a Heisenberg XYZ two-qubit system in the presence of an
inhomogeneous magnetic field is investigated. For a certain value of spin-orbit
parameter $D$, the ground state entanglement tends to vanish suddenly and when
$D$ crosses its critical value $D_c$, the entanglement undergoes a revival. The
maximum value of the entanglement occurs in the revival region. In finite
temperatures there are revival regions in $D-T$ plane. In these regions,
entanglement first increases with increasing temperature and then decreases and
ultimately vanishes for temperatures above a critical value. This critical
temperature is an increasing function of $D$, thus the nonzero entanglement can
exist for larger temperatures. In addition, the amount of entanglement in the
revival region depends on the spin-orbit parameter. Also, the entanglement
teleportation via the quantum channel constructed by the above system is
investigated and finally the influence of the spin-orbit interaction on the
fidelity of teleportation and entanglement of replica state is studied.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 11:57:44 GMT"
}
] | 2012-07-12T00:00:00 | [
[
"Kheirandish",
"Fardin",
""
],
[
"Akhtarshenas",
"S. Javad",
""
],
[
"Mohammadi",
"Hamidreza",
""
]
] | [
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] |
801.1898 | Maggy Tomova | Maggy Tomova | Cut-disks for level spheres in link and tangle complements | 18 pages, 10 figures. The main theorem has been modified to include
an additional hypothesis | null | null | null | math.GT | null | Wu has shown that if a link or a knot $L$ in $S^3$ in thin position has thin
spheres, then the thin sphere of lowest width is an essential surface in the
link complement. In this paper we show that if we further assume that $L
\subset S^3$ is prime, then the thin sphere of lowest width also does not have
any vertical cut-disks. We also prove the result for a specific kind of tangles
in $S^2 \times [-1,1]$.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 12:29:33 GMT"
},
{
"version": "v2",
"created": "Fri, 8 Feb 2008 17:37:39 GMT"
},
{
"version": "v3",
"created": "Wed, 30 Apr 2008 13:38:28 GMT"
}
] | 2008-04-30T00:00:00 | [
[
"Tomova",
"Maggy",
""
]
] | [
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] |
801.1899 | Misha Verbitsky | Misha Verbitsky | Positive forms on hyperkahler manifolds | 33 pages | Osaka J. Math. Volume 47, Number 2 (2010), 353-384 | null | null | math.CV math.AG math.DG | null | Let $(M,I,J,K)$ be a hyperkaehler manifold, $\dim_\R M =4n$. We study
positive, Dolbeault-closed $(2p,0)$-forms on $(M,I)$. These forms are
quaternionic analogues of the positive $(p,p)$-forms. We construct an injective
homomorphism mapping Dolbeault-closed $(2p,0)$-forms to closed
$(n+p,n+p)$-forms, and positive $(2p,0)$-forms to positive $(n+p,n+p)$-forms.
This construction is used to prove a hyperkaehler version of the classical
Skoda-El Mir theorem, which says that a trivial extension of a closed, positive
current over a pluripolar set is again closed. We also prove the hyperkaehler
version of the Sibony's lemma, showing that a closed, positive $(2p,0)$-form
defined outside of a compact complex subvariety $Z\subset (M,I)$, $\codim Z >
2p$ is locally integrable in a neighbourhood of $Z$. These results are used to
prove polystability of derived direct images of certain coherent sheaves.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 13:38:25 GMT"
}
] | 2010-06-29T00:00:00 | [
[
"Verbitsky",
"Misha",
""
]
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801.19 | Fardin Kheirandish | Fardin Kheirandish and Morteza Soltani | Equivalent approaches to electromagnetic field quantization in a linear
dielectric | 28 pages, | null | null | null | quant-ph | null | It is shown that the minimal coupling method is equivalent to the
Huttner-Barnet and phenomenological approaches up to a canonical
transformation.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 13:11:21 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Kheirandish",
"Fardin",
""
],
[
"Soltani",
"Morteza",
""
]
] | [
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] |
801.1901 | Thomas Walcher | Thomas Walcher | Hadron structure at small momentum transfer | 7 pages, 9 figures. Contribution to the International School of
Nuclear Physics, 29th Ccourse, "Quarks in Hadrons and Nuclei", Erice, Sicily,
16 - 24 September 2007 | Prog.Part.Nucl.Phys.61:106-112,2008 | 10.1016/j.ppnp.2007.12.027 | null | hep-ph | null | Giving three examples, the form factors of the nucleon, the polarisability of
the charged pion and the interference of the $S_{11}(1535)$ with the
$D_{13}(1520)$ excitation of the nucleon in the $\eta p$-decay channel, it is
argued that the hadron structure at low momentum transfer is highly significant
for studying QCD.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 13:15:49 GMT"
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] | 2008-11-26T00:00:00 | [
[
"Walcher",
"Thomas",
""
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] |
801.1902 | Fardin Kheirandish | Fardin Kheirandish and Morteza Soltani | Extension of the Huttner-Barnett model to a magnetodielectric medium | 25 pages | Phys. Rev. A 78, 012102 (2008) | 10.1103/PhysRevA.78.012102 | null | quant-ph | null | The Huttner$-$Barnett model is extended to a magnetodielectric medium by
adding a new matter field to this model. The eigenoperators for the coupled
system are calculated and electromagnetic field is written in terms of these
operators. The electric and magnetic susceptibility of the medium are
explicitly derived and shown to satisfy the Kramers$-$Kronig relations. It is
shown that the results obtained in this model are equivalent to the results
obtained from the phenomenological methods.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 13:16:08 GMT"
}
] | 2012-07-12T00:00:00 | [
[
"Kheirandish",
"Fardin",
""
],
[
"Soltani",
"Morteza",
""
]
] | [
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] |
801.1903 | Sergey Pankratov | S.S. Pankratov (1), M. Baldo (2), U. Lombardo (2), E.E. Saperstein (1)
and M.V. Zverev (1); ((1)RRC "Kurchatov Institute", Moscow, Russia, (2)INFN,
Sezione di Catania, Catania, Italy) | The microscopic pairing gap in a slab of nuclear matter for the Argonne
v18 NN-potential | 20 pages, 8 figures | Nucl.Phys.A811:127-139,2008 | 10.1016/j.nuclphysa.2008.07.002 | null | nucl-th | null | Ab initio gap equation for ^1S_0 pairing in a nuclear slab is solved for the
Argonne v18 NN-potential. The gap function is compared in detail with the one
found previously for the separable form of the Paris potential. The difference
between the two gaps turned out to be about 10%. Dependence of the gap on the
chemical potential mu is analyzed.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 13:36:52 GMT"
}
] | 2008-11-07T00:00:00 | [
[
"Pankratov",
"S. S.",
""
],
[
"Baldo",
"M.",
""
],
[
"Lombardo",
"U.",
""
],
[
"Saperstein",
"E. E.",
""
],
[
"Zverev",
"M. V.",
""
],
[
";",
"",
""
]
] | [
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] |
801.1904 | Valentin Gutev | Valentin Gutev and Vesko Valov | Open maps having the Bula property | 16 pages | Fund. Math. 205 (2009), no. 2, 91-104 | 10.4064/fm205-2-1 | null | math.GN | null | Every open continuous map f from a space X onto a paracompact C-space Y
admits two disjoint closed subsets of X so that their image by f is Y provided
all fibers of f are infinite and C*-embedded in X. Applications are
demonstrated for the existence of "disjoint" usco multiselections of set-valued
l.s.c. mappings defined on paracompact C-spaces, and for special type of
factorizations of open continuous maps from metrizable spaces onto paracompact
C-spaces. This settles several open questions.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 13:38:47 GMT"
}
] | 2018-05-22T00:00:00 | [
[
"Gutev",
"Valentin",
""
],
[
"Valov",
"Vesko",
""
]
] | [
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] |
801.1905 | Pasquale Mazzotta | Pasquale Mazzotta (1 and 2) and Simona Giacintucci (2 and 3) ((1)
Dipartimento di Fisica Universita' di Roma ``Tor Vergata'', (2)
Harvard-Smithsonian Center for Astrophysics, (3) INAF - Istituto di
Radioastronomia Bologna) | Do radio core-halos and cold fronts in non major merging clusters
originate from the same gas sloshing? | 4 pages inc. 6 figures (2color). Accepted for publication in ApJL | null | 10.1086/529433 | null | astro-ph | null | We show an interesting correlation between the surface brightness and
temperature structure of the relaxed clusters RXJ1720.1+2638 and MS1455.0+2232,
hosting a pair of cold fronts, and their central core--halo radio source. We
discuss the possibility that the origin of this diffuse radio emission may be
strictly connected with the gas sloshing mechanism suggested to explain the
formation of cold fronts in non major merging clusters. We show that the
radiative lifetime of the relativistic electrons is much shorter than the
timescale on which they can be transported from the central galaxy up to the
radius of the outermost cold front. This strongly indicates that the observed
diffuse radio emission is likely produced by electrons re--accelerated via some
kind of turbulence generated within the cluster volume limited by the cold
fronts during the gas sloshing.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 14:44:49 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Mazzotta",
"Pasquale",
"",
"1 and 2"
],
[
"Giacintucci",
"Simona",
"",
"2 and 3"
]
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] |
801.1906 | Pierre Fima | Pierre Fima, Leonid Vainerman (LMNO) | Twisting and Rieffel's deformation of locally compact quantum groups.
Deformation of the Haar measure | null | null | 10.1007/s00220-008-0559-5 | null | math.OA | null | We develop the twisting construction for locally compact quantum groups. A
new feature, in contrast to the previous work of M. Enock and the second
author, is a non-trivial deformation of the Haar measure. Then we construct
Rieffel's deformation of locally compact quantum groups and show that it is
dual to the twisting. This allows to give new interesting concrete examples of
locally compact quantum groups, in particular, deformations of the classical
$az+b$ group and of the Woronowicz' quantum $az+b$ group.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 15:22:29 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Fima",
"Pierre",
"",
"LMNO"
],
[
"Vainerman",
"Leonid",
"",
"LMNO"
]
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] |
801.1907 | Pierre Fima | Pierre Fima (LM-Besan\c{c}on), Leonid Vainerman (LMNO) | A locally compact quantum group of triangular matrices | null | null | null | null | math.OA | null | We construct a one parameter deformation of the group of $2\times 2$ upper
triangular matrices with determinant 1 using the twisting construction. An
interesting feature of this new example of a locally compact quantum group is
that the Haar measure is deformed in a non-trivial way. Also, we give a
complete description of the dual $\cs$-algebra and the dual comultiplication.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 15:23:33 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Fima",
"Pierre",
"",
"LM-Besançon"
],
[
"Vainerman",
"Leonid",
"",
"LMNO"
]
] | [
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] |
801.1908 | David Bugg | D.V. Bugg (Queen Mary, University of London, UK) | Experimental disagreements with Extended Unitarity | 24 pages, 12 figures. To be published in Euro. Phys. J C | Eur.Phys.J.C54:73-87,2008 | 10.1140/epjc/s10052-007-0515-0 | null | hep-ex | null | In production processes, e.g. J/Psi -> omega-pi-pi or pbar-p -> 3pi, the
sigma and fo(980) overlap in the same partial wave. The conjecture of Extended
Unitarity (EU) states that the pi-pi pair should have the same phase variation
as pi-pi elastic scattering. This is an extension of Watson's theorem beyond
its original derivation, which stated only that the s-dependence of a single
resonance should be universal. The prediction of EU is that the deep dip
observed in pi-pi elastic scattering close to 1 GeV should also appear in
production data. Four sets of data disagree with this prediction. All require
different relative magnitudes of sigma and fo(980). That being so, a fresh
conjecture is to rewrite the 2-body unitarity relation for production in terms
of observed magnitudes. This leads to a prediction different to EU. Central
production data from the AFS experiment fit naturally to this hypothesis.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 15:28:32 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Bugg",
"D. V.",
"",
"Queen Mary, University of London, UK"
]
] | [
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801.1909 | Louigi Addario-Berry | Louigi Addario-Berry, Nicolas Broutin, G\'abor Lugosi | Effective resistance of random trees | Published in at http://dx.doi.org/10.1214/08-AAP572 the Annals of
Applied Probability (http://www.imstat.org/aap/) by the Institute of
Mathematical Statistics (http://www.imstat.org) | Annals of Applied Probability 2009, Vol. 19, No. 3, 1092-1107 | 10.1214/08-AAP572 | IMS-AAP-AAP572 | math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the effective resistance $R_n$ and conductance $C_n$ between
the root and leaves of a binary tree of height $n$. In this electrical network,
the resistance of each edge $e$ at distance $d$ from the root is defined by
$r_e=2^dX_e$ where the $X_e$ are i.i.d. positive random variables bounded away
from zero and infinity. It is shown that
$\mathbf{E}R_n=n\mathbf{E}X_e-(\operatorname
{\mathbf{Var}}(X_e)/\mathbf{E}X_e)\ln n+O(1)$ and $\operatorname
{\mathbf{Var}}(R_n)=O(1)$. Moreover, we establish sub-Gaussian tail bounds for
$R_n$. We also discuss some possible extensions to supercritical Galton--Watson
trees.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 15:46:46 GMT"
},
{
"version": "v2",
"created": "Fri, 7 Aug 2009 12:16:03 GMT"
}
] | 2009-08-07T00:00:00 | [
[
"Addario-Berry",
"Louigi",
""
],
[
"Broutin",
"Nicolas",
""
],
[
"Lugosi",
"Gábor",
""
]
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] |
801.191 | Francesco Mainardi | Francesco Mainardi, Sergei Rogosin | The origin of infinitely divisible distributions: from de Finetti's
problem to Levy-Khintchine formula | 26 pages | Mathematical Methods in Economics and Finance (MMEF), Vol 1
(2006), pp 37-55 | null | null | math.HO math.PR | null | The article provides an historical survey of the early contributions on
infinitely divisible distributions starting from the pioneering works of de
Finetti in 1929 up to the canonical forms developed in the thirties by
Kolmogorov, Levy and Khintchine. Particular attention is paid to single out the
personal contributions of the above authors that were published in Italian,
French or Russian during the period 1929-1938. In Appendix we report the
translation from the Russian into English of a fundamental paper by Khintchine
published in Moscow in 1937.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 17:21:00 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Mainardi",
"Francesco",
""
],
[
"Rogosin",
"Sergei",
""
]
] | [
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801.1911 | Henri Gouin | Henri Gouin (MSNMGP, LMMT) | The wetting problem of fluids on solid surfaces. Part 2: the contact
angle hysteresis | Preprint 26 pages | Continuum Mechanics and Thermodynamics 15, 6 (2003) 597-611 | 10.1007/s00161-003-0137-1 | null | physics.class-ph | null | In part 1, we proposed a model of dynamics of wetting for slow movements near
a contact line formed at the interface of two immiscible fluids and a solid
when viscous dissipation remains bounded. The contact line is not a material
line and a Young-Dupr\'e equation for the apparent dynamic contact angle taking
into account the line celerity was proposed. In this paper we consider a form
of the interfacial energy of a solid surface in which many small oscillations
are superposed on a slowly varying function. For a capillary tube, a scaling
analysis of the microscopic law associated with the Young-Dupr\'e dynamic
equation yields a macroscopic equation for the motion of the contact line. The
value of the deduced apparent dynamic contact angle yields for the average
response of the line motion a phenomenon akin to the stick-slip motion of the
contact line on the solid wall. The contact angle hysteresis phenomenon and the
modelling of experimentally well-known results expressing the dependence of the
apparent dynamic contact angle on the celerity of the line are obtained.
Furthermore, a qualitative explanation of the maximum speed of wetting (and
dewetting) can be given.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 17:27:53 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Gouin",
"Henri",
"",
"MSNMGP, LMMT"
]
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801.1912 | Andrew Brooke-Taylor | Andrew D. Brooke-Taylor and Sy-David Friedman | Large cardinals and gap-1 morasses | 49 pages | Annals of Pure and Applied Logic 159, no. 1-2 (2009), pp 71-99 | 10.1016/j.apal.2008.10.007 | null | math.LO | null | We present a new partial order for directly forcing morasses to exist that
enjoys a significant homogeneity property. We then use this forcing in a
reverse Easton iteration to obtain an extension universe with morasses at every
regular uncountable cardinal, while preserving all n-superstrong (0<n<omega+1),
hyperstrong and 1-extendible cardinals. In the latter case, a preliminary
forcing to make the GCH hold is required. Our forcing yields morasses that
satisfy an extra property related to the homogeneity of the partial order; we
refer to them as mangroves and prove that their existence is equivalent to the
existence of morasses. Finally, we exhibit a partial order that forces
universal morasses to exist at every regular uncountable cardinal, and use this
to show that universal morasses are consistent with n-superstrong, hyperstrong,
and 1-extendible cardinals. This all contributes to the second author's outer
model programme, the aim of which is to show that L-like principles can hold in
outer models which nevertheless contain large cardinals.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 18:04:52 GMT"
}
] | 2012-02-28T00:00:00 | [
[
"Brooke-Taylor",
"Andrew D.",
""
],
[
"Friedman",
"Sy-David",
""
]
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] |
801.1913 | Yuri A. Rylov | Yuri A. Rylov | Geometrical dynamics: spin as a result of rotation with superluminal
speed | 38 pages, 1 figure, New version of stabilizing vector | null | null | null | physics.gen-ph | null | Dynamics is considered as a corollary of the space-time geometry. Evolution
of a particle in the space-time is described as a chain of connected equivalent
geometrical objects. Space-time geometry is determined uniquely by the world
function $\sigma $. Proper modification of the Minkowskian world function for
large space-time interval leads to wobbling of the chain, consisted of timelike
straight segments. Statistical description of the stochastic world chain
coincides with the quantum description by means of the Schr\"{o}dinger
equation. Proper modification of the Minkowskian world function for small
space-time interval may lead to appearance of a world chain, having a shape of
a helix with timelike axis. Links of the chain are spacelike straight segments.
Such a world chain describes a spatial evolution of a particle. In other words,
the helical world chain describes the particle rotation with superluminal
velocity. The helical world chain associated with the classical Dirac particle,
whose world line is a helix. Length of world chain link cannot be arbitrary. It
is determined by the space-time geometry and, in particular, by the elementary
length. There exists some discrimination mechanism, which can discriminate some
world chains.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 18:08:18 GMT"
},
{
"version": "v2",
"created": "Thu, 17 Jan 2008 09:10:11 GMT"
},
{
"version": "v3",
"created": "Sat, 8 Mar 2008 15:48:00 GMT"
},
{
"version": "v4",
"created": "Wed, 28 May 2008 13:55:09 GMT"
}
] | 2008-05-28T00:00:00 | [
[
"Rylov",
"Yuri A.",
""
]
] | [
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801.1914 | Andrea Rapisarda | A. Pluchino, A. Rapisarda and C. Tsallis | A closer look at the indications of q-generalized Central Limit Theorem
behavior in quasi-stationary states of the HMF model | 11 pages, 8 figures. Text and figures added, Physica A in press | PHYSICA A 387 (2008) 3121 | 10.1016/j.physa.2008.01.112 | null | cond-mat.stat-mech astro-ph nucl-th physics.plasm-ph | null | We give a closer look at the Central Limit Theorem (CLT) behavior in
quasi-stationary states of the Hamiltonian Mean Field model, a paradigmatic one
for long-range-interacting classical many-body systems. We present new
calculations which show that, following their time evolution, we can observe
and classify three kinds of long-standing quasi-stationary states (QSS) with
different correlations. The frequency of occurrence of each class depends on
the size of the system. The different microsocopic nature of the QSS leads to
different dynamical correlations and therefore to different results for the
observed CLT behavior.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 14:11:20 GMT"
},
{
"version": "v2",
"created": "Fri, 18 Jan 2008 18:53:06 GMT"
}
] | 2008-03-17T00:00:00 | [
[
"Pluchino",
"A.",
""
],
[
"Rapisarda",
"A.",
""
],
[
"Tsallis",
"C.",
""
]
] | [
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] |
801.1915 | Chiu Fan Lee | Chiu Fan Lee | Dynamical density functional theory with hydrodynamic interaction | This paper has been withdrawn | null | null | null | cond-mat.soft cond-mat.stat-mech | null | This paper has been withdrawn by the author due to the incorrect application
of the divergence theorem to Eqs 7, 8 and 9.
| [
{
"version": "v1",
"created": "Mon, 14 Jan 2008 18:41:20 GMT"
},
{
"version": "v2",
"created": "Mon, 14 Jan 2008 22:22:20 GMT"
},
{
"version": "v3",
"created": "Wed, 16 Jan 2008 16:54:56 GMT"
},
{
"version": "v4",
"created": "Thu, 17 Jan 2008 15:21:49 GMT"
}
] | 2008-01-17T00:00:00 | [
[
"Lee",
"Chiu Fan",
""
]
] | [
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] |
801.1916 | Konstantinos Lagoudakis G. | K. G. Lagoudakis, M. Wouters, M. Richard, A. Baas, I. Carusotto, R.
Andre, Le Si Dang, B. Deveaud-Pledran | Quantised Vortices in an Exciton-Polariton Fluid | 14 pages, 4 figures | Nature Physics 4, 706-710 (2008) | 10.1038/nphys1051 | null | cond-mat.other | null | One of the most striking quantum effects in a low temperature interacting
Bose gas is superfluidity. First observed in liquid 4He, this phenomenon has
been intensively studied in a variety of systems for its amazing features such
as the persistence of superflows and the quantization of the angular momentum
of vortices. The achievement of Bose-Einstein condensation (BEC) in dilute
atomic gases provided an exceptional opportunity to observe and study
superfluidity in an extremely clean and controlled environment. In the solid
state, Bose-Einstein condensation of exciton polaritons has now been reported
several times. Polaritons are strongly interacting light-matter
quasi-particles, naturally occurring in semiconductor microcavities in the
strong coupling regime and constitute a very interesting example of composite
bosons. Even though pioneering experiments have recently addressed the
propagation of a fluid of coherent polaritons, still no conclusive evidence is
yet available of its superfluid nature. In the present Letter, we report the
observation of spontaneous formation of pinned quantised vortices in the
Bose-condensed phase of a polariton fluid by means of phase and amplitude
imaging. Theoretical insight into the possible origin of such vortices is
presented in terms of a generalised Gross-Pitaevskii equation. The implications
of our observations concerning the superfluid nature of the non-equilibrium
polariton fluid are finally discussed.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 19:14:41 GMT"
}
] | 2009-06-16T00:00:00 | [
[
"Lagoudakis",
"K. G.",
""
],
[
"Wouters",
"M.",
""
],
[
"Richard",
"M.",
""
],
[
"Baas",
"A.",
""
],
[
"Carusotto",
"I.",
""
],
[
"Andre",
"R.",
""
],
[
"Dang",
"Le Si",
""
],
[
"Deveaud-Pledran",
"B.",
""
]
] | [
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801.1917 | Zoltan Nagy | Zoltan Nagy and Davison E. Soper | Parton showers with quantum interference: leading color, spin averaged | 35 pages, 13 figures | JHEP 0803:030,2008 | 10.1088/1126-6708/2008/03/030 | CERN-PH-TH/2007-261 | hep-ph | null | We have previously described a mathematical formulation for a parton shower
based on the approximation of strongly ordered virtualities of successive
parton splittings. Quantum interference, including interference among different
color and spin states, is included. In this paper, we add the further
approximations of taking only the leading color limit and averaging over spins,
as is common in parton shower Monte Carlo event generators. Soft gluon
interference effects remain with this approximation. We find that the leading
color, spin averaged shower in our formalism is similar to that in other shower
formulations. We discuss some of the differences.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 19:22:04 GMT"
}
] | 2009-04-30T00:00:00 | [
[
"Nagy",
"Zoltan",
""
],
[
"Soper",
"Davison E.",
""
]
] | [
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] |
801.1918 | D Viswanath | D. Viswanath, P. Cvitanovic | Stable Manifolds and the Transition to Turbulence in Pipe Flow | null | Journal of Fluid Mechanics, vol. 627 (2009), p. 215-233 | 10.1017/S0022112009006041 | null | physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Lower-branch traveling waves and equilibria computed in pipe flow and other
shear flows appear intermediate between turbulent and laminar motions. We take
a step towards connecting these lower-branch solutions to transition by
deriving a numerical method for finding certain special disturbances of the
laminar flow in a short pipe. These special disturbances cause the disturbed
velocity field to approach the lower-branch solution by evolving along its
stable manifold. If the disturbance were slightly smaller, the flow would
relaminarize, and if slightly larger, it would transition to a turbulent state.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 20:04:49 GMT"
},
{
"version": "v2",
"created": "Wed, 24 Dec 2008 20:23:20 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Viswanath",
"D.",
""
],
[
"Cvitanovic",
"P.",
""
]
] | [
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] |
801.1919 | Helge Glockner | Helge Glockner | Solutions to open problems in Neeb's recent survey on
infinite-dimensional Lie groups | 23 pages | null | null | null | math.GR math.DG | null | We solve three open problems concerning infinite-dimensional Lie groups posed
in a recent survey article by K.-H. Neeb:
(1) There exists a subgroup of some infinite-dimensional Lie group G which
does not admit an initial Lie subgroup structure;
(2) The pathology cannot occur if G is a direct limit of an ascending
sequence of finite-dimensional Lie groups;
(3) Every such direct limit group is a ``topological group with Lie algebra''
in the sense of Hofmann and Morris.
Moreover, we prove a version of Borel's Theorem announced in the survey,
ensuring the existence of compactly supported smooth diffeomorphisms with given
Taylor series around a fixed point p (provided the tangent map at p has
positive determinant).
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 23:04:11 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Glockner",
"Helge",
""
]
] | [
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] |
801.192 | L. C. Garcia de Andrade | Garcia de Andrade | Testing a Riemannian twisted solar loop model from EUV data and magnetic
topology | Departamento de Fisica Teorica-IF-UERJ | null | null | null | astro-ph | null | Compact Riemannian solar twisted magnetic flux tube surfaces model are tested
against solar extreme ultraviolet (EUV) lines observations, allowing us to
compute the diameter and height of solar plasma loops. The relation between
magnetic and torsion energies is found for a nonplanar solar twisted
(torsioned) loop to be $10^{9}$, which shows that the contribution of torsion
energy to the solar loop is extremely weaker than the magnetic energy
contribution. In this case solar loops of up $5000 km$ in diameter can be
reached. The height of $220.000 km$ is used to obtain an estimate for torsion
based on the Riemannian flux tube surface, which yields ${\tau}_{0}=0.9{\times}
10^{-8} m^{-1}$ which coincides with one of the data of
$(0.9{\pm}0.4){\times}10^{-8}m^{-1}$ obtained by Lopez-Fuentes et al (2003).
This result tells us that the Riemannian flux tube model for plasma solar loops
is consistent with experimental results in solar physics. These results are
obtained for a homogeneous twisted solar loop. By making use of Moffatt-Ricca
theorem for the bounds on torsional energy of unknotted vortex filaments,
applied to magnetic topology, one places bounds on the lengths of EUV solar
loops. New results as the vorticity of the plasma flow along the tube is also
computed in terms of the flux tube twist.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 20:37:06 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"de Andrade",
"Garcia",
""
]
] | [
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] |
801.1921 | Angelo Tartaglia | A. Tartaglia, M. Capone, V. Cardone, N. Radicella | Fitting the luminosity data from type Ia supernovae in the frame of the
Cosmic Defect theory | 13 pages, 2 figures; Modified to improve the visibility of figures | Int.J.Mod.Phys.D18:501-512,2009 | 10.1142/S0218271809014534 | null | gr-qc | null | The Cosmic Defect (CD) theory is reviewed and used to fit the data for the
accelerated expansion of the universe, obtained from the apparent luminosity of
192 SnIa's. The fit from CD is compared with the one obtained by means of
$\Lambda $CDM. The results from both theories are in good agreement and the
fits are satisfactory. The correspondence between both approaches is discussed
and interpreted.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 21:58:24 GMT"
},
{
"version": "v2",
"created": "Wed, 16 Jan 2008 15:45:26 GMT"
}
] | 2009-05-12T00:00:00 | [
[
"Tartaglia",
"A.",
""
],
[
"Capone",
"M.",
""
],
[
"Cardone",
"V.",
""
],
[
"Radicella",
"N.",
""
]
] | [
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] |
801.1922 | Ruslan Prozorov | Ruslan Prozorov, Andrew F. Fidler, Jacob Hoberg, Paul C. Canfield | The Suprafroth (Superconducting Froth) | null | Nature Physics 4, 327 - 332 (2008) | 10.1038/nphys888 | null | cond-mat.supr-con | null | The structure and dynamics of froths have been subjects of intense interest
due to the desire to understand the behaviour of complex systems where
topological intricacy prohibits exact evaluation of the ground state. The
dynamics of a traditional froth involves drainage and drying in the cell
boundaries, thus it is irreversible. We report a new member to the froths
family: suprafroth, in which the cell boundaries are superconducting and the
cell interior is normal phase. Despite very different microscopic origin,
topological analysis of the structure of the suprafroth shows that statistical
von Neumann and Lewis laws apply. Furthermore, for the first time in the
analysis of froths there is a global measurable property, the magnetic moment,
which can be directly related to the suprafroth structure. We propose that this
suprafroth is a new, model system for the analysis of the complex physics of
two-dimensional froths.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:07:28 GMT"
}
] | 2009-02-02T00:00:00 | [
[
"Prozorov",
"Ruslan",
""
],
[
"Fidler",
"Andrew F.",
""
],
[
"Hoberg",
"Jacob",
""
],
[
"Canfield",
"Paul C.",
""
]
] | [
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] |
801.1923 | Wlodzimierz Jelonek | Wlodzimierz Jelonek | Bi-Hermitian gray surfaces II | 17 pages | Differential Geom. and its Applications 27(2009)64-74 | null | null | math.DG | null | The aim of this paper is to classify bi-Hermitian compact surfaces $(M,g)$
whose Ricci tensor $\rho$ satisfies the relation $\nabla_X\rho(X,X)
=\frac13X\tau g(X,X)$.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 22:03:03 GMT"
}
] | 2016-02-25T00:00:00 | [
[
"Jelonek",
"Wlodzimierz",
""
]
] | [
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] |
801.1924 | Martin P. W. Zerner | Elena Kosygina and Martin P.W. Zerner | Positively and negatively excited random walks on integers, with
branching processes | 31 pages, 4 figures. Minor changes | null | null | null | math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider excited random walks on the integers with a bounded number of
i.i.d. cookies per site which may induce drifts both to the left and to the
right. We extend the criteria for recurrence and transience by M. Zerner and
for positivity of speed by A.-L. Basdevant and A. Singh to this case and also
prove an annealed central limit theorem. The proofs are based on results from
the literature concerning branching processes with migration and make use of a
certain renewal structure.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 23:36:28 GMT"
},
{
"version": "v2",
"created": "Sun, 28 Sep 2008 11:47:00 GMT"
}
] | 2008-09-28T00:00:00 | [
[
"Kosygina",
"Elena",
""
],
[
"Zerner",
"Martin P. W.",
""
]
] | [
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] |
801.1925 | Paul M. Aoki | Rowena Luk, Melissa Ho, Paul M. Aoki | A Framework for Designing Teleconsultation Systems in Africa | 5 pages | Proc. Int'l Conf. on Health Informatics in Africa (HELINA),
Bamako, Mali, Jan. 2007, 28(1-5) | null | null | cs.HC | null | All of the countries within Africa experience a serious shortage of medical
professionals, particularly specialists, a problem that is only exacerbated by
high emigration of doctors with better prospects overseas. As a result, those
that remain in Africa, particularly those practicing in rural regions,
experience a shortage of specialists and other colleagues with whom to exchange
ideas. Telemedicine and teleconsultation are key areas that attempt to address
this problem by leveraging remote expertise for local problems. This paper
presents an overview of teleconsultation in the developing world, with a
particular focus on how lessons learned apply to Africa. By teleconsultation,
we are addressing non-real-time communication between health care professionals
for the purposes of providing expertise and informal recommendations, without
the real-time, interactive requirements typical of diagnosis and patient care,
which is impractical for the vast majority of existing medical practices. From
these previous experiences, we draw a set of guidelines and examine their
relevance to Ghana in particular. Based on 6 weeks of needs assessment, we
identify key variables that guide our framework, and then illustrate how our
framework is used to inform the iterative design of a prototype system.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 23:39:30 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Luk",
"Rowena",
""
],
[
"Ho",
"Melissa",
""
],
[
"Aoki",
"Paul M.",
""
]
] | [
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] |
801.1926 | Aaron Lee | Aaron T. Lee, Edward W. Thommes, Frederic A. Rasio | Resonance Trapping in Protoplanetary Disks. I. Coplanar Systems | 10 pages, 8 color figures. Accepted to the Astrophysical Journal. v2
- Added new figure, reflects accepted version | Astrophys.J.691:1684-1696,2009 | 10.1088/0004-637X/691/2/1684 | null | astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Mean-motion resonances (MMRs) are likely to play an important role both
during and after the lifetime of a protostellar gas disk. We study the
dynamical evolution and stability of planetary systems containing two giant
planets on circular orbits near a 2:1 resonance and closer. We find that by
having the outer planet migrate inward, the two planets can capture into either
the 2:1, 5:3, or 3:2 MMR. We use direct numerical integrations of ~1000 systems
in which the planets are initially locked into one of these resonances and
allowed to evolve for up to ~10^7 yr. We find that the final eccentricity
distribution in systems which ultimately become unstable gives a good fit to
observed exoplanets. Next, we integrate ~500 two-planet systems in which the
outer planet is driven to continuously migrate inward, resonantly capturing the
inner; the systems are evolved until either instability sets in or the planets
reach the star. We find that although the 5:3 resonance rapidly becomes
unstable under migration, the 2:1 and 3:2 are very stable. Thus the lack of
observed exoplanets in resonances closer than 2:1, if it continues to hold up,
may be a primordial signature of the planet formation process.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 23:44:59 GMT"
},
{
"version": "v2",
"created": "Tue, 23 Sep 2008 23:17:01 GMT"
}
] | 2009-06-23T00:00:00 | [
[
"Lee",
"Aaron T.",
""
],
[
"Thommes",
"Edward W.",
""
],
[
"Rasio",
"Frederic A.",
""
]
] | [
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] |
801.1927 | Paul M. Aoki | Rowena Luk, Melissa Ho, Paul M. Aoki | Asynchronous Remote Medical Consultation for Ghana | 10 pages | null | 10.1145/1357054.1357173 | null | cs.HC | null | Computer-mediated communication systems can be used to bridge the gap between
doctors in underserved regions with local shortages of medical expertise and
medical specialists worldwide. To this end, we describe the design of a
prototype remote consultation system intended to provide the social,
institutional and infrastructural context for sustained, self-organizing growth
of a globally-distributed Ghanaian medical community. The design is grounded in
an iterative design process that included two rounds of extended design
fieldwork throughout Ghana and draws on three key design principles (social
networks as a framework on which to build incentives within a self-organizing
network; optional and incremental integration with existing referral
mechanisms; and a weakly-connected, distributed architecture that allows for a
highly interactive, responsive system despite failures in connectivity). We
discuss initial experiences from an ongoing trial deployment in southern Ghana.
| [
{
"version": "v1",
"created": "Sat, 12 Jan 2008 23:43:18 GMT"
}
] | 2016-09-05T00:00:00 | [
[
"Luk",
"Rowena",
""
],
[
"Ho",
"Melissa",
""
],
[
"Aoki",
"Paul M.",
""
]
] | [
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801.1928 | Michael E. Peskin | Michael E. Peskin | Supersymmetry in Elementary Particle Physics | 75 pages, 36 figures | null | null | SLAC-PUB-13079 | hep-ph | null | These lectures, presented at the 2006 TASI summer school, give a general
introduction to supersymmetry, emphasizing its application to models of
elementary particle physics at the 100 GeV energy scale. I discuss the
following topics: the construction of supersymmetric Lagrangians with scalars,
fermions, and gauge bosons, the structure and mass spectrum of the Minimal
Supersymmetric Standard Model (MSSM), the measurement of the parameters of the
MSSM at high-energy colliders, and the solutions that the MSSM gives to the
problems of electroweak symmetry breaking and dark matter.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 01:22:05 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Peskin",
"Michael E.",
""
]
] | [
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801.1929 | Eric Larson | Eric Larson | The DNA Inequality in Non-Convex Regions | Versions 7--9 contains more figures, a summary of the proof, and
other modifications. Version 6 has corrected a couple of minor notational
problems with version 5. Versions 5--9 are (the same) major generalization of
the theorem proved in versions 1--4 | null | null | null | math.MG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A simple plane closed curve $\Gamma$ satisfies the DNA Inequality if the
average curvature of any closed curve contained inside $\Gamma$ exceeds the
average curvature of $\Gamma$. In 1997 Lagarias and Richardson proved that all
convex curves satisfy the DNA Inequality and asked whether this is true for any
non-convex curve. They conjectured that the DNA Inequality holds for certain
L-shaped curves. In this paper, we disprove this conjecture for all L-Shapes
and construct a large class of non-convex curves for which the DNA Inequality
holds. We also give a polynomial-time procedure for determining whether any
specific curve in a much larger class satisfies the DNA Inequality.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 02:49:43 GMT"
},
{
"version": "v2",
"created": "Mon, 21 Jan 2008 06:25:55 GMT"
},
{
"version": "v3",
"created": "Mon, 17 Mar 2008 19:55:35 GMT"
},
{
"version": "v4",
"created": "Wed, 14 May 2008 16:12:10 GMT"
},
{
"version": "v5",
"created": "Sun, 15 Jun 2008 19:01:20 GMT"
},
{
"version": "v6",
"created": "Sat, 28 Jun 2008 05:23:03 GMT"
},
{
"version": "v7",
"created": "Fri, 17 Oct 2008 06:34:00 GMT"
},
{
"version": "v8",
"created": "Thu, 5 Feb 2009 05:29:31 GMT"
},
{
"version": "v9",
"created": "Wed, 8 Apr 2009 04:10:35 GMT"
}
] | 2009-04-08T00:00:00 | [
[
"Larson",
"Eric",
""
]
] | [
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] |
801.193 | David Gilbank | David G. Gilbank and Michael L. Balogh (U. Waterloo) | Tracking Down a Critical Halo Mass for Killing Galaxies through the
Growth of the Red-Sequence | MNRAS letters accepted. 5 pages, 1 figure | null | 10.1111/j.1745-3933.2008.00445.x | null | astro-ph | null | Red-sequence galaxies record the history of terminated star-formation in the
Universe and can thus provide important clues to the mechanisms responsible for
this termination. We construct composite samples of published cluster and field
galaxy photometry in order to study the build-up of galaxies on the
red-sequence, as parameterised by the dwarf-to-giant ratio (DGR). We find that
the DGR in clusters is higher than that of the field at all redshifts, implying
that the faint end of the red-sequence was established first in clusters. We
find that the DGR evolves with redshift for both samples, consistent with the
``down-sizing'' picture of star formation. We examine the predictions of
semi-analytic models for the DGR and find that neither the magnitude of its
environmental dependence nor its evolution is correctly predicted in the
models. Red-sequence DGRs are consistently too high in the models, the most
likely explanation being that the strangulation mechanism used to remove hot
gas from satellite galaxies is too efficient. Finally we present a simple toy
model including a threshold mass, below which galaxies are not strangled, and
show that this can predict the observed evolution of the field DGR.
| [
{
"version": "v1",
"created": "Mon, 14 Jan 2008 14:28:28 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Gilbank",
"David G.",
"",
"U. Waterloo"
],
[
"Balogh",
"Michael L.",
"",
"U. Waterloo"
]
] | [
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] |
801.1931 | Anca Radulescu | Anca Radulescu, Kingsley Cox, Paul Adams | Hebbian Inspecificity in the Oja Model | 42 pages (including appendices and references); 13 figures | null | null | null | q-bio.NC q-bio.QM | null | Recent work on Long Term Potentiation in brain slices shows that Hebb's rule
is not completely synapse-specific, probably due to intersynapse diffusion of
calcium or other factors. We extend the classical Oja unsupervised model of
learning by a single linear neuron to include Hebbian inspecificity, by
introducing an error matrix E, which expresses possible crosstalk between
updating at different connections. We show the modified algorithm converges to
the leading eigenvector of the matrix EC, where C is the input covariance
matrix. When there is no inspecificity, this gives the classical result of
convergence to the first principal component of the input distribution (PC1).
We then study the outcome of learning using different versions of E. In the
most biologically plausible case, arising when there are no intrinsically
privileged connections, E has diagonal elements Q and off- diagonal elements
(1-Q)/(n-1), where Q, the quality, is expected to decrease with the number of
inputs n. We analyze this error-onto-all case in detail, for both uncorrelated
and correlated inputs. We study the dependence of the angle theta between PC1
and the leading eigenvector of EC on b, n and the amount of input activity or
correlation. (We do this analytically and using Matlab calculations.) We find
that theta increases (learning becomes gradually less useful) with increases in
b, particularly for intermediate (i.e. biologically-realistic) correlation
strength, although some useful learning always occurs up to the trivial limit Q
= 1/n. We discuss the relation of our results to Hebbian unsupervised learning
in the brain.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 03:16:12 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Radulescu",
"Anca",
""
],
[
"Cox",
"Kingsley",
""
],
[
"Adams",
"Paul",
""
]
] | [
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] |
801.1932 | Zhi-Gang Wang | Z. G. Wang | Strong decays $B_{s0} \to B_s \pi$ and $B_{s1} \to B^*_s \pi $ with
light-cone QCD sum rules | 15 pages, 2 figures, revised version | Eur.Phys.J.C56:181-187,2008 | 10.1140/epjc/s10052-008-0646-y | null | hep-ph | null | In this article, we calculate the strong coupling constants $g_{B_{s0} B_s
\eta}$ and $g_{B_{s1} B^*_s \eta}$ with the light-cone QCD sum rules. Then we
take into account the small $\eta-\pi^0$ transition matrix according to
Dashen's theorem, and obtain the small decay widths for the isospin violation
processes $B_{s0}\to B_s\eta\to B_s\pi^0$ and $B_{s1}\to B_s^*\eta\to
B_s^*\pi^0$. We can search the strange-bottomed $(0^+,1^+)$ mesons $B_{s0}$ and
$B_{s1}$ in the invariant $B_s \pi^0$ and $B^*_s \pi^0$ mass distributions
respectively.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 04:03:49 GMT"
},
{
"version": "v2",
"created": "Wed, 27 Feb 2008 02:06:14 GMT"
},
{
"version": "v3",
"created": "Wed, 12 Mar 2008 08:54:58 GMT"
},
{
"version": "v4",
"created": "Wed, 19 Mar 2008 00:24:02 GMT"
}
] | 2008-08-15T00:00:00 | [
[
"Wang",
"Z. G.",
""
]
] | [
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801.1933 | Takehisa Fujita | Takehisa Fujita | Critical Review of Path Integral Formulation | 14 pages, no figure | null | null | null | hep-th | null | The path integral formulation in quantum mechanics corresponds to the first
quantization since it is just to rewrite the quantum mechanical amplitude into
many dimensional integrations over discretized coordinates $x_n$. However, the
path integral expression cannot be connected to the dynamics of classical
mechanics, even though, superficially, there is some similarity between them.
Further, the field theory path integral in terms of many dimensional
integrations over fields does not correspond to the field quantization. We
clarify the essential difference between Feynman's original formulation of path
integral in QED and the modern version of the path integral method prevailing
in lattice field theory calculations, and show that the former can make a
correct second quantization while the latter cannot quantize fields at all and
its physical meaning is unknown.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 04:28:38 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Fujita",
"Takehisa",
""
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] |
801.1934 | Z.K.-H. Chu | Zotin K.-H. Chu | Possible Knot-type Time-dependent Quantum-mechanically Dynamical System | There are two figures | null | null | null | physics.gen-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We illustrate schematically a possible traversing along the path of
trefoil-type and $8_{18}$ knots during a specific time period by considering a
quantum-mechanic system which satisfies a specific kind of phase dynamics of
quantum mechanics. This result is relevant to the composite particle which is
present in the initial or final configuration.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 04:38:35 GMT"
},
{
"version": "v2",
"created": "Thu, 9 Apr 2009 06:00:44 GMT"
}
] | 2009-04-09T00:00:00 | [
[
"Chu",
"Zotin K. -H.",
""
]
] | [
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801.1935 | Dara Faroughy | Dara Faroughy | Slowly evolving early universe and a phenomenological model for
time-dependent fundamental constants and the leptonic masses | 7 pages, 1 figure | null | null | null | physics.gen-ph | null | A phenomenological model with an extreme accuracy is proposed for the cosmic
time variation of the primordial fundamental constants (e, h, G and c) and the
leptonic masses. The model is purely exploratory in that at the very early
times the light speed is purposely modeled to be negligibly small, indicating a
very slowly expanding universe around t=0. The impact of this idea in cosmology
and its modeling is overwhelming.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 05:39:22 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Faroughy",
"Dara",
""
]
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] |
801.1936 | Felix Izrailev M | G.L.Celardo, F.M.Izrailev, S.Sorathia, V.G.Zelevinsky, G.P.Berman | Continuum shell model: From Ericson to conductance fluctuations | 10 pages, 6 figures, corrected style and figures | AIP Conference Proceedings, Vol. 995, 2008, XIV, 232 p | 10.1063/1.2915620 | null | cond-mat.mes-hall cond-mat.stat-mech | null | We discuss an approach for studying the properties of mesoscopic systems,
where discrete and continuum parts of the spectrum are equally important. The
approach can be applied (i) to stable heavy nuclei and complex atoms near the
continuum threshold, (ii) to nuclei far from the region of nuclear stability,
both of the regions being of great current interest, and (iii) to mesoscopic
devices with interacting electrons. The goal is to develop a new consistent
version of the continuum shell model that simultaneously takes into account
strong interaction between fermions and coupling to the continuum. Main
attention is paid to the formation of compound resonances, their statistical
properties, and correlations of the cross sections. We study the Ericson
fluctuations of overlapping resonances and show that the continuum shell model
nicely describes universal properties of the conductance fluctuations.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 05:39:28 GMT"
},
{
"version": "v2",
"created": "Wed, 16 Jan 2008 03:26:51 GMT"
}
] | 2014-07-29T00:00:00 | [
[
"Celardo",
"G. L.",
""
],
[
"Izrailev",
"F. M.",
""
],
[
"Sorathia",
"S.",
""
],
[
"Zelevinsky",
"V. G.",
""
],
[
"Berman",
"G. P.",
""
]
] | [
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] |
801.1937 | Masahiro Inui | Akira Ni\'egawa | Absence of coexisting phase of quark-antiquark and diquark condensed
phases in the extended Gross-Neveu model in $2 + 1$ dimensions | 9 pages | Mod.Phys.Lett.A23:933-942,2008 | 10.1142/S0217732308026960 | null | hep-ph | null | We show that the coexisting phase of quark-antiquark and diquark condensed
phases is absent in the cold quark matter in the $2 + 1$ dimensional extended
Gross-Neveu model, which is in sharp contrast to the case of $3 + 1$
dimensional Nambu--Jona-Lasinio model.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 06:32:51 GMT"
}
] | 2008-11-26T00:00:00 | [
[
"Niégawa",
"Akira",
""
]
] | [
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] |
801.1938 | Eliot Brenner | Eliot Brenner, Florin Spinu | Artin formalism for Selberg zeta functions of co-finite Kleinian groups | 14 pages. In v2 added key reference and clarified relationship to
certain results in the literature | null | null | null | math.NT | null | Let $\Gamma\backslash\mathbb H^3$ be a finite-volume quotient of the
upper-half space, where $\Gamma\subset {\rm SL}(2,\mathbb C)$ is a discrete
subgroup. To a finite dimensional unitary representation $\chi$ of $\Gamma$ one
associates the Selberg zeta function $Z(s;\Gamma;\chi)$. In this paper we prove
the Artin formalism for the Selberg zeta function. Namely, if $\tilde\Gamma$ is
a finite index group extension of $\Gamma$ in ${\rm SL}(2,\mathbb C)$, and
$\pi={\rm Ind}_{\Gamma}^{\tilde\Gamma}\chi$ is the induced representation, then
$Z(s;\Gamma;\chi)=Z(s;\tilde\Gamma;\pi)$. In the second part of the paper we
prove by a direct method the analogous identity for the scattering function,
namely $\phi(s;\Gamma;\chi)=\phi(s;\tilde\Gamma;\pi)$, for an appropriate
normalization of the Eisenstein series.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 07:20:33 GMT"
},
{
"version": "v2",
"created": "Sat, 19 Jan 2008 22:00:32 GMT"
}
] | 2008-01-19T00:00:00 | [
[
"Brenner",
"Eliot",
""
],
[
"Spinu",
"Florin",
""
]
] | [
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] |
801.1939 | Mojtaba Mohammadi Najafabadi | Mojtaba Mohammadi Najafabadi | Probing of $Wtb$ Anomalous Couplings via the $tW$ Channel of Single Top
Production | 11 pages, 4 figures | JHEP 0803:024,2008 | 10.1088/1126-6708/2008/03/024 | null | hep-ph | null | The potential of LHC for investigation of the $W$-$t$-$b$ vertex through the
$tW$ channel of single top quark production is studied. Unlike the other two
single top quark production processes ($t-$channel and $s-$channel), the $tW$
channel provides the possibility to study the $Wtb$ vertex without receiving
contamination from FCNC. This study has been done at parton level but is
involved the separation of signal from backgrounds when both $W$-bosons decay
to leptons. In this study $\mathcal{CP}$ is assumed to be conserved. The 68%
C.L. bounds on the non-Standard Model couplings are estimated.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 07:14:01 GMT"
},
{
"version": "v2",
"created": "Mon, 18 Feb 2008 09:03:34 GMT"
},
{
"version": "v3",
"created": "Sun, 16 Mar 2008 08:25:09 GMT"
}
] | 2009-01-06T00:00:00 | [
[
"Najafabadi",
"Mojtaba Mohammadi",
""
]
] | [
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] |
801.194 | Liyun Hu | Hong-yi Fan and Li-yun Hu | Relation between quantum tomography and optical Fresnel transform | 7 pages, no figure | null | null | null | quant-ph | null | Corresponding to optical Fresnel transformation characteristic of ray
transfer matrix elements (A;B;C;D); AD-BC = 1, there exists Fresnel operator
F(A;B;C;D) in quantum optics, we show that under the Fresnel transformation the
pure position density |x><x| becomes the tomographic density |x>_rs,rs_<x|,
which is just the Radon transform of the Wigner operator, i.e.,
F|x><x|F^(+) = |x>_rs,rs_<x|= \int dx'dp'delta[x-(Dx'-Bp')]*Wigner operator
where s, r are the complex-value expression of (A;B;C;D). So the probability
distribution for the Fresnel quadrature phase is the tomography (Radon
transform of Wigner function), and the tomogram of a state |phi> is just the
wave function of its Fresnel transformed state F|phi>, i.e. rs_<x||phi>=
<x|F^(+)|phi>. Similarly, we find F|p><p|F^(+) = |p>_rs,rs_<p|= \int
dx'dp'delta[x-(Ap'-Cx')]*Wigner operator.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 08:26:31 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Fan",
"Hong-yi",
""
],
[
"Hu",
"Li-yun",
""
]
] | [
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] |
801.1941 | Jun He | Jun He, Yong-Sheng Zhang, Xiang-Fa Zhou, Qun-Feng Chen, Guang-Can Guo | Active Quantum Memory Using Oscillating Dark States | The authors declare that the paper should be withdrawn | null | null | null | quant-ph | null | An active method for long time storage of quantum superposition state in
atomic system using the Oscillating Dark States (ODS) is presented. Quantum
state of a three-level $\Lambda$ configuration atomic system oscillates
periodically between two ground levels, when two pairs of classical detuning
laser fields driving the system into the ODS under evolving adiabatic
conditions. When considering another uploading/unloading adiabatic conditions
and applying the oscillation of the ODS to quantum state storage, surprisingly,
we can obtain the greatly suppressed decoherence of the system and high
fidelity of the retrieved state, even if decay factor of coherence term of the
system density matrix $\gamma_{21}$$\cdot$ $t$$ \gg$1. The storage time is not
limited by coherence decay time of the atomic system any longer, and can be
thousands of times longer than that in those passive schemes without additional
laser fields.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 09:15:15 GMT"
},
{
"version": "v2",
"created": "Fri, 25 Jan 2008 09:26:01 GMT"
}
] | 2009-09-29T00:00:00 | [
[
"He",
"Jun",
""
],
[
"Zhang",
"Yong-Sheng",
""
],
[
"Zhou",
"Xiang-Fa",
""
],
[
"Chen",
"Qun-Feng",
""
],
[
"Guo",
"Guang-Can",
""
]
] | [
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801.1942 | Magali Rocher | Michel Matignon (IMB), Magali Rocher (IMB) | On smooth curves endowed with a large automorphism $p$-group in
characteristic $p>0$ | The section 3, concerning base change and big actions, is new | null | null | null | math.NT math.AG | null | Let $k$ be an algebraically closed field of characteristic $p>0$ and $C$ a
connected nonsingular projective curve over $k$ with genus $g \geq 2$. This
paper continues the work begun by Lehr and Matignon, namely the study of "big
actions", i.e. the pairs $(C,G)$ where $G$ is a $p$-subgroup of the
$k$-automorphism group of $C$ such that$\frac{|G|}{g} >\frac{2 p}{p-1}$. If
$G_2$ denotes the second ramification group of $G$ at the unique ramification
point of the cover $C \to C/G$, we display necessary conditions on $G_2$ for
$(C,G)$ to be a big action, which allows us to pursue the classification of big
actions. Our main source of examples comes from the construction of curves with
many rational points using ray class field theory for global function fields,
as initiated by J-P. Serre and followed by Lauter and Auer. In particular, we
obtain explicit examples of big actions with $G_2$ abelian of large exponent.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 09:37:43 GMT"
},
{
"version": "v2",
"created": "Thu, 24 Jan 2008 20:33:15 GMT"
}
] | 2008-01-24T00:00:00 | [
[
"Matignon",
"Michel",
"",
"IMB"
],
[
"Rocher",
"Magali",
"",
"IMB"
]
] | [
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] |
801.1943 | Shicheng Wang | Michel Boileau, Yi Ni, Shicheng Wang | On standard forms of 1--dominations between knots with same Gromov
volumes | 15 pages | null | null | null | math.GT | null | Let $k$ and $k'$ be two knots in 3-sphere. Say $k$ 1--dominates $k'$, if
there is a proper degree 1 map $f\co E(k)\to E(k')$, between knot exterior of
$k_i$.
Theorem: Suppose that any companion of $k$ is prime. If $k$ 1--dominates $k'$
with the same Gromov volume, then $k'$ can be obtained from $k$ by finitely
many de-satellizations.
The condition of "same Gromov volume" clearly can not be removed. We also
give a new construction of 1-domination between knots with same Gromov volume
to show that the condition "any companion of $k$ is prime" can not be removed.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 09:38:16 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Boileau",
"Michel",
""
],
[
"Ni",
"Yi",
""
],
[
"Wang",
"Shicheng",
""
]
] | [
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-0.0730497763,
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] |
801.1944 | Koji Nagata | Koji Nagata | Additional information decreases the estimated entanglement using the
Jaynes principle | To appear in Journal of Statistical Mechanics: Theory and Experiment | J. Stat. Mech. (2008) P03020 | 10.1088/1742-5468/2008/03/P03020 | null | quant-ph | null | We study a particular example considered in {[Phys. Rev. A {\bf 59,} 1799
(1999)]}, concerning the statistical inference of quantum entanglement using
the Jaynes principle. Assume a Clauser-Horne-Simony-Holt (CHSH) Bell operator,
a sum of two operators $\sqrt{2}(X+Z)$. Given only an average of the Bell-CHSH
operator, we may overestimate entanglement. However, the estimated entanglement
is decreased (never increases) when we use the expectation value of the
operator $X$ as additional information. A minimum entanglement state is
obtained by minimizing the variance of the observable $X$.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 09:43:52 GMT"
},
{
"version": "v2",
"created": "Sun, 30 Mar 2008 15:22:25 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Nagata",
"Koji",
""
]
] | [
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801.1945 | Koji Nagata | Koji Nagata | Unconditional no-hidden-variables theorem | Foundations of Physics, (2008), (accepted for publication) | null | null | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, [{arXiv:0810.3134}] is accepted and published. We present ultimate
version of no-hidden-variables theorem. We derive a proposition concerning the
quantum theory under the existence of the Bloch sphere in a single spin-1/2
system. The existence of a single classical probability space for measurement
outcome within the formalism of von Neumann's projective measurement does not
coexist with the proposition concerning the quantum theory. We have to give up
the existence of such a classical probability space for measurement outcome in
the two-dimensional Hilbert space formalism of the quantum theory. The quantum
theory does not accept a hidden-variable interpretation in the two-dimensional
space.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 09:50:14 GMT"
},
{
"version": "v2",
"created": "Mon, 19 May 2008 07:54:50 GMT"
},
{
"version": "v3",
"created": "Thu, 19 Jun 2008 07:49:49 GMT"
},
{
"version": "v4",
"created": "Tue, 21 Oct 2008 14:17:35 GMT"
},
{
"version": "v5",
"created": "Fri, 28 Nov 2008 07:10:57 GMT"
}
] | 2008-11-28T00:00:00 | [
[
"Nagata",
"Koji",
""
]
] | [
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] |
801.1946 | Shicheng Wang | Pierre Derbez and Shicheng Wang | Finiteness of mapping degrees and ${\rm PSL}(2,{\R})$-volume on graph
manifolds | 15 pages 4 figures | null | null | null | math.GT math.AT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For given closed orientable 3-manifolds $M$ and $N$ let $\c{D}(M,N)$ be the
set of mapping degrees from $M$ to $N$. We address the problem: For which $N$,
$\c{D}(M,N)$ is finite for all $M$? The answer is known in Thurston's picture
of closed orientable irreducible 3-manifolds unless the target is a non-trivial
graph manifold. We prove that for each closed non-trivial graph manifold $N$,
$\c{D}(M,N)$ is finite for all graph manifold $M$.
The proof uses a recently developed standard forms of maps between graph
manifolds and the estimation of the $\widetilde{\rm PSL}(2,{\R})$-volume for
certain class of graph manifolds.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 10:11:19 GMT"
},
{
"version": "v2",
"created": "Tue, 26 Feb 2008 01:30:08 GMT"
},
{
"version": "v3",
"created": "Tue, 14 Oct 2008 09:29:10 GMT"
}
] | 2008-10-14T00:00:00 | [
[
"Derbez",
"Pierre",
""
],
[
"Wang",
"Shicheng",
""
]
] | [
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801.1947 | Hans Gerd Evertz | Peter Pippan, Steven R. White, and Hans Gerd Evertz | Efficient Matrix Product State Method for periodic boundary conditions | Final published version | Phys. Rev. B 81, 081103(R) (2010) | 10.1103/PhysRevB.81.081103 | null | cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce an efficient method to calculate the ground state of
one-dimensional lattice models with periodic boundary conditions. The method
works in the representation of Matrix Product States (MPS), related to the
Density Matrix Renormalization Group (DMRG) method. It improves on a previous
approach by Verstraete et al. We introduce a factorization procedure for long
products of MPS matrices, which reduces the computational effort from m^5 to
m^3, where m is the matrix dimension, and m ~ 100 - 1000 in typical cases. We
test the method on the S=1/2 and S=1 Heisenberg chains. It is also applicable
to non-translationally invariant cases. The new method makes ground state
calculations with periodic boundary conditions about as efficient as
traditional DMRG calculations for systems with open boundaries.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 11:08:46 GMT"
},
{
"version": "v2",
"created": "Sun, 24 Feb 2008 10:42:40 GMT"
},
{
"version": "v3",
"created": "Tue, 16 Feb 2010 11:00:44 GMT"
}
] | 2010-02-16T00:00:00 | [
[
"Pippan",
"Peter",
""
],
[
"White",
"Steven R.",
""
],
[
"Evertz",
"Hans Gerd",
""
]
] | [
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801.1948 | Naoki Imai | Naoki Imai | On the connected components of moduli spaces of finite flat models | 13 pages | Amer. J. Math. 132 (2010), no. 5, 1189-1204 | 10.1353/ajm.2010.0006 | null | math.NT math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove that the non-ordinary component is connected in the moduli spaces of
finite flat models of two-dimensional local Galois representations over finite
fields. This was conjectured by Kisin. As an application to global Galois
representations, we prove a theorem on the modularity comparing a deformation
ring and a Hecke ring.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 11:44:26 GMT"
},
{
"version": "v2",
"created": "Fri, 14 Mar 2008 19:32:28 GMT"
},
{
"version": "v3",
"created": "Mon, 6 Oct 2008 09:14:53 GMT"
},
{
"version": "v4",
"created": "Sun, 14 Nov 2010 01:16:37 GMT"
}
] | 2020-11-24T00:00:00 | [
[
"Imai",
"Naoki",
""
]
] | [
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801.1949 | Sohrab Behnia | Sohrab Behnia, Amin Jafari, Wiria Soltanpoor, Okhtai Jahanbakhsh | Possibility of using dual frequency to control chaotic oscillations of a
spherical bubble | null | null | null | null | nlin.CD | null | Acoustic cavitation bubbles are known to exhibit highly nonlinear and
unpredictable chaotic dynamics. Their inevitable role in applications like
sonoluminescence, sonochemistry and medical procedures suggests that their
dynamics be controlled. Reducing chaotic oscillations could be the first step
in controlling the bubble dynamics by increasing the predictability of the
bubble response to an applied acoustic field. One way to achieve this concept
is to perturb the acoustic forcing. Recently, due to the improvements
associated with using dual frequency sources, this method has been the subject
of many studies which have proved its applicability and advantages. Due to this
reason, in this paper, the oscillations of a spherical bubble driven by a dual
frequency source, were studied and compared to the ones driven by a single
source. Results indicated that using dual frequency had a strong impact on
reducing the chaotic oscillations to regular ones. The governing parameters
influencing its dynamics are the secondary frequency and its phase difference
with the fundamental frequency. Also using dual frequency forcing may arm us by
the possibility of generating oscillations of desired amplitudes. To our
knowledge the investigation of the ability of using a dual frequency forcing to
control chaotic oscillations are presented for the first time in this paper.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 11:31:35 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Behnia",
"Sohrab",
""
],
[
"Jafari",
"Amin",
""
],
[
"Soltanpoor",
"Wiria",
""
],
[
"Jahanbakhsh",
"Okhtai",
""
]
] | [
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] |
801.195 | Shkalikov | A. M. Savchuk | Uniform asyptotic formulae for eigenfunctions of Sturm--Liouville
operators with singular potentials | 8 pages | null | null | null | math.SP math.FA | null | In this paper we study a Sturm--Liouville operator $Ly=-y''+q(x)y$ in the
space $L_2[0,\pi]$ with Direchlet boundary conditions. Here the potential $q$
is a fitst order distribution $q\in W_2^{-1}[0,\pi]$. Such operators were
defined in our previous papers. Here we study an asymptotic behaviour of
eigenfunctions with uniform estimates of rests. We obtain this estimates also
for potentials from Sobolev spaces $q\in W_2^{\theta-1}$, where
$\theta\in[0,1/2)$.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 11:36:46 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Savchuk",
"A. M.",
""
]
] | [
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] |
801.1951 | Andreas Kyprianou A.E. | A. E. Kyprianou, V. Rivero, R. Song | Convexity and smoothness of scale functions and de Finetti's control
problem | null | null | null | null | math.PR math.ST stat.TH | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Under appropriate conditions, we obtain smoothness and convexity properties
of $q$-scale functions for spectrally negative L\'evy processes. Our method
appeals directly to very recent developments in the theory of potential
analysis of subordinators. As an application of the latter results to scale
functions, we are able to continue the very recent work of \cite{APP2007} and
\cite{Loe}. We strengthen their collective conclusions by showing, amongst
other results, that whenever the L\'evy measure has a density which is log
convex then for $q>0$ the scale function $W^{(q)}$ is convex on some half line
$(a^*,\infty)$ where $a^*$ is the largest value at which $W^{(q)\prime}$
attains its global minimum. As a consequence we deduce that de Finetti's
classical actuarial control problem is solved by a barrier strategy where the
barrier is positioned at height $a^*$.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 12:15:27 GMT"
},
{
"version": "v2",
"created": "Wed, 16 Jan 2008 23:57:02 GMT"
},
{
"version": "v3",
"created": "Mon, 25 Aug 2008 11:35:32 GMT"
}
] | 2008-08-25T00:00:00 | [
[
"Kyprianou",
"A. E.",
""
],
[
"Rivero",
"V.",
""
],
[
"Song",
"R.",
""
]
] | [
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-0.0435016006,
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-0.0454257578,
0.0580888055,
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] |
801.1952 | Augusto Alcalde | A. M. Alcalde, C. L. Romano, L. Sanz, G. E. Marques | Phonon modulation of the spin-orbit interaction as a spin relaxation
mechanism in InSb quantum dots | 5 page, 2 figures, accepted in Phonons 2007 proceedings | null | null | null | cond-mat.mes-hall | null | We calculate the spin relaxation rates in a parabolic InSb quantum dots due
to the spin interaction with acoustical phonons. We considered the deformation
potential mechanism as the dominant electron-phonon coupling in the
Pavlov-Firsov spin-phonon Hamiltonian. By studying suitable choices of magnetic
field and lateral dot size, we determine regions where the spin relaxation
rates can be practically suppressed. We analyze the behavior of the spin
relaxation rates as a function of an external magnetic field and mean quantum
dot radius. Effects of the spin admixture due to Dresselhaus contribution to
spin-orbit interaction are also discussed.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 12:54:12 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Alcalde",
"A. M.",
""
],
[
"Romano",
"C. L.",
""
],
[
"Sanz",
"L.",
""
],
[
"Marques",
"G. E.",
""
]
] | [
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801.1953 | Jaime Forero-Romero | Jaime E. Forero-Romero | Predictability in Semi-Analytic Models of Galaxy Formation | 10 pages, 5 figures, submitted to MNRAS | null | null | null | astro-ph | null | We propose a general framework to scrutinize the performance of semi-analytic
codes of galaxy formation. The approach is based on the analysis of the outputs
from the model after a series of perturbations in the input parameters
controlling the baryonic physics. The perturbations are chosen in a way that
they do not change the results in the luminosity function or mass function of
the galaxy population. We apply this approach on a particular semi-analytic
model called GalICS. We chose to perturb the parameters controlling the
efficiency of star formation and the efficiency of supernova feedback. We keep
track of the baryonic and observable properties of the central galaxies in a
sample of dark matter halos with masses ranging from 10^{10} M_sol to 10^{13}
M_sol. We find very different responses depending on the halo mass. For small
dark matter halos its central galaxy responds in a highly predictable way to
small perturbation in the star formation and feedback efficiency. For massive
dark matter halos, minor perturbations in the input parameters can induce large
fluctuations on the properties of its central galaxy, at least $\sim 0.1$ in
(B-V) color or $\sim 0.5$ mag in U or r filter, in a seemingly random fashion.
We quantify this behavior through an objective scalar function we call
predictability. We argue that finding the origin of this behavior needs
additional information from other approximations and different semi-analytic
codes. Furthermore, the implementation of an scalar objective function, such as
the predictability, opens the door to quantitative benchmarking of
semi-analytic codes based on its numerical performance.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 13:54:54 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Forero-Romero",
"Jaime E.",
""
]
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801.1954 | Marcelo Samuel Berman | Marcelo Samuel Berman | A General Relativistic Rotating Evolutionary Universe - Part II | 7 pages including front cover. Published | Astrophysics and Space Science 315,367-369 (2008) | 10.1007/s10509-008-9830-7 | null | physics.gen-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As a sequel to (Berman, 2008a), we show that the rotation of the Universe can
be dealt by generalised Gaussian metrics, defined in this paper.
Robertson-Walker's metric has been employed with proper-time, in its standard
applications; the generalised Gaussian metric imply in the use of a
non-constant temporal metric coefficient modifying Robertson-Walker's standard
form. Experimental predictions are made
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 22:11:03 GMT"
},
{
"version": "v2",
"created": "Tue, 5 Feb 2008 12:47:11 GMT"
},
{
"version": "v3",
"created": "Wed, 6 Aug 2008 21:21:15 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Berman",
"Marcelo Samuel",
""
]
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801.1955 | Jaime Forero-Romero | Jaime E. Forero-Romero | The Coarse Geometry of Merger Trees in \Lambda CDM | 7 pages, 5 figures, submitted to MNRAS | null | 10.1111/j.1365-2966.2009.15281.x | null | astro-ph | null | We introduce the contour process to describe the geometrical properties of
merger trees. The contour process produces a one-dimensional object, the
contour walk, which is a translation of the merger tree. We portray the contour
walk through its length and action. The length is proportional to to the number
of progenitors in the tree, and the action can be interpreted as a proxy of the
mean length of a branch in a merger tree.
We obtain the contour walk for merger trees extracted from the public
database of the Millennium Run and also for merger trees constructed with a
public Monte-Carlo code which implements a Markovian algorithm. The trees
correspond to halos of final masses between 10^{11} h^{-1} M_sol and 10^{14}
h^{-1} M_sol. We study how the length and action of the walks evolve with the
mass of the final halo. In all the cases, except for the action measured from
Markovian trees, we find a transitional scale around 3 \times 10^{12} h^{-1}
M_sol. As a general trend the length and action measured from the Markovian
trees show a large scatter in comparison with the case of the Millennium Run
trees.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 14:09:47 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Forero-Romero",
"Jaime E.",
""
]
] | [
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] |
801.1956 | Takenori Okamoto Joten | Takenori J. Okamoto, Saku Tsuneta, Bruce W. Lites, Masahito Kubo,
Takaaki Yokoyama, Thomas E. Berger, Kiyoshi Ichimoto, Yukio Katsukawa,
Shin'ichi Nagata, Kazunari Shibata, Toshifumi Shimizu, Richard A. Shine,
Yoshinori Suematsu, Theodore D. Tarbell, and Alan M. Title | Emergence of a Helical Flux Rope Under an Active Region Prominence | 10 pages, 2 figures, accepted for publication in ApJ Letters | null | 10.1086/528792 | null | astro-ph | null | Continuous observations were obtained of active region 10953 with the Solar
Optical Telescope (SOT) on board the \emph{Hinode} satellite during 2007 April
28 to May 9. A prominence was located over the polarity inversion line (PIL) in
the south-east of the main sunspot. These observations provided us with a time
series of vector magnetic fields on the photosphere under the prominence. We
found four features: (1) The abutting opposite-polarity regions on the two
sides along the PIL first grew laterally in size and then narrowed. (2) These
abutting regions contained vertically-weak, but horizontally-strong magnetic
fields. (3) The orientations of the horizontal magnetic fields along the PIL on
the photosphere gradually changed with time from a normal-polarity
configuration to a inverse-polarity one. (4) The horizontal-magnetic field
region was blueshifted. These indicate that helical flux rope was emerging from
below the photosphere into the corona along the PIL under the pre-existing
prominence. We suggest that this supply of a helical magnetic flux into the
corona is associated with evolution and maintenance of active-region
prominences.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 14:32:51 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Okamoto",
"Takenori J.",
""
],
[
"Tsuneta",
"Saku",
""
],
[
"Lites",
"Bruce W.",
""
],
[
"Kubo",
"Masahito",
""
],
[
"Yokoyama",
"Takaaki",
""
],
[
"Berger",
"Thomas E.",
""
],
[
"Ichimoto",
"Kiyoshi",
""
],
[
"Katsukawa",
"Yukio",
""
],
[
"Nagata",
"Shin'ichi",
""
],
[
"Shibata",
"Kazunari",
""
],
[
"Shimizu",
"Toshifumi",
""
],
[
"Shine",
"Richard A.",
""
],
[
"Suematsu",
"Yoshinori",
""
],
[
"Tarbell",
"Theodore D.",
""
],
[
"Title",
"Alan M.",
""
]
] | [
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] |
801.1957 | Marek Radzikowski | Marek J. Radzikowski | Phase Space Factor for Two-Body Decay if One Product is a Stable Tachyon | 15 pages; LaTeX; corrected terminology ("phase _space_ factor") &
improved wording in Intro. and Concl | null | null | null | hep-th | null | We calculate the phase space factor for a two-body decay in which one of the
products is a tachyon. Two threshold conditions, a lower and an upper one, are
derived in terms of the masses of the particles and the speed of a preferred
frame. Implicit in the derivation is a consistently formulated quantum field
theory of tachyons in which spontaneous Lorentz symmetry breaking occurs. The
result is to be contrasted with a parallel calculation by Hughes and
Stephenson, which, however, implicitly adheres to strict Lorentz invariance of
the underlying quantum field theory and produces the conclusion that there is
no threshold for this process.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 15:46:30 GMT"
},
{
"version": "v2",
"created": "Tue, 15 Jan 2008 04:48:37 GMT"
},
{
"version": "v3",
"created": "Tue, 5 Feb 2008 08:08:21 GMT"
}
] | 2008-02-05T00:00:00 | [
[
"Radzikowski",
"Marek J.",
""
]
] | [
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801.1958 | Takenori Okamoto Joten | T. J. Okamoto, S. Tsuneta, T. E. Berger, K. Ichimoto, Y. Katsukawa, B.
W. Lites, S. Nagata, K. Shibata, T. Shimizu, R. A. Shine, Y. Suematsu, T. D.
Tarbell, A. M. Title | Coronal transverse magnetohydrodynamic waves in a solar prominence | 10 pages, 3 figures, published in Science (Hinode special issue) | Science 318:1577-1580,2007 | 10.1126/sci= | null | astro-ph | null | Solar prominences are cool 10$^4$ Kelvin plasma clouds supported in the
surrounding 10$^6$ Kelvin coronal plasma by as-yet undetermined mechanisms.
Observations from \emph{Hinode} show fine-scale threadlike structures
oscillating in the plane of the sky with periods of several minutes. We suggest
these transverse magnetohydrodynamic waves may represent Alfv\'en waves
propagating on coronal magnetic field lines and these may play a role in
heating the corona.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 15:02:41 GMT"
}
] | 2009-07-09T00:00:00 | [
[
"Okamoto",
"T. J.",
""
],
[
"Tsuneta",
"S.",
""
],
[
"Berger",
"T. E.",
""
],
[
"Ichimoto",
"K.",
""
],
[
"Katsukawa",
"Y.",
""
],
[
"Lites",
"B. W.",
""
],
[
"Nagata",
"S.",
""
],
[
"Shibata",
"K.",
""
],
[
"Shimizu",
"T.",
""
],
[
"Shine",
"R. A.",
""
],
[
"Suematsu",
"Y.",
""
],
[
"Tarbell",
"T. D.",
""
],
[
"Title",
"A. M.",
""
]
] | [
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801.1959 | Oriol Romero-Isart | Alex Monras and Oriol Romero-Isart | Quantum Information Processing with Quantum Zeno Many-Body Dynamics | 13 pages, 8 figures. Significantly extended, including two-qubit
gates and parity measurements. To appear in Quantum Information & Computation | Quant. Inf. Comp. 10, 201 (2010) | null | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how the quantum Zeno effect can be exploited to control quantum
many-body dynamics for quantum information and computation purposes. In
particular, we consider a one dimensional array of three level systems
interacting via a nearest-neighbour interaction. By encoding the qubit on two
levels and using simple projective frequent measurements yielding the quantum
Zeno effect, we demonstrate how to implement a well defined quantum register,
quantum state transfer on demand, universal two-qubit gates and two-qubit
parity measurements. Thus, we argue that the main ingredients for universal
quantum computation can be achieved in a spin chain with an always-on and
constant many-body Hamiltonian. We also show some possible modifications of the
initially assumed dynamics in order to create maximally entangled qubit pairs
and single qubit gates.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 15:12:45 GMT"
},
{
"version": "v2",
"created": "Fri, 20 Nov 2009 12:41:09 GMT"
}
] | 2010-02-11T00:00:00 | [
[
"Monras",
"Alex",
""
],
[
"Romero-Isart",
"Oriol",
""
]
] | [
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801.196 | Alfio Bonanno | Alfio Bonanno, Vadim Urpin | Magnetic shear-driven instability and turbulent mixing in magnetized
protostellar disks | 8 pages, 6 figures, A&A to appear | null | 10.1051/0004-6361:20077562 | null | astro-ph | null | Observations of protostellar disks indicate the presence of the magnetic
field of thermal (or superthermal) strength. In such a strong magnetic field,
many MHD instabilities responsible for turbulent transport of the angular
momentum are suppressed. We consider the shear-driven instability that can
occur in protostellar disks even if the field is superthermal. This instability
is caused by the combined influence of shear and compressibility in a
magnetized gas and can be an efficient mechanism to generate turbulence in
disks. The typical growth time is of the order of several rotation periods.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 15:30:12 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Bonanno",
"Alfio",
""
],
[
"Urpin",
"Vadim",
""
]
] | [
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-0.0185579639,
-0.0286240522,
-0.0452530533,
0.0869142413,
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0.0068012611,
0.1180437282,
-0.0693540201,
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] |
801.1961 | Fabio Trani | F. Buonocore, F. Trani, D. Ninno, A. Di Matteo, G. Cantele and G.
Iadonisi | Ab initio calculations of electron affinity and ionization potential of
carbon nanotubes | null | Nanotechnology 19, 025711 (2008) | 10.1088/0957-4484/19/02/025711 | null | cond-mat.mtrl-sci | null | By combining ab initio all-electron localized orbital and pseudopotential
plane-wave approaches we report on calculations of the electron affinity (EA)
and the ionization potential (IP) of (5, 5) and (7, 0) single-wall carbon
nanotubes. The role played by finite-size effects and nanotube termination has
been analysed by comparing several hydrogen-passivated and not passivated
nanotube segments. The dependence of the EA and IP on both the quantum
confinement effect, due to the nanotube finite length, and the charge
accumulation on the edges, is studied in detail. Also, the EA and IP are
compared to the energies of the lowest unoccupied and highest occupied states,
respectively, upon increasing the nanotube length. We report a slow convergence
with respect to the number of atoms. The effect of nanotube packing in arrays
on the electronic properties is eventually elucidated as a function of the
intertube distance.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 15:34:23 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Buonocore",
"F.",
""
],
[
"Trani",
"F.",
""
],
[
"Ninno",
"D.",
""
],
[
"Di Matteo",
"A.",
""
],
[
"Cantele",
"G.",
""
],
[
"Iadonisi",
"G.",
""
]
] | [
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] |
801.1962 | Gert De Cooman | Gert de Cooman, Matthias C. M. Troffaes, Enrique Miranda | n-Monotone exact functionals | null | Journal of Mathematical Analysis and Applications 347 (2008)
143-156 | 10.1016/j.jmaa.2008.05.071 | null | math.FA math.PR | null | We study n-monotone functionals, which constitute a generalisation of
n-monotone set functions. We investigate their relation to the concepts of
exactness and natural extension, which generalise the notions of coherence and
natural extension in the behavioural theory of imprecise probabilities. We
improve upon a number of results in the literature, and prove among other
things a representation result for exact n-monotone functionals in terms of
Choquet integrals.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 15:44:12 GMT"
}
] | 2018-08-10T00:00:00 | [
[
"de Cooman",
"Gert",
""
],
[
"Troffaes",
"Matthias C. M.",
""
],
[
"Miranda",
"Enrique",
""
]
] | [
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] |
801.1963 | Delio Mugnolo | Delio Mugnolo | Asymptotics of semigroups generated by operator matrices | null | null | 10.1007/s40065-014-0107-4 | null | math.FA math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We survey some known results about operator semigroup generated by operator
matrices with diagonal or coupled domain. These abstract results are applied to
the characterization of well-/ill-posedness for a class of evolution equations
with dynamic boundary conditions on domains or metric graphs. In particular,
our ill-posedness results on the heat equation with general Wentzell-type
boundary conditions complement those previously obtained by, among others,
Bandle-von Below-Reichel and Vitillaro-V\'azquez.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:05:47 GMT"
},
{
"version": "v2",
"created": "Sun, 1 Dec 2013 21:05:03 GMT"
}
] | 2019-06-05T00:00:00 | [
[
"Mugnolo",
"Delio",
""
]
] | [
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] |
801.1964 | Zengru Di | Yanqing Hu, Jinshan Wu, Zengru Di | Enhance the Efficiency of Heuristic Algorithm for Maximizing Modularity
Q | 9 pages, 3 figures | null | 10.1209/0295-5075/85/18009 | null | physics.soc-ph | null | Modularity Q is an important function for identifying community structure in
complex networks. In this paper, we prove that the modularity maximization
problem is equivalent to a nonconvex quadratic programming problem. This result
provide us a simple way to improve the efficiency of heuristic algorithms for
maximizing modularity Q. Many numerical results demonstrate that it is very
effective.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:13:43 GMT"
}
] | 2009-11-13T00:00:00 | [
[
"Hu",
"Yanqing",
""
],
[
"Wu",
"Jinshan",
""
],
[
"Di",
"Zengru",
""
]
] | [
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] |
801.1965 | Ruisheng Liu | R. S. Liu (1 and 2), L. Michalak (3), C. M. Canali (3), L. Samuelson
(2) and H. Pettersson (1 and 2) ((1) Center for Applied Mathematics and
Physics, Halmstad University, Halmstad, Sweden, (2) Solid State Physics/ the
Nanometer Structure Consortium, Lund University, Lund, Sweden, (3) Department
of Physics and Mathematics, School of Pure and Applied Natural Sciences,
Kalmar University, Kalmar, Sweden) | Tunneling Anisotropic Magnetoresistance in Co/AlOx/Au Tunnel Junctions | 11 pages, 5 figures. Accpted for publishing on Nano Letters, 2008 | null | 10.1021/nl072985p | null | physics.pop-ph | null | We observe spin-valve-like effects in nano-scaled thermally evaporated
Co/AlOx/Au tunnel junctions. The tunneling magnetoresistance is anisotropic and
depends on the relative orientation of the magnetization direction of the Co
electrode with respect to the current direction. We attribute this effect to a
two-step magnetization reversal and an anisotropic density of states resulting
from spin-orbit interaction. The results of this study points to future
applications of novel spintronics devices involving only one ferromagnetic
layer.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:24:45 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Liu",
"R. S.",
"",
"1 and 2"
],
[
"Michalak",
"L.",
"",
"1 and 2"
],
[
"Canali",
"C. M.",
"",
"1 and 2"
],
[
"Samuelson",
"L.",
"",
"1 and 2"
],
[
"Pettersson",
"H.",
"",
"1 and 2"
]
] | [
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] |
801.1966 | Gert De Cooman | Gert de Cooman and Enrique Miranda | Symmetry of models versus models of symmetry | 61 pages | null | null | null | math.ST stat.TH | null | A model for a subject's beliefs about a phenomenon may exhibit symmetry, in
the sense that it is invariant under certain transformations. On the other
hand, such a belief model may be intended to represent that the subject
believes or knows that the phenomenon under study exhibits symmetry. We defend
the view that these are fundamentally different things, even though the
difference cannot be captured by Bayesian belief models. In fact, the failure
to distinguish between both situations leads to Laplace's so-called Principle
of Insufficient Reason, which has been criticised extensively in the
literature.
We show that there are belief models (imprecise probability models, coherent
lower previsions) that generalise and include the Bayesian belief models, but
where this fundamental difference can be captured. This leads to two notions of
symmetry for such belief models: weak invariance (representing symmetry of
beliefs) and strong invariance (modelling beliefs of symmetry). We discuss
various mathematical as well as more philosophical aspects of these notions. We
also discuss a few examples to show the relevance of our findings both to
probabilistic modelling and to statistical inference, and to the notion of
exchangeability in particular.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:15:17 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"de Cooman",
"Gert",
""
],
[
"Miranda",
"Enrique",
""
]
] | [
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] |
801.1967 | Ivan Arzhantsev | Ivan V. Arzhantsev | Projective embeddings of homogeneous spaces with small boundary | 15 pages | Izv. Ross. Akad. Nauk Ser. Mat. 73:3 (2009), 5-22; translation in
Izvestiya Math. 73:3 (2009), 437-453 | 10.1070/IM2009v073n03ABEH002453 | null | math.AG math.AC | null | We study open equivariant projective embeddings of homogeneous spaces such
that the complement of the open orbit does not contain divisors. Criterions of
existence of such an embedding are considered and finiteness of isomorphism
classes of embeddings for a given homogeneous space is proved. Any embedding
with small boundary is realized as a GIT-quotient associated with a
linearization of the trivial line bundle on the space of the canonical
embedding. The generalized Cox's construction and the theory of bunched rings
allow us to describe basic geometric properties of embeddings with small
boundary in combinatorial terms.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:23:07 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Arzhantsev",
"Ivan V.",
""
]
] | [
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] |
801.1968 | Iosif Galanakis | I. Galanakis, E. Sasioglu and K. Ozdogan | 3d-electron induced magnetic phase transition in half-metallic
semi-Heusler alloys | null | Physical Review B 77, 214417 (2008) | 10.1103/PhysRevB.77.214417 | null | cond-mat.mtrl-sci | null | We study the effect of the non-magnetic 3\textit{d} atoms on the magnetic
properties of the half-metallic (HM) semi-Heusler alloys Co$_{1-x}$Cu$_{x}$MnSb
and Ni$_{1-x}$Cu$_{x}$MnSb ($0 \leq x \leq 1$) using first-principles
calculations. We determine the magnetic phase diagram of both systems at zero
temperature and obtain a phase transition from a ferromagnetic to an
antiferromagnetic state. For low Cu concentrations the ferromagnetic RKKY-like
exchange mechanism is dominating, while the antiferromagnetic superexchange
coupling becomes important for larger Cu content leading to the observed
magnetic phase transition. A strong dependence of the magnetism in both systems
on the position of the Fermi level within the HM gap is obtained. Obtained
results are in good agreement with the available experimental data.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 16:24:54 GMT"
}
] | 2015-05-13T00:00:00 | [
[
"Galanakis",
"I.",
""
],
[
"Sasioglu",
"E.",
""
],
[
"Ozdogan",
"K.",
""
]
] | [
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] |
801.1969 | Pierre Albin | Pierre Albin, Frederic Rochon | Families index for manifolds with hyperbolic cusp singularities | Changed the convention used for eta forms | null | null | null | math.DG math.AP | null | Manifolds with fibered hyperbolic cusp metrics include hyperbolic manifolds
with cusps and locally symmetric spaces of Q-rank one. We extend Vaillant's
treatment of Dirac-type operators associated to these metrics by weaking the
hypotheses on the boundary families through the use of Fredholm perturbations
as in the family index theorem of Melrose and Piazza and by treating the index
of families of such operators. We also extend the index theorem of Moroianu and
Leichtnam-Mazzeo-Piazza to families of perturbed Dirac-type operators
associated to fibered cusp metrics (sometimes known as fibered boundary
metrics).
| [
{
"version": "v1",
"created": "Mon, 14 Jan 2008 18:13:29 GMT"
},
{
"version": "v2",
"created": "Tue, 8 Apr 2008 15:29:23 GMT"
}
] | 2008-04-08T00:00:00 | [
[
"Albin",
"Pierre",
""
],
[
"Rochon",
"Frederic",
""
]
] | [
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801.197 | Hannes Jung | Hannes Jung | Vector meson cross sections at HERA | on behalf of the H1 and ZEUS Collaborations, to be published in
Proceedings of ISMD07 | Acta Phys.Polon.Supp.1:531-534,2008 | null | null | hep-ex | null | Inelastic and elastic (exclusive) cross section measurements of vector meson
production at HERA are discussed.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 17:20:10 GMT"
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] | 2009-01-16T00:00:00 | [
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] |
801.1971 | Guenter Nimtz | G. Nimtz and A.A. Stahlhofen | Comment on "Direct space-time observation of pulse tunneling in an
electromagnetic band gap" | null | null | null | null | quant-ph | null | The investigation presented by Doiron, Hache, and Winful [Phys. Rev. A 76,
023823 (2007)] is not valid for the tunneling process as claimed in the paper.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 17:21:39 GMT"
}
] | 2008-01-15T00:00:00 | [
[
"Nimtz",
"G.",
""
],
[
"Stahlhofen",
"A. A.",
""
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801.1972 | Joel Shapiro | Paul S. Bourdon and Joel H. Shapiro | Intertwining relations and extended eigenvalues for analytic Toeplitz
operators | 23 pages, one figure, pdfLaTex format | null | null | null | math.FA math.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the intertwining relations between analytic Toeplitz operators
induced on the Hardy space H^2 by analytic functions bounded on the open unit
disc. Our work centers on the connection between intertwining between the
Toeplitz operators the image containment between their symbols, as well as on
the nature of the intertwining operator. We use our results to study the
"extended eigenvalues" of analytic Toeplitz operators, i.e., the special case
where the operator is intertwined with a scalar multiple of itself.
| [
{
"version": "v1",
"created": "Sun, 13 Jan 2008 17:23:46 GMT"
},
{
"version": "v2",
"created": "Tue, 31 Mar 2009 14:59:26 GMT"
}
] | 2009-03-31T00:00:00 | [
[
"Bourdon",
"Paul S.",
""
],
[
"Shapiro",
"Joel H.",
""
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