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801.0273
Mark Coffey
Mark W. Coffey
On a three-dimensional symmetric Ising tetrahedron, and contributions to the theory of the dilogarithm and Clausen functions
56 pages, no figures Proposition 10 added, proving another conjecture
J.Math.Phys.49:043510,2008
10.1063/1.2902996
null
math-ph math.MP
null
Perturbative quantum field theory for the Ising model at the three-loop level yields a tetrahedral Feynman diagram C(a,b) with masses a and b and four other lines with unit mass. The completely symmetric tetrahedron C^Tet \equiv C(1,1) has been of interest from many points of view, with several representations and conjectures having been given in the literature. We prove a conjectured exponentially fast convergent sum for C(1,1), as well as a previously empirical relation for C(1,1) as a remarkable difference of Clausen function values. Our presentation includes Propositions extending the theory of the dilogarithm Li_2 and Clausen Cl_2 functions, as well as their relation to other special functions of mathematical physics. The results strengthen connections between Feynman diagram integrals, volumes in hyperbolic space, number theory, and special functions and numbers, specifically including dilogarithms, Clausen function values, and harmonic numbers.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 04:06:18 GMT" }, { "version": "v2", "created": "Mon, 21 Jan 2008 22:36:39 GMT" } ]
2008-11-26T00:00:00
[ [ "Coffey", "Mark W.", "" ] ]
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801.0274
Douglas Scott
Gregory Paciga, Douglas Scott and Edward L. Chapin
Strong lensing of submillimetre galaxies: A tracer of foreground structure?
Replaced to match accepted version, including new Appendix on evolutionary model and additional author, now 11 pages
null
10.1111/j.1365-2966.2009.14627.x
null
astro-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
The steep source counts and negative K-corrections of bright submillimetre galaxies (SMGs) suggest that a significant fraction of those observed at high flux densities may be gravitationally lensed, and that the lensing objects may often lie at redshifts above 1, where clusters of galaxies are difficult to detect through other means. In this case follow-up of bright SMGs may be used to identify dense structures along the line of sight. Here we investigate the probability for SMGs to experience strong lensing, using the latest N-body simulations and observed source flux and redshift distributions. We find that almost all high redshift sources with a flux density above 100mJy will be lensed, if they are not relatively local galaxies. We also give estimates of the fraction of sources experiencing strong lensing as a function of observed flux density. This has implications for planning follow-up observations for bright SMGs discovered in future surveys with SCUBA-2 and other instruments. The largest uncertainty in these calculations is the maximum allowed lensing amplification, which is dominated by the presently unknown spatial extent of SMGs.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 04:47:06 GMT" }, { "version": "v2", "created": "Wed, 11 Feb 2009 18:27:18 GMT" } ]
2015-05-13T00:00:00
[ [ "Paciga", "Gregory", "" ], [ "Scott", "Douglas", "" ], [ "Chapin", "Edward L.", "" ] ]
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801.0275
Vincent Tan
Vincent Y. F. Tan, Vivek K. Goyal
Estimating Signals with Finite Rate of Innovation from Noisy Samples: A Stochastic Algorithm
Submitted to IEEE Transactions on Signal Processing
IEEE Trans. on Signal Processing, vol. 56, no. 10, pp. 5135-5146, October 2008
10.1109/TSP.2008.928510
null
stat.AP cs.IT math.IT
null
As an example of the recently-introduced concept of rate of innovation, signals that are linear combinations of a finite number of Diracs per unit time can be acquired by linear filtering followed by uniform sampling. However, in reality, samples are rarely noiseless. In this paper, we introduce a novel stochastic algorithm to reconstruct a signal with finite rate of innovation from its noisy samples. Even though variants of this problem has been approached previously, satisfactory solutions are only available for certain classes of sampling kernels, for example kernels which satisfy the Strang-Fix condition. In this paper, we consider the infinite-support Gaussian kernel, which does not satisfy the Strang-Fix condition. Other classes of kernels can be employed. Our algorithm is based on Gibbs sampling, a Markov chain Monte Carlo (MCMC) method. Extensive numerical simulations demonstrate the accuracy and robustness of our algorithm.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 05:19:35 GMT" }, { "version": "v2", "created": "Thu, 3 Jan 2008 01:09:41 GMT" } ]
2009-03-09T00:00:00
[ [ "Tan", "Vincent Y. F.", "" ], [ "Goyal", "Vivek K.", "" ] ]
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801.0276
Nithin Nagaraj
Nikhil Balaji and Nithin Nagaraj
Cryptanalysis of a Chaotic Image Encryption Algorithm
11 pages, 4 figures, 1 table. Poster presented at National Conference on Nonlinear Systems and Dynamics, Physical Research Laboratory, Ahmedabad, Jan 3-5, 2008. Made changes to the paper based on Chengqing Li's useful comments
null
null
null
nlin.CD
null
Line map, an invertible, two-dimensional chaotic encryption algorithm was introduced recently. In this paper, we propose several weaknesses of the method based on standard cryptanalytic attacks. We perform a side-channel attack by observing the execution time of the encryption algorithm and successfully reduce the key space by a factor of 10^4 for a key length of 16 digits. We find the existence of equivalent keys which reduce the key space by a significant margin, even in the absence of any attack. Also, we find that the ciphertext is not sensitive to small changes in the plaintext due to poor diffusion.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 05:59:17 GMT" }, { "version": "v2", "created": "Sat, 12 Jan 2008 15:01:32 GMT" } ]
2008-01-12T00:00:00
[ [ "Balaji", "Nikhil", "" ], [ "Nagaraj", "Nithin", "" ] ]
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801.0277
Chetan Gadgil
Chetan J Gadgil
Size-independent differences between the mean of discrete stochastic systems and the corresponding continuous deterministic systems
16 pages
null
null
null
q-bio.OT q-bio.QM
null
In this paper I show that, for a class of reaction networks, the discrete stochastic nature of the reacting species and reactions results in qualitative and quantitative differences between the mean of exact stochastic simulations and the prediction of the corresponding deterministic system. The differences are independent of the number of molecules of each species in the system under consideration. These reaction networks are open systems of chemical reactions with no zero-order reaction rates systems. They are characterized by at least two stationary points, one of which is a nonzero stable point, and one unstable trivial solution (stability based on a linear stability analysis of the deterministic system). Starting from a nonzero initial condition, the deterministic system never reaches the zero stationary point due to its unstable nature. In contrast, the result presented here proves that this zero-state is the only stable stationary state for the discrete stochastic system. This result generalizes previous theoretical studies and simulations of specific systems and provides a theoretical basis for analyzing a class of systems that exhibit such inconsistent behavior. This result has implications in the simulation of infection, apoptosis, and population kinetics, as it can be shown that for certain models the stochastic simulations will always yield different predictions for the mean behavior than the deterministic simulations.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 07:05:41 GMT" } ]
2008-01-03T00:00:00
[ [ "Gadgil", "Chetan J", "" ] ]
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801.0278
Amir Daneshgar
Amir Daneshgar, Hossein Hajiabolhassan and Ramin Javadi
On The Isoperimetric Spectrum of Graphs and Its Approximations
null
J. Combinatorial Theory, Series B, 2010
10.1016/j.jctb.2010.01.002
null
math.CO
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
In this paper we consider higher isoperimetric numbers of a (finite directed) graph. In this regard we focus on the $n$th mean isoperimetric constant of a directed graph as the minimum of the mean outgoing normalized flows from a given set of $n$ disjoint subsets of the vertex set of the graph. We show that the second mean isoperimetric constant in this general setting, coincides with (the mean version of) the classical Cheeger constant of the graph, while for the rest of the spectrum we show that there is a fundamental difference between the $n$th isoperimetric constant and the number obtained by taking the minimum over all $n$-partitions. In this direction, we show that our definition is the correct one in the sense that it satisfies a Federer-Fleming-type theorem, and we also define and present examples for the concept of a supergeometric graph as a graph whose mean isoperimetric constants are attained on partitions at all levels. Moreover, considering the ${\bf NP}$-completeness of the isoperimetric problem on graphs, we address ourselves to the approximation problem where we prove general spectral inequalities that give rise to a general Cheeger-type inequality as well. On the other hand, we also consider some algorithmic aspects of the problem where we show connections to orthogonal representations of graphs and following J.~Malik and J.~Shi ($2000$) we study the close relationships to the well-known $k$-means algorithm and normalized cuts method.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 07:49:58 GMT" }, { "version": "v2", "created": "Fri, 30 Jan 2015 23:25:07 GMT" } ]
2015-02-03T00:00:00
[ [ "Daneshgar", "Amir", "" ], [ "Hajiabolhassan", "Hossein", "" ], [ "Javadi", "Ramin", "" ] ]
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801.0279
Diego Falceta-Goncalves Prof. Dr.
D. Falceta-Goncalves (NAT-Unicsul, UW-Madison), A. Lazarian (UW-Madison), G. Kowal (UW-Madison)
Studies of regular and random magnetic fields in the ISM: statistics of polarization vectors and the Chandrasekhar-Fermi technique
submitted to ApJ, 42 pages
null
10.1086/587479
null
astro-ph
null
Polarimetry is extensively used as a tool to trace the interstellar magnetic field projected on the plane of sky. Moreover, it is also possible to estimate the magnetic field intensity from polarimetric maps based on the Chandrasekhar-Fermi method. In this work, we present results for turbulent, isothermal, 3-D simulations of sub/supersonic and sub/super-Alfvenic cases. With the cubes, assuming perfect grain alignment, we created synthetic polarimetric maps for different orientations of the mean magnetic field with respect to the line of sight (LOS). We show that the dispersion of the polarization angle depends on the angle of the mean magnetic field regarding the LOS and on the Alfvenic Mach number. However, the second order structure function of the polarization angle follows the relation $SF \propto l^{\alpha}$, $\alpha$ being dependent exclusively on the Alfvenic Mach number. The results show an anti-correlation between the polarization degree and the column density, with exponent $\gamma \sim -0.5$, in agreement with observations, which is explained by the increase in the dispersion of the polarization angle along the LOS within denser regions. However, this effect was observed exclusively on supersonic, but sub-Alfvenic, simulations. For the super-Alfvenic, and the subsonic model, the polarization degree showed to be intependent on the column density. Our major quantitative result is a generalized equation for the CF method, which allowed us to determine the magnetic field strength from the polarization maps with errors $< 20%$. We also account for the role of observational resolution on the CF method.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 08:41:21 GMT" } ]
2009-11-13T00:00:00
[ [ "Falceta-Goncalves", "D.", "", "NAT-Unicsul, UW-Madison" ], [ "Lazarian", "A.", "", "UW-Madison" ], [ "Kowal", "G.", "", "UW-Madison" ] ]
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801.028
Anjan Ananda Sen
Anjan A. Sen and Diego Pavon
Reconstructing the interaction rate in holographic models of dark energy
7 pages, three eps figures, Latex Style, Accepted for Publication in Phys.Lett.B
Phys.Lett.B664:7-11,2008
10.1016/j.physletb.2008.04.055
null
astro-ph
null
We reconstruct the interaction rate of the holographic dark energy model recently proposed by Zimdahl and Pav\'{o}n \cite{wd} in the redshift interval $0 < z < 1.8$ with observational data from supernovae type Ia, baryon acoustic oscillations, gas mass fraction in galaxy clusters, and the growth factor. It shows a reasonable behavior in the sense that it increases with expansion from a small or vanishing value in the long past but starts decreasing at recent times. The later feature suggests that the equation of state parameter of dark energy does not cross the phantom divide.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 08:36:56 GMT" }, { "version": "v2", "created": "Mon, 28 Apr 2008 04:27:19 GMT" } ]
2009-06-23T00:00:00
[ [ "Sen", "Anjan A.", "" ], [ "Pavon", "Diego", "" ] ]
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801.0281
Hanzhong Wu
Hanzhong Wu
On Certain Hypotheses in Optimal Control Theory and the Relationship of the Maximum Principle with the Dynamic Programming Method Proposed by L. I. Rozonoer
18pages
null
null
null
math.OC
null
In this paper we will study three hypotheses proposed by L. I. Rozonoer (Automation and Remote Control, 2003, vol.64, no.8, pp.1237--1240) in optimal control theory in order to derive conditions for the existence of an optimal control under all initial conditions, and the relationships between Pontryagin maximum principle and the dynamic programming method.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 08:44:31 GMT" } ]
2008-01-03T00:00:00
[ [ "Wu", "Hanzhong", "" ] ]
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801.0282
Nilanjana Datta
Nilanjana Datta and Renato Renner
Smooth Renyi Entropies and the Quantum Information Spectrum
null
IEEE Transactions on Information Theory, vol. 55, pp. 2807-2815, 2009
10.1109/TIT.2009.2018340
null
quant-ph
null
Many of the traditional results in information theory, such as the channel coding theorem or the source coding theorem, are restricted to scenarios where the underlying resources are independent and identically distributed (i.i.d.) over a large number of uses. To overcome this limitation, two different techniques, the information spectrum method and the smooth entropy framework, have been developed independently. They are based on new entropy measures, called spectral entropy rates and smooth entropies, respectively, that generalize Shannon entropy (in the classical case) and von Neumann entropy (in the more general quantum case). Here, we show that the two techniques are closely related. More precisely, the spectral entropy rate can be seen as the asymptotic limit of the smooth entropy. Our results apply to the quantum setting and thus include the classical setting as a special case.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 19:14:55 GMT" } ]
2009-06-28T00:00:00
[ [ "Datta", "Nilanjana", "" ], [ "Renner", "Renato", "" ] ]
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801.0283
Mikhail G. Katz
Mikhail G. Katz and Steven Shnider
Cayley 4-form, comass, and triality isomorphisms
20 pages
null
null
null
math.DG math.MG math.RT
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Following an idea of Dadok, Harvey and Lawson, we apply the triality property of SO(8) to study the comass of certain self-dual 4-forms on R^8. In particular, we prove that the Cayley 4-form has comass 1 and that any self-dual 4-form realizing the maximal Wirtinger ratio is SO(8)-conjugate to the Cayley 4-form. We also use triality to prove that the stabilizer in SO(8) of the Cayley form is Spin(7). The results have applications in systolic geometry, calibrated geometry, and Spin(7) manifolds.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 08:57:50 GMT" }, { "version": "v2", "created": "Fri, 24 Oct 2008 10:48:43 GMT" } ]
2008-10-24T00:00:00
[ [ "Katz", "Mikhail G.", "" ], [ "Shnider", "Steven", "" ] ]
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801.0284
Harish Seshadri
Harish Seshadri, Fangyang Zheng
Complex product manifolds cannot be negatively curved
6 Pages. To appear in The Asian Journal of Mathematics
null
null
null
math.DG math.CV
null
We show that if $M = X \times Y$ is the product of two complex manifolds (of positive dimensions), then $M$ does not admit any complete K\"ahler metric with bisectional curvature bounded between two negative constants. More generally, a locally-trivial holomorphic fibre-bundle does not admit such a metric.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 09:14:10 GMT" } ]
2008-01-03T00:00:00
[ [ "Seshadri", "Harish", "" ], [ "Zheng", "Fangyang", "" ] ]
[ 0.0105376961, 0.0708208084, -0.0389912315, 0.1054120734, 0.0113100316, 0.0086302618, -0.0240594149, -0.0642676577, 0.0015139527, 0.0197530612, -0.0580421686, -0.0711952746, 0.0434380099, 0.0266338661, 0.1287225485, 0.0467847958, -0.0656251013, 0.0314551108, 0.0247849431, 0.0944589525, 0.0542038977, -0.004879755, 0.0011950718, 0.0555145256, -0.0298402291, 0.000247023, -0.016172234, 0.0117664114, 0.0987653062, 0.0881866515, 0.0414252579, -0.0290912967, -0.0515826382, 0.0173307359, -0.127880007, 0.1572755575, -0.0490549952, 0.1068163142, 0.0674038082, 0.1098120436, -0.017693501, 0.1396756768, -0.0373529457, -0.0567315407, 0.0265168454, 0.0520039126, -0.0043560881, 0.1183311343, -0.0405124985, -0.0427592918, -0.072973989, 0.0535953902, 0.0473230928, -0.0901525989, -0.0637527704, 0.0116903484, -0.0273593944, 0.0000801316, -0.0358784869, -0.0597272664, 0.0607570447, -0.1017610282, -0.016511593, 0.0273827985, -0.0818675458, -0.0034842854, -0.0157626625, -0.0407933481, -0.0094260015, 0.0379380472, -0.1164588034, 0.0295359753, -0.0374933705, 0.1235736534, 0.0351763628, 0.0111871604, 0.0468550101, 0.1055993065, 0.0550464466, -0.0240126066, 0.071897395, 0.0960504264, 0.0746122748, 0.0314317085, -0.010122274, -0.0085307946, -0.0348721109, -0.0428529084, -0.092305772, 0.0134924641, 0.0279679, 0.0048300214, -0.0865951702, 0.0379146449, 0.0519102961, 0.0136328889, 0.017014781, 0.0575740896, -0.0001717824, 0.0576677062, -0.0405359045, 0.103446126, 0.0332104191, 0.0534549654, 0.1533436626, 0.0485869125, -0.0222455971, 0.0517698713, -0.0177403092, 0.0233104844, 0.0393656977, -0.0503656268, -0.0483528711, 0.10747163, 0.0712888911, -0.0662336051, -0.069931455, -0.0319231935, 0.006313256, -0.001626585, 0.002046396, -0.0068515507, 0.003121522, -0.0710548535, 0.0251360051, -0.0010568415, -0.0944589525, -0.0004764929, -0.1481947601, -0.0627698004, 0.0728335604, -0.0293019339, 0.0102217412, -0.0855185837, -0.0066116587, 0.1220757887, 0.0338423289, 0.0063366601, -0.0186062604, 0.0270785447, -0.0072318669, 0.0245509017, 0.0643612742, -0.0411444083, 0.0364401862, 0.0708676204, 0.0127318306, 0.067871891, 0.1129949987, 0.0437890738, -0.0116552422, -0.0116610937, 0.0239658002, -0.0391316563, -0.0079690963, -0.0312912837, 0.0518634878, -0.0178222228, 0.0491018035, -0.0529868826, 0.1208587736, 0.0479316004, 0.04514651, 0.0474167094, 0.1311565787, -0.0462933108, -0.0273359902, -0.0159030873, -0.0319231935, -0.1527819633, 0.0075829285, -0.0728335604, -0.1516585797, -0.0552336797, 0.0129424678, 0.0969865918, -0.1168332696, -0.1592414975, -0.0772335306, 0.0615995936, 0.0677314699, 0.152126655, 0.025112601, -0.0482124463, -0.0455443785, 0.054765597, -0.000080543, -0.0056930473, 0.0688548684, 0.0241296273, -0.1220757887, 0.0945993736, 0.0469018184, 0.0895908996, 0.044655025, -0.1289097816, 0.0679655075, -0.0508337058, 0.0523315705, -0.0693697557, 0.0863143206, -0.0169211645, 0.0948334187, 0.0293019339, -0.0560294166, -0.0130477864, 0.068901673, 0.0798547938, -0.100450404, 0.0399742052, 0.0391316563, 0.0198934861, 0.0168626551, 0.1411735415, 0.0819611624, 0.0435784347, -0.0515358299, 0.0454039574, -0.0749867409, 0.1030716598, -0.0343572199, 0.0975482911, 0.0388742127, -0.0193785951, 0.0117371567, 0.0069802729, -0.0020156782, -0.0398805887, 0.0391550623, 0.0521443374, 0.0223626178, 0.0012660156, -0.0655314848, -0.0159850009, 0.0156222377, -0.0234509092, -0.0380082615, -0.0083435616, -0.0972674415, -0.0620208681, -0.0192849785, -0.0296764001, 0.0223509166, 0.0609910861, -0.0158094708, 0.0453103408, -0.0479316004, 0.0231466554, -0.0370018817, -0.0613655522, -0.0135158682, 0.1294714808, 0.0000360432, 0.0062898523, -0.0544379391, 0.0100754658 ]
801.0285
Harish Seshadri
Harish Seshadri
An elementary approach to some rigidity theorems
5 Pages
null
null
null
math.DG
null
Using elementary comparison geometry, we prove: Let $(M,g)$ be a simply-connected complete Riemannian manifold of dimension $\ge 3$. Suppose that the sectional curvature $K$ satisfies $ -1-s(r) \le K \le -1$, where $r$ denotes distance to a fixed point in $M$. If $\lim_{r \rt \infty} e^{2r}s(r) =0$, then $(M,g)$ has to be isometric to ${\mathbb H}^n$. The same proof also yields that if $K$ satisfies $-s(r) \le K \le 0$ where $\lim_{r \rt \infty} r^2s(r)=0$, then $(M,g)$ is isometric to $\R^n$, a result due to Greene and Wu. Our second result is a local one: Let $(M,g)$ be any Riemannian manifold. For $a \in \R$, if $K \le a$ on a geodesic ball $B_p(R)$ in $M$ and $K = a$ on $\partial B_p(R)$, then $K= a $ on $B_p(R)$.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 09:25:23 GMT" } ]
2008-01-03T00:00:00
[ [ "Seshadri", "Harish", "" ] ]
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801.0286
Viktor Soshnikov
V. N. Soshnikov
Non-linear equations for electron waves in Maxwellian low-collision ion-electron plasmas
13 pages, no figures, PDF
null
null
null
physics.plasm-ph
null
The before described general principles and methodology of calculating electron wave propagation in homogeneous isotropic half-infinity slab of Maxwellian plasma with indefinite but in principal value sense taken integrals in characteristic equations, and the use of 2D Laplace transform method are applied to an evaluation of collision damping decrements of plane electron longitudinal and transverse waves. Damping decrement tends to infinity when the wave frequency tends to electron Langmuir frequency from above values. We considered recurrent relations for amplitudes of the overtones which form in their sum the all solution of the plasma wave non-linear equations including collision damping and quadratic (non-linear) terms. Collisionless damping at frequencies more the Langmuir one is possible only in non-Maxwellian plasmas.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 09:58:58 GMT" }, { "version": "v2", "created": "Sun, 30 Mar 2008 13:13:39 GMT" } ]
2008-03-30T00:00:00
[ [ "Soshnikov", "V. N.", "" ] ]
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801.0287
Alan Kostelecky
Alan Kostelecky and Neil Russell
Data Tables for Lorentz and CPT Violation
155 pages, 2024 edition
Rev.Mod.Phys. 83: 11 (2011)
10.1103/RevModPhys.83.11
null
hep-ph astro-ph gr-qc hep-ex hep-th
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
This work tabulates measured and derived values of coefficients for Lorentz and CPT violation in the Standard-Model Extension. Summary tables are extracted listing maximal attained sensitivities in the matter, photon, neutrino, and gravity sectors. Tables presenting definitions and properties are also compiled.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 09:41:36 GMT" }, { "version": "v10", "created": "Fri, 13 Jan 2017 16:04:18 GMT" }, { "version": "v11", "created": "Mon, 8 Jan 2018 20:45:38 GMT" }, { "version": "v12", "created": "Thu, 3 Jan 2019 17:03:59 GMT" }, { "version": "v13", "created": "Fri, 3 Jan 2020 19:20:27 GMT" }, { "version": "v14", "created": "Sat, 2 Jan 2021 02:35:44 GMT" }, { "version": "v15", "created": "Sun, 23 Jan 2022 20:31:11 GMT" }, { "version": "v16", "created": "Mon, 9 Jan 2023 14:38:11 GMT" }, { "version": "v17", "created": "Fri, 5 Jan 2024 16:18:54 GMT" }, { "version": "v2", "created": "Thu, 22 Jan 2009 18:29:13 GMT" }, { "version": "v3", "created": "Tue, 5 Jan 2010 02:00:01 GMT" }, { "version": "v4", "created": "Thu, 6 Jan 2011 21:28:27 GMT" }, { "version": "v5", "created": "Fri, 13 Jan 2012 11:38:36 GMT" }, { "version": "v6", "created": "Thu, 24 Jan 2013 01:34:25 GMT" }, { "version": "v7", "created": "Thu, 23 Jan 2014 00:07:28 GMT" }, { "version": "v8", "created": "Mon, 19 Jan 2015 23:41:30 GMT" }, { "version": "v9", "created": "Fri, 26 Feb 2016 20:07:41 GMT" } ]
2024-01-08T00:00:00
[ [ "Kostelecky", "Alan", "" ], [ "Russell", "Neil", "" ] ]
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801.0288
C. M. Hubert Chen
C. M. Hubert Chen, D. E. Harris, Fiona A. Harrison and Peter H. Mao
Constraints on the average magnetic field strength of relic radio sources 0917+75 and 1401-33 from XMM-Newton observations
11 pages, 5 figures. Accepted by MNRAS
MNRAS 383 (3), 1259-1268, 1/2008
10.1111/j.1365-2966.2007.12633.x
null
astro-ph
null
We observed two relic radio sources, 0917+75 and 1401-33, with the XMM-Newton X-ray observatory. We did not detect any X-ray emission, thermal or non-thermal, in excess of the local background level from either target. This imposes new upper limits on the X-ray flux due to inverse Compton scattering of photons from the cosmic microwave background by relativistic electrons in the relic sources, and new lower limits on the magnetic field strength from the relative strength of the radio and X-ray emission. The combination of radio and X-ray observations provides a measure of the magnetic field independent of equipartition or minimum energy assumptions. Due to increasing sensitivity of radio observations, the known population of cluster relics has been growing; however, studies of non-thermal X-ray emission from relics remain scarce. Our study adds to the small sample of relics studied in X-rays. In both relics, our field strength lower limits are slightly larger than estimates of the equipartition magnetic field.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 10:24:52 GMT" } ]
2008-02-14T00:00:00
[ [ "Chen", "C. M. Hubert", "" ], [ "Harris", "D. E.", "" ], [ "Harrison", "Fiona A.", "" ], [ "Mao", "Peter H.", "" ] ]
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801.0289
Marie Ferbus-Zanda
Marie Ferbus-Zanda (LIAFA), Serge Grigorieff (LIAFA)
Is Randomness "Native" to Computer Science?
43 pages
Current Trends in Theoretical Computer Science. Vol2, World Scientific (Ed.) (2004) 141-180
null
null
math.LO cs.CC
null
We survey the Kolmogorov's approach to the notion of randomness through the Kolmogorov complexity theory. The original motivation of Kolmogorov was to give up a quantitative definition of information. In this theory, an object is randomness in the sense that it has a large information content. Afterwards, we present parts of the work of Martin-Lof, Schnorr, Chaitin and Levin which supply a mathematical notion of randomness throughout diverse theories from the the 60' up to recently.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 10:26:55 GMT" } ]
2008-01-03T00:00:00
[ [ "Ferbus-Zanda", "Marie", "", "LIAFA" ], [ "Grigorieff", "Serge", "", "LIAFA" ] ]
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801.029
Riou Nakamura
Riou Nakamura, Masa-aki Hashimoto, Kiyotomo Ichiki
Cosmic microwave background constraints on a decaying cosmological term related to the thermal evolution
null
Phys.Rev.D77:123511,2008
10.1103/PhysRevD.77.123511
null
astro-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We constrain the thermal evolution of the universe with a decaying cosmological term by using the method of the analysis for the Wilkinson Microwave Anisotropy Probe (WMAP) observation data. The cosmological term is assumed to be a function of the scale factor that increases toward the early universe, and the radiation energy density is lower compared to that in the model with the standard cosmological "constant" (LCDM). The decrease in the radiation density affects the thermal history of the universe; e.g. the photon decoupling occurs at higher-z compared to the case of the standard LCDM model. As a consequence, a decaying cosmological term affects the cosmic microwave background anisotropy. Thanks to the Markov-chain Monte Carlo method, we compare the angular power spectrum in the decaying LCDM model with the CMB data, and we get severe constraints on parameters of the model.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 15:06:44 GMT" }, { "version": "v2", "created": "Wed, 11 Jun 2008 14:19:47 GMT" } ]
2008-11-26T00:00:00
[ [ "Nakamura", "Riou", "" ], [ "Hashimoto", "Masa-aki", "" ], [ "Ichiki", "Kiyotomo", "" ] ]
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801.0291
Michael Ivanov A
Michael A. Ivanov
Asymptotic freedom in low-energy quantum gravity
3 pages, no figure, Latex; v2, v3 - correction of numerical errors
null
null
null
hep-th gr-qc quant-ph
null
It is suggested in the model of low-energy quantum gravity by the author, that the background of super-strong interacting gravitons exists. It is shown here that micro-particles at very small distances should be almost free if the gravitational attraction is caused by a pressure of these gravitons.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 10:58:45 GMT" }, { "version": "v2", "created": "Sun, 6 Jan 2008 16:49:02 GMT" }, { "version": "v3", "created": "Fri, 11 Jan 2008 09:06:20 GMT" } ]
2011-11-10T00:00:00
[ [ "Ivanov", "Michael A.", "" ] ]
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801.0292
Bing Dong
Bing Dong, X.L. Lei, N.J.M. Horing
First-order coherent resonant tunneling through an interacting coupled-quantum-dot interferometer: generic quantum rate equations and current noise
14 pages, 12 figures
Phys. Rev. B 77, 085309 (2008)
10.1103/PhysRevB.77.085309
null
cond-mat.mes-hall
null
We carry out a detailed analysis of coherent resonant tunneling through two coupled quantum dots (CQD) in a parallel arrangement in the weak tunneling limit. We establish a set of quantum rate equations (QREs) in terms of the eigenstate-representation by means of a generic quantum Langevin equation approach, which is valid for arbitrary bias-voltage, temperature, and interdot hopping strength. Based on linear-response theory, we further derive the current and frequency-independent shot noise formulae. Our results reveal that a previously used formula for evaluating Schottky-type noise of a "classical" single-electron transistor is a direct result of linear-response theory, and it remains applicable for small quantum devices with internal coupling. Our numerical calculations show some interesting transport features (i) for a series-CQD: the appearance of a NDC due to the bias-voltage-induced shifting of bare levels or a finite interdot Coulomb repulsion, and (ii) for a parallel CQD in strong interdot Coulomb repulsion regime: finite-bias-induced AB oscillations of current, and magnetic-flux-controllable negative differential conductance and a huge Fano factor.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 11:06:46 GMT" } ]
2009-11-13T00:00:00
[ [ "Dong", "Bing", "" ], [ "Lei", "X. L.", "" ], [ "Horing", "N. J. M.", "" ] ]
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801.0293
J. R. Goicoechea
Javier R. Goicoechea
The far-IR view of Sgr B2 and Orion KL
''Far-Infrared and Submillimeter Emission of the Interstellar Medium: Models meet extragalactic and Galactic Observations''. Proceedings of the FIR Workshop 2007. Eds. C. Kramer, R. Simon et al
null
10.1051/eas:0831014
null
astro-ph
null
We summarize the main highlights from ISO observations towards Sgr B2 and Orion KL in the far-IR domain (~43 to 197 um). Both Star-Forming Regions are among the best sources to construct a template for more distant and unresolved regions (e.g., extragalactic). We stress some peculiarities in the interpretation (excitation and radiative transfer) of far-IR spectral lines and dust continuum emission.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 11:30:04 GMT" } ]
2015-05-13T00:00:00
[ [ "Goicoechea", "Javier R.", "" ] ]
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801.0294
Ying-Qiu Gu
Ying-Qiu Gu
Functions and Relations for an Evolving Star with Spherical Symmetry
9 pages, no figure
null
null
null
physics.gen-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
In this paper, we drive and simplify some important equations and relations for an evolving star with spherical symmetry, and then give some simple analysis for their properties and implications. In the light-cone coordinate system, these equations and relations have a normal and neat form which is much accessible than the usual Einstein field equation. So they may be helpful for students to study general relativity and for researchers to do further discussion.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:01:38 GMT" }, { "version": "v2", "created": "Sun, 2 Mar 2008 04:37:48 GMT" }, { "version": "v3", "created": "Fri, 7 Mar 2008 16:25:33 GMT" }, { "version": "v4", "created": "Tue, 27 Jan 2009 13:47:25 GMT" }, { "version": "v5", "created": "Sat, 12 Sep 2009 01:40:40 GMT" }, { "version": "v6", "created": "Fri, 19 May 2017 12:06:41 GMT" } ]
2017-05-22T00:00:00
[ [ "Gu", "Ying-Qiu", "" ] ]
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801.0295
Bijaya Sahoo Dr.
B. K. Sahoo, B. P. Das
Electron correlation effects in the dipole polarizabilities of the ground states of Be, Mg, Ca, Sr, Ba and Yb
3 tables, 1 figure
null
null
null
physics.atom-ph physics.chem-ph
null
We investigate the role of electron correlation effects in the electric dipole polarizabilities of the ground states of the alkaline earth and ytterbium atoms by employing the relativistic coupled-cluster (RCC) theory. These effects are incorporated via the residual Coulomb interaction to all orders in the RCC singles and doubles approximation. The perturbed wavefunctions used in the calculations of the polarizabilities are obtained by directly solving the first order perturbed RCC equations, thereby avoiding the sum-over-states approach. Our results are compared with other calculations and available experimental data.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 12:48:28 GMT" } ]
2008-01-03T00:00:00
[ [ "Sahoo", "B. K.", "" ], [ "Das", "B. P.", "" ] ]
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801.0296
Yang Sun
J. A. Sheikh, G. H. Bhat, Y. Sun, G. B. Vakil, R. Palit
Triaxial projected shell model study of gamma-vibrational bands in even-even Er isotopes
6 pages, 9 figures
Phys.Rev.C77:034313,2008
10.1103/PhysRevC.77.034313
null
nucl-th nucl-ex
null
We expand the triaxial projected shell model basis to include triaxially-deformed multi-quasiparticle states. This allows us to study the yrast and gamma-vibrational bands up to high spins for both gamma-soft and well-deformed nuclei. As the first application, a systematic study of the high-spin states in Er-isotopes is performed. The calculated yrast and gamma-bands are compared with the known experimental data, and it is shown that the agreement between theory and experiment is quite satisfactory. The calculation leads to predictions for bands based on one- and two-gamma phonon where current data are still sparse. It is observed that gamma-bands for neutron-deficient isotopes of 156Er and 158Er are close to the yrast band, and further these bands are predicted to be nearly degenerate for high-spin states.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 13:55:06 GMT" } ]
2008-11-26T00:00:00
[ [ "Sheikh", "J. A.", "" ], [ "Bhat", "G. H.", "" ], [ "Sun", "Y.", "" ], [ "Vakil", "G. B.", "" ], [ "Palit", "R.", "" ] ]
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801.0297
Scott Kominers
Justin G. Chen, Scott D. Kominers, Robert W. Sinnott
Walk versus Wait: The Lazy Mathematician Wins
3 pages
null
null
null
math.HO
null
In this recreational mathematics note, we address a simple, yet instructive question: Justin has to travel a distance of d miles along a bus route. Along this route, there are n bus stops i, each spaced at a distance of d_i from the starting point. At each bus stop, Justin is faced with a choice: to walk or to wait. If he walks on, he can still catch a bus at the next bus stop--but if a bus passes him while he walks, he is almost assured a longer wait. We model Justin's decision constraint and completely solve the model in a special case. The answer is intuitive: the optimal strategy is the laziest.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 20:59:14 GMT" }, { "version": "v2", "created": "Thu, 10 Jan 2008 02:49:50 GMT" }, { "version": "v3", "created": "Sun, 27 Jan 2008 20:51:09 GMT" } ]
2008-01-27T00:00:00
[ [ "Chen", "Justin G.", "" ], [ "Kominers", "Scott D.", "" ], [ "Sinnott", "Robert W.", "" ] ]
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801.0298
Richard Herrmann
Richard Herrmann
Curvature interaction in collective space
updated version, 10 pages, 2 figures
International Journal of Modern Physics E, Vol. 21, (2012) 1250103
10.1142/S0218301312501030
null
nucl-th
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
For the Riemannian space, built from the collective coordinates used within nuclear models, an additional interaction with the metric is investigated, using the collective equivalent to Einstein's curvature scalar. The coupling strength is determined using a fit with the AME2003 ground state masses. An extended finite-range droplet model including curvature is introduced, which generates significant improvements for light nuclei and nuclei in the trans-fermium region.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 14:09:04 GMT" }, { "version": "v2", "created": "Thu, 22 Nov 2012 14:39:59 GMT" } ]
2012-11-26T00:00:00
[ [ "Herrmann", "Richard", "" ] ]
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801.0299
Debanjan Chowdhury
Debanjan Chowdhury and Amit Dutta
The effect of long range interactions on the stability of classical and quantum solids
7 pages REVTEX (including 1 ps figure)
null
null
null
cond-mat.stat-mech
null
We generalise the celebrated Peierls' argument to study the stability of a long-range interacting classical solid. Long-range interaction implies that all the atomic oscillators are coupled to each other via a harmonic potential, though the coupling strength decays as a power-law $1/x^{\alpha}$, where $x$ is the distance between the oscillators. We show that for the range parameter $\alpha <2$, the long-range interaction dominates and the one-dimensional system retains a crystalline order even at a finite temperature whereas for $\alpha \geq2$, the long-range crystalline order vanishes even at an infinitesimally small temperature. We also study the effect of quantum fluctuations on the melting behaviour of a one-dimensional solid at T=0, extending Peierls' arguments to the case of quantum oscillators.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 15:12:55 GMT" } ]
2008-01-03T00:00:00
[ [ "Chowdhury", "Debanjan", "" ], [ "Dutta", "Amit", "" ] ]
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801.03
Maciej Dunajski
Robert L. Bryant, Maciej Dunajski, Michael Eastwood
Metrisability of two-dimensional projective structures
Minor corrections. Final version published in the Journal of Differential Geometry
null
null
DAMTP-2007-127
math.DG math-ph math.AP math.MP nlin.SI
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We carry out the programme of R. Liouville \cite{Liouville} to construct an explicit local obstruction to the existence of a Levi--Civita connection within a given projective structure $[\Gamma]$ on a surface. The obstruction is of order 5 in the components of a connection in a projective class. It can be expressed as a point invariant for a second order ODE whose integral curves are the geodesics of $[\Gamma]$ or as a weighted scalar projective invariant of the projective class. If the obstruction vanishes we find the sufficient conditions for the existence of a metric in the real analytic case. In the generic case they are expressed by the vanishing of two invariants of order 6 in the connection. In degenerate cases the sufficient obstruction is of order at most 8.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 15:24:12 GMT" }, { "version": "v2", "created": "Sun, 14 Feb 2010 22:18:48 GMT" } ]
2010-02-15T00:00:00
[ [ "Bryant", "Robert L.", "" ], [ "Dunajski", "Maciej", "" ], [ "Eastwood", "Michael", "" ] ]
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801.0301
Erhan Iltan
E. O. Iltan
Lepton flavor violating $l_i\to l_j \gamma\gamma$ decays induced by scalar unparticle
10 pages, 5 figures, 1 table
Mod.Phys.Lett.A23:3331-3339,2008
10.1142/S021773230802714X
null
hep-ph
null
We study the radiative lepton flavor violating l_i -> l_j \gamma\gamma decays in the case that the lepton flavor violation is induced by the scalar unparticle mediation. We restrict the scaling dimension d_u and the scalar unparticle-photon-photon coupling by using the experimental upper limit of the branching ratio of the decay \mu -> e \gamma\gamma. Furthermore, we predict the BRs of the other radiative decays by using the restrictions we get. We observe that the measurements of upper limits of BRs of these decays ensure considerable information for testing the possible signals coming from unparticle physics
[ { "version": "v1", "created": "Tue, 1 Jan 2008 15:47:47 GMT" } ]
2009-02-11T00:00:00
[ [ "Iltan", "E. O.", "" ] ]
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801.0302
Maxim Kharitonov
Maxim Yu. Kharitonov and Konstantin B. Efetov
Mesoscopic conductance fluctuations in graphene samples
4+ pages, 2 figures
Phys. Rev. B 78, 033404 (2008)
10.1103/PhysRevB.78.033404
null
cond-mat.mes-hall cond-mat.dis-nn
null
Mesoscopic conductance fluctuations in graphene samples at energies not very close to the Dirac point are studied analytically. We demonstrate that the conductance variance $<[\delta G]^2>$ is very sensitive to the elastic scattering breaking the valley symmetry. In the absence of such scattering (disorder potential smooth at atomic scales, trigonal warping negligible), the variance $<[\delta G]^2 > = 4 < [\delta G]^2 >_\text{metal}$ is four times greater than that in conventional metals, which is due to the two-fold valley degeneracy. In the absence of intervalley scattering, but for strong intravalley scattering and/or strong warping $<[\delta G]^2 > =2 < [\delta G]^2 >_\text{metal}$. Only in the limit of strong intervalley scattering $<[\delta G]^2 > = < [\delta G]^2 >_\text{metal}$. Our theory explains recent numerical results and can be used for comparison with existing experiments.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 15:59:35 GMT" } ]
2009-03-25T00:00:00
[ [ "Kharitonov", "Maxim Yu.", "" ], [ "Efetov", "Konstantin B.", "" ] ]
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801.0303
Anna Stasto
T.C. Rogers, A.M. Stasto, M. I. Strikman
Unitarity Constraints on Semi-hard Jet Production in Impact Parameter Space
12 pages, 7 figures
Phys.Rev.D77:114009,2008
10.1103/PhysRevD.77.114009
null
hep-ph
null
The perturbative QCD formula for minijet production consitutes an important ingredient in models describing the total cross section and multiparticle production in hadron-hadron scattering at high energies. Using arguments based on s-channel unitarity we set bounds on the minimum value of p_T for which the leading twist minijet formula can be used. For large impact parameters where correlations between partons appear to be small we find that the minimum value of p_T should be greater than 2.5 GeV for LHC energies and greater than 3.5 GeV for cosmic ray energies of about 50 TeV. We also argue that for collisions with values of impact parameters typical for heavy particle production the values of minimum p_T are likely to be considerably larger. We also analyze and quantify the potential role of saturation effects in the gluon density. We find that although saturation effects alone are not sufficient to restore unitarity, they are likely to play an important role at LHC energies.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 16:10:37 GMT" } ]
2008-11-26T00:00:00
[ [ "Rogers", "T. C.", "" ], [ "Stasto", "A. M.", "" ], [ "Strikman", "M. I.", "" ] ]
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801.0304
Ajay Patwardhan
Ajay Patwardhan, Kartik Prabhu, M.S.R. Kumar
Cosmological Perturbation Theory to second order for curvature, density, and gravity waves on FRW background; and the WMAP results of inhomogeneity and clustering in the early universe
45 pages, 2 figures, NIUS /HBCSE project
null
null
null
hep-th gr-qc
null
The second order perturbation calculations for gravity wave and Einstein equation for space time and matter are presented for the FRW metric cosmological model. While exact equations are found, suitable approximations are made to obtain definite results. In the gravity wave case the small wavelength case allows nearly locally flat background for obtaining a fit to the WMAP data. In the density and curvature case the FRW background is retained for the length scale of WMAP. Clustering and inhomogeneity are understood. The gravity wave ripples from Big Bang couple nonlinearly and redistribute the modes to higher values of 'l' giving consistency with the WMAP results. The order by order consistency of Einstein equations relate the second order perturbations in the curvature and density and the wrinkles in spacetime caused by the gravity wave modes reorganize these distributions. The radiation data of WMAP gives the picture of a FRW spacetime deformed and wrinkled consistent with matter distribution to one hundred thousandths parts variation.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 16:15:11 GMT" } ]
2008-01-03T00:00:00
[ [ "Patwardhan", "Ajay", "" ], [ "Prabhu", "Kartik", "" ], [ "Kumar", "M. S. R.", "" ] ]
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801.0305
Cristine Nunes Ferreira crisnfer
C. A. Ballon Bayona, Cristine N. Ferreira
Static strings in global AdS space and quark anti-quark potential
8 pages, 8 figures. V3 with a new discussion of the relation between the Wilson loop considered in the article and the Polyakov loops. New figures and a correction of figure 1. Accepted for publication in PRD
Phys.Rev.D78:026004,2008
10.1103/PhysRevD.78.026004
null
hep-th
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We investigate the finite temperature quark anti-quark problem in a compact space $S^{n-1}\times S^1$ by considering static strings in global $AdS_{n+1}$ space with $n\ge 3$. For high temperatures we work in the black hole metric where two possible solutions show up : the big black hole and the small black hole. Using the AdS/CFT correspondence, we calculate the quark anti-quark potential (free energy) as a function of the distance. We show that this potential can be intrepeted as confining for the $AdS$ space and deconfining for the big black hole. We find for the small black hole a confining limit for the potential but this solution is instable following the Hawking-Page criteria. Our results for the free energy reinforce the Witten interpretation of the confinement/deconfinement transition as the dual of the well-known Hawking-Page transition.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 17:36:03 GMT" }, { "version": "v2", "created": "Fri, 11 Jan 2008 16:38:42 GMT" }, { "version": "v3", "created": "Sat, 7 Jun 2008 16:10:24 GMT" } ]
2008-11-07T00:00:00
[ [ "Bayona", "C. A. Ballon", "" ], [ "Ferreira", "Cristine N.", "" ] ]
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801.0306
Frederick M. Goodman
Frederick M. Goodman
Cellularity of Cyclotomic Birman--Wenzl--Murakami algebras
Minor corrections, added figure
null
null
null
math.QA math.RA math.RT
null
We show that the cyclotomic Birman-Wenzl-Murakami algebras are cellular by producing a cellular basis of affine tangle diagrams.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 17:45:51 GMT" }, { "version": "v2", "created": "Sat, 2 Feb 2008 00:20:27 GMT" }, { "version": "v3", "created": "Wed, 28 May 2008 23:15:05 GMT" } ]
2008-05-29T00:00:00
[ [ "Goodman", "Frederick M.", "" ] ]
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801.0307
Franz E Schunck
Franz E. Schunck and Eckehard W. Mielke
TOPICAL REVIEW: General relativistic boson stars
45 pages, 3 figures
Class.Quant.Grav.20:R301-R356,2003
10.1088/0264-9381/20/20/201
null
astro-ph
null
There is accumulating evidence that (fundamental) scalar fields may exist in Nature. The gravitational collapse of such a boson cloud would lead to a boson star (BS) as a new type of a compact object. Similarly as for white dwarfs and neutron stars, there exists a limiting mass, below which a BS is stable against complete gravitational collapse to a black hole. According to the form of the self-interaction of the basic constituents and the spacetime symmetry, we can distinguish mini-, axidilaton, soliton, charged, oscillating and rotating BSs. Their compactness prevents a Newtonian approximation, however, modifications of general relativity, as in the case of Jordan-Brans-Dicke theory as a low energy limit of strings, would provide them with gravitational memory. In general, a BS is a compact, completely regular configuration with structured layers due to the anisotropy of scalar matter, an exponentially decreasing 'halo', a critical mass inversely proportional to constituent mass, an effective radius, and a large particle number. Due to the Heisenberg principle, there exists a completely stable branch, and as a coherent state, it allows for rotating solutions with quantised angular momentum. In this review, we concentrate on the fascinating possibilities of detecting the various subtypes of (excited) BSs: Possible signals include gravitational redshift and (micro-)lensing, emission of gravitational waves, or, in the case of a giant BS, its dark matter contribution to the rotation curves of galactic halos.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 17:45:52 GMT" } ]
2019-04-03T00:00:00
[ [ "Schunck", "Franz E.", "" ], [ "Mielke", "Eckehard W.", "" ] ]
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801.0308
Haichau Chang
Hai-Chau Chang and Wu-Yi Hsiang
The epic journey from Kepler's laws to Newton's law of universal gravitation revisited
22 pages, 9 figures
null
null
null
physics.hist-ph physics.gen-ph
null
In this article, we review the main results of Volume I of Newton's Principia which relates Kepler's law of planets and universal gravitation. In order to clarify the reasoning of Newton, elementary and simple proofs are given to inspire earnest young students. All proofs are based on either the symmetry of spheres or taking great advantage of Kepler's law of area which also reflects the symmetry of centripedal forces.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 17:58:49 GMT" } ]
2008-01-03T00:00:00
[ [ "Chang", "Hai-Chau", "" ], [ "Hsiang", "Wu-Yi", "" ] ]
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801.0309
Ian Hutchinson
I. H. Hutchinson
Ion collection by oblique surfaces of an object in a transversely-flowing strongly-magnetized plasma
Four pages, 2 figures. Submitted to Phys. Rev. Letters
null
10.1103/PhysRevLett.101.035004
null
physics.plasm-ph physics.flu-dyn
null
The equations governing a collisionless obliquely-flowing plasma around an ion-absorbing object in a strong magnetic field are shown to have an exact analytic solution even for arbitrary (two-dimensional) object-shape, when temperature is uniform, and diffusive transport can be ignored. The solution has an extremely simple geometric embodiment. It shows that the ion collection flux density to a convex body's surface depends only upon the orientation of the surface, and provides the theoretical justification and calibration of oblique `Mach-probes'. The exponential form of this exact solution helps explain the approximate fit of this function to previous numerical solutions.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 18:47:38 GMT" } ]
2009-11-13T00:00:00
[ [ "Hutchinson", "I. H.", "" ] ]
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801.031
Kwan-yuet Ho
Kwan-yuet Ho
Entanglement between a Two-level System and a Quantum Harmonic Oscillator
8 pages, 8 figures
null
null
null
quant-ph
null
The entanglement between a Pauli-like two-level system and a quantum harmonic oscillator enhanced by an interaction between them and a $\delta$-pulse sequence is studied, with the decoherence due to their coupling with a Markovian bath. Without the Markovian bath, the entanglement is enhanced to maximum possible values. With the Markovian bath, the entanglement is enhanced up to some time and then dissipated, with the system in thermal equilibrium with the Markovian bath after a very long time. The time for achieving the maximum entanglement shows discontinuous jumps over the parameters of decoherence.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 19:46:22 GMT" }, { "version": "v2", "created": "Wed, 16 Apr 2008 15:28:54 GMT" } ]
2008-04-16T00:00:00
[ [ "Ho", "Kwan-yuet", "" ] ]
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801.0311
Tatyana Sharpee
Tatyana O. Sharpee
Comparison of objective functions for estimating linear-nonlinear models
to appear in Advances in Neural Information Processing Systems 21 (NIPS, 2007)
null
null
null
q-bio.NC q-bio.QM
null
This paper compares a family of methods for characterizing neural feature selectivity with natural stimuli in the framework of the linear-nonlinear model. In this model, the neural firing rate is a nonlinear function of a small number of relevant stimulus components. The relevant stimulus dimensions can be found by maximizing one of the family of objective functions, Renyi divergences of different orders. We show that maximizing one of them, Renyi divergence of order 2, is equivalent to least-square fitting of the linear-nonlinear model to neural data. Next, we derive reconstruction errors in relevant dimensions found by maximizing Renyi divergences of arbitrary order in the asymptotic limit of large spike numbers. We find that the smallest rrors are obtained with Renyi divergence of order 1, also known as Kullback-Leibler divergence. This corresponds to finding relevant dimensions by maximizing mutual information. We numerically test how these optimization schemes perform in the regime of low signal-to-noise ratio (small number of spikes and increasing neural noise) for model visual neurons. We find that optimization schemes based on either least square fitting or information maximization perform well even when number of spikes is small. Information maximization provides slightly, but significantly, better reconstructions than least square fitting. This makes the problem of finding relevant dimensions, together with the problem of lossy compression, one of examples where information-theoretic measures are no more data limited than those derived from least squares.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 07:13:48 GMT" } ]
2008-01-03T00:00:00
[ [ "Sharpee", "Tatyana O.", "" ] ]
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801.0312
Nicolas Cowan
Nicolas B. Cowan and Zeljko Ivezic
The Environment of Galaxies at Low Redshift
15 pages, 5 figures, ApJL accepted, fixed author listings
null
10.1086/528986
null
astro-ph
null
We compare environmental effects in two analogous samples of galaxies, one from the Sloan Digital Sky Survey (SDSS) and the other from a semi-analytic model (SAM) based on the Millennium Simulation (MS), to test to what extent current SAMs of galaxy formation are reproducing environmental effects. We estimate the large-scale environment of each galaxy using a Bayesian density estimator based on distances to all ten nearest neighbors and compare broad-band photometric properties of the two samples as a function of environment. The feedbacks implemented in the semi-analytic model produce a qualitatively correct galaxy population with similar environmental dependence as that seen in SDSS galaxies. In detail, however, the colors of MS galaxies exhibit an exaggerated dependence on environment: the field contains too many blue galaxies while clusters contain too many red galaxies, compared to the SDSS sample. We also find that the MS contains a population of highly clustered, relatively faint red galaxies with velocity dispersions comparable to their Hubble flow. Such high-density galaxies, if they exist, would be overlooked in any low-redshift survey since their membership to a cluster cannot be determined due to the "Fingers of God" effect.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 19:55:48 GMT" }, { "version": "v2", "created": "Tue, 15 Jan 2008 07:06:42 GMT" } ]
2009-11-13T00:00:00
[ [ "Cowan", "Nicolas B.", "" ], [ "Ivezic", "Zeljko", "" ] ]
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801.0313
Hung Pham
Hung Le Pham
The kernel and continuity ideals of homomorphisms from C_0(\Omega)
22 pages
null
null
null
math.FA
null
We give a description of the continuity ideals and the kernels of homomorphisms from the algebras of continuous functions on locally compact spaces into Banach algebras.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 20:19:42 GMT" } ]
2008-01-03T00:00:00
[ [ "Pham", "Hung Le", "" ] ]
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801.0314
Andy Shearer
Andy Shearer
High-time Resolution Astrophysics and Pulsars
Review; 21 pages, 5 figures, 86 references. Book chapter to appear in: D.Phelan, O.Ryan & A.Shearer, eds.: High Time Resolution Astrophysics (Astrophysics and Space Science Library, Springer, 2007). The original publication will be available at http://www.springerlink.com
High Time Resolution Astrophysics, Astrophysics and Space Science Library, Vol. 351. Edited by D. Phelan, O. Ryan, and A. Shearer. Berlin: Springer, 2008
10.1007/978-1-4020-6518-7_1
null
astro-ph
null
The discovery of pulsars in 1968 heralded an era where the temporal characteristics of detectors had to be reassessed. Up to this point detector integration times would normally be measured in minutes rather seconds and definitely not on sub-second time scales. At the start of the 21st century pulsar observations are still pushing the limits of detector telescope capabilities. Flux variations on times scales less than 1 nsec have been observed during giant radio pulses. Pulsar studies over the next 10 to 20 years will require instruments with time resolutions down to microseconds and below, high-quantum quantum efficiency, reasonable energy resolution and sensitive to circular and linear polarisation of stochastic signals. This chapter is review of temporally resolved optical observations of pulsars. It concludes with estimates of the observability of pulsars with both existing telescopes and into the ELT era.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 21:02:46 GMT" } ]
2015-05-13T00:00:00
[ [ "Shearer", "Andy", "" ] ]
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801.0315
Hung Pham
Hung Le Pham
Uncountable families of prime z-ideals in C_0(R)
12 pages
null
10.1112/blms/bdp009
null
math.RA
null
Denote by $\continuum=2^{\aleph_0}$ the cardinal of continuum. We construct an intriguing family $(P_\alpha: \alpha\in\continuum)$ of prime $z$-ideals in $\C_0(\reals)$ with the following properties: If $f\in P_{i_0}$ for some $i_0\in\continuum$, then $f\in P_i$ for all but finitely many $i\in \continuum$; $\bigcap_{i\neq i_0} P_i \nsubset P_{i_0}$ for each $\i_0\in \continuum$. We also construct a well-ordered increasing chain, as well as a well-ordered decreasing chain, of order type $\kappa$ of prime $z$-ideals in $\C_0(\reals)$ for any ordinal $\kappa$ of cardinality $\continuum$.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 21:05:42 GMT" } ]
2014-02-26T00:00:00
[ [ "Pham", "Hung Le", "" ] ]
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801.0316
Ersen Mete
E. Mete, D. Uner, M. Cakmak, O. Gulseren, and S. Ellialtioglu
Effect of molecular and electronic structure on the light harvesting properties of dye sensitizers
Single pdf file, 14 pages with 7 figures and 4 tables
J. Phys. Chem. C 2007, 111, 7539-7547
10.1021/jp0659812
null
cond-mat.mtrl-sci
null
The systematic trends in structural and electronic properties of perylene diimide (PDI) derived dye molecules have been investigated by DFT calculations based on projector augmented wave (PAW) method including gradient corrected exchange-correlation effects. TDDFT calculations have been performed to study the visible absorbance activity of these complexes. The effect of different ligands and halogen atoms attached to PDI were studied to characterize the light harvesting properties. The atomic size and electronegativity of the halogen were observed to alter the relaxed molecular geometries which in turn influenced the electronic behavior of the dye molecules. Ground state molecular structure of isolated dye molecules studied in this work depends on both the halogen atom and the carboxylic acid groups. DFT calculations revealed that the carboxylic acid ligands did not play an important role in changing the HOMO-LUMO gap of the sensitizer. However, they serve as anchor between the PDI and substrate titania surface of the solar cell or photocatalyst. A commercially available dye-sensitizer, ruthenium bipyridine (RuBpy), was also studied for electronic and structural properties in order to make a comparison with PDI derivatives for light harvesting properties. Results of this work suggest that fluorinated, chlorinated, brominated, and iyodinated PDI compounds can be useful as sensitizers in solar cells and in artificial photosynthesis.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 21:47:45 GMT" } ]
2008-01-15T00:00:00
[ [ "Mete", "E.", "" ], [ "Uner", "D.", "" ], [ "Cakmak", "M.", "" ], [ "Gulseren", "O.", "" ], [ "Ellialtioglu", "S.", "" ] ]
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801.0317
Serge Preston
V. Ciancio, M. Dolfin, M. Francaviglia, S. Preston
Uniform materials and the multiplicative decomposition of the deformation gradient in finite elasto-plasticity
null
null
10.1515/JNETDY.2008.009
null
cond-mat.mtrl-sci cond-mat.other
null
In this work we analyze the relation between the multiplicative decomposition $\mathbf F=\mathbf F^{e}\mathbf F^{p}$ of the deformation gradient as a product of the elastic and plastic factors and the theory of uniform materials. We prove that postulating such a decomposition is equivalent to having a uniform material model with two configurations - total $\phi$ and the inelastic $\phi_{1}$. We introduce strain tensors characterizing different types of evolutions of the material and discuss the form of the internal energy and that of the dissipative potential. The evolution equations are obtained for the configurations $(\phi,\phi_{1})$ and the material metric $\mathbf g$. Finally the dissipative inequality for the materials of this type is presented.It is shown that the conditions of positivity of the internal dissipation terms related to the processes of plastic and metric evolution provide the anisotropic yield criteria.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 21:48:41 GMT" } ]
2015-05-13T00:00:00
[ [ "Ciancio", "V.", "" ], [ "Dolfin", "M.", "" ], [ "Francaviglia", "M.", "" ], [ "Preston", "S.", "" ] ]
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801.0318
M. Spiropulu
Maria Spiropulu
To appear in the proceedings of 15th International Conference on Supersymmetry and the Unification of Fundamental Interactions (SUSY07), Karlsruhe, Germany, 26 Jul - 1 Aug 2007
null
null
null
hep-ex
null
I discuss the program of work towards discoveries at the LHC, and I include seeds for orientation and navigation in the parameter space given the foreseen multitude of excesses at startup.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 22:05:24 GMT" } ]
2008-01-03T00:00:00
[ [ "Spiropulu", "Maria", "" ] ]
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801.0319
Christian Corda
Christian Corda
A non-geodesic motion in the R^-1 theory of gravity tuned with observations
Accepted for Modern Physics Letters A
Mod.Phys.Lett.A23:109-114,2008
10.1142/S0217732308026248
null
astro-ph
null
In the general picture of high order theories of gravity, recently, the R^-1 theory has been analyzed in two different frameworks. In this letter a third context is added, considering an explicit coupling between the R^-1 function of the Ricci scalar and the matter Lagrangian. The result is a non-geodesic motion of test particles which, in principle, could be connected with Dark Matter and Pioneer anomaly problems.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 22:43:24 GMT" }, { "version": "v2", "created": "Tue, 8 Jan 2008 11:26:26 GMT" }, { "version": "v3", "created": "Fri, 11 Jan 2008 08:05:18 GMT" } ]
2008-11-26T00:00:00
[ [ "Corda", "Christian", "" ] ]
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801.032
Moninder Modgil
Moninder Singh Modgil
Climate Control Using Nuclear Energy
17 pages, 6 figures
null
null
null
physics.gen-ph physics.ao-ph physics.geo-ph
null
We examine implications of anthropogenic low pressure regions, - created by injecting heat from nuclear reactors, into atmosphere. We suggest the possibility that such artificially generated low pressure regions, near hurricanes could disrupt their growth, path, and intensity. This method can also create controlled tropical stroms, which lead to substantial rainfall in arid areas, such as - (1)Sahara desert, (2) Australian interior desert, and (3) Indian Thar desert. A simple vortex suction model is developed to study, effect on atmospheric dynamics, by such a nuclear heat injection system.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 22:45:11 GMT" } ]
2008-01-03T00:00:00
[ [ "Modgil", "Moninder Singh", "" ] ]
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801.0321
Darrin Casebeer
Darrin Casebeer, E. Baron, Karen Leighly, Darko Jevremovic, David Branch
A Self-Consistent NLTE-Spectra Synthesis Model of FeLoBAL QSOs
Accepted for publication in ApJ/removed misleading remarks about CLOUDY in section 2
null
10.1086/528671
null
astro-ph
null
We present detailed radiative transfer spectral synthesis models for the Iron Low Ionization Broad Absorption Line (FeLoBAL) active galactic nuclei (AGN) FIRST J121442.3+280329 and ISO J005645.1-273816. Detailed NLTE spectral synthesis with a spherically symmetric outflow reproduces the observed spectra very well across a large wavelength range. While exact spherical symmetry is probably not required, our model fits are of high quality and thus very large covering fractions are strongly implied by our results. We constrain the kinetic energy and mass in the ejecta and discuss their implications on the accretion rate. Our results support the idea that FeLoBALs may be an evolutionary stage in the development of more ``ordinary'' QSOs.
[ { "version": "v1", "created": "Tue, 1 Jan 2008 23:17:38 GMT" }, { "version": "v2", "created": "Fri, 18 Jan 2008 18:34:15 GMT" } ]
2009-11-13T00:00:00
[ [ "Casebeer", "Darrin", "" ], [ "Baron", "E.", "" ], [ "Leighly", "Karen", "" ], [ "Jevremovic", "Darko", "" ], [ "Branch", "David", "" ] ]
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801.0322
Pierre Vanhove
Michael B. Green (Cambridge U., DAMTP), Jorge G. Russo (ICREA, Barcelona & Barcelona U., ECM), Pierre Vanhove (Saclay, SPhT)
Low energy expansion of the four-particle genus-one amplitude in type II superstring theory
JHEP style. 6 eps figures. 50 pages
JHEP 0802:020,2008
10.1088/1126-6708/2008/02/020
DAMTP-2007-96; SPhT-T-07-126; UB-ECM-PF 07/29
hep-th
null
A diagrammatic expansion of coefficients in the low-momentum expansion of the genus-one four-particle amplitude in type II superstring theory is developed. This is applied to determine coefficients up to order s^6R^4 (where s is a Mandelstam invariant and R^4 the linearized super-curvature), and partial results are obtained beyond that order. This involves integrating powers of the scalar propagator on a toroidal world-sheet, as well as integrating over the modulus of the torus. At any given order in s the coefficients of these terms are given by rational numbers multiplying multiple zeta values (or Euler--Zagier sums) that, up to the order studied here, reduce to products of Riemann zeta values. We are careful to disentangle the analytic pieces from logarithmic threshold terms, which involves a discussion of the conditions imposed by unitarity. We further consider the compactification of the amplitude on a circle of radius r, which results in a plethora of terms that are power-behaved in r. These coefficients provide boundary `data' that must be matched by any non-perturbative expression for the low-energy expansion of the four-graviton amplitude. The paper includes an appendix by Don Zagier.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 19:33:16 GMT" } ]
2009-12-15T00:00:00
[ [ "Green", "Michael B.", "", "Cambridge U., DAMTP" ], [ "Russo", "Jorge G.", "", "ICREA,\n Barcelona & Barcelona U., ECM" ], [ "Vanhove", "Pierre", "", "Saclay, SPhT" ] ]
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801.0323
Jose Ademir Sales Lima
J. A. S. Lima, S. H. Pereira
Chemical Potential and the Nature of the Dark Energy: The case of phantom
7 pages, 5 figures
Phys.Rev.D78:083504,2008
10.1103/PhysRevD.78.083504
null
astro-ph
null
The influence of a possible non zero chemical potential $\mu$ on the nature of dark energy is investigated by assuming that the dark energy is a relativistic perfect simple fluid obeying the equation of state (EoS), $p=\omega \rho$ ($\omega <0, constant$). The entropy condition, $S \geq 0$, implies that the possible values of $\omega$ are heavily dependent on the magnitude, as well as on the sign of the chemical potential. For $\mu >0$, the $\omega$-parameter must be greater than -1 (vacuum is forbidden) while for $\mu < 0$ not only the vacuum but even a phantomlike behavior ($\omega <-1$) is allowed. In any case, the ratio between the chemical potential and temperature remains constant, that is, $\mu/T=\mu_0/T_0$. Assuming that the dark energy constituents have either a bosonic or fermionic nature, the general form of the spectrum is also proposed. For bosons $\mu$ is always negative and the extended Wien's law allows only a dark component with $\omega < -1/2$ which includes vacuum and the phantomlike cases. The same happens in the fermionic branch for $\mu <0$. However, fermionic particles with $\mu >0$ are permmited only if $-1 < \omega < -1/2$. The thermodynamics and statistical arguments constrain the EoS parameter to be $\omega < -1/2$, a result surprisingly close to the maximal value required to accelerate a FRW type universe dominated by matter and dark energy ($\omega \lesssim -10/21$).
[ { "version": "v1", "created": "Wed, 2 Jan 2008 00:29:11 GMT" } ]
2008-11-26T00:00:00
[ [ "Lima", "J. A. S.", "" ], [ "Pereira", "S. H.", "" ] ]
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801.0324
Efren Ruiz
Soren Eilers, Gunnar Restorff, Efren Ruiz
Nonsplitting in Kirchberg's ideal-related KK-theory
14 pages, minor typos fixed, 5 figures added
Canadian Mathematical Bulletin 54 (2011), 68-81
10.4153/CMB-2010-083-7
CPH-SYM-00
math.OA
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
A universal coefficient theorem in the setting of Kirchberg's ideal-related KK-theory was obtained in the fundamental case of a C*-algebra with one specified ideal by Bonkat and proved there to split, unnaturally, under certain conditions. Employing certain K-theoretical information derivable from the given operator algebras in a way introduced here, we shall demonstrate that Bonkat's UCT does not split in general. Related methods lead to information on the complexity of the K-theory which must be used to classify *-isomorphisms for purely infinite C*-algebras with one non-trivial ideal.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 00:56:27 GMT" }, { "version": "v2", "created": "Thu, 7 Feb 2008 15:13:07 GMT" }, { "version": "v3", "created": "Fri, 24 Sep 2010 08:01:37 GMT" } ]
2013-09-05T00:00:00
[ [ "Eilers", "Soren", "" ], [ "Restorff", "Gunnar", "" ], [ "Ruiz", "Efren", "" ] ]
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801.0325
Sadataka Furui
Sadataka Furui
Propagator of the lattice domain wall fermion and the staggered fermion
15 pages 3 figures, title changed, added references and revised. version to be bublished in Few-Body Systems
Few Body Syst.45:51-63,2009; Erratum-ibid.46:73-74,2009
10.1007/s00601-009-0008-9 10.1007/s00601-009-0053-4
null
hep-lat
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
The propagator of the domain wall fermion is calculated from the gauge configurations of the RBC-UKQCD collaborations with 2+1 dynamical flavors of $16^3\times 32\times 16$ lattice. The ambiguity of the phase is adjusted such that the overlap of the solution of the conjugate gradient method and the plane wave at the source becomes real. The mass function becomes close to those of Kogut-Susskind fermion, but no anomalous behavior for $u/d$-quark mass and s-quark mass ratio close to 0.75 appears.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 01:01:35 GMT" }, { "version": "v2", "created": "Thu, 13 Mar 2008 11:44:39 GMT" }, { "version": "v3", "created": "Tue, 6 May 2008 09:35:57 GMT" }, { "version": "v4", "created": "Fri, 29 Aug 2008 01:47:34 GMT" }, { "version": "v5", "created": "Tue, 13 Jan 2009 00:15:00 GMT" } ]
2009-05-20T00:00:00
[ [ "Furui", "Sadataka", "" ] ]
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801.0326
Yi-Fang Chang
Yi-Fang Chang
Loop Quantum Theory Applied to Biology and Nonlinear Whole Biology
10 pages
null
null
null
physics.gen-ph
null
The loop quantum theory, which constitutes a very small discontinuous space, as new method is applied to biology. The model of protein folding and lungs is proposed. In the model, some known results are used, and four approximate conclusions are obtained: their structures are quantized, their space regions are finite, various singularities correspond to folding and crossed points, and different types of catastrophe exist. Further, based on the inseparability and correlativity of the biological systems, the nonlinear whole biology is proposed, and four basic hypotheses are formed. It may unify reductionism and holism, structuralism and functionalism. Finally, the medical meaning of the theory is discussed briefly.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 01:06:03 GMT" } ]
2008-01-03T00:00:00
[ [ "Chang", "Yi-Fang", "" ] ]
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801.0327
Kevin Bleakley
G\'erard Biau, Kevin Bleakley, L\'aszl\'o Gy\"orfi and Gy\"orgy Ottucs\'ak
Nonparametric sequential prediction of time series
article + 2 figures
null
null
null
stat.ME math.PR
null
Time series prediction covers a vast field of every-day statistical applications in medical, environmental and economic domains. In this paper we develop nonparametric prediction strategies based on the combination of a set of 'experts' and show the universal consistency of these strategies under a minimum of conditions. We perform an in-depth analysis of real-world data sets and show that these nonparametric strategies are more flexible, faster and generally outperform ARMA methods in terms of normalized cumulative prediction error.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 02:00:15 GMT" } ]
2008-01-03T00:00:00
[ [ "Biau", "Gérard", "" ], [ "Bleakley", "Kevin", "" ], [ "Györfi", "László", "" ], [ "Ottucsák", "György", "" ] ]
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801.0328
Xiaoying Li
Xiaoying Li, Lei Yang, Liang Cui, Zhe Yu Ou and Daoyin Yu
Fiber based source of photon pairs at telecom band with high temporal coherence and brightness for quantum information processing
4 pages, 4 figures, submitted
null
10.1364/OL.33.000593
null
quant-ph
null
We experimentally demonstrate a bright pulsed source of correlated photon pairs at 1550 nm telecom band by pumping 300 m dispersion shifted fiber with a 4 ps pulse train. We investigate the coherence property of the source by measuring the second order intensity correlation function $g^{(2)}$ of individual signal (idler) photons. A preliminary Hong-Ou-Mandel type two-photon interference experiment with two such sources confirms the high temporal and spatial coherence of the source. The source is suitable for multi-photon quantum interference of independent sources, required in quantum information processing.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 02:21:44 GMT" } ]
2009-11-13T00:00:00
[ [ "Li", "Xiaoying", "" ], [ "Yang", "Lei", "" ], [ "Cui", "Liang", "" ], [ "Ou", "Zhe Yu", "" ], [ "Yu", "Daoyin", "" ] ]
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801.0329
Taekyun Kim
Taekyun Kim
Euler Numbers and polynomials associated with zeta functions
12 pages
null
10.1155/2008/581582
null
math.NT
null
In this paper we give some interesting identities between Euler numbers and zeta functions. Finally we will give the new values of Euler zeta function at positive even integers.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 02:38:01 GMT" } ]
2015-05-13T00:00:00
[ [ "Kim", "Taekyun", "" ] ]
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801.033
George Lowther
George Lowther
Properties of Expectations of Functions of Martingale Diffusions
24 pages
null
null
null
math.PR
null
Given a real valued and time-inhomogeneous martingale diffusion X, we investigate the properties of functions defined by the conditional expectation f(t,X_t)=E[g(X_T)|F_t]. We show that whenever g is monotonic or Lipschitz continuous then f(t,x) will also be monotonic or Lipschitz continuous in x. If g is convex then f(t,x) will be convex in x and decreasing in t. We also define the marginal support of a process and show that it almost surely contains the paths of the process. Although f need not be jointly continuous, we show that it will be continuous on the marginal support of X. We prove these results for a generalization of diffusion processes that we call `almost-continuous diffusions', and includes all continuous and strong Markov processes.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 02:39:17 GMT" } ]
2008-01-03T00:00:00
[ [ "Lowther", "George", "" ] ]
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801.0331
Freddy Zen Permana
Arianto, Freddy P. Zen, Triyanta, Bobby E. Gunara (ITB, Udayana University and Indonesia Center for Theoretical and Mathematical Physics (ICTMP), INDONESIA)
Attractor Solutions in Lorentz Violating Scalar-Vector-Tensor Theory
one additional figure and references added, accepted in Phys. Rev. D
Phys.Rev.D77:123517,2008
10.1103/PhysRevD.77.123517
null
hep-th
null
We investigate properties of attractors for scalar field in the Lorentz violating scalar-vector-tensor theory of gravity. In this framework, both the effective coupling and potential functions determine the stabilities of the fixed points. In the model, we consider the constants of slope of the effective coupling and potential functions which lead to the quadratic effective coupling vector with the (inverse) power-law potential. For the case of purely scalar field, there are only two stable attractor solutions in the inflationary scenario. In the presence of a barotropic fluid, the fluid dominated solution is absent. We find two scaling solutions: the kinetic scaling solution and the scalar field scaling solutions. We show the stable attractors in regions of ($\gamma$, $\xi$) parameter space and in phase plane plot for different qualitative evolutions. From the standard nucleosynthesis, we derive the constraints for the value of the coupling parameter.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 03:39:08 GMT" }, { "version": "v2", "created": "Thu, 13 Mar 2008 07:09:53 GMT" } ]
2008-11-26T00:00:00
[ [ "Arianto", "", "", "ITB, Udayana\n University and Indonesia Center for Theoretical and Mathematical Physics" ], [ "Zen", "Freddy P.", "", "ITB, Udayana\n University and Indonesia Center for Theoretical and Mathematical Physics" ], [ "Triyanta", "", "", "ITB, Udayana\n University and Indonesia Center for Theoretical and Mathematical Physics" ], [ "Gunara", "Bobby E.", "", "ITB, Udayana\n University and Indonesia Center for Theoretical and Mathematical Physics" ] ]
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801.0332
Daniel Davis
Daniel G. Davis
Explicit fibrant replacement for discrete G-spectra
13 pages
null
null
null
math.AT
null
If C is the model category of simplicial presheaves on a site with enough points, with fibrations equal to the global fibrations, then it is well-known that the fibrant objects are, in general, mysterious. Thus, it is not surprising that, when G is a profinite group, the fibrant objects in the model category of discrete G-spectra are also difficult to get a handle on. However, with simplicial presheaves, it is possible to construct an explicit fibrant model for an object in C, under certain finiteness conditions. Similarly, in this paper, we show that if G has finite virtual cohomological dimension and X is a discrete G-spectrum, then there is an explicit fibrant model for X. Also, we give several applications of this concrete model related to closed subgroups of G.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 03:57:15 GMT" } ]
2008-01-03T00:00:00
[ [ "Davis", "Daniel G.", "" ] ]
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801.0333
Jinn-Ouk Gong
Jinn-Ouk Gong, Seong Chan Park
Minimal gauge inflation
(v1) 12 pages, 3 figures, 1 table; (v2) 2 figures, analysis with respect to the WMAP5 data set included, miscellaneous changes including the title
null
null
SNUTP 07-013
hep-ph astro-ph gr-qc hep-th
null
We consider a gauge inflation model in the simplest orbifold M4 x S1/Z2 with the minimal non-Abelian SU(2) hidden sector gauge symmetry. The inflaton potential is fully radiatively generated solely by gauge self-interactions. Following the virtue of gauge inflation idea, the inflaton, a part of the five dimensional gauge boson, is automatically protected by the gauge symmetry and its potential is stable against quantum corrections. We show that the model perfectly fits the recent cosmological observations, including the recent WMAP 5-year data, in a wide range of the model parameters. In the perturbative regime of gauge interactions (g_{4D} <= 1/(2pi R M_P)) with the moderately compactified radius (10 <= R M_P <= 100) the anticipated magnitude of the curvature perturbation power spectrum and the value of the corresponding spectral index are in perfect agreement with the recent observations. The model also predicts a large fraction of the gravitational waves, negligible non-Gaussianity, and high enough reheating temperature.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 04:08:26 GMT" }, { "version": "v2", "created": "Sat, 12 Apr 2008 15:38:54 GMT" } ]
2008-04-12T00:00:00
[ [ "Gong", "Jinn-Ouk", "" ], [ "Park", "Seong Chan", "" ] ]
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801.0334
N. D. Ramesh Bhat
N. D. Ramesh Bhat, Steven J. Tingay, and Haydon S. Knight
Bright Giant Pulses from the Crab Nebula Pulsar: Statistical Properties, Pulse Broadening and Scattering due to the Nebula
8 pages, 8 figures, Accepted for publication in ApJ
null
10.1086/528735
null
astro-ph
null
We report observations of Crab giant pulses made with the Australia Telescope Compact Array and a baseband recorder system, made simultaneously at two frequencies, 1300 and 1470 MHz. These observations were sensitive to pulses with amplitudes \ga 3 kJy and widths \ga 0.5 $\mu$s. Our analysis led to the detection of more than 700 such bright giant pulses over 3 hours, and using this large sample we investigate their amplitude, width, arrival time and energy distributions. The brightest pulse detected in our data has a peak amplitude of $\sim$ 45 kJy and a width of $\sim$ 0.5 $\mu$s, and therefore an inferred brightness temperature of $\sim 10^{35}$ K. The duration of giant-pulse emission is typically $\sim$1 $\mu$s, however it can also be as long as 10 $\mu$s. The pulse shape at a high time resolution (128 ns) shows rich diversity and complexity in structure and is marked by an unusually low degree of scattering. We discuss possible implications for scattering due to the nebula, and for underlying structures and electron densities.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 04:22:20 GMT" } ]
2009-11-13T00:00:00
[ [ "Bhat", "N. D. Ramesh", "" ], [ "Tingay", "Steven J.", "" ], [ "Knight", "Haydon S.", "" ] ]
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801.0335
Andrew Stewart
A. M. Stewart
Longitudinal and transverse components of a vector field
9 pages pdf format. Includes derivation and extension of the Frahm relation and volume integrals of projectors
Sri Lankan Journal of Physics 12, 33-42 (2011)
10.4038/sljp.v12i0.3504
null
physics.class-ph physics.gen-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
A unified account, from a pedagogical perspective, is given of the longitudinal and transverse projective delta functions proposed by Belinfante and of their relation to the Helmholtz theorem for the decomposition of a three-vector field into its longitudinal and transverse components. It is argued that the results are applicable to fields that are time-dependent as well as fields that are time-independent.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 04:54:40 GMT" }, { "version": "v2", "created": "Mon, 13 Jul 2009 01:09:57 GMT" }, { "version": "v3", "created": "Sun, 27 Jun 2010 05:29:32 GMT" }, { "version": "v4", "created": "Mon, 28 Nov 2011 00:28:50 GMT" }, { "version": "v5", "created": "Sat, 8 Nov 2014 02:39:37 GMT" } ]
2014-11-11T00:00:00
[ [ "Stewart", "A. M.", "" ] ]
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801.0336
Carl Akerlof
Fang Yuan, Carl W. Akerlof
Astronomical Image Subtraction by Cross-Convolution
6 pages including 2 figures, accepted for publication in ApJ
null
10.1086/529040
null
astro-ph
null
In recent years, there has been a proliferation of wide-field sky surveys to search for a variety of transient objects. Using relatively short focal lengths, the optics of these systems produce undersampled stellar images often marred by a variety of aberrations. As participants in such activities, we have developed a new algorithm for image subtraction that no longer requires high quality reference images for comparison. The computational efficiency is comparable with similar procedures currently in use. The general technique is cross-convolution: two convolution kernels are generated to make a test image and a reference image separately transform to match as closely as possible. In analogy to the optimization technique for generating smoothing splines, the inclusion of an RMS width penalty term constrains the diffusion of stellar images. In addition, by evaluating the convolution kernels on uniformly spaced subimages across the total area, these routines can accomodate point spread functions that vary considerably across the focal plane.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 04:55:29 GMT" } ]
2009-11-13T00:00:00
[ [ "Yuan", "Fang", "" ], [ "Akerlof", "Carl W.", "" ] ]
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801.0337
Brian Whitworth
Brian Whitworth
The Physical World as a Virtual Reality
The argument that virtual reality information simulations may be relevant to modern physics theory is a little outside the mainstream, but even people in Physics now consider this possibility, e.g. Svozil
null
null
CDMTCS0316
cs.OH
null
This paper explores the idea that the universe is a virtual reality created by information processing, and relates this strange idea to the findings of modern physics about the physical world. The virtual reality concept is familiar to us from online worlds, but our world as a virtual reality is usually a subject for science fiction rather than science. Yet logically the world could be an information simulation running on a multi-dimensional space-time screen. Indeed, if the essence of the universe is information, matter, charge, energy and movement could be aspects of information, and the many conservation laws could be a single law of information conservation. If the universe were a virtual reality, its creation at the big bang would no longer be paradoxical, as every virtual system must be booted up. It is suggested that whether the world is an objective reality or a virtual reality is a matter for science to resolve. Modern information science can suggest how core physical properties like space, time, light, matter and movement could derive from information processing. Such an approach could reconcile relativity and quantum theories, with the former being how information processing creates space-time, and the latter how it creates energy and matter.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 05:04:27 GMT" }, { "version": "v2", "created": "Sat, 5 Jan 2008 08:00:28 GMT" } ]
2008-01-05T00:00:00
[ [ "Whitworth", "Brian", "" ] ]
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801.0338
Bakir Babic
B. Babi\'c, R. Ghai and K. Dimitrov
Magnetophoresis of Flexible DNA-based Dumbbell Structures
4 pages, 3 figures, preprint, to be published in APL
null
10.1063/1.2834698
null
cond-mat.soft cond-mat.other
null
Controlled movement and manipulation of magnetic micro and nanostructures using magnetic forces can give rise to important applications in biomedecine, diagnostics and immunology. We report controlled magnetophoresis and stretching, in aqueous solution, of a DNA-based dumbbell structure containing magnetic and diamagnetic microspheres. The velocity and stretching of the dumbbell were experimentally measured and correlated with a theoretical model based on the forces acting on individual magnetic beads or the entire dumbbell structures. The results show that precise and predictable manipulation of dumbbell structures is achievable and can potentially be applied to immunomagnetic cell separators.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 06:05:56 GMT" } ]
2009-11-13T00:00:00
[ [ "Babić", "B.", "" ], [ "Ghai", "R.", "" ], [ "Dimitrov", "K.", "" ] ]
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801.0339
Keita Tono
Fumio Sakai, Mohammad Saleem and Keita Tono
Hyperelliptic plane curves of type (d,d-2)
14 pages
null
null
null
math.AG
null
In a previous paper, we classified and constructed all rational plane curves of type (d,d-2). In this paper, we generalize these results to irreducible plane curves of type (d,d-2) with positive genus.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 05:39:46 GMT" } ]
2008-01-03T00:00:00
[ [ "Sakai", "Fumio", "" ], [ "Saleem", "Mohammad", "" ], [ "Tono", "Keita", "" ] ]
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801.034
Adam Tenenbaum
Adam J. Tenenbaum and Raviraj S. Adve
Sum Rate Maximization using Linear Precoding and Decoding in the Multiuser MIMO Downlink
6 pages, 4 figures, uses ieeetran.cls
null
null
null
cs.IT math.IT
null
We propose an algorithm to maximize the instantaneous sum data rate transmitted by a base station in the downlink of a multiuser multiple-input, multiple-output system. The transmitter and the receivers may each be equipped with multiple antennas and each user may receive more than one data stream. We show that maximizing the sum rate is closely linked to minimizing the product of mean squared errors (PMSE). The algorithm employs an uplink/downlink duality to iteratively design transmit-receive linear precoders, decoders, and power allocations that minimize the PMSE for all data streams under a sum power constraint. Numerical simulations illustrate the effectiveness of the algorithm and support the use of the PMSE criterion in maximizing the overall instantaneous data rate.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 05:54:33 GMT" } ]
2008-01-03T00:00:00
[ [ "Tenenbaum", "Adam J.", "" ], [ "Adve", "Raviraj S.", "" ] ]
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801.0341
Michael Chertkov
Michael Chertkov (Los Alamos)
Exactness of Belief Propagation for Some Graphical Models with Loops
12 pages, 1 figure, submitted to JSTAT
J. Stat. Mech. (2008) P10016
10.1088/1742-5468/2008/10/P10016
LANL LA-UR-07-8441
cond-mat.stat-mech cond-mat.other cs.AI cs.IT math.IT
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
It is well known that an arbitrary graphical model of statistical inference defined on a tree, i.e. on a graph without loops, is solved exactly and efficiently by an iterative Belief Propagation (BP) algorithm convergent to unique minimum of the so-called Bethe free energy functional. For a general graphical model on a loopy graph the functional may show multiple minima, the iterative BP algorithm may converge to one of the minima or may not converge at all, and the global minimum of the Bethe free energy functional is not guaranteed to correspond to the optimal Maximum-Likelihood (ML) solution in the zero-temperature limit. However, there are exceptions to this general rule, discussed in \cite{05KW} and \cite{08BSS} in two different contexts, where zero-temperature version of the BP algorithm finds ML solution for special models on graphs with loops. These two models share a key feature: their ML solutions can be found by an efficient Linear Programming (LP) algorithm with a Totally-Uni-Modular (TUM) matrix of constraints. Generalizing the two models we consider a class of graphical models reducible in the zero temperature limit to LP with TUM constraints. Assuming that a gedanken algorithm, g-BP, funding the global minimum of the Bethe free energy is available we show that in the limit of zero temperature g-BP outputs the ML solution. Our consideration is based on equivalence established between gapless Linear Programming (LP) relaxation of the graphical model in the $T\to 0$ limit and respective LP version of the Bethe-Free energy minimization.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 06:07:07 GMT" }, { "version": "v2", "created": "Sun, 15 Jun 2008 15:00:41 GMT" }, { "version": "v3", "created": "Thu, 24 Jul 2008 23:35:51 GMT" }, { "version": "v4", "created": "Tue, 2 Sep 2008 21:25:37 GMT" } ]
2009-11-13T00:00:00
[ [ "Chertkov", "Michael", "", "Los Alamos" ] ]
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801.0342
Alexei Kitaev
Alexei Kitaev and William A. Webb
Wavefunction preparation and resampling using a quantum computer
version 2: a shorter, more focused introduction
null
null
null
quant-ph
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We present an algorithm that prepares multidimensional Gaussian wavefunctions on qubit arrays and an application of such wavefunctions to multidimensional resampling, a technique useful in quantum digital simulation.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 07:04:22 GMT" }, { "version": "v2", "created": "Tue, 6 Oct 2009 00:39:22 GMT" } ]
2009-10-06T00:00:00
[ [ "Kitaev", "Alexei", "" ], [ "Webb", "William A.", "" ] ]
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801.0343
Combes Francoise
F. Combes (Observatoire de Paris, LERMA)
Secular evolution of disk galaxies
8 pages, 4 figures, in "Formation and Evolution of Galaxy Disks", ed. J. Funes & E. Corsini
null
null
null
astro-ph
null
Galaxy disks evolve through angular momentum transfers between sub-components, like gas, stars, or dark matter halos, through non axi-symmetric instabilities. The speed of this evolution is boosted in presence of a large fraction of cold and dissipative gas component. When the visible matter dominates over the whole disk, angular momentum is exchanged between gas and stars only. The gas is driven towards the center by bars, stalled transiently in resonance rings, and driven further by embedded bars, which it contributes to destroy. From a small-scale molecular torus, the gas can then inflow from viscous torques, dynamical friction, or m=1 perturbations. In the weakened bar phases, multiple-speed spiral patterns can develop and help the galaxy to accrete external gas flowing from cosmic filaments. The various phases of secular evolution are illustrated by numerical simulations.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 06:29:57 GMT" } ]
2008-01-03T00:00:00
[ [ "Combes", "F.", "", "Observatoire de Paris, LERMA" ] ]
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801.0344
Jae Yong Lee
Jae Yong Lee
Not T-parity but C-parity
14 pages, 2 figures
null
null
KIAS-P07100
hep-ph
null
We revisit the Littlest Higgs model with $T$-parity, and discover a $Z_2$ symmetry on collective symmetry. It is dubbed collective parity ($\EuScript{C}$-parity). We demonstrate that $T$-parity is consistent with $\EuScript{C}$-parity. We further investigate the origin of the collective symmetry in the context of composite Higgs and find a new path to the UV complete theory of the model. In addition, we demonstrate that $T$-parity violating processes naturally take place.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 06:42:23 GMT" } ]
2008-01-03T00:00:00
[ [ "Lee", "Jae Yong", "" ] ]
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801.0345
Emmanuel Candes
Emmanuel J. Cand\`es, Yaniv Plan
Near-ideal model selection by $\ell_1$ minimization
Published in at http://dx.doi.org/10.1214/08-AOS653 the Annals of Statistics (http://www.imstat.org/aos/) by the Institute of Mathematical Statistics (http://www.imstat.org)
Annals of Statistics 2009, Vol. 37, No. 5A, 2145-2177
10.1214/08-AOS653
IMS-AOS-AOS653
math.ST stat.TH
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
We consider the fundamental problem of estimating the mean of a vector $y=X\beta+z$, where $X$ is an $n\times p$ design matrix in which one can have far more variables than observations, and $z$ is a stochastic error term--the so-called "$p>n$" setup. When $\beta$ is sparse, or, more generally, when there is a sparse subset of covariates providing a close approximation to the unknown mean vector, we ask whether or not it is possible to accurately estimate $X\beta$ using a computationally tractable algorithm. We show that, in a surprisingly wide range of situations, the lasso happens to nearly select the best subset of variables. Quantitatively speaking, we prove that solving a simple quadratic program achieves a squared error within a logarithmic factor of the ideal mean squared error that one would achieve with an oracle supplying perfect information about which variables should and should not be included in the model. Interestingly, our results describe the average performance of the lasso; that is, the performance one can expect in an vast majority of cases where $X\beta$ is a sparse or nearly sparse superposition of variables, but not in all cases. Our results are nonasymptotic and widely applicable, since they simply require that pairs of predictor variables are not too collinear.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 07:06:12 GMT" }, { "version": "v2", "created": "Sun, 6 Jan 2008 01:10:27 GMT" }, { "version": "v3", "created": "Fri, 21 Aug 2009 05:15:34 GMT" } ]
2009-08-21T00:00:00
[ [ "Candès", "Emmanuel J.", "" ], [ "Plan", "Yaniv", "" ] ]
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801.0346
Sagar Chakraborty Mr.
Sagar Chakraborty
Two point third order correlation functions for quasi-geostrophic turbulence: Kolmogorov-Landau approach
null
Phys. Fluids 20, 075106 (2008)
10.1063/1.2957017
null
physics.flu-dyn
null
We use the more intuitive approach due to Kolmogorov (and subsequently, Landau in his text on fluid dynamics) to calculate some third-order structure functions for quasi-geostrophic turbulence for the forward cascade of pseudo-potential enstrophy and the inverse energy cascade in quasi-geostrophic turbulence.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 07:07:25 GMT" } ]
2008-07-23T00:00:00
[ [ "Chakraborty", "Sagar", "" ] ]
[ -0.0171296727, 0.0406721793, 0.0614645667, -0.0499707907, -0.0028441546, 0.0086079994, -0.0321875028, -0.0858333483, -0.0413627923, 0.0146138668, -0.0151071623, -0.0386743359, -0.0772500113, 0.0336427242, -0.0106736729, 0.0466163866, -0.0033328249, -0.0525359288, 0.0341853499, 0.1042825803, -0.1104981005, -0.1510469615, 0.0026915413, 0.0659042224, -0.0396609269, 0.0087806527, 0.007843392, 0.0615632273, 0.0531278811, -0.0666934997, 0.0283891317, -0.0102112079, -0.0667428225, -0.0162910707, -0.0254786909, 0.1561772227, -0.063191101, 0.1233237758, -0.0445445478, 0.0762634203, 0.0527332462, -0.0629937798, -0.1073410138, -0.0261199754, 0.0346539803, -0.131512478, 0.0309789311, -0.0252320431, 0.0881025046, -0.0336920545, -0.095008634, -0.0213350132, 0.0370711274, -0.0310282614, -0.0123385433, 0.0164143946, -0.053522516, 0.046098426, -0.0256020147, -0.1105967611, 0.0355419107, -0.1381226182, -0.0176722966, -0.0256266799, -0.0552983806, -0.0415107831, -0.0024772664, 0.0384770185, -0.0068753003, 0.0588994324, -0.0638323873, 0.0526839159, 0.0267119296, -0.0314475633, -0.0543117896, -0.0148358494, -0.0492555164, -0.0101187155, -0.043705944, -0.0581594892, 0.0572715588, 0.0269585773, 0.0212856829, 0.1092155352, -0.0326314718, -0.0145275407, 0.0151934884, -0.0232465304, -0.1520335525, 0.0868199393, -0.0269832406, 0.0673347786, -0.0392416231, -0.0251827147, 0.0130846519, 0.0056759766, 0.0777433068, -0.0511053726, 0.0537198335, -0.050710734, -0.0883491486, 0.0399815664, 0.0385756753, -0.0556930155, 0.1706801057, 0.0134052942, -0.0163650643, -0.0051611001, 0.0261446405, -0.100188233, 0.0387236662, 0.0074117589, -0.0872145742, -0.029696364, 0.0539664812, -0.0526839159, -0.0409188271, -0.040795505, -0.1103994399, -0.0375890844, -0.0201264396, -0.0515493378, 0.122435838, 0.1195747331, 0.0154648013, -0.0310775898, 0.0160567556, -0.0585047975, -0.0426453613, 0.0216186568, 0.0978697464, -0.0410421528, 0.0020502578, -0.0632404312, -0.0068444693, -0.0444212221, 0.0108648241, 0.041313462, 0.015267483, -0.0188068748, 0.0445198826, 0.074980855, 0.0893850699, -0.0569755845, 0.0326561332, 0.097968407, -0.0804070979, -0.0336920545, -0.0485648997, 0.0038569509, -0.0238631498, 0.0033883206, 0.0015939598, -0.063783057, -0.0765100718, -0.0790752023, 0.0948606431, -0.0098720677, 0.0304363072, -0.0468876995, 0.0176229663, 0.0124495346, 0.0172899924, -0.0330014415, 0.0125605259, -0.1064530835, -0.1469032764, -0.0254046973, -0.0850440711, -0.0974257812, -0.0257500038, 0.0093417754, -0.1193774119, -0.0661015436, 0.0426946916, 0.004969948, -0.0263666231, -0.1088209003, 0.0060551972, 0.0910622701, 0.0506614074, -0.0391676314, 0.0576661974, -0.0081701996, -0.0442239046, 0.1853802949, 0.0112286294, -0.0105133513, 0.0031370486, 0.0831695497, -0.0217296481, 0.0912595913, 0.0921475217, -0.0162294079, -0.0470110215, -0.1157270297, 0.0013534784, 0.0242207889, -0.0317928679, 0.0263912864, 0.0493295081, 0.0076337415, 0.1278620809, -0.0515000075, 0.0116664292, -0.012332377, 0.021852972, -0.0782859325, -0.1296379566, -0.004519816, 0.0299430117, -0.0042855013, 0.018646555, 0.0373424366, -0.0154031394, -0.022000961, -0.1517375708, 0.094416678, 0.0098659014, -0.0071281139, -0.1120766476, 0.0674334392, 0.0259473212, 0.0260706451, 0.1101034656, -0.04202874, 0.085438706, -0.1510469615, 0.0404501967, -0.1771916002, 0.0850934014, 0.0562849678, -0.033494737, -0.0087744864, 0.0018776044, -0.0330754369, 0.1348668784, 0.0686666742, -0.064769648, -0.0503654294, -0.0191768464, 0.0590967499, -0.0704918653, -0.0061600222, 0.0828735754, -0.0041991742, -0.0032804124, 0.0167966969, 0.006930796, -0.0360845365, 0.055791676, 0.0173639879, 0.0310282614, 0.028586451, -0.0807030797, 0.0546077676 ]
801.0347
Sagar Chakraborty Mr.
Sagar Chakraborty
On scaling laws in turbulent magnetohydrodynamic Rayleigh-Benard convection
This is typos-corrected version of the earlier version. It has some minor changes. This brief work is not, in any sense, complete. Certain ideas have been put forward whose applicability and validity have to be checked. More work is on the way; constructive critisisms are most welcome
Physica D 237, 3233 (2008)
10.1016/j.physd.2008.08.001
null
physics.flu-dyn
null
We invoke the concepts of magnetic boundary layer and magnetic Rayleigh number and use the magnetic energy dissipation rates in the bulk and the boundary layers to derive some scaling laws expressing how Nusselt number depends on magnetic Rayleigh number, Prandtl number and magnetic Prandtl number for the simple case of turbulent magnetohydrodynamic Rayleigh-Benard convection in the presence of uniform vertical magnetic field.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 07:11:33 GMT" }, { "version": "v2", "created": "Tue, 12 Feb 2008 12:46:06 GMT" } ]
2009-11-13T00:00:00
[ [ "Chakraborty", "Sagar", "" ] ]
[ 0.0862277895, -0.0148176122, 0.1309484094, -0.0860938951, 0.012909621, 0.0243464075, -0.1130958721, -0.0300369058, -0.0623053797, 0.0036207193, -0.0670363083, 0.0215792637, -0.1157737523, 0.119701311, 0.0931010172, 0.0715887025, 0.0057686036, -0.0199613757, 0.0730615407, 0.0445421003, -0.0111243669, -0.0558784641, 0.146658659, 0.0726598576, -0.1371075362, -0.0339421518, 0.0671255663, 0.0613681227, 0.0723920688, -0.027827654, 0.0292558577, -0.0747575313, -0.1022058204, -0.0666792542, -0.0349017233, 0.0573959313, -0.0675718784, 0.0193923265, -0.0494069159, -0.0232752543, -0.0429130532, 0.0050963438, -0.1398746818, 0.1528177857, 0.0276268125, -0.0719457567, -0.051593855, -0.0349240415, 0.1810248047, -0.0268457644, -0.0350356176, -0.0415964276, 0.009322376, -0.0035621405, -0.0208093729, 0.0968500525, 0.0249712467, 0.0255514551, 0.0182653852, -0.1600480676, -0.0275152344, -0.0581546649, -0.0403244346, 0.0023040941, -0.0435825251, 0.0416187458, -0.0320899487, 0.0133336196, 0.0609218068, 0.026265556, -0.0118607841, -0.0546734184, 0.0867633671, 0.0021743842, -0.0753823668, -0.0297244862, 0.0074590165, 0.0492730215, 0.013132778, 0.0518170111, 0.0800686628, -0.0864955783, 0.0110462615, 0.0076208049, -0.0160672907, -0.0000557892, 0.0549412072, 0.0037880868, -0.1311269403, -0.0309518501, 0.036954768, 0.0392309651, -0.06922324, 0.0437610485, 0.0363522433, 0.0265110284, 0.105062224, -0.054316368, 0.07212428, -0.032893315, -0.0357720368, 0.0440511554, 0.0091047976, -0.0569049865, 0.1151489094, 0.0401905403, 0.0150072956, -0.0486035533, -0.065161787, 0.0027225132, 0.0792206675, -0.0165693928, 0.0893073529, -0.0467736684, -0.0303493254, -0.0303270109, -0.0391193889, -0.0329602621, -0.0556106754, -0.0223826282, -0.0319783688, -0.0271804985, 0.1118461937, 0.0006429706, 0.0526203737, -0.0426898971, -0.0156321339, 0.0304162726, 0.0066835466, 0.0816307589, 0.0357720368, -0.0529327951, -0.0070294393, -0.1563882977, -0.0057462878, 0.0032023003, -0.0230744146, -0.0178302284, 0.1113998815, 0.0051075015, 0.0177967548, 0.0103600547, 0.0852458999, -0.0355711952, -0.0259754527, 0.1381786913, -0.0445867293, 0.0030963006, 0.0217689462, 0.0167702343, -0.0279615484, 0.0586456098, -0.0285863876, -0.0234537814, 0.0395880193, -0.063331902, 0.0571727753, 0.017584756, 0.0224049427, -0.0514599606, 0.0124409916, 0.041685693, -0.092654705, -0.087477468, 0.0627516955, 0.0005170961, -0.0198051669, -0.0250605103, -0.0553875193, -0.1123817712, 0.0051549221, -0.0234984122, 0.0117157325, -0.0839962214, 0.1105072498, 0.0244133547, 0.0389408618, -0.181828171, 0.030996481, 0.0978319421, -0.0107394215, 0.0403913818, 0.0041060853, -0.0508797504, -0.0050768172, 0.1020272896, -0.0141258258, -0.0020223586, 0.0777032003, -0.0624839067, -0.075114578, 0.0057741823, -0.0365084521, -0.0046946611, -0.0789082497, -0.1036340222, 0.0740880594, 0.0274036564, 0.0147395069, -0.0056068148, 0.0409046412, 0.0687322989, 0.1121139824, 0.0696695521, 0.0154424515, 0.0705621839, -0.0494069159, -0.0901107192, 0.0043682945, 0.0288318601, 0.042846106, 0.0740434304, 0.0414179042, -0.0582885593, -0.0725259632, -0.0326701552, -0.0989923626, 0.0776139349, 0.0038996653, 0.0341876224, 0.0161342379, 0.0007901146, -0.0567264594, 0.0530220568, 0.0272920784, -0.0188790653, 0.2167298943, -0.0499424934, 0.0881023109, 0.0876559913, 0.0293674357, 0.0380259193, -0.0117268907, 0.0232306235, 0.0320676342, -0.154960081, 0.0628409535, 0.0664114654, -0.0885039866, -0.0297244862, 0.0192138012, 0.0736417472, -0.0523079559, -0.0145721398, 0.0382713936, 0.0714101791, -0.047577031, 0.0643584207, 0.0025690927, -0.0206866357, 0.0164354984, -0.0127645694, -0.0398111753, -0.0714101791, -0.0980997309, -0.0224607326 ]
801.0348
ShengLi Qin
Sheng-Li Qin, Jun-Hui Zhao, James M. Moran, Daniel P. Marrone, Nimesh A. Patel, Jun-Jie Wang, Sheng-Yuan Liu, Yi-Jehng Kuan
Infall and Outflow of Molecular Gas in Sgr B2
44 pages, 14 figures Accepted for publication in The Astrophysical Journal
null
10.1086/529067
null
astro-ph
null
Observations of two H$_2$CO ($3_{03}-2_{02}$ and $3_{21}-2_{20}$) lines and continuum emission at 1.3 mm towards Sgr B2(N) and Sgr B2(M) have been carried out with the SMA. The mosaic maps of Sgr B2(N) and Sgr B2(M) in both continuum and lines show a complex distribution of dust and molecular gas in both clumps and filaments surrounding the compact star formation cores. We have observed a decelerating outflow originated from the Sgr B2(M) core, showing that both the red-shifted and blue-shifted outflow components have a common terminal velocity. This terminal velocity is 58$\pm$2 km s$^{-1}$. It provides an excellent method in determination of the systematic velocity of the molecular cloud. The SMA observations have also shown that a large fraction of absorption against the two continuum cores is red-shifted with respect to the systematic velocities of Sgr B2(N) and Sgr B2(M), respectively, suggesting that the majority of the dense molecular gas is flowing into the two major cores where massive stars have been formed. We have solved the radiative transfer in a multi-level system with LVG approximation. The observed H$_2$CO line intensities and their ratios can be adequately fitted with this model for the most of the gas components. However, the line intensities between the higher energy level transition H$_2$CO ($3_{21}-2_{20}$) and the lower energy level transition H$_2$CO ($3_{03}-2_{02}$) is reversed in the red-shifted outflow region of Sgr B2(M), suggesting the presence of inversion in population between the ground levels in the two K ladders (K$_{-1}$= 0 and 2). The possibility of weak maser processes for the H$_2$CO emission in Sgr B2(M) is discussed.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:11:09 GMT" } ]
2009-11-13T00:00:00
[ [ "Qin", "Sheng-Li", "" ], [ "Zhao", "Jun-Hui", "" ], [ "Moran", "James M.", "" ], [ "Marrone", "Daniel P.", "" ], [ "Patel", "Nimesh A.", "" ], [ "Wang", "Jun-Jie", "" ], [ "Liu", "Sheng-Yuan", "" ], [ "Kuan", "Yi-Jehng", "" ] ]
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801.0349
Marie Ferbus-Zanda
Marie Ferbus-Zanda (LIAFA), Serge Grigorieff (LIAFA)
Church, Cardinal and Ordinal Representations of Integers and Kolmogorov complexity
16 pages
Dans Denis Richard's 60th Biirthday Conference - Denis Richard's 60th Biirthday Conference, France (2002)
null
null
math.LO cs.CC cs.LO
null
We consider classical representations of integers: Church's function iterators, cardinal equivalence classes of sets, ordinal equivalence classes of totally ordered sets. Since programs do not work on abstract entities and require formal representations of objects, we effectivize these abstract notions in order to allow them to be computed by programs. To any such effectivized representation is then associated a notion of Kolmogorov complexity. We prove that these Kolmogorov complexities form a strict hierarchy which coincides with that obtained by relativization to jump oracles and/or allowance of infinite computations.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:35:27 GMT" } ]
2008-01-03T00:00:00
[ [ "Ferbus-Zanda", "Marie", "", "LIAFA" ], [ "Grigorieff", "Serge", "", "LIAFA" ] ]
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801.035
Marie Ferbus-Zanda
Marie Ferbus-Zanda (LIAFA), Serge Grigorieff (LIAFA)
Refinment of the "up to a constant" ordering using contructive co-immunity and alike. Application to the Min/Max hierarchy of Kolmogorov complexities
41 pages
null
null
null
math.LO cs.CC
null
We introduce orderings between total functions f,g: N -> N which refine the pointwise "up to a constant" ordering <=cte and also insure that f(x) is often much less thang(x). With such orderings, we prove a strong hierarchy theorem for Kolmogorov complexities obtained with jump oracles and/or Max or Min of partial recursive functions. We introduce a notion of second order conditional Kolmogorov complexity which yields a uniform bound for the "up to a constant" comparisons involved in the hierarchy theorem.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:35:59 GMT" } ]
2008-01-07T00:00:00
[ [ "Ferbus-Zanda", "Marie", "", "LIAFA" ], [ "Grigorieff", "Serge", "", "LIAFA" ] ]
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801.0351
Marie Ferbus-Zanda
Marie Ferbus-Zanda (LIAFA), Serge Grigorieff (LIAFA)
Kolmogorov complexities Kmax, Kmin on computable partially ordered sets
35 pages
Theoretical Computer Science 352 (2006) 159-180
null
null
math.LO cs.LO
null
We introduce a machine free mathematical framework to get a natural formalization of some general notions of infinite computation in the context of Kolmogorov complexity. Namely, the classes Max^{X\to D}_{PR} and Max^{X\to D}_{Rec} of functions X \to D which are pointwise maximum of partial or total computable sequences of functions where D = (D,<) is some computable partially ordered set. The enumeration theorem and the invariance theorem always hold for Max^{X\to D}_{PR}, leading to a variant KD;max of Kolmogorov complexity. We characterize the orders D such that the enumeration theorem (resp. the invariance theorem) also holds for Max^{X\to D}_{Rec} . It turns out that Max^{X\to D}_{Rec} may satisfy the invariance theorem but not the enumeration theorem. Also, when Max^{X\to D}_{Rec} satisfies the invariance theorem then the Kolmogorov complexities associated to Max^{X\to D}_{Rec} and Max^{X\to D}_{PR} are equal (up to a constant). Letting K^D_{min} = K^{D^{rev}}_{max}, where D^{rev} is the reverse order, we prove that either K^D_{min} =_{ct} K^D_{max} =_{ct} K^D (=_{ct} is equality up to a constant) or K^D_{min}, K^D_{max} are <=_{ct} incomparable and <_{ct} K^D and >_{ct} K^{0',D}. We characterize the orders leading to each case. We also show that K^D_{min}, K^D_{max} cannot be both much smaller than K^D at any point. These results are proved in a more general setting with two orders on D, one extending the other.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:36:29 GMT" } ]
2008-01-07T00:00:00
[ [ "Ferbus-Zanda", "Marie", "", "LIAFA" ], [ "Grigorieff", "Serge", "", "LIAFA" ] ]
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801.0352
Anant Sahai
Anant Sahai and Pulkit Grover
The price of certainty: "waterslide curves" and the gap to capacity
37 pages, 13 figures. Submitted to IEEE Transactions on Information Theory. This version corrects a subtle bug in the proofs of the original submission and improves the bounds significantly
null
null
UCB/EECS-2008-1
cs.IT math.IT
null
The classical problem of reliable point-to-point digital communication is to achieve a low probability of error while keeping the rate high and the total power consumption small. Traditional information-theoretic analysis uses `waterfall' curves to convey the revolutionary idea that unboundedly low probabilities of bit-error are attainable using only finite transmit power. However, practitioners have long observed that the decoder complexity, and hence the total power consumption, goes up when attempting to use sophisticated codes that operate close to the waterfall curve. This paper gives an explicit model for power consumption at an idealized decoder that allows for extreme parallelism in implementation. The decoder architecture is in the spirit of message passing and iterative decoding for sparse-graph codes. Generalized sphere-packing arguments are used to derive lower bounds on the decoding power needed for any possible code given only the gap from the Shannon limit and the desired probability of error. As the gap goes to zero, the energy per bit spent in decoding is shown to go to infinity. This suggests that to optimize total power, the transmitter should operate at a power that is strictly above the minimum demanded by the Shannon capacity. The lower bound is plotted to show an unavoidable tradeoff between the average bit-error probability and the total power used in transmission and decoding. In the spirit of conventional waterfall curves, we call these `waterslide' curves.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:36:34 GMT" } ]
2008-01-03T00:00:00
[ [ "Sahai", "Anant", "" ], [ "Grover", "Pulkit", "" ] ]
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801.0353
Marie Ferbus-Zanda
Marie Ferbus-Zanda (LIAFA), Serge Grigorieff (LIAFA)
Set theoretical Representations of Integers, I
56 pages
Mathematical Logic Quaterly 52, Number 4 (2006) 375-403
10.1002/malq.200510040
null
math.LO cs.CC
null
We reconsider some classical natural semantics of integers (namely iterators of functions, cardinals of sets, index of equivalence relations), in the perspective of Kolmogorov complexity. To each such semantics one can attach a simple representation of integers that we suitably effectivize in order to develop an associated Kolmogorov theory. Such effectivizations are particular instances of a general notion of "self-enumerated system" that we introduce in this paper. Our main result asserts that, with such effectivizations, Kolmogorov theory allows to quantitatively distinguish the underlying semantics. We characterize the families obtained by such effectivizations and prove that the associated Kolmogorov complexities constitute a hierarchy which coincides with that of Kolmogorov complexities defined via jump oracles and/or infinite computations. This contrasts with the well-known fact that usual Kolmogorov complexity does not depend (up to a constant) on the chosen arithmetic representation of integers, let it be in any base unary, binary et so on. Also, in a conceptual point of view, our result can be seen as a mean to measure the degree of abstraction of these diverse semantics.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:37:01 GMT" } ]
2008-01-03T00:00:00
[ [ "Ferbus-Zanda", "Marie", "", "LIAFA" ], [ "Grigorieff", "Serge", "", "LIAFA" ] ]
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801.0354
Marie Ferbus-Zanda
Marie Ferbus-Zanda (LIAFA), Serge Grigorieff (LIAFA)
Kolmogorov complexity in perspective
37 pages
null
null
null
math.LO cs.CC cs.IT math.IT
null
We survey the diverse approaches to the notion of information content: from Shannon entropy to Kolmogorov complexity. The main applications of Kolmogorov complexity are presented namely, the mathematical notion of randomness (which goes back to the 60's with the work of Martin-Lof, Schnorr, Chaitin, Levin), and classification, which is a recent idea with provocative implementation by Vitanyi and Cilibrasi.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:38:18 GMT" } ]
2008-01-03T00:00:00
[ [ "Ferbus-Zanda", "Marie", "", "LIAFA" ], [ "Grigorieff", "Serge", "", "LIAFA" ] ]
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801.0355
Mili Biswas
Mili Biswas
Comparative study of the radius of sensitivity of the optical model potentials for $^6$Li+$^{58,64}$Ni and $^{16}$O+$^{58,64}$Ni
Accepted for publication as a Brief Report in Physical Review C (4 pages, 5 figures)
Phys.Rev.C77:017602,2008
10.1103/PhysRevC.77.017602
null
nucl-ex
null
Radii of sensitivity were estimated for the $^{6}$Li+$^{58,64}$Ni system at energies near the Coulomb barrier. For comparison purposes, such radii were also estimated for stable $^{16}$O scattered from same target isotopes. The elastic scattering data were analysed with folded real potential generated from DDM3Y nucleon-nucleon interaction and an imaginary potential of volume Woods-Saxon form. The most sensitive radii for $^{16}$O+$^{58,64}$Ni system are found to be energy independent and close to the strong absorption radius. For $^{6}$Li projectile, unlike its strongly bound counterpart, the crossing radius increases with decreasing energy. However, no two crossing situation has been observed for both $^{6}$Li+$^{58,64}$Ni and $^{16}$O+$^{58,64}$Ni systems at the top of the barrier.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:51:11 GMT" } ]
2008-12-18T00:00:00
[ [ "Biswas", "Mili", "" ] ]
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801.0356
Pulak Ranjan Giri
Pulak Ranjan Giri
Localization at threshold in noncommutative space
4 pages, no figure, Refs. added
Phys.Lett.A372:5123-5125,2008
10.1016/j.physleta.2008.06.001
SINP/TNP/2008/01
hep-th math-ph math.MP quant-ph
null
The ground state energy of a scale symmetric system usually does not possess any lower bound, thus making the system quantum mechanically unstable. Self-adjointness and renormalization techniques usually provide the system a scale and thus making the ground state bounded from below. We on the other hand use noncommutative quantum mechanics and exploit the noncommutative parameter \Theta as a scale for a scale symmetric system. The resulting Hamiltonian for the system then allows an unusual bound state at the threshold of the energy, E=0. Apart from the Hamiltonian \hat{H} we also compute the other two generators of the so(2,1) algebra, the dilation \hat{D} and the conformal generator \hat{K} in the noncommutative space. The so(2,1) algebra is not closed in the noncommutative space, but the limit \Theta\to 0 smoothly goes to the so(2,1) algebra restoring the conformal symmetry. We also discuss the system for large noncommutative parameter.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 08:55:00 GMT" }, { "version": "v2", "created": "Thu, 7 Feb 2008 11:36:44 GMT" } ]
2008-11-26T00:00:00
[ [ "Giri", "Pulak Ranjan", "" ] ]
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801.0357
Wei-Rong Zhong
Wei-Rong Zhong, Yuan-Zhi Shao, Li Li, Feng-Hua Wang, and Zhen-Hui He
Spatiotemporal Noise Triggering Infiltrative Tumor Growth under Immune Surveillance
8 pages, 6 figures
null
10.1209/0295-5075/82/20003
null
q-bio.OT q-bio.PE
null
A spatiotemporal noise is assumed to reflect the environmental fluctuation in a spatially extended tumor system. We introduce firstly the structure factor to reveal the invasive tumor growth quantitatively. The homogenous environment can lead to an expansive growth of the tumor cells, while the inhomogenous environment underlies an infiltrative growth. The different responses of above two cases are separated by a characteristic critical intensity of the spatiotemporal noise. Theoretical and numerical results present a close annotation to the clinical images.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 09:09:56 GMT" } ]
2009-11-13T00:00:00
[ [ "Zhong", "Wei-Rong", "" ], [ "Shao", "Yuan-Zhi", "" ], [ "Li", "Li", "" ], [ "Wang", "Feng-Hua", "" ], [ "He", "Zhen-Hui", "" ] ]
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801.0358
Morten Stejner
Morten Stejner, Fridolin Weber, Jes Madsen
Signature of deconfinement with spin down compression in cooling hybrid stars
30 pages, 13 figures. Updated to match the version published in ApJ
Astrophys.J.694:1019-1033,2009
10.1088/0004-637X/694/2/1019
null
astro-ph hep-ph nucl-th
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
The thermal evolution of neutron stars is coupled to their spin down and the resulting changes in structure and chemical composition. This coupling correlates stellar surface temperatures with rotational state as well as time. We report an extensive investigation of the coupling between spin down and cooling for hybrid stars which undergo a phase transition to deconfined quark matter at the high densities present in stars at low rotation frequencies. The thermal balance of neutron stars is re-analyzed to incorporate phase transitions and the related latent heat self-consistently, and numerical calculations are undertaken to simultaneously evolve the stellar structure and temperature distribution. We find that the changes in stellar structure and chemical composition with the introduction of a pure quark matter phase in the core delay the cooling and produce a period of increasing surface temperature for strongly superfluid stars of strong and intermediate magnetic field strength. The latent heat of deconfinement is found to reinforce this signature if quark matter is superfluid and it can dominate the thermal balance during the formation of a pure quark matter core. At other times it is less important and does not significantly change the thermal evolution.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 09:12:14 GMT" }, { "version": "v2", "created": "Sun, 5 Apr 2009 19:31:57 GMT" } ]
2009-06-23T00:00:00
[ [ "Stejner", "Morten", "" ], [ "Weber", "Fridolin", "" ], [ "Madsen", "Jes", "" ] ]
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801.0359
Miloslav Znojil
Miloslav Znojil
Matrix Hamiltonians with an algebraic guarantee of unbroken PT-symmetry
25 pp., partially presented during the 6th International Workshop on Pseudo Hermitian Hamiltonians in Quantum Physics (16th-18th of July 2007, City University, London, http://www.staff.city.ac.uk/~fring/PT/)
J. Phys. A: Math. Theor. 41 (2008) 244027
10.1088/1751-8113/41/24/244027
null
math-ph math.MP
null
Quantum bound-state energies are assumed generated by PT-symmetric Hamiltonians H where P is, typically, parity. It is known that their spectrum only remains real and observable (i.e., in the language of physics, the PT-symmetry remains unbroken) inside a certain domain D of couplings. We show that the boundary of this domain (i.e., certain stability and observability horizon formed by the Kato's exceptional points) remains algebraic (i.e., we determine it by closed formulae) for a certain toy-model family of N-dimensional anharmonic-oscillator-related matrix Hamiltonians with dimensions between N=2 and N=11.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 09:18:41 GMT" } ]
2008-09-09T00:00:00
[ [ "Znojil", "Miloslav", "" ] ]
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801.036
Hank Miller
Justin M. Conroy, H. G. Miller
Color Superconductivity and Tsallis Statistics
null
Phys.Rev.D78:054010,2008
10.1103/PhysRevD.78.054010
null
hep-ph cond-mat.supr-con nucl-th
null
The generalized non-extensive statistics proposed by Tsallis have been successfully utilized in many systems where long range interactions are present. For high density quark matter an attractive long range interaction arising from single gluon exchange suggests the formation of a diquark condensate. We study the effects on this color superconducting phase for two quark flavors due to a change to Tsallis statistics. By numerically solving the gap equation we obtain a generalization of the universality condition, $\frac{2\phi_{0}}{T_{C}}\approx 3.52$ and determine the temperature dependence of the gap. For the Tsallis parameter $q\approx 1$ the specific heat is exponential becoming more linear as q increases. This suggests that for larger values of q s-wave color superconductors behave like high $T_c$ superconductors rather than weak superconductors.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 09:27:14 GMT" } ]
2009-01-09T00:00:00
[ [ "Conroy", "Justin M.", "" ], [ "Miller", "H. G.", "" ] ]
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801.0361
Jiangfeng Du
Jiangfeng Du, Lingzhi Hu, Ya Wang, Jianda Wu, Meisheng Zhao, and Dieter Suter
Is the quantum adiabatic theorem consistent?
4 pages, 3 figures
null
null
null
quant-ph
null
The quantum adiabatic theorem states that if a quantum system starts in an eigenstate of the Hamiltonian, and this Hamiltonian varies sufficiently slowly, the system stays in this eigenstate. We investigate experimentally the conditions that must be fulfilled for this theorem to hold. We show that the traditional adiabatic condition as well as some conditions that were recently suggested are either not sufficient or not necessary. Experimental evidence is presented by a simple experiment using nuclear spins.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 09:50:17 GMT" } ]
2008-01-03T00:00:00
[ [ "Du", "Jiangfeng", "" ], [ "Hu", "Lingzhi", "" ], [ "Wang", "Ya", "" ], [ "Wu", "Jianda", "" ], [ "Zhao", "Meisheng", "" ], [ "Suter", "Dieter", "" ] ]
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801.0362
Armin L\"uhr
Armin L\"uhr and Alejandro Saenz
Antiproton and proton collisions with the alkali metal atoms Li, Na, and K
null
null
10.1103/PhysRevA.77.052713
null
physics.atom-ph
null
Single-electron ionization and excitation cross sections as well as cross sections for excitation into the first excited p state of the alkali metal atoms Li(2s), Na(3s) and K(4s) colliding with antiprotons and protons were calculated using a time-dependent channel-coupling approach. For antiprotons an impact-energy range from 0.25 to 1000 keV and for protons from 2 to 1000 keV was considered. The target atoms are treated as effective one-electron systems using a model potential. The results are compared with theoretical and experimental data from literature and calculated cross sections for antiproton-hydrogen collisions. For proton collisions a good overall agreement is found which confirms the present numerical approach, whereas discrepancies are found between the present antiproton cross sections and those calculated by Stary et al., J.Phys.B 23, 263 (1990).
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:30:53 GMT" } ]
2009-11-13T00:00:00
[ [ "Lühr", "Armin", "" ], [ "Saenz", "Alejandro", "" ] ]
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801.0363
S. N. Kaul
S. Kumar, S. N. Kaul, J. Rodriguez Fernandez, L. Fernandez Barquin and P. F. Henry
Correlation between site preference of ternary Mn addition in LaAg and superconductivity
The manuscript has 25 pages that include the text, 2 Tables and 12 Figures. The manuscript contains unpublished results which are of paramount interest to the Condensed Matter Physics Community at large and particularly to those engaged in the pursuit of research in Unconventional Superconductivity
Preliminary results have been briefly reported in Europhys. Lett. 74, 138 (2006)
10.1063/1.2952525
null
cond-mat.mtrl-sci cond-mat.supr-con
null
The results of an extensive investigation of structure, surface morphology, composition and the superconducting-normal phase diagram of a new unconventional superconductor LaAg1-cMnc with nominal composition c = 0.0, 0.025, 0.05, 0.1, 0.2 and 0.3, reveal the following. The alloys with c = 0, 0.025 and 0.05 are essentially single phase alloys with the actual Mn concentration, x, same as the nominal one, i.e., c = x, whereas in the alloys with c = 0.1, 0.2 and 0.3, the actual Mn concentration of the majority phase (crystalline grains) is x = 0.050(1), 0.080(1) and 0.100(1), respectively. The ternary Mn addition does not alter the CsCl structure of the parent compound LaAg. Neither a structural phase transition occurs nor a long-range antiferromagnetic order exists at any temperature within the range 1.8K < = T < = 50K in any of the Mn containing alloys. Mn has exclusive La (Ag) site preference in the alloy (alloys) with x = c = 0.025 (x < = 0.05 or c < = 0.1) whereas in the alloy with x = c = 0.05, Mn has essentially no site preference in that all the Mn atoms either occupy the La sites or the Ag sites. In the alloys (alloy) with x < = 0.05 (x = c = 0.025), substitution of Ag (La) by Mn at the Ag (La) sub-lattice sites in LaAg host gives rise to unconventional superconductivity (destroys the conventional phonon-mediated superconductivity prevalent in the parent LaAg compound).
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:11:36 GMT" } ]
2009-11-13T00:00:00
[ [ "Kumar", "S.", "" ], [ "Kaul", "S. N.", "" ], [ "Fernandez", "J. Rodriguez", "" ], [ "Barquin", "L. Fernandez", "" ], [ "Henry", "P. F.", "" ] ]
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801.0364
Pellegrini Vittorio
Sokratis Kalliakos, Vittorio Pellegrini, Cesar Pascual Garcia, Aron Pinczuk, Loren N. Pfeiffer, Ken. W. West
Optical control of energy-level structure of few electrons in AlGaAs/GaAs quantum dots
To appear in NanoLetters
null
10.1021/nl072904p
null
cond-mat.mes-hall cond-mat.mtrl-sci
null
Optical control of the lateral quantum confinement and number of electrons confined in nanofabricated GaAs/AlGaAs quantum dots is achieved by illumination with a weak laser beam that is absorbed in the AlGaAs barrier. Precise tuning of energy-level structure and electron population is demonstrated by monitoring the low-lying transitions of the electrons from the lowest quantum-dot energy shells by resonant inelastic light scattering. These findings open the way to the manipulation of single electrons in these quantum dots without the need of external metallic gates.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:22:40 GMT" } ]
2015-05-13T00:00:00
[ [ "Kalliakos", "Sokratis", "" ], [ "Pellegrini", "Vittorio", "" ], [ "Garcia", "Cesar Pascual", "" ], [ "Pinczuk", "Aron", "" ], [ "Pfeiffer", "Loren N.", "" ], [ "West", "Ken. W.", "" ] ]
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801.0365
Sanzo Miyazawa
Sanzo Miyazawa and Akira R. Kinjo
Properties of contact matrices induced by pairwise interactions in proteins
Errata in DOI:10.1103/PhysRevE.77.051910 has been corrected in the present version
Physical Review E, 77, 051910, 2008
10.1103/PhysRevE.77.051910
null
q-bio.BM
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
The total conformational energy is assumed to consist of pairwise interaction energies between atoms or residues, each of which is expressed as a product of a conformation-dependent function (an element of a contact matrix, C-matrix) and a sequence-dependent energy parameter (an element of a contact energy matrix, E-matrix). Such pairwise interactions in proteins force native C-matrices to be in a relationship as if the interactions are a Go-like potential [N. Go, Annu. Rev. Biophys. Bioeng. 12. 183 (1983)] for the native C-matrix, because the lowest bound of the total energy function is equal to the total energy of the native conformation interacting in a Go-like pairwise potential. This relationship between C- and E-matrices corresponds to (a) a parallel relationship between the eigenvectors of the C- and E-matrices and a linear relationship between their eigenvalues, and (b) a parallel relationship between a contact number vector and the principal eigenvectors of the C- and E-matrices; the E-matrix is expanded in a series of eigenspaces with an additional constant term, which corresponds to a threshold of contact energy that approximately separates native contacts from non-native ones. These relationships are confirmed in 182 representatives from each family of the SCOP database by examining inner products between the principal eigenvector of the C-matrix, that of the E-matrix evaluated with a statistical contact potential, and a contact number vector. In addition, the spectral representation of C- and E-matrices reveals that pairwise residue-residue interactions, which depends only on the types of interacting amino acids but not on other residues in a protein, are insufficient and other interactions including residue connectivities and steric hindrance are needed to make native structures the unique lowest energy conformations.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:37:16 GMT" }, { "version": "v2", "created": "Tue, 22 Jan 2008 06:43:43 GMT" }, { "version": "v3", "created": "Wed, 31 Aug 2011 07:53:25 GMT" } ]
2011-09-01T00:00:00
[ [ "Miyazawa", "Sanzo", "" ], [ "Kinjo", "Akira R.", "" ] ]
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801.0366
Merce Romero-Gomez
M. Romero-Gomez
The formation of spiral arms and rings in barred galaxies
6 pages, 3 figures, conference proceedings of "Semaine de l'Astrophysique Francaise", Grenoble 2007, eds. J. Bouvier, A. Chalabaev, C. Charbonnel
null
10.1142/9789812818805_0022
LAM-07-07
astro-ph
null
We propose a theory to explain the formation of both spirals and rings in barred galaxies using a common dynamical framework. It is based on the orbital motion driven by the unstable equilibrium points of the rotating bar potential. Thus, spirals, rings and pseudo-rings are related to the invariant manifolds associated to the periodic orbits around these equilibrium points. We examine the parameter space of three barred galaxy models and discuss the formation of the different morphological structures according to the properties of the bar model. We also study the influence of the shape of the rotation curve in the outer parts, by making families of models with rising, flat or falling rotation curves in the outer parts. The differences between spiral and ringed structures arise from differences in the dynamical parameters of the host galaxies.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:50:41 GMT" } ]
2016-11-23T00:00:00
[ [ "Romero-Gomez", "M.", "" ] ]
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801.0367
Roman Skibinski
H. Witala, J. Golak, R. Skibinski, W. Glockle, W. N. Polyzou, H. Kamada
Relativity and the low energy nd Ay puzzle
29 pages, 2 ps figures
Phys.Rev.C77:034004,2008
10.1103/PhysRevC.77.034004
null
nucl-th
null
We solve the Faddeev equation in an exactly Poincare invariant formulation of the three-nucleon problem. The dynamical input is a relativistic nucleon-nucleon interaction that is exactly on-shell equivalent to the high precision CDBonn NN interaction. S-matrix cluster properties dictate how the two-body dynamics is embedded in the three-nucleon mass operator. We find that for neutron laboratory energies above 20 MeV relativistic effects on Ay are negligible. For energies below 20 MeV dynamical effects lower the nucleon analyzing power maximum slightly by 2% and Wigner rotations lower it further up to 10 % increasing thus disagreement between data and theory. This indicates that three-nucleon forces must provide an even larger increase of the Ay maximum than expected up to now.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 10:52:40 GMT" } ]
2008-11-26T00:00:00
[ [ "Witala", "H.", "" ], [ "Golak", "J.", "" ], [ "Skibinski", "R.", "" ], [ "Glockle", "W.", "" ], [ "Polyzou", "W. N.", "" ], [ "Kamada", "H.", "" ] ]
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801.0368
Neil Drummond
N. D. Drummond and R. J. Needs
Quantum Monte Carlo, Density Functional Theory, and Pair Potential Studies of Solid Neon
null
Phys. Rev. B 73, 024107 (2006)
10.1103/PhysRevB.73.024107
null
cond-mat.mtrl-sci
null
We report quantum Monte Carlo (QMC), plane-wave density-functional theory (DFT), and interatomic pair-potential calculations of the zero-temperature equation of state (EOS) of solid neon. We find that the DFT EOS depends strongly on the choice of exchange-correlation functional, whereas the QMC EOS is extremely close to both the experimental EOS and the EOS obtained using the best semiempirical pair potential in the literature. This suggests that QMC is able to give an accurate treatment of van der Waals forces in real materials, unlike DFT. We calculate the QMC EOS up to very high densities, beyond the range of values for which experimental data are currently available. At high densities the QMC EOS is more accurate than the pair-potential EOS. We generate a different pair potential for neon by a direct evaluation of the QMC energy as a function of the separation of an isolated pair of neon atoms. The resulting pair potential reproduces the EOS more accurately than the equivalent potential generated using the coupled-cluster CCSD(T) method.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 11:02:26 GMT" } ]
2008-01-03T00:00:00
[ [ "Drummond", "N. D.", "" ], [ "Needs", "R. J.", "" ] ]
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801.0369
Irina Kmit
Irina Kmit
Classical solvability of nonlinear initial-boundary problems for first-order hyperbolic systems
12 pages
null
null
null
math.AP
null
We prove the global classical solvability of initial-boundary problems for semilinear first-order hyperbolic systems subjected to local and nonlocal nonlinear boundary conditions. We also establish lower bounds for the order of nonlinearity demarkating a frontier between regular cases (classical solvability) and singular cases (blow-up of solutions).
[ { "version": "v1", "created": "Wed, 2 Jan 2008 11:15:16 GMT" } ]
2008-01-03T00:00:00
[ [ "Kmit", "Irina", "" ] ]
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801.037
Parongama Sen
Parongama Sen
Funnelling related phase transitions in networks
4 pages, revtex4, 6 figures This paper is withdrawn as it required some correction
null
null
CUPhysics/14/2007
cond-mat.dis-nn physics.soc-ph
null
Funnelling effect, in the context of searching on networks, precisely indicates that the search takes place through a few specific nodes. We define the funnelling capacity $f$ of a node as the fraction of successful dynamic paths through it with a fixed target. We claim that there is a funnelling effect if the distribution $D(f)$ of the fraction of nodes with funnelling capacity $f$ shows a power law behaviour. We find that a transition from a search with funnelling effect to that without any such effect can exist and is driven by the parameters defining the network.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 11:20:34 GMT" }, { "version": "v2", "created": "Mon, 8 Mar 2010 06:46:08 GMT" } ]
2010-03-09T00:00:00
[ [ "Sen", "Parongama", "" ] ]
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801.0371
Hyesung Kang
Santabrata Das, Hyesung Kang, Dongsu Ryu, and Jungyeon Cho
Propagation of UHE Protons through Magnetized Cosmic Web
24 pages, 8 figures, corrected typos
null
10.1086/588278
null
astro-ph
null
If ultra-high-energy cosmic rays (UHECRs) originate from extragalactic sources, understanding the propagation of charged particles through the magnetized large scale structure (LSS) of the universe is crucial in the search for the astrophysical accelerators. Based on a novel model of the turbulence dynamo, we estimate the intergalactic magnetic fields (IGMFs) in cosmological simulations of the formation of the LSS. Under the premise that the sources of UHECRs are strongly associated with the LSS, we consider a model in which protons with E >10^{19} eV are injected by sources that represent active galactic nuclei located inside clusters of galaxies. With the model IGMFs, we then follow the trajectories of the protons, while taking into account the energy losses due to interactions with the cosmic background radiation. For observers located inside groups of galaxies like ours, about 70% and 35% of UHECR events above 60 EeV arrive within ~15 degree and ~5 degree, respectively, of the source position with time delays of less than ~10^7 yr. This implies that the arrival direction of super-GZK protons might exhibit a correlation with the distribution of cosmological sources on the sky. In this model, nearby sources (within 10 - 20 Mpc) should contribute significantly to the particle flux above ~10^{20} eV.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 11:18:08 GMT" }, { "version": "v2", "created": "Fri, 16 May 2008 00:07:17 GMT" } ]
2009-11-13T00:00:00
[ [ "Das", "Santabrata", "" ], [ "Kang", "Hyesung", "" ], [ "Ryu", "Dongsu", "" ], [ "Cho", "Jungyeon", "" ] ]
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801.0372
Neil Drummond
N. D. Drummond, P. Lopez Rios, A. Ma, J. R. Trail, G. Spink, M. D. Towler, and R. J. Needs
Quantum Monte Carlo study of the Ne atom and the Ne+ ion
null
J. Chem. Phys. 124, 224104 (2006)
10.1063/1.2204600
null
cond-mat.mtrl-sci
null
We report all-electron and pseudopotential calculations of the ground-stateenergies of the neutral Ne atom and the Ne+ ion using the variational and diffusion quantum Monte Carlo (DMC) methods. We investigate different levels of Slater-Jastrow trial wave function: (i) using Hartree-Fock orbitals, (ii) using orbitals optimized within a Monte Carlo procedure in the presence of a Jastrow factor, and (iii) including backflow correlations in the wave function. Small reductions in the total energy are obtained by optimizing the orbitals, while more significant reductions are obtained by incorporating backflow correlations. We study the finite-time-step and fixed-node biases in the DMC energy and show that there is a strong tendency for these errors to cancel when the first ionization potential (IP) is calculated. DMC gives highly accurate values for the IP of Ne at all the levels of trial wave function that we have considered.
[ { "version": "v1", "created": "Wed, 2 Jan 2008 11:20:08 GMT" } ]
2008-01-03T00:00:00
[ [ "Drummond", "N. D.", "" ], [ "Rios", "P. Lopez", "" ], [ "Ma", "A.", "" ], [ "Trail", "J. R.", "" ], [ "Spink", "G.", "" ], [ "Towler", "M. D.", "" ], [ "Needs", "R. J.", "" ] ]
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