id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0401073 | Shin'ichi Nojiri | Iver Brevik, Shin'ichi Nojiri, Sergei D. Odintsov, Luciano Vanzo | Entropy and universality of Cardy-Verlinde formula in dark energy
universe | LaTeX file, 39 pages, references are added | Phys.Rev.D70:043520,2004 | 10.1103/PhysRevD.70.043520 | null | hep-th astro-ph gr-qc | null | We study the entropy of a FRW universe filled with dark energy (cosmological
constant, quintessence or phantom). For general or time-dependent equation of
state $p=w\rho$ the entropy is expressed in terms of energy, Casimir energy,
and $w$. The correspondent expression reminds one about 2d CFT entropy only for
confor... | [
{
"created": "Mon, 12 Jan 2004 14:12:04 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Apr 2004 11:34:24 GMT",
"version": "v2"
}
] | 2009-01-14 | [
[
"Brevik",
"Iver",
""
],
[
"Nojiri",
"Shin'ichi",
""
],
[
"Odintsov",
"Sergei D.",
""
],
[
"Vanzo",
"Luciano",
""
]
] | We study the entropy of a FRW universe filled with dark energy (cosmological constant, quintessence or phantom). For general or time-dependent equation of state $p=w\rho$ the entropy is expressed in terms of energy, Casimir energy, and $w$. The correspondent expression reminds one about 2d CFT entropy only for conforma... | 14.142437 | 13.941066 | 14.573669 | 13.813878 | 14.251631 | 14.942837 | 14.476344 | 14.576053 | 13.746458 | 16.120766 | 13.535048 | 13.510795 | 13.863379 | 13.935186 | 14.004906 | 13.658121 | 13.511293 | 13.843196 | 13.413556 | 14.550234 | 13.232554 |
hep-th/9701004 | Cornwall John | John M. Cornwall (UCLA) | Large-Order Perturbation Theory in Infrared-Unstable Superrenormalizable
Field Theories | 28 pages, Latex, three .eps figures | Phys.Rev. D55 (1997) 6209-6217 | 10.1103/PhysRevD.55.6209 | UCLA/96/TEP/36 | hep-th | null | We study the factorial divergences of Euclidean $\phi^3_5$, a problem with
connections both to high-energy multiparticle scattering in d=4 and to d=3 (or
high-temperature) gauge theory, which like $\phi^3_5$ is infrared-unstable and
superrenormalizable. At large external momentum p (or small mass M) and large
order N... | [
{
"created": "Thu, 2 Jan 1997 18:43:54 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Cornwall",
"John M.",
"",
"UCLA"
]
] | We study the factorial divergences of Euclidean $\phi^3_5$, a problem with connections both to high-energy multiparticle scattering in d=4 and to d=3 (or high-temperature) gauge theory, which like $\phi^3_5$ is infrared-unstable and superrenormalizable. At large external momentum p (or small mass M) and large order N o... | 11.970798 | 14.138912 | 12.992045 | 12.170307 | 13.829338 | 13.395119 | 13.315839 | 12.679172 | 12.134238 | 13.480562 | 12.434118 | 12.226455 | 12.184966 | 11.830921 | 12.326377 | 11.933734 | 11.962309 | 12.077725 | 12.104837 | 12.568345 | 12.182596 |
2203.04973 | Pratik Rath | Xi Dong, Donald Marolf, Pratik Rath, Amirhossein Tajdini and Zhencheng
Wang | The Spacetime Geometry of Fixed-Area States in Gravitational Systems | 32 pages, 7 figures | null | 10.1007/JHEP08(2022)158 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The concept of fixed-area states has proven useful for recent studies of
quantum gravity, especially in connection with gravitational holography. We
explore the Lorentz-signature spacetime geometry intrinsic to such fixed-area
states in this paper. This contrasts with previous treatments which focused
instead on Eucl... | [
{
"created": "Wed, 9 Mar 2022 19:00:00 GMT",
"version": "v1"
}
] | 2022-09-07 | [
[
"Dong",
"Xi",
""
],
[
"Marolf",
"Donald",
""
],
[
"Rath",
"Pratik",
""
],
[
"Tajdini",
"Amirhossein",
""
],
[
"Wang",
"Zhencheng",
""
]
] | The concept of fixed-area states has proven useful for recent studies of quantum gravity, especially in connection with gravitational holography. We explore the Lorentz-signature spacetime geometry intrinsic to such fixed-area states in this paper. This contrasts with previous treatments which focused instead on Euclid... | 12.914412 | 12.212698 | 13.252189 | 11.526784 | 11.903241 | 12.248179 | 13.14864 | 11.18632 | 12.015282 | 13.629155 | 11.865264 | 11.676062 | 12.461823 | 11.781658 | 12.009283 | 11.903553 | 11.909154 | 11.532573 | 11.950279 | 12.232902 | 11.922168 |
2207.12963 | Podist Kurashvili | Podist Kurashvili, Levan Chotorlishvili | Quantum discord and entropic measures of two relativistic fermions | 18 pages, 10 figures | null | 10.1088/1751-8121/aca7a0 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present work, we study the interplay between relativistic effects and
quantumness in the system of two relativistic fermions. In particular, we
explore entropic measures of quantum correlations and quantum discord before
and after application of a boost and subsequent Wigner rotation. We also study
the positiv... | [
{
"created": "Tue, 26 Jul 2022 15:16:16 GMT",
"version": "v1"
}
] | 2022-12-21 | [
[
"Kurashvili",
"Podist",
""
],
[
"Chotorlishvili",
"Levan",
""
]
] | In the present work, we study the interplay between relativistic effects and quantumness in the system of two relativistic fermions. In particular, we explore entropic measures of quantum correlations and quantum discord before and after application of a boost and subsequent Wigner rotation. We also study the positive ... | 11.439067 | 13.128626 | 12.102609 | 11.916593 | 13.014764 | 13.34046 | 12.702371 | 12.365231 | 11.746652 | 12.662541 | 11.563839 | 11.939779 | 11.330132 | 11.311731 | 11.234353 | 11.645386 | 11.609801 | 11.407028 | 11.196087 | 11.442329 | 11.412689 |
hep-th/9203050 | Robert Mann | Dan Christensen and Robert B. Mann | The Causal Structure of Two-Dimensional Spacetimes | 27 pgs., 5 figures (unavailable) | Class.Quant.Grav.9:1769-1786,1992 | 10.1088/0264-9381/9/7/010 | null | hep-th | null | We investigate the causal structure of $(1+1)$-dimensional spacetimes. For
two sets of field equations we show that at least locally any spacetime is a
solution for an appropriate choice of the matter fields. For the theories under
consideration we investigate how smoothness of their black hole solutions
affects time... | [
{
"created": "Wed, 18 Mar 1992 15:08:18 GMT",
"version": "v1"
}
] | 2010-04-06 | [
[
"Christensen",
"Dan",
""
],
[
"Mann",
"Robert B.",
""
]
] | We investigate the causal structure of $(1+1)$-dimensional spacetimes. For two sets of field equations we show that at least locally any spacetime is a solution for an appropriate choice of the matter fields. For the theories under consideration we investigate how smoothness of their black hole solutions affects time o... | 8.919978 | 9.728277 | 8.222985 | 8.599936 | 8.69055 | 8.96457 | 9.672664 | 8.362045 | 9.410039 | 9.345561 | 8.655867 | 8.670862 | 8.553872 | 8.435272 | 8.587945 | 8.678495 | 8.69084 | 8.688696 | 8.649708 | 8.523602 | 8.513826 |
1102.0232 | Edmond Iancu | Y. Hatta, E. Iancu, A.H. Mueller, D.N. Triantafyllopoulos | Radiation by a heavy quark in N=4 SYM at strong coupling | 22 pages | null | 10.1016/j.nuclphysb.2011.04.011 | CERN-PH-TH-2011-021 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the AdS/CFT correspondence in the supergravity approximation, we
compute the energy density radiated by a heavy quark undergoing some arbitrary
motion in the vacuum of the strongly coupled N=4 supersymmetric Yang-Mills
theory. We find that this energy is fully generated via backreaction from the
near-boundary e... | [
{
"created": "Tue, 1 Feb 2011 17:42:48 GMT",
"version": "v1"
}
] | 2015-05-27 | [
[
"Hatta",
"Y.",
""
],
[
"Iancu",
"E.",
""
],
[
"Mueller",
"A. H.",
""
],
[
"Triantafyllopoulos",
"D. N.",
""
]
] | Using the AdS/CFT correspondence in the supergravity approximation, we compute the energy density radiated by a heavy quark undergoing some arbitrary motion in the vacuum of the strongly coupled N=4 supersymmetric Yang-Mills theory. We find that this energy is fully generated via backreaction from the near-boundary end... | 6.823239 | 7.270798 | 8.176766 | 7.101514 | 6.948525 | 7.330612 | 7.274147 | 7.485875 | 6.795525 | 8.976813 | 7.114802 | 6.631844 | 6.934889 | 6.780461 | 6.792912 | 6.90044 | 6.780122 | 6.677615 | 6.754977 | 7.00461 | 6.805805 |
1012.5725 | Hideki Ishihara | Takahisa Igata, Hideki Ishihara, and Yohsuke Takamori | Chaos in Geodesic Motion around a Black Ring | 6 pages, 6 figures | Phys.Rev.D83:047501,2011 | 10.1103/PhysRevD.83.047501 | OCU-PHYS 343, AP-GR 87 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study bound orbits of a free particle around a singly rotating black ring.
We find there exists chaotic motion of a particle which is gravitationally
bound to the black ring by using the Poincare map.
| [
{
"created": "Tue, 28 Dec 2010 09:10:40 GMT",
"version": "v1"
}
] | 2011-02-15 | [
[
"Igata",
"Takahisa",
""
],
[
"Ishihara",
"Hideki",
""
],
[
"Takamori",
"Yohsuke",
""
]
] | We study bound orbits of a free particle around a singly rotating black ring. We find there exists chaotic motion of a particle which is gravitationally bound to the black ring by using the Poincare map. | 17.752647 | 12.473992 | 12.401705 | 11.920428 | 13.526071 | 11.279764 | 11.632128 | 8.810169 | 11.900352 | 12.543614 | 11.472528 | 13.597244 | 13.910806 | 12.475414 | 13.160972 | 13.122549 | 13.924091 | 12.642297 | 13.756222 | 12.789824 | 13.78264 |
hep-th/9404098 | null | E. Ivanov and A. Sutulin | Sigma Models in (4,4) Harmonic Superspace | 33 p, BONN-TH-94-02 | Nucl.Phys. B432 (1994) 246-280; Erratum-ibid. B483 (1997) 531 | 10.1016/0550-3213(94)90602-5 | null | hep-th | null | We define basics of $(4,4)\;\; 2D$ harmonic superspace with two independent
sets of $SU(2)$ harmonic variables and apply it to construct new superfield
actions of $(4,4)$ supersymmetric two-dimensional sigma models with torsion and
mutually commuting left and right complex structures, as well as of their
massive defo... | [
{
"created": "Fri, 15 Apr 1994 22:30:05 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ivanov",
"E.",
""
],
[
"Sutulin",
"A.",
""
]
] | We define basics of $(4,4)\;\; 2D$ harmonic superspace with two independent sets of $SU(2)$ harmonic variables and apply it to construct new superfield actions of $(4,4)$ supersymmetric two-dimensional sigma models with torsion and mutually commuting left and right complex structures, as well as of their massive deform... | 8.348849 | 8.160276 | 9.54989 | 7.961811 | 8.200682 | 8.178971 | 7.673824 | 7.77675 | 7.716317 | 10.851937 | 8.046775 | 8.1004 | 8.400762 | 7.819285 | 7.98036 | 7.898104 | 7.864726 | 7.865649 | 8.157609 | 8.299109 | 7.857343 |
1010.4803 | John Kehayias | Michael Dine, Guido Festuccia, John Kehayias and Weitao Wu | Axions in the Landscape and String Theory | 18 pages; v2, updated and added references | JHEP 1101:012,2011 | 10.1007/JHEP01(2011)012 | SCIPP 10/07 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | While axions seem ubiquitous in critical string theories, whether they might
survive in any string theoretic description of nature is a difficult question.
With some mild assumptions, one can frame the issues in the case that there is
an approximate supersymmetry below the underlying string scale. The problem of
axio... | [
{
"created": "Fri, 22 Oct 2010 20:01:28 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Nov 2010 17:30:53 GMT",
"version": "v2"
}
] | 2011-01-27 | [
[
"Dine",
"Michael",
""
],
[
"Festuccia",
"Guido",
""
],
[
"Kehayias",
"John",
""
],
[
"Wu",
"Weitao",
""
]
] | While axions seem ubiquitous in critical string theories, whether they might survive in any string theoretic description of nature is a difficult question. With some mild assumptions, one can frame the issues in the case that there is an approximate supersymmetry below the underlying string scale. The problem of axions... | 10.314191 | 10.702462 | 11.285624 | 10.176865 | 11.820787 | 12.00731 | 12.403775 | 11.319039 | 10.23689 | 11.468961 | 10.765973 | 10.422946 | 10.626601 | 10.279853 | 10.746403 | 10.656563 | 10.808336 | 10.576921 | 10.508869 | 10.725376 | 10.675571 |
1205.7072 | Frans Klinkhamer | F. R. Klinkhamer | On vacuum-energy decay from particle production | 10 pages, v6: published version with Note Added in Proof | Mod. Phys. Lett. A 27, 1250150 (2012) | 10.1142/S0217732312501507 | KA-TP-23-2012 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A simplified (but consistent) description of particle-production backreaction
effects in de Sitter spacetime is given.
| [
{
"created": "Thu, 31 May 2012 18:53:34 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jun 2012 17:47:35 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Jun 2012 17:28:11 GMT",
"version": "v3"
},
{
"created": "Mon, 18 Jun 2012 18:11:35 GMT",
"version": "v4"
},
{
"cr... | 2012-08-03 | [
[
"Klinkhamer",
"F. R.",
""
]
] | A simplified (but consistent) description of particle-production backreaction effects in de Sitter spacetime is given. | 40.587456 | 20.384237 | 26.508492 | 23.035629 | 21.855101 | 21.706875 | 20.030933 | 19.811892 | 21.660421 | 27.759222 | 19.440289 | 22.904079 | 25.179625 | 24.273075 | 22.581232 | 21.209856 | 23.10313 | 20.015886 | 25.450426 | 23.639906 | 21.356861 |
hep-th/9905211 | Ruth Britto-Pacumio | Ruth Britto-Pacumio, Andrew Strominger and Anastasia Volovich | Holography for Coset Spaces | Harvmac, 23 pages. Additions/correction to section 3.2 | JHEP 9911:013,1999 | 10.1088/1126-6708/1999/11/013 | HUTP-99/A023 | hep-th | null | M/string theory on noncompact, negatively curved, cosets which generalize
$AdS_{D+1}=SO(D,2)/SO(D,1)$ is considered. Holographic descriptions in terms of
a conformal field theory on the boundary of the spacetime are proposed.
Examples include $SU(2,1)/U(2)$, which is a Euclidean signature (4,0) space
with no supersym... | [
{
"created": "Thu, 27 May 1999 19:18:17 GMT",
"version": "v1"
},
{
"created": "Mon, 31 May 1999 18:48:02 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Britto-Pacumio",
"Ruth",
""
],
[
"Strominger",
"Andrew",
""
],
[
"Volovich",
"Anastasia",
""
]
] | M/string theory on noncompact, negatively curved, cosets which generalize $AdS_{D+1}=SO(D,2)/SO(D,1)$ is considered. Holographic descriptions in terms of a conformal field theory on the boundary of the spacetime are proposed. Examples include $SU(2,1)/U(2)$, which is a Euclidean signature (4,0) space with no supersymme... | 5.67392 | 4.917557 | 5.659539 | 4.651103 | 4.933666 | 4.709615 | 5.105291 | 4.727026 | 4.979829 | 6.50106 | 4.980044 | 4.914449 | 5.012167 | 4.657352 | 4.851166 | 4.947457 | 4.894028 | 4.721904 | 4.772815 | 5.080474 | 4.882854 |
hep-th/9804065 | Harald Dorn | H. Dorn | The mass term in non-Abelian gauge field dynamics on matrix D-branes and
T-duality in the $\sigma$-model approach | 13 pages, Latex, some typos corrected | JHEP 9804:013,1998 | 10.1088/1126-6708/1998/04/013 | HU Berlin-EP-98/21 | hep-th | null | The formal extension of the T-duality rules for open strings from Abelian to
non-Abelian gauge field background leads in a well known manner to the notion
of matrix valued D-brane position. The application of this concept to the
non-Abelian gauge field RG $\beta $-function of the corresponding $\sigma
$-model yields ... | [
{
"created": "Wed, 8 Apr 1998 12:17:13 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Apr 1998 09:33:13 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Dorn",
"H.",
""
]
] | The formal extension of the T-duality rules for open strings from Abelian to non-Abelian gauge field background leads in a well known manner to the notion of matrix valued D-brane position. The application of this concept to the non-Abelian gauge field RG $\beta $-function of the corresponding $\sigma $-model yields a ... | 11.784668 | 11.363845 | 11.517232 | 11.054615 | 11.859325 | 12.056643 | 11.109005 | 11.065139 | 10.666738 | 12.508959 | 11.315028 | 10.852596 | 10.850106 | 10.386001 | 10.313561 | 10.436212 | 10.51602 | 10.357996 | 11.058657 | 11.006826 | 10.88035 |
hep-th/9407150 | P. K. Ghosh | Pijush K. Ghosh, Avinash Khare and Prasanta K. Panigrahi | $B \wedge F$ Term by Spontaneous Symmetry Breaking in a generalized
Abelian Higgs Model | 7 pages, RevTeX, IP/BBSR/94-20 | J.Phys. G21 (1995) 1303-1306 | 10.1088/0954-3899/21/10/003 | null | hep-th | null | We show that the topological $B \wedge F$ term in $3+1$ dimensions can be
generated via spontaneous symmetry breaking in a generalized Abelian Higgs
model. Further, we also show that even in $D$ dimensions $ ( D \geq 3 ) $, a $B
\wedge F$ term gives rise to the topological massive excitations of the Abelian
gauge fie... | [
{
"created": "Fri, 22 Jul 1994 18:41:29 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ghosh",
"Pijush K.",
""
],
[
"Khare",
"Avinash",
""
],
[
"Panigrahi",
"Prasanta K.",
""
]
] | We show that the topological $B \wedge F$ term in $3+1$ dimensions can be generated via spontaneous symmetry breaking in a generalized Abelian Higgs model. Further, we also show that even in $D$ dimensions $ ( D \geq 3 ) $, a $B \wedge F$ term gives rise to the topological massive excitations of the Abelian gauge field... | 6.313934 | 4.736533 | 5.467831 | 4.77021 | 4.900452 | 4.799055 | 4.719386 | 4.791216 | 4.799636 | 5.588067 | 4.80551 | 4.969104 | 5.656703 | 5.001275 | 5.037883 | 4.906131 | 4.9226 | 4.797139 | 5.039664 | 5.808899 | 5.133175 |
0805.1461 | Michael Kuchiev | Michael Yu. Kuchiev | Charges of dyons in N=2 supersymmetric gauge theory | 31 pages | Nucl.Phys.B803:113-134,2008 | 10.1016/j.nuclphysb.2008.05.022 | null | hep-th | http://creativecommons.org/licenses/by-nc-sa/3.0/ | Expressions for electric and magnetic charges of dyons, which become massless
in the strong-coupling limit of the supersymmetric N=2 gauge theory with an
arbitrary gauge group are presented. Transitions into different vacua of the N
=1 gauge theory, when the N=2 supersymmetry is broken explicitly to the N =1
case, ar... | [
{
"created": "Sat, 10 May 2008 10:26:42 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kuchiev",
"Michael Yu.",
""
]
] | Expressions for electric and magnetic charges of dyons, which become massless in the strong-coupling limit of the supersymmetric N=2 gauge theory with an arbitrary gauge group are presented. Transitions into different vacua of the N =1 gauge theory, when the N=2 supersymmetry is broken explicitly to the N =1 case, are ... | 8.066896 | 8.489211 | 8.292251 | 7.690833 | 8.180301 | 8.3585 | 7.767375 | 7.619247 | 7.541831 | 8.651987 | 7.584606 | 7.552883 | 7.970247 | 7.357118 | 7.540991 | 7.668555 | 7.525069 | 7.557818 | 7.837203 | 8.07964 | 7.679085 |
1301.1803 | Antal Jakovac | A. Jakovac, P. Mati | Spectral function of the Bloch-Nordsieck model at finite temperature | 16 pages, 9 figures, revtex4-1 | null | 10.1103/PhysRevD.87.125007 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we determine the exact fermionic spectral function of the
Bloch-Nordsieck model at finite temperature. Analytic results are presented for
some special parameters, for other values we have numerical results. The
spectral function is finite and normalizable for any nonzero temperature
values. The real tim... | [
{
"created": "Wed, 9 Jan 2013 10:36:14 GMT",
"version": "v1"
}
] | 2013-06-12 | [
[
"Jakovac",
"A.",
""
],
[
"Mati",
"P.",
""
]
] | In this paper we determine the exact fermionic spectral function of the Bloch-Nordsieck model at finite temperature. Analytic results are presented for some special parameters, for other values we have numerical results. The spectral function is finite and normalizable for any nonzero temperature values. The real time ... | 11.838237 | 10.726286 | 9.841221 | 9.476168 | 9.91303 | 10.084317 | 10.136486 | 10.779642 | 9.582226 | 10.080335 | 10.706786 | 9.804907 | 10.436258 | 9.753896 | 9.824303 | 10.302541 | 10.25631 | 10.328582 | 9.897617 | 10.595819 | 10.22351 |
2202.01239 | Ling-Xiao Xu | Andrea Luzio, Ling-Xiao Xu | On the Derivation of Chiral Symmetry Breaking in QCD-like Theories and
S-confining Theories | 24 pages+appendix; v2: references added, minor revision, conclusion
unchanged | null | 10.1007/JHEP08(2022)016 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Recent works argue that the pattern of chiral symmetry breaking in QCD-like
theories can be derived from supersymmetric (SUSY) QCD with perturbation of
anomaly-mediated SUSY breaking (AMSB). Nevertheless, despite the fact that AMSB
needs to be a small (but still exact) perturbation, there are two other major
problems... | [
{
"created": "Wed, 2 Feb 2022 19:00:09 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Jun 2022 10:43:21 GMT",
"version": "v2"
}
] | 2022-08-24 | [
[
"Luzio",
"Andrea",
""
],
[
"Xu",
"Ling-Xiao",
""
]
] | Recent works argue that the pattern of chiral symmetry breaking in QCD-like theories can be derived from supersymmetric (SUSY) QCD with perturbation of anomaly-mediated SUSY breaking (AMSB). Nevertheless, despite the fact that AMSB needs to be a small (but still exact) perturbation, there are two other major problems r... | 9.650359 | 9.319105 | 9.371964 | 8.91496 | 9.983059 | 9.907486 | 9.561052 | 9.470937 | 8.668869 | 9.843211 | 9.35814 | 9.13711 | 9.452965 | 9.117184 | 9.340622 | 9.382514 | 9.215048 | 9.310738 | 9.285567 | 9.560059 | 9.09516 |
hep-th/0203235 | Edi Halyo | Edi Halyo | Holographic Inflation | 19 pages in phyzzx.tex | JHEP 0402:062,2004 | 10.1088/1126-6708/2004/02/062 | null | hep-th | null | Using the de Sitter/CFT correspondence we describe a scenario of holographic
inflation which is driven by a three dimensional boundary field theory. We find
that inflationary constraints severely restrict the $\beta$--function, the
anomalous dimensions and the value of the $C$--function of the boundary theory.
The sc... | [
{
"created": "Tue, 26 Mar 2002 17:45:02 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Halyo",
"Edi",
""
]
] | Using the de Sitter/CFT correspondence we describe a scenario of holographic inflation which is driven by a three dimensional boundary field theory. We find that inflationary constraints severely restrict the $\beta$--function, the anomalous dimensions and the value of the $C$--function of the boundary theory. The scen... | 8.779696 | 9.102233 | 8.397612 | 8.55361 | 9.256887 | 8.924513 | 9.054323 | 8.268354 | 8.488956 | 9.38773 | 8.574641 | 8.770006 | 8.679819 | 8.406838 | 8.816073 | 8.873438 | 8.796946 | 8.639988 | 8.935624 | 8.611561 | 8.640416 |
1903.02807 | Christian Saemann | Branislav Jurco, Christian Saemann, Urs Schreiber, Martin Wolf | Higher Structures in M-Theory | 22 pages, Introductory Article to Proceedings of LMS/EPSRC Durham
Symposium Higher Structures in M-Theory, August 2018, references updated | null | 10.1002/prop.201910001 | DMUS-MP-19-02, EMPG-19-06 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The key open problem of string theory remains its non-perturbative completion
to M-theory. A decisive hint to its inner workings comes from numerous
appearances of higher structures in the limits of M-theory that are already
understood, such as higher degree flux fields and their dualities, or the
higher algebraic st... | [
{
"created": "Thu, 7 Mar 2019 10:14:01 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Mar 2019 21:13:02 GMT",
"version": "v2"
}
] | 2021-07-28 | [
[
"Jurco",
"Branislav",
""
],
[
"Saemann",
"Christian",
""
],
[
"Schreiber",
"Urs",
""
],
[
"Wolf",
"Martin",
""
]
] | The key open problem of string theory remains its non-perturbative completion to M-theory. A decisive hint to its inner workings comes from numerous appearances of higher structures in the limits of M-theory that are already understood, such as higher degree flux fields and their dualities, or the higher algebraic stru... | 9.613612 | 10.11877 | 11.99192 | 9.406005 | 10.357596 | 10.320134 | 9.903605 | 9.462798 | 9.711316 | 11.613994 | 9.378264 | 8.941253 | 9.850752 | 9.230163 | 9.148268 | 8.746707 | 8.965954 | 8.89722 | 9.177024 | 9.638042 | 8.956141 |
hep-th/9907163 | Tim Prestidge | Tim Prestidge | Dynamic and Thermodynamic Stability and Negative Modes in
Schwarzschild-Anti-de Sitter | 21 pages, 5 figures, LaTeX | Phys.Rev. D61 (2000) 084002 | 10.1103/PhysRevD.61.084002 | DAMTP-1999-89 | hep-th | null | The thermodynamic properties of Schwarzschild-anti-de Sitter black holes
confined within finite isothermal cavities are examined. In contrast to the
Schwarzschild case, the infinite cavity limit may be taken which, if suitably
stated, remains double valued. This allows the correspondence between
non-existence of nega... | [
{
"created": "Tue, 20 Jul 1999 13:49:35 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Prestidge",
"Tim",
""
]
] | The thermodynamic properties of Schwarzschild-anti-de Sitter black holes confined within finite isothermal cavities are examined. In contrast to the Schwarzschild case, the infinite cavity limit may be taken which, if suitably stated, remains double valued. This allows the correspondence between non-existence of negati... | 10.07031 | 9.680418 | 9.353202 | 9.198935 | 9.382363 | 10.210461 | 9.283898 | 9.334413 | 9.095518 | 9.327753 | 9.259131 | 9.720679 | 9.685493 | 9.058 | 9.313813 | 9.46542 | 9.585568 | 9.25782 | 9.312655 | 9.520266 | 9.092125 |
1810.03612 | Carlo Meneghelli | Federico Bonetti, Carlo Meneghelli, Leonardo Rastelli | VOAs labelled by complex reflection groups and 4d SCFTs | 70 pages | null | 10.1007/JHEP05(2019)155 | null | hep-th math.QA math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define and study a class of $\mathcal{N}=2$ vertex operator algebras
$\mathcal{W}_{\mathcal{\mathsf{G}}}$ labelled by complex reflection groups.
They are extensions of the $\mathcal{N}=2$ super Virasoro algebra obtained by
introducing additional generators, in correspondence with the invariants of the
complex refl... | [
{
"created": "Mon, 8 Oct 2018 18:00:00 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Mar 2019 15:55:34 GMT",
"version": "v2"
}
] | 2019-06-26 | [
[
"Bonetti",
"Federico",
""
],
[
"Meneghelli",
"Carlo",
""
],
[
"Rastelli",
"Leonardo",
""
]
] | We define and study a class of $\mathcal{N}=2$ vertex operator algebras $\mathcal{W}_{\mathcal{\mathsf{G}}}$ labelled by complex reflection groups. They are extensions of the $\mathcal{N}=2$ super Virasoro algebra obtained by introducing additional generators, in correspondence with the invariants of the complex reflec... | 3.539513 | 3.54181 | 3.834188 | 3.52333 | 3.610751 | 3.585507 | 3.557545 | 3.445379 | 3.482158 | 4.016765 | 3.508168 | 3.356565 | 3.535245 | 3.37376 | 3.376224 | 3.393922 | 3.388507 | 3.368502 | 3.367735 | 3.423586 | 3.390934 |
0711.3986 | Dan Radu Grigore | D. R. Grigore | Cohomological Aspects of Gauge Invariance in the Causal Approach | 57 pages, no figures | Rom.J.Phys.55:386-438,2010 | null | null | hep-th | null | Quantum theory of the gauge models in the causal approach leads to some
cohomology problems. We investigate these problems in detail.
| [
{
"created": "Mon, 26 Nov 2007 12:31:35 GMT",
"version": "v1"
}
] | 2011-03-17 | [
[
"Grigore",
"D. R.",
""
]
] | Quantum theory of the gauge models in the causal approach leads to some cohomology problems. We investigate these problems in detail. | 36.530479 | 18.864109 | 26.572117 | 19.54142 | 19.75617 | 20.398808 | 22.448492 | 19.250967 | 19.248138 | 23.981749 | 21.902073 | 24.054308 | 25.585758 | 24.114042 | 22.570137 | 22.873083 | 22.655256 | 22.528618 | 24.663246 | 27.892403 | 22.386082 |
hep-th/0306242 | Romuald A. Janik | Jan Ambjorn, Romuald A. Janik | Towards a diagrammatic derivation of the Veneziano-Yankielowicz-Taylor
superpotential | 8 pages, 2 figures | Phys.Lett. B569 (2003) 81-84 | 10.1016/j.physletb.2003.07.018 | null | hep-th | null | We show how it is possible to integrate out chiral matter fields in N=1
supersymmetric theories and in this way derive in a simple diagrammatic way the
$N_f S \log S - S \log \det X$ part of the Veneziano-Yankielowicz-Taylor
superpotential.
| [
{
"created": "Wed, 25 Jun 2003 10:29:30 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Ambjorn",
"Jan",
""
],
[
"Janik",
"Romuald A.",
""
]
] | We show how it is possible to integrate out chiral matter fields in N=1 supersymmetric theories and in this way derive in a simple diagrammatic way the $N_f S \log S - S \log \det X$ part of the Veneziano-Yankielowicz-Taylor superpotential. | 15.132895 | 11.420929 | 15.694142 | 10.410572 | 11.451311 | 10.974946 | 11.740065 | 11.247643 | 12.350773 | 18.003027 | 11.863615 | 12.590935 | 12.229501 | 11.555797 | 12.280766 | 11.560076 | 11.430146 | 11.65595 | 12.248331 | 13.846298 | 12.013965 |
hep-th/0609213 | Angel M. Uranga | L. E. Ibanez, A. M. Uranga | Neutrino Majorana Masses from String Theory Instanton Effects | 40 pages, 4 figures (v2: added references, small corrections)(v3:
minor corrections) | JHEP 0703:052,2007 | 10.1088/1126-6708/2007/03/052 | IFT-UAM/CSIC-06-45, CERN-PH-TH/2006-199 | hep-th hep-ph | null | Finding a plausible origin for right-handed neutrino Majorana masses in
semirealistic compactifications of string theory remains one of the most
difficult problems in string phenomenology. We argue that right-handed neutrino
Majorana masses are induced by non-perturbative instanton effects in certain
classes of strin... | [
{
"created": "Thu, 28 Sep 2006 18:59:28 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Oct 2006 13:23:15 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Feb 2007 11:09:25 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Ibanez",
"L. E.",
""
],
[
"Uranga",
"A. M.",
""
]
] | Finding a plausible origin for right-handed neutrino Majorana masses in semirealistic compactifications of string theory remains one of the most difficult problems in string phenomenology. We argue that right-handed neutrino Majorana masses are induced by non-perturbative instanton effects in certain classes of string ... | 7.156908 | 7.60966 | 7.57861 | 7.161134 | 8.312103 | 7.752548 | 8.095643 | 7.870918 | 6.955852 | 7.628681 | 7.129421 | 6.787532 | 7.283723 | 6.972424 | 7.003548 | 6.720442 | 6.82938 | 6.921143 | 6.917722 | 7.078098 | 6.829253 |
2204.02425 | Andrei Linde | Renata Kallosh and Andrei Linde | Hybrid cosmological attractors | 28 pages, 6 figures We expanded a discussion of the problem of
topological defects, of its possible resolution, and of the implementation of
this scenario in supergravity | null | 10.1103/PhysRevD.106.023522 | null | hep-th astro-ph.CO gr-qc | http://creativecommons.org/licenses/by/4.0/ | We construct $\alpha$-attractor versions of hybrid inflation models. In these
models, the potential of the inflaton field $\varphi$ is uplifted by the
potential of the second field $\chi$. This uplifting ends due to a tachyonic
instability with respect to the field $\chi$, which appears when $\varphi$
becomes smaller... | [
{
"created": "Tue, 5 Apr 2022 18:03:50 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jun 2022 22:22:34 GMT",
"version": "v2"
}
] | 2022-08-31 | [
[
"Kallosh",
"Renata",
""
],
[
"Linde",
"Andrei",
""
]
] | We construct $\alpha$-attractor versions of hybrid inflation models. In these models, the potential of the inflaton field $\varphi$ is uplifted by the potential of the second field $\chi$. This uplifting ends due to a tachyonic instability with respect to the field $\chi$, which appears when $\varphi$ becomes smaller t... | 6.293666 | 6.389308 | 6.200203 | 6.188572 | 6.551715 | 6.310725 | 6.368262 | 6.198362 | 6.303451 | 6.43501 | 6.105656 | 5.949293 | 5.874501 | 5.995651 | 5.873787 | 6.14895 | 6.074769 | 6.10219 | 5.910617 | 6.24566 | 5.862278 |
hep-th/9803027 | Oleg Lunin | Francesco Antonuccio, Oleg Lunin, Stephen S. Pinsky (Ohio State
University) | Bound States of Dimensionally Reduced {SYM}_{2+1} at Finite N | 14 pages, REVTEX | Phys.Lett. B429 (1998) 327-335 | 10.1016/S0370-2693(98)00432-8 | OHSTPY-HEP-TH-98-004 | hep-th | null | We consider the dimensional reduction of N=1 {SYM}_{2+1} to 1+1 dimensions.
The gauge groups we consider are U(N) and SU(N), where N is finite. We
formulate the continuum bound state problem in the light-cone formalism, and
show that any normalizable SU(N) bound state must be a superposition of an
infinite number of ... | [
{
"created": "Tue, 3 Mar 1998 22:13:14 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Antonuccio",
"Francesco",
"",
"Ohio State\n University"
],
[
"Lunin",
"Oleg",
"",
"Ohio State\n University"
],
[
"Pinsky",
"Stephen S.",
"",
"Ohio State\n University"
]
] | We consider the dimensional reduction of N=1 {SYM}_{2+1} to 1+1 dimensions. The gauge groups we consider are U(N) and SU(N), where N is finite. We formulate the continuum bound state problem in the light-cone formalism, and show that any normalizable SU(N) bound state must be a superposition of an infinite number of Fo... | 10.615308 | 8.45948 | 9.872331 | 8.342727 | 9.207397 | 10.079037 | 9.186776 | 8.577808 | 8.934607 | 10.291261 | 8.613289 | 9.636507 | 9.485194 | 9.254786 | 9.149619 | 9.41825 | 9.119734 | 9.052291 | 9.323482 | 9.733135 | 9.425706 |
hep-th/9801057 | Ron Donagi | Gottfried Curio and Ron Y. Donagi | Moduli in N=1 heterotic/F-theory duality | Latex, 26 pages. Acknowledgements added | Nucl.Phys. B518 (1998) 603-631 | 10.1016/S0550-3213(98)00185-0 | IASSNS-HEP-97/139 | hep-th math.AG | null | The moduli in a 4D N=1 heterotic compactification on an elliptic CY, as well
as in the dual F-theoretic compactification, break into "base" parameters which
are even (under the natural involution of the elliptic curves), and "fiber" or
twisting parameters; the latter include a continuous part which is odd, as well
as... | [
{
"created": "Mon, 12 Jan 1998 20:28:50 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Jan 1998 00:14:31 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Curio",
"Gottfried",
""
],
[
"Donagi",
"Ron Y.",
""
]
] | The moduli in a 4D N=1 heterotic compactification on an elliptic CY, as well as in the dual F-theoretic compactification, break into "base" parameters which are even (under the natural involution of the elliptic curves), and "fiber" or twisting parameters; the latter include a continuous part which is odd, as well as a... | 10.003374 | 11.16493 | 12.71694 | 10.486582 | 10.279983 | 10.42067 | 9.505753 | 9.824626 | 9.594966 | 12.030406 | 9.902511 | 9.700116 | 10.602767 | 9.816143 | 9.589047 | 9.848465 | 9.895267 | 9.599036 | 9.747489 | 10.85659 | 9.709339 |
hep-th/0503196 | Maria A. Lledo | L. Andrianopoli, S. Ferrara, M. A. Lledo, O. Macia | Integration of massive states as contractions of non linear
$\sigma$-models | AMS-LaTeX, 33 pages | J.Math.Phys. 46 (2005) 072307 | 10.1063/1.1960719 | CERN-PH-TH/2005-049, FTUV-05/0325 | hep-th | null | We consider the contraction of some non linear sigma models which appear in
effective supergravity theories. In particular we consider the contractions of
maximally symmetric spaces corresponding to N=1 and N=2 theories, as they
appear in certain low energy effective supergravity actions with mass
deformations.
The... | [
{
"created": "Thu, 24 Mar 2005 23:13:04 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Andrianopoli",
"L.",
""
],
[
"Ferrara",
"S.",
""
],
[
"Lledo",
"M. A.",
""
],
[
"Macia",
"O.",
""
]
] | We consider the contraction of some non linear sigma models which appear in effective supergravity theories. In particular we consider the contractions of maximally symmetric spaces corresponding to N=1 and N=2 theories, as they appear in certain low energy effective supergravity actions with mass deformations. The con... | 11.591545 | 10.052214 | 11.20534 | 10.72455 | 10.065008 | 10.188757 | 9.541744 | 9.599623 | 10.706495 | 10.97681 | 10.0299 | 10.142605 | 10.721411 | 10.598745 | 9.877947 | 9.979194 | 9.927632 | 10.382071 | 10.051478 | 10.495365 | 10.097001 |
hep-th/9908006 | Takuhiro Kitao | Takuhiro Kitao and Nobuyoshi Ohta | Spectrum of Maxwell-Chern-Simons Theory Realized on Type IIB Brane | 30 pages, LaTex, four figures, typos corrected and final version | Nucl.Phys. B578 (2000) 215-238 | 10.1016/S0550-3213(99)00715-4 | UT-Komaba/99-11 and OU-HET 323 | hep-th | null | We study the 3D field theory on one D3-brane stretched between (r,s) and
(p,q)5-branes. The boundary conditions are determined from the analysis of NS5
and D5 charges of the two 5-branes. We carry out the mode expansions for all
the fields and identify the field theory as Maxwell-Chern-Simons theory. We
examine the m... | [
{
"created": "Mon, 2 Aug 1999 09:51:53 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Oct 1999 17:46:53 GMT",
"version": "v2"
},
{
"created": "Tue, 16 Nov 1999 12:58:42 GMT",
"version": "v3"
},
{
"created": "Sat, 18 Dec 1999 05:02:31 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Kitao",
"Takuhiro",
""
],
[
"Ohta",
"Nobuyoshi",
""
]
] | We study the 3D field theory on one D3-brane stretched between (r,s) and (p,q)5-branes. The boundary conditions are determined from the analysis of NS5 and D5 charges of the two 5-branes. We carry out the mode expansions for all the fields and identify the field theory as Maxwell-Chern-Simons theory. We examine the mas... | 9.212669 | 8.734939 | 9.429047 | 8.335484 | 9.628458 | 9.594487 | 9.263395 | 8.943912 | 8.728816 | 10.442979 | 8.406776 | 8.852941 | 9.178783 | 8.715568 | 8.602068 | 8.858089 | 8.869598 | 8.715885 | 8.868381 | 9.241911 | 8.699566 |
1205.5754 | J\"urgen Struckmeier | J\"urgen Struckmeier and Hermine Reichau | General U(N) gauge transformations in the realm of covariant Hamiltonian
field theory | 36 pages, Symposium on Exciting Physics: Quarks and gluons/atomic
nuclei/biological systems/networks, Makutsi Safari Farm, South Africa, 13-20
November 2011; Exciting Interdisciplinary Physics, Walter Greiner, Ed., FIAS
Interdisciplinary Science Series, Springer International Publishing
Switzerland, 2013 | null | 10.1007/978-3-319-00047-3_31 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A consistent, local coordinate formulation of covariant Hamiltonian field
theory is presented. While the covariant canonical field equations are
equivalent to the Euler-Lagrange field equations, the covariant canonical
transformation theory offers more general means for defining mappings that
preserve the action func... | [
{
"created": "Thu, 24 May 2012 10:49:01 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Mar 2013 13:39:40 GMT",
"version": "v10"
},
{
"created": "Fri, 26 Apr 2013 16:28:45 GMT",
"version": "v11"
},
{
"created": "Fri, 3 May 2013 16:38:01 GMT",
"version": "v12"
},
{
... | 2018-05-10 | [
[
"Struckmeier",
"Jürgen",
""
],
[
"Reichau",
"Hermine",
""
]
] | A consistent, local coordinate formulation of covariant Hamiltonian field theory is presented. While the covariant canonical field equations are equivalent to the Euler-Lagrange field equations, the covariant canonical transformation theory offers more general means for defining mappings that preserve the action functi... | 9.809178 | 10.660913 | 10.16546 | 10.059967 | 11.145821 | 10.542593 | 10.718081 | 9.79359 | 9.589607 | 11.471849 | 9.61925 | 9.529315 | 9.512612 | 9.116458 | 9.361815 | 9.462152 | 9.823833 | 9.22808 | 9.168746 | 9.613191 | 9.341751 |
hep-th/9302049 | Martin Rocek | Amit Giveon and Martin Rocek | On the BRST Operator Structure of the N=2 String | 22 pages, Latex, NSF-ITP-93-17, ITP-SB-93-09, RIP-148-93 | Nucl.Phys. B400 (1993) 145-160 | 10.1016/0550-3213(93)90401-A | null | hep-th | null | The BRST operator cohomology of $N=2$ $2d$ supergravity coupled to matter is
presented. Descent equations for primary superfields of the matter sector are
derived. We find one copy of the cohomology at ghost number one, two
independent copies at ghost number two, and conjecture that there is a copy at
ghost number th... | [
{
"created": "Fri, 12 Feb 1993 21:04:09 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Giveon",
"Amit",
""
],
[
"Rocek",
"Martin",
""
]
] | The BRST operator cohomology of $N=2$ $2d$ supergravity coupled to matter is presented. Descent equations for primary superfields of the matter sector are derived. We find one copy of the cohomology at ghost number one, two independent copies at ghost number two, and conjecture that there is a copy at ghost number thre... | 7.395676 | 6.78275 | 8.149627 | 6.802644 | 7.091672 | 7.19601 | 6.656326 | 6.792091 | 6.99849 | 8.07541 | 6.699342 | 7.031333 | 8.080237 | 7.061041 | 6.974852 | 7.070741 | 6.820434 | 6.8272 | 7.076573 | 7.527005 | 7.021451 |
0906.0089 | Ariel Edery | A. Edery, N. Graham and I. MacDonald | 3D scalar model as a 4D perfect conductor limit: dimensional reduction
and variational boundary conditions | 14 pages, 2 figures | Phys.Rev.D79:125018,2009 | 10.1103/PhysRevD.79.125018 | NSF-KITP-09-37 | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Under dimensional reduction, a system in D spacetime dimensions will not
necessarily yield its D-1-dimensional analog version. Among other things, this
result will depend on the boundary conditions and the dimension D of the
system. We investigate this question for scalar and abelian gauge fields under
boundary condi... | [
{
"created": "Sat, 30 May 2009 15:19:23 GMT",
"version": "v1"
}
] | 2009-06-24 | [
[
"Edery",
"A.",
""
],
[
"Graham",
"N.",
""
],
[
"MacDonald",
"I.",
""
]
] | Under dimensional reduction, a system in D spacetime dimensions will not necessarily yield its D-1-dimensional analog version. Among other things, this result will depend on the boundary conditions and the dimension D of the system. We investigate this question for scalar and abelian gauge fields under boundary conditi... | 11.43475 | 11.942922 | 11.627431 | 11.236333 | 11.547 | 11.495102 | 12.120657 | 11.659858 | 11.150424 | 12.961611 | 11.542261 | 10.978407 | 10.700336 | 10.500286 | 10.742938 | 10.999478 | 11.016049 | 10.772881 | 10.800688 | 11.272552 | 10.830969 |
0907.1170 | Kazuo Ghoroku | Kazuo Ghoroku, Akihiro Nakamura and Fumihiko Toyoda | Stability of D brane Anti D brane Systems in Confining Gauge Theories | 19 pages, 7 figures | Eur.Phys.J.C71:1522,2011 | 10.1140/epjc/s10052-010-1522-0 | FIT-HE-09-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the stability of a special form of D brane embedding which is
regarded as a bound state of D$_n$ and anti-D$_n$-brane embedded in a 10D
supergravity background which is dual to a confining gauge theory. For D5
branes with $U(1)$ flux, their bound state configuration can be regarded as the
baryonium vertex. F... | [
{
"created": "Tue, 7 Jul 2009 09:26:20 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Sep 2009 01:06:38 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Oct 2009 01:13:11 GMT",
"version": "v3"
},
{
"created": "Thu, 15 Oct 2009 05:20:03 GMT",
"version": "v4"
},
{
"cre... | 2011-03-03 | [
[
"Ghoroku",
"Kazuo",
""
],
[
"Nakamura",
"Akihiro",
""
],
[
"Toyoda",
"Fumihiko",
""
]
] | We study the stability of a special form of D brane embedding which is regarded as a bound state of D$_n$ and anti-D$_n$-brane embedded in a 10D supergravity background which is dual to a confining gauge theory. For D5 branes with $U(1)$ flux, their bound state configuration can be regarded as the baryonium vertex. For... | 10.53615 | 9.259645 | 10.415749 | 9.174064 | 8.904144 | 9.522899 | 9.106224 | 9.398941 | 9.614414 | 10.677028 | 8.794916 | 9.038741 | 9.716187 | 9.392323 | 9.42906 | 9.236906 | 9.629071 | 8.993413 | 9.233386 | 9.433199 | 9.177783 |
hep-th/0405218 | Benedicte Ponsot | Benedicte Ponsot | Form factors in the SS model and its RSOS restrictions | 16 pages, 5 tables; v2:misprints corrected, clearer notations,
discussion extended; v4: formula for the SS trace operator corrected,
additional numerical checks on the central charge, proposal for p-function of
exponential fields now coherent with the trace, submitted to NPB. v5:table 1
added, references added,... | null | null | null | hep-th cond-mat.other | null | New integral representations for form factors in the two parametric SS model
are proposed. Some form factors in the parafermionic sine-Gordon model and in
an integrable perturbation of SU(2) coset conformal field theories are
straightforwardly obtained by different quantum group restrictions. Numerical
checks on the ... | [
{
"created": "Tue, 25 May 2004 09:12:05 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Jun 2004 02:14:38 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Jun 2004 08:25:42 GMT",
"version": "v3"
},
{
"created": "Thu, 10 Jun 2004 04:20:15 GMT",
"version": "v4"
},
{
"cre... | 2007-05-23 | [
[
"Ponsot",
"Benedicte",
""
]
] | New integral representations for form factors in the two parametric SS model are proposed. Some form factors in the parafermionic sine-Gordon model and in an integrable perturbation of SU(2) coset conformal field theories are straightforwardly obtained by different quantum group restrictions. Numerical checks on the va... | 13.515718 | 9.641696 | 18.75559 | 10.0027 | 9.621119 | 9.218542 | 8.922273 | 11.358298 | 9.560503 | 19.884226 | 10.244444 | 10.81313 | 15.279287 | 11.662816 | 11.037371 | 10.339853 | 10.25174 | 11.214668 | 11.533266 | 15.686215 | 11.379519 |
1102.0478 | Jurgen Baacke | Jurgen Baacke and Nina Kevlishvili | Erratum: One-loop corrections to the string tension of the vortex in the
Abelian Higgs model | 2 pages, 1 figure | Phys.Rev.D78:085008,2008; Erratum-ibid.D82:129905,2010 | 10.1103/PhysRevD.82.129905 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We correct two errors in our previous computation of one-loop corrections to
the vortex string tension: (i) the contribution of the longitudinal and
timelike modes of the gauge fields were forgotten and are included now; (ii) a
trivial error in the numerical code has led to considerable errors in the
subtracted integ... | [
{
"created": "Wed, 2 Feb 2011 16:35:17 GMT",
"version": "v1"
}
] | 2011-11-10 | [
[
"Baacke",
"Jurgen",
""
],
[
"Kevlishvili",
"Nina",
""
]
] | We correct two errors in our previous computation of one-loop corrections to the vortex string tension: (i) the contribution of the longitudinal and timelike modes of the gauge fields were forgotten and are included now; (ii) a trivial error in the numerical code has led to considerable errors in the subtracted integra... | 12.478071 | 14.450749 | 12.057648 | 11.809032 | 13.122139 | 12.325953 | 13.954308 | 11.895797 | 11.724405 | 13.675333 | 11.649549 | 11.092086 | 11.411573 | 10.900379 | 10.931855 | 11.322953 | 11.552483 | 11.749652 | 10.720588 | 11.718704 | 11.166509 |
hep-th/9903108 | Reza Abbaspur | Reza Abbaspur | Branes at Angles from DBI Action | Latex file, 19 pages, 1 ps figure, the section on the non-marginal
configurations of parallel branes has been modified and some other references
have been included | null | null | IPM/P-99/012 | hep-th | null | In this paper we investigate about several configurations of two intersecting
branes at arbitrary angles. We choose the viewpoint of a brane source and a
brane probe and use the low-energy dynamics of p-branes. For each p-brane this
dynamics is governed by a generic DBI action including a WZ term, which couples
to th... | [
{
"created": "Thu, 11 Mar 1999 19:10:11 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Apr 2000 17:02:42 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Abbaspur",
"Reza",
""
]
] | In this paper we investigate about several configurations of two intersecting branes at arbitrary angles. We choose the viewpoint of a brane source and a brane probe and use the low-energy dynamics of p-branes. For each p-brane this dynamics is governed by a generic DBI action including a WZ term, which couples to the ... | 9.251451 | 9.024721 | 10.266947 | 8.929866 | 9.167019 | 9.355993 | 9.15976 | 9.1611 | 9.127661 | 10.386923 | 8.969218 | 8.832583 | 9.232091 | 8.826594 | 8.805589 | 8.931263 | 8.971133 | 8.68556 | 8.968243 | 9.537939 | 8.888314 |
1605.04921 | Gustavo Brito | Antonio Accioly, Jos\'e Helay\"el-Neto, Gilson Correia, Gustavo Brito,
Jos\'e de Almeida, Wallace Herdy | Interparticle potential energy for D-dimensional electromagnetic models
from the corresponding scalar ones | null | Phys. Rev. D 93, 105042 (2016) | 10.1103/PhysRevD.93.105042 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using a method based on the generating functional plus a kind of
"correspondence principle" --- which acts as a bridge between the
electromagnetic and scalar fields --- it is shown that the interparticle
potential energy concerning a given $D$-dimensional electromagnetic model can
be obtained in a simple way from tha... | [
{
"created": "Mon, 16 May 2016 20:01:17 GMT",
"version": "v1"
}
] | 2016-06-22 | [
[
"Accioly",
"Antonio",
""
],
[
"Helayël-Neto",
"José",
""
],
[
"Correia",
"Gilson",
""
],
[
"Brito",
"Gustavo",
""
],
[
"de Almeida",
"José",
""
],
[
"Herdy",
"Wallace",
""
]
] | Using a method based on the generating functional plus a kind of "correspondence principle" --- which acts as a bridge between the electromagnetic and scalar fields --- it is shown that the interparticle potential energy concerning a given $D$-dimensional electromagnetic model can be obtained in a simple way from that ... | 13.088304 | 12.601439 | 12.873697 | 12.409984 | 12.320157 | 12.326614 | 12.366487 | 12.322671 | 12.602069 | 12.690649 | 12.017202 | 12.091615 | 12.391881 | 12.053897 | 11.811214 | 11.854546 | 11.88148 | 11.649693 | 12.00342 | 12.057873 | 11.911147 |
1410.4833 | Gustavo Monteiro | Gustavo M. Monteiro, Alexander G. Abanov and V. P. Nair | Hydrodynamics with gauge anomaly: Variational principle and Hamiltonian
formulation | 8 pages, no figures | Phys. Rev. D 91, 125033 (2015) | 10.1103/PhysRevD.91.125033 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a variational principle for relativistic hydrodynamics with
gauge-anomaly terms for a fluid coupled to an Abelian background gauge field.
For this we utilize the Clebsch parametrization of the velocity field. We also
set up the Hamiltonian formulation and the canonical framework for the theory.
While the e... | [
{
"created": "Fri, 17 Oct 2014 19:45:34 GMT",
"version": "v1"
}
] | 2015-10-06 | [
[
"Monteiro",
"Gustavo M.",
""
],
[
"Abanov",
"Alexander G.",
""
],
[
"Nair",
"V. P.",
""
]
] | We present a variational principle for relativistic hydrodynamics with gauge-anomaly terms for a fluid coupled to an Abelian background gauge field. For this we utilize the Clebsch parametrization of the velocity field. We also set up the Hamiltonian formulation and the canonical framework for the theory. While the equ... | 8.075429 | 8.463731 | 8.095334 | 8.434757 | 8.219385 | 9.018467 | 8.076283 | 8.026246 | 8.428105 | 10.313234 | 7.989545 | 7.650929 | 8.023791 | 7.794463 | 8.122574 | 7.864229 | 8.079126 | 7.795342 | 8.118619 | 8.664325 | 7.791375 |
hep-th/0011278 | Pietro Antonio Grassi | P.A. Grassi (New York Univ.) and P. van Nieuwenhuizen (YITP, Stony
Brook) | No van Dam-Veltman-Zakharov Discontinuity for Supergravity in AdS Space | November 2000, 7pp, misprints and typos corrected | Phys.Lett.B499:174-178,2001 | 10.1016/S0370-2693(01)00023-5 | YITP-00-78, NYU-TH/00/11/03 | hep-th | null | Adding explicit mass terms for the spin 2 and spin 3/2 field of N=1 anti-de
Sitter supergravity, the limit M --> 0 for these mass terms is smooth: there is
no van Dam-Veltman-Zakharov mass discontinuity in the propagators when the
cosmological constant is non-vanishing.
| [
{
"created": "Wed, 29 Nov 2000 20:55:54 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Dec 2000 23:34:26 GMT",
"version": "v2"
}
] | 2011-07-19 | [
[
"Grassi",
"P. A.",
"",
"New York Univ."
],
[
"van Nieuwenhuizen",
"P.",
"",
"YITP, Stony\n Brook"
]
] | Adding explicit mass terms for the spin 2 and spin 3/2 field of N=1 anti-de Sitter supergravity, the limit M --> 0 for these mass terms is smooth: there is no van Dam-Veltman-Zakharov mass discontinuity in the propagators when the cosmological constant is non-vanishing. | 11.896716 | 9.7545 | 10.018699 | 8.790606 | 10.202539 | 9.432046 | 7.81634 | 7.901514 | 9.286415 | 10.604078 | 9.16691 | 8.873912 | 8.726634 | 8.17286 | 8.772322 | 8.904212 | 8.9223 | 8.32697 | 8.787842 | 10.31285 | 8.816798 |
1511.02971 | Lars Brink | Lars Brink | Maximally Supersymmetric Yang-Mills Theory. The Story of N = 4
Yang-Mills Theory | Talk given at "60 years of Yang-Mills Theory", Singapore May 25-28,
2015. 15 pages | null | 10.1142/S0217751X16300027 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a personally colored account of the history behind N=4 Yang-Mills
Theory.
| [
{
"created": "Tue, 10 Nov 2015 02:35:43 GMT",
"version": "v1"
}
] | 2016-01-20 | [
[
"Brink",
"Lars",
""
]
] | This is a personally colored account of the history behind N=4 Yang-Mills Theory. | 73.658844 | 20.716549 | 26.944607 | 19.952864 | 24.100414 | 21.225863 | 20.071436 | 21.686407 | 17.958963 | 22.93631 | 21.539597 | 22.24157 | 27.503372 | 22.392786 | 22.647758 | 21.227629 | 21.295961 | 23.986311 | 20.583 | 26.955904 | 25.099476 |
hep-th/9611067 | Peter Bouwknegt | Peter Bouwknegt, Jim McCarthy and Peter van Nieuwenhuizen | Fusing the coordinates of quantum superspace | 9 pages, TeX with amssym.def, two references added | Phys.Lett.B394:82-86,1997 | 10.1016/S0370-2693(96)01679-6 | ADP-96-35/M46, ITP-SB-96-60 | hep-th | null | We introduce the notion of a fused quantum superplane by allowing for terms
$\theta\theta\sim x$ in the defining relations. We develop the differential
calculus for a large class of fused quantum superplanes related to particular
solutions of the Yang-Baxter equation.
| [
{
"created": "Mon, 11 Nov 1996 00:22:48 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Mar 1997 02:41:01 GMT",
"version": "v2"
}
] | 2009-09-11 | [
[
"Bouwknegt",
"Peter",
""
],
[
"McCarthy",
"Jim",
""
],
[
"van Nieuwenhuizen",
"Peter",
""
]
] | We introduce the notion of a fused quantum superplane by allowing for terms $\theta\theta\sim x$ in the defining relations. We develop the differential calculus for a large class of fused quantum superplanes related to particular solutions of the Yang-Baxter equation. | 16.283003 | 15.869946 | 16.412542 | 13.909977 | 13.956167 | 13.970655 | 13.855749 | 13.547664 | 15.084808 | 17.333344 | 13.296735 | 16.062902 | 16.282738 | 15.483588 | 14.805902 | 15.143145 | 14.959283 | 14.833207 | 15.704252 | 16.127575 | 13.71422 |
2212.02994 | Meng-Sen Ma | Li-Hua Wang, Yun He, Meng-Sen Ma | Fractional phase transitions of RN-AdS black hole at Davies points | 13 pages, 4 figures, to be published in Chinese Physics C | null | 10.1088/1674-1137/aca957 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We perform a study of phase transitions of RN-AdS black hole at its Davies
points according to a generalized Ehrenfest classification of phase transition
established on the basis of fractional derivatives. Davies points label the
positions where heat capacity diverges. According to the usual Ehrenfest
classification,... | [
{
"created": "Tue, 6 Dec 2022 14:11:52 GMT",
"version": "v1"
}
] | 2023-02-15 | [
[
"Wang",
"Li-Hua",
""
],
[
"He",
"Yun",
""
],
[
"Ma",
"Meng-Sen",
""
]
] | We perform a study of phase transitions of RN-AdS black hole at its Davies points according to a generalized Ehrenfest classification of phase transition established on the basis of fractional derivatives. Davies points label the positions where heat capacity diverges. According to the usual Ehrenfest classification, s... | 8.115658 | 8.089758 | 7.569496 | 7.44857 | 7.536218 | 7.615045 | 8.042912 | 7.449012 | 7.957158 | 8.012148 | 7.876291 | 7.557302 | 7.761118 | 7.540132 | 7.462636 | 7.25711 | 7.549714 | 7.367338 | 7.768623 | 7.664167 | 7.554048 |
hep-th/0007126 | Michael Gutperle | Michael Gutperle (Harvard University) | Non-BPS D-branes and enhanced symmetry in an asymmetric orbifold | 19 pages, harvmac (b), no figures, v2: reference added, v3: reference
added, version to appear in JHEP | JHEP 0008:036,2000 | 10.1088/1126-6708/2000/08/036 | HUTP-00/A026 | hep-th | null | In this paper properties of D branes in a nine dimensional asymmetric
orbifold are discussed, using a $(-1)^{F_L}\sigma_{1/2}$ projection, where
$F_L$ is the leftmoving space-time fermion number and $\sigma_{1/2}$ is a
freely acting shift of order two. There are two types of non BPS D branes,
which are stable at $R>2... | [
{
"created": "Mon, 17 Jul 2000 02:38:02 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jul 2000 13:24:56 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Aug 2000 18:32:12 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Gutperle",
"Michael",
"",
"Harvard University"
]
] | In this paper properties of D branes in a nine dimensional asymmetric orbifold are discussed, using a $(-1)^{F_L}\sigma_{1/2}$ projection, where $F_L$ is the leftmoving space-time fermion number and $\sigma_{1/2}$ is a freely acting shift of order two. There are two types of non BPS D branes, which are stable at $R>2$ ... | 7.418701 | 7.327681 | 8.894466 | 7.12152 | 7.315685 | 7.243487 | 7.351627 | 7.501038 | 7.278515 | 9.984186 | 7.178754 | 7.117446 | 7.788106 | 7.106555 | 7.192893 | 7.242149 | 7.540483 | 7.067421 | 7.255251 | 7.497036 | 7.039483 |
hep-th/9904053 | Hani Kaldass | A. Bohm, H. Kaldass | Relativistic Partial Wave Analysis Using the Velocity Basis of the
Poincare Group | 14 pages; revtex | Phys.Rev.A60:4606-4615,1999 | 10.1103/PhysRevA.60.4606 | null | hep-th math-ph math.MP quant-ph | null | The velocity basis of the Poincare group is used in the direct product space
of two irreducible unitary representations of the Poincare group. The velocity
basis with total angular momentum j will be used for the definition of
relativistic Gamow vectors.
| [
{
"created": "Wed, 7 Apr 1999 22:09:57 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Bohm",
"A.",
""
],
[
"Kaldass",
"H.",
""
]
] | The velocity basis of the Poincare group is used in the direct product space of two irreducible unitary representations of the Poincare group. The velocity basis with total angular momentum j will be used for the definition of relativistic Gamow vectors. | 16.436607 | 15.202688 | 14.091576 | 14.161462 | 14.889221 | 15.931034 | 15.29477 | 15.592109 | 13.681578 | 17.352678 | 14.540218 | 14.517232 | 14.478726 | 13.701056 | 14.897079 | 14.681082 | 14.210403 | 15.341517 | 14.28301 | 14.202779 | 14.020043 |
hep-th/0004139 | Mccartor | Gary McCartor | Regulating the $P^+ = 0$ Singularity | 6 pages and uses sprocl.sty | null | null | SMUHEP/00-06 | hep-th | null | I shall discuss the regulation of the $P^+ = 0$ singularity and give some
examples. Regulating the singularity induces new operators into the theory.
This process seems rather different for the case of ultraviolet singularities
than for the case of infrared singularities.
| [
{
"created": "Wed, 19 Apr 2000 16:16:29 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"McCartor",
"Gary",
""
]
] | I shall discuss the regulation of the $P^+ = 0$ singularity and give some examples. Regulating the singularity induces new operators into the theory. This process seems rather different for the case of ultraviolet singularities than for the case of infrared singularities. | 17.597597 | 13.104712 | 13.568555 | 14.424645 | 14.516517 | 16.239223 | 14.898479 | 15.056976 | 13.457062 | 15.510779 | 15.441478 | 13.655588 | 14.280062 | 14.090622 | 13.331534 | 13.778171 | 14.43733 | 13.400523 | 13.960084 | 14.665964 | 14.070856 |
1705.08732 | Amir H. Fatollahi | Amir H. Fatollahi | A Lattice Inspired Model for Monopole Dynamics | v1: 12 pages, 5 figs. v2: title is changed, and also presentation! | null | null | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The site-reduction of U(1) lattice gauge theory along the spatial directions
is used to model the monopole dynamics. The reduced theory is that of the
angle-valued coordinates on the discrete worldline. Below the critical coupling
$g_{c}=1.125$ and temperature $T_c=0.335$ the model exhibits a first order
phase transi... | [
{
"created": "Tue, 23 May 2017 15:01:23 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Jul 2021 05:54:28 GMT",
"version": "v2"
}
] | 2021-07-27 | [
[
"Fatollahi",
"Amir H.",
""
]
] | The site-reduction of U(1) lattice gauge theory along the spatial directions is used to model the monopole dynamics. The reduced theory is that of the angle-valued coordinates on the discrete worldline. Below the critical coupling $g_{c}=1.125$ and temperature $T_c=0.335$ the model exhibits a first order phase transiti... | 15.625075 | 15.291372 | 14.345358 | 13.423477 | 13.386731 | 14.699669 | 15.40443 | 13.735568 | 13.275467 | 15.912031 | 14.965433 | 12.982921 | 13.559031 | 13.436319 | 13.749982 | 13.415072 | 13.604398 | 13.360723 | 13.511538 | 13.877872 | 13.580222 |
0812.1759 | Papantonopoulos Eleftherios | Eleftherios Papantonopoulos and Petros Skamagoulis | Hawking Radiation via Gravitational Anomalies in Non-spherical
Topologies | 25 pages, no figures, version to be published in Phys. Rev. D | Phys.Rev.D79:084022,2009 | 10.1103/PhysRevD.79.084022 | null | hep-th gr-qc | http://creativecommons.org/licenses/by-nc-sa/3.0/ | We study the method of calculating the Hawking radiation via gravitational
anomalies in gravitational backgrounds of constant negative curvature. We apply
the method to topological black holes and also to topological black holes
conformally coupled to a scalar field.
| [
{
"created": "Tue, 9 Dec 2008 18:08:56 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Dec 2008 19:10:47 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Mar 2009 16:44:39 GMT",
"version": "v3"
}
] | 2009-07-24 | [
[
"Papantonopoulos",
"Eleftherios",
""
],
[
"Skamagoulis",
"Petros",
""
]
] | We study the method of calculating the Hawking radiation via gravitational anomalies in gravitational backgrounds of constant negative curvature. We apply the method to topological black holes and also to topological black holes conformally coupled to a scalar field. | 10.627313 | 8.43023 | 10.962478 | 8.821894 | 8.830656 | 10.05266 | 9.520432 | 9.305365 | 8.505683 | 9.471683 | 8.66606 | 10.201841 | 10.007451 | 9.459304 | 9.878582 | 9.768218 | 10.192464 | 10.083008 | 9.646573 | 10.023082 | 9.303188 |
1406.6043 | Robert A. Jefferson | Ben Freivogel, Robert A. Jefferson, Laurens Kabir, and I-Sheng Yang | Geometry of the Infalling Causal Patch | 21 pages, 7 figures. Minor edits/reformatting. Consistent with
version published in PRD | Phys. Rev. D 91, 044036 (2015) | 10.1103/PhysRevD.91.044036 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The firewall paradox states that an observer falling into an old black hole
must see a violation of unitarity, locality, or the equivalence principle.
Motivated by this remarkable conflict, we analyze the causal structure of black
hole spacetimes in order to determine whether all the necessary ingredients for
the par... | [
{
"created": "Mon, 23 Jun 2014 19:50:51 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Mar 2015 20:17:29 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Freivogel",
"Ben",
""
],
[
"Jefferson",
"Robert A.",
""
],
[
"Kabir",
"Laurens",
""
],
[
"Yang",
"I-Sheng",
""
]
] | The firewall paradox states that an observer falling into an old black hole must see a violation of unitarity, locality, or the equivalence principle. Motivated by this remarkable conflict, we analyze the causal structure of black hole spacetimes in order to determine whether all the necessary ingredients for the parad... | 8.614254 | 7.382451 | 8.073377 | 6.862613 | 7.457777 | 7.666323 | 7.243812 | 7.083925 | 7.080418 | 8.490704 | 6.868984 | 6.879466 | 7.337494 | 7.036618 | 6.966395 | 6.769074 | 6.859325 | 7.046878 | 7.11005 | 7.077727 | 6.950044 |
hep-th/0109041 | Ramzi R. Khuri | Ramzi R. Khuri | Fundamental Strings and Cosmology | 7 pages, harvmac, reference added | Phys.Lett.B520:353-356,2001 | 10.1016/S0370-2693(01)01137-6 | BCCUNY-HEP/01-02 | hep-th astro-ph gr-qc | null | We show that the velocity-dependent forces between parallel fundamental
strings moving apart in a D-dimensional spacetime imply an expanding universe
in (D-1)-dimensional spacetime.
| [
{
"created": "Wed, 5 Sep 2001 21:31:40 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Nov 2001 22:08:32 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Khuri",
"Ramzi R.",
""
]
] | We show that the velocity-dependent forces between parallel fundamental strings moving apart in a D-dimensional spacetime imply an expanding universe in (D-1)-dimensional spacetime. | 26.216648 | 13.561384 | 19.400839 | 14.16489 | 12.547067 | 10.628325 | 11.214937 | 13.194599 | 14.78913 | 24.752954 | 12.513391 | 18.328463 | 20.244011 | 18.908688 | 18.560692 | 18.076975 | 16.552975 | 20.877857 | 18.450628 | 20.937815 | 18.352022 |
1505.07871 | Diego Regalado | Dagoberto Escobar, Aitor Landete, Fernando Marchesano, Diego Regalado | Large field inflation from D-branes | 5 pages, 3 figures. Typos corrected and plots updated | Phys. Rev. D 93, 081301 (2016) | 10.1103/PhysRevD.93.081301 | IFT-UAM/CSIC-15-056, MPP-2015-109 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose new large field inflation scenarios built on the framework of
F-term axion monodromy. Our setup is based on string compactifications where
D-branes create potentials for closed string axions via F-terms. Because the
source of the axion potential is different from the standard sources of moduli
stabilisatio... | [
{
"created": "Thu, 28 May 2015 21:52:54 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Dec 2015 16:47:17 GMT",
"version": "v2"
}
] | 2016-04-13 | [
[
"Escobar",
"Dagoberto",
""
],
[
"Landete",
"Aitor",
""
],
[
"Marchesano",
"Fernando",
""
],
[
"Regalado",
"Diego",
""
]
] | We propose new large field inflation scenarios built on the framework of F-term axion monodromy. Our setup is based on string compactifications where D-branes create potentials for closed string axions via F-terms. Because the source of the axion potential is different from the standard sources of moduli stabilisation,... | 8.90279 | 8.367048 | 10.230458 | 8.395867 | 8.52183 | 8.495948 | 8.111812 | 7.799153 | 8.616746 | 10.268403 | 8.242687 | 8.445938 | 8.851089 | 8.547119 | 8.572052 | 8.128311 | 8.407819 | 8.402799 | 8.388385 | 9.219521 | 8.160058 |
0708.1075 | Olaf Lechtenfeld | Anton Galajinsky, Olaf Lechtenfeld, Kirill Polovnikov | N=4 superconformal Calogero models | 1+21 pages; v2: slight changes in section 4, new subsection 5.3 with
additional results (a full list of n=3 and n=4 models), acknowledgments and
one reference added, JHEP version | JHEP0711:008,2007 | 10.1088/1126-6708/2007/11/008 | null | hep-th | null | We continue the research initiated in hep-th/0607215 and apply our method of
conformal automorphisms to generate various N=4 superconformal quantum
many-body systems on the real line from a set of decoupled particles extended
by fermionic degrees of freedom. The su(1,1|2) invariant models are governed by
two scalar p... | [
{
"created": "Wed, 8 Aug 2007 10:23:42 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Nov 2007 10:33:42 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Galajinsky",
"Anton",
""
],
[
"Lechtenfeld",
"Olaf",
""
],
[
"Polovnikov",
"Kirill",
""
]
] | We continue the research initiated in hep-th/0607215 and apply our method of conformal automorphisms to generate various N=4 superconformal quantum many-body systems on the real line from a set of decoupled particles extended by fermionic degrees of freedom. The su(1,1|2) invariant models are governed by two scalar pot... | 10.620933 | 10.424181 | 13.180858 | 9.952157 | 11.162903 | 10.737777 | 10.742785 | 10.271255 | 10.262934 | 12.587279 | 10.238494 | 10.161563 | 10.992796 | 10.321374 | 10.560884 | 10.320368 | 10.268491 | 10.211921 | 10.01685 | 10.681287 | 10.086898 |
1402.4200 | Yuji Tachikawa | Yuji Tachikawa | Moduli spaces of SO(8) instantons on smooth ALE spaces as Higgs branches
of 4d N=2 supersymmetric theories | 18 pages, 10 figures; v2: additional references and minor changes;
published version | null | 10.1007/JHEP06(2014)056 | IPMU-14-0029, UT-14-5 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The worldvolume theory of D3-branes probing four D7-branes and an O7-plane on
$\mathbb{C}^2/\mathbb{Z}_2$ is given by a supersymmetric USp x USp gauge
theory. We demonstrate that, at least for a particular choice of the holonomy
at infinity, we can go to a dual description of the gauge theory, where we can
add a Faye... | [
{
"created": "Tue, 18 Feb 2014 01:28:11 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Jun 2014 01:55:18 GMT",
"version": "v2"
}
] | 2019-08-19 | [
[
"Tachikawa",
"Yuji",
""
]
] | The worldvolume theory of D3-branes probing four D7-branes and an O7-plane on $\mathbb{C}^2/\mathbb{Z}_2$ is given by a supersymmetric USp x USp gauge theory. We demonstrate that, at least for a particular choice of the holonomy at infinity, we can go to a dual description of the gauge theory, where we can add a Fayet-... | 6.2581 | 5.683927 | 7.332246 | 5.966809 | 5.888172 | 5.40375 | 6.190547 | 5.989933 | 5.849113 | 8.317526 | 5.927794 | 5.624723 | 6.434171 | 5.969818 | 5.655194 | 5.715922 | 5.574583 | 5.760405 | 5.811096 | 6.2254 | 5.719706 |
1304.0366 | Peng Huang | Peng Huang, Yong-chang Huang | Stability of the holographic description of the Universe | 11 pages | Eur. Phys. J. C 73 (2013) 2366 | 10.1140/epjc/s10052-013-2366-1 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the stability of the holographic description of the universe.
By treating the perturbation globally, we discover that this description is
stable, which is support for the holographic description of the universe.
| [
{
"created": "Mon, 1 Apr 2013 14:34:02 GMT",
"version": "v1"
}
] | 2013-04-02 | [
[
"Huang",
"Peng",
""
],
[
"Huang",
"Yong-chang",
""
]
] | We investigate the stability of the holographic description of the universe. By treating the perturbation globally, we discover that this description is stable, which is support for the holographic description of the universe. | 18.372896 | 12.886113 | 13.263236 | 12.15583 | 11.588413 | 11.225868 | 12.135725 | 12.13372 | 13.697008 | 13.215267 | 13.826506 | 14.606833 | 13.522121 | 13.76275 | 13.732118 | 13.393379 | 14.179819 | 13.601014 | 13.771724 | 13.428384 | 13.331691 |
hep-th/0003267 | Horacio E. Camblong | Horacio E. Camblong, Luis N. Epele, Huner Fanchiotti and Carlos A.
Garcia Canal | Dimensional Transmutation and Dimensional Regularization in Quantum
Mechanics. II: Rotational Invariance | 29 pages. To appear in Annals of Physics | Ann.Phys.287:57-100,2001 | 10.1006/aphy.2000.6093 | null | hep-th quant-ph | null | A thorough analysis is presented of the class of central fields of force that
exhibit: (i) dimensional transmutation and (ii) rotational invariance. Using
dimensional regularization, the two-dimensional delta-function potential and
the $D$-dimensional inverse square potential are studied. In particular, the
following... | [
{
"created": "Wed, 29 Mar 2000 08:40:31 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Jan 2001 05:24:51 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Camblong",
"Horacio E.",
""
],
[
"Epele",
"Luis N.",
""
],
[
"Fanchiotti",
"Huner",
""
],
[
"Canal",
"Carlos A. Garcia",
""
]
] | A thorough analysis is presented of the class of central fields of force that exhibit: (i) dimensional transmutation and (ii) rotational invariance. Using dimensional regularization, the two-dimensional delta-function potential and the $D$-dimensional inverse square potential are studied. In particular, the following f... | 10.294392 | 10.512245 | 11.152078 | 11.023223 | 11.058564 | 10.963936 | 11.008098 | 9.617505 | 10.289771 | 10.749348 | 10.112143 | 10.0501 | 9.625678 | 9.300145 | 9.851837 | 10.116924 | 9.594948 | 9.552622 | 9.849986 | 9.895758 | 9.998035 |
hep-th/0211072 | John F. Donoghue | N. E. J Bjerrum-Bohr, John F. Donoghue, and Barry R. Holstein | Quantum Gravitational Corrections to the Nonrelativistic Scattering
Potential of Two Masses | 27 pages, 17 figures | Phys.Rev.D67:084033,2003; Erratum-ibid.D71:069903,2005 | 10.1103/PhysRevD.67.084033 10.1103/PhysRevD.71.069903 | null | hep-th gr-qc hep-ph | null | We treat general relativity as an effective field theory, obtaining the full
nonanalytic component of the scattering matrix potential to one-loop order. The
lowest order vertex rules for the resulting effective field theory are
presented and the one-loop diagrams which yield the leading nonrelativistic
post-Newtonian... | [
{
"created": "Fri, 8 Nov 2002 16:53:43 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Bjerrum-Bohr",
"N. E. J",
""
],
[
"Donoghue",
"John F.",
""
],
[
"Holstein",
"Barry R.",
""
]
] | We treat general relativity as an effective field theory, obtaining the full nonanalytic component of the scattering matrix potential to one-loop order. The lowest order vertex rules for the resulting effective field theory are presented and the one-loop diagrams which yield the leading nonrelativistic post-Newtonian a... | 12.434883 | 13.199611 | 12.253768 | 11.979078 | 12.049623 | 12.00075 | 13.020221 | 12.005775 | 12.780746 | 12.156732 | 12.673027 | 12.317146 | 11.96374 | 11.902908 | 11.770212 | 12.1678 | 12.435894 | 12.224374 | 13.098045 | 12.607141 | 12.0444 |
hep-th/9112017 | null | J. Luis Miramontes and Joaquin Sanchez Guillen | Universality and Non-Perturbative Definitions of 2D Quantum Gravity from
Matrix Models | 20 pages | Int.J.Mod.Phys.A7:6457-6472,1992 | 10.1142/S0217751X92002957 | null | hep-th | null | The universality of the non-perturbative definition of Hermitian one-matrix
models following the quantum, stochastic, or $d=1$-like stabilization is
discussed in comparison with other procedures. We also present another
alternative definition, which illustrates the need of new physical input for
$d=0$ matrix models t... | [
{
"created": "Mon, 9 Dec 1991 15:18:14 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Miramontes",
"J. Luis",
""
],
[
"Guillen",
"Joaquin Sanchez",
""
]
] | The universality of the non-perturbative definition of Hermitian one-matrix models following the quantum, stochastic, or $d=1$-like stabilization is discussed in comparison with other procedures. We also present another alternative definition, which illustrates the need of new physical input for $d=0$ matrix models to ... | 18.151287 | 15.630597 | 19.049017 | 15.137286 | 16.252254 | 17.417845 | 17.278229 | 15.261535 | 15.677482 | 19.576002 | 16.146133 | 15.657177 | 18.314034 | 16.715651 | 16.306496 | 15.314981 | 15.624987 | 15.316048 | 15.753731 | 17.796408 | 14.769137 |
hep-th/0305152 | Filipe Freire | Mboyo Esole and Filipe Freire | The unphysical nature of the SL(2,R) symmetry and its associated
condensates in Yang-Mills theories | 5 pages (revtex4), final version to appear in Phys. Rev. D | Phys.Rev. D69 (2004) 041701 | 10.1103/PhysRevD.69.041701 | null | hep-th | null | BRST cohomology methods are used to explain the origin of the SL(2,R)
symmetry in Yang-Mills theories. Clear evidence is provided for the unphysical
nature of this symmetry. This is obtained from the analysis of a local
functional of mass dimension two and constitutes a no-go statement for giving a
physical meaning t... | [
{
"created": "Sat, 17 May 2003 16:45:10 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Jan 2004 14:00:51 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Esole",
"Mboyo",
""
],
[
"Freire",
"Filipe",
""
]
] | BRST cohomology methods are used to explain the origin of the SL(2,R) symmetry in Yang-Mills theories. Clear evidence is provided for the unphysical nature of this symmetry. This is obtained from the analysis of a local functional of mass dimension two and constitutes a no-go statement for giving a physical meaning to ... | 12.445065 | 11.297973 | 10.914409 | 11.037927 | 10.32211 | 10.711236 | 11.337247 | 11.819184 | 10.667966 | 12.48215 | 10.67463 | 10.53575 | 9.90354 | 10.711123 | 10.386707 | 10.296456 | 10.451176 | 11.026097 | 10.560693 | 10.764697 | 10.923637 |
0706.2546 | Giuseppe Mussardo | Giuseppe Mussardo | Kink Confinement and Supersymmetry | 29 pages, 12 figures | JHEP 0708:003,2007 | 10.1088/1126-6708/2007/08/003 | null | hep-th cond-mat.stat-mech hep-lat | null | We analyze non-integrable deformations of two-dimensional N=1 supersymmetric
quantum field theories with kink excitations. As example, we consider the
multi-frequency Super Sine Gordon model. At weak coupling, this model is robust
with respect to kink confinement phenomena, in contrast to the purely bosonic
case. If ... | [
{
"created": "Mon, 18 Jun 2007 08:05:57 GMT",
"version": "v1"
}
] | 2009-11-18 | [
[
"Mussardo",
"Giuseppe",
""
]
] | We analyze non-integrable deformations of two-dimensional N=1 supersymmetric quantum field theories with kink excitations. As example, we consider the multi-frequency Super Sine Gordon model. At weak coupling, this model is robust with respect to kink confinement phenomena, in contrast to the purely bosonic case. If we... | 9.66146 | 9.683747 | 10.586951 | 9.322904 | 9.493705 | 9.388107 | 9.24448 | 9.532914 | 9.02334 | 11.067118 | 9.054187 | 9.341621 | 9.545405 | 9.382115 | 9.256523 | 9.347604 | 9.073911 | 9.177737 | 9.097869 | 10.10938 | 9.06446 |
hep-th/0103165 | John H. Schwarz | John H. Schwarz | Comments on Born-Infeld Theory | 10 pages; talk presented at Strings 2001 | null | null | CALT-68-2322, CITUSC/01-006 | hep-th | null | The low-energy effective action of supersymmetric D-brane systems consists of
two terms, one of which is of the Born-Infeld type and one of which is of the
Chern-Simons type. I briefly review the status of our understanding of these
terms for both the Abelian and non-Abelian cases.
| [
{
"created": "Tue, 20 Mar 2001 19:01:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Schwarz",
"John H.",
""
]
] | The low-energy effective action of supersymmetric D-brane systems consists of two terms, one of which is of the Born-Infeld type and one of which is of the Chern-Simons type. I briefly review the status of our understanding of these terms for both the Abelian and non-Abelian cases. | 5.089199 | 4.847229 | 5.190089 | 4.687242 | 4.731028 | 4.719101 | 4.818873 | 4.605809 | 4.764526 | 5.114319 | 4.744231 | 4.954153 | 5.21291 | 4.659081 | 4.655576 | 4.790379 | 4.689589 | 4.822532 | 4.83409 | 5.080459 | 4.64786 |
1001.1103 | Jan Gutowski | U. Gran, J. Gutowski, G. Papadopoulos | M-theory backgrounds with 30 Killing spinors are maximally
supersymmetric | 37 pages, latex. Minor changes. | JHEP 1003:112,2010 | 10.1007/JHEP03(2010)112 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that all M-theory backgrounds which admit more than 29 Killing
spinors are maximally supersymmetric. In particular, we find that the
supercovariant curvature of all backgrounds which preserve 30 supersymmetries,
subject to field equations and Bianchi identities, vanishes, and that there are
no such solutions ... | [
{
"created": "Thu, 7 Jan 2010 16:06:23 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Mar 2010 12:42:43 GMT",
"version": "v2"
}
] | 2010-05-07 | [
[
"Gran",
"U.",
""
],
[
"Gutowski",
"J.",
""
],
[
"Papadopoulos",
"G.",
""
]
] | We show that all M-theory backgrounds which admit more than 29 Killing spinors are maximally supersymmetric. In particular, we find that the supercovariant curvature of all backgrounds which preserve 30 supersymmetries, subject to field equations and Bianchi identities, vanishes, and that there are no such solutions wh... | 6.805806 | 5.769446 | 8.113063 | 5.889424 | 6.48175 | 6.003754 | 5.795794 | 6.110911 | 5.848592 | 8.923321 | 6.058207 | 6.247721 | 7.212325 | 6.174112 | 6.296171 | 6.251829 | 6.137088 | 6.327942 | 6.307748 | 6.867897 | 6.191763 |
1408.1715 | Erik Plauschinn | Erik Plauschinn | On T-duality transformations for the three-sphere | 42 pages; v2: references added; v3: published version | null | 10.1016/j.nuclphysb.2015.02.008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study collective T-duality transformations along one, two and three
directions of isometry for the three-sphere with H-flux. Our aim is to obtain
new non-geometric backgrounds along lines similar to the example of the
three-torus. However, the resulting backgrounds turn out to be geometric in
nature. To perform th... | [
{
"created": "Thu, 7 Aug 2014 21:18:04 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Sep 2014 15:51:01 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Mar 2015 12:54:56 GMT",
"version": "v3"
}
] | 2015-03-26 | [
[
"Plauschinn",
"Erik",
""
]
] | We study collective T-duality transformations along one, two and three directions of isometry for the three-sphere with H-flux. Our aim is to obtain new non-geometric backgrounds along lines similar to the example of the three-torus. However, the resulting backgrounds turn out to be geometric in nature. To perform the ... | 11.528886 | 12.234348 | 12.708701 | 11.148055 | 11.515116 | 11.639266 | 11.117319 | 10.742476 | 10.305774 | 14.093451 | 10.638774 | 10.844708 | 11.61283 | 11.099064 | 11.19941 | 10.905996 | 10.730867 | 10.850595 | 10.680251 | 11.911426 | 10.484964 |
1512.04104 | Mohammad Reza Tanhayi | Mohammad Reza Tanhayi | Thermalization of Mutual Information in Hyperscaling Violating
Backgrounds | 24 pages, no figures, conclusion and introduction improved, ref.s
added, typos corrected, generalization of arXiv:1406.7677 (thermalization of
mutual information part) to time-dependent hyperscaling violating geometries,
accepted for publication in JHEP | JHEP 03 (2016) 202 | 10.1007/JHEP03(2016)202 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study certain features of scaling behaviors of the mutual information
during a process of thermalization, more precisely we extend the time scaling
behavior of mutual information which has been discussed in
\cite{Alishahiha:2014jxa} to time-dependent hyperscaling violating geometries.
We use the holographic descri... | [
{
"created": "Sun, 13 Dec 2015 19:17:23 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Dec 2015 15:01:40 GMT",
"version": "v2"
},
{
"created": "Mon, 14 Mar 2016 17:55:50 GMT",
"version": "v3"
}
] | 2016-05-04 | [
[
"Tanhayi",
"Mohammad Reza",
""
]
] | We study certain features of scaling behaviors of the mutual information during a process of thermalization, more precisely we extend the time scaling behavior of mutual information which has been discussed in \cite{Alishahiha:2014jxa} to time-dependent hyperscaling violating geometries. We use the holographic descript... | 11.532447 | 10.674647 | 12.389869 | 9.828803 | 10.866817 | 10.141698 | 9.549705 | 10.61818 | 10.343607 | 12.6585 | 10.572264 | 10.826715 | 11.06859 | 10.398774 | 10.642039 | 10.523623 | 10.014843 | 10.679314 | 10.21232 | 11.025191 | 10.55784 |
0905.1663 | Harvey B. Meyer | Harvey B. Meyer | Finite Volume Effects in Thermal Field Theory | (14+1) pages | JHEP 0907:059,2009 | 10.1088/1126-6708/2009/07/059 | MIT-CTP 4035 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the effect of a finite volume on the thermodynamic potentials of a
relativistic quantum field theory defined on a hypertorus at vanishing chemical
potential. Using the symmetries of the Euclidean partition function, we
interpret the thermodynamic observables as the expectation value of the
energy-momentum ... | [
{
"created": "Mon, 11 May 2009 17:44:53 GMT",
"version": "v1"
}
] | 2009-07-28 | [
[
"Meyer",
"Harvey B.",
""
]
] | We analyze the effect of a finite volume on the thermodynamic potentials of a relativistic quantum field theory defined on a hypertorus at vanishing chemical potential. Using the symmetries of the Euclidean partition function, we interpret the thermodynamic observables as the expectation value of the energy-momentum te... | 8.280517 | 8.882668 | 8.037825 | 7.5521 | 8.147523 | 8.143732 | 7.679441 | 8.131396 | 7.548051 | 7.977523 | 7.955119 | 8.043844 | 7.787519 | 7.792189 | 7.869029 | 7.671847 | 7.515889 | 8.321826 | 7.691836 | 7.880592 | 7.769813 |
hep-th/0010182 | Kasper Peeters | Kasper Peeters, Pierre Vanhove and Anders Westerberg | Supersymmetric R^4 actions and quantum corrections to superspace torsion
constraints | 8 pages. Summarises the methods and results of hep-th/0010167 | null | null | DAMTP-2000-91, NORDITA-2000/87 HE, SPHT-T00/117 | hep-th | null | We present the supersymmetrisation of the anomaly-related R^4 term in eleven
dimensions and show that it induces no non-trivial modifications to the
on-shell supertranslation algebra and the superspace torsion constraints before
inclusion of gauge-field terms.
| [
{
"created": "Fri, 20 Oct 2000 17:18:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Peeters",
"Kasper",
""
],
[
"Vanhove",
"Pierre",
""
],
[
"Westerberg",
"Anders",
""
]
] | We present the supersymmetrisation of the anomaly-related R^4 term in eleven dimensions and show that it induces no non-trivial modifications to the on-shell supertranslation algebra and the superspace torsion constraints before inclusion of gauge-field terms. | 23.646187 | 17.755213 | 25.08876 | 16.753168 | 19.338968 | 16.485701 | 19.337683 | 18.595751 | 15.695261 | 24.233854 | 17.416592 | 18.531977 | 21.98665 | 19.95713 | 18.802246 | 19.002563 | 18.973465 | 19.314491 | 18.325718 | 21.540064 | 19.341726 |
2209.04632 | Javier Mart\'in-Garc\'ia | Javier Martin-Garcia | Quantum Complexity and Holography | 151 pages, Ph. D. thesis (2020). Introductory chapter summarizes the
motivations for connecting entanglement and complexity with gravity, while
chapters 2, 3 and 4 are closely based on arXiv:1510.00349, arXiv:1710.06415,
arXiv:1805.05291 and arXiv:1912.00904 | null | null | null | hep-th | http://creativecommons.org/licenses/by-nc-sa/4.0/ | This thesis develops recent work on the so called Volume-Complexity and
Action-Complexity conjectures. According to this family of proposals, geometric
quantities can be defined in some holographic gravitational theories that can
be mapped with the concept of quantum complexity for states in a dual
quantum-mechanical... | [
{
"created": "Sat, 10 Sep 2022 10:31:33 GMT",
"version": "v1"
}
] | 2022-09-13 | [
[
"Martin-Garcia",
"Javier",
""
]
] | This thesis develops recent work on the so called Volume-Complexity and Action-Complexity conjectures. According to this family of proposals, geometric quantities can be defined in some holographic gravitational theories that can be mapped with the concept of quantum complexity for states in a dual quantum-mechanical t... | 12.259656 | 12.600455 | 12.506344 | 11.11086 | 11.722359 | 11.727936 | 12.412333 | 11.052128 | 11.110269 | 12.389996 | 10.654284 | 11.491756 | 11.429162 | 11.322322 | 10.948274 | 11.161371 | 11.348096 | 11.093783 | 11.504773 | 11.670935 | 11.004578 |
1202.5733 | Gregory Korchemsky | Burkhard Eden, Paul Heslop, Gregory P. Korchemsky, Vladimir A.
Smirnov, Emery Sokatchev | Five-loop Konishi in N=4 SYM | 42 pages, 7 figures; v2: reference added, minor corrections | null | 10.1016/j.nuclphysb.2012.04.015 | CERN-PH-TH/2012-053; DCPT-12/11; HU-EP-12/07; HU-MATH 2012-04;
IPhT-T12/014; LAPTH-011/12 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a new method for computing the Konishi anomalous dimension in N=4
SYM at weak coupling. It does not rely on the conventional Feynman diagram
technique and is not restricted to the planar limit. It is based on the OPE
analysis of the four-point correlation function of stress-tensor multiplets,
which has bee... | [
{
"created": "Sun, 26 Feb 2012 08:54:57 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Mar 2012 07:59:19 GMT",
"version": "v2"
},
{
"created": "Wed, 9 May 2012 06:41:00 GMT",
"version": "v3"
}
] | 2015-06-04 | [
[
"Eden",
"Burkhard",
""
],
[
"Heslop",
"Paul",
""
],
[
"Korchemsky",
"Gregory P.",
""
],
[
"Smirnov",
"Vladimir A.",
""
],
[
"Sokatchev",
"Emery",
""
]
] | We present a new method for computing the Konishi anomalous dimension in N=4 SYM at weak coupling. It does not rely on the conventional Feynman diagram technique and is not restricted to the planar limit. It is based on the OPE analysis of the four-point correlation function of stress-tensor multiplets, which has been ... | 5.871305 | 6.047605 | 6.826278 | 6.032732 | 6.530125 | 6.307662 | 6.182068 | 6.010628 | 5.876787 | 7.793706 | 5.850706 | 6.321737 | 6.375983 | 5.901178 | 5.939368 | 5.87385 | 5.83287 | 5.881883 | 5.886907 | 6.24961 | 5.830404 |
hep-th/0006108 | Dmitri Vassilevich | W. Kummer, D.V. Vassilevich | Renormalizability of the open string sigma model and emergence of
D-branes | 24 pages, a reference and discussion (about 1 page, sec. 3.3 and 4.1)
added, typos corrected | JHEP 0007 (2000) 012 | 10.1088/1126-6708/2000/07/012 | TUW-00-18 | hep-th | null | Rederiving the one-loop divergences for the most general coupling of the open
string sigma model by the heat kernel technique, we distinguish the classical
background field from the mean field of the effective action. The latter is
arbitrary, i.e. does not fulfil the boundary conditions. As a consequence a new
diverg... | [
{
"created": "Thu, 15 Jun 2000 12:02:25 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Jun 2000 13:22:05 GMT",
"version": "v2"
},
{
"created": "Mon, 3 Jul 2000 11:12:25 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Kummer",
"W.",
""
],
[
"Vassilevich",
"D. V.",
""
]
] | Rederiving the one-loop divergences for the most general coupling of the open string sigma model by the heat kernel technique, we distinguish the classical background field from the mean field of the effective action. The latter is arbitrary, i.e. does not fulfil the boundary conditions. As a consequence a new divergen... | 12.600152 | 12.392436 | 13.258633 | 11.975069 | 12.321264 | 13.309157 | 12.899555 | 12.531661 | 11.798954 | 13.841024 | 12.419373 | 11.830556 | 11.833439 | 11.372879 | 11.682597 | 11.389217 | 11.363385 | 11.671155 | 11.858901 | 11.721238 | 11.635581 |
1209.2727 | Carlos A. S. Almeida | L. J. S. Sousa, J. E. G. Silva, C. A. S. Almeida | A 6D standing wave Braneworld | 19 pages, 4 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We constructed a six-dimensional version of the standing wave model with an
anisotropic 4-brane generated by a phantom-like scalar field. The model
represents a braneworld where the compact (on-brane) dimension is assumed to be
sufficiently small in order to describe our universe (hybrid compactification).
The propos... | [
{
"created": "Wed, 12 Sep 2012 20:50:53 GMT",
"version": "v1"
}
] | 2012-09-14 | [
[
"Sousa",
"L. J. S.",
""
],
[
"Silva",
"J. E. G.",
""
],
[
"Almeida",
"C. A. S.",
""
]
] | We constructed a six-dimensional version of the standing wave model with an anisotropic 4-brane generated by a phantom-like scalar field. The model represents a braneworld where the compact (on-brane) dimension is assumed to be sufficiently small in order to describe our universe (hybrid compactification). The proposed... | 14.713175 | 10.957417 | 14.415265 | 11.997117 | 12.656104 | 13.080788 | 12.981688 | 11.1991 | 12.768641 | 15.102618 | 12.054317 | 12.999331 | 13.809154 | 13.499228 | 13.774663 | 13.453437 | 13.634442 | 13.362831 | 13.21786 | 14.32434 | 13.379182 |
hep-th/9405082 | Tonatiuh Matos | Tonatiuh Matos | Exact Solutions of G-Invariant Chiral Equations | 8 TeX pages. Seminar presented at the First Mexican-Russian Meeting
on Mathematical Physics, Mexico city, 1993 | Mathematical Notes 58(1995)1178-1182 | 10.1007/BF02305001 | Cinvestav 26/1995 | hep-th | null | We give a methodology for solving the chiral equations $(\alpha g_{,z}
g^{-1})_{,\overline z} + (\alpha g_{,\overline z} g^{-1})_{,z} \ = \ 0 $ where
$g$ belongs to some Lie group $G$. The solutions are writing in terms of
Harmonic maps. The method could be used even for some infinite Lie groups.
(Preprint CIEA-gr-94... | [
{
"created": "Thu, 12 May 1994 17:23:53 GMT",
"version": "v1"
}
] | 2022-11-08 | [
[
"Matos",
"Tonatiuh",
""
]
] | We give a methodology for solving the chiral equations $(\alpha g_{,z} g^{-1})_{,\overline z} + (\alpha g_{,\overline z} g^{-1})_{,z} \ = \ 0 $ where $g$ belongs to some Lie group $G$. The solutions are writing in terms of Harmonic maps. The method could be used even for some infinite Lie groups. (Preprint CIEA-gr-94/0... | 12.314095 | 12.754113 | 12.407963 | 11.014498 | 12.883361 | 12.374192 | 12.278317 | 13.261386 | 11.783799 | 14.319576 | 11.450266 | 10.586497 | 11.834621 | 10.932801 | 11.283449 | 10.647651 | 10.957635 | 11.180457 | 11.1597 | 11.864039 | 11.084643 |
hep-th/0608056 | Eric R. Sharpe | E. Sharpe | Derived categories and stacks in physics | 27 pages, LaTeX, 2 figures, contribution to proceedings of Vienna
homological mirror symmetry conference, June 2006; v2: refs added | null | null | null | hep-th | null | In this note we review how both derived categories and stacks enter physics.
The physical realization of each has many formal similarities. For example, in
both cases, equivalences are realized via renormalization group flow: in the
case of derived categories, (boundary) renormalization group flow realizes the
mathem... | [
{
"created": "Tue, 8 Aug 2006 23:21:46 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Sep 2006 04:49:26 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Sharpe",
"E.",
""
]
] | In this note we review how both derived categories and stacks enter physics. The physical realization of each has many formal similarities. For example, in both cases, equivalences are realized via renormalization group flow: in the case of derived categories, (boundary) renormalization group flow realizes the mathemat... | 14.648055 | 13.931798 | 16.181372 | 13.449076 | 13.467362 | 14.413104 | 13.401891 | 13.822358 | 13.786142 | 17.369102 | 12.490026 | 13.385685 | 14.553166 | 12.88339 | 13.682482 | 13.815604 | 13.722469 | 13.185994 | 13.067814 | 14.125546 | 13.219792 |
hep-th/0306259 | Hagi Ahmedov | H. Ahmedov and I. H. Duru | Casimir energy inside a triangle | Latex, 13 pages | J.Math.Phys. 45 (2004) 965 | 10.1063/1.1643196 | null | hep-th | null | For certain class of triangles (with angles proportional to $\fr{\pi}{N}$,
$N\geq 3$) we formulate image method by making use of the group $G_N$ generated
by reflections with respect to the three lines which form the triangle under
consideration. We formulate the renormalization procedure by classification of
subgrou... | [
{
"created": "Thu, 26 Jun 2003 10:54:45 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ahmedov",
"H.",
""
],
[
"Duru",
"I. H.",
""
]
] | For certain class of triangles (with angles proportional to $\fr{\pi}{N}$, $N\geq 3$) we formulate image method by making use of the group $G_N$ generated by reflections with respect to the three lines which form the triangle under consideration. We formulate the renormalization procedure by classification of subgroups... | 15.644385 | 14.663492 | 14.748113 | 12.850977 | 13.120324 | 12.655422 | 13.700007 | 13.208617 | 12.947903 | 17.169228 | 13.995496 | 12.492208 | 12.986379 | 12.827756 | 12.609185 | 12.754305 | 13.056192 | 13.196889 | 13.361452 | 13.17628 | 13.441369 |
1212.3322 | Taizan Watari | Ryoichi Nishio and Taizan Watari | Skewness Dependence of GPD / DVCS, Conformal OPE and AdS/CFT
Correspondence I: Wavefunctions of Regge Trajectory | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Traditional idea of Pomeron/Reggeon description for hadron scattering is now
being given theoretical foundation in gravity dual descriptions, where Pomeron
corresponds to exchange of spin-j\in 2Z states in the graviton trajectory.
Deeply virtual compton scattering (DVCS) is essentially a 2 to 2 scattering
process of ... | [
{
"created": "Thu, 13 Dec 2012 20:55:53 GMT",
"version": "v1"
}
] | 2012-12-14 | [
[
"Nishio",
"Ryoichi",
""
],
[
"Watari",
"Taizan",
""
]
] | Traditional idea of Pomeron/Reggeon description for hadron scattering is now being given theoretical foundation in gravity dual descriptions, where Pomeron corresponds to exchange of spin-j\in 2Z states in the graviton trajectory. Deeply virtual compton scattering (DVCS) is essentially a 2 to 2 scattering process of a ... | 13.855145 | 15.436413 | 12.241967 | 12.015454 | 17.161444 | 16.349672 | 16.181217 | 15.027095 | 11.780512 | 11.496514 | 14.450402 | 13.880601 | 13.456301 | 13.894176 | 14.730494 | 13.6873 | 14.788658 | 13.977196 | 13.512407 | 12.807461 | 13.379208 |
1904.10277 | Alexandra Anokhina | Aleksandra Anokhina, Alexei Morozov, Aleksandr Popolitov | Nimble evolution for pretzel Khovanov polynomials | 16 pages | Eur. Phys. J. C 79 (2019) 867 | 10.1140/epjc/s10052-019-7303-5 | null | hep-th math-ph math.GT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We conjecture explicit evolution formulas for Khovanov polynomials for
pretzel knots in some regions in the windings space. Our description is
exhaustive for genera 1 and 2. As previously observed, evolution at T != -1 is
not fully smooth: it switches abruptly at the boundaries between different
regions. We reveal th... | [
{
"created": "Tue, 23 Apr 2019 12:32:38 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Sep 2019 15:34:14 GMT",
"version": "v2"
}
] | 2020-01-29 | [
[
"Anokhina",
"Aleksandra",
""
],
[
"Morozov",
"Alexei",
""
],
[
"Popolitov",
"Aleksandr",
""
]
] | We conjecture explicit evolution formulas for Khovanov polynomials for pretzel knots in some regions in the windings space. Our description is exhaustive for genera 1 and 2. As previously observed, evolution at T != -1 is not fully smooth: it switches abruptly at the boundaries between different regions. We reveal that... | 20.621237 | 23.070267 | 23.189684 | 19.633495 | 21.534735 | 22.252762 | 21.701971 | 20.342936 | 20.243093 | 23.429905 | 20.086739 | 21.31461 | 21.738489 | 20.547943 | 21.493006 | 20.5383 | 20.491171 | 20.074575 | 20.254396 | 20.462927 | 20.055252 |
1410.0016 | Scott Watson | Ogan \"Ozsoy, Kuver Sinha, Scott Watson | How Well Can We Really Determine the Scale of Inflation? | 35 Pages, 3 figures, references added | Phys. Rev. D 91, 103509 (2015) | 10.1103/PhysRevD.91.103509 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A detection of primordial B-modes has been heralded not only as a smoking gun
for the existence of inflation, but also as a way to establish the scale at
which inflation took place. In this paper we critically reinvestigate the
connection between a detection of primordial gravity waves and the scale of
inflation. We ... | [
{
"created": "Tue, 30 Sep 2014 20:00:12 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Nov 2014 05:10:01 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Özsoy",
"Ogan",
""
],
[
"Sinha",
"Kuver",
""
],
[
"Watson",
"Scott",
""
]
] | A detection of primordial B-modes has been heralded not only as a smoking gun for the existence of inflation, but also as a way to establish the scale at which inflation took place. In this paper we critically reinvestigate the connection between a detection of primordial gravity waves and the scale of inflation. We co... | 8.440752 | 8.954488 | 8.571978 | 8.117239 | 9.296885 | 9.006102 | 8.94856 | 8.182552 | 8.635474 | 9.463616 | 8.693269 | 8.687376 | 8.339414 | 8.361316 | 8.604219 | 8.786457 | 8.378864 | 8.416553 | 8.183568 | 8.433515 | 8.303217 |
hep-th/0206055 | J. Fernando Barbero G. | J. Fernando Barbero G., Eduardo J. S. Villase\~nor | Kinetic Terms for 2-Forms in Four Dimensions | 20 pages, REVTEX, accepted for publication in Phys. Rev. D | Phys.Rev. D66 (2002) 045013 | 10.1103/PhysRevD.66.045013 | null | hep-th | null | We study the general form of the possible kinetic terms for 2-form fields in
four dimensions, under the restriction that they have a semibounded energy
density. This is done by using covariant symplectic techniques and generalizes
previous partial results in this direction.
| [
{
"created": "Fri, 7 Jun 2002 07:40:26 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"G.",
"J. Fernando Barbero",
""
],
[
"Villaseñor",
"Eduardo J. S.",
""
]
] | We study the general form of the possible kinetic terms for 2-form fields in four dimensions, under the restriction that they have a semibounded energy density. This is done by using covariant symplectic techniques and generalizes previous partial results in this direction. | 14.639201 | 12.248104 | 12.964747 | 12.167629 | 12.047433 | 10.983438 | 10.701612 | 13.40185 | 12.62748 | 13.715472 | 11.924511 | 11.435947 | 13.235337 | 12.226373 | 12.746447 | 11.894801 | 12.168429 | 11.61345 | 12.1264 | 12.038213 | 12.082523 |
hep-th/0001014 | Franz-Marc Boas | Franz-Marc Boas | Gauge theories in local causal perturbation theory | PhD thesis, 84 pages | null | null | DESY-THESIS-1999-032, ISSN 1435-8085 | hep-th | null | In this thesis quantum gauge theories are considered in the framework of
local, causal perturbation theory. Gauge invariance is described in terms of
the BRS formalism. Local interacting field operators are constructed
perturbatively and field equations are established. A nilpotent BRS
transformation is defined on th... | [
{
"created": "Tue, 4 Jan 2000 16:00:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Boas",
"Franz-Marc",
""
]
] | In this thesis quantum gauge theories are considered in the framework of local, causal perturbation theory. Gauge invariance is described in terms of the BRS formalism. Local interacting field operators are constructed perturbatively and field equations are established. A nilpotent BRS transformation is defined on the ... | 11.148473 | 12.68447 | 11.968548 | 10.903165 | 11.574478 | 12.31879 | 12.088738 | 10.518427 | 11.217045 | 12.513672 | 10.913079 | 10.162571 | 10.743764 | 10.707483 | 10.593455 | 10.628202 | 10.948081 | 10.508717 | 10.23638 | 11.050239 | 10.105733 |
1804.04045 | Kimball A. Milton | Prachi Parashar, Kimball A. Milton, Yang Li, Hannah Day, Xin Guo,
Stephen A. Fulling, and Ines Cavero-Pelaez | Quantum Electromagnetic Stress Tensor in an Inhomogeneous Medium | 24 pages, 6 figures | Phys. Rev. D 97, 125009 (2018) | 10.1103/PhysRevD.97.125009 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Continuing a program of examining the behavior of the vacuum expectation
value of the stress tensor in a background which varies only in a single
direction, we here study the electromagnetic stress tensor in a medium with
permittivity depending on a single spatial coordinate, specifically, a planar
dielectric half-sp... | [
{
"created": "Wed, 11 Apr 2018 15:24:28 GMT",
"version": "v1"
}
] | 2018-06-20 | [
[
"Parashar",
"Prachi",
""
],
[
"Milton",
"Kimball A.",
""
],
[
"Li",
"Yang",
""
],
[
"Day",
"Hannah",
""
],
[
"Guo",
"Xin",
""
],
[
"Fulling",
"Stephen A.",
""
],
[
"Cavero-Pelaez",
"Ines",
""
]
] | Continuing a program of examining the behavior of the vacuum expectation value of the stress tensor in a background which varies only in a single direction, we here study the electromagnetic stress tensor in a medium with permittivity depending on a single spatial coordinate, specifically, a planar dielectric half-spac... | 10.240979 | 9.58937 | 10.247342 | 9.609939 | 9.648401 | 9.150512 | 9.585655 | 9.196743 | 9.15377 | 10.095573 | 9.583589 | 9.131707 | 9.175381 | 9.159106 | 9.123775 | 8.885118 | 9.17759 | 8.978277 | 9.450055 | 9.112468 | 9.439714 |
hep-th/0002035 | Julia | B. Julia | Superdualities: Below and beyond U-duality | Based on talks delivered at Utrecht, Bures sur Yvette, Tel-Aviv and
Dubna to appear in Proceedings: ``Supersymmetries and Quantum Symmetries'' | null | null | LPTENS-00/02 | hep-th | null | Hidden symmetries are the backbone of Integrable two-dimensional theories.
They provide classical solutions of higher dimensional models as well, they
seem to survive partially quantisation and their discrete remnants in M-theory
called U-dualities, would provide a way to control infinities and
nonperturbative effect... | [
{
"created": "Fri, 4 Feb 2000 13:08:34 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Julia",
"B.",
""
]
] | Hidden symmetries are the backbone of Integrable two-dimensional theories. They provide classical solutions of higher dimensional models as well, they seem to survive partially quantisation and their discrete remnants in M-theory called U-dualities, would provide a way to control infinities and nonperturbative effects ... | 17.241621 | 17.842979 | 18.649141 | 16.539124 | 16.425476 | 19.236376 | 16.219687 | 16.481024 | 16.561321 | 17.993599 | 16.233437 | 15.642393 | 16.022638 | 15.931495 | 15.971538 | 15.898236 | 16.003626 | 15.550035 | 15.805106 | 15.592651 | 16.039864 |
hep-th/9506191 | Sailer | K. Sailer, and W. Greiner | Renormalized finite temperature effective potential of $SU(2)$
Yang-Mills theory | 46 pages, LATEX, 5 figures, figures available upon request,
(submitted to Wigner Memorial Vol. of Heavy-Ion Phys. (Acta Phys. Hung.)) | null | 10.1007/BF03053628 | KLTE-DTP/1995/2 | hep-th | null | It is shown that the renormalized finite temperature effective potential for
continuum $SU(2)$ Yang-Mills theory develops a non-perturbative minimum for
sufficiently strong coupling, i.e. below a critical temperature. The
corresponding phase can be the candidate for the confining phase of the
continuum theory and bec... | [
{
"created": "Thu, 29 Jun 1995 11:35:45 GMT",
"version": "v1"
}
] | 2022-02-23 | [
[
"Sailer",
"K.",
""
],
[
"Greiner",
"W.",
""
]
] | It is shown that the renormalized finite temperature effective potential for continuum $SU(2)$ Yang-Mills theory develops a non-perturbative minimum for sufficiently strong coupling, i.e. below a critical temperature. The corresponding phase can be the candidate for the confining phase of the continuum theory and becom... | 10.059216 | 10.406591 | 10.215442 | 9.168135 | 9.982801 | 10.82426 | 10.351373 | 9.805051 | 10.023911 | 9.776596 | 9.676888 | 9.559436 | 9.542643 | 9.71517 | 9.312873 | 9.696234 | 9.364601 | 9.755525 | 9.512513 | 9.714899 | 9.385942 |
2404.16230 | Bekir Can L\"utf\"uo\u{g}lu | B. Hamil and B.C. L\"utf\"uo\u{g}lu | Pair creation in a space with spin noncommutativity of coordinates | 12 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Schwinger pair creation process for Dirac fermions in the
presence of a Volkov plane wave and a constant external electric field by
applying spin non-commutativity of coordinates. Using the Schwinger proper time
method, the probability of pair creation from vacuum is calculated precisely
and analytically... | [
{
"created": "Wed, 24 Apr 2024 22:05:02 GMT",
"version": "v1"
}
] | 2024-04-26 | [
[
"Hamil",
"B.",
""
],
[
"Lütfüoğlu",
"B. C.",
""
]
] | We study the Schwinger pair creation process for Dirac fermions in the presence of a Volkov plane wave and a constant external electric field by applying spin non-commutativity of coordinates. Using the Schwinger proper time method, the probability of pair creation from vacuum is calculated precisely and analytically. ... | 7.419128 | 7.3686 | 6.597103 | 6.987265 | 7.776273 | 8.146757 | 8.015073 | 7.286411 | 6.929595 | 7.638405 | 7.193064 | 7.058558 | 7.422513 | 7.060723 | 6.846647 | 7.059696 | 6.798586 | 6.996496 | 6.767766 | 7.250463 | 6.794975 |
1712.02233 | Georgi Dvali | Gia Dvali | Area Law Micro-State Entropy from Criticality and Spherical Symmetry | 7 pages | Phys. Rev. D 97, 105005 (2018) | 10.1103/PhysRevD.97.105005 | null | hep-th cond-mat.quant-gas gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is often assumed that the area law of micro-state entropy and the
holography are intrinsic properties exclusively of the gravitational systems,
such as black holes. We construct a non-gravitational model that exhibits an
entropy that scales as area of a sphere of one dimension less. It is
represented by a non-rela... | [
{
"created": "Wed, 6 Dec 2017 15:34:42 GMT",
"version": "v1"
}
] | 2018-05-16 | [
[
"Dvali",
"Gia",
""
]
] | It is often assumed that the area law of micro-state entropy and the holography are intrinsic properties exclusively of the gravitational systems, such as black holes. We construct a non-gravitational model that exhibits an entropy that scales as area of a sphere of one dimension less. It is represented by a non-relati... | 7.33933 | 6.91025 | 7.004911 | 6.803781 | 6.769582 | 7.199238 | 7.16618 | 7.04236 | 6.880173 | 8.603025 | 6.753405 | 6.969215 | 7.08682 | 6.902917 | 7.030641 | 7.293995 | 6.989566 | 7.013389 | 7.146616 | 7.232355 | 6.867156 |
1104.3043 | Roberto Casadio | G.L. Alberghi, R. Casadio, O. Micu, A. Orlandi | Brane-world black holes and the scale of gravity | 4 pages, no figure | null | 10.1007/JHEP09(2011)023 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A particle in four dimensions should behave like a classical black hole if
the horizon radius is larger than the Compton wavelength or, equivalently, if
its degeneracy (measured by entropy in units of the Planck scale) is large. For
spherically symmetric black holes in 4 + d dimensions, both arguments again
lead to a... | [
{
"created": "Fri, 15 Apr 2011 13:10:31 GMT",
"version": "v1"
}
] | 2015-05-27 | [
[
"Alberghi",
"G. L.",
""
],
[
"Casadio",
"R.",
""
],
[
"Micu",
"O.",
""
],
[
"Orlandi",
"A.",
""
]
] | A particle in four dimensions should behave like a classical black hole if the horizon radius is larger than the Compton wavelength or, equivalently, if its degeneracy (measured by entropy in units of the Planck scale) is large. For spherically symmetric black holes in 4 + d dimensions, both arguments again lead to a m... | 10.560663 | 12.295089 | 10.636598 | 10.001809 | 11.755054 | 12.003386 | 11.700526 | 10.708621 | 10.074664 | 12.379241 | 10.698894 | 10.381778 | 10.266961 | 10.053779 | 10.310163 | 10.382501 | 10.992241 | 10.490415 | 10.138646 | 10.782459 | 10.269875 |
1201.3604 | Gabriele Honecker | Gabriele Honecker and Joris Vanhoof | Yukawa couplings and masses of non-chiral states for the Standard Model
on D6-branes on T6/Z6' | 52 pages (including 8p. appendix); 5 figures; 14 tables; v2:
discussion in section 4.1.3 extended, footnote 5 added, typos corrected,
accepted by JHEP | null | 10.1007/JHEP04(2012)085 | MZ-TH/12-04 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The perturbative leading order open string three-point couplings for the
Standard Model with hidden USp(6) on fractional D6-branes on T6/Z6' from
arXiv:0806.3039 [hep-th], arXiv:0910.0843 [hep-th] are computed. Physical
Yukawa couplings consisting of holomorphic Wilsonian superpotential terms times
a non-holomorphic ... | [
{
"created": "Tue, 17 Jan 2012 20:10:47 GMT",
"version": "v1"
},
{
"created": "Fri, 30 Mar 2012 12:34:36 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Honecker",
"Gabriele",
""
],
[
"Vanhoof",
"Joris",
""
]
] | The perturbative leading order open string three-point couplings for the Standard Model with hidden USp(6) on fractional D6-branes on T6/Z6' from arXiv:0806.3039 [hep-th], arXiv:0910.0843 [hep-th] are computed. Physical Yukawa couplings consisting of holomorphic Wilsonian superpotential terms times a non-holomorphic pr... | 14.374134 | 14.157946 | 15.181615 | 12.110949 | 13.740819 | 13.39876 | 11.486918 | 11.840179 | 12.394785 | 16.585884 | 12.099664 | 12.299824 | 12.687504 | 12.481603 | 13.010806 | 12.64707 | 13.004783 | 12.628221 | 12.542397 | 13.327542 | 13.13954 |
1604.08765 | Esperanza Lopez | Emilia da Silva, Esperanza Lopez, Javier Mas and Alexandre Serantes | Holographic Quenches with a Gap | 19 pages, 17 figures | null | 10.1007/JHEP06(2016)172 | IFT-UAM/CSIC-16-039 | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In order to holographically model quenches with a gapped final hamiltonian,
we consider a gravity-scalar theory in anti-de Sitter space with an infrared
hard wall. We allow a time dependent profile for the scalar field at the wall.
This induces an energy exchange between bulk and wall and generates an
oscillating sca... | [
{
"created": "Fri, 29 Apr 2016 10:29:33 GMT",
"version": "v1"
}
] | 2016-07-20 | [
[
"da Silva",
"Emilia",
""
],
[
"Lopez",
"Esperanza",
""
],
[
"Mas",
"Javier",
""
],
[
"Serantes",
"Alexandre",
""
]
] | In order to holographically model quenches with a gapped final hamiltonian, we consider a gravity-scalar theory in anti-de Sitter space with an infrared hard wall. We allow a time dependent profile for the scalar field at the wall. This induces an energy exchange between bulk and wall and generates an oscillating scala... | 10.804307 | 10.30931 | 12.017328 | 10.190739 | 10.993433 | 10.097243 | 9.837423 | 10.143337 | 9.890907 | 12.407043 | 10.055923 | 9.659431 | 10.102198 | 9.989666 | 9.919039 | 9.71486 | 9.884105 | 9.808639 | 10.08132 | 10.412345 | 9.760899 |
hep-th/0205181 | Miloslav Znojil | Miloslav Znojil, Frantisek Gemperle and Omar Mustafa | Asymptotic solvability of an imaginary cubic oscillator with spikes | 20 pages and 2 figures | J.Phys.A35:5781-5793,2002 | 10.1088/0305-4470/35/27/317 | null | hep-th | null | For the PT symmetric potential of Dorey, Dunning and Tateo we show that in
the large angular momentum (i.e., strongly spiked) limit the low-lying
eigenstates of this popular non-Hermitian problem coincide with the shifted
Hermitian harmonic oscillators calculated at the zero angular momentum. This
type of an approxim... | [
{
"created": "Fri, 17 May 2002 14:18:06 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Znojil",
"Miloslav",
""
],
[
"Gemperle",
"Frantisek",
""
],
[
"Mustafa",
"Omar",
""
]
] | For the PT symmetric potential of Dorey, Dunning and Tateo we show that in the large angular momentum (i.e., strongly spiked) limit the low-lying eigenstates of this popular non-Hermitian problem coincide with the shifted Hermitian harmonic oscillators calculated at the zero angular momentum. This type of an approximat... | 19.155922 | 18.577383 | 22.426537 | 19.815516 | 19.582884 | 20.605776 | 22.210606 | 18.854738 | 19.745232 | 24.460524 | 19.167221 | 17.418896 | 17.688696 | 16.988821 | 17.13044 | 16.786549 | 16.965178 | 17.23424 | 16.504848 | 17.252842 | 17.048452 |
hep-th/0106058 | Gregory Gabadadze | Gia Dvali, Gregory Gabadadze, Marko Kolanovic, Francesco Nitti | Scales of Gravity | 51 pages; 7 ps figures; v2 minor improvements | Phys.Rev.D65:024031,2002 | 10.1103/PhysRevD.65.024031 | NYU-TH-01/06/03; TPI-MINN-01/26 | hep-th hep-ph | null | We propose a framework in which the quantum gravity scale can be as low as
$10^{-3}$ eV. The key assumption is that the Standard Model ultraviolet cutoff
is much higher than the quantum gravity scale. This ensures that we observe
conventional weak gravity. We construct an explicit brane-world model in which
the brane... | [
{
"created": "Thu, 7 Jun 2001 05:21:27 GMT",
"version": "v1"
},
{
"created": "Sun, 15 Jul 2001 23:36:08 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Dvali",
"Gia",
""
],
[
"Gabadadze",
"Gregory",
""
],
[
"Kolanovic",
"Marko",
""
],
[
"Nitti",
"Francesco",
""
]
] | We propose a framework in which the quantum gravity scale can be as low as $10^{-3}$ eV. The key assumption is that the Standard Model ultraviolet cutoff is much higher than the quantum gravity scale. This ensures that we observe conventional weak gravity. We construct an explicit brane-world model in which the brane-l... | 7.700274 | 9.045996 | 7.973277 | 8.018209 | 8.360519 | 8.125555 | 8.395924 | 8.354843 | 8.156363 | 8.563153 | 7.933751 | 8.19733 | 7.908234 | 7.915493 | 7.81619 | 8.0796 | 8.052115 | 7.947542 | 8.08484 | 8.060494 | 7.98646 |
hep-th/9911247 | Ivangoe Pestov | I.B. Pestov | K\"ahler Fermions on the Weitzenb\"ock space-time | LATeX, 7 pages, no figures and tables | null | null | JINR E2-96-423 | hep-th | null | The K\"ahler-Dirac equation is derived on the Weitzenb\"ock space-time, which
has a quadruplet of parallel vector fields as the fundamental structure. A
consistent system of equations for the K\"ahler fields and parallel vector
fields is obtained.
Key words: teleparallelism, fermions, internal symmetry, equations.
| [
{
"created": "Tue, 30 Nov 1999 08:32:49 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Pestov",
"I. B.",
""
]
] | The K\"ahler-Dirac equation is derived on the Weitzenb\"ock space-time, which has a quadruplet of parallel vector fields as the fundamental structure. A consistent system of equations for the K\"ahler fields and parallel vector fields is obtained. Key words: teleparallelism, fermions, internal symmetry, equations. | 14.369559 | 12.745386 | 9.945037 | 10.495451 | 10.922953 | 14.879456 | 13.200637 | 10.25274 | 11.000465 | 12.331318 | 12.134336 | 11.48628 | 10.269111 | 10.590549 | 10.33049 | 11.926279 | 11.050935 | 10.900779 | 11.161395 | 9.988184 | 11.443674 |
hep-th/9509096 | Henrik Aratyn | H. Aratyn, L.A. Ferreira, J.F. Gomes and A.H. Zimerman | Constrained KP Models as Integrable Matrix Hierarchies | LaTeX, 19 pgs | J.Math.Phys.38:1559-1576,1997 | 10.1063/1.531908 | IFT-P/041/95, UICHEP-TH/95-9 | hep-th nlin.SI solv-int | null | We formulate the constrained KP hierarchy (denoted by \cKP$_{K+1,M}$) as an
affine ${\widehat {sl}} (M+K+1)$ matrix integrable hierarchy generalizing the
Drinfeld-Sokolov hierarchy. Using an algebraic approach, including the graded
structure of the generalized Drinfeld-Sokolov hierarchy, we are able to find
several n... | [
{
"created": "Fri, 15 Sep 1995 21:29:32 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Aratyn",
"H.",
""
],
[
"Ferreira",
"L. A.",
""
],
[
"Gomes",
"J. F.",
""
],
[
"Zimerman",
"A. H.",
""
]
] | We formulate the constrained KP hierarchy (denoted by \cKP$_{K+1,M}$) as an affine ${\widehat {sl}} (M+K+1)$ matrix integrable hierarchy generalizing the Drinfeld-Sokolov hierarchy. Using an algebraic approach, including the graded structure of the generalized Drinfeld-Sokolov hierarchy, we are able to find several new... | 10.061563 | 10.943404 | 10.849622 | 9.245708 | 9.906973 | 9.624465 | 9.937293 | 9.409284 | 9.264491 | 11.421917 | 9.571173 | 9.40165 | 9.664361 | 9.177585 | 9.511088 | 9.693649 | 9.025757 | 9.419216 | 9.3364 | 10.291074 | 9.579747 |
1712.10071 | Paul K. Townsend | Eric A. Bergshoeff, Jan Rosseel, Paul K. Townsend | Gravity and the spin-2 planar Schroedinger equation | 5 pages. Additional references, with discussion, in v2, plus improved
analysis of parity violation | Phys. Rev. Lett. 120, 141601 (2018) | 10.1103/PhysRevLett.120.141601 | DAMTP-2017-47 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A Schroedinger equation proposed for the GMP gapped spin-2 mode of fractional
Quantum Hall states is found from a novel non-relativistic limit, applicable
only in 2+1 dimensions, of the massive spin-2 Fierz-Pauli field equations. It
is also found from a novel null reduction of the linearized Einstein field
equations ... | [
{
"created": "Thu, 28 Dec 2017 22:19:55 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Mar 2018 22:33:21 GMT",
"version": "v2"
}
] | 2018-04-11 | [
[
"Bergshoeff",
"Eric A.",
""
],
[
"Rosseel",
"Jan",
""
],
[
"Townsend",
"Paul K.",
""
]
] | A Schroedinger equation proposed for the GMP gapped spin-2 mode of fractional Quantum Hall states is found from a novel non-relativistic limit, applicable only in 2+1 dimensions, of the massive spin-2 Fierz-Pauli field equations. It is also found from a novel null reduction of the linearized Einstein field equations in... | 12.592134 | 11.233354 | 12.307829 | 11.661534 | 11.233571 | 12.177116 | 9.851238 | 10.436196 | 10.788155 | 13.007778 | 10.735901 | 11.194655 | 11.573694 | 10.916405 | 11.061383 | 11.451136 | 11.021152 | 10.862188 | 11.083207 | 11.904007 | 11.110359 |
hep-th/0512281 | Pietro Menotti | Pietro Menotti | Semiclassical and quantum Liouville theory | 12 pages, 1 figure, Contributed to 5th Meeting on Constrained
Dynamics and Quantum Gravity (QG05), Cala Gonone, Sardinia, Italy, 12-16 Sep
2005 | J.Phys.Conf.Ser. 33 (2006) 26-37 | 10.1088/1742-6596/33/1/003 | IFUP-TH/2005-04 | hep-th | null | We develop a functional integral approach to quantum Liouville field theory
completely independent of the hamiltonian approach. To this end on the sphere
topology we solve the Riemann-Hilbert problem for three singularities of finite
strength and a fourth one infinitesimal, by determining perturbatively the
Poincare'... | [
{
"created": "Thu, 22 Dec 2005 09:04:21 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Menotti",
"Pietro",
""
]
] | We develop a functional integral approach to quantum Liouville field theory completely independent of the hamiltonian approach. To this end on the sphere topology we solve the Riemann-Hilbert problem for three singularities of finite strength and a fourth one infinitesimal, by determining perturbatively the Poincare' a... | 10.171397 | 10.637093 | 11.682105 | 10.064113 | 10.009821 | 10.482726 | 10.204571 | 10.924718 | 10.572103 | 11.953704 | 10.61834 | 10.454662 | 10.632179 | 10.14795 | 10.346187 | 10.124082 | 10.30443 | 10.136762 | 10.178151 | 10.682528 | 10.121221 |
1712.09994 | Junjie Rao | Yang An, Yi Li, Zhinan Li, Junjie Rao | All-loop Mondrian Diagrammatics and 4-particle Amplituhedron | 41 pages, 44 figures, 2 appendices. Figures improved for v3 | JHEP 1806 (2018) 023 | 10.1007/JHEP06(2018)023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on 1712.09990 which handles the 4-particle amplituhedron at 3-loop, we
have found an extremely simple pattern, yet far more non-trivial than one might
naturally expect: the all-loop Mondrian diagrammatics. By further simplifying
and rephrasing the key relation of positivity in the amplituhedron setting,
remarka... | [
{
"created": "Thu, 28 Dec 2017 18:54:47 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Jun 2018 11:14:11 GMT",
"version": "v2"
},
{
"created": "Wed, 20 Jun 2018 17:08:27 GMT",
"version": "v3"
}
] | 2018-06-21 | [
[
"An",
"Yang",
""
],
[
"Li",
"Yi",
""
],
[
"Li",
"Zhinan",
""
],
[
"Rao",
"Junjie",
""
]
] | Based on 1712.09990 which handles the 4-particle amplituhedron at 3-loop, we have found an extremely simple pattern, yet far more non-trivial than one might naturally expect: the all-loop Mondrian diagrammatics. By further simplifying and rephrasing the key relation of positivity in the amplituhedron setting, remarkabl... | 19.835014 | 21.264717 | 20.704107 | 19.92626 | 21.313318 | 21.707771 | 21.986986 | 21.84584 | 20.645267 | 24.345779 | 19.664471 | 18.927589 | 19.456467 | 18.994841 | 19.297691 | 18.886925 | 19.456503 | 18.87937 | 19.038702 | 20.137369 | 19.065693 |
1105.5825 | {\Dj}or{\dj}e Radi\v{c}evi\'c | Djordje Radicevic | Connecting the Holographic and Wilsonian Renormalization Groups | 11 pages, 1 figure; metadata modified in v2; added references and
minor changes in v3; v4 as published in JHEP | JHEP 1112:023, 2011 | 10.1007/JHEP12(2011)023 | PUPT-2379 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inspired by the AdS/CFT correspondence, we develop an explicit formal duality
between the planar limit of a d-dimensional gauge theory and a classical field
theory in a (d+1)-dimensional anti-de Sitter space. The key ingredient is the
identification of fields in AdS with generalized Hubbard-Stratonovich
transforms of... | [
{
"created": "Sun, 29 May 2011 21:00:11 GMT",
"version": "v1"
},
{
"created": "Tue, 31 May 2011 04:21:45 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Jul 2011 11:20:46 GMT",
"version": "v3"
},
{
"created": "Tue, 21 Feb 2012 02:43:06 GMT",
"version": "v4"
}
] | 2012-02-22 | [
[
"Radicevic",
"Djordje",
""
]
] | Inspired by the AdS/CFT correspondence, we develop an explicit formal duality between the planar limit of a d-dimensional gauge theory and a classical field theory in a (d+1)-dimensional anti-de Sitter space. The key ingredient is the identification of fields in AdS with generalized Hubbard-Stratonovich transforms of s... | 6.979309 | 6.356566 | 7.196587 | 6.33878 | 6.647105 | 6.803334 | 6.268822 | 6.034994 | 6.186961 | 7.89866 | 6.342331 | 6.434706 | 6.847814 | 6.487336 | 6.794067 | 6.425117 | 6.41837 | 6.210113 | 6.4882 | 6.815016 | 6.353099 |
hep-th/0411087 | Ahmad Ghodsi | Mohsen Alishahiha, Ahmad Ghodsi and Amir E. Mosaffa | On Isolated Conformal Fixed Points and Noncritical String Theory | 17 pages, Latex file | JHEP0501:017,2005 | 10.1088/1126-6708/2005/01/017 | IPM/P-2004/066 | hep-th | null | We search for the gravity description of unidentified field theories at their
conformal fixed points by studying the low energy effective action of six
dimensional noncritical string theory. We find constant dilaton solutions by
solving both the equations of motion and BPS equations. Our solutions include a
free para... | [
{
"created": "Mon, 8 Nov 2004 13:17:27 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Alishahiha",
"Mohsen",
""
],
[
"Ghodsi",
"Ahmad",
""
],
[
"Mosaffa",
"Amir E.",
""
]
] | We search for the gravity description of unidentified field theories at their conformal fixed points by studying the low energy effective action of six dimensional noncritical string theory. We find constant dilaton solutions by solving both the equations of motion and BPS equations. Our solutions include a free parame... | 13.754759 | 12.17907 | 16.105875 | 12.293945 | 14.209987 | 12.297622 | 13.425758 | 12.851354 | 12.872532 | 17.343817 | 12.724452 | 13.13979 | 14.206745 | 13.846602 | 13.114888 | 13.869324 | 13.709863 | 12.963777 | 13.839945 | 14.849863 | 13.043392 |
2304.12945 | Rodolfo Jos\'e Bueno Rogerio | R. J. Bueno Rogerio, R. T. Cavalcanti, J. M. Hoff da Silva, C. H.
Coronado Villalobos | Revisiting Takahashi's inversion theorem in discrete symmetry-based dual
frameworks | 7 pages | Physics Letters A, 481, 129028 (2023) | 10.1016/j.physleta.2023.129028 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The so-called Takahashi's \emph{Inversion Theorem}, the reconstruction of a
given spinor based on its bilinear covariants, are re-examined, considering
alternative dual structures. In contrast to the classical results, where the
Dirac dual structure plays the central role, new duals are built using the
discrete symme... | [
{
"created": "Mon, 24 Apr 2023 16:40:18 GMT",
"version": "v1"
}
] | 2023-07-27 | [
[
"Rogerio",
"R. J. Bueno",
""
],
[
"Cavalcanti",
"R. T.",
""
],
[
"da Silva",
"J. M. Hoff",
""
],
[
"Villalobos",
"C. H. Coronado",
""
]
] | The so-called Takahashi's \emph{Inversion Theorem}, the reconstruction of a given spinor based on its bilinear covariants, are re-examined, considering alternative dual structures. In contrast to the classical results, where the Dirac dual structure plays the central role, new duals are built using the discrete symmetr... | 16.917154 | 14.453897 | 16.824917 | 14.592579 | 15.117226 | 14.300525 | 14.948718 | 14.686956 | 14.456037 | 17.007805 | 14.710042 | 15.009306 | 15.439066 | 14.651122 | 15.040084 | 14.755812 | 14.815087 | 15.465828 | 15.090488 | 15.705765 | 15.803063 |
2210.14801 | Peter West | Kevin Nguyen and Peter West | Universal derivation of the asymptotic charges of bosonic massless
particles | 9 pages, References added and commented on | null | 10.1016/j.physletb.2023.138060 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We present a unified treatment of the conserved asymptotic charges associated
with any bosonic massless particle in any spacetime dimension. In particular we
provide master formulae for the asymptotic charges and the central extensions
in the corresponding charge algebras. These formulae can be explicitly
evaluated f... | [
{
"created": "Wed, 26 Oct 2022 15:50:36 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Jun 2023 14:56:07 GMT",
"version": "v2"
}
] | 2023-08-09 | [
[
"Nguyen",
"Kevin",
""
],
[
"West",
"Peter",
""
]
] | We present a unified treatment of the conserved asymptotic charges associated with any bosonic massless particle in any spacetime dimension. In particular we provide master formulae for the asymptotic charges and the central extensions in the corresponding charge algebras. These formulae can be explicitly evaluated for... | 8.706198 | 8.609205 | 8.43343 | 7.556073 | 8.27938 | 8.465423 | 8.677873 | 8.259332 | 7.607917 | 9.156939 | 8.368559 | 7.983608 | 8.040059 | 7.74129 | 7.596418 | 8.00401 | 7.851454 | 8.239354 | 8.019479 | 8.697387 | 7.693347 |
1507.00260 | Reiji Yoshioka | Hiroshi Itoyama, Reiji Yoshioka | Developments of theory of effective prepotential from extended
Seiberg-Witten system and matrix models | 60 pages, 5 figures, to be submitted to PTEP as an invited review
article and based in part on the talk delivered by one of the authors (H.I.)
in the workshop held at Shizuoka University, Shizuoka, Japan, on December 5,
2014; v2: minor corrections, references added | null | 10.1093/ptep/ptv124 | OCU-PHYS 427 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a semi-pedagogical review of a medium size on the exact determination
of and the role played by the low energy effective prepotential ${\cal F}$ in
QFT with (broken) extended supersymmetry, which began with the work of Seiberg
and Witten in 1994. While paying an attention to an overall view of this
subject la... | [
{
"created": "Wed, 1 Jul 2015 15:28:57 GMT",
"version": "v1"
},
{
"created": "Sun, 5 Jul 2015 12:32:05 GMT",
"version": "v2"
}
] | 2015-09-30 | [
[
"Itoyama",
"Hiroshi",
""
],
[
"Yoshioka",
"Reiji",
""
]
] | This is a semi-pedagogical review of a medium size on the exact determination of and the role played by the low energy effective prepotential ${\cal F}$ in QFT with (broken) extended supersymmetry, which began with the work of Seiberg and Witten in 1994. While paying an attention to an overall view of this subject last... | 14.024487 | 13.638724 | 14.686435 | 13.154396 | 13.925475 | 14.105005 | 13.373072 | 13.961705 | 13.590234 | 17.197077 | 12.894395 | 12.982437 | 14.207649 | 13.303533 | 13.408775 | 12.913682 | 12.894648 | 13.272274 | 13.22506 | 13.902182 | 13.305005 |
1610.02074 | Hideo Suganuma | Hideo Suganuma, Yuya Nakagawa and Kohei Matsumoto (Kyoto U.) | 1+1 Large $N_c$ QCD and its Holographic Dual -Soliton Picture of Baryons
in Single-Flavor World | 5 pages, 3 figures | null | 10.7566/JPSCP.13.020013 | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study baryons in holographic QCD corresponding to 1+1 dimensional
single-flavor ($N_f$=1) QCD for the first time. We formulate 1+1 QCD using an
$S^1$-compactified D2/D8/$\overline{\rm D8}$ branes in the superstring theory,
and describe the baryon as a topological configuration in 1+1 $N_f$=1 QCD,
corresponding to ... | [
{
"created": "Thu, 6 Oct 2016 21:18:02 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Nov 2016 13:59:30 GMT",
"version": "v2"
}
] | 2017-03-08 | [
[
"Suganuma",
"Hideo",
"",
"Kyoto U."
],
[
"Nakagawa",
"Yuya",
"",
"Kyoto U."
],
[
"Matsumoto",
"Kohei",
"",
"Kyoto U."
]
] | We study baryons in holographic QCD corresponding to 1+1 dimensional single-flavor ($N_f$=1) QCD for the first time. We formulate 1+1 QCD using an $S^1$-compactified D2/D8/$\overline{\rm D8}$ branes in the superstring theory, and describe the baryon as a topological configuration in 1+1 $N_f$=1 QCD, corresponding to $\... | 6.887567 | 7.009943 | 7.339889 | 6.786093 | 6.740191 | 7.264604 | 6.848266 | 6.428627 | 6.47665 | 7.549201 | 6.620339 | 6.594196 | 6.999453 | 6.752856 | 6.752217 | 6.716294 | 6.881203 | 6.68676 | 6.815308 | 6.997299 | 6.651265 |
1606.08784 | Michele Maggiore | Michele Maggiore | Nonlocal Infrared Modifications of Gravity. A Review | 58 pages, 12 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review an approach developed in the last few years by our group in which
GR is modified in the infrared, at an effective level, by nonlocal terms
associated to a mass scale. We begin by recalling the notion of quantum
effective action and its associated nonlocalities, illustrating some of their
features with the a... | [
{
"created": "Tue, 28 Jun 2016 16:57:07 GMT",
"version": "v1"
}
] | 2016-06-29 | [
[
"Maggiore",
"Michele",
""
]
] | We review an approach developed in the last few years by our group in which GR is modified in the infrared, at an effective level, by nonlocal terms associated to a mass scale. We begin by recalling the notion of quantum effective action and its associated nonlocalities, illustrating some of their features with the ano... | 9.104429 | 8.626796 | 8.715035 | 8.017812 | 8.810335 | 8.642477 | 9.17327 | 8.748886 | 8.915306 | 8.904186 | 8.826554 | 8.488888 | 8.582338 | 8.544098 | 8.660949 | 8.603081 | 8.649479 | 8.531305 | 8.722443 | 8.606747 | 8.502588 |
2107.03656 | Nick R.D. Zhu | Satoshi Nawata, Rui-Dong Zhu | Instanton counting and O-vertex | 14+17 pages; a mathematica file that can help the readers to check
our results is attached; typos corrected in v5 | JHEP09 (2021) 190 | 10.1007/JHEP09(2021)190 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present closed-form expressions of unrefined instanton partition functions
for gauge groups of type $BCD$ as sums over Young diagrams. For
$\mathrm{SO}(n)$ gauge groups, we provide a fivebrane web picture of our
formula based on the vertex-operator formalism of the topological vertex with a
new type called O-verte... | [
{
"created": "Thu, 8 Jul 2021 07:44:18 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Jul 2021 06:31:48 GMT",
"version": "v2"
},
{
"created": "Wed, 8 Sep 2021 09:04:57 GMT",
"version": "v3"
},
{
"created": "Sat, 7 May 2022 06:17:13 GMT",
"version": "v4"
},
{
"crea... | 2023-02-01 | [
[
"Nawata",
"Satoshi",
""
],
[
"Zhu",
"Rui-Dong",
""
]
] | We present closed-form expressions of unrefined instanton partition functions for gauge groups of type $BCD$ as sums over Young diagrams. For $\mathrm{SO}(n)$ gauge groups, we provide a fivebrane web picture of our formula based on the vertex-operator formalism of the topological vertex with a new type called O-vertex ... | 17.760729 | 14.288433 | 22.305178 | 14.572658 | 13.441093 | 13.516764 | 15.357565 | 15.738823 | 13.727802 | 26.379196 | 13.735987 | 13.617592 | 16.739548 | 14.812678 | 13.485563 | 13.697521 | 14.007784 | 14.801138 | 14.416511 | 16.887373 | 14.064886 |
2307.06355 | Dimitris Skliros P. | Dimitri Skliros | Moving NS Punctures on Super Spheres | 39 pages, no figures. Expanded some of the discussion and added a few
references | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One of the subtleties that has made superstring perturbation theory intricate
at high string loop order is the fact that, as shown by Donagi and Witten,
supermoduli space is not holomorphically projected, nor is it holomorphically
split. In recent years, Sen introduced the notion of vertical integration in
moduli spa... | [
{
"created": "Wed, 12 Jul 2023 18:00:01 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Dec 2023 16:58:06 GMT",
"version": "v2"
}
] | 2023-12-06 | [
[
"Skliros",
"Dimitri",
""
]
] | One of the subtleties that has made superstring perturbation theory intricate at high string loop order is the fact that, as shown by Donagi and Witten, supermoduli space is not holomorphically projected, nor is it holomorphically split. In recent years, Sen introduced the notion of vertical integration in moduli space... | 12.440492 | 13.657389 | 13.7513 | 12.545831 | 14.063705 | 14.474522 | 15.125334 | 12.8658 | 13.475577 | 15.150565 | 12.8741 | 12.123569 | 12.485579 | 11.717773 | 12.129133 | 11.731969 | 12.018514 | 11.788616 | 12.073539 | 12.180685 | 12.124649 |
hep-th/0211104 | Ben Gripaios | B. M. Gripaios (Oxford) | Variational Analysis of Deconfinement in Compact U(1) Gauge Theory | 15 pages | Phys.Rev. D67 (2003) 025023 | 10.1103/PhysRevD.67.025023 | OUTP-02 41P | hep-th hep-lat hep-ph | null | A variational method is used to analyse compact U(1) gauge theory in
2+1-dimensions at finite temperature, T, weak coupling, g and where the
fundamental magnetic monopoles have magnetic charge 2\pi n/g. The theory
undergoes a critical transition from a confining phase at temperatures below
T_c=2g^2/n^2\pi to a deconf... | [
{
"created": "Tue, 12 Nov 2002 12:37:36 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Gripaios",
"B. M.",
"",
"Oxford"
]
] | A variational method is used to analyse compact U(1) gauge theory in 2+1-dimensions at finite temperature, T, weak coupling, g and where the fundamental magnetic monopoles have magnetic charge 2\pi n/g. The theory undergoes a critical transition from a confining phase at temperatures below T_c=2g^2/n^2\pi to a deconfin... | 7.509504 | 7.67983 | 7.617854 | 6.995096 | 7.842954 | 7.840926 | 7.646946 | 7.724191 | 6.873879 | 7.756612 | 7.004629 | 7.137439 | 7.065 | 6.968536 | 6.964753 | 6.992882 | 7.269254 | 7.075329 | 6.769468 | 7.302935 | 7.146045 |
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