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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2203.08799 | Mohammad Reza Setare | M. R. Setare and M. Koohgard | The minimal entanglement wedge cross section in the GMMG/GCFT flat
holography | 20 pages, 3 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We focus on a proper candidate for the entanglement wedge in asymptotically
flat bulk geometries that are described by the generalized minimal massive
gravity (GMMG) in the context of the flat holography. To this end, we describe
the boundary by two dimensional Galilean conformal field theory (GCFT) at the
bipartite ... | [
{
"created": "Wed, 2 Mar 2022 14:19:57 GMT",
"version": "v1"
}
] | 2022-03-18 | [
[
"Setare",
"M. R.",
""
],
[
"Koohgard",
"M.",
""
]
] | We focus on a proper candidate for the entanglement wedge in asymptotically flat bulk geometries that are described by the generalized minimal massive gravity (GMMG) in the context of the flat holography. To this end, we describe the boundary by two dimensional Galilean conformal field theory (GCFT) at the bipartite mi... | 8.751799 | 7.353424 | 10.438321 | 7.409676 | 6.934692 | 6.747882 | 7.456138 | 7.466871 | 7.036797 | 11.050521 | 7.109993 | 7.965071 | 9.032621 | 8.173885 | 8.370317 | 8.122143 | 8.128454 | 8.292227 | 8.038717 | 9.340223 | 8.244764 |
2310.16522 | Enrique Alvarez | Enrique \'Alvarez, Jes\'us Anero and Irene S\'anchez-Ruiz | The origin of the cosmological constant | LaTeX, 17 pages, cosmetic changes | null | null | IFT-UAM/CSIC-23-133 | hep-th | http://creativecommons.org/licenses/by/4.0/ | It is well-known that in unimodular gravity the cosmological constant is not
sourced by a constant energy density, but rather appears as some sort of
integration constant. In this work we try to flesh this out by studying in some
detail a couple of examples, one from cosmology and the other from
gravitational collaps... | [
{
"created": "Wed, 25 Oct 2023 10:16:13 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Dec 2023 13:21:35 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Mar 2024 09:30:36 GMT",
"version": "v3"
}
] | 2024-03-11 | [
[
"Álvarez",
"Enrique",
""
],
[
"Anero",
"Jesús",
""
],
[
"Sánchez-Ruiz",
"Irene",
""
]
] | It is well-known that in unimodular gravity the cosmological constant is not sourced by a constant energy density, but rather appears as some sort of integration constant. In this work we try to flesh this out by studying in some detail a couple of examples, one from cosmology and the other from gravitational collapse. | 9.665087 | 6.449353 | 6.709408 | 6.698457 | 5.876832 | 6.722579 | 6.645908 | 6.705949 | 7.550753 | 7.017725 | 7.350755 | 7.605404 | 7.445296 | 7.374194 | 7.223734 | 7.25913 | 7.676602 | 7.211336 | 7.701683 | 7.944957 | 7.781671 |
1510.08065 | John Terning | Kevin F. Cleary and John Terning | Marginal Breaking of Conformal SUSY QCD | 12 pages, no figures | null | 10.1007/JHEP07(2016)096 | null | hep-th hep-ph | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We provide an example of a 4D theory that exhibits the
Contino-Pomarol-Rattazzi mechanism, where breaking conformal symmetry by an
almost marginal operator leads to a light pseudo-Goldstone boson, the dilaton,
and a parametrically suppressed contribution to vacuum energy. We consider SUSY
QCD at the edge of the confo... | [
{
"created": "Tue, 27 Oct 2015 20:07:36 GMT",
"version": "v1"
}
] | 2016-08-24 | [
[
"Cleary",
"Kevin F.",
""
],
[
"Terning",
"John",
""
]
] | We provide an example of a 4D theory that exhibits the Contino-Pomarol-Rattazzi mechanism, where breaking conformal symmetry by an almost marginal operator leads to a light pseudo-Goldstone boson, the dilaton, and a parametrically suppressed contribution to vacuum energy. We consider SUSY QCD at the edge of the conform... | 7.254438 | 7.048017 | 7.227258 | 6.652386 | 7.19135 | 6.993915 | 6.824775 | 7.330516 | 6.573192 | 7.214162 | 6.343522 | 6.650389 | 7.215251 | 6.861719 | 7.046344 | 7.022432 | 6.890945 | 6.968944 | 6.751657 | 7.418889 | 6.781606 |
hep-th/9410135 | null | A. Aghamohammadi, M. Khorrami and A. Shariati | $h$-Deformation as a Contraction of $q$-Deformation | 6 pages, LaTeX, IPM-94-61 | J. Phys. A 28 (1995) L225 | 10.1088/0305-4470/28/8/001 | null | hep-th | null | We show that $h$-deformation can be obtained, by a singular limit of a
similarity transformation, from $q$-deformation; to be specefic, we obtain
$\GL_h(2)$, its differential structure, its inhomogenous extension, and
$\Uh{\sl(2)}$ from their $q$-deformed counterparts.
| [
{
"created": "Wed, 19 Oct 1994 10:52:27 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Aghamohammadi",
"A.",
""
],
[
"Khorrami",
"M.",
""
],
[
"Shariati",
"A.",
""
]
] | We show that $h$-deformation can be obtained, by a singular limit of a similarity transformation, from $q$-deformation; to be specefic, we obtain $\GL_h(2)$, its differential structure, its inhomogenous extension, and $\Uh{\sl(2)}$ from their $q$-deformed counterparts. | 16.762405 | 13.086103 | 16.321844 | 13.201458 | 15.269043 | 16.426355 | 15.548003 | 12.247125 | 12.89032 | 20.591738 | 13.475141 | 13.270565 | 15.745005 | 13.704463 | 13.93737 | 13.299918 | 13.018113 | 13.328935 | 13.843416 | 14.979036 | 13.982435 |
hep-th/9605162 | Vladimir Smirnov | V.A. Smirnov | Four-dimensional integration by parts with differential renormalization
as a method of evaluation of Feynman diagrams | 6 pages, latex | Theor.Math.Phys. 108 (1997) 953-957; Teor.Mat.Fiz. 108N1 (1996)
129-134 | 10.1007/BF02070521 | null | hep-th hep-ph | null | It is shown how strictly four-dimensional integration by parts combined with
differential renormalization and its infrared analogue can be applied for
calculation of Feynman diagrams.
| [
{
"created": "Wed, 22 May 1996 20:55:40 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Smirnov",
"V. A.",
""
]
] | It is shown how strictly four-dimensional integration by parts combined with differential renormalization and its infrared analogue can be applied for calculation of Feynman diagrams. | 30.705626 | 25.961073 | 20.186266 | 21.381565 | 26.933542 | 27.297096 | 23.163673 | 17.815546 | 20.244343 | 24.833132 | 24.280397 | 23.915545 | 24.34697 | 23.841476 | 26.871395 | 23.430771 | 24.704742 | 22.520525 | 22.881123 | 22.9596 | 24.450092 |
0912.5457 | Alexey Koshelev | Alexey S. Koshelev | SFT non-locality in cosmology: solutions, perturbations and
observational evidences | To be published in Proceedings of Invisible Universe 2009 | AIP Conf.Proc.1241:630-638,2010 | 10.1063/1.3462695 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note cosmological models coming out of the String Field Theory (SFT)
in application to the Dark Energy are reviewed. A way of constructing solutions
in the case of linear models is outlined, cosmological perturbations and
observational evidences of such models are explored. We explicitly demonstrate
the stabi... | [
{
"created": "Wed, 30 Dec 2009 20:56:27 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Koshelev",
"Alexey S.",
""
]
] | In this note cosmological models coming out of the String Field Theory (SFT) in application to the Dark Energy are reviewed. A way of constructing solutions in the case of linear models is outlined, cosmological perturbations and observational evidences of such models are explored. We explicitly demonstrate the stabili... | 20.36837 | 19.786104 | 19.052788 | 19.382257 | 20.094921 | 20.294886 | 18.21398 | 19.441967 | 20.059425 | 18.688051 | 19.250614 | 18.344116 | 18.53405 | 17.368649 | 17.932369 | 18.277252 | 18.84602 | 17.232784 | 17.825087 | 17.273926 | 18.660772 |
0902.3930 | Davide Fioravanti | Diego Bombardelli, Davide Fioravanti and Roberto Tateo | Thermodynamic Bethe Ansatz for planar AdS/CFT: a proposal | Main typos corrected, notations fixed, references added | J.Phys.A42:375401,2009 | 10.1088/1751-8113/42/37/375401 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Moving from the mirror theory Bethe-Yang equations proposed by Arutyunov and
Frolov, we derive the thermodynamic Bethe Ansatz equations which should control
the spectrum of the planar $\text{AdS}_5/\text{CFT}_4$ correspondence. The
associated set of universal functional relations (Y-system) satisfied by the
exponenti... | [
{
"created": "Mon, 23 Feb 2009 20:51:52 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Mar 2009 20:53:42 GMT",
"version": "v2"
}
] | 2009-09-28 | [
[
"Bombardelli",
"Diego",
""
],
[
"Fioravanti",
"Davide",
""
],
[
"Tateo",
"Roberto",
""
]
] | Moving from the mirror theory Bethe-Yang equations proposed by Arutyunov and Frolov, we derive the thermodynamic Bethe Ansatz equations which should control the spectrum of the planar $\text{AdS}_5/\text{CFT}_4$ correspondence. The associated set of universal functional relations (Y-system) satisfied by the exponential... | 8.974166 | 9.383659 | 11.911536 | 8.392141 | 8.738745 | 9.693599 | 8.56007 | 8.015294 | 8.122574 | 15.786904 | 8.219621 | 7.906053 | 10.351985 | 8.127353 | 7.874113 | 7.979916 | 7.821782 | 7.928035 | 8.092832 | 9.797919 | 7.981528 |
0801.4536 | Oleg Evnin | Ben Craps, Frederik De Roo and Oleg Evnin | Quantum evolution across singularities: the case of geometrical
resolutions | 25 pages, 1 figure | JHEP 0804:036,2008 | 10.1088/1126-6708/2008/04/036 | null | hep-th | null | We continue the study of time-dependent Hamiltonians with an isolated
singularity in their time dependence, describing propagation on singular
space-times. In previous work, two of us have proposed a "minimal subtraction"
prescription for the simplest class of such systems, involving Hamiltonians
with only one singul... | [
{
"created": "Tue, 29 Jan 2008 17:48:03 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Craps",
"Ben",
""
],
[
"De Roo",
"Frederik",
""
],
[
"Evnin",
"Oleg",
""
]
] | We continue the study of time-dependent Hamiltonians with an isolated singularity in their time dependence, describing propagation on singular space-times. In previous work, two of us have proposed a "minimal subtraction" prescription for the simplest class of such systems, involving Hamiltonians with only one singular... | 14.515207 | 16.498898 | 16.378265 | 13.8188 | 15.6228 | 16.765465 | 15.607 | 15.575252 | 14.04484 | 15.848494 | 14.471937 | 13.822414 | 14.150761 | 13.789966 | 14.35871 | 14.228622 | 14.31677 | 14.056883 | 14.138526 | 14.233865 | 13.937686 |
hep-th/0412281 | Ian Vernon | David Jennings, Ian R. Vernon, Anne-Christine Davis, Carsten van de
Bruck | Bulk black holes radiating in non-Z_2 brane-world spacetimes | 29 pages, 10 figures | JCAP 0504 (2005) 013 | 10.1088/1475-7516/2005/04/013 | DCPT-04/43 | hep-th | null | In this paper we present a general asymmetric brane model involving arbitrary
energy transport to and from an embedded 4-D FRW universe. We derive a locally
defined mass function for the 5D spacetime and describe its time evolution on
the brane. We then specialise our model to the two cases of graviton production
in ... | [
{
"created": "Wed, 22 Dec 2004 22:15:55 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Jennings",
"David",
""
],
[
"Vernon",
"Ian R.",
""
],
[
"Davis",
"Anne-Christine",
""
],
[
"van de Bruck",
"Carsten",
""
]
] | In this paper we present a general asymmetric brane model involving arbitrary energy transport to and from an embedded 4-D FRW universe. We derive a locally defined mass function for the 5D spacetime and describe its time evolution on the brane. We then specialise our model to the two cases of graviton production in th... | 17.238365 | 16.051279 | 15.599968 | 14.192146 | 14.113508 | 15.789431 | 14.934954 | 15.293592 | 15.509762 | 17.860796 | 15.574352 | 14.694624 | 14.96169 | 14.676147 | 15.482249 | 15.491772 | 15.166984 | 14.393148 | 15.342274 | 14.923677 | 15.038703 |
hep-th/9509041 | Ayse Humeyra Bilge | Ayse Humeyra Bilge, Tekin Dereli, Sahin Kocak | An Explicit Construction of Self-dual 2-forms in Eight Dimensions | null | null | null | null | hep-th | null | The geometry of self-dual 2-forms in eight dimensions is studied. These
2-forms determine an $n^2-n+1$ dimensional manifold ${\cal S}_{2n}$. We prove
that for add $n$, it has only one dimensionallinear subspaces. In eight
dimensions, the self-dual forms of Corrigan et al constitue a seven dimensional
linear subspace ... | [
{
"created": "Fri, 8 Sep 1995 15:04:41 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bilge",
"Ayse Humeyra",
""
],
[
"Dereli",
"Tekin",
""
],
[
"Kocak",
"Sahin",
""
]
] | The geometry of self-dual 2-forms in eight dimensions is studied. These 2-forms determine an $n^2-n+1$ dimensional manifold ${\cal S}_{2n}$. We prove that for add $n$, it has only one dimensionallinear subspaces. In eight dimensions, the self-dual forms of Corrigan et al constitue a seven dimensional linear subspace of... | 13.866222 | 13.184586 | 17.08115 | 13.156752 | 14.34401 | 15.90481 | 15.225373 | 13.544822 | 14.884697 | 18.665834 | 13.791458 | 13.21333 | 14.562485 | 13.716146 | 14.252974 | 13.028108 | 13.810632 | 13.850816 | 14.105909 | 14.758835 | 13.584578 |
1302.0529 | Oscar Loaiza-Brito | Cesar Damian, Luis R. Diaz-Barron, Oscar Loaiza-Brito and M. Sabido | Slow-Roll Inflation in Non-geometric Flux Compactification | 26 figures. (v2) Typos corrected. (v3) Eq. (2.7) and two typos on
Table 1 and 2 were corrected. We have added an explicit expression for the
scalar potential and an explanatory note at the end of the introduction.
Results unchanged | null | 10.1007/JHEP06(2013)109 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By implementing a genetic algorithm we search for stable vacua in Type IIB
non-geometric flux compactification on an isotropic torus with orientifold
3-planes. We find that the number of stable dS and AdS vacua are of the same
order. Moreover we find that in all dS vacua the multi-field slow-roll
inflationary conditi... | [
{
"created": "Sun, 3 Feb 2013 20:15:26 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Apr 2013 19:45:50 GMT",
"version": "v2"
},
{
"created": "Sun, 10 Nov 2013 22:34:40 GMT",
"version": "v3"
}
] | 2015-06-12 | [
[
"Damian",
"Cesar",
""
],
[
"Diaz-Barron",
"Luis R.",
""
],
[
"Loaiza-Brito",
"Oscar",
""
],
[
"Sabido",
"M.",
""
]
] | By implementing a genetic algorithm we search for stable vacua in Type IIB non-geometric flux compactification on an isotropic torus with orientifold 3-planes. We find that the number of stable dS and AdS vacua are of the same order. Moreover we find that in all dS vacua the multi-field slow-roll inflationary condition... | 7.807658 | 6.709206 | 7.614582 | 6.491134 | 7.19243 | 7.211974 | 6.860682 | 6.529813 | 6.560388 | 8.66554 | 6.408978 | 6.572856 | 6.978562 | 6.686215 | 6.702497 | 6.579012 | 6.843935 | 6.639023 | 6.601908 | 7.164789 | 6.620047 |
hep-th/9610032 | Enrique Alvarez | Enrique Alvarez and Yuri Kubyshin (UAM Madrid; and MSU Moscow) | Is the String Coupling Constant invariant under T-duality? | LaTeX, 13 pag. Contributions to Santa Margherita and S. Petersburg
meetings | Nucl.Phys.Proc.Suppl. 57 (1997) 44-51 | 10.1016/S0920-5632(97)00352-6 | FTUAM-96/24 | hep-th | null | It is well known that under T-duality the sigma model dilaton (which is
normally thought to be related to the string coupling constant through the
simple formula $\kappa = exp <\phi >$), undergoes an additive shift. On the
other hand, Kugo and Zwiebach, using a simplified form of string field theory,
claim that the s... | [
{
"created": "Mon, 7 Oct 1996 09:49:45 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Alvarez",
"Enrique",
"",
"UAM Madrid; and MSU Moscow"
],
[
"Kubyshin",
"Yuri",
"",
"UAM Madrid; and MSU Moscow"
]
] | It is well known that under T-duality the sigma model dilaton (which is normally thought to be related to the string coupling constant through the simple formula $\kappa = exp <\phi >$), undergoes an additive shift. On the other hand, Kugo and Zwiebach, using a simplified form of string field theory, claim that the str... | 10.506858 | 9.854851 | 10.020026 | 10.582972 | 10.204505 | 10.753755 | 10.236392 | 10.096382 | 9.527221 | 11.084478 | 9.903568 | 9.55433 | 9.634777 | 9.443467 | 9.697659 | 9.66194 | 9.999681 | 9.500167 | 9.69742 | 9.902255 | 9.68938 |
1412.2778 | Mehrdad Mirbabayi | Mehrdad Mirbabayi | Massive Gravity: A Lorentz-Symmetric Aether | 7 pages | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a heuristic introduction to massive gravity based on an analogy with
perfect fluids. I will argue that massive gravity can be thought of as Einstein
gravity in the presence of a medium with unusual properties.
| [
{
"created": "Mon, 8 Dec 2014 21:22:06 GMT",
"version": "v1"
}
] | 2014-12-10 | [
[
"Mirbabayi",
"Mehrdad",
""
]
] | This is a heuristic introduction to massive gravity based on an analogy with perfect fluids. I will argue that massive gravity can be thought of as Einstein gravity in the presence of a medium with unusual properties. | 14.654398 | 11.656053 | 10.965542 | 11.60694 | 9.792191 | 12.196115 | 11.966353 | 11.628606 | 10.376406 | 13.133363 | 11.716991 | 12.372412 | 11.136531 | 11.139413 | 11.636629 | 11.302202 | 11.600262 | 11.384341 | 11.176572 | 11.266935 | 11.585149 |
hep-th/9903045 | Nikolaos Mavromatos | G.A. Diamandis, B.C. Georgalas, N.E. Mavromatos, E. Papantonopoulos | On `Graceful Exit' from inflationary phase in two-dimensional Liouville
String Cosmology | 23 pages LATEX, six eps figures incorporated | Phys.Lett. B461 (1999) 57-65 | 10.1016/S0370-2693(99)00808-4 | NTUA-75/99, OUTP-98-90P, UOA-NPPS-1/99 | hep-th gr-qc | null | Within the context of a super-critical (Liouville) string, we discuss
(target-space) two-dimensional string cosmology. A numerical analysis indicates
that the identification of time with the Liouville mode results in an expanding
universe with matter which exhibits an inflationary phase, and `graceful exit'
from it, ... | [
{
"created": "Thu, 4 Mar 1999 16:36:04 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Diamandis",
"G. A.",
""
],
[
"Georgalas",
"B. C.",
""
],
[
"Mavromatos",
"N. E.",
""
],
[
"Papantonopoulos",
"E.",
""
]
] | Within the context of a super-critical (Liouville) string, we discuss (target-space) two-dimensional string cosmology. A numerical analysis indicates that the identification of time with the Liouville mode results in an expanding universe with matter which exhibits an inflationary phase, and `graceful exit' from it, te... | 11.017636 | 10.13499 | 10.508882 | 9.891606 | 10.773931 | 10.597198 | 10.963246 | 9.821174 | 9.901497 | 10.760822 | 10.074731 | 10.032404 | 10.422563 | 10.083365 | 10.188621 | 9.980193 | 10.396744 | 10.24848 | 10.114356 | 10.659358 | 10.279073 |
1812.04643 | Pesando Igor | Riccardo Finotello, Igor Pesando | The Classical Solution for the Bosonic String in the Presence of Three
D-branes Rotated by Arbitrary SO(4) Elements | 41 pages, 8 figures | null | 10.1016/j.nuclphysb.2019.02.010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the classical instantonic contribution to the open string
configuration associated with three D-branes with relative rotation matrices in
SO(4) which corresponds to the computation of the classical part of the
correlator of three non Abelian twist fields. We write the classical solution
as a sum of a prod... | [
{
"created": "Tue, 11 Dec 2018 19:01:14 GMT",
"version": "v1"
}
] | 2019-03-27 | [
[
"Finotello",
"Riccardo",
""
],
[
"Pesando",
"Igor",
""
]
] | We consider the classical instantonic contribution to the open string configuration associated with three D-branes with relative rotation matrices in SO(4) which corresponds to the computation of the classical part of the correlator of three non Abelian twist fields. We write the classical solution as a sum of a produc... | 14.828261 | 15.360875 | 14.601263 | 13.798319 | 14.915698 | 14.921628 | 15.622479 | 14.109491 | 13.745531 | 16.165127 | 14.446279 | 13.298985 | 13.865232 | 13.478687 | 14.0496 | 13.835927 | 13.347507 | 13.596923 | 13.758005 | 14.507112 | 13.49012 |
2311.16297 | Kazuki Ikeda | Kazuki Ikeda | Quantum-classical simulation of quantum field theory by quantum circuit
learning | null | null | null | null | hep-th cs.LG hep-ph nucl-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We employ quantum circuit learning to simulate quantum field theories (QFTs).
Typically, when simulating QFTs with quantum computers, we encounter
significant challenges due to the technical limitations of quantum devices when
implementing the Hamiltonian using Pauli spin matrices. To address this
challenge, we lever... | [
{
"created": "Mon, 27 Nov 2023 20:18:39 GMT",
"version": "v1"
}
] | 2023-11-29 | [
[
"Ikeda",
"Kazuki",
""
]
] | We employ quantum circuit learning to simulate quantum field theories (QFTs). Typically, when simulating QFTs with quantum computers, we encounter significant challenges due to the technical limitations of quantum devices when implementing the Hamiltonian using Pauli spin matrices. To address this challenge, we leverag... | 10.407649 | 10.082771 | 9.734954 | 9.549773 | 10.109201 | 10.410828 | 10.565818 | 10.52513 | 9.554838 | 10.383276 | 9.929961 | 10.219542 | 9.49182 | 9.598311 | 10.090773 | 10.368413 | 10.051337 | 9.943225 | 9.746497 | 9.531721 | 9.463278 |
1803.07336 | Josef Kluson | J. Kluson | Remark About Non-Relativistic String in Newton-Cartan Background and
Null Reduction | 14 pages,v2:references added, published version | null | 10.1007/JHEP05(2018)041 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze non-relativistic string in Newton-Cartan background that was found
recently in [arXiv:1705.03535 [hep-th]]. We find its Hamiltonian formulation
and study structure of constraints. We also discuss a relation between string
in Newton-Cartan Background and T-duality along null reduction.
| [
{
"created": "Tue, 20 Mar 2018 09:51:39 GMT",
"version": "v1"
},
{
"created": "Thu, 24 May 2018 08:05:43 GMT",
"version": "v2"
}
] | 2018-06-13 | [
[
"Kluson",
"J.",
""
]
] | We analyze non-relativistic string in Newton-Cartan background that was found recently in [arXiv:1705.03535 [hep-th]]. We find its Hamiltonian formulation and study structure of constraints. We also discuss a relation between string in Newton-Cartan Background and T-duality along null reduction. | 12.930384 | 8.388677 | 12.024839 | 9.882665 | 8.963056 | 9.139957 | 8.224611 | 9.42101 | 9.651413 | 12.349545 | 9.268678 | 10.315447 | 12.95569 | 10.558651 | 10.636284 | 10.245514 | 10.275052 | 9.854032 | 9.975525 | 12.383759 | 10.545702 |
1602.03428 | Kirill Krasnov | Yannick Herfray, Kirill Krasnov, Carlos Scarinci and Yuri Shtanov | A 4D gravity theory and G2-holonomy manifolds | 25 pages | Adv.Theor.Math.Phys. 22 (2018) 2001-2034 | 10.4310/ATMP.2018.v22.n8.a5 | null | hep-th gr-qc math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Bryant and Salamon gave a construction of metrics of G2 holonomy on the total
space of the bundle of anti-self-dual (ASD) 2-forms over a 4-dimensional
self-dual Einstein manifold. We generalise it by considering the total space of
an SO(3) bundle (with fibers R^3) over a 4-dimensional base, with a connection
on this ... | [
{
"created": "Wed, 10 Feb 2016 16:08:19 GMT",
"version": "v1"
}
] | 2022-12-06 | [
[
"Herfray",
"Yannick",
""
],
[
"Krasnov",
"Kirill",
""
],
[
"Scarinci",
"Carlos",
""
],
[
"Shtanov",
"Yuri",
""
]
] | Bryant and Salamon gave a construction of metrics of G2 holonomy on the total space of the bundle of anti-self-dual (ASD) 2-forms over a 4-dimensional self-dual Einstein manifold. We generalise it by considering the total space of an SO(3) bundle (with fibers R^3) over a 4-dimensional base, with a connection on this bu... | 6.373455 | 6.212494 | 6.412736 | 5.733707 | 6.480015 | 6.243212 | 6.075379 | 5.930701 | 5.784582 | 6.849553 | 6.254192 | 5.855083 | 5.762708 | 5.696129 | 5.810866 | 5.806196 | 5.710254 | 5.729726 | 5.697636 | 6.116301 | 5.789064 |
1309.4790 | Preston Jones | Preston Jones, Gerardo Munoz, Doug Singleton, Triyanta | Field localization and mass generation in an alternative 5-dimensional
brane model | Presented at APS DPF 2013 - correction made to integrand for scalar
field confinement from the principle reference | null | null | DPF2013-84 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This proceedings is based on a talk given at the APS DPF 2013 on an
alternative 5-dimensional brane world model which is related to but has some
physically distinct features from the Randall-Sundrum brane world model. The
spin dependent localization of 5D fields for the alternative model are
different and in some way... | [
{
"created": "Wed, 18 Sep 2013 20:20:38 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Jun 2015 19:36:34 GMT",
"version": "v2"
}
] | 2015-06-12 | [
[
"Jones",
"Preston",
""
],
[
"Munoz",
"Gerardo",
""
],
[
"Singleton",
"Doug",
""
],
[
"Triyanta",
"",
""
]
] | This proceedings is based on a talk given at the APS DPF 2013 on an alternative 5-dimensional brane world model which is related to but has some physically distinct features from the Randall-Sundrum brane world model. The spin dependent localization of 5D fields for the alternative model are different and in some ways ... | 14.08513 | 15.928327 | 13.959369 | 13.665806 | 14.338785 | 14.696119 | 15.291903 | 13.507779 | 12.992105 | 13.719609 | 14.118267 | 13.791327 | 12.918788 | 13.377658 | 13.048363 | 14.180407 | 13.637085 | 13.053814 | 13.705217 | 13.562963 | 13.909821 |
1910.03603 | Evyatar Sabag | Shlomo S. Razamat and Evyatar Sabag | Sequences of $6d$ SCFTs on generic Riemann surfaces | 57 pages, 27 figures, v3: anomaly notations improved (see footnote 3) | null | 10.1007/JHEP01(2020)086 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider compactifications of $6d$ minimal $(D_{N+3},D_{N+3})$ type
conformal matter SCFTs on a generic Riemann surface. We derive the theories
corresponding to three punctured spheres (trinions) with three maximal
punctures, from which one can construct models corresponding to generic
surfaces. The trinion models... | [
{
"created": "Tue, 8 Oct 2019 18:00:10 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Feb 2020 09:59:57 GMT",
"version": "v2"
},
{
"created": "Thu, 25 Jun 2020 09:52:25 GMT",
"version": "v3"
}
] | 2020-06-26 | [
[
"Razamat",
"Shlomo S.",
""
],
[
"Sabag",
"Evyatar",
""
]
] | We consider compactifications of $6d$ minimal $(D_{N+3},D_{N+3})$ type conformal matter SCFTs on a generic Riemann surface. We derive the theories corresponding to three punctured spheres (trinions) with three maximal punctures, from which one can construct models corresponding to generic surfaces. The trinion models a... | 7.743183 | 6.908165 | 9.28194 | 7.057062 | 7.244588 | 7.125309 | 7.180366 | 7.197608 | 6.902083 | 9.454499 | 7.052582 | 7.444089 | 8.495612 | 7.452477 | 7.49507 | 7.408912 | 7.394482 | 7.350429 | 7.399974 | 8.228148 | 7.410574 |
1604.05181 | Adel Rezaei-Aghdam | M. Aali-Javanangrouh and A. Rezaei-Aghdam | From Basu-Harvey to Nahm equation via 3-Lie bialgebra | 7 pages. Two references are added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the concept of 3-Lie bialgebra; we construct the Bagger- Lambert-
Gustavson (BLG) model on the Manin triple $\cal D$ of the especial 3-Lie
bialgebra $({\cal D},{\cal A}_{\cal G},{\cal A}_{{\cal G}^*}^*)$ which is in
correspondence with Manin triple of Lie bialgebra $({\cal D},{\cal G},{\cal
G}^*)$. We have show... | [
{
"created": "Mon, 18 Apr 2016 14:37:20 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Mar 2018 11:15:40 GMT",
"version": "v2"
}
] | 2018-03-08 | [
[
"Aali-Javanangrouh",
"M.",
""
],
[
"Rezaei-Aghdam",
"A.",
""
]
] | Using the concept of 3-Lie bialgebra; we construct the Bagger- Lambert- Gustavson (BLG) model on the Manin triple $\cal D$ of the especial 3-Lie bialgebra $({\cal D},{\cal A}_{\cal G},{\cal A}_{{\cal G}^*}^*)$ which is in correspondence with Manin triple of Lie bialgebra $({\cal D},{\cal G},{\cal G}^*)$. We have shown ... | 5.411477 | 5.769104 | 6.593989 | 5.22824 | 5.512764 | 5.489084 | 5.548862 | 5.217401 | 5.474575 | 7.262984 | 4.851549 | 5.194792 | 5.358273 | 5.165113 | 5.16578 | 5.122644 | 5.323542 | 5.093294 | 5.193006 | 5.52441 | 5.168604 |
hep-th/0205081 | Ali Tayefeh Rezakhani | M.R. Setare | Trace Anomaly and Backreaction of the Dynamical Casimir Effect | 8 pages, no figures, typos corrected, discussion added, has been
accepted for the publication in GRG | Gen.Rel.Grav. 35 (2003) 2279-2286 | 10.1023/A:1027314126258 | null | hep-th | null | The Casimir energy for massless scalar field which satisfies priodic boundary
conditions in two-dimensional domain wall background is calculated by making
use of general properties of renormalized stress-tensor. The line element of
domain wall is time dependent, the trace anomaly which is the nonvanishing
$T^{\mu}_{\... | [
{
"created": "Thu, 9 May 2002 04:46:20 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Jul 2003 11:24:46 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Setare",
"M. R.",
""
]
] | The Casimir energy for massless scalar field which satisfies priodic boundary conditions in two-dimensional domain wall background is calculated by making use of general properties of renormalized stress-tensor. The line element of domain wall is time dependent, the trace anomaly which is the nonvanishing $T^{\mu}_{\mu... | 12.918702 | 12.667271 | 13.677041 | 12.480918 | 11.908322 | 13.347421 | 12.245528 | 12.210113 | 12.020147 | 13.914805 | 11.748604 | 11.793501 | 11.770636 | 11.846775 | 12.040452 | 11.067416 | 11.536004 | 12.29686 | 12.000295 | 11.60575 | 11.748452 |
1701.05772 | Massimo Taronna | Massimo Taronna | On the Non-Local Obstruction to Interacting Higher Spins in Flat Space | 22+12 pages. v2: typos corrected, references added | null | 10.1007/JHEP05(2017)026 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Owing to a renewed interest in flat space higher spin gauge theories, in this
note we provide further details and clarifications on the results presented in
arXiv:1107.5843 and arXiv: 1209.5755, which investigated their locality
properties. Focusing, for simplicity, on quartic amplitudes with one of the
external legs... | [
{
"created": "Fri, 20 Jan 2017 12:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Mar 2017 15:52:34 GMT",
"version": "v2"
}
] | 2017-05-24 | [
[
"Taronna",
"Massimo",
""
]
] | Owing to a renewed interest in flat space higher spin gauge theories, in this note we provide further details and clarifications on the results presented in arXiv:1107.5843 and arXiv: 1209.5755, which investigated their locality properties. Focusing, for simplicity, on quartic amplitudes with one of the external legs h... | 11.228821 | 10.615269 | 12.148995 | 11.006675 | 11.530261 | 11.365786 | 11.608348 | 11.165977 | 10.659389 | 12.661989 | 10.621933 | 10.265747 | 10.943767 | 10.695826 | 10.535143 | 10.428311 | 10.911344 | 10.603533 | 10.708131 | 10.795892 | 10.470778 |
hep-th/0604019 | Marcelo Gomes | A. F. Ferrari, M. Gomes, J. R. S. Nascimento, A. Yu. Petrov, A. J. da
Silva | On the duality of three-dimensional superfield theories | 18 pages,2 figures, revtex4, v2: corrected references | Phys.Rev.D73:105010,2006 | 10.1103/PhysRevD.73.105010 | null | hep-th | null | Within the superfield approach, we consider the duality between the
supersymmetric Maxwell-Chern-Simons and self-dual theories in three spacetime
dimensions. Using a gauge embedding method, we construct the dual theory to the
self-dual model interacting with a matter superfield, which turns out to be not
the Maxwell-... | [
{
"created": "Tue, 4 Apr 2006 19:49:46 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Apr 2006 20:31:52 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Ferrari",
"A. F.",
""
],
[
"Gomes",
"M.",
""
],
[
"Nascimento",
"J. R. S.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"da Silva",
"A. J.",
""
]
] | Within the superfield approach, we consider the duality between the supersymmetric Maxwell-Chern-Simons and self-dual theories in three spacetime dimensions. Using a gauge embedding method, we construct the dual theory to the self-dual model interacting with a matter superfield, which turns out to be not the Maxwell-Ch... | 7.864372 | 6.483907 | 7.949514 | 6.614372 | 6.622067 | 6.836845 | 6.847505 | 6.5669 | 6.331337 | 8.096147 | 6.669824 | 6.534915 | 7.790892 | 6.944135 | 6.83788 | 6.683317 | 6.835796 | 6.727158 | 6.869277 | 7.493645 | 6.626346 |
1605.03361 | \"Umit Ertem | \"Umit Ertem | Twistor spinors and extended conformal superalgebras | 16 pages, published version | J. Geom. Phys. 152 (2020) 103654 | 10.1016/j.geomphys.2020.103654 | null | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the first-order symmetry operators of twistor spinors can be
constructed from conformal Killing-Yano forms in conformally-flat backgrounds.
We express the conditions on conformal Killing-Yano forms to obtain mutually
commuting symmetry operators of twistor spinors. Conformal superalgebras which
consist o... | [
{
"created": "Wed, 11 May 2016 10:17:28 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Mar 2020 09:23:33 GMT",
"version": "v2"
}
] | 2020-03-30 | [
[
"Ertem",
"Ümit",
""
]
] | We show that the first-order symmetry operators of twistor spinors can be constructed from conformal Killing-Yano forms in conformally-flat backgrounds. We express the conditions on conformal Killing-Yano forms to obtain mutually commuting symmetry operators of twistor spinors. Conformal superalgebras which consist of ... | 5.810108 | 6.027763 | 6.013347 | 5.686023 | 5.541608 | 5.864653 | 5.943294 | 5.520325 | 5.641448 | 6.058156 | 5.532087 | 5.508727 | 5.706629 | 5.563992 | 5.364716 | 5.583833 | 5.299822 | 5.664941 | 5.46481 | 5.834417 | 5.339025 |
1002.1790 | Sven Krippendorf | Sven Krippendorf, Matthew J. Dolan, Anshuman Maharana, Fernando
Quevedo | D-branes at Toric Singularities: Model Building, Yukawa Couplings and
Flavour Physics | 55 pages, v2: typos corrected, minor comments added | JHEP 1006:092,2010 | 10.1007/JHEP06(2010)092 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss general properties of D-brane model building at toric
singularities. Using dimer techniques to obtain the gauge theory from the
structure of the singularity, we extract results on the matter sector and
superpotential of the corresponding gauge theory. We show that the number of
families in toric phases is ... | [
{
"created": "Tue, 9 Feb 2010 14:03:10 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Apr 2010 22:42:53 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Krippendorf",
"Sven",
""
],
[
"Dolan",
"Matthew J.",
""
],
[
"Maharana",
"Anshuman",
""
],
[
"Quevedo",
"Fernando",
""
]
] | We discuss general properties of D-brane model building at toric singularities. Using dimer techniques to obtain the gauge theory from the structure of the singularity, we extract results on the matter sector and superpotential of the corresponding gauge theory. We show that the number of families in toric phases is al... | 9.198215 | 9.477532 | 10.958151 | 9.249397 | 9.069092 | 9.257256 | 8.968187 | 9.924446 | 8.881032 | 11.578052 | 8.951137 | 8.866052 | 9.455757 | 9.282211 | 9.271015 | 9.153902 | 9.01837 | 9.091783 | 8.995067 | 9.287274 | 8.932464 |
hep-th/0008047 | P. S. Howe | P. Heslop and P.S. Howe | Chiral Superfields in IIB Supergravity | 8 pages. Slightly longer version with more detail about the boundary
of AdS superspace | Phys.Lett. B502 (2001) 259-264 | 10.1016/S0370-2693(01)00149-6 | KCL-TH-00-48 | hep-th | null | The field strength superfield of IIB supergravity on $AdS_5\xz S^5$ is
expanded in harmonics on $S^5$ with coefficients which are $D=5, N=8$ chiral
superfields. On the boundary of $AdS_5$ these superfields map to $D=4,N=4$
chiral superfields and both sets of superfields obey additional fourth-order
constraints. The c... | [
{
"created": "Fri, 4 Aug 2000 16:29:13 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Dec 2000 11:17:22 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Heslop",
"P.",
""
],
[
"Howe",
"P. S.",
""
]
] | The field strength superfield of IIB supergravity on $AdS_5\xz S^5$ is expanded in harmonics on $S^5$ with coefficients which are $D=5, N=8$ chiral superfields. On the boundary of $AdS_5$ these superfields map to $D=4,N=4$ chiral superfields and both sets of superfields obey additional fourth-order constraints. The con... | 6.289378 | 5.97203 | 7.082778 | 5.448175 | 5.818814 | 5.260965 | 5.826881 | 5.458978 | 5.935163 | 8.008317 | 5.837628 | 5.741489 | 6.098346 | 5.696183 | 5.643922 | 5.574217 | 5.606981 | 5.642362 | 5.671609 | 6.10498 | 5.660748 |
hep-th/0406031 | David Bailin | D. Bailin & A. Love | Non-minimal Higgs content in standard-like models from D-branes at a Z_N
singularity | LaTeX, 14 pages. A paragraph generalising the results to left-right
symmetric models has been added | Phys.Lett. B598 (2004) 83-91 | 10.1016/j.physletb.2004.07.043 | null | hep-th | null | We show that attempts to construct the standard model, or the MSSM, by
placing D3-branes and D7-branes at a Z_N orbifold or orientifold singularity
all require that the electroweak Higgs content is non-minimal. For the orbifold
the lower bound on the number n(H) + n({\bar{H}}) of electroweak Higgs doublets
is the num... | [
{
"created": "Thu, 3 Jun 2004 08:18:47 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Jun 2004 10:01:22 GMT",
"version": "v2"
},
{
"created": "Thu, 1 Jul 2004 10:54:53 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Bailin",
"D.",
""
],
[
"Love",
"A.",
""
]
] | We show that attempts to construct the standard model, or the MSSM, by placing D3-branes and D7-branes at a Z_N orbifold or orientifold singularity all require that the electroweak Higgs content is non-minimal. For the orbifold the lower bound on the number n(H) + n({\bar{H}}) of electroweak Higgs doublets is the numbe... | 10.832088 | 10.205123 | 9.809487 | 8.878256 | 11.954118 | 10.755216 | 9.899253 | 9.631006 | 9.093827 | 11.07491 | 9.331921 | 10.056346 | 9.697365 | 9.662851 | 9.915559 | 10.02416 | 10.212405 | 10.168393 | 9.518455 | 10.614591 | 9.739969 |
2108.02309 | Washington Taylor | David R. Morrison and Washington Taylor | Charge completeness and the massless charge lattice in F-theory models
of supergravity | 43 pages; v2: comments on charge completeness in M-theory, references
added | null | 10.1007/JHEP12(2021)040 | MIT-CTP-5172, UCSB-MATH-2021-03 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We prove that, for every 6D supergravity theory that has an F-theory
description, the property of charge completeness for the connected component of
the gauge group (meaning that all charges in the corresponding charge lattice
are realized by massive or massless states in the theory) is equivalent to a
standard assum... | [
{
"created": "Wed, 4 Aug 2021 22:57:13 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Aug 2021 19:55:03 GMT",
"version": "v2"
}
] | 2022-01-05 | [
[
"Morrison",
"David R.",
""
],
[
"Taylor",
"Washington",
""
]
] | We prove that, for every 6D supergravity theory that has an F-theory description, the property of charge completeness for the connected component of the gauge group (meaning that all charges in the corresponding charge lattice are realized by massive or massless states in the theory) is equivalent to a standard assumpt... | 9.483816 | 9.126109 | 10.679369 | 8.621494 | 9.211595 | 9.747329 | 9.587372 | 8.998481 | 9.279544 | 11.468007 | 9.135878 | 9.085322 | 9.938203 | 9.296273 | 9.066895 | 9.308113 | 9.531864 | 8.996325 | 9.192634 | 9.834905 | 9.368298 |
1106.3169 | Henryk Arodz | H. Arodz and Z. Swierczynski | Swaying oscillons in the signum-Gordon model | 12 pages, 3 figures | null | 10.1103/PhysRevD.84.067701 | null | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a new class of oscillons in the (1+1)-dimensional signum-Gordon
model. The oscillons periodically move to and fro in the space. They have
finite total energy, finite size, and are strictly periodic in time. The
corresponding solutions of the scalar field equation are explicitly constructed
from the second ... | [
{
"created": "Thu, 16 Jun 2011 08:40:15 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Arodz",
"H.",
""
],
[
"Swierczynski",
"Z.",
""
]
] | We present a new class of oscillons in the (1+1)-dimensional signum-Gordon model. The oscillons periodically move to and fro in the space. They have finite total energy, finite size, and are strictly periodic in time. The corresponding solutions of the scalar field equation are explicitly constructed from the second or... | 10.51052 | 10.820235 | 10.432509 | 8.762355 | 10.486396 | 10.288294 | 10.399926 | 8.996928 | 8.509519 | 12.301575 | 8.923528 | 9.250681 | 9.490479 | 9.479691 | 9.457452 | 9.137732 | 9.276059 | 9.111854 | 9.332633 | 10.164302 | 9.496972 |
hep-th/0009006 | Ellwanger | U. Ellwanger | Brane Universes, AdS/CFT, Hamiltonian Formalism and the Renormalization
Group | 24 pages, 1 fig., based on a lecture at the LPT Orsay | null | null | LPT Orsay 00-64 | hep-th hep-ph | null | The AdS/CFT correspondence is developed from classical solutions on AdS_5
with two boundaries. The corresponding limits and the reduction of degrees of
freedom are discussed, as well as the required renormalization on the field
theory side. The Hamiltonian first-order approach towards the solution of
coupled gravitat... | [
{
"created": "Fri, 1 Sep 2000 13:14:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ellwanger",
"U.",
""
]
] | The AdS/CFT correspondence is developed from classical solutions on AdS_5 with two boundaries. The corresponding limits and the reduction of degrees of freedom are discussed, as well as the required renormalization on the field theory side. The Hamiltonian first-order approach towards the solution of coupled gravitatio... | 16.8827 | 15.935715 | 14.960392 | 14.923175 | 14.855512 | 15.282253 | 15.525186 | 16.432341 | 14.282173 | 14.802673 | 16.179411 | 14.491728 | 15.052176 | 14.709079 | 15.098085 | 15.176219 | 14.740927 | 15.506227 | 14.538859 | 15.026647 | 15.138238 |
hep-th/9703117 | Eduardo Ramos | Eduardo Ramos | Three dimensional strings. I. Classical theory | 15 pages, LaTeX (elsart macros), I drop a conjecture about the
quantization of the model that now seems unwarranted. This does not alter the
results of the paper. A few misprints are also corrected | null | null | FTUAM 97/3 | hep-th | null | I consider a three-dimensional string theory whose action, besides the
standard area term, contains one of the form $\int_{\Sigma}
\epsilon_{\mu\nu\sigma} X^{\mu} d X^{\nu} \wedge d X^{\sigma}$. In the case of
closed strings this extra term has a simple geometrical interpretation as the
volume enclosed by the surface... | [
{
"created": "Mon, 17 Mar 1997 11:52:14 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Apr 1997 12:34:46 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Ramos",
"Eduardo",
""
]
] | I consider a three-dimensional string theory whose action, besides the standard area term, contains one of the form $\int_{\Sigma} \epsilon_{\mu\nu\sigma} X^{\mu} d X^{\nu} \wedge d X^{\sigma}$. In the case of closed strings this extra term has a simple geometrical interpretation as the volume enclosed by the surface. ... | 8.587531 | 9.58612 | 9.2792 | 8.694046 | 10.152642 | 9.028647 | 9.009257 | 8.626904 | 8.932783 | 9.743372 | 9.23407 | 8.281734 | 8.176166 | 8.314964 | 8.256547 | 8.040143 | 8.132344 | 7.97694 | 8.284214 | 8.415514 | 8.012811 |
hep-th/0403197 | Carlo Piccioni | L.Girardello, C.Piccioni, M.Porrati | D-Brane Interactions in a Gravitational Shock Wave Background | To be published in Modern Physics Letters A, revised version with
references added, 12 pages | Mod.Phys.Lett. A19 (2004) 2059-2068 | 10.1142/S0217732304015336 | null | hep-th | null | We study D-branes in the background of a gravitational shock wave. We
consider the case of parallel D-branes located on opposite sides with respect
to the shock wave. Their interaction is studied by evaluating the cylinder
diagram using the boundary states technique. Boundary states are defined at
each D-brane and th... | [
{
"created": "Fri, 19 Mar 2004 20:12:18 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Jul 2004 21:21:03 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Girardello",
"L.",
""
],
[
"Piccioni",
"C.",
""
],
[
"Porrati",
"M.",
""
]
] | We study D-branes in the background of a gravitational shock wave. We consider the case of parallel D-branes located on opposite sides with respect to the shock wave. Their interaction is studied by evaluating the cylinder diagram using the boundary states technique. Boundary states are defined at each D-brane and thei... | 9.808568 | 10.831362 | 10.039664 | 9.422352 | 10.458053 | 9.771446 | 11.11742 | 9.896177 | 10.032284 | 10.318682 | 10.144933 | 9.711303 | 9.342297 | 9.427093 | 10.665962 | 9.928875 | 9.898104 | 9.979881 | 9.648121 | 9.816136 | 9.57884 |
hep-th/0208167 | David A. Lowe | Kevin Goldstein and David A. Lowe | Initial state effects on the cosmic microwave background and
trans-planckian physics | 10 pages, harvmac, references added, expanded discussion | Phys.Rev. D67 (2003) 063502 | 10.1103/PhysRevD.67.063502 | BROWN-HET-1329 | hep-th astro-ph gr-qc | null | There exist a one complex parameter family of de Sitter invariant vacua,
known as alpha vacua. In the context of slow roll inflation, we show that all
but the Bunch-Davies vacuum generates unacceptable production of high energy
particles at the end of inflation. As a simple model for the effects of
trans-planckian ph... | [
{
"created": "Thu, 22 Aug 2002 20:51:13 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Sep 2002 18:26:20 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Goldstein",
"Kevin",
""
],
[
"Lowe",
"David A.",
""
]
] | There exist a one complex parameter family of de Sitter invariant vacua, known as alpha vacua. In the context of slow roll inflation, we show that all but the Bunch-Davies vacuum generates unacceptable production of high energy particles at the end of inflation. As a simple model for the effects of trans-planckian phys... | 9.433343 | 10.369431 | 9.012095 | 8.874868 | 9.348382 | 9.985044 | 10.375872 | 9.313388 | 9.323466 | 10.008692 | 9.524445 | 8.926251 | 9.0315 | 9.101577 | 9.110038 | 9.247554 | 8.9582 | 8.918081 | 9.283471 | 9.121854 | 9.191656 |
1005.4848 | Axel Kleinschmidt | Ling Bao, Axel Kleinschmidt, Bengt E. W. Nilsson, Daniel Persson,
Boris Pioline | Rigid Calabi-Yau threefolds, Picard Eisenstein series and instantons | 8 pages, for the proceedings of Quantum Theories and Symmetries VI | null | null | null | hep-th math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Type IIA string theory compactified on a rigid Calabi-Yau threefold gives
rise to a classical moduli space that carries an isometric action of U(2,1).
Various quantum corrections break this continuous isometry to a discrete
subgroup. Focussing on the case where the intermediate Jacobian of the
Calabi-Yau admits compl... | [
{
"created": "Wed, 26 May 2010 15:41:21 GMT",
"version": "v1"
}
] | 2010-05-27 | [
[
"Bao",
"Ling",
""
],
[
"Kleinschmidt",
"Axel",
""
],
[
"Nilsson",
"Bengt E. W.",
""
],
[
"Persson",
"Daniel",
""
],
[
"Pioline",
"Boris",
""
]
] | Type IIA string theory compactified on a rigid Calabi-Yau threefold gives rise to a classical moduli space that carries an isometric action of U(2,1). Various quantum corrections break this continuous isometry to a discrete subgroup. Focussing on the case where the intermediate Jacobian of the Calabi-Yau admits complex... | 6.156453 | 6.962529 | 8.470059 | 6.47594 | 7.157891 | 6.892556 | 6.978694 | 7.094161 | 6.581355 | 10.395634 | 6.90457 | 6.305746 | 6.630123 | 6.08527 | 6.186435 | 6.251515 | 6.204477 | 6.173362 | 6.037588 | 6.524455 | 6.084519 |
hep-th/0207184 | Laurent Baulieu | L. Baulieu (LPTHE) | Going down from a 3-form in 16 dimensions | 14 pages | Phys.Lett. B544 (2002) 367-373 | 10.1016/S0370-2693(02)02511-X | PAR-LPTHE 02-39 | hep-th | null | Group theory indicates the existence of a $SO(8) X SO(7) \subset SO(16)$
invariant self-duality equation for a 3-form in 16 dimensions. It is a signal
for interesting topological field theories, especially on 8-dimensional
manifolds with holonomy group smaller than or equal to Spin(7), with a gauge
symmetry that is S... | [
{
"created": "Fri, 19 Jul 2002 14:13:12 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Baulieu",
"L.",
"",
"LPTHE"
]
] | Group theory indicates the existence of a $SO(8) X SO(7) \subset SO(16)$ invariant self-duality equation for a 3-form in 16 dimensions. It is a signal for interesting topological field theories, especially on 8-dimensional manifolds with holonomy group smaller than or equal to Spin(7), with a gauge symmetry that is SO(... | 12.882553 | 11.627789 | 13.296059 | 11.838432 | 11.964574 | 11.744243 | 12.205727 | 11.618458 | 12.148478 | 14.590483 | 12.338382 | 11.481095 | 12.113039 | 11.63554 | 11.178179 | 11.568919 | 10.806847 | 11.913093 | 11.436593 | 12.952288 | 12.099563 |
hep-th/9409178 | P. Ramadevi | B. Basu-Mallick and P. Ramadevi | Construction of Yangian algebra through a multi-deformation parameter
dependent rational $R$-matrix | 14 pages plain LATEX | null | null | IMSc preprint-94/38 | hep-th | null | Yang-Baxterising a braid group representation associated with multideformed
version of $GL_{q}(N)$ quantum group and taking the corresponding $q\rightarrow
1$ limit, we obtain a rational $R$-matrix which depends on $\left ( 1+ {N(N-1)
\over 2} \right ) $ number of deformation parameters. By using such rational
$R$-ma... | [
{
"created": "Wed, 28 Sep 1994 19:26:20 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Basu-Mallick",
"B.",
""
],
[
"Ramadevi",
"P.",
""
]
] | Yang-Baxterising a braid group representation associated with multideformed version of $GL_{q}(N)$ quantum group and taking the corresponding $q\rightarrow 1$ limit, we obtain a rational $R$-matrix which depends on $\left ( 1+ {N(N-1) \over 2} \right ) $ number of deformation parameters. By using such rational $R$-matr... | 7.580907 | 7.9303 | 8.442777 | 7.133842 | 6.961057 | 7.763426 | 7.847753 | 7.367566 | 7.110241 | 8.66926 | 7.218104 | 7.370232 | 7.62254 | 7.028507 | 7.119328 | 7.032773 | 7.40388 | 7.148645 | 7.334553 | 7.660515 | 7.100351 |
1102.1219 | Luca Mazzucato | Brenno Carlini Vallilo and Luca Mazzucato | The Konishi multiplet at strong coupling | 4 pages; v2: corrections and improvements, conclusions unchanged | null | 10.1007/JHEP12(2011)029 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a method to compute from first principles the anomalous
dimension of short operators in N=4 super Yang-Mills theory at strong coupling,
where they are described in terms of superstring vertex operators in an anti-de
Sitter background. We focus on the Konishi multiplet, dual to the first massive
level of ... | [
{
"created": "Mon, 7 Feb 2011 00:54:14 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Feb 2011 19:27:56 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Vallilo",
"Brenno Carlini",
""
],
[
"Mazzucato",
"Luca",
""
]
] | We introduce a method to compute from first principles the anomalous dimension of short operators in N=4 super Yang-Mills theory at strong coupling, where they are described in terms of superstring vertex operators in an anti-de Sitter background. We focus on the Konishi multiplet, dual to the first massive level of th... | 5.13613 | 4.678707 | 6.714548 | 4.469319 | 4.361222 | 4.397756 | 4.668663 | 4.524484 | 4.401325 | 6.065053 | 4.69772 | 4.655677 | 5.363976 | 4.538136 | 4.793649 | 4.640997 | 4.398911 | 4.620807 | 4.439355 | 5.310465 | 4.795149 |
hep-th/9403185 | Peter West | P. West | $W$ Strings and Cohomology in Parafermionic Theories | 14 pages, KCL-TH-94-4. A few sentences of clarification are added on
page 11 and equation (27) is extended | Phys.Lett. B329 (1994) 199-207 | 10.1016/0370-2693(94)90761-7 | null | hep-th | null | By enforcing locality we relate the cohomology found in parafermionic
theories to that occurring in $W$ strings. This link provides a systematic
method of finding states in the cohomology of $W_{2,s}$ strings.
| [
{
"created": "Wed, 30 Mar 1994 14:00:06 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Apr 1994 11:44:24 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Apr 1994 13:54:34 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"West",
"P.",
""
]
] | By enforcing locality we relate the cohomology found in parafermionic theories to that occurring in $W$ strings. This link provides a systematic method of finding states in the cohomology of $W_{2,s}$ strings. | 29.858196 | 15.965858 | 25.231306 | 15.254125 | 15.662617 | 14.833965 | 15.776196 | 15.249615 | 15.104847 | 27.548563 | 16.04705 | 17.883472 | 19.088799 | 16.64299 | 17.083393 | 17.321442 | 16.717644 | 16.4207 | 17.196039 | 18.965023 | 16.85327 |
hep-th/0208028 | Kluson Josef | J. Kluson | Time Dependent Solution in Open Bosonic String Field Theory | 13 pages | null | null | null | hep-th | null | In this paper we present time dependent solution of the open bosonic string
field theory describing the motion of the tachyon on unstable D-brane.
| [
{
"created": "Sat, 3 Aug 2002 18:03:57 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kluson",
"J.",
""
]
] | In this paper we present time dependent solution of the open bosonic string field theory describing the motion of the tachyon on unstable D-brane. | 11.513416 | 5.747229 | 10.892764 | 6.320704 | 5.546936 | 6.542473 | 5.666175 | 5.733999 | 5.446126 | 11.063282 | 5.752591 | 6.22892 | 8.457101 | 6.424564 | 6.606093 | 6.51545 | 5.98421 | 6.583052 | 6.085626 | 7.733685 | 6.559957 |
0912.2974 | Everton Murilo Carvalho Abreu | E. M. C. Abreu, A. C. R. Mendes, C. Neves, W. Oliveira, R. C. N. Silva
and C. Wotzasek | Obtaining non-Abelian field theories via Faddeev-Jackiw symplectic
formalism | 6 pages. Revtex 4.1 | Phys.Lett.A374:3603-3607,2010 | 10.1016/j.physleta.2010.07.006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we have shown that it is possible to construct non-Abelian field
theories employing, in a systematic way, the Faddeev-Jackiw symplectic
formalism. This approach follows two steps. In the first step, the original
Abelian fields are modified in order to introduce the non-Abelian algebra.
After that, the Fa... | [
{
"created": "Tue, 15 Dec 2009 18:24:51 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Abreu",
"E. M. C.",
""
],
[
"Mendes",
"A. C. R.",
""
],
[
"Neves",
"C.",
""
],
[
"Oliveira",
"W.",
""
],
[
"Silva",
"R. C. N.",
""
],
[
"Wotzasek",
"C.",
""
]
] | In this work we have shown that it is possible to construct non-Abelian field theories employing, in a systematic way, the Faddeev-Jackiw symplectic formalism. This approach follows two steps. In the first step, the original Abelian fields are modified in order to introduce the non-Abelian algebra. After that, the Fadd... | 6.572586 | 6.013889 | 6.269332 | 6.147408 | 5.775499 | 6.104888 | 6.083297 | 5.519821 | 6.091316 | 6.843354 | 6.066286 | 5.912796 | 6.358621 | 5.974918 | 5.87944 | 5.818234 | 5.963534 | 5.898112 | 6.050803 | 6.385134 | 5.861192 |
2205.09282 | Mois\'es Bravo-Gaete | Mois\'es Bravo-Gaete, Luis Guajardo and Julio Oliva | Non-linear charged planar black holes in four-dimensional
Scalar-Gauss-Bonnet theories | 10 pages, 3 figures, Accepted for publication in Physical Review D | null | 10.1103/PhysRevD.106.024017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we consider the recently proposed well-defined theory that
permits a healthy $D\to 4$ limit of the Einstein-Gauss-Bonnet combination,
which requires the addition of a scalar degree of freedom. We continue the
construction of exact, hairy black hole solutions in this theory in the
presence of matter sour... | [
{
"created": "Thu, 19 May 2022 02:12:13 GMT",
"version": "v1"
},
{
"created": "Thu, 26 May 2022 02:46:12 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Jul 2022 13:48:52 GMT",
"version": "v3"
}
] | 2022-07-27 | [
[
"Bravo-Gaete",
"Moisés",
""
],
[
"Guajardo",
"Luis",
""
],
[
"Oliva",
"Julio",
""
]
] | In this work, we consider the recently proposed well-defined theory that permits a healthy $D\to 4$ limit of the Einstein-Gauss-Bonnet combination, which requires the addition of a scalar degree of freedom. We continue the construction of exact, hairy black hole solutions in this theory in the presence of matter source... | 13.231654 | 11.795647 | 11.545707 | 10.646546 | 12.034146 | 11.688506 | 11.108301 | 10.941521 | 11.553216 | 12.27638 | 12.003354 | 12.090101 | 12.003408 | 11.768599 | 11.801414 | 11.708091 | 11.917032 | 12.04489 | 12.231665 | 12.021649 | 11.953625 |
1803.03078 | Rafael Hernandez | Rafael Hernandez, Juan Miguel Nieto, Roberto Ruiz | Pulsating strings with mixed three-form flux | 10 pages. Latex | null | 10.1007/JHEP04(2018)078 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Circular strings pulsating in $AdS_3 \times S^3 \times T^4$ with mixed R-R
and NS-NS three-form fluxes can be described by an integrable deformation of
the one-dimensional Neumann-Rosochatius mechanical model. In this article we
find a general class of pulsating solutions to this integrable system that can
be express... | [
{
"created": "Thu, 8 Mar 2018 13:22:01 GMT",
"version": "v1"
}
] | 2018-05-23 | [
[
"Hernandez",
"Rafael",
""
],
[
"Nieto",
"Juan Miguel",
""
],
[
"Ruiz",
"Roberto",
""
]
] | Circular strings pulsating in $AdS_3 \times S^3 \times T^4$ with mixed R-R and NS-NS three-form fluxes can be described by an integrable deformation of the one-dimensional Neumann-Rosochatius mechanical model. In this article we find a general class of pulsating solutions to this integrable system that can be expressed... | 5.072366 | 4.505659 | 6.17672 | 4.238465 | 4.410376 | 4.512816 | 4.335044 | 4.555203 | 4.416288 | 6.678507 | 4.570292 | 4.63286 | 4.978467 | 4.734846 | 4.73281 | 4.567557 | 4.660116 | 4.568264 | 4.584167 | 4.895367 | 4.751194 |
hep-th/9504110 | Cezary Juszczak | Malgorzata Klimek, Jerzy Lukierski | kappa-deformed realisation of D=4 conformal algebra | 13 pages, to appear in the memorial Issue of Acta Physica Polonica B
dedicated to the memory of Professor Jan Rzewuski | Acta Phys. Polon. B26 (1995) 1209-1216 | null | null | hep-th | null | We describe the generators of kappa-conformal transformations, leaving
invariant the kappa-deformed d'Alembert equation. In such a way one obtains the
conformal extension of the off-shell spin zero realization of kappa-deformed
Poincare algebra. Finally the algebraic structure of kappa-deformed conformal
algebra is d... | [
{
"created": "Fri, 21 Apr 1995 12:54:58 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Klimek",
"Malgorzata",
""
],
[
"Lukierski",
"Jerzy",
""
]
] | We describe the generators of kappa-conformal transformations, leaving invariant the kappa-deformed d'Alembert equation. In such a way one obtains the conformal extension of the off-shell spin zero realization of kappa-deformed Poincare algebra. Finally the algebraic structure of kappa-deformed conformal algebra is dis... | 9.594703 | 9.858868 | 10.804728 | 8.18908 | 9.466402 | 8.929423 | 9.015384 | 9.402184 | 8.859837 | 12.042237 | 8.913119 | 8.780413 | 10.5805 | 9.248191 | 9.00981 | 8.655757 | 8.953624 | 9.893259 | 9.224666 | 10.74002 | 8.975258 |
hep-th/9508121 | Leonid Burakovsky | L. Burakovsky, L.P. Horwitz and W.C. Schieve | On Relativistic Bose-Einstein Condensation | null | null | null | null | hep-th | null | We discuss the properties of an ideal relativistic gas of events possessing
Bose-Einstein statistics. We find that the mass spectrum of such a system is
bounded by $\mu \leq m\leq 2M/\mu _K,$ where $\mu $ is the usual chemical
potential, $M$ is an intrinsic dimensional scale parameter for the motion of an
event in sp... | [
{
"created": "Thu, 24 Aug 1995 09:51:08 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Burakovsky",
"L.",
""
],
[
"Horwitz",
"L. P.",
""
],
[
"Schieve",
"W. C.",
""
]
] | We discuss the properties of an ideal relativistic gas of events possessing Bose-Einstein statistics. We find that the mass spectrum of such a system is bounded by $\mu \leq m\leq 2M/\mu _K,$ where $\mu $ is the usual chemical potential, $M$ is an intrinsic dimensional scale parameter for the motion of an event in spac... | 8.639998 | 6.145529 | 8.846359 | 6.989907 | 5.947496 | 5.748748 | 5.970167 | 6.768019 | 7.159204 | 9.37392 | 7.291639 | 7.942912 | 8.503497 | 8.034558 | 7.79676 | 7.425252 | 7.729607 | 8.11606 | 7.959355 | 8.455653 | 8.105964 |
0901.4428 | Derek Harland | Derek Harland and R. S. Ward | Dynamics of Periodic Monopoles | 12 pages, 1 figure More details of numerical methods included | Phys.Lett.B675:262-266,2009 | 10.1016/j.physletb.2009.03.074 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | BPS monopoles which are periodic in one of the spatial directions correspond,
via a generalized Nahm transform, to solutions of the Hitchin equations on a
cylinder. A one-parameter family of solutions of these equations, representing
a geodesic in the 2-monopole moduli space, is constructed numerically. It
correspond... | [
{
"created": "Wed, 28 Jan 2009 10:26:21 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Apr 2009 13:35:30 GMT",
"version": "v2"
}
] | 2011-03-28 | [
[
"Harland",
"Derek",
""
],
[
"Ward",
"R. S.",
""
]
] | BPS monopoles which are periodic in one of the spatial directions correspond, via a generalized Nahm transform, to solutions of the Hitchin equations on a cylinder. A one-parameter family of solutions of these equations, representing a geodesic in the 2-monopole moduli space, is constructed numerically. It corresponds ... | 10.247881 | 7.586271 | 10.901128 | 8.083288 | 7.601788 | 7.686816 | 8.083891 | 8.111232 | 7.709451 | 12.163053 | 7.737216 | 7.942274 | 9.055905 | 8.555994 | 7.986948 | 8.454234 | 8.003726 | 8.740026 | 8.316211 | 8.505844 | 8.051784 |
1403.5281 | David Garner | David Garner, Sanjaye Ramgoolam, Congkao Wen | Thresholds of Large N Factorization in CFT4 : Exploring bulk spacetime
in AdS5 | 52 pages, 6 figures | null | 10.1007/JHEP11(2014)076 | QMUL-PH-13-15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Large $N$ factorization ensures that, for low-dimension gauge-invariant
operators in the half-BPS sector of ${\cal N}=4$ SYM, products of holomorphic
traces have vanishing correlators with single anti-holomorphic traces. This
vanishing is necessary to consistently map trace operators in the CFT$_4$ to a
Fock space of... | [
{
"created": "Thu, 20 Mar 2014 20:07:14 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Dec 2014 14:18:22 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Garner",
"David",
""
],
[
"Ramgoolam",
"Sanjaye",
""
],
[
"Wen",
"Congkao",
""
]
] | Large $N$ factorization ensures that, for low-dimension gauge-invariant operators in the half-BPS sector of ${\cal N}=4$ SYM, products of holomorphic traces have vanishing correlators with single anti-holomorphic traces. This vanishing is necessary to consistently map trace operators in the CFT$_4$ to a Fock space of g... | 12.173923 | 11.695829 | 12.456788 | 10.895413 | 12.166575 | 11.505425 | 11.875982 | 11.425749 | 10.999214 | 13.755094 | 11.387768 | 10.786925 | 11.568717 | 10.941549 | 10.904639 | 11.076619 | 11.020689 | 11.135167 | 10.90006 | 11.301313 | 11.049828 |
1208.6136 | Cosimo Restuccia | Stefan Fredenhagen, Cosimo Restuccia | The geometry of the limit of N=2 minimal models | 35 pages, 3 figures; v2 minor corrections, version to be published in
J. Phys. A | null | 10.1088/1751-8113/46/4/045402 | AEI-2012-087 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the limit of two-dimensional N=(2,2) superconformal minimal
models when the central charge approaches c=3. Starting from a geometric
description as non-linear sigma models, we show that one can obtain two
different limit theories. One is the free theory of two bosons and two
fermions, the other one is a c... | [
{
"created": "Thu, 30 Aug 2012 11:05:23 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jan 2013 11:05:37 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Fredenhagen",
"Stefan",
""
],
[
"Restuccia",
"Cosimo",
""
]
] | We consider the limit of two-dimensional N=(2,2) superconformal minimal models when the central charge approaches c=3. Starting from a geometric description as non-linear sigma models, we show that one can obtain two different limit theories. One is the free theory of two bosons and two fermions, the other one is a con... | 7.377164 | 5.910087 | 8.545412 | 6.339902 | 6.498113 | 6.213559 | 6.314739 | 5.826172 | 6.278265 | 8.497975 | 6.232666 | 6.54666 | 8.293447 | 6.602868 | 6.885239 | 6.863002 | 6.85322 | 6.853701 | 6.784219 | 7.870905 | 6.847826 |
1203.1443 | Niklas Beisert | Niklas Beisert, Song He, Burkhard U. W. Schwab, Cristian Vergu | Null Polygonal Wilson Loops in Full N=4 Superspace | 55 pages, v2: reference added | J. Phys. A45 (2012) 265402 | 10.1088/1751-8113/45/26/265402 | AEI-2012-007; NSF-KITP-12-011 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the one-loop expectation value of light-like polygonal Wilson
loops in N=4 super-Yang-Mills theory in full superspace. When projecting to
chiral superspace we recover the known results for tree-level
next-to-maximally-helicity-violating (NMHV) scattering amplitude. The one-loop
MHV amplitude is also includ... | [
{
"created": "Wed, 7 Mar 2012 11:30:17 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Mar 2012 09:57:32 GMT",
"version": "v2"
}
] | 2012-06-18 | [
[
"Beisert",
"Niklas",
""
],
[
"He",
"Song",
""
],
[
"Schwab",
"Burkhard U. W.",
""
],
[
"Vergu",
"Cristian",
""
]
] | We compute the one-loop expectation value of light-like polygonal Wilson loops in N=4 super-Yang-Mills theory in full superspace. When projecting to chiral superspace we recover the known results for tree-level next-to-maximally-helicity-violating (NMHV) scattering amplitude. The one-loop MHV amplitude is also included... | 8.359844 | 7.702443 | 11.216261 | 7.227587 | 7.801355 | 7.664755 | 8.045449 | 7.933849 | 7.471775 | 10.809545 | 7.727615 | 7.615969 | 8.405628 | 7.814658 | 8.02801 | 7.842391 | 7.667966 | 8.109548 | 7.854023 | 8.200127 | 7.775034 |
0809.1042 | Usha Kulshreshtha Dr. | Usha Kulshreshtha | Vector Schwinger Model with a Photon Mass Term on the Light-Front | 06pages, conference | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Vector Schwinger model with a mass term for the photon, describing 2D
electrodyn amics with massless fermions, studied by us recently, represents a
new class of models. This theory becomes gauge-invariant when studied on the
light-front. Thi s is in contrast to the instant-form theory which is
gauge-noninvariant. We ... | [
{
"created": "Fri, 5 Sep 2008 15:04:16 GMT",
"version": "v1"
}
] | 2008-09-08 | [
[
"Kulshreshtha",
"Usha",
""
]
] | Vector Schwinger model with a mass term for the photon, describing 2D electrodyn amics with massless fermions, studied by us recently, represents a new class of models. This theory becomes gauge-invariant when studied on the light-front. Thi s is in contrast to the instant-form theory which is gauge-noninvariant. We qu... | 16.280762 | 14.54893 | 16.010754 | 14.310559 | 13.706293 | 15.247714 | 14.579487 | 14.257442 | 13.913578 | 17.456535 | 14.222589 | 14.46983 | 14.723558 | 14.181272 | 14.801067 | 14.827543 | 14.518922 | 14.776843 | 15.714334 | 15.126048 | 15.518627 |
hep-th/0409122 | Neil Turok | Paul L. McFadden and Neil Turok | Conformal symmetry of brane world effective actions | 5 pages, published version | Phys.Rev.D71:021901,2005 | 10.1103/PhysRevD.71.021901 | DAMTP-2004-97 | hep-th | null | A simple derivation of the low-energy effective action for brane worlds is
given, highlighting the role of conformal invariance. We show how to improve
the effective action for a positive- and negative-tension brane pair using the
AdS/CFT correspondence.
| [
{
"created": "Mon, 13 Sep 2004 19:21:01 GMT",
"version": "v1"
},
{
"created": "Mon, 31 Jan 2005 18:16:22 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"McFadden",
"Paul L.",
""
],
[
"Turok",
"Neil",
""
]
] | A simple derivation of the low-energy effective action for brane worlds is given, highlighting the role of conformal invariance. We show how to improve the effective action for a positive- and negative-tension brane pair using the AdS/CFT correspondence. | 9.427684 | 7.533002 | 7.965709 | 7.40002 | 8.070848 | 8.020953 | 7.185137 | 7.643954 | 6.766871 | 8.890315 | 7.340871 | 7.426532 | 8.103247 | 7.481078 | 7.601094 | 7.439623 | 7.651671 | 7.619589 | 7.503105 | 7.989892 | 7.539132 |
hep-th/9812099 | Jim Wheeler | A. Wehner (Utah State University) and J.T. Wheeler (Utah State
University) | Conformal actions in any dimension | 35 pages, now includes comparisons with other theories; one added
reference | Nucl.Phys. B557 (1999) 380-406 | 10.1016/S0550-3213(99)00367-3 | USU-FTG-117 | hep-th gr-qc | null | Biconformal gauging of the conformal group has a scale-invariant volume form,
permitting a single form of the action to be invariant in any dimension. We
display several 2n-dim scale-invariant polynomial actions and a dual action. We
solve the field equations for the most general action linear in the curvatures
for a... | [
{
"created": "Fri, 11 Dec 1998 20:33:52 GMT",
"version": "v1"
},
{
"created": "Tue, 4 May 1999 19:28:19 GMT",
"version": "v2"
},
{
"created": "Thu, 13 May 1999 02:57:54 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Wehner",
"A.",
"",
"Utah State University"
],
[
"Wheeler",
"J. T.",
"",
"Utah State\n University"
]
] | Biconformal gauging of the conformal group has a scale-invariant volume form, permitting a single form of the action to be invariant in any dimension. We display several 2n-dim scale-invariant polynomial actions and a dual action. We solve the field equations for the most general action linear in the curvatures for a m... | 13.300577 | 13.099039 | 13.298368 | 11.903894 | 12.504409 | 13.436713 | 13.608912 | 12.212893 | 12.827838 | 14.757456 | 12.616216 | 11.795175 | 12.079475 | 11.789943 | 11.762177 | 11.966199 | 12.255649 | 11.73771 | 12.328587 | 12.527705 | 12.291036 |
1309.4052 | Antoine Van Proeyen | Sergio Ferrara, Renata Kallosh, Antoine Van Proeyen | On the Supersymmetric Completion of $R+R^2$ Gravity and Cosmology | 11 pages; accepted for publication in JHEP; v2: typos corrected in
(3.17) and in discussion | null | 10.1007/JHEP11(2013)134 | CERN-PH-TH/2013-220 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit and clarify the supersymmetric versions of $R+ R^2$ gravity, in
view of the renewed interest to these models in cosmology. We emphasize that
the content of the dual standard supergravity theory in the old minimal
formulation necessarily includes two massive chiral multiplets, that we call
the inflaton and ... | [
{
"created": "Mon, 16 Sep 2013 17:57:07 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Oct 2013 07:28:02 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Ferrara",
"Sergio",
""
],
[
"Kallosh",
"Renata",
""
],
[
"Van Proeyen",
"Antoine",
""
]
] | We revisit and clarify the supersymmetric versions of $R+ R^2$ gravity, in view of the renewed interest to these models in cosmology. We emphasize that the content of the dual standard supergravity theory in the old minimal formulation necessarily includes two massive chiral multiplets, that we call the inflaton and th... | 7.713273 | 7.417295 | 7.839871 | 6.812006 | 7.270879 | 7.465873 | 7.50457 | 7.075299 | 6.669582 | 7.376394 | 7.076931 | 7.294859 | 7.299422 | 6.874104 | 7.328058 | 7.175497 | 7.044304 | 7.329962 | 6.954727 | 7.261405 | 7.416579 |
1505.05886 | Jacob Bourjaily | Jacob L. Bourjaily and Jaroslav Trnka | Local Integrand Representations of All Two-Loop Amplitudes in Planar SYM | Corrections made including an important erratum: merging finite
integrands does not always result in finite integrals. Language modified to
reflect this fact, but implications are left to future work. 58 pages, 85
figures, and a Mathematica package (with a demonstration notebook) | null | 10.1007/JHEP08(2015)119 | CALT-TH-2015-026 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use generalized unitarity at the integrand-level to directly construct
local, manifestly dual-conformally invariant formulae for all two-loop
scattering amplitudes in planar, maximally supersymmetric Yang-Mills theory
(SYM). This representation separates contributions into manifestly finite and
divergent terms---i... | [
{
"created": "Thu, 21 May 2015 20:00:34 GMT",
"version": "v1"
},
{
"created": "Thu, 18 May 2017 18:27:59 GMT",
"version": "v2"
}
] | 2017-05-22 | [
[
"Bourjaily",
"Jacob L.",
""
],
[
"Trnka",
"Jaroslav",
""
]
] | We use generalized unitarity at the integrand-level to directly construct local, manifestly dual-conformally invariant formulae for all two-loop scattering amplitudes in planar, maximally supersymmetric Yang-Mills theory (SYM). This representation separates contributions into manifestly finite and divergent terms---in ... | 8.530632 | 9.410131 | 9.944413 | 8.557521 | 8.65461 | 8.77763 | 8.460685 | 8.295198 | 8.37101 | 11.127349 | 8.654409 | 8.626333 | 9.051262 | 8.389528 | 8.301769 | 8.789018 | 8.480608 | 8.267624 | 8.438995 | 8.700062 | 8.619022 |
1201.3191 | Paolo Benincasa | Paolo Benincasa | Exploration of the Tree-Level S-Matrix of Massless Particles | 6 pages, 1 table, contribution to the proceeding of the XVII European
Workshop on String Theory | null | 10.1002/prop.201200006 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In recent years, the BCFW construction provided a very powerful tool for
computing scattering amplitudes as well as it shed light on the perturbation
theory structure. In this talk, we discuss the long-standing issue of the
boundary term arising when the amplitudes do not vanish as some momenta are
taken to infinity ... | [
{
"created": "Mon, 16 Jan 2012 10:00:07 GMT",
"version": "v1"
}
] | 2016-01-20 | [
[
"Benincasa",
"Paolo",
""
]
] | In recent years, the BCFW construction provided a very powerful tool for computing scattering amplitudes as well as it shed light on the perturbation theory structure. In this talk, we discuss the long-standing issue of the boundary term arising when the amplitudes do not vanish as some momenta are taken to infinity al... | 10.480198 | 9.451634 | 10.226803 | 9.425722 | 9.987969 | 9.636011 | 10.129422 | 9.239979 | 8.619921 | 9.522554 | 9.342081 | 9.373981 | 9.383076 | 9.251572 | 9.114697 | 9.175342 | 8.627495 | 9.168451 | 9.316158 | 9.509694 | 9.727215 |
0708.3452 | In Yong Park | I. Y. Park | Scattering on D3-branes | 15 pages, minor typos corrected, version that will appear in PLB | Phys.Lett.B660:583-591,2008 | 10.1016/j.physletb.2007.11.101 | null | hep-th | null | In a direct open string approach we analyze scattering of massless states on
a stack of D3-branes. First we construct vertex operators on the D-branes. The
4+6 splitting for the fermionic part is made possible by inserting
appropriately defined projection operators. With the vertex operators
constructed we compute va... | [
{
"created": "Sat, 25 Aug 2007 22:15:58 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Jan 2008 19:25:02 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Park",
"I. Y.",
""
]
] | In a direct open string approach we analyze scattering of massless states on a stack of D3-branes. First we construct vertex operators on the D-branes. The 4+6 splitting for the fermionic part is made possible by inserting appropriately defined projection operators. With the vertex operators constructed we compute vari... | 13.416741 | 11.192756 | 13.391865 | 11.287962 | 11.341878 | 12.693004 | 12.04816 | 11.672288 | 11.605722 | 14.172075 | 11.240655 | 11.722703 | 13.007917 | 12.195647 | 11.855843 | 12.081267 | 12.333423 | 11.916224 | 11.856031 | 12.875797 | 11.483658 |
hep-th/0703259 | Igor Salom | Igor Salom | Extension of Conformal (Super)Symmetry using Heisenberg and Parabose
operators | null | null | null | null | hep-th | null | In this paper we investigate a particular possibility to extend C(1,3)
conformal symmetry using Heisenberg operators, and a related possibility to
extend conformal supersymmetry using parabose operators. The symmetry proposed
is of a simple mathematical form, as is the form of necessary symmetry breaking
that reduces... | [
{
"created": "Wed, 28 Mar 2007 13:48:41 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Salom",
"Igor",
""
]
] | In this paper we investigate a particular possibility to extend C(1,3) conformal symmetry using Heisenberg operators, and a related possibility to extend conformal supersymmetry using parabose operators. The symmetry proposed is of a simple mathematical form, as is the form of necessary symmetry breaking that reduces i... | 9.719356 | 9.848242 | 10.416673 | 9.681247 | 10.800776 | 10.591935 | 9.924068 | 9.943649 | 9.815845 | 11.152472 | 9.762836 | 9.522198 | 9.593307 | 9.38339 | 9.200184 | 9.278327 | 9.456736 | 9.099045 | 9.272145 | 9.715262 | 9.133523 |
hep-th/9905051 | Cesar D. Fosco | C.D. Fosco and F.A. Schaposnik | Making Sense of Singular Gauge Transformations in 1+1 and 2+1 Fermion
Models | 14 pages, Latex | Phys.Lett. B477 (2000) 341-347 | 10.1016/S0370-2693(00)00179-9 | null | hep-th | null | We study the problem of decoupling fermion fields in 1+1 and 2+1 dimensions,
in interaction with a gauge field, by performing local transformations of the
fermions in the functional integral. This could always be done if singular
(large) gauge transformations were allowed, since any gauge field configuration
may be r... | [
{
"created": "Fri, 7 May 1999 12:05:18 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Fosco",
"C. D.",
""
],
[
"Schaposnik",
"F. A.",
""
]
] | We study the problem of decoupling fermion fields in 1+1 and 2+1 dimensions, in interaction with a gauge field, by performing local transformations of the fermions in the functional integral. This could always be done if singular (large) gauge transformations were allowed, since any gauge field configuration may be rep... | 9.437457 | 9.54975 | 10.346645 | 8.931275 | 10.12143 | 9.546894 | 8.997132 | 9.203928 | 9.588485 | 10.197466 | 9.210504 | 9.051077 | 9.499501 | 9.276884 | 8.960686 | 9.096659 | 9.262181 | 8.952095 | 9.145915 | 9.261841 | 9.390378 |
hep-th/9512108 | Vipul Periwal | Vipul Periwal | Halpern-Huang directions in effective scalar field theory | 6 pages, plain TeX | Mod.Phys.Lett. A11 (1996) 2915-2920 | 10.1142/S0217732396002885 | PUPT-1567 | hep-th | null | Halpern and Huang recently showed that there are relevant directions in the
space of interactions at the Gaussian fixed point. I show that their result can
be derived from Polchinski's form of the Wilson renormalization group. The
derivation shows that the existence of these directions is independent of the
cutoff fu... | [
{
"created": "Thu, 14 Dec 1995 18:51:54 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Periwal",
"Vipul",
""
]
] | Halpern and Huang recently showed that there are relevant directions in the space of interactions at the Gaussian fixed point. I show that their result can be derived from Polchinski's form of the Wilson renormalization group. The derivation shows that the existence of these directions is independent of the cutoff func... | 13.858548 | 8.585306 | 10.929009 | 9.397349 | 10.317978 | 10.621629 | 9.112677 | 9.803467 | 8.696495 | 12.567575 | 12.725768 | 9.242442 | 10.163827 | 9.129543 | 9.438574 | 8.871581 | 9.592301 | 9.181679 | 9.250096 | 10.685343 | 11.869336 |
2207.08784 | Jose Antonio Oller | J. A. Oller | Unitarizing non-relativistic Coulomb scattering | 12 pages, 2 figures | null | 10.1016/j.physletb.2022.137568 | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | We compare the exactly solvable nonrelativistic Coulomb scattering with two
recent unitarization methods for infinite-range forces. These methods require
to calculate perturbatively the corresponding partial-wave amplitudes, which
are then unitarized. We calculate the Coulomb partial-wave amplitudes up to the
one-loo... | [
{
"created": "Mon, 18 Jul 2022 17:40:57 GMT",
"version": "v1"
}
] | 2022-11-16 | [
[
"Oller",
"J. A.",
""
]
] | We compare the exactly solvable nonrelativistic Coulomb scattering with two recent unitarization methods for infinite-range forces. These methods require to calculate perturbatively the corresponding partial-wave amplitudes, which are then unitarized. We calculate the Coulomb partial-wave amplitudes up to the one-loop ... | 7.337977 | 7.649455 | 6.781667 | 6.527098 | 7.620897 | 7.924067 | 7.161392 | 7.188688 | 7.133938 | 7.471188 | 7.119321 | 7.116927 | 6.786371 | 6.789321 | 6.778269 | 7.034646 | 6.98967 | 6.99423 | 6.592581 | 6.958366 | 6.714165 |
1601.04432 | Rutger H. Boels | Rutger Boels, Bernd A. Kniehl, Gang Yang | Towards a four-loop form factor | 9 Pages, Radcor/Loopfest 2015 Proceedings | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The four-loop, two-point form factor contains the first non-planar correction
to the lightlike cusp anomalous dimension. This anomalous dimension is a
universal function which appears in many applications. Its planar part in N = 4
SYM is known, in principle, exactly from AdS/CFT and integrability while its
non-planar... | [
{
"created": "Mon, 18 Jan 2016 09:11:33 GMT",
"version": "v1"
}
] | 2016-01-19 | [
[
"Boels",
"Rutger",
""
],
[
"Kniehl",
"Bernd A.",
""
],
[
"Yang",
"Gang",
""
]
] | The four-loop, two-point form factor contains the first non-planar correction to the lightlike cusp anomalous dimension. This anomalous dimension is a universal function which appears in many applications. Its planar part in N = 4 SYM is known, in principle, exactly from AdS/CFT and integrability while its non-planar p... | 10.057718 | 10.246349 | 11.03995 | 9.950665 | 10.702345 | 10.992109 | 10.754403 | 10.698799 | 9.902055 | 11.414412 | 10.153155 | 9.799604 | 10.191543 | 9.92802 | 9.744329 | 10.01204 | 10.151626 | 10.191222 | 9.899074 | 10.51757 | 9.754761 |
hep-th/0310049 | Giampiero Esposito Dr. | Giuseppe Bimonte, Enrico Calloni, Luciano Di Fiore, Giampiero
Esposito, Leopoldo Milano, Luigi Rosa | On the photon Green functions in curved space-time | 22 pages, plain Tex. All sections and appendices have been improved | Class.Quant.Grav. 21 (2004) 647-659 | 10.1088/0264-9381/21/2/022 | DSF 2003/27 | hep-th gr-qc | null | Quantization of electrodynamics in curved space-time in the Lorenz gauge and
with arbitrary gauge parameter makes it necessary to study Green functions of
non-minimal operators with variable coefficients. Starting from the integral
representation of photon Green functions, we link them to the evaluation of
integrals ... | [
{
"created": "Mon, 6 Oct 2003 11:50:41 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Nov 2003 16:31:48 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Bimonte",
"Giuseppe",
""
],
[
"Calloni",
"Enrico",
""
],
[
"Di Fiore",
"Luciano",
""
],
[
"Esposito",
"Giampiero",
""
],
[
"Milano",
"Leopoldo",
""
],
[
"Rosa",
"Luigi",
""
]
] | Quantization of electrodynamics in curved space-time in the Lorenz gauge and with arbitrary gauge parameter makes it necessary to study Green functions of non-minimal operators with variable coefficients. Starting from the integral representation of photon Green functions, we link them to the evaluation of integrals in... | 10.77663 | 10.898767 | 10.22988 | 9.397094 | 11.126314 | 10.391054 | 11.193658 | 9.483062 | 9.848251 | 10.390476 | 9.8661 | 9.657794 | 9.559566 | 9.761256 | 9.668178 | 9.778862 | 9.86696 | 9.912533 | 9.895354 | 9.95079 | 9.741714 |
hep-th/9809033 | Jose Fernandez Barbon | J. L. F. Barbon, I. I. Kogan and E. Rabinovici | On Stringy Thresholds in SYM/AdS Thermodynamics | 49 pages, harvmac, seven Postscript figures | Nucl.Phys.B544:104-144,1999 | 10.1016/S0550-3213(98)00868-2 | CERN-TH/98-206, OUTP-98-48P | hep-th | null | We consider aspects of the role of stringy scales and Hagedorn temperatures
in the correspondence between various field theories and AdS-type spaces. The
boundary theory is set on a toroidal world-volume to enable small scales to
appear in the supergravity backgrounds also for low field-theory temperatures.
We find t... | [
{
"created": "Fri, 4 Sep 1998 17:01:07 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Barbon",
"J. L. F.",
""
],
[
"Kogan",
"I. I.",
""
],
[
"Rabinovici",
"E.",
""
]
] | We consider aspects of the role of stringy scales and Hagedorn temperatures in the correspondence between various field theories and AdS-type spaces. The boundary theory is set on a toroidal world-volume to enable small scales to appear in the supergravity backgrounds also for low field-theory temperatures. We find tha... | 18.38945 | 18.279507 | 20.481113 | 17.203413 | 18.068943 | 18.193201 | 17.574028 | 18.128944 | 17.897635 | 20.733311 | 17.767622 | 17.583542 | 18.839676 | 18.050018 | 18.077513 | 17.362682 | 18.019423 | 17.898714 | 17.949949 | 18.48484 | 17.198278 |
1502.05711 | Marcel Vonk | Marcel Vonk | Resurgence and Topological Strings | 11 pages, 7 figures. Pedestrian introduction to 1308.1695 and
1407.4821, based on my talk at String Math 2014. Submitted for the
proceedings of that conference | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The mathematical idea of resurgence allows one to obtain nonperturbative
information from the large-order behavior of perturbative expansions. This idea
can be very fruitful in physics applications, in particular if one does not
have access to such nonperturbative information from first principles. An
important examp... | [
{
"created": "Thu, 19 Feb 2015 21:00:12 GMT",
"version": "v1"
}
] | 2015-02-23 | [
[
"Vonk",
"Marcel",
""
]
] | The mathematical idea of resurgence allows one to obtain nonperturbative information from the large-order behavior of perturbative expansions. This idea can be very fruitful in physics applications, in particular if one does not have access to such nonperturbative information from first principles. An important example... | 5.903815 | 5.362067 | 5.935016 | 5.395945 | 5.361597 | 5.764334 | 5.429826 | 5.570476 | 5.433282 | 5.770401 | 5.283359 | 5.441755 | 5.620842 | 5.317513 | 5.258988 | 5.289176 | 5.447265 | 5.572931 | 5.398759 | 5.59096 | 5.465454 |
hep-th/0406260 | Jorge Pullin | Rodolfo Gambini, Rafael Porto, Jorge Pullin | Realistic clocks, universal decoherence and the black hole information
paradox | 3 Pages, RevTex, no figures | Phys.Rev.Lett. 93 (2004) 240401 | 10.1103/PhysRevLett.93.240401 | LSU-REL-062804 | hep-th astro-ph gr-qc quant-ph | null | Ordinary quantum mechanics is formulated on the basis of the existence of an
ideal classical clock external to the system under study. This is clearly an
idealization. As emphasized originally by Salecker and Wigner and more recently
by other authors, there exist limits in nature to how ``classical'' even the
best po... | [
{
"created": "Mon, 28 Jun 2004 22:50:01 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gambini",
"Rodolfo",
""
],
[
"Porto",
"Rafael",
""
],
[
"Pullin",
"Jorge",
""
]
] | Ordinary quantum mechanics is formulated on the basis of the existence of an ideal classical clock external to the system under study. This is clearly an idealization. As emphasized originally by Salecker and Wigner and more recently by other authors, there exist limits in nature to how ``classical'' even the best poss... | 11.072943 | 13.281405 | 11.761984 | 10.782058 | 13.23957 | 12.269369 | 12.114141 | 11.838503 | 11.926222 | 11.690907 | 11.289762 | 11.053941 | 10.496902 | 10.492455 | 11.444929 | 10.631591 | 11.254626 | 10.401404 | 10.682043 | 10.42221 | 10.798443 |
1811.06623 | Timoth\'e Poulain | Timoth\'e Poulain | On the quantum structure of spacetime and its relation to the quantum
theory of fields: $\kappa$-Poincar\'e invariant field theories and other
examples | Ph.D. Thesis, 151 pages | null | null | NNT : 2018SACLS331 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dissertation deals with noncommutative field theories, namely field
theories compatible with the existence of a minimal (quantum gravity) length
scale. Two families of quantum spacetime are considered. One is characterized
by semisimple Lie algebras of coordinates. The other is characterized by
solvable Lie algeb... | [
{
"created": "Thu, 15 Nov 2018 23:14:52 GMT",
"version": "v1"
}
] | 2018-11-19 | [
[
"Poulain",
"Timothé",
""
]
] | The dissertation deals with noncommutative field theories, namely field theories compatible with the existence of a minimal (quantum gravity) length scale. Two families of quantum spacetime are considered. One is characterized by semisimple Lie algebras of coordinates. The other is characterized by solvable Lie algebra... | 6.145129 | 6.156099 | 6.417482 | 6.024958 | 6.563496 | 6.468627 | 6.245007 | 6.18149 | 5.828649 | 6.363234 | 5.8957 | 5.946329 | 6.146554 | 5.955781 | 5.92905 | 5.926404 | 5.779594 | 5.920695 | 6.009447 | 6.138509 | 5.987425 |
hep-th/0510011 | Pawel Maslanka | Piotr Kosinski, Pawel Maslanka | Unitarity in the noncommutative theories | 8 pages, no figures;some changes in the main text, and the list of
references modified | null | null | null | hep-th | null | Simple argument in favour of unitarity, to all orders, of space-like
noncommutative theory is given.
| [
{
"created": "Mon, 3 Oct 2005 11:27:56 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Oct 2005 11:30:36 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Dec 2005 13:18:43 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Kosinski",
"Piotr",
""
],
[
"Maslanka",
"Pawel",
""
]
] | Simple argument in favour of unitarity, to all orders, of space-like noncommutative theory is given. | 63.582119 | 16.698765 | 31.738577 | 19.728508 | 19.269005 | 22.961647 | 26.316477 | 18.58651 | 18.49531 | 29.444176 | 24.206345 | 20.615334 | 23.577602 | 20.926151 | 22.174204 | 20.329384 | 23.167845 | 19.449272 | 22.118162 | 26.918648 | 21.695528 |
2007.16083 | Adil Belhaj | A. Belhaj, A. El Balali, W. El Hadri, H. El Moumni, M. A. Essebani, M.
B. Sedra | On Phase Transition Behaviors of Kerr-Sen Black Hole | Latex, 17 pages, 4 figues, 1 table. Accepted for publication in
IJGMMP (2020) | null | 10.1142/S0219887820501698 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate phase transitions and critical behaviors of the Kerr-Sen black
hole in four dimensions. Computing the involved thermodynamical quantities
including the specific heat and using the Ehrenfest scheme, we show that such a
black hole undergoes a second-order phase transition. Adopting a new metric
form deri... | [
{
"created": "Fri, 31 Jul 2020 14:02:44 GMT",
"version": "v1"
}
] | 2020-10-28 | [
[
"Belhaj",
"A.",
""
],
[
"Balali",
"A. El",
""
],
[
"Hadri",
"W. El",
""
],
[
"Moumni",
"H. El",
""
],
[
"Essebani",
"M. A.",
""
],
[
"Sedra",
"M. B.",
""
]
] | We investigate phase transitions and critical behaviors of the Kerr-Sen black hole in four dimensions. Computing the involved thermodynamical quantities including the specific heat and using the Ehrenfest scheme, we show that such a black hole undergoes a second-order phase transition. Adopting a new metric form derive... | 15.249202 | 12.787277 | 13.180666 | 12.631882 | 14.974603 | 12.864005 | 13.246191 | 11.644337 | 14.298446 | 14.794173 | 15.090578 | 13.88539 | 13.903637 | 13.354993 | 14.427327 | 14.21979 | 13.989 | 13.201515 | 14.260397 | 13.569366 | 13.894457 |
2006.14038 | Mario Martone | Mario Martone | The constraining power of Coulomb Branch Geometry: lectures on
Seiberg-Witten theory | This is the writeup of the lectures given at the Winter School "YRISW
2020" to appear in a special issue of JPhysA | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The constraining mathematical structure of the Coulomb branch of four
dimensional $\mathcal{N}=2$ supersymmetric theories is discussed. The
presentation follows a somewhat different route from other excellent reviews on
the subject and it is geared towards using this tool to classify four
dimensional $\mathcal{N}=2$ ... | [
{
"created": "Wed, 24 Jun 2020 20:47:29 GMT",
"version": "v1"
}
] | 2020-06-26 | [
[
"Martone",
"Mario",
""
]
] | The constraining mathematical structure of the Coulomb branch of four dimensional $\mathcal{N}=2$ supersymmetric theories is discussed. The presentation follows a somewhat different route from other excellent reviews on the subject and it is geared towards using this tool to classify four dimensional $\mathcal{N}=2$ su... | 9.143162 | 4.805015 | 10.91254 | 5.065567 | 5.141775 | 5.012893 | 4.761312 | 5.152783 | 4.900369 | 10.06251 | 5.177532 | 6.610394 | 8.751092 | 6.925507 | 6.954206 | 6.731064 | 6.899311 | 6.766828 | 7.08827 | 8.781425 | 6.936345 |
2212.09416 | Zoltan Bajnok | Zoltan Bajnok, Janos Balog, Istvan Vona | The full analytic trans-series in integrable field theories | 13 pages | null | 10.1016/j.physletb.2023.138075 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We analyze a family of generalized energy densities in integrable quantum
field theories in the presence of an external field coupled to a conserved
charge. By using the Wiener-Hopf technique to solve the linear thermodynamic
Bethe ansatz equations we derive the full analytic trans-series for these
observables in ter... | [
{
"created": "Mon, 19 Dec 2022 12:49:13 GMT",
"version": "v1"
}
] | 2023-08-09 | [
[
"Bajnok",
"Zoltan",
""
],
[
"Balog",
"Janos",
""
],
[
"Vona",
"Istvan",
""
]
] | We analyze a family of generalized energy densities in integrable quantum field theories in the presence of an external field coupled to a conserved charge. By using the Wiener-Hopf technique to solve the linear thermodynamic Bethe ansatz equations we derive the full analytic trans-series for these observables in terms... | 12.507385 | 11.909548 | 12.683877 | 11.227418 | 11.989345 | 11.667775 | 12.289458 | 10.630412 | 10.825914 | 15.626703 | 11.65978 | 12.048024 | 12.423238 | 12.08027 | 12.07045 | 11.767608 | 11.896573 | 12.003895 | 12.070755 | 13.114388 | 11.695118 |
0905.3938 | Mario Trigiante | L. Andrianopoli, R. D'Auria, E.Orazi and M. Trigiante | First Order Description of D=4 static Black Holes and the
Hamilton-Jacobi equation | A clarifying discussion on the existence of the prepotential and a
comment on multiple attractors are added; typos corrected, references added | Nucl.Phys.B833:1-16,2010 | 10.1016/j.nuclphysb.2010.02.020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we discuss the application of the Hamilton-Jacobi formalism to
the first order description of four dimensional spherically symmetric and
static black holes. In particular we show that the prepotential characterizing
the flow coincides with the Hamilton principal function associated with the
one-dimension... | [
{
"created": "Mon, 25 May 2009 16:45:24 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Jun 2009 16:56:55 GMT",
"version": "v2"
}
] | 2010-05-19 | [
[
"Andrianopoli",
"L.",
""
],
[
"D'Auria",
"R.",
""
],
[
"Orazi",
"E.",
""
],
[
"Trigiante",
"M.",
""
]
] | In this note we discuss the application of the Hamilton-Jacobi formalism to the first order description of four dimensional spherically symmetric and static black holes. In particular we show that the prepotential characterizing the flow coincides with the Hamilton principal function associated with the one-dimensional... | 8.200693 | 7.397298 | 8.413078 | 7.192875 | 7.438498 | 8.229838 | 8.006167 | 7.167985 | 7.295452 | 8.78788 | 7.266691 | 7.262719 | 7.72745 | 7.311842 | 7.29792 | 7.303109 | 7.274031 | 7.250504 | 7.287265 | 7.705413 | 7.348547 |
hep-th/9903147 | Christian Ekstrand | C. Ekstrand | A Simple Algebraic Derivation of the Covariant Anomaly and Schwinger
Term | 16 pages | J.Math.Phys. 41 (2000) 7294-7303 | 10.1063/1.1285018 | null | hep-th | null | An expression for the curvature of the "covariant" determinant line bundle is
given in even dimensional space-time. The usefulness is guaranteed by its
prediction of the covariant anomaly and Schwinger term. It allows a parallel
derivation of the consistent anomaly and Schwinger term, and their covariant
counterparts... | [
{
"created": "Wed, 17 Mar 1999 12:32:26 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ekstrand",
"C.",
""
]
] | An expression for the curvature of the "covariant" determinant line bundle is given in even dimensional space-time. The usefulness is guaranteed by its prediction of the covariant anomaly and Schwinger term. It allows a parallel derivation of the consistent anomaly and Schwinger term, and their covariant counterparts, ... | 14.584753 | 12.675829 | 14.761336 | 12.900638 | 12.80744 | 11.735186 | 11.546356 | 11.857429 | 11.600183 | 14.387282 | 12.493988 | 13.528146 | 13.682879 | 13.413936 | 12.937073 | 13.307968 | 12.503214 | 12.635122 | 12.644636 | 13.675456 | 12.612748 |
1201.0025 | Petr Dunin-Barkowski | Petr Dunin-Barkowski, Alexey Sleptsov, Andrey Smirnov | Explicit computation of Drinfeld associator in the case of the
fundamental representation of gl(N) | 14 pages, 2 figures; several flaws indicated by referees corrected | J. Phys. A: Math. Theor. 45 385204 (2012) | 10.1088/1751-8113/45/38/385204 | ITEP/TH-64/11 | hep-th math.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We solve the regularized Knizhnik-Zamolodchikov equation and find an explicit
expression for the Drinfeld associator. We restrict to the case of the
fundamental representation of $gl(N)$. Several tests of the results are
presented. It can be explicitly seen that components of this solution for the
associator coincide... | [
{
"created": "Thu, 29 Dec 2011 21:32:11 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Jan 2012 21:50:41 GMT",
"version": "v2"
},
{
"created": "Sat, 1 Sep 2012 09:36:02 GMT",
"version": "v3"
}
] | 2012-09-04 | [
[
"Dunin-Barkowski",
"Petr",
""
],
[
"Sleptsov",
"Alexey",
""
],
[
"Smirnov",
"Andrey",
""
]
] | We solve the regularized Knizhnik-Zamolodchikov equation and find an explicit expression for the Drinfeld associator. We restrict to the case of the fundamental representation of $gl(N)$. Several tests of the results are presented. It can be explicitly seen that components of this solution for the associator coincide w... | 10.558821 | 10.064905 | 11.052307 | 9.367793 | 9.658986 | 10.328028 | 10.13656 | 9.43872 | 9.953543 | 11.296219 | 9.871166 | 9.262166 | 9.849068 | 9.59889 | 9.413191 | 9.713638 | 9.476615 | 9.391045 | 9.783916 | 10.233915 | 9.449738 |
hep-th/9304156 | null | Jonathan Underwood | Aspects of Non-Abelian Toda Theories | 29 pages, Imperial/TP/92-93/30 | null | null | null | hep-th | null | We present a definition of the non-abelian generalisations of affine Toda
theory related from the outset to vertex operator constructions of the
corresponding Kac-Moody algebra $\gh$. Reuslts concerning conjugacy classes of
the Weyl group of the finite Lie algebra $\fing$ to embeddings of $A_1$ in
$\fing$ are used bo... | [
{
"created": "Fri, 30 Apr 1993 13:28:29 GMT",
"version": "v1"
},
{
"created": "Fri, 7 May 1993 12:11:31 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Underwood",
"Jonathan",
""
]
] | We present a definition of the non-abelian generalisations of affine Toda theory related from the outset to vertex operator constructions of the corresponding Kac-Moody algebra $\gh$. Reuslts concerning conjugacy classes of the Weyl group of the finite Lie algebra $\fing$ to embeddings of $A_1$ in $\fing$ are used both... | 13.470021 | 12.942342 | 15.222093 | 12.995364 | 13.466218 | 13.205025 | 13.876927 | 13.012025 | 13.278461 | 15.693803 | 12.441547 | 12.757852 | 13.512153 | 12.433194 | 12.908858 | 12.716281 | 12.660591 | 12.493813 | 12.619627 | 14.014167 | 12.149277 |
hep-th/9802149 | Aaron K. Grant | Oded Kenneth and Shmuel Nussinov | A New Variant of the Casimir Effect and Its Exact Evaluation | 10 pages, latex, one figure | null | null | null | hep-th | null | A new version of the Casimir effect where the two plates conduct in specific,
different, directions is considered. By direct functional integration the
evaluation of the Casimir energy as a function of the angle between the
conduction directions is reduced to quadratures. Other applications of the
method and a magnet... | [
{
"created": "Fri, 20 Feb 1998 22:04:38 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kenneth",
"Oded",
""
],
[
"Nussinov",
"Shmuel",
""
]
] | A new version of the Casimir effect where the two plates conduct in specific, different, directions is considered. By direct functional integration the evaluation of the Casimir energy as a function of the angle between the conduction directions is reduced to quadratures. Other applications of the method and a magnetic... | 18.354399 | 15.663502 | 17.392874 | 16.698284 | 14.743757 | 13.941036 | 16.474897 | 15.218449 | 15.667482 | 20.22225 | 16.441431 | 15.371099 | 16.955013 | 16.256105 | 16.897203 | 16.882084 | 15.954301 | 15.413605 | 16.27841 | 17.580114 | 15.667005 |
1401.2207 | Chan Y. Park | Chan Y. Park | 2d SCFT from M-branes and its spectral network | 10 pages, 26 figures, contribution to the Proceedings of String-Math
2013; v2: minor changes, version to appear in the proceedings | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the low-energy limit of the two-dimensional theory on multiple
M2-branes suspended between a flat M5-brane and a curved M5-brane. We argue
that it is described by an $\mathcal{N}=(2,2)$ supersymmetric Landau-Ginzburg
model with the superpotential determined by the shape of the curved M5-branes,
which flow... | [
{
"created": "Thu, 9 Jan 2014 23:48:48 GMT",
"version": "v1"
},
{
"created": "Mon, 5 May 2014 07:25:18 GMT",
"version": "v2"
}
] | 2014-05-06 | [
[
"Park",
"Chan Y.",
""
]
] | We consider the low-energy limit of the two-dimensional theory on multiple M2-branes suspended between a flat M5-brane and a curved M5-brane. We argue that it is described by an $\mathcal{N}=(2,2)$ supersymmetric Landau-Ginzburg model with the superpotential determined by the shape of the curved M5-branes, which flows ... | 6.19231 | 4.41851 | 6.72446 | 5.115742 | 4.727708 | 4.884669 | 4.658381 | 4.810091 | 4.689395 | 7.250981 | 4.611928 | 5.491864 | 6.432477 | 5.625005 | 5.357171 | 5.322867 | 5.517371 | 5.338402 | 5.493383 | 6.512878 | 5.411399 |
hep-th/0011191 | Arkady Tseytlin | R.R. Metsaev and A.A. Tseytlin | Superparticle and superstring in AdS_3 x S^3 Ramond-Ramond background in
light-cone gauge | 32 pages, latex | J.Math.Phys.42:2987-3014,2001 | 10.1063/1.1377274 | FIAN/TD/00-18, OHSTPY-HEP-T-00-029 | hep-th | null | We discuss superparticle and superstring dynamics in AdS_3 x S^3 supported by
R-R 3-form background using light-cone gauge approach. Starting with the
superalgebra psu(1,1|2) + psu(1,1|2) representing the basic symmetry of this
background we find the light-cone superparticle Hamiltonian. We determine the
harmonic dec... | [
{
"created": "Tue, 21 Nov 2000 18:10:29 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Metsaev",
"R. R.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We discuss superparticle and superstring dynamics in AdS_3 x S^3 supported by R-R 3-form background using light-cone gauge approach. Starting with the superalgebra psu(1,1|2) + psu(1,1|2) representing the basic symmetry of this background we find the light-cone superparticle Hamiltonian. We determine the harmonic decom... | 5.150018 | 4.578875 | 6.422149 | 4.488326 | 4.805368 | 4.630433 | 4.812109 | 4.527994 | 4.698438 | 6.220102 | 4.855862 | 4.827998 | 5.563522 | 4.928541 | 4.876906 | 4.82607 | 4.832877 | 4.797698 | 4.958024 | 5.693007 | 4.906167 |
hep-th/0003200 | Marco Matone | G. Bertoldi, J.M. Isidro, M. Matone and P. Pasti | The Concept of a Noncommutative Riemann Surface | 1+16 pages, LaTeX | Phys.Lett. B484 (2000) 323-332 | 10.1016/S0370-2693(00)00648-1 | null | hep-th math.AG | null | We consider the compactification M(atrix) theory on a Riemann surface Sigma
of genus g>1. A natural generalization of the case of the torus leads to
construct a projective unitary representation of pi_1(\Sigma), realized on the
Hilbert space of square integrable functions on the upper half--plane. A
uniquely determin... | [
{
"created": "Wed, 22 Mar 2000 17:23:52 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bertoldi",
"G.",
""
],
[
"Isidro",
"J. M.",
""
],
[
"Matone",
"M.",
""
],
[
"Pasti",
"P.",
""
]
] | We consider the compactification M(atrix) theory on a Riemann surface Sigma of genus g>1. A natural generalization of the case of the torus leads to construct a projective unitary representation of pi_1(\Sigma), realized on the Hilbert space of square integrable functions on the upper half--plane. A uniquely determined... | 9.285335 | 9.417734 | 9.888963 | 8.669092 | 9.978339 | 9.765644 | 10.21664 | 9.179409 | 9.119679 | 10.550176 | 9.274896 | 9.001071 | 9.084338 | 8.939793 | 8.849577 | 8.800607 | 8.971791 | 8.979588 | 8.904759 | 9.200025 | 8.719606 |
2304.02024 | Yu. M. Poluektov | Yu.M. Poluektov | Does a massless Goldstone boson exist? | 20 pages, 4 figures | null | null | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Classical and quantum complex nonlinear scalar fields are considered. A new
approach to the quantization of nonlinear fields and the construction of a
perturbation theory with allowance for spontaneous symmetry breaking is
proposed, based on the use of the relativistic model of a self-consistent field
as the main app... | [
{
"created": "Tue, 4 Apr 2023 12:33:23 GMT",
"version": "v1"
}
] | 2023-04-06 | [
[
"Poluektov",
"Yu. M.",
""
]
] | Classical and quantum complex nonlinear scalar fields are considered. A new approach to the quantization of nonlinear fields and the construction of a perturbation theory with allowance for spontaneous symmetry breaking is proposed, based on the use of the relativistic model of a self-consistent field as the main appro... | 7.163863 | 7.523869 | 6.891005 | 6.784303 | 7.65765 | 7.492557 | 7.452887 | 7.071442 | 6.991344 | 7.610531 | 7.04427 | 6.878788 | 7.096991 | 6.734251 | 6.977785 | 6.944416 | 6.820573 | 6.928597 | 6.793381 | 6.952823 | 6.923339 |
hep-th/9405191 | null | A. de Rujula | Effects of Virtual Monopoles | 21 pages + 5 PS figures (7273fg1 thru 7273fg5 available via anonymous
ftp to /archive/electronic/cern/9405 on darssrv1.cern.ch) requires PHYZZX
macro, CERN-TH.7273/94 | Nucl.Phys.B435:257-276,1995 | 10.1016/0550-3213(94)00436-I | null | hep-th | null | Electromagnetism would be a ``more unified'' theory if there were elementary
magnetic monopoles and/or particles with both electric and magnetic charges
(dyons). I discuss the simplest possibilities for the addition of these
entities onto the Standard Model, and their empirical consequences. Lower
limits on the masse... | [
{
"created": "Tue, 31 May 1994 10:22:45 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"de Rujula",
"A.",
""
]
] | Electromagnetism would be a ``more unified'' theory if there were elementary magnetic monopoles and/or particles with both electric and magnetic charges (dyons). I discuss the simplest possibilities for the addition of these entities onto the Standard Model, and their empirical consequences. Lower limits on the masses ... | 9.164553 | 10.459192 | 9.283996 | 9.021161 | 9.697605 | 10.448884 | 10.745304 | 10.47399 | 9.25833 | 10.049769 | 9.610349 | 9.190711 | 9.607297 | 9.321945 | 9.648528 | 9.362581 | 9.41414 | 9.369211 | 9.258129 | 9.111877 | 9.235449 |
0912.2719 | Sachin Jain | Sachin Jain | Universal properties of thermal and electrical conductivity of gauge
theory plasmas from holography | 13 pages, appendix added, close to journal version | JHEP 1006:023,2010 | 10.1007/JHEP06(2010)023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose that for conformal field theories admitting gravity duals, the
thermal conductivity is fixed by the central charges in a universal manner.
Though we do not have a proof as yet, we have checked our proposal against
several examples. This proposal, if correct, allows us to express electrical
conductivity in ... | [
{
"created": "Mon, 14 Dec 2009 20:05:56 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Apr 2010 20:12:45 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Jun 2010 14:09:41 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Jain",
"Sachin",
""
]
] | We propose that for conformal field theories admitting gravity duals, the thermal conductivity is fixed by the central charges in a universal manner. Though we do not have a proof as yet, we have checked our proposal against several examples. This proposal, if correct, allows us to express electrical conductivity in te... | 10.412292 | 8.66227 | 10.031057 | 8.031966 | 8.234989 | 8.012925 | 7.587409 | 8.481346 | 8.329601 | 11.183308 | 7.653997 | 8.409738 | 9.374846 | 8.542797 | 8.842536 | 8.60923 | 8.844371 | 9.069738 | 8.320755 | 9.256876 | 8.819498 |
hep-th/9407116 | Mei Fang Chu | Meifang Chu and Peter Goddard | Quantisation of a particle moving on a group manifold | DAMTP-94-41, 11 pages | Phys.Lett. B337 (1994) 285-293 | 10.1016/0370-2693(94)90977-6 | null | hep-th | null | The Hilbert space of a free massless particle moving on a group manifold is
studied in details using canonical quantisation. While the simplest model is
invariant under a global symmetry, $G \times G$, there is a very natural way to
``factorise" the theory so that only one copy of the global symmetry is
preserved. In... | [
{
"created": "Tue, 19 Jul 1994 20:31:24 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Chu",
"Meifang",
""
],
[
"Goddard",
"Peter",
""
]
] | The Hilbert space of a free massless particle moving on a group manifold is studied in details using canonical quantisation. While the simplest model is invariant under a global symmetry, $G \times G$, there is a very natural way to ``factorise" the theory so that only one copy of the global symmetry is preserved. In t... | 9.272678 | 8.234832 | 9.264135 | 7.484076 | 8.090813 | 7.647461 | 8.21749 | 7.559898 | 7.786788 | 9.461916 | 7.84889 | 8.014205 | 8.225029 | 7.851801 | 8.166382 | 7.898215 | 7.969024 | 7.944584 | 8.020715 | 8.328293 | 7.888871 |
2205.06216 | Andrea E. V. Ferrari | Andrea E. V. Ferrari | Supersymmetric ground states of 3d $\mathcal{N}=4$ SUSY gauge theories
and Heisenberg Algebras | Scipost version. Minor notational change in the appendix, typos
corrected | SciPost Phys. 14, 063 (2023) | 10.21468/SciPostPhys.14.4.063 | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We consider 3d $\mathcal{N} = 4$ theories on the geometry
$\Sigma\times\mathbb{R}$, where $\Sigma$ is a closed and connected Riemann
surface, from the point of view of a quantum mechanics on $\mathbb{R}$.
Focussing on the elementary mirror pair in the presence of real deformation
parameters, namely SQED with one hype... | [
{
"created": "Thu, 12 May 2022 17:01:21 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Nov 2022 21:25:15 GMT",
"version": "v2"
},
{
"created": "Fri, 21 Apr 2023 16:18:54 GMT",
"version": "v3"
}
] | 2023-04-24 | [
[
"Ferrari",
"Andrea E. V.",
""
]
] | We consider 3d $\mathcal{N} = 4$ theories on the geometry $\Sigma\times\mathbb{R}$, where $\Sigma$ is a closed and connected Riemann surface, from the point of view of a quantum mechanics on $\mathbb{R}$. Focussing on the elementary mirror pair in the presence of real deformation parameters, namely SQED with one hyperm... | 6.595922 | 6.411694 | 7.704327 | 5.873668 | 6.799424 | 6.684272 | 6.70401 | 6.534807 | 5.944773 | 8.376178 | 6.043576 | 6.007131 | 6.67328 | 6.09776 | 6.102141 | 6.12564 | 6.027966 | 5.933901 | 5.989446 | 6.694571 | 6.011611 |
hep-th/9603127 | Dan Kabat | Daniel Kabat and Philippe Pouliot | A Comment on Zero-brane Quantum Mechanics | 9 pages, harvmac, improved treatment of 2+1 problem | Phys.Rev.Lett.77:1004-1007,1996 | 10.1103/PhysRevLett.77.1004 | RU--96--17 | hep-th | null | We consider low energy, non-relativistic scattering of two Dirichlet
zero-branes as an exercise in quantum mechanics. For weak string coupling and
sufficiently small velocity, the dynamics is governed by an effective U(2)
gauge theory in 0+1 dimensions. At low energies, D-brane scattering can
reliably probe distances... | [
{
"created": "Tue, 19 Mar 1996 03:38:42 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Apr 1996 06:06:43 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Kabat",
"Daniel",
""
],
[
"Pouliot",
"Philippe",
""
]
] | We consider low energy, non-relativistic scattering of two Dirichlet zero-branes as an exercise in quantum mechanics. For weak string coupling and sufficiently small velocity, the dynamics is governed by an effective U(2) gauge theory in 0+1 dimensions. At low energies, D-brane scattering can reliably probe distances m... | 12.050986 | 9.982406 | 12.672997 | 9.38301 | 10.021328 | 10.773809 | 10.128951 | 10.358796 | 9.221397 | 13.263056 | 10.246027 | 10.07778 | 11.712908 | 9.97601 | 10.040525 | 9.643029 | 9.910769 | 10.178679 | 9.933021 | 11.846453 | 10.282195 |
hep-th/9301012 | Ronald Rietman | Bernard Nienhuis and Ronald Rietman | A Solvable Model for Intersecting Loops | 9 pages LaTex, uses epsf.sty | null | null | ITFA-92-35 | hep-th | null | We show that some models with non-local (and non-localizable) interactions
have a property, called quasi-locality, which allows for the definition of a
transfer matrix. We give the Yang-Baxter equation as a sufficient condition for
the existence of a family of commuting transfer matrices and solve them for a
loop mod... | [
{
"created": "Tue, 5 Jan 1993 14:43:10 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nienhuis",
"Bernard",
""
],
[
"Rietman",
"Ronald",
""
]
] | We show that some models with non-local (and non-localizable) interactions have a property, called quasi-locality, which allows for the definition of a transfer matrix. We give the Yang-Baxter equation as a sufficient condition for the existence of a family of commuting transfer matrices and solve them for a loop model... | 13.380583 | 12.266164 | 14.048273 | 12.475702 | 13.120062 | 12.702531 | 14.307527 | 11.916471 | 12.836861 | 16.047907 | 13.093559 | 13.084516 | 12.813536 | 13.36552 | 13.109509 | 12.881327 | 12.811676 | 12.861564 | 13.02594 | 13.184564 | 12.785501 |
hep-th/9301125 | Swapna Mahapatra | Swapna Mahapatra | On the Rotating Charged Black String Solution | 12 pages, IMSC-93/6,(Phyzzx macro), January 1993 | Phys.Rev. D50 (1994) 947-951 | 10.1103/PhysRevD.50.947 | null | hep-th | null | A rotating charged black string solution in the low energy effective field
theory describing five dimensional heterotic string theory is constructed. The
solution is labelled by mass, electric charge, axion charge and angular
momentum per unit length. The extremal limit of this solution is also studied.
| [
{
"created": "Wed, 27 Jan 1993 14:53:56 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Mahapatra",
"Swapna",
""
]
] | A rotating charged black string solution in the low energy effective field theory describing five dimensional heterotic string theory is constructed. The solution is labelled by mass, electric charge, axion charge and angular momentum per unit length. The extremal limit of this solution is also studied. | 8.942971 | 5.552451 | 5.662625 | 4.799966 | 5.114993 | 4.704647 | 5.249468 | 4.678905 | 5.301166 | 5.422654 | 5.026325 | 5.889258 | 6.238789 | 5.864136 | 6.200943 | 5.64482 | 5.420903 | 5.364449 | 5.850591 | 5.735715 | 5.498799 |
hep-th/0101096 | Chris Pope | M. Cvetic, G.W. Gibbons, H. Lu and C.N. Pope | Supersymmetric Non-singular Fractional D2-branes and NS-NS 2-branes | Latex, 30 pages | Nucl.Phys.B606:18-44,2001 | 10.1016/S0550-3213(01)00236-X | null | hep-th | null | We obtain regular deformed D2-brane solutions with fractional D2-branes
arising as wrapped D4-branes. The space transverse to the D2-brane is a
complete Ricci-flat 7-manifold of G_2 holonomy, which is asymptotically conical
with principal orbits that are topologically CP^3 or the flag manifold
SU(3)/(U(1) x U(1)). We... | [
{
"created": "Tue, 16 Jan 2001 23:49:09 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Cvetic",
"M.",
""
],
[
"Gibbons",
"G. W.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
]
] | We obtain regular deformed D2-brane solutions with fractional D2-branes arising as wrapped D4-branes. The space transverse to the D2-brane is a complete Ricci-flat 7-manifold of G_2 holonomy, which is asymptotically conical with principal orbits that are topologically CP^3 or the flag manifold SU(3)/(U(1) x U(1)). We o... | 6.724449 | 6.69341 | 7.842448 | 6.488231 | 6.765607 | 6.691131 | 7.102005 | 6.612422 | 6.445272 | 8.313547 | 6.43633 | 6.499493 | 7.042634 | 6.521861 | 6.589962 | 6.684499 | 6.689288 | 6.432817 | 6.644369 | 7.036771 | 6.504465 |
1205.5180 | Lincoln D. Carr | Allan Adams, Lincoln D. Carr, Thomas Schaefer, Peter Steinberg, and
John E. Thomas | Strongly Correlated Quantum Fluids: Ultracold Quantum Gases, Quantum
Chromodynamic Plasmas, and Holographic Duality | 138 pages, 25 figures, review associated with New Journal of Physics
special issue "Focus on Strongly Correlated Quantum Fluids: from Ultracold
Quantum Gases to QCD Plasmas"
(http://iopscience.iop.org/1367-2630/focus/Focus%20on%20Strongly%20Correlated%20Quantum%20Fluids%20-%20from%20Ultracold%20Quantum%20Gases%20... | New J. Phys. v. 14, p. 115009 (2012) | 10.1088/1367-2630/14/11/115009 | null | hep-th cond-mat.quant-gas nucl-ex nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Strongly correlated quantum fluids are phases of matter that are
intrinsically quantum mechanical, and that do not have a simple description in
terms of weakly interacting quasi-particles. Two systems that have recently
attracted a great deal of interest are the quark-gluon plasma, a plasma of
strongly interacting qu... | [
{
"created": "Wed, 23 May 2012 14:14:33 GMT",
"version": "v1"
}
] | 2015-03-20 | [
[
"Adams",
"Allan",
""
],
[
"Carr",
"Lincoln D.",
""
],
[
"Schaefer",
"Thomas",
""
],
[
"Steinberg",
"Peter",
""
],
[
"Thomas",
"John E.",
""
]
] | Strongly correlated quantum fluids are phases of matter that are intrinsically quantum mechanical, and that do not have a simple description in terms of weakly interacting quasi-particles. Two systems that have recently attracted a great deal of interest are the quark-gluon plasma, a plasma of strongly interacting quar... | 6.230834 | 7.09609 | 6.899934 | 6.346388 | 7.23796 | 7.104826 | 7.742249 | 6.529827 | 6.441714 | 7.056578 | 6.636753 | 6.039637 | 5.959813 | 5.903184 | 6.038798 | 6.112017 | 6.100418 | 5.803335 | 6.196549 | 6.150819 | 6.214928 |
2407.17133 | Oliver Schnetz | Oliver Schnetz, Simon Theil | Notes on graphical functions with numerator structure | 11 pages, 1 figure | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In these notes we generalize the theory of graphical functions from scalar
theories to theories with spin.
| [
{
"created": "Wed, 24 Jul 2024 10:09:42 GMT",
"version": "v1"
}
] | 2024-07-25 | [
[
"Schnetz",
"Oliver",
""
],
[
"Theil",
"Simon",
""
]
] | In these notes we generalize the theory of graphical functions from scalar theories to theories with spin. | 41.299049 | 18.397751 | 31.903635 | 16.956129 | 19.57143 | 16.323381 | 15.991968 | 16.300444 | 15.51332 | 24.628134 | 23.017946 | 21.758171 | 20.823055 | 19.969473 | 20.046827 | 21.641245 | 19.429853 | 19.517519 | 18.821497 | 21.865356 | 24.448957 |
hep-th/9512081 | null | A.A. Tseytlin | Heterotic - type I superstring duality and low-energy effective actions | 16 pages, harvmac | Nucl.Phys.B467:383-398,1996 | 10.1016/0550-3213(96)00080-6 | Imperial/TP/95-96/16 | hep-th | null | We compare order $R^4$ terms in the 10-dimensional effective actions of
SO(32) heterotic and type I superstrings from the point of view of duality
between the two theories. Some of these terms do not receive higher-loop
corrections being related by supersymmetry to `anomaly-cancelling' terms which
depend on the antis... | [
{
"created": "Mon, 11 Dec 1995 22:37:13 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Tseytlin",
"A. A.",
""
]
] | We compare order $R^4$ terms in the 10-dimensional effective actions of SO(32) heterotic and type I superstrings from the point of view of duality between the two theories. Some of these terms do not receive higher-loop corrections being related by supersymmetry to `anomaly-cancelling' terms which depend on the antisym... | 9.332109 | 9.127522 | 10.305875 | 8.424491 | 8.312542 | 8.611654 | 8.972951 | 7.750443 | 8.532519 | 10.522448 | 7.975669 | 8.216383 | 9.012565 | 8.348854 | 8.275218 | 8.30321 | 8.072062 | 8.221372 | 8.215927 | 8.956886 | 8.138254 |
2002.12746 | Andrei Mironov | H. Awata, H. Kanno, A. Mironov, A. Morozov | Shiraishi functor and non-Kerov deformation of Macdonald polynomials | 17 pages | Eur. Phys. J. C80 (2020) 994 | 10.1140/epjc/s10052-020-08540-4 | FIAN/TD-02/20; IITP/TH-02/20; ITEP/TH-02/20; MIPT/TH-02/20 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We suggest a further generalization of the hypergeometric-like series due to
M. Noumi and J. Shiraishi by substituting the Pochhammer symbol with a nearly
arbitrary function. Moreover, this generalization is valid for the entire
Shiraishi series, not only for its Noumi-Shiraishi part. The theta function
needed in the... | [
{
"created": "Fri, 28 Feb 2020 14:36:56 GMT",
"version": "v1"
}
] | 2020-11-03 | [
[
"Awata",
"H.",
""
],
[
"Kanno",
"H.",
""
],
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | We suggest a further generalization of the hypergeometric-like series due to M. Noumi and J. Shiraishi by substituting the Pochhammer symbol with a nearly arbitrary function. Moreover, this generalization is valid for the entire Shiraishi series, not only for its Noumi-Shiraishi part. The theta function needed in the r... | 12.900382 | 14.410548 | 15.148456 | 13.144743 | 14.276225 | 13.851119 | 13.663205 | 13.942082 | 13.269964 | 15.843649 | 13.042425 | 12.803471 | 13.404623 | 12.67358 | 13.05402 | 12.655422 | 12.677579 | 12.437367 | 12.866282 | 13.438328 | 12.324114 |
1211.2397 | Paulo Assis | P. E. G. Assis | A(2|1) spectral equivalences and nonlocal integrals of motion | null | null | 10.1088/1751-8113/46/19/195204 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the spectral correspondence between a particular class of
Schrodinger equations and supersymmetric quantum integrable model (QIM). The
latter, a quantized version of the Ablowitz-Kaupp-Newell-Segur (AKNS) hierarchy
of nonlinear equations, corresponds to the thermodynamic limit of the
Perk-Schultz lattice mod... | [
{
"created": "Sun, 11 Nov 2012 11:23:27 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Nov 2012 17:19:57 GMT",
"version": "v2"
}
] | 2015-06-12 | [
[
"Assis",
"P. E. G.",
""
]
] | We study the spectral correspondence between a particular class of Schrodinger equations and supersymmetric quantum integrable model (QIM). The latter, a quantized version of the Ablowitz-Kaupp-Newell-Segur (AKNS) hierarchy of nonlinear equations, corresponds to the thermodynamic limit of the Perk-Schultz lattice model... | 10.573749 | 11.702206 | 13.647191 | 10.386788 | 11.143485 | 10.905614 | 11.733766 | 10.161448 | 10.999878 | 12.000801 | 10.236832 | 10.743654 | 11.37529 | 10.349277 | 10.485659 | 10.634792 | 10.358544 | 10.522158 | 10.478069 | 11.491088 | 10.481219 |
2002.09933 | Pietro Menotti | Pietro Menotti | Real analyticity of accessory parameters | 24 pages LaTex | null | null | IFUP-TH/2020 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the problem of the real analytic dependence of the accessory
parameters of Liouville theory on the moduli of the problem, for general
elliptic singularities. We give a simplified proof of the almost everywhere
real analyticity in the case of a single accessory parameter as it occurs e.g.
in the sphere top... | [
{
"created": "Sun, 23 Feb 2020 16:22:01 GMT",
"version": "v1"
}
] | 2020-02-27 | [
[
"Menotti",
"Pietro",
""
]
] | We consider the problem of the real analytic dependence of the accessory parameters of Liouville theory on the moduli of the problem, for general elliptic singularities. We give a simplified proof of the almost everywhere real analyticity in the case of a single accessory parameter as it occurs e.g. in the sphere topol... | 12.605765 | 12.517787 | 13.120405 | 12.12209 | 12.229523 | 13.506642 | 12.257715 | 13.260363 | 11.411571 | 16.169174 | 12.245625 | 12.190473 | 12.992045 | 12.204801 | 12.278886 | 12.218832 | 12.481617 | 12.02611 | 12.100864 | 12.787396 | 11.989913 |
1810.08093 | Jes\'us Montero | Yolanda Lozano, Niall T. Macpherson, Jes\'us Montero | $AdS_6$ T-duals and Type IIB $AdS_6\times S^2$ Geometries with 7-Branes | 36 pages plus appendices. 3 figures. v2: reference added. v3: section
5 improved, version accepted in JHEP | null | 10.1007/JHEP01(2019)116 | FPAUO-18/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the first $AdS_6$ backgrounds in Type IIB supergravity known in
the literature, namely those constructed via T-duality from the Brandhuber-Oz
solution to massive IIA, fit within an extension of the global $AdS_6 \times
S^2$ solutions with 7-branes warped over a Riemann surface $\Sigma$, recently
classifi... | [
{
"created": "Thu, 18 Oct 2018 14:58:42 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Oct 2018 18:46:25 GMT",
"version": "v2"
},
{
"created": "Thu, 10 Jan 2019 16:19:01 GMT",
"version": "v3"
}
] | 2019-02-20 | [
[
"Lozano",
"Yolanda",
""
],
[
"Macpherson",
"Niall T.",
""
],
[
"Montero",
"Jesús",
""
]
] | We show that the first $AdS_6$ backgrounds in Type IIB supergravity known in the literature, namely those constructed via T-duality from the Brandhuber-Oz solution to massive IIA, fit within an extension of the global $AdS_6 \times S^2$ solutions with 7-branes warped over a Riemann surface $\Sigma$, recently classified... | 8.103395 | 7.327909 | 11.098537 | 7.411755 | 8.026258 | 7.392355 | 7.606114 | 7.794716 | 7.726982 | 11.877007 | 7.602147 | 7.192848 | 8.169838 | 7.844411 | 7.594794 | 7.576529 | 7.450187 | 7.68459 | 7.81931 | 8.755692 | 7.532372 |
1707.03866 | Grigory Tarnopolsky | Simone Giombi, Igor R. Klebanov, Grigory Tarnopolsky | Bosonic Tensor Models at Large $N$ and Small $\epsilon$ | 20 pages, 3 figures, v2: minor corrections, references added | Phys. Rev. D 96, 106014 (2017) | 10.1103/PhysRevD.96.106014 | PUPT-2528 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the spectrum of the large $N$ quantum field theory of bosonic
rank-$3$ tensors, whose quartic interactions are such that the perturbative
expansion is dominated by the melonic diagrams. We use the Schwinger-Dyson
equations to determine the scaling dimensions of the bilinear operators of
arbitrary spin. Using... | [
{
"created": "Wed, 12 Jul 2017 18:52:48 GMT",
"version": "v1"
},
{
"created": "Sun, 6 Aug 2017 20:05:40 GMT",
"version": "v2"
}
] | 2017-11-29 | [
[
"Giombi",
"Simone",
""
],
[
"Klebanov",
"Igor R.",
""
],
[
"Tarnopolsky",
"Grigory",
""
]
] | We study the spectrum of the large $N$ quantum field theory of bosonic rank-$3$ tensors, whose quartic interactions are such that the perturbative expansion is dominated by the melonic diagrams. We use the Schwinger-Dyson equations to determine the scaling dimensions of the bilinear operators of arbitrary spin. Using t... | 6.191509 | 5.950027 | 6.372463 | 6.037509 | 6.234812 | 6.190096 | 5.902526 | 5.962941 | 5.941525 | 7.234027 | 5.910282 | 6.016801 | 6.33962 | 6.031888 | 6.104857 | 6.082935 | 5.829628 | 6.095346 | 6.024751 | 6.119151 | 6.067176 |
hep-th/9212154 | Masafumi Fukuma | M.Fukuma, S.Hosono and H.Kawai | Lattice Topological Field Theory in Two Dimensions | 29 pages (Latex) + 19 figures (uuencoded through uufiles) | Commun. Math. Phys. 161 (1994) 157-176 | 10.1007/BF02099416 | CLNS92/1173 | hep-th | null | The lattice definition of a two-dimensional topological field theory (TFT) is
given generically, and the exact solution is obtained explicitly. In
particular, the set of all lattice topological field theories is shown to be in
one-to-one correspondence with the set of all associative algebras $R$, and the
physical Hi... | [
{
"created": "Mon, 28 Dec 1992 21:47:10 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Fukuma",
"M.",
""
],
[
"Hosono",
"S.",
""
],
[
"Kawai",
"H.",
""
]
] | The lattice definition of a two-dimensional topological field theory (TFT) is given generically, and the exact solution is obtained explicitly. In particular, the set of all lattice topological field theories is shown to be in one-to-one correspondence with the set of all associative algebras $R$, and the physical Hilb... | 7.554527 | 6.808568 | 8.274435 | 6.6408 | 7.31773 | 6.625761 | 6.912858 | 6.857293 | 6.842888 | 8.033862 | 6.584182 | 6.56393 | 7.251905 | 6.534339 | 6.69062 | 6.674593 | 6.71401 | 6.47638 | 6.725823 | 7.084501 | 6.568179 |
1209.0791 | Zoltan Bajnok | Zoltan Bajnok and Romuald A. Janik | Six and seven loop Konishi from Luscher corrections | 18 pages, typos corrected | null | 10.1007/JHEP11(2012)002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper we derive six and seven loop formulas for the anomalous
dimension of the Konishi operator in N=4 SYM from string theory using the
technique of Luscher corrections. We derive analytically the integrand using
the worldsheet S-matrix and evaluate the resulting integral and infinite sum
using a combi... | [
{
"created": "Tue, 4 Sep 2012 20:18:04 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Oct 2012 11:48:44 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Bajnok",
"Zoltan",
""
],
[
"Janik",
"Romuald A.",
""
]
] | In the present paper we derive six and seven loop formulas for the anomalous dimension of the Konishi operator in N=4 SYM from string theory using the technique of Luscher corrections. We derive analytically the integrand using the worldsheet S-matrix and evaluate the resulting integral and infinite sum using a combina... | 11.054334 | 11.871665 | 14.875657 | 10.982309 | 12.024808 | 11.026116 | 10.770889 | 11.287373 | 9.8216 | 13.756897 | 10.474498 | 10.670322 | 12.189816 | 11.05987 | 10.594882 | 10.625864 | 10.588179 | 10.435691 | 11.25303 | 11.610331 | 10.547266 |
1903.02838 | Christoph Schweigert | J\"urgen Fuchs, Christoph Schweigert | Full Logarithmic Conformal Field theory - an Attempt at a Status Report | 13 pages, Contribution to Proceedings of LMS/EPSRC Durham Symposium
Higher Structures in M-Theory, August 2018 | null | 10.1002/prop.201910018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Logarithmic conformal field theories are based on vertex algebras with
non-semisimple representation categories. While examples of such theories have
been known for more than 25 years, some crucial aspects of local logarithmic
CFTs have been understood only recently, with the help of a description of
conformal blocks... | [
{
"created": "Thu, 7 Mar 2019 11:17:22 GMT",
"version": "v1"
}
] | 2021-07-28 | [
[
"Fuchs",
"Jürgen",
""
],
[
"Schweigert",
"Christoph",
""
]
] | Logarithmic conformal field theories are based on vertex algebras with non-semisimple representation categories. While examples of such theories have been known for more than 25 years, some crucial aspects of local logarithmic CFTs have been understood only recently, with the help of a description of conformal blocks b... | 7.313631 | 9.4749 | 12.734586 | 9.520616 | 11.6359 | 8.750867 | 9.938068 | 8.563518 | 8.482011 | 11.625942 | 8.772548 | 7.190456 | 7.651589 | 7.163215 | 6.954438 | 7.33077 | 7.097806 | 6.836309 | 7.198398 | 7.957268 | 7.243217 |
2106.12518 | Ming-Zhi Chung | Bo-Ting Chen, Ming-Zhi Chung, Yu-tin Huang, Man Kuan Tam | Minimal spin deflection of Kerr-Newman and Supersymmetric black hole | 28 pages, 6 figures, 1 ancillary file | null | 10.1007/JHEP10(2021)011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent studies have shown that minimal couplings for massive spinning
particles, which in the classical limit reproduce the leading PM Kerr black
hole dynamics, leads to an Eikonal S-matrix exhibiting spin-entanglement
suppression. In this paper we trace this phenomenon to the suppression of
spin-flipping components ... | [
{
"created": "Wed, 23 Jun 2021 16:33:46 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Dec 2021 02:35:23 GMT",
"version": "v2"
}
] | 2021-12-06 | [
[
"Chen",
"Bo-Ting",
""
],
[
"Chung",
"Ming-Zhi",
""
],
[
"Huang",
"Yu-tin",
""
],
[
"Tam",
"Man Kuan",
""
]
] | Recent studies have shown that minimal couplings for massive spinning particles, which in the classical limit reproduce the leading PM Kerr black hole dynamics, leads to an Eikonal S-matrix exhibiting spin-entanglement suppression. In this paper we trace this phenomenon to the suppression of spin-flipping components in... | 15.189711 | 14.555504 | 14.473453 | 13.172647 | 14.651073 | 14.519327 | 13.412306 | 13.871166 | 13.334135 | 17.337933 | 13.470316 | 12.681049 | 14.313091 | 13.398102 | 13.453365 | 12.723126 | 12.903145 | 12.237861 | 13.136021 | 13.67068 | 13.043464 |
2109.13240 | Andrea Fontanella | Andrea Fontanella and Juan Miguel Nieto Garc\'ia | Classical string solutions in Non-Relativistic AdS$_5\times$S$^5$:
Closed and Twisted sectors | 41 pages, 5 figures. v2: typos corrected, few comments and references
added. Matching the published version | Journal of Physics A: Mathematical and Theoretical (2022) | 10.1088/1751-8121/ac4abd | HU-EP-21/35, DMUS-MP-21/15 | hep-th | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We find classical closed string solutions to the non-relativistic
AdS$_5\times$S$^5$ string theory which are the analogue of the BMN and GKP
solutions for the relativistic theory. We show that non-relativistic
AdS$_5\times$S$^5$ string theory admits a $\mathbb{Z}_2$ orbifold symmetry
which allows us to impose twisted... | [
{
"created": "Mon, 27 Sep 2021 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Feb 2022 13:42:42 GMT",
"version": "v2"
}
] | 2022-02-03 | [
[
"Fontanella",
"Andrea",
""
],
[
"García",
"Juan Miguel Nieto",
""
]
] | We find classical closed string solutions to the non-relativistic AdS$_5\times$S$^5$ string theory which are the analogue of the BMN and GKP solutions for the relativistic theory. We show that non-relativistic AdS$_5\times$S$^5$ string theory admits a $\mathbb{Z}_2$ orbifold symmetry which allows us to impose twisted b... | 6.716853 | 5.842112 | 7.198457 | 5.846945 | 6.014939 | 5.811227 | 5.812023 | 5.955592 | 5.904896 | 7.081949 | 5.944581 | 5.989429 | 6.580716 | 5.981949 | 6.0381 | 5.840409 | 5.640167 | 6.193219 | 6.003096 | 6.759427 | 5.90638 |
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