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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2407.07044 | Danai Roumelioti | Danai Roumelioti, Stelios Stefas, George Zoupanos | Fuzzy Gravity: Four-Dimensional Gravity on a Covariant Noncommutative
Space and Unification with Internal Interactions | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present work we present an extended description of the covariant
noncommutative space, which accommodates the Fuzzy Gravity model constructed
previously. It is based on the historical lesson that the use of larger
algebras containing all generators of the isometry of the continuous one helped
in formulating a ... | [
{
"created": "Tue, 9 Jul 2024 17:05:41 GMT",
"version": "v1"
}
] | 2024-07-10 | [
[
"Roumelioti",
"Danai",
""
],
[
"Stefas",
"Stelios",
""
],
[
"Zoupanos",
"George",
""
]
] | In the present work we present an extended description of the covariant noncommutative space, which accommodates the Fuzzy Gravity model constructed previously. It is based on the historical lesson that the use of larger algebras containing all generators of the isometry of the continuous one helped in formulating a fu... | 10.427073 | 10.774691 | 10.593135 | 10.052274 | 10.36414 | 10.384531 | 10.105454 | 10.234698 | 10.138743 | 10.497112 | 10.084748 | 9.82943 | 10.130526 | 10.009131 | 10.193132 | 10.120569 | 10.326432 | 9.835508 | 10.052777 | 10.354179 | 10.064818 |
hep-th/9605109 | Burkhard Kleihaus | Burkhard Kleihaus (1), Jutta Kunz (1) and Abha Sood (1) ((1)
Department of Physics, Universitaet Oldenburg, Germany) | Sequences of Einstein-Yang-Mills-Dilaton Black Holes | 71 pages, Latex2e, 29 ps-figures included | Phys.Rev. D54 (1996) 5070-5092 | 10.1103/PhysRevD.54.5070 | null | hep-th gr-qc hep-ph | null | Einstein-Yang-Mills-dilaton theory possesses sequences of neutral static
spherically symmetric black hole solutions. The solutions depend on the dilaton
coupling constant $\gamma$ and on the horizon. The SU(2) solutions are labelled
by the number of nodes $n$ of the single gauge field function, whereas the
SO(3) solu... | [
{
"created": "Wed, 15 May 1996 17:23:43 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Kleihaus",
"Burkhard",
""
],
[
"Kunz",
"Jutta",
""
],
[
"Sood",
"Abha",
""
]
] | Einstein-Yang-Mills-dilaton theory possesses sequences of neutral static spherically symmetric black hole solutions. The solutions depend on the dilaton coupling constant $\gamma$ and on the horizon. The SU(2) solutions are labelled by the number of nodes $n$ of the single gauge field function, whereas the SO(3) soluti... | 6.0136 | 5.857489 | 5.778262 | 5.663297 | 5.882023 | 6.077361 | 5.716822 | 5.534398 | 5.769094 | 6.270155 | 5.700068 | 5.68654 | 5.704791 | 5.610517 | 5.648358 | 5.524579 | 5.576519 | 5.410817 | 5.627294 | 5.774142 | 5.608994 |
hep-th/0502203 | Roman Buniy | Roman V. Buniy, Stephen D.H. Hsu | Instabilities and the null energy condition | 5 pages, 1 figure, revtex, presentation improved, minor changes | Phys.Lett. B632 (2006) 543-546 | 10.1016/j.physletb.2005.10.075 | null | hep-th astro-ph gr-qc hep-ph | null | We show that violation of the null energy condition implies instability in a
broad class of models, including classical gauge theories with scalar and
fermionic matter as well as any perfect fluid. When applied to the dark energy,
our results imply that $w = p / \rho$ is unlikely to be less than -1.
| [
{
"created": "Tue, 22 Feb 2005 21:04:23 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Mar 2005 00:11:10 GMT",
"version": "v2"
},
{
"created": "Wed, 8 Jun 2005 21:48:29 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Buniy",
"Roman V.",
""
],
[
"Hsu",
"Stephen D. H.",
""
]
] | We show that violation of the null energy condition implies instability in a broad class of models, including classical gauge theories with scalar and fermionic matter as well as any perfect fluid. When applied to the dark energy, our results imply that $w = p / \rho$ is unlikely to be less than -1. | 9.348067 | 7.134106 | 8.891199 | 8.518258 | 7.402758 | 7.568959 | 6.848466 | 7.406429 | 7.117612 | 10.016422 | 7.498896 | 8.364615 | 9.18248 | 8.560661 | 8.319225 | 8.650118 | 8.608801 | 8.358013 | 8.754334 | 9.100445 | 8.561082 |
2403.12127 | Yiwen Pan | Yiwen Pan, Peihe Yang | Modularity of Schur index, modular differential equations, and
high-temperature asymptotics | 44 pages; v2, typo corrected, references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we analytically explore the modularity of the flavored Schur
index of 4d $\mathcal{N} = 2$ SCFTs. We focus on the $A_1$ theories of
class-$\mathcal{S}$ and $\mathcal{N} = 4$ theories with $SU(N)$ gauge group. We
work out the modular orbit of the flavored index and defect index, compute the
dimension of ... | [
{
"created": "Mon, 18 Mar 2024 18:00:01 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Apr 2024 01:40:14 GMT",
"version": "v2"
}
] | 2024-04-16 | [
[
"Pan",
"Yiwen",
""
],
[
"Yang",
"Peihe",
""
]
] | In this paper we analytically explore the modularity of the flavored Schur index of 4d $\mathcal{N} = 2$ SCFTs. We focus on the $A_1$ theories of class-$\mathcal{S}$ and $\mathcal{N} = 4$ theories with $SU(N)$ gauge group. We work out the modular orbit of the flavored index and defect index, compute the dimension of th... | 8.039896 | 7.949379 | 9.319656 | 7.591763 | 8.200101 | 7.519586 | 8.235505 | 7.93437 | 7.309072 | 9.764951 | 7.621177 | 7.505367 | 7.935236 | 7.43258 | 7.540002 | 7.447943 | 7.475996 | 7.324819 | 7.369832 | 8.177566 | 7.485486 |
1908.03502 | Mohsen Alishahiha | Amin Akhavan and Mohsen Alishahiha | An Infalling Observer and Behind the Horizon Cutoff | 11 pages, one figure, refs added. Published version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using Papadodimas and Raju construction of operators describing the interior
of a black hole, we present a general relation between partition functions of
operators describing inside and outside the black hole horizon. In particular
for an eternal black hole the partition function of the interior modes may be
given i... | [
{
"created": "Thu, 8 Aug 2019 12:07:22 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jan 2020 16:34:43 GMT",
"version": "v2"
}
] | 2020-01-24 | [
[
"Akhavan",
"Amin",
""
],
[
"Alishahiha",
"Mohsen",
""
]
] | Using Papadodimas and Raju construction of operators describing the interior of a black hole, we present a general relation between partition functions of operators describing inside and outside the black hole horizon. In particular for an eternal black hole the partition function of the interior modes may be given in ... | 15.161994 | 12.656637 | 14.854983 | 12.689739 | 12.322081 | 12.624114 | 12.363047 | 13.321405 | 12.150656 | 17.193031 | 13.068537 | 12.772028 | 13.390087 | 13.009608 | 13.175469 | 12.431934 | 12.356823 | 12.42657 | 12.785439 | 13.913147 | 12.66991 |
0806.3250 | Juan Antonio Nieto | J. A. Nieto, E. A. Leon | Issues of duality in Abelian Gauge Theory and in Linearized Gravity | 18 pages, Latex, minor changes, references added | Rev. Mex. Fis. 55 (2009) 262-269 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We start by describing two of the main proposals for duality in Abelian gauge
theories, namely $F$(ield strength)-duality approach and the $S$% -duality
formalism. We then discuss how $F$-duality and $S$-duality can be applied to
the case of linearized gravity. By emphasizing the similarities and differences
between ... | [
{
"created": "Thu, 19 Jun 2008 17:38:30 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Oct 2008 15:29:02 GMT",
"version": "v2"
},
{
"created": "Thu, 7 May 2009 16:48:49 GMT",
"version": "v3"
}
] | 2014-05-27 | [
[
"Nieto",
"J. A.",
""
],
[
"Leon",
"E. A.",
""
]
] | We start by describing two of the main proposals for duality in Abelian gauge theories, namely $F$(ield strength)-duality approach and the $S$% -duality formalism. We then discuss how $F$-duality and $S$-duality can be applied to the case of linearized gravity. By emphasizing the similarities and differences between th... | 10.263989 | 9.826736 | 9.757692 | 9.128316 | 9.476139 | 9.286318 | 10.58956 | 9.899511 | 9.282247 | 10.89535 | 9.139321 | 9.447824 | 10.026184 | 9.587566 | 10.281139 | 9.3236 | 9.244258 | 9.184946 | 10.054564 | 10.547824 | 9.940699 |
1904.07217 | Ramon Miravitllas | Ramon Miravitllas Mas | Resurgence, a problem of missing exponential corrections in asymptotic
expansions | null | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well known that perturbative expansions of path integrals are
divergent. These expansions are to be understood as asymptotic expansions,
which encode the limiting behaviour of the path integral for positive small
coupling. Conventionally, the method of Borel summation assigns a finite answer
to the divergent ex... | [
{
"created": "Mon, 15 Apr 2019 17:49:47 GMT",
"version": "v1"
}
] | 2019-04-16 | [
[
"Mas",
"Ramon Miravitllas",
""
]
] | It is well known that perturbative expansions of path integrals are divergent. These expansions are to be understood as asymptotic expansions, which encode the limiting behaviour of the path integral for positive small coupling. Conventionally, the method of Borel summation assigns a finite answer to the divergent expa... | 8.308163 | 9.161612 | 8.635204 | 8.092661 | 8.839718 | 8.424232 | 8.57955 | 8.352605 | 8.09672 | 8.690912 | 8.06351 | 7.946683 | 8.112895 | 7.864163 | 7.913604 | 7.98667 | 8.198318 | 7.870661 | 7.764536 | 8.16222 | 7.621543 |
1001.4810 | Jean-Pierre Gazeau | Jean-Pierre Gazeau, Petr Siegl and Ahmed Youssef | Krein Spaces in de Sitter Quantum Theories | null | SIGMA 6 (2010), 011, 23 pages | 10.3842/SIGMA.2010.011 | null | hep-th gr-qc math-ph math.MP | http://creativecommons.org/licenses/by-nc-sa/3.0/ | Experimental evidences and theoretical motivations lead to consider the
curved space-time relativity based on the de Sitter group $SO_0(1,4)$ or
$Sp(2,2)$ as an appealing substitute to the flat space-time Poincare
relativity. Quantum elementary systems are then associated to unitary
irreducible representations of tha... | [
{
"created": "Wed, 27 Jan 2010 18:34:53 GMT",
"version": "v1"
}
] | 2010-01-28 | [
[
"Gazeau",
"Jean-Pierre",
""
],
[
"Siegl",
"Petr",
""
],
[
"Youssef",
"Ahmed",
""
]
] | Experimental evidences and theoretical motivations lead to consider the curved space-time relativity based on the de Sitter group $SO_0(1,4)$ or $Sp(2,2)$ as an appealing substitute to the flat space-time Poincare relativity. Quantum elementary systems are then associated to unitary irreducible representations of that ... | 13.318569 | 15.593152 | 12.878269 | 12.91608 | 14.444333 | 13.950126 | 15.019566 | 12.994819 | 13.84239 | 14.684162 | 13.524636 | 13.204602 | 12.871215 | 12.662584 | 12.402054 | 12.725039 | 12.92732 | 12.884131 | 13.259502 | 13.322187 | 12.734404 |
2110.03386 | Otari Sakhelashvili | Otari Sakhelashvili | On dual formulation of Axion solution to strong-CP problem | null | null | 10.1103/PhysRevD.105.085020 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | An exact duality between axion with arbitrary potential and antisymmetric
form-field has been derived some time ago. Using this duality, the axion
solution to strong-CP problem has been formulated as a gauge invariant theory
of forms. In this description, the QCD axion is represented by a Kalb-Ramond
field which is e... | [
{
"created": "Thu, 7 Oct 2021 12:25:56 GMT",
"version": "v1"
}
] | 2022-04-29 | [
[
"Sakhelashvili",
"Otari",
""
]
] | An exact duality between axion with arbitrary potential and antisymmetric form-field has been derived some time ago. Using this duality, the axion solution to strong-CP problem has been formulated as a gauge invariant theory of forms. In this description, the QCD axion is represented by a Kalb-Ramond field which is eat... | 13.065562 | 12.958663 | 12.836309 | 11.182361 | 13.275619 | 12.913673 | 12.746103 | 12.237383 | 11.785013 | 14.114501 | 12.119039 | 12.18358 | 12.049447 | 11.926081 | 12.581924 | 12.251074 | 12.303205 | 12.177345 | 11.852682 | 12.337113 | 12.275195 |
1911.09934 | Yuichi Enoki | Yuichi Enoki, Taizan Watari | Modular Forms as Classification Invariants of 4D N=2 Heterotic--IIA Dual
Vacua | v2: 75 pages. typo and grammatical corrections, as well as minor
corrections | null | 10.1007/JHEP06(2020)021 | IPMU19-0168 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We focus on 4D $\mathcal{N}=2$ string vacua described both by perturbative
Heterotic theory and by Type IIA theory; a Calabi--Yau three-fold $X_{\rm IIA}$
in the Type IIA language is further assumed to have a regular K3-fibration. It
is well-known that one can assign a modular form $\Phi$ to such a vacuum by
counting... | [
{
"created": "Fri, 22 Nov 2019 09:09:28 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Dec 2019 12:55:36 GMT",
"version": "v2"
}
] | 2020-06-24 | [
[
"Enoki",
"Yuichi",
""
],
[
"Watari",
"Taizan",
""
]
] | We focus on 4D $\mathcal{N}=2$ string vacua described both by perturbative Heterotic theory and by Type IIA theory; a Calabi--Yau three-fold $X_{\rm IIA}$ in the Type IIA language is further assumed to have a regular K3-fibration. It is well-known that one can assign a modular form $\Phi$ to such a vacuum by counting p... | 9.109722 | 9.276178 | 10.416179 | 8.911787 | 9.603385 | 9.65656 | 8.685407 | 8.924055 | 8.888855 | 10.699797 | 9.188856 | 8.575521 | 9.450209 | 8.38885 | 8.789927 | 8.629461 | 8.592719 | 8.802285 | 8.436598 | 8.938416 | 8.570613 |
1506.04293 | Edward Witten | Edward Witten | More On Gauge Theory And Geometric Langlands | 79 pp, minor corrections in v. 2, more detailed description of
electric eigenbrane in v. 3 | null | null | null | hep-th math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The geometric Langlands correspondence was described some years ago in terms
of $S$-duality of $\N=4$ super Yang-Mills theory. Some additional matters
relevant to this story are described here. The main goal is to explain directly
why an $A$-brane of a certain simple kind can be an eigenbrane for the action
of 't Hoo... | [
{
"created": "Sat, 13 Jun 2015 16:41:19 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Nov 2016 17:55:19 GMT",
"version": "v2"
},
{
"created": "Fri, 28 Jul 2017 15:29:59 GMT",
"version": "v3"
}
] | 2017-07-31 | [
[
"Witten",
"Edward",
""
]
] | The geometric Langlands correspondence was described some years ago in terms of $S$-duality of $\N=4$ super Yang-Mills theory. Some additional matters relevant to this story are described here. The main goal is to explain directly why an $A$-brane of a certain simple kind can be an eigenbrane for the action of 't Hooft... | 11.124518 | 8.949293 | 12.332765 | 9.612954 | 9.855409 | 9.735206 | 9.909095 | 9.951988 | 9.596062 | 11.874773 | 9.51786 | 9.437167 | 10.397703 | 10.001206 | 9.607187 | 9.582527 | 9.465377 | 9.682858 | 9.737823 | 10.357011 | 9.592532 |
hep-th/0212233 | Gottfried Curio | Gottfried Curio | Superpotential of the M-theory conifold and type IIA string theory | 34 pages, latex; reference added, discussion added (sect. 4), minor
changes | Int.J.Mod.Phys.A19:521-556,2004 | 10.1142/S0217751X04017720 | HU-EP-02/59 | hep-th | null | The membrane instanton superpotential for $M$-theory on the $G_2$ holonomy
manifold given by the cone on ${\bf S^3}\x {\bf S^3}$ is given by the
dilogarithm and has Heisenberg monodromy group in the quantum moduli space. We
compare this to a Heisenberg group action on the type IIA hypermultiplet moduli
space for the ... | [
{
"created": "Thu, 19 Dec 2002 17:45:41 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Jan 2003 12:25:46 GMT",
"version": "v2"
},
{
"created": "Tue, 28 Jan 2003 08:55:13 GMT",
"version": "v3"
}
] | 2010-12-03 | [
[
"Curio",
"Gottfried",
""
]
] | The membrane instanton superpotential for $M$-theory on the $G_2$ holonomy manifold given by the cone on ${\bf S^3}\x {\bf S^3}$ is given by the dilogarithm and has Heisenberg monodromy group in the quantum moduli space. We compare this to a Heisenberg group action on the type IIA hypermultiplet moduli space for the un... | 11.559514 | 10.217052 | 12.841917 | 10.378231 | 10.839146 | 10.217576 | 10.551499 | 9.940464 | 9.995673 | 14.704054 | 10.718461 | 10.156634 | 11.363918 | 10.078491 | 10.456248 | 10.041462 | 10.026359 | 10.43343 | 9.818055 | 10.845929 | 10.635995 |
2201.13366 | Hank Chen | Hank Chen, Florian Girelli | (2-)Drinfel'd Double and (2-)BF Theory | 40 pages; 0 figures (v2: adjusted \tilde t = t^*, fixed some minor
errors and typos) | Phys. Rev. D 106, 105017 (2022) | 10.1103/PhysRevD.106.105017 | null | hep-th cond-mat.str-el gr-qc math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | The gauge symmetry and shift/translational symmetry of a 3D BF action, which
are associated to a pair of dual Lie algebras, can be combined to form the
Drinfel'd double. This combined symmetry is the gauge symmetry of the
Chern-Simons action which is equivalent to the BF action, up to some boundary
term. We show that... | [
{
"created": "Mon, 31 Jan 2022 17:26:36 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Feb 2022 21:55:09 GMT",
"version": "v2"
}
] | 2022-11-22 | [
[
"Chen",
"Hank",
""
],
[
"Girelli",
"Florian",
""
]
] | The gauge symmetry and shift/translational symmetry of a 3D BF action, which are associated to a pair of dual Lie algebras, can be combined to form the Drinfel'd double. This combined symmetry is the gauge symmetry of the Chern-Simons action which is equivalent to the BF action, up to some boundary term. We show that s... | 6.903725 | 7.670819 | 7.546363 | 6.567994 | 7.442522 | 7.614845 | 7.635565 | 7.360799 | 6.990498 | 8.082618 | 6.893505 | 6.59913 | 6.520166 | 6.625228 | 6.588244 | 6.606508 | 6.730489 | 6.546188 | 6.701261 | 6.780027 | 6.51461 |
0901.3412 | Sunandan Gangopadhyay | Joseph Ben Geloun, Sunandan Gangopadhyay, Frederik G Scholtz | Harmonic oscillator in a background magnetic field in noncommutative
quantum phase-space | 7 pages Latex | Europhys.Lett.86:51001,2009 | 10.1209/0295-5075/86/51001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We solve explicitly the two-dimensional harmonic oscillator and the harmonic
oscillator in a background magnetic field in noncommutative phase-space without
making use of any type of representation. A key observation that we make is
that for a specific choice of the noncommutative parameters, the time reversal
symmet... | [
{
"created": "Thu, 22 Jan 2009 14:25:28 GMT",
"version": "v1"
}
] | 2009-08-03 | [
[
"Geloun",
"Joseph Ben",
""
],
[
"Gangopadhyay",
"Sunandan",
""
],
[
"Scholtz",
"Frederik G",
""
]
] | We solve explicitly the two-dimensional harmonic oscillator and the harmonic oscillator in a background magnetic field in noncommutative phase-space without making use of any type of representation. A key observation that we make is that for a specific choice of the noncommutative parameters, the time reversal symmetry... | 7.936517 | 7.60728 | 7.639596 | 7.308703 | 8.192037 | 8.220063 | 8.274817 | 7.519042 | 7.409222 | 8.480028 | 7.17872 | 7.603581 | 7.918161 | 7.497592 | 7.515077 | 7.559074 | 7.54912 | 7.84452 | 7.477473 | 7.707989 | 7.666544 |
hep-th/0507278 | Antonios Papazoglou | Eleftherios Papantonopoulos (Athens, Tech. U.) and Antonios Papazoglou
(ITP, Lausanne) | Cosmological Evolution of a Purely Conical Codimension-2 Brane World | 20 pages, 4 figures, typo corrected | JHEP 0509 (2005) 012 | 10.1088/1126-6708/2005/09/012 | null | hep-th gr-qc | null | We study the cosmological evolution of isotropic matter on an infinitely thin
conical codimension-two brane-world. Our analysis is based on the boundary
dynamics of a six-dimensional model in the presence of an induced gravity term
on the brane and a Gauss-Bonnet term in the bulk. With the assumption that the
bulk co... | [
{
"created": "Thu, 28 Jul 2005 13:05:49 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Sep 2005 14:21:27 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Papantonopoulos",
"Eleftherios",
"",
"Athens, Tech. U."
],
[
"Papazoglou",
"Antonios",
"",
"ITP, Lausanne"
]
] | We study the cosmological evolution of isotropic matter on an infinitely thin conical codimension-two brane-world. Our analysis is based on the boundary dynamics of a six-dimensional model in the presence of an induced gravity term on the brane and a Gauss-Bonnet term in the bulk. With the assumption that the bulk cont... | 8.002647 | 8.390761 | 7.847675 | 7.70514 | 8.281897 | 7.952043 | 7.932078 | 7.656737 | 7.71431 | 8.853793 | 7.967121 | 7.853559 | 7.961133 | 7.878436 | 8.061025 | 7.847215 | 7.788276 | 8.119705 | 7.777363 | 7.828924 | 7.894651 |
2205.02535 | Qingjun Jin | Qingjun Jin and Yi Li | Five-loop anomalous dimensions of $\phi^Q$ operators in a scalar theory
with $O(N)$ symmetry | 17 pages, 9 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We compute the complete $Q$-dependence of anomalous dimensions of traceless
symmetric tensor operator $\phi^Q$ in $O(N)$ scalar theory to five-loop. The
renormalization factors are extracted from $\phi^Q\rightarrow Q\phi$ form
factors, and the integrand of form factors are constructed with the help of
unitarity cut m... | [
{
"created": "Thu, 5 May 2022 09:45:31 GMT",
"version": "v1"
},
{
"created": "Mon, 16 May 2022 02:55:47 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Aug 2022 08:29:53 GMT",
"version": "v3"
}
] | 2022-08-30 | [
[
"Jin",
"Qingjun",
""
],
[
"Li",
"Yi",
""
]
] | We compute the complete $Q$-dependence of anomalous dimensions of traceless symmetric tensor operator $\phi^Q$ in $O(N)$ scalar theory to five-loop. The renormalization factors are extracted from $\phi^Q\rightarrow Q\phi$ form factors, and the integrand of form factors are constructed with the help of unitarity cut met... | 9.312762 | 9.907528 | 13.665597 | 10.952201 | 11.502358 | 12.150265 | 11.341686 | 11.623519 | 10.533095 | 13.779275 | 9.588347 | 9.038171 | 9.987486 | 8.801521 | 9.278293 | 8.874419 | 9.542682 | 9.246178 | 9.031661 | 10.213321 | 8.939298 |
1812.07946 | Sander Mooij | Sander Mooij, Mikhail Shaposhnikov and Thibault Voumard | Hidden and explicit quantum scale invariance | Minor changes, updated references, matches published version | Phys. Rev. D 99, 085013 (2019) | 10.1103/PhysRevD.99.085013 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There exist renormalisation schemes that explicitly preserve the scale
invariance of a theory at the quantum level. Imposing a scale invariant
renormalisation breaks renormalisability and induces new non-trivial operators
in the theory. In this work, we study the effects of such scale invariant
renormalisation proced... | [
{
"created": "Wed, 19 Dec 2018 13:56:53 GMT",
"version": "v1"
},
{
"created": "Fri, 3 May 2019 08:59:11 GMT",
"version": "v2"
}
] | 2019-05-08 | [
[
"Mooij",
"Sander",
""
],
[
"Shaposhnikov",
"Mikhail",
""
],
[
"Voumard",
"Thibault",
""
]
] | There exist renormalisation schemes that explicitly preserve the scale invariance of a theory at the quantum level. Imposing a scale invariant renormalisation breaks renormalisability and induces new non-trivial operators in the theory. In this work, we study the effects of such scale invariant renormalisation procedur... | 7.259855 | 7.717248 | 7.165645 | 7.064706 | 7.315919 | 6.942104 | 7.460163 | 7.022668 | 7.262357 | 7.486592 | 7.149049 | 7.280735 | 7.084929 | 6.915647 | 6.979379 | 6.837046 | 6.689699 | 7.055086 | 6.854107 | 7.169589 | 7.004598 |
2312.13210 | Marco Scalisi | Dieter Lust, Joaquin Masias, Benjamin Muntz, Marco Scalisi | Starobinsky Inflation in the Swampland | 38 pages, 2 figures, 2 appendices; v2: minor corrections, refs and
note added | null | null | LMU-ASC 38/23, MPP-2023-281 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that the Starobinsky model of inflation, realised via an $R^2$ term
in the Lagrangian, can originate from quantum effects due to a tower of light
species. By means of two separate arguments, we show how this implies that the
scale of the $R^2$ term must be of order of the species scale $\Lambda_s$,
namely th... | [
{
"created": "Wed, 20 Dec 2023 17:27:11 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Feb 2024 14:00:27 GMT",
"version": "v2"
}
] | 2024-02-19 | [
[
"Lust",
"Dieter",
""
],
[
"Masias",
"Joaquin",
""
],
[
"Muntz",
"Benjamin",
""
],
[
"Scalisi",
"Marco",
""
]
] | We argue that the Starobinsky model of inflation, realised via an $R^2$ term in the Lagrangian, can originate from quantum effects due to a tower of light species. By means of two separate arguments, we show how this implies that the scale of the $R^2$ term must be of order of the species scale $\Lambda_s$, namely the ... | 8.939358 | 7.839096 | 8.555927 | 7.706091 | 7.877692 | 7.595314 | 7.656244 | 7.88715 | 7.218265 | 8.837824 | 7.580043 | 8.162823 | 8.87867 | 8.234947 | 8.08565 | 8.30548 | 8.238831 | 8.005712 | 8.492844 | 8.353822 | 8.125046 |
0811.0814 | Neil Barnaby | Neil Barnaby | Nonlocal Inflation | 6 pages, no figures. Conference proceedings for Theory Canada 4.
Accepted for publication in the Canadian Journal of Physics | Can.J.Phys.87:189-194,2009 | 10.1139/P08-089 | null | hep-th astro-ph gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the possibility of realizing inflation in nonlocal field theories
containing infinitely many derivatives. Such constructions arise naturally in
string field theory and also in a number of toy models, such as the p-adic
string. After reviewing the complications (ghosts and instabilities) that arise
when wo... | [
{
"created": "Wed, 5 Nov 2008 21:00:02 GMT",
"version": "v1"
}
] | 2010-11-02 | [
[
"Barnaby",
"Neil",
""
]
] | We consider the possibility of realizing inflation in nonlocal field theories containing infinitely many derivatives. Such constructions arise naturally in string field theory and also in a number of toy models, such as the p-adic string. After reviewing the complications (ghosts and instabilities) that arise when work... | 9.359249 | 8.393905 | 9.932834 | 8.96314 | 9.274151 | 8.795614 | 9.054014 | 9.433042 | 8.623563 | 10.641243 | 9.021916 | 9.024666 | 9.310027 | 9.062654 | 9.107596 | 9.549006 | 9.230311 | 9.403265 | 9.029605 | 9.585976 | 8.889025 |
1911.09193 | Nicol\'as Grandi | Laura Cruciani, Nicolas Grandi | Holographic metals at finite doping | 12 pages, 5 figures | null | null | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the electron star solution to the model that was recently
proposed by Kiritsis and Li in order to describe a holographic superconductor
at finite doping. We do so by finding a map between the doped model and the
standard undoped one. In this way, we are able to describe the holographic
metallic phase at ... | [
{
"created": "Wed, 20 Nov 2019 22:09:50 GMT",
"version": "v1"
}
] | 2019-11-22 | [
[
"Cruciani",
"Laura",
""
],
[
"Grandi",
"Nicolas",
""
]
] | We construct the electron star solution to the model that was recently proposed by Kiritsis and Li in order to describe a holographic superconductor at finite doping. We do so by finding a map between the doped model and the standard undoped one. In this way, we are able to describe the holographic metallic phase at fi... | 9.699312 | 7.334239 | 9.146914 | 7.947288 | 7.879358 | 7.444614 | 7.429587 | 7.248541 | 7.518662 | 9.300808 | 7.630336 | 8.33532 | 9.872023 | 8.998381 | 8.548626 | 8.549162 | 8.136974 | 8.333966 | 8.50457 | 9.752622 | 7.974208 |
2102.07190 | Harold Blas | H. Blas, M. Cerna Magui\~na and L.F. dos Santos | Modified non-linear Schr\"odinger models, ${\cal C}{\cal P}_s{\cal T}_d$
symmetry, dark solitons and infinite towers of anomalous charges | 12pages, 10 figures. NODYCON2021 conference | null | null | null | hep-th math-ph math.MP nlin.SI | http://creativecommons.org/licenses/by-nc-nd/4.0/ | Some modified (defocusing) non-linear Schr\"odinger models (MNLS) possess
infinite towers of anomalous conservation laws with asymptotically conserved
charges. The so-called anomalies of the quasi-conservation laws vanish upon
space-time integration for a special ${\cal C}{\cal P}_s{\cal T}_d$ symmetric
field configu... | [
{
"created": "Sun, 14 Feb 2021 16:26:12 GMT",
"version": "v1"
}
] | 2021-02-16 | [
[
"Blas",
"H.",
""
],
[
"Maguiña",
"M. Cerna",
""
],
[
"Santos",
"L. F. dos",
""
]
] | Some modified (defocusing) non-linear Schr\"odinger models (MNLS) possess infinite towers of anomalous conservation laws with asymptotically conserved charges. The so-called anomalies of the quasi-conservation laws vanish upon space-time integration for a special ${\cal C}{\cal P}_s{\cal T}_d$ symmetric field configura... | 13.749486 | 13.8588 | 15.97911 | 13.330564 | 13.247273 | 14.528877 | 13.614011 | 12.989274 | 13.302299 | 18.253902 | 13.214848 | 12.835012 | 14.030154 | 13.069082 | 12.708928 | 12.9923 | 12.646668 | 12.749411 | 12.83735 | 14.440056 | 12.790552 |
0708.0759 | Thomas Konstandin | Andres Hernandez, Thomas Konstandin, Michael G. Schmidt | Effective Action in a General Chiral Model: Next to Leading Order
Derivative Expansion in the Worldline Method | 33 pages, minor changes, published version | Nucl.Phys.B793:425-450,2008 | 10.1016/j.nuclphysb.2007.10.005 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a formalism to determine the imaginary part of a general chiral
model in the derivative expansion. Our formalism is based on the worldline path
integral for the covariant current that can be given in an explicit chiral and
gauge covariant form. The effective action is then obtained by integrating the
covar... | [
{
"created": "Mon, 6 Aug 2007 13:12:15 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Oct 2008 10:26:56 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Hernandez",
"Andres",
""
],
[
"Konstandin",
"Thomas",
""
],
[
"Schmidt",
"Michael G.",
""
]
] | We present a formalism to determine the imaginary part of a general chiral model in the derivative expansion. Our formalism is based on the worldline path integral for the covariant current that can be given in an explicit chiral and gauge covariant form. The effective action is then obtained by integrating the covaria... | 11.82975 | 11.769123 | 12.485873 | 10.958414 | 10.630713 | 11.277092 | 11.244847 | 11.006777 | 10.598154 | 12.763927 | 10.810289 | 11.757341 | 10.941422 | 10.768689 | 10.705867 | 10.474819 | 10.925282 | 11.240346 | 11.04135 | 11.447656 | 11.022376 |
1910.12869 | Andrea Manenti | Andrea Manenti | Differential operators for superconformal correlation functions | Fixed typos in Table 2 and Figure 2 | J. High Energ. Phys. 2020, 145 (2020) | 10.1007/JHEP04(2020)145 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a systematic method to expand in components four dimensional
superconformal multiplets. The results cover all possible $\mathcal{N} = 1$
multiplets and some cases of interest for $\mathcal{N} = 2$. As an application
of the formalism we prove that certain $\mathcal{N} = 2$ spinning chiral
operators (also kn... | [
{
"created": "Mon, 28 Oct 2019 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Nov 2019 18:11:57 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Apr 2020 14:34:27 GMT",
"version": "v3"
},
{
"created": "Fri, 31 Jul 2020 17:45:14 GMT",
"version": "v4"
}
] | 2020-08-03 | [
[
"Manenti",
"Andrea",
""
]
] | We present a systematic method to expand in components four dimensional superconformal multiplets. The results cover all possible $\mathcal{N} = 1$ multiplets and some cases of interest for $\mathcal{N} = 2$. As an application of the formalism we prove that certain $\mathcal{N} = 2$ spinning chiral operators (also know... | 7.166461 | 7.214098 | 7.872731 | 7.043169 | 7.507119 | 6.774519 | 7.136009 | 6.892629 | 6.93016 | 8.126801 | 6.859095 | 6.834409 | 7.555583 | 7.07091 | 6.924654 | 6.977441 | 7.128706 | 7.033826 | 7.097641 | 7.377229 | 6.96564 |
2102.06190 | Julius Grimminger | Antoine Bourget, Julius F. Grimminger, Amihay Hanany, Marcus Sperling
and Zhenghao Zhong | Branes, Quivers, and the Affine Grassmannian | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Brane systems provide a large class of gauge theories that arise in string
theory. This paper demonstrates how such brane systems fit with a somewhat
exotic geometric object, called the affine Grassmannian. This gives a strong
motivation to study physical aspects of the affine Grassmannian. Explicit
quivers are prese... | [
{
"created": "Thu, 11 Feb 2021 18:53:37 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Apr 2021 16:25:54 GMT",
"version": "v2"
}
] | 2021-04-07 | [
[
"Bourget",
"Antoine",
""
],
[
"Grimminger",
"Julius F.",
""
],
[
"Hanany",
"Amihay",
""
],
[
"Sperling",
"Marcus",
""
],
[
"Zhong",
"Zhenghao",
""
]
] | Brane systems provide a large class of gauge theories that arise in string theory. This paper demonstrates how such brane systems fit with a somewhat exotic geometric object, called the affine Grassmannian. This gives a strong motivation to study physical aspects of the affine Grassmannian. Explicit quivers are present... | 20.661039 | 16.753254 | 21.699301 | 17.647099 | 18.088667 | 18.12229 | 18.894337 | 17.083773 | 17.531902 | 24.058035 | 17.722782 | 17.734306 | 19.112907 | 17.542732 | 17.692764 | 16.922277 | 17.693487 | 17.11661 | 17.390186 | 19.141207 | 17.54517 |
1307.6158 | Bojan Nikoli\'c | Ljubica Davidovic, Bojan Nikolic, Branislav Sazdovic | Canonical approach to the closed string noncommutativity | We add the Sec. 4. where we compared our results with previous ones.
We also improved Abstract, Introduction and Conclusion as described above. In
addition, we corrected all typos and grammatical errors we noticed | Eur. Phys. J. C Vol. 74, Issue 1, 2014 | 10.1140/epjc/s10052-014-2734-5 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the closed string moving in the weakly curved background and its
totally T-dualized background. Using T-duality transformation laws, we find the
structure of the Poisson brackets in the T-dual space corresponding to the
fundamental Poisson brackets in the original theory. From this structure we
obtain tha... | [
{
"created": "Tue, 23 Jul 2013 17:06:02 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Nov 2013 19:02:17 GMT",
"version": "v2"
}
] | 2014-02-04 | [
[
"Davidovic",
"Ljubica",
""
],
[
"Nikolic",
"Bojan",
""
],
[
"Sazdovic",
"Branislav",
""
]
] | We consider the closed string moving in the weakly curved background and its totally T-dualized background. Using T-duality transformation laws, we find the structure of the Poisson brackets in the T-dual space corresponding to the fundamental Poisson brackets in the original theory. From this structure we obtain that ... | 11.157161 | 11.85872 | 13.41731 | 10.75491 | 12.792467 | 12.673439 | 12.024688 | 11.707539 | 11.178446 | 13.8564 | 11.2484 | 10.994204 | 11.553092 | 10.805079 | 10.39726 | 11.13123 | 11.063245 | 10.756187 | 10.599929 | 11.284776 | 10.8119 |
hep-th/0005193 | Yuri Shtanov | Yu. V. Shtanov (Bogolyubov Institute, Kiev) | On Brane-World Cosmology | 10 pages, revtex, an important note added: all the results presented
in this paper were previously obtained in hep-ph/0003173, of which the author
was not aware | null | null | null | hep-th gr-qc hep-ph | null | In the study of three-brane cosmological models, an unusual law of
cosmological expansion on the brane has been reported. According to this law,
the energy density of matter on the brane quadratically enters the right-hand
side of the new equations for the brane world, in contrast with the standard
cosmology, where i... | [
{
"created": "Mon, 22 May 2000 22:19:54 GMT",
"version": "v1"
},
{
"created": "Tue, 23 May 2000 20:41:45 GMT",
"version": "v2"
},
{
"created": "Wed, 24 May 2000 20:33:45 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Shtanov",
"Yu. V.",
"",
"Bogolyubov Institute, Kiev"
]
] | In the study of three-brane cosmological models, an unusual law of cosmological expansion on the brane has been reported. According to this law, the energy density of matter on the brane quadratically enters the right-hand side of the new equations for the brane world, in contrast with the standard cosmology, where it ... | 7.350181 | 7.430181 | 7.095006 | 7.019487 | 6.662478 | 7.227643 | 6.828696 | 6.6983 | 7.049848 | 7.439806 | 6.797091 | 7.149105 | 6.992179 | 6.905429 | 6.995805 | 6.976013 | 6.872668 | 6.781442 | 6.944686 | 6.882333 | 6.846443 |
hep-th/9609201 | Mikhail Volkov | Mikhail S.Volkov | Negative modes around Einstein-Yang-Mills sphalerons and black holes | 19 pp, LaTeX, epsf, 2 postscript figures, Published in "Geometry and
Integrable Models", Eds. P.N. Pyatov \& S.N.Solodukhin, World Scientific
1996, pp. 55-77 | null | null | null | hep-th | null | The dynamics of small perturbations around sphaleron and black hole solutions
in the Einstein-Yang-Mills theory for the gauge group $SU(2)$ is investigated.
The perturbations can be split into the two independent sectors in accordance
with their parity; each sector contains negative modes. The even-parity
negative mo... | [
{
"created": "Wed, 25 Sep 1996 14:39:03 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Volkov",
"Mikhail S.",
""
]
] | The dynamics of small perturbations around sphaleron and black hole solutions in the Einstein-Yang-Mills theory for the gauge group $SU(2)$ is investigated. The perturbations can be split into the two independent sectors in accordance with their parity; each sector contains negative modes. The even-parity negative mode... | 8.315463 | 7.013114 | 7.199285 | 6.961189 | 7.328839 | 6.805545 | 7.894973 | 6.966447 | 7.069157 | 7.878783 | 7.405901 | 7.14525 | 7.189213 | 7.345273 | 7.246763 | 7.361667 | 7.409527 | 7.629421 | 7.28774 | 7.368766 | 7.294348 |
hep-th/0001192 | Shin'ichi Nojiri | Shin'ichi Nojiri, Sergei D. Odintsov and Sergio Zerbini | Quantum (in)stability of dilatonic AdS backgrounds and holographic
renormalization group with gravity | LaTeX file, 19 pages, misprints corrected | Phys.Rev.D62:064006,2000 | 10.1103/PhysRevD.62.064006 | NDA-FP-71 | hep-th | null | Stability of dilatonic AdS spaces due to quantum effects of dilaton coupled
conformal matter is considered. When such spaces do not exist on classical
level, their dynamical generation occurs. Explicit examples corresponding to
quantum creation of d4 dilatonic AdS Universe and of d2 dilatonic AdS Black
Hole (BH) are ... | [
{
"created": "Fri, 28 Jan 2000 02:30:36 GMT",
"version": "v1"
},
{
"created": "Sun, 30 Jan 2000 11:59:20 GMT",
"version": "v2"
},
{
"created": "Mon, 28 Feb 2000 09:20:11 GMT",
"version": "v3"
}
] | 2009-09-17 | [
[
"Nojiri",
"Shin'ichi",
""
],
[
"Odintsov",
"Sergei D.",
""
],
[
"Zerbini",
"Sergio",
""
]
] | Stability of dilatonic AdS spaces due to quantum effects of dilaton coupled conformal matter is considered. When such spaces do not exist on classical level, their dynamical generation occurs. Explicit examples corresponding to quantum creation of d4 dilatonic AdS Universe and of d2 dilatonic AdS Black Hole (BH) are pr... | 17.966005 | 16.690138 | 18.502262 | 15.88351 | 17.72657 | 15.12976 | 17.050793 | 14.980873 | 15.973445 | 20.229918 | 16.347334 | 15.0782 | 16.7994 | 15.740008 | 16.648058 | 15.681351 | 15.215967 | 16.378855 | 16.145815 | 16.718039 | 16.100147 |
hep-th/9810036 | P. Menotti | P. Menotti (Department of Physics, University of Pisa, Italy) | Regge-Liouville action from group theory | 4 pages LaTeX, to appear in the proceedings of ``Path Integrals from
peV to TeV'', Florence-Italy, August 25-29, 1998 | null | null | IFUP-TH 48/98 | hep-th gr-qc hep-lat | null | We work out the constraints imposed by SL(2C) invariance for sphere topology
and modular invariance for torus topology, on the discretized form of Liouville
action in Polyakov's non local covariant form. These are sufficient to
completely fix the discretized action except for the overall normalization
constant and a ... | [
{
"created": "Tue, 6 Oct 1998 08:31:57 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Menotti",
"P.",
"",
"Department of Physics, University of Pisa, Italy"
]
] | We work out the constraints imposed by SL(2C) invariance for sphere topology and modular invariance for torus topology, on the discretized form of Liouville action in Polyakov's non local covariant form. These are sufficient to completely fix the discretized action except for the overall normalization constant and a te... | 13.843305 | 12.313659 | 11.820198 | 10.4067 | 11.429947 | 11.691462 | 10.969385 | 11.472074 | 10.928339 | 13.107518 | 10.991758 | 10.636806 | 11.483841 | 10.255387 | 10.958615 | 10.791517 | 11.244187 | 10.402946 | 10.640221 | 11.447606 | 11.091562 |
1106.3494 | Agostino Patella | Agostino Patella | GMOR-like relation in IR-conformal gauge theories | 28 pages, 1 PDF figure | Phys.Rev. D84 (2011) 125033 | 10.1103/PhysRevD.84.125033 | CERN-PH-TH/2011-144 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A generalization of the GMOR relation to the case of infrared-conformal gauge
theories is discussed. The starting point is the chiral Ward identity
connecting the isovector pseudoscalar susceptibility to the chiral condensate,
in a mass-deformed theory. A renormalization-group analysis shows that the
pseudoscalar sus... | [
{
"created": "Fri, 17 Jun 2011 14:21:26 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Mar 2012 19:03:21 GMT",
"version": "v2"
}
] | 2012-03-29 | [
[
"Patella",
"Agostino",
""
]
] | A generalization of the GMOR relation to the case of infrared-conformal gauge theories is discussed. The starting point is the chiral Ward identity connecting the isovector pseudoscalar susceptibility to the chiral condensate, in a mass-deformed theory. A renormalization-group analysis shows that the pseudoscalar susce... | 7.2972 | 7.354933 | 6.88159 | 6.64814 | 7.239251 | 8.417822 | 7.81515 | 7.574634 | 6.469843 | 7.085149 | 7.942444 | 6.439672 | 6.328561 | 6.352157 | 6.353682 | 6.519301 | 6.427578 | 6.219669 | 6.238842 | 6.248538 | 6.79755 |
hep-th/0511115 | Roman Buniy | Roman V. Buniy, Arjun Berera and Thomas W. Kephart | Asymmetric inflation: exact solutions | 42 pages, 24 figures, 3 tables | Phys.Rev. D73 (2006) 063529 | 10.1103/PhysRevD.73.063529 | null | hep-th astro-ph gr-qc hep-ph | null | We provide exact solutions to the Einstein equations when the Universe
contains vacuum energy plus a uniform arrangements of magnetic fields, strings,
or domain walls. Such a universe has planar symmetry, i. e., it is homogeneous
but, not isotropic. Further exact solutions are obtained when dust is included
and appro... | [
{
"created": "Wed, 9 Nov 2005 21:05:13 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Buniy",
"Roman V.",
""
],
[
"Berera",
"Arjun",
""
],
[
"Kephart",
"Thomas W.",
""
]
] | We provide exact solutions to the Einstein equations when the Universe contains vacuum energy plus a uniform arrangements of magnetic fields, strings, or domain walls. Such a universe has planar symmetry, i. e., it is homogeneous but, not isotropic. Further exact solutions are obtained when dust is included and approxi... | 17.634947 | 19.730202 | 16.226072 | 17.210279 | 19.13595 | 17.848808 | 19.182581 | 15.94882 | 18.080862 | 18.503025 | 17.760012 | 18.716619 | 16.613304 | 16.183798 | 16.984962 | 17.106438 | 17.704281 | 17.10236 | 17.189161 | 16.887064 | 16.685549 |
1802.10441 | Ricardo Schiappa | In\^es Aniceto, G\"ok\c{c}e Ba\c{s}ar, Ricardo Schiappa | A Primer on Resurgent Transseries and Their Asymptotics | 192 pages, 76 plots in 41 figures, jheppub-nosort.sty; v2: small
changes, corrections & typos, added refs | null | 10.1016/j.physrep.2019.02.003 | NSF-ITP-17-153 | hep-th hep-lat hep-ph math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The computation of observables in general interacting theories, be them
quantum mechanical, field, gauge or string theories, is a non-trivial problem
which in many cases can only be addressed by resorting to perturbative methods.
In most physically interesting problems these perturbative expansions result in
asymptot... | [
{
"created": "Wed, 28 Feb 2018 14:47:51 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Jan 2019 10:14:40 GMT",
"version": "v2"
}
] | 2021-01-13 | [
[
"Aniceto",
"Inês",
""
],
[
"Başar",
"Gökçe",
""
],
[
"Schiappa",
"Ricardo",
""
]
] | The computation of observables in general interacting theories, be them quantum mechanical, field, gauge or string theories, is a non-trivial problem which in many cases can only be addressed by resorting to perturbative methods. In most physically interesting problems these perturbative expansions result in asymptotic... | 9.139093 | 9.298577 | 10.210443 | 9.331952 | 10.38183 | 10.25795 | 9.85242 | 9.660398 | 9.202441 | 10.761628 | 9.333877 | 8.92423 | 9.055506 | 9.097588 | 9.275928 | 8.901597 | 9.39785 | 9.096557 | 8.982202 | 9.660406 | 9.15536 |
hep-th/0302168 | David Dudal | D. Dudal, H. Verschelde, V. E. R. Lemes, M. S. Sarandy, S. P. Sorella,
M. Picariello | Gluon-ghost condensate of mass dimension 2 in the Curci-Ferrari gauge | 17 pages | Annals Phys. 308 (2003) 62-77 | 10.1016/S0003-4916(03)00131-3 | null | hep-th | null | The effective potential for an on-shell BRST invariant gluon-ghost condensate
of mass dimension 2 in the Curci-Ferrari gauge in SU(N) Yang-Mills is analysed
by combining the local composite operator technique with the algebraic
renormalization. We pay attention to the gauge parameter independence of the
vacuum energy... | [
{
"created": "Thu, 20 Feb 2003 14:00:56 GMT",
"version": "v1"
}
] | 2007-06-22 | [
[
"Dudal",
"D.",
""
],
[
"Verschelde",
"H.",
""
],
[
"Lemes",
"V. E. R.",
""
],
[
"Sarandy",
"M. S.",
""
],
[
"Sorella",
"S. P.",
""
],
[
"Picariello",
"M.",
""
]
] | The effective potential for an on-shell BRST invariant gluon-ghost condensate of mass dimension 2 in the Curci-Ferrari gauge in SU(N) Yang-Mills is analysed by combining the local composite operator technique with the algebraic renormalization. We pay attention to the gauge parameter independence of the vacuum energy o... | 9.868445 | 6.805438 | 10.65155 | 7.93619 | 7.665652 | 7.819847 | 8.116985 | 7.787941 | 7.643697 | 11.66486 | 8.431931 | 8.91326 | 9.328613 | 9.413729 | 8.907225 | 9.02562 | 9.149533 | 9.054912 | 9.312403 | 9.3816 | 9.233397 |
1412.5281 | Hiroshi Kunitomo | Hiroshi Kunitomo | Symmetries and Feynman Rules for Ramond Sector in Open Superstring Field
Theory | 30 pages, 13 figures; v2 a small explanation is added; v3 minor
corrections | null | 10.1093/ptep/ptv027 | YITP-14-106 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the symmetries of the action suppelemented by the constraint in
the WZW-type open superstring field theory. It is found that this pseudo-action
has additional symmetries provided we impose the constraint after the
transformation. Respecting these additional symmetries, we propose a
prescription for the new... | [
{
"created": "Wed, 17 Dec 2014 08:19:44 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Feb 2015 03:01:04 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Feb 2015 09:42:57 GMT",
"version": "v3"
}
] | 2016-06-21 | [
[
"Kunitomo",
"Hiroshi",
""
]
] | We examine the symmetries of the action suppelemented by the constraint in the WZW-type open superstring field theory. It is found that this pseudo-action has additional symmetries provided we impose the constraint after the transformation. Respecting these additional symmetries, we propose a prescription for the new F... | 11.648974 | 9.674251 | 11.448818 | 9.269283 | 10.725731 | 10.178998 | 9.825331 | 10.223885 | 10.044081 | 12.018681 | 10.488579 | 10.469563 | 11.146191 | 10.218784 | 10.465322 | 10.223562 | 10.85812 | 10.219736 | 10.269698 | 11.128083 | 10.661918 |
2010.02061 | Konstantinos Koutrolikos | I. L. Buchbinder, S. James Gates Jr., K. Koutrolikos | Hierarchy of Supersymmetric Higher Spin Connections | null | Phys. Rev. D 102, 125018 (2020) | 10.1103/PhysRevD.102.125018 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We focus on the geometrical reformulation of free higher spin supermultiplets
in $4\rm{D},~\mathcal{N}=1$ flat superspace. We find that there is a de
Wit-Freedman like hierarchy of superconnections with simple gauge
transformations. The requirement for sensible free equations of motion imposes
constraints on the gaug... | [
{
"created": "Mon, 5 Oct 2020 14:50:55 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Nov 2020 17:33:31 GMT",
"version": "v2"
}
] | 2021-01-04 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Gates",
"S. James",
"Jr."
],
[
"Koutrolikos",
"K.",
""
]
] | We focus on the geometrical reformulation of free higher spin supermultiplets in $4\rm{D},~\mathcal{N}=1$ flat superspace. We find that there is a de Wit-Freedman like hierarchy of superconnections with simple gauge transformations. The requirement for sensible free equations of motion imposes constraints on the gauge ... | 14.03412 | 12.649536 | 15.357993 | 12.289843 | 13.894365 | 12.387465 | 14.073762 | 12.876048 | 11.829003 | 17.964241 | 11.808539 | 13.227082 | 13.110024 | 13.084992 | 13.192742 | 12.732168 | 12.893937 | 12.977062 | 12.977755 | 13.626516 | 12.764083 |
1107.3023 | Yu-Xiao Liu | Shao-Wen Wei, Yu-Xiao Liu | Equatorial and quasi-equatorial gravitational lensing by Kerr black hole
pierced by a cosmic string | 29 pages, 9 figures | Phys. Rev. D85 (2012) 064044 | 10.1103/PhysRevD.85.064044 | USTC-ICTS-11-09 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper, we study numerically the equatorial lensing and
quasiequatorial lensing by Kerr black hole pierced by a cosmic string in the
strong deflection limit. We calculate the strong deflection limit coefficients
and the deflection angle, which are found to depend closely on the cosmic
string parameter $... | [
{
"created": "Fri, 15 Jul 2011 09:40:46 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Feb 2012 16:04:55 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Apr 2012 01:54:39 GMT",
"version": "v3"
}
] | 2012-04-06 | [
[
"Wei",
"Shao-Wen",
""
],
[
"Liu",
"Yu-Xiao",
""
]
] | In the present paper, we study numerically the equatorial lensing and quasiequatorial lensing by Kerr black hole pierced by a cosmic string in the strong deflection limit. We calculate the strong deflection limit coefficients and the deflection angle, which are found to depend closely on the cosmic string parameter $\b... | 6.144831 | 7.227664 | 5.493187 | 5.579811 | 6.210398 | 6.014891 | 7.5404 | 5.867561 | 6.604963 | 6.111105 | 6.646267 | 6.194741 | 5.726063 | 5.858509 | 5.77655 | 5.829726 | 6.283014 | 5.856588 | 6.155271 | 5.83812 | 6.14025 |
1202.1227 | Giampiero Esposito Dr. | Giampiero Esposito, Guglielmo Fucci, Alexander Yu. Kamenshchik, Klaus
Kirsten | Spectral methods in quantum field theory and quantum cosmology | 40 pages, Latex, submitted to the Stuart Dowker special issue of J.
Phys. A | null | 10.1088/1751-8113/45/37/374004 | DSF preprint 2012/2 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the application of the spectral zeta-function to the 1- loop
properties of quantum field theories on manifolds with boundary, with emphasis
on Euclidean quantum gravity and quantum cosmology. As was shown in the
literature some time ago, the only boundary conditions that are completely
invariant under infin... | [
{
"created": "Mon, 6 Feb 2012 18:01:04 GMT",
"version": "v1"
}
] | 2015-06-04 | [
[
"Esposito",
"Giampiero",
""
],
[
"Fucci",
"Guglielmo",
""
],
[
"Kamenshchik",
"Alexander Yu.",
""
],
[
"Kirsten",
"Klaus",
""
]
] | We review the application of the spectral zeta-function to the 1- loop properties of quantum field theories on manifolds with boundary, with emphasis on Euclidean quantum gravity and quantum cosmology. As was shown in the literature some time ago, the only boundary conditions that are completely invariant under infinit... | 12.899376 | 10.523655 | 11.623296 | 10.249819 | 10.642192 | 11.019909 | 12.210337 | 9.999423 | 10.398954 | 13.4988 | 10.563169 | 11.546654 | 12.045316 | 11.605968 | 11.70097 | 11.258792 | 11.395543 | 11.59396 | 11.409876 | 11.864842 | 11.435568 |
hep-th/0002245 | Glenn Barnich | Glenn Barnich, Friedemann Brandt and Marc Henneaux | Local BRST cohomology in gauge theories | 150 pages Latex file, minimal corrections, final version | Phys.Rept.338:439-569,2000 | 10.1016/S0370-1573(00)00049-1 | ITP-UH-03/00, ULB-TH-00/05 | hep-th hep-ph | null | The general solution of the anomaly consistency condition (Wess-Zumino
equation) has been found recently for Yang-Mills gauge theory. The general form
of the counterterms arising in the renormalization of gauge invariant operators
(Kluberg-Stern and Zuber conjecture) and in gauge theories of the Yang-Mills
type with ... | [
{
"created": "Tue, 29 Feb 2000 01:46:50 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Mar 2000 15:04:13 GMT",
"version": "v2"
},
{
"created": "Mon, 13 Nov 2000 18:56:02 GMT",
"version": "v3"
}
] | 2010-11-15 | [
[
"Barnich",
"Glenn",
""
],
[
"Brandt",
"Friedemann",
""
],
[
"Henneaux",
"Marc",
""
]
] | The general solution of the anomaly consistency condition (Wess-Zumino equation) has been found recently for Yang-Mills gauge theory. The general form of the counterterms arising in the renormalization of gauge invariant operators (Kluberg-Stern and Zuber conjecture) and in gauge theories of the Yang-Mills type with no... | 9.006796 | 10.366139 | 10.461897 | 10.025654 | 10.42392 | 9.971271 | 10.515759 | 10.143219 | 9.623819 | 12.564285 | 9.345171 | 9.436254 | 9.555635 | 9.183233 | 9.292455 | 9.074172 | 9.009728 | 9.24966 | 9.220287 | 9.566041 | 9.259176 |
2002.12084 | Ugo Moschella | Henri Epstein and Ugo Moschella | QFT and topology in two dimensions: $SL(2,{\Bbb R})$-symmetry and the de
Sitter universe | 43 pages, 1 figure | null | 10.1007/s00023-021-01030-7 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study bosonic Quantum Field Theory on the double covering
$\widetilde{dS}_{2}$ of the 2-dimensional de Sitter universe, identified to a
coset space of the group $SL(2,{\Bbb R})$. The latter acts effectively on
$\widetilde{dS}_{2}$ and can be interpreted as it relativity group. The
manifold is locally identical to ... | [
{
"created": "Thu, 27 Feb 2020 13:32:19 GMT",
"version": "v1"
}
] | 2021-09-01 | [
[
"Epstein",
"Henri",
""
],
[
"Moschella",
"Ugo",
""
]
] | We study bosonic Quantum Field Theory on the double covering $\widetilde{dS}_{2}$ of the 2-dimensional de Sitter universe, identified to a coset space of the group $SL(2,{\Bbb R})$. The latter acts effectively on $\widetilde{dS}_{2}$ and can be interpreted as it relativity group. The manifold is locally identical to th... | 9.017239 | 9.416672 | 9.356971 | 9.713713 | 10.460417 | 9.240779 | 9.324549 | 9.796436 | 9.321139 | 10.554538 | 9.357835 | 8.882314 | 9.26123 | 9.068715 | 9.023704 | 8.8225 | 9.082848 | 9.002582 | 8.984507 | 9.347376 | 9.017368 |
0707.3755 | Klaus Kirsten | Klaus Kirsten and Paul Loya | Computation of determinants using contour integrals | 15 pages, to appear in American Journal of Physics | Am.J.Phys.76:60-64,2008 | 10.1119/1.2794348 | null | hep-th | null | It is shown how the pre-exponential factor of the Feynman propagator for a
large class of potentials can be computed using contour integrals. This is of
direct relevance in the context of tunnelling processes in quantum theories.
The prerequisites for this analysis are accessible to advanced undergraduate
students an... | [
{
"created": "Wed, 25 Jul 2007 14:34:18 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kirsten",
"Klaus",
""
],
[
"Loya",
"Paul",
""
]
] | It is shown how the pre-exponential factor of the Feynman propagator for a large class of potentials can be computed using contour integrals. This is of direct relevance in the context of tunnelling processes in quantum theories. The prerequisites for this analysis are accessible to advanced undergraduate students and ... | 11.499846 | 11.629379 | 9.641754 | 10.035834 | 10.723512 | 11.829747 | 10.232527 | 11.271068 | 11.272219 | 10.09916 | 11.049232 | 11.087779 | 10.492375 | 10.509491 | 11.030115 | 11.493768 | 10.975797 | 10.73724 | 10.352669 | 10.350639 | 10.63876 |
hep-th/9702109 | David Kastor | Fay Dowker, David Kastor and Jennie Traschen | U-Duality, D-Branes and Black Hole Emission Rates: Agreements and
Disagreements | 30 pages, harvmac; Clarification is added on the size of disagreement
claimed; Remarks are added on treating the limit in which two charges are
small | Phys. Rev. D 58, 124025 (1998) | 10.1103/PhysRevD.58.124025 | UMHEP-437, Imperial/TP/96-97/24 | hep-th | null | An expression for the spacetime absorption coefficient of a scalar field in a
five dimensional, near extremal black hole background is derived, which has the
same form as that presented by Maldacena and Strominger, but is valid over a
larger, U-duality invariant region of parameter space and in general disagrees
with... | [
{
"created": "Thu, 13 Feb 1997 21:42:16 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Mar 1997 02:53:26 GMT",
"version": "v2"
}
] | 2016-08-25 | [
[
"Dowker",
"Fay",
""
],
[
"Kastor",
"David",
""
],
[
"Traschen",
"Jennie",
""
]
] | An expression for the spacetime absorption coefficient of a scalar field in a five dimensional, near extremal black hole background is derived, which has the same form as that presented by Maldacena and Strominger, but is valid over a larger, U-duality invariant region of parameter space and in general disagrees with t... | 8.997701 | 8.623055 | 9.79398 | 8.848309 | 9.221601 | 9.216114 | 8.748958 | 9.179936 | 8.665207 | 9.703824 | 8.558637 | 8.264693 | 8.762445 | 8.448194 | 8.740169 | 8.622913 | 8.664542 | 8.262721 | 8.686665 | 9.248919 | 8.66155 |
1903.05476 | Jie Jiang | Jie Jiang, Xiao-Wei Li | Modified "complexity equals action" conjecture | arXiv admin note: text overlap with arXiv:1811.07347 | Phys. Rev. D 100, 066026 (2019) | 10.1103/PhysRevD.100.066026 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we first use the "complexity equals action" conjecture to
discuss the complexity growth rate in both perturbation Einsteinian cubic
gravity and non-perturbation Einstein-Weyl gravity. We find that the CA
complexity rate in these cases is divergent. To avoid this divergence, we
modify the original conje... | [
{
"created": "Tue, 12 Mar 2019 17:01:46 GMT",
"version": "v1"
}
] | 2019-10-02 | [
[
"Jiang",
"Jie",
""
],
[
"Li",
"Xiao-Wei",
""
]
] | In this paper, we first use the "complexity equals action" conjecture to discuss the complexity growth rate in both perturbation Einsteinian cubic gravity and non-perturbation Einstein-Weyl gravity. We find that the CA complexity rate in these cases is divergent. To avoid this divergence, we modify the original conject... | 16.183069 | 10.270475 | 13.928504 | 11.312509 | 12.419808 | 10.345392 | 10.733805 | 10.459354 | 10.700437 | 15.645011 | 11.153631 | 11.734518 | 12.247519 | 11.315272 | 11.344316 | 11.572414 | 11.667987 | 11.715499 | 11.854113 | 12.934577 | 11.481174 |
hep-th/9505046 | Keith Dienes | Keith R. Dienes and Alon E. Faraggi (IAS, Princeton) | Gauge Coupling Unification in Realistic Free-Fermionic String Models | 81 pages, standard LaTeX, 7 figures (Encapsulated PostScript),
expanded published version | Nucl.Phys. B457 (1995) 409-483 | 10.1016/0550-3213(95)00497-1 | IASSNS-HEP-94/113 (May 1995) | hep-th hep-ph | null | We discuss the unification of gauge couplings within the framework of a wide
class of realistic free-fermionic string models which have appeared in the
literature, including the flipped SU(5), SO(6)xSO(4), and various
SU(3)xSU(2)xU(1) models. If the matter spectrum below the string scale is that
of the Minimal Supers... | [
{
"created": "Tue, 9 May 1995 06:12:36 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Dec 1995 19:43:53 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Dienes",
"Keith R.",
"",
"IAS, Princeton"
],
[
"Faraggi",
"Alon E.",
"",
"IAS, Princeton"
]
] | We discuss the unification of gauge couplings within the framework of a wide class of realistic free-fermionic string models which have appeared in the literature, including the flipped SU(5), SO(6)xSO(4), and various SU(3)xSU(2)xU(1) models. If the matter spectrum below the string scale is that of the Minimal Supersym... | 5.787828 | 6.164424 | 5.926792 | 5.888816 | 6.063678 | 6.34585 | 6.279794 | 6.08716 | 5.709276 | 6.304062 | 6.026455 | 5.868481 | 5.761435 | 5.732821 | 5.715757 | 5.862181 | 5.783345 | 5.780786 | 5.648619 | 5.87119 | 5.901673 |
1011.1324 | Jeong-Hyuck Park | Imtak Jeon, Kanghoon Lee and Jeong-Hyuck Park | Differential geometry with a projection: Application to double field
theory | 1+22 pages, No figure; a previous result on 4-index tensor removed,
presentation improved | JHEP 1104:014,2011 | 10.1007/JHEP04(2011)014 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In recent development of double field theory, as for the description of the
massless sector of closed strings, the spacetime dimension is formally doubled,
i.e. from D to D+D, and the T-duality is realized manifestly as a global O(D,D)
rotation. In this paper, we conceive a differential geometry characterized by a
O(... | [
{
"created": "Fri, 5 Nov 2010 05:57:52 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Feb 2011 00:39:47 GMT",
"version": "v2"
}
] | 2011-04-08 | [
[
"Jeon",
"Imtak",
""
],
[
"Lee",
"Kanghoon",
""
],
[
"Park",
"Jeong-Hyuck",
""
]
] | In recent development of double field theory, as for the description of the massless sector of closed strings, the spacetime dimension is formally doubled, i.e. from D to D+D, and the T-duality is realized manifestly as a global O(D,D) rotation. In this paper, we conceive a differential geometry characterized by a O(D,... | 10.553716 | 9.463705 | 11.480074 | 9.401666 | 9.738502 | 9.950275 | 10.225393 | 9.478473 | 9.820607 | 11.980475 | 9.774002 | 9.164516 | 10.272505 | 9.537002 | 9.544452 | 9.46509 | 9.600915 | 9.177788 | 9.913404 | 10.426043 | 9.572165 |
0807.4578 | Archil Kobakhidze | Archil Kobakhidze | Domain walls and gauge field localization in strongly-coupled pure
Yang-Mills theories | 9 pages, 3 figures, v2: minor corrections, references added; to be
published in IJTP | Int.J.Theor.Phys.50:1335-1341,2011 | 10.1007/s10773-010-0640-7 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a mechanism of gauge field localization on a domain wall within
the framework of strongly coupled pure Yang-Mills theory.
| [
{
"created": "Tue, 29 Jul 2008 05:49:25 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Dec 2010 06:11:49 GMT",
"version": "v2"
}
] | 2011-04-04 | [
[
"Kobakhidze",
"Archil",
""
]
] | We present a mechanism of gauge field localization on a domain wall within the framework of strongly coupled pure Yang-Mills theory. | 15.665144 | 8.613852 | 10.762026 | 10.925098 | 9.708225 | 9.974436 | 9.469505 | 10.377309 | 9.420116 | 10.428697 | 9.467424 | 11.547314 | 12.107697 | 11.236295 | 11.473967 | 11.523533 | 10.536097 | 11.798876 | 11.205112 | 12.035487 | 10.449788 |
2001.01832 | Masud Chaichian | M. Chaichian, M. N. Mnatsakanova, Yu. S. Vernov | Towards an Axiomatic Formulation of Noncommutative Quantum Field Theory.
II | 20 pages. arXiv admin note: substantial text overlap with
arXiv:hep-th/0612112, arXiv:hep-th/0611097 | Nucl. Phys. B 950, 114846 (2020) | 10.1016/j.nuclphysb.2019.114846 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Classical results of the axiomatic quantum field theory, namely the
irreducibility of the set of field operators, Reeh and Schlieder's theorems and
generalized Haag's theorem, are proven in $SO(1,1)$ invariant quantum field
theory, of which an important example is noncommutative quantum field theory.
New consequences... | [
{
"created": "Sat, 14 Dec 2019 13:45:35 GMT",
"version": "v1"
}
] | 2020-01-08 | [
[
"Chaichian",
"M.",
""
],
[
"Mnatsakanova",
"M. N.",
""
],
[
"Vernov",
"Yu. S.",
""
]
] | Classical results of the axiomatic quantum field theory, namely the irreducibility of the set of field operators, Reeh and Schlieder's theorems and generalized Haag's theorem, are proven in $SO(1,1)$ invariant quantum field theory, of which an important example is noncommutative quantum field theory. New consequences o... | 7.676902 | 7.736701 | 7.035025 | 7.335506 | 8.135924 | 7.313364 | 8.232221 | 7.408299 | 7.823806 | 8.003364 | 7.248439 | 7.186282 | 7.707912 | 7.243041 | 7.444235 | 7.162039 | 7.260582 | 6.977948 | 7.27446 | 7.543796 | 7.200566 |
hep-th/9612241 | Carlos Castro | Carlos Castro | On the Integrability Aspects of the Self Dual Membrane | 46 pages, tex file. Extended updated version of hep-th/9605029 and
hep-th/9612160 | null | null | null | hep-th | null | The exact quantum integrability aspects of a sector of the membrane is
investigated. It is found that spherical membranes moving in flat target
spacetime backgrounds admit a class of integrable solutions linked to SU(infty)
SDYM equations (dimensionally reduced to one temporal dimension). After a
suitable ansatz, the... | [
{
"created": "Fri, 27 Dec 1996 06:12:32 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Castro",
"Carlos",
""
]
] | The exact quantum integrability aspects of a sector of the membrane is investigated. It is found that spherical membranes moving in flat target spacetime backgrounds admit a class of integrable solutions linked to SU(infty) SDYM equations (dimensionally reduced to one temporal dimension). After a suitable ansatz, the S... | 18.335657 | 16.4077 | 18.862371 | 16.4056 | 18.904945 | 17.439283 | 18.062883 | 19.019003 | 16.423832 | 20.588116 | 17.018833 | 17.461563 | 18.919033 | 17.542021 | 17.447687 | 17.316814 | 17.346777 | 16.987768 | 17.073259 | 18.469599 | 17.365696 |
hep-th/9202064 | null | F. A. Schaposnik | Anomalies and Deconfinement | 23 pages | null | null | null | hep-th | null | I discuss how instanton effects can be wiped-out due to the existence of
anomalies. I first consider Compact Quantum Electrodynamics in 3 dimensions
where confinement of electric charge is destroyed when fermions are added so
that a Chern-Simons term is generated as a one-loop effect. I also show that a
similar pheno... | [
{
"created": "Wed, 19 Feb 1992 09:12:57 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Schaposnik",
"F. A.",
""
]
] | I discuss how instanton effects can be wiped-out due to the existence of anomalies. I first consider Compact Quantum Electrodynamics in 3 dimensions where confinement of electric charge is destroyed when fermions are added so that a Chern-Simons term is generated as a one-loop effect. I also show that a similar phenome... | 12.253042 | 9.973797 | 10.918336 | 10.661622 | 9.660783 | 11.424126 | 11.586384 | 10.77752 | 10.961678 | 11.647704 | 10.43634 | 10.214974 | 11.75055 | 10.732631 | 10.516418 | 9.988924 | 10.206001 | 10.443629 | 10.879699 | 12.101348 | 10.490575 |
2311.02751 | Wei Li | Dmitry Galakhov and Wei Li | Charging solid partitions | 33 pages, 7 figures; v2: references updated, typos fixed, JHEP
version | null | 10.1007/JHEP01(2024)043 | null | hep-th math-ph math.CO math.MP math.QA math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Solid partitions are the 4D generalization of the plane partitions in 3D and
Young diagrams in 2D, and they can be visualized as stacking of 4D unit-size
boxes in the positive corner of a 4D room. Physically, solid partitions arise
naturally as 4D molten crystals that count equivariant D-brane BPS states on
the simpl... | [
{
"created": "Sun, 5 Nov 2023 20:12:40 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Apr 2024 21:39:55 GMT",
"version": "v2"
}
] | 2024-04-11 | [
[
"Galakhov",
"Dmitry",
""
],
[
"Li",
"Wei",
""
]
] | Solid partitions are the 4D generalization of the plane partitions in 3D and Young diagrams in 2D, and they can be visualized as stacking of 4D unit-size boxes in the positive corner of a 4D room. Physically, solid partitions arise naturally as 4D molten crystals that count equivariant D-brane BPS states on the simples... | 7.2899 | 7.170209 | 7.375282 | 6.363579 | 7.216223 | 6.520245 | 7.321378 | 6.483282 | 6.260163 | 7.60765 | 6.658662 | 6.725367 | 6.793221 | 6.578121 | 6.802395 | 6.423597 | 6.507877 | 6.592959 | 6.485069 | 6.860136 | 6.664124 |
1208.1494 | Aristomenis Donos | Aristomenis Donos and Jerome P. Gauntlett | Supersymmetric quantum criticality supported by baryonic charges | 30 pages, 4 figures, very minor changes, version published in JHEP | null | 10.1007/JHEP10(2012)120 | Imperial/TP/2012/JG/04 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of the $AdS_4\times Q^{111}$ solution of D=11 supergravity we
construct supersymmetric zero temperature black brane solutions that
interpolate between $AdS_4$ in the UV and $AdS_2\times \mathbb{R}^2$ in the IR.
The dual N=2 SCFT has a $U(1)^2$ baryonic symmetry and the solutions carry
electric charge w... | [
{
"created": "Tue, 7 Aug 2012 19:18:43 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Oct 2012 10:00:58 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Donos",
"Aristomenis",
""
],
[
"Gauntlett",
"Jerome P.",
""
]
] | In the context of the $AdS_4\times Q^{111}$ solution of D=11 supergravity we construct supersymmetric zero temperature black brane solutions that interpolate between $AdS_4$ in the UV and $AdS_2\times \mathbb{R}^2$ in the IR. The dual N=2 SCFT has a $U(1)^2$ baryonic symmetry and the solutions carry electric charge wit... | 5.327479 | 4.472691 | 5.520835 | 4.563595 | 4.628386 | 4.724089 | 4.503476 | 4.44464 | 4.454779 | 6.146395 | 4.415596 | 4.612953 | 5.283896 | 4.670743 | 4.772433 | 4.675797 | 4.760981 | 4.811758 | 4.905529 | 5.331637 | 4.740845 |
0806.4862 | Reza Moazzemi | Reza Moazzemi, Abdollah Mohammadi, Siamak S. Gousheh | A Renormalized perturbation theory for problems with nontrivial boundary
conditions or backgrounds in two space-time dimensions | 7 pages, 2 figures, revtex4, submmited to Eur. Phys. J. C | Eur.Phys.J.C56:585-590,2008 | 10.1140/epjc/s10052-008-0680-9 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we discuss the effects of nontrivial boundary conditions or
backgrounds, including non-perturbative ones, on the renormalization program
for systems in two dimensions. Here we present an alternative renormalization
procedure such that these non-perturbative conditions can be taken into account
in a self... | [
{
"created": "Mon, 30 Jun 2008 11:38:35 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Jul 2008 12:20:41 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Moazzemi",
"Reza",
""
],
[
"Mohammadi",
"Abdollah",
""
],
[
"Gousheh",
"Siamak S.",
""
]
] | In this paper we discuss the effects of nontrivial boundary conditions or backgrounds, including non-perturbative ones, on the renormalization program for systems in two dimensions. Here we present an alternative renormalization procedure such that these non-perturbative conditions can be taken into account in a self-c... | 8.619896 | 8.708578 | 8.313621 | 8.036832 | 8.038457 | 8.382379 | 8.46644 | 8.024809 | 7.901946 | 8.778621 | 8.188437 | 8.174825 | 8.056984 | 8.121662 | 8.227696 | 8.256101 | 8.153102 | 8.089806 | 8.116447 | 8.413116 | 8.062041 |
2006.08644 | Tanay Kibe | Tanay Kibe, Ayan Mukhopadhyay, Alexander Soloviev and Hareram Swain | $SL(2,R)$ lattices as information processors | 23 pages, 13 figures; conclusions expanded with summary, more
comments and references added | Phys. Rev. D 102, 086008 (2020) | 10.1103/PhysRevD.102.086008 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Black holes past their Page times should act as efficient scramblers and
information mirrors. The information of the infalling bits are rapidly encoded
by the old black hole in the Hawking quanta, but it should take time that is
exponential in the Page time entropy to decode the interior. Motivated by the
features of... | [
{
"created": "Mon, 15 Jun 2020 18:00:11 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Sep 2020 05:53:57 GMT",
"version": "v2"
}
] | 2020-10-14 | [
[
"Kibe",
"Tanay",
""
],
[
"Mukhopadhyay",
"Ayan",
""
],
[
"Soloviev",
"Alexander",
""
],
[
"Swain",
"Hareram",
""
]
] | Black holes past their Page times should act as efficient scramblers and information mirrors. The information of the infalling bits are rapidly encoded by the old black hole in the Hawking quanta, but it should take time that is exponential in the Page time entropy to decode the interior. Motivated by the features of f... | 17.867615 | 18.031292 | 18.606607 | 15.749937 | 17.657383 | 17.434328 | 16.562378 | 16.319971 | 16.043303 | 19.025757 | 16.23875 | 16.468311 | 17.289404 | 16.229412 | 16.164923 | 17.063868 | 15.883066 | 16.21422 | 16.005411 | 16.627316 | 15.844867 |
hep-th/0502055 | Mizuno Shuntaro | Makoto Tanabe and Shuntaro Mizuno | BPS pp-wave brane cosmological solutions in string theory | 10 pages | JHEP0505:016,2005 | 10.1088/1126-6708/2005/05/016 | WU-AP/213/05 | hep-th astro-ph gr-qc hep-ph | null | We construct time dependent BPS pp-wave brane solutions in the context of
M-theory and type II supergravity. It is found that N-brane solutions we
considered satisfy the crossing rule as S-brane solutions but 1/8 supersymmetry
remains. By applying them to the cosmological setting, inflationary solutions
are obtained.... | [
{
"created": "Fri, 4 Feb 2005 13:52:56 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Tanabe",
"Makoto",
""
],
[
"Mizuno",
"Shuntaro",
""
]
] | We construct time dependent BPS pp-wave brane solutions in the context of M-theory and type II supergravity. It is found that N-brane solutions we considered satisfy the crossing rule as S-brane solutions but 1/8 supersymmetry remains. By applying them to the cosmological setting, inflationary solutions are obtained. D... | 16.866804 | 14.469081 | 15.850322 | 14.144365 | 15.992609 | 15.018201 | 15.150254 | 14.27141 | 14.408844 | 19.81897 | 13.953476 | 15.146275 | 16.048107 | 15.830367 | 15.312682 | 15.351981 | 15.633374 | 15.305455 | 15.23492 | 16.178957 | 14.646756 |
1301.7194 | Samrat Bhowmick | Souvik Banerjee, Samrat Bhowmick, Sudipta Mukherji | Anisotropic branes | 13 pages, 4 figures | null | 10.1016/j.physletb.2013.08.041 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a class of anisotropic brane configurations which shows BKL
oscillations near their cosmological singularities. Near horizon limits of
these solutions represent Kasner space embedded in AdS background. Dynamical
probe branes in these geometries inherit anisotropies from the background.
Amusingly, for a pro... | [
{
"created": "Wed, 30 Jan 2013 10:55:36 GMT",
"version": "v1"
}
] | 2015-06-12 | [
[
"Banerjee",
"Souvik",
""
],
[
"Bhowmick",
"Samrat",
""
],
[
"Mukherji",
"Sudipta",
""
]
] | We present a class of anisotropic brane configurations which shows BKL oscillations near their cosmological singularities. Near horizon limits of these solutions represent Kasner space embedded in AdS background. Dynamical probe branes in these geometries inherit anisotropies from the background. Amusingly, for a probe... | 14.135175 | 12.670925 | 14.335125 | 10.947408 | 12.353838 | 10.925588 | 12.129052 | 12.398113 | 10.641971 | 14.453765 | 12.955471 | 12.197841 | 14.186724 | 12.531978 | 12.749972 | 12.632644 | 12.437256 | 13.103436 | 11.879506 | 14.102718 | 11.882329 |
hep-th/9411087 | Klaus | K. Bresser | All bicovariant differential calculi on Glq(3,C) and SLq(3,C) | 24 pages, LaTeX | J.Phys. A28 (1995) 2545-2562 | 10.1088/0305-4470/28/9/015 | GOET-TP 87/94 | hep-th math.QA q-alg | null | All bicovariant first order differential calculi on the quantum group
GLq(3,C) are determined. There are two distinct one-parameter families of
calculi. In terms of a suitable basis of 1-forms the commutation relations can
be expressed with the help of the R-matrix of GLq(3,C). Some calculi induce
bicovariant differe... | [
{
"created": "Sat, 12 Nov 1994 19:09:32 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Bresser",
"K.",
""
]
] | All bicovariant first order differential calculi on the quantum group GLq(3,C) are determined. There are two distinct one-parameter families of calculi. In terms of a suitable basis of 1-forms the commutation relations can be expressed with the help of the R-matrix of GLq(3,C). Some calculi induce bicovariant different... | 5.14139 | 5.332918 | 5.725593 | 5.298913 | 5.197629 | 5.296097 | 5.19324 | 5.189662 | 5.152706 | 6.818337 | 4.968097 | 5.182314 | 5.187684 | 4.974704 | 5.068322 | 4.896427 | 5.070831 | 5.130908 | 4.854844 | 5.07899 | 4.961237 |
1812.09257 | Davide Gaiotto | Kevin Costello and Davide Gaiotto | Twisted Holography | Updated reference | null | null | null | hep-th math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive and test a novel holographic duality in the B-model topological
string theory. The duality relates the B-model on certain Calabi-Yau
three-folds to two-dimensional chiral algebras defined as gauged
$\beta\gamma\,$ systems. The duality conjecturally captures a topological
sector of more familiar $\mathrm{AdS... | [
{
"created": "Fri, 21 Dec 2018 16:53:19 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Dec 2018 22:10:17 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Feb 2019 17:09:05 GMT",
"version": "v3"
},
{
"created": "Fri, 8 Jan 2021 14:53:26 GMT",
"version": "v4"
}
] | 2021-01-11 | [
[
"Costello",
"Kevin",
""
],
[
"Gaiotto",
"Davide",
""
]
] | We derive and test a novel holographic duality in the B-model topological string theory. The duality relates the B-model on certain Calabi-Yau three-folds to two-dimensional chiral algebras defined as gauged $\beta\gamma\,$ systems. The duality conjecturally captures a topological sector of more familiar $\mathrm{AdS}_... | 8.103968 | 7.149449 | 9.103734 | 6.648571 | 7.620137 | 7.443851 | 7.428 | 7.273255 | 7.00809 | 8.696478 | 7.540779 | 7.087106 | 8.092912 | 7.003482 | 7.524967 | 6.980814 | 7.263053 | 7.291514 | 7.323421 | 7.747168 | 7.408637 |
hep-th/0607076 | Valentina Giangreco M. Puletti Mrs | Valentina Giangreco M. Puletti | Operator Product Expansion for Pure Spinor Superstring on AdS(5)*S(5) | 18 pages, no figure, corrected typos and added acknowledgements | JHEP0610:057,2006 | 10.1088/1126-6708/2006/10/057 | UUITP-11/06 | hep-th | null | The tree-level operator product expansion coefficients of the matter currents
are calculated in the pure spinor formalism for type IIB superstring in the
AdS(5)*S(5) background.
| [
{
"created": "Wed, 12 Jul 2006 10:48:14 GMT",
"version": "v1"
},
{
"created": "Sun, 16 Jul 2006 07:47:26 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Puletti",
"Valentina Giangreco M.",
""
]
] | The tree-level operator product expansion coefficients of the matter currents are calculated in the pure spinor formalism for type IIB superstring in the AdS(5)*S(5) background. | 9.715828 | 5.308938 | 8.768727 | 5.719845 | 5.349867 | 5.764001 | 6.028214 | 5.755411 | 5.53342 | 8.076522 | 5.624761 | 6.192467 | 9.074689 | 7.067208 | 6.133968 | 6.517101 | 6.308993 | 6.307 | 6.627143 | 7.935379 | 6.501965 |
2101.03642 | Mario Neves Junior | M. J. Neves, Jorge B. de Oliveira, L. P. R. Ospedal, J. A.
Helay\"el-Neto | Dispersion Relations in Non-Linear Electrodynamics and the Kinematics of
the Compton Effect in a Magnetic Background | 13 pages, 9 figures, accepted version in Physical Review D | Phys. Rev. D 104, 015006 (2021) | 10.1103/PhysRevD.104.015006 | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Non-linear electrodynamic models are re-assessed in this paper to pursue an
investigation of the kinematics of the Compton effect in a magnetic background.
Before considering specific models, we start off by presenting a general
non-linear Lagrangian built up in terms of the most general Lorentz- and
gauge-invariant ... | [
{
"created": "Sun, 10 Jan 2021 23:57:32 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Jan 2021 16:17:31 GMT",
"version": "v2"
},
{
"created": "Mon, 7 Jun 2021 20:48:52 GMT",
"version": "v3"
}
] | 2021-07-14 | [
[
"Neves",
"M. J.",
""
],
[
"de Oliveira",
"Jorge B.",
""
],
[
"Ospedal",
"L. P. R.",
""
],
[
"Helayël-Neto",
"J. A.",
""
]
] | Non-linear electrodynamic models are re-assessed in this paper to pursue an investigation of the kinematics of the Compton effect in a magnetic background. Before considering specific models, we start off by presenting a general non-linear Lagrangian built up in terms of the most general Lorentz- and gauge-invariant co... | 11.067717 | 10.602819 | 10.617375 | 10.086787 | 11.28278 | 10.706745 | 11.02848 | 9.877487 | 10.380956 | 11.332293 | 10.387094 | 10.466271 | 10.35893 | 10.269256 | 10.295288 | 10.4706 | 10.504628 | 10.381495 | 10.375554 | 10.586056 | 10.299314 |
1207.6666 | Zvi Bern | Z. Bern, J. J. M. Carrasco, H. Johansson and R. Roiban | The Five-Loop Four-Point Amplitude of N=4 super-Yang-Mills Theory | 5 pages, 4 figures, RevTex. Ancillary file included. v2 minor
corrections, corrected references and overall phase in eq. (5), matching
journal version | Phys. Rev. Lett. 109, 241602 (2012) | 10.1103/PhysRevLett.109.241602 | UCLA/12/TEP/105; SU-ITP-12/22; Saclay--IPhT--T12/056 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the method of maximal cuts, we construct the complete D-dimensional
integrand of the five-loop four-point amplitude of N = 4 super-Yang-Mills
theory, including nonplanar contributions. In the critical dimension where this
amplitude becomes ultraviolet divergent, we present a compact explicit
expression for the ... | [
{
"created": "Fri, 27 Jul 2012 23:19:01 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Dec 2012 08:14:28 GMT",
"version": "v2"
}
] | 2015-03-20 | [
[
"Bern",
"Z.",
""
],
[
"Carrasco",
"J. J. M.",
""
],
[
"Johansson",
"H.",
""
],
[
"Roiban",
"R.",
""
]
] | Using the method of maximal cuts, we construct the complete D-dimensional integrand of the five-loop four-point amplitude of N = 4 super-Yang-Mills theory, including nonplanar contributions. In the critical dimension where this amplitude becomes ultraviolet divergent, we present a compact explicit expression for the no... | 9.300528 | 7.074081 | 9.227228 | 7.61218 | 8.344305 | 8.041378 | 7.251042 | 7.636692 | 7.224575 | 9.704662 | 7.424284 | 7.851714 | 8.301517 | 7.716411 | 7.583308 | 7.833842 | 7.73226 | 7.455493 | 7.213189 | 8.379288 | 7.501547 |
2203.16532 | Yuho Sakatani | Yuho Sakatani, Shozo Uehara | Gauged sigma models and exceptional dressing cosets | 36 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Poisson-Lie (PL) T-duality is a generalized T-duality based on the Lie
algebra of the Drinfel'd double. In particular, when we consider the PL
T-duality of a coset space, the dual space is found to be a generalized coset
space, which is called the dressing coset. In this paper, we investigate an
extension of the ... | [
{
"created": "Wed, 30 Mar 2022 17:59:57 GMT",
"version": "v1"
}
] | 2022-03-31 | [
[
"Sakatani",
"Yuho",
""
],
[
"Uehara",
"Shozo",
""
]
] | The Poisson-Lie (PL) T-duality is a generalized T-duality based on the Lie algebra of the Drinfel'd double. In particular, when we consider the PL T-duality of a coset space, the dual space is found to be a generalized coset space, which is called the dressing coset. In this paper, we investigate an extension of the dr... | 6.510578 | 6.277903 | 7.306078 | 5.928279 | 6.35712 | 6.484121 | 6.153856 | 6.760914 | 6.016286 | 7.969267 | 6.220254 | 6.311733 | 6.625898 | 6.04328 | 6.378475 | 6.197107 | 6.327532 | 6.360428 | 6.127059 | 6.665817 | 6.227561 |
1702.03938 | Congkao Wen | Ferdinando Gliozzi, Andrea L. Guerrieri, Anastasios C. Petkou, Congkao
Wen | The analytic structure of conformal blocks and the generalized
Wilson-Fisher fixed points | 38 pages, no figures; v2: 40 pages, typos corrected, references
added; v3: matches published JHEP version, one reference added | JHEP 1704 (2017) 056 | 10.1007/JHEP04(2017)056 | CALT-TH-2017-009 | hep-th cond-mat.stat-mech hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe in detail the method used in our previous work arXiv:1611.10344
to study the Wilson-Fisher critical points nearby generalized free CFTs,
exploiting the analytic structure of conformal blocks as functions of the
conformal dimension of the exchanged operator. Our method is equivalent to the
mechanism of con... | [
{
"created": "Mon, 13 Feb 2017 19:00:07 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Feb 2017 17:36:30 GMT",
"version": "v2"
},
{
"created": "Tue, 2 May 2017 04:47:02 GMT",
"version": "v3"
}
] | 2017-05-24 | [
[
"Gliozzi",
"Ferdinando",
""
],
[
"Guerrieri",
"Andrea L.",
""
],
[
"Petkou",
"Anastasios C.",
""
],
[
"Wen",
"Congkao",
""
]
] | We describe in detail the method used in our previous work arXiv:1611.10344 to study the Wilson-Fisher critical points nearby generalized free CFTs, exploiting the analytic structure of conformal blocks as functions of the conformal dimension of the exchanged operator. Our method is equivalent to the mechanism of confo... | 8.138605 | 8.736393 | 9.937788 | 8.431572 | 8.071218 | 8.520312 | 7.993024 | 8.463969 | 8.32009 | 11.13995 | 8.211362 | 7.697958 | 8.645584 | 8.057505 | 7.862741 | 7.794042 | 7.984347 | 7.804702 | 7.893322 | 8.503485 | 7.920631 |
1105.0244 | Ben Freivogel | Ben Freivogel | Making predictions in the multiverse | 20 pages, 3 figures; invited review for Classical and Quantum
Gravity; v2: references improved | null | 10.1088/0264-9381/28/20/204007 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I describe reasons to think we are living in an eternally inflating
multiverse where the observable "constants" of nature vary from place to place.
The major obstacle to making predictions in this context is that we must
regulate the infinities of eternal inflation. I review a number of proposed
regulators, or measur... | [
{
"created": "Mon, 2 May 2011 05:32:22 GMT",
"version": "v1"
},
{
"created": "Sun, 18 Sep 2011 06:09:01 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Freivogel",
"Ben",
""
]
] | I describe reasons to think we are living in an eternally inflating multiverse where the observable "constants" of nature vary from place to place. The major obstacle to making predictions in this context is that we must regulate the infinities of eternal inflation. I review a number of proposed regulators, or measures... | 12.03316 | 9.900513 | 10.540697 | 9.196064 | 10.216699 | 9.864512 | 9.360041 | 9.643221 | 10.078506 | 11.372291 | 9.869327 | 9.613628 | 9.93676 | 9.659945 | 9.908174 | 9.791202 | 9.564792 | 9.854971 | 9.710649 | 10.324203 | 9.853928 |
1812.11282 | Inori Ueba | Yukihiro Fujimoto, Kouhei Hasegawa, Kenji Nishiwaki, Makoto Sakamoto,
Kentaro Tatsumi, Inori Ueba | Extended supersymmetry with central charges in higher dimensional Dirac
action | 15 pages | Phys. Rev. D 99, 065002 (2019) | 10.1103/PhysRevD.99.065002 | null | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new realization of extended quantum-mechanical supersymmetry (QM SUSY) with
central extension is investigated. We first show that two different sets of
$d+2$ ($d+1$) supercharges for $d=$ even (odd), each of which satisfies an
$\mathcal{N}=d+2$ ($d+1$) extended QM SUSY algebra without central extension,
are hidden ... | [
{
"created": "Sat, 29 Dec 2018 04:17:49 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Feb 2019 03:12:48 GMT",
"version": "v2"
}
] | 2019-03-27 | [
[
"Fujimoto",
"Yukihiro",
""
],
[
"Hasegawa",
"Kouhei",
""
],
[
"Nishiwaki",
"Kenji",
""
],
[
"Sakamoto",
"Makoto",
""
],
[
"Tatsumi",
"Kentaro",
""
],
[
"Ueba",
"Inori",
""
]
] | A new realization of extended quantum-mechanical supersymmetry (QM SUSY) with central extension is investigated. We first show that two different sets of $d+2$ ($d+1$) supercharges for $d=$ even (odd), each of which satisfies an $\mathcal{N}=d+2$ ($d+1$) extended QM SUSY algebra without central extension, are hidden in... | 5.665627 | 5.626817 | 6.00916 | 5.83752 | 5.594218 | 5.479304 | 5.839771 | 5.655726 | 5.680165 | 6.68288 | 5.626422 | 5.434275 | 5.433192 | 5.35609 | 5.348794 | 5.504116 | 5.455856 | 5.456432 | 5.304447 | 5.558849 | 5.395698 |
hep-th/0408189 | Amir Masoud Ghezelbash | A.M. Ghezelbash, R.B. Mann | Atiyah-Hitchin M-Branes | 18 pages, 5 figures, one paragraph added in the conclusions, typos
corrected | JHEP0410:012,2004 | 10.1088/1126-6708/2004/10/012 | null | hep-th gr-qc | null | We present new M2 and M5 brane solutions in M-theory based on transverse
Atiyah-Hitchin space and other self-dual geometries. One novel feature of these
solutions is that they have bolt-like fixed points yet still preserve 1/4 of
the supersymmetry. All the solutions can be reduced down to ten dimensional
intersecting... | [
{
"created": "Wed, 25 Aug 2004 19:35:16 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Oct 2004 17:54:47 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Ghezelbash",
"A. M.",
""
],
[
"Mann",
"R. B.",
""
]
] | We present new M2 and M5 brane solutions in M-theory based on transverse Atiyah-Hitchin space and other self-dual geometries. One novel feature of these solutions is that they have bolt-like fixed points yet still preserve 1/4 of the supersymmetry. All the solutions can be reduced down to ten dimensional intersecting b... | 10.939144 | 7.389259 | 12.216735 | 8.486192 | 8.411325 | 7.284154 | 8.387619 | 7.812549 | 7.911187 | 13.730732 | 8.588447 | 8.445428 | 10.717731 | 8.346533 | 8.659716 | 8.759341 | 8.491345 | 8.848362 | 8.82051 | 11.168054 | 8.871067 |
hep-th/9412053 | Michael Flohr | Michael Flohr | On a New Universal Class of Phase Transitions and Quantum Hall Effect | 35 pages LaTeX plus 3 HUGE PostScript figures | null | null | null | hep-th cond-mat | null | We study the possible phase transitions between (2+1)-dimensional abelian
Chern-Simons theories. We show that they may be described by non-unitary
rational conformal field theories with c_eff = 1. As an example we choose the
fractional quantum Hall effect and derive all its main features from the
discrete fractal str... | [
{
"created": "Tue, 6 Dec 1994 19:49:56 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Dec 1994 13:48:35 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Flohr",
"Michael",
""
]
] | We study the possible phase transitions between (2+1)-dimensional abelian Chern-Simons theories. We show that they may be described by non-unitary rational conformal field theories with c_eff = 1. As an example we choose the fractional quantum Hall effect and derive all its main features from the discrete fractal struc... | 15.062659 | 16.098904 | 16.631292 | 16.594091 | 15.976503 | 16.708101 | 15.36134 | 15.900393 | 15.328275 | 18.475153 | 14.541102 | 15.182125 | 15.303101 | 14.474001 | 15.404133 | 15.044409 | 15.603723 | 15.051459 | 15.030925 | 15.612318 | 14.831751 |
hep-th/0202168 | Jan Louis | Jan Louis and Andrei Micu | Type II Theories Compactified on Calabi-Yau Threefolds in the Presence
of Background Fluxes | 36 pages, Latex, version to appear in Nucl. Phys. B | Nucl.Phys.B635:395-431,2002 | 10.1016/S0550-3213(02)00338-3 | null | hep-th | null | Compactifications of type II theories on Calabi-Yau threefolds including
electric and magnetic background fluxes are discussed. We derive the bosonic
part of the four-dimensional low energy effective action and show that it is a
non-canonical N=2 supergravity which includes a massive two-form. The
symplectic invarian... | [
{
"created": "Mon, 25 Feb 2002 14:08:19 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Mar 2002 18:36:31 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Apr 2002 16:08:07 GMT",
"version": "v3"
}
] | 2010-11-19 | [
[
"Louis",
"Jan",
""
],
[
"Micu",
"Andrei",
""
]
] | Compactifications of type II theories on Calabi-Yau threefolds including electric and magnetic background fluxes are discussed. We derive the bosonic part of the four-dimensional low energy effective action and show that it is a non-canonical N=2 supergravity which includes a massive two-form. The symplectic invariance... | 7.477614 | 6.445656 | 7.668045 | 6.412922 | 6.766501 | 6.894087 | 7.066015 | 6.529237 | 6.873541 | 8.561145 | 6.826952 | 6.672908 | 7.209436 | 6.557747 | 6.457949 | 6.46928 | 6.593952 | 6.725721 | 6.60939 | 7.189231 | 6.76745 |
1909.12348 | Christopher Hull | N. Chaemjumrus and C.M. Hull | The Doubled Geometry of Nilmanifold Reductions | 38 pages | null | 10.1007/JHEP12(2019)157 | Imperial-TP-2019-CH-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A class of special holonomy spaces arise as nilmanifolds fibred over a line
interval and are dual to intersecting brane solutions of string theory. Further
dualities relate these to T-folds, exotic branes, essentially doubled spaces
and spaces with R-flux. We develop the doubled geometry of these spaces, with
the var... | [
{
"created": "Thu, 26 Sep 2019 19:24:01 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Dec 2019 17:37:32 GMT",
"version": "v2"
}
] | 2020-01-29 | [
[
"Chaemjumrus",
"N.",
""
],
[
"Hull",
"C. M.",
""
]
] | A class of special holonomy spaces arise as nilmanifolds fibred over a line interval and are dual to intersecting brane solutions of string theory. Further dualities relate these to T-folds, exotic branes, essentially doubled spaces and spaces with R-flux. We develop the doubled geometry of these spaces, with the vario... | 15.803467 | 12.017428 | 17.417809 | 12.295452 | 12.423027 | 12.501038 | 11.184464 | 11.77611 | 11.392197 | 19.14422 | 12.491533 | 12.156895 | 14.239241 | 12.648912 | 12.456649 | 12.344781 | 12.90647 | 12.566664 | 11.889839 | 13.916604 | 12.100217 |
2310.07624 | Shi Cheng | Shi Cheng | Surgery and Matter for 3d Theories | 34 pages, many figures | null | null | null | hep-th math.GT | http://creativecommons.org/licenses/by/4.0/ | We try to give a geometric construction for 3d $\mathcal{N}=2$ gauge theories
using three-manifolds and Dehn surgeries. We follow the story that wrapping
M5-branes on plumbing three-manifolds leads to 3d theories with mixed
Chern-Simons levels. This construction can be decorated by adding non-compact
Lagrangian subma... | [
{
"created": "Wed, 11 Oct 2023 16:07:30 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Aug 2024 14:21:09 GMT",
"version": "v2"
}
] | 2024-08-09 | [
[
"Cheng",
"Shi",
""
]
] | We try to give a geometric construction for 3d $\mathcal{N}=2$ gauge theories using three-manifolds and Dehn surgeries. We follow the story that wrapping M5-branes on plumbing three-manifolds leads to 3d theories with mixed Chern-Simons levels. This construction can be decorated by adding non-compact Lagrangian submani... | 9.795918 | 9.784452 | 10.651924 | 8.912867 | 10.005454 | 10.217006 | 10.187804 | 9.628458 | 8.897781 | 10.982168 | 8.688447 | 9.234818 | 9.757836 | 8.99875 | 9.303264 | 9.218727 | 9.411622 | 9.04266 | 9.132733 | 9.577974 | 9.017751 |
1405.4935 | Mokhtar Hassaine | Moises Bravo-Gaete and Mokhtar Hassaine | Thermodynamics of a BTZ black hole solution with an Horndeski source | 7 pages | Phys. Rev. D 90, 024008, 2014 | 10.1103/PhysRevD.90.024008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In three dimensions, we consider a particular truncation of the Horndeski
action that reduces to the Einstein-Hilbert Lagrangian with a cosmological
constant $\Lambda$ and a scalar field whose dynamics is governed by its usual
kinetic term together with a nonminimal kinetic coupling. Requiring the radial
component of... | [
{
"created": "Tue, 20 May 2014 02:48:38 GMT",
"version": "v1"
}
] | 2015-06-19 | [
[
"Bravo-Gaete",
"Moises",
""
],
[
"Hassaine",
"Mokhtar",
""
]
] | In three dimensions, we consider a particular truncation of the Horndeski action that reduces to the Einstein-Hilbert Lagrangian with a cosmological constant $\Lambda$ and a scalar field whose dynamics is governed by its usual kinetic term together with a nonminimal kinetic coupling. Requiring the radial component of t... | 6.928833 | 6.708589 | 6.477391 | 6.43143 | 6.525051 | 6.664571 | 6.627752 | 6.324626 | 6.504528 | 6.910137 | 6.532273 | 6.553197 | 6.634153 | 6.461547 | 6.445656 | 6.421831 | 6.492118 | 6.558081 | 6.504904 | 6.438145 | 6.495314 |
hep-th/9311026 | Bern | Z. Bern, L. Dixon, D.A. Kosower | New QCD Results from String Theory | talk presented by Z.B. at Strings 1993, May 24-29, Berkeley CA, 16
pages | null | null | Saclay/SPhT--T93/116, SLAC-PUB-6388, UCLA/93/TEP/40 | hep-th hep-ph | null | We discuss new results in QCD obtained with string-based methods. These
methods were originally derived from superstring theory and are significantly
more efficient than conventional Feynman rules. This technology was a key
ingredient in the first calculation of the one-loop five-gluon amplitude. We
also present a co... | [
{
"created": "Thu, 4 Nov 1993 03:54:32 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bern",
"Z.",
""
],
[
"Dixon",
"L.",
""
],
[
"Kosower",
"D. A.",
""
]
] | We discuss new results in QCD obtained with string-based methods. These methods were originally derived from superstring theory and are significantly more efficient than conventional Feynman rules. This technology was a key ingredient in the first calculation of the one-loop five-gluon amplitude. We also present a conj... | 10.769249 | 10.321071 | 9.658968 | 8.873146 | 10.582248 | 10.280499 | 9.184481 | 10.505951 | 9.399772 | 10.141071 | 10.391693 | 9.646343 | 10.172615 | 9.717616 | 9.899626 | 9.950271 | 9.652307 | 9.844061 | 9.772001 | 9.949196 | 9.720436 |
hep-th/9509110 | Ninoslav Bralic | N. Bralic, C.D. Fosco, F.A. Schaposnik | On the Quantization of the Abelian Chern-Simons Coefficient at Finite
Temperature | 11 pages, LaTeX, no figures, no special macros. Some discussion and
references added. A minor error corrected. Final version to appear in Phys.
Lett. B | Phys.Lett. B383 (1996) 199-204 | 10.1016/0370-2693(96)00737-X | null | hep-th | null | We show that when the Abelian \CS\ theory coupled to matter fields is
quantized in a vacuum with non vanishing magnetic flux (or electric charge),
the requirement of gauge invariance at finite temperature leads to the
quantization of the \CS\ coefficient and its quantum corrections, in a manner
similar to the non-Abe... | [
{
"created": "Thu, 21 Sep 1995 01:26:25 GMT",
"version": "v1"
},
{
"created": "Mon, 20 May 1996 19:46:22 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Bralic",
"N.",
""
],
[
"Fosco",
"C. D.",
""
],
[
"Schaposnik",
"F. A.",
""
]
] | We show that when the Abelian \CS\ theory coupled to matter fields is quantized in a vacuum with non vanishing magnetic flux (or electric charge), the requirement of gauge invariance at finite temperature leads to the quantization of the \CS\ coefficient and its quantum corrections, in a manner similar to the non-Abeli... | 12.492454 | 10.901442 | 12.939972 | 9.394753 | 9.064524 | 9.797174 | 8.934208 | 10.906849 | 10.081149 | 12.128561 | 9.86527 | 9.566593 | 11.300138 | 9.605332 | 9.849451 | 9.590489 | 9.314727 | 9.578023 | 9.754293 | 10.639379 | 9.511044 |
0704.0784 | Massimo Bianchi | Massimo Bianchi, Francesco Fucito and Jose F. Morales | D-brane Instantons on the T^6/Z_3 orientifold | 31 pages, no figures | JHEP0707:038,2007 | 10.1088/1126-6708/2007/07/038 | null | hep-th | null | We give a detailed microscopic derivation of gauge and stringy instanton
generated superpotentials for gauge theories living on D3-branes at
Z_3-orientifold singularities. Gauge instantons are generated by D(-1)-branes
and lead to Affleck, Dine and Seiberg (ADS) like superpotentials in the
effective N=1 gauge theorie... | [
{
"created": "Thu, 5 Apr 2007 19:33:30 GMT",
"version": "v1"
},
{
"created": "Thu, 31 May 2007 10:19:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bianchi",
"Massimo",
""
],
[
"Fucito",
"Francesco",
""
],
[
"Morales",
"Jose F.",
""
]
] | We give a detailed microscopic derivation of gauge and stringy instanton generated superpotentials for gauge theories living on D3-branes at Z_3-orientifold singularities. Gauge instantons are generated by D(-1)-branes and lead to Affleck, Dine and Seiberg (ADS) like superpotentials in the effective N=1 gauge theories ... | 7.434882 | 7.587143 | 8.796948 | 7.005849 | 8.111191 | 7.995391 | 7.490922 | 7.134656 | 6.842597 | 8.33806 | 7.247571 | 7.176245 | 7.594066 | 7.002137 | 7.180145 | 7.060578 | 7.090189 | 7.181377 | 6.976986 | 7.357867 | 7.137074 |
hep-th/0104175 | S. Mignemi | S. Mignemi | Black holes and conformal mechanics | 5 pages, plain TeX | Mod.Phys.Lett. A16 (2001) 1997-2002 | 10.1142/S0217732301005370 | null | hep-th | null | We show how the motion of a charged particle near the horizon of an extreme
Reissner-Nordstrom black hole can lead to different forms of conformal
mechanics, depending on the choice of the time coordinate.
| [
{
"created": "Fri, 20 Apr 2001 11:13:09 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Mignemi",
"S.",
""
]
] | We show how the motion of a charged particle near the horizon of an extreme Reissner-Nordstrom black hole can lead to different forms of conformal mechanics, depending on the choice of the time coordinate. | 8.232413 | 5.304038 | 7.30135 | 6.001364 | 6.246029 | 5.556663 | 6.000022 | 5.687003 | 5.958662 | 6.082175 | 6.243059 | 6.415242 | 7.28231 | 6.593554 | 6.739347 | 6.574357 | 6.454429 | 6.732329 | 6.456236 | 7.240258 | 6.335585 |
1504.02316 | Edilberto Oliveira Silva | Luis B. Castro and Edilberto O. Silva | Quantum dynamics of a spin-1/2 charged particle in the presence of
magnetic field with scalar and vector couplings | arXiv admin note: text overlap with arXiv:1403.4113 | Eur. Phys. J. C 75 (2015) 7, 321 | 10.1140/epjc/s10052-015-3545-z | null | hep-th | http://creativecommons.org/licenses/publicdomain/ | The quantum dynamics of a spin-1/2 charged particle in the presence of
magnetic field is analyzed for the general case where scalar and vector
couplings are considered. The energy spectra are explicitly computed for
different physical situations, as well as their dependencies on the magnetic
field strength, spin proj... | [
{
"created": "Thu, 9 Apr 2015 14:04:56 GMT",
"version": "v1"
}
] | 2015-07-13 | [
[
"Castro",
"Luis B.",
""
],
[
"Silva",
"Edilberto O.",
""
]
] | The quantum dynamics of a spin-1/2 charged particle in the presence of magnetic field is analyzed for the general case where scalar and vector couplings are considered. The energy spectra are explicitly computed for different physical situations, as well as their dependencies on the magnetic field strength, spin projec... | 10.466863 | 9.461858 | 9.205582 | 8.244907 | 9.421626 | 9.608715 | 9.892095 | 8.792693 | 8.660058 | 9.316187 | 8.75681 | 9.024377 | 9.57903 | 9.387087 | 9.54001 | 9.176978 | 9.473835 | 9.789383 | 9.32859 | 9.819617 | 9.261319 |
1702.04661 | Paul S. Aspinwall | Paul S. Aspinwall, M. Ronen Plesser and Kangkang Wang | Mirror Symmetry and Discriminants | 33 pages | null | null | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the locus, together with multiplicities, of "bad" conformal field
theories in the compactified moduli space of N=(2,2) superconformal field
theories in the context of the generalization of the Batyrev mirror
construction using the gauged linear sigma-model. We find this discriminant of
singular theories is... | [
{
"created": "Wed, 15 Feb 2017 16:01:54 GMT",
"version": "v1"
}
] | 2017-02-16 | [
[
"Aspinwall",
"Paul S.",
""
],
[
"Plesser",
"M. Ronen",
""
],
[
"Wang",
"Kangkang",
""
]
] | We analyze the locus, together with multiplicities, of "bad" conformal field theories in the compactified moduli space of N=(2,2) superconformal field theories in the context of the generalization of the Batyrev mirror construction using the gauged linear sigma-model. We find this discriminant of singular theories is d... | 10.253578 | 10.578794 | 12.634459 | 9.700126 | 10.681433 | 9.645543 | 9.72146 | 10.469704 | 9.991187 | 14.796943 | 9.774317 | 9.863645 | 10.945489 | 9.786674 | 9.606411 | 9.83098 | 10.096411 | 9.924013 | 9.953605 | 10.870079 | 9.491671 |
2402.01847 | Federico Piazza | Francesco Nitti, Federico Piazza and Alexander Taskov | Relativity of the event: examples in JT gravity and linearized GR | 40 pages, 10 Figures. Comments welcome. v2: improved discussion,
references added | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Observables in quantum gravity are famously defined asymptotically, at the
boundary of AdS or Minkowski spaces. However, by gauge fixing a coordinate
system or suitably dressing the field operators, an approximate, "quasi-local"
approach is also possible, that can give account of the measurements performed
by a set o... | [
{
"created": "Fri, 2 Feb 2024 19:03:22 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Apr 2024 08:11:54 GMT",
"version": "v2"
}
] | 2024-05-01 | [
[
"Nitti",
"Francesco",
""
],
[
"Piazza",
"Federico",
""
],
[
"Taskov",
"Alexander",
""
]
] | Observables in quantum gravity are famously defined asymptotically, at the boundary of AdS or Minkowski spaces. However, by gauge fixing a coordinate system or suitably dressing the field operators, an approximate, "quasi-local" approach is also possible, that can give account of the measurements performed by a set of ... | 13.282277 | 12.956067 | 14.190475 | 13.107458 | 13.85536 | 13.227407 | 13.914447 | 12.229053 | 13.133065 | 15.740199 | 12.965511 | 12.917196 | 13.261706 | 12.851171 | 12.746772 | 12.776779 | 12.891426 | 12.984899 | 12.961836 | 13.153684 | 12.971389 |
1712.09549 | Adolfo Guarino | Adolfo Guarino | Hypermultiplet gaugings and supersymmetric solutions from 11D and
massive IIA supergravity on H$^{(p,q)}$ spaces | 10 pages, 3 tables. v2: Published version. v3: minor edits, added
clarifications | null | 10.1140/epjc/s10052-018-5672-9 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Supersymmetric $\,\textrm{AdS}_{4}\,$, $\,\textrm{AdS}_{2} \times
\Sigma_{2}\,$ and asymptotically AdS$_{4}$ black hole solutions are studied in
the context of non-minimal $\,\mathcal{N}=2\,$ supergravity models involving
three vector multiplets (STU-model) and Abelian gaugings of the universal
hypermultiplet moduli ... | [
{
"created": "Wed, 27 Dec 2017 11:21:34 GMT",
"version": "v1"
},
{
"created": "Wed, 9 May 2018 16:05:03 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Aug 2019 15:43:55 GMT",
"version": "v3"
}
] | 2019-08-08 | [
[
"Guarino",
"Adolfo",
""
]
] | Supersymmetric $\,\textrm{AdS}_{4}\,$, $\,\textrm{AdS}_{2} \times \Sigma_{2}\,$ and asymptotically AdS$_{4}$ black hole solutions are studied in the context of non-minimal $\,\mathcal{N}=2\,$ supergravity models involving three vector multiplets (STU-model) and Abelian gaugings of the universal hypermultiplet moduli sp... | 5.71574 | 4.775988 | 6.481454 | 5.153199 | 4.990304 | 5.010654 | 4.891077 | 4.776868 | 5.045547 | 8.059923 | 4.867643 | 5.039999 | 5.632432 | 5.14843 | 5.080779 | 5.12683 | 5.025608 | 5.119125 | 5.144228 | 5.649061 | 4.942204 |
1406.6694 | Shuichi Yokoyama | Shuichi Yokoyama | More on BPS States in N=4 Supersymmetric Yang-Mills Theory on R x S3 | 37 pages, v2: typos corrected, comments and Acknowledgements added | null | 10.1007/JHEP12(2014)163 | TIFR/TH/14-19 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform a systematic analysis on supersymmetric states in N=4
supersymmetric Yang-Mills theory (SYM) on R x S^3. We find a new set of 1/16
BPS equations and determine the precise configuration of the supersymmetric
states by solving all 1/16 BPS equations when they are valued in Cartan
subalgebra of a gauge group ... | [
{
"created": "Wed, 25 Jun 2014 20:00:17 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Sep 2014 19:54:52 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Yokoyama",
"Shuichi",
""
]
] | We perform a systematic analysis on supersymmetric states in N=4 supersymmetric Yang-Mills theory (SYM) on R x S^3. We find a new set of 1/16 BPS equations and determine the precise configuration of the supersymmetric states by solving all 1/16 BPS equations when they are valued in Cartan subalgebra of a gauge group an... | 7.264635 | 7.265106 | 7.118904 | 6.704692 | 6.851315 | 6.786852 | 6.795549 | 7.17964 | 6.487376 | 8.660095 | 6.82018 | 6.714962 | 7.105876 | 6.653867 | 6.807722 | 6.80655 | 6.680743 | 6.564446 | 6.81403 | 7.06205 | 6.857439 |
hep-th/9802111 | Parthasarathi Majumdar | Parthasarathi Majumdar and Soumitra SenGupta | Gaugino mass in the Heterotic string with Scherk-Schwarz
compactification | 4 pages Revtex, no figures | Phys.Lett. B445 (1998) 129-133 | 10.1016/S0370-2693(98)01494-4 | SINP-98/05 | hep-th | null | The generic observable sector gaugino mass in the weakly-coupled heterotic
string compactified to four dimensions by the Scherk-Schwarz scheme (together
with hidden sector gaugino condensation inducing the super-Higgs effect with a
vanishing cosmological constant) is shown to be non-zero at tree level, being
of the o... | [
{
"created": "Mon, 16 Feb 1998 11:52:18 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Majumdar",
"Parthasarathi",
""
],
[
"SenGupta",
"Soumitra",
""
]
] | The generic observable sector gaugino mass in the weakly-coupled heterotic string compactified to four dimensions by the Scherk-Schwarz scheme (together with hidden sector gaugino condensation inducing the super-Higgs effect with a vanishing cosmological constant) is shown to be non-zero at tree level, being of the ord... | 10.588262 | 9.930603 | 10.613478 | 9.473303 | 9.425529 | 9.069263 | 8.407428 | 8.969163 | 8.229597 | 11.716165 | 8.608334 | 9.415363 | 10.032722 | 9.524755 | 9.658494 | 9.200443 | 9.168668 | 9.368704 | 9.369102 | 9.934929 | 9.106483 |
hep-th/0603100 | Dorothea Bahns | K. Pohlmeyer | The Algebra of Observables of the closed Bosonic String in
(1+3)-dimensional Minkowski-Space: updating the structural Analysis | null | Mod.Phys.Lett.A21:1783-1794,2006 | 10.1142/S0217732306021025 | null | hep-th | null | The purpose of the present paper is the communication of some results and
observations which shed new light on the algebraic structure of the algebra of
string observables both in the classical and in the quantum theory.
| [
{
"created": "Mon, 13 Mar 2006 19:05:15 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Pohlmeyer",
"K.",
""
]
] | The purpose of the present paper is the communication of some results and observations which shed new light on the algebraic structure of the algebra of string observables both in the classical and in the quantum theory. | 10.681768 | 9.902217 | 9.254325 | 9.244653 | 8.874627 | 9.476329 | 9.941753 | 9.27767 | 9.313144 | 9.046981 | 9.299265 | 9.436025 | 10.755949 | 9.81927 | 9.921309 | 10.141047 | 9.812144 | 9.771845 | 9.88442 | 10.971524 | 9.218707 |
hep-th/0408075 | David Nolland | David Nolland | Topology, normalisability and the Schr\"odinger equation: Compact QED
(2+1) | 7 pages | null | null | null | hep-th | null | For the special case of compact QED in (2+1) dimensions, we calculate the
non-Gaussian vacuum wave-functional to second order in the monopole fugacity
and obtain the effective photon mass. Our method presents some hope for
understanding the connection between variational and systematic approaches to
understanding the... | [
{
"created": "Tue, 10 Aug 2004 12:29:48 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nolland",
"David",
""
]
] | For the special case of compact QED in (2+1) dimensions, we calculate the non-Gaussian vacuum wave-functional to second order in the monopole fugacity and obtain the effective photon mass. Our method presents some hope for understanding the connection between variational and systematic approaches to understanding the n... | 17.903845 | 16.503738 | 18.734186 | 13.673692 | 15.871468 | 15.270471 | 15.566026 | 14.571268 | 13.289351 | 15.944988 | 13.997806 | 15.053163 | 16.294416 | 14.611964 | 14.393811 | 15.052058 | 14.648541 | 15.399172 | 14.92561 | 15.827777 | 14.552024 |
hep-th/0108193 | Ysmyung | Y. S. Myung (Inje Univ) | A gauge boson from the Kaluza-Klein approach of the Randall-Sundrum
brane world | 7 pages, typo corrected and comments added | null | null | INJE-TP-01-08 | hep-th | null | We clarify a mechanism to obtain a massless gauge boson from the Kaluza-Klein
approach of the Randall-Sundrum(RS) brane world. This corresponds exactly to
the same mechanism of achieving a localization of the gauge boson by adding
both the bulk and brane mass terms. Accordingly this work puts another example
for a lo... | [
{
"created": "Mon, 27 Aug 2001 10:14:14 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Aug 2001 06:15:34 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Myung",
"Y. S.",
"",
"Inje Univ"
]
] | We clarify a mechanism to obtain a massless gauge boson from the Kaluza-Klein approach of the Randall-Sundrum(RS) brane world. This corresponds exactly to the same mechanism of achieving a localization of the gauge boson by adding both the bulk and brane mass terms. Accordingly this work puts another example for a loca... | 12.699944 | 10.231783 | 11.464073 | 11.299597 | 11.668106 | 11.751226 | 11.369804 | 10.843958 | 10.728097 | 11.948194 | 10.350344 | 10.974345 | 11.724257 | 11.357178 | 11.0682 | 11.337228 | 11.064466 | 11.176825 | 11.433662 | 11.382612 | 10.901447 |
hep-th/9705168 | null | V.E. Rochev | On solving Schwinger-Dyson equations for non-Abelian gauge theory | 12 pages, Plain LaTeX, no figures, extended and revised version
published in Journal of Physics A | J.Phys.A31:409-416,1998 | 10.1088/0305-4470/31/1/034 | null | hep-th | null | A method for solving Schwinger-Dyson equations for the Green function
generating functional of non-Abelian gauge theory is proposed. The method is
based on an approximation of Schwinger-Dyson equations by exactly soluble
equations. For the SU(2) model the first step equations of the iteration scheme
are solved which ... | [
{
"created": "Thu, 22 May 1997 15:03:04 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Dec 1997 15:40:56 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Rochev",
"V. E.",
""
]
] | A method for solving Schwinger-Dyson equations for the Green function generating functional of non-Abelian gauge theory is proposed. The method is based on an approximation of Schwinger-Dyson equations by exactly soluble equations. For the SU(2) model the first step equations of the iteration scheme are solved which de... | 7.90141 | 7.356851 | 7.98595 | 7.601079 | 8.491005 | 7.833181 | 7.976173 | 7.944277 | 6.971179 | 8.179961 | 7.605017 | 7.370166 | 7.432387 | 7.627897 | 7.377654 | 7.665354 | 7.479872 | 7.729259 | 7.429461 | 7.615951 | 7.515138 |
2310.16438 | Yong-Liang Ma | Fan Lin and Yong-Liang Ma | Baryons as Vortexes on the $\eta^{\prime}$ Domain Wall | 13 pages | J-Ref: JHEP 05 (2024) 270 | null | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the recent construction of $N_f=1$ baryons on the $\eta^\prime$
domain wall can be understood as vortexes of the principal effective theory --
the Chern-Simons-Higgs theory -- on a 2+1-dimensional sheet. This theory has a
series of vertex solutions, and the vortex with unit topological charge
naturally s... | [
{
"created": "Wed, 25 Oct 2023 08:04:11 GMT",
"version": "v1"
},
{
"created": "Tue, 28 May 2024 10:14:52 GMT",
"version": "v2"
}
] | 2024-05-29 | [
[
"Lin",
"Fan",
""
],
[
"Ma",
"Yong-Liang",
""
]
] | We show that the recent construction of $N_f=1$ baryons on the $\eta^\prime$ domain wall can be understood as vortexes of the principal effective theory -- the Chern-Simons-Higgs theory -- on a 2+1-dimensional sheet. This theory has a series of vertex solutions, and the vortex with unit topological charge naturally spi... | 11.201194 | 12.427364 | 11.09643 | 10.77865 | 11.324736 | 11.223425 | 11.38966 | 10.764887 | 10.321424 | 11.013436 | 10.369747 | 10.367876 | 11.497246 | 10.223673 | 10.384902 | 10.102537 | 10.274991 | 10.202919 | 10.600906 | 11.591368 | 9.90601 |
1809.04896 | Yakov Shnir | Tomasz Romanczukiewicz and Yakov Shnir | Some Recent Developments on Kink Collisions and Related Topics | 26 pages, 9 figures; invited chapter to "A dynamical perspective on
the {\phi}4 model: Past, present and future", Eds. P.G. Kevrekidis and J.
Cuevas-Maraver; Springer book class with svmult.cls included | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review recent works on modeling of dynamics of kinks in 1+1 dimensional
$\phi^4$ theory and other related models, like sine-Gordon model or $\phi^6$
theory. We discuss how the spectral structure of small perturbations can affect
the dynamics of non-perturbative states, such as kinks or oscillons. We
describe diffe... | [
{
"created": "Thu, 13 Sep 2018 11:56:25 GMT",
"version": "v1"
}
] | 2018-09-14 | [
[
"Romanczukiewicz",
"Tomasz",
""
],
[
"Shnir",
"Yakov",
""
]
] | We review recent works on modeling of dynamics of kinks in 1+1 dimensional $\phi^4$ theory and other related models, like sine-Gordon model or $\phi^6$ theory. We discuss how the spectral structure of small perturbations can affect the dynamics of non-perturbative states, such as kinks or oscillons. We describe differe... | 6.965272 | 6.578264 | 7.132409 | 6.54441 | 6.774264 | 6.726248 | 6.819218 | 6.587613 | 6.286339 | 7.320145 | 6.352752 | 6.54372 | 6.694586 | 6.497151 | 6.72224 | 6.684449 | 6.633031 | 6.643133 | 6.496573 | 6.566064 | 6.665274 |
hep-th/9605147 | Lawrence Horwitz | Oskar Pelc and L. P. Horwitz | Generalization of the Coleman-Mandula Theorem to Higher Dimension | 42 pages, Latex | J.Math.Phys. 38 (1997) 139-172 | 10.1063/1.531846 | IASSNS-96/31; TAUP 2175-94 | hep-th | null | The Coleman-Mandula theorem, which states that space-time and internal
symmetries cannot be combined in any but a trivial way, is generalized to an
arbitrarily higher spacelike dimension. Prospects for further generalizations
of the theorem (space-like representations, larger time-like dimension,
infinite number of p... | [
{
"created": "Tue, 21 May 1996 16:26:17 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Pelc",
"Oskar",
""
],
[
"Horwitz",
"L. P.",
""
]
] | The Coleman-Mandula theorem, which states that space-time and internal symmetries cannot be combined in any but a trivial way, is generalized to an arbitrarily higher spacelike dimension. Prospects for further generalizations of the theorem (space-like representations, larger time-like dimension, infinite number of par... | 9.452692 | 10.974494 | 9.784527 | 9.664474 | 9.874841 | 9.75511 | 11.054628 | 10.121953 | 8.922585 | 9.024581 | 9.957025 | 9.505147 | 9.125078 | 9.507575 | 9.281528 | 8.980512 | 9.720598 | 9.600393 | 9.599059 | 9.461652 | 9.149763 |
hep-th/9705023 | Michael Gutperle | Michael Gutperle (DAMTP, University of Cambridge) | Contact terms, symmetries and D-instantons | 18 pages, Latex | Nucl.Phys. B508 (1997) 133-146 | 10.1016/S0550-3213(97)00507-5 | DAMTP-97-44 | hep-th | null | The scattering of NS-NS antisymmetric tensor states in the presence of
D-instantons in type IIB superstring theory is studied. It is shown that in
order to preserve gauge invariance, spacetime supersymmetry and picture
changing symmetry the inclusion of boundary contact terms for closed string
antisymmetric tensor ve... | [
{
"created": "Mon, 5 May 1997 15:13:05 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Gutperle",
"Michael",
"",
"DAMTP, University of Cambridge"
]
] | The scattering of NS-NS antisymmetric tensor states in the presence of D-instantons in type IIB superstring theory is studied. It is shown that in order to preserve gauge invariance, spacetime supersymmetry and picture changing symmetry the inclusion of boundary contact terms for closed string antisymmetric tensor vert... | 9.635588 | 7.708575 | 8.951421 | 7.566663 | 8.46562 | 8.360137 | 8.23601 | 7.787368 | 7.666119 | 9.451204 | 7.778535 | 8.262156 | 10.443828 | 8.32418 | 7.850086 | 8.098426 | 8.18018 | 8.872585 | 8.352106 | 9.670377 | 8.718573 |
hep-th/0209197 | Yang Haitang | Haitang Yang | Stress Tensors in p-adic String Theory and Truncated OSFT | 18 pages, 3 figures | JHEP 0211 (2002) 007 | 10.1088/1126-6708/2002/11/007 | null | hep-th | null | We construct the stress tensors for the p-adic string model and for the pure
tachyonic sector of open string field theory by naive metric covariantization
of the action. Then we give the concrete energy density of a lump solution of
the p-adic model. In the cubic open bosonic string field theory, we also give
the ene... | [
{
"created": "Tue, 24 Sep 2002 02:03:21 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Sep 2002 16:20:43 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Oct 2002 23:32:34 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Yang",
"Haitang",
""
]
] | We construct the stress tensors for the p-adic string model and for the pure tachyonic sector of open string field theory by naive metric covariantization of the action. Then we give the concrete energy density of a lump solution of the p-adic model. In the cubic open bosonic string field theory, we also give the energ... | 12.893239 | 12.781224 | 13.898472 | 12.679191 | 14.719957 | 14.178442 | 13.271227 | 12.834761 | 12.348574 | 14.966453 | 11.93504 | 12.235007 | 13.321234 | 12.186741 | 12.380065 | 12.396186 | 12.512013 | 12.571332 | 12.099508 | 12.254816 | 12.208325 |
2211.07927 | Watse Sybesma | Watse Sybesma | A Zoo of Deformed Jackiw-Teitelboim Models near Large Dimensional Black
Holes | v2: Implemented changed of published version. v1: 12 pages, 1 figure,
1 table and one page of appendices | null | 10.1007/JHEP01(2023)141 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We consider a charged Lifshitz black hole in the large transverse dimension
limit. In this setup, the dynamics near the black hole horizon are shown to be
effectively governed by a family of two-dimensional models of dilaton gravity
depending on the ratio of the dynamical parameter characterizing the black hole
and t... | [
{
"created": "Tue, 15 Nov 2022 06:23:36 GMT",
"version": "v1"
},
{
"created": "Sat, 4 Feb 2023 21:50:55 GMT",
"version": "v2"
}
] | 2023-02-22 | [
[
"Sybesma",
"Watse",
""
]
] | We consider a charged Lifshitz black hole in the large transverse dimension limit. In this setup, the dynamics near the black hole horizon are shown to be effectively governed by a family of two-dimensional models of dilaton gravity depending on the ratio of the dynamical parameter characterizing the black hole and the... | 8.517501 | 8.567888 | 8.637844 | 8.425066 | 8.694127 | 8.407384 | 8.515067 | 7.955728 | 8.174577 | 8.863004 | 7.882443 | 8.09018 | 8.112246 | 8.300236 | 8.476033 | 8.642116 | 8.325535 | 8.318913 | 8.2224 | 8.261314 | 8.437362 |
hep-th/0610178 | Florian Bauer | Florian Bauer | The Cosmological Constant and Discrete Space-Times | 98 pages, PhD thesis | null | null | null | hep-th gr-qc hep-ph | null | In this thesis the cosmological constant is investigated from two points of
view. First, we study the influence of a time-dependent cosmological constant
on the late-time expansion of the universe. Thereby, we consider several
combinations of scaling laws motivated by renormalisation group running and
different choic... | [
{
"created": "Mon, 16 Oct 2006 16:02:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bauer",
"Florian",
""
]
] | In this thesis the cosmological constant is investigated from two points of view. First, we study the influence of a time-dependent cosmological constant on the late-time expansion of the universe. Thereby, we consider several combinations of scaling laws motivated by renormalisation group running and different choices... | 11.297994 | 11.033918 | 10.933672 | 10.39405 | 12.641725 | 11.60762 | 11.39456 | 10.7071 | 10.68032 | 10.773218 | 10.740069 | 10.663214 | 10.570656 | 10.380374 | 10.397069 | 10.628952 | 10.721148 | 10.66967 | 10.686404 | 10.613749 | 10.506732 |
1011.6241 | Emil Nissimov | Eduardo Guendelman, Alexander Kaganovich, Emil Nissimov and Svetlana
Pacheva | Space-Time Compactification, Non-Singular Black Holes, Wormholes and
Braneworlds via Lightlike Branes | 16 pages, to appear in "Sixth Summer School and Conference on Modern
Mathematical Physics", ed. B. Dragovic et.al., Belgrade Univ. Press (2011),
few typos in Appendix corrected | "Sixth Mathematical Physics Meeting'', pp. 217-234, B. Dragovic
and Z. Rakic (eds.), Belgrade Inst. Phys. Press (2011) | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a concise general scheme for constructing solutions of
Einstein-Maxwell-Kalb-Ramond gravity-matter system in bulk space-time
interacting self-consistently with one or more (widely separated)
codimension-one electrically charged lightlike branes. The lightlike brane
dynamics is explicitly given by manifest... | [
{
"created": "Mon, 29 Nov 2010 14:29:40 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Dec 2010 14:52:14 GMT",
"version": "v2"
}
] | 2016-11-29 | [
[
"Guendelman",
"Eduardo",
""
],
[
"Kaganovich",
"Alexander",
""
],
[
"Nissimov",
"Emil",
""
],
[
"Pacheva",
"Svetlana",
""
]
] | We describe a concise general scheme for constructing solutions of Einstein-Maxwell-Kalb-Ramond gravity-matter system in bulk space-time interacting self-consistently with one or more (widely separated) codimension-one electrically charged lightlike branes. The lightlike brane dynamics is explicitly given by manifestly... | 12.488493 | 12.081469 | 12.935502 | 11.924067 | 12.787932 | 11.976763 | 12.940278 | 11.248382 | 11.234586 | 14.243149 | 11.554513 | 11.707989 | 12.579062 | 11.650057 | 11.781917 | 11.879259 | 11.792306 | 11.193668 | 11.409653 | 12.311621 | 11.262619 |
1012.1300 | Hisham Sati | Hisham Sati | M-theory, the signature theorem, and geometric invariants | 17 pages | Phys.Rev.D83:126010,2011 | 10.1103/PhysRevD.83.126010 | null | hep-th math.AT math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The equations of motion and the Bianchi identity of the C-field in M-theory
are encoded in terms of the signature operator. We then reformulate the
topological part of the action in M-theory using the signature, which leads to
connections to the geometry of the underlying manifold, including positive
scalar curvature... | [
{
"created": "Mon, 6 Dec 2010 20:17:23 GMT",
"version": "v1"
}
] | 2011-07-08 | [
[
"Sati",
"Hisham",
""
]
] | The equations of motion and the Bianchi identity of the C-field in M-theory are encoded in terms of the signature operator. We then reformulate the topological part of the action in M-theory using the signature, which leads to connections to the geometry of the underlying manifold, including positive scalar curvature. ... | 15.420463 | 16.63517 | 18.197355 | 15.799802 | 15.924374 | 17.564068 | 16.591734 | 16.892174 | 14.650409 | 19.980526 | 15.631597 | 14.83453 | 15.819089 | 15.108261 | 14.849024 | 14.636744 | 14.721522 | 15.059269 | 15.203315 | 16.071127 | 14.571936 |
1505.05861 | Yifan Wang | Yifan Wang, Xi Yin | Supervertices and Non-renormalization Conditions in Maximal Supergravity
Theories | 52 pages, 6 figures, reference added, section 3 expanded and section
5 restructured | null | null | MIT-CTP/4673 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct higher derivative supervertices in an effective theory of
maximal supergravity in various dimensions, in the super spinor helicity
formalism, and derive non-renormalization conditions on up to 14-derivative
order couplings from supersymmetry. These non-renormalization conditions
include Laplace type equa... | [
{
"created": "Thu, 21 May 2015 19:53:06 GMT",
"version": "v1"
},
{
"created": "Fri, 29 May 2015 16:27:04 GMT",
"version": "v2"
}
] | 2015-06-01 | [
[
"Wang",
"Yifan",
""
],
[
"Yin",
"Xi",
""
]
] | We construct higher derivative supervertices in an effective theory of maximal supergravity in various dimensions, in the super spinor helicity formalism, and derive non-renormalization conditions on up to 14-derivative order couplings from supersymmetry. These non-renormalization conditions include Laplace type equati... | 10.267226 | 8.329058 | 11.445454 | 8.630238 | 8.47063 | 8.893843 | 8.729752 | 8.115186 | 8.750676 | 10.874454 | 9.008979 | 9.134096 | 10.534462 | 9.096034 | 9.20707 | 9.000017 | 9.077848 | 8.902167 | 9.419944 | 10.443568 | 9.11181 |
1908.05221 | Yvonne Geyer | Yvonne Geyer, Ricardo Monteiro, Ricardo Stark-Much\~ao | Two-Loop Scattering Amplitudes: Double-Forward Limit and
Colour-Kinematics Duality | 32 pages plus appendices, 17 figures | null | 10.1007/JHEP12(2019)049 | QMUL-PH-19-18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose new formulae for the two-loop n-point D-dimensional integrands of
scattering amplitudes in Yang-Mills theory and gravity. The loop integrands are
written as a double-forward limit of tree-level trivalent diagrams, and are
inferred from the formalism of the two-loop scattering equations. We discuss
the rela... | [
{
"created": "Wed, 14 Aug 2019 16:50:33 GMT",
"version": "v1"
}
] | 2020-01-29 | [
[
"Geyer",
"Yvonne",
""
],
[
"Monteiro",
"Ricardo",
""
],
[
"Stark-Muchão",
"Ricardo",
""
]
] | We propose new formulae for the two-loop n-point D-dimensional integrands of scattering amplitudes in Yang-Mills theory and gravity. The loop integrands are written as a double-forward limit of tree-level trivalent diagrams, and are inferred from the formalism of the two-loop scattering equations. We discuss the relati... | 8.420981 | 8.457164 | 9.721305 | 8.036674 | 8.409469 | 7.899498 | 8.243723 | 7.582787 | 8.155973 | 10.152617 | 7.816391 | 8.104231 | 8.742756 | 7.834928 | 7.945683 | 7.835518 | 7.573825 | 7.91477 | 8.163735 | 8.584929 | 7.763006 |
0812.3614 | G\'abor Zsolt T\'oth | Gabor Zsolt Toth | Proposal to improve the behaviour of self-energy contributions to the
S-matrix | 24 pages, 1 figure; v2: revised version; v3: section 3 improved.
Accepted for publication in Central European Journal of Physics; v4: minor
text misprints corrected | Central Eur.J.Phys.8:527-541,2010 | 10.2478/s11534-009-0139-0 | SISSA 84/2008/EP | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A simple modification of the definition of the S-matrix is proposed. It is
expected that the divergences related to nonzero self-energies are considerably
milder with the modified definition than with the usual one. This conjecture is
verified in a few examples using perturbation theory. The proposed formula is
writt... | [
{
"created": "Thu, 18 Dec 2008 18:33:06 GMT",
"version": "v1"
},
{
"created": "Sun, 1 Feb 2009 20:07:22 GMT",
"version": "v2"
},
{
"created": "Mon, 31 Aug 2009 17:12:39 GMT",
"version": "v3"
},
{
"created": "Sat, 10 Oct 2009 11:44:58 GMT",
"version": "v4"
}
] | 2011-04-07 | [
[
"Toth",
"Gabor Zsolt",
""
]
] | A simple modification of the definition of the S-matrix is proposed. It is expected that the divergences related to nonzero self-energies are considerably milder with the modified definition than with the usual one. This conjecture is verified in a few examples using perturbation theory. The proposed formula is written... | 9.945044 | 9.206664 | 8.931186 | 9.470709 | 9.445143 | 10.137605 | 9.955956 | 9.260523 | 9.227032 | 10.260327 | 8.609971 | 9.038816 | 8.441593 | 8.696849 | 8.738382 | 8.768454 | 8.874441 | 8.674218 | 8.631538 | 8.796124 | 8.714254 |
hep-th/0407023 | Alexander Sevrin | Alexander Sevrin | Prospects from Strings and Branes | 10 pages, 5 figures, contribution to the proceedings of XXXIXth
Rencontres de Moriond on Electroweak Interactions and Unified Theories,
references added | null | null | null | hep-th hep-ex hep-ph | null | A brief, non-technical and non-exhaustive review of D(irichlet)-branes and
(some) of their applications is given.
| [
{
"created": "Sun, 4 Jul 2004 18:38:53 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Jul 2004 11:56:04 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Sevrin",
"Alexander",
""
]
] | A brief, non-technical and non-exhaustive review of D(irichlet)-branes and (some) of their applications is given. | 18.601452 | 7.160102 | 9.417707 | 6.932614 | 8.35408 | 7.831213 | 7.280668 | 7.113274 | 8.203197 | 10.539112 | 9.556396 | 7.305369 | 9.582319 | 7.632027 | 7.35273 | 7.442412 | 7.162686 | 7.426782 | 7.573967 | 9.649585 | 7.716781 |
hep-th/9407096 | Toshio Nakatsu | Toshio Nakatsu | On the string equation at $c=1$ | 17pp,INS-Rep.1043, to appear in Mod.Phys.Lett.A, Some modifications
have been performed from the view of the double scaled field theory.And also
the relation with the classical (genus 0) results is described | Mod.Phys.Lett.A9:3313-3324,1994 | 10.1142/S0217732394003130 | null | hep-th | null | The analogue of the string equation which specifies the partition function of
$c=1$ string with a compactification radius $\beta \in \mbox{$\bf{Z}$}_{\geq 1}
$ is described in the framework of the Toda lattice hierarchy.
| [
{
"created": "Sat, 16 Jul 1994 04:25:10 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Oct 1994 20:14:55 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Nakatsu",
"Toshio",
""
]
] | The analogue of the string equation which specifies the partition function of $c=1$ string with a compactification radius $\beta \in \mbox{$\bf{Z}$}_{\geq 1} $ is described in the framework of the Toda lattice hierarchy. | 11.258016 | 8.765807 | 12.110487 | 9.358914 | 10.055853 | 8.0869 | 9.476356 | 8.871619 | 8.62697 | 13.354176 | 8.766629 | 9.094817 | 12.06511 | 9.393028 | 9.633712 | 9.478631 | 9.34024 | 9.572769 | 9.181149 | 10.994576 | 9.588851 |
hep-th/0102101 | Marcelo Gomes | H. O. Girotti, M. Gomes, V. O. Rivelles and A. J. da Silva | The Noncommutative Supersymmetric Nonlinear Sigma Model | 15 pages, 7 figures, revtex, minor modifications in the text,
references added | Int.J.Mod.Phys. A17 (2002) 1503-1516 | 10.1142/S0217751X02009850 | null | hep-th | null | We show that the noncommutativity of space-time destroys the
renormalizability of the 1/N expansion of the O(N) Gross-Neveu model. A similar
statement holds for the noncommutative nonlinear sigma model. However, we show
that, up to the subleading order in 1/N expansion, the noncommutative
supersymmetric O(N) nonlinea... | [
{
"created": "Fri, 16 Feb 2001 14:52:24 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Jun 2001 18:58:54 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Girotti",
"H. O.",
""
],
[
"Gomes",
"M.",
""
],
[
"Rivelles",
"V. O.",
""
],
[
"da Silva",
"A. J.",
""
]
] | We show that the noncommutativity of space-time destroys the renormalizability of the 1/N expansion of the O(N) Gross-Neveu model. A similar statement holds for the noncommutative nonlinear sigma model. However, we show that, up to the subleading order in 1/N expansion, the noncommutative supersymmetric O(N) nonlinear ... | 6.57796 | 6.549373 | 7.005019 | 6.289245 | 6.94775 | 6.569089 | 6.604806 | 6.575483 | 6.494562 | 7.417953 | 6.324386 | 6.477424 | 6.652278 | 6.190988 | 6.331071 | 6.397596 | 6.262868 | 6.424493 | 6.355657 | 6.464025 | 6.281532 |
0801.2064 | Joseph A. Minahan | J. A. Minahan, O. Ohlsson Sax | Finite size effects for giant magnons on physical strings | 24 pages, 7 figures; v2 typos fixed | Nucl.Phys.B801:97-117,2008 | 10.1016/j.nuclphysb.2008.04.018 | UUITP-20/07 | hep-th | null | Using finite gap methods, we find the leading order finite size corrections
for an arbitrary number of giant magnons on physical strings, where the sum of
the momenta is a multiple of 2\pi. Our results are valid for the
Hofman-Maldacena fundamental giant magnons as well as their dyonic
generalizations. The energy cor... | [
{
"created": "Mon, 14 Jan 2008 20:20:20 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Feb 2008 03:30:42 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Minahan",
"J. A.",
""
],
[
"Sax",
"O. Ohlsson",
""
]
] | Using finite gap methods, we find the leading order finite size corrections for an arbitrary number of giant magnons on physical strings, where the sum of the momenta is a multiple of 2\pi. Our results are valid for the Hofman-Maldacena fundamental giant magnons as well as their dyonic generalizations. The energy corre... | 7.778256 | 8.184829 | 8.691201 | 7.570152 | 7.842414 | 8.419837 | 7.85933 | 7.532969 | 7.42343 | 8.695325 | 7.686092 | 7.340177 | 7.781926 | 7.259373 | 7.868393 | 7.26781 | 7.438451 | 7.587002 | 7.367576 | 7.691784 | 7.400063 |
2002.11085 | Nathan Moynihan | Nathan Moynihan and Jeff Murugan | On-Shell Electric-Magnetic Duality and the Dual Graviton | null | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using on-shell amplitude methods, we explore 4-dimensional Electric-Magnetic
duality and its double copy. We show explicitly that the on-shell scattering
amplitudes know about `dual' photons (and dual gravitons), that the off-shell
photon propagator double copies to the graviton propagator and that the
magnetic part ... | [
{
"created": "Tue, 25 Feb 2020 18:31:27 GMT",
"version": "v1"
}
] | 2020-02-26 | [
[
"Moynihan",
"Nathan",
""
],
[
"Murugan",
"Jeff",
""
]
] | Using on-shell amplitude methods, we explore 4-dimensional Electric-Magnetic duality and its double copy. We show explicitly that the on-shell scattering amplitudes know about `dual' photons (and dual gravitons), that the off-shell photon propagator double copies to the graviton propagator and that the magnetic part of... | 9.116453 | 8.667424 | 8.934875 | 8.668076 | 9.619786 | 9.323799 | 9.087514 | 8.994431 | 8.847914 | 10.379414 | 8.691072 | 8.949176 | 8.595645 | 8.572137 | 8.991741 | 8.940207 | 8.890388 | 8.873445 | 8.742219 | 8.855943 | 8.701838 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.