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
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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9310171 | Miroslav Doresic | V.Bardek, M.Doresic and S.Meljanac | Example of q-deformed Field Theory | 13 pages,LaTex | Int. J. Mod. Phys. A9 (1994) 4185-4194 | 10.1142/S0217751X94001709 | null | hep-th | null | The non-relativistic Chern-Simons theory with the single-valued anyonic field
is proposed as an example of q-deformed field theory. The corresponding
q-deformed algebra interpolating between bosons and fermions,both in position
and momentum spaces, is analyzed.A possible generalization to a space with an
arbitrary di... | [
{
"created": "Tue, 26 Oct 1993 14:33:37 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bardek",
"V.",
""
],
[
"Doresic",
"M.",
""
],
[
"Meljanac",
"S.",
""
]
] | The non-relativistic Chern-Simons theory with the single-valued anyonic field is proposed as an example of q-deformed field theory. The corresponding q-deformed algebra interpolating between bosons and fermions,both in position and momentum spaces, is analyzed.A possible generalization to a space with an arbitrary dime... | 12.008847 | 10.273028 | 12.020064 | 10.48955 | 11.263812 | 10.394651 | 9.54876 | 10.631811 | 10.116027 | 13.839041 | 10.424173 | 11.064335 | 12.640553 | 11.969355 | 11.491976 | 11.68769 | 11.088754 | 11.243912 | 11.279983 | 11.989622 | 11.160674 |
0911.2665 | Ioannis Bakas | Ioannis Bakas, Francois Bourliot, Dieter Lust, Marios Petropoulos | Mixmaster universe in Horava-Lifshitz gravity | 1+35 pages, 4 figures | Class.Quant.Grav.27:045013,2010 | 10.1088/0264-9381/27/4/045013 | CPHT-RR111.1109, LMU-ASC 48/09, MPP-2009-180 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider spatially homogeneous (but generally non-isotropic) cosmologies
in the recently proposed Horava-Lifshitz gravity and compare them to those of
general relativity using Hamiltonian methods. In all cases, the problem is
described by an effective point particle moving in a potential well with
exponentially st... | [
{
"created": "Fri, 13 Nov 2009 17:57:35 GMT",
"version": "v1"
}
] | 2011-02-25 | [
[
"Bakas",
"Ioannis",
""
],
[
"Bourliot",
"Francois",
""
],
[
"Lust",
"Dieter",
""
],
[
"Petropoulos",
"Marios",
""
]
] | We consider spatially homogeneous (but generally non-isotropic) cosmologies in the recently proposed Horava-Lifshitz gravity and compare them to those of general relativity using Hamiltonian methods. In all cases, the problem is described by an effective point particle moving in a potential well with exponentially stee... | 11.153405 | 11.780639 | 10.229119 | 10.491212 | 11.138741 | 11.459359 | 11.556599 | 10.209954 | 10.594728 | 11.649254 | 11.081223 | 10.798649 | 10.493099 | 10.424191 | 10.711563 | 10.735345 | 11.210979 | 10.417023 | 10.956346 | 10.805263 | 10.929437 |
2405.02072 | Thomas Van Riet | T. Hertog, S. Maenaut, B. Missoni, R. Tielemans, T. Van Riet | Stability of Axion-Saxion wormholes | 29 pages, O(10) pictures, v2 reference updated | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We reconsider the perturbative stability of Euclidean axion wormholes. The
quadratic action that governs linear perturbations is derived directly in
Euclidean gravity. We demonstrate explicitly that a stability analysis in which
one treats the axion as a normal two-form gauge field is equivalent to one
performed in t... | [
{
"created": "Fri, 3 May 2024 13:05:47 GMT",
"version": "v1"
},
{
"created": "Sun, 28 Jul 2024 10:15:57 GMT",
"version": "v2"
}
] | 2024-07-30 | [
[
"Hertog",
"T.",
""
],
[
"Maenaut",
"S.",
""
],
[
"Missoni",
"B.",
""
],
[
"Tielemans",
"R.",
""
],
[
"Van Riet",
"T.",
""
]
] | We reconsider the perturbative stability of Euclidean axion wormholes. The quadratic action that governs linear perturbations is derived directly in Euclidean gravity. We demonstrate explicitly that a stability analysis in which one treats the axion as a normal two-form gauge field is equivalent to one performed in the... | 9.11998 | 8.302555 | 8.294038 | 8.534656 | 7.787939 | 7.885938 | 7.986439 | 7.727121 | 7.972707 | 9.901261 | 8.202686 | 8.53445 | 8.427194 | 8.446739 | 8.506869 | 8.397065 | 8.331258 | 8.385478 | 8.701845 | 8.748092 | 8.436489 |
hep-th/9203075 | null | E. Abdalla, M. Forger | Current Algebra of WZNW Models at and away from Criticality | 10 pages | Mod. Phys. Lett. A7 (1992) 2437-2448 | 10.1142/S0217732392003888 | null | hep-th | null | We derive the current algebra of principal chiral models with a Wess-Zumino
term. At the critical coupling where the model becomes conformally invariant
(Wess-Zumino-Novikov-Witten theory), this algebra reduces to two commuting
Kac-Moody algebras, while in the limit where the coupling constant is taken to
zero (ordin... | [
{
"created": "Sat, 28 Mar 1992 16:23:00 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Abdalla",
"E.",
""
],
[
"Forger",
"M.",
""
]
] | We derive the current algebra of principal chiral models with a Wess-Zumino term. At the critical coupling where the model becomes conformally invariant (Wess-Zumino-Novikov-Witten theory), this algebra reduces to two commuting Kac-Moody algebras, while in the limit where the coupling constant is taken to zero (ordinar... | 5.81016 | 5.835678 | 5.880346 | 5.157075 | 5.325333 | 5.077283 | 5.558911 | 5.430918 | 5.047252 | 5.379598 | 5.726479 | 5.558432 | 5.604663 | 5.321245 | 5.452018 | 5.415073 | 5.488311 | 5.479055 | 5.475016 | 5.767703 | 5.576794 |
hep-th/9604004 | Jacques Distler | Luis Alvarez-Gaume, Jacques Distler, Costas Kounnas and Marcos Marino | Large Softly broken N=2 QCD | 40 pages, LaTeX, 13 figures, uses epsf.sty | Int.J.Mod.Phys.A11:4745-4777,1996 | 10.1142/S0217751X96002170 | CERN-TH/9669, US-FT-13/96, UTTG-96-03 | hep-th | null | We analyze the possible soft breaking of $N=2$ supersymmetric Yang-Mills
theory with and without matter flavour preserving the analyticity properties of
the Seiberg-Witten solution. For small supersymmetry breaking parameter with
respect to the dynamical scale of the theory we obtain an exact expression for
the effec... | [
{
"created": "Mon, 1 Apr 1996 20:34:30 GMT",
"version": "v1"
}
] | 2009-07-09 | [
[
"Alvarez-Gaume",
"Luis",
""
],
[
"Distler",
"Jacques",
""
],
[
"Kounnas",
"Costas",
""
],
[
"Marino",
"Marcos",
""
]
] | We analyze the possible soft breaking of $N=2$ supersymmetric Yang-Mills theory with and without matter flavour preserving the analyticity properties of the Seiberg-Witten solution. For small supersymmetry breaking parameter with respect to the dynamical scale of the theory we obtain an exact expression for the effecti... | 10.32192 | 8.584851 | 11.008236 | 8.942887 | 10.499473 | 9.388009 | 10.026165 | 9.483857 | 9.29212 | 11.462072 | 9.625827 | 9.390355 | 10.072848 | 9.581878 | 10.014485 | 9.783062 | 9.834178 | 9.38583 | 9.541314 | 10.207554 | 9.911861 |
1612.05123 | Gianluca Inverso | Gianluca Inverso, Henning Samtleben and Mario Trigiante | Type II origin of dyonic gaugings | 32 pages, v2: new appendix on relation to N=4 Janus solutions,
version to appear in PRD | Phys. Rev. D 95, 066020 (2017) | 10.1103/PhysRevD.95.066020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dyonic gaugings of four-dimensional supergravity typically exhibit a richer
vacuum structure compared to their purely electric counterparts, but their
higher-dimensional origin often remains more mysterious. We consider a class of
dyonic gaugings with gauge groups of the type (SO(p,q)xSO(p',q'))$\ltimes N$
with $N$ n... | [
{
"created": "Thu, 15 Dec 2016 16:02:58 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Mar 2017 13:33:56 GMT",
"version": "v2"
}
] | 2017-04-05 | [
[
"Inverso",
"Gianluca",
""
],
[
"Samtleben",
"Henning",
""
],
[
"Trigiante",
"Mario",
""
]
] | Dyonic gaugings of four-dimensional supergravity typically exhibit a richer vacuum structure compared to their purely electric counterparts, but their higher-dimensional origin often remains more mysterious. We consider a class of dyonic gaugings with gauge groups of the type (SO(p,q)xSO(p',q'))$\ltimes N$ with $N$ nil... | 6.65553 | 6.091936 | 8.292404 | 6.108197 | 6.341941 | 7.176361 | 6.314253 | 6.705167 | 6.086782 | 8.233956 | 6.56828 | 6.12289 | 6.81754 | 6.315307 | 6.357412 | 6.165801 | 6.115747 | 5.901069 | 6.076542 | 6.600664 | 5.957868 |
1412.3382 | Mikhail Shifman | M. Shifman, K. Stepanyantz | Exact Adler Function in Supersymmetric QCD | 5 pages, 1 figure | Phys. Rev. Lett. 114, 051601 (2015) | 10.1103/PhysRevLett.114.051601 | FTPI-MINN-14/41, UMN-TH-3412/14 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Adler function D is found {\em exactly} in supersymmetric QCD. Our exact
formula relates D(Q^2) to the anomalous dimension of the matter superfields
\gamma (\alpha_s(Q^2)). En rout we prove another theorem: the absence of the
so-called singlet contribution to D. While such singlet contributions are
present in ind... | [
{
"created": "Wed, 10 Dec 2014 17:41:29 GMT",
"version": "v1"
}
] | 2015-03-05 | [
[
"Shifman",
"M.",
""
],
[
"Stepanyantz",
"K.",
""
]
] | The Adler function D is found {\em exactly} in supersymmetric QCD. Our exact formula relates D(Q^2) to the anomalous dimension of the matter superfields \gamma (\alpha_s(Q^2)). En rout we prove another theorem: the absence of the so-called singlet contribution to D. While such singlet contributions are present in indiv... | 16.79295 | 15.523783 | 14.974259 | 11.851428 | 14.098233 | 13.771918 | 16.268351 | 15.629818 | 13.876882 | 15.009205 | 14.979633 | 13.217577 | 13.029335 | 12.908883 | 13.156375 | 13.583383 | 13.119058 | 13.274686 | 12.527965 | 14.440202 | 13.530478 |
hep-th/9706179 | Ilya L. Shapiro | A.L. Maroto (Universidad Autonoma de Madrid) I.L. Shapiro
(Universidade Federal de Juiz de Fora and Tomsk State Pedagogical University) | On the inflationary solutions in higher-derivative gravity with dilaton
field | 13 pages, LaTeX, no figures | Phys.Lett.B414:34-44,1997 | 10.1016/S0370-2693(97)01146-5 | FTUAM/97-2; NF/DF-01/97 | hep-th | null | We discuss the existence of de Sitter inflationary solutions for the
string-inspired fourth-derivative gravity theories with dilaton field. We
consider a space-time of arbitrary dimension D and an arbitrary parametrization
of the target space metric. The specific features of the theory in dimension
D=4 and those of t... | [
{
"created": "Wed, 25 Jun 1997 13:49:53 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Maroto",
"A. L.",
"",
"Universidad Autonoma de Madrid"
],
[
"Shapiro",
"I. L.",
"",
"Universidade Federal de Juiz de Fora and Tomsk State Pedagogical University"
]
] | We discuss the existence of de Sitter inflationary solutions for the string-inspired fourth-derivative gravity theories with dilaton field. We consider a space-time of arbitrary dimension D and an arbitrary parametrization of the target space metric. The specific features of the theory in dimension D=4 and those of the... | 9.811619 | 9.496107 | 8.344467 | 8.293017 | 8.056535 | 8.682148 | 9.304513 | 7.834244 | 8.608128 | 8.844668 | 8.684429 | 8.666023 | 9.228753 | 9.030571 | 9.185945 | 9.330248 | 9.258172 | 8.98472 | 8.970724 | 9.292567 | 9.02209 |
hep-th/0601003 | Karim Benakli | I. Antoniadis, K. Benakli, A. Delgado, M. Quir\'os and M. Tuckmantel | Split extended supersymmetry from intersecting branes | 32 pages, 3 figures | Nucl.Phys.B744:156-179,2006 | 10.1016/j.nuclphysb.2006.03.012 | null | hep-th hep-ph | null | We study string realizations of split extended supersymmetry, recently
proposed in hep-ph/0507192. Supersymmetry is broken by small ($\epsilon $)
deformations of intersection angles of $D$-branes giving tree-level masses of
order $m_0^2\sim \epsilon M_s^2$, where $M_s$ is the string scale, to localized
scalars. We sh... | [
{
"created": "Fri, 30 Dec 2005 21:03:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Antoniadis",
"I.",
""
],
[
"Benakli",
"K.",
""
],
[
"Delgado",
"A.",
""
],
[
"Quirós",
"M.",
""
],
[
"Tuckmantel",
"M.",
""
]
] | We study string realizations of split extended supersymmetry, recently proposed in hep-ph/0507192. Supersymmetry is broken by small ($\epsilon $) deformations of intersection angles of $D$-branes giving tree-level masses of order $m_0^2\sim \epsilon M_s^2$, where $M_s$ is the string scale, to localized scalars. We show... | 7.895015 | 8.43172 | 7.738659 | 7.123877 | 8.723101 | 8.470957 | 8.132802 | 7.846547 | 7.602814 | 8.110868 | 7.443853 | 7.7862 | 7.408036 | 7.636472 | 7.726206 | 7.74293 | 7.740169 | 7.754635 | 7.477538 | 7.474842 | 7.587735 |
2106.07957 | Joan Elias Mir\'o | Joan Elias Mir\'o, Andrea Guerrieri | Dual EFT Bootstrap: QCD flux tubes | 21 pages + appendices + references | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a bootstrap approach to Effective Field Theories (EFTs) based on
the concept of duality in optimisation theory. As a first application, we
consider the fascinating set of EFTs for confining flux tubes. The outcome of
our analysis are optimal bounds on the scattering amplitude of Goldstone
excitations of th... | [
{
"created": "Tue, 15 Jun 2021 08:19:00 GMT",
"version": "v1"
}
] | 2021-06-16 | [
[
"Miró",
"Joan Elias",
""
],
[
"Guerrieri",
"Andrea",
""
]
] | We develop a bootstrap approach to Effective Field Theories (EFTs) based on the concept of duality in optimisation theory. As a first application, we consider the fascinating set of EFTs for confining flux tubes. The outcome of our analysis are optimal bounds on the scattering amplitude of Goldstone excitations of the ... | 11.048774 | 7.969951 | 10.315049 | 8.207919 | 8.479935 | 8.019403 | 8.152657 | 8.182771 | 8.109129 | 9.962534 | 8.320208 | 8.535228 | 9.594142 | 8.74702 | 8.662062 | 8.870058 | 8.625362 | 8.469622 | 8.574754 | 9.222214 | 8.392816 |
1902.05273 | Yu Nakayama | Yu Nakayama | Conformal equations that are not Virasoro or Weyl invariant | 18 pages, v2: appendix added | null | 10.1007/s11005-019-01186-8 | RUP-19-5 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | While the argument by Zamolodchikov and Polchinski suggests global conformal
invariance implies Virasoro invariance in two-dimensional unitary conformal
field theories with discrete dilatation spectrum, it is not the case in more
general situations without these assumptions. We indeed show that almost all
the globall... | [
{
"created": "Thu, 14 Feb 2019 09:16:06 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Feb 2019 06:19:43 GMT",
"version": "v2"
}
] | 2019-05-22 | [
[
"Nakayama",
"Yu",
""
]
] | While the argument by Zamolodchikov and Polchinski suggests global conformal invariance implies Virasoro invariance in two-dimensional unitary conformal field theories with discrete dilatation spectrum, it is not the case in more general situations without these assumptions. We indeed show that almost all the globally ... | 10.384294 | 10.028575 | 11.048968 | 10.153967 | 10.093567 | 9.295738 | 11.410675 | 9.31359 | 9.71205 | 12.067778 | 9.335121 | 8.577063 | 8.869705 | 8.971667 | 9.37958 | 9.220387 | 9.218188 | 8.932975 | 8.604535 | 8.750443 | 9.342758 |
1611.08125 | Karl Landsteiner | Christian Copetti, Jorge Fern\'andez-Pend\'as, Karl Landsteiner | Axial Hall effect and universality of holographic Weyl semi-metals | 27 pages, 9 figures, v2: references added, some typos fixed; v3 minor
changes | null | 10.1007/JHEP02(2017)138 | IFT-UAM/CSIC-16-132 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The holographic Weyl semimetal is a model of a strongly coupled topological
semi-metal. A topological quantum phase transition separates a topological
phase with non-vanishing anomalous Hall conductivity from a trivial state. We
investigate how this phase transition depends on the parameters of the scalar
potential (... | [
{
"created": "Thu, 24 Nov 2016 10:13:06 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Dec 2016 16:12:00 GMT",
"version": "v2"
},
{
"created": "Wed, 22 Feb 2017 09:23:00 GMT",
"version": "v3"
}
] | 2017-04-05 | [
[
"Copetti",
"Christian",
""
],
[
"Fernández-Pendás",
"Jorge",
""
],
[
"Landsteiner",
"Karl",
""
]
] | The holographic Weyl semimetal is a model of a strongly coupled topological semi-metal. A topological quantum phase transition separates a topological phase with non-vanishing anomalous Hall conductivity from a trivial state. We investigate how this phase transition depends on the parameters of the scalar potential (ma... | 7.285273 | 6.610554 | 7.515957 | 6.325205 | 6.407455 | 6.879373 | 6.988988 | 6.643301 | 6.338823 | 7.301826 | 6.405302 | 6.627544 | 6.897281 | 6.873271 | 7.188793 | 7.080091 | 6.954198 | 6.833446 | 6.745917 | 6.915529 | 6.80721 |
hep-th/9407166 | Marco Vekic | Marco Vekic, Shao Liu, and Herbert W. Hamber | Random Ising Spins in Two Dimensions - A Flat Space Realization of the
KPZ Exponents | RevTeX 3.0, 17 pages + 15 postscript figures available upon request,
CERN-TH-7355/94 | Phys.Rev. D51 (1995) 4287-4294 | 10.1103/PhysRevD.51.4287 | null | hep-th cond-mat hep-lat | null | A model describing Ising spins with short range interactions moving randomly
in a plane is considered. In the presence of a hard core repulsion, which
prevents the Ising spins from overlapping, the model is analogous to a
dynamically triangulated Ising model with spins constrained to move on a flat
surface. As a func... | [
{
"created": "Mon, 25 Jul 1994 18:44:15 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Jul 1994 00:45:46 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Vekic",
"Marco",
""
],
[
"Liu",
"Shao",
""
],
[
"Hamber",
"Herbert W.",
""
]
] | A model describing Ising spins with short range interactions moving randomly in a plane is considered. In the presence of a hard core repulsion, which prevents the Ising spins from overlapping, the model is analogous to a dynamically triangulated Ising model with spins constrained to move on a flat surface. As a functi... | 9.47796 | 6.454637 | 9.088579 | 7.507236 | 7.434413 | 7.366051 | 7.145108 | 6.676868 | 7.011339 | 10.667702 | 7.787961 | 8.648582 | 9.454233 | 8.687142 | 8.723801 | 8.519047 | 8.590113 | 8.673026 | 8.675463 | 9.412845 | 8.600389 |
2201.09364 | Eric Lescano | Eric Lescano and Sourav Roychowdhury | Heterotic Kerr-Schild Double Field Theory and its double Yang-Mills
formulation | 33 pages, v2: Section 6 (Discussion) with clarifications. We are very
grateful to our anonymous JHEP referee. Matches published version | JHEP04(2022)090 | 10.1007/JHEP04(2022)090 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We present a formulation of heterotic Double Field Theory (DFT), where the
fundamental fields are in $O(D,D)$ representations. The theory is obtained
splitting an $O(D,D+K)$ duality invariant DFT. This procedure produces a
Green-Schwarz mechanism for the generalized metric, and a fundamental gauge
field which transfo... | [
{
"created": "Sun, 23 Jan 2022 20:55:50 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Apr 2022 12:43:18 GMT",
"version": "v2"
}
] | 2022-04-26 | [
[
"Lescano",
"Eric",
""
],
[
"Roychowdhury",
"Sourav",
""
]
] | We present a formulation of heterotic Double Field Theory (DFT), where the fundamental fields are in $O(D,D)$ representations. The theory is obtained splitting an $O(D,D+K)$ duality invariant DFT. This procedure produces a Green-Schwarz mechanism for the generalized metric, and a fundamental gauge field which transform... | 12.029915 | 13.327369 | 13.442693 | 12.8013 | 12.40986 | 13.805358 | 13.325847 | 11.925565 | 12.62654 | 13.640971 | 12.409081 | 12.378338 | 12.024651 | 11.746167 | 12.346474 | 12.206346 | 11.842251 | 12.1926 | 11.891966 | 12.346045 | 11.657776 |
hep-th/0610033 | Aaron Simons | Paul S. Aspinwall, Alexander Maloney and Aaron Simons | Black Hole Entropy, Marginal Stability and Mirror Symmetry | 24 pages | JHEP0707:034,2007 | 10.1088/1126-6708/2007/07/034 | DUKE-CGTP-06-01, SLAC-PUB-12048 | hep-th | null | We consider the superconformal quantum mechanics associated to BPS black
holes in type IIB Calabi-Yau compactifications. This quantum mechanics
describes the dynamics of D-branes in the near-horizon attractor geometry of
the black hole. In many cases, the black hole entropy can be found by counting
the number of chir... | [
{
"created": "Tue, 3 Oct 2006 16:11:02 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Aspinwall",
"Paul S.",
""
],
[
"Maloney",
"Alexander",
""
],
[
"Simons",
"Aaron",
""
]
] | We consider the superconformal quantum mechanics associated to BPS black holes in type IIB Calabi-Yau compactifications. This quantum mechanics describes the dynamics of D-branes in the near-horizon attractor geometry of the black hole. In many cases, the black hole entropy can be found by counting the number of chiral... | 7.94735 | 8.432984 | 9.592248 | 7.908662 | 8.539304 | 8.547949 | 8.345104 | 7.983572 | 8.272316 | 9.95986 | 7.540243 | 7.789019 | 8.442702 | 7.618215 | 7.583637 | 7.828359 | 7.984659 | 7.783796 | 7.568856 | 8.437684 | 7.771919 |
hep-th/9909224 | Igor Krichever | I. M. Krichever (Columbia University and Landau Institute for
Theoretical Physics) | Elliptic analog of the Toda lattice | 25 pages, LaTeX | null | null | null | hep-th | null | The action-angle variables for N-particle Hamiltonian system with the
Hamiltonian $H=\sum_{n=0}^{N-1} \ln sh^{-2}(p_n/2)+\ln(\wp(x_n-x_{n+1})-
\wp(x_n+x_{n+1})), x_N=x_0,$ are constructed, and the system is solved in terms
of the Riemann $\theta$-functions. It is shown that this system describes pole
dynamics of the ... | [
{
"created": "Thu, 30 Sep 1999 13:27:39 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Nov 1999 17:17:51 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Krichever",
"I. M.",
"",
"Columbia University and Landau Institute for\n Theoretical Physics"
]
] | The action-angle variables for N-particle Hamiltonian system with the Hamiltonian $H=\sum_{n=0}^{N-1} \ln sh^{-2}(p_n/2)+\ln(\wp(x_n-x_{n+1})- \wp(x_n+x_{n+1})), x_N=x_0,$ are constructed, and the system is solved in terms of the Riemann $\theta$-functions. It is shown that this system describes pole dynamics of the el... | 6.261842 | 7.037703 | 7.440109 | 6.540276 | 7.136791 | 7.096977 | 6.714044 | 6.986744 | 6.332026 | 8.389617 | 6.448125 | 6.567121 | 6.794055 | 6.21731 | 6.192153 | 6.200428 | 6.494355 | 6.620138 | 6.281588 | 6.741796 | 6.27629 |
1906.04853 | Steven Weinberg | Raphael Flauger, Steven Weinberg | Absorption of Gravitational Waves from Distant Sources | null | Phys. Rev. D 99, 123030 (2019) | 10.1103/PhysRevD.99.123030 | UTTG-03-19 | hep-th astro-ph.CO astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The rate of gravitational wave absorption by inverse bremsstrahlung is
calculated. It increases with decreasing frequency $\nu$ as $\nu^{-3}$.
Nevertheless, because of the near cancellation of absorption by stimulated
emission, the ionized gas in galaxy clusters does not block gravitational waves
at the nanohertz fre... | [
{
"created": "Tue, 11 Jun 2019 22:54:36 GMT",
"version": "v1"
}
] | 2019-07-03 | [
[
"Flauger",
"Raphael",
""
],
[
"Weinberg",
"Steven",
""
]
] | The rate of gravitational wave absorption by inverse bremsstrahlung is calculated. It increases with decreasing frequency $\nu$ as $\nu^{-3}$. Nevertheless, because of the near cancellation of absorption by stimulated emission, the ionized gas in galaxy clusters does not block gravitational waves at the nanohertz frequ... | 10.438334 | 12.499742 | 10.152308 | 9.697568 | 10.335986 | 12.16877 | 10.477113 | 10.853721 | 9.816033 | 9.994106 | 11.378405 | 10.624171 | 9.506311 | 9.37885 | 9.665295 | 9.232054 | 10.338542 | 9.474031 | 10.121468 | 9.495602 | 11.602088 |
2402.00494 | Joerg Teschner | Davide Gaiotto and J\"org Teschner | Quantum Analytic Langlands Correspondence | 88 pages | null | null | DESY-24-017 | hep-th math-ph math.AG math.MP nlin.SI | http://creativecommons.org/licenses/by/4.0/ | The analytic Langlands correspondence describes the solution to the spectral
problem for the quantised Hitchin Hamiltonians. It is related to the S-duality
of $\cal{N}=4$ super Yang-Mills theory. We propose a one-parameter deformation
of the Analytic Langlands Correspondence, and discuss its relations to quantum
fiel... | [
{
"created": "Thu, 1 Feb 2024 11:05:06 GMT",
"version": "v1"
}
] | 2024-02-02 | [
[
"Gaiotto",
"Davide",
""
],
[
"Teschner",
"Jörg",
""
]
] | The analytic Langlands correspondence describes the solution to the spectral problem for the quantised Hitchin Hamiltonians. It is related to the S-duality of $\cal{N}=4$ super Yang-Mills theory. We propose a one-parameter deformation of the Analytic Langlands Correspondence, and discuss its relations to quantum field ... | 10.343624 | 9.01317 | 12.064903 | 8.595237 | 10.04468 | 9.785951 | 8.944084 | 8.911939 | 9.770899 | 12.322609 | 9.095739 | 9.429486 | 10.15552 | 9.340742 | 9.349661 | 9.410055 | 9.541398 | 9.284011 | 9.703727 | 9.538082 | 9.055397 |
1608.04408 | Katy Clough Dr | Katy Clough, Eugene A. Lim, Brandon S. DiNunno, Willy Fischler,
Raphael Flauger, Sonia Paban | Robustness of Inflation to Inhomogeneous Initial Conditions | 14 pages, 14 figures, updated for journal version and amended sign
convention for chi | JCAP 1709 (2017) no.09, 025 | 10.1088/1475-7516/2017/09/025 | KCL-PH-TH/2016-53 | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the effects of inhomogeneous initial conditions in both the
scalar field profile and the extrinsic curvature on different inflationary
models. In particular, we compare the robustness of small field inflation to
that of large field inflation, using numerical simulations with Einstein
gravity in 3+1 dimens... | [
{
"created": "Mon, 15 Aug 2016 21:05:46 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Dec 2017 07:35:17 GMT",
"version": "v2"
}
] | 2017-12-21 | [
[
"Clough",
"Katy",
""
],
[
"Lim",
"Eugene A.",
""
],
[
"DiNunno",
"Brandon S.",
""
],
[
"Fischler",
"Willy",
""
],
[
"Flauger",
"Raphael",
""
],
[
"Paban",
"Sonia",
""
]
] | We consider the effects of inhomogeneous initial conditions in both the scalar field profile and the extrinsic curvature on different inflationary models. In particular, we compare the robustness of small field inflation to that of large field inflation, using numerical simulations with Einstein gravity in 3+1 dimensio... | 8.783152 | 10.179711 | 9.257103 | 9.166937 | 9.296049 | 9.960843 | 10.097762 | 9.415065 | 9.179252 | 9.370813 | 9.184098 | 8.878653 | 8.688344 | 8.649961 | 8.816709 | 8.831008 | 8.868635 | 8.92587 | 9.038132 | 8.907483 | 8.921482 |
hep-th/9903098 | Pankaj Sharan | Pankaj Sharan, Anupama Mehra, Krishnendu Dasgupta, M. Sami (Jamia
Millia Islamia, New Delhi, INDIA) | Gauge conditions for an Abelian Chern-Simons system consistent with
equations of motion | 9 pages, Latex. To appear in Nuovo Cimento | Nuovo Cim. B114 (1999) 861-871 | null | null | hep-th | null | Complete constraint analysis and choice of gauge conditions consistent with
equations of motion is done for Abelian Chern Simons field interacting
minimally with a complex scalar field. The Dirac-Schwinger consistency
condition is satisfied by the reduced phase space Hamiltonian density with
respect to the the Dirac ... | [
{
"created": "Thu, 11 Mar 1999 09:33:01 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Sharan",
"Pankaj",
"",
"Jamia\n Millia Islamia, New Delhi, INDIA"
],
[
"Mehra",
"Anupama",
"",
"Jamia\n Millia Islamia, New Delhi, INDIA"
],
[
"Dasgupta",
"Krishnendu",
"",
"Jamia\n Millia Islamia, New Delhi, INDIA"
],
[
"Sami",
"M.",
"",... | Complete constraint analysis and choice of gauge conditions consistent with equations of motion is done for Abelian Chern Simons field interacting minimally with a complex scalar field. The Dirac-Schwinger consistency condition is satisfied by the reduced phase space Hamiltonian density with respect to the the Dirac br... | 14.959986 | 11.317909 | 17.304527 | 11.782907 | 13.552835 | 13.073044 | 13.88206 | 11.699477 | 11.481637 | 16.97967 | 11.733245 | 11.977198 | 14.100358 | 12.735387 | 13.003332 | 12.738372 | 12.907982 | 12.296041 | 13.012671 | 14.599686 | 12.837274 |
2405.03683 | Ivano Basile | Christian Aoufia, Ivano Basile, Giorgio Leone | Species scale, worldsheet CFTs and emergent geometry | 35 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study infinite-distance limits in the moduli space of perturbative string
vacua. The remarkable interplay of string dualities seems to determine a highly
non-trivial dichotomy, summarized by the emergent string conjecture, by which
in some duality frame either internal dimensions decompactify or a unique
critical ... | [
{
"created": "Mon, 6 May 2024 17:57:06 GMT",
"version": "v1"
}
] | 2024-05-07 | [
[
"Aoufia",
"Christian",
""
],
[
"Basile",
"Ivano",
""
],
[
"Leone",
"Giorgio",
""
]
] | We study infinite-distance limits in the moduli space of perturbative string vacua. The remarkable interplay of string dualities seems to determine a highly non-trivial dichotomy, summarized by the emergent string conjecture, by which in some duality frame either internal dimensions decompactify or a unique critical st... | 14.154819 | 12.389706 | 17.101439 | 13.439244 | 13.296005 | 13.773343 | 12.984921 | 13.032027 | 12.688598 | 17.175816 | 13.869333 | 13.359159 | 14.40648 | 13.432693 | 13.441183 | 13.829558 | 13.374318 | 13.461843 | 12.590407 | 13.971869 | 13.203215 |
2007.04327 | Igor Broeckel | Igor Broeckel, Michele Cicoli, Anshuman Maharana, Kajal Singh, Kuver
Sinha | Moduli Stabilisation and the Statistics of SUSY Breaking in the
Landscape | 22 pages + appendices, 4 figures | null | 10.1007/JHEP10(2020)015 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The statistics of the supersymmetry breaking scale in the string landscape
has been extensively studied in the past finding either a power-law behaviour
induced by uniform distributions of F-terms or a logarithmic distribution
motivated by dynamical supersymmetry breaking. These studies focused mainly on
type IIB flu... | [
{
"created": "Wed, 8 Jul 2020 18:00:03 GMT",
"version": "v1"
}
] | 2020-10-28 | [
[
"Broeckel",
"Igor",
""
],
[
"Cicoli",
"Michele",
""
],
[
"Maharana",
"Anshuman",
""
],
[
"Singh",
"Kajal",
""
],
[
"Sinha",
"Kuver",
""
]
] | The statistics of the supersymmetry breaking scale in the string landscape has been extensively studied in the past finding either a power-law behaviour induced by uniform distributions of F-terms or a logarithmic distribution motivated by dynamical supersymmetry breaking. These studies focused mainly on type IIB flux ... | 5.447464 | 5.512182 | 5.581369 | 5.282504 | 5.610904 | 6.037422 | 6.089875 | 5.500877 | 5.155134 | 5.560034 | 5.216763 | 5.370197 | 5.326934 | 5.136049 | 5.374266 | 5.312354 | 5.247626 | 5.232476 | 5.165869 | 5.361916 | 5.090658 |
2407.09131 | D. Migu\'elez-Caballero | A. Alonso-Izquierdo, D. Migu\'elez-Caballero, L.M. Nieto | Scattering between orthogonally wobbling kinks | 20 pages, 11 figures | null | null | null | hep-th math-ph math.MP nlin.PS | http://creativecommons.org/licenses/by/4.0/ | The resonant energy transfer mechanism, responsible for the presence of
fractal patterns in the velocity diagrams of kink-antikink scattering, is
analyzed for a family of two-component scalar field theory models, in which the
kink solutions have two shape modes (one longitudinal and one orthogonal to the
kink orbit),... | [
{
"created": "Fri, 12 Jul 2024 09:58:26 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jul 2024 14:48:37 GMT",
"version": "v2"
}
] | 2024-07-17 | [
[
"Alonso-Izquierdo",
"A.",
""
],
[
"Miguélez-Caballero",
"D.",
""
],
[
"Nieto",
"L. M.",
""
]
] | The resonant energy transfer mechanism, responsible for the presence of fractal patterns in the velocity diagrams of kink-antikink scattering, is analyzed for a family of two-component scalar field theory models, in which the kink solutions have two shape modes (one longitudinal and one orthogonal to the kink orbit), i... | 12.516394 | 10.899757 | 11.706509 | 9.756938 | 11.24073 | 10.19966 | 10.670834 | 9.642779 | 10.082642 | 12.507689 | 10.551736 | 10.891973 | 11.125031 | 10.341755 | 10.958362 | 10.873231 | 10.931055 | 10.16759 | 10.839448 | 11.114012 | 10.549422 |
1905.11305 | Takuya Okuda | Hirotaka Hayashi, Takuya Okuda, and Yutaka Yoshida | Wall-crossing and operator ordering for 't Hooft operators in N=2 gauge
theories | 57 pages, many figures; comments added, statements clarified, typos
fixed, version in JHEP | null | 10.1007/JHEP11(2019)116 | UT-Komaba-19-2, IPMU19-0058 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study half-BPS 't Hooft line operators in 4d $\mathcal{N}=2$ $U(N)$ gauge
theories on $S^1\times \mathbb{R}^3$ with an $\Omega$-deformation. The recently
proposed brane construction of 't Hooft operators shows that non-perturbative
contributions to their correlator are identified with the Witten indices of
quiver ... | [
{
"created": "Mon, 27 May 2019 15:43:06 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Dec 2019 06:58:30 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Hayashi",
"Hirotaka",
""
],
[
"Okuda",
"Takuya",
""
],
[
"Yoshida",
"Yutaka",
""
]
] | We study half-BPS 't Hooft line operators in 4d $\mathcal{N}=2$ $U(N)$ gauge theories on $S^1\times \mathbb{R}^3$ with an $\Omega$-deformation. The recently proposed brane construction of 't Hooft operators shows that non-perturbative contributions to their correlator are identified with the Witten indices of quiver su... | 5.649919 | 4.861764 | 6.322295 | 5.067361 | 4.840494 | 4.91893 | 4.868577 | 4.939047 | 5.014683 | 6.909605 | 4.994973 | 5.130662 | 5.755103 | 5.247417 | 5.343223 | 5.074328 | 5.17082 | 5.093305 | 5.284745 | 5.543992 | 5.325882 |
1607.05919 | Jon Chkareuli | J.L. Chkareuli and Z. Kepuladze | Gauge Symmetries Emerging from Extra Dimensions | 24 pages, published version, to appear in Physical Review D (2016) | null | 10.1103/PhysRevD.94.065013 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that extra dimensions with a properly chosen compactification scheme
could be a natural source for emergent gauge symmetries. Actually, some
proposed vector field potential terms or polynomial vector field constraints
introduced in five-dimensional Abelian and non-Abelian gauge theory is shown to
smoothly le... | [
{
"created": "Wed, 20 Jul 2016 11:25:35 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Aug 2016 04:46:57 GMT",
"version": "v2"
},
{
"created": "Sun, 28 Aug 2016 13:52:32 GMT",
"version": "v3"
},
{
"created": "Wed, 7 Sep 2016 17:36:22 GMT",
"version": "v4"
}
] | 2016-12-21 | [
[
"Chkareuli",
"J. L.",
""
],
[
"Kepuladze",
"Z.",
""
]
] | We argue that extra dimensions with a properly chosen compactification scheme could be a natural source for emergent gauge symmetries. Actually, some proposed vector field potential terms or polynomial vector field constraints introduced in five-dimensional Abelian and non-Abelian gauge theory is shown to smoothly lead... | 14.142635 | 17.053995 | 14.870892 | 14.316071 | 16.737114 | 16.304241 | 16.618881 | 14.96586 | 14.504518 | 16.145672 | 14.77454 | 14.527326 | 13.913297 | 14.078993 | 14.596007 | 14.348225 | 14.83232 | 14.038339 | 13.888168 | 14.378113 | 14.157905 |
0706.4245 | Dmitri Kazakov | D. I. Kazakov and L. V. Bork | Conformal Invariance = Finiteness and Beta Deformed N=4 SYM Theory | 15 pages, Latex, 1 figure axodraw style | JHEP 0708:071,2007 | 10.1088/1126-6708/2007/08/071 | null | hep-th | null | We claim that if by a choice of the couplings the theory can be made
conformally invariant (vanishing of the beta functions) it is automatically
finite and vice versa. This is demonstrated by explicit example in
supersymmetric gauge theory. The formalism is then applied to the beta deformed
${\cal N}=4$ SYM theory an... | [
{
"created": "Thu, 28 Jun 2007 14:24:42 GMT",
"version": "v1"
}
] | 2009-04-30 | [
[
"Kazakov",
"D. I.",
""
],
[
"Bork",
"L. V.",
""
]
] | We claim that if by a choice of the couplings the theory can be made conformally invariant (vanishing of the beta functions) it is automatically finite and vice versa. This is demonstrated by explicit example in supersymmetric gauge theory. The formalism is then applied to the beta deformed ${\cal N}=4$ SYM theory and ... | 10.174237 | 9.995855 | 10.131397 | 9.177954 | 9.852528 | 9.950054 | 10.16182 | 9.344535 | 9.499789 | 10.964284 | 8.90957 | 9.300591 | 9.698469 | 9.32957 | 9.534113 | 9.869922 | 9.409344 | 9.541235 | 9.179744 | 9.777571 | 9.505918 |
0903.5242 | Anton Rebhan | Anton Rebhan, Andreas Schmitt, Peter van Nieuwenhuizen | One-loop results for kink and domain wall profiles at zero and finite
temperature | REVTEX4 24 pages, 4 figures. v3: minor rewordings in abstract and
introduction, consistency with previous results clarified, references added | Phys.Rev.D80:045012,2009 | 10.1103/PhysRevD.80.045012 | TUW-09-02, YITP-SB-09-03 | hep-th cond-mat.stat-mech hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using dimensional regularization, we compute the one-loop quantum and thermal
corrections to the profile of the bosonic 1+1-dimensional phi^4 kink, the
sine-Gordon kink and the CP^1 kink, and higher-dimensional phi^4 kink domain
walls. Starting from the Heisenberg field equation in the presence of the
nontrivial kink... | [
{
"created": "Mon, 30 Mar 2009 18:56:44 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Apr 2009 21:40:15 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Jul 2009 16:50:10 GMT",
"version": "v3"
}
] | 2009-09-02 | [
[
"Rebhan",
"Anton",
""
],
[
"Schmitt",
"Andreas",
""
],
[
"van Nieuwenhuizen",
"Peter",
""
]
] | Using dimensional regularization, we compute the one-loop quantum and thermal corrections to the profile of the bosonic 1+1-dimensional phi^4 kink, the sine-Gordon kink and the CP^1 kink, and higher-dimensional phi^4 kink domain walls. Starting from the Heisenberg field equation in the presence of the nontrivial kink b... | 11.18583 | 12.205959 | 11.620023 | 11.262775 | 11.97644 | 12.201238 | 12.561832 | 11.805285 | 12.145503 | 12.455321 | 11.882958 | 11.517169 | 11.487357 | 11.180271 | 11.505817 | 11.634789 | 11.16153 | 11.28629 | 11.261234 | 11.294665 | 11.453462 |
1806.02665 | Oliver Gould | Oliver Gould, Arttu Rajantie and Cheng Xie | Worldline sphaleron for thermal Schwinger pair production | 15 pages, 4 figures, published in PRD | Phys. Rev. D 98, 056022 (2018) | 10.1103/PhysRevD.98.056022 | IMPERIAL-TP-2018-OG-1, HIP-2018-17-TH | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | With increasing temperatures, Schwinger pair production changes from a
quantum tunnelling to a classical, thermal process, determined by a worldline
sphaleron. We show this and calculate the corresponding rate of pair production
for both spinor and scalar quantum electrodynamics, including the semiclassical
prefactor... | [
{
"created": "Thu, 7 Jun 2018 13:25:03 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Oct 2018 08:51:01 GMT",
"version": "v2"
}
] | 2018-10-10 | [
[
"Gould",
"Oliver",
""
],
[
"Rajantie",
"Arttu",
""
],
[
"Xie",
"Cheng",
""
]
] | With increasing temperatures, Schwinger pair production changes from a quantum tunnelling to a classical, thermal process, determined by a worldline sphaleron. We show this and calculate the corresponding rate of pair production for both spinor and scalar quantum electrodynamics, including the semiclassical prefactor. ... | 10.482827 | 10.831842 | 10.737959 | 8.944583 | 10.098516 | 10.493548 | 9.855573 | 10.1697 | 9.481165 | 10.982224 | 9.515378 | 9.742749 | 9.992805 | 9.688142 | 9.914913 | 9.640512 | 9.606342 | 9.428608 | 9.916443 | 10.311877 | 9.536695 |
hep-th/0210181 | Mariano Quiros | A. Delgado, G. v. Gersdorff and M. Quiros | Brane-assisted Scherk-Schwarz supersymmetry breaking in orbifolds | 12 pages, 5 figures | JHEP 0212:002,2002 | 10.1088/1126-6708/2002/12/002 | IEM-FT-228/02 | hep-th hep-ph | null | We have analyzed the interplay between Scherk-Schwarz supersymmetry breaking
and general fermion (gaugino or gravitino) mass terms localized on the fixed
point branes of the S^1/Z_2 orbifold. Analytic solutions for eigenfunctions and
eigenvalues are found in all cases. All results are checked by numerical
calculation... | [
{
"created": "Fri, 18 Oct 2002 16:04:18 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Delgado",
"A.",
""
],
[
"Gersdorff",
"G. v.",
""
],
[
"Quiros",
"M.",
""
]
] | We have analyzed the interplay between Scherk-Schwarz supersymmetry breaking and general fermion (gaugino or gravitino) mass terms localized on the fixed point branes of the S^1/Z_2 orbifold. Analytic solutions for eigenfunctions and eigenvalues are found in all cases. All results are checked by numerical calculations ... | 10.952488 | 10.23573 | 11.217961 | 9.91453 | 10.49155 | 10.999028 | 10.010074 | 10.645849 | 9.888088 | 11.68686 | 10.468408 | 10.134227 | 10.254393 | 10.177277 | 10.271322 | 10.131353 | 9.94222 | 9.982213 | 10.008644 | 10.323837 | 9.837203 |
1603.08524 | Ethan Dyer | Nathan Benjamin, Ethan Dyer, A. Liam Fitzpatrick, Alexander Maloney,
Eric Perlmutter | Small Black Holes and Near-Extremal CFTs | 41 pages + appendices, 6 figures | null | 10.1007/JHEP08(2016)023 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Pure theories of AdS$_3$ quantum gravity are conjectured to be dual to CFTs
with sparse spectra of light primary operators. The sparsest possible spectrum
consistent with modular invariance includes only black hole states above the
vacuum. Witten conjectured the existence of a family of extremal CFTs, which
realize t... | [
{
"created": "Mon, 28 Mar 2016 20:00:04 GMT",
"version": "v1"
}
] | 2016-08-24 | [
[
"Benjamin",
"Nathan",
""
],
[
"Dyer",
"Ethan",
""
],
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Maloney",
"Alexander",
""
],
[
"Perlmutter",
"Eric",
""
]
] | Pure theories of AdS$_3$ quantum gravity are conjectured to be dual to CFTs with sparse spectra of light primary operators. The sparsest possible spectrum consistent with modular invariance includes only black hole states above the vacuum. Witten conjectured the existence of a family of extremal CFTs, which realize thi... | 10.102029 | 9.638183 | 11.71369 | 9.215765 | 10.184666 | 10.327584 | 9.574607 | 9.480815 | 9.363489 | 13.300907 | 8.961697 | 9.567019 | 10.011134 | 9.620617 | 9.677914 | 9.796988 | 9.251812 | 9.477616 | 9.209827 | 10.098903 | 9.232685 |
0810.4909 | Gregory Moore | Daniel L. Jafferis and Gregory W. Moore | Wall crossing in local Calabi Yau manifolds | 20pp., 1 figure | null | null | RUNHETC-2008-22 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the BPS states of a D6-brane wrapping the conifold and bound to
collections of D2 and D0 branes. We find that in addition to the complexified
Kahler parameter of the rigid sphere it is necessary to introduce an extra real
parameter to describe BPS partition functions and marginal stability walls. The
supergr... | [
{
"created": "Mon, 27 Oct 2008 19:16:31 GMT",
"version": "v1"
}
] | 2008-10-28 | [
[
"Jafferis",
"Daniel L.",
""
],
[
"Moore",
"Gregory W.",
""
]
] | We study the BPS states of a D6-brane wrapping the conifold and bound to collections of D2 and D0 branes. We find that in addition to the complexified Kahler parameter of the rigid sphere it is necessary to introduce an extra real parameter to describe BPS partition functions and marginal stability walls. The supergrav... | 9.982447 | 9.682339 | 13.909813 | 9.442573 | 9.176361 | 9.331293 | 9.774338 | 9.810207 | 8.660184 | 14.643736 | 9.313886 | 9.592082 | 10.977663 | 9.573112 | 9.54936 | 9.034431 | 9.434249 | 9.621998 | 9.511558 | 11.696326 | 9.771817 |
2104.06584 | Christian Kunz | Christian Kunz | A Note on Classical Aspects of the Four Dimensional Anomaly-Free Twistor
String | 7 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The recently introduced anomaly-free twistor string in four dimensions is
shown to be defined not just in flat but also in curved twistor space. Further,
arguments are given that the classical limit of the corresponding string field
theory, if it exists, is related to general relativity, in particular to the
Isenberg... | [
{
"created": "Wed, 14 Apr 2021 02:11:22 GMT",
"version": "v1"
}
] | 2021-04-15 | [
[
"Kunz",
"Christian",
""
]
] | The recently introduced anomaly-free twistor string in four dimensions is shown to be defined not just in flat but also in curved twistor space. Further, arguments are given that the classical limit of the corresponding string field theory, if it exists, is related to general relativity, in particular to the Isenberg a... | 12.220239 | 14.014592 | 14.201728 | 12.527434 | 13.021584 | 12.751204 | 12.393192 | 13.216953 | 12.355379 | 15.475576 | 12.569448 | 11.607533 | 12.097448 | 12.099202 | 11.198741 | 11.808531 | 11.668306 | 11.627381 | 11.607139 | 12.677059 | 11.512132 |
1909.01169 | Jean-Luc Lehners | Jean-Luc Lehners and K.S. Stelle | A Safe Beginning for the Universe? | 15 pages plus references, 1 figure, v2: references added and typos
fixed | Phys. Rev. D 100, 083540 (2019) | 10.1103/PhysRevD.100.083540 | Imperial/TP/2019/KSS/02 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | When general relativity is augmented by quadratic gravity terms, it becomes a
renormalisable theory of gravity. This theory may admit a non-Gaussian fixed
point as envisaged in the asymptotic safety program, rendering the theory
trustworthy to energies up to the Planck scale and even beyond. We show that
requiring ph... | [
{
"created": "Tue, 3 Sep 2019 13:34:23 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Oct 2019 07:54:27 GMT",
"version": "v2"
}
] | 2019-11-06 | [
[
"Lehners",
"Jean-Luc",
""
],
[
"Stelle",
"K. S.",
""
]
] | When general relativity is augmented by quadratic gravity terms, it becomes a renormalisable theory of gravity. This theory may admit a non-Gaussian fixed point as envisaged in the asymptotic safety program, rendering the theory trustworthy to energies up to the Planck scale and even beyond. We show that requiring phys... | 11.233574 | 12.083858 | 11.056382 | 10.162807 | 11.276807 | 11.442607 | 11.409887 | 10.918737 | 10.881124 | 12.435061 | 11.836177 | 11.521508 | 10.866055 | 10.918408 | 10.95711 | 10.890245 | 11.031586 | 11.124646 | 11.014046 | 11.138813 | 10.746957 |
1011.0403 | Anton Gerasimov | Anton A. Gerasimov and Dimitri R. Lebedev | On topological field theory representation of higher analogs of
classical special functions | 21 pages, typos are fixed and important reference is added | JHEP 1109:076,2011 | 10.1007/JHEP09(2011)076 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Looking for a quantum field theory model of Archimedean algebraic geometry a
class of infinite-dimensional integral representations of classical special
functions was introduced. Precisely the special functions such as Whittaker
functions and Gamma-function were identified with correlation functions in
topological fi... | [
{
"created": "Mon, 1 Nov 2010 18:16:56 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jul 2011 17:18:51 GMT",
"version": "v2"
}
] | 2011-09-20 | [
[
"Gerasimov",
"Anton A.",
""
],
[
"Lebedev",
"Dimitri R.",
""
]
] | Looking for a quantum field theory model of Archimedean algebraic geometry a class of infinite-dimensional integral representations of classical special functions was introduced. Precisely the special functions such as Whittaker functions and Gamma-function were identified with correlation functions in topological fiel... | 12.40075 | 12.379694 | 14.174697 | 11.586311 | 12.108345 | 12.437813 | 12.504015 | 12.062157 | 11.063545 | 13.752536 | 11.34175 | 11.393474 | 11.549337 | 11.075451 | 11.561283 | 11.145151 | 11.541425 | 11.042564 | 11.013261 | 11.891163 | 11.385935 |
1410.4595 | Anastasia Golubtsova | I. Ya. Aref'eva, A. A. Golubtsova | Shock waves in Lifshitz-like spacetimes | 35 pages, 6 figures; v3: typos corrected. Version to appear in JHEP | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct shock waves for Lifshitz-like geometries in four- and
five-dimensional effective theories as well as in D3-D7 and D4-D6 brane
systems. The solutions to the domain wall profile equations are found. Further,
the study makes a connection with the implications for the quark-gluon plasma
formation in heavy-io... | [
{
"created": "Thu, 16 Oct 2014 21:56:22 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Nov 2014 20:00:07 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Mar 2015 16:25:41 GMT",
"version": "v3"
}
] | 2015-03-24 | [
[
"Aref'eva",
"I. Ya.",
""
],
[
"Golubtsova",
"A. A.",
""
]
] | We construct shock waves for Lifshitz-like geometries in four- and five-dimensional effective theories as well as in D3-D7 and D4-D6 brane systems. The solutions to the domain wall profile equations are found. Further, the study makes a connection with the implications for the quark-gluon plasma formation in heavy-ion ... | 8.159529 | 7.959909 | 9.00143 | 7.753108 | 8.047535 | 8.043317 | 8.421549 | 7.456889 | 7.594637 | 8.997014 | 7.739535 | 7.998164 | 8.20582 | 7.739558 | 7.811399 | 7.855441 | 7.921392 | 7.935218 | 7.901421 | 8.414244 | 7.683608 |
hep-th/9411096 | null | V. A. Tsokur, Yu. M. Zinoviev | Spontaneous supersymmetry breaking in N=3 supergravity with matter | 12 pages, plain LaTeX, no figures | Phys.Atom.Nucl. 59 (1996) 2185-2191; Yad.Fiz. 59N12 (1996)
1169-1176 | null | IHEP 94-114 | hep-th | null | In this paper we investigate the problem of spontaneous supersymmetry
breaking without a cosmological term in $N=3$ supergravity with matter vector
multiplets, scalar fields geometry being $SU(3,m)/SU(3)\otimes SU(m)\otimes
U(1)$. At first, we consider the case of minimal coupling with different
possible gaugings (co... | [
{
"created": "Mon, 14 Nov 1994 16:54:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Tsokur",
"V. A.",
""
],
[
"Zinoviev",
"Yu. M.",
""
]
] | In this paper we investigate the problem of spontaneous supersymmetry breaking without a cosmological term in $N=3$ supergravity with matter vector multiplets, scalar fields geometry being $SU(3,m)/SU(3)\otimes SU(m)\otimes U(1)$. At first, we consider the case of minimal coupling with different possible gaugings (comp... | 7.275346 | 6.502673 | 7.84021 | 6.648718 | 7.291526 | 6.697512 | 6.832149 | 6.664932 | 6.465123 | 8.157866 | 6.707622 | 6.521599 | 6.80826 | 6.570592 | 6.539612 | 6.556077 | 6.8022 | 6.669713 | 6.673432 | 6.799129 | 6.693199 |
1001.4356 | Chaiho Rim Prof | Alexander Belavin and Chaiho Rim | Bulk one-point function on disk in one-matrix model | 8 pages | Phys.Lett.B687:264-266,2010 | 10.1016/j.physletb.2010.03.020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider bulk correlation numbers on disk in one-matrix model. Using the
recently found so-called resonance transformation from the KdV to the Liouville
frame, we obtain an explicit expression for the bulk one-point function. The
result is consistent with the form of FZZ one-point function in the boundary
Liouvill... | [
{
"created": "Mon, 25 Jan 2010 09:48:30 GMT",
"version": "v1"
}
] | 2010-04-30 | [
[
"Belavin",
"Alexander",
""
],
[
"Rim",
"Chaiho",
""
]
] | We consider bulk correlation numbers on disk in one-matrix model. Using the recently found so-called resonance transformation from the KdV to the Liouville frame, we obtain an explicit expression for the bulk one-point function. The result is consistent with the form of FZZ one-point function in the boundary Liouville ... | 19.148643 | 14.218629 | 21.316942 | 13.469179 | 14.198577 | 13.732203 | 13.024341 | 14.217157 | 13.879028 | 22.413309 | 13.719986 | 15.265425 | 18.961191 | 16.151436 | 17.116287 | 17.002583 | 16.440502 | 15.946566 | 16.141203 | 17.474394 | 16.58197 |
1505.00854 | Kazuharu Bamba | Kazuharu Bamba, Sergei D. Odintsov and Petr V. Tretyakov | Inflation in a conformally-invariant two-scalar-field theory with an
extra $R^2$ term | 18 pages, 4 figures, version accepted for publication in European
Physical Journal C | null | null | FU-PCG-03, OCHA-PP-334 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore inflationary cosmology in a theory where there are two scalar
fields which non-minimally couple to the Ricci scalar and an additional $R^2$
term, which breaks the conformal invariance. Particularly, we investigate the
slow-roll inflation in the case of one dynamical scalar field and that of two
dynamical s... | [
{
"created": "Tue, 5 May 2015 01:16:45 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jul 2015 00:47:00 GMT",
"version": "v2"
}
] | 2015-07-10 | [
[
"Bamba",
"Kazuharu",
""
],
[
"Odintsov",
"Sergei D.",
""
],
[
"Tretyakov",
"Petr V.",
""
]
] | We explore inflationary cosmology in a theory where there are two scalar fields which non-minimally couple to the Ricci scalar and an additional $R^2$ term, which breaks the conformal invariance. Particularly, we investigate the slow-roll inflation in the case of one dynamical scalar field and that of two dynamical sca... | 6.979375 | 6.242027 | 6.244449 | 5.772497 | 6.433076 | 6.297703 | 6.322539 | 5.831403 | 6.299871 | 6.810919 | 6.166087 | 6.761224 | 6.670238 | 6.510087 | 6.526026 | 6.513263 | 6.568244 | 6.378434 | 6.553648 | 6.325458 | 6.695173 |
hep-th/0311142 | Soumitra SenGupta | Debaprasad Maity and Soumitra SenGupta | Cosmic Optical Activity in a Randall-Sundrum Braneworld with Bulk
Kalb-Ramond field | 12 Pages, Latex, No figures,Version revised thoroughly, Accepted for
publication in Classical and Quantum Gravity | Class.Quant.Grav.21:3379-3387,2004 | 10.1088/0264-9381/21/14/004 | null | hep-th astro-ph gr-qc | null | Optical activity of electromagnetic waves in a string inspired Kalb-Ramond
cosmological background is studied in presence of extra spacetime dimension.
The Kalb-Ramond-electromagnetic coupling which originates from the gauge
anomaly cancelling Chern-Simons term in a string inspired model, is explicitly
calculated fol... | [
{
"created": "Mon, 17 Nov 2003 09:14:32 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jan 2004 08:59:53 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Jun 2004 12:41:54 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Maity",
"Debaprasad",
""
],
[
"SenGupta",
"Soumitra",
""
]
] | Optical activity of electromagnetic waves in a string inspired Kalb-Ramond cosmological background is studied in presence of extra spacetime dimension. The Kalb-Ramond-electromagnetic coupling which originates from the gauge anomaly cancelling Chern-Simons term in a string inspired model, is explicitly calculated follo... | 10.646386 | 9.937146 | 9.900679 | 9.422125 | 9.231065 | 10.260032 | 10.043171 | 9.517783 | 9.548186 | 11.417473 | 9.276409 | 9.383141 | 9.993553 | 9.358443 | 9.356606 | 9.33701 | 9.427707 | 9.268784 | 9.769767 | 9.48163 | 9.513021 |
1908.03574 | G\'abor S\'arosi | M\'ark Mezei and G\'abor S\'arosi | Chaos in the butterfly cone | 35 pages, 15 figures. v2: published version | null | 10.1007/JHEP01(2020)186 | null | hep-th cond-mat.stat-mech cond-mat.str-el nlin.CD quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A simple probe of chaos and operator growth in many-body quantum systems is
the out of time ordered four point function. In a large class of local systems,
the effects of chaos in this correlator build up exponentially fast inside the
so called butterfly cone. It has been previously observed that the growth of
these ... | [
{
"created": "Fri, 9 Aug 2019 18:00:00 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Feb 2020 01:04:37 GMT",
"version": "v2"
}
] | 2020-02-19 | [
[
"Mezei",
"Márk",
""
],
[
"Sárosi",
"Gábor",
""
]
] | A simple probe of chaos and operator growth in many-body quantum systems is the out of time ordered four point function. In a large class of local systems, the effects of chaos in this correlator build up exponentially fast inside the so called butterfly cone. It has been previously observed that the growth of these ef... | 6.598678 | 7.251944 | 7.438983 | 6.609325 | 7.079695 | 7.238512 | 6.982319 | 6.488117 | 6.734046 | 7.69912 | 6.526134 | 6.337122 | 6.672458 | 6.417192 | 6.539631 | 6.401753 | 6.434702 | 6.424556 | 6.329663 | 6.620966 | 6.278532 |
1602.07476 | Gor Sarkissian | Hasmik Poghosyan and Gor Sarkissian | Comments on fusion matrix in N=1 super Liouville field theory | 28 pages, comment and reference added | Nucl.Phys.B 909 (2016) 458-479 | 10.1016/j.nuclphysb.2016.05.023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study several aspects of the $N=1$ super Liouville theory. We show that
certain elements of the fusion matrix in the Neveu-Schwarz sector related to
the structure constants according to the same rules which we observe in
rational conformal field theory. We collect some evidences that these relations
should hold al... | [
{
"created": "Wed, 24 Feb 2016 12:21:23 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Mar 2016 10:11:46 GMT",
"version": "v2"
}
] | 2023-04-11 | [
[
"Poghosyan",
"Hasmik",
""
],
[
"Sarkissian",
"Gor",
""
]
] | We study several aspects of the $N=1$ super Liouville theory. We show that certain elements of the fusion matrix in the Neveu-Schwarz sector related to the structure constants according to the same rules which we observe in rational conformal field theory. We collect some evidences that these relations should hold also... | 12.796202 | 11.089738 | 14.476327 | 10.062393 | 11.012644 | 10.436584 | 11.558731 | 11.448305 | 10.623794 | 15.392066 | 10.824203 | 11.784024 | 13.861218 | 11.992473 | 12.152446 | 12.263751 | 12.011152 | 11.873528 | 12.094446 | 12.972775 | 12.021828 |
1506.00663 | Martin Luu | Martin Luu | Local Langlands Duality and a Duality of Conformal Field Theories | null | Communications in Number Theory and Phys. 10 (2016), 1-22 | 10.1016/j.cnsns.2004.04.004 | null | hep-th math-ph math.MP math.NT math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the numerical local Langlands duality for GL_n and the T -
duality of two-dimensional quantum gravity arise from one and the same symmetry
principle. The unifying theme is that the local Fourier transform in both its
l-adic and complex incarnation gives rise to symmetries of arithmetic and
geometric loca... | [
{
"created": "Mon, 1 Jun 2015 20:21:01 GMT",
"version": "v1"
}
] | 2019-09-11 | [
[
"Luu",
"Martin",
""
]
] | We show that the numerical local Langlands duality for GL_n and the T - duality of two-dimensional quantum gravity arise from one and the same symmetry principle. The unifying theme is that the local Fourier transform in both its l-adic and complex incarnation gives rise to symmetries of arithmetic and geometric local ... | 21.008108 | 24.854237 | 22.477407 | 23.049473 | 23.722202 | 24.319952 | 27.539232 | 21.897551 | 22.256651 | 28.920883 | 20.041668 | 21.160727 | 23.188198 | 19.488338 | 20.215034 | 19.583813 | 21.369839 | 18.936131 | 21.265854 | 23.104019 | 20.263212 |
hep-th/0604017 | David Kutasov | E. Antonyan, J.A. Harvey, S. Jensen and D. Kutasov | NJL and QCD from String Theory | 31 pages, harvmac | null | null | EFI-06-05 | hep-th | null | We study a configuration of D-branes in string theory that is described at
low energies by a four-dimensional field theory with a dynamically broken
chiral symmetry. In a certain region of the parameter space of the brane
configuration the low-energy theory is a non-local generalization of the
Nambu-Jona-Lasinio (NJL... | [
{
"created": "Mon, 3 Apr 2006 20:16:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Antonyan",
"E.",
""
],
[
"Harvey",
"J. A.",
""
],
[
"Jensen",
"S.",
""
],
[
"Kutasov",
"D.",
""
]
] | We study a configuration of D-branes in string theory that is described at low energies by a four-dimensional field theory with a dynamically broken chiral symmetry. In a certain region of the parameter space of the brane configuration the low-energy theory is a non-local generalization of the Nambu-Jona-Lasinio (NJL) ... | 5.52108 | 5.252399 | 5.671328 | 5.266656 | 5.421648 | 5.230137 | 5.157369 | 5.192964 | 5.164413 | 6.751947 | 5.142028 | 5.174363 | 5.533447 | 5.292048 | 5.322325 | 5.321223 | 5.214254 | 5.207787 | 5.326354 | 5.700836 | 5.184127 |
1605.04670 | Robert Brandenberger | W. S. Hipolito-Ricaldi, Robert Brandenberger, Elisa G.M. Ferreira, L.
L. Graef | Particle Production in Ekpyrotic Scenarios | 8 pages | null | 10.1088/1475-7516/2016/11/024 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Parker particle production in the Ekpyrotic scenario (in
particular in the New Ekpyrotic model) and show that the density of particles
produced by the end of the phase of Ekpyrotic contraction is sufficient to lead
to a hot state of matter after the bounce. Hence, no separate reheating
mechanism is necess... | [
{
"created": "Mon, 16 May 2016 07:31:27 GMT",
"version": "v1"
}
] | 2016-11-15 | [
[
"Hipolito-Ricaldi",
"W. S.",
""
],
[
"Brandenberger",
"Robert",
""
],
[
"Ferreira",
"Elisa G. M.",
""
],
[
"Graef",
"L. L.",
""
]
] | We consider Parker particle production in the Ekpyrotic scenario (in particular in the New Ekpyrotic model) and show that the density of particles produced by the end of the phase of Ekpyrotic contraction is sufficient to lead to a hot state of matter after the bounce. Hence, no separate reheating mechanism is necessar... | 9.045585 | 8.948748 | 7.146307 | 6.571274 | 7.844054 | 6.997229 | 7.55633 | 7.322418 | 7.108418 | 6.895855 | 7.820785 | 7.536672 | 7.143373 | 6.865729 | 7.082584 | 7.487473 | 7.416399 | 7.067523 | 7.417039 | 7.173199 | 7.34322 |
1404.6495 | J\'er\^ome Gleyzes | J\'er\^ome Gleyzes, David Langlois, Federico Piazza and Filippo
Vernizzi | Healthy theories beyond Horndeski | 5 pages, version accepted in PRL | Phys. Rev. Lett. 114, 211101 (2015) | 10.1103/PhysRevLett.114.211101 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a new class of scalar-tensor theories that extend Horndeski, or
"generalized galileon", models. Despite possessing equations of motion of
higher order in derivatives, we show that the true propagating degrees of
freedom obey well-behaved second-order equations and are thus free from
Ostrogradski instabil... | [
{
"created": "Fri, 25 Apr 2014 18:18:21 GMT",
"version": "v1"
},
{
"created": "Mon, 12 May 2014 15:33:22 GMT",
"version": "v2"
},
{
"created": "Tue, 19 May 2015 18:27:28 GMT",
"version": "v3"
}
] | 2015-06-03 | [
[
"Gleyzes",
"Jérôme",
""
],
[
"Langlois",
"David",
""
],
[
"Piazza",
"Federico",
""
],
[
"Vernizzi",
"Filippo",
""
]
] | We introduce a new class of scalar-tensor theories that extend Horndeski, or "generalized galileon", models. Despite possessing equations of motion of higher order in derivatives, we show that the true propagating degrees of freedom obey well-behaved second-order equations and are thus free from Ostrogradski instabilit... | 6.477992 | 7.247748 | 7.298418 | 6.890821 | 8.257673 | 7.649407 | 7.363167 | 6.979978 | 6.867563 | 7.126835 | 6.56969 | 6.774925 | 6.395636 | 6.476352 | 6.958234 | 6.620916 | 6.506876 | 6.663385 | 6.332232 | 6.639945 | 6.42437 |
hep-th/9211002 | null | Toshiki Isse | Unification of Gravity, Gauge and Higgs Fields by Confined Quantum
Fields-Mathematical Formulation- | 17 pages | Mod.Phys.Lett. A8 (1993) 837-850 | 10.1142/S0217732393000878 | null | hep-th | null | Dynamics of quantized free fields ( of spin 0 and 1/2 ) contained in a
subspace $V_*$ of an N+4 dimensional flat space $V$ is studied. The space $V_*$
is considered as a neighborhood of a four dimensional submanifold $M$
arbitrarily embedded into $V$. We study the system as a simple model of unified
theory of gravity... | [
{
"created": "Mon, 2 Nov 1992 09:39:17 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Isse",
"Toshiki",
""
]
] | Dynamics of quantized free fields ( of spin 0 and 1/2 ) contained in a subspace $V_*$ of an N+4 dimensional flat space $V$ is studied. The space $V_*$ is considered as a neighborhood of a four dimensional submanifold $M$ arbitrarily embedded into $V$. We study the system as a simple model of unified theory of gravity (... | 9.096859 | 6.758814 | 7.971787 | 7.593468 | 7.466379 | 7.337255 | 7.725883 | 7.811513 | 7.682659 | 8.993741 | 7.8544 | 7.732475 | 8.074208 | 7.938298 | 7.870571 | 7.848608 | 7.979878 | 7.926174 | 8.009413 | 8.070773 | 8.117399 |
hep-th/9505015 | Winfried Pfister | Winfried Pfister | Mixed Symmetry Solutions of Generalized Three-Particle Bargmann-Wigner
Equations in the Strong-Coupling Limit | 17 pages | NuovoCim.A108:1427-1444,1995 | 10.1007/BF02821059 | Tue-prep-95-05-2 | hep-th | null | Starting from a nonlinear isospinor-spinor field equation, generalized
three-particle Bargmann-Wigner equations are derived. In the strong-coupling
limit, a special class of spin 1/2 bound-states are calculated. These solutions
which are antisymmetric with respect to all indices, have mixed symmetries in
isospin-supe... | [
{
"created": "Tue, 2 May 1995 14:33:31 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Pfister",
"Winfried",
""
]
] | Starting from a nonlinear isospinor-spinor field equation, generalized three-particle Bargmann-Wigner equations are derived. In the strong-coupling limit, a special class of spin 1/2 bound-states are calculated. These solutions which are antisymmetric with respect to all indices, have mixed symmetries in isospin-supers... | 12.759938 | 13.335893 | 13.532936 | 12.212782 | 13.360604 | 12.316535 | 12.819921 | 12.656698 | 12.449072 | 14.976791 | 12.567892 | 11.993879 | 12.031651 | 12.132204 | 12.044268 | 12.348658 | 11.572674 | 11.468537 | 11.487954 | 11.89992 | 11.669644 |
hep-th/9702014 | Kutasov David | S. Elitzur, A. Giveon, D. Kutasov | Branes and N=1 Duality in String Theory | 8 pages, harvmac; minor changes, additional references | Phys.Lett. B400 (1997) 269-274 | 10.1016/S0370-2693(97)00375-4 | null | hep-th | null | We propose a construction of dual pairs in four dimensional N=1
supersymmetric Yang-Mills theory using branes in type IIA string theory.
| [
{
"created": "Sun, 2 Feb 1997 22:13:00 GMT",
"version": "v1"
},
{
"created": "Sun, 9 Feb 1997 21:50:30 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Elitzur",
"S.",
""
],
[
"Giveon",
"A.",
""
],
[
"Kutasov",
"D.",
""
]
] | We propose a construction of dual pairs in four dimensional N=1 supersymmetric Yang-Mills theory using branes in type IIA string theory. | 8.580479 | 4.831196 | 8.105719 | 4.875018 | 5.255254 | 4.702966 | 5.044535 | 5.007179 | 5.097622 | 7.542059 | 5.145513 | 6.101025 | 7.767147 | 6.082837 | 5.995804 | 6.287756 | 5.89002 | 6.342579 | 6.164663 | 7.330359 | 6.26187 |
1104.4446 | Klaus Bering | Klaus Bering | A Note on Angular Momentum Commutators in Light-Cone Formulation of Open
Bosonic String Theory | 11 pages, LaTeX. v2: Various pedagogical improvements | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We recalculate in a systematic and pedagogical way one of the most important
results of Bosonic open string theory in the light-cone formulation, namely the
[J^{-i},J^{-j}] commutators, which together with Lorentz covariance, famously
yield the critical dimension D=26 and the normal order constant a=1. We use
traditi... | [
{
"created": "Fri, 22 Apr 2011 14:20:53 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Feb 2012 19:50:25 GMT",
"version": "v2"
}
] | 2012-02-29 | [
[
"Bering",
"Klaus",
""
]
] | We recalculate in a systematic and pedagogical way one of the most important results of Bosonic open string theory in the light-cone formulation, namely the [J^{-i},J^{-j}] commutators, which together with Lorentz covariance, famously yield the critical dimension D=26 and the normal order constant a=1. We use tradition... | 18.189068 | 18.765594 | 19.245455 | 14.26595 | 17.528362 | 16.122953 | 16.457653 | 15.057177 | 13.994218 | 21.249882 | 14.688244 | 15.640093 | 17.571808 | 15.8054 | 15.447682 | 15.891207 | 15.879341 | 15.1003 | 15.71909 | 16.901794 | 15.442052 |
hep-th/0201192 | Osman Teoman Turgut | E. Toprak (1), O. T. Turgut (1 and 2) ((1) Bogazici University,
Istanbul and (2) KTH, Stockholm) | Large N limit of SO(N) gauge theory of fermions and bosons | 27 pages, no figures | J.Math.Phys. 43 (2002) 3074-3096 | 10.1063/1.1467097 | null | hep-th | null | In this paper we study the large N_c limit of SO(N_c) gauge theory coupled to
a Majorana field and a real scalar field in 1+1 dimensions extending ideas of
Rajeev. We show that the phase space of the resulting classical theory of
bilinears, which are the mesonic operators of this theory, is OSp_1(H|H
)/U(H_+|H_+), wh... | [
{
"created": "Thu, 24 Jan 2002 13:48:31 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Toprak",
"E.",
"",
"1 and 2"
],
[
"Turgut",
"O. T.",
"",
"1 and 2"
]
] | In this paper we study the large N_c limit of SO(N_c) gauge theory coupled to a Majorana field and a real scalar field in 1+1 dimensions extending ideas of Rajeev. We show that the phase space of the resulting classical theory of bilinears, which are the mesonic operators of this theory, is OSp_1(H|H )/U(H_+|H_+), wher... | 9.038592 | 8.987664 | 8.96806 | 8.639716 | 9.253566 | 9.334974 | 8.462416 | 7.99377 | 8.357291 | 9.670362 | 8.364687 | 8.45677 | 8.513648 | 8.367278 | 8.83919 | 8.655934 | 8.732109 | 8.489409 | 8.414468 | 8.577776 | 8.478871 |
1402.5027 | Jeong-Hyuck Park | Jeong-Hyuck Park and Yoonji Suh | U-gravity : ${\mathbf{SL}(N)}$ | 1+36 pages. Comments added. To appear in JHEP | JHEP 1406 (2014) 102 | 10.1007/JHEP06(2014)102 | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a duality manifest gravitational theory for the special linear
group, ${\mathbf{SL}(N)}$ with $N{\neq 4}$. The spacetime is formally extended,
to have the dimension $\textstyle{\frac{1}{2}} N(N-1)$, yet is `gauged'.
Consequently the theory is subject to a section condition. We introduce a
semi-covariant ... | [
{
"created": "Thu, 20 Feb 2014 15:19:52 GMT",
"version": "v1"
},
{
"created": "Tue, 27 May 2014 08:50:21 GMT",
"version": "v2"
}
] | 2014-07-08 | [
[
"Park",
"Jeong-Hyuck",
""
],
[
"Suh",
"Yoonji",
""
]
] | We construct a duality manifest gravitational theory for the special linear group, ${\mathbf{SL}(N)}$ with $N{\neq 4}$. The spacetime is formally extended, to have the dimension $\textstyle{\frac{1}{2}} N(N-1)$, yet is `gauged'. Consequently the theory is subject to a section condition. We introduce a semi-covariant de... | 8.557132 | 8.462978 | 9.327023 | 8.943912 | 9.201435 | 9.417436 | 9.1624 | 9.01832 | 8.829578 | 10.243631 | 8.344463 | 8.388239 | 8.87501 | 8.454085 | 8.603922 | 8.484034 | 8.765619 | 8.397309 | 8.399784 | 8.715603 | 8.218274 |
1707.04217 | Andrew Bond | Andrew D. Bond, Daniel F. Litim | More asymptotic safety guaranteed | 62 pages, 16 figures, 9 tables. v2: References added, minor typos
corrected; version accepted for publication in PRD | Phys. Rev. D 97, 085008 (2018) | 10.1103/PhysRevD.97.085008 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study interacting fixed points and phase diagrams of simple and
semi-simple quantum field theories in four dimensions involving non-abelian
gauge fields, fermions and scalars in the Veneziano limit. Particular emphasis
is put on new phenomena which arise due to the semisimple nature of the theory.
Using matter fie... | [
{
"created": "Thu, 13 Jul 2017 16:42:50 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Mar 2018 14:14:20 GMT",
"version": "v2"
}
] | 2018-04-18 | [
[
"Bond",
"Andrew D.",
""
],
[
"Litim",
"Daniel F.",
""
]
] | We study interacting fixed points and phase diagrams of simple and semi-simple quantum field theories in four dimensions involving non-abelian gauge fields, fermions and scalars in the Veneziano limit. Particular emphasis is put on new phenomena which arise due to the semisimple nature of the theory. Using matter field... | 9.49151 | 9.793303 | 10.62929 | 9.112168 | 9.810845 | 10.146537 | 10.543478 | 9.5954 | 9.363419 | 11.478944 | 9.333726 | 9.579736 | 9.534744 | 9.067802 | 9.368045 | 9.402699 | 9.568099 | 9.274635 | 9.248491 | 9.217727 | 9.028572 |
1012.2717 | Antonio Accioly | Antonio Accioly, Jos\'e Helay\"el-Neto, and Eslley Scatena | Upper bounds on the photon mass | null | Phys.Rev.D82:065026,2010 | 10.1103/PhysRevD.82.065026 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/3.0/ | The effects of a nonzero photon rest mass can be incorporated into
electromagnetism in a simple way using the Proca equations. In this vein, two
interesting implications regarding the possible existence of a massive photon
in nature, i.e., tiny alterations in the known values of both the anomalous
magnetic moment of ... | [
{
"created": "Mon, 13 Dec 2010 13:02:31 GMT",
"version": "v1"
}
] | 2016-08-14 | [
[
"Accioly",
"Antonio",
""
],
[
"Helayël-Neto",
"José",
""
],
[
"Scatena",
"Eslley",
""
]
] | The effects of a nonzero photon rest mass can be incorporated into electromagnetism in a simple way using the Proca equations. In this vein, two interesting implications regarding the possible existence of a massive photon in nature, i.e., tiny alterations in the known values of both the anomalous magnetic moment of th... | 11.507351 | 14.032941 | 11.235717 | 10.520938 | 11.488437 | 11.541908 | 11.33222 | 11.560487 | 11.41989 | 11.939596 | 12.705881 | 11.660333 | 11.125258 | 11.173399 | 11.186847 | 11.43385 | 11.299443 | 10.851128 | 11.327171 | 11.183374 | 11.52185 |
0911.0082 | David Dudal | D. Dudal, N. Vandersickel, H. Verschelde, S.P. Sorella | Aspects of the Gribov-Zwanziger framework | 12 pages, proceeding for the International Workshop on QCD Green's
Functions, Confinement, and Phenomenology (QCD-TNT09) | PoS QCD-TNT09:012,2009 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The existence of gauge (Gribov) copies disturbs the usual Faddeev-Popov
quantization procedure in the Landau gauge. It is a very hard job to treat
these in the continuum, even in a partial manner. A decent way to do so was
worked out by Gribov, and later on by Zwanziger. The final point was a
renormalizable action (t... | [
{
"created": "Sat, 31 Oct 2009 14:22:53 GMT",
"version": "v1"
}
] | 2011-07-14 | [
[
"Dudal",
"D.",
""
],
[
"Vandersickel",
"N.",
""
],
[
"Verschelde",
"H.",
""
],
[
"Sorella",
"S. P.",
""
]
] | The existence of gauge (Gribov) copies disturbs the usual Faddeev-Popov quantization procedure in the Landau gauge. It is a very hard job to treat these in the continuum, even in a partial manner. A decent way to do so was worked out by Gribov, and later on by Zwanziger. The final point was a renormalizable action (the... | 7.014603 | 7.059721 | 7.840606 | 7.133701 | 7.801457 | 7.503883 | 7.715943 | 7.225454 | 7.222878 | 8.273938 | 7.100247 | 7.045019 | 7.102051 | 6.885003 | 7.095713 | 7.18723 | 7.146413 | 6.966515 | 6.911095 | 7.160669 | 6.926491 |
hep-th/0105316 | null | Sergiu I. Vacaru and Florian Catalin Popa | Dirac Spinor Waves and Solitons in Anisotropic Taub-NUT Spaces | revtex, 16 pages, version 4, affiliation changed, accepted to CQG | Class.Quant.Grav. 18 (2001) 4921-4938 | 10.1088/0264-9381/18/22/314 | null | hep-th gr-qc math-ph math.MP | null | We apply a new general method of anholonomic frames with associated nonlinear
connection structure to construct new classes of exact solutions of
Einstein-Dirac equations in five dimensional (5D)gravity. Such solutions are
parametrized by off-diagonal metrics in coordinate (holonomic) bases, or,
equivalently, by diag... | [
{
"created": "Thu, 31 May 2001 13:48:41 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jun 2001 09:24:11 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Oct 2001 18:44:50 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Vacaru",
"Sergiu I.",
""
],
[
"Popa",
"Florian Catalin",
""
]
] | We apply a new general method of anholonomic frames with associated nonlinear connection structure to construct new classes of exact solutions of Einstein-Dirac equations in five dimensional (5D)gravity. Such solutions are parametrized by off-diagonal metrics in coordinate (holonomic) bases, or, equivalently, by diagon... | 12.589896 | 14.068612 | 12.901529 | 12.019371 | 13.697519 | 13.412631 | 13.870855 | 12.262953 | 12.39313 | 14.763145 | 13.109784 | 12.75325 | 12.313585 | 11.938592 | 12.559625 | 12.709944 | 12.87189 | 12.329551 | 13.172285 | 12.630493 | 12.445638 |
1904.08876 | Manya Sahni Miss | Rajesh Kumar Gupta, Sameer Murthy, Manya Sahni | On the localization manifold of 5d supersymmetric spinning black holes | null | null | 10.1007/JHEP10(2019)172 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the localization equations relevant to the quantum entropy of
spinning supersymmetric black holes in five-dimensional asymptotically flat
space. The precise problem is to classify all solutions to the off-shell
supersymmetry equations in N=2 supergravity coupled to $n_\text{v}+1$ vector
multiplets around t... | [
{
"created": "Thu, 18 Apr 2019 16:30:17 GMT",
"version": "v1"
}
] | 2020-01-08 | [
[
"Gupta",
"Rajesh Kumar",
""
],
[
"Murthy",
"Sameer",
""
],
[
"Sahni",
"Manya",
""
]
] | We analyze the localization equations relevant to the quantum entropy of spinning supersymmetric black holes in five-dimensional asymptotically flat space. The precise problem is to classify all solutions to the off-shell supersymmetry equations in N=2 supergravity coupled to $n_\text{v}+1$ vector multiplets around the... | 8.337342 | 7.750327 | 9.145034 | 7.448575 | 7.236498 | 7.707236 | 7.433204 | 7.538142 | 7.608564 | 9.335779 | 7.475194 | 7.274677 | 7.888839 | 7.335559 | 7.300707 | 7.309043 | 7.242906 | 7.386704 | 7.180795 | 8.489661 | 7.138564 |
1707.07702 | Thomas Hertog | S. W. Hawking and Thomas Hertog | A Smooth Exit from Eternal Inflation? | 15 pages; v2: added explicit calculation of higher-spin toy-model;
v3: minor changes to provide more context, references added, version accepted
for publication in JHEP | null | 10.1007/JHEP04(2018)147 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The usual theory of inflation breaks down in eternal inflation. We derive a
dual description of eternal inflation in terms of a deformed Euclidean CFT
located at the threshold of eternal inflation. The partition function gives the
amplitude of different geometries of the threshold surface in the no-boundary
state. It... | [
{
"created": "Mon, 24 Jul 2017 18:15:04 GMT",
"version": "v1"
},
{
"created": "Sun, 4 Mar 2018 10:11:05 GMT",
"version": "v2"
},
{
"created": "Fri, 20 Apr 2018 14:46:19 GMT",
"version": "v3"
}
] | 2018-05-23 | [
[
"Hawking",
"S. W.",
""
],
[
"Hertog",
"Thomas",
""
]
] | The usual theory of inflation breaks down in eternal inflation. We derive a dual description of eternal inflation in terms of a deformed Euclidean CFT located at the threshold of eternal inflation. The partition function gives the amplitude of different geometries of the threshold surface in the no-boundary state. Its ... | 11.46994 | 13.120427 | 13.148432 | 12.232325 | 12.14393 | 14.733897 | 13.026853 | 12.486374 | 13.251761 | 14.226092 | 12.805561 | 12.935147 | 12.284769 | 11.58498 | 12.363267 | 12.579977 | 12.245064 | 11.648272 | 11.572221 | 11.900591 | 12.154858 |
2401.07905 | Jani Kastikainen | Niko Jokela, Jani Kastikainen, Jos\'e Manuel Pen\'in, Helime
Ruotsalainen | Flavors of entanglement | 69 pages, 3 figures, 5 appendices | null | null | HIP-2024-2/TH | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We employ holography to investigate Liu-Mezei renormalization group monotones
in conformal field theories influenced by massive flavor degrees of freedom. We
examine the entanglement entropy of a spherical subregion in three holographic
field theories - $\mathcal{N}=1$ Klebanov-Witten theory, $\mathcal{N}=4$ SYM
theo... | [
{
"created": "Mon, 15 Jan 2024 19:00:01 GMT",
"version": "v1"
}
] | 2024-01-17 | [
[
"Jokela",
"Niko",
""
],
[
"Kastikainen",
"Jani",
""
],
[
"Penín",
"José Manuel",
""
],
[
"Ruotsalainen",
"Helime",
""
]
] | We employ holography to investigate Liu-Mezei renormalization group monotones in conformal field theories influenced by massive flavor degrees of freedom. We examine the entanglement entropy of a spherical subregion in three holographic field theories - $\mathcal{N}=1$ Klebanov-Witten theory, $\mathcal{N}=4$ SYM theory... | 9.570111 | 9.204906 | 11.011312 | 8.505709 | 9.457696 | 8.401841 | 9.04274 | 9.440279 | 9.082773 | 11.946257 | 8.995275 | 9.236213 | 10.208179 | 8.948312 | 8.816452 | 8.925283 | 9.045049 | 9.257062 | 9.349815 | 9.959658 | 9.112166 |
2407.02565 | Xin Gao | Xu Cao, Hongfei Gao, and Xin Gao | Orientifold Calabi-Yau Threefolds: Divisor Exchanges and
Multi-Reflections | 55 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the Kreuzer-Skarke database of 4-dimensional reflexive polytopes, we
systematically constructed a new database of orientifold Calabi-Yau threefolds
with $h^{1,1}(X) \leq 12$. Our approach involved non-trivial $\mathbb{Z}_2$
involutions, incorporating both divisor exchanges and multi-divisor reflections
acting o... | [
{
"created": "Tue, 2 Jul 2024 18:00:02 GMT",
"version": "v1"
}
] | 2024-07-04 | [
[
"Cao",
"Xu",
""
],
[
"Gao",
"Hongfei",
""
],
[
"Gao",
"Xin",
""
]
] | Using the Kreuzer-Skarke database of 4-dimensional reflexive polytopes, we systematically constructed a new database of orientifold Calabi-Yau threefolds with $h^{1,1}(X) \leq 12$. Our approach involved non-trivial $\mathbb{Z}_2$ involutions, incorporating both divisor exchanges and multi-divisor reflections acting on ... | 9.607929 | 10.167804 | 11.539474 | 9.430006 | 9.847333 | 9.654813 | 9.464752 | 9.132959 | 9.450091 | 13.389126 | 9.006104 | 9.171689 | 9.720078 | 9.263961 | 9.513476 | 9.46834 | 9.642167 | 9.165647 | 9.281466 | 10.322705 | 9.221855 |
1104.2692 | Kazuharu Bamba | Kazuharu Bamba, Shin'ichi Nojiri, Sergei D. Odintsov and Misao Sasaki | Screening of cosmological constant for De Sitter Universe in non-local
gravity, phantom-divide crossing and finite-time future singularities | 42 pages, no figure, version accepted for publication in General
Relativity and Gravitation | null | 10.1007/s10714-012-1342-7 | YITP-11-46 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate de Sitter solutions in non-local gravity as well as in
non-local gravity with Lagrange constraint multiplier. We examine a condition
to avoid a ghost and discuss a screening scenario for a cosmological constant
in de Sitter solutions. Furthermore, we explicitly demonstrate that three types
of the finit... | [
{
"created": "Thu, 14 Apr 2011 08:16:29 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Jun 2011 10:21:36 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Feb 2012 02:25:37 GMT",
"version": "v3"
}
] | 2015-05-27 | [
[
"Bamba",
"Kazuharu",
""
],
[
"Nojiri",
"Shin'ichi",
""
],
[
"Odintsov",
"Sergei D.",
""
],
[
"Sasaki",
"Misao",
""
]
] | We investigate de Sitter solutions in non-local gravity as well as in non-local gravity with Lagrange constraint multiplier. We examine a condition to avoid a ghost and discuss a screening scenario for a cosmological constant in de Sitter solutions. Furthermore, we explicitly demonstrate that three types of the finite-... | 7.060347 | 6.605385 | 6.69534 | 6.479248 | 6.720012 | 6.46784 | 6.170193 | 6.343633 | 6.50719 | 6.571532 | 6.291286 | 6.691953 | 6.818142 | 6.716438 | 6.695621 | 6.708529 | 6.855049 | 6.472551 | 6.751187 | 6.678921 | 6.65853 |
hep-th/0002203 | Hidenori Sonoda | Hidenori Sonoda | QED out of matter | latex, 19 pages, 9 figures | Nucl.Phys. B585 (2000) 725-740 | 10.1016/S0550-3213(00)00340-0 | KOBE-TH-00-01 | hep-th hep-ph | null | The Wilsonian renormalization group implies that an arbitrary four
dimensional field theory with an ultraviolet cutoff is equivalent to a theory
which is renormalizable by power counting at energy scales much below the
cutoff. This applies to any theory including those with non-renormalizable
interactions as long as ... | [
{
"created": "Thu, 24 Feb 2000 03:56:19 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Sonoda",
"Hidenori",
""
]
] | The Wilsonian renormalization group implies that an arbitrary four dimensional field theory with an ultraviolet cutoff is equivalent to a theory which is renormalizable by power counting at energy scales much below the cutoff. This applies to any theory including those with non-renormalizable interactions as long as we... | 10.663074 | 8.710036 | 9.328889 | 8.810163 | 9.802724 | 9.125535 | 9.01074 | 9.476622 | 8.768943 | 9.814775 | 8.470952 | 8.863381 | 9.440577 | 8.464888 | 8.917377 | 8.774707 | 8.944402 | 8.933935 | 8.69603 | 9.020496 | 8.529147 |
2102.01680 | Silvia Nagy | Miguel Campiglia and Silvia Nagy | A double copy for asymptotic symmetries in the self-dual sector | 45 pages, 1 figure, replaced to match published version | null | 10.1007/JHEP03(2021)262 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a double copy construction for the symmetries of the self-dual
sectors of Yang-Mills (YM) and gravity, in the light-cone formulation. We find
an infinite set of double copy constructible symmetries. We focus on two
families which correspond to the residual diffeomorphisms on the gravitational
side. For the fi... | [
{
"created": "Tue, 2 Feb 2021 18:50:58 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Dec 2021 21:35:21 GMT",
"version": "v2"
}
] | 2021-12-23 | [
[
"Campiglia",
"Miguel",
""
],
[
"Nagy",
"Silvia",
""
]
] | We give a double copy construction for the symmetries of the self-dual sectors of Yang-Mills (YM) and gravity, in the light-cone formulation. We find an infinite set of double copy constructible symmetries. We focus on two families which correspond to the residual diffeomorphisms on the gravitational side. For the firs... | 8.092889 | 7.631066 | 8.718951 | 7.369874 | 8.02758 | 7.569231 | 7.950115 | 7.691766 | 7.422199 | 9.142776 | 7.317609 | 7.125775 | 7.798765 | 7.301157 | 7.247881 | 7.065757 | 7.258024 | 7.23478 | 7.332267 | 7.999859 | 7.048729 |
hep-th/0002036 | V. Suneeta | T.R. Govindarajan, V. Suneeta and S. Vaidya | Horizon States for AdS Black Holes | 18 pages, 2 figures, version to appear in Nuclear Physics B | Nucl.Phys. B583 (2000) 291-303 | 10.1016/S0550-3213(00)00336-9 | IMSc/2000/02/03, TIFR/TH/00-08 | hep-th gr-qc | null | We study the time-independent modes of a massless scalar field in various
black hole backgrounds, and show that for these black holes, the
time-independent mode is localised at the horizon. A similar analysis is done
for time-independent equilibrium modes of the five dimensional plane AdS black
hole. A self-adjointne... | [
{
"created": "Fri, 4 Feb 2000 16:21:02 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Feb 2000 12:32:33 GMT",
"version": "v2"
},
{
"created": "Tue, 25 Jul 2000 13:42:44 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Govindarajan",
"T. R.",
""
],
[
"Suneeta",
"V.",
""
],
[
"Vaidya",
"S.",
""
]
] | We study the time-independent modes of a massless scalar field in various black hole backgrounds, and show that for these black holes, the time-independent mode is localised at the horizon. A similar analysis is done for time-independent equilibrium modes of the five dimensional plane AdS black hole. A self-adjointness... | 12.585195 | 12.275344 | 12.237266 | 11.436673 | 11.773835 | 11.264359 | 10.959219 | 11.66518 | 11.121652 | 13.254609 | 11.70133 | 11.353276 | 11.696307 | 10.823099 | 11.397554 | 11.154189 | 11.176502 | 10.995915 | 11.430098 | 11.909596 | 10.75367 |
hep-th/0412011 | Eugen Radu | Vanush Paturyan, Eugen Radu and D. H. Tchrakian | Rotating regular solutions in Einstein-Yang-Mills-Higgs theory | 7 pages, 4 figures: misprints corrected | Phys.Lett. B609 (2005) 360-366 | 10.1016/j.physletb.2005.02.001 | null | hep-th gr-qc | null | We construct new axially symmetric rotating solutions of
Einstein-Yang-Mills-Higgs theory. These globally regular configurations possess
a nonvanishing electric charge which equals the total angular momentum, and
zero topological charge, representing a monopole-antimonopole system rotating
around the symmetry axis th... | [
{
"created": "Wed, 1 Dec 2004 16:48:10 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jan 2005 17:07:59 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Paturyan",
"Vanush",
""
],
[
"Radu",
"Eugen",
""
],
[
"Tchrakian",
"D. H.",
""
]
] | We construct new axially symmetric rotating solutions of Einstein-Yang-Mills-Higgs theory. These globally regular configurations possess a nonvanishing electric charge which equals the total angular momentum, and zero topological charge, representing a monopole-antimonopole system rotating around the symmetry axis thro... | 9.859197 | 9.400745 | 8.60112 | 8.324215 | 8.331903 | 8.447639 | 8.447807 | 8.093451 | 8.282462 | 9.155665 | 8.273756 | 9.030709 | 9.41502 | 9.166139 | 8.871627 | 8.96238 | 9.425079 | 9.183929 | 8.933334 | 9.891485 | 9.147545 |
1811.11528 | Sagar F. Lokhande | William Cottrell, Ben Freivogel, Diego M. Hofman, Sagar F. Lokhande | How to Build the Thermofield Double State | are welcome. 47 pages, 8 figures. v2: Improved discussion of
uniqueness and CFT primaries | null | 10.1007/JHEP02(2019)058 | null | hep-th cond-mat.str-el quant-ph | http://creativecommons.org/licenses/by/4.0/ | Given two copies of any quantum mechanical system, one may want to prepare
them in the thermofield double state for the purpose of studying thermal
physics or black holes. However, the thermofield double is a unique entangled
pure state and may be difficult to prepare. We propose a local interacting
Hamiltonian for t... | [
{
"created": "Wed, 28 Nov 2018 13:00:33 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Dec 2018 13:34:02 GMT",
"version": "v2"
}
] | 2019-02-20 | [
[
"Cottrell",
"William",
""
],
[
"Freivogel",
"Ben",
""
],
[
"Hofman",
"Diego M.",
""
],
[
"Lokhande",
"Sagar F.",
""
]
] | Given two copies of any quantum mechanical system, one may want to prepare them in the thermofield double state for the purpose of studying thermal physics or black holes. However, the thermofield double is a unique entangled pure state and may be difficult to prepare. We propose a local interacting Hamiltonian for the... | 7.134351 | 7.285102 | 7.346969 | 6.861093 | 7.096715 | 6.763031 | 7.077604 | 7.334533 | 6.867329 | 7.354159 | 6.753797 | 6.57381 | 6.787278 | 6.649116 | 6.475398 | 6.591337 | 6.613073 | 6.701684 | 6.424549 | 6.581354 | 6.34681 |
1908.01422 | Alexander Migdal | Alexander Migdal | Analytic and Numerical Study of Navier-Stokes Loop Equation in
Turbulence | 14 pages, 2 figures, one reference to Mathematica notebook on Wolfram
Cloud | null | null | null | hep-th nlin.CD physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We developed analytic approach to the non-planar loop equation, which we
derived in previous papers \cite{M19a},\cite{M19b},\cite{M19c}. We found
quadratic integral equation for the vorticity distribution $\Omega(r)$ we
introduced on a minimal surface. There are no corrections to the minimal
surface though: it is sti... | [
{
"created": "Sun, 4 Aug 2019 23:17:55 GMT",
"version": "v1"
}
] | 2019-08-06 | [
[
"Migdal",
"Alexander",
""
]
] | We developed analytic approach to the non-planar loop equation, which we derived in previous papers \cite{M19a},\cite{M19b},\cite{M19c}. We found quadratic integral equation for the vorticity distribution $\Omega(r)$ we introduced on a minimal surface. There are no corrections to the minimal surface though: it is still... | 17.202051 | 19.410856 | 18.452477 | 18.143408 | 18.946644 | 19.369614 | 19.337627 | 18.650307 | 17.824341 | 22.431271 | 18.210026 | 18.426819 | 17.262659 | 17.463362 | 17.136522 | 17.939566 | 17.753195 | 17.61603 | 17.775709 | 17.512869 | 17.070219 |
1403.0585 | Stefano Cremonesi | Stefano Cremonesi, Amihay Hanany, Noppadol Mekareeya, Alberto
Zaffaroni | Coulomb branch Hilbert series and Hall-Littlewood polynomials | v1: 40 pages + appendices, 3 figures; v2: minor revision, version to
appear in JHEP | null | 10.1007/JHEP09(2014)178 | CERN-PH-TH/2013-278, IMPERIAL-TP-14-SC-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There has been a recent progress in understanding the chiral ring of 3d
$\mathcal{N}=4$ superconformal gauge theories by explicitly constructing an
exact generating function (Hilbert series) counting BPS operators on the
Coulomb branch. In this paper we introduce Coulomb branch Hilbert series in the
presence of backg... | [
{
"created": "Mon, 3 Mar 2014 21:00:30 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Sep 2014 16:12:49 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Cremonesi",
"Stefano",
""
],
[
"Hanany",
"Amihay",
""
],
[
"Mekareeya",
"Noppadol",
""
],
[
"Zaffaroni",
"Alberto",
""
]
] | There has been a recent progress in understanding the chiral ring of 3d $\mathcal{N}=4$ superconformal gauge theories by explicitly constructing an exact generating function (Hilbert series) counting BPS operators on the Coulomb branch. In this paper we introduce Coulomb branch Hilbert series in the presence of backgro... | 5.72384 | 5.228929 | 6.350533 | 5.437116 | 5.722396 | 5.504497 | 5.371047 | 5.218267 | 5.327904 | 6.873999 | 5.246505 | 5.352676 | 5.77716 | 5.369174 | 5.414583 | 5.355346 | 5.428874 | 5.289125 | 5.318684 | 5.615728 | 5.287745 |
2108.00068 | Shaun Hampton | Bin Guo and Shaun Hampton | The Dual of a Tidal Force in the D1D5 CFT | 21 pages, 4 figures | null | 10.1007/JHEP07(2023)149 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was demonstrated that a string probe falling radially within a
superstratum geometry would experience tidal forces. These tidal forces were
shown to excite the string by converting its kinetic energy into stringy
excitations. Using the AdS/CFT correspondence we seek to understand this
behavior from the perspective... | [
{
"created": "Fri, 30 Jul 2021 20:24:33 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Nov 2021 16:49:42 GMT",
"version": "v2"
}
] | 2023-08-02 | [
[
"Guo",
"Bin",
""
],
[
"Hampton",
"Shaun",
""
]
] | It was demonstrated that a string probe falling radially within a superstratum geometry would experience tidal forces. These tidal forces were shown to excite the string by converting its kinetic energy into stringy excitations. Using the AdS/CFT correspondence we seek to understand this behavior from the perspective o... | 7.986494 | 7.154343 | 8.366117 | 7.062241 | 7.39928 | 7.463716 | 7.342683 | 7.494055 | 7.353739 | 8.85439 | 7.40215 | 7.332822 | 8.010186 | 7.40119 | 7.515448 | 7.188838 | 7.624365 | 7.425305 | 7.492131 | 7.882131 | 7.355945 |
2008.01384 | Yuqi Lei | Yu-Qi Lei, Xian-Hui Ge and Cheng Ran | Chaos of Particle Motion near the Black Hole with Quasi-topological
Electromagnetism | 32 pages, 13 figures, 3 tables | Phys. Rev. D 104, 046020 (2021) | 10.1103/PhysRevD.104.046020 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the chaotic behavior of particle motion in a black hole with
quasi-topological electromagnetism. The chaos bound is found to be violated in
the higher order expansion of the metric function and the electric potential
near the horizon. We draw the Poincare sections of particle motion
corresponding to the ch... | [
{
"created": "Tue, 4 Aug 2020 07:46:49 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Aug 2020 08:42:48 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Sep 2021 15:26:34 GMT",
"version": "v3"
}
] | 2021-09-02 | [
[
"Lei",
"Yu-Qi",
""
],
[
"Ge",
"Xian-Hui",
""
],
[
"Ran",
"Cheng",
""
]
] | We explore the chaotic behavior of particle motion in a black hole with quasi-topological electromagnetism. The chaos bound is found to be violated in the higher order expansion of the metric function and the electric potential near the horizon. We draw the Poincare sections of particle motion corresponding to the chao... | 7.179496 | 6.941806 | 6.649159 | 6.524984 | 6.547202 | 6.720236 | 7.068584 | 6.517232 | 6.725708 | 7.214781 | 6.803939 | 6.548545 | 6.97568 | 6.645389 | 6.727841 | 6.385171 | 6.69197 | 6.472095 | 6.871132 | 6.902778 | 6.79622 |
1707.08584 | Cristhiam Lopez-Arcos | Humberto Gomez, Cristhiam Lopez-Arcos, Pedro Talavera | One-loop Parke-Taylor factors for quadratic propagators from massless
scattering equations | 43 pages, new appendix added, few typos corrected. Accepted for
publication in JHEP | null | 10.1007/JHEP10(2017)175 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we reconsider the Cachazo-He-Yuan construction (CHY) of the so
called scattering amplitudes at one-loop, in order to obtain quadratic
propagators. In theories with colour ordering the key ingredient is the
redefinition of the Parke-Taylor factors. After classifying all the possible
one-loop CHY-integran... | [
{
"created": "Wed, 26 Jul 2017 18:00:37 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Aug 2017 13:40:57 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Nov 2017 15:22:23 GMT",
"version": "v3"
}
] | 2017-12-06 | [
[
"Gomez",
"Humberto",
""
],
[
"Lopez-Arcos",
"Cristhiam",
""
],
[
"Talavera",
"Pedro",
""
]
] | In this paper we reconsider the Cachazo-He-Yuan construction (CHY) of the so called scattering amplitudes at one-loop, in order to obtain quadratic propagators. In theories with colour ordering the key ingredient is the redefinition of the Parke-Taylor factors. After classifying all the possible one-loop CHY-integrands... | 11.711338 | 11.047544 | 13.919445 | 10.250176 | 10.888887 | 10.652953 | 10.701585 | 11.271681 | 11.068363 | 14.560575 | 10.985583 | 9.909364 | 10.735074 | 9.899058 | 10.259048 | 10.428755 | 10.107486 | 9.885071 | 9.841045 | 11.379983 | 10.007236 |
hep-th/9607122 | Ayrton Zadra | L.O. Buffon, D. Dalmazi and A. Zadra | Classical and quantum N=1 super $W_\infty$-algebras | 10 pages, latex, no figures | Mod.Phys.Lett. A11 (1996) 2339-2350 | 10.1142/S0217732396002332 | null | hep-th | null | We construct higher-spin N=1 super algebras as extensions of the super
Virasoro algebra containing generators for all spins $s\ge 3/2$. We find two
distinct classical (Poisson) algebras on the phase super space. Our results
indicate that only one of them can be consistently quantized.
| [
{
"created": "Mon, 15 Jul 1996 18:22:57 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Buffon",
"L. O.",
""
],
[
"Dalmazi",
"D.",
""
],
[
"Zadra",
"A.",
""
]
] | We construct higher-spin N=1 super algebras as extensions of the super Virasoro algebra containing generators for all spins $s\ge 3/2$. We find two distinct classical (Poisson) algebras on the phase super space. Our results indicate that only one of them can be consistently quantized. | 11.734844 | 9.750299 | 10.691955 | 9.869598 | 10.207016 | 10.139539 | 10.717572 | 9.470349 | 9.565239 | 12.508822 | 9.619071 | 10.535434 | 11.338996 | 10.23263 | 10.255192 | 10.82022 | 10.545518 | 10.268986 | 10.525664 | 11.13612 | 10.204315 |
1905.12636 | Sridip Pal | Shouvik Ganguly, Sridip Pal | Bounds on the density of states and the spectral gap in CFT$_{2}$ | v2: 26 pages, 10 figures, optimality of the lower bound included, new
section on connection to sphere packing v3: approximates the published
version, reference added | Phys. Rev. D 101, 106022, 2020 | 10.1103/PhysRevD.101.106022 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We improve the recently discovered upper and lower bounds on the $O(1)$
correction to the Cardy formula for the density of states integrated over an
energy window (of width $2\delta$), centered at high energy in 2 dimensional
conformal field theory. We prove optimality of the lower bound for $\delta\to
1^{-}$. We pro... | [
{
"created": "Wed, 29 May 2019 18:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Jan 2020 16:53:25 GMT",
"version": "v2"
},
{
"created": "Tue, 19 May 2020 20:04:14 GMT",
"version": "v3"
}
] | 2020-05-27 | [
[
"Ganguly",
"Shouvik",
""
],
[
"Pal",
"Sridip",
""
]
] | We improve the recently discovered upper and lower bounds on the $O(1)$ correction to the Cardy formula for the density of states integrated over an energy window (of width $2\delta$), centered at high energy in 2 dimensional conformal field theory. We prove optimality of the lower bound for $\delta\to 1^{-}$. We prove... | 13.466805 | 12.620725 | 13.253023 | 12.407348 | 13.334776 | 12.283925 | 13.234295 | 13.192884 | 13.10239 | 13.363256 | 12.597018 | 12.25316 | 13.021233 | 12.534939 | 12.220105 | 12.672469 | 12.562131 | 12.776146 | 12.670886 | 13.429719 | 12.333135 |
hep-th/9802161 | Edward G. Timoshenko | N.A. Sveshnikov, E.G. Timoshenko | The partition function versus boundary conditions and confinement in the
Yang-Mills theory | 14 pages, RevTeX, submitted to Phys. Rev. D | Phys.Rev. D58 (1998) 085024 | 10.1103/PhysRevD.58.085024 | null | hep-th cond-mat.stat-mech hep-ph | null | We analyse dependence of the partition function on the boundary condition for
the longitudinal component of the electric field strength in gauge field
theories. In a physical gauge the Gauss law constraint may be resolved
explicitly expressing this component via an integral of the physical
transversal variables. In p... | [
{
"created": "Mon, 23 Feb 1998 19:57:18 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Sveshnikov",
"N. A.",
""
],
[
"Timoshenko",
"E. G.",
""
]
] | We analyse dependence of the partition function on the boundary condition for the longitudinal component of the electric field strength in gauge field theories. In a physical gauge the Gauss law constraint may be resolved explicitly expressing this component via an integral of the physical transversal variables. In par... | 13.471931 | 13.911641 | 12.963904 | 12.716954 | 14.196061 | 14.447371 | 14.347664 | 14.112529 | 12.253583 | 15.035352 | 13.205954 | 13.380688 | 13.600616 | 13.283261 | 13.174713 | 13.985669 | 13.29307 | 13.74909 | 13.239998 | 13.312671 | 13.031375 |
1705.04568 | Ivan Kharuk | Ivan Kharuk | Coset space construction and inverse Higgs phenomenon for the conformal
group | 30 pages, 1 figure | null | null | INR-TH-2017-014 | hep-th math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that conformally invariant theories can be obtained within the
framework of the coset space construction. The corresponding technique is
applicable for the construction of representations of the unbroken conformal
group, as well as of a spontaneously broken one. A special role of the
"Nambu-Goldstone fiel... | [
{
"created": "Fri, 12 May 2017 13:51:32 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Aug 2017 11:13:01 GMT",
"version": "v2"
}
] | 2017-08-02 | [
[
"Kharuk",
"Ivan",
""
]
] | It is shown that conformally invariant theories can be obtained within the framework of the coset space construction. The corresponding technique is applicable for the construction of representations of the unbroken conformal group, as well as of a spontaneously broken one. A special role of the "Nambu-Goldstone fields... | 12.067225 | 10.95478 | 12.289553 | 11.332217 | 11.282147 | 11.713299 | 11.560274 | 10.530552 | 11.432853 | 12.204673 | 10.789194 | 11.108907 | 11.673826 | 11.424027 | 11.338346 | 11.600176 | 11.316644 | 11.354811 | 11.690036 | 11.736742 | 11.005861 |
hep-th/9203055 | null | G.Bonacina, A.Gamba and M.Martellini | Interacting Euclidean 3D Quantum Gravity | 19 pages | Phys.Rev.D45:3577-3583,1992 | 10.1103/PhysRevD.45.3577 | null | hep-th | null | We show that Euclidean 3D-gravity coupled to a Gaussian scalar massive matter
field in first-order dreibein formalism gives a quantum theory which has a
finite perturbative expansion around a non-vanishing background. We also
discuss a possible mechanism to generate a non-trivial background metric
starting from Rovel... | [
{
"created": "Fri, 20 Mar 1992 13:17:00 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Bonacina",
"G.",
""
],
[
"Gamba",
"A.",
""
],
[
"Martellini",
"M.",
""
]
] | We show that Euclidean 3D-gravity coupled to a Gaussian scalar massive matter field in first-order dreibein formalism gives a quantum theory which has a finite perturbative expansion around a non-vanishing background. We also discuss a possible mechanism to generate a non-trivial background metric starting from Rovelli... | 13.979895 | 15.379517 | 13.367143 | 12.398796 | 14.188688 | 12.018769 | 13.990748 | 12.465719 | 12.993396 | 12.512616 | 13.798218 | 12.722883 | 12.389863 | 12.486519 | 12.727027 | 13.709176 | 12.546878 | 12.391228 | 12.810158 | 12.75724 | 12.025866 |
hep-th/9807230 | Micha Berkooz | Micha Berkooz (Institute for Advanced Study, Princeton) | A Proposal on Some Microscopic Aspects of the AdS/CFT Duality | 32 pages, harvmac | Nucl.Phys. B553 (1999) 205-230 | 10.1016/S0550-3213(99)00220-5 | null | hep-th | null | We suggest a model of the large N limit ${\cal N}=4$ D=4 SU(N) SYM as a gas
of 3-branes in a 10 dimensional space. Field theory analysis suggests that this
10 dimensional space does not carry the usual gravity dynamics but rather a
contraction of it. Using a non-local transformation some aspects of the
dynamics of th... | [
{
"created": "Thu, 30 Jul 1998 20:07:59 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Berkooz",
"Micha",
"",
"Institute for Advanced Study, Princeton"
]
] | We suggest a model of the large N limit ${\cal N}=4$ D=4 SU(N) SYM as a gas of 3-branes in a 10 dimensional space. Field theory analysis suggests that this 10 dimensional space does not carry the usual gravity dynamics but rather a contraction of it. Using a non-local transformation some aspects of the dynamics of this... | 10.37663 | 10.258603 | 10.511781 | 9.820443 | 10.061241 | 9.803452 | 10.401657 | 9.845539 | 9.789512 | 11.575529 | 9.58928 | 10.066741 | 10.115161 | 9.866549 | 9.708647 | 10.22288 | 10.165048 | 9.781073 | 9.908334 | 10.208338 | 9.750924 |
0712.2821 | Claudia de Rham | Claudia de Rham, Stefan Hofmann, Justin Khoury and Andrew J. Tolley | Cascading Gravity and Degravitation | 31 pages, 1 figure | JCAP 0802:011,2008 | 10.1088/1475-7516/2008/02/011 | null | hep-th | null | We construct a cascading brane model of gravity in which the behavior of the
gravitational force law interpolates from (n+4)-dimensional to
(n+3)-dimensional all the way down to 4-dimensional from longer to shorter
length scales. We show that at the linearized level, this model exhibits the
features necessary for deg... | [
{
"created": "Mon, 17 Dec 2007 21:12:49 GMT",
"version": "v1"
}
] | 2009-11-19 | [
[
"de Rham",
"Claudia",
""
],
[
"Hofmann",
"Stefan",
""
],
[
"Khoury",
"Justin",
""
],
[
"Tolley",
"Andrew J.",
""
]
] | We construct a cascading brane model of gravity in which the behavior of the gravitational force law interpolates from (n+4)-dimensional to (n+3)-dimensional all the way down to 4-dimensional from longer to shorter length scales. We show that at the linearized level, this model exhibits the features necessary for degra... | 9.315245 | 9.040707 | 9.526425 | 9.018392 | 8.961118 | 9.085138 | 8.539874 | 8.692347 | 9.249969 | 9.819558 | 8.999764 | 8.906613 | 9.042591 | 8.886096 | 8.813251 | 9.046968 | 8.925579 | 8.987092 | 8.948745 | 9.06129 | 8.829393 |
1305.6690 | Chanyong Park | Chanyong Park | Notes on the holographic Lifshitz theory | 17 pages, major revision | null | 10.1155/2014/917632 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | On the Lifshitz black brane geometry of an Einstein-Maxwell-dilaton gravity,
we holographically investigate electric DC conductivities and the role of
impurity in a non-relativistic Lifshitz medium with two different charge
carriers, impurity and Lifshitz matter. The conductivity carried by Lifshitz
matter is proport... | [
{
"created": "Wed, 29 May 2013 04:38:27 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Nov 2013 06:48:30 GMT",
"version": "v2"
}
] | 2015-07-14 | [
[
"Park",
"Chanyong",
""
]
] | On the Lifshitz black brane geometry of an Einstein-Maxwell-dilaton gravity, we holographically investigate electric DC conductivities and the role of impurity in a non-relativistic Lifshitz medium with two different charge carriers, impurity and Lifshitz matter. The conductivity carried by Lifshitz matter is proportio... | 9.711994 | 9.793646 | 9.839774 | 9.127851 | 9.66258 | 9.89022 | 9.898809 | 9.444996 | 8.991321 | 10.213164 | 9.182997 | 8.704307 | 8.973691 | 8.720614 | 8.903248 | 8.581632 | 8.782255 | 8.667321 | 8.934664 | 9.378311 | 8.538378 |
2006.01163 | Damiano Anselmi | Damiano Anselmi | Quantum field theories of arbitrary-spin massive multiplets and Palatini
quantum gravity | 34 pages; v2: references added, JHEP | J. High Energy Phys. 07 (2020) 176 | 10.1007/JHEP07(2020)176 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formulate quantum field theories of massive fields of arbitrary spins. The
presence of both physical and fake particles, organized into multiplets, makes
it possible to fulfill the requirements of locality, unitarity and
renormalizability at the same time. The theories admit cubic and quartic
self-interactions and... | [
{
"created": "Mon, 1 Jun 2020 18:01:04 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Jul 2020 23:28:36 GMT",
"version": "v2"
}
] | 2020-07-28 | [
[
"Anselmi",
"Damiano",
""
]
] | We formulate quantum field theories of massive fields of arbitrary spins. The presence of both physical and fake particles, organized into multiplets, makes it possible to fulfill the requirements of locality, unitarity and renormalizability at the same time. The theories admit cubic and quartic self-interactions and c... | 4.290033 | 9.147346 | 9.471057 | 8.931619 | 8.66303 | 9.059674 | 8.544926 | 8.248748 | 8.803681 | 10.102886 | 8.037102 | 6.471656 | 6.843001 | 6.980719 | 6.071327 | 6.468303 | 6.74656 | 6.238167 | 6.4136 | 7.607605 | 5.499118 |
hep-th/0312034 | Luzi Bergamin | L. Bergamin and P. Minkowski | No Supersymmetry without Supergravity: Induced Supersymmetry
Representations on Composite Effective Fields | 15 pages, LaTeX | null | null | null | hep-th | null | Induced supersymmetry representations on composite operators are studied. In
superspace the ensuing transformation rules (trivially) lead to an effective
superfield. On the other hand, an induced representation must exist for
non-linear (``on-shell'') supersymmetry as well. As this choice of the
representation is phy... | [
{
"created": "Wed, 3 Dec 2003 12:59:42 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bergamin",
"L.",
""
],
[
"Minkowski",
"P.",
""
]
] | Induced supersymmetry representations on composite operators are studied. In superspace the ensuing transformation rules (trivially) lead to an effective superfield. On the other hand, an induced representation must exist for non-linear (``on-shell'') supersymmetry as well. As this choice of the representation is physi... | 16.632359 | 17.325939 | 17.092405 | 16.16217 | 17.104294 | 17.256952 | 16.772839 | 16.270592 | 15.962922 | 18.926079 | 16.497677 | 14.627636 | 15.279043 | 14.756077 | 15.323258 | 14.523156 | 15.294679 | 14.653962 | 14.983327 | 15.586729 | 15.526644 |
hep-th/0302105 | Fernando Marchesano | D. Cremades, L.E. Ibanez and F. Marchesano | Yukawa couplings in intersecting D-brane models | 47 pages, using JHEP3.cls, 11 figures. Typos and other minor
corrections. References added | JHEP 0307 (2003) 038 | 10.1088/1126-6708/2003/07/038 | FTUAM-03/2 IFT-UAM/CSIC-03-06 | hep-th hep-ph | null | We compute the Yukawa couplings among chiral fields in toroidal Type II
compactifications with wrapping D6-branes intersecting at angles. Those models
can yield realistic standard model spectrum living at the intersections. The
Yukawa couplings depend both on the Kahler and open string moduli but not on
the complex s... | [
{
"created": "Fri, 14 Feb 2003 18:06:40 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Mar 2003 19:25:20 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Cremades",
"D.",
""
],
[
"Ibanez",
"L. E.",
""
],
[
"Marchesano",
"F.",
""
]
] | We compute the Yukawa couplings among chiral fields in toroidal Type II compactifications with wrapping D6-branes intersecting at angles. Those models can yield realistic standard model spectrum living at the intersections. The Yukawa couplings depend both on the Kahler and open string moduli but not on the complex str... | 7.116777 | 7.095731 | 8.381156 | 6.710959 | 7.30008 | 7.351011 | 7.377235 | 7.072447 | 6.917243 | 8.457238 | 6.732717 | 6.982964 | 7.653361 | 7.075269 | 7.061774 | 6.745704 | 6.924057 | 6.858556 | 6.980354 | 7.517729 | 6.983457 |
1308.1238 | Shoichi Ichinose | Shoichi Ichinose | Velocity-Field Theory, Boltzmann's Transport Equation and Geometry | 6 pages, 2 figures, Presentation at
APPC12(Makuhari,Chiba,Japan,2013.7.14-19),JPS Conference Proceedings (in
press) | null | null | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Boltzmann equation describes the time development of the velocity
distribution in the continuum fluid matter. We formulate the equation using the
field theory where the {\it velocity-field} plays the central role. The matter
(constituent particles) fields appear as the density and the viscosity. {\it
Fluctuation} is ... | [
{
"created": "Tue, 6 Aug 2013 11:11:54 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Oct 2013 03:01:41 GMT",
"version": "v2"
}
] | 2013-10-10 | [
[
"Ichinose",
"Shoichi",
""
]
] | Boltzmann equation describes the time development of the velocity distribution in the continuum fluid matter. We formulate the equation using the field theory where the {\it velocity-field} plays the central role. The matter (constituent particles) fields appear as the density and the viscosity. {\it Fluctuation} is ex... | 22.802935 | 26.468895 | 22.740986 | 23.382318 | 25.086889 | 25.19095 | 25.844666 | 24.348148 | 24.452396 | 25.491039 | 23.368193 | 22.886644 | 22.78253 | 22.081099 | 22.201252 | 22.134098 | 22.481068 | 22.009226 | 22.871857 | 22.309341 | 22.463007 |
2306.05964 | Marco Alberto Javarone | Marco Alberto Javarone | Low-temperature Holographic Screens Correspond to Einstein-Rosen Bridges | 17 pages, 5 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent conjectures on the complexity of black holes suggest that their
evolution manifests in the structural properties of Einstein-Rosen bridges,
like the length and volume. The complexity of black holes relates to the
computational complexity of their dual, namely holographic, quantum systems
identified via the Gau... | [
{
"created": "Fri, 9 Jun 2023 15:33:20 GMT",
"version": "v1"
}
] | 2023-06-12 | [
[
"Javarone",
"Marco Alberto",
""
]
] | Recent conjectures on the complexity of black holes suggest that their evolution manifests in the structural properties of Einstein-Rosen bridges, like the length and volume. The complexity of black holes relates to the computational complexity of their dual, namely holographic, quantum systems identified via the Gauge... | 12.889508 | 14.033339 | 13.779912 | 13.141429 | 13.693418 | 14.058928 | 13.39706 | 13.539242 | 12.88942 | 13.290813 | 13.171607 | 12.431883 | 12.681681 | 12.541189 | 12.621989 | 12.712665 | 12.967904 | 12.503816 | 12.533792 | 12.414433 | 12.727711 |
1201.4020 | Vladimir Rochev | V. E. Rochev | Asymptotic behavior in a model with Yukawa interaction from
Schwinger-Dyson equations | 15 pages; journal version | J.Phys.A:Math.Theor.45(2012)205401 | 10.1088/1751-8113/45/20/205401 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A system of Schwinger-Dyson equations for pseudoscalar four-dimensional
Yukawa model in the two-particle approximation is investigated. The simplest
iterative solution of the system corresponds to the mean-field approximation
(or, equivalently, to the leading order of 1/N-expansion) and includes a
non-physical Landau... | [
{
"created": "Thu, 19 Jan 2012 11:00:19 GMT",
"version": "v1"
},
{
"created": "Sun, 6 May 2012 09:39:14 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Rochev",
"V. E.",
""
]
] | A system of Schwinger-Dyson equations for pseudoscalar four-dimensional Yukawa model in the two-particle approximation is investigated. The simplest iterative solution of the system corresponds to the mean-field approximation (or, equivalently, to the leading order of 1/N-expansion) and includes a non-physical Landau p... | 9.763596 | 9.087526 | 10.101716 | 9.501952 | 10.888164 | 9.751113 | 9.646244 | 9.550591 | 9.243573 | 10.368903 | 8.804273 | 9.113785 | 9.296662 | 8.893835 | 8.960629 | 9.108863 | 8.926264 | 8.851769 | 8.946404 | 9.372453 | 8.735752 |
hep-th/0605256 | Jihn E. Kim | Ian-Woo Kim and Jihn E. Kim | Modification of Decay Constants of Superstring Axions: Effects of Flux
Compactification and Axion Mixing | 6 pages with 3 figures, revtex; figure added,section of axion mixing
modified | Phys.Lett. B639 (2006) 342-347 | 10.1016/j.physletb.2006.06.033 | null | hep-th astro-ph hep-ph | null | We study possibilities for lowering the decay constants of superstring
axions. In the heterotic Calabi-Yau compactification, a localized
model-dependent axion can appear at a nearly collapsing 2-cycle. The effect of
flux can be used for generating warp factor suppression of the axion decay
constant. We also point out... | [
{
"created": "Thu, 25 May 2006 19:57:08 GMT",
"version": "v1"
},
{
"created": "Mon, 29 May 2006 07:41:38 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Jun 2006 00:59:15 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Kim",
"Ian-Woo",
""
],
[
"Kim",
"Jihn E.",
""
]
] | We study possibilities for lowering the decay constants of superstring axions. In the heterotic Calabi-Yau compactification, a localized model-dependent axion can appear at a nearly collapsing 2-cycle. The effect of flux can be used for generating warp factor suppression of the axion decay constant. We also point out t... | 13.365576 | 13.914863 | 13.145213 | 12.659768 | 13.736959 | 13.507151 | 13.408471 | 13.881319 | 13.211269 | 15.171718 | 13.174891 | 12.714359 | 12.411364 | 12.438555 | 12.540956 | 12.649413 | 12.654315 | 12.936674 | 12.758275 | 13.065967 | 12.307724 |
2210.02473 | Maciej Kolanowski | Gary T. Horowitz, Maciej Kolanowski and Jorge E. Santos | Almost all extremal black holes in AdS are singular | 41 pages, 7 figures, v3: accepted for publication in JHEP | null | 10.1007/JHEP01(2023)162 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the geometry near the horizon of a generic, four-dimensional
extremal black hole. When the cosmological constant is negative, we show that
(in almost all cases) tidal forces diverge as one crosses the horizon, and this
singularity is stronger for larger black holes. In particular, this applies to
gener... | [
{
"created": "Wed, 5 Oct 2022 18:00:07 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Oct 2022 07:43:32 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Dec 2022 17:00:02 GMT",
"version": "v3"
}
] | 2023-02-15 | [
[
"Horowitz",
"Gary T.",
""
],
[
"Kolanowski",
"Maciej",
""
],
[
"Santos",
"Jorge E.",
""
]
] | We investigate the geometry near the horizon of a generic, four-dimensional extremal black hole. When the cosmological constant is negative, we show that (in almost all cases) tidal forces diverge as one crosses the horizon, and this singularity is stronger for larger black holes. In particular, this applies to generic... | 7.605276 | 7.991633 | 7.922071 | 7.225736 | 7.481197 | 7.54385 | 7.556028 | 6.953037 | 7.16177 | 7.2335 | 7.23307 | 7.461529 | 7.580565 | 7.310268 | 7.618464 | 7.40677 | 7.430765 | 7.25064 | 7.5955 | 7.389347 | 7.436112 |
1312.7273 | Andre Franca | Gia Dvali, Sarah Folkerts, Andre Franca | On How Neutrino Protects the Axion | 9 pages | Phys. Rev. D 89, 105025 (2014) | 10.1103/PhysRevD.89.105025 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how the neutrino can sacrifice itself to quantum gravity and save the
axion solution to the strong-CP problem. This mechanism puts an upper bound on
the lightest neutrino mass.
| [
{
"created": "Fri, 27 Dec 2013 14:43:37 GMT",
"version": "v1"
}
] | 2014-05-28 | [
[
"Dvali",
"Gia",
""
],
[
"Folkerts",
"Sarah",
""
],
[
"Franca",
"Andre",
""
]
] | We show how the neutrino can sacrifice itself to quantum gravity and save the axion solution to the strong-CP problem. This mechanism puts an upper bound on the lightest neutrino mass. | 15.62986 | 15.802321 | 13.673764 | 12.349539 | 13.348515 | 15.626884 | 12.015882 | 12.979225 | 13.786668 | 13.773506 | 12.919589 | 14.995842 | 13.906902 | 13.56239 | 14.78274 | 14.014505 | 14.584847 | 14.473639 | 13.108578 | 13.22892 | 14.81384 |
hep-th/9706087 | Michael Spalinski | Ansar Fayyazuddin and Michael Spalinski | The Seiberg-Witten Differential From M-Theory | 14 pages, Latex. References added, typos corrected | Nucl.Phys. B508 (1997) 219-228 | 10.1016/S0550-3213(97)00613-5 | HUTP-97/A027 | hep-th | null | The form of the Seiberg-Witten differential is derived from the M-theory
approach to N=2 supersymmetric Yang-Mills theories by directly imposing the BPS
condition for twobranes ending on fivebranes. The BPS condition also implies
that the pullback of the Kahler form onto the space part of the twobrane
world-volume va... | [
{
"created": "Thu, 12 Jun 1997 23:30:06 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Jul 1997 14:56:24 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Fayyazuddin",
"Ansar",
""
],
[
"Spalinski",
"Michael",
""
]
] | The form of the Seiberg-Witten differential is derived from the M-theory approach to N=2 supersymmetric Yang-Mills theories by directly imposing the BPS condition for twobranes ending on fivebranes. The BPS condition also implies that the pullback of the Kahler form onto the space part of the twobrane world-volume vani... | 8.724512 | 6.707316 | 9.840187 | 6.988891 | 7.769103 | 6.596621 | 7.063068 | 6.230061 | 7.169971 | 11.19341 | 7.162679 | 7.771691 | 8.322798 | 7.738818 | 7.560657 | 7.55532 | 7.181813 | 8.024765 | 7.872097 | 8.257388 | 7.366753 |
2110.13275 | Fernando Quevedo | C.P. Burgess and F. Quevedo | Who's Afraid of the Supersymmetric Dark? The Standard Model vs
Low-Energy Supergravity | 28 pages | null | 10.1002/prop.202200077 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Use of supergravity equations in astronomy and late-universe cosmology is
often criticized on three grounds: (i) phenomenological success usually depends
on the supergravity form for the scalar potential applying at the relevant
energies; (ii) the low-energy scalar potential is extremely sensitive to
quantum effects ... | [
{
"created": "Mon, 25 Oct 2021 21:28:56 GMT",
"version": "v1"
}
] | 2022-09-07 | [
[
"Burgess",
"C. P.",
""
],
[
"Quevedo",
"F.",
""
]
] | Use of supergravity equations in astronomy and late-universe cosmology is often criticized on three grounds: (i) phenomenological success usually depends on the supergravity form for the scalar potential applying at the relevant energies; (ii) the low-energy scalar potential is extremely sensitive to quantum effects in... | 11.946182 | 13.216263 | 12.800803 | 11.577933 | 13.796491 | 13.07516 | 12.855019 | 12.96863 | 12.14283 | 13.887933 | 12.331767 | 11.63524 | 11.655457 | 11.532304 | 11.762533 | 11.874137 | 11.839304 | 11.923663 | 11.651079 | 11.986698 | 11.836537 |
1912.07143 | Brad Cownden | Brad Cownden | Examining Instabilities Due to Driven Scalars in AdS | v1: 29 pages, 6 figures v2: Added reference and small changes to
Discussion. 30 pages, 6 figures v3: To appear in JHEP. Added holographic
interpretation, review of resummation procedure, and moved discussion of
all-normalizable resonances to appendix. 34 pages, 6 figures | null | 10.1007/JHEP12(2020)013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the study of the non-linear perturbative theory of weakly turbulent
energy cascades in AdS$_{d+1}$ to include solutions of driven systems, i.e.
those with time-dependent sources on the AdS boundary. This necessitates the
activation of non-normalizable modes in the linear solution for the massive
bulk scalar... | [
{
"created": "Mon, 16 Dec 2019 00:42:42 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Apr 2020 21:40:31 GMT",
"version": "v2"
},
{
"created": "Tue, 13 Oct 2020 21:21:03 GMT",
"version": "v3"
}
] | 2020-12-30 | [
[
"Cownden",
"Brad",
""
]
] | We extend the study of the non-linear perturbative theory of weakly turbulent energy cascades in AdS$_{d+1}$ to include solutions of driven systems, i.e. those with time-dependent sources on the AdS boundary. This necessitates the activation of non-normalizable modes in the linear solution for the massive bulk scalar f... | 14.569801 | 15.791768 | 15.338254 | 13.207383 | 15.014904 | 15.401404 | 14.978944 | 13.460917 | 13.905185 | 18.814802 | 13.654543 | 13.967774 | 13.929205 | 13.200778 | 13.449755 | 13.837071 | 13.705175 | 13.163272 | 13.759193 | 14.659619 | 13.570225 |
hep-th/0611337 | Angel Sanchez | Angel Sanchez, Alejandro Ayala and Gabriella Piccinelli | Effective potential at finite temperature in a constant hypermagnetic
field: Ring diagrams in the Standard Model | 15 pages, 8 Postscript figures | Phys.Rev.D75:043004,2007 | 10.1103/PhysRevD.75.043004 | null | hep-th astro-ph hep-ph | null | We study the symmetry breaking phenomenon in the standard model during the
electroweak phase transition in the presence of a constant hypermagnetic field.
We compute the finite temperature effective potential up to the contribution of
ring diagrams in the weak field, high temperature limit and show that under
these c... | [
{
"created": "Wed, 29 Nov 2006 23:26:01 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Sanchez",
"Angel",
""
],
[
"Ayala",
"Alejandro",
""
],
[
"Piccinelli",
"Gabriella",
""
]
] | We study the symmetry breaking phenomenon in the standard model during the electroweak phase transition in the presence of a constant hypermagnetic field. We compute the finite temperature effective potential up to the contribution of ring diagrams in the weak field, high temperature limit and show that under these con... | 9.919138 | 8.433509 | 7.082844 | 7.248535 | 9.648958 | 9.328233 | 9.69276 | 9.119886 | 6.511115 | 7.304221 | 8.413527 | 9.48931 | 9.266044 | 8.720243 | 9.821212 | 8.71256 | 9.504708 | 9.443431 | 9.425787 | 8.494765 | 9.787306 |
hep-th/9512014 | Oleg Soloviev | Oleg A. Soloviev | Is a truly marginal perturbation of the $G_k\times G_k$ WZNW model at
$k=-2c_V(G)$ an exception to the rule? | Latex file, 12 pp | null | 10.1016/0370-2693(96)00564-3 | QMW-PH-95-50 | hep-th | null | It is shown that there exists a truly marginal deformation of the direct sum
of two $G_k$ WZNW models at $k=-2c_V(G)$ (where $c_V(G)$ is the eigenvalue of
the quadratic Casimir operator in the adjoint representation of the group $G$)
which does not seem to fit the Chaudhuri-Schwartz criterion for truly marginal
pertu... | [
{
"created": "Mon, 4 Dec 1995 17:37:00 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Dec 1995 12:10:00 GMT",
"version": "v2"
},
{
"created": "Wed, 6 Dec 1995 11:51:10 GMT",
"version": "v3"
},
{
"created": "Tue, 12 Dec 1995 18:43:03 GMT",
"version": "v4"
}
] | 2009-10-28 | [
[
"Soloviev",
"Oleg A.",
""
]
] | It is shown that there exists a truly marginal deformation of the direct sum of two $G_k$ WZNW models at $k=-2c_V(G)$ (where $c_V(G)$ is the eigenvalue of the quadratic Casimir operator in the adjoint representation of the group $G$) which does not seem to fit the Chaudhuri-Schwartz criterion for truly marginal perturb... | 10.024413 | 7.626806 | 10.029623 | 7.947727 | 8.235275 | 7.367763 | 7.086096 | 8.048617 | 8.228071 | 10.370442 | 7.604469 | 7.826565 | 8.338424 | 7.512512 | 7.689042 | 7.622062 | 8.126227 | 8.153181 | 7.204539 | 9.025025 | 7.759207 |
1601.08218 | Adrian Koenigstein | Adrian Koenigstein, Johannes Kirsch, Horst Stoecker, Juergen
Struckmeier, David Vasak, Matthias Hanauske | Gauge Theory by canonical Transformations | 27 pages | null | 10.1142/S0218301316420052 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Electromagnetism, the strong and the weak interaction are commonly formulated
as gauge theories in a Lagrangian description. In this paper we present an
alternative formal derivation of U(1)-gauge theory in a manifestly covariant
Hamilton formalism. We make use of canonical transformations as our guiding
tool to form... | [
{
"created": "Fri, 29 Jan 2016 18:35:49 GMT",
"version": "v1"
}
] | 2016-06-03 | [
[
"Koenigstein",
"Adrian",
""
],
[
"Kirsch",
"Johannes",
""
],
[
"Stoecker",
"Horst",
""
],
[
"Struckmeier",
"Juergen",
""
],
[
"Vasak",
"David",
""
],
[
"Hanauske",
"Matthias",
""
]
] | Electromagnetism, the strong and the weak interaction are commonly formulated as gauge theories in a Lagrangian description. In this paper we present an alternative formal derivation of U(1)-gauge theory in a manifestly covariant Hamilton formalism. We make use of canonical transformations as our guiding tool to formal... | 10.053636 | 10.032882 | 10.251065 | 9.514457 | 10.85041 | 9.774068 | 10.93794 | 9.229004 | 9.873815 | 10.605531 | 9.352031 | 9.268187 | 9.402637 | 9.015285 | 9.072723 | 9.210788 | 8.830294 | 9.217604 | 9.511155 | 9.543807 | 9.045353 |
hep-th/9910008 | P. Narayana Swamy | R. Acharya and P. Narayana Swamy | No Eigenvalue in Finite Quantum Electrodynamics | 13 pages, Latex | Int.J.Mod.Phys. A12 (1997) 3799-3809 | 10.1142/S0217751X97001961 | null | hep-th | null | We re-examine Quantum Electrodynamics (QED) with massless electron as a
finite quantum field theory as advocated by Gell-Mann-Low, Baker-Johnson,
Adler, Jackiw and others. We analyze the Dyson-Schwinger equation satisfied by
the massless electron in finite QED and conclude that the theory admits no
nontrivial eigenva... | [
{
"created": "Fri, 1 Oct 1999 15:51:13 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Acharya",
"R.",
""
],
[
"Swamy",
"P. Narayana",
""
]
] | We re-examine Quantum Electrodynamics (QED) with massless electron as a finite quantum field theory as advocated by Gell-Mann-Low, Baker-Johnson, Adler, Jackiw and others. We analyze the Dyson-Schwinger equation satisfied by the massless electron in finite QED and conclude that the theory admits no nontrivial eigenvalu... | 10.864472 | 11.021267 | 10.06533 | 10.761323 | 10.244669 | 10.366851 | 10.525941 | 10.433066 | 9.484321 | 12.317326 | 9.737231 | 9.270134 | 10.07266 | 9.568428 | 10.066117 | 10.31064 | 9.444908 | 9.654362 | 9.695194 | 9.827029 | 9.536918 |
1406.4188 | Gary T. Horowitz | Eric Mefford and Gary T. Horowitz | A Simple Holographic Insulator | 14 pages, 6 figures; v2: references added | Phys. Rev. D 90, 084042 (2014) | 10.1103/PhysRevD.90.084042 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a simple holographic model of an insulator. Unlike most previous
holographic insulators, the zero temperature infrared geometry is completely
nonsingular. Both the low temperature DC conductivity and the optical
conductivity at zero temperature satisfy power laws with the same exponent,
given by the scalin... | [
{
"created": "Mon, 16 Jun 2014 22:59:09 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jul 2014 00:11:25 GMT",
"version": "v2"
}
] | 2014-10-29 | [
[
"Mefford",
"Eric",
""
],
[
"Horowitz",
"Gary T.",
""
]
] | We present a simple holographic model of an insulator. Unlike most previous holographic insulators, the zero temperature infrared geometry is completely nonsingular. Both the low temperature DC conductivity and the optical conductivity at zero temperature satisfy power laws with the same exponent, given by the scaling ... | 9.549211 | 9.222729 | 10.148725 | 7.999583 | 9.636169 | 7.599704 | 9.34702 | 7.925758 | 8.968474 | 9.483893 | 9.018284 | 8.707961 | 9.25545 | 8.435294 | 8.48189 | 8.443119 | 9.128155 | 8.597818 | 8.813968 | 9.595599 | 8.532293 |
0809.0282 | Stefano De Leo | Stefano De Leo, Pietro Rotelli | Fermion-Fermion Bound State Condition for Scalar Exchanges | null | null | 10.1103/PhysRevD.78.025006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The condition for the existence of a bound state between two fermions
exchanging massive scalars is derived. For low scalar mass, we reproduce the
scalar field model result. The high scalar mass result exhibits a somewhat
different inequality condition.
| [
{
"created": "Mon, 1 Sep 2008 17:11:19 GMT",
"version": "v1"
}
] | 2009-11-13 | [
[
"De Leo",
"Stefano",
""
],
[
"Rotelli",
"Pietro",
""
]
] | The condition for the existence of a bound state between two fermions exchanging massive scalars is derived. For low scalar mass, we reproduce the scalar field model result. The high scalar mass result exhibits a somewhat different inequality condition. | 26.871838 | 22.017616 | 21.329098 | 18.792517 | 22.94861 | 25.828978 | 22.450821 | 23.953093 | 21.919321 | 21.557142 | 23.414536 | 21.969269 | 22.255976 | 22.092922 | 22.29171 | 24.282442 | 23.255976 | 23.82263 | 22.975645 | 22.305107 | 22.825428 |
2401.03879 | Kang Zhou | Yi-Jian Du, Kang Zhou | Multi-trace YMS amplitudes from soft behavior | 39 pages, 3 figures | null | null | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | Tree level multi-trace Yang-Mills-scalar (YMS) amplitudes have been shown to
satisfy a recursive expansion formula, which expresses any YMS amplitude by
those with fewer gluons and/or scalar traces. In an earlier work, the
single-trace expansion formula has been shown to be determined by the
universality of soft beha... | [
{
"created": "Mon, 8 Jan 2024 13:20:04 GMT",
"version": "v1"
}
] | 2024-01-09 | [
[
"Du",
"Yi-Jian",
""
],
[
"Zhou",
"Kang",
""
]
] | Tree level multi-trace Yang-Mills-scalar (YMS) amplitudes have been shown to satisfy a recursive expansion formula, which expresses any YMS amplitude by those with fewer gluons and/or scalar traces. In an earlier work, the single-trace expansion formula has been shown to be determined by the universality of soft behavi... | 9.543674 | 9.266644 | 10.114527 | 8.327588 | 9.276963 | 9.426077 | 8.968609 | 8.340542 | 8.638035 | 11.58068 | 8.35408 | 8.531384 | 9.048114 | 8.635366 | 8.773052 | 8.663001 | 8.636569 | 8.669991 | 8.530681 | 8.948231 | 8.510097 |
hep-th/0401179 | V\'aclav Kare\v{s} | Vaclav Kares | 0-brane Quantum Chemistry | 26 pages, 7 figures | Nucl.Phys. B689 (2004) 53-75 | 10.1016/j.nuclphysb.2004.04.008 | null | hep-th | null | We apply two different numerical methods to solve for the boundstate of two
0-branes in three dimensions. One method is developed by us in this work and we
compare it to a method existing in the literature. In spite of considering only
three dimensional Minkowski space we obtain interesting results which should
give ... | [
{
"created": "Sat, 24 Jan 2004 12:50:20 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Kares",
"Vaclav",
""
]
] | We apply two different numerical methods to solve for the boundstate of two 0-branes in three dimensions. One method is developed by us in this work and we compare it to a method existing in the literature. In spite of considering only three dimensional Minkowski space we obtain interesting results which should give so... | 15.246416 | 13.355795 | 13.246995 | 12.76579 | 12.312751 | 12.915308 | 13.114079 | 12.782857 | 12.669861 | 15.040859 | 12.844551 | 12.687536 | 14.395919 | 13.687153 | 13.08713 | 13.630347 | 13.542845 | 13.15012 | 12.798621 | 14.496754 | 12.885809 |
hep-th/9111028 | Kresimir Demeterfi | Jean Avan and Antal Jevicki | String field actions from W-infinity | 18 pages | Mod.Phys.Lett. A7 (1992) 357-370 | 10.1142/S0217732392000306 | null | hep-th | null | Starting from $W_{\infty}$ as a fundamental symmetry and using the coadjoint
orbit method, we derive an action for one dimensional strings. It is shown that
on the simplest nontrivial orbit this gives the single scalar collective field
theory. On higher orbits one finds generalized KdV type field theories with
increa... | [
{
"created": "Fri, 15 Nov 1991 03:44:18 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Avan",
"Jean",
""
],
[
"Jevicki",
"Antal",
""
]
] | Starting from $W_{\infty}$ as a fundamental symmetry and using the coadjoint orbit method, we derive an action for one dimensional strings. It is shown that on the simplest nontrivial orbit this gives the single scalar collective field theory. On higher orbits one finds generalized KdV type field theories with increasi... | 16.733358 | 13.489518 | 20.617342 | 12.475233 | 13.643814 | 13.085882 | 12.596169 | 12.358852 | 13.064836 | 16.675579 | 13.562481 | 12.779814 | 15.932758 | 12.709189 | 13.050471 | 12.555194 | 13.145477 | 12.94693 | 12.765169 | 15.414086 | 13.469072 |
hep-th/0507178 | Kasper Peeters | Kasper Peeters, Jan Plefka and Steffen Stern | Higher-derivative gauge field terms in the M-theory action | 14 pages, 1 figure; v2: typo corrected | JHEP 0508 (2005) 095 | 10.1088/1126-6708/2005/08/095 | AEI-2005-126 | hep-th | null | We use superparticle vertex operator correlators in the light-cone gauge to
determine the (DF)^2 R^2 and (DF)^4 terms in the M-theory effective action. Our
results, when compactified on a circle, reproduce terms in the type-IIA string
effective action obtained through string amplitude calculations.
| [
{
"created": "Tue, 19 Jul 2005 14:13:32 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Aug 2005 09:18:37 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Peeters",
"Kasper",
""
],
[
"Plefka",
"Jan",
""
],
[
"Stern",
"Steffen",
""
]
] | We use superparticle vertex operator correlators in the light-cone gauge to determine the (DF)^2 R^2 and (DF)^4 terms in the M-theory effective action. Our results, when compactified on a circle, reproduce terms in the type-IIA string effective action obtained through string amplitude calculations. | 11.894294 | 10.668335 | 12.855025 | 8.528265 | 10.407745 | 8.601831 | 8.400696 | 8.595981 | 8.504452 | 14.331688 | 9.152638 | 9.793414 | 10.735942 | 9.769911 | 9.924077 | 9.275272 | 10.02507 | 9.238433 | 9.491256 | 11.250519 | 9.943652 |
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