id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0603129 | James Cline | J.J. Blanco-Pillado, C.P. Burgess, J.M. Cline, C. Escoda, M.
Gomez-Reino, R. Kallosh, A. Linde, F. Quevedo | Inflating in a Better Racetrack | 20 pages, 7 figures. Brief discussion on the non-gaussianity of this
model, one more figure of the field trajectories added as well as other minor
changes to the text | JHEP 0609:002,2006 | 10.1088/1126-6708/2006/09/002 | DAMTP-2006-20, SU-ITP-06-07 | hep-th astro-ph gr-qc hep-ph | null | We present a new version of our racetrack inflation scenario which, unlike
our original proposal, is based on an explicit compactification of type IIB
string theory: the Calabi-Yau manifold P^4_[1,1,1,6,9]. The axion-dilaton and
all complex structure moduli are stabilized by fluxes. The remaining 2 Kahler
moduli are ... | [
{
"created": "Thu, 16 Mar 2006 23:04:24 GMT",
"version": "v1"
},
{
"created": "Tue, 23 May 2006 20:33:27 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Blanco-Pillado",
"J. J.",
""
],
[
"Burgess",
"C. P.",
""
],
[
"Cline",
"J. M.",
""
],
[
"Escoda",
"C.",
""
],
[
"Gomez-Reino",
"M.",
""
],
[
"Kallosh",
"R.",
""
],
[
"Linde",
"A.",
""
],
[
"Quevedo... | We present a new version of our racetrack inflation scenario which, unlike our original proposal, is based on an explicit compactification of type IIB string theory: the Calabi-Yau manifold P^4_[1,1,1,6,9]. The axion-dilaton and all complex structure moduli are stabilized by fluxes. The remaining 2 Kahler moduli are st... | 6.577198 | 6.094866 | 7.501272 | 5.857011 | 6.22421 | 6.279195 | 6.064581 | 6.15708 | 6.071654 | 7.462572 | 6.157667 | 6.301398 | 6.669146 | 6.135907 | 6.182626 | 6.061097 | 6.132376 | 6.262999 | 6.113567 | 6.646897 | 6.206876 |
hep-th/9907153 | Atsushi Nakamula | Masaru Kamata and Atsushi Nakamula | One-parameter family of selfdual solutions in classical Yang-Mills
theory | 11 pages, Latex, no figures | Phys.Lett. B463 (1999) 257-262 | 10.1016/S0370-2693(99)00981-8 | null | hep-th | null | The ADHM construction, which yields (anti-)selfdual configurations in
classical Yang-Mills theories, is applied to an infinite dimensional l^2 vector
space, and as a consequence, a family of (anti-)selfdual configurations with a
parameter q is obtained for SU(2) Yang-Mills theory. This l^2 formulation can
be seen as ... | [
{
"created": "Mon, 19 Jul 1999 08:55:48 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Kamata",
"Masaru",
""
],
[
"Nakamula",
"Atsushi",
""
]
] | The ADHM construction, which yields (anti-)selfdual configurations in classical Yang-Mills theories, is applied to an infinite dimensional l^2 vector space, and as a consequence, a family of (anti-)selfdual configurations with a parameter q is obtained for SU(2) Yang-Mills theory. This l^2 formulation can be seen as a ... | 9.885832 | 9.777648 | 10.47057 | 8.342651 | 9.438594 | 9.037406 | 8.975688 | 8.845194 | 8.758788 | 11.45472 | 8.777616 | 9.151581 | 9.710645 | 9.140496 | 8.924085 | 9.118282 | 9.349483 | 8.937499 | 9.084799 | 9.467534 | 9.013929 |
1812.03870 | Laurent Baulieu | Laurent Baulieu | On Stochastic Quantisation of Supersymmetric Theories | null | null | 10.1016/j.physletb.2019.01.048 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explain how stochastic TQFT supersymmetry can be made compatible with
space supersymmetry. Taking the case of N=2 supersymmetric quantum mechanics,
(the proof would be the same for the Wess-Zumino model), we determine the
kernels that ensure the convergence of the stochastic process toward the
standard path integr... | [
{
"created": "Mon, 10 Dec 2018 15:22:57 GMT",
"version": "v1"
}
] | 2019-03-27 | [
[
"Baulieu",
"Laurent",
""
]
] | We explain how stochastic TQFT supersymmetry can be made compatible with space supersymmetry. Taking the case of N=2 supersymmetric quantum mechanics, (the proof would be the same for the Wess-Zumino model), we determine the kernels that ensure the convergence of the stochastic process toward the standard path integral... | 14.490412 | 14.354377 | 17.502275 | 13.829957 | 13.712488 | 15.521174 | 14.063095 | 15.037158 | 14.466018 | 15.883157 | 14.528527 | 13.649635 | 14.300385 | 13.907877 | 14.944229 | 14.659327 | 13.82525 | 14.130296 | 13.908603 | 15.085535 | 13.549162 |
hep-th/0205150 | Martijn G. C. Eenink | A. Collinucci, M. de Roo, M. G. C. Eenink | Supersymmetric Yang-Mills theory at order alpha'^3 | 15 pages LaTeX | JHEP 0206 (2002) 024 | 10.1088/1126-6708/2002/06/024 | UG-02/39 | hep-th | null | We construct the order alpha'^3 terms in the supersymmetric Yang-Mills action
in ten dimensions for an arbitrary gauge group. The result can be expressed in
terms of the structure constants of the Yang-Mills group, and is therefore
independent of abelian factors. The alpha'^3 invariant obtained here is
independent of... | [
{
"created": "Wed, 15 May 2002 14:57:13 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Collinucci",
"A.",
""
],
[
"de Roo",
"M.",
""
],
[
"Eenink",
"M. G. C.",
""
]
] | We construct the order alpha'^3 terms in the supersymmetric Yang-Mills action in ten dimensions for an arbitrary gauge group. The result can be expressed in terms of the structure constants of the Yang-Mills group, and is therefore independent of abelian factors. The alpha'^3 invariant obtained here is independent of t... | 11.241638 | 10.479833 | 12.216999 | 9.514519 | 9.136319 | 11.048966 | 10.074806 | 10.193774 | 9.306844 | 13.553025 | 8.771253 | 9.172732 | 10.155107 | 9.337941 | 9.03891 | 9.442411 | 9.22103 | 8.993561 | 9.128876 | 10.166396 | 9.347134 |
2011.01960 | Till Heckelbacher | Martin Enriquez-Rojo and Till Heckelbacher | Asymptotic symmetries in spatially flat FRW | 44 pages | Phys. Rev. D 103, 064009 (2021) | 10.1103/PhysRevD.103.064009 | LMU-ASC 42/20 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform an off-shell treatment of asymptotically decelerating spatially
flat FRW spacetimes at future null infinity. We obtain supertranslation and
superrotation-like asymptotic diffeomorphisms which are consistent with the
global symmetries of FRW and we compute how the asymptotic data is transformed
under them. ... | [
{
"created": "Tue, 3 Nov 2020 19:04:33 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Jul 2021 14:36:03 GMT",
"version": "v2"
}
] | 2021-07-22 | [
[
"Enriquez-Rojo",
"Martin",
""
],
[
"Heckelbacher",
"Till",
""
]
] | We perform an off-shell treatment of asymptotically decelerating spatially flat FRW spacetimes at future null infinity. We obtain supertranslation and superrotation-like asymptotic diffeomorphisms which are consistent with the global symmetries of FRW and we compute how the asymptotic data is transformed under them. Fu... | 10.691677 | 13.254894 | 10.639877 | 9.73365 | 9.946739 | 10.788767 | 13.553714 | 9.977034 | 11.636898 | 12.63359 | 10.947115 | 10.661439 | 10.182432 | 9.931681 | 10.166468 | 10.490333 | 10.056732 | 9.980193 | 9.852545 | 10.551796 | 9.857417 |
hep-th/0609175 | S. Stieberger | Stephan Stieberger, Tomasz R. Taylor | Multi-Gluon Scattering in Open Superstring Theory | 34 pages, REVTeX, 2 figs | Phys.Rev.D74:126007,2006 | 10.1103/PhysRevD.74.126007 | LMU-ASC 50/06 | hep-th hep-ph math.NT | null | We discuss the amplitudes describing N-gluon scattering in type I superstring
theory, on a disk world-sheet. After reviewing the general structure of
amplitudes and the complications created by the presence of a large number of
vertices at the boundary, we focus on the most promising case of maximally
helicity violat... | [
{
"created": "Mon, 25 Sep 2006 20:23:54 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Oct 2006 21:25:05 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Stieberger",
"Stephan",
""
],
[
"Taylor",
"Tomasz R.",
""
]
] | We discuss the amplitudes describing N-gluon scattering in type I superstring theory, on a disk world-sheet. After reviewing the general structure of amplitudes and the complications created by the presence of a large number of vertices at the boundary, we focus on the most promising case of maximally helicity violatin... | 9.514962 | 9.588055 | 11.330829 | 9.48837 | 10.782343 | 10.374189 | 10.321804 | 10.279627 | 10.139314 | 11.504043 | 9.200393 | 9.29292 | 9.298425 | 9.196265 | 9.14826 | 9.219989 | 9.271783 | 9.26805 | 9.342457 | 9.697325 | 9.102523 |
1807.06579 | Mafalda Dias | Mafalda Dias, Jonathan Frazer, Ander Retolaza, Alexander Westphal | Primordial Gravitational Waves and the Swampland | 4 pages, 2 figures. References added to match published version | Fortsch.Phys. 67 (2019) no.1-2, 1800063 | null | DESY-18-125 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The swampland conjectures seek to distinguish effective field theories which
can be consistently embedded in a theory of quantum gravity from those which
can not (and are hence referred to as being in the swampland). We consider two
such conjectures, known as the Swampland Distance and de Sitter Conjectures,
showing ... | [
{
"created": "Tue, 17 Jul 2018 17:45:50 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Apr 2019 01:41:26 GMT",
"version": "v2"
}
] | 2019-04-04 | [
[
"Dias",
"Mafalda",
""
],
[
"Frazer",
"Jonathan",
""
],
[
"Retolaza",
"Ander",
""
],
[
"Westphal",
"Alexander",
""
]
] | The swampland conjectures seek to distinguish effective field theories which can be consistently embedded in a theory of quantum gravity from those which can not (and are hence referred to as being in the swampland). We consider two such conjectures, known as the Swampland Distance and de Sitter Conjectures, showing th... | 6.913955 | 6.606888 | 6.770532 | 5.889678 | 6.257038 | 5.935123 | 6.115697 | 6.112366 | 5.767492 | 7.338552 | 5.574867 | 5.734251 | 5.625209 | 5.9825 | 6.040618 | 5.840972 | 5.905103 | 5.650395 | 5.835623 | 5.888009 | 5.711112 |
hep-th/0608031 | Yuuichirou Shibusa | T. Aoyama, T. Kuroki and Y. Shibusa | Dynamical Generation of Non-Abelian Gauge Group via the Improved
Perturbation Theory | 31 pages, published version | Phys.Rev.D74:106004,2006 | 10.1103/PhysRevD.74.106004 | RIKEN-TH-75 | hep-th | null | It was suggested that the massive Yang-Mills-Chern-Simons matrix model has
three phases and that in one of them a non-Abelian gauge symmetry is
dynamically generated. The analysis was at the one-loop level around a
classical solution of fuzzy sphere type. We obtain evidences that three phases
are indeed realized as n... | [
{
"created": "Fri, 4 Aug 2006 08:37:27 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Nov 2006 07:46:22 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Aoyama",
"T.",
""
],
[
"Kuroki",
"T.",
""
],
[
"Shibusa",
"Y.",
""
]
] | It was suggested that the massive Yang-Mills-Chern-Simons matrix model has three phases and that in one of them a non-Abelian gauge symmetry is dynamically generated. The analysis was at the one-loop level around a classical solution of fuzzy sphere type. We obtain evidences that three phases are indeed realized as non... | 10.089864 | 9.330248 | 10.2052 | 8.597172 | 9.635101 | 9.572092 | 9.906093 | 8.906674 | 9.006457 | 10.107199 | 9.122961 | 9.373713 | 9.62923 | 9.525927 | 9.31354 | 9.212276 | 9.089162 | 9.276378 | 9.249757 | 9.563515 | 9.283595 |
hep-th/0203140 | Jeremy Michelson | Jeremy Michelson | (Twisted) Toroidal Compactification of pp-Waves | 22 pages REVTeX 4 and AMSLaTeX. v3: References and a paragraph on
nine dimensional Killing spinors were added. v4: A few typos corrected and a
footnote was modified | Phys.Rev.D66:066002,2002 | 10.1103/PhysRevD.66.066002 | RUNHETC-2002-08 | hep-th | null | The maximally supersymmetric type IIB pp-wave is compactified on spatial
circles, with and without an auxiliary rotational twist. All spatial circles of
constant radius are identified. Without the twist, an S$^1$ compactification
can preserve 24, 20 or 16 supercharges. $T^2$ compactifications can preserve
20, 18 or 1... | [
{
"created": "Fri, 15 Mar 2002 00:25:45 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Mar 2002 00:28:51 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Mar 2002 19:36:46 GMT",
"version": "v3"
},
{
"created": "Thu, 2 May 2002 14:28:55 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Michelson",
"Jeremy",
""
]
] | The maximally supersymmetric type IIB pp-wave is compactified on spatial circles, with and without an auxiliary rotational twist. All spatial circles of constant radius are identified. Without the twist, an S$^1$ compactification can preserve 24, 20 or 16 supercharges. $T^2$ compactifications can preserve 20, 18 or 16 ... | 9.809323 | 9.517381 | 10.402746 | 8.651888 | 9.218848 | 9.740092 | 9.290421 | 9.036258 | 8.958643 | 12.06291 | 8.412601 | 8.755739 | 10.263067 | 9.060877 | 8.705263 | 8.861725 | 9.164203 | 8.991865 | 9.015625 | 9.92643 | 8.889448 |
1003.4485 | John Baez | John C. Baez, John Huerta | An Invitation to Higher Gauge Theory | 60 pages, based on lectures at the 2nd School and Workshop on Quantum
Gravity and Quantum Geometry at the 2009 Corfu Summer Institute | General Relativity and Gravitation 43 (2011), 2335-2392 | 10.1007/s10714-010-1070-9 | null | hep-th gr-qc math.CT math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this easy introduction to higher gauge theory, we describe parallel
transport for particles and strings in terms of 2-connections on 2-bundles.
Just as ordinary gauge theory involves a gauge group, this generalization
involves a gauge '2-group'. We focus on 6 examples. First, every abelian Lie
group gives a Lie 2-... | [
{
"created": "Tue, 23 Mar 2010 18:12:52 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Feb 2015 01:09:26 GMT",
"version": "v2"
}
] | 2015-05-18 | [
[
"Baez",
"John C.",
""
],
[
"Huerta",
"John",
""
]
] | In this easy introduction to higher gauge theory, we describe parallel transport for particles and strings in terms of 2-connections on 2-bundles. Just as ordinary gauge theory involves a gauge group, this generalization involves a gauge '2-group'. We focus on 6 examples. First, every abelian Lie group gives a Lie 2-gr... | 4.611766 | 5.294222 | 5.431921 | 5.138114 | 5.416265 | 5.310767 | 5.290675 | 5.028581 | 5.079768 | 5.529625 | 4.780268 | 4.771187 | 4.935321 | 4.657269 | 4.664943 | 4.666206 | 4.692565 | 4.602399 | 4.743397 | 4.862374 | 4.661918 |
2406.18182 | John Gracey | J.A. Gracey | Perspective on properties of renormalization schemes at high loops | 10 latex pages | null | null | LTH 1374 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We report on recent work on a class of renormalization schemes in QCD, termed
the MOMt schemes. None of the renormalization group functions of the eight QCD
MOMt schemes involve even zetas to five loops. A new scheme is introduced for
scalar $\phi^3$ theory in six dimensions where the full Laurent series in the
regul... | [
{
"created": "Wed, 26 Jun 2024 08:58:17 GMT",
"version": "v1"
}
] | 2024-06-27 | [
[
"Gracey",
"J. A.",
""
]
] | We report on recent work on a class of renormalization schemes in QCD, termed the MOMt schemes. None of the renormalization group functions of the eight QCD MOMt schemes involve even zetas to five loops. A new scheme is introduced for scalar $\phi^3$ theory in six dimensions where the full Laurent series in the regular... | 20.506462 | 18.225142 | 17.200132 | 17.023144 | 21.389744 | 20.881552 | 20.541258 | 19.830952 | 16.786509 | 19.404608 | 18.657497 | 19.592915 | 16.972725 | 17.369879 | 19.481823 | 17.853889 | 18.452631 | 18.62208 | 16.63133 | 18.160322 | 17.999945 |
1708.08409 | Anirban Basu | Anirban Basu | Low momentum expansion of one loop amplitudes in heterotic string theory | 67 pages, LaTeX, 14 figures | null | 10.1007/JHEP11(2017)139 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the low momentum expansion of the four graviton and the two
graviton--two gluon amplitudes in heterotic string theory at one loop in ten
dimensions, and analyze contributions upto the D^2 R^4 interaction from the
four graviton amplitude, and the D^4 R^2 F^2 interaction from the two
graviton--two gluon amp... | [
{
"created": "Mon, 28 Aug 2017 16:43:00 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Sep 2017 15:26:42 GMT",
"version": "v2"
}
] | 2018-01-17 | [
[
"Basu",
"Anirban",
""
]
] | We consider the low momentum expansion of the four graviton and the two graviton--two gluon amplitudes in heterotic string theory at one loop in ten dimensions, and analyze contributions upto the D^2 R^4 interaction from the four graviton amplitude, and the D^4 R^2 F^2 interaction from the two graviton--two gluon ampli... | 9.533379 | 7.733098 | 10.596765 | 7.737782 | 8.75526 | 8.451989 | 7.919846 | 8.200641 | 7.443181 | 10.859694 | 7.166647 | 7.986089 | 9.012465 | 8.077994 | 8.283119 | 8.238123 | 7.722435 | 8.12289 | 7.936569 | 9.447904 | 8.357551 |
0801.0619 | Changhyun Ahn | Changhyun Ahn | Meta-Stable Brane Configurations by Quartic Superpotential for
Bifundamentals | 30 pp, 8 figures; pages 7 and 14 improved; to appear in IJMPA | Int.J.Mod.Phys.A24:5697-5724,2009 | 10.1142/S0217751X09044711 | KIAS-P08001 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The type IIA nonsupersymmetric meta-stable brane configuration consisting of
three NS5-branes, D4-branes and anti-D4-branes where the electric gauge theory
superpotential has a quartic term for the bifundamentals besides a mass term is
constructed. By adding the orientifold 4-plane and 6-plane to this brane
configura... | [
{
"created": "Fri, 4 Jan 2008 01:27:38 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 2008 04:56:43 GMT",
"version": "v2"
},
{
"created": "Sat, 14 Mar 2009 03:06:38 GMT",
"version": "v3"
}
] | 2010-03-04 | [
[
"Ahn",
"Changhyun",
""
]
] | The type IIA nonsupersymmetric meta-stable brane configuration consisting of three NS5-branes, D4-branes and anti-D4-branes where the electric gauge theory superpotential has a quartic term for the bifundamentals besides a mass term is constructed. By adding the orientifold 4-plane and 6-plane to this brane configurati... | 8.575365 | 5.919483 | 10.50557 | 6.141288 | 5.808812 | 6.176901 | 5.868635 | 5.567005 | 6.233674 | 11.227956 | 6.519823 | 7.332219 | 8.777516 | 7.614775 | 7.448957 | 7.600251 | 7.765416 | 7.574636 | 7.526745 | 8.907964 | 7.745993 |
hep-th/9604197 | Armen Nersessian | A. Nersessian, V. Ter-Antonyan, M. Tsulaia | A note on quantum Bohlin transformation | 6 pages, LaTeX | Mod.Phys.Lett. A11 (1996) 1605-1611 | 10.1142/S0217732396001600 | null | hep-th | null | It is shown, that the reduction of the circular quantum oscillator by the
$Z_2$-group action results to the two systems: a two-dimensional hydrogen atom,
and a ``charge - charged magnetic vortex" one, with the spin $\frac 12$.
Analogously, the $Z_N$-reduction of the two-dimensional system with the central
potential $... | [
{
"created": "Tue, 30 Apr 1996 18:25:05 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Nersessian",
"A.",
""
],
[
"Ter-Antonyan",
"V.",
""
],
[
"Tsulaia",
"M.",
""
]
] | It is shown, that the reduction of the circular quantum oscillator by the $Z_2$-group action results to the two systems: a two-dimensional hydrogen atom, and a ``charge - charged magnetic vortex" one, with the spin $\frac 12$. Analogously, the $Z_N$-reduction of the two-dimensional system with the central potential $r^... | 10.127126 | 8.985555 | 9.794164 | 9.099991 | 9.820297 | 9.151431 | 9.965071 | 9.683588 | 8.86346 | 10.688652 | 9.132809 | 9.306338 | 9.050511 | 8.617418 | 9.2839 | 9.179035 | 9.220795 | 9.015017 | 9.040373 | 9.195584 | 9.155851 |
2203.02747 | Ugo Moschella | Emil Akhmedov, Henri Epstein and Ugo Moschella | The massless thermal field and the thermal fermion bosonization in two
dimensions | null | null | 10.1007/JHEP09(2022)123 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We come back to the issue of bosonization of fermions in two spacetime
dimension and give a new costruction in the steady state case where left and
right moving particles can coexist at two different temperatures. A crucial
role in our construction is played by translation invariant infrared states and
the correspond... | [
{
"created": "Sat, 5 Mar 2022 13:58:22 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Aug 2022 22:20:25 GMT",
"version": "v2"
}
] | 2022-09-28 | [
[
"Akhmedov",
"Emil",
""
],
[
"Epstein",
"Henri",
""
],
[
"Moschella",
"Ugo",
""
]
] | We come back to the issue of bosonization of fermions in two spacetime dimension and give a new costruction in the steady state case where left and right moving particles can coexist at two different temperatures. A crucial role in our construction is played by translation invariant infrared states and the correspondin... | 14.047168 | 12.059937 | 14.600963 | 12.534 | 12.896627 | 12.762792 | 11.352475 | 12.651367 | 12.066604 | 16.515497 | 12.614862 | 13.012145 | 13.239891 | 12.758031 | 12.904205 | 12.748453 | 13.250597 | 12.900296 | 13.434989 | 14.130876 | 12.723894 |
1811.11442 | Chethan Gowdigere | Chethan N Gowdigere, Jagannath Santara and Sumedha | Conformal Bootstrap Signatures of the Tricritical Ising Universality
Class | version published in Physical Review D, improved and additional
figures, expanded version | Phys. Rev. D 101, 116020 (2020) | 10.1103/PhysRevD.101.116020 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the tricritical Ising universality class using conformal bootstrap
techniques. By studying bootstrap constraints originating from multiple
correlators on the CFT data of multiple OPEs, we are able to determine the
scaling dimension of the spin field $\Delta_\sigma$ in various non-integer
dimensions $2 \le d ... | [
{
"created": "Wed, 28 Nov 2018 08:38:50 GMT",
"version": "v1"
},
{
"created": "Mon, 10 May 2021 06:22:27 GMT",
"version": "v2"
}
] | 2021-05-11 | [
[
"Gowdigere",
"Chethan N",
""
],
[
"Santara",
"Jagannath",
""
],
[
"Sumedha",
"",
""
]
] | We study the tricritical Ising universality class using conformal bootstrap techniques. By studying bootstrap constraints originating from multiple correlators on the CFT data of multiple OPEs, we are able to determine the scaling dimension of the spin field $\Delta_\sigma$ in various non-integer dimensions $2 \le d \l... | 6.666919 | 7.0722 | 6.603729 | 6.379297 | 7.34251 | 7.598735 | 6.440723 | 6.603689 | 6.031089 | 7.692285 | 6.662547 | 6.608806 | 6.316299 | 6.207398 | 6.57509 | 6.532315 | 6.27984 | 6.428643 | 6.144542 | 6.74127 | 6.094211 |
hep-th/9602177 | Juergen Schulze | J\"urgen Schulze | Coulomb Gas on the Half Plane | 27 pages, elsart, epsf, 4 figures, one example added, accepted for
publication in Nuclear Physics B | Nucl.Phys. B489 (1997) 580-602 | 10.1016/S0550-3213(97)00021-7 | null | hep-th | null | The Coulomb-gas description of minimal models is considered on the half
plane. Screening prescriptions are developed by the perturbative expansion of
the Liouville theory with imaginary coupling and with Neumann boundary
condition on the bosonic field. To generate the conformal blocks of more
general boundary conditi... | [
{
"created": "Thu, 29 Feb 1996 22:14:21 GMT",
"version": "v1"
},
{
"created": "Sun, 22 Dec 1996 00:30:31 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Schulze",
"Jürgen",
""
]
] | The Coulomb-gas description of minimal models is considered on the half plane. Screening prescriptions are developed by the perturbative expansion of the Liouville theory with imaginary coupling and with Neumann boundary condition on the bosonic field. To generate the conformal blocks of more general boundary condition... | 18.028946 | 17.739803 | 22.019081 | 15.945498 | 15.221203 | 14.511812 | 15.578557 | 15.942487 | 15.757483 | 19.168692 | 15.347476 | 15.657801 | 20.297043 | 16.226425 | 16.338797 | 15.583065 | 16.510918 | 15.168694 | 15.696343 | 20.15361 | 15.389949 |
2203.07386 | Andrea Fontanella | Andrea Fontanella and Stijn J. van Tongeren | Coset space actions for nonrelativistic strings | 28 pages, v3: introduction and references improved, matching the
published version in JHEP | null | 10.1007/JHEP06(2022)080 | HU-EP-22/09 | hep-th | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We formulate the stringy nonrelativistic limits of the flat space and
AdS$_5\times$S$^5$ string as coset models, based on the string Bargmann and
extended string Newton-Hooke algebras respectively. Our construction mimics the
typical relativistic one, but differs in several interesting ways. Using our
coset formulati... | [
{
"created": "Mon, 14 Mar 2022 18:00:01 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Mar 2022 20:00:56 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Jun 2022 09:55:14 GMT",
"version": "v3"
}
] | 2022-07-06 | [
[
"Fontanella",
"Andrea",
""
],
[
"van Tongeren",
"Stijn J.",
""
]
] | We formulate the stringy nonrelativistic limits of the flat space and AdS$_5\times$S$^5$ string as coset models, based on the string Bargmann and extended string Newton-Hooke algebras respectively. Our construction mimics the typical relativistic one, but differs in several interesting ways. Using our coset formulation... | 13.133272 | 9.082026 | 13.556207 | 9.867476 | 10.477077 | 9.926394 | 9.899389 | 9.508374 | 10.007389 | 16.959808 | 9.798536 | 10.73249 | 12.957776 | 10.938044 | 10.944239 | 10.303887 | 10.406184 | 10.771028 | 10.994578 | 13.728801 | 10.102024 |
hep-th/0703170 | Omid Saremi | Omid Saremi | Shear Waves, Sound Waves On A Shimmering Horizon | McGill University | null | null | null | hep-th | null | In the context of the so called ``membrane paradigm'' of black holes/branes,
it has been known for sometime that the dynamics of small fluctuations on the
stretched horizon can be viewed as corresponding to diffusion of a conserved
charge in simple fluids. To study shear waves in this context properly, one
must defin... | [
{
"created": "Mon, 19 Mar 2007 19:36:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Saremi",
"Omid",
""
]
] | In the context of the so called ``membrane paradigm'' of black holes/branes, it has been known for sometime that the dynamics of small fluctuations on the stretched horizon can be viewed as corresponding to diffusion of a conserved charge in simple fluids. To study shear waves in this context properly, one must define ... | 7.709028 | 8.796986 | 8.137915 | 7.23539 | 8.372299 | 8.054946 | 8.205023 | 7.709005 | 7.913475 | 8.582262 | 7.47328 | 7.421927 | 7.710936 | 7.396598 | 7.561502 | 7.290048 | 7.513332 | 7.263522 | 7.560145 | 7.390853 | 7.277879 |
hep-th/0307005 | Masatoshi Sato | Masatoshi Sato | Non-Abelian Statistics of Axion Strings | 10 pages, 1 figure, references and comments added | Phys.Lett. B575 (2003) 126-130 | 10.1016/j.physletb.2003.09.047 | null | hep-th | null | We examine an axion string coupled to a Majorana fermion. It is found that
there exist a Majorana-Weyl zero mode on the string. Due to the zero mode, the
axion strings obey non-abelian statistics.
| [
{
"created": "Tue, 1 Jul 2003 07:44:26 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Sep 2003 04:02:39 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Sato",
"Masatoshi",
""
]
] | We examine an axion string coupled to a Majorana fermion. It is found that there exist a Majorana-Weyl zero mode on the string. Due to the zero mode, the axion strings obey non-abelian statistics. | 10.276214 | 8.98803 | 8.442079 | 8.028457 | 8.821836 | 8.159508 | 8.65255 | 7.841999 | 8.126609 | 9.537127 | 8.638472 | 8.534106 | 9.193576 | 8.394741 | 8.747869 | 8.303705 | 8.285452 | 8.131528 | 8.174961 | 9.379655 | 8.544575 |
hep-th/9410163 | R. Jagannathan | R. Chakrabarti and R. Jagannathan | On a nonstandard two-parametric quantum algebra and its connections with
$U_{p,q}(gl(2))$ and $U_{p,q}(gl(1|1))$ | 17pages, LaTeX, Preprint No. imsc-94/43 Revised version: A note added
at the end of the paper correcting and clarifying the bibliography | Z.Phys. C66 (1995) 523-528 | 10.1007/BF01556381 | null | hep-th | null | A quantum algebra $U_{p,q}(\zeta ,H,X_\pm )$ associated with a nonstandard
$R$-matrix with two deformation parameters$(p,q)$ is studied and, in
particular, its universal ${\cal R}$-matrix is derived using Reshetikhin's
method. Explicit construction of the $(p,q)$-dependent nonstandard $R$-matrix
is obtained through a... | [
{
"created": "Fri, 21 Oct 1994 15:09:18 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Oct 1994 14:11:27 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Chakrabarti",
"R.",
""
],
[
"Jagannathan",
"R.",
""
]
] | A quantum algebra $U_{p,q}(\zeta ,H,X_\pm )$ associated with a nonstandard $R$-matrix with two deformation parameters$(p,q)$ is studied and, in particular, its universal ${\cal R}$-matrix is derived using Reshetikhin's method. Explicit construction of the $(p,q)$-dependent nonstandard $R$-matrix is obtained through a c... | 5.514483 | 5.745751 | 6.06952 | 5.340572 | 5.841341 | 5.388532 | 5.441966 | 5.496883 | 5.303541 | 6.100325 | 5.392989 | 5.571937 | 5.482194 | 5.454207 | 5.379051 | 5.467507 | 5.664895 | 5.411299 | 5.401401 | 5.645323 | 5.362398 |
1608.07795 | Anastasios Petkou | E. G. Filothodoros, A. C. Petkou and N. D. Vlachos | $3d$ fermion-boson map with imaginary chemical potential | 19 pages | Phys. Rev. D 95, 065029 (2017) | 10.1103/PhysRevD.95.065029 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the three-dimensional $U(N)$ Gross-Neveu and CP$^{N-1}$ models in
the canonical formalism with fixed $U(1)$ charge. For large-$N$ this is closely
related to coupling the models to abelian Chern-Simons in a monopole
background. We show that the presence of the imaginary chemical potential for
the $U(1)$ charg... | [
{
"created": "Sun, 28 Aug 2016 10:00:14 GMT",
"version": "v1"
}
] | 2017-04-05 | [
[
"Filothodoros",
"E. G.",
""
],
[
"Petkou",
"A. C.",
""
],
[
"Vlachos",
"N. D.",
""
]
] | We study the three-dimensional $U(N)$ Gross-Neveu and CP$^{N-1}$ models in the canonical formalism with fixed $U(1)$ charge. For large-$N$ this is closely related to coupling the models to abelian Chern-Simons in a monopole background. We show that the presence of the imaginary chemical potential for the $U(1)$ charge ... | 7.990808 | 6.357149 | 8.740016 | 6.95943 | 7.050566 | 7.155035 | 7.324509 | 6.894745 | 7.041873 | 9.179536 | 6.694852 | 7.295995 | 8.003427 | 7.218455 | 7.338036 | 7.425196 | 7.137486 | 7.285276 | 7.378545 | 7.87468 | 7.356952 |
hep-th/0509097 | Jeff Harvey | Jeffrey A. Harvey | TASI 2003 Lectures on Anomalies | 59 pages, no figures | null | null | EFI 05-16 | hep-th | null | These lecture notes review the structure of anomalies and present some of
their applications in field theory, string theory and M theory. They expand on
material presented at the TASI 2003 summer school and the 2005 International
Spring School on String Theory in Hangzhou, China.
| [
{
"created": "Tue, 13 Sep 2005 18:15:29 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Harvey",
"Jeffrey A.",
""
]
] | These lecture notes review the structure of anomalies and present some of their applications in field theory, string theory and M theory. They expand on material presented at the TASI 2003 summer school and the 2005 International Spring School on String Theory in Hangzhou, China. | 9.163645 | 7.643603 | 8.931806 | 7.142131 | 7.312387 | 7.445859 | 7.741765 | 6.92654 | 6.817183 | 8.247183 | 6.727525 | 6.958794 | 7.89337 | 6.655111 | 7.035138 | 7.317429 | 7.06114 | 7.199898 | 6.873937 | 7.566471 | 6.75888 |
2003.02827 | Mich\`ele Levi | Mich\`ele Levi, Andrew J. McLeod, Matthew von Hippel | N$^3$LO gravitational spin-orbit coupling at order $G^4$ | 27 pp, 11 figures, 1 table, 30 pp PDF appendix, ancillary .m file,
published | JHEP 2107 (2021) 115 | 10.1007/JHEP07(2021)115 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we derive for the first time the N$^3$LO gravitational
spin-orbit coupling at order $G^4$ in the post-Newtonian (PN) approximation
within the effective field theory (EFT) of gravitating spinning objects. This
represents the first computation in a spinning sector involving three-loop
integration. We prov... | [
{
"created": "Thu, 5 Mar 2020 18:55:39 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Jan 2021 22:21:19 GMT",
"version": "v2"
},
{
"created": "Mon, 19 Jul 2021 15:21:18 GMT",
"version": "v3"
}
] | 2021-07-20 | [
[
"Levi",
"Michèle",
""
],
[
"McLeod",
"Andrew J.",
""
],
[
"von Hippel",
"Matthew",
""
]
] | In this paper we derive for the first time the N$^3$LO gravitational spin-orbit coupling at order $G^4$ in the post-Newtonian (PN) approximation within the effective field theory (EFT) of gravitating spinning objects. This represents the first computation in a spinning sector involving three-loop integration. We provid... | 8.91265 | 8.461653 | 9.087916 | 7.961075 | 8.591449 | 8.630902 | 9.112563 | 7.923923 | 7.979387 | 9.879647 | 8.312286 | 8.371964 | 8.625087 | 8.364219 | 8.439854 | 7.963706 | 8.499625 | 8.088773 | 8.509847 | 8.607406 | 8.390381 |
hep-th/0109215 | Kazuyuki Fujii | Kazuyuki Fujii | Geometry of Generalized Coherent States : Some Calculations of Chern
Characters | Latex File, 1+22 pages | null | null | null | hep-th math-ph math.MP quant-ph | null | This is a continuation of the preceding paper (hep-ph/0108219).
First of all we make a brief review of generalized coherent states based on
Lie algebra su(1,1) and prove that the resolution of unity can be obtained by
the curvature form of some bundle. Next for a set of generalized coherent
states we define a unive... | [
{
"created": "Fri, 28 Sep 2001 02:24:51 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Fujii",
"Kazuyuki",
""
]
] | This is a continuation of the preceding paper (hep-ph/0108219). First of all we make a brief review of generalized coherent states based on Lie algebra su(1,1) and prove that the resolution of unity can be obtained by the curvature form of some bundle. Next for a set of generalized coherent states we define a universal... | 13.267367 | 13.080775 | 13.333884 | 11.903164 | 13.818216 | 13.113935 | 12.922605 | 12.179251 | 11.765846 | 12.616442 | 12.122087 | 12.083117 | 12.877271 | 11.795914 | 12.271371 | 12.162756 | 12.17251 | 11.80635 | 11.759625 | 11.957088 | 12.054058 |
hep-th/0606012 | Boris Kors | Henriette Elvang, Daniel Z. Freedman, and Boris Kors | Anomaly Cancellation in Supergravity with Fayet-Iliopoulos Couplings | 27 pages | JHEP 0611:068,2006 | 10.1088/1126-6708/2006/11/068 | CERN-PH-TH/2006-086, MIT-CTP-3743 | hep-th | null | We review and clarify the cancellation conditions for gauge anomalies which
occur when N=1, D=4 supergravity is coupled to a Kahler non-linear sigma-model
with gauged isometries and Fayet-Iliopoulos couplings. For a flat sigma-model
target space and vanishing Fayet-Iliopoulos couplings, consistency requires
just the ... | [
{
"created": "Thu, 1 Jun 2006 14:40:56 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Elvang",
"Henriette",
""
],
[
"Freedman",
"Daniel Z.",
""
],
[
"Kors",
"Boris",
""
]
] | We review and clarify the cancellation conditions for gauge anomalies which occur when N=1, D=4 supergravity is coupled to a Kahler non-linear sigma-model with gauged isometries and Fayet-Iliopoulos couplings. For a flat sigma-model target space and vanishing Fayet-Iliopoulos couplings, consistency requires just the co... | 7.430214 | 6.464766 | 7.299378 | 6.309837 | 6.400592 | 6.87678 | 6.677264 | 6.447632 | 6.561133 | 7.517025 | 6.51168 | 6.790044 | 6.938189 | 6.599468 | 6.640024 | 6.645267 | 6.645606 | 6.769174 | 6.667619 | 6.729228 | 6.553113 |
1108.0551 | Michele Maio | M. Maio | Simple current extensions and permutation orbifolds in string theory | 5 pages, 4 figures, extended version of the Proceedings of the
Cargese Summer School 2010 "Formal Developments and Applications" | Nucl. Phys. B (Proc. Suppl.) 216 (2011) 252 | 10.1016/j.nuclphysbps.2011.05.004 | NIKHEF/2011-023 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review extensions by integer spin simple currents in two-dimensional
conformal field theories and their applications in string theory. In
particular, we study the problem of resolving the fixed points of a simple
current and apply the formalism to the permutation orbifold. In terms of string
compactifications, we ... | [
{
"created": "Tue, 2 Aug 2011 11:52:28 GMT",
"version": "v1"
}
] | 2011-08-03 | [
[
"Maio",
"M.",
""
]
] | We review extensions by integer spin simple currents in two-dimensional conformal field theories and their applications in string theory. In particular, we study the problem of resolving the fixed points of a simple current and apply the formalism to the permutation orbifold. In terms of string compactifications, we co... | 13.356875 | 10.497921 | 15.427358 | 10.443342 | 11.582047 | 11.09215 | 10.956272 | 10.758369 | 10.102103 | 16.614607 | 10.12348 | 11.898251 | 12.817591 | 10.845771 | 11.754459 | 11.923126 | 11.836766 | 12.17332 | 11.404398 | 13.858802 | 11.310828 |
0708.2144 | Eric Woolgar | E. Woolgar | Some Applications of Ricci Flow in Physics | Minor corrections in Sections IV and VI. Invited talk at Theory
Canada III meeting, June 2007; submitted to Proceedings. Dedicated to Rafael
D Sorkin on the occasion of his 60th birthday | Can.J.Phys.86:645,2008 | 10.1139/P07-146 | null | hep-th gr-qc math.DG | null | I discuss certain applications of the Ricci flow in physics. I first review
how it arises in the renormalization group (RG) flow of a nonlinear sigma
model. I then review the concept of a Ricci soliton and recall how a soliton
was used to discuss the RG flow of mass in 2-dimensions. I then present recent
results obta... | [
{
"created": "Thu, 16 Aug 2007 06:50:14 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Aug 2007 04:52:23 GMT",
"version": "v2"
},
{
"created": "Mon, 31 Dec 2007 04:03:04 GMT",
"version": "v3"
}
] | 2009-11-13 | [
[
"Woolgar",
"E.",
""
]
] | I discuss certain applications of the Ricci flow in physics. I first review how it arises in the renormalization group (RG) flow of a nonlinear sigma model. I then review the concept of a Ricci soliton and recall how a soliton was used to discuss the RG flow of mass in 2-dimensions. I then present recent results obtain... | 8.706186 | 7.263993 | 7.626855 | 7.55528 | 7.55256 | 7.410306 | 7.396316 | 7.521315 | 7.376763 | 8.045269 | 7.508692 | 7.550793 | 7.435887 | 7.323264 | 7.271723 | 7.049301 | 7.166031 | 7.327007 | 7.540514 | 7.668597 | 7.588433 |
hep-th/9607201 | John Schwarz | John H. Schwarz | Lectures on Superstring and M Theory Dualities | 67 pages, latex, 1 figure; Lectures given at the ICTP Spring School
(March 1996) and the TASI Summer School (June 1996), TASI96 | Nucl.Phys.Proc.Suppl.55B:1-32,1997 | 10.1016/S0920-5632(97)00070-4 | null | hep-th | null | These lectures begin by reviewing the evidence for S duality of the
toroidally compactified heterotic string in 4d that was obtained in the period
1992--94. Next they review recently discovered dualities that relate all five
of the 10d superstring theories and a quantum extension of 11d supergravity
called M theory. ... | [
{
"created": "Thu, 25 Jul 1996 23:44:00 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Sep 1996 19:53:09 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Schwarz",
"John H.",
""
]
] | These lectures begin by reviewing the evidence for S duality of the toroidally compactified heterotic string in 4d that was obtained in the period 1992--94. Next they review recently discovered dualities that relate all five of the 10d superstring theories and a quantum extension of 11d supergravity called M theory. Th... | 10.753547 | 9.411861 | 10.67722 | 10.058558 | 10.288876 | 10.166967 | 9.68301 | 9.293891 | 9.112156 | 10.502883 | 9.328782 | 9.570809 | 9.605728 | 9.202765 | 9.060443 | 9.63396 | 9.255193 | 9.277806 | 9.403921 | 9.49778 | 8.521249 |
hep-th/0212258 | Wolfgang Bietenholz | W. Bietenholz, F. Hofheinz and J. Nishimura | Non--Commutative Field Theories beyond Perturbation Theory | 8 pages, 8 figures, talk presented at 35th Ahrenshoop Symposium | Fortsch.Phys. 51 (2003) 745-752 | 10.1002/prop.200310092 | HU-EP-02/63 | hep-th gr-qc hep-lat | null | We investigate two models in non-commutative (NC) field theory by means of
Monte Carlo simulations. Even if we start from the Euclidean lattice
formulation, such simulations are only feasible after mapping the systems onto
dimensionally reduced matrix models. Using this technique, we measure Wilson
loops in 2d NC gau... | [
{
"created": "Fri, 20 Dec 2002 10:37:36 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Bietenholz",
"W.",
""
],
[
"Hofheinz",
"F.",
""
],
[
"Nishimura",
"J.",
""
]
] | We investigate two models in non-commutative (NC) field theory by means of Monte Carlo simulations. Even if we start from the Euclidean lattice formulation, such simulations are only feasible after mapping the systems onto dimensionally reduced matrix models. Using this technique, we measure Wilson loops in 2d NC gauge... | 12.744451 | 13.026756 | 13.604914 | 12.297137 | 13.340457 | 13.875799 | 13.460774 | 12.869272 | 12.53861 | 15.011767 | 12.800894 | 12.318016 | 13.3779 | 12.355659 | 12.206032 | 12.573129 | 12.388587 | 12.772277 | 12.099756 | 13.526058 | 11.933543 |
1003.2850 | Ram Brustein | Ram Brustein, A.J.M. Medved | Bounds on Black Hole Entropy in Unitary Theories of Gravity | 16 pages, no figures | JHEP 1004:103,2010 | 10.1007/JHEP04(2010)103 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider unitary and weakly coupled theories of gravity that extend
Einstein gravity and reduce to it asymptotically at large distances. Our
discussion is restricted to such theories that, similarly to Einstein gravity,
contain black holes as semiclassical states in a range of scales. We show that,
at a given scal... | [
{
"created": "Mon, 15 Mar 2010 05:51:54 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Brustein",
"Ram",
""
],
[
"Medved",
"A. J. M.",
""
]
] | We consider unitary and weakly coupled theories of gravity that extend Einstein gravity and reduce to it asymptotically at large distances. Our discussion is restricted to such theories that, similarly to Einstein gravity, contain black holes as semiclassical states in a range of scales. We show that, at a given scale,... | 7.929837 | 7.531141 | 8.416515 | 7.534106 | 7.590945 | 8.177896 | 8.043272 | 7.856336 | 7.716234 | 7.953046 | 7.850296 | 7.605644 | 7.730539 | 7.447425 | 7.677073 | 7.5093 | 7.655082 | 7.607733 | 7.402126 | 7.607993 | 7.606881 |
hep-th/0204043 | Shlomo S. Razamat | Shlomo S. Razamat | Marginal Deformations of N=4 SYM and of its Supersymmetric Orbifold
Descendants | 102 pages, MSc thesis | null | null | null | hep-th | null | In this thesis exactly marginal deformations of field theories living on
D3-branes at low energies are studied. These theories include
N=4 supersymmetric Yang-Mills theory and theories obtained from it via the
orbifolding procedure.
| [
{
"created": "Thu, 4 Apr 2002 13:55:35 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Razamat",
"Shlomo S.",
""
]
] | In this thesis exactly marginal deformations of field theories living on D3-branes at low energies are studied. These theories include N=4 supersymmetric Yang-Mills theory and theories obtained from it via the orbifolding procedure. | 13.159167 | 5.984659 | 8.555409 | 6.300139 | 7.592918 | 6.382659 | 6.512136 | 6.436434 | 6.143025 | 9.47622 | 6.513261 | 7.327798 | 8.37632 | 7.36917 | 7.573967 | 6.948223 | 7.360708 | 7.1109 | 7.375667 | 8.736935 | 7.004129 |
1003.0797 | Daniel Brattan Mr | Daniel K. Brattan | Charged, conformal non-relativistic hydrodynamics | 31 pages, 1 figure, JHEP3 style, refs added, typos corrected, missing
terms in spatial charge current and field corrections added, to be published
in JHEP | JHEP 1010:015, 2010 | 10.1007/JHEP10(2010)015 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We embed a holographic model of an U(1) charged fluid with Galilean
invariance in string theory and calculate its specific heat capacity and
Prandtl number. Such theories are generated by a R-symmetry twist along a null
direction of a N=1 superconformal theory. We study the hydrodynamic properties
of such systems emp... | [
{
"created": "Wed, 3 Mar 2010 13:14:36 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Sep 2010 16:44:41 GMT",
"version": "v2"
}
] | 2010-12-01 | [
[
"Brattan",
"Daniel K.",
""
]
] | We embed a holographic model of an U(1) charged fluid with Galilean invariance in string theory and calculate its specific heat capacity and Prandtl number. Such theories are generated by a R-symmetry twist along a null direction of a N=1 superconformal theory. We study the hydrodynamic properties of such systems emplo... | 13.051468 | 10.604018 | 13.537719 | 9.803352 | 10.895748 | 10.781663 | 10.25743 | 10.779298 | 9.603384 | 12.797749 | 10.328685 | 10.901675 | 12.662349 | 11.472344 | 11.098236 | 11.067645 | 11.483389 | 11.193951 | 11.851916 | 12.456337 | 11.057826 |
hep-th/9411168 | null | S. Bellucci, S. Krivonos and A. Sorin | Linearizing $W_{2,4}$ and $WB_2$ Algebras | 13 pages, LaTeX | Phys.Lett. B347 (1995) 260-268 | 10.1016/0370-2693(95)00002-3 | JINR E2-94-440,LNF-94/069(P) | hep-th | null | It has recently been shown that the $W_3$ and $W_3^{(2)}$ algebras can be
considered as subalgebras in some linear conformal algebras. In this paper we
show that the nonlinear algebras $W_{2,4}$ and $WB_2$ as well as
Zamolodchikov's spin $5/2$ superalgebra also can be embedded as subalgebras
into some linear conforma... | [
{
"created": "Wed, 23 Nov 1994 12:21:37 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Nov 1994 12:04:31 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Bellucci",
"S.",
""
],
[
"Krivonos",
"S.",
""
],
[
"Sorin",
"A.",
""
]
] | It has recently been shown that the $W_3$ and $W_3^{(2)}$ algebras can be considered as subalgebras in some linear conformal algebras. In this paper we show that the nonlinear algebras $W_{2,4}$ and $WB_2$ as well as Zamolodchikov's spin $5/2$ superalgebra also can be embedded as subalgebras into some linear conformal ... | 4.702174 | 3.968913 | 5.306117 | 4.135348 | 4.122244 | 4.126325 | 3.947582 | 4.119247 | 4.005301 | 5.219312 | 4.036226 | 4.136204 | 5.09912 | 4.303051 | 4.121352 | 4.170571 | 4.116723 | 4.239968 | 4.227427 | 4.928723 | 4.118923 |
hep-th/0112040 | Kyungho Oh | Kyungho Oh and Radu Tatar | Duality and Confinement in N=1 Supersymmetric Theories from Geometric
Transitions | 52 pages, 10 figures, references added and minor corrections | Adv.Theor.Math.Phys. 6 (2003) 141-196 | null | HUTP-01/A060, HU-EP-01/55 | hep-th | null | We study large N dualities for a general class of N=1 theories realized on
type IIB D5 branes wrapping 2-cycles of local Calabi-Yau threefolds or as
effective field theories on D4 branes in type IIA brane configurations. We
completely solve the issue of the classical moduli space for N=2, U(N_1)x ... x
U(N_n) theorie... | [
{
"created": "Wed, 5 Dec 2001 23:37:18 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Dec 2001 21:09:14 GMT",
"version": "v2"
},
{
"created": "Thu, 10 Jan 2002 02:47:04 GMT",
"version": "v3"
},
{
"created": "Wed, 15 May 2002 17:20:07 GMT",
"version": "v4"
},
{
"cre... | 2007-05-23 | [
[
"Oh",
"Kyungho",
""
],
[
"Tatar",
"Radu",
""
]
] | We study large N dualities for a general class of N=1 theories realized on type IIB D5 branes wrapping 2-cycles of local Calabi-Yau threefolds or as effective field theories on D4 branes in type IIA brane configurations. We completely solve the issue of the classical moduli space for N=2, U(N_1)x ... x U(N_n) theories ... | 9.560143 | 8.367302 | 11.290172 | 8.422778 | 8.978415 | 8.587707 | 8.769436 | 9.118361 | 8.639848 | 12.560374 | 9.25331 | 9.171741 | 9.974802 | 9.18266 | 9.129323 | 8.962274 | 9.036543 | 9.173889 | 9.266018 | 10.004045 | 8.945703 |
2101.07297 | Harold Steinacker | Stefan Fredenhagen and Harold C. Steinacker | Exploring the gravity sector of emergent higher-spin gravity: effective
action and a solution | 39 pages, v2: minor issues fixed, conclusion unchanged V3: Appendix
E.1 corrected, no change of results or conclusions | JHEP 05 (2021) 183 | 10.1007/JHEP05(2021)183 | UWThPh 2021-1 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We elaborate the description of the semi-classical gravity sector of
Yang-Mills matrix models on a covariant quantum FLRW background. The basic
geometric structure is a frame, which arises from the Poisson structure on an
underlying $S^2$ bundle over space-time. The equations of motion for the
associated Weitzenb\"oc... | [
{
"created": "Mon, 18 Jan 2021 19:32:39 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jul 2021 10:20:18 GMT",
"version": "v2"
},
{
"created": "Fri, 10 Mar 2023 20:39:12 GMT",
"version": "v3"
}
] | 2023-03-14 | [
[
"Fredenhagen",
"Stefan",
""
],
[
"Steinacker",
"Harold C.",
""
]
] | We elaborate the description of the semi-classical gravity sector of Yang-Mills matrix models on a covariant quantum FLRW background. The basic geometric structure is a frame, which arises from the Poisson structure on an underlying $S^2$ bundle over space-time. The equations of motion for the associated Weitzenb\"ock ... | 11.828227 | 10.508295 | 10.795315 | 9.874636 | 10.168837 | 10.645781 | 10.556026 | 10.320117 | 9.735929 | 10.444089 | 10.335566 | 10.525484 | 10.557153 | 10.27931 | 10.269218 | 10.198428 | 10.049787 | 10.180522 | 10.703895 | 10.445016 | 10.140218 |
1109.3200 | William Divine Linch III | Osvaldo Chandia, William D. Linch III, and Brenno Carlini Vallilo | The Covariant Superstring on K3 | 18 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compactify the pure spinor formalism on a K3 surface. The pure spinor
splits into a six-dimensional pure spinor, a projective superspace harmonic,
and 6 non-covariant variables. A homological algebra argument reduces the
calculation of the cohomology of the Berkovits differential to a "small"
Hilbert space which i... | [
{
"created": "Wed, 14 Sep 2011 20:05:20 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Sep 2011 18:37:35 GMT",
"version": "v2"
}
] | 2011-09-28 | [
[
"Chandia",
"Osvaldo",
""
],
[
"Linch",
"William D.",
"III"
],
[
"Vallilo",
"Brenno Carlini",
""
]
] | We compactify the pure spinor formalism on a K3 surface. The pure spinor splits into a six-dimensional pure spinor, a projective superspace harmonic, and 6 non-covariant variables. A homological algebra argument reduces the calculation of the cohomology of the Berkovits differential to a "small" Hilbert space which is ... | 13.968161 | 12.904132 | 16.903793 | 12.533176 | 12.576648 | 12.99173 | 12.392152 | 13.117772 | 12.098776 | 17.937637 | 12.644727 | 12.457236 | 13.528971 | 12.515677 | 12.860448 | 12.721424 | 12.608097 | 12.52139 | 12.42417 | 13.307079 | 12.210422 |
hep-th/9610112 | Miguel S. Costa | Miguel S. Costa and Malcolm J. Perry (D.A.M.T.P./ University of
Cambridge) | Kaluza-Klein electrically charged black branes in M-theory | 16 pages, uses latex and epsf macro, figures included | Class.Quant.Grav.14:603-614,1997 | 10.1088/0264-9381/14/3/007 | null | hep-th | null | We present a class of Kaluza-Klein electrically charged black p-brane
solutions of ten-dimensional, type IIA superstring theory. Uplifting to eleven
dimensions these solutions are studied in the context of M-theory. They can be
interpreted either as a p+1 extended object trapped around the eleventh
dimension along wh... | [
{
"created": "Wed, 16 Oct 1996 20:24:22 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Costa",
"Miguel S.",
"",
"D.A.M.T.P./ University of\n Cambridge"
],
[
"Perry",
"Malcolm J.",
"",
"D.A.M.T.P./ University of\n Cambridge"
]
] | We present a class of Kaluza-Klein electrically charged black p-brane solutions of ten-dimensional, type IIA superstring theory. Uplifting to eleven dimensions these solutions are studied in the context of M-theory. They can be interpreted either as a p+1 extended object trapped around the eleventh dimension along whic... | 7.844962 | 8.273793 | 8.743789 | 7.332466 | 8.251562 | 8.144103 | 8.187329 | 7.914008 | 7.895781 | 9.312881 | 7.494507 | 7.219952 | 7.693279 | 7.133636 | 7.052634 | 7.407 | 7.378527 | 7.262006 | 7.370335 | 7.739249 | 7.297179 |
hep-th/0006172 | Bhaskar Dutta | R. Arnowitt and B. Dutta | Yukawa Textures in Horava-Witten M-Theory | 28 pages, Revtex | Nucl.Phys.B592:143-163,2001 | 10.1016/S0550-3213(00)00608-8 | null | hep-th hep-ph | null | Recent advances in 11 dimensional Horava-Witten M-theory based on
non-standard embeddings with torus fibered Calabi-Yau manifolds have allowed
the construction of three generation models with Wilson line breaking to the
Standard Model gauge symmetry. Central to these constructions is the existence
of a set of 5-brane... | [
{
"created": "Wed, 21 Jun 2000 20:35:16 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Arnowitt",
"R.",
""
],
[
"Dutta",
"B.",
""
]
] | Recent advances in 11 dimensional Horava-Witten M-theory based on non-standard embeddings with torus fibered Calabi-Yau manifolds have allowed the construction of three generation models with Wilson line breaking to the Standard Model gauge symmetry. Central to these constructions is the existence of a set of 5-branes ... | 10.856921 | 9.9431 | 10.767539 | 9.30539 | 9.797347 | 10.551349 | 10.015584 | 9.36382 | 9.345737 | 10.553429 | 10.335981 | 10.050587 | 10.536167 | 9.916873 | 10.177983 | 10.214161 | 10.021911 | 10.124301 | 9.924645 | 10.566797 | 10.480213 |
hep-th/0312010 | Satoshi Nagaoka | Satoshi Nagaoka | Higher Dimensional Recombination of Intersecting D-branes | 18 pages, 2 figures, JHEP style. v3:references added, minor
corrections, English improved | JHEP 0402 (2004) 063 | 10.1088/1126-6708/2004/02/063 | UT-Komaba/03-19 | hep-th | null | We study recombinations of D-brane systems intersecting at more than one
angle using super Yang-Mills theory. We find the condensation of an
off-diagonal tachyon mode relates to the recombination, as was clarified for
branes at one angle in hep-th/0303204. For branes at two angles, after the
tachyon mode between two ... | [
{
"created": "Mon, 1 Dec 2003 07:39:30 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Dec 2003 08:31:07 GMT",
"version": "v2"
},
{
"created": "Fri, 27 Feb 2004 07:41:40 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Nagaoka",
"Satoshi",
""
]
] | We study recombinations of D-brane systems intersecting at more than one angle using super Yang-Mills theory. We find the condensation of an off-diagonal tachyon mode relates to the recombination, as was clarified for branes at one angle in hep-th/0303204. For branes at two angles, after the tachyon mode between two D2... | 11.535265 | 11.554383 | 13.079634 | 10.55 | 11.493697 | 11.30605 | 11.245914 | 11.214454 | 10.496821 | 13.162453 | 11.281784 | 10.804716 | 11.706531 | 10.970407 | 11.146645 | 11.033411 | 10.66612 | 11.191085 | 10.766348 | 11.236258 | 10.701238 |
hep-th/0410175 | Xiaojun Wang | Xiao-Jun Wang and Neng-Chao Xiao | A note on brane/flux annihilation and dS vacua in string theory | 14 pages, 3 eps figures, v2: typos modified and references added | null | null | USTC-ICTS-04-21 | hep-th | null | We reconsider the dynamics of p anti-D3 branes inside the Klebanov-Strassler
geometry, in which M units of R-R 3-form flux and K units of NS-NS 3-form flux
are presented in deformed conifold. We find that anti-D3 branes blow up into a
spherical D5-brane at weak string coupling via quantum tunnelling. The D5-brane
can... | [
{
"created": "Sat, 16 Oct 2004 03:50:32 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Oct 2004 09:51:35 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Wang",
"Xiao-Jun",
""
],
[
"Xiao",
"Neng-Chao",
""
]
] | We reconsider the dynamics of p anti-D3 branes inside the Klebanov-Strassler geometry, in which M units of R-R 3-form flux and K units of NS-NS 3-form flux are presented in deformed conifold. We find that anti-D3 branes blow up into a spherical D5-brane at weak string coupling via quantum tunnelling. The D5-brane can b... | 9.740958 | 8.475015 | 10.808191 | 8.364715 | 8.296368 | 7.816137 | 8.293188 | 8.622697 | 8.501182 | 10.794765 | 7.903049 | 8.238899 | 9.526989 | 8.980392 | 8.499378 | 7.909412 | 8.509766 | 8.617638 | 8.845797 | 9.63676 | 8.33609 |
0812.0552 | Glenn Barnich | Glenn Barnich and Cedric Troessaert | Manifest spin 2 duality with electric and magnetic sources | 32 pages Latex file, minor cosmetic changes, reference added | JHEP 0901:030,2009 | 10.1088/1126-6708/2009/01/030 | ULB-TH/08-29 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the formulation of spin 2 fields on Minkowski space which makes the
action manifestly invariant under duality rotations to the case of interactions
with external electric and magnetic sources by adding suitable potentials for
the longitudinal and trace parts. In this framework, the string singularity of
the... | [
{
"created": "Tue, 2 Dec 2008 17:19:34 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Jan 2009 15:36:04 GMT",
"version": "v2"
}
] | 2010-04-28 | [
[
"Barnich",
"Glenn",
""
],
[
"Troessaert",
"Cedric",
""
]
] | We extend the formulation of spin 2 fields on Minkowski space which makes the action manifestly invariant under duality rotations to the case of interactions with external electric and magnetic sources by adding suitable potentials for the longitudinal and trace parts. In this framework, the string singularity of the l... | 14.027411 | 13.34093 | 16.685135 | 13.31986 | 13.323631 | 14.254193 | 13.087775 | 13.30346 | 12.973742 | 14.567346 | 12.15047 | 12.396587 | 14.192014 | 13.036745 | 12.990547 | 13.31537 | 13.703744 | 13.022478 | 12.971 | 13.889678 | 13.389119 |
1509.01065 | Athanasios Lahanas | G. A. Diamandis, A. B. Lahanas and K. Tamvakis | Towards a formulation of $f(R)$ supergravity | 21 pages, references added, typos corrected | Phys. Rev. D 92, 105023 (2015) | 10.1103/PhysRevD.92.105023 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The supersymmetric completion of $R+R^2$ gravity is known to be equivalent to
standard supergravity coupled to two chiral supermultiples with a K\"ahler
potential of the no-scale type. The generalization of this programme to $f(R)$
gravity can be carried out in an analogous framework in terms of four chiral
multiplet... | [
{
"created": "Thu, 3 Sep 2015 13:13:16 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Sep 2015 07:45:34 GMT",
"version": "v2"
},
{
"created": "Fri, 20 Nov 2015 12:51:37 GMT",
"version": "v3"
}
] | 2015-11-23 | [
[
"Diamandis",
"G. A.",
""
],
[
"Lahanas",
"A. B.",
""
],
[
"Tamvakis",
"K.",
""
]
] | The supersymmetric completion of $R+R^2$ gravity is known to be equivalent to standard supergravity coupled to two chiral supermultiples with a K\"ahler potential of the no-scale type. The generalization of this programme to $f(R)$ gravity can be carried out in an analogous framework in terms of four chiral multiplets ... | 13.589316 | 12.130697 | 13.067667 | 12.022145 | 11.298023 | 11.674675 | 12.73498 | 11.092171 | 11.41092 | 12.87197 | 11.980392 | 12.86368 | 12.426004 | 12.054521 | 12.227242 | 12.41228 | 12.052377 | 12.38519 | 12.124957 | 12.593781 | 12.396035 |
hep-th/9403026 | Jean-Loup Gervais | Jean-Loup Gervais, Jean-Francois Roussel | Solving the Strongly Coupled 2D Gravity: 2. Fractional-Spin Operators,
and Topological Three-Point Functions | 45 pages Latex file, 14 figures (uuencoded) | Nucl.Phys. B426 (1994) 140-186 | 10.1016/0550-3213(94)90130-9 | LPTENS-94/01 | hep-th | null | Progress along the line of a previous article are reported. One main point is
to include chiral operators with fractional quantum group spins (fourth or
sixth of integers) which are needed to achieve modular invariance. We extend
the study of the chiral bootstrap (recently completed by E. Cremmer, and the
present aut... | [
{
"created": "Fri, 4 Mar 1994 13:57:37 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Gervais",
"Jean-Loup",
""
],
[
"Roussel",
"Jean-Francois",
""
]
] | Progress along the line of a previous article are reported. One main point is to include chiral operators with fractional quantum group spins (fourth or sixth of integers) which are needed to achieve modular invariance. We extend the study of the chiral bootstrap (recently completed by E. Cremmer, and the present autho... | 18.341282 | 18.827665 | 19.25523 | 15.947455 | 19.47073 | 18.106457 | 19.213495 | 18.09264 | 17.899458 | 21.855724 | 17.243778 | 16.25597 | 17.905903 | 16.701019 | 17.003073 | 16.681601 | 17.056175 | 16.836647 | 16.663792 | 17.144093 | 17.001646 |
hep-th/0604161 | Ofer Aharony | Ofer Aharony, Jacob Sonnenschein and Shimon Yankielowicz | A holographic model of deconfinement and chiral symmetry restoration | 30 pages, 7 figures, latex. v2: minor corrections and added reference
to parallel work | Annals Phys.322:1420-1443,2007 | 10.1016/j.aop.2006.11.002 | WIS/05/06-APR-DPP, TAUP-2824/06 | hep-th | null | We analyze the finite temperature behavior of the Sakai-Sugimoto model, which
is a holographic dual of a theory which spontaneously breaks a U(N_f)_L x
U(N_f)_R chiral flavor symmetry at zero temperature. The theory involved is a
4+1 dimensional supersymmetric SU(N_c) gauge theory compactified on a circle of
radius R... | [
{
"created": "Mon, 24 Apr 2006 15:16:08 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Jun 2006 07:15:05 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Aharony",
"Ofer",
""
],
[
"Sonnenschein",
"Jacob",
""
],
[
"Yankielowicz",
"Shimon",
""
]
] | We analyze the finite temperature behavior of the Sakai-Sugimoto model, which is a holographic dual of a theory which spontaneously breaks a U(N_f)_L x U(N_f)_R chiral flavor symmetry at zero temperature. The theory involved is a 4+1 dimensional supersymmetric SU(N_c) gauge theory compactified on a circle of radius R w... | 4.456851 | 4.577232 | 5.051438 | 4.405767 | 4.278002 | 4.907569 | 4.443794 | 4.404956 | 4.345929 | 4.969326 | 4.422675 | 4.554334 | 4.672164 | 4.490869 | 4.400505 | 4.395302 | 4.6168 | 4.511813 | 4.533666 | 4.648338 | 4.334814 |
1710.05791 | Alexander Krikun | Tomas Andrade, Alexander Krikun, Koenraad Schalm and Jan Zaanen | Doping the holographic Mott insulator | 27 pages, 9 figures. Accepted in Nature Physics | null | 10.1038/s41567-018-0217-6 | null | hep-th cond-mat.str-el cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Mott insulators form because of strong electron repulsions, being at the
heart of strongly correlated electron physics. Conventionally these are
understood as classical "traffic jams" of electrons described by a short-ranged
entangled product ground state. Exploiting the holographic duality, which maps
the physics of... | [
{
"created": "Mon, 16 Oct 2017 15:50:25 GMT",
"version": "v1"
},
{
"created": "Sat, 2 Jun 2018 21:46:00 GMT",
"version": "v2"
}
] | 2018-08-03 | [
[
"Andrade",
"Tomas",
""
],
[
"Krikun",
"Alexander",
""
],
[
"Schalm",
"Koenraad",
""
],
[
"Zaanen",
"Jan",
""
]
] | Mott insulators form because of strong electron repulsions, being at the heart of strongly correlated electron physics. Conventionally these are understood as classical "traffic jams" of electrons described by a short-ranged entangled product ground state. Exploiting the holographic duality, which maps the physics of d... | 10.665396 | 11.703506 | 12.851661 | 11.948205 | 12.688492 | 12.621646 | 11.200599 | 11.498054 | 11.674244 | 14.661277 | 10.307494 | 10.40983 | 11.115436 | 10.732336 | 10.289361 | 10.245279 | 10.117822 | 10.727969 | 10.695137 | 10.994634 | 10.524284 |
1405.7388 | Nelson R. F. Braga | Nelson R. F. Braga and Edmond Iancu | Anomalous dimensions from rotating open strings in AdS/CFT | V2: two related references included | null | 10.1007/JHEP08(2014)104 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new entry within the dictionary of the AdS/CFT duality at strong
coupling: in the limit of a large spin or a large R-charge, the anomalous
dimension of the gauge theory operator dual to a semiclassical rotating string
is proportional to the string proper length. This conjecture is motivated by a
generali... | [
{
"created": "Wed, 28 May 2014 20:16:14 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Jun 2014 02:57:23 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Braga",
"Nelson R. F.",
""
],
[
"Iancu",
"Edmond",
""
]
] | We propose a new entry within the dictionary of the AdS/CFT duality at strong coupling: in the limit of a large spin or a large R-charge, the anomalous dimension of the gauge theory operator dual to a semiclassical rotating string is proportional to the string proper length. This conjecture is motivated by a generaliza... | 7.347437 | 7.76633 | 8.692361 | 7.442522 | 8.348527 | 8.066821 | 8.072528 | 7.684999 | 7.600813 | 8.271533 | 7.900797 | 7.435297 | 7.383594 | 7.337913 | 7.490549 | 7.536803 | 7.507905 | 7.321176 | 7.381922 | 7.271776 | 7.33925 |
0709.3428 | Soumitra SenGupta | Biswarup Mukhopadhyaya, Somasri Sen and Soumitra SenGupta | Bulk antisymmetric tensor fields in a Randall-Sundrum model | 8 Pages, Latex | Phys.Rev.D76:121501,2007 | 10.1103/PhysRevD.76.121501 | null | hep-th hep-ph | null | We consider bulk antisymmetric tensor fields of various ranks in a
Randall-Sundrum scenario. We show that, rank-2 onwards, the zero-modes of the
projections of these fields on the (3+1) dimensional visible brane become
increasingly weaker as the rank of the tensor increases. All such tensor fields
of rank 4 or more a... | [
{
"created": "Fri, 21 Sep 2007 12:53:51 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Mukhopadhyaya",
"Biswarup",
""
],
[
"Sen",
"Somasri",
""
],
[
"SenGupta",
"Soumitra",
""
]
] | We consider bulk antisymmetric tensor fields of various ranks in a Randall-Sundrum scenario. We show that, rank-2 onwards, the zero-modes of the projections of these fields on the (3+1) dimensional visible brane become increasingly weaker as the rank of the tensor increases. All such tensor fields of rank 4 or more are... | 13.867918 | 13.460791 | 11.974821 | 11.853307 | 13.211741 | 12.672079 | 12.552446 | 11.160627 | 11.911039 | 14.200233 | 12.065223 | 13.048661 | 11.924926 | 12.157254 | 12.147843 | 12.600869 | 12.347599 | 12.415986 | 11.934485 | 12.415616 | 12.238812 |
1101.0877 | Kuldeep Kumar | Rabin Banerjee, Biswajit Chakraborty and Kuldeep Kumar | Reply to "Comment on 'Noncommutative gauge theories and Lorentz
symmetry'" | 5 pages, LaTeX, appeared in Phys. Rev. D | Phys. Rev. D 77 (2008) 048702 | 10.1103/PhysRevD.77.048702 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a reply to "Comment on 'Noncommutative gauge theories and Lorentz
symmetry,'" Phys. Rev. D 77 (2008) 048701 by Alfredo Iorio.
| [
{
"created": "Wed, 5 Jan 2011 04:08:56 GMT",
"version": "v1"
}
] | 2011-01-06 | [
[
"Banerjee",
"Rabin",
""
],
[
"Chakraborty",
"Biswajit",
""
],
[
"Kumar",
"Kuldeep",
""
]
] | This is a reply to "Comment on 'Noncommutative gauge theories and Lorentz symmetry,'" Phys. Rev. D 77 (2008) 048701 by Alfredo Iorio. | 9.827104 | 8.660921 | 9.042333 | 8.001793 | 7.457777 | 8.38122 | 9.369599 | 7.709114 | 9.624685 | 8.38745 | 7.85362 | 7.898752 | 8.720366 | 8.043666 | 8.216671 | 7.629258 | 8.503022 | 8.006663 | 8.186829 | 8.921415 | 7.460503 |
hep-th/0211098 | Mina Aganagic | Mina Aganagic, Albrecht Klemm, Marcos Marino and Cumrun Vafa | Matrix Model as a Mirror of Chern-Simons Theory | harvmac, 54 pages, 13 figures | JHEP 0402 (2004) 010 | 10.1088/1126-6708/2004/02/010 | HUTP-02/A057, HU-EP-02/47 | hep-th | null | Using mirror symmetry, we show that Chern-Simons theory on certain manifolds
such as lens spaces reduces to a novel class of Hermitian matrix models, where
the measure is that of unitary matrix models. We show that this agrees with the
more conventional canonical quantization of Chern-Simons theory. Moreover,
large N... | [
{
"created": "Mon, 11 Nov 2002 21:38:03 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Aganagic",
"Mina",
""
],
[
"Klemm",
"Albrecht",
""
],
[
"Marino",
"Marcos",
""
],
[
"Vafa",
"Cumrun",
""
]
] | Using mirror symmetry, we show that Chern-Simons theory on certain manifolds such as lens spaces reduces to a novel class of Hermitian matrix models, where the measure is that of unitary matrix models. We show that this agrees with the more conventional canonical quantization of Chern-Simons theory. Moreover, large N d... | 5.809406 | 6.269613 | 8.186173 | 5.921466 | 5.95726 | 6.004037 | 5.63326 | 6.127738 | 6.232277 | 8.709315 | 5.914181 | 5.963889 | 7.052038 | 5.977615 | 5.78035 | 5.959448 | 6.11787 | 5.917909 | 6.098122 | 7.152772 | 6.019486 |
hep-th/0304045 | Vasilis Niarchos | David Kutasov and Vasilis Niarchos | Tachyon Effective Actions In Open String Theory | harvmac, 19 pages; v2 two references added; v3 additional comments
and a reference | Nucl.Phys. B666 (2003) 56-70 | 10.1016/S0550-3213(03)00498-X | null | hep-th | null | We argue that the Dirac-Born-Infeld (DBI) action coupled to a tachyon, that
is known to reproduce some aspects of open string dynamics, can be obtained
from open string theory in a certain limit, which generalizes the limit leading
to the usual DBI action. This helps clarify which aspects of the full open
string theo... | [
{
"created": "Mon, 7 Apr 2003 17:34:44 GMT",
"version": "v1"
},
{
"created": "Sun, 20 Apr 2003 22:39:14 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Jun 2003 17:07:45 GMT",
"version": "v3"
}
] | 2010-04-05 | [
[
"Kutasov",
"David",
""
],
[
"Niarchos",
"Vasilis",
""
]
] | We argue that the Dirac-Born-Infeld (DBI) action coupled to a tachyon, that is known to reproduce some aspects of open string dynamics, can be obtained from open string theory in a certain limit, which generalizes the limit leading to the usual DBI action. This helps clarify which aspects of the full open string theory... | 6.808741 | 5.849318 | 7.112065 | 5.74909 | 5.962774 | 5.909986 | 5.964097 | 5.650057 | 5.372953 | 6.967606 | 5.364534 | 5.748062 | 7.140191 | 6.062387 | 5.861913 | 5.784633 | 5.680763 | 5.737522 | 6.107793 | 6.723342 | 5.730308 |
hep-th/9509036 | Alexander Kalloniatis | S.S. Pinsky (The Ohio-State University) and A.C. Kalloniatis
(Max-Planck Institut fuer Kernphysik, Heidelberg) | Light-Front QCD(1+1) Coupled to Adjoint Scalar Matter | LaTex, 13 pages. Submitted to Physics Letters B | Phys.Lett. B365 (1996) 225-232 | 10.1016/0370-2693(95)01259-1 | OHSTPY-HEP-TH-93-014 | hep-th | null | We consider adjoint scalar matter coupled to QCD(1+1) in light-cone
quantization on a finite `interval' with periodic boundary conditions. We work
with the gauge group SU(2) which is modified to ${\rm{SU(2)/Z_2}}$ by the
non-trivial topology. The model is interesting for various nonperturbative
approaches because it ... | [
{
"created": "Thu, 7 Sep 1995 15:14:05 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Pinsky",
"S. S.",
"",
"The Ohio-State University"
],
[
"Kalloniatis",
"A. C.",
"",
"Max-Planck Institut fuer Kernphysik, Heidelberg"
]
] | We consider adjoint scalar matter coupled to QCD(1+1) in light-cone quantization on a finite `interval' with periodic boundary conditions. We work with the gauge group SU(2) which is modified to ${\rm{SU(2)/Z_2}}$ by the non-trivial topology. The model is interesting for various nonperturbative approaches because it is... | 11.207272 | 11.538672 | 11.22274 | 11.028827 | 11.511009 | 11.653863 | 11.647243 | 11.168189 | 11.179048 | 12.936718 | 11.173206 | 10.780056 | 11.264454 | 10.633289 | 10.983647 | 10.651792 | 10.8529 | 10.56272 | 10.557846 | 11.01465 | 10.65812 |
0911.3578 | Madad Ali Valuyan | M.A. Valuyan, and S.S. Gousheh | Dirichlet Casimir Energy for a Scalar Field in a Sphere: An Alternative
Method | 17 pages, 7 figures, 2 tables; Accepted for publication in Int. J.
Mod. Phys. A | Int.J.Mod.Phys.A25:1165-1183,2010 | 10.1142/S0217751X10048408 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we compute the leading order of the Casimir energy for a free
massless scalar field confined in a sphere in three spatial dimensions, with
the Dirichlet boundary condition. When one tabulates all of the reported values
of the Casimir energies for two closed geometries, cubical and spherical, in
differen... | [
{
"created": "Wed, 18 Nov 2009 15:43:14 GMT",
"version": "v1"
}
] | 2010-05-27 | [
[
"Valuyan",
"M. A.",
""
],
[
"Gousheh",
"S. S.",
""
]
] | In this paper we compute the leading order of the Casimir energy for a free massless scalar field confined in a sphere in three spatial dimensions, with the Dirichlet boundary condition. When one tabulates all of the reported values of the Casimir energies for two closed geometries, cubical and spherical, in different ... | 8.2566 | 8.518277 | 8.953703 | 8.490285 | 8.569972 | 8.703961 | 8.769827 | 8.071529 | 8.177327 | 9.29245 | 8.135434 | 8.185431 | 8.232191 | 8.061573 | 8.232847 | 8.438193 | 8.289461 | 8.224554 | 8.077729 | 8.352742 | 8.103975 |
0808.0324 | Wung-Hong Huang | Wung-Hong Huang, Kuo-Wei Huang | Thermodynamics on Noncommutative Geometry in Coherent State Formalism | Add analysis about thermodynamics of squeezed coherent state, Latex
12 pages | Phys.Lett.B670:416-420,2009 | 10.1016/j.physletb.2008.11.012 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The thermodynamics of ideal gas on the noncommutative geometry in the
coherent state formalism is investigated. We first evaluate the statistical
interparticle potential and see that there are residual "attraction (repulsion)
potential" between boson (fermion) in the high temperature limit. The
characters could be tr... | [
{
"created": "Mon, 4 Aug 2008 08:56:04 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Aug 2008 13:03:58 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Aug 2008 14:31:35 GMT",
"version": "v3"
},
{
"created": "Wed, 13 Aug 2008 09:25:11 GMT",
"version": "v4"
},
{
"cre... | 2009-01-16 | [
[
"Huang",
"Wung-Hong",
""
],
[
"Huang",
"Kuo-Wei",
""
]
] | The thermodynamics of ideal gas on the noncommutative geometry in the coherent state formalism is investigated. We first evaluate the statistical interparticle potential and see that there are residual "attraction (repulsion) potential" between boson (fermion) in the high temperature limit. The characters could be trac... | 10.023697 | 10.260376 | 10.314247 | 9.520593 | 10.060056 | 10.095338 | 10.483739 | 9.63943 | 9.277295 | 10.07343 | 9.420231 | 9.286962 | 9.383699 | 9.373925 | 9.328199 | 9.51303 | 9.364675 | 9.032938 | 9.377109 | 9.224831 | 9.177563 |
hep-th/0701179 | Seiji Terashima | Seiji Terashima | Supertubes in Matrix model and DBI action | 24 pages, references added, version to appear in JHEP | JHEP 0703:075,2007 | 10.1088/1126-6708/2007/03/075 | YITP-07-01 | hep-th | null | We show the equivalence between the supertube solutions with an arbitrary
cross section in two different actions, the DBI action for the D2-brane and the
matrix model action for the D0-branes. More precisely, the equivalence between
the supertubes in the D2-brane picture and the D0-brane picture is shown in the
bound... | [
{
"created": "Fri, 19 Jan 2007 12:30:59 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Feb 2007 11:24:15 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Mar 2007 07:05:34 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Terashima",
"Seiji",
""
]
] | We show the equivalence between the supertube solutions with an arbitrary cross section in two different actions, the DBI action for the D2-brane and the matrix model action for the D0-branes. More precisely, the equivalence between the supertubes in the D2-brane picture and the D0-brane picture is shown in the boundar... | 8.820403 | 7.679956 | 10.072804 | 7.6486 | 8.409479 | 8.720394 | 8.536364 | 7.726304 | 8.053269 | 8.986184 | 7.732361 | 7.954732 | 8.563421 | 8.022479 | 8.463257 | 7.878973 | 7.979273 | 7.876956 | 7.877508 | 8.759076 | 7.974853 |
0712.1873 | Mohammad Reza Setare | M. R. Setare, J. Sadeghi, A. R. Amani | Shape invariance method for quintom model in the bent brane background | 13 pages, no figure | Phys.Lett.B660:299-306,2008 | 10.1016/j.physletb.2008.01.024 | null | hep-th | null | In the present paper, we study the braneworld scenarios in the presence of
quintom dark energy coupled by gravity. The first-order formalism for the bent
brane (for both de Sitter and anti-de Sitter geometry), leads us to discuss the
shape invariance method in the bent brane systems. So, by using the
fluctuations of ... | [
{
"created": "Wed, 12 Dec 2007 06:26:56 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Setare",
"M. R.",
""
],
[
"Sadeghi",
"J.",
""
],
[
"Amani",
"A. R.",
""
]
] | In the present paper, we study the braneworld scenarios in the presence of quintom dark energy coupled by gravity. The first-order formalism for the bent brane (for both de Sitter and anti-de Sitter geometry), leads us to discuss the shape invariance method in the bent brane systems. So, by using the fluctuations of me... | 11.552752 | 10.528586 | 12.037691 | 9.935308 | 9.892383 | 10.01089 | 10.868162 | 11.43829 | 10.11467 | 10.670222 | 10.515924 | 10.127372 | 10.456585 | 10.093242 | 9.979674 | 10.453441 | 9.925516 | 9.973701 | 10.513531 | 10.878331 | 10.496827 |
1812.10209 | Sok-Hyon Won | Ok Song An, Yong Hae Ko, Sok-Hyon Won | Super-Weyl Anomaly from Holography and Rigid Supersymmetry Algebra on
Two-Sphere | 17 pages | Phys. Rev. D 99, 106007 (2019) | 10.1103/PhysRevD.99.106007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Operators transform anomalously under the symmetry in the presence of quantum
anomalies. We study this aspect of the super-Weyl anomaly in $\mathcal N=(1,1)$
superconformal field theories (SCFTs), in the context of AdS/CFT. In
particular, we carry out holographic renormalization for $(1,1)$ pure AdS$_3$
supergravity ... | [
{
"created": "Wed, 26 Dec 2018 03:00:21 GMT",
"version": "v1"
}
] | 2019-05-22 | [
[
"An",
"Ok Song",
""
],
[
"Ko",
"Yong Hae",
""
],
[
"Won",
"Sok-Hyon",
""
]
] | Operators transform anomalously under the symmetry in the presence of quantum anomalies. We study this aspect of the super-Weyl anomaly in $\mathcal N=(1,1)$ superconformal field theories (SCFTs), in the context of AdS/CFT. In particular, we carry out holographic renormalization for $(1,1)$ pure AdS$_3$ supergravity th... | 6.057178 | 5.531048 | 6.662919 | 5.801009 | 6.29151 | 5.875253 | 5.760075 | 5.744217 | 5.511689 | 6.860242 | 6.129939 | 5.846089 | 6.338712 | 5.94464 | 5.838721 | 5.950654 | 5.806899 | 6.161142 | 6.008214 | 6.286454 | 6.04617 |
hep-th/0307210 | Paul Heslop | P.J. Heslop and P.S. Howe | Aspects of N=4 SYM | 49 pages. Added reference and acknowledgements | JHEP 0401 (2004) 058 | 10.1088/1126-6708/2004/01/058 | KCL-TH-03-12 | hep-th | null | The properties of gauge-invariant composite operators and their correlation
functions in N=4 SYM are discussed in the analytic superspace formalism. A
complete classification of the different types of operators in the theory is
given. Operators can be either protected or unprotected according to whether
they do not o... | [
{
"created": "Tue, 22 Jul 2003 10:39:42 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Oct 2003 15:33:59 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Heslop",
"P. J.",
""
],
[
"Howe",
"P. S.",
""
]
] | The properties of gauge-invariant composite operators and their correlation functions in N=4 SYM are discussed in the analytic superspace formalism. A complete classification of the different types of operators in the theory is given. Operators can be either protected or unprotected according to whether they do not or ... | 6.861635 | 7.507971 | 7.406765 | 6.765628 | 7.090326 | 6.649669 | 6.612197 | 6.746874 | 6.615593 | 8.033706 | 6.756658 | 6.595843 | 6.968839 | 6.637091 | 6.539217 | 6.670103 | 6.63802 | 6.591598 | 6.616441 | 6.929346 | 6.679262 |
1907.07298 | Aleksandr N. Pinzul | Felipe Rodrigues de Almeida, Aleksandr Pinzul and Allen Stern | Non-commutative $AdS_2/CFT_1$ duality: the case of massive and
interacting scalar fields | 34 pages | Phys. Rev. D 100, 086005 (2019) | 10.1103/PhysRevD.100.086005 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue the study of the nocommutative $AdS_2 / CFT_1$ correspondence. We
extend our previous results obtained for a free massless scalar field to the
case of a massive scalar field. Both the free and interacting cases are
considered. For both cases it is confirmed that to the leading order in
noncommutative corr... | [
{
"created": "Wed, 17 Jul 2019 01:21:41 GMT",
"version": "v1"
}
] | 2019-10-16 | [
[
"de Almeida",
"Felipe Rodrigues",
""
],
[
"Pinzul",
"Aleksandr",
""
],
[
"Stern",
"Allen",
""
]
] | We continue the study of the nocommutative $AdS_2 / CFT_1$ correspondence. We extend our previous results obtained for a free massless scalar field to the case of a massive scalar field. Both the free and interacting cases are considered. For both cases it is confirmed that to the leading order in noncommutative correc... | 8.398298 | 7.435116 | 8.797991 | 7.560367 | 7.805033 | 7.856664 | 7.922544 | 7.968616 | 7.435066 | 8.358273 | 7.456105 | 7.903644 | 7.863911 | 7.59734 | 7.870479 | 8.022962 | 7.89498 | 7.731655 | 7.507513 | 7.730274 | 7.657104 |
hep-th/0012201 | Matteo Bertolini | M. Bertolini and M. Trigiante | How much can supergravity teach us about microscopic features of BPS
black holes? | 17 pages, latex. To appear in the proceedings of the IX Marcel
Grossman Meeting (Rome, July 2000), the TMR conference "Integrability
Nonperturbative Effects And Symmetry In Quantum Field Theory" (Paris,
September 2000) and the RTN conference ``The Quantum Structure of Spacetime
and the Geometric Nature of Funda... | null | null | NORDITA-2000/125 HE, SPIN-2000/36 | hep-th | null | We review recent results in the study of regular four dimensional BPS black
holes in toroidally compactified type II (or M) theory. We discuss the
generating solution for this kind of black holes, its microscopic
description(s), and compute the corresponding microscopic entropy. These
achievements, which provide a de... | [
{
"created": "Wed, 20 Dec 2000 22:46:09 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bertolini",
"M.",
""
],
[
"Trigiante",
"M.",
""
]
] | We review recent results in the study of regular four dimensional BPS black holes in toroidally compactified type II (or M) theory. We discuss the generating solution for this kind of black holes, its microscopic description(s), and compute the corresponding microscopic entropy. These achievements, which provide a desc... | 12.231078 | 11.517175 | 13.791629 | 11.527647 | 10.639599 | 11.196185 | 11.041021 | 11.287302 | 10.93938 | 13.292116 | 11.388302 | 11.692922 | 12.692262 | 11.448685 | 11.84586 | 11.38156 | 11.602206 | 11.616685 | 11.586051 | 12.416525 | 11.616331 |
0910.3225 | Joan Simon | Joan Simon | Small Black holes vs horizonless solutions in AdS | 10 pages; v2 improved entropy discussion and new references included | Phys.Rev.D81:024003,2010 | 10.1103/PhysRevD.81.024003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is argued that the appropriate macroscopic description of half-BPS mesonic
chiral operators in generic $d=4$ ${\cal N}=1$ toric gauge theories is in terms
of the geometric quantization of smooth horizonless configurations. The
relevance of different ensemble macroscopic descriptions is emphasized :
lorentzian vs e... | [
{
"created": "Fri, 16 Oct 2009 20:46:35 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Nov 2009 10:34:13 GMT",
"version": "v2"
}
] | 2010-01-27 | [
[
"Simon",
"Joan",
""
]
] | It is argued that the appropriate macroscopic description of half-BPS mesonic chiral operators in generic $d=4$ ${\cal N}=1$ toric gauge theories is in terms of the geometric quantization of smooth horizonless configurations. The relevance of different ensemble macroscopic descriptions is emphasized : lorentzian vs euc... | 20.610147 | 16.997099 | 19.125666 | 16.63773 | 18.670523 | 17.463799 | 18.056541 | 16.474566 | 17.99296 | 22.038624 | 18.180159 | 16.941444 | 17.076939 | 16.157656 | 16.661663 | 17.081858 | 17.492126 | 17.815498 | 16.659302 | 17.925928 | 16.705349 |
1708.03048 | Jason Wien | Donald Marolf and Jason Wien | The Torus Operator in Holography | 42 pages, 24 figures, introduction rewritten for clarity, appendix
added | null | 10.1007/JHEP01(2018)105 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the non-local operator ${\mathcal T}$ defined in 2-dimensional
CFTs by the path integral over a torus with two punctures. Using the AdS/CFT
correspondence, we study the spectrum and ground state of this operator in
holographic such CFTs in the limit of large central charge $c$. In one region
of moduli spa... | [
{
"created": "Thu, 10 Aug 2017 02:00:29 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Oct 2017 20:06:43 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Dec 2017 01:27:43 GMT",
"version": "v3"
}
] | 2018-03-14 | [
[
"Marolf",
"Donald",
""
],
[
"Wien",
"Jason",
""
]
] | We consider the non-local operator ${\mathcal T}$ defined in 2-dimensional CFTs by the path integral over a torus with two punctures. Using the AdS/CFT correspondence, we study the spectrum and ground state of this operator in holographic such CFTs in the limit of large central charge $c$. In one region of moduli space... | 10.332887 | 10.977088 | 10.939487 | 10.171928 | 10.296803 | 10.785336 | 11.538653 | 10.537841 | 10.091622 | 13.157279 | 10.294325 | 9.977571 | 10.787839 | 10.183784 | 10.370962 | 10.070032 | 10.36363 | 10.178745 | 10.152429 | 10.949517 | 9.874023 |
hep-th/0001015 | Alice Rogers | Alice Rogers | Canonical Quantization and Topological Theories | LaTeX, 8 pages, talk given at QG99, Third Meeting on Constrained
Dynamics and Quantum Gravity, Villasimius (Sardinia, Italy) September 13-17,
1999 | Nucl.Phys.Proc.Suppl. 88 (2000) 377-380 | 10.1016/S0920-5632(00)00806-9 | KCL-MTH-99-50 | hep-th | null | The canonical quantization of the topological particle is described; it is
shown that BRST quantization of the model gives the supersymmetric quantum
mechanical model considered by Witten when investigating Morse theory, and the
rigorous path integral method appropriate for this model is discussed.
Possibilities for ... | [
{
"created": "Tue, 4 Jan 2000 16:36:29 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Rogers",
"Alice",
""
]
] | The canonical quantization of the topological particle is described; it is shown that BRST quantization of the model gives the supersymmetric quantum mechanical model considered by Witten when investigating Morse theory, and the rigorous path integral method appropriate for this model is discussed. Possibilities for th... | 15.872146 | 14.688181 | 17.360981 | 13.815887 | 12.634836 | 12.795117 | 13.652451 | 13.956939 | 13.627695 | 17.156763 | 14.652555 | 14.149741 | 16.735849 | 15.178122 | 14.383627 | 14.236396 | 14.389554 | 14.475308 | 14.45412 | 16.745403 | 14.151695 |
1111.5852 | Fabian Ruehle | Michael Blaszczyk, Stefan Groot Nibbelink, Fabian Ruehle | Gauged Linear Sigma Models for toroidal orbifold resolutions | 71 pages, 2 figures | JHEP 1205:053,2012 | 10.1007/JHEP05(2012)053 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Toroidal orbifolds and their resolutions are described within the framework
of (2,2) Gauged Linear Sigma Models (GLSMs). Our procedure describes two-tori
as hypersurfaces in (weighted) projective spaces. The description is chosen
such that the orbifold singularities correspond to the zeros of their
homogeneous coordi... | [
{
"created": "Thu, 24 Nov 2011 21:15:08 GMT",
"version": "v1"
}
] | 2012-06-18 | [
[
"Blaszczyk",
"Michael",
""
],
[
"Nibbelink",
"Stefan Groot",
""
],
[
"Ruehle",
"Fabian",
""
]
] | Toroidal orbifolds and their resolutions are described within the framework of (2,2) Gauged Linear Sigma Models (GLSMs). Our procedure describes two-tori as hypersurfaces in (weighted) projective spaces. The description is chosen such that the orbifold singularities correspond to the zeros of their homogeneous coordina... | 12.314409 | 11.828746 | 13.103812 | 11.547832 | 11.977719 | 12.619576 | 12.507513 | 12.056593 | 11.573769 | 14.38977 | 11.200959 | 11.190837 | 12.005898 | 11.407977 | 12.422482 | 12.067369 | 11.712562 | 11.178573 | 11.29678 | 11.585105 | 11.463254 |
1409.6754 | Sebastian Fischetti | Sebastian Fischetti, Donald Marolf, Aron C. Wall | A paucity of bulk entangling surfaces: AdS wormholes with de Sitter
interiors | 27+10 pages. v2: minor modifications to address referee comments. v3:
fixed typos | Class. Quant. Grav. 32 (2015) 6, 065011 | 10.1088/0264-9381/32/6/065011 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study and construct spacetimes, dubbed planar AdS-dS-wormholes, satisfying
the null energy condition and having two asymptotically AdS boundaries
connected through a (non-traversable) inflating wormhole. As for other
wormholes, it is natural to expect dual descriptions in terms of two
disconnected CFTs in appropri... | [
{
"created": "Tue, 23 Sep 2014 20:48:57 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Aug 2015 20:58:01 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Jan 2016 14:54:16 GMT",
"version": "v3"
}
] | 2016-01-20 | [
[
"Fischetti",
"Sebastian",
""
],
[
"Marolf",
"Donald",
""
],
[
"Wall",
"Aron C.",
""
]
] | We study and construct spacetimes, dubbed planar AdS-dS-wormholes, satisfying the null energy condition and having two asymptotically AdS boundaries connected through a (non-traversable) inflating wormhole. As for other wormholes, it is natural to expect dual descriptions in terms of two disconnected CFTs in appropriat... | 11.535373 | 12.752165 | 13.700752 | 11.36494 | 11.836211 | 13.024278 | 13.124278 | 12.388962 | 11.944505 | 13.764762 | 11.322373 | 11.271778 | 11.747481 | 11.037908 | 11.345859 | 11.488499 | 11.401019 | 10.977278 | 11.248067 | 12.064029 | 11.128635 |
hep-th/0202204 | Hrvoje Nikolic | H. Nikolic | The general-covariant and gauge-invariant theory of quantum particles in
classical backgrounds | 34 pages, revised, to appear in Int. J. Mod. Phys. D | Int.J.Mod.Phys.D12:407-444,2003 | 10.1142/S0218271803002779 | null | hep-th gr-qc | null | A new approach to the concept of particles and their production in quantum
field theory is developed. A local operator describing the current of particle
density is constructed for scalar and spinor fields in arbitrary gravitational
and electromagnetic backgrounds. This enables one to describe particles in a
local, g... | [
{
"created": "Thu, 28 Feb 2002 13:53:37 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Oct 2002 09:11:47 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Nikolic",
"H.",
""
]
] | A new approach to the concept of particles and their production in quantum field theory is developed. A local operator describing the current of particle density is constructed for scalar and spinor fields in arbitrary gravitational and electromagnetic backgrounds. This enables one to describe particles in a local, gen... | 7.106788 | 7.766936 | 7.407395 | 6.790151 | 7.277844 | 7.1968 | 7.547246 | 6.86553 | 7.032808 | 7.926939 | 7.001492 | 7.00084 | 7.041256 | 7.058293 | 6.953943 | 7.304325 | 7.073993 | 6.868908 | 6.942891 | 7.095934 | 7.010652 |
2208.05700 | Peter M. Lavrov | P.M. Lavrov | On interactions of massless spin 3 and scalar fields | 11 pages, v2: ref added, minor corrections, v3: typos corrected,
section Discussion extended, published version, v4:in Section 4 and
Discussion correction of conclusions about cubic vertices made | Eur. Phys. J. C (2022) 82:1059 | 10.1140/epjc/s10052-022-11038-w | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using new approach for the deformation procedure in the case of reducible
gauge theories (Lavrov in Eur. Phys. J. C 82:429, 2022), it is shown that in
the model of massless spin 3 field and a real scalar field local cubic and
quartic vertices invariant under original gauge transformations can be
explicitly constructe... | [
{
"created": "Thu, 11 Aug 2022 08:52:08 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Aug 2022 05:26:49 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Sep 2022 11:20:20 GMT",
"version": "v3"
},
{
"created": "Thu, 24 Nov 2022 02:56:56 GMT",
"version": "v4"
},
{
"c... | 2023-04-28 | [
[
"Lavrov",
"P. M.",
""
]
] | Using new approach for the deformation procedure in the case of reducible gauge theories (Lavrov in Eur. Phys. J. C 82:429, 2022), it is shown that in the model of massless spin 3 field and a real scalar field local cubic and quartic vertices invariant under original gauge transformations can be explicitly constructed. | 18.813818 | 13.441805 | 15.065152 | 12.033585 | 11.852411 | 13.23551 | 12.57873 | 12.055328 | 12.488592 | 21.07432 | 12.704903 | 13.400064 | 13.950381 | 13.053188 | 12.694377 | 12.476886 | 12.47841 | 12.42972 | 13.131183 | 14.629707 | 13.366321 |
1610.05886 | Shu Lin | Er-dong Guo and Shu Lin | Quark Mass Correction to Chiral Separation Effect and Pseudoscalar
Condensate | 23 pages, 5 figures. additional normalizable modes included,
published version | null | 10.1007/JHEP01(2017)111 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derived an analytic structure of the quark mass correction to chiral
separation effect (CSE) in small mass regime. We confirmed this structure by a
D3/D7 holographic model study in a finite density, finite magnetic field
background. The quark mass correction to CSE can be related to correlators of
pseudo-scalar co... | [
{
"created": "Wed, 19 Oct 2016 07:10:48 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Nov 2017 00:44:53 GMT",
"version": "v2"
}
] | 2017-11-20 | [
[
"Guo",
"Er-dong",
""
],
[
"Lin",
"Shu",
""
]
] | We derived an analytic structure of the quark mass correction to chiral separation effect (CSE) in small mass regime. We confirmed this structure by a D3/D7 holographic model study in a finite density, finite magnetic field background. The quark mass correction to CSE can be related to correlators of pseudo-scalar cond... | 10.16776 | 12.555738 | 11.138221 | 10.72537 | 10.595739 | 11.386793 | 11.126012 | 11.631305 | 11.414847 | 12.057709 | 10.411145 | 10.499382 | 10.410719 | 10.168863 | 10.439547 | 10.315897 | 10.399377 | 10.517148 | 10.262301 | 10.382701 | 10.165261 |
1510.08486 | Slava Rychkov | Slava Rychkov, Pierre Yvernay | Remarks on the Convergence Properties of the Conformal Block Expansion | 12pp | null | 10.1016/j.physletb.2016.01.004 | CERN PH-TH/2015-253 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how to refine conformal block expansion convergence estimates from
hep-th/1208.6449. In doing so we find a novel explicit formula for the 3d
conformal blocks on the real axis.
| [
{
"created": "Wed, 28 Oct 2015 21:01:24 GMT",
"version": "v1"
}
] | 2016-02-17 | [
[
"Rychkov",
"Slava",
""
],
[
"Yvernay",
"Pierre",
""
]
] | We show how to refine conformal block expansion convergence estimates from hep-th/1208.6449. In doing so we find a novel explicit formula for the 3d conformal blocks on the real axis. | 19.372112 | 27.918264 | 23.824299 | 21.674936 | 29.049095 | 28.365046 | 24.580259 | 24.728172 | 22.589394 | 24.970587 | 20.562042 | 20.606842 | 22.823303 | 18.558165 | 19.993879 | 22.22636 | 18.945967 | 21.8696 | 19.420174 | 20.485527 | 19.788855 |
2001.07117 | Subham Dutta Chowdhury | Soumangsu Chakraborty, Subham Dutta Chowdhury, Tushar Gopalka, Suman
Kundu, Shiraz Minwalla, Amiya Mishra | Classification of all 3 particle S-matrices quadratic in photons or
gravitons | added references | null | 10.1007/JHEP04(2020)110 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly construct every kinematically allowed three particle
graviton-graviton-$P$ and photon-photon-$P$ S-matrix in every dimension and for
every choice of the little group representation of the massive particle $P$. We
also explicitly construct the spacetime Lagrangian that generates each of these
couplings. ... | [
{
"created": "Mon, 20 Jan 2020 14:23:47 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Feb 2020 09:46:30 GMT",
"version": "v2"
}
] | 2020-05-20 | [
[
"Chakraborty",
"Soumangsu",
""
],
[
"Chowdhury",
"Subham Dutta",
""
],
[
"Gopalka",
"Tushar",
""
],
[
"Kundu",
"Suman",
""
],
[
"Minwalla",
"Shiraz",
""
],
[
"Mishra",
"Amiya",
""
]
] | We explicitly construct every kinematically allowed three particle graviton-graviton-$P$ and photon-photon-$P$ S-matrix in every dimension and for every choice of the little group representation of the massive particle $P$. We also explicitly construct the spacetime Lagrangian that generates each of these couplings. In... | 10.267456 | 10.004748 | 10.435286 | 9.418861 | 10.550076 | 10.368064 | 9.412518 | 9.852256 | 9.402753 | 11.181212 | 9.541285 | 9.540752 | 10.351442 | 9.537059 | 9.794642 | 9.559234 | 9.440966 | 9.382355 | 9.556535 | 10.687651 | 9.629959 |
1210.4238 | Masato Nozawa | Hideo Kodama and Masato Nozawa | Classification and stability of vacua in maximal gauged supergravity | 26 pages, 2 tables; v2: improved arguments on vacuum classification,
typos corrected; v3: final version to appear in JHEP | null | 10.1007/JHEP01(2013)045 | KEK-TH-1582; KEK-Cosmo-105 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article presents a systematic study of critical points for the SL(8,
R)-type gauging in four dimensional maximal gauged supergravity. We determine
all the possible vacua for which the origin of the moduli space becomes a
critical point. We formulate a new tool which enables us to find analytically
the mass spect... | [
{
"created": "Tue, 16 Oct 2012 03:13:29 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Oct 2012 02:21:28 GMT",
"version": "v2"
},
{
"created": "Mon, 7 Jan 2013 05:17:55 GMT",
"version": "v3"
}
] | 2015-06-11 | [
[
"Kodama",
"Hideo",
""
],
[
"Nozawa",
"Masato",
""
]
] | This article presents a systematic study of critical points for the SL(8, R)-type gauging in four dimensional maximal gauged supergravity. We determine all the possible vacua for which the origin of the moduli space becomes a critical point. We formulate a new tool which enables us to find analytically the mass spectru... | 8.059524 | 8.873146 | 10.014895 | 8.352302 | 8.776226 | 9.008883 | 9.08901 | 8.297984 | 8.821187 | 10.343296 | 8.520382 | 8.417344 | 8.228027 | 8.048463 | 8.203996 | 8.263816 | 8.172277 | 8.133564 | 8.147774 | 8.448185 | 8.334262 |
hep-th/0506054 | Ichiro Oda | Ichiro Oda, Mario Tonin | Worldline Approach of Topological BF Theory | 12 pages, no figures, references added | Phys.Lett. B623 (2005) 155-164 | 10.1016/j.physletb.2005.07.037 | EDO-EP-50, DFPD 05/TH/17 | hep-th | null | We present a worldline description of topological non-abelian BF theory in
arbitrary space-time dimensions. It is shown that starting with a trivial
classical action defined on the worldline, the BRST cohomology has a natural
representation as the sum of the de Rham cohomology. Based on this observation,
we construct... | [
{
"created": "Tue, 7 Jun 2005 08:03:24 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Jun 2005 10:22:26 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Oda",
"Ichiro",
""
],
[
"Tonin",
"Mario",
""
]
] | We present a worldline description of topological non-abelian BF theory in arbitrary space-time dimensions. It is shown that starting with a trivial classical action defined on the worldline, the BRST cohomology has a natural representation as the sum of the de Rham cohomology. Based on this observation, we construct a... | 8.941916 | 8.802686 | 9.760891 | 7.925461 | 8.094954 | 8.304564 | 8.53616 | 8.156091 | 8.239773 | 10.348454 | 7.904526 | 8.684756 | 8.908167 | 8.161313 | 8.296108 | 8.42163 | 8.199563 | 8.451401 | 8.197097 | 8.802862 | 8.364899 |
1601.06851 | Yu Nakayama | Yu Nakayama | Bootstrapping critical Ising model on three-dimensional real projective
space | 5 pages with appendix, v2: published version with updates | Phys. Rev. Lett. 116, 141602 (2016) | 10.1103/PhysRevLett.116.141602 | IPMU16-0008 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given a conformal data on a flat Euclidean space, we use crosscap conformal
bootstrap equations to numerically solve the Lee-Yang model as well as the
critical Ising model on a three-dimensional real projective space. We check the
rapid convergence of our bootstrap program in two-dimensions from the exact
solutions a... | [
{
"created": "Mon, 25 Jan 2016 23:55:32 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Apr 2016 01:58:05 GMT",
"version": "v2"
}
] | 2016-04-20 | [
[
"Nakayama",
"Yu",
""
]
] | Given a conformal data on a flat Euclidean space, we use crosscap conformal bootstrap equations to numerically solve the Lee-Yang model as well as the critical Ising model on a three-dimensional real projective space. We check the rapid convergence of our bootstrap program in two-dimensions from the exact solutions ava... | 9.146725 | 9.6114 | 11.8001 | 8.865164 | 9.255293 | 9.694579 | 8.878351 | 8.943106 | 8.847057 | 13.201103 | 8.818377 | 8.893787 | 8.952288 | 8.915413 | 9.068795 | 8.814602 | 8.622035 | 8.597497 | 8.856048 | 9.544488 | 8.580419 |
0808.1583 | Paul K. Townsend | Igor A. Bandos and Paul K. Townsend | SDiff Gauge Theory and the M2 Condensate | 38 pp. Minor revision of version 2 | JHEP 0902:013,2009 | 10.1088/1126-6708/2009/02/013 | DAMTP=2008-65 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a general formalism for the construction, in $D$-dimensional
Minkowski space, of gauge theories for which the gauge group is the
infinite-dimensional group SDiff$_n$ of volume-preserving diffeomorphisms of
some closed $n$-dimensional manifold. We then focus on the D=3 SDiff$_3$
superconformal gauge theory ... | [
{
"created": "Mon, 11 Aug 2008 21:02:11 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Dec 2008 18:57:41 GMT",
"version": "v2"
},
{
"created": "Sun, 18 Jan 2009 10:21:38 GMT",
"version": "v3"
}
] | 2009-02-09 | [
[
"Bandos",
"Igor A.",
""
],
[
"Townsend",
"Paul K.",
""
]
] | We develop a general formalism for the construction, in $D$-dimensional Minkowski space, of gauge theories for which the gauge group is the infinite-dimensional group SDiff$_n$ of volume-preserving diffeomorphisms of some closed $n$-dimensional manifold. We then focus on the D=3 SDiff$_3$ superconformal gauge theory de... | 5.504058 | 5.390814 | 5.819268 | 4.970437 | 5.370853 | 4.972049 | 5.62949 | 5.216999 | 5.009133 | 6.262764 | 5.10985 | 5.185267 | 5.494746 | 5.320563 | 5.195876 | 5.224463 | 5.126837 | 5.225053 | 5.088523 | 5.669111 | 5.191711 |
2205.10326 | Vincent Rivasseau | Mohamed Ouerfelli, Vincent Rivasseau and Mohamed Tamaazousti | The Tensor Track VII: From Quantum Gravity to Artificial Intelligence | 23 pages, 7 figures, 1 table | null | null | null | hep-th cs.NA math-ph math.MP math.NA | http://creativecommons.org/licenses/by/4.0/ | Assuming some familiarity with quantum field theory and with the tensor track
approach that one of us presented in the previous series Tensor Track I to VI,
we provide, as usual, the developments in quantum gravity of the last two
years. Next we present in some detail two algorithms inspired by Random Tensor
Theory w... | [
{
"created": "Sat, 30 Apr 2022 20:18:26 GMT",
"version": "v1"
}
] | 2023-01-06 | [
[
"Ouerfelli",
"Mohamed",
""
],
[
"Rivasseau",
"Vincent",
""
],
[
"Tamaazousti",
"Mohamed",
""
]
] | Assuming some familiarity with quantum field theory and with the tensor track approach that one of us presented in the previous series Tensor Track I to VI, we provide, as usual, the developments in quantum gravity of the last two years. Next we present in some detail two algorithms inspired by Random Tensor Theory whi... | 29.919037 | 37.652233 | 35.073704 | 29.326433 | 34.826218 | 34.727318 | 31.420496 | 30.537649 | 31.202959 | 37.631752 | 30.473864 | 31.085674 | 31.806526 | 30.71879 | 30.912951 | 30.012379 | 31.962229 | 30.361774 | 32.575783 | 32.188015 | 29.301022 |
hep-th/9603082 | Per Stjernberg | Ulf H. Danielsson and P\"ar Stjernberg (Uppsala University) | Notes on Equivalences and Higgs Branches in N=2 Supersymmetric
Yang-Mills Theory | 11 pages, Latex | Phys.Lett. B380 (1996) 68-74 | 10.1016/0370-2693(96)00431-5 | UUITP-4/96 | hep-th | null | In this paper we investigate how various equivalences between effective field
theories of $N=2$ SUSY Yang-Mills theory with matter can be understood through
Higgs breaking, i.e. by giving expectation values to squarks. We give explicit
expressions for the flat directions for a wide class of examples.
| [
{
"created": "Wed, 13 Mar 1996 15:56:03 GMT",
"version": "v1"
}
] | 2016-08-15 | [
[
"Danielsson",
"Ulf H.",
"",
"Uppsala University"
],
[
"Stjernberg",
"Pär",
"",
"Uppsala University"
]
] | In this paper we investigate how various equivalences between effective field theories of $N=2$ SUSY Yang-Mills theory with matter can be understood through Higgs breaking, i.e. by giving expectation values to squarks. We give explicit expressions for the flat directions for a wide class of examples. | 15.045065 | 10.559325 | 11.531404 | 11.781447 | 11.9144 | 11.351885 | 10.580851 | 11.154016 | 11.020629 | 14.110834 | 11.555728 | 11.548611 | 12.044179 | 10.72689 | 11.049079 | 11.806899 | 10.918864 | 11.133439 | 10.959637 | 12.033728 | 11.109358 |
2212.07344 | Xing-Yue Wei | Sung-Soo Kim, Yuji Sugimoto, Xing-Yue Wei, Futoshi Yagi | $DE$-type little strings from glued brane webs | v2: 97 pages, 32 figures, typos corrected and clarifications added | JHEP05(2023)214 | 10.1007/JHEP05(2023)214 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We propose brane web configurations for $D$-type and $E$-type
$\mathcal{N}=(1,0)$ little string theories based on a trivalent or quadrivalent
gluing of 5-brane web diagrams. Tri-/quadri-valent gluing is a powerful way of
computing 5d/6d partition functions for supersymmetric gauge theories based on
the topological ve... | [
{
"created": "Wed, 14 Dec 2022 17:13:32 GMT",
"version": "v1"
},
{
"created": "Mon, 29 May 2023 13:33:19 GMT",
"version": "v2"
}
] | 2023-05-30 | [
[
"Kim",
"Sung-Soo",
""
],
[
"Sugimoto",
"Yuji",
""
],
[
"Wei",
"Xing-Yue",
""
],
[
"Yagi",
"Futoshi",
""
]
] | We propose brane web configurations for $D$-type and $E$-type $\mathcal{N}=(1,0)$ little string theories based on a trivalent or quadrivalent gluing of 5-brane web diagrams. Tri-/quadri-valent gluing is a powerful way of computing 5d/6d partition functions for supersymmetric gauge theories based on the topological vert... | 6.425642 | 5.956986 | 7.303125 | 5.826695 | 6.166669 | 6.010659 | 5.998451 | 5.517612 | 5.728878 | 7.282967 | 5.755684 | 5.861284 | 6.653134 | 5.989074 | 5.913435 | 6.065351 | 5.994104 | 5.915803 | 6.016622 | 6.678387 | 6.154442 |
1012.4972 | Ta-Sheng Tai | Ta-Sheng Tai | Seiberg-Witten prepotential from WZNW conformal block: Langlands duality
and Selberg trace formula | 8 pages | Mod.Phys.Lett.A27:1250129,2012 | 10.1142/S0217732312501295 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how SU(2) $N_f=4$ Seiberg-Witten prepotentials are derived form
$\hat{\mathfrak{sl}}_{2,k}$ ($k\to2$) four-point conformal blocks via
considering Langlands duality.
| [
{
"created": "Wed, 22 Dec 2010 13:43:21 GMT",
"version": "v1"
}
] | 2012-08-06 | [
[
"Tai",
"Ta-Sheng",
""
]
] | We show how SU(2) $N_f=4$ Seiberg-Witten prepotentials are derived form $\hat{\mathfrak{sl}}_{2,k}$ ($k\to2$) four-point conformal blocks via considering Langlands duality. | 13.960028 | 11.15101 | 18.31851 | 11.229276 | 12.810424 | 12.71121 | 12.833077 | 11.430937 | 10.990438 | 19.799652 | 11.396999 | 11.513443 | 13.688867 | 11.966302 | 11.683494 | 12.215446 | 11.618468 | 10.834142 | 11.511623 | 13.698697 | 11.603326 |
1705.00292 | Pablo Bueno | Nikolay Bobev, Pablo Bueno and Yannick Vreys | Comments on Squashed-sphere Partition Functions | 40 pages, 7 figures, 1 table; v2: additional comments and
clarifications added, updated bibliography | JHEP 1707 (2017) 093 | 10.1007/JHEP07(2017)093 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the partition function of odd-dimensional conformal field theories
placed on spheres with a squashed metric. We establish that the round sphere
provides a local extremum for the free energy which, in general, is not a
global extremum. In addition, we show that the leading quadratic correction to
the free ene... | [
{
"created": "Sun, 30 Apr 2017 09:46:45 GMT",
"version": "v1"
},
{
"created": "Wed, 17 May 2017 07:43:41 GMT",
"version": "v2"
}
] | 2017-07-21 | [
[
"Bobev",
"Nikolay",
""
],
[
"Bueno",
"Pablo",
""
],
[
"Vreys",
"Yannick",
""
]
] | We study the partition function of odd-dimensional conformal field theories placed on spheres with a squashed metric. We establish that the round sphere provides a local extremum for the free energy which, in general, is not a global extremum. In addition, we show that the leading quadratic correction to the free energ... | 5.047489 | 5.189708 | 5.273669 | 4.897887 | 5.120188 | 5.04158 | 4.734159 | 4.776612 | 4.91707 | 5.79653 | 4.776898 | 4.813129 | 5.119719 | 4.87102 | 4.941733 | 4.972114 | 4.931442 | 4.815354 | 4.826552 | 5.086741 | 4.849026 |
hep-th/0304186 | Jelper Striet | F.A.Bais and J.Striet | Charge instabilities due to local charge conjugation symmetry in
(2+1)-dimensions | Latex, 26 pages, 12 figures | Nucl.Phys. B666 (2003) 243-268 | 10.1016/S0550-3213(03)00497-8 | ITFA-2003-20 | hep-th hep-ph | null | Alice electrodynamics (AED) is a theory of electrodynamics in which charge
conjugation is a local gauge symmetry. In this paper we investigate a charge
instability in alice electrodynamics in (2+1)-dimensions due to this local
charge conjugation. The instability manifests itself through the creation of a
pair of alic... | [
{
"created": "Tue, 22 Apr 2003 10:02:16 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Jun 2003 07:52:24 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Bais",
"F. A.",
""
],
[
"Striet",
"J.",
""
]
] | Alice electrodynamics (AED) is a theory of electrodynamics in which charge conjugation is a local gauge symmetry. In this paper we investigate a charge instability in alice electrodynamics in (2+1)-dimensions due to this local charge conjugation. The instability manifests itself through the creation of a pair of alice ... | 11.613898 | 11.069416 | 11.525135 | 10.402565 | 11.85777 | 10.451991 | 10.949968 | 10.884591 | 10.568423 | 13.704081 | 11.835242 | 10.317952 | 10.230491 | 9.953911 | 10.551152 | 10.123835 | 10.20056 | 10.321108 | 10.230009 | 10.94151 | 11.435298 |
1602.00607 | Merab Gogberashvili Prof | Merab Gogberashvili, Irakli Mantidze, Otari Sakhelashvili and Tsotne
Shengelia | Standing Waves Braneworlds | Journal version of the review paper, 39 pages, 15 figures | Int. J. Mod. Phys., D 25 (2016) 1630019 | 10.1142/S0218271816300196 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The class of non-stationary braneworld models generated by the coupled
gravitational and scalar fields is reviewed. The model represents a brane in a
space-time with single time and one large (infinite) and several small
(compact) space-like extra dimensions. In some particular cases the model has
the solutions corre... | [
{
"created": "Fri, 29 Jan 2016 08:47:59 GMT",
"version": "v1"
},
{
"created": "Wed, 18 May 2016 06:24:40 GMT",
"version": "v2"
}
] | 2016-05-19 | [
[
"Gogberashvili",
"Merab",
""
],
[
"Mantidze",
"Irakli",
""
],
[
"Sakhelashvili",
"Otari",
""
],
[
"Shengelia",
"Tsotne",
""
]
] | The class of non-stationary braneworld models generated by the coupled gravitational and scalar fields is reviewed. The model represents a brane in a space-time with single time and one large (infinite) and several small (compact) space-like extra dimensions. In some particular cases the model has the solutions corresp... | 14.164404 | 14.421535 | 11.635642 | 12.187151 | 13.407171 | 13.169657 | 13.360795 | 12.77141 | 12.992854 | 15.411547 | 13.47357 | 14.07473 | 13.577101 | 13.142259 | 12.975051 | 12.934611 | 13.881535 | 13.173642 | 13.828042 | 13.194303 | 13.461769 |
2212.14702 | Hugo Camargo | Hugo A. Camargo, Viktor Jahnke, Keun-Young Kim, Mitsuhiro Nishida | Krylov Complexity in Free and Interacting Scalar Field Theories with
Bounded Power Spectrum | V4: Added a clarification about the numerical fitting of the growth
rate of the Lanczos coefficients in Sec. 3.2. (See Eqs. 3.25-3.27 and above
paragraphs) | null | 10.1007/JHEP05(2023)226 | null | hep-th cond-mat.stat-mech quant-ph | http://creativecommons.org/licenses/by/4.0/ | We study a notion of operator growth known as Krylov complexity in free and
interacting massive scalar quantum field theories in $d$-dimensions at finite
temperature. We consider the effects of mass, one-loop self-energy due to
perturbative interactions, and finite ultraviolet cutoffs in continuous
momentum space. Th... | [
{
"created": "Fri, 30 Dec 2022 13:45:42 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Jan 2023 08:19:23 GMT",
"version": "v2"
},
{
"created": "Thu, 18 May 2023 02:23:28 GMT",
"version": "v3"
},
{
"created": "Mon, 1 Apr 2024 01:24:55 GMT",
"version": "v4"
}
] | 2024-04-02 | [
[
"Camargo",
"Hugo A.",
""
],
[
"Jahnke",
"Viktor",
""
],
[
"Kim",
"Keun-Young",
""
],
[
"Nishida",
"Mitsuhiro",
""
]
] | We study a notion of operator growth known as Krylov complexity in free and interacting massive scalar quantum field theories in $d$-dimensions at finite temperature. We consider the effects of mass, one-loop self-energy due to perturbative interactions, and finite ultraviolet cutoffs in continuous momentum space. Thes... | 13.124267 | 12.298895 | 16.051065 | 10.963137 | 11.952801 | 11.033148 | 12.175307 | 12.093158 | 11.494291 | 13.751418 | 10.561317 | 11.145414 | 12.835376 | 11.723834 | 11.366078 | 11.706863 | 11.564341 | 11.543496 | 11.418712 | 12.695213 | 11.339787 |
0812.3507 | Chang-Young Ee | Ee Chang-Young, Daeho Lee, Youngone Lee | Coordinate Dependence of Chern-Simons Theory on Noncommutative AdS3 | LaTeX 24 pages, action added, minor corrections | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the coordinate dependence of noncommutative theory by studying
the solutions of noncommutative $U(1,1)\times U(1,1)$ Chern-Simons theory on
$AdS_3$ in the polar and rectangular coordinates. We assume that only the space
coordinates are noncommuting. The two coordinate systems are equivalent only up
to ... | [
{
"created": "Thu, 18 Dec 2008 11:03:35 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Dec 2008 02:48:15 GMT",
"version": "v2"
},
{
"created": "Sun, 4 Jan 2009 04:18:55 GMT",
"version": "v3"
},
{
"created": "Fri, 6 Mar 2009 06:27:53 GMT",
"version": "v4"
}
] | 2009-03-06 | [
[
"Chang-Young",
"Ee",
""
],
[
"Lee",
"Daeho",
""
],
[
"Lee",
"Youngone",
""
]
] | We investigate the coordinate dependence of noncommutative theory by studying the solutions of noncommutative $U(1,1)\times U(1,1)$ Chern-Simons theory on $AdS_3$ in the polar and rectangular coordinates. We assume that only the space coordinates are noncommuting. The two coordinate systems are equivalent only up to fi... | 5.887105 | 5.776459 | 6.147055 | 5.535568 | 5.841704 | 6.421482 | 5.972729 | 5.539576 | 5.619748 | 6.187704 | 5.774653 | 5.66647 | 5.978071 | 5.730058 | 5.751721 | 5.87239 | 5.760582 | 5.736397 | 5.788503 | 5.923298 | 5.740542 |
hep-th/0309061 | V. Parameswaran Nair | V.P. Nair | Yang-Mills theory, 2+1 and 3+1 dimensions | 11 pages, LaTeX, Talk at "Space-time and Fundamental Interactions:
Quantum Aspects", conference in honor of A.P. Balachandran's 65th birthday,
Italy, May 2003; to be published in Mod. Phys. Lett | null | 10.1142/S0217732303012647 | CCNY-HEP 03/6 | hep-th | null | I review the analysis of (2+1)-dimensional Yang-Mills ($YM_{2+1})$ theory via
the use of gauge-invariant matrix variables. The vacuum wavefunction, string
tension, the propagator mass for gluons, its relation to the magnetic mass for
$YM_{3+1}$ at nonzero temperature and the extension of our analysis to the
Yang-Mill... | [
{
"created": "Fri, 5 Sep 2003 03:51:29 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Nair",
"V. P.",
""
]
] | I review the analysis of (2+1)-dimensional Yang-Mills ($YM_{2+1})$ theory via the use of gauge-invariant matrix variables. The vacuum wavefunction, string tension, the propagator mass for gluons, its relation to the magnetic mass for $YM_{3+1}$ at nonzero temperature and the extension of our analysis to the Yang-Mills-... | 9.192968 | 7.267259 | 9.2645 | 7.154668 | 7.630737 | 7.054593 | 7.429385 | 7.300783 | 7.068749 | 8.643214 | 7.375867 | 7.484872 | 8.624934 | 7.892118 | 8.060737 | 7.911651 | 7.967983 | 7.732123 | 7.754123 | 8.214448 | 7.829882 |
1706.03782 | Daniel Carney | Daniel Carney, Laurent Chaurette, Dominik Neuenfeld and Gordon Walter
Semenoff | Infrared quantum information | 5 pages. v2: slightly expanded remarks on black holes, including
explicit proposal for BH entropy; refs and acknowledgements added. version
submitted to PRL | Phys. Rev. Lett. 119, 180502 (2017) | 10.1103/PhysRevLett.119.180502 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss information-theoretic properties of low-energy photons and
gravitons in the S-matrix. Given an incoming n-particle momentum eigenstate, we
demonstrate that unobserved soft photons decohere nearly all outgoing momentum
superpositions of charged particles, while the universality of gravity implies
that soft ... | [
{
"created": "Mon, 12 Jun 2017 18:00:09 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jun 2017 22:02:17 GMT",
"version": "v2"
}
] | 2017-11-08 | [
[
"Carney",
"Daniel",
""
],
[
"Chaurette",
"Laurent",
""
],
[
"Neuenfeld",
"Dominik",
""
],
[
"Semenoff",
"Gordon Walter",
""
]
] | We discuss information-theoretic properties of low-energy photons and gravitons in the S-matrix. Given an incoming n-particle momentum eigenstate, we demonstrate that unobserved soft photons decohere nearly all outgoing momentum superpositions of charged particles, while the universality of gravity implies that soft gr... | 9.210034 | 10.6923 | 9.539874 | 9.09757 | 9.860054 | 9.905927 | 9.702159 | 10.254967 | 8.853882 | 11.572185 | 8.99786 | 9.24332 | 9.6895 | 9.02387 | 8.643186 | 9.314756 | 9.010151 | 8.919399 | 8.800575 | 9.212629 | 8.899077 |
1507.02641 | Ehsan Hatefi | Ehsan Hatefi | On New Bulk Singularity Structures, RR Couplings in Asymmetric Picture
and Their All Order $\alpha'$ Corrections | 34 pages, minor clarifications added. Published version in EPJC | Eur. Phys. J. C (2017) 77:520 | 10.1140/epjc/s10052-017-5108-y | null | hep-th gr-qc hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have analyzed in detail four and five point functions of the string theory
amplitudes, including a closed string Ramond-Ramond (RR) in an asymmetric
picture and either two or three transverse scalar fields in both IIA and IIB.
The complete forms of these S-matrices are derived and these asymmetric
S-matrices are a... | [
{
"created": "Thu, 9 Jul 2015 18:32:16 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jan 2016 19:21:40 GMT",
"version": "v2"
},
{
"created": "Sun, 30 Apr 2017 19:50:26 GMT",
"version": "v3"
},
{
"created": "Tue, 25 Jul 2017 10:03:36 GMT",
"version": "v4"
}
] | 2017-08-08 | [
[
"Hatefi",
"Ehsan",
""
]
] | We have analyzed in detail four and five point functions of the string theory amplitudes, including a closed string Ramond-Ramond (RR) in an asymmetric picture and either two or three transverse scalar fields in both IIA and IIB. The complete forms of these S-matrices are derived and these asymmetric S-matrices are als... | 16.699112 | 11.635055 | 17.195793 | 14.50152 | 12.379121 | 12.33749 | 12.389503 | 12.133717 | 12.852115 | 19.626873 | 13.053699 | 14.320372 | 16.703169 | 14.977684 | 14.28421 | 13.973703 | 13.93895 | 14.371046 | 15.24593 | 16.849112 | 14.753824 |
1811.01023 | Yusuke Yamada | Renata Kallosh, Andrei Linde, Yusuke Yamada | Planck 2018 and Brane Inflation Revisited | 29 pages, 8 figures | null | 10.1007/JHEP01(2019)008 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit phenomenological as well as string-theoretical aspects of D-brane
inflation cosmological models. Phenomenologically these models stand out on par
with $\alpha$-attractors, as models with Planck-compatible values of $n_s$,
moving down to the sweet spot in the data with decreasing value of $r$. On the
formal... | [
{
"created": "Fri, 2 Nov 2018 18:00:24 GMT",
"version": "v1"
}
] | 2019-01-30 | [
[
"Kallosh",
"Renata",
""
],
[
"Linde",
"Andrei",
""
],
[
"Yamada",
"Yusuke",
""
]
] | We revisit phenomenological as well as string-theoretical aspects of D-brane inflation cosmological models. Phenomenologically these models stand out on par with $\alpha$-attractors, as models with Planck-compatible values of $n_s$, moving down to the sweet spot in the data with decreasing value of $r$. On the formal s... | 13.503291 | 12.721479 | 13.339409 | 12.023249 | 13.091064 | 13.034673 | 12.761891 | 10.880336 | 12.352165 | 14.04632 | 12.055696 | 12.271762 | 12.50887 | 11.828179 | 12.28283 | 12.045758 | 12.189723 | 11.482458 | 12.111974 | 12.372102 | 11.786874 |
hep-th/0104044 | Michael Gutperle | Michael Gutperle and Wafic A. Sabra | A Supersymmetric Solution in N=2 Gauged Supergravity with the Universal
Hypermultiplet | 15 pages, Latex, no figures | Phys.Lett. B511 (2001) 311-318 | 10.1016/S0370-2693(01)00643-8 | HUTP-01/A017 | hep-th | null | We present supersymmetric solutions for the theory of gauged supergravity in
five dimensions obtained by gauging the shift symmetry of the axion of the
universal hypermultiplet. This gauged theory can also be obtained by
dimensionally reducing M-theory on a Calabi-Yau threefold with background flux.
The solution foun... | [
{
"created": "Thu, 5 Apr 2001 21:06:37 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Gutperle",
"Michael",
""
],
[
"Sabra",
"Wafic A.",
""
]
] | We present supersymmetric solutions for the theory of gauged supergravity in five dimensions obtained by gauging the shift symmetry of the axion of the universal hypermultiplet. This gauged theory can also be obtained by dimensionally reducing M-theory on a Calabi-Yau threefold with background flux. The solution found ... | 9.051991 | 8.347293 | 10.575307 | 8.590445 | 8.978506 | 8.808487 | 8.576053 | 7.398609 | 7.923313 | 11.656568 | 8.675519 | 8.131197 | 10.054369 | 8.431343 | 8.412351 | 8.50253 | 8.412578 | 8.62339 | 8.284976 | 10.144443 | 8.311828 |
hep-th/9903181 | Changhyun Ahn | Changhyun Ahn and Hoil Kim | Branes at $\C^4/\Ga$ Singularity from Toric Geometry | 1 figure, 4 tables, latex file and 26 pages:v1 added mathematical
results on projective crepant resolutions by Dais et al and refs added:v2
typos corrected and the beginning paragrphs in section 3 clarified | JHEP 9904 (1999) 012 | 10.1088/1126-6708/1999/04/012 | SNUTP-99-011 | hep-th | null | We study toric singularities of the form of $\C^4/\Ga$ for finite abelian
groups $\Ga \subset SU(4)$. In particular, we consider the simplest case
$\Ga=\Z_2 \times \Z_2 \times \Z_2$ and find explicitly charge matrices for
partial resolutions of this orbifold by extending the method by Morrison and
Plesser. We obtain ... | [
{
"created": "Mon, 22 Mar 1999 08:06:49 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Mar 1999 06:19:51 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Apr 1999 12:07:15 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Ahn",
"Changhyun",
""
],
[
"Kim",
"Hoil",
""
]
] | We study toric singularities of the form of $\C^4/\Ga$ for finite abelian groups $\Ga \subset SU(4)$. In particular, we consider the simplest case $\Ga=\Z_2 \times \Z_2 \times \Z_2$ and find explicitly charge matrices for partial resolutions of this orbifold by extending the method by Morrison and Plesser. We obtain th... | 6.494656 | 6.396145 | 7.105575 | 6.117596 | 6.8555 | 6.75881 | 6.561615 | 6.590453 | 6.365494 | 8.142928 | 6.056787 | 6.097259 | 6.540292 | 6.143359 | 6.255868 | 6.091756 | 6.178093 | 6.179845 | 6.272621 | 6.527718 | 5.996265 |
hep-th/0009112 | Yaron Oz | Yaron Oz, Tony Pantev and Daniel Waldram | Brane-Antibrane Systems on Calabi-Yau Spaces | 25 pages, Latex | JHEP 0102:045,2001 | 10.1088/1126-6708/2001/02/045 | CERN-TH/2000-174 | hep-th | null | We propose a correspondence between brane-antibrane systems and stable
triples (E_1,E_2,T), where E_1,E_2 are holomorphic vector bundles and the
tachyon T is a map between them. We demonstrate that, under the assumption of
holomorphicity, the brane-antibrane field equations reduce to a set of vortex
equations, which ... | [
{
"created": "Thu, 14 Sep 2000 12:27:51 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Oz",
"Yaron",
""
],
[
"Pantev",
"Tony",
""
],
[
"Waldram",
"Daniel",
""
]
] | We propose a correspondence between brane-antibrane systems and stable triples (E_1,E_2,T), where E_1,E_2 are holomorphic vector bundles and the tachyon T is a map between them. We demonstrate that, under the assumption of holomorphicity, the brane-antibrane field equations reduce to a set of vortex equations, which ar... | 7.784097 | 8.037155 | 8.453337 | 7.368215 | 7.696796 | 8.239033 | 7.995564 | 7.537905 | 7.389285 | 8.255918 | 7.833055 | 7.497376 | 8.005843 | 7.471837 | 7.300931 | 7.33168 | 7.231566 | 7.1884 | 7.562357 | 7.876452 | 7.294507 |
2303.12482 | Azadeh Mohammadi | Dionisio Bazeia, Jo\~ao G. F. Campos and Azadeh Mohammadi | Kink-antikink collisions in the $\phi^8$ model: short-range to
long-range journey | null | JHEP 05 (2023) 116 | 10.1007/JHEP05(2023)116 | null | hep-th nlin.PS | http://creativecommons.org/licenses/by/4.0/ | We studied kink-antikink collisions in (1+1)-dimensional spacetime for all
$Z_2$ symmetric $\phi^8$ models with four degenerate minima. Such a polynomial
model has only one free parameter, allowing us to conduct an exhaustive
analysis. We performed detailed simulations in all three sectors of the model.
We observed r... | [
{
"created": "Wed, 22 Mar 2023 11:50:25 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Jun 2023 16:31:43 GMT",
"version": "v2"
}
] | 2023-06-26 | [
[
"Bazeia",
"Dionisio",
""
],
[
"Campos",
"João G. F.",
""
],
[
"Mohammadi",
"Azadeh",
""
]
] | We studied kink-antikink collisions in (1+1)-dimensional spacetime for all $Z_2$ symmetric $\phi^8$ models with four degenerate minima. Such a polynomial model has only one free parameter, allowing us to conduct an exhaustive analysis. We performed detailed simulations in all three sectors of the model. We observed res... | 12.588783 | 10.542406 | 13.242749 | 11.098482 | 12.543823 | 11.435486 | 11.825111 | 11.338319 | 11.426067 | 14.311135 | 10.98616 | 11.675416 | 12.127656 | 11.282255 | 11.61989 | 11.420157 | 11.669255 | 11.629754 | 11.806066 | 12.434566 | 11.5046 |
1011.0463 | Fernando C. Lombardo | C.D. Fosco, F.C. Lombardo, and F.D. Mazzitelli | Inertial forces and dissipation on accelerated boundaries | 7 pages, no figures | Phys.Rev.D82:125039,2010 | 10.1103/PhysRevD.82.125039 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study dissipative effects due to inertial forces acting on matter fields
confined to accelerated boundaries in $1+1$, $2+1$, and $3+1$ dimensions. These
matter fields describe the internal degrees of freedom of `mirrors' and impose,
on the surfaces where they are defined, boundary conditions on a fluctuating
`vacu... | [
{
"created": "Mon, 1 Nov 2010 22:25:58 GMT",
"version": "v1"
}
] | 2011-03-07 | [
[
"Fosco",
"C. D.",
""
],
[
"Lombardo",
"F. C.",
""
],
[
"Mazzitelli",
"F. D.",
""
]
] | We study dissipative effects due to inertial forces acting on matter fields confined to accelerated boundaries in $1+1$, $2+1$, and $3+1$ dimensions. These matter fields describe the internal degrees of freedom of `mirrors' and impose, on the surfaces where they are defined, boundary conditions on a fluctuating `vacuum... | 10.8909 | 8.948481 | 9.775716 | 9.161942 | 9.278738 | 9.393385 | 9.523391 | 9.948982 | 9.18822 | 10.348698 | 9.088775 | 9.944592 | 9.912507 | 9.275685 | 9.955969 | 9.705562 | 9.442163 | 9.349131 | 9.659329 | 9.580201 | 9.757517 |
2106.09560 | Romanczukiewicz Tomasz Ph.D. | Patrick Dorey, Anastasia Gorina, Ilya Perapechka, Tomasz
Roma\'nczukiewicz and Yakov Shnir | Resonance structures in kink-antikink collisions in a deformed
sine-Gordon model | 40 pages, 31 figures | null | 10.1007/JHEP09(2021)145 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study kink-antikink collisions in a model which interpolates smoothly
between the completely integrable sine-Gordon theory, the $\phi^4$ model, and a
$\phi^6$-like model with three degenerate vacua. We find a rich variety of
behaviours, including integrability breaking, resonance windows with
increasingly irregula... | [
{
"created": "Thu, 17 Jun 2021 14:40:48 GMT",
"version": "v1"
}
] | 2021-10-13 | [
[
"Dorey",
"Patrick",
""
],
[
"Gorina",
"Anastasia",
""
],
[
"Perapechka",
"Ilya",
""
],
[
"Romańczukiewicz",
"Tomasz",
""
],
[
"Shnir",
"Yakov",
""
]
] | We study kink-antikink collisions in a model which interpolates smoothly between the completely integrable sine-Gordon theory, the $\phi^4$ model, and a $\phi^6$-like model with three degenerate vacua. We find a rich variety of behaviours, including integrability breaking, resonance windows with increasingly irregular ... | 9.048515 | 7.141112 | 8.795728 | 7.711415 | 7.291893 | 7.138049 | 7.086531 | 7.690567 | 6.977843 | 9.479513 | 7.133292 | 7.422091 | 8.665336 | 7.89075 | 7.479308 | 7.458698 | 7.569072 | 7.591386 | 7.560269 | 8.421107 | 7.619452 |
1806.09703 | Pedro Liendo | Mikhail Isachenkov, Pedro Liendo, Yannick Linke, Volker Schomerus | Calogero-Sutherland Approach to Defect Blocks | v2: changes for clarity | null | 10.1007/JHEP10(2018)204 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Extended objects such as line or surface operators, interfaces or boundaries
play an important role in conformal field theory. Here we propose a systematic
approach to the relevant conformal blocks which are argued to coincide with the
wave functions of an integrable multi-particle Calogero-Sutherland problem.
This g... | [
{
"created": "Mon, 25 Jun 2018 21:11:36 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Nov 2018 20:02:22 GMT",
"version": "v2"
}
] | 2018-11-14 | [
[
"Isachenkov",
"Mikhail",
""
],
[
"Liendo",
"Pedro",
""
],
[
"Linke",
"Yannick",
""
],
[
"Schomerus",
"Volker",
""
]
] | Extended objects such as line or surface operators, interfaces or boundaries play an important role in conformal field theory. Here we propose a systematic approach to the relevant conformal blocks which are argued to coincide with the wave functions of an integrable multi-particle Calogero-Sutherland problem. This gen... | 16.548183 | 14.015765 | 21.784941 | 13.430135 | 14.029124 | 13.109249 | 14.146352 | 14.744143 | 14.198354 | 21.562929 | 14.239316 | 13.868523 | 17.776197 | 15.621309 | 15.028743 | 14.261941 | 14.850536 | 15.222484 | 15.582553 | 18.349642 | 14.361428 |
hep-th/0008147 | Marianne Rooman | M. Rooman and Ph. Spindel | Holonomies, anomalies and the Fefferman-Graham ambiguity in AdS3 gravity | LaTeX, 26 pages, 1 figure, modified version that will appear in Nucl.
Phys. B | Nucl.Phys. B594 (2001) 329-353 | 10.1016/S0550-3213(00)00636-2 | null | hep-th | null | Using the Chern-Simon formulation of (2+1) gravity, we derive, for the
general asymptotic metrics given by the Fefferman-Graham-Lee theorems, the
emergence of the Liouville mode associated to the boundary degrees of freedom
of (2+1) dimensional anti de Sitter geometries. Holonomies are described
through multi-valued ... | [
{
"created": "Fri, 18 Aug 2000 09:57:13 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Nov 2000 08:34:00 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Rooman",
"M.",
""
],
[
"Spindel",
"Ph.",
""
]
] | Using the Chern-Simon formulation of (2+1) gravity, we derive, for the general asymptotic metrics given by the Fefferman-Graham-Lee theorems, the emergence of the Liouville mode associated to the boundary degrees of freedom of (2+1) dimensional anti de Sitter geometries. Holonomies are described through multi-valued ga... | 12.407975 | 11.018443 | 12.722052 | 10.959733 | 11.089695 | 10.908051 | 10.916449 | 10.897676 | 11.424325 | 13.762198 | 10.935984 | 10.929945 | 12.250216 | 11.30931 | 11.047074 | 11.559566 | 10.876472 | 11.039624 | 11.334514 | 12.20342 | 11.023088 |
1812.09314 | Xinan Zhou | Dalimil Maz\'a\v{c}, Leonardo Rastelli, Xinan Zhou | An Analytic Approach to BCFT$_d$ | 67 pages, 8 figures | null | 10.1007/JHEP12(2019)004 | PUPT-2580; YITP-44 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop an analytic approach to Boundary Conformal Field Theory (BCFT),
focussing on the two-point function of a general pair of scalar primary
operators. The resulting crossing equation can be thought of as a vector
equation in an infinite-dimensional space ${\cal V}$ of analytic functions of a
single complex var... | [
{
"created": "Fri, 21 Dec 2018 18:52:42 GMT",
"version": "v1"
}
] | 2020-01-29 | [
[
"Mazáč",
"Dalimil",
""
],
[
"Rastelli",
"Leonardo",
""
],
[
"Zhou",
"Xinan",
""
]
] | We develop an analytic approach to Boundary Conformal Field Theory (BCFT), focussing on the two-point function of a general pair of scalar primary operators. The resulting crossing equation can be thought of as a vector equation in an infinite-dimensional space ${\cal V}$ of analytic functions of a single complex varia... | 8.659827 | 8.728236 | 10.127515 | 8.400055 | 8.7751 | 8.829465 | 9.086646 | 8.563441 | 8.535716 | 11.375977 | 8.657784 | 8.529133 | 8.698226 | 8.501502 | 8.589618 | 8.551934 | 8.663323 | 8.459299 | 8.197492 | 8.947541 | 8.381172 |
hep-th/9511072 | Mikhail Plyushchay | G. Grignani, M. Plyushchay and P. Sodano | A Pseudoclassical Model for $P,T-$Invariant Planar Fermions | 24 pages, LaTeX, minor stylistic corrections, to appear in Nucl.
Phys. B | Nucl.Phys. B464 (1996) 189-212 | 10.1016/0550-3213(96)00062-4 | null | hep-th | null | A pseudoclassical model is proposed for the description of planar
$P,T-$invariant massive fermions. The quantization of the model leads to the
(2+1)-dimensional $P,T-$invariant fermion model used recently in
$P,T-$conserving theories of high-T${}_c$ superconductors. The rich symmetry of
the quantum model is elucidate... | [
{
"created": "Fri, 10 Nov 1995 14:44:46 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Feb 1996 00:30:14 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Grignani",
"G.",
""
],
[
"Plyushchay",
"M.",
""
],
[
"Sodano",
"P.",
""
]
] | A pseudoclassical model is proposed for the description of planar $P,T-$invariant massive fermions. The quantization of the model leads to the (2+1)-dimensional $P,T-$invariant fermion model used recently in $P,T-$conserving theories of high-T${}_c$ superconductors. The rich symmetry of the quantum model is elucidated ... | 7.058442 | 6.037256 | 7.307318 | 5.928648 | 6.067677 | 5.715847 | 6.274053 | 5.991505 | 6.00257 | 7.439616 | 6.04104 | 6.558653 | 6.89439 | 6.470631 | 6.371712 | 6.1271 | 6.323209 | 6.300646 | 6.449076 | 6.957346 | 6.454576 |
hep-th/0606082 | Debashis Ghoshal | Debashis Ghoshal | On the relation between p-adic and ordinary strings | 13 pages harvmac (b), 2 eps figures; v2: revtex, shortened, published
version | Phys. Rev. Lett. 97, 151601 (2006) | 10.1103/PhysRevLett.97.151601 | AEI-2006-045, HRI-P-0606001 | hep-th | null | The amplitudes for the tree-level scattering of the open string tachyons,
generalised to the field of p-adic numbers, define the p-adic string theory.
There is empirical evidence of its relation to the ordinary string theory in
the p_to_1 limit. We revisit this limit from a worldsheet perspective and argue
that it is... | [
{
"created": "Fri, 9 Jun 2006 08:43:04 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Oct 2006 08:40:02 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Ghoshal",
"Debashis",
""
]
] | The amplitudes for the tree-level scattering of the open string tachyons, generalised to the field of p-adic numbers, define the p-adic string theory. There is empirical evidence of its relation to the ordinary string theory in the p_to_1 limit. We revisit this limit from a worldsheet perspective and argue that it is n... | 9.977378 | 8.711624 | 11.670837 | 10.472981 | 10.138485 | 10.290147 | 10.041962 | 10.577445 | 9.908463 | 11.512104 | 9.180129 | 9.205123 | 10.31057 | 9.186244 | 9.490284 | 10.053137 | 9.136115 | 9.46169 | 9.518105 | 10.552307 | 9.24313 |
2012.01816 | Diana Lopez Nacir | Diana L. L\'opez Nacir and Juli\'an Rovner | Quantum backreaction of $O(N)$-symmetric scalar fields and de Sitter
spacetimes at the renormalization point: renormalization schemes and the
screening of the cosmological constant | 14 pages, 3 figures; v2 agrees with the published version; in v2 we
introduced new clarifications and we replaced the figures by new ones in
order to fix a mistake in v1 and to provide additional details of the results | Phys. Rev. D 103, 125002 (2021) | 10.1103/PhysRevD.103.125002 | null | hep-th astro-ph.CO gr-qc | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We consider a theory of $N$ self-interacting quantum scalar fields with
quartic $O(N)$-symmetric potential, with a coupling constant $\lambda$, in a
generic curved spacetime. We analyze the renormalization process of the
Semiclassical Einstein Equations at leading order in the $1/N$ expansion for
different renormailz... | [
{
"created": "Thu, 3 Dec 2020 10:43:22 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jun 2021 23:57:51 GMT",
"version": "v2"
}
] | 2021-06-03 | [
[
"Nacir",
"Diana L. López",
""
],
[
"Rovner",
"Julián",
""
]
] | We consider a theory of $N$ self-interacting quantum scalar fields with quartic $O(N)$-symmetric potential, with a coupling constant $\lambda$, in a generic curved spacetime. We analyze the renormalization process of the Semiclassical Einstein Equations at leading order in the $1/N$ expansion for different renormailzat... | 7.378428 | 7.69544 | 7.475039 | 7.422671 | 7.419559 | 7.625205 | 7.880286 | 7.494761 | 7.497256 | 7.960278 | 7.576429 | 7.311414 | 7.331156 | 7.200959 | 7.445447 | 7.274792 | 7.220022 | 7.106309 | 7.271324 | 7.323401 | 7.308083 |
hep-th/9303012 | null | J.J.M. Verbaarschot and I. Zahed | Spectral Density of the QCD Dirac Operator near Zero Virtuality | 9 pages + 1 figure, SUNY-NTG-93/2 | Phys.Rev.Lett. 70 (1993) 3852-3855 | 10.1103/PhysRevLett.70.3852 | null | hep-th | null | We investigate the spectral properties of a random matrix model, which in the
large $N$ limit, embodies the essentials of the QCD partition function at low
energy. The exact spectral density and its pair correlation function are
derived for an arbitrary number of flavors and zero topological charge. Their
microscopic... | [
{
"created": "Tue, 2 Mar 1993 17:56:41 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Verbaarschot",
"J. J. M.",
""
],
[
"Zahed",
"I.",
""
]
] | We investigate the spectral properties of a random matrix model, which in the large $N$ limit, embodies the essentials of the QCD partition function at low energy. The exact spectral density and its pair correlation function are derived for an arbitrary number of flavors and zero topological charge. Their microscopic l... | 9.283254 | 5.341994 | 9.367685 | 6.729427 | 5.645037 | 5.05786 | 5.215484 | 6.326081 | 6.794596 | 9.215448 | 7.100761 | 8.328032 | 8.611579 | 8.380782 | 8.038235 | 8.190875 | 7.734854 | 8.800886 | 8.179661 | 8.64477 | 8.222605 |
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