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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2306.04800 | Nomaan X | Nomaan X | Quantum Field Theory On Causal Sets | Invited chapter for the Causal Sets section of the Handbook of
Quantum Gravity (Eds. C. Bambi, L. Modesto and I. L. Shapiro, Springer,
expected in 2023). arXiv admin note: text overlap with arXiv:1812.10228 | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We give a broad overview of a construction of a theory for matter on fixed
causal set backgrounds. We introduce the Sorkin-Johnston formalism for a free
(real) scalar field theory that is applicable to regions of continuum
spacetimes as well as to causal sets. We show examples in the causal set,
starting from the con... | [
{
"created": "Wed, 7 Jun 2023 21:47:59 GMT",
"version": "v1"
}
] | 2023-06-09 | [
[
"X",
"Nomaan",
""
]
] | We give a broad overview of a construction of a theory for matter on fixed causal set backgrounds. We introduce the Sorkin-Johnston formalism for a free (real) scalar field theory that is applicable to regions of continuum spacetimes as well as to causal sets. We show examples in the causal set, starting from the const... | 16.397011 | 14.569698 | 13.88355 | 14.025887 | 16.349276 | 15.582 | 17.516678 | 14.148706 | 15.661955 | 15.668776 | 16.989037 | 15.733383 | 15.506789 | 15.181567 | 15.899862 | 15.619348 | 16.526196 | 15.730412 | 15.925088 | 16.0739 | 16.018457 |
0909.4272 | Simone Giombi | Simone Giombi, Vasily Pestun | The 1/2 BPS 't Hooft loops in N=4 SYM as instantons in 2d Yang-Mills | 30 pages, no figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the recent conjecture on the relation between a certain 1/8 BPS
subsector of 4d N=4 SYM on S^2 and 2d Yang-Mills theory by turning on circular
1/2 BPS 't Hooft operators linked with S^2. We show that localization predicts
that these 't Hooft operators and their correlation functions with Wilson
operators on... | [
{
"created": "Wed, 23 Sep 2009 19:51:28 GMT",
"version": "v1"
}
] | 2009-09-24 | [
[
"Giombi",
"Simone",
""
],
[
"Pestun",
"Vasily",
""
]
] | We extend the recent conjecture on the relation between a certain 1/8 BPS subsector of 4d N=4 SYM on S^2 and 2d Yang-Mills theory by turning on circular 1/2 BPS 't Hooft operators linked with S^2. We show that localization predicts that these 't Hooft operators and their correlation functions with Wilson operators on S... | 7.048184 | 6.133662 | 7.537996 | 6.166349 | 6.391609 | 5.983373 | 6.473118 | 6.029631 | 6.274414 | 7.724154 | 5.870926 | 6.324481 | 6.966058 | 6.407325 | 6.559456 | 6.473875 | 6.201316 | 6.323283 | 6.147562 | 6.856588 | 6.29214 |
hep-th/9805185 | Arnd Zapletal | H. Babujian, A. Fring, M. Karowski and A. Zapletal | Exact Form Factors in Integrable Quantum Field Theories: the Sine-Gordon
Model | 55 pages, 7 figures, LaTeX | Nucl.Phys. B538 (1999) 535-586 | 10.1016/S0550-3213(98)00737-8 | null | hep-th cond-mat nlin.SI solv-int | null | We provide detailed arguments on how to derive properties of generalized form
factors, originally proposed by one of the authors (M.K.) and Weisz twenty
years ago, solely based on the assumption of "minimal analyticity" and the
validity of the LSZ reduction formalism. These properties constitute
consistency equations... | [
{
"created": "Wed, 27 May 1998 13:24:21 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Nov 1998 17:17:04 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Jan 1999 11:23:41 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Babujian",
"H.",
""
],
[
"Fring",
"A.",
""
],
[
"Karowski",
"M.",
""
],
[
"Zapletal",
"A.",
""
]
] | We provide detailed arguments on how to derive properties of generalized form factors, originally proposed by one of the authors (M.K.) and Weisz twenty years ago, solely based on the assumption of "minimal analyticity" and the validity of the LSZ reduction formalism. These properties constitute consistency equations w... | 13.786067 | 12.583433 | 15.075672 | 12.050248 | 13.705101 | 11.611142 | 12.01615 | 11.544394 | 11.376437 | 14.647466 | 11.708948 | 12.436212 | 13.687819 | 12.025594 | 12.117039 | 12.257849 | 12.211023 | 12.193446 | 12.708715 | 13.798575 | 11.771845 |
2303.04819 | Ivonne Zavala | Michele Cicoli, Joseph P. Conlon, Anshuman Maharana, Susha
Parameswaran, Fernando Quevedo, Ivonne Zavala | String Cosmology: from the Early Universe to Today | Invited Review for Physics Reports, 190 pages. V2: References added,
typos corrected, minor additions | null | null | null | hep-th astro-ph.CO gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We review applications of string theory to cosmology, from primordial times
to the present-day accelerated expansion. Starting with a brief overview of
cosmology and string compactifications, we discuss in detail moduli
stabilisation, inflation in string theory, the impact of string theory on
post-inflationary dynami... | [
{
"created": "Wed, 8 Mar 2023 19:00:01 GMT",
"version": "v1"
},
{
"created": "Fri, 5 May 2023 10:33:53 GMT",
"version": "v2"
}
] | 2023-05-08 | [
[
"Cicoli",
"Michele",
""
],
[
"Conlon",
"Joseph P.",
""
],
[
"Maharana",
"Anshuman",
""
],
[
"Parameswaran",
"Susha",
""
],
[
"Quevedo",
"Fernando",
""
],
[
"Zavala",
"Ivonne",
""
]
] | We review applications of string theory to cosmology, from primordial times to the present-day accelerated expansion. Starting with a brief overview of cosmology and string compactifications, we discuss in detail moduli stabilisation, inflation in string theory, the impact of string theory on post-inflationary dynamics... | 7.66179 | 9.237336 | 7.626988 | 7.350449 | 7.869858 | 7.930285 | 9.184184 | 8.03102 | 7.882502 | 8.67857 | 7.962203 | 7.834761 | 7.67402 | 7.488806 | 7.522119 | 7.842981 | 7.453956 | 7.660619 | 7.410826 | 7.709098 | 7.380301 |
0805.2898 | Pei-Ming Ho | Pei-Ming Ho, Yosuke Imamura, Yutaka Matsuo, Shotaro Shiba | M5-brane in three-form flux and multiple M2-branes | 33 pages | JHEP 0808:014,2008 | 10.1088/1126-6708/2008/08/014 | UT-08-16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the Bagger-Lambert-Gustavsson model associated with the
Nambu-Poisson algebra as a theory describing a single M5-brane. We argue that
the model is a gauge theory associated with the volume-preserving
diffeomorphism in the three-dimenisonal internal space. We derive gauge
transformations, actions, super... | [
{
"created": "Mon, 19 May 2008 16:46:11 GMT",
"version": "v1"
}
] | 2009-12-10 | [
[
"Ho",
"Pei-Ming",
""
],
[
"Imamura",
"Yosuke",
""
],
[
"Matsuo",
"Yutaka",
""
],
[
"Shiba",
"Shotaro",
""
]
] | We investigate the Bagger-Lambert-Gustavsson model associated with the Nambu-Poisson algebra as a theory describing a single M5-brane. We argue that the model is a gauge theory associated with the volume-preserving diffeomorphism in the three-dimenisonal internal space. We derive gauge transformations, actions, supersy... | 6.991153 | 5.847395 | 8.292743 | 6.077329 | 6.482587 | 5.988938 | 6.294263 | 6.166711 | 6.133199 | 8.232323 | 6.083824 | 6.559988 | 6.754187 | 6.416079 | 6.310529 | 6.447265 | 6.429936 | 6.694028 | 6.255654 | 7.085684 | 6.498687 |
1507.00590 | Joseph Ben Geloun | Joseph Ben Geloun | A power counting theorem for a $p^{2a}\phi^4$ tensorial group field
theory | 15 pages, 7 figures | null | null | ICMPA/2015/04 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a tensorial group field theory endowed with weighted interaction
terms of the form $p^{2a} \phi^4$. The model can be seen as a field theory over
$d=3,4$ copies of $U(1)$ where formal powers of Laplacian operators, namely
$\Delta^{a}$, $a>0$, act on tensorial $\phi^4$-interactions producing, after
Fourier... | [
{
"created": "Thu, 2 Jul 2015 14:00:34 GMT",
"version": "v1"
}
] | 2015-07-03 | [
[
"Geloun",
"Joseph Ben",
""
]
] | We introduce a tensorial group field theory endowed with weighted interaction terms of the form $p^{2a} \phi^4$. The model can be seen as a field theory over $d=3,4$ copies of $U(1)$ where formal powers of Laplacian operators, namely $\Delta^{a}$, $a>0$, act on tensorial $\phi^4$-interactions producing, after Fourier t... | 9.63161 | 9.714285 | 10.801291 | 9.090523 | 9.872515 | 10.05056 | 9.296844 | 9.473211 | 9.280808 | 10.770517 | 8.881015 | 8.985059 | 9.690905 | 9.250977 | 9.090031 | 8.973736 | 9.198768 | 9.289197 | 9.079553 | 9.609261 | 9.369366 |
2003.08396 | Domenico Orlando | Domenico Orlando and Susanne Reffert and Francesco Sannino | Charging the Conformal Window | 15 pages | Phys. Rev. D 103, 105026 (2021) | 10.1103/PhysRevD.103.105026 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the properties of near-conformal dynamics in a sector of large
charge when approaching the lower boundary of the conformal window from the
chirally broken phase. To elucidate our approach we use the time-honored
example of the phenomenologically relevant SU(2) color theory featuring $N_f$
Dirac fermion... | [
{
"created": "Wed, 18 Mar 2020 18:00:02 GMT",
"version": "v1"
}
] | 2021-06-14 | [
[
"Orlando",
"Domenico",
""
],
[
"Reffert",
"Susanne",
""
],
[
"Sannino",
"Francesco",
""
]
] | We investigate the properties of near-conformal dynamics in a sector of large charge when approaching the lower boundary of the conformal window from the chirally broken phase. To elucidate our approach we use the time-honored example of the phenomenologically relevant SU(2) color theory featuring $N_f$ Dirac fermions ... | 11.240858 | 10.657612 | 11.716732 | 10.957421 | 12.576719 | 11.377495 | 10.989046 | 10.912095 | 10.304996 | 12.39994 | 11.20348 | 11.395772 | 11.333447 | 10.939502 | 11.686851 | 11.176086 | 11.129182 | 11.462229 | 10.860869 | 11.579788 | 10.906415 |
1302.7032 | Monica Guica | Mirjam Cveti\v{c}, Monica Guica and Zain H. Saleem | General black holes, untwisted | 34 pages | null | 10.1007/JHEP09(2013)017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use solution-generating techniques to construct interpolating geometries
between general asymptotically flat, charged, rotating, non-extremal black
holes in four and five dimensions and their subtracted geometries. In the
four-dimensional case, this is achieved by the use of Harrison transformations,
whereas in th... | [
{
"created": "Wed, 27 Feb 2013 23:42:21 GMT",
"version": "v1"
}
] | 2015-06-15 | [
[
"Cvetič",
"Mirjam",
""
],
[
"Guica",
"Monica",
""
],
[
"Saleem",
"Zain H.",
""
]
] | We use solution-generating techniques to construct interpolating geometries between general asymptotically flat, charged, rotating, non-extremal black holes in four and five dimensions and their subtracted geometries. In the four-dimensional case, this is achieved by the use of Harrison transformations, whereas in the ... | 10.151945 | 7.890205 | 9.204506 | 7.954597 | 8.17658 | 8.216191 | 8.466218 | 7.94222 | 8.058736 | 9.878992 | 7.913024 | 8.426486 | 8.6407 | 8.096143 | 8.498543 | 8.112758 | 8.585094 | 8.16593 | 8.31337 | 8.869233 | 8.47974 |
hep-th/0401125 | Peter Kaste | Matthias R. Gaberdiel and Peter Kaste | Generalised discrete torsion and mirror symmetry for G_2 manifolds | LaTeX, 25 pages, 1 figure; v2: one reference added and comment about
higher loop modular invariance corrected, version to be published | JHEP 0408:001,2004 | 10.1088/1126-6708/2004/08/001 | null | hep-th | null | A generalisation of discrete torsion is introduced in which different
discrete torsion phases are considered for the different fixed points or twist
fields of a twisted sector. The constraints that arise from modular invariance
are analysed carefully. As an application we show how all the different
resolutions of the... | [
{
"created": "Mon, 19 Jan 2004 17:54:23 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Aug 2004 13:30:41 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Kaste",
"Peter",
""
]
] | A generalisation of discrete torsion is introduced in which different discrete torsion phases are considered for the different fixed points or twist fields of a twisted sector. The constraints that arise from modular invariance are analysed carefully. As an application we show how all the different resolutions of the T... | 7.485477 | 7.434373 | 9.854931 | 7.35642 | 8.700974 | 7.629107 | 7.708843 | 7.746416 | 7.438199 | 9.972648 | 7.447433 | 6.932361 | 7.823286 | 7.150635 | 7.451444 | 7.219908 | 7.384918 | 7.28129 | 7.148621 | 7.263205 | 7.104712 |
hep-th/0702176 | Saul Ramos-Sanchez | Felix Ploger, Saul Ramos-Sanchez, Michael Ratz and Patrick K.S.
Vaudrevange | Mirage Torsion | 26 pages, 3 figures, v2: matches version published in JHEP | JHEP 0704:063,2007 | 10.1088/1126-6708/2007/04/063 | TUM-HEP-659/07 | hep-th | null | Z_NxZ_M orbifold models admit the introduction of a discrete torsion phase.
We find that models with discrete torsion have an alternative description in
terms of torsionless models. More specifically, discrete torsion can be 'gauged
away' by changing the shifts by lattice vectors. Similarly, a large class of
the so-c... | [
{
"created": "Wed, 21 Feb 2007 19:09:19 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Apr 2007 14:24:41 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Ploger",
"Felix",
""
],
[
"Ramos-Sanchez",
"Saul",
""
],
[
"Ratz",
"Michael",
""
],
[
"Vaudrevange",
"Patrick K. S.",
""
]
] | Z_NxZ_M orbifold models admit the introduction of a discrete torsion phase. We find that models with discrete torsion have an alternative description in terms of torsionless models. More specifically, discrete torsion can be 'gauged away' by changing the shifts by lattice vectors. Similarly, a large class of the so-cal... | 10.722824 | 8.837799 | 8.72668 | 8.110785 | 8.52834 | 8.725051 | 9.441981 | 8.347943 | 8.076792 | 9.348941 | 8.457515 | 8.213881 | 8.415957 | 7.981486 | 8.052112 | 8.376681 | 8.455825 | 8.690262 | 8.329149 | 8.643983 | 8.657119 |
hep-th/0401157 | Pierre Martinetti | F. Girelli, T. Krajewski, P. Martinetti | An algebraic Birkhoff decomposition for the continuous renormalization
group | null | J.Math.Phys. 45 (2004) 4679-4697 | 10.1063/1.1794366 | null | hep-th math-ph math.MP | null | This paper aims at presenting the first steps towards a formulation of the
Exact Renormalization Group Equation in the Hopf algebra setting of Connes and
Kreimer. It mostly deals with some algebraic preliminaries allowing to
formulate perturbative renormalization within the theory of differential
equations. The relat... | [
{
"created": "Thu, 22 Jan 2004 15:16:18 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Girelli",
"F.",
""
],
[
"Krajewski",
"T.",
""
],
[
"Martinetti",
"P.",
""
]
] | This paper aims at presenting the first steps towards a formulation of the Exact Renormalization Group Equation in the Hopf algebra setting of Connes and Kreimer. It mostly deals with some algebraic preliminaries allowing to formulate perturbative renormalization within the theory of differential equations. The relatio... | 9.910123 | 9.72474 | 10.104652 | 8.655454 | 9.922511 | 8.633096 | 8.618467 | 9.670444 | 8.262089 | 11.163719 | 8.985263 | 8.615365 | 8.64179 | 8.721987 | 8.886287 | 8.691772 | 8.474958 | 9.083023 | 8.603958 | 8.859835 | 8.99328 |
2207.03385 | Stuart Dowker | J.S.Dowker | Remarks on the Aharonov-Bohm Green function | 7 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Some elementary algebraic points regarding the Green function for a localised
flux tube are developed. A calculation of the effective action density is
included.
| [
{
"created": "Thu, 7 Jul 2022 15:51:59 GMT",
"version": "v1"
}
] | 2022-07-08 | [
[
"Dowker",
"J. S.",
""
]
] | Some elementary algebraic points regarding the Green function for a localised flux tube are developed. A calculation of the effective action density is included. | 80.286354 | 45.044167 | 46.885792 | 36.407314 | 29.918324 | 39.567623 | 43.959633 | 36.932793 | 37.690788 | 42.433155 | 39.702625 | 38.320068 | 39.334293 | 38.110245 | 37.508999 | 39.158409 | 37.184795 | 38.008888 | 38.46003 | 41.64769 | 36.676044 |
1712.04861 | Eric Perlmutter | David Meltzer, Eric Perlmutter | Beyond $a=c$: Gravitational Couplings to Matter and the Stress Tensor
OPE | 42+25 pages. v2: added refs, minor changes | null | 10.1007/JHEP07(2018)157 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive constraints on the operator product expansion of two stress tensors
in conformal field theories (CFTs), both generic and holographic. We point out
that in large $N$ CFTs with a large gap to single-trace higher spin operators,
the stress tensor sector is not only universal, but isolated: that is, $\langle
TT... | [
{
"created": "Wed, 13 Dec 2017 16:53:51 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Dec 2017 15:44:06 GMT",
"version": "v2"
}
] | 2018-08-15 | [
[
"Meltzer",
"David",
""
],
[
"Perlmutter",
"Eric",
""
]
] | We derive constraints on the operator product expansion of two stress tensors in conformal field theories (CFTs), both generic and holographic. We point out that in large $N$ CFTs with a large gap to single-trace higher spin operators, the stress tensor sector is not only universal, but isolated: that is, $\langle TT{\... | 6.932271 | 6.807671 | 7.813833 | 6.615339 | 6.754819 | 7.047504 | 7.004291 | 6.920366 | 6.569682 | 8.165171 | 6.369582 | 6.603035 | 7.06954 | 6.64442 | 6.540977 | 6.445071 | 6.497645 | 6.492324 | 6.548645 | 7.037913 | 6.466657 |
1303.0274 | Lavinia Heisenberg | Paul de Fromont, Claudia de Rham, Lavinia Heisenberg and Andrew Matas | Superluminality in the Bi- and Multi- Galileon | 32 pages, minor changes, few references added | null | null | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We re-explore the Bi- and Multi-Galileon models with trivial asymptotic
conditions at infinity and show that propagation of superluminal fluctuations
is a common and unavoidable feature of these theories, unlike previously
claimed in the literature. We show that all Multi-Galileon theories containing
a Cubic Galileon... | [
{
"created": "Fri, 1 Mar 2013 20:43:14 GMT",
"version": "v1"
},
{
"created": "Thu, 2 May 2013 10:36:43 GMT",
"version": "v2"
}
] | 2013-05-03 | [
[
"de Fromont",
"Paul",
""
],
[
"de Rham",
"Claudia",
""
],
[
"Heisenberg",
"Lavinia",
""
],
[
"Matas",
"Andrew",
""
]
] | We re-explore the Bi- and Multi-Galileon models with trivial asymptotic conditions at infinity and show that propagation of superluminal fluctuations is a common and unavoidable feature of these theories, unlike previously claimed in the literature. We show that all Multi-Galileon theories containing a Cubic Galileon t... | 6.78239 | 6.917908 | 7.226183 | 6.624666 | 7.024135 | 6.615087 | 6.520333 | 6.372531 | 6.63586 | 8.169451 | 6.626299 | 6.288854 | 6.733976 | 6.64074 | 6.320837 | 6.088813 | 6.531367 | 6.282442 | 6.723224 | 6.629376 | 6.319982 |
hep-th/9302040 | Solodukhin-63942 | S.N.Solodukhin | Two-dimensional Black Hole With Torsion | 11 pages, Preprint JINR E2-93-33 | Phys.Lett. B319 (1993) 87-95 | 10.1016/0370-2693(93)90786-H | null | hep-th | null | The 2D model of gravity with zweibeins $e^{a}$ and the Lorentz connection
one-form $\omega^{a}_{\ b}$ as independent gravitational variables is
considered and it is shown that the classical equations of motion are exactly
integrated in coordinate system determined by components of 2D torsion. For
some choice of integ... | [
{
"created": "Wed, 10 Feb 1993 18:36:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Solodukhin",
"S. N.",
""
]
] | The 2D model of gravity with zweibeins $e^{a}$ and the Lorentz connection one-form $\omega^{a}_{\ b}$ as independent gravitational variables is considered and it is shown that the classical equations of motion are exactly integrated in coordinate system determined by components of 2D torsion. For some choice of integra... | 13.125916 | 8.741569 | 10.220234 | 8.907775 | 7.910996 | 7.215903 | 8.091309 | 9.017871 | 9.150552 | 9.159576 | 9.283595 | 9.720065 | 10.351136 | 9.988682 | 9.396317 | 9.605451 | 10.209859 | 9.70668 | 10.077775 | 10.218833 | 9.915823 |
2309.07904 | Haiying Cai | Haiying Cai | Diffeomorphism on-shell breaking from radion stabilization | 16 pages, v2 redefine the gauge parameter \epsilon^\prime to be
\epsilon; symmetry is on-shell broken | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present for the first time the nonlinear diffeomorphism in the Randall
Sundrum model that can keep the effective Lagrangian invariant in any order of
expansion. We will show that the off-shell diffeomorphism shapes the
interaction structure. However the radion mass is in fact protected by an
on-shell diffeomorphis... | [
{
"created": "Thu, 14 Sep 2023 17:53:32 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Oct 2023 17:32:18 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Feb 2024 15:53:28 GMT",
"version": "v3"
}
] | 2024-02-06 | [
[
"Cai",
"Haiying",
""
]
] | We present for the first time the nonlinear diffeomorphism in the Randall Sundrum model that can keep the effective Lagrangian invariant in any order of expansion. We will show that the off-shell diffeomorphism shapes the interaction structure. However the radion mass is in fact protected by an on-shell diffeomorphism,... | 14.281903 | 13.246522 | 12.906861 | 11.809708 | 13.312052 | 13.780864 | 12.723826 | 13.221923 | 11.653213 | 12.85932 | 12.448891 | 12.18589 | 12.791675 | 11.920065 | 12.775383 | 13.283142 | 12.918633 | 12.592796 | 12.15337 | 12.961098 | 12.67647 |
1204.3790 | Andrea Velenich | Dirk Kreimer and Andrea Velenich | Field diffeomorphisms and the algebraic structure of perturbative
expansions | 8 pages, 2 figures | Letters in Mathematical Physics: Volume 103, Issue 2 (2013), Page
171-181 | 10.1007/s11005-012-0589-y | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider field diffeomorphisms in the context of real scalar field
theories. Starting from free field theories we apply non-linear field
diffeomorphisms to the fields and study the perturbative expansion for the
transformed theories. We find that tree level amplitudes for the transformed
fields must satisfy BCFW t... | [
{
"created": "Tue, 17 Apr 2012 13:32:58 GMT",
"version": "v1"
}
] | 2015-06-04 | [
[
"Kreimer",
"Dirk",
""
],
[
"Velenich",
"Andrea",
""
]
] | We consider field diffeomorphisms in the context of real scalar field theories. Starting from free field theories we apply non-linear field diffeomorphisms to the fields and study the perturbative expansion for the transformed theories. We find that tree level amplitudes for the transformed fields must satisfy BCFW typ... | 12.093125 | 12.055331 | 13.301434 | 11.052847 | 12.486279 | 11.810071 | 10.972422 | 11.15735 | 11.36446 | 13.381109 | 10.691476 | 11.438988 | 12.180905 | 11.29857 | 11.082197 | 11.245067 | 11.244732 | 11.506852 | 10.816756 | 11.896727 | 10.945792 |
hep-th/0301185 | Antti J. Niemi | M Luebcke, A.J. Niemi and K. Torokoff | Asymptotically Free Yang-Mills Classical Mechanics with Self-Linked
Orbits | 9 pages incl. 5 figs | Phys.Lett. B568 (2003) 176-180 | 10.1016/j.physletb.2003.06.059 | null | hep-th | null | We construct a classical mechanics Hamiltonian which exhibits spontaneous
symmetry breaking akin the Coleman-Weinberg mechanism, dimensional
transmutation, and asymptotically free self-similarity congruent with the
beta-function of four dimensional Yang-Mills theory. Its classical equations of
motion support stable p... | [
{
"created": "Thu, 23 Jan 2003 16:46:15 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Luebcke",
"M",
""
],
[
"Niemi",
"A. J.",
""
],
[
"Torokoff",
"K.",
""
]
] | We construct a classical mechanics Hamiltonian which exhibits spontaneous symmetry breaking akin the Coleman-Weinberg mechanism, dimensional transmutation, and asymptotically free self-similarity congruent with the beta-function of four dimensional Yang-Mills theory. Its classical equations of motion support stable per... | 19.865217 | 16.744062 | 20.049753 | 15.730029 | 18.738977 | 18.247623 | 18.567907 | 16.534239 | 16.389816 | 21.291073 | 15.896072 | 16.91828 | 18.180592 | 16.952417 | 17.439066 | 16.486206 | 16.483578 | 17.223637 | 17.529984 | 18.035183 | 16.91997 |
2101.05990 | Kazumi Okuyama | Kazumi Okuyama | Quenched free energy from spacetime D-branes | 24 pages; v2: reference added. v3: to appear in JHEP | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We propose a useful integral representation of the quenched free energy which
is applicable to any random systems. Our formula involves the generating
function of multi-boundary correlators, which can be interpreted on the bulk
gravity side as spacetime D-branes introduced by Marolf and Maxfield in
[arXiv:2002.08950]... | [
{
"created": "Fri, 15 Jan 2021 07:05:48 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Jan 2021 23:02:15 GMT",
"version": "v2"
},
{
"created": "Sat, 30 Jan 2021 09:30:22 GMT",
"version": "v3"
}
] | 2021-02-02 | [
[
"Okuyama",
"Kazumi",
""
]
] | We propose a useful integral representation of the quenched free energy which is applicable to any random systems. Our formula involves the generating function of multi-boundary correlators, which can be interpreted on the bulk gravity side as spacetime D-branes introduced by Marolf and Maxfield in [arXiv:2002.08950]. ... | 10.543042 | 9.265203 | 10.973372 | 9.54912 | 9.320615 | 10.479593 | 9.348435 | 9.210921 | 8.989377 | 11.742899 | 9.397776 | 8.920312 | 9.775958 | 9.00196 | 9.013463 | 8.596994 | 8.916809 | 8.939187 | 9.060021 | 10.241111 | 9.044855 |
2101.02226 | Alessia Benedetta Platania | Ivano Basile and Alessia Platania | Cosmological $\alpha'$-corrections from the functional renormalization
group | 31 pages, 9 figures. V2: References added and minor modifications.
Matches published version | J. High Energ. Phys. 2021, 45 (2021) | 10.1007/JHEP06(2021)045 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We employ the techniques of the Functional Renormalization Group in string
theory, in order to derive an effective mini-superspace action for cosmological
backgrounds to all orders in the string scale $\alpha'$. To this end, T-duality
plays a crucial role, classifying all perturbative curvature corrections in
terms o... | [
{
"created": "Wed, 6 Jan 2021 19:03:23 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Jun 2021 19:40:14 GMT",
"version": "v2"
}
] | 2021-06-11 | [
[
"Basile",
"Ivano",
""
],
[
"Platania",
"Alessia",
""
]
] | We employ the techniques of the Functional Renormalization Group in string theory, in order to derive an effective mini-superspace action for cosmological backgrounds to all orders in the string scale $\alpha'$. To this end, T-duality plays a crucial role, classifying all perturbative curvature corrections in terms of ... | 8.173027 | 7.962183 | 8.379088 | 7.20439 | 7.704912 | 7.34997 | 7.500321 | 7.371938 | 7.155363 | 8.220563 | 7.288972 | 7.540845 | 7.617759 | 7.615864 | 7.861798 | 7.816228 | 7.558631 | 7.604237 | 7.71927 | 8.035575 | 7.607066 |
2309.14036 | Alexei Nurmagambetov | A.M. Arslanaliev, A.J. Nurmagambetov | Taking the Null-Hypersurface Limit in the Parikh-Wilczek Membrane
Approach | 20 pages, pdflatex | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We consider subtleties of the horizon (null-hypersurface) limit in the
Parikh-Wilczek Membrane Approach to Black Holes. Specifically, we refine the
correspondence between the (projected) Einstein equations of gravity with
matter and the Raychaudhuri-Damour-Navier-Stokes (RDNS) equations of
relativistic hydrodynamics.... | [
{
"created": "Mon, 25 Sep 2023 11:03:41 GMT",
"version": "v1"
}
] | 2023-09-26 | [
[
"Arslanaliev",
"A. M.",
""
],
[
"Nurmagambetov",
"A. J.",
""
]
] | We consider subtleties of the horizon (null-hypersurface) limit in the Parikh-Wilczek Membrane Approach to Black Holes. Specifically, we refine the correspondence between the (projected) Einstein equations of gravity with matter and the Raychaudhuri-Damour-Navier-Stokes (RDNS) equations of relativistic hydrodynamics. F... | 10.681371 | 11.817079 | 11.035311 | 10.668243 | 11.393269 | 11.158714 | 11.304285 | 11.242093 | 10.598805 | 12.382581 | 10.962033 | 10.583827 | 10.510027 | 10.105548 | 10.034193 | 10.401258 | 10.427835 | 10.568169 | 10.184758 | 10.456086 | 10.34227 |
hep-th/9311061 | Masud Chaichian | M. Chaichian and A.P.Demichev | Large Quantum Poincare Subgroup of q-Conformal Group and q-Minkowski
Geometry | 12 pages, Latex, HU-SEFT R 1993-15 | null | null | null | hep-th | null | We construct quantum deformation of Poincar\'e group using as a starting
point $SU(2,2)$ conformal group and twistor-like definition of the Minkowski
space. We obtain quantum deformation of $SU(2,2)$ as a real form of
multiparametric $GL(4,C)_{q_{ij},r}$. It is shown that Poincar\'e subgroup
exists for special nonsta... | [
{
"created": "Wed, 10 Nov 1993 14:34:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Chaichian",
"M.",
""
],
[
"Demichev",
"A. P.",
""
]
] | We construct quantum deformation of Poincar\'e group using as a starting point $SU(2,2)$ conformal group and twistor-like definition of the Minkowski space. We obtain quantum deformation of $SU(2,2)$ as a real form of multiparametric $GL(4,C)_{q_{ij},r}$. It is shown that Poincar\'e subgroup exists for special nonstand... | 10.351967 | 10.680775 | 10.916795 | 9.795682 | 12.272868 | 12.15058 | 11.137785 | 11.15665 | 10.52509 | 12.006694 | 10.151462 | 9.891757 | 9.852375 | 9.953061 | 10.495012 | 10.415895 | 10.062738 | 10.098291 | 10.325587 | 9.987495 | 9.897676 |
hep-th/9501068 | Jose M. Izquierdo | P.K. Townsend | The eleven-dimensional supermembrane revisited | 10 pages, phyzzx.tex, no figures | Phys.Lett.B350:184-187,1995 | 10.1016/0370-2693(95)00397-4 | DAMTP-R/95/2 | hep-th gr-qc | null | It is argued that the type IIA 10-dimensional superstring theory is actually
a compactified 11-dimensional supermembrane theory in which the fundamental
supermembrane is identified with the the solitonic membrane of 11-dimensional
supergravity. The charged extreme black holes of the 10-dimensional type IIA
string the... | [
{
"created": "Tue, 17 Jan 1995 17:15:14 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Townsend",
"P. K.",
""
]
] | It is argued that the type IIA 10-dimensional superstring theory is actually a compactified 11-dimensional supermembrane theory in which the fundamental supermembrane is identified with the the solitonic membrane of 11-dimensional supergravity. The charged extreme black holes of the 10-dimensional type IIA string theor... | 6.15798 | 5.899602 | 6.836132 | 5.692231 | 6.341675 | 5.844043 | 5.896231 | 6.03206 | 5.880186 | 6.939731 | 5.757684 | 5.690518 | 6.32506 | 5.844228 | 5.74827 | 5.775473 | 6.030373 | 5.84831 | 5.987841 | 6.207305 | 5.75544 |
hep-th/0011238 | Martin Schnabl | Martin Schnabl | Constraints on the tachyon condensate from anomalous symmetries | 6 pages | Phys.Lett. B504 (2001) 61-63 | 10.1016/S0370-2693(01)00282-9 | SISSA 109/2000/EP | hep-th | null | Using anomalous symmetries of the cubic string field theory vertex we derive
set of relations between the coefficients of the tachyon condensate. They are
in agreement with the results obtained from level truncation approximation.
| [
{
"created": "Mon, 27 Nov 2000 14:54:02 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Schnabl",
"Martin",
""
]
] | Using anomalous symmetries of the cubic string field theory vertex we derive set of relations between the coefficients of the tachyon condensate. They are in agreement with the results obtained from level truncation approximation. | 13.164164 | 7.927314 | 12.833688 | 8.122731 | 7.243721 | 8.470272 | 8.374858 | 7.921502 | 8.283823 | 13.540158 | 7.506848 | 9.871594 | 12.083387 | 9.297139 | 10.087413 | 10.383661 | 9.514613 | 9.909184 | 9.409959 | 12.399869 | 9.114719 |
hep-th/0512084 | Orfeu Bertolami | O. Bertolami, J.G. Rosa | Gravitational Quantum Well | Latex file, 13 pages plus 2 eps figures and style files; invited talk
presented by O.B. To appear in the Proceedings of the Fourth Meeting on
Constrained Dynamics and Quantum Gravity (QG05), Cala Gonone, Sardegna,
Italy, 12-16 September 2005; typos corrected, references updated | J.Phys.Conf.Ser. 33 (2006) 118-130 | 10.1088/1742-6596/33/1/011 | null | hep-th | null | We discuss the implications of a model of noncommutative Quantum Mechanics
where noncommutativity is extended to the phase space. We analyze how this
model affects the problem of the two-dimensional gravitational quantum well and
use the latest experimental results for the energy states of neutrons in the
Earth's gra... | [
{
"created": "Wed, 7 Dec 2005 15:13:15 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Jan 2006 14:37:00 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Bertolami",
"O.",
""
],
[
"Rosa",
"J. G.",
""
]
] | We discuss the implications of a model of noncommutative Quantum Mechanics where noncommutativity is extended to the phase space. We analyze how this model affects the problem of the two-dimensional gravitational quantum well and use the latest experimental results for the energy states of neutrons in the Earth's gravi... | 10.051789 | 9.136431 | 9.761671 | 8.979315 | 9.793788 | 9.428007 | 9.079764 | 9.160386 | 9.301172 | 9.75126 | 10.024564 | 9.732845 | 9.565893 | 9.621629 | 9.493855 | 9.740016 | 9.699142 | 9.790247 | 9.795126 | 9.697138 | 10.038051 |
1510.04864 | Artymowski Michal | Michal Artymowski, Zygmunt Lalak, Marek Lewicki | Inflation and dark energy from $f(R)$ gravity | 6 pages, 3 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inflationary paradigm has several issues, such as the pre-inflationary
horizon problem or the eternal inflation. To avoid that the standard
Starobinsky inflation has been extended to $R + \alpha R^n$ and $R + \alpha R^n
-\delta R^{2-n}$ models as well as Brans-Dicke generalisation of those $f(R)$
models. The region o... | [
{
"created": "Fri, 16 Oct 2015 12:36:55 GMT",
"version": "v1"
}
] | 2015-10-19 | [
[
"Artymowski",
"Michal",
""
],
[
"Lalak",
"Zygmunt",
""
],
[
"Lewicki",
"Marek",
""
]
] | Inflationary paradigm has several issues, such as the pre-inflationary horizon problem or the eternal inflation. To avoid that the standard Starobinsky inflation has been extended to $R + \alpha R^n$ and $R + \alpha R^n -\delta R^{2-n}$ models as well as Brans-Dicke generalisation of those $f(R)$ models. The region of ... | 10.49092 | 9.657352 | 9.472956 | 9.457759 | 10.720608 | 10.010825 | 10.234601 | 9.199198 | 9.521017 | 10.029211 | 9.103356 | 9.564049 | 9.878957 | 9.752626 | 9.820485 | 9.119373 | 9.337322 | 9.540133 | 9.332211 | 9.938691 | 9.259726 |
hep-th/0004012 | Fedor Gubarev | F.V.Gubarev, V.I.Zakharov | The Berry Phase and Monopoles in Non-Abelian Gauge Theories | 18 pp., Latex2e, 4 figures, psfig.sty | Int.J.Mod.Phys. A17 (2002) 157-174 | 10.1142/S0217751X02005840 | ITEP-TH-14/00 | hep-th hep-lat | null | We consider the quantum mechanical notion of the geometrical (Berry) phase in
SU(2) gauge theory, both in the continuum and on the lattice. It is shown that
in the coherent state basis eigenvalues of the Wilson loop operator naturally
decompose into the geometrical and dynamical phase factors. Moreover, for each
Wils... | [
{
"created": "Mon, 3 Apr 2000 18:22:35 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Gubarev",
"F. V.",
""
],
[
"Zakharov",
"V. I.",
""
]
] | We consider the quantum mechanical notion of the geometrical (Berry) phase in SU(2) gauge theory, both in the continuum and on the lattice. It is shown that in the coherent state basis eigenvalues of the Wilson loop operator naturally decompose into the geometrical and dynamical phase factors. Moreover, for each Wilson... | 9.205374 | 9.333434 | 8.828328 | 8.938134 | 8.496499 | 8.79556 | 9.368979 | 8.759048 | 8.695008 | 9.936201 | 8.388655 | 8.83739 | 8.967672 | 8.747828 | 8.980748 | 9.002919 | 8.841879 | 8.911451 | 8.950367 | 9.393562 | 8.805839 |
2405.07779 | Gustavo De Brito | Gustavo P. de Brito, Antonio D. Pereira | Infrared gluon propagator in the Refined Gribov-Zwanziger scenario at
one-loop order in the Landau gauge | 12 pages (including refs.); 6 figures | null | null | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Refined Gribov-Zwanziger (RGZ) action in the Landau gauge provides a
local and renormalizable framework to account for the existence of
infinitesimal Gribov copies in the path integral together with other relevant
infrared effects such as the formation of condensates. The properties of the
tree-level gluon propag... | [
{
"created": "Mon, 13 May 2024 14:24:21 GMT",
"version": "v1"
}
] | 2024-05-14 | [
[
"de Brito",
"Gustavo P.",
""
],
[
"Pereira",
"Antonio D.",
""
]
] | The Refined Gribov-Zwanziger (RGZ) action in the Landau gauge provides a local and renormalizable framework to account for the existence of infinitesimal Gribov copies in the path integral together with other relevant infrared effects such as the formation of condensates. The properties of the tree-level gluon propagat... | 7.158497 | 6.20119 | 6.567928 | 5.982162 | 6.865722 | 6.393135 | 6.693738 | 6.561003 | 6.465113 | 7.315549 | 6.416641 | 6.370522 | 6.849495 | 6.450652 | 6.403611 | 6.570943 | 6.686748 | 6.544331 | 6.365134 | 6.447521 | 6.541293 |
hep-th/0010066 | Hiroshi Itoyama | B. Chen, H. Itoyama, T. Matsuo and K. Murakami | Correspondence between Noncommutative Soliton and Open String/D-brane
System via Gaussian Damping Factor | 17 pages, Latex | Prog.Theor.Phys. 105 (2001) 853-868 | 10.1143/PTP.105.853 | OU-HET-361 | hep-th | null | The gaussian damping factor (g.d.f.) and the new interaction vertex with the
symplectic tensor are the characteristic properties of the N-point
scalar-vector scattering amplitudes of the p-p' (p < p') open string system
which realizes noncommutative geometry. The g.d.f. is here interpreted as a
form factor of the Dp-... | [
{
"created": "Tue, 10 Oct 2000 12:03:04 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Chen",
"B.",
""
],
[
"Itoyama",
"H.",
""
],
[
"Matsuo",
"T.",
""
],
[
"Murakami",
"K.",
""
]
] | The gaussian damping factor (g.d.f.) and the new interaction vertex with the symplectic tensor are the characteristic properties of the N-point scalar-vector scattering amplitudes of the p-p' (p < p') open string system which realizes noncommutative geometry. The g.d.f. is here interpreted as a form factor of the Dp-br... | 13.681079 | 12.671508 | 15.790074 | 12.717712 | 13.475838 | 13.876342 | 13.906711 | 12.894617 | 13.816494 | 14.960642 | 12.900661 | 12.609498 | 13.667021 | 12.970078 | 12.795512 | 12.387984 | 12.720724 | 12.519023 | 13.013104 | 14.155022 | 12.369246 |
2407.19003 | Xinyu Sun | Xinyu Sun and Shao-Kai Jian | Holographic dual of defect CFT with corner contributions | 4.2 pages + supplemental material, 3 figures | null | null | null | hep-th cond-mat.stat-mech | http://creativecommons.org/licenses/by/4.0/ | We study defect CFT within the framework of holographic duality, emphasizing
the impact of corner contributions. We model distinct conformal defects using
interface branes that differ in tensions and are connected by a corner.
Employing the relationship between CFT scaling dimensions and Euclidean gravity
actions, we... | [
{
"created": "Fri, 26 Jul 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-07-30 | [
[
"Sun",
"Xinyu",
""
],
[
"Jian",
"Shao-Kai",
""
]
] | We study defect CFT within the framework of holographic duality, emphasizing the impact of corner contributions. We model distinct conformal defects using interface branes that differ in tensions and are connected by a corner. Employing the relationship between CFT scaling dimensions and Euclidean gravity actions, we o... | 22.977901 | 19.33251 | 22.61252 | 20.299313 | 20.220423 | 22.471504 | 22.476643 | 20.095184 | 21.165161 | 21.971493 | 20.490286 | 19.865644 | 22.01589 | 20.069836 | 19.884098 | 20.327204 | 20.512535 | 20.4862 | 20.272121 | 21.216593 | 20.876858 |
1306.4347 | Juan Jottar | Jan de Boer and Juan I. Jottar | Entanglement Entropy and Higher Spin Holography in AdS$_3$ | 36 pages + appendices, 6 figures | JHEP 1404:089,2014 | 10.1007/JHEP04(2014)089 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A holographic correspondence has been recently developed between higher spin
theories in three-dimensional anti-de Sitter space (AdS_3) and two-dimensional
Conformal Field Theories (CFTs) with extended symmetries. A class of such
dualities involves SL(N,R)\times SL(N,R) Chern-Simons gauge theories in the
(2+1)-dimens... | [
{
"created": "Tue, 18 Jun 2013 20:47:45 GMT",
"version": "v1"
}
] | 2018-10-09 | [
[
"de Boer",
"Jan",
""
],
[
"Jottar",
"Juan I.",
""
]
] | A holographic correspondence has been recently developed between higher spin theories in three-dimensional anti-de Sitter space (AdS_3) and two-dimensional Conformal Field Theories (CFTs) with extended symmetries. A class of such dualities involves SL(N,R)\times SL(N,R) Chern-Simons gauge theories in the (2+1)-dimensio... | 4.629246 | 4.638263 | 5.550528 | 4.662368 | 4.865296 | 4.938271 | 5.023803 | 4.625513 | 4.543481 | 6.155118 | 4.521553 | 4.493726 | 4.913732 | 4.612747 | 4.690004 | 4.597847 | 4.571548 | 4.65441 | 4.728699 | 4.902293 | 4.595183 |
hep-th/0008106 | Miguel S. Costa | Miguel S. Costa (Princeton University) and Malcolm J. Perry (Cambridge
University) | Interacting Black Holes | 22 pages, 4 figures, Latex | Nucl.Phys. B591 (2000) 469-487 | 10.1016/S0550-3213(00)00577-0 | PUPT-1947, DAMTP-2000-76 | hep-th gr-qc | null | We revisit the geometry representing l collinear Schwarzschild black holes.
It is seen that the black holes' horizons are deformed by their mutual
gravitational attraction. The geometry has a string like conical singularity
that connects the holes but has nevertheless a well defined action. Using
standard gravitation... | [
{
"created": "Sat, 12 Aug 2000 21:17:48 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Costa",
"Miguel S.",
"",
"Princeton University"
],
[
"Perry",
"Malcolm J.",
"",
"Cambridge\n University"
]
] | We revisit the geometry representing l collinear Schwarzschild black holes. It is seen that the black holes' horizons are deformed by their mutual gravitational attraction. The geometry has a string like conical singularity that connects the holes but has nevertheless a well defined action. Using standard gravitational... | 15.754734 | 14.277812 | 14.464207 | 13.593711 | 13.715669 | 13.665787 | 13.745592 | 14.013105 | 14.564885 | 15.000423 | 13.89776 | 14.517001 | 15.099381 | 14.814899 | 14.59188 | 14.249476 | 14.315763 | 14.382614 | 14.639997 | 14.904572 | 14.5301 |
hep-th/9609216 | Michael Engelhardt | Michael Engelhardt and Shimon Levit (Weizmann Institute) | Variational Master Field for Large-N Interacting Matrix Models - Free
Random Variables on Trial | 24 pages, 16 figures | Nucl.Phys. B488 (1997) 735-774 | 10.1016/S0550-3213(97)00043-6 | null | hep-th cond-mat nucl-th | null | Matrices are said to behave as free non-commuting random variables if the
action which governs their dynamics constrains only their eigenvalues, i.e.
depends on traces of powers of individual matrices. The authors use recently
developed mathematical techniques in combination with a standard variational
principle to f... | [
{
"created": "Fri, 27 Sep 1996 16:36:05 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Engelhardt",
"Michael",
"",
"Weizmann Institute"
],
[
"Levit",
"Shimon",
"",
"Weizmann Institute"
]
] | Matrices are said to behave as free non-commuting random variables if the action which governs their dynamics constrains only their eigenvalues, i.e. depends on traces of powers of individual matrices. The authors use recently developed mathematical techniques in combination with a standard variational principle to for... | 17.250896 | 16.584604 | 15.193129 | 15.285354 | 16.52668 | 16.203648 | 16.765556 | 14.568156 | 14.730071 | 19.995314 | 15.838063 | 14.340652 | 13.861634 | 14.154934 | 14.158414 | 13.848586 | 13.916 | 14.164528 | 13.973258 | 15.192621 | 14.480235 |
2406.02698 | Paul Ryan | Simon Ekhammar, Nikolay Gromov, Paul Ryan | New Approach to Strongly Coupled N = 4 SYM via Integrability | V2. Fixed typos | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Finding a systematic expansion of the spectrum of free superstrings on
AdS${}_5\times $S${}^5$, or equivalently strongly coupled N = 4 SYM in the
planar limit, remains an outstanding challenge. No first principle string
theory methods are readily available, instead the sole tool at our disposal is
the integrability-b... | [
{
"created": "Tue, 4 Jun 2024 18:23:54 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Jun 2024 17:31:54 GMT",
"version": "v2"
}
] | 2024-06-07 | [
[
"Ekhammar",
"Simon",
""
],
[
"Gromov",
"Nikolay",
""
],
[
"Ryan",
"Paul",
""
]
] | Finding a systematic expansion of the spectrum of free superstrings on AdS${}_5\times $S${}^5$, or equivalently strongly coupled N = 4 SYM in the planar limit, remains an outstanding challenge. No first principle string theory methods are readily available, instead the sole tool at our disposal is the integrability-bas... | 8.670957 | 8.824799 | 9.863476 | 8.508019 | 9.304157 | 8.719467 | 9.504429 | 8.768073 | 8.578543 | 9.854334 | 8.545075 | 8.693555 | 8.696891 | 8.566513 | 8.616822 | 8.649482 | 8.595825 | 8.534739 | 8.68903 | 8.978309 | 8.892518 |
0804.4335 | Jorgen Rasmussen | Jorgen Rasmussen, Paul A. Pearce | W-Extended Fusion Algebra of Critical Percolation | 30 pages | J.Phys.A41:295208,2008 | 10.1088/1751-8113/41/29/295208 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Two-dimensional critical percolation is the member LM(2,3) of the infinite
series of Yang-Baxter integrable logarithmic minimal models LM(p,p'). We
consider the continuum scaling limit of this lattice model as a `rational'
logarithmic conformal field theory with extended W=W_{2,3} symmetry and use a
lattice approach ... | [
{
"created": "Mon, 28 Apr 2008 07:24:49 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Rasmussen",
"Jorgen",
""
],
[
"Pearce",
"Paul A.",
""
]
] | Two-dimensional critical percolation is the member LM(2,3) of the infinite series of Yang-Baxter integrable logarithmic minimal models LM(p,p'). We consider the continuum scaling limit of this lattice model as a `rational' logarithmic conformal field theory with extended W=W_{2,3} symmetry and use a lattice approach on... | 12.418324 | 12.147614 | 14.638444 | 12.133763 | 12.947316 | 11.941364 | 12.521498 | 11.232337 | 11.718841 | 15.521858 | 11.975015 | 12.070612 | 13.672359 | 11.839202 | 12.475783 | 12.165537 | 12.228374 | 11.684865 | 12.056412 | 12.945664 | 12.02707 |
hep-th/0206174 | B. Stefanski jr. | B. Stefanski, jr | D-branes, Orientifolds and K-theory | 6 pages, to appear in the proceedings of the RTN meeting ``The
Quantum Structure of Spacetime and the Geometric Nature of Fundamental
Interactions'', (Corfu, September 2001) | null | 10.1002/1521-3978(200209)50:8/9<986::AID-PROP986>3.0.CO;2-# | null | hep-th | null | The complete D-brane spectrum in $\Zop_2$ orientifolds is computed. Stable
non-BPS D-branes with both integral and torsion charges are found. The relation
to K-theory is discussed and a new K-theory relevant to orientifolds is
suggested.
| [
{
"created": "Wed, 19 Jun 2002 08:22:34 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Stefanski",
"B.",
""
],
[
"jr",
"",
""
]
] | The complete D-brane spectrum in $\Zop_2$ orientifolds is computed. Stable non-BPS D-branes with both integral and torsion charges are found. The relation to K-theory is discussed and a new K-theory relevant to orientifolds is suggested. | 13.696068 | 9.620062 | 14.436669 | 8.436141 | 8.43665 | 9.411608 | 9.143805 | 8.899093 | 8.172498 | 14.15189 | 8.347305 | 9.213018 | 11.781619 | 9.831791 | 9.915655 | 9.779431 | 9.959543 | 9.940459 | 10.064692 | 12.527974 | 9.46986 |
2106.14580 | Nam Nguyen | Nam Nguyen | An effective theory for higher-dimensional black holes and applications
to metastable antibranes | Ph.D. Thesis, Supervisor: Vasileios Niarchos, Durham Univesity, 2021,
University link: http://etheses.dur.ac.uk/14040/; 143 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Despite their consequential applications, metastable states of antibranes in
warped throats are not yet fully understood. In this thesis, we provide new
information on various aspects of these metastable antibranes through
applications of the blackfold effective theory for higher-dimensional black
holes. As concrete ... | [
{
"created": "Mon, 28 Jun 2021 11:23:10 GMT",
"version": "v1"
}
] | 2021-06-29 | [
[
"Nguyen",
"Nam",
""
]
] | Despite their consequential applications, metastable states of antibranes in warped throats are not yet fully understood. In this thesis, we provide new information on various aspects of these metastable antibranes through applications of the blackfold effective theory for higher-dimensional black holes. As concrete ex... | 7.546451 | 7.679189 | 8.292553 | 7.2394 | 7.537678 | 7.775504 | 7.399928 | 7.504734 | 7.412185 | 8.693039 | 7.302813 | 7.744427 | 7.743299 | 7.633968 | 7.667784 | 7.441117 | 7.646948 | 7.482428 | 7.556049 | 7.717645 | 7.558029 |
hep-th/0103052 | Ichiro Oda | Ichiro Oda | A New Mechanism for Trapping of Photon | 7 pages, LaTex 2e, no figures | null | null | EDO-EP-38 | hep-th | null | We propose a new mechanism for trapping bulk gauge field, giving rise to a
massless photon on a flat Minkowski 3-brane in the Randall-Sundrum model in
five space-time dimensions. The mechanism we propose employs the topological
Higgs mechansim where a topological term and a 3-form gauge potential play an
important ro... | [
{
"created": "Wed, 7 Mar 2001 20:38:21 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Oda",
"Ichiro",
""
]
] | We propose a new mechanism for trapping bulk gauge field, giving rise to a massless photon on a flat Minkowski 3-brane in the Randall-Sundrum model in five space-time dimensions. The mechanism we propose employs the topological Higgs mechansim where a topological term and a 3-form gauge potential play an important role... | 12.492582 | 11.103662 | 12.141753 | 9.955207 | 11.321904 | 10.924455 | 10.90679 | 10.508857 | 10.364547 | 11.203331 | 10.945325 | 11.636963 | 10.848803 | 11.284811 | 10.942094 | 11.003516 | 11.397244 | 11.132351 | 11.001729 | 11.187622 | 11.407531 |
1707.03431 | Fidel I. Schaposnik Massolo | Tatsuo Azeyanagi (1), Frank Ferrari (1,2) and Fidel I. Schaposnik
Massolo (2) ((1) U. L. Brussels (2) IBS-CTPU Seoul) | Phase Diagram of Planar Matrix Quantum Mechanics, Tensor, and
Sachdev-Ye-Kitaev Models | 14 pages, 5 figures, minor changes in v2 | Phys. Rev. Lett. 120, 061602 (2018) | 10.1103/PhysRevLett.120.061602 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the phase diagram of a $\text{U}(N)^{2}\times\text{O}(D)$
invariant fermionic planar matrix quantum mechanics [equivalently tensor or
complex Sachdev-Ye-Kitaev (SYK) models] in the new large $D$ limit, dominated
by melonic graphs. The Schwinger-Dyson equations can have two solutions
describing either a hig... | [
{
"created": "Tue, 11 Jul 2017 18:52:08 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Feb 2018 06:27:27 GMT",
"version": "v2"
}
] | 2018-02-14 | [
[
"Azeyanagi",
"Tatsuo",
"",
"U. L. Brussels"
],
[
"Ferrari",
"Frank",
"",
"U. L. Brussels",
"IBS-CTPU Seoul"
],
[
"Massolo",
"Fidel I. Schaposnik",
"",
"IBS-CTPU Seoul"
]
] | We compute the phase diagram of a $\text{U}(N)^{2}\times\text{O}(D)$ invariant fermionic planar matrix quantum mechanics [equivalently tensor or complex Sachdev-Ye-Kitaev (SYK) models] in the new large $D$ limit, dominated by melonic graphs. The Schwinger-Dyson equations can have two solutions describing either a high ... | 9.910657 | 10.358525 | 10.644194 | 9.272652 | 10.17358 | 9.787063 | 9.652504 | 9.464671 | 9.70072 | 10.720378 | 9.028584 | 9.49299 | 9.638741 | 9.243791 | 9.494729 | 9.371135 | 9.47519 | 9.619273 | 9.386398 | 9.687112 | 9.381666 |
1404.5052 | Peter Minkowski | Peter Minkowski | Mass Generation in QCD -- Oscillating Quarks and Gluons | 58 pages, 11 figures, Conference: Workshop on Flavour, N T U,
Singapore, 10.-14. February 2014 | null | 10.1142/S0217751X14440151 | null | hep-th math.SP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The present lecture is devoted to embedding the approximate genuine harmonic
oscillator structure of valence q qbar mesons and in more detail the q q q
configurations for up,down,strange - flavored baryons in Q C D for three light
flavors of quark.
| [
{
"created": "Sun, 20 Apr 2014 16:47:26 GMT",
"version": "v1"
}
] | 2015-06-19 | [
[
"Minkowski",
"Peter",
""
]
] | The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence q qbar mesons and in more detail the q q q configurations for up,down,strange - flavored baryons in Q C D for three light flavors of quark. | 65.255257 | 100.741646 | 57.404968 | 49.690689 | 61.276886 | 75.521439 | 59.410828 | 86.654121 | 45.875637 | 61.401394 | 64.999512 | 60.305908 | 58.394466 | 47.434856 | 55.073826 | 62.325428 | 51.041153 | 60.214561 | 48.638962 | 54.673103 | 59.117718 |
hep-th/9607216 | Ingo Gaida | Ingo Gaida (Humboldt University Berlin) | The Hypermultiplet in N = 2 Superspace | 12 pages, no figures, standard latex | null | null | HUB-EP-96-35 | hep-th | null | Global N=2 supersymmetry in four dimensions with a Fayet-Sohnius
hypermultiplet and a complex central charge is studied in N = 2 superspace. It
is shown how to construct the complete expansion of the hypermultiplet with
respect to the central charge. In addition the low-energy effective action is
discussed and it is ... | [
{
"created": "Mon, 29 Jul 1996 08:54:59 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gaida",
"Ingo",
"",
"Humboldt University Berlin"
]
] | Global N=2 supersymmetry in four dimensions with a Fayet-Sohnius hypermultiplet and a complex central charge is studied in N = 2 superspace. It is shown how to construct the complete expansion of the hypermultiplet with respect to the central charge. In addition the low-energy effective action is discussed and it is sh... | 13.012508 | 10.925059 | 14.066613 | 10.212084 | 10.307037 | 10.846945 | 10.524292 | 10.717068 | 10.538175 | 13.179561 | 9.53246 | 10.582125 | 11.552373 | 10.494067 | 10.595153 | 10.148156 | 10.818476 | 10.126186 | 10.690737 | 11.472293 | 10.266237 |
hep-th/0002150 | Alok Kumar | Alok Kumar | Non-Planar String Networks on Tori | 11 pages, latex, one figure, very minor English corrections | JHEP 0003 (2000) 010 | 10.1088/1126-6708/2000/03/010 | CERN-TH/2000-059 | hep-th | null | Type II strings in D=5 contain particle-like 1/8 supersymmetric BPS states.
In this note we give a string-network representation of such states by
considering (periodic) non-planar $(p,q,r)$-string networks of eight
dimensional type II string theory on $T^3$. We obtain the BPS mass formula of
such states, in terms of... | [
{
"created": "Fri, 18 Feb 2000 10:53:15 GMT",
"version": "v1"
},
{
"created": "Sun, 20 Feb 2000 08:37:26 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Feb 2000 15:57:40 GMT",
"version": "v3"
},
{
"created": "Wed, 1 Mar 2000 09:57:50 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Kumar",
"Alok",
""
]
] | Type II strings in D=5 contain particle-like 1/8 supersymmetric BPS states. In this note we give a string-network representation of such states by considering (periodic) non-planar $(p,q,r)$-string networks of eight dimensional type II string theory on $T^3$. We obtain the BPS mass formula of such states, in terms of c... | 11.142149 | 11.138425 | 12.773416 | 10.819753 | 10.571233 | 10.526099 | 10.655249 | 10.190843 | 10.581165 | 12.291214 | 10.825001 | 10.599339 | 11.10976 | 10.173104 | 10.475139 | 10.515484 | 10.550076 | 10.445733 | 10.238505 | 10.943772 | 10.553932 |
1910.13929 | Daniel Logares | Carlos Hoyos, Niko Jokela and Daniel Logares | Scattering length from holographic duality | 17 pages, 4 figures | Phys. Rev. D 101, 046028 (2020) | 10.1103/PhysRevD.101.046028 | HIP-2019-35/TH | hep-th cond-mat.stat-mech cond-mat.str-el hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Interesting theories with short range interactions include QCD in the
hadronic phase and cold atom systems. The scattering length in two-to-two
elastic scattering process captures the most elementary features of the
interactions, such as whether they are attractive or repulsive. However, even
this basic quantity is n... | [
{
"created": "Wed, 30 Oct 2019 15:29:55 GMT",
"version": "v1"
}
] | 2020-03-04 | [
[
"Hoyos",
"Carlos",
""
],
[
"Jokela",
"Niko",
""
],
[
"Logares",
"Daniel",
""
]
] | Interesting theories with short range interactions include QCD in the hadronic phase and cold atom systems. The scattering length in two-to-two elastic scattering process captures the most elementary features of the interactions, such as whether they are attractive or repulsive. However, even this basic quantity is not... | 9.182508 | 9.38066 | 9.737144 | 8.621318 | 9.348819 | 9.872048 | 8.64415 | 8.640697 | 8.363294 | 9.665051 | 8.875273 | 8.660158 | 9.015116 | 8.47063 | 8.532552 | 8.815139 | 8.33067 | 8.527272 | 8.389718 | 8.706872 | 8.686322 |
2407.17350 | Jiahao Zheng | Jiaqun Jiang, Satoshi Nawata, Jiahao Zheng | 2d dualities from 4d | 21 pages, 8 Figures, 1 Table | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find new $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,2)$ dualities through the
twisted compactifications of 4d supersymmetric theories on $S^2$. Our findings
include dualities for both $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,2)$
non-Abelian gauge theories, as well as $\mathcal{N}=(0,2)$
Gauge/Landau-Ginzburg duality.
| [
{
"created": "Wed, 24 Jul 2024 15:19:29 GMT",
"version": "v1"
}
] | 2024-07-25 | [
[
"Jiang",
"Jiaqun",
""
],
[
"Nawata",
"Satoshi",
""
],
[
"Zheng",
"Jiahao",
""
]
] | We find new $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,2)$ dualities through the twisted compactifications of 4d supersymmetric theories on $S^2$. Our findings include dualities for both $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,2)$ non-Abelian gauge theories, as well as $\mathcal{N}=(0,2)$ Gauge/Landau-Ginzburg duality. | 3.670462 | 3.239791 | 3.732708 | 3.149094 | 3.19483 | 3.369559 | 3.262716 | 3.080161 | 3.137828 | 3.760123 | 3.148016 | 3.278026 | 3.761714 | 3.30431 | 3.339849 | 3.407023 | 3.263864 | 3.313701 | 3.369417 | 3.667189 | 3.280427 |
hep-th/0608001 | Barak Kol | Barak Kol | The Power of Action: "The" Derivation of the Black Hole Negative Mode | 16 pages, 1 figure. v2: Published version including an expanded
introduction and minor changes. The title of the published version was
changed due to an editorial request to "Gauge-eliminated derivation of the
black hole negative mode" | Phys.Rev.D77:044039,2008 | 10.1103/PhysRevD.77.044039 | null | hep-th gr-qc | null | The negative mode of the Schwarzschild black hole is central to Euclidean
quantum gravity around hot flat space and for the Gregory-Laflamme black string
instability. Numerous gauges were employed in the past to analyze it. Here
_the_ analytic derivation is found, based on postponing the gauge fixing, on
the power of... | [
{
"created": "Tue, 1 Aug 2006 11:49:09 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Mar 2008 06:46:34 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Kol",
"Barak",
""
]
] | The negative mode of the Schwarzschild black hole is central to Euclidean quantum gravity around hot flat space and for the Gregory-Laflamme black string instability. Numerous gauges were employed in the past to analyze it. Here _the_ analytic derivation is found, based on postponing the gauge fixing, on the power of t... | 23.373468 | 20.003902 | 22.945175 | 18.669619 | 18.703972 | 18.852514 | 18.314816 | 17.659307 | 19.477831 | 23.923145 | 19.089153 | 20.907743 | 20.585171 | 20.870625 | 22.0123 | 20.715305 | 20.770626 | 19.96287 | 20.863979 | 21.939068 | 21.225033 |
0908.1016 | Frederic P. Schuller | Frederic P. Schuller, Christof Witte, Mattias N.R. Wohlfarth | Causal structure and algebraic classification of area metric spacetimes
in four dimensions | 47 pages, 2 figures | Annals Phys.325:1853-1883,2010 | 10.1016/j.aop.2010.04.008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Area metric manifolds emerge as a refinement of symplectic and metric
geometry in four dimensions, where in numerous situations of physical interest
they feature as effective matter backgrounds. In this article, this prompts us
to identify those area metric manifolds that qualify as viable spacetime
backgrounds in th... | [
{
"created": "Fri, 7 Aug 2009 10:19:35 GMT",
"version": "v1"
}
] | 2011-03-28 | [
[
"Schuller",
"Frederic P.",
""
],
[
"Witte",
"Christof",
""
],
[
"Wohlfarth",
"Mattias N. R.",
""
]
] | Area metric manifolds emerge as a refinement of symplectic and metric geometry in four dimensions, where in numerous situations of physical interest they feature as effective matter backgrounds. In this article, this prompts us to identify those area metric manifolds that qualify as viable spacetime backgrounds in the ... | 15.803844 | 16.673119 | 15.83841 | 13.982566 | 16.291059 | 17.000719 | 17.146933 | 15.782122 | 15.378241 | 15.688257 | 15.203025 | 14.739307 | 14.606778 | 14.379097 | 14.605883 | 14.960292 | 15.052421 | 14.312098 | 14.959134 | 14.99113 | 14.784385 |
hep-th/9511181 | Jayme Vaz Jr. | J. Vaz, Jr. and W. A. Rodrigues, Jr. | Maxwell and Dirac theories as an already unified theory | REVTeX, 15 pages, talk given at the International Conference on the
Theory of the Electron, Sept.95, Mexico City. To appear in the proceedings | null | null | RP IMECC-UNICAMP 45/95 | hep-th | null | In this paper we formulate Maxwell and Dirac theories as an already unified
theory (in the sense of Misner and Wheeler). We introduce Dirac spinors as
"Dirac square root" of the Faraday bivector, and use this in order to find a
spinorial representation of Maxwell equations. Then we show that under certain
circunstanc... | [
{
"created": "Sat, 25 Nov 1995 19:49:23 GMT",
"version": "v1"
}
] | 2012-08-27 | [
[
"Vaz,",
"J.",
"Jr."
],
[
"Rodrigues,",
"W. A.",
"Jr."
]
] | In this paper we formulate Maxwell and Dirac theories as an already unified theory (in the sense of Misner and Wheeler). We introduce Dirac spinors as "Dirac square root" of the Faraday bivector, and use this in order to find a spinorial representation of Maxwell equations. Then we show that under certain circunstances... | 10.554043 | 11.399056 | 10.805508 | 10.342287 | 10.741995 | 10.484982 | 11.394529 | 11.015681 | 10.444538 | 10.905759 | 10.676936 | 10.377108 | 9.941962 | 9.913513 | 10.513947 | 10.25989 | 10.656253 | 9.96342 | 10.196513 | 10.002964 | 9.949395 |
1510.06461 | Rudnei O. Ramos | J. F. de Medeiros Neto, Rudnei O. Ramos, Carlos Rafael M. Santos,
Rodrigo F. Ozela, Gabriel C. Magalh\~aes and Van S\'ergio Alves | Suppressing vacuum fluctuations with vortex excitations | 20 pages, 1 eps figure | Phys. Rev. D 92, 105021 (2015) | 10.1103/PhysRevD.92.105021 | null | hep-th cond-mat.other hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Casimir force for a planar gauge model is studied considering perfect
conducting and perfect magnetically permeable boundaries. By using an effective
model describing planar vortex excitations, we determine the effect these can
have on the Casimir force between parallel lines. Two different mappings
between model... | [
{
"created": "Thu, 22 Oct 2015 00:19:44 GMT",
"version": "v1"
}
] | 2015-11-11 | [
[
"Neto",
"J. F. de Medeiros",
""
],
[
"Ramos",
"Rudnei O.",
""
],
[
"Santos",
"Carlos Rafael M.",
""
],
[
"Ozela",
"Rodrigo F.",
""
],
[
"Magalhães",
"Gabriel C.",
""
],
[
"Alves",
"Van Sérgio",
""
]
] | The Casimir force for a planar gauge model is studied considering perfect conducting and perfect magnetically permeable boundaries. By using an effective model describing planar vortex excitations, we determine the effect these can have on the Casimir force between parallel lines. Two different mappings between models ... | 13.176911 | 12.811635 | 13.979212 | 12.547067 | 12.594542 | 12.498541 | 13.470888 | 12.002284 | 11.643132 | 13.727034 | 12.361637 | 12.08093 | 12.669293 | 12.547928 | 12.352569 | 12.493681 | 12.752851 | 12.502499 | 12.336364 | 12.675532 | 12.631686 |
1012.4462 | Kurt Hinterbichler | Kurt Hinterbichler, Justin Khoury and Horatiu Nastase | Towards a UV Completion for Chameleon Scalar Theories | 28 pages, 2 figures. v3 parameter values corrected | JHEP 1103:061,2011; Erratum-ibid.1106:072,2011 | 10.1007/JHEP03(2011)061 10.1007/JHEP06(2011)072 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Chameleons are scalar fields that couple directly to ordinary matter with
gravitational strength, but which nevertheless evade the stringent constraints
on tests of gravity because of properties they acquire in the presence of high
ambient matter density. Chameleon theories were originally constructed in a
bottom-up,... | [
{
"created": "Mon, 20 Dec 2010 21:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Mar 2011 21:12:16 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Jun 2011 02:58:06 GMT",
"version": "v3"
}
] | 2011-07-13 | [
[
"Hinterbichler",
"Kurt",
""
],
[
"Khoury",
"Justin",
""
],
[
"Nastase",
"Horatiu",
""
]
] | Chameleons are scalar fields that couple directly to ordinary matter with gravitational strength, but which nevertheless evade the stringent constraints on tests of gravity because of properties they acquire in the presence of high ambient matter density. Chameleon theories were originally constructed in a bottom-up, p... | 12.249765 | 10.655862 | 10.956661 | 9.996632 | 11.031241 | 11.4433 | 10.924216 | 10.733636 | 9.477485 | 10.803518 | 9.431685 | 9.898639 | 10.065898 | 9.918434 | 10.049259 | 9.913257 | 10.244012 | 9.704757 | 9.938428 | 9.836597 | 10.230212 |
hep-th/9507159 | Juergen Berges | J. Berges, N. Tetradis and C. Wetterich | Critical equation of state from the average action | Latex, 8 pages, 2 uuencoded figures | Phys.Rev.Lett. 77 (1996) 873-876 | 10.1103/PhysRevLett.77.873 | HD-THEP-95-27, OUTP 95-27 P | hep-th cond-mat | null | The scaling form of the critical equation of state is computed for
$O(N)$-symmetric models. We employ a method based on an exact flow equation for
a coarse grained free energy. A suitable truncation is solved numerically.
| [
{
"created": "Fri, 28 Jul 1995 08:17:12 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Berges",
"J.",
""
],
[
"Tetradis",
"N.",
""
],
[
"Wetterich",
"C.",
""
]
] | The scaling form of the critical equation of state is computed for $O(N)$-symmetric models. We employ a method based on an exact flow equation for a coarse grained free energy. A suitable truncation is solved numerically. | 11.071878 | 7.862064 | 8.493255 | 7.430558 | 8.112251 | 7.673316 | 7.454156 | 8.083619 | 7.308214 | 8.472031 | 9.187521 | 9.154037 | 9.33685 | 8.760371 | 8.819149 | 9.083869 | 8.771435 | 9.447014 | 9.211125 | 9.175996 | 9.138855 |
hep-th/9508177 | Paul Townsend | J.M. Izquierdo, N.D. Lambert, G. Papadopoulos and P.K. Townsend | Dyonic Membranes | Phyzzx. 27 pp. Additional para. added to introduction | Nucl.Phys.B460:560-578,1996 | 10.1016/0550-3213(95)00606-0 | R/95/40 | hep-th | null | We present dyonic multi-membrane solutions of the N=2 D=8 supergravity theory
that serves as the effective field theory of the $T^2$-compactified type II
superstring theory. The `electric' charge is fractional for generic asymptotic
values of an axion field, as for D=4 dyons. These membrane solutions are
supersymmetr... | [
{
"created": "Thu, 31 Aug 1995 15:57:21 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Oct 1995 17:51:17 GMT",
"version": "v2"
},
{
"created": "Mon, 20 Nov 1995 17:34:55 GMT",
"version": "v3"
}
] | 2009-10-09 | [
[
"Izquierdo",
"J. M.",
""
],
[
"Lambert",
"N. D.",
""
],
[
"Papadopoulos",
"G.",
""
],
[
"Townsend",
"P. K.",
""
]
] | We present dyonic multi-membrane solutions of the N=2 D=8 supergravity theory that serves as the effective field theory of the $T^2$-compactified type II superstring theory. The `electric' charge is fractional for generic asymptotic values of an axion field, as for D=4 dyons. These membrane solutions are supersymmetric... | 6.828202 | 6.592909 | 7.326193 | 6.456956 | 6.821077 | 6.992366 | 6.845369 | 6.667181 | 6.539869 | 7.876924 | 6.727117 | 6.695502 | 6.831212 | 6.788801 | 6.664593 | 6.873507 | 6.697344 | 6.671516 | 6.603857 | 7.01836 | 6.608255 |
hep-th/9411054 | Alexios Polychronakos | Alexios P. Polychronakos | Waves and Solitons in the Continuum Limit of the Calogero-Sutherland
Model | Version to appear in Physical Rerview Letters; contains some new
results and explanations | Phys.Rev.Lett. 74 (1995) 5153-5157 | 10.1103/PhysRevLett.74.5153 | CERN-TH.7496/94 | hep-th cond-mat | null | We examine a collection of particles interacting with inverse-square two-body
potentials in the thermodynamic limit. We find explicit large-amplitude density
waves and soliton solutions for the motion of the system. Waves can be
constructed as coherent states of either solitons or phonons. Therefore, either
solitons ... | [
{
"created": "Tue, 8 Nov 1994 13:39:34 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Dec 1994 14:04:29 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Dec 1994 10:31:10 GMT",
"version": "v3"
},
{
"created": "Wed, 3 May 1995 16:12:40 GMT",
"version": "v4"
}
] | 2009-10-28 | [
[
"Polychronakos",
"Alexios P.",
""
]
] | We examine a collection of particles interacting with inverse-square two-body potentials in the thermodynamic limit. We find explicit large-amplitude density waves and soliton solutions for the motion of the system. Waves can be constructed as coherent states of either solitons or phonons. Therefore, either solitons or... | 10.672843 | 10.960881 | 11.216593 | 10.695827 | 10.015565 | 9.816825 | 11.25483 | 10.658057 | 10.78567 | 11.941291 | 10.532568 | 10.619702 | 11.234506 | 10.430164 | 10.574762 | 10.652801 | 10.46234 | 10.638992 | 10.960831 | 11.368159 | 10.271591 |
1606.07870 | Dumitru Astefanesei | Andres Anabalon, Dumitru Astefanesei, and David Choque | Hairy AdS Solitons | 12 pages, no figures; v2: small changes and fixed typos | null | 10.1016/j.physletb.2016.08.049 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct exact hairy AdS soliton solutions in Einstein-dilaton gravity
theory. We examine their thermodynamic properties and discuss the role of these
solutions for the existence of first order phase transitions for hairy black
holes. The negative energy density associated to hairy AdS solitons can be
interpreted... | [
{
"created": "Sat, 25 Jun 2016 05:07:02 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jul 2016 18:28:59 GMT",
"version": "v2"
}
] | 2016-08-31 | [
[
"Anabalon",
"Andres",
""
],
[
"Astefanesei",
"Dumitru",
""
],
[
"Choque",
"David",
""
]
] | We construct exact hairy AdS soliton solutions in Einstein-dilaton gravity theory. We examine their thermodynamic properties and discuss the role of these solutions for the existence of first order phase transitions for hairy black holes. The negative energy density associated to hairy AdS solitons can be interpreted a... | 7.9063 | 7.945901 | 9.089727 | 7.50592 | 7.626104 | 7.330344 | 7.7569 | 7.520334 | 7.366545 | 8.674952 | 7.966262 | 7.622589 | 7.267564 | 7.500033 | 7.54306 | 7.596043 | 7.596103 | 7.453146 | 7.203705 | 7.671971 | 7.209469 |
hep-th/0407234 | Ewald Roessl | A. Gruppuso, E. Roessl and M. Shaposhnikov | Einstein static universe as a brane in extra dimensions | 45 pages, 3 figures | JHEP 0408 (2004) 011 | 10.1088/1126-6708/2004/08/011 | null | hep-th | null | We present a brane-world scenario in which two regions of $AdS_5$ space-time
are glued together along a 3-brane with constant positive curvature such that
{\em all} spatial dimensions form a compact manifold of topology $S^4$. It
turns out that the induced geometry on the brane is given by Einstein's static
universe.... | [
{
"created": "Tue, 27 Jul 2004 13:58:53 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Gruppuso",
"A.",
""
],
[
"Roessl",
"E.",
""
],
[
"Shaposhnikov",
"M.",
""
]
] | We present a brane-world scenario in which two regions of $AdS_5$ space-time are glued together along a 3-brane with constant positive curvature such that {\em all} spatial dimensions form a compact manifold of topology $S^4$. It turns out that the induced geometry on the brane is given by Einstein's static universe. I... | 6.219418 | 6.605296 | 6.410245 | 5.922379 | 6.744984 | 6.577973 | 6.573849 | 6.456426 | 6.177508 | 6.428636 | 6.126721 | 6.17084 | 6.240256 | 6.069338 | 6.11138 | 6.186747 | 6.247644 | 6.095159 | 6.204008 | 6.107161 | 6.098608 |
1811.07438 | Nabil Iqbal | Samuel E. Gralla, Nabil Iqbal | Effective Field Theory of Force-Free Electrodynamics | 15 pages; v2: some conventions changed, typos corrected | Phys. Rev. D 99, 105004 (2019) | 10.1103/PhysRevD.99.105004 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Force-free electrodynamics (FFE) is a closed set of equations for the
electromagnetic field of a magnetically dominated plasma. There are strong
arguments for the existence of force-free plasmas near pulsars and active black
holes, but FFE alone cannot account for the observational signatures, such as
coherent radio ... | [
{
"created": "Mon, 19 Nov 2018 00:38:00 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Feb 2019 21:38:25 GMT",
"version": "v2"
}
] | 2019-05-22 | [
[
"Gralla",
"Samuel E.",
""
],
[
"Iqbal",
"Nabil",
""
]
] | Force-free electrodynamics (FFE) is a closed set of equations for the electromagnetic field of a magnetically dominated plasma. There are strong arguments for the existence of force-free plasmas near pulsars and active black holes, but FFE alone cannot account for the observational signatures, such as coherent radio em... | 9.232578 | 9.087789 | 8.236076 | 8.000919 | 8.438471 | 8.565685 | 9.361361 | 8.322724 | 8.461752 | 9.579844 | 8.76577 | 8.042518 | 7.924798 | 7.970495 | 7.914341 | 8.010697 | 8.343892 | 8.136436 | 7.891215 | 8.354927 | 8.258045 |
hep-th/0411057 | Francesco Benini | Francesco Benini (Pisa, Scuola Normale Superiore & SISSA, Trieste) | The Coulomb branch of the Leigh-Strassler deformation and matrix models | 19 pages, 2 figures, latex | JHEP0412:068,2004 | 10.1088/1126-6708/2004/12/068 | null | hep-th | null | The Dijkgraaf-Vafa approach is used in order to study the Coulomb branch of
the Leigh-Strassler massive deformation of N=4 SYM with gauge group U(N). The
theory has N=1 SUSY and an N-dimensional Coulomb branch of vacua, which can be
described by a family of ``generalized'' Seiberg-Witten curves. The matrix
model anal... | [
{
"created": "Thu, 4 Nov 2004 18:27:35 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Benini",
"Francesco",
"",
"Pisa, Scuola Normale Superiore & SISSA, Trieste"
]
] | The Dijkgraaf-Vafa approach is used in order to study the Coulomb branch of the Leigh-Strassler massive deformation of N=4 SYM with gauge group U(N). The theory has N=1 SUSY and an N-dimensional Coulomb branch of vacua, which can be described by a family of ``generalized'' Seiberg-Witten curves. The matrix model analys... | 8.882972 | 8.09455 | 9.900168 | 8.10685 | 8.128372 | 8.438328 | 8.606917 | 8.144056 | 8.193455 | 10.665703 | 8.035132 | 8.076534 | 8.256754 | 8.041841 | 8.145994 | 7.926589 | 8.076527 | 7.940717 | 8.255973 | 8.283548 | 8.00483 |
1211.3867 | Mariana Grana | Mariana Gra\~na and Hagen Triendl | Generalized N=1 and N=2 structures in M-theory and type II orientifolds | 29 pages | JHEP 1303 (2013) 145 | 10.1007/JHEP03(2013)145 | IPhT-t12/099 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider M-theory and type IIA reductions to four dimensions with N=2 and
N=1 supersymmetry and discuss their interconnection. Our work is based on the
framework of Exceptional Generalized Geometry (EGG), which extends the tangent
bundle to include all symmetries in M-theory and type II string theory,
covariantizi... | [
{
"created": "Fri, 16 Nov 2012 11:58:46 GMT",
"version": "v1"
}
] | 2015-06-12 | [
[
"Graña",
"Mariana",
""
],
[
"Triendl",
"Hagen",
""
]
] | We consider M-theory and type IIA reductions to four dimensions with N=2 and N=1 supersymmetry and discuss their interconnection. Our work is based on the framework of Exceptional Generalized Geometry (EGG), which extends the tangent bundle to include all symmetries in M-theory and type II string theory, covariantizing... | 8.935139 | 8.987413 | 9.76983 | 8.403811 | 9.078593 | 8.862 | 8.549394 | 8.281123 | 8.09838 | 10.746268 | 8.083543 | 8.433879 | 8.95508 | 8.467758 | 8.59371 | 8.582762 | 8.335223 | 8.585111 | 8.671767 | 8.958584 | 8.495589 |
1310.1839 | Yasha Neiman | Yasha Neiman | Action and entanglement in gravity and field theory | 4 pages, 2 figures | Phys. Rev. Lett. 111, 261302 (2013) | 10.1103/PhysRevLett.111.261302 | IGC-13/10-3 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In non-gravitational quantum field theory, the entanglement entropy across a
surface depends on the short-distance regularization. Quantum gravity should
not require such regularization, and it's been conjectured that the
entanglement entropy there is always given by the black hole entropy formula
evaluated on the en... | [
{
"created": "Mon, 7 Oct 2013 15:59:44 GMT",
"version": "v1"
}
] | 2014-01-01 | [
[
"Neiman",
"Yasha",
""
]
] | In non-gravitational quantum field theory, the entanglement entropy across a surface depends on the short-distance regularization. Quantum gravity should not require such regularization, and it's been conjectured that the entanglement entropy there is always given by the black hole entropy formula evaluated on the enta... | 9.552912 | 9.794766 | 9.585203 | 8.890133 | 10.317663 | 10.048679 | 9.338542 | 9.169507 | 8.74252 | 9.883567 | 8.742936 | 8.606292 | 9.048185 | 8.503795 | 8.596173 | 8.654504 | 8.801622 | 8.750585 | 9.034475 | 9.186507 | 8.666502 |
2401.09399 | R Loll | J. Ambj{\o}rn, R. Loll | Causal Dynamical Triangulations: Gateway to Nonperturbative Quantum
Gravity | 27 pages, 7 figures, invited contribution to Encyclopedia of
Mathematical Physics 2nd Edition | null | null | null | hep-th gr-qc hep-lat | http://creativecommons.org/licenses/by/4.0/ | A powerful strategy to treat quantum field theories beyond perturbation
theory is by putting them on a lattice. However, the dynamical and symmetry
structure of general relativity have for a long time stood in the way of a
well-defined lattice formulation of quantum gravity. These issues are resolved
by using Causal ... | [
{
"created": "Wed, 17 Jan 2024 18:29:16 GMT",
"version": "v1"
}
] | 2024-01-18 | [
[
"Ambjørn",
"J.",
""
],
[
"Loll",
"R.",
""
]
] | A powerful strategy to treat quantum field theories beyond perturbation theory is by putting them on a lattice. However, the dynamical and symmetry structure of general relativity have for a long time stood in the way of a well-defined lattice formulation of quantum gravity. These issues are resolved by using Causal Dy... | 8.067523 | 7.701422 | 7.932838 | 7.540279 | 8.076353 | 8.15998 | 7.857167 | 7.568657 | 7.42394 | 8.788363 | 7.443449 | 7.301489 | 7.208052 | 7.347166 | 7.277275 | 7.533172 | 7.440954 | 7.315228 | 7.419251 | 7.290391 | 7.202765 |
0706.1224 | Vincent Rivasseau | V. Rivasseau | Constructive Matrix Theory | 12 pages, 3 figures | JHEP 0709:008,2007 | 10.1088/1126-6708/2007/09/008 | null | hep-th | null | We extend the technique of constructive expansions to compute the connected
functions of matrix models in a uniform way as the size of the matrix
increases. This provides the main missing ingredient for a non-perturbative
construction of the $\phi^{\star 4}_4$ field theory on the Moyal four
dimensional space.
| [
{
"created": "Fri, 8 Jun 2007 18:12:15 GMT",
"version": "v1"
}
] | 2009-11-18 | [
[
"Rivasseau",
"V.",
""
]
] | We extend the technique of constructive expansions to compute the connected functions of matrix models in a uniform way as the size of the matrix increases. This provides the main missing ingredient for a non-perturbative construction of the $\phi^{\star 4}_4$ field theory on the Moyal four dimensional space. | 14.847229 | 14.534389 | 16.938879 | 13.690763 | 15.412557 | 12.751077 | 14.738485 | 13.517316 | 15.05737 | 16.293169 | 14.989848 | 12.459806 | 13.64198 | 12.750672 | 14.553228 | 14.137507 | 13.746052 | 13.892196 | 14.198252 | 14.572964 | 12.962356 |
1001.2808 | George Savvidy K | George Savvidy | Topological mass generation in four-dimensional gauge theory | 18 pages, Note added addressing the question of minimal number of
derivarives in the cubic vertices for high spin fields, references added | Phys.Lett.B694:65-73,2010 | 10.1016/j.physletb.2010.09.036 | NRCPS-HE-10-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Lagrangian of non-Abelian tensor gauge fields describes the interaction
of the Yang-Mills and massless tensor bosons of increasing helicities. We have
found a metric-independent gauge invariant density which is a four-dimensional
analog of the Chern-Simons density. The Lagrangian augmented by this
Chern-Simons-li... | [
{
"created": "Sat, 16 Jan 2010 12:43:21 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Nov 2010 14:50:31 GMT",
"version": "v2"
},
{
"created": "Sun, 25 Oct 2020 13:49:41 GMT",
"version": "v3"
}
] | 2020-10-27 | [
[
"Savvidy",
"George",
""
]
] | The Lagrangian of non-Abelian tensor gauge fields describes the interaction of the Yang-Mills and massless tensor bosons of increasing helicities. We have found a metric-independent gauge invariant density which is a four-dimensional analog of the Chern-Simons density. The Lagrangian augmented by this Chern-Simons-like... | 13.331289 | 10.731758 | 14.367953 | 11.543763 | 12.264903 | 10.469534 | 11.765389 | 11.175903 | 11.222822 | 14.815589 | 11.264247 | 11.990757 | 13.207757 | 12.331779 | 12.270718 | 12.212858 | 12.343251 | 12.231739 | 12.063421 | 12.790046 | 12.076346 |
hep-th/9503138 | Margaret Gabler | L.C. Biedenharn and L.P. Horwitz | Quarks in the Skyrme-'t Hooft-Witten Model | Latex, 6 pages, no figures | Z.Phys. C65 (1995) 551-554 | 10.1007/BF01556143 | IASSNS-HEP 95/20 | hep-th | null | The three-flavor Skyrme-'t Hooft-Witten model is interpreted in terms of a
quark-like substructure, leading to a new model of explicitly confined
color-free ``quarks'' reminiscent of Gell-Mann's original pre-color quarks, but
with unexpected and significant differences.
| [
{
"created": "Tue, 21 Mar 1995 14:27:46 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Biedenharn",
"L. C.",
""
],
[
"Horwitz",
"L. P.",
""
]
] | The three-flavor Skyrme-'t Hooft-Witten model is interpreted in terms of a quark-like substructure, leading to a new model of explicitly confined color-free ``quarks'' reminiscent of Gell-Mann's original pre-color quarks, but with unexpected and significant differences. | 22.194122 | 19.586521 | 17.94537 | 18.912695 | 21.409891 | 20.83761 | 20.848743 | 19.339586 | 20.792034 | 21.921213 | 18.580412 | 19.021446 | 19.258591 | 18.708046 | 19.785788 | 19.295074 | 19.366579 | 19.24897 | 19.249489 | 19.794046 | 19.858805 |
2008.02187 | Andrei Kovtun | A. Kovtun, M. Zantedeschi | Breaking BEC: Quantum evolution of unstable condensates | null | Physical Review D 105, 085019 (2022) | 10.1103/PhysRevD.105.085019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we numerically explore the quantum behavior of a classically
unstable relativistic Bose-Einstein condensate (BEC). The main goal is to study
the phenomenon of so-called quantum break time which amounts to a significant
departure from a semiclassical mean-field description. It has been suggested
previousl... | [
{
"created": "Wed, 5 Aug 2020 15:21:32 GMT",
"version": "v1"
},
{
"created": "Mon, 31 Aug 2020 10:18:08 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Apr 2022 10:18:04 GMT",
"version": "v3"
}
] | 2022-04-27 | [
[
"Kovtun",
"A.",
""
],
[
"Zantedeschi",
"M.",
""
]
] | In this work we numerically explore the quantum behavior of a classically unstable relativistic Bose-Einstein condensate (BEC). The main goal is to study the phenomenon of so-called quantum break time which amounts to a significant departure from a semiclassical mean-field description. It has been suggested previously ... | 12.919238 | 13.333623 | 12.440619 | 12.169662 | 11.396652 | 12.224235 | 12.542197 | 13.537077 | 12.078315 | 13.8699 | 11.771116 | 11.765764 | 11.923552 | 11.821331 | 11.821996 | 11.567724 | 11.729877 | 12.048007 | 11.745198 | 11.620399 | 11.911974 |
1204.6288 | Yuho Sakatani | Masafumi Fukuma, Yuho Sakatani | Conformal higher-order viscoelastic fluid mechanics | 26 pages; v2: minor corrections; v3: minor corrections, to appear in
JHEP | JHEP 1206 (2012) 102 | 10.1007/JHEP06(2012)102 | KUNS-2391; MISC-2012-08 | hep-th cond-mat.stat-mech gr-qc nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a generally covariant formulation of conformal higher-order
viscoelastic fluid mechanics with strain allowed to take arbitrarily large
values. We give a general prescription to determine the dynamics of a
relativistic viscoelastic fluid in a way consistent with the hypothesis of
local thermodynamic equilib... | [
{
"created": "Fri, 27 Apr 2012 18:40:48 GMT",
"version": "v1"
},
{
"created": "Wed, 2 May 2012 08:50:39 GMT",
"version": "v2"
},
{
"created": "Mon, 28 May 2012 06:50:12 GMT",
"version": "v3"
}
] | 2012-06-27 | [
[
"Fukuma",
"Masafumi",
""
],
[
"Sakatani",
"Yuho",
""
]
] | We present a generally covariant formulation of conformal higher-order viscoelastic fluid mechanics with strain allowed to take arbitrarily large values. We give a general prescription to determine the dynamics of a relativistic viscoelastic fluid in a way consistent with the hypothesis of local thermodynamic equilibri... | 10.735743 | 10.797311 | 11.453951 | 11.098683 | 11.483318 | 12.234661 | 11.526064 | 11.111979 | 9.73179 | 12.062608 | 10.167865 | 10.507679 | 11.309531 | 10.517758 | 10.724946 | 10.398003 | 10.543138 | 10.572173 | 10.534693 | 11.329262 | 10.184622 |
0707.2455 | Alberto Salvio | A. Salvio, M. Shaposhnikov | Chiral Asymmetry from a 5D Higgs Mechanism | 30 pages, 5 figures, uses axodraw.sty. Extended version, matches the
article published on JHEP | JHEP 0711:037,2007 | 10.1088/1126-6708/2007/11/037 | null | hep-th hep-ph | null | An intriguing feature of the Standard Model is that the representations of
the unbroken gauge symmetries are vector-like whereas those of the
spontaneously broken gauge symmetries are chiral. Here we provide a toy model
which shows that a natural explanation of this property could emerge in higher
dimensional field t... | [
{
"created": "Tue, 17 Jul 2007 09:53:56 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Nov 2007 14:00:30 GMT",
"version": "v2"
}
] | 2009-04-30 | [
[
"Salvio",
"A.",
""
],
[
"Shaposhnikov",
"M.",
""
]
] | An intriguing feature of the Standard Model is that the representations of the unbroken gauge symmetries are vector-like whereas those of the spontaneously broken gauge symmetries are chiral. Here we provide a toy model which shows that a natural explanation of this property could emerge in higher dimensional field the... | 7.980691 | 7.388003 | 7.821902 | 7.339022 | 7.988064 | 7.682047 | 7.356207 | 7.809326 | 7.389898 | 8.143868 | 7.894612 | 7.60837 | 7.529251 | 7.454165 | 7.457508 | 7.644767 | 7.547451 | 7.546595 | 7.525369 | 7.650433 | 7.257205 |
2107.07525 | Luca Cassia | Luca Cassia and Maxim Zabzine | On refined Chern-Simons and refined ABJ matrix models | v2: 30 pages, minor revisions, added comments on relations to quantum
mirror curves in Section 2.5, added comments on ABJ integrals in Appendix C,
Lett.Math.Phys. version | null | 10.1007/s11005-022-01518-1 | UUITP-32/21 | hep-th math-ph math.MP math.QA | http://creativecommons.org/licenses/by/4.0/ | We consider the matrix model of $U(N)$ refined Chern-Simons theory on $S^3$
for the unknot. We derive a $q$-difference operator whose insertion in the
matrix integral reproduces an infinite set of Ward identities which we
interpret as $q$-Virasoro constraints. The constraints are rewritten as
difference equations for... | [
{
"created": "Thu, 15 Jul 2021 18:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Mar 2022 10:51:50 GMT",
"version": "v2"
}
] | 2022-03-23 | [
[
"Cassia",
"Luca",
""
],
[
"Zabzine",
"Maxim",
""
]
] | We consider the matrix model of $U(N)$ refined Chern-Simons theory on $S^3$ for the unknot. We derive a $q$-difference operator whose insertion in the matrix integral reproduces an infinite set of Ward identities which we interpret as $q$-Virasoro constraints. The constraints are rewritten as difference equations for t... | 8.15561 | 8.453362 | 10.260516 | 7.735076 | 7.855306 | 8.071866 | 8.390501 | 7.891097 | 7.532165 | 10.141957 | 8.228291 | 7.952875 | 8.635718 | 7.943766 | 8.16326 | 8.328892 | 8.130109 | 7.91513 | 7.766367 | 8.357845 | 7.904963 |
1603.06411 | Ljubica Davidovic | Ljubica Davidovi\'c | Open string T-duality in a weakly curved background | null | The European Physical Journal C (2016) 76:660 | 10.1140/epjc/s10052-016-4524-8 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a theory of an open string moving in a weakly curved background,
composed of a constant metric and a linearly coordinate dependent Kalb-Ramond
field with an infinitesimal field strength. We find its T-dual using the
generalized Buscher procedure developed for the closed string moving in a
weakly curved ba... | [
{
"created": "Mon, 21 Mar 2016 12:41:58 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Apr 2017 12:05:33 GMT",
"version": "v2"
}
] | 2017-04-25 | [
[
"Davidović",
"Ljubica",
""
]
] | We consider a theory of an open string moving in a weakly curved background, composed of a constant metric and a linearly coordinate dependent Kalb-Ramond field with an infinitesimal field strength. We find its T-dual using the generalized Buscher procedure developed for the closed string moving in a weakly curved back... | 11.600126 | 10.917106 | 12.919823 | 10.704165 | 12.884777 | 12.128577 | 11.685205 | 11.799776 | 11.266393 | 12.891451 | 10.861796 | 10.943962 | 11.787645 | 10.997867 | 11.441507 | 11.24315 | 10.986605 | 11.081241 | 10.988997 | 11.792613 | 10.722939 |
hep-th/0608065 | Sunandan Gangopadhyay | Biswajit Chakraborty, Sunandan Gangopadhyay, Arindam Ghosh Hazra | Normal ordering and noncommutativity in open bosonic strings | 10 pages latex, references added | Phys.Rev.D74:105011,2006 | 10.1103/PhysRevD.74.105011 | null | hep-th | null | Noncommutativity in an open bosonic string moving in the presence of a
background Neveu-Schwarz two-form field $B_{\mu \nu}$ is investigated in a
conformal field theory approach, leading to noncommutativity at the boundaries.
In contrast to several discussions, in which boundary conditions are taken as
Dirac constrai... | [
{
"created": "Thu, 10 Aug 2006 06:05:25 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Nov 2006 11:30:39 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Chakraborty",
"Biswajit",
""
],
[
"Gangopadhyay",
"Sunandan",
""
],
[
"Hazra",
"Arindam Ghosh",
""
]
] | Noncommutativity in an open bosonic string moving in the presence of a background Neveu-Schwarz two-form field $B_{\mu \nu}$ is investigated in a conformal field theory approach, leading to noncommutativity at the boundaries. In contrast to several discussions, in which boundary conditions are taken as Dirac constraint... | 9.936723 | 8.343509 | 10.834437 | 9.422864 | 9.927085 | 7.583919 | 8.371414 | 8.035332 | 9.040714 | 11.035018 | 8.429733 | 9.401002 | 10.15941 | 9.39145 | 9.472414 | 9.369644 | 9.192737 | 9.165249 | 9.21515 | 9.545856 | 9.26527 |
1506.05792 | William Donnelly | William Donnelly and Aron C. Wall | Geometric entropy and edge modes of the electromagnetic field | 41 pages, an extended version of arXiv:1412.1895 | Phys. Rev. D 94, 104053 (2016) | 10.1103/PhysRevD.94.104053 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the vacuum entanglement entropy of Maxwell theory in a class of
curved spacetimes by Kaluza-Klein reduction of the theory onto a
two-dimensional base manifold. Using two-dimensional duality, we express the
geometric entropy of the electromagnetic field as the entropy of a tower of
scalar fields, constant... | [
{
"created": "Thu, 18 Jun 2015 19:55:55 GMT",
"version": "v1"
}
] | 2016-11-29 | [
[
"Donnelly",
"William",
""
],
[
"Wall",
"Aron C.",
""
]
] | We calculate the vacuum entanglement entropy of Maxwell theory in a class of curved spacetimes by Kaluza-Klein reduction of the theory onto a two-dimensional base manifold. Using two-dimensional duality, we express the geometric entropy of the electromagnetic field as the entropy of a tower of scalar fields, constant e... | 10.203432 | 10.852532 | 10.991355 | 10.183226 | 9.987167 | 9.428575 | 9.769825 | 10.637118 | 10.220571 | 12.669185 | 10.306626 | 10.419823 | 10.2455 | 9.874984 | 10.115205 | 10.080008 | 10.178709 | 10.452435 | 10.230988 | 10.765779 | 10.482655 |
hep-th/9912109 | Axel Winterhalder | Michael Forger and Axel Winterhalder | New Approach to the Integrability of the Calogero Models | Latex2e, 44 pages, no figures | null | null | RT-MAP 99/07 | hep-th | null | We develop a new, systematic approach towards studying the integrability of
the ordinary Calogero-Moser-Sutherland models as well as the elliptic Calogero
models associated with arbitrary (semi-)simple Lie algebras and with symmetric
pairs of Lie algebras. It is based on the introduction of a function F, defined
on t... | [
{
"created": "Mon, 13 Dec 1999 20:22:20 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Forger",
"Michael",
""
],
[
"Winterhalder",
"Axel",
""
]
] | We develop a new, systematic approach towards studying the integrability of the ordinary Calogero-Moser-Sutherland models as well as the elliptic Calogero models associated with arbitrary (semi-)simple Lie algebras and with symmetric pairs of Lie algebras. It is based on the introduction of a function F, defined on the... | 6.139954 | 7.000323 | 6.991032 | 6.64792 | 6.685062 | 6.712989 | 6.925455 | 6.764102 | 6.204164 | 7.290003 | 6.563365 | 6.131968 | 6.26951 | 6.296103 | 6.205258 | 6.037729 | 6.084961 | 6.183778 | 6.022727 | 6.125198 | 5.987773 |
1003.2991 | Debaprasad Maity | Jiunn-Wei Chen, Ying-Jer Kao, Debaprasad Maity, Wen-Yu Wen, Chen-Pin
Yeh | Towards A Holographic Model of D-Wave Superconductors | 14 pages, 2 figures, Some typos corrected, Matched with the published
version | Phys.Rev.D81:106008,2010 | 10.1103/PhysRevD.81.106008 | null | hep-th cond-mat.supr-con gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The holographic model for S-wave high T_c superconductors developed by
Hartnoll, Herzog and Horowitz is generalized to describe D-wave
superconductors. The 3+1 dimensional gravitational theory consists a symmetric,
traceless second-rank tensor field and a U(1) gauge field in the background of
the AdS black hole. Belo... | [
{
"created": "Mon, 15 Mar 2010 18:58:44 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Mar 2010 16:03:48 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Mar 2010 11:15:09 GMT",
"version": "v3"
},
{
"created": "Fri, 9 Apr 2010 12:46:00 GMT",
"version": "v4"
},
{
"cr... | 2015-03-13 | [
[
"Chen",
"Jiunn-Wei",
""
],
[
"Kao",
"Ying-Jer",
""
],
[
"Maity",
"Debaprasad",
""
],
[
"Wen",
"Wen-Yu",
""
],
[
"Yeh",
"Chen-Pin",
""
]
] | The holographic model for S-wave high T_c superconductors developed by Hartnoll, Herzog and Horowitz is generalized to describe D-wave superconductors. The 3+1 dimensional gravitational theory consists a symmetric, traceless second-rank tensor field and a U(1) gauge field in the background of the AdS black hole. Below ... | 7.036542 | 7.143569 | 7.323403 | 6.638337 | 6.547087 | 6.429963 | 6.778768 | 6.531157 | 6.152828 | 7.705799 | 6.272862 | 6.804218 | 6.745743 | 6.32935 | 6.341918 | 6.544162 | 6.242464 | 6.279694 | 6.38538 | 6.898048 | 6.385112 |
1702.02350 | Arnab Priya Saha | Arnab Priya Saha | Double Soft Limit of Graviton Amplitude from the Cachazo-He-Yuan
Formalism | 10 pages v2: Title changed, abstract modified, references updated,
published in PRD | Phys. Rev. D 96, 045002 (2017) | 10.1103/PhysRevD.96.045002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a complete analysis for double soft limit of graviton scattering
amplitude using the formalism proposed by Cachazo, He and Yuan. Our results
agree with that obtained via BCFW recursion relations in arXiv:1504.05558. In
addition we find precise relations between degenerate and nondegenerate
solutions of sca... | [
{
"created": "Wed, 8 Feb 2017 10:04:29 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Aug 2017 12:24:39 GMT",
"version": "v2"
}
] | 2017-08-04 | [
[
"Saha",
"Arnab Priya",
""
]
] | We present a complete analysis for double soft limit of graviton scattering amplitude using the formalism proposed by Cachazo, He and Yuan. Our results agree with that obtained via BCFW recursion relations in arXiv:1504.05558. In addition we find precise relations between degenerate and nondegenerate solutions of scatt... | 10.419803 | 9.763494 | 10.932639 | 8.107441 | 8.353429 | 8.019696 | 8.157457 | 7.291087 | 7.822174 | 12.647857 | 7.680064 | 8.765488 | 8.901225 | 8.555171 | 8.466083 | 9.090231 | 8.588104 | 8.707595 | 8.665565 | 9.228107 | 8.781405 |
1703.09511 | Danijel Pikuti\'c | Daniel Meljanac, Stjepan Meljanac, Danijel Pikuti\'c, Kumar S. Gupta | Twisted statistics and the structure of Lie-deformed Minkowski spaces | 6 pages; version accepted for publication in Phys. Rev. D | Phys. Rev. D 96, 105008 (2017) | 10.1103/PhysRevD.96.105008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the realizations of noncommutative coordinates that are linear
in the Lorentz generators form a closed Lie algebra under certain conditions.
The star product and the coproduct for the momentum generators are obtained for
these Lie algebras and the corresponding twist satisfies the cocycle and
normalizati... | [
{
"created": "Tue, 28 Mar 2017 11:33:05 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Nov 2017 11:11:19 GMT",
"version": "v2"
}
] | 2017-11-15 | [
[
"Meljanac",
"Daniel",
""
],
[
"Meljanac",
"Stjepan",
""
],
[
"Pikutić",
"Danijel",
""
],
[
"Gupta",
"Kumar S.",
""
]
] | We show that the realizations of noncommutative coordinates that are linear in the Lorentz generators form a closed Lie algebra under certain conditions. The star product and the coproduct for the momentum generators are obtained for these Lie algebras and the corresponding twist satisfies the cocycle and normalization... | 8.799388 | 8.164707 | 9.288792 | 8.254434 | 8.298095 | 8.131713 | 7.820607 | 8.37179 | 7.758471 | 9.843129 | 7.842704 | 8.147577 | 8.121004 | 8.010072 | 8.113207 | 8.237741 | 8.095353 | 8.008897 | 7.998156 | 8.307189 | 8.079796 |
1304.7760 | Adam Bzowski | Adam Bzowski, Paul McFadden, Kostas Skenderis | Implications of conformal invariance in momentum space | 62 pages + list of results (28 pages) + appendices; v3: journal
version, v4: typos fixed, comments added | null | 10.1007/JHEP03(2014)111 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a comprehensive analysis of the implications of conformal
invariance for 3-point functions of the stress-energy tensor, conserved
currents and scalar operators in general dimension and in momentum space. Our
starting point is a novel and very effective decomposition of tensor
correlators which reduces thei... | [
{
"created": "Mon, 29 Apr 2013 19:58:04 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Jul 2013 12:39:49 GMT",
"version": "v2"
},
{
"created": "Sun, 26 Nov 2017 21:02:44 GMT",
"version": "v3"
},
{
"created": "Sat, 29 Dec 2018 11:13:32 GMT",
"version": "v4"
}
] | 2019-01-01 | [
[
"Bzowski",
"Adam",
""
],
[
"McFadden",
"Paul",
""
],
[
"Skenderis",
"Kostas",
""
]
] | We present a comprehensive analysis of the implications of conformal invariance for 3-point functions of the stress-energy tensor, conserved currents and scalar operators in general dimension and in momentum space. Our starting point is a novel and very effective decomposition of tensor correlators which reduces their ... | 6.125261 | 6.463385 | 7.002965 | 6.155899 | 6.647994 | 6.185239 | 6.839633 | 6.219335 | 6.624939 | 7.050325 | 6.48458 | 6.150317 | 6.019388 | 6.108195 | 6.020419 | 6.411646 | 6.103813 | 6.003615 | 5.92936 | 6.142114 | 6.067411 |
1906.08975 | Zebin Qiu | Kenji Fukushima, Shota Imaki, Zebin Qiu | Anomalous Casimir effect in axion electrodynamics | 8 pages, 2 figures; typos in Eqs.(30) and (A6) fixed; results
unchanged; accepted in PRD | Phys. Rev. D 100, 045013 (2019) | 10.1103/PhysRevD.100.045013 | null | hep-th cond-mat.mes-hall hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Casimir effect in axion electrodynamics. A finite $\theta$-term
affects the energy dispersion relation of photon if $\theta$ is time and/or
space dependent. We focus on a special case with linearly inhomogeneous
$\theta$ along the $z$-axis. Then we demonstrate that the Casimir force between
two parallel ... | [
{
"created": "Fri, 21 Jun 2019 06:35:54 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Aug 2019 05:42:42 GMT",
"version": "v2"
}
] | 2019-08-21 | [
[
"Fukushima",
"Kenji",
""
],
[
"Imaki",
"Shota",
""
],
[
"Qiu",
"Zebin",
""
]
] | We study the Casimir effect in axion electrodynamics. A finite $\theta$-term affects the energy dispersion relation of photon if $\theta$ is time and/or space dependent. We focus on a special case with linearly inhomogeneous $\theta$ along the $z$-axis. Then we demonstrate that the Casimir force between two parallel pl... | 6.273261 | 5.951196 | 5.86777 | 5.82545 | 6.17454 | 6.040423 | 6.129807 | 5.780209 | 5.680214 | 6.828235 | 5.926145 | 5.78401 | 6.017757 | 5.822678 | 6.019194 | 5.803142 | 5.885504 | 5.892568 | 5.832094 | 6.044167 | 5.914675 |
1505.07421 | Boris Altshuler | Boris L. Altshuler | Sakharov's induced gravity on the AdS background: SM scale as inverse
mass parameter of the Schwinger-DeWitt expansion | 26 pages, Latex; Contents and Section 5.4 added | Phys. Rev. D 92, 065007 (2015) | 10.1103/PhysRevD.92.065007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One loop quantum effective action W of scalar field 'living' on the AdS
background of the Randall-Sundrum model is defined here by now popular way
which excludes bulk UV divergencies; thus induced Planck mass is given not by
the UV regularization parameter, like in Sakharov's pioneer work, but by the
location of the ... | [
{
"created": "Wed, 27 May 2015 18:07:14 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jul 2015 13:51:52 GMT",
"version": "v2"
},
{
"created": "Sun, 11 Oct 2015 05:20:01 GMT",
"version": "v3"
}
] | 2015-10-13 | [
[
"Altshuler",
"Boris L.",
""
]
] | One loop quantum effective action W of scalar field 'living' on the AdS background of the Randall-Sundrum model is defined here by now popular way which excludes bulk UV divergencies; thus induced Planck mass is given not by the UV regularization parameter, like in Sakharov's pioneer work, but by the location of the UV... | 16.051765 | 17.255766 | 17.751997 | 16.156149 | 16.72937 | 17.513441 | 16.559555 | 17.046638 | 15.706439 | 19.673529 | 16.452696 | 15.884003 | 15.63267 | 15.601382 | 16.091114 | 15.800028 | 16.296402 | 15.698199 | 15.406664 | 15.823008 | 15.472603 |
hep-th/0109034 | Yves Brihaye | Y. Brihaye, J. Burzlaff, V. Paturyan, D. H. Tchrakian | The 1-soliton in the SO(3) gauged Skyrme model with mass term | new title, typos corrected, LaTeX, 8 pages, 4 figures | Nonlinearity 15 (2002) 385-392 | 10.1088/0951-7715/15/2/308 | null | hep-th | null | The solitons of the SO(3) gauged Skyrme model with no pion-mass potential
were studied in Refs. {nl,jmp}. Here, the effects of the inclusion of this
potential are studied. In contrast with the (ungauged) Skyrme model, where the
effect of this potential on the solitons is marginal, here it turns out to be
decisive, re... | [
{
"created": "Wed, 5 Sep 2001 07:56:20 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Jan 2002 08:02:13 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Brihaye",
"Y.",
""
],
[
"Burzlaff",
"J.",
""
],
[
"Paturyan",
"V.",
""
],
[
"Tchrakian",
"D. H.",
""
]
] | The solitons of the SO(3) gauged Skyrme model with no pion-mass potential were studied in Refs. {nl,jmp}. Here, the effects of the inclusion of this potential are studied. In contrast with the (ungauged) Skyrme model, where the effect of this potential on the solitons is marginal, here it turns out to be decisive, resu... | 8.767063 | 7.923697 | 8.111815 | 7.457081 | 7.885498 | 7.584658 | 7.690671 | 7.919955 | 7.858447 | 8.987795 | 7.560313 | 7.355813 | 7.659018 | 7.435655 | 7.502608 | 7.44381 | 7.603008 | 7.163403 | 7.333282 | 7.878129 | 7.508655 |
1711.07873 | Roldao da Rocha | Luca Fabbri, Roldao da Rocha | Unveiling a spinor field classification with non-Abelian gauge
symmetries | 12 pages | Phys. Lett. B 780, 427 (2018) | 10.1016/j.physletb.2018.03.029 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A spinor fields classification with non-Abelian gauge symmetries is
introduced, generalizing the the U(1) gauge symmetries-based Lounesto's
classification. Here, a more general classification, contrary to the Lounesto's
one, encompasses spinor multiplets, corresponding to non-Abelian gauge fields.
The particular case... | [
{
"created": "Tue, 21 Nov 2017 16:18:16 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Mar 2018 20:44:58 GMT",
"version": "v2"
}
] | 2018-03-28 | [
[
"Fabbri",
"Luca",
""
],
[
"da Rocha",
"Roldao",
""
]
] | A spinor fields classification with non-Abelian gauge symmetries is introduced, generalizing the the U(1) gauge symmetries-based Lounesto's classification. Here, a more general classification, contrary to the Lounesto's one, encompasses spinor multiplets, corresponding to non-Abelian gauge fields. The particular case o... | 12.257051 | 12.274735 | 13.02297 | 12.448665 | 13.481082 | 12.127528 | 13.733126 | 13.428077 | 12.656279 | 13.799572 | 12.214541 | 12.215901 | 12.459491 | 12.015686 | 11.632688 | 12.146194 | 12.446835 | 11.884395 | 12.156631 | 12.654387 | 11.74546 |
2402.18230 | Jesse Huhtala | Jesse Huhtala, Iiro Vilja | Practical Derivations of Fermion and Gauge Boson Reduction Formulae in
Curved Spacetimes | null | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | LSZ-type reduction formulae are derived for gauge fields and fermions in
curved spacetime. The formulae are derived using a conserved current method
applicable also to flat spacetimes. The method generalizes to more general
quantum field theories. The formulae are then applied to a few problems to
illustrate their us... | [
{
"created": "Wed, 28 Feb 2024 10:53:17 GMT",
"version": "v1"
}
] | 2024-02-29 | [
[
"Huhtala",
"Jesse",
""
],
[
"Vilja",
"Iiro",
""
]
] | LSZ-type reduction formulae are derived for gauge fields and fermions in curved spacetime. The formulae are derived using a conserved current method applicable also to flat spacetimes. The method generalizes to more general quantum field theories. The formulae are then applied to a few problems to illustrate their use. | 12.043447 | 9.736693 | 10.176044 | 9.966342 | 10.166397 | 10.434848 | 9.815422 | 9.522293 | 9.96042 | 10.069861 | 9.415481 | 8.397243 | 9.359059 | 8.751238 | 8.817091 | 8.337334 | 8.342946 | 8.066153 | 8.940866 | 9.671559 | 8.607075 |
2001.04902 | George Savvidy K | George Savvidy | Yang-Mills Classical and Quantum Mechanics and Maximally Chaotic
Dynamical Systems | 13 pages, 2 figures. arXiv admin note: substantial text overlap with
arXiv:2001.01785 | null | null | NRCPS-HE-02-2020 | hep-th astro-ph.GA hep-lat nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The maximally chaotic dynamical systems (DS) are the systems which have
nonzero Kolmogorov entropy. The Anosov C-condition defines a reach class of
hyperbolic dynamical systems that have exponential instability of the phase
trajectories and positive Kolmogorov entropy and are therefore maximally
chaotic. The interest... | [
{
"created": "Mon, 13 Jan 2020 08:31:55 GMT",
"version": "v1"
}
] | 2020-01-15 | [
[
"Savvidy",
"George",
""
]
] | The maximally chaotic dynamical systems (DS) are the systems which have nonzero Kolmogorov entropy. The Anosov C-condition defines a reach class of hyperbolic dynamical systems that have exponential instability of the phase trajectories and positive Kolmogorov entropy and are therefore maximally chaotic. The interest i... | 10.51769 | 11.265891 | 11.059097 | 10.354565 | 11.169859 | 11.372421 | 11.203918 | 11.064301 | 10.348113 | 11.051582 | 10.524686 | 10.806023 | 9.959997 | 10.46028 | 10.330705 | 10.420821 | 10.747782 | 10.510412 | 10.768974 | 10.228084 | 10.10568 |
hep-th/0601064 | Tianjun Li | Ching-Ming Chen, Tianjun Li, Dimitri V. Nanopoulos | Type IIA Pati-Salam Flux Vacua | RevTex4, 44 pages, 28 tables, references added, version to appear in
NPB | Nucl.Phys.B740:79-104,2006 | 10.1016/j.nuclphysb.2006.01.039 | ACT-01-06, MIFP-06-02 | hep-th hep-ph | null | We show that for supersymmetric AdS vacua on Type IIA orientifolds with flux
compactifications, the RR tadpole cancellation conditions can be completely
relaxed, and then the four-dimensional N=1 supersymmetry conditions are the
main constraints on consistent intersecting D6-brane model building. We
construct two kin... | [
{
"created": "Tue, 10 Jan 2006 22:06:20 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Jan 2006 20:55:54 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Chen",
"Ching-Ming",
""
],
[
"Li",
"Tianjun",
""
],
[
"Nanopoulos",
"Dimitri V.",
""
]
] | We show that for supersymmetric AdS vacua on Type IIA orientifolds with flux compactifications, the RR tadpole cancellation conditions can be completely relaxed, and then the four-dimensional N=1 supersymmetry conditions are the main constraints on consistent intersecting D6-brane model building. We construct two kinds... | 5.407463 | 5.307128 | 5.825104 | 5.113148 | 5.253166 | 5.206748 | 5.371392 | 5.134943 | 4.999611 | 5.896425 | 5.330654 | 5.368569 | 5.5103 | 5.240124 | 5.343767 | 5.443454 | 5.328576 | 5.180984 | 5.264869 | 5.652829 | 5.367598 |
hep-th/0406091 | Gonzalo A. Palma | Gonzalo A. Palma, Anne-Christine Davis (DAMTP, University of
Cambridge) | Low Energy Branes, Effective Theory and Cosmology | 19 pages, 4 figures | Phys.Rev. D70 (2004) 064021 | 10.1103/PhysRevD.70.064021 | null | hep-th astro-ph hep-ph | null | The low energy regime of cosmological BPS-brane configurations with a bulk
scalar field is studied. We construct a systematic method to obtain
five-dimensional solutions to the full system of equations governing the
geometry and dynamics of the bulk. This is done for an arbitrary bulk scalar
field potential and takin... | [
{
"created": "Thu, 10 Jun 2004 14:51:29 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Palma",
"Gonzalo A.",
"",
"DAMTP, University of\n Cambridge"
],
[
"Davis",
"Anne-Christine",
"",
"DAMTP, University of\n Cambridge"
]
] | The low energy regime of cosmological BPS-brane configurations with a bulk scalar field is studied. We construct a systematic method to obtain five-dimensional solutions to the full system of equations governing the geometry and dynamics of the bulk. This is done for an arbitrary bulk scalar field potential and taking ... | 10.350622 | 9.373237 | 9.186768 | 9.616836 | 9.929417 | 9.970655 | 10.024464 | 9.476731 | 9.59403 | 10.370751 | 8.873252 | 9.626954 | 9.541207 | 10.01365 | 9.734146 | 9.999461 | 10.077623 | 9.971514 | 9.785528 | 9.495702 | 9.604027 |
hep-th/0408147 | Ralph Blumenhagen | R. Blumenhagen, T. Weigand | Chiral Gepner Model Orientifolds | LaTeX, Contribution to the proceedings of the conference "SUSY 2004",
Tsukuba, June 17-23, 2004 | null | null | MPP-2004-96 | hep-th | null | We summarize recent progress in constructing orientifolds of Gepner models, a
phenomenologically interesting class of exactly solvable string
compactifications with viable gauge groups and chiral matter.
| [
{
"created": "Thu, 19 Aug 2004 11:26:29 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Blumenhagen",
"R.",
""
],
[
"Weigand",
"T.",
""
]
] | We summarize recent progress in constructing orientifolds of Gepner models, a phenomenologically interesting class of exactly solvable string compactifications with viable gauge groups and chiral matter. | 11.908473 | 8.380856 | 10.815874 | 7.939989 | 8.541544 | 8.240799 | 7.96317 | 7.814833 | 7.954233 | 12.977957 | 8.996592 | 9.120395 | 10.074441 | 9.218648 | 9.275234 | 8.94107 | 9.736254 | 9.045597 | 8.894284 | 10.246716 | 9.005908 |
hep-th/9712039 | Marco Matone | G. Bertoldi and M. Matone | Beta Function, C--Theorem and WDVV Equations in 4D N=2 SYM | 6 pages, LaTeX, References added | Phys.Lett. B425 (1998) 104-106 | 10.1016/S0370-2693(98)00200-7 | DFPD97/TH/55 | hep-th hep-ph | null | We show that the exact $beta$--function of 4D N=2 SYM plays the role of the
metric whose inverse satisfies the WDVV--like equations $\F_{ikl}\beta^{lm}
\F_{mnj}=\F_{jkl}\beta^{lm}\F_{mni}$. The conjecture that the WDVV--like
equations are equivalent to the identity involving the $u$--modulus and the
prepotential $\F$... | [
{
"created": "Fri, 5 Dec 1997 00:46:49 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jan 1998 12:56:46 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Bertoldi",
"G.",
""
],
[
"Matone",
"M.",
""
]
] | We show that the exact $beta$--function of 4D N=2 SYM plays the role of the metric whose inverse satisfies the WDVV--like equations $\F_{ikl}\beta^{lm} \F_{mnj}=\F_{jkl}\beta^{lm}\F_{mni}$. The conjecture that the WDVV--like equations are equivalent to the identity involving the $u$--modulus and the prepotential $\F$, ... | 11.974801 | 12.682156 | 12.018308 | 11.795585 | 13.326565 | 13.788696 | 12.657624 | 12.041075 | 12.394921 | 16.332151 | 11.38581 | 10.559731 | 12.028892 | 11.56243 | 11.070065 | 11.462854 | 11.85584 | 11.086287 | 11.385644 | 12.06713 | 10.838597 |
hep-th/9509153 | Ryu Sasaki | M.F. Mourad and R. Sasaki | Non-Linear Sigma Models on a Half Plane | 25 pages, latex, no figures | Int.J.Mod.Phys. A11 (1996) 3127-3144 | 10.1142/S0217751X96001504 | YITP-95-4 | hep-th | null | In the context of integrable field theory with boundary, the integrable
non-linear sigma models in two dimensions, for example, the $O(N)$, the
principal chiral, the ${\rm CP}^{N-1}$ and the complex Grassmannian sigma
models are discussed on a half plane. In contrast to the well known cases of
sine-Gordon, non-linear... | [
{
"created": "Wed, 27 Sep 1995 07:29:06 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Mourad",
"M. F.",
""
],
[
"Sasaki",
"R.",
""
]
] | In the context of integrable field theory with boundary, the integrable non-linear sigma models in two dimensions, for example, the $O(N)$, the principal chiral, the ${\rm CP}^{N-1}$ and the complex Grassmannian sigma models are discussed on a half plane. In contrast to the well known cases of sine-Gordon, non-linear S... | 6.116482 | 6.252477 | 7.527351 | 6.16299 | 6.751028 | 6.182831 | 6.099835 | 6.168666 | 5.734482 | 7.502214 | 6.004124 | 5.717246 | 6.345211 | 5.951667 | 5.984401 | 5.936578 | 5.843822 | 5.818497 | 5.876884 | 5.943446 | 5.761293 |
hep-th/0211152 | Yaron Antebi | Ofer Aharony, Yaron E. Antebi, Micha Berkooz, and Ram Fishman | "Holey Sheets" - Pfaffians and Subdeterminants as D-brane Operators in
Large N Gauge Theories | 39 pages, 10 figures, harvmac | JHEP 0212:069,2002 | 10.1088/1126-6708/2002/12/069 | WIS/44/02-NOV-DPP | hep-th | null | In the AdS/CFT correspondence, wrapped D3-branes (such as "giant gravitons")
on the string theory side of the correspondence have been identified with
Pfaffian, determinant and subdeterminant operators on the field theory side. We
substantiate this identification by showing that the presence of pairs of such
operator... | [
{
"created": "Mon, 18 Nov 2002 12:04:41 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Aharony",
"Ofer",
""
],
[
"Antebi",
"Yaron E.",
""
],
[
"Berkooz",
"Micha",
""
],
[
"Fishman",
"Ram",
""
]
] | In the AdS/CFT correspondence, wrapped D3-branes (such as "giant gravitons") on the string theory side of the correspondence have been identified with Pfaffian, determinant and subdeterminant operators on the field theory side. We substantiate this identification by showing that the presence of pairs of such operators ... | 8.624984 | 7.888996 | 9.062767 | 7.995342 | 8.228718 | 7.448813 | 7.67327 | 7.704788 | 7.460764 | 10.286252 | 8.135221 | 8.045546 | 8.800363 | 8.130792 | 8.364877 | 7.944326 | 8.350588 | 8.476804 | 8.148488 | 8.674884 | 8.135015 |
1805.10360 | Pablo Gonzalez | Pablo Gonz\'alez, Gonzalo A. Palma, Nelson Videla | Covariant evolution of perturbations during reheating in two-field
inflation | null | null | 10.1088/1475-7516/2018/12/001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a covariant method for studying the effects of a reheating phase
on the primordial adiabatic and isocurvature perturbations in two-field models
of inflation. To model the decay of the scalar fields into radiation at the end
of inflation, we introduce a prescription in which radiation is treated as an
addit... | [
{
"created": "Fri, 25 May 2018 20:44:15 GMT",
"version": "v1"
}
] | 2018-12-12 | [
[
"González",
"Pablo",
""
],
[
"Palma",
"Gonzalo A.",
""
],
[
"Videla",
"Nelson",
""
]
] | We develop a covariant method for studying the effects of a reheating phase on the primordial adiabatic and isocurvature perturbations in two-field models of inflation. To model the decay of the scalar fields into radiation at the end of inflation, we introduce a prescription in which radiation is treated as an additio... | 7.963146 | 8.4123 | 8.165096 | 7.503179 | 7.821491 | 8.281745 | 7.99475 | 7.602484 | 7.64957 | 7.679478 | 7.962557 | 7.820501 | 7.916459 | 7.870476 | 7.991848 | 7.999645 | 8.096841 | 7.891958 | 7.689912 | 7.856831 | 7.734323 |
0909.3364 | Chaiho Rim Prof | Hyeong-Chan Kim, Youngone Lee, Chaiho Rim | Braided Statistics from Abelian Twist in $\kappa$-Minkowski Spacetime | 6pages, no figures | null | 10.1142/S0217732310033311 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | $\kappa$-deformed commutation relation between quantum operators is
constructed via abelian twist deformation in $\kappa$-Minkowski spacetime. The
commutation relation is written in terms of universal $R$-matrix satisfying
braided statistics. The equal-time commutator function turns out to vanish in
this framework.
| [
{
"created": "Fri, 18 Sep 2009 06:47:23 GMT",
"version": "v1"
}
] | 2015-05-14 | [
[
"Kim",
"Hyeong-Chan",
""
],
[
"Lee",
"Youngone",
""
],
[
"Rim",
"Chaiho",
""
]
] | $\kappa$-deformed commutation relation between quantum operators is constructed via abelian twist deformation in $\kappa$-Minkowski spacetime. The commutation relation is written in terms of universal $R$-matrix satisfying braided statistics. The equal-time commutator function turns out to vanish in this framework. | 14.732959 | 11.61301 | 11.495039 | 9.493737 | 9.678565 | 10.630712 | 9.987605 | 9.542474 | 9.229774 | 14.3624 | 9.259704 | 10.297146 | 10.482787 | 9.966734 | 10.562987 | 10.125269 | 9.361326 | 10.547977 | 9.865387 | 11.382115 | 10.353859 |
hep-th/9803174 | Igor V. Volovich | I.V. Volovich | Large N Gauge Theories and Anti-de Sitter Bag Model | 6 pages, Latex | null | null | SMI-08-1998 | hep-th gr-qc hep-ph | null | Using a proposal of Maldacena one describes the large N limit of gauge
theories in terms of supergravity solutions on anti-de Sitter space. From this
point of view we discuss a possible scenario for quark confinement in gauge
theory by describing hadrons as strongly curved universes. In particular an
interpretation o... | [
{
"created": "Fri, 20 Mar 1998 19:21:00 GMT",
"version": "v1"
},
{
"created": "Sat, 21 Mar 1998 16:30:20 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Volovich",
"I. V.",
""
]
] | Using a proposal of Maldacena one describes the large N limit of gauge theories in terms of supergravity solutions on anti-de Sitter space. From this point of view we discuss a possible scenario for quark confinement in gauge theory by describing hadrons as strongly curved universes. In particular an interpretation of ... | 13.270467 | 13.164085 | 13.318598 | 13.066874 | 13.142688 | 13.092978 | 13.344121 | 12.712735 | 13.524172 | 14.206485 | 13.295869 | 12.60529 | 12.388725 | 12.653174 | 13.146869 | 12.54602 | 13.044838 | 12.534969 | 12.24768 | 12.723089 | 12.611997 |
2001.06467 | A. Yu. Petrov | M. Gomes, T. Mariz, J. R. Nascimento, A. Yu. Petrov, A. J. da Silva | 1/N Expansion for Horava-Lifshitz like four-fermion models | 12 pages | Eur. Phys. J. C 80, 518 (2020) | 10.1140/epjc/s10052-020-8100-x | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a class of four-fermion Gross-Neveu like models in four dimensions
with critical exponents $z=2$ and $z=3$. The models with $z=2$ are known to be
perturbatively nonrenormalizable but are shown to be renormalizable in the
context of the $1/N$ expansion. We calculate explicitly the effective potential
for thes... | [
{
"created": "Fri, 17 Jan 2020 18:36:59 GMT",
"version": "v1"
}
] | 2020-06-12 | [
[
"Gomes",
"M.",
""
],
[
"Mariz",
"T.",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"da Silva",
"A. J.",
""
]
] | We study a class of four-fermion Gross-Neveu like models in four dimensions with critical exponents $z=2$ and $z=3$. The models with $z=2$ are known to be perturbatively nonrenormalizable but are shown to be renormalizable in the context of the $1/N$ expansion. We calculate explicitly the effective potential for these ... | 5.072219 | 4.107486 | 4.740532 | 4.427851 | 4.405454 | 4.059346 | 4.539352 | 3.914943 | 4.06482 | 4.885082 | 4.425931 | 4.301526 | 4.669718 | 4.421906 | 4.568647 | 4.176376 | 4.334265 | 4.34859 | 4.459233 | 4.614145 | 4.219841 |
1403.0436 | Jon Chkareuli | J.L. Chkareuli | Photon and photino as Nambu-Goldstone zero modes in an emergent SUSY QED | 23 pages, to appear in Eur. Phys. J. C 74 (2014) issue 6. arXiv admin
note: substantial text overlap with arXiv:1305.6898 | null | 10.1140/epjc/s10052-014-2906-3 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that supersymmetry with its well known advantages, such as
naturalness, grand unification and dark matter candidate seems to possess one
more attractive feature: it may trigger, through its own spontaneous violation
in the visible sector, a dynamical generation of gauge fields as massless
Nambu-Goldstone mod... | [
{
"created": "Mon, 3 Mar 2014 14:02:48 GMT",
"version": "v1"
},
{
"created": "Sun, 15 Jun 2014 23:22:01 GMT",
"version": "v2"
}
] | 2015-06-18 | [
[
"Chkareuli",
"J. L.",
""
]
] | We argue that supersymmetry with its well known advantages, such as naturalness, grand unification and dark matter candidate seems to possess one more attractive feature: it may trigger, through its own spontaneous violation in the visible sector, a dynamical generation of gauge fields as massless Nambu-Goldstone modes... | 13.27409 | 14.246715 | 12.971915 | 12.483424 | 13.850182 | 14.136088 | 13.771208 | 13.886059 | 12.744876 | 14.502619 | 13.225451 | 13.16415 | 12.607715 | 12.887575 | 12.939734 | 13.154011 | 13.331656 | 13.177176 | 12.623383 | 12.97369 | 13.479021 |
hep-th/0012020 | Don N. Page | Don N. Page | Thermodynamics of Near-Extreme Black Holes | 12 pages, Latex, submitted for the proceedings of JGRG10, the 10th
meeting of the Japanese Society of General Relativity and Gravitation, Osaka,
2000 Sept. 11-14 | null | null | Alberta Thy 13-00 | hep-th gr-qc | null | The thermodynamics of nearly-extreme charged black holes depends upon the
number of ground states at fixed large charge and upon the distribution of
excited energy states. Here three possibilities are examined: (1) Ground state
highly degenerate (as suggested by the large semiclassical Hawking entropy of
an extreme R... | [
{
"created": "Mon, 4 Dec 2000 17:59:56 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Page",
"Don N.",
""
]
] | The thermodynamics of nearly-extreme charged black holes depends upon the number of ground states at fixed large charge and upon the distribution of excited energy states. Here three possibilities are examined: (1) Ground state highly degenerate (as suggested by the large semiclassical Hawking entropy of an extreme Rei... | 12.875739 | 14.448197 | 12.667384 | 12.286922 | 14.558475 | 13.981599 | 14.313296 | 12.385119 | 13.135308 | 13.722506 | 12.517283 | 12.648164 | 12.000981 | 11.901995 | 12.929357 | 12.045574 | 12.863849 | 12.272046 | 13.01285 | 12.256444 | 12.589927 |
hep-th/0606132 | Matthias Schmidt | E. Fischer, G. Rudolph, M. Schmidt | A Lattice Gauge Model of Singular Marsden-Weinstein Reduction. Part I.
Kinematics | 27 pages, 6 figures | J.Geom.Phys. 57 (2007) 1193-1213 | 10.1016/j.geomphys.2006.09.008 | null | hep-th math-ph math.MP | null | The simplest nontrivial toy model of a classical SU(3) lattice gauge theory
is studied in the Hamiltonian approach. By means of singular symplectic
reduction, the reduced phase space is constructed. Two equivalent descriptions
of this space in terms of a symplectic covering as well as in terms of
invariants are deriv... | [
{
"created": "Thu, 15 Jun 2006 08:21:32 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Fischer",
"E.",
""
],
[
"Rudolph",
"G.",
""
],
[
"Schmidt",
"M.",
""
]
] | The simplest nontrivial toy model of a classical SU(3) lattice gauge theory is studied in the Hamiltonian approach. By means of singular symplectic reduction, the reduced phase space is constructed. Two equivalent descriptions of this space in terms of a symplectic covering as well as in terms of invariants are derived... | 10.395623 | 8.797447 | 10.075109 | 8.898221 | 8.636177 | 9.586414 | 8.798272 | 9.3811 | 9.00376 | 10.258659 | 9.349358 | 8.977601 | 9.679945 | 9.682992 | 9.568006 | 8.838264 | 8.663065 | 9.205622 | 9.751223 | 9.100965 | 9.191915 |
1112.5371 | Bernard de Wit | Nabamita Banerjee, Bernard de Wit and Stefanos Katmadas | The off-shell 4D/5D connection | 35 pages; minor text changes and one more reference | null | 10.1007/JHEP03(2012)061 | ITP-UU-11/44; Nikhef-2011-031; CPHT-RR106.1211 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A systematic off-shell reduction scheme from five to four space-time
dimensions is presented for supergravity theories with eight supercharges. It
is applicable to theories with higher-derivative couplings and it is used to
address a number of open questions regarding BPS black holes in five
dimensions. Under this re... | [
{
"created": "Thu, 22 Dec 2011 16:34:44 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Mar 2012 17:38:15 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Banerjee",
"Nabamita",
""
],
[
"de Wit",
"Bernard",
""
],
[
"Katmadas",
"Stefanos",
""
]
] | A systematic off-shell reduction scheme from five to four space-time dimensions is presented for supergravity theories with eight supercharges. It is applicable to theories with higher-derivative couplings and it is used to address a number of open questions regarding BPS black holes in five dimensions. Under this redu... | 6.33657 | 5.824115 | 7.475949 | 5.965696 | 5.938581 | 5.846775 | 5.940094 | 5.917173 | 6.211679 | 7.535693 | 5.815227 | 5.999691 | 6.392333 | 5.936393 | 5.963007 | 5.972818 | 6.078187 | 6.046307 | 6.002367 | 6.401375 | 5.903086 |
hep-th/0111025 | Ren-Jie Zhang | C.P. Burgess, P. Martineau, F. Quevedo, G. Rajesh and R.-J. Zhang | Brane-Antibrane Inflation in Orbifold and Orientifold Models | 30 pages, 2 figures. Substantial changes on version 1. New
cosmological scenarios proposed including the dilaton as the inflaton. Main
conclusions unchanged | JHEP 0203:052,2002 | 10.1088/1126-6708/2002/03/052 | DAMTP-2001-97, EFI-0147, McGill-01/23 | hep-th astro-ph hep-ph | null | We analyse the cosmological implications of brane-antibrane systems in
string-theoretic orbifold and orientifold models. In a class of realistic
models, consistency conditions require branes and antibranes to be stuck at
different fixed points, and so their mutual attraction generates a potential
for one of the radii... | [
{
"created": "Mon, 5 Nov 2001 20:10:30 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Nov 2001 02:36:11 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Feb 2002 19:03:30 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Burgess",
"C. P.",
""
],
[
"Martineau",
"P.",
""
],
[
"Quevedo",
"F.",
""
],
[
"Rajesh",
"G.",
""
],
[
"Zhang",
"R. -J.",
""
]
] | We analyse the cosmological implications of brane-antibrane systems in string-theoretic orbifold and orientifold models. In a class of realistic models, consistency conditions require branes and antibranes to be stuck at different fixed points, and so their mutual attraction generates a potential for one of the radii o... | 10.226147 | 10.678756 | 10.787468 | 9.972627 | 11.171531 | 11.824924 | 11.333627 | 10.847082 | 10.25988 | 11.313767 | 9.807125 | 9.715033 | 9.965874 | 9.628219 | 9.656283 | 9.945923 | 9.674005 | 9.845636 | 9.699883 | 10.130286 | 9.608168 |
hep-th/0004145 | Rudra Prakash Malik | E. Harikumar (Univ. of Hyderabad), R. P. Malik (Bose Centre, Calcutta)
and M. Sivakumar (Univ. of Hyderabad) | Hodge decomposition theorem for Abelian two form gauge theory | LaTeX, 18 pages, no figures, minor corrections, references updated,
typos corrected, journal reference given | J.Phys.A33:7149-7164,2000 | 10.1088/0305-4470/33/40/312 | null | hep-th | null | We show that the BRST/anti-BRST invariant 3+1 dimensional 2-form gauge theory
has further nilpotent symmetries (dual BRST /anti-dual BRST) that leave the
gauge fixing term invariant. The generator for the dual BRST symmetry is
analogous to the co-exterior derivative of differential geometry. There exists
a bosonic sy... | [
{
"created": "Thu, 20 Apr 2000 12:08:42 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Sep 2000 10:14:47 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Oct 2000 15:40:34 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Harikumar",
"E.",
"",
"Univ. of Hyderabad"
],
[
"Malik",
"R. P.",
"",
"Bose Centre, Calcutta"
],
[
"Sivakumar",
"M.",
"",
"Univ. of Hyderabad"
]
] | We show that the BRST/anti-BRST invariant 3+1 dimensional 2-form gauge theory has further nilpotent symmetries (dual BRST /anti-dual BRST) that leave the gauge fixing term invariant. The generator for the dual BRST symmetry is analogous to the co-exterior derivative of differential geometry. There exists a bosonic symm... | 7.960747 | 6.156804 | 8.508194 | 6.422243 | 6.626116 | 6.002386 | 6.262289 | 6.164083 | 6.776952 | 8.974971 | 6.731994 | 7.167839 | 7.602898 | 7.124238 | 6.938479 | 7.174982 | 6.933209 | 6.830667 | 6.955901 | 7.490329 | 7.137754 |
1512.01554 | Roy Ben-Israel | Roy Ben-Israel, Amit Giveon, Nissan Itzhaki, Lior Liram | On the Stringy Hartle-Hawking State | null | null | 10.1007/JHEP03(2016)019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that non-perturbative $\alpha'$ stringy effects render the
Hartle-Hawking state associated with the $SL(2)/U(1)$ eternal black hole
singular at the horizon. We discuss implications of this observation on
firewalls in string theory.
| [
{
"created": "Fri, 4 Dec 2015 21:00:06 GMT",
"version": "v1"
}
] | 2016-03-23 | [
[
"Ben-Israel",
"Roy",
""
],
[
"Giveon",
"Amit",
""
],
[
"Itzhaki",
"Nissan",
""
],
[
"Liram",
"Lior",
""
]
] | We argue that non-perturbative $\alpha'$ stringy effects render the Hartle-Hawking state associated with the $SL(2)/U(1)$ eternal black hole singular at the horizon. We discuss implications of this observation on firewalls in string theory. | 12.721489 | 10.101268 | 13.413543 | 9.535821 | 11.334447 | 10.123388 | 10.00634 | 9.909636 | 10.740954 | 15.086531 | 10.812086 | 10.574215 | 13.648418 | 10.167392 | 9.663893 | 10.211987 | 10.720638 | 11.103543 | 10.320117 | 13.350577 | 10.261374 |
hep-th/9501052 | Douglas A. Singleton | Douglas Singleton | Exact Schwarzschild-Like Solution for Yang-Mills Theories | 11 pages LaTeX | Phys.Rev.D51:5911-5914,1995 | 10.1103/PhysRevD.51.5911 | null | hep-th | null | Drawing on the parallel between general relativity and Yang-Mills theory we
obtain an exact Schwarzschild-like solution for SU(2) gauge fields coupled to a
massless scalar field. Pushing the analogy further we speculate that this
classical solution to the Yang-Mills equations shows confinement in the same
way that pa... | [
{
"created": "Fri, 13 Jan 1995 18:52:48 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Singleton",
"Douglas",
""
]
] | Drawing on the parallel between general relativity and Yang-Mills theory we obtain an exact Schwarzschild-like solution for SU(2) gauge fields coupled to a massless scalar field. Pushing the analogy further we speculate that this classical solution to the Yang-Mills equations shows confinement in the same way that part... | 9.936769 | 9.776139 | 9.459611 | 8.805293 | 9.373496 | 10.356366 | 9.051009 | 8.783924 | 8.770369 | 9.477775 | 9.529496 | 9.424135 | 8.921441 | 8.7533 | 8.8216 | 8.90487 | 9.159161 | 8.778517 | 8.911273 | 8.855066 | 9.263194 |
hep-th/9304025 | null | Frank De Jonghe | Schwinger--Dyson BRST symmetry and the Batalin--Vilkovisky Lagrangian
Quantisation of Gauge Theories with Open or Reducible Gauge Algebras | 10p, CERN-TH-6858/93, KUL-TF-93/13 | J.Math.Phys. 35 (1994) 2734-2742 | 10.1063/1.530482 | null | hep-th | null | In this short note we extend the results of Alfaro and Damgaard on the origin
of antifields to theories with a gauge algebra that is open or reducible.
| [
{
"created": "Wed, 7 Apr 1993 15:46:44 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"De Jonghe",
"Frank",
""
]
] | In this short note we extend the results of Alfaro and Damgaard on the origin of antifields to theories with a gauge algebra that is open or reducible. | 17.353453 | 15.1003 | 19.378405 | 14.408431 | 15.584155 | 16.419338 | 14.57582 | 14.257222 | 14.136506 | 23.798933 | 14.515328 | 12.998127 | 16.106556 | 14.554984 | 13.388899 | 12.788168 | 12.969726 | 13.484389 | 14.560995 | 14.799963 | 13.599672 |
hep-th/0501074 | Heinrich Saller | Heinrich Saller | The Hilbert spaces for stable and unstable particles | 20 pages, macros includes | null | null | 2005-2 | hep-th | null | The Hilbert spaces for stable scattering states and particles are determined
by the representations of the characterizing Euclidean and Poincar\'e group and
given, respectively, by the square integrable functions on the momentum
2-spheres for a fixed absolute value of momentum and on the energy-momentum
3-hyperboloid... | [
{
"created": "Tue, 11 Jan 2005 11:13:48 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Saller",
"Heinrich",
""
]
] | The Hilbert spaces for stable scattering states and particles are determined by the representations of the characterizing Euclidean and Poincar\'e group and given, respectively, by the square integrable functions on the momentum 2-spheres for a fixed absolute value of momentum and on the energy-momentum 3-hyperboloids ... | 15.69494 | 17.298319 | 17.728256 | 16.386999 | 17.522137 | 18.408215 | 16.913267 | 16.888674 | 17.030947 | 19.930552 | 15.97519 | 15.793938 | 15.703473 | 15.098665 | 16.211376 | 15.437141 | 16.115736 | 16.144503 | 15.548244 | 16.821356 | 15.581239 |
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