id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0810.2449 | Walter Vinci | Walter Vinci | A Generalized Construction for Lumps and Non-Abelian Vortices | 12 pages, no figures, Contribution to "Continuous Advances in QCD
2008", Minneapolis, May 2008 | null | 10.1142/9789812838667_0026 | IFUP-TH/2008-33 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the general vortex solution in a fully-Higgsed, color-flavor
locked vacuum of a non-Abelian gauge theory, where the gauge group is taken to
be the product of an arbitrary simple group and U(1), with a Fayet-Iliopoulos
term. The strict correspondence between vortices and lumps in the associated
Non-Linear... | [
{
"created": "Tue, 14 Oct 2008 13:35:22 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Vinci",
"Walter",
""
]
] | We construct the general vortex solution in a fully-Higgsed, color-flavor locked vacuum of a non-Abelian gauge theory, where the gauge group is taken to be the product of an arbitrary simple group and U(1), with a Fayet-Iliopoulos term. The strict correspondence between vortices and lumps in the associated Non-Linear S... | 9.394994 | 7.33634 | 9.115523 | 7.705124 | 8.156866 | 6.788133 | 6.711132 | 7.2784 | 7.676678 | 9.712823 | 7.184799 | 8.32082 | 8.673053 | 8.28287 | 8.272486 | 8.158333 | 8.104039 | 8.23432 | 8.095216 | 8.58809 | 8.198297 |
1302.3183 | Lorenz von Smekal | Lorenz von Smekal and Manon Bischoff | Lattice BRST without Neuberger 0/0 problem | Talk presented at Quark Confinement and the Hadron Spectrum X,
October 8-12, 2012, Munich, Germany | null | null | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We illustrate in a simple toy model how the methods of SUSY quantum mechanics
and topological quantum field theory can be used for covariant gauge-fixing
with unbroken BRST symmetry on a finite lattice.
| [
{
"created": "Wed, 13 Feb 2013 18:29:15 GMT",
"version": "v1"
}
] | 2013-02-14 | [
[
"von Smekal",
"Lorenz",
""
],
[
"Bischoff",
"Manon",
""
]
] | We illustrate in a simple toy model how the methods of SUSY quantum mechanics and topological quantum field theory can be used for covariant gauge-fixing with unbroken BRST symmetry on a finite lattice. | 17.243059 | 12.618312 | 13.36728 | 13.559428 | 12.11979 | 13.251955 | 12.997632 | 13.872433 | 12.243373 | 13.43344 | 11.96228 | 13.233643 | 13.101937 | 13.170269 | 13.025712 | 12.68329 | 12.871233 | 12.493711 | 12.875947 | 12.991457 | 11.794618 |
1002.3373 | Emmanuil Saridakis | Sourish Dutta, Emmanuel N. Saridakis | Overall observational constraints on the running parameter \lambda of
Horava-Lifshitz gravity | 9 pages, 2 figures, version published at JCAP | JCAP 1005:013,2010 | 10.1088/1475-7516/2010/05/013 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use observational data from Type Ia Supernovae (SNIa), Baryon Acoustic
Oscillations (BAO), and Cosmic Microwave Background (CMB), along with
requirements of Big Bang Nucleosynthesis (BBN), to constrain the running
parameter $\lambda$ of Horava-Lifshitz gravity, which determines the flow
between the Ultra-Violet an... | [
{
"created": "Wed, 17 Feb 2010 21:03:43 GMT",
"version": "v1"
},
{
"created": "Tue, 4 May 2010 15:12:44 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Dutta",
"Sourish",
""
],
[
"Saridakis",
"Emmanuel N.",
""
]
] | We use observational data from Type Ia Supernovae (SNIa), Baryon Acoustic Oscillations (BAO), and Cosmic Microwave Background (CMB), along with requirements of Big Bang Nucleosynthesis (BBN), to constrain the running parameter $\lambda$ of Horava-Lifshitz gravity, which determines the flow between the Ultra-Violet and ... | 7.145869 | 6.702329 | 7.079873 | 6.229486 | 6.741144 | 6.457298 | 6.985508 | 6.118126 | 6.35146 | 6.993634 | 6.625336 | 6.800004 | 6.602274 | 6.501465 | 6.685962 | 6.593252 | 6.478316 | 6.373775 | 6.501304 | 6.685668 | 6.472658 |
hep-th/0009044 | Igor O. Cherednikov | Igor O. Cherednikov | Calculation of Ground State Energy for Confined Fermion Fields | 10 pages, LaTeX; no figures. Version to appear in Phys. Lett. B
(2001) | Phys.Lett. B498 (2001) 40-46 | 10.1016/S0370-2693(00)01338-1 | null | hep-th | null | A method for renormalization of the Casimir energy of confined fermion fields
in (1+1)D is proposed. It is based on the extraction of singularities which
appear as poles at the point of physical value of the regularization parameter,
and subsequent compensation of them by means of redefinition of the "bare"
constants... | [
{
"created": "Wed, 6 Sep 2000 15:14:41 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Sep 2000 13:40:29 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Dec 2000 12:47:53 GMT",
"version": "v3"
},
{
"created": "Fri, 15 Dec 2000 15:25:09 GMT",
"version": "v4"
}
] | 2016-09-06 | [
[
"Cherednikov",
"Igor O.",
""
]
] | A method for renormalization of the Casimir energy of confined fermion fields in (1+1)D is proposed. It is based on the extraction of singularities which appear as poles at the point of physical value of the regularization parameter, and subsequent compensation of them by means of redefinition of the "bare" constants. ... | 13.230188 | 12.226371 | 12.361596 | 11.839115 | 12.391508 | 11.897958 | 11.679923 | 11.730743 | 12.361399 | 14.255107 | 12.262269 | 11.014571 | 11.167113 | 11.497591 | 12.000149 | 11.518259 | 11.737256 | 11.459308 | 11.494335 | 11.610198 | 11.543447 |
hep-th/0612281 | Wellington Galleas | W. Galleas and M.J. Martins | Exact solution and finite size properties of the $U_{q}[osp(2|2m)]$
vertex model | 40 pages, 8 figures, latex | Nucl.Phys.B768:219-246,2007 | 10.1016/j.nuclphysb.2007.01.022 | UFSCARF-TH-12-17 | hep-th nlin.SI | null | We have diagonalized the transfer matrix of the $U_{q}[osp(2|2m)]$ vertex
model by means of the algebraic Bethe ansatz method for a variety of grading
possibilities. This allowed us to investigate the thermodynamic limit as well
as the finite size properties of the corresponding spin chain in the massless
regime. The... | [
{
"created": "Wed, 27 Dec 2006 17:12:05 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Galleas",
"W.",
""
],
[
"Martins",
"M. J.",
""
]
] | We have diagonalized the transfer matrix of the $U_{q}[osp(2|2m)]$ vertex model by means of the algebraic Bethe ansatz method for a variety of grading possibilities. This allowed us to investigate the thermodynamic limit as well as the finite size properties of the corresponding spin chain in the massless regime. The l... | 7.565616 | 7.788167 | 8.7547 | 7.272051 | 8.028546 | 8.127993 | 7.357269 | 7.679617 | 7.226499 | 9.196857 | 7.242664 | 7.020702 | 8.047685 | 6.989175 | 7.220479 | 7.409186 | 7.186235 | 6.966334 | 7.27713 | 8.152484 | 7.276156 |
1803.00490 | Prabal Adhikari | Prabal Adhikari, Soma B. Beleznay and Massimo Mannarelli | Finite Density Two Color Chiral Perturbation Theory Revisited | 9 pages, 5 figures | Eur. Phys. J. C (2018) 78:441 | 10.1140/epjc/s10052-018-5934-6 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit two-color, two-flavor chiral perturbation theory at finite isospin
and baryon density. We investigate the phase diagram obtained varying the
isospin and the baryon chemical potentials, focusing on the phase transition
occurring when the two chemical potentials are equal and exceed the pion mass
(which is d... | [
{
"created": "Thu, 1 Mar 2018 16:41:03 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jun 2018 13:53:30 GMT",
"version": "v2"
}
] | 2018-06-05 | [
[
"Adhikari",
"Prabal",
""
],
[
"Beleznay",
"Soma B.",
""
],
[
"Mannarelli",
"Massimo",
""
]
] | We revisit two-color, two-flavor chiral perturbation theory at finite isospin and baryon density. We investigate the phase diagram obtained varying the isospin and the baryon chemical potentials, focusing on the phase transition occurring when the two chemical potentials are equal and exceed the pion mass (which is deg... | 6.392236 | 7.528975 | 6.653478 | 6.741345 | 7.266736 | 7.126042 | 7.289412 | 7.399851 | 6.367123 | 7.657675 | 6.998326 | 6.798912 | 6.540262 | 6.561951 | 6.463193 | 6.832321 | 6.677532 | 7.007713 | 6.547871 | 6.67994 | 6.529331 |
2311.04278 | Jorge Russo | Luca Mezincescu, Jorge G. Russo and Paul K. Townsend | Hamiltonian birefringence and Born-Infeld limits | 39 pages. V3: Expanded version with additional material | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using Hamiltonian methods, we find six relativistic theories of nonlinear
electrodynamics for which plane wave perturbations about a constant uniform
background are not birefringent. All have the same conformal strong-field limit
to Bialynicki-Birula (BB) electrodynamics, but only four avoid superluminal
propagation:... | [
{
"created": "Tue, 7 Nov 2023 19:00:03 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Dec 2023 10:43:15 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Feb 2024 18:19:07 GMT",
"version": "v3"
}
] | 2024-02-22 | [
[
"Mezincescu",
"Luca",
""
],
[
"Russo",
"Jorge G.",
""
],
[
"Townsend",
"Paul K.",
""
]
] | Using Hamiltonian methods, we find six relativistic theories of nonlinear electrodynamics for which plane wave perturbations about a constant uniform background are not birefringent. All have the same conformal strong-field limit to Bialynicki-Birula (BB) electrodynamics, but only four avoid superluminal propagation: B... | 11.413821 | 9.453744 | 11.210463 | 9.996889 | 10.448246 | 9.224729 | 10.463072 | 9.683712 | 9.711082 | 11.978662 | 9.694142 | 9.693753 | 10.583709 | 10.042254 | 9.981894 | 10.469055 | 9.946298 | 9.761624 | 9.843993 | 10.92743 | 9.842559 |
0910.3488 | Chiang-Mei Chen | Chiang-Mei Chen, Dmitri V. Gal'tsov, Nobuyoshi Ohta, Dmitry G. Orlov | Global solutions for higher-dimensional stretched small black holes | 26 pages, 19 figures, minor corrections | null | 10.1103/PhysRevD.81.024002 | KU-TP 037 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Small black holes in heterotic string theory have vanishing horizon area at
the supergravity level, but the horizon is stretched to the finite radius
$AdS_2 \times S^{D-2}$ geometry once higher curvature corrections are turned
on. This has been demonstrated to give good agreement with microscopic entropy
counting. Pr... | [
{
"created": "Mon, 19 Oct 2009 09:17:47 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Dec 2009 01:54:29 GMT",
"version": "v2"
}
] | 2013-05-29 | [
[
"Chen",
"Chiang-Mei",
""
],
[
"Gal'tsov",
"Dmitri V.",
""
],
[
"Ohta",
"Nobuyoshi",
""
],
[
"Orlov",
"Dmitry G.",
""
]
] | Small black holes in heterotic string theory have vanishing horizon area at the supergravity level, but the horizon is stretched to the finite radius $AdS_2 \times S^{D-2}$ geometry once higher curvature corrections are turned on. This has been demonstrated to give good agreement with microscopic entropy counting. Prev... | 7.101295 | 7.142796 | 7.185412 | 6.827292 | 7.4558 | 7.168094 | 7.283949 | 6.642544 | 6.788729 | 7.680165 | 6.964093 | 6.818573 | 6.84867 | 6.778905 | 6.810834 | 6.70318 | 6.744472 | 6.742875 | 6.63954 | 7.041409 | 6.637037 |
1906.02891 | David Choque Quispe | David Choque Quispe | Agujeros Negros con Pelo y Dualidad AdS/CFT | 121 pages, 12 figures, A thesis submitted for the degree of Doctor of
Philosophy | null | null | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | The present thesis is based in the material previously published in
[arXiv:1501.04252, arXiv:1511.08759, arXiv:1606.07870] and it is organized in
the following way. The second chapter is shown as the isometric group of the
space time AdS is exactly (isomorphic) match to the conformal group of the dual
CFT theory. We ... | [
{
"created": "Fri, 7 Jun 2019 04:06:07 GMT",
"version": "v1"
}
] | 2019-06-10 | [
[
"Quispe",
"David Choque",
""
]
] | The present thesis is based in the material previously published in [arXiv:1501.04252, arXiv:1511.08759, arXiv:1606.07870] and it is organized in the following way. The second chapter is shown as the isometric group of the space time AdS is exactly (isomorphic) match to the conformal group of the dual CFT theory. We pr... | 8.041702 | 8.377081 | 8.326241 | 8.075233 | 8.268666 | 8.053616 | 8.076041 | 8.056497 | 7.837667 | 8.597854 | 7.843194 | 7.978528 | 8.115712 | 7.913968 | 7.996364 | 7.976004 | 7.926883 | 7.985842 | 7.868312 | 8.124269 | 7.89066 |
hep-th/0312180 | R. S. Ward | R.S. Ward | Symmetric Calorons | 12 pages, typos corrected | Phys.Lett. B582 (2004) 203-210 | 10.1016/j.physletb.2003.12.051 | DCPT-03/63 | hep-th nlin.SI | null | Calorons (periodic instantons) interpolate between monopoles and instantons,
and their holonomy gives approximate Skyrmion configurations. We show that, for
each caloron charge N \leq 4, there exists a one-parameter family of calorons
which are symmetric under subgroups of the three-dimensional rotation group. In
eac... | [
{
"created": "Tue, 16 Dec 2003 10:37:35 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Mar 2004 11:32:16 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Ward",
"R. S.",
""
]
] | Calorons (periodic instantons) interpolate between monopoles and instantons, and their holonomy gives approximate Skyrmion configurations. We show that, for each caloron charge N \leq 4, there exists a one-parameter family of calorons which are symmetric under subgroups of the three-dimensional rotation group. In each ... | 8.661077 | 7.539659 | 6.766093 | 6.628199 | 7.289127 | 7.260068 | 8.100683 | 7.10289 | 6.660428 | 8.186429 | 6.802128 | 6.661563 | 7.287025 | 6.636228 | 6.715284 | 6.633235 | 6.880151 | 6.833584 | 6.671878 | 7.471825 | 6.937359 |
1305.1278 | Roberto Tateo Dr. | Michele Caselle, Davide Fioravanti, Ferdinando Gliozzi and Roberto
Tateo | Quantisation of the effective string with TBA | 25 pages, 2 PDF figures, PDFLatex. v2: typos corrected, two
references added, new comments in sections 6 and 7. v3: minor amendments, to
be published in JHEP | null | null | null | hep-th hep-lat math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In presence of a static pair of sources, the spectrum of low-lying states of
whatever confining gauge theory in D space-time dimensions is described, at
large source separations, by an effective string theory. In the far infrared
the latter flows, in the static gauge, to a two-dimensional massless free-field
theory. ... | [
{
"created": "Mon, 6 May 2013 19:02:56 GMT",
"version": "v1"
},
{
"created": "Fri, 10 May 2013 18:15:30 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Jun 2013 12:24:12 GMT",
"version": "v3"
}
] | 2013-06-20 | [
[
"Caselle",
"Michele",
""
],
[
"Fioravanti",
"Davide",
""
],
[
"Gliozzi",
"Ferdinando",
""
],
[
"Tateo",
"Roberto",
""
]
] | In presence of a static pair of sources, the spectrum of low-lying states of whatever confining gauge theory in D space-time dimensions is described, at large source separations, by an effective string theory. In the far infrared the latter flows, in the static gauge, to a two-dimensional massless free-field theory. It... | 9.10609 | 9.531494 | 10.696968 | 9.298079 | 9.439961 | 9.262271 | 9.248003 | 9.451074 | 9.003855 | 11.675405 | 9.210273 | 8.852175 | 9.4666 | 8.923386 | 8.938845 | 8.959998 | 8.628116 | 8.626802 | 8.754549 | 9.246359 | 8.86572 |
1503.05159 | Shlomo S. Razamat | Davide Gaiotto and Shlomo S. Razamat | N=1 theories of class S_k | 73 pages, 24 figures. v2: minor corrections and changes | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct classes of ${\cal N}=1$ superconformal theories elements of
which are labeled by punctured Riemann surfaces. Degenerations of the surfaces
correspond, in some cases, to weak coupling limits. Different classes are
labeled by two integers (N,k). The k=1 case coincides with A_{N-1} ${\cal N}=2$
theories of ... | [
{
"created": "Tue, 17 Mar 2015 18:46:10 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jul 2015 06:07:04 GMT",
"version": "v2"
}
] | 2015-07-22 | [
[
"Gaiotto",
"Davide",
""
],
[
"Razamat",
"Shlomo S.",
""
]
] | We construct classes of ${\cal N}=1$ superconformal theories elements of which are labeled by punctured Riemann surfaces. Degenerations of the surfaces correspond, in some cases, to weak coupling limits. Different classes are labeled by two integers (N,k). The k=1 case coincides with A_{N-1} ${\cal N}=2$ theories of cl... | 7.175267 | 7.709325 | 7.892323 | 6.841346 | 7.074001 | 7.570535 | 7.345996 | 7.203528 | 7.105353 | 8.753732 | 7.187034 | 7.107695 | 7.496799 | 7.104818 | 7.063719 | 7.198883 | 7.110124 | 6.934806 | 7.06155 | 7.608004 | 7.181736 |
1703.10159 | Suvrat Raju | Suvrat Raju | The Sensitivity of Black Holes to Low Energy Excitations | 5 pages | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by-nc-sa/4.0/ | A general principle of statistical mechanics is that low energy excitations
of a thermal state change expectation values of observables by a very small
amount. However some observables in the vicinity of the horizon of a large
black hole in anti-de Sitter space naively seem to violate this bound. This
potential viola... | [
{
"created": "Wed, 29 Mar 2017 17:57:50 GMT",
"version": "v1"
}
] | 2017-03-30 | [
[
"Raju",
"Suvrat",
""
]
] | A general principle of statistical mechanics is that low energy excitations of a thermal state change expectation values of observables by a very small amount. However some observables in the vicinity of the horizon of a large black hole in anti-de Sitter space naively seem to violate this bound. This potential violati... | 8.452833 | 8.97064 | 9.65317 | 8.751336 | 8.922361 | 8.434313 | 7.823912 | 8.676721 | 8.373821 | 9.532144 | 8.000814 | 7.995348 | 8.471062 | 7.734174 | 7.933235 | 8.205925 | 8.020974 | 7.978412 | 8.045221 | 8.593517 | 7.923865 |
hep-th/9410200 | Simon Brian Davis | Simon Davis | The Four-Point Function on a Surface of Infinite Genus | 11 pages, TeX, 2 figures. The power in the exponential term in
equation (10) is now typed uniformly and the square in the denominator in
equation (14) has been removed | Mod.Phys.Lett. A9 (1994) 1299-1308 | 10.1142/S021773239400112X | DAMTP-R/94/1 | hep-th | null | The four-point function arising in the scattering of closed bosonic strings
in their tachyonic ground state is evaluated on a surface of infinite genus.
The amplitude has poles corresponding to physical intermediate states and
divergences at the boundary of moduli space, but no new types of divergences
result from th... | [
{
"created": "Wed, 26 Oct 1994 18:31:55 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Jul 1996 13:42:00 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Davis",
"Simon",
""
]
] | The four-point function arising in the scattering of closed bosonic strings in their tachyonic ground state is evaluated on a surface of infinite genus. The amplitude has poles corresponding to physical intermediate states and divergences at the boundary of moduli space, but no new types of divergences result from the ... | 10.249022 | 9.381746 | 10.245163 | 8.857406 | 9.539196 | 8.881113 | 10.01348 | 9.534815 | 8.138105 | 11.824158 | 9.177956 | 9.34955 | 10.087018 | 9.275252 | 9.225726 | 9.430505 | 9.369807 | 8.932398 | 8.999552 | 10.147283 | 9.770778 |
hep-th/0505059 | Heinrich Saller | Heinrich Saller | Gauge coupling constants as residues of spacetime representations | 49 pages | Int.J.Theor.Phys. 45 (2006) 276-342 | 10.1007/s10773-005-9021-z | MPP-2005-39 | hep-th | null | The gauge coupling constants in the electroweak standard model can be written
as mass ratios, e.g. the coupling constant for isospin interactions
$g_2^2=2{m_W^2\over m^2}\sim 2({80\over169})^2\sim{1\over 2.3}$ with the mass
of the charged weak boson and the mass parameter characterizing the ground
state degeneracy. A... | [
{
"created": "Fri, 6 May 2005 09:15:15 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Saller",
"Heinrich",
""
]
] | The gauge coupling constants in the electroweak standard model can be written as mass ratios, e.g. the coupling constant for isospin interactions $g_2^2=2{m_W^2\over m^2}\sim 2({80\over169})^2\sim{1\over 2.3}$ with the mass of the charged weak boson and the mass parameter characterizing the ground state degeneracy. A t... | 12.906477 | 14.911465 | 13.557473 | 13.494498 | 15.243422 | 15.518502 | 14.291159 | 14.380653 | 13.776564 | 14.40353 | 12.875134 | 12.653008 | 12.765358 | 12.700726 | 12.794264 | 12.700814 | 13.159067 | 12.992198 | 12.962667 | 12.702588 | 12.757183 |
hep-th/9503228 | Itzhak Bars | Itzhak Bars | STRINGY EVIDENCE FOR D=11 STRUCTURE IN STRONGLY COUPLED TYPE II-A
SUPERSTRING | LaTeX, revtex, 2-column, 10 pages. | Phys.Rev. D52 (1995) 3567-3575 | 10.1103/PhysRevD.52.3567 | USC-95/HEP-B2. | hep-th | null | Witten proposed that the low energy physics of strongly coupled D=10 type-IIA
superstring may be described by D=11 supergravity. To explore the stringy
aspects of the underlying theory we examine the stringy massive states. We
propose a systematic formula for identifying non-perturbative states in D=10
type-IIA super... | [
{
"created": "Sat, 1 Apr 1995 06:05:58 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Bars",
"Itzhak",
""
]
] | Witten proposed that the low energy physics of strongly coupled D=10 type-IIA superstring may be described by D=11 supergravity. To explore the stringy aspects of the underlying theory we examine the stringy massive states. We propose a systematic formula for identifying non-perturbative states in D=10 type-IIA superst... | 9.340305 | 9.388311 | 8.989272 | 8.463881 | 9.877117 | 9.825535 | 8.516418 | 8.777534 | 8.62088 | 10.149073 | 8.556851 | 8.52423 | 8.809004 | 8.427236 | 8.661178 | 8.541395 | 8.554747 | 8.496222 | 8.66271 | 8.954982 | 8.500549 |
2310.19716 | Luca Romano | Eric Bergshoeff and Luca Romano | Non-Relativistic Heterotic String Theory | 12 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this work we consider heterotic-gravity as the low-energy approximation to
heterotic string theory. We define a consistent non-relativistic limit of
heterotic gravity that includes the Yang-Mills Chern-Simons term. We perform
three tests on the heterotic limit: we use it to (i) derive the
non-relativistic transfor... | [
{
"created": "Mon, 30 Oct 2023 16:43:38 GMT",
"version": "v1"
}
] | 2023-10-31 | [
[
"Bergshoeff",
"Eric",
""
],
[
"Romano",
"Luca",
""
]
] | In this work we consider heterotic-gravity as the low-energy approximation to heterotic string theory. We define a consistent non-relativistic limit of heterotic gravity that includes the Yang-Mills Chern-Simons term. We perform three tests on the heterotic limit: we use it to (i) derive the non-relativistic transforma... | 7.85123 | 7.283011 | 8.047836 | 7.127697 | 7.177743 | 7.124263 | 7.206481 | 6.878981 | 7.052989 | 8.436304 | 6.724813 | 7.192472 | 7.396808 | 7.157186 | 7.221661 | 7.497565 | 7.22954 | 7.19748 | 7.143103 | 7.877859 | 7.258492 |
hep-th/9908173 | Helmut Kroger | T. Heinzl, H. Kr\"oger and N. Scheu | Loss of Causality in Discretized Light-Cone Quantisation | Text (REVTEX file) + 4 figures (4 epsf files + 4 ps files) | null | null | null | hep-th hep-lat | null | We demonstrate that front form quantisation with periodicity in a compact
light-like direction (discretized light-cone quantisation) violates
microcausality.
| [
{
"created": "Thu, 26 Aug 1999 20:12:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Heinzl",
"T.",
""
],
[
"Kröger",
"H.",
""
],
[
"Scheu",
"N.",
""
]
] | We demonstrate that front form quantisation with periodicity in a compact light-like direction (discretized light-cone quantisation) violates microcausality. | 25.879456 | 14.454509 | 18.695118 | 13.813372 | 15.412008 | 14.347219 | 15.819232 | 14.532906 | 13.765179 | 22.175484 | 14.928571 | 15.713821 | 17.05028 | 15.864643 | 17.688383 | 17.676159 | 17.627575 | 18.451817 | 15.11124 | 18.742752 | 19.981979 |
hep-th/0606060 | Roberto Auzzi | R. Auzzi, M. Shifman and A. Yung | Domain Lines as Fractional Strings | 28 pages, 13 figure, v2 typos fixed and reference added | Phys.Rev.D74:045007,2006 | 10.1103/PhysRevD.74.045007 | FTPI-MINN-06-17, UMN-TH-2504-06 | hep-th | null | We consider N=2 supersymmetric quantum electrodynamics (SQED) with 2 flavors,
the Fayet--Iliopoulos parameter, and a mass term $\beta$ which breaks the
extended supersymmetry down to N=1. The bulk theory has two vacua; at $\beta=0$
the BPS-saturated domain wall interpolating between them has a moduli space
parameteri... | [
{
"created": "Wed, 7 Jun 2006 19:43:58 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jul 2006 15:41:26 GMT",
"version": "v2"
}
] | 2010-05-27 | [
[
"Auzzi",
"R.",
""
],
[
"Shifman",
"M.",
""
],
[
"Yung",
"A.",
""
]
] | We consider N=2 supersymmetric quantum electrodynamics (SQED) with 2 flavors, the Fayet--Iliopoulos parameter, and a mass term $\beta$ which breaks the extended supersymmetry down to N=1. The bulk theory has two vacua; at $\beta=0$ the BPS-saturated domain wall interpolating between them has a moduli space parameterize... | 7.533623 | 8.104408 | 8.52024 | 8.007925 | 8.433859 | 8.425803 | 8.063398 | 8.261427 | 8.028589 | 9.262093 | 7.846237 | 7.482049 | 8.25788 | 7.580652 | 7.800276 | 7.840382 | 7.421643 | 7.666289 | 7.78055 | 8.091901 | 7.724972 |
1206.6132 | Joseph Marsano | Herb Clemens, Joseph Marsano, Tony Pantev, Stuart Raby, Hsian-Hua
Tseng | A Global SU(5) F-theory model with Wilson line breaking | 95 pages (71 pages + 1 Appendix); v2 references added, minor
corrections | null | 10.1007/JHEP01(2013)150 | EFI-12-14; OHSTPY-HEP-T-12-002 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We engineer compact SU(5) Grand Unified Theories in F-theory in which
GUT-breaking is achieved by a discrete Wilson line. Because the internal gauge
field is flat, these models avoid the high scale threshold corrections
associated with hypercharge flux. Along the way, we exemplify the
`local-to-global' approach in F-... | [
{
"created": "Tue, 26 Jun 2012 22:02:19 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jul 2012 15:42:19 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Clemens",
"Herb",
""
],
[
"Marsano",
"Joseph",
""
],
[
"Pantev",
"Tony",
""
],
[
"Raby",
"Stuart",
""
],
[
"Tseng",
"Hsian-Hua",
""
]
] | We engineer compact SU(5) Grand Unified Theories in F-theory in which GUT-breaking is achieved by a discrete Wilson line. Because the internal gauge field is flat, these models avoid the high scale threshold corrections associated with hypercharge flux. Along the way, we exemplify the `local-to-global' approach in F-th... | 12.626995 | 12.703157 | 13.137769 | 12.35477 | 13.637287 | 12.398275 | 12.210401 | 12.563396 | 12.298478 | 13.919014 | 11.639368 | 11.893644 | 13.162196 | 12.019506 | 11.891449 | 11.900911 | 12.07016 | 12.022776 | 11.998303 | 13.066773 | 11.640059 |
1611.06177 | Johannes Walcher | Richard Eager, Sam Alexandre Selmani and Johannes Walcher | Exponential Networks and Representations of Quivers | 82 pages, 60 figures, typos fixed | null | 10.1007/JHEP08(2017)063 | null | hep-th math.AG math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the geometric description of BPS states in supersymmetric theories
with eight supercharges in terms of geodesic networks on suitable spectral
curves. We lift and extend several constructions of Gaiotto-Moore-Neitzke from
gauge theory to local Calabi-Yau threefolds and related models. The
differential is mult... | [
{
"created": "Fri, 18 Nov 2016 17:54:03 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Jul 2017 10:55:03 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Eager",
"Richard",
""
],
[
"Selmani",
"Sam Alexandre",
""
],
[
"Walcher",
"Johannes",
""
]
] | We study the geometric description of BPS states in supersymmetric theories with eight supercharges in terms of geodesic networks on suitable spectral curves. We lift and extend several constructions of Gaiotto-Moore-Neitzke from gauge theory to local Calabi-Yau threefolds and related models. The differential is multi-... | 13.757748 | 13.736344 | 16.643574 | 13.956726 | 14.972445 | 14.890891 | 13.776299 | 13.725986 | 14.282541 | 17.23064 | 13.383965 | 13.442823 | 15.141231 | 13.524723 | 13.250438 | 13.472124 | 13.268271 | 13.916777 | 13.226873 | 14.340926 | 13.26817 |
1711.00864 | Federico Carta | T. Daniel Brennan, Federico Carta, Cumrun Vafa | The String Landscape, the Swampland, and the Missing Corner | null | null | null | IFT-UAM/CSIC-17-105 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a brief overview of the string landscape and techniques used to
construct string compactifications. We then explain how this motivates the
notion of the swampland and review a number of conjectures that attempt to
characterize theories in the swampland. We also compare holography in the
context of superstring... | [
{
"created": "Thu, 2 Nov 2017 18:00:26 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Nov 2017 17:12:37 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Jun 2018 01:11:37 GMT",
"version": "v3"
}
] | 2018-06-28 | [
[
"Brennan",
"T. Daniel",
""
],
[
"Carta",
"Federico",
""
],
[
"Vafa",
"Cumrun",
""
]
] | We give a brief overview of the string landscape and techniques used to construct string compactifications. We then explain how this motivates the notion of the swampland and review a number of conjectures that attempt to characterize theories in the swampland. We also compare holography in the context of superstrings ... | 10.926332 | 11.921117 | 11.856292 | 11.551323 | 12.474846 | 12.985449 | 12.588449 | 12.280109 | 11.511141 | 12.990233 | 11.291281 | 11.471819 | 11.406381 | 11.110913 | 10.989167 | 10.772368 | 11.045851 | 11.119077 | 11.348496 | 11.170003 | 10.941521 |
1711.07990 | Orestis Loukas | Orestis Loukas | A matrix CFT at multiple large charges | 1+36 pages, 2 figures, minor clarifications added, version to be
published in JHEP | null | 10.1007/JHEP06(2018)164 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate matrix models in three dimensions where the global
$\text{SU}(N)$ symmetry acts via the adjoint map. Analyzing their ground state
which is homogeneous in space and can carry either a unique or multiple fixed
charges, we show the existence of at least two distinct fixed points of the
renormalization gro... | [
{
"created": "Tue, 21 Nov 2017 19:00:15 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Jun 2018 05:14:32 GMT",
"version": "v2"
}
] | 2018-08-01 | [
[
"Loukas",
"Orestis",
""
]
] | We investigate matrix models in three dimensions where the global $\text{SU}(N)$ symmetry acts via the adjoint map. Analyzing their ground state which is homogeneous in space and can carry either a unique or multiple fixed charges, we show the existence of at least two distinct fixed points of the renormalization group... | 16.834993 | 16.898563 | 17.453444 | 16.157433 | 16.472626 | 15.55461 | 17.89155 | 15.960975 | 15.106698 | 18.651884 | 17.168417 | 17.404732 | 17.109812 | 16.289875 | 16.812695 | 16.352413 | 16.807083 | 16.433218 | 16.554884 | 17.589632 | 16.27734 |
1112.0409 | Peter Horvathy | P-M. Zhang and P. A. Horvathy | Chiral decomposition in the non-commutative Landau problem | 23 pages, 22 figures, in press in Annals of Physics | null | 10.1016/j.aop.2012.02.014 | null | hep-th cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The decomposition of the non-commutative Landau (NCL) system into two
uncoupled one-dimensional chiral components, advocated by Alvarez, Gomis,
Kamimura and Plyushchay [1], is generalized to nonvanishing electric fields.
This allows us to discuss the main properties of the NCL problem including its
exotic Newton-Hook... | [
{
"created": "Fri, 2 Dec 2011 09:34:12 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Mar 2012 10:29:30 GMT",
"version": "v2"
}
] | 2012-03-14 | [
[
"Zhang",
"P-M.",
""
],
[
"Horvathy",
"P. A.",
""
]
] | The decomposition of the non-commutative Landau (NCL) system into two uncoupled one-dimensional chiral components, advocated by Alvarez, Gomis, Kamimura and Plyushchay [1], is generalized to nonvanishing electric fields. This allows us to discuss the main properties of the NCL problem including its exotic Newton-Hooke ... | 10.612247 | 11.364797 | 15.119168 | 11.064841 | 11.327933 | 10.61577 | 12.358211 | 11.546794 | 9.959471 | 13.196139 | 10.458923 | 9.885481 | 9.945869 | 9.942938 | 9.745317 | 9.576808 | 9.668295 | 9.361706 | 10.125367 | 10.271361 | 9.717055 |
hep-th/9612080 | John Schwarz | Mina Aganagic, Costin Popescu, and John H. Schwarz | Gauge-Invariant and Gauge-Fixed D-Brane Actions | 33 pages, latex, no figures; revised as requested by referee | Nucl.Phys. B495 (1997) 99-126 | 10.1016/S0550-3213(97)00180-6 | CALT-68-2088 | hep-th | null | The first part of this paper presents actions for Dirichlet p-branes embedded
in a flat 10-dimensional space-time. The fields of the (p+1)-dimensional
world-volume theories are the 10d space-time coordinates $ X^m$, a pair of
Majorana-Weyl spinors $\theta_1$ and $\theta_2$, and a U(1) gauge field
$A_{\mu}$. The N = 2... | [
{
"created": "Sat, 7 Dec 1996 23:11:03 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Dec 1996 19:18:29 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Feb 1997 21:58:26 GMT",
"version": "v3"
}
] | 2016-09-06 | [
[
"Aganagic",
"Mina",
""
],
[
"Popescu",
"Costin",
""
],
[
"Schwarz",
"John H.",
""
]
] | The first part of this paper presents actions for Dirichlet p-branes embedded in a flat 10-dimensional space-time. The fields of the (p+1)-dimensional world-volume theories are the 10d space-time coordinates $ X^m$, a pair of Majorana-Weyl spinors $\theta_1$ and $\theta_2$, and a U(1) gauge field $A_{\mu}$. The N = 2A ... | 5.129534 | 5.050637 | 5.185791 | 4.818656 | 5.060591 | 4.878992 | 4.864135 | 4.844823 | 4.708466 | 5.415101 | 4.676133 | 4.759621 | 4.913008 | 4.670173 | 4.714381 | 4.73423 | 4.73558 | 4.724426 | 4.745182 | 4.92688 | 4.709439 |
0907.1364 | Sannino Francesco | Francesco Sannino (CP3-Origins) | QCD Dual | RevTeX, 13 pages. Added discussion on operator matching and flavor
decoupling. Version to match the published one | Phys.Rev.D80:065011,2009 | 10.1103/PhysRevD.80.065011 | CP3-Origins:2009-6 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We uncover a novel solution of the 't Hooft anomaly matching conditions for
QCD. Interestingly in the perturbative regime the new gauge theory, if
interpreted as a possible QCD dual, predicts the critical number of flavors
above which QCD in the nonperturbative regime, develops an infrared stable
fixed point. Remarka... | [
{
"created": "Thu, 9 Jul 2009 06:48:39 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Jul 2009 10:02:30 GMT",
"version": "v2"
},
{
"created": "Tue, 18 Aug 2009 20:21:13 GMT",
"version": "v3"
}
] | 2009-09-25 | [
[
"Sannino",
"Francesco",
"",
"CP3-Origins"
]
] | We uncover a novel solution of the 't Hooft anomaly matching conditions for QCD. Interestingly in the perturbative regime the new gauge theory, if interpreted as a possible QCD dual, predicts the critical number of flavors above which QCD in the nonperturbative regime, develops an infrared stable fixed point. Remarkabl... | 12.873502 | 11.986846 | 12.608149 | 11.231273 | 14.281234 | 12.773557 | 12.56881 | 11.726714 | 11.219024 | 12.204126 | 11.09507 | 11.699812 | 12.174405 | 11.576402 | 11.871583 | 11.877232 | 12.016391 | 11.600217 | 11.245458 | 11.815701 | 11.18395 |
2305.15664 | Wagner Oliveira dos Santos | W. Oliveira dos Santos, E. R. Bezerra de Mello | Vacuum polarization induced by a cosmic string and a brane in AdS
spacetime | 23 pages, 4 figures; Version accepted for publication in EPJC | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate the vacuum polarization effects associated to a
charged quantum massive scalar field on a $(D+1)$-dimensional anti-de Sitter
background induced by a magnetic-flux-carrying cosmic string in the braneworld
model context. We consider the brane parallel to the anti-de Sitter boundary
and the ... | [
{
"created": "Thu, 25 May 2023 02:23:39 GMT",
"version": "v1"
},
{
"created": "Wed, 31 May 2023 07:05:02 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Aug 2023 04:01:07 GMT",
"version": "v3"
}
] | 2023-08-03 | [
[
"Santos",
"W. Oliveira dos",
""
],
[
"de Mello",
"E. R. Bezerra",
""
]
] | In this paper we investigate the vacuum polarization effects associated to a charged quantum massive scalar field on a $(D+1)$-dimensional anti-de Sitter background induced by a magnetic-flux-carrying cosmic string in the braneworld model context. We consider the brane parallel to the anti-de Sitter boundary and the co... | 5.200623 | 3.627765 | 5.410918 | 4.29139 | 4.470187 | 4.041562 | 4.204526 | 4.037918 | 4.082289 | 5.421573 | 4.141701 | 4.638288 | 5.08229 | 4.784235 | 4.718574 | 4.698332 | 4.693381 | 4.680744 | 4.72944 | 5.215989 | 4.811491 |
hep-th/0203194 | Matej Pavsic | C. Castro and M. Pavsic | Clifford Algebra of Spacetime and the Conformal Group | 15 pages; published version of the paper | Int.J.Theor.Phys. 42 (2003) 1693-1705 | null | null | hep-th gr-qc | null | We demonstrate the emergence of the conformal group SO(4,2) from the Clifford
algebra of spacetime. The latter algebra is a manifold, called Clifford space,
which is assumed to be the arena in which physics takes place. A Clifford space
does not contain only points (events), but also lines, surfaces, volumes,
etc...,... | [
{
"created": "Thu, 21 Mar 2002 08:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Nov 2003 09:21:37 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Castro",
"C.",
""
],
[
"Pavsic",
"M.",
""
]
] | We demonstrate the emergence of the conformal group SO(4,2) from the Clifford algebra of spacetime. The latter algebra is a manifold, called Clifford space, which is assumed to be the arena in which physics takes place. A Clifford space does not contain only points (events), but also lines, surfaces, volumes, etc..., a... | 9.641046 | 10.289621 | 10.476576 | 9.414059 | 9.775844 | 10.486741 | 9.258242 | 9.965197 | 9.369349 | 11.059813 | 9.577502 | 9.627662 | 9.680243 | 9.469431 | 9.548264 | 9.604954 | 9.649702 | 9.556308 | 9.745579 | 9.7729 | 9.50529 |
2105.06579 | Xiao-Liang Qi | Xiao-Liang Qi | Entanglement island, miracle operators and the firewall | 21 pages, 7 figures, final published version | J. High Energ. Phys. 2022, 85 (2022) | 10.1007/JHEP01(2022)085 | null | hep-th gr-qc quant-ph | http://creativecommons.org/licenses/by-nc-nd/4.0/ | In this paper, we obtain some general results on information retrieval from
the black hole interior, based on the recent progress on quantum extremal
surface formula and entanglement island. We study an AdS black hole coupled to
a bath with generic dynamics, and ask whether it is possible to retrieve
information abou... | [
{
"created": "Thu, 13 May 2021 22:59:45 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Feb 2022 03:58:22 GMT",
"version": "v2"
}
] | 2022-02-03 | [
[
"Qi",
"Xiao-Liang",
""
]
] | In this paper, we obtain some general results on information retrieval from the black hole interior, based on the recent progress on quantum extremal surface formula and entanglement island. We study an AdS black hole coupled to a bath with generic dynamics, and ask whether it is possible to retrieve information about ... | 13.175866 | 13.990047 | 15.004465 | 13.164449 | 13.657167 | 13.934586 | 13.172875 | 13.64735 | 13.064898 | 15.168453 | 13.619357 | 12.596512 | 13.681904 | 12.528539 | 13.083165 | 12.686333 | 13.503419 | 12.778634 | 12.660972 | 13.404771 | 12.868281 |
1812.06059 | Wei Li | Ling-Yan Hung, Wei Li and Charles M. Melby-Thompson | Wilson line networks in $p$-adic AdS/CFT | 34 pages, 5 figures; v2: typos corrected, published version | JHEP05(2019)118 | 10.1007/JHEP05(2019)118 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The $p$-adic AdS/CFT is a holographic duality based on the $p$-adic number
field $\mathbb{Q}_p$. For a $p$-adic CFT living on $\mathbb{Q}_p$ and with
complex-valued fields, the bulk theory is defined on the Bruhat-Tits tree,
which can be viewed as the bulk dual of $\mathbb{Q}_p$. We propose that bulk
theory can be fo... | [
{
"created": "Fri, 14 Dec 2018 18:15:18 GMT",
"version": "v1"
},
{
"created": "Wed, 22 May 2019 09:41:40 GMT",
"version": "v2"
}
] | 2019-06-26 | [
[
"Hung",
"Ling-Yan",
""
],
[
"Li",
"Wei",
""
],
[
"Melby-Thompson",
"Charles M.",
""
]
] | The $p$-adic AdS/CFT is a holographic duality based on the $p$-adic number field $\mathbb{Q}_p$. For a $p$-adic CFT living on $\mathbb{Q}_p$ and with complex-valued fields, the bulk theory is defined on the Bruhat-Tits tree, which can be viewed as the bulk dual of $\mathbb{Q}_p$. We propose that bulk theory can be form... | 4.17373 | 3.6747 | 4.30938 | 3.597099 | 3.578129 | 3.852517 | 3.720539 | 3.71528 | 3.779685 | 4.457166 | 3.715944 | 3.864619 | 4.303839 | 3.86367 | 3.887592 | 3.893821 | 3.851884 | 3.793844 | 3.843223 | 4.20712 | 3.869743 |
2001.05129 | Jiang Long | Jiang Long | Logarithmic behaviour of connected correlation function in CFT | 41 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $(m)$-type connected correlation functions of OPE blocks with
respect to one spatial region in two dimensional conformal field theory. We
find logarithmic divergence for these correlation functions. We justify the
logarithmic behaviour from three different approaches: massless free scalar
theory, Selberg int... | [
{
"created": "Wed, 15 Jan 2020 04:28:02 GMT",
"version": "v1"
}
] | 2020-01-16 | [
[
"Long",
"Jiang",
""
]
] | We study $(m)$-type connected correlation functions of OPE blocks with respect to one spatial region in two dimensional conformal field theory. We find logarithmic divergence for these correlation functions. We justify the logarithmic behaviour from three different approaches: massless free scalar theory, Selberg integ... | 20.013863 | 18.36186 | 20.182461 | 17.75658 | 17.553263 | 19.093386 | 19.804098 | 16.382174 | 17.771578 | 21.632757 | 18.076759 | 17.810686 | 19.883572 | 18.27422 | 18.394838 | 18.475574 | 19.053833 | 18.504803 | 17.698956 | 20.750984 | 18.551115 |
1910.09406 | Hongfei Shu | Katsushi Ito and Hongfei Shu | TBA equations for the Schr\"odinger equation with a regular singularity | 39 pages, typos corrected | J.Phys.A 53 (2020) 33, 335201 | 10.1088/1751-8121/ab96ee | TIT/HEP-676, NORDITA 2019-092 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the Thermodynamic Bethe Ansatz (TBA) equations for the
Schr\"odinger equation with an arbitrary polynomial potential and a regular
singular (simple and double pole) term. The TBA equations provide a non-trivial
generalization of the ODE/IM correspondence and also give a solution for the
Riemann-Hilbert prob... | [
{
"created": "Mon, 21 Oct 2019 14:31:46 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Feb 2020 15:45:40 GMT",
"version": "v2"
}
] | 2021-01-08 | [
[
"Ito",
"Katsushi",
""
],
[
"Shu",
"Hongfei",
""
]
] | We derive the Thermodynamic Bethe Ansatz (TBA) equations for the Schr\"odinger equation with an arbitrary polynomial potential and a regular singular (simple and double pole) term. The TBA equations provide a non-trivial generalization of the ODE/IM correspondence and also give a solution for the Riemann-Hilbert proble... | 8.249694 | 7.560442 | 9.361679 | 7.558752 | 8.476561 | 8.796872 | 8.127921 | 7.50283 | 7.670682 | 9.313705 | 7.866204 | 8.074389 | 7.924708 | 8.002701 | 7.83428 | 7.959824 | 7.853273 | 7.590355 | 7.897925 | 8.099664 | 7.684084 |
hep-th/9402057 | null | Dongsu Bak, R. Jackiw and So-Young Pi | Non-Abelian Chern-Simons Particles and their Quantization | 18 pages, MIT preprint CTP # 2276 | Phys.Rev.D49:6778-6786,1994 | 10.1103/PhysRevD.49.6778 | null | hep-th | null | A many--body Schr\"odinger equation for non--Abelian Chern--Simons particles
is obtained from both point--particle and field--theoretic pictures. We present
a particle Lagrangian and a field theoretic Lagrange density, and discuss their
properties. Both are quantized by the symplectic method of Hamiltonian
reduction.... | [
{
"created": "Wed, 9 Feb 1994 23:42:00 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Bak",
"Dongsu",
""
],
[
"Jackiw",
"R.",
""
],
[
"Pi",
"So-Young",
""
]
] | A many--body Schr\"odinger equation for non--Abelian Chern--Simons particles is obtained from both point--particle and field--theoretic pictures. We present a particle Lagrangian and a field theoretic Lagrange density, and discuss their properties. Both are quantized by the symplectic method of Hamiltonian reduction. A... | 9.085906 | 8.550993 | 9.5404 | 8.117667 | 8.648059 | 8.341251 | 8.463687 | 8.135047 | 8.215175 | 9.194341 | 8.315923 | 7.99272 | 8.353869 | 7.8576 | 7.970417 | 7.949878 | 7.846758 | 8.155639 | 7.911778 | 8.076561 | 7.90984 |
hep-th/9806089 | Miguel Ortiz | M. Banados and M. Ortiz | The central charge in three dimensional anti-de Sitter space | 9 pages, Latex | Class.Quant.Grav. 16 (1999) 1733-1736 | 10.1088/0264-9381/16/6/307 | null | hep-th | null | This paper collects the various ways of computing the central charge
$c=3l/2G$ arising in 3d asymptotically anti-de Sitter spaces, in the
Chern-Simons formulation. Their similarities and differences are displayed.
| [
{
"created": "Thu, 11 Jun 1998 15:42:44 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Banados",
"M.",
""
],
[
"Ortiz",
"M.",
""
]
] | This paper collects the various ways of computing the central charge $c=3l/2G$ arising in 3d asymptotically anti-de Sitter spaces, in the Chern-Simons formulation. Their similarities and differences are displayed. | 15.191228 | 10.394147 | 13.009531 | 12.337899 | 11.125314 | 9.73638 | 12.620482 | 10.382258 | 11.302859 | 12.068344 | 12.732956 | 11.81676 | 11.872075 | 11.803749 | 11.937003 | 11.450057 | 12.255633 | 11.44374 | 12.377093 | 11.304908 | 11.885579 |
hep-th/9509119 | Krzysztof Pilch | Peter Bouwknegt, Jim McCarthy and Krzysztof Pilch | The W_3 algebra: modules, semi-infinite cohomology and BV-algebras | 144 pages; 23 uuencoded ps figures; uses macros tables.tex, epsf and
amssym.def (version 2.1 or later) | Lect.Notes Phys.M42:1-204,1996 | 10.1007/978-3-540-68719-1 | ADP-95-46/M38, USC-95/18 | hep-th math.QA q-alg | null | The noncritical $D=4$ $W_3$ string is a model of $W_3$ gravity coupled to two
free scalar fields. In this paper we discuss its BRST quantization in direct
analogy with that of the $D=2$ (Virasoro) string. In particular, we calculate
the physical spectrum as a problem in BRST cohomology. The corresponding
operator coh... | [
{
"created": "Fri, 22 Sep 1995 05:12:31 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bouwknegt",
"Peter",
""
],
[
"McCarthy",
"Jim",
""
],
[
"Pilch",
"Krzysztof",
""
]
] | The noncritical $D=4$ $W_3$ string is a model of $W_3$ gravity coupled to two free scalar fields. In this paper we discuss its BRST quantization in direct analogy with that of the $D=2$ (Virasoro) string. In particular, we calculate the physical spectrum as a problem in BRST cohomology. The corresponding operator cohom... | 8.50163 | 6.931109 | 9.331445 | 7.324026 | 8.930785 | 9.068128 | 8.374323 | 7.25075 | 7.691262 | 11.190077 | 7.204574 | 7.612991 | 9.143426 | 7.840042 | 8.25641 | 7.968378 | 8.157926 | 7.957993 | 8.018626 | 9.053414 | 7.820632 |
2207.04970 | Jung-Wook Kim | Jung-Wook Kim | Quantum corrections to frame-dragging in scattering amplitudes | accepted version for publication in Phys.Rev.D; discussion on the
equivalence principle has been changed to a more conservative tone; 7 pages,
1 TikZ figure, 1 ancillary file | Phys. Rev. D 106, L081901 (2022) | 10.1103/PhysRevD.106.L081901 | QMUL-PH-22-20 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Frame-dragging effect manifests itself as polarization direction rotation
when linearly polarized electromagnetic/gravitational wave scatters from a
spinning point source through gravitational interactions, an effect also known
as the gravitational Faraday rotation. Treating general relativity as an
effective field t... | [
{
"created": "Mon, 11 Jul 2022 15:50:29 GMT",
"version": "v1"
},
{
"created": "Sat, 16 Jul 2022 15:03:34 GMT",
"version": "v2"
},
{
"created": "Wed, 12 Oct 2022 08:05:16 GMT",
"version": "v3"
}
] | 2022-10-21 | [
[
"Kim",
"Jung-Wook",
""
]
] | Frame-dragging effect manifests itself as polarization direction rotation when linearly polarized electromagnetic/gravitational wave scatters from a spinning point source through gravitational interactions, an effect also known as the gravitational Faraday rotation. Treating general relativity as an effective field the... | 11.189845 | 12.209649 | 10.273959 | 11.057723 | 11.259777 | 11.130673 | 11.674581 | 10.446266 | 10.184136 | 10.770412 | 9.448167 | 9.464292 | 9.76673 | 10.142602 | 10.288047 | 10.004519 | 9.535481 | 9.817994 | 9.99611 | 10.134618 | 10.182702 |
0808.3062 | Ricardo Machado de Amorim | Ricardo Amorim | Dynamical symmetries in noncommutative theories | 20 pages, Latex. Some changes in the text. Version accepted for
publication in Physical Review D | Phys.Rev.D78:105003,2008 | 10.1103/PhysRevD.78.105003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present work we study dynamical space-time symmetries in
noncommutative relativistic theories by using the minimal canonical extension
of the Doplicher, Fredenhagen and Roberts algebra. Our formalism is constructed
in an extended space-time with independent degrees of freedom associated with
the object of nonc... | [
{
"created": "Fri, 22 Aug 2008 11:55:32 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Aug 2008 13:34:05 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Sep 2008 20:19:42 GMT",
"version": "v3"
},
{
"created": "Fri, 17 Oct 2008 16:57:12 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Amorim",
"Ricardo",
""
]
] | In the present work we study dynamical space-time symmetries in noncommutative relativistic theories by using the minimal canonical extension of the Doplicher, Fredenhagen and Roberts algebra. Our formalism is constructed in an extended space-time with independent degrees of freedom associated with the object of noncom... | 9.001615 | 8.211681 | 9.744433 | 8.111115 | 8.735362 | 7.590699 | 8.062745 | 8.318466 | 8.344844 | 9.560225 | 8.104429 | 7.866714 | 8.448806 | 7.969788 | 8.526541 | 8.103147 | 8.030953 | 8.181467 | 8.17329 | 8.461266 | 8.038857 |
hep-th/9610020 | Atsushi Okazaki | Koji Harada, Atsushi Okazaki | Perturbative Tamm-Dancoff Renormalization | 20 pages, RevTeX, 10 figures | Phys.Rev. D55 (1997) 6198-6208 | 10.1103/PhysRevD.55.6198 | KYUSHU-HET 35 | hep-th | null | A new two-step renormalization procedure is proposed. In the first step, the
effects of high-energy states are considered in the conventional (Feynman)
perturbation theory. In the second step, the coupling to many-body states is
eliminated by a similarity transformation. The resultant effective Hamiltonian
contains o... | [
{
"created": "Thu, 3 Oct 1996 12:07:16 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Harada",
"Koji",
""
],
[
"Okazaki",
"Atsushi",
""
]
] | A new two-step renormalization procedure is proposed. In the first step, the effects of high-energy states are considered in the conventional (Feynman) perturbation theory. In the second step, the coupling to many-body states is eliminated by a similarity transformation. The resultant effective Hamiltonian contains onl... | 9.028996 | 9.396519 | 8.594129 | 8.126381 | 8.174992 | 9.040965 | 8.656633 | 9.148669 | 8.807301 | 8.650797 | 8.583582 | 8.599319 | 8.410722 | 8.362012 | 8.36359 | 8.307692 | 8.496391 | 8.752304 | 8.491611 | 8.390833 | 8.567651 |
1601.07954 | Vakhid Gani | Vakhid A. Gani, Mariya A. Lizunova, Roman V. Radomskiy | Scalar triplet on a domain wall: an exact solution | 14 pages, 4 figures; v2: typos corrected, references added, minor
changes to match version published in JHEP | JHEP 04 (2016) 043 | 10.1007/JHEP04(2016)043 | null | hep-th math-ph math.MP nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a model with a real scalar Higgs field and a scalar triplet field
that allows existence of a topological defect -- a domain wall. The wall breaks
the global $O(3)$ symmetry of the model, which gives rise to non-Abelian
orientational degrees of freedom. We found an exact analytic solution that
describes a dom... | [
{
"created": "Fri, 29 Jan 2016 00:21:23 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Apr 2016 13:12:56 GMT",
"version": "v2"
}
] | 2016-12-02 | [
[
"Gani",
"Vakhid A.",
""
],
[
"Lizunova",
"Mariya A.",
""
],
[
"Radomskiy",
"Roman V.",
""
]
] | We study a model with a real scalar Higgs field and a scalar triplet field that allows existence of a topological defect -- a domain wall. The wall breaks the global $O(3)$ symmetry of the model, which gives rise to non-Abelian orientational degrees of freedom. We found an exact analytic solution that describes a domai... | 8.633689 | 7.359852 | 8.459583 | 7.769709 | 8.247548 | 7.653211 | 7.967183 | 7.59206 | 7.599536 | 8.988449 | 7.486093 | 7.708004 | 8.296758 | 7.908294 | 7.825699 | 7.948504 | 7.78272 | 7.733685 | 7.673665 | 8.061295 | 7.651009 |
1606.00940 | Fabricio Augusto Barone Rangel PhD | L. H. C. Borges, A. F. Ferrari, F. A. Barone | New effects in the interaction between electromagnetic sources mediated
by nonminimal Lorentz violating interactions | 17 Latex pages | Eur. Phys. J. C, v. 76, p. 599, 2016 | 10.1140/epjc/s10052-016-4460-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper is dedicated to the study of interactions between external sources
for the electromagnetic field in a Lorentz symmetry breaking scenario. We focus
on a particular higher derivative, Lorentz violating interaction that arises
from a specific model that was argued to lead to interesting effects in the low
ene... | [
{
"created": "Fri, 3 Jun 2016 01:14:23 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Nov 2016 05:10:02 GMT",
"version": "v2"
}
] | 2016-11-17 | [
[
"Borges",
"L. H. C.",
""
],
[
"Ferrari",
"A. F.",
""
],
[
"Barone",
"F. A.",
""
]
] | This paper is dedicated to the study of interactions between external sources for the electromagnetic field in a Lorentz symmetry breaking scenario. We focus on a particular higher derivative, Lorentz violating interaction that arises from a specific model that was argued to lead to interesting effects in the low energ... | 10.593455 | 9.818195 | 10.511691 | 9.443613 | 9.629486 | 9.981761 | 10.399106 | 10.299987 | 9.553603 | 10.745355 | 10.283164 | 10.06501 | 10.158141 | 9.912747 | 10.163684 | 9.892623 | 10.112919 | 9.915705 | 10.132188 | 10.315713 | 9.822433 |
1509.00027 | Ioannis Florakis | Carlo Angelantonj, Ioannis Florakis, Mirian Tsulaia | Generalised universality of gauge thresholds in heterotic vacua with and
without supersymmetry | 33 pages | Nucl. Phys. B:900, 170-197, 2015 | 10.1016/j.nuclphysb.2015.09.007 | CERN-PH-TH-2015-211 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study one-loop quantum corrections to gauge couplings in heterotic vacua
with spontaneous supersymmetry breaking. Although in non-supersymmetric
constructions these corrections are not protected and are typically model
dependent, we show how a universal behaviour of threshold differences, typical
of supersymmetric... | [
{
"created": "Mon, 31 Aug 2015 20:18:01 GMT",
"version": "v1"
}
] | 2015-10-28 | [
[
"Angelantonj",
"Carlo",
""
],
[
"Florakis",
"Ioannis",
""
],
[
"Tsulaia",
"Mirian",
""
]
] | We study one-loop quantum corrections to gauge couplings in heterotic vacua with spontaneous supersymmetry breaking. Although in non-supersymmetric constructions these corrections are not protected and are typically model dependent, we show how a universal behaviour of threshold differences, typical of supersymmetric v... | 10.910813 | 11.508536 | 14.438549 | 11.100102 | 11.088804 | 11.774318 | 12.188519 | 11.880112 | 11.767697 | 14.235713 | 11.086058 | 11.277269 | 12.27094 | 11.306962 | 11.134188 | 11.236333 | 11.284461 | 11.111013 | 11.126039 | 12.3332 | 10.913641 |
1506.05379 | Alexander Krikun | Alexander Krikun | Phases of holographic d-wave superconductor | 18 pages, 7 figures | null | null | NORDITA-2015-71 | hep-th cond-mat.str-el cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study different phases in the holographic model of d-wave superconductor.
These are described by solutions to the classical equations of motion found in
different ansatze. Apart from the known homogeneous d-wave superconducting
phase we find three new solutions. Two of them represent two distinct families
of the s... | [
{
"created": "Wed, 17 Jun 2015 16:24:06 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Krikun",
"Alexander",
""
]
] | We study different phases in the holographic model of d-wave superconductor. These are described by solutions to the classical equations of motion found in different ansatze. Apart from the known homogeneous d-wave superconducting phase we find three new solutions. Two of them represent two distinct families of the spa... | 10.915725 | 11.699254 | 11.965899 | 10.097637 | 12.732081 | 11.624645 | 12.15395 | 10.199803 | 11.402887 | 11.259168 | 10.490498 | 10.858107 | 11.250051 | 10.686924 | 10.86094 | 10.601942 | 10.79283 | 10.597359 | 10.926409 | 11.09826 | 10.36977 |
hep-th/0306113 | Massimo Giovannini | M. Gasperini, M. Giovannini, G. Veneziano | Perturbations in a non-singular bouncing Universe | 14 pages in Latex style, 5 included figures | Phys.Lett. B569 (2003) 113-122 | 10.1016/j.physletb.2003.07.028 | CERN-TH/2003-128, BA-TH/03-463 | hep-th astro-ph gr-qc hep-ph | null | We complement the low-energy gravi-dilaton effective action of string theory
with a non-local, general-covariant dilaton potential, and obtain homogeneous
solutions describing a non-singular (bouncing-curvature) cosmology. We then
compute, both analytically and numerically, the spectrum of amplified scalar
and tensor... | [
{
"created": "Thu, 12 Jun 2003 15:29:55 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Gasperini",
"M.",
""
],
[
"Giovannini",
"M.",
""
],
[
"Veneziano",
"G.",
""
]
] | We complement the low-energy gravi-dilaton effective action of string theory with a non-local, general-covariant dilaton potential, and obtain homogeneous solutions describing a non-singular (bouncing-curvature) cosmology. We then compute, both analytically and numerically, the spectrum of amplified scalar and tensor p... | 11.2572 | 9.747779 | 10.439873 | 9.139162 | 9.41855 | 8.744156 | 9.691978 | 9.105758 | 9.741717 | 10.243807 | 9.20545 | 9.537936 | 9.967086 | 9.375587 | 9.500031 | 9.739532 | 9.319237 | 9.644069 | 9.544497 | 10.247004 | 9.443629 |
hep-th/0401057 | Didina Serban | D. Serban and M. Staudacher | Planar N=4 gauge theory and the Inozemtsev long range spin chain | 31 pages, no figure; v1: one reference added, minor changes; v2:
slightly extended discussion of rapidity, references added | JHEP 0406 (2004) 001 | 10.1088/1126-6708/2004/06/001 | AEI-2004-001, SPhT-T04/002 | hep-th | null | We investigate whether the (planar, two complex scalar) dilatation operator
of N=4 gauge theory can be, perturbatively and, perhaps, non-perturbatively,
described by an integrable long range spin chain with elliptic exchange
interaction. Such a chain was introduced some time ago by Inozemtsev. In the
limit of suffici... | [
{
"created": "Fri, 9 Jan 2004 20:30:04 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Feb 2004 14:47:43 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Apr 2004 16:53:34 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Serban",
"D.",
""
],
[
"Staudacher",
"M.",
""
]
] | We investigate whether the (planar, two complex scalar) dilatation operator of N=4 gauge theory can be, perturbatively and, perhaps, non-perturbatively, described by an integrable long range spin chain with elliptic exchange interaction. Such a chain was introduced some time ago by Inozemtsev. In the limit of sufficien... | 8.870222 | 8.907723 | 10.066004 | 8.386379 | 9.318176 | 8.853259 | 8.732882 | 8.38414 | 8.659553 | 9.801805 | 8.538317 | 8.659388 | 8.828305 | 8.463862 | 8.592311 | 8.692428 | 8.54856 | 8.490655 | 8.466146 | 8.598042 | 8.404692 |
0911.4654 | Troels Harmark | Jay Armas and Troels Harmark | Uniqueness Theorem for Black Hole Space-Times with Multiple Disconnected
Horizons | 28 pages, 5 figures. v3: Further improvements on uniqueness theorem,
Lemma introduced for clarity of derivation, new quantities introduced to
treat special case with zero flux, refs. added, typos fixed | JHEP 1005:093,2010 | 10.1007/JHEP05(2010)093 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show uniqueness of stationary and asymptotically flat black hole
space-times with multiple disconnected horizons and with two rotational Killing
vector fields in the context of five-dimensional minimal supergravity
(Einstein-Maxwell-Chern-Simons gravity). The novelty in this work is the
introduction in the uniquen... | [
{
"created": "Tue, 24 Nov 2009 15:43:35 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Dec 2009 11:15:58 GMT",
"version": "v2"
},
{
"created": "Tue, 25 May 2010 13:20:22 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Armas",
"Jay",
""
],
[
"Harmark",
"Troels",
""
]
] | We show uniqueness of stationary and asymptotically flat black hole space-times with multiple disconnected horizons and with two rotational Killing vector fields in the context of five-dimensional minimal supergravity (Einstein-Maxwell-Chern-Simons gravity). The novelty in this work is the introduction in the uniquenes... | 13.064563 | 12.0811 | 12.992637 | 11.214089 | 11.546166 | 11.64271 | 12.970808 | 12.596937 | 11.714533 | 13.310046 | 11.423869 | 11.829158 | 12.032526 | 11.716698 | 11.956662 | 11.792909 | 11.88161 | 11.841934 | 12.006454 | 12.963681 | 11.999748 |
2007.03866 | Min-Seok Seo | Min-Seok Seo | Eternal inflation in light of Wheeler-DeWitt equation | 22 pages, version published in JCAP | JCAP 11 (2020) 007 | 10.1088/1475-7516/2020/11/007 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Wheeler-DeWitt equation provides the probability distribution for the
curvature perturbation, the gauge invariant quantum fluctuation of the
inflaton. From this, we can find a tower of power spectra which is not found in
a perturbative approach. Since the power spectrum for the modes that cross the
horizon contri... | [
{
"created": "Wed, 8 Jul 2020 02:50:16 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Nov 2020 00:00:21 GMT",
"version": "v2"
}
] | 2020-11-09 | [
[
"Seo",
"Min-Seok",
""
]
] | The Wheeler-DeWitt equation provides the probability distribution for the curvature perturbation, the gauge invariant quantum fluctuation of the inflaton. From this, we can find a tower of power spectra which is not found in a perturbative approach. Since the power spectrum for the modes that cross the horizon contribu... | 10.747387 | 11.172964 | 10.761167 | 10.287855 | 10.655419 | 10.613903 | 10.846203 | 11.033053 | 10.945827 | 11.380981 | 10.294529 | 10.276971 | 10.077696 | 10.152158 | 10.337731 | 10.339223 | 10.205001 | 10.234779 | 10.316537 | 10.227534 | 9.952892 |
1912.09450 | Aaron Hillman | Aaron Hillman | Symbol Recursion for the dS Wave Function | null | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a recursive rule for the symbol of perturbative contributions to
the vacuum wave function of a conformally coupled scalar in FRW cosmologies.
The rule applies exactly for a class of interactions and cosmologies, which
contains {\lambda}{\phi}^3 in dS_4, a case of particular relevance as a source
of buildin... | [
{
"created": "Thu, 19 Dec 2019 18:26:09 GMT",
"version": "v1"
}
] | 2019-12-20 | [
[
"Hillman",
"Aaron",
""
]
] | We present a recursive rule for the symbol of perturbative contributions to the vacuum wave function of a conformally coupled scalar in FRW cosmologies. The rule applies exactly for a class of interactions and cosmologies, which contains {\lambda}{\phi}^3 in dS_4, a case of particular relevance as a source of building ... | 12.958428 | 11.905295 | 15.322849 | 11.696586 | 12.423445 | 12.90589 | 13.773605 | 12.83313 | 11.085159 | 14.19332 | 10.890143 | 11.761906 | 13.601683 | 12.034413 | 11.903632 | 11.606425 | 12.079015 | 11.915879 | 11.835307 | 12.751906 | 12.011723 |
2305.09055 | Johann (Jan) Rafelski | Johann Rafelski, Jeremiah Birrell, Andrew Steinmetz, Cheng Tao Yang | A short survey of matter-antimatter evolution in the primordial universe | 52 pages, 25 figures (some double) Remo Ruffini Festschrift | MDPI Universe 2023, 9(7), 309 | 10.3390/universe9070309 | null | hep-th astro-ph.CO hep-ph | http://creativecommons.org/licenses/by/4.0/ | We offer a survey of the matter-antimatter evolution within the primordial
Universe. While the origin of the tiny matter-antimatter asymmetry has remained
one of the big questions in modern cosmology, antimatter itself has played a
large role for much of the Universe's early history. In our study of the
evolution of ... | [
{
"created": "Mon, 15 May 2023 22:37:37 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jun 2023 15:58:17 GMT",
"version": "v2"
}
] | 2023-08-15 | [
[
"Rafelski",
"Johann",
""
],
[
"Birrell",
"Jeremiah",
""
],
[
"Steinmetz",
"Andrew",
""
],
[
"Yang",
"Cheng Tao",
""
]
] | We offer a survey of the matter-antimatter evolution within the primordial Universe. While the origin of the tiny matter-antimatter asymmetry has remained one of the big questions in modern cosmology, antimatter itself has played a large role for much of the Universe's early history. In our study of the evolution of th... | 11.814237 | 13.988825 | 12.312804 | 11.68975 | 13.520377 | 13.629474 | 12.286227 | 12.383047 | 12.67618 | 12.386209 | 12.049849 | 12.01858 | 11.44327 | 11.799424 | 11.638646 | 11.721372 | 11.841141 | 11.608442 | 11.771021 | 11.806271 | 11.814065 |
hep-th/0203228 | Guillermo Raul Zemba | Henry D. Herce, Guillermo R. Zemba | A new class of Matrix Models arising from the W-infinity Algebra | 8 pages, 1 figure | Phys.Lett. B537 (2002) 141-146 | 10.1016/S0370-2693(02)01879-8 | null | hep-th cond-mat.mes-hall math-ph math.MP | null | We present a new class of hermitian one-matrix models originated in the
W-infinity algebra: more precisely, the polynomials defining the W-infinity
generators in their fermionic bilinear form are shown to expand the orthogonal
basis of a class of random hermitian matrix models. The corresponding
potentials are given,... | [
{
"created": "Mon, 25 Mar 2002 13:16:01 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Herce",
"Henry D.",
""
],
[
"Zemba",
"Guillermo R.",
""
]
] | We present a new class of hermitian one-matrix models originated in the W-infinity algebra: more precisely, the polynomials defining the W-infinity generators in their fermionic bilinear form are shown to expand the orthogonal basis of a class of random hermitian matrix models. The corresponding potentials are given, a... | 14.848801 | 15.416615 | 17.618877 | 13.479932 | 14.740133 | 13.901619 | 14.035196 | 12.432237 | 13.353917 | 15.979997 | 13.483075 | 13.085005 | 15.445211 | 13.393375 | 13.298079 | 13.733789 | 13.418344 | 13.498922 | 13.724638 | 15.005159 | 13.781772 |
hep-th/9903176 | Peter Bouwknegt | Peter Bouwknegt, Leung Chim and David Ridout | Exclusion statistics in conformal field theory and the UCPF for WZW
models | plain TeX, 31 pages; ref added | Nucl.Phys.B572:574-608,2000 | 10.1016/S0550-3213(99)00777-4 | ADP-99-12/M78 | hep-th cond-mat.stat-mech math.QA | null | In this paper we further elaborate on the notion of fractional exclusion
statistics, as introduced by Haldane, in two-dimensional conformal field
theory, and its connection to the Universal Chiral Partition Function as
defined by McCoy and collaborators. We will argue that in general, besides the
pseudo-particles int... | [
{
"created": "Sun, 21 Mar 1999 06:48:46 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Apr 1999 02:02:51 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Bouwknegt",
"Peter",
""
],
[
"Chim",
"Leung",
""
],
[
"Ridout",
"David",
""
]
] | In this paper we further elaborate on the notion of fractional exclusion statistics, as introduced by Haldane, in two-dimensional conformal field theory, and its connection to the Universal Chiral Partition Function as defined by McCoy and collaborators. We will argue that in general, besides the pseudo-particles intro... | 10.403558 | 9.54423 | 13.726324 | 10.432435 | 11.21529 | 10.572968 | 11.194394 | 9.914355 | 10.379005 | 15.039614 | 9.70989 | 8.792475 | 10.115292 | 9.666986 | 9.454815 | 9.018409 | 9.256377 | 9.576839 | 9.101892 | 10.972022 | 9.095137 |
hep-th/9403091 | Samuel Anderegg | S. Anderegg and V. Mukhanov | Path Integral Quantization of Cosmological Perturbations | 16 pages, ETH-TH/94-09 | Phys.Lett. B331 (1994) 30-38 | 10.1016/0370-2693(94)90939-3 | null | hep-th | null | We derive the first order canonical formulation of cosmological perturbation
theory in a Universe filled by a few scalar fields. This theory is quantized
via well-defined Hamiltonian path integral. The propagator which describes the
evolution of the initial (for instance, vacuum) state, is calculated.
| [
{
"created": "Wed, 16 Mar 1994 16:01:12 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Anderegg",
"S.",
""
],
[
"Mukhanov",
"V.",
""
]
] | We derive the first order canonical formulation of cosmological perturbation theory in a Universe filled by a few scalar fields. This theory is quantized via well-defined Hamiltonian path integral. The propagator which describes the evolution of the initial (for instance, vacuum) state, is calculated. | 15.260833 | 15.302762 | 13.251436 | 12.285369 | 13.966446 | 13.628489 | 14.420564 | 12.451511 | 13.147128 | 15.453952 | 13.296474 | 12.933914 | 12.992993 | 12.227825 | 12.461268 | 13.010554 | 13.23439 | 13.087021 | 12.835175 | 12.94232 | 12.564141 |
hep-th/9812202 | null | J.S.Dowker | Effective actions on the squashed three-sphere | 23 pages, JyTeX. Conclusion slightly amended, one equation and minor
misprints corrected | Class.Quant.Grav. 16 (1999) 1937-1953 | 10.1088/0264-9381/16/6/323 | Imperial/TP/98-99/27 | hep-th | null | The effective actions of a scalar and massless spin-half field are determined
as functions of the deformation of a symmetrically squashed three-sphere. The
extreme oblate case is particularly examined as pertinant to a high temperature
statistical mechanical interpretation that may be relevant for the holographic
pri... | [
{
"created": "Tue, 22 Dec 1998 13:29:44 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Jan 1999 08:50:55 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Dowker",
"J. S.",
""
]
] | The effective actions of a scalar and massless spin-half field are determined as functions of the deformation of a symmetrically squashed three-sphere. The extreme oblate case is particularly examined as pertinant to a high temperature statistical mechanical interpretation that may be relevant for the holographic princ... | 13.749513 | 12.585378 | 14.478036 | 12.70869 | 13.539977 | 13.15994 | 13.621059 | 14.404543 | 12.670692 | 14.830538 | 12.546795 | 13.508694 | 12.973854 | 13.183036 | 12.941715 | 13.089555 | 13.448051 | 12.931849 | 13.041182 | 13.468209 | 13.360254 |
hep-th/9304154 | Ashoke Sen | John H. Schwarz and Ashoke Sen | Duality Symmetric Actions | phyzzx.tex, 31 pages, NSF-ITP-93-46 | Nucl.Phys.B411:35-63,1994 | 10.1016/0550-3213(94)90053-1 | null | hep-th | null | It is frequently useful to construct dual descriptions of theories containing
antisymmetric tensor fields by introducing a new potential whose curl gives the
dual field strength, thereby interchanging field equations with Bianchi
identities. We describe a general procedure for constructing actions containing
both pot... | [
{
"created": "Thu, 29 Apr 1993 18:18:58 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Schwarz",
"John H.",
""
],
[
"Sen",
"Ashoke",
""
]
] | It is frequently useful to construct dual descriptions of theories containing antisymmetric tensor fields by introducing a new potential whose curl gives the dual field strength, thereby interchanging field equations with Bianchi identities. We describe a general procedure for constructing actions containing both poten... | 7.639771 | 8.000233 | 8.600874 | 7.273917 | 7.723745 | 7.755937 | 7.462394 | 7.485195 | 7.678014 | 9.293913 | 7.531283 | 7.855315 | 7.981621 | 7.599923 | 7.705946 | 7.769099 | 7.651636 | 7.676738 | 7.634264 | 7.838399 | 7.731286 |
1301.7220 | Rafael Hernandez | Rafael Hernandez, Juan Miguel Nieto | Holographic correlation functions of hexagon Wilson loops with one local
operator | 12 pages. Latex. v2: Reference added. v3: Added clarifications,
published version | Phys.Lett.B726:417-421,2013 | 10.1016/j.physletb.2013.08.029 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the ratio of the correlation function of an hexagon light-like
Wilson loop with one local operator over the expectation value of the Wilson
loop within the strong-coupling regime of the AdS/CFT correspondence. We choose
the hexagon Wilson loop within a class of minimal solutions obtained by cutting
and gl... | [
{
"created": "Wed, 30 Jan 2013 13:35:24 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Feb 2013 14:06:41 GMT",
"version": "v2"
},
{
"created": "Fri, 27 Sep 2013 15:14:20 GMT",
"version": "v3"
}
] | 2013-09-30 | [
[
"Hernandez",
"Rafael",
""
],
[
"Nieto",
"Juan Miguel",
""
]
] | We consider the ratio of the correlation function of an hexagon light-like Wilson loop with one local operator over the expectation value of the Wilson loop within the strong-coupling regime of the AdS/CFT correspondence. We choose the hexagon Wilson loop within a class of minimal solutions obtained by cutting and glui... | 10.793614 | 11.224307 | 10.714945 | 9.841597 | 10.932673 | 10.92133 | 11.106042 | 9.9146 | 10.278379 | 12.390321 | 9.900506 | 9.845544 | 10.181821 | 9.973335 | 9.76145 | 9.975323 | 9.827475 | 10.198211 | 9.995905 | 10.6658 | 9.84627 |
1402.2837 | Shao-Wen Wei | Shao-Wen Wei, Yu-Xiao Liu | Triple points and phase diagrams in the extended phase space of charged
Gauss-Bonnet black holes in AdS space | 17 pages, 15 figures, 2 tables, typos corrected and references added | Phys. Rev. D 90, 044057 (2014) | 10.1103/PhysRevD.90.044057 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the triple points and phase diagrams in the extended phase space of
the charged Gauss-Bonnet black holes in $d$-dimensional anti-de Sitter space,
where the cosmological constant appears as a dynamical pressure of the system
and its conjugate quantity is the thermodynamic volume of the black holes.
Employing ... | [
{
"created": "Wed, 12 Feb 2014 14:36:41 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2014 06:49:19 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Aug 2014 09:30:24 GMT",
"version": "v3"
}
] | 2014-08-26 | [
[
"Wei",
"Shao-Wen",
""
],
[
"Liu",
"Yu-Xiao",
""
]
] | We study the triple points and phase diagrams in the extended phase space of the charged Gauss-Bonnet black holes in $d$-dimensional anti-de Sitter space, where the cosmological constant appears as a dynamical pressure of the system and its conjugate quantity is the thermodynamic volume of the black holes. Employing th... | 6.243783 | 5.862119 | 5.285523 | 5.051975 | 5.927532 | 5.94997 | 6.238242 | 5.477348 | 5.720372 | 5.695636 | 6.051052 | 6.00633 | 5.871637 | 5.89484 | 5.849041 | 5.965461 | 5.95134 | 5.467787 | 6.255062 | 6.195987 | 6.025037 |
1906.05852 | Kristan Jensen | Kristan Jensen | Scrambling in nearly thermalized states at large central charge | 6 pages, 1 figure; v2: minor fixes, updated references | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $2d$ conformal field theory (CFT) at large central charge $c$ and
finite temperature $T$ with heavy operators inserted at spatial infinity. The
heavy operators produce a nearly thermalized steady state at an effective
temperature $T_{\rm eff}\leq T$. Under some assumptions, we find an effective
Schwarzian-li... | [
{
"created": "Thu, 13 Jun 2019 17:53:22 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Jun 2019 17:10:05 GMT",
"version": "v2"
}
] | 2019-06-18 | [
[
"Jensen",
"Kristan",
""
]
] | We study $2d$ conformal field theory (CFT) at large central charge $c$ and finite temperature $T$ with heavy operators inserted at spatial infinity. The heavy operators produce a nearly thermalized steady state at an effective temperature $T_{\rm eff}\leq T$. Under some assumptions, we find an effective Schwarzian-like... | 7.657845 | 7.013816 | 8.76237 | 6.517244 | 7.074471 | 7.242019 | 7.151373 | 6.528316 | 7.045365 | 9.235796 | 6.88799 | 6.828944 | 7.891607 | 7.048711 | 6.838479 | 7.269262 | 7.062739 | 7.22589 | 6.994291 | 8.010458 | 7.034871 |
1707.06439 | Si-wen Li | Si-wen Li | Holographic heavy-baryons in the Witten-Sakai-Sugimoto model with the
D0-D4 background | 28 pages, 1 figure, 1 table, add some references and fix some typos
in this version | Phys. Rev. D 96, 106018 (2017) | 10.1103/PhysRevD.96.106018 | null | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the holographic analysis of light-baryon spectrum in \cite{key-50}
to the case involving the heavy flavors. With the construction of the
Witten-Sakai-Sugimoto model in the D0-D4 background, we use the mechanism
proposed in \cite{key-59,key-60,key-61} by including two light and one heavy
flavor branes, to de... | [
{
"created": "Thu, 20 Jul 2017 10:34:26 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jul 2017 09:13:27 GMT",
"version": "v2"
},
{
"created": "Wed, 8 Nov 2017 08:09:12 GMT",
"version": "v3"
}
] | 2017-11-30 | [
[
"Li",
"Si-wen",
""
]
] | We extend the holographic analysis of light-baryon spectrum in \cite{key-50} to the case involving the heavy flavors. With the construction of the Witten-Sakai-Sugimoto model in the D0-D4 background, we use the mechanism proposed in \cite{key-59,key-60,key-61} by including two light and one heavy flavor branes, to desc... | 8.170335 | 7.426497 | 8.497236 | 7.787245 | 8.147189 | 8.470046 | 8.192046 | 7.663474 | 7.484972 | 9.128338 | 7.826938 | 7.818697 | 8.113837 | 8.159875 | 8.286016 | 8.254733 | 8.230659 | 8.042685 | 7.944288 | 8.378523 | 7.997889 |
2102.05000 | Ivan K. Kostov | Ivan Kostov and Valentina B. Petkova | Octagon with finite bridge: free fermions and determinant identities | 29 pages, no figures. Minor corrections in v2 | null | 10.1007/JHEP06(2021)098 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We continue the study of the octagon form factor which helps to evaluate a
class of four-point correlation functions in $\mathcal{N}=4$ SYM theory. The
octagon is characterised, besides the kinematical parameters, by a "bridge" of
$\ell$ propagators connecting two non-adjacent operators. In this paper we
construct an... | [
{
"created": "Tue, 9 Feb 2021 18:07:19 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Apr 2021 15:14:50 GMT",
"version": "v2"
}
] | 2021-06-30 | [
[
"Kostov",
"Ivan",
""
],
[
"Petkova",
"Valentina B.",
""
]
] | We continue the study of the octagon form factor which helps to evaluate a class of four-point correlation functions in $\mathcal{N}=4$ SYM theory. The octagon is characterised, besides the kinematical parameters, by a "bridge" of $\ell$ propagators connecting two non-adjacent operators. In this paper we construct an o... | 9.802441 | 9.871877 | 11.049559 | 8.669886 | 8.613318 | 9.194849 | 9.24392 | 9.241178 | 8.839763 | 11.067176 | 8.9426 | 9.226681 | 9.634309 | 8.912922 | 9.18176 | 9.075784 | 9.220015 | 8.791953 | 8.657395 | 9.494799 | 8.867677 |
1307.1107 | Enrique Gallegos | E. A. Gallegos, A. J. da Silva, D. Spehler | Some Generalizations in Supersymmetric Quantum Mechanics and the
Supersymmetric $\varepsilon$-System Revisited | 15 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss two distinct aspects in supersymmetric quantum mechanics. First,
we introduce a new class of operators A and $\bar{A}$ in terms of
anticommutators between the momentum operator and N+1 arbitrary
superpotentials. We show that these operators reduce to the conventional ones
which are the starting point in st... | [
{
"created": "Wed, 3 Jul 2013 18:54:43 GMT",
"version": "v1"
}
] | 2013-07-04 | [
[
"Gallegos",
"E. A.",
""
],
[
"da Silva",
"A. J.",
""
],
[
"Spehler",
"D.",
""
]
] | We discuss two distinct aspects in supersymmetric quantum mechanics. First, we introduce a new class of operators A and $\bar{A}$ in terms of anticommutators between the momentum operator and N+1 arbitrary superpotentials. We show that these operators reduce to the conventional ones which are the starting point in stan... | 11.673629 | 12.497873 | 12.175854 | 11.860001 | 12.93437 | 13.097094 | 13.515842 | 12.314939 | 11.419643 | 14.075949 | 11.527399 | 11.287795 | 11.725657 | 11.357367 | 11.466475 | 11.227803 | 11.422627 | 11.214418 | 11.419714 | 11.539228 | 11.280396 |
hep-th/9805038 | Muneto Nitta | Muneto Nitta (KEK, Osaka Univ.) | Moduli Space of Global Symmetry in N=1 Supersymmetric Theories and the
Quasi-Nambu-Goldstone Bosons | LaTex, 42 pages, 8 figures, final version to appear in
Int.J.Mod.Phys.A | Int.J.Mod.Phys.A14:2397-2430,1999 | 10.1142/S0217751X99001202 | KEK-TH-572 | hep-th | null | We derive the moduli space for the global symmetry in N=1 supersymmetric
theories. We show, at the generic points, it coincides with the space of
quasi-Nambu-Goldstone (QNG) bosons, which appear besides the ordinary
Nambu-Goldstone (NG) bosons when global symmetry G breaks down spontaneously to
its subgroup H with pr... | [
{
"created": "Thu, 7 May 1998 13:25:39 GMT",
"version": "v1"
},
{
"created": "Wed, 20 May 1998 15:31:19 GMT",
"version": "v2"
},
{
"created": "Sat, 20 Mar 1999 13:21:17 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Nitta",
"Muneto",
"",
"KEK, Osaka Univ."
]
] | We derive the moduli space for the global symmetry in N=1 supersymmetric theories. We show, at the generic points, it coincides with the space of quasi-Nambu-Goldstone (QNG) bosons, which appear besides the ordinary Nambu-Goldstone (NG) bosons when global symmetry G breaks down spontaneously to its subgroup H with pres... | 8.278344 | 8.599087 | 8.602517 | 7.64988 | 7.932388 | 7.585049 | 7.645342 | 7.450028 | 7.540168 | 9.393056 | 7.508427 | 8.076043 | 8.049807 | 7.897144 | 7.899616 | 7.879779 | 7.806449 | 7.952318 | 7.929636 | 8.36507 | 7.855866 |
1201.1398 | Antonio Soares de Castro | T.R. Cardoso, L.B. Castro, A.S. de Castro | An effective singular oscillator for Duffin-Kemmer-Petiau particles with
a nonminimal vector coupling: a two-fold degeneracy | 1 figure. arXiv admin note: substantial text overlap with
arXiv:1009.1597 | null | 10.1088/1751-8113/45/7/075302 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Scalar and vector bosons in the background of one-dimensional nonminimal
vector linear plus inversely linear potentials are explored in a unified way in
the context of the Duffin-Kemmer-Petiau theory. The problem is mapped into a
Sturm-Liouville problem with an effective singular oscillator. With boundary
conditions ... | [
{
"created": "Fri, 6 Jan 2012 12:00:05 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Cardoso",
"T. R.",
""
],
[
"Castro",
"L. B.",
""
],
[
"de Castro",
"A. S.",
""
]
] | Scalar and vector bosons in the background of one-dimensional nonminimal vector linear plus inversely linear potentials are explored in a unified way in the context of the Duffin-Kemmer-Petiau theory. The problem is mapped into a Sturm-Liouville problem with an effective singular oscillator. With boundary conditions em... | 8.868356 | 7.164432 | 8.226295 | 7.484749 | 7.833465 | 6.637477 | 7.219557 | 7.623181 | 7.05486 | 9.52693 | 7.175225 | 7.733799 | 8.318483 | 7.91427 | 7.548156 | 7.649407 | 7.436334 | 7.51685 | 8.087747 | 8.494672 | 7.423924 |
1412.3787 | Piotr Tourkine | Eduardo Casali and Piotr Tourkine | Infrared behaviour of the one-loop scattering equations and supergravity
integrands | 23 pages, 5 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The recently introduced ambitwistor string led to a striking proposal for
one-loop maximal supergravity amplitudes, localised on the solutions of the
ambitwistor one-loop scattering equations. However, these amplitudes have not
yet been explicitly analysed due to the apparent complexity of the equations
that determin... | [
{
"created": "Thu, 11 Dec 2014 20:20:47 GMT",
"version": "v1"
}
] | 2014-12-12 | [
[
"Casali",
"Eduardo",
""
],
[
"Tourkine",
"Piotr",
""
]
] | The recently introduced ambitwistor string led to a striking proposal for one-loop maximal supergravity amplitudes, localised on the solutions of the ambitwistor one-loop scattering equations. However, these amplitudes have not yet been explicitly analysed due to the apparent complexity of the equations that determine ... | 9.927765 | 10.50079 | 11.810905 | 9.239252 | 10.88965 | 9.550878 | 10.526024 | 9.970811 | 8.936765 | 11.386983 | 9.403325 | 9.257136 | 9.974888 | 9.297567 | 9.953935 | 9.374304 | 9.807057 | 9.739776 | 8.992341 | 9.433399 | 9.404645 |
2109.11534 | Lara Anderson | Lara B. Anderson, James Gray, Mohsen Karkheiran, Paul-Konstantin
Oehlmann and Nikhil Raghuram | $\mathbb{P}^1$-fibrations in F-theory and String Dualities | 63 pages, 6 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this work we study F-theory compactifications on elliptically fibered
Calabi-Yau n-folds which have $\mathbb{P}^1$-fibered base manifolds. Such
geometries, which we study in both 4- and 6-dimensions, are both ubiquitous
within the set of Calabi-Yau manifolds and play a crucial role in
heterotic/F-theory duality. W... | [
{
"created": "Thu, 23 Sep 2021 17:56:41 GMT",
"version": "v1"
}
] | 2021-09-24 | [
[
"Anderson",
"Lara B.",
""
],
[
"Gray",
"James",
""
],
[
"Karkheiran",
"Mohsen",
""
],
[
"Oehlmann",
"Paul-Konstantin",
""
],
[
"Raghuram",
"Nikhil",
""
]
] | In this work we study F-theory compactifications on elliptically fibered Calabi-Yau n-folds which have $\mathbb{P}^1$-fibered base manifolds. Such geometries, which we study in both 4- and 6-dimensions, are both ubiquitous within the set of Calabi-Yau manifolds and play a crucial role in heterotic/F-theory duality. We ... | 4.825705 | 4.95505 | 5.403627 | 4.746643 | 5.035662 | 5.152941 | 5.232948 | 4.769858 | 4.809871 | 5.785957 | 4.848917 | 4.648167 | 4.90013 | 4.662411 | 4.724423 | 4.763025 | 4.630451 | 4.630041 | 4.70687 | 4.791142 | 4.70768 |
hep-th/0701269 | Johanna Knapp | Johanna Knapp, Harun Omer | Matrix Factorizations and Homological Mirror Symmetry on the Torus | 41 pages, 9 figures, v2: reference added, minor corrections and
clarifications, version published in JHEP | JHEP 0703:088,2007 | 10.1088/1126-6708/2007/03/088 | CERN-PH-TH/2007-021 | hep-th | null | We consider matrix factorizations and homological mirror symmetry on the
torus T^2 using a Landau-Ginzburg description. We identify the basic matrix
factorizations of the Landau-Ginzburg superpotential and compute the full
spectrum, taking into account the explicit dependence on bulk and boundary
moduli. We verify ho... | [
{
"created": "Mon, 29 Jan 2007 21:29:59 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Mar 2007 15:40:09 GMT",
"version": "v2"
}
] | 2009-11-13 | [
[
"Knapp",
"Johanna",
""
],
[
"Omer",
"Harun",
""
]
] | We consider matrix factorizations and homological mirror symmetry on the torus T^2 using a Landau-Ginzburg description. We identify the basic matrix factorizations of the Landau-Ginzburg superpotential and compute the full spectrum, taking into account the explicit dependence on bulk and boundary moduli. We verify homo... | 8.623952 | 7.908015 | 7.780684 | 7.4005 | 7.301784 | 7.330565 | 6.180528 | 7.216584 | 7.052904 | 9.923121 | 6.698807 | 7.081013 | 8.470899 | 7.432929 | 7.617493 | 7.581531 | 7.251203 | 7.355412 | 7.466601 | 8.677641 | 7.085198 |
1705.05865 | Scott Collier | Minjae Cho, Scott Collier, Xi Yin | Genus Two Modular Bootstrap | 23 pages, 6 figures. v2: updated references, typos corrected. v3-v5:
minor typos corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Virasoro conformal block decomposition of the genus two
partition function of a two-dimensional CFT by expanding around a Z3-invariant
Riemann surface that is a three-fold cover of the Riemann sphere branched at
four points, and explore constraints from genus two modular invariance and
unitarity. In part... | [
{
"created": "Tue, 16 May 2017 18:02:10 GMT",
"version": "v1"
},
{
"created": "Thu, 18 May 2017 16:46:24 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Nov 2018 03:27:26 GMT",
"version": "v3"
},
{
"created": "Mon, 3 Dec 2018 15:32:41 GMT",
"version": "v4"
},
{
"cr... | 2018-12-05 | [
[
"Cho",
"Minjae",
""
],
[
"Collier",
"Scott",
""
],
[
"Yin",
"Xi",
""
]
] | We study the Virasoro conformal block decomposition of the genus two partition function of a two-dimensional CFT by expanding around a Z3-invariant Riemann surface that is a three-fold cover of the Riemann sphere branched at four points, and explore constraints from genus two modular invariance and unitarity. In partic... | 9.792656 | 9.324384 | 11.333814 | 9.517015 | 10.487884 | 10.252579 | 9.37359 | 9.488093 | 8.50089 | 13.039259 | 9.211547 | 9.123757 | 10.495185 | 9.205207 | 9.036708 | 8.926538 | 8.810163 | 9.173629 | 8.670258 | 10.084548 | 8.5594 |
2011.06352 | Arkajyoti Manna | Subhroneel Chakrabarti, Divyanshu Gupta, Arkajyoti Manna, Madhusudhan
Raman | Irrelevant Deformations of Chiral Bosons | v2: 26 pages. Substantial changes in Sections 4 and 5. Abstract
updated, typos corrected, references and acknowledgement added | J. High Energ. Phys. 2021, 28 (2021) | 10.1007/JHEP02(2021)028 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study $ \text{T}\overline{\text{T}} $ deformations of chiral bosons using
the formalism due to Sen. For arbitrary numbers of left- and right-chiral
bosons, we find that the $ \text{T}\overline{\text{T}} $-deformed Lagrangian
can be computed in closed form, giving rise to a novel non-local action in
Sen's formalism... | [
{
"created": "Thu, 12 Nov 2020 12:46:41 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Dec 2020 09:15:12 GMT",
"version": "v2"
}
] | 2021-02-16 | [
[
"Chakrabarti",
"Subhroneel",
""
],
[
"Gupta",
"Divyanshu",
""
],
[
"Manna",
"Arkajyoti",
""
],
[
"Raman",
"Madhusudhan",
""
]
] | We study $ \text{T}\overline{\text{T}} $ deformations of chiral bosons using the formalism due to Sen. For arbitrary numbers of left- and right-chiral bosons, we find that the $ \text{T}\overline{\text{T}} $-deformed Lagrangian can be computed in closed form, giving rise to a novel non-local action in Sen's formalism. ... | 4.932221 | 4.793921 | 5.167709 | 4.694217 | 4.824417 | 4.802866 | 4.76588 | 4.808938 | 4.799679 | 5.597494 | 4.512555 | 4.779668 | 5.008355 | 4.74015 | 4.753303 | 4.757731 | 4.743421 | 4.706867 | 4.731915 | 5.111886 | 4.758221 |
hep-th/0404165 | M. Alain Berard | Alain B\'erard (LPMC - EA 3468), Herve Mohrbach (LPMC - EA 3468) | Spin Hall effect and Berry phase of spinning particles | published with the following title: Spin Hall effect and Berry phase
of spinning particles | Phys.Lett. A352 (2006) 190-195 | 10.1016/j.physleta.2005.11.071 | null | hep-th cond-mat.other | null | We consider the adiabatic evolution of the Dirac equation in order to compute
its Berry curvature in momentum space. It is found that the position operator
acquires an anomalous contribution due to the non Abelian Berry gauge
connection making the quantum mechanic algebra noncommutative. A generalization
to any known... | [
{
"created": "Thu, 22 Apr 2004 08:49:19 GMT",
"version": "v1"
},
{
"created": "Fri, 7 May 2004 09:53:22 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Sep 2004 06:51:50 GMT",
"version": "v3"
},
{
"created": "Tue, 20 Sep 2005 15:38:06 GMT",
"version": "v4"
},
{
"cr... | 2016-08-16 | [
[
"Bérard",
"Alain",
"",
"LPMC - EA 3468"
],
[
"Mohrbach",
"Herve",
"",
"LPMC - EA 3468"
]
] | We consider the adiabatic evolution of the Dirac equation in order to compute its Berry curvature in momentum space. It is found that the position operator acquires an anomalous contribution due to the non Abelian Berry gauge connection making the quantum mechanic algebra noncommutative. A generalization to any known s... | 11.440965 | 11.276237 | 12.056926 | 11.073376 | 13.037037 | 11.643821 | 12.478856 | 11.132688 | 11.303361 | 13.240298 | 11.118621 | 10.983685 | 11.660667 | 11.468943 | 11.441729 | 11.077236 | 11.048835 | 11.493995 | 11.17633 | 11.775577 | 11.14127 |
2102.08932 | Abu Mohammad Khan | Abu Mohammad Khan | Continuous Spin Representation from Contraction of the Conformal Algebra | Accepted for Publication in the Journal of Mathematical Physics | null | 10.1063/5.0026059 | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | In this paper, we discuss the In\"on\"u-Winger contraction of the conformal
algebra. We start with the light-cone form of the Poincar\'e algebra and extend
it to write down the conformal algebra in $d$ dimensions. To contract the
conformal algebra, we choose five dimensions for simplicity and compactify the
third tra... | [
{
"created": "Mon, 15 Feb 2021 23:03:05 GMT",
"version": "v1"
}
] | 2021-03-31 | [
[
"Khan",
"Abu Mohammad",
""
]
] | In this paper, we discuss the In\"on\"u-Winger contraction of the conformal algebra. We start with the light-cone form of the Poincar\'e algebra and extend it to write down the conformal algebra in $d$ dimensions. To contract the conformal algebra, we choose five dimensions for simplicity and compactify the third trans... | 9.830721 | 8.265183 | 8.868578 | 8.257853 | 8.378449 | 8.538268 | 9.005946 | 8.326589 | 8.562719 | 8.985213 | 8.360584 | 8.102343 | 8.998569 | 8.108865 | 8.301517 | 8.130518 | 7.996974 | 8.25463 | 8.344883 | 8.881417 | 8.251602 |
hep-th/9503130 | Zerbini Sergio | A.A. Btysenko, S.D. Odintsov and S. Zerbini | HIGH TEMPERATURE EXPANSION OF STRING FREE ENERGY IN HYPERBOLIC SPACE | 7 pages, latex file, no figures. | Mod.Phys.Lett.A10:1619-1626,1995 | 10.1142/S0217732395001745 | null | hep-th | null | The high temperature behaviour of the open bosonic string free energy in the
space $S^1 \otimes H^N$ with vanishingly small curvature is investigated. The
leading term of the high temperature expansion of the one-loop free energy,
near the Hagedorn instability, is obtained. The problem of infrared
regularization of t... | [
{
"created": "Tue, 21 Mar 1995 07:47:07 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Btysenko",
"A. A.",
""
],
[
"Odintsov",
"S. D.",
""
],
[
"Zerbini",
"S.",
""
]
] | The high temperature behaviour of the open bosonic string free energy in the space $S^1 \otimes H^N$ with vanishingly small curvature is investigated. The leading term of the high temperature expansion of the one-loop free energy, near the Hagedorn instability, is obtained. The problem of infrared regularization of the... | 14.785411 | 12.995069 | 12.952742 | 11.922157 | 12.581138 | 13.942359 | 12.694844 | 11.9498 | 12.31648 | 12.672228 | 12.693905 | 11.894833 | 12.054021 | 11.898397 | 11.990994 | 11.486702 | 12.057559 | 12.458505 | 11.467553 | 11.982861 | 12.023214 |
hep-th/9404016 | Castanos Garza Octavio-ICNUC | O. Casta\~nos, R. L\'opez-Pe\~na and V.I. Man'ko | Noether's Theorem and time-dependent quantum invariants | Plain TeX, 23 pages, preprint of Instituto de Ciencias Nucleares,
UNAM Departamento de F\ii sica and Matem\'aticas Aplicadas, No. 01 (1994) | J.Phys. A27 (1994) 1751-1770 | 10.1088/0305-4470/27/5/035 | null | hep-th | null | The time dependent-integrals of motion, linear in position and momentum
operators, of a quantum system are extracted from Noether's theorem
prescription by means of special time-dependent variations of coordinates. For
the stationary case of the generalized two-dimensional harmonic oscillator, the
time-independent in... | [
{
"created": "Mon, 4 Apr 1994 23:38:58 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Castaños",
"O.",
""
],
[
"López-Peña",
"R.",
""
],
[
"Man'ko",
"V. I.",
""
]
] | The time dependent-integrals of motion, linear in position and momentum operators, of a quantum system are extracted from Noether's theorem prescription by means of special time-dependent variations of coordinates. For the stationary case of the generalized two-dimensional harmonic oscillator, the time-independent inte... | 12.76754 | 13.478402 | 12.753247 | 12.322533 | 12.667186 | 13.386684 | 13.642344 | 13.980349 | 13.157718 | 15.243931 | 12.85444 | 12.398444 | 12.592602 | 12.01399 | 12.959679 | 12.568671 | 12.881707 | 12.75675 | 12.635101 | 12.589581 | 12.578193 |
hep-th/0011106 | Igor Filippov | Igor Filippov, Stephen S. Pinsky, John R. Hiller | Renormalizing DLCQ Using Supersymmetry | 13 pages, 2 figures, changed content | Phys.Lett.B506:221-230,2001 | 10.1016/S0370-2693(01)00410-5 | null | hep-th hep-ph | null | Recent string theory developments suggest the necessity to understand
supersymmetric gauge theories non-perturbatively, in various dimensions. In
this work we show that there is a standard Hamiltonian formulation that
generates a finite and supersymmetric result at every order of the DLCQ
approximation scheme. We pre... | [
{
"created": "Mon, 13 Nov 2000 19:26:14 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Mar 2001 19:54:58 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Filippov",
"Igor",
""
],
[
"Pinsky",
"Stephen S.",
""
],
[
"Hiller",
"John R.",
""
]
] | Recent string theory developments suggest the necessity to understand supersymmetric gauge theories non-perturbatively, in various dimensions. In this work we show that there is a standard Hamiltonian formulation that generates a finite and supersymmetric result at every order of the DLCQ approximation scheme. We prese... | 14.16566 | 13.608773 | 14.264971 | 13.140482 | 12.682671 | 13.425234 | 13.043013 | 12.647226 | 11.944263 | 14.202142 | 12.254088 | 13.388941 | 14.069427 | 13.16872 | 13.332068 | 13.591219 | 13.342152 | 13.589521 | 13.370614 | 13.722613 | 13.127165 |
hep-th/9306022 | null | Peter Schupp, Paul Watts, and Bruno Zumino | Cartan Calculus for Hopf Algebras and Quantum Groups | 15 pages (submitted to Comm. Math. Phys.) | null | null | NSF-ITP-93-75, LBL-34215, and UCB-PTH-93/20 | hep-th math.QA | null | A generalization of the differential geometry of forms and vector fields to
the case of quantum Lie algebras is given. In an abstract formulation that
incorporates many existing examples of differential geometry on quantum groups,
we combine an exterior derivative, inner derivations, Lie derivatives, forms
and functi... | [
{
"created": "Thu, 3 Jun 1993 22:07:18 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Schupp",
"Peter",
""
],
[
"Watts",
"Paul",
""
],
[
"Zumino",
"Bruno",
""
]
] | A generalization of the differential geometry of forms and vector fields to the case of quantum Lie algebras is given. In an abstract formulation that incorporates many existing examples of differential geometry on quantum groups, we combine an exterior derivative, inner derivations, Lie derivatives, forms and function... | 10.630747 | 9.165804 | 12.053834 | 9.251749 | 7.996985 | 9.561165 | 7.126383 | 9.985169 | 8.766037 | 13.387571 | 9.44521 | 10.165625 | 11.433379 | 10.154557 | 9.707818 | 9.898165 | 10.06139 | 10.157351 | 10.1431 | 11.102579 | 9.911344 |
hep-th/0312175 | Sang-Jin Sin | Sunggeun Lee and Sang-Jin Sin | Localized tachyon condensation and G-parity conservation | 12 pages, 2 figures, final form to appear in JHEP | JHEP 0401 (2004) 054 | 10.1088/1126-6708/2004/01/054 | null | hep-th | null | We study the condensation of localized tachyon in non-supersymmetric orbifold
${\C^2/\Z_n}$. We first show that the G-parities of chiral primaries are
preserved under the condensation of localized tachyon(CLT) given by the chiral
primaries. Using this, we finalize the proof of the conjecture that the
lowest-tachyon-m... | [
{
"created": "Tue, 16 Dec 2003 09:57:14 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Dec 2003 10:04:46 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Jan 2004 12:15:59 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Lee",
"Sunggeun",
""
],
[
"Sin",
"Sang-Jin",
""
]
] | We study the condensation of localized tachyon in non-supersymmetric orbifold ${\C^2/\Z_n}$. We first show that the G-parities of chiral primaries are preserved under the condensation of localized tachyon(CLT) given by the chiral primaries. Using this, we finalize the proof of the conjecture that the lowest-tachyon-mas... | 11.616796 | 12.379215 | 14.591537 | 11.289603 | 11.226751 | 11.930298 | 11.776731 | 11.513559 | 10.783463 | 14.46857 | 11.034789 | 11.169789 | 12.064014 | 11.28384 | 11.501722 | 11.474426 | 11.314872 | 10.700353 | 10.688379 | 12.395296 | 10.732295 |
1306.5670 | Stam Nicolis | M. Axenides, E. G. Floratos and S. Nicolis | Modular discretization of the AdS2/CFT1 Holography | 33 pages LaTeX2e, 1 JPEG figure. Typos corrected, references added.
Clarification of several points in the abstract and the text | JHEP 1402 (2014) 109 | 10.1007/JHEP02(2014)109 | CERN-PH-TH/2013-149 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a finite discretization for the black hole geometry and dynamics.
We realize our proposal, in the case of extremal black holes, for which the
radial and temporal near horizon geometry is known to be
AdS$_2=SL(2,\mathbb{R})/SO(1,1,\mathbb{R})$. We implement its discretization by
replacing the set of real nu... | [
{
"created": "Mon, 24 Jun 2013 16:50:57 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Aug 2013 12:24:52 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Apr 2014 10:33:56 GMT",
"version": "v3"
}
] | 2014-04-28 | [
[
"Axenides",
"M.",
""
],
[
"Floratos",
"E. G.",
""
],
[
"Nicolis",
"S.",
""
]
] | We propose a finite discretization for the black hole geometry and dynamics. We realize our proposal, in the case of extremal black holes, for which the radial and temporal near horizon geometry is known to be AdS$_2=SL(2,\mathbb{R})/SO(1,1,\mathbb{R})$. We implement its discretization by replacing the set of real numb... | 7.892212 | 8.461917 | 7.97545 | 7.922896 | 8.408463 | 8.086679 | 8.129279 | 7.74651 | 7.891795 | 8.670792 | 7.55799 | 7.906565 | 7.747912 | 7.570355 | 7.757128 | 7.825457 | 7.75214 | 7.702129 | 7.867843 | 7.992329 | 7.716342 |
hep-th/9412225 | Yongsung Yoon | Younghoon Park and Yongsung Yoon | Dynamical Supersymmetry of a Vortex System with $1/r^{2}$ Potential | revtex 3.0, 13 pages, no figure | null | null | null | hep-th | null | The Pauli Hamiltonian for a spin $\frac{1}{2}$ charged particle interacting
with a point magnetic vortex and $1/r^{2}$ potential exhibits a dynamical
supersymmetry $Osp(1,1)$ on the plane except at the origin. Using this
symmetry, the spectrum and the wave functions have been obtained. And, the
dynamical supersymmetr... | [
{
"created": "Thu, 29 Dec 1994 13:28:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Park",
"Younghoon",
""
],
[
"Yoon",
"Yongsung",
""
]
] | The Pauli Hamiltonian for a spin $\frac{1}{2}$ charged particle interacting with a point magnetic vortex and $1/r^{2}$ potential exhibits a dynamical supersymmetry $Osp(1,1)$ on the plane except at the origin. Using this symmetry, the spectrum and the wave functions have been obtained. And, the dynamical supersymmetry ... | 10.558113 | 8.646918 | 12.504403 | 9.445823 | 10.241353 | 9.609677 | 8.811993 | 8.733476 | 8.648331 | 11.434666 | 8.733586 | 9.025704 | 10.517782 | 9.335435 | 9.467377 | 9.353074 | 8.98359 | 9.332119 | 9.117342 | 10.514024 | 8.970489 |
1405.2743 | Kiyoharu Kawana | Kiyoharu Kawana | Reconsideration of the Coleman's Baby Universe | 13 pages, 3 figures; typos are corrected, and references are added
(v3) | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reconsider the Coleman's mechanism that solves the Cosmological Constant
Problem by the baby universes. We use the Lorentzian path integral and allow
each universe has a different effective field theory and a vacuum. By using the
probability distribution of coupling constants, it is shown that the
cosmological con... | [
{
"created": "Mon, 12 May 2014 13:19:32 GMT",
"version": "v1"
},
{
"created": "Fri, 16 May 2014 04:37:32 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Jun 2015 03:02:32 GMT",
"version": "v3"
}
] | 2015-06-18 | [
[
"Kawana",
"Kiyoharu",
""
]
] | We reconsider the Coleman's mechanism that solves the Cosmological Constant Problem by the baby universes. We use the Lorentzian path integral and allow each universe has a different effective field theory and a vacuum. By using the probability distribution of coupling constants, it is shown that the cosmological const... | 14.295893 | 12.117574 | 11.950692 | 12.478154 | 13.01541 | 13.996848 | 13.282021 | 12.228473 | 12.472455 | 12.983413 | 11.130673 | 11.915257 | 12.27501 | 12.545528 | 12.584084 | 12.489994 | 12.581918 | 12.461856 | 12.56362 | 12.247306 | 11.732327 |
1711.04786 | Nikolay Gromov | David Grabner, Nikolay Gromov, Vladimir Kazakov, Gregory Korchemsky | Strongly \gamma-deformed N=4 SYM as an integrable CFT | 5 pages, 1 figure; typos corrected | Phys. Rev. Lett. 120, 111601 (2018) | 10.1103/PhysRevLett.120.111601 | KCL-MTH-17-04, LPTENS--17/31, IPhT--T17/171 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate by explicit multi-loop calculation that \gamma-deformed planar
N=4 SYM, supplemented with a set of double-trace counter-terms, has two
nontrivial fixed points in the recently proposed double scaling limit,
combining vanishing 't Hooft coupling and large imaginary deformation
parameter. We provide evide... | [
{
"created": "Mon, 13 Nov 2017 19:00:22 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Nov 2017 23:00:30 GMT",
"version": "v2"
},
{
"created": "Sun, 24 Dec 2017 10:17:52 GMT",
"version": "v3"
}
] | 2018-03-21 | [
[
"Grabner",
"David",
""
],
[
"Gromov",
"Nikolay",
""
],
[
"Kazakov",
"Vladimir",
""
],
[
"Korchemsky",
"Gregory",
""
]
] | We demonstrate by explicit multi-loop calculation that \gamma-deformed planar N=4 SYM, supplemented with a set of double-trace counter-terms, has two nontrivial fixed points in the recently proposed double scaling limit, combining vanishing 't Hooft coupling and large imaginary deformation parameter. We provide evidenc... | 7.194854 | 6.694497 | 8.514875 | 6.480362 | 6.343884 | 6.824045 | 6.269157 | 6.539297 | 6.779513 | 10.598597 | 6.50317 | 6.522988 | 7.327121 | 6.760376 | 6.542944 | 6.60762 | 6.643835 | 6.556643 | 6.640196 | 7.561481 | 6.599519 |
hep-th/9511186 | Hiroshi Ishikawa | Hiroshi Ishikawa (YITP, Kyoto Univ.) | On the equivalence of fermionic string to bosonic string in two
dimensions | 13 pages, latex | Phys.Lett. B385 (1996) 117-124 | 10.1016/0370-2693(96)00850-7 | YITP-95-11 | hep-th | null | Two-dimensional fermionic string theory is shown to have a structure of
topological model, which is isomorphic to a tensor product of two topological
ghost systems independent of each other. One of them is identified with $c=1$
bosonic string theory while the other has trivial physical contents. This fact
enables us ... | [
{
"created": "Mon, 27 Nov 1995 05:40:17 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ishikawa",
"Hiroshi",
"",
"YITP, Kyoto Univ."
]
] | Two-dimensional fermionic string theory is shown to have a structure of topological model, which is isomorphic to a tensor product of two topological ghost systems independent of each other. One of them is identified with $c=1$ bosonic string theory while the other has trivial physical contents. This fact enables us to... | 6.786552 | 5.916952 | 7.569679 | 6.005827 | 6.06705 | 5.510023 | 5.801961 | 5.996992 | 6.096246 | 7.546291 | 5.953763 | 6.320598 | 6.81208 | 6.259315 | 6.21547 | 6.227322 | 6.193155 | 6.279957 | 6.327318 | 6.735152 | 6.221729 |
1209.4476 | Kiyoshi Shiraishi | Kiyoshi Shiraishi | Can Virtual Cosmic Strings Shift the Hawking Temperature? | 3 pages, no figure | Europhysics Letters 20, No. 6, pp. 483-485, 1992 | 10.1209/0295-5075/20/6/002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The amount of the Hawking radiation in Hartle-Hawking vacuum around the
Schwarzschild black hole is calculated in the presence of the cloud of
virtual-cosmic-string loops near the black hole. Recently, Coleman, Preskill
and Wilczek have discussed the black-hole temperature in such situation. We
show, in this letter, ... | [
{
"created": "Thu, 20 Sep 2012 09:42:58 GMT",
"version": "v1"
}
] | 2012-09-21 | [
[
"Shiraishi",
"Kiyoshi",
""
]
] | The amount of the Hawking radiation in Hartle-Hawking vacuum around the Schwarzschild black hole is calculated in the presence of the cloud of virtual-cosmic-string loops near the black hole. Recently, Coleman, Preskill and Wilczek have discussed the black-hole temperature in such situation. We show, in this letter, it... | 12.127811 | 14.870745 | 12.646092 | 11.679991 | 13.138642 | 12.60351 | 14.309345 | 13.147631 | 12.472452 | 11.620151 | 12.316304 | 11.600428 | 11.617779 | 11.445608 | 11.933996 | 11.784243 | 11.595992 | 11.21 | 11.790813 | 10.990937 | 11.869726 |
hep-th/0408239 | Marco Maceda | M. Maceda | On the Wheeler-DeWitt equation for Kasner-like Cosmologies | 12 pages | null | null | null | hep-th | null | The Wheeler-DeWitt equation is obtained for Kasner-like cosmologies. Some
solutions to this equation are presented for empty space, space filled with a
cosmological constant and in the presence of a scalar field. We also briefly
discuss a non-commutative extension of these results.
| [
{
"created": "Tue, 31 Aug 2004 16:19:41 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Maceda",
"M.",
""
]
] | The Wheeler-DeWitt equation is obtained for Kasner-like cosmologies. Some solutions to this equation are presented for empty space, space filled with a cosmological constant and in the presence of a scalar field. We also briefly discuss a non-commutative extension of these results. | 8.722218 | 6.945696 | 6.894986 | 6.790948 | 6.868145 | 6.681761 | 6.567533 | 6.419976 | 7.220409 | 7.844829 | 7.172254 | 7.067235 | 6.874967 | 7.07154 | 7.23434 | 7.078117 | 7.167378 | 7.202367 | 7.211531 | 7.331001 | 7.290814 |
2312.16110 | Tung Tran | Harold C. Steinacker and Tung Tran | Spinorial description for Lorentzian $\mathfrak{hs}$-IKKT | v1 | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We introduce a novel spinorial description for the higher-spin gauge theory
induced by the IKKT matrix model on an FLRW spacetime with Lorentzian
signature, called Lorentzian $\mathfrak{hs}$-IKKT theory. The new description
is based on Weyl spinors transforming under the space-like isometry subgroup
$SL(2,\mathbb{C})... | [
{
"created": "Tue, 26 Dec 2023 16:27:41 GMT",
"version": "v1"
}
] | 2023-12-27 | [
[
"Steinacker",
"Harold C.",
""
],
[
"Tran",
"Tung",
""
]
] | We introduce a novel spinorial description for the higher-spin gauge theory induced by the IKKT matrix model on an FLRW spacetime with Lorentzian signature, called Lorentzian $\mathfrak{hs}$-IKKT theory. The new description is based on Weyl spinors transforming under the space-like isometry subgroup $SL(2,\mathbb{C})$ ... | 6.259725 | 5.978646 | 6.399252 | 5.636191 | 5.777337 | 6.287608 | 6.310669 | 5.849867 | 5.752593 | 6.549046 | 5.872869 | 6.09065 | 6.185869 | 5.948148 | 5.966237 | 6.132199 | 6.020704 | 5.946788 | 6.194318 | 6.172162 | 5.989081 |
1712.08078 | Joris Raeymaekers | Andrea Campoleoni, Stefan Fredenhagen and Joris Raeymaekers | Quantizing higher-spin gravity in free-field variables | 31 pages + appendices. V2: typos corrected, reference added | null | 10.1007/JHEP02(2018)126 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the formulation of massless higher-spin gravity on AdS$_3$ in a
gauge in which the fundamental variables satisfy free field Poisson brackets.
This gauge choice leaves a small portion of the gauge freedom unfixed, which
should be further quotiented out. We show that doing so leads to a bulk version
of the Cou... | [
{
"created": "Thu, 21 Dec 2017 16:50:21 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Feb 2018 09:27:28 GMT",
"version": "v2"
}
] | 2018-04-04 | [
[
"Campoleoni",
"Andrea",
""
],
[
"Fredenhagen",
"Stefan",
""
],
[
"Raeymaekers",
"Joris",
""
]
] | We study the formulation of massless higher-spin gravity on AdS$_3$ in a gauge in which the fundamental variables satisfy free field Poisson brackets. This gauge choice leaves a small portion of the gauge freedom unfixed, which should be further quotiented out. We show that doing so leads to a bulk version of the Coulo... | 9.04199 | 9.202766 | 9.960783 | 8.682461 | 9.508937 | 9.818221 | 9.790903 | 8.386257 | 8.490325 | 10.407495 | 8.772606 | 8.599237 | 8.938902 | 8.504749 | 8.51863 | 8.628443 | 8.796763 | 8.707908 | 8.423846 | 9.094013 | 8.567921 |
hep-th/0404012 | Radoslav Rashkov | H. Dimov and R.C. Rashkov | Generalized pulsating strings | v.2 references added, citations corrected, 18 pages | JHEP 0405 (2004) 068 | 10.1088/1126-6708/2004/05/068 | null | hep-th | null | In this paper we consider new solutions for pulsating strings. For this
purpose we use tha idea of the generalized ansatz for folded and circular
strings in hep-th/0311004. We find the solutions to the resulting
Neumann-Rosochatius integrable system and the corrections to the energy. To do
that we use the approach de... | [
{
"created": "Fri, 2 Apr 2004 11:22:35 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Apr 2004 08:20:30 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dimov",
"H.",
""
],
[
"Rashkov",
"R. C.",
""
]
] | In this paper we consider new solutions for pulsating strings. For this purpose we use tha idea of the generalized ansatz for folded and circular strings in hep-th/0311004. We find the solutions to the resulting Neumann-Rosochatius integrable system and the corrections to the energy. To do that we use the approach deve... | 13.83214 | 11.303523 | 18.010592 | 11.543516 | 12.903969 | 12.491864 | 13.154647 | 10.837027 | 11.158221 | 14.623319 | 12.087972 | 11.861135 | 14.323734 | 12.074345 | 12.668814 | 12.423611 | 12.310681 | 11.899811 | 12.311997 | 14.255862 | 12.079594 |
hep-th/9906207 | Yuji Ohta | Yuji Ohta (Res. Inst. Math. Sci., Kyoto Univ.) | Picard-Fuchs Equations and Whitham Hierarchy in N=2 Supersymmetric
SU(r+1) Yang-Mills Theory | to be published in J. Math. Phys, revtex, 14 pages | J.Math.Phys.40:6292-6301,1999 | 10.1063/1.533093 | null | hep-th | null | In general, Whitham dynamics involves infinitely many parameters called
Whitham times, but in the context of N=2 supersymmetric Yang-Mills theory it
can be regarded as a finite system by restricting the number of Whitham times
appropriately. For example, in the case of SU(r+1) gauge theory without
hypermultiplets, th... | [
{
"created": "Sun, 27 Jun 1999 07:12:04 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Jun 1999 08:36:11 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Oct 1999 09:38:49 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Ohta",
"Yuji",
"",
"Res. Inst. Math. Sci., Kyoto Univ."
]
] | In general, Whitham dynamics involves infinitely many parameters called Whitham times, but in the context of N=2 supersymmetric Yang-Mills theory it can be regarded as a finite system by restricting the number of Whitham times appropriately. For example, in the case of SU(r+1) gauge theory without hypermultiplets, ther... | 6.936547 | 6.065642 | 7.602504 | 6.056359 | 6.476452 | 6.065002 | 6.246027 | 6.087999 | 5.724871 | 7.867575 | 6.317541 | 6.242561 | 6.524206 | 5.979989 | 6.228956 | 6.356287 | 6.119641 | 6.088526 | 5.978781 | 6.713737 | 6.284508 |
hep-th/0012115 | Everton Murilo C. de Abreu | E. M. C. Abreu (UNESP/Guaratingueta), J. Ananias Neto, W. Oliveira and
G. Oliveira-Neto (U.F.J.F.) | Non-Abelian BFFT embedding, Schr\"odinger quantization and the anomaly
of the O(N) nonlinear sigma model | 16 pages, revtex, no figures | null | null | null | hep-th | null | We embed the O(N) nonlinear sigma model in a non-Abelian gauge theory. As a
first class system, it is quantized using two different approaches: the
functional Schr\"odinger method and the non-local field-antifield procedure.
Firstly, the quantization is performed with the functional Schr\"{o}dinger
method, for N=2, o... | [
{
"created": "Wed, 13 Dec 2000 16:32:42 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Abreu",
"E. M. C.",
"",
"UNESP/Guaratingueta"
],
[
"Neto",
"J. Ananias",
"",
"U.F.J.F."
],
[
"Oliveira",
"W.",
"",
"U.F.J.F."
],
[
"Oliveira-Neto",
"G.",
"",
"U.F.J.F."
]
] | We embed the O(N) nonlinear sigma model in a non-Abelian gauge theory. As a first class system, it is quantized using two different approaches: the functional Schr\"odinger method and the non-local field-antifield procedure. Firstly, the quantization is performed with the functional Schr\"{o}dinger method, for N=2, obt... | 9.831461 | 8.511613 | 8.418951 | 8.09112 | 8.358473 | 8.384124 | 8.071144 | 8.11857 | 8.167115 | 9.429743 | 8.173012 | 8.329756 | 8.700373 | 8.331511 | 8.207602 | 8.188805 | 8.239496 | 8.424254 | 8.45706 | 8.666065 | 8.183249 |
2207.14777 | El Hassan Saidi | Youssra Boujakhrout and El Hassan Saidi | Minuscule ABCDE Lax Operators from 4D Chern-Simons Theory | LaTeX, 40 pages, 14 Figures | Nucl.Phys.B 981 (2022) 115859 | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using 4D Chern-Simons (CS) theory with gauge symmetry $G$ having minuscule
coweights, we develop a suitable operator basis to deal with the explicit
calculation of the Lax operator of integrable spin chain satisfying the RLL
equation. Using this basis, we derive the oscillator realisations of the full
list of the min... | [
{
"created": "Fri, 29 Jul 2022 16:39:45 GMT",
"version": "v1"
}
] | 2022-08-01 | [
[
"Boujakhrout",
"Youssra",
""
],
[
"Saidi",
"El Hassan",
""
]
] | Using 4D Chern-Simons (CS) theory with gauge symmetry $G$ having minuscule coweights, we develop a suitable operator basis to deal with the explicit calculation of the Lax operator of integrable spin chain satisfying the RLL equation. Using this basis, we derive the oscillator realisations of the full list of the minus... | 11.32857 | 12.452188 | 12.333317 | 10.504005 | 11.953103 | 11.703504 | 11.527532 | 11.131783 | 11.097313 | 12.606107 | 10.866516 | 11.099009 | 11.555182 | 11.062224 | 11.219613 | 10.933979 | 11.233592 | 11.025015 | 11.355298 | 11.937641 | 10.842743 |
1708.05348 | Stephen Flood | S. P. Flood, J. M. Speight | Chern-Simons deformation of vortices on compact domains | 22 pages, 3 figures | null | 10.1016/j.geomphys.2018.07.009 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Existence of Maxwell-Chern-Simons-Higgs (MCSH) vortices in a Hermitian line
bundle $\L$ over a general compact Riemann surface $\Sigma$ is proved by a
continuation method. The solutions are proved to be smooth both spatially and
as functions of the Chern-Simons deformation parameter $\kappa$, and exist for
all $|\kap... | [
{
"created": "Thu, 17 Aug 2017 16:13:01 GMT",
"version": "v1"
}
] | 2018-09-26 | [
[
"Flood",
"S. P.",
""
],
[
"Speight",
"J. M.",
""
]
] | Existence of Maxwell-Chern-Simons-Higgs (MCSH) vortices in a Hermitian line bundle $\L$ over a general compact Riemann surface $\Sigma$ is proved by a continuation method. The solutions are proved to be smooth both spatially and as functions of the Chern-Simons deformation parameter $\kappa$, and exist for all $|\kappa... | 4.512225 | 4.615349 | 4.909798 | 4.591402 | 4.970935 | 4.959704 | 4.756862 | 4.64783 | 4.530884 | 5.057329 | 4.5281 | 4.499692 | 4.671166 | 4.48525 | 4.574799 | 4.557661 | 4.582104 | 4.49759 | 4.521859 | 4.72071 | 4.477126 |
1307.4787 | Andre Lukas | Lara B. Anderson, Andrei Constantin, James Gray, Andre Lukas and Eran
Palti | A Comprehensive Scan for Heterotic SU(5) GUT models | 33 pages, Latex | null | 10.1007/JHEP01(2014)047 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Compactifications of heterotic theories on smooth Calabi-Yau manifolds
remains one of the most promising approaches to string phenomenology. In two
previous papers, http://arXiv.org/abs/arXiv:1106.4804 and
http://arXiv.org/abs/arXiv:1202.1757, large classes of such vacua were
constructed, using sums of line bundles o... | [
{
"created": "Wed, 17 Jul 2013 20:48:51 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Anderson",
"Lara B.",
""
],
[
"Constantin",
"Andrei",
""
],
[
"Gray",
"James",
""
],
[
"Lukas",
"Andre",
""
],
[
"Palti",
"Eran",
""
]
] | Compactifications of heterotic theories on smooth Calabi-Yau manifolds remains one of the most promising approaches to string phenomenology. In two previous papers, http://arXiv.org/abs/arXiv:1106.4804 and http://arXiv.org/abs/arXiv:1202.1757, large classes of such vacua were constructed, using sums of line bundles ove... | 7.451723 | 7.079888 | 7.969368 | 7.208327 | 7.229769 | 7.249144 | 6.768251 | 7.44601 | 6.724583 | 8.395567 | 7.144652 | 7.049302 | 7.152212 | 7.029687 | 7.091375 | 7.193403 | 7.033041 | 7.056688 | 6.982309 | 7.183133 | 7.003568 |
2406.05345 | Zhang-Yu Nie | Zi-Qiang Zhao, Zhang-Yu Nie, Jing-Fei Zhang, Xin Zhang, Matteo
Baggioli | Dynamical and thermodynamic crossovers in the supercritical region of a
holographic superfluid model | 17 pages, 9 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many physical systems, including classical fluids, present in their phase
diagram the competition between two phases that are separated by a line of
first-order phase transitions which terminates at a so-called critical point.
Despite several proposals, in the supercritical region beyond the critical
point, whether t... | [
{
"created": "Sat, 8 Jun 2024 04:11:23 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Jun 2024 06:02:14 GMT",
"version": "v2"
}
] | 2024-06-12 | [
[
"Zhao",
"Zi-Qiang",
""
],
[
"Nie",
"Zhang-Yu",
""
],
[
"Zhang",
"Jing-Fei",
""
],
[
"Zhang",
"Xin",
""
],
[
"Baggioli",
"Matteo",
""
]
] | Many physical systems, including classical fluids, present in their phase diagram the competition between two phases that are separated by a line of first-order phase transitions which terminates at a so-called critical point. Despite several proposals, in the supercritical region beyond the critical point, whether the... | 10.543368 | 11.93944 | 11.782282 | 11.206406 | 11.310081 | 11.904166 | 11.570839 | 11.37739 | 11.092089 | 11.396698 | 10.304444 | 10.052703 | 10.385707 | 10.143023 | 10.331397 | 10.480618 | 10.503912 | 10.000799 | 9.860233 | 10.737214 | 10.02864 |
1406.3626 | Andreas Stergiou | Benjamin Grinstein, Andreas Stergiou, David Stone, Ming Zhong | A challenge to the $a$-theorem in six dimensions | 4 pages. v2: Fixed typos, added references | Phys. Rev. Lett. 113, 231602 (2014) | 10.1103/PhysRevLett.113.231602 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The possibility of a strong $a$-theorem in six dimensions is examined in
multi-flavor $\phi^3$ theory. Contrary to the case in two and four dimensions,
we find that in perturbation theory the relevant quantity $\tilde{a}$ increases
monotonically along flows away from the trivial fixed point. $\tilde{a}$ is a
natural ... | [
{
"created": "Fri, 13 Jun 2014 20:00:01 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Apr 2015 20:01:33 GMT",
"version": "v2"
}
] | 2015-04-24 | [
[
"Grinstein",
"Benjamin",
""
],
[
"Stergiou",
"Andreas",
""
],
[
"Stone",
"David",
""
],
[
"Zhong",
"Ming",
""
]
] | The possibility of a strong $a$-theorem in six dimensions is examined in multi-flavor $\phi^3$ theory. Contrary to the case in two and four dimensions, we find that in perturbation theory the relevant quantity $\tilde{a}$ increases monotonically along flows away from the trivial fixed point. $\tilde{a}$ is a natural ex... | 6.817281 | 5.993622 | 7.629321 | 6.523108 | 6.605614 | 5.985535 | 6.707101 | 6.271839 | 6.23124 | 7.385026 | 6.153867 | 6.387664 | 6.579193 | 6.489519 | 6.429521 | 6.34418 | 6.666307 | 6.290629 | 6.580575 | 6.761144 | 6.251976 |
hep-th/9211059 | Neil Marcus | Neil Marcus (U of Tel-Aviv) | A tour through N=2 strings | 24 Pages (LaTeX) (Revision: History updated, reference fixed.), Rome
String Theory Workshop 1992 (Talk presented at the Rome conference on
``String theory, quantum gravity and the unification of fundamental
interactions'', Sept 1992.) | null | null | TAUP-2002-92 | hep-th | null | I give an overview of open, closed and heterotic N=2 strings. At the tree
level I derive the effective field theories of all the strings, and discuss the
group theory of the N=2 open string and the interaction between its open and
closed sectors. At one loop N=2 string loop amplitudes and partition functions
have inc... | [
{
"created": "Fri, 13 Nov 1992 12:33:29 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Nov 1992 10:14:19 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Marcus",
"Neil",
"",
"U of Tel-Aviv"
]
] | I give an overview of open, closed and heterotic N=2 strings. At the tree level I derive the effective field theories of all the strings, and discuss the group theory of the N=2 open string and the interaction between its open and closed sectors. At one loop N=2 string loop amplitudes and partition functions have incur... | 14.82724 | 15.94189 | 14.717633 | 14.065382 | 14.710993 | 14.833357 | 14.976015 | 14.225749 | 13.696783 | 16.654699 | 13.928331 | 13.424981 | 14.128585 | 13.563399 | 13.582716 | 13.437251 | 13.397633 | 13.594942 | 13.869959 | 14.080309 | 13.387747 |
hep-th/9404182 | Jacek Dziarmaga | Jacek Dziarmaga | Only hybrid anyons can exist in broken symmetry phase of nonrelativistic
$U(1)^{2}$ Chern-Simons theory | 10 pages in plain Latex (one argument added, version accepted for
publication in Phys.Rev.D(Rapid Communications) ) | null | 10.1103/PhysRevD.50.R2376 | null | hep-th cond-mat | null | We present two examples of parity-invariant $[U(1)]^{2}$ Chern-Simons-Higgs
models with spontaneously broken symmetry. The models possess topological
vortex excitations. It is argued that the smallest possible flux quanta are
composites of one quantum of each type $(1,1)$. These hybrid anyons will
dominate the statis... | [
{
"created": "Fri, 29 Apr 1994 11:01:17 GMT",
"version": "v1"
},
{
"created": "Tue, 3 May 1994 08:11:52 GMT",
"version": "v2"
},
{
"created": "Thu, 14 Jul 1994 13:51:37 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"Dziarmaga",
"Jacek",
""
]
] | We present two examples of parity-invariant $[U(1)]^{2}$ Chern-Simons-Higgs models with spontaneously broken symmetry. The models possess topological vortex excitations. It is argued that the smallest possible flux quanta are composites of one quantum of each type $(1,1)$. These hybrid anyons will dominate the statisti... | 14.493885 | 13.571185 | 16.207174 | 13.813193 | 13.916462 | 13.856956 | 14.137079 | 14.214496 | 13.342743 | 18.431574 | 13.811571 | 13.585057 | 14.594493 | 13.735067 | 13.749782 | 13.658229 | 14.667164 | 13.962165 | 13.884596 | 15.30444 | 13.84994 |
1202.4690 | Kallosh Renata | Renata Kallosh | On Absence of 3-loop Divergence in N=4 Supergravity | 5 pages | null | 10.1103/PhysRevD.85.081702 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that N=4 supergravity is 3-loop UV finite because the relevant
supersymmetric candidate counterterm is known to be SL(2, R)x SO(6) invariant,
which violates the Noether-Gaillard-Zumino current conservation. Analogous
arguments, based on the universality properties of groups of type E7, also
apply to N=5,6,8 ... | [
{
"created": "Tue, 21 Feb 2012 16:18:46 GMT",
"version": "v1"
}
] | 2013-05-30 | [
[
"Kallosh",
"Renata",
""
]
] | We argue that N=4 supergravity is 3-loop UV finite because the relevant supersymmetric candidate counterterm is known to be SL(2, R)x SO(6) invariant, which violates the Noether-Gaillard-Zumino current conservation. Analogous arguments, based on the universality properties of groups of type E7, also apply to N=5,6,8 in... | 18.762482 | 17.305641 | 21.208719 | 16.400421 | 16.466551 | 17.589596 | 19.493193 | 16.389387 | 15.773838 | 22.324017 | 16.525284 | 16.79612 | 18.028625 | 16.351952 | 16.280191 | 17.365273 | 17.364168 | 16.465317 | 16.678028 | 19.045406 | 16.515013 |
hep-th/0105191 | Pei-Ming Ho | Pei-Ming Ho, Shun-Pei Miao | Noncommutative Differential Calculus for D-brane in Non-Constant B Field
Background | 21 pages, Latex file, references added, minor modification | Phys.Rev.D64:126002,2001 | 10.1103/PhysRevD.64.126002 | null | hep-th | null | In this paper we try to construct noncommutative Yang-Mills theory for
generic Poisson manifolds. It turns out that the noncommutative differential
calculus defined in an old work is exactly what we need. Using this calculus,
we generalize results about the Seiberg-Witten map, the Dirac-Born-Infeld
action, the matrix... | [
{
"created": "Sat, 19 May 2001 16:36:25 GMT",
"version": "v1"
},
{
"created": "Tue, 29 May 2001 05:39:25 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Jun 2001 02:12:24 GMT",
"version": "v3"
}
] | 2009-05-12 | [
[
"Ho",
"Pei-Ming",
""
],
[
"Miao",
"Shun-Pei",
""
]
] | In this paper we try to construct noncommutative Yang-Mills theory for generic Poisson manifolds. It turns out that the noncommutative differential calculus defined in an old work is exactly what we need. Using this calculus, we generalize results about the Seiberg-Witten map, the Dirac-Born-Infeld action, the matrix m... | 9.467611 | 7.375917 | 10.249413 | 7.567965 | 7.433373 | 7.261017 | 8.27783 | 7.507955 | 7.444455 | 9.95994 | 7.560021 | 7.669923 | 8.56108 | 8.154311 | 7.587169 | 7.554276 | 7.34876 | 7.848914 | 7.810562 | 9.020522 | 7.688097 |
hep-th/9909190 | Anton Galajinsky | Stefano Bellucci and Anton Galajinsky (INFN, Frascati) | Consistent Batalin--Fradkin quantization of Infinitely Reducible First
Class Constraints | 5 pages, LaTex. Minor corrections including the title. The version to
appear in Phys. Rev. D | Phys.Rev. D62 (2000) 027501 | 10.1103/PhysRevD.62.027501 | null | hep-th | null | We reconsider the problem of BRST quantization of a mechanics with infinitely
reducible first class constraints. Following an earlier recipe [Phys. Lett. B
381, 105, (1996)], the original phase space is extended by purely auxiliary
variables, the constraint set in the enlarged space being first stage of
reducibility.... | [
{
"created": "Mon, 27 Sep 1999 20:22:53 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Mar 2000 16:36:50 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Bellucci",
"Stefano",
"",
"INFN, Frascati"
],
[
"Galajinsky",
"Anton",
"",
"INFN, Frascati"
]
] | We reconsider the problem of BRST quantization of a mechanics with infinitely reducible first class constraints. Following an earlier recipe [Phys. Lett. B 381, 105, (1996)], the original phase space is extended by purely auxiliary variables, the constraint set in the enlarged space being first stage of reducibility. T... | 11.862818 | 11.271482 | 13.820602 | 10.35569 | 11.107668 | 11.793167 | 11.624711 | 10.785606 | 9.673446 | 15.901204 | 10.322452 | 10.660008 | 11.97735 | 11.591414 | 10.726164 | 11.062407 | 11.18065 | 11.28017 | 10.799882 | 12.004275 | 10.427051 |
1105.4870 | Omid Saremi | Omid Saremi and Kiyoumars A. Sohrabi | Causal three-point functions and nonlinear second-order hydrodynamic
coefficients in AdS/CFT | typos corrected, a reference added | null | 10.1007/JHEP11(2011)147 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of $\mathcal{N}=4$ SYM, we compute the finite 't Hooft
coupling $\lambda$ correction to the non-linear second-order hydrodynamic
coefficient $\lambda_3$ from a Kubo formula based on fully retarded three-point
functions using AdS/CFT. Although $\lambda_3$ is known to vanish in the
infinite 't Hooft coup... | [
{
"created": "Tue, 24 May 2011 19:52:36 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Oct 2011 21:52:55 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Saremi",
"Omid",
""
],
[
"Sohrabi",
"Kiyoumars A.",
""
]
] | In the context of $\mathcal{N}=4$ SYM, we compute the finite 't Hooft coupling $\lambda$ correction to the non-linear second-order hydrodynamic coefficient $\lambda_3$ from a Kubo formula based on fully retarded three-point functions using AdS/CFT. Although $\lambda_3$ is known to vanish in the infinite 't Hooft coupli... | 6.253999 | 5.040771 | 5.587496 | 5.341614 | 5.53286 | 5.25705 | 5.058828 | 5.318937 | 5.319332 | 6.249416 | 5.294968 | 5.508444 | 5.736934 | 5.507688 | 5.596012 | 5.434615 | 5.422522 | 5.294687 | 5.504123 | 5.794891 | 5.491437 |
1611.03490 | Carlos Nunez | Georgios Itsios, Carlos Nunez and Dimitrios Zoakos | Mesons from (non) Abelian T-dual backgrounds | 26 pages plus many long appendices | null | 10.1007/JHEP01(2017)011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study mesonic excitations in a Quantum Field Theory dual to
the non Abelian T-dual of $AdS_5\times S^5$, using a D6 brane probe on the
Sfetsos-Thompson background. Before and after the duality, we observe
interesting differences between the spectra and interpret them. The spectrum of
masses and the in... | [
{
"created": "Thu, 10 Nov 2016 21:00:01 GMT",
"version": "v1"
}
] | 2017-02-01 | [
[
"Itsios",
"Georgios",
""
],
[
"Nunez",
"Carlos",
""
],
[
"Zoakos",
"Dimitrios",
""
]
] | In this work we study mesonic excitations in a Quantum Field Theory dual to the non Abelian T-dual of $AdS_5\times S^5$, using a D6 brane probe on the Sfetsos-Thompson background. Before and after the duality, we observe interesting differences between the spectra and interpret them. The spectrum of masses and the inte... | 8.852156 | 8.272613 | 9.612335 | 7.759377 | 8.676816 | 8.489827 | 8.120378 | 7.286915 | 8.023418 | 10.679933 | 8.234296 | 7.646707 | 8.803329 | 7.753204 | 8.27376 | 7.976968 | 7.937768 | 7.778964 | 7.770211 | 8.410736 | 7.959581 |
2207.03126 | Yun Zhi Du | Yun-Zhi Du, Huai-Fan Li, Ren Zhao | Overview of thermodynamic properties for Reissner-Nordstrom-de Sitter
spacetime in induced phase space | null | null | 10.1140/epjc/s10052-022-10797-w | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Since the black hole and cosmological horizons in the de Sitter (dS)
spacetime with the Reissner-Nordstrom (RN) black hole are not independent to
each other, which is caused by the gravitational effect, the interplay between
two horizons should be considered. Based on this, by introducing the
interactive entropy the ... | [
{
"created": "Thu, 7 Jul 2022 07:14:05 GMT",
"version": "v1"
}
] | 2022-10-19 | [
[
"Du",
"Yun-Zhi",
""
],
[
"Li",
"Huai-Fan",
""
],
[
"Zhao",
"Ren",
""
]
] | Since the black hole and cosmological horizons in the de Sitter (dS) spacetime with the Reissner-Nordstrom (RN) black hole are not independent to each other, which is caused by the gravitational effect, the interplay between two horizons should be considered. Based on this, by introducing the interactive entropy the RN... | 8.595403 | 9.07074 | 8.01718 | 7.96694 | 8.794493 | 8.199313 | 9.024479 | 8.251559 | 8.597103 | 8.985183 | 8.2398 | 8.497726 | 8.05582 | 8.110204 | 8.510905 | 8.286592 | 8.301583 | 8.043446 | 8.132864 | 8.428196 | 8.260349 |
hep-th/9708038 | Red Hat Linux User | Yoonbai Kim | Thirring Model in Lower Dimensions: Nonperturbative Approaches | 9 pages of LaTeX, Talk given at the International Workshop on
Prespectives of Strong Coupling Gauge Theories(SCGT96), Nagoya, Japani,
November 1996 | null | null | null | hep-th | null | A reformulation of the Thirring model as a gauge theory on both continuum
spacetime and discretized lattice is reviewed. In (1+1) dimensions, our result
reproduces consistently the bosonization of the massless Thirring model. In
(2+1) dimensions, the analysis by use of Schwinger-Dyson equation is shown to
exhibit dyn... | [
{
"created": "Thu, 7 Aug 1997 00:00:43 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kim",
"Yoonbai",
""
]
] | A reformulation of the Thirring model as a gauge theory on both continuum spacetime and discretized lattice is reviewed. In (1+1) dimensions, our result reproduces consistently the bosonization of the massless Thirring model. In (2+1) dimensions, the analysis by use of Schwinger-Dyson equation is shown to exhibit dynam... | 7.700513 | 6.375495 | 6.907248 | 6.339978 | 7.533769 | 6.392894 | 6.231968 | 6.430771 | 6.180161 | 7.021502 | 6.819211 | 6.67632 | 6.857339 | 6.874576 | 7.266227 | 7.078205 | 7.143399 | 7.05245 | 7.106583 | 6.780525 | 7.055213 |
0908.0004 | Steven B. Giddings | Steven B. Giddings and Rafael A. Porto | The gravitational S-matrix | 46 pages, 10 figures | Phys.Rev.D81:025002,2010 | 10.1103/PhysRevD.81.025002 | CERN-PH-TH/2009-142 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the hypothesized existence of an S-matrix for gravity, and
some of its expected general properties. We first discuss basic questions
regarding existence of such a matrix, including those of infrared divergences
and description of asymptotic states. Distinct scattering behavior occurs in
the Born, eikon... | [
{
"created": "Mon, 3 Aug 2009 19:12:36 GMT",
"version": "v1"
}
] | 2011-08-02 | [
[
"Giddings",
"Steven B.",
""
],
[
"Porto",
"Rafael A.",
""
]
] | We investigate the hypothesized existence of an S-matrix for gravity, and some of its expected general properties. We first discuss basic questions regarding existence of such a matrix, including those of infrared divergences and description of asymptotic states. Distinct scattering behavior occurs in the Born, eikonal... | 15.581126 | 17.529776 | 18.365267 | 16.587847 | 16.862566 | 19.308558 | 17.935228 | 17.01627 | 17.131144 | 19.667057 | 16.740826 | 15.64475 | 16.547773 | 15.800208 | 16.09774 | 16.164248 | 16.801039 | 15.945087 | 15.675718 | 16.433464 | 16.133846 |
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