id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1311.2312 | Eva Silverstein | Eva Silverstein | Les Houches lectures on inflationary observables and string theory | 40 pages, 1 figure | null | null | SU-ITP-13/22 | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | These lectures cover the theoretical structure and phenomenology of some
basic mechanisms for inflation. A full treatment of the problem requires
`ultraviolet completion' because of the sensitivity of inflation to quantum
gravity effects, while the observables are elegantly parameterized using low
energy field theory... | [
{
"created": "Sun, 10 Nov 2013 22:33:24 GMT",
"version": "v1"
}
] | 2013-11-12 | [
[
"Silverstein",
"Eva",
""
]
] | These lectures cover the theoretical structure and phenomenology of some basic mechanisms for inflation. A full treatment of the problem requires `ultraviolet completion' because of the sensitivity of inflation to quantum gravity effects, while the observables are elegantly parameterized using low energy field theory. ... | 17.937941 | 17.298954 | 18.971653 | 17.305305 | 19.231932 | 19.754269 | 19.473568 | 17.771738 | 16.75145 | 21.039715 | 17.627836 | 16.211683 | 16.814976 | 16.507072 | 15.942509 | 16.783047 | 16.279757 | 15.864318 | 16.891344 | 16.625044 | 16.548412 |
2205.09765 | Julien Barrat | Julien Barrat, Aleix Gimenez-Grau, Pedro Liendo | A dispersion relation for defect CFT | 30 pages, 1 figure | null | 10.1007/JHEP02(2023)255 | HU-EP-22/18-RTG | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a dispersion relation for defect CFT that reconstructs two-point
functions in the presence of a defect as an integral of a single discontinuity.
The main virtue of this formula is that it streamlines explicit bootstrap
calculations, bypassing the resummation of conformal blocks. As applications we
reproduc... | [
{
"created": "Thu, 19 May 2022 18:00:01 GMT",
"version": "v1"
}
] | 2023-03-22 | [
[
"Barrat",
"Julien",
""
],
[
"Gimenez-Grau",
"Aleix",
""
],
[
"Liendo",
"Pedro",
""
]
] | We present a dispersion relation for defect CFT that reconstructs two-point functions in the presence of a defect as an integral of a single discontinuity. The main virtue of this formula is that it streamlines explicit bootstrap calculations, bypassing the resummation of conformal blocks. As applications we reproduce ... | 9.563593 | 8.386863 | 9.170587 | 7.863194 | 8.084191 | 8.608705 | 8.117728 | 8.27315 | 8.190134 | 10.795789 | 8.278024 | 8.325252 | 8.994328 | 8.304485 | 8.289742 | 8.476728 | 8.527248 | 8.312904 | 8.558649 | 9.260087 | 8.75793 |
1112.4162 | Agustin Sabio Vera | G. Chachamis and A. Sabio Vera | The colour octet representation of the non-forward BFKL Green function | 12 pages, 7 figures | null | 10.1016/j.physletb.2012.02.036 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We factorize the infrared divergences of the non-forward BFKL Green function
for a general t-channel projection of the color quantum numbers and study the
properties of the infrared finite remainder in the case of color octet
exchange. The octet Green function is compared with the singlet case for
different values of... | [
{
"created": "Sun, 18 Dec 2011 14:35:37 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Chachamis",
"G.",
""
],
[
"Vera",
"A. Sabio",
""
]
] | We factorize the infrared divergences of the non-forward BFKL Green function for a general t-channel projection of the color quantum numbers and study the properties of the infrared finite remainder in the case of color octet exchange. The octet Green function is compared with the singlet case for different values of t... | 6.942883 | 8.389995 | 8.68584 | 7.563285 | 8.938148 | 7.984004 | 7.981964 | 7.87513 | 7.279101 | 8.077337 | 7.702917 | 7.454196 | 7.117977 | 6.753241 | 6.972301 | 7.012147 | 7.10876 | 7.047918 | 6.893874 | 6.940783 | 6.943465 |
hep-th/9806057 | Stefano De Leo | Stefano De Leo (Dip. di Fisica, INFN, Lecce, Italia), Waldyr A.
Rodrigues, Jr. (UNICAMP/IMECC, Campinas, Brasil) | Quaternionic Electron Theory: Dirac's Equation | 14 pags, Revtex, Int. J. Theor. Phys. (published, May 98) | Int.J.Theor.Phys. 37 (1998) 1511-1530 | null | null | hep-th | null | We perform a one-dimensional complexified quaternionic version of the Dirac
equation based on $i$-complex geometry. The problem of the missing complex
parameters in Quaternionic Quantum Mechanics with $i$-complex geometry is
overcome by a nice ``trick'' which allows to avoid the Dirac algebra
constraints in formulati... | [
{
"created": "Sat, 6 Jun 1998 23:07:20 GMT",
"version": "v1"
}
] | 2012-08-27 | [
[
"De Leo",
"Stefano",
"",
"Dip. di Fisica, INFN, Lecce, Italia"
],
[
"Rodrigues,",
"Waldyr A.",
"Jr.",
"UNICAMP/IMECC, Campinas, Brasil"
]
] | We perform a one-dimensional complexified quaternionic version of the Dirac equation based on $i$-complex geometry. The problem of the missing complex parameters in Quaternionic Quantum Mechanics with $i$-complex geometry is overcome by a nice ``trick'' which allows to avoid the Dirac algebra constraints in formulating... | 18.30382 | 16.670475 | 17.966452 | 15.406278 | 18.030424 | 16.951401 | 16.991831 | 16.549749 | 16.844749 | 19.755856 | 17.109497 | 17.197872 | 16.575108 | 16.636848 | 17.24264 | 17.549225 | 17.313263 | 17.003231 | 16.950317 | 15.838256 | 17.027512 |
1606.08081 | Vadim Kaplunovsky | Jacob Claussen and Vadim Kaplunovsky | Deconstructing the E_0 SCFT to Solve the Orbifold Paradox of the
Heterotic M Theory | 30 pages, several colored figures; version v2 fixes acknowledgements | null | null | UTTG-11-16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many heterotic orbifold models have massless twisted-sector particles with
simultaneous E8_1 and E8_2 charges. In the strong-coupling M-theory dual of the
heterotic string this poses a paradox: Since the E8_1 and E8_2 live at opposite
ends of the x^10 dimension, where could a massless particle with both types of
char... | [
{
"created": "Sun, 26 Jun 2016 20:23:25 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Jun 2016 20:41:23 GMT",
"version": "v2"
}
] | 2016-06-30 | [
[
"Claussen",
"Jacob",
""
],
[
"Kaplunovsky",
"Vadim",
""
]
] | Many heterotic orbifold models have massless twisted-sector particles with simultaneous E8_1 and E8_2 charges. In the strong-coupling M-theory dual of the heterotic string this poses a paradox: Since the E8_1 and E8_2 live at opposite ends of the x^10 dimension, where could a massless particle with both types of charge... | 9.196285 | 10.594091 | 10.365194 | 9.287266 | 10.971766 | 10.53465 | 9.901463 | 9.775103 | 9.361129 | 10.692162 | 9.326096 | 9.39614 | 9.425021 | 9.30158 | 9.561289 | 9.392136 | 9.520272 | 9.420033 | 9.411967 | 9.63871 | 9.095566 |
hep-th/9805009 | Armen Nersessian | A. Nersessian | The Hamiltonian Formalism for the Generalized Rigid Particles | 11 pages, LaTeX | Theor.Math.Phys. 117 (1998) 1214-1222; Teor.Mat.Fiz. 117 (1998)
130-139 | null | JINR P2-98-108 | hep-th | null | The Hamiltonian formulation for the mechanical systems with
reparametrization-invariant Lagrangians, depending on the worldline external
curvatures is given, which is based on the use of moving frame.
A complete sets of constraints are found for the Lagrangians with quadratic
dependence on curvatures, for the lagra... | [
{
"created": "Sat, 2 May 1998 10:10:53 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nersessian",
"A.",
""
]
] | The Hamiltonian formulation for the mechanical systems with reparametrization-invariant Lagrangians, depending on the worldline external curvatures is given, which is based on the use of moving frame. A complete sets of constraints are found for the Lagrangians with quadratic dependence on curvatures, for the lagrangia... | 9.963379 | 8.021548 | 9.621789 | 8.680805 | 7.964182 | 8.338263 | 7.417617 | 8.268147 | 8.36501 | 9.498747 | 7.774708 | 8.610657 | 8.937114 | 8.556421 | 8.52852 | 8.764446 | 8.470532 | 8.770646 | 8.536978 | 9.4818 | 8.617126 |
hep-th/0104248 | Chris Austin | Chris Austin | A Brief Summary of the Group-Variation Equations | 9 pages, LaTeX2e | null | null | null | hep-th hep-lat hep-ph | null | A brief summary is given of the Group-Variation Equations and the island
diagram confinement mechanism, with an explanation of the prediction that the
cylinder-topology minimal-area spanning surface term in the correlation
function of two Wilson loops at large $N_c$, when it exists, must have a
pre-exponential factor... | [
{
"created": "Sun, 29 Apr 2001 20:15:43 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Austin",
"Chris",
""
]
] | A brief summary is given of the Group-Variation Equations and the island diagram confinement mechanism, with an explanation of the prediction that the cylinder-topology minimal-area spanning surface term in the correlation function of two Wilson loops at large $N_c$, when it exists, must have a pre-exponential factor, ... | 16.671021 | 13.237142 | 16.435682 | 13.951512 | 13.332104 | 13.317956 | 12.565372 | 13.890917 | 13.932698 | 16.777506 | 13.552137 | 13.925954 | 15.086351 | 13.709953 | 14.946466 | 13.810448 | 13.762051 | 13.608361 | 14.066196 | 14.722008 | 14.390559 |
2101.12529 | Vassilis Papadopoulos | Constantin Bachas and Vassilis Papadopoulos | Phases of Holographic Interfaces | 57 pages, 14 figures. Minor changes | null | 10.1007/JHEP04(2021)262 | null | hep-th cond-mat.stat-mech gr-qc | http://creativecommons.org/licenses/by/4.0/ | We compute the phase diagram of the simplest holographic bottom-up model of
conformal interfaces. The model consists of a thin domain wall between
three-dimensional Anti-de Sitter (AdS) vacua, anchored on a boundary circle. We
distinguish five phases depending on the existence of a black hole, the
intersection of its... | [
{
"created": "Fri, 29 Jan 2021 11:32:53 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Feb 2021 16:07:10 GMT",
"version": "v2"
},
{
"created": "Thu, 1 Apr 2021 19:09:04 GMT",
"version": "v3"
}
] | 2021-05-12 | [
[
"Bachas",
"Constantin",
""
],
[
"Papadopoulos",
"Vassilis",
""
]
] | We compute the phase diagram of the simplest holographic bottom-up model of conformal interfaces. The model consists of a thin domain wall between three-dimensional Anti-de Sitter (AdS) vacua, anchored on a boundary circle. We distinguish five phases depending on the existence of a black hole, the intersection of its h... | 13.494196 | 15.263463 | 15.193705 | 13.662268 | 14.590023 | 14.542996 | 17.45882 | 15.349501 | 13.527672 | 16.175894 | 13.360261 | 13.793981 | 14.532396 | 13.673373 | 13.977726 | 13.68424 | 13.530606 | 13.653708 | 13.593822 | 14.603749 | 12.819638 |
hep-th/9304053 | null | K. Ranganathan, H. Sonoda, and B. Zwiebach | Connections on the State-Space over Conformal Field Theories | 54pp. MIT-CTP-2193 | Nucl.Phys. B414 (1994) 405-460 | 10.1016/0550-3213(94)90436-7 | null | hep-th | null | Motivated by the problem of background independence of closed string field
theory we study geometry on the infinite vector bundle of local fields over the
space of conformal field theories (CFT's). With any connection we can associate
an excluded domain $D$ for the integral of marginal operators, and an operator
one-... | [
{
"created": "Tue, 13 Apr 1993 17:40:08 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ranganathan",
"K.",
""
],
[
"Sonoda",
"H.",
""
],
[
"Zwiebach",
"B.",
""
]
] | Motivated by the problem of background independence of closed string field theory we study geometry on the infinite vector bundle of local fields over the space of conformal field theories (CFT's). With any connection we can associate an excluded domain $D$ for the integral of marginal operators, and an operator one-fo... | 9.517701 | 10.191939 | 10.700022 | 9.633409 | 10.010668 | 10.09008 | 10.310798 | 9.586048 | 9.637539 | 10.633112 | 9.208126 | 9.158202 | 9.426785 | 9.080154 | 9.076875 | 9.014537 | 9.105807 | 9.126122 | 9.33972 | 9.272181 | 9.284894 |
hep-th/0202041 | Giovanni Feverati | Giovanni Feverati, Paul A. Pearce and Francesco Ravanini | Lattice Approach to Excited TBA Boundary Flows: Tricritical Ising Model | 11 pages, 3 figures, LaTeX; v2: some useful notations and one
reference added; to appear in PLB | Phys.Lett. B534 (2002) 216-223 | 10.1016/S0370-2693(02)01648-9 | null | hep-th | null | We show how a lattice approach can be used to derive Thermodynamic Bethe
Ansatz (TBA) equations describing all excitations for boundary flows. The
method is illustrated for a prototypical flow of the tricritical Ising model by
considering the continuum scaling limit of the A4 lattice model with integrable
boundaries.... | [
{
"created": "Thu, 7 Feb 2002 05:54:52 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Mar 2002 00:10:47 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Feverati",
"Giovanni",
""
],
[
"Pearce",
"Paul A.",
""
],
[
"Ravanini",
"Francesco",
""
]
] | We show how a lattice approach can be used to derive Thermodynamic Bethe Ansatz (TBA) equations describing all excitations for boundary flows. The method is illustrated for a prototypical flow of the tricritical Ising model by considering the continuum scaling limit of the A4 lattice model with integrable boundaries. F... | 11.907014 | 8.40911 | 15.146499 | 9.932063 | 9.666279 | 9.149643 | 8.853466 | 9.508164 | 10.225752 | 16.101133 | 10.023848 | 10.963243 | 13.688482 | 11.683544 | 11.066218 | 11.641106 | 11.05635 | 11.259291 | 11.551477 | 13.357525 | 11.747952 |
0804.0851 | Richard Shurtleff | Richard Shurtleff | Quantum Fields and Translations | 25 pages, 3 figures, Version 2 corrects three typos: (i) p5 line 4
add subscript (\Phi), (ii) Eq 7, delete P factor on left, (iii) Eq 12, delete
(p) on left | null | null | null | hep-th astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Modifications of a free quantum field calculation using translation-related
concepts and general translation representations yield quantum fields for
massive particles that as a consequence follow the classical trajectories of
electrodynamics and geometrodynamics. The work allows an explanation for the
unexpectedly h... | [
{
"created": "Sun, 6 Apr 2008 11:43:55 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Apr 2008 13:41:09 GMT",
"version": "v2"
}
] | 2008-04-17 | [
[
"Shurtleff",
"Richard",
""
]
] | Modifications of a free quantum field calculation using translation-related concepts and general translation representations yield quantum fields for massive particles that as a consequence follow the classical trajectories of electrodynamics and geometrodynamics. The work allows an explanation for the unexpectedly hig... | 40.746426 | 37.076981 | 34.009453 | 32.575485 | 36.70002 | 38.575264 | 36.5196 | 33.197197 | 30.966433 | 36.237949 | 34.420471 | 35.795124 | 34.471561 | 32.091953 | 36.959126 | 35.619053 | 36.168209 | 34.956089 | 33.756989 | 32.914474 | 34.599953 |
hep-th/0602172 | Brihaye Yves | Y. Brihaye (Universite de Mons, Belgium), T. Delsate (Universite de
Mons, Belgium) and B. Hartmann (International University Bremen, Germany) | Inflating branes inside abelian strings | 14 Latex pages, 11 postscript figures; references added, discussion
extended; reference added | Phys.Rev.D74:044015,2006 | 10.1103/PhysRevD.74.044015 | null | hep-th | null | We study a 6-dimensional brane world model with an abelian string residing in
the two extra dimensions. We study both static as well as inflating branes and
find analytic solutions for the case of trivial matter fields in the bulk. Next
to singular space-times, we also find solutions which are regular including
cigar... | [
{
"created": "Fri, 17 Feb 2006 15:25:23 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Feb 2006 14:50:17 GMT",
"version": "v2"
},
{
"created": "Thu, 9 Mar 2006 16:34:04 GMT",
"version": "v3"
},
{
"created": "Mon, 26 Jun 2006 11:29:41 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Brihaye",
"Y.",
"",
"Universite de Mons, Belgium"
],
[
"Delsate",
"T.",
"",
"Universite de\n Mons, Belgium"
],
[
"Hartmann",
"B.",
"",
"International University Bremen, Germany"
]
] | We study a 6-dimensional brane world model with an abelian string residing in the two extra dimensions. We study both static as well as inflating branes and find analytic solutions for the case of trivial matter fields in the bulk. Next to singular space-times, we also find solutions which are regular including cigar-l... | 13.172837 | 12.029717 | 12.643365 | 11.507956 | 12.450312 | 12.457284 | 12.496861 | 11.536491 | 12.452797 | 13.323143 | 12.150818 | 11.990517 | 12.208177 | 11.994934 | 12.043113 | 11.715303 | 12.171352 | 11.949407 | 12.267889 | 12.438608 | 11.837404 |
hep-th/0108086 | Pat Malone | D.G.C. McKeon (University of Western Ontario), T.N. Sherry (National
University of Ireland, Galway) | AdS2 Models in an Embedding Superspace | null | null | null | null | hep-th | null | An embedding superspace, whose Bosonic part is the flat 2 + 1 dimensional
embedding space for AdS2, is introduced. Superfields and several supersymmetric
models are examined in the embedded AdS2 superspace.
| [
{
"created": "Mon, 13 Aug 2001 15:05:14 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Nov 2002 17:18:28 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"McKeon",
"D. G. C.",
"",
"University of Western Ontario"
],
[
"Sherry",
"T. N.",
"",
"National\n University of Ireland, Galway"
]
] | An embedding superspace, whose Bosonic part is the flat 2 + 1 dimensional embedding space for AdS2, is introduced. Superfields and several supersymmetric models are examined in the embedded AdS2 superspace. | 17.121302 | 11.650146 | 14.260702 | 12.667962 | 13.880297 | 14.569617 | 14.108997 | 12.261737 | 13.343472 | 16.024147 | 12.862892 | 12.807357 | 13.829011 | 12.621248 | 12.346457 | 13.991707 | 13.403821 | 12.569966 | 13.745461 | 13.058831 | 13.174396 |
2208.11501 | Nicolas Boulanger | Nicolas Boulanger, Paul P. Cook, Josh A. O'Connor and Peter West | Higher dualisations of linearised gravity and the $A_1^{+++}$ algebra | 46 pages, no figures. Published version. One reference added, some
content moved to an appendix | null | 10.1007/JHEP12(2022)152 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The non-linear realisation based on $A_1^{+++}$ is known to describe gravity
in terms of both the graviton and the dual graviton. We extend this analysis at
the linearised level to find the equations of motion for the first higher dual
description of gravity that it contains. We also give a systematic method for
find... | [
{
"created": "Wed, 24 Aug 2022 12:52:28 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jun 2023 13:49:08 GMT",
"version": "v2"
}
] | 2023-06-13 | [
[
"Boulanger",
"Nicolas",
""
],
[
"Cook",
"Paul P.",
""
],
[
"O'Connor",
"Josh A.",
""
],
[
"West",
"Peter",
""
]
] | The non-linear realisation based on $A_1^{+++}$ is known to describe gravity in terms of both the graviton and the dual graviton. We extend this analysis at the linearised level to find the equations of motion for the first higher dual description of gravity that it contains. We also give a systematic method for findin... | 11.496196 | 9.167467 | 12.061248 | 9.379776 | 9.542099 | 9.080315 | 9.678953 | 9.642985 | 10.326114 | 12.843562 | 9.41475 | 10.232766 | 11.52727 | 10.379317 | 9.998801 | 10.286374 | 9.397532 | 10.008404 | 10.505467 | 11.374002 | 10.116604 |
1511.02167 | Sudarshan Fernando | Sudarshan Fernando, Murat Gunaydin | Massless conformal fields, AdS_{d+1}/CFT_d higher spin algebras and
their deformations | 41 pages; LaTeX file; Minor improvements in presentation; Typos
corrected; References added; Version published in NPB | Nucl.Phys.B 904: 494-526, 2016 | 10.1016/j.nuclphysb.2016.01.024 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend our earlier work on the minimal unitary representation of $SO(d,2)$
and its deformations for $d=4,5$ and $6$ to arbitrary dimensions $d$. We show
that there is a one-to-one correspondence between the minrep of $SO(d,2)$ and
its deformations and massless conformal fields in Minkowskian spacetimes in $d$
dime... | [
{
"created": "Fri, 6 Nov 2015 17:19:55 GMT",
"version": "v1"
},
{
"created": "Sun, 15 Nov 2015 16:24:58 GMT",
"version": "v2"
},
{
"created": "Mon, 8 Feb 2016 19:24:36 GMT",
"version": "v3"
}
] | 2016-02-17 | [
[
"Fernando",
"Sudarshan",
""
],
[
"Gunaydin",
"Murat",
""
]
] | We extend our earlier work on the minimal unitary representation of $SO(d,2)$ and its deformations for $d=4,5$ and $6$ to arbitrary dimensions $d$. We show that there is a one-to-one correspondence between the minrep of $SO(d,2)$ and its deformations and massless conformal fields in Minkowskian spacetimes in $d$ dimens... | 5.464532 | 5.082484 | 6.075755 | 5.143374 | 5.290046 | 5.228451 | 5.095811 | 4.942143 | 4.982245 | 6.339581 | 5.048496 | 5.350823 | 5.409499 | 5.152279 | 5.148581 | 5.195693 | 5.23287 | 5.122373 | 5.111332 | 5.658494 | 5.111855 |
hep-th/9903042 | Debashis Ghoshal | Stefan Forste (U.Bonn), Debashis Ghoshal (MRI) and Stefan Theisen
(U.Munich) | Stringy Corrections to the Wilson Loop in N=4 Super Yang-Mills Theory | 14 pages, harvmac (b) | JHEP 9908 (1999) 013 | 10.1088/1126-6708/1999/08/013 | MRI-PHY/P990204 | hep-th | null | We study stringy fluctuations as a source for corrections to the Wilson loop
as obtained from the superstrings on (adS_5 x S^5)/ N=4 SYM correspondence. We
give a formal expression in terms of determinants of two dimensional operators
for the leading order correction.
| [
{
"created": "Thu, 4 Mar 1999 17:06:45 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Forste",
"Stefan",
"",
"U.Bonn"
],
[
"Ghoshal",
"Debashis",
"",
"MRI"
],
[
"Theisen",
"Stefan",
"",
"U.Munich"
]
] | We study stringy fluctuations as a source for corrections to the Wilson loop as obtained from the superstrings on (adS_5 x S^5)/ N=4 SYM correspondence. We give a formal expression in terms of determinants of two dimensional operators for the leading order correction. | 16.269121 | 15.373816 | 16.155151 | 14.936251 | 16.854872 | 18.254255 | 13.201764 | 15.054865 | 15.540722 | 18.571932 | 14.812757 | 13.9866 | 15.118649 | 15.250303 | 14.610149 | 14.488851 | 14.463234 | 14.430017 | 15.029796 | 15.461499 | 14.648275 |
1111.4529 | Jaemo Park | Dongmin Gang, Chiung Hwang, Seok Kim and Jaemo Park | Tests of AdS$_4$/CFT$_3$ correspondence for $\mathcal{N}=2$ chiral-like
theory | 16 pages, 1 figure; typos corrected, references added | null | 10.1007/JHEP02(2012)079 | SNUTP11-010; KIAS-P12011 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the superconformal index and the partition function for the
chiral-like Chern-Simons-matter theory proposed for M2-branes probing the cones
over $M^{3,2}$ and find perfect agreements with the gravity index and the
gravitational free energy.
| [
{
"created": "Sat, 19 Nov 2011 03:16:36 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Jan 2012 23:52:02 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Gang",
"Dongmin",
""
],
[
"Hwang",
"Chiung",
""
],
[
"Kim",
"Seok",
""
],
[
"Park",
"Jaemo",
""
]
] | We investigate the superconformal index and the partition function for the chiral-like Chern-Simons-matter theory proposed for M2-branes probing the cones over $M^{3,2}$ and find perfect agreements with the gravity index and the gravitational free energy. | 15.031573 | 9.878529 | 18.641495 | 10.439884 | 9.782241 | 12.063146 | 11.455614 | 11.86596 | 11.007939 | 19.621519 | 10.243059 | 11.878333 | 17.986326 | 12.642722 | 12.298369 | 12.168288 | 12.423039 | 12.22928 | 11.801979 | 15.230118 | 11.844634 |
0806.4692 | M. B. Paranjape | Avinash Khare, M. B. Paranjape | Suppression of quantum tunneling for all spins for easy-axis systems | 4 pages, no figures, | null | 10.1103/PhysRevB.83.172401 | UdeM-GPP-TH-08-168 | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The semi-classical limit of quantum spin systems corresponds to a dynamical
Lagrangian which contains the usual kinetic energy, the couplings and
interactions of the spins and an additional, first order kinematical term which
corresponds to the Wess-Zumino-Novikov-Witten (WZNW) term for the spin degree
of freedom \ci... | [
{
"created": "Sat, 28 Jun 2008 15:15:20 GMT",
"version": "v1"
}
] | 2013-05-29 | [
[
"Khare",
"Avinash",
""
],
[
"Paranjape",
"M. B.",
""
]
] | The semi-classical limit of quantum spin systems corresponds to a dynamical Lagrangian which contains the usual kinetic energy, the couplings and interactions of the spins and an additional, first order kinematical term which corresponds to the Wess-Zumino-Novikov-Witten (WZNW) term for the spin degree of freedom \cite... | 14.911087 | 16.024315 | 15.435106 | 14.557792 | 14.667328 | 15.39331 | 14.424314 | 14.434053 | 14.52657 | 16.009329 | 14.792047 | 14.358548 | 14.673884 | 14.505475 | 14.248655 | 14.587258 | 14.328984 | 14.390295 | 14.626398 | 15.296911 | 14.549658 |
hep-th/0401076 | Laurent Freidel | Laurent Freidel and David Louapre | Ponzano-Regge model revisited I: Gauge fixing, observables and
interacting spinning particles | 48 pages, 15 figures | Class.Quant.Grav. 21 (2004) 5685-5726 | 10.1088/0264-9381/21/24/002 | null | hep-th gr-qc | null | We show how to properly gauge fix all the symmetries of the Ponzano-Regge
model for 3D quantum gravity. This amounts to do explicit finite computations
for transition amplitudes. We give the construction of the transition
amplitudes in the presence of interacting quantum spinning particles. We
introduce a notion of o... | [
{
"created": "Mon, 12 Jan 2004 21:13:31 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Freidel",
"Laurent",
""
],
[
"Louapre",
"David",
""
]
] | We show how to properly gauge fix all the symmetries of the Ponzano-Regge model for 3D quantum gravity. This amounts to do explicit finite computations for transition amplitudes. We give the construction of the transition amplitudes in the presence of interacting quantum spinning particles. We introduce a notion of ope... | 11.093522 | 10.837521 | 10.455385 | 9.949659 | 11.375738 | 10.475881 | 10.382884 | 9.700565 | 10.156942 | 10.275099 | 9.957538 | 10.404575 | 10.207352 | 10.025427 | 10.126563 | 10.122379 | 10.137878 | 9.630874 | 10.221791 | 10.047898 | 10.239449 |
hep-th/0406252 | Ruth Gregory | Ruth Gregory, Richard Whisker, Kris Beckwith, Chris Done | Observing braneworld black holes | 25 pages latex JHEP style, 3 figures | JCAP 0410:013,2004 | 10.1088/1475-7516/2004/10/013 | IPPP/04/33, DCPT/04/66 | hep-th astro-ph hep-ph | null | Spacetime in the vicinity of an event horizon can be probed using
observations which explore the dynamics of the accretion disc. Many high energy
theories of gravity lead to modifications of the near horizon regime,
potentially providing a testing ground for these theories. In this paper, we
explore the impact of bra... | [
{
"created": "Mon, 28 Jun 2004 08:22:56 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Gregory",
"Ruth",
""
],
[
"Whisker",
"Richard",
""
],
[
"Beckwith",
"Kris",
""
],
[
"Done",
"Chris",
""
]
] | Spacetime in the vicinity of an event horizon can be probed using observations which explore the dynamics of the accretion disc. Many high energy theories of gravity lead to modifications of the near horizon regime, potentially providing a testing ground for these theories. In this paper, we explore the impact of brane... | 13.752214 | 12.629951 | 12.217308 | 11.33359 | 11.880911 | 13.828684 | 13.1113 | 12.656531 | 12.790403 | 12.926432 | 13.114166 | 12.255073 | 11.610018 | 11.722104 | 11.914805 | 11.967661 | 11.707188 | 11.998581 | 11.816011 | 11.669767 | 11.942005 |
2102.12779 | Matsuo Sato | Masaki Honda, Matsuo Sato, Taiki Tohshima | Superstring Backgrounds in String Geometry | 15 pages. arXiv admin note: text overlap with arXiv:2003.12487 | Adv.High Energy Phys. 2021 (2021) 9993903 | 10.1155/2021/9993903 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | String geometry theory is a candidate of the non-perturbative formulation of
string theory. In order to determine the string vacuum, we need to clarify how
superstring backgrounds are described in string geometry theory. In this paper,
we show that all the type IIA, IIB, SO(32) type I, and SO(32) and $E_8 \times
E_8$... | [
{
"created": "Thu, 25 Feb 2021 10:54:20 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Jun 2021 10:16:50 GMT",
"version": "v2"
}
] | 2022-02-01 | [
[
"Honda",
"Masaki",
""
],
[
"Sato",
"Matsuo",
""
],
[
"Tohshima",
"Taiki",
""
]
] | String geometry theory is a candidate of the non-perturbative formulation of string theory. In order to determine the string vacuum, we need to clarify how superstring backgrounds are described in string geometry theory. In this paper, we show that all the type IIA, IIB, SO(32) type I, and SO(32) and $E_8 \times E_8$ h... | 6.463414 | 4.810295 | 6.54359 | 5.314942 | 5.764261 | 5.925915 | 5.740317 | 4.741206 | 5.306929 | 7.099391 | 5.616529 | 5.894319 | 6.308244 | 5.900724 | 6.043914 | 5.858628 | 6.041113 | 5.966857 | 5.958618 | 6.342041 | 6.011179 |
1207.2333 | Aninda Sinha | Arpan Bhattacharyya, Ling-Yan Hung, Kallol Sen and Aninda Sinha | On c-theorems in arbitrary dimensions | 25 pages, v3: reference added, Cotton tensor dependence of
counterterm at eight-derivative order shown, v4: published version | Phys. Rev. D 86, 106006 (2012) | 10.1103/PhysRevD.86.106006 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dilaton action in 3+1 dimensions plays a crucial role in the proof of the
a-theorem. This action arises using Wess-Zumino consistency conditions and
crucially relies on the existence of the trace anomaly. Since there are no
anomalies in odd dimensions, it is interesting to ask how such an action could
arise other... | [
{
"created": "Tue, 10 Jul 2012 12:38:30 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Jul 2012 07:18:19 GMT",
"version": "v2"
},
{
"created": "Thu, 9 Aug 2012 10:41:29 GMT",
"version": "v3"
},
{
"created": "Tue, 20 Nov 2012 06:29:04 GMT",
"version": "v4"
}
] | 2013-05-30 | [
[
"Bhattacharyya",
"Arpan",
""
],
[
"Hung",
"Ling-Yan",
""
],
[
"Sen",
"Kallol",
""
],
[
"Sinha",
"Aninda",
""
]
] | The dilaton action in 3+1 dimensions plays a crucial role in the proof of the a-theorem. This action arises using Wess-Zumino consistency conditions and crucially relies on the existence of the trace anomaly. Since there are no anomalies in odd dimensions, it is interesting to ask how such an action could arise otherwi... | 8.774792 | 8.275942 | 8.992911 | 8.05437 | 8.395178 | 8.384672 | 8.406251 | 7.805882 | 7.750659 | 9.06253 | 7.891958 | 8.091105 | 8.698805 | 8.151177 | 8.337786 | 8.247468 | 7.865984 | 8.15849 | 7.97514 | 8.796134 | 8.50633 |
hep-th/0703163 | Xin-Hui Zhang | Yi-Shi Duan, Xin-Hui Zhang and Li Zhao | Topological aspect of black hole with Skyrme hair | 10 pages,0 figures | Int.J.Mod.Phys.A21:5895-5904,2006 | 10.1142/S0217751X06033994 | null | hep-th | null | Based on the $\phi$-mapping topological current theory, we show that the
presence of the black hole leaves fractional baryon charge outside the horizon
in the Einstein-Skyrme theory. A topological current is derived from the
Einstein-Skyrme system, which corresponds to the monopoles around the black
hole. The branch ... | [
{
"created": "Mon, 19 Mar 2007 02:27:59 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Duan",
"Yi-Shi",
""
],
[
"Zhang",
"Xin-Hui",
""
],
[
"Zhao",
"Li",
""
]
] | Based on the $\phi$-mapping topological current theory, we show that the presence of the black hole leaves fractional baryon charge outside the horizon in the Einstein-Skyrme theory. A topological current is derived from the Einstein-Skyrme system, which corresponds to the monopoles around the black hole. The branch pr... | 15.460965 | 9.443213 | 13.125105 | 9.344148 | 10.346156 | 10.754467 | 11.117317 | 9.136971 | 9.879748 | 13.090669 | 10.069808 | 12.302472 | 13.420689 | 12.385983 | 12.821603 | 12.500422 | 12.54281 | 11.951193 | 12.581552 | 13.336843 | 13.456375 |
1511.08208 | Mirjam Cvtic | Mirjam Cvetic, Antonella Grassi, Denis Klevers, Maximilian
Poretschkin, Peng Song | Origin of Abelian Gauge Symmetries in Heterotic/F-theory Duality | 52 pages, 15 figures | null | 10.1007/JHEP04(2016)041 | UPR-1275-T CERN-PH-TH-2015-273 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study aspects of heterotic/F-theory duality for compactifications with
Abelian gauge symmetries. We consider F-theory on general Calabi-Yau manifolds
with a rank one Mordell-Weil group of rational sections. By rigorously
performing the stable degeneration limit in a class of toric models, we derive
both the Calabi... | [
{
"created": "Wed, 25 Nov 2015 20:59:35 GMT",
"version": "v1"
}
] | 2016-05-04 | [
[
"Cvetic",
"Mirjam",
""
],
[
"Grassi",
"Antonella",
""
],
[
"Klevers",
"Denis",
""
],
[
"Poretschkin",
"Maximilian",
""
],
[
"Song",
"Peng",
""
]
] | We study aspects of heterotic/F-theory duality for compactifications with Abelian gauge symmetries. We consider F-theory on general Calabi-Yau manifolds with a rank one Mordell-Weil group of rational sections. By rigorously performing the stable degeneration limit in a class of toric models, we derive both the Calabi-Y... | 3.529967 | 6.027524 | 6.856495 | 5.565096 | 5.939488 | 6.121408 | 5.922688 | 5.713701 | 5.639492 | 6.715305 | 5.712792 | 5.191391 | 5.519803 | 5.165298 | 5.080349 | 5.208339 | 5.22851 | 5.155247 | 4.861064 | 5.456875 | 5.049258 |
hep-th/0501191 | Laurent Freidel | Laurent Freidel, Artem Starodubtsev | Quantum gravity in terms of topological observables | 19 pages | null | null | null | hep-th gr-qc | null | We recast the action principle of four dimensional General Relativity so that
it becomes amenable for perturbation theory which doesn't break general
covariance. The coupling constant becomes dimensionless (G_{Newton} \Lambda)
and extremely small 10^{-120}. We give an expression for the generating
functional of pertu... | [
{
"created": "Mon, 24 Jan 2005 17:29:34 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Feb 2005 22:07:06 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Freidel",
"Laurent",
""
],
[
"Starodubtsev",
"Artem",
""
]
] | We recast the action principle of four dimensional General Relativity so that it becomes amenable for perturbation theory which doesn't break general covariance. The coupling constant becomes dimensionless (G_{Newton} \Lambda) and extremely small 10^{-120}. We give an expression for the generating functional of perturb... | 10.881911 | 11.256709 | 10.551335 | 9.496286 | 10.508353 | 9.989833 | 10.138391 | 9.630834 | 9.805606 | 11.131763 | 9.930172 | 9.462336 | 9.911271 | 9.475176 | 9.710304 | 9.454528 | 9.886897 | 9.516047 | 9.980271 | 9.888373 | 9.386812 |
0903.2581 | Vassilios Zamarias | Vassilios Zamarias | Conical singularities regularized in warped six-dimensional flux
compactification and their induced brane cosmology | 14 pages | J.Phys.Conf.Ser.189:012047,2009 | 10.1088/1742-6596/189/1/012047 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the regularization of codimension-2 singularities in warped
six-dimensional Einstein-Maxwell axisymmetric models by replacing them by
codimension-1 branes of a ring form, situated around the axis of symmetry.
Further we consider the case of one capped regularized conical brane of
codimension one and study ... | [
{
"created": "Sat, 14 Mar 2009 21:41:53 GMT",
"version": "v1"
}
] | 2009-11-05 | [
[
"Zamarias",
"Vassilios",
""
]
] | We discuss the regularization of codimension-2 singularities in warped six-dimensional Einstein-Maxwell axisymmetric models by replacing them by codimension-1 branes of a ring form, situated around the axis of symmetry. Further we consider the case of one capped regularized conical brane of codimension one and study th... | 18.525652 | 14.989687 | 18.488323 | 15.762123 | 15.476702 | 15.026153 | 15.868578 | 15.482267 | 15.887444 | 19.105999 | 16.370813 | 16.158903 | 17.6532 | 16.811256 | 16.444061 | 16.945614 | 16.824709 | 16.521057 | 16.509693 | 17.992008 | 17.120518 |
0810.2236 | Jose M. Isidro | S. Abraham, P. Fernandez de Cordoba, J.M. Isidro, J.L.G. Santander | The Ricci flow on Riemann surfaces | 7 pages, refs. added, minor corrections | JP J.Geom.Topol.9:215-223,2009 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish a 1-to-1 relation between metrics on compact Riemann surfaces
without boundary, and mechanical systems having those surfaces as configuration
spaces.
| [
{
"created": "Mon, 13 Oct 2008 13:45:19 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Oct 2008 14:27:14 GMT",
"version": "v2"
},
{
"created": "Mon, 8 Dec 2008 20:01:38 GMT",
"version": "v3"
}
] | 2010-02-10 | [
[
"Abraham",
"S.",
""
],
[
"de Cordoba",
"P. Fernandez",
""
],
[
"Isidro",
"J. M.",
""
],
[
"Santander",
"J. L. G.",
""
]
] | We establish a 1-to-1 relation between metrics on compact Riemann surfaces without boundary, and mechanical systems having those surfaces as configuration spaces. | 14.744425 | 10.414177 | 13.595697 | 11.46611 | 11.167017 | 12.557604 | 12.610457 | 11.570511 | 11.392639 | 14.49099 | 12.420409 | 13.642914 | 14.173036 | 13.93731 | 13.854171 | 12.857809 | 13.910965 | 13.746334 | 14.520123 | 14.671262 | 13.00777 |
1910.13061 | Andr\'es Fabio Goya | Gaston Giribet, Andres Goya, Edmundo Lavia, Julio Oliva | Critical points of the Exotic Massive 3D Gravity | 14 pages, 1 figure | null | 10.1016/j.physletb.2020.135618 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Exotic Massive 3D Gravity (EMG) is a higher order generalization of
Topologically Massive Gravity. As in other theories of this sort, the conserved
charges associated to the asymptotic diffeomorphisms that preserve the boundary
conditions in AdS3 spacetime span two copies of the Virasoro algebra with
non-vanishing ce... | [
{
"created": "Tue, 29 Oct 2019 03:05:11 GMT",
"version": "v1"
}
] | 2020-07-22 | [
[
"Giribet",
"Gaston",
""
],
[
"Goya",
"Andres",
""
],
[
"Lavia",
"Edmundo",
""
],
[
"Oliva",
"Julio",
""
]
] | Exotic Massive 3D Gravity (EMG) is a higher order generalization of Topologically Massive Gravity. As in other theories of this sort, the conserved charges associated to the asymptotic diffeomorphisms that preserve the boundary conditions in AdS3 spacetime span two copies of the Virasoro algebra with non-vanishing cent... | 7.332954 | 6.01469 | 7.284747 | 6.119077 | 6.335954 | 5.653677 | 5.594667 | 5.633638 | 6.065788 | 7.182478 | 6.097011 | 5.871839 | 6.75281 | 6.341553 | 6.367121 | 6.162009 | 6.113826 | 6.013598 | 6.569788 | 7.351478 | 6.184587 |
0707.0894 | Tsutomu Kobayashi | Tsutomu Kobayashi, Yu-ichi Takamizu | Hybrid compactifications and brane gravity in six dimensions | 15 pages, 2 figures; v2: references added; v3: accepted for
publication in Class. Quant. Grav | Class.Quant.Grav.25:015007,2007 | 10.1088/0264-9381/25/1/015007 | WU-AP/271/07 | hep-th gr-qc | null | We consider a six-dimensional axisymmetric Einstein-Maxwell model of warped
braneworlds. The bulk is bounded by two branes, one of which is a conical
3-brane and the other is a 4-brane wrapped around the axis of symmetry. The
latter brane is assumed to be our universe. If the tension of the 3-brane is
fine-tuned, it ... | [
{
"created": "Fri, 6 Jul 2007 01:37:42 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Jul 2007 13:09:47 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Nov 2007 01:33:42 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Kobayashi",
"Tsutomu",
""
],
[
"Takamizu",
"Yu-ichi",
""
]
] | We consider a six-dimensional axisymmetric Einstein-Maxwell model of warped braneworlds. The bulk is bounded by two branes, one of which is a conical 3-brane and the other is a 4-brane wrapped around the axis of symmetry. The latter brane is assumed to be our universe. If the tension of the 3-brane is fine-tuned, it fo... | 7.969478 | 7.432383 | 8.428198 | 7.649282 | 7.976755 | 7.7633 | 8.090369 | 7.857347 | 7.606291 | 8.53986 | 7.424167 | 7.822996 | 7.725786 | 7.612681 | 7.640775 | 7.724948 | 7.927882 | 7.476333 | 7.729908 | 7.696207 | 7.77397 |
hep-th/9807165 | Fabian Gaioli | Edgardo T. Garcia Alvarez and Fabian H. Gaioli | On the quantum electrodynamics of moving bodies | 21 pages, 2 figures, Latex | Int.J.Theor.Phys. 36 (1997) 2391-2407 | null | null | hep-th | null | A new synthesis of the principles of relativity and quantum mechanics is
developed by replacing the Poincar\'e group for the de Sitter one. The new
relativistic quantum mechanics is an indefinite mass theory which is reduced to
the standard theory on the mass shell. The charge conjugation acquires a
geometrical meani... | [
{
"created": "Tue, 21 Jul 1998 23:40:03 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Alvarez",
"Edgardo T. Garcia",
""
],
[
"Gaioli",
"Fabian H.",
""
]
] | A new synthesis of the principles of relativity and quantum mechanics is developed by replacing the Poincar\'e group for the de Sitter one. The new relativistic quantum mechanics is an indefinite mass theory which is reduced to the standard theory on the mass shell. The charge conjugation acquires a geometrical meaning... | 9.584727 | 9.478525 | 8.784922 | 8.633625 | 9.27292 | 9.257108 | 9.130986 | 8.720616 | 8.933978 | 9.012742 | 9.057506 | 9.022045 | 8.487908 | 8.48442 | 8.465989 | 8.456509 | 8.682425 | 8.279151 | 8.462301 | 8.503233 | 8.504383 |
1008.3980 | Ali Chamseddine | Ali H. Chamseddine and Alain Connes | Noncommutative Geometric Spaces with Boundary: Spectral Action | 26 pages | J.Geom.Phys.61:317-332,2011 | 10.1016/j.geomphys.2010.10.002 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study spectral action for Riemannian manifolds with boundary, and then
generalize this to noncommutative spaces which are products of a Riemannian
manifold times a finite space. We determine the boundary conditions consistent
with the hermiticity of the Dirac operator. We then define spectral triples of
noncommuta... | [
{
"created": "Tue, 24 Aug 2010 08:03:40 GMT",
"version": "v1"
}
] | 2010-11-23 | [
[
"Chamseddine",
"Ali H.",
""
],
[
"Connes",
"Alain",
""
]
] | We study spectral action for Riemannian manifolds with boundary, and then generalize this to noncommutative spaces which are products of a Riemannian manifold times a finite space. We determine the boundary conditions consistent with the hermiticity of the Dirac operator. We then define spectral triples of noncommutati... | 7.791184 | 7.369534 | 8.106867 | 7.538962 | 7.893296 | 8.711507 | 8.082339 | 7.449716 | 7.868743 | 8.325835 | 7.002388 | 7.493903 | 7.753389 | 7.568699 | 7.148963 | 7.047882 | 7.624721 | 7.057034 | 7.061603 | 7.801437 | 6.947068 |
0910.3722 | Shingo Takeuchi | Yoshinori Matsuo, Sang-Jin Sin, Shingo Takeuchi, Takuya Tsukioka | Magnetic conductivity and Chern-Simons Term in Holographic Hydrodynamics
of Charged AdS Black Hole | 19 pages, 2 figures; v2 discussion on classification of perturbation
fields based on helicity base, third order in dispersion relation and more
discussion on magnetic conductivity are added, some typos are corrected and
references are added; v3 published version | JHEP 1004:071,2010 | 10.1007/JHEP04(2010)071 | APCTP-Pre2009-011 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the effects of the Chern-Simons term in the hydrodynamics of the
five-dimensional Reissner-Nordstrom-AdS background. We work out the decoupling
problem of the equations of motion and calculate the retarded Green functions
explicitly. We then find that the Chern-Simons term induces the magnetic
conductivity c... | [
{
"created": "Tue, 20 Oct 2009 17:15:16 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Mar 2010 19:40:04 GMT",
"version": "v2"
},
{
"created": "Sun, 23 May 2010 15:12:08 GMT",
"version": "v3"
}
] | 2010-05-27 | [
[
"Matsuo",
"Yoshinori",
""
],
[
"Sin",
"Sang-Jin",
""
],
[
"Takeuchi",
"Shingo",
""
],
[
"Tsukioka",
"Takuya",
""
]
] | We study the effects of the Chern-Simons term in the hydrodynamics of the five-dimensional Reissner-Nordstrom-AdS background. We work out the decoupling problem of the equations of motion and calculate the retarded Green functions explicitly. We then find that the Chern-Simons term induces the magnetic conductivity cau... | 12.245934 | 10.304261 | 11.671061 | 10.515513 | 10.208299 | 9.59193 | 9.482435 | 9.685617 | 9.094332 | 11.875682 | 10.106252 | 10.597538 | 11.175421 | 10.871938 | 10.509576 | 9.984593 | 10.196229 | 10.502335 | 10.419899 | 11.48581 | 10.438553 |
hep-th/0205199 | Eve Mariel Santangelo | C.G. Beneventano, E.M. Santangelo and A. Wipf | Spectral asymmetry for bag boundary conditions | Some minor changes. To appear in Journal of Physics A: Mathematical
and General | J.Phys.A35:9343,2002 | 10.1088/0305-4470/35/44/305 | La Plata Th 02-02; FSUJ-TPI-02-02 | hep-th math-ph math.MP | null | We give an expression, in terms of boundary spectral functions, for the
spectral asymmetry of the Euclidean Dirac operator in two dimensions, when its
domain is determined by local boundary conditions, and the manifold is of
product type. As an application, we explicitly evaluate the asymmetry in the
case of a finite... | [
{
"created": "Mon, 20 May 2002 16:18:03 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Sep 2002 14:24:57 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Beneventano",
"C. G.",
""
],
[
"Santangelo",
"E. M.",
""
],
[
"Wipf",
"A.",
""
]
] | We give an expression, in terms of boundary spectral functions, for the spectral asymmetry of the Euclidean Dirac operator in two dimensions, when its domain is determined by local boundary conditions, and the manifold is of product type. As an application, we explicitly evaluate the asymmetry in the case of a finite-l... | 8.167507 | 7.844569 | 8.740685 | 7.751672 | 7.824421 | 8.408499 | 8.272851 | 9.048615 | 8.4307 | 8.950053 | 8.911534 | 8.256904 | 8.277621 | 7.634975 | 8.08039 | 8.125025 | 8.195828 | 8.286353 | 8.176896 | 8.514882 | 7.780278 |
hep-th/9209097 | null | B. Rusakov | From hermitian matrix model to lattice gauge theory | 8pages, Latex | null | null | TAUP 1996-92 | hep-th hep-lat | null | I consider a lattice model of a gauge field interacting with matrix-valued
scalars in $D$ dimensions. The model includes an adjustable parameter $\s$,
which plays role of the string tension. In the limit $\s=\infty$ the model
coincides with Kazakov-Migdal's ``induced QCD", where Wilson loops obey a zero
area law. The... | [
{
"created": "Thu, 24 Sep 1992 15:13:12 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rusakov",
"B.",
""
]
] | I consider a lattice model of a gauge field interacting with matrix-valued scalars in $D$ dimensions. The model includes an adjustable parameter $\s$, which plays role of the string tension. In the limit $\s=\infty$ the model coincides with Kazakov-Migdal's ``induced QCD", where Wilson loops obey a zero area law. The l... | 9.2139 | 8.260674 | 10.261837 | 8.4745 | 8.953305 | 8.51545 | 8.923085 | 8.59387 | 8.535262 | 10.409639 | 8.203668 | 8.459565 | 8.956318 | 8.423552 | 8.472074 | 8.209563 | 8.431347 | 8.229754 | 8.519863 | 8.978157 | 8.342428 |
hep-th/9406096 | null | C.M. Becchi, R. Collina and C. Imbimbo | A Functional and Lagrangian Formulation of Two-Dimensional Topological
Gravity | 11 pages, harvmac, CERN-TH-7302/94, GEF-Th-6/1994 | null | null | null | hep-th | null | We reconsider two-dimensional topological gravity in a functional and
lagrangian framework. We derive its Slavnov-Taylor identities and discuss its
(in)dependence on the background gauge. Correlators of reparamerization
invariant observables are shown to be globally defined forms on moduli space.
The potential obstru... | [
{
"created": "Wed, 15 Jun 1994 09:10:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Becchi",
"C. M.",
""
],
[
"Collina",
"R.",
""
],
[
"Imbimbo",
"C.",
""
]
] | We reconsider two-dimensional topological gravity in a functional and lagrangian framework. We derive its Slavnov-Taylor identities and discuss its (in)dependence on the background gauge. Correlators of reparamerization invariant observables are shown to be globally defined forms on moduli space. The potential obstruct... | 9.997436 | 9.997252 | 11.853534 | 9.839312 | 9.19226 | 8.645871 | 9.485961 | 9.800141 | 9.554815 | 11.285281 | 8.91925 | 9.13312 | 9.782173 | 9.264259 | 9.542397 | 9.481913 | 9.471992 | 9.109853 | 9.718566 | 9.583048 | 9.212029 |
hep-th/0509019 | Joshua Feinberg | Joshua Feinberg and Shlomi Hillel | Stable Fermion Bag Solitons in the Massive Gross-Neveu Model: Inverse
Scattering Analysis | 10 pages, revtex, no figures; v2: typos corrected, references added;
v3: version accepted for publication in the PRD. referencess added. Some
minor clarifications added at the beginning of section 3 | Phys.Rev. D72 (2005) 105009 | 10.1103/PhysRevD.72.105009 | null | hep-th | null | Formation of fermion bag solitons is an important paradigm in the theory of
hadron structure. We study this phenomenon non-perturbatively in the 1+1
dimensional Massive Gross-Neveu model, in the large $N$ limit. We find,
applying inverse scattering techniques, that the extremal static bag
configurations are reflectio... | [
{
"created": "Thu, 1 Sep 2005 23:19:14 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Sep 2005 19:37:52 GMT",
"version": "v2"
},
{
"created": "Fri, 28 Oct 2005 21:33:59 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Feinberg",
"Joshua",
""
],
[
"Hillel",
"Shlomi",
""
]
] | Formation of fermion bag solitons is an important paradigm in the theory of hadron structure. We study this phenomenon non-perturbatively in the 1+1 dimensional Massive Gross-Neveu model, in the large $N$ limit. We find, applying inverse scattering techniques, that the extremal static bag configurations are reflectionl... | 9.414289 | 9.07198 | 9.565996 | 8.886819 | 8.733555 | 9.057214 | 8.54847 | 9.247115 | 8.686768 | 9.705031 | 9.033416 | 8.730252 | 8.972482 | 8.863042 | 9.097904 | 8.893843 | 8.966061 | 8.940764 | 8.762923 | 9.013381 | 8.866926 |
2206.06187 | Erik Tonni | Mihail Mintchev, Diego Pontello, Erik Tonni | Entanglement entropies of an interval in the free Schr\"odinger field
theory on the half line | 54 pages, 11 figures | JHEP 09 (2022) 090 | 10.1007/JHEP09(2022)090 | null | hep-th cond-mat.stat-mech math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the entanglement entropies of an interval adjacent to the boundary
of the half line for the free fermionic spinless Schr\"odinger field theory at
finite density and zero temperature, with either Neumann or Dirichlet boundary
conditions. They are finite functions of the dimensionless parameter given by
the pr... | [
{
"created": "Mon, 13 Jun 2022 14:21:37 GMT",
"version": "v1"
}
] | 2022-09-20 | [
[
"Mintchev",
"Mihail",
""
],
[
"Pontello",
"Diego",
""
],
[
"Tonni",
"Erik",
""
]
] | We study the entanglement entropies of an interval adjacent to the boundary of the half line for the free fermionic spinless Schr\"odinger field theory at finite density and zero temperature, with either Neumann or Dirichlet boundary conditions. They are finite functions of the dimensionless parameter given by the prod... | 7.374535 | 7.270637 | 8.404755 | 6.973004 | 7.410451 | 7.33716 | 6.99337 | 6.950572 | 6.759912 | 8.929272 | 7.466646 | 6.89075 | 8.066617 | 7.09442 | 7.175603 | 7.108245 | 6.843945 | 7.406578 | 7.282575 | 7.927026 | 7.023194 |
hep-th/0606018 | Hiroshi Umetsu | Satoshi Iso, Hiroshi Umetsu, Frank Wilczek | Anomalies, Hawking Radiations and Regularity in Rotating Black Holes | 21 pages, minor corrections, added an appendix to summarize our
notations for the Kaluza-Klein reduction | Phys.Rev.D74:044017,2006 | 10.1103/PhysRevD.74.044017 | MIT-CTP-3730, KEK-TH-1077, OIQP-06-02 | hep-th gr-qc hep-ph | null | This is an extended version of our previous letter hep-th/0602146. In this
paper we consider rotating black holes and show that the flux of Hawking
radiation can be determined by anomaly cancellation conditions and regularity
requirement at the horizon. By using a dimensional reduction technique, each
partial wave of... | [
{
"created": "Fri, 2 Jun 2006 10:36:18 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Jan 2008 02:09:12 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Mar 2008 06:27:00 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Iso",
"Satoshi",
""
],
[
"Umetsu",
"Hiroshi",
""
],
[
"Wilczek",
"Frank",
""
]
] | This is an extended version of our previous letter hep-th/0602146. In this paper we consider rotating black holes and show that the flux of Hawking radiation can be determined by anomaly cancellation conditions and regularity requirement at the horizon. By using a dimensional reduction technique, each partial wave of q... | 9.803472 | 8.345058 | 10.057443 | 8.942143 | 8.720923 | 8.608715 | 8.178425 | 8.23251 | 8.593451 | 10.009568 | 8.310317 | 8.716004 | 9.247752 | 8.774418 | 8.983787 | 8.842495 | 8.683679 | 8.938258 | 8.907061 | 9.399826 | 8.86544 |
hep-th/9802140 | Ingo Gaida | Ingo Gaida (DAMTP, University of Cambridge) | N = 2 Supersymmetric Quantum Black Holes in Five Dimensional Heterotic
String Vacua | 11 pages, standard latex | Phys.Lett. B429 (1998) 297-303 | 10.1016/S0370-2693(98)00446-8 | DAMTP-98-11 | hep-th | null | Exact black hole solutions of the five dimensional heterotic $S$-$T$-$U$
model including all perturbative quantum corrections and preserving $1/2$ of
$N=2$ supersymmetry are studied. It is shown that the quantum corrections yield
a bound on electric charges and harmonic functions of the solutions.
| [
{
"created": "Fri, 20 Feb 1998 10:28:56 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Gaida",
"Ingo",
"",
"DAMTP, University of Cambridge"
]
] | Exact black hole solutions of the five dimensional heterotic $S$-$T$-$U$ model including all perturbative quantum corrections and preserving $1/2$ of $N=2$ supersymmetry are studied. It is shown that the quantum corrections yield a bound on electric charges and harmonic functions of the solutions. | 12.352695 | 9.001814 | 12.044825 | 9.211448 | 9.142879 | 8.755222 | 9.695779 | 8.227624 | 7.828146 | 10.861364 | 10.677567 | 9.293753 | 9.942175 | 9.155013 | 9.691609 | 9.631481 | 9.549277 | 9.486245 | 9.02846 | 9.708168 | 9.47051 |
hep-th/9903039 | Marco Laucelli Meana | Marco Laucelli Meana and Jes\'us Puente Pe\~nalba | On the microcanonical description of D-brane thermodynamics | LaTeX 27 pages, 5 figures, Also avalable at
http://condmat1.ciencias.uniovi.es (V2)Minor changes, references added and a
clarification of the role of the ND and DN directions | Nucl.Phys. B560 (1999) 154-180 | null | FFUOV-99/03 | hep-th | null | We study the microcanonical description of string gases in the presence of
D-branes. We obtain exact expressions for the single string density of states
and draw the regions in phase space where asymptotic approximations are valid.
We are able to describe the whole range of energies including the SYM phase of
the D-b... | [
{
"created": "Wed, 3 Mar 1999 18:30:14 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Mar 1999 19:50:18 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Meana",
"Marco Laucelli",
""
],
[
"Peñalba",
"Jesús Puente",
""
]
] | We study the microcanonical description of string gases in the presence of D-branes. We obtain exact expressions for the single string density of states and draw the regions in phase space where asymptotic approximations are valid. We are able to describe the whole range of energies including the SYM phase of the D-bra... | 11.865695 | 10.951671 | 13.105533 | 11.318216 | 11.663845 | 11.369683 | 10.888595 | 10.907728 | 11.054576 | 12.732017 | 11.398344 | 11.073786 | 11.409773 | 10.689574 | 10.902713 | 10.901842 | 10.720355 | 10.94687 | 10.999285 | 11.138414 | 10.784532 |
0910.3680 | Richard Hill | Richard J. Hill | SU(3)/SU(2): the simplest Wess-Zumino-Witten term | 11 pages, 1 figure; references added | Phys.Rev.D81:065032,2010 | 10.1103/PhysRevD.81.065032 | EFI Preprint 09-23 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The observation that SU(3)/SU(2) ~ S^5 implies the existence of a
particularly simple quantized topological action, or Wess-Zumino-Witten (WZW)
term. This action plays an important role in anomaly cancellation in extensions
of the Standard Model electroweak sector. A closed form is presented for the
action coupled to... | [
{
"created": "Tue, 20 Oct 2009 14:51:11 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Oct 2009 21:37:14 GMT",
"version": "v2"
}
] | 2010-04-14 | [
[
"Hill",
"Richard J.",
""
]
] | The observation that SU(3)/SU(2) ~ S^5 implies the existence of a particularly simple quantized topological action, or Wess-Zumino-Witten (WZW) term. This action plays an important role in anomaly cancellation in extensions of the Standard Model electroweak sector. A closed form is presented for the action coupled to a... | 5.931585 | 5.953858 | 5.913502 | 5.580543 | 6.153274 | 5.854465 | 5.992037 | 5.945107 | 5.678984 | 6.315498 | 5.777721 | 5.651782 | 5.718948 | 5.54246 | 5.989731 | 5.91825 | 5.763362 | 5.649008 | 5.717455 | 5.688591 | 5.672328 |
0907.0410 | Hari Kunduri | Hari K. Kunduri, James Lucietti | Static near-horizon geometries in five dimensions | Latex, 28 pages. v2: minor changes, reference added | Class. Quantum Grav. 26: 245010, 2009 | 10.1088/0264-9381/26/24/245010 | DCPT-09/41, DAMTP-2009-49 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the classification of static near-horizon geometries of
stationary extremal (not necessarily BPS) black hole solutions of five
dimensional Einstein-Maxwell theory coupled to a Chern-Simons term with
coupling xi (with xi=1 corresponding to supergravity). Assuming the black holes
have two rotational symmetr... | [
{
"created": "Thu, 2 Jul 2009 16:30:26 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Dec 2009 12:54:37 GMT",
"version": "v2"
}
] | 2009-12-23 | [
[
"Kunduri",
"Hari K.",
""
],
[
"Lucietti",
"James",
""
]
] | We consider the classification of static near-horizon geometries of stationary extremal (not necessarily BPS) black hole solutions of five dimensional Einstein-Maxwell theory coupled to a Chern-Simons term with coupling xi (with xi=1 corresponding to supergravity). Assuming the black holes have two rotational symmetrie... | 5.213551 | 5.058636 | 5.556406 | 5.011503 | 5.286622 | 5.153455 | 4.958139 | 5.046248 | 4.927731 | 5.891914 | 5.0941 | 4.936698 | 5.002258 | 4.905655 | 4.926686 | 4.880718 | 4.912366 | 4.765361 | 4.935049 | 5.101363 | 4.879453 |
1704.03989 | Xiao-Xiong Zeng | Rong-Gen Cai, Xiao-Xiong Zeng, Hai-Qing Zhang | Influence of inhomogeneities on holographic mutual information and
butterfly effect | a footnote is added and some typos are revised | JHEP 1707 (2017) 082 | 10.1007/JHEP07(2017)082 | null | hep-th gr-qc | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We study the effect of inhomogeneity, which is induced by the graviton mass
in massive gravity, on the mutual information and the chaotic behavior of a
2+1-dimensional field theory from the gauge/gravity duality. When the system is
near-homogeneous, the mutual information increases as the graviton mass grows.
However... | [
{
"created": "Thu, 13 Apr 2017 04:15:26 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Apr 2017 13:37:25 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Jun 2017 12:26:38 GMT",
"version": "v3"
}
] | 2017-07-21 | [
[
"Cai",
"Rong-Gen",
""
],
[
"Zeng",
"Xiao-Xiong",
""
],
[
"Zhang",
"Hai-Qing",
""
]
] | We study the effect of inhomogeneity, which is induced by the graviton mass in massive gravity, on the mutual information and the chaotic behavior of a 2+1-dimensional field theory from the gauge/gravity duality. When the system is near-homogeneous, the mutual information increases as the graviton mass grows. However, ... | 7.279032 | 7.001146 | 7.277583 | 6.672391 | 6.958481 | 7.408284 | 6.875087 | 7.060312 | 6.707726 | 7.810244 | 6.91565 | 6.93698 | 7.109747 | 6.965664 | 7.179132 | 7.016284 | 7.053524 | 6.971129 | 6.966792 | 7.319226 | 6.940156 |
1301.1495 | Amin Faraji Astaneh | Amin Faraji Astaneh, Amir Esmaeil Mosaffa | Holographic Entanglement Entropy for Excited States in Two Dimensional
CFT | 18 pages, Refs. added | JHEP03(2013)135 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use holographic methods to study the entanglement entropy for excited
states in a two dimensional conformal field theory. The entangling area is a
single interval and the excitations are produced by in and out vertex operators
with given scaling dimensions. On the gravity side we provide the excitations
by turning... | [
{
"created": "Tue, 8 Jan 2013 11:22:41 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Jan 2013 08:46:26 GMT",
"version": "v2"
}
] | 2013-03-27 | [
[
"Astaneh",
"Amin Faraji",
""
],
[
"Mosaffa",
"Amir Esmaeil",
""
]
] | We use holographic methods to study the entanglement entropy for excited states in a two dimensional conformal field theory. The entangling area is a single interval and the excitations are produced by in and out vertex operators with given scaling dimensions. On the gravity side we provide the excitations by turning o... | 11.014167 | 10.896764 | 12.926201 | 10.583484 | 11.349435 | 10.36132 | 11.00921 | 9.865077 | 10.930711 | 14.425697 | 10.642862 | 10.817587 | 11.261293 | 10.256923 | 10.621662 | 10.267967 | 10.577945 | 10.588842 | 10.602777 | 10.857872 | 10.326543 |
2306.07345 | Brian Kent | Elena C\'aceres, Tyler Guglielmo, Brian Kent, Anderson Misobuchi | Out-of-time-order correlators and Lyapunov exponents in sparse SYK | 22 pages + 18 pages Appendices, 13 Figures. Version submitted to JHEP
for publication | null | 10.1007/JHEP11(2023)088 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We use a combination of analytical and numerical methods to study out-of-time
order correlators (OTOCs) in the sparse Sachdev-Ye-Kitaev (SYK) model. We find
that at a given order of N , the standard result for the q-local, all-to-all
SYK, obtained through the sum over ladder diagrams, is corrected by a series in
the ... | [
{
"created": "Mon, 12 Jun 2023 18:07:08 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Nov 2023 00:40:45 GMT",
"version": "v2"
}
] | 2023-11-30 | [
[
"Cáceres",
"Elena",
""
],
[
"Guglielmo",
"Tyler",
""
],
[
"Kent",
"Brian",
""
],
[
"Misobuchi",
"Anderson",
""
]
] | We use a combination of analytical and numerical methods to study out-of-time order correlators (OTOCs) in the sparse Sachdev-Ye-Kitaev (SYK) model. We find that at a given order of N , the standard result for the q-local, all-to-all SYK, obtained through the sum over ladder diagrams, is corrected by a series in the sp... | 9.802321 | 10.528024 | 11.512118 | 9.499399 | 10.328052 | 9.917795 | 11.181569 | 9.929296 | 10.622074 | 12.032658 | 10.074717 | 9.995746 | 10.815495 | 10.100109 | 10.15502 | 10.522097 | 10.133299 | 10.125737 | 9.971034 | 10.967586 | 10.49778 |
hep-th/0310296 | Shin'ichi Nojiri | Shin'ichi Nojiri and Sergei D. Odintsov | Quantum effects and stability of chameleon cosmology | LaTeX file, 10 pages, references are added | Mod.Phys.Lett.A19:1273-1280,2004 | 10.1142/S0217732304015282 | null | hep-th astro-ph gr-qc | null | One possibility to explain the current accelerated expansion of the universe
may be related with the presence of cosmologically evolving scalar whose mass
depends on the local matter density (chameleon cosmology). We point out that
matter quantum effects in such scalar-tensor theory produce the chameleon
scalar field... | [
{
"created": "Fri, 31 Oct 2003 15:22:39 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Nov 2003 21:18:27 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Nojiri",
"Shin'ichi",
""
],
[
"Odintsov",
"Sergei D.",
""
]
] | One possibility to explain the current accelerated expansion of the universe may be related with the presence of cosmologically evolving scalar whose mass depends on the local matter density (chameleon cosmology). We point out that matter quantum effects in such scalar-tensor theory produce the chameleon scalar field d... | 15.630508 | 13.275927 | 15.990585 | 13.489036 | 14.803117 | 14.722333 | 16.327103 | 13.306235 | 14.34613 | 16.394537 | 13.503136 | 14.025863 | 14.193056 | 14.054179 | 13.964539 | 13.747726 | 14.244236 | 13.606596 | 13.955794 | 14.517218 | 13.778069 |
hep-th/0411262 | Amihay Hanany | Sergio Benvenuti and Amihay Hanany | New results on superconformal quivers | 51 pages, many figures | JHEP0604:032,2006 | 10.1088/1126-6708/2006/04/032 | MIT-CTP-3505 | hep-th | null | All superconformal quivers are shown to satisfy the relation c = a and are
thus good candidates for being the field theory living on D3 branes probing CY
singularities. We systematically study 3 block and 4 block chiral quivers which
admit a superconformal fixed point of the RG equation. Most of these theories
are kn... | [
{
"created": "Mon, 29 Nov 2004 18:53:31 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Benvenuti",
"Sergio",
""
],
[
"Hanany",
"Amihay",
""
]
] | All superconformal quivers are shown to satisfy the relation c = a and are thus good candidates for being the field theory living on D3 branes probing CY singularities. We systematically study 3 block and 4 block chiral quivers which admit a superconformal fixed point of the RG equation. Most of these theories are know... | 9.03327 | 8.73145 | 9.329307 | 8.50863 | 8.858258 | 8.7214 | 8.946059 | 8.591308 | 8.448663 | 9.616079 | 8.429082 | 8.192556 | 8.528161 | 8.394389 | 8.413526 | 8.329224 | 8.442379 | 8.350643 | 8.462565 | 8.649186 | 8.326272 |
2206.09437 | Francesco Fucito | Dario Consoli, Francesco Fucito, Jose Francisco Morales, Rubik
Poghossian | CFT description of BH's and ECO's: QNMs, superradiance, echoes and tidal
responses | 32 pages, references and explanations added to match the referee's
observations | null | 10.1007/JHEP12(2022)115 | null | hep-th gr-qc | http://creativecommons.org/publicdomain/zero/1.0/ | Using conformal field theory and localization tecniques we study the
propagation of waves in gravity backgrounds described by Schr\"odinger like
equations with Fuchsian singularities. Exact formulae for the connection
matrices relating the asymptotic behaviour of the wave functions near the
singularities are obtained... | [
{
"created": "Sun, 19 Jun 2022 15:59:21 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Jul 2022 11:59:01 GMT",
"version": "v2"
},
{
"created": "Tue, 13 Sep 2022 12:30:57 GMT",
"version": "v3"
}
] | 2023-01-04 | [
[
"Consoli",
"Dario",
""
],
[
"Fucito",
"Francesco",
""
],
[
"Morales",
"Jose Francisco",
""
],
[
"Poghossian",
"Rubik",
""
]
] | Using conformal field theory and localization tecniques we study the propagation of waves in gravity backgrounds described by Schr\"odinger like equations with Fuchsian singularities. Exact formulae for the connection matrices relating the asymptotic behaviour of the wave functions near the singularities are obtained i... | 12.572912 | 11.374875 | 11.614531 | 10.291688 | 11.620566 | 11.449798 | 11.1552 | 9.567241 | 10.243677 | 10.622958 | 10.874542 | 10.813099 | 11.060096 | 10.835808 | 11.891614 | 11.249325 | 10.945659 | 11.097006 | 11.089025 | 11.317219 | 11.199992 |
hep-th/0401130 | Tekin Dereli | T. Dereli (Koc University), R. W. Tucker (Lancaster University) | On the Energy-Momentum Density of Gravitational Plane Waves | 10 pages, no figures | Class.Quant.Grav. 21 (2004) 1459-1465 | 10.1088/0264-9381/21/6/013 | null | hep-th gr-qc | null | By embedding Einstein's original formulation of GR into a broader context we
show that a dynamic covariant description of gravitational stress-energy
emerges naturally from a variational principle. A tensor $T^G$ is constructed
from a contraction of the Bel tensor with a symmetric covariant second degree
tensor field... | [
{
"created": "Tue, 20 Jan 2004 08:03:47 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Dereli",
"T.",
"",
"Koc University"
],
[
"Tucker",
"R. W.",
"",
"Lancaster University"
]
] | By embedding Einstein's original formulation of GR into a broader context we show that a dynamic covariant description of gravitational stress-energy emerges naturally from a variational principle. A tensor $T^G$ is constructed from a contraction of the Bel tensor with a symmetric covariant second degree tensor field $... | 15.653641 | 19.803972 | 14.678946 | 14.622602 | 17.1952 | 17.383595 | 17.244762 | 16.108675 | 17.96472 | 18.11602 | 15.144997 | 14.573467 | 14.403898 | 13.968179 | 14.845901 | 15.416577 | 15.672664 | 14.211437 | 14.374027 | 14.451722 | 14.196918 |
2211.05437 | Apollonas S. Matsoukas-Roubeas | Apollonas S. Matsoukas-Roubeas, Federico Roccati, Julien Cornelius,
Zhenyu Xu, Aurelia Chenu, Adolfo del Campo | Non-Hermitian Hamiltonian Deformations in Quantum Mechanics | 28 pages, 6 figures | J. High Energ. Phys. 2023, 60 (2023) | 10.1007/JHEP01(2023)060 | null | hep-th cond-mat.stat-mech math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The construction of exactly-solvable models has recently been advanced by
considering integrable $T\bar{T}$ deformations and related Hamiltonian
deformations in quantum mechanics. We introduce a broader class of
non-Hermitian Hamiltonian deformations in a nonrelativistic setting, to account
for the description of a l... | [
{
"created": "Thu, 10 Nov 2022 09:25:59 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jan 2023 11:41:34 GMT",
"version": "v2"
}
] | 2023-01-18 | [
[
"Matsoukas-Roubeas",
"Apollonas S.",
""
],
[
"Roccati",
"Federico",
""
],
[
"Cornelius",
"Julien",
""
],
[
"Xu",
"Zhenyu",
""
],
[
"Chenu",
"Aurelia",
""
],
[
"del Campo",
"Adolfo",
""
]
] | The construction of exactly-solvable models has recently been advanced by considering integrable $T\bar{T}$ deformations and related Hamiltonian deformations in quantum mechanics. We introduce a broader class of non-Hermitian Hamiltonian deformations in a nonrelativistic setting, to account for the description of a lar... | 7.860383 | 8.643639 | 8.515063 | 8.019259 | 8.671463 | 8.531117 | 8.156981 | 8.093078 | 7.756662 | 9.094378 | 7.857456 | 7.808434 | 8.174732 | 7.821937 | 7.963406 | 7.864278 | 7.949827 | 7.939566 | 7.935554 | 8.170122 | 7.990288 |
hep-th/9502116 | Douglas A. Singleton | Douglas Singleton | Axially Symmetric Solutions for SU(2) Yang-Mills Theory | 15 pages LaTeX | J.Math.Phys. 37 (1996) 4574-4583 | 10.1063/1.531659 | null | hep-th | null | By casting the Yang-Mills-Higgs equations of an SU(2) theory in the form of
the Ernst equations of general relativity, it is shown how the known exact
solutions of general relativity can be used to give similiar solutions for
Yang-Mills theory. Thus all the known exact solutions of general relativity
with axial symme... | [
{
"created": "Sun, 19 Feb 1995 00:26:14 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Singleton",
"Douglas",
""
]
] | By casting the Yang-Mills-Higgs equations of an SU(2) theory in the form of the Ernst equations of general relativity, it is shown how the known exact solutions of general relativity can be used to give similiar solutions for Yang-Mills theory. Thus all the known exact solutions of general relativity with axial symmetr... | 8.864532 | 9.443859 | 9.090567 | 8.435814 | 9.084385 | 8.593575 | 9.360517 | 8.516456 | 8.32585 | 9.303558 | 8.615952 | 8.37605 | 8.496007 | 8.481245 | 8.548696 | 8.504848 | 8.512963 | 8.453105 | 8.638702 | 8.686711 | 8.443117 |
1505.04978 | Markku Oksanen | R. Bufalo, M. Oksanen, A. Tureanu | How unimodular gravity theories differ from general relativity at
quantum level | 35 pages; v4: included a full treatment of nonlocally linearly
dependent generators as Appendix A, Refs. 28 and 29 added, extended the
discussion on physical degrees of freedom, boundary terms, and conclusions | Eur. Phys. J. C 75 (2015) 477 | 10.1140/epjc/s10052-015-3683-3 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate path integral quantization of two versions of unimodular
gravity. First a fully diffeomorphism-invariant theory is analyzed, which does
not include a unimodular condition on the metric, while still being equivalent
to other unimodular gravity theories at the classical level. The path integral
has the s... | [
{
"created": "Tue, 19 May 2015 12:57:29 GMT",
"version": "v1"
},
{
"created": "Wed, 20 May 2015 17:35:15 GMT",
"version": "v2"
},
{
"created": "Tue, 28 Jul 2015 18:28:20 GMT",
"version": "v3"
},
{
"created": "Wed, 7 Oct 2015 13:00:39 GMT",
"version": "v4"
}
] | 2015-10-08 | [
[
"Bufalo",
"R.",
""
],
[
"Oksanen",
"M.",
""
],
[
"Tureanu",
"A.",
""
]
] | We investigate path integral quantization of two versions of unimodular gravity. First a fully diffeomorphism-invariant theory is analyzed, which does not include a unimodular condition on the metric, while still being equivalent to other unimodular gravity theories at the classical level. The path integral has the sam... | 7.600599 | 8.453412 | 7.997664 | 7.069629 | 7.967782 | 8.35771 | 8.290254 | 7.890056 | 8.151512 | 8.811196 | 7.511889 | 7.34237 | 7.616238 | 7.612827 | 7.698545 | 7.326522 | 7.460659 | 7.663712 | 7.643621 | 7.501184 | 7.539941 |
1603.00969 | Varghese Mathai | Varghese Mathai, Jonathan Rosenberg | Group dualities, T-dualities, and twisted K-theory | 29 pages, mild revision | J. London Math. Soc. (2) 97 (2018) 1-23 | 10.1112/jlms.12085 | null | hep-th math.AT math.KT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper explores further the connection between Langlands duality and
T-duality for compact simple Lie groups, which appeared in work of Daenzer-Van
Erp and Bunke-Nikolaus. We show that Langlands duality gives rise to
isomorphisms of twisted K-groups, but that these K-groups are trivial except in
the simplest case... | [
{
"created": "Thu, 3 Mar 2016 04:26:42 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Mar 2017 01:05:00 GMT",
"version": "v2"
}
] | 2018-02-08 | [
[
"Mathai",
"Varghese",
""
],
[
"Rosenberg",
"Jonathan",
""
]
] | This paper explores further the connection between Langlands duality and T-duality for compact simple Lie groups, which appeared in work of Daenzer-Van Erp and Bunke-Nikolaus. We show that Langlands duality gives rise to isomorphisms of twisted K-groups, but that these K-groups are trivial except in the simplest case o... | 8.828088 | 10.284311 | 12.304302 | 9.187411 | 10.82241 | 10.245353 | 9.91701 | 10.187311 | 10.696565 | 12.577662 | 9.409389 | 8.923239 | 9.896928 | 8.867567 | 9.197652 | 9.13506 | 9.027583 | 9.182421 | 8.772983 | 9.412398 | 8.889396 |
hep-th/9308127 | Roger Brooks | R. Brooks, J.-G. Demers and C. Lucchesi | Twisting to Abelian BF/Chern-Simons Theories | 19 pages, CTP #2237, LaTeX | Nucl.Phys. B415 (1994) 353-372 | 10.1016/0550-3213(94)90115-5 | null | hep-th | null | Starting from a $D=3$, $N=4$ supersymmetric theory for matter fields, a twist
with a Grassmann parity change is defined which maps the theory into a gauge
fixed, abelian $BF$ theory on curved 3-manifolds. After adding surface terms to
this theory, the twist is seen to map the resulting supersymmetric action to
two un... | [
{
"created": "Thu, 26 Aug 1993 21:03:32 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Brooks",
"R.",
""
],
[
"Demers",
"J. -G.",
""
],
[
"Lucchesi",
"C.",
""
]
] | Starting from a $D=3$, $N=4$ supersymmetric theory for matter fields, a twist with a Grassmann parity change is defined which maps the theory into a gauge fixed, abelian $BF$ theory on curved 3-manifolds. After adding surface terms to this theory, the twist is seen to map the resulting supersymmetric action to two unco... | 9.470032 | 10.03058 | 9.995319 | 8.862575 | 8.850902 | 9.386461 | 9.513965 | 9.259059 | 8.790933 | 11.050596 | 9.054932 | 8.911806 | 9.638824 | 9.072799 | 9.005251 | 9.354993 | 9.241193 | 9.131518 | 9.08078 | 9.460097 | 9.317579 |
1112.1049 | Christian Schubert | Idrish Huet, Michel Rausch de Traubenberg, Christian Schubert | The Euler-Heisenberg Lagrangian beyond one loop | 11 pages, 2 figures, talk given by Christian Schubert at QFEXT11,
Benasque, Spain, Sept. 18-24, 2011, to appear in the conference proceedings | null | 10.1142/S2010194512007507 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review what is presently known about higher loop corrections to the
Euler-Heisenberg Lagrangian and its Scalar QED analogue. The use of those
corrections as a tool for the study of the properties of the QED perturbation
series is outlined. As a further step in a long-term effort to prove or
disprove the convergenc... | [
{
"created": "Mon, 5 Dec 2011 20:34:36 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Huet",
"Idrish",
""
],
[
"de Traubenberg",
"Michel Rausch",
""
],
[
"Schubert",
"Christian",
""
]
] | We review what is presently known about higher loop corrections to the Euler-Heisenberg Lagrangian and its Scalar QED analogue. The use of those corrections as a tool for the study of the properties of the QED perturbation series is outlined. As a further step in a long-term effort to prove or disprove the convergence ... | 10.503116 | 8.947452 | 9.553977 | 8.709064 | 9.156497 | 9.276534 | 9.147164 | 9.046988 | 8.439209 | 9.874846 | 8.835953 | 9.379991 | 9.462525 | 9.243169 | 9.470162 | 9.424584 | 9.120391 | 9.370069 | 9.175298 | 9.523459 | 9.330123 |
1607.04205 | Toshiaki Fujimori | Toshiaki Fujimori, Syo Kamata, Tatsuhiro Misumi, Muneto Nitta,
Norisuke Sakai | Non-perturbative Contributions from Complexified Solutions in
$\mathbb{C}P^{N-1}$ Models | 49 pages, 10 figures; Corrected Fig.4 and Fig.5 | Phys. Rev. D 94, 105002 (2016) | 10.1103/PhysRevD.94.105002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the non-perturbative contributions from real and complex saddle
point solutions in the $\mathbb{C}P^1$ quantum mechanics with fermionic degrees
of freedom, using the Lefschetz thimble formalism beyond the gaussian
approximation. We find bion solutions, which correspond to (complexified)
instanton-antiinsta... | [
{
"created": "Thu, 14 Jul 2016 16:52:21 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jul 2016 16:29:48 GMT",
"version": "v2"
}
] | 2016-11-09 | [
[
"Fujimori",
"Toshiaki",
""
],
[
"Kamata",
"Syo",
""
],
[
"Misumi",
"Tatsuhiro",
""
],
[
"Nitta",
"Muneto",
""
],
[
"Sakai",
"Norisuke",
""
]
] | We discuss the non-perturbative contributions from real and complex saddle point solutions in the $\mathbb{C}P^1$ quantum mechanics with fermionic degrees of freedom, using the Lefschetz thimble formalism beyond the gaussian approximation. We find bion solutions, which correspond to (complexified) instanton-antiinstant... | 7.314614 | 7.220535 | 8.042503 | 6.982922 | 7.562432 | 7.147066 | 7.578531 | 6.842846 | 6.695988 | 8.397436 | 6.814752 | 6.796119 | 7.438121 | 6.947714 | 7.084501 | 7.068089 | 6.905703 | 6.899812 | 6.888884 | 7.433216 | 6.883455 |
0708.0632 | Mikhail Shifman | M. Shifman | Some Theoretical Developments in SUSY | 20 pages. Plenary Talk at the 15th International Conference on
Supersymmetry and the Unification of Fundamental Interactions SUSY 07,
Karlsruhe, Germany, July 26 - August 1, 2007. Submitted for the SUSY07
proceedings | null | null | FTPI-MINN-07/24, UMN-TH-2613/07 | hep-th hep-ph | null | I review theoretical developments of the last year or so in nonperturbative
supersymmetry. Topics: (i) Metastable vacua at strong coupling; (ii)
Non-Abelian flux tubes, confined monopoles; (iii) One step beyond Seiberg's
duality; (iv) Planar equivalence; (v) Multileg/multiloop amplitudes; (vi) N=
(2,0) sigma model on... | [
{
"created": "Sat, 4 Aug 2007 15:16:52 GMT",
"version": "v1"
}
] | 2007-08-07 | [
[
"Shifman",
"M.",
""
]
] | I review theoretical developments of the last year or so in nonperturbative supersymmetry. Topics: (i) Metastable vacua at strong coupling; (ii) Non-Abelian flux tubes, confined monopoles; (iii) One step beyond Seiberg's duality; (iv) Planar equivalence; (v) Multileg/multiloop amplitudes; (vi) N= (2,0) sigma model on t... | 7.956088 | 7.599876 | 7.928797 | 7.103421 | 7.483899 | 8.107005 | 7.243167 | 7.634596 | 7.50364 | 7.917967 | 8.118271 | 7.395761 | 7.225818 | 7.163842 | 7.333152 | 7.587773 | 7.296893 | 7.473282 | 7.057209 | 7.256125 | 7.849199 |
1312.0053 | Kei-Ichi Kondo | Kei-Ichi Kondo | Stability of magnetic condensation and mass generation for confinement
in SU(2) Yang-Mills theory | 12 pages, no figures; Talk given at the QCD-TNT-III-From quarks and
gluons to hadronic matter: A bridge too far? 2-6 September, 2013, European
Centre for Theoretical Studies in Nuclear Physics and Related Areas (ECT*),
Villazzano, Trento (Italy) | null | null | CHIBA-EP-203 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the framework of the functional renormalization group, we reexamine the
stability of the Yang-Mills vacuum with a chromomagnetic condensation. We show
that the Nielsen-Olesen instability of the Savvidy vacuum with a homogeneous
chromomagnetic condensation disappears in the $SU(2)$ Yang-Mills theory. As a
physical ... | [
{
"created": "Sat, 30 Nov 2013 02:55:30 GMT",
"version": "v1"
}
] | 2013-12-03 | [
[
"Kondo",
"Kei-Ichi",
""
]
] | In the framework of the functional renormalization group, we reexamine the stability of the Yang-Mills vacuum with a chromomagnetic condensation. We show that the Nielsen-Olesen instability of the Savvidy vacuum with a homogeneous chromomagnetic condensation disappears in the $SU(2)$ Yang-Mills theory. As a physical me... | 7.698657 | 6.544291 | 8.204278 | 6.581812 | 6.585325 | 6.602418 | 6.230262 | 6.253482 | 6.794704 | 8.81781 | 6.967966 | 7.078406 | 7.521568 | 7.545221 | 7.018505 | 7.16242 | 7.348216 | 7.448822 | 7.328933 | 7.826769 | 7.345712 |
1608.07753 | Pavel Putrov | Abhijit Gadde, Pavel Putrov | Exact solutions of (0,2) Landau-Ginzburg models | 18 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study the low energy physics of Landau-Ginzburg models with
N=(0,2) supersymmetry. We exhibit a number of classes of relatively simple LG
models where the conformal field theory at the low energy fixed point can be
explicitly identified. One interesting class of fixed points can be thought of
as "het... | [
{
"created": "Sun, 28 Aug 2016 00:30:06 GMT",
"version": "v1"
}
] | 2016-08-30 | [
[
"Gadde",
"Abhijit",
""
],
[
"Putrov",
"Pavel",
""
]
] | In this paper we study the low energy physics of Landau-Ginzburg models with N=(0,2) supersymmetry. We exhibit a number of classes of relatively simple LG models where the conformal field theory at the low energy fixed point can be explicitly identified. One interesting class of fixed points can be thought of as "heter... | 6.815343 | 6.07629 | 7.685574 | 6.542191 | 6.168215 | 6.515832 | 6.029247 | 6.32149 | 6.208067 | 7.806203 | 6.299944 | 6.354848 | 7.152427 | 6.332032 | 6.545306 | 6.682856 | 6.571154 | 6.339222 | 6.280328 | 7.048339 | 6.287819 |
hep-th/9810057 | Jose Francisco Gomes | J.F.Gomes, F.E. Mendon\c{c}a da Silveira, G.M. Sotkov and A.H.
Zimerman | Singular Non-Abelian Toda Theories | Latex, 12 pages | null | null | null | hep-th | null | The algebraic conditions that specific gauged G/H-WZW model have to satisfy
in order to give rise to Non-Abelian Toda models with singular metric with or
without torsion are found. The classical algebras of symmetries corresponding
to grade one rank 2 and 3 singular NA-Toda models are derived.
| [
{
"created": "Thu, 8 Oct 1998 11:56:22 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Gomes",
"J. F.",
""
],
[
"da Silveira",
"F. E. Mendonça",
""
],
[
"Sotkov",
"G. M.",
""
],
[
"Zimerman",
"A. H.",
""
]
] | The algebraic conditions that specific gauged G/H-WZW model have to satisfy in order to give rise to Non-Abelian Toda models with singular metric with or without torsion are found. The classical algebras of symmetries corresponding to grade one rank 2 and 3 singular NA-Toda models are derived. | 22.408409 | 20.776783 | 21.763268 | 18.389147 | 18.919424 | 18.807852 | 20.37126 | 21.491034 | 19.156096 | 23.67915 | 18.902205 | 19.761028 | 22.051897 | 19.615116 | 18.909075 | 19.202852 | 18.6455 | 19.624147 | 18.901291 | 21.24608 | 18.061697 |
hep-th/9910131 | Carlo Rovelli | Carlo Rovelli | The century of the incomplete revolution: searching for general
relativistic quantum field theory | To appear in the Journal of Mathematical Physics 2000 Special Issue | J.Math.Phys.41:3776-3800,2000 | 10.1063/1.533327 | null | hep-th gr-qc | null | In fundamental physics, this has been the century of quantum mechanics and
general relativity. It has also been the century of the long search for a
conceptual framework capable of embracing the astonishing features of the world
that have been revealed by these two ``first pieces of a conceptual
revolution''. I discu... | [
{
"created": "Sun, 17 Oct 1999 19:43:18 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Rovelli",
"Carlo",
""
]
] | In fundamental physics, this has been the century of quantum mechanics and general relativity. It has also been the century of the long search for a conceptual framework capable of embracing the astonishing features of the world that have been revealed by these two ``first pieces of a conceptual revolution''. I discuss... | 13.207166 | 15.378285 | 13.276455 | 13.407094 | 15.132812 | 14.381521 | 15.215118 | 13.609325 | 13.497552 | 15.172681 | 13.649687 | 12.922179 | 12.998202 | 12.639524 | 13.024948 | 12.392084 | 12.652261 | 12.537764 | 12.543151 | 12.977588 | 13.202191 |
1711.06365 | Shu Lin | Si-wen Li and Shu Lin | D-instantons in Real Time Dynamics | 29 pages, 3 figures. Added computation details and Sec 4.3 on the
justification of analytic continuation. Main results not changed. To appear
in PRD | Phys. Rev. D 98, 066002 (2018) | 10.1103/PhysRevD.98.066002 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Instanton is known to exist in Euclidean spacetime only. Their role in real
time dynamics is usually understood as tunneling effect by Wick rotation. We
illustrate other effects of instanton in holography by investigating 5d
effective gravity theory of the black D3-brane-D-instanton system. The
supergravity descripti... | [
{
"created": "Fri, 17 Nov 2017 01:15:15 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Sep 2018 09:41:33 GMT",
"version": "v2"
}
] | 2018-09-19 | [
[
"Li",
"Si-wen",
""
],
[
"Lin",
"Shu",
""
]
] | Instanton is known to exist in Euclidean spacetime only. Their role in real time dynamics is usually understood as tunneling effect by Wick rotation. We illustrate other effects of instanton in holography by investigating 5d effective gravity theory of the black D3-brane-D-instanton system. The supergravity description... | 10.490262 | 10.979553 | 11.0653 | 10.338333 | 11.098205 | 10.810019 | 11.000791 | 10.695221 | 10.385921 | 12.118443 | 10.388612 | 10.195904 | 10.389052 | 10.024427 | 9.980361 | 10.350223 | 10.134309 | 10.198351 | 10.293597 | 9.972786 | 10.190848 |
2306.03077 | Marcos A Anacleto | M. A. Anacleto, F. A. Brito and E. Passos | Modified metrics of acoustic black holes: A review | 17 pages, 2 figures. arXiv admin note: text overlap with
arXiv:2212.13850, arXiv:2112.13573 | Phys Sci & Biophys J 2023, 7(1): 000245 | 10.23880/psbj-16000245 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this brief review, we will address acoustic black holes arising from
quantum field theory in the Lorentz-violating and non-commutative background.
Thus, we consider canonical acoustic black holes with effective metrics for the
purpose of investigating Hawking radiation and entropy. We show that due to the
generali... | [
{
"created": "Mon, 5 Jun 2023 17:53:13 GMT",
"version": "v1"
}
] | 2023-06-12 | [
[
"Anacleto",
"M. A.",
""
],
[
"Brito",
"F. A.",
""
],
[
"Passos",
"E.",
""
]
] | In this brief review, we will address acoustic black holes arising from quantum field theory in the Lorentz-violating and non-commutative background. Thus, we consider canonical acoustic black holes with effective metrics for the purpose of investigating Hawking radiation and entropy. We show that due to the generalize... | 11.438423 | 10.171836 | 9.066554 | 9.363747 | 10.311195 | 9.683428 | 10.508265 | 9.815493 | 9.868495 | 9.569858 | 9.764532 | 10.358394 | 9.775074 | 9.716621 | 10.606602 | 9.744975 | 10.025262 | 10.037632 | 10.027277 | 9.690154 | 10.329242 |
hep-th/9510036 | Lukas Nellen | Myriam Mondragon, Lukas Nellen, Michael G. Schmidt, Christian Schubert | Axial Couplings on the World-Line | 12 pages, LaTeX 2e with array and epsf packages, Postscript figures.
Submitted to Phys. Lett. B. Minor corrections, fixed a number of typos | Phys.Lett. B366 (1996) 212-219 | 10.1016/0370-2693(95)01392-X | IASSNS-HEP-95/74, HD-THEP-95-43, HUB-EP-95/17 | hep-th hep-ph | null | We construct a world-line representation for the fermionic one-loop effective
action with axial and also vector, scalar, and pseudo-scalar couplings. We use
this expression to compute a few selected scattering amplitudes. These allow us
to verify that our method yields the same results as standard field theory. In
pa... | [
{
"created": "Sun, 8 Oct 1995 22:59:35 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Oct 1995 23:24:17 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Mondragon",
"Myriam",
""
],
[
"Nellen",
"Lukas",
""
],
[
"Schmidt",
"Michael G.",
""
],
[
"Schubert",
"Christian",
""
]
] | We construct a world-line representation for the fermionic one-loop effective action with axial and also vector, scalar, and pseudo-scalar couplings. We use this expression to compute a few selected scattering amplitudes. These allow us to verify that our method yields the same results as standard field theory. In part... | 10.399875 | 9.60294 | 9.335635 | 9.172629 | 9.012629 | 9.031266 | 8.858602 | 9.210724 | 8.62982 | 9.298732 | 8.913577 | 9.330628 | 9.029482 | 9.17851 | 9.12941 | 9.121813 | 9.855944 | 9.127548 | 9.400514 | 9.381443 | 9.272864 |
1312.5740 | Eric Perlmutter | Eric Perlmutter | Comments on Renyi entropy in AdS$_3$/CFT$_2$ | 41 pages. v3: various minor clarifications; added Subsection 4.3
including a result on the entanglement limit; added refs | null | 10.1007/JHEP05(2014)052 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend and refine recent results on Renyi entropy in two-dimensional
conformal field theories at large central charge. To do so, we examine the
effects of higher spin symmetry and of allowing unequal left and right central
charges, at leading and subleading order in large total central charge. The
result is a stra... | [
{
"created": "Thu, 19 Dec 2013 20:59:06 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Dec 2013 20:05:16 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Mar 2014 20:10:06 GMT",
"version": "v3"
}
] | 2015-06-18 | [
[
"Perlmutter",
"Eric",
""
]
] | We extend and refine recent results on Renyi entropy in two-dimensional conformal field theories at large central charge. To do so, we examine the effects of higher spin symmetry and of allowing unequal left and right central charges, at leading and subleading order in large total central charge. The result is a straig... | 11.151315 | 10.239519 | 13.354586 | 10.539564 | 11.167771 | 11.839504 | 10.714391 | 11.055425 | 10.082724 | 14.169971 | 10.486856 | 10.320879 | 11.146118 | 10.588878 | 10.645566 | 10.719131 | 10.483242 | 10.750668 | 10.461065 | 11.382474 | 10.765598 |
1610.07189 | Frederico Santos | R. Casana, M. M. Ferreira Jr, F. E. P. dos Santos | Gupta-Bleuler's quantization of a parity-odd CPT-even electrodynamics of
the standard model extension | null | null | 10.1103/PhysRevD.94.125011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | {Following a successfully quantization scheme previously }{{% developed {\ in
Ref. \cite{GUPTAEVEN} for a}} parity-even {gauge sector} {of the SME, we}} have
established the Gupta-Bleuler {% quantization {of a} {\ parity-odd} and
CPT-even }electrodynamics of {the }standard model extension (SME) {without
recoursing to... | [
{
"created": "Sun, 23 Oct 2016 16:10:15 GMT",
"version": "v1"
}
] | 2017-01-04 | [
[
"Casana",
"R.",
""
],
[
"Ferreira",
"M. M.",
"Jr"
],
[
"Santos",
"F. E. P. dos",
""
]
] | {Following a successfully quantization scheme previously }{{% developed {\ in Ref. \cite{GUPTAEVEN} for a}} parity-even {gauge sector} {of the SME, we}} have established the Gupta-Bleuler {% quantization {of a} {\ parity-odd} and CPT-even }electrodynamics of {the }standard model extension (SME) {without recoursing to a... | 18.334293 | 20.256927 | 18.333603 | 17.128006 | 19.295429 | 17.317429 | 17.958918 | 16.93482 | 17.195749 | 20.24859 | 17.252853 | 16.881468 | 16.927588 | 16.184551 | 16.418245 | 16.208759 | 16.64682 | 16.796165 | 16.358114 | 17.489571 | 16.91782 |
1310.3854 | Hirotaka Hayashi | Hirotaka Hayashi, Hee-Cheol Kim and Takahiro Nishinaka | Topological strings and 5d T_N partition functions | 79 pages, 27 figures; v2: minor improvements, references added | null | 10.1007/JHEP06(2014)014 | IFT-UAM/CSIC-13-101, RUNHETC-2013-22 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We evaluate the Nekrasov partition function of 5d gauge theories engineered
by webs of 5-branes, using the refined topological vertex on the dual
Calabi-Yau threefolds. The theories include certain non-Lagrangian theories
such as the T_N theory. The refined topological vertex computation generically
contains contribu... | [
{
"created": "Mon, 14 Oct 2013 21:06:59 GMT",
"version": "v1"
},
{
"created": "Tue, 6 May 2014 08:47:51 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Hayashi",
"Hirotaka",
""
],
[
"Kim",
"Hee-Cheol",
""
],
[
"Nishinaka",
"Takahiro",
""
]
] | We evaluate the Nekrasov partition function of 5d gauge theories engineered by webs of 5-branes, using the refined topological vertex on the dual Calabi-Yau threefolds. The theories include certain non-Lagrangian theories such as the T_N theory. The refined topological vertex computation generically contains contributi... | 5.765465 | 5.667424 | 7.454947 | 5.944304 | 5.68315 | 5.97065 | 5.980467 | 6.008598 | 5.734547 | 7.339879 | 5.747328 | 5.605781 | 6.193827 | 5.704939 | 5.53394 | 5.486233 | 5.813147 | 5.513672 | 5.801671 | 6.234131 | 5.638064 |
1308.3352 | Pinaki Banerjee | Pinaki Banerjee and B. Sathiapalan | Holographic Brownian Motion in 1+1 Dimensions | 39 pages, 4 figures; New discussion on holographic RG in subsection
5.1 and new section 6 on different time scales. Modified discussion on zero
temperature dissipation in section 3. Typos corrected , references added.
Revised version to appear in Nucl. Phys. B | Nucl. Phys. B 884 (2014) 74 -105 | 10.1016/j.nuclphysb.2014.04.016 | IMSc/2013/08/6 | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the motion of a stochastic string in the background of a BTZ black
hole. In the 1+1 dimensional boundary theory this corresponds to a very heavy
external particle (e.g, a quark), interacting with the fields of a CFT at
finite temperature, and describing Brownian motion. The equations of motion for
a string i... | [
{
"created": "Thu, 15 Aug 2013 10:44:16 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Aug 2013 16:09:04 GMT",
"version": "v2"
},
{
"created": "Thu, 17 Apr 2014 14:03:11 GMT",
"version": "v3"
}
] | 2014-05-07 | [
[
"Banerjee",
"Pinaki",
""
],
[
"Sathiapalan",
"B.",
""
]
] | We study the motion of a stochastic string in the background of a BTZ black hole. In the 1+1 dimensional boundary theory this corresponds to a very heavy external particle (e.g, a quark), interacting with the fields of a CFT at finite temperature, and describing Brownian motion. The equations of motion for a string in ... | 9.725227 | 9.600043 | 9.805493 | 9.022415 | 9.590172 | 9.63159 | 8.933394 | 9.542051 | 9.568464 | 11.714013 | 9.37745 | 9.308648 | 9.65088 | 9.246207 | 9.190846 | 9.509416 | 9.709941 | 9.375743 | 9.506805 | 9.699961 | 9.466262 |
hep-th/9605235 | Michael Lashkevich | Michael Yu. Lashkevich | Fusion of RSOS Models as a Coset Construction | 8 pages, plain TeX, minor mistakes corrected | null | null | LANDAU-96-TMP-2 | hep-th | null | Using the vertex operator approach we show that fusion of the RSOS models can
be considered as a kind of coset construction which is very similar to the
coset construction of minimal models in conformal field theory. We reproduce
the excitation spectrum and $S$-matrix of the fusion RSOS models in the regime
III and s... | [
{
"created": "Sun, 2 Jun 1996 19:02:12 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Jun 1996 17:33:26 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Lashkevich",
"Michael Yu.",
""
]
] | Using the vertex operator approach we show that fusion of the RSOS models can be considered as a kind of coset construction which is very similar to the coset construction of minimal models in conformal field theory. We reproduce the excitation spectrum and $S$-matrix of the fusion RSOS models in the regime III and sho... | 9.864463 | 7.904547 | 10.181061 | 7.876362 | 7.824274 | 7.705746 | 8.301679 | 7.339972 | 7.514828 | 10.906795 | 8.331284 | 8.190451 | 10.193681 | 8.505867 | 8.405396 | 8.011704 | 8.127285 | 8.257098 | 8.315204 | 9.350291 | 8.224027 |
1908.02235 | Stefan Floerchinger | Stefan Floerchinger | Real Clifford algebras and their spinors for relativistic fermions | 42 pages | null | null | null | hep-th cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Real Clifford algebras for arbitrary number of space and time dimensions as
well as their representations in terms of spinors are reviewed and discussed.
The Clifford algebras are classified in terms of isomorphic matrix algebras of
real, complex or quaternionic type. Spinors are defined as elements of minimal
or qua... | [
{
"created": "Tue, 6 Aug 2019 16:20:47 GMT",
"version": "v1"
}
] | 2019-08-07 | [
[
"Floerchinger",
"Stefan",
""
]
] | Real Clifford algebras for arbitrary number of space and time dimensions as well as their representations in terms of spinors are reviewed and discussed. The Clifford algebras are classified in terms of isomorphic matrix algebras of real, complex or quaternionic type. Spinors are defined as elements of minimal or quasi... | 4.09587 | 8.421614 | 8.13129 | 7.656407 | 7.074873 | 8.023542 | 7.685034 | 8.248942 | 7.791004 | 8.834879 | 7.773861 | 6.20093 | 6.619739 | 6.654459 | 6.642874 | 5.928956 | 6.870558 | 5.971179 | 6.913809 | 7.134987 | 6.005494 |
hep-th/0004101 | Ruth A. W. Gregory | Ruth Gregory | Black string instabilities in anti-de Sitter space | 8 pages revtex, 2 figures, published version | Class.Quant.Grav.17:L125-L132,2000 | 10.1088/0264-9381/17/18/103 | DTP/00/31 | hep-th | null | We show how to extend the usual black string instability of vacuum or charged
black p-branes to the anti-de Sitter background. The string fragments in an
analogous fashion to the $\Lambda=0$ case, the main difference being that
instead of a periodic array of black holes forming, an accumulation of ``mini''
black hole... | [
{
"created": "Thu, 13 Apr 2000 17:24:57 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Sep 2000 13:35:59 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Gregory",
"Ruth",
""
]
] | We show how to extend the usual black string instability of vacuum or charged black p-branes to the anti-de Sitter background. The string fragments in an analogous fashion to the $\Lambda=0$ case, the main difference being that instead of a periodic array of black holes forming, an accumulation of ``mini'' black holes ... | 12.653491 | 12.568891 | 12.116791 | 11.433869 | 12.503643 | 12.935122 | 12.837577 | 11.824039 | 12.259524 | 12.939867 | 12.252654 | 10.926042 | 10.935042 | 10.960952 | 11.203429 | 11.130283 | 11.111726 | 11.446627 | 11.748711 | 12.097428 | 11.334546 |
1104.0722 | Tristan Hubsch | S. J. Gates Jr. and T. Hubsch | On Dimensional Extension of Supersymmetry: From Worldlines to
Worldsheets | LaTeX 3 times, added reference, minor edits and typo correction | Adv. in Th. Math. Phys. 16 (2012) 1619-1667 | 10.4310/ATMP.2012.v16.n6.a2 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There exist myriads of off-shell worldline supermultiplets for
(N{\leq}32)-extended supersymmetry in which every supercharge maps a component
field to precisely one other component field or its derivative. A subset of
these extends to off-shell worldsheet (p,q)-supersymmetry and is characterized
by the twin theorems ... | [
{
"created": "Tue, 5 Apr 2011 01:50:48 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Apr 2011 16:30:18 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Gates",
"S. J.",
"Jr."
],
[
"Hubsch",
"T.",
""
]
] | There exist myriads of off-shell worldline supermultiplets for (N{\leq}32)-extended supersymmetry in which every supercharge maps a component field to precisely one other component field or its derivative. A subset of these extends to off-shell worldsheet (p,q)-supersymmetry and is characterized by the twin theorems 2.... | 9.309525 | 10.353577 | 11.934032 | 9.716499 | 11.137405 | 10.679634 | 10.381778 | 9.793736 | 10.07348 | 11.59343 | 9.441508 | 9.414062 | 9.324126 | 9.343 | 9.527107 | 9.01911 | 9.333256 | 9.243343 | 9.288022 | 9.660705 | 9.099834 |
hep-th/0606064 | J. Manuel Solano-Altamirano | R. Cartas-Fuentevilla and J. M. Solano-Altamirano | Fluctons | null | Int.J.Geom.Meth.Mod.Phys.05:375-386,2008 | 10.1142/S0219887808002849 | null | hep-th | null | From the perspective of topological field theory we explore the physics
beyond instantons. We propose the fluctons as nonperturbative topological
fluctuations of vacuum, from which the self-dual domain of instantons is
attained as a particular case. Invoking the Atiyah-Singer index theorem, we
determine the dimension... | [
{
"created": "Wed, 7 Jun 2006 21:20:19 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Oct 2006 18:32:52 GMT",
"version": "v2"
},
{
"created": "Wed, 4 Oct 2006 21:52:31 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Cartas-Fuentevilla",
"R.",
""
],
[
"Solano-Altamirano",
"J. M.",
""
]
] | From the perspective of topological field theory we explore the physics beyond instantons. We propose the fluctons as nonperturbative topological fluctuations of vacuum, from which the self-dual domain of instantons is attained as a particular case. Invoking the Atiyah-Singer index theorem, we determine the dimension o... | 11.530926 | 12.093232 | 11.216366 | 11.035864 | 12.289971 | 11.823048 | 11.125136 | 12.001122 | 12.074253 | 12.870261 | 11.632824 | 11.640862 | 11.181098 | 11.360321 | 11.007058 | 11.351162 | 10.900142 | 11.149095 | 11.166776 | 10.692829 | 10.898862 |
hep-th/9305033 | Hovik Toomassian | Hovik Toomassian | The Free Field Representation of SU(3) Conformal Field Theory | 24 pages, LANDAU-TMP-91-1 | Int.J.Mod.Phys. A8 (1993) 4031-4053 | 10.1142/S0217751X9300165X | null | hep-th | null | (Revised LaTex version).The structure of free field representation and some
correlation functions of the SU(3) CFT are considered.
| [
{
"created": "Sat, 8 May 1993 20:15:26 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jul 1993 22:41:50 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Toomassian",
"Hovik",
""
]
] | (Revised LaTex version).The structure of free field representation and some correlation functions of the SU(3) CFT are considered. | 38.020832 | 25.343458 | 39.184277 | 21.835371 | 19.642038 | 19.810526 | 19.408579 | 21.861275 | 22.619062 | 50.605312 | 23.025223 | 21.696016 | 27.422333 | 23.4055 | 21.483047 | 20.699211 | 22.377319 | 21.499115 | 20.27375 | 29.170174 | 20.908428 |
hep-th/0607248 | Angelos Fotopoulos | A. Fotopoulos, K.L. Panigrahi, M. Tsulaia | On Lagrangian formulation of Higher Spin Theories on AdS | Published Version; minor corrections;added equation (3.83) | Phys.Rev.D74:085029,2006 | 10.1103/PhysRevD.74.085029 | null | hep-th | null | In this short note we present a Lagrangian formulation for free bosonic
Higher Spin fields which belong to massless reducible representations of
D-dimensional Anti de Sitter group using an ambient space formalism.
| [
{
"created": "Mon, 31 Jul 2006 14:19:04 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Aug 2006 12:51:29 GMT",
"version": "v2"
},
{
"created": "Tue, 31 Oct 2006 10:28:14 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Fotopoulos",
"A.",
""
],
[
"Panigrahi",
"K. L.",
""
],
[
"Tsulaia",
"M.",
""
]
] | In this short note we present a Lagrangian formulation for free bosonic Higher Spin fields which belong to massless reducible representations of D-dimensional Anti de Sitter group using an ambient space formalism. | 15.501544 | 8.384804 | 12.500379 | 9.000793 | 10.161016 | 9.783311 | 8.26093 | 8.796476 | 8.51792 | 12.262719 | 8.942528 | 9.594671 | 11.695844 | 10.163698 | 10.211505 | 9.83152 | 9.530944 | 9.38939 | 9.852277 | 11.170261 | 9.474401 |
hep-th/0212215 | Ben Craps | Micha Berkooz, Ben Craps, David Kutasov, Govindan Rajesh | Comments on Cosmological Singularities in String Theory | harvmac, 40 pages; v2: references added | JHEP 0303 (2003) 031 | 10.1088/1126-6708/2003/03/031 | WIS/46/02-DEC-DPP, EFI-02-45 | hep-th | null | We compute string scattering amplitudes in an orbifold of Minkowski space by
a boost, and show how certain divergences in the four point function are
associated with graviton exchange near the singularity. These divergences
reflect large tree-level backreaction of the gravitational field. Near the
singularity, all ex... | [
{
"created": "Wed, 18 Dec 2002 15:27:51 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Dec 2002 14:46:19 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Berkooz",
"Micha",
""
],
[
"Craps",
"Ben",
""
],
[
"Kutasov",
"David",
""
],
[
"Rajesh",
"Govindan",
""
]
] | We compute string scattering amplitudes in an orbifold of Minkowski space by a boost, and show how certain divergences in the four point function are associated with graviton exchange near the singularity. These divergences reflect large tree-level backreaction of the gravitational field. Near the singularity, all exci... | 9.908308 | 8.911711 | 10.82207 | 8.779346 | 9.726542 | 8.837153 | 9.069433 | 8.58162 | 8.918056 | 10.945364 | 9.650033 | 9.277068 | 9.731513 | 9.038797 | 9.34259 | 9.416574 | 9.119525 | 9.063682 | 9.225396 | 9.386517 | 9.112779 |
0910.0370 | Masato Taki | Masato Taki | M2-branes Theories without 3+1 Dimensional Parents via Un-Higgsing | 60 pages, 52 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | N=2 quiver Chern-Simons theory has lately attracted attention as the world
volume theory of multiple M2 branes on a Calabi-Yau 4-fold. We study the
connection between the stringy derivation of M2 brane theories and the forward
algorithm which gives the toric Calabi-Yau 4-fold as the moduli space of the
quiver theory.... | [
{
"created": "Fri, 2 Oct 2009 10:23:57 GMT",
"version": "v1"
}
] | 2009-10-05 | [
[
"Taki",
"Masato",
""
]
] | N=2 quiver Chern-Simons theory has lately attracted attention as the world volume theory of multiple M2 branes on a Calabi-Yau 4-fold. We study the connection between the stringy derivation of M2 brane theories and the forward algorithm which gives the toric Calabi-Yau 4-fold as the moduli space of the quiver theory. T... | 6.275123 | 5.551867 | 6.58242 | 5.853036 | 5.810112 | 5.641737 | 5.947546 | 5.610366 | 5.759396 | 7.218086 | 5.638486 | 5.716481 | 6.27259 | 5.756719 | 5.830148 | 5.79237 | 5.579126 | 5.92408 | 5.844965 | 6.048372 | 5.811698 |
hep-th/9811180 | Friedemann Brandt | Friedemann Brandt, Ulrich Theis | D=4, N=1 Supersymmetric Henneaux-Knaepen Models | 20 pages, uses amsmath.sty | Nucl.Phys. B550 (1999) 495-510 | 10.1016/S0550-3213(99)00186-8 | null | hep-th | null | We construct N=1 supersymmetric versions of four-dimensional
Freedman-Townsend models and generalizations thereof found recently by Henneaux
and Knaepen, with couplings between 1-form and 2-form gauge potentials. The
models are presented both in a superfield formulation with linearly realized
supersymmetry and in WZ ... | [
{
"created": "Thu, 19 Nov 1998 17:09:31 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Brandt",
"Friedemann",
""
],
[
"Theis",
"Ulrich",
""
]
] | We construct N=1 supersymmetric versions of four-dimensional Freedman-Townsend models and generalizations thereof found recently by Henneaux and Knaepen, with couplings between 1-form and 2-form gauge potentials. The models are presented both in a superfield formulation with linearly realized supersymmetry and in WZ ga... | 9.132144 | 7.680401 | 10.177148 | 7.753522 | 7.931716 | 7.543596 | 7.763502 | 7.78934 | 7.913054 | 10.235926 | 7.995005 | 8.24265 | 9.289517 | 8.396084 | 8.139745 | 7.802479 | 8.131935 | 7.892773 | 7.959811 | 8.886755 | 8.270999 |
hep-th/0303033 | David Berenstein | David Berenstein | Solving matrix models using holomorphy | 38 pages, JHEP style, 1 figure | JHEP 0306 (2003) 019 | 10.1088/1126-6708/2003/06/019 | null | hep-th | null | We investigate the relationship between supersymmetric gauge theories with
moduli spaces and matrix models. Particular attention is given to situations
where the moduli space gets quantum corrected. These corrections are controlled
by holomorphy. It is argued that these quantum deformations give rise to
non-trivial r... | [
{
"created": "Tue, 4 Mar 2003 23:00:47 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Berenstein",
"David",
""
]
] | We investigate the relationship between supersymmetric gauge theories with moduli spaces and matrix models. Particular attention is given to situations where the moduli space gets quantum corrected. These corrections are controlled by holomorphy. It is argued that these quantum deformations give rise to non-trivial rel... | 10.010399 | 9.34827 | 11.141893 | 9.224169 | 10.026796 | 9.161222 | 9.552464 | 9.929076 | 10.064068 | 11.744322 | 9.271111 | 9.346892 | 10.115115 | 9.889314 | 9.360037 | 9.547255 | 9.390815 | 9.539524 | 9.502234 | 10.359052 | 9.326262 |
1009.1661 | Leo Rodriguez | Bradly K. Button, Leo Rodriguez, Catherine A. Whiting and Tuna
Yildirim | A Near Horizon CFT Dual for Kerr-Newman-$AdS$ | 15 pages. Major edits and revisions. Final version accepted for
publication in IJMPA | Int.J.Mod.Phys.A26:3077-3090,2011 | 10.1142/S0217751X11053663 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the near horizon regime of a Kerr-Newman-$AdS$ (KN$AdS$) black
hole, given by its two dimensional analogue $a la$ Robinson and Wilczek (2005
Phys. Rev. Lett. 95 011303), is asymptotically $AdS_2$ and dual to a one
dimensional quantum conformal field theory (CFT). The s-wave contribution of
the resulting ... | [
{
"created": "Wed, 8 Sep 2010 23:09:04 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Sep 2010 11:40:50 GMT",
"version": "v2"
},
{
"created": "Sat, 28 May 2011 02:05:12 GMT",
"version": "v3"
}
] | 2011-07-20 | [
[
"Button",
"Bradly K.",
""
],
[
"Rodriguez",
"Leo",
""
],
[
"Whiting",
"Catherine A.",
""
],
[
"Yildirim",
"Tuna",
""
]
] | We show that the near horizon regime of a Kerr-Newman-$AdS$ (KN$AdS$) black hole, given by its two dimensional analogue $a la$ Robinson and Wilczek (2005 Phys. Rev. Lett. 95 011303), is asymptotically $AdS_2$ and dual to a one dimensional quantum conformal field theory (CFT). The s-wave contribution of the resulting CF... | 7.096309 | 7.441722 | 8.003348 | 6.791057 | 7.0218 | 7.243983 | 7.40615 | 6.692371 | 6.698504 | 8.874523 | 6.641856 | 6.966859 | 7.411698 | 7.033376 | 7.352149 | 6.874569 | 7.295515 | 7.07978 | 7.20391 | 7.531913 | 7.05934 |
hep-th/9709007 | Emil Yuzbashyan | A. N. Leznov, and E. A. Yuzbashyan | Fine Structure of Matrix Darboux-Toda Integrable Mapping | 5 pages, no figures | Phys.Lett. A242 (1998) 31-35 | 10.1016/S0375-9601(98)00135-2 | null | hep-th nlin.SI | null | We show here that matrix Darboux-Toda transformation can be written as a
product of a number of mappings. Each of these mappings is a symmetry of the
matrix nonlinear Shrodinger system of integro-differential equations. We thus
introduce a completely new type of discrete transformations for this system.
The discrete ... | [
{
"created": "Mon, 1 Sep 1997 10:57:14 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Jun 2003 03:17:04 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Leznov",
"A. N.",
""
],
[
"Yuzbashyan",
"E. A.",
""
]
] | We show here that matrix Darboux-Toda transformation can be written as a product of a number of mappings. Each of these mappings is a symmetry of the matrix nonlinear Shrodinger system of integro-differential equations. We thus introduce a completely new type of discrete transformations for this system. The discrete sy... | 13.521638 | 13.02794 | 15.033434 | 12.924194 | 11.999715 | 15.141913 | 13.418091 | 11.755155 | 11.984487 | 20.49069 | 11.970143 | 12.421247 | 12.354574 | 12.330415 | 12.256794 | 13.134828 | 12.771209 | 13.199533 | 11.986801 | 13.299782 | 12.093389 |
hep-th/0701030 | Ying-Qiu Gu | Ying-Qiu Gu | Local Lorentz Transformation and Mass-Energy Relation of Spinor | 14 pages, no figure | Physics Essays Vol. 31: 1-6(2018) | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we strictly establish classical concepts and relations
according to a Dirac equation with scalar, vector and nonlinear potentials. To
calculate classical parameters for moving spinor, the local Lorentz
transformations for parameters are derived. The calculation shows that
different kinds of potentials ... | [
{
"created": "Thu, 4 Jan 2007 15:31:54 GMT",
"version": "v1"
},
{
"created": "Sat, 4 Apr 2009 08:39:12 GMT",
"version": "v2"
},
{
"created": "Tue, 30 May 2017 12:52:52 GMT",
"version": "v3"
},
{
"created": "Mon, 11 Dec 2017 15:47:58 GMT",
"version": "v4"
}
] | 2017-12-27 | [
[
"Gu",
"Ying-Qiu",
""
]
] | In this paper, we strictly establish classical concepts and relations according to a Dirac equation with scalar, vector and nonlinear potentials. To calculate classical parameters for moving spinor, the local Lorentz transformations for parameters are derived. The calculation shows that different kinds of potentials re... | 17.294641 | 17.947447 | 16.905731 | 16.621202 | 17.191965 | 17.710936 | 17.695709 | 18.223938 | 17.830914 | 18.990685 | 17.2834 | 16.740562 | 16.157377 | 16.122435 | 16.746992 | 16.34878 | 16.444124 | 16.440231 | 16.595482 | 16.59474 | 16.349056 |
hep-th/9412073 | Karen Brewster | Abhay Ashtekar and Jerzy Lewandowski | Differential Geometry on the Space of Connections via Graphs and
Projective Limits | Minor corrections have been made. 54 pages, LATEX file, no figures | J.Geom.Phys. 17 (1995) 191-230 | 10.1016/0393-0440(95)00028-G | CGPG-94/12-4 | hep-th gr-qc | null | In a quantum mechanical treatment of gauge theories (including general
relativity), one is led to consider a certain completion, $\agb$, of the space
$\ag$ of gauge equivalent connections. This space serves as the quantum
configuration space, or, as the space of all Euclidean histories over which one
must integrate i... | [
{
"created": "Thu, 8 Dec 1994 18:41:47 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Jan 1996 16:50:44 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Ashtekar",
"Abhay",
""
],
[
"Lewandowski",
"Jerzy",
""
]
] | In a quantum mechanical treatment of gauge theories (including general relativity), one is led to consider a certain completion, $\agb$, of the space $\ag$ of gauge equivalent connections. This space serves as the quantum configuration space, or, as the space of all Euclidean histories over which one must integrate in ... | 8.090426 | 8.896028 | 8.78683 | 7.999505 | 8.687791 | 8.68257 | 8.489303 | 8.183001 | 8.099365 | 8.368371 | 8.222278 | 8.206835 | 8.121037 | 7.674159 | 7.918896 | 7.928644 | 7.740388 | 7.686505 | 7.918537 | 8.17792 | 7.830672 |
2404.19160 | Tomohiro Matsuda | Tomohiro Matsuda | How to define the Unruh-DeWitt detector on manifolds | 21 pages, 6 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The vacuum of an accelerating observer is defined on the local inertial
frame, which is called a ``moving frame''. However, in the discussion of the
Unruh-deWitt detector, many papers define the vacuum on a fixed frame. This
paper discusses the Unruh-deWitt detector by defining the vacuum directly on
the local inerti... | [
{
"created": "Mon, 29 Apr 2024 23:50:02 GMT",
"version": "v1"
}
] | 2024-05-01 | [
[
"Matsuda",
"Tomohiro",
""
]
] | The vacuum of an accelerating observer is defined on the local inertial frame, which is called a ``moving frame''. However, in the discussion of the Unruh-deWitt detector, many papers define the vacuum on a fixed frame. This paper discusses the Unruh-deWitt detector by defining the vacuum directly on the local inertial... | 12.301446 | 10.869791 | 12.028369 | 11.426893 | 12.014102 | 14.38305 | 12.822258 | 11.541276 | 12.383484 | 13.096893 | 10.914807 | 10.969728 | 11.005638 | 11.082324 | 11.245512 | 10.735735 | 10.940464 | 11.069002 | 11.355557 | 10.919643 | 11.112224 |
1304.5946 | Jeong-Hyuck Park | Jeong-Hyuck Park | Comments on double field theory and diffeomorphisms | 1+34 pages; A minute change of the title from "diffeomorphism" to
"diffeomorphisms". To appear in JHEP | JHEP 1306 (2013) 098 | 10.1007/JHEP06(2013)098 | DAMTP-2013-30 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As the theory is subject to a section condition, coordinates in double field
theory do not represent physical points in an injective manner. We argue that a
physical point should be rather one-to-one identified with a `gauge orbit' in
the coordinate space. The diffeomorphism symmetry then implies an invariance
under ... | [
{
"created": "Mon, 22 Apr 2013 13:30:33 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Jun 2013 08:56:50 GMT",
"version": "v2"
}
] | 2013-07-05 | [
[
"Park",
"Jeong-Hyuck",
""
]
] | As the theory is subject to a section condition, coordinates in double field theory do not represent physical points in an injective manner. We argue that a physical point should be rather one-to-one identified with a `gauge orbit' in the coordinate space. The diffeomorphism symmetry then implies an invariance under ar... | 15.392348 | 15.563974 | 15.395681 | 13.000262 | 14.77553 | 14.818358 | 14.339179 | 13.400371 | 13.650299 | 15.964396 | 13.021257 | 12.39336 | 12.81856 | 12.611779 | 12.253326 | 12.424878 | 12.870515 | 12.327329 | 12.667841 | 12.206111 | 12.694508 |
hep-th/9210077 | Harnad John | J. Harnad and M.-A. Wisse | Isospectral flow in Loop Algebras and Quasiperiodic Solutions of the
Sine-Gordon Equation | 12 pgs | J.Math.Phys. 34 (1993) 3518-3526 | 10.1063/1.530041 | Univ. de Montr\'eal preprint, CRM-1831 | hep-th | null | The sine-Gordon equation is considered in the hamiltonian framework provided
by the Adler-Kostant-Symes theorem. The phase space, a finite dimensional
coadjoint orbit in the dual space $\grg^*$ of a loop algebra $\grg$, is
parametrized by a finite dimensional symplectic vector space $W$ embedded into
$\grg^*$ by a mo... | [
{
"created": "Wed, 14 Oct 1992 17:30:03 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Harnad",
"J.",
""
],
[
"Wisse",
"M. -A.",
""
]
] | The sine-Gordon equation is considered in the hamiltonian framework provided by the Adler-Kostant-Symes theorem. The phase space, a finite dimensional coadjoint orbit in the dual space $\grg^*$ of a loop algebra $\grg$, is parametrized by a finite dimensional symplectic vector space $W$ embedded into $\grg^*$ by a mome... | 8.04469 | 8.385671 | 9.734701 | 8.421472 | 8.320772 | 9.071332 | 7.912841 | 7.593026 | 7.187212 | 9.676945 | 8.272234 | 7.807549 | 7.981794 | 7.664993 | 7.863648 | 7.732169 | 7.910305 | 7.695976 | 7.701966 | 7.943008 | 7.720281 |
hep-th/0701181 | Fabio Pascoal | F. Pascoal, L.F.A. Oliveira, F.S.S. Rosa and C. Farina | Estimative for the size of the compactification radius of a one extra
dimension Universe | null | Braz.J.Phys.38:581-586,2008 | 10.1590/S0103-97332008000500009 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we use the Casimir effect to probe the existence of one extra
dimension. We begin by evaluating the Casimir pressure between two plates in a
$M^4\times S^1$ manifold, and then use an appropriate statistical analysis in
order to compare the theoretical expression with a recent experimental data and
set b... | [
{
"created": "Fri, 19 Jan 2007 13:41:00 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Mar 2007 19:35:01 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Sep 2008 12:49:25 GMT",
"version": "v3"
}
] | 2011-08-31 | [
[
"Pascoal",
"F.",
""
],
[
"Oliveira",
"L. F. A.",
""
],
[
"Rosa",
"F. S. S.",
""
],
[
"Farina",
"C.",
""
]
] | In this work, we use the Casimir effect to probe the existence of one extra dimension. We begin by evaluating the Casimir pressure between two plates in a $M^4\times S^1$ manifold, and then use an appropriate statistical analysis in order to compare the theoretical expression with a recent experimental data and set bou... | 9.43503 | 6.722819 | 7.37369 | 7.172029 | 7.964456 | 7.759518 | 7.668241 | 7.945018 | 7.178642 | 7.839931 | 7.874729 | 8.1758 | 7.578239 | 7.450668 | 7.820973 | 7.984661 | 7.871877 | 7.605376 | 7.853351 | 7.433948 | 8.014833 |
1208.3373 | Antonio Padilla | Edmund J. Copeland, Antonio Padilla and Paul M. Saffin | The cosmology of the Fab-Four | Stability analysis corrected. New matter dominated solution with
stable cosmological perturbations added | null | 10.1088/1475-7516/2012/12/026 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have recently proposed a novel self tuning mechanism to alleviate the
famous cosmological constant problem, based on the general scalar tensor theory
proposed by Horndeski. The self-tuning model ends up consisting of four
geometric terms in the action, with each term containing a free potential
function of the sca... | [
{
"created": "Thu, 16 Aug 2012 13:57:06 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Dec 2013 16:19:02 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Copeland",
"Edmund J.",
""
],
[
"Padilla",
"Antonio",
""
],
[
"Saffin",
"Paul M.",
""
]
] | We have recently proposed a novel self tuning mechanism to alleviate the famous cosmological constant problem, based on the general scalar tensor theory proposed by Horndeski. The self-tuning model ends up consisting of four geometric terms in the action, with each term containing a free potential function of the scala... | 12.82879 | 11.631087 | 11.645891 | 10.897265 | 12.867346 | 12.434198 | 12.427962 | 11.405388 | 11.813412 | 12.756781 | 11.479256 | 11.82713 | 11.218424 | 11.311373 | 11.462912 | 11.525451 | 11.916214 | 11.543414 | 11.833302 | 12.051333 | 11.552188 |
hep-th/9302126 | Gary Horowitz | Gary T. Horowitz and Dean L. Welch | Exact Three Dimensional Black Holes in String Theory | 11 pages, NSF-ITP-93-21, harvmac | Phys.Rev.Lett.71:328-331,1993 | 10.1103/PhysRevLett.71.328 | null | hep-th gr-qc | null | A black hole solution to three dimensional general relativity with a negative
cosmological constant has recently been found. We show that a slight
modification of this solution yields an exact solution to string theory. This
black hole is equivalent (under duality) to the previously discussed three
dimensional black ... | [
{
"created": "Fri, 26 Feb 1993 00:37:00 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Horowitz",
"Gary T.",
""
],
[
"Welch",
"Dean L.",
""
]
] | A black hole solution to three dimensional general relativity with a negative cosmological constant has recently been found. We show that a slight modification of this solution yields an exact solution to string theory. This black hole is equivalent (under duality) to the previously discussed three dimensional black st... | 6.15757 | 5.296936 | 5.524553 | 5.126821 | 5.376768 | 5.428207 | 5.737778 | 5.369968 | 5.314282 | 5.733684 | 5.392654 | 5.877566 | 5.615334 | 5.41779 | 5.82046 | 5.570912 | 5.647195 | 5.459831 | 5.573109 | 5.517776 | 5.506243 |
hep-th/9210022 | Judy Mack | C. R. Hagen | Comment on Gauge-Independent Analysis of Chern-Simons Theory with Matter
Coupling | 4 pages | Phys.Rev.Lett. 70 (1993) 3518 | 10.1103/PhysRevLett.70.3518 | UR-1280 | hep-th | null | It is shown that a recently proposed relativistic field theory of anyons is
mathematically flawed and also does not satisfy reasonable criteria for such a
theory.
| [
{
"created": "Mon, 5 Oct 1992 16:37:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Hagen",
"C. R.",
""
]
] | It is shown that a recently proposed relativistic field theory of anyons is mathematically flawed and also does not satisfy reasonable criteria for such a theory. | 15.530787 | 8.794071 | 12.601028 | 10.682247 | 9.21276 | 10.300289 | 9.994687 | 10.705841 | 11.228926 | 13.03963 | 11.119756 | 12.049685 | 13.079453 | 11.190755 | 11.494871 | 12.002876 | 11.258585 | 12.006571 | 11.63261 | 12.568563 | 11.105404 |
1610.07790 | Komeil Babaei Velni | Komeil Babaei Velni and H. Babaei-Aghbolagh | On SL(2;R) symmetry in nonlinear electrodynamics theories | 14 pages; V2: an appendix is added, final version to appear in
Nuclear Physics B | Nucl.Phys. B913 (2016) 987-1000 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, it has been observed that the Noether-Gaillard-Zumino (NGZ)
identity holds order by order in $\alpha'$ expansion in nonlinear
electrodynamics theories as Born-Infeld (BI) and Bossard-Nicolai (BN). The
nonlinear electrodynamics theory that couples to an axion field is invariant
under the $SL(2,R)$ duality in... | [
{
"created": "Tue, 25 Oct 2016 08:52:40 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Dec 2016 08:43:24 GMT",
"version": "v2"
}
] | 2016-12-28 | [
[
"Velni",
"Komeil Babaei",
""
],
[
"Babaei-Aghbolagh",
"H.",
""
]
] | Recently, it has been observed that the Noether-Gaillard-Zumino (NGZ) identity holds order by order in $\alpha'$ expansion in nonlinear electrodynamics theories as Born-Infeld (BI) and Bossard-Nicolai (BN). The nonlinear electrodynamics theory that couples to an axion field is invariant under the $SL(2,R)$ duality in a... | 6.183702 | 6.525479 | 6.960817 | 5.642049 | 5.701256 | 5.687324 | 5.865417 | 5.587735 | 5.475247 | 7.241233 | 5.651168 | 5.847524 | 6.050272 | 5.490988 | 5.592063 | 5.72145 | 5.787803 | 5.797787 | 5.638912 | 6.098704 | 5.84748 |
1405.5290 | Arash Arabi Ardehali | Arash Arabi Ardehali, Leopoldo A. Pando Zayas | On Exactly Marginal Deformations Dual to $B$-Field Moduli of IIB Theory
on SE$_5$ | 28 pages, JHEP style. v2: minor corrections, added references and
acknowledgements. v3: a number of speculative comments regarding the
application of the Konishi anomaly equation to our problem are removed. v4:
the proposal in Eq. (2.4) added back as a conjecture | JHEP 2014 (9), 164 | 10.1007/JHEP09(2014)164 | MCTP-14-14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complex dimension of the space of exactly marginal deformations for
quiver CFTs dual to IIB theory compactified on $Y^{p,q}$ is known to be
generically three. Simple general formulas already exist for two of the exactly
marginal directions in the space of couplings, one of which corresponds to the
sum of the (inv... | [
{
"created": "Wed, 21 May 2014 03:45:55 GMT",
"version": "v1"
},
{
"created": "Mon, 26 May 2014 03:32:28 GMT",
"version": "v2"
},
{
"created": "Sun, 15 Jun 2014 01:19:40 GMT",
"version": "v3"
},
{
"created": "Thu, 31 Jul 2014 20:05:55 GMT",
"version": "v4"
}
] | 2015-06-12 | [
[
"Ardehali",
"Arash Arabi",
""
],
[
"Zayas",
"Leopoldo A. Pando",
""
]
] | The complex dimension of the space of exactly marginal deformations for quiver CFTs dual to IIB theory compactified on $Y^{p,q}$ is known to be generically three. Simple general formulas already exist for two of the exactly marginal directions in the space of couplings, one of which corresponds to the sum of the (inver... | 10.628606 | 9.949659 | 12.039399 | 9.487783 | 10.301637 | 9.936203 | 10.007511 | 9.805051 | 9.655468 | 12.753257 | 9.135732 | 10.058607 | 11.07702 | 9.798003 | 9.846035 | 9.91067 | 10.046055 | 9.701872 | 9.725924 | 10.722415 | 9.674998 |
hep-th/9803087 | Witold Skiba | Gustavo Dotti, Aneesh V. Manohar, and Witold Skiba (UC, San Diego) | Supersymmetric gauge theories with a free algebra of invariants | 19 pages, Section 2.1 extended, references added | Nucl.Phys. B531 (1998) 507-524 | 10.1016/S0550-3213(98)00523-9 | UCSD/PTH 98-09 | hep-th | null | We study the low-energy dynamics of all N=1 supersymmetric gauge theories
whose basic gauge invariant fields are unconstrained. This set includes all
theories whose matter Dynkin index is less than the index of the adjoint
representation. We study the dynamically generated superpotential in these
theories, and show t... | [
{
"created": "Wed, 11 Mar 1998 02:23:40 GMT",
"version": "v1"
},
{
"created": "Sat, 29 Aug 1998 23:58:08 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Dotti",
"Gustavo",
"",
"UC, San Diego"
],
[
"Manohar",
"Aneesh V.",
"",
"UC, San Diego"
],
[
"Skiba",
"Witold",
"",
"UC, San Diego"
]
] | We study the low-energy dynamics of all N=1 supersymmetric gauge theories whose basic gauge invariant fields are unconstrained. This set includes all theories whose matter Dynkin index is less than the index of the adjoint representation. We study the dynamically generated superpotential in these theories, and show tha... | 8.34546 | 7.968146 | 8.121249 | 7.318877 | 7.988303 | 8.172622 | 7.994112 | 7.887852 | 7.789273 | 9.177543 | 7.625042 | 7.608809 | 8.245131 | 8.04756 | 7.760669 | 8.16394 | 7.745155 | 7.856471 | 7.66715 | 8.498647 | 7.739923 |
hep-th/9803010 | Levon Mardoyan | L.G. Mardoyan, A.N. Sissakian, V.M. Ter--Antonyan | Hidden Symmetry of the Yang--Coulomb System | 6 pages, LaTeX file | null | 10.1142/S0217732399001395 | null | hep-th | null | The bound system composed of the Yang monopole coupled to a particle of the
isospin by the SU(2) and Coulomb interaction is considered. The generalized
Runge--Lenz vector and the SO(6) group of hidden symmetry are established. It
is also shown that the group of hidden symmetry make it possible to calculate
the spectr... | [
{
"created": "Mon, 2 Mar 1998 14:15:49 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Mardoyan",
"L. G.",
""
],
[
"Sissakian",
"A. N.",
""
],
[
"Ter--Antonyan",
"V. M.",
""
]
] | The bound system composed of the Yang monopole coupled to a particle of the isospin by the SU(2) and Coulomb interaction is considered. The generalized Runge--Lenz vector and the SO(6) group of hidden symmetry are established. It is also shown that the group of hidden symmetry make it possible to calculate the spectrum... | 12.513482 | 10.026823 | 12.493893 | 9.88184 | 10.362257 | 9.428704 | 9.496606 | 10.651814 | 10.161254 | 11.77976 | 9.902482 | 10.600983 | 11.754373 | 11.199838 | 10.993908 | 11.033427 | 11.510391 | 10.872663 | 11.185374 | 11.364799 | 10.934477 |
hep-th/9903032 | Gravity Research Group | A. Burinskii | Spinning Particle as a Non-trivial Rotating Super Black Hole with Broken
N=2 Supersymmetry | 28 pages, LaTeX, invited talk at the Second International Symposium
on Frontiers of Fundamental Physics (Hyderabad, December 30, 1998 - January
1, 1999). In this version the Introduction and Conclusion are extended, and
one new section is added containing the self-consistent super-Kerr-Newman
solutions to broke... | Class.Quant.Grav.16:3497-3516,1999 | 10.1088/0264-9381/16/11/305 | null | hep-th gr-qc quant-ph | null | Non-trivial supergeneralization of the Kerr-Newman solution is considered as
representing a combined model of the Kerr-Newman spinning particle and
superparticle.
We show that the old problem of obtaining non-trivial super black hole
solutions can be resolved in supergravity broken by Goldstone fermion.
Non-linear ... | [
{
"created": "Wed, 3 Mar 1999 12:31:26 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Apr 1999 13:09:43 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Burinskii",
"A.",
""
]
] | Non-trivial supergeneralization of the Kerr-Newman solution is considered as representing a combined model of the Kerr-Newman spinning particle and superparticle. We show that the old problem of obtaining non-trivial super black hole solutions can be resolved in supergravity broken by Goldstone fermion. Non-linear real... | 15.62128 | 13.356859 | 15.631425 | 13.854997 | 13.989004 | 14.934495 | 13.669159 | 12.811969 | 13.875582 | 16.129442 | 13.558895 | 13.910182 | 14.639911 | 14.006816 | 13.778949 | 13.912251 | 14.093807 | 13.896005 | 14.331565 | 14.439305 | 14.045034 |
hep-th/9603090 | Andrei Linde | Sergio Ferrara and Renata Kallosh | Universality of Sypersymmetric Attractors | few misprints removed, version to appear in Phys. Rev. 20 pages, 1
figure | Phys. Rev. D 54, 1525 (1996) | 10.1103/PhysRevD.54.1525 | CERN-TH/96-66, SU-ITP-96-10 | hep-th | null | The macroscopic entropy-area formula for supersymmetric black holes in
N=2,4,8 theories is found to be universal: in d=4 it is always given by the
square of the largest of the central charges extremized in the moduli space.
The proof of universality is based on the fact that the doubling of unbroken
supersymmetry nea... | [
{
"created": "Thu, 14 Mar 1996 06:42:48 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jun 1996 00:03:24 GMT",
"version": "v2"
}
] | 2016-08-24 | [
[
"Ferrara",
"Sergio",
""
],
[
"Kallosh",
"Renata",
""
]
] | The macroscopic entropy-area formula for supersymmetric black holes in N=2,4,8 theories is found to be universal: in d=4 it is always given by the square of the largest of the central charges extremized in the moduli space. The proof of universality is based on the fact that the doubling of unbroken supersymmetry near ... | 9.279402 | 9.673098 | 10.532968 | 8.887774 | 9.848078 | 10.527592 | 10.32966 | 8.893563 | 9.006427 | 10.017542 | 8.809913 | 9.461916 | 9.515113 | 8.881565 | 9.134583 | 9.132734 | 9.125804 | 9.421514 | 8.974596 | 9.710283 | 8.88904 |
hep-th/0603117 | Tom Steele | V. Elias, T.G. Steele | Massless Scalar Field Propagator in a Quantized Space-Time | 6 pages, 1 eps figure embedded in manuscript | Int.J.Mod.Phys.E16:51-58,2007 | 10.1142/S0218301307004886 | null | hep-th | null | We consider in detail the analytic behaviour of the non-interacting massless
scalar field two-point function in H.S. Snyder's discretized non-commuting
spacetime. The propagator we find is purely real on the Euclidean side of the
complex $p^2$ plane and goes like $1/p^2$ as $p^2\to 0$ from either the
Euclidean or Min... | [
{
"created": "Tue, 14 Mar 2006 22:04:31 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Elias",
"V.",
""
],
[
"Steele",
"T. G.",
""
]
] | We consider in detail the analytic behaviour of the non-interacting massless scalar field two-point function in H.S. Snyder's discretized non-commuting spacetime. The propagator we find is purely real on the Euclidean side of the complex $p^2$ plane and goes like $1/p^2$ as $p^2\to 0$ from either the Euclidean or Minko... | 6.96216 | 7.481189 | 7.403555 | 7.216794 | 7.836495 | 7.532361 | 7.626595 | 7.352414 | 7.235402 | 7.917944 | 7.152507 | 6.963326 | 6.778633 | 6.871907 | 7.007047 | 6.902411 | 7.052535 | 6.69933 | 6.91105 | 7.011459 | 6.652681 |
hep-th/9403198 | Nathan Seiberg | K. Intriligator, R.G. Leigh and N. Seiberg | Exact Superpotentials in Four Dimensions | 32 pages, RU-94-26 | Phys.Rev.D50:1092-1104,1994 | 10.1103/PhysRevD.50.1092 | null | hep-th hep-ph | null | Supersymmetric gauge theories in four dimensions can display interesting
non-perturbative phenomena. Although the superpotential dynamically generated
by these phenomena can be highly nontrivial, it can often be exactly
determined. We discuss some general techniques for analyzing the Wilsonian
superpotential and demo... | [
{
"created": "Thu, 31 Mar 1994 19:38:18 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Intriligator",
"K.",
""
],
[
"Leigh",
"R. G.",
""
],
[
"Seiberg",
"N.",
""
]
] | Supersymmetric gauge theories in four dimensions can display interesting non-perturbative phenomena. Although the superpotential dynamically generated by these phenomena can be highly nontrivial, it can often be exactly determined. We discuss some general techniques for analyzing the Wilsonian superpotential and demons... | 10.582016 | 8.630385 | 10.478241 | 8.777604 | 8.993827 | 8.572306 | 8.630583 | 8.821957 | 9.388459 | 10.51869 | 8.372636 | 8.757263 | 10.042247 | 8.831873 | 8.932432 | 9.002069 | 8.603891 | 8.688346 | 9.016232 | 10.246286 | 8.732634 |
hep-th/9507128 | Brzezinski Tomasz | Tomasz Brzezinski and Jacob Katriel | Representation-theoretic derivation of the Temperley-Lieb-Martin
algebras | 12 pages, LaTeX, to appear in J. Phys. A | J.Phys. A28 (1995) 5305-5312 | 10.1088/0305-4470/28/18/019 | null | hep-th | null | Explicit expressions for the Temperley-Lieb-Martin algebras, i.e., the
quotients of the Hecke algebra that admit only representations corresponding to
Young diagrams with a given maximum number of columns (or rows), are obtained,
making explicit use of the Hecke algebra representation theory. Similar
techniques are u... | [
{
"created": "Tue, 25 Jul 1995 08:19:30 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Brzezinski",
"Tomasz",
""
],
[
"Katriel",
"Jacob",
""
]
] | Explicit expressions for the Temperley-Lieb-Martin algebras, i.e., the quotients of the Hecke algebra that admit only representations corresponding to Young diagrams with a given maximum number of columns (or rows), are obtained, making explicit use of the Hecke algebra representation theory. Similar techniques are use... | 9.33412 | 9.077004 | 10.320082 | 8.121312 | 8.749753 | 8.687474 | 8.532963 | 8.261636 | 10.339402 | 12.146204 | 8.61441 | 8.944519 | 9.105076 | 8.743601 | 8.560472 | 8.534222 | 8.996305 | 8.666695 | 8.686289 | 9.847336 | 8.541532 |
1309.5160 | Lakshya Bhardwaj | Lakshya Bhardwaj and Yuji Tachikawa | Classification of 4d N=2 gauge theories | 46 pages, v2: Corrected typos along with a typo reported by A.
Sciarappa and updated the list of known Seiberg-Witten solutions, v3:
Corrected a typo reported by G. Zafrir and updated the list of known
Seiberg-Witten solutions | null | 10.1007/JHEP12(2013)100 | IPMU-13-0179, UT-13-33 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We classify all possible four-dimensional N=2 supersymmetric UV-complete
gauge theories composed of semi-simple gauge groups and hypermultiplets. We
also give appropriate references for all theories with known Seiberg-Witten
solutions.
| [
{
"created": "Fri, 20 Sep 2013 03:20:51 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Jul 2017 22:50:00 GMT",
"version": "v2"
},
{
"created": "Thu, 30 May 2019 20:33:24 GMT",
"version": "v3"
}
] | 2019-06-03 | [
[
"Bhardwaj",
"Lakshya",
""
],
[
"Tachikawa",
"Yuji",
""
]
] | We classify all possible four-dimensional N=2 supersymmetric UV-complete gauge theories composed of semi-simple gauge groups and hypermultiplets. We also give appropriate references for all theories with known Seiberg-Witten solutions. | 16.808477 | 15.720053 | 14.144739 | 15.325859 | 13.002219 | 13.034395 | 13.983409 | 12.162354 | 11.390146 | 16.583393 | 12.64453 | 14.117948 | 13.043812 | 13.378165 | 13.121475 | 13.338402 | 12.863143 | 12.450974 | 13.042981 | 14.362948 | 12.640618 |
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