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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0802.1556 | Ashoke Sen | Shamik Banerjee, Ashoke Sen, Yogesh K. Srivastava | Partition Functions of Torsion >1 Dyons in Heterotic String Theory on
T^6 | LaTeX file, 16 pages | JHEP 0805:098,2008 | 10.1088/1126-6708/2008/05/098 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The original proposal of Dijkgraaf, Verlinde and Verlinde for the quarter BPS
dyon partition function in heterotic string theory on T^6 is known to correctly
produce the degeneracy of dyons of torsion 1, i.e. dyons for which gcd(Q\wedge
P)=1. We propose a generalization of this formula for dyons of arbitrary
torsion.... | [
{
"created": "Tue, 12 Feb 2008 02:52:52 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Banerjee",
"Shamik",
""
],
[
"Sen",
"Ashoke",
""
],
[
"Srivastava",
"Yogesh K.",
""
]
] | The original proposal of Dijkgraaf, Verlinde and Verlinde for the quarter BPS dyon partition function in heterotic string theory on T^6 is known to correctly produce the degeneracy of dyons of torsion 1, i.e. dyons for which gcd(Q\wedge P)=1. We propose a generalization of this formula for dyons of arbitrary torsion. O... | 7.328313 | 6.21417 | 10.143654 | 6.371987 | 5.893697 | 6.003887 | 5.891756 | 6.054755 | 6.649216 | 9.005409 | 6.335454 | 6.698082 | 7.663679 | 7.086791 | 6.742672 | 6.823753 | 6.906766 | 6.878903 | 6.747925 | 7.586142 | 6.731853 |
1010.3933 | N. E. J. Bjerrum-Bohr | N.E.J. Bjerrum-Bohr, Poul H. Damgaard, Thomas Sondergaard, Pierre
Vanhove | The Momentum Kernel of Gauge and Gravity Theories | 19 pages, 1 figure | JHEP 1101:001,2011 | 10.1007/JHEP01(2011)001 | IPHT-T10/14, IHES/P/10/45 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive an explicit formula for factorizing an $n$-point closed string
amplitude into open string amplitudes. Our results are phrased in terms of a
momentum kernel which in the limit of infinite string tension reduces to the
corresponding field theory kernel. The same momentum kernel encodes the
monodromy relations... | [
{
"created": "Tue, 19 Oct 2010 14:37:56 GMT",
"version": "v1"
}
] | 2011-01-27 | [
[
"Bjerrum-Bohr",
"N. E. J.",
""
],
[
"Damgaard",
"Poul H.",
""
],
[
"Sondergaard",
"Thomas",
""
],
[
"Vanhove",
"Pierre",
""
]
] | We derive an explicit formula for factorizing an $n$-point closed string amplitude into open string amplitudes. Our results are phrased in terms of a momentum kernel which in the limit of infinite string tension reduces to the corresponding field theory kernel. The same momentum kernel encodes the monodromy relations w... | 9.235005 | 8.827387 | 9.711122 | 9.047687 | 9.158569 | 8.66744 | 8.633637 | 9.112131 | 9.173167 | 9.799359 | 9.288517 | 9.499372 | 8.945955 | 8.87068 | 9.028444 | 9.137094 | 9.223819 | 9.245587 | 9.136256 | 9.493678 | 9.030836 |
hep-th/0411097 | Kuperstein Stanislav | S. Kuperstein | Meson spectroscopy from holomorphic probes on the warped deformed
conifold | 22 pages, JHEP style, 2 figures | JHEP 0503:014,2005 | 10.1088/1126-6708/2005/03/014 | TAUP-2789-04 | hep-th | null | We study D7 brane probes holomorphically embedded in the Klebanov-Strassler
model. Analyzing the $\kappa$-symmetry condition for D7 branes wrapping a
4-cycle of a deformed conifold we find configurations that do not break N=1
supersymmetry of the background. We compute the fluctuations of the probe
around one of thes... | [
{
"created": "Tue, 9 Nov 2004 18:00:34 GMT",
"version": "v1"
}
] | 2009-08-18 | [
[
"Kuperstein",
"S.",
""
]
] | We study D7 brane probes holomorphically embedded in the Klebanov-Strassler model. Analyzing the $\kappa$-symmetry condition for D7 branes wrapping a 4-cycle of a deformed conifold we find configurations that do not break N=1 supersymmetry of the background. We compute the fluctuations of the probe around one of these ... | 6.727602 | 5.633291 | 7.596597 | 5.365126 | 5.52705 | 5.119472 | 5.462505 | 5.426335 | 5.869086 | 6.963881 | 5.71721 | 5.533922 | 6.586289 | 5.889954 | 5.774849 | 5.671587 | 5.789692 | 5.551755 | 5.8603 | 6.712415 | 5.618461 |
hep-th/9608141 | Frank Antonsen | Frank Antonsen, Karsten Bormann | Propagators in Curved Space | standard LaTeX, 34 pages | null | null | null | hep-th | null | We demonstrate how to obtain explicitly the propagators for quantum fields
residing in curved space-time using the heat kernel for which a new
construction procedure exists. Propagators are determined for the case of
Rindler, Friedman-Robertson-Walker, Schwarzschild and general conformally flat
metrics, both for scal... | [
{
"created": "Wed, 21 Aug 1996 09:16:54 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Antonsen",
"Frank",
""
],
[
"Bormann",
"Karsten",
""
]
] | We demonstrate how to obtain explicitly the propagators for quantum fields residing in curved space-time using the heat kernel for which a new construction procedure exists. Propagators are determined for the case of Rindler, Friedman-Robertson-Walker, Schwarzschild and general conformally flat metrics, both for scalar... | 10.085234 | 10.208727 | 9.314996 | 9.23461 | 9.611089 | 10.366126 | 10.324891 | 9.751706 | 9.692554 | 9.5496 | 9.41339 | 9.526628 | 9.286552 | 9.394843 | 9.379618 | 9.373698 | 9.445687 | 9.192703 | 9.44405 | 9.328775 | 9.222675 |
1512.07626 | Nikita G. Misuna | V.E. Didenko, N.G. Misuna, M.A. Vasiliev | Charges in nonlinear higher-spin theory | 23 pages; V3: typos corrected; references and acknowledgement added;
example of the topological contribution to spin-4 charge added; new Section
3.1 added establishing relation of our construction for asymptotic charges
with the canonical one. Version published in JHEP | JHEP 03 (2017) 164 | 10.1007/JHEP03(2017)164 | FIAN/TD/2015-19 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Nonlinear higher-spin equations in four dimensions admit a closed two-form
that defines a gauge-invariant global charge as an integral over a
two-dimensional cycle. In this paper we argue that this charge gives rise to
partitions depending on various lower- and higher-spin chemical potentials
identified with modules ... | [
{
"created": "Wed, 23 Dec 2015 20:54:06 GMT",
"version": "v1"
},
{
"created": "Sun, 18 Sep 2016 23:50:23 GMT",
"version": "v2"
},
{
"created": "Wed, 29 Mar 2017 15:20:54 GMT",
"version": "v3"
}
] | 2017-04-04 | [
[
"Didenko",
"V. E.",
""
],
[
"Misuna",
"N. G.",
""
],
[
"Vasiliev",
"M. A.",
""
]
] | Nonlinear higher-spin equations in four dimensions admit a closed two-form that defines a gauge-invariant global charge as an integral over a two-dimensional cycle. In this paper we argue that this charge gives rise to partitions depending on various lower- and higher-spin chemical potentials identified with modules of... | 15.94416 | 17.973888 | 17.807766 | 15.48205 | 17.289129 | 18.38777 | 17.979727 | 16.477839 | 16.562231 | 18.691544 | 16.357868 | 15.710963 | 16.509245 | 15.108846 | 15.426225 | 15.396444 | 15.077153 | 15.503965 | 15.405771 | 16.373205 | 15.361827 |
1512.04401 | Aurelio Romero-Berm\'udez | Antonio M. Garc\'ia-Garc\'ia and Aurelio Romero-Berm\'udez | Drude weight and Mazur-Suzuki bounds in holography | 37 pages, 6 figures | Phys. Rev. D 93, 066015 (2016) | 10.1103/PhysRevD.93.066015 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the Drude weight and the related Mazur-Suzuki (MS) bound in a
broad variety of strongly coupled field theories with a gravity dual at finite
temperature and chemical potential. We revisit the derivation of the recently
proposed universal expression for the Drude weight for Einstein-Maxwell-dilaton
(EMd... | [
{
"created": "Mon, 14 Dec 2015 16:45:55 GMT",
"version": "v1"
}
] | 2016-04-06 | [
[
"García-García",
"Antonio M.",
""
],
[
"Romero-Bermúdez",
"Aurelio",
""
]
] | We investigate the Drude weight and the related Mazur-Suzuki (MS) bound in a broad variety of strongly coupled field theories with a gravity dual at finite temperature and chemical potential. We revisit the derivation of the recently proposed universal expression for the Drude weight for Einstein-Maxwell-dilaton (EMd) ... | 7.157194 | 7.626741 | 8.23972 | 6.988084 | 7.453964 | 7.415441 | 6.781564 | 7.12931 | 6.874418 | 8.436563 | 6.94473 | 6.87322 | 7.031076 | 6.896078 | 6.768916 | 6.977277 | 6.792377 | 7.005236 | 6.677864 | 7.127479 | 6.750228 |
2109.02996 | Ashis Saha | Ashis Saha, Sunandan Gangopadhyay and Jyoti Prasad Saha | Mutual information, islands in black holes and the Page curve | v1: 5 pages LaTex and 1 figure, v2: 9 pages Latex and 1 figure, v3:
Additional comments have been added, to appear in EPJC | European Physical Journal C 82, 476 (2022) | 10.1140/epjc/s10052-022-10426-6 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The role played by the mutual information of subsystems on the Page curve is
explored in this paper. With the total system consisting of the black hole and
radiation, together with the inclusion of island, we observe that the vanishing
of mutual information between $B_+$ and $B_-$ which in turn means the
disconnected... | [
{
"created": "Tue, 7 Sep 2021 11:16:12 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Feb 2022 06:15:28 GMT",
"version": "v2"
},
{
"created": "Mon, 16 May 2022 13:58:40 GMT",
"version": "v3"
}
] | 2022-05-25 | [
[
"Saha",
"Ashis",
""
],
[
"Gangopadhyay",
"Sunandan",
""
],
[
"Saha",
"Jyoti Prasad",
""
]
] | The role played by the mutual information of subsystems on the Page curve is explored in this paper. With the total system consisting of the black hole and radiation, together with the inclusion of island, we observe that the vanishing of mutual information between $B_+$ and $B_-$ which in turn means the disconnected p... | 12.238628 | 8.927503 | 11.882366 | 9.382194 | 9.818015 | 9.247186 | 9.416807 | 9.495707 | 8.967874 | 11.992198 | 9.629971 | 10.937111 | 11.200946 | 10.335331 | 10.153678 | 10.702703 | 10.497231 | 10.679826 | 10.687276 | 10.868102 | 10.769452 |
1301.6368 | Michel Pleimling | Nickolas Gray, Djordje Minic, and Michel Pleimling | On non-equilibrium physics and string theory | 29 pages, one figure, invited review article to appear in Int. J.
Mod. Phys. A | Int. J. Mod. Phys. A 28, 1330009 (2013) | 10.1142/S0217751X13300093 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we review the relation between string theory and
non-equilibrium physics based on our previously published work. First we
explain why a theory of quantum gravity and non-equilibrium statistical physics
should be related in the first place. Then we present the necessary background
from the recent resea... | [
{
"created": "Sun, 27 Jan 2013 15:46:12 GMT",
"version": "v1"
}
] | 2013-03-18 | [
[
"Gray",
"Nickolas",
""
],
[
"Minic",
"Djordje",
""
],
[
"Pleimling",
"Michel",
""
]
] | In this article we review the relation between string theory and non-equilibrium physics based on our previously published work. First we explain why a theory of quantum gravity and non-equilibrium statistical physics should be related in the first place. Then we present the necessary background from the recent researc... | 6.637354 | 6.593369 | 7.033056 | 6.592313 | 6.395362 | 6.820117 | 7.020566 | 6.439994 | 6.439661 | 7.162681 | 6.511634 | 6.347173 | 6.517998 | 6.370891 | 6.4064 | 6.335756 | 6.411902 | 6.411865 | 6.476446 | 6.669603 | 6.357253 |
hep-th/0205120 | Olkhov | O. A. Olkhov | Topological interpretation of Dirac equation and geometrisation of
electromagnetic field | 9 pages, LaTex, Contibution to Proceedings of the XXIV International
Workshop on the Fundamental Problems of High Energy Physics and Field Theory,
27-29 June, Protvino, Russia | null | null | null | hep-th | null | A new concept of geometrization of electromagnetic field is proposed. Instead
of the concept of extended field and its point sources, the interacting
Maxwellian and Dirac electron--positron fields are considered as a microscopic
unified closed connected nonmetrized space--time 4-manifold. Within this
approach, the Di... | [
{
"created": "Mon, 13 May 2002 17:31:18 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Olkhov",
"O. A.",
""
]
] | A new concept of geometrization of electromagnetic field is proposed. Instead of the concept of extended field and its point sources, the interacting Maxwellian and Dirac electron--positron fields are considered as a microscopic unified closed connected nonmetrized space--time 4-manifold. Within this approach, the Dira... | 9.789348 | 8.889803 | 10.683441 | 9.422524 | 10.095299 | 9.161496 | 10.546255 | 9.375499 | 9.069228 | 10.744807 | 9.233775 | 8.949383 | 9.62106 | 9.407716 | 9.405846 | 9.388477 | 9.637443 | 8.907855 | 9.066119 | 9.553567 | 9.297514 |
hep-th/0201080 | null | F. Cannata (Bologna), M. V. Ioffe (St.Petersburg), D. N. Nishnianidze
(St.Petersburg and Kutaisi) | New Methods for Two-Dimensional Schr\"odinger Equation: SUSY-separation
of Variables and Shape Invariance | 25 pages, Latex, Journal of Physics A, to be published | J.Phys.A35:1389-1404,2002 | 10.1088/0305-4470/35/6/305 | null | hep-th math-ph math.MP nlin.SI quant-ph | null | Two new methods for investigation of two-dimensional quantum systems, whose
Hamiltonians are not amenable to separation of variables, are proposed. 1)The
first one - $SUSY-$ separation of variables - is based on the intertwining
relations of Higher order SUSY Quantum Mechanics (HSUSY QM) with supercharges
allowing fo... | [
{
"created": "Sun, 13 Jan 2002 16:16:33 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cannata",
"F.",
"",
"Bologna"
],
[
"Ioffe",
"M. V.",
"",
"St.Petersburg"
],
[
"Nishnianidze",
"D. N.",
"",
"St.Petersburg and Kutaisi"
]
] | Two new methods for investigation of two-dimensional quantum systems, whose Hamiltonians are not amenable to separation of variables, are proposed. 1)The first one - $SUSY-$ separation of variables - is based on the intertwining relations of Higher order SUSY Quantum Mechanics (HSUSY QM) with supercharges allowing for ... | 7.893246 | 6.701897 | 9.156336 | 6.911808 | 7.659255 | 7.433109 | 7.46311 | 7.158843 | 7.255069 | 8.690475 | 6.970613 | 7.436974 | 7.693851 | 7.439261 | 7.730892 | 7.307553 | 7.483123 | 7.464575 | 7.462563 | 7.85726 | 7.271058 |
hep-th/9807171 | Riccardo Argurio | Riccardo Argurio | Brane Physics in M-theory | 206 pages, Latex (three times), no figures. PhD thesis (Universite
Libre de Bruxelles). One reference modified | null | null | ULB-TH-98/15 | hep-th | null | The thesis begins with an introduction to M-theory (at a graduate student's
level), starting from perturbative string theory and proceeding to dualities,
D-branes and finally Matrix theory. The following chapter treats, in a
self-contained way, of general classical p-brane solutions. Black and extremal
branes are rev... | [
{
"created": "Wed, 22 Jul 1998 16:38:56 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Sep 1998 15:52:44 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Argurio",
"Riccardo",
""
]
] | The thesis begins with an introduction to M-theory (at a graduate student's level), starting from perturbative string theory and proceeding to dualities, D-branes and finally Matrix theory. The following chapter treats, in a self-contained way, of general classical p-brane solutions. Black and extremal branes are revie... | 8.796543 | 9.115867 | 10.150336 | 9.154889 | 8.862103 | 9.065669 | 9.320045 | 9.755247 | 8.981892 | 11.298201 | 9.018389 | 8.679998 | 9.383267 | 8.989709 | 8.935018 | 8.951026 | 8.913651 | 8.884321 | 9.149776 | 9.344698 | 8.935497 |
hep-th/9701087 | Dr N. Mavromatos | I.J.R. Aitchison, N.E. Mavromatos, D. Mc Neill | Inverse Landau-Khalatnikov Transformation and Infrared Critical
Exponents of (2+1)-dimensional Quantum Electrodynamics | 13 pages LATEX, 1 Figure (included automatically) | Phys.Lett. B402 (1997) 154-158 | 10.1016/S0370-2693(97)00447-4 | OUTP-96-76-P | hep-th cond-mat | null | By applying an inverse Landau-Khalatnikov transformation, connecting
(resummed) Schwinger-Dyson treatments in non-local and Landau gauges of
$QED_3$, we derive the infrared behaviour of the wave-function renormalization
in the Landau gauge, and the associated critical exponents in the normal phase
of the theory (no m... | [
{
"created": "Fri, 17 Jan 1997 19:46:38 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Aitchison",
"I. J. R.",
""
],
[
"Mavromatos",
"N. E.",
""
],
[
"Neill",
"D. Mc",
""
]
] | By applying an inverse Landau-Khalatnikov transformation, connecting (resummed) Schwinger-Dyson treatments in non-local and Landau gauges of $QED_3$, we derive the infrared behaviour of the wave-function renormalization in the Landau gauge, and the associated critical exponents in the normal phase of the theory (no mas... | 10.145626 | 8.236348 | 9.059391 | 8.847776 | 8.947962 | 9.824288 | 10.22664 | 9.528447 | 8.593689 | 9.875453 | 9.382815 | 9.217529 | 9.262996 | 9.275155 | 9.577211 | 9.623964 | 9.359952 | 9.396016 | 9.322481 | 9.366006 | 9.304202 |
hep-th/0406093 | Sebastian de Haro | Sebastian de Haro, Miguel Tierz | Brownian Motion, Chern-Simons Theory, and 2d Yang-Mills | 12 pages, v2: typos corrected, reference added | Phys.Lett. B601 (2004) 201-208 | 10.1016/j.physletb.2004.09.033 | AEI-2004-044 | hep-th cond-mat.stat-mech math-ph math.MP | null | We point out a precise connection between Brownian motion, Chern-Simons
theory on S^3, and 2d Yang-Mills theory on the cylinder. The probability of
reunion for N vicious walkers on a line gives the partition function of
Chern-Simons theory on S^3 with gauge group U(N). The probability of starting
with an equal-spacin... | [
{
"created": "Thu, 10 Jun 2004 20:01:42 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Dec 2004 08:44:52 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"de Haro",
"Sebastian",
""
],
[
"Tierz",
"Miguel",
""
]
] | We point out a precise connection between Brownian motion, Chern-Simons theory on S^3, and 2d Yang-Mills theory on the cylinder. The probability of reunion for N vicious walkers on a line gives the partition function of Chern-Simons theory on S^3 with gauge group U(N). The probability of starting with an equal-spacing ... | 9.604526 | 10.289918 | 11.224129 | 9.00624 | 9.991394 | 9.774249 | 9.842787 | 9.862701 | 10.284105 | 11.13685 | 10.031244 | 9.46477 | 9.659703 | 9.251497 | 9.322308 | 9.598166 | 9.600076 | 9.433275 | 9.257259 | 9.55067 | 9.244918 |
hep-th/9705012 | Hitoshi Sato | Hitoshi Sato | Non-Perturbative Superpotentials in Landau-Ginzburg Compactification | 9 pages, Latex 2.09, no figure | null | null | OU-HET 263 | hep-th alg-geom math.AG | null | We study the Landau-Ginzburg models which correspond to Calabi-Yau
four-folds. We construct the index of the typical states which correspond to
toric divisors. This index shows that whether a corresponding divisor can
generate a non-perturbative superpotential. For an application, we consider the
phase transition in ... | [
{
"created": "Sun, 4 May 1997 11:24:30 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Sato",
"Hitoshi",
""
]
] | We study the Landau-Ginzburg models which correspond to Calabi-Yau four-folds. We construct the index of the typical states which correspond to toric divisors. This index shows that whether a corresponding divisor can generate a non-perturbative superpotential. For an application, we consider the phase transition in te... | 11.679131 | 10.915218 | 14.088983 | 10.940759 | 10.962049 | 11.013605 | 10.988748 | 10.695247 | 10.696295 | 13.321317 | 10.619145 | 10.707401 | 12.197927 | 11.06117 | 10.67605 | 10.789976 | 10.898622 | 10.831799 | 11.237916 | 12.364025 | 10.764677 |
hep-th/9912228 | N. L. Harshman | Arno R. Bohm, N.L. Harshman and M.J. Mithaiwala | Relativistic Resonances, Relativistic Gamow Vectors and Representations
of the Poincare' Semigroup | 11 pages, 1 figure. To be published in Proceedings of the
International Symposium `Quantum Theory and Symmetries' (Goslar, 18-22 July
1999), H.-D. Doebner, V.K. Dobrev, J.-D. Hennig and W. Luecke, eds | null | null | null | hep-th | null | The foundations of time asymmetric quantum theory are reviewed and are
applied to the construction of relativistic Gamow vectors. Relativistic Gamow
vectors are obtained from the resonance pole of the S-matrix and furnish an
irreducible representation of the Poincare' semigroup. They have all the
properties needed to... | [
{
"created": "Wed, 22 Dec 1999 16:57:05 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bohm",
"Arno R.",
""
],
[
"Harshman",
"N. L.",
""
],
[
"Mithaiwala",
"M. J.",
""
]
] | The foundations of time asymmetric quantum theory are reviewed and are applied to the construction of relativistic Gamow vectors. Relativistic Gamow vectors are obtained from the resonance pole of the S-matrix and furnish an irreducible representation of the Poincare' semigroup. They have all the properties needed to r... | 11.837627 | 11.664598 | 13.105292 | 11.714754 | 11.281871 | 10.238198 | 12.126027 | 10.839249 | 10.252759 | 13.927982 | 10.895434 | 11.472875 | 10.993055 | 10.675515 | 10.659914 | 10.960249 | 10.729616 | 11.24668 | 10.321751 | 10.96898 | 10.941461 |
0812.3761 | Harold Steinacker | Harold Steinacker | Covariant Field Equations, Gauge Fields and Conservation Laws from
Yang-Mills Matrix Models | 31 pages. V2: minor corrections, references added | JHEP 0902:044,2009 | 10.1088/1126-6708/2009/02/044 | UWTHPh-2008-20 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The effective geometry and the gravitational coupling of nonabelian gauge and
scalar fields on generic NC branes in Yang-Mills matrix models is determined.
Covariant field equations are derived from the basic matrix equations of
motions, known as Yang-Mills algebra. Remarkably, the equations of motion for
the Poisson... | [
{
"created": "Fri, 19 Dec 2008 14:52:10 GMT",
"version": "v1"
},
{
"created": "Sun, 4 Jan 2009 13:53:13 GMT",
"version": "v2"
}
] | 2010-08-12 | [
[
"Steinacker",
"Harold",
""
]
] | The effective geometry and the gravitational coupling of nonabelian gauge and scalar fields on generic NC branes in Yang-Mills matrix models is determined. Covariant field equations are derived from the basic matrix equations of motions, known as Yang-Mills algebra. Remarkably, the equations of motion for the Poisson s... | 11.840741 | 12.5662 | 13.810046 | 12.473478 | 13.091683 | 13.759141 | 12.308034 | 13.179466 | 13.22915 | 15.753724 | 12.252324 | 11.618175 | 12.193818 | 11.761342 | 11.829685 | 11.327112 | 11.784401 | 11.535447 | 12.440083 | 12.387547 | 11.794814 |
0711.0825 | Arjun Berera | A. Berera (Edinburgh), D. Hochberg (CAB, Madrid) | Gauge symmetry and Slavnov-Taylor identities for randomly stirred fluids | 5 pages, no figures, In Press Physical Review Letters, 2007 | Phys.Rev.Lett.99:254501,2007 | 10.1103/PhysRevLett.99.254501 | null | hep-th cond-mat.stat-mech hep-lat hep-ph physics.flu-dyn | null | The path integral for randomly forced incompressible fluids is shown to have
an underlying Becchi-Rouet-Stora (BRS) symmetry as a consequence of Galilean
invariance. This symmetry must be respected to have a consistent generating
functional, free from both an overall infinite factor and spurious relations
amongst cor... | [
{
"created": "Tue, 6 Nov 2007 10:07:26 GMT",
"version": "v1"
}
] | 2009-02-10 | [
[
"Berera",
"A.",
"",
"Edinburgh"
],
[
"Hochberg",
"D.",
"",
"CAB, Madrid"
]
] | The path integral for randomly forced incompressible fluids is shown to have an underlying Becchi-Rouet-Stora (BRS) symmetry as a consequence of Galilean invariance. This symmetry must be respected to have a consistent generating functional, free from both an overall infinite factor and spurious relations amongst corre... | 8.689963 | 8.442872 | 9.320094 | 8.15512 | 8.683334 | 8.826756 | 8.192121 | 8.558084 | 9.019108 | 9.026589 | 8.384733 | 8.788913 | 8.428363 | 8.44264 | 8.531442 | 8.401293 | 8.528423 | 8.630211 | 8.598727 | 8.703026 | 8.254113 |
hep-th/0205124 | Jian-zu Zhang | Jian-zu Zhang | Testing Abelian dyon - fermion Bound System | 13 pages. Phys. Lett. B (in press) | Phys.Lett. B532 (2002) 215-221 | 10.1016/S0370-2693(02)01535-6 | null | hep-th quant-ph | null | Characteristics of Abelian dyon - fermion bound system, parity - violating
effects, a new series of energy spectra, effects related to the non - vanishing
electric dipole moment, feature of spin orientation etc, are analyzed and
compared with hydrogen - like atom. These analyses explore possibility of a new
approach ... | [
{
"created": "Tue, 14 May 2002 09:30:54 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Zhang",
"Jian-zu",
""
]
] | Characteristics of Abelian dyon - fermion bound system, parity - violating effects, a new series of energy spectra, effects related to the non - vanishing electric dipole moment, feature of spin orientation etc, are analyzed and compared with hydrogen - like atom. These analyses explore possibility of a new approach of... | 40.52536 | 43.886066 | 38.060658 | 33.954887 | 34.989357 | 37.466106 | 36.356293 | 37.288548 | 38.014648 | 35.603519 | 36.409069 | 32.760666 | 32.842583 | 33.343365 | 33.194752 | 32.043655 | 33.235344 | 31.743996 | 33.066631 | 33.012421 | 34.398968 |
2404.13107 | Viola Gattus | Viola Gattus and Apostolos Pilaftsis | Supergeometric Approach to Quantum Field Theory | 13 pages, Proceedings to Corfu Summer Institute 2023 (27 August - 1
October 2023, Corfu, Greece) | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review a recently proposed SuperGeometric (SG) approach to Quantum Field
Theories (QFTs) that allow for scalar-fermion field transformations in a
manifestly reparameterisation covariant manner. By adopting natural choices for
the field-space supermetric, we show how a non-trivial field-space Riemannian
curvature c... | [
{
"created": "Fri, 19 Apr 2024 15:53:51 GMT",
"version": "v1"
}
] | 2024-04-23 | [
[
"Gattus",
"Viola",
""
],
[
"Pilaftsis",
"Apostolos",
""
]
] | We review a recently proposed SuperGeometric (SG) approach to Quantum Field Theories (QFTs) that allow for scalar-fermion field transformations in a manifestly reparameterisation covariant manner. By adopting natural choices for the field-space supermetric, we show how a non-trivial field-space Riemannian curvature can... | 12.188058 | 9.602147 | 11.731734 | 10.472639 | 10.695119 | 9.927485 | 10.09403 | 10.40357 | 10.673107 | 12.787746 | 11.196863 | 11.657101 | 11.351484 | 11.505614 | 11.702641 | 11.381161 | 11.443387 | 11.662924 | 11.1851 | 11.85316 | 11.578703 |
0806.3513 | Tapobrata Sarkar | Tapobrata Sarkar, Gautam Sengupta, Bhupendra Nath Tiwari | Thermodynamic Geometry and Extremal Black Holes in String Theory | 1 + 33 pages, LaTeX, 4 eps figures | JHEP0810:076,2008 | 10.1088/1126-6708/2008/10/076 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a generalisation of thermodynamic geometry to degenerate quantum
ground states at zero temperatures exemplified by charged extremal black holes
in type II string theories. Several examples of extremal charged black holes
with non degenerate thermodynamic geometries and finite but non zero state
space scalar ... | [
{
"created": "Mon, 23 Jun 2008 08:34:34 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Sarkar",
"Tapobrata",
""
],
[
"Sengupta",
"Gautam",
""
],
[
"Tiwari",
"Bhupendra Nath",
""
]
] | We study a generalisation of thermodynamic geometry to degenerate quantum ground states at zero temperatures exemplified by charged extremal black holes in type II string theories. Several examples of extremal charged black holes with non degenerate thermodynamic geometries and finite but non zero state space scalar cu... | 15.577316 | 13.880478 | 16.13904 | 13.961636 | 14.304828 | 14.276885 | 14.335888 | 13.957062 | 13.879555 | 16.391754 | 13.497272 | 13.992167 | 15.375205 | 13.808771 | 14.48356 | 14.273996 | 14.35113 | 14.04165 | 14.083992 | 14.642919 | 13.873878 |
1706.07000 | Ariunzul Davgadorj | Ariunzul Davgadorj, Rikard von Unge | $\mathcal{N} = 2$ super Yang-Mills theory in Projective Superspace | null | Phys. Rev. D 97, 105017 (2018) | 10.1103/PhysRevD.97.105017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find a formulation of $\mathcal{N}=2$ supersymmetric Yang-Mills theory in
Projective superspace. In particular we find an expression for the field
strength in terms of an unconstrained prepotential which is desirable when
quantizing the theory. We use this to write the action in terms of the
prepotential and show ... | [
{
"created": "Wed, 21 Jun 2017 16:47:55 GMT",
"version": "v1"
},
{
"created": "Fri, 25 May 2018 17:24:45 GMT",
"version": "v2"
}
] | 2018-05-28 | [
[
"Davgadorj",
"Ariunzul",
""
],
[
"von Unge",
"Rikard",
""
]
] | We find a formulation of $\mathcal{N}=2$ supersymmetric Yang-Mills theory in Projective superspace. In particular we find an expression for the field strength in terms of an unconstrained prepotential which is desirable when quantizing the theory. We use this to write the action in terms of the prepotential and show th... | 6.48559 | 5.479024 | 6.076874 | 5.496016 | 5.619651 | 5.599471 | 5.946877 | 5.369668 | 5.692949 | 6.226854 | 5.040829 | 5.499415 | 5.866271 | 5.653424 | 5.778607 | 5.585967 | 5.594553 | 5.481424 | 5.713671 | 5.853641 | 5.319548 |
hep-th/0402009 | Yu Nakayama | Yu Nakayama | Liouville Field Theory -- A decade after the revolution | 264 pages, 31 figures, based on master's thesis defended 31/01/2004,
v2,3,4,5,6,7: references added, typos corrected, abridged version published
in IJMPA | Int.J.Mod.Phys.A19:2771-2930,2004 | 10.1142/S0217751X04019500 | UT-04-02 | hep-th | null | We review recent developments (up to January 2004) of the Liouville field
theory and its matrix model dual. This review consists of three parts. In part
I, we review the bosonic Liouville theory. After briefly reviewing the
necessary background, we discuss the bulk structure constants (the DOZZ
formula) and the bound... | [
{
"created": "Mon, 2 Feb 2004 03:05:04 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Feb 2004 13:08:22 GMT",
"version": "v2"
},
{
"created": "Fri, 13 Feb 2004 15:11:23 GMT",
"version": "v3"
},
{
"created": "Fri, 12 Mar 2004 06:26:12 GMT",
"version": "v4"
},
{
"cre... | 2011-05-05 | [
[
"Nakayama",
"Yu",
""
]
] | We review recent developments (up to January 2004) of the Liouville field theory and its matrix model dual. This review consists of three parts. In part I, we review the bosonic Liouville theory. After briefly reviewing the necessary background, we discuss the bulk structure constants (the DOZZ formula) and the boundar... | 5.227896 | 4.957021 | 6.547989 | 5.062618 | 5.59867 | 5.286264 | 5.152188 | 5.111228 | 5.037678 | 7.332239 | 5.303968 | 5.461106 | 5.938418 | 5.424335 | 5.310696 | 5.270703 | 5.32844 | 5.187456 | 5.239634 | 5.595138 | 5.242717 |
hep-th/0206236 | N. E. J. Bjerrum-Bohr | N. E. J. Bjerrum-Bohr | Leading quantum gravitational corrections to scalar QED | 14 pages, 33 figures, typos corrected | Phys.Rev. D66 (2002) 084023 | 10.1103/PhysRevD.66.084023 | null | hep-th gr-qc | null | We consider the leading post-Newtonian and quantum corrections to the
non-relativistic scattering amplitude of charged scalars in the combined theory
of general relativity and scalar QED. The combined theory is treated as an
effective field theory. This allows for a consistent quantization of the
gravitational field.... | [
{
"created": "Wed, 26 Jun 2002 12:39:44 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Oct 2002 21:04:57 GMT",
"version": "v2"
},
{
"created": "Mon, 3 Sep 2007 16:55:46 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Bjerrum-Bohr",
"N. E. J.",
""
]
] | We consider the leading post-Newtonian and quantum corrections to the non-relativistic scattering amplitude of charged scalars in the combined theory of general relativity and scalar QED. The combined theory is treated as an effective field theory. This allows for a consistent quantization of the gravitational field. T... | 6.171274 | 7.649841 | 5.525362 | 6.105816 | 5.170001 | 5.435559 | 6.995002 | 5.253115 | 7.254954 | 5.757743 | 6.41485 | 6.788713 | 6.230708 | 6.154275 | 6.238786 | 6.119257 | 6.648371 | 6.216794 | 6.474688 | 6.209696 | 6.521814 |
0905.4373 | Jorge Rocha | Jorge V. Rocha | Evaporation of large black holes in AdS: greybody factor and decay rate | 20 pages, 2 figures; v2: added references, published version | null | 10.1088/1126-6708/2009/08/027 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a massless, minimally coupled scalar field propagating through
the geometry of a black 3-brane in an asymptotically $AdS_5 \times S^5$ space.
The wave equation for modes traveling purely in the holographic direction
reduces to a Heun equation and the corresponding greybody factor is obtained
numerically. ... | [
{
"created": "Wed, 27 May 2009 10:43:47 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Sep 2009 11:50:39 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"Rocha",
"Jorge V.",
""
]
] | We consider a massless, minimally coupled scalar field propagating through the geometry of a black 3-brane in an asymptotically $AdS_5 \times S^5$ space. The wave equation for modes traveling purely in the holographic direction reduces to a Heun equation and the corresponding greybody factor is obtained numerically. Ap... | 8.231008 | 8.36998 | 9.083933 | 8.364882 | 8.461864 | 8.155192 | 9.240479 | 7.574802 | 8.362576 | 8.506891 | 8.31327 | 7.793447 | 8.182216 | 7.872744 | 7.916823 | 7.784585 | 7.835827 | 7.868806 | 7.958494 | 8.171015 | 7.870203 |
2007.07190 | Ian Jack | I. Jack and D.R.T. Jones | Anomalous dimensions for $\phi^n$ in scale invariant $d=3$ theory | 25 pages, 8 figures, 4 tables. Uses tikz. Additional references and
acknowledgements added. Minor corrections and additions made | Phys. Rev. D 102, 085012 (2020) | 10.1103/PhysRevD.102.085012 | LTH1239 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently it was shown that the scaling dimension of the operator $\phi^n$ in
scale-invariant $d=3$ theory may be computed semiclassically, and this was
verified to leading order (two loops) in perturbation theory at leading and
subleading $n$. Here we extend this verification to six loops, once again at
leading and s... | [
{
"created": "Tue, 14 Jul 2020 17:08:45 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jul 2020 10:57:12 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Sep 2020 07:46:01 GMT",
"version": "v3"
}
] | 2020-10-28 | [
[
"Jack",
"I.",
""
],
[
"Jones",
"D. R. T.",
""
]
] | Recently it was shown that the scaling dimension of the operator $\phi^n$ in scale-invariant $d=3$ theory may be computed semiclassically, and this was verified to leading order (two loops) in perturbation theory at leading and subleading $n$. Here we extend this verification to six loops, once again at leading and sub... | 9.9446 | 7.976433 | 9.705275 | 8.814739 | 8.210605 | 8.543113 | 8.458756 | 8.971716 | 8.730588 | 10.297966 | 8.453259 | 8.94289 | 9.409549 | 9.033849 | 8.769108 | 8.97457 | 8.797026 | 8.901548 | 8.861677 | 9.601854 | 8.682233 |
1801.06098 | Ricardo Renan Landim | G. Alencar, I. C. Jardim and R. R. Landim | $p-$forms non-minimally coupled to gravity in Randall-Sundrum scenarios | 28 pages, 13 figures. Accepted for publication in epjc | null | 10.1140/epjc/s10052-018-5829-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study the coupling of $p$-form fields with geometrical
tensor fields, namely Ricci, Einstein, Horndeski and Riemann in Randall-Sundrum
scenarios with co-dimension one. We consider delta-like and branes generated by
a kink and a domain wall. We begin by a detailed study of the Kalb-Ramond (KR)
field. ... | [
{
"created": "Wed, 17 Jan 2018 18:54:00 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Jan 2018 18:30:45 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Jan 2018 17:16:20 GMT",
"version": "v3"
},
{
"created": "Mon, 23 Apr 2018 17:02:09 GMT",
"version": "v4"
}
] | 2018-06-13 | [
[
"Alencar",
"G.",
""
],
[
"Jardim",
"I. C.",
""
],
[
"Landim",
"R. R.",
""
]
] | In this paper we study the coupling of $p$-form fields with geometrical tensor fields, namely Ricci, Einstein, Horndeski and Riemann in Randall-Sundrum scenarios with co-dimension one. We consider delta-like and branes generated by a kink and a domain wall. We begin by a detailed study of the Kalb-Ramond (KR) field. Th... | 15.698412 | 15.260825 | 15.258326 | 14.13986 | 15.499829 | 15.047512 | 15.417747 | 14.897971 | 14.002172 | 16.931185 | 15.065037 | 14.936321 | 14.752642 | 14.698043 | 14.644501 | 14.678954 | 14.858667 | 14.639439 | 14.531199 | 15.076136 | 14.846093 |
1404.4733 | Emil Nissimov | Eduardo Guendelman, Emil Nissimov, Svetlana Pacheva, Mahary Vasihoun | A New Mechanism of Dynamical Spontaneous Breaking of Supersymmetry | v2 7 pages, few minor improvements for clarity, reformatted to
conform the journal style, to appear in Bulgarian Journal of Physics, vol.41,
#4 | Bulg. J. Phys. 41 (2014) 123-129 | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a qualitatively new mechanism for dynamical spontaneous breakdown
of supersymmetry. Specifically, we construct a modified formulation of standard
minimal N=1 supergravity. The modification is based on an idea worked out in
detail in previous publications by some of us, where we proposed a new
formulation o... | [
{
"created": "Fri, 18 Apr 2014 09:56:50 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Aug 2014 07:53:18 GMT",
"version": "v2"
}
] | 2014-11-03 | [
[
"Guendelman",
"Eduardo",
""
],
[
"Nissimov",
"Emil",
""
],
[
"Pacheva",
"Svetlana",
""
],
[
"Vasihoun",
"Mahary",
""
]
] | We present a qualitatively new mechanism for dynamical spontaneous breakdown of supersymmetry. Specifically, we construct a modified formulation of standard minimal N=1 supergravity. The modification is based on an idea worked out in detail in previous publications by some of us, where we proposed a new formulation of ... | 9.988574 | 9.221109 | 10.135662 | 9.418774 | 9.286185 | 9.76629 | 9.465384 | 9.296874 | 9.693685 | 10.954598 | 9.79447 | 10.207734 | 10.058181 | 9.827254 | 10.18311 | 9.895473 | 9.89051 | 10.217645 | 9.851715 | 10.113635 | 9.997423 |
2206.10794 | Dionisio Bazeia | D. Bazeia, A.S. Lob\~ao Jr | Mechanism to control the internal structure of thick brane | 8 pages, 10 figures. To appear in EPJC as a Letter | Eur. Phys. J. C 82 (2022) 579 | 10.1140/epjc/s10052-022-10546-z | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study braneworlds generated by several scalar fields. The
investigation describes the necessary formalism to examine models and evaluate
the conditions for the stability of the gravitational sector under linear
perturbations. In particular, we develop a mechanism that help us investigate
distinct situ... | [
{
"created": "Wed, 22 Jun 2022 01:25:16 GMT",
"version": "v1"
}
] | 2022-07-07 | [
[
"Bazeia",
"D.",
""
],
[
"Lobão",
"A. S.",
"Jr"
]
] | In this work we study braneworlds generated by several scalar fields. The investigation describes the necessary formalism to examine models and evaluate the conditions for the stability of the gravitational sector under linear perturbations. In particular, we develop a mechanism that help us investigate distinct situat... | 21.066708 | 15.468719 | 18.873106 | 16.817305 | 17.322788 | 16.007376 | 14.89595 | 15.964388 | 15.929501 | 19.061075 | 16.741245 | 18.02828 | 19.211054 | 18.325216 | 18.571222 | 18.289791 | 17.997906 | 17.560022 | 18.361795 | 19.433811 | 18.947697 |
hep-th/0304101 | Jerzy Kowalski-Glikman | Jerzy Kowalski-Glikman and Sebastian Nowak | Doubly Special Relativity and de Sitter space | 26 pages, one formula (67) corrected; some remarks added | Class.Quant.Grav.20:4799-4816,2003 | 10.1088/0264-9381/20/22/006 | null | hep-th | null | In this paper we recall the construction of Doubly Special Relativity (DSR)
as a theory with energy-momentum space being the four dimensional de Sitter
space. Then the bases of the DSR theory can be understood as different
coordinate systems on this space. We investigate the emerging geometrical
picture of Doubly Spe... | [
{
"created": "Thu, 10 Apr 2003 16:15:19 GMT",
"version": "v1"
},
{
"created": "Sat, 3 May 2003 09:38:12 GMT",
"version": "v2"
},
{
"created": "Sat, 11 Oct 2003 22:48:24 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Kowalski-Glikman",
"Jerzy",
""
],
[
"Nowak",
"Sebastian",
""
]
] | In this paper we recall the construction of Doubly Special Relativity (DSR) as a theory with energy-momentum space being the four dimensional de Sitter space. Then the bases of the DSR theory can be understood as different coordinate systems on this space. We investigate the emerging geometrical picture of Doubly Speci... | 9.326009 | 8.269327 | 8.779053 | 8.254169 | 8.740609 | 8.281688 | 8.539011 | 8.28616 | 8.363883 | 9.872673 | 8.077512 | 8.210986 | 8.705542 | 8.427397 | 8.390656 | 8.478944 | 8.263799 | 8.485968 | 8.380539 | 8.570834 | 8.326208 |
0710.2182 | Michael Wohlgenannt | Josip Trampetic, Michael Wohlgenannt | Remarks on the 2nd order Seiberg-Witten maps | 4 pages; to be published in Phys. Rev. D | Phys.Rev.D76:127703,2007 | 10.1103/PhysRevD.76.127703 | Preprint ESI 1964 (2007) | hep-th hep-ph | null | In this report, we discuss the Seiberg-Witten maps up to the second order in
the noncommutative parameter $\theta$. They add to the recently published
solutions in [1]. Expressions for the vector, fermion and Higgs fields are
given explicitly.
| [
{
"created": "Thu, 11 Oct 2007 15:34:07 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Dec 2007 14:25:33 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Trampetic",
"Josip",
""
],
[
"Wohlgenannt",
"Michael",
""
]
] | In this report, we discuss the Seiberg-Witten maps up to the second order in the noncommutative parameter $\theta$. They add to the recently published solutions in [1]. Expressions for the vector, fermion and Higgs fields are given explicitly. | 12.496678 | 9.079206 | 8.960011 | 7.872558 | 9.344114 | 8.255943 | 8.349548 | 8.701402 | 7.59196 | 9.490929 | 8.138389 | 8.266743 | 8.632571 | 8.394623 | 8.123898 | 8.494949 | 8.227216 | 8.209199 | 8.812928 | 8.696121 | 8.586023 |
hep-th/0511103 | Mariano Cadoni | Mariano Cadoni | Statistical entropy of the Schwarzschild black hole | 3 pages no figures | Mod.Phys.Lett. A21 (2006) 1879-1888 | 10.1142/S0217732306021165 | null | hep-th | null | We derive the statistical entropy of the Schwarzschild black hole by
considering the asymptotic symmetry algebra near the $\cal{I^{-}}$ boundary of
the spacetime at past null infinity. Using a two-dimensional description and
the Weyl invariance of black hole thermodynamics this symmetry algebra can be
mapped into the... | [
{
"created": "Wed, 9 Nov 2005 08:34:10 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Cadoni",
"Mariano",
""
]
] | We derive the statistical entropy of the Schwarzschild black hole by considering the asymptotic symmetry algebra near the $\cal{I^{-}}$ boundary of the spacetime at past null infinity. Using a two-dimensional description and the Weyl invariance of black hole thermodynamics this symmetry algebra can be mapped into the V... | 7.462492 | 7.407097 | 6.971978 | 6.592581 | 6.702356 | 6.647545 | 6.910534 | 6.634129 | 6.490889 | 8.233022 | 6.711213 | 6.947561 | 7.021194 | 6.747062 | 6.84078 | 6.981046 | 6.984733 | 7.087055 | 6.847619 | 6.767648 | 6.919154 |
hep-th/0103055 | Andreas Fring | O.A. Castro-Alvaredo and A. Fring | Scaling functions from q-deformed Virasoro characters | 31 pages of Latex, 5 figures | J.Phys.A35:609-636,2002 | 10.1088/0305-4470/35/3/310 | null | hep-th cond-mat math-ph math.MP | null | We propose a renormalization group scaling function which is constructed from
q-deformed fermionic versions of Virasoro characters. By comparison with
alternative methods, which take their starting point in the massive theories,
we demonstrate that these new functions contain qualitatively the same
information. We sh... | [
{
"created": "Thu, 8 Mar 2001 16:54:36 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Castro-Alvaredo",
"O. A.",
""
],
[
"Fring",
"A.",
""
]
] | We propose a renormalization group scaling function which is constructed from q-deformed fermionic versions of Virasoro characters. By comparison with alternative methods, which take their starting point in the massive theories, we demonstrate that these new functions contain qualitatively the same information. We show... | 13.724976 | 12.772831 | 14.472899 | 13.658685 | 13.401597 | 13.843718 | 13.281977 | 12.729826 | 13.333569 | 14.416551 | 12.75908 | 13.274248 | 14.152593 | 12.941648 | 13.270961 | 13.046897 | 13.001019 | 13.144329 | 13.195809 | 13.1617 | 12.813496 |
1602.06290 | Martin Einhorn | Martin B Einhorn and D R Timothy Jones | Induced Gravity II: Grand Unification | 44 pages, 5 figures, 2 tables. v2 has new discussion concerning
stability of SSB plus related appendix. Additional references added. v3 is
version to be published; contains minor revisions | JHEP 05 (2016) 185 | 10.1007/JHEP05(2016)185 | NSF-KITP-16-014, MCTP-16-04, LTH 1074 | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by-nc-sa/4.0/ | As an illustration of a renormalizable, asymptotically-free model of induced
gravity, we consider an $SO(10)$ gauge theory interacting with a real scalar
multiplet in the adjoint representation. We show that dimensional transmutation
can occur, spontaneously breaking $SO(10)$ to $SU(5){\otimes}U(1),$ while
inducing t... | [
{
"created": "Fri, 19 Feb 2016 20:49:15 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Mar 2016 00:46:30 GMT",
"version": "v2"
},
{
"created": "Tue, 3 May 2016 05:44:53 GMT",
"version": "v3"
}
] | 2016-06-08 | [
[
"Einhorn",
"Martin B",
""
],
[
"Jones",
"D R Timothy",
""
]
] | As an illustration of a renormalizable, asymptotically-free model of induced gravity, we consider an $SO(10)$ gauge theory interacting with a real scalar multiplet in the adjoint representation. We show that dimensional transmutation can occur, spontaneously breaking $SO(10)$ to $SU(5){\otimes}U(1),$ while inducing the... | 9.565508 | 10.180765 | 9.95294 | 9.784314 | 10.280752 | 9.857152 | 10.534783 | 9.954432 | 9.123968 | 10.392602 | 9.550376 | 9.287438 | 9.353024 | 9.24848 | 9.437602 | 9.459676 | 9.429601 | 9.17128 | 9.198017 | 9.262514 | 9.359695 |
1411.5321 | Carlos A. Hernaski | Carlos Hernaski | Quantization and stability of bumblebee electrodynamics | Improved exposition; typos corrected; to be published in Phys. Rev.
D; 34 pages | null | 10.1103/PhysRevD.90.124036 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The quantization of a vector model presenting spontaneous breaking of Lorentz
symmetry in flat Minkowski spacetime is discussed. The Stueckelberg trick of
introducing an auxiliary field along with a local symmetry in the initial
Lagrangian is used to convert the second-class constraints present in the
initial Lagrang... | [
{
"created": "Mon, 20 Oct 2014 19:54:07 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Nov 2014 21:22:27 GMT",
"version": "v2"
}
] | 2015-06-23 | [
[
"Hernaski",
"Carlos",
""
]
] | The quantization of a vector model presenting spontaneous breaking of Lorentz symmetry in flat Minkowski spacetime is discussed. The Stueckelberg trick of introducing an auxiliary field along with a local symmetry in the initial Lagrangian is used to convert the second-class constraints present in the initial Lagrangia... | 8.056846 | 7.443775 | 8.262971 | 7.365767 | 7.529303 | 7.462739 | 7.937394 | 7.282519 | 7.695644 | 7.850205 | 7.540345 | 7.876784 | 7.582134 | 7.531398 | 7.620911 | 7.782204 | 7.700636 | 7.70311 | 7.70734 | 7.75901 | 7.663127 |
hep-th/9207056 | Lnc | Lay Nam Chang, Chopin Soo | Einstein manifolds in Ashtekar variables: explicit examples | 32 pages, uses harvmac, VPI-IHEP-92-5 | null | null | null | hep-th gr-qc | null | We show that all solutions to the vacuum Einstein field equations may be
mapped to instanton configurations of the Ashtekar variables. These solutions
are characterized by properties of the moduli space of the instantons. We
exhibit explicit forms of these configurations for several well-known
solutions, and indicate... | [
{
"created": "Thu, 16 Jul 1992 03:35:26 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Jul 1992 07:22:25 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Chang",
"Lay Nam",
""
],
[
"Soo",
"Chopin",
""
]
] | We show that all solutions to the vacuum Einstein field equations may be mapped to instanton configurations of the Ashtekar variables. These solutions are characterized by properties of the moduli space of the instantons. We exhibit explicit forms of these configurations for several well-known solutions, and indicate a... | 12.641581 | 10.404954 | 10.169899 | 9.609782 | 10.295117 | 10.157446 | 9.914576 | 10.4239 | 10.45926 | 10.342029 | 10.349907 | 10.495128 | 10.634636 | 10.416538 | 10.537555 | 10.30431 | 10.305471 | 10.566751 | 10.337417 | 10.793305 | 10.104094 |
1508.01207 | David Tong | David Tong and Carl Turner | Vortices and Monopoles in a Harmonic Trap | 24 pages + appendices. 5 figures. v2: references added | null | 10.1007/JHEP12(2015)098 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Omega-deformation is a harmonic trap, penning certain excitations near
the origin in a manner consistent with supersymmetry. Here we explore the
dynamics of BPS monopoles and vortices in such a trap. We pay particular
attention to monopoles in the Higgs phase, when they are confined to a vortex
string. Unusually ... | [
{
"created": "Wed, 5 Aug 2015 20:10:24 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Sep 2015 07:30:50 GMT",
"version": "v2"
}
] | 2016-01-27 | [
[
"Tong",
"David",
""
],
[
"Turner",
"Carl",
""
]
] | The Omega-deformation is a harmonic trap, penning certain excitations near the origin in a manner consistent with supersymmetry. Here we explore the dynamics of BPS monopoles and vortices in such a trap. We pay particular attention to monopoles in the Higgs phase, when they are confined to a vortex string. Unusually fo... | 11.255987 | 10.982807 | 11.979416 | 10.354917 | 10.203936 | 10.138391 | 10.833421 | 10.056589 | 10.010466 | 13.61556 | 9.464666 | 9.930375 | 11.425768 | 10.558278 | 10.078434 | 10.290667 | 10.399924 | 9.956586 | 10.523055 | 10.739442 | 10.185742 |
1504.08244 | Napat Poovuttikul | Andrei Parnachev, Napat Poovuttikul | Topological Entanglement Entropy, Ground State Degeneracy and Holography | harvmac, 27 pages, 6 figures, v3: section 4 re-written, references
added, accepted to JHEP | null | null | TCDMATH-15-13 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Topological entanglement entropy, a measure of the long-ranged entanglement,
is related to the degeneracy of the ground state on a higher genus surface. The
exact relation depends on the details of the topological theory. We consider a
class of holographic models where such relation might be similar to the one
exhibi... | [
{
"created": "Thu, 30 Apr 2015 14:38:06 GMT",
"version": "v1"
},
{
"created": "Fri, 22 May 2015 14:10:59 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Sep 2015 13:02:16 GMT",
"version": "v3"
}
] | 2015-12-21 | [
[
"Parnachev",
"Andrei",
""
],
[
"Poovuttikul",
"Napat",
""
]
] | Topological entanglement entropy, a measure of the long-ranged entanglement, is related to the degeneracy of the ground state on a higher genus surface. The exact relation depends on the details of the topological theory. We consider a class of holographic models where such relation might be similar to the one exhibite... | 6.732632 | 7.500761 | 7.272588 | 6.959527 | 7.749672 | 8.184542 | 7.523898 | 7.183849 | 7.520647 | 7.157101 | 7.064492 | 7.081519 | 6.916308 | 7.104654 | 6.971035 | 6.820285 | 6.925684 | 7.253608 | 6.999809 | 6.726504 | 7.126667 |
1301.0721 | Shotaro Shiba | Hiroaki Kanno, Kazunobu Maruyoshi, Shotaro Shiba, Masato Taki | W_3 irregular states and isolated N=2 superconformal field theories | 1+53 pages, 1 figure; v2: minor corrections | null | 10.1007/JHEP03(2013)147 | KEK-TH-1595, RIKEN-MP-66 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the proposal that the six-dimensional (2,0) theory on the Riemann
surface with irregular punctures leads to a four-dimensional gauge theory
coupled to the isolated N=2 superconformal theories of Argyres-Douglas type,
and to two-dimensional conformal field theory with irregular states. Following
the approac... | [
{
"created": "Fri, 4 Jan 2013 13:42:09 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Feb 2013 15:46:32 GMT",
"version": "v2"
}
] | 2015-06-12 | [
[
"Kanno",
"Hiroaki",
""
],
[
"Maruyoshi",
"Kazunobu",
""
],
[
"Shiba",
"Shotaro",
""
],
[
"Taki",
"Masato",
""
]
] | We explore the proposal that the six-dimensional (2,0) theory on the Riemann surface with irregular punctures leads to a four-dimensional gauge theory coupled to the isolated N=2 superconformal theories of Argyres-Douglas type, and to two-dimensional conformal field theory with irregular states. Following the approach ... | 7.451128 | 7.329873 | 8.633698 | 7.441138 | 7.189295 | 7.238671 | 7.583405 | 6.730252 | 7.6002 | 10.963376 | 6.834932 | 6.801105 | 7.89958 | 6.802872 | 7.043525 | 7.105314 | 7.249969 | 7.014734 | 6.970202 | 7.676517 | 6.784323 |
1604.08871 | Dionisio Bazeia | D. Bazeia, L. Losano, M.A. Marques, R. Menezes, R. da Rocha | Compact Q-balls | 6 pages, 6 figures; to appear in PLB | Phys. Lett. B 758 (2016) 146 | 10.1016/j.physletb.2016.04.060 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we deal with non-topological solutions of the Q-ball type in two
space-time dimensions, in models described by a single complex scalar field
that engenders global symmetry. The main novelty is the presence of stable
Q-balls solutions that live in a compact interval of the real line and appear
from a fami... | [
{
"created": "Fri, 29 Apr 2016 15:21:37 GMT",
"version": "v1"
},
{
"created": "Tue, 3 May 2016 15:05:25 GMT",
"version": "v2"
}
] | 2016-05-24 | [
[
"Bazeia",
"D.",
""
],
[
"Losano",
"L.",
""
],
[
"Marques",
"M. A.",
""
],
[
"Menezes",
"R.",
""
],
[
"da Rocha",
"R.",
""
]
] | In this work we deal with non-topological solutions of the Q-ball type in two space-time dimensions, in models described by a single complex scalar field that engenders global symmetry. The main novelty is the presence of stable Q-balls solutions that live in a compact interval of the real line and appear from a family... | 12.267477 | 7.038328 | 11.488297 | 9.710568 | 9.496583 | 9.016001 | 8.465479 | 8.823665 | 8.733465 | 13.003893 | 9.769268 | 10.053978 | 11.931947 | 10.751101 | 10.472867 | 10.503474 | 10.346933 | 10.258078 | 10.330714 | 11.880198 | 10.949692 |
1007.0556 | Feodor A. Smirnov | M. Jimbo, T. Miwa, F. Smirnov | Hidden Grassmann structure in the XXZ model V: sine-Gordon model | 36 pages. Some corrections are done in latest version, especially in
the subsection 10.3 | Lett.Math.Phys.96:325-365,2011 | 10.1007/s11005-010-0438-9 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study one-point functions of the sine-Gordon model on a cylinder. Our
approach is based on a fermionic description of the space of descendent fields,
developed in our previous works for conformal field theory and the sine-Gordon
model on the plane. In the present paper we make an essential addition by
giving a con... | [
{
"created": "Sun, 4 Jul 2010 14:59:26 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Mar 2011 12:30:30 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Apr 2013 07:44:16 GMT",
"version": "v3"
}
] | 2013-04-25 | [
[
"Jimbo",
"M.",
""
],
[
"Miwa",
"T.",
""
],
[
"Smirnov",
"F.",
""
]
] | We study one-point functions of the sine-Gordon model on a cylinder. Our approach is based on a fermionic description of the space of descendent fields, developed in our previous works for conformal field theory and the sine-Gordon model on the plane. In the present paper we make an essential addition by giving a conne... | 10.026225 | 9.243203 | 12.341742 | 9.29923 | 9.355981 | 9.794393 | 9.805439 | 9.237556 | 8.916701 | 11.07198 | 9.445967 | 9.104008 | 10.724496 | 9.273202 | 9.643769 | 9.68248 | 9.699425 | 9.248788 | 9.450607 | 10.260448 | 9.244619 |
1309.0278 | Shlomo S. Razamat | Shlomo S. Razamat | On the N=2 superconformal index and eigenfunctions of the elliptic RS
model | 21 pages, harvmac. v2: added references | null | 10.1007/s11005-014-0682-5 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define an infinite sequence of superconformal indices, I_n, generalizing
the Schur index for N=2 theories. For theories of class S we then suggest a
recursive technique to completely determine I_n. The information encoded in the
sequence of indices is equivalent to the N=2 superconformal index depending on
the max... | [
{
"created": "Mon, 2 Sep 2013 00:09:10 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Sep 2013 18:27:33 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Razamat",
"Shlomo S.",
""
]
] | We define an infinite sequence of superconformal indices, I_n, generalizing the Schur index for N=2 theories. For theories of class S we then suggest a recursive technique to completely determine I_n. The information encoded in the sequence of indices is equivalent to the N=2 superconformal index depending on the maxim... | 9.224314 | 8.244609 | 11.214887 | 7.367433 | 8.497696 | 7.455192 | 7.570381 | 7.601112 | 7.493532 | 11.114736 | 8.122175 | 8.27402 | 9.294003 | 8.321279 | 8.023808 | 8.755583 | 8.094035 | 8.573542 | 8.406043 | 9.281368 | 7.921498 |
hep-th/9205112 | Arley | Arlen Anderson | The Global Problem of Time | 8 pp., McGill 92-15 | null | null | null | hep-th | null | Time does not obviously appear amongst the coordinates on the constrained
phase space of general relativity in the Hamiltonian formulation. Recent work
in finite-dimensional models claims that topological obstructions generically
make the global definition of time impossible. It is shown here that a time
coordinate c... | [
{
"created": "Fri, 29 May 1992 18:04:42 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Anderson",
"Arlen",
""
]
] | Time does not obviously appear amongst the coordinates on the constrained phase space of general relativity in the Hamiltonian formulation. Recent work in finite-dimensional models claims that topological obstructions generically make the global definition of time impossible. It is shown here that a time coordinate can... | 13.094879 | 11.536002 | 11.323013 | 10.582621 | 10.926352 | 11.574828 | 12.012856 | 11.62186 | 10.643552 | 11.911777 | 10.451129 | 10.056862 | 10.540798 | 9.943649 | 10.105014 | 9.827634 | 10.196893 | 9.807116 | 10.072046 | 9.968011 | 10.108038 |
hep-th/9204002 | null | T. T. Burwick and A. H. Chamseddine | Classical and Quantum Considerations of Two-dimensional Gravity | 18 pages | Nucl.Phys. B384 (1992) 411-430 | 10.1016/0550-3213(92)90473-O | null | hep-th | null | The two-dimensional theory of gravity describing a graviton-dilaton system is
considered. The graviton-dilaton coupling can be fixed such that the quantum
theory remains free of the conformal anomaly for any conformal dimension of the
coupled matter system, even if the dilaton does not appear as Lagrange
multiplier. ... | [
{
"created": "Thu, 2 Apr 1992 15:02:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Burwick",
"T. T.",
""
],
[
"Chamseddine",
"A. H.",
""
]
] | The two-dimensional theory of gravity describing a graviton-dilaton system is considered. The graviton-dilaton coupling can be fixed such that the quantum theory remains free of the conformal anomaly for any conformal dimension of the coupled matter system, even if the dilaton does not appear as Lagrange multiplier. In... | 11.787975 | 10.526428 | 10.693475 | 10.386519 | 11.296622 | 10.848851 | 10.245443 | 10.212946 | 9.897714 | 13.474138 | 10.077725 | 11.234355 | 10.687525 | 10.428329 | 11.335738 | 10.923684 | 10.642651 | 10.466808 | 10.668173 | 11.364202 | 10.917909 |
hep-th/9201080 | null | P. Furlan, A. Ch. Ganchev, R. Paunov, V. B. Petkova | Solutions of the Knizhnik - Zamolodchikov Equation with Rational
Isospins and the Reduction to the Minimal Models | 40 pages | Nucl.Phys. B394 (1993) 665-706 | 10.1016/0550-3213(93)90227-G | null | hep-th | null | In the spirit of the quantum Hamiltonian reduction we establish a relation
between the chiral $n$-point functions, as well as the equations governing
them, of the $A_1^{(1)}$ WZNW conformal theory and the corresponding Virasoro
minimal models. The WZNW correlators are described as solutions of the Knizhnik
- Zamolodc... | [
{
"created": "Fri, 31 Jan 1992 17:23:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Furlan",
"P.",
""
],
[
"Ganchev",
"A. Ch.",
""
],
[
"Paunov",
"R.",
""
],
[
"Petkova",
"V. B.",
""
]
] | In the spirit of the quantum Hamiltonian reduction we establish a relation between the chiral $n$-point functions, as well as the equations governing them, of the $A_1^{(1)}$ WZNW conformal theory and the corresponding Virasoro minimal models. The WZNW correlators are described as solutions of the Knizhnik - Zamolodchi... | 8.589929 | 9.178783 | 9.750692 | 8.538374 | 8.375508 | 9.451923 | 9.225125 | 9.500152 | 8.892558 | 11.005413 | 8.572402 | 8.104713 | 8.588521 | 8.044461 | 8.324578 | 8.108092 | 7.971964 | 8.082184 | 7.939662 | 9.011834 | 7.906711 |
hep-th/0506158 | Andrei Mironov | A.Mironov | Matrix Models vs. Matrix Integrals | 10 pages, contribution to the International Workshop "Classical and
Quantum Integrable Systems", Dubna, Russia, 2005 | Theor.Math.Phys.146:63-72,2006; Teor.Mat.Fiz.146:77-89,2006 | 10.1007/s11232-006-0007-7 | null | hep-th | null | In a brief review, we discuss interrelations between arbitrary solutions of
the loop equations that describe Hermitean one-matrix model and particular
(multi-cut) solutions that describe concrete matrix integrals. These latter
ones enjoy a series of specific properties and, in particular, are described in
terms of Se... | [
{
"created": "Mon, 20 Jun 2005 19:43:25 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Mironov",
"A.",
""
]
] | In a brief review, we discuss interrelations between arbitrary solutions of the loop equations that describe Hermitean one-matrix model and particular (multi-cut) solutions that describe concrete matrix integrals. These latter ones enjoy a series of specific properties and, in particular, are described in terms of Seib... | 16.3428 | 13.413748 | 18.140245 | 13.217029 | 14.25973 | 14.324552 | 14.581771 | 13.604118 | 14.02684 | 18.159086 | 12.956133 | 13.140504 | 15.797866 | 14.540365 | 14.424342 | 14.235704 | 14.267321 | 13.637791 | 14.215774 | 16.08457 | 13.607768 |
hep-th/0304265 | Ramond | P. Ramond | Dirac's Footsteps and Supersymmetry | Invited Talk at Dirac's Centennial Symposium, Tallahasse, Florida,
Dec 2002 | Int.J.Mod.Phys. A19S1 (2004) 89-98 | 10.1142/S0217751X04018610 | UFIFT-HET-03-07 | hep-th | null | One hundred years after its creator's birth, the Dirac equation stands as the
cornerstone of XXth Century physics. But it is much more, as it carries the
seeds of supersymmetry. Dirac also invented the light-cone, or "front form"
dynamics, which plays a crucial role in string theory and in elucidating the
finiteness ... | [
{
"created": "Wed, 30 Apr 2003 14:54:54 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Ramond",
"P.",
""
]
] | One hundred years after its creator's birth, the Dirac equation stands as the cornerstone of XXth Century physics. But it is much more, as it carries the seeds of supersymmetry. Dirac also invented the light-cone, or "front form" dynamics, which plays a crucial role in string theory and in elucidating the finiteness of... | 12.075813 | 11.21093 | 13.946617 | 11.067063 | 12.259369 | 12.830355 | 12.416743 | 11.756421 | 11.513501 | 13.296144 | 11.22681 | 11.501841 | 11.443682 | 10.921272 | 10.764728 | 11.268483 | 11.213446 | 11.358858 | 10.883626 | 11.279412 | 11.219748 |
1509.02930 | Olaf Hohm | Olaf Hohm and Barton Zwiebach | Double Metric, Generalized Metric and $\alpha'$-Geometry | 20 pages | Phys. Rev. D 93, 064035 (2016) | 10.1103/PhysRevD.93.064035 | MIT-CTP-4714 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We relate the unconstrained `double metric' of the `$\alpha'$-geometry'
formulation of double field theory to the constrained generalized metric
encoding the spacetime metric and b-field. This is achieved by integrating out
auxiliary field components of the double metric in an iterative procedure that
induces an infi... | [
{
"created": "Wed, 9 Sep 2015 20:16:04 GMT",
"version": "v1"
}
] | 2016-03-23 | [
[
"Hohm",
"Olaf",
""
],
[
"Zwiebach",
"Barton",
""
]
] | We relate the unconstrained `double metric' of the `$\alpha'$-geometry' formulation of double field theory to the constrained generalized metric encoding the spacetime metric and b-field. This is achieved by integrating out auxiliary field components of the double metric in an iterative procedure that induces an infini... | 10.292448 | 8.737213 | 11.289983 | 8.861057 | 9.549816 | 10.416699 | 9.535487 | 8.90348 | 9.107792 | 11.308352 | 8.909323 | 9.518618 | 9.766553 | 9.294398 | 9.369689 | 9.769958 | 9.760354 | 9.294524 | 8.970931 | 10.469127 | 9.476824 |
1702.02954 | Peter Lowdon | Peter Lowdon | The non-perturbative structure of the photon and gluon propagators | 17 pages; v2: additional comments added, matches published version | Phys. Rev. D 96, 065013 (2017) | 10.1103/PhysRevD.96.065013 | SLAC-PUB-16924 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The non-perturbative structure of the photon and gluon propagators plays an
important role in governing the dynamics of quantum electrodynamics (QED) and
quantum chromodynamics (QCD) respectively. Although it is often assumed that
these interacting field propagators can be decomposed into longitudinal and
transverse ... | [
{
"created": "Thu, 9 Feb 2017 19:10:06 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Sep 2017 18:53:00 GMT",
"version": "v2"
}
] | 2017-09-21 | [
[
"Lowdon",
"Peter",
""
]
] | The non-perturbative structure of the photon and gluon propagators plays an important role in governing the dynamics of quantum electrodynamics (QED) and quantum chromodynamics (QCD) respectively. Although it is often assumed that these interacting field propagators can be decomposed into longitudinal and transverse co... | 6.181313 | 5.942234 | 5.75224 | 5.507606 | 5.977081 | 5.938176 | 6.273787 | 5.966219 | 5.973775 | 6.01953 | 5.953337 | 6.077323 | 5.72061 | 5.616338 | 5.816452 | 5.823845 | 5.671901 | 5.820221 | 5.630609 | 5.622802 | 5.757928 |
1512.02886 | Gabriel Menezes | G. Menezes, N. F. Svaiter | Radiative processes of uniformly accelerated entangled atoms | Accepted for publication in Physical Review A. arXiv admin note: text
overlap with arXiv:gr-qc/9408019 by other authors | Phys. Rev. A 93, 052117 (2016) | 10.1103/PhysRevA.93.052117 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study radiative processes of uniformly accelerated entangled atoms,
interacting with an electromagnetic field prepared in the Minkowski vacuum
state. We discuss the structure of the rate of variation of the atomic energy
for two atoms travelling in different hyperbolic world lines. We identify the
contributions of... | [
{
"created": "Wed, 9 Dec 2015 15:00:55 GMT",
"version": "v1"
},
{
"created": "Wed, 11 May 2016 03:24:42 GMT",
"version": "v2"
}
] | 2016-06-01 | [
[
"Menezes",
"G.",
""
],
[
"Svaiter",
"N. F.",
""
]
] | We study radiative processes of uniformly accelerated entangled atoms, interacting with an electromagnetic field prepared in the Minkowski vacuum state. We discuss the structure of the rate of variation of the atomic energy for two atoms travelling in different hyperbolic world lines. We identify the contributions of v... | 10.556826 | 11.588369 | 9.396306 | 8.591262 | 10.698769 | 10.736259 | 11.628575 | 8.851942 | 10.428766 | 10.36968 | 10.310534 | 10.55245 | 10.39566 | 10.310601 | 10.803359 | 10.317744 | 10.514736 | 10.012389 | 10.599001 | 10.51104 | 10.648915 |
0903.4894 | Ho-Ung Yee | Mahdi Torabian, Ho-Ung Yee | Holographic nonlinear hydrodynamics from AdS/CFT with
multiple/non-Abelian symmetries | 37 pages, v3: errors corrected, reference added, JHEP version | JHEP 0908:020,2009 | 10.1088/1126-6708/2009/08/020 | IC/2009/016 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study viscous hydrodynamics of hot conformal field theory plasma with
multiple/non-Abelian symmetries in the framework of AdS/CFT correspondence,
using a recently proposed method of directly solving bulk gravity in derivative
expansion of local plasma parameters. Our motivation is to better describe the
real QCD p... | [
{
"created": "Mon, 30 Mar 2009 17:48:32 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Apr 2009 12:49:02 GMT",
"version": "v2"
},
{
"created": "Fri, 14 Aug 2009 06:53:22 GMT",
"version": "v3"
}
] | 2009-08-14 | [
[
"Torabian",
"Mahdi",
""
],
[
"Yee",
"Ho-Ung",
""
]
] | We study viscous hydrodynamics of hot conformal field theory plasma with multiple/non-Abelian symmetries in the framework of AdS/CFT correspondence, using a recently proposed method of directly solving bulk gravity in derivative expansion of local plasma parameters. Our motivation is to better describe the real QCD pla... | 10.427109 | 11.825156 | 12.040645 | 10.721922 | 11.295912 | 11.890803 | 11.178736 | 11.555216 | 10.445294 | 13.264499 | 10.157112 | 10.628615 | 10.822366 | 10.434624 | 10.46214 | 10.653524 | 10.745076 | 10.434835 | 10.559172 | 10.888848 | 10.221176 |
1007.1724 | Andrew K. Waldron | Roberto Bonezzi, Emanuele Latini and Andrew Waldron | Gravity, Two Times, Tractors, Weyl Invariance and Six Dimensional
Quantum Mechanics | 27 pages, LaTeX | Phys.Rev.D82:064037,2010 | 10.1103/PhysRevD.82.064037 | null | hep-th gr-qc math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Fefferman and Graham showed some time ago that four dimensional conformal
geometries could be analyzed in terms of six dimensional, ambient, Riemannian
geometries admitting a closed homothety. Recently it was shown how conformal
geometry provides a description of physics manifestly invariant under local
choices of un... | [
{
"created": "Sat, 10 Jul 2010 14:53:55 GMT",
"version": "v1"
}
] | 2014-11-21 | [
[
"Bonezzi",
"Roberto",
""
],
[
"Latini",
"Emanuele",
""
],
[
"Waldron",
"Andrew",
""
]
] | Fefferman and Graham showed some time ago that four dimensional conformal geometries could be analyzed in terms of six dimensional, ambient, Riemannian geometries admitting a closed homothety. Recently it was shown how conformal geometry provides a description of physics manifestly invariant under local choices of unit... | 12.459544 | 13.905033 | 15.030631 | 12.914735 | 14.945704 | 14.809447 | 14.33079 | 13.386081 | 13.485352 | 16.42387 | 13.002554 | 12.389218 | 12.672167 | 11.883363 | 11.772771 | 12.581051 | 12.940435 | 11.766128 | 12.215898 | 12.607787 | 12.379018 |
2112.10725 | Davood Mahdavian Yekta | H. Babaei-Aghbolagh, Davood Mahdavian Yekta, Komeil Babaei Velni, H.
Mohammadzadeh | Complexity growth in Gubser-Rocha models with momentum relaxation | 25 pages, 3 figures and 1 table, Accepted for publication in EPJC.
arXiv admin note: text overlap with arXiv:1808.09917 by other authors | null | 10.1140/epjc/s10052-022-10253-9 | IPM/P-2021/51 | hep-th | http://creativecommons.org/licenses/by/4.0/ | The Einstein-Maxwell-Axion-Dilaton (EMAD) theories, based on the Gubser-Rocha
(GR) model, are very interesting in holographic calculations of strongly
correlated systems in the condensed matter physics. Due to the presence of
spatially dependent massless axionic scalar fields, the momentum is relaxed and
we have no t... | [
{
"created": "Mon, 20 Dec 2021 18:16:55 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Apr 2022 12:05:09 GMT",
"version": "v2"
}
] | 2022-05-18 | [
[
"Babaei-Aghbolagh",
"H.",
""
],
[
"Yekta",
"Davood Mahdavian",
""
],
[
"Velni",
"Komeil Babaei",
""
],
[
"Mohammadzadeh",
"H.",
""
]
] | The Einstein-Maxwell-Axion-Dilaton (EMAD) theories, based on the Gubser-Rocha (GR) model, are very interesting in holographic calculations of strongly correlated systems in the condensed matter physics. Due to the presence of spatially dependent massless axionic scalar fields, the momentum is relaxed and we have no tra... | 9.636148 | 8.306745 | 11.207026 | 8.480128 | 8.33849 | 8.50687 | 8.444194 | 8.109302 | 8.282772 | 9.878144 | 8.114108 | 8.69335 | 9.580338 | 8.955317 | 8.902579 | 8.725188 | 8.966492 | 8.965398 | 8.894454 | 9.962045 | 8.888838 |
hep-th/9806202 | Landau Network | A.Yu. Kamenshchik, I.M. Khalatnikov (Landau Institute for Theoretical
Physics, Moscow), M. Martellini (University of Milan) | Comment about UV regularization of basic commutators in string theories | LaTeX, 9 pages, no figures, submitted to Physics Letters B | Phys.Rev. D59 (1999) 046005 | 10.1103/PhysRevD.59.046005 | null | hep-th | null | Recently proposed by Hwang, Marnelius and Saltsidis zeta regularization of
basic commutators in string theories is generalized to the string models with
non-trivial vacuums. It is shown that implementation of this regularization
implies the cancellation of dangerous terms in the commutators between Virasoro
generator... | [
{
"created": "Wed, 24 Jun 1998 15:43:09 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Kamenshchik",
"A. Yu.",
"",
"Landau Institute for Theoretical\n Physics, Moscow"
],
[
"Khalatnikov",
"I. M.",
"",
"Landau Institute for Theoretical\n Physics, Moscow"
],
[
"Martellini",
"M.",
"",
"University of Milan"
]
] | Recently proposed by Hwang, Marnelius and Saltsidis zeta regularization of basic commutators in string theories is generalized to the string models with non-trivial vacuums. It is shown that implementation of this regularization implies the cancellation of dangerous terms in the commutators between Virasoro generators,... | 22.255781 | 23.800329 | 34.532356 | 18.679569 | 19.55489 | 23.098665 | 24.687344 | 20.735821 | 18.532829 | 25.431835 | 19.234873 | 16.831995 | 20.719969 | 17.985359 | 20.997519 | 19.078037 | 18.345718 | 19.270386 | 18.478443 | 20.159353 | 17.174623 |
hep-th/0507068 | Mariusz Dabrowski P. | Mariusz P. Dabrowski, Tomasz Denkiewicz and David Blaschke | The conformal status of $\omega=-3/2$ Brans-Dicke cosmology | REVTEX4, 19 pages, 8 figures, references added | AnnalenPhys.16:237,2007 | 10.1002/andp.200610230 | MPG-VT-UR 262/05 | hep-th astro-ph gr-qc | null | Following recent fit of supernovae data to Brans-Dicke theory which favours
the model with $\omega = - 3/2$ \cite{fabris} we discuss the status of this
special case of Brans-Dicke cosmology in both isotropic and anisotropic
framework. It emerges that the limit $\omega = -3/2$ is consistent only with
the vacuum field ... | [
{
"created": "Thu, 7 Jul 2005 08:38:34 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Jul 2005 11:12:31 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Jan 2006 19:00:20 GMT",
"version": "v3"
},
{
"created": "Fri, 6 Jan 2006 08:10:10 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Dabrowski",
"Mariusz P.",
""
],
[
"Denkiewicz",
"Tomasz",
""
],
[
"Blaschke",
"David",
""
]
] | Following recent fit of supernovae data to Brans-Dicke theory which favours the model with $\omega = - 3/2$ \cite{fabris} we discuss the status of this special case of Brans-Dicke cosmology in both isotropic and anisotropic framework. It emerges that the limit $\omega = -3/2$ is consistent only with the vacuum field eq... | 7.059752 | 7.053794 | 6.97717 | 7.052543 | 7.667985 | 7.591048 | 7.578545 | 7.242988 | 7.028337 | 7.266807 | 7.073645 | 7.10851 | 6.905286 | 6.884797 | 7.014511 | 6.817101 | 6.915531 | 6.866036 | 6.998533 | 6.918575 | 6.95035 |
hep-th/0511087 | Hisham Sati | Hisham Sati | The Elliptic curves in gauge theory, string theory, and cohomology | 23 pages, typos corrected, minor clarifications | JHEP 0603 (2006) 096 | 10.1088/1126-6708/2006/03/096 | null | hep-th | null | Elliptic curves play a natural and important role in elliptic cohomology. In
earlier work with I. Kriz, thes elliptic curves were interpreted physically in
two ways: as corresponding to the intersection of M2 and M5 in the context of
(the reduction of M-theory to) type IIA and as the elliptic fiber leading to
F-theor... | [
{
"created": "Tue, 8 Nov 2005 04:02:18 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Nov 2005 22:06:18 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Sati",
"Hisham",
""
]
] | Elliptic curves play a natural and important role in elliptic cohomology. In earlier work with I. Kriz, thes elliptic curves were interpreted physically in two ways: as corresponding to the intersection of M2 and M5 in the context of (the reduction of M-theory to) type IIA and as the elliptic fiber leading to F-theory ... | 10.268895 | 11.675709 | 11.913672 | 10.436331 | 10.649746 | 11.847636 | 11.643723 | 10.782696 | 10.62746 | 13.560321 | 10.271238 | 9.986369 | 10.47285 | 10.181442 | 10.382516 | 10.118536 | 10.273734 | 10.235223 | 10.465831 | 10.716229 | 10.213369 |
hep-th/9607200 | Peter Cho | Peter Cho and Per Kraus | Symplectic SUSY Gauge Theories with Antisymmetric Matter | 21 pages, Revtex | Phys.Rev. D54 (1996) 7640-7649 | 10.1103/PhysRevD.54.7640 | CALT-68-2062 | hep-th hep-ph | null | We investigate the confining phase vacua of supersymmetric $Sp(2\NC)$ gauge
theories that contain matter in both fundamental and antisymmetric
representations. The moduli spaces of such models with $\NF=3$ quark flavors
and $\NA=1$ antisymmetric field are analogous to that of SUSY QCD with
$\NF=\NC+1$ flavors. In par... | [
{
"created": "Thu, 25 Jul 1996 20:53:34 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Cho",
"Peter",
""
],
[
"Kraus",
"Per",
""
]
] | We investigate the confining phase vacua of supersymmetric $Sp(2\NC)$ gauge theories that contain matter in both fundamental and antisymmetric representations. The moduli spaces of such models with $\NF=3$ quark flavors and $\NA=1$ antisymmetric field are analogous to that of SUSY QCD with $\NF=\NC+1$ flavors. In parti... | 9.825638 | 10.269605 | 10.603323 | 9.367795 | 10.315261 | 10.401519 | 9.648699 | 9.851746 | 9.34984 | 11.181866 | 9.390635 | 9.676348 | 9.825757 | 9.499051 | 9.65206 | 9.806263 | 9.418762 | 9.397897 | 9.626022 | 9.792936 | 9.433646 |
0801.3836 | Josh Guffin | Josh Guffin and Eric Sharpe | A-twisted Landau-Ginzburg models | 64 Pages, LaTeX | J. Geom. Phys. 59 (2009) 1547-1580 | 10.1016/j.geomphys.2009.07.014 | VPI-IPNAS-08-01, ILL-TH-08-1 | hep-th | null | In this paper we discuss correlation functions in certain A-twisted
Landau-Ginzburg models. Although B-twisted Landau-Ginzburg models have been
discussed extensively in the literature, virtually no work has been done on
A-twisted theories. In particular, we study examples of Landau-Ginzburg models
over topologically ... | [
{
"created": "Thu, 24 Jan 2008 20:36:02 GMT",
"version": "v1"
}
] | 2017-08-31 | [
[
"Guffin",
"Josh",
""
],
[
"Sharpe",
"Eric",
""
]
] | In this paper we discuss correlation functions in certain A-twisted Landau-Ginzburg models. Although B-twisted Landau-Ginzburg models have been discussed extensively in the literature, virtually no work has been done on A-twisted theories. In particular, we study examples of Landau-Ginzburg models over topologically no... | 8.746429 | 8.082413 | 10.229973 | 7.833869 | 7.517695 | 8.296745 | 7.400332 | 7.905278 | 7.589463 | 11.143082 | 7.957408 | 8.177357 | 9.288722 | 8.296047 | 8.142208 | 8.435307 | 8.448697 | 8.351545 | 8.302349 | 9.501234 | 8.312314 |
0812.3617 | Agostino Patella | Luigi Del Debbio, Agostino Patella | Center symmetry and the orientifold planar equivalence | 27 pages, 7 eps figures | JHEP 0903:071,2009 | 10.1088/1126-6708/2009/03/071 | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the center symmetry of SU(N) gauge theories with fermions in the
two-index representations, by computing the effective potential of the Polyakov
loop in the large-mass expansion on the lattice. In the large-N limit and at
non-zero temperature, we find that the center symmetry is Z_N for fermions in
the adjoi... | [
{
"created": "Thu, 18 Dec 2008 18:36:18 GMT",
"version": "v1"
}
] | 2011-06-24 | [
[
"Del Debbio",
"Luigi",
""
],
[
"Patella",
"Agostino",
""
]
] | We study the center symmetry of SU(N) gauge theories with fermions in the two-index representations, by computing the effective potential of the Polyakov loop in the large-mass expansion on the lattice. In the large-N limit and at non-zero temperature, we find that the center symmetry is Z_N for fermions in the adjoint... | 7.221764 | 6.919383 | 7.870417 | 7.037629 | 6.742894 | 7.166261 | 7.397734 | 6.712475 | 7.008827 | 8.553416 | 6.910933 | 6.762424 | 6.921443 | 6.735443 | 6.797896 | 6.880866 | 7.064994 | 6.757768 | 6.84847 | 6.990198 | 6.667098 |
1009.2887 | Giampiero Esposito Dr. | Giampiero Esposito, Raju Roychowdhury, Claudio Rubano, Paolo
Scudellaro | On the transition from complex to real scalar fields in modern cosmology | 21 pages, 6 figures. In the new version, sections I, IV and VI have
been improved, and two words have been added at the beginning of the title | null | 10.1142/S0219887811005956 | DSF 2010/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study some problems arising from the introduction of a complex scalar
field in cosmology, modelling its possible behaviors in both the inflationary
and dark energy stages of the universe. Such examples contribute to show that,
while the complex nature of the scalar field can be indeed important during
inflation, i... | [
{
"created": "Wed, 15 Sep 2010 10:13:35 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Nov 2010 13:14:32 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Apr 2011 14:47:15 GMT",
"version": "v3"
}
] | 2015-05-19 | [
[
"Esposito",
"Giampiero",
""
],
[
"Roychowdhury",
"Raju",
""
],
[
"Rubano",
"Claudio",
""
],
[
"Scudellaro",
"Paolo",
""
]
] | We study some problems arising from the introduction of a complex scalar field in cosmology, modelling its possible behaviors in both the inflationary and dark energy stages of the universe. Such examples contribute to show that, while the complex nature of the scalar field can be indeed important during inflation, it ... | 13.705319 | 14.12748 | 13.108912 | 13.181801 | 12.947875 | 13.772059 | 13.804292 | 12.975874 | 13.297755 | 13.275087 | 13.645379 | 13.612888 | 12.848921 | 12.989977 | 13.035884 | 13.25254 | 13.317389 | 12.552273 | 13.001146 | 13.43663 | 13.598336 |
1210.5008 | Leonardo Mondaini | Leonardo Mondaini | Obtaining a closed-form representation for the dual bosonic thermal
Green function by using methods of integration on the complex plane | To appear in Rev. Bras. Ens. Fis., 7 pages | Rev. Bras. Ens. Fis. 34, 3305 (2012) | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive an exact closed-form representation for the Euclidean thermal Green
function of the two-dimensional (2D) free massless scalar field in coordinate
space. This can be interpreted as the real part of a complex analytic function
of a variable that conformally maps the infinite strip $-\infty<x<\infty$
($0<\tau<... | [
{
"created": "Thu, 18 Oct 2012 02:14:20 GMT",
"version": "v1"
}
] | 2012-10-23 | [
[
"Mondaini",
"Leonardo",
""
]
] | We derive an exact closed-form representation for the Euclidean thermal Green function of the two-dimensional (2D) free massless scalar field in coordinate space. This can be interpreted as the real part of a complex analytic function of a variable that conformally maps the infinite strip $-\infty<x<\infty$ ($0<\tau<\b... | 6.755188 | 7.320735 | 7.546813 | 7.008245 | 7.258057 | 7.424216 | 6.937768 | 6.830454 | 6.051867 | 6.893085 | 6.398021 | 6.539035 | 6.650074 | 6.343747 | 6.412211 | 6.435849 | 6.422783 | 6.313749 | 6.308424 | 6.622015 | 6.136276 |
hep-th/0102207 | Archil Kobakhidze | Z. Berezhiani, M. Chaichian, A.B. Kobakhidze and Z.-H. Yu | Vanishing of cosmological constant and fully localized gravity in a
Brane World with extra time(s) | 15 pages, comments and references added, version accepted in Phys.
Lett. B | Phys.Lett. B517 (2001) 387-396 | 10.1016/S0370-2693(01)01022-X | HIP-2001-04/TH | hep-th hep-ph | null | We construct an intersecting brane configuration in six-dimensional space
with one extra space-like and one extra time-like dimensions. With a certain
additional symmetry imposed on the extra space-time we have found that
effective four-dimensional cosmological constant vanishes automatically,
providing the static so... | [
{
"created": "Wed, 28 Feb 2001 15:16:47 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Aug 2001 08:19:46 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Berezhiani",
"Z.",
""
],
[
"Chaichian",
"M.",
""
],
[
"Kobakhidze",
"A. B.",
""
],
[
"Yu",
"Z. -H.",
""
]
] | We construct an intersecting brane configuration in six-dimensional space with one extra space-like and one extra time-like dimensions. With a certain additional symmetry imposed on the extra space-time we have found that effective four-dimensional cosmological constant vanishes automatically, providing the static solu... | 16.136951 | 16.838594 | 14.249796 | 14.026382 | 14.592907 | 15.808924 | 14.94311 | 14.522734 | 14.510588 | 17.070976 | 14.907262 | 14.884026 | 15.105787 | 14.25059 | 15.488794 | 14.480728 | 15.336094 | 14.638158 | 14.520379 | 14.924133 | 14.584775 |
0801.2306 | Michael Bordag | M. Bordag, V.Skalozub | Polarization tensor of charged gluons in color magnetic background field
at finite temperature | 28 pages, submitted to Phys.Rev.D | Phys.Rev.D77:105013,2008 | 10.1103/PhysRevD.77.105013 | null | hep-th | null | We calculate the polarization tensor of charged gluons in a Abelian
homogeneous magnetic background field at finite temperature in one loop order
Lorentz background field gauge in full generality. Thereby we first determine
the ten independent tensor structures. For the calculation of the corresponding
form factors w... | [
{
"created": "Tue, 15 Jan 2008 14:22:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Bordag",
"M.",
""
],
[
"Skalozub",
"V.",
""
]
] | We calculate the polarization tensor of charged gluons in a Abelian homogeneous magnetic background field at finite temperature in one loop order Lorentz background field gauge in full generality. Thereby we first determine the ten independent tensor structures. For the calculation of the corresponding form factors we ... | 11.66433 | 10.416481 | 12.199162 | 10.724192 | 10.883702 | 11.287222 | 10.82849 | 10.632126 | 11.065231 | 13.651484 | 11.664513 | 11.077394 | 11.246514 | 10.436104 | 10.607682 | 10.652095 | 10.382865 | 10.748479 | 11.101287 | 10.735039 | 11.054715 |
1810.06954 | Mariana Carrillo-Gonzalez | Mariana Carrillo-Gonzalez, Robert F. Penna | Asymptotic symmetries of three dimensional gravity and the membrane
paradigm | 15 pages | null | 10.1007/JHEP02(2019)125 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The asymptotic symmetry group of three-dimensional (anti) de Sitter space is
the two dimensional conformal group with central charge $c=3\ell/2G$. Usually
the asymptotic charge algebra is derived using the symplectic structure of the
bulk Einstein equations. Here, we derive the asymptotic charge algebra by a
differen... | [
{
"created": "Tue, 16 Oct 2018 12:36:19 GMT",
"version": "v1"
}
] | 2019-03-27 | [
[
"Carrillo-Gonzalez",
"Mariana",
""
],
[
"Penna",
"Robert F.",
""
]
] | The asymptotic symmetry group of three-dimensional (anti) de Sitter space is the two dimensional conformal group with central charge $c=3\ell/2G$. Usually the asymptotic charge algebra is derived using the symplectic structure of the bulk Einstein equations. Here, we derive the asymptotic charge algebra by a different ... | 4.648603 | 4.301666 | 4.738173 | 4.45927 | 4.566989 | 4.631166 | 4.64219 | 4.260908 | 4.507342 | 5.058889 | 4.374257 | 4.253272 | 4.573801 | 4.233078 | 4.414612 | 4.35554 | 4.343341 | 4.295576 | 4.371511 | 4.488744 | 4.479702 |
2110.05793 | Mahsa Lezgi | Mohammad Ali-Akbari, Mahsa Lezgi | Note on stability and holographic subregion complexity | null | null | 10.1140/epjc/s10052-022-10071-z | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | We study holographic subregion complexity in a spatially anisotropic field
theory, which expresses a confinement-deconfinement phase transition. Its
holographic dual is a five-dimensional anisotropic holographic model
characterized by a Van der Waals-like phase transition between small and large
black holes. We propo... | [
{
"created": "Tue, 12 Oct 2021 07:44:17 GMT",
"version": "v1"
}
] | 2022-02-23 | [
[
"Ali-Akbari",
"Mohammad",
""
],
[
"Lezgi",
"Mahsa",
""
]
] | We study holographic subregion complexity in a spatially anisotropic field theory, which expresses a confinement-deconfinement phase transition. Its holographic dual is a five-dimensional anisotropic holographic model characterized by a Van der Waals-like phase transition between small and large black holes. We propose... | 11.507527 | 9.942965 | 12.667144 | 10.236265 | 10.755038 | 10.136765 | 10.747905 | 10.639972 | 10.442164 | 13.125274 | 10.501987 | 10.960524 | 11.250063 | 10.506632 | 10.790199 | 11.093887 | 10.763665 | 11.070437 | 10.790629 | 11.136163 | 10.87278 |
hep-th/9512057 | Gennady Danilov | G. S. Danilov | Unimodular transformations of the supermanifolds and the calculation of
the multi-loop amplitudes in the superstring theory | 44 pages, LATEX | Nucl.Phys.B463:443-488,1996 | 10.1016/0550-3213(96)00006-5 | Preprint PNPI-2075, 1995 | hep-th | null | The modular transformations of the $(1|1)$ complex supermanifolds in the
like-Schottky modular parameterization are discussed. It is shown that these
"supermodular" transformations depend on the spinor structure of the
supermanifold by terms proportional to the odd modular parameters. The above
terms are calculated i... | [
{
"created": "Fri, 8 Dec 1995 13:35:17 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Danilov",
"G. S.",
""
]
] | The modular transformations of the $(1|1)$ complex supermanifolds in the like-Schottky modular parameterization are discussed. It is shown that these "supermodular" transformations depend on the spinor structure of the supermanifold by terms proportional to the odd modular parameters. The above terms are calculated in ... | 12.319111 | 13.383199 | 13.375394 | 12.642715 | 13.480452 | 12.943098 | 13.323296 | 12.137523 | 12.101703 | 15.570521 | 12.103983 | 12.050941 | 12.122504 | 11.557408 | 12.206565 | 11.917973 | 12.620625 | 11.743437 | 11.771921 | 12.446312 | 11.597159 |
1807.01792 | Mehrab Momennia | Mehrab Momennia, Seyed Hossein Hendi and Fatemeh Soltani Bidgoli | Stability and Quasinormal Modes of Black Holes in Conformal Weyl Gravity | 16 pages with 8 captioned figures and 5 tables. Published version | Phys. Lett. B 813 (2021) 136028 | 10.1016/j.physletb.2020.136028 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we first investigate the thermal stability of black holes in
conformal Weyl gravity with a comparison with the Schwarzschild black holes.
Then, we consider a minimally coupled massive scalar perturbation and calculate
the quasinormal modes in asymptotically dS spacetime by employing the sixth
order WKB... | [
{
"created": "Wed, 4 Jul 2018 21:35:44 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 2019 05:47:54 GMT",
"version": "v2"
},
{
"created": "Tue, 22 Dec 2020 08:36:40 GMT",
"version": "v3"
}
] | 2022-08-09 | [
[
"Momennia",
"Mehrab",
""
],
[
"Hendi",
"Seyed Hossein",
""
],
[
"Bidgoli",
"Fatemeh Soltani",
""
]
] | In this paper, we first investigate the thermal stability of black holes in conformal Weyl gravity with a comparison with the Schwarzschild black holes. Then, we consider a minimally coupled massive scalar perturbation and calculate the quasinormal modes in asymptotically dS spacetime by employing the sixth order WKB a... | 5.723618 | 5.44436 | 5.024037 | 4.808569 | 5.474821 | 5.194319 | 5.626647 | 4.519267 | 5.362581 | 4.85099 | 5.688833 | 5.317187 | 5.060603 | 5.227436 | 5.275178 | 5.303974 | 5.544045 | 4.944625 | 5.353823 | 5.126201 | 5.29163 |
hep-th/9502014 | Jean-Marc Daul | Jean-Marc DAUL | Q-states Potts model on a random planar lattice | 12 pages, 1 PostScript figure, with epsf | null | null | LPTENS 94- | hep-th | null | We propose a matrix-model derivation of the scaling exponents of the critical
and tricritical q-states Potts model coupled to gravity on a sphere. In close
analogy with the $O(n)$ model, we reduce the determination of the
one-loop-to-vacuum expectation to the resolution of algebraic equations; and
find the explicit s... | [
{
"created": "Thu, 2 Feb 1995 11:56:57 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"DAUL",
"Jean-Marc",
""
]
] | We propose a matrix-model derivation of the scaling exponents of the critical and tricritical q-states Potts model coupled to gravity on a sphere. In close analogy with the $O(n)$ model, we reduce the determination of the one-loop-to-vacuum expectation to the resolution of algebraic equations; and find the explicit sca... | 16.686771 | 17.246378 | 15.708776 | 16.132051 | 17.05024 | 18.204197 | 15.896439 | 16.675169 | 15.070634 | 19.994442 | 16.79747 | 16.482906 | 15.940804 | 15.533702 | 16.913828 | 16.37994 | 16.303347 | 16.726088 | 15.999828 | 16.556763 | 16.732067 |
hep-th/0006024 | Miao Li | Miao Li | Black Holes and Spacetime Physics in String/M Theory | 33 pages, harvmac | null | null | null | hep-th gr-qc hep-ph | null | In addition to briefly reviewing recent progress in studying black hole
physics in string/M theory, we describe several robust features pertaining to
spacetime physics that one can glean by studying quantum physics of black
holes. In particular, we review 't Hooft's S-matrix ansatz which results in a
noncommutative h... | [
{
"created": "Mon, 5 Jun 2000 14:09:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Li",
"Miao",
""
]
] | In addition to briefly reviewing recent progress in studying black hole physics in string/M theory, we describe several robust features pertaining to spacetime physics that one can glean by studying quantum physics of black holes. In particular, we review 't Hooft's S-matrix ansatz which results in a noncommutative hor... | 15.562478 | 13.744836 | 16.101494 | 14.372013 | 14.785785 | 16.015087 | 13.358347 | 13.584484 | 14.258785 | 16.189648 | 14.591254 | 14.237836 | 14.559861 | 14.089524 | 15.067724 | 15.079993 | 14.943772 | 13.687999 | 14.564964 | 14.762807 | 14.590733 |
hep-th/9607124 | Jeremy S. Heyl | Jeremy S. Heyl and Lars Hernquist | An Analytic Form for the Effective Lagrangian of QED and its Application
to Pair Production and Photon Splitting | ReVTeX, 9 pages, 4 figures, to be published in Phys. Rev. D | Phys.Rev. D55 (1997) 2449-2454 | 10.1103/PhysRevD.55.2449 | null | hep-th astro-ph | null | We derive an analytic form for the Heisenberg-Euler Lagrangian in the limit
where the component of the electric field parallel to the magnetic field is
small. We expand these analytic functions to all orders in the field strength
($F_{\mu\nu}F^{\mu\nu}$) in the limits of weak and strong fields, and use these
function... | [
{
"created": "Mon, 15 Jul 1996 22:02:42 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Heyl",
"Jeremy S.",
""
],
[
"Hernquist",
"Lars",
""
]
] | We derive an analytic form for the Heisenberg-Euler Lagrangian in the limit where the component of the electric field parallel to the magnetic field is small. We expand these analytic functions to all orders in the field strength ($F_{\mu\nu}F^{\mu\nu}$) in the limits of weak and strong fields, and use these functions ... | 6.141077 | 6.324913 | 5.803249 | 5.367451 | 5.606636 | 5.624126 | 5.841646 | 5.859613 | 5.530637 | 5.926682 | 5.49456 | 5.872404 | 5.313743 | 5.487991 | 5.724268 | 5.558416 | 5.715539 | 5.379034 | 5.594485 | 5.406192 | 5.577193 |
hep-th/9806052 | Kenji Mohri | Kenji Mohri (KEK) | K\"ahler Moduli Space of a D-Brane at Orbifold Singularities | 41 pages (double spacing version) | Commun.Math.Phys. 202 (1999) 669-699 | 10.1007/s002200050601 | null | hep-th | null | We develop a method to analyze systematically the configuration space of a
D-brane localized at the orbifold singular point of a Calabi--Yau $d$-fold of
the form ${\Bbb C}^d/\Gamma$ using the theory of toric quotients. This approach
elucidates the structure of the K\"ahler moduli space associated with the
problem. As... | [
{
"created": "Mon, 8 Jun 1998 05:08:59 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Jun 1998 04:14:26 GMT",
"version": "v2"
},
{
"created": "Wed, 10 Jun 1998 03:12:24 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Mohri",
"Kenji",
"",
"KEK"
]
] | We develop a method to analyze systematically the configuration space of a D-brane localized at the orbifold singular point of a Calabi--Yau $d$-fold of the form ${\Bbb C}^d/\Gamma$ using the theory of toric quotients. This approach elucidates the structure of the K\"ahler moduli space associated with the problem. As a... | 7.516108 | 8.178522 | 8.695939 | 7.595536 | 7.859637 | 7.828517 | 7.288403 | 6.882715 | 7.527976 | 9.584663 | 7.542845 | 7.494745 | 8.36804 | 7.380534 | 7.11603 | 7.235021 | 7.106529 | 7.410725 | 7.284781 | 7.939873 | 7.389562 |
0808.2060 | Anirban Basu | Anirban Basu | Constraining the D3-brane effective action | 22 pages, LaTeX | JHEP 0809:124,2008 | 10.1088/1126-6708/2008/09/124 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider higher derivative corrections of the type D^{2k} R^2 in the
effective action of the D3-brane with trivial normal bundle. Based on the
perturbative disc and annulus amplitudes, and constraints of supersymmetry and
duality, we argue that these interactions are protected, at least for small
values of k. Thei... | [
{
"created": "Thu, 14 Aug 2008 20:38:40 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Basu",
"Anirban",
""
]
] | We consider higher derivative corrections of the type D^{2k} R^2 in the effective action of the D3-brane with trivial normal bundle. Based on the perturbative disc and annulus amplitudes, and constraints of supersymmetry and duality, we argue that these interactions are protected, at least for small values of k. Their ... | 8.720988 | 7.714558 | 11.3207 | 7.733821 | 7.44769 | 7.661578 | 7.450227 | 8.066481 | 7.445433 | 10.99828 | 7.808935 | 7.983823 | 9.760905 | 8.097368 | 7.775846 | 8.105062 | 7.842708 | 8.215184 | 7.858415 | 9.840126 | 8.118813 |
hep-th/0006136 | Dariusz Chruscinski | D. Chruscinski | Quasi-local structure of p-form theory | 25 pages, LaTeX | Acta Phys.Polon. B32 (2001) 147-182 | null | null | hep-th | null | We show that the Hamiltonian dynamics of the self-interacting, abelian p-form
theory in D=2p+2 dimensional space-time gives rise to the quasi-local
structure. Roughly speaking, it means that the field energy is localized but on
closed 2p-dimensional surfaces (quasi-localized). From the mathematical point
of view this... | [
{
"created": "Mon, 19 Jun 2000 08:07:18 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Jun 2000 09:46:36 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Chruscinski",
"D.",
""
]
] | We show that the Hamiltonian dynamics of the self-interacting, abelian p-form theory in D=2p+2 dimensional space-time gives rise to the quasi-local structure. Roughly speaking, it means that the field energy is localized but on closed 2p-dimensional surfaces (quasi-localized). From the mathematical point of view this a... | 14.061884 | 12.989159 | 14.042339 | 12.636979 | 12.600281 | 13.700968 | 12.905633 | 12.806212 | 13.198441 | 14.358463 | 12.830759 | 13.113888 | 13.81163 | 13.005732 | 13.049301 | 13.44102 | 13.362828 | 13.460816 | 13.183486 | 13.907307 | 12.686592 |
hep-th/0307059 | Amir Masoud Ghezelbash | R. Clarkson, A.M. Ghezelbash, R.B. Mann | Entropic N-bound and Maximal Mass Conjecture Violations in Four
Dimensional Taub-Bolt(NUT)-dS Spacetimes | 37 pages, 22 figures, 3 tables, few typos corrected, version to
appear in Nucl. Phys. B | Nucl.Phys. B674 (2003) 329-364 | 10.1016/j.nuclphysb.2003.09.039 | null | hep-th gr-qc | null | We show that the class of four-dimensional Taub-Bolt(NUT) spacetimes with
positive cosmological constant for some values of NUT charges are stable and
have entropies that are greater than that of de Sitter spacetime, in violation
of the entropic N-bound conjecture. We also show that the maximal mass
conjecture, which... | [
{
"created": "Sun, 6 Jul 2003 00:01:21 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Oct 2003 17:49:56 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Clarkson",
"R.",
""
],
[
"Ghezelbash",
"A. M.",
""
],
[
"Mann",
"R. B.",
""
]
] | We show that the class of four-dimensional Taub-Bolt(NUT) spacetimes with positive cosmological constant for some values of NUT charges are stable and have entropies that are greater than that of de Sitter spacetime, in violation of the entropic N-bound conjecture. We also show that the maximal mass conjecture, which s... | 8.94665 | 7.163522 | 9.607893 | 8.000149 | 7.380378 | 7.707019 | 6.999004 | 7.661808 | 7.465535 | 10.0403 | 7.278409 | 7.795179 | 8.080074 | 8.066235 | 7.940704 | 7.994903 | 7.676498 | 8.130138 | 7.864285 | 8.418205 | 7.800128 |
hep-th/9612185 | Manfred Requardt | Manfred Requardt | Emergence of Space-Time on the Planck Scale within the Scheme of
Dynamical Cellular Networks and Random Graphs | 5 pages, Latex | null | null | Re-96-04 | hep-th gr-qc | null | The following is a short report about recent work on discrete
physics/mathematics on the Planckscale and the use of the concept of ''random
graphs'' in this business, appearing in the group21-proceedings (Gosslar 1996)
| [
{
"created": "Wed, 18 Dec 1996 09:33:51 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Requardt",
"Manfred",
""
]
] | The following is a short report about recent work on discrete physics/mathematics on the Planckscale and the use of the concept of ''random graphs'' in this business, appearing in the group21-proceedings (Gosslar 1996) | 37.129623 | 48.233364 | 40.533157 | 39.335201 | 46.534046 | 49.128967 | 46.537716 | 34.975243 | 36.248016 | 41.837734 | 38.230179 | 37.358604 | 42.531952 | 41.207787 | 42.226551 | 40.09441 | 39.681965 | 40.205021 | 43.133034 | 40.431946 | 38.793343 |
hep-th/0503198 | Anastasia Volovich | Ruth Britto, Bo Feng, Radu Roiban, Marcus Spradlin, Anastasia Volovich | All Split Helicity Tree-Level Gluon Amplitudes | 15 pages, harvmac, v2: typos corrected | Phys.Rev. D71 (2005) 105017 | 10.1103/PhysRevD.71.105017 | PUPT-2157, NSF-KITP-05-18 | hep-th hep-ph | null | Recently a new recursion relation for tree-level gluon amplitudes in gauge
theory has been discovered. We solve this recursion to obtain explicit formulas
for the closed set of amplitudes with arbitrarily many positive and negative
helicity gluons in a split helicity configuration. The solution admits a simple
diagra... | [
{
"created": "Fri, 25 Mar 2005 03:00:58 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Apr 2006 14:39:16 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Britto",
"Ruth",
""
],
[
"Feng",
"Bo",
""
],
[
"Roiban",
"Radu",
""
],
[
"Spradlin",
"Marcus",
""
],
[
"Volovich",
"Anastasia",
""
]
] | Recently a new recursion relation for tree-level gluon amplitudes in gauge theory has been discovered. We solve this recursion to obtain explicit formulas for the closed set of amplitudes with arbitrarily many positive and negative helicity gluons in a split helicity configuration. The solution admits a simple diagramm... | 9.965912 | 8.001244 | 8.603362 | 7.611784 | 8.563384 | 7.65577 | 7.327217 | 7.718598 | 8.158457 | 10.060603 | 7.723891 | 8.555238 | 9.41348 | 8.795568 | 8.61623 | 8.623915 | 8.407622 | 8.807214 | 8.550633 | 9.384067 | 8.525929 |
1910.12312 | Thomas Schaefer | Aleksey Cherman, Syo Kamata, Thomas Schaefer, Mithat \"Unsal | Flow of Hagedorn singularities and phase transitions in large $N$ gauge
theories | 7 pages, 6 figures | Phys. Rev. D 101, 014012 (2020) | 10.1103/PhysRevD.101.014012 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the singularity structure of the $(-1)^F$ graded partition
function in QCD with $n_f \geq 1$ massive adjoint fermions in the large-$N$
limit. Here, $F$ is fermion number and $N$ is the number of colors. The large
$N$ partition function is made reliably calculable by taking space to be a
small three-sph... | [
{
"created": "Sun, 27 Oct 2019 18:01:23 GMT",
"version": "v1"
}
] | 2020-01-22 | [
[
"Cherman",
"Aleksey",
""
],
[
"Kamata",
"Syo",
""
],
[
"Schaefer",
"Thomas",
""
],
[
"Ünsal",
"Mithat",
""
]
] | We investigate the singularity structure of the $(-1)^F$ graded partition function in QCD with $n_f \geq 1$ massive adjoint fermions in the large-$N$ limit. Here, $F$ is fermion number and $N$ is the number of colors. The large $N$ partition function is made reliably calculable by taking space to be a small three-spher... | 7.43841 | 7.671927 | 8.158129 | 6.894435 | 8.183877 | 7.896372 | 7.343228 | 7.159902 | 7.141232 | 8.229835 | 7.125661 | 7.364303 | 7.456752 | 7.049015 | 7.335036 | 7.065161 | 6.919814 | 7.136713 | 7.187619 | 7.269183 | 7.085722 |
2401.00890 | Gideon Vos | Souvik Banerjee, Gideon Vos | Behind-the-horizon excitations from a single 2d CFT | 25 pages, 4 figures, 2 appendices | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we consider the atypical non-equilibrium state found in
[1708.06328] which holographically represents a behind-the-horizon excitation
in a blackhole spacetime. The special feature of this state is that it looks
like an equilibrium state when probed by a class of low-energy operators.
First, we retrieve ... | [
{
"created": "Sat, 30 Dec 2023 21:29:05 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Feb 2024 15:54:13 GMT",
"version": "v2"
},
{
"created": "Thu, 13 Jun 2024 13:50:31 GMT",
"version": "v3"
}
] | 2024-06-14 | [
[
"Banerjee",
"Souvik",
""
],
[
"Vos",
"Gideon",
""
]
] | In this work, we consider the atypical non-equilibrium state found in [1708.06328] which holographically represents a behind-the-horizon excitation in a blackhole spacetime. The special feature of this state is that it looks like an equilibrium state when probed by a class of low-energy operators. First, we retrieve th... | 14.057665 | 14.81916 | 15.917993 | 13.769612 | 15.231578 | 15.006525 | 14.693219 | 14.214323 | 13.59413 | 15.187078 | 12.795651 | 13.505924 | 14.058314 | 13.15222 | 13.702615 | 13.474347 | 13.969127 | 13.748201 | 13.366567 | 14.043909 | 12.881177 |
hep-th/9312085 | Hector DE Vega | H.J. de Vega, J. Ram\'irez Mittelbrunn, M. Ram\'on Medrano and N.
S\'anchez | The General Solution of the 2-D Sigma Model Stringy Black Hole and the
Massless Complex Sine-Gordon Model | 12 pages, uses phyzzx, LPTHE-PAR 93/53 | Phys.Lett. B323 (1994) 133-138 | 10.1016/0370-2693(94)90281-X | null | hep-th | null | The exact general solution for a sigma model having the $2-d$ stringy black
hole (SBH) as internal manifold is found in closed form. We also give the exact
solution for the massless complex Sine-Gordon (MCSG) model. Both, models and
their solutions are related by analytic continuation. The solution is expressed
in te... | [
{
"created": "Fri, 10 Dec 1993 15:05:46 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Dec 1993 15:40:36 GMT",
"version": "v2"
}
] | 2016-08-14 | [
[
"de Vega",
"H. J.",
""
],
[
"Mittelbrunn",
"J. Ramírez",
""
],
[
"Medrano",
"M. Ramón",
""
],
[
"Sánchez",
"N.",
""
]
] | The exact general solution for a sigma model having the $2-d$ stringy black hole (SBH) as internal manifold is found in closed form. We also give the exact solution for the massless complex Sine-Gordon (MCSG) model. Both, models and their solutions are related by analytic continuation. The solution is expressed in term... | 14.70818 | 13.658489 | 14.907256 | 11.673495 | 12.583105 | 11.101729 | 10.511917 | 11.690795 | 12.405884 | 15.596246 | 11.477816 | 12.368525 | 13.868253 | 13.182731 | 12.821855 | 12.495764 | 12.642963 | 13.196021 | 12.729886 | 13.916156 | 12.866983 |
1302.6382 | Roberto Emparan | Roberto Emparan, Ryotaku Suzuki, Kentaro Tanabe | The large D limit of General Relativity | 50 pages, 2 figures; v3: improved discussion of conceptual points | JHEP 1306 (2013) 009 | 10.1007/JHEP06(2013)009 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | General Relativity simplifies dramatically in the limit that the number of
spacetime dimensions D is infinite: it reduces to a theory of non-interacting
particles, of finite radius but vanishingly small cross sections, which do not
emit nor absorb radiation of any finite frequency. Non-trivial black hole
dynamics occ... | [
{
"created": "Tue, 26 Feb 2013 10:20:04 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Mar 2013 16:27:22 GMT",
"version": "v2"
},
{
"created": "Fri, 31 May 2013 10:40:41 GMT",
"version": "v3"
}
] | 2015-06-15 | [
[
"Emparan",
"Roberto",
""
],
[
"Suzuki",
"Ryotaku",
""
],
[
"Tanabe",
"Kentaro",
""
]
] | General Relativity simplifies dramatically in the limit that the number of spacetime dimensions D is infinite: it reduces to a theory of non-interacting particles, of finite radius but vanishingly small cross sections, which do not emit nor absorb radiation of any finite frequency. Non-trivial black hole dynamics occur... | 11.534761 | 12.110873 | 11.413318 | 10.828845 | 11.711391 | 12.532168 | 10.959158 | 11.494149 | 10.721362 | 12.195322 | 10.891032 | 10.885209 | 10.607082 | 10.587153 | 10.816215 | 10.552946 | 10.36182 | 10.513288 | 10.837646 | 11.136587 | 10.563334 |
2109.15022 | Haidar Sheikhahmadi | Haidar Sheikhahmadi | On the origin of the holographic universe | 8 Pages, some new explanations and references added | Modern Physics Letters A, Vol. 37, No. 33n34, 2250231 (2022) | 10.1142/S0217732322502315 | null | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | In this work, we reexamine the holographic dark energy concept proposed
already for cosmological applications. By considering, more precisely, the
bounds on the entropy arising from lattice field theory on one side and
Bekenstein-Hawking entropy of black holes on another side, it is shown that the
so-called holograph... | [
{
"created": "Thu, 30 Sep 2021 11:36:32 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Jan 2023 10:37:58 GMT",
"version": "v2"
}
] | 2023-03-02 | [
[
"Sheikhahmadi",
"Haidar",
""
]
] | In this work, we reexamine the holographic dark energy concept proposed already for cosmological applications. By considering, more precisely, the bounds on the entropy arising from lattice field theory on one side and Bekenstein-Hawking entropy of black holes on another side, it is shown that the so-called holographic... | 10.726401 | 9.884225 | 10.053026 | 10.12105 | 10.683386 | 10.253363 | 11.022915 | 9.75082 | 10.252874 | 9.585029 | 10.312029 | 9.699368 | 9.947559 | 9.944418 | 10.245883 | 9.796457 | 9.881412 | 9.945334 | 10.112294 | 9.830831 | 10.155893 |
hep-th/9506075 | Pietro Fre | A. Ceresole, M. Billo', R. D'Auria, S. Ferrara, P. Fre', T. Regge, P.
Soriani, A. Van Proeyen | A Search for Non-Perturbative Dualities of Local $N=2$ Yang--Mills
Theories from Calabi--Yau Threefolds | Latex. Version of previous paper with enlarged and revised appendix
35 pages, plain LaTeX | Class.Quant.Grav. 13 (1996) 831-864 | 10.1088/0264-9381/13/5/007 | SISSA 64/95/EP, POLFIS-TH 07/95, CERN-TH 95/140, IFUM 508/FT,
KUL-TF-95/18, UCLA/95/TEP/19 | hep-th | null | The generalisation of the rigid special geometry of the vector multiplet
quantum moduli space to the case of supergravity is discussed through the
notion of a dynamical Calabi--Yau threefold. Duality symmetries of this
manifold are connected with the analogous dualities associated with the
dynamical Riemann surface o... | [
{
"created": "Sun, 11 Jun 1995 17:47:38 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jun 1995 19:37:49 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Jan 1996 07:36:59 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"Ceresole",
"A.",
""
],
[
"Billo'",
"M.",
""
],
[
"D'Auria",
"R.",
""
],
[
"Ferrara",
"S.",
""
],
[
"Fre'",
"P.",
""
],
[
"Regge",
"T.",
""
],
[
"Soriani",
"P.",
""
],
[
"Van Proeyen",
"A.",
... | The generalisation of the rigid special geometry of the vector multiplet quantum moduli space to the case of supergravity is discussed through the notion of a dynamical Calabi--Yau threefold. Duality symmetries of this manifold are connected with the analogous dualities associated with the dynamical Riemann surface of ... | 9.788365 | 10.107842 | 9.860558 | 9.398779 | 9.989366 | 9.496198 | 10.020288 | 8.731595 | 9.450933 | 10.331507 | 9.041481 | 9.633911 | 9.580564 | 9.015545 | 9.2451 | 9.262556 | 9.109258 | 9.06565 | 8.850345 | 9.848716 | 9.167776 |
hep-th/0302071 | Tasneem Zehra Husain | Tasneem Zehra Husain | That's a wrap! | 19 pages, typos corrected | JHEP 0304 (2003) 053 | 10.1088/1126-6708/2003/04/053 | USITP-02-04 | hep-th | null | Calibration technology provides us with a fast and elegant way to find the
supergravity solutions for BPS wrapped M-branes. Its true potential had however
remained untapped due to the absence of a classification of calibrations in
spacetimes with non-trivial flux. The applications of this method were thus
limited in ... | [
{
"created": "Tue, 11 Feb 2003 13:39:43 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Apr 2003 12:57:48 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Husain",
"Tasneem Zehra",
""
]
] | Calibration technology provides us with a fast and elegant way to find the supergravity solutions for BPS wrapped M-branes. Its true potential had however remained untapped due to the absence of a classification of calibrations in spacetimes with non-trivial flux. The applications of this method were thus limited in pr... | 13.607018 | 12.198846 | 15.439177 | 12.424376 | 14.497776 | 12.457874 | 12.697649 | 12.824009 | 12.693709 | 16.765778 | 13.617144 | 11.128985 | 13.426966 | 12.052656 | 11.582591 | 11.248611 | 11.320285 | 11.939531 | 12.278625 | 14.032035 | 12.661433 |
hep-th/0009094 | Stephan Durr | Stephan D\"urr | The phase transition in the multiflavour Schwinger model | 6 pages, talk given at International Conference on Quantization,
Gauge Theory, and Strings: Conference Dedicated to the Memory of Professor
Efim Fradkin, 5-10 June 2000, Moscow, Russia | null | null | null | hep-th | null | A summary is given of a quantization of the multiflavour Schwinger model on a
finite-temperature cylinder with chirality-breaking boundary conditions at its
spatial ends, and it is shown that the analytic expression for the chiral
condensate implies that the theory exhibits a second order phase transition
with $T_c =... | [
{
"created": "Tue, 12 Sep 2000 14:12:23 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dürr",
"Stephan",
""
]
] | A summary is given of a quantization of the multiflavour Schwinger model on a finite-temperature cylinder with chirality-breaking boundary conditions at its spatial ends, and it is shown that the analytic expression for the chiral condensate implies that the theory exhibits a second order phase transition with $T_c = 0... | 12.909111 | 11.60113 | 12.198908 | 11.009809 | 12.411842 | 11.617911 | 11.347669 | 10.344579 | 10.306752 | 13.568565 | 11.293383 | 11.362997 | 11.363746 | 10.936088 | 10.90033 | 11.253623 | 10.540735 | 10.719296 | 10.684331 | 11.208995 | 10.671813 |
hep-th/0504193 | Kunihito Uzawa | Hideo Kodama, Kunihito Uzawa | Moduli Instability in Warped Compactifications of the Type IIB
Supergravity | 24 pages, no figure. Typos corrected, and some arguments in section 5
are added | JHEP 0507 (2005) 061 | 10.1088/1126-6708/2005/07/061 | null | hep-th gr-qc hep-ph | null | We show that the conifold and deformed-conifold warped compactifications of
the ten-dimensional type IIB supergravity, including the Klebanov-Strassler
solution, are dynamically unstable in the moduli sector representing the scale
of a Calabi-Yau space, although it can be practically stable for a quite long
time in a... | [
{
"created": "Mon, 25 Apr 2005 01:31:37 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Apr 2005 22:56:17 GMT",
"version": "v2"
},
{
"created": "Wed, 26 Apr 2006 00:33:36 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Kodama",
"Hideo",
""
],
[
"Uzawa",
"Kunihito",
""
]
] | We show that the conifold and deformed-conifold warped compactifications of the ten-dimensional type IIB supergravity, including the Klebanov-Strassler solution, are dynamically unstable in the moduli sector representing the scale of a Calabi-Yau space, although it can be practically stable for a quite long time in a r... | 12.161263 | 11.881916 | 12.749368 | 11.806754 | 10.968348 | 11.47578 | 12.511262 | 11.229752 | 11.263192 | 14.069477 | 10.665176 | 11.240055 | 11.720598 | 11.464322 | 11.330056 | 11.246277 | 11.197299 | 11.400496 | 11.153832 | 12.013532 | 11.067933 |
hep-th/9701050 | Guest Account Cts | A S Vytheeswaran (Bangalore University, India) | Gauge Invariances in the Proca model | Latex file, 18 pages, Revised version with extra equation and note
added in page 4, reference added, minor spelling corrections. To appear in
Int J Mod Phys A | Int.J.Mod.Phys. A13 (1998) 765-778 | 10.1142/S0217751X98000330 | null | hep-th | null | We show that the abelian Proca model, which is gauge non-invariant with
second class constraints can be converted into gauge theories with first class
constraints. The method used, which we call Gauge Unfixing employs a projection
operator defined in the original phase space. This operator can be constructed
in more ... | [
{
"created": "Mon, 13 Jan 1997 10:14:20 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Jun 1997 07:29:22 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Vytheeswaran",
"A S",
"",
"Bangalore University, India"
]
] | We show that the abelian Proca model, which is gauge non-invariant with second class constraints can be converted into gauge theories with first class constraints. The method used, which we call Gauge Unfixing employs a projection operator defined in the original phase space. This operator can be constructed in more th... | 9.505371 | 7.334038 | 9.269864 | 7.517373 | 7.397307 | 7.117168 | 7.630251 | 7.398593 | 7.46444 | 9.382491 | 7.278495 | 7.811158 | 8.639869 | 8.373508 | 7.8399 | 8.33388 | 8.096192 | 7.909886 | 8.190041 | 8.931141 | 7.949946 |
hep-th/9210122 | Keith Joshi | David C. Dunbar and Keith G. Joshi | Characters for Coset Conformal Field Theories | 20 pages in plain TEX | Int.J.Mod.Phys.A8:4103-4122,1993 | 10.1142/S0217751X93001685 | LTH-92-292 & SWAT-92-02 | hep-th | null | We solve the Kac-Moody branching equation to obtain explicit formulae for the
characters of coset conformal field theories and then apply these to specific
examples to determine the integer shift of the conformal weights of primary
fields. We also present an example of coset conformal field theory which cannot
be des... | [
{
"created": "Thu, 22 Oct 1992 12:19:00 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Dunbar",
"David C.",
""
],
[
"Joshi",
"Keith G.",
""
]
] | We solve the Kac-Moody branching equation to obtain explicit formulae for the characters of coset conformal field theories and then apply these to specific examples to determine the integer shift of the conformal weights of primary fields. We also present an example of coset conformal field theory which cannot be descr... | 15.794046 | 14.048363 | 16.47744 | 12.872178 | 15.011257 | 15.25698 | 15.403418 | 12.879622 | 12.716281 | 15.574998 | 12.054182 | 13.193765 | 13.526211 | 12.722583 | 13.682107 | 13.758544 | 13.391201 | 12.92572 | 12.598548 | 13.768661 | 13.243191 |
1302.2924 | Anton van Niekerk | Alex Buchel, Luis Lehner, Robert C. Myers and Anton van Niekerk | Quantum quenches of holographic plasmas | 60 pages, 10 figures, 3 appendices | null | 10.1007/JHEP05(2013)067 | UWO-TH-13/2 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We employ holographic techniques to study quantum quenches at finite
temperature, where the quenches involve varying the coupling of the boundary
theory to a relevant operator with an arbitrary conformal dimension
$2\leq\D\leq4$. The evolution of the system is studied by evaluating the
expectation value of the quench... | [
{
"created": "Tue, 12 Feb 2013 21:02:49 GMT",
"version": "v1"
}
] | 2015-06-15 | [
[
"Buchel",
"Alex",
""
],
[
"Lehner",
"Luis",
""
],
[
"Myers",
"Robert C.",
""
],
[
"van Niekerk",
"Anton",
""
]
] | We employ holographic techniques to study quantum quenches at finite temperature, where the quenches involve varying the coupling of the boundary theory to a relevant operator with an arbitrary conformal dimension $2\leq\D\leq4$. The evolution of the system is studied by evaluating the expectation value of the quenched... | 7.933571 | 7.698158 | 8.285944 | 7.38389 | 8.007262 | 7.842871 | 7.31403 | 7.482015 | 7.629966 | 8.816357 | 6.930333 | 7.203648 | 7.826005 | 7.275006 | 7.44293 | 7.439983 | 7.523638 | 7.438923 | 7.481714 | 7.738224 | 7.227932 |
1908.09570 | Shao-Jun Zhang | Haitang Li, Yong Chen and Shao-Jun Zhang | Photon orbits and phase transitions in Born-Infeld-dilaton black holes | 7 pages, 7 figures | null | 10.1016/j.nuclphysb.2020.114975 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Relations between photon orbits and thermodynamical phase transitions are
explored in Born-Infeld-dilaton-AdS black hole. The coupling between the
electromagnetic field and the dialton field is chosen such that the full phase
diagram contains zeroth-order and first-order phase transitions as well as RPT.
We find that... | [
{
"created": "Mon, 26 Aug 2019 09:52:12 GMT",
"version": "v1"
}
] | 2020-04-22 | [
[
"Li",
"Haitang",
""
],
[
"Chen",
"Yong",
""
],
[
"Zhang",
"Shao-Jun",
""
]
] | Relations between photon orbits and thermodynamical phase transitions are explored in Born-Infeld-dilaton-AdS black hole. The coupling between the electromagnetic field and the dialton field is chosen such that the full phase diagram contains zeroth-order and first-order phase transitions as well as RPT. We find that t... | 7.619534 | 7.616002 | 6.799734 | 6.627733 | 7.900699 | 7.883823 | 7.867728 | 6.864145 | 7.543814 | 7.585494 | 7.366981 | 7.511128 | 7.476945 | 7.510546 | 7.465518 | 7.73891 | 7.598931 | 7.554392 | 7.687863 | 7.803083 | 7.545352 |
hep-th/0310200 | Kerstin E. Kunze | Kerstin E. Kunze | Stochastic inflation on the brane | 9 pages | Phys.Lett. B587 (2004) 1-6 | 10.1016/j.physletb.2004.03.002 | null | hep-th astro-ph gr-qc | null | Chaotic inflation on the brane is considered in the context of stochastic
inflation. It is found that there is a regime in which eternal inflation on the
brane takes place. The corresponding probability distributions are found in
certain cases. The stationary probability distribution over a comoving volume
and the cr... | [
{
"created": "Tue, 21 Oct 2003 12:54:09 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Kunze",
"Kerstin E.",
""
]
] | Chaotic inflation on the brane is considered in the context of stochastic inflation. It is found that there is a regime in which eternal inflation on the brane takes place. The corresponding probability distributions are found in certain cases. The stationary probability distribution over a comoving volume and the crea... | 12.764894 | 12.871144 | 13.069718 | 11.878007 | 11.669708 | 12.253703 | 11.860943 | 11.304933 | 11.846131 | 12.591308 | 11.774778 | 12.269012 | 12.33567 | 11.983027 | 12.532255 | 11.684588 | 12.050317 | 12.39287 | 11.993745 | 11.739689 | 12.029752 |
2303.08159 | Hun Jang | Hun Jang | Gauge Theory on Fiber Bundle of Hypercomplex Algebras | 17 pages, 2 figures; v3: version published in Nucl. Phys. B 993
(2023) 116281 | Nucl. Phys. B 993 (2023) 116281 | 10.1016/j.nuclphysb.2023.116281 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | I introduce a way of constructing a fiber bundle whose fibers are given by
hypercomplex algebras and woven by appropriate structure group, and present
that a novel gauge theory can be built on the hypercomplex fiber bundle. In
this work, I aim to answer a question about how nature selects one preferred
vacuum among d... | [
{
"created": "Tue, 14 Mar 2023 18:21:05 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Jun 2023 16:05:02 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Jun 2023 04:14:20 GMT",
"version": "v3"
}
] | 2023-06-29 | [
[
"Jang",
"Hun",
""
]
] | I introduce a way of constructing a fiber bundle whose fibers are given by hypercomplex algebras and woven by appropriate structure group, and present that a novel gauge theory can be built on the hypercomplex fiber bundle. In this work, I aim to answer a question about how nature selects one preferred vacuum among deg... | 13.291666 | 14.062674 | 13.525833 | 13.25295 | 13.421041 | 13.972364 | 12.957483 | 13.440872 | 13.448468 | 13.459214 | 12.857217 | 13.112193 | 12.812589 | 12.418365 | 12.98556 | 12.800759 | 12.908858 | 12.495331 | 12.690816 | 13.136353 | 12.442025 |
1005.4680 | Oliver Rosten | Oliver J. Rosten | An Extension of Pohlmeyer's Theorem | v1: 29 pages; v2: 30 pages, minor tweaks; v3: published with very
minor changes | J.Phys.A43:495401,2010 | 10.1088/1751-8113/43/49/495401 | null | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Applying the Exact Renormalization Group to scalar field theory in Euclidean
space of general (not necessarily integer) dimension, it is proven that the
only fixed-point with vanishing anomalous dimension is the Gaussian one. The
proof requires positivity of the two-point connected correlation function
together with ... | [
{
"created": "Tue, 25 May 2010 20:00:27 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Aug 2010 20:02:15 GMT",
"version": "v2"
},
{
"created": "Sun, 21 Nov 2010 19:26:21 GMT",
"version": "v3"
}
] | 2011-03-28 | [
[
"Rosten",
"Oliver J.",
""
]
] | Applying the Exact Renormalization Group to scalar field theory in Euclidean space of general (not necessarily integer) dimension, it is proven that the only fixed-point with vanishing anomalous dimension is the Gaussian one. The proof requires positivity of the two-point connected correlation function together with a ... | 9.721544 | 9.041965 | 8.71515 | 8.142274 | 8.703006 | 8.726794 | 8.254459 | 8.689239 | 8.224911 | 9.652753 | 8.562385 | 8.232639 | 8.614015 | 8.186958 | 8.387721 | 8.373499 | 8.444212 | 8.388965 | 8.364601 | 8.811493 | 8.34322 |
hep-th/9204056 | null | Gerald Dunne and Roman Jackiw | Chern-Simons Solitons, Toda Theories and the Chiral Model | null | Commun.Math.Phys. 150 (1992) 519-535 | 10.1007/BF02096959 | null | hep-th | null | The two-dimensional self-dual Chern--Simons equations are equivalent to the
conditions for static, zero-energy solutions of the $(2+1)$-dimensional gauged
nonlinear Schr\"odinger equation with Chern--Simons matter-gauge dynamics. In
this paper we classify all finite charge $SU(N)$ solutions by first
transforming the ... | [
{
"created": "Fri, 17 Apr 1992 18:05:45 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dunne",
"Gerald",
""
],
[
"Jackiw",
"Roman",
""
]
] | The two-dimensional self-dual Chern--Simons equations are equivalent to the conditions for static, zero-energy solutions of the $(2+1)$-dimensional gauged nonlinear Schr\"odinger equation with Chern--Simons matter-gauge dynamics. In this paper we classify all finite charge $SU(N)$ solutions by first transforming the se... | 8.003062 | 6.253538 | 9.049288 | 6.870677 | 8.732699 | 6.210579 | 6.70509 | 7.065739 | 7.333532 | 9.637733 | 6.728789 | 7.241835 | 8.190697 | 7.435242 | 7.414811 | 7.707147 | 7.210115 | 7.373211 | 7.386744 | 8.217436 | 7.34779 |
0712.4086 | Alberto Iglesias | Gregory Gabadadze and Alberto Iglesias | Mass Screening in Modified Gravity | 16 pages, 4 figures, A contribution to the Proceedings of the
International Workshop on Cosmology and Gravitation, Peyresq 12, June 16-22,
2007, Peyresq, France | Class.Quant.Grav.25:154008,2008 | 10.1088/0264-9381/25/15/154008 | NYU-TH-07/12/01 | hep-th | null | Models of modified gravity introduce extra degrees of freedom, which for
consistency with the data, should be suppressed at observable scales. In the
models that share properties of massive gravity such a suppression is due to
nonlinear interactions: An isolated massive astrophysical object creates a halo
of a nonzer... | [
{
"created": "Wed, 26 Dec 2007 19:05:04 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gabadadze",
"Gregory",
""
],
[
"Iglesias",
"Alberto",
""
]
] | Models of modified gravity introduce extra degrees of freedom, which for consistency with the data, should be suppressed at observable scales. In the models that share properties of massive gravity such a suppression is due to nonlinear interactions: An isolated massive astrophysical object creates a halo of a nonzero ... | 15.608023 | 17.489424 | 15.286637 | 13.730244 | 15.980453 | 15.414648 | 16.486273 | 13.885016 | 15.354482 | 15.299107 | 14.366291 | 14.255311 | 14.66715 | 14.069249 | 15.050978 | 14.638322 | 13.984806 | 14.2864 | 14.062819 | 14.970368 | 14.530201 |
2103.15839 | David Meltzer | David Meltzer | Dispersion Formulas in QFTs, CFTs, and Holography | 63 pages plus appendices, 3 figures | null | 10.1007/JHEP05(2021)098 | CALT-TH-2021-012 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study momentum space dispersion formulas in general QFTs and their
applications for CFT correlation functions. We show, using two independent
methods, that QFT dispersion formulas can be written in terms of causal
commutators. The first derivation uses analyticity properties of retarded
correlators in momentum spa... | [
{
"created": "Mon, 29 Mar 2021 18:00:03 GMT",
"version": "v1"
}
] | 2021-07-23 | [
[
"Meltzer",
"David",
""
]
] | We study momentum space dispersion formulas in general QFTs and their applications for CFT correlation functions. We show, using two independent methods, that QFT dispersion formulas can be written in terms of causal commutators. The first derivation uses analyticity properties of retarded correlators in momentum space... | 7.658362 | 8.263511 | 8.566958 | 7.370456 | 8.171278 | 8.106977 | 8.124701 | 7.930185 | 7.252532 | 9.358934 | 7.506147 | 7.324399 | 7.890101 | 7.51112 | 7.691485 | 7.568077 | 7.629243 | 7.445532 | 7.529587 | 7.931055 | 7.370739 |
1607.03735 | Hayden Lee | Hayden Lee, Daniel Baumann, Guilherme L. Pimentel | Non-Gaussianity as a Particle Detector | 55 pages, 10 figures | null | 10.1007/JHEP12(2016)040 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the imprints of massive particles with spin on cosmological
correlators. Using the framework of the effective field theory of inflation, we
classify the couplings of these particles to the Goldstone boson of broken time
translations and the graviton. We show that it is possible to generate
observable non-Gau... | [
{
"created": "Wed, 13 Jul 2016 13:56:35 GMT",
"version": "v1"
}
] | 2016-12-23 | [
[
"Lee",
"Hayden",
""
],
[
"Baumann",
"Daniel",
""
],
[
"Pimentel",
"Guilherme L.",
""
]
] | We study the imprints of massive particles with spin on cosmological correlators. Using the framework of the effective field theory of inflation, we classify the couplings of these particles to the Goldstone boson of broken time translations and the graviton. We show that it is possible to generate observable non-Gauss... | 5.301116 | 4.780628 | 5.717744 | 4.700612 | 5.035336 | 4.50398 | 4.920873 | 4.7346 | 4.654082 | 5.71938 | 4.611532 | 4.692789 | 5.218627 | 5.038876 | 5.030346 | 4.851509 | 4.847518 | 4.823973 | 4.909127 | 4.981756 | 4.892404 |
1805.06467 | Jonathan Heckman | Jonathan J. Heckman and Tom Rudelius | Top Down Approach to 6D SCFTs | v4: 122 pages, 4 figures, further typos corrected | null | 10.1088/1751-8121/aafc81 | null | hep-th math.AG math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Six-dimensional superconformal field theories (6D SCFTs) occupy a central
place in the study of quantum field theories encountered in high energy theory.
This article reviews the top down construction and study of this rich class of
quantum field theories, in particular, how they are realized by suitable
backgrounds ... | [
{
"created": "Wed, 16 May 2018 18:00:08 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Jul 2018 22:24:10 GMT",
"version": "v2"
},
{
"created": "Wed, 20 Feb 2019 15:56:47 GMT",
"version": "v3"
},
{
"created": "Sat, 10 Aug 2019 23:43:04 GMT",
"version": "v4"
}
] | 2019-08-13 | [
[
"Heckman",
"Jonathan J.",
""
],
[
"Rudelius",
"Tom",
""
]
] | Six-dimensional superconformal field theories (6D SCFTs) occupy a central place in the study of quantum field theories encountered in high energy theory. This article reviews the top down construction and study of this rich class of quantum field theories, in particular, how they are realized by suitable backgrounds in... | 9.981794 | 9.813883 | 11.51435 | 10.065603 | 10.184404 | 10.125351 | 10.215111 | 9.898842 | 9.615494 | 11.029705 | 9.400039 | 9.339134 | 9.928418 | 9.739096 | 9.755466 | 9.666336 | 9.730365 | 9.435023 | 9.617729 | 9.623672 | 9.24865 |
1707.04751 | Prarit Agarwal | Prarit Agarwal, Antonio Sciarappa, Jaewon Song | N=1 Lagrangians for generalized Argyres-Douglas theories | 26 pages; v4: refs added | null | 10.1007/JHEP10(2017)211 | SNUTP17-003, KIAS-P17053 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find $\mathcal{N}=1$ Lagrangian gauge theories that flow to generalized
Argyres-Douglas theories with $\mathcal{N}=2$ supersymmetry. We find that
certain SU quiver gauge theories flow to generalized Argyres-Douglas theories
of type $(A_{k-1}, A_{mk-1})$ and $(I_{m, k m}, S)$. We also find quiver gauge
theories of ... | [
{
"created": "Sat, 15 Jul 2017 15:37:01 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Aug 2017 16:14:58 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Oct 2017 15:28:29 GMT",
"version": "v3"
},
{
"created": "Thu, 2 Nov 2017 01:10:35 GMT",
"version": "v4"
}
] | 2018-01-17 | [
[
"Agarwal",
"Prarit",
""
],
[
"Sciarappa",
"Antonio",
""
],
[
"Song",
"Jaewon",
""
]
] | We find $\mathcal{N}=1$ Lagrangian gauge theories that flow to generalized Argyres-Douglas theories with $\mathcal{N}=2$ supersymmetry. We find that certain SU quiver gauge theories flow to generalized Argyres-Douglas theories of type $(A_{k-1}, A_{mk-1})$ and $(I_{m, k m}, S)$. We also find quiver gauge theories of SO... | 4.904342 | 5.03651 | 5.822896 | 4.807047 | 4.80903 | 5.048161 | 5.686852 | 5.112884 | 4.944066 | 6.143767 | 5.11084 | 4.876824 | 5.553818 | 4.97451 | 4.954032 | 4.978715 | 4.914794 | 4.87553 | 4.943024 | 5.632465 | 4.955337 |
hep-th/0509184 | Sergei Winitzki | Jaume Garriga, Delia Schwartz-Perlov, Alexander Vilenkin, and Sergei
Winitzki | Probabilities in the inflationary multiverse | 18 pages, RevTeX 4, 2 figures. Discussion of the full probability in
Sec.VI is sharpened; the conclusions are strengthened. Note added explaining
the relation to recent work by Easther, Lim and Martin. Some references added | JCAP 0601:017,2006 | 10.1088/1475-7516/2006/01/017 | null | hep-th astro-ph gr-qc | null | Inflationary cosmology leads to the picture of a "multiverse," involving an
infinite number of (spatially infinite) post-inflationary thermalized regions,
called pocket universes. In the context of theories with many vacua, such as
the landscape of string theory, the effective constants of Nature are
randomized by qu... | [
{
"created": "Fri, 23 Sep 2005 19:45:19 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Oct 2005 01:44:38 GMT",
"version": "v2"
},
{
"created": "Sun, 27 Nov 2005 17:45:38 GMT",
"version": "v3"
}
] | 2011-05-05 | [
[
"Garriga",
"Jaume",
""
],
[
"Schwartz-Perlov",
"Delia",
""
],
[
"Vilenkin",
"Alexander",
""
],
[
"Winitzki",
"Sergei",
""
]
] | Inflationary cosmology leads to the picture of a "multiverse," involving an infinite number of (spatially infinite) post-inflationary thermalized regions, called pocket universes. In the context of theories with many vacua, such as the landscape of string theory, the effective constants of Nature are randomized by quan... | 9.355215 | 10.150866 | 8.751768 | 8.711153 | 10.183516 | 9.092571 | 10.267345 | 9.080613 | 9.350679 | 9.669424 | 8.845976 | 8.417139 | 8.336044 | 8.554437 | 8.532725 | 8.521005 | 8.711945 | 8.495614 | 8.509222 | 8.643826 | 8.355224 |
hep-th/9706010 | Hongsu Kim | Hongsu Kim (Ewha Women's Univ., Korea) | The Absence of Fermionic Superradiance (A Simple Demonstration) | 16 pages, Revtex | JCAP0811:007,2008 | 10.1088/1475-7516/2008/11/007 | null | hep-th gr-qc | null | Superradiant scattering, which can be thought of as the wave analogue of the
Penrose process is revisited. As is well-known, boson fields display
superradiance provided they have frequency in a certain range whereas fermion
fields do not. A succinct superradiance-checking algorithm employing particle
number or energy... | [
{
"created": "Mon, 2 Jun 1997 10:12:29 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kim",
"Hongsu",
"",
"Ewha Women's Univ., Korea"
]
] | Superradiant scattering, which can be thought of as the wave analogue of the Penrose process is revisited. As is well-known, boson fields display superradiance provided they have frequency in a certain range whereas fermion fields do not. A succinct superradiance-checking algorithm employing particle number or energy c... | 9.260589 | 9.077678 | 8.957969 | 8.621943 | 8.644416 | 9.26264 | 8.803432 | 8.32625 | 8.904564 | 9.091997 | 9.010425 | 8.826272 | 8.558998 | 8.532519 | 8.593865 | 9.122346 | 8.801682 | 8.518646 | 8.633372 | 8.368592 | 8.699603 |
hep-th/0201242 | Rafael de Lima Rodrigues | R. de Lima Rodrigues, W. Pires de Almeida and I. Fonseca Neto | Supersymmetric Classical Mechanics: Free Case | 13 pages, no figures | null | null | null | hep-th | null | We present a review work on Supersymmetric Classical Mechanics in the context
of a Lagrangian formalism, with $N=1-$supersymmetry. We show that the N=1
supersymmetry does not allow the introduction of a potential energy term
depending on a single commuting supercoordinate, $\phi (t;\Theta)$.
| [
{
"created": "Tue, 29 Jan 2002 20:13:17 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rodrigues",
"R. de Lima",
""
],
[
"de Almeida",
"W. Pires",
""
],
[
"Neto",
"I. Fonseca",
""
]
] | We present a review work on Supersymmetric Classical Mechanics in the context of a Lagrangian formalism, with $N=1-$supersymmetry. We show that the N=1 supersymmetry does not allow the introduction of a potential energy term depending on a single commuting supercoordinate, $\phi (t;\Theta)$. | 12.128473 | 10.936708 | 12.90172 | 11.482641 | 12.223724 | 13.285028 | 11.65129 | 10.946087 | 11.760377 | 12.987484 | 10.509774 | 10.668277 | 12.23256 | 10.643359 | 10.488707 | 10.75197 | 10.575821 | 10.848264 | 11.230111 | 12.407943 | 10.687546 |
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