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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2309.03938 | David Andriot | David Andriot, Dimitrios Tsimpis, Timm Wrase | Accelerated expansion of an open universe, and string theory
realizations | v2: 38 pages, few additions. As ancillary file we provide the
notebook allowing to reproduce all Figures, in particular the complete
cosmological solutions | null | null | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, many works have tried to realize cosmological accelerated expansion
in string theory models in the asymptotic regions of field space, with a
typical scalar potential $V(\varphi)$ having an exponential fall-off
$e^{-\gamma\, \varphi}$. Those attempts have been plagued by the fact that $V$
is too steep, namel... | [
{
"created": "Thu, 7 Sep 2023 18:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Nov 2023 08:53:18 GMT",
"version": "v2"
}
] | 2023-11-17 | [
[
"Andriot",
"David",
""
],
[
"Tsimpis",
"Dimitrios",
""
],
[
"Wrase",
"Timm",
""
]
] | Recently, many works have tried to realize cosmological accelerated expansion in string theory models in the asymptotic regions of field space, with a typical scalar potential $V(\varphi)$ having an exponential fall-off $e^{-\gamma\, \varphi}$. Those attempts have been plagued by the fact that $V$ is too steep, namely ... | 8.938134 | 8.073076 | 8.845311 | 7.961843 | 8.187241 | 8.134275 | 8.403478 | 7.909094 | 7.879178 | 9.572064 | 8.129272 | 8.10521 | 8.515026 | 8.346782 | 8.497024 | 8.424369 | 8.091274 | 8.2486 | 8.314336 | 8.499277 | 8.226123 |
2106.15184 | Fran\c{c}ois Rondeau | Ignatios Antoniadis, Chrysoula Markou, Fran\c{c}ois Rondeau | Aspects of compactification on a linear dilaton background | 50 pages. Published version | J. High Energ. Phys. 2021, 137 (2021) | 10.1007/JHEP09(2021)137 | MPP-2021-102 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the most general Kaluza-Klein (KK) compactification on
$S^1/\mathbb{Z}_2$ of a five dimensional ($5D$) graviton-dilaton system, with a
non-vanishing dilaton background varying linearly along the fifth dimension. We
show that this background produces a Higgs mechanism for the KK vector coming
from the $5D$... | [
{
"created": "Tue, 29 Jun 2021 09:02:47 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Sep 2021 13:24:19 GMT",
"version": "v2"
}
] | 2021-09-30 | [
[
"Antoniadis",
"Ignatios",
""
],
[
"Markou",
"Chrysoula",
""
],
[
"Rondeau",
"François",
""
]
] | We consider the most general Kaluza-Klein (KK) compactification on $S^1/\mathbb{Z}_2$ of a five dimensional ($5D$) graviton-dilaton system, with a non-vanishing dilaton background varying linearly along the fifth dimension. We show that this background produces a Higgs mechanism for the KK vector coming from the $5D$ m... | 6.517982 | 6.83905 | 7.221906 | 6.554556 | 6.803212 | 6.571768 | 6.772047 | 6.516552 | 6.504397 | 7.720832 | 6.447827 | 6.319002 | 6.729382 | 6.29546 | 6.472338 | 6.596485 | 6.516654 | 6.499631 | 6.404276 | 6.675581 | 6.386596 |
2304.10055 | Yutaka Hosotani | Yutaka Hosotani | Holography in anomaly flow in orbifold gauge theory | 17 pages, 7 figures, proceeding for Corfu Summer Institute 2022,
minor corrections in references | null | null | OU-HET-1179 | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | In orbifold gauge theory and gauge-Higgs unification models, gauge anomaly
flows with an Aharonov-Bohm phase $\theta_H$ in the fifth dimension. We analyze
$SU(2)$ gauge theory with doublet fermions in the flat $M^4 \times (S^1/Z_2)$
spacetime and in the Randall-Sundrum (RS) warped space. With orbifold boundary
condit... | [
{
"created": "Thu, 20 Apr 2023 02:39:15 GMT",
"version": "v1"
},
{
"created": "Wed, 24 May 2023 03:38:25 GMT",
"version": "v2"
}
] | 2023-05-25 | [
[
"Hosotani",
"Yutaka",
""
]
] | In orbifold gauge theory and gauge-Higgs unification models, gauge anomaly flows with an Aharonov-Bohm phase $\theta_H$ in the fifth dimension. We analyze $SU(2)$ gauge theory with doublet fermions in the flat $M^4 \times (S^1/Z_2)$ spacetime and in the Randall-Sundrum (RS) warped space. With orbifold boundary conditio... | 9.219721 | 9.470499 | 8.271843 | 8.348948 | 8.875357 | 9.141739 | 8.567699 | 9.0871 | 7.937357 | 8.632248 | 9.01049 | 9.14362 | 8.599622 | 8.555087 | 9.042429 | 9.144623 | 8.917822 | 8.999466 | 8.432837 | 8.745847 | 8.794113 |
2312.02127 | Diptarka Das | Diptarka Das, Santanu Mandal, Anurag Sarkar | Chaotic and Thermal Aspects in the Highly Excited String S-Matrix | 45 pages, 14 figures, References and numerical analysis updated,
presentation improved, matches JHEP accepted version | null | null | null | hep-th cond-mat.stat-mech nlin.CD | http://creativecommons.org/licenses/by/4.0/ | We compute tree level scattering amplitudes involving more than one highly
excited states and tachyons in bosonic string theory. We use these amplitudes
to understand chaotic and thermal aspects of the excited string states lending
support to the Susskind-Horowitz-Polchinski correspondence principle. The
unaveraged a... | [
{
"created": "Mon, 4 Dec 2023 18:53:39 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Dec 2023 18:33:48 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Aug 2024 14:46:44 GMT",
"version": "v3"
}
] | 2024-08-09 | [
[
"Das",
"Diptarka",
""
],
[
"Mandal",
"Santanu",
""
],
[
"Sarkar",
"Anurag",
""
]
] | We compute tree level scattering amplitudes involving more than one highly excited states and tachyons in bosonic string theory. We use these amplitudes to understand chaotic and thermal aspects of the excited string states lending support to the Susskind-Horowitz-Polchinski correspondence principle. The unaveraged amp... | 13.58223 | 12.247303 | 15.041177 | 11.892581 | 13.064126 | 12.128852 | 11.988042 | 11.071137 | 11.250419 | 14.749812 | 11.482869 | 11.904048 | 13.819463 | 12.561665 | 12.560331 | 12.105948 | 12.069719 | 12.360508 | 12.514132 | 13.928741 | 12.452147 |
2007.11333 | Flavio Tonioni | Susha Parameswaran, Flavio Tonioni | Non-supersymmetric String Models from Anti-D3-/D7-branes in Strongly
Warped Throats | 72 pages + 3 appendices + references, 3 figures; v2: JHEP version,
references and clarifications added, typos corrected; v3: corrections in app.
B.3 and sssec. 4.3.2 (with corresponding edits, main conclusions unchanged),
clarification in sssec. 5.1.1 | Journal of High Energy Physics volume 2020, Article number: 174
(2020) | 10.1007/JHEP12(2020)174 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article discusses model-building scenarios including anti-D3-/D7-branes,
in which supersymmetry is broken spontaneously, despite having no scale at
which sparticles appear and standard supersymmetry is restored. If the branes
are placed on singularities at the tip of warped throats in Calabi-Yau
orientifold flux... | [
{
"created": "Wed, 22 Jul 2020 10:44:07 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Feb 2021 10:43:31 GMT",
"version": "v2"
},
{
"created": "Thu, 5 May 2022 10:06:58 GMT",
"version": "v3"
}
] | 2022-05-06 | [
[
"Parameswaran",
"Susha",
""
],
[
"Tonioni",
"Flavio",
""
]
] | This article discusses model-building scenarios including anti-D3-/D7-branes, in which supersymmetry is broken spontaneously, despite having no scale at which sparticles appear and standard supersymmetry is restored. If the branes are placed on singularities at the tip of warped throats in Calabi-Yau orientifold flux c... | 10.900166 | 11.098834 | 11.992887 | 9.873449 | 10.247158 | 10.861043 | 10.881872 | 10.61576 | 10.290851 | 11.933054 | 10.291994 | 9.704703 | 10.87144 | 10.449973 | 10.325871 | 10.007051 | 10.179806 | 10.18311 | 10.100497 | 10.672219 | 10.353283 |
2205.11339 | Yuya Tanizaki | Yuya Tanizaki, Mithat \"Unsal | Semiclassics with 't Hooft flux background for QCD with $2$-index quarks | 24 pages, no figure | JHEP 08 (2022) 038 | 10.1007/JHEP08(2022)038 | YITP-22-45 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study quantum chromodynamics including the two-index symmetric or
anti-symmetric quark (QCD(Sym/ASym)) on small $\mathbb{R}^2\times T^2$ with a
suitable magnetic flux. We first discuss the 't Hooft anomaly of these theories
and claim that discrete chiral symmetry should be spontaneously broken
completely to satisf... | [
{
"created": "Mon, 23 May 2022 14:32:39 GMT",
"version": "v1"
},
{
"created": "Fri, 27 May 2022 22:07:08 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Jun 2022 23:29:43 GMT",
"version": "v3"
}
] | 2022-08-05 | [
[
"Tanizaki",
"Yuya",
""
],
[
"Ünsal",
"Mithat",
""
]
] | We study quantum chromodynamics including the two-index symmetric or anti-symmetric quark (QCD(Sym/ASym)) on small $\mathbb{R}^2\times T^2$ with a suitable magnetic flux. We first discuss the 't Hooft anomaly of these theories and claim that discrete chiral symmetry should be spontaneously broken completely to satisfy ... | 7.754223 | 7.295764 | 8.486184 | 6.976847 | 7.200711 | 7.388083 | 6.867249 | 6.938704 | 6.815646 | 8.855458 | 6.7648 | 7.210409 | 7.746615 | 7.104448 | 7.156145 | 7.002373 | 7.027937 | 6.963399 | 7.093486 | 7.555974 | 7.068916 |
2311.14432 | Mathieu Giroux | Giacomo Brunello, Giulio Crisanti, Mathieu Giroux, Pierpaolo
Mastrolia, Sid Smith | Fourier Calculus from Intersection Theory | 15 pages and 3 figures, matching the published version | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Building on recent advances in studying the co-homological properties of
Feynman integrals, we apply intersection theory to the computation of Fourier
integrals. We discuss applications pertinent to gravitational bremsstrahlung
and deep inelastic scattering in the saturation regime. After identifying the
bases of mas... | [
{
"created": "Fri, 24 Nov 2023 12:18:17 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Apr 2024 12:42:27 GMT",
"version": "v2"
}
] | 2024-04-11 | [
[
"Brunello",
"Giacomo",
""
],
[
"Crisanti",
"Giulio",
""
],
[
"Giroux",
"Mathieu",
""
],
[
"Mastrolia",
"Pierpaolo",
""
],
[
"Smith",
"Sid",
""
]
] | Building on recent advances in studying the co-homological properties of Feynman integrals, we apply intersection theory to the computation of Fourier integrals. We discuss applications pertinent to gravitational bremsstrahlung and deep inelastic scattering in the saturation regime. After identifying the bases of maste... | 14.561944 | 12.895373 | 13.739892 | 11.250784 | 12.831851 | 12.675982 | 13.056418 | 12.253676 | 12.08127 | 14.164546 | 12.818647 | 13.333353 | 12.538943 | 12.870079 | 13.095832 | 14.329699 | 13.465936 | 13.19508 | 13.189154 | 12.816444 | 13.458314 |
hep-th/0106273 | Andrei A. Galiautdinov | Andrei A. Galiautdinov and David R. Finkelstein (Georgia Institute of
Technology) | Chronon corrections to the Dirac equation | 14 pages, no figures. Accepted to J.Math.Phys | null | 10.1063/1.1505666 | null | hep-th | null | The Dirac equation is not semisimple. We therefore regard it as a contraction
of a simpler decontracted theory. The decontracted theory is necessarily purely
algebraic and non-local. In one simple model the algebra is a Clifford algebra
with 6N generators. The quantum imaginary $\hbar i$ is the contraction of a
dynam... | [
{
"created": "Thu, 28 Jun 2001 17:24:47 GMT",
"version": "v1"
},
{
"created": "Sat, 29 Jun 2002 00:24:58 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Galiautdinov",
"Andrei A.",
"",
"Georgia Institute of\n Technology"
],
[
"Finkelstein",
"David R.",
"",
"Georgia Institute of\n Technology"
]
] | The Dirac equation is not semisimple. We therefore regard it as a contraction of a simpler decontracted theory. The decontracted theory is necessarily purely algebraic and non-local. In one simple model the algebra is a Clifford algebra with 6N generators. The quantum imaginary $\hbar i$ is the contraction of a dynamic... | 16.542053 | 17.943138 | 15.724772 | 14.880201 | 18.807775 | 16.356506 | 17.061041 | 15.919526 | 16.265558 | 17.555128 | 15.563911 | 15.339732 | 15.284205 | 15.261022 | 15.480292 | 15.601274 | 15.754449 | 15.938397 | 15.947159 | 16.160519 | 15.516215 |
hep-th/0507165 | Emil M. Prodanov | Rossen I. Ivanov and Emil M. Prodanov | Haunted Kaluza Universe with Four-dimensional Lorentzian Flat, Kerr, and
Taub-NUT Slices | 11 pages | Phys.Lett. B609 (2005) 1-6 | 10.1016/j.physletb.2005.01.036 | null | hep-th | null | The duality between the original Kaluza's theory and Klein's subsequent
modification is duality between slicing and threading decomposition of the
five-dimensional spacetime. The field equations of the original Kaluza's theory
lead to the interpretation of the four-dimensional Lorentzian Kerr and
Taub--NUT solutions ... | [
{
"created": "Mon, 18 Jul 2005 09:31:06 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Ivanov",
"Rossen I.",
""
],
[
"Prodanov",
"Emil M.",
""
]
] | The duality between the original Kaluza's theory and Klein's subsequent modification is duality between slicing and threading decomposition of the five-dimensional spacetime. The field equations of the original Kaluza's theory lead to the interpretation of the four-dimensional Lorentzian Kerr and Taub--NUT solutions as... | 19.124605 | 19.660269 | 17.083317 | 18.33765 | 19.550922 | 18.667135 | 19.265238 | 18.721502 | 18.686014 | 18.051559 | 19.144262 | 18.303345 | 18.270927 | 17.934824 | 18.278879 | 18.154394 | 19.108902 | 17.484766 | 19.481234 | 18.637976 | 18.469862 |
hep-th/0402124 | Oren Bergman Dr. | Oren Bergman and Shlomo S. Razamat (Technion) | Imaginary time D-branes to all orders | 19 pages, 5 figures | JHEP 0406:046,2004 | 10.1088/1126-6708/2004/06/046 | null | hep-th | null | Extending the work of Gaiotto, Itzhaki and Rastelli in hep-th/0304192, we
derive a general prescription for computing amplitudes involving a periodic
array of D-branes in imaginary time to arbitrary order. We use this
prescription to show that closed string amplitudes with b boundaries are
identical to closed string ... | [
{
"created": "Tue, 17 Feb 2004 10:28:24 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Bergman",
"Oren",
"",
"Technion"
],
[
"Razamat",
"Shlomo S.",
"",
"Technion"
]
] | Extending the work of Gaiotto, Itzhaki and Rastelli in hep-th/0304192, we derive a general prescription for computing amplitudes involving a periodic array of D-branes in imaginary time to arbitrary order. We use this prescription to show that closed string amplitudes with b boundaries are identical to closed string am... | 9.268991 | 9.665863 | 10.500479 | 8.909674 | 9.534389 | 9.36888 | 8.649576 | 9.266183 | 9.1695 | 11.588463 | 8.456589 | 8.618992 | 9.035092 | 8.530302 | 8.664073 | 8.61605 | 8.881204 | 8.651931 | 8.641002 | 9.237353 | 8.794059 |
hep-th/9403051 | Denis Juriev | D.Juriev (D.V.Yur'ev) | Algebraic Structures of Quantum Projective Field Theory Related to
Fusion and Braiding. Hidden Additive Weight | AMS-TEX, amsppt style, 16 pages, accepted for a publication in
J.MATH.PHYS. (Typographical errors are excluded) | J.Math.Phys. 35 (1994) 3368-3379 | 10.1063/1.530473 | null | hep-th | null | The interaction of various algebraic structures describing fusion, braiding
and group symmetries in quantum projective field theory is an object of an
investigation in the paper. Structures of projective Zamolodchikov al- gebras,
their represntations, spherical correlation functions, correlation characters
and envelo... | [
{
"created": "Tue, 8 Mar 1994 12:49:49 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Mar 1994 10:01:31 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Juriev",
"D.",
"",
"D.V.Yur'ev"
]
] | The interaction of various algebraic structures describing fusion, braiding and group symmetries in quantum projective field theory is an object of an investigation in the paper. Structures of projective Zamolodchikov al- gebras, their represntations, spherical correlation functions, correlation characters and envelopp... | 18.462801 | 18.879343 | 21.222719 | 17.86224 | 19.277262 | 21.783731 | 20.838913 | 19.706818 | 18.562662 | 22.741936 | 19.181858 | 18.223261 | 19.342722 | 17.893547 | 18.407022 | 18.891752 | 17.935909 | 18.029228 | 18.002451 | 19.32217 | 17.540905 |
2004.10647 | Emilio Torrente-Lujan | A. Belhaj, A. El Balali, W. El Hadri, Y. Hassouni, and E.
Torrente-Lujan | Phase Transitions of Quintessential AdS Black Holes in
M-theory/Superstring Inspired Models | null | null | 10.1142/S0217751X21500573 | FISPAC-TH/20-31415, UQBAR-TH/20-27182 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $d$-dimensional $AdS$ black holes surrounded by Dark Energy (DE),
embedded in $D$-dimensional M-theory/superstring inspired models having $AdS_d
\times \mathbb{S}^{d+k}$ space-time with $D=2d+k$. We focus on the
thermodynamic Hawking-Page phase transitions of quintessential DE black hole
solutions, whose mic... | [
{
"created": "Wed, 22 Apr 2020 15:44:44 GMT",
"version": "v1"
}
] | 2021-04-21 | [
[
"Belhaj",
"A.",
""
],
[
"Balali",
"A. El",
""
],
[
"Hadri",
"W. El",
""
],
[
"Hassouni",
"Y.",
""
],
[
"Torrente-Lujan",
"E.",
""
]
] | We study $d$-dimensional $AdS$ black holes surrounded by Dark Energy (DE), embedded in $D$-dimensional M-theory/superstring inspired models having $AdS_d \times \mathbb{S}^{d+k}$ space-time with $D=2d+k$. We focus on the thermodynamic Hawking-Page phase transitions of quintessential DE black hole solutions, whose micro... | 10.039513 | 10.614511 | 9.695281 | 8.771579 | 9.594911 | 9.937426 | 10.042249 | 9.498958 | 9.765098 | 11.370768 | 10.063806 | 9.755244 | 9.708723 | 9.287094 | 9.885028 | 9.776825 | 9.956427 | 9.899097 | 9.621988 | 10.312728 | 9.471155 |
hep-th/0609148 | Cosmas Zachos | Cosmas K Zachos | A Classical Bound on Quantum Entropy | Latex2e, 7 pages, publication version | J.Phys.A40:F407-F412,2007 | 10.1088/1751-8113/40/21/F02 | ANL-HEP-PR-06-74 | hep-th gr-qc physics.comp-ph quant-ph | null | A classical upper bound for quantum entropy is identified and illustrated,
$0\leq S_q \leq \ln (e \sigma^2 / 2\hbar)$, involving the variance $\sigma^2$
in phase space of the classical limit distribution of a given system. A
fortiori, this further bounds the corresponding information-theoretical
generalizations of th... | [
{
"created": "Thu, 21 Sep 2006 19:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Dec 2006 16:09:55 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Feb 2007 21:40:16 GMT",
"version": "v3"
},
{
"created": "Thu, 5 Apr 2007 14:49:20 GMT",
"version": "v4"
},
{
"cre... | 2008-11-26 | [
[
"Zachos",
"Cosmas K",
""
]
] | A classical upper bound for quantum entropy is identified and illustrated, $0\leq S_q \leq \ln (e \sigma^2 / 2\hbar)$, involving the variance $\sigma^2$ in phase space of the classical limit distribution of a given system. A fortiori, this further bounds the corresponding information-theoretical generalizations of the ... | 16.038277 | 13.001701 | 13.260957 | 14.00126 | 13.944025 | 15.792971 | 14.330939 | 16.374975 | 15.382776 | 15.273904 | 14.654654 | 12.646038 | 13.552557 | 12.421803 | 12.424031 | 12.887293 | 13.002058 | 13.12326 | 12.283296 | 13.105074 | 13.67842 |
1105.4792 | Ivica Smoli\'c | Loriano Bonora, Maro Cvitan, Predrag Dominis Prester, Silvio Pallua,
Ivica Smoli\'c | Gravitational Chern-Simons Lagrangian terms and spherically symmetric
spacetimes | 16 pages, updated to match published version | Class.Quant.Grav.28:195009,2011 | 10.1088/0264-9381/28/19/195009 | SISSA 23/2011/EP, ZTF-11-05 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that for general spherically symmetric configurations, contributions
of general gravitational and mixed gauge-gravitational Chern-Simons terms to
the equations of motion vanish identically in $D>3$ dimensions. This implies
that such terms in the action do not affect Birkhoff's theorem or any
previously known ... | [
{
"created": "Tue, 24 May 2011 14:57:53 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Jun 2011 10:13:41 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Feb 2012 09:56:57 GMT",
"version": "v3"
}
] | 2012-02-06 | [
[
"Bonora",
"Loriano",
""
],
[
"Cvitan",
"Maro",
""
],
[
"Prester",
"Predrag Dominis",
""
],
[
"Pallua",
"Silvio",
""
],
[
"Smolić",
"Ivica",
""
]
] | We show that for general spherically symmetric configurations, contributions of general gravitational and mixed gauge-gravitational Chern-Simons terms to the equations of motion vanish identically in $D>3$ dimensions. This implies that such terms in the action do not affect Birkhoff's theorem or any previously known sp... | 10.148884 | 11.091766 | 9.762526 | 9.99178 | 11.039378 | 11.359904 | 11.161324 | 10.239385 | 10.189475 | 10.956514 | 9.855926 | 10.021722 | 9.978361 | 9.577244 | 9.925118 | 10.068973 | 10.193387 | 9.772243 | 9.694239 | 9.622169 | 9.775074 |
2101.06325 | Keiju Murata Dr | Takaaki Ishii, Keiju Murata, Jorge E. Santos, Benson Way | Multioscillating black holes | 40 pages, 8 figures | null | 10.1007/JHEP05(2021)011 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study rotating global AdS solutions in five-dimensional Einstein gravity
coupled to a multiplet complex scalar within a cohomogeneity-1 ansatz. The
onset of the gravitational and scalar field superradiant instabilities of the
Myers-Perry-AdS black hole mark bifurcation points to black resonators and
hairy Myers-Pe... | [
{
"created": "Fri, 15 Jan 2021 23:23:27 GMT",
"version": "v1"
}
] | 2021-05-19 | [
[
"Ishii",
"Takaaki",
""
],
[
"Murata",
"Keiju",
""
],
[
"Santos",
"Jorge E.",
""
],
[
"Way",
"Benson",
""
]
] | We study rotating global AdS solutions in five-dimensional Einstein gravity coupled to a multiplet complex scalar within a cohomogeneity-1 ansatz. The onset of the gravitational and scalar field superradiant instabilities of the Myers-Perry-AdS black hole mark bifurcation points to black resonators and hairy Myers-Perr... | 10.212807 | 10.077465 | 10.358653 | 8.959039 | 10.191324 | 9.75061 | 9.833064 | 9.298676 | 9.486621 | 9.906449 | 9.843225 | 9.813788 | 9.575534 | 9.675637 | 9.894916 | 9.994266 | 9.819961 | 9.684035 | 9.553212 | 9.511542 | 9.759354 |
2312.12517 | Urs Schreiber | Hisham Sati and Urs Schreiber | Flux Quantization on Phase Space | 23 pages; v3: published version, with a little more background added
to section 3.1; v2: more references added & typos fixed | Annales Henri Poincar\'e (2024) | 10.1007/s00023-024-01438-x | null | hep-th math-ph math.AT math.DG math.KT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | While it has become widely appreciated that (higher) gauge theories need,
besides their variational phase space data, to be equipped with "flux
quantization laws" in generalized differential cohomology, there used to be no
general prescription for how to define and construct the resulting
flux-quantized phase space s... | [
{
"created": "Tue, 19 Dec 2023 19:00:04 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Dec 2023 17:50:05 GMT",
"version": "v2"
},
{
"created": "Wed, 8 May 2024 15:11:00 GMT",
"version": "v3"
}
] | 2024-05-09 | [
[
"Sati",
"Hisham",
""
],
[
"Schreiber",
"Urs",
""
]
] | While it has become widely appreciated that (higher) gauge theories need, besides their variational phase space data, to be equipped with "flux quantization laws" in generalized differential cohomology, there used to be no general prescription for how to define and construct the resulting flux-quantized phase space sta... | 14.594532 | 16.041616 | 17.711136 | 14.692567 | 17.046333 | 16.922632 | 15.795507 | 15.57795 | 14.578875 | 17.838425 | 14.38919 | 14.633336 | 13.663798 | 14.468708 | 14.165288 | 14.350513 | 13.872291 | 13.630786 | 13.506249 | 15.677508 | 14.501793 |
hep-th/0207030 | Tonguc Rador | Tonguc Rador | Uniting Gross-Neveu and Massive Schwinger Models | Version to appear in Phys. Lett. B | Phys.Lett. B546 (2002) 153-156 | 10.1016/S0370-2693(02)02692-8 | null | hep-th | null | We show that it is possible to obtain the Gross-Neveu model in 1+1 dimensions
from gauge fields only. This is reminiscent of the fact that in 1+1 dimensions
the gauge field tensor is essentially a pseudo-scalar. We also show that it is
possible in this context to combine the Gross-Neveu model with the massive
Schwing... | [
{
"created": "Wed, 3 Jul 2002 09:24:59 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jul 2002 09:34:16 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Jul 2002 07:42:18 GMT",
"version": "v3"
},
{
"created": "Thu, 19 Sep 2002 11:04:42 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Rador",
"Tonguc",
""
]
] | We show that it is possible to obtain the Gross-Neveu model in 1+1 dimensions from gauge fields only. This is reminiscent of the fact that in 1+1 dimensions the gauge field tensor is essentially a pseudo-scalar. We also show that it is possible in this context to combine the Gross-Neveu model with the massive Schwinger... | 6.108285 | 5.255128 | 5.420863 | 5.454526 | 5.125025 | 5.461627 | 5.118025 | 5.552069 | 5.227856 | 6.409207 | 5.36561 | 5.609072 | 5.573267 | 5.517692 | 5.462042 | 5.5051 | 5.548824 | 5.370809 | 5.299575 | 5.694192 | 5.395758 |
hep-th/9309136 | null | Daniel Armand-Ugon, Rodolfo Gambini, Pablo Mora | Intersecting Braids and Intersecting Knot Theory | 14 pages (6 figures included) | J.Knot Theor.Ramifications 4:1-12,1995 | null | IFFC-93-06 | hep-th math.QA | null | An extension of the Artin Braid Group with new operators that generate double
and triple intersections is considered. The extended Alexander theorem,
relating intersecting closed braids and intersecting knots is proved for double
and triple intersections, and a counter example is given for the case of
quadruple inter... | [
{
"created": "Fri, 24 Sep 1993 21:03:26 GMT",
"version": "v1"
}
] | 2009-09-01 | [
[
"Armand-Ugon",
"Daniel",
""
],
[
"Gambini",
"Rodolfo",
""
],
[
"Mora",
"Pablo",
""
]
] | An extension of the Artin Braid Group with new operators that generate double and triple intersections is considered. The extended Alexander theorem, relating intersecting closed braids and intersecting knots is proved for double and triple intersections, and a counter example is given for the case of quadruple interse... | 12.712774 | 11.307687 | 12.210043 | 11.045658 | 12.863346 | 11.121156 | 11.573964 | 10.988373 | 11.813434 | 13.60868 | 11.060682 | 11.805367 | 11.45579 | 10.889671 | 11.26763 | 11.271474 | 10.9781 | 11.172336 | 11.333663 | 11.177166 | 11.155939 |
1906.03865 | Suguru Okumura | Takaaki Ishii, Suguru Okumura, Jun-ichi Sakamoto and Kentaroh Yoshida | Gravitational perturbations as $T\bar{T}$-deformations in 2D dilaton
gravity systems | 24 pages, references added | null | null | KUNS-2765, YITP-19-48 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider gravitational perturbations of 2D dilaton gravity systems and
show that these can be recast into $T\bar{T}$-deformations (at least) under
certain conditions, where $T$ means the energy-momentum tensor of the matter
field coupled to a dilaton gravity. In particular, the class of theories under
this conditi... | [
{
"created": "Mon, 10 Jun 2019 09:32:50 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Jul 2019 08:48:03 GMT",
"version": "v2"
}
] | 2019-07-04 | [
[
"Ishii",
"Takaaki",
""
],
[
"Okumura",
"Suguru",
""
],
[
"Sakamoto",
"Jun-ichi",
""
],
[
"Yoshida",
"Kentaroh",
""
]
] | We consider gravitational perturbations of 2D dilaton gravity systems and show that these can be recast into $T\bar{T}$-deformations (at least) under certain conditions, where $T$ means the energy-momentum tensor of the matter field coupled to a dilaton gravity. In particular, the class of theories under this condition... | 6.138834 | 6.564831 | 7.175953 | 6.64086 | 6.356679 | 6.578446 | 6.591876 | 6.654527 | 6.551937 | 8.837418 | 6.239684 | 6.457416 | 6.328134 | 5.988471 | 6.006611 | 6.177681 | 6.12539 | 6.090625 | 5.960088 | 6.308077 | 6.084893 |
hep-th/9702084 | Julie Blum | Julie D. Blum | H-Dyons and S-Duality | 16 pages, uses harvmac.tex, arguments are drastically changed but the
conclusions remain unchanged | Nucl.Phys.B507:245-258,1997 | 10.1016/S0550-3213(97)00547-6 | IASSNS-HEP-97/8 | hep-th | null | We present a relatively simple argument showing that the H-dyon states
required by S-duality of the heterotic string on $T^6$ are present provided
that the BPS dyons required by S-duality of N=4 supersymmetric Yang-Mills
theory are present. We also conjecture and provide evidence that H-dyons at
singularities where t... | [
{
"created": "Mon, 10 Feb 1997 18:25:45 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Mar 1997 05:51:05 GMT",
"version": "v2"
}
] | 2009-08-18 | [
[
"Blum",
"Julie D.",
""
]
] | We present a relatively simple argument showing that the H-dyon states required by S-duality of the heterotic string on $T^6$ are present provided that the BPS dyons required by S-duality of N=4 supersymmetric Yang-Mills theory are present. We also conjecture and provide evidence that H-dyons at singularities where the... | 10.024069 | 7.850383 | 10.415624 | 8.035974 | 9.083889 | 8.516238 | 8.227797 | 7.728807 | 7.676595 | 11.407537 | 8.155575 | 8.674898 | 9.075031 | 8.590846 | 8.794999 | 8.589108 | 7.878537 | 8.668665 | 8.628527 | 9.00761 | 8.877967 |
hep-th/9507024 | Jose M. Figueroa-O'Farrill | JM Figueroa-O'Farrill | Are all TCFTs obtained by twisting N=2 SCFTs? | 9 pages (5 physical pages), .dvi.uu (+ some hyperlinks) added some
references (my apologies) | null | null | QMW-PH-95-18 | hep-th | null | A large class of two-dimensional topological conformal field theories (TCFTs)
are obtained by the twisting construction of Witten and Eguchi-Yang. However
there seem to exist TCFTs which are not obtained in this way; for instance,
TCFTs obtained from the Kazama algebra and critical string theories with
generic backgr... | [
{
"created": "Wed, 5 Jul 1995 12:18:26 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Jul 1995 22:10:15 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Figueroa-O'Farrill",
"JM",
""
]
] | A large class of two-dimensional topological conformal field theories (TCFTs) are obtained by the twisting construction of Witten and Eguchi-Yang. However there seem to exist TCFTs which are not obtained in this way; for instance, TCFTs obtained from the Kazama algebra and critical string theories with generic backgrou... | 8.135552 | 8.521044 | 8.859673 | 7.274084 | 7.74755 | 7.584239 | 7.842141 | 7.522769 | 7.689474 | 9.100733 | 7.344834 | 7.50877 | 7.678376 | 7.469186 | 7.466523 | 7.500909 | 7.271388 | 7.504177 | 7.47732 | 7.582183 | 7.367133 |
1012.5930 | Hiroyuki Kitamoto | Hiroyuki Kitamoto, Yoshihisa Kitazawa | Non-linear sigma model in de Sitter space | 34pages | Phys.Rev.D83:104043,2011 | 10.1103/PhysRevD.83.104043 | KEK-TH-1430 | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate infra-red dynamics of the non-linear sigma model in de Sitter
space. In the presence of minimally coupled massless scalar fields, the de
Sitter symmetry is dynamically broken and physical constants become time
dependent. We find that the coupling constant of the non-linear sigma model
becomes time depe... | [
{
"created": "Wed, 29 Dec 2010 12:44:56 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Jan 2011 06:51:08 GMT",
"version": "v2"
},
{
"created": "Thu, 22 Sep 2011 17:47:48 GMT",
"version": "v3"
}
] | 2011-09-23 | [
[
"Kitamoto",
"Hiroyuki",
""
],
[
"Kitazawa",
"Yoshihisa",
""
]
] | We investigate infra-red dynamics of the non-linear sigma model in de Sitter space. In the presence of minimally coupled massless scalar fields, the de Sitter symmetry is dynamically broken and physical constants become time dependent. We find that the coupling constant of the non-linear sigma model becomes time depend... | 6.655883 | 6.692067 | 6.890213 | 6.064011 | 6.237623 | 6.420334 | 6.291368 | 6.414324 | 6.452091 | 7.28024 | 6.651614 | 6.510977 | 6.455636 | 6.489838 | 6.622707 | 6.556644 | 6.548851 | 6.469907 | 6.527365 | 6.505895 | 6.417923 |
hep-th/0302192 | Takemichi Okui | Lawrence J. Hall, Yasunori Nomura, Takemichi Okui, Steven J. Oliver | Explicit Supersymmetry Breaking on Boundaries of Warped Extra Dimensions | 30 pages, version to appear in Nucl. Phys. B | Nucl.Phys.B677:87-114,2004 | 10.1016/j.nuclphysb.2003.10.042 | null | hep-th hep-ph | null | Explicit supersymmetry breaking is studied in higher dimensional theories by
having boundaries respect only a subgroup of the bulk symmetry. If the boundary
symmetry is the maximal subgroup allowed by the boundary conditions imposed on
the fields, then the symmetry can be consistently gauged; otherwise gauging
leads ... | [
{
"created": "Tue, 25 Feb 2003 05:17:05 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Oct 2003 22:57:12 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Hall",
"Lawrence J.",
""
],
[
"Nomura",
"Yasunori",
""
],
[
"Okui",
"Takemichi",
""
],
[
"Oliver",
"Steven J.",
""
]
] | Explicit supersymmetry breaking is studied in higher dimensional theories by having boundaries respect only a subgroup of the bulk symmetry. If the boundary symmetry is the maximal subgroup allowed by the boundary conditions imposed on the fields, then the symmetry can be consistently gauged; otherwise gauging leads to... | 10.172894 | 10.681705 | 10.610972 | 10.210032 | 10.833591 | 12.390726 | 10.585627 | 10.859738 | 9.974184 | 10.850512 | 10.115355 | 10.341352 | 10.03511 | 9.798699 | 10.119448 | 10.258945 | 10.34829 | 10.014063 | 10.151761 | 10.344696 | 10.319957 |
0808.2728 | David D. K. Chow | David D. K. Chow | Charged rotating black holes in six-dimensional gauged supergravity | 9 pages; v2: minor changes | Class.Quant.Grav.27:065004,2010 | 10.1088/0264-9381/27/6/065004 | DAMTP-2008-73 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain non-extremal charged rotating black holes in six-dimensional SU(2)
gauged supergravity with two independent angular momenta and one U(1) charge.
These include supersymmetric black holes without naked closed timelike curves.
| [
{
"created": "Wed, 20 Aug 2008 15:20:58 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Feb 2010 21:34:14 GMT",
"version": "v2"
}
] | 2010-05-28 | [
[
"Chow",
"David D. K.",
""
]
] | We obtain non-extremal charged rotating black holes in six-dimensional SU(2) gauged supergravity with two independent angular momenta and one U(1) charge. These include supersymmetric black holes without naked closed timelike curves. | 8.014482 | 5.050982 | 7.966417 | 5.623988 | 6.044261 | 5.701419 | 5.374049 | 5.500887 | 5.400857 | 8.548429 | 5.431362 | 6.553367 | 8.774532 | 6.833272 | 6.79244 | 7.027514 | 6.75783 | 6.565759 | 6.829788 | 8.188834 | 6.124602 |
hep-th/0507018 | Neil D. Lambert | Neil D. Lambert and Gregory W. Moore | Distinguishing Off-Shell Supergravities With On-Shell Physics | References added | Phys.Rev. D72 (2005) 085018 | 10.1103/PhysRevD.72.085018 | null | hep-th | null | We show that it is possible to distinguish between different off-shell
completions of supergravity at the on-shell level. We focus on the comparison
of the ``new minimal'' formulation of off-shell four-dimensional N=1
supergravity with the ``old minimal'' formulation. We show that there are
3-manifolds which admit su... | [
{
"created": "Fri, 1 Jul 2005 19:08:26 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Aug 2005 19:03:23 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Oct 2005 16:26:16 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Lambert",
"Neil D.",
""
],
[
"Moore",
"Gregory W.",
""
]
] | We show that it is possible to distinguish between different off-shell completions of supergravity at the on-shell level. We focus on the comparison of the ``new minimal'' formulation of off-shell four-dimensional N=1 supergravity with the ``old minimal'' formulation. We show that there are 3-manifolds which admit supe... | 6.969387 | 6.588679 | 7.397903 | 6.478605 | 6.448069 | 6.364699 | 6.458692 | 6.159291 | 6.392246 | 8.339119 | 6.450431 | 6.396816 | 7.103116 | 6.573088 | 6.325838 | 6.533997 | 6.422754 | 6.401444 | 6.817125 | 7.076685 | 6.396114 |
hep-th/0002156 | Karin Bautier | K. Bautier, F. Englert, M. Rooman and Ph. Spindel | The Fefferman-Graham Ambiguity and AdS Black Holes | Latex, 14 pages; one reference modified, minor misprints corrected | Phys.Lett. B479 (2000) 291-298 | 10.1016/S0370-2693(00)00339-7 | ULB-TH-00/03,UMH-MG-00/01 | hep-th gr-qc | null | Asymptotically anti-de Sitter space-times in pure gravity with negative
cosmological constant are described, in all space-time dimensions greater than
two, by classical degrees of freedom on the conformal boundary at space-like
infinity. Their effective boundary action has a conformal anomaly for even
dimensions and ... | [
{
"created": "Fri, 18 Feb 2000 15:33:49 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Mar 2000 15:22:30 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Bautier",
"K.",
""
],
[
"Englert",
"F.",
""
],
[
"Rooman",
"M.",
""
],
[
"Spindel",
"Ph.",
""
]
] | Asymptotically anti-de Sitter space-times in pure gravity with negative cosmological constant are described, in all space-time dimensions greater than two, by classical degrees of freedom on the conformal boundary at space-like infinity. Their effective boundary action has a conformal anomaly for even dimensions and is... | 8.359075 | 8.665437 | 8.993761 | 7.823874 | 8.285132 | 8.531609 | 8.653955 | 8.173246 | 8.080022 | 9.304523 | 8.062315 | 7.69686 | 7.836465 | 7.677659 | 7.83496 | 7.713966 | 7.800388 | 7.821665 | 8.259452 | 7.925711 | 7.832578 |
1902.07211 | James Edwards Prof | James P. Edwards and Mariana Kirchbach | Massless Rarita-Schwinger field from a divergenceless
anti-symmetric-tensor spinor of pure spin-$3/2$ | 18 pages. Updated to journal version | International Journal of Modern Physics A Vol. 34, No. 11, 1950060
(2019) | 10.1142/S0217751X1950060X | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the Rarita-Schwinger basis vectors, $U^\mu$, spanning the direct
product space, $U^\mu:=A^\mu\otimes u_M$, of a massless four-vector, $ A^\mu $,
with massless Majorana spinors, $u_M$, together with the associated
field-strength tensor, ${\mathcal T}^{\mu\nu}:=p^\mu U^\nu -p^\nu U^\mu$. The
${\mathcal T}^... | [
{
"created": "Tue, 19 Feb 2019 03:19:18 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Jun 2019 15:57:55 GMT",
"version": "v2"
}
] | 2019-06-04 | [
[
"Edwards",
"James P.",
""
],
[
"Kirchbach",
"Mariana",
""
]
] | We construct the Rarita-Schwinger basis vectors, $U^\mu$, spanning the direct product space, $U^\mu:=A^\mu\otimes u_M$, of a massless four-vector, $ A^\mu $, with massless Majorana spinors, $u_M$, together with the associated field-strength tensor, ${\mathcal T}^{\mu\nu}:=p^\mu U^\nu -p^\nu U^\mu$. The ${\mathcal T}^{\... | 4.381187 | 4.874083 | 4.492137 | 4.337003 | 4.672103 | 4.639819 | 4.623007 | 4.534778 | 4.441442 | 4.458157 | 4.517647 | 4.502335 | 4.396032 | 4.295601 | 4.454368 | 4.32599 | 4.337144 | 4.431072 | 4.424479 | 4.35924 | 4.425549 |
hep-th/0005205 | Chang-Yeong Lee | Eunsang Kim, Hoil Kim, Chang-Yeong Lee | Matrix Theory Compactification on Noncommutative $T^4/Z_2$ | 19 pages, LaTeX, review part shortened and corrected | J.Math.Phys. 42 (2001) 2677-2688 | 10.1063/1.1371265 | UTTG-10-00 | hep-th | null | In this paper, we construct gauge bundles on a noncommutative toroidal
orbifold $T^4_\theta/Z_2$. First, we explicitly construct a bundle with
constant curvature connections on a noncommutative $T^4_\theta$ following
Rieffel's method. Then, applying the appropriate quotient conditions for its
$Z_2$ orbifold, we find ... | [
{
"created": "Mon, 22 May 2000 22:02:25 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Sep 2000 02:53:19 GMT",
"version": "v2"
},
{
"created": "Thu, 22 Feb 2001 21:40:40 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Kim",
"Eunsang",
""
],
[
"Kim",
"Hoil",
""
],
[
"Lee",
"Chang-Yeong",
""
]
] | In this paper, we construct gauge bundles on a noncommutative toroidal orbifold $T^4_\theta/Z_2$. First, we explicitly construct a bundle with constant curvature connections on a noncommutative $T^4_\theta$ following Rieffel's method. Then, applying the appropriate quotient conditions for its $Z_2$ orbifold, we find a ... | 6.621019 | 6.396122 | 7.739814 | 6.066664 | 6.767804 | 6.433329 | 6.525656 | 6.36947 | 5.866343 | 8.852542 | 6.450723 | 6.410108 | 7.178918 | 6.30168 | 6.627162 | 6.412485 | 6.429195 | 6.131679 | 6.228512 | 7.166265 | 6.394254 |
1002.3298 | Jan Ambjorn | J. Ambjorn, A. Gorlich, S. Jordan, J. Jurkiewicz and R. Loll | CDT meets Horava-Lifshitz gravity | 17 pages, 3 figures. Typos corrected, a few remarks added. | Phys.Lett.B690:413-419,2010 | 10.1016/j.physletb.2010.05.054 | null | hep-th gr-qc hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The theory of causal dynamical triangulations (CDT) attempts to define a
nonperturbative theory of quantum gravity as a sum over space-time geometries.
One of the ingredients of the CDT framework is a global time foliation, which
also plays a central role in the quantum gravity theory recently formulated by
Ho\v{r}av... | [
{
"created": "Wed, 17 Feb 2010 16:10:03 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Apr 2010 12:08:04 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Ambjorn",
"J.",
""
],
[
"Gorlich",
"A.",
""
],
[
"Jordan",
"S.",
""
],
[
"Jurkiewicz",
"J.",
""
],
[
"Loll",
"R.",
""
]
] | The theory of causal dynamical triangulations (CDT) attempts to define a nonperturbative theory of quantum gravity as a sum over space-time geometries. One of the ingredients of the CDT framework is a global time foliation, which also plays a central role in the quantum gravity theory recently formulated by Ho\v{r}ava.... | 5.582767 | 5.111383 | 5.69459 | 5.213226 | 5.785251 | 5.509042 | 5.595877 | 5.110363 | 4.869097 | 5.147732 | 5.092144 | 5.29814 | 5.324813 | 5.390829 | 5.220467 | 5.122808 | 5.29144 | 5.185789 | 5.353498 | 5.51474 | 5.211545 |
hep-th/0512056 | Natalia Shuhmaher | Natalia Shuhmaher and Robert Brandenberger | Brane gas-driven bulk expansion as a precursor stage to brane inflation | 5 pages, no figures, same as published one | Phys.Rev.Lett. 96 (2006) 161301 | 10.1103/PhysRevLett.96.161301 | null | hep-th astro-ph gr-qc hep-ph | null | We propose a new way of obtaining slow-roll inflation in the context of
higher dimensional models motivated by string and M theory. In our model, all
extra spatial dimensions are orbifolded. The initial conditions are taken to be
a hot dense bulk brane gas which drives an initial phase of isotropic bulk
expansion. Th... | [
{
"created": "Mon, 5 Dec 2005 21:43:50 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Apr 2006 21:06:02 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Shuhmaher",
"Natalia",
""
],
[
"Brandenberger",
"Robert",
""
]
] | We propose a new way of obtaining slow-roll inflation in the context of higher dimensional models motivated by string and M theory. In our model, all extra spatial dimensions are orbifolded. The initial conditions are taken to be a hot dense bulk brane gas which drives an initial phase of isotropic bulk expansion. This... | 9.627324 | 9.853435 | 10.24958 | 9.768488 | 9.587678 | 9.000003 | 9.928506 | 10.613008 | 9.944153 | 11.084004 | 9.494099 | 9.678388 | 9.88275 | 9.35868 | 9.335719 | 9.346694 | 9.380559 | 9.555202 | 9.301478 | 9.88689 | 9.266265 |
1110.6901 | Saul Ramos-Sanchez | Mark Goodsell, Saul Ramos-Sanchez, Andreas Ringwald | Kinetic Mixing of U(1)s in Heterotic Orbifolds | 28 pages | null | 10.1007/JHEP01(2012)021 | CERN-PH-TH/2011-253; DESY 11-184 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study kinetic mixing between massless U(1) gauge symmetries in the bosonic
formulation of heterotic orbifold compactifications. For non-prime Z_N
factorisable orbifolds, we find a simple expression of the mixing in terms of
the properties of the N=2 subsectors, which helps understand under what
conditions mixing c... | [
{
"created": "Mon, 31 Oct 2011 18:50:40 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Goodsell",
"Mark",
""
],
[
"Ramos-Sanchez",
"Saul",
""
],
[
"Ringwald",
"Andreas",
""
]
] | We study kinetic mixing between massless U(1) gauge symmetries in the bosonic formulation of heterotic orbifold compactifications. For non-prime Z_N factorisable orbifolds, we find a simple expression of the mixing in terms of the properties of the N=2 subsectors, which helps understand under what conditions mixing can... | 8.445719 | 9.245836 | 10.935531 | 8.50063 | 9.895452 | 9.75594 | 9.254151 | 8.950815 | 9.061371 | 9.391132 | 9.010975 | 8.357364 | 8.820852 | 8.485572 | 8.360954 | 8.589689 | 8.52028 | 8.497433 | 8.152532 | 8.824044 | 8.467471 |
1205.4684 | Anton Rebhan | Anton Rebhan and Dominik Steineder | Probing Two Holographic Models of Strongly Coupled Anisotropic Plasma | JHEP style, 26 pages, 10 figures. v2: references added, slightly
extended discussion of comparison with hard anisotropic loop results and
correspondingly updated fig. 6 (version to appear in JHEP) | null | 10.1007/JHEP08(2012)020 | TUW-12-15 | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quark-gluon plasma during its initial phase after its production in heavy-ion
collisions is expected to have substantial pressure anisotropies. In order to
model this situation by a strongly coupled N=4 super-Yang-Mills plasma with
fixed anisotropy by means of AdS/CFT duality, two models have been discussed in
the li... | [
{
"created": "Mon, 21 May 2012 18:48:23 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Jul 2012 09:42:45 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Rebhan",
"Anton",
""
],
[
"Steineder",
"Dominik",
""
]
] | Quark-gluon plasma during its initial phase after its production in heavy-ion collisions is expected to have substantial pressure anisotropies. In order to model this situation by a strongly coupled N=4 super-Yang-Mills plasma with fixed anisotropy by means of AdS/CFT duality, two models have been discussed in the lite... | 8.252646 | 8.223488 | 9.493232 | 7.851845 | 8.655092 | 8.406758 | 8.267996 | 7.672514 | 7.599477 | 9.300352 | 7.93405 | 7.567639 | 7.790628 | 7.619507 | 7.838205 | 7.933279 | 7.84581 | 8.237872 | 7.808942 | 7.873556 | 7.939767 |
2108.04856 | Maxim Kurkov | Maxim Kurkov and Patrizia Vitale | Four-dimensional noncommutative deformations of $U(1)$ gauge theory and
$L_{\infty}$ bootstrap | 16 pages, revised version, accepted for publication in JHEP | null | null | null | hep-th gr-qc math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | We construct a family of four-dimensional noncommutative deformations of
$U(1)$ gauge theory following a general scheme, recently proposed in JHEP 08
(2020) 041 for a class of coordinate-dependent noncommutative algebras. This
class includes the $\mathfrak{su}(2)$, the $\mathfrak{su}(1,1)$ and the angular
(or $\lambd... | [
{
"created": "Tue, 10 Aug 2021 18:14:40 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Dec 2021 22:22:07 GMT",
"version": "v2"
}
] | 2021-12-23 | [
[
"Kurkov",
"Maxim",
""
],
[
"Vitale",
"Patrizia",
""
]
] | We construct a family of four-dimensional noncommutative deformations of $U(1)$ gauge theory following a general scheme, recently proposed in JHEP 08 (2020) 041 for a class of coordinate-dependent noncommutative algebras. This class includes the $\mathfrak{su}(2)$, the $\mathfrak{su}(1,1)$ and the angular (or $\lambda$... | 7.204863 | 6.659211 | 7.595453 | 6.770479 | 7.244445 | 6.794956 | 7.104498 | 6.494236 | 6.785898 | 7.272096 | 6.813336 | 6.57213 | 7.036998 | 6.844569 | 6.834079 | 6.840062 | 6.974347 | 6.83113 | 6.924373 | 7.035766 | 6.992927 |
1009.3939 | Valentina Forini | Valentina Forini | Quark-antiquark potential in AdS at one loop | 16 pages. Typos corrected, minor changes | JHEP 1011:079,2010 | 10.1007/JHEP11(2010)079 | AEI-2010-150 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive an exact analytical expression for the one-loop partition function
of a string in AdS_5xS^5 background with world-surface ending on two
anti-parallel lines. All quantum fluctuations are shown to be governed by
integrable, single-gap Lame' operators. The first strong coupling correction to
the quark-antiquar... | [
{
"created": "Mon, 20 Sep 2010 20:03:00 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Oct 2010 13:47:22 GMT",
"version": "v2"
}
] | 2011-06-21 | [
[
"Forini",
"Valentina",
""
]
] | We derive an exact analytical expression for the one-loop partition function of a string in AdS_5xS^5 background with world-surface ending on two anti-parallel lines. All quantum fluctuations are shown to be governed by integrable, single-gap Lame' operators. The first strong coupling correction to the quark-antiquark ... | 13.542654 | 12.018282 | 15.785599 | 11.65904 | 11.703933 | 12.380641 | 11.465733 | 11.293537 | 11.774728 | 17.280746 | 12.507283 | 12.223899 | 13.787455 | 12.616447 | 12.148028 | 12.485644 | 12.738685 | 12.083008 | 12.371694 | 14.107315 | 12.610384 |
1305.2069 | Chunshan Lin | Chunshan Lin | SO(3) massive gravity | 5 pages, 1 figure, V2: some typos corrected, remove some remarks
about sound speed; V3: add some comments about Minkowskian solution, and more
references; V4: published version | Phys.Lett. B727 (2013) 31-36 | 10.1016/j.physletb.2013.10.031 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we propose a massive gravity theory with 5 degrees of freedom.
The mass term is constructed by 3 Stuckelberg scalar fields, which respects
SO(3) symmetry in the fields' configuration. By the analysis on the linear
cosmological perturbations, we found that such 5 d.o.f are free from ghost
instability, g... | [
{
"created": "Thu, 9 May 2013 12:15:54 GMT",
"version": "v1"
},
{
"created": "Fri, 10 May 2013 16:12:29 GMT",
"version": "v2"
},
{
"created": "Mon, 20 May 2013 17:53:18 GMT",
"version": "v3"
},
{
"created": "Tue, 5 Aug 2014 05:30:11 GMT",
"version": "v4"
}
] | 2014-08-06 | [
[
"Lin",
"Chunshan",
""
]
] | In this paper, we propose a massive gravity theory with 5 degrees of freedom. The mass term is constructed by 3 Stuckelberg scalar fields, which respects SO(3) symmetry in the fields' configuration. By the analysis on the linear cosmological perturbations, we found that such 5 d.o.f are free from ghost instability, gra... | 9.600206 | 9.643604 | 8.586849 | 7.872929 | 8.752687 | 9.210999 | 8.302559 | 8.054677 | 9.124499 | 9.862085 | 9.645683 | 7.882644 | 7.665826 | 7.334159 | 7.906326 | 7.847949 | 7.603498 | 7.522079 | 7.824069 | 8.114614 | 8.548489 |
hep-th/0509214 | Ashish Saxena | Ashish Saxena, Geoff Potvin, Stefano Giusto and Amanda W. Peet | Smooth geometries with four charges in four dimensions | 1+32 pages, LaTeX, v2: references added, typographical errors
corrected | JHEP0604:010,2006 | 10.1088/1126-6708/2006/04/010 | null | hep-th | null | A class of axially symmetric, rotating four-dimensional geometries carrying
D1, D5, KK monopole and momentum charges is constructed. The geometries are
found to be free of horizons and singulaties, and are candidates to be the
gravity duals of microstates of the (0,4) CFT. These geometries are constructed
by performi... | [
{
"created": "Wed, 28 Sep 2005 16:14:02 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Dec 2005 21:10:44 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Saxena",
"Ashish",
""
],
[
"Potvin",
"Geoff",
""
],
[
"Giusto",
"Stefano",
""
],
[
"Peet",
"Amanda W.",
""
]
] | A class of axially symmetric, rotating four-dimensional geometries carrying D1, D5, KK monopole and momentum charges is constructed. The geometries are found to be free of horizons and singulaties, and are candidates to be the gravity duals of microstates of the (0,4) CFT. These geometries are constructed by performing... | 11.289418 | 9.603702 | 12.400008 | 9.806057 | 9.779611 | 10.217278 | 9.797703 | 9.406022 | 9.476745 | 12.298589 | 9.326758 | 9.069228 | 11.026484 | 9.810235 | 9.530748 | 9.486119 | 9.494689 | 9.89656 | 9.283761 | 11.118995 | 9.475154 |
1510.02200 | Kentaro Tanabe | Kentaro Tanabe | Black rings at large D | 43 pages, 5 figures, published version in JHEP | null | 10.1007/JHEP02(2016)151 | KEK-TH-1867 | hep-th gr-qc | http://creativecommons.org/publicdomain/zero/1.0/ | We study the effective theory of slowly rotating black holes at the infinite
limit of the spacetime dimension D. This large D effective theory is obtained
by integrating the Einstein equation with respect to the radial direction. The
effective theory gives equations for non-linear dynamical deformations of the
slowly... | [
{
"created": "Thu, 8 Oct 2015 05:00:36 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Mar 2016 01:29:10 GMT",
"version": "v2"
}
] | 2016-03-23 | [
[
"Tanabe",
"Kentaro",
""
]
] | We study the effective theory of slowly rotating black holes at the infinite limit of the spacetime dimension D. This large D effective theory is obtained by integrating the Einstein equation with respect to the radial direction. The effective theory gives equations for non-linear dynamical deformations of the slowly r... | 8.252273 | 7.350083 | 8.569064 | 7.455174 | 7.91678 | 8.373346 | 7.839999 | 7.027052 | 7.601094 | 8.281662 | 7.41801 | 7.990843 | 8.158621 | 7.823125 | 8.061456 | 7.671772 | 7.75678 | 7.967474 | 7.906196 | 8.543393 | 7.92432 |
hep-th/9607142 | Anjan Kundu | Anjan Kundu | Generation of Integrable Quantum Nonultralocal Model through Braided
Yang-Baxter Equation | 6 pages, latex, no figures, invited talk at the Int. Conf. on
Problems in QFT ( Alushta, May 13-18, 1996), to appear in the proceedings | null | null | SINP-TNP/96-12 | hep-th | null | Formulating quantum integrability for nonultralocal models (NM) parallel to
the familiar approach of inverse scattering method is a long standing problem.
After reviewing our result regarding algebraic structures of ultralocal models,
we look for the algebra underlying NM. We propose an universal equation
represented... | [
{
"created": "Wed, 17 Jul 1996 14:00:47 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kundu",
"Anjan",
""
]
] | Formulating quantum integrability for nonultralocal models (NM) parallel to the familiar approach of inverse scattering method is a long standing problem. After reviewing our result regarding algebraic structures of ultralocal models, we look for the algebra underlying NM. We propose an universal equation represented b... | 23.857733 | 21.952845 | 27.969772 | 22.428614 | 23.100906 | 22.493567 | 22.520514 | 22.300726 | 22.145464 | 29.443037 | 21.010633 | 21.654415 | 22.887484 | 21.555906 | 22.140982 | 21.563166 | 21.745928 | 21.669336 | 20.866417 | 23.009825 | 20.698362 |
2302.14068 | Muldrow Etheredge | Muldrow Etheredge, I\~naki Garc\'ia Etxebarria, Ben Heidenreich,
Sebastian Rauch | Branes and symmetries for $\mathcal N=3$ S-folds | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe the higher-form and non-invertible symmetries of 4d $\mathcal N=
3$ S-folds using the brane dynamics of their holographic duals. In cases with
enhancement to $\mathcal N=4$ supersymmetry, our analysis reproduces the known
field theory results of Aharony, Seiberg and Tachikawa, and is compatible with
the e... | [
{
"created": "Mon, 27 Feb 2023 19:00:01 GMT",
"version": "v1"
}
] | 2023-03-01 | [
[
"Etheredge",
"Muldrow",
""
],
[
"Etxebarria",
"Iñaki García",
""
],
[
"Heidenreich",
"Ben",
""
],
[
"Rauch",
"Sebastian",
""
]
] | We describe the higher-form and non-invertible symmetries of 4d $\mathcal N= 3$ S-folds using the brane dynamics of their holographic duals. In cases with enhancement to $\mathcal N=4$ supersymmetry, our analysis reproduces the known field theory results of Aharony, Seiberg and Tachikawa, and is compatible with the eff... | 7.528095 | 6.852713 | 8.967931 | 6.934248 | 7.260956 | 6.811222 | 7.171342 | 7.057961 | 6.900717 | 10.471429 | 6.789184 | 7.307971 | 7.785414 | 7.012877 | 7.138334 | 6.951833 | 6.956616 | 6.81924 | 6.864156 | 7.58462 | 6.75254 |
hep-th/9312079 | Takashi Suzuki | Takashi Suzuki | More on $U_q(su(1,1))$ with $q$ a Root of Unity | 24 pages | J.Math.Phys. 35 (1994) 6857-6874 | 10.1063/1.530646 | Edinburgh/92-93/05 | hep-th math.QA | null | Highest weight representations of $U_q(su(1,1))$ with $q=\exp \pi i/N$ are
investigated. The structures of the irreducible hieghesat weight modules are
discussed in detail. The Clebsch-Gordan decomposition for the tensor product of
two irreducible representations is discussed. By using the results, a
representation o... | [
{
"created": "Fri, 10 Dec 1993 10:04:51 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Suzuki",
"Takashi",
""
]
] | Highest weight representations of $U_q(su(1,1))$ with $q=\exp \pi i/N$ are investigated. The structures of the irreducible hieghesat weight modules are discussed in detail. The Clebsch-Gordan decomposition for the tensor product of two irreducible representations is discussed. By using the results, a representation of ... | 7.562375 | 7.655919 | 7.541088 | 6.676113 | 7.098796 | 7.140436 | 6.980782 | 7.270185 | 6.865406 | 8.557014 | 6.813908 | 6.827411 | 7.316382 | 6.859747 | 6.829373 | 6.828314 | 6.830677 | 6.775076 | 6.966166 | 7.3875 | 6.887686 |
1407.3118 | Mir Faizal | Mir Faizal | Multiverse in the Third Quantized Formalism | 8 pages, 0 figures, accepted for publication in Comm. Theor. Phys | Comm. Theor. Phys. 62: 697, 2014 | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we will analyze the third quantization of gravity in path
integral formalism. We will use the time-dependent version of Wheeler-DeWitt
equation to analyze the multiverse in this formalism. We will propose a
mechanism for baryogenesis to occurs in the multiverse, without violating the
baryon number conse... | [
{
"created": "Fri, 11 Jul 2014 11:32:47 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Jul 2014 00:43:02 GMT",
"version": "v2"
}
] | 2014-10-29 | [
[
"Faizal",
"Mir",
""
]
] | In this paper we will analyze the third quantization of gravity in path integral formalism. We will use the time-dependent version of Wheeler-DeWitt equation to analyze the multiverse in this formalism. We will propose a mechanism for baryogenesis to occurs in the multiverse, without violating the baryon number conserv... | 8.998992 | 6.906862 | 7.171844 | 6.99438 | 7.12732 | 6.727872 | 7.520458 | 6.816989 | 7.509247 | 7.912611 | 7.277254 | 7.34897 | 7.569785 | 7.239913 | 7.177023 | 7.071935 | 7.19693 | 7.040315 | 7.511122 | 7.653377 | 7.329369 |
0909.3415 | Matteo Siccardi | G.C. Rossi, M. Siccardi, Ya.S. Stanev, K. Yoshida | Matrix Model and beta-deformed N=4 SYM | 25 pages, uses JHEP3.cls; v2: minor corrections, references added;
matches published version | JHEP 0912:043,2009 | 10.1088/1126-6708/2009/12/043 | ROM2F/2009/18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work is the result of the ideas developed by Ken Yoshida about the
possibility of extending the range of applications of the matrix model approach
to the computation of the holomorphic superpotential of the beta-deformed N=4
super Yang-Mills theory both in the presence of a mass term and in the massless
limit. O... | [
{
"created": "Fri, 18 Sep 2009 11:59:13 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Feb 2010 10:46:10 GMT",
"version": "v2"
}
] | 2010-02-02 | [
[
"Rossi",
"G. C.",
""
],
[
"Siccardi",
"M.",
""
],
[
"Stanev",
"Ya. S.",
""
],
[
"Yoshida",
"K.",
""
]
] | This work is the result of the ideas developed by Ken Yoshida about the possibility of extending the range of applications of the matrix model approach to the computation of the holomorphic superpotential of the beta-deformed N=4 super Yang-Mills theory both in the presence of a mass term and in the massless limit. Our... | 10.328569 | 10.25711 | 11.262155 | 10.008633 | 10.542449 | 9.818427 | 10.973282 | 10.825873 | 10.227769 | 11.910903 | 9.479049 | 9.684908 | 9.657789 | 9.525812 | 9.681221 | 10.104539 | 9.72513 | 9.607531 | 9.336338 | 9.860115 | 9.335739 |
hep-th/0512264 | Simon Dalley | S. Dalley | SU(N_c -> infinity) Lattice Data and Degrees of Freedom of the QCD
string | 9 pages, (v2) 2 refs added | Phys.Rev. D74 (2006) 014025 | 10.1103/PhysRevD.74.014025 | SWAT/05/453 | hep-th hep-ph | null | Lattice simulation data on the critical temperature and long-distance
potential, that probe the degrees of freedom of the QCD string, are critically
reviewed. It is emphasized that comparison of experimental or SU(N_c) lattice
data, at finite number of colors N_c, with free string theory can be misleading
due to stri... | [
{
"created": "Wed, 21 Dec 2005 15:53:48 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Dec 2005 12:17:34 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Dalley",
"S.",
""
]
] | Lattice simulation data on the critical temperature and long-distance potential, that probe the degrees of freedom of the QCD string, are critically reviewed. It is emphasized that comparison of experimental or SU(N_c) lattice data, at finite number of colors N_c, with free string theory can be misleading due to string... | 12.178737 | 12.50867 | 13.274619 | 12.193853 | 12.946601 | 13.754339 | 11.816369 | 11.627896 | 11.466191 | 13.47164 | 11.921345 | 10.985504 | 12.041258 | 11.462169 | 11.446389 | 11.583745 | 11.142406 | 11.523231 | 11.373446 | 11.588113 | 11.513216 |
hep-th/9801170 | Roberto Casalbuoni, Geneva | R. Casalbuoni | Algebraic treatment of compactification on noncommutative tori | 8 pages, Latex, shortened version as accepted for publication in
Physics Letters | Phys.Lett. B431 (1998) 69-72 | 10.1016/S0370-2693(98)00542-5 | UGVA-DPT/1998/01-996 | hep-th | null | In this paper we study the compactification conditions of the M theory on
D-dimensional noncommutative tori. The main tool used for this analysis is the
algebra A(Z^D) of the projective representations of the abelian group Z^D. We
exhibit the explicit solutions in the space of the multiplication algebra of
A(Z^D), th... | [
{
"created": "Mon, 26 Jan 1998 14:45:59 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Feb 1998 08:09:26 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Apr 1998 12:27:38 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Casalbuoni",
"R.",
""
]
] | In this paper we study the compactification conditions of the M theory on D-dimensional noncommutative tori. The main tool used for this analysis is the algebra A(Z^D) of the projective representations of the abelian group Z^D. We exhibit the explicit solutions in the space of the multiplication algebra of A(Z^D), that... | 10.52449 | 9.778549 | 10.68337 | 9.711136 | 10.702409 | 9.688868 | 9.864071 | 8.812815 | 9.167968 | 11.472624 | 9.109866 | 8.890862 | 9.583283 | 8.801677 | 8.757854 | 9.006661 | 8.969351 | 8.959113 | 8.911382 | 9.738149 | 8.805155 |
1210.4266 | Thomas Ortiz | Thomas Ortiz, Henning Samtleben | SO(9) supergravity in two dimensions | 35 pages, 1 figure | null | 10.1007/JHEP01(2013)183 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present maximal supergravity in two dimensions with gauge group SO(9). The
construction is based on selecting the proper embedding of the gauge group into
the infinite-dimensional symmetry group of the ungauged theory. The bosonic
part of the Lagrangian is given by a (dilaton-)gravity coupled non-linear
gauged sig... | [
{
"created": "Tue, 16 Oct 2012 06:51:52 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Ortiz",
"Thomas",
""
],
[
"Samtleben",
"Henning",
""
]
] | We present maximal supergravity in two dimensions with gauge group SO(9). The construction is based on selecting the proper embedding of the gauge group into the infinite-dimensional symmetry group of the ungauged theory. The bosonic part of the Lagrangian is given by a (dilaton-)gravity coupled non-linear gauged sigma... | 8.095523 | 7.307478 | 9.117777 | 7.274515 | 7.62391 | 7.79503 | 8.046965 | 6.67659 | 7.333686 | 10.376962 | 7.347948 | 7.256257 | 8.176073 | 7.407157 | 7.403698 | 7.548359 | 7.558861 | 7.421677 | 7.561204 | 8.266129 | 7.436461 |
0711.4511 | Dmitriy Kulikov | D. A. Kulikov and R. S. Tutik | A new approach to the relativistic treatment of the fermion-boson
system, based on the extension of the SL(2,C) group | v3: revised version (to appear in Mod. Phys. Lett. A) | Mod.Phys.Lett.A23:1829-1840,2008 | 10.1142/S0217732308027205 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new technique for constructing the relativistic wave equation for the
two-body system composed of the spin-1/2 and spin-0 particles is proposed. The
method is based on the extension of the SL(2,C) group to the Sp(4,C) one. The
obtained equation includes the interaction potentials, having both the
Lorentz-vector and... | [
{
"created": "Wed, 28 Nov 2007 14:36:24 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Nov 2007 12:21:17 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Jul 2008 10:00:12 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Kulikov",
"D. A.",
""
],
[
"Tutik",
"R. S.",
""
]
] | A new technique for constructing the relativistic wave equation for the two-body system composed of the spin-1/2 and spin-0 particles is proposed. The method is based on the extension of the SL(2,C) group to the Sp(4,C) one. The obtained equation includes the interaction potentials, having both the Lorentz-vector and L... | 7.136052 | 6.833109 | 5.846708 | 5.958978 | 6.658424 | 6.428079 | 6.232624 | 6.299929 | 6.077302 | 6.550547 | 6.2953 | 6.511526 | 6.317215 | 6.452188 | 6.332444 | 6.56219 | 6.131785 | 6.657425 | 6.429338 | 6.455766 | 6.601467 |
2406.05772 | Parthajit Biswas | Parthajit Biswas, Bobby Ezhuthachan, Arnab Kundu, Baishali Roy | Moving Mirrors, OTOCs and Scrambling | 30 pages, 6 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We explore the physics of scrambling in the moving mirror models, in which a
two-dimensional CFT is subjected to a time-dependent boundary condition. It is
well-known that by choosing an appropriate mirror profile, one can model
quantum aspects of black holes in two-dimensions, ranging from Hawking
radiation in an et... | [
{
"created": "Sun, 9 Jun 2024 13:11:02 GMT",
"version": "v1"
}
] | 2024-06-11 | [
[
"Biswas",
"Parthajit",
""
],
[
"Ezhuthachan",
"Bobby",
""
],
[
"Kundu",
"Arnab",
""
],
[
"Roy",
"Baishali",
""
]
] | We explore the physics of scrambling in the moving mirror models, in which a two-dimensional CFT is subjected to a time-dependent boundary condition. It is well-known that by choosing an appropriate mirror profile, one can model quantum aspects of black holes in two-dimensions, ranging from Hawking radiation in an eter... | 12.606822 | 13.836514 | 14.125318 | 11.507988 | 13.944141 | 12.385137 | 12.580793 | 11.972768 | 12.341098 | 13.608585 | 11.917343 | 12.143091 | 12.175676 | 11.805052 | 11.667372 | 11.877242 | 11.466591 | 11.745092 | 12.018002 | 12.038775 | 12.160048 |
0709.0655 | Gian Paolo Vacca | P. L. Iafelice and G. P. Vacca | Colored Spin Systems, BKP Evolution and finite N_c effects | 17 pages, 4 figures, references update, to appear on EPJC | Eur.Phys.J.C52:581-589,2007 | 10.1140/epjc/s10052-007-0429-x | null | hep-th | null | Even within the framework of the leading logarithmic approximation the
eigenvalues of the BKP kernel for states of more than three reggeized gluons
are unknown in general, contrary to the planar limit case where the problem
becomes integrable. We consider a 4-gluon kernel for a finite number of colors
and define some... | [
{
"created": "Wed, 5 Sep 2007 13:53:14 GMT",
"version": "v1"
},
{
"created": "Sun, 30 Sep 2007 14:33:03 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Iafelice",
"P. L.",
""
],
[
"Vacca",
"G. P.",
""
]
] | Even within the framework of the leading logarithmic approximation the eigenvalues of the BKP kernel for states of more than three reggeized gluons are unknown in general, contrary to the planar limit case where the problem becomes integrable. We consider a 4-gluon kernel for a finite number of colors and define some s... | 15.747227 | 16.060513 | 13.040989 | 12.932681 | 16.595457 | 15.344648 | 16.248375 | 15.159793 | 13.513867 | 14.146982 | 16.477091 | 13.581203 | 12.842442 | 12.814516 | 14.054112 | 14.152323 | 14.08467 | 13.684079 | 13.350457 | 12.330786 | 13.183419 |
hep-th/9503031 | Arefeva Irina | I.Ya.Aref'eva, P.B.Medvedev and A.P.Zubarev | $N$-point amplitudes for d=2 c=1 Discrete States from String Field
Theory | 12 pages, latex, 1 figure | Mod.Phys.Lett. A10 (1995) 2225-2238 | 10.1142/S0217732395002386 | SMI-01-95 | hep-th | null | Starting from string field theory for 2d gravity coupled to c=1 matter we
analyze N-point off-shell tree amplitudes of discrete states. The amplitudes
exhibit the pole structure and we use the oscillator representation to extract
the residues. The residues are generated by a simple effective action. We show
that the ... | [
{
"created": "Mon, 6 Mar 1995 08:36:35 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Aref'eva",
"I. Ya.",
""
],
[
"Medvedev",
"P. B.",
""
],
[
"Zubarev",
"A. P.",
""
]
] | Starting from string field theory for 2d gravity coupled to c=1 matter we analyze N-point off-shell tree amplitudes of discrete states. The amplitudes exhibit the pole structure and we use the oscillator representation to extract the residues. The residues are generated by a simple effective action. We show that the ef... | 14.309512 | 9.732411 | 15.921591 | 10.985196 | 11.753336 | 12.656674 | 12.110218 | 10.872298 | 11.058836 | 16.452108 | 11.651038 | 11.779277 | 13.694404 | 12.820677 | 12.633306 | 13.014728 | 12.806172 | 12.189264 | 13.05858 | 13.520874 | 12.632183 |
1709.08181 | Kazuo Fujikawa | Kazuo Fujikawa | Characteristics of Chiral Anomaly in View of Various Applications | 14 pages. Some explanations are added. This version is to be
published in PRD | Phys. Rev. D 97, 016018 (2018) | 10.1103/PhysRevD.97.016018 | null | hep-th cond-mat.mes-hall nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In view of the recent applications of chiral anomaly to various fields beyond
particle physics, we discuss some basic aspects of chiral anomaly which may
help deepen our understanding of chiral anomaly in particle physics also. It is
first shown that Berry's phase (and its generalization) for the Weyl model $H
=v_{F}... | [
{
"created": "Sun, 24 Sep 2017 10:57:53 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Jan 2018 08:41:28 GMT",
"version": "v2"
}
] | 2018-02-07 | [
[
"Fujikawa",
"Kazuo",
""
]
] | In view of the recent applications of chiral anomaly to various fields beyond particle physics, we discuss some basic aspects of chiral anomaly which may help deepen our understanding of chiral anomaly in particle physics also. It is first shown that Berry's phase (and its generalization) for the Weyl model $H =v_{F} \... | 8.371799 | 9.70336 | 9.13569 | 8.628917 | 9.519344 | 8.969689 | 9.114728 | 8.705423 | 8.535708 | 9.926756 | 8.618442 | 8.302588 | 8.36412 | 8.189262 | 8.166907 | 8.160354 | 8.360259 | 8.324567 | 8.315848 | 8.645894 | 8.217663 |
1508.00110 | Adrian Koenigstein | Adrian Koenigstein, Francesco Giacosa, Dirk H. Rischke | Classical and quantum theory of the massive spin-two field | 43 pages | null | 10.1016/j.aop.2016.01.024 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we review classical and quantum field theory of massive
non-interacting spin-two fields. We derive the equations of motion and
Fierz-Pauli constraints via three different methods: the eigenvalue equations
for the Casimir invariants of the Poincar\'{e} group, a Lagrangian approach,
and a covariant Hamil... | [
{
"created": "Sat, 1 Aug 2015 11:21:14 GMT",
"version": "v1"
}
] | 2016-03-23 | [
[
"Koenigstein",
"Adrian",
""
],
[
"Giacosa",
"Francesco",
""
],
[
"Rischke",
"Dirk H.",
""
]
] | In this paper, we review classical and quantum field theory of massive non-interacting spin-two fields. We derive the equations of motion and Fierz-Pauli constraints via three different methods: the eigenvalue equations for the Casimir invariants of the Poincar\'{e} group, a Lagrangian approach, and a covariant Hamilto... | 6.198824 | 6.284348 | 6.285366 | 5.566587 | 5.892458 | 6.320606 | 6.005924 | 6.03098 | 5.876686 | 5.983261 | 5.747497 | 5.655054 | 5.847109 | 5.663531 | 5.718931 | 5.798801 | 5.838097 | 5.769889 | 5.701837 | 5.840239 | 5.739764 |
1402.1452 | Adam Ritz | Xun Wang, Adam Ritz | Kerr-AdS Black Holes and Force-Free Magnetospheres | 37 pages, 9 figures; v2: comments added and typos corrected | Phys. Rev. D 89, 106011 (2014) | 10.1103/PhysRevD.89.106011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain analogs of the Blandford-Znajek split monopole solution for
force-free magnetospheres around a slowly rotating Kerr-AdS black hole. For
small black holes, we find an analytic solution to first order in the ratio of
horizon radius to AdS scale, $r_H/l$, which exhibits a radial Poynting flux and
for $r_H/l \r... | [
{
"created": "Thu, 6 Feb 2014 18:45:12 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Mar 2014 22:22:29 GMT",
"version": "v2"
}
] | 2014-06-11 | [
[
"Wang",
"Xun",
""
],
[
"Ritz",
"Adam",
""
]
] | We obtain analogs of the Blandford-Znajek split monopole solution for force-free magnetospheres around a slowly rotating Kerr-AdS black hole. For small black holes, we find an analytic solution to first order in the ratio of horizon radius to AdS scale, $r_H/l$, which exhibits a radial Poynting flux and for $r_H/l \rig... | 7.111709 | 7.40088 | 7.446611 | 6.857042 | 7.183115 | 7.600951 | 7.620123 | 7.025981 | 7.057585 | 8.02789 | 7.409879 | 6.801042 | 7.007258 | 6.914009 | 6.913658 | 7.12972 | 7.02319 | 6.936753 | 6.94139 | 7.186866 | 6.834094 |
1207.1438 | Daniel Krefl | Daniel Krefl, Johannes Walcher | ABCD of Beta Ensembles and Topological Strings | 33 pages, 1 figure | null | 10.1007/JHEP11(2012)111 | CERN-PH-TH-2012-189; UCB-PTH-12/11 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study beta-ensembles with Bn, Cn, and Dn eigenvalue measure and their
relation with refined topological strings. Our results generalize the familiar
connections between local topological strings and matrix models leading to An
measure, and illustrate that all those classical eigenvalue ensembles, and
their topolog... | [
{
"created": "Thu, 5 Jul 2012 20:00:04 GMT",
"version": "v1"
}
] | 2015-06-05 | [
[
"Krefl",
"Daniel",
""
],
[
"Walcher",
"Johannes",
""
]
] | We study beta-ensembles with Bn, Cn, and Dn eigenvalue measure and their relation with refined topological strings. Our results generalize the familiar connections between local topological strings and matrix models leading to An measure, and illustrate that all those classical eigenvalue ensembles, and their topologic... | 18.393799 | 18.441362 | 22.031832 | 18.599323 | 19.627443 | 19.982195 | 18.981743 | 17.891687 | 17.350576 | 23.21627 | 18.618731 | 17.387894 | 19.4727 | 17.588533 | 17.5802 | 18.138096 | 17.560751 | 17.718166 | 17.666025 | 19.199415 | 17.36632 |
1604.05325 | Hans Jockers | Andreas Gerhardus and Hans Jockers | Quantum periods of Calabi-Yau fourfolds | 63 pages, v2: clarifications and minor corrections, v3: minor
corrections and published in Nucl.Phys.B | Nucl.Phys. B913 (2016) 425-474 | 10.1016/j.nuclphysb.2016.09.021 | BONN-TH-2016-02 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study the quantum periods together with their Picard-Fuchs
differential equations of Calabi-Yau fourfolds. In contrast to Calabi-Yau
threefolds, we argue that the large volume points of Calabi-Yau fourfolds
generically are regular singular points of the Picard-Fuchs operators of
non-maximally unipoten... | [
{
"created": "Mon, 18 Apr 2016 20:00:09 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Aug 2016 13:08:52 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Nov 2016 09:53:39 GMT",
"version": "v3"
}
] | 2016-11-09 | [
[
"Gerhardus",
"Andreas",
""
],
[
"Jockers",
"Hans",
""
]
] | In this work we study the quantum periods together with their Picard-Fuchs differential equations of Calabi-Yau fourfolds. In contrast to Calabi-Yau threefolds, we argue that the large volume points of Calabi-Yau fourfolds generically are regular singular points of the Picard-Fuchs operators of non-maximally unipotent ... | 7.167923 | 8.502923 | 8.767642 | 7.192578 | 7.459116 | 7.845397 | 7.953672 | 7.214859 | 7.469516 | 9.920832 | 7.352149 | 7.051647 | 7.358584 | 6.94158 | 6.992971 | 7.060081 | 7.083179 | 7.200607 | 7.062707 | 7.554075 | 7.001344 |
hep-th/9305104 | Gernot Muenster | G. Muenster | The role of mathematics in contemporary theoretical physics | 6 pages, MS-TPI-93-02 | null | null | null | hep-th | null | Talk given at the 6th Philosophy-and-Physics-Workshop ``Epistemological
Aspects of the Role of Mathematics in Physical Science'', FEST, Heidelberg,
Feb. 1993
| [
{
"created": "Fri, 21 May 1993 13:11:21 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Muenster",
"G.",
""
]
] | Talk given at the 6th Philosophy-and-Physics-Workshop ``Epistemological Aspects of the Role of Mathematics in Physical Science'', FEST, Heidelberg, Feb. 1993 | 20.919851 | 18.391787 | 17.022234 | 14.011656 | 19.311771 | 15.801538 | 15.889141 | 19.594017 | 16.998102 | 19.986834 | 17.008173 | 17.535196 | 14.27667 | 15.049234 | 15.26338 | 16.290234 | 14.945815 | 16.3993 | 14.537379 | 16.423065 | 14.248219 |
1409.0969 | Chao Wu | Jun Ouyang and Chao Wu | A classification of long-range interactions between two stacks of $p$ \&
$p'$-branes | 26 pages, 7 tables | null | 10.1088/0253-6102/63/2/12 | USTC-ICTS-14-16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the computations of the long-range interactions between two
parallel stacks of branes in \cite{Wu and Wang, Prof. Lu's lecture notes} to
various cases when two stacks of branes are not placed parallel to each other.
We classify the nature of interaction (repulsive or attractive) for each
special case an... | [
{
"created": "Wed, 3 Sep 2014 07:06:56 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Ouyang",
"Jun",
""
],
[
"Wu",
"Chao",
""
]
] | We generalize the computations of the long-range interactions between two parallel stacks of branes in \cite{Wu and Wang, Prof. Lu's lecture notes} to various cases when two stacks of branes are not placed parallel to each other. We classify the nature of interaction (repulsive or attractive) for each special case and ... | 15.254467 | 12.809052 | 15.909281 | 13.111856 | 14.554033 | 14.187038 | 14.818344 | 13.34896 | 13.196589 | 16.033596 | 12.859571 | 13.07227 | 13.801843 | 13.017718 | 14.09124 | 13.67498 | 13.456834 | 13.246831 | 13.338579 | 14.591815 | 13.158838 |
2312.11607 | Pierre Heidmann | Pierre Heidmann and Madhur Mehta | Electromagnetic Entrapment in Gravity | 37 pages + Appendix, 14 figures | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive specific properties of electromagnetism when gravitational effects
are not negligible and analyze their impact on new physics at the horizons of
black holes. We show that a neutral configuration of charges in a region of
high redshift, characterized by a large $g^{tt}$, produces a highly localized
electroma... | [
{
"created": "Mon, 18 Dec 2023 19:00:00 GMT",
"version": "v1"
}
] | 2023-12-20 | [
[
"Heidmann",
"Pierre",
""
],
[
"Mehta",
"Madhur",
""
]
] | We derive specific properties of electromagnetism when gravitational effects are not negligible and analyze their impact on new physics at the horizons of black holes. We show that a neutral configuration of charges in a region of high redshift, characterized by a large $g^{tt}$, produces a highly localized electromagn... | 15.477233 | 16.480169 | 16.623724 | 15.335338 | 16.250031 | 16.066797 | 16.578527 | 15.94801 | 15.58994 | 16.653282 | 15.514848 | 14.867041 | 15.008397 | 14.83267 | 15.177119 | 15.338277 | 15.191127 | 14.888317 | 14.764131 | 15.029857 | 14.796368 |
hep-th/0311089 | Alejandro Corichi | Alejandro Corichi and Jeronimo Cortez | Note on Self-Duality and the Kodama State | 4 pages, no figures. References and discussion added. Final version
to appear in PRD | Phys.Rev. D69 (2004) 047702 | 10.1103/PhysRevD.69.047702 | ICN-UNAM-03/12 | hep-th gr-qc math-ph math.MP | null | An interesting interplay between self-duality, the Kodama (Chern-Simons)
state and knot invariants is shown to emerge in the quantum theory of an
Abelian gauge theory. More precisely, when a self-dual representation of the
CCR is chosen, the corresponding vacuum in the Schroedinger representation is
precisely given b... | [
{
"created": "Tue, 11 Nov 2003 17:47:25 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Nov 2003 17:27:52 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Feb 2004 20:28:12 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Corichi",
"Alejandro",
""
],
[
"Cortez",
"Jeronimo",
""
]
] | An interesting interplay between self-duality, the Kodama (Chern-Simons) state and knot invariants is shown to emerge in the quantum theory of an Abelian gauge theory. More precisely, when a self-dual representation of the CCR is chosen, the corresponding vacuum in the Schroedinger representation is precisely given by ... | 12.205892 | 8.941001 | 9.317406 | 9.558965 | 9.116919 | 9.634343 | 9.400702 | 9.524691 | 9.851132 | 10.595275 | 9.338239 | 10.075877 | 10.13484 | 10.268153 | 10.883483 | 10.357646 | 10.804454 | 10.194984 | 10.010374 | 10.437356 | 10.467605 |
1702.01193 | Lavinia Heisenberg | Jose Beltran Jimenez, Lavinia Heisenberg, Ryotaro Kase, Ryo Namba and
Shinji Tsujikawa | Instabilities in Horndeski Yang-Mills inflation | 8 pages, 2 figures | Phys. Rev. D 95, 063533 (2017) | 10.1103/PhysRevD.95.063533 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A non-abelian $SU(2)$ gauge field with a non-minimal Horndeski coupling to
gravity gives rise to a de Sitter solution followed by a graceful exit to a
radiation-dominated epoch. In this Horndeski Yang-Mills (HYM) theory we derive
the second-order action for tensor perturbations on the homogeneous and
isotropic quasi ... | [
{
"created": "Fri, 3 Feb 2017 22:34:04 GMT",
"version": "v1"
}
] | 2017-04-05 | [
[
"Jimenez",
"Jose Beltran",
""
],
[
"Heisenberg",
"Lavinia",
""
],
[
"Kase",
"Ryotaro",
""
],
[
"Namba",
"Ryo",
""
],
[
"Tsujikawa",
"Shinji",
""
]
] | A non-abelian $SU(2)$ gauge field with a non-minimal Horndeski coupling to gravity gives rise to a de Sitter solution followed by a graceful exit to a radiation-dominated epoch. In this Horndeski Yang-Mills (HYM) theory we derive the second-order action for tensor perturbations on the homogeneous and isotropic quasi de... | 5.671216 | 5.60858 | 4.928071 | 4.942909 | 5.275095 | 5.284928 | 5.622984 | 4.934608 | 5.069452 | 4.891256 | 4.892553 | 5.416113 | 5.13289 | 4.949826 | 5.212801 | 5.23019 | 5.290694 | 5.086452 | 5.082249 | 5.168643 | 5.18078 |
1904.03957 | S. Danial Forghani | S. Danial Forghani, S. Habib Mazharimousavi, and Mustafa Halilsoy | Higher Dimensional Particle Model in Third-Order Lovelock Gravity | 7 pages, 1 figure (7 subfigures) | null | 10.1140/epjp/s13360-020-00602-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By using the formalism of thin-shells, we construct a geometrical model of a
particle in third-order Lovelock gravity. This particular theory which is valid
at least in 7 dimensions, provides enough degrees of freedom and grounds
towards such a construction. The particle consists of a flat interior and a
non-black ho... | [
{
"created": "Mon, 8 Apr 2019 11:15:29 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Aug 2019 16:59:36 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Feb 2020 09:22:54 GMT",
"version": "v3"
},
{
"created": "Sun, 13 Sep 2020 07:01:31 GMT",
"version": "v4"
}
] | 2020-09-15 | [
[
"Forghani",
"S. Danial",
""
],
[
"Mazharimousavi",
"S. Habib",
""
],
[
"Halilsoy",
"Mustafa",
""
]
] | By using the formalism of thin-shells, we construct a geometrical model of a particle in third-order Lovelock gravity. This particular theory which is valid at least in 7 dimensions, provides enough degrees of freedom and grounds towards such a construction. The particle consists of a flat interior and a non-black hole... | 17.832081 | 16.187708 | 13.905861 | 13.396038 | 17.105474 | 15.890566 | 17.167063 | 14.148975 | 17.421837 | 15.224477 | 16.734528 | 15.781124 | 13.658066 | 14.425659 | 15.04833 | 14.938672 | 15.457548 | 13.875089 | 15.461555 | 14.097878 | 15.493844 |
hep-th/9909068 | Jonathan R. Ellis | John Ellis (CERN), N.E. Mavromatos (Oxford) and Elizabeth Winstanley
(Oxford) | Logarithmic Operators Fold D branes into AdS_3 | 10 pages revtex, one eps figure included | Phys.Lett.B476:165-171,2000 | 10.1016/S0370-2693(00)00128-3 | CERN-TH/99--279, OUTP--99--42P | hep-th gr-qc | null | We use logarithmic conformal field theory techniques to describe recoil
effects in the scattering of two Dirichlet branes in D dimensions. In the
particular case that a D1 brane strikes a D3 brane perpendicularly, thereby
folding it, we find that the recoil space-time is maximally symmetric, with
AdS_3 x E_{D-3} geom... | [
{
"created": "Fri, 10 Sep 1999 16:11:06 GMT",
"version": "v1"
}
] | 2009-09-11 | [
[
"Ellis",
"John",
"",
"CERN"
],
[
"Mavromatos",
"N. E.",
"",
"Oxford"
],
[
"Winstanley",
"Elizabeth",
"",
"Oxford"
]
] | We use logarithmic conformal field theory techniques to describe recoil effects in the scattering of two Dirichlet branes in D dimensions. In the particular case that a D1 brane strikes a D3 brane perpendicularly, thereby folding it, we find that the recoil space-time is maximally symmetric, with AdS_3 x E_{D-3} geomet... | 11.107306 | 9.425537 | 10.843253 | 9.761529 | 9.509732 | 9.580505 | 9.642863 | 9.171584 | 8.624048 | 10.94741 | 9.210758 | 9.410627 | 10.342766 | 9.094959 | 9.351552 | 9.174158 | 9.728683 | 9.713041 | 9.028852 | 10.170677 | 9.127337 |
1101.2891 | Francisco A. Brito | M. A. Anacleto, F. A. Brito, E. Passos | Superresonance effect from a rotating acoustic black hole and Lorentz
symmetry breaking | 9 pages, version to appear in PLB | Phys.Lett.B703:609-613,2011 | 10.1016/j.physletb.2011.08.040 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the possibility of the acoustic superresonance phenomenon
(analog to the superradiance in black hole physics), i.e., the amplification of
a sound wave by reflection from the ergoregion of a rotating acoustic black
hole with Lorentz symmetry breaking. For rotating black holes the effect of
superradiance... | [
{
"created": "Fri, 14 Jan 2011 20:58:33 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Aug 2011 20:53:54 GMT",
"version": "v2"
}
] | 2011-09-13 | [
[
"Anacleto",
"M. A.",
""
],
[
"Brito",
"F. A.",
""
],
[
"Passos",
"E.",
""
]
] | We investigate the possibility of the acoustic superresonance phenomenon (analog to the superradiance in black hole physics), i.e., the amplification of a sound wave by reflection from the ergoregion of a rotating acoustic black hole with Lorentz symmetry breaking. For rotating black holes the effect of superradiance c... | 11.196591 | 10.421436 | 9.136121 | 8.937552 | 9.50801 | 10.604236 | 10.484309 | 9.051903 | 9.261209 | 10.482749 | 10.102228 | 9.989191 | 9.897039 | 9.692323 | 9.984488 | 10.359041 | 10.395978 | 9.741138 | 10.37851 | 9.941898 | 10.137378 |
hep-th/0702035 | David Skinner | Rutger Boels, Lionel Mason & David Skinner | From Twistor Actions to MHV Diagrams | 12 pages, RevTeX | Phys.Lett.B648:90-96,2007 | 10.1016/j.physletb.2007.02.058 | null | hep-th hep-ph | null | We show that MHV diagrams are the Feynman diagrams of certain twistor actions
for gauge theories in an axial gauge. The gauge symmetry of the twistor action
is larger than that on space-time and this allows us to fix a gauge that makes
the MHV formalism manifest but which is inaccessible from space-time. The
framewor... | [
{
"created": "Mon, 5 Feb 2007 18:20:55 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Boels",
"Rutger",
""
],
[
"Mason",
"Lionel",
""
],
[
"Skinner",
"David",
""
]
] | We show that MHV diagrams are the Feynman diagrams of certain twistor actions for gauge theories in an axial gauge. The gauge symmetry of the twistor action is larger than that on space-time and this allows us to fix a gauge that makes the MHV formalism manifest but which is inaccessible from space-time. The framework ... | 10.509135 | 9.643614 | 12.105091 | 10.194685 | 10.510921 | 11.550996 | 9.963719 | 9.414221 | 10.617616 | 13.286011 | 10.378746 | 10.297659 | 10.760628 | 10.275689 | 10.823385 | 10.770972 | 10.510548 | 10.545969 | 10.090381 | 10.651703 | 10.384624 |
1012.2387 | Dylan Albrecht | Dylan Albrecht (College of William and Mary) | Weighted Power Counting and Perturbative Unitarity | 12 pages, version published in Phys. Rev. D | Phys.Rev.D83:045029,2011 | 10.1103/PhysRevD.83.045029 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the relationship between renormalizability and unitarity at a
Lifshitz point in d dimensions. We test tree unitarity for theories containing
only scalars and fermions, and for pure gauge theory. In both cases, we find
the requirement of weighted power-counting renormalizability is equivalent to
that of tr... | [
{
"created": "Fri, 10 Dec 2010 21:03:30 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Feb 2011 19:41:50 GMT",
"version": "v2"
}
] | 2011-03-23 | [
[
"Albrecht",
"Dylan",
"",
"College of William and Mary"
]
] | We consider the relationship between renormalizability and unitarity at a Lifshitz point in d dimensions. We test tree unitarity for theories containing only scalars and fermions, and for pure gauge theory. In both cases, we find the requirement of weighted power-counting renormalizability is equivalent to that of tree... | 10.260528 | 9.226286 | 9.29253 | 8.407521 | 8.520095 | 9.03638 | 8.325327 | 8.724959 | 9.246145 | 9.617732 | 9.082438 | 9.203682 | 9.326838 | 8.766744 | 9.019108 | 8.929178 | 9.143253 | 9.309325 | 8.937778 | 9.130937 | 8.744335 |
1107.0543 | Bin Chen | Bin Chen and Jia-ju Zhang | General Hidden Conformal Symmetry of 4D Kerr-Newman and 5D Kerr Black
Holes | 25 pages; Typos corrected; Revision in accordance to the changes in
1106.4148 | null | 10.1007/JHEP08(2011)114 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There are two known CFT duals, namely the J-picture and the Q-picture, for a
four-dimensional Kerr-Newman black hole, corresponding to the angular momentum
$J$ and the electric charge $Q$ respectively. In our recent study we found a
one-parameter class of CFT duals for extremal Kerr-Newman black hole,
connecting thes... | [
{
"created": "Mon, 4 Jul 2011 06:56:58 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Aug 2011 02:05:01 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Dec 2011 03:14:19 GMT",
"version": "v3"
}
] | 2015-05-28 | [
[
"Chen",
"Bin",
""
],
[
"Zhang",
"Jia-ju",
""
]
] | There are two known CFT duals, namely the J-picture and the Q-picture, for a four-dimensional Kerr-Newman black hole, corresponding to the angular momentum $J$ and the electric charge $Q$ respectively. In our recent study we found a one-parameter class of CFT duals for extremal Kerr-Newman black hole, connecting these ... | 7.87366 | 6.830688 | 8.352702 | 6.967238 | 7.203887 | 7.236354 | 6.956335 | 6.805746 | 7.189162 | 8.10377 | 6.677602 | 7.153677 | 7.509851 | 7.156431 | 7.333963 | 7.393421 | 7.32035 | 7.199974 | 7.197429 | 7.662309 | 7.41793 |
hep-th/9411213 | Spenta Wadia | Spenta R. Wadia | $W_\infty$ Algebra and Geometric Formulation of QCD$_2$ | 3 pages, latex, conference talk | null | null | null | hep-th | null | We review the gauge invariant formulation of 2-dim. QCD. We show that the
non-linear gauge invariant phase space is the coset $W_\infty/W_{+\infty}\times
W_{-\infty}$ ,which is specified by the $N=\infty$ master-field of this model.
The meson fields correspond to the local coordinates of the coset. We comment
on the ... | [
{
"created": "Tue, 29 Nov 1994 13:37:44 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Wadia",
"Spenta R.",
""
]
] | We review the gauge invariant formulation of 2-dim. QCD. We show that the non-linear gauge invariant phase space is the coset $W_\infty/W_{+\infty}\times W_{-\infty}$ ,which is specified by the $N=\infty$ master-field of this model. The meson fields correspond to the local coordinates of the coset. We comment on the st... | 12.351085 | 9.979197 | 12.697271 | 10.167145 | 10.234759 | 9.817814 | 9.412813 | 9.676373 | 9.518538 | 12.78394 | 10.166914 | 9.928808 | 11.621941 | 10.088268 | 10.499866 | 10.224367 | 9.992202 | 9.965665 | 10.425794 | 12.000484 | 10.546042 |
1609.06723 | Solomon Endlich | Solomon Endlich and Riccardo Penco | A Modern Approach to Superradiance | 39 pages (v2 contains many added details and corrects an error in v1.
In particular, the instability rates for leading vector bound states are
computed exactly in the large Compton wavelength limit.) | null | 10.1007/JHEP05(2017)052 | null | hep-th astro-ph.HE gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we provide a simple and modern discussion of rotational
superradiance based on quantum field theory. We work with an effective theory
valid at scales much larger than the size of the spinning object responsible
for superradiance. Within this framework, the probability of absorption by an
object at rest... | [
{
"created": "Wed, 21 Sep 2016 20:00:02 GMT",
"version": "v1"
},
{
"created": "Sat, 10 Dec 2016 02:22:19 GMT",
"version": "v2"
}
] | 2017-06-07 | [
[
"Endlich",
"Solomon",
""
],
[
"Penco",
"Riccardo",
""
]
] | In this paper, we provide a simple and modern discussion of rotational superradiance based on quantum field theory. We work with an effective theory valid at scales much larger than the size of the spinning object responsible for superradiance. Within this framework, the probability of absorption by an object at rest c... | 6.03673 | 6.85323 | 6.224488 | 5.965763 | 6.756466 | 6.634233 | 6.998425 | 6.382545 | 6.334852 | 6.425797 | 6.273592 | 6.012309 | 5.761122 | 5.939337 | 5.907654 | 5.960557 | 5.99977 | 5.924916 | 5.859284 | 5.738514 | 6.007875 |
1610.05584 | Junya Yagi | Junya Yagi | Branes and integrable lattice models | 16 pages. Invited review article for Modern Physics Letters A. v2:
published version | Mod. Phys. Lett. A 32 (2017) 1730003 | 10.1142/S0217732317300038 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a brief review of my work on the correspondence between
four-dimensional $\mathcal{N} = 1$ supersymmetric field theories realized by
brane tilings and two-dimensional integrable lattice models. I explain how to
construct integrable lattice models from extended operators in partially
topological quantum field ... | [
{
"created": "Tue, 18 Oct 2016 12:52:32 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Jan 2017 09:20:09 GMT",
"version": "v2"
}
] | 2017-01-09 | [
[
"Yagi",
"Junya",
""
]
] | This is a brief review of my work on the correspondence between four-dimensional $\mathcal{N} = 1$ supersymmetric field theories realized by brane tilings and two-dimensional integrable lattice models. I explain how to construct integrable lattice models from extended operators in partially topological quantum field th... | 8.63096 | 6.30738 | 8.812759 | 6.833269 | 6.088814 | 6.344518 | 7.187669 | 6.277548 | 6.36026 | 9.133732 | 6.764323 | 6.890298 | 8.310443 | 6.965682 | 7.141681 | 7.012251 | 6.937092 | 7.027007 | 6.918279 | 7.955735 | 6.996255 |
0809.3464 | Peter Freund | Peter G.O. Freund | Dynamical Spin II | Contribution to "Fundamental Interactions - A Memorial Volume for
Wolfgang Kummer", World Scientific, to be published | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The possibility of building all particles from spinless constituents is
explored. Composite fermions are formed from bosonic carriers of electric and
magnetic charge of a composite abelian gauge field. Internal attributes are
accounted for by dimensional reduction from a higher-dimensional space-time in
which the abe... | [
{
"created": "Fri, 19 Sep 2008 21:25:34 GMT",
"version": "v1"
}
] | 2008-09-23 | [
[
"Freund",
"Peter G. O.",
""
]
] | The possibility of building all particles from spinless constituents is explored. Composite fermions are formed from bosonic carriers of electric and magnetic charge of a composite abelian gauge field. Internal attributes are accounted for by dimensional reduction from a higher-dimensional space-time in which the abeli... | 14.21991 | 13.904237 | 14.11149 | 13.018064 | 13.037137 | 13.736596 | 13.638499 | 12.507648 | 13.14784 | 12.843486 | 12.651787 | 12.447086 | 13.670785 | 12.319934 | 12.445089 | 12.989033 | 12.104238 | 12.850389 | 12.775874 | 13.634893 | 12.66785 |
2111.14747 | Laurent Freidel | Laurent Freidel | A canonical bracket for open gravitational system | 13 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | This paper shows that the generalization of the Barnich-Troessaert bracket
recently proposed to represent the extended corner algebra can be obtained as
the canonical bracket for an extended gravitational Lagrangian. This extension
effectively allows one to reabsorb the symplectic flux into the dressing of the
Lagran... | [
{
"created": "Mon, 29 Nov 2021 17:50:50 GMT",
"version": "v1"
}
] | 2021-11-30 | [
[
"Freidel",
"Laurent",
""
]
] | This paper shows that the generalization of the Barnich-Troessaert bracket recently proposed to represent the extended corner algebra can be obtained as the canonical bracket for an extended gravitational Lagrangian. This extension effectively allows one to reabsorb the symplectic flux into the dressing of the Lagrangi... | 16.179489 | 12.587117 | 14.014359 | 12.314856 | 11.763109 | 12.462715 | 12.546552 | 12.105068 | 12.037814 | 16.611691 | 13.535933 | 13.280544 | 13.755674 | 12.682261 | 12.574906 | 12.749064 | 12.846395 | 12.836199 | 13.385203 | 13.851951 | 14.997622 |
1201.6434 | Jiro Soda | Jiro Soda | Statistical Anisotropy from Anisotropic Inflation | 32 pages, 5 figures, invited review for CQG, published version | null | 10.1088/0264-9381/29/8/083001 | KUNS-2383 | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review an inflationary scenario with the anisotropic expansion rate. An
anisotropic inflationary universe can be realized by a vector field coupled
with an inflaton, which can be regarded as a counter example to the cosmic
no-hair conjecture. We show generality of anisotropic inflation and derive a
universal prope... | [
{
"created": "Tue, 31 Jan 2012 04:18:31 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Mar 2012 07:44:16 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Soda",
"Jiro",
""
]
] | We review an inflationary scenario with the anisotropic expansion rate. An anisotropic inflationary universe can be realized by a vector field coupled with an inflaton, which can be regarded as a counter example to the cosmic no-hair conjecture. We show generality of anisotropic inflation and derive a universal propert... | 6.695007 | 6.452936 | 6.697607 | 6.061681 | 6.541072 | 6.511397 | 6.206088 | 5.826767 | 5.993671 | 6.511827 | 6.291587 | 6.176154 | 6.345628 | 6.109869 | 6.116927 | 6.370868 | 6.206416 | 6.313097 | 6.284048 | 6.138496 | 6.140178 |
2009.07136 | Max Hubner | Max Hubner | Local $G_2$-Manifolds, Higgs Bundles and a Colored Quantum Mechanics | 70 pages, 16 figures, JHEP version | null | 10.1007/JHEP05(2021)002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | M-theory on local $G_2$-manifolds engineers 4d minimally supersymmetric gauge
theories. We consider ALE-fibered $G_2$-manifolds and study the 4d physics from
the view point of a partially twisted 7d supersymmetric Yang-Mills theory and
its Higgs bundle. Euclidean M2-brane instantons descend to non-perturbative
effect... | [
{
"created": "Tue, 15 Sep 2020 14:37:15 GMT",
"version": "v1"
},
{
"created": "Sat, 8 May 2021 16:38:38 GMT",
"version": "v2"
}
] | 2021-05-19 | [
[
"Hubner",
"Max",
""
]
] | M-theory on local $G_2$-manifolds engineers 4d minimally supersymmetric gauge theories. We consider ALE-fibered $G_2$-manifolds and study the 4d physics from the view point of a partially twisted 7d supersymmetric Yang-Mills theory and its Higgs bundle. Euclidean M2-brane instantons descend to non-perturbative effects ... | 8.364237 | 7.222237 | 7.900869 | 7.507242 | 8.076047 | 7.930665 | 7.059501 | 7.172837 | 7.543794 | 8.99585 | 7.428919 | 7.467792 | 7.888815 | 7.043575 | 7.027609 | 7.138996 | 7.215565 | 7.24611 | 7.028547 | 7.782165 | 7.234971 |
1906.06131 | Olaf Kr\"uger PhD | Olaf Kr\"uger | Log-Expansions from Combinatorial Dyson-Schwinger Equations | 26 pages | null | 10.1007/s11005-020-01288-8 | UWThPh 2019-18 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a precise connection between combinatorial Dyson-Schwinger equations
and log-expansions for Green's functions in quantum field theory. The latter
are triangular power series in the coupling constant $\alpha$ and a logarithmic
energy scale $L$ --- a reordering of terms as $G(\alpha,L) = 1 \pm \sum_{j \geq
0} \... | [
{
"created": "Fri, 14 Jun 2019 11:23:13 GMT",
"version": "v1"
}
] | 2020-08-26 | [
[
"Krüger",
"Olaf",
""
]
] | We give a precise connection between combinatorial Dyson-Schwinger equations and log-expansions for Green's functions in quantum field theory. The latter are triangular power series in the coupling constant $\alpha$ and a logarithmic energy scale $L$ --- a reordering of terms as $G(\alpha,L) = 1 \pm \sum_{j \geq 0} \al... | 6.820403 | 7.05226 | 7.3022 | 6.715593 | 7.203083 | 6.65329 | 7.234984 | 7.053849 | 6.654709 | 7.046544 | 6.745924 | 6.805506 | 6.581597 | 6.610451 | 6.736326 | 6.838651 | 6.81085 | 6.7648 | 6.600772 | 6.87708 | 6.536232 |
1912.04804 | Joseph Tooby-Smith | B. C. Allanach, Ben Gripaios and Joseph Tooby-Smith | Geometric General Solution to the $U(1)$ Anomaly Equations | 11 pages. v3: Much expanded explanatory exposition | null | 10.1007/JHEP05(2020)065 | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Costa et al. [Phys. Rev. Lett. 123, 151601 (2019)] recently gave a general
solution to the anomaly equations for $n$ charges in a $U(1)$ gauge theory.
`Primitive' solutions of chiral fermion charges were parameterised and it was
shown how operations performed upon them (concatenation with other primitive
solutions an... | [
{
"created": "Tue, 10 Dec 2019 16:37:19 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Feb 2020 15:18:49 GMT",
"version": "v2"
},
{
"created": "Mon, 6 Apr 2020 12:50:26 GMT",
"version": "v3"
}
] | 2020-06-24 | [
[
"Allanach",
"B. C.",
""
],
[
"Gripaios",
"Ben",
""
],
[
"Tooby-Smith",
"Joseph",
""
]
] | Costa et al. [Phys. Rev. Lett. 123, 151601 (2019)] recently gave a general solution to the anomaly equations for $n$ charges in a $U(1)$ gauge theory. `Primitive' solutions of chiral fermion charges were parameterised and it was shown how operations performed upon them (concatenation with other primitive solutions and ... | 12.769415 | 13.811248 | 12.458478 | 11.741043 | 13.82638 | 14.348413 | 13.407871 | 13.514092 | 11.914061 | 12.956454 | 12.325565 | 11.279931 | 11.207792 | 11.395127 | 11.677467 | 11.526542 | 11.774742 | 11.662883 | 11.193962 | 11.234664 | 11.933984 |
1110.6767 | Larisa Jonke | Marija Dimitrijevic and Larisa Jonke | Gauge theory on kappa-Minkowski revisited: the twist approach | Based on talks given at QTS7 (Prague), BW2011 (Donji Milanovac),
Corfu2011, BlagojevicFest (Divcibare) | null | 10.1088/1742-6596/343/1/012049 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Kappa-Minkowski space-time is an example of noncommutative space-time with
potentially interesting phenomenology. However, the construction of field
theories on this space is plagued with ambiguities. We propose to resolve
certain ambiguities by clarifying the geometrical picture of gauge
transformations on the kappa... | [
{
"created": "Mon, 31 Oct 2011 12:21:22 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Dimitrijevic",
"Marija",
""
],
[
"Jonke",
"Larisa",
""
]
] | Kappa-Minkowski space-time is an example of noncommutative space-time with potentially interesting phenomenology. However, the construction of field theories on this space is plagued with ambiguities. We propose to resolve certain ambiguities by clarifying the geometrical picture of gauge transformations on the kappa-M... | 7.292132 | 5.803674 | 7.416693 | 5.802083 | 6.593197 | 5.848444 | 5.888021 | 5.8121 | 5.80591 | 7.735703 | 6.076994 | 6.519441 | 6.597844 | 6.404433 | 6.589953 | 6.100072 | 6.414163 | 6.497203 | 6.443735 | 6.752177 | 6.404678 |
hep-th/0103237 | Andrea Cappelli | Andrea Cappelli, Riccardo Guida, Nicodemo Magnoli | Exact Consequences of the Trace Anomaly in Four Dimensions | 39 pages, 3 tables; published version, some misprints corrected;
Mathematica routines can be found at:
http://arturo.fi.infn.it/cappelli/papers/ttt/ | Nucl.Phys. B618 (2001) 371-406 | 10.1016/S0550-3213(01)00489-8 | SphT T-01/027, DFF 371/01/2001, Ge-TH-03/2001 | hep-th | null | The general form of the stress-tensor three-point function in four dimensions
is obtained by solving the Ward identities for the diffeomorphism and Weyl
symmetries. Several properties of this correlator are discussed, such as the
renormalization and scheme independence and the analogies with the anomalous
chiral tria... | [
{
"created": "Wed, 28 Mar 2001 15:02:59 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Dec 2001 15:30:02 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Cappelli",
"Andrea",
""
],
[
"Guida",
"Riccardo",
""
],
[
"Magnoli",
"Nicodemo",
""
]
] | The general form of the stress-tensor three-point function in four dimensions is obtained by solving the Ward identities for the diffeomorphism and Weyl symmetries. Several properties of this correlator are discussed, such as the renormalization and scheme independence and the analogies with the anomalous chiral triang... | 8.067964 | 7.722466 | 8.32393 | 7.33466 | 7.705854 | 7.949743 | 7.502409 | 7.246829 | 7.012744 | 8.670295 | 6.915159 | 7.561637 | 7.634183 | 7.29664 | 7.450332 | 7.41468 | 7.401285 | 7.809839 | 7.48561 | 7.563783 | 7.568387 |
1707.06245 | Phillip Szepietowski | Alejandra Castro, Cynthia Keeler, and Phillip Szepietowski | Tweaking one-loop determinants in AdS$_3$ | 36+18 pages | null | 10.1007/JHEP10(2017)070 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the subject of one-loop determinants in AdS$_3$ gravity via the
quasinormal mode method. Our goal is to evaluate a one-loop determinant with
chiral boundary conditions for the metric field; chirality is achieved by
imposing Dirichlet boundary conditions on certain components while others
satisfy Neumann. A... | [
{
"created": "Wed, 19 Jul 2017 18:00:26 GMT",
"version": "v1"
}
] | 2017-11-22 | [
[
"Castro",
"Alejandra",
""
],
[
"Keeler",
"Cynthia",
""
],
[
"Szepietowski",
"Phillip",
""
]
] | We revisit the subject of one-loop determinants in AdS$_3$ gravity via the quasinormal mode method. Our goal is to evaluate a one-loop determinant with chiral boundary conditions for the metric field; chirality is achieved by imposing Dirichlet boundary conditions on certain components while others satisfy Neumann. Alo... | 12.521754 | 12.21917 | 14.119196 | 12.110108 | 13.632216 | 13.185969 | 12.557775 | 11.968205 | 12.076458 | 15.058735 | 12.086223 | 11.813645 | 12.230403 | 12.077434 | 12.180261 | 11.704742 | 11.816591 | 11.969592 | 12.064434 | 13.041048 | 11.922643 |
0907.3093 | Taekyung Kim Mr. | Sung-Soo Kim (ULB), Taekyung Kim, Yoonbai Kim (Sungkyunkwan U.) | Surplus Solid Angle as an Imprint of Horava-Lifshitz Gravity | 23 pages, 1 figure; minor changes, published version | null | 10.1103/PhysRevD.80.124002 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the electrostatic field of a point charge coupled to
Horava-Lifshitz gravity and find an exact solution describing the space with a
surplus (or deficit) solid angle. Although, theoretically in general
relativity, a surplus angle is hardly to be obtained in the presence of
ordinary matter with positive ene... | [
{
"created": "Fri, 17 Jul 2009 17:44:37 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Dec 2009 05:44:14 GMT",
"version": "v2"
}
] | 2013-05-29 | [
[
"Kim",
"Sung-Soo",
"",
"ULB"
],
[
"Kim",
"Taekyung",
"",
"Sungkyunkwan U."
],
[
"Kim",
"Yoonbai",
"",
"Sungkyunkwan U."
]
] | We consider the electrostatic field of a point charge coupled to Horava-Lifshitz gravity and find an exact solution describing the space with a surplus (or deficit) solid angle. Although, theoretically in general relativity, a surplus angle is hardly to be obtained in the presence of ordinary matter with positive energ... | 13.01693 | 11.389882 | 12.660048 | 11.547754 | 12.451683 | 12.318498 | 12.189455 | 11.90682 | 11.313431 | 12.223677 | 12.344381 | 12.462711 | 11.779915 | 11.800812 | 11.737329 | 11.806242 | 12.191726 | 11.554249 | 11.896877 | 11.775003 | 12.08131 |
1302.6063 | Kenichi Konishi | Kenichi Konishi | Confinement via strongly-coupled non-Abelian monopoles | Latex 17 pages. arXiv admin note: text overlap with arXiv:1301.0420 | null | 10.1142/9789814566254_0041 | IFUP-TH/2013-06 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | New types of confinement phase emerge as singular SCFT's appearing as
infrared-fixed-points of N=2 supersymmetric QCD (SQCD) are perturbed by an N=1
adjoint mass term. Based on a recent remarkable work on infrared-fixed-point
SCFT of highest criticalities by Gaiotto, Seiberg and Tachikawa, we discuss
physics of certa... | [
{
"created": "Mon, 25 Feb 2013 11:49:05 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Mar 2013 11:11:25 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Mar 2013 17:04:41 GMT",
"version": "v3"
}
] | 2017-08-23 | [
[
"Konishi",
"Kenichi",
""
]
] | New types of confinement phase emerge as singular SCFT's appearing as infrared-fixed-points of N=2 supersymmetric QCD (SQCD) are perturbed by an N=1 adjoint mass term. Based on a recent remarkable work on infrared-fixed-point SCFT of highest criticalities by Gaiotto, Seiberg and Tachikawa, we discuss physics of certain... | 15.874413 | 13.145865 | 16.967133 | 13.08591 | 13.233421 | 13.189648 | 12.215706 | 13.449645 | 12.191478 | 16.201614 | 13.603243 | 12.957703 | 14.296028 | 13.190812 | 12.746663 | 12.67585 | 12.736073 | 13.063771 | 13.075699 | 13.881599 | 12.75664 |
hep-th/0303126 | Jesper Jacobsen | Vladimir S Dotsenko, Jesper Lykke Jacobsen, Raoul Santachiara | Parafermionic theory with the symmetry Z_N, for N odd | 34 pages, 1 figure. v2: note added in proof | Nucl.Phys. B664 (2003) 477-511 | 10.1016/S0550-3213(03)00391-2 | null | hep-th cond-mat | null | We construct a parafermionic conformal theory with the symmetry Z_N, for N
odd, based on the second solution of Fateev-Zamolodchikov for the corresponding
parafermionic chiral algebra. Primary operators are classified according to
their transformation properties under the dihedral group D_N, as singlet,
doublet 1,2,.... | [
{
"created": "Fri, 14 Mar 2003 07:08:02 GMT",
"version": "v1"
},
{
"created": "Wed, 7 May 2003 14:08:24 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dotsenko",
"Vladimir S",
""
],
[
"Jacobsen",
"Jesper Lykke",
""
],
[
"Santachiara",
"Raoul",
""
]
] | We construct a parafermionic conformal theory with the symmetry Z_N, for N odd, based on the second solution of Fateev-Zamolodchikov for the corresponding parafermionic chiral algebra. Primary operators are classified according to their transformation properties under the dihedral group D_N, as singlet, doublet 1,2,...... | 10.631967 | 9.439847 | 11.786328 | 10.001905 | 9.794388 | 10.240703 | 8.961185 | 10.457006 | 10.066424 | 13.938271 | 10.267652 | 10.095793 | 11.271168 | 10.513954 | 10.53564 | 9.98726 | 10.719961 | 10.521073 | 10.725942 | 11.398867 | 10.413898 |
hep-th/0508091 | Stoil Donev | Stoil Donev, Maria Tashkova | Integrability-Nonintegrability Structures and Individual Photons'
Description as Finite Field Objects | 17 pages, no figures, Latex | null | null | null | hep-th math-ph math.MP | null | This paper presents an attempt to come to a natural field model of individual
photons considered as finite entities and propagating along some distinguished
direction in space in a consistent translational-rotational manner. The
starting assumption reflects their most trustful property to propagate
translationally in... | [
{
"created": "Fri, 12 Aug 2005 12:53:03 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Donev",
"Stoil",
""
],
[
"Tashkova",
"Maria",
""
]
] | This paper presents an attempt to come to a natural field model of individual photons considered as finite entities and propagating along some distinguished direction in space in a consistent translational-rotational manner. The starting assumption reflects their most trustful property to propagate translationally in a... | 21.293261 | 22.820131 | 20.625412 | 21.895191 | 23.328239 | 21.61779 | 22.577827 | 21.337357 | 21.609795 | 21.756964 | 22.162254 | 21.030039 | 20.018549 | 20.306868 | 20.197884 | 20.958712 | 21.375912 | 20.273039 | 20.63122 | 21.160872 | 20.863503 |
2008.10739 | Elda Guzman Elda Guzman-Herrera | Elda Guzman-Herrera and Nora Breton | Euler-Heisenberg waves propagating in a magnetic background | 15 pages, 5 figures, 7 plots | null | 10.1140/epjc/s10052-020-08783-1 | null | hep-th gr-qc physics.optics | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the Euler-Heisenberg solutions that describe electromagnetic waves
propagating through very intense uniform magnetic or electric background, with
the effective metric approach. We first explore the case of a magnetic
background: as a result of the interaction between the wave and the background
there is bir... | [
{
"created": "Mon, 24 Aug 2020 22:40:22 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Dec 2020 02:08:25 GMT",
"version": "v2"
}
] | 2021-02-24 | [
[
"Guzman-Herrera",
"Elda",
""
],
[
"Breton",
"Nora",
""
]
] | We derive the Euler-Heisenberg solutions that describe electromagnetic waves propagating through very intense uniform magnetic or electric background, with the effective metric approach. We first explore the case of a magnetic background: as a result of the interaction between the wave and the background there is biref... | 10.95191 | 12.11769 | 10.629622 | 10.792114 | 12.463496 | 12.283665 | 11.884562 | 10.843113 | 10.481797 | 11.011294 | 11.12764 | 11.006696 | 10.951567 | 10.818958 | 11.213643 | 11.229179 | 11.241336 | 10.694701 | 11.117492 | 10.518891 | 10.759652 |
hep-th/9709066 | Mike Cassidy | M. J. Cassidy and S. W. Hawking | Models for Chronology Selection | 20 pages, Latex | Phys.Rev. D57 (1998) 2372-2380 | 10.1103/PhysRevD.57.2372 | DAMTP R-97/47 | hep-th | null | In this paper, we derive an expression for the grand canonical partition
function for a fluid of hot, rotating massless scalar field particles in the
Einstein universe. We consider the number of states with a given energy as one
increases the angular momentum so that the fluid rotates with an increasing
angular veloc... | [
{
"created": "Tue, 9 Sep 1997 08:07:13 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Cassidy",
"M. J.",
""
],
[
"Hawking",
"S. W.",
""
]
] | In this paper, we derive an expression for the grand canonical partition function for a fluid of hot, rotating massless scalar field particles in the Einstein universe. We consider the number of states with a given energy as one increases the angular momentum so that the fluid rotates with an increasing angular velocit... | 8.616304 | 9.01031 | 8.199286 | 7.815849 | 9.107486 | 8.922338 | 8.748893 | 8.368862 | 8.165135 | 8.616139 | 8.268766 | 8.479747 | 8.058237 | 8.041652 | 8.219837 | 8.102774 | 8.244853 | 8.117908 | 7.831506 | 8.1986 | 8.185506 |
hep-th/0404051 | Jeong-Hyuck Park | Sangmin Lee and Jeong-Hyuck Park | Noncentral extension of the $AdS_{5} \times S^{5}$ superalgebra:
supermultiplet of brane charges | 1+29 pages, no figure; comments and refs added, to appear in JHEP | JHEP 0406:038,2004 | 10.1088/1126-6708/2004/06/038 | IHES/P/04/15, STR-04-007, CERN-PH-TH/2004-064 | hep-th math-ph math.MP | null | We propose an extension of the su(2,2|4) superalgebra to incorporate the
$F1/D1$ string charges in type IIB string theory on the $AdS_{5} \times S^{5}$
background, or the electro-magnetic charges in the dual super Yang-Mills
theory. With the charges introduced, the superalgebra inevitably undergoes a
noncentral exten... | [
{
"created": "Tue, 6 Apr 2004 16:12:12 GMT",
"version": "v1"
},
{
"created": "Tue, 25 May 2004 09:28:43 GMT",
"version": "v2"
}
] | 2009-05-13 | [
[
"Lee",
"Sangmin",
""
],
[
"Park",
"Jeong-Hyuck",
""
]
] | We propose an extension of the su(2,2|4) superalgebra to incorporate the $F1/D1$ string charges in type IIB string theory on the $AdS_{5} \times S^{5}$ background, or the electro-magnetic charges in the dual super Yang-Mills theory. With the charges introduced, the superalgebra inevitably undergoes a noncentral extensi... | 9.367268 | 8.588051 | 9.739256 | 8.910899 | 9.018532 | 9.523206 | 9.068374 | 8.701951 | 8.384693 | 11.416376 | 8.714465 | 8.596487 | 9.342602 | 8.872656 | 8.790204 | 8.759336 | 8.80404 | 8.647868 | 8.971156 | 9.349149 | 8.906806 |
hep-th/0703125 | Hugo Garcia-Compean | I. Galaviz, H. Garcia-Compean, M. Przanowski, F.J. Turrubiates | Deformation Quantization of Fermi Fields | 19+1 pages, no figures, revtex4 file style | Annals Phys.323:827-844,2008 | 10.1016/j.aop.2007.05.006 | Cinvestav-13-07 | hep-th | null | Deformation quantization for any Grassmann scalar free field is described via
the Weyl-Wigner-Moyal formalism. The Stratonovich-Weyl quantizer, the Moyal
$\star$-product and the Wigner functional are obtained by extending the
formalism proposed recently in [35] to the fermionic systems of infinite number
of degrees o... | [
{
"created": "Wed, 14 Mar 2007 00:43:42 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Galaviz",
"I.",
""
],
[
"Garcia-Compean",
"H.",
""
],
[
"Przanowski",
"M.",
""
],
[
"Turrubiates",
"F. J.",
""
]
] | Deformation quantization for any Grassmann scalar free field is described via the Weyl-Wigner-Moyal formalism. The Stratonovich-Weyl quantizer, the Moyal $\star$-product and the Wigner functional are obtained by extending the formalism proposed recently in [35] to the fermionic systems of infinite number of degrees of ... | 8.107317 | 7.335869 | 7.908438 | 6.996119 | 7.069917 | 6.895784 | 6.948417 | 6.586549 | 6.895875 | 8.523028 | 7.198543 | 7.06612 | 7.428138 | 6.9048 | 6.988006 | 7.077733 | 7.173931 | 7.130202 | 6.952988 | 7.17065 | 7.055327 |
0810.3296 | Mohammad Reza Setare | M. R. Setare and E. N. Saridakis | Correspondence between Holographic and Gauss-Bonnet dark energy models | 10 pages, no figures. Has been accepted for publication in Physics
Letters B | Phys.Lett.B670:1-4,2008 | 10.1016/j.physletb.2008.10.029 | null | hep-th astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present work we investigate the cosmological implications of
holographic dark energy density in the Gauss-Bonnet framework. By formulating
independently the two cosmological scenarios, and by enforcing their
simultaneous validity, we show that there is a correspondence between the
holographic dark energy scena... | [
{
"created": "Sat, 18 Oct 2008 08:17:03 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"Setare",
"M. R.",
""
],
[
"Saridakis",
"E. N.",
""
]
] | In the present work we investigate the cosmological implications of holographic dark energy density in the Gauss-Bonnet framework. By formulating independently the two cosmological scenarios, and by enforcing their simultaneous validity, we show that there is a correspondence between the holographic dark energy scenari... | 12.116285 | 11.009729 | 10.823409 | 10.86412 | 10.603081 | 11.10133 | 11.041622 | 10.266831 | 10.355033 | 11.238098 | 10.995599 | 10.846332 | 11.41156 | 10.948616 | 11.116617 | 11.207285 | 10.985952 | 10.66178 | 11.192782 | 11.603998 | 11.218957 |
hep-th/0008079 | Mikhail Shaposhnikov | Seif Randjbar-Daemi and Mikhail Shaposhnikov | Fermion zero-modes on brane-worlds | Latex, 5 pages. A factor "2" mistake that propagated through a number
of equations is corrected. Conclusions unchanged | Phys.Lett. B492 (2000) 361-364 | 10.1016/S0370-2693(00)01100-X | UNIL-IPT-00-17, IC/2000/134 | hep-th hep-ph | null | We study localization of bulk fermions on a brane with inclusion of
Yang-Mills and scalar backgrounds in higher dimensions and give the conditions
under which localized chiral fermions can be obtained.
| [
{
"created": "Wed, 9 Aug 2000 14:38:32 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Sep 2000 15:08:52 GMT",
"version": "v2"
},
{
"created": "Mon, 18 Jun 2001 08:05:12 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Randjbar-Daemi",
"Seif",
""
],
[
"Shaposhnikov",
"Mikhail",
""
]
] | We study localization of bulk fermions on a brane with inclusion of Yang-Mills and scalar backgrounds in higher dimensions and give the conditions under which localized chiral fermions can be obtained. | 16.69582 | 6.362298 | 10.701361 | 8.319304 | 8.589573 | 9.031633 | 7.805586 | 8.069635 | 8.26081 | 10.884745 | 9.088369 | 9.505537 | 10.791792 | 9.931207 | 9.976852 | 9.703461 | 10.300012 | 9.80328 | 10.187304 | 11.210532 | 9.960239 |
0801.0234 | Orlando Alvarez | Orlando Alvarez, Blazej Ruszczycki | Target Space Duality: The Dilaton Field | 11 pages | null | null | null | hep-th | null | Classical target space duality transformations are studied for the non-linear
sigma model with a dilaton field. Working within the framework of the
Hamiltonian formalism we require the duality transformation to be a property
only of the target spaces. We obtain a set of restrictions on the geometrical
data.
| [
{
"created": "Mon, 31 Dec 2007 19:29:59 GMT",
"version": "v1"
}
] | 2008-01-03 | [
[
"Alvarez",
"Orlando",
""
],
[
"Ruszczycki",
"Blazej",
""
]
] | Classical target space duality transformations are studied for the non-linear sigma model with a dilaton field. Working within the framework of the Hamiltonian formalism we require the duality transformation to be a property only of the target spaces. We obtain a set of restrictions on the geometrical data. | 14.15676 | 9.886358 | 11.630283 | 9.859079 | 10.712919 | 11.165008 | 11.088873 | 10.388235 | 10.318665 | 12.470014 | 9.762986 | 10.348769 | 11.9266 | 10.357334 | 10.701327 | 10.546378 | 10.62518 | 9.968431 | 10.18513 | 11.677351 | 10.548881 |
hep-th/0007111 | G. Vlasov | G. Vlasov (Moscow Aviat. and Landau) | The superfluidity of fermions coupled to gravity | LaTeX, 10 pages, no figures | null | null | null | hep-th gr-qc hep-ph | null | We investigate superfluidity of the relativistic fermi-gas with gravitational
interaction. The excitation spectrum is obtained within the linearized theory.
While superfluidity may take place at a definite ratio of the Fermi momentum,
rest mass and coupling constant, the metric coefficients play predominant role
form... | [
{
"created": "Fri, 14 Jul 2000 13:35:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Vlasov",
"G.",
"",
"Moscow Aviat. and Landau"
]
] | We investigate superfluidity of the relativistic fermi-gas with gravitational interaction. The excitation spectrum is obtained within the linearized theory. While superfluidity may take place at a definite ratio of the Fermi momentum, rest mass and coupling constant, the metric coefficients play predominant role formin... | 20.472307 | 21.986216 | 18.389782 | 20.063559 | 18.727341 | 20.721128 | 19.922981 | 18.61569 | 18.916965 | 21.293911 | 18.921356 | 18.759481 | 20.637491 | 19.042837 | 19.053701 | 19.293064 | 19.292534 | 19.198425 | 18.52973 | 19.984585 | 18.572596 |
1702.06935 | Masanori Hanada | Masanori Hanada, Hidehiko Shimada and Masaki Tezuka | Universality in Chaos: Lyapunov Spectrum and Random Matrix Theory | 5 pages + supplementary materials. v2: minor corrections, references
added. v3: a lot more evidence added. v4: the version appeared in Phys. Rev.
E | Phys. Rev. E 97, 022224 (2018) | 10.1103/PhysRevE.97.022224 | null | hep-th math-ph math.MP nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose the existence of a new universality in classical chaotic systems
when the number of degrees of freedom is large: the statistical property of the
Lyapunov spectrum is described by Random Matrix Theory. We demonstrate it by
studying the finite-time Lyapunov exponents of the matrix model of a stringy
black ho... | [
{
"created": "Wed, 22 Feb 2017 18:36:24 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Apr 2017 04:41:15 GMT",
"version": "v2"
},
{
"created": "Mon, 16 Oct 2017 04:16:55 GMT",
"version": "v3"
},
{
"created": "Mon, 12 Mar 2018 01:27:38 GMT",
"version": "v4"
}
] | 2018-03-13 | [
[
"Hanada",
"Masanori",
""
],
[
"Shimada",
"Hidehiko",
""
],
[
"Tezuka",
"Masaki",
""
]
] | We propose the existence of a new universality in classical chaotic systems when the number of degrees of freedom is large: the statistical property of the Lyapunov spectrum is described by Random Matrix Theory. We demonstrate it by studying the finite-time Lyapunov exponents of the matrix model of a stringy black hole... | 8.951169 | 8.289295 | 9.418661 | 8.549441 | 8.630398 | 8.974705 | 9.212976 | 8.791176 | 8.352614 | 11.186164 | 8.5124 | 8.096446 | 9.647868 | 8.388265 | 8.426562 | 8.179373 | 8.21355 | 8.046765 | 8.86088 | 9.152782 | 8.319218 |
hep-th/0112182 | Andrew K. Waldron | Stanley Deser and Andrew Waldron | Inconsistencies of Massive Charged Gravitating Higher Spins | 25 pages, latex | Nucl.Phys.B631:369-387,2002 | 10.1016/S0550-3213(02)00199-2 | BRX-TH 478 | hep-th gr-qc hep-ph nucl-th | null | We examine the causality and degrees of freedom (DoF) problems encountered by
charged, gravitating, massive higher spin fields. For spin s=3/2, making the
metric dynamical yields improved causality bounds. These involve only the mass,
the product eM_P of the charge and Planck mass and the cosmological constant
\Lambd... | [
{
"created": "Wed, 19 Dec 2001 20:13:12 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Deser",
"Stanley",
""
],
[
"Waldron",
"Andrew",
""
]
] | We examine the causality and degrees of freedom (DoF) problems encountered by charged, gravitating, massive higher spin fields. For spin s=3/2, making the metric dynamical yields improved causality bounds. These involve only the mass, the product eM_P of the charge and Planck mass and the cosmological constant \Lambda.... | 16.588028 | 17.452694 | 15.815748 | 15.213134 | 16.110952 | 16.926321 | 16.879517 | 15.362952 | 16.074743 | 18.579575 | 15.765924 | 15.608034 | 15.861163 | 15.456516 | 15.743661 | 15.979381 | 16.095848 | 15.520666 | 15.494491 | 15.802272 | 15.465482 |
1309.2189 | Erik Tonni | Andrea Coser, Luca Tagliacozzo, Erik Tonni | On R\'enyi entropies of disjoint intervals in conformal field theory | 66 pages, 34 figures | J. Stat. Mech. (2014) P01008 | 10.1088/1742-5468/2014/01/P01008 | null | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the R\'enyi entropies of N disjoint intervals in the conformal field
theories given by the free compactified boson and the Ising model. They are
computed as the 2N point function of twist fields, by employing the partition
function of the model on a particular class of Riemann surfaces. The results
are writt... | [
{
"created": "Mon, 9 Sep 2013 15:20:50 GMT",
"version": "v1"
}
] | 2014-01-27 | [
[
"Coser",
"Andrea",
""
],
[
"Tagliacozzo",
"Luca",
""
],
[
"Tonni",
"Erik",
""
]
] | We study the R\'enyi entropies of N disjoint intervals in the conformal field theories given by the free compactified boson and the Ising model. They are computed as the 2N point function of twist fields, by employing the partition function of the model on a particular class of Riemann surfaces. The results are written... | 7.086367 | 6.330725 | 9.11859 | 6.615602 | 7.273073 | 6.809002 | 6.188269 | 6.486611 | 6.847316 | 10.090061 | 6.266613 | 6.723768 | 7.300831 | 6.830139 | 6.717175 | 6.743765 | 6.834949 | 6.627145 | 6.613392 | 7.21653 | 6.468915 |
2108.13542 | Yuji Tachikawa | Yuji Tachikawa and Mayuko Yamashita | Topological modular forms and the absence of all heterotic global
anomalies | 36 pages; v2: incorporates many suggestions by a helpful anonymous
referee | null | 10.1007/s00220-023-04761-2 | null | hep-th math-ph math.AT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reformulate the question of the absence of global anomalies of heterotic
string theory mathematically in terms of a certain natural transformation
$\mathrm{TMF}^\bullet\to (I_{\mathbb{Z}}\Omega^\text{string})^{\bullet-20}$,
from topological modular forms to the Anderson dual of string bordism groups,
using the Seg... | [
{
"created": "Mon, 30 Aug 2021 22:41:06 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Apr 2023 14:09:14 GMT",
"version": "v2"
}
] | 2023-07-26 | [
[
"Tachikawa",
"Yuji",
""
],
[
"Yamashita",
"Mayuko",
""
]
] | We reformulate the question of the absence of global anomalies of heterotic string theory mathematically in terms of a certain natural transformation $\mathrm{TMF}^\bullet\to (I_{\mathbb{Z}}\Omega^\text{string})^{\bullet-20}$, from topological modular forms to the Anderson dual of string bordism groups, using the Segal... | 7.969151 | 8.399227 | 8.943816 | 7.143925 | 8.03171 | 7.989759 | 8.088222 | 8.57775 | 7.670027 | 9.552563 | 7.564477 | 7.3551 | 7.608458 | 7.122722 | 7.335331 | 7.283529 | 7.255196 | 7.292207 | 7.264819 | 7.653116 | 7.030092 |
1804.10124 | Masataka Matsumoto | Masataka Matsumoto and Shin Nakamura | Critical Exponents of Nonequilibrium Phase Transitions in AdS/CFT
Correspondence | 8 pages, 14 figures. v2: typos corrected, published version in PRD | Phys. Rev. D 98, 106027 (2018) | 10.1103/PhysRevD.98.106027 | null | hep-th cond-mat.stat-mech cond-mat.str-el nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study critical phenomena of nonequilibrium phase transitions by using the
AdS/CFT correspondence. Our system consists of charged particles interacting
with a heat bath of neutral gauge particles. The system is in current-driven
nonequilibrium steady state, and the nonequilibrium phase transition is
associated with... | [
{
"created": "Thu, 26 Apr 2018 15:57:57 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Dec 2018 19:30:09 GMT",
"version": "v2"
}
] | 2018-12-06 | [
[
"Matsumoto",
"Masataka",
""
],
[
"Nakamura",
"Shin",
""
]
] | We study critical phenomena of nonequilibrium phase transitions by using the AdS/CFT correspondence. Our system consists of charged particles interacting with a heat bath of neutral gauge particles. The system is in current-driven nonequilibrium steady state, and the nonequilibrium phase transition is associated with n... | 7.435768 | 6.766271 | 7.073825 | 6.607473 | 6.519092 | 6.797303 | 6.394207 | 6.750016 | 6.599048 | 7.627022 | 6.65024 | 7.053859 | 6.921372 | 6.85011 | 6.745396 | 7.01398 | 7.044055 | 6.956581 | 7.223491 | 6.929226 | 7.023038 |
0906.3518 | Alexei Morozov | A.Morozov | Unitary Integrals and Related Matrix Models | 27 pages | Theor.Math.Phys.162:1-33,2010; Teor.Mat.Fiz.161:3-40,2010 | 10.1007/s11232-010-0001-y | ITEP/TH-20/09 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Concise review of the basic properties of unitary matrix integrals. They are
studied with the help of the three matrix models: the ordinary unitary model,
Brezin-Gross-Witten model and the Harish-Charndra-Itzykson-Zuber model.
Especial attention is paid to the tricky sides of the story, from De
Wit-t'Hooft anomaly in... | [
{
"created": "Thu, 18 Jun 2009 20:14:16 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Oct 2010 21:43:37 GMT",
"version": "v2"
},
{
"created": "Tue, 12 Oct 2010 05:34:08 GMT",
"version": "v3"
}
] | 2011-04-07 | [
[
"Morozov",
"A.",
""
]
] | Concise review of the basic properties of unitary matrix integrals. They are studied with the help of the three matrix models: the ordinary unitary model, Brezin-Gross-Witten model and the Harish-Charndra-Itzykson-Zuber model. Especial attention is paid to the tricky sides of the story, from De Wit-t'Hooft anomaly in u... | 15.693596 | 15.667056 | 17.167742 | 15.120543 | 15.314905 | 14.829226 | 16.404766 | 16.240648 | 14.192024 | 20.090361 | 14.842179 | 14.347857 | 15.74878 | 14.669969 | 14.363219 | 14.566804 | 14.540413 | 14.928877 | 13.970162 | 14.642682 | 14.667768 |
1410.4594 | Mikhail Isachenkov | Mikhail Isachenkov, Ingo Kirsch, Volker Schomerus | Chiral Ring of Strange Metals: The Multicolor Limit | 25 pages, 4 figures | null | 10.1016/j.nuclphysb.2015.06.010 | DESY 14-169 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The low energy limit of a dense 2D adjoint QCD is described by a family of
${\cal N}=(2,2)$ supersymmetric coset conformal field theories. In previous
work we constructed chiral primaries for a small number $N < 6$ of colors. Our
aim in the present note is to determine the chiral ring in the multicolor limit
where $N... | [
{
"created": "Thu, 16 Oct 2014 21:34:14 GMT",
"version": "v1"
}
] | 2015-12-09 | [
[
"Isachenkov",
"Mikhail",
""
],
[
"Kirsch",
"Ingo",
""
],
[
"Schomerus",
"Volker",
""
]
] | The low energy limit of a dense 2D adjoint QCD is described by a family of ${\cal N}=(2,2)$ supersymmetric coset conformal field theories. In previous work we constructed chiral primaries for a small number $N < 6$ of colors. Our aim in the present note is to determine the chiral ring in the multicolor limit where $N$ ... | 8.881051 | 7.90489 | 10.106731 | 8.386961 | 8.789851 | 8.863418 | 8.22013 | 7.85504 | 7.574956 | 9.865341 | 8.054749 | 7.981553 | 8.749064 | 7.871572 | 8.298642 | 8.487625 | 8.290285 | 8.19467 | 7.987186 | 8.850849 | 7.965012 |
2406.04125 | Takayuki Hirayama | Takayuki Hirayama | Particle creation using the classical stochastic method | 8 pages | null | null | null | hep-th hep-lat quant-ph | http://creativecommons.org/licenses/by/4.0/ | We compute the particle creation of a harmonic oscillator using the classical
stochastic method. This method reproduces all the vacuum expectation values in
quantum theory. We prepare the vacuum state at the initial time and evolve it
over time using Langevin equations of motion. By averaging over the ensemble,
we co... | [
{
"created": "Thu, 6 Jun 2024 14:47:45 GMT",
"version": "v1"
}
] | 2024-06-07 | [
[
"Hirayama",
"Takayuki",
""
]
] | We compute the particle creation of a harmonic oscillator using the classical stochastic method. This method reproduces all the vacuum expectation values in quantum theory. We prepare the vacuum state at the initial time and evolve it over time using Langevin equations of motion. By averaging over the ensemble, we comp... | 10.36629 | 10.270927 | 9.345171 | 9.525674 | 10.342906 | 9.459243 | 10.778928 | 9.20346 | 10.002172 | 10.344433 | 9.487897 | 10.180939 | 10.393175 | 10.001491 | 9.91709 | 9.651795 | 9.954979 | 9.764899 | 9.779552 | 10.620565 | 9.398643 |
2202.02986 | Yunfeng Jiang | Janko B\"ohm, Jesper Lykke Jacobsen, Yunfeng Jiang, Yang Zhang | Geometric Algebra and Algebraic Geometry of Loop and Potts Models | 66 pages | null | 10.1007/JHEP05(2022)068 | USTC-ICTS/PCFT-22-03 | hep-th cond-mat.stat-mech nlin.SI | http://creativecommons.org/licenses/by/4.0/ | We uncover a connection between two seemingly separate subjects in integrable
models: the representation theory of the affine Temperley-Lieb algebra, and the
algebraic structure of solutions to the Bethe equations of the XXZ spin chain.
We study the solution of Bethe equations analytically by computational
algebraic ... | [
{
"created": "Mon, 7 Feb 2022 07:56:03 GMT",
"version": "v1"
}
] | 2022-06-01 | [
[
"Böhm",
"Janko",
""
],
[
"Jacobsen",
"Jesper Lykke",
""
],
[
"Jiang",
"Yunfeng",
""
],
[
"Zhang",
"Yang",
""
]
] | We uncover a connection between two seemingly separate subjects in integrable models: the representation theory of the affine Temperley-Lieb algebra, and the algebraic structure of solutions to the Bethe equations of the XXZ spin chain. We study the solution of Bethe equations analytically by computational algebraic ge... | 9.909104 | 8.578032 | 11.651362 | 9.387575 | 8.8153 | 9.903641 | 8.743088 | 9.764229 | 8.926281 | 11.656603 | 9.324662 | 9.112447 | 9.687414 | 9.462108 | 9.334229 | 8.999227 | 9.18176 | 9.318735 | 9.269478 | 9.842371 | 9.004836 |
0704.1085 | Teruhiko Kawano | Teruhiko Kawano, Hirosi Ooguri, and Yutaka Ookouchi | Gauge Mediation in String Theory | 7 pages, 1 figure, harvmac. v2: references added and typos corrected | Phys.Lett.B652:40-42,2007 | 10.1016/j.physletb.2007.06.056 | CALT-68-2642, UT-07-12 | hep-th hep-ph | null | We show that a large class of phenomenologically viable models for gauge
mediation of supersymmetry breaking based on meta-stable vacua can be realized
in local Calabi-Yau compactifications of string theory.
| [
{
"created": "Mon, 9 Apr 2007 09:03:00 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Apr 2007 10:23:39 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Kawano",
"Teruhiko",
""
],
[
"Ooguri",
"Hirosi",
""
],
[
"Ookouchi",
"Yutaka",
""
]
] | We show that a large class of phenomenologically viable models for gauge mediation of supersymmetry breaking based on meta-stable vacua can be realized in local Calabi-Yau compactifications of string theory. | 7.892327 | 5.263704 | 5.633092 | 4.760918 | 5.627146 | 5.237077 | 5.476138 | 5.364018 | 4.788173 | 5.617718 | 5.263236 | 5.884874 | 6.041378 | 5.712359 | 5.605561 | 6.384467 | 5.829125 | 6.177547 | 5.411101 | 5.621171 | 5.544224 |
0902.4387 | Ahmad Ghodsi | Mohammad R. Garousi, Ahmad Ghodsi | The RN/CFT Correspondence | 14 pages, latex; Version published in PLB. | Phys.Lett.B687:79-83,2010 | 10.1016/j.physletb.2010.03.002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently it has been shown in 0901.0931 [hep-th] that the approach to
extremality for the non-extremal Reissner-Nordstrom black hole is not
continuous. The non-extremal RN black hole splits into two spacetimes at the
extremality: an extremal black hole and a disconnected $AdS_2\times S^2$ space
which has been called ... | [
{
"created": "Wed, 25 Feb 2009 15:06:04 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Mar 2009 13:42:04 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Mar 2009 13:18:03 GMT",
"version": "v3"
},
{
"created": "Sun, 23 Aug 2009 11:33:36 GMT",
"version": "v4"
},
{
"cr... | 2014-11-18 | [
[
"Garousi",
"Mohammad R.",
""
],
[
"Ghodsi",
"Ahmad",
""
]
] | Recently it has been shown in 0901.0931 [hep-th] that the approach to extremality for the non-extremal Reissner-Nordstrom black hole is not continuous. The non-extremal RN black hole splits into two spacetimes at the extremality: an extremal black hole and a disconnected $AdS_2\times S^2$ space which has been called th... | 6.10253 | 5.412029 | 6.155589 | 5.437856 | 5.654632 | 5.189694 | 5.078043 | 5.356259 | 5.531724 | 5.903593 | 5.211144 | 5.504288 | 5.835491 | 5.43595 | 5.590143 | 5.617381 | 5.480145 | 5.591619 | 5.479839 | 5.708734 | 5.490377 |
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