id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1903.04718 | Toshihiro Ota | Tetsuya Akutagawa, Koji Hashimoto, Keiju Murata, Toshihiro Ota | Chaos of QCD string from holography | 12 pages, 13 figures | Phys. Rev. D 100, 046009 (2019) | 10.1103/PhysRevD.100.046009 | OU-HET-1000 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is challenging to quantify chaos of QCD, because non-perturbative QCD
accompanies non-local observables. By using holography, we find that QCD
strings at large $N_c$ and strong coupling limit exhibit chaos, and measure
their Lyapunov exponent at zero temperature. A pair of a quark and an antiquark
separated by $L_... | [
{
"created": "Tue, 12 Mar 2019 04:02:35 GMT",
"version": "v1"
}
] | 2019-08-14 | [
[
"Akutagawa",
"Tetsuya",
""
],
[
"Hashimoto",
"Koji",
""
],
[
"Murata",
"Keiju",
""
],
[
"Ota",
"Toshihiro",
""
]
] | It is challenging to quantify chaos of QCD, because non-perturbative QCD accompanies non-local observables. By using holography, we find that QCD strings at large $N_c$ and strong coupling limit exhibit chaos, and measure their Lyapunov exponent at zero temperature. A pair of a quark and an antiquark separated by $L_q$... | 9.538869 | 9.959513 | 10.128135 | 9.624085 | 9.028641 | 9.581627 | 9.159441 | 9.45913 | 9.325275 | 11.112879 | 9.059866 | 9.52046 | 9.405906 | 9.477714 | 9.809637 | 9.932324 | 9.740308 | 10.006669 | 9.211798 | 9.655137 | 9.32055 |
1306.1734 | Marcos Marino | Yasuyuki Hatsuda, Marcos Marino, Sanefumi Moriyama and Kazumi Okuyama | Non-perturbative effects and the refined topological string | 38 pages, 5 figures | null | 10.1007/JHEP09(2014)168 | DESY 13-096, TIT/HEP-627 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The partition function of ABJM theory on the three-sphere has
non-perturbative corrections due to membrane instantons in the M-theory dual.
We show that the full series of membrane instanton corrections is completely
determined by the refined topological string on the Calabi-Yau manifold known
as local P1xP1, in the ... | [
{
"created": "Fri, 7 Jun 2013 14:11:30 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Hatsuda",
"Yasuyuki",
""
],
[
"Marino",
"Marcos",
""
],
[
"Moriyama",
"Sanefumi",
""
],
[
"Okuyama",
"Kazumi",
""
]
] | The partition function of ABJM theory on the three-sphere has non-perturbative corrections due to membrane instantons in the M-theory dual. We show that the full series of membrane instanton corrections is completely determined by the refined topological string on the Calabi-Yau manifold known as local P1xP1, in the Ne... | 4.126149 | 3.95648 | 6.302338 | 4.190354 | 4.203156 | 4.085031 | 4.061755 | 3.903171 | 4.226048 | 5.490764 | 4.129142 | 4.184379 | 4.608846 | 4.067402 | 4.23401 | 4.379722 | 4.330308 | 4.227266 | 4.111035 | 4.679012 | 4.107596 |
hep-th/0009180 | Miele Gennaro | Fedele Lizzi, Gianpiero Mangano and Gennaro Miele | Another Alternative to Compactification: Noncommutative Geometry and
Randall-Sundrum Models | 7 pages, LaTeX | Mod.Phys.Lett. A16 (2001) 1-8 | 10.1142/S021773230100305X | DSF 29/2000 | hep-th hep-ph math-ph math.MP | null | We observe that the main feature of the Randall-Sundrum model, used to solve
the hierarchy problem, is already present in a class of Yang-Mills plus gravity
theories inspired by noncommutative geometry. Strikingly the same expression
for the Higgs potential is found in two models which have no apparent
connection. So... | [
{
"created": "Fri, 22 Sep 2000 15:05:12 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Lizzi",
"Fedele",
""
],
[
"Mangano",
"Gianpiero",
""
],
[
"Miele",
"Gennaro",
""
]
] | We observe that the main feature of the Randall-Sundrum model, used to solve the hierarchy problem, is already present in a class of Yang-Mills plus gravity theories inspired by noncommutative geometry. Strikingly the same expression for the Higgs potential is found in two models which have no apparent connection. Some... | 12.8712 | 10.949514 | 11.607831 | 11.117387 | 10.502707 | 11.863149 | 10.974732 | 10.531707 | 11.059492 | 12.48938 | 10.591334 | 10.68619 | 10.795012 | 10.679436 | 10.315516 | 10.558442 | 10.704877 | 10.674584 | 11.041911 | 10.483874 | 10.649595 |
1509.08370 | Ahmad Mohamadnejad | Ahmad Mohamadnejad | Reformulation of the Georgi-Glashow model and some constraints on its
classical fields | 17 pages | Phys. Rev. D 92, 125029 (2015) | 10.1103/PhysRevD.92.125029 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the SU(2) Georgi-Glashow model and suggest a decomposition for its
fields and obtain a Lagrangian based on new variables. We use Cho's restricted
decomposition as a result of a vacuum condition of the Georgi-Glashow model.
This model with no external sources leads us to the Cho extended decomposition.
We int... | [
{
"created": "Mon, 28 Sep 2015 15:50:09 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Jan 2016 17:13:02 GMT",
"version": "v2"
}
] | 2016-01-11 | [
[
"Mohamadnejad",
"Ahmad",
""
]
] | We study the SU(2) Georgi-Glashow model and suggest a decomposition for its fields and obtain a Lagrangian based on new variables. We use Cho's restricted decomposition as a result of a vacuum condition of the Georgi-Glashow model. This model with no external sources leads us to the Cho extended decomposition. We inter... | 15.551729 | 15.431607 | 15.87749 | 16.168434 | 17.05315 | 15.576629 | 15.591312 | 15.051682 | 15.577854 | 17.33182 | 14.711113 | 16.050016 | 15.618609 | 15.507148 | 15.146579 | 15.801147 | 15.956849 | 15.977259 | 15.440716 | 16.104116 | 15.470147 |
1105.3172 | Zheng Sun | Zheng Sun | Vacuum statistics and parameter tuning for F-term supersymmetry breaking | 18 pages, 1 figure; v2: add references, published version | JHEP 1109:107,2011 | 10.1007/JHEP09(2011)107 | TIFR/TH/11-22 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We carry out a model-independent EFT method study on the vacuum statistics of
general F-term SUSY breaking models. Assuming a smooth distribution of
Lagrangian parameters, SUSY breaking vacua are rare in global SUSY models with
a canonical K\"ahler potential, and have a peaked distribution near the cut-off
of the SUS... | [
{
"created": "Mon, 16 May 2011 18:49:10 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Nov 2011 19:17:25 GMT",
"version": "v2"
}
] | 2013-10-08 | [
[
"Sun",
"Zheng",
""
]
] | We carry out a model-independent EFT method study on the vacuum statistics of general F-term SUSY breaking models. Assuming a smooth distribution of Lagrangian parameters, SUSY breaking vacua are rare in global SUSY models with a canonical K\"ahler potential, and have a peaked distribution near the cut-off of the SUSY ... | 10.825672 | 10.329757 | 10.365328 | 9.531151 | 9.945489 | 10.180129 | 10.025663 | 10.115749 | 9.726489 | 11.404716 | 10.624142 | 10.141328 | 10.250837 | 9.807904 | 10.082151 | 9.947223 | 10.374231 | 10.313945 | 9.876639 | 10.235023 | 10.161668 |
0812.0526 | El Hassan Saidi | Lalla Btissam Drissi, Houda Jehjouh, El Hassan Saidi | Topological String on Toric CY3s in Large Complex Structure Limit | Latex, 38 pages, 12 figures. To appear in Nucl Phys B | Nucl.Phys.B813:315-348,2009 | 10.1016/j.nuclphysb.2008.11.030 | Lab/UFR-HEP-0807-GNPHE-0807 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a non planar topological vertex formalism and we use it to study
the A-model partition function $\mathcal{Z}_{top}$ of topological string on the
class of toric Calabi-Yau threefolds (CY3) in large complex structure limit. To
that purpose, we first consider the $T^{2}\times R$ special Lagrangian
fibration o... | [
{
"created": "Tue, 2 Dec 2008 15:03:43 GMT",
"version": "v1"
}
] | 2009-03-12 | [
[
"Drissi",
"Lalla Btissam",
""
],
[
"Jehjouh",
"Houda",
""
],
[
"Saidi",
"El Hassan",
""
]
] | We develop a non planar topological vertex formalism and we use it to study the A-model partition function $\mathcal{Z}_{top}$ of topological string on the class of toric Calabi-Yau threefolds (CY3) in large complex structure limit. To that purpose, we first consider the $T^{2}\times R$ special Lagrangian fibration of ... | 7.127643 | 7.466614 | 8.000841 | 7.02085 | 7.667835 | 7.630383 | 7.129662 | 7.259983 | 7.151685 | 8.773981 | 7.473907 | 6.898154 | 7.190352 | 6.901628 | 7.010461 | 7.186617 | 7.082585 | 6.914777 | 6.903691 | 6.929185 | 6.941506 |
hep-th/0201055 | Lee Hyun Min | Kang-Sin Choi, Jihn E. Kim and Hyun Min Lee (Seoul National
University) | Dual Description of Brane World Cosmological Constant with $H_{MNPQ}$ | Latex file of 8 pages including 6 eps figures, to appear in Journal
of the Korean Physical Society (March 2002) | J.KoreanPhys.Soc.40:207-213,2002 | null | null | hep-th | null | We present a short review of the recent 5D self-tuning solution of the
cosmological constant problem with $1/H^2$ term, and present the dual
description of the solution. In the dual description, we show that the presence
of the coupling of the dual field($\sigma$) to the brane(which is a bit
different from the origin... | [
{
"created": "Wed, 9 Jan 2002 08:47:40 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Choi",
"Kang-Sin",
"",
"Seoul National\n University"
],
[
"Kim",
"Jihn E.",
"",
"Seoul National\n University"
],
[
"Lee",
"Hyun Min",
"",
"Seoul National\n University"
]
] | We present a short review of the recent 5D self-tuning solution of the cosmological constant problem with $1/H^2$ term, and present the dual description of the solution. In the dual description, we show that the presence of the coupling of the dual field($\sigma$) to the brane(which is a bit different from the original... | 11.928275 | 10.387034 | 10.66116 | 9.472673 | 10.605745 | 9.197065 | 10.749414 | 10.075015 | 8.972063 | 11.027559 | 9.551572 | 9.628841 | 10.873324 | 10.333363 | 10.322336 | 10.198227 | 10.305752 | 10.231703 | 9.821338 | 10.435401 | 10.492153 |
2209.05868 | Edwan Pr\'eau | M. J\"arvinen, E. Kiritsis, F. Nitti and E. Pr\'eau | Tachyon-dependent Chern-Simons terms and the V-QCD Baryon | 42 pages + Appendix, 2 figures, Accepted for publication in JHEP | null | 10.1007/JHEP12(2022)160 | CCTP-2022-4, ITCP-2022/2, APCTP Pre2022 - 020 | hep-th | http://creativecommons.org/licenses/by/4.0/ | The structure of the five-dimensional Tachyon-Chern-Simons action and its
relevance to single-baryon states in the context of the V-QCD models for
holographic QCD with backreacting flavor are analyzed. The most general form of
the Tachyon-Chern-Simons 5-form, compatible with symmetries and flavor
anomalies is determi... | [
{
"created": "Tue, 13 Sep 2022 10:31:06 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Dec 2022 12:37:58 GMT",
"version": "v2"
}
] | 2023-01-18 | [
[
"Järvinen",
"M.",
""
],
[
"Kiritsis",
"E.",
""
],
[
"Nitti",
"F.",
""
],
[
"Préau",
"E.",
""
]
] | The structure of the five-dimensional Tachyon-Chern-Simons action and its relevance to single-baryon states in the context of the V-QCD models for holographic QCD with backreacting flavor are analyzed. The most general form of the Tachyon-Chern-Simons 5-form, compatible with symmetries and flavor anomalies is determine... | 8.470728 | 8.980391 | 8.856336 | 8.293246 | 8.416181 | 8.275393 | 8.317687 | 8.288103 | 8.424734 | 9.285115 | 7.868064 | 8.49206 | 8.569036 | 8.338917 | 8.030207 | 8.350408 | 8.1967 | 8.087109 | 8.14714 | 8.496432 | 8.238703 |
1806.05774 | Ashish Shukla | Pavel Kovtun and Ashish Shukla | Kubo formulas for thermodynamic transport coefficients | v1: 21 pages, 1 figure; v2: footnotes added, version published in
JHEP | JHEP10(2018)007 | 10.1007/JHEP10(2018)007 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Uncharged relativistic fluids in 3+1 dimensions have three independent
thermodynamic transport coefficients at second order in the derivative
expansion. Fluids with a single global $U(1)$ current have nine, out of which
seven are parity preserving. We derive the Kubo formulas for all nine
thermodynamic transport coef... | [
{
"created": "Fri, 15 Jun 2018 00:19:48 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Oct 2018 19:08:21 GMT",
"version": "v2"
}
] | 2018-10-05 | [
[
"Kovtun",
"Pavel",
""
],
[
"Shukla",
"Ashish",
""
]
] | Uncharged relativistic fluids in 3+1 dimensions have three independent thermodynamic transport coefficients at second order in the derivative expansion. Fluids with a single global $U(1)$ current have nine, out of which seven are parity preserving. We derive the Kubo formulas for all nine thermodynamic transport coeffi... | 7.004178 | 5.633693 | 6.964991 | 5.690648 | 6.027613 | 5.714799 | 5.681966 | 5.506737 | 5.514953 | 6.4003 | 5.575153 | 5.460334 | 6.105519 | 5.634173 | 5.442728 | 5.790206 | 5.585409 | 5.696788 | 5.72638 | 6.346177 | 5.882025 |
1611.04935 | Ruth Gregory | Ruth Gregory and Ian G. Moss | The Fate of the Higgs Vacuum | 6 pages, 2 figures. Talk presented at ICHEP2016, 38th International
Conference on High Energy Physics, 3-10 August 2016, Chicago, USA. To appear
in the conference proceedings | null | null | DCPT-16/47 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This talk reviews our recent work showing how tiny black holes can act as
nucleation sites for the decay of the metastable Higgs vacuum. We start by
discussing the formation of thin wall bubbles of true vacuum inside a false
vacuum, and show how adding a black hole lowers the action of the Euclidean
tunneling solutio... | [
{
"created": "Tue, 15 Nov 2016 17:03:20 GMT",
"version": "v1"
}
] | 2016-11-16 | [
[
"Gregory",
"Ruth",
""
],
[
"Moss",
"Ian G.",
""
]
] | This talk reviews our recent work showing how tiny black holes can act as nucleation sites for the decay of the metastable Higgs vacuum. We start by discussing the formation of thin wall bubbles of true vacuum inside a false vacuum, and show how adding a black hole lowers the action of the Euclidean tunneling solution,... | 11.772856 | 10.161065 | 11.926384 | 10.200436 | 10.528378 | 11.946487 | 11.339739 | 10.505309 | 10.266883 | 13.112372 | 10.415595 | 10.776541 | 11.532952 | 10.95511 | 10.620439 | 10.89959 | 11.338487 | 10.579453 | 10.64463 | 11.680243 | 10.538531 |
hep-th/0308113 | Alexey Selivanov B. | V. D. Ivashchuk, V. N. Melnikov, A.B. Selivanov | Cosmological solutions in multidimensional model with multiple
exponential potential | 22 pages, 1 figure | JHEP 0309 (2003) 059 | 10.1088/1126-6708/2003/09/059 | null | hep-th | null | A family of cosmological solutions with $(n+1)$ Ricci-flat spaces in the
theory with several scalar fields and multiple exponential potential is
obtained when coupling vectors in exponents obey certain relations. Two
subclasses of solutions with power-law and exponential behaviour of scale
factors are singled out. It... | [
{
"created": "Mon, 18 Aug 2003 16:39:45 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Sep 2003 14:39:06 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Ivashchuk",
"V. D.",
""
],
[
"Melnikov",
"V. N.",
""
],
[
"Selivanov",
"A. B.",
""
]
] | A family of cosmological solutions with $(n+1)$ Ricci-flat spaces in the theory with several scalar fields and multiple exponential potential is obtained when coupling vectors in exponents obey certain relations. Two subclasses of solutions with power-law and exponential behaviour of scale factors are singled out. It i... | 14.976391 | 12.232295 | 13.770936 | 11.715 | 12.659435 | 12.011554 | 12.155532 | 11.111973 | 13.082899 | 13.660316 | 12.861522 | 14.038589 | 13.92205 | 13.928487 | 13.844347 | 13.688655 | 13.713719 | 13.261839 | 14.368449 | 13.696963 | 14.004461 |
1306.2643 | D. S. Berman | David S. Berman and Daniel C. Thompson | Duality Symmetric String and M-Theory | Review article. 122 pages. V2 Published Version in Physics Reports | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review recent developments in duality symmetric string theory. We begin
with the world sheet doubled formalism which describes strings in an extended
space time with extra coordinates conjugate to winding modes. This formalism is
T-duality symmetric and can accommodate non-geometric T-fold backgrounds which
are be... | [
{
"created": "Tue, 11 Jun 2013 20:03:02 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Dec 2014 08:17:01 GMT",
"version": "v2"
}
] | 2014-12-10 | [
[
"Berman",
"David S.",
""
],
[
"Thompson",
"Daniel C.",
""
]
] | We review recent developments in duality symmetric string theory. We begin with the world sheet doubled formalism which describes strings in an extended space time with extra coordinates conjugate to winding modes. This formalism is T-duality symmetric and can accommodate non-geometric T-fold backgrounds which are beyo... | 7.998652 | 8.485197 | 9.828471 | 7.779202 | 8.346045 | 8.066875 | 8.533067 | 7.770472 | 7.842079 | 10.324561 | 7.788134 | 8.058287 | 8.489001 | 7.931465 | 7.970926 | 8.098907 | 7.897763 | 7.902088 | 7.841712 | 8.486103 | 7.832684 |
1601.00231 | Robert Brandenberger | Robert H. Brandenberger, Yi-Fu Cai, Sumit R. Das, Elisa G.M. Ferreira,
Ian A. Morrison, Yi Wang | Fluctuations in a Cosmology with a Space-Like Singularity and their
Gauge Theory Dual Description | 19 pages, 3 figures, wording in the introductory section modified | Phys. Rev. D 94, 083508 (2016) | 10.1103/PhysRevD.94.083508 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a time-dependent deformation of anti-de-Sitter (AdS) space-time
which contains a cosmological "singularity" - a space-like region of high
curvature. Making use of the AdS/CFT correspondence we can map the bulk
dynamics onto the boundary. The boundary theory has a time dependent coupling
constant which bec... | [
{
"created": "Sat, 2 Jan 2016 22:37:37 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Jan 2016 08:08:31 GMT",
"version": "v2"
}
] | 2016-10-12 | [
[
"Brandenberger",
"Robert H.",
""
],
[
"Cai",
"Yi-Fu",
""
],
[
"Das",
"Sumit R.",
""
],
[
"Ferreira",
"Elisa G. M.",
""
],
[
"Morrison",
"Ian A.",
""
],
[
"Wang",
"Yi",
""
]
] | We consider a time-dependent deformation of anti-de-Sitter (AdS) space-time which contains a cosmological "singularity" - a space-like region of high curvature. Making use of the AdS/CFT correspondence we can map the bulk dynamics onto the boundary. The boundary theory has a time dependent coupling constant which becom... | 7.260307 | 7.928434 | 7.4722 | 7.141482 | 7.456283 | 7.615226 | 7.357585 | 7.274019 | 7.271526 | 7.974766 | 7.096685 | 7.191424 | 7.391169 | 7.088308 | 7.397815 | 6.994396 | 7.083734 | 7.16873 | 7.168989 | 7.040804 | 7.056366 |
2009.12370 | Jun Nian | Marina David, Jun Nian | Universal Entropy and Hawking Radiation of Near-Extremal AdS$_4$ Black
Holes | 25 pages, 2 figures; v2: Sec. 2.1 and Sec. 2.3 updated; v3: published
version in JHEP, minor changes in Sec. 2 and 3 | JHEP 04(2021)256 | 10.1007/JHEP04(2021)256 | LCTP-20-23 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the Bekenstein-Hawking entropy of near-extremal asymptotically
AdS$_4$ electrically charged rotating black holes using three different
methods: (i) from the gravity solution, (ii) from the near-horizon Kerr/CFT
correspondence and (iii) from the boundary conformal field theory. The results
from these three ... | [
{
"created": "Fri, 25 Sep 2020 17:59:59 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Dec 2020 08:10:26 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Apr 2021 06:49:48 GMT",
"version": "v3"
}
] | 2022-05-02 | [
[
"David",
"Marina",
""
],
[
"Nian",
"Jun",
""
]
] | We compute the Bekenstein-Hawking entropy of near-extremal asymptotically AdS$_4$ electrically charged rotating black holes using three different methods: (i) from the gravity solution, (ii) from the near-horizon Kerr/CFT correspondence and (iii) from the boundary conformal field theory. The results from these three di... | 5.404306 | 4.91643 | 5.640697 | 4.99906 | 5.357746 | 4.889253 | 5.379967 | 4.888519 | 5.00339 | 6.077221 | 4.962419 | 4.903663 | 5.392356 | 4.920104 | 4.87435 | 4.852281 | 5.076186 | 4.865094 | 4.879235 | 5.37919 | 4.922184 |
1512.08550 | Jorge Rocha | Pedro Aniceto, Paolo Pani and Jorge V. Rocha | Radiating black holes in Einstein-Maxwell-dilaton theory and cosmic
censorship violation | 1+18 pages, no figures; v2: Expanded test of cosmic censorship in
section 5 to solutions with a time-dependent dilaton, in which case an
explicit violation of cosmic censorship is found. Small additions to the
title, abstract, introduction and conclusions accordingly. Includes new
appendix with detailed discuss... | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct exact, time-dependent, black hole solutions of
Einstein-Maxwell-dilaton theory with arbitrary dilaton coupling, $a$. For $a=1$
this theory arises as the four-dimensional low-energy effective description of
heterotic string theory. These solutions represent electrically charged,
spherically symmetric blac... | [
{
"created": "Mon, 28 Dec 2015 22:50:33 GMT",
"version": "v1"
},
{
"created": "Wed, 11 May 2016 14:00:48 GMT",
"version": "v2"
},
{
"created": "Tue, 24 May 2016 08:05:52 GMT",
"version": "v3"
}
] | 2016-05-25 | [
[
"Aniceto",
"Pedro",
""
],
[
"Pani",
"Paolo",
""
],
[
"Rocha",
"Jorge V.",
""
]
] | We construct exact, time-dependent, black hole solutions of Einstein-Maxwell-dilaton theory with arbitrary dilaton coupling, $a$. For $a=1$ this theory arises as the four-dimensional low-energy effective description of heterotic string theory. These solutions represent electrically charged, spherically symmetric black ... | 5.081189 | 5.411469 | 5.157694 | 5.066442 | 5.209997 | 4.984144 | 5.251107 | 5.016768 | 5.366539 | 5.53891 | 5.022491 | 5.062263 | 4.995547 | 4.92767 | 4.959705 | 4.919712 | 5.088005 | 4.810182 | 5.062877 | 4.954891 | 5.141421 |
hep-th/9409105 | Jean-Bruno Erismann | L. Guieu, V. Yu. Ovsienko | Structures Symplectiques sur les Espaces de Courbes Projectives et
Affines | 41 pages | null | 10.1016/0393-0440(94)00024-X | CPT-93/P.2980 | hep-th math.SG | null | A symplectic structure on the space of nondegenerate and nonparametrized
curves in a locally affine manifold is defined. We also consider several
interesting spaces of nondegenerate projective curves endowed with Poisson
structures. This construction connects the Virasoro algebra and the
Gel'fand-Dikii bracket with t... | [
{
"created": "Mon, 19 Sep 1994 14:00:40 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Guieu",
"L.",
""
],
[
"Ovsienko",
"V. Yu.",
""
]
] | A symplectic structure on the space of nondegenerate and nonparametrized curves in a locally affine manifold is defined. We also consider several interesting spaces of nondegenerate projective curves endowed with Poisson structures. This construction connects the Virasoro algebra and the Gel'fand-Dikii bracket with the... | 10.654936 | 10.171853 | 11.274739 | 9.603475 | 11.160336 | 12.124389 | 11.554819 | 9.99627 | 12.200032 | 14.332457 | 9.841132 | 10.371343 | 12.190982 | 11.003713 | 11.338447 | 10.442444 | 10.591448 | 10.704918 | 10.260325 | 12.180923 | 10.541648 |
0804.4114 | Branko Dragovich | Branko Dragovich | Zeta Nonlocal Scalar Fields | 13 pages, submitted to Theoretical and Mathematical Physics | Theor.Math.Phys.157:1671-1677,2008 | 10.1007/s11232-008-0139-z | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider some nonlocal and nonpolynomial scalar field models originated
from p-adic string theory. Infinite number of spacetime derivatives is
determined by the operator valued Riemann zeta function through d'Alembertian
$\Box$ in its argument. Construction of the corresponding Lagrangians L starts
with the exact ... | [
{
"created": "Fri, 25 Apr 2008 14:19:07 GMT",
"version": "v1"
}
] | 2009-01-26 | [
[
"Dragovich",
"Branko",
""
]
] | We consider some nonlocal and nonpolynomial scalar field models originated from p-adic string theory. Infinite number of spacetime derivatives is determined by the operator valued Riemann zeta function through d'Alembertian $\Box$ in its argument. Construction of the corresponding Lagrangians L starts with the exact La... | 12.347766 | 13.532755 | 13.313438 | 12.493988 | 12.263599 | 13.578325 | 13.000483 | 12.092253 | 12.18031 | 13.914945 | 12.284601 | 12.271626 | 12.744712 | 12.090026 | 12.15243 | 11.949455 | 11.995006 | 11.975547 | 11.759008 | 12.485019 | 11.573978 |
1605.05597 | Yuhma Asano | Yuhma Asano, Veselin G. Filev, Samuel Kov\'a\v{c}ik and Denjoe
O'Connor | The Flavoured BFSS Model at High Temperature | 36 pages 11 figures and tables; v2: major revision for clarification,
numerical results updated and typos corrected | null | 10.1007/JHEP01(2017)113 | DIAS-STP-16-04 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the high temperature series expansion of the Berkooz-Douglas matrix
model which describes the D0/D4--brane system. At high temperature the model is
weakly coupled and we develop the series to second order. We check our results
against the high temperature regime of the bosonic model (without fermions) and
fi... | [
{
"created": "Wed, 18 May 2016 14:22:30 GMT",
"version": "v1"
},
{
"created": "Tue, 2 May 2017 14:59:37 GMT",
"version": "v2"
}
] | 2017-05-03 | [
[
"Asano",
"Yuhma",
""
],
[
"Filev",
"Veselin G.",
""
],
[
"Kováčik",
"Samuel",
""
],
[
"O'Connor",
"Denjoe",
""
]
] | We study the high temperature series expansion of the Berkooz-Douglas matrix model which describes the D0/D4--brane system. At high temperature the model is weakly coupled and we develop the series to second order. We check our results against the high temperature regime of the bosonic model (without fermions) and find... | 9.389664 | 9.66447 | 10.759583 | 8.740228 | 8.481544 | 9.021996 | 9.100331 | 9.064498 | 8.666643 | 10.361745 | 8.952655 | 8.746924 | 8.906284 | 8.703165 | 8.643356 | 8.397243 | 8.628478 | 8.423359 | 8.813311 | 9.176305 | 8.40751 |
1304.0404 | Tomislav Prokopec | Gianrocco Lazzari and Tomislav Prokopec | Symmetry breaking in de Sitter: a stochastic effective theory approach | 25 pages, 3 eps figures | null | null | ITP-UU-13/06, SPIN-13/04 | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider phase transitions on (eternal) de Sitter in an O(N) symmetric
scalar field theory. Making use of Starobinsky's stochastic inflation we prove
that deep infrared scalar modes cannot form a condensate -- and hence they see
an effective potential that allows no phase transition. We show that by proving
convex... | [
{
"created": "Mon, 1 Apr 2013 18:04:25 GMT",
"version": "v1"
}
] | 2013-04-02 | [
[
"Lazzari",
"Gianrocco",
""
],
[
"Prokopec",
"Tomislav",
""
]
] | We consider phase transitions on (eternal) de Sitter in an O(N) symmetric scalar field theory. Making use of Starobinsky's stochastic inflation we prove that deep infrared scalar modes cannot form a condensate -- and hence they see an effective potential that allows no phase transition. We show that by proving convexit... | 11.317697 | 11.899814 | 11.087324 | 10.910607 | 10.957484 | 11.37614 | 11.802862 | 10.877419 | 10.599661 | 11.490649 | 10.417956 | 10.803014 | 10.612083 | 10.756616 | 10.707767 | 10.725842 | 10.692838 | 10.845207 | 10.770371 | 10.954099 | 10.371872 |
1911.02654 | Norihiro Iizuka | Norihiro Iizuka, Akihiro Ishibashi, Kengo Maeda | Conformally invariant averaged null energy condition from AdS/CFT | 27 pages, 2 figures. v2: section 5 corrected. references added | null | 10.1007/JHEP03(2020)161 | OU-HET-1028 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the compatibility of the AdS/CFT duality with the bulk and boundary
causality, and derive a conformally invariant averaged null energy condition
(CANEC) for quantum field theories in 3 and 5-dimensional curved boundaries.
This is the generalization of the averaged null energy condition (ANEC) in
Minkowski sp... | [
{
"created": "Wed, 6 Nov 2019 22:23:15 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Mar 2020 04:05:56 GMT",
"version": "v2"
}
] | 2020-04-22 | [
[
"Iizuka",
"Norihiro",
""
],
[
"Ishibashi",
"Akihiro",
""
],
[
"Maeda",
"Kengo",
""
]
] | We study the compatibility of the AdS/CFT duality with the bulk and boundary causality, and derive a conformally invariant averaged null energy condition (CANEC) for quantum field theories in 3 and 5-dimensional curved boundaries. This is the generalization of the averaged null energy condition (ANEC) in Minkowski spac... | 8.260568 | 8.978519 | 9.038356 | 8.279299 | 8.60577 | 8.286136 | 8.236226 | 8.158204 | 8.040853 | 10.414493 | 8.197013 | 7.556449 | 8.401854 | 7.876186 | 7.69755 | 7.83549 | 7.845754 | 7.588036 | 7.609475 | 8.152357 | 7.715397 |
hep-th/9604175 | Kechkin O. V. | O.Kechkin, M.Yurova | Kramer--Neugebauer Transformation for Einstein--Maxwell--Dilaton--Axion
Theory | 13 pages, RevTex, no figures | Phys.Rev.D54:6132-6135,1996 | 10.1103/PhysRevD.54.6132 | null | hep-th | null | The Kramer--Neugebauer--like transformation is constructed for the stationary
axisymmetric D=4 Einstein--Maxwell--dilaton--axion system. This transformation
directly maps the dualized sigma--model equations of the theory into the
nondualized ones. Also the new chiral $4 \times 4$ matrix representation of the
problem ... | [
{
"created": "Sun, 28 Apr 1996 18:09:36 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Kechkin",
"O.",
""
],
[
"Yurova",
"M.",
""
]
] | The Kramer--Neugebauer--like transformation is constructed for the stationary axisymmetric D=4 Einstein--Maxwell--dilaton--axion system. This transformation directly maps the dualized sigma--model equations of the theory into the nondualized ones. Also the new chiral $4 \times 4$ matrix representation of the problem is... | 16.638304 | 12.381104 | 13.290671 | 10.794175 | 11.847908 | 12.010949 | 12.250376 | 11.175839 | 11.004143 | 15.138491 | 11.710462 | 11.543425 | 12.189392 | 10.734604 | 11.18499 | 11.359818 | 12.182172 | 10.854419 | 12.318488 | 11.721004 | 11.74578 |
hep-th/0406183 | Nikolaos Tetradis | N. Tetradis (U. of Athens) | Brane Cosmology with Matter in the Bulk (II) | 15 pages | Class.Quant.Grav. 21 (2004) 5221-5232 | 10.1088/0264-9381/21/22/013 | null | hep-th | null | We derive exact solutions of the Einstein equations in the context of the
Randall-Sundrum model with matter on the brane and in the bulk. We present two
models in which the brane moves within a time-dependent bulk. We study the
cosmological evolution on the brane. Our solutions display novel behaviour,
such as an exp... | [
{
"created": "Tue, 22 Jun 2004 08:02:06 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Tetradis",
"N.",
"",
"U. of Athens"
]
] | We derive exact solutions of the Einstein equations in the context of the Randall-Sundrum model with matter on the brane and in the bulk. We present two models in which the brane moves within a time-dependent bulk. We study the cosmological evolution on the brane. Our solutions display novel behaviour, such as an expan... | 8.412413 | 6.604421 | 7.75109 | 6.944005 | 6.535836 | 6.175484 | 6.487339 | 6.591808 | 6.380998 | 7.463331 | 6.577086 | 7.085555 | 7.385274 | 7.186579 | 7.095092 | 7.242088 | 6.966062 | 6.998205 | 7.194526 | 7.379001 | 7.271986 |
hep-th/0701053 | Cliff Burgess | C.P. Burgess | Introduction to Effective Field Theory | Review article prepared for Annual Reviews of Nuclear and Particle
Science, LaTex, 55 pages; new references added | Ann.Rev.Nucl.Part.Sci.57:329-362,2007 | 10.1146/annurev.nucl.56.080805.140508 | null | hep-th astro-ph gr-qc hep-ph | null | This review summarizes Effective Field Theory techniques, which are the
modern theoretical tools for exploiting the existence of hierarchies of scale
in a physical problem. The general theoretical framework is described, and
explicitly evaluated for a simple model. Power-counting results are illustrated
for a few cas... | [
{
"created": "Mon, 8 Jan 2007 04:18:12 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Jan 2007 08:44:10 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Burgess",
"C. P.",
""
]
] | This review summarizes Effective Field Theory techniques, which are the modern theoretical tools for exploiting the existence of hierarchies of scale in a physical problem. The general theoretical framework is described, and explicitly evaluated for a simple model. Power-counting results are illustrated for a few cases... | 15.388863 | 16.387535 | 14.606583 | 13.68087 | 16.13658 | 15.464453 | 15.395126 | 14.316767 | 14.71861 | 14.87483 | 13.544104 | 13.490477 | 13.840523 | 13.80672 | 13.881551 | 14.042854 | 13.720195 | 14.050078 | 13.508623 | 14.495022 | 13.472979 |
1902.02149 | Ion Vasile Vancea | Ion V. Vancea | Backreaction of particle production on physical gravitons in the de
Sitter space | 13 pages | null | null | null | hep-th astro-ph.HE gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the effects of the scalar particle production on the physical
graviton operator in the de Sitter space. Our analysis is done for the
sub-horizon modes at large values of the conformal time. In this limit, we
completely determine the correction to the scalar energy-momentum tensor at the
first order in the W... | [
{
"created": "Wed, 6 Feb 2019 12:51:05 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Mar 2019 15:42:27 GMT",
"version": "v2"
}
] | 2019-03-21 | [
[
"Vancea",
"Ion V.",
""
]
] | We derive the effects of the scalar particle production on the physical graviton operator in the de Sitter space. Our analysis is done for the sub-horizon modes at large values of the conformal time. In this limit, we completely determine the correction to the scalar energy-momentum tensor at the first order in the WKB... | 10.427556 | 9.818406 | 10.535733 | 9.748773 | 9.32884 | 9.968574 | 9.937277 | 9.564652 | 9.845934 | 11.450287 | 9.728456 | 9.807338 | 10.019998 | 9.718784 | 9.987939 | 9.763946 | 10.123417 | 9.485874 | 10.184879 | 10.080238 | 9.613009 |
hep-th/0303089 | Saurya Das | Saurya Das, Viqar Husain | Anti-de Sitter black holes, perfect fluids, and holography | Minor changes to match published version. 9 Pages, Revtex | Class.Quant.Grav.20:4387-4401,2003 | 10.1088/0264-9381/20/20/304 | null | hep-th gr-qc | null | We consider asymptotically anti-de Sitter black holes in $d$-spacetime
dimensions in the thermodynamically stable regime. We show that the
Bekenstein-Hawking entropy and its leading order corrections due to thermal
fluctuations can be reproduced by a weakly interacting fluid of bosons and
fermions (`dual gas') in $\D... | [
{
"created": "Tue, 11 Mar 2003 01:54:11 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Sep 2003 23:44:21 GMT",
"version": "v2"
},
{
"created": "Fri, 20 Feb 2004 18:28:43 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Das",
"Saurya",
""
],
[
"Husain",
"Viqar",
""
]
] | We consider asymptotically anti-de Sitter black holes in $d$-spacetime dimensions in the thermodynamically stable regime. We show that the Bekenstein-Hawking entropy and its leading order corrections due to thermal fluctuations can be reproduced by a weakly interacting fluid of bosons and fermions (`dual gas') in $\Del... | 9.210238 | 8.306469 | 7.772647 | 7.365201 | 7.982097 | 8.671135 | 8.900487 | 7.779262 | 8.543705 | 8.667298 | 8.023845 | 8.178308 | 7.948595 | 7.94181 | 7.838024 | 7.95239 | 8.079251 | 7.985872 | 7.748658 | 8.029082 | 8.013892 |
2003.08173 | Sanjaye Ramgoolam | Robert de Mello Koch, Sanjaye Ramgoolam | Perturbative 4D conformal field theories and representation theory of
diagram algebras | 67 pages, many figures; V2-minor typos corrected | JHEP 05 (2020) 020 | 10.1007/JHEP05(2020)020 | QMUL-PH-20-03 | hep-th math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The correlators of free four dimensional conformal field theories (CFT4) have
been shown to be given by amplitudes in two-dimensional $so(4,2)$ equivariant
topological field theories (TFT2), by using a vertex operator formalism for the
correlators. We show that this can be extended to perturbative interacting
conform... | [
{
"created": "Wed, 18 Mar 2020 12:10:12 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Aug 2020 14:50:16 GMT",
"version": "v2"
}
] | 2020-08-13 | [
[
"Koch",
"Robert de Mello",
""
],
[
"Ramgoolam",
"Sanjaye",
""
]
] | The correlators of free four dimensional conformal field theories (CFT4) have been shown to be given by amplitudes in two-dimensional $so(4,2)$ equivariant topological field theories (TFT2), by using a vertex operator formalism for the correlators. We show that this can be extended to perturbative interacting conformal... | 12.615526 | 14.00155 | 14.343816 | 13.061584 | 13.872128 | 14.127325 | 12.897055 | 12.652056 | 12.644076 | 16.532078 | 12.808444 | 12.507369 | 13.322164 | 12.632945 | 12.731623 | 12.860001 | 12.693733 | 12.709398 | 12.535013 | 13.189446 | 12.87697 |
2107.00671 | Alessio Baldazzi | Alessio Baldazzi and Kevin Falls | Essential Quantum Einstein Gravity | v2: clarifying remarks on inessential couplings at Gaussian fixed
points, a discussion on the inclusion of matter and additional references
added. Matches published version | Universe 2021, 7(8), 294 | 10.3390/universe7080294 | null | hep-th gr-qc | http://creativecommons.org/publicdomain/zero/1.0/ | The non-perturbative renormalisation of quantum gravity is investigated
allowing for the metric to be reparameterised along the RG flow, such that only
the essential couplings constants are renormalised. This allows us to identify
a universality class of quantum gravity which is guaranteed to be unitary,
since the ph... | [
{
"created": "Thu, 1 Jul 2021 18:00:22 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Aug 2021 15:50:39 GMT",
"version": "v2"
}
] | 2021-08-11 | [
[
"Baldazzi",
"Alessio",
""
],
[
"Falls",
"Kevin",
""
]
] | The non-perturbative renormalisation of quantum gravity is investigated allowing for the metric to be reparameterised along the RG flow, such that only the essential couplings constants are renormalised. This allows us to identify a universality class of quantum gravity which is guaranteed to be unitary, since the phys... | 6.851279 | 6.940142 | 7.277645 | 6.680064 | 6.784355 | 6.715543 | 6.946084 | 6.638314 | 6.448394 | 8.436994 | 6.511204 | 6.648448 | 7.122365 | 6.738802 | 6.517528 | 6.819641 | 6.754389 | 6.570313 | 6.645503 | 7.176442 | 6.59476 |
0712.1427 | Piotr Su{\l}kowski | Robbert Dijkgraaf and Piotr Su{\l}kowski | Instantons on ALE spaces and orbifold partitions | 28 pages, 10 figures; reference added | JHEP 0803:013,2008 | 10.1088/1126-6708/2008/03/013 | ITFA-2007-26, IFT-UW-2007-5, BONN-TH-2007-12 | hep-th math.AG math.CO | null | We consider N=4 theories on ALE spaces of $A_{k-1}$ type. As is well known,
their partition functions coincide with $A_{k-1}$ affine characters. We show
that these partition functions are equal to the generating functions of some
peculiar classes of partitions which we introduce under the name 'orbifold
partitions'. ... | [
{
"created": "Mon, 10 Dec 2007 10:39:52 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Mar 2008 04:30:31 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Dijkgraaf",
"Robbert",
""
],
[
"Sułkowski",
"Piotr",
""
]
] | We consider N=4 theories on ALE spaces of $A_{k-1}$ type. As is well known, their partition functions coincide with $A_{k-1}$ affine characters. We show that these partition functions are equal to the generating functions of some peculiar classes of partitions which we introduce under the name 'orbifold partitions'. Th... | 9.313755 | 8.395494 | 10.090654 | 7.815771 | 8.599902 | 8.112982 | 8.355323 | 8.171627 | 7.920042 | 10.232965 | 8.425362 | 8.283647 | 8.63959 | 8.429458 | 8.430714 | 8.316245 | 8.120371 | 8.292765 | 8.420449 | 8.74788 | 8.138274 |
hep-th/0008086 | Dominique Toublan | D. Toublan and J.J.M. Verbaarschot | Dirac Spectrum in Adjoint QCD | Invited talk at the "Fourth Workshop on Continuous Advances in QCD",
Minneapolis, May 12-14, 2000, 15 pages, Latex, 1 figure | null | null | SUNY-NTG-00/46 | hep-th | null | In this lecture we discuss some exact results for the low-lying spectrum of
the Dirac operator in adjoint QCD. In particular, we find an analytical
expression for the slope of the average spectral density. These results are
obtained by means of a generating function which is an extension of the QCD
partition function... | [
{
"created": "Thu, 10 Aug 2000 21:55:21 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Toublan",
"D.",
""
],
[
"Verbaarschot",
"J. J. M.",
""
]
] | In this lecture we discuss some exact results for the low-lying spectrum of the Dirac operator in adjoint QCD. In particular, we find an analytical expression for the slope of the average spectral density. These results are obtained by means of a generating function which is an extension of the QCD partition function w... | 7.101623 | 6.714414 | 7.655187 | 6.389262 | 6.624191 | 6.28335 | 6.979461 | 6.834581 | 6.77977 | 7.622234 | 6.366115 | 6.541493 | 6.971527 | 6.698488 | 7.005747 | 6.560661 | 6.784701 | 6.932847 | 6.805037 | 6.760652 | 6.832815 |
hep-th/9812222 | Ademir eugenio de Santana | F.C. Khanna, A.E. Santana, A. Matos Neto, J.D.M. Vianna and T. Kopf | Spinorial density matrix equation and gauge covariance | LaTex, 17 pages | null | null | null | hep-th | null | In this work we apply the Lie group representation method introduced in the
real time formalism for finite-temperature quantum-field theory, thermofield
dynamics, to derive a spinorial density matrix equation. Symmetry properties of
such equation are analysed, and as a basic result it is shown that one solution
is th... | [
{
"created": "Wed, 23 Dec 1998 13:14:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Khanna",
"F. C.",
""
],
[
"Santana",
"A. E.",
""
],
[
"Neto",
"A. Matos",
""
],
[
"Vianna",
"J. D. M.",
""
],
[
"Kopf",
"T.",
""
]
] | In this work we apply the Lie group representation method introduced in the real time formalism for finite-temperature quantum-field theory, thermofield dynamics, to derive a spinorial density matrix equation. Symmetry properties of such equation are analysed, and as a basic result it is shown that one solution is the ... | 17.655111 | 19.289408 | 16.984173 | 17.62862 | 17.097349 | 19.966682 | 18.292965 | 16.984787 | 18.514824 | 17.126591 | 16.182093 | 16.077477 | 16.533766 | 16.588289 | 15.720049 | 16.236975 | 16.591248 | 16.198425 | 15.987382 | 15.970021 | 15.983724 |
0807.1564 | Shinya Tomizawa | Shinya Tomizawa and Akihiro Ishibashi | Charged Black Holes in a Rotating Gross-Perry-Sorkin Monopole Background | 25 pages, 6 figures | Class.Quant.Grav.25:245007,2008 | 10.1088/0264-9381/25/24/245007 | KEK-TH-1261 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a new class of stationary charged black hole solutions to
five-dimensional Einstein-Maxwell-Chern-Simons theories. We construct the
solutions by utilizing so called the squashing transformation. At infinity, our
solutions behave as a four-dimensional flat spacetime plus a `circle' and hence
describe a Kalu... | [
{
"created": "Thu, 10 Jul 2008 00:44:30 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"Tomizawa",
"Shinya",
""
],
[
"Ishibashi",
"Akihiro",
""
]
] | We present a new class of stationary charged black hole solutions to five-dimensional Einstein-Maxwell-Chern-Simons theories. We construct the solutions by utilizing so called the squashing transformation. At infinity, our solutions behave as a four-dimensional flat spacetime plus a `circle' and hence describe a Kaluza... | 9.003374 | 7.554833 | 8.448965 | 7.532258 | 7.617405 | 7.57224 | 8.019963 | 7.777704 | 7.933608 | 9.290979 | 7.780362 | 8.069987 | 8.776722 | 8.287848 | 8.200725 | 8.273226 | 7.978684 | 8.278782 | 8.230441 | 8.747411 | 8.175019 |
hep-th/0207186 | Hagi Ahmedov | H. Ahmedov and I.H. Duru | Casimir force between surfaces close to each other | Latex, 20 pages, added references, corrected typos, changed content | J.Math.Phys. 44 (2003) 5487-5503 | 10.1063/1.1624471 | FGE 02-1 | hep-th | null | Casimir interactions (due to the massless scalar field fluctuations) of two
surfaces which are close to each other are studied.
After a brief general presentation, explicit calculations for co-axial
cylinders, co-centric spheres and co-axial cones are performed.
| [
{
"created": "Sun, 21 Jul 2002 14:20:37 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Jul 2002 14:01:46 GMT",
"version": "v2"
},
{
"created": "Sun, 9 Feb 2003 13:42:43 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Ahmedov",
"H.",
""
],
[
"Duru",
"I. H.",
""
]
] | Casimir interactions (due to the massless scalar field fluctuations) of two surfaces which are close to each other are studied. After a brief general presentation, explicit calculations for co-axial cylinders, co-centric spheres and co-axial cones are performed. | 13.603639 | 13.483303 | 13.602496 | 11.754034 | 12.496636 | 11.082581 | 12.942388 | 12.286667 | 11.37132 | 14.201404 | 11.961088 | 11.178085 | 12.077583 | 11.809708 | 11.735855 | 11.238905 | 11.535183 | 12.098622 | 11.821574 | 12.100241 | 11.24817 |
hep-th/9410182 | Hyeonjoon Shin | Jae Kwan Kim and Hyeonjoon Shin | Low Energy Description of Fermion Pairs in Topologically Massive
QED$_{2+1}$ with $N$ Flavours | 14 pages, revtex, KAIST-CHEP-94/S3 | Phys.Lett. B343 (1995) 323-328 | 10.1016/0370-2693(94)01459-P | null | hep-th | null | In topologically massive QED$_{2+1}$ with $N$ flavours, there is the
possibility that two equal-charged fermions can form a bound state pair in
either s-wave or p-wave. We are concerned about the s-wave pairs and obtain the
low energy effective action describing them. It is shown that the fermion pairs
behave like do... | [
{
"created": "Tue, 25 Oct 1994 09:19:39 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Kim",
"Jae Kwan",
""
],
[
"Shin",
"Hyeonjoon",
""
]
] | In topologically massive QED$_{2+1}$ with $N$ flavours, there is the possibility that two equal-charged fermions can form a bound state pair in either s-wave or p-wave. We are concerned about the s-wave pairs and obtain the low energy effective action describing them. It is shown that the fermion pairs behave like doub... | 10.879758 | 10.461712 | 10.963287 | 9.84599 | 10.118922 | 9.533944 | 9.337866 | 10.468388 | 9.447723 | 10.110701 | 9.916496 | 9.87018 | 9.987167 | 9.498312 | 9.957281 | 10.17497 | 9.75627 | 9.945345 | 9.451669 | 9.758872 | 9.609501 |
1607.07301 | Dong Bai | Dong Bai | Softness, Polynomial Boundedness and Amplitudes' Positivity | 7 pages; accepted version | null | 10.1209/0295-5075/120/21001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note, we study the connections between infrared (IR) and ultraviolet
(UV) behaviors of scattering amplitudes of massless channels by exploiting
dispersion relations and positivity bounds. Given forward scattering
amplitudes, which scale as $\mathcal{A}(s)\sim s^M$ in the IR ($s\to0$) and
could be embedded int... | [
{
"created": "Mon, 25 Jul 2016 15:02:46 GMT",
"version": "v1"
},
{
"created": "Sat, 10 Sep 2016 11:03:59 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Dec 2017 16:32:30 GMT",
"version": "v3"
}
] | 2018-02-14 | [
[
"Bai",
"Dong",
""
]
] | In this note, we study the connections between infrared (IR) and ultraviolet (UV) behaviors of scattering amplitudes of massless channels by exploiting dispersion relations and positivity bounds. Given forward scattering amplitudes, which scale as $\mathcal{A}(s)\sim s^M$ in the IR ($s\to0$) and could be embedded into ... | 5.686126 | 5.489715 | 5.675077 | 5.305986 | 5.436583 | 5.467332 | 5.818218 | 5.309001 | 5.271434 | 5.736131 | 5.309963 | 5.511427 | 5.52534 | 5.501333 | 5.477069 | 5.401632 | 5.335971 | 5.511784 | 5.479182 | 5.594727 | 5.402773 |
1301.0969 | Yong-Wan Kim | Yong-Wan Kim, Yun Soo Myung, Young-Jai Park | A massive graviton in topologically new massive gravity | 13 pages, REVTeX, version to appear in PRD | null | 10.1103/PhysRevD.87.064020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the topologically new massive gravity in three dimensions. It
turns out that a single massive mode is propagating in the flat spacetime,
comparing to the conformal Chern-Simons gravity which has no physically
propagating degrees of freedom. Also we discuss the realization of the BMS/GCA
correspondence.... | [
{
"created": "Sun, 6 Jan 2013 03:20:18 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Mar 2013 01:28:40 GMT",
"version": "v2"
}
] | 2013-03-27 | [
[
"Kim",
"Yong-Wan",
""
],
[
"Myung",
"Yun Soo",
""
],
[
"Park",
"Young-Jai",
""
]
] | We investigate the topologically new massive gravity in three dimensions. It turns out that a single massive mode is propagating in the flat spacetime, comparing to the conformal Chern-Simons gravity which has no physically propagating degrees of freedom. Also we discuss the realization of the BMS/GCA correspondence. | 11.591763 | 8.923772 | 11.115677 | 10.4741 | 10.107972 | 10.667458 | 10.18709 | 9.312052 | 10.113189 | 13.196429 | 9.998394 | 9.941803 | 11.335989 | 10.499716 | 10.24697 | 10.521813 | 10.454378 | 10.275731 | 10.689867 | 11.844386 | 10.470305 |
hep-th/9410197 | Gary McCartor | Gary McCartor | The Vacuum in the Light-Cone Representation | 7pages, SMUHEP/94-24 | null | null | null | hep-th | null | The mechanism by which the physical vacuum can be different from the
perturbative vacuum in the light-cone representation is described and
illustrated.
| [
{
"created": "Wed, 26 Oct 1994 15:34:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"McCartor",
"Gary",
""
]
] | The mechanism by which the physical vacuum can be different from the perturbative vacuum in the light-cone representation is described and illustrated. | 25.064074 | 11.16377 | 12.875251 | 10.882157 | 9.98143 | 11.657017 | 11.091271 | 11.084864 | 10.748673 | 14.173806 | 13.334996 | 13.265627 | 14.147042 | 13.090104 | 13.443065 | 13.474418 | 13.636332 | 13.319967 | 12.950855 | 14.417245 | 15.508819 |
hep-th/0409273 | Daniel Grumiller | L. Bergamin, D. Grumiller, A. Iorio and C. Nunez | Chemistry of Chern-Simons Supergravity: reduction to a BPS kink,
oxidation to M-theory and thermodynamical aspects | 39 pages, 2 figures. v2: reference added, minor changes, typos | JHEP0411:021,2004 | 10.1088/1126-6708/2004/11/021 | TUW-04-27, LU-ITP-04/022, MIT-CTP-3546 | hep-th gr-qc | null | We construct a supersymmetric extension of the two dimensional
Kaluza-Klein-reduced gravitational Chern-Simons term, and globally study its
solutions, labelled by mass and U(1) charge c. The kink solution is BPS, and in
an appropriate conformal frame all solutions asymptotically approach AdS. The
thermodynamics of th... | [
{
"created": "Mon, 27 Sep 2004 15:46:56 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Nov 2004 10:37:13 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bergamin",
"L.",
""
],
[
"Grumiller",
"D.",
""
],
[
"Iorio",
"A.",
""
],
[
"Nunez",
"C.",
""
]
] | We construct a supersymmetric extension of the two dimensional Kaluza-Klein-reduced gravitational Chern-Simons term, and globally study its solutions, labelled by mass and U(1) charge c. The kink solution is BPS, and in an appropriate conformal frame all solutions asymptotically approach AdS. The thermodynamics of the ... | 15.960232 | 14.304364 | 17.122004 | 15.119327 | 14.933494 | 15.346657 | 14.463876 | 15.550176 | 13.576163 | 16.849485 | 14.465282 | 15.22948 | 16.149426 | 14.828922 | 14.565679 | 14.987646 | 14.658498 | 14.871097 | 14.742797 | 15.683197 | 14.651167 |
hep-th/0411193 | Paolo Grinza | P. Grinza and B. Ponsot | Form factors in the massless coset models su(2)_k+1 \otimes su(2)_k
/su(2)_2k+1 - Part II | 16 pages, 4 eps figure, LaTeX; v2: numerical checks improved, to
appear in Nucl. Phys. B | Nucl.Phys. B718 (2005) 394-412 | 10.1016/j.nuclphysb.2005.04.018 | null | hep-th cond-mat.stat-mech math-ph math.MP | null | Massless flows from the coset model su(2)_k+1 \otimes su(2)_k /su(2)_2k+1 to
the minimal model M_k+2 are studied from the viewpoint of form factors. These
flows include in particular the flow from the Tricritical Ising model to the
Ising model. By analogy with the magnetization operator in the flow TIM -> IM,
we cons... | [
{
"created": "Mon, 22 Nov 2004 12:10:58 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Apr 2005 09:14:18 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Grinza",
"P.",
""
],
[
"Ponsot",
"B.",
""
]
] | Massless flows from the coset model su(2)_k+1 \otimes su(2)_k /su(2)_2k+1 to the minimal model M_k+2 are studied from the viewpoint of form factors. These flows include in particular the flow from the Tricritical Ising model to the Ising model. By analogy with the magnetization operator in the flow TIM -> IM, we constr... | 7.306141 | 7.896881 | 9.450886 | 6.829741 | 6.904471 | 6.788573 | 7.218766 | 7.027238 | 7.217496 | 9.744744 | 6.648269 | 6.987342 | 8.414832 | 6.978679 | 6.949872 | 6.837543 | 7.015163 | 7.005374 | 7.228315 | 7.914553 | 7.008498 |
0801.2385 | Jared Kaplan | Nima Arkani-Hamed and Jared Kaplan | On Tree Amplitudes in Gauge Theory and Gravity | 22 pages, 3 figures | JHEP 0804:076,2008 | 10.1088/1126-6708/2008/04/076 | null | hep-th | null | The BCFW recursion relations provide a powerful way to compute tree
amplitudes in gauge theories and gravity, but only hold if some amplitudes
vanish when two of the momenta are taken to infinity in a particular complex
direction. This is a very surprising property, since individual Feynman
diagrams all diverge at in... | [
{
"created": "Wed, 16 Jan 2008 17:12:56 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Arkani-Hamed",
"Nima",
""
],
[
"Kaplan",
"Jared",
""
]
] | The BCFW recursion relations provide a powerful way to compute tree amplitudes in gauge theories and gravity, but only hold if some amplitudes vanish when two of the momenta are taken to infinity in a particular complex direction. This is a very surprising property, since individual Feynman diagrams all diverge at infi... | 8.82324 | 9.271712 | 9.441685 | 8.354166 | 8.81356 | 9.421363 | 8.689827 | 8.647463 | 8.419581 | 10.570941 | 8.36151 | 8.386558 | 8.943238 | 8.446413 | 8.249178 | 8.372422 | 8.145893 | 8.613094 | 8.403538 | 8.708003 | 8.186535 |
1107.4642 | Emilio Elizalde | I. Brevik, E. Elizalde, S. Nojiri, S.D. Odintsov | Viscous Little Rip Cosmology | 10 pages, version to appear in PRD | null | 10.1103/PhysRevD.84.103508 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dark energy of phantom or quintessence nature with an equation of state
parameter $w$ almost equal to -1 often leads the universe evolution to a
finite-time future singularity. An elegant solution to this problem has been
recently proposed \cite{frampton11} under the form of the so-called Little Rip
cosmology which a... | [
{
"created": "Fri, 22 Jul 2011 23:08:41 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Oct 2011 15:45:50 GMT",
"version": "v2"
}
] | 2013-05-29 | [
[
"Brevik",
"I.",
""
],
[
"Elizalde",
"E.",
""
],
[
"Nojiri",
"S.",
""
],
[
"Odintsov",
"S. D.",
""
]
] | Dark energy of phantom or quintessence nature with an equation of state parameter $w$ almost equal to -1 often leads the universe evolution to a finite-time future singularity. An elegant solution to this problem has been recently proposed \cite{frampton11} under the form of the so-called Little Rip cosmology which app... | 10.793077 | 11.80691 | 10.011673 | 10.068627 | 10.883299 | 10.304405 | 11.357007 | 10.320704 | 10.874563 | 10.83371 | 10.308947 | 10.224002 | 10.226883 | 10.299994 | 10.673546 | 10.456515 | 10.64689 | 10.051394 | 10.884093 | 10.271474 | 10.444259 |
2207.00399 | Harold Steinacker | Joanna L. Karczmarek, Harold C. Steinacker | Cosmic time evolution and propagator from a Yang-Mills matrix model | 26 apages, 1 figure. V2: pre-and post-BB correlation fixed,
references added. V3: improved presentation, published version | null | 10.1088/1751-8121/acc61e | UWThPh-2022-8 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a solution of a IKKT-type matrix model which can be considered as
a 1+1-dimensional space-time with Minkowski signature and a Big Bounce-like
singularity. A suitable $i\varepsilon$ regularization of the Lorentzian matrix
integral is proposed, which leads to the standard $i\varepsilon$-prescription
for the... | [
{
"created": "Fri, 1 Jul 2022 13:13:52 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Nov 2022 10:35:16 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Mar 2023 08:44:09 GMT",
"version": "v3"
}
] | 2023-04-12 | [
[
"Karczmarek",
"Joanna L.",
""
],
[
"Steinacker",
"Harold C.",
""
]
] | We consider a solution of a IKKT-type matrix model which can be considered as a 1+1-dimensional space-time with Minkowski signature and a Big Bounce-like singularity. A suitable $i\varepsilon$ regularization of the Lorentzian matrix integral is proposed, which leads to the standard $i\varepsilon$-prescription for the e... | 11.054805 | 9.517102 | 10.29899 | 9.681847 | 9.778273 | 9.664808 | 9.894177 | 9.635281 | 9.338602 | 10.996085 | 9.437298 | 9.293392 | 9.595686 | 9.507894 | 9.365923 | 9.294535 | 9.286382 | 9.386292 | 9.58322 | 9.477331 | 9.620268 |
1209.4681 | Alfredo Suzuki T | Alfredo Takashi Suzuki, Jorge Henrique Sales and Luis Alberto Soriano | Zero Mode Effect Generalization for the Electromagnetic Current in the
Light Front | 13 pages, 3 figures. arXiv admin note: substantial text overlap with
arXiv:hep-th/0509116 | null | 10.1103/PhysRevD.88.025036 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider in this work the electromagnetic current for a system composed by
two charged bosons and show that it has a structure of many bodies even in the
impulse approximation, when described in the light front time $x^+$. In terms
of the two-body component for the bound state, the current contains two-body
operat... | [
{
"created": "Thu, 20 Sep 2012 22:49:11 GMT",
"version": "v1"
}
] | 2013-08-09 | [
[
"Suzuki",
"Alfredo Takashi",
""
],
[
"Sales",
"Jorge Henrique",
""
],
[
"Soriano",
"Luis Alberto",
""
]
] | We consider in this work the electromagnetic current for a system composed by two charged bosons and show that it has a structure of many bodies even in the impulse approximation, when described in the light front time $x^+$. In terms of the two-body component for the bound state, the current contains two-body operator... | 20.647345 | 18.470171 | 17.842993 | 17.079679 | 16.737999 | 19.097429 | 17.412315 | 19.738234 | 16.847176 | 18.142231 | 18.14731 | 17.874207 | 17.563147 | 17.996607 | 18.244604 | 18.834736 | 17.838501 | 18.388037 | 17.724079 | 18.563377 | 18.821156 |
1701.05103 | Milad Porforough | Milad Porforough | Magnetic charge quantization from SYM considerations | 11 pages, minor changes, published version | null | 10.1209/0295-5075/127/41001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An intersecting D3-D3' system contains magnetic monopole solutions due to D-
strings stretched between two branes. These magnetic charges satisfy the usual
Dirac quantization relation. We show that this quantization condition can also
be obtained directly by SUSY and gauge invariance arguments of the theory and
concl... | [
{
"created": "Wed, 18 Jan 2017 15:30:27 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Mar 2017 13:44:40 GMT",
"version": "v2"
},
{
"created": "Thu, 27 Jul 2017 13:46:34 GMT",
"version": "v3"
},
{
"created": "Fri, 27 Sep 2019 15:07:56 GMT",
"version": "v4"
}
] | 2019-09-30 | [
[
"Porforough",
"Milad",
""
]
] | An intersecting D3-D3' system contains magnetic monopole solutions due to D- strings stretched between two branes. These magnetic charges satisfy the usual Dirac quantization relation. We show that this quantization condition can also be obtained directly by SUSY and gauge invariance arguments of the theory and conclud... | 20.492182 | 21.19112 | 19.512667 | 17.50975 | 20.061331 | 19.573273 | 19.977859 | 18.880396 | 18.641251 | 20.981718 | 17.763212 | 17.490042 | 18.939156 | 17.633244 | 17.588453 | 17.424154 | 17.506674 | 17.089504 | 17.893915 | 18.536718 | 16.985554 |
hep-th/0410279 | Oscar J. C. Dias | Oscar J. C. Dias, Jose' P. S. Lemos | Pair creation of higher dimensional black holes on a de Sitter
background | 10 pages; 1 figure included; RexTeX4. v2: References added. Published
version. v3: Typo in equation (46) fixed | Phys.Rev. D70 (2004) 124023 | 10.1103/PhysRevD.70.124023 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study in detail the quantum process in which a pair of black holes is
created in a higher D-dimensional de Sitter (dS) background. The energy to
materialize and accelerate the pair comes from the positive cosmological
constant. The instantons that describe the process are obtained from the
Tangherlini black hole s... | [
{
"created": "Thu, 28 Oct 2004 17:07:47 GMT",
"version": "v1"
},
{
"created": "Sun, 19 Dec 2004 21:47:29 GMT",
"version": "v2"
},
{
"created": "Tue, 3 Nov 2009 21:20:43 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Dias",
"Oscar J. C.",
""
],
[
"Lemos",
"Jose' P. S.",
""
]
] | We study in detail the quantum process in which a pair of black holes is created in a higher D-dimensional de Sitter (dS) background. The energy to materialize and accelerate the pair comes from the positive cosmological constant. The instantons that describe the process are obtained from the Tangherlini black hole sol... | 8.338959 | 7.649178 | 8.080072 | 7.536348 | 6.947268 | 7.170794 | 7.33785 | 7.282996 | 7.601483 | 8.272076 | 7.877519 | 7.838229 | 8.136562 | 8.06406 | 7.727094 | 7.865851 | 7.789182 | 7.761374 | 8.027012 | 8.171118 | 8.006654 |
hep-th/0209212 | Kaustubh Agashe | K. Agashe, A. Delgado (Johns Hopkins University) | A note on CFT dual of RS model with gauge fields in bulk | Latex, 18 pages. In the revised version, conclusions and equations in
sections 3 and 4 (which provide more mathematical backing for the duality)
have been added | Phys.Rev. D67 (2003) 046003 | 10.1103/PhysRevD.67.046003 | null | hep-th hep-ph | null | It has been conjectured that the (weakly coupled) Randall-Sundrum (RS) model
with gauge fields in the bulk is dual to a (strongly coupled) 4D conformal
field theory (CFT) with an UV cut-off and in which global symmetries of the CFT
are gauged. We elucidate features of this dual CFT which are crucial for a
complete un... | [
{
"created": "Wed, 25 Sep 2002 18:05:48 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Dec 2002 20:59:37 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Agashe",
"K.",
"",
"Johns Hopkins University"
],
[
"Delgado",
"A.",
"",
"Johns Hopkins University"
]
] | It has been conjectured that the (weakly coupled) Randall-Sundrum (RS) model with gauge fields in the bulk is dual to a (strongly coupled) 4D conformal field theory (CFT) with an UV cut-off and in which global symmetries of the CFT are gauged. We elucidate features of this dual CFT which are crucial for a complete unde... | 5.797474 | 6.106394 | 5.899167 | 5.484131 | 6.323775 | 6.034391 | 6.088594 | 5.756642 | 5.741908 | 6.30281 | 5.848393 | 5.871006 | 5.786119 | 5.591436 | 5.819479 | 5.774195 | 5.807213 | 5.771726 | 5.652277 | 5.770535 | 5.763552 |
1001.4779 | Constantinos Papageorgakis | Neil Lambert and Constantinos Papageorgakis | Relating U(N)xU(N) to SU(N)xSU(N) Chern-Simons Membrane theories | 16 pages, Latex; v2: references added; v3: Clarifications added | JHEP 1004:104,2010 | 10.1007/JHEP04(2010)104 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By integrating out the U(1)_B gauge field, we show that the U(n)xU(n) ABJM
theory at level k is equivalent to a Z_k identification of the
(SU(n)xSU(n))/Z_n Chern-Simons theory, but only when n and k are coprime. As a
consequence, the k=1 ABJM model for two M2-branes in R^8 can be identified with
the N=8 (SU(2)xSU(2))... | [
{
"created": "Tue, 26 Jan 2010 19:22:38 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Feb 2010 18:07:10 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Apr 2010 17:22:22 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Lambert",
"Neil",
""
],
[
"Papageorgakis",
"Constantinos",
""
]
] | By integrating out the U(1)_B gauge field, we show that the U(n)xU(n) ABJM theory at level k is equivalent to a Z_k identification of the (SU(n)xSU(n))/Z_n Chern-Simons theory, but only when n and k are coprime. As a consequence, the k=1 ABJM model for two M2-branes in R^8 can be identified with the N=8 (SU(2)xSU(2))/Z... | 4.920894 | 4.474389 | 5.566748 | 4.403246 | 4.389637 | 4.649835 | 4.386726 | 4.35517 | 4.308976 | 5.611632 | 4.48782 | 4.186452 | 5.148472 | 4.462618 | 4.298725 | 4.366954 | 4.354033 | 4.425555 | 4.322123 | 4.758209 | 4.516992 |
hep-th/9312171 | null | M. Cadoni and S. Mignemi | Classical and Semiclassical Properties of Extremal Black Holes with
Dilaton and Modulus Fields | 25 pages (3 figures available upon request), plain TEX,INFN-CA-20-93
(typographical errors corrected) | Nucl.Phys.B427:669-696,1994 | 10.1016/0550-3213(94)90644-0 | null | hep-th gr-qc | null | We discuss both classical and semiclassical properties of extremal black
holes in theories where the dilaton and a modulus field are present. We find
that the corresponding 2-dim geometry is asymptotically anti-de Sitter rather
then asymptotically flat as in the purely dilatonic case. This fact has many
important con... | [
{
"created": "Tue, 21 Dec 1993 22:05:00 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Jan 1994 12:13:00 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Cadoni",
"M.",
""
],
[
"Mignemi",
"S.",
""
]
] | We discuss both classical and semiclassical properties of extremal black holes in theories where the dilaton and a modulus field are present. We find that the corresponding 2-dim geometry is asymptotically anti-de Sitter rather then asymptotically flat as in the purely dilatonic case. This fact has many important conse... | 7.666595 | 6.618004 | 7.475741 | 6.737636 | 6.991428 | 6.620296 | 6.8785 | 6.618167 | 6.820379 | 7.497153 | 6.644434 | 7.054942 | 7.163029 | 6.879656 | 7.118261 | 7.124207 | 7.217984 | 6.933697 | 7.145658 | 7.277918 | 6.966904 |
1007.2412 | Andrew Fitzpatrick | A. Liam Fitzpatrick, Emanuel Katz, David Poland, David Simmons-Duffin | Effective Conformal Theory and the Flat-Space Limit of AdS | 46 pages, 2 figures. v2: JHEP published version | JHEP 1107:023,2011 | 10.1007/JHEP07(2011)023 | BUHET-07-14-10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop the idea of an effective conformal theory describing the low-lying
spectrum of the dilatation operator in a CFT. Such an effective theory is
useful when the spectrum contains a hierarchy in the dimension of operators,
and a small parameter whose role is similar to that of 1/N in a large N gauge
theory. The... | [
{
"created": "Wed, 14 Jul 2010 20:00:02 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Oct 2011 00:24:36 GMT",
"version": "v2"
}
] | 2011-10-11 | [
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Katz",
"Emanuel",
""
],
[
"Poland",
"David",
""
],
[
"Simmons-Duffin",
"David",
""
]
] | We develop the idea of an effective conformal theory describing the low-lying spectrum of the dilatation operator in a CFT. Such an effective theory is useful when the spectrum contains a hierarchy in the dimension of operators, and a small parameter whose role is similar to that of 1/N in a large N gauge theory. These... | 6.654396 | 7.362821 | 7.244888 | 7.024865 | 7.386271 | 7.438137 | 7.252149 | 7.195664 | 7.065998 | 7.584165 | 6.930354 | 6.735435 | 6.977957 | 6.627883 | 6.730643 | 6.784754 | 6.669894 | 6.864003 | 6.65596 | 6.827374 | 6.713862 |
1304.3398 | Walter Tangarife | Elena Caceres, Arnab Kundu, Juan F. Pedraza and Walter Tangarife | Strong Subadditivity, Null Energy Condition and Charged Black Holes | 27 pages, v3 matches the published version | JHEP 01 (2014) 084 | 10.1007/JHEP01(2014)084 | UTTG-08-13; TCC-005-13 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the Hubeny-Rangamani-Takayanagi (HRT) conjectured formula for
entanglement entropy in the context of the AdS/CFT correspondence with
time-dependent backgrounds, we investigate the relation between the bulk null
energy condition (NEC) of the stress-energy tensor with the strong
sub-additivity (SSA) property of e... | [
{
"created": "Thu, 11 Apr 2013 19:13:10 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Apr 2013 19:06:37 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Mar 2014 16:01:09 GMT",
"version": "v3"
}
] | 2014-03-20 | [
[
"Caceres",
"Elena",
""
],
[
"Kundu",
"Arnab",
""
],
[
"Pedraza",
"Juan F.",
""
],
[
"Tangarife",
"Walter",
""
]
] | Using the Hubeny-Rangamani-Takayanagi (HRT) conjectured formula for entanglement entropy in the context of the AdS/CFT correspondence with time-dependent backgrounds, we investigate the relation between the bulk null energy condition (NEC) of the stress-energy tensor with the strong sub-additivity (SSA) property of ent... | 7.573419 | 7.475915 | 8.146408 | 7.147017 | 7.44042 | 7.627782 | 7.588739 | 7.307025 | 6.860744 | 8.493771 | 7.138608 | 7.454576 | 7.400606 | 7.067701 | 7.030105 | 6.971773 | 7.15392 | 7.114483 | 7.180646 | 7.457555 | 7.047105 |
2205.11477 | K\'evin Nguyen | Laura Donnay, Kevin Nguyen, Romain Ruzziconi | Loop-corrected subleading soft theorem and the celestial stress-tensor | 20 pages + appendices; v2: added comments; v3: added funding
acknowledgment | null | 10.1007/JHEP09(2022)063 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate that the one-loop exact subleading soft graviton theorem
automatically follows from conservation of the BMS charges, provided that the
hard and soft fluxes separately represent the extended BMS algebra at null
infinity. This confirms that superrotations are genuine symmetries of the
gravitational $\mat... | [
{
"created": "Mon, 23 May 2022 17:26:29 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Sep 2022 10:53:58 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Jun 2023 08:04:09 GMT",
"version": "v3"
}
] | 2023-06-22 | [
[
"Donnay",
"Laura",
""
],
[
"Nguyen",
"Kevin",
""
],
[
"Ruzziconi",
"Romain",
""
]
] | We demonstrate that the one-loop exact subleading soft graviton theorem automatically follows from conservation of the BMS charges, provided that the hard and soft fluxes separately represent the extended BMS algebra at null infinity. This confirms that superrotations are genuine symmetries of the gravitational $\mathc... | 12.416856 | 10.01951 | 14.42522 | 10.562317 | 11.071956 | 10.883665 | 10.4446 | 10.403483 | 10.910023 | 12.818189 | 10.614953 | 12.096418 | 11.803594 | 11.657557 | 12.003592 | 11.40813 | 11.664424 | 11.278213 | 11.688229 | 12.207006 | 11.36636 |
2407.20225 | Changnan Peng | Changnan Peng, Maria Cristina Diamantini, Lena Funcke, Syed Muhammad
Ali Hassan, Karl Jansen, Stefan K\"uhn, Di Luo, Pranay Naredi | Hamiltonian Lattice Formulation of Compact Maxwell-Chern-Simons Theory | null | null | null | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Chern-Simons theory is a topological quantum field theory with numerous
applications in condensed matter and high-energy physics, including the study
of anomalies, fermion/boson dualities, and the fractional quantum Hall effect.
In this work, a Hamiltonian lattice formulation for 2+1D compact
Maxwell-Chern-Simons the... | [
{
"created": "Mon, 29 Jul 2024 17:58:15 GMT",
"version": "v1"
}
] | 2024-07-30 | [
[
"Peng",
"Changnan",
""
],
[
"Diamantini",
"Maria Cristina",
""
],
[
"Funcke",
"Lena",
""
],
[
"Hassan",
"Syed Muhammad Ali",
""
],
[
"Jansen",
"Karl",
""
],
[
"Kühn",
"Stefan",
""
],
[
"Luo",
"Di",
""
],
... | Chern-Simons theory is a topological quantum field theory with numerous applications in condensed matter and high-energy physics, including the study of anomalies, fermion/boson dualities, and the fractional quantum Hall effect. In this work, a Hamiltonian lattice formulation for 2+1D compact Maxwell-Chern-Simons theor... | 5.593674 | 5.516294 | 5.431789 | 5.116516 | 5.385304 | 5.59019 | 5.579646 | 5.387969 | 5.311923 | 5.858372 | 5.38349 | 5.300243 | 5.292917 | 5.333929 | 5.350199 | 5.210471 | 5.2991 | 5.30732 | 5.228657 | 5.397346 | 5.247382 |
1407.3323 | Andrei Zelnikov | Valeri P. Frolov and Andrei Zelnikov | Charged particles in higher dimensional homogeneous gravitational field:
Self-energy and self-force | 43 pages, two subsections added, a few tables and references added | null | 10.1007/JHEP10(2014)068 | Alberta Thy 13-14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A problem of self-energy and self-force for a charged point-like particle in
a higher dimensional homogeneous gravitational field is considered. We study
two cases, when a particle has usual electric charge and a case when it has a
scalar charge, which is a source of a scalar massless minimally coupled field.
We assu... | [
{
"created": "Fri, 11 Jul 2014 23:53:33 GMT",
"version": "v1"
},
{
"created": "Sat, 30 Aug 2014 00:59:33 GMT",
"version": "v2"
},
{
"created": "Thu, 11 Sep 2014 20:16:24 GMT",
"version": "v3"
}
] | 2015-06-22 | [
[
"Frolov",
"Valeri P.",
""
],
[
"Zelnikov",
"Andrei",
""
]
] | A problem of self-energy and self-force for a charged point-like particle in a higher dimensional homogeneous gravitational field is considered. We study two cases, when a particle has usual electric charge and a case when it has a scalar charge, which is a source of a scalar massless minimally coupled field. We assume... | 8.3114 | 8.678299 | 7.739929 | 7.917031 | 8.740602 | 8.026704 | 8.924153 | 7.978474 | 8.460967 | 8.56766 | 8.269492 | 8.150786 | 7.682126 | 7.967687 | 8.012543 | 7.995917 | 7.923036 | 8.021353 | 7.999113 | 7.929739 | 7.947093 |
1111.3613 | Lasha Berezhiani | L. Berezhiani, G. Chkareuli, C. de Rham, G. Gabadadze, A. J. Tolley | On Black Holes in Massive Gravity | 17 LateX pages | null | 10.1103/PhysRevD.85.044024 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In massive gravity the so-far-found black hole solutions on Minkowski space
happen to convert horizons into a certain type of singularities. Here we
explore whether these singularities can be avoided if space-time is not
asymptotically Minkowskian. We find an exact analytic black hole (BH) solution
which evades the a... | [
{
"created": "Tue, 15 Nov 2011 19:21:30 GMT",
"version": "v1"
}
] | 2013-05-30 | [
[
"Berezhiani",
"L.",
""
],
[
"Chkareuli",
"G.",
""
],
[
"de Rham",
"C.",
""
],
[
"Gabadadze",
"G.",
""
],
[
"Tolley",
"A. J.",
""
]
] | In massive gravity the so-far-found black hole solutions on Minkowski space happen to convert horizons into a certain type of singularities. Here we explore whether these singularities can be avoided if space-time is not asymptotically Minkowskian. We find an exact analytic black hole (BH) solution which evades the abo... | 10.40544 | 11.908107 | 11.152403 | 10.330468 | 11.281784 | 10.609504 | 10.90607 | 11.013925 | 10.686601 | 12.539264 | 10.99939 | 10.137276 | 10.115745 | 9.550993 | 9.883075 | 9.657729 | 9.694789 | 9.616659 | 9.924152 | 10.188853 | 9.975357 |
0801.3503 | Iftikhar Ahmad | Iftikhar Ahmad, Yun-Song Piao, Cong-Feng Qiao | On Number of Nflation Fields | 13 pages, 3 figures;added more comments,to publish in JCAP | JCAP0806:023,2008 | 10.1088/1475-7516/2008/06/023 | null | hep-th | null | We study the Nflation model, in which a collection of massive scalar fields
drive the inflation simultaneously. We find, when the number of fields is
larger than the square of ratio of the Planck scale $M_p$ to the average value
$\bar m$ of fields masses, the slow roll inflation region will disappear. This
suggests t... | [
{
"created": "Wed, 23 Jan 2008 05:52:09 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Jun 2008 04:16:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Ahmad",
"Iftikhar",
""
],
[
"Piao",
"Yun-Song",
""
],
[
"Qiao",
"Cong-Feng",
""
]
] | We study the Nflation model, in which a collection of massive scalar fields drive the inflation simultaneously. We find, when the number of fields is larger than the square of ratio of the Planck scale $M_p$ to the average value $\bar m$ of fields masses, the slow roll inflation region will disappear. This suggests tha... | 10.769416 | 10.315039 | 10.470594 | 10.416401 | 10.204469 | 10.082332 | 10.534999 | 9.354195 | 10.266778 | 11.369849 | 9.728047 | 9.605309 | 10.399878 | 9.850834 | 10.093149 | 10.06689 | 9.939857 | 10.07483 | 9.976916 | 10.305329 | 9.910035 |
hep-th/0604069 | Lisa Freyhult | Lisa Freyhult and Charlotte Kristjansen | A Universality Test of the Quantum String Bethe Ansatz | 12 pages, references added | Phys.Lett.B638:258-264,2006 | 10.1016/j.physletb.2006.05.021 | NORDITA-2006-11 | hep-th | null | We show that the quantum corrected string Bethe ansatz passes an important
universality test by demonstrating that it correctly incorporates the
non-analytical terms in the string sigma model one-loop correction for rational
three-spin strings with two out of the three spins identical. Subsequently, we
use the quantu... | [
{
"created": "Mon, 10 Apr 2006 14:48:01 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Apr 2006 17:30:36 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Freyhult",
"Lisa",
""
],
[
"Kristjansen",
"Charlotte",
""
]
] | We show that the quantum corrected string Bethe ansatz passes an important universality test by demonstrating that it correctly incorporates the non-analytical terms in the string sigma model one-loop correction for rational three-spin strings with two out of the three spins identical. Subsequently, we use the quantum ... | 9.202269 | 10.232066 | 12.045036 | 8.732218 | 10.579463 | 9.738766 | 9.889725 | 9.168221 | 8.839625 | 13.718291 | 8.924998 | 9.236305 | 10.637113 | 8.80582 | 9.197166 | 8.921761 | 9.195327 | 8.836132 | 8.879823 | 10.350664 | 8.695053 |
hep-th/9612008 | Stephen Fletcher Hewson | S. F. Hewson and M. J. Perry | The twelve dimensional super (2+2)-brane | 32 pages LaTex, no figures, minor comments and address(!) added | Nucl.Phys. B492 (1997) 249-277 | 10.1016/S0550-3213(97)80035-1 | DAMTP-R-96-55 | hep-th | null | We discuss supersymmetry in twelve dimensions and present a covariant
supersymmetric action for a brane with worldsheet signature (2,2), called a
super (2+2)-brane, propagating in the osp(64,12) superspace. This superspace is
explicitly constructed, and is trivial in the sense that the spinorial part is
a trivial bun... | [
{
"created": "Sat, 30 Nov 1996 11:33:18 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Dec 1996 12:52:01 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Hewson",
"S. F.",
""
],
[
"Perry",
"M. J.",
""
]
] | We discuss supersymmetry in twelve dimensions and present a covariant supersymmetric action for a brane with worldsheet signature (2,2), called a super (2+2)-brane, propagating in the osp(64,12) superspace. This superspace is explicitly constructed, and is trivial in the sense that the spinorial part is a trivial bundl... | 9.499261 | 10.383886 | 10.925705 | 9.738081 | 9.855101 | 10.078181 | 10.239573 | 10.089594 | 9.458967 | 11.526641 | 9.004993 | 8.990499 | 9.653114 | 9.342175 | 9.291626 | 9.031166 | 9.2649 | 9.104719 | 9.520167 | 9.892918 | 8.902516 |
hep-th/0612106 | Tomasz Taylor | Tomasz R. Taylor | Threshold Effects Beyond the Standard Model | To appear in the book "String theory and fundamental interactions"
(published in celebration of the 65th birthday of Gabriele Veneziano), eds.
M. Gasperini and J. Maharana (Lecture Notes in Physics, Springer
Berlin/Heidelberg, 2007 | Lect.NotesPhys.737:553-560,2008 | null | null | hep-th | null | In this contribution to the Festschrift celebrating Gabriele Veneziano on his
65th birthday, I discuss the threshold effects of extra dimensions and their
applications to physics beyond the standard model, focusing on superstring
theory.
| [
{
"created": "Tue, 12 Dec 2006 15:33:55 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Taylor",
"Tomasz R.",
""
]
] | In this contribution to the Festschrift celebrating Gabriele Veneziano on his 65th birthday, I discuss the threshold effects of extra dimensions and their applications to physics beyond the standard model, focusing on superstring theory. | 11.31856 | 8.364906 | 9.263806 | 7.776048 | 7.815256 | 7.830537 | 7.090961 | 8.244743 | 8.289206 | 8.753776 | 7.564638 | 8.073292 | 8.285439 | 7.743426 | 8.203695 | 7.635827 | 7.736905 | 7.947557 | 7.746848 | 8.710809 | 8.229794 |
2012.12275 | Takuya Okuda | Hirotaka Hayashi, Takuya Okuda, Yutaka Yoshida | ABCD of 't Hooft operators | 76 pages, many figures; v2: comments added, statements clarified,
typos fixed, version in JHEP | null | 10.1007/JHEP04(2021)241 | UT-Komaba-20-3, IPMU20-0110 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We compute by supersymmetric localization the expectation values of half-BPS
't Hooft line operators in $\mathcal{N}=2$ $U(N)$, $SO(N)$ and $USp(N)$ gauge
theories on $S^1 \times \mathbb{R}^3$ with an $\Omega$-deformation. We evaluate
the non-perturbative contributions due to monopole screening by calculating the
sup... | [
{
"created": "Tue, 22 Dec 2020 19:00:02 GMT",
"version": "v1"
},
{
"created": "Mon, 3 May 2021 06:08:23 GMT",
"version": "v2"
}
] | 2021-05-12 | [
[
"Hayashi",
"Hirotaka",
""
],
[
"Okuda",
"Takuya",
""
],
[
"Yoshida",
"Yutaka",
""
]
] | We compute by supersymmetric localization the expectation values of half-BPS 't Hooft line operators in $\mathcal{N}=2$ $U(N)$, $SO(N)$ and $USp(N)$ gauge theories on $S^1 \times \mathbb{R}^3$ with an $\Omega$-deformation. We evaluate the non-perturbative contributions due to monopole screening by calculating the super... | 4.854513 | 4.317466 | 6.886896 | 4.152222 | 4.222062 | 4.051551 | 4.433334 | 4.400225 | 4.217259 | 6.849539 | 4.253081 | 4.562215 | 5.617685 | 4.698101 | 4.616292 | 4.536185 | 4.491388 | 4.588638 | 4.597432 | 5.354085 | 4.786909 |
hep-th/9912149 | Oliver Schnetz | Oliver Schnetz | Calculation of the phi^4 6-loop non-zeta transcendental | 9 pages, LaTeX, no figures | null | null | null | hep-th | null | We present an analytic calculation of the first transcendental in
phi^4-Theory that is not of the form zeta(2n+1). It is encountered at 6 loops
and known to be a weight 8 double sum. Here it is obtained by reducing multiple
zeta values of depth <= 4. We give a closed expression in terms of a
zeta-related sum for a fa... | [
{
"created": "Thu, 16 Dec 1999 18:23:52 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Schnetz",
"Oliver",
""
]
] | We present an analytic calculation of the first transcendental in phi^4-Theory that is not of the form zeta(2n+1). It is encountered at 6 loops and known to be a weight 8 double sum. Here it is obtained by reducing multiple zeta values of depth <= 4. We give a closed expression in terms of a zeta-related sum for a fami... | 19.849228 | 20.798649 | 19.826385 | 19.462343 | 21.006853 | 20.568058 | 21.56282 | 20.369852 | 17.808109 | 20.406986 | 20.313026 | 18.262821 | 19.96455 | 19.521538 | 19.905558 | 19.117319 | 19.203287 | 18.248554 | 18.50812 | 18.81954 | 18.582743 |
1411.3669 | Jamie McDonald | J. I. McDonald and Graham M. Shore | Gravitational leptogenesis, C, CP and strong equivalence | 32 pages, 5 figures | null | 10.1007/JHEP02(2015)076 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The origin of matter-antimatter asymmetry is one of the most important
outstanding problems at the interface of particle physics and cosmology.
Gravitational leptogenesis (baryogenesis) provides a possible mechanism through
explicit couplings of spacetime curvature to appropriate lepton (or baryon)
currents. In this ... | [
{
"created": "Thu, 13 Nov 2014 19:17:50 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"McDonald",
"J. I.",
""
],
[
"Shore",
"Graham M.",
""
]
] | The origin of matter-antimatter asymmetry is one of the most important outstanding problems at the interface of particle physics and cosmology. Gravitational leptogenesis (baryogenesis) provides a possible mechanism through explicit couplings of spacetime curvature to appropriate lepton (or baryon) currents. In this pa... | 7.47472 | 8.622584 | 7.350715 | 7.161911 | 8.780037 | 7.893031 | 8.431084 | 7.877931 | 7.495306 | 7.899363 | 7.513358 | 7.121952 | 7.259079 | 7.321199 | 7.606569 | 7.041836 | 7.482381 | 7.290751 | 7.230882 | 7.430194 | 7.287598 |
hep-th/9604075 | Dirk Schlingemann | Dirk Schlingemann | Kink States in $P(\phi)_2$-Models (An Algebraic Approach) | 37pp, latex2e | null | null | DESY 96-051 | hep-th | null | Several two-dimensional quantum field theory models have more than one vacuum
state. Familiar examples are the Sine-Gordon and the $\phi^4_2$-model. It is
known that these models possess states, called kink states, which interpolate
different vacua. A general construction scheme for kink states in the framework
of al... | [
{
"created": "Mon, 15 Apr 1996 08:44:50 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Schlingemann",
"Dirk",
""
]
] | Several two-dimensional quantum field theory models have more than one vacuum state. Familiar examples are the Sine-Gordon and the $\phi^4_2$-model. It is known that these models possess states, called kink states, which interpolate different vacua. A general construction scheme for kink states in the framework of alge... | 6.229887 | 6.430817 | 6.718162 | 6.073176 | 6.669752 | 6.71301 | 6.406274 | 6.172557 | 6.583718 | 7.156868 | 6.300921 | 6.184622 | 6.278957 | 6.202526 | 6.317654 | 6.159257 | 6.177516 | 5.945044 | 6.270317 | 5.966753 | 5.939638 |
1107.2095 | Hyun Seok Yang | Hyun Seok Yang and Sangheon Yun | Calabi-Yau Manifolds, Hermitian Yang-Mills Instantons and Mirror
Symmetry | v5; 49 pages, version to appear in Advances in High Energy Physics | Adv. High Energy Phys. 2017 (2017) 7962426 | 10.1155/2017/7962426 | null | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We address the issue why Calabi-Yau manifolds exist with a mirror pair. We
observe that the irreducible spinor representation of the Lorentz group Spin(6)
requires us to consider the vector spaces of two-forms and four-forms on an
equal footing. The doubling of the two-form vector space due to the Hodge
duality doubl... | [
{
"created": "Mon, 11 Jul 2011 19:09:00 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jun 2014 18:35:11 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Jul 2014 16:13:49 GMT",
"version": "v3"
},
{
"created": "Mon, 14 Jul 2014 02:53:30 GMT",
"version": "v4"
},
{
"cr... | 2017-11-13 | [
[
"Yang",
"Hyun Seok",
""
],
[
"Yun",
"Sangheon",
""
]
] | We address the issue why Calabi-Yau manifolds exist with a mirror pair. We observe that the irreducible spinor representation of the Lorentz group Spin(6) requires us to consider the vector spaces of two-forms and four-forms on an equal footing. The doubling of the two-form vector space due to the Hodge duality doubles... | 7.095076 | 7.215474 | 7.728492 | 7.051248 | 7.574508 | 7.757686 | 7.282029 | 7.131083 | 6.781554 | 8.010765 | 6.816343 | 6.912343 | 7.184309 | 6.847595 | 6.991765 | 7.059785 | 6.871574 | 6.783602 | 6.727244 | 6.952632 | 6.796481 |
hep-th/0603210 | Fernando Marchesano | Fernando Marchesano | D6-branes and torsion | 35 pages, 1 figure. One reference added | JHEP0605:019,2006 | 10.1088/1126-6708/2006/05/019 | LMU-ASC 21/06 | hep-th | null | The D6-brane spectrum of type IIA vacua based on twisted tori and RR
background fluxes is analyzed. In particular, we compute the torsion factors of
the (co)homology groups H_n and describe the effect that they have on D6-brane
physics. For instance, the fact that H_3 contains Z_N subgroups explains why RR
tadpole co... | [
{
"created": "Tue, 28 Mar 2006 16:55:55 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Apr 2006 20:29:41 GMT",
"version": "v2"
},
{
"created": "Sat, 13 May 2006 09:10:57 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Marchesano",
"Fernando",
""
]
] | The D6-brane spectrum of type IIA vacua based on twisted tori and RR background fluxes is analyzed. In particular, we compute the torsion factors of the (co)homology groups H_n and describe the effect that they have on D6-brane physics. For instance, the fact that H_3 contains Z_N subgroups explains why RR tadpole cond... | 10.745132 | 10.529451 | 10.732732 | 9.39543 | 10.17332 | 10.631254 | 9.988179 | 9.346515 | 9.195529 | 12.987164 | 9.349788 | 9.771619 | 9.946245 | 9.37109 | 9.88426 | 9.539157 | 10.148235 | 9.867358 | 9.494805 | 9.482602 | 9.892021 |
hep-th/0303020 | Rene Reinbacher | Burt A. Ovrut, Tony Pantev and Rene Reinbacher | Invariant Homology on Standard Model Manifolds | 57 pages, 13 figures | JHEP 0401 (2004) 059 | 10.1088/1126-6708/2004/01/059 | null | hep-th | null | Torus-fibered Calabi-Yau threefolds Z, with base dP_9 and fundamental group
pi_1(Z)=Z_2 X Z_2, are reviewed. It is shown that Z=X/(Z_2 X Z_2), where X=B
X_{P_1} B' are elliptically fibered Calabi-Yau threefolds that admit a freely
acting Z_2 X Z_2 automorphism group. B and B' are rational elliptic surfaces,
each with... | [
{
"created": "Tue, 4 Mar 2003 19:47:03 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Ovrut",
"Burt A.",
""
],
[
"Pantev",
"Tony",
""
],
[
"Reinbacher",
"Rene",
""
]
] | Torus-fibered Calabi-Yau threefolds Z, with base dP_9 and fundamental group pi_1(Z)=Z_2 X Z_2, are reviewed. It is shown that Z=X/(Z_2 X Z_2), where X=B X_{P_1} B' are elliptically fibered Calabi-Yau threefolds that admit a freely acting Z_2 X Z_2 automorphism group. B and B' are rational elliptic surfaces, each with a... | 7.258055 | 6.035861 | 8.142055 | 6.415051 | 6.618091 | 6.502007 | 6.924915 | 6.452476 | 6.398034 | 8.579684 | 5.917918 | 6.035841 | 6.717084 | 6.425601 | 6.202728 | 6.273785 | 6.350001 | 6.116279 | 6.490021 | 6.606277 | 6.411019 |
1104.5312 | Naoki Sasakura | Naoki Sasakura | Tensor models and hierarchy of n-ary algebras | 13 pages, some references updated and corrected | Int.J.Mod.Phys.A26:3249-3258,2011 | 10.1142/S0217751X1105381X | YITP-11-51 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Tensor models are generalization of matrix models, and are studied as models
of quantum gravity. It is shown that the symmetry of the rank-three tensor
models is generated by a hierarchy of n-ary algebras starting from the usual
commutator, and the 3-ary algebra symmetry reported in the previous paper is
just a singl... | [
{
"created": "Thu, 28 Apr 2011 07:00:05 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Jul 2011 02:00:57 GMT",
"version": "v2"
}
] | 2011-08-03 | [
[
"Sasakura",
"Naoki",
""
]
] | Tensor models are generalization of matrix models, and are studied as models of quantum gravity. It is shown that the symmetry of the rank-three tensor models is generated by a hierarchy of n-ary algebras starting from the usual commutator, and the 3-ary algebra symmetry reported in the previous paper is just a single ... | 8.741133 | 9.278287 | 11.128174 | 8.194285 | 9.058321 | 9.920697 | 9.921538 | 8.939995 | 8.267918 | 10.385572 | 8.448725 | 8.696843 | 9.139241 | 8.736697 | 8.874276 | 8.921966 | 9.040733 | 8.814507 | 8.482375 | 8.680443 | 8.523704 |
hep-th/0503247 | Francesco Nitti | F. Nitti, M. Porrati and J.-W. Rombouts | Naturalness in Cosmological Initial Conditions | 35 pages, 8 figures | Phys.Rev. D72 (2005) 063503 | 10.1103/PhysRevD.72.063503 | null | hep-th astro-ph gr-qc | null | We propose a novel approach to the problem of constraining cosmological
initial conditions. Within the framework of effective field theory, we classify
initial conditions in terms of boundary terms added to the effective action
describing the cosmological evolution below Planckian energies. These boundary
terms can b... | [
{
"created": "Thu, 31 Mar 2005 19:47:07 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Nitti",
"F.",
""
],
[
"Porrati",
"M.",
""
],
[
"Rombouts",
"J. -W.",
""
]
] | We propose a novel approach to the problem of constraining cosmological initial conditions. Within the framework of effective field theory, we classify initial conditions in terms of boundary terms added to the effective action describing the cosmological evolution below Planckian energies. These boundary terms can be ... | 9.601132 | 9.669579 | 9.904714 | 9.600192 | 10.683284 | 10.198972 | 10.873247 | 9.780982 | 9.392828 | 11.14031 | 9.634989 | 9.676835 | 9.421368 | 9.352082 | 9.396952 | 9.269378 | 9.101398 | 9.366593 | 9.324137 | 9.616862 | 9.421018 |
hep-th/9612237 | Shinsuke M. Nishigaki | S. Higuchi, C. Itoi, S. M. Nishigaki, N. Sakai | Renormalization group approach to multiple-arc random matrix models | 11 pages, 1 figure, LaTeX + a4.sty, epsf.sty | Phys.Lett. B398 (1997) 123-129 | 10.1016/S0370-2693(97)00196-2 | UT-KOMABA/96-28, NUP-A-96-14, NBI-HE-96-65, TIT/HEP-351 | hep-th cond-mat | null | We study critical and universal behaviors of unitary invariant non-gaussian
random matrix ensembles within the framework of the large-N renormalization
group. For a simple double-well model we find an unstable fixed point and a
stable inverse-gaussian fixed point. The former is identified as the critical
point of sin... | [
{
"created": "Thu, 26 Dec 1996 15:23:23 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Higuchi",
"S.",
""
],
[
"Itoi",
"C.",
""
],
[
"Nishigaki",
"S. M.",
""
],
[
"Sakai",
"N.",
""
]
] | We study critical and universal behaviors of unitary invariant non-gaussian random matrix ensembles within the framework of the large-N renormalization group. For a simple double-well model we find an unstable fixed point and a stable inverse-gaussian fixed point. The former is identified as the critical point of singl... | 16.134005 | 15.121782 | 18.017958 | 15.282905 | 15.377948 | 18.37142 | 16.563021 | 15.996559 | 14.623225 | 18.080074 | 15.971572 | 15.169168 | 15.382557 | 14.891213 | 14.888309 | 15.055712 | 14.966179 | 14.674142 | 14.914361 | 16.153648 | 14.906971 |
hep-th/9804153 | Friedemann Brandt | Friedemann Brandt | Deformations of global symmetries in the extended antifield formalism | 23 pages, latex; version to appear in J. Math. Phys | J.Math.Phys. 40 (1999) 1023-1040 | 10.1063/1.532704 | null | hep-th | null | It is outlined how deformations of field theoretical rigid symmetries can be
constructed and classified by cohomological means in the extended antifield
formalism. Special attention is devoted to deformations referring only to a
subset of the rigid symmetries of a given model and leading to a nontrivial
extension of ... | [
{
"created": "Thu, 23 Apr 1998 11:51:35 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Apr 1998 19:34:43 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Nov 1998 12:15:14 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Brandt",
"Friedemann",
""
]
] | It is outlined how deformations of field theoretical rigid symmetries can be constructed and classified by cohomological means in the extended antifield formalism. Special attention is devoted to deformations referring only to a subset of the rigid symmetries of a given model and leading to a nontrivial extension of th... | 10.384483 | 8.018525 | 9.490068 | 7.973806 | 8.411489 | 8.483627 | 8.322832 | 8.321877 | 8.245468 | 9.801571 | 8.345465 | 8.531627 | 8.568234 | 8.671612 | 8.390821 | 8.505859 | 8.466113 | 8.455228 | 8.581221 | 8.912465 | 8.440654 |
1803.02462 | Eric Zaslow | Eric Zaslow | Wavefunctions for a Class of Branes in Three-space | 10 pages | null | null | null | hep-th math.AG math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Wavefunctions are proposed for a class of Lagrangian branes in three
complex-dimensional space. The branes are asymptotic to Legendrian surfaces of
genus g. The expansion of these wavefunctions in appropriate coordinates
conjecturally encodes all-genus open Gromov-Witten invariants, i.e. the free
energy of the topolo... | [
{
"created": "Tue, 6 Mar 2018 22:56:06 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Apr 2018 21:42:58 GMT",
"version": "v2"
}
] | 2018-04-11 | [
[
"Zaslow",
"Eric",
""
]
] | Wavefunctions are proposed for a class of Lagrangian branes in three complex-dimensional space. The branes are asymptotic to Legendrian surfaces of genus g. The expansion of these wavefunctions in appropriate coordinates conjecturally encodes all-genus open Gromov-Witten invariants, i.e. the free energy of the topologi... | 15.13402 | 17.554258 | 18.8174 | 14.638654 | 16.376356 | 17.362658 | 15.589611 | 14.987075 | 16.982986 | 22.827261 | 15.040869 | 14.526997 | 17.758549 | 15.626395 | 13.953349 | 13.367917 | 13.617296 | 13.5198 | 14.675703 | 17.48908 | 14.046796 |
hep-th/9910185 | Bin Wang | Bin Wang and Elcio Abdalla | Holography in (2+1)-dimensional cosmological models | 9 pages, to be published in Phys. Lett. B | Phys.Lett. B466 (1999) 122-126 | 10.1016/S0370-2693(99)01122-3 | null | hep-th | null | The cosmic holographic principle suggested by Fischler and Susskind has been
examined in (2+1)-dimensional cosmological models. Analogously to the
(3+1)-dimensional counterpart, the holographic principle is satisfied in all
flat and open universes. For (2+1)-dimensional closed universes the holographic
principle cann... | [
{
"created": "Sat, 23 Oct 1999 18:32:54 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Wang",
"Bin",
""
],
[
"Abdalla",
"Elcio",
""
]
] | The cosmic holographic principle suggested by Fischler and Susskind has been examined in (2+1)-dimensional cosmological models. Analogously to the (3+1)-dimensional counterpart, the holographic principle is satisfied in all flat and open universes. For (2+1)-dimensional closed universes the holographic principle cannot... | 9.024678 | 7.703103 | 8.897489 | 7.311635 | 7.853708 | 7.619407 | 7.147531 | 7.392498 | 7.125519 | 8.552599 | 7.250453 | 7.742117 | 8.078329 | 7.821672 | 7.911582 | 7.722569 | 7.735156 | 7.643991 | 8.021301 | 8.206285 | 8.056665 |
1206.2349 | Iosif Bena | Iosif Bena, Hagen Triendl, Bert Vercnocke | Black Holes and Fourfolds | 26 pages, 1 figure | null | 10.1007/JHEP08(2012)124 | IPhT-T12/047 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish the relation between the structure governing supersymmetric and
non-supersymmetric four- and five-dimensional black holes and multicenter
solutions and Calabi-Yau flux compactifications of M-theory and type IIB string
theory. We find that the known BPS and almost-BPS multicenter black hole
solutions can ... | [
{
"created": "Mon, 11 Jun 2012 20:00:00 GMT",
"version": "v1"
}
] | 2015-06-05 | [
[
"Bena",
"Iosif",
""
],
[
"Triendl",
"Hagen",
""
],
[
"Vercnocke",
"Bert",
""
]
] | We establish the relation between the structure governing supersymmetric and non-supersymmetric four- and five-dimensional black holes and multicenter solutions and Calabi-Yau flux compactifications of M-theory and type IIB string theory. We find that the known BPS and almost-BPS multicenter black hole solutions can be... | 9.233033 | 8.813878 | 11.259589 | 8.963841 | 9.763351 | 8.752513 | 9.269055 | 8.957296 | 9.035731 | 11.219748 | 8.681277 | 8.793398 | 9.725501 | 9.167861 | 9.160995 | 8.73811 | 9.03156 | 8.998599 | 9.245532 | 9.932355 | 9.047247 |
2104.12724 | Irina Aref'eva | Irina Aref'eva and Igor Volovich | Quantum explosions of black holes and thermal coordinates | 36 pages, 18 figures, Latex | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The Hawking temperature for Schwarzschild black hole $T_H=1/8\pi M$ is
singular in the limit of vanishing mass $M\to 0$. However, the Schwarzschild
metric itself is regular in this limit, it is reduced to the Minkowski metric
and there are no reasons to believe that the temperature becomes infinite. This
discrepancy ... | [
{
"created": "Mon, 26 Apr 2021 17:17:26 GMT",
"version": "v1"
}
] | 2021-04-27 | [
[
"Aref'eva",
"Irina",
""
],
[
"Volovich",
"Igor",
""
]
] | The Hawking temperature for Schwarzschild black hole $T_H=1/8\pi M$ is singular in the limit of vanishing mass $M\to 0$. However, the Schwarzschild metric itself is regular in this limit, it is reduced to the Minkowski metric and there are no reasons to believe that the temperature becomes infinite. This discrepancy ma... | 5.48397 | 5.734905 | 5.572518 | 5.243181 | 5.370765 | 5.358818 | 5.730087 | 5.390914 | 5.648005 | 5.845126 | 5.430212 | 5.467078 | 5.394375 | 5.322575 | 5.436059 | 5.426805 | 5.326431 | 5.531727 | 5.468431 | 5.378508 | 5.401731 |
hep-th/0310201 | David Nolland | D. Nolland | Cancellation of divergences in ${\cal N}=4$ SYM/Type IIB Supergravity
correspondence | 7 pages | Phys.Lett. B579 (2004) 235-238 | 10.1016/j.physletb.2003.10.084 | LTH608 | hep-th | null | Using Schr\"odinger functional methods, we show that in the ${\cal N}=4$
SYM/Type IIB Supergravity correspondence the renormalisation of the boundary
Newton and gravitational constants arising from bulk fields cancels when we sum
over all the Kaluza-Klein modes of Supergravity. This accords with the expected
finitene... | [
{
"created": "Tue, 21 Oct 2003 15:03:48 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Nolland",
"D.",
""
]
] | Using Schr\"odinger functional methods, we show that in the ${\cal N}=4$ SYM/Type IIB Supergravity correspondence the renormalisation of the boundary Newton and gravitational constants arising from bulk fields cancels when we sum over all the Kaluza-Klein modes of Supergravity. This accords with the expected finiteness... | 9.104894 | 9.456506 | 9.794808 | 8.550187 | 8.233994 | 8.464187 | 9.192484 | 8.428156 | 8.897631 | 8.910525 | 8.93266 | 9.021853 | 8.489286 | 8.500152 | 8.511106 | 9.003724 | 8.656677 | 9.031196 | 8.486213 | 8.79228 | 8.485332 |
1907.03781 | Enrique Alvarez | Enrique Alvarez, Jesus Anero and Raquel Santos-Garcia | Scalar Weyl anomalies and the dynamics of the gravitational field | 24 pages, streamlined, some errata fixed | null | null | IFT-UAM/CSIC-19-90 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The generalization of scale invariance when gravitational effects are
considered is Weyl invariance, namely, invariance under (global or local)
rescalings of the metric. In this work, we discuss in some details the
implications of the fact that the value of the anomaly for the global Weyl
invariant coupling of scalar... | [
{
"created": "Mon, 8 Jul 2019 18:00:24 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Nov 2019 07:45:08 GMT",
"version": "v2"
},
{
"created": "Sat, 18 Jun 2022 12:41:42 GMT",
"version": "v3"
},
{
"created": "Wed, 7 Sep 2022 13:29:36 GMT",
"version": "v4"
},
{
"cre... | 2022-10-14 | [
[
"Alvarez",
"Enrique",
""
],
[
"Anero",
"Jesus",
""
],
[
"Santos-Garcia",
"Raquel",
""
]
] | The generalization of scale invariance when gravitational effects are considered is Weyl invariance, namely, invariance under (global or local) rescalings of the metric. In this work, we discuss in some details the implications of the fact that the value of the anomaly for the global Weyl invariant coupling of scalar f... | 8.817036 | 8.352938 | 8.540141 | 7.389803 | 7.907889 | 7.940956 | 7.912045 | 7.688634 | 8.122115 | 9.250006 | 7.889368 | 7.569047 | 8.295505 | 8.125987 | 7.871676 | 7.927578 | 7.86652 | 7.674035 | 7.572982 | 8.169449 | 7.893379 |
hep-th/0202049 | Bogdan Kulik | A. Boyarsky and B. Kulik | Brane-Bulk Interaction in Topological Theory | 10 pages, minor corrections, references added, to appear in Phys.
Lett. B | Phys.Lett. B532 (2002) 357-362 | 10.1016/S0370-2693(02)01570-8 | YITP-SB-02-05 | hep-th | null | In this letter we address the problem of inducing boundary degrees of freedom
from a bulk theory whose action contains higher-derivative corrections. As a
model example we consider a topological theory with an action that has only a
``higher-derivative'' term. By choosing specific coupling of the brane to the
bulk we... | [
{
"created": "Fri, 8 Feb 2002 00:15:17 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Mar 2002 19:50:16 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Boyarsky",
"A.",
""
],
[
"Kulik",
"B.",
""
]
] | In this letter we address the problem of inducing boundary degrees of freedom from a bulk theory whose action contains higher-derivative corrections. As a model example we consider a topological theory with an action that has only a ``higher-derivative'' term. By choosing specific coupling of the brane to the bulk we s... | 11.023482 | 9.868766 | 9.472159 | 9.144389 | 10.368731 | 9.735112 | 9.426668 | 9.648416 | 8.97737 | 10.913477 | 8.977491 | 8.938317 | 9.692497 | 8.932517 | 9.102118 | 9.460664 | 9.102106 | 8.955773 | 9.294884 | 9.733912 | 9.3565 |
0904.0367 | Shin'ichi Nojiri | Yusaku Ito and Shin'ichi Nojiri | Gauss-Bonnet Chameleon Mechanism of Dark Energy | LaTeX 11 pages, no figure | Phys.Rev.D79:103008,2009 | 10.1103/PhysRevD.79.103008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As a model of the current accelerated expansion of the universe, we consider
a model of the scalar-Einstein-Gauss-Bonnet gravity. This model includes the
propagating scalar modes, which might give a large correction to the Newton
law. In order to avoid this problem, we propose an extension of the Chameleon
mechanism ... | [
{
"created": "Thu, 2 Apr 2009 11:44:51 GMT",
"version": "v1"
}
] | 2009-07-30 | [
[
"Ito",
"Yusaku",
""
],
[
"Nojiri",
"Shin'ichi",
""
]
] | As a model of the current accelerated expansion of the universe, we consider a model of the scalar-Einstein-Gauss-Bonnet gravity. This model includes the propagating scalar modes, which might give a large correction to the Newton law. In order to avoid this problem, we propose an extension of the Chameleon mechanism wh... | 7.340325 | 7.174766 | 6.51518 | 6.590323 | 7.067318 | 7.049809 | 6.528443 | 6.717252 | 7.039389 | 6.675179 | 7.116925 | 6.637042 | 6.547585 | 6.521032 | 6.796549 | 6.642342 | 6.756029 | 6.39113 | 6.790764 | 6.708147 | 6.868566 |
hep-th/0509170 | David Kutasov | David Kutasov | Accelerating Branes and the String/Black Hole Transition | 32 pages, harvmac | null | null | null | hep-th | null | String theory in Euclidean flat space with a spacelike linear dilaton
contains a D1-brane which looks like a semi-infinite hairpin. In addition to
its curved shape, this ``hairpin brane'' has a condensate of the open string
tachyon stretched between its two sides. The tachyon smears the brane and
shifts the location ... | [
{
"created": "Thu, 22 Sep 2005 00:38:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kutasov",
"David",
""
]
] | String theory in Euclidean flat space with a spacelike linear dilaton contains a D1-brane which looks like a semi-infinite hairpin. In addition to its curved shape, this ``hairpin brane'' has a condensate of the open string tachyon stretched between its two sides. The tachyon smears the brane and shifts the location of... | 6.905442 | 6.747881 | 7.277081 | 6.375794 | 6.692358 | 7.026431 | 6.727641 | 6.289675 | 6.4031 | 7.943751 | 6.402159 | 6.468553 | 6.510405 | 6.266577 | 6.424204 | 6.416129 | 6.445463 | 6.428068 | 6.253911 | 6.613526 | 6.367444 |
hep-th/0205103 | Brett McInnes | Brett McInnes | Stringy Instability of Topologically Non-Trivial Ads Black Holes and of
desitter S-Brane Spacetimes | References added, NPB version | Nucl.Phys.B660:373-388,2003 | 10.1016/S0550-3213(03)00268-2 | null | hep-th | null | Seiberg and Witten have discussed a specifically "stringy" kind of
instability which arises in connection with "large" branes in asymptotically
AdS spacetimes. It is easy to see that this instability actually arises in most
five-dimensional asymptotically AdS black hole string spacetimes with
non-trivial horizon topo... | [
{
"created": "Sat, 11 May 2002 07:42:39 GMT",
"version": "v1"
},
{
"created": "Sat, 18 May 2002 07:20:25 GMT",
"version": "v2"
},
{
"created": "Thu, 30 May 2002 05:16:02 GMT",
"version": "v3"
},
{
"created": "Wed, 11 Dec 2002 14:12:25 GMT",
"version": "v4"
},
{
"c... | 2010-12-23 | [
[
"McInnes",
"Brett",
""
]
] | Seiberg and Witten have discussed a specifically "stringy" kind of instability which arises in connection with "large" branes in asymptotically AdS spacetimes. It is easy to see that this instability actually arises in most five-dimensional asymptotically AdS black hole string spacetimes with non-trivial horizon topolo... | 10.033681 | 10.493129 | 10.555857 | 10.486124 | 10.345834 | 10.570971 | 10.404091 | 10.404419 | 10.217854 | 11.369354 | 10.201172 | 9.609982 | 9.858646 | 9.430581 | 9.730179 | 9.567734 | 9.736108 | 9.81655 | 9.61751 | 9.893394 | 9.699124 |
hep-th/9806229 | Francesco Sannino | Francesco Sannino (Yale University) | From Super QCD to QCD | Contribution to the proceedings of the MRST-98 meeting. 9 pages,
RevTeX | null | 10.1063/1.57083 | YCTP-P19-98 | hep-th hep-ph | null | We present a ``toy'' model for breaking supersymmetric gauge theories at the
effective Lagrangian level. We show that it is possible to achieve the
decoupling of gluinos and squarks, below a given supersymmetry breaking scale
m, in the fundamental theory for super QCD once a suitable choice of
supersymmetry breaking ... | [
{
"created": "Mon, 29 Jun 1998 14:41:33 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Sannino",
"Francesco",
"",
"Yale University"
]
] | We present a ``toy'' model for breaking supersymmetric gauge theories at the effective Lagrangian level. We show that it is possible to achieve the decoupling of gluinos and squarks, below a given supersymmetry breaking scale m, in the fundamental theory for super QCD once a suitable choice of supersymmetry breaking te... | 12.492332 | 11.505675 | 11.58445 | 11.489975 | 11.56752 | 11.26212 | 12.723778 | 11.204888 | 11.318352 | 13.429761 | 11.352775 | 11.684804 | 12.400629 | 12.074929 | 11.85701 | 12.019454 | 12.01322 | 12.20346 | 12.092402 | 12.088441 | 12.010611 |
2405.17553 | Matti Jarvinen | Matti Jarvinen, Dorin Weissman | A black hole effective theory for strongly interacting matter | 10 pages, 2 figures | null | null | APCTP Pre2024 - 012 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish a new tool for studying strongly coupled matter: an effective
theory of black holes in gravity, which maps to a hydrodynamic description of
field theories via the gauge-gravity duality. Our approach is inspired by
previously known effective theories found in the limit of high number of
dimensions. We arg... | [
{
"created": "Mon, 27 May 2024 18:00:01 GMT",
"version": "v1"
}
] | 2024-05-29 | [
[
"Jarvinen",
"Matti",
""
],
[
"Weissman",
"Dorin",
""
]
] | We establish a new tool for studying strongly coupled matter: an effective theory of black holes in gravity, which maps to a hydrodynamic description of field theories via the gauge-gravity duality. Our approach is inspired by previously known effective theories found in the limit of high number of dimensions. We argue... | 12.146934 | 11.878888 | 12.717907 | 11.100875 | 12.489158 | 11.310803 | 11.81633 | 11.14127 | 11.03474 | 11.918456 | 12.094091 | 11.344527 | 11.665941 | 11.691628 | 11.388881 | 11.474722 | 11.519935 | 11.12512 | 11.345294 | 11.988424 | 11.053453 |
2302.04895 | Henriette Elvang | Alan Shih-Kuan Chen, Henriette Elvang, Aidan Herderschee | Bootstrapping the String KLT Kernel | 8 pages, LCTP-23-01 | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that a generalized version of the 4-point string theory KLT
double-copy map is the most general solution to the minimal-rank double-copy
bootstrap in effective field theory. This follows from significant restrictions
of the 4-point map resulting from the 6-point bootstrap analysis. The
generalized 4-point dou... | [
{
"created": "Thu, 9 Feb 2023 19:00:33 GMT",
"version": "v1"
}
] | 2023-02-13 | [
[
"Chen",
"Alan Shih-Kuan",
""
],
[
"Elvang",
"Henriette",
""
],
[
"Herderschee",
"Aidan",
""
]
] | We show that a generalized version of the 4-point string theory KLT double-copy map is the most general solution to the minimal-rank double-copy bootstrap in effective field theory. This follows from significant restrictions of the 4-point map resulting from the 6-point bootstrap analysis. The generalized 4-point doubl... | 12.684854 | 13.636425 | 14.105213 | 11.857878 | 13.004786 | 14.133294 | 13.464565 | 13.197125 | 12.078082 | 14.208032 | 11.886463 | 12.583924 | 13.274964 | 12.491885 | 12.186576 | 12.857367 | 12.526567 | 12.388584 | 12.576929 | 13.262567 | 12.341723 |
hep-th/0604132 | Shahn Majid | S. Majid | Algebraic approach to quantum gravity III: noncommmutative Riemannian
geometry | 25 pages, 1 .eps figure, to appear in collection B. Fauser and J.
Tolksdorf, eds., Birkhauser | null | null | null | hep-th gr-qc math.QA | null | This is a self-contained introduction to quantum Riemannian geometry based on
quantum groups as frame groups, and its proposed role in quantum gravity. Much
of the article is about the generalisation of classical Riemannian geometry
that arises naturally as the classical limit; a theory with nonsymmetric metric
and a... | [
{
"created": "Wed, 19 Apr 2006 12:05:05 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Majid",
"S.",
""
]
] | This is a self-contained introduction to quantum Riemannian geometry based on quantum groups as frame groups, and its proposed role in quantum gravity. Much of the article is about the generalisation of classical Riemannian geometry that arises naturally as the classical limit; a theory with nonsymmetric metric and a s... | 21.531843 | 20.183128 | 16.580103 | 16.328991 | 19.01272 | 18.189301 | 21.569836 | 19.302311 | 18.56673 | 24.16 | 18.532131 | 18.05118 | 18.847309 | 17.807306 | 17.623381 | 18.119131 | 18.818329 | 17.862453 | 17.159561 | 18.776417 | 17.049992 |
2406.19988 | James Edwards | F. Bastianelli, O. Corradini, J.P. Edwards, D.G.C. McKeon, C. Schubert | Unified worldline treatment of Yukawa and axial couplings | 32 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a worldline representation of the one-loop effective action for a
Dirac particle coupled to external scalar, pseudoscalar, vector and axialvector
fields. Extending previous work by two of the authors on the pure
vector-axialvector case to all four couplings, it allows one to treat the real
and the imaginar... | [
{
"created": "Fri, 28 Jun 2024 15:19:24 GMT",
"version": "v1"
}
] | 2024-07-01 | [
[
"Bastianelli",
"F.",
""
],
[
"Corradini",
"O.",
""
],
[
"Edwards",
"J. P.",
""
],
[
"McKeon",
"D. G. C.",
""
],
[
"Schubert",
"C.",
""
]
] | We provide a worldline representation of the one-loop effective action for a Dirac particle coupled to external scalar, pseudoscalar, vector and axialvector fields. Extending previous work by two of the authors on the pure vector-axialvector case to all four couplings, it allows one to treat the real and the imaginary ... | 10.67208 | 11.119939 | 11.380002 | 9.885762 | 11.514648 | 11.011122 | 10.766641 | 10.558531 | 10.145908 | 10.851333 | 10.122529 | 9.848965 | 9.886878 | 9.961401 | 10.117959 | 9.85966 | 10.210287 | 9.880022 | 9.883075 | 10.293653 | 9.889943 |
hep-th/0306210 | Mikhail Plyushchay | Andres Anabalon and Mikhail S. Plyushchay | Interaction via reduction and nonlinear superconformal symmetry | 12 pages; typos corrected | Phys.Lett. B572 (2003) 202-209 | 10.1016/j.physletb.2003.08.030 | null | hep-th math-ph math.MP nlin.SI | null | We show that the reduction of a planar free spin-1/2 particle system by the
constraint fixing its total angular momentum produces the one-dimensional
Akulov-Pashnev-Fubini-Rabinovici superconformal mechanics model with the
nontrivially coupled boson and fermion degrees of freedom. The modification of
the constraint b... | [
{
"created": "Fri, 20 Jun 2003 21:54:34 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jun 2003 14:43:48 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Sep 2003 20:21:34 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Anabalon",
"Andres",
""
],
[
"Plyushchay",
"Mikhail S.",
""
]
] | We show that the reduction of a planar free spin-1/2 particle system by the constraint fixing its total angular momentum produces the one-dimensional Akulov-Pashnev-Fubini-Rabinovici superconformal mechanics model with the nontrivially coupled boson and fermion degrees of freedom. The modification of the constraint by ... | 13.562782 | 15.096462 | 16.822048 | 13.93214 | 14.327478 | 15.06845 | 14.025311 | 13.707567 | 13.766809 | 18.309559 | 13.432069 | 13.2285 | 14.168335 | 13.884 | 13.967752 | 13.351568 | 13.428508 | 13.25296 | 13.341186 | 13.788466 | 13.106792 |
hep-th/0402195 | Gary McCartor | Yuji Nakawaki and Gary McCartor | Extended Hamiltonian Formalism of the Pure Space-Like Axial Gauge
Schwinger Model II | 19 pages | Prog.Theor.Phys. 111 (2004) 943-960 | 10.1143/PTP.111.943 | SMUHEP/04-01 | hep-th | null | Canonical methods are not sufficient to properly quantize space-like axial
gauges. In this paper, we obtain guiding principles which allow the
construction of an extended Hamiltonian formalism for pure space-like axial
gauge fields. To do so, we clarify the general role residual gauge fields play
in the space-like ax... | [
{
"created": "Tue, 24 Feb 2004 21:55:36 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Nakawaki",
"Yuji",
""
],
[
"McCartor",
"Gary",
""
]
] | Canonical methods are not sufficient to properly quantize space-like axial gauges. In this paper, we obtain guiding principles which allow the construction of an extended Hamiltonian formalism for pure space-like axial gauge fields. To do so, we clarify the general role residual gauge fields play in the space-like axia... | 9.360443 | 9.693414 | 10.096998 | 9.487231 | 9.93895 | 10.098399 | 9.60749 | 9.577103 | 9.305258 | 10.79641 | 9.570355 | 9.314543 | 9.634855 | 9.372353 | 9.598297 | 9.258503 | 9.527859 | 9.545835 | 9.329612 | 9.834914 | 9.190496 |
hep-th/9301114 | null | M. Bonini, M. D'Attanasio and G. Marchesini | Perturbative renormalization and infrared finiteness in the Wilson
renormalization group: the massless scalar case | Latex file, 21 pages and 6 figures (included), Parma Univ. preprint
UPRF-92-360 | Nucl.Phys. B409 (1993) 441-464 | 10.1016/0550-3213(93)90588-G | null | hep-th | null | A new proof of perturbative renormalizability and infrared finiteness for a
scalar massless theory is obtained from a formulation of renormalized field
theory based on the Wilson renormalization group. The loop expansion of the
renormalized Green functions is deduced from the Polchinski equation of
renormalization gr... | [
{
"created": "Wed, 27 Jan 1993 15:59:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Bonini",
"M.",
""
],
[
"D'Attanasio",
"M.",
""
],
[
"Marchesini",
"G.",
""
]
] | A new proof of perturbative renormalizability and infrared finiteness for a scalar massless theory is obtained from a formulation of renormalized field theory based on the Wilson renormalization group. The loop expansion of the renormalized Green functions is deduced from the Polchinski equation of renormalization grou... | 7.29178 | 7.68512 | 7.913724 | 7.297083 | 7.999727 | 8.139728 | 7.759581 | 7.577369 | 7.406774 | 8.996047 | 7.206007 | 7.306699 | 7.313725 | 7.076198 | 7.245401 | 7.264732 | 7.378802 | 7.082322 | 7.216823 | 7.429752 | 7.293461 |
1007.1457 | Pedro Pina Avelino | P.P. Avelino, D. Bazeia, R. Menezes, J.G.G.S. Ramos | Localized D-dimensional global k-defects | 6 pages, published version | Eur.Phys.J.C71:1683,2011 | 10.1140/epjc/s10052-011-1683-5 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly demonstrate the existence of static global defect solutions of
arbitrary dimensionality whose energy does not diverge at spatial infinity, by
considering maximally symmetric solutions described by an action with
non-standard kinetic terms in a D+1 dimensional Minkowski space-time. We
analytically determ... | [
{
"created": "Thu, 8 Jul 2010 20:00:08 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Oct 2010 18:41:47 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Jul 2011 08:25:28 GMT",
"version": "v3"
}
] | 2011-07-05 | [
[
"Avelino",
"P. P.",
""
],
[
"Bazeia",
"D.",
""
],
[
"Menezes",
"R.",
""
],
[
"Ramos",
"J. G. G. S.",
""
]
] | We explicitly demonstrate the existence of static global defect solutions of arbitrary dimensionality whose energy does not diverge at spatial infinity, by considering maximally symmetric solutions described by an action with non-standard kinetic terms in a D+1 dimensional Minkowski space-time. We analytically determin... | 12.155704 | 11.706219 | 12.558421 | 11.9519 | 11.562042 | 11.098511 | 10.995735 | 11.58566 | 10.895159 | 12.12811 | 11.912451 | 11.334119 | 11.85017 | 11.213793 | 11.127295 | 11.479525 | 11.425367 | 11.295866 | 11.533668 | 11.155985 | 11.4271 |
1606.01770 | Herondy Mota | H. F. Mota, E. R. Bezerra de Mello, C. H. G. Bessa, V. B. Bezerra | Light-Cone Fluctuations in the Cosmic String Spacetime | 19 pages, 1 figure | Phys. Rev. D 94, 024039 (2016) | 10.1103/PhysRevD.94.024039 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we consider light-cone fluctuations arising as a consequence of
the nontrivial topology of the locally flat cosmic string spacetime. By setting
the light-cone along the z-direction we are able to develop a full analysis to
calculate the renormalized graviton two-point function, as well as the mean
squar... | [
{
"created": "Mon, 6 Jun 2016 14:48:00 GMT",
"version": "v1"
}
] | 2016-07-27 | [
[
"Mota",
"H. F.",
""
],
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Bessa",
"C. H. G.",
""
],
[
"Bezerra",
"V. B.",
""
]
] | In this paper we consider light-cone fluctuations arising as a consequence of the nontrivial topology of the locally flat cosmic string spacetime. By setting the light-cone along the z-direction we are able to develop a full analysis to calculate the renormalized graviton two-point function, as well as the mean square ... | 9.237816 | 9.498857 | 9.146457 | 8.31926 | 9.002451 | 9.080542 | 8.576521 | 9.126163 | 8.481193 | 9.692613 | 8.874193 | 8.804279 | 9.170874 | 9.153328 | 8.818788 | 8.66674 | 9.107054 | 8.701866 | 9.151128 | 9.166947 | 9.010579 |
hep-th/0203089 | Kluson Josef | J. Kluson | Marginal Deformations In the Open Bosonic String Field Theory for N
D0-branes | 14 pages | Class.Quant.Grav. 20 (2003) 827-844 | 10.1088/0264-9381/20/5/304 | null | hep-th | null | In this short note we give an example of the exact solution of the open
bosonic string field theory defined on the background of $N$ coincided
D0-branes. This solution leads to the change of the original background to the
background where D0-branes are localised in general positions.
| [
{
"created": "Sun, 10 Mar 2002 11:09:35 GMT",
"version": "v1"
}
] | 2017-01-18 | [
[
"Kluson",
"J.",
""
]
] | In this short note we give an example of the exact solution of the open bosonic string field theory defined on the background of $N$ coincided D0-branes. This solution leads to the change of the original background to the background where D0-branes are localised in general positions. | 12.027816 | 8.059215 | 9.78007 | 7.842738 | 8.628622 | 8.638299 | 7.905687 | 8.967013 | 8.757175 | 9.530278 | 8.557374 | 7.823744 | 8.293563 | 8.467413 | 8.797441 | 8.069395 | 7.857615 | 8.213726 | 8.299505 | 8.909119 | 8.652476 |
hep-th/0510154 | Andrzej Borowiec | A. Borowiec (IFT, Wroclaw Univ.), J. Lukierski (IFT, Wroclaw Univ.),
V.N. Tolstoy (INP, Moscow State Univ.) | On Twist Quantizations of D=4 Lorentz and Poincare Algebras | 6 pages, presented during the XIVth International Colloquium on
Integrable Systems (ISQS-14), Prague, June 16-18, 2005; to appear in Czech.
J. Phys. v.55 no. 11 (2005) | Czech.J.Phys.55:11,2005 | 10.1007/s10582-006-0008-7 | null | hep-th math-ph math.MP math.QA | null | We use the decomposition of o(3,1)=sl(2;C)_1\oplus sl(2;C)_2 in order to
describe nonstandard quantum deformation of o(3,1) linked with Jordanian
deformation of sl(2;C}. Using twist quantization technique we obtain the
deformed coproducts and antipodes which can be expressed in terms of real
physical Lorentz generato... | [
{
"created": "Tue, 18 Oct 2005 14:58:14 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Borowiec",
"A.",
"",
"IFT, Wroclaw Univ."
],
[
"Lukierski",
"J.",
"",
"IFT, Wroclaw Univ."
],
[
"Tolstoy",
"V. N.",
"",
"INP, Moscow State Univ."
]
] | We use the decomposition of o(3,1)=sl(2;C)_1\oplus sl(2;C)_2 in order to describe nonstandard quantum deformation of o(3,1) linked with Jordanian deformation of sl(2;C}. Using twist quantization technique we obtain the deformed coproducts and antipodes which can be expressed in terms of real physical Lorentz generators... | 10.013669 | 8.274747 | 10.761892 | 8.231467 | 8.074953 | 7.68803 | 7.814449 | 8.201384 | 7.467509 | 11.070908 | 8.14056 | 8.271635 | 9.54457 | 8.558012 | 8.43938 | 8.466173 | 8.223546 | 8.297596 | 8.407161 | 9.308024 | 8.738303 |
1107.1325 | Jonathan Pearson Mr | Richard A. Battye, Jonathan A. Pearson, Adam Moss | X-type and Y-type junction stability in domain wall networks | 24 pages, 13 figures; typos fixed | null | 10.1103/PhysRevD.84.125032 | null | hep-th astro-ph.CO cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop an analytic formalism that allows one to quantify the stability
properties of X-type and Y-type junctions in domain wall networks in two
dimensions. A similar approach might be applicable to more general defect
systems involving junctions that appear in a range of physical situations, for
example, in the c... | [
{
"created": "Thu, 7 Jul 2011 09:38:44 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Jan 2012 10:07:32 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Battye",
"Richard A.",
""
],
[
"Pearson",
"Jonathan A.",
""
],
[
"Moss",
"Adam",
""
]
] | We develop an analytic formalism that allows one to quantify the stability properties of X-type and Y-type junctions in domain wall networks in two dimensions. A similar approach might be applicable to more general defect systems involving junctions that appear in a range of physical situations, for example, in the con... | 9.180621 | 10.787569 | 10.177379 | 9.527941 | 10.938858 | 11.184129 | 10.317931 | 9.70668 | 9.798162 | 11.18615 | 9.462195 | 9.603244 | 9.892311 | 9.382865 | 9.675519 | 9.669025 | 9.577992 | 9.58271 | 9.345075 | 9.701352 | 9.252048 |
hep-th/9412207 | Giovanni Felder | Giovanni Felder | Elliptic quantum groups | 9 pages, LaTeX | null | null | null | hep-th | null | This note for the Proceedings of the International Congress of Mathematical
Physics gives an account of a construction of an ``elliptic quantum group''
associated with each simple classical Lie algebra. It is closely related to
elliptic face models of statistical mechanics, and, in its semiclassical limit,
to the Wes... | [
{
"created": "Thu, 22 Dec 1994 11:03:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Felder",
"Giovanni",
""
]
] | This note for the Proceedings of the International Congress of Mathematical Physics gives an account of a construction of an ``elliptic quantum group'' associated with each simple classical Lie algebra. It is closely related to elliptic face models of statistical mechanics, and, in its semiclassical limit, to the Wess-... | 9.857754 | 11.212521 | 10.422997 | 8.787238 | 8.892724 | 9.752196 | 9.193438 | 9.939004 | 9.353757 | 11.075681 | 9.389037 | 9.020069 | 9.753986 | 8.645976 | 8.789515 | 8.479613 | 8.945865 | 8.718728 | 8.567583 | 9.57697 | 8.287393 |
0907.3238 | Arkady Tseytlin | A.A. Tseytlin | Quantum strings in AdS5 x S5 and AdS/CFT duality | 13 pages. Contribution to proceedings of the conference: "Crossing
the boundaries: Gauge dynamics at strong coupling", honoring the 60th
birthday of M.A. Shifman, Minneapolis, May 14-17, 2009. misprints corrected | Int.J.Mod.Phys.A25:319-331,2010 | 10.1142/S0217751X10048640 | IMPERIAL-TP-AT-2009-4 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review some recent progress in understanding the spectrum of
energies/dimensions of strings/operators in AdS5 x S5 -- planar N=4 super
Yang-Mills correspondence. We consider leading strong coupling corrections to
the energy of lightest massive string modes in AdS5 x S5, which should be dual
to members of the Konis... | [
{
"created": "Sat, 18 Jul 2009 18:57:13 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jul 2009 09:50:02 GMT",
"version": "v2"
},
{
"created": "Fri, 31 Jul 2009 12:53:10 GMT",
"version": "v3"
},
{
"created": "Wed, 23 Sep 2009 15:59:25 GMT",
"version": "v4"
},
{
"c... | 2020-12-08 | [
[
"Tseytlin",
"A. A.",
""
]
] | We review some recent progress in understanding the spectrum of energies/dimensions of strings/operators in AdS5 x S5 -- planar N=4 super Yang-Mills correspondence. We consider leading strong coupling corrections to the energy of lightest massive string modes in AdS5 x S5, which should be dual to members of the Konishi... | 9.622322 | 8.699225 | 11.366529 | 8.708439 | 9.098223 | 9.333963 | 8.470793 | 8.622971 | 8.18012 | 12.93614 | 8.665873 | 8.795875 | 9.463434 | 8.936213 | 9.303516 | 8.602591 | 8.902452 | 8.887445 | 8.85982 | 9.539465 | 8.818252 |
hep-th/9301082 | null | Jun Liu | Evolution of Pure States into Mixed States | 6 pages | null | null | SU-ITP-93-1 | hep-th | null | In the formulation of Banks, Peskin and Susskind, we show that one can
construct evolution equations for the quantum mechanical density matrix $\rho$
with operators which do not commute with hamiltonian which evolve pure states
into mixed states, preserve the normalization and positivity of $\rho$ and
conserve energy... | [
{
"created": "Tue, 19 Jan 1993 21:29:00 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Jan 1993 18:29:00 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Liu",
"Jun",
""
]
] | In the formulation of Banks, Peskin and Susskind, we show that one can construct evolution equations for the quantum mechanical density matrix $\rho$ with operators which do not commute with hamiltonian which evolve pure states into mixed states, preserve the normalization and positivity of $\rho$ and conserve energy. ... | 17.162294 | 17.131523 | 18.712948 | 14.927734 | 14.64851 | 13.256029 | 15.478502 | 14.279623 | 14.256868 | 16.640974 | 14.7995 | 14.493984 | 14.574471 | 14.356545 | 14.320017 | 14.171038 | 15.189012 | 14.309195 | 14.363603 | 15.340848 | 15.070943 |
0706.0442 | Nikolay Bobev | N.P. Bobev and R.C. Rashkov | Spiky Strings, Giant Magnons and beta-deformations | 20 pages, 2 figures; v2: typos corrected, references added | Phys.Rev.D76:046008,2007 | 10.1103/PhysRevD.76.046008 | null | hep-th | null | We study rigid string solutions rotating on the S^3 subspace of the
beta-deformed AdS_5xS^5 background found by Lunin and Maldacena. For particular
values of the parameters of the solutions we find the known giant magnon and
single spike strings. We present a single spike string solution on the deformed
S^3 and find ... | [
{
"created": "Mon, 4 Jun 2007 14:10:44 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jun 2007 00:11:36 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bobev",
"N. P.",
""
],
[
"Rashkov",
"R. C.",
""
]
] | We study rigid string solutions rotating on the S^3 subspace of the beta-deformed AdS_5xS^5 background found by Lunin and Maldacena. For particular values of the parameters of the solutions we find the known giant magnon and single spike strings. We present a single spike string solution on the deformed S^3 and find ho... | 7.369856 | 5.830643 | 8.47295 | 6.043156 | 6.055519 | 6.261308 | 6.040132 | 5.804433 | 6.000499 | 7.976639 | 6.18839 | 6.332229 | 7.544551 | 6.427852 | 6.654013 | 6.372308 | 6.528223 | 6.339796 | 6.605162 | 7.468602 | 6.758769 |
1407.3478 | Dionisio Bazeia | D. Bazeia, L. Losano, M.A. Marques, R. Menezes | From Kinks to Compactons | 7 pages, 7 figures; new version, to appear in PLB | Phys. Lett. B 736 (2014) 515 | 10.1016/j.physletb.2014.08.015 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work deals with the presence of localized structures in relativistic
systems described by a single real scalar field in two-dimensional spacetime.
We concentrate on kinks and compactons in models with standard kinematics, and
we develop a procedure that help us to smoothly go from kinks to compactons in
the sugg... | [
{
"created": "Sun, 13 Jul 2014 15:22:28 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Aug 2014 21:00:18 GMT",
"version": "v2"
}
] | 2014-08-26 | [
[
"Bazeia",
"D.",
""
],
[
"Losano",
"L.",
""
],
[
"Marques",
"M. A.",
""
],
[
"Menezes",
"R.",
""
]
] | This work deals with the presence of localized structures in relativistic systems described by a single real scalar field in two-dimensional spacetime. We concentrate on kinks and compactons in models with standard kinematics, and we develop a procedure that help us to smoothly go from kinks to compactons in the sugges... | 13.663226 | 8.331507 | 13.161885 | 9.883127 | 10.177056 | 10.089657 | 9.681866 | 8.536607 | 9.292142 | 14.884915 | 9.915735 | 10.879981 | 12.597748 | 11.567747 | 11.329318 | 11.488321 | 11.207026 | 11.353194 | 11.642671 | 12.424823 | 11.482447 |
2301.02342 | Satoshi Nawata | Yanyan Chen, Jiaqun Jiang, Satoshi Nawata and Yilu Shao | Instantons on Young diagrams with matters | 32 pages, Mathematica file is attached: v2, typos corrected, JHEP
version | null | 10.1007/JHEP03(2023)120 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We present the unrefined instanton partition functions of various 5d gauge
theories with matter beyond the fundamental representation as sums over Young
diagrams. By using these explicit expressions, we verify a range of identities
among the instanton partition functions predicted by Higgsing procedures of
fivebrane ... | [
{
"created": "Fri, 6 Jan 2023 00:33:15 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Mar 2023 17:33:04 GMT",
"version": "v2"
}
] | 2023-04-05 | [
[
"Chen",
"Yanyan",
""
],
[
"Jiang",
"Jiaqun",
""
],
[
"Nawata",
"Satoshi",
""
],
[
"Shao",
"Yilu",
""
]
] | We present the unrefined instanton partition functions of various 5d gauge theories with matter beyond the fundamental representation as sums over Young diagrams. By using these explicit expressions, we verify a range of identities among the instanton partition functions predicted by Higgsing procedures of fivebrane we... | 17.493715 | 14.17096 | 17.619699 | 14.306486 | 13.574288 | 13.741357 | 14.373767 | 14.48705 | 13.28974 | 18.944759 | 12.447092 | 13.614285 | 15.029928 | 13.676014 | 13.601481 | 13.987904 | 14.187596 | 14.628686 | 14.735435 | 14.701299 | 13.547602 |
2306.05206 | Marina David | Marina David, Nizar Ezroura, and Finn Larsen | The Attractor Flow for AdS$_5$ Black Holes in $\mathcal{N} = 2$ Gauged
Supergravity | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study the flow equations for BPS black holes in $\mathcal{N} = 2$
five-dimensional gauged supergravity coupled to any number of vector multiplets
via FI couplings. We develop the Noether-Wald procedure in this context and
exhibit the conserved charges as explicit integrals of motion, in the sense
that they can be ... | [
{
"created": "Thu, 8 Jun 2023 14:03:25 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Aug 2023 10:50:47 GMT",
"version": "v2"
}
] | 2023-08-28 | [
[
"David",
"Marina",
""
],
[
"Ezroura",
"Nizar",
""
],
[
"Larsen",
"Finn",
""
]
] | We study the flow equations for BPS black holes in $\mathcal{N} = 2$ five-dimensional gauged supergravity coupled to any number of vector multiplets via FI couplings. We develop the Noether-Wald procedure in this context and exhibit the conserved charges as explicit integrals of motion, in the sense that they can be co... | 10.904694 | 11.38723 | 13.254463 | 10.98946 | 10.872619 | 10.716158 | 11.535015 | 11.019893 | 11.451458 | 13.264789 | 11.029666 | 10.663099 | 11.291284 | 11.151145 | 10.888337 | 10.810828 | 10.591781 | 10.526729 | 10.99206 | 11.002131 | 11.003558 |
hep-th/0306168 | Clifford V. Johnson | James E. Carlisle, Clifford V. Johnson | Holographic RG Flows and Universal Structures on the Coulomb Branch of
N=2 Supersymmetric Large n Gauge Theory | 14 pages, LaTeX, 1 figure | JHEP 0307 (2003) 039 | 10.1088/1126-6708/2003/07/039 | DCPT-03/25 | hep-th | null | We report on our results of D3-brane probing a large class of generalised
type IIB supergravity solutions presented very recently in the literature. The
structure of the solutions is controlled by a single non-linear differential
equation. These solutions correspond to renormalisation group flows from pure
N=4 supers... | [
{
"created": "Wed, 18 Jun 2003 18:06:55 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jul 2003 16:54:27 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Carlisle",
"James E.",
""
],
[
"Johnson",
"Clifford V.",
""
]
] | We report on our results of D3-brane probing a large class of generalised type IIB supergravity solutions presented very recently in the literature. The structure of the solutions is controlled by a single non-linear differential equation. These solutions correspond to renormalisation group flows from pure N=4 supersym... | 13.260878 | 13.079625 | 14.620875 | 12.558732 | 13.131891 | 12.924538 | 13.117929 | 13.148955 | 12.753609 | 15.217995 | 12.284078 | 12.767184 | 13.664235 | 12.360921 | 12.960878 | 12.770329 | 12.795301 | 12.939602 | 12.652091 | 13.451492 | 12.594472 |
hep-th/0501205 | Seiji Sakoda | Seiji Sakoda | Euclidean Path Integral of the Gauge Field -- Holomorphic Representation | 39 pages | null | null | null | hep-th | null | Basing on the canonical quantization of a BRS invariant Lagrangian, we
construct holomorphic representation of path integrals for Faddeev-Popov(FP)
ghosts as well as for unphysical degrees of the gauge field from covariant
operator formalism. A thorough investigation of a simple soluble gauge model
with finite degree... | [
{
"created": "Wed, 26 Jan 2005 08:08:10 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Sakoda",
"Seiji",
""
]
] | Basing on the canonical quantization of a BRS invariant Lagrangian, we construct holomorphic representation of path integrals for Faddeev-Popov(FP) ghosts as well as for unphysical degrees of the gauge field from covariant operator formalism. A thorough investigation of a simple soluble gauge model with finite degrees ... | 12.030202 | 11.662938 | 12.414533 | 11.085127 | 11.318476 | 11.678102 | 12.530389 | 11.607493 | 11.218735 | 13.444346 | 11.531317 | 11.215903 | 11.344774 | 11.121007 | 11.104548 | 11.032491 | 10.59752 | 10.592191 | 10.795449 | 11.644326 | 11.151552 |
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