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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1510.04219 | Eugenio Megias | Eugenio Megias | Out-of-equilibrium energy flow and steady state configurations in
AdS/CFT | 7 pages, 3 figures. Talk given by E.Megias at the European Physical
Society Conference on High Energy Physics (EPS-HEP2015), Vienna, Austria,
22-29 July 2015; v2 references added, acknowledgments extended | null | null | MPP-2015-218 | hep-th cond-mat.stat-mech cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study out-of-equilibrium energy flow in a strongly coupled system by using
the AdS/CFT correspondence. In particular, we describe the appearance of a
steady state connecting two asymptotic equilibrium systems. We obtain results
within the linear response regime.
| [
{
"created": "Wed, 14 Oct 2015 18:06:07 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Oct 2015 16:26:01 GMT",
"version": "v2"
}
] | 2015-10-22 | [
[
"Megias",
"Eugenio",
""
]
] | We study out-of-equilibrium energy flow in a strongly coupled system by using the AdS/CFT correspondence. In particular, we describe the appearance of a steady state connecting two asymptotic equilibrium systems. We obtain results within the linear response regime. | 13.1737 | 11.147367 | 12.645225 | 9.88768 | 9.241526 | 10.549771 | 9.98481 | 9.200521 | 9.204235 | 10.538836 | 9.820876 | 11.118804 | 11.914891 | 10.715929 | 11.540079 | 11.411764 | 11.287789 | 10.780565 | 11.824979 | 12.257837 | 11.423037 |
1401.5257 | Yu Nakayama | Yu Nakayama | $a-c$ test of holography vs quantum renormalization group | 6 pages, v2: minor corrections, v3: to be published in MPLA with all
the comments by referee 2 of JHEP taken into account | null | 10.1142/S0217732314501582 | IPMU 14-0011 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that a "constructive derivation" of the AdS/CFT correspondence based
on the quantum local renormalization group in large N quantum field theories
consistently provides the a-c holographic Weyl anomaly in d=4 at the curvature
squared order in the bulk action. The consistency of the construction further
predict... | [
{
"created": "Tue, 21 Jan 2014 10:42:14 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Feb 2014 01:31:08 GMT",
"version": "v2"
},
{
"created": "Thu, 24 Jul 2014 04:53:53 GMT",
"version": "v3"
}
] | 2014-09-18 | [
[
"Nakayama",
"Yu",
""
]
] | We show that a "constructive derivation" of the AdS/CFT correspondence based on the quantum local renormalization group in large N quantum field theories consistently provides the a-c holographic Weyl anomaly in d=4 at the curvature squared order in the bulk action. The consistency of the construction further predicts ... | 22.779722 | 19.66242 | 23.467216 | 18.129784 | 19.763432 | 21.037857 | 23.132637 | 19.534443 | 18.552967 | 25.802505 | 20.037485 | 20.32855 | 20.242472 | 19.344355 | 20.788296 | 20.12409 | 20.14027 | 19.931017 | 20.475468 | 22.043789 | 20.408031 |
hep-th/9905060 | Ramchander R. Sastry | Ramchander R. Sastry | Quantum Gravitodynamics | 10 pages, 1 eps figure, explanation added | null | null | null | hep-th gr-qc math-ph math.MP | null | The infinite dimensional generalization of the quantum mechanics of extended
objects, namely, the quantum field theory of extended objects is employed to
address the hitherto nonrenormalizable gravitational interaction following
which the cosmological constant problem is addressed. The response of an
electron to a we... | [
{
"created": "Sun, 9 May 1999 20:16:45 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Oct 1999 19:06:03 GMT",
"version": "v2"
},
{
"created": "Sat, 8 Apr 2000 06:07:23 GMT",
"version": "v3"
},
{
"created": "Wed, 12 Apr 2000 14:22:46 GMT",
"version": "v4"
},
{
"cre... | 2009-09-25 | [
[
"Sastry",
"Ramchander R.",
""
]
] | The infinite dimensional generalization of the quantum mechanics of extended objects, namely, the quantum field theory of extended objects is employed to address the hitherto nonrenormalizable gravitational interaction following which the cosmological constant problem is addressed. The response of an electron to a weak... | 16.737625 | 12.290854 | 14.501513 | 13.026939 | 12.864745 | 13.193569 | 12.53531 | 11.625294 | 13.823407 | 15.192271 | 14.440656 | 14.079389 | 14.789363 | 13.838035 | 14.800891 | 14.088953 | 14.050222 | 14.755956 | 14.698419 | 15.119937 | 14.452014 |
hep-th/0205132 | Per Anders Sundell | E. Sezgin, P. Sundell | Analysis of Higher Spin Field Equations in Four Dimensions | Latex, 30 pages, several clarifications and few references added | JHEP 0207 (2002) 055 | 10.1088/1126-6708/2002/07/055 | null | hep-th | null | The minimal bosonic higher spin gauge theory in four dimensions contains
massless particles of spin s=0,2,4,.. that arise in the symmetric product of
two spin 0 singletons. It is based on an infinite dimensional extension of the
AdS_4 algebra a la Vasiliev. We derive an expansion scheme in which the
gravitational gau... | [
{
"created": "Tue, 14 May 2002 15:15:42 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Jul 2002 09:29:48 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Sezgin",
"E.",
""
],
[
"Sundell",
"P.",
""
]
] | The minimal bosonic higher spin gauge theory in four dimensions contains massless particles of spin s=0,2,4,.. that arise in the symmetric product of two spin 0 singletons. It is based on an infinite dimensional extension of the AdS_4 algebra a la Vasiliev. We derive an expansion scheme in which the gravitational gauge... | 10.44654 | 10.801172 | 12.509424 | 9.515882 | 9.439467 | 8.910077 | 10.038517 | 9.164336 | 9.986115 | 12.083234 | 10.042338 | 9.088469 | 10.732873 | 9.765195 | 9.942768 | 9.514162 | 9.354772 | 9.773889 | 9.672768 | 10.96665 | 9.540909 |
1312.2647 | Fu Chun-E | Chun-E Fu, Yu-Xiao Liu, Heng Guo, Feng-Wei Chen, and Sheng-Li Zhang | Localization of $q-$form fields on $AdS_{p+1}$ branes | 13 pages | Physics Letters B 735 (2014) 7 | 10.1016/j.physletb.2014.06.010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we investigate localization of a free massless $q-$form bulk
field on thin and thick $AdS_{p+1}$ branes with codimension one. It is found
that the zero mode of the $q-$form field with $q>(p+2)/2$ can be localized on
the thin negative tension brane, which is different from the flat brane case
given in [... | [
{
"created": "Tue, 10 Dec 2013 02:39:24 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Dec 2013 03:08:45 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Jun 2014 07:11:24 GMT",
"version": "v3"
},
{
"created": "Fri, 13 Jun 2014 01:19:29 GMT",
"version": "v4"
}
] | 2015-06-18 | [
[
"Fu",
"Chun-E",
""
],
[
"Liu",
"Yu-Xiao",
""
],
[
"Guo",
"Heng",
""
],
[
"Chen",
"Feng-Wei",
""
],
[
"Zhang",
"Sheng-Li",
""
]
] | In this paper, we investigate localization of a free massless $q-$form bulk field on thin and thick $AdS_{p+1}$ branes with codimension one. It is found that the zero mode of the $q-$form field with $q>(p+2)/2$ can be localized on the thin negative tension brane, which is different from the flat brane case given in [JH... | 5.632215 | 3.832848 | 5.091792 | 4.316286 | 4.38982 | 4.395274 | 4.308007 | 4.40706 | 4.142387 | 5.124545 | 4.427515 | 4.679177 | 5.05251 | 4.642129 | 4.566757 | 4.689223 | 4.710753 | 4.601219 | 4.705392 | 4.867816 | 4.708801 |
1201.0176 | Joseph Ben Geloun | Joseph Ben Geloun and Dine Ousmane Samary | 3D Tensor Field Theory: Renormalization and One-loop $\beta$-functions | 42 pages, 14 figures; improved version, some statements corrected,
more comments | null | null | pi-qg-252; ICMPA-MPA/2011/018 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove that the rank 3 analogue of the tensor model defined in
[arXiv:1111.4997 [hep-th]] is renormalizable at all orders of perturbation. The
proof is given in the momentum space. The one-loop $\gamma$- and
$\beta$-functions of the model are also determined. We find that the model with
a unique coupling constant f... | [
{
"created": "Fri, 30 Dec 2011 20:09:46 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Sep 2012 00:32:41 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Geloun",
"Joseph Ben",
""
],
[
"Samary",
"Dine Ousmane",
""
]
] | We prove that the rank 3 analogue of the tensor model defined in [arXiv:1111.4997 [hep-th]] is renormalizable at all orders of perturbation. The proof is given in the momentum space. The one-loop $\gamma$- and $\beta$-functions of the model are also determined. We find that the model with a unique coupling constant for... | 6.917367 | 6.367405 | 7.186131 | 6.845708 | 7.994757 | 7.994913 | 7.327034 | 6.641407 | 6.812275 | 8.583707 | 6.315494 | 6.612018 | 6.879152 | 6.542913 | 6.574791 | 6.239548 | 6.684752 | 6.189635 | 6.741848 | 6.901993 | 6.447919 |
hep-th/9307068 | null | Cardoso de Melo, M.C. Nemes and Saulo C.S. Silva | Axial Currents in Electrodynamics P.C.R | 9 pages IFUSP/P-1057 | null | null | null | hep-th | null | In the present work we argue that the usual assumption that magnetic currents
possess the vector structure characteristic of electric currents may be the
source of several difficulties in the theory of magnetic monopoles. We propose
an {\it axial} magnetic current instead and show that such difficulties are
solved. C... | [
{
"created": "Fri, 9 Jul 1993 14:41:48 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"de Melo",
"Cardoso",
""
],
[
"Nemes",
"M. C.",
""
],
[
"Silva",
"Saulo C. S.",
""
]
] | In the present work we argue that the usual assumption that magnetic currents possess the vector structure characteristic of electric currents may be the source of several difficulties in the theory of magnetic monopoles. We propose an {\it axial} magnetic current instead and show that such difficulties are solved. Cha... | 16.533001 | 15.844219 | 15.965541 | 16.493881 | 16.543264 | 15.663308 | 16.258579 | 17.005125 | 13.758859 | 15.609628 | 16.796528 | 16.812286 | 15.060666 | 15.160939 | 15.33549 | 16.022659 | 14.935777 | 15.930476 | 16.061937 | 14.862144 | 15.637389 |
2310.15966 | Tancredi Schettini Gherardini | R. Alawadhi, D. Angella, A. Leonardo and T. Schettini Gherardini | Constructing and Machine Learning Calabi-Yau Five-folds | 40 pages, 8 tables, 2 figures; v2: published in Fortschritte der
Physik - Progress of Physics, minor changes in the introduction, conclusion
and acknowledgements, references added | Fortschr. Phys. 2023, 2300262 | 10.1002/prop.202300262 | null | hep-th cs.LG math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct all possible complete intersection Calabi-Yau five-folds in a
product of four or less complex projective spaces, with up to four constraints.
We obtain $27068$ spaces, which are not related by permutations of rows and
columns of the configuration matrix, and determine the Euler number for all of
them. Ex... | [
{
"created": "Tue, 24 Oct 2023 16:07:08 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Jan 2024 19:00:00 GMT",
"version": "v2"
}
] | 2024-01-11 | [
[
"Alawadhi",
"R.",
""
],
[
"Angella",
"D.",
""
],
[
"Leonardo",
"A.",
""
],
[
"Gherardini",
"T. Schettini",
""
]
] | We construct all possible complete intersection Calabi-Yau five-folds in a product of four or less complex projective spaces, with up to four constraints. We obtain $27068$ spaces, which are not related by permutations of rows and columns of the configuration matrix, and determine the Euler number for all of them. Excl... | 11.817969 | 13.326012 | 14.390966 | 12.536762 | 14.637568 | 15.940302 | 14.743103 | 14.165386 | 13.576651 | 15.808612 | 12.926383 | 12.829258 | 12.412162 | 12.299839 | 12.643515 | 12.411662 | 11.945243 | 12.353482 | 11.691508 | 12.238372 | 11.595494 |
2210.07180 | Behnam Pourhassan | Behnam Pourhassan, \.Izzet Sakall{\i} | Non-perturbative correction to the Horava-Lifshitz black hole
thermodynamics | 23 pages, 15 figures | Chinese Journal of Physics 79 (2022) 322-338 | 10.1016/j.cjph.2022.09.006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we consider non-perturbative quantum correction which appears
as exponential term in the black hole entropy. We study consequence
thermodynamics of the Ho\v{r}ava-Lifshitz black hole at quantum scales. We
consider two cases of Kehagius-Sfetsos and Lu-Mei-Pop solutions and investigate
black hole stabili... | [
{
"created": "Mon, 26 Sep 2022 20:20:58 GMT",
"version": "v1"
}
] | 2022-10-14 | [
[
"Pourhassan",
"Behnam",
""
],
[
"Sakallı",
"İzzet",
""
]
] | In this paper, we consider non-perturbative quantum correction which appears as exponential term in the black hole entropy. We study consequence thermodynamics of the Ho\v{r}ava-Lifshitz black hole at quantum scales. We consider two cases of Kehagius-Sfetsos and Lu-Mei-Pop solutions and investigate black hole stability... | 6.889115 | 7.258035 | 6.538827 | 6.682812 | 7.176417 | 7.719055 | 7.19267 | 6.067879 | 7.353796 | 7.106394 | 7.018899 | 6.623944 | 6.50632 | 6.431376 | 6.476462 | 6.779409 | 6.595039 | 6.618032 | 6.563473 | 6.588315 | 6.722637 |
hep-th/0609150 | Niayesh Afshordi | Niayesh Afshordi (ITC, Harvard), Daniel J.H. Chung, Ghazal Geshnizjani
(UW-Madison) | Cuscuton: A Causal Field Theory with an Infinite Speed of Sound | 11 pages, 1 figure, added discussion of "coupled cuscuton", matches
the published version in PRD | Phys.Rev.D75:083513,2007 | 10.1103/PhysRevD.75.083513 | null | hep-th astro-ph gr-qc hep-ph | null | We introduce a model of scalar field dark energy, Cuscuton, which can be
realized as the incompressible (or infinite speed of sound) limit of a scalar
field theory with a non-canonical kinetic term (or k-essence). Even though
perturbations of Cuscuton propagate superluminally, we show that they have a
locally degener... | [
{
"created": "Thu, 21 Sep 2006 21:18:54 GMT",
"version": "v1"
},
{
"created": "Sat, 28 Apr 2007 01:08:21 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Afshordi",
"Niayesh",
"",
"ITC, Harvard"
],
[
"Chung",
"Daniel J. H.",
"",
"UW-Madison"
],
[
"Geshnizjani",
"Ghazal",
"",
"UW-Madison"
]
] | We introduce a model of scalar field dark energy, Cuscuton, which can be realized as the incompressible (or infinite speed of sound) limit of a scalar field theory with a non-canonical kinetic term (or k-essence). Even though perturbations of Cuscuton propagate superluminally, we show that they have a locally degenerat... | 8.617132 | 9.444386 | 8.933101 | 8.877639 | 9.799777 | 9.338497 | 9.602202 | 8.896962 | 9.352992 | 10.057929 | 9.141806 | 8.707724 | 8.453912 | 8.444649 | 8.64709 | 8.459945 | 8.756696 | 8.516134 | 8.534483 | 8.801039 | 8.704871 |
hep-th/0307110 | Kleihaus | B. Kleihaus, J. Kunz, Ya. Shnir | Monopole--Antimonopole Chains | 9 pages, 2 figures | Phys.Lett. B570 (2003) 237-243 | 10.1016/j.physletb.2003.07.059 | null | hep-th | null | We present new static axially symmetric solutions of SU(2) Yang-Mills-Higgs
theory, representing chains of monopoles and antimonopoles in static
equilibrium. They correspond to saddlepoints of the energy functional and exist
both in the topologically trivial sector and in the sector with topological
charge one.
| [
{
"created": "Fri, 11 Jul 2003 15:05:42 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Kleihaus",
"B.",
""
],
[
"Kunz",
"J.",
""
],
[
"Shnir",
"Ya.",
""
]
] | We present new static axially symmetric solutions of SU(2) Yang-Mills-Higgs theory, representing chains of monopoles and antimonopoles in static equilibrium. They correspond to saddlepoints of the energy functional and exist both in the topologically trivial sector and in the sector with topological charge one. | 6.989469 | 4.741693 | 6.138505 | 5.178348 | 5.421638 | 5.010586 | 5.449425 | 5.219883 | 4.841705 | 6.586552 | 5.615475 | 5.910218 | 6.206819 | 6.254067 | 5.863115 | 5.578526 | 6.128685 | 5.962013 | 6.209333 | 6.728874 | 6.031798 |
1010.6075 | Hiroaki Tanaka | Tatsuma Nishioka and Hiroaki Tanaka | Lifshitz-like Janus Solutions | 19 pages, 5 figures; v2: minor corrections | JHEP 1102:023,2011 | 10.1007/JHEP02(2011)023 | PUPT-2355, UT-10-19 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct Lifshitz-like Janus solutions in the Einstein-scalar theory with
cosmological constant in arbitrary dimensions. They are holographically dual to
z=2 Lifshitz-like field theories with a defect. The four-dimensional solutions
can be embedded into type IIB supergravity as dilatonic deformations of AdS_5 x
Y... | [
{
"created": "Thu, 28 Oct 2010 20:01:16 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Nov 2010 09:30:01 GMT",
"version": "v2"
}
] | 2011-02-16 | [
[
"Nishioka",
"Tatsuma",
""
],
[
"Tanaka",
"Hiroaki",
""
]
] | We construct Lifshitz-like Janus solutions in the Einstein-scalar theory with cosmological constant in arbitrary dimensions. They are holographically dual to z=2 Lifshitz-like field theories with a defect. The four-dimensional solutions can be embedded into type IIB supergravity as dilatonic deformations of AdS_5 x Y^5... | 6.990297 | 5.356006 | 8.050158 | 5.287654 | 5.431535 | 5.192646 | 5.935981 | 5.700884 | 5.573814 | 8.684916 | 5.13661 | 5.79904 | 6.99858 | 5.75109 | 5.9186 | 5.771945 | 5.865502 | 5.459171 | 5.633807 | 6.928762 | 5.497391 |
0704.3118 | S. Ole Warnaar | S Ole Warnaar | Proof of the Flohr-Grabow-Koehn conjectures for characters of
logarithmic conformal field theory | 13 pages, 1 figure | J.Phys.A40:12243,2007 | 10.1088/1751-8113/40/40/015 | null | hep-th math-ph math.MP math.QA | null | In a recent paper Flohr, Grabow and Koehn conjectured that the characters of
the logarithmic conformal field theory c_{k,1}, of central charge
c=1-6(k-1)^2/k, admit fermionic representations labelled by the Lie algebra
D_k. In this note we provide a simple analytic proof of this conjecture.
| [
{
"created": "Tue, 24 Apr 2007 04:57:30 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Warnaar",
"S Ole",
""
]
] | In a recent paper Flohr, Grabow and Koehn conjectured that the characters of the logarithmic conformal field theory c_{k,1}, of central charge c=1-6(k-1)^2/k, admit fermionic representations labelled by the Lie algebra D_k. In this note we provide a simple analytic proof of this conjecture. | 12.32841 | 9.548771 | 13.448978 | 10.249321 | 8.280554 | 8.692592 | 10.809762 | 8.991374 | 10.225123 | 12.931089 | 9.924461 | 10.236573 | 11.90365 | 10.974889 | 11.202785 | 11.612244 | 11.292479 | 11.518209 | 10.512555 | 11.686974 | 10.666985 |
hep-th/9610238 | Daniel J. Waldram | Andre Lukas, Burt A. Ovrut, Daniel Waldram | String and M-Theory Cosmological Solutions with Ramond Forms | 34 pages, Latex, 3 figures using epsf | Nucl.Phys. B495 (1997) 365-399 | 10.1016/S0550-3213(97)00194-6 | UPR-723T, IASSNS-HEP-96/107, PUPT-1656 | hep-th | null | A general framework for studying a large class of cosmological solutions of
the low-energy limit of type II string theory and of M-theory, with non-trivial
Ramond form fields excited, is presented. The framework is applicable to
spacetimes decomposable into a set of flat or, more generally, maximally
symmetric spatia... | [
{
"created": "Wed, 30 Oct 1996 02:36:47 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Oct 1996 09:03:47 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Dec 1996 17:01:24 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Lukas",
"Andre",
""
],
[
"Ovrut",
"Burt A.",
""
],
[
"Waldram",
"Daniel",
""
]
] | A general framework for studying a large class of cosmological solutions of the low-energy limit of type II string theory and of M-theory, with non-trivial Ramond form fields excited, is presented. The framework is applicable to spacetimes decomposable into a set of flat or, more generally, maximally symmetric spatial ... | 8.817455 | 8.756055 | 8.870055 | 8.714735 | 9.158693 | 8.811872 | 8.950522 | 8.672254 | 8.65248 | 9.713322 | 8.418177 | 8.123855 | 8.813371 | 8.758815 | 8.428628 | 8.261057 | 8.26569 | 8.422871 | 8.509624 | 8.992765 | 8.299761 |
2302.08307 | Ahmed Farag Ali | Ahmed Farag Ali, Emmanuel Moulay, Kimet Jusufi, Hassan Alshal | Unitary symmetries in wormhole geometry and its thermodynamics | 20 pages, revtex4, 1 figure, Published in European Physical Journal C | Eur. Phys. J. C 82, 1170 (2022) | 10.1140/epjc/s10052-022-11095-1 | null | hep-th gr-qc quant-ph | http://creativecommons.org/licenses/by/4.0/ | From a geometric point of view, we show that the unitary symmetries $U(1)$
and $SU(2)$ stem fundamentally from Schwarzschild and Reissner-Nordstr\"om
wormhole geometry through spacetime complexification. Then, we develop quantum
tunneling which makes these wormholes traversable for particles. Finally, this
leads to w... | [
{
"created": "Fri, 30 Dec 2022 19:29:34 GMT",
"version": "v1"
}
] | 2023-02-17 | [
[
"Ali",
"Ahmed Farag",
""
],
[
"Moulay",
"Emmanuel",
""
],
[
"Jusufi",
"Kimet",
""
],
[
"Alshal",
"Hassan",
""
]
] | From a geometric point of view, we show that the unitary symmetries $U(1)$ and $SU(2)$ stem fundamentally from Schwarzschild and Reissner-Nordstr\"om wormhole geometry through spacetime complexification. Then, we develop quantum tunneling which makes these wormholes traversable for particles. Finally, this leads to wor... | 12.141302 | 12.266971 | 10.299032 | 11.062253 | 12.257887 | 11.823112 | 11.710481 | 11.63491 | 12.179004 | 11.548322 | 10.999106 | 11.122334 | 10.553585 | 10.690239 | 10.768786 | 11.15311 | 10.727606 | 10.383607 | 10.922799 | 10.200484 | 11.167268 |
2108.02735 | Taniya Mandal | Taniya Mandal, Arunabha Saha | Large $D$ Black Holes in an environment | 36 pages, 2 tables | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct dynamical black hole solutions to Einstein Equations in presence
of matter in the large $D$ limit. The matter stress tensors that we consider
are weak in the sense that they source asymptotic spacetimes with internal
curvatures of the order of $\mathcal{O}(D^0)$. Apart from this, we work with a
generic s... | [
{
"created": "Thu, 5 Aug 2021 16:55:22 GMT",
"version": "v1"
}
] | 2021-08-06 | [
[
"Mandal",
"Taniya",
""
],
[
"Saha",
"Arunabha",
""
]
] | We construct dynamical black hole solutions to Einstein Equations in presence of matter in the large $D$ limit. The matter stress tensors that we consider are weak in the sense that they source asymptotic spacetimes with internal curvatures of the order of $\mathcal{O}(D^0)$. Apart from this, we work with a generic str... | 9.598214 | 9.047396 | 9.119071 | 8.312351 | 9.215229 | 9.520534 | 9.382464 | 8.758951 | 8.968853 | 9.984996 | 8.727671 | 9.492605 | 9.258513 | 9.112918 | 9.102458 | 9.338203 | 9.427589 | 9.624965 | 9.403617 | 9.628887 | 9.308126 |
hep-th/9802024 | Phillial Oh | Phillial Oh | Integrable Extension of Nonlinear Sigma Model | 11 pages, Latex | J.Phys. A31 (1998) L325-L330 | null | SNUTP/98-005 | hep-th | null | We propose an integrable extension of nonlinear sigma model on the target
space of Hermitian symmetric space (HSS). Starting from a discussion of soliton
solutions of O(3) model and an integrally extended version of it, we construct
general theory defined on arbitrary HSS by using the coadjoint orbit method. It
is ba... | [
{
"created": "Thu, 5 Feb 1998 07:11:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Oh",
"Phillial",
""
]
] | We propose an integrable extension of nonlinear sigma model on the target space of Hermitian symmetric space (HSS). Starting from a discussion of soliton solutions of O(3) model and an integrally extended version of it, we construct general theory defined on arbitrary HSS by using the coadjoint orbit method. It is base... | 14.105829 | 12.603144 | 15.974063 | 12.667068 | 13.083221 | 13.530635 | 14.430898 | 13.076122 | 12.977285 | 15.366465 | 13.31882 | 13.318684 | 13.601192 | 12.992259 | 12.898112 | 13.109178 | 12.643355 | 13.047115 | 13.129928 | 14.349182 | 12.803454 |
1711.04832 | Vasilis Niarchos | Adi Armoni and Vasilis Niarchos | Phases of QCD$_3$ from Non-SUSY Seiberg Duality and Brane Dynamics | 33 pages, 7 figures, 4 tables; v2 minor cosmetic changes and addition
of remarks | Phys. Rev. D 97, 106001 (2018) | 10.1103/PhysRevD.97.106001 | DCPT-17/35 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a non-supersymmetric USp Yang-Mills Chern-Simons gauge theory
coupled to fundamental flavours. The theory is realised in type IIB string
theory via an embedding in a Hanany-Witten brane configuration which includes
an orientifold and anti-branes. We argue that the theory admits a magnetic
Seiberg dual. Us... | [
{
"created": "Mon, 13 Nov 2017 20:17:12 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Nov 2017 21:08:56 GMT",
"version": "v2"
}
] | 2018-05-09 | [
[
"Armoni",
"Adi",
""
],
[
"Niarchos",
"Vasilis",
""
]
] | We consider a non-supersymmetric USp Yang-Mills Chern-Simons gauge theory coupled to fundamental flavours. The theory is realised in type IIB string theory via an embedding in a Hanany-Witten brane configuration which includes an orientifold and anti-branes. We argue that the theory admits a magnetic Seiberg dual. Usin... | 10.691637 | 9.750731 | 12.154301 | 10.06422 | 10.679515 | 9.535689 | 10.302135 | 10.238198 | 10.18708 | 12.171616 | 9.112447 | 9.921603 | 10.940208 | 10.297526 | 10.093646 | 9.70621 | 10.046141 | 9.971265 | 9.904092 | 10.740046 | 9.96865 |
1008.4505 | Eugenio Megias | E. Megias, H.J. Pirner, K.Veschgini | Thermodynamics of AdS/QCD within the 5D dilaton-gravity model | 4 pages, 4 figures. To appear in the proceedings of 15th
International Conference in Quantum Chromodynamics (QCD 10), Montpellier,
France, 28 Jun - 3 Jul 2010 | Nucl.Phys.Proc.Suppl.207-208:333-336,2010 | 10.1016/j.nuclphysbps.2010.10.082 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the pressure, entropy density, trace anomaly and speed of sound
of the gluon plasma using the dilaton potential of Ref. arXiv:0911.0627[hep-ph]
in the dilaton-gravity theory of AdS/QCD. The finite temperature observables
are calculated from the Black Hole solutions of the Einstein equations, and
using th... | [
{
"created": "Thu, 26 Aug 2010 13:23:48 GMT",
"version": "v1"
}
] | 2011-02-03 | [
[
"Megias",
"E.",
""
],
[
"Pirner",
"H. J.",
""
],
[
"Veschgini",
"K.",
""
]
] | We calculate the pressure, entropy density, trace anomaly and speed of sound of the gluon plasma using the dilaton potential of Ref. arXiv:0911.0627[hep-ph] in the dilaton-gravity theory of AdS/QCD. The finite temperature observables are calculated from the Black Hole solutions of the Einstein equations, and using the ... | 9.190257 | 8.535316 | 7.500495 | 7.547176 | 10.825724 | 10.293662 | 9.618369 | 8.395448 | 7.280869 | 9.970566 | 8.772209 | 8.586903 | 7.884494 | 8.099635 | 8.840487 | 9.424463 | 9.003231 | 8.896619 | 8.17475 | 8.490072 | 8.486603 |
0906.5492 | Franziska Synatschke | Holger Gies, Franziska Synatschke and Andreas Wipf | Supersymmetry breaking as a quantum phase transition | 5 pages, 2 figures, discussion of results extended, version to appear
as a Rapid Communication in Phys. Rev. D | null | 10.1103/PhysRevD.80.101701 | null | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore supersymmetry breaking in the light of a rich fixed-point
structure of two-dimensional supersymmetric Wess-Zumino models with one
supercharge using the functional renormalization group (RG). We relate the
dynamical breaking of supersymmetry to an RG relevant control parameter of the
superpotential which is... | [
{
"created": "Tue, 30 Jun 2009 12:00:08 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Nov 2009 08:35:44 GMT",
"version": "v2"
}
] | 2013-05-29 | [
[
"Gies",
"Holger",
""
],
[
"Synatschke",
"Franziska",
""
],
[
"Wipf",
"Andreas",
""
]
] | We explore supersymmetry breaking in the light of a rich fixed-point structure of two-dimensional supersymmetric Wess-Zumino models with one supercharge using the functional renormalization group (RG). We relate the dynamical breaking of supersymmetry to an RG relevant control parameter of the superpotential which is a... | 8.499939 | 8.525264 | 9.505195 | 8.258656 | 8.504477 | 8.476013 | 8.202784 | 8.02238 | 7.929492 | 9.316784 | 8.588424 | 8.44712 | 8.995881 | 8.701493 | 8.575887 | 8.570752 | 8.437847 | 8.423134 | 8.304971 | 8.968368 | 8.279609 |
2101.08640 | Jean Alexandre | Jean Alexandre and Janos Polonyi | Tunnelling and dynamical violation of the Null Energy Condition | 7 pages, 1 figure | Phys. Rev. D 103, 105020 (2021) | 10.1103/PhysRevD.103.105020 | KCL-PH-TH/2021-01 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Null Energy Condition is considered the most fundamental of the energy
conditions, on which several key results, such as the singularity theorems, are
based. The Casimir effect is one of the rare equilibrium mechanisms by which it
is breached without invoking modified gravity or non-minimal couplings to
exotic ma... | [
{
"created": "Thu, 21 Jan 2021 14:36:34 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Apr 2021 15:41:56 GMT",
"version": "v2"
}
] | 2021-05-26 | [
[
"Alexandre",
"Jean",
""
],
[
"Polonyi",
"Janos",
""
]
] | The Null Energy Condition is considered the most fundamental of the energy conditions, on which several key results, such as the singularity theorems, are based. The Casimir effect is one of the rare equilibrium mechanisms by which it is breached without invoking modified gravity or non-minimal couplings to exotic matt... | 10.359026 | 11.771759 | 10.862916 | 10.15621 | 10.643729 | 10.25299 | 10.736915 | 10.661109 | 10.306384 | 10.598872 | 10.545079 | 10.202928 | 9.927521 | 9.963135 | 10.246657 | 10.217973 | 10.584793 | 9.943702 | 9.968148 | 10.139377 | 10.425013 |
2205.14402 | Vladimir Dzhunushaliev | Vladimir Dzhunushaliev and Vladimir Folomeev | Quasiparticles in nonperturbative vacuum | 7 pages, 3 figures | null | null | null | hep-th hep-ph | http://creativecommons.org/publicdomain/zero/1.0/ | The model of nonperturbative vacuum in SU(2) Yang-Mills theory coupled to a
nonlinear spinor field is suggested. By analogy with Abelian magnetic monopole
dominance in quantum chromodynamics, it is assumed that the dominant
contribution to such vacuum is coming from quasiparticles described by
dipolelike solutions ex... | [
{
"created": "Sat, 28 May 2022 11:28:26 GMT",
"version": "v1"
}
] | 2022-05-31 | [
[
"Dzhunushaliev",
"Vladimir",
""
],
[
"Folomeev",
"Vladimir",
""
]
] | The model of nonperturbative vacuum in SU(2) Yang-Mills theory coupled to a nonlinear spinor field is suggested. By analogy with Abelian magnetic monopole dominance in quantum chromodynamics, it is assumed that the dominant contribution to such vacuum is coming from quasiparticles described by dipolelike solutions exis... | 7.550817 | 8.045405 | 7.631799 | 7.615764 | 7.569765 | 8.119933 | 7.287554 | 7.337658 | 7.502934 | 8.253184 | 7.117311 | 7.492188 | 7.380085 | 7.221399 | 7.291414 | 7.207307 | 7.26456 | 7.293609 | 7.415601 | 7.461698 | 7.222767 |
hep-th/0105034 | Savas Dimopoulos | Savas Dimopoulos | Soft Supersymmetry Breaking and the Supersymmetric Standard Model | Invited talk presented at the "Thirty Years of Supersymmetry"
Symposium, University of Minnesota, October 13-15, 2000 | Nucl.Phys.Proc.Suppl. 101 (2001) 183-194 | 10.1016/S0920-5632(01)01504-3 | null | hep-th hep-ph | null | We recall how the idea of Softly Broken Supersymmetry led to the construction
of the Supersymmetric Standard Model in 1981. Its first prediction, the
supersymmetric unification of gauge couplings, was conclusively verified by the
LEP and SLC experiments 10 years later. Its other predictions include: the
existence of ... | [
{
"created": "Thu, 3 May 2001 12:06:18 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Dimopoulos",
"Savas",
""
]
] | We recall how the idea of Softly Broken Supersymmetry led to the construction of the Supersymmetric Standard Model in 1981. Its first prediction, the supersymmetric unification of gauge couplings, was conclusively verified by the LEP and SLC experiments 10 years later. Its other predictions include: the existence of su... | 5.986433 | 6.38117 | 5.638156 | 5.279603 | 6.328303 | 6.412408 | 6.22196 | 6.195621 | 5.473776 | 5.806821 | 6.045381 | 5.685025 | 5.264384 | 5.421832 | 5.627159 | 5.622435 | 5.44159 | 5.573325 | 5.371924 | 5.259368 | 5.630844 |
hep-th/0003148 | Shin'ichi Nojiri | Shin'ichi Nojiri, Octavio Obregon, Sergei D. Odintsov, and Sachiko
Ogushi | Dilatonic Brane-World Black Holes, Gravity Localization and Newton
Constant | LaTeX file, 25 pages | Phys.Rev.D62:064017,2000 | 10.1103/PhysRevD.62.064017 | OCH-PP-150, NDA-FP-72 | hep-th | null | The family of brane-world solutions of d+1-dimensional dilatonic gravity is
presented. It includes flat brane with small cosmological constant and (anti)
de Sitter brane, dilatonic brane-world black holes (Schwarzschild-(anti-) de
Sitter, Kerr, etc). Gravitational and dilatonic perturbations around such
branes are fo... | [
{
"created": "Fri, 17 Mar 2000 06:39:48 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Nojiri",
"Shin'ichi",
""
],
[
"Obregon",
"Octavio",
""
],
[
"Odintsov",
"Sergei D.",
""
],
[
"Ogushi",
"Sachiko",
""
]
] | The family of brane-world solutions of d+1-dimensional dilatonic gravity is presented. It includes flat brane with small cosmological constant and (anti) de Sitter brane, dilatonic brane-world black holes (Schwarzschild-(anti-) de Sitter, Kerr, etc). Gravitational and dilatonic perturbations around such branes are foun... | 12.573715 | 11.243311 | 11.627434 | 11.137589 | 10.981652 | 11.643209 | 11.809092 | 10.491811 | 11.185961 | 13.976966 | 11.018713 | 11.650148 | 12.232905 | 11.791779 | 11.652354 | 12.016455 | 11.650851 | 11.601349 | 11.800656 | 12.243076 | 11.533153 |
1708.04934 | Diego Julio Cirilo-Lombardo | Diego Julio Cirilo-Lombardo | Non-Riemannian geometry, Born-Infeld models and trace free gravitational
equations | Accepted in JHEAp. Full analysis of recent research (with many
appendices from previous works to be self contained) and new results. 41
pages plus a figure. New references and the figure at the final of the text.
arXiv admin note: text overlap with arXiv:1409.8014 by other authors | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Non-Riemannian generalization of the standard Born-Infeld (BI) Lagrangian is
introduced and analized from a theory of gravitation with dynamical torsion
field. The field equations derived from the proposed action lead to a trace
free gravitational equation (non-riemannian analog to the trace free equation
(TFE) from[... | [
{
"created": "Tue, 15 Aug 2017 07:18:25 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Aug 2017 11:03:29 GMT",
"version": "v2"
}
] | 2017-08-21 | [
[
"Cirilo-Lombardo",
"Diego Julio",
""
]
] | Non-Riemannian generalization of the standard Born-Infeld (BI) Lagrangian is introduced and analized from a theory of gravitation with dynamical torsion field. The field equations derived from the proposed action lead to a trace free gravitational equation (non-riemannian analog to the trace free equation (TFE) from[1]... | 17.077431 | 18.397589 | 17.193298 | 17.056494 | 18.455318 | 18.983358 | 18.789274 | 18.108511 | 17.506069 | 18.440321 | 17.477474 | 16.745663 | 17.055937 | 16.571501 | 17.05773 | 16.426119 | 16.491991 | 16.192839 | 16.968128 | 16.631109 | 16.322357 |
1601.00450 | Peter Mati | P. Mati | Critical scaling in the large-$N$ $O(N)$ model in higher dimensions and
its possible connection to quantum gravity | the section about quantum gravity is improved; Appendix added; new
references added; matches PRD version | Phys. Rev. D 94, 065025 (2016) | 10.1103/PhysRevD.94.065025 | null | hep-th cond-mat.stat-mech hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The critical scaling of the large-$N$ $O(N)$ model in higher dimensions using
the exact renormalization group equations has been studied, motivated by the
recently found non-trivial fixed point in $4<d<6$ dimensions with metastable
critical potential. Particular attention is paid to the case of $d=5$ where the
scalin... | [
{
"created": "Mon, 4 Jan 2016 11:02:39 GMT",
"version": "v1"
},
{
"created": "Sun, 31 Jan 2016 20:33:08 GMT",
"version": "v2"
},
{
"created": "Tue, 27 Sep 2016 08:25:00 GMT",
"version": "v3"
}
] | 2016-09-28 | [
[
"Mati",
"P.",
""
]
] | The critical scaling of the large-$N$ $O(N)$ model in higher dimensions using the exact renormalization group equations has been studied, motivated by the recently found non-trivial fixed point in $4<d<6$ dimensions with metastable critical potential. Particular attention is paid to the case of $d=5$ where the scaling ... | 9.244131 | 8.43557 | 8.784762 | 8.041338 | 8.751977 | 9.181876 | 8.455883 | 8.46773 | 8.664086 | 8.954572 | 8.354455 | 8.166142 | 8.719918 | 8.219939 | 8.137432 | 8.145375 | 8.080696 | 8.157739 | 7.862291 | 8.653438 | 7.988096 |
hep-th/0408107 | Jacobus Verbaarschot | K. Splittorff and J.J.M. Verbaarschot | QCD Dirac Spectra and the Toda Lattice | 15 pages and 2 figures; Invited talk at Continous Advances in QCD
2004, Minneapolis, May 2004 | null | 10.1142/9789812702326_0002 | SUNY-NTG-04/05 | hep-th | null | We discuss the spectrum of the QCD Dirac operator both at zero and at nonzero
baryon chemical potential. We show that, in the ergodic domain of QCD, the
Dirac spectrum can be obtained from the replica limit of a Toda lattice
equation. At zero chemical potential this method explains the factorization of
known results ... | [
{
"created": "Thu, 12 Aug 2004 21:16:11 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Splittorff",
"K.",
""
],
[
"Verbaarschot",
"J. J. M.",
""
]
] | We discuss the spectrum of the QCD Dirac operator both at zero and at nonzero baryon chemical potential. We show that, in the ergodic domain of QCD, the Dirac spectrum can be obtained from the replica limit of a Toda lattice equation. At zero chemical potential this method explains the factorization of known results in... | 8.765709 | 6.674479 | 7.850814 | 6.712787 | 7.366956 | 7.812143 | 7.63606 | 6.723132 | 7.079824 | 8.725798 | 7.735809 | 7.718804 | 8.285393 | 7.790822 | 7.784219 | 7.672576 | 7.450767 | 7.836975 | 7.73467 | 8.570525 | 8.238153 |
1304.1466 | Korkut Bardakci | Korkut Bardakci | Scalar Field Theories On The World Sheet: Cutoff Independent Treatment | 27 pages, 4 figures, typos corrected and minor revisions made | null | 10.1007/JHEP06(2013)066 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Following earlier work on the same topic, we consider once more scalar field
theories on the world sheet parametrized by the light cone coordinates. For
most of the way, we use the same approach as in the previous work, but there is
an important new development. To avoid the light cone singularity at p^{+}=0,
one wor... | [
{
"created": "Thu, 4 Apr 2013 18:59:26 GMT",
"version": "v1"
},
{
"created": "Fri, 31 May 2013 23:01:16 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"Bardakci",
"Korkut",
""
]
] | Following earlier work on the same topic, we consider once more scalar field theories on the world sheet parametrized by the light cone coordinates. For most of the way, we use the same approach as in the previous work, but there is an important new development. To avoid the light cone singularity at p^{+}=0, one world... | 9.983777 | 10.01193 | 10.44663 | 9.252405 | 9.893805 | 9.720325 | 9.610151 | 9.392292 | 9.341536 | 11.250607 | 9.440419 | 9.636367 | 9.738074 | 9.665133 | 9.442862 | 9.47142 | 9.515194 | 9.525016 | 9.410196 | 10.048943 | 9.415754 |
hep-th/9711078 | Washington Taylor | Daniel Kabat (IAS) and Washington Taylor (Princeton) | Spherical membranes in Matrix theory | 21 pages LaTeX. V2: references added; V3: reference added, minor
corrections | Adv.Theor.Math.Phys.2:181-206,1998 | null | IASSNS-HEP-97/121, PUPT-1734 | hep-th | null | We consider membranes of spherical topology in uncompactified Matrix theory.
In general for large membranes Matrix theory reproduces the classical membrane
dynamics up to 1/N corrections; for certain simple membrane configurations, the
equations of motion agree exactly at finite N. We derive a general formula for
the... | [
{
"created": "Tue, 11 Nov 1997 20:22:50 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Nov 1997 18:11:08 GMT",
"version": "v2"
},
{
"created": "Sat, 31 Jan 1998 05:49:47 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Kabat",
"Daniel",
"",
"IAS"
],
[
"Taylor",
"Washington",
"",
"Princeton"
]
] | We consider membranes of spherical topology in uncompactified Matrix theory. In general for large membranes Matrix theory reproduces the classical membrane dynamics up to 1/N corrections; for certain simple membrane configurations, the equations of motion agree exactly at finite N. We derive a general formula for the o... | 12.253537 | 11.927962 | 12.75738 | 10.926031 | 12.760379 | 12.366934 | 11.150073 | 12.184519 | 11.056413 | 12.865732 | 11.660144 | 11.733608 | 12.426487 | 11.736174 | 11.683115 | 11.691731 | 11.833764 | 11.440193 | 11.691856 | 11.875564 | 11.521665 |
hep-th/0307221 | Leonardo Rastelli | Davide Gaiotto, Nissan Itzhaki and Leonardo Rastelli | On the BCFT Description of Holes in the c=1 Matrix Model | LaTex, 7 pages | Phys.Lett. B575 (2003) 111-114 | 10.1016/j.physletb.2003.09.046 | PUPT-2091 | hep-th | null | We propose a Boundary Conformal Field Theory description of hole states in
the c=1 matrix model.
| [
{
"created": "Tue, 22 Jul 2003 17:06:43 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Gaiotto",
"Davide",
""
],
[
"Itzhaki",
"Nissan",
""
],
[
"Rastelli",
"Leonardo",
""
]
] | We propose a Boundary Conformal Field Theory description of hole states in the c=1 matrix model. | 19.374897 | 9.448255 | 21.462364 | 10.706005 | 11.534534 | 11.380591 | 9.582251 | 10.268765 | 10.290306 | 19.506998 | 10.473916 | 11.30348 | 14.538651 | 10.930882 | 11.578126 | 11.320673 | 11.274382 | 11.022321 | 10.845783 | 14.672604 | 11.23798 |
1208.3204 | Amir Esmaeil Mosaffa | Amir Esmaeil Mosaffa | Symmetric Orbifolds and Entanglement Entropy for Primary Excitations in
Two Dimensional CFT | 5 pages | null | null | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the techniques in symmetric orbifolding to calculate the Entanglement
Entropy of a single interval in a two dimensional conformal field theory on a
circle which is excited to a pure highest weight state. This is achieved by
calculating the Reney Entropy which is found in terms of a 2n-point function of
primary... | [
{
"created": "Wed, 15 Aug 2012 20:06:53 GMT",
"version": "v1"
}
] | 2012-08-17 | [
[
"Mosaffa",
"Amir Esmaeil",
""
]
] | We use the techniques in symmetric orbifolding to calculate the Entanglement Entropy of a single interval in a two dimensional conformal field theory on a circle which is excited to a pure highest weight state. This is achieved by calculating the Reney Entropy which is found in terms of a 2n-point function of primary o... | 15.744776 | 14.442649 | 17.689991 | 12.776917 | 12.764079 | 14.006297 | 13.834119 | 11.727388 | 13.234318 | 17.939796 | 12.106719 | 15.160863 | 14.965115 | 14.232059 | 14.396029 | 13.502351 | 13.708774 | 14.790498 | 14.589786 | 14.613104 | 13.886443 |
1505.05174 | Filipe Moura | Filipe Moura | On the temperature dependence of the absorption cross section for black
holes in string theory | 10 pages. arXiv admin note: substantial text overlap with
arXiv:1406.2012 | Int.J.Mod.Phys.D24(2015)09,1542011 | 10.1142/S0218271815420110 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the low frequency absorption cross section of spherically symmetric
nonextremal d-dimensional black holes. In the presence of alpha' corrections,
this quantity must have an explicit dependence on the Hawking temperature of
the form 1/T_H. This property of the low frequency absorption cross section is
shared ... | [
{
"created": "Tue, 19 May 2015 20:24:36 GMT",
"version": "v1"
}
] | 2015-05-21 | [
[
"Moura",
"Filipe",
""
]
] | We study the low frequency absorption cross section of spherically symmetric nonextremal d-dimensional black holes. In the presence of alpha' corrections, this quantity must have an explicit dependence on the Hawking temperature of the form 1/T_H. This property of the low frequency absorption cross section is shared by... | 10.801211 | 9.768469 | 9.823529 | 9.061821 | 10.489552 | 8.80035 | 9.911519 | 9.25709 | 9.121123 | 10.945986 | 9.518354 | 9.501513 | 9.839331 | 9.380132 | 10.28773 | 10.05213 | 9.251271 | 9.291289 | 9.476502 | 10.162009 | 9.539362 |
2405.02623 | Alessandra D'Alise | Michele Arzano, Alessandra D'Alise, Domenico Frattulillo | Entanglement entropy and horizon temperature in conformal quantum
mechanics | 21 pages, 0 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The generators of radial conformal symmetries in Minkowski space-time can be
put in correspondence with generators of time evolution in conformal quantum
mechanics. Within this correspondence we show that in conformal quantum
mechanics the state corresponding to the inertial vacuum for a conformally
invariant field i... | [
{
"created": "Sat, 4 May 2024 09:46:17 GMT",
"version": "v1"
}
] | 2024-05-07 | [
[
"Arzano",
"Michele",
""
],
[
"D'Alise",
"Alessandra",
""
],
[
"Frattulillo",
"Domenico",
""
]
] | The generators of radial conformal symmetries in Minkowski space-time can be put in correspondence with generators of time evolution in conformal quantum mechanics. Within this correspondence we show that in conformal quantum mechanics the state corresponding to the inertial vacuum for a conformally invariant field in ... | 10.791769 | 9.792025 | 10.853588 | 10.215793 | 9.418729 | 9.31927 | 10.127444 | 9.157788 | 10.006824 | 12.760897 | 10.475567 | 10.724033 | 10.985327 | 10.669238 | 10.642143 | 10.544926 | 10.83091 | 10.133994 | 10.704581 | 11.266082 | 10.23895 |
hep-th/9303073 | Francesco Toppan | E. Ivanov and F. Toppan | N=2 Superconformal Affine Liouville Theory | 12 pages, latex, preprint ENSLAPP-L-422/93 and JINR E2-93-72 | Phys.Lett. B309 (1993) 289-296 | 10.1016/0370-2693(93)90936-C | null | hep-th | null | We present a new supersymmetric integrable model: the $N=2$ superconformal
affine Liouville theory. It interpolates between the $N=2$ super Liouville and
$N=2$ super sine-Gordon theories and possesses a Lax representation on the
complex affine Kac-Moody superalgebra ${\hat {sl(2| 2)^{(1)}}}$. We show that
the higher ... | [
{
"created": "Thu, 11 Mar 1993 21:01:26 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ivanov",
"E.",
""
],
[
"Toppan",
"F.",
""
]
] | We present a new supersymmetric integrable model: the $N=2$ superconformal affine Liouville theory. It interpolates between the $N=2$ super Liouville and $N=2$ super sine-Gordon theories and possesses a Lax representation on the complex affine Kac-Moody superalgebra ${\hat {sl(2| 2)^{(1)}}}$. We show that the higher sp... | 5.419055 | 5.082135 | 6.58096 | 5.043706 | 4.896661 | 5.471684 | 5.514709 | 5.122137 | 4.94354 | 7.027399 | 4.905427 | 5.035235 | 5.645376 | 4.989844 | 5.106049 | 4.987984 | 4.87432 | 5.094917 | 5.091815 | 5.520551 | 4.89718 |
hep-th/9411089 | Sardanashvily Gennadi | G.Sardanashvily (Moscow State University) | Five Lectures on the Jet Methods in Field Theory | total 113 pp, LaTeX file | null | null | TP\94\223 | hep-th | null | The fibre bundle formulation of gauge theory is generally accepted. The jet
manifold machinery completes this formulation and provides the adequate
mathematical description of dynamics of fields represented by sections of fibre
bundles. Theory of differential operators, Lagrangian and Hamiltonian
formalisms on bundle... | [
{
"created": "Sun, 13 Nov 1994 00:43:16 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Sardanashvily",
"G.",
"",
"Moscow State University"
]
] | The fibre bundle formulation of gauge theory is generally accepted. The jet manifold machinery completes this formulation and provides the adequate mathematical description of dynamics of fields represented by sections of fibre bundles. Theory of differential operators, Lagrangian and Hamiltonian formalisms on bundles ... | 13.042253 | 12.420945 | 13.354567 | 11.420286 | 11.438928 | 12.615777 | 12.382202 | 11.911227 | 13.186664 | 14.807894 | 12.028456 | 12.479409 | 13.03896 | 12.476444 | 12.377288 | 12.874453 | 12.742694 | 12.40025 | 12.543447 | 13.11796 | 12.249506 |
2405.17169 | Parinya Karndumri | Parinya Karndumri | Janus and RG-flow interfaces from matter-coupled F(4) gauged
supergravity | 20 pages, 2 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study supersymmetric Janus solutions from matter-coupled $F(4)$ gauged
supergravity coupled to three vector multiplets and $SO(4)\sim SO(3)\times
SO(3)$ gauge group. There are two supersymmetric $AdS_6$ vacua preserving all
supersymmetries with $SO(3)\times SO(3)$ and $SO(3)_{\textrm{diag}}$ symmetries
dual to $N=... | [
{
"created": "Mon, 27 May 2024 13:47:52 GMT",
"version": "v1"
}
] | 2024-05-28 | [
[
"Karndumri",
"Parinya",
""
]
] | We study supersymmetric Janus solutions from matter-coupled $F(4)$ gauged supergravity coupled to three vector multiplets and $SO(4)\sim SO(3)\times SO(3)$ gauge group. There are two supersymmetric $AdS_6$ vacua preserving all supersymmetries with $SO(3)\times SO(3)$ and $SO(3)_{\textrm{diag}}$ symmetries dual to $N=2$... | 3.804599 | 3.235785 | 4.333825 | 3.33181 | 3.230014 | 3.247631 | 3.250237 | 3.256821 | 3.215762 | 4.567775 | 3.328493 | 3.4602 | 3.989659 | 3.579085 | 3.554225 | 3.551131 | 3.557922 | 3.651852 | 3.481014 | 3.94529 | 3.536802 |
1401.4336 | Yasuho Yamashita | Yasuho Yamashita, Takahiro Tanaka | Mapping de Rham-Gabadadze-Tolley bigravity into braneworld setup | 16 pages, 1 figure | null | 10.1088/1475-7516/2014/06/004 | YITP-14-5 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss whether or not bigravity theory can be embedded into the
braneworld setup. As a candidate, we consider Dvali-Gabadadze-Porrati two-brane
model with the Goldberger-Wise radion stabilization. We will show that we can
construct a ghost free model whose low energy spectrum is composed of a
massless graviton an... | [
{
"created": "Fri, 17 Jan 2014 13:28:39 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2014 06:17:27 GMT",
"version": "v2"
}
] | 2015-06-18 | [
[
"Yamashita",
"Yasuho",
""
],
[
"Tanaka",
"Takahiro",
""
]
] | We discuss whether or not bigravity theory can be embedded into the braneworld setup. As a candidate, we consider Dvali-Gabadadze-Porrati two-brane model with the Goldberger-Wise radion stabilization. We will show that we can construct a ghost free model whose low energy spectrum is composed of a massless graviton and ... | 7.971671 | 7.863931 | 7.608604 | 6.463094 | 6.816473 | 7.418443 | 7.240409 | 6.67643 | 6.428371 | 7.607895 | 7.100217 | 7.193515 | 7.308572 | 6.984629 | 7.245688 | 7.07916 | 7.029877 | 7.301886 | 6.980501 | 7.175294 | 7.074281 |
1510.07974 | Hajar Ebrahim | M. Ali-Akbari, H. Ebrahim, S. Heshmatian | Thermal Quench at Finite t'Hooft Coupling | 6 pages, 9 figures | null | null | IPM/P-2015/049 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using holography we have studied thermal electric field quench for infinite
and finite t'Hooft coupling constant. The set-up we consider here is D7-brane
embedded in ($\alpha'$ corrected) AdS-black hole background. It is well-known
that due to a time-dependent electric field on the probe brane, a
time-dependent curre... | [
{
"created": "Tue, 27 Oct 2015 16:34:32 GMT",
"version": "v1"
}
] | 2015-10-28 | [
[
"Ali-Akbari",
"M.",
""
],
[
"Ebrahim",
"H.",
""
],
[
"Heshmatian",
"S.",
""
]
] | Using holography we have studied thermal electric field quench for infinite and finite t'Hooft coupling constant. The set-up we consider here is D7-brane embedded in ($\alpha'$ corrected) AdS-black hole background. It is well-known that due to a time-dependent electric field on the probe brane, a time-dependent current... | 8.756157 | 7.494472 | 8.709368 | 7.874385 | 7.528725 | 7.208251 | 7.737103 | 7.606614 | 7.327795 | 9.012133 | 7.594394 | 7.626195 | 8.101851 | 7.930737 | 7.826451 | 7.783676 | 7.483459 | 7.698767 | 7.805316 | 8.305177 | 7.617135 |
1209.0334 | Robert de Mello Koch | Robert de Mello Koch, Sanjaye Ramgoolam and Congkao Wen | On the refined counting of graphs on surfaces | 57 pages, 12 figures; v2: Typos corrected; references added | null | 10.1016/j.nuclphysb.2013.01.023 | QMUL-PH-12-13; WITS-CTP-104 | hep-th math.GR math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Ribbon graphs embedded on a Riemann surface provide a useful way to describe
the double line Feynman diagrams of large N computations and a variety of other
QFT correlator and scattering amplitude calculations, e.g in MHV rules for
scattering amplitudes, as well as in ordinary QED. Their counting is a special
case of... | [
{
"created": "Mon, 3 Sep 2012 12:59:44 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Sep 2012 15:19:11 GMT",
"version": "v2"
},
{
"created": "Fri, 22 Mar 2013 16:47:34 GMT",
"version": "v3"
}
] | 2015-06-11 | [
[
"Koch",
"Robert de Mello",
""
],
[
"Ramgoolam",
"Sanjaye",
""
],
[
"Wen",
"Congkao",
""
]
] | Ribbon graphs embedded on a Riemann surface provide a useful way to describe the double line Feynman diagrams of large N computations and a variety of other QFT correlator and scattering amplitude calculations, e.g in MHV rules for scattering amplitudes, as well as in ordinary QED. Their counting is a special case of t... | 16.129389 | 14.832211 | 17.145824 | 15.304987 | 15.708124 | 14.399832 | 15.741757 | 14.423846 | 15.366457 | 20.464994 | 14.642926 | 14.847686 | 14.609983 | 13.987226 | 14.798464 | 14.939893 | 14.271145 | 14.821735 | 13.949711 | 14.712674 | 14.201069 |
1712.09914 | Sergey Solodukhin N. | Clement Berthiere, Debajyoti Sarkar and Sergey N. Solodukhin | The quantum fate of black hole horizons | 17 pages, no figures; title slightly changed, more remarks, new
footnotes and references, version to appear in PLB | null | 10.1016/j.physletb.2018.09.027 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The presence of a horizon is the principal marker for black holes as they
appear in the classical theory of gravity. In General Relativity (GR), horizons
have several defining properties. First, there exists a static spherically
symmetric solution to vacuum Einstein equations which possesses a horizon
defined as a nu... | [
{
"created": "Thu, 28 Dec 2017 16:16:29 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Jan 2018 18:22:35 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Jan 2018 16:36:24 GMT",
"version": "v3"
},
{
"created": "Fri, 14 Sep 2018 07:39:54 GMT",
"version": "v4"
}
] | 2018-09-19 | [
[
"Berthiere",
"Clement",
""
],
[
"Sarkar",
"Debajyoti",
""
],
[
"Solodukhin",
"Sergey N.",
""
]
] | The presence of a horizon is the principal marker for black holes as they appear in the classical theory of gravity. In General Relativity (GR), horizons have several defining properties. First, there exists a static spherically symmetric solution to vacuum Einstein equations which possesses a horizon defined as a null... | 7.36658 | 7.543532 | 7.302828 | 6.886875 | 7.846893 | 7.639866 | 7.56959 | 7.332167 | 7.398475 | 8.055497 | 7.628869 | 7.116437 | 7.120182 | 7.039568 | 7.17066 | 7.212399 | 7.234142 | 7.023095 | 7.202072 | 6.89336 | 7.115457 |
1502.06770 | James B. Hartle | James Hartle and Thomas Hertog | Quantum Transitions Between Classical Histories: Bouncing Cosmologies | 37 pages, 5 figures, minor corrections, results not changed | Phys. Rev. D 92, 063509 (2015) | 10.1103/PhysRevD.92.063509 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a quantum theory of gravity spacetime behaves classically when quantum
probabilities are high for histories of geometry and field that are correlated
in time by the Einstein equation. Probabilities follow from the quantum state.
This quantum perspective on classicality has important implications: (a)
Classical his... | [
{
"created": "Tue, 24 Feb 2015 11:32:07 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jul 2015 17:17:00 GMT",
"version": "v2"
},
{
"created": "Fri, 28 Aug 2015 04:02:01 GMT",
"version": "v3"
}
] | 2015-09-16 | [
[
"Hartle",
"James",
""
],
[
"Hertog",
"Thomas",
""
]
] | In a quantum theory of gravity spacetime behaves classically when quantum probabilities are high for histories of geometry and field that are correlated in time by the Einstein equation. Probabilities follow from the quantum state. This quantum perspective on classicality has important implications: (a) Classical histo... | 12.032348 | 12.165285 | 13.014458 | 11.999225 | 12.522521 | 13.687554 | 12.80341 | 12.106719 | 12.029706 | 14.622729 | 11.274207 | 11.609721 | 11.396024 | 11.51955 | 11.234482 | 11.366482 | 11.195163 | 11.772184 | 11.441843 | 11.704828 | 11.250094 |
2002.05221 | David Kubiznak | Finnian Gray, Ian Holst, David Kubiznak, Gloria Odak, Dalila M. Pirvu,
Tales Rick Perche | Conformally Coupled Scalar in Rotating Black Hole Spacetimes | 8 pages, no figures v2: upgraded published version | Phys. Rev. D 101, 084031 (2020) | 10.1103/PhysRevD.101.084031 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate separability of conformally coupled scalar field equation in
general (off-shell) Kerr-NUT-AdS spacetimes in all dimensions. The separability
is intrinsically characterized by the existence of a complete set of mutually
commuting conformal wave operators that can be constructed from a hidden
symmetry of... | [
{
"created": "Wed, 12 Feb 2020 20:29:01 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Apr 2020 23:05:39 GMT",
"version": "v2"
}
] | 2020-05-05 | [
[
"Gray",
"Finnian",
""
],
[
"Holst",
"Ian",
""
],
[
"Kubiznak",
"David",
""
],
[
"Odak",
"Gloria",
""
],
[
"Pirvu",
"Dalila M.",
""
],
[
"Perche",
"Tales Rick",
""
]
] | We demonstrate separability of conformally coupled scalar field equation in general (off-shell) Kerr-NUT-AdS spacetimes in all dimensions. The separability is intrinsically characterized by the existence of a complete set of mutually commuting conformal wave operators that can be constructed from a hidden symmetry of t... | 9.017048 | 7.912613 | 7.61974 | 6.924769 | 7.643198 | 7.680434 | 7.676987 | 7.240181 | 7.661582 | 8.614256 | 7.704493 | 7.824337 | 8.300689 | 7.698191 | 7.78604 | 7.720196 | 7.736707 | 7.723244 | 7.72371 | 8.372075 | 7.92299 |
0906.1819 | Dionysios Anninos | Dionysios Anninos | Sailing from Warped AdS_3 to Warped dS_3 in Topologically Massive
Gravity | 1+24 pages, 1 figure | JHEP 1002:046,2010 | 10.1007/JHEP02(2010)046 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Three-dimensional warped anti-de Sitter space in topologically massive
gravity with a negative cosmological constant has been proposed to be
holographically dual to a two-dimensional conformal field theory. We extend
this proposal to both positive and vanishing values of the cosmological
constant where stretched warp... | [
{
"created": "Wed, 10 Jun 2009 18:39:24 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jan 2010 01:54:53 GMT",
"version": "v2"
}
] | 2010-02-23 | [
[
"Anninos",
"Dionysios",
""
]
] | Three-dimensional warped anti-de Sitter space in topologically massive gravity with a negative cosmological constant has been proposed to be holographically dual to a two-dimensional conformal field theory. We extend this proposal to both positive and vanishing values of the cosmological constant where stretched warped... | 6.776546 | 6.742267 | 6.899244 | 6.352593 | 6.76585 | 6.2756 | 6.637029 | 6.281398 | 6.029617 | 7.026762 | 6.214684 | 6.477045 | 6.653697 | 6.371469 | 6.4118 | 6.32323 | 6.461002 | 6.389017 | 6.414665 | 6.717304 | 6.32406 |
1404.0619 | Stefano Negro | Stefano Negro | On sinh-Gordon Thermodynamic Bethe Ansatz and fermionic basis | 27 pages, 13 figures. Correction of some typos and minor reformatting | IJMPA, vol. 29 (2014) 1450111 | 10.1142/S0217751X14501115 | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/3.0/ | We review the construction of the fermionic basis for sinh-Gordon model and
investigate numerically the ultra-violet limit of the one-point functions. We
then compare the predictions obtained from this formalism against previously
established results.
| [
{
"created": "Wed, 2 Apr 2014 17:14:38 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Apr 2014 12:22:09 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Jun 2014 09:27:03 GMT",
"version": "v3"
}
] | 2014-08-05 | [
[
"Negro",
"Stefano",
""
]
] | We review the construction of the fermionic basis for sinh-Gordon model and investigate numerically the ultra-violet limit of the one-point functions. We then compare the predictions obtained from this formalism against previously established results. | 19.647533 | 13.73436 | 21.475079 | 14.111574 | 12.710544 | 13.931756 | 13.525784 | 13.184992 | 13.863971 | 21.11694 | 12.729488 | 14.408872 | 19.221783 | 15.535676 | 15.563602 | 15.30609 | 15.237374 | 15.801637 | 15.582762 | 17.591581 | 15.224302 |
2203.13017 | Yvonne Geyer | Yvonne Geyer, Lionel Mason | The SAGEX Review on Scattering Amplitudes, Chapter 6: Ambitwistor
Strings and Amplitudes from the Worldsheet | 46 pages + appendices, see also the overview article arXiv:2203.13011 | null | null | SAGEX-22-07 | hep-th gr-qc hep-ph math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | Starting with Witten's twistor string, chiral string theories have emerged
that describe field theory amplitudes without the towers of massive states of
conventional strings. These models are known as ambitwistor strings due to
their target space; the space of complexified null geodesics, also called
ambitwistor spac... | [
{
"created": "Thu, 24 Mar 2022 12:00:21 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Apr 2022 15:47:57 GMT",
"version": "v2"
}
] | 2022-04-08 | [
[
"Geyer",
"Yvonne",
""
],
[
"Mason",
"Lionel",
""
]
] | Starting with Witten's twistor string, chiral string theories have emerged that describe field theory amplitudes without the towers of massive states of conventional strings. These models are known as ambitwistor strings due to their target space; the space of complexified null geodesics, also called ambitwistor space.... | 9.786048 | 9.480419 | 11.929704 | 9.492572 | 10.097651 | 9.813448 | 9.416578 | 9.656809 | 9.299854 | 12.23035 | 9.288335 | 9.799537 | 10.138093 | 9.577979 | 9.719708 | 9.529812 | 9.674086 | 9.932852 | 9.78407 | 10.334114 | 9.661756 |
hep-th/9305074 | Konstadinos Sfetsos | Konstadinos Sfetsos | Effective Action and Exact Geometry in Chiral Gauged WZW Models | 19 pages, harvmac, USC-93/HEP-S1, (A typo in eq. 4.5 is corrected and
a note is added ) | null | null | null | hep-th | null | Following recent work on the effective quantum action of gauged WZW models,
we suggest such an action for {\it chiral} gauged WZW models which in many
respects differ from the usual gauged WZW models. Using the effective action we
compute the conformally exact expressions for the metric, the antisymmetric
tensor, and... | [
{
"created": "Mon, 17 May 1993 16:56:21 GMT",
"version": "v1"
},
{
"created": "Sat, 22 May 1993 21:04:18 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Aug 1993 11:01:35 GMT",
"version": "v3"
}
] | 2008-02-03 | [
[
"Sfetsos",
"Konstadinos",
""
]
] | Following recent work on the effective quantum action of gauged WZW models, we suggest such an action for {\it chiral} gauged WZW models which in many respects differ from the usual gauged WZW models. Using the effective action we compute the conformally exact expressions for the metric, the antisymmetric tensor, and t... | 6.919674 | 6.097334 | 7.023495 | 6.152451 | 6.460746 | 6.254172 | 6.413742 | 6.049936 | 5.947248 | 7.515459 | 6.056073 | 6.337986 | 6.884439 | 6.337286 | 6.49743 | 6.364079 | 6.324951 | 6.247155 | 6.232735 | 6.848025 | 6.265697 |
1902.08023 | Olaf Lechtenfeld | Sergey Fedoruk, Evgeny Ivanov, Olaf Lechtenfeld | Supersymmetric hyperbolic Calogero-Sutherland models by gauging | 1+18 pages; v2: one reference added, minor corrections, matches
published version | null | 10.1016/j.nuclphysb.2019.114633 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Novel $\mathcal{N}{=}\,2$ and $\mathcal{N}{=}\,4$ supersymmetric extensions
of the Calogero-Sutherland hyperbolic systems are obtained by gauging the ${\rm
U}(n)$ isometry of matrix superfield models. The bosonic core of the
$\mathcal{N}{=}\,2$ models is the standard $A_{n-1}$ Calogero-Sutherland
hyperbolic system, w... | [
{
"created": "Thu, 21 Feb 2019 13:13:58 GMT",
"version": "v1"
},
{
"created": "Fri, 10 May 2019 14:50:24 GMT",
"version": "v2"
}
] | 2019-06-26 | [
[
"Fedoruk",
"Sergey",
""
],
[
"Ivanov",
"Evgeny",
""
],
[
"Lechtenfeld",
"Olaf",
""
]
] | Novel $\mathcal{N}{=}\,2$ and $\mathcal{N}{=}\,4$ supersymmetric extensions of the Calogero-Sutherland hyperbolic systems are obtained by gauging the ${\rm U}(n)$ isometry of matrix superfield models. The bosonic core of the $\mathcal{N}{=}\,2$ models is the standard $A_{n-1}$ Calogero-Sutherland hyperbolic system, whe... | 4.504425 | 4.085618 | 5.058886 | 4.1034 | 4.009585 | 4.024946 | 3.749946 | 3.848425 | 4.119123 | 5.370753 | 4.15546 | 4.317742 | 4.726601 | 4.261699 | 4.317245 | 4.165471 | 4.203953 | 4.1461 | 4.186239 | 4.679961 | 4.124405 |
1904.05201 | Sergei Kuzenko | Sergei M. Kuzenko | Superconformal vector multiplet self-couplings and generalised
Fayet-Iliopoulos terms | 10 pages; V2: references and comments added | null | 10.1016/j.physletb.2019.05.047 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As an extension of the recent construction of generalised Fayet-Iliopoulos
terms in ${\cal N}=1$ supergravity given in [1], we present self-interactions
for a vector multiplet coupled to conformal supergravity. They are used to
construct new models for spontaneously broken local supersymmetry.
| [
{
"created": "Wed, 10 Apr 2019 14:12:45 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Apr 2019 14:00:14 GMT",
"version": "v2"
}
] | 2019-06-05 | [
[
"Kuzenko",
"Sergei M.",
""
]
] | As an extension of the recent construction of generalised Fayet-Iliopoulos terms in ${\cal N}=1$ supergravity given in [1], we present self-interactions for a vector multiplet coupled to conformal supergravity. They are used to construct new models for spontaneously broken local supersymmetry. | 10.170099 | 5.577567 | 7.553101 | 6.68035 | 6.085786 | 5.935019 | 6.342415 | 5.851818 | 6.228718 | 8.366772 | 6.857291 | 6.743569 | 7.616568 | 7.093088 | 6.686471 | 6.481305 | 6.486885 | 6.891687 | 6.895489 | 7.437847 | 6.886197 |
hep-th/0303167 | Philippe Brax | Philippe Brax, Adam Falkowski and Zygmunt Lalak | Cosmological constant and kinetic supersymmetry breakdown on a moving
brane | 21 pages | Nucl.Phys. B667 (2003) 149-169 | 10.1016/S0550-3213(03)00548-0 | null | hep-th | null | We consider cosmological solutions in 5d locally supersymmetric theories
including boundary actions, with either opposite tension branes for identical
brane chiralities or equal tension branes for flipped brane chiralities. We
analyse the occurrence of supersymmetry breakdown in both situations. We find
that supersym... | [
{
"created": "Wed, 19 Mar 2003 16:40:51 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Brax",
"Philippe",
""
],
[
"Falkowski",
"Adam",
""
],
[
"Lalak",
"Zygmunt",
""
]
] | We consider cosmological solutions in 5d locally supersymmetric theories including boundary actions, with either opposite tension branes for identical brane chiralities or equal tension branes for flipped brane chiralities. We analyse the occurrence of supersymmetry breakdown in both situations. We find that supersymme... | 9.063277 | 9.309764 | 8.907972 | 8.532597 | 8.897414 | 8.432869 | 8.773729 | 8.317125 | 8.433706 | 9.558078 | 8.473381 | 9.053994 | 8.840119 | 8.913375 | 8.777916 | 8.856131 | 8.962055 | 8.70286 | 8.939754 | 8.952142 | 9.024125 |
1701.06710 | Machiko Hatsuda | Machiko Hatsuda, Kiyoshi Kamimura and Warren Siegel | Manifestly T-dual formulation of AdS space | 35 pages, v2: Explanation of the relation to other approaches, a
pedagogical review and references are added, to appear in JHEP | null | 10.1007/JHEP05(2017)069 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a manifestly T-dual formulation of curved spaces such as an AdS
space. For group manifolds related by the orthogonal vielbein fields the three
form H=dB in the doubled space is universal at least locally. We construct an
affine nondegenerate doubled bosonic AdS algebra to define the AdS space with
the Ramo... | [
{
"created": "Tue, 24 Jan 2017 02:23:35 GMT",
"version": "v1"
},
{
"created": "Wed, 3 May 2017 08:04:38 GMT",
"version": "v2"
}
] | 2017-06-07 | [
[
"Hatsuda",
"Machiko",
""
],
[
"Kamimura",
"Kiyoshi",
""
],
[
"Siegel",
"Warren",
""
]
] | We present a manifestly T-dual formulation of curved spaces such as an AdS space. For group manifolds related by the orthogonal vielbein fields the three form H=dB in the doubled space is universal at least locally. We construct an affine nondegenerate doubled bosonic AdS algebra to define the AdS space with the Ramond... | 15.20726 | 15.84651 | 16.474852 | 13.760715 | 15.951414 | 14.600351 | 15.475329 | 15.189098 | 13.61146 | 17.214323 | 14.846302 | 14.694564 | 15.204931 | 13.955472 | 14.320065 | 14.581054 | 14.122987 | 14.361049 | 14.282826 | 16.065889 | 13.671394 |
hep-th/0405036 | Alexios P. Polychronakos | A. Alekseev, A.P. Polychronakos, M. Smedback | Remarks on the black hole entropy and Hawking spectrum in Loop Quantum
Gravity | null | Phys.Rev. D71 (2005) 067501 | 10.1103/PhysRevD.71.067501 | CCNY-HEP-04/3, UUITP-13/04 | hep-th gr-qc | null | In this note we reply to the criticism by Corichi concerning our proposal for
an equidistant area spectrum in loop quantum gravity. We further comment on the
emission properties of black holes and on the statistics of links.
| [
{
"created": "Tue, 4 May 2004 18:03:07 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Alekseev",
"A.",
""
],
[
"Polychronakos",
"A. P.",
""
],
[
"Smedback",
"M.",
""
]
] | In this note we reply to the criticism by Corichi concerning our proposal for an equidistant area spectrum in loop quantum gravity. We further comment on the emission properties of black holes and on the statistics of links. | 27.858953 | 17.635918 | 15.591413 | 14.297118 | 19.297512 | 19.96673 | 17.114576 | 14.303976 | 17.44009 | 16.646376 | 17.798237 | 16.741676 | 16.485275 | 16.108034 | 16.382862 | 17.341831 | 17.2929 | 15.725879 | 16.823647 | 16.724384 | 16.842516 |
1811.01125 | Paolo Benincasa | Nima Arkani-Hamed and Paolo Benincasa | On the Emergence of Lorentz Invariance and Unitarity from the Scattering
Facet of Cosmological Polytopes | 9 pages, figures in tikz | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The concepts of Lorentz invariance of local (flat space) physics, and
unitarity of time evolution and the S-matrix, are famously rigid and robust,
admitting no obvious consistent theoretical deformations, and confirmed to
incredible accuracy by experiments. But neither of these notions seem to appear
directly in desc... | [
{
"created": "Fri, 2 Nov 2018 23:35:48 GMT",
"version": "v1"
}
] | 2018-11-06 | [
[
"Arkani-Hamed",
"Nima",
""
],
[
"Benincasa",
"Paolo",
""
]
] | The concepts of Lorentz invariance of local (flat space) physics, and unitarity of time evolution and the S-matrix, are famously rigid and robust, admitting no obvious consistent theoretical deformations, and confirmed to incredible accuracy by experiments. But neither of these notions seem to appear directly in descri... | 11.377037 | 11.71593 | 11.981175 | 10.484484 | 11.774559 | 11.917661 | 11.626223 | 11.342154 | 11.354989 | 13.673028 | 10.676918 | 10.872007 | 11.41605 | 11.111794 | 11.342624 | 10.875292 | 11.181116 | 11.276137 | 11.022184 | 11.967172 | 10.701365 |
hep-th/0107212 | P. S. Howe | P.J. Heslop and P.S. Howe | OPEs and 3-point correlators of protected operators in N=4 SYM | 22 pages | Nucl.Phys. B626 (2002) 265-286 | 10.1016/S0550-3213(02)00023-8 | null | hep-th | null | Two- and three-point correlation functions of arbitrary protected operators
are constructed in N=4 SYM using analytic superspace methods. The OPEs of two
chiral primary multiplets are given. It is shown that the $n$-point functions
of protected operators for $n\leq4$ are invariant under $U(1)_Y$ and it is
argued that... | [
{
"created": "Tue, 24 Jul 2001 17:40:27 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Heslop",
"P. J.",
""
],
[
"Howe",
"P. S.",
""
]
] | Two- and three-point correlation functions of arbitrary protected operators are constructed in N=4 SYM using analytic superspace methods. The OPEs of two chiral primary multiplets are given. It is shown that the $n$-point functions of protected operators for $n\leq4$ are invariant under $U(1)_Y$ and it is argued that t... | 7.990612 | 6.387335 | 8.453722 | 7.127598 | 7.072179 | 7.055356 | 7.440279 | 6.66266 | 6.739633 | 8.44637 | 6.875223 | 7.123601 | 7.57328 | 7.012484 | 7.104285 | 7.006791 | 7.089447 | 6.961645 | 7.100649 | 7.568452 | 7.039824 |
1010.0566 | Stuart Dowker | J.S.Dowker | Determinants and conformal anomalies of GJMS operators on spheres | 20 pages. Last major revision. Section on holographic aspects added | J.Phys.A44:115402,2011 | 10.1088/1751-8113/44/11/115402 | null | hep-th gr-qc math-ph math.DG math.MP math.SP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The conformal anomalies and functional determinants of the Branson--GJMS
operators, P_{2k}, on the d-dimensional sphere are evaluated in explicit terms
for any d and k such that k < d/2+1 (if d is even). The determinants are given
in terms of multiple gamma functions and a rational multiplicative anomaly,
which vanis... | [
{
"created": "Mon, 4 Oct 2010 12:35:07 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Oct 2010 15:36:27 GMT",
"version": "v2"
},
{
"created": "Mon, 18 Oct 2010 18:02:53 GMT",
"version": "v3"
},
{
"created": "Wed, 20 Oct 2010 18:44:03 GMT",
"version": "v4"
},
{
"cr... | 2011-03-02 | [
[
"Dowker",
"J. S.",
""
]
] | The conformal anomalies and functional determinants of the Branson--GJMS operators, P_{2k}, on the d-dimensional sphere are evaluated in explicit terms for any d and k such that k < d/2+1 (if d is even). The determinants are given in terms of multiple gamma functions and a rational multiplicative anomaly, which vanishe... | 14.148143 | 14.271199 | 16.456585 | 13.975606 | 16.676672 | 14.878154 | 14.8235 | 13.937384 | 14.012095 | 16.528732 | 13.966209 | 13.478858 | 14.196733 | 13.236811 | 13.326978 | 13.094655 | 13.229784 | 13.378896 | 12.828547 | 14.076959 | 13.46995 |
hep-th/0411138 | Mikhail Krivoruchenko | M. I. Krivoruchenko, Amand Faessler, A. A. Raduta, C. Fuchs | Gauge invariant counterparts and quantization of systems under holonomic
constraints | 5 pages REVTeX, new references added | Phys.Lett. B608 (2005) 164-170 | 10.1016/j.physletb.2004.12.058 | null | hep-th quant-ph | null | Systems under holonomic constraints are classified within the generalized
Hamiltonian framework as second-class constraints systems. We show that each
system of point particles with holonomic constraints has a hidden gauge
symmetry which allows to quantize it in the original phase space as a
first-class constraints s... | [
{
"created": "Mon, 15 Nov 2004 10:14:51 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Mar 2005 13:26:16 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Krivoruchenko",
"M. I.",
""
],
[
"Faessler",
"Amand",
""
],
[
"Raduta",
"A. A.",
""
],
[
"Fuchs",
"C.",
""
]
] | Systems under holonomic constraints are classified within the generalized Hamiltonian framework as second-class constraints systems. We show that each system of point particles with holonomic constraints has a hidden gauge symmetry which allows to quantize it in the original phase space as a first-class constraints sys... | 9.510574 | 7.37642 | 9.97651 | 8.164544 | 8.731046 | 8.687337 | 7.74885 | 7.749562 | 7.569807 | 9.960527 | 8.423411 | 7.962371 | 8.955698 | 8.560534 | 8.06832 | 8.404013 | 8.227159 | 8.009552 | 8.681002 | 8.423326 | 8.806744 |
hep-th/0001057 | Kenji Suzuki | Kenji Suzuki | D0-D4 system and QCD_{3+1} | 10 pages, REVTeX; typos corrected | Phys.Rev. D63 (2001) 084011 | 10.1103/PhysRevD.63.084011 | null | hep-th | null | We consider a $(3+1)$-dimensional QCD model using a dual supergravity
description with a non-extremal $D0$-$D4$ brane background. We calculate the
spectrum of glueball masses and Wilson loops in the background. The mass
spectrum is shown to coincide with one in non-extremal $D4$-brane systems, and
an area low of spat... | [
{
"created": "Tue, 11 Jan 2000 06:11:22 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Jan 2001 06:06:42 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Suzuki",
"Kenji",
""
]
] | We consider a $(3+1)$-dimensional QCD model using a dual supergravity description with a non-extremal $D0$-$D4$ brane background. We calculate the spectrum of glueball masses and Wilson loops in the background. The mass spectrum is shown to coincide with one in non-extremal $D4$-brane systems, and an area low of spatia... | 10.652147 | 9.948854 | 10.186024 | 9.274055 | 11.588406 | 10.159487 | 9.913067 | 9.562623 | 9.732154 | 11.93956 | 9.198358 | 10.300097 | 10.188611 | 10.136957 | 10.665627 | 10.23748 | 10.265339 | 10.204013 | 10.392065 | 10.348775 | 10.309199 |
hep-th/0603127 | Qing-Guo Huang | Qing-Guo Huang, Miao Li and Wei Song | Weak gravity conjecture in the asymptotical dS and AdS background | 4 pages; version for publication in JHEP (title changed) | JHEP0610:059,2006 | 10.1088/1126-6708/2006/10/059 | null | hep-th | null | The cosmological observations provide a strong evidence that there is a
positive cosmological constant in our universe and thus the spacetime is
asymptotical de Sitter space. The conjecture of gravity as the weakest force in
the asymptotical dS space leads to a lower bound on the U(1) gauge coupling
$g$, or equivalen... | [
{
"created": "Thu, 16 Mar 2006 13:41:53 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Oct 2006 22:38:01 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Huang",
"Qing-Guo",
""
],
[
"Li",
"Miao",
""
],
[
"Song",
"Wei",
""
]
] | The cosmological observations provide a strong evidence that there is a positive cosmological constant in our universe and thus the spacetime is asymptotical de Sitter space. The conjecture of gravity as the weakest force in the asymptotical dS space leads to a lower bound on the U(1) gauge coupling $g$, or equivalentl... | 7.398798 | 7.245729 | 7.304286 | 6.974302 | 7.274039 | 7.426183 | 7.746183 | 7.06194 | 7.058923 | 7.970506 | 7.082169 | 6.946744 | 7.46518 | 7.12768 | 6.79105 | 6.967271 | 7.042141 | 7.107378 | 6.942575 | 7.673851 | 7.130069 |
2206.08090 | Wung-Hong Huang | Wung-Hong Huang | Tri-Scalar CFT and Holographic Bi-Fishchain Model | Add several comments and many references | Int. J. Mod. Phys. A 38 (2023) 2350135 | null | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | Bi-scalar CFT from $\gamma$ deformed $\cal N$=4 SYM describes the fishnet
theory which is integrable in the planar limit. The holographic dual of the
planar model is the fishchain model. The derivation of the weak-strong duality
from the first principle was presented in a recent paper (The Holographic
Fishchain arXiv... | [
{
"created": "Thu, 16 Jun 2022 11:12:46 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Aug 2023 08:04:55 GMT",
"version": "v2"
}
] | 2023-11-01 | [
[
"Huang",
"Wung-Hong",
""
]
] | Bi-scalar CFT from $\gamma$ deformed $\cal N$=4 SYM describes the fishnet theory which is integrable in the planar limit. The holographic dual of the planar model is the fishchain model. The derivation of the weak-strong duality from the first principle was presented in a recent paper (The Holographic Fishchain arXiv:1... | 11.776059 | 10.964436 | 13.275191 | 10.567219 | 11.286283 | 12.000216 | 11.442962 | 10.265092 | 10.723557 | 14.174032 | 11.079899 | 10.539561 | 10.935248 | 10.004011 | 10.146083 | 9.950802 | 10.080012 | 10.068926 | 10.280484 | 10.973829 | 10.326138 |
1911.00129 | Mishkat Al Alvi | Mishkat Al Alvi, Arshad Momen | Classicalization in Derivatively Coupled Scalar Field Theories: A
Feasibility Study | 12 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been suggested that a certain class of UV-incomplete quantum field
theories can avoid unitarity violation above the cut-off energy scale by
forming classical configurations at a length scale much larger than the cut-off
length. This phenomenon has been named classicalization and is characterized by
a length sc... | [
{
"created": "Thu, 31 Oct 2019 22:09:08 GMT",
"version": "v1"
}
] | 2019-11-04 | [
[
"Alvi",
"Mishkat Al",
""
],
[
"Momen",
"Arshad",
""
]
] | It has been suggested that a certain class of UV-incomplete quantum field theories can avoid unitarity violation above the cut-off energy scale by forming classical configurations at a length scale much larger than the cut-off length. This phenomenon has been named classicalization and is characterized by a length scal... | 9.532169 | 9.385013 | 9.076715 | 8.839018 | 9.686753 | 9.36515 | 9.739642 | 9.5626 | 8.922475 | 9.367663 | 9.66903 | 9.088449 | 9.024147 | 8.562441 | 8.902397 | 9.022295 | 8.846526 | 8.729243 | 8.744516 | 8.958849 | 8.995302 |
hep-th/0204008 | Gary Gibbons | G. W. Gibbons | Cosmological Evolution of the Rolling Tachyon | 6 pages, no figures, typos corrected and two refs inserted | Phys.Lett.B537:1-4,2002 | 10.1016/S0370-2693(02)01881-6 | DAMTP-2002-38 | hep-th | null | The cosmological effects of the tachyon rolling down to its ground state are
discussed by coupling a simple effective field theory for the tachyon field to
Einstein gravity. As the tachyon rolls down to the minimum of its potential the
universe expands. Depending upon initial conditions, the scale factor may or
may n... | [
{
"created": "Sun, 31 Mar 2002 18:35:36 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Apr 2002 11:03:50 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Gibbons",
"G. W.",
""
]
] | The cosmological effects of the tachyon rolling down to its ground state are discussed by coupling a simple effective field theory for the tachyon field to Einstein gravity. As the tachyon rolls down to the minimum of its potential the universe expands. Depending upon initial conditions, the scale factor may or may not... | 8.088049 | 7.690761 | 8.112985 | 7.319797 | 7.502444 | 8.373774 | 7.6619 | 8.046511 | 7.497313 | 8.962387 | 7.244251 | 7.139828 | 7.796318 | 7.161508 | 7.380455 | 7.288503 | 7.426467 | 7.410626 | 7.316255 | 7.550065 | 7.157778 |
hep-th/0611068 | Dermot O'Reilly | D. O'Reilly | String Corrected Supergravity; A Complete and Consistent Non-Minimal
Solution | 10 pages | null | null | null | hep-th | null | We complete the solution to string corrected (deformed),
D=10, N=1 Supergravity as the non-minimal low energy limit of string theory.
We reaffirm a previously given solution, and we make important corrections to
that solution.
We solve what was an apparently intractable Bianchi identity in superspace,
and we in... | [
{
"created": "Mon, 6 Nov 2006 19:29:19 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Nov 2006 19:17:08 GMT",
"version": "v2"
},
{
"created": "Fri, 10 Nov 2006 16:54:26 GMT",
"version": "v3"
},
{
"created": "Mon, 13 Nov 2006 16:27:37 GMT",
"version": "v4"
},
{
"cre... | 2007-05-23 | [
[
"O'Reilly",
"D.",
""
]
] | We complete the solution to string corrected (deformed), D=10, N=1 Supergravity as the non-minimal low energy limit of string theory. We reaffirm a previously given solution, and we make important corrections to that solution. We solve what was an apparently intractable Bianchi identity in superspace, and we introduce ... | 19.946976 | 15.557296 | 17.863676 | 15.400218 | 15.112858 | 14.465894 | 14.487185 | 14.731926 | 14.602516 | 16.924675 | 15.341599 | 15.54069 | 16.8016 | 15.650353 | 16.014494 | 15.348083 | 15.878693 | 16.355305 | 15.593721 | 16.404121 | 15.740995 |
1603.07367 | Andrew K. Waldron | A. Rod Gover and Andrew Waldron | Renormalized Volume | 31 pages, LaTeX, 5 figures, anomaly formula generalized to any bulk
geometry, improved discussion of hypersurfaces with boundary | Communications in Mathematical Physics, volume 354, issue 3, pages
1205-1244, 2017 | 10.1007/s00220-017-2920-z | null | hep-th gr-qc math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a universal distributional calculus for regulated volumes of
metrics that are singular along hypersurfaces. When the hypersurface is a
conformal infinity we give simple integrated distribution expressions for the
divergences and anomaly of the regulated volume functional valid for any choice
of regulator. ... | [
{
"created": "Wed, 23 Mar 2016 21:17:34 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Oct 2016 00:48:16 GMT",
"version": "v2"
}
] | 2017-10-03 | [
[
"Gover",
"A. Rod",
""
],
[
"Waldron",
"Andrew",
""
]
] | We develop a universal distributional calculus for regulated volumes of metrics that are singular along hypersurfaces. When the hypersurface is a conformal infinity we give simple integrated distribution expressions for the divergences and anomaly of the regulated volume functional valid for any choice of regulator. Fo... | 13.383862 | 16.14596 | 16.934027 | 14.05494 | 13.358987 | 15.117056 | 15.402855 | 14.894129 | 13.180946 | 16.598093 | 14.421678 | 13.689102 | 13.584007 | 13.069038 | 13.621101 | 13.632749 | 13.761454 | 13.593451 | 13.338793 | 13.895762 | 13.074028 |
1203.6398 | Kiyoshi Shiraishi | Nahomi Kan (Yamaguchi Junior College), Koichiro Kobayashi and Kiyoshi
Shiraishi (Yamaguchi University) | Nambu-Jona-Lasinio Model and Deconstructed Dimension | 11 pages, 5 figures | Pioneer Journal of Mathematical Physics and its Applications,
Volume 1, Issue 2 (2012) pp. 53-65 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Nambu-Jona-Lasinio model with the mass matrix which appears in a
deconstruction model is investigated. We consider two models. In Model A, a
mass matrix belonging to a type used in dimensional deconstruction is
introduced. In Model B, the four-fermion interaction has a structure of the
matrix of the type of dimen... | [
{
"created": "Thu, 29 Mar 2012 00:00:07 GMT",
"version": "v1"
}
] | 2013-01-15 | [
[
"Kan",
"Nahomi",
"",
"Yamaguchi Junior College"
],
[
"Kobayashi",
"Koichiro",
"",
"Yamaguchi University"
],
[
"Shiraishi",
"Kiyoshi",
"",
"Yamaguchi University"
]
] | The Nambu-Jona-Lasinio model with the mass matrix which appears in a deconstruction model is investigated. We consider two models. In Model A, a mass matrix belonging to a type used in dimensional deconstruction is introduced. In Model B, the four-fermion interaction has a structure of the matrix of the type of dimensi... | 11.319779 | 10.024781 | 9.348539 | 9.701363 | 11.568565 | 9.966406 | 11.025301 | 10.462322 | 10.171952 | 10.913808 | 9.801975 | 9.88855 | 9.702364 | 9.645874 | 10.081563 | 10.043904 | 10.388356 | 10.581269 | 9.824691 | 10.020882 | 9.936409 |
2112.08336 | David Peinador Veiga | Ricardo Monteiro, Silvia Nagy, Donal O'Connell, David Peinador Veiga
and Matteo Sergola | NS-NS Spacetimes from Amplitudes | 41 pages + appendices, 2 pdf figures. v2: minor changes, published
version | null | 10.1007/JHEP06(2022)021 | QMUL-PH-21-53 | hep-th | http://creativecommons.org/licenses/by/4.0/ | Recent work has shown how on-shell three-point amplitudes in gauge theory and
gravity, representing the coupling to massive particles, correspond in the
classical limit to the curvature spinors of linearised solutions. This
connection, made explicit via the KMOC formalism in split metric signature,
turns the double c... | [
{
"created": "Wed, 15 Dec 2021 18:33:57 GMT",
"version": "v1"
},
{
"created": "Sat, 22 Oct 2022 11:28:15 GMT",
"version": "v2"
}
] | 2022-10-25 | [
[
"Monteiro",
"Ricardo",
""
],
[
"Nagy",
"Silvia",
""
],
[
"O'Connell",
"Donal",
""
],
[
"Veiga",
"David Peinador",
""
],
[
"Sergola",
"Matteo",
""
]
] | Recent work has shown how on-shell three-point amplitudes in gauge theory and gravity, representing the coupling to massive particles, correspond in the classical limit to the curvature spinors of linearised solutions. This connection, made explicit via the KMOC formalism in split metric signature, turns the double cop... | 14.581757 | 15.743173 | 15.304064 | 12.939979 | 13.920915 | 14.420779 | 14.711351 | 13.615422 | 13.562393 | 17.014837 | 13.893188 | 14.058599 | 14.225183 | 13.836477 | 14.047157 | 14.060724 | 13.722573 | 13.944025 | 13.478675 | 14.661039 | 13.697855 |
hep-th/0505045 | Yoshinao Sato | Yoshinao Sato | Dissolving D0-brane into D2-brane with background B-field | 42 pages, 20 figures, JHEP style; references added, clarifications
added in section 3.1; references added | JHEP 0512 (2005) 032 | 10.1088/1126-6708/2005/12/032 | UT-Komaba/05-4 | hep-th | null | D0-branes on a D2-brane with a constant background B-field are unstable due
to the presence of a tachyonic mode and expected to dissolve into the D2-brane
to formulate a constant D0-charge density. In this paper we study such a
dissolution process in terms of a noncommutative gauge theory. Our results show
that the l... | [
{
"created": "Thu, 5 May 2005 12:46:31 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jul 2005 05:48:23 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Sep 2005 07:58:58 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Sato",
"Yoshinao",
""
]
] | D0-branes on a D2-brane with a constant background B-field are unstable due to the presence of a tachyonic mode and expected to dissolve into the D2-brane to formulate a constant D0-charge density. In this paper we study such a dissolution process in terms of a noncommutative gauge theory. Our results show that the loc... | 7.009863 | 6.798706 | 7.667506 | 6.436719 | 6.575101 | 7.18356 | 6.830831 | 6.59437 | 6.496853 | 8.240156 | 6.559121 | 6.542461 | 7.159117 | 6.531604 | 6.415552 | 6.472694 | 6.469847 | 6.461354 | 6.53114 | 6.975364 | 6.571586 |
1011.5570 | Keijo Kajantie | K. Kajantie, M. Vepsalainen | Spatial scalar correlator in strongly coupled hot N=4 Yang-Mills theory | 15 pages, 11 figures, reference added, equation corrected, numerical
constant analytically evaluated | Phys.Rev.D83:066003,2011 | 10.1103/PhysRevD.83.066003 | HIP-2010-32/TH | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use AdS/CFT duality to compute in N=4 Yang-Mills theory the finite
temperature spatial correlator G(r) of the scalar operator F^2, integrated over
imaginary time. The computation is carried out both at zero frequency and
integrating the spectral function over frequencies. The result is compared with
a perturbative... | [
{
"created": "Thu, 25 Nov 2010 09:03:43 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Dec 2010 11:45:47 GMT",
"version": "v2"
}
] | 2011-03-21 | [
[
"Kajantie",
"K.",
""
],
[
"Vepsalainen",
"M.",
""
]
] | We use AdS/CFT duality to compute in N=4 Yang-Mills theory the finite temperature spatial correlator G(r) of the scalar operator F^2, integrated over imaginary time. The computation is carried out both at zero frequency and integrating the spectral function over frequencies. The result is compared with a perturbative c... | 10.217277 | 9.343847 | 10.193574 | 8.467437 | 9.980514 | 9.641277 | 9.872326 | 9.374981 | 9.369421 | 11.5592 | 8.988809 | 8.266082 | 9.00425 | 8.593567 | 8.509033 | 8.821421 | 8.481196 | 8.476167 | 8.520806 | 9.924318 | 8.308402 |
1501.05315 | Matthew Walters | A. Liam Fitzpatrick, Jared Kaplan, and Matthew T. Walters | Virasoro Conformal Blocks and Thermality from Classical Background
Fields | 27+7 pages, 3 figures; typos corrected, citations added | JHEP 11 (2015) 200 | 10.1007/JHEP11(2015)200 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that in 2d CFTs at large central charge, the coupling of the stress
tensor to heavy operators can be re-absorbed by placing the CFT in a
non-trivial background metric. This leads to a more precise computation of the
Virasoro conformal blocks between heavy and light operators, which are shown to
be equivalent ... | [
{
"created": "Wed, 21 Jan 2015 21:00:20 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Feb 2015 19:04:54 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Oct 2015 17:18:53 GMT",
"version": "v3"
}
] | 2015-12-08 | [
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Kaplan",
"Jared",
""
],
[
"Walters",
"Matthew T.",
""
]
] | We show that in 2d CFTs at large central charge, the coupling of the stress tensor to heavy operators can be re-absorbed by placing the CFT in a non-trivial background metric. This leads to a more precise computation of the Virasoro conformal blocks between heavy and light operators, which are shown to be equivalent to... | 6.347187 | 6.195078 | 7.332689 | 6.082036 | 5.845139 | 6.361279 | 6.140667 | 6.049137 | 5.991286 | 7.612815 | 6.137307 | 6.13712 | 6.520505 | 6.118825 | 6.24362 | 6.159507 | 6.148098 | 6.116276 | 6.101654 | 6.448734 | 6.225897 |
2408.03670 | Ashis Saha | Souvik Paul, Anirban Roy Chowdhury, Ashis Saha, Sunandan Gangopadhyay | Information theoretic measures for Lifshitz system | 51 pages LaTex, multiple figures, comments are welcome | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we have studied various mixed state information theoretic
quantities for an excited state of Lifshitz spacetime in $3+1$-dimensions. This
geometry is the gravity dual to a class of $2+1$-dimensional quantum field
theories having Lifshitz symmetry. We have holographically calculated mutual
information, e... | [
{
"created": "Wed, 7 Aug 2024 10:25:30 GMT",
"version": "v1"
}
] | 2024-08-08 | [
[
"Paul",
"Souvik",
""
],
[
"Chowdhury",
"Anirban Roy",
""
],
[
"Saha",
"Ashis",
""
],
[
"Gangopadhyay",
"Sunandan",
""
]
] | In this work, we have studied various mixed state information theoretic quantities for an excited state of Lifshitz spacetime in $3+1$-dimensions. This geometry is the gravity dual to a class of $2+1$-dimensional quantum field theories having Lifshitz symmetry. We have holographically calculated mutual information, ent... | 7.605803 | 7.320929 | 7.970082 | 7.08367 | 7.212455 | 6.745145 | 6.615305 | 6.8933 | 6.793849 | 8.200602 | 6.879798 | 6.872453 | 7.355309 | 6.974667 | 7.017141 | 6.962064 | 6.960939 | 6.811995 | 6.815191 | 7.205276 | 6.829536 |
0804.0412 | Kewang Jin | Antal Jevicki, Kewang Jin | Solitons and AdS String Solutions | 10 pages, 3 figures, contribution to Proceedings of Osaka workshop,
OCU, December 2007 | Int.J.Mod.Phys.A23:2289-2298,2008 | 10.1142/S0217751X0804113X | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this contribution we describe some soliton based techniques for generating
classical AdS string solutions. The methods introduced are useful for further
understanding of rotating AdS configurations with spikes which correspond to
higher twist operators in SYM theory. The main identification (accomplished in
arXiv:... | [
{
"created": "Wed, 2 Apr 2008 19:21:14 GMT",
"version": "v1"
}
] | 2009-09-29 | [
[
"Jevicki",
"Antal",
""
],
[
"Jin",
"Kewang",
""
]
] | In this contribution we describe some soliton based techniques for generating classical AdS string solutions. The methods introduced are useful for further understanding of rotating AdS configurations with spikes which correspond to higher twist operators in SYM theory. The main identification (accomplished in arXiv:07... | 17.29229 | 14.266478 | 17.120159 | 13.831639 | 14.073677 | 14.985267 | 15.201123 | 13.740458 | 15.464467 | 18.966249 | 13.903503 | 14.47212 | 15.994951 | 14.27125 | 15.132804 | 14.968659 | 14.441075 | 15.03975 | 14.597904 | 15.711517 | 14.883096 |
2406.04310 | Ehsan Hatefi | Armin Hatefi, Ehsan Hatefi, Roberto J. Lopez-Sastre | Neural Networks Assisted Metropolis-Hastings for Bayesian Estimation of
Critical Exponent on Elliptic Black Hole Solution in 4D Using Quantum
Perturbation Theory | V2: 3 extra figures for loss functions on Gaussian proposal
distributions are added. Section 4 is modified. 37 pages, 14 figures | null | null | null | hep-th gr-qc math-ph math.MP quant-ph | http://creativecommons.org/licenses/by/4.0/ | It is well-known that the critical gravitational collapse produces continuous
self-similar solutions characterized by the Choptuik critical exponent,
$\gamma$. We examine the solutions in the domains of the linear perturbation
equations, considering the numerical measurement errors. Specifically, we study
quantum per... | [
{
"created": "Thu, 6 Jun 2024 17:55:55 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jun 2024 15:46:22 GMT",
"version": "v2"
}
] | 2024-06-21 | [
[
"Hatefi",
"Armin",
""
],
[
"Hatefi",
"Ehsan",
""
],
[
"Lopez-Sastre",
"Roberto J.",
""
]
] | It is well-known that the critical gravitational collapse produces continuous self-similar solutions characterized by the Choptuik critical exponent, $\gamma$. We examine the solutions in the domains of the linear perturbation equations, considering the numerical measurement errors. Specifically, we study quantum pertu... | 15.850147 | 13.901031 | 13.988645 | 13.390246 | 14.014291 | 13.383675 | 14.281434 | 12.628972 | 14.090754 | 14.276689 | 14.122976 | 14.587828 | 14.220974 | 14.335792 | 14.258336 | 14.864776 | 13.986693 | 13.477126 | 14.083233 | 14.192603 | 14.238649 |
0811.2359 | Enrique Moreno | E. F. Moreno, F. A. Schaposnik | BPS Equations and the Stress Tensor | 13 pages, LaTex | Phys.Lett.B673:72-76,2009 | 10.1016/j.physletb.2009.01.063 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We exploit the relationship between the space components of the
energy-momentum tensor and the supercurrent to discuss the connection between
the BPS equations and the vanishing of the components of the stress tensor in
various supersymmetric theories with solitons.
Using the fact that certain combination of superc... | [
{
"created": "Fri, 14 Nov 2008 15:28:30 GMT",
"version": "v1"
}
] | 2010-05-27 | [
[
"Moreno",
"E. F.",
""
],
[
"Schaposnik",
"F. A.",
""
]
] | We exploit the relationship between the space components of the energy-momentum tensor and the supercurrent to discuss the connection between the BPS equations and the vanishing of the components of the stress tensor in various supersymmetric theories with solitons. Using the fact that certain combination of supercharg... | 8.868827 | 7.987237 | 8.601711 | 7.43127 | 8.178908 | 8.25556 | 7.964399 | 7.631583 | 7.847021 | 8.214087 | 7.385847 | 7.777294 | 7.882731 | 7.393164 | 7.585288 | 7.334992 | 7.890895 | 7.473413 | 7.468454 | 7.921111 | 7.740988 |
hep-th/9502009 | Murat Gunaydin | Murat Gunaydin and Hermann Nicolai | Seven Dimensional Octonionic Yang-Mills Instanton and its Extension to
an Heterotic String Soliton | 7 pages, Latex document. This is the final version that appeared in
Phys. Lett. B that includes an extra paragraph about the physical properties
of the octonionic two-brane. We have also put an addendum regarding some
related references that were brought to our attention recently | Phys.Lett.B351:169-172,1995; Addendum-ibid.B376:329,1996 | 10.1016/0370-2693(95)00375-U | null | hep-th | null | We construct an octonionic instanton solution to the seven dimensional
Yang-Mills theory based on the exceptional gauge group $G_2$ which is the
automorphism group of the division algebra of octonions. This octonionic
instanton has an extension to a solitonic two-brane solution of the low energy
effective theory of t... | [
{
"created": "Wed, 1 Feb 1995 23:13:37 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Feb 1996 19:12:32 GMT",
"version": "v2"
}
] | 2011-02-09 | [
[
"Gunaydin",
"Murat",
""
],
[
"Nicolai",
"Hermann",
""
]
] | We construct an octonionic instanton solution to the seven dimensional Yang-Mills theory based on the exceptional gauge group $G_2$ which is the automorphism group of the division algebra of octonions. This octonionic instanton has an extension to a solitonic two-brane solution of the low energy effective theory of the... | 5.262977 | 4.566978 | 5.259892 | 4.589396 | 4.834293 | 4.8552 | 4.956511 | 4.473835 | 4.823306 | 5.475462 | 4.638343 | 4.623787 | 4.696435 | 4.456304 | 4.724981 | 4.577897 | 4.67837 | 4.428359 | 4.566697 | 4.84726 | 4.627248 |
hep-th/9410002 | null | M. Kibler | Application of Non-Bijective Transformations to Various Potentials | 8 pages, Tex, LYCEN 8766 | null | null | null | hep-th | null | Some results about non-bijective quadratic transformations generalizing the
Kustaanheimo-Stiefel and the Levi-Civita transformations are reviewed in \S 1.
The three remaining sections are devoted to new results: \S 2 deals with the
Lie algebras under constraints associated to some Hurwitz transformations; \S 3
and \S... | [
{
"created": "Mon, 3 Oct 1994 15:14:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kibler",
"M.",
""
]
] | Some results about non-bijective quadratic transformations generalizing the Kustaanheimo-Stiefel and the Levi-Civita transformations are reviewed in \S 1. The three remaining sections are devoted to new results: \S 2 deals with the Lie algebras under constraints associated to some Hurwitz transformations; \S 3 and \S 4... | 8.553932 | 8.855387 | 10.292656 | 8.300592 | 8.128379 | 9.459633 | 8.37725 | 9.623092 | 8.930803 | 9.479243 | 8.072706 | 8.119989 | 8.478803 | 7.879291 | 8.450665 | 8.208299 | 8.089 | 8.040723 | 8.608984 | 8.826045 | 7.915829 |
1805.00284 | Yogesh Dandekar | Sayantani Bhattacharyya, Parthajit Biswas, Yogesh Dandekar | Black holes in presence of cosmological constant: Second order in 1/D | 55 pages, v2: minor corrections | null | 10.1007/JHEP10(2018)171 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have extended the results of arXiv:1704.06076 upto second subleading order
in an expansion around large dimension D. Unlike the previous case, there are
non-trivial metric corrections at this order. Due to our `background-covariant'
formalism, the dependence on Ricci and the Riemann curvature tensor of the
backgro... | [
{
"created": "Tue, 1 May 2018 12:12:54 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Jul 2018 10:40:54 GMT",
"version": "v2"
}
] | 2018-11-14 | [
[
"Bhattacharyya",
"Sayantani",
""
],
[
"Biswas",
"Parthajit",
""
],
[
"Dandekar",
"Yogesh",
""
]
] | We have extended the results of arXiv:1704.06076 upto second subleading order in an expansion around large dimension D. Unlike the previous case, there are non-trivial metric corrections at this order. Due to our `background-covariant' formalism, the dependence on Ricci and the Riemann curvature tensor of the backgroun... | 17.255142 | 14.880303 | 18.299351 | 15.704327 | 16.454985 | 15.403791 | 16.617071 | 15.832567 | 15.56175 | 19.338512 | 15.239355 | 15.610111 | 17.358866 | 16.105844 | 15.166565 | 15.793436 | 16.15642 | 15.796081 | 15.819047 | 16.620974 | 15.758307 |
hep-th/0411040 | Jessie Shelton | Jessie Shelton | Closed Superstring Emission from Rolling Tachyon Backgrounds | 23 pages | JHEP0501:037,2005 | 10.1088/1126-6708/2005/01/037 | MIT-CTP-3556 | hep-th | null | We compute the lowest components of the Type II Ramond-Ramond boundary state
for the tachyon profile $T (X) = \lambda e ^{X ^ 0/\sqrt{2}}$ by direct path
integral evaluation. The calculation is made possible by noting that the
integrals involved in the requisite disk one-point functions reduce to
integrals over the p... | [
{
"created": "Wed, 3 Nov 2004 17:02:06 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Shelton",
"Jessie",
""
]
] | We compute the lowest components of the Type II Ramond-Ramond boundary state for the tachyon profile $T (X) = \lambda e ^{X ^ 0/\sqrt{2}}$ by direct path integral evaluation. The calculation is made possible by noting that the integrals involved in the requisite disk one-point functions reduce to integrals over the pro... | 7.338681 | 7.466704 | 8.388391 | 6.911348 | 7.663468 | 7.327789 | 7.041992 | 7.211608 | 7.064356 | 8.68794 | 6.904005 | 7.085905 | 7.399129 | 7.182786 | 7.366203 | 7.006549 | 7.203996 | 7.142419 | 7.272355 | 7.532447 | 7.207184 |
hep-th/9305137 | Miguel Angel Vazquez Mozo | M.A.R. Osorio and M.A. Vazquez-Mozo | Variations on Kaluza-Klein Cosmology | 22 pages, 7 figures in a uuencoded file (using uufiles), LaTeX,
FTUAM-93/13 (LaTeX errors corrected) | Mod.Phys.Lett.A8:3111-3128,1993 | 10.1142/S0217732393002063 | null | hep-th | null | We investigate the cosmological consequences of having quantum fields living
in a space with compactified dimensions. We will show that the equation of
state is not modified by topological effects and so the dynamics of the
universe remains as it is in the infinite volume limit. On the contrary the
thermal history of... | [
{
"created": "Tue, 25 May 1993 17:20:13 GMT",
"version": "v1"
},
{
"created": "Wed, 26 May 1993 15:24:54 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Osorio",
"M. A. R.",
""
],
[
"Vazquez-Mozo",
"M. A.",
""
]
] | We investigate the cosmological consequences of having quantum fields living in a space with compactified dimensions. We will show that the equation of state is not modified by topological effects and so the dynamics of the universe remains as it is in the infinite volume limit. On the contrary the thermal history of t... | 14.583503 | 12.416321 | 12.833858 | 11.599271 | 12.897799 | 13.466543 | 13.011042 | 12.587253 | 12.495007 | 14.0122 | 12.362927 | 13.694185 | 13.426606 | 13.282815 | 13.803731 | 13.746936 | 13.487342 | 13.572842 | 13.26577 | 13.145313 | 13.033585 |
1505.03571 | Humberto Gomez | Freddy Cachazo, Humberto Gomez | Computation of Contour Integrals on ${\cal M}_{0,n}$ | 36+11 pp | null | 10.1007/JHEP04(2016)108 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Contour integrals of rational functions over ${\cal M}_{0,n}$, the moduli
space of $n$-punctured spheres, have recently appeared at the core of the
tree-level S-matrix of massless particles in arbitrary dimensions. The contour
is determined by the critical points of a certain Morse function on ${\cal
M}_{0,n}$. The i... | [
{
"created": "Wed, 13 May 2015 23:16:52 GMT",
"version": "v1"
}
] | 2016-05-25 | [
[
"Cachazo",
"Freddy",
""
],
[
"Gomez",
"Humberto",
""
]
] | Contour integrals of rational functions over ${\cal M}_{0,n}$, the moduli space of $n$-punctured spheres, have recently appeared at the core of the tree-level S-matrix of massless particles in arbitrary dimensions. The contour is determined by the critical points of a certain Morse function on ${\cal M}_{0,n}$. The int... | 8.118406 | 7.810259 | 9.77831 | 7.672012 | 8.839088 | 8.164532 | 7.727818 | 7.098652 | 7.477916 | 10.113295 | 7.587227 | 7.637456 | 7.595652 | 7.566169 | 7.478602 | 7.483222 | 7.594435 | 7.506745 | 7.651775 | 8.080573 | 7.519071 |
2309.14467 | Gerben Oling | Leo Bidussi, Troels Harmark, Jelle Hartong, Niels A. Obers, Gerben
Oling | Longitudinal Galilean and Carrollian limits of non-relativistic strings | 29+3 pages; v2: minor changes | null | 10.1007/JHEP12(2023)141 | NORDITA-2023-042 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well known that one can take an infinite speed of light limit that
gives rise to non-relativistic strings with a relativistic worldsheet sigma
model but with a non-relativistic target space geometry. In this work we
systematically explore two further limits in which the worldsheet becomes
non-Lorentzian. The fi... | [
{
"created": "Mon, 25 Sep 2023 18:59:41 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Dec 2023 14:59:12 GMT",
"version": "v2"
}
] | 2023-12-29 | [
[
"Bidussi",
"Leo",
""
],
[
"Harmark",
"Troels",
""
],
[
"Hartong",
"Jelle",
""
],
[
"Obers",
"Niels A.",
""
],
[
"Oling",
"Gerben",
""
]
] | It is well known that one can take an infinite speed of light limit that gives rise to non-relativistic strings with a relativistic worldsheet sigma model but with a non-relativistic target space geometry. In this work we systematically explore two further limits in which the worldsheet becomes non-Lorentzian. The firs... | 8.509319 | 6.969408 | 9.066298 | 7.517015 | 7.823138 | 7.744931 | 8.356373 | 7.144029 | 7.392272 | 9.505618 | 7.551136 | 7.953061 | 8.475098 | 7.84665 | 7.749771 | 7.889372 | 7.79503 | 7.741421 | 7.693878 | 8.427463 | 7.816695 |
0809.1137 | Kazuo Ghoroku | Kazuo Ghoroku, Masafumi Ishihara, Akihiro Nakamura and Fumihiko Toyoda | Baryonium in Confining Gauge Theories | 13 pages, 4 figures | JHEP 0904:041,2009 | 10.1088/1126-6708/2009/04/041 | FIT HE - 08-03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show a new class of embedding solutions of D5 brane, which wraps on $S^5$
in the AdS${}_5\times S^5$ space-time and contains fundamental strings as U(1)
flux to form a baryon vertex. The new solution given here is different from the
baryon vertex since it consists of two same side (north or south) poles of
$S^5$ a... | [
{
"created": "Sat, 6 Sep 2008 05:59:08 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Jan 2009 09:48:53 GMT",
"version": "v2"
},
{
"created": "Tue, 24 Feb 2009 08:36:44 GMT",
"version": "v3"
}
] | 2009-04-17 | [
[
"Ghoroku",
"Kazuo",
""
],
[
"Ishihara",
"Masafumi",
""
],
[
"Nakamura",
"Akihiro",
""
],
[
"Toyoda",
"Fumihiko",
""
]
] | We show a new class of embedding solutions of D5 brane, which wraps on $S^5$ in the AdS${}_5\times S^5$ space-time and contains fundamental strings as U(1) flux to form a baryon vertex. The new solution given here is different from the baryon vertex since it consists of two same side (north or south) poles of $S^5$ as ... | 10.313077 | 9.780371 | 10.158155 | 9.187188 | 10.081056 | 9.616044 | 10.0752 | 9.947259 | 8.968225 | 10.784138 | 10.128685 | 9.787443 | 9.678794 | 9.476735 | 9.527209 | 9.494122 | 9.547174 | 9.505494 | 9.72296 | 10.228871 | 9.550329 |
hep-th/0511207 | Hiroshi Suzuki | Hiroto So and Hiroshi Suzuki | Zero-dimensional analogue of the global gauge anomaly | 6 pages, uses PTPTeX.cls, the final version to appear in Prog. Theor.
Phys | Prog.Theor.Phys. 115 (2006) 467-471 | 10.1143/PTP.115.467 | NIIG-DP-05-3, RIKEN-TH-57 | hep-th hep-lat | null | A zero-dimensional analogue of Witten's global gauge anomaly is considered.
For example, a zero-dimensional reduction of the two-dimensional $\SO(2N)$
Yang-Mills theory with a single Majorana-Weyl fermion in the fundamental
representation suffers from this anomaly. Another example is a zero-dimensional
reduction of t... | [
{
"created": "Mon, 21 Nov 2005 11:20:15 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jan 2006 07:23:48 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"So",
"Hiroto",
""
],
[
"Suzuki",
"Hiroshi",
""
]
] | A zero-dimensional analogue of Witten's global gauge anomaly is considered. For example, a zero-dimensional reduction of the two-dimensional $\SO(2N)$ Yang-Mills theory with a single Majorana-Weyl fermion in the fundamental representation suffers from this anomaly. Another example is a zero-dimensional reduction of two... | 8.019462 | 7.946757 | 7.622872 | 7.404295 | 8.936219 | 7.922139 | 7.856124 | 7.442472 | 7.442637 | 9.537944 | 6.979331 | 6.705689 | 7.379018 | 7.033905 | 7.132915 | 6.846518 | 6.700838 | 6.790937 | 6.749699 | 7.700878 | 6.855839 |
1106.2683 | Yaron Oz | Igor Itkin and Yaron Oz | Penrose Inequality for Asymptotically AdS Spaces | 4 pages, Latex, ref. added | null | 10.1016/j.physletb.2012.01.007 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In general relativity, the Penrose inequality relates the mass and the
entropy associated with a gravitational background. If the inequality is
violated by an initial Cauchy data, it suggests a creation of a naked
singularity, thus providing means to consider the cosmic censorship hypothesis.
We propose a general for... | [
{
"created": "Tue, 14 Jun 2011 12:04:50 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Jul 2011 07:21:32 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Itkin",
"Igor",
""
],
[
"Oz",
"Yaron",
""
]
] | In general relativity, the Penrose inequality relates the mass and the entropy associated with a gravitational background. If the inequality is violated by an initial Cauchy data, it suggests a creation of a naked singularity, thus providing means to consider the cosmic censorship hypothesis. We propose a general form ... | 8.674189 | 7.739772 | 7.963588 | 7.503747 | 9.233375 | 9.437898 | 8.512641 | 9.088053 | 8.153314 | 10.659901 | 8.41354 | 7.883099 | 8.17731 | 7.58919 | 8.12728 | 7.722548 | 7.641405 | 7.748076 | 7.750336 | 8.181295 | 7.685272 |
2312.13850 | Torben Skrzypek | Torben Skrzypek, Arkady A. Tseytlin | On AdS/CFT duality in the twisted sector of string theory on $AdS_5
\times S^5/\mathbb{Z}_2$ orbifold background | 29 pages, 3 figures; v2: an issue of residual irregularity of the
$S^1$-fibration over $S^2$ in the resolution of the original orbifold
singularity is pointed out, main conclusions are unchanged | null | null | Imperial-TP-AT-2023-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider type IIB string theory on an $AdS_5 \times S^5/\mathbb{Z}_2$
orbifold background, which should be dual to 4d $\mathcal{N}=2$ superconformal
$SU(N)\times SU(N)$ gauge theory with two bi-fundamental hypermultiplets. The
correlator of two chiral BPS operators from the twisted sector of this quiver
CFT exhibi... | [
{
"created": "Thu, 21 Dec 2023 13:47:37 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Jul 2024 08:42:35 GMT",
"version": "v2"
}
] | 2024-07-12 | [
[
"Skrzypek",
"Torben",
""
],
[
"Tseytlin",
"Arkady A.",
""
]
] | We consider type IIB string theory on an $AdS_5 \times S^5/\mathbb{Z}_2$ orbifold background, which should be dual to 4d $\mathcal{N}=2$ superconformal $SU(N)\times SU(N)$ gauge theory with two bi-fundamental hypermultiplets. The correlator of two chiral BPS operators from the twisted sector of this quiver CFT exhibits... | 5.932608 | 5.810297 | 6.814291 | 5.586513 | 5.586873 | 6.037111 | 5.802078 | 5.649468 | 5.717338 | 7.366815 | 5.605701 | 5.787645 | 6.141935 | 5.672609 | 5.828318 | 5.771505 | 5.756129 | 5.741002 | 5.751258 | 6.207015 | 5.726652 |
1406.1588 | Mar\'ia Montserrat Ju\'arez-Aubry | Eloy Ay\'on-Beato, Mokhtar Hassa\"ine, Mar\'ia Montserrat
Ju\'arez-Aubry | Towards the uniqueness of Lifshitz black holes and solitons in New
Massive Gravity | 10 pages, 5 figures | Phys. Rev. D 90, 044026 (2014) | 10.1103/PhysRevD.90.044026 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove that the z=1 and z=3 Lifshitz black hole solutions of New Massive
Gravity in three dimensions are the only static axisymmetric solutions that can
be cast in a Kerr-Schild form with a seed metric given by the Lifshitz
spacetime. Correspondingly, we study the issue of uniqueness of Lifshitz
solitons when consi... | [
{
"created": "Fri, 6 Jun 2014 05:49:10 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Feb 2015 00:05:23 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Jul 2015 18:19:42 GMT",
"version": "v3"
}
] | 2015-07-16 | [
[
"Ayón-Beato",
"Eloy",
""
],
[
"Hassaïne",
"Mokhtar",
""
],
[
"Juárez-Aubry",
"María Montserrat",
""
]
] | We prove that the z=1 and z=3 Lifshitz black hole solutions of New Massive Gravity in three dimensions are the only static axisymmetric solutions that can be cast in a Kerr-Schild form with a seed metric given by the Lifshitz spacetime. Correspondingly, we study the issue of uniqueness of Lifshitz solitons when conside... | 8.137249 | 7.449678 | 8.023542 | 7.077995 | 8.438068 | 8.052109 | 8.103916 | 7.120331 | 7.358935 | 8.612231 | 7.477989 | 7.291899 | 7.879976 | 7.303731 | 7.615599 | 7.382101 | 7.476873 | 6.953187 | 7.4791 | 7.918107 | 7.48779 |
1102.1073 | Derek Teaney | Simon Caron-Huot, Paul M. Chesler, Derek Teaney | Fluctuation, dissipation, and thermalization in non-equilibrium AdS_5
black hole geometries | 28 pages, 6 figures | Phys.Rev.D84:026012,2011 | 10.1103/PhysRevD.84.026012 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a simple recipe for computing dissipation and fluctuations
(commutator and anti-commutator correlation functions) for non-equilibrium
black hole geometries. The recipe formulates Hawking radiation as an initial
value problem, and is suitable for numerical work. We show how to package the
fluctuation and dissi... | [
{
"created": "Sat, 5 Feb 2011 15:02:32 GMT",
"version": "v1"
}
] | 2011-08-12 | [
[
"Caron-Huot",
"Simon",
""
],
[
"Chesler",
"Paul M.",
""
],
[
"Teaney",
"Derek",
""
]
] | We give a simple recipe for computing dissipation and fluctuations (commutator and anti-commutator correlation functions) for non-equilibrium black hole geometries. The recipe formulates Hawking radiation as an initial value problem, and is suitable for numerical work. We show how to package the fluctuation and dissipa... | 9.192629 | 8.069685 | 8.960649 | 8.042388 | 8.949605 | 8.243475 | 9.030141 | 8.30886 | 8.058561 | 9.645566 | 8.32703 | 8.252009 | 8.519609 | 8.304196 | 8.462561 | 8.637867 | 8.489175 | 8.269849 | 8.350123 | 8.762324 | 8.425034 |
hep-th/9405045 | null | V. D. Lyakhovsky | Group-like Structures in Quantum Lie Algebras and the Process of
Quantization | 10 pages | null | null | SPBU-IP-94-2, St.Petersburg | hep-th alg-geom math.QA | null | For a certain class of Lie bialgebras $(A,A^*)$ the corresponding quantum
universal enveloping algebras $U_q(A)$ are prooved to be equivalent to quantum
groups Fun$_q(F^*)$, $F^*$ being the factor group for the dual group $G^*$.
This property can be used to simplify the process of quantization. The
described class ap... | [
{
"created": "Fri, 6 May 1994 12:36:56 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Lyakhovsky",
"V. D.",
""
]
] | For a certain class of Lie bialgebras $(A,A^*)$ the corresponding quantum universal enveloping algebras $U_q(A)$ are prooved to be equivalent to quantum groups Fun$_q(F^*)$, $F^*$ being the factor group for the dual group $G^*$. This property can be used to simplify the process of quantization. The described class appe... | 10.062234 | 11.315638 | 10.560492 | 9.414584 | 11.793139 | 10.327378 | 10.187734 | 9.841404 | 9.732791 | 10.998736 | 8.824532 | 9.210227 | 9.92765 | 8.971242 | 9.105514 | 9.018627 | 9.083693 | 9.109715 | 8.620179 | 9.339793 | 9.138128 |
hep-th/0205007 | Ioannis Bakas | I. Bakas and C. Sourdis | Notes on Periodic Solitons | 11 pages, latex; proceedings of the 2001 RTN meeting in Corfu | Fortsch.Phys. 50 (2002) 815-824 | 10.1002/1521-3978(200209)50:8/9<815::AID-PROP815>3.0.CO;2-Z | null | hep-th | null | We consider static solutions of the sine-Gordon theory defined on a cylinder,
which can be either periodic or quasi-periodic in space. They are described by
the different modes of a simple pendulum moving in an inverted effective
potential and correspond to its libration or rotation. We review the
decomposition of th... | [
{
"created": "Wed, 1 May 2002 03:19:43 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bakas",
"I.",
""
],
[
"Sourdis",
"C.",
""
]
] | We consider static solutions of the sine-Gordon theory defined on a cylinder, which can be either periodic or quasi-periodic in space. They are described by the different modes of a simple pendulum moving in an inverted effective potential and correspond to its libration or rotation. We review the decomposition of the ... | 10.873991 | 11.15378 | 11.432223 | 10.241526 | 10.322956 | 10.188793 | 10.373232 | 9.952476 | 10.007487 | 11.74761 | 10.212804 | 10.529457 | 10.816284 | 10.226704 | 10.240347 | 10.094981 | 10.105833 | 10.650134 | 10.177588 | 10.94257 | 10.109954 |
hep-th/9711063 | Daniela | Daniela Bigatti, Leonard Susskind | A note on discrete light cone quantization | 4 pages, LaTeX; two misprints and a reference corrected | Phys.Lett.B425:351-353,1998 | 10.1016/S0370-2693(98)00105-1 | SU-ITP 97/47 | hep-th | null | In this brief note we would like to discuss, in a simple model system, the
conditions under which the discrete light cone quantization framework should be
trusted as an approximation scheme, with regard, in particular, to the size and
mass of the system. Specifically, we are going to discuss ``quark-antiquark''
bound... | [
{
"created": "Mon, 10 Nov 1997 21:57:15 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Nov 1997 23:33:53 GMT",
"version": "v2"
},
{
"created": "Wed, 12 Nov 1997 21:51:04 GMT",
"version": "v3"
}
] | 2009-10-07 | [
[
"Bigatti",
"Daniela",
""
],
[
"Susskind",
"Leonard",
""
]
] | In this brief note we would like to discuss, in a simple model system, the conditions under which the discrete light cone quantization framework should be trusted as an approximation scheme, with regard, in particular, to the size and mass of the system. Specifically, we are going to discuss ``quark-antiquark'' bound s... | 14.784297 | 13.395285 | 13.206063 | 12.581387 | 13.804808 | 14.551278 | 13.148056 | 12.377474 | 12.514567 | 13.954115 | 13.258879 | 12.83634 | 12.912516 | 12.524253 | 12.893829 | 12.639688 | 12.978185 | 12.356816 | 12.936212 | 12.665579 | 12.74092 |
hep-th/0311177 | Satabhisa Dasgupta | Satabhisa Dasgupta and Tathagata Dasgupta | Nonsinglet Sector of $c=1$ Matrix Model and 2D Black Hole | 54 pages, 10 figures | null | null | RUNHETC-2003-30 | hep-th | null | Extending our recent work (\arXiv{\tt hep-th/0310106}) we study the
nonsinglet sector of $c=1$ matrix model by renormalization group analysis for a
gauged matrix quantum mechanics on circle with an appropriate gauge breaking
term to incorporate the effect of world-sheet vortices. The flow equations
indicate BKT phase... | [
{
"created": "Thu, 20 Nov 2003 20:39:25 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dasgupta",
"Satabhisa",
""
],
[
"Dasgupta",
"Tathagata",
""
]
] | Extending our recent work (\arXiv{\tt hep-th/0310106}) we study the nonsinglet sector of $c=1$ matrix model by renormalization group analysis for a gauged matrix quantum mechanics on circle with an appropriate gauge breaking term to incorporate the effect of world-sheet vortices. The flow equations indicate BKT phase t... | 12.549047 | 12.70621 | 14.418731 | 11.836448 | 13.293644 | 12.528115 | 13.588669 | 12.191211 | 12.288355 | 14.672967 | 11.940191 | 11.988373 | 12.598349 | 11.997068 | 11.819917 | 12.393346 | 12.191185 | 12.143919 | 11.972723 | 12.82471 | 12.09289 |
2204.06961 | Antonio Amariti | Antonio Amariti, Simone Rota | Webs of 3d $\mathcal{N} = 2$ dualities with D-type superpotentials | 34 pages, 1 figure | null | 10.1007/JHEP01(2023)124 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study 3d $\mathcal{N}=2$ dualities arising from the compactification of 4d
$\mathcal{N}=1$ $Usp(2 n)$ SQCD with two antisymmetric rank-two tensors and
$D_{k+2}$-type superpotential, with odd $k$. The analysis is carried out by
using field theory methods and by checking the various steps on the three
sphere partiti... | [
{
"created": "Thu, 14 Apr 2022 13:40:07 GMT",
"version": "v1"
}
] | 2023-02-08 | [
[
"Amariti",
"Antonio",
""
],
[
"Rota",
"Simone",
""
]
] | We study 3d $\mathcal{N}=2$ dualities arising from the compactification of 4d $\mathcal{N}=1$ $Usp(2 n)$ SQCD with two antisymmetric rank-two tensors and $D_{k+2}$-type superpotential, with odd $k$. The analysis is carried out by using field theory methods and by checking the various steps on the three sphere partition... | 9.704123 | 8.53341 | 10.709852 | 8.469105 | 8.623797 | 8.696218 | 8.708703 | 8.572762 | 8.2958 | 11.809266 | 8.581822 | 8.795352 | 9.713104 | 8.588624 | 8.63597 | 8.683212 | 8.848331 | 8.868891 | 8.909599 | 9.981616 | 8.820765 |
1911.06320 | Yuho Sakatani | Yuho Sakatani | U-duality extension of Drinfel'd double | 34 pages; v2: references added, expanded the discussion of the
Yang-Baxter deformation; v3: a reference added, typos corrected, to appear in
PTEP; v4: footnotes 5 and 8 added, a redundant condition in Eq.(6.20) removed | Prog Theor Exp Phys (2020) | 10.1093/ptep/ptz172 | null | hep-th math.DG math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A family of algebras $\mathcal{E}_n$ that extends the Lie algebra of the
Drinfel'd double is proposed. This allows us to systematically construct the
generalized frame fields $E_A{}^I$ which realize the proposed algebra by means
of the generalized Lie derivative, i.e., $\hat{\mathcal{L}}_{E_A}E_B{}^I = -
\mathcal{F}_... | [
{
"created": "Thu, 14 Nov 2019 18:59:48 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Nov 2019 17:18:08 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Feb 2020 15:27:58 GMT",
"version": "v3"
},
{
"created": "Fri, 24 Apr 2020 16:00:00 GMT",
"version": "v4"
}
] | 2020-04-27 | [
[
"Sakatani",
"Yuho",
""
]
] | A family of algebras $\mathcal{E}_n$ that extends the Lie algebra of the Drinfel'd double is proposed. This allows us to systematically construct the generalized frame fields $E_A{}^I$ which realize the proposed algebra by means of the generalized Lie derivative, i.e., $\hat{\mathcal{L}}_{E_A}E_B{}^I = - \mathcal{F}_{A... | 7.255506 | 6.451657 | 7.460295 | 6.460905 | 6.735122 | 6.315403 | 6.209674 | 6.11704 | 6.017224 | 9.172043 | 6.150152 | 6.125132 | 6.673089 | 6.248346 | 6.065897 | 6.177089 | 6.346032 | 6.387065 | 6.012793 | 6.609671 | 6.096089 |
1808.06620 | Henry Lin Mr. | Henry W. Lin | Cayley graphs and complexity geometry | 16 pages, 3 figures | null | 10.1007/JHEP02(2019)063 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The basic idea of quantum complexity geometry is to endow the space of
unitary matrices with a metric, engineered to make complex operators far from
the origin, and simple operators near. By restricting our attention to a finite
subgroup of the unitary group, we observe that this idea can be made rigorous:
the comple... | [
{
"created": "Mon, 20 Aug 2018 18:00:09 GMT",
"version": "v1"
}
] | 2019-02-20 | [
[
"Lin",
"Henry W.",
""
]
] | The basic idea of quantum complexity geometry is to endow the space of unitary matrices with a metric, engineered to make complex operators far from the origin, and simple operators near. By restricting our attention to a finite subgroup of the unitary group, we observe that this idea can be made rigorous: the complexi... | 9.344251 | 9.929199 | 11.51156 | 9.292118 | 9.772923 | 9.106926 | 9.707582 | 9.738278 | 9.730469 | 10.55552 | 9.98983 | 9.190978 | 9.097989 | 9.113309 | 9.572553 | 9.374757 | 9.543933 | 9.380626 | 8.979204 | 8.95229 | 9.142924 |
hep-th/9606013 | Nsc Kipt | A. A. Zheltukhin | Tension as a Perturbative Parameter in Non--Linear String Equations in
Curved Space--Time | 6 pages, LATEX. Submitted to Class.Quantum Grav | Class.Quant.Grav. 13 (1996) 2357-2360 | 10.1088/0264-9381/13/9/003 | null | hep-th | null | A perturbation theory with respect to tension parameter
$\gamma/\alpha^\prime$ for the non--linear equations of string, moving in
curved space--time is considered. Obtained are linearized motion equations for
the functions of the $n-$th degree of approximation ($n=0,1,2$)
| [
{
"created": "Tue, 4 Jun 1996 08:20:53 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Zheltukhin",
"A. A.",
""
]
] | A perturbation theory with respect to tension parameter $\gamma/\alpha^\prime$ for the non--linear equations of string, moving in curved space--time is considered. Obtained are linearized motion equations for the functions of the $n-$th degree of approximation ($n=0,1,2$) | 16.981836 | 16.161894 | 15.41643 | 14.772215 | 16.9846 | 14.516239 | 15.075071 | 16.146099 | 15.267994 | 14.144719 | 15.650074 | 14.049807 | 14.835428 | 13.848739 | 13.963223 | 14.163205 | 13.756288 | 14.702238 | 14.998016 | 14.855803 | 14.30581 |
hep-th/0304228 | Rafael Montemayor | H. Casini, R. Montemayor and Luis F. Urrutia | Duality for symmetric second rank tensors. II. The linearized
gravitational field | 20 pages, no figures | Phys.Rev. D68 (2003) 065011 | 10.1103/PhysRevD.68.065011 | null | hep-th | null | The construction of dual theories for linearized gravity in four dimensions
is considered. Our approach is based on the parent Lagrangian method previously
developed for the massive spin-two case, but now considered for the zero mass
case. This leads to a dual theory described in terms of a rank two symmetric
tensor,... | [
{
"created": "Sat, 26 Apr 2003 12:27:28 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Casini",
"H.",
""
],
[
"Montemayor",
"R.",
""
],
[
"Urrutia",
"Luis F.",
""
]
] | The construction of dual theories for linearized gravity in four dimensions is considered. Our approach is based on the parent Lagrangian method previously developed for the massive spin-two case, but now considered for the zero mass case. This leads to a dual theory described in terms of a rank two symmetric tensor, a... | 10.450423 | 10.167315 | 10.080931 | 9.556501 | 10.11518 | 9.853703 | 9.84342 | 9.168344 | 9.809165 | 10.768803 | 9.644206 | 9.843369 | 10.015268 | 9.620114 | 9.597682 | 9.816885 | 10.082017 | 9.765723 | 9.997957 | 9.93245 | 9.477607 |
hep-th/0205178 | Tsuda | K.Shima, Y.Tanii and M.Tsuda | Linearizing N = 2 Nonlinear Supersymmetry | 8 pages, Latex, some typos corrected some more discussions added | Phys.Lett. B546 (2002) 162-166 | 10.1016/S0370-2693(02)02670-9 | SIT-LP-02/05, STUPP-02-166 | hep-th | null | We investigate for the N = 2 supersymmetry (SUSY) a relation between a vector
supermultiplet of the linear SUSY and the Volkov-Akulov model of the nonlinear
SUSY. We express component fields of the vector supermultiplet in terms of
Nambu-Goldstone fermion fields at the leading orders in a SUSY invariant way,
and show... | [
{
"created": "Fri, 17 May 2002 05:18:36 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Sep 2002 02:12:11 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Shima",
"K.",
""
],
[
"Tanii",
"Y.",
""
],
[
"Tsuda",
"M.",
""
]
] | We investigate for the N = 2 supersymmetry (SUSY) a relation between a vector supermultiplet of the linear SUSY and the Volkov-Akulov model of the nonlinear SUSY. We express component fields of the vector supermultiplet in terms of Nambu-Goldstone fermion fields at the leading orders in a SUSY invariant way, and show t... | 8.447498 | 7.566373 | 8.673291 | 6.689399 | 7.848261 | 6.990161 | 8.055042 | 6.944962 | 7.099885 | 9.891467 | 7.65853 | 7.829093 | 8.303177 | 7.8552 | 8.173988 | 8.128754 | 7.654437 | 7.9688 | 7.855579 | 8.433786 | 7.662458 |
1908.04873 | A. Yu. Petrov | A. J. G. Carvalho, D. R. Granado, J. R. Nascimento, A. Yu. Petrov | Non-Abelian aether-like term in four dimensions | 13 pages, minor corrections | Eur. Phys. J. C79, 817 (2019) | 10.1140/epjc/s10052-019-7342-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The non-Abelian aether-like Lorentz-breaking term, involving triple and
quartic self-coupling vertices, is generated from the non-Abelian
generalization of the Lorentz-breaking extended QED including only a minimal
spinor-vector interaction. This term is shown explicitly to be finite and
non-ambiguous.
| [
{
"created": "Tue, 13 Aug 2019 22:02:40 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Aug 2019 12:01:46 GMT",
"version": "v2"
}
] | 2019-10-08 | [
[
"Carvalho",
"A. J. G.",
""
],
[
"Granado",
"D. R.",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
]
] | The non-Abelian aether-like Lorentz-breaking term, involving triple and quartic self-coupling vertices, is generated from the non-Abelian generalization of the Lorentz-breaking extended QED including only a minimal spinor-vector interaction. This term is shown explicitly to be finite and non-ambiguous. | 17.151209 | 12.676098 | 14.670073 | 13.370321 | 15.861727 | 16.427647 | 13.397323 | 14.762731 | 12.956043 | 19.657204 | 12.457385 | 15.63286 | 15.265244 | 14.800259 | 15.550639 | 14.343228 | 14.619704 | 14.967756 | 14.918983 | 15.627435 | 13.871324 |
2209.08121 | Francisco A. Brito | Jose L. Paulino, Francisco A. Brito | The physics of intersecting thick to thin branes | 15 pages, 9 figures | null | 10.1016/j.physletb.2023.137771 | null | hep-th cond-mat.str-el | http://creativecommons.org/licenses/by/4.0/ | We model four-dimensional junctions made out of intersections of co-dimension
one brane living in higher-dimensional spacetimes through domain walls. We take
a new look at the problem of localizing fermion states on brane junctions as a
result of intersecting one thick brane to others sufficiently thin. All the
brane... | [
{
"created": "Fri, 16 Sep 2022 18:21:49 GMT",
"version": "v1"
}
] | 2023-03-22 | [
[
"Paulino",
"Jose L.",
""
],
[
"Brito",
"Francisco A.",
""
]
] | We model four-dimensional junctions made out of intersections of co-dimension one brane living in higher-dimensional spacetimes through domain walls. We take a new look at the problem of localizing fermion states on brane junctions as a result of intersecting one thick brane to others sufficiently thin. All the branes ... | 17.257784 | 16.247984 | 16.668539 | 15.490729 | 16.388699 | 14.432274 | 17.3708 | 16.161388 | 15.77133 | 17.088612 | 16.384022 | 15.853882 | 16.323357 | 16.225473 | 16.010555 | 15.557441 | 16.142439 | 15.586733 | 16.198818 | 16.956285 | 15.992529 |
1903.08613 | Alexander Migdal | Alexander Migdal | Universal Area Law in Turbulence | 10 pages, 0 figures, inserted missing factor od 2 in recurrent
equation for vorticity correlations | null | null | null | hep-th nlin.CD physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We re-visit the Area Law in Turbulence discovered many years ago \cite{M93}
and verified recently in numerical experiments\cite{S19}. We derive this law in
a simpler way, at the same time outlining the limits of its applicability.
Using the PDF for velocity circulation as a functional of the loop in
coordinate space,... | [
{
"created": "Wed, 20 Mar 2019 16:54:53 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Mar 2019 15:56:26 GMT",
"version": "v2"
},
{
"created": "Mon, 1 Apr 2019 06:02:02 GMT",
"version": "v3"
}
] | 2019-04-02 | [
[
"Migdal",
"Alexander",
""
]
] | We re-visit the Area Law in Turbulence discovered many years ago \cite{M93} and verified recently in numerical experiments\cite{S19}. We derive this law in a simpler way, at the same time outlining the limits of its applicability. Using the PDF for velocity circulation as a functional of the loop in coordinate space, w... | 12.330606 | 12.000595 | 12.783114 | 11.671782 | 12.240732 | 13.095682 | 12.143575 | 12.001034 | 11.638355 | 14.527103 | 11.721957 | 12.184708 | 12.365973 | 11.863907 | 11.731315 | 12.044006 | 12.120111 | 11.974404 | 11.804602 | 12.545286 | 11.835959 |
hep-th/0310044 | Ryang Shijong | Shijong Ryang | String Propagators in Time-Dependent and Time-Independent Homogeneous
Plane Waves | 15 pages, LaTeX, no figures, minor corrections added | JHEP 0311 (2003) 007 | 10.1088/1126-6708/2003/11/007 | null | hep-th | null | For a special time-dependent homogeneous plane wave background that includes
a null singularity we construct the closed string propagators. We carry out the
summation over the oscillator modes and extract the worldsheet spacetime
structures of string propagators specially near the singularity. We construct
the closed... | [
{
"created": "Mon, 6 Oct 2003 05:16:29 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Nov 2003 02:13:25 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Ryang",
"Shijong",
""
]
] | For a special time-dependent homogeneous plane wave background that includes a null singularity we construct the closed string propagators. We carry out the summation over the oscillator modes and extract the worldsheet spacetime structures of string propagators specially near the singularity. We construct the closed s... | 12.084067 | 10.709193 | 11.578284 | 9.881351 | 10.835066 | 9.99836 | 10.943876 | 10.306762 | 10.83117 | 12.242002 | 9.617719 | 10.135108 | 11.318737 | 10.105679 | 9.978116 | 10.257442 | 10.167334 | 10.178332 | 10.016448 | 10.720413 | 10.140375 |
1410.0048 | Vladimir O. Soloviev | Vladimir O. Soloviev | Bigravity in tetrad Hamiltonian formalism and matter couplings | 25 pages, 1 table | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The tetrad approach is used to resolve the matrix square root appearing in
the dRGT potential. Constraints and their algebra are derived for the minimal
case. It is shown that the number of gravitational degrees of freedom
corresponds to one massless and one massive gravitational fields when two sorts
of matter separ... | [
{
"created": "Tue, 30 Sep 2014 21:04:15 GMT",
"version": "v1"
}
] | 2014-10-02 | [
[
"Soloviev",
"Vladimir O.",
""
]
] | The tetrad approach is used to resolve the matrix square root appearing in the dRGT potential. Constraints and their algebra are derived for the minimal case. It is shown that the number of gravitational degrees of freedom corresponds to one massless and one massive gravitational fields when two sorts of matter separat... | 17.146467 | 14.275156 | 12.999696 | 13.2891 | 13.575736 | 14.111773 | 13.71668 | 13.054682 | 12.433328 | 14.263331 | 13.584334 | 12.807046 | 13.755178 | 12.614068 | 12.957001 | 12.884995 | 12.620762 | 12.184074 | 12.796866 | 13.258247 | 12.763699 |
0907.2655 | El Hassan Saidi | El Hassan Saidi | Tetrahedron in F-theory Compactification | 27 pages, 9 figures | null | null | Lab/UFR-HEP 0901, GNPHE/0901 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Complex tetrahedral surface $\mathcal{T}$ is a non planar projective surface
that is generated by four intersecting complex projective planes $CP^{2}$. In
this paper, we study the family $\{\mathcal{T}_{m}\} $ of blow ups of
$\mathcal{T}$ and exhibit the link of these $\mathcal{T}_{m}$s with the set of
del Pezzo surf... | [
{
"created": "Wed, 15 Jul 2009 17:03:29 GMT",
"version": "v1"
}
] | 2009-07-16 | [
[
"Saidi",
"El Hassan",
""
]
] | Complex tetrahedral surface $\mathcal{T}$ is a non planar projective surface that is generated by four intersecting complex projective planes $CP^{2}$. In this paper, we study the family $\{\mathcal{T}_{m}\} $ of blow ups of $\mathcal{T}$ and exhibit the link of these $\mathcal{T}_{m}$s with the set of del Pezzo surfac... | 11.282382 | 11.131557 | 13.518908 | 10.955658 | 12.310848 | 12.048762 | 12.449721 | 11.344359 | 11.028017 | 14.828024 | 10.762689 | 10.321671 | 10.652628 | 10.884576 | 10.142635 | 10.040733 | 10.219808 | 10.840358 | 10.325359 | 11.784856 | 10.776096 |
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