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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1004.3664 | Daniel Puigdomenech | Jorge Alfaro, Dom\`enec Espriu, Daniel Puigdom\`enech | The emergence of geometry: a two-dimensional toy model | 18 pages | Phys.Rev.D82:045018,2010 | 10.1103/PhysRevD.82.045018 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the similarities between the effective chiral lagrangrian, relevant
for low-energy strong interactions, and the Einstein-Hilbert action. We use
these analogies to suggest a specific mechanism whereby gravitons would emerge
as Goldstone bosons of a global SO(D) X GL(D) symmetry broken down to SO(D) by
fermio... | [
{
"created": "Wed, 21 Apr 2010 10:00:07 GMT",
"version": "v1"
}
] | 2012-09-17 | [
[
"Alfaro",
"Jorge",
""
],
[
"Espriu",
"Domènec",
""
],
[
"Puigdomènech",
"Daniel",
""
]
] | We review the similarities between the effective chiral lagrangrian, relevant for low-energy strong interactions, and the Einstein-Hilbert action. We use these analogies to suggest a specific mechanism whereby gravitons would emerge as Goldstone bosons of a global SO(D) X GL(D) symmetry broken down to SO(D) by fermion ... | 9.348979 | 10.368539 | 10.320146 | 10.209547 | 11.102643 | 10.649009 | 10.346039 | 10.469571 | 9.699219 | 10.808086 | 10.117428 | 9.609487 | 9.464772 | 9.527586 | 9.68163 | 9.866298 | 9.875363 | 9.333965 | 9.530651 | 9.179466 | 9.736352 |
1109.0335 | Hongwei Yu | Jiawei Hu, Hongwei Yu | Entanglement generation outside a Schwarzschild black hole and the
Hawking effect | 15 pages, no figures, Revtex | JHEP 08(2011)137 | 10.1007/JHEP08(2011)137 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the Hawking effect by studying the asymptotic entanglement of two
mutually independent two-level atoms placed at a fixed radial distance outside
a Schwarzschild black hole in the framework of open quantum systems. We treat
the two-atom system as an open quantum system in a bath of fluctuating
quantized mas... | [
{
"created": "Fri, 2 Sep 2011 00:26:53 GMT",
"version": "v1"
}
] | 2011-09-05 | [
[
"Hu",
"Jiawei",
""
],
[
"Yu",
"Hongwei",
""
]
] | We examine the Hawking effect by studying the asymptotic entanglement of two mutually independent two-level atoms placed at a fixed radial distance outside a Schwarzschild black hole in the framework of open quantum systems. We treat the two-atom system as an open quantum system in a bath of fluctuating quantized massl... | 6.271466 | 7.178371 | 6.131018 | 5.829369 | 6.628941 | 6.458626 | 7.147806 | 5.838791 | 6.714951 | 6.058078 | 6.540397 | 6.346684 | 6.201432 | 6.17593 | 6.237853 | 6.190459 | 6.280176 | 6.207584 | 6.510154 | 6.150702 | 6.463602 |
hep-th/9907103 | Marko Kolanovic | A. Ilakovac, M. Kolanovic, S. Pallua and P.Prester | Violation of the string hypothesis and Heisenberg XXZ spin chain | 15 pages, 7 Postscript figures | Phys.Rev. B60 (1999) 7271 | 10.1103/PhysRevB.60.7271 | null | hep-th cond-mat math-ph math.MP | null | In this paper we count the numbers of real and complex solutions to Bethe
constraints in the two particle sector of the XXZ model. We find exact number
of exceptions to the string conjecture and total number of solutions which is
required for completeness.
| [
{
"created": "Wed, 14 Jul 1999 09:09:08 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Ilakovac",
"A.",
""
],
[
"Kolanovic",
"M.",
""
],
[
"Pallua",
"S.",
""
],
[
"Prester",
"P.",
""
]
] | In this paper we count the numbers of real and complex solutions to Bethe constraints in the two particle sector of the XXZ model. We find exact number of exceptions to the string conjecture and total number of solutions which is required for completeness. | 22.464169 | 18.168892 | 19.99884 | 16.064739 | 21.401964 | 15.728188 | 17.172089 | 15.009448 | 15.946079 | 18.952147 | 16.405666 | 16.959761 | 18.809452 | 17.277866 | 17.401695 | 17.208771 | 17.196159 | 18.480825 | 17.742586 | 18.891991 | 17.217131 |
hep-th/0406236 | Bodo Geyer | B. Geyer and P.M. Lavrov | Basic properties of Fedosov supermanifolds | 10 pages, Latex, Contribution to Special Issue of Vestnik of Tomsk
State Pedagogical University devoted to 70th Anniversary of Physical and
Mathematical Department | TSPU Vestnik 44N7 (2004) 62-68 | null | null | hep-th | null | Basic properties of even (odd) supermanifolds endowed with a connection
respecting a given symplectic structure are studied. Such supermanifolds can be
considered as generalization of Fedosov manifolds to the supersymmetric case.
| [
{
"created": "Fri, 25 Jun 2004 10:40:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Geyer",
"B.",
""
],
[
"Lavrov",
"P. M.",
""
]
] | Basic properties of even (odd) supermanifolds endowed with a connection respecting a given symplectic structure are studied. Such supermanifolds can be considered as generalization of Fedosov manifolds to the supersymmetric case. | 8.437825 | 6.295854 | 8.270636 | 6.971816 | 6.292793 | 5.578732 | 6.115669 | 6.255231 | 6.898438 | 11.529469 | 5.744617 | 6.386725 | 7.808702 | 6.492174 | 6.935023 | 6.63073 | 6.782575 | 6.64957 | 6.858612 | 7.710814 | 6.904793 |
2311.08498 | Stefan Groot Nibbelink | Stefan Groot Nibbelink | GLSM resolutions of torsional heterotic Z2xZ2 orbifolds | 12 pages LaTeX, prepared as proceedings for the workshop GLSM@30 at
the Simons Center, revised based on comments by a referee | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Heterotic toriodal Z2xZ2 orbifolds may possess discrete torsion between the
two defining orbifold twists in the form of additional cocycle factors in their
one-loop partition functions. Using Gauged Linear Sigma Models (GLSMs) the
consequences of discrete torsion can be uncovered when the orbifold is smoothed
out by ... | [
{
"created": "Tue, 14 Nov 2023 19:42:59 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jul 2024 20:05:19 GMT",
"version": "v2"
}
] | 2024-07-12 | [
[
"Nibbelink",
"Stefan Groot",
""
]
] | Heterotic toriodal Z2xZ2 orbifolds may possess discrete torsion between the two defining orbifold twists in the form of additional cocycle factors in their one-loop partition functions. Using Gauged Linear Sigma Models (GLSMs) the consequences of discrete torsion can be uncovered when the orbifold is smoothed out by sw... | 20.224482 | 15.196912 | 21.755779 | 15.658591 | 17.083755 | 17.204287 | 16.468863 | 15.473264 | 15.783648 | 23.562649 | 16.824314 | 16.443447 | 17.601696 | 16.505781 | 16.490841 | 16.745359 | 16.134512 | 16.239979 | 16.790329 | 19.201241 | 16.421906 |
2303.16108 | Juan Miguel Nieto Garc\'ia | Juan Miguel Nieto Garc\'ia, Roberto Ruiz, Alessandro Torrielli | Infinite-dimensional R-matrices for the relativistic scattering of
massless modes on $\boldsymbol{\mathrm{AdS}_2}$ | 22 pages. v2: minor modifications, references added. v3: discussion
on crossing expanded, references added | null | null | DMUS-MP-23/07, ZMP-HH/23-4 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct infinite-dimensional R-matrices that generalise the relativistic
scattering of massless modes with the same chirality on $\mathrm{AdS}_2$ near
the Berestein-Maldacena-Nastase vacuum. We show that the infrared limit of the
R-matrices reproduces finite-dimensional scattering of massless modes on
$\mathrm{A... | [
{
"created": "Tue, 28 Mar 2023 16:24:06 GMT",
"version": "v1"
},
{
"created": "Sat, 1 Apr 2023 18:04:03 GMT",
"version": "v2"
},
{
"created": "Sun, 21 May 2023 11:10:37 GMT",
"version": "v3"
}
] | 2023-05-23 | [
[
"García",
"Juan Miguel Nieto",
""
],
[
"Ruiz",
"Roberto",
""
],
[
"Torrielli",
"Alessandro",
""
]
] | We construct infinite-dimensional R-matrices that generalise the relativistic scattering of massless modes with the same chirality on $\mathrm{AdS}_2$ near the Berestein-Maldacena-Nastase vacuum. We show that the infrared limit of the R-matrices reproduces finite-dimensional scattering of massless modes on $\mathrm{AdS... | 10.93832 | 9.754866 | 11.646394 | 9.600815 | 9.755422 | 12.919789 | 10.597945 | 10.108854 | 9.585593 | 11.469511 | 9.885031 | 9.565245 | 10.220645 | 9.551957 | 9.638076 | 10.251877 | 9.87766 | 10.250513 | 9.66566 | 9.984646 | 10.44101 |
hep-th/9803245 | Christian Jaekel | Christian Jaekel | The Relation Between KMS-states for Different Temperatures | latex, 24 pages | Annales Henri Poincare 5 (2004) 579-606 | null | null | hep-th | null | Given a thermal field theory for some temperature $\beta^{-1}$, we construct
the theory at an arbitrary temperature $ 1 / \beta'$. Our work is based on a
construction invented by Buchholz and Junglas, which we adapt to thermal field
theories. In a first step we construct states which closely resemble KMS states
for t... | [
{
"created": "Mon, 30 Mar 1998 14:53:10 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Apr 1998 16:13:17 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Nov 1998 16:04:08 GMT",
"version": "v3"
},
{
"created": "Wed, 7 Apr 1999 15:07:46 GMT",
"version": "v4"
},
{
"cre... | 2007-05-23 | [
[
"Jaekel",
"Christian",
""
]
] | Given a thermal field theory for some temperature $\beta^{-1}$, we construct the theory at an arbitrary temperature $ 1 / \beta'$. Our work is based on a construction invented by Buchholz and Junglas, which we adapt to thermal field theories. In a first step we construct states which closely resemble KMS states for the... | 7.478063 | 8.652699 | 8.569871 | 7.812493 | 7.981678 | 8.444708 | 8.118461 | 8.027783 | 8.176538 | 9.477413 | 8.104184 | 7.908468 | 7.633524 | 7.449808 | 7.50718 | 7.437415 | 7.325374 | 7.53538 | 7.449671 | 7.649024 | 7.435225 |
hep-th/9707123 | Ashoke Sen | Ashoke Sen | A Note on Enhanced Gauge Symmetries in M- and String Theory | LaTeX file, 12 pages, minor sign errors corrected | JHEP 9709:001,1997 | 10.1088/1126-6708/1997/09/001 | MRI-PHY/P970717 | hep-th | null | Two different mechanisms exist in non-perturbative String / M- theory for
enhanced SU(N) (SO(2N)) gauge symmetries. It can appear in type IIA string
theory or M-theory near an $A_{N-1}$ (D_N) type singularity where membrnes
wrapped around two cycles become massless, or it can appear due to coincident
D-branes (and or... | [
{
"created": "Sun, 13 Jul 1997 11:04:56 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Aug 1997 04:13:23 GMT",
"version": "v2"
}
] | 2010-02-04 | [
[
"Sen",
"Ashoke",
""
]
] | Two different mechanisms exist in non-perturbative String / M- theory for enhanced SU(N) (SO(2N)) gauge symmetries. It can appear in type IIA string theory or M-theory near an $A_{N-1}$ (D_N) type singularity where membrnes wrapped around two cycles become massless, or it can appear due to coincident D-branes (and orie... | 7.038871 | 7.644629 | 7.339796 | 6.670036 | 7.137007 | 7.026062 | 7.977887 | 7.163113 | 6.72754 | 7.923593 | 6.990322 | 6.562418 | 6.79258 | 6.446545 | 6.529406 | 6.663492 | 6.656657 | 6.686715 | 6.73549 | 6.677323 | 6.501981 |
hep-th/0404153 | Dmitry Talalaev | D. Talalaev | Quantization of the Gaudin System | 9 pages | null | null | ITEP-TH-14/04 | hep-th math.QA nlin.SI | null | In this article we exploit the known commutative family in Y(gl(n)) - the
Bethe subalgebra - and its special limit to construct quantization of the
Gaudin integrable system. We give explicit expressions for quantum hamiltonians
QI_k(u), k=1,..., n. At small order k=1,...,3 they coincide with the
quasiclassic ones, ev... | [
{
"created": "Wed, 21 Apr 2004 05:55:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Talalaev",
"D.",
""
]
] | In this article we exploit the known commutative family in Y(gl(n)) - the Bethe subalgebra - and its special limit to construct quantization of the Gaudin integrable system. We give explicit expressions for quantum hamiltonians QI_k(u), k=1,..., n. At small order k=1,...,3 they coincide with the quasiclassic ones, even... | 21.554438 | 22.163782 | 31.167515 | 21.52379 | 22.352631 | 24.705484 | 23.416847 | 22.611282 | 20.421436 | 24.043081 | 19.250278 | 20.263311 | 22.22473 | 20.019989 | 19.583319 | 20.042131 | 18.879011 | 19.543219 | 18.182386 | 19.918167 | 18.001369 |
hep-th/9307067 | null | L. Baulieu and E. Rabinovici | On the Calculability of Observables in Topological Quantum Mechanical
Models | Latex file. 18 pages. preprint Racah Institute 151-Paris LPTHE 93-28.
(THIS IS THE SAME VERSION AS THE ONE SENT TWO DAYS AGO BUT WITH LINES
CORRECTLY TRUNCATED. WITH APOLOGIES FROM THE AUTHORS) | Phys.Lett. B316 (1993) 93-101 | 10.1016/0370-2693(93)90663-3 | null | hep-th | null | We consider a superconformal quantum mechanical system which has been chosen
on the basis of a local BRST topological invariance. We suggest that it truly
leads to topological observables which we compute. The absences of a ground
state and of a mass gap are special features of this system.
| [
{
"created": "Fri, 9 Jul 1993 14:43:36 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jul 1993 14:24:39 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Baulieu",
"L.",
""
],
[
"Rabinovici",
"E.",
""
]
] | We consider a superconformal quantum mechanical system which has been chosen on the basis of a local BRST topological invariance. We suggest that it truly leads to topological observables which we compute. The absences of a ground state and of a mass gap are special features of this system. | 17.111174 | 13.518131 | 16.193907 | 13.154703 | 14.378064 | 16.160259 | 14.753677 | 14.474643 | 13.30287 | 18.220936 | 14.953117 | 15.014778 | 15.818682 | 15.434053 | 14.781322 | 15.99894 | 16.130205 | 14.952978 | 15.709986 | 16.705416 | 15.144625 |
2401.11637 | Eric R. Sharpe | E. Sharpe | A survey of recent developments in GLSMs | 20 pages, LaTeX; v2: references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we briefly survey some developments in gauged linear sigma
models (GLSMs). Specifically, we give an overview of progress on constructions
of GLSMs for various geometries, GLSM-based computations of quantum cohomology,
quantum sheaf cohomology, and quantum K theory rings, as well as
two-dimensional abe... | [
{
"created": "Mon, 22 Jan 2024 00:20:38 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Feb 2024 01:55:31 GMT",
"version": "v2"
}
] | 2024-02-02 | [
[
"Sharpe",
"E.",
""
]
] | In this article we briefly survey some developments in gauged linear sigma models (GLSMs). Specifically, we give an overview of progress on constructions of GLSMs for various geometries, GLSM-based computations of quantum cohomology, quantum sheaf cohomology, and quantum K theory rings, as well as two-dimensional abeli... | 8.54882 | 7.864559 | 9.133608 | 6.843041 | 7.052491 | 7.143909 | 7.15996 | 7.239209 | 6.954395 | 11.122002 | 6.992166 | 7.380918 | 8.341578 | 7.379301 | 7.490415 | 7.580625 | 7.694545 | 7.631064 | 7.744916 | 7.943129 | 7.358882 |
hep-th/9204018 | 7353 | E. Brezin and S. Hikami | A naive matrix-model approach to two-dimensional quantum gravity coupled
to matter of arbitrary central charge | P. 11 | Phys.Lett. B283 (1992) 203-208 | 10.1016/0370-2693(92)90008-R | null | hep-th | null | In the usual matrix-model approach to random discretized two-dimensional
manifolds, one introduces n Ising spins on each cell, i.e. a discrete version
of 2D quantum gravity coupled to matter with a central charge n/2. The
matrix-model consists then of an integral over $2^{n}$ matrices, which we are
unable to solve fo... | [
{
"created": "Wed, 8 Apr 1992 06:41:09 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Brezin",
"E.",
""
],
[
"Hikami",
"S.",
""
]
] | In the usual matrix-model approach to random discretized two-dimensional manifolds, one introduces n Ising spins on each cell, i.e. a discrete version of 2D quantum gravity coupled to matter with a central charge n/2. The matrix-model consists then of an integral over $2^{n}$ matrices, which we are unable to solve for ... | 13.438082 | 13.649433 | 14.621593 | 12.904692 | 13.993184 | 14.868246 | 14.420838 | 12.738405 | 12.846986 | 16.373806 | 13.08893 | 13.35813 | 13.123588 | 12.945703 | 13.186978 | 13.436049 | 13.607894 | 13.266159 | 12.651262 | 13.602769 | 13.018696 |
0904.2431 | Kazunobu Maruyoshi | Kazunobu Maruyoshi | Quiver Gauge Theory and Extended Electric-magnetic Duality | 24 pages; v2: references added, typos corrected | JHEP 0909:061,2009 | 10.1088/1126-6708/2009/09/061 | YITP-09-26 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct N=1 A-D-E quiver gauge theory with the gauge kinetic term which
depends on the adjoint chiral superfields, as a low energy effective theory on
D5-branes wrapped on 2-cycles of Calabi-Yau 3-fold in IIB string theory. The
field-dependent gauge kinetic term can be engineered by introducing B-field
which hol... | [
{
"created": "Thu, 16 Apr 2009 08:58:43 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Jul 2009 03:14:57 GMT",
"version": "v2"
}
] | 2011-04-14 | [
[
"Maruyoshi",
"Kazunobu",
""
]
] | We construct N=1 A-D-E quiver gauge theory with the gauge kinetic term which depends on the adjoint chiral superfields, as a low energy effective theory on D5-branes wrapped on 2-cycles of Calabi-Yau 3-fold in IIB string theory. The field-dependent gauge kinetic term can be engineered by introducing B-field which holom... | 5.576441 | 5.623511 | 6.704225 | 5.646493 | 6.023704 | 5.677849 | 5.962607 | 5.650383 | 5.522177 | 6.883427 | 5.343345 | 5.358439 | 5.655431 | 5.464337 | 5.599772 | 5.484436 | 5.470326 | 5.346752 | 5.545852 | 5.812458 | 5.301595 |
1406.5129 | Bartomeu Fiol | Bartomeu Fiol, Blai Garolera and Genis Torrents | Exact probes of orientifolds | 28 pages. v2: Added references | null | 10.1007/JHEP09(2014)169 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the exact vacuum expectation value of circular Wilson loops for
Euclidean ${\cal N}=4$ super Yang-Mills with $G=SO(N),Sp(N)$, in the
fundamental and spinor representations. These field theories are dual to type
IIB string theory compactified on $AdS_5\times {\mathbb R} {\mathbb P}^5$ plus
certain choices o... | [
{
"created": "Thu, 19 Jun 2014 17:52:23 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Jul 2014 17:56:51 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Fiol",
"Bartomeu",
""
],
[
"Garolera",
"Blai",
""
],
[
"Torrents",
"Genis",
""
]
] | We compute the exact vacuum expectation value of circular Wilson loops for Euclidean ${\cal N}=4$ super Yang-Mills with $G=SO(N),Sp(N)$, in the fundamental and spinor representations. These field theories are dual to type IIB string theory compactified on $AdS_5\times {\mathbb R} {\mathbb P}^5$ plus certain choices of ... | 8.018727 | 8.279555 | 8.945861 | 7.404353 | 8.076898 | 8.273066 | 7.672813 | 7.928854 | 7.515023 | 9.274231 | 7.5604 | 7.670122 | 7.980255 | 7.442435 | 7.468652 | 7.557319 | 7.666877 | 7.505281 | 7.366045 | 8.03292 | 7.515624 |
hep-th/0010018 | Jun-Chen Su | Jun-Chen Su | Alternative Formulation of The Quantum Electroweak Theory | 16 pages,3 figures | null | null | null | hep-th | null | The quantization of the electroweak theory is performed starting from the
Lagrangian given in the so-called unitary gauge in which the unphysical
Goldstone fields disappear. In such a Lagrangian, the unphysical longitudinal
components of the gauge fields and the residual gauge degrees of freedom are
naturally elimina... | [
{
"created": "Wed, 4 Oct 2000 08:30:52 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Dec 2005 08:04:14 GMT",
"version": "v10"
},
{
"created": "Mon, 23 Oct 2000 01:30:26 GMT",
"version": "v2"
},
{
"created": "Thu, 2 Nov 2000 05:04:57 GMT",
"version": "v3"
},
{
"cr... | 2007-05-23 | [
[
"Su",
"Jun-Chen",
""
]
] | The quantization of the electroweak theory is performed starting from the Lagrangian given in the so-called unitary gauge in which the unphysical Goldstone fields disappear. In such a Lagrangian, the unphysical longitudinal components of the gauge fields and the residual gauge degrees of freedom are naturally eliminate... | 7.561292 | 7.840915 | 7.551901 | 7.250243 | 7.943406 | 7.829925 | 7.923561 | 7.720382 | 7.687148 | 8.1668 | 7.637566 | 7.479734 | 7.257896 | 7.177259 | 7.244488 | 7.268104 | 7.342921 | 7.355034 | 7.088993 | 7.319586 | 7.184023 |
hep-th/9708099 | Hyung Won Lee | H.W. Lee, Y.S. Myung (Inje U.) and Jin Young Kim (Kunsan Nat'l U.) | The role of fixed scalars in scattering off a 5D black hole | minor typo errors were corrected, 20 pages no figure, RevTeX | Phys. Rev. D 58, 104006 (1998) | 10.1103/PhysRevD.58.104006 | INJE-TP-97-3 | hep-th | null | We discuss the role of fixed scalars($\nu,\lambda$) in scattering off a
five-dimensional balck hole. The issue is to explain the disagreement of the
greybody factor for $\lambda$ between the semiclassical and effective string
calculations. In the effective string approach, this is related to the
operators with dimens... | [
{
"created": "Tue, 19 Aug 1997 04:43:33 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Aug 1997 04:47:36 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Jun 1998 05:20:37 GMT",
"version": "v3"
},
{
"created": "Sun, 11 Oct 1998 09:40:53 GMT",
"version": "v4"
}
] | 2016-08-25 | [
[
"Lee",
"H. W.",
"",
"Inje U."
],
[
"Myung",
"Y. S.",
"",
"Inje U."
],
[
"Kim",
"Jin Young",
"",
"Kunsan Nat'l U."
]
] | We discuss the role of fixed scalars($\nu,\lambda$) in scattering off a five-dimensional balck hole. The issue is to explain the disagreement of the greybody factor for $\lambda$ between the semiclassical and effective string calculations. In the effective string approach, this is related to the operators with dimensio... | 14.160868 | 12.970288 | 13.385062 | 13.338497 | 13.612826 | 13.793155 | 12.401481 | 13.979261 | 13.903213 | 14.434445 | 12.982487 | 13.305087 | 13.852119 | 12.970226 | 12.991114 | 13.495728 | 12.964089 | 12.640664 | 12.839603 | 13.559978 | 13.572414 |
hep-th/9904104 | Rob Leigh | David Berenstein and Robert G. Leigh | Superstring Perturbation Theory and Ramond-Ramond Backgrounds | 17 pages, LaTeX, 4 figures, uses epsf, latexsym, hyperref packages
Section on realization of supersymmetry algebra has been expanded | Phys. Rev. D 60, 106002 (1999) | 10.1103/PhysRevD.60.106002 | ILL-(TH)-99-02 | hep-th | null | We consider perturbative Type II superstring theory in the covariant NSR
formalism in the presence of NSNS and RR backgrounds. A concrete example that
we have in mind is the geometry of D3-branes which in the near-horizon region
is AdS_5 x S_5, although our methods may be applied to other backgrounds as
well. We show... | [
{
"created": "Wed, 14 Apr 1999 23:14:16 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Apr 1999 17:03:19 GMT",
"version": "v2"
}
] | 2016-08-25 | [
[
"Berenstein",
"David",
""
],
[
"Leigh",
"Robert G.",
""
]
] | We consider perturbative Type II superstring theory in the covariant NSR formalism in the presence of NSNS and RR backgrounds. A concrete example that we have in mind is the geometry of D3-branes which in the near-horizon region is AdS_5 x S_5, although our methods may be applied to other backgrounds as well. We show h... | 8.989717 | 8.813416 | 9.264595 | 8.421871 | 9.137116 | 8.652963 | 9.155866 | 8.631114 | 8.292664 | 10.275388 | 8.781632 | 8.415774 | 9.184938 | 8.53265 | 8.885831 | 8.657214 | 8.362444 | 8.65424 | 8.612484 | 9.46629 | 8.633053 |
hep-th/0209122 | Ashoke Sen | Ashoke Sen | Time and Tachyon | LaTeX file, 24 pages | Int.J.Mod.Phys.A18:4869-4888,2003 | 10.1142/S0217751X03015313 | MRI-P-020902 | hep-th gr-qc | null | Recent analysis suggests that the classical dynamics of a tachyon on an
unstable D-brane is described by a scalar Born-Infeld type action with a
runaway potential. The classical configurations in this theory at late time are
in one to one correspondence with the configuration of a system of
non-interacting (incoheren... | [
{
"created": "Mon, 16 Sep 2002 09:23:32 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Sen",
"Ashoke",
""
]
] | Recent analysis suggests that the classical dynamics of a tachyon on an unstable D-brane is described by a scalar Born-Infeld type action with a runaway potential. The classical configurations in this theory at late time are in one to one correspondence with the configuration of a system of non-interacting (incoherent)... | 10.762888 | 10.877808 | 11.821785 | 10.024944 | 10.154235 | 11.209653 | 11.529045 | 10.300355 | 10.294669 | 11.604538 | 9.90921 | 9.673508 | 10.624033 | 9.625056 | 10.071448 | 10.154576 | 9.949327 | 9.951116 | 9.744208 | 10.549573 | 9.955501 |
2210.02474 | Pratik Nandy | Budhaditya Bhattacharjee, Pratik Nandy, Tanay Pathak | Krylov complexity in large-$q$ and double-scaled SYK model | v4: minor changes, published version in JHEP | JHEP 08 (2023) 099 | 10.1007/JHEP08(2023)099 | YITP-22-106 | hep-th cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Considering the large-$q$ expansion of the Sachdev-Ye-Kitaev (SYK) model in
the two-stage limit, we compute the Lanczos coefficients, Krylov complexity,
and the higher Krylov cumulants in subleading order, along with the $t/q$
effects. The Krylov complexity naturally describes the "size" of the
distribution, while th... | [
{
"created": "Wed, 5 Oct 2022 18:00:11 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Oct 2022 14:07:11 GMT",
"version": "v2"
},
{
"created": "Mon, 6 Feb 2023 09:44:31 GMT",
"version": "v3"
},
{
"created": "Fri, 18 Aug 2023 02:50:46 GMT",
"version": "v4"
}
] | 2023-08-21 | [
[
"Bhattacharjee",
"Budhaditya",
""
],
[
"Nandy",
"Pratik",
""
],
[
"Pathak",
"Tanay",
""
]
] | Considering the large-$q$ expansion of the Sachdev-Ye-Kitaev (SYK) model in the two-stage limit, we compute the Lanczos coefficients, Krylov complexity, and the higher Krylov cumulants in subleading order, along with the $t/q$ effects. The Krylov complexity naturally describes the "size" of the distribution, while the ... | 9.773739 | 8.795375 | 11.102074 | 8.239024 | 8.558522 | 8.542821 | 8.287157 | 8.468317 | 8.527781 | 10.999671 | 8.594335 | 8.637131 | 9.628306 | 8.787679 | 8.79379 | 8.788169 | 8.637386 | 8.884974 | 8.897345 | 9.687606 | 8.594632 |
hep-th/0211203 | Jose D. Edelstein | J.D. Edelstein, A. Paredes and A.V. Ramallo | Let's Twist Again: General Metrics of G(2) Holonomy from Gauged
Supergravity | 31 pages, latex; v2: minor changes, references added | JHEP 0301 (2003) 011 | 10.1088/1126-6708/2003/01/011 | US-FT-5/02 | hep-th | null | We construct all complete metrics of cohomogeneity one G(2) holonomy with S^3
x S^3 principal orbits from gauged supergravity. Our approach rests on a
generalization of the twisting procedure used in this framework. It corresponds
to a non-trivial embedding of the special Lagrangian three-cycle wrapped by the
D6-bran... | [
{
"created": "Thu, 21 Nov 2002 20:09:15 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Dec 2002 12:26:15 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Edelstein",
"J. D.",
""
],
[
"Paredes",
"A.",
""
],
[
"Ramallo",
"A. V.",
""
]
] | We construct all complete metrics of cohomogeneity one G(2) holonomy with S^3 x S^3 principal orbits from gauged supergravity. Our approach rests on a generalization of the twisting procedure used in this framework. It corresponds to a non-trivial embedding of the special Lagrangian three-cycle wrapped by the D6-branes... | 16.561737 | 13.634357 | 19.262459 | 13.148414 | 14.648234 | 14.775896 | 15.855583 | 13.214543 | 14.279634 | 21.749657 | 12.7668 | 13.770348 | 15.724787 | 13.671242 | 13.456882 | 14.163783 | 14.040806 | 13.469555 | 13.813421 | 15.450433 | 13.710359 |
0812.0871 | Han-Ying Guo | Han-Ying Guo, Chao-Guang Huang, Hong-Tu Wu and Bin Zhou | The Principle of Relativity, Kinematics and Algebraic Relations | 11 pages | Sci. China G53:591-597,2010 | 10.1007/s11433-010-0162-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on the principle of relativity and the postulate on universal invariant
constants (c,l), all possible kinematics can be set up with sub-symmetries of
the Umov-Weyl-Fock transformations for the inertial motions. Further, in the
combinatory approach, all these symmetries are intrinsically related to each
other, e... | [
{
"created": "Thu, 4 Dec 2008 07:17:03 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Dec 2008 09:38:54 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Guo",
"Han-Ying",
""
],
[
"Huang",
"Chao-Guang",
""
],
[
"Wu",
"Hong-Tu",
""
],
[
"Zhou",
"Bin",
""
]
] | Based on the principle of relativity and the postulate on universal invariant constants (c,l), all possible kinematics can be set up with sub-symmetries of the Umov-Weyl-Fock transformations for the inertial motions. Further, in the combinatory approach, all these symmetries are intrinsically related to each other, e.g... | 24.088884 | 24.584633 | 24.748682 | 21.778984 | 22.385954 | 23.750153 | 24.529562 | 24.105444 | 23.970961 | 25.913389 | 23.992569 | 21.630684 | 22.415602 | 22.285217 | 21.333685 | 21.060944 | 22.311167 | 21.823744 | 21.897314 | 23.749916 | 22.100729 |
hep-th/0001037 | Michihiro Naka | Michihiro Naka, Masatoshi Nozaki | Boundary states in Gepner models | 15 pages, no figures, LaTeX, typos corrected, reference added | JHEP 0005 (2000) 027 | 10.1088/1126-6708/2000/05/027 | UT-872 | hep-th | null | We extend the construction of the boundary states in Gepner models to the
non-diagonal modular invariant theories, and derive the same supersymmetric
conditions as the diagonal theories. We also investigate the relation between
the microscopic charges of the boundary states and Ramond charges of the B-type
D-branes o... | [
{
"created": "Sun, 9 Jan 2000 10:36:31 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Feb 2000 12:19:08 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Naka",
"Michihiro",
""
],
[
"Nozaki",
"Masatoshi",
""
]
] | We extend the construction of the boundary states in Gepner models to the non-diagonal modular invariant theories, and derive the same supersymmetric conditions as the diagonal theories. We also investigate the relation between the microscopic charges of the boundary states and Ramond charges of the B-type D-branes on ... | 10.1869 | 8.061444 | 10.827575 | 8.033571 | 9.181427 | 8.057403 | 8.572767 | 7.885965 | 8.187985 | 12.275608 | 7.889631 | 8.727741 | 9.542247 | 9.161295 | 8.784338 | 8.752675 | 9.043816 | 8.832211 | 8.86379 | 9.771845 | 8.613447 |
hep-th/9804071 | Zerbini Sergio | Emilio Elizalde, Antonio Filippi, Luciano Vanzo and Sergio Zerbini | Is the multiplicative anomaly dependent on the regularization ? | 4 pages, LaTex | null | null | Imperial/TP/97-98/37 | hep-th | null | In a recent work, T.S. Evans has claimed that the multiplicative anomaly
associated with the zeta-function regularization of functional determinants is
regularization dependent. We show that, if one makes use of consistent
definitions, this is not the case and clarify some points in Evans' argument.
| [
{
"created": "Thu, 9 Apr 1998 15:37:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Elizalde",
"Emilio",
""
],
[
"Filippi",
"Antonio",
""
],
[
"Vanzo",
"Luciano",
""
],
[
"Zerbini",
"Sergio",
""
]
] | In a recent work, T.S. Evans has claimed that the multiplicative anomaly associated with the zeta-function regularization of functional determinants is regularization dependent. We show that, if one makes use of consistent definitions, this is not the case and clarify some points in Evans' argument. | 12.556272 | 10.552857 | 11.558684 | 10.062141 | 9.503294 | 10.118705 | 11.734565 | 10.162942 | 8.564934 | 13.394732 | 9.716439 | 9.624111 | 10.36247 | 9.250068 | 9.449298 | 9.679091 | 9.974407 | 9.014466 | 9.226012 | 9.89335 | 10.031481 |
hep-th/9703025 | null | A. N. Leznov | Two-dimensional Ultra-Toda integrable mappings and chains (Abelian case) | LaTeX file | Theor.Math.Phys. 117 (1998) 1194-1207; Teor.Mat.Fiz. 117 (1998)
107-122 | null | null | hep-th | null | The new class of integrable mappings and chains is introduced. Corresponding
(1+2) integrable systems invariant with respect to such discrete
transformations are represented in explicit form. Soliton like solutions of
them are represented in terms of matrix elements of fundamental representations
of semisimple A_n al... | [
{
"created": "Tue, 4 Mar 1997 15:06:39 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Leznov",
"A. N.",
""
]
] | The new class of integrable mappings and chains is introduced. Corresponding (1+2) integrable systems invariant with respect to such discrete transformations are represented in explicit form. Soliton like solutions of them are represented in terms of matrix elements of fundamental representations of semisimple A_n alge... | 21.117729 | 20.663681 | 23.047544 | 17.878056 | 21.586411 | 19.655785 | 19.130938 | 19.156717 | 19.104902 | 22.307816 | 18.120935 | 18.743404 | 18.742809 | 17.537889 | 17.996542 | 17.785112 | 18.599417 | 17.860456 | 17.620314 | 18.121662 | 17.044619 |
hep-th/9712133 | Martin B. Halpern | M.B. Halpern (UC Berkeley, LBNL) and C. Schwartz (UC Berkeley) | Asymptotic Search for Ground States of SU(2) Matrix Theory | 51 pages | Int.J.Mod.Phys.A13:4367-4408,1998 | 10.1142/S0217751X98002110 | UCB-PTH-97/63, LBNL-41142 | hep-th | null | We introduce a complete set of gauge-invariant variables and a generalized
Born-Oppenheimer formulation to search for normalizable zero-energy asymptotic
solutions of the Schrodinger equation of SU(2) matrix theory. The asymptotic
method gives only ground state candidates, which must be further tested for
global stab... | [
{
"created": "Mon, 15 Dec 1997 23:34:16 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Halpern",
"M. B.",
"",
"UC Berkeley, LBNL"
],
[
"Schwartz",
"C.",
"",
"UC Berkeley"
]
] | We introduce a complete set of gauge-invariant variables and a generalized Born-Oppenheimer formulation to search for normalizable zero-energy asymptotic solutions of the Schrodinger equation of SU(2) matrix theory. The asymptotic method gives only ground state candidates, which must be further tested for global stabil... | 17.714703 | 18.633923 | 20.454521 | 14.409132 | 16.779995 | 18.084091 | 16.308971 | 16.910517 | 14.682129 | 18.878073 | 16.45013 | 16.533762 | 17.032681 | 16.221233 | 15.421673 | 15.936341 | 16.229246 | 16.053963 | 16.73407 | 17.921234 | 16.571383 |
hep-th/0306127 | Skenderis Kostas | Glenn Barnich, Tobias Hurth and Kostas Skenderis | Comments on the Gauge Fixed BRST Cohomology and the Quantum Noether
Method | 24 pages, example section improved, short version without background
material will appear in Physics Letters B | Phys.Lett.B588:111-118,2004 | 10.1016/j.physletb.2004.03.035 | CERN-TH/2003-127, SLAC-PUB-9929, ULB-TH-03/22, ITFA-2003-30 | hep-th hep-ph | null | We discuss in detail the relation between the gauge fixed and gauge invariant
BRST cohomology. We showed previously that in certain gauges some cohomology
classes of the gauge-fixed BRST differential do not correspond to gauge
invariant observables. We now show that in addition ``accidental'' conserved
currents may a... | [
{
"created": "Fri, 13 Jun 2003 15:06:19 GMT",
"version": "v1"
},
{
"created": "Sun, 15 Jun 2003 16:02:12 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Mar 2004 19:54:35 GMT",
"version": "v3"
}
] | 2011-04-20 | [
[
"Barnich",
"Glenn",
""
],
[
"Hurth",
"Tobias",
""
],
[
"Skenderis",
"Kostas",
""
]
] | We discuss in detail the relation between the gauge fixed and gauge invariant BRST cohomology. We showed previously that in certain gauges some cohomology classes of the gauge-fixed BRST differential do not correspond to gauge invariant observables. We now show that in addition ``accidental'' conserved currents may app... | 9.381206 | 8.849275 | 9.038991 | 8.064978 | 8.345211 | 9.028029 | 8.964511 | 8.787127 | 8.8123 | 9.461032 | 8.186953 | 8.493273 | 8.380864 | 8.202567 | 8.52211 | 8.408202 | 8.489825 | 8.184959 | 8.735374 | 8.686892 | 8.265982 |
2003.11016 | Yifan Wang | Yifan Wang | Taming Defects in $\mathcal{N}=4$ Super-Yang-Mills | 91 pages, 2 figures; v3: minor corrections and more references added | null | 10.1007/JHEP08(2020)021 | PUPT-2608 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study correlation functions involving extended defect operators in the
four-dimensional ${\cal N}=4$ super-Yang-Mills (SYM). The main tool is
supersymmetric localization with respect to the supercharge $\cal Q$ introduced
in \cite{Pestun:2009nn} which computes observables in the $\cal Q$-cohomology.
We classify ge... | [
{
"created": "Tue, 24 Mar 2020 17:59:59 GMT",
"version": "v1"
},
{
"created": "Sat, 23 May 2020 19:59:30 GMT",
"version": "v2"
},
{
"created": "Mon, 14 Dec 2020 21:22:47 GMT",
"version": "v3"
}
] | 2020-12-16 | [
[
"Wang",
"Yifan",
""
]
] | We study correlation functions involving extended defect operators in the four-dimensional ${\cal N}=4$ super-Yang-Mills (SYM). The main tool is supersymmetric localization with respect to the supercharge $\cal Q$ introduced in \cite{Pestun:2009nn} which computes observables in the $\cal Q$-cohomology. We classify gene... | 6.154628 | 6.508014 | 7.109738 | 6.005572 | 6.363787 | 6.32465 | 6.479488 | 6.317656 | 6.151847 | 7.233251 | 5.950225 | 5.964062 | 6.477087 | 6.138828 | 5.945171 | 5.892508 | 6.229287 | 6.049456 | 6.037424 | 6.64901 | 5.997777 |
hep-th/9804085 | Andy Strominger | Juan Maldacena and Andrew Strominger | AdS3 Black Holes and a Stringy Exclusion Principle | 24 pages, harvmac. References added | JHEP 9812:005,1998 | 10.1088/1126-6708/1998/12/005 | null | hep-th | null | The duality relating near-horizon microstates of black holes obtained as
orbifolds of a subset of AdS3 to the states of a conformal field theory is
analyzed in detail. The SL(2,R) invariant vacuum on AdS3 corresponds to the
NS-NS vacuum of the conformal field theory. The effect of the orbifolding is to
produce a dens... | [
{
"created": "Sun, 12 Apr 1998 21:44:54 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Apr 1998 03:32:33 GMT",
"version": "v2"
},
{
"created": "Mon, 11 May 1998 13:42:18 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Maldacena",
"Juan",
""
],
[
"Strominger",
"Andrew",
""
]
] | The duality relating near-horizon microstates of black holes obtained as orbifolds of a subset of AdS3 to the states of a conformal field theory is analyzed in detail. The SL(2,R) invariant vacuum on AdS3 corresponds to the NS-NS vacuum of the conformal field theory. The effect of the orbifolding is to produce a densit... | 8.954012 | 8.360036 | 9.758553 | 8.096784 | 8.45532 | 8.72202 | 8.543526 | 8.129198 | 8.033163 | 9.962522 | 8.484041 | 8.262106 | 8.320291 | 8.332692 | 8.332349 | 8.453843 | 8.26088 | 8.140944 | 8.289297 | 8.337564 | 8.162731 |
1810.05407 | Humberto Gomez | Humberto Gomez | Scattering Equations and a new Factorization for Amplitudes I: Gauge
Theories | 50+7 pages and typos fixed. Some modifications were made to improve
the text | null | 10.1007/JHEP05(2019)128 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we show how a double-cover (DC) extension of the Cachazo, He and
Yuan formalism (CHY) can be used to provide a new realization for the
factorization of the amplitudes involving gluons and scalar fields. First, we
propose a graphic representation for a color-ordered Yang-Mills (YM) and
special Yang-Mills-... | [
{
"created": "Fri, 12 Oct 2018 08:45:00 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Mar 2019 09:57:18 GMT",
"version": "v2"
}
] | 2019-06-26 | [
[
"Gomez",
"Humberto",
""
]
] | In this work we show how a double-cover (DC) extension of the Cachazo, He and Yuan formalism (CHY) can be used to provide a new realization for the factorization of the amplitudes involving gluons and scalar fields. First, we propose a graphic representation for a color-ordered Yang-Mills (YM) and special Yang-Mills-Sc... | 10.470367 | 9.434114 | 11.816876 | 9.809604 | 10.683042 | 10.906487 | 10.35175 | 9.743953 | 9.980536 | 12.468679 | 9.583628 | 9.447965 | 10.509105 | 9.713126 | 9.311663 | 9.263744 | 9.479327 | 9.457908 | 9.915099 | 10.579538 | 9.636659 |
2007.05984 | Greg Kaplanek | Greg Kaplanek and C.P. Burgess | Qubits on the Horizon: Decoherence and Thermalization near Black Holes | 24 pages plus appendix, 2 figures v2) now published in JHEP, typos
fixed and added subsection on the frame independence of the Markovian limit | JHEP 01 (2021) 098 | 10.1007/JHEP01(2021)098 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the late-time evolution of a qubit (or Unruh-De Witt detector)
that hovers very near to the event horizon of a Schwarzschild black hole, while
interacting with a free quantum scalar field. The calculation is carried out
perturbatively in the dimensionless qubit/field coupling $g$, but rather than
computing... | [
{
"created": "Sun, 12 Jul 2020 13:25:11 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Jan 2021 16:22:59 GMT",
"version": "v2"
}
] | 2021-01-21 | [
[
"Kaplanek",
"Greg",
""
],
[
"Burgess",
"C. P.",
""
]
] | We examine the late-time evolution of a qubit (or Unruh-De Witt detector) that hovers very near to the event horizon of a Schwarzschild black hole, while interacting with a free quantum scalar field. The calculation is carried out perturbatively in the dimensionless qubit/field coupling $g$, but rather than computing t... | 6.263827 | 6.957757 | 6.513353 | 6.22225 | 6.783578 | 6.487759 | 7.235971 | 6.554933 | 6.612341 | 7.507005 | 6.097933 | 6.275867 | 6.389747 | 6.302484 | 6.202969 | 6.045995 | 6.178566 | 6.328179 | 6.13759 | 6.22431 | 6.135929 |
1608.06223 | Alessio Notari | Alessio Notari, Konrad Tywoniuk | Dissipative Axial Inflation | 22 pages, 27 figures | null | 10.1088/1475-7516/2016/12/038 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze in detail the background cosmological evolution of a scalar field
coupled to a massless abelian gauge field through an axial term
$\frac{\phi}{f_\gamma} F \tilde{F}$, such as in the case of an axion. Gauge
fields in this case are known to experience tachyonic growth and therefore can
backreact on the backg... | [
{
"created": "Mon, 22 Aug 2016 16:52:13 GMT",
"version": "v1"
}
] | 2016-12-28 | [
[
"Notari",
"Alessio",
""
],
[
"Tywoniuk",
"Konrad",
""
]
] | We analyze in detail the background cosmological evolution of a scalar field coupled to a massless abelian gauge field through an axial term $\frac{\phi}{f_\gamma} F \tilde{F}$, such as in the case of an axion. Gauge fields in this case are known to experience tachyonic growth and therefore can backreact on the backgro... | 7.443816 | 8.791838 | 8.887624 | 8.539416 | 8.783481 | 9.252207 | 8.932771 | 8.833114 | 8.413765 | 9.21914 | 8.480927 | 7.850292 | 7.7304 | 7.823351 | 7.839333 | 7.776267 | 7.76129 | 7.789887 | 7.74048 | 7.986109 | 7.855688 |
1104.1793 | Konstantin Zarembo | D. Sorokin, A. Tseytlin, L. Wulff and K. Zarembo | Superstrings in AdS(2)xS(2)xT(6) | 49 pages, 1 figure; v2: misprints corrected, references added | null | 10.1088/1751-8113/44/27/275401 | MIFPA-11-11, NORDITA-2011-30, Imperial-TP-AT-2011-2 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the type IIB Green-Schwarz superstring theory on AdS(2)xS(2)xT(6)
supported by homogeneous Ramond-Ramond 5-form flux and its type IIA T-duals.
One motivation is to understand the solution of this theory based on
integrability. This background is a limit of a 1/4 supersymmetric supergravity
solution descri... | [
{
"created": "Sun, 10 Apr 2011 18:39:28 GMT",
"version": "v1"
},
{
"created": "Thu, 19 May 2011 14:26:50 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Sorokin",
"D.",
""
],
[
"Tseytlin",
"A.",
""
],
[
"Wulff",
"L.",
""
],
[
"Zarembo",
"K.",
""
]
] | We consider the type IIB Green-Schwarz superstring theory on AdS(2)xS(2)xT(6) supported by homogeneous Ramond-Ramond 5-form flux and its type IIA T-duals. One motivation is to understand the solution of this theory based on integrability. This background is a limit of a 1/4 supersymmetric supergravity solution describi... | 5.854389 | 5.393787 | 6.676649 | 5.685863 | 5.917588 | 5.8709 | 5.561563 | 5.273726 | 5.655363 | 7.284744 | 5.617394 | 5.756397 | 6.403018 | 5.73846 | 5.696197 | 5.638058 | 5.676732 | 5.879816 | 5.816883 | 6.166248 | 5.616599 |
1904.11445 | Blaise Gout\'eraux | Andrea Amoretti, Daniel Are\'an, Blaise Gout\'eraux and Daniele Musso | Diffusion and universal relaxation of holographic phonons | v3: Typos fixed, discussion improved, version published in JHEP. v2:
minor typos fixed, references added. v1: 24 pages plus appendices, contains
an extended discussion of parts of arXiv:1812.08118 as well as new material | null | 10.1007/JHEP10(2019)068 | CPHT-RR018.042019;IFT-UAM/CSIC-19-55 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In phases where translations are spontaneously broken, new gapless degrees of
freedom appear in the low energy spectrum (the phonons). At long wavelengths,
they couple to small fluctuations of the conserved densities of the system.
This mixing is captured by new diffusive transport coefficients, as well as
qualitativ... | [
{
"created": "Thu, 25 Apr 2019 16:41:03 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jul 2019 10:49:18 GMT",
"version": "v2"
},
{
"created": "Mon, 30 Sep 2019 10:55:30 GMT",
"version": "v3"
}
] | 2020-01-08 | [
[
"Amoretti",
"Andrea",
""
],
[
"Areán",
"Daniel",
""
],
[
"Goutéraux",
"Blaise",
""
],
[
"Musso",
"Daniele",
""
]
] | In phases where translations are spontaneously broken, new gapless degrees of freedom appear in the low energy spectrum (the phonons). At long wavelengths, they couple to small fluctuations of the conserved densities of the system. This mixing is captured by new diffusive transport coefficients, as well as qualitativel... | 12.96642 | 10.856914 | 12.844098 | 10.99429 | 11.00089 | 10.267733 | 10.596279 | 11.182444 | 10.816387 | 13.11557 | 10.279642 | 10.66622 | 11.391222 | 10.57146 | 10.544393 | 10.73529 | 10.324751 | 10.270721 | 10.699445 | 10.654195 | 10.6893 |
hep-th/0504030 | Alexander Machavariani | A. I. Machavariani | Conformal group of transformations of the quantum field operators in the
momentum space and the five dimensional Lagrangian approach | LATEX, 33 pages | null | null | null | hep-th | null | Conformal group of transformations in the momentum space, consisting of
translations $p'_{\mu}=p_{\mu}+h_{\mu}$, rotations
$p'_{\mu}=\Lambda^{\nu}_{\mu}p_{\nu}$, dilatation $p'_{\mu}=\lambda p_{\mu}$
and inversion $p'_{\mu}= -M^2p_{\mu}/p^2$ of the four-momentum $p_{\mu}$, is
used for the five dimensional generalizat... | [
{
"created": "Mon, 4 Apr 2005 17:50:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Machavariani",
"A. I.",
""
]
] | Conformal group of transformations in the momentum space, consisting of translations $p'_{\mu}=p_{\mu}+h_{\mu}$, rotations $p'_{\mu}=\Lambda^{\nu}_{\mu}p_{\nu}$, dilatation $p'_{\mu}=\lambda p_{\mu}$ and inversion $p'_{\mu}= -M^2p_{\mu}/p^2$ of the four-momentum $p_{\mu}$, is used for the five dimensional generalizatio... | 5.351194 | 5.401145 | 5.14637 | 5.072384 | 5.599971 | 5.428654 | 5.414189 | 4.93303 | 5.164568 | 5.415668 | 5.168722 | 5.065279 | 5.035704 | 5.035678 | 4.973388 | 5.145261 | 5.026689 | 5.005405 | 5.055683 | 4.928134 | 4.997409 |
hep-th/0012182 | Masashi Naganuma | Kenji Ito, Masashi Naganuma, Hodaka Oda, Norisuke Sakai | An Exact Solution of BPS Junctions and Its Properties | LaTeX file, 10 page, 3 eps figure; uses espcrc2.sty (twocolumn). Talk
presented by N. Sakai at the SUSY 30 workshop in Minnesota, October 16-27,
2000. To appear in Nuclear Physics B (Proceedings Supplement). References
added | Nucl.Phys.Proc.Suppl. 101 (2001) 304-313 | 10.1016/S0920-5632(01)01515-8 | TIT/HEP 460 | hep-th hep-ph | null | We have obtained an exact solution for the BPS domain wall junction for a N=1
supersymmetric theory in four dimensions and studied its properties. The model
is a simplified version of the N=2 SU(2) gauge theory with N_f=1 broken to N=1
by the mass of the adjoint chiral superfield. We define mode equations and
demonst... | [
{
"created": "Wed, 20 Dec 2000 03:11:06 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Dec 2000 04:52:48 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Ito",
"Kenji",
""
],
[
"Naganuma",
"Masashi",
""
],
[
"Oda",
"Hodaka",
""
],
[
"Sakai",
"Norisuke",
""
]
] | We have obtained an exact solution for the BPS domain wall junction for a N=1 supersymmetric theory in four dimensions and studied its properties. The model is a simplified version of the N=2 SU(2) gauge theory with N_f=1 broken to N=1 by the mass of the adjoint chiral superfield. We define mode equations and demonstra... | 8.508959 | 7.31652 | 9.713495 | 8.113066 | 9.286179 | 7.779607 | 8.006606 | 7.957594 | 7.891492 | 10.365652 | 8.055918 | 8.286375 | 8.993418 | 8.336187 | 8.366143 | 8.325889 | 8.19964 | 8.31016 | 8.28792 | 9.133268 | 8.182788 |
1112.1323 | She-Sheng Xue | She-Sheng Xue | The phase and critical point of quantum Einstein-Cartan gravity | 15 pages, 7 figures, the version to appear in Phys. Lett. B. We have
clarified that Eqs. (E.5) and (E.6) of Phys. Rev. D82 (2010) 064039 were
obtained by using the strong coupling expansion in terms of (M^2_h/8g^2) =
0.1 | null | 10.1016/j.physletb.2012.04.024 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By introducing diffeomorphism and local Lorentz gauge invariant holonomy
fields, we study in the recent article [S.-S. Xue, Phys. Rev. D82 (2010)
064039] the quantum Einstein-Cartan gravity in the framework of Regge calculus.
On the basis of strong coupling expansion, mean-field approximation and
dynamical equations ... | [
{
"created": "Sat, 3 Dec 2011 19:34:08 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Feb 2012 15:40:35 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Apr 2012 17:19:40 GMT",
"version": "v3"
}
] | 2015-06-03 | [
[
"Xue",
"She-Sheng",
""
]
] | By introducing diffeomorphism and local Lorentz gauge invariant holonomy fields, we study in the recent article [S.-S. Xue, Phys. Rev. D82 (2010) 064039] the quantum Einstein-Cartan gravity in the framework of Regge calculus. On the basis of strong coupling expansion, mean-field approximation and dynamical equations sa... | 8.370846 | 8.714192 | 8.957958 | 8.350169 | 9.191737 | 8.75416 | 8.599648 | 8.55753 | 8.062072 | 9.765316 | 7.930814 | 8.127652 | 8.136337 | 7.688021 | 8.123522 | 8.114155 | 7.949704 | 8.13398 | 8.012956 | 8.036309 | 7.873507 |
hep-th/9605029 | Jose N. Pecina-Cruz | Carlos Castro ( University of Texas at Austin ) | On the Exact Quantum Integrability of the Membrane | 35 pages; Revised Tex file; some minor details have been added | null | null | null | hep-th | null | The exact quantum integrability problem of the membrane is investigated. It
is found that the spherical membrane moving in flat target spacetime
backgrounds is an exact quantum integrable system for a particular class of
solutions of the light-cone gauge equations of motion : a dimensionally-reduced
$SU(\infty)$ Yang... | [
{
"created": "Mon, 6 May 1996 02:03:31 GMT",
"version": "v1"
},
{
"created": "Fri, 17 May 1996 02:16:13 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Castro",
"Carlos",
"",
"University of Texas at Austin"
]
] | The exact quantum integrability problem of the membrane is investigated. It is found that the spherical membrane moving in flat target spacetime backgrounds is an exact quantum integrable system for a particular class of solutions of the light-cone gauge equations of motion : a dimensionally-reduced $SU(\infty)$ Yang-M... | 11.515467 | 10.21872 | 12.659611 | 10.886042 | 10.652683 | 10.654901 | 11.114323 | 10.856456 | 10.302502 | 14.296397 | 10.586825 | 10.979354 | 11.659914 | 10.79875 | 10.949955 | 11.043159 | 10.877274 | 10.692977 | 10.973955 | 11.279646 | 11.12764 |
1910.09866 | Yakov Shnir | Ilya Perapechka and Yakov Shnir | Kinks bounded by fermions | 5 pages, 4 figures | Phys. Rev. D 101, 021701 (2020) | 10.1103/PhysRevD.101.021701 | null | hep-th nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present and study new mechanism of interaction between the solitons based
on the exchange interaction mediated by the localized fermion states. As
particular examples, we consider solutions of simple 1+1 dimensional scalar
field theories with self-interaction potentials, including sine-Gordon model
and the polynom... | [
{
"created": "Tue, 22 Oct 2019 09:55:48 GMT",
"version": "v1"
}
] | 2020-02-05 | [
[
"Perapechka",
"Ilya",
""
],
[
"Shnir",
"Yakov",
""
]
] | We present and study new mechanism of interaction between the solitons based on the exchange interaction mediated by the localized fermion states. As particular examples, we consider solutions of simple 1+1 dimensional scalar field theories with self-interaction potentials, including sine-Gordon model and the polynomia... | 10.26962 | 8.90844 | 9.531831 | 9.039662 | 9.032677 | 8.35944 | 8.672985 | 8.600082 | 9.034124 | 9.445786 | 8.7098 | 9.072531 | 9.278048 | 8.761398 | 8.995005 | 9.101067 | 8.876451 | 9.024517 | 9.119463 | 9.08831 | 8.745218 |
hep-th/0501140 | Roberto Trinchero | Roberto Trinchero | Quantum symmetries of faces models and the double triangle algebra | 28 pages, 4 figures, new typesetting and a few corrections | Adv.Theor.Math.Phys.10:49-75,2006 | null | null | hep-th math-ph math.MP math.QA | null | Symmetries of trigonometric integrable two dimensional statistical face
models are considered. The corresponding symmetry operators on the Hilbert
space of states of the quantum version of these models define a weak *-Hopf
algebra isomorphic to the Ocneanu double triangle algebra.
| [
{
"created": "Tue, 18 Jan 2005 20:38:58 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Mar 2006 18:41:31 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Trinchero",
"Roberto",
""
]
] | Symmetries of trigonometric integrable two dimensional statistical face models are considered. The corresponding symmetry operators on the Hilbert space of states of the quantum version of these models define a weak *-Hopf algebra isomorphic to the Ocneanu double triangle algebra. | 18.058847 | 16.921858 | 21.685383 | 19.205353 | 19.962257 | 18.92837 | 18.979521 | 14.140949 | 16.834126 | 20.546284 | 16.498232 | 17.526617 | 16.050823 | 15.229727 | 16.955252 | 16.183647 | 17.7934 | 17.599451 | 15.575407 | 15.980409 | 18.251139 |
1606.06306 | Dan Xie | Yifan Wang, Dan Xie, Stephen S.-T. Yau, Shing-Tung Yau | 4d N=2 SCFT from Complete Intersection Singularity | 46 pages, 85 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Detailed studies of four dimensional N=2 superconformal field theories (SCFT)
defined by isolated complete intersection singularities are performed: we
compute the Coulomb branch spectrum, Seiberg-Witten solutions and central
charges. Most of our theories have exactly marginal deformations and we
identify the weakly ... | [
{
"created": "Mon, 20 Jun 2016 20:04:02 GMT",
"version": "v1"
}
] | 2016-06-22 | [
[
"Wang",
"Yifan",
""
],
[
"Xie",
"Dan",
""
],
[
"Yau",
"Stephen S. -T.",
""
],
[
"Yau",
"Shing-Tung",
""
]
] | Detailed studies of four dimensional N=2 superconformal field theories (SCFT) defined by isolated complete intersection singularities are performed: we compute the Coulomb branch spectrum, Seiberg-Witten solutions and central charges. Most of our theories have exactly marginal deformations and we identify the weakly co... | 8.188987 | 8.207076 | 11.652841 | 8.215959 | 8.259759 | 8.260802 | 9.016463 | 7.880457 | 8.053443 | 12.930261 | 7.885028 | 7.858483 | 9.206456 | 7.84195 | 7.839533 | 7.966228 | 7.965381 | 7.775696 | 7.589818 | 8.860904 | 7.734997 |
0710.5339 | Toshio Nakatsu | Toshio Nakatsu and Kanehisa Takasaki | Melting Crystal, Quantum Torus and Toda Hierarchy | Final version to be published in Commun. Math. Phys. . A new section
is added and devoted to Conclusion and discussion, where, in particular, a
possible relation with the generating function of the absolute Gromov-Witten
invariants on CP^1 is commented. Two references are added. Typos are
corrected. 32 pages. 4... | Commun.Math.Phys.285:445-468,2009 | 10.1007/s00220-008-0583-5 | null | hep-th math-ph math.MP math.QA nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Searching for the integrable structures of supersymmetric gauge theories and
topological strings, we study melting crystal, which is known as random plane
partition, from the viewpoint of integrable systems. We show that a series of
partition functions of melting crystals gives rise to a tau function of the
one-dimen... | [
{
"created": "Mon, 29 Oct 2007 06:07:24 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jun 2008 06:53:32 GMT",
"version": "v2"
}
] | 2008-12-18 | [
[
"Nakatsu",
"Toshio",
""
],
[
"Takasaki",
"Kanehisa",
""
]
] | Searching for the integrable structures of supersymmetric gauge theories and topological strings, we study melting crystal, which is known as random plane partition, from the viewpoint of integrable systems. We show that a series of partition functions of melting crystals gives rise to a tau function of the one-dimensi... | 10.04222 | 10.521906 | 12.856825 | 10.31604 | 10.317671 | 9.933094 | 11.247252 | 10.64359 | 9.960762 | 14.18695 | 10.357867 | 9.711513 | 11.257773 | 9.903041 | 9.854875 | 9.860373 | 10.193706 | 10.136486 | 9.870382 | 11.006035 | 10.068515 |
1712.02351 | Hongbin Chen | Hongbin Chen, A. Liam Fitzpatrick, Jared Kaplan, Daliang Li | The AdS$_3$ Propagator and the Fate of Locality | 42+17 pages, 7 figures | null | 10.1007/JHEP04(2018)075 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We recently used Virasoro symmetry considerations to propose an exact formula
for a bulk proto-field $\phi$ in AdS$_3$. In this paper we study the propagator
$\langle \phi \phi \rangle$. We show that many techniques from the study of
conformal blocks can be generalized to compute it, including the semiclassical
monod... | [
{
"created": "Wed, 6 Dec 2017 19:00:01 GMT",
"version": "v1"
}
] | 2018-05-23 | [
[
"Chen",
"Hongbin",
""
],
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Kaplan",
"Jared",
""
],
[
"Li",
"Daliang",
""
]
] | We recently used Virasoro symmetry considerations to propose an exact formula for a bulk proto-field $\phi$ in AdS$_3$. In this paper we study the propagator $\langle \phi \phi \rangle$. We show that many techniques from the study of conformal blocks can be generalized to compute it, including the semiclassical monodro... | 8.872811 | 9.916681 | 10.992028 | 9.191037 | 9.784246 | 8.988704 | 9.172717 | 9.209208 | 9.024831 | 11.503497 | 8.921891 | 8.56583 | 9.18794 | 8.451769 | 8.865534 | 8.628268 | 8.298934 | 8.613739 | 8.569579 | 9.177186 | 8.667563 |
hep-th/9303128 | null | Christian Grosche | Path Integration Via Summation of Perturbation Expansions and
Applications to Totally Reflecting Boundaries, and Potential Steps | 8 pages, AmSTeX, SISSA/46/93/FM | Phys.Rev.Lett. 71 (1993) 1-4 | 10.1103/PhysRevLett.71.1 | null | hep-th | null | The path integral for the propagator is expanded into a perturbation series,
which can be exactly summed in the case of $\delta$-function perturbations
giving a closed expression for the (energy-dependent) Green function. Making
the strength of the $\delta$-function perturbation infinite repulsive, produces
a totally... | [
{
"created": "Tue, 23 Mar 1993 15:18:59 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Grosche",
"Christian",
""
]
] | The path integral for the propagator is expanded into a perturbation series, which can be exactly summed in the case of $\delta$-function perturbations giving a closed expression for the (energy-dependent) Green function. Making the strength of the $\delta$-function perturbation infinite repulsive, produces a totally r... | 13.415532 | 13.713818 | 14.830538 | 13.038569 | 14.349248 | 12.149961 | 12.68926 | 12.467298 | 12.513398 | 15.786269 | 12.39918 | 12.201645 | 13.25266 | 12.518032 | 12.635809 | 12.591866 | 12.843598 | 12.50887 | 12.971274 | 13.124811 | 12.507868 |
1003.3278 | Christopher Herzog | Christopher P. Herzog | An Analytic Holographic Superconductor | 20 pages; v2 ref, comment about non-mean field exponents added; v3
several typos fixed | Phys.Rev.D81:126009,2010 | 10.1103/PhysRevD.81.126009 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a holographic superconductor that admits an analytic treatment
near the phase transition. In the dual 3+1 dimensional field theory, the phase
transition occurs when a scalar operator of scaling dimension two gets a vacuum
expectation value. We calculate current-current correlation functions along
with ... | [
{
"created": "Wed, 17 Mar 2010 00:59:37 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Apr 2010 15:28:28 GMT",
"version": "v2"
},
{
"created": "Sun, 16 Jan 2011 14:43:07 GMT",
"version": "v3"
}
] | 2011-01-18 | [
[
"Herzog",
"Christopher P.",
""
]
] | We investigate a holographic superconductor that admits an analytic treatment near the phase transition. In the dual 3+1 dimensional field theory, the phase transition occurs when a scalar operator of scaling dimension two gets a vacuum expectation value. We calculate current-current correlation functions along with th... | 11.558029 | 11.885786 | 11.410744 | 10.674907 | 12.083617 | 11.863149 | 10.725805 | 11.01532 | 10.648344 | 13.651129 | 10.957623 | 11.00963 | 11.574328 | 11.41798 | 11.155126 | 11.633886 | 11.000386 | 11.221012 | 11.413121 | 11.692595 | 10.901795 |
hep-th/9810170 | Gordon W. Semenoff | J. Ambj{\o}rn, Yu. M. Makeenko and G. W. Semenoff | Thermodynamics of D0-branes in matrix theory | 13 pages, 1 figure | Phys.Lett. B445 (1999) 307-315 | 10.1016/S0370-2693(98)01434-8 | null | hep-th | null | We examine the matrix theory representation of D0-brane dynamics at finite
temperature. In this case, violation of supersymmetry by temperature leads to a
non-trivial static potential between D0-branes at any finite temperature. We
compute the static potential in the 1-loop approximation and show that it is
short-ran... | [
{
"created": "Thu, 22 Oct 1998 06:56:19 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Ambjørn",
"J.",
""
],
[
"Makeenko",
"Yu. M.",
""
],
[
"Semenoff",
"G. W.",
""
]
] | We examine the matrix theory representation of D0-brane dynamics at finite temperature. In this case, violation of supersymmetry by temperature leads to a non-trivial static potential between D0-branes at any finite temperature. We compute the static potential in the 1-loop approximation and show that it is short-range... | 9.990587 | 9.31642 | 9.678232 | 8.707914 | 9.601843 | 9.432648 | 8.82929 | 8.912884 | 8.589839 | 9.976881 | 8.63619 | 8.740788 | 9.534996 | 9.235552 | 8.841411 | 9.175598 | 8.75713 | 8.979784 | 9.075705 | 9.649844 | 8.72734 |
hep-th/0108199 | Andrey Bytsenko | A.A. Bytsenko, M.C. Falleiros, A.E. Goncalves and Z.G. Kuznetsova | Determinant Line Bundles and Topological Invariants of Hyperbolic
Geometry - Expository Remarks | 10 pages. To appear in G@C, special issue devoted to QG, Unified
Models and Strings, to mark 100th Anniversary of Tomsk State Pedagogical
University. Editor - S.D. Odintsov | Grav.Cosmol. 8 (2002) 91-95 | 10.1142/S0217751X02010352 | null | hep-th | null | We give some remarks on twisted determinant line bundles and Chern-Simons
topological invariants associated with real hyperbolic manifolds. Index of a
twisted Dirac operator is derived. We discuss briefly application of obtained
results in topological quantum field theory.
| [
{
"created": "Mon, 27 Aug 2001 16:34:58 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Bytsenko",
"A. A.",
""
],
[
"Falleiros",
"M. C.",
""
],
[
"Goncalves",
"A. E.",
""
],
[
"Kuznetsova",
"Z. G.",
""
]
] | We give some remarks on twisted determinant line bundles and Chern-Simons topological invariants associated with real hyperbolic manifolds. Index of a twisted Dirac operator is derived. We discuss briefly application of obtained results in topological quantum field theory. | 15.117395 | 13.760145 | 12.64198 | 12.041666 | 12.904896 | 14.456582 | 12.629788 | 13.326961 | 12.745186 | 15.38902 | 11.658415 | 13.709879 | 12.952874 | 13.127925 | 12.961054 | 13.271369 | 12.927036 | 13.339881 | 13.00583 | 13.41118 | 13.625185 |
hep-th/0211226 | David Hasler | David Hasler, Jens Hoppe | Zero Energy States of Reduced Super Yang-Mills Theories in $d+1 = 4,6$
and 10 dimensions are necessarily $Spin(d)$ invariant | null | null | null | null | hep-th | null | We consider reduced Super Yang-Mills Theory in $d+1$ dimensions, where
$d=2,3,5,9$. We present commutators to prove that for $d=3,5$ and 9 a possible
ground state must be a $Spin(d)$ singlet. We also discuss the case $d=2$, where
we give an upper bound on the total angular momentum and show that for odd
dimensional g... | [
{
"created": "Sat, 23 Nov 2002 19:49:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Hasler",
"David",
""
],
[
"Hoppe",
"Jens",
""
]
] | We consider reduced Super Yang-Mills Theory in $d+1$ dimensions, where $d=2,3,5,9$. We present commutators to prove that for $d=3,5$ and 9 a possible ground state must be a $Spin(d)$ singlet. We also discuss the case $d=2$, where we give an upper bound on the total angular momentum and show that for odd dimensional gau... | 8.902787 | 9.002147 | 9.043549 | 8.112249 | 8.697216 | 8.858922 | 8.205755 | 8.265962 | 8.268393 | 9.399187 | 8.279199 | 7.86668 | 8.663522 | 8.464777 | 8.237125 | 8.259091 | 8.342668 | 8.774579 | 8.27241 | 8.551129 | 8.215014 |
1004.2346 | Levay Peter | P\'eter L\'evay and Szil\'ard Szalay | The attractor mechanism as a distillation procedure | 38 pages LaTex | Phys.Rev.D82:026002,2010 | 10.1103/PhysRevD.82.026002 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a recent paper it has been shown that for double extremal static
spherically symmetric BPS black hole solutions in the STU model the well-known
process of moduli stabilization at the horizon can be recast in a form of a
distillation procedure of a three-qubit entangled state of GHZ-type. By
studying the full flow ... | [
{
"created": "Wed, 14 Apr 2010 08:08:00 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Lévay",
"Péter",
""
],
[
"Szalay",
"Szilárd",
""
]
] | In a recent paper it has been shown that for double extremal static spherically symmetric BPS black hole solutions in the STU model the well-known process of moduli stabilization at the horizon can be recast in a form of a distillation procedure of a three-qubit entangled state of GHZ-type. By studying the full flow in... | 11.438813 | 12.326412 | 12.762183 | 11.223042 | 11.595114 | 11.889649 | 12.069428 | 11.7567 | 11.32273 | 14.020353 | 11.557497 | 11.162713 | 11.656228 | 11.167246 | 11.382854 | 11.051131 | 11.229539 | 11.034593 | 11.103959 | 12.043161 | 11.163309 |
2212.13968 | Alexander A. Voronov | Hisham Sati, Alexander A. Voronov | Mysterious Triality and M-Theory | 69 pages. This is an updated version, which takes into account
corrections and improvements of the final version of the mathematical
companion paper arXiv:2111.14810 [hep-th] | null | null | IPMU23-0001 | hep-th math.AG math.AT math.QA | http://creativecommons.org/licenses/by/4.0/ | In a previous paper, we introduced Mysterious Triality as an extension, via
algebraic topology in the form of rational homotopy theory, of Mysterious
Duality by Iqbal, Neitzke, and Vafa, which provides connections between
physics, in the form of dimensional reduction of M-theory, and algebraic
geometry, in the form o... | [
{
"created": "Wed, 28 Dec 2022 17:28:25 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Jan 2023 18:39:36 GMT",
"version": "v2"
}
] | 2023-01-10 | [
[
"Sati",
"Hisham",
""
],
[
"Voronov",
"Alexander A.",
""
]
] | In a previous paper, we introduced Mysterious Triality as an extension, via algebraic topology in the form of rational homotopy theory, of Mysterious Duality by Iqbal, Neitzke, and Vafa, which provides connections between physics, in the form of dimensional reduction of M-theory, and algebraic geometry, in the form of ... | 9.265695 | 8.951971 | 11.125587 | 9.02858 | 9.286536 | 9.642076 | 9.592274 | 8.749613 | 8.950968 | 11.933634 | 9.20659 | 9.0465 | 9.644922 | 8.926047 | 8.973276 | 9.093695 | 8.904146 | 8.910851 | 9.302559 | 9.566187 | 9.103804 |
hep-th/0107168 | Dimitra Karabali | Dimitra Karabali and Bunji Sakita | Orthogonal basis for the energy eigenfunctions of the Chern-Simons
matrix model | 11 pages, LaTeX, minor typo corrections, section 6 slightly extended
to include more information on Jack polynomials | Phys.Rev. B65 (2002) 075304 | 10.1103/PhysRevB.65.075304 | CCNY-HEP 01/06 | hep-th cond-mat.mes-hall | null | We study the spectrum of the Chern-Simons matrix model and identify an
orthogonal set of states. The connection to the spectrum of the Calogero model
is discussed.
| [
{
"created": "Fri, 20 Jul 2001 00:56:27 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Dec 2001 04:23:27 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Karabali",
"Dimitra",
""
],
[
"Sakita",
"Bunji",
""
]
] | We study the spectrum of the Chern-Simons matrix model and identify an orthogonal set of states. The connection to the spectrum of the Calogero model is discussed. | 11.407442 | 7.502181 | 9.257613 | 7.61682 | 7.296067 | 7.308971 | 7.921909 | 7.28106 | 7.858029 | 10.431145 | 8.322612 | 8.755112 | 9.804153 | 8.409643 | 8.38057 | 8.283372 | 8.509715 | 8.869303 | 8.586944 | 10.087001 | 8.759817 |
0805.4819 | Hernando Quevedo | H. Quevedo, A. Sanchez and A. Vazquez | Thermodynamic systems as bosonic strings | New references, comments and corrections added | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply variational principles in the context of geometrothermodynamics. The
thermodynamic phase space ${\cal T}$ and the space of equilibrium states ${\cal
E}$ turn out to be described by Riemannian metrics which are invariant with
respect to Legendre transformations and satisfy the differential equations
following... | [
{
"created": "Fri, 30 May 2008 18:01:53 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Nov 2008 05:37:40 GMT",
"version": "v2"
},
{
"created": "Sun, 14 Dec 2008 22:20:26 GMT",
"version": "v3"
},
{
"created": "Wed, 11 Feb 2009 01:58:51 GMT",
"version": "v4"
},
{
"cr... | 2009-09-09 | [
[
"Quevedo",
"H.",
""
],
[
"Sanchez",
"A.",
""
],
[
"Vazquez",
"A.",
""
]
] | We apply variational principles in the context of geometrothermodynamics. The thermodynamic phase space ${\cal T}$ and the space of equilibrium states ${\cal E}$ turn out to be described by Riemannian metrics which are invariant with respect to Legendre transformations and satisfy the differential equations following f... | 7.34579 | 8.166436 | 7.412374 | 7.22419 | 7.378575 | 8.145903 | 7.734736 | 6.969552 | 7.535432 | 7.518597 | 7.103387 | 7.17546 | 7.158876 | 7.412123 | 7.252836 | 7.180536 | 7.125908 | 7.068738 | 7.411962 | 7.315267 | 7.052647 |
1207.0222 | Markus Huber Q. | Markus Q. Huber, Axel Maas, Lorenz von Smekal | Two- and three-point functions in two-dimensional Landau-gauge
Yang-Mills theory: Continuum results | 24 pages; added references, improved choices of parameters for vertex
models; identical to version published in JHEP | JHEP11(2012)035 | 10.1007/JHEP11(2012)035 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the Dyson-Schwinger equations for the gluon and ghost
propagators and the ghost-gluon vertex of Landau-gauge gluodynamics in two
dimensions. While this simplifies some aspects of the calculations as compared
to three and four dimensions, new complications arise due to a mixing of
different momentum reg... | [
{
"created": "Sun, 1 Jul 2012 15:51:07 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Nov 2012 11:56:26 GMT",
"version": "v2"
}
] | 2012-11-20 | [
[
"Huber",
"Markus Q.",
""
],
[
"Maas",
"Axel",
""
],
[
"von Smekal",
"Lorenz",
""
]
] | We investigate the Dyson-Schwinger equations for the gluon and ghost propagators and the ghost-gluon vertex of Landau-gauge gluodynamics in two dimensions. While this simplifies some aspects of the calculations as compared to three and four dimensions, new complications arise due to a mixing of different momentum regim... | 8.646848 | 9.570067 | 8.512569 | 8.564733 | 9.075862 | 9.280627 | 9.49054 | 8.988716 | 8.463463 | 9.316035 | 8.587455 | 8.492375 | 8.549386 | 8.621826 | 8.234017 | 8.591383 | 8.6453 | 8.546457 | 8.373201 | 8.763751 | 8.373784 |
hep-th/9701048 | Dudas | E. Dudas and J. Mourad | On the strongly coupled heterotic string | Latex, 14 pages, Misprints corrected | Phys.Lett. B400 (1997) 71-79 | 10.1016/S0370-2693(97)00335-3 | LPTHE-Orsay 96/104,GPS 96/110 | hep-th | null | We analyze in detail the anomaly cancellation conditions for the strongly
coupled $E_8 \times E_8$ heterotic string introduced by Horava and Witten and
find new features compared to the ten-dimensional Green-Schwarz mechanism. We
project onto ten dimensions the corresponding Lagrangian of the zero-mode
fields. We fin... | [
{
"created": "Mon, 13 Jan 1997 18:46:58 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Feb 1997 15:08:18 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Dudas",
"E.",
""
],
[
"Mourad",
"J.",
""
]
] | We analyze in detail the anomaly cancellation conditions for the strongly coupled $E_8 \times E_8$ heterotic string introduced by Horava and Witten and find new features compared to the ten-dimensional Green-Schwarz mechanism. We project onto ten dimensions the corresponding Lagrangian of the zero-mode fields. We find ... | 12.152515 | 12.425242 | 12.290944 | 11.444419 | 11.653677 | 10.792737 | 11.699341 | 10.870502 | 10.751296 | 12.889684 | 10.895912 | 11.079339 | 11.399358 | 11.151291 | 10.877572 | 11.367903 | 11.297202 | 11.412801 | 10.863636 | 11.332049 | 11.232106 |
1406.5124 | Eric D'Hoker | Eric D'Hoker and Michael Gutperle | Holographic Entropy and Calabi's Diastasis | 34 pages, 3 figures | null | 10.1007/JHEP10(2014)093 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The entanglement entropy for interfaces and junctions of two-dimensional CFTs
is evaluated on holographically dual half-BPS solutions to six-dimensional Type
4b supergravity with m anti-symmetric tensor supermultiplets. It is shown that
the moduli space for an N-junction solution projects to N points in the Kaehler
m... | [
{
"created": "Thu, 19 Jun 2014 17:46:26 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"D'Hoker",
"Eric",
""
],
[
"Gutperle",
"Michael",
""
]
] | The entanglement entropy for interfaces and junctions of two-dimensional CFTs is evaluated on holographically dual half-BPS solutions to six-dimensional Type 4b supergravity with m anti-symmetric tensor supermultiplets. It is shown that the moduli space for an N-junction solution projects to N points in the Kaehler man... | 10.074354 | 10.220622 | 11.880219 | 9.52899 | 9.621424 | 9.637207 | 10.331214 | 9.560608 | 9.553237 | 13.488348 | 9.536982 | 9.373378 | 10.215347 | 9.292627 | 9.528988 | 9.391773 | 9.541227 | 9.23483 | 9.379071 | 10.787147 | 9.393329 |
1910.00198 | Stepan Sidorov Dr. | Stepan Sidorov | Hidden Supersymmetries of Deformed Supersymmetric Mechanics | 10 pages, 3 figures. To appear in the Proceedings of the
International Conference on Integrable Systems and Quantum Symmetries
(ISQS26), 8-12 July 2019, Prague | null | 10.1088/1742-6596/1416/1/012032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider quantum models corresponding to superymmetrizations of the
two-dimensional harmonic oscillator based on worldline $d=1$ realizations of
the supergroup SU$(\,{\cal N}/2\,|1)$, where the number of supersymmetries
${\cal N}$ is arbitrary even number. Constructed models possess the hidden
supersymmetry SU$(\,... | [
{
"created": "Tue, 1 Oct 2019 04:23:08 GMT",
"version": "v1"
}
] | 2020-01-08 | [
[
"Sidorov",
"Stepan",
""
]
] | We consider quantum models corresponding to superymmetrizations of the two-dimensional harmonic oscillator based on worldline $d=1$ realizations of the supergroup SU$(\,{\cal N}/2\,|1)$, where the number of supersymmetries ${\cal N}$ is arbitrary even number. Constructed models possess the hidden supersymmetry SU$(\,{\... | 8.550377 | 8.710057 | 9.056508 | 8.196689 | 8.317416 | 7.852586 | 7.551563 | 7.793166 | 8.255792 | 8.692065 | 7.88078 | 8.002621 | 8.604316 | 7.716872 | 7.780067 | 7.754529 | 8.117781 | 7.824321 | 7.558826 | 8.517711 | 7.676238 |
1302.6348 | Leonardo Modesto | Leonardo Modesto | Super-renormalizable Gravity | 3 pages, proceedings of the 13th Marcel Grossmann Meeting, Stockholm,
Sweden, July 1-7, 2012 | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review a class of higher derivative theories of gravity consistent at
quantum level. This class is marked by a non-polynomal entire function (form
factor), which averts extra degrees of freedom (including ghosts) and improves
the high energy behaviour of the loop amplitudes. By power counting arguments,
it is prov... | [
{
"created": "Tue, 26 Feb 2013 07:39:35 GMT",
"version": "v1"
}
] | 2013-02-27 | [
[
"Modesto",
"Leonardo",
""
]
] | We review a class of higher derivative theories of gravity consistent at quantum level. This class is marked by a non-polynomal entire function (form factor), which averts extra degrees of freedom (including ghosts) and improves the high energy behaviour of the loop amplitudes. By power counting arguments, it is proved... | 12.879095 | 8.065556 | 11.663302 | 9.251949 | 8.515414 | 8.497169 | 8.284301 | 9.589573 | 9.203234 | 13.450223 | 9.269732 | 10.387706 | 11.462456 | 10.692501 | 10.835817 | 10.566194 | 10.566791 | 10.649276 | 11.191752 | 11.077709 | 11.051811 |
0711.1178 | Gerald V. Dunne | Gerald V. Dunne | Functional Determinants in Quantum Field Theory | Plenary talk at QTS5 (Quantum Theory and Symmetries); 16 pp, 2 figs | J.Phys.A41:304006,2008 | 10.1088/1751-8113/41/30/304006 | null | hep-th | null | Functional determinants of differential operators play a prominent role in
theoretical and mathematical physics, and in particular in quantum field
theory. They are, however, difficult to compute in non-trivial cases. For one
dimensional problems, a classical result of Gel'fand and Yaglom dramatically
simplifies the ... | [
{
"created": "Wed, 7 Nov 2007 22:44:21 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Dunne",
"Gerald V.",
""
]
] | Functional determinants of differential operators play a prominent role in theoretical and mathematical physics, and in particular in quantum field theory. They are, however, difficult to compute in non-trivial cases. For one dimensional problems, a classical result of Gel'fand and Yaglom dramatically simplifies the pr... | 6.848186 | 5.926459 | 6.073941 | 5.933424 | 5.982752 | 5.707755 | 5.869737 | 5.420273 | 5.438754 | 6.12586 | 5.545983 | 5.814729 | 5.895364 | 5.581094 | 5.58223 | 5.896158 | 5.718495 | 5.69533 | 5.680914 | 6.056507 | 5.828557 |
hep-th/9511201 | Mark DE WILD Propitius | Mark de Wild Propitius and F. Alexander Bais | Discrete gauge theories | 85+2 pages, LaTeX, 13 eps figures uuencoded. Lectures presented by
the second author at the CRM-CAP Summer School `Particles and Fields 94',
Bannf, Alberta, Canada, August 16-24, 1994. Some minor typos corrected,
references added, figures slightly changed, a discussion expanded. Postscript
version also availabl... | null | null | PAR-LPTHE 95-46 and ITFA-95-46 | hep-th | null | In these lecture notes, we present a self-contained discussion of planar
gauge theories broken down to some finite residual gauge group H via the Higgs
mechanism. The main focus is on the discrete H gauge theory describing the long
distance physics of such a model. The spectrum features global H charges,
magnetic vor... | [
{
"created": "Tue, 28 Nov 1995 18:38:42 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Mar 1996 17:34:19 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Propitius",
"Mark de Wild",
""
],
[
"Bais",
"F. Alexander",
""
]
] | In these lecture notes, we present a self-contained discussion of planar gauge theories broken down to some finite residual gauge group H via the Higgs mechanism. The main focus is on the discrete H gauge theory describing the long distance physics of such a model. The spectrum features global H charges, magnetic vorti... | 7.150746 | 7.372901 | 8.214781 | 7.067707 | 7.102898 | 7.594907 | 7.203228 | 7.402411 | 7.331049 | 8.152134 | 6.989169 | 7.064217 | 7.209754 | 6.938402 | 7.133074 | 7.050432 | 6.977829 | 6.957037 | 6.876926 | 7.070945 | 7.004498 |
0910.1993 | Ramond | Pierre Ramond | Still in Light-Cone Superspace | Invited Talk at Shifmania, St PAul-Minneapolis, May 2009 | Int.J.Mod.Phys.A25:367-380,2010 | 10.1142/S0217751X10048676 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The recently formulated Bagger-Lambert-Gustavsson (BLG) theory in three
dimensions is described in terms of a constrained chiral superfield in
light-cone superspace. We discuss the use of Superconformal symmetry to
determine the form of its interactions, in complete analogy with N=4
SuperYang-Mills in four dimensions... | [
{
"created": "Sun, 11 Oct 2009 10:52:19 GMT",
"version": "v1"
}
] | 2010-02-16 | [
[
"Ramond",
"Pierre",
""
]
] | The recently formulated Bagger-Lambert-Gustavsson (BLG) theory in three dimensions is described in terms of a constrained chiral superfield in light-cone superspace. We discuss the use of Superconformal symmetry to determine the form of its interactions, in complete analogy with N=4 SuperYang-Mills in four dimensions. | 7.994738 | 5.479373 | 8.228192 | 5.444502 | 5.794968 | 5.874515 | 5.141691 | 5.265634 | 5.742065 | 7.10467 | 5.355292 | 5.678711 | 6.061107 | 5.518298 | 5.467957 | 5.547144 | 5.465272 | 5.583212 | 5.675462 | 6.653045 | 5.464974 |
hep-th/9707226 | Christophe Grojean | Ph Brax, C. Grojean and C.A. Savoy | Geometrical approach to duality in N=1 supersymmetric theories | 14 pages, LaTex | null | null | CERN-TH/97-171, Saclay T97/084 | hep-th | null | We investigate the geometry of the moduli spaces of dual electric and
magnetic N=1 supersymmetric field theories. Using the SU(N_c) gauge group as a
guideline we show that the electric and magnetic moduli spaces coincide for a
suitable choice of the Kahler potential of the magnetic theory. We analyse the
Kahler struc... | [
{
"created": "Mon, 28 Jul 1997 07:48:51 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Brax",
"Ph",
""
],
[
"Grojean",
"C.",
""
],
[
"Savoy",
"C. A.",
""
]
] | We investigate the geometry of the moduli spaces of dual electric and magnetic N=1 supersymmetric field theories. Using the SU(N_c) gauge group as a guideline we show that the electric and magnetic moduli spaces coincide for a suitable choice of the Kahler potential of the magnetic theory. We analyse the Kahler structu... | 8.954153 | 7.954216 | 9.744487 | 7.213898 | 7.740773 | 7.632434 | 7.972121 | 7.619687 | 6.963433 | 9.291832 | 7.684596 | 7.377915 | 7.912587 | 7.325065 | 7.619534 | 7.306051 | 7.545541 | 7.770235 | 7.426854 | 8.281297 | 7.087712 |
0809.5234 | Arkady Tseytlin | M. Beccaria, V. Forini, A. Tirziu and A.A. Tseytlin | Structure of large spin expansion of anomalous dimensions at strong
coupling | 43 pages. v2: minor comments added, misprints corrected; v3: one-loop
coefficients are expressed in terms of one constant not fixed by our method
of computation, conclusion about parity invariance is unchanged, note added;
v4: minor correctionsin eq (3.34) and below (3.37) | Nucl.Phys.B812:144-180,2009 | 10.1016/j.nuclphysb.2008.12.013 | AEI-2008-076, HU-EP-08/31, Imperial-TP-AT-2008-4 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The anomalous dimensions of planar N=4 SYM theory operators like tr(Phi D^S
Phi) expanded in large spin S have the asymptotics \gamma= f ln S + f_c + 1/S
(f_11 ln S + f_10) + ..., where f (the universal scaling function or cusp
anomaly), f_c and f_mn are given by power series in the `t Hooft coupling
\lambda. The sub... | [
{
"created": "Tue, 30 Sep 2008 19:04:38 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Oct 2008 18:39:21 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Dec 2008 19:02:19 GMT",
"version": "v3"
},
{
"created": "Sun, 18 Jan 2009 14:55:02 GMT",
"version": "v4"
}
] | 2009-07-13 | [
[
"Beccaria",
"M.",
""
],
[
"Forini",
"V.",
""
],
[
"Tirziu",
"A.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | The anomalous dimensions of planar N=4 SYM theory operators like tr(Phi D^S Phi) expanded in large spin S have the asymptotics \gamma= f ln S + f_c + 1/S (f_11 ln S + f_10) + ..., where f (the universal scaling function or cusp anomaly), f_c and f_mn are given by power series in the `t Hooft coupling \lambda. The suble... | 6.109107 | 6.721578 | 8.052818 | 6.261759 | 7.453755 | 7.261942 | 6.988658 | 6.80611 | 6.376009 | 8.090074 | 6.409897 | 6.119884 | 6.990567 | 6.194041 | 6.257857 | 6.204997 | 6.365574 | 6.197796 | 6.23869 | 6.749252 | 6.312117 |
1202.0170 | Bojan Nikoli\'c | B. Nikolic and B. Sazdovic | Dirichlet boundary conditions in type IIB superstring theory and
fermionic T-duality | null | JHEP 06 (2012) 101 | 10.1007/JHEP06(2012)101 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we investigate the relation between consequences of Dirichlet
boundary conditions (momenta noncommutativity and parameters of the effective
theory) and background fields of fermionic T-dual theory. We impose Dirichlet
boundary conditions on the endpoints of the open string propagating in
background of... | [
{
"created": "Wed, 1 Feb 2012 13:32:12 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Jul 2012 17:36:52 GMT",
"version": "v2"
}
] | 2012-07-03 | [
[
"Nikolic",
"B.",
""
],
[
"Sazdovic",
"B.",
""
]
] | In this article we investigate the relation between consequences of Dirichlet boundary conditions (momenta noncommutativity and parameters of the effective theory) and background fields of fermionic T-dual theory. We impose Dirichlet boundary conditions on the endpoints of the open string propagating in background of t... | 11.000578 | 10.46126 | 11.418159 | 9.994671 | 11.219417 | 10.714697 | 11.649188 | 10.022531 | 10.769313 | 11.316129 | 9.814449 | 10.492571 | 11.069311 | 9.891064 | 10.364753 | 10.115735 | 9.862022 | 10.074553 | 10.237383 | 10.732884 | 10.050495 |
2005.11240 | Joonho Kim | Prarit Agarwal, Sunjin Choi, Joonho Kim, Seok Kim, June Nahmgoong | AdS black holes and finite N indices | 19 pages, 8 figures | Phys. Rev. D 103, 126006 (2021) | 10.1103/PhysRevD.103.126006 | QMUL-PH-20-11, SNUTP20-001, KIAS-P20020 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the index of 4d $\mathcal{N}=4$ Yang-Mills theory with $U(N)$ gauge
group, focussing on the physics of the dual BPS black holes in $AdS_5\times
S^5$. Certain aspects of these black holes can be studied from finite $N$
indices with reasonably large $N^2$. We make numerical studies of the index for
$N\leq 6$, ... | [
{
"created": "Fri, 22 May 2020 15:43:43 GMT",
"version": "v1"
}
] | 2021-06-09 | [
[
"Agarwal",
"Prarit",
""
],
[
"Choi",
"Sunjin",
""
],
[
"Kim",
"Joonho",
""
],
[
"Kim",
"Seok",
""
],
[
"Nahmgoong",
"June",
""
]
] | We study the index of 4d $\mathcal{N}=4$ Yang-Mills theory with $U(N)$ gauge group, focussing on the physics of the dual BPS black holes in $AdS_5\times S^5$. Certain aspects of these black holes can be studied from finite $N$ indices with reasonably large $N^2$. We make numerical studies of the index for $N\leq 6$, by... | 9.031661 | 8.501821 | 10.289443 | 8.103821 | 7.993363 | 8.220639 | 8.348163 | 8.268673 | 8.309584 | 10.607859 | 8.39828 | 8.35269 | 9.339952 | 8.463287 | 8.361054 | 8.377793 | 8.438959 | 8.36656 | 8.416376 | 9.032938 | 8.337102 |
1001.0371 | Xian-Hui Ge | Xian-Hui Ge, Sang-Jin Sin | Acoustic black holes for relativistic fluids | 16 pages. typos corrected, contents expanded | JHEP 1006:087,2010 | 10.1007/JHEP06(2010)087 | null | hep-th cond-mat.quant-gas cond-mat.supr-con gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a new acoustic black hole metric from the Abelian Higgs model. In
the non-relativistic limit, while the Abelian Higgs model becomes the
Ginzburg-Landau model, the metric reduces to an ordinary Unruh type. We
investigate the possibility of using (type I and II) superconductors as the
acoustic black holes. We... | [
{
"created": "Sun, 3 Jan 2010 13:35:32 GMT",
"version": "v1"
},
{
"created": "Thu, 13 May 2010 00:24:09 GMT",
"version": "v2"
},
{
"created": "Fri, 14 May 2010 05:46:21 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Ge",
"Xian-Hui",
""
],
[
"Sin",
"Sang-Jin",
""
]
] | We derive a new acoustic black hole metric from the Abelian Higgs model. In the non-relativistic limit, while the Abelian Higgs model becomes the Ginzburg-Landau model, the metric reduces to an ordinary Unruh type. We investigate the possibility of using (type I and II) superconductors as the acoustic black holes. We p... | 13.104661 | 12.644594 | 11.23398 | 11.5396 | 11.183702 | 12.349954 | 10.840947 | 11.713159 | 11.946197 | 13.290377 | 11.361272 | 11.904285 | 12.450526 | 11.638111 | 12.204097 | 11.893581 | 11.697782 | 11.281927 | 11.832844 | 12.266915 | 11.563024 |
1312.7736 | Mokhtar Hassaine | Moises Bravo-Gaete and Mokhtar Hassaine | Lifshitz black holes with a time-dependent scalar field in Horndeski
theory | New version with lot of corrections | PhysRevD.89.104028 (2014) | 10.1103/PhysRevD.89.104028 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In arbitrary dimensions, we consider a particular Horndeski action given by
the Einstein-Hilbert Lagrangian with a cosmological constant term, while the
source part is described by a real scalar field with its usual kinetic term
together with a nonminimal kinetic coupling. In order to evade the no-hair
theorem, we lo... | [
{
"created": "Mon, 30 Dec 2013 15:22:44 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Apr 2014 23:07:27 GMT",
"version": "v2"
}
] | 2014-06-13 | [
[
"Bravo-Gaete",
"Moises",
""
],
[
"Hassaine",
"Mokhtar",
""
]
] | In arbitrary dimensions, we consider a particular Horndeski action given by the Einstein-Hilbert Lagrangian with a cosmological constant term, while the source part is described by a real scalar field with its usual kinetic term together with a nonminimal kinetic coupling. In order to evade the no-hair theorem, we look... | 9.380755 | 9.411992 | 9.294865 | 8.216715 | 8.83159 | 9.44857 | 9.150646 | 8.537315 | 9.152791 | 9.433573 | 8.816192 | 8.893169 | 8.914607 | 8.755019 | 8.997809 | 8.832031 | 9.024039 | 8.656344 | 9.308272 | 9.054689 | 8.692506 |
1806.01283 | Zhuo Chen | Zhuo Chen, Tony Pantev, Eric Sharpe | Landau-Ginzburg models for certain fiber products with curves | 17 pages; LaTeX | null | 10.1016/j.geomphys.2018.11.012 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we describe a physical realization of a family of non-compact
Kahler threefolds with trivial canonical bundle in hybrid Landau-Ginzburg
models, motivated by some recent non-Kahler solutions of Strominger systems,
and utilizing some recent ideas from GLSMs. We consider threefolds given as
fiber products ... | [
{
"created": "Mon, 4 Jun 2018 18:00:02 GMT",
"version": "v1"
}
] | 2019-01-30 | [
[
"Chen",
"Zhuo",
""
],
[
"Pantev",
"Tony",
""
],
[
"Sharpe",
"Eric",
""
]
] | In this paper we describe a physical realization of a family of non-compact Kahler threefolds with trivial canonical bundle in hybrid Landau-Ginzburg models, motivated by some recent non-Kahler solutions of Strominger systems, and utilizing some recent ideas from GLSMs. We consider threefolds given as fiber products of... | 10.601645 | 10.392552 | 12.681158 | 9.975388 | 11.195424 | 11.230307 | 11.020318 | 9.917627 | 10.297986 | 13.441192 | 10.537102 | 9.518107 | 10.742863 | 9.944838 | 10.277243 | 9.91761 | 10.103741 | 9.767438 | 9.750546 | 10.902276 | 9.997042 |
1710.09701 | Asuka Ito | Asuka Ito, Jiro Soda | Anisotropic Constant-roll Inflation | 13 pages, 3 figures | Eur.Phys.J. C78 (2018) no.1, 55 | 10.1140/epjc/s10052-018-5534-5 | KOBE-COSMO-17-15 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study constant-roll inflation in the presence of a gauge field coupled to
an inflaton. By imposing the constant anisotropy condition, we find new exact
anisotropic constant-roll inflationary solutions which include anisotropic
power-law inflation as a special case. We also numerically show that the new
anisotropic... | [
{
"created": "Thu, 26 Oct 2017 13:58:02 GMT",
"version": "v1"
},
{
"created": "Sun, 11 Feb 2018 08:12:03 GMT",
"version": "v2"
}
] | 2018-02-13 | [
[
"Ito",
"Asuka",
""
],
[
"Soda",
"Jiro",
""
]
] | We study constant-roll inflation in the presence of a gauge field coupled to an inflaton. By imposing the constant anisotropy condition, we find new exact anisotropic constant-roll inflationary solutions which include anisotropic power-law inflation as a special case. We also numerically show that the new anisotropic s... | 5.208248 | 4.704935 | 4.696914 | 4.801804 | 5.080393 | 5.000774 | 5.014485 | 4.813953 | 5.069462 | 4.717509 | 4.532326 | 4.961144 | 4.899819 | 4.784429 | 4.933504 | 4.952811 | 4.996877 | 4.912808 | 4.907597 | 4.82709 | 4.517768 |
1511.03646 | Paolo Glorioso | Michael Crossley, Paolo Glorioso and Hong Liu | Effective field theory of dissipative fluids | 110 pages, 2 figures, v.2 references and acknowledgments added,
misprints corrected, clarifications in numerous places including a new sec.
III C. v.3 notations streamlined and got rid of tau_a, minor clarifications.
Removed Appendix G on conformal fluids which is expanded and included in
arXiv:1701.07817 | null | null | MIT-CTP/4734 | hep-th cond-mat.stat-mech gr-qc hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop an effective field theory for dissipative fluids which governs the
dynamics of long-lived gapless modes associated with conserved quantities. The
resulting theory gives a path integral formulation of fluctuating hydrodynamics
which systematically incorporates nonlinear interactions of noises. The
dynamical... | [
{
"created": "Wed, 11 Nov 2015 20:32:34 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Jun 2016 18:40:05 GMT",
"version": "v2"
},
{
"created": "Fri, 27 Jan 2017 18:07:19 GMT",
"version": "v3"
}
] | 2017-01-30 | [
[
"Crossley",
"Michael",
""
],
[
"Glorioso",
"Paolo",
""
],
[
"Liu",
"Hong",
""
]
] | We develop an effective field theory for dissipative fluids which governs the dynamics of long-lived gapless modes associated with conserved quantities. The resulting theory gives a path integral formulation of fluctuating hydrodynamics which systematically incorporates nonlinear interactions of noises. The dynamical v... | 10.587252 | 10.666044 | 10.934794 | 10.854215 | 10.846479 | 10.439569 | 10.435258 | 10.521221 | 10.787316 | 12.304464 | 10.499633 | 10.804807 | 10.506602 | 10.453716 | 10.505851 | 10.612175 | 10.484058 | 10.260404 | 10.523258 | 10.567418 | 10.516093 |
0802.2637 | M. Hossein Dehghani | M. H. Dehghani, N. Alinejadi and S. H. Hendi | Topological Black Holes in Lovelock-Born-Infeld Gravity | 14 pages | Phys.Rev.D77:104025,2008 | 10.1103/PhysRevD.77.104025 | null | hep-th | http://creativecommons.org/licenses/publicdomain/ | In this paper, we present topological black holes of third order Lovelock
gravity in the presence of cosmological constant and nonlinear electromagnetic
Born-Infeld field. Depending on the metric parameters, these solutions may be
interpreted as black hole solutions with inner and outer event horizons, an
extreme bla... | [
{
"created": "Tue, 19 Feb 2008 11:50:20 GMT",
"version": "v1"
},
{
"created": "Sat, 24 May 2008 10:13:17 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Dehghani",
"M. H.",
""
],
[
"Alinejadi",
"N.",
""
],
[
"Hendi",
"S. H.",
""
]
] | In this paper, we present topological black holes of third order Lovelock gravity in the presence of cosmological constant and nonlinear electromagnetic Born-Infeld field. Depending on the metric parameters, these solutions may be interpreted as black hole solutions with inner and outer event horizons, an extreme black... | 5.841367 | 4.704764 | 5.59854 | 4.902883 | 4.850648 | 4.451195 | 4.42833 | 4.524052 | 4.658563 | 6.095769 | 4.951656 | 5.26635 | 5.820302 | 5.451044 | 5.361373 | 5.452812 | 5.305991 | 5.23253 | 5.321592 | 5.705801 | 5.360128 |
2309.00512 | Nicki Mullins | Nicki Mullins, Mauricio Hippert, Lorenzo Gavassino, Jorge Noronha | Relativistic hydrodynamic fluctuations from an effective action:
causality, stability, and the information current | 28 pages | null | null | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Causality is necessary for retarded Green's functions to remain retarded in
all inertial frames in relativity, which ensures that dissipation of
fluctuations is a Lorentz invariant concept. For first-order BDNK theories with
stochastic fluctuations, introduced via the Schwinger-Keldysh formalism, we
show that imposin... | [
{
"created": "Fri, 1 Sep 2023 14:59:59 GMT",
"version": "v1"
}
] | 2023-09-04 | [
[
"Mullins",
"Nicki",
""
],
[
"Hippert",
"Mauricio",
""
],
[
"Gavassino",
"Lorenzo",
""
],
[
"Noronha",
"Jorge",
""
]
] | Causality is necessary for retarded Green's functions to remain retarded in all inertial frames in relativity, which ensures that dissipation of fluctuations is a Lorentz invariant concept. For first-order BDNK theories with stochastic fluctuations, introduced via the Schwinger-Keldysh formalism, we show that imposing ... | 10.699702 | 10.926375 | 10.680332 | 10.399275 | 10.80382 | 10.744779 | 10.866934 | 10.571299 | 10.234225 | 11.555298 | 10.095737 | 10.188166 | 10.213182 | 9.964855 | 10.147904 | 10.152086 | 10.228244 | 10.355825 | 10.352977 | 10.700426 | 10.30442 |
1608.01293 | Hossein Yavartanoo | M.M. Sheikh-Jabbari and H. Yavartanoo | Horizon Fluffs: Near Horizon Soft Hairs as Microstates of Generic AdS3
Black Holes | 21 pages, 1 figure, minor corrections, improvements in the
presentation | Phys. Rev. D 95, 044007 (2017) | 10.1103/PhysRevD.95.044007 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In [1] the horizon fluffs proposal is put forward to identify microstates of
generic non-extremal three-dimensional Banados-Teitelboim-Zanelli (BTZ) black
holes. The proposal is that black hole microstates, which were dubbed as
horizon fluffs, are states labelled by the conserved charges associated with
non-trivial d... | [
{
"created": "Wed, 3 Aug 2016 19:14:11 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Aug 2016 06:43:39 GMT",
"version": "v2"
},
{
"created": "Fri, 28 Oct 2016 17:01:18 GMT",
"version": "v3"
}
] | 2017-02-15 | [
[
"Sheikh-Jabbari",
"M. M.",
""
],
[
"Yavartanoo",
"H.",
""
]
] | In [1] the horizon fluffs proposal is put forward to identify microstates of generic non-extremal three-dimensional Banados-Teitelboim-Zanelli (BTZ) black holes. The proposal is that black hole microstates, which were dubbed as horizon fluffs, are states labelled by the conserved charges associated with non-trivial dif... | 7.948504 | 7.643565 | 8.081134 | 7.280815 | 7.626431 | 7.579158 | 8.018687 | 7.723073 | 7.937821 | 9.041919 | 7.744215 | 7.597128 | 7.813747 | 7.473841 | 7.773058 | 7.5384 | 7.726394 | 7.722035 | 7.638648 | 7.9401 | 7.486856 |
1312.6374 | Xu Xiaobao | Nan Bai, Yi-Hong Gao, Xiao-bao Xu | Note on Mutual Information between Two Intervals of Extremal BTZ | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we compute mutual information between two intervals in CFTs dual
to extremal BTZ (UV CFT) and near horizon limit of extremal BTZ (IR CFT) using
the replica technique in some limiting regimes, which can be compared with
holographic description.
| [
{
"created": "Sun, 22 Dec 2013 12:12:27 GMT",
"version": "v1"
}
] | 2013-12-24 | [
[
"Bai",
"Nan",
""
],
[
"Gao",
"Yi-Hong",
""
],
[
"Xu",
"Xiao-bao",
""
]
] | In this note we compute mutual information between two intervals in CFTs dual to extremal BTZ (UV CFT) and near horizon limit of extremal BTZ (IR CFT) using the replica technique in some limiting regimes, which can be compared with holographic description. | 15.235228 | 9.686238 | 13.666512 | 9.610069 | 8.473288 | 8.588487 | 10.088158 | 8.105418 | 9.26505 | 10.953938 | 8.990995 | 9.515834 | 10.790161 | 9.730218 | 8.994596 | 9.818929 | 8.675484 | 9.580786 | 9.741384 | 11.370741 | 9.27267 |
0808.1345 | Waldemar Schulgin | Waldemar Schulgin, Jan Troost | Backreacted T-folds and non-geometric regions in configuration space | 25 pages, 4 figures; v2: minor changes, reference added | JHEP 0812:098,2008 | 10.1088/1126-6708/2008/12/098 | LPTENS-08/49 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide the backreaction of the T-fold doubly T-dual to a background with
NSNS three-form flux on a three-torus. We extend the backreacted T-fold to
include cases with a flux localized in one out of three directions. We analyze
the resulting monodromy domain walls and vortices. In these backgrounds, we
give an ana... | [
{
"created": "Mon, 11 Aug 2008 16:42:36 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Jan 2009 23:28:32 GMT",
"version": "v2"
}
] | 2009-01-17 | [
[
"Schulgin",
"Waldemar",
""
],
[
"Troost",
"Jan",
""
]
] | We provide the backreaction of the T-fold doubly T-dual to a background with NSNS three-form flux on a three-torus. We extend the backreacted T-fold to include cases with a flux localized in one out of three directions. We analyze the resulting monodromy domain walls and vortices. In these backgrounds, we give an analy... | 16.508997 | 16.974375 | 17.086029 | 14.531492 | 15.416206 | 15.548522 | 15.537946 | 15.459661 | 14.613749 | 18.390079 | 14.225116 | 13.913814 | 15.787992 | 14.593766 | 14.282285 | 13.938131 | 13.989175 | 14.445367 | 14.277893 | 15.318998 | 14.040622 |
hep-th/0011178 | M. A. R. Osorio | M. A. R. Osorio, Mar\'ia Su\'arez (University of Oviedo, Asturias,
Spain) | On the effective character of a non abelian DBI action | Old section 3 suppressed, the end of old section 4 is now an
appendix. For the obssesed reader, we also stress that the work has nothing
to do with any proposal of modification for the DBI action in the non abelian
case | Phys.Lett. B502 (2001) 239-245 | 10.1016/S0370-2693(01)00195-2 | null | hep-th | null | We study the way Lorentz covariance can be reconstructed from Matrix Theory
as a IMF description of M-theory. The problem is actually related to the
interplay between a non abelian Dirac-Born-Infeld action and Super-Yang-Mills
as its generalized non-relativistic approximation. All this physics shows up by
means of an... | [
{
"created": "Mon, 20 Nov 2000 19:03:55 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Nov 2000 09:47:06 GMT",
"version": "v2"
}
] | 2016-08-15 | [
[
"Osorio",
"M. A. R.",
"",
"University of Oviedo, Asturias,\n Spain"
],
[
"Suárez",
"María",
"",
"University of Oviedo, Asturias,\n Spain"
]
] | We study the way Lorentz covariance can be reconstructed from Matrix Theory as a IMF description of M-theory. The problem is actually related to the interplay between a non abelian Dirac-Born-Infeld action and Super-Yang-Mills as its generalized non-relativistic approximation. All this physics shows up by means of an a... | 15.635865 | 15.382586 | 16.690952 | 15.008916 | 15.041666 | 15.859371 | 15.169161 | 14.913071 | 15.323985 | 17.419233 | 14.292729 | 14.572894 | 15.129763 | 14.634759 | 14.755024 | 14.450464 | 14.77894 | 14.653557 | 14.456778 | 15.030852 | 14.465473 |
1910.04962 | Kantaro Ohmori | Clay Cordova and Kantaro Ohmori | Anomaly Obstructions to Symmetry Preserving Gapped Phases | 35 pages, 9 figures; references added | null | null | null | hep-th cond-mat.str-el math-ph math.AT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Anomalies are renormalization group invariants that constrain the dynamics of
quantum field theories. We show that certain anomalies for discrete global
symmetries imply that the underlying theory either spontaneously breaks its
generalized global symmetry or is gapless. We identify an obstruction,
formulated in term... | [
{
"created": "Fri, 11 Oct 2019 03:58:46 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Jan 2020 04:53:23 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Cordova",
"Clay",
""
],
[
"Ohmori",
"Kantaro",
""
]
] | Anomalies are renormalization group invariants that constrain the dynamics of quantum field theories. We show that certain anomalies for discrete global symmetries imply that the underlying theory either spontaneously breaks its generalized global symmetry or is gapless. We identify an obstruction, formulated in terms ... | 8.601985 | 7.945524 | 9.265025 | 7.71513 | 7.616822 | 7.788437 | 7.312975 | 7.220691 | 7.689735 | 9.948789 | 7.081724 | 7.484772 | 7.970172 | 7.594118 | 7.655262 | 7.358676 | 7.338776 | 7.359775 | 7.430578 | 8.116716 | 7.540924 |
hep-th/0410165 | Marcos Marino | Marcos Marino | Les Houches lectures on matrix models and topological strings | 63 pages, 8 figures, minor corrections | null | null | CERN-PH-TH/2004-199 | hep-th | null | In these lecture notes for the Les Houches School on Applications of Random
Matrices in Physics we give an introduction to the connections between matrix
models and topological strings. We first review some basic results of matrix
model technology and then we focus on type B topological strings. We present
the main r... | [
{
"created": "Thu, 14 Oct 2004 10:58:36 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Jan 2005 15:05:17 GMT",
"version": "v2"
},
{
"created": "Mon, 18 Jul 2005 10:18:56 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Marino",
"Marcos",
""
]
] | In these lecture notes for the Les Houches School on Applications of Random Matrices in Physics we give an introduction to the connections between matrix models and topological strings. We first review some basic results of matrix model technology and then we focus on type B topological strings. We present the main res... | 7.312869 | 7.259244 | 8.685964 | 7.150307 | 7.505412 | 7.241742 | 7.221511 | 7.340944 | 7.457524 | 7.871218 | 6.877467 | 6.777423 | 7.329353 | 7.115362 | 7.062898 | 6.890507 | 6.970136 | 6.670731 | 7.058953 | 7.480117 | 6.768504 |
hep-th/9910023 | S. Solodukhin | Kostas Skenderis and Sergey N. Solodukhin | Quantum effective action from the AdS/CFT correspondence | 12 pages, latex, no figures; v2: minor improvements and two
references added | Phys.Lett.B472:316-322,2000 | 10.1016/S0370-2693(99)01467-7 | SPIN-1999/23 | hep-th gr-qc math.DG | null | We obtain an Einstein metric of constant negative curvature given an
arbitrary boundary metric in three dimensions, and a conformally flat one given
an arbitrary conformally flat boundary metric in other dimensions. In order to
compute the on-shell value of the gravitational action for these solutions, we
propose to ... | [
{
"created": "Mon, 4 Oct 1999 14:57:14 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Oct 1999 12:32:58 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Skenderis",
"Kostas",
""
],
[
"Solodukhin",
"Sergey N.",
""
]
] | We obtain an Einstein metric of constant negative curvature given an arbitrary boundary metric in three dimensions, and a conformally flat one given an arbitrary conformally flat boundary metric in other dimensions. In order to compute the on-shell value of the gravitational action for these solutions, we propose to in... | 9.575662 | 9.426866 | 10.0029 | 8.45303 | 10.121231 | 8.994108 | 9.930619 | 8.791817 | 9.142521 | 10.477574 | 8.886751 | 9.052986 | 9.396972 | 9.211912 | 9.266745 | 9.010411 | 8.970325 | 8.980879 | 9.13027 | 9.582017 | 8.973655 |
hep-th/0011277 | Sergei Larin | S.A. Larin | The method of direct expansions of Feynman integrals | 7 pages, latex, no figures | Phys.Lett. B514 (2001) 366-370 | 10.1016/S0370-2693(01)00825-5 | INR-THSL-11-2000 | hep-th | null | The universal method of expansion of integrals is suggested. It allows in
particular to derive the threshold expansion of Feynman integrals.
| [
{
"created": "Wed, 29 Nov 2000 23:55:11 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Larin",
"S. A.",
""
]
] | The universal method of expansion of integrals is suggested. It allows in particular to derive the threshold expansion of Feynman integrals. | 24.694248 | 14.022677 | 14.578353 | 14.235605 | 13.197588 | 13.979566 | 14.863323 | 15.190858 | 12.012318 | 14.434157 | 14.586319 | 15.443933 | 15.456727 | 15.51113 | 15.548935 | 16.499399 | 15.803053 | 15.38631 | 15.852665 | 14.564968 | 14.857956 |
2103.06905 | Christopher Verhaaren | Julian Heeck, Arvind Rajaraman, Rebecca Riley, Christopher B.
Verhaaren | Mapping Gauged Q-Balls | 19 pages, 6 figures; v2: matches published version. v3: fixed typo in
Eq.(3). v4: fixed typos in Fig. 4 | Phys. Rev. D 103, 116004 (2021) | 10.1103/PhysRevD.103.116004 | UCI-TR-2021-10 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Scalar field theories with particular U(1)-symmetric potentials contain
non-topological soliton solutions called Q-balls. Promoting the U(1) to a gauge
symmetry leads to the more complicated situation of gauged Q-balls. The soliton
solutions to the resulting set of nonlinear differential equations have
markedly diffe... | [
{
"created": "Thu, 11 Mar 2021 19:01:49 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Apr 2021 00:03:50 GMT",
"version": "v2"
},
{
"created": "Mon, 13 Sep 2021 21:51:48 GMT",
"version": "v3"
},
{
"created": "Tue, 13 Jun 2023 06:32:30 GMT",
"version": "v4"
}
] | 2023-06-14 | [
[
"Heeck",
"Julian",
""
],
[
"Rajaraman",
"Arvind",
""
],
[
"Riley",
"Rebecca",
""
],
[
"Verhaaren",
"Christopher B.",
""
]
] | Scalar field theories with particular U(1)-symmetric potentials contain non-topological soliton solutions called Q-balls. Promoting the U(1) to a gauge symmetry leads to the more complicated situation of gauged Q-balls. The soliton solutions to the resulting set of nonlinear differential equations have markedly differe... | 8.31537 | 7.843699 | 7.481452 | 7.355884 | 7.472491 | 7.641622 | 7.951571 | 7.596324 | 7.478403 | 8.03559 | 7.340124 | 7.983612 | 7.849275 | 7.71598 | 7.865158 | 7.904577 | 7.872153 | 7.80182 | 7.867228 | 7.807345 | 7.968775 |
1906.04489 | Mousumi Maitra | Mousumi Maitra, Debaprasad Maity, Bibhas Ranjan Majhi | Near horizon symmetries, emergence of Goldstone modes and thermality | Modified version, to appear in Euro. Phys. J. Plus | Eur. Phys. J. Plus 135, 483 (2020) | 10.1140/epjp/s13360-020-00451-3 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For a long time it is believed that black hole horizon are thermal and
quantum mechanical in nature. The microscopic origin of this thermality is the
main question behind our present investigation, which reveals possible
importance of near horizon symmetry. It is this symmetry which is assumed to be
spontaneously bro... | [
{
"created": "Tue, 11 Jun 2019 10:43:57 GMT",
"version": "v1"
},
{
"created": "Tue, 5 May 2020 11:24:54 GMT",
"version": "v2"
}
] | 2020-08-06 | [
[
"Maitra",
"Mousumi",
""
],
[
"Maity",
"Debaprasad",
""
],
[
"Majhi",
"Bibhas Ranjan",
""
]
] | For a long time it is believed that black hole horizon are thermal and quantum mechanical in nature. The microscopic origin of this thermality is the main question behind our present investigation, which reveals possible importance of near horizon symmetry. It is this symmetry which is assumed to be spontaneously broke... | 14.40639 | 14.950957 | 14.312623 | 13.085439 | 14.331561 | 14.024319 | 14.5618 | 13.669511 | 14.144368 | 15.87112 | 13.848345 | 14.069789 | 14.143939 | 13.859704 | 13.556542 | 13.986266 | 13.975121 | 13.672203 | 13.89727 | 14.440938 | 13.650888 |
hep-th/9809112 | Hagen Kleinert | H. Kleinert, E. Babaev | Two Phase Transitions in Chiral Gross-Neveu Model in $2+ \epsilon$
Dimensions at Low N | Author Information under
http://www.physik.fu-berlin.de/~kleinert/institution.html . Latest update of
paper also at
http://www.physik.fu-berlin.de/~kleinert/kleiner_re269/preprint.html | Phys.Lett. B438 (1998) 311-320 | 10.1016/S0370-2693(98)00983-6 | null | hep-th | null | We show that the chiral Gross-Neveu model in $2+ \epsilon$ dimensions has for
a small number $N$ of fermions two phase transitions corresponding to pair
formation and pair condensation.
In the first transition, fermions and antifermions acquire spontaneously a
mass and are bound to pairs which behave like a Bose li... | [
{
"created": "Wed, 16 Sep 1998 06:18:20 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Kleinert",
"H.",
""
],
[
"Babaev",
"E.",
""
]
] | We show that the chiral Gross-Neveu model in $2+ \epsilon$ dimensions has for a small number $N$ of fermions two phase transitions corresponding to pair formation and pair condensation. In the first transition, fermions and antifermions acquire spontaneously a mass and are bound to pairs which behave like a Bose liquid... | 8.021722 | 8.778297 | 8.489627 | 7.829925 | 8.697781 | 8.695087 | 8.644113 | 8.347795 | 7.678903 | 8.188156 | 8.145387 | 8.019418 | 8.027913 | 7.635177 | 7.727887 | 7.927457 | 7.774663 | 7.527805 | 7.803569 | 7.965263 | 7.821342 |
1505.06264 | Mauricio Bellini | Jes\'us Mart\'in Romero, Mauricio Bellini (IFIMAR, CONICET & UNMdP) | Dyonic Reissner-Nordstr\"om black hole: extended Dirac quantization from
5D invariants | version accepted in Astrophys. & Space Sciences | null | null | null | hep-th gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of present work is to extend the application of Weitzeb\"{o}ck
Induced Matter Theory (WIMT) to a dyonic Reissner-Nordstr\"{o}m Black Hole
(RNBH), by proposing a condition compatible with a quantization relation
between gravitational mass and both magnetic and electric charges from a
geometric product defined ... | [
{
"created": "Sat, 23 May 2015 02:27:06 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Jul 2015 21:50:57 GMT",
"version": "v2"
},
{
"created": "Wed, 26 Aug 2015 20:44:39 GMT",
"version": "v3"
},
{
"created": "Thu, 10 Sep 2015 00:24:07 GMT",
"version": "v4"
}
] | 2015-09-11 | [
[
"Romero",
"Jesús Martín",
"",
"IFIMAR, CONICET & UNMdP"
],
[
"Bellini",
"Mauricio",
"",
"IFIMAR, CONICET & UNMdP"
]
] | The aim of present work is to extend the application of Weitzeb\"{o}ck Induced Matter Theory (WIMT) to a dyonic Reissner-Nordstr\"{o}m Black Hole (RNBH), by proposing a condition compatible with a quantization relation between gravitational mass and both magnetic and electric charges from a geometric product defined as... | 16.012903 | 15.745336 | 11.55548 | 11.483405 | 13.505263 | 13.114704 | 16.823902 | 11.991414 | 14.622562 | 13.320827 | 15.483958 | 14.462731 | 13.085763 | 13.476418 | 14.540177 | 13.702719 | 15.512343 | 12.774616 | 12.765449 | 13.991272 | 14.991745 |
hep-th/0503158 | Charles Suggs | R. L. Jaffe | The Casimir Effect and the Quantum Vacuum | 9 pages, 3 figures, uses aip class and the package floatftm to float
text around figures | Phys.Rev. D72 (2005) 021301 | 10.1103/PhysRevD.72.021301 | MIT-CTP-3614 | hep-th astro-ph hep-ph quant-ph | null | In discussions of the cosmological constant, the Casimir effect is often
invoked as decisive evidence that the zero point energies of quantum fields are
"real''. On the contrary, Casimir effects can be formulated and Casimir forces
can be computed without reference to zero point energies. They are
relativistic, quant... | [
{
"created": "Mon, 21 Mar 2005 19:24:29 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Jaffe",
"R. L.",
""
]
] | In discussions of the cosmological constant, the Casimir effect is often invoked as decisive evidence that the zero point energies of quantum fields are "real''. On the contrary, Casimir effects can be formulated and Casimir forces can be computed without reference to zero point energies. They are relativistic, quantum... | 2.587708 | 7.381914 | 7.430896 | 6.398447 | 7.491579 | 7.044523 | 6.927332 | 6.580418 | 6.083116 | 7.881224 | 6.177262 | 5.69753 | 6.32679 | 5.756012 | 6.019983 | 5.878814 | 5.718099 | 5.824418 | 5.621257 | 6.209856 | 5.736572 |
hep-th/0301043 | Igor Tyutin | Igor Batalin and Igor Tyutin | BRST-Invariant Constraint Algebra in Terms of Commutators and Quantum
Antibrackets | 20 pages; some misprints are removed | Theor.Math.Phys. 138 (2004) 1-17; Teor.Mat.Fiz. 138 (2004) 3-22 | 10.1023/B:TAMP.0000010628.58719.a4 | FIAN 03/03 | hep-th | null | General structure of BRST-invariant constraint algebra is established, in its
commutator and antibracket forms, by means of formulation of algebra-generating
equations in yet more extended phase space. New ghost-type variables behave as
fields and antifields with respect to quantum antibrackets. Explicit form of
BRST... | [
{
"created": "Wed, 8 Jan 2003 13:13:23 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Jan 2003 11:23:12 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Dec 2006 14:48:47 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Batalin",
"Igor",
""
],
[
"Tyutin",
"Igor",
""
]
] | General structure of BRST-invariant constraint algebra is established, in its commutator and antibracket forms, by means of formulation of algebra-generating equations in yet more extended phase space. New ghost-type variables behave as fields and antifields with respect to quantum antibrackets. Explicit form of BRST-i... | 21.177151 | 18.193792 | 22.320162 | 19.393877 | 19.495735 | 19.014973 | 20.072344 | 19.570673 | 17.311975 | 24.067656 | 18.929098 | 18.774805 | 20.847492 | 19.356951 | 19.288363 | 19.654799 | 19.049559 | 19.354296 | 18.678482 | 19.275009 | 18.53447 |
hep-th/0511066 | Jorge Stephany | N.Hatcher, A.Restuccia and J.Stephany | The quantum algebra of superspace | 20 pages;changes in the nomenclature | Phys.Rev.D73:046008,2006 | 10.1103/PhysRevD.73.046008 | SB/F/05-333 | hep-th | null | We present the complete set of $N=1$, $D=4$ quantum algebras associated to
massive superparticles. We obtain the explicit solution of these algebras
realized in terms of unconstrained operators acting on the Hilbert space of
superfields. These solutions are expressed using the chiral, anti-chiral and
tensorial projec... | [
{
"created": "Fri, 4 Nov 2005 23:27:02 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Mar 2006 20:55:09 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Hatcher",
"N.",
""
],
[
"Restuccia",
"A.",
""
],
[
"Stephany",
"J.",
""
]
] | We present the complete set of $N=1$, $D=4$ quantum algebras associated to massive superparticles. We obtain the explicit solution of these algebras realized in terms of unconstrained operators acting on the Hilbert space of superfields. These solutions are expressed using the chiral, anti-chiral and tensorial projecto... | 7.964124 | 8.081997 | 8.719589 | 7.439281 | 7.57791 | 7.775393 | 8.048246 | 7.801189 | 7.443864 | 8.9136 | 7.512485 | 7.513621 | 7.84371 | 7.441933 | 7.575511 | 7.871554 | 7.35306 | 7.605909 | 7.536738 | 7.793798 | 7.731308 |
1205.3869 | Jeong-Hyuck Park | Neil B. Copland, Sung Moon Ko and Jeong-Hyuck Park | Superconformal Yang-Mills quantum mechanics and Calogero model with
OSp(N|2,R) symmetry | 1+28 pages, no figure; Refs added. To appear in JHEP | JHEP 07 (2012) 076 | 10.1007/JHEP07(2012)076 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In spacetime dimension two, pure Yang-Mills possesses no physical degrees of
freedom, and consequently it admits a supersymmetric extension to couple to an
arbitrary number, N say, of Majorana-Weyl gauginos. This results in (N,0) super
Yang-Mills. Further, its dimensional reduction to mechanics doubles the number
of ... | [
{
"created": "Thu, 17 May 2012 07:42:30 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Jul 2012 11:42:52 GMT",
"version": "v2"
}
] | 2012-07-19 | [
[
"Copland",
"Neil B.",
""
],
[
"Ko",
"Sung Moon",
""
],
[
"Park",
"Jeong-Hyuck",
""
]
] | In spacetime dimension two, pure Yang-Mills possesses no physical degrees of freedom, and consequently it admits a supersymmetric extension to couple to an arbitrary number, N say, of Majorana-Weyl gauginos. This results in (N,0) super Yang-Mills. Further, its dimensional reduction to mechanics doubles the number of su... | 11.129307 | 10.934433 | 11.614071 | 9.673873 | 10.852887 | 11.997325 | 11.527402 | 9.796974 | 10.222623 | 13.488363 | 9.880255 | 10.184193 | 10.950179 | 10.352863 | 10.277784 | 10.530735 | 10.018928 | 10.020095 | 10.04342 | 11.188727 | 10.37818 |
hep-th/0106054 | Bin Chen | Bin Chen and Feng-Li Lin | Holographic Cosmic Quintessence on Dilatonic Brane World | 16pages, no figure, Latex; revised version, references added, typos
corrected, abstract and comments improved; final version, will appear in PRD | Phys.Rev. D65 (2002) 044007 | 10.1103/PhysRevD.65.044007 | null | hep-th gr-qc hep-ph | null | Recently quintessence is proposed to explain the observation data of
supernova indicating a time-varying cosmological constant and accelerating
universe. Inspired by this and its mysterious origin, we look for the
possibility of quintessence as the holographic dark matters dominated in the
late time in the brane worl... | [
{
"created": "Wed, 6 Jun 2001 16:25:11 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Jun 2001 17:23:20 GMT",
"version": "v2"
},
{
"created": "Sat, 8 Dec 2001 18:35:20 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Chen",
"Bin",
""
],
[
"Lin",
"Feng-Li",
""
]
] | Recently quintessence is proposed to explain the observation data of supernova indicating a time-varying cosmological constant and accelerating universe. Inspired by this and its mysterious origin, we look for the possibility of quintessence as the holographic dark matters dominated in the late time in the brane world ... | 10.682828 | 9.987612 | 11.163932 | 10.171921 | 10.449405 | 11.57644 | 10.816897 | 10.436841 | 10.304838 | 11.674685 | 10.09294 | 10.602403 | 10.711806 | 10.204298 | 10.547814 | 10.816978 | 10.368443 | 10.600487 | 10.062987 | 10.836946 | 10.207162 |
2002.04624 | Chrysostomos Kalousios | James Drummond, Jack Foster, \"Omer G\"urdo\u{g}an, Chrysostomos
Kalousios | Tropical fans, scattering equations and amplitudes | 31 pages | null | 10.1007/JHEP11(2021)071 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a family of tropical fans related to Grassmannian cluster
algebras. These fans are related to the kinematic space of massless scattering
processes in a number of ways. For each fan associated to the Grassmannian
${\rm Gr}(k,n)$ there is a notion of a generalised $\phi^3$ amplitude and an
associated set of... | [
{
"created": "Tue, 11 Feb 2020 19:00:15 GMT",
"version": "v1"
}
] | 2021-11-24 | [
[
"Drummond",
"James",
""
],
[
"Foster",
"Jack",
""
],
[
"Gürdoğan",
"Ömer",
""
],
[
"Kalousios",
"Chrysostomos",
""
]
] | We describe a family of tropical fans related to Grassmannian cluster algebras. These fans are related to the kinematic space of massless scattering processes in a number of ways. For each fan associated to the Grassmannian ${\rm Gr}(k,n)$ there is a notion of a generalised $\phi^3$ amplitude and an associated set of s... | 8.801469 | 8.031535 | 9.405309 | 8.390121 | 8.422626 | 8.438025 | 8.577383 | 7.901022 | 7.79434 | 10.386408 | 8.466764 | 8.473578 | 8.716491 | 8.164201 | 8.249114 | 8.174422 | 8.56019 | 8.40733 | 7.933958 | 8.829027 | 8.055826 |
hep-th/9609028 | Izumi Joichi | M. Hotta, H. Inoue, I. Joichi and M. Tanaka | High Momentum Behavior of Geometric Bremsstrahlung in the Expanding
Universe | 27 pages, LATEX file | Prog.Theor.Phys. 96 (1996) 1103-1122 | 10.1143/PTP.96.1103 | TU/96/496 | hep-th | null | We shall discuss various kinds of geometric bremsstrahlung processes in the
spatially flat Robertson-Walker universe. Despite that the temperature of the
universe is much higher than particle masses and the Hubble parameter, the
transition probability of these processes do not vanish. It is also pointed out
that expl... | [
{
"created": "Tue, 3 Sep 1996 01:25:38 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Hotta",
"M.",
""
],
[
"Inoue",
"H.",
""
],
[
"Joichi",
"I.",
""
],
[
"Tanaka",
"M.",
""
]
] | We shall discuss various kinds of geometric bremsstrahlung processes in the spatially flat Robertson-Walker universe. Despite that the temperature of the universe is much higher than particle masses and the Hubble parameter, the transition probability of these processes do not vanish. It is also pointed out that explic... | 15.765819 | 16.617392 | 14.867998 | 13.540533 | 16.681305 | 15.079551 | 14.317795 | 15.292549 | 15.653645 | 15.297056 | 14.136928 | 15.369337 | 14.65325 | 15.022241 | 15.265513 | 15.451513 | 15.243869 | 15.431029 | 15.052352 | 14.618248 | 15.453868 |
1312.3006 | Bret Underwood | Bret Underwood, Yunxiao Zhai | Non-Linear Resonance in Relativistic Preheating | 17 pages, 10 figures. v2: Added references. v3: Added some
references, additional discussion on particle production | JCAP 04 (2014) 002 | 10.1088/1475-7516/2014/04/002 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inflation in the early Universe can be followed by a brief period of
preheating, resulting in rapid and non-equilibrium particle production through
the dynamics of parametric resonance. However, the parametric resonance effect
is very sensitive to the linearity of the reheating sector. Additional
self-interactions in... | [
{
"created": "Wed, 11 Dec 2013 00:30:45 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jan 2014 00:08:49 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Apr 2014 16:20:55 GMT",
"version": "v3"
}
] | 2014-04-03 | [
[
"Underwood",
"Bret",
""
],
[
"Zhai",
"Yunxiao",
""
]
] | Inflation in the early Universe can be followed by a brief period of preheating, resulting in rapid and non-equilibrium particle production through the dynamics of parametric resonance. However, the parametric resonance effect is very sensitive to the linearity of the reheating sector. Additional self-interactions in t... | 7.262489 | 7.625855 | 7.232571 | 6.974364 | 7.535589 | 7.598228 | 7.625803 | 7.410442 | 6.892387 | 7.634791 | 6.912209 | 6.930088 | 6.75346 | 6.704928 | 6.876372 | 6.824441 | 6.86563 | 6.860754 | 6.83374 | 6.948458 | 6.688004 |
2012.07710 | Karunava Sil | Karunava Sil | Pole skipping and chaos in anisotropic plasma: a holographic study | 41 pages, 3 figures, Conclusion modified, Accepted for publication in
JHEP | null | 10.1007/JHEP03(2021)232 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Recently, a direct signature of chaos in many body system has been realized
from the energy density retarded Green's function using the phenomenon of `pole
skipping'. Moreover, special locations in the complex frequency and momentum
plane are found, known as the pole skipping points such that the retarded
Green's fun... | [
{
"created": "Mon, 14 Dec 2020 17:02:42 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Dec 2020 16:14:53 GMT",
"version": "v2"
},
{
"created": "Sun, 28 Feb 2021 18:36:34 GMT",
"version": "v3"
}
] | 2021-04-07 | [
[
"Sil",
"Karunava",
""
]
] | Recently, a direct signature of chaos in many body system has been realized from the energy density retarded Green's function using the phenomenon of `pole skipping'. Moreover, special locations in the complex frequency and momentum plane are found, known as the pole skipping points such that the retarded Green's funct... | 14.266654 | 12.332411 | 15.479127 | 12.330789 | 13.660984 | 12.789186 | 13.207724 | 12.580688 | 12.953276 | 15.207897 | 12.22777 | 13.255614 | 13.817292 | 12.687675 | 13.031105 | 13.03916 | 13.009928 | 12.855366 | 12.845347 | 13.778562 | 12.776603 |
hep-th/0608097 | Yannick Meurice | Y. Meurice | At Which Order Should we Truncate Perturbative Series? | 7 pages, 2 figs., talk given at Continuous Advances in QCD 2006 | null | 10.1142/9789812708267_0037 | null | hep-th hep-ph | null | Perturbative coefficients grow factorially with the order and one needs a
prescription to truncate the series in order to obtain a finite result. A
common prescription consists in dropping the smallest contribution at a given
coupling and all the higher orders terms. We discuss the error associated with
this procedur... | [
{
"created": "Tue, 15 Aug 2006 03:08:14 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Meurice",
"Y.",
""
]
] | Perturbative coefficients grow factorially with the order and one needs a prescription to truncate the series in order to obtain a finite result. A common prescription consists in dropping the smallest contribution at a given coupling and all the higher orders terms. We discuss the error associated with this procedure.... | 14.234879 | 15.512427 | 12.982267 | 12.575581 | 14.977406 | 14.330755 | 14.342151 | 15.362713 | 12.784306 | 14.112361 | 14.024068 | 13.865492 | 13.113959 | 12.714959 | 14.080195 | 12.929958 | 12.981144 | 13.508217 | 12.848253 | 13.052217 | 13.48042 |
hep-th/0412228 | Matthias Blau | Matthias Blau, Monica Borunda, Martin O'Loughlin | On the Hagedorn Behaviour of Singular Scale-Invariant Plane Waves | 15 pages, LaTeX2e, v2: JHEP3.cls, one reference added | JHEP 0510 (2005) 047 | 10.1088/1126-6708/2005/10/047 | null | hep-th | null | As a step towards understanding the properties of string theory in
time-dependent and singular spacetimes, we study the divergence of density
operators for string ensembles in singular scale-invariant plane waves, i.e.
those plane waves that arise as the Penrose limits of generic power-law
spacetime singularities. We... | [
{
"created": "Mon, 20 Dec 2004 15:05:09 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Feb 2005 14:20:14 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Blau",
"Matthias",
""
],
[
"Borunda",
"Monica",
""
],
[
"O'Loughlin",
"Martin",
""
]
] | As a step towards understanding the properties of string theory in time-dependent and singular spacetimes, we study the divergence of density operators for string ensembles in singular scale-invariant plane waves, i.e. those plane waves that arise as the Penrose limits of generic power-law spacetime singularities. We s... | 10.31502 | 9.113115 | 11.630708 | 8.836951 | 9.430943 | 8.256101 | 8.570035 | 8.792283 | 9.101206 | 12.43692 | 8.881078 | 9.596736 | 10.138272 | 9.407359 | 9.198215 | 9.202894 | 9.326221 | 9.282014 | 9.16283 | 10.449233 | 9.213141 |
1004.1392 | Pierre Vanhove | Pierre Vanhove | The critical ultraviolet behaviour of N=8 supergravity amplitudes | latex. 5 pages. v2: Added references and minor changes | null | null | IHES/P/10/13, IPHT-T-/10/045 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the critical ultraviolet behaviour of the four-graviton amplitude
in N=8 supergravity to all order in perturbation. We use the
Bern-Carrasco-Johansson diagrammatic expansion for N=8 supergravity multiloop
amplitudes, where numerator factors are squares of the Lorentz factor of N=4
super-Yang-Mills amplitud... | [
{
"created": "Thu, 8 Apr 2010 18:18:18 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Apr 2010 16:41:58 GMT",
"version": "v2"
}
] | 2010-04-15 | [
[
"Vanhove",
"Pierre",
""
]
] | We analyze the critical ultraviolet behaviour of the four-graviton amplitude in N=8 supergravity to all order in perturbation. We use the Bern-Carrasco-Johansson diagrammatic expansion for N=8 supergravity multiloop amplitudes, where numerator factors are squares of the Lorentz factor of N=4 super-Yang-Mills amplitudes... | 7.967535 | 7.975418 | 9.463818 | 7.779462 | 8.240879 | 7.845343 | 8.168221 | 8.205956 | 7.378131 | 8.892302 | 7.843218 | 7.491272 | 7.953615 | 7.692461 | 7.257594 | 7.562947 | 7.597476 | 7.721779 | 7.627053 | 8.276023 | 7.578039 |
hep-th/9805118 | null | M. Caffo, H. Czyz, S. Laporta and E. Remiddi | The Master Differential Equations for the 2-loop Sunrise Selfmass
Amplitudes | 28 pages, Latex, 2 encapsulated Postscript figures with epsfig,
mistype corrected in Eq.(56) | Nuovo Cim.A111:365-389,1998 | null | DFUB 98-5, TP-USL/98/4 | hep-th hep-ph | null | The master differential equations in the external square momentum p^2 for the
master integrals of the two-loop sunrise graph, in n-continuous dimensions and
for arbitrary values of the internal masses, are derived. The equations are
then used for working out the values at p^2 = 0 and the expansions in p^2 at
p^2 =0, ... | [
{
"created": "Tue, 19 May 1998 16:10:45 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Jul 1998 10:37:09 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Caffo",
"M.",
""
],
[
"Czyz",
"H.",
""
],
[
"Laporta",
"S.",
""
],
[
"Remiddi",
"E.",
""
]
] | The master differential equations in the external square momentum p^2 for the master integrals of the two-loop sunrise graph, in n-continuous dimensions and for arbitrary values of the internal masses, are derived. The equations are then used for working out the values at p^2 = 0 and the expansions in p^2 at p^2 =0, in... | 12.87515 | 11.194231 | 8.311218 | 8.735464 | 11.161279 | 11.350947 | 9.853521 | 10.075377 | 9.176305 | 9.878662 | 9.942843 | 9.809541 | 9.172091 | 8.801098 | 10.190878 | 9.870531 | 10.368102 | 9.478801 | 9.141518 | 8.388929 | 10.726954 |
1405.4684 | Jiang Long | Bin Chen and Jiang Long | Strong Subadditivity and Emergent Surface | 18 pages, 8 figures, replace "residual entropy" to "differential
entropy" | Phys. Rev. D 90, 066012 (2014) | 10.1103/PhysRevD.90.066012 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we introduce two bounds which we call the Upper Differential
Entropy and the Lower Differential Entropy for an infinite family of
intervals(strips) in quantum field theory. The two bounds are equal provided
that the theory is translational invariant and the entanglement entropy varies
smoothly with res... | [
{
"created": "Mon, 19 May 2014 11:41:04 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Jun 2014 09:55:09 GMT",
"version": "v2"
}
] | 2014-10-01 | [
[
"Chen",
"Bin",
""
],
[
"Long",
"Jiang",
""
]
] | In this paper, we introduce two bounds which we call the Upper Differential Entropy and the Lower Differential Entropy for an infinite family of intervals(strips) in quantum field theory. The two bounds are equal provided that the theory is translational invariant and the entanglement entropy varies smoothly with respe... | 12.627925 | 10.229078 | 13.628205 | 10.77465 | 10.956325 | 10.851865 | 11.745557 | 11.080108 | 11.417873 | 15.038739 | 11.866379 | 11.131485 | 12.386144 | 11.690279 | 11.252361 | 11.188415 | 11.327126 | 11.536563 | 11.772749 | 12.239247 | 12.160802 |
1109.4903 | Francisco Turrubiates Dr. | Ruben Cordero, Erik Diaz, Hugo Garcia-Compean and Francisco J.
Turrubiates | Quantum string cosmology in the phase space | 12 pages, 4 figures, to appear in the Proceedings of the VIII Mexican
Workshop on Gravitation and Mathematical Physics | null | 10.1063/1.3647533 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Deformation quantization is applied to quantize gravitational systems coupled
with matter. This quantization procedure is performed explicitly for quantum
cosmology of these systems in a flat minisuper(phase)space. The procedure is
employed in a quantum string minisuperspace corresponding to an axion-dilaton
system i... | [
{
"created": "Thu, 22 Sep 2011 18:31:11 GMT",
"version": "v1"
}
] | 2015-05-30 | [
[
"Cordero",
"Ruben",
""
],
[
"Diaz",
"Erik",
""
],
[
"Garcia-Compean",
"Hugo",
""
],
[
"Turrubiates",
"Francisco J.",
""
]
] | Deformation quantization is applied to quantize gravitational systems coupled with matter. This quantization procedure is performed explicitly for quantum cosmology of these systems in a flat minisuper(phase)space. The procedure is employed in a quantum string minisuperspace corresponding to an axion-dilaton system in ... | 13.186984 | 13.387076 | 12.217016 | 10.647263 | 11.624878 | 11.612055 | 12.372175 | 11.14318 | 12.680935 | 13.378165 | 12.127808 | 11.797841 | 11.688596 | 11.279426 | 11.343222 | 11.361057 | 11.4379 | 11.247186 | 11.311585 | 11.567204 | 11.355661 |
1209.6562 | Max Atkin | Max R. Atkin and Stefan Zohren | Analytical approaches to 2D CDT coupled to matter | 4 pages, 2 figure, Based on a talk given at "Gravity, Quantum, and
Black Holes" session of IC-MSQUARE 2012, Budapest, to appear in the
proceedings, IOP Conference Series | J.Phys.Conf.Ser. 410 (2013) 012131 | 10.1088/1742-6596/410/1/012131 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review some recent results by Ambjorn et al. (1202.4435) and the authors
(1202.4322,1203.5034) in which multicritical points of the CDT matrix model
were found and in a particular example identified with a hard dimer model. This
identification requires solving the combinatorial problem of counting
configurations o... | [
{
"created": "Fri, 28 Sep 2012 16:11:33 GMT",
"version": "v1"
}
] | 2013-07-15 | [
[
"Atkin",
"Max R.",
""
],
[
"Zohren",
"Stefan",
""
]
] | We review some recent results by Ambjorn et al. (1202.4435) and the authors (1202.4322,1203.5034) in which multicritical points of the CDT matrix model were found and in a particular example identified with a hard dimer model. This identification requires solving the combinatorial problem of counting configurations of ... | 17.633961 | 17.731621 | 17.729267 | 16.110123 | 16.987339 | 17.030508 | 15.863951 | 15.3587 | 16.070105 | 20.810654 | 15.53782 | 16.01985 | 16.089771 | 15.391137 | 15.015931 | 14.54561 | 14.603564 | 15.917135 | 14.634609 | 17.278368 | 14.391105 |
1505.02381 | Robert Brandenberger | Robert H. Brandenberger (McGill Univ.) | String Gas Cosmology after Planck | Invited review article for the "focus issue" of Classical and Quantum
Gravity : "Planck and the fundamentals of cosmology", 17 pages, 3 figures | null | 10.1088/0264-9381/32/23/234002 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the status of String Gas Cosmology after the 2015 Planck data
release. String gas cosmology predicts an almost scale-invariant spectrum of
cosmological perturbations with a slight red tilt, like the simplest
inflationary models. It also predicts a scale-invariant spectrum of
gravitational waves with a sligh... | [
{
"created": "Sun, 10 May 2015 13:50:44 GMT",
"version": "v1"
}
] | 2015-11-18 | [
[
"Brandenberger",
"Robert H.",
"",
"McGill Univ."
]
] | We review the status of String Gas Cosmology after the 2015 Planck data release. String gas cosmology predicts an almost scale-invariant spectrum of cosmological perturbations with a slight red tilt, like the simplest inflationary models. It also predicts a scale-invariant spectrum of gravitational waves with a slight ... | 4.008945 | 4.016963 | 4.114212 | 3.922693 | 3.870435 | 3.765025 | 3.833511 | 3.81262 | 3.923395 | 4.466989 | 3.955835 | 4.023263 | 4.240314 | 4.059429 | 4.088975 | 4.141171 | 3.933638 | 4.078895 | 4.00498 | 4.04746 | 4.061704 |
0806.0394 | Olaf Lechtenfeld | Tatiana A. Ivanova, Olaf Lechtenfeld | Yang-Mills Instantons and Dyons on Group Manifolds | 1+7 pages | Phys.Lett.B670:91-94,2008 | 10.1016/j.physletb.2008.10.027 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Euclidean SU(N) Yang-Mills theory on the space GxR, where G is a
compact semisimple Lie group, and introduce first-order BPS-type equations
which imply the full Yang-Mills equations. For gauge fields invariant under the
adjoint G-action these BPS equations reduce to first-order matrix equations, to
which ... | [
{
"created": "Mon, 2 Jun 2008 21:00:01 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"Ivanova",
"Tatiana A.",
""
],
[
"Lechtenfeld",
"Olaf",
""
]
] | We consider Euclidean SU(N) Yang-Mills theory on the space GxR, where G is a compact semisimple Lie group, and introduce first-order BPS-type equations which imply the full Yang-Mills equations. For gauge fields invariant under the adjoint G-action these BPS equations reduce to first-order matrix equations, to which we... | 9.054536 | 8.77452 | 9.859189 | 7.77671 | 9.034803 | 8.027268 | 7.753868 | 8.006572 | 8.044201 | 11.015327 | 8.334963 | 8.707478 | 9.206389 | 8.570697 | 8.267665 | 8.49145 | 8.37642 | 8.754255 | 8.621622 | 9.200526 | 8.44542 |
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