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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2404.00877 | Yikun Jiang | Ling-Yan Hung and Yikun Jiang | Building up quantum spacetimes with BCFT Legos | 11 pages, 6 figures, expanded version of essay written for the
Gravity Research Foundation 2024 Awards for Essays on Gravitation | null | null | null | hep-th cond-mat.str-el gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Is it possible to read off the quantum gravity dual of a CFT directly from
its operator algebra? In this essay, we present a step-by-step recipe
synthesizing results and techniques from conformal bootstrap, topological
symmetries, tensor networks, a novel symmetry-preserving real-space
renormalization algorithm devis... | [
{
"created": "Mon, 1 Apr 2024 03:14:36 GMT",
"version": "v1"
}
] | 2024-04-02 | [
[
"Hung",
"Ling-Yan",
""
],
[
"Jiang",
"Yikun",
""
]
] | Is it possible to read off the quantum gravity dual of a CFT directly from its operator algebra? In this essay, we present a step-by-step recipe synthesizing results and techniques from conformal bootstrap, topological symmetries, tensor networks, a novel symmetry-preserving real-space renormalization algorithm devised... | 18.498062 | 20.381113 | 18.864294 | 15.914186 | 18.630583 | 18.309441 | 19.338102 | 17.611897 | 18.162474 | 22.466183 | 17.666681 | 16.428717 | 17.030491 | 16.692993 | 16.228874 | 16.430702 | 16.308088 | 16.578634 | 17.118155 | 17.43796 | 15.689308 |
hep-th/0301098 | Klaus Behrndt | Klaus Behrndt | Intersecting branes from 7-manifolds with G_2 holonomy | 7 pages, Latex, talk presented at the 35th Symposium Ahrenshoop,
August 2002 | Fortsch.Phys. 51 (2003) 664-669 | 10.1002/prop.200310080 | null | hep-th | null | In this talk I discuss intersecting brane configurations coming from explicit
metrics with G_2 holonomy. An example of a 7-manifold which representing a R^3
bundle over a self-dual Einstein space is described and the potential appearing
after compactification over the 6-d twistor space is derived.
| [
{
"created": "Wed, 15 Jan 2003 13:30:42 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Behrndt",
"Klaus",
""
]
] | In this talk I discuss intersecting brane configurations coming from explicit metrics with G_2 holonomy. An example of a 7-manifold which representing a R^3 bundle over a self-dual Einstein space is described and the potential appearing after compactification over the 6-d twistor space is derived. | 21.207378 | 16.362904 | 18.845629 | 16.839333 | 14.336787 | 18.57147 | 16.700666 | 16.187538 | 16.276695 | 21.922123 | 17.480968 | 17.530602 | 18.933838 | 17.922676 | 18.2773 | 17.008968 | 17.540821 | 17.274279 | 18.033957 | 19.399733 | 17.535418 |
hep-th/9410123 | Jorge Stephany Ruiz | R.Gianvittorio, A.Restuccia and J.Stephany | A New Action Principle for Witten's Topological Field Theory | 8 pages, SB/F-94-225 | Phys. Lett. B347 (1995) 279 | 10.1016/0370-2693(95)00061-O | null | hep-th | null | In this letter a new gauge invariant, metric independent action is introduced
from which Witten's Topological Quantum Field Theory may be obtained after
gauge fixing using standard BRST techniques. In our model the BRST algebra of
transformations, under which the effective action is invariant, close off-shell
in dist... | [
{
"created": "Tue, 18 Oct 1994 15:36:45 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Gianvittorio",
"R.",
""
],
[
"Restuccia",
"A.",
""
],
[
"Stephany",
"J.",
""
]
] | In this letter a new gauge invariant, metric independent action is introduced from which Witten's Topological Quantum Field Theory may be obtained after gauge fixing using standard BRST techniques. In our model the BRST algebra of transformations, under which the effective action is invariant, close off-shell in distin... | 16.233929 | 16.187769 | 15.764334 | 14.439137 | 15.789126 | 15.802028 | 14.953474 | 14.481936 | 15.222815 | 18.021013 | 14.902842 | 15.807306 | 15.319722 | 15.006101 | 15.255172 | 15.806029 | 15.339488 | 15.025153 | 15.268581 | 15.334325 | 14.365873 |
hep-th/9412096 | Klaus Lang | Werner Ruehl | Double Scaling Limits and Catastrophes of the zerodimensional O(N)
Vector Sigma Model: The A-Series | 20 pages, LaTeX, two figures available from author on request | null | null | KL-TH-94/21 | hep-th | null | We evaluate the partition functions in the neighbourhood of catastrophes by
saddle point integration and express them in terms of generalized Airy
functions.
| [
{
"created": "Mon, 12 Dec 1994 10:26:57 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Ruehl",
"Werner",
""
]
] | We evaluate the partition functions in the neighbourhood of catastrophes by saddle point integration and express them in terms of generalized Airy functions. | 18.348063 | 11.65333 | 17.682261 | 14.670738 | 14.108267 | 12.408785 | 12.092773 | 12.810744 | 11.491945 | 16.310053 | 13.664831 | 14.337876 | 15.568966 | 14.59986 | 15.101307 | 14.287572 | 13.502731 | 14.298333 | 15.283185 | 16.051872 | 14.37511 |
1106.5503 | Yu Nakayama | Yu Nakayama and Hirosi Ooguri | Comments on Worldsheet Description of the Omega Background | 11 pages | Int. J. Mod. Phys. A 27 (2012) 1250122 | 10.1142/S0217751X12501229 | CALT-68-2837; IPMU11-0094 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Nekrasov's partition function is defined on a flat bundle of R^4 over S^1
called the Omega background. When the fibration is self-dual, the partition
function is known to be equal to the topological string partition function,
which computes scattering amplitudes of self-dual gravitons and graviphotons in
type II supe... | [
{
"created": "Mon, 27 Jun 2011 20:00:04 GMT",
"version": "v1"
}
] | 2012-10-08 | [
[
"Nakayama",
"Yu",
""
],
[
"Ooguri",
"Hirosi",
""
]
] | Nekrasov's partition function is defined on a flat bundle of R^4 over S^1 called the Omega background. When the fibration is self-dual, the partition function is known to be equal to the topological string partition function, which computes scattering amplitudes of self-dual gravitons and graviphotons in type II supers... | 5.962804 | 5.241386 | 6.045787 | 4.937003 | 5.038666 | 5.076295 | 5.330801 | 5.028001 | 5.00737 | 6.135088 | 4.892547 | 4.894924 | 4.891213 | 4.862617 | 5.004999 | 4.98027 | 4.72427 | 4.84335 | 4.928362 | 4.97331 | 4.908866 |
hep-th/9310096 | P. K. Ghosh | Pijush K. Ghosh | Bogomol'nyi Equations of Maxwell-Chern-Simons vortices from a
generalized Abelian Higgs Model | 30 pages(4 figures not included), RevTeX, IP/BBSR/93-62 | Phys.Rev. D49 (1994) 5458-5468 | 10.1103/PhysRevD.49.5458 | null | hep-th | null | We consider a generalization of the abelian Higgs model with a Chern-Simons
term by modifying two terms of the usual Lagrangian. We multiply a dielectric
function with the Maxwell kinetic energy term and incorporate nonminimal
interaction by considering generalized covariant derivative. We show that for a
particular ... | [
{
"created": "Sun, 17 Oct 1993 19:16:57 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ghosh",
"Pijush K.",
""
]
] | We consider a generalization of the abelian Higgs model with a Chern-Simons term by modifying two terms of the usual Lagrangian. We multiply a dielectric function with the Maxwell kinetic energy term and incorporate nonminimal interaction by considering generalized covariant derivative. We show that for a particular ch... | 8.338324 | 8.109521 | 8.613166 | 7.698468 | 8.004772 | 8.145679 | 7.905574 | 8.194342 | 7.36537 | 9.200502 | 7.411119 | 7.648753 | 8.451272 | 7.744571 | 7.799791 | 7.706872 | 8.005831 | 7.753474 | 7.498059 | 8.172188 | 7.841319 |
2103.15168 | Balthazar de Vaulchier | Herv\'e Partouche, Nicolaos Toumbas and Balthazar de Vaulchier | Wavefunction of the universe: Reparametrization invariance and field
redefinitions of the minisuperspace path integral | 1+56 pages, 1 figure | null | 10.1016/j.nuclphysb.2021.115600 | CPHT-RR027.032021 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We consider the Hartle-Hawking wavefunction of the universe defined as a
Euclidean path integral that satisfies the "no-boundary proposal." We focus on
the simplest minisuperspace model that comprises a single scale factor degree
of freedom and a positive cosmological constant. The model can be seen as a
non-linear $... | [
{
"created": "Sun, 28 Mar 2021 16:33:26 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Nov 2021 10:54:19 GMT",
"version": "v2"
}
] | 2021-11-17 | [
[
"Partouche",
"Hervé",
""
],
[
"Toumbas",
"Nicolaos",
""
],
[
"de Vaulchier",
"Balthazar",
""
]
] | We consider the Hartle-Hawking wavefunction of the universe defined as a Euclidean path integral that satisfies the "no-boundary proposal." We focus on the simplest minisuperspace model that comprises a single scale factor degree of freedom and a positive cosmological constant. The model can be seen as a non-linear $\s... | 7.427887 | 7.885362 | 8.091561 | 7.792523 | 7.702581 | 8.24334 | 8.455609 | 7.714575 | 7.613643 | 8.670543 | 7.548389 | 7.507461 | 7.508845 | 7.46637 | 7.357011 | 7.473063 | 7.460058 | 7.400502 | 7.546886 | 7.545471 | 7.365494 |
2003.06823 | Rafael I. Nepomechie | Rafael I. Nepomechie | The $A_m^{(1)}$ Q-system | 13 pages, v2: references added, and appendix removed; v3: more
references added, version to appear in Int. J. Mod. Phys. Lett. A | null | 10.1142/S0217732320502600 | UMTG-307 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a Q-system for the $A_m^{(1)}$ quantum integrable spin chain. We
also find compact determinant expressions for all the Q-functions, both for the
rational and trigonometric cases.
| [
{
"created": "Sun, 15 Mar 2020 13:16:13 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Mar 2020 17:03:01 GMT",
"version": "v2"
},
{
"created": "Sat, 8 Aug 2020 13:48:17 GMT",
"version": "v3"
}
] | 2020-08-11 | [
[
"Nepomechie",
"Rafael I.",
""
]
] | We propose a Q-system for the $A_m^{(1)}$ quantum integrable spin chain. We also find compact determinant expressions for all the Q-functions, both for the rational and trigonometric cases. | 10.687893 | 9.267091 | 13.369913 | 8.938531 | 6.994255 | 7.998803 | 8.084134 | 7.814006 | 7.261037 | 11.660257 | 7.960433 | 8.122005 | 11.134355 | 8.464309 | 7.831281 | 7.628992 | 8.149872 | 8.122078 | 8.000534 | 9.930364 | 7.696561 |
2207.12681 | Yuan Zhong | Yuan Zhong | Singular P\"oschl-Teller II potentials and gravitating kinks | 13 pages, 2 figures. Minor revision of the text, Fig. 2 is redrawn,
and some new references are added | JHEP09(2022)165 | 10.1007/JHEP09(2022)165 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We report a two-dimensional (2D) gravitating kink model, for which both the
background field equations and the linear perturbation equation are exactly
solvable. The background solution describes a sine-Gordon kink that
interpolating between two asymptotic AdS$_2$ spaces, and can be regarded as a
2D thick brane world... | [
{
"created": "Tue, 26 Jul 2022 06:48:06 GMT",
"version": "v1"
},
{
"created": "Sat, 30 Jul 2022 04:35:15 GMT",
"version": "v2"
}
] | 2022-09-22 | [
[
"Zhong",
"Yuan",
""
]
] | We report a two-dimensional (2D) gravitating kink model, for which both the background field equations and the linear perturbation equation are exactly solvable. The background solution describes a sine-Gordon kink that interpolating between two asymptotic AdS$_2$ spaces, and can be regarded as a 2D thick brane world s... | 7.516185 | 5.989083 | 7.31087 | 6.055834 | 6.038479 | 6.0317 | 6.561346 | 6.223079 | 6.21036 | 7.352495 | 6.074128 | 6.421359 | 6.838444 | 6.498879 | 6.534361 | 6.726938 | 6.371047 | 6.37096 | 6.597905 | 6.845496 | 6.247505 |
1005.3581 | Motomu Tsuda | Kazunari Shima and Motomu Tsuda | Phase Transition of NLSUSY Space-Time and Unity of Nature | 12 pages, Talk given at Scale and Duality in Quantum Science
Workshop, Constituents, Fundamental Forces and Symmetries of the Universe
04-06 November, 2009, RIMS-YITP, Kyoto University, Kyoto | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The mysterious relation between the large scale structure of the universe and
the tiny (Planck) scale structure of the particle physics, e.g. the observed
mysterious relation between the (dark) energy density (and the dark matter) of
the universe and the origin of the tiny neutrino mass (and the SUSY breaking
mass sc... | [
{
"created": "Thu, 20 May 2010 03:12:49 GMT",
"version": "v1"
}
] | 2010-05-21 | [
[
"Shima",
"Kazunari",
""
],
[
"Tsuda",
"Motomu",
""
]
] | The mysterious relation between the large scale structure of the universe and the tiny (Planck) scale structure of the particle physics, e.g. the observed mysterious relation between the (dark) energy density (and the dark matter) of the universe and the origin of the tiny neutrino mass (and the SUSY breaking mass scal... | 9.713393 | 9.248513 | 10.094885 | 8.452556 | 9.34992 | 9.255616 | 8.575482 | 8.587967 | 8.669497 | 10.787559 | 9.354092 | 8.890698 | 9.100241 | 9.15862 | 9.140126 | 9.370965 | 9.387023 | 9.071511 | 9.326947 | 9.2708 | 9.582159 |
hep-th/0408093 | Mohammad Shikakhwa | A.Albeed and M.S.Shikakhwa | The Spin Interaction of a Dirac Particle in an Aharonov-Bohm Potential
in First Order Scattering | 9 pages, two figures.Published version. Title and content slightly
modified | Int.J.Theor. Phys. vol.46, pp 405 (2007) | null | null | hep-th math-ph math.MP quant-ph | null | For a Dirac particle in an Aharonov-Bohm (AB) potential, it is shown that the
spin interaction (SI) operator which governs the transitions in the spin sector
of the first order S-matrix is related to one of the generators of rotation in
the spin space of the particle. This operator, which is given by the projection
o... | [
{
"created": "Wed, 11 Aug 2004 19:55:42 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Nov 2007 13:12:31 GMT",
"version": "v2"
}
] | 2007-11-13 | [
[
"Albeed",
"A.",
""
],
[
"Shikakhwa",
"M. S.",
""
]
] | For a Dirac particle in an Aharonov-Bohm (AB) potential, it is shown that the spin interaction (SI) operator which governs the transitions in the spin sector of the first order S-matrix is related to one of the generators of rotation in the spin space of the particle. This operator, which is given by the projection of ... | 9.713678 | 10.695249 | 9.726405 | 9.465075 | 9.959551 | 10.455634 | 9.946033 | 10.950709 | 9.386528 | 10.402586 | 9.469262 | 9.477063 | 9.215321 | 8.974262 | 9.629907 | 9.448721 | 9.328417 | 9.516829 | 9.356185 | 9.097935 | 9.509811 |
0803.3304 | Boris Kosyakov | B. P. Kosyakov | Electromagnetic radiation in even-dimensional spacetimes | 12 pages, no figures, this paper is dedicated to Prof. J. L.
Buchbinder in celebration of his sixtieth birthday; v2: minor misprints are
corrected, a further relevant reference is added | Int.J.Mod.Phys.A23:4695-4708,2008 | 10.1142/S0217751X08041451 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The basic concepts and mathematical constructions of the Maxwell--Lorentz
electrodynamics in flat spacetime of an arbitrary even dimension $d=2n$ are
briefly reviewed. We show that the retarded field strength ${\cal
F}^{(2n)}_{\mu\nu}$ due to a point charge living in a $2n$-dimensional world
can be algebraically expr... | [
{
"created": "Sun, 23 Mar 2008 06:00:19 GMT",
"version": "v1"
},
{
"created": "Mon, 31 Mar 2008 17:45:56 GMT",
"version": "v2"
}
] | 2008-12-25 | [
[
"Kosyakov",
"B. P.",
""
]
] | The basic concepts and mathematical constructions of the Maxwell--Lorentz electrodynamics in flat spacetime of an arbitrary even dimension $d=2n$ are briefly reviewed. We show that the retarded field strength ${\cal F}^{(2n)}_{\mu\nu}$ due to a point charge living in a $2n$-dimensional world can be algebraically expres... | 6.964162 | 7.137089 | 6.971842 | 6.275523 | 7.236216 | 7.265729 | 7.356163 | 6.731162 | 6.636511 | 7.72726 | 6.79638 | 6.71608 | 6.338579 | 6.249539 | 7.008617 | 7.097683 | 6.827565 | 6.507417 | 6.443935 | 6.720264 | 6.80247 |
0707.0405 | Orlando Panella | O. Panella | Casimir-Polder intermolecular forces in minimal length theories | 1 Figure. Version published by Physical Review D. Few references
added, typos corrected | Phys.Rev.D76:045012,2007 | 10.1103/PhysRevD.76.045012 | null | hep-th hep-ph | null | Generalized uncertainty relations are known to provide a minimal length
$\hbar\sqrt{\beta}$. The effect of such minimal length in the Casimir-Polder
interactions between neutral atoms (molecules) is studied. The first order
correction term in the minimal uncertainty parameter is derived and found to
describe an attra... | [
{
"created": "Tue, 3 Jul 2007 12:40:01 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Sep 2007 14:51:03 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Panella",
"O.",
""
]
] | Generalized uncertainty relations are known to provide a minimal length $\hbar\sqrt{\beta}$. The effect of such minimal length in the Casimir-Polder interactions between neutral atoms (molecules) is studied. The first order correction term in the minimal uncertainty parameter is derived and found to describe an attract... | 9.696186 | 10.542198 | 9.155687 | 8.731704 | 9.894698 | 10.848598 | 9.616961 | 9.205861 | 9.230088 | 8.665978 | 9.162837 | 8.756908 | 8.755096 | 8.244106 | 8.398715 | 8.6852 | 9.046867 | 8.896742 | 8.905152 | 9.069873 | 8.886865 |
2312.08275 | Luca Capizzi | Luca Capizzi, Andrei Rotaru | Thermal entanglement in conformal junctions | Minor changes. Published version | JHEP05 (2024) 010 | null | null | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a quantum junction described by a 1+1-dimensional boundary
conformal field theory (BCFT). Our analysis focuses on correlations emerging at
finite temperature, achieved through the computation of entanglement measures.
Our approach relies on characterizing correlation functions of twist fields
using BCFT t... | [
{
"created": "Wed, 13 Dec 2023 16:43:56 GMT",
"version": "v1"
},
{
"created": "Sat, 25 May 2024 07:13:25 GMT",
"version": "v2"
}
] | 2024-05-28 | [
[
"Capizzi",
"Luca",
""
],
[
"Rotaru",
"Andrei",
""
]
] | We consider a quantum junction described by a 1+1-dimensional boundary conformal field theory (BCFT). Our analysis focuses on correlations emerging at finite temperature, achieved through the computation of entanglement measures. Our approach relies on characterizing correlation functions of twist fields using BCFT tec... | 11.077336 | 12.192432 | 12.177618 | 11.252684 | 12.054377 | 11.459737 | 11.549875 | 12.080815 | 11.967298 | 13.953086 | 10.874999 | 11.2364 | 12.009096 | 11.451068 | 11.583099 | 11.750234 | 11.514001 | 11.517908 | 11.151637 | 12.179461 | 11.094292 |
hep-th/9910248 | Paul S. Aspinwall | Paul S. Aspinwall and M. Ronen Plesser | Heterotic String Corrections from the Dual Type II String | 21 pages, 5 figures, refs added | JHEP 0004:025,2000 | 10.1088/1126-6708/2000/04/025 | DUKE-CGTP-99-08 | hep-th | null | We introduce a method of using the a dual type IIA string to compute
alpha'-corrections to the moduli space of heterotic string compactifications.
In particular we study the hypermultiplet moduli space of a heterotic string on
a K3 surface. One application of this machinery shows that type IIB strings
compactified on... | [
{
"created": "Fri, 29 Oct 1999 19:15:47 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Nov 1999 19:25:11 GMT",
"version": "v2"
}
] | 2011-10-11 | [
[
"Aspinwall",
"Paul S.",
""
],
[
"Plesser",
"M. Ronen",
""
]
] | We introduce a method of using the a dual type IIA string to compute alpha'-corrections to the moduli space of heterotic string compactifications. In particular we study the hypermultiplet moduli space of a heterotic string on a K3 surface. One application of this machinery shows that type IIB strings compactified on a... | 8.66829 | 8.362208 | 10.367157 | 8.026177 | 8.517997 | 8.487993 | 8.61363 | 8.249806 | 8.630809 | 10.938446 | 7.945643 | 8.421732 | 8.76564 | 8.47545 | 8.28057 | 8.217916 | 8.455186 | 8.161199 | 8.356895 | 8.559358 | 8.333077 |
1809.04381 | Cheng-Yang Lee | Cheng-Yang Lee | Fermionic degeneracy and non-local contributions in flag-dipole spinors
and mass dimension one fermions | 8 pages. Published in EPJC | Eur. Phys. J. C (2021) 81:90 | 10.1140/epjc/s10052-021-08860-z | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a mass dimension one fermionic field associated with flag-dipole
spinors. These spinors are related to Elko (flag-pole spinors) by a
one-parameter matrix transformation $\mathcal{Z}(z)$ where $z$ is a complex
number. The theory is non-local and non-covariant. While it is possible to
obtain a Lorentz-inva... | [
{
"created": "Wed, 12 Sep 2018 12:34:06 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Feb 2021 07:18:20 GMT",
"version": "v2"
}
] | 2021-02-04 | [
[
"Lee",
"Cheng-Yang",
""
]
] | We construct a mass dimension one fermionic field associated with flag-dipole spinors. These spinors are related to Elko (flag-pole spinors) by a one-parameter matrix transformation $\mathcal{Z}(z)$ where $z$ is a complex number. The theory is non-local and non-covariant. While it is possible to obtain a Lorentz-invari... | 9.315918 | 9.246736 | 8.987795 | 8.750672 | 9.190902 | 8.729154 | 9.442706 | 8.554129 | 8.919771 | 10.189976 | 8.783481 | 8.797353 | 8.916614 | 8.710098 | 8.937029 | 8.945183 | 8.882082 | 9.075442 | 8.74422 | 8.855524 | 8.966245 |
1206.6127 | Josua Groeger | Josua Groeger | Vertex Operators of Super Wilson Loops | 11 pages | Phys. Rev. D 86, 105039 (2012) | 10.1103/PhysRevD.86.105039 | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the supersymmetric Wilson loop as introduced by Caron-Huot, which
attaches to lightlike polygons certain edge and vertex operators, whose shape
is determined by supersymmetry constraints. We state explicit formulas for the
vertex operators to all orders in the Gra{\ss}mann expansion, thus filling a
gap in th... | [
{
"created": "Tue, 26 Jun 2012 21:37:38 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Jun 2012 19:16:54 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Nov 2012 11:47:33 GMT",
"version": "v3"
}
] | 2013-01-24 | [
[
"Groeger",
"Josua",
""
]
] | We study the supersymmetric Wilson loop as introduced by Caron-Huot, which attaches to lightlike polygons certain edge and vertex operators, whose shape is determined by supersymmetry constraints. We state explicit formulas for the vertex operators to all orders in the Gra{\ss}mann expansion, thus filling a gap in the ... | 16.292788 | 13.884169 | 14.820557 | 13.93435 | 11.971533 | 14.565058 | 15.059291 | 12.67456 | 14.547972 | 16.381632 | 15.616103 | 13.77936 | 13.953229 | 13.246854 | 13.815924 | 14.334514 | 13.665725 | 13.710009 | 13.689676 | 13.502202 | 13.644543 |
hep-th/9302069 | null | S. Pratik Khastgir and Jnanadeva Maharana | Topology changing processes and symmetries of string effective action | 23 pages, IP/BBSR/93-8 | Nucl.Phys. B406 (1993) 145-164 | 10.1016/0550-3213(93)90164-K | null | hep-th | null | Wormhole solutions corresponding to space-time geometries $R^1\times
S^1\times S^2$ and $R^1\times S^3$ are obtained from reduced string effective
action and the action is written in a manifestly $O(d,d)$ invariant form. A
general treatment is given for obtaining wormhole solutions of different
topologies from dimens... | [
{
"created": "Sun, 14 Feb 1993 22:08:23 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Khastgir",
"S. Pratik",
""
],
[
"Maharana",
"Jnanadeva",
""
]
] | Wormhole solutions corresponding to space-time geometries $R^1\times S^1\times S^2$ and $R^1\times S^3$ are obtained from reduced string effective action and the action is written in a manifestly $O(d,d)$ invariant form. A general treatment is given for obtaining wormhole solutions of different topologies from dimensio... | 7.460339 | 6.225727 | 7.631903 | 6.769428 | 7.599081 | 7.073629 | 7.134455 | 6.953064 | 6.713019 | 8.304342 | 6.558777 | 7.033011 | 7.205653 | 7.09613 | 7.316175 | 7.043608 | 6.819973 | 7.238531 | 6.928025 | 7.202667 | 6.945351 |
1005.3157 | Nobuyuki Fukui | Nobuyuki Fukui, Kei-Ichi Kondo, Akihiro Shibata and Toru Shinohara | Jackiw-Nohl-Rebbi two-instanton as a source of magnetic monopole loop | 11 pages, 3 figures | Phys.Rev.D82:045015,2010 | 10.1103/PhysRevD.82.045015 | CHIBA-EP-183/KEK Preprint 2010-8 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate that a Jackiw-Nohl-Rebbi solution as the most general
two-instanton generates a circular loop of magnetic monopole in
four-dimensional Euclidean SU(2) Yang-Mills theory, in contrast to the
one-instanton solution in the regular gauge for which no such magnetic monopole
loops exist. These results togethe... | [
{
"created": "Tue, 18 May 2010 11:01:21 GMT",
"version": "v1"
}
] | 2014-11-21 | [
[
"Fukui",
"Nobuyuki",
""
],
[
"Kondo",
"Kei-Ichi",
""
],
[
"Shibata",
"Akihiro",
""
],
[
"Shinohara",
"Toru",
""
]
] | We demonstrate that a Jackiw-Nohl-Rebbi solution as the most general two-instanton generates a circular loop of magnetic monopole in four-dimensional Euclidean SU(2) Yang-Mills theory, in contrast to the one-instanton solution in the regular gauge for which no such magnetic monopole loops exist. These results together ... | 10.443979 | 8.755163 | 11.179586 | 8.943012 | 10.311801 | 8.566488 | 8.823034 | 9.059053 | 9.17903 | 12.152246 | 8.867347 | 9.791787 | 9.617002 | 9.594625 | 10.220319 | 9.686324 | 9.768285 | 10.11284 | 9.606571 | 10.417077 | 9.897067 |
hep-th/0312150 | Leonid Slad | L.M. Slad | Mass Spectra in the Doubly Symmetric Theory of Infinite-Component Fields | 14 pages, 4 figures, 1 table, LaTeX. V3 is a journal version with a
modified Introduction and with another translation into English language of
the title and the text | Theor.Math.Phys. 142 (2005) 15-28; Teor.Mat.Fiz. 142 (2005) 21-36 | null | null | hep-th | null | We consider the problem of the characteristics of mass spectra in the doubly
symmetric theory of fields transforming under the proper Lorentz group
representations decomposable into an infinite direct sum of finite-dimensional
irreducible representations. We show that there exists a range of free
parameters of the th... | [
{
"created": "Sat, 13 Dec 2003 10:15:33 GMT",
"version": "v1"
},
{
"created": "Sat, 20 Dec 2003 10:27:34 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Mar 2005 10:18:16 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Slad",
"L. M.",
""
]
] | We consider the problem of the characteristics of mass spectra in the doubly symmetric theory of fields transforming under the proper Lorentz group representations decomposable into an infinite direct sum of finite-dimensional irreducible representations. We show that there exists a range of free parameters of the theo... | 15.066078 | 12.696875 | 15.740756 | 12.636126 | 12.033656 | 12.533845 | 14.288164 | 12.458169 | 11.720922 | 15.919629 | 12.767961 | 14.131414 | 13.551193 | 13.378816 | 14.193324 | 14.004491 | 14.340762 | 13.894527 | 13.80966 | 14.332179 | 13.755844 |
hep-th/9601047 | Valerie Nowak | Stephen L. Adler | Projective Group Representations in Quaternionic Hilbert Space | 16 pages, no figures, plain Tex | J.Math.Phys. 37 (1996) 2352-2360 | 10.1063/1.531514 | IASSNS-HEP 96/02 | hep-th | null | We extend the discussion of projective group representations in quaternionic
Hilbert space which was given in our recent book. The associativity condition
for quaternionic projective representations is formulated in terms of unitary
operators and then analyzed in terms of their generator structure. The
multi--central... | [
{
"created": "Wed, 10 Jan 1996 20:42:40 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Adler",
"Stephen L.",
""
]
] | We extend the discussion of projective group representations in quaternionic Hilbert space which was given in our recent book. The associativity condition for quaternionic projective representations is formulated in terms of unitary operators and then analyzed in terms of their generator structure. The multi--centralit... | 17.801958 | 20.113913 | 17.730036 | 16.081268 | 20.105396 | 17.041595 | 17.527239 | 17.628378 | 16.188904 | 20.290289 | 17.311262 | 15.993289 | 17.499556 | 17.495842 | 16.974035 | 16.103544 | 16.709181 | 17.259638 | 17.034668 | 17.9191 | 16.263922 |
hep-th/9112018 | Ayrton Zadra | L. Alvarez-Gaume, H. Itoyama, J.L. Manes and A. Zadra | Superloop Equations and Two Dimensional Supergravity | 34 pages | Int.J.Mod.Phys. A7 (1992) 5337-5368 | 10.1142/S0217751X92002441 | null | hep-th | null | We propose a discrete model whose continuum limit reproduces the string
susceptibility and the scaling dimensions of $(2,4m)$-minimal superconformal
models coupled to $2D$-supergravity. The basic assumption in our presentation
is a set of super-Virasoro constraints imposed on the partition function. We
recover the Ne... | [
{
"created": "Mon, 9 Dec 1991 17:18:03 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Alvarez-Gaume",
"L.",
""
],
[
"Itoyama",
"H.",
""
],
[
"Manes",
"J. L.",
""
],
[
"Zadra",
"A.",
""
]
] | We propose a discrete model whose continuum limit reproduces the string susceptibility and the scaling dimensions of $(2,4m)$-minimal superconformal models coupled to $2D$-supergravity. The basic assumption in our presentation is a set of super-Virasoro constraints imposed on the partition function. We recover the Neve... | 12.679541 | 11.230582 | 14.777583 | 11.480643 | 9.807102 | 10.894375 | 10.618315 | 11.609749 | 10.870561 | 19.082514 | 10.469085 | 11.91205 | 13.854155 | 11.970559 | 11.746758 | 11.123118 | 11.67597 | 12.090898 | 12.053563 | 14.150383 | 11.79583 |
1106.5141 | Bin Chen | Bin Chen, Jiang Long and Jun-bao Wu | Spin-3 Topological Massive Gravity | 19 pages. Arguments improved,references added, published version | Phys. Lett. B705(2011)513-520 | 10.1016/j.physletb.2011.10.044 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the spin-3 topological massive gravity(TMG), paying
special attention to its properties at the chiral point. We propose an action
describing the high spin fields coupled to TMG. We discuss the spin-3
fluctuations around the AdS$_3$ vacuum and find that there is an extra local
massive mode, bes... | [
{
"created": "Sat, 25 Jun 2011 14:51:59 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Nov 2011 10:24:39 GMT",
"version": "v2"
}
] | 2020-04-29 | [
[
"Chen",
"Bin",
""
],
[
"Long",
"Jiang",
""
],
[
"Wu",
"Jun-bao",
""
]
] | In this paper, we study the spin-3 topological massive gravity(TMG), paying special attention to its properties at the chiral point. We propose an action describing the high spin fields coupled to TMG. We discuss the spin-3 fluctuations around the AdS$_3$ vacuum and find that there is an extra local massive mode, besid... | 5.213249 | 5.812346 | 5.649256 | 5.226414 | 5.233644 | 5.365499 | 5.560163 | 5.297189 | 5.050367 | 6.172978 | 5.061826 | 5.282362 | 5.290315 | 5.110023 | 5.04865 | 5.342742 | 4.918375 | 5.191529 | 5.068686 | 5.153903 | 5.078595 |
hep-th/0208041 | Umut Gursoy | Umut Gursoy | Vector operators in the BMN correspondence | 46 pages with 24 figures | JHEP 0307 (2003) 048 | 10.1088/1126-6708/2003/07/048 | CTP-MIT-3296 | hep-th | null | We consider a BMN operator with one scalar, phi, and one vector, D_{m}Z,
impurity field and compute the anomalous dimension both at planar and torus
levels. This "mixed" operator corresponds to a string state with two creation
operators which belong to different SO(4) sectors of the background. The
anomalous dimensio... | [
{
"created": "Tue, 6 Aug 2002 06:09:27 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Gursoy",
"Umut",
""
]
] | We consider a BMN operator with one scalar, phi, and one vector, D_{m}Z, impurity field and compute the anomalous dimension both at planar and torus levels. This "mixed" operator corresponds to a string state with two creation operators which belong to different SO(4) sectors of the background. The anomalous dimension ... | 9.5492 | 8.836904 | 11.401419 | 8.49542 | 9.211294 | 8.801471 | 9.325149 | 8.494314 | 8.641852 | 10.41677 | 8.630925 | 9.006701 | 8.851124 | 8.522722 | 8.920873 | 8.930046 | 8.823211 | 8.714053 | 8.997291 | 9.41076 | 8.93706 |
1811.11470 | Ali Mollabashi | M. Reza Mohammadi Mozaffar and Ali Mollabashi | Entanglement Evolution in Lifshitz-type Scalar Theories | 28 pages, v2: a minor clarification, matches JHEP version | null | 10.1007/JHEP01(2019)137 | MPP-2018-282, IPM/P-2018/079 | hep-th cond-mat.stat-mech cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study propagation of entanglement after a mass quench in free scalar
Lifshitz theories. We show that entanglement entropy goes across three distinct
growth regimes before relaxing to a generalized Gibbs ensemble, namely 'initial
rapid growth', 'main linear growth' and 'tortoise saturation'. We show that
although a... | [
{
"created": "Wed, 28 Nov 2018 10:03:16 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jan 2019 13:51:58 GMT",
"version": "v2"
}
] | 2019-02-20 | [
[
"Mozaffar",
"M. Reza Mohammadi",
""
],
[
"Mollabashi",
"Ali",
""
]
] | We study propagation of entanglement after a mass quench in free scalar Lifshitz theories. We show that entanglement entropy goes across three distinct growth regimes before relaxing to a generalized Gibbs ensemble, namely 'initial rapid growth', 'main linear growth' and 'tortoise saturation'. We show that although a w... | 15.846233 | 16.355625 | 17.966906 | 15.424251 | 18.584099 | 15.803083 | 16.45627 | 16.821135 | 15.290927 | 19.226679 | 15.088477 | 15.910089 | 16.425974 | 15.552624 | 15.431243 | 16.061474 | 16.007421 | 15.576083 | 15.36066 | 16.427416 | 15.121058 |
hep-th/9806083 | Yukiko Umeno | Yukiko Umeno, Masahiro Shiroishi, Miki Wadati | Fermionic R-Operator for the Fermion Chain Model | 12 pages, 4 figures | null | 10.1143/JPSJ.67.1930 | null | hep-th | null | The integrability of the one-dimensional (1D) fermion chain model is
investigated in the framework of the Quantum Inverse Scattering Method (QISM).
We introduce a new R-operator for the fermion chain model, which is expressed
in terms of the fermion operators. The R-operator satisfies a new type of the
Yang-Baxter re... | [
{
"created": "Thu, 11 Jun 1998 07:16:36 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Umeno",
"Yukiko",
""
],
[
"Shiroishi",
"Masahiro",
""
],
[
"Wadati",
"Miki",
""
]
] | The integrability of the one-dimensional (1D) fermion chain model is investigated in the framework of the Quantum Inverse Scattering Method (QISM). We introduce a new R-operator for the fermion chain model, which is expressed in terms of the fermion operators. The R-operator satisfies a new type of the Yang-Baxter rela... | 7.018821 | 6.660682 | 7.575012 | 6.424534 | 7.219882 | 7.109636 | 6.897853 | 6.719495 | 6.834443 | 7.715031 | 6.672605 | 6.75096 | 7.015679 | 6.418953 | 6.561561 | 6.963242 | 6.740527 | 6.639482 | 6.772156 | 7.367269 | 6.64572 |
hep-th/9403070 | Brian Dolan | Brian Dolan | Co-Variant Derivatives And The Renormalisation Group | 25 pages PlainTeX, (bdolan@thphys.may.ie) | Int.J.Mod.Phys. A10 (1995) 2439-2466 | 10.1142/S0217751X95001170 | DIAS-STP-94-05 | hep-th cond-mat | null | The renormalisation group equation for $N$-point correlation functions can be
interpreted in a geometrical manner as an equation for Lie transport of
amplitudes in the space of couplings. The vector field generating the
diffeomorphism has components given by the $\beta$-functions of the theory. It
is argued that this... | [
{
"created": "Fri, 11 Mar 1994 18:19:37 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Dolan",
"Brian",
""
]
] | The renormalisation group equation for $N$-point correlation functions can be interpreted in a geometrical manner as an equation for Lie transport of amplitudes in the space of couplings. The vector field generating the diffeomorphism has components given by the $\beta$-functions of the theory. It is argued that this s... | 6.28526 | 6.793379 | 7.080008 | 6.543923 | 6.475609 | 6.816706 | 6.661754 | 6.388054 | 6.51666 | 7.642544 | 6.653473 | 6.320423 | 6.649706 | 6.399669 | 6.634952 | 6.294878 | 6.318719 | 6.417043 | 6.526808 | 6.277815 | 6.307946 |
hep-th/0601020 | El Hassan Saidi | El Hassan Saidi | Topological SL(2) Gauge Theory on Conifold | 42 pages | null | null | null | hep-th | null | Using a two component $SL(2) $ isospinor formalism, we study the link between
conifold $T^{\ast}\mathbb{S}^{3}$ and q-deformed non commutative holomorphic
geometry in complex four dimensions. Then, thinking about conifold as a
projective complex three dimension hypersurface embedded in non compact
$WP^{5}(1,-1,1,-1,1... | [
{
"created": "Wed, 4 Jan 2006 07:40:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Saidi",
"El Hassan",
""
]
] | Using a two component $SL(2) $ isospinor formalism, we study the link between conifold $T^{\ast}\mathbb{S}^{3}$ and q-deformed non commutative holomorphic geometry in complex four dimensions. Then, thinking about conifold as a projective complex three dimension hypersurface embedded in non compact $WP^{5}(1,-1,1,-1,1,-... | 9.717535 | 8.814673 | 10.045877 | 8.749371 | 9.700686 | 9.693748 | 9.098965 | 8.954153 | 8.66927 | 10.298253 | 8.921002 | 9.197706 | 9.491603 | 8.986411 | 9.162081 | 9.291713 | 9.247201 | 8.976781 | 8.772732 | 9.610885 | 9.04824 |
2309.15307 | Yu Nakayama | Yu Nakayama | Functional renormalization group approach to dipolar fixed point which
is scale-invariant but non-conformal | 15 pages | null | null | YITP-23-119 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A dipolar fixed point introduced by Aharony and Fisher is a physical example
of interacting scale-invariant but non-conformal field theories. We find that
the perturbative critical exponents computed in $\epsilon$ expansions violate
the conformal bootstrap bound. We formulate the functional renormalization
group equa... | [
{
"created": "Tue, 26 Sep 2023 23:38:17 GMT",
"version": "v1"
}
] | 2023-09-28 | [
[
"Nakayama",
"Yu",
""
]
] | A dipolar fixed point introduced by Aharony and Fisher is a physical example of interacting scale-invariant but non-conformal field theories. We find that the perturbative critical exponents computed in $\epsilon$ expansions violate the conformal bootstrap bound. We formulate the functional renormalization group equati... | 14.300718 | 14.53677 | 15.524402 | 14.358548 | 13.032851 | 13.703283 | 15.338113 | 12.946215 | 12.837301 | 15.238981 | 12.666401 | 13.232366 | 14.392477 | 13.427241 | 13.029287 | 13.1471 | 13.540146 | 12.520787 | 13.725018 | 14.232975 | 12.399003 |
hep-th/9310111 | Nicola Maggiore | Nicola Maggiore and Martin Schaden | Landau gauge within the Gribov horizon | 17 pages, NYU-TH-93/10/05 | Phys.Rev. D50 (1994) 6616-6625 | 10.1103/PhysRevD.50.6616 | null | hep-th | null | We consider a model which effectively restricts the functional integral of
Yang--Mills theories to the fundamental modular region. Using algebraic
arguments, we prove that this theory has the same divergences as ordinary Yang
Mills theory in the Landau gauge and that it is unitary. The restriction of the
functional i... | [
{
"created": "Mon, 18 Oct 1993 16:07:06 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Maggiore",
"Nicola",
""
],
[
"Schaden",
"Martin",
""
]
] | We consider a model which effectively restricts the functional integral of Yang--Mills theories to the fundamental modular region. Using algebraic arguments, we prove that this theory has the same divergences as ordinary Yang Mills theory in the Landau gauge and that it is unitary. The restriction of the functional int... | 11.12559 | 8.684434 | 10.655638 | 8.496984 | 9.14932 | 8.80901 | 8.353687 | 8.136692 | 8.255148 | 11.0504 | 8.575458 | 9.108164 | 9.46181 | 9.536717 | 9.52007 | 9.740462 | 9.659698 | 9.838902 | 9.132421 | 9.901337 | 9.430429 |
2304.00589 | Leonard Susskind | Leonard Susskind | A Paradox and its Resolution Illustrate Principles of de Sitter
Holography | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Semiclassical gravity and the holographic description of the static patch of
de Sitter space appear to disagree about properties of correlation functions.
Certain holographic correlation functions are necessarily real whereas their
semiclassical counterparts have both real and imaginary parts. The resolution
of this ... | [
{
"created": "Sun, 2 Apr 2023 18:10:05 GMT",
"version": "v1"
}
] | 2023-04-04 | [
[
"Susskind",
"Leonard",
""
]
] | Semiclassical gravity and the holographic description of the static patch of de Sitter space appear to disagree about properties of correlation functions. Certain holographic correlation functions are necessarily real whereas their semiclassical counterparts have both real and imaginary parts. The resolution of this ap... | 11.720154 | 8.856774 | 11.452381 | 8.028727 | 8.319699 | 9.610867 | 8.486128 | 8.272018 | 8.625516 | 13.604906 | 9.67146 | 9.42154 | 10.34605 | 9.93985 | 9.665495 | 9.737977 | 9.16141 | 9.614513 | 9.50374 | 10.044984 | 9.480127 |
hep-th/9503017 | Sung-Kil Yang | T. Eguchi, K. Hori and S.-K. Yang | Topological $\sigma$-Models and Large-$N$ Matrix Integral | 25 pages, phyzzx, no figures | Int.J.Mod.Phys. A10 (1995) 4203 | 10.1016/0920-5632(95)00632-X | UT-700 | hep-th | null | In this paper we describe in some detail the representation of the
topological $CP^1$ model in terms of a matrix integral which we have introduced
in a previous article. We first discuss the integrable structure of the $CP^1$
model and show that it is governed by an extension of the 1-dimensional Toda
hierarchy. We t... | [
{
"created": "Fri, 3 Mar 1995 06:45:26 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Eguchi",
"T.",
""
],
[
"Hori",
"K.",
""
],
[
"Yang",
"S. -K.",
""
]
] | In this paper we describe in some detail the representation of the topological $CP^1$ model in terms of a matrix integral which we have introduced in a previous article. We first discuss the integrable structure of the $CP^1$ model and show that it is governed by an extension of the 1-dimensional Toda hierarchy. We the... | 5.772377 | 5.61502 | 6.617069 | 5.549101 | 5.629572 | 5.760571 | 5.556291 | 5.843258 | 5.693067 | 6.690567 | 5.435392 | 5.569833 | 5.998507 | 5.437635 | 5.713521 | 5.509962 | 5.559373 | 5.459759 | 5.560356 | 5.824807 | 5.624903 |
0903.4827 | Eric R. Bittner | Eric R. Bittner and Jeremy B. Maddox and Donald J. Kouri | A Supersymmetric Approach to Excited States via Quantum Monte Carlo | null | null | null | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present here a supersymmetric (SUSY) approach for determining excitation
energies within the context of a quantum Monte Carlo scheme. By using the fact
that SUSY quantum mechanics gives rises to a series of isospectral
Hamiltonians, we show that Monte Carlo ground-state calculations in the SUSY
partners can be use... | [
{
"created": "Fri, 27 Mar 2009 15:32:23 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Mar 2009 17:36:56 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Jun 2009 18:49:26 GMT",
"version": "v3"
}
] | 2009-06-18 | [
[
"Bittner",
"Eric R.",
""
],
[
"Maddox",
"Jeremy B.",
""
],
[
"Kouri",
"Donald J.",
""
]
] | We present here a supersymmetric (SUSY) approach for determining excitation energies within the context of a quantum Monte Carlo scheme. By using the fact that SUSY quantum mechanics gives rises to a series of isospectral Hamiltonians, we show that Monte Carlo ground-state calculations in the SUSY partners can be used ... | 10.075515 | 10.475718 | 10.420249 | 9.990721 | 10.22215 | 11.140175 | 10.839042 | 9.510565 | 9.720872 | 10.669635 | 9.614375 | 9.989496 | 10.5831 | 10.156491 | 9.86746 | 10.363279 | 10.078833 | 9.912351 | 9.988986 | 10.354018 | 9.903375 |
hep-th/0003212 | J. M. Maillard | S. Boukraa, J-M.Maillard | Let's Baxterise | 38 pages, no figure | null | 10.1023/A:1004842717830 | null | hep-th | null | We recall the concept of Baxterisation of an R-matrix, or of a monodromy
matrix, which corresponds to build, from one point in the $ R$-matrix parameter
space, the algebraic variety where the spectral parameter(s) live. We show that
the Baxterisation, which amounts to studying the iteration of a birational
transforma... | [
{
"created": "Thu, 23 Mar 2000 17:20:32 GMT",
"version": "v1"
}
] | 2015-06-25 | [
[
"Boukraa",
"S.",
""
],
[
"Maillard",
"J-M.",
""
]
] | We recall the concept of Baxterisation of an R-matrix, or of a monodromy matrix, which corresponds to build, from one point in the $ R$-matrix parameter space, the algebraic variety where the spectral parameter(s) live. We show that the Baxterisation, which amounts to studying the iteration of a birational transformati... | 16.952019 | 17.82457 | 22.530577 | 17.155123 | 18.978508 | 20.821655 | 19.055513 | 17.832603 | 19.240059 | 21.20068 | 17.587458 | 16.790787 | 18.137112 | 17.10807 | 17.23119 | 17.340908 | 17.253666 | 17.063742 | 16.850389 | 17.672567 | 16.719801 |
hep-th/0507029 | Kentaroh Yoshida | Hyeonjoon Shin, Kentaroh Yoshida | Thermodynamic Behavior of Fuzzy Membranes in PP-Wave Matrix Model | 13 pages, 4 figures, LaTeX | Phys.Lett. B627 (2005) 188-196 | 10.1016/j.physletb.2005.09.007 | KEK-TH-1021 | hep-th | null | We discuss a two-body interaction of membrane fuzzy spheres in a pp-wave
matrix model at finite temperature by considering a fuzzy sphere rotates with a
constant radius r around the other one sitting at the origin in the SO(6)
symmetric space. This system of two fuzzy spheres is supersymmetric at zero
temperature and... | [
{
"created": "Mon, 4 Jul 2005 00:38:12 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Shin",
"Hyeonjoon",
""
],
[
"Yoshida",
"Kentaroh",
""
]
] | We discuss a two-body interaction of membrane fuzzy spheres in a pp-wave matrix model at finite temperature by considering a fuzzy sphere rotates with a constant radius r around the other one sitting at the origin in the SO(6) symmetric space. This system of two fuzzy spheres is supersymmetric at zero temperature and t... | 10.553782 | 10.899773 | 12.501911 | 10.438695 | 10.751962 | 11.130793 | 10.315248 | 10.03127 | 10.391335 | 12.534999 | 9.775652 | 10.519897 | 11.152514 | 10.320207 | 10.43386 | 10.287612 | 10.213567 | 10.237488 | 10.655508 | 10.681053 | 10.077268 |
1310.6357 | Dario Rosa | Dario Rosa | Generalized geometry of two-dimensional vacua | 31 pages, 1 figure. v2: minor corrections, references added | null | 10.1007/JHEP07(2014)111 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the conditions for unbroken supersymmetry for a Mink_2, (2,0)
vacuum, arising from Type II supergravity on a compact eight-dimensional
manifold M_8. When specialized to internal manifolds enjoying SU(4)xSU(4)
structure the resulting system is elegantly rewritten in terms of generalized
complex geometry. Thi... | [
{
"created": "Wed, 23 Oct 2013 20:00:02 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Dec 2014 11:28:58 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Rosa",
"Dario",
""
]
] | We derive the conditions for unbroken supersymmetry for a Mink_2, (2,0) vacuum, arising from Type II supergravity on a compact eight-dimensional manifold M_8. When specialized to internal manifolds enjoying SU(4)xSU(4) structure the resulting system is elegantly rewritten in terms of generalized complex geometry. This ... | 13.213635 | 13.057325 | 15.056422 | 11.809993 | 13.123574 | 11.394876 | 13.224751 | 11.899566 | 11.952003 | 13.6526 | 11.58732 | 11.906252 | 13.338529 | 11.91142 | 11.997844 | 11.668735 | 11.998933 | 12.163945 | 11.477748 | 13.096431 | 11.793895 |
hep-th/0611227 | Maurizio Gasperini | M. Gasperini | A new scale in the sky | 6 pages, 2 figures included with epsfig. Essay written for the 2006
Awards for Essays on Gravitation (Gravity Research Foundation), and awarded
with "Honorable Mention". To appear in Int. J Mod. Phys. D (December 2006,
Special Issue) | Int.J.Mod.Phys.D15:2147-2152,2006 | 10.1142/S0218271806009480 | CERN-PH-TH/2006-031 | hep-th | null | The existence of a new ultraviolet scale $\Lambda=g M_P$ for effective
theories with gravity and U(1) gauge fields has recently been conjectured as a
possible criterion for distinguishing parts of the swampland from the string
landscape. Here we discuss a possible phenomenological signature of this scale,
for electro... | [
{
"created": "Tue, 21 Nov 2006 18:57:44 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gasperini",
"M.",
""
]
] | The existence of a new ultraviolet scale $\Lambda=g M_P$ for effective theories with gravity and U(1) gauge fields has recently been conjectured as a possible criterion for distinguishing parts of the swampland from the string landscape. Here we discuss a possible phenomenological signature of this scale, for electroma... | 15.658853 | 12.878729 | 13.141105 | 12.381801 | 12.843825 | 12.929652 | 12.51236 | 11.253721 | 12.09594 | 13.561604 | 11.624861 | 12.282912 | 12.892 | 12.68963 | 12.045985 | 11.386057 | 12.567653 | 11.96222 | 12.648077 | 13.543665 | 11.959765 |
hep-th/9606012 | Hitoshi Konno | Hitoshi Konno | Dynamical Correlation Functions and Finite-size Scaling in
Ruijsenaars-Schneider Model | 27 pages, PS file, to be published in Nucl.Phys.B | Nucl.Phys. B473 (1996) 579-600 | 10.1016/0550-3213(96)00208-8 | YITP-96-4 | hep-th | null | The trigonometric Ruijsenaars-Schneider model is diagonalized by means of the
Macdonald symmetric functions. We evaluate the dynamical density-density
correlation function and the one-particle retarded Green function as well as
their thermodynamic limit. Based on these results and finite-size scaling
analysis, we sho... | [
{
"created": "Tue, 4 Jun 1996 08:33:27 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Konno",
"Hitoshi",
""
]
] | The trigonometric Ruijsenaars-Schneider model is diagonalized by means of the Macdonald symmetric functions. We evaluate the dynamical density-density correlation function and the one-particle retarded Green function as well as their thermodynamic limit. Based on these results and finite-size scaling analysis, we show ... | 10.609994 | 8.936832 | 11.099811 | 9.028388 | 10.171215 | 10.653676 | 9.5767 | 9.234207 | 8.452293 | 11.338498 | 9.022494 | 9.341119 | 9.717934 | 9.202573 | 9.063228 | 9.084502 | 9.127841 | 9.094091 | 8.670944 | 9.706344 | 9.21927 |
2407.17384 | Benjamin J. Stone Mr | Benjamin J. Stone | Correlation functions of conserved currents in (super)conformal field
theory | PhD Thesis, 207 pages. Based on arXiv:2102.04827, arXiv:2108.01865,
arXiv:2204.04899, arXiv:2210.13135, arXiv:2302.00593, arXiv:2305.02233 and
arXiv:2307.11435 | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This thesis is dedicated to analysing the general structure of two- and
three-point correlation functions of conserved currents of arbitrary integer or
half-integer spins in three- and four-dimensional (super)conformal field
theory.
| [
{
"created": "Wed, 24 Jul 2024 16:07:45 GMT",
"version": "v1"
}
] | 2024-07-25 | [
[
"Stone",
"Benjamin J.",
""
]
] | This thesis is dedicated to analysing the general structure of two- and three-point correlation functions of conserved currents of arbitrary integer or half-integer spins in three- and four-dimensional (super)conformal field theory. | 8.334977 | 4.918145 | 7.276535 | 5.521537 | 6.222276 | 6.310571 | 5.884369 | 5.340329 | 5.605474 | 8.133727 | 5.455665 | 6.725202 | 7.848471 | 6.694683 | 6.46403 | 6.632364 | 6.597277 | 6.666511 | 6.848262 | 7.760881 | 6.57483 |
1802.05638 | Roldao da Rocha | D. M. Dantas, R. da Rocha, C. A. S. Almeida | Monopoles on string-like models and the Coulomb's law | 14 pages, 7 figures | null | 10.1016/j.physletb.2018.05.003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The t'Hooft-Polyakov monopole mass can be substantially altered, in the thick
GS and HC brane-world setup, and can be employed to constrain the brane
thickness limit. In this work, we comprise a brief review regarding gauge
fields localization in the string-like six dimensional brane-world models
setup. The correctio... | [
{
"created": "Thu, 15 Feb 2018 16:24:47 GMT",
"version": "v1"
}
] | 2018-08-01 | [
[
"Dantas",
"D. M.",
""
],
[
"da Rocha",
"R.",
""
],
[
"Almeida",
"C. A. S.",
""
]
] | The t'Hooft-Polyakov monopole mass can be substantially altered, in the thick GS and HC brane-world setup, and can be employed to constrain the brane thickness limit. In this work, we comprise a brief review regarding gauge fields localization in the string-like six dimensional brane-world models setup. The correction ... | 22.847843 | 19.855358 | 21.556385 | 20.081421 | 20.144539 | 21.731707 | 20.510033 | 18.292864 | 19.653723 | 23.901424 | 19.769199 | 21.274815 | 20.587488 | 20.313105 | 20.143814 | 21.006407 | 20.648521 | 20.265795 | 20.762318 | 20.5935 | 20.227285 |
hep-th/0112085 | Sei-Hoon Moon | Sei-Hoon Moon | Global Black Branes (Extended Global Defects Surrounded by Horizons),
Brane Worlds and the Cosmological Constant | 33 pages, 5 figures | Nucl.Phys. B624 (2002) 327-359 | 10.1016/S0550-3213(01)00657-5 | null | hep-th gr-qc | null | We study global defects coupled to higher-dimensional gravity with a negative
cosmological constant. This paper is mainly devoted to studying global black
brane solutions which are extended global defects surrounded by horizons. We
find series solutions in a few separated regions and confirm numerically that
they can... | [
{
"created": "Tue, 11 Dec 2001 11:06:43 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Moon",
"Sei-Hoon",
""
]
] | We study global defects coupled to higher-dimensional gravity with a negative cosmological constant. This paper is mainly devoted to studying global black brane solutions which are extended global defects surrounded by horizons. We find series solutions in a few separated regions and confirm numerically that they can b... | 7.412889 | 7.346933 | 7.082351 | 6.978243 | 7.077424 | 7.594144 | 7.065432 | 6.943998 | 6.887367 | 7.259976 | 7.169014 | 7.038396 | 7.139529 | 7.031669 | 6.825432 | 6.911337 | 6.955426 | 6.962893 | 6.912504 | 7.258339 | 6.90967 |
1910.11852 | Sebastian Mizera | Sebastian Mizera, Andrzej Pokraka | From Infinity to Four Dimensions: Higher Residue Pairings and Feynman
Integrals | 41 pages, reference added | JHEP 2002 (2020) 159 | 10.1007/JHEP02(2020)159 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a surprising phenomenon in which Feynman integrals in
$D=4-2\varepsilon$ space-time dimensions as $\varepsilon \to 0$ can be fully
characterized by their behavior in the opposite limit, $\varepsilon \to
\infty$. More concretely, we consider vector bundles of Feynman integrals over
kinematic spaces, whose con... | [
{
"created": "Fri, 25 Oct 2019 17:18:21 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Nov 2020 03:51:05 GMT",
"version": "v2"
}
] | 2020-11-03 | [
[
"Mizera",
"Sebastian",
""
],
[
"Pokraka",
"Andrzej",
""
]
] | We study a surprising phenomenon in which Feynman integrals in $D=4-2\varepsilon$ space-time dimensions as $\varepsilon \to 0$ can be fully characterized by their behavior in the opposite limit, $\varepsilon \to \infty$. More concretely, we consider vector bundles of Feynman integrals over kinematic spaces, whose conne... | 8.032088 | 8.216773 | 8.725552 | 7.778042 | 8.522161 | 8.697209 | 8.782351 | 7.656967 | 7.957972 | 9.475813 | 8.139124 | 8.208334 | 8.131571 | 7.92767 | 7.989315 | 7.928482 | 7.961908 | 7.82093 | 7.944592 | 8.255555 | 7.828915 |
2209.15020 | Maximilian Koegler | Maximilian Koegler, Marc Schneider | Vacuum Induced Ground-State Instabilities | 11 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the hydrogen atom's bound state electron as a probe and investigate
the consequences inflicted by time-resolved vacuum effects. Explicitly, we
derive a closed form for the time-dependent modification of the Maxwell
equations emanating from vacuum fluctuations in quantum electrodynamics. As a
consequence, we fi... | [
{
"created": "Thu, 29 Sep 2022 18:00:01 GMT",
"version": "v1"
}
] | 2022-10-03 | [
[
"Koegler",
"Maximilian",
""
],
[
"Schneider",
"Marc",
""
]
] | We use the hydrogen atom's bound state electron as a probe and investigate the consequences inflicted by time-resolved vacuum effects. Explicitly, we derive a closed form for the time-dependent modification of the Maxwell equations emanating from vacuum fluctuations in quantum electrodynamics. As a consequence, we find... | 18.918112 | 19.256742 | 16.675869 | 15.867288 | 18.567585 | 18.465195 | 19.319355 | 17.746441 | 19.388607 | 18.205624 | 16.999067 | 18.590223 | 17.323788 | 17.124908 | 17.464319 | 18.144735 | 17.2666 | 17.637243 | 17.877453 | 18.060509 | 18.012581 |
1210.2585 | Roberto Bonezzi | Roberto Bonezzi | U(N) spinning particles and higher spin fields on Kaehler backgrounds | 5 pages. Based on the talk presented at Conference QFTG 2012, 31 Jul
- 4 Aug 2012. Tomsk, Russia. To appear in Tomsk State Pedagogical University
Bulletin | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this short contribution we will review the quantization of U(N) spinning
particles with complex target spaces, producing equations for higher spin
fields on complex backgrounds. We will focus first on flat complex space, and
subsequently discuss how to extend our model on suitable Kaehler manifolds. In
the final s... | [
{
"created": "Tue, 9 Oct 2012 12:51:37 GMT",
"version": "v1"
}
] | 2012-10-10 | [
[
"Bonezzi",
"Roberto",
""
]
] | In this short contribution we will review the quantization of U(N) spinning particles with complex target spaces, producing equations for higher spin fields on complex backgrounds. We will focus first on flat complex space, and subsequently discuss how to extend our model on suitable Kaehler manifolds. In the final sec... | 18.227339 | 15.937474 | 16.967712 | 14.84952 | 17.45842 | 15.771662 | 16.156166 | 15.299989 | 16.366001 | 18.908024 | 16.37429 | 16.032274 | 17.124029 | 16.2162 | 15.119633 | 15.893544 | 16.048906 | 16.254629 | 16.680443 | 15.789063 | 16.39045 |
2208.09771 | Victoria Abakumova | V. A. Abakumova, S. L. Lyakhovich | Global conserved quantities and unfree gauge symmetry | 6 pages, to appear in PEPAN Letters | null | 10.1134/S1547477122050028 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a class of theories with unfree gauge symmetry, whose gauge
parameters are restricted by differential equations. We demonstrate that such
theories admit global conserved quantities, whose on-shell values are defined
by asymptotics of the fields rather than Cauchy data. The global conserved
quantities can ... | [
{
"created": "Sun, 21 Aug 2022 01:17:59 GMT",
"version": "v1"
}
] | 2022-10-19 | [
[
"Abakumova",
"V. A.",
""
],
[
"Lyakhovich",
"S. L.",
""
]
] | We consider a class of theories with unfree gauge symmetry, whose gauge parameters are restricted by differential equations. We demonstrate that such theories admit global conserved quantities, whose on-shell values are defined by asymptotics of the fields rather than Cauchy data. The global conserved quantities can be... | 15.81746 | 14.139472 | 15.854868 | 13.346237 | 11.7863 | 12.125946 | 11.622611 | 11.548253 | 14.234386 | 19.172289 | 12.979386 | 13.236283 | 14.950925 | 13.711222 | 14.074536 | 13.091486 | 13.665929 | 13.335498 | 14.453586 | 15.034605 | 13.863347 |
hep-th/9812107 | Gaida | R. Gaida, V. Tretyak, Yu. Yaremko (Institute for Condensed Matter
Physics) | Quasi-Relativistic Center-of-Mass Variables in Applications | 12 pages, Latex2e | J.Phys.Condens.Matter 3 (1998) 425-437 | null | null | hep-th | null | Collective center-of-mass variables are introduced in the Lagrangian
formalism of the relativistic classical mechanics of directly interacting
particles. It is shown that the transition to the Hamiltonian formalism leads
to the Bakamjian-Thomas model. The quantum-mechanical system consisting of two
spinless particles... | [
{
"created": "Mon, 14 Dec 1998 11:59:17 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gaida",
"R.",
"",
"Institute for Condensed Matter\n Physics"
],
[
"Tretyak",
"V.",
"",
"Institute for Condensed Matter\n Physics"
],
[
"Yaremko",
"Yu.",
"",
"Institute for Condensed Matter\n Physics"
]
] | Collective center-of-mass variables are introduced in the Lagrangian formalism of the relativistic classical mechanics of directly interacting particles. It is shown that the transition to the Hamiltonian formalism leads to the Bakamjian-Thomas model. The quantum-mechanical system consisting of two spinless particles i... | 10.870797 | 11.281053 | 10.868496 | 10.291945 | 11.783223 | 12.655814 | 11.08917 | 12.480846 | 10.110434 | 13.147432 | 11.110674 | 9.956618 | 10.05493 | 9.895425 | 9.638626 | 9.820926 | 9.513352 | 9.622579 | 9.826931 | 10.516802 | 9.971937 |
hep-th/0007141 | Hiroshi Ishikawa | Hiroshi Ishikawa and Satoshi Watamura (Tohoku University) | Free Field Realization of D-brane in Group Manifold | 23 pages, latex2e with amsmath | JHEP 0008 (2000) 044 | 10.1088/1126-6708/2000/08/044 | TU-595 | hep-th | null | We construct the boundary state for the D-brane in the SU(2) group manifold
directly in terms of the group variables. We propose a matching condition for
the left- and the right-moving sectors including the zero modes that describes
a D-brane of the Neumann-type. The free field realization of the WZW model is
used to... | [
{
"created": "Tue, 18 Jul 2000 11:19:27 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Ishikawa",
"Hiroshi",
"",
"Tohoku University"
],
[
"Watamura",
"Satoshi",
"",
"Tohoku University"
]
] | We construct the boundary state for the D-brane in the SU(2) group manifold directly in terms of the group variables. We propose a matching condition for the left- and the right-moving sectors including the zero modes that describes a D-brane of the Neumann-type. The free field realization of the WZW model is used to o... | 8.230209 | 7.402997 | 8.747942 | 6.942924 | 7.579947 | 7.556357 | 7.964937 | 7.413694 | 7.470595 | 8.628954 | 7.468834 | 7.715281 | 8.393331 | 7.749879 | 7.546388 | 7.592362 | 7.636763 | 7.597748 | 7.728096 | 8.247368 | 7.693461 |
hep-th/0402006 | Bozhidar Zakhariev Iliev | Bozhidar Z. Iliev (Institute for Nuclear Research and Nuclear Energy,
Bulgarian Academy of Sciences, Sofia, Bulgaria) | Lagrangian quantum field theory in momentum picture. I. Free scalar
fields | 56 LaTeX pages. The packages AMS-LaTeX and amsfonts are required. For
related papers, visit the "publication" pages at
http://theo.inrne.bas.bg/~bozho/ | null | null | null | hep-th math-ph math.MP quant-ph | null | The work contains a detailed investigation of free neutral (Hermitian) or
charged (non-Hermitian) scalar fields and the describing them (system of)
Klein-Gordon equation(s) in momentum picture of motion. A form of the field
equation(s) in terms of creation and annihilation operators is derived. An
analysis of the (an... | [
{
"created": "Sun, 1 Feb 2004 08:27:49 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Iliev",
"Bozhidar Z.",
"",
"Institute for Nuclear Research and Nuclear Energy,\n Bulgarian Academy of Sciences, Sofia, Bulgaria"
]
] | The work contains a detailed investigation of free neutral (Hermitian) or charged (non-Hermitian) scalar fields and the describing them (system of) Klein-Gordon equation(s) in momentum picture of motion. A form of the field equation(s) in terms of creation and annihilation operators is derived. An analysis of the (anti... | 13.217287 | 12.060284 | 11.757722 | 10.872422 | 12.194705 | 11.832991 | 12.155512 | 11.05818 | 11.39626 | 12.75942 | 10.63224 | 11.651952 | 11.92509 | 11.230141 | 11.311686 | 11.105924 | 11.271384 | 11.592313 | 11.290672 | 11.491546 | 11.303857 |
hep-th/0611308 | Roberto Zucchini | Roberto Zucchini | BiHermitian Supersymmetric Quantum Mechanics | 45 pages, no figure; new results added in section 8 | Class.Quant.Grav.24:2073-2098,2007 | 10.1088/0264-9381/24/8/009 | DFUB 06 | hep-th math-ph math.DG math.MP | null | BiHermitian geometry, discovered long ago by Gates, Hull and Rocek, is the
most general sigma model target space geometry allowing for (2,2) world sheet
supersymmetry. In this paper, we work out supersymmetric quantum mechanics for
a biHermitian target space. We display the full supersymmetry of the model and
illustr... | [
{
"created": "Tue, 28 Nov 2006 15:26:21 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Dec 2006 10:26:18 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Zucchini",
"Roberto",
""
]
] | BiHermitian geometry, discovered long ago by Gates, Hull and Rocek, is the most general sigma model target space geometry allowing for (2,2) world sheet supersymmetry. In this paper, we work out supersymmetric quantum mechanics for a biHermitian target space. We display the full supersymmetry of the model and illustrat... | 8.84466 | 7.652709 | 10.822271 | 7.677572 | 7.880416 | 8.322826 | 7.742666 | 7.989189 | 7.141944 | 9.629442 | 7.696589 | 7.346781 | 8.974908 | 7.62429 | 7.600463 | 7.865745 | 7.551525 | 7.792592 | 8.01423 | 8.84866 | 7.897828 |
1201.4302 | Sergey Yu. Vernov | E. Elizalde, A. J. Lopez-Revelles, S. D. Odintsov, S. Yu. Vernov | Cosmological models with Yang-Mills fields | 14 pages, v2: refs. added | Phys. Atom. Nucl. 76 (2013) 996-1003 | 10.1134/S1063778813080097 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Cosmological models with an SU(2) Yang-Mills field are studied. For a
specific model with a minimally coupled Yang-Mills Lagrangian, which includes
an arbitrary function of the second-order term and a fourth-order term, a
corresponding reconstruction program is proposed. It is shown that the model
with minimal coupli... | [
{
"created": "Fri, 20 Jan 2012 14:21:53 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Mar 2012 14:00:18 GMT",
"version": "v2"
}
] | 2013-08-27 | [
[
"Elizalde",
"E.",
""
],
[
"Lopez-Revelles",
"A. J.",
""
],
[
"Odintsov",
"S. D.",
""
],
[
"Vernov",
"S. Yu.",
""
]
] | Cosmological models with an SU(2) Yang-Mills field are studied. For a specific model with a minimally coupled Yang-Mills Lagrangian, which includes an arbitrary function of the second-order term and a fourth-order term, a corresponding reconstruction program is proposed. It is shown that the model with minimal coupling... | 6.736905 | 6.025068 | 6.386277 | 6.1266 | 6.2747 | 6.512263 | 6.63961 | 6.165639 | 6.277056 | 6.794202 | 6.513121 | 6.457903 | 6.716624 | 6.449098 | 6.561337 | 6.260853 | 6.405297 | 6.455036 | 6.612202 | 6.537389 | 6.253472 |
1912.06146 | Mohamed Elmi | Philip Candelas, Xenia de la Ossa, Mohamed Elmi and Duco van Straten | A One Parameter Family of Calabi-Yau Manifolds with Attractor Points of
Rank Two | 84 pages, 24 colour figures, 14 tables | null | 10.1007/JHEP10(2020)202 | null | hep-th math.AG math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the process of studying the zeta-function for one parameter families of
Calabi-Yau manifolds we have been led to a manifold, first studied by Verrill,
for which the quartic numerator of the zeta-function factorises into two
quadrics remarkably often. Among these factorisations, we find persistent
factorisations; t... | [
{
"created": "Thu, 12 Dec 2019 19:00:02 GMT",
"version": "v1"
}
] | 2020-12-02 | [
[
"Candelas",
"Philip",
""
],
[
"de la Ossa",
"Xenia",
""
],
[
"Elmi",
"Mohamed",
""
],
[
"van Straten",
"Duco",
""
]
] | In the process of studying the zeta-function for one parameter families of Calabi-Yau manifolds we have been led to a manifold, first studied by Verrill, for which the quartic numerator of the zeta-function factorises into two quadrics remarkably often. Among these factorisations, we find persistent factorisations; the... | 9.782565 | 10.842623 | 11.962246 | 10.173799 | 10.653156 | 10.762498 | 10.811679 | 10.926268 | 10.27909 | 11.762259 | 9.978202 | 9.715165 | 10.010544 | 9.859596 | 10.063105 | 9.865444 | 9.735674 | 9.758032 | 9.773459 | 10.296348 | 9.666824 |
hep-th/9506067 | Anton Kapustin | S.Skorik, A.Kapustin | Surface excitations and surface energy of the antiferromagnetic XXZ
chain by the Bethe ansatz approach | Revtex file with 2 figures. Complementary remarks added | J.Phys.A29:1629-1638,1996 | 10.1088/0305-4470/29/8/011 | USC-95-015, CALT-68-1998 | hep-th | null | We study boundary bound states using the Bethe ansatz formalism for the
finite $XXZ$ $(\Delta>1)$ chain in a boundary magnetic field $h$. Boundary
bound states are represented by the ``boundary strings'' similar to those
described in the work of H.Saleur, S.Skorik. We find that for certain values of
$h$ the ground st... | [
{
"created": "Fri, 9 Jun 1995 21:11:09 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Jun 1995 00:17:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Skorik",
"S.",
""
],
[
"Kapustin",
"A.",
""
]
] | We study boundary bound states using the Bethe ansatz formalism for the finite $XXZ$ $(\Delta>1)$ chain in a boundary magnetic field $h$. Boundary bound states are represented by the ``boundary strings'' similar to those described in the work of H.Saleur, S.Skorik. We find that for certain values of $h$ the ground stat... | 7.878977 | 7.917027 | 9.377288 | 7.964847 | 9.219052 | 8.479514 | 8.351322 | 7.920261 | 7.919085 | 9.205524 | 7.661547 | 7.722449 | 8.346646 | 7.878678 | 7.860079 | 7.79041 | 7.589816 | 7.483587 | 7.822437 | 8.356359 | 7.668188 |
hep-th/0606204 | Yasuhiro Sekino | Ben Freivogel, Yasuhiro Sekino, Leonard Susskind, Chen-Pin Yeh | A Holographic Framework for Eternal Inflation | 53 pages, 7 figures; v2: minor corrections, typos in section 6.2
corrected | Phys.Rev.D74:086003,2006 | 10.1103/PhysRevD.74.086003 | SU-ITP-06-18, OIQP-06-07, UCB-PTH-06/12, LBNL-60518 | hep-th | null | In this paper we provide some circumstantial evidence for a holographic
duality between bubble nucleation in an eternally inflating universe and a
Euclidean conformal field theory. The holographic correspondence (which is
different than Strominger's dS/CFT duality) relates the decay of
(3+1)-dimensional de Sitter spa... | [
{
"created": "Wed, 21 Jun 2006 09:48:50 GMT",
"version": "v1"
},
{
"created": "Sun, 30 Jul 2006 04:35:07 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Freivogel",
"Ben",
""
],
[
"Sekino",
"Yasuhiro",
""
],
[
"Susskind",
"Leonard",
""
],
[
"Yeh",
"Chen-Pin",
""
]
] | In this paper we provide some circumstantial evidence for a holographic duality between bubble nucleation in an eternally inflating universe and a Euclidean conformal field theory. The holographic correspondence (which is different than Strominger's dS/CFT duality) relates the decay of (3+1)-dimensional de Sitter space... | 7.86563 | 8.197765 | 8.624749 | 7.16481 | 7.739429 | 7.504744 | 7.249533 | 7.605465 | 7.623565 | 8.798841 | 7.094748 | 7.289846 | 7.775147 | 7.210123 | 7.439415 | 7.323837 | 7.318818 | 7.25784 | 7.291079 | 7.742856 | 7.355519 |
1503.08607 | Alikram Aliev | Alikram N. Aliev | Superradiance and instability of small rotating charged AdS black holes
in all dimensions | 20 pages, REVTeX; Minor changes, new references added | null | 10.1140/epjc/s10052-016-3902-6 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Rotating small AdS black holes exhibit the superradiant instability to
low-frequency scalar perturbations, which is amenable to a complete analytic
description in four dimensions. In this paper, we extend this description to
all higher dimensions, focusing on slowly rotating charged AdS black holes with
a single angu... | [
{
"created": "Mon, 30 Mar 2015 09:20:03 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Sep 2015 21:34:32 GMT",
"version": "v2"
}
] | 2016-03-23 | [
[
"Aliev",
"Alikram N.",
""
]
] | Rotating small AdS black holes exhibit the superradiant instability to low-frequency scalar perturbations, which is amenable to a complete analytic description in four dimensions. In this paper, we extend this description to all higher dimensions, focusing on slowly rotating charged AdS black holes with a single angula... | 7.715864 | 7.593005 | 7.28689 | 7.312702 | 7.66118 | 7.685301 | 7.979566 | 7.280784 | 7.400606 | 8.026644 | 7.311945 | 7.192864 | 7.164034 | 7.172582 | 7.490815 | 7.406103 | 7.365152 | 7.441766 | 7.247835 | 7.377629 | 7.191984 |
1406.6000 | Sungjay Lee | Jeffrey A. Harvey, David Kutasov and Sungjay Lee | Comments on Quantum Higgs Vacua | 1+13 pages | null | null | EFI-14-20 | hep-th | http://creativecommons.org/licenses/publicdomain/ | We study two-dimensional N=(4,4) supersymmetric gauge theories which do not
have classical Higgs branches, but are believed to have isolated quantum Higgs
vacua. We provide arguments for the existence of such vacua based on brane
dynamics in string theory and the supersymmetric partition sums of the gauge
theories.
| [
{
"created": "Mon, 23 Jun 2014 17:40:11 GMT",
"version": "v1"
}
] | 2014-06-24 | [
[
"Harvey",
"Jeffrey A.",
""
],
[
"Kutasov",
"David",
""
],
[
"Lee",
"Sungjay",
""
]
] | We study two-dimensional N=(4,4) supersymmetric gauge theories which do not have classical Higgs branches, but are believed to have isolated quantum Higgs vacua. We provide arguments for the existence of such vacua based on brane dynamics in string theory and the supersymmetric partition sums of the gauge theories. | 8.025488 | 6.518556 | 8.912837 | 6.344878 | 6.702522 | 6.672377 | 6.57355 | 6.692639 | 6.155435 | 8.867723 | 6.672416 | 6.576554 | 7.959065 | 6.481667 | 6.560807 | 6.594238 | 6.60421 | 6.868398 | 6.646543 | 7.749641 | 6.608005 |
hep-th/9707177 | Francis Vendrell | M.E. Ortiz, F. Vendrell | Thermal radiation in non-static curved spacetimes: quantum mechanical
path integrals and configuration space topology | 20 pages, major revised version, 9 figures, new title | Phys.Rev.D59:084005,1999 | 10.1103/PhysRevD.59.084005 | Imperial/TP/96-97/55 | hep-th gr-qc quant-ph | null | A quantum mechanical path integral derivation is given of a thermal
propagator in non-static Gui spacetime. The thermal nature of the propagator is
understood in terms of homotopically non-trivial paths in the configuration
space appropriate to tortoise coordinates. The connection to thermal emission
from collapsing ... | [
{
"created": "Mon, 21 Jul 1997 12:06:11 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Jun 1998 12:51:49 GMT",
"version": "v2"
}
] | 2009-12-15 | [
[
"Ortiz",
"M. E.",
""
],
[
"Vendrell",
"F.",
""
]
] | A quantum mechanical path integral derivation is given of a thermal propagator in non-static Gui spacetime. The thermal nature of the propagator is understood in terms of homotopically non-trivial paths in the configuration space appropriate to tortoise coordinates. The connection to thermal emission from collapsing bl... | 22.863613 | 18.821434 | 18.584139 | 17.038849 | 17.851894 | 21.644562 | 16.806726 | 17.488962 | 18.646349 | 20.284304 | 19.115227 | 17.480703 | 17.144897 | 16.304695 | 17.794741 | 17.478199 | 17.579174 | 17.235983 | 17.719719 | 16.252874 | 17.346041 |
hep-th/9909199 | Erich Poppitz | Alan Chodos and Erich Poppitz | Warp Factors and Extended Sources in Two Transverse Dimensions | 11 pages, LaTeX; References and acknowledgments added | Phys.Lett.B471:119-127,1999 | 10.1016/S0370-2693(99)01356-8 | YCTP-P26-99 | hep-th hep-ph | null | We study the solutions of the Einstein equations in (d+2)-dimensions,
describing parallel p-branes (p=d-1) in a space with two transverse dimensions
of positive gaussian curvature. These solutions generalize the solutions of
Deser and Jackiw of point particle sources in (2+1)-dimensional gravity with
cosmological con... | [
{
"created": "Tue, 28 Sep 1999 18:48:54 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Sep 1999 17:16:42 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Chodos",
"Alan",
""
],
[
"Poppitz",
"Erich",
""
]
] | We study the solutions of the Einstein equations in (d+2)-dimensions, describing parallel p-branes (p=d-1) in a space with two transverse dimensions of positive gaussian curvature. These solutions generalize the solutions of Deser and Jackiw of point particle sources in (2+1)-dimensional gravity with cosmological const... | 8.691094 | 8.362328 | 8.444551 | 7.448838 | 8.535596 | 7.928468 | 7.71869 | 7.888756 | 7.685728 | 8.692763 | 7.512879 | 7.736401 | 7.952233 | 7.649323 | 7.620074 | 7.934491 | 7.665782 | 7.421916 | 7.932261 | 8.044329 | 7.860581 |
hep-th/9711022 | Alexander Bylev | A.B.Bylev, V.A.Franke, E.V.Prokhvatilov | Zero-mode contribution to the light-front Hamiltonian of Yukawa type
models | 14 pages, Latex, revised version with minor changes, Submitted to
J.Phys.G | J.Phys.G24:939-952,1998 | 10.1088/0954-3899/24/5/003 | null | hep-th | null | Light-front Hamiltonian for Yukawa type models is determined without the
framework of canonical light-front formalism. Special attention is given to the
contribution of zero modes.
| [
{
"created": "Wed, 5 Nov 1997 10:07:00 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Nov 1997 15:09:00 GMT",
"version": "v2"
},
{
"created": "Thu, 13 Nov 1997 08:19:40 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Bylev",
"A. B.",
""
],
[
"Franke",
"V. A.",
""
],
[
"Prokhvatilov",
"E. V.",
""
]
] | Light-front Hamiltonian for Yukawa type models is determined without the framework of canonical light-front formalism. Special attention is given to the contribution of zero modes. | 24.678322 | 18.028412 | 15.303706 | 14.619686 | 22.080389 | 20.843918 | 18.782413 | 17.079203 | 14.231217 | 18.687031 | 15.860868 | 17.466019 | 16.727064 | 17.194077 | 17.602501 | 16.886383 | 16.927837 | 17.567753 | 16.557302 | 16.343927 | 16.568253 |
hep-th/9904042 | Sanefumi Moriyama | Hiroyuki Hata and Sanefumi Moriyama | Conformal Symmetry and A New Gauge in the Matrix Model | 17 pages, LaTeX, no figures; v2: Introduction modified, references
added and typos corrected; v3: Introduction changed; v4: Eq.(12) corrected;
v5: final version to appear in Phys. Rev. D | Phys. Rev. D 60, 126006 (1999) | 10.1103/PhysRevD.60.126006 | KUNS-1568 | hep-th | null | We generalize the background gauge in the Matrix model to propose a new gauge
which is useful for discussing the conformal symmetry. In this gauge, the
special conformal transformation (SCT) as the isometry of the near-horizon
geometry of the D-particle solution is directly reproduced with the correct
coefficient as ... | [
{
"created": "Wed, 7 Apr 1999 06:16:05 GMT",
"version": "v1"
},
{
"created": "Sat, 17 Apr 1999 03:15:36 GMT",
"version": "v2"
},
{
"created": "Fri, 11 Jun 1999 07:06:26 GMT",
"version": "v3"
},
{
"created": "Fri, 16 Jul 1999 05:55:03 GMT",
"version": "v4"
},
{
"cr... | 2016-08-25 | [
[
"Hata",
"Hiroyuki",
""
],
[
"Moriyama",
"Sanefumi",
""
]
] | We generalize the background gauge in the Matrix model to propose a new gauge which is useful for discussing the conformal symmetry. In this gauge, the special conformal transformation (SCT) as the isometry of the near-horizon geometry of the D-particle solution is directly reproduced with the correct coefficient as th... | 11.054982 | 8.219242 | 10.769765 | 9.049786 | 9.247534 | 9.003091 | 9.393683 | 8.765061 | 8.562707 | 12.650553 | 9.690988 | 10.114281 | 10.385259 | 10.36609 | 10.45243 | 10.134425 | 10.050601 | 9.871705 | 10.203073 | 10.725013 | 9.806516 |
1906.10072 | Finnian Gray | Ramiro Cayuso, Finnian Gray, David Kubiznak, Aoibheann Margalit,
Renato Gomes Souza, Leander Thiele | Principal Tensor Strikes Again: Separability of Vector Equations with
Torsion | 8 pages | null | 10.1016/j.physletb.2019.07.007 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many black hole spacetimes with a 3-form field exhibit a hidden symmetry
encoded in a torsion generalization of the principal Killing--Yano tensor. This
tensor determines basic properties of such black holes while also underlying
the separability of the Hamilton--Jacobi, Klein--Gordon, and (torsion-modified)
Dirac fi... | [
{
"created": "Mon, 24 Jun 2019 16:45:07 GMT",
"version": "v1"
}
] | 2019-07-10 | [
[
"Cayuso",
"Ramiro",
""
],
[
"Gray",
"Finnian",
""
],
[
"Kubiznak",
"David",
""
],
[
"Margalit",
"Aoibheann",
""
],
[
"Souza",
"Renato Gomes",
""
],
[
"Thiele",
"Leander",
""
]
] | Many black hole spacetimes with a 3-form field exhibit a hidden symmetry encoded in a torsion generalization of the principal Killing--Yano tensor. This tensor determines basic properties of such black holes while also underlying the separability of the Hamilton--Jacobi, Klein--Gordon, and (torsion-modified) Dirac fiel... | 7.51461 | 7.073548 | 6.887047 | 6.401653 | 6.962934 | 7.111794 | 6.753853 | 6.671872 | 6.995849 | 8.459328 | 6.936099 | 7.520957 | 7.221041 | 6.826297 | 7.561632 | 7.228761 | 7.646785 | 6.793722 | 7.254913 | 6.863493 | 7.409303 |
hep-th/9302118 | Louis Crane | David N. Yetter and Louis Crane | We Are Not Stuck With Gluing | 2 pages | null | null | null | hep-th math.QA | null | We show that the construction of Ocneanu, which yields 1 for any 4D manifold,
is not identical to our construction, which gives different numbers for
different manifolds.
| [
{
"created": "Wed, 24 Feb 1993 20:35:29 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Yetter",
"David N.",
""
],
[
"Crane",
"Louis",
""
]
] | We show that the construction of Ocneanu, which yields 1 for any 4D manifold, is not identical to our construction, which gives different numbers for different manifolds. | 15.905602 | 18.360275 | 16.03768 | 14.921073 | 16.048405 | 16.796175 | 17.115429 | 13.44426 | 14.313565 | 17.380114 | 15.522692 | 16.465776 | 15.666717 | 14.538271 | 14.707866 | 14.11828 | 15.928608 | 15.896477 | 15.692564 | 16.482832 | 14.033573 |
1512.05785 | Piotr Sulkowski | Masahide Manabe, Piotr Su{\l}kowski | Quantum curves and conformal field theory | 90 pages, published version | Phys. Rev. D 95, 126003 (2017) | 10.1103/PhysRevD.95.126003 | CALT-2015-061 | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | To a given algebraic curve we assign an infinite family of quantum curves
(Schr\"odinger equations), which are in one-to-one correspondence with, and
have the structure of, Virasoro singular vectors. For a spectral curve of a
matrix model we build such quantum curves out of an appropriate representation
of the Viraso... | [
{
"created": "Thu, 17 Dec 2015 21:00:10 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Jul 2017 11:48:24 GMT",
"version": "v2"
}
] | 2017-07-07 | [
[
"Manabe",
"Masahide",
""
],
[
"Sułkowski",
"Piotr",
""
]
] | To a given algebraic curve we assign an infinite family of quantum curves (Schr\"odinger equations), which are in one-to-one correspondence with, and have the structure of, Virasoro singular vectors. For a spectral curve of a matrix model we build such quantum curves out of an appropriate representation of the Virasoro... | 10.980671 | 10.837114 | 13.105486 | 10.763779 | 11.911039 | 10.818425 | 11.691572 | 11.466979 | 11.377069 | 14.568222 | 10.3143 | 10.466801 | 11.195955 | 10.310965 | 10.472772 | 10.529887 | 10.667177 | 10.387992 | 10.545189 | 10.69948 | 10.35346 |
1902.01700 | Shin-Ichiro Kumamoto | Ken-Ichi Aoki, Tamao Kobayashi, Shin-Ichiro Kumamoto, Shinnosuke Onai,
Daisuke Sato | Singularity Free Direct Calculation of Spontaneous Mass Generation | null | The Science Reports of Kanazawa University 61(2017) 1 | null | KANAZAWA-18-08 | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new iterative method to directly calculate the spontaneous mass
generation. It is regarded as a new regularization method resembling the finite
volume calculation which assures non-negative fluctuation property at every
stage. We work with the Nambu--Jona-Lasinio model and the strong coupling gauge
theor... | [
{
"created": "Mon, 4 Feb 2019 03:53:06 GMT",
"version": "v1"
}
] | 2019-02-06 | [
[
"Aoki",
"Ken-Ichi",
""
],
[
"Kobayashi",
"Tamao",
""
],
[
"Kumamoto",
"Shin-Ichiro",
""
],
[
"Onai",
"Shinnosuke",
""
],
[
"Sato",
"Daisuke",
""
]
] | We propose a new iterative method to directly calculate the spontaneous mass generation. It is regarded as a new regularization method resembling the finite volume calculation which assures non-negative fluctuation property at every stage. We work with the Nambu--Jona-Lasinio model and the strong coupling gauge theory ... | 19.872303 | 18.621048 | 21.013258 | 19.480631 | 21.537773 | 19.255831 | 19.560928 | 18.874767 | 18.588192 | 20.554798 | 19.532841 | 19.344234 | 18.861443 | 19.048464 | 18.974337 | 18.801584 | 19.401583 | 19.215162 | 18.859688 | 18.683311 | 18.543659 |
hep-th/9706064 | Kyoung Ho Han | Kwanghoon Hahm, KyoungHo Han and H. J. Shin | Composite Skyrme Model with Vector Mesons | LaTeX, 9 pages, 3 figures, to be published in Phys. Rev. D | Phys.Rev. D56 (1997) 1812-1815 | 10.1103/PhysRevD.56.1812 | SNUCTP 97-080 | hep-th | null | We study the composite Skyrme model, proposed by Cheung and G\"{u}rsey,
introducing vector mesons in a chiral Lagrangian. We calculate the static
properties of baryons and compare with results obtained from models without
vector mesons.
| [
{
"created": "Tue, 10 Jun 1997 06:25:48 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Hahm",
"Kwanghoon",
""
],
[
"Han",
"KyoungHo",
""
],
[
"Shin",
"H. J.",
""
]
] | We study the composite Skyrme model, proposed by Cheung and G\"{u}rsey, introducing vector mesons in a chiral Lagrangian. We calculate the static properties of baryons and compare with results obtained from models without vector mesons. | 10.866682 | 9.045992 | 8.055139 | 9.061519 | 8.911199 | 10.579526 | 8.220571 | 10.272235 | 8.504875 | 9.067042 | 8.853117 | 10.271026 | 9.686215 | 9.534258 | 9.711606 | 10.434641 | 9.48556 | 10.149003 | 9.144836 | 9.658377 | 9.966962 |
hep-th/0611279 | Kwang Sik Jeong | Kiwoon Choi, Kwang Sik Jeong | String theoretic QCD axion with stabilized saxion and the pattern of
supersymmetry breaking | JHEP style, 21 pages, 3 figures; typos corrected | JHEP 0701:103,2007 | 10.1088/1126-6708/2007/01/103 | KAIST-TH 2006/11 | hep-th hep-ph | null | String theoretic axion is a prime candidate for the QCD axion solving the
strong CP problem. For a successful realization of the QCD axion in string
theory, one needs to stabilize moduli including the scalar partner (saxion) of
the QCD axion, while keeping the QCD axion unfixed until the low energy QCD
instanton effe... | [
{
"created": "Mon, 27 Nov 2006 05:07:14 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Dec 2006 06:13:46 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Dec 2006 17:20:55 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Choi",
"Kiwoon",
""
],
[
"Jeong",
"Kwang Sik",
""
]
] | String theoretic axion is a prime candidate for the QCD axion solving the strong CP problem. For a successful realization of the QCD axion in string theory, one needs to stabilize moduli including the scalar partner (saxion) of the QCD axion, while keeping the QCD axion unfixed until the low energy QCD instanton effect... | 7.130882 | 6.844206 | 7.236266 | 6.721862 | 7.148254 | 7.159318 | 6.960501 | 6.943764 | 6.934523 | 7.562775 | 6.794302 | 7.098864 | 7.175997 | 6.891516 | 6.837743 | 6.917711 | 7.059493 | 6.836289 | 7.092729 | 6.919018 | 6.774457 |
hep-th/9510073 | Richard Grimm | R. Grimm | Supergravity, Linear Multiplets, and Chern-Simons Forms | null | null | null | null | hep-th | null | Some general features of locally supersymmetric theories (N=1 in four
dimensions) involving Chern-Simons forms and antisymmetric tensors are sketched
out. The relevance of the three-form multiplet both for the description of
Chern-Simons forms and the supersymmetry properties of the gaugino condensate
is pointed out.... | [
{
"created": "Wed, 11 Oct 1995 16:27:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Grimm",
"R.",
""
]
] | Some general features of locally supersymmetric theories (N=1 in four dimensions) involving Chern-Simons forms and antisymmetric tensors are sketched out. The relevance of the three-form multiplet both for the description of Chern-Simons forms and the supersymmetry properties of the gaugino condensate is pointed out. | 11.517406 | 7.60249 | 10.013547 | 8.514589 | 8.646813 | 8.231744 | 9.519993 | 8.23927 | 8.053375 | 9.434524 | 9.148114 | 8.589454 | 9.860593 | 8.79503 | 8.744758 | 8.64945 | 8.731589 | 9.156526 | 8.948343 | 9.939409 | 8.790702 |
hep-th/0512251 | Konstadinos Sfetsos | P.Marios Petropoulos and Konstadinos Sfetsos | NS5-branes on an ellipsis and novel marginal deformations with
parafermions | 24 pages | JHEP0601:167,2006 | 10.1088/1126-6708/2006/01/167 | null | hep-th | null | We consider NS5-branes distributed along the circumference of an ellipsis and
explicitly construct the corresponding gravitational background. This provides
a continuous line of deformations between the limiting cases, considered
before, in which the ellipsis degenerates into a circle or into a bar. We show
that a sl... | [
{
"created": "Tue, 20 Dec 2005 13:26:03 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Petropoulos",
"P. Marios",
""
],
[
"Sfetsos",
"Konstadinos",
""
]
] | We consider NS5-branes distributed along the circumference of an ellipsis and explicitly construct the corresponding gravitational background. This provides a continuous line of deformations between the limiting cases, considered before, in which the ellipsis degenerates into a circle or into a bar. We show that a slig... | 10.551582 | 11.181076 | 11.173529 | 10.200107 | 10.795187 | 11.569705 | 11.277608 | 10.316018 | 10.107599 | 12.566553 | 10.115026 | 10.144235 | 10.568459 | 10.000756 | 9.913823 | 10.124424 | 10.266369 | 9.802136 | 9.725694 | 10.505096 | 10.238955 |
hep-th/9910223 | Heinrich Saller | Heinrich Saller (MPI fuer Physik, Werner-Heisenberg-Institut,
Muenchen) | Duality Induced Reflections and CPT | 18 pages, latex, macros included | Int.J.Theor.Phys. 39 (2000) 321-340 | null | MPI-PhT/99-51 | hep-th | null | The linear particle-antiparticle conjugation $\ty C$ and position space
reflection $\ty P$ as well as the antilinear time reflection $\ty T$ are shown
to be inducable by the selfduality of representations for the operation groups
$\SU(2)$, $\SL(\C^2)$ and $\R$ for spin, Lorentz transformations and time
translations r... | [
{
"created": "Thu, 28 Oct 1999 09:23:45 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Saller",
"Heinrich",
"",
"MPI fuer Physik, Werner-Heisenberg-Institut,\n Muenchen"
]
] | The linear particle-antiparticle conjugation $\ty C$ and position space reflection $\ty P$ as well as the antilinear time reflection $\ty T$ are shown to be inducable by the selfduality of representations for the operation groups $\SU(2)$, $\SL(\C^2)$ and $\R$ for spin, Lorentz transformations and time translations res... | 15.702661 | 15.775949 | 17.354464 | 15.898198 | 16.232639 | 16.033991 | 16.464607 | 16.093973 | 14.371108 | 17.045801 | 13.941966 | 14.336912 | 15.344173 | 14.622308 | 14.816828 | 14.538201 | 14.682695 | 14.701554 | 15.006647 | 14.714905 | 14.370563 |
hep-th/9405081 | Hugo Compean | H. Garcia-Compean, J.F. Plebanski, M. Przanowski | On Self-dual Gravity Structures on Ground Ring Manifolds in
Two-Dimensional String Theory | 17+1 pages, TeX, no figures, corrected ps version | Rev.Mex.Fis.40:547,1994 | null | CINVESTAV-PHYS 06/94 | hep-th | null | We generalize the geometric structures generated by Witten's ground ring. It
is shown that these generalized structures involve in a natural way some
geometric constructions from Self-dual gravity [1,12]. The formal twistor
construction on full quantum ground ring manifold is also given.
| [
{
"created": "Thu, 12 May 1994 16:15:39 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Aug 2001 01:40:52 GMT",
"version": "v2"
}
] | 2011-10-11 | [
[
"Garcia-Compean",
"H.",
""
],
[
"Plebanski",
"J. F.",
""
],
[
"Przanowski",
"M.",
""
]
] | We generalize the geometric structures generated by Witten's ground ring. It is shown that these generalized structures involve in a natural way some geometric constructions from Self-dual gravity [1,12]. The formal twistor construction on full quantum ground ring manifold is also given. | 39.8381 | 33.714489 | 46.032169 | 33.814751 | 37.66674 | 39.746822 | 39.358089 | 39.199715 | 34.101894 | 58.193581 | 36.164509 | 34.57515 | 38.068378 | 33.352844 | 33.557301 | 33.523792 | 35.144077 | 35.831966 | 34.5228 | 40.680447 | 32.819633 |
hep-th/0605014 | Mark Hindmarsh | Mark Hindmarsh and P.M. Saffin | Scaling in a SU(2)/Z_3 model of cosmic superstring networks | 12pp, 3 figs | JHEP0608:066,2006 | 10.1088/1126-6708/2006/08/066 | null | hep-th | null | Motivated by recent developments in superstring theory in the cosmological
context, we examine a field theory which contains string networks with 3-way
junctions. We perform numerical simulations of this model, identify the length
scales of the network that forms, and provide evidence that the length scales
tend towa... | [
{
"created": "Mon, 1 May 2006 15:09:50 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Hindmarsh",
"Mark",
""
],
[
"Saffin",
"P. M.",
""
]
] | Motivated by recent developments in superstring theory in the cosmological context, we examine a field theory which contains string networks with 3-way junctions. We perform numerical simulations of this model, identify the length scales of the network that forms, and provide evidence that the length scales tend toward... | 13.148025 | 13.162995 | 11.778055 | 12.128963 | 12.629421 | 13.145092 | 13.290994 | 12.765765 | 12.508733 | 11.736658 | 12.378327 | 13.132721 | 12.420616 | 12.603501 | 12.496854 | 12.826201 | 12.604527 | 12.70858 | 12.802338 | 13.071738 | 12.273199 |
2312.04206 | Tomoki Nosaka | Sanefumi Moriyama, Tomoki Nosaka | Affine Symmetries for ABJM Partition Function and its Generalization | 37 pages, 5 pdf figures; v2: figure 5 added, published version | null | null | NITEP 191, OCU-PHYS 587 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Partially motivated by the fact that the grand partition function of the ABJM
theory or its generalization is expressed by a spectral operator enjoying
symmetries of the Weyl group, it was found that the grand partition function
satisfies the q-Painleve equation, which is constructed from the affine Weyl
group. In th... | [
{
"created": "Thu, 7 Dec 2023 10:47:06 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Jul 2024 04:54:49 GMT",
"version": "v2"
}
] | 2024-07-24 | [
[
"Moriyama",
"Sanefumi",
""
],
[
"Nosaka",
"Tomoki",
""
]
] | Partially motivated by the fact that the grand partition function of the ABJM theory or its generalization is expressed by a spectral operator enjoying symmetries of the Weyl group, it was found that the grand partition function satisfies the q-Painleve equation, which is constructed from the affine Weyl group. In this... | 10.366015 | 10.63426 | 12.623187 | 9.872795 | 10.969882 | 10.633431 | 9.824343 | 10.002997 | 10.770212 | 11.406139 | 10.019983 | 10.031237 | 10.993433 | 10.418204 | 10.39312 | 10.317445 | 10.110939 | 10.48163 | 10.202485 | 10.787504 | 9.709925 |
2404.03069 | Victor Mishnyakov | V.Mishnyakov, A.Morozov, M.Reva, P.Suprun | From equations in coordinate space to Picard-Fuchs and back | null | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue the development of a position space approach to equations for
Feynman multi-loop integrals. The key idea of the approach is that unintegrated
products of Greens functions in position space are still loop integral in
momentum space. The natural place to start are the famous banana diagrams,
which we explor... | [
{
"created": "Wed, 3 Apr 2024 21:17:25 GMT",
"version": "v1"
}
] | 2024-04-05 | [
[
"Mishnyakov",
"V.",
""
],
[
"Morozov",
"A.",
""
],
[
"Reva",
"M.",
""
],
[
"Suprun",
"P.",
""
]
] | We continue the development of a position space approach to equations for Feynman multi-loop integrals. The key idea of the approach is that unintegrated products of Greens functions in position space are still loop integral in momentum space. The natural place to start are the famous banana diagrams, which we explore ... | 12.369102 | 12.418247 | 13.242041 | 11.627531 | 13.599724 | 12.631848 | 13.611963 | 12.813228 | 12.149529 | 13.378201 | 11.653463 | 11.614733 | 12.493455 | 12.100386 | 12.12924 | 12.196077 | 12.4209 | 11.940997 | 12.116878 | 12.930643 | 11.967823 |
1510.03291 | Leonardo Ospedal | P.C. Malta, L.P.R. Ospedal, K. Veiga and J.A. Helay\"el-Neto | Comparative aspects of spin-dependent interaction potentials for
spin-1/2 and spin-1 matter fields | In this version (v5), a Corrigendum has been added after the
published paper | Adv.High Energy Phys. 2016 (2016) 2531436 | 10.1155/2016/2531436 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper sets out to establish a comparative study between classes of spin-
and velocity-dependent potentials for spin-1/2 and spin-1 matter
currents/sources in the non-relativistic regime. Both (neutral massive) scalar
and vector particles are considered to mediate the interactions between
(pseudo-)scalar sources ... | [
{
"created": "Mon, 12 Oct 2015 14:11:53 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Dec 2015 10:24:42 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Feb 2016 12:59:51 GMT",
"version": "v3"
},
{
"created": "Thu, 9 Jun 2016 19:22:27 GMT",
"version": "v4"
},
{
"cre... | 2017-01-03 | [
[
"Malta",
"P. C.",
""
],
[
"Ospedal",
"L. P. R.",
""
],
[
"Veiga",
"K.",
""
],
[
"Helayël-Neto",
"J. A.",
""
]
] | This paper sets out to establish a comparative study between classes of spin- and velocity-dependent potentials for spin-1/2 and spin-1 matter currents/sources in the non-relativistic regime. Both (neutral massive) scalar and vector particles are considered to mediate the interactions between (pseudo-)scalar sources or... | 14.257238 | 16.53356 | 15.327935 | 14.479935 | 15.515742 | 14.825245 | 13.802106 | 15.448551 | 14.811311 | 15.641719 | 14.211698 | 14.298577 | 14.576581 | 14.156307 | 13.9736 | 14.344855 | 14.125984 | 14.326519 | 14.328162 | 14.753451 | 14.249069 |
hep-th/9701160 | Carlos Naon | M.V.Man\'ias, C.M. Na\'on and M.L.Trobo | Path-integral fermion-boson decoupling at finite temperature | 12 pages, latex, no figures | Phys.Lett. B416 (1998) 157-162 | 10.1016/S0370-2693(97)01293-8 | La Plata 97-01 | hep-th | null | We show how to extend the standard functional approach to bosonisation, based
on a decoupling change of path-integral variables, to the case in which a
finite temperature is considered. As examples, in order to both illustrate and
check the procedure, we derive the thermodynamical partition functions for the
Thirring... | [
{
"created": "Tue, 28 Jan 1997 15:04:49 GMT",
"version": "v1"
}
] | 2016-08-15 | [
[
"Manías",
"M. V.",
""
],
[
"Naón",
"C. M.",
""
],
[
"Trobo",
"M. L.",
""
]
] | We show how to extend the standard functional approach to bosonisation, based on a decoupling change of path-integral variables, to the case in which a finite temperature is considered. As examples, in order to both illustrate and check the procedure, we derive the thermodynamical partition functions for the Thirring a... | 11.414798 | 8.932973 | 10.187316 | 8.807792 | 8.793538 | 8.436805 | 9.036361 | 8.94434 | 8.375314 | 11.419557 | 8.587873 | 9.029114 | 10.626822 | 9.4295 | 9.825595 | 9.664963 | 9.325071 | 9.145776 | 9.770442 | 10.307103 | 9.234349 |
hep-th/0410281 | Filipe Paccetti Correia | Filipe Paccetti Correia, Michael G. Schmidt, Zurab Tavartkiladze | (BPS) Fayet-Iliopoulos Terms in 5D Orbifold SUGRA | LaTeX, 11 pages, 2 figures, extended discussion after (25) and (49),
version published in PLB | Phys.Lett. B613 (2005) 83-90 | 10.1016/j.physletb.2005.03.002 | CERN-PH-TH/2004-211 and HD-THEP-04-42 | hep-th hep-ph | null | We discuss Fayet-Iliopoulos terms in the context of five-dimensional
supergravity compactified on an orbifold. For this purpose we use our
superfield formulation of the off-shell 5D SUGRA. In the case of tuned FI
terms, contrary to other claims, we find BPS solutions which ensure that N=1
supersymmetry is unbroken al... | [
{
"created": "Thu, 28 Oct 2004 17:51:37 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Apr 2005 16:22:24 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Correia",
"Filipe Paccetti",
""
],
[
"Schmidt",
"Michael G.",
""
],
[
"Tavartkiladze",
"Zurab",
""
]
] | We discuss Fayet-Iliopoulos terms in the context of five-dimensional supergravity compactified on an orbifold. For this purpose we use our superfield formulation of the off-shell 5D SUGRA. In the case of tuned FI terms, contrary to other claims, we find BPS solutions which ensure that N=1 supersymmetry is unbroken also... | 10.938213 | 10.454727 | 10.633962 | 9.917551 | 10.258933 | 10.211375 | 10.387995 | 10.01751 | 10.069859 | 12.101019 | 10.105652 | 10.162886 | 10.345417 | 9.830006 | 9.992152 | 10.339878 | 10.25772 | 10.509791 | 9.993663 | 10.364928 | 10.398777 |
hep-th/9706161 | Paul Fendley | Paul Fendley | Excited-state energies and supersymmetric indices | 20 pages, 6 figures, amslatex. Revision adds appendix describing
analogous calculation for a free Dirac fermion. To appear in Advances in
Theoretical and Mathematical Physics | null | null | null | hep-th | null | We study multi-soliton states in two-dimensional N=2 supersymmetric theories.
We calculate their energy exactly as a function of mass and volume in the
simplest integrable N=2 theory, the sine-Gordon model at a particular coupling.
These energies are related to the expectation value $I= tr [\exp(in\pi F)
\exp(-H/T)]$... | [
{
"created": "Tue, 24 Jun 1997 01:54:03 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Sep 1997 21:27:27 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Fendley",
"Paul",
""
]
] | We study multi-soliton states in two-dimensional N=2 supersymmetric theories. We calculate their energy exactly as a function of mass and volume in the simplest integrable N=2 theory, the sine-Gordon model at a particular coupling. These energies are related to the expectation value $I= tr [\exp(in\pi F) \exp(-H/T)]$, ... | 11.695473 | 12.542921 | 15.690887 | 10.823225 | 13.697329 | 14.552673 | 13.268176 | 11.392799 | 11.663609 | 15.123689 | 11.829443 | 11.288898 | 13.288086 | 10.576098 | 10.948637 | 11.579929 | 11.22963 | 11.171609 | 11.527201 | 12.780328 | 10.917729 |
1805.00399 | Dana Stanley Fine | Dana S. Fine and Stephen F. Sawin | Rigorous path integrals for supersymmetric quantum mechanics: completing
the path integral proof of the index theorem | 28 pages, see also arXiv:1605.06982v2 which gives more technical
detail, but less physics overview | null | null | null | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many introductory courses in quantum mechanics include Feynman's time-slicing
definition of the path integral, with a complete derivation of the propagator
in the simplest of cases. However, attempts to generalize this, for instance to
non-quadratic potentials, encounter formidable analytic issues in showing the
succ... | [
{
"created": "Tue, 1 May 2018 15:32:09 GMT",
"version": "v1"
}
] | 2018-05-02 | [
[
"Fine",
"Dana S.",
""
],
[
"Sawin",
"Stephen F.",
""
]
] | Many introductory courses in quantum mechanics include Feynman's time-slicing definition of the path integral, with a complete derivation of the propagator in the simplest of cases. However, attempts to generalize this, for instance to non-quadratic potentials, encounter formidable analytic issues in showing the succes... | 9.115236 | 9.595673 | 10.282318 | 8.695266 | 10.294205 | 10.270925 | 10.000479 | 8.864834 | 9.393159 | 10.250408 | 9.186284 | 8.49405 | 8.813102 | 8.563905 | 8.608625 | 8.689958 | 8.653633 | 8.69188 | 8.636449 | 9.018869 | 8.460198 |
2209.04296 | Yuan-Tai Wang | Yuan-Tai Wang and Wen-Bin Pan | Pole-skipping of Holographic Correlators: Aspects of Gauge Symmetry and
Generalizations | 23 pages; typos and errors are fixed | null | 10.1007/JHEP01(2023)174 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the framework of anti-de Sitter space/conformal field theory (AdS/CFT), we
study the pole-skipping phenomenon of the holographic correlators of boundary
operators. We explore the locations of the pole-skipping points case by case
with the models of $U(1)$-gauged form fields propagating in the asymptotic AdS
bulk o... | [
{
"created": "Fri, 9 Sep 2022 13:43:36 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Apr 2023 13:13:57 GMT",
"version": "v2"
}
] | 2023-04-18 | [
[
"Wang",
"Yuan-Tai",
""
],
[
"Pan",
"Wen-Bin",
""
]
] | In the framework of anti-de Sitter space/conformal field theory (AdS/CFT), we study the pole-skipping phenomenon of the holographic correlators of boundary operators. We explore the locations of the pole-skipping points case by case with the models of $U(1)$-gauged form fields propagating in the asymptotic AdS bulk of ... | 15.818586 | 15.370987 | 15.809515 | 14.153882 | 15.289553 | 15.23562 | 15.284173 | 14.348328 | 13.963799 | 17.109076 | 13.951579 | 14.576766 | 14.95919 | 14.423822 | 14.962592 | 14.924496 | 14.543471 | 14.646019 | 14.18723 | 14.962104 | 14.249616 |
2407.11849 | Carlos Mafra | Carlos R. Mafra | Towards massive field-theory amplitudes from the cohomology of pure
spinor superspace | 14 pages. Compile with xetex to obtain correct offsets for hyperlink
pointers | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By analogy with the formula for the massless string disk amplitudes, we
define massive field-theory tree amplitudes and conjecture that the BRST
cohomology structure of pure spinor superspace fixes their form. We give
evidence by deriving the pure spinor superspace expression of the massive
field-theory n-point tree ... | [
{
"created": "Tue, 16 Jul 2024 15:30:09 GMT",
"version": "v1"
}
] | 2024-07-17 | [
[
"Mafra",
"Carlos R.",
""
]
] | By analogy with the formula for the massless string disk amplitudes, we define massive field-theory tree amplitudes and conjecture that the BRST cohomology structure of pure spinor superspace fixes their form. We give evidence by deriving the pure spinor superspace expression of the massive field-theory n-point tree am... | 9.654976 | 9.814837 | 11.029527 | 8.96689 | 9.762597 | 9.303827 | 9.052859 | 8.88297 | 9.582133 | 11.685431 | 8.312617 | 8.94728 | 9.532945 | 8.515504 | 8.948933 | 9.251622 | 8.655509 | 8.670719 | 9.130736 | 9.547799 | 8.87328 |
0909.1879 | Toshiya Kawai | Toshiya Kawai | Twisted Elliptic Genera of N=2 SCFTs in Two Dimensions | 28 pages; v2 refs added | null | 10.1088/1751-8113/45/39/395401 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The elliptic genera of two-dimensional N=2 superconformal field theories can
be twisted by the action of the integral Heisenberg group if their U(1) charges
are fractional. The basic properties of the resulting twisted elliptic genera
and the associated twisted Witten indices are investigated with due attention
to th... | [
{
"created": "Thu, 10 Sep 2009 07:44:25 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Sep 2009 07:00:47 GMT",
"version": "v2"
}
] | 2015-05-14 | [
[
"Kawai",
"Toshiya",
""
]
] | The elliptic genera of two-dimensional N=2 superconformal field theories can be twisted by the action of the integral Heisenberg group if their U(1) charges are fractional. The basic properties of the resulting twisted elliptic genera and the associated twisted Witten indices are investigated with due attention to thei... | 10.508609 | 10.960052 | 11.987962 | 9.443543 | 10.148052 | 10.386534 | 10.856515 | 10.780457 | 10.469994 | 13.880899 | 10.374036 | 9.893724 | 11.470458 | 10.149304 | 10.024518 | 9.710453 | 10.021532 | 9.988639 | 10.017921 | 11.389806 | 9.971602 |
hep-th/0501012 | Shesansu Pal | Shesansu Pal | A new Ricci flat geometry | 7pp, Kahlerian behavior is mentioned in section 2, along with two
references and a note | Phys.Lett. B614 (2005) 201-206 | 10.1016/j.physletb.2005.03.077 | null | hep-th | null | We are proposing a new Ricci flat metric constructed from an infinite family
of Sasaki-Einstein, $Y^{(p,q)}$, geometries. This geometry contains a free
parameter $s$ and in the $s\to 0$ limit we get back the usual CY. When this
geometry is probed both by a stack of D3 and fractional D3 branes then the
corresponding s... | [
{
"created": "Mon, 3 Jan 2005 20:19:17 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jan 2005 17:33:56 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Pal",
"Shesansu",
""
]
] | We are proposing a new Ricci flat metric constructed from an infinite family of Sasaki-Einstein, $Y^{(p,q)}$, geometries. This geometry contains a free parameter $s$ and in the $s\to 0$ limit we get back the usual CY. When this geometry is probed both by a stack of D3 and fractional D3 branes then the corresponding sup... | 11.982792 | 11.313493 | 12.947992 | 10.684051 | 11.266428 | 11.120204 | 11.126874 | 10.903461 | 11.000937 | 13.602935 | 10.547559 | 10.418428 | 11.477921 | 10.422078 | 10.385214 | 10.331318 | 10.380271 | 10.84141 | 10.225023 | 11.851428 | 10.579722 |
hep-th/0306060 | Victor Red'kov | V.M. Red'kov | Monopole BPS-Solutions of the Yang-Mills Equations in Space of Euclid,
Riemann, and Lobachevski | 7 pages | null | null | null | hep-th | null | Procedure of finding of the Bogomolny-Prasad-Sommerfield monopole solutions
in the Georgi-Glashow model is investigated in detail on the backgrounds of
three space models of constant curvature: Euclid, Riemann, Lobachevski's.
Classification of possible solutions is given. It is shown that among all
solutions there ex... | [
{
"created": "Sat, 7 Jun 2003 07:40:16 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Red'kov",
"V. M.",
""
]
] | Procedure of finding of the Bogomolny-Prasad-Sommerfield monopole solutions in the Georgi-Glashow model is investigated in detail on the backgrounds of three space models of constant curvature: Euclid, Riemann, Lobachevski's. Classification of possible solutions is given. It is shown that among all solutions there exis... | 15.294029 | 15.32507 | 16.297878 | 14.529587 | 16.747633 | 15.612854 | 16.656307 | 14.656359 | 15.615836 | 15.844436 | 14.82256 | 14.662447 | 14.331681 | 14.029757 | 14.155913 | 14.335634 | 13.820392 | 14.136935 | 14.623608 | 14.977445 | 14.742344 |
0708.0022 | Jeff Jones | T. Banks, S. Echols, J. L. Jones | Embedding the Pentagon | 39 pages | JHEP 0710:105,2007 | 10.1088/1126-6708/2007/10/105 | scipp-07/13 | hep-th hep-ph | null | The Pentagon Model is an explicit supersymmetric extension of the Standard
Model, which involves a new strongly-interacting SU(5) gauge theory at
TeV-scale energies. We show that the Pentagon can be embedded into an SU(5) x
SU(5) x SU(5) gauge group at the GUT scale. The doublet-triplet splitting
problem, and proton ... | [
{
"created": "Tue, 31 Jul 2007 20:52:07 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Sep 2007 23:08:05 GMT",
"version": "v2"
}
] | 2009-11-18 | [
[
"Banks",
"T.",
""
],
[
"Echols",
"S.",
""
],
[
"Jones",
"J. L.",
""
]
] | The Pentagon Model is an explicit supersymmetric extension of the Standard Model, which involves a new strongly-interacting SU(5) gauge theory at TeV-scale energies. We show that the Pentagon can be embedded into an SU(5) x SU(5) x SU(5) gauge group at the GUT scale. The doublet-triplet splitting problem, and proton de... | 7.621255 | 6.520828 | 7.430636 | 6.454893 | 6.580568 | 6.34262 | 6.534278 | 6.337999 | 6.109857 | 7.468307 | 7.127567 | 7.243352 | 6.990365 | 6.886184 | 6.707025 | 7.153505 | 6.955736 | 7.046375 | 6.80548 | 6.995467 | 7.32988 |
1411.5627 | Xiao Mei Kuang | Xiao-Mei Kuang, Eleftherios Papantonopoulos, Bin Wang, Jian-Pin Wu | Dynamically generated gap from holography in the charged black brane
with hyperscaling violation | 17 pages,8 figures,version published in JHEP. arXiv admin note: text
overlap with arXiv:1409.2945 | JHEP 04(2015)137 | 10.1007/JHEP04(2015)137 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We holographically investigate the effects of a dipole coupling between a
fermion field and a $U(1)$ gauge field on the dual fermionic sector in the
charged gravity bulk with hyperscaling violation. We analytically study the
features of the ultraviolet and infrared Green's functions of the dual
fermionic system and w... | [
{
"created": "Thu, 20 Nov 2014 18:06:35 GMT",
"version": "v1"
},
{
"created": "Mon, 4 May 2015 08:50:22 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Kuang",
"Xiao-Mei",
""
],
[
"Papantonopoulos",
"Eleftherios",
""
],
[
"Wang",
"Bin",
""
],
[
"Wu",
"Jian-Pin",
""
]
] | We holographically investigate the effects of a dipole coupling between a fermion field and a $U(1)$ gauge field on the dual fermionic sector in the charged gravity bulk with hyperscaling violation. We analytically study the features of the ultraviolet and infrared Green's functions of the dual fermionic system and we ... | 9.165795 | 7.173552 | 9.307115 | 7.823301 | 7.694613 | 7.687053 | 8.013073 | 7.509161 | 7.140388 | 9.81457 | 7.307508 | 8.12429 | 8.487506 | 8.309318 | 8.312947 | 8.042617 | 8.049008 | 8.024442 | 8.135608 | 8.779911 | 8.000786 |
1709.09222 | Nobuchika Okada | Anish Ghoshal, Anupam Mazumdar, Nobuchika Okada, Desmond Villalba | On the Stability of Infinite Derivative Abelian Higgs | 7 pages, 2 figures, the version accepted for publication in Physical
Review D | Phys. Rev. D 97, 076011 (2018) | 10.1103/PhysRevD.97.076011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the stringy effects by modifying the local kinetic term of an
Abelian Higgs field by the Gaussian kinetic term we show that the Higgs field
does not possess any instability, the Yukawa coupling between the scalar and
the fermion, the gauge coupling, and the self interaction of the Higgs yields
exponentia... | [
{
"created": "Tue, 26 Sep 2017 19:01:08 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Oct 2017 13:44:42 GMT",
"version": "v2"
},
{
"created": "Sat, 7 Apr 2018 22:16:38 GMT",
"version": "v3"
}
] | 2018-05-02 | [
[
"Ghoshal",
"Anish",
""
],
[
"Mazumdar",
"Anupam",
""
],
[
"Okada",
"Nobuchika",
""
],
[
"Villalba",
"Desmond",
""
]
] | Motivated by the stringy effects by modifying the local kinetic term of an Abelian Higgs field by the Gaussian kinetic term we show that the Higgs field does not possess any instability, the Yukawa coupling between the scalar and the fermion, the gauge coupling, and the self interaction of the Higgs yields exponentiall... | 17.178947 | 18.145676 | 17.374313 | 16.430855 | 16.788057 | 17.453817 | 18.5795 | 17.850115 | 16.708332 | 17.03093 | 16.066006 | 16.009682 | 15.764653 | 15.711934 | 16.050629 | 16.036415 | 15.753653 | 16.263138 | 15.493394 | 16.139122 | 15.356455 |
1909.09208 | William Divine Linch III | Katrin Becker, Melanie Becker, Daniel Butter, William D. Linch III,
Stephen Randall | Five-dimensional Supergravity in N = 1/2 Superspace | Published version. Contains improvements over v1 including relation
to new-minimal supergravity and various formulations of off-shell 5D, N=1
supergravity | null | 10.1007/JHEP03(2020)098 | MI-TH-191 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct 5D, N = 1 supergravity in a 4D, N = 1 superspace with an extra
bosonic coordinate. This represents four of the supersymmetries and the
associated Poincar\'e symmetries manifestly. The remaining four supersymmetries
and the rest of the Poincar\'e symmetries are represented linearly but not
manifestly. In ... | [
{
"created": "Thu, 19 Sep 2019 19:36:17 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Apr 2020 13:13:57 GMT",
"version": "v2"
}
] | 2020-04-22 | [
[
"Becker",
"Katrin",
""
],
[
"Becker",
"Melanie",
""
],
[
"Butter",
"Daniel",
""
],
[
"Linch",
"William D.",
"III"
],
[
"Randall",
"Stephen",
""
]
] | We construct 5D, N = 1 supergravity in a 4D, N = 1 superspace with an extra bosonic coordinate. This represents four of the supersymmetries and the associated Poincar\'e symmetries manifestly. The remaining four supersymmetries and the rest of the Poincar\'e symmetries are represented linearly but not manifestly. In th... | 6.645584 | 5.888641 | 7.416335 | 6.002926 | 6.17296 | 6.464814 | 6.122875 | 6.118771 | 6.159422 | 7.932953 | 5.968501 | 6.271108 | 6.849426 | 6.134113 | 6.163424 | 6.191479 | 6.101787 | 6.236724 | 6.047575 | 7.02624 | 6.15482 |
hep-th/0205225 | Xin-zhou Li | Xin-zhou Li and Xiang-hua Zhai | Rigorous proof of attractive nature for Casimir force of p-odd hypercube | 7 pages, no figure | J. Phys A: Math. Gen. 34 (2001)11053-11057 | 10.1088/0305-4470/34/49/320 | null | hep-th | null | The Casimir effect giving rise to an attractive force between the
configuration boundaries that confine the massless scalar field is rigorously
proven for odd dimensional hypercube with the Dirichlet boundary conditions and
different spacetime dimensions D by the Epstein zeta function regularization.
| [
{
"created": "Wed, 22 May 2002 04:19:38 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Li",
"Xin-zhou",
""
],
[
"Zhai",
"Xiang-hua",
""
]
] | The Casimir effect giving rise to an attractive force between the configuration boundaries that confine the massless scalar field is rigorously proven for odd dimensional hypercube with the Dirichlet boundary conditions and different spacetime dimensions D by the Epstein zeta function regularization. | 19.383957 | 15.985549 | 16.280634 | 17.702728 | 15.18307 | 15.983637 | 17.064127 | 14.472614 | 15.195717 | 20.217491 | 16.250656 | 15.816642 | 16.834049 | 15.564338 | 15.382975 | 16.195845 | 16.492617 | 15.611179 | 15.664323 | 16.738291 | 14.913391 |
2405.19409 | Vivek Saxena | Vivek Saxena | A T-Duality of Non-Supersymmetric Heterotic Strings and an implication
for Topological Modular Forms | 26 pages + appendices; references updated | null | null | null | hep-th math-ph math.AT math.MP | http://creativecommons.org/licenses/by/4.0/ | Motivated by recent developments connecting non-supersymmetric heterotic
string theory to the theory of Topological Modular Forms (TMF), we show that
the worldsheet theory with central charge $(17,\frac{3}{2})$ obtained by
fibering the $(E_8)_1 \times (E_8)_1$ current algebra over the
$\mathcal{N}=(0,1)$ sigma model ... | [
{
"created": "Wed, 29 May 2024 18:00:11 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jun 2024 04:59:55 GMT",
"version": "v2"
}
] | 2024-06-11 | [
[
"Saxena",
"Vivek",
""
]
] | Motivated by recent developments connecting non-supersymmetric heterotic string theory to the theory of Topological Modular Forms (TMF), we show that the worldsheet theory with central charge $(17,\frac{3}{2})$ obtained by fibering the $(E_8)_1 \times (E_8)_1$ current algebra over the $\mathcal{N}=(0,1)$ sigma model on... | 8.288768 | 7.908125 | 10.16634 | 8.296278 | 8.584642 | 8.851366 | 8.993304 | 8.680008 | 8.248244 | 9.496177 | 7.984619 | 8.083162 | 8.724109 | 8.230231 | 8.128477 | 8.42428 | 8.214973 | 8.403257 | 8.064429 | 8.73029 | 8.067863 |
1808.05648 | Oren Bergman Prof. | Eran Avraham and Oren Bergman | A note on D0-branes and instantons in 5d supersymmetric gauge theories | 30 pages, 6 figures. Typos corrected | null | 10.1007/JHEP11(2018)183 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We refine a previous proposal for obtaining the multi-instanton partition
function from the supersymmetric index of the 1d supersymmetric gauge theory on
the worldline of D0-branes. We provide examples where the refinements are
crucial for obtaining the correct result.
| [
{
"created": "Thu, 16 Aug 2018 19:11:14 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Nov 2018 15:38:10 GMT",
"version": "v2"
}
] | 2018-12-26 | [
[
"Avraham",
"Eran",
""
],
[
"Bergman",
"Oren",
""
]
] | We refine a previous proposal for obtaining the multi-instanton partition function from the supersymmetric index of the 1d supersymmetric gauge theory on the worldline of D0-branes. We provide examples where the refinements are crucial for obtaining the correct result. | 11.906713 | 9.579849 | 10.007198 | 8.539067 | 8.580131 | 8.677374 | 8.505138 | 8.431561 | 8.389929 | 11.049037 | 8.601147 | 9.365728 | 10.501195 | 9.360057 | 9.265167 | 9.696787 | 9.381231 | 9.79171 | 9.351623 | 9.960555 | 9.07148 |
1010.5240 | Adam Brown | Adam R. Brown and Alex Dahlen | Bubbles of Nothing and the Fastest Decay in the Landscape | 18 pages, 8 figures; v2: minor changes | Phys.Rev.D84:043518,2011 | 10.1103/PhysRevD.84.043518 | PUPT-2357 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The rate and manner of vacuum decay are calculated in an explicit flux
compactification, including all thick-wall and gravitational effects. For
landscapes built of many units of a single flux, the fastest decay is usually
to discharge just one unit. By contrast, for landscapes built of a single unit
each of many dif... | [
{
"created": "Mon, 25 Oct 2010 20:00:03 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Sep 2011 04:10:29 GMT",
"version": "v2"
}
] | 2011-09-26 | [
[
"Brown",
"Adam R.",
""
],
[
"Dahlen",
"Alex",
""
]
] | The rate and manner of vacuum decay are calculated in an explicit flux compactification, including all thick-wall and gravitational effects. For landscapes built of many units of a single flux, the fastest decay is usually to discharge just one unit. By contrast, for landscapes built of a single unit each of many diffe... | 15.490882 | 13.443381 | 16.434385 | 14.081545 | 15.413446 | 14.029284 | 14.800961 | 14.662339 | 14.438325 | 16.763107 | 13.937559 | 14.123237 | 15.115214 | 14.057544 | 14.508689 | 14.674863 | 14.666884 | 14.807494 | 14.330713 | 14.285106 | 13.881935 |
1905.01319 | Dalimil Mazac | Thomas Hartman, Dalimil Maz\'a\v{c}, Leonardo Rastelli | Sphere Packing and Quantum Gravity | 70 pages, 7 figures | null | 10.1007/JHEP12(2019)048 | null | hep-th math.MG math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish a precise relation between the modular bootstrap, used to
constrain the spectrum of 2D CFTs, and the sphere packing problem in Euclidean
geometry. The modular bootstrap bound for chiral algebra $U(1)^c$ maps exactly
to the Cohn-Elkies linear programming bound on the sphere packing density in
$d=2c$ dimen... | [
{
"created": "Fri, 3 May 2019 18:00:09 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Sep 2019 00:01:47 GMT",
"version": "v2"
}
] | 2020-01-29 | [
[
"Hartman",
"Thomas",
""
],
[
"Mazáč",
"Dalimil",
""
],
[
"Rastelli",
"Leonardo",
""
]
] | We establish a precise relation between the modular bootstrap, used to constrain the spectrum of 2D CFTs, and the sphere packing problem in Euclidean geometry. The modular bootstrap bound for chiral algebra $U(1)^c$ maps exactly to the Cohn-Elkies linear programming bound on the sphere packing density in $d=2c$ dimensi... | 6.902205 | 8.048751 | 8.575369 | 7.390335 | 7.598927 | 7.097306 | 7.080012 | 7.445454 | 7.354188 | 8.200035 | 7.333766 | 6.801238 | 6.873258 | 6.736413 | 6.733963 | 6.734365 | 6.560985 | 6.768919 | 6.669873 | 6.789848 | 6.620816 |
hep-th/0610024 | Andrzej Wereszczynski | C. Adam, J. Sanchez-Guillen, A. Wereszczynski | New Integrable Sectors in Skyrme and 4-dimensional CP^n Model | 23 pages | J.Phys.A40:1907,2007 | 10.1088/1751-8113/40/8/015 | null | hep-th | null | The application of a weak integrability concept to the Skyrme and $CP^n$
models in 4 dimensions is investigated. A new integrable subsystem of the
Skyrme model, allowing also for non-holomorphic solutions, is derived. This
procedure can be applied to the massive Skyrme model, as well. Moreover, an
example of a family... | [
{
"created": "Mon, 2 Oct 2006 07:59:20 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Adam",
"C.",
""
],
[
"Sanchez-Guillen",
"J.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | The application of a weak integrability concept to the Skyrme and $CP^n$ models in 4 dimensions is investigated. A new integrable subsystem of the Skyrme model, allowing also for non-holomorphic solutions, is derived. This procedure can be applied to the massive Skyrme model, as well. Moreover, an example of a family o... | 8.249387 | 8.114022 | 8.260444 | 8.001746 | 8.159097 | 8.395264 | 8.025944 | 7.829456 | 7.685664 | 9.027472 | 7.651063 | 7.721468 | 7.96751 | 7.847449 | 7.780877 | 7.81205 | 7.922654 | 7.781675 | 7.946164 | 8.026706 | 7.760252 |
hep-th/0011163 | Violeta Calian | V. Calian, G. Stoenescu | Renormalization of non-locally regularized BRST-anti-BRST theories | 9 pages | null | null | null | hep-th | null | An extension of the non-local regularization scheme is formulated in the
Sp(2) symmetric Lagrangian BRST quantization framework. It generates a
systematic treatment of the anomalous quantum master equations and allows to
substract the divergences as well as to calculate genuine higher loop BRST and
anti-BRST anomalie... | [
{
"created": "Fri, 17 Nov 2000 20:57:38 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Calian",
"V.",
""
],
[
"Stoenescu",
"G.",
""
]
] | An extension of the non-local regularization scheme is formulated in the Sp(2) symmetric Lagrangian BRST quantization framework. It generates a systematic treatment of the anomalous quantum master equations and allows to substract the divergences as well as to calculate genuine higher loop BRST and anti-BRST anomalies. | 16.68771 | 12.845678 | 17.14094 | 13.054629 | 13.090559 | 13.366379 | 13.607193 | 13.264805 | 12.335643 | 19.039679 | 12.160219 | 13.053693 | 15.578356 | 13.353518 | 13.038634 | 13.04797 | 12.844771 | 13.908981 | 13.321589 | 15.803177 | 13.334609 |
1704.08353 | Vakhid Gani | Aliakbar Moradi Marjaneh, Vakhid A. Gani, Danial Saadatmand, Sergey V.
Dmitriev, Kurosh Javidan | Multi-kink collisions in the $\phi^6$ model | 21 pages, 8 figures; v2: minor changes to match version published in
JHEP | JHEP 07 (2017) 028 | 10.1007/JHEP07(2017)028 | null | hep-th cond-mat.mtrl-sci math-ph math.MP nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study simultaneous collisions of two, three, and four kinks and antikinks
of the $\phi^6$ model at the same spatial point. Unlike the $\phi^4$ kinks, the
$\phi^6$ kinks are asymmetric and this enriches the variety of the collision
scenarios. In our numerical simulations we observe both reflection and bound
state f... | [
{
"created": "Wed, 26 Apr 2017 21:18:58 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Jul 2017 11:16:41 GMT",
"version": "v2"
}
] | 2017-07-11 | [
[
"Marjaneh",
"Aliakbar Moradi",
""
],
[
"Gani",
"Vakhid A.",
""
],
[
"Saadatmand",
"Danial",
""
],
[
"Dmitriev",
"Sergey V.",
""
],
[
"Javidan",
"Kurosh",
""
]
] | We study simultaneous collisions of two, three, and four kinks and antikinks of the $\phi^6$ model at the same spatial point. Unlike the $\phi^4$ kinks, the $\phi^6$ kinks are asymmetric and this enriches the variety of the collision scenarios. In our numerical simulations we observe both reflection and bound state for... | 7.309423 | 6.778626 | 7.590981 | 6.549627 | 7.133851 | 6.435392 | 6.822682 | 6.711423 | 6.804423 | 7.541056 | 6.857408 | 6.629306 | 7.03503 | 6.552367 | 6.839086 | 6.521711 | 6.508262 | 6.718882 | 6.787086 | 7.304394 | 6.713064 |
1902.03221 | Sebastien Renaux-Petel | Jacopo Fumagalli, Sebastian Garcia-Saenz, Lucas Pinol, S\'ebastien
Renaux-Petel and John Ronayne | Hyper non-Gaussianities in inflation with strongly non-geodesic motion | 5 pages + appendices, 5 figures. Claim regarding the loss of
perturbative control removed. New result of the enhancement of higher-order
correlation functions in flattened configurations | Phys. Rev. Lett. 123, 201302 (2019) | 10.1103/PhysRevLett.123.201302 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Several recent proposals to embed inflation into high-energy physics rely on
inflationary dynamics characterized by a strongly non-geodesic motion in
negatively curved field space. This naturally leads to a transient instability
of perturbations on sub-Hubble scales, and to their exponential amplification.
Supported ... | [
{
"created": "Fri, 8 Feb 2019 18:30:24 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Oct 2019 20:01:26 GMT",
"version": "v2"
}
] | 2019-11-20 | [
[
"Fumagalli",
"Jacopo",
""
],
[
"Garcia-Saenz",
"Sebastian",
""
],
[
"Pinol",
"Lucas",
""
],
[
"Renaux-Petel",
"Sébastien",
""
],
[
"Ronayne",
"John",
""
]
] | Several recent proposals to embed inflation into high-energy physics rely on inflationary dynamics characterized by a strongly non-geodesic motion in negatively curved field space. This naturally leads to a transient instability of perturbations on sub-Hubble scales, and to their exponential amplification. Supported by... | 13.132971 | 11.145932 | 12.14638 | 10.344532 | 11.756578 | 11.779859 | 11.67545 | 11.14425 | 11.156223 | 13.1579 | 11.829011 | 11.115729 | 10.867664 | 10.721434 | 11.014035 | 10.917362 | 11.339347 | 10.454543 | 10.788535 | 10.722816 | 10.923052 |
0903.4432 | Sergio Caracciolo | Sergio Caracciolo, Andrea Sportiello | Spanning Forests on Random Planar Lattices | 43 pages, Dedicated to Edouard Brezin and Giorgio Parisi, on the
occasion of their special birthday | J.Statist.Phys.135:1063-1104,2009 | 10.1007/s10955-009-9733-1 | null | hep-th cond-mat.stat-mech hep-lat math-ph math.CO math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The generating function for spanning forests on a lattice is related to the
q-state Potts model in a certain q -> 0 limit, and extends the analogous notion
for spanning trees, or dense self-avoiding branched polymers. Recent works have
found a combinatorial perturbative equivalence also with the (quadratic action)
O(... | [
{
"created": "Wed, 25 Mar 2009 19:17:07 GMT",
"version": "v1"
}
] | 2009-09-01 | [
[
"Caracciolo",
"Sergio",
""
],
[
"Sportiello",
"Andrea",
""
]
] | The generating function for spanning forests on a lattice is related to the q-state Potts model in a certain q -> 0 limit, and extends the analogous notion for spanning trees, or dense self-avoiding branched polymers. Recent works have found a combinatorial perturbative equivalence also with the (quadratic action) O(n)... | 11.699944 | 12.986311 | 13.379198 | 11.630632 | 14.235528 | 13.177971 | 12.628476 | 11.756184 | 12.670502 | 14.93813 | 11.769294 | 11.680996 | 11.831276 | 11.23697 | 12.40287 | 11.965275 | 11.91888 | 11.259103 | 11.076864 | 11.711897 | 11.595016 |
1702.02069 | Dafni Marchioro | M. Botta Cantcheff, Alexandre L. Gadelha, D\'afni F. Z. Marchioro,
Daniel Luiz Nedel | Entanglement from Dissipation and Holographic Interpretation | Major changes. Last section removed from the old version. New section
on the dual gravitational solution and the teleportation mechanism included.
Figure added. References changed | Eur. Phys. J. C78 (2018) no.2, 105 | 10.1140/epjc/s10052-018-5545-2 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study a dissipative field theory where the dissipation
process is manifestly related to dynamical entanglement and put it in the
holographic context. Such endeavour is realized by further development of a
canonical approach to study quantum dissipation, which consists of doubling the
degrees of freedo... | [
{
"created": "Tue, 7 Feb 2017 15:46:07 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Jun 2017 18:46:34 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Feb 2018 18:54:51 GMT",
"version": "v3"
}
] | 2018-02-12 | [
[
"Cantcheff",
"M. Botta",
""
],
[
"Gadelha",
"Alexandre L.",
""
],
[
"Marchioro",
"Dáfni F. Z.",
""
],
[
"Nedel",
"Daniel Luiz",
""
]
] | In this work we study a dissipative field theory where the dissipation process is manifestly related to dynamical entanglement and put it in the holographic context. Such endeavour is realized by further development of a canonical approach to study quantum dissipation, which consists of doubling the degrees of freedom ... | 10.903053 | 11.489297 | 11.348648 | 10.816036 | 10.659726 | 10.166101 | 10.669676 | 11.269608 | 10.485352 | 11.816712 | 10.618793 | 10.225302 | 10.832462 | 10.60166 | 10.60662 | 10.487104 | 10.251913 | 10.598187 | 10.552891 | 10.901728 | 10.471002 |
1012.3561 | Veronika E. Hubeny | Veronika E. Hubeny | Holographic dual of collimated radiation | 26 pages, 6 figures, invited contribution to the New Journal of
Physics Focus Issue "Strongly Correlated Quantum Fluids: From Ultracold
Quantum Gases to QCD Plasmas" | New J.Phys.13:035006,2011 | 10.1088/1367-2630/13/3/035006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new and simple method of estimating the radiation due to an
accelerated quark in a strongly coupled medium, within the framework of the
AdS/CFT correspondence. In particular, we offer a heuristic explanation of the
collimated nature of synchrotron radiation produced by a circling quark, which
was recentl... | [
{
"created": "Thu, 16 Dec 2010 11:16:42 GMT",
"version": "v1"
}
] | 2011-03-28 | [
[
"Hubeny",
"Veronika E.",
""
]
] | We propose a new and simple method of estimating the radiation due to an accelerated quark in a strongly coupled medium, within the framework of the AdS/CFT correspondence. In particular, we offer a heuristic explanation of the collimated nature of synchrotron radiation produced by a circling quark, which was recently ... | 10.543961 | 10.390326 | 10.998309 | 10.013976 | 11.346803 | 10.288964 | 10.681899 | 10.003992 | 10.2156 | 10.993467 | 9.826381 | 9.975213 | 10.305533 | 10.110525 | 10.13485 | 10.121193 | 10.535524 | 10.082993 | 10.220178 | 10.141939 | 10.07111 |
0901.3431 | Ahmad Ghodsi | Mohsen Alishahiha and Ahmad Ghodsi | Non-relativistic D3-brane in the presence of higher derivative
corrections | 20 pages. v2: typos corrected, one reference added. v3: Minor
corrections, To appear in PRD | Phys.Rev.D80:026004,2009 | 10.1103/PhysRevD.80.026004 | IPM/P-2009/002 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using alpha'^3 terms of type IIB supergravity action we study higher order
corrections to the non-relativistic non-extremal D3-brane. Utilizing the
corrected solution we evaluate corrections to temperature, entropy and shear
viscosity. We also compute the eta/s ratio which although within the range of
validity of the... | [
{
"created": "Thu, 22 Jan 2009 08:40:12 GMT",
"version": "v1"
},
{
"created": "Sun, 1 Feb 2009 08:47:54 GMT",
"version": "v2"
},
{
"created": "Tue, 14 Jul 2009 15:02:32 GMT",
"version": "v3"
}
] | 2009-08-12 | [
[
"Alishahiha",
"Mohsen",
""
],
[
"Ghodsi",
"Ahmad",
""
]
] | Using alpha'^3 terms of type IIB supergravity action we study higher order corrections to the non-relativistic non-extremal D3-brane. Utilizing the corrected solution we evaluate corrections to temperature, entropy and shear viscosity. We also compute the eta/s ratio which although within the range of validity of the s... | 12.388548 | 9.889639 | 12.068053 | 9.559455 | 11.388397 | 10.375051 | 10.518723 | 9.752557 | 9.283748 | 13.593241 | 9.010312 | 10.229239 | 11.621907 | 9.790683 | 10.390484 | 9.829045 | 10.607831 | 10.429134 | 9.851529 | 12.38201 | 10.060543 |
hep-th/0411162 | Jurgen Baacke | Jurgen Baacke and Nina Kevlishvili | Self-consistent bounces in two dimensions | 30 pages, 12 figures | Phys.Rev. D71 (2005) 025008 | 10.1103/PhysRevD.71.025008 | DO-TH-04-11 | hep-th gr-qc hep-ph | null | We compute bounce solutions describing false vacuum decay in a Phi**4 model
in two dimensions in the Hartree approximation, thus going beyond the usual
one-loop corrections to the decay rate. We use zero energy mode functions of
the fluctuation operator for the numerical computation of the functional
determinant and ... | [
{
"created": "Thu, 18 Nov 2004 16:22:49 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Nov 2004 12:48:40 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Baacke",
"Jurgen",
""
],
[
"Kevlishvili",
"Nina",
""
]
] | We compute bounce solutions describing false vacuum decay in a Phi**4 model in two dimensions in the Hartree approximation, thus going beyond the usual one-loop corrections to the decay rate. We use zero energy mode functions of the fluctuation operator for the numerical computation of the functional determinant and th... | 11.530805 | 11.656957 | 11.621835 | 10.772788 | 11.714757 | 12.172919 | 12.326342 | 12.278286 | 10.562484 | 11.597509 | 11.158735 | 11.045832 | 11.354903 | 10.946233 | 11.224902 | 11.711685 | 11.162447 | 11.529829 | 11.050344 | 11.535425 | 10.888031 |
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