id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0411256 | Girma Hailu | Girma Hailu | Quantum Geometries of $A_{2}$ | 19 pages, more typos fixed and clarifying notes added | JHEP 0502:017,2005 | 10.1088/1126-6708/2005/02/017 | null | hep-th | null | We solve $\mathcal{N}=1$ supersymmetric $A_{2}$ type $U(N)\times U(N)$ matrix
models obtained by deforming $\mathcal{N}=2$ with symmetric tree level
superpotentials of any degree exactly in the planar limit. These theories can
be geometrically engineered from string theories by wrapping D-branes over
Calabi-Yau three... | [
{
"created": "Mon, 29 Nov 2004 20:13:29 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Dec 2004 19:07:48 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Jan 2005 17:38:24 GMT",
"version": "v3"
}
] | 2010-12-03 | [
[
"Hailu",
"Girma",
""
]
] | We solve $\mathcal{N}=1$ supersymmetric $A_{2}$ type $U(N)\times U(N)$ matrix models obtained by deforming $\mathcal{N}=2$ with symmetric tree level superpotentials of any degree exactly in the planar limit. These theories can be geometrically engineered from string theories by wrapping D-branes over Calabi-Yau threefo... | 10.095942 | 8.962885 | 13.019007 | 8.739197 | 10.143245 | 8.704757 | 8.061104 | 8.83417 | 8.843182 | 12.601389 | 8.869548 | 8.714468 | 9.88574 | 8.594952 | 8.460451 | 8.576496 | 8.444708 | 9.105985 | 8.727437 | 9.481962 | 8.560847 |
1702.04160 | Christian Saemann | Christian Saemann and Martin Wolf | Supersymmetric Yang-Mills Theory as Higher Chern-Simons Theory | v2: 25 pages, conventions improved, typos fixed, published version | JHEP 07 (2017) 111 | 10.1007/JHEP07(2017)111 | EMPG-17-02, DMUS-MP-17/02 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We observe that the string field theory actions for the topological sigma
models describe higher or categorified Chern-Simons theories. These theories
yield dynamical equations for connective structures on higher principal
bundles. As a special case, we consider holomorphic higher Chern-Simons theory
on the ambitwist... | [
{
"created": "Tue, 14 Feb 2017 11:26:32 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Jul 2017 09:20:35 GMT",
"version": "v2"
}
] | 2017-07-27 | [
[
"Saemann",
"Christian",
""
],
[
"Wolf",
"Martin",
""
]
] | We observe that the string field theory actions for the topological sigma models describe higher or categorified Chern-Simons theories. These theories yield dynamical equations for connective structures on higher principal bundles. As a special case, we consider holomorphic higher Chern-Simons theory on the ambitwistor... | 10.408957 | 9.873065 | 10.47065 | 10.373179 | 9.731226 | 8.543493 | 10.248098 | 10.119419 | 10.467422 | 11.651621 | 10.573048 | 10.924438 | 10.654662 | 10.228905 | 9.822606 | 9.762418 | 9.86294 | 10.557931 | 9.990643 | 10.572624 | 10.464692 |
0806.3515 | Cosmas Zachos | Thomas L Curtright, David B Fairlie, and Cosmas K Zachos | Ternary Virasoro - Witt Algebra | 6 pages, LateX | Phys.Lett.B666:386-390,2008 | 10.1016/j.physletb.2008.06.060 | ANL-HEP-PR-08-35 and UMTG - 7 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A 3-bracket variant of the Virasoro-Witt algebra is constructed through the
use of su(1,1) enveloping algebra techniques. The Leibniz rules for 3-brackets
acting on other 3-brackets in the algebra are discussed and verified in various
situations.
| [
{
"created": "Mon, 23 Jun 2008 18:14:15 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Curtright",
"Thomas L",
""
],
[
"Fairlie",
"David B",
""
],
[
"Zachos",
"Cosmas K",
""
]
] | A 3-bracket variant of the Virasoro-Witt algebra is constructed through the use of su(1,1) enveloping algebra techniques. The Leibniz rules for 3-brackets acting on other 3-brackets in the algebra are discussed and verified in various situations. | 11.15501 | 10.053815 | 11.653972 | 9.481581 | 8.632402 | 9.375088 | 10.100016 | 9.280231 | 9.842821 | 11.295987 | 9.381093 | 8.828446 | 9.897576 | 8.88416 | 8.837672 | 9.074408 | 9.582365 | 8.42347 | 8.851286 | 9.229149 | 8.854566 |
hep-th/9803183 | Alexander Popov | A.D.Popov | Self-Dual Yang-Mills: Symmetries and Moduli Space | 42 pages, LaTeX2e | Rev.Math.Phys. 11 (1999) 1091-1149 | 10.1142/S0129055X99000350 | null | hep-th | null | Geometry of the solution space of the self-dual Yang-Mills (SDYM) equations
in Euclidean four-dimensional space is studied. Combining the twistor and
group-theoretic approaches, we describe the full infinite-dimensional symmetry
group of the SDYM equations and its action on the space of local solutions to
the field e... | [
{
"created": "Mon, 23 Mar 1998 14:17:10 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Jun 1998 10:17:43 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Popov",
"A. D.",
""
]
] | Geometry of the solution space of the self-dual Yang-Mills (SDYM) equations in Euclidean four-dimensional space is studied. Combining the twistor and group-theoretic approaches, we describe the full infinite-dimensional symmetry group of the SDYM equations and its action on the space of local solutions to the field equ... | 6.76696 | 6.671932 | 7.078806 | 6.498462 | 6.79512 | 7.219493 | 7.397873 | 6.840818 | 6.64591 | 7.927279 | 6.379629 | 6.686455 | 6.690985 | 6.440165 | 6.811529 | 6.710944 | 6.785124 | 6.536971 | 6.589105 | 6.582868 | 6.401772 |
2305.17128 | Sergey Frolov Dr. | Sergey Frolov, Anton Pribytok, Alessandro Sfondrini | Ground state energy of twisted $AdS_{3}\times S^{3}\times T^{4}$
superstring and the TBA | 31 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We use the lightcone $AdS_{3}\times S^{3}\times T^{4}$ superstring sigma
model with fermions and bosons subject to twisted boundary conditions to find
the ground state energy in the semi-classical approximation where effective
string tension $h$ and the light-cone momentum $L$ are sent to infinity in such
a way that ... | [
{
"created": "Fri, 26 May 2023 17:51:22 GMT",
"version": "v1"
}
] | 2023-05-29 | [
[
"Frolov",
"Sergey",
""
],
[
"Pribytok",
"Anton",
""
],
[
"Sfondrini",
"Alessandro",
""
]
] | We use the lightcone $AdS_{3}\times S^{3}\times T^{4}$ superstring sigma model with fermions and bosons subject to twisted boundary conditions to find the ground state energy in the semi-classical approximation where effective string tension $h$ and the light-cone momentum $L$ are sent to infinity in such a way that ${... | 6.121268 | 5.629378 | 6.868022 | 5.762815 | 5.613719 | 5.659623 | 5.664412 | 5.573434 | 5.659901 | 7.329384 | 5.537227 | 5.630432 | 5.998622 | 5.689771 | 5.626728 | 5.671083 | 5.654798 | 5.731517 | 5.689563 | 6.126401 | 5.488064 |
0810.2809 | Matthew Headrick | Matthew Headrick | A note on tachyon actions in string theory | 17 pages; v2: comments on implications for string field theory added;
refs added | Phys.Rev.D79:046009,2009 | 10.1103/PhysRevD.79.046009 | BRX-TH-602 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A number of spacetime fields in string theory (notably the metric, dilaton,
bosonic and type 0 bulk closed-string tachyon, and bosonic open-string tachyon)
have the following property: whenever the spacetime field configuration
factorizes in an appropriate sense, the matter sector of the world-sheet theory
factorizes... | [
{
"created": "Wed, 15 Oct 2008 21:33:37 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Dec 2008 02:01:22 GMT",
"version": "v2"
}
] | 2009-03-12 | [
[
"Headrick",
"Matthew",
""
]
] | A number of spacetime fields in string theory (notably the metric, dilaton, bosonic and type 0 bulk closed-string tachyon, and bosonic open-string tachyon) have the following property: whenever the spacetime field configuration factorizes in an appropriate sense, the matter sector of the world-sheet theory factorizes i... | 7.169425 | 8.144244 | 7.598653 | 7.303001 | 8.103376 | 7.909914 | 7.384026 | 7.299364 | 7.402408 | 9.498519 | 7.173161 | 7.346804 | 7.723191 | 7.082251 | 6.93444 | 6.931863 | 7.18316 | 7.266666 | 7.102369 | 7.891087 | 7.147237 |
hep-th/9407035 | Joakim Hallin | I. Bengtsson and J. Hallin | SL(2,R) Yang-Mills theory on a circle | 10 pages, Goteborg ITP 94-19, Contains two files: A latex file with
all figures drawn in latex and a tar archive including a slightly modified
latex file (uses psfig) and nicer postscript figures+necessary macros | Mod.Phys.Lett. A9 (1994) 3245-3254 | 10.1142/S0217732394003063 | null | hep-th | null | The kinematics of SL(2,R) Yang-Mills theory on a circle is considered, for
reasons that are spelled out. The gauge transformations exhibit hyperbolic
fixed points, and this results in a physical configuration space with a
non-Hausdorff "network" topology. The ambiguity encountered in canonical
quantization is then mu... | [
{
"created": "Wed, 6 Jul 1994 12:19:05 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bengtsson",
"I.",
""
],
[
"Hallin",
"J.",
""
]
] | The kinematics of SL(2,R) Yang-Mills theory on a circle is considered, for reasons that are spelled out. The gauge transformations exhibit hyperbolic fixed points, and this results in a physical configuration space with a non-Hausdorff "network" topology. The ambiguity encountered in canonical quantization is then much... | 14.617122 | 14.607038 | 15.191384 | 14.241019 | 15.021027 | 14.938857 | 13.302249 | 14.57483 | 13.874719 | 14.60323 | 14.113407 | 14.382183 | 14.469547 | 14.328435 | 13.920646 | 14.302612 | 14.413156 | 13.794971 | 14.397725 | 14.211043 | 13.689997 |
hep-th/0105165 | Stoytcho Yazadjiev | Stoytcho S. Yazadjiev, Plamen P. Fiziev, Todor L. Boyadjiev, Michail
D. Todorov | Electrically Charged Einstein-Born-Infeld Black Holes with Massive
Dilaton | 6 pages, 4 figures, LaTeX; v2 comments, references and
acknowledgements added | Mod.Phys.Lett. A16 (2001) 2143-2150 | 10.1142/S0217732301005564 | null | hep-th astro-ph gr-qc | null | We numerically construct static and spherically symmetric electrically
charged black hole solutions in Einstein-Born-Infeld gravity with massive
dilaton. The numerical solutions show that the dilaton potential allows many
more black hole causal structures than the massless dilaton. We find that
depending on the black... | [
{
"created": "Thu, 17 May 2001 08:32:46 GMT",
"version": "v1"
},
{
"created": "Mon, 28 May 2001 07:45:10 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Yazadjiev",
"Stoytcho S.",
""
],
[
"Fiziev",
"Plamen P.",
""
],
[
"Boyadjiev",
"Todor L.",
""
],
[
"Todorov",
"Michail D.",
""
]
] | We numerically construct static and spherically symmetric electrically charged black hole solutions in Einstein-Born-Infeld gravity with massive dilaton. The numerical solutions show that the dilaton potential allows many more black hole causal structures than the massless dilaton. We find that depending on the black h... | 7.06185 | 6.628056 | 6.973142 | 6.269944 | 6.720115 | 6.287129 | 6.775412 | 6.341812 | 6.689241 | 6.830202 | 6.63355 | 6.969898 | 6.758292 | 6.604122 | 6.688704 | 6.538142 | 6.546605 | 6.528819 | 6.640858 | 7.150337 | 6.839021 |
hep-th/9705127 | Hiroaki Kanno | L. Baulieu, H. Kanno and I. M. Singer | Cohomological Yang-Mills Theory in Eight Dimensions | 9 pages, latex, Talk given at APCTP Winter School on Dualities in
String Theory, (Sokcho, Korea), February 24-28, 1997 | null | 10.1142/9789814447287_0011 | null | hep-th | null | We construct nearly topological Yang-Mills theories on eight dimensional
manifolds with a special holonomy group. These manifolds are the Joyce manifold
with $Spin(7)$ holonomy and the Calabi-Yau manifold with SU(4) holonomy. An
invariant closed four form $T_{\mu\nu\rho\sigma}$ on the manifold allows us to
define an ... | [
{
"created": "Sat, 17 May 1997 02:05:33 GMT",
"version": "v1"
}
] | 2016-11-03 | [
[
"Baulieu",
"L.",
""
],
[
"Kanno",
"H.",
""
],
[
"Singer",
"I. M.",
""
]
] | We construct nearly topological Yang-Mills theories on eight dimensional manifolds with a special holonomy group. These manifolds are the Joyce manifold with $Spin(7)$ holonomy and the Calabi-Yau manifold with SU(4) holonomy. An invariant closed four form $T_{\mu\nu\rho\sigma}$ on the manifold allows us to define an an... | 6.589032 | 5.744446 | 7.617943 | 6.085773 | 6.437004 | 6.400736 | 6.356236 | 6.059802 | 5.842385 | 8.520733 | 6.021212 | 6.013764 | 6.568924 | 6.21563 | 5.902857 | 6.118222 | 6.060918 | 6.182908 | 6.371781 | 6.743628 | 6.048686 |
hep-th/0511190 | Peter Horvathy | A. Comtet, P. A. Horvathy | The Dirac equation in Taub-NUT space | An importatn misprint in a reference is corrected. Plain Tex. 8 pages | Phys.Lett. B349 (1995) 49-56 | 10.1016/0370-2693(95)00219-B | null | hep-th | null | Using chiral supersymmetry, we show that the massless Dirac equation in the
Taub-NUT gravitational instanton field is exactly soluble and explain the
arisal and the use of the dynamical (super) symmetry.
| [
{
"created": "Fri, 18 Nov 2005 14:55:42 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Dec 2005 18:11:25 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Comtet",
"A.",
""
],
[
"Horvathy",
"P. A.",
""
]
] | Using chiral supersymmetry, we show that the massless Dirac equation in the Taub-NUT gravitational instanton field is exactly soluble and explain the arisal and the use of the dynamical (super) symmetry. | 16.207693 | 12.254407 | 13.94162 | 12.880307 | 11.93868 | 13.972452 | 12.993582 | 13.365703 | 13.388685 | 16.207085 | 13.692398 | 14.153112 | 14.2533 | 13.361889 | 14.158134 | 13.996377 | 13.409683 | 14.494193 | 14.237611 | 14.691757 | 13.730742 |
1712.01594 | \"Umit Ertem | \"Ozg\"ur A\c{c}{\i}k, \"Umit Ertem | Spin raising and lowering operators for Rarita-Schwinger fields | 10 pages, an appendix added, published version | Phys. Rev. D 98, 066004 (2018) | 10.1103/PhysRevD.98.066004 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Spin raising and lowering operators for massless field equations constructed
from twistor spinors are considered. Solutions of the spin-$\frac{3}{2}$
massless Rarita-Schwinger equation from source-free Maxwell fields and twistor
spinors are constructed. It is shown that this construction requires Ricci-flat
backgroun... | [
{
"created": "Tue, 5 Dec 2017 12:11:23 GMT",
"version": "v1"
},
{
"created": "Sat, 15 Sep 2018 11:12:34 GMT",
"version": "v2"
}
] | 2018-09-19 | [
[
"Açık",
"Özgür",
""
],
[
"Ertem",
"Ümit",
""
]
] | Spin raising and lowering operators for massless field equations constructed from twistor spinors are considered. Solutions of the spin-$\frac{3}{2}$ massless Rarita-Schwinger equation from source-free Maxwell fields and twistor spinors are constructed. It is shown that this construction requires Ricci-flat backgrounds... | 7.638119 | 7.575169 | 7.413057 | 6.771821 | 7.545093 | 7.360235 | 7.260732 | 6.945529 | 6.851988 | 7.740639 | 6.830168 | 7.267022 | 6.977392 | 6.927654 | 6.95751 | 6.93436 | 6.892788 | 6.862947 | 6.903995 | 7.002427 | 6.706537 |
2202.05026 | Axel Kleinschmidt | Joaquim Gomis, Axel Kleinschmidt | Infinite-dimensional algebras as extensions of kinematic algebras | 48 pages. Contribution to a special Frontiers volume on
"Non-Lorentzian Geometry and its Applications". v2: very minor corrections | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Kinematic algebras can be realised on geometric spaces and constrain the
physical models that can live on these spaces. Different types of kinematic
algebras exist and we consider the interplay of these algebras for
non-relativistic limits of a relativistic system, including both the Galilei
and the Carroll limit. We... | [
{
"created": "Thu, 10 Feb 2022 13:31:08 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Apr 2022 19:26:50 GMT",
"version": "v2"
}
] | 2022-04-26 | [
[
"Gomis",
"Joaquim",
""
],
[
"Kleinschmidt",
"Axel",
""
]
] | Kinematic algebras can be realised on geometric spaces and constrain the physical models that can live on these spaces. Different types of kinematic algebras exist and we consider the interplay of these algebras for non-relativistic limits of a relativistic system, including both the Galilei and the Carroll limit. We d... | 12.326985 | 11.270866 | 12.955854 | 11.628068 | 12.630662 | 11.673449 | 11.458477 | 11.117338 | 11.735107 | 15.260978 | 11.068696 | 11.293824 | 11.970914 | 11.621353 | 11.509085 | 11.093385 | 11.253 | 11.355279 | 11.788385 | 12.057947 | 11.360819 |
hep-th/9408024 | null | Rainer Dick | Non-Standard Fermion Propagators from Conformal Field Theory | 15 pages, Latex, LMU-TPW 94-10 | null | 10.1007/3-540-59163-X_261 | null | hep-th | null | It is shown that Weyl spinors in 4D Minkowski space are composed of primary
fields of half-integer conformal weights. This yields representations of
fermionic 2-point functions in terms of correlators of primary fields with a
factorized transformation behavior under the Lorentz group. I employ this
observation to det... | [
{
"created": "Thu, 4 Aug 1994 09:05:44 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Dick",
"Rainer",
""
]
] | It is shown that Weyl spinors in 4D Minkowski space are composed of primary fields of half-integer conformal weights. This yields representations of fermionic 2-point functions in terms of correlators of primary fields with a factorized transformation behavior under the Lorentz group. I employ this observation to deter... | 10.590792 | 11.222563 | 11.853059 | 11.250097 | 11.118974 | 11.080861 | 11.295928 | 10.328882 | 10.453481 | 11.789622 | 10.922473 | 10.752195 | 10.883214 | 10.776096 | 10.734015 | 10.759496 | 10.466446 | 10.966245 | 10.604865 | 10.78371 | 10.36974 |
0706.3373 | Gabriel Cardoso | Gabriel Lopes Cardoso, Anna Ceresole, Gianguido Dall'Agata, Johannes
M. Oberreuter, Jan Perz | First-order flow equations for extremal black holes in very special
geometry | 21 pages. v2: Summary section added | JHEP 0710:063,2007 | 10.1088/1126-6708/2007/10/063 | DFPD-07TH10, LMU-ASC 38/07, MPP-2007-73 | hep-th | null | We construct interpolating solutions describing single-center static extremal
non-supersymmetric black holes in four-dimensional N=2 supergravity theories
with cubic prepotentials. To this end, we derive and solve first-order flow
equations for rotating electrically charged extremal black holes in a Taub-NUT
geometry... | [
{
"created": "Fri, 22 Jun 2007 16:22:14 GMT",
"version": "v1"
},
{
"created": "Sun, 30 Sep 2007 09:05:50 GMT",
"version": "v2"
}
] | 2009-11-18 | [
[
"Cardoso",
"Gabriel Lopes",
""
],
[
"Ceresole",
"Anna",
""
],
[
"Dall'Agata",
"Gianguido",
""
],
[
"Oberreuter",
"Johannes M.",
""
],
[
"Perz",
"Jan",
""
]
] | We construct interpolating solutions describing single-center static extremal non-supersymmetric black holes in four-dimensional N=2 supergravity theories with cubic prepotentials. To this end, we derive and solve first-order flow equations for rotating electrically charged extremal black holes in a Taub-NUT geometry i... | 7.910772 | 6.012411 | 8.866324 | 6.190125 | 6.831857 | 6.624786 | 6.680133 | 6.408374 | 6.25869 | 8.24028 | 6.630639 | 6.252893 | 7.589376 | 6.607742 | 6.495078 | 6.560151 | 6.442271 | 6.367243 | 6.705613 | 8.254669 | 6.656867 |
1408.1298 | Jiang Long | Jiang Long | Higher Spin Entanglement Entropy | 49 pages,1 figure, to be published in JHEP | null | 10.1007/JHEP12(2014)055 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we develop a perturbation formulation to calculate the single
interval higher spin R$\acute{e}$nyi and entanglement entropy for two
dimensional conformal field theory with $\mathcal{W}_{\infty}(\lambda)$
symmetry. The system is at finite temperature and is deformed by higher spin
chemical potential. We... | [
{
"created": "Wed, 6 Aug 2014 14:42:28 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Dec 2014 19:38:32 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Long",
"Jiang",
""
]
] | In this paper, we develop a perturbation formulation to calculate the single interval higher spin R$\acute{e}$nyi and entanglement entropy for two dimensional conformal field theory with $\mathcal{W}_{\infty}(\lambda)$ symmetry. The system is at finite temperature and is deformed by higher spin chemical potential. We m... | 5.442506 | 4.938701 | 5.843205 | 4.910394 | 5.176788 | 5.159744 | 4.866874 | 4.919172 | 5.0591 | 5.836527 | 5.015034 | 5.077846 | 5.235322 | 4.963538 | 5.047306 | 5.071918 | 4.968775 | 4.982839 | 5.023047 | 5.319109 | 5.072748 |
0712.3167 | Victor Chernyak | Victor L. Chernyak | On Mass Spectrum in SQCD, and Problems with the Seiberg Duality. Equal
quark masses | 31 pages; text improved; corrections in sections 5,8; appendix added
about 't Hooft triangles | J.Exp.Theor.Phys.110:383-405,2010 | 10.1134/S1063776110030039 | null | hep-th astro-ph hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dynamical scenario is considered for N=1 SQCD, with N_c colors and
N_c<N_F<3N_c flavors with small but nonzero current quark masses m_Q\neq 0, in
which quarks form the diquark-condensate phase. This means that colorless
chiral quark pairs condense coherently in the vacuum, <{\bar Q}Q>\neq 0, while
quarks alone do... | [
{
"created": "Wed, 19 Dec 2007 11:58:10 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Dec 2007 10:19:35 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Jan 2008 14:46:17 GMT",
"version": "v3"
},
{
"created": "Mon, 24 Mar 2008 11:54:54 GMT",
"version": "v4"
},
{
"c... | 2010-05-12 | [
[
"Chernyak",
"Victor L.",
""
]
] | The dynamical scenario is considered for N=1 SQCD, with N_c colors and N_c<N_F<3N_c flavors with small but nonzero current quark masses m_Q\neq 0, in which quarks form the diquark-condensate phase. This means that colorless chiral quark pairs condense coherently in the vacuum, <{\bar Q}Q>\neq 0, while quarks alone don'... | 10.503225 | 10.18715 | 10.592744 | 9.249492 | 10.385502 | 11.705912 | 10.481802 | 10.292769 | 9.590881 | 11.264776 | 10.192282 | 9.792193 | 9.772368 | 9.523711 | 10.219228 | 10.044576 | 9.704867 | 9.78136 | 9.679765 | 10.298273 | 9.709188 |
hep-th/0303010 | Pavel Kovtun | Pavel Kovtun and Laurence G. Yaffe | Hydrodynamic Fluctuations, Long-time Tails, and Supersymmetry | null | Phys.Rev. D68 (2003) 025007 | 10.1103/PhysRevD.68.025007 | UW/PT 03-05 | hep-th hep-ph | null | Hydrodynamic fluctuations at non-zero temperature can cause slow relaxation
toward equilibrium even in observables which are not locally conserved. A
classic example is the stress-stress correlator in a normal fluid, which, at
zero wavenumber, behaves at large times as t^{-3/2}. A novel feature of the
effective theor... | [
{
"created": "Mon, 3 Mar 2003 03:11:27 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Kovtun",
"Pavel",
""
],
[
"Yaffe",
"Laurence G.",
""
]
] | Hydrodynamic fluctuations at non-zero temperature can cause slow relaxation toward equilibrium even in observables which are not locally conserved. A classic example is the stress-stress correlator in a normal fluid, which, at zero wavenumber, behaves at large times as t^{-3/2}. A novel feature of the effective theory ... | 7.025234 | 7.704443 | 7.47882 | 7.1963 | 7.323983 | 7.621547 | 7.671988 | 7.427148 | 7.50771 | 8.014645 | 6.882808 | 7.018289 | 7.265899 | 6.974609 | 7.128094 | 7.022948 | 7.198124 | 7.043875 | 7.121417 | 7.407476 | 6.899124 |
2312.05888 | Vitaly Velizhanin | B.A. Kniehl, V.N. Velizhanin | Anomalous dimensions of twist-two operators in extended N=2 and N=4
super Yang-Mills theories | 16 pages, 5 figures, minor changes, reference added | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform direct diagrammatic calculations of the anomalous dimensions of
twist-two operators in extended N=2 and N=4 super Yang-Mills theories (SYM). In
the case of N=4 SYM, we compute the four-loop anomalous dimension of the
twist-two operator for several fixed values of Lorentz spin. This is the first
direct diag... | [
{
"created": "Sun, 10 Dec 2023 13:42:16 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Dec 2023 15:03:16 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Mar 2024 17:41:06 GMT",
"version": "v3"
}
] | 2024-03-08 | [
[
"Kniehl",
"B. A.",
""
],
[
"Velizhanin",
"V. N.",
""
]
] | We perform direct diagrammatic calculations of the anomalous dimensions of twist-two operators in extended N=2 and N=4 super Yang-Mills theories (SYM). In the case of N=4 SYM, we compute the four-loop anomalous dimension of the twist-two operator for several fixed values of Lorentz spin. This is the first direct diagra... | 6.404164 | 5.444353 | 6.337267 | 5.718657 | 5.805196 | 5.820937 | 5.751685 | 5.728311 | 5.53445 | 6.553112 | 5.35816 | 5.745798 | 5.770866 | 5.765936 | 5.703961 | 5.729946 | 5.777503 | 5.543701 | 5.868322 | 5.99868 | 5.596047 |
1609.08694 | Tomas Ortin | Tomas Ortin and Camilla Santoli | Supersymmetric solutions of SU(2)-Fayet-Iliopoulos-gauged N=2,d=4
supergravity | Latex 2e file, 37 pages, 1 figure. A paragraph on Fayet-Iliopoulos
gaugings rewritten and minor typos corrected. Version to be published in
Nuclear Physics B | null | 10.1016/j.nuclphysb.2016.12.023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the construction of supersymmetric solutions of theories of
N=2,d=4 supergravity with a SU(2) gauging and SU(2) Fayet-Iliopoulos terms. In
these theories an SU(2) isometry subgroup of the Special Kahler manifold is
gauged together with a SU(2) R-symmetry subgroup. We construct several
solutions of the CP3 ... | [
{
"created": "Tue, 27 Sep 2016 22:20:41 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Jan 2017 10:12:12 GMT",
"version": "v2"
}
] | 2017-04-05 | [
[
"Ortin",
"Tomas",
""
],
[
"Santoli",
"Camilla",
""
]
] | We explore the construction of supersymmetric solutions of theories of N=2,d=4 supergravity with a SU(2) gauging and SU(2) Fayet-Iliopoulos terms. In these theories an SU(2) isometry subgroup of the Special Kahler manifold is gauged together with a SU(2) R-symmetry subgroup. We construct several solutions of the CP3 qu... | 9.448893 | 10.02809 | 11.62839 | 9.72076 | 10.470128 | 10.088459 | 10.350325 | 9.262687 | 9.31721 | 12.062366 | 10.381401 | 9.292973 | 10.168982 | 9.156322 | 9.546279 | 10.058393 | 9.60277 | 9.24627 | 9.329069 | 10.163478 | 9.411438 |
hep-th/0408038 | Stuart Dowker | J.S.Dowker | Determinants on lens spaces and cyclotomic units | 18 pages, 1 figure | J.Phys. A38 (2005) 1049-1062 | 10.1088/0305-4470/38/5/007 | null | hep-th gr-qc math.NT | null | The Laplacian functional determinants for conformal scalars and coexact
one-forms are evaluated in closed form on inhomogeneous lens spaces of certain
orders, including all odd primes when the essential part of the expression is
given, formally as a cyclotomic unit
| [
{
"created": "Wed, 4 Aug 2004 21:04:39 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Dowker",
"J. S.",
""
]
] | The Laplacian functional determinants for conformal scalars and coexact one-forms are evaluated in closed form on inhomogeneous lens spaces of certain orders, including all odd primes when the essential part of the expression is given, formally as a cyclotomic unit | 53.651894 | 46.354759 | 46.608784 | 47.947948 | 43.958885 | 40.467186 | 47.651096 | 36.463684 | 35.849743 | 63.008339 | 40.837048 | 45.687164 | 44.055775 | 43.013599 | 43.043106 | 43.968647 | 40.65044 | 43.760983 | 44.412994 | 42.009857 | 39.667755 |
hep-th/9612069 | null | J. Ambjorn, M. Carfora, A. Marzuoli | The geometry of dynamical triangulations | 166 pages, Revtex (latex) file | Lect.NotesPhys.50:197,1997 | null | Preprint-DFNT/Pavia/9/96 | hep-th gr-qc hep-lat | null | We discuss the geometry of dynamical triangulations associated with
3-dimensional and 4-dimensional simplicial quantum gravity. We provide
analytical expressions for the canonical partition function in both cases, and
study its large volume behavior. In the space of the coupling constants of the
theory, we characteri... | [
{
"created": "Fri, 6 Dec 1996 13:28:37 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Ambjorn",
"J.",
""
],
[
"Carfora",
"M.",
""
],
[
"Marzuoli",
"A.",
""
]
] | We discuss the geometry of dynamical triangulations associated with 3-dimensional and 4-dimensional simplicial quantum gravity. We provide analytical expressions for the canonical partition function in both cases, and study its large volume behavior. In the space of the coupling constants of the theory, we characterize... | 9.90823 | 11.124614 | 10.431403 | 9.789285 | 11.367835 | 10.460796 | 10.408213 | 10.389211 | 10.789882 | 10.338789 | 10.516742 | 9.870465 | 9.85393 | 9.730197 | 9.606741 | 10.112304 | 9.89883 | 9.598208 | 9.999638 | 10.261052 | 9.834867 |
1105.0933 | Antonio Amariti | Antonio Amariti, Massimo Siani | Z-extremization and F-theorem in Chern-Simons matter theories | 28 pages, 3 figures, JHEP.cls, minor corrections, references added | null | 10.1007/JHEP10(2011)016 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The three dimensional exact R symmetry of N=2 SCFTs extremizes the partition
function localized on a three sphere. Here we verify this statement at weak
coupling. We give a detailed analysis for two classes of models. The first one
is an SU(N)_k gauge theory at large k with both fundamental and adjoint matter
fields,... | [
{
"created": "Wed, 4 May 2011 20:27:23 GMT",
"version": "v1"
},
{
"created": "Tue, 17 May 2011 17:32:21 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Amariti",
"Antonio",
""
],
[
"Siani",
"Massimo",
""
]
] | The three dimensional exact R symmetry of N=2 SCFTs extremizes the partition function localized on a three sphere. Here we verify this statement at weak coupling. We give a detailed analysis for two classes of models. The first one is an SU(N)_k gauge theory at large k with both fundamental and adjoint matter fields, w... | 12.475977 | 11.996204 | 14.13475 | 11.559588 | 11.897248 | 13.23474 | 11.469388 | 11.182564 | 11.072919 | 16.668705 | 11.677831 | 11.281373 | 12.000449 | 11.56066 | 11.499611 | 11.28403 | 11.548056 | 11.638006 | 11.008543 | 12.538789 | 11.688213 |
hep-th/9711142 | Young-Jai Park | Mu-In Park and Young-Jai Park | Note on the Abelian Pure CS Theory Based on the Improved BFT Method | 12 pages, latex, no figures, final published version | J.KoreanPhys.Soc.31:802-806,1997 | null | SOGANG-HEP 211/97 | hep-th | null | We reconsider the Abelian pure Chern-Simons theory in three dimensions by
using our improved Batalin-Fradkin-Tyutin Hamiltonian formalism. As a result,
we show several novel features, including the connection of the Dirac brackets.
In particular, through the path integral quantization, we obtain the desired
new type ... | [
{
"created": "Wed, 19 Nov 1997 06:18:46 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Park",
"Mu-In",
""
],
[
"Park",
"Young-Jai",
""
]
] | We reconsider the Abelian pure Chern-Simons theory in three dimensions by using our improved Batalin-Fradkin-Tyutin Hamiltonian formalism. As a result, we show several novel features, including the connection of the Dirac brackets. In particular, through the path integral quantization, we obtain the desired new type of... | 11.479253 | 8.094824 | 10.504373 | 8.471499 | 8.346101 | 8.228487 | 8.74102 | 8.369525 | 8.174246 | 11.670724 | 8.261965 | 8.863906 | 10.403483 | 9.420876 | 9.305211 | 9.16611 | 9.55708 | 9.243385 | 9.356243 | 10.34243 | 9.14335 |
hep-th/0510267 | Hans-Thomas Elze | Hans-Thomas Elze | Quantum fields, cosmological constant and symmetry doubling | Replaced by published version, no change in contents - Int. J. Theor.
Phys. (2007) | Int.J.Theor.Phys.46:2063-2081,2007 | 10.1007/s10773-006-9337-3 | null | hep-th gr-qc quant-ph | null | Energy-parity has been introduced by Kaplan and Sundrum as a protective
symmetry that suppresses matter contributions to the cosmological constant
[KS05]. It is shown here that this symmetry, schematically Energy --> - Energy,
arises in the Hilbert space representation of the classical phase space
dynamics of matter.... | [
{
"created": "Mon, 31 Oct 2005 10:32:42 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Mar 2007 16:36:52 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Elze",
"Hans-Thomas",
""
]
] | Energy-parity has been introduced by Kaplan and Sundrum as a protective symmetry that suppresses matter contributions to the cosmological constant [KS05]. It is shown here that this symmetry, schematically Energy --> - Energy, arises in the Hilbert space representation of the classical phase space dynamics of matter. C... | 20.730824 | 23.472269 | 21.572477 | 19.052187 | 21.892372 | 20.976763 | 21.793753 | 20.951551 | 19.198572 | 21.600206 | 22.126696 | 19.504425 | 19.467306 | 19.197752 | 19.624136 | 19.393791 | 19.082191 | 19.058308 | 19.608776 | 19.390951 | 19.097542 |
1410.5549 | Zhiguang Xiao | Wenhe Cai, Chao Wu, Zhiguang Xiao | Baryons in the Sakai-Sugimoto model in the D0-D4 background | 15 pages, 3 figures | null | 10.1103/PhysRevD.90.106001 | USTC-ICTS-14-18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The baryon spectrum in the Sakai-Sugimoto model in the D4 background with
smeared D0 charges is studied. We follow the instanton description of baryons
by Hata et al.[Prog. Theor. Phys. 117, 1157]. The background corresponds to an
excited state with nonzero glue condensate $\langle {\rm tr} (F_{\mu\nu}\tilde
F^{\mu\n... | [
{
"created": "Tue, 21 Oct 2014 06:20:03 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Cai",
"Wenhe",
""
],
[
"Wu",
"Chao",
""
],
[
"Xiao",
"Zhiguang",
""
]
] | The baryon spectrum in the Sakai-Sugimoto model in the D4 background with smeared D0 charges is studied. We follow the instanton description of baryons by Hata et al.[Prog. Theor. Phys. 117, 1157]. The background corresponds to an excited state with nonzero glue condensate $\langle {\rm tr} (F_{\mu\nu}\tilde F^{\mu\nu}... | 7.865016 | 7.013945 | 8.810266 | 7.213525 | 7.934434 | 7.955834 | 7.511298 | 7.578379 | 7.077231 | 9.1513 | 7.211138 | 7.35781 | 7.621446 | 7.451881 | 7.445058 | 7.235971 | 7.544611 | 7.390439 | 7.360335 | 7.913408 | 7.581817 |
hep-th/9708074 | Paul Townsend | P.K. Townsend | M-branes at angles | 5pp Latex. To appear in proceedings of 1997 Trieste conference on
"Duality Symmetries in String Theory - II". Minor corrections | Nucl.Phys.Proc.Suppl. 67 (1998) 88-92 | 10.1016/S0920-5632(98)00124-8 | null | hep-th | null | Supersymmetric configurations of non-orthogonally intersecting M-5-branes can
be obtained by rotation of one of a pair of parallel M-5-branes. Examples
preserving 1/4, 3/16 and 1/8 supersymmetry are reviewed.
| [
{
"created": "Wed, 13 Aug 1997 15:02:02 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Aug 1997 14:21:32 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Townsend",
"P. K.",
""
]
] | Supersymmetric configurations of non-orthogonally intersecting M-5-branes can be obtained by rotation of one of a pair of parallel M-5-branes. Examples preserving 1/4, 3/16 and 1/8 supersymmetry are reviewed. | 9.418594 | 6.325244 | 8.701661 | 7.088608 | 6.888576 | 6.865928 | 6.628871 | 6.469953 | 7.250727 | 11.692947 | 6.739483 | 6.779947 | 8.966252 | 7.225652 | 6.863253 | 6.786022 | 6.722679 | 6.68274 | 7.359521 | 8.278969 | 6.848366 |
2105.05814 | Koichi Nagasaki | Koichi Nagasaki | D5-brane in AdS black holes with nonzero gauge flux | 15 pages, 14 figures, Typo corrected | null | 10.1142/S0217751X21501906 | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | We find the probe D5-brane solution on the black home spacetime which is
asymptomatically AdS_5 x S^5. These black holes have spherical, hyperbolic and
toroidal structures. Depending on the gauge flux on the D5-brane, the D5-brane
behaves differently. This By adding the fundamental string, the potential
energy of the... | [
{
"created": "Wed, 12 May 2021 17:24:30 GMT",
"version": "v1"
},
{
"created": "Sun, 6 Jun 2021 04:59:52 GMT",
"version": "v2"
}
] | 2021-11-17 | [
[
"Nagasaki",
"Koichi",
""
]
] | We find the probe D5-brane solution on the black home spacetime which is asymptomatically AdS_5 x S^5. These black holes have spherical, hyperbolic and toroidal structures. Depending on the gauge flux on the D5-brane, the D5-brane behaves differently. This By adding the fundamental string, the potential energy of the i... | 19.023634 | 16.449356 | 19.347599 | 16.470453 | 14.581399 | 16.680557 | 15.89098 | 15.2052 | 15.006104 | 22.596445 | 14.800972 | 16.059259 | 17.986822 | 15.883691 | 15.883335 | 16.630352 | 15.379752 | 16.314541 | 16.645502 | 18.091198 | 15.700826 |
0810.2365 | Joanna L. Karczmarek | Joanna L. Karczmarek and Daoyan Wang | Into the bulk: reconstructing spacetime from the c=1 matrix model | 19 pages, 3 figures | Phys.Rev.D82:126004,2010 | 10.1103/PhysRevD.82.126004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We write down exact solutions in the collective field theory of the c=1
matrix model and in dilaton-gravity coupled to a massless scalar. Using the
known correspondence between these two theories at the null boundaries of
spacetime, we make a connection between scalar fields in these two theories in
the bulk of space... | [
{
"created": "Tue, 14 Oct 2008 19:43:21 GMT",
"version": "v1"
}
] | 2010-12-28 | [
[
"Karczmarek",
"Joanna L.",
""
],
[
"Wang",
"Daoyan",
""
]
] | We write down exact solutions in the collective field theory of the c=1 matrix model and in dilaton-gravity coupled to a massless scalar. Using the known correspondence between these two theories at the null boundaries of spacetime, we make a connection between scalar fields in these two theories in the bulk of spaceti... | 11.171835 | 10.045214 | 11.435276 | 9.816901 | 9.875769 | 10.121856 | 11.004378 | 10.296756 | 9.680935 | 11.434186 | 9.68828 | 10.147536 | 10.296846 | 9.956975 | 9.603734 | 10.17942 | 10.024629 | 9.32125 | 9.73088 | 10.829062 | 9.574379 |
hep-th/0006013 | Guang-Hong Chen | Guang-Hong Chen and Yong-Shi Wu | Comments on Noncommutative Open String Theory: V-duality and Holography | 23 pages, RevTex, typos corrected,PRD final version | Phys.Rev. D63 (2001) 086003 | 10.1103/PhysRevD.63.086003 | NSF-ITP-00-47 | hep-th | null | In this paper we study the interplay of electric and magnetic backgrounds in
determining the decoupling limit of coincident D-branes towards a
noncommutative Yang-Mills (NCYM) or open string (NCOS) theory. No decoupling
limit has been found for NCYM with space-time noncommutativity. It is suggested
that there is a ne... | [
{
"created": "Thu, 1 Jun 2000 22:48:24 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Jun 2000 21:48:39 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Dec 2000 20:14:22 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Chen",
"Guang-Hong",
""
],
[
"Wu",
"Yong-Shi",
""
]
] | In this paper we study the interplay of electric and magnetic backgrounds in determining the decoupling limit of coincident D-branes towards a noncommutative Yang-Mills (NCYM) or open string (NCOS) theory. No decoupling limit has been found for NCYM with space-time noncommutativity. It is suggested that there is a new ... | 9.524309 | 8.730798 | 9.559557 | 8.338803 | 8.981887 | 8.600034 | 8.436262 | 8.596118 | 8.292555 | 10.940519 | 8.219502 | 8.099392 | 9.406621 | 8.596997 | 8.578445 | 8.608298 | 8.841938 | 8.324755 | 8.666864 | 9.150854 | 8.251466 |
2110.05919 | Turmoli Neogi | Nabamita Banerjee, Arindam Bhattacharjee, Surajit Biswas and Turmoli
Neogi | Dual Theory for maximally $\mathcal{N}$ extended flat Supergravity | 23 pages, typos corrected, 2 references added, some explanation
included | null | 10.1007/JHEP05(2022)179 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Maximally $\mathcal{N}$ extended $2+1$ dimensional flat Supergravity theories
exist for a class of super-Poincar\'{e} algebras for arbitrary $\mathcal{N}$.
They have rich asymptotic structures and contain all interesting topological
supergravity solutions in presence of non-trivial holonomy. For the asymptotic
symmet... | [
{
"created": "Tue, 12 Oct 2021 12:05:21 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Mar 2022 16:42:12 GMT",
"version": "v2"
}
] | 2022-06-15 | [
[
"Banerjee",
"Nabamita",
""
],
[
"Bhattacharjee",
"Arindam",
""
],
[
"Biswas",
"Surajit",
""
],
[
"Neogi",
"Turmoli",
""
]
] | Maximally $\mathcal{N}$ extended $2+1$ dimensional flat Supergravity theories exist for a class of super-Poincar\'{e} algebras for arbitrary $\mathcal{N}$. They have rich asymptotic structures and contain all interesting topological supergravity solutions in presence of non-trivial holonomy. For the asymptotic symmetry... | 10.775438 | 8.696354 | 9.285988 | 8.738732 | 8.633592 | 9.25438 | 9.325548 | 9.387938 | 9.140557 | 10.128876 | 8.895762 | 9.370468 | 9.26549 | 9.008751 | 9.037899 | 8.697853 | 8.970356 | 9.120016 | 9.124551 | 9.19228 | 9.03231 |
1809.05770 | Irfan Ilgin | Irfan Ilgin | Bekenstein bound in the bulk and AdS/CFT | 34 pages, 3 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we identify the change in the boundary full modular
hamiltonian with the bulk observables for spherically symmetric excitations.
The identification is demonstrated for perturbative as well as non perturbative
excitations. We introduce the notion of the sphere of ignorance, that describes
the bulk regio... | [
{
"created": "Sat, 15 Sep 2018 21:06:42 GMT",
"version": "v1"
}
] | 2018-09-18 | [
[
"Ilgin",
"Irfan",
""
]
] | In this paper, we identify the change in the boundary full modular hamiltonian with the bulk observables for spherically symmetric excitations. The identification is demonstrated for perturbative as well as non perturbative excitations. We introduce the notion of the sphere of ignorance, that describes the bulk region ... | 13.466286 | 12.654997 | 13.816085 | 12.244761 | 13.044035 | 12.268538 | 13.136482 | 12.768672 | 12.721333 | 14.22845 | 12.573255 | 11.700145 | 12.958017 | 12.07197 | 11.855497 | 12.132699 | 11.789141 | 12.323432 | 11.918838 | 12.783924 | 12.338829 |
hep-th/9406003 | Stam Nicolis | A. Hulsebos, C. P. Korthals-Altes and S. Nicolis | Gauge Theories with a Layered Phase | 17 pages+9 figures (in LATeX and PostScript in a uuencoded,
compressed tar file appended at the end of the LATeX file) , CPT-94/P.3036 | Nucl.Phys. B450 (1995) 437-451 | 10.1016/0550-3213(95)00306-D | null | hep-th | null | We study abelian gauge theories with anisotropic couplings in $4+D$
dimensions. A layered phase is present, in the absence as well as in the
presence of fermions. A line of second order transitions separates the layered
from the Coulomb phase, if $D\leq 3$.
| [
{
"created": "Wed, 1 Jun 1994 12:13:54 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Hulsebos",
"A.",
""
],
[
"Korthals-Altes",
"C. P.",
""
],
[
"Nicolis",
"S.",
""
]
] | We study abelian gauge theories with anisotropic couplings in $4+D$ dimensions. A layered phase is present, in the absence as well as in the presence of fermions. A line of second order transitions separates the layered from the Coulomb phase, if $D\leq 3$. | 9.932606 | 9.165586 | 9.250085 | 8.41629 | 8.082607 | 8.966768 | 8.56437 | 8.244366 | 9.101282 | 8.476502 | 9.122428 | 8.472043 | 9.225799 | 8.686836 | 8.649992 | 8.723944 | 8.713426 | 8.680962 | 9.206357 | 9.034192 | 8.287201 |
hep-th/9502060 | Weston Robert | Michio Jimbo, Rinat Kedem, Hitoshi Konno, Tetsuji Miwa and Robert
Weston | Difference Equations in Spin Chains with a Boundary | 28 pages, LaTeX with amssymbols.sty, 7 uuencoded postscript figures | Nucl.Phys. B448 (1995) 429-456 | 10.1016/0550-3213(95)00218-H | RIMS-1005, CRM-2246 | hep-th | null | Correlation functions and form factors in vertex models or spin chains are
known to satisfy certain difference equations called the quantum
Knizhnik-Zamolodchikov equations. We find similar difference equations for the
case of semi-infinite spin chain systems with integrable boundary conditions.
We derive these equat... | [
{
"created": "Fri, 10 Feb 1995 03:10:50 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Jimbo",
"Michio",
""
],
[
"Kedem",
"Rinat",
""
],
[
"Konno",
"Hitoshi",
""
],
[
"Miwa",
"Tetsuji",
""
],
[
"Weston",
"Robert",
""
]
] | Correlation functions and form factors in vertex models or spin chains are known to satisfy certain difference equations called the quantum Knizhnik-Zamolodchikov equations. We find similar difference equations for the case of semi-infinite spin chain systems with integrable boundary conditions. We derive these equatio... | 8.965656 | 8.807063 | 10.796099 | 8.139662 | 8.626542 | 8.704331 | 8.865133 | 8.258733 | 7.693864 | 11.1868 | 8.18003 | 7.760713 | 9.038465 | 7.725217 | 7.677305 | 7.635631 | 7.667462 | 7.648711 | 7.782813 | 8.68587 | 7.77218 |
hep-th/0610317 | Mikhail Plyushchay | Peter A. Horvathy, Mikhail S. Plyushchay and Mauricio Valenzuela | Bosonized supersymmetry of anyons and supersymmetric exotic particle on
the non-commutative plane | 18 pages; new section on noncommutative coordinates and refs added,
the version to appear in Nucl. Phys. B | Nucl.Phys.B768:247-262,2007 | 10.1016/j.nuclphysb.2007.01.021 | null | hep-th math-ph math.MP quant-ph | null | A covariant set of linear differential field equations, describing an N=1
supersymmetric anyon system in (2+1)D, is proposed in terms of Wigner's
deformation of the bosonic Heisenberg algebra. The non-relativistic
``Jackiw-Nair'' limit extracts the ordinary bosonic and fermionic degrees of
freedom from the Heisenberg... | [
{
"created": "Mon, 30 Oct 2006 19:13:41 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Jan 2007 03:49:43 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Horvathy",
"Peter A.",
""
],
[
"Plyushchay",
"Mikhail S.",
""
],
[
"Valenzuela",
"Mauricio",
""
]
] | A covariant set of linear differential field equations, describing an N=1 supersymmetric anyon system in (2+1)D, is proposed in terms of Wigner's deformation of the bosonic Heisenberg algebra. The non-relativistic ``Jackiw-Nair'' limit extracts the ordinary bosonic and fermionic degrees of freedom from the Heisenberg-W... | 12.089274 | 9.750966 | 14.036166 | 10.523258 | 9.897062 | 10.063134 | 9.846732 | 10.509605 | 10.244933 | 15.80852 | 10.06321 | 9.953163 | 11.916226 | 10.22239 | 10.328503 | 10.176387 | 9.818763 | 10.076557 | 10.362993 | 12.114656 | 10.655564 |
1612.07672 | Andreas Kapfer | Andreas Kapfer | Geometric Symmetries and Topological Terms in F-theory and Field Theory | PhD Thesis | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this thesis we investigate topological aspects and arithmetic structures
in quantum field theory and string theory. Particular focus is put on
consistent truncations of supergravity and compactifications of F-theory.
| [
{
"created": "Thu, 22 Dec 2016 16:04:48 GMT",
"version": "v1"
}
] | 2016-12-23 | [
[
"Kapfer",
"Andreas",
""
]
] | In this thesis we investigate topological aspects and arithmetic structures in quantum field theory and string theory. Particular focus is put on consistent truncations of supergravity and compactifications of F-theory. | 9.591631 | 6.110763 | 8.784044 | 6.438642 | 6.914947 | 7.088583 | 6.546276 | 6.256729 | 6.619611 | 8.338332 | 6.939296 | 7.069153 | 7.708681 | 7.094096 | 7.050494 | 6.894615 | 6.79496 | 6.896734 | 6.581025 | 7.568773 | 7.064122 |
hep-th/9406162 | John Gracey | J.A. Gracey | The Beta-Function of the Chiral Gross Neveu Model at O(1/N^2) | 17 latex pages, 3 figures available from author on request, LTH-335 | Phys.Rev.D50:2840-2847,1994; Erratum-ibid.D59:109904,1999 | 10.1103/PhysRevD.50.2840 10.1103/PhysRevD.59.109904 | null | hep-th | null | We compute the $O(1/N^2)$ correction to the critical exponent $2\lambda$ $=$
$-$ $\beta^\prime(g_c)$ for the chiral Gross Neveu model in arbitrary
dimensions by substituting the corrections to the asymptotic scaling forms of
the propagators into the Schwinger Dyson equations and solving the resulting
consistency equa... | [
{
"created": "Fri, 24 Jun 1994 09:25:00 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Gracey",
"J. A.",
""
]
] | We compute the $O(1/N^2)$ correction to the critical exponent $2\lambda$ $=$ $-$ $\beta^\prime(g_c)$ for the chiral Gross Neveu model in arbitrary dimensions by substituting the corrections to the asymptotic scaling forms of the propagators into the Schwinger Dyson equations and solving the resulting consistency equati... | 11.327982 | 10.194595 | 11.955748 | 10.38325 | 10.409903 | 10.290813 | 9.232432 | 8.797059 | 9.537793 | 13.870584 | 9.308904 | 9.89291 | 10.865123 | 10.548539 | 10.326947 | 10.266613 | 9.585023 | 10.158994 | 10.164873 | 11.167669 | 9.852136 |
2304.12977 | Ashutosh Dash | Ashutosh Dash, Ankit Kumar Panda | Charged participants and their electromagnetic fields in an expanding
fluid | 13 pages, 5 figures. Minor revisions and a new figure showing domain
of influence added | null | null | null | hep-th nucl-th physics.flu-dyn | http://creativecommons.org/licenses/by/4.0/ | We investigate the space-time dependence of electromagnetic fields produced
by charged participants in an expanding fluid. To address this problem, we need
to solve the Maxwell's equations coupled to the hydrodynamics conservation
equation, specifically the relativistic magnetohydrodynamics (RMHD) equations,
since th... | [
{
"created": "Tue, 25 Apr 2023 16:35:18 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Nov 2023 15:05:21 GMT",
"version": "v2"
}
] | 2023-11-23 | [
[
"Dash",
"Ashutosh",
""
],
[
"Panda",
"Ankit Kumar",
""
]
] | We investigate the space-time dependence of electromagnetic fields produced by charged participants in an expanding fluid. To address this problem, we need to solve the Maxwell's equations coupled to the hydrodynamics conservation equation, specifically the relativistic magnetohydrodynamics (RMHD) equations, since the ... | 10.537504 | 11.397242 | 10.576804 | 9.922319 | 11.197267 | 11.642668 | 11.274525 | 11.048529 | 10.456582 | 11.217435 | 10.426739 | 10.488397 | 10.237497 | 10.096057 | 10.35549 | 10.755275 | 10.455001 | 10.596214 | 9.93128 | 10.339028 | 10.192558 |
hep-th/0205083 | Adam Ritz | A. Ritz, M. Shifman, A. Vainshtein | Counting Domain Walls in N=1 Super Yang-Mills Theory | 28 pages, RevTeX, 3 figures; v2: discussion of the index slightly
expanded, using an alternative regulator, and references added; v3: typos
corrected, to appear in Phys. Rev. D | Phys.Rev. D66 (2002) 065015 | 10.1103/PhysRevD.66.065015 | null | hep-th | null | We study the multiplicity of BPS domain walls in N=1 super Yang-Mills theory,
by passing to a weakly coupled Higgs phase through the addition of fundamental
matter. The number of domain walls connecting two specified vacuum states is
then determined via the Witten index of the induced worldvolume theory, which
is inv... | [
{
"created": "Thu, 9 May 2002 18:13:31 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Jun 2002 11:19:21 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Aug 2002 14:34:40 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Ritz",
"A.",
""
],
[
"Shifman",
"M.",
""
],
[
"Vainshtein",
"A.",
""
]
] | We study the multiplicity of BPS domain walls in N=1 super Yang-Mills theory, by passing to a weakly coupled Higgs phase through the addition of fundamental matter. The number of domain walls connecting two specified vacuum states is then determined via the Witten index of the induced worldvolume theory, which is invar... | 7.176864 | 7.635363 | 9.801908 | 7.571839 | 7.660261 | 7.180399 | 7.394826 | 7.849848 | 7.711303 | 9.488847 | 7.064042 | 7.10708 | 8.019176 | 7.198665 | 7.089083 | 7.17771 | 7.192777 | 7.062701 | 7.437314 | 7.867436 | 6.943815 |
2207.04559 | Job Furtado Neto | J. Furtado, C. R. Muniz, M. S. Cunha, J. E. G. Silva | On quantum traversability of wormholes | 5 pages, two columuns, 3 figures | null | 10.1142/S0218271823500566 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | In this paper we study the possibility of non-relativistic quantum particles
to traverse the generalized Ellis-Bronnikov wormholes by considering quantum
effects, such as tunneling. We have used the generalized Ellis-Bronnikov
wormhole metric and found that for $n=2$ we have a single barrier shaped
effective potentia... | [
{
"created": "Sun, 10 Jul 2022 22:42:33 GMT",
"version": "v1"
}
] | 2023-08-16 | [
[
"Furtado",
"J.",
""
],
[
"Muniz",
"C. R.",
""
],
[
"Cunha",
"M. S.",
""
],
[
"Silva",
"J. E. G.",
""
]
] | In this paper we study the possibility of non-relativistic quantum particles to traverse the generalized Ellis-Bronnikov wormholes by considering quantum effects, such as tunneling. We have used the generalized Ellis-Bronnikov wormhole metric and found that for $n=2$ we have a single barrier shaped effective potential ... | 5.904558 | 6.311737 | 5.452783 | 5.377993 | 5.718973 | 5.890892 | 6.19881 | 5.322883 | 6.183948 | 5.516985 | 5.906735 | 5.8199 | 5.371612 | 5.684864 | 5.696375 | 5.604957 | 5.688629 | 5.465783 | 5.954092 | 5.454931 | 5.624178 |
2203.08842 | A. Ramesh Chandra | A. Ramesh Chandra, Jan de Boer, Mario Flory, Michal P. Heller, Sergio
H\"ortner, Andrew Rolph | Cost of holographic path integrals | 53 pages + appendices, 15 figures; v2: added references, v3: minor
corrections, added a figure in section 4 | SciPost Phys. 14, 061 (2023) | 10.21468/SciPostPhys.14.4.061 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider proposals for the cost of holographic path integrals.
Gravitational path integrals within finite radial cutoff surfaces have a
precise map to path integrals in $T\bar T$ deformed holographic CFTs. In
Nielsen's geometric formulation cost is the length of a
not-necessarily-geodesic path in a metric space of... | [
{
"created": "Wed, 16 Mar 2022 18:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Jun 2022 17:43:28 GMT",
"version": "v2"
},
{
"created": "Mon, 10 Oct 2022 11:02:59 GMT",
"version": "v3"
}
] | 2023-04-05 | [
[
"Chandra",
"A. Ramesh",
""
],
[
"de Boer",
"Jan",
""
],
[
"Flory",
"Mario",
""
],
[
"Heller",
"Michal P.",
""
],
[
"Hörtner",
"Sergio",
""
],
[
"Rolph",
"Andrew",
""
]
] | We consider proposals for the cost of holographic path integrals. Gravitational path integrals within finite radial cutoff surfaces have a precise map to path integrals in $T\bar T$ deformed holographic CFTs. In Nielsen's geometric formulation cost is the length of a not-necessarily-geodesic path in a metric space of o... | 16.10181 | 17.772781 | 17.887119 | 15.000559 | 16.854427 | 17.669395 | 17.237389 | 15.527107 | 15.584593 | 20.931261 | 14.753345 | 15.624476 | 17.06163 | 15.41542 | 15.729241 | 16.017206 | 15.573432 | 15.594907 | 15.107141 | 17.054497 | 15.55625 |
1409.4948 | Paul Mansfield | James P. Edwards and Paul Mansfield | QED as the tensionless limit of the spinning string with contact
interaction | 11 pages, no figures | null | 10.1016/j.physletb.2015.05.024 | DCPT-14/39 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We outline how QED with spinor matter can be described by the tensionless
limit of spinning strings with contact interactions. The strings represent
electric lines of force with charges at their ends. The contact interaction is
constructed from a delta-function on the world-sheet which, although off-shell,
decouples ... | [
{
"created": "Wed, 17 Sep 2014 11:21:52 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Edwards",
"James P.",
""
],
[
"Mansfield",
"Paul",
""
]
] | We outline how QED with spinor matter can be described by the tensionless limit of spinning strings with contact interactions. The strings represent electric lines of force with charges at their ends. The contact interaction is constructed from a delta-function on the world-sheet which, although off-shell, decouples fr... | 13.786077 | 12.734783 | 13.943871 | 13.216206 | 14.164901 | 13.569584 | 14.944724 | 13.248528 | 14.125072 | 16.942724 | 13.51827 | 13.696125 | 13.812163 | 13.203617 | 13.39831 | 14.164089 | 13.56327 | 13.197684 | 13.245646 | 13.438905 | 13.015755 |
hep-th/0403009 | Nobuhito Maru | Minoru Eto, Nobuhito Maru and Norisuke Sakai | Radius Stabilization in a Supersymmetric Warped Compactification | 6 pages, revtex, Errors of the products of distributions are
corrected and the results are reanalyzed, references added, final version to
appear in PRD | Phys.Rev.D70:086002,2004 | 10.1103/PhysRevD.70.086002 | TIT/HEP-517 | hep-th hep-ph | null | A supersymmetric (SUSY) model of radius stabilization is constructed for the
S^1/Z_2 warped compactifications with a hypermultiplet in five dimensions.
Requiring the continuity of scalar field across the boundaries, we obtain
radius stabilization preserving SUSY, realizing the SUSY extension of the
Goldberger-Wise me... | [
{
"created": "Mon, 1 Mar 2004 19:00:05 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Apr 2004 11:01:47 GMT",
"version": "v2"
},
{
"created": "Tue, 20 Apr 2004 08:14:37 GMT",
"version": "v3"
},
{
"created": "Tue, 7 Sep 2004 06:13:11 GMT",
"version": "v4"
}
] | 2010-11-19 | [
[
"Eto",
"Minoru",
""
],
[
"Maru",
"Nobuhito",
""
],
[
"Sakai",
"Norisuke",
""
]
] | A supersymmetric (SUSY) model of radius stabilization is constructed for the S^1/Z_2 warped compactifications with a hypermultiplet in five dimensions. Requiring the continuity of scalar field across the boundaries, we obtain radius stabilization preserving SUSY, realizing the SUSY extension of the Goldberger-Wise mech... | 11.277538 | 10.515115 | 11.306932 | 10.74637 | 11.913286 | 10.834102 | 10.905786 | 10.771886 | 10.259344 | 12.218156 | 10.862828 | 10.19069 | 10.155574 | 10.093323 | 10.660135 | 10.440442 | 10.232175 | 10.261531 | 10.387044 | 10.79433 | 10.288873 |
1501.00211 | Peter Mati | P. Mati | Vanishing Beta Function curves from the Functional Renormalisation Group | 29 pages, 44 figures, uses revtex4-1, some minor improvements,
Appendix is added | Phys. Rev. D 91, 125038 (2015) | 10.1103/PhysRevD.91.125038 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we will discuss the derivation of the so-called vanishing beta
function curves which can be used to explore the fixed point structure of the
theory under consideration. This can be applied to the O($N$) symmetric
theories, essentially, for arbitrary dimensions ($D$) and field component
($N$). We will sh... | [
{
"created": "Wed, 31 Dec 2014 21:17:12 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Jan 2015 12:50:12 GMT",
"version": "v2"
},
{
"created": "Wed, 16 Sep 2015 21:54:54 GMT",
"version": "v3"
}
] | 2015-09-18 | [
[
"Mati",
"P.",
""
]
] | In this paper we will discuss the derivation of the so-called vanishing beta function curves which can be used to explore the fixed point structure of the theory under consideration. This can be applied to the O($N$) symmetric theories, essentially, for arbitrary dimensions ($D$) and field component ($N$). We will show... | 8.399194 | 9.049505 | 9.2613 | 8.240028 | 10.318089 | 9.075576 | 9.274078 | 8.793995 | 8.393366 | 10.267208 | 8.544986 | 8.487613 | 8.528271 | 8.174155 | 8.256419 | 8.373059 | 8.464508 | 8.348115 | 7.979604 | 8.365688 | 8.165151 |
hep-th/9411044 | Suzuki Takeshi | Takeshi Suzuki | Finite-Dimensionality of the Space of Conformal Blocks | 9 pages, AMS-Tex Version 2.1 | null | null | RIMS-996 | hep-th | null | Without using Gabber's theorem, the finite-dimensionality of the space of
conformal blocks in the WZNW-models is proved.
| [
{
"created": "Mon, 7 Nov 1994 12:04:48 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Dec 1994 07:28:23 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Suzuki",
"Takeshi",
""
]
] | Without using Gabber's theorem, the finite-dimensionality of the space of conformal blocks in the WZNW-models is proved. | 22.873154 | 12.732636 | 21.984087 | 17.447067 | 15.206437 | 15.947821 | 15.975324 | 12.410759 | 12.913306 | 17.070076 | 12.422876 | 12.376824 | 20.181814 | 13.18823 | 12.6554 | 12.634303 | 12.801975 | 12.478746 | 13.438928 | 19.187151 | 14.891685 |
hep-th/0112101 | Takao Suyama | Takao Suyama | Charged Tachyons and Gauge Symmetry Breaking | 19 pages, 2 figures | JHEP 0202 (2002) 033 | 10.1088/1126-6708/2002/02/033 | KEK-TH-795 | hep-th | null | We discuss the condensation of charged tachyons in the heterotic theory on
the Kaluza-Klein Melvin background. The arguments are based on duality
relations which are expected to hold from the adiabatic argument. It is argued
that in many cases the rank of the gauge group is not changed by the
condensation, as opposed... | [
{
"created": "Wed, 12 Dec 2001 05:04:32 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Suyama",
"Takao",
""
]
] | We discuss the condensation of charged tachyons in the heterotic theory on the Kaluza-Klein Melvin background. The arguments are based on duality relations which are expected to hold from the adiabatic argument. It is argued that in many cases the rank of the gauge group is not changed by the condensation, as opposed t... | 10.334786 | 8.167777 | 10.188377 | 8.275097 | 7.637376 | 8.10461 | 7.842544 | 8.648287 | 8.154795 | 10.663081 | 8.235016 | 8.909093 | 10.252967 | 8.578277 | 9.256192 | 8.639042 | 8.344934 | 9.204649 | 8.739919 | 10.524255 | 8.729951 |
hep-th/0312245 | Dileep Jatkar | Debashis Ghoshal, Dileep P. Jatkar and Maximilian Kreuzer | NS Fivebrane and Tachyon Condensation | 20 pages, harvmac | J.Math.Phys. 46 (2005) 062301 | 10.1063/1.1922069 | HRI-P/0312-001, TUW-03-39 | hep-th | null | We argue that a semi-infinite D6-brane ending on an NS5-brane can be obtained
from the condensation of the tachyon on the unstable D9-brane of type IIA
theory. The construction uses a combination of the descriptions of these branes
as solitons of the worldvolume theory of the D9-brane. The NS5-brane, in
particular, i... | [
{
"created": "Fri, 19 Dec 2003 15:15:10 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ghoshal",
"Debashis",
""
],
[
"Jatkar",
"Dileep P.",
""
],
[
"Kreuzer",
"Maximilian",
""
]
] | We argue that a semi-infinite D6-brane ending on an NS5-brane can be obtained from the condensation of the tachyon on the unstable D9-brane of type IIA theory. The construction uses a combination of the descriptions of these branes as solitons of the worldvolume theory of the D9-brane. The NS5-brane, in particular, inv... | 8.573742 | 7.444301 | 10.025152 | 7.342833 | 7.311465 | 7.300926 | 7.383467 | 7.660268 | 7.709002 | 10.682878 | 7.83381 | 7.50178 | 9.180842 | 8.045772 | 7.73946 | 7.652229 | 7.81756 | 7.80593 | 7.936466 | 9.051827 | 7.863352 |
2207.03055 | Ali Kaya | Ali Kaya | Superhairs on the Branes of D =11 Supergravity | 16 pages, dedicated to the memory of Rahmi G\"uven, v2: comments and
references added, to appear in Phy. Rev. D | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that membrane and fivebrane of D=11 supergravity theory can
support nongauge, linearized spin-3/2 superhairs. Supercharges associated with
these fields are calculated. We also generalize the solutions to some
overlapping cases and discuss possible implications of their existence.
| [
{
"created": "Thu, 7 Jul 2022 02:47:56 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Oct 2022 12:51:27 GMT",
"version": "v2"
}
] | 2022-10-20 | [
[
"Kaya",
"Ali",
""
]
] | It is shown that membrane and fivebrane of D=11 supergravity theory can support nongauge, linearized spin-3/2 superhairs. Supercharges associated with these fields are calculated. We also generalize the solutions to some overlapping cases and discuss possible implications of their existence. | 29.36994 | 24.409437 | 23.557041 | 20.961584 | 22.176863 | 20.167727 | 25.484415 | 19.46969 | 20.625977 | 24.669882 | 20.593231 | 20.191086 | 22.277546 | 20.712599 | 21.681522 | 21.204269 | 20.547237 | 20.580091 | 20.305325 | 22.227409 | 19.330919 |
hep-th/0206072 | Frederik Denef | Frederik Denef | Quantum Quivers and Hall/Hole Halos | 39 pages, 10 figures. v2: minor errors corrected and some parts
rewritten for clarity. v3: references added | JHEP 0210:023,2002 | 10.1088/1126-6708/2002/10/023 | null | hep-th | null | Two pictures of BPS bound states in Calabi-Yau compactifications of type II
string theory exist, one as a set of particles at equilibrium separations from
each other, the other as a fusion of D-branes at a single point of space. We
show how quiver quantum mechanics smoothly interpolates between the two, and
use this,... | [
{
"created": "Sun, 9 Jun 2002 23:20:47 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Aug 2002 11:23:47 GMT",
"version": "v2"
},
{
"created": "Tue, 13 Aug 2002 19:04:22 GMT",
"version": "v3"
}
] | 2011-09-29 | [
[
"Denef",
"Frederik",
""
]
] | Two pictures of BPS bound states in Calabi-Yau compactifications of type II string theory exist, one as a set of particles at equilibrium separations from each other, the other as a fusion of D-branes at a single point of space. We show how quiver quantum mechanics smoothly interpolates between the two, and use this, t... | 11.041717 | 10.796739 | 11.070292 | 9.796352 | 10.491708 | 9.736632 | 10.474026 | 9.971391 | 10.032708 | 11.853524 | 10.36652 | 9.617335 | 10.239934 | 9.450015 | 9.559439 | 10.053343 | 10.039245 | 9.408512 | 9.517494 | 9.927556 | 9.58165 |
2002.02317 | Juraj Tekel | M\'aria \v{S}ubjakov\'a, Juraj Tekel | Second moment fuzzy-field-theory-like matrix models | 21 pages, 3 figures; v2 - slight modifications, references added,
published version | J. High Energ. Phys. 2020, 88 (2020) | 10.1007/JHEP06(2020)088 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We solve a multitrace matrix model approximating the real quartic scalar
field theory on the fuzzy sphere and obtain its phase diagram. We generalize
this method to models with modified kinetic terms and demonstrate its use by
investigating models related to the removal of the UV/IR mixing. We show that
for the fuzzy... | [
{
"created": "Thu, 6 Feb 2020 15:46:07 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Jun 2020 20:32:59 GMT",
"version": "v2"
}
] | 2020-06-24 | [
[
"Šubjaková",
"Mária",
""
],
[
"Tekel",
"Juraj",
""
]
] | We solve a multitrace matrix model approximating the real quartic scalar field theory on the fuzzy sphere and obtain its phase diagram. We generalize this method to models with modified kinetic terms and demonstrate its use by investigating models related to the removal of the UV/IR mixing. We show that for the fuzzy s... | 12.534273 | 9.553847 | 13.572191 | 10.540771 | 10.412421 | 10.783631 | 9.531174 | 10.475567 | 10.497796 | 14.131941 | 10.888387 | 11.151373 | 12.598147 | 11.446672 | 11.603876 | 11.754855 | 11.092576 | 11.799649 | 11.457384 | 12.319314 | 11.557092 |
hep-th/0311039 | Jorgen Rasmussen | F. Lesage, P. Mathieu, J. Rasmussen, H. Saleur | Logarithmic lift of the su(2)_{-1/2} model | 28 pages, 9 figures, v2: presentation modified, version to be
published | Nucl.Phys.B686:313-346,2004 | 10.1016/j.nuclphysb.2004.02.039 | null | hep-th | null | This paper carries on the investigation of the non-unitary su(2)_{-1/2} WZW
model. An essential tool in our first work on this topic was a free-field
representation, based on a c=-2 \eta\xi ghost system, and a Lorentzian boson.
It turns out that there are several ``versions'' of the \eta\xi system,
allowing different... | [
{
"created": "Wed, 5 Nov 2003 17:54:14 GMT",
"version": "v1"
},
{
"created": "Sun, 23 May 2004 01:39:17 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Lesage",
"F.",
""
],
[
"Mathieu",
"P.",
""
],
[
"Rasmussen",
"J.",
""
],
[
"Saleur",
"H.",
""
]
] | This paper carries on the investigation of the non-unitary su(2)_{-1/2} WZW model. An essential tool in our first work on this topic was a free-field representation, based on a c=-2 \eta\xi ghost system, and a Lorentzian boson. It turns out that there are several ``versions'' of the \eta\xi system, allowing different s... | 10.833893 | 10.744871 | 12.943375 | 10.636316 | 10.756351 | 11.02858 | 10.892076 | 10.754745 | 10.647374 | 13.174356 | 10.270445 | 10.392406 | 11.15574 | 10.403498 | 10.475347 | 10.629361 | 10.363935 | 10.460374 | 10.465571 | 11.54585 | 10.414318 |
0708.3656 | Ramond | Pierre Ramond | Memoirs of an Early String Theorist | Contribution to the "Birth of String Theory" Commemorative Volume | null | null | UFIFT-HEP-07-12 | hep-th | null | I worked on String Theory over a period of five years during the First String
Era, the most intellectually satisfying years of my scientific life. One of the
early prospectors in the String Theory Mine, I was fortunate enough to
contribute to the birth of this subject, which retains after these many years,
its magica... | [
{
"created": "Mon, 27 Aug 2007 17:51:07 GMT",
"version": "v1"
}
] | 2007-08-28 | [
[
"Ramond",
"Pierre",
""
]
] | I worked on String Theory over a period of five years during the First String Era, the most intellectually satisfying years of my scientific life. One of the early prospectors in the String Theory Mine, I was fortunate enough to contribute to the birth of this subject, which retains after these many years, its magical ... | 20.08198 | 20.462658 | 23.726772 | 20.713661 | 21.608862 | 20.477104 | 21.571142 | 21.763334 | 21.955175 | 20.974737 | 21.092707 | 20.328085 | 20.009501 | 21.249994 | 20.537643 | 20.785151 | 19.720026 | 20.569933 | 20.107323 | 20.778273 | 19.902197 |
1307.0809 | Tatsuo Azeyanagi | Tatsuo Azeyanagi, Masanori Hanada, Masazumi Honda, Yoshinori Matsuo
and Shotaro Shiba | A new look at instantons and large-N limit | 10 pages | null | 10.1007/JHEP05(2014)008 | YITP-13-50, KEK-TH-1638 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze instantons in the very strongly coupled large-$N$ limit
($N\to\infty$ with $g^2$ fixed) of large-$N$ gauge theories, where the effect
of the instantons remains finite. By using the exact partition function of
four-dimensional ${\cal N}=2^*$ gauge theories as a concrete example, we
demonstrate that each ins... | [
{
"created": "Tue, 2 Jul 2013 19:56:06 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Azeyanagi",
"Tatsuo",
""
],
[
"Hanada",
"Masanori",
""
],
[
"Honda",
"Masazumi",
""
],
[
"Matsuo",
"Yoshinori",
""
],
[
"Shiba",
"Shotaro",
""
]
] | We analyze instantons in the very strongly coupled large-$N$ limit ($N\to\infty$ with $g^2$ fixed) of large-$N$ gauge theories, where the effect of the instantons remains finite. By using the exact partition function of four-dimensional ${\cal N}=2^*$ gauge theories as a concrete example, we demonstrate that each insta... | 5.753551 | 5.781787 | 6.312654 | 5.460911 | 5.498826 | 5.428056 | 5.39302 | 5.464659 | 5.219595 | 6.705538 | 5.562437 | 5.609082 | 5.851577 | 5.607416 | 5.377811 | 5.375507 | 5.516316 | 5.521812 | 5.574194 | 5.929399 | 5.326266 |
hep-th/9801037 | null | Rika Endo, Rie Kuriki, Shin'ichi Nojiri, and Akio Sugamoto | A Rule of Thumb Derivation of Born-Infeld Action for D-branes | 9 pages, Latex, minor corrections | Mod.Phys.Lett. A13 (1998) 1309-1318 | 10.1142/S0217732398001364 | OCHA-PP-107, NDA-FP-43 | hep-th | null | A rule of thumb derivation of the Dirac-Born-Infeld action for D-branes is
studied \`a la Fradkin and Tseytlin, by simply integrating out of the
superstring coordinates in a narrow strip attached to the D-branes. In case of
superstrings, the coupling of Ramond-Ramond fields as well as the
Dirac-Born-Infeld type coupl... | [
{
"created": "Thu, 8 Jan 1998 05:57:25 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jan 1998 06:32:19 GMT",
"version": "v2"
},
{
"created": "Mon, 19 Apr 1999 04:59:31 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Endo",
"Rika",
""
],
[
"Kuriki",
"Rie",
""
],
[
"Nojiri",
"Shin'ichi",
""
],
[
"Sugamoto",
"Akio",
""
]
] | A rule of thumb derivation of the Dirac-Born-Infeld action for D-branes is studied \`a la Fradkin and Tseytlin, by simply integrating out of the superstring coordinates in a narrow strip attached to the D-branes. In case of superstrings, the coupling of Ramond-Ramond fields as well as the Dirac-Born-Infeld type couplin... | 9.063178 | 8.340213 | 9.77427 | 8.15505 | 9.953654 | 8.339998 | 8.4862 | 8.203502 | 8.155147 | 11.539804 | 8.316699 | 8.003917 | 8.937689 | 8.320487 | 8.401834 | 8.152412 | 8.169032 | 8.196663 | 8.481689 | 9.190544 | 7.949067 |
hep-th/0403152 | Ivan K. Kostov | V. Kazakov and I. Kostov | Instantons in Non-Critical strings from the Two-Matrix Model | References and figures added, improved presentation | null | 10.1142/9789812775344_0045 | SPhT-04/026, LPTENS-04/10 | hep-th | null | We derive the non-perturbative corrections to the free energy of the
two-matrix model in terms of its algebraic curve. The eigenvalue instantons are
associated with the vanishing cycles of the curve. For the (p,q) critical
points our results agree with the geometrical interpretation of the instanton
effects recently ... | [
{
"created": "Mon, 15 Mar 2004 14:16:04 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Mar 2004 19:21:54 GMT",
"version": "v2"
},
{
"created": "Fri, 14 May 2004 19:06:08 GMT",
"version": "v3"
}
] | 2016-11-23 | [
[
"Kazakov",
"V.",
""
],
[
"Kostov",
"I.",
""
]
] | We derive the non-perturbative corrections to the free energy of the two-matrix model in terms of its algebraic curve. The eigenvalue instantons are associated with the vanishing cycles of the curve. For the (p,q) critical points our results agree with the geometrical interpretation of the instanton effects recently di... | 10.075205 | 9.408212 | 12.057343 | 9.291099 | 9.419465 | 9.144047 | 8.704554 | 9.140553 | 9.079308 | 12.550498 | 9.101138 | 9.365841 | 11.349933 | 9.522159 | 9.482133 | 9.34723 | 9.150727 | 9.199644 | 9.333354 | 11.621509 | 9.288961 |
2404.11600 | Roman Mauch | Roman Mauch and Lorenzo Ruggeri | Super Yang-Mills on Branched Covers and Weighted Projective Spaces | 22 pages; 9 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this work we conjecture the Coulomb branch partition function, including
flux and instanton contributions, for the $\mathcal{N}=2$ vector multiplet on
weighted projective space $\mathbb{CP}^2_{\boldsymbol{N}}$ for equivariant
Donaldson-Witten and ``Pestun-like'' theories. More precisely, we claim that
this partiti... | [
{
"created": "Wed, 17 Apr 2024 17:50:31 GMT",
"version": "v1"
}
] | 2024-04-18 | [
[
"Mauch",
"Roman",
""
],
[
"Ruggeri",
"Lorenzo",
""
]
] | In this work we conjecture the Coulomb branch partition function, including flux and instanton contributions, for the $\mathcal{N}=2$ vector multiplet on weighted projective space $\mathbb{CP}^2_{\boldsymbol{N}}$ for equivariant Donaldson-Witten and ``Pestun-like'' theories. More precisely, we claim that this partition... | 8.10413 | 8.671521 | 8.806614 | 7.941378 | 8.585346 | 8.311523 | 8.493738 | 8.288493 | 8.617744 | 9.809966 | 8.272967 | 8.08862 | 7.705533 | 7.597693 | 8.142035 | 8.244399 | 7.909616 | 7.644169 | 7.986559 | 8.028062 | 7.809964 |
hep-th/0512338 | Patricio Gaete | Patricio Gaete and Clovis Wotzasek | Physical and mathematical evidences for a negative-rank tensor | 7 pages | Phys.Lett.B634:545-551,2006 | 10.1016/j.physletb.2006.02.027 | USM-TH-178 | hep-th | null | We propose and study the properties of a new potential demanded by the
self-consistency of the duality scheme in electromagnetic-like field theories
of totally anti-symmetric tensors in diverse dimensions. Physical implications
of this new potential is manifest under the presence of scalar condensates in
the Julia-To... | [
{
"created": "Thu, 29 Dec 2005 14:00:07 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gaete",
"Patricio",
""
],
[
"Wotzasek",
"Clovis",
""
]
] | We propose and study the properties of a new potential demanded by the self-consistency of the duality scheme in electromagnetic-like field theories of totally anti-symmetric tensors in diverse dimensions. Physical implications of this new potential is manifest under the presence of scalar condensates in the Julia-Toul... | 25.972336 | 25.650972 | 24.692465 | 25.355804 | 24.196102 | 24.418962 | 24.538469 | 23.238039 | 23.496929 | 24.151875 | 23.72937 | 23.772179 | 24.668959 | 23.308231 | 23.183365 | 25.562832 | 23.733187 | 24.58741 | 23.969019 | 24.761724 | 24.735651 |
1012.2069 | Evgeny Ivanov | E.A. Ivanov, A.V. Smilga | Dirac Operator on Complex Manifolds and Supersymmetric Quantum Mechanics | 0 + 30 pages, essential revision, new comments and refs. added, typos
corrected, published version | IJMP A 27 (2012) 1230024 (30 pages) | 10.1142/S0217751X12300244 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore a new simple N=2 SQM model describing the motion over complex
manifolds in external gauge fields. The nilpotent supercharge Q of the model
can be interpreted as a (twisted) exterior holomorphic derivative, such that
the model realizes the twisted Dolbeault complex. The sum Q + \bar Q can be
interpreted as ... | [
{
"created": "Thu, 9 Dec 2010 18:29:50 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Oct 2012 15:06:59 GMT",
"version": "v2"
}
] | 2012-10-17 | [
[
"Ivanov",
"E. A.",
""
],
[
"Smilga",
"A. V.",
""
]
] | We explore a new simple N=2 SQM model describing the motion over complex manifolds in external gauge fields. The nilpotent supercharge Q of the model can be interpreted as a (twisted) exterior holomorphic derivative, such that the model realizes the twisted Dolbeault complex. The sum Q + \bar Q can be interpreted as th... | 8.542609 | 7.777528 | 9.139677 | 7.73653 | 7.913656 | 7.598912 | 7.798948 | 7.463484 | 7.855628 | 9.777144 | 7.183235 | 8.019513 | 8.44227 | 7.908694 | 7.431305 | 7.912747 | 7.661205 | 7.769196 | 7.793066 | 8.439952 | 7.524802 |
hep-th/9806210 | Christoph Adam | Christoph Adam | Theta vacuum in different gauges | Latex file, 12 pages | Mod.Phys.Lett. A14 (1999) 185-198 | 10.1142/S0217732399000225 | null | hep-th | null | In some recent papers it is claimed that the physical significance of the
vacuum angle theta for QCD-like theories depends on the chosen gauge condition.
We criticise the arguments that were given in support of this claim, and show
by explicit construction for the case of QED$_2$ that and why they fail,
confirming th... | [
{
"created": "Thu, 25 Jun 1998 18:13:03 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Adam",
"Christoph",
""
]
] | In some recent papers it is claimed that the physical significance of the vacuum angle theta for QCD-like theories depends on the chosen gauge condition. We criticise the arguments that were given in support of this claim, and show by explicit construction for the case of QED$_2$ that and why they fail, confirming ther... | 13.787171 | 13.004981 | 12.307768 | 11.229838 | 13.772409 | 12.405269 | 11.71424 | 12.11204 | 11.671956 | 12.44944 | 12.35009 | 11.400373 | 11.951042 | 11.858811 | 12.502367 | 12.729243 | 11.812035 | 12.044722 | 11.751257 | 11.890474 | 12.02232 |
1205.6257 | Igor Kondrashuk | Pedro Allendes, Bernd Kniehl, Igor Kondrashuk, Eduardo A. Notte
Cuello, Marko Rojas Medar | Solution to Bethe-Salpeter equation via Mellin-Barnes transform | 33 pages, 9 figures, revised version, all the factors and symbols of
integration are written explcitly, symbols of proportionality are removed,
section 2 is extended, section 6.3 is shortened | null | 10.1016/j.nuclphysb.2013.01.012 | DESY-12-087 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Mellin-Barnes transform of triangle ladder-like scalar diagram in
d=4 dimensions. It is shown how the multi-fold MB transform of the momentum
integral corresponding to an arbitrary number of rungs is reduced to the
two-fold MB transform. For this purpose we use Belokurov-Usyukina reduction
method for four... | [
{
"created": "Tue, 29 May 2012 04:11:20 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Oct 2012 12:31:12 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Allendes",
"Pedro",
""
],
[
"Kniehl",
"Bernd",
""
],
[
"Kondrashuk",
"Igor",
""
],
[
"Cuello",
"Eduardo A. Notte",
""
],
[
"Medar",
"Marko Rojas",
""
]
] | We consider Mellin-Barnes transform of triangle ladder-like scalar diagram in d=4 dimensions. It is shown how the multi-fold MB transform of the momentum integral corresponding to an arbitrary number of rungs is reduced to the two-fold MB transform. For this purpose we use Belokurov-Usyukina reduction method for four-d... | 11.103821 | 11.493115 | 11.737917 | 10.840213 | 11.696304 | 11.32365 | 11.883695 | 10.991937 | 10.954871 | 13.04915 | 11.244174 | 11.191597 | 10.687508 | 10.503675 | 10.680326 | 10.840639 | 10.753451 | 10.919814 | 10.733531 | 10.661592 | 10.523529 |
1504.05922 | Pramod Padmanabhan Mr. | Miguel Jorge Bernabe Ferreira, Pramod Padmanabhan and Paulo
Teotonio-Sobrinho | Toric code-like models from the parameter space of $3D$ lattice gauge
theories | 12 pages, 7 figures. This paper is an extension of the one
http://arxiv.org/abs/1310.8483. Slightly modified to make it more
self-contained | null | null | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A state sum construction on closed manifolds \'{a} la Kuperberg can be used
to construct the partition functions of $3D$ lattice gauge theories based on
involutory Hopf algebras, $\mathcal{A}$, of which the group algebras,
$\mathbb{C}G$, are a particular case. Transfer matrices can be obtained by
carrying out this co... | [
{
"created": "Wed, 22 Apr 2015 18:53:11 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Dec 2015 22:24:58 GMT",
"version": "v2"
}
] | 2015-12-14 | [
[
"Ferreira",
"Miguel Jorge Bernabe",
""
],
[
"Padmanabhan",
"Pramod",
""
],
[
"Teotonio-Sobrinho",
"Paulo",
""
]
] | A state sum construction on closed manifolds \'{a} la Kuperberg can be used to construct the partition functions of $3D$ lattice gauge theories based on involutory Hopf algebras, $\mathcal{A}$, of which the group algebras, $\mathbb{C}G$, are a particular case. Transfer matrices can be obtained by carrying out this cons... | 9.202297 | 10.674658 | 10.348436 | 9.89981 | 10.01929 | 9.794107 | 10.080082 | 10.124663 | 9.46707 | 11.917209 | 9.475554 | 9.211139 | 9.616565 | 9.117395 | 9.055573 | 9.325071 | 9.275515 | 9.306946 | 9.314381 | 9.518795 | 9.025704 |
hep-th/0102189 | Richard Wittman | Richard S. Wittman | Pedagogical Reflections on Color Confinement in Chromostatics | 8 pages | null | null | null | hep-th | null | Abelian and nonabelian gauge invariant states are directly compared to
revisit how the unconfined abelian theory is expressed. It is argued that the
Yang-Mills equations have no obvious physical content apart from their relation
to underlying physical states. The main observation is that the physical states
of electr... | [
{
"created": "Tue, 27 Feb 2001 09:20:04 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Wittman",
"Richard S.",
""
]
] | Abelian and nonabelian gauge invariant states are directly compared to revisit how the unconfined abelian theory is expressed. It is argued that the Yang-Mills equations have no obvious physical content apart from their relation to underlying physical states. The main observation is that the physical states of electros... | 18.593954 | 20.304293 | 17.384449 | 18.766039 | 20.108732 | 19.476725 | 20.513445 | 20.212225 | 18.32613 | 20.433704 | 17.536007 | 16.798952 | 17.312904 | 16.758261 | 17.005972 | 17.498926 | 17.071913 | 16.462091 | 17.262524 | 16.316673 | 17.492767 |
hep-th/9307098 | R. Sollacher | R. Sollacher | Collective Coordinate Quantization: Relativistic and Gauge Symmetric
Aspects | LaTex, 27 pages, GSI-93-56 | null | null | null | hep-th hep-ph | null | The introduction and quantization of a center-of-mass coordinate is
demonstrated for the one-soliton sector of nonlinear field theories in (1+1)
dimensions. The present approach strongly emphazises the gauge and
BRST-symmetry aspects of collective coordinate quantization. A gauge is
presented which is independent of ... | [
{
"created": "Thu, 15 Jul 1993 08:59:52 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Sollacher",
"R.",
""
]
] | The introduction and quantization of a center-of-mass coordinate is demonstrated for the one-soliton sector of nonlinear field theories in (1+1) dimensions. The present approach strongly emphazises the gauge and BRST-symmetry aspects of collective coordinate quantization. A gauge is presented which is independent of an... | 11.317248 | 11.6758 | 10.974949 | 10.794567 | 11.449347 | 11.246901 | 10.90099 | 10.612987 | 11.17078 | 10.857041 | 11.028154 | 10.946915 | 10.522421 | 10.620953 | 10.783405 | 11.002823 | 10.591638 | 10.585613 | 10.607188 | 10.382192 | 10.721461 |
hep-th/9603187 | null | Dmitri Sorokin and Francesco Toppan | Hamiltonian Reduction of Supersymmetric WZNW Models on Bosonic Groups
and Superstrings | LaTeX file, 32 pages, final version to appear in Nucl. Phys. B | Nucl.Phys. B480 (1996) 457-484 | 10.1016/S0550-3213(96)00499-3 | DFPD 96/TH/15 | hep-th | null | It is shown that an alternative supersymmetric version of the Liouville
equation extracted from D=3 Green-Schwarz superstring equations naturally
arises as a super-Toda model obtained from a properly constrained
supersymmetric WZNW theory based on the $sl(2, R)$ algebra. Hamiltonian
reduction is performed by imposing... | [
{
"created": "Thu, 28 Mar 1996 14:49:57 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Apr 1996 10:46:56 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Jul 1996 13:44:28 GMT",
"version": "v3"
},
{
"created": "Fri, 13 Sep 1996 11:21:30 GMT",
"version": "v4"
}
] | 2016-09-06 | [
[
"Sorokin",
"Dmitri",
""
],
[
"Toppan",
"Francesco",
""
]
] | It is shown that an alternative supersymmetric version of the Liouville equation extracted from D=3 Green-Schwarz superstring equations naturally arises as a super-Toda model obtained from a properly constrained supersymmetric WZNW theory based on the $sl(2, R)$ algebra. Hamiltonian reduction is performed by imposing a... | 11.17625 | 12.941123 | 13.064151 | 10.763147 | 11.626349 | 12.533588 | 11.733423 | 11.624509 | 10.709724 | 14.007357 | 11.166045 | 11.074976 | 11.980247 | 10.886103 | 10.924823 | 11.305506 | 11.434161 | 11.168192 | 10.71046 | 11.604209 | 10.988533 |
2308.05093 | Saurabh Gupta | Ansha S Nair, Saurabh Gupta | On the Quantization of FLPR Model | 17 pages, No figures, Dedicated to the memory of Prof. G. Rajasekaran
(Rajaji), who was an excellent teacher, a great leader and an inspiring
mentor | Mod. Phys. Lett. A 39 (2024) 02, 2350186 | 10.1142/S0217732323501869 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We quantize the Friedberg-Lee-Pang-Ren (FLPR) model, using an admissible
gauge condition, within the framework of modified Faddeev-Jackiw formalism.
Further, we deduce the gauge symmetries and establish off-shell nilpotent and
absolutely anti-commuting (anti-)BRST symmetries. We also show that the
physical states of ... | [
{
"created": "Wed, 9 Aug 2023 17:44:47 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Feb 2024 09:22:22 GMT",
"version": "v2"
}
] | 2024-02-29 | [
[
"Nair",
"Ansha S",
""
],
[
"Gupta",
"Saurabh",
""
]
] | We quantize the Friedberg-Lee-Pang-Ren (FLPR) model, using an admissible gauge condition, within the framework of modified Faddeev-Jackiw formalism. Further, we deduce the gauge symmetries and establish off-shell nilpotent and absolutely anti-commuting (anti-)BRST symmetries. We also show that the physical states of th... | 9.166032 | 5.978919 | 8.69765 | 6.726118 | 6.654811 | 5.853194 | 6.163218 | 5.423311 | 5.810351 | 7.859971 | 6.687306 | 7.237962 | 7.763063 | 8.030718 | 7.239655 | 7.581072 | 7.366709 | 7.430664 | 7.001113 | 8.10345 | 7.529299 |
1610.06078 | Tomas Andrade | Tomas Andrade, Elena Caceres and Cynthia Keeler | Boundary Causality vs Hyperbolicity for Spherical Black Holes in
Gauss-Bonnet | 17 pages, 6 figures | null | 10.1088/1361-6382/aa7101 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the constraints boundary causality places on the allowable
Gauss-Bonnet gravitational couplings in asymptotically AdS spaces, specifically
considering spherical black hole solutions. We additionally consider the
hyperbolicity properties of these solutions, positing that
hyperbolicity-violating solutions ar... | [
{
"created": "Wed, 19 Oct 2016 15:55:41 GMT",
"version": "v1"
}
] | 2017-06-21 | [
[
"Andrade",
"Tomas",
""
],
[
"Caceres",
"Elena",
""
],
[
"Keeler",
"Cynthia",
""
]
] | We explore the constraints boundary causality places on the allowable Gauss-Bonnet gravitational couplings in asymptotically AdS spaces, specifically considering spherical black hole solutions. We additionally consider the hyperbolicity properties of these solutions, positing that hyperbolicity-violating solutions are ... | 7.479628 | 8.641425 | 7.954332 | 7.801351 | 8.054005 | 7.518126 | 7.954952 | 7.678041 | 7.19587 | 8.676454 | 7.537521 | 7.749558 | 7.338028 | 7.426736 | 7.534219 | 7.585176 | 7.639496 | 7.787377 | 7.464834 | 7.677642 | 7.562764 |
hep-th/9907063 | Minoru Hirayama | M. Hirayama (Toyama Univ.), M. Ueno (Toyama Univ.) | Non-Abelian Stokes Theorem for Wilson Loops Associated with General
Gauge Groups | 11 pages, PTPTEX, corrected some typos | Prog.Theor.Phys.103:151-159,2000 | 10.1143/PTP.103.151 | Toyama 102 | hep-th | null | A formula constituting the non-Abelian Stokes theorem for general semi-simple
compact gauge groups is presented. The formula involves a path integral over a
group space and is applicable to Wilson loop variables irrespective of the
topology of loops. Some simple expressions analogous to the 't Hooft tensor of
a magne... | [
{
"created": "Fri, 9 Jul 1999 08:15:56 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Dec 1999 07:52:55 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Hirayama",
"M.",
"",
"Toyama Univ."
],
[
"Ueno",
"M.",
"",
"Toyama Univ."
]
] | A formula constituting the non-Abelian Stokes theorem for general semi-simple compact gauge groups is presented. The formula involves a path integral over a group space and is applicable to Wilson loop variables irrespective of the topology of loops. Some simple expressions analogous to the 't Hooft tensor of a magneti... | 12.401913 | 12.73897 | 13.267035 | 11.599314 | 12.511399 | 12.468157 | 12.547539 | 10.857059 | 11.914481 | 12.767589 | 11.396279 | 11.887923 | 11.866302 | 11.453079 | 11.91853 | 11.389174 | 11.787416 | 11.249156 | 11.902168 | 11.76579 | 11.592573 |
1810.08147 | Dieter L\"ust | Sergio Ferrara, Alex Kehagias, Dieter Lust | Bimetric, Conformal Supergravity and its Superstring Embedding | 33 pages, revised version with corrected typos and references added | null | 10.1007/JHEP05(2019)100 | CERN-TH-2018-222, MPP-2018-249, LMU-ASC 64/18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the connection between Weyl$^2$ supergravity and superstrings and
further discuss holography between 4-dimensional, ${\cal N}=4$ superconformal
Weyl$^2$ supergravity and ${\cal N}=8$, higher spin-four theory on $AdS_5$. The
Weyl$^2$ plus Einstein supergravity theory is a special kind of a bimetric
gravity ... | [
{
"created": "Thu, 18 Oct 2018 16:41:05 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Nov 2018 16:40:16 GMT",
"version": "v2"
}
] | 2019-06-26 | [
[
"Ferrara",
"Sergio",
""
],
[
"Kehagias",
"Alex",
""
],
[
"Lust",
"Dieter",
""
]
] | We discuss the connection between Weyl$^2$ supergravity and superstrings and further discuss holography between 4-dimensional, ${\cal N}=4$ superconformal Weyl$^2$ supergravity and ${\cal N}=8$, higher spin-four theory on $AdS_5$. The Weyl$^2$ plus Einstein supergravity theory is a special kind of a bimetric gravity th... | 7.664576 | 7.741363 | 8.207794 | 7.621793 | 8.020578 | 7.661088 | 7.826856 | 7.51321 | 7.266286 | 8.486411 | 7.449455 | 7.324095 | 7.726118 | 7.428801 | 7.643419 | 7.466111 | 7.497252 | 7.544547 | 7.410803 | 7.675106 | 7.472234 |
hep-th/0703048 | Allan Adams | Allan Adams | Conformal Field Theory and the Reid Conjecture | 4 pages, revtex | null | null | MIT-CTP 3816 | hep-th math.AG | null | We construct special pairs of quantum sigma models on Kahler Calabi-Yau and
non-Kahler Fu-Yau manifolds which flow to the same conformal field theories in
their "small-radius" phases. This smooth description of a novel type of
topology change constitutes strong evidence for Reid's conjecture on the
connectedness of m... | [
{
"created": "Tue, 6 Mar 2007 20:28:06 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Adams",
"Allan",
""
]
] | We construct special pairs of quantum sigma models on Kahler Calabi-Yau and non-Kahler Fu-Yau manifolds which flow to the same conformal field theories in their "small-radius" phases. This smooth description of a novel type of topology change constitutes strong evidence for Reid's conjecture on the connectedness of mod... | 12.999634 | 14.144537 | 19.456758 | 13.175179 | 12.418789 | 12.87776 | 15.442903 | 13.017231 | 13.838786 | 21.011745 | 12.379744 | 13.417895 | 15.267517 | 12.96881 | 13.685711 | 13.092154 | 13.939862 | 12.720667 | 13.441668 | 16.002659 | 11.910881 |
hep-th/0508231 | Shahrokh Parvizi | Shahrokh Parvizi, Alireza Tavanfar | Minimal redefinition of the OSV ensemble | 23 pages, v2: minor changes | J.Math.Phys. 47 (2006) 122304 | 10.1063/1.2393149 | IPM/P-2005/059 | hep-th | null | In the interesting conjecture, Z_{BH} = |Z_{top}|^2, proposed by Ooguri,
Strominger and Vafa (OSV), the black hole ensemble is a mixed ensemble and the
resulting degeneracy of states, as obtained from the ensemble inverse-Laplace
integration, suffers from prefactors which do not respect the electric-magnetic
duality.... | [
{
"created": "Tue, 30 Aug 2005 18:12:07 GMT",
"version": "v1"
},
{
"created": "Sat, 3 Sep 2005 12:02:27 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Parvizi",
"Shahrokh",
""
],
[
"Tavanfar",
"Alireza",
""
]
] | In the interesting conjecture, Z_{BH} = |Z_{top}|^2, proposed by Ooguri, Strominger and Vafa (OSV), the black hole ensemble is a mixed ensemble and the resulting degeneracy of states, as obtained from the ensemble inverse-Laplace integration, suffers from prefactors which do not respect the electric-magnetic duality. O... | 11.514767 | 12.260714 | 13.145417 | 11.310632 | 12.601302 | 12.002249 | 12.021641 | 11.699372 | 11.995072 | 13.307231 | 11.809807 | 11.816538 | 11.746963 | 11.137745 | 11.118388 | 11.24389 | 11.140409 | 11.068614 | 10.898214 | 11.770756 | 11.078093 |
hep-th/0607134 | Daniel S. Freed | Daniel S. Freed | Pions and Generalized Cohomology | 29 pages, minor changes and added Proposition 4.4 | null | null | null | hep-th math.AT | null | The Wess-Zumino-Witten term was first introduced in the low energy
sigma-model which describes pions, the Goldstone bosons for the broken flavor
symmetry in quantum chromodynamics. We introduce a new definition of this term
in arbitrary gravitational backgrounds. It matches several features of the
fundamental gauge t... | [
{
"created": "Wed, 19 Jul 2006 21:16:49 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Jul 2007 16:23:17 GMT",
"version": "v2"
}
] | 2007-07-05 | [
[
"Freed",
"Daniel S.",
""
]
] | The Wess-Zumino-Witten term was first introduced in the low energy sigma-model which describes pions, the Goldstone bosons for the broken flavor symmetry in quantum chromodynamics. We introduce a new definition of this term in arbitrary gravitational backgrounds. It matches several features of the fundamental gauge the... | 9.914277 | 9.674062 | 10.196569 | 9.700311 | 9.911242 | 10.000546 | 9.604277 | 10.260621 | 9.672865 | 11.073295 | 9.665272 | 9.622484 | 9.924416 | 9.786522 | 10.076718 | 9.726173 | 9.725679 | 9.793406 | 9.711222 | 10.275064 | 9.874184 |
hep-th/0104146 | Angelos Fotopoulos | A. Fotopoulos | On $(\alpha')^2$ corrections to the D-brane action for non-geodesic
world-volume embeddings | 34 pages, LaTeX, 4 Postscript figures, expanded introduction and
conclusions, typos corrected, references added, final version to appear in
JHEP09(2001)005 | JHEP 0109:005,2001 | 10.1088/1126-6708/2001/09/005 | CPHT-S021.0401 | hep-th | null | In hep-th/9903210 (curvature)$^2$ terms of the effective D-brane action were
derived to lowest order in the string coupling. Their results are correct up to
ambiguous terms which involve the second fundamental form of the D-brane. We
compute five point string amplitudes on the disk. We compare the subleading
order in... | [
{
"created": "Tue, 17 Apr 2001 17:31:00 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Sep 2001 17:51:39 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Fotopoulos",
"A.",
""
]
] | In hep-th/9903210 (curvature)$^2$ terms of the effective D-brane action were derived to lowest order in the string coupling. Their results are correct up to ambiguous terms which involve the second fundamental form of the D-brane. We compute five point string amplitudes on the disk. We compare the subleading order in $... | 10.002995 | 8.709536 | 10.021575 | 8.622572 | 9.477264 | 8.990785 | 8.890098 | 8.673516 | 8.756389 | 11.698563 | 8.763344 | 8.86807 | 9.387979 | 8.750278 | 8.791786 | 8.723673 | 9.272995 | 9.131951 | 8.942005 | 9.112245 | 8.903935 |
hep-th/0007255 | Chen-Gang Zhou | Chen-Gang Zhou | Noncommutative Scalar Solitons at Finite $\theta$ | Harvmac, 16 pages, 2 figures | null | null | null | hep-th | null | We investigate the behavior of the noncommutative scalar soliton solutions at
finite noncommutative scale $\theta$. A detailed analysis of the equation of
the motion indicates that fewer and fewer soliton solutions exist as $\theta$
is decreased and thus the solitonic sector of the theory exhibits an overall
hierarch... | [
{
"created": "Mon, 31 Jul 2000 20:14:25 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Zhou",
"Chen-Gang",
""
]
] | We investigate the behavior of the noncommutative scalar soliton solutions at finite noncommutative scale $\theta$. A detailed analysis of the equation of the motion indicates that fewer and fewer soliton solutions exist as $\theta$ is decreased and thus the solitonic sector of the theory exhibits an overall hierarchy ... | 7.613471 | 6.565876 | 7.262906 | 6.859463 | 7.14995 | 7.000928 | 7.192266 | 6.900109 | 6.839819 | 7.232658 | 6.6921 | 6.916198 | 7.001632 | 6.849276 | 6.766886 | 7.004985 | 7.038829 | 6.894804 | 6.767826 | 6.969105 | 6.72163 |
1607.08593 | Munir Al-Hashimi | M.H. Al-Hashimi, M. Salman, and A.M. Shalaby | The General Solution for the Relativistic and Nonrelativistic
Schr\"odinger Equation for the $\delta^{(n)}$-Function Potential in
1-dimension Using Cutoff Regularization, and the Fate of Universality | 36 pages, 7 figures. arXiv admin note: substantial text overlap with
arXiv:1503.00786 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A general method has been developed to solve the Schr\"odinger equation for
an arbitrary derivative of the $\delta$-function potential in 1-d using cutoff
regularization. The work treats both the relativistic and nonrelativistic
cases. A distinction in the treatment has been made between the case when the
derivative ... | [
{
"created": "Thu, 28 Jul 2016 19:47:40 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Feb 2019 18:51:28 GMT",
"version": "v2"
}
] | 2019-02-08 | [
[
"Al-Hashimi",
"M. H.",
""
],
[
"Salman",
"M.",
""
],
[
"Shalaby",
"A. M.",
""
]
] | A general method has been developed to solve the Schr\"odinger equation for an arbitrary derivative of the $\delta$-function potential in 1-d using cutoff regularization. The work treats both the relativistic and nonrelativistic cases. A distinction in the treatment has been made between the case when the derivative $n... | 7.649562 | 7.247051 | 7.965737 | 7.208063 | 6.84979 | 6.775596 | 7.0317 | 7.478599 | 7.145148 | 8.449268 | 7.004891 | 7.179688 | 7.33285 | 7.108373 | 7.019748 | 7.20315 | 7.155171 | 7.181158 | 7.116505 | 7.428678 | 7.116925 |
1508.04281 | Daniil Kalinov | D. Kalinov (HSE, Moscow) | On radiation due to homogeneously accelerating sources | 20 pages, no figures | null | 10.1103/PhysRevD.92.084048 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The core of this work is an old and broadly discussed problem of the
electromagnetic radiation in the case of the hyperbolic motion. We prove that
the radiation is non-zero in the lab (Minkowski) frame. Further, we attempt to
understand this subject better by using co-moving non-inertial frames of
reference, investig... | [
{
"created": "Tue, 18 Aug 2015 11:34:02 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Oct 2015 21:14:15 GMT",
"version": "v2"
}
] | 2015-11-04 | [
[
"Kalinov",
"D.",
"",
"HSE, Moscow"
]
] | The core of this work is an old and broadly discussed problem of the electromagnetic radiation in the case of the hyperbolic motion. We prove that the radiation is non-zero in the lab (Minkowski) frame. Further, we attempt to understand this subject better by using co-moving non-inertial frames of reference, investigat... | 17.522396 | 18.154097 | 14.13402 | 14.196478 | 16.394299 | 15.173748 | 18.22349 | 15.841515 | 14.232365 | 16.35363 | 16.210691 | 16.275888 | 15.081713 | 15.249146 | 15.155143 | 15.177286 | 16.155968 | 15.53628 | 15.571612 | 14.848252 | 16.464638 |
1309.0674 | Kofinas Georgios | Georgios Kofinas, Maria Irakleidou | Self-gravitating branes again | 32 pages | Phys. Rev. D 89, 065015 (2014) | 10.1103/PhysRevD.89.065015 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We raise on theoretical grounds the question of the physical relevance of
Israel matching conditions and their generalizations to higher codimensions,
the standard cornerstone of the braneworld and other membrane scenarios. Our
reasoning is twofold: First, the incapability of the conventional matching
conditions to a... | [
{
"created": "Tue, 3 Sep 2013 13:41:36 GMT",
"version": "v1"
}
] | 2014-03-19 | [
[
"Kofinas",
"Georgios",
""
],
[
"Irakleidou",
"Maria",
""
]
] | We raise on theoretical grounds the question of the physical relevance of Israel matching conditions and their generalizations to higher codimensions, the standard cornerstone of the braneworld and other membrane scenarios. Our reasoning is twofold: First, the incapability of the conventional matching conditions to acc... | 14.342093 | 14.079775 | 15.495893 | 13.52207 | 14.629356 | 14.895087 | 14.704828 | 13.641485 | 13.962853 | 15.110632 | 13.82604 | 13.677727 | 13.602551 | 13.416217 | 13.270844 | 13.938015 | 13.922315 | 13.504659 | 13.352338 | 13.599079 | 13.117702 |
1307.7864 | KaiXi Feng | Kaixi Feng, Taotao Qiu, Yun-Song Piao | Curvaton with nonminimal derivative coupling to gravity | 11 pages | null | 10.1016/j.physletb.2014.01.008 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show a curvaton model, in which the curvaton has a nonminimal derivative
coupling to gravity. Thanks to such a coupling, we find that the
scale-invariance of the perturbations can be achieved for arbitrary values of
the equation-of-state of background, provided that it is nearly a constant. We
also discussed about... | [
{
"created": "Tue, 30 Jul 2013 08:14:42 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Jan 2014 07:02:30 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Feng",
"Kaixi",
""
],
[
"Qiu",
"Taotao",
""
],
[
"Piao",
"Yun-Song",
""
]
] | We show a curvaton model, in which the curvaton has a nonminimal derivative coupling to gravity. Thanks to such a coupling, we find that the scale-invariance of the perturbations can be achieved for arbitrary values of the equation-of-state of background, provided that it is nearly a constant. We also discussed about t... | 7.50887 | 7.940153 | 7.074071 | 7.05096 | 7.320267 | 7.003131 | 7.525529 | 7.219995 | 7.616835 | 7.395517 | 7.108641 | 7.780893 | 7.719649 | 7.401542 | 7.522782 | 7.615473 | 7.377676 | 7.428301 | 7.647589 | 7.353072 | 7.363911 |
2301.12870 | Thomas Oosthuyse | Thomas Oosthuyse, David Dudal | Interplay between chiral media and perfect electromagnetic conductor
plates: repulsive vs. attractive Casimir force transitions | 8 pages, 7 figures | SciPost Phys. 15, 213 (2023) | 10.21468/SciPostPhys.15.5.213 | null | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We determine the Casimir energies and forces in a variety of potentially
experimentally viable setups, consisting of parallel plates made of perfect
electromagnetic conductors (PEMCs), which generalize perfect electric
conductors (PECs) and perfect magnetic conductors (PMCs), and Weyl semimetals
(WSMs). Where compari... | [
{
"created": "Mon, 30 Jan 2023 13:24:04 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Feb 2023 09:26:00 GMT",
"version": "v2"
},
{
"created": "Fri, 24 Feb 2023 12:59:17 GMT",
"version": "v3"
},
{
"created": "Wed, 13 Sep 2023 14:53:54 GMT",
"version": "v4"
},
{
"cr... | 2023-11-29 | [
[
"Oosthuyse",
"Thomas",
""
],
[
"Dudal",
"David",
""
]
] | We determine the Casimir energies and forces in a variety of potentially experimentally viable setups, consisting of parallel plates made of perfect electromagnetic conductors (PEMCs), which generalize perfect electric conductors (PECs) and perfect magnetic conductors (PMCs), and Weyl semimetals (WSMs). Where compariso... | 9.271352 | 9.523693 | 9.59756 | 8.558682 | 9.53365 | 9.674664 | 9.155264 | 9.131892 | 9.155591 | 11.635196 | 9.022054 | 9.144553 | 9.36838 | 9.090287 | 9.023388 | 9.127425 | 9.185443 | 8.982894 | 9.271382 | 9.598063 | 8.79004 |
1401.7980 | Martin Schnabl | Matej Kudrna, Miroslav Rapcak, Martin Schnabl | Ising model conformal boundary conditions from open string field theory | 41 pages, 3 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given a consistent choice of conformally invariant boundary conditions in a
two dimensional conformal field theory, one can construct new consistent
boundary conditions by deforming with a relevant boundary operator and flowing
to the infrared, or by a marginal deformation. Open string field theory
provides a very un... | [
{
"created": "Thu, 30 Jan 2014 20:50:13 GMT",
"version": "v1"
}
] | 2014-01-31 | [
[
"Kudrna",
"Matej",
""
],
[
"Rapcak",
"Miroslav",
""
],
[
"Schnabl",
"Martin",
""
]
] | Given a consistent choice of conformally invariant boundary conditions in a two dimensional conformal field theory, one can construct new consistent boundary conditions by deforming with a relevant boundary operator and flowing to the infrared, or by a marginal deformation. Open string field theory provides a very univ... | 12.643841 | 9.858275 | 13.950952 | 11.16365 | 11.203269 | 11.523479 | 11.473223 | 11.106316 | 10.626383 | 14.391234 | 11.182291 | 10.899414 | 12.734631 | 11.454082 | 11.068996 | 11.372755 | 11.216526 | 10.949167 | 11.760683 | 13.09216 | 10.910888 |
1803.00450 | Kimball A. Milton | Kimball Milton and Iver Brevik | Casimir Energies for Isorefractive or Diaphanous Balls | 9 pages, 5 figures, submitted to Symmetry | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is familiar that the Casimir self-energy of a homogeneous dielectric ball
is divergent, although a finite self-energy can be extracted through second
order in the deviation of the permittivity from the vacuum value. The exception
occurs when the speed of light inside the spherical boundary is the same as
that outs... | [
{
"created": "Thu, 1 Mar 2018 15:35:14 GMT",
"version": "v1"
}
] | 2018-03-02 | [
[
"Milton",
"Kimball",
""
],
[
"Brevik",
"Iver",
""
]
] | It is familiar that the Casimir self-energy of a homogeneous dielectric ball is divergent, although a finite self-energy can be extracted through second order in the deviation of the permittivity from the vacuum value. The exception occurs when the speed of light inside the spherical boundary is the same as that outsid... | 9.51403 | 8.901157 | 10.703216 | 8.753988 | 8.975338 | 8.088941 | 8.979452 | 8.81292 | 8.777502 | 11.07604 | 8.366839 | 8.775683 | 9.655176 | 8.990564 | 8.867635 | 8.853233 | 8.783037 | 8.77633 | 8.861808 | 9.331616 | 8.786694 |
0806.1788 | Ivo Sachs | Ivo Sachs, Sergey N. Solodukhin | Quasi-Normal Modes in Topologically Massive Gravity | 13 pages, typos corrected | JHEP 0808:003,2008 | 10.1088/1126-6708/2008/08/003 | LMU-ASC 35/08 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We determine the black hole quasi-normal mode spectrum for tensor
perturbations in topologically massive AdS-gravity. In the special case of
chiral gravity quasi-normal modes are absent despite of the presence of a
horizon. In the process we uncover a simple algebraic structure in the quasi
normal modes spectrum: the... | [
{
"created": "Wed, 11 Jun 2008 04:43:57 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jun 2008 06:16:36 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Sep 2008 11:42:21 GMT",
"version": "v3"
}
] | 2009-12-10 | [
[
"Sachs",
"Ivo",
""
],
[
"Solodukhin",
"Sergey N.",
""
]
] | We determine the black hole quasi-normal mode spectrum for tensor perturbations in topologically massive AdS-gravity. In the special case of chiral gravity quasi-normal modes are absent despite of the presence of a horizon. In the process we uncover a simple algebraic structure in the quasi normal modes spectrum: the t... | 13.747612 | 11.225962 | 14.702417 | 11.986524 | 12.053676 | 12.530441 | 11.359241 | 12.31035 | 11.202373 | 15.333817 | 11.399397 | 12.154362 | 12.397252 | 11.926146 | 12.675422 | 12.50564 | 12.26755 | 11.993274 | 11.927635 | 13.14543 | 12.332803 |
hep-th/9810006 | Gabor Takacs | G. Takacs (INFN Sez. di Bologna), G.M.T. Watts (King's College,
London) | Non-unitarity in quantum affine Toda theory and perturbed conformal
field theory | 29 pp, LaTex2e, 6 eps and 1 ps figures | Nucl.Phys. B547 (1999) 538-568 | 10.1016/S0550-3213(99)00100-5 | DFUB-98-18, KCL-MTH-98-38 | hep-th | null | There has been some debate about the validity of quantum affine Toda field
theory at imaginary coupling, owing to the non-unitarity of the action, and
consequently of its usefulness as a model of perturbed conformal field theory.
Drawing on our recent work, we investigate the two simplest affine Toda
theories for whi... | [
{
"created": "Thu, 1 Oct 1998 14:17:36 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Takacs",
"G.",
"",
"INFN Sez. di Bologna"
],
[
"Watts",
"G. M. T.",
"",
"King's College,\n London"
]
] | There has been some debate about the validity of quantum affine Toda field theory at imaginary coupling, owing to the non-unitarity of the action, and consequently of its usefulness as a model of perturbed conformal field theory. Drawing on our recent work, we investigate the two simplest affine Toda theories for which... | 9.797531 | 10.893398 | 11.865188 | 9.920846 | 11.103638 | 10.609789 | 11.076891 | 10.095603 | 10.016191 | 12.329757 | 10.337615 | 9.908637 | 10.110978 | 9.70883 | 10.004365 | 9.909716 | 9.819329 | 9.840339 | 9.896281 | 10.282769 | 9.873724 |
hep-th/9411041 | Kalmykov M. Yu | L.V.Avdeev, D.I.Kazakov and M.Yu.Kalmykov | The Background-Field Method and Noninvariant Renormalization | 12 pages, LATEX | null | null | JINR E2-94-388 | hep-th | null | We investigate the consistency of the background-field formalism when
applying various regularizations and renormalization schemes. By an example of
a two-dimensional $\sigma$ model it is demonstrated that the background-field
method gives incorrect results when the regularization (and/or renormalization)
is noninvar... | [
{
"created": "Thu, 3 Nov 1994 22:38:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Avdeev",
"L. V.",
""
],
[
"Kazakov",
"D. I.",
""
],
[
"Kalmykov",
"M. Yu.",
""
]
] | We investigate the consistency of the background-field formalism when applying various regularizations and renormalization schemes. By an example of a two-dimensional $\sigma$ model it is demonstrated that the background-field method gives incorrect results when the regularization (and/or renormalization) is noninvaria... | 8.832886 | 5.604114 | 8.559684 | 6.989616 | 8.236746 | 5.761578 | 5.792782 | 6.608156 | 6.770736 | 9.121717 | 7.290366 | 7.464111 | 8.155448 | 7.821544 | 7.956665 | 7.542536 | 7.484501 | 7.693953 | 7.759012 | 7.806325 | 7.531757 |
2307.16801 | Yangrui Hu | Yangrui Hu and Sabrina Pasterski | Detector Operators for Celestial Symmetries | null | null | 10.1007/JHEP12(2023)035 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper presents a systematic cataloging of the generators of celestial
symmetries on phase space. Starting from the celestial OPEs, we first show how
to extract a representation of the general-spin analog of the wedge subalgebra
of $w_{1+\infty}$ on the phase space of massless matter fields of arbitrary
helicity.... | [
{
"created": "Mon, 31 Jul 2023 16:11:03 GMT",
"version": "v1"
}
] | 2023-12-07 | [
[
"Hu",
"Yangrui",
""
],
[
"Pasterski",
"Sabrina",
""
]
] | This paper presents a systematic cataloging of the generators of celestial symmetries on phase space. Starting from the celestial OPEs, we first show how to extract a representation of the general-spin analog of the wedge subalgebra of $w_{1+\infty}$ on the phase space of massless matter fields of arbitrary helicity. T... | 14.465697 | 12.969728 | 15.557036 | 12.74006 | 13.554294 | 13.14208 | 13.519446 | 13.131033 | 12.724384 | 17.82378 | 12.816801 | 13.368784 | 14.398514 | 12.999779 | 13.018727 | 13.006061 | 13.260802 | 12.966412 | 12.998208 | 14.387491 | 13.260409 |
1810.13440 | Onkar Parrikar | Vijay Balasubramanian, David Berenstein, Aitor Lewkowycz, Alexandra
Miller, Onkar Parrikar and Charles Rabideau | Emergent classical spacetime from microstates of an incipient black hole | 47 pages, 9 figures | null | 10.1007/JHEP01(2019)197 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Black holes have an enormous underlying space of microstates, but universal
macroscopic physics characterized by mass, charge and angular momentum as well
as a causally disconnected interior. This leads two related puzzles: (1) How
does the effective factorization of interior and exterior degrees of freedom
emerge in... | [
{
"created": "Wed, 31 Oct 2018 17:54:25 GMT",
"version": "v1"
}
] | 2019-02-20 | [
[
"Balasubramanian",
"Vijay",
""
],
[
"Berenstein",
"David",
""
],
[
"Lewkowycz",
"Aitor",
""
],
[
"Miller",
"Alexandra",
""
],
[
"Parrikar",
"Onkar",
""
],
[
"Rabideau",
"Charles",
""
]
] | Black holes have an enormous underlying space of microstates, but universal macroscopic physics characterized by mass, charge and angular momentum as well as a causally disconnected interior. This leads two related puzzles: (1) How does the effective factorization of interior and exterior degrees of freedom emerge in g... | 9.311832 | 9.129384 | 9.107747 | 8.650867 | 9.377556 | 9.135345 | 9.278359 | 8.566239 | 8.84882 | 10.116128 | 8.872835 | 8.703321 | 8.740558 | 8.465162 | 8.492501 | 9.016611 | 8.514977 | 8.711155 | 8.456498 | 8.665157 | 8.611156 |
hep-th/9705188 | Ori Ganor | Ori J. Ganor, Rajesh Gopakumar and Sanjaye Ramgoolam | Higher Loop Effects in M(atrix) Orbifolds | Discussion of the discrepancy with M(atrix)-theory is clarified. We
emphasize the fact that the main problem is not a numerical one but in the
factors of N. We also made minor corrections to the text, 24pp TeX | Nucl.Phys. B511 (1998) 243-263 | 10.1016/S0550-3213(97)00654-8 | PUPT-1680 | hep-th | null | Scattering of zero branes off the fixed point in $R^8/Z_2$, as described by a
super-quantum mechanics with eight supercharges, displays some novel effects
relevant to Matrix theory in non-compact backgrounds. The leading long distance
behaviour of the moduli space metric receives no correction at one loop in
Matrix t... | [
{
"created": "Fri, 23 May 1997 23:19:24 GMT",
"version": "v1"
},
{
"created": "Mon, 26 May 1997 23:31:35 GMT",
"version": "v2"
},
{
"created": "Sun, 8 Jun 1997 22:12:28 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Ganor",
"Ori J.",
""
],
[
"Gopakumar",
"Rajesh",
""
],
[
"Ramgoolam",
"Sanjaye",
""
]
] | Scattering of zero branes off the fixed point in $R^8/Z_2$, as described by a super-quantum mechanics with eight supercharges, displays some novel effects relevant to Matrix theory in non-compact backgrounds. The leading long distance behaviour of the moduli space metric receives no correction at one loop in Matrix the... | 12.040658 | 10.167991 | 13.8486 | 10.528584 | 10.658499 | 10.601761 | 10.613657 | 10.842159 | 10.193233 | 14.686417 | 10.066354 | 10.033162 | 11.677563 | 10.388532 | 10.162704 | 10.331803 | 10.206312 | 10.393557 | 10.455119 | 11.227587 | 10.413781 |
hep-th/9411127 | Flad | J. Madore, T. Masson, J. Mourad | Linear connections on matrix geometries | 14p, LPTHE-ORSAY 94/96 | Class.Quant.Grav.12:1429-1440,1995 | 10.1088/0264-9381/12/6/009 | null | hep-th | null | A general definition of a linear connection in noncommutative geometry has
been recently proposed. Two examples are given of linear connections in
noncommutative geometries which are based on matrix algebras. They both possess
a unique metric connection.
| [
{
"created": "Thu, 17 Nov 1994 10:14:43 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Dec 1994 14:15:33 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Madore",
"J.",
""
],
[
"Masson",
"T.",
""
],
[
"Mourad",
"J.",
""
]
] | A general definition of a linear connection in noncommutative geometry has been recently proposed. Two examples are given of linear connections in noncommutative geometries which are based on matrix algebras. They both possess a unique metric connection. | 9.837571 | 6.67083 | 8.420393 | 7.085615 | 7.45847 | 7.624589 | 7.394026 | 7.118774 | 7.679784 | 7.705301 | 7.738874 | 7.880773 | 8.507753 | 7.78423 | 7.635732 | 7.724005 | 7.814488 | 7.834715 | 8.302355 | 8.463324 | 8.080505 |
1011.3481 | Andrei Mironov | A.Mironov, A.Morozov and Sh.Shakirov | Brezin-Gross-Witten model as "pure gauge" limit of Selberg integrals | 21 pages | JHEP 1103:102,2011 | 10.1007/JHEP03(2011)102 | FIAN/TD-08/10; ITEP/TH-39/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The AGT relation identifies the Nekrasov functions for various N=2 SUSY gauge
theories with the 2d conformal blocks, which possess explicit Dotsenko-Fateev
matrix model (beta-ensemble) representations the latter being polylinear
combinations of Selberg integrals. The "pure gauge" limit of these matrix
models is, howe... | [
{
"created": "Mon, 15 Nov 2010 19:44:02 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Dec 2010 19:36:25 GMT",
"version": "v2"
}
] | 2011-03-30 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
],
[
"Shakirov",
"Sh.",
""
]
] | The AGT relation identifies the Nekrasov functions for various N=2 SUSY gauge theories with the 2d conformal blocks, which possess explicit Dotsenko-Fateev matrix model (beta-ensemble) representations the latter being polylinear combinations of Selberg integrals. The "pure gauge" limit of these matrix models is, howeve... | 11.894393 | 11.20574 | 12.197224 | 10.224041 | 11.246083 | 10.549109 | 10.931925 | 10.462887 | 10.102894 | 14.728551 | 10.887561 | 10.638209 | 11.232179 | 10.155264 | 10.549557 | 10.823187 | 10.040532 | 10.517259 | 10.436831 | 11.13333 | 10.225822 |
hep-th/9412244 | Theordpt | A. A. Deriglazov | Notes on Lagrangean and Hamiltonian Symmetries | 7 pages, LaTeX | null | null | null | hep-th | null | The Hamiltonization of local symmetries of the form $\delta q^A =
\ea{R_a}^A(q,\dot q)$ or $\delta q^A = \dot\ea{R_a}^A (q,\dot q)$ for arbitrary
Lagrangean model $L(q^A,\dot q^A)$ is considered. We show as the initial
symmetries are transformed in the transition from $L$ to first order action,
and then to the Hamilt... | [
{
"created": "Sun, 1 Jan 1995 15:13:09 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Deriglazov",
"A. A.",
""
]
] | The Hamiltonization of local symmetries of the form $\delta q^A = \ea{R_a}^A(q,\dot q)$ or $\delta q^A = \dot\ea{R_a}^A (q,\dot q)$ for arbitrary Lagrangean model $L(q^A,\dot q^A)$ is considered. We show as the initial symmetries are transformed in the transition from $L$ to first order action, and then to the Hamilton... | 6.68097 | 6.369241 | 7.541255 | 6.960567 | 6.849398 | 6.093639 | 6.575821 | 6.485564 | 6.348792 | 7.966822 | 6.487842 | 6.301219 | 6.363518 | 6.119596 | 6.108911 | 6.112351 | 6.400978 | 6.103135 | 6.323454 | 6.534537 | 6.269569 |
hep-th/0403202 | Saurya Das | Saurya Das | Black Hole Thermodynamics: Entropy, Information and Beyond | Plenary talk given at the Fifth International Conference on
Gravitation and Cosmology, Cochin, 7 January 2004. 13 pages, Revtex | Pramana63:797-816,2004 | 10.1007/BF02705201 | null | hep-th gr-qc | null | We review some recent advances in black hole thermodynamics, including
statistical mechanical origins of black hole entropy and its leading order
corrections, from the viewpoints of various quantum gravity theories. We then
examine the information loss problem and some possible approaches to its
resolution. Finally, ... | [
{
"created": "Sat, 20 Mar 2004 22:01:36 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Das",
"Saurya",
""
]
] | We review some recent advances in black hole thermodynamics, including statistical mechanical origins of black hole entropy and its leading order corrections, from the viewpoints of various quantum gravity theories. We then examine the information loss problem and some possible approaches to its resolution. Finally, we... | 10.28049 | 9.038536 | 8.81475 | 9.294514 | 9.391003 | 9.588236 | 9.66818 | 8.364985 | 9.261037 | 8.793027 | 9.223504 | 9.716326 | 9.016313 | 8.98598 | 9.640531 | 9.581044 | 9.879579 | 9.083345 | 9.553665 | 9.047693 | 9.369456 |
1507.00354 | Netta Engelhardt | Netta Engelhardt and Sebastian Fischetti | Covariant Constraints on Hole-ography | 26+4 pages, 16 figures; v2: references added, typos fixed | Class. Quantum Grav. 32 (2015) 195021 | 10.1088/0264-9381/32/19/195021 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Hole-ography is a prescription relating the areas of surfaces in an AdS bulk
to the differential entropy of a family of intervals in the dual CFT. In (2+1)
bulk dimensions, or in higher dimensions when the bulk features a sufficient
degree of symmetry, we prove that there are surfaces in the bulk that cannot be
compl... | [
{
"created": "Wed, 1 Jul 2015 20:03:49 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jul 2015 19:06:12 GMT",
"version": "v2"
}
] | 2015-09-21 | [
[
"Engelhardt",
"Netta",
""
],
[
"Fischetti",
"Sebastian",
""
]
] | Hole-ography is a prescription relating the areas of surfaces in an AdS bulk to the differential entropy of a family of intervals in the dual CFT. In (2+1) bulk dimensions, or in higher dimensions when the bulk features a sufficient degree of symmetry, we prove that there are surfaces in the bulk that cannot be complet... | 15.759291 | 14.287271 | 15.824702 | 13.101088 | 12.892403 | 12.809947 | 12.167443 | 12.465222 | 12.39918 | 14.579327 | 12.477583 | 11.881269 | 12.960183 | 12.180017 | 12.539115 | 12.096122 | 12.911681 | 12.217282 | 12.594667 | 12.817905 | 12.288691 |
1109.5182 | Pascal Vaudrevange | Koushik Dutta, Pascal M. Vaudrevange, Alexander Westphal | The Overshoot Problem in Inflation after Tunneling | 14 pages, 4 figures | JCAP 1201 (2012) 026 | 10.1088/1475-7516/2012/01/026 | DESY 11-160 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show the absence of the usual parametrically large overshoot problem of
small-field inflation if initiated by a Coleman-De Luccia (CDL) tunneling
transition from an earlier vacuum in the limit of small inflationary scale
compared to the tunneling scale. For low-power monomial exit potentials
$V(\phi)\sim\phi^n, n<... | [
{
"created": "Fri, 23 Sep 2011 20:00:09 GMT",
"version": "v1"
}
] | 2015-07-24 | [
[
"Dutta",
"Koushik",
""
],
[
"Vaudrevange",
"Pascal M.",
""
],
[
"Westphal",
"Alexander",
""
]
] | We show the absence of the usual parametrically large overshoot problem of small-field inflation if initiated by a Coleman-De Luccia (CDL) tunneling transition from an earlier vacuum in the limit of small inflationary scale compared to the tunneling scale. For low-power monomial exit potentials $V(\phi)\sim\phi^n, n<4$... | 12.690125 | 13.316858 | 12.247602 | 11.060086 | 12.921776 | 12.448769 | 13.542099 | 13.346263 | 11.59704 | 13.615758 | 11.597239 | 11.844612 | 11.483474 | 11.400026 | 11.609055 | 11.424501 | 11.526284 | 11.716561 | 11.257795 | 12.091211 | 11.508938 |
hep-th/9710194 | D. V. Antonov | D.V.Antonov (Humboldt University, Berlin and ITEP, Moscow) | 't Hooft Loop Average in the Vicinity of the Londons' Limit and the
Quartic Cumulant of the Field Strength Tensors | 5 pages, LaTeX, references are added | null | null | null | hep-th | null | The next-to-leading term in the weight factor of the string representation of
the 't Hooft loop average defined on the string world-sheet is found in the
Abelian Higgs Model near the Londons' limit. This term emerges due to the
finiteness of the coupling constant and, in contrast to the Londons' limit,
where only the... | [
{
"created": "Sun, 26 Oct 1997 19:17:39 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Nov 1997 19:33:56 GMT",
"version": "v2"
},
{
"created": "Fri, 28 Nov 1997 18:00:51 GMT",
"version": "v3"
},
{
"created": "Wed, 17 Dec 1997 11:34:04 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Antonov",
"D. V.",
"",
"Humboldt University, Berlin and ITEP, Moscow"
]
] | The next-to-leading term in the weight factor of the string representation of the 't Hooft loop average defined on the string world-sheet is found in the Abelian Higgs Model near the Londons' limit. This term emerges due to the finiteness of the coupling constant and, in contrast to the Londons' limit, where only the b... | 11.09636 | 10.06901 | 10.600242 | 9.458732 | 10.511348 | 11.402845 | 10.350953 | 11.329983 | 9.719347 | 11.971667 | 10.668101 | 10.50423 | 9.671613 | 9.85288 | 10.621226 | 10.417043 | 10.442971 | 10.31742 | 10.466292 | 9.801991 | 10.772525 |
1012.2906 | Stephen D. H. Hsu | Stephen D.H. Hsu | Physical consequences of the QED theta angle | 4 pages, latex, 1 figure | null | null | null | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a simple gedanken experiment which illustrates the physical
effects of the QED theta angle, a fundamental parameter of Nature that has yet
to be measured. The effects are manifest in quantum phases analogous to those
in the Aharonov-Bohm effect, although they are not intrinsically topological.
We also der... | [
{
"created": "Tue, 14 Dec 2010 00:13:29 GMT",
"version": "v1"
}
] | 2010-12-15 | [
[
"Hsu",
"Stephen D. H.",
""
]
] | We describe a simple gedanken experiment which illustrates the physical effects of the QED theta angle, a fundamental parameter of Nature that has yet to be measured. The effects are manifest in quantum phases analogous to those in the Aharonov-Bohm effect, although they are not intrinsically topological. We also deriv... | 9.149575 | 8.99805 | 7.852939 | 7.368663 | 7.362939 | 8.387922 | 7.633486 | 8.494034 | 8.081499 | 9.178437 | 9.046792 | 8.79841 | 8.234264 | 8.215652 | 8.033077 | 8.355165 | 8.464785 | 8.470187 | 8.262442 | 8.279199 | 8.597304 |
hep-th/9311162 | Mark de Wild Propitius | F.A. Bais and M. de Wild Propitius | Quantumgroups in the Higgs Phase | 19 pages in Latex, ITFA-93-30 | Theor.Math.Phys. 98 (1994) 357-367; Teor.Mat.Fiz. 98 (1994)
509-523 | 10.1007/BF01102213 | null | hep-th | null | In the Higgs phase we may be left with a residual finite symmetry group H of
the condensate. The topological interactions between the magnetic- and electric
excitations in these so-called discrete H gauge theories are completely
described by the Hopf algebra or quantumgroup D(H). In 2+1 dimensional space
time we may ... | [
{
"created": "Sun, 28 Nov 1993 17:45:41 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Bais",
"F. A.",
""
],
[
"Propitius",
"M. de Wild",
""
]
] | In the Higgs phase we may be left with a residual finite symmetry group H of the condensate. The topological interactions between the magnetic- and electric excitations in these so-called discrete H gauge theories are completely described by the Hopf algebra or quantumgroup D(H). In 2+1 dimensional space time we may ad... | 8.674456 | 8.257281 | 10.496174 | 8.484139 | 8.952518 | 8.422618 | 8.468156 | 8.388457 | 8.499117 | 10.886188 | 7.679842 | 7.950858 | 8.751912 | 8.087583 | 8.094952 | 7.983834 | 8.138351 | 8.127863 | 8.165451 | 8.752819 | 7.918141 |
0912.2352 | Vasilis Niarchos | Roberto Emparan, Troels Harmark, Vasilis Niarchos and Niels A. Obers | New Horizons for Black Holes and Branes | 54 pages, 7 figures; v2 added references, added comments in the
subsection discussing the physical properties of helical black rings; v3
added references, fixed minor typos | JHEP 1004:046,2010 | 10.1007/JHEP04(2010)046 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate a systematic scan of the landscape of black holes in any
spacetime dimension using the recently proposed blackfold effective worldvolume
theory. We focus primarily on asymptotically flat stationary vacuum solutions,
where we uncover large classes of new black holes. These include helical black
strings and... | [
{
"created": "Mon, 14 Dec 2009 15:15:36 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Dec 2009 18:28:02 GMT",
"version": "v2"
},
{
"created": "Sat, 3 Apr 2010 12:48:52 GMT",
"version": "v3"
}
] | 2015-03-13 | [
[
"Emparan",
"Roberto",
""
],
[
"Harmark",
"Troels",
""
],
[
"Niarchos",
"Vasilis",
""
],
[
"Obers",
"Niels A.",
""
]
] | We initiate a systematic scan of the landscape of black holes in any spacetime dimension using the recently proposed blackfold effective worldvolume theory. We focus primarily on asymptotically flat stationary vacuum solutions, where we uncover large classes of new black holes. These include helical black strings and b... | 12.405864 | 14.585109 | 14.793504 | 13.348298 | 14.107944 | 14.333519 | 14.228331 | 13.920503 | 13.369234 | 15.491178 | 12.881659 | 13.16388 | 12.439141 | 12.618324 | 12.666503 | 12.974676 | 12.867988 | 12.09165 | 12.877965 | 12.66387 | 12.701526 |
2010.10500 | Herbert Hamber | Herbert W. Hamber and Lu Heng Sunny Yu | Dyson's Equations for Quantum Gravity in the Hartree-Fock Approximation | 71 pages, 21 figures. More typos fixed, references added | Conforms to published version in Symmetry Jan 2021 | 10.3390/sym1010000 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Unlike scalar and gauge field theories in four dimensions, gravity is not
perturbatively renormalizable and as a result perturbation theory is badly
divergent. Often the method of choice for investigating nonperturbative effects
has been the lattice formulation, and in the case of gravity the Regge-Wheeler
lattice pa... | [
{
"created": "Tue, 20 Oct 2020 17:54:00 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Nov 2020 21:06:56 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Jan 2021 19:01:47 GMT",
"version": "v3"
}
] | 2021-01-12 | [
[
"Hamber",
"Herbert W.",
""
],
[
"Yu",
"Lu Heng Sunny",
""
]
] | Unlike scalar and gauge field theories in four dimensions, gravity is not perturbatively renormalizable and as a result perturbation theory is badly divergent. Often the method of choice for investigating nonperturbative effects has been the lattice formulation, and in the case of gravity the Regge-Wheeler lattice path... | 9.377124 | 10.075627 | 10.324524 | 9.570362 | 10.222205 | 10.26945 | 10.160633 | 10.091595 | 9.61856 | 9.630956 | 9.926103 | 9.28228 | 9.504379 | 9.320652 | 9.409488 | 9.242112 | 9.245497 | 9.25417 | 9.333169 | 9.405051 | 9.176457 |
0904.0559 | Frank Ferrari | Frank Ferrari and Vincent Wens (U. Libre de Bruxelles and Intl. Solvay
Inst.) | Flavors in the microscopic approach to N=1 gauge theories | 20 pages, 1 figure; v2: typos corrected, refs added | JHEP 0905:124,2009 | 10.1088/1126-6708/2009/05/124 | LPTENS-09/06 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note, we solve an extended version of the N=1 super Yang-Mills theory
with gauge group U(N), an adjoint chiral multiplet and Nf flavors of quarks, by
using the N=1 microscopic formalism based on Nekrasov's sums over colored
partitions. Our main new result is the computation of the general mesonic
operators. W... | [
{
"created": "Fri, 3 Apr 2009 12:11:46 GMT",
"version": "v1"
},
{
"created": "Wed, 27 May 2009 14:43:20 GMT",
"version": "v2"
}
] | 2010-12-17 | [
[
"Ferrari",
"Frank",
"",
"U. Libre de Bruxelles and Intl. Solvay\n Inst."
],
[
"Wens",
"Vincent",
"",
"U. Libre de Bruxelles and Intl. Solvay\n Inst."
]
] | In this note, we solve an extended version of the N=1 super Yang-Mills theory with gauge group U(N), an adjoint chiral multiplet and Nf flavors of quarks, by using the N=1 microscopic formalism based on Nekrasov's sums over colored partitions. Our main new result is the computation of the general mesonic operators. We ... | 11.473923 | 9.255892 | 12.947647 | 9.032664 | 9.827835 | 9.355086 | 9.504755 | 9.589869 | 8.77319 | 13.044512 | 8.917966 | 10.67606 | 11.039821 | 10.423603 | 10.505432 | 10.764654 | 10.432883 | 10.264435 | 10.746585 | 11.187763 | 10.058794 |
hep-th/9209063 | null | M. Temple-Raston and D. Alexander | Differential cross-sections and escape plots for low energy $SU(2)$ BPS
magnetic monopole dynamics | 21 pages, TeX (3 figs., 1 Table, and 2 colour plates available upon
request), Con-92-3 | Nucl.Phys. B397 (1993) 195-213 | 10.1016/0550-3213(93)90341-L | null | hep-th | null | We compute the low-energy classical differential scattering cross-section for
BPS $SU(2)$ magnetic monopoles using the geodesic approximation to the actual
dynamics and 16K parallel processors on a CM2. Numerical experiments suggest
that the quantum BPS magnetic monopole differential cross-section is
well-approximate... | [
{
"created": "Thu, 17 Sep 1992 17:17:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Temple-Raston",
"M.",
""
],
[
"Alexander",
"D.",
""
]
] | We compute the low-energy classical differential scattering cross-section for BPS $SU(2)$ magnetic monopoles using the geodesic approximation to the actual dynamics and 16K parallel processors on a CM2. Numerical experiments suggest that the quantum BPS magnetic monopole differential cross-section is well-approximated ... | 12.481792 | 13.903242 | 13.570502 | 12.209155 | 12.232438 | 13.147032 | 13.187493 | 12.861724 | 12.723527 | 14.456427 | 12.30961 | 12.152093 | 12.388557 | 12.02447 | 12.121548 | 11.791125 | 11.741004 | 12.06894 | 12.253326 | 12.52073 | 11.799604 |
hep-th/9509034 | Jouko Mickelsson | E. Langmann and J. Mickelsson | Scattering matrix in external field problems | AmsTex file (uses amstex.tex and amsppt.sty) 22 ouput pages | J.Math.Phys. 37 (1996) 3933-3953 | 10.1063/1.531609 | null | hep-th | null | We discuss several aspects of second quantized scattering operators $\hat S$
for fermions in external time dependent fields. We derive our results on a
general, abstract level having in mind as a main application potentials of the
Yang--Mills type and in various dimensions. We present a new and powerful
method for pr... | [
{
"created": "Thu, 7 Sep 1995 14:58:21 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Langmann",
"E.",
""
],
[
"Mickelsson",
"J.",
""
]
] | We discuss several aspects of second quantized scattering operators $\hat S$ for fermions in external time dependent fields. We derive our results on a general, abstract level having in mind as a main application potentials of the Yang--Mills type and in various dimensions. We present a new and powerful method for prov... | 14.742442 | 14.307073 | 15.25874 | 13.856565 | 14.991127 | 14.969879 | 15.197705 | 14.464414 | 14.785936 | 15.971797 | 14.099397 | 14.440311 | 14.318515 | 14.039155 | 14.435877 | 14.318224 | 14.49743 | 13.790081 | 14.297176 | 14.973434 | 14.317282 |
hep-th/9205044 | Kuramoto | T. Kuramoto | Quantum Hamiltonian Reduction of Super Kac-Moody Algebra II | 16 pages | Nucl.Phys. B411 (1994) 821-838 | 10.1016/0550-3213(94)90472-3 | YNUE-PH-92-01 | hep-th | null | The quantum Hamiltonian reduction on the OSp(1,2) super Kac-Moody algebra is
described in the BRST formalism. Using a free field representation of the KM
currents, the super Kac-Moody algebra is shown to be reduced to a
superconformal one via the Hamiltonian reduction. This reduction is manifestly
supersymmetric beca... | [
{
"created": "Fri, 15 May 1992 06:18:42 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Kuramoto",
"T.",
""
]
] | The quantum Hamiltonian reduction on the OSp(1,2) super Kac-Moody algebra is described in the BRST formalism. Using a free field representation of the KM currents, the super Kac-Moody algebra is shown to be reduced to a superconformal one via the Hamiltonian reduction. This reduction is manifestly supersymmetric becaus... | 9.635818 | 9.348589 | 11.501386 | 8.054808 | 8.082339 | 8.764833 | 8.91003 | 7.674754 | 7.871468 | 12.814132 | 8.181997 | 8.676147 | 9.570521 | 8.627914 | 8.148326 | 8.463998 | 8.006734 | 8.615427 | 8.254101 | 9.539349 | 8.056185 |
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