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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0905.0522 | Jun-Bao Wu | Bin Chen, Jun-Bao Wu | Tree-level Split Helicity Amplitudes in Ambitwistor Space | 20 pages, 16 figures; minor changes; clarifications added, 22 pages,
16 figures | Phys.Rev.D80:125031,2009 | 10.1103/PhysRevD.80.125031 | KIAS-P09018 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study all tree-level split helicity gluon amplitudes by using the recently
proposed BCFW recursion relation and Hodges diagrams in ambitwistor space. We
pick out the contributing diagrams and find that all of them can be divided
into triangles in a suitable way. We give the explicit expressions for all of
these am... | [
{
"created": "Tue, 5 May 2009 03:43:06 GMT",
"version": "v1"
},
{
"created": "Tue, 12 May 2009 09:15:45 GMT",
"version": "v2"
},
{
"created": "Thu, 30 Jul 2009 05:27:20 GMT",
"version": "v3"
}
] | 2010-01-07 | [
[
"Chen",
"Bin",
""
],
[
"Wu",
"Jun-Bao",
""
]
] | We study all tree-level split helicity gluon amplitudes by using the recently proposed BCFW recursion relation and Hodges diagrams in ambitwistor space. We pick out the contributing diagrams and find that all of them can be divided into triangles in a suitable way. We give the explicit expressions for all of these ampl... | 13.526242 | 10.486633 | 14.282084 | 10.819595 | 10.845859 | 11.202471 | 9.691189 | 9.841158 | 10.756338 | 15.953635 | 10.389203 | 10.021448 | 12.357002 | 11.584022 | 10.130176 | 10.865091 | 10.329788 | 10.135256 | 10.955538 | 12.40287 | 10.835461 |
hep-th/9404145 | Valeri Dvoeglazov | Valeri V. Dvoeglazov | The Dirac-Dowker Oscillator | LaTeX file, 4pp. Preprint EFUAZ 94-03 | Nuovo Cim.A107:1785-1788,1994 | 10.1007/BF02780711 | null | hep-th | null | The oscillator-like interaction is introduced in the equation for the
particle of arbitrary spin, given by Dirac and re-written to a matrix form by
Dowker.
| [
{
"created": "Sat, 23 Apr 1994 01:49:51 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Dvoeglazov",
"Valeri V.",
""
]
] | The oscillator-like interaction is introduced in the equation for the particle of arbitrary spin, given by Dirac and re-written to a matrix form by Dowker. | 51.60939 | 40.03307 | 41.636051 | 37.205204 | 34.977428 | 39.905888 | 48.187145 | 35.108158 | 36.458076 | 35.464687 | 38.016163 | 39.478725 | 37.856789 | 37.609158 | 37.859695 | 41.179039 | 37.248642 | 35.5793 | 33.64291 | 37.504436 | 36.194908 |
2112.06967 | Arpan Bhattacharyya | Aranya Bhattacharya, Arpan Bhattacharyya, Pratik Nandy, Ayan K. Patra | Bath deformations, islands and holographic complexity | 27 pages, 7 figures, minor typo corrected and references updated | Phys. Rev. D 105, 066019 (2022) | 10.1103/PhysRevD.105.066019 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Considering a doubly holographic model, we study the evolution of holographic
subregion complexity corresponding to deformations of bath state by a relevant
scalar operator, which corresponds to a renormalization group flow from the
AdS-Schwarzschild to the Kasner universe in the bulk. The subregion complexity
shows ... | [
{
"created": "Mon, 13 Dec 2021 19:09:35 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Dec 2021 06:59:21 GMT",
"version": "v2"
}
] | 2022-04-08 | [
[
"Bhattacharya",
"Aranya",
""
],
[
"Bhattacharyya",
"Arpan",
""
],
[
"Nandy",
"Pratik",
""
],
[
"Patra",
"Ayan K.",
""
]
] | Considering a doubly holographic model, we study the evolution of holographic subregion complexity corresponding to deformations of bath state by a relevant scalar operator, which corresponds to a renormalization group flow from the AdS-Schwarzschild to the Kasner universe in the bulk. The subregion complexity shows a ... | 11.38956 | 8.433786 | 11.64457 | 8.652154 | 9.402596 | 9.442316 | 8.517796 | 8.869871 | 9.224483 | 13.575807 | 8.646052 | 10.197574 | 11.102491 | 10.050467 | 10.048684 | 9.684181 | 9.681415 | 10.230127 | 9.836057 | 11.417408 | 9.770287 |
hep-th/0110251 | Nikolai Sushilov | S. I. Kruglov | Dirac-K\"Ahler Equation | 42 pages, LaTeX. Corrections in Eqs. (29), (88), (99). Extended
version of hep-th/0110060 | Int. J. Theor. Phys. 41 (2002) 653-687 | null | null | hep-th | null | Tensor, matrix and quaternion formulations of Dirac-K\"ahler equation for
massive and massless fields are considered. The equation matrices obtained are
simple linear combinations of matrix elements in the 16-dimensional space. The
projection matrix-dyads defining all the 16 independent equation solutions are
found. ... | [
{
"created": "Sat, 27 Oct 2001 15:10:45 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 2002 21:22:51 GMT",
"version": "v2"
},
{
"created": "Mon, 7 Apr 2003 21:54:03 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Kruglov",
"S. I.",
""
]
] | Tensor, matrix and quaternion formulations of Dirac-K\"ahler equation for massive and massless fields are considered. The equation matrices obtained are simple linear combinations of matrix elements in the 16-dimensional space. The projection matrix-dyads defining all the 16 independent equation solutions are found. A ... | 13.761572 | 9.590229 | 14.657076 | 11.109646 | 10.895416 | 10.355043 | 10.774465 | 11.204316 | 11.159498 | 17.713848 | 11.808963 | 12.284728 | 13.736321 | 12.974294 | 13.046223 | 12.808817 | 12.906588 | 12.633101 | 13.054085 | 14.122702 | 12.583721 |
2112.04326 | Janos Balog | Sinya Aoki and J\'anos Balog | HKLL bulk reconstruction for small $\Delta$ | 28 pages, LaTeX, no figures | null | 10.1007/JHEP02(2022)015 | null | hep-th | http://creativecommons.org/licenses/by-nc-nd/4.0/ | We discuss the extension of the HKLL (Hamilton, Kabat, Lifschytz, and Lowe)
bulk reconstruction for non-interacting scalar fields corresponding to
conformal weights $\Delta$ smaller than the original condition $\Delta > d-1$.
We give explicit formulas for the cases $d-2<\Delta\leq d-1$ and $\Delta=d-s$
with integer $... | [
{
"created": "Wed, 8 Dec 2021 15:14:08 GMT",
"version": "v1"
},
{
"created": "Sun, 19 Dec 2021 14:33:03 GMT",
"version": "v2"
}
] | 2022-02-16 | [
[
"Aoki",
"Sinya",
""
],
[
"Balog",
"János",
""
]
] | We discuss the extension of the HKLL (Hamilton, Kabat, Lifschytz, and Lowe) bulk reconstruction for non-interacting scalar fields corresponding to conformal weights $\Delta$ smaller than the original condition $\Delta > d-1$. We give explicit formulas for the cases $d-2<\Delta\leq d-1$ and $\Delta=d-s$ with integer $s$... | 9.884665 | 8.905807 | 11.698588 | 8.35569 | 8.783525 | 8.870289 | 9.604815 | 7.983757 | 8.67467 | 11.506424 | 8.194204 | 7.680113 | 8.863105 | 7.892905 | 8.070927 | 7.899942 | 8.092304 | 7.941482 | 8.020968 | 9.081373 | 8.255028 |
hep-th/9811114 | Luiz Alberto Manzoni Vieira Junior | L. A. Manzoni, B. M. Pimentel and J. L. Tomazelli | Axial Anomaly through Analytic Regularization | 8 pages, LaTeX, no figures | Mod.Phys.Lett. A14 (1999) 177-184 | 10.1142/S0217732399000213 | null | hep-th | null | In this work we consider the 2-point Green's functions in (1+1) dimensional
quantum electrodynamics and show that the correct implementation of analytic
regularization gives a gauge invariant result for the vaccum polarization
amplitude and the correct coefficient for the axial anomaly.
| [
{
"created": "Thu, 12 Nov 1998 19:02:35 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Manzoni",
"L. A.",
""
],
[
"Pimentel",
"B. M.",
""
],
[
"Tomazelli",
"J. L.",
""
]
] | In this work we consider the 2-point Green's functions in (1+1) dimensional quantum electrodynamics and show that the correct implementation of analytic regularization gives a gauge invariant result for the vaccum polarization amplitude and the correct coefficient for the axial anomaly. | 12.65232 | 9.594559 | 10.707879 | 9.238935 | 11.332863 | 9.656537 | 9.033765 | 9.562895 | 9.305942 | 11.470113 | 9.46602 | 9.802397 | 9.935928 | 10.088891 | 9.873002 | 10.296276 | 9.894975 | 10.652493 | 9.934337 | 10.113174 | 10.236919 |
hep-th/0205021 | Bernd Schroers | F. A. Bais, N. M. Muller and B. J. Schroers | Quantum group symmetry and particle scattering in (2+1)-dimensional
quantum gravity | 45 pages, amslatex | Nucl.Phys. B640 (2002) 3-45 | 10.1016/S0550-3213(02)00572-2 | HWM-01-45, EMPG-02-07, ITFA-2002-12 | hep-th gr-qc math.QA | null | Starting with the Chern-Simons formulation of (2+1)-dimensional gravity we
show that the gravitational interactions deform the Poincare symmetry of flat
space-time to a quantum group symmetry. The relevant quantum group is the
quantum double of the universal cover of the (2+1)-dimensional Lorentz group,
or Lorentz do... | [
{
"created": "Thu, 2 May 2002 13:34:37 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bais",
"F. A.",
""
],
[
"Muller",
"N. M.",
""
],
[
"Schroers",
"B. J.",
""
]
] | Starting with the Chern-Simons formulation of (2+1)-dimensional gravity we show that the gravitational interactions deform the Poincare symmetry of flat space-time to a quantum group symmetry. The relevant quantum group is the quantum double of the universal cover of the (2+1)-dimensional Lorentz group, or Lorentz doub... | 5.899747 | 6.424085 | 5.965233 | 5.292375 | 5.920243 | 6.10273 | 5.619067 | 5.891359 | 5.814298 | 6.91643 | 5.746507 | 5.309668 | 5.562898 | 5.522364 | 5.543831 | 5.464141 | 5.829175 | 5.49969 | 5.516341 | 5.747141 | 5.589422 |
1611.01198 | Michael Geracie | Michael Geracie | Galilean Geometry in Condensed Matter Systems | PhD Thesis, 92 Pages, contains substantial overlap with
arXiv:1407.1242, arXiv:1408.6843, arXiv:1503.02680, arXiv:1503.02682, and
arXiv:1609.06729 | null | null | null | hep-th cond-mat.mes-hall gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a systematic means to impose Galilean invariance within field
theory. We begin by defining the most general background geometries consistent
with Galilean invariance and then turn to applications within effective field
theory, fluid dynamics, and the quantum Hall effect.
| [
{
"created": "Thu, 3 Nov 2016 21:24:53 GMT",
"version": "v1"
}
] | 2023-02-02 | [
[
"Geracie",
"Michael",
""
]
] | We present a systematic means to impose Galilean invariance within field theory. We begin by defining the most general background geometries consistent with Galilean invariance and then turn to applications within effective field theory, fluid dynamics, and the quantum Hall effect. | 12.007545 | 10.747586 | 10.921557 | 9.827317 | 10.147246 | 9.691284 | 10.359085 | 10.692261 | 10.61031 | 10.018435 | 10.473291 | 10.582593 | 11.246005 | 10.489639 | 10.39171 | 10.428586 | 10.171924 | 10.453063 | 11.032101 | 10.760933 | 10.443629 |
1301.3387 | Hossein Yavartanoo | Maria Johnstone, M. M. Sheikh-Jabbari, Joan Simon and Hossein
Yavartanoo | Near-Extremal Vanishing Horizon AdS5 Black Holes and Their CFT Duals | 36 pages, 3 figures, updated to published version | JHEP04(2013)045 | 10.1007/JHEP04(2013)045 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider families of charged rotating asymptotically AdS5 Extremal black
holes with Vanishing Horizon (EVH black holes) whose near horizon geometries
develop locally AdS3 throats. Using the AdS3/CFT2 duality, we propose an
EVH/CFT2 correspondence to describe the near-horizon low energy IR dynamics of
near-EVH blac... | [
{
"created": "Tue, 15 Jan 2013 15:54:24 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Apr 2013 03:36:49 GMT",
"version": "v2"
}
] | 2015-06-12 | [
[
"Johnstone",
"Maria",
""
],
[
"Sheikh-Jabbari",
"M. M.",
""
],
[
"Simon",
"Joan",
""
],
[
"Yavartanoo",
"Hossein",
""
]
] | We consider families of charged rotating asymptotically AdS5 Extremal black holes with Vanishing Horizon (EVH black holes) whose near horizon geometries develop locally AdS3 throats. Using the AdS3/CFT2 duality, we propose an EVH/CFT2 correspondence to describe the near-horizon low energy IR dynamics of near-EVH black ... | 8.295572 | 7.507525 | 10.041348 | 7.595116 | 7.80913 | 7.50097 | 7.536681 | 7.480784 | 7.84354 | 10.349422 | 7.796548 | 7.96217 | 8.362711 | 7.756215 | 8.379883 | 7.783646 | 7.704118 | 7.975918 | 7.986808 | 8.650034 | 7.862572 |
hep-th/9409179 | Yuji Satoh | Y. Kazama, Y. Satoh and A. Tsuchiya | A Unified Approach to Solvable Models of Dilaton Gravity in
Two-Dimensions Based on Symmetry | 29 pages, LaTeX | Phys.Rev.D51:4265-4276,1995 | 10.1103/PhysRevD.51.4265 | UT-Komaba 94-16 | hep-th | null | A large class of solvable models of dilaton gravity in two space-time
dimensions, capable of describing black hole geometry, are analyzed in a
unified way as non-linear sigma models possessing a special symmetry. This
symmetry, which can be neatly formulated in the target-space-covariant manner,
allows one to decompo... | [
{
"created": "Thu, 29 Sep 1994 12:18:38 GMT",
"version": "v1"
},
{
"created": "Sat, 1 Oct 1994 12:15:05 GMT",
"version": "v2"
}
] | 2011-07-19 | [
[
"Kazama",
"Y.",
""
],
[
"Satoh",
"Y.",
""
],
[
"Tsuchiya",
"A.",
""
]
] | A large class of solvable models of dilaton gravity in two space-time dimensions, capable of describing black hole geometry, are analyzed in a unified way as non-linear sigma models possessing a special symmetry. This symmetry, which can be neatly formulated in the target-space-covariant manner, allows one to decompose... | 11.317928 | 9.462217 | 12.032775 | 10.187817 | 10.385509 | 10.552312 | 10.078979 | 9.403152 | 9.962531 | 11.686857 | 9.975961 | 10.73152 | 11.053325 | 10.571452 | 10.808919 | 10.856261 | 10.921577 | 10.396915 | 10.594463 | 10.651299 | 10.629857 |
1511.06304 | Maxim Zabzine | Jian Qiu, Luigi Tizzano, Jacob Winding and Maxim Zabzine | Modular properties of full 5D SYM partition function | 32 pages, refs and comments added, example added | null | 10.1007/JHEP03(2016)193 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study properties of the full partition function for the $U(1)$ 5D
$\mathcal{N}=2^*$ gauge theory with adjoint hypermultiplet of mass $M$. This
theory is ultimately related to abelian 6D (2,0) theory. We construct the full
non-perturbative partition function on toric Sasaki-Einstein manifolds by
gluing flat copies ... | [
{
"created": "Thu, 19 Nov 2015 18:49:51 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Dec 2015 11:55:14 GMT",
"version": "v2"
},
{
"created": "Mon, 28 Mar 2016 08:33:45 GMT",
"version": "v3"
}
] | 2016-05-04 | [
[
"Qiu",
"Jian",
""
],
[
"Tizzano",
"Luigi",
""
],
[
"Winding",
"Jacob",
""
],
[
"Zabzine",
"Maxim",
""
]
] | We study properties of the full partition function for the $U(1)$ 5D $\mathcal{N}=2^*$ gauge theory with adjoint hypermultiplet of mass $M$. This theory is ultimately related to abelian 6D (2,0) theory. We construct the full non-perturbative partition function on toric Sasaki-Einstein manifolds by gluing flat copies of... | 7.933959 | 8.326685 | 10.819884 | 8.27397 | 8.10964 | 8.075495 | 8.281622 | 8.544732 | 8.478972 | 11.256239 | 8.076644 | 8.070978 | 8.632135 | 7.82461 | 7.913332 | 7.740183 | 7.98697 | 8.127173 | 7.950629 | 8.827556 | 7.721464 |
hep-th/0106117 | Jerome P. Gauntlett | Jerome P. Gauntlett, Nakwoo Kim, Dario Martelli and Daniel Waldram | Wrapped fivebranes and N=2 super Yang-Mills theory | 24 Latex pages, two figures;v2 typos corrected, references added | Phys.Rev. D64 (2001) 106008 | 10.1103/PhysRevD.64.106008 | QMUL-PH-01-07 | hep-th | null | We construct D=10 supergravity solutions corresponding to type IIB fivebranes
wrapping a two-sphere in a Calabi-Yau two-fold. These are related in the IR to
the large N limit of pure N=2 SU(N) super Yang-Mills theory. We show that the
singularities in the IR correspond to the wrapped branes being distributed on a
rin... | [
{
"created": "Thu, 14 Jun 2001 08:03:29 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Aug 2001 13:26:45 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Gauntlett",
"Jerome P.",
""
],
[
"Kim",
"Nakwoo",
""
],
[
"Martelli",
"Dario",
""
],
[
"Waldram",
"Daniel",
""
]
] | We construct D=10 supergravity solutions corresponding to type IIB fivebranes wrapping a two-sphere in a Calabi-Yau two-fold. These are related in the IR to the large N limit of pure N=2 SU(N) super Yang-Mills theory. We show that the singularities in the IR correspond to the wrapped branes being distributed on a ring.... | 7.909171 | 6.674992 | 9.286796 | 7.344266 | 7.261673 | 7.131965 | 6.698335 | 7.136511 | 7.178089 | 9.650168 | 6.949172 | 7.492278 | 8.322695 | 7.622585 | 7.339952 | 7.488311 | 7.442223 | 7.693153 | 7.364093 | 8.178622 | 7.572955 |
2008.09117 | Ling Lin | Fabio Apruzzi, Markus Dierigl, Ling Lin | The Fate of Discrete 1-Form Symmetries in 6d | 48 pages + appendices, 1 figure; v3: typos correct, improved
discussion, published version | SciPost Phys. 12, 047 (2022) | 10.21468/SciPostPhys.12.2.047 | CERN-TH-2020-132 | hep-th | http://creativecommons.org/licenses/by/4.0/ | Recently introduced generalized global symmetries have been useful in order
to understand non-perturbative aspects of quantum field theories in four and
lower dimensions. In this paper we focus on 1-form symmetries of weakly coupled
6d supersymmetric gauge theories coupled to dynamical tensor multiplets. We
study the... | [
{
"created": "Thu, 20 Aug 2020 18:00:00 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Sep 2020 14:35:34 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Feb 2022 12:46:24 GMT",
"version": "v3"
}
] | 2022-02-02 | [
[
"Apruzzi",
"Fabio",
""
],
[
"Dierigl",
"Markus",
""
],
[
"Lin",
"Ling",
""
]
] | Recently introduced generalized global symmetries have been useful in order to understand non-perturbative aspects of quantum field theories in four and lower dimensions. In this paper we focus on 1-form symmetries of weakly coupled 6d supersymmetric gauge theories coupled to dynamical tensor multiplets. We study the c... | 11.052771 | 11.13052 | 12.801398 | 10.998469 | 11.457947 | 11.430081 | 10.924069 | 11.010018 | 10.921963 | 13.213859 | 10.991772 | 10.813411 | 11.571509 | 10.667488 | 10.890686 | 10.702672 | 10.588424 | 11.051269 | 10.855621 | 11.384794 | 10.471983 |
1111.6709 | Takuya Saka | Katsushi Ito, Hiroaki Nakajima, Takuya Saka and Shin Sasaki | N=4 Instanton Calculus in Omega and R-R Backgrounds | 28 pages | Nuclear Physics B 860 (2012) 267 | 10.1016/j.nuclphysb.2012.03.001 | TIT/HEP-615; KIAS-P11060 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the instanton calculus for N=4 super Yang-Mills theory in
ten-dimensional Omega-background with the R-symmetry Wilson line gauge field.
From the ADHM construction of instantons in the background, we obtain the
deformed instanton effective action. For a certain case we get the effective
action of N=2^* theory... | [
{
"created": "Tue, 29 Nov 2011 07:03:32 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Dec 2011 05:27:46 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Jan 2012 08:37:23 GMT",
"version": "v3"
},
{
"created": "Mon, 2 Apr 2012 13:31:33 GMT",
"version": "v4"
}
] | 2015-06-03 | [
[
"Ito",
"Katsushi",
""
],
[
"Nakajima",
"Hiroaki",
""
],
[
"Saka",
"Takuya",
""
],
[
"Sasaki",
"Shin",
""
]
] | We study the instanton calculus for N=4 super Yang-Mills theory in ten-dimensional Omega-background with the R-symmetry Wilson line gauge field. From the ADHM construction of instantons in the background, we obtain the deformed instanton effective action. For a certain case we get the effective action of N=2^* theory i... | 7.948313 | 6.128107 | 9.146657 | 6.711623 | 6.937224 | 6.69216 | 6.837796 | 6.553546 | 6.742138 | 9.009849 | 6.736041 | 7.010984 | 8.020259 | 7.269318 | 6.98348 | 7.096964 | 7.17812 | 7.165454 | 6.924306 | 8.420734 | 7.280274 |
2109.06938 | Joel Acosta | Joel Acosta, Alan Garbarz, Andres Goya, Mauricio Leston | One-Loop Partition Function, Gauge Accessibility and Spectra in AdS$_3$
Gravity | 25 pages | null | 10.1007/JHEP12(2021)097 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We continue the study of the one-loop partition function of AdS$_3$ gravity
with focus on the square-integrability condition on the fluctuating fields. In
a previous work we found that the Brown-Henneaux boundary conditions follow
directly from the $L^2$ condition. Here we rederive the partition function as a
ratio o... | [
{
"created": "Tue, 14 Sep 2021 19:31:02 GMT",
"version": "v1"
}
] | 2022-01-05 | [
[
"Acosta",
"Joel",
""
],
[
"Garbarz",
"Alan",
""
],
[
"Goya",
"Andres",
""
],
[
"Leston",
"Mauricio",
""
]
] | We continue the study of the one-loop partition function of AdS$_3$ gravity with focus on the square-integrability condition on the fluctuating fields. In a previous work we found that the Brown-Henneaux boundary conditions follow directly from the $L^2$ condition. Here we rederive the partition function as a ratio of ... | 11.837145 | 12.475277 | 12.98604 | 12.313312 | 12.547278 | 12.582403 | 13.417061 | 11.891291 | 12.376494 | 14.287057 | 11.734543 | 11.819849 | 12.152907 | 11.545412 | 11.619928 | 11.510943 | 11.472123 | 11.41503 | 11.265668 | 12.058267 | 11.547267 |
0707.1329 | Michele Arzano | Michele Arzano and Antonino Marciano | Fock space, quantum fields and kappa-Poincar\'e symmetries | RevTeX, 17 pages, 5 figures | Phys.Rev.D76:125005,2007 | 10.1103/PhysRevD.76.125005 | null | hep-th | null | We study the quantization of a linear scalar field, whose symmetries are
described by the kappa-Poincare' Hopf-algebra, via deformed Fock space
construction. The one-particle sector of the theory exhibits a natural
(planckian) cut-off for the field modes. At the multi-particle level the
non-trivial co-algebra structu... | [
{
"created": "Tue, 10 Jul 2007 15:16:17 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Arzano",
"Michele",
""
],
[
"Marciano",
"Antonino",
""
]
] | We study the quantization of a linear scalar field, whose symmetries are described by the kappa-Poincare' Hopf-algebra, via deformed Fock space construction. The one-particle sector of the theory exhibits a natural (planckian) cut-off for the field modes. At the multi-particle level the non-trivial co-algebra structure... | 10.720311 | 10.264692 | 9.593671 | 9.349527 | 9.2307 | 9.140084 | 9.985255 | 8.989032 | 9.382918 | 10.047214 | 8.96087 | 9.475746 | 9.772567 | 9.406294 | 9.186148 | 9.288266 | 9.227362 | 9.58999 | 9.272475 | 9.537684 | 8.958694 |
hep-th/9704090 | Anton Zabrodin | I.Krichever, P.Wiegmann and A.Zabrodin | Elliptic solutions to difference non-linear equations and related
many-body problems | 22 pages, Latex with emlines2.sty | Commun.Math.Phys. 193 (1998) 373-396 | 10.1007/s002200050333 | null | hep-th | null | We study algebro-geometric (finite-gap) and elliptic solutions of fully
discretized KP or 2D Toda equations. In bilinear form they are Hirota's
difference equation for $\tau$-functions. Starting from a given algebraic
curve, we express the $\tau$-function and the Baker-Akhiezer function in terms
of the Riemann theta ... | [
{
"created": "Fri, 11 Apr 1997 00:59:55 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Krichever",
"I.",
""
],
[
"Wiegmann",
"P.",
""
],
[
"Zabrodin",
"A.",
""
]
] | We study algebro-geometric (finite-gap) and elliptic solutions of fully discretized KP or 2D Toda equations. In bilinear form they are Hirota's difference equation for $\tau$-functions. Starting from a given algebraic curve, we express the $\tau$-function and the Baker-Akhiezer function in terms of the Riemann theta fu... | 6.62647 | 7.097806 | 7.694457 | 6.576829 | 7.793303 | 7.537799 | 6.981884 | 6.872992 | 6.993362 | 9.120465 | 6.51635 | 6.600061 | 6.646325 | 6.375991 | 6.639313 | 6.507539 | 6.582198 | 6.61061 | 6.503104 | 6.865787 | 6.582389 |
hep-th/9612157 | Nathan Seiberg | Tom Banks, Nathan Seiberg and Stephen Shenker | Branes from Matrices | 17 pages. A number of new conceptual issues added. Some misprints
corrected | Nucl.Phys.B490:91-106,1997 | 10.1016/S0550-3213(97)00105-3 | RU-96-117 | hep-th | null | Various aspects of branes in the recently proposed matrix model for M theory
are discussed. A careful analysis of the supersymmetry algebra of the matrix
model uncovers some central charges which can be activated only in the large
$N$ limit. We identify the states with non-zero charges as branes of different
dimensio... | [
{
"created": "Fri, 13 Dec 1996 20:00:25 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Jan 1997 18:53:10 GMT",
"version": "v2"
}
] | 2009-09-15 | [
[
"Banks",
"Tom",
""
],
[
"Seiberg",
"Nathan",
""
],
[
"Shenker",
"Stephen",
""
]
] | Various aspects of branes in the recently proposed matrix model for M theory are discussed. A careful analysis of the supersymmetry algebra of the matrix model uncovers some central charges which can be activated only in the large $N$ limit. We identify the states with non-zero charges as branes of different dimensions... | 10.786455 | 9.095203 | 11.550458 | 8.254865 | 8.369094 | 8.202348 | 8.147023 | 8.400571 | 8.818851 | 12.596905 | 8.827579 | 9.393313 | 10.366164 | 9.087546 | 8.910705 | 9.199836 | 9.032918 | 9.343861 | 9.035925 | 10.585258 | 9.392156 |
hep-th/0210215 | Florian Conrady | Florian Conrady (Heidelberg U. & Potsdam, Max Planck Inst.), Christoph
Schweigert (Paris U., VI-VII & Aachen, Tech. Hochschul.) | Topologizations of Chiral Representations | 24pp, section on open questions added | Commun.Math.Phys. 245 (2004) 429-448 | 10.1007/s00220-003-1034-y | HD-THEP-02-10, AEI-2002-085, PAR-LPTHE/02-44, PITHA 02/13 | hep-th math-ph math.FA math.MP | null | We analyze and compare two families of topologies that have been proposed for
representation spaces of chiral algebras by Huang and Gaberdiel & Goddard
respectively. We show, in particular, that for suitable pairs the topology of
Gaberdiel & Goddard is coarser. We also give a new proof that the chiral
two-point block... | [
{
"created": "Tue, 22 Oct 2002 14:45:54 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Nov 2003 15:41:41 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Conrady",
"Florian",
"",
"Heidelberg U. & Potsdam, Max Planck Inst."
],
[
"Schweigert",
"Christoph",
"",
"Paris U., VI-VII & Aachen, Tech. Hochschul."
]
] | We analyze and compare two families of topologies that have been proposed for representation spaces of chiral algebras by Huang and Gaberdiel & Goddard respectively. We show, in particular, that for suitable pairs the topology of Gaberdiel & Goddard is coarser. We also give a new proof that the chiral two-point blocks ... | 9.673098 | 9.756352 | 14.488999 | 8.830625 | 9.198832 | 10.210173 | 10.727568 | 8.632598 | 10.574691 | 13.392076 | 9.585932 | 10.110986 | 11.109993 | 10.121755 | 9.952083 | 10.547601 | 10.628796 | 9.442751 | 10.111567 | 10.593521 | 9.205681 |
1305.5684 | Diego Rodriguez-Gomez | Diego Rodriguez-Gomez, Gabi Zafrir | On the 5d instanton index as a Hilbert series | 13 pages, 2 figures | null | 10.1016/j.nuclphysb.2013.11.006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The superconformal index for N=2 5d theories contains a non-perturbative part
arising from 5d instantonic operators which coincides with the Nekrasov
instanton partition function. In this note, for pure gauge theories, we
elaborate on the relation between such instanton index and the Hilbert series
of the instanton m... | [
{
"created": "Fri, 24 May 2013 11:05:47 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Rodriguez-Gomez",
"Diego",
""
],
[
"Zafrir",
"Gabi",
""
]
] | The superconformal index for N=2 5d theories contains a non-perturbative part arising from 5d instantonic operators which coincides with the Nekrasov instanton partition function. In this note, for pure gauge theories, we elaborate on the relation between such instanton index and the Hilbert series of the instanton mod... | 6.983716 | 6.034246 | 6.926714 | 5.907979 | 6.490439 | 6.153763 | 6.336493 | 6.108539 | 6.451 | 7.265053 | 6.070138 | 6.172922 | 6.800166 | 6.137915 | 6.30581 | 6.354656 | 6.463827 | 6.268516 | 6.187291 | 6.848846 | 6.36676 |
1112.2876 | Thomas Mohaupt | Thomas Mohaupt, Owen Vaughan | The Hesse potential, the c-map and black hole solutions | 76 pages. Second revised version: substantial extension. Further
references added and discussion extended. Construction of axion-free non-BPS
extremal solutions for a class of non-homogeneous target spaces added.
Accepted for publication in JHEP | null | 10.1007/JHEP07(2012)163 | LTH 933 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a new formulation of the local c-map, which makes use of the real
formulation of special Kahler geometry and the associated Hesse potential. As
an application we use the temporal version of the c-map to derive the black
hole attractor equations from geometric properties of the scalar manifold, and
we const... | [
{
"created": "Tue, 13 Dec 2011 12:30:25 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jan 2012 18:18:19 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Jul 2012 09:47:20 GMT",
"version": "v3"
}
] | 2017-08-23 | [
[
"Mohaupt",
"Thomas",
""
],
[
"Vaughan",
"Owen",
""
]
] | We present a new formulation of the local c-map, which makes use of the real formulation of special Kahler geometry and the associated Hesse potential. As an application we use the temporal version of the c-map to derive the black hole attractor equations from geometric properties of the scalar manifold, and we constru... | 14.722383 | 11.508454 | 16.271315 | 11.558726 | 12.446198 | 12.953554 | 14.19259 | 11.726277 | 12.807626 | 15.924492 | 13.159951 | 12.88348 | 14.121984 | 14.045038 | 13.709849 | 13.176387 | 12.974284 | 12.781834 | 13.057082 | 15.329415 | 13.550408 |
hep-th/9511037 | null | J.M.F. Labastida | Topological Quantum Field Theory: A Progress Report | latex, 17 pages, talk given at the IV Fall Workshop on Differential
Geometry and its Applications, 1995 | null | null | USC-FT-26-95 | hep-th alg-geom math.AG math.QA q-alg | null | A brief introduction to Topological Quantum Field Theory as well as a
description of recent progress made in the field is presented. I concentrate
mainly on the connection between Chern-Simons gauge theory and Vassiliev
invariants, and Donaldson theory and its generalizations and Seiberg-Witten
invariants. Emphasis i... | [
{
"created": "Mon, 6 Nov 1995 08:25:13 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Labastida",
"J. M. F.",
""
]
] | A brief introduction to Topological Quantum Field Theory as well as a description of recent progress made in the field is presented. I concentrate mainly on the connection between Chern-Simons gauge theory and Vassiliev invariants, and Donaldson theory and its generalizations and Seiberg-Witten invariants. Emphasis is ... | 9.080765 | 7.910349 | 8.97752 | 7.952519 | 8.873096 | 8.551855 | 9.117299 | 8.584278 | 7.959292 | 9.228888 | 8.353624 | 8.1724 | 8.545618 | 8.083434 | 8.035868 | 8.303137 | 8.22436 | 7.788144 | 8.000273 | 8.418329 | 8.177212 |
hep-th/0007099 | Joachim Rahmfeld | P. Claus, J. Rahmfeld, H. Robins, J. Tannenhauser, Y. Zunger | Isometries in anti-de Sitter and Conformal Superspaces | 19 pages, LaTeX | JHEP 0007:047,2000 | 10.1088/1126-6708/2000/07/047 | null | hep-th | null | We derive explicit forms for the superisometries of a wide class of
supercoset manifolds, including those with fermionic generators in the
stability group. We apply the results to construct the action of SU(2,2|4) on
three supercoset manifolds: (10|32)-dimensional AdS_5 x S^5 superspace,
(4|16)-dimensional conformal ... | [
{
"created": "Wed, 12 Jul 2000 21:10:20 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Claus",
"P.",
""
],
[
"Rahmfeld",
"J.",
""
],
[
"Robins",
"H.",
""
],
[
"Tannenhauser",
"J.",
""
],
[
"Zunger",
"Y.",
""
]
] | We derive explicit forms for the superisometries of a wide class of supercoset manifolds, including those with fermionic generators in the stability group. We apply the results to construct the action of SU(2,2|4) on three supercoset manifolds: (10|32)-dimensional AdS_5 x S^5 superspace, (4|16)-dimensional conformal su... | 5.313151 | 4.989063 | 6.138778 | 4.940094 | 5.26264 | 4.86937 | 5.27039 | 4.807804 | 5.239874 | 6.086814 | 4.924823 | 5.189514 | 5.469631 | 5.126723 | 5.208971 | 5.008387 | 5.047025 | 5.163936 | 5.118957 | 5.429084 | 5.117896 |
hep-th/9905135 | Ashok Das | Ashok Das and Sergio A. Pernice | Supersymmetry and Singular Potentials | 28 pages | Nucl.Phys. B561 (1999) 357-384 | 10.1016/S0550-3213(99)00541-6 | null | hep-th | null | The breaking of supersymmetry due to singular potentials in supersymmetric
quantum mechanics is critically analyzed. It is shown that, when properly
regularized, these potentials respect supersymmetry, even when the
regularization parameter is removed.
| [
{
"created": "Tue, 18 May 1999 17:46:56 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Das",
"Ashok",
""
],
[
"Pernice",
"Sergio A.",
""
]
] | The breaking of supersymmetry due to singular potentials in supersymmetric quantum mechanics is critically analyzed. It is shown that, when properly regularized, these potentials respect supersymmetry, even when the regularization parameter is removed. | 11.640115 | 6.14536 | 8.785213 | 6.958209 | 6.658638 | 5.923954 | 5.52076 | 6.543667 | 6.857353 | 10.805376 | 7.244863 | 7.347735 | 9.441331 | 7.92163 | 7.969782 | 7.731357 | 8.054044 | 7.97693 | 8.468837 | 9.780476 | 7.793432 |
hep-th/0304021 | Hoshino | Y. Hoshino | Low-Energy Theorem Approach to One-Particle Singularity in QED{2+1} | 18 pages, REVTeX4,abstract modefied and section three changed | JHEP 0305 (2003) 075 | 10.1088/1126-6708/2003/05/075 | null | hep-th | null | We evaluate the propagator of scalar and spinor in three dimensional quantum
electrodynamics with the use of Ward-Identity for soft-photon emission
vertex.We work well in position space to treat infrared divergences in our
model. Exponentiation of one-photon matrix element yields a full propagator in
position space.I... | [
{
"created": "Wed, 2 Apr 2003 21:44:09 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Apr 2003 23:43:36 GMT",
"version": "v2"
},
{
"created": "Wed, 16 Apr 2003 00:52:07 GMT",
"version": "v3"
},
{
"created": "Thu, 8 May 2003 01:59:43 GMT",
"version": "v4"
},
{
"cre... | 2009-11-10 | [
[
"Hoshino",
"Y.",
""
]
] | We evaluate the propagator of scalar and spinor in three dimensional quantum electrodynamics with the use of Ward-Identity for soft-photon emission vertex.We work well in position space to treat infrared divergences in our model. Exponentiation of one-photon matrix element yields a full propagator in position space.It ... | 19.856695 | 19.871122 | 16.999254 | 18.230612 | 19.14917 | 20.225311 | 19.893156 | 19.687084 | 18.664291 | 22.340883 | 17.911594 | 19.008669 | 19.225702 | 18.638792 | 19.468901 | 18.469612 | 19.141212 | 19.102947 | 18.522636 | 18.605698 | 18.857395 |
hep-th/9912249 | Barton Zwiebach | Ashoke Sen and Barton Zwiebach | Tachyon condensation in string field theory | 13 pages, LaTex | JHEP 0003:002,2000 | 10.1088/1126-6708/2000/03/002 | MRI-PHY/P991238, CTP-MIT-2934 | hep-th | null | It has been conjectured that at a stationary point of the tachyon potential
for the D-brane of bosonic string theory, the negative energy density exactly
cancels the D-brane tension. We evaluate this tachyon potential by off-shell
calculations in open string field theory. Surprisingly, the condensation of the
tachyon... | [
{
"created": "Fri, 24 Dec 1999 21:56:09 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Sen",
"Ashoke",
""
],
[
"Zwiebach",
"Barton",
""
]
] | It has been conjectured that at a stationary point of the tachyon potential for the D-brane of bosonic string theory, the negative energy density exactly cancels the D-brane tension. We evaluate this tachyon potential by off-shell calculations in open string field theory. Surprisingly, the condensation of the tachyon m... | 8.546014 | 8.245938 | 9.412452 | 7.671464 | 9.001723 | 8.296994 | 8.077033 | 7.8265 | 7.619044 | 10.266006 | 7.816991 | 8.278251 | 8.562399 | 7.956251 | 8.27534 | 7.882778 | 7.870019 | 8.017915 | 8.306301 | 8.842433 | 7.974247 |
1709.03832 | Ahmad Mohamadnejad | Ahmad Mohamadnejad | Vacuum and Symmetry Breaking: New Approach | 19 pages, published in International Journal of Theoretical Physics | Int.J.Theor.Phys. 59 (2020) 8, 2625-2638 | 10.1007/s10773-020-04532-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new mechanism for symmetry breaking in which, apart from
particle degrees of freedom, topological degrees of freedom also emerge. In
this method, a decomposition for the fields of the Yang-Mills-Higgs theory is
introduced and Lagrangian is written based on new variables. This new
Lagrangian does not chan... | [
{
"created": "Tue, 12 Sep 2017 13:34:46 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Mar 2018 14:00:17 GMT",
"version": "v2"
},
{
"created": "Sat, 25 Jul 2020 12:18:27 GMT",
"version": "v3"
}
] | 2020-07-28 | [
[
"Mohamadnejad",
"Ahmad",
""
]
] | We propose a new mechanism for symmetry breaking in which, apart from particle degrees of freedom, topological degrees of freedom also emerge. In this method, a decomposition for the fields of the Yang-Mills-Higgs theory is introduced and Lagrangian is written based on new variables. This new Lagrangian does not change... | 8.490619 | 8.129447 | 8.116974 | 8.062722 | 8.444496 | 8.477525 | 8.37801 | 7.71236 | 8.036569 | 8.693011 | 7.882439 | 8.080713 | 7.999951 | 7.911489 | 7.974565 | 7.888871 | 8.024833 | 7.856589 | 7.799059 | 7.984982 | 8.005858 |
2405.10061 | Jianfei Xu | Xuhao Jiang and Jianfei Xu | Warped CFT duals of the Pleba\'{n}ski-Demia\'{n}ski family of solutions | 26 pages | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we analyze the symmetry properties of the complete family of
type D spacetimes generalized form the Pleba\'{n}ski-Demia\'{n}ski solution in
four dimensions holographically in terms of a warped CFT. The generalized
Pleba\'{n}ski-Demia\'{n}ski solutions are black hole-like spacetimes
characterized by sev... | [
{
"created": "Thu, 16 May 2024 12:50:51 GMT",
"version": "v1"
}
] | 2024-05-17 | [
[
"Jiang",
"Xuhao",
""
],
[
"Xu",
"Jianfei",
""
]
] | In this paper, we analyze the symmetry properties of the complete family of type D spacetimes generalized form the Pleba\'{n}ski-Demia\'{n}ski solution in four dimensions holographically in terms of a warped CFT. The generalized Pleba\'{n}ski-Demia\'{n}ski solutions are black hole-like spacetimes characterized by seven... | 10.315598 | 10.296895 | 10.159727 | 9.532746 | 9.460459 | 10.917871 | 10.495984 | 9.940994 | 9.949991 | 11.556339 | 9.99753 | 9.892268 | 9.930645 | 9.550805 | 9.812559 | 9.766525 | 9.999132 | 9.549496 | 9.845373 | 9.97051 | 9.860264 |
0711.0192 | Andrei Mironov | A.Mironov, A.Morozov and T.Tomaras | Some properties of the Alday-Maldacena minimum | 10 pages | Phys.Lett.B659:723-731,2008 | 10.1016/j.physletb.2007.11.025 | ITEP-TH-39/07 | hep-th | null | The Alday-Maldacena solution, relevant to the n=4 gluon amplitude in N=4 SYM
at strong coupling, was recently identified as a minimum of the regularized
action in the moduli space of solutions of the AdS_5 sigma-model equations of
motion. Analogous solutions of the Nambu-Goto equations for the n=4 case are
presented ... | [
{
"created": "Thu, 1 Nov 2007 19:12:17 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
],
[
"Tomaras",
"T.",
""
]
] | The Alday-Maldacena solution, relevant to the n=4 gluon amplitude in N=4 SYM at strong coupling, was recently identified as a minimum of the regularized action in the moduli space of solutions of the AdS_5 sigma-model equations of motion. Analogous solutions of the Nambu-Goto equations for the n=4 case are presented an... | 10.464565 | 10.253972 | 9.915788 | 9.113455 | 10.644123 | 10.535278 | 9.659337 | 9.92838 | 9.688811 | 10.608456 | 9.647327 | 9.561178 | 9.093431 | 9.487576 | 9.889573 | 9.759195 | 9.539771 | 9.818443 | 9.823893 | 9.197723 | 9.511911 |
2009.01211 | Congkao Wen | Michael B. Green, Congkao Wen | Maximal $U(1)_Y$-violating $n$-point correlators in $\mathcal{N}=4$
super-Yang-Mills theory | 67 pages; v2: 68 pages, minor corrections, references added, matches
JHEP version | null | 10.1007/JHEP02(2021)042 | QMUL-PH-20-23 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper concerns a special class of $n$-point correlation functions of
operators in the stress tensor supermultiplet of $\mathcal{N}=4$ supersymmetric
$SU(N)$ Yang-Mills theory. These are "maximal $U(1)_Y$-violating" correlators
that violate the bonus $U(1)_Y$ charge by a maximum of $2(n-4)$ units. We will
demonst... | [
{
"created": "Wed, 2 Sep 2020 17:36:51 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Feb 2021 11:27:00 GMT",
"version": "v2"
}
] | 2021-02-24 | [
[
"Green",
"Michael B.",
""
],
[
"Wen",
"Congkao",
""
]
] | This paper concerns a special class of $n$-point correlation functions of operators in the stress tensor supermultiplet of $\mathcal{N}=4$ supersymmetric $SU(N)$ Yang-Mills theory. These are "maximal $U(1)_Y$-violating" correlators that violate the bonus $U(1)_Y$ charge by a maximum of $2(n-4)$ units. We will demonstra... | 5.23839 | 5.443745 | 5.489741 | 5.062505 | 5.202945 | 5.066357 | 5.14639 | 5.153008 | 4.965233 | 6.277734 | 5.084566 | 5.073013 | 5.274405 | 5.025763 | 5.090712 | 5.217029 | 5.134303 | 5.000403 | 5.071522 | 5.353134 | 5.100287 |
1102.4847 | Tudor Dan Dimofte | Tudor Dimofte | Quantum Riemann Surfaces in Chern-Simons Theory | 110 pages, 14 figures; v2: references added and clarified, discussion
of character varieties (Sec. 2) improved; v3: small typos corrected in Sec
6.3.2 | null | null | null | hep-th math.GT math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct from first principles the operator 'A-hat' that annihilates the
partition functions (or wavefunctions) of three-dimensional Chern-Simons theory
with gauge groups SU(2), SL(2,R), or SL(2,C) on a knot complement M. The
operator 'A-hat' is a quantization of the knot complement's classical
A-polynomial A(l,m... | [
{
"created": "Wed, 23 Feb 2011 21:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Apr 2011 17:49:09 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Aug 2011 19:32:59 GMT",
"version": "v3"
}
] | 2015-03-19 | [
[
"Dimofte",
"Tudor",
""
]
] | We construct from first principles the operator 'A-hat' that annihilates the partition functions (or wavefunctions) of three-dimensional Chern-Simons theory with gauge groups SU(2), SL(2,R), or SL(2,C) on a knot complement M. The operator 'A-hat' is a quantization of the knot complement's classical A-polynomial A(l,m).... | 11.749383 | 11.076143 | 13.481053 | 11.009518 | 11.217242 | 11.805812 | 13.145495 | 11.676001 | 10.41228 | 14.652041 | 10.605623 | 10.355474 | 11.817944 | 10.399755 | 10.376962 | 10.27772 | 10.849234 | 10.221204 | 10.493952 | 11.718 | 10.543874 |
1502.05057 | Chia-Hsien Shen | Clifford Cheung, Chia-Hsien Shen, and Jaroslav Trnka | Simple Recursion Relations for General Field Theories | 27 pages and 2 figures; v2: typos corrected to match journal version | JHEP 2015:118 | 10.1007/JHEP06(2015)118 | CALT-TH-2015-005 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | On-shell methods offer an alternative definition of quantum field theory at
tree-level, replacing Feynman diagrams with recursion relations and interaction
vertices with a handful of seed scattering amplitudes. In this paper we
determine the simplest recursion relations needed to construct a general
four-dimensional ... | [
{
"created": "Tue, 17 Feb 2015 21:02:49 GMT",
"version": "v1"
},
{
"created": "Wed, 20 May 2015 23:53:12 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Nov 2015 18:00:19 GMT",
"version": "v3"
}
] | 2015-11-10 | [
[
"Cheung",
"Clifford",
""
],
[
"Shen",
"Chia-Hsien",
""
],
[
"Trnka",
"Jaroslav",
""
]
] | On-shell methods offer an alternative definition of quantum field theory at tree-level, replacing Feynman diagrams with recursion relations and interaction vertices with a handful of seed scattering amplitudes. In this paper we determine the simplest recursion relations needed to construct a general four-dimensional qu... | 2.528877 | 7.315067 | 7.963429 | 6.823287 | 7.386891 | 8.080673 | 7.437741 | 7.247353 | 7.29041 | 7.633082 | 6.933198 | 6.289732 | 5.793451 | 5.79529 | 6.346585 | 5.988576 | 6.595934 | 5.912744 | 5.750858 | 6.011638 | 5.908757 |
hep-th/0610055 | Marios Petropoulos | P.M. Petropoulos, K. Sfetsos | Non-Abelian coset string backgrounds from asymptotic and initial data | 26 pages | JHEP 0704:033,2007 | 10.1088/1126-6708/2007/04/033 | CPHT-RR052.0606, NEIP-06-06 | hep-th | null | We describe hierarchies of exact string backgrounds obtained as non-Abelian
cosets of orthogonal groups and having a space--time realization in terms of
gauged WZW models. For each member in these hierarchies, the target-space
backgrounds are generated by the ``boundary'' backgrounds of the next member.
We explicitly... | [
{
"created": "Wed, 4 Oct 2006 20:17:44 GMT",
"version": "v1"
}
] | 2010-10-27 | [
[
"Petropoulos",
"P. M.",
""
],
[
"Sfetsos",
"K.",
""
]
] | We describe hierarchies of exact string backgrounds obtained as non-Abelian cosets of orthogonal groups and having a space--time realization in terms of gauged WZW models. For each member in these hierarchies, the target-space backgrounds are generated by the ``boundary'' backgrounds of the next member. We explicitly d... | 15.519146 | 14.744632 | 16.576969 | 14.006602 | 15.956587 | 15.298074 | 16.522118 | 13.824804 | 14.273611 | 18.354105 | 13.782507 | 13.755175 | 15.800121 | 14.028114 | 14.179503 | 13.571968 | 14.143657 | 13.57749 | 14.205999 | 15.706559 | 13.295761 |
hep-th/9410050 | Ruth Gregory | Ruth Gregory and Raymond Laflamme | Evidence for the Stability of Extremal Black p-Branes | minor changes to references, 15 pages + 1 figure | Phys.Rev.D51:305-309,1995 | 10.1103/PhysRevD.51.305 | DAMTP/R-94/40, LA-UR-94-3323 | hep-th gr-qc | null | We investigate the stability of the extremal black p-brane which contains a
n-form and a dilaton. We show that the instability due to the s-mode, which was
present in the uncharged and non-extremal p-brane, disappears in the extreme
case. This is shown to be consistent with an entropy argument which shows that
the ze... | [
{
"created": "Fri, 7 Oct 1994 16:49:25 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Dec 1994 17:47:32 GMT",
"version": "v2"
}
] | 2009-12-30 | [
[
"Gregory",
"Ruth",
""
],
[
"Laflamme",
"Raymond",
""
]
] | We investigate the stability of the extremal black p-brane which contains a n-form and a dilaton. We show that the instability due to the s-mode, which was present in the uncharged and non-extremal p-brane, disappears in the extreme case. This is shown to be consistent with an entropy argument which shows that the zero... | 9.129269 | 8.21806 | 9.675137 | 8.253532 | 8.625082 | 8.235976 | 7.801028 | 8.965135 | 8.347776 | 9.10388 | 8.181693 | 8.386417 | 8.981204 | 8.231788 | 8.234365 | 8.370227 | 8.38553 | 8.228432 | 8.153971 | 9.025496 | 7.988795 |
1507.01229 | Lee Smolin | Lee Smolin | Dynamics of the cosmological and Newton's constant | 18 pages, For a related talk see http://pirsa.org/15060033/ | null | 10.1088/0264-9381/33/2/025011 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A modification of general relativity is presented in which Newton's constant
and the cosmological constant become a conjugate pair of dynamical variables.
| [
{
"created": "Sun, 5 Jul 2015 15:22:28 GMT",
"version": "v1"
}
] | 2016-01-13 | [
[
"Smolin",
"Lee",
""
]
] | A modification of general relativity is presented in which Newton's constant and the cosmological constant become a conjugate pair of dynamical variables. | 10.234662 | 5.775538 | 5.509465 | 5.736812 | 5.9415 | 5.642253 | 5.49403 | 5.351044 | 6.456863 | 5.917025 | 6.15737 | 6.279103 | 6.774466 | 6.590735 | 6.409013 | 6.787278 | 6.716302 | 6.375053 | 7.240107 | 6.996558 | 6.878 |
hep-th/9708008 | null | Nemanja Kaloper and Keith A. Olive | Singularities In Scalar-Tensor Cosmologies | 23 pages, latex, no figures | Phys.Rev.D57:811-822,1998 | 10.1103/PhysRevD.57.811 | UMN-TH-1602/97, WATPHYS-THY-97/06 | hep-th astro-ph gr-qc | null | In this article, we examine the possibility that there exist special
scalar-tensor theories of gravity with completely nonsingular FRW solutions.
Our investigation in fact shows that while most probes living in such a
Universe never see the singularity, gravity waves always do. This is because
they couple to both the... | [
{
"created": "Tue, 5 Aug 1997 00:29:22 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Kaloper",
"Nemanja",
""
],
[
"Olive",
"Keith A.",
""
]
] | In this article, we examine the possibility that there exist special scalar-tensor theories of gravity with completely nonsingular FRW solutions. Our investigation in fact shows that while most probes living in such a Universe never see the singularity, gravity waves always do. This is because they couple to both the m... | 11.698686 | 11.301596 | 11.744613 | 11.188239 | 12.00985 | 12.432659 | 12.712756 | 11.602798 | 11.74171 | 12.569057 | 10.540188 | 10.756978 | 11.120809 | 10.775376 | 10.783072 | 10.610388 | 11.201685 | 10.400674 | 10.902008 | 10.923544 | 11.039761 |
1612.08569 | Piotr T. Chru\'sciel | P.T. Chru\'sciel, M. H\"orzinger | Compact singularity-free Kerr-Newman-de Sitter instantons | introduction expanded, version as published in PRD | Phys. Rev. D 95, 086012 (2017) | 10.1103/PhysRevD.95.086012 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Generalising arXiv:1511.08496, we construct further families of compact
Einstein-Maxwell instantons associated with the Kerr-Newman metrics with a
positive cosmological constant.
| [
{
"created": "Tue, 27 Dec 2016 10:58:51 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Apr 2017 19:05:40 GMT",
"version": "v2"
}
] | 2017-04-19 | [
[
"Chruściel",
"P. T.",
""
],
[
"Hörzinger",
"M.",
""
]
] | Generalising arXiv:1511.08496, we construct further families of compact Einstein-Maxwell instantons associated with the Kerr-Newman metrics with a positive cosmological constant. | 17.340115 | 13.941614 | 12.816463 | 11.533579 | 15.704424 | 13.23022 | 13.322612 | 12.843553 | 14.32015 | 13.522431 | 13.13127 | 15.511436 | 13.317375 | 13.756986 | 14.630929 | 14.368802 | 13.765326 | 13.3846 | 12.962739 | 12.727465 | 13.848732 |
2406.05725 | Alberto Alonso-Izquierdo Dr | A. Alonso-Izquierdo, J. Mateos Guillarte, M. Rees and A. Wereszczynski | Spectral wall in collisions of excited Abelian Higgs vortices | 6 pages, 4 figures and ancillary files (5 videos) | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find a spectral wall in collisions of two vortices in the Abelian Higgs
model at the critical coupling. It occurs if the out-of-phase mode of initially
separated vortices is excited.
| [
{
"created": "Sun, 9 Jun 2024 10:32:59 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Jun 2024 08:42:41 GMT",
"version": "v2"
}
] | 2024-06-17 | [
[
"Alonso-Izquierdo",
"A.",
""
],
[
"Guillarte",
"J. Mateos",
""
],
[
"Rees",
"M.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | We find a spectral wall in collisions of two vortices in the Abelian Higgs model at the critical coupling. It occurs if the out-of-phase mode of initially separated vortices is excited. | 17.953875 | 9.329647 | 12.81608 | 12.193063 | 10.506832 | 10.533254 | 11.856993 | 10.307753 | 12.004195 | 15.333801 | 11.932895 | 13.564554 | 14.472238 | 14.685633 | 14.285033 | 14.277471 | 12.992957 | 13.542535 | 12.829508 | 14.608555 | 14.051851 |
1609.01943 | Ahmad Ghodsi | Ahmad Ghodsi and Ghadir Jafari | Gravitational Couplings on D-brane Revisited | 15 pages | null | 10.1007/JHEP11(2016)161 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gravitational couplings in bulk space-time include those terms which are
fixed by scattering amplitude of strings and ambiguous terms that are coming
from the field redefinitions. These field redefinitions can be fixed in the
bulk by ghost-free condition. In this paper we have revised the effective
gravitational coup... | [
{
"created": "Wed, 7 Sep 2016 11:29:52 GMT",
"version": "v1"
}
] | 2016-11-29 | [
[
"Ghodsi",
"Ahmad",
""
],
[
"Jafari",
"Ghadir",
""
]
] | Gravitational couplings in bulk space-time include those terms which are fixed by scattering amplitude of strings and ambiguous terms that are coming from the field redefinitions. These field redefinitions can be fixed in the bulk by ghost-free condition. In this paper we have revised the effective gravitational coupli... | 16.804884 | 12.948721 | 14.537189 | 12.716478 | 13.440603 | 13.483345 | 12.869881 | 14.473376 | 12.734012 | 16.920967 | 13.184891 | 13.182611 | 14.814194 | 13.795191 | 13.681871 | 13.707244 | 13.210749 | 13.802666 | 13.197052 | 14.890766 | 13.075746 |
1412.4127 | Miguel Paulos | Miguel F. Paulos | JuliBootS: a hands-on guide to the conformal bootstrap | 29 pages | null | null | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce {\tt JuliBootS}, a package for numerical conformal bootstrap
computations coded in {\tt Julia}. The centre-piece of {\tt JuliBootS} is an
implementation of Dantzig's simplex method capable of handling arbitrary
precision linear programming problems with continuous search spaces. Current
supported feature... | [
{
"created": "Fri, 12 Dec 2014 21:03:49 GMT",
"version": "v1"
}
] | 2014-12-16 | [
[
"Paulos",
"Miguel F.",
""
]
] | We introduce {\tt JuliBootS}, a package for numerical conformal bootstrap computations coded in {\tt Julia}. The centre-piece of {\tt JuliBootS} is an implementation of Dantzig's simplex method capable of handling arbitrary precision linear programming problems with continuous search spaces. Current supported features ... | 16.556984 | 18.676266 | 17.801224 | 15.723554 | 16.504959 | 19.357277 | 17.0509 | 17.357504 | 16.195829 | 18.05452 | 16.013727 | 15.356111 | 14.767232 | 14.636906 | 15.178281 | 14.229734 | 15.525275 | 15.085639 | 15.160278 | 15.165614 | 15.773571 |
2211.10136 | Matthias Blau | Matthias Blau, Mbambu Kakona, George Thompson | 3 Definitions of BF Theory on Homology 3-Spheres | 48 pages | null | 10.1007/JHEP04(2023)146 | null | hep-th math.GT | http://creativecommons.org/licenses/by/4.0/ | 3-dimensional BF theory with gauge group $G$ (= Chern-Simons theory with
non-compact gauge group $TG$) is a deceptively simple yet subtle topological
gauge theory. Formally, its partition function is a sum/integral over the
moduli space $\mathcal{M}$ of flat connections, weighted by the Ray-Singer
torsion. In practic... | [
{
"created": "Fri, 18 Nov 2022 10:30:57 GMT",
"version": "v1"
}
] | 2023-05-17 | [
[
"Blau",
"Matthias",
""
],
[
"Kakona",
"Mbambu",
""
],
[
"Thompson",
"George",
""
]
] | 3-dimensional BF theory with gauge group $G$ (= Chern-Simons theory with non-compact gauge group $TG$) is a deceptively simple yet subtle topological gauge theory. Formally, its partition function is a sum/integral over the moduli space $\mathcal{M}$ of flat connections, weighted by the Ray-Singer torsion. In practice,... | 9.557476 | 9.554351 | 10.150922 | 8.800497 | 9.763233 | 9.640599 | 10.081546 | 9.232355 | 9.212287 | 10.291717 | 8.6445 | 8.589433 | 9.097277 | 8.557754 | 8.795421 | 8.539343 | 8.606519 | 8.838859 | 8.497506 | 8.741669 | 8.809029 |
1103.5470 | Andrei Mironov | A.Mironov, A.Morozov, A.Popolitov and Sh.Shakirov | Resolvents and Seiberg-Witten representation for Gaussian beta-ensemble | 15 pages | Theor.Math.Phys.171 (2012) 505-522; Teor.Mat.Fiz.171 (2012) 96-115 | 10.1007/s11232-012-0049-y | FIAN/TD-03/11; ITEP/TH-07/11 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The exact free energy of matrix model always obeys the Seiberg-Witten (SW)
equations on a complex curve defined by singularities of the quasiclassical
resolvent. The role of SW differential is played by the exact one-point
resolvent. We show that these properties are preserved in generalization of
matrix models to be... | [
{
"created": "Mon, 28 Mar 2011 20:09:19 GMT",
"version": "v1"
},
{
"created": "Tue, 17 May 2011 13:58:49 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
],
[
"Popolitov",
"A.",
""
],
[
"Shakirov",
"Sh.",
""
]
] | The exact free energy of matrix model always obeys the Seiberg-Witten (SW) equations on a complex curve defined by singularities of the quasiclassical resolvent. The role of SW differential is played by the exact one-point resolvent. We show that these properties are preserved in generalization of matrix models to beta... | 13.128526 | 12.24258 | 15.49762 | 13.033547 | 11.124502 | 11.674505 | 12.460578 | 11.944212 | 12.130466 | 17.389448 | 11.412385 | 12.232371 | 14.007964 | 12.893778 | 12.56753 | 12.889855 | 12.41252 | 12.973894 | 12.61206 | 14.447636 | 12.433505 |
1709.00850 | Roberto Bonezzi | Roberto Bonezzi | Induced Action for Conformal Higher Spins from Worldline Path Integrals | 24 pages, references added, minor typos corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Conformal higher spin (CHS) fields, despite being non unitary, provide a
remarkable example of a consistent interacting higher spin theory in flat space
background, that is local to all orders. The non-linear action is defined as
the logarithmically UV divergent part of a one-loop scalar effective action. In
this pap... | [
{
"created": "Mon, 4 Sep 2017 08:00:32 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Nov 2017 13:30:24 GMT",
"version": "v2"
}
] | 2017-11-30 | [
[
"Bonezzi",
"Roberto",
""
]
] | Conformal higher spin (CHS) fields, despite being non unitary, provide a remarkable example of a consistent interacting higher spin theory in flat space background, that is local to all orders. The non-linear action is defined as the logarithmically UV divergent part of a one-loop scalar effective action. In this paper... | 11.582102 | 11.347614 | 13.214545 | 10.361306 | 11.364265 | 11.71762 | 11.479483 | 10.162441 | 9.817833 | 12.556505 | 10.91723 | 10.529613 | 10.736223 | 10.053679 | 10.51023 | 10.199818 | 10.258131 | 10.580635 | 10.354804 | 10.623369 | 9.863048 |
hep-th/0503063 | Steven Gratton | Steven Gratton and Neil Turok | Langevin Analysis of Eternal Inflation | 22 pages, 2 figures | Phys.Rev. D72 (2005) 043507 | 10.1103/PhysRevD.72.043507 | null | hep-th astro-ph gr-qc | null | It has been widely claimed that inflation is generically eternal to the
future, even in models where the inflaton potential monotonically increases
away from its minimum. The idea is that quantum fluctuations allow the field to
jump uphill, thereby continually revitalizing the inflationary process in some
regions. In... | [
{
"created": "Mon, 7 Mar 2005 16:19:30 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Gratton",
"Steven",
""
],
[
"Turok",
"Neil",
""
]
] | It has been widely claimed that inflation is generically eternal to the future, even in models where the inflaton potential monotonically increases away from its minimum. The idea is that quantum fluctuations allow the field to jump uphill, thereby continually revitalizing the inflationary process in some regions. In t... | 11.817828 | 13.735513 | 12.839426 | 12.310101 | 13.382484 | 13.65345 | 13.844007 | 13.216858 | 12.798035 | 14.409778 | 11.166471 | 11.406855 | 11.515579 | 11.108099 | 11.219725 | 11.242043 | 11.555017 | 11.252027 | 11.274838 | 11.165239 | 10.956382 |
hep-th/9903007 | Paolo Di Vecchia | Paolo Di Vecchia | An introduction to AdS/CFT correspondence | 7 pages, Latex (Talk given at the 32nd International Symposium on the
Theory of Elementary Particles, Buckow (Germany), Sept. 1-5, 1998) | Fortsch.Phys.48:87-92,2000 | 10.1002/(SICI)1521-3978(20001)48:1/3<87::AID-PROP87>3.0.CO;2-S | Nordita-99/14 HE | hep-th | null | This is an introduction to the Maldacena conjecture on the equivalence
between ${\cal{N}}=4$ super Yang-Mills in Minkowski space-time and type IIB
string theory compactified on $AdS_5 \otimes S_5 $.
| [
{
"created": "Sun, 28 Feb 1999 17:10:31 GMT",
"version": "v1"
}
] | 2017-04-26 | [
[
"Di Vecchia",
"Paolo",
""
]
] | This is an introduction to the Maldacena conjecture on the equivalence between ${\cal{N}}=4$ super Yang-Mills in Minkowski space-time and type IIB string theory compactified on $AdS_5 \otimes S_5 $. | 4.592027 | 3.484866 | 3.952622 | 3.790195 | 4.051392 | 3.944895 | 3.680877 | 3.566029 | 3.922372 | 4.015044 | 3.621123 | 3.844864 | 3.700422 | 3.885177 | 4.047292 | 3.847512 | 3.896151 | 3.858229 | 3.81078 | 4.014731 | 3.91408 |
2203.14449 | Zhang Yaobo | Bo Feng, Tingfei Li, Hongbin Wang, Yaobo Zhang | Reduction of General One-loop Integrals Using Auxiliary Vector | 24 pages,no figures | null | 10.1007/JHEP05(2022)065 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As a key method to deal with loop integrals, Integration-By-Parts (IBP)
method can be used to do reduction as well as establish the differential
equations for master integrals. However, when talking about tensor reduction,
the Passarino-Veltman (PV) reduction method is also widely used for one-loop
integrals. Recentl... | [
{
"created": "Mon, 28 Mar 2022 02:15:38 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Mar 2022 05:07:49 GMT",
"version": "v2"
},
{
"created": "Sun, 17 Apr 2022 16:32:54 GMT",
"version": "v3"
}
] | 2022-06-01 | [
[
"Feng",
"Bo",
""
],
[
"Li",
"Tingfei",
""
],
[
"Wang",
"Hongbin",
""
],
[
"Zhang",
"Yaobo",
""
]
] | As a key method to deal with loop integrals, Integration-By-Parts (IBP) method can be used to do reduction as well as establish the differential equations for master integrals. However, when talking about tensor reduction, the Passarino-Veltman (PV) reduction method is also widely used for one-loop integrals. Recently,... | 9.95872 | 10.619416 | 9.338963 | 8.619822 | 9.427985 | 9.762962 | 10.225553 | 9.128016 | 8.845644 | 10.062846 | 9.636447 | 9.248403 | 9.090618 | 9.216227 | 9.241775 | 9.39102 | 9.021615 | 9.608259 | 9.150703 | 9.424397 | 9.332798 |
2307.03573 | Roberto Emparan | Nejc \v{C}eplak, Roberto Emparan, Andrea Puhm, Marija Toma\v{s}evi\'c | The correspondence between rotating black holes and fundamental strings | 48 pages, 11 figures. v2: 50 pages, 11 figures. Added discussion of
ensembles in the correspondence and other smaller improvements. v3: published
version | JHEP 11 (2023) 226 | 10.1007/JHEP11(2023)226 | CPHT-RR037.072023 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The correspondence principle between strings and black holes is a general
framework for matching black holes and massive states of fundamental strings at
a point where their physical properties (such as mass, entropy and temperature)
smoothly agree with each other. This correspondence becomes puzzling when
attempting... | [
{
"created": "Fri, 7 Jul 2023 13:07:47 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Sep 2023 04:28:33 GMT",
"version": "v2"
},
{
"created": "Sun, 3 Dec 2023 19:07:15 GMT",
"version": "v3"
}
] | 2023-12-05 | [
[
"Čeplak",
"Nejc",
""
],
[
"Emparan",
"Roberto",
""
],
[
"Puhm",
"Andrea",
""
],
[
"Tomašević",
"Marija",
""
]
] | The correspondence principle between strings and black holes is a general framework for matching black holes and massive states of fundamental strings at a point where their physical properties (such as mass, entropy and temperature) smoothly agree with each other. This correspondence becomes puzzling when attempting t... | 13.840362 | 14.246155 | 14.663726 | 13.090569 | 14.260257 | 14.002771 | 13.152787 | 13.394812 | 13.317331 | 14.089204 | 13.118276 | 12.913587 | 13.278996 | 12.945276 | 13.26009 | 12.922882 | 13.290595 | 13.000126 | 13.146379 | 13.475268 | 13.514132 |
0807.2314 | Romanczukiewicz Tomasz | Tomasz Romanczukiewicz | Negative radiation pressure in case of two interacting fields | 15 pages, 6 figures | Acta Phys.Polon.B39:3449-3462,2008 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a simple toy model, which although probably does not have any direct
physical applications, can serve as a nice pedagogical example for explanation
strange phenomenon of negative radiation pressure and can also give some
insight for understanding the interaction between radiation and a vortex. The
model disc... | [
{
"created": "Tue, 15 Jul 2008 07:32:00 GMT",
"version": "v1"
}
] | 2008-12-19 | [
[
"Romanczukiewicz",
"Tomasz",
""
]
] | We study a simple toy model, which although probably does not have any direct physical applications, can serve as a nice pedagogical example for explanation strange phenomenon of negative radiation pressure and can also give some insight for understanding the interaction between radiation and a vortex. The model discus... | 12.291966 | 11.565894 | 11.049343 | 11.154592 | 11.135855 | 13.478318 | 11.819166 | 11.756825 | 11.316525 | 11.286783 | 11.347585 | 10.686756 | 10.83811 | 10.360782 | 10.368539 | 10.674322 | 11.088855 | 10.605176 | 10.907853 | 10.660489 | 11.081873 |
hep-th/0604149 | Manoel Messias Ferreira Junior | H. Belich, T. Costa-Soares, M.M. Ferreira Jr., J.A. Helayel-Neto, and
F. M. O. Mouchereck | Lorentz-violating corrections on the hydrogen spectrum induced by a
non-minimal coupling | 7 pages, revtex style, no figures | Phys.Rev. D74 (2006) 065009 | 10.1103/PhysRevD.74.065009 | null | hep-th | null | The influence of a Lorentz-violating fixed background on fermions is
considered by means of a torsion-free non-minimal coupling. The
non-relativistic regime is assessed and the Lorentz-violating Hamiltonian is
determined. The effect of this Hamiltonian on the hydrogen spectrum is
determined to first-order evaluation ... | [
{
"created": "Thu, 20 Apr 2006 22:52:38 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Belich",
"H.",
""
],
[
"Costa-Soares",
"T.",
""
],
[
"Ferreira",
"M. M.",
"Jr."
],
[
"Helayel-Neto",
"J. A.",
""
],
[
"Mouchereck",
"F. M. O.",
""
]
] | The influence of a Lorentz-violating fixed background on fermions is considered by means of a torsion-free non-minimal coupling. The non-relativistic regime is assessed and the Lorentz-violating Hamiltonian is determined. The effect of this Hamiltonian on the hydrogen spectrum is determined to first-order evaluation (i... | 10.2941 | 8.739187 | 9.978054 | 9.036399 | 9.209746 | 9.114021 | 8.995113 | 8.798951 | 9.019047 | 9.952626 | 9.318439 | 9.689992 | 9.681616 | 9.678055 | 9.838113 | 9.836473 | 9.362903 | 9.782173 | 9.409203 | 9.533144 | 9.594794 |
1807.11540 | Martin Schvellinger | Nicolas Kovensky, Gustavo Michalski and Martin Schvellinger | Deep inelastic scattering from polarized spin-$1/2$ hadrons at low $x$
from string theory | 39 pages, 8 figures | null | 10.1007/JHEP10(2018)084 | null | hep-th hep-ex hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study polarized deep inelastic scattering of charged leptons from
spin-$1/2$ hadrons at low values of the Bjorken parameter and large 't Hooft
coupling in terms of the gauge/string theory duality. We calculate the
structure functions from type IIB superstring theory scattering amplitudes. We
discuss the role of th... | [
{
"created": "Mon, 30 Jul 2018 19:30:00 GMT",
"version": "v1"
}
] | 2018-11-14 | [
[
"Kovensky",
"Nicolas",
""
],
[
"Michalski",
"Gustavo",
""
],
[
"Schvellinger",
"Martin",
""
]
] | We study polarized deep inelastic scattering of charged leptons from spin-$1/2$ hadrons at low values of the Bjorken parameter and large 't Hooft coupling in terms of the gauge/string theory duality. We calculate the structure functions from type IIB superstring theory scattering amplitudes. We discuss the role of the ... | 8.629946 | 8.243322 | 8.488175 | 7.653913 | 8.228955 | 8.349166 | 7.738205 | 8.139333 | 7.777634 | 9.353945 | 7.762658 | 8.423738 | 8.31632 | 8.078297 | 7.94767 | 8.615263 | 8.007698 | 8.298174 | 7.975036 | 8.224134 | 8.367308 |
1210.0201 | Federico Piazza | Giulia Gubitosi, Federico Piazza and Filippo Vernizzi | The Effective Field Theory of Dark Energy | 39 pages; typos corrected and clarifications added; matches the JCAP
version | null | 10.1088/1475-7516/2013/02/032 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a universal description of dark energy and modified gravity that
includes all single-field models. By extending a formalism previously applied
to inflation, we consider the metric universally coupled to matter fields and
we write in terms of it the most general unitary gauge action consistent with
the resi... | [
{
"created": "Sun, 30 Sep 2012 13:54:32 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Feb 2013 21:28:56 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Gubitosi",
"Giulia",
""
],
[
"Piazza",
"Federico",
""
],
[
"Vernizzi",
"Filippo",
""
]
] | We propose a universal description of dark energy and modified gravity that includes all single-field models. By extending a formalism previously applied to inflation, we consider the metric universally coupled to matter fields and we write in terms of it the most general unitary gauge action consistent with the residu... | 8.539703 | 9.159019 | 9.878077 | 8.937559 | 10.154806 | 9.948588 | 10.686331 | 9.327085 | 9.546522 | 10.576895 | 9.53436 | 9.326378 | 9.031006 | 8.991214 | 9.550834 | 9.049397 | 9.436782 | 9.257721 | 8.757463 | 9.233663 | 8.855992 |
1310.5152 | Rakibur Rahman | Marc Henneaux, Gustavo Lucena Gomez and Rakibur Rahman | Gravitational Interactions of Higher-Spin Fermions | typos corrected, published in JHEP | null | 10.1007/JHEP01(2014)087 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the cubic interactions of a massless higher-spin fermion with
gravity in flat space and present covariant 2-s-s vertices, compatible with the
gauge symmetries of the system, preserving parity. This explicit construction
relies on the BRST deformation scheme that assumes locality and Poincare
invariance... | [
{
"created": "Fri, 18 Oct 2013 20:01:24 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Sep 2014 15:13:38 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Henneaux",
"Marc",
""
],
[
"Gomez",
"Gustavo Lucena",
""
],
[
"Rahman",
"Rakibur",
""
]
] | We investigate the cubic interactions of a massless higher-spin fermion with gravity in flat space and present covariant 2-s-s vertices, compatible with the gauge symmetries of the system, preserving parity. This explicit construction relies on the BRST deformation scheme that assumes locality and Poincare invariance. ... | 18.90802 | 16.841724 | 20.844416 | 16.615236 | 17.981373 | 16.256912 | 18.054358 | 17.560839 | 16.445337 | 21.606569 | 17.594839 | 17.943249 | 18.393442 | 17.274624 | 18.026646 | 17.990549 | 17.426748 | 17.028452 | 17.810669 | 19.237532 | 17.374748 |
1306.5488 | David Turton | Samir D. Mathur, David Turton | The flaw in the firewall argument | 52 pages, 13 figures, v3: comments on Rindler space added, references
added | Nucl. Phys. B 884 (2014) 566 | 10.1016/j.nuclphysb.2014.05.012 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A lot of confusion surrounds the issue of black hole complementarity, because
the question has been considered without discussing the mechanism which
guarantees unitarity. Considering such a mechanism leads to the following: (1)
The Hawking quanta with energy E of order the black hole temperature T carry
information,... | [
{
"created": "Sun, 23 Jun 2013 23:41:38 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Nov 2013 20:54:04 GMT",
"version": "v2"
},
{
"created": "Wed, 28 May 2014 19:18:57 GMT",
"version": "v3"
}
] | 2014-05-29 | [
[
"Mathur",
"Samir D.",
""
],
[
"Turton",
"David",
""
]
] | A lot of confusion surrounds the issue of black hole complementarity, because the question has been considered without discussing the mechanism which guarantees unitarity. Considering such a mechanism leads to the following: (1) The Hawking quanta with energy E of order the black hole temperature T carry information, a... | 14.953161 | 14.827328 | 16.921062 | 14.512214 | 15.749371 | 15.82675 | 16.461231 | 15.313076 | 14.911538 | 16.611897 | 13.959302 | 14.065332 | 15.073466 | 14.642193 | 14.422603 | 14.413433 | 14.756551 | 14.42018 | 14.410661 | 14.896249 | 14.630768 |
hep-th/9809180 | Yuji Ohta | Yuji Ohta (Res. Inst. Math. Sci., Kyoto Univ.) | Differential Equations for Scaling Relation in N=2 Supersymmetric SU(2)
Yang-Mills Theory Coupled with Massive Hypermultiplet | revtex | J.Math.Phys. 40 (1999) 1891-1900 | 10.1063/1.532839 | null | hep-th | null | Differential equations for scaling relation of prepotential in N=2
supersymmetric SU(2) Yang-Mills theory coupled with massive matter
hypermultiplet are proposed and are explicitly demonstrated in one flavour
($N_f =1$) theory. By applying Whitham dynamics, the first order derivative of
the prepotential over the $T_0... | [
{
"created": "Fri, 25 Sep 1998 10:01:25 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Feb 1999 06:47:00 GMT",
"version": "v2"
},
{
"created": "Mon, 31 May 1999 12:10:21 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Ohta",
"Yuji",
"",
"Res. Inst. Math. Sci., Kyoto Univ."
]
] | Differential equations for scaling relation of prepotential in N=2 supersymmetric SU(2) Yang-Mills theory coupled with massive matter hypermultiplet are proposed and are explicitly demonstrated in one flavour ($N_f =1$) theory. By applying Whitham dynamics, the first order derivative of the prepotential over the $T_0$ ... | 10.59211 | 10.31332 | 10.874872 | 8.991293 | 9.980597 | 10.617841 | 9.485096 | 9.740259 | 9.450952 | 11.84481 | 9.563232 | 8.897642 | 9.961016 | 9.331848 | 8.927202 | 8.7892 | 8.763218 | 8.825803 | 9.068848 | 9.944745 | 8.927967 |
1610.08063 | Shira Chapman Ms. | Shira Chapman, Hugo Marrochio and Robert C. Myers | Complexity of Formation in Holography | 37+32 pages, 24 figures; v2 - added appendix (Insights from MERA),
added references, corrected typos | JHEP 1701 (2017) 062 | 10.1007/JHEP01(2017)062 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was recently conjectured that the quantum complexity of a holographic
boundary state can be computed by evaluating the gravitational action on a bulk
region known as the Wheeler-DeWitt patch. We apply this complexity=action
duality to evaluate the `complexity of formation' (arXiv:1509.07876,
arXiv:1512.04993), i.e... | [
{
"created": "Tue, 25 Oct 2016 20:00:09 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Nov 2016 03:20:25 GMT",
"version": "v2"
}
] | 2017-06-15 | [
[
"Chapman",
"Shira",
""
],
[
"Marrochio",
"Hugo",
""
],
[
"Myers",
"Robert C.",
""
]
] | It was recently conjectured that the quantum complexity of a holographic boundary state can be computed by evaluating the gravitational action on a bulk region known as the Wheeler-DeWitt patch. We apply this complexity=action duality to evaluate the `complexity of formation' (arXiv:1509.07876, arXiv:1512.04993), i.e.,... | 6.109823 | 6.566931 | 6.683361 | 5.517885 | 5.873653 | 6.507865 | 6.152807 | 6.080937 | 6.318508 | 7.903056 | 5.794141 | 5.558946 | 5.938421 | 5.283644 | 5.154846 | 5.486107 | 5.412367 | 5.503996 | 5.450257 | 5.812299 | 5.555443 |
hep-th/0506184 | Pavel Kovtun | Pavel K. Kovtun and Andrei O. Starinets | Quasinormal modes and holography | 28 pages; v2: typos fixed, ref. added | Phys.Rev.D72:086009,2005 | 10.1103/PhysRevD.72.086009 | NSF-KITP-05-41 | hep-th gr-qc hep-ph | null | Quasinormal frequencies of electromagnetic and gravitational perturbations in
asymptotically AdS spacetime can be identified with poles of the corresponding
real-time Green's functions in a holographically dual finite temperature field
theory. The quasinormal modes are defined for gauge-invariant quantities which
obe... | [
{
"created": "Wed, 22 Jun 2005 03:13:27 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Oct 2005 02:37:22 GMT",
"version": "v2"
}
] | 2009-07-09 | [
[
"Kovtun",
"Pavel K.",
""
],
[
"Starinets",
"Andrei O.",
""
]
] | Quasinormal frequencies of electromagnetic and gravitational perturbations in asymptotically AdS spacetime can be identified with poles of the corresponding real-time Green's functions in a holographically dual finite temperature field theory. The quasinormal modes are defined for gauge-invariant quantities which obey ... | 5.783437 | 5.862392 | 6.026406 | 5.593254 | 5.196013 | 5.304048 | 5.522341 | 5.220238 | 5.182659 | 7.044787 | 5.515165 | 5.254089 | 5.548128 | 5.433978 | 5.49822 | 5.280985 | 5.36162 | 5.439873 | 5.634343 | 5.43804 | 5.485595 |
0811.3624 | Michael Kiermaier | Henriette Elvang (IAS), Daniel Z. Freedman (MIT), Michael Kiermaier
(MIT) | Proof of the MHV vertex expansion for all tree amplitudes in N=4 SYM
theory | 40 pages, 7 figures | JHEP 0906:068,2009 | 10.1088/1126-6708/2009/06/068 | MIT-CTP-4000, UUITP-26/08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove the MHV vertex expansion for all tree amplitudes of N=4 SYM theory.
The proof uses a shift acting on all external momenta, and we show that every
N^kMHV tree amplitude falls off as 1/z^k, or faster, for large z under this
shift. The MHV vertex expansion allows us to derive compact and efficient
generating fu... | [
{
"created": "Fri, 21 Nov 2008 20:00:30 GMT",
"version": "v1"
}
] | 2009-07-22 | [
[
"Elvang",
"Henriette",
"",
"IAS"
],
[
"Freedman",
"Daniel Z.",
"",
"MIT"
],
[
"Kiermaier",
"Michael",
"",
"MIT"
]
] | We prove the MHV vertex expansion for all tree amplitudes of N=4 SYM theory. The proof uses a shift acting on all external momenta, and we show that every N^kMHV tree amplitude falls off as 1/z^k, or faster, for large z under this shift. The MHV vertex expansion allows us to derive compact and efficient generating func... | 7.616806 | 7.270433 | 7.754678 | 7.100944 | 7.014938 | 6.949569 | 6.307391 | 7.033509 | 6.666425 | 7.635237 | 6.744283 | 6.843734 | 7.519058 | 7.051888 | 7.108708 | 7.167164 | 7.130951 | 7.288045 | 6.959193 | 7.19358 | 7.111687 |
2207.13996 | Xuan Li | Xuan Li, Yuan-Chun Jing, Fu-Zhong Yang | D-brane Superpotentials and Geometric Invariants in Complete
Intersection Calabi-Yau Manifolds | 29 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By blowing up the ambient space along the curve wrapped by B-branes, we study
the brane superpotentials and Ooguri-Vafa invariants on complete intersections
Calabi-Yau threefolds. On the topological B-model side, B-brane superpotentials
are expressed in terms of the period integral of the blow-up manifolds. By
mirror... | [
{
"created": "Thu, 28 Jul 2022 10:28:18 GMT",
"version": "v1"
}
] | 2022-07-29 | [
[
"Li",
"Xuan",
""
],
[
"Jing",
"Yuan-Chun",
""
],
[
"Yang",
"Fu-Zhong",
""
]
] | By blowing up the ambient space along the curve wrapped by B-branes, we study the brane superpotentials and Ooguri-Vafa invariants on complete intersections Calabi-Yau threefolds. On the topological B-model side, B-brane superpotentials are expressed in terms of the period integral of the blow-up manifolds. By mirror m... | 8.29312 | 7.895031 | 9.548519 | 6.610212 | 8.35831 | 8.406893 | 7.465284 | 7.546851 | 7.29237 | 9.897216 | 7.02559 | 6.817498 | 8.473251 | 7.039701 | 7.218651 | 6.928686 | 7.566072 | 6.952841 | 7.215535 | 7.7277 | 6.958131 |
hep-th/9603156 | Vipul Periwal | Vipul Periwal and {\O}yvind Tafjord | D-brane recoil | Plain TeX, 5 pages | Phys.Rev.D54:3690-3692,1996 | 10.1103/PhysRevD.54.R3690 | PUPT-1607 | hep-th | null | It is shown that there are logarithmic operators in D-brane backgrounds that
lead to infrared divergences in open string loop amplitudes. These divergences
can be cancelled by changing the closed string background by operators that
correspond to the D-brane moving with constant velocity after some instant in
time, si... | [
{
"created": "Sat, 23 Mar 1996 18:02:25 GMT",
"version": "v1"
}
] | 2009-12-30 | [
[
"Periwal",
"Vipul",
""
],
[
"Tafjord",
"Øyvind",
""
]
] | It is shown that there are logarithmic operators in D-brane backgrounds that lead to infrared divergences in open string loop amplitudes. These divergences can be cancelled by changing the closed string background by operators that correspond to the D-brane moving with constant velocity after some instant in time, sinc... | 10.136537 | 9.725445 | 11.225911 | 9.327812 | 8.699082 | 9.031932 | 9.445128 | 7.969303 | 8.533332 | 12.167284 | 8.530137 | 8.90301 | 10.410868 | 9.178985 | 8.987396 | 9.346082 | 9.051171 | 9.220307 | 9.338393 | 10.400284 | 9.201299 |
1411.7987 | Paolo Benincasa | Paolo Benincasa, Eduardo Conde, David Gordo | On the Regularization of On-Shell Diagrams | 5 pages, 3 figures | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this letter we discuss a regularization scheme for the integration of
generic on-shell forms. The basic idea is to extend the three-particle
amplitudes to the space of unphysical helicities keeping the dimension of the
related coupling constant fixed, and construct on-shell forms out of them. We
briefly discuss th... | [
{
"created": "Fri, 28 Nov 2014 20:11:22 GMT",
"version": "v1"
}
] | 2014-12-01 | [
[
"Benincasa",
"Paolo",
""
],
[
"Conde",
"Eduardo",
""
],
[
"Gordo",
"David",
""
]
] | In this letter we discuss a regularization scheme for the integration of generic on-shell forms. The basic idea is to extend the three-particle amplitudes to the space of unphysical helicities keeping the dimension of the related coupling constant fixed, and construct on-shell forms out of them. We briefly discuss the ... | 13.128976 | 12.556927 | 13.482978 | 11.882117 | 12.958944 | 12.819555 | 13.542964 | 12.514147 | 12.12331 | 14.041304 | 12.599602 | 12.452135 | 12.621146 | 12.20668 | 12.505971 | 12.383818 | 12.541536 | 12.396324 | 12.39323 | 12.856338 | 12.095078 |
1412.1492 | Alfredo Perez | Claudio Bunster and Alfredo Perez | Superselection rule for the cosmological constant in three-dimensional
spacetime | 7 pages, 1 table | null | 10.1103/PhysRevD.91.024029 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Efforts to understand the origin of the cosmological constant {\Lambda} and
its observed value have led to consider it as a dynamical field rather than as
a universal constant. Then the possibility arises that the universe, or regions
of it, might be in a superposition of quantum states with different values of
{\Lam... | [
{
"created": "Wed, 3 Dec 2014 21:20:10 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Bunster",
"Claudio",
""
],
[
"Perez",
"Alfredo",
""
]
] | Efforts to understand the origin of the cosmological constant {\Lambda} and its observed value have led to consider it as a dynamical field rather than as a universal constant. Then the possibility arises that the universe, or regions of it, might be in a superposition of quantum states with different values of {\Lambd... | 8.758281 | 8.861197 | 8.20972 | 7.516778 | 8.535695 | 8.202182 | 8.780288 | 8.235525 | 7.757962 | 8.763799 | 8.023713 | 7.972572 | 7.848037 | 7.903563 | 7.971804 | 7.919653 | 8.170241 | 7.679196 | 8.174327 | 8.253653 | 8.051558 |
hep-th/0304093 | Sumit Das | Sumit R. Das and Antal Jevicki | Large-N Collective Fields and Holography | 27 pages, harvmac. v2: references added | Phys.Rev. D68 (2003) 044011 | 10.1103/PhysRevD.68.044011 | UK-03-04,Brown-HET-1350 | hep-th | null | We propose that the euclidean bilocal collective field theory of critical
large-N vector models provides a complete definition of the proposed dual
theory of higher spin fields in anti de-Sitter spaces. We show how this bilocal
field can be decomposed into an infinite number of even spin fields in one more
dimension.... | [
{
"created": "Wed, 9 Apr 2003 22:17:39 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Apr 2003 18:57:09 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Das",
"Sumit R.",
""
],
[
"Jevicki",
"Antal",
""
]
] | We propose that the euclidean bilocal collective field theory of critical large-N vector models provides a complete definition of the proposed dual theory of higher spin fields in anti de-Sitter spaces. We show how this bilocal field can be decomposed into an infinite number of even spin fields in one more dimension. T... | 13.922602 | 14.113367 | 15.841976 | 13.49087 | 14.725103 | 13.322428 | 14.06988 | 15.051018 | 13.790236 | 16.695099 | 14.694027 | 14.108159 | 14.018816 | 13.951527 | 14.449951 | 14.267722 | 14.217473 | 14.198817 | 14.16434 | 14.557295 | 13.956068 |
hep-th/9403030 | Daniel R. D. Scott | D.R.D. Scott | Classical Functional Bethe Ansatz for $SL(N)$: separation of variables
for the magnetic chain | 14pp LaTex,DAMTP 94-17 | J.Math.Phys. 35 (1994) 5831-5843 | 10.1063/1.530712 | null | hep-th | null | The Functional Bethe Ansatz (FBA) proposed by Sklyanin is a method which
gives separation variables for systems for which an $R$-matrix is known.
Previously the FBA was only known for $SL(2)$ and $SL(3)$ (and associated)
$R$-matrices. In this paper I advance Sklyanin's program by giving the FBA for
certain systems wi... | [
{
"created": "Fri, 4 Mar 1994 14:10:36 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Scott",
"D. R. D.",
""
]
] | The Functional Bethe Ansatz (FBA) proposed by Sklyanin is a method which gives separation variables for systems for which an $R$-matrix is known. Previously the FBA was only known for $SL(2)$ and $SL(3)$ (and associated) $R$-matrices. In this paper I advance Sklyanin's program by giving the FBA for certain systems with... | 7.19614 | 7.825173 | 8.743775 | 7.2644 | 7.103715 | 7.009767 | 7.482333 | 7.743834 | 7.287149 | 7.937106 | 7.086933 | 6.869809 | 7.258366 | 6.833903 | 6.780905 | 6.814395 | 6.880728 | 6.963531 | 6.904265 | 7.390831 | 6.719537 |
1809.01224 | Jos\'e M. Figueroa-O'Farrill | Jos\'e Figueroa-O'Farrill and Stefan Prohazka | Spatially isotropic homogeneous spacetimes | 51 pages, 6 figures, 17 tables. Updated references and corrected an
inconsequential error in Section 4.2.5 | null | 10.1007/JHEP01(2019)229 | EMPG-18-01 | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We classify simply-connected homogeneous ($D+1$)-dimensional spacetimes for
kinematical and aristotelian Lie groups with $D$-dimensional space isotropy for
all $D\geq 0$. Besides well-known spacetimes like Minkowski and (anti) de
Sitter we find several new classes of geometries, some of which exist only for
$D=1,2$. ... | [
{
"created": "Tue, 4 Sep 2018 19:57:31 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Jan 2019 21:49:05 GMT",
"version": "v2"
},
{
"created": "Wed, 8 May 2019 16:03:53 GMT",
"version": "v3"
},
{
"created": "Sun, 17 Oct 2021 18:58:54 GMT",
"version": "v4"
}
] | 2021-10-19 | [
[
"Figueroa-O'Farrill",
"José",
""
],
[
"Prohazka",
"Stefan",
""
]
] | We classify simply-connected homogeneous ($D+1$)-dimensional spacetimes for kinematical and aristotelian Lie groups with $D$-dimensional space isotropy for all $D\geq 0$. Besides well-known spacetimes like Minkowski and (anti) de Sitter we find several new classes of geometries, some of which exist only for $D=1,2$. Th... | 8.074324 | 7.34504 | 8.539084 | 7.567057 | 7.871209 | 7.469665 | 7.681047 | 7.686895 | 7.361147 | 9.424263 | 7.28457 | 7.683319 | 8.014955 | 7.69086 | 7.537045 | 7.808114 | 7.820663 | 7.729058 | 7.678297 | 8.132648 | 7.492415 |
hep-th/0508022 | Chang-Young Ee | Yong-Wan Kim, Ee Chang-Young, Seung-Kook Kim, Young-Jai Park | Improved BFT embedding having chain-structure | 15 pages, LaTeX file | Phys.Lett. B632 (2006) 427-432 | 10.1016/j.physletb.2005.10.028 | SOGANG-HEP 315/05 | hep-th | null | We newly revisit the gauge non-invariant chiral Schwinger model with a=1 in
view of the chain structure. As a result, we show that the Dirac brackets can
be easily read off from the exact symplectic algebra of second-class
constraints. Furthermore, by using an improved BFT embedding preserving the
chain structure, we... | [
{
"created": "Wed, 3 Aug 2005 08:01:09 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Sep 2005 05:33:31 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Kim",
"Yong-Wan",
""
],
[
"Chang-Young",
"Ee",
""
],
[
"Kim",
"Seung-Kook",
""
],
[
"Park",
"Young-Jai",
""
]
] | We newly revisit the gauge non-invariant chiral Schwinger model with a=1 in view of the chain structure. As a result, we show that the Dirac brackets can be easily read off from the exact symplectic algebra of second-class constraints. Furthermore, by using an improved BFT embedding preserving the chain structure, we o... | 16.064024 | 13.351338 | 20.191298 | 14.130499 | 12.683734 | 13.158941 | 12.925443 | 13.422644 | 12.843825 | 20.259037 | 13.678183 | 14.106256 | 15.871887 | 14.842947 | 13.797328 | 13.978725 | 13.421912 | 14.225607 | 14.964199 | 16.374697 | 14.547231 |
hep-th/0301227 | Stefano Bellucci | Stefano Bellucci | Constant magnetic field and 2d non-commutative inverted oscillator | 7 pages, LaTeX file, no figures, PACS number: 03.65.-w | Phys.Rev. D67 (2003) 105014 | 10.1103/PhysRevD.67.105014 | null | hep-th | null | We consider a two-dimensional non-commutative inverted oscillator in the
presence of a constant magnetic field, coupled to the system in a
``symplectic'' and ``Poisson'' way. We show that it has a discrete energy
spectrum for some value of the magnetic field.
| [
{
"created": "Tue, 28 Jan 2003 11:04:19 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Bellucci",
"Stefano",
""
]
] | We consider a two-dimensional non-commutative inverted oscillator in the presence of a constant magnetic field, coupled to the system in a ``symplectic'' and ``Poisson'' way. We show that it has a discrete energy spectrum for some value of the magnetic field. | 10.221603 | 7.571101 | 9.746185 | 8.2394 | 7.668553 | 7.814071 | 8.480974 | 7.579263 | 7.067471 | 10.708573 | 7.755071 | 8.875638 | 10.081704 | 8.867734 | 8.668472 | 8.904972 | 8.584996 | 8.516799 | 9.007896 | 9.604409 | 8.618182 |
1612.06385 | Daliang Li | A. Liam Fitzpatrick, Jared Kaplan, Daliang Li, and Junpu Wang | Exact Virasoro Blocks from Wilson Lines and Background-Independent
Operators | V3- Added some references V2- Significantly Expanded Appendix on
Regulation; 32+21 pages | null | 10.1007/JHEP07(2017)092 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Aspects of black hole thermodynamics and information loss can be derived as a
consequence of Virasoro symmetry. To bolster the connection between Virasoro
conformal blocks and AdS$_3$ quantum gravity, we study sl$(2)$ Chern-Simons
Wilson line networks and revisit the idea that they compute a variety of
CFT$_2$ observ... | [
{
"created": "Mon, 19 Dec 2016 21:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Apr 2017 15:28:44 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Sep 2017 19:52:16 GMT",
"version": "v3"
}
] | 2017-09-13 | [
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Kaplan",
"Jared",
""
],
[
"Li",
"Daliang",
""
],
[
"Wang",
"Junpu",
""
]
] | Aspects of black hole thermodynamics and information loss can be derived as a consequence of Virasoro symmetry. To bolster the connection between Virasoro conformal blocks and AdS$_3$ quantum gravity, we study sl$(2)$ Chern-Simons Wilson line networks and revisit the idea that they compute a variety of CFT$_2$ observab... | 10.419744 | 10.267213 | 11.960027 | 9.580064 | 10.3981 | 10.435883 | 10.130289 | 9.923259 | 10.363581 | 11.554271 | 9.62053 | 9.905025 | 10.473361 | 10.015082 | 9.965456 | 9.763968 | 9.821708 | 9.889663 | 9.759202 | 10.730145 | 9.934472 |
1507.02477 | Javier Magan | Javier M. Magan | Fast Scramblers, Democratic Walks and Information Fields | 43 pages, 1 figure | null | null | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a family of weighted random walks on complete graphs. These
`democratic walks' turn out to be explicitly solvable, and we find the
hierarchy window for which the characteristic time scale saturates the
so-called fast scrambling conjecture. We show that these democratic walks
describe well the properties of i... | [
{
"created": "Thu, 9 Jul 2015 12:18:52 GMT",
"version": "v1"
}
] | 2015-07-10 | [
[
"Magan",
"Javier M.",
""
]
] | We study a family of weighted random walks on complete graphs. These `democratic walks' turn out to be explicitly solvable, and we find the hierarchy window for which the characteristic time scale saturates the so-called fast scrambling conjecture. We show that these democratic walks describe well the properties of inf... | 20.340805 | 23.62315 | 21.872824 | 19.249962 | 20.712753 | 24.528187 | 21.535036 | 21.185326 | 19.105272 | 24.251423 | 19.149708 | 19.723454 | 18.813709 | 18.326723 | 18.487295 | 18.785723 | 19.479883 | 19.183451 | 18.356249 | 18.736172 | 18.439331 |
2207.14557 | Joachim Herrmann | Joachim Herrmann | Towards a unified theory of the fundamental physical interactions based
on the underlying geometric structure of the tangent bundle | 23 pages, no figures | Eur. Phys. J C 82, 947 (2022) | 10.1140/epjc/s10052-022-10781-4 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper pursues the hypothesis that the tangent bundle (TB) with the
central extended little groups of the SO(3,1) group as gauge group is the
underlying geometric structure for a unified theory of the fundamental physical
interactions. Based on this hypothesis as a first step recently I presented a
generalized th... | [
{
"created": "Fri, 29 Jul 2022 09:11:57 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Feb 2023 13:15:32 GMT",
"version": "v2"
}
] | 2023-02-27 | [
[
"Herrmann",
"Joachim",
""
]
] | This paper pursues the hypothesis that the tangent bundle (TB) with the central extended little groups of the SO(3,1) group as gauge group is the underlying geometric structure for a unified theory of the fundamental physical interactions. Based on this hypothesis as a first step recently I presented a generalized theo... | 11.627287 | 13.033895 | 12.245957 | 11.973613 | 12.683097 | 13.065014 | 13.668327 | 12.77637 | 12.143262 | 12.785607 | 11.785487 | 11.697902 | 11.476394 | 11.505592 | 11.359076 | 11.753712 | 11.609317 | 11.496648 | 11.664961 | 11.948302 | 11.476021 |
hep-th/0404210 | Pierre van Baal | Falk Bruckmann, Daniel Nogradi, Pierre van Baal | Higher charge calorons with non-trivial holonomy | 25 pages, 4 figures in 15 parts; small corrections - version to be
published | Nucl.Phys. B698 (2004) 233-254 | 10.1016/j.nuclphysb.2004.07.038 | null | hep-th hep-lat | null | The full ADHM-Nahm formalism is employed to find exact higher charge caloron
solutions with non-trivial holonomy, extended beyond the axially symmetric
solutions found earlier. Particularly interesting is the case where the
constituent monopoles, that make up these solutions, are not necessarily
well-separated. This ... | [
{
"created": "Tue, 27 Apr 2004 13:07:36 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Sep 2004 19:25:40 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Bruckmann",
"Falk",
""
],
[
"Nogradi",
"Daniel",
""
],
[
"van Baal",
"Pierre",
""
]
] | The full ADHM-Nahm formalism is employed to find exact higher charge caloron solutions with non-trivial holonomy, extended beyond the axially symmetric solutions found earlier. Particularly interesting is the case where the constituent monopoles, that make up these solutions, are not necessarily well-separated. This is... | 14.987075 | 13.718998 | 15.243771 | 12.921114 | 14.752573 | 14.252398 | 14.462383 | 13.730706 | 13.502263 | 15.24702 | 14.324022 | 13.566921 | 13.931294 | 13.976585 | 14.124337 | 13.721981 | 13.374638 | 13.905735 | 13.81905 | 14.060513 | 13.816169 |
hep-th/9804193 | Gleb E. Arutyunov | Yu. M. Zinoviev | On Wilson Criterion | latex, 6 pages | null | 10.1007/BF02557195 | null | hep-th | null | U(1) gauge theory with the Villain action on a cubic lattice approximation of
three- and four-dimensional torus is considered. The naturally chosen
correlation functions converge to the correlation functions of the R-gauge
electrodynamics on three- and four-dimensional torus as the lattice spacing
approaches zero onl... | [
{
"created": "Wed, 29 Apr 1998 09:17:54 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Zinoviev",
"Yu. M.",
""
]
] | U(1) gauge theory with the Villain action on a cubic lattice approximation of three- and four-dimensional torus is considered. The naturally chosen correlation functions converge to the correlation functions of the R-gauge electrodynamics on three- and four-dimensional torus as the lattice spacing approaches zero only ... | 14.003059 | 15.428318 | 15.271184 | 14.316415 | 15.594033 | 16.353796 | 16.414856 | 15.636741 | 14.855384 | 16.968479 | 14.746222 | 13.477178 | 14.337159 | 13.342213 | 13.456674 | 13.879416 | 13.543694 | 13.40601 | 13.66778 | 13.917324 | 14.023209 |
hep-th/9607150 | Akira Niegawa | A. Ni\'egawa | Screening of mass singularities and finite soft-photon production rate
in hot QCD | 41pages, Figures are not included | Phys.Rev.D56:1073-1090,1997 | 10.1103/PhysRevD.56.1073 | OCU-PHYS 160 | hep-th | null | The production rate of a soft photon from a hot quark-gluon plasma is
computed to leading order at logarithmic accuracy. The canonical
hard-thermal-loop resummation scheme leads to logarithmically divergent
production rate due to mass singularities. We show that these mass
singularities are screened by employing the ... | [
{
"created": "Thu, 18 Jul 1996 03:25:04 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Feb 1997 01:17:50 GMT",
"version": "v2"
}
] | 2016-08-15 | [
[
"Niégawa",
"A.",
""
]
] | The production rate of a soft photon from a hot quark-gluon plasma is computed to leading order at logarithmic accuracy. The canonical hard-thermal-loop resummation scheme leads to logarithmically divergent production rate due to mass singularities. We show that these mass singularities are screened by employing the ef... | 9.792604 | 9.714097 | 8.908561 | 8.326307 | 10.028795 | 9.964417 | 10.050352 | 9.862881 | 8.449507 | 9.745537 | 9.783073 | 9.797429 | 9.284833 | 8.928333 | 9.113053 | 9.457992 | 9.392872 | 9.557221 | 8.97872 | 9.129665 | 8.959142 |
hep-th/0209083 | null | H.Culetu (Ovidius University) | On the gravitational energy of the Hawking wormhole | 9 pages, chapter 4 removed, to appear in Int. Jour. Mod. Phys. A | Int.J.Mod.Phys. A18 (2003) 4251-4256 | 10.1142/S0217751X03016124 | null | hep-th | null | The surface energy for a conformally flat spacetime which represents the
Hawking wormhole in spherical (static) Rindler coordinates is computed using
the Hawking - Hunter formalism for non asymptotically - flat spacetimes.
The physical gravitational Hamiltonian is proportional to the Rindler
acceleration g of the h... | [
{
"created": "Tue, 10 Sep 2002 11:25:16 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Sep 2002 14:24:53 GMT",
"version": "v2"
},
{
"created": "Fri, 4 Jul 2003 11:21:55 GMT",
"version": "v3"
}
] | 2016-09-06 | [
[
"Culetu",
"H.",
"",
"Ovidius University"
]
] | The surface energy for a conformally flat spacetime which represents the Hawking wormhole in spherical (static) Rindler coordinates is computed using the Hawking - Hunter formalism for non asymptotically - flat spacetimes. The physical gravitational Hamiltonian is proportional to the Rindler acceleration g of the hyper... | 20.129065 | 23.311605 | 18.976154 | 18.108969 | 21.435352 | 20.526144 | 23.40925 | 17.909822 | 21.367949 | 18.292944 | 19.001282 | 19.599373 | 17.983265 | 18.020273 | 18.44492 | 18.370356 | 18.558435 | 16.516411 | 17.812241 | 17.850204 | 18.266863 |
2203.08087 | Yvonne Geyer | Giulia Albonico, Yvonne Geyer, Lionel Mason | From Twistor-Particle Models to Massive Amplitudes | null | SIGMA 18 (2022), 045, 21 pages | 10.3842/SIGMA.2022.045 | null | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by-sa/4.0/ | In his twistor-particle programme of the 1970's, Roger Penrose introduced a
representation of the massive particle phase space in terms of a pair of
twistors subject to an internal symmetry group. Here we use this representation
to introduce a chiral string whose target is a complexification of this space,
extended s... | [
{
"created": "Tue, 15 Mar 2022 17:15:38 GMT",
"version": "v1"
},
{
"created": "Sun, 19 Jun 2022 06:31:41 GMT",
"version": "v2"
}
] | 2022-06-22 | [
[
"Albonico",
"Giulia",
""
],
[
"Geyer",
"Yvonne",
""
],
[
"Mason",
"Lionel",
""
]
] | In his twistor-particle programme of the 1970's, Roger Penrose introduced a representation of the massive particle phase space in terms of a pair of twistors subject to an internal symmetry group. Here we use this representation to introduce a chiral string whose target is a complexification of this space, extended so ... | 13.863645 | 13.64848 | 14.284267 | 12.63888 | 14.721803 | 13.170467 | 13.616446 | 12.785305 | 13.421371 | 16.276264 | 13.014097 | 12.804627 | 13.353707 | 13.065799 | 13.190834 | 13.017991 | 13.056007 | 12.952257 | 12.978208 | 13.235195 | 13.125906 |
hep-th/0102074 | Harold Steinacker | Harold Steinacker | Aspects of the q-deformed Fuzzy Sphere | 5 pages. Talk presented at the Euroconference ``Brane New World and
Noncommutative Geometry'' in Villa Gualino, Torino, Italy, October 2 - 7,
2000 | Mod.Phys.Lett. A16 (2001) 361-366 | 10.1142/S0217732301003462 | null | hep-th math.QA | null | These notes are a short review of the q-deformed fuzzy sphere S^2_{q,N},
which is a ``finite'' noncommutative 2-sphere covariant under the quantum group
U_q(su(2)). We discuss its real structure, differential calculus and
integration for both real q and q a phase, and show how actions for Yang-Mills
and Chern- Simons... | [
{
"created": "Wed, 14 Feb 2001 12:30:04 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Steinacker",
"Harold",
""
]
] | These notes are a short review of the q-deformed fuzzy sphere S^2_{q,N}, which is a ``finite'' noncommutative 2-sphere covariant under the quantum group U_q(su(2)). We discuss its real structure, differential calculus and integration for both real q and q a phase, and show how actions for Yang-Mills and Chern- Simons-l... | 10.092173 | 8.466397 | 11.580532 | 7.952851 | 9.051685 | 8.783692 | 10.162094 | 7.603655 | 8.526501 | 12.781735 | 8.381032 | 8.63975 | 9.043978 | 8.276547 | 8.694086 | 8.658601 | 8.639173 | 8.435816 | 7.96525 | 9.707881 | 7.988339 |
hep-th/9503129 | Andreas Wisskirchen | Ralph Blumenhagen and Andreas Wisskirchen | A Note On ADE String Compactifications | 11 pages, plain TeX, no postscript figures | Phys.Lett. B355 (1995) 99-106 | 10.1016/0370-2693(95)00709-T | BONN-TH-95-05, IFP-504-UNC | hep-th | null | We address the question whether so-called m-invariants of the N=2 super
Virasoro algebra can be used for the construction of reasonable
four-dimensional string models. It turns out that an infinite subset of those
are pathological in the sense that - although N=2 supersymmetric - the Ramond
sector is not isomorphic t... | [
{
"created": "Tue, 21 Mar 1995 07:37:13 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Blumenhagen",
"Ralph",
""
],
[
"Wisskirchen",
"Andreas",
""
]
] | We address the question whether so-called m-invariants of the N=2 super Virasoro algebra can be used for the construction of reasonable four-dimensional string models. It turns out that an infinite subset of those are pathological in the sense that - although N=2 supersymmetric - the Ramond sector is not isomorphic to ... | 16.334433 | 18.586872 | 21.144442 | 15.820001 | 18.189623 | 16.063082 | 16.521141 | 16.898937 | 16.307129 | 18.979952 | 16.19973 | 16.058083 | 16.927822 | 15.375246 | 16.146673 | 14.950069 | 15.890088 | 15.752083 | 16.240005 | 16.013124 | 15.961082 |
1905.00434 | Jean-Fran\c{c}ois Fortin | Jean-Fran\c{c}ois Fortin, Witold Skiba | New Methods for Conformal Correlation Functions | 1+89 pages, 2 figures, extended discussion in Section 4, streamlined
notation in Sections 5 and 6, extra identities in Appendix B, added
references | null | 10.1007/JHEP06(2020)028 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The most general operator product expansion in conformal field theory is
obtained using the embedding space formalism and a new uplift for general
quasi-primary operators. The uplift introduced here, based on quasi-primary
operators with spinor indices only and standard projection operators, allows a
unified treatmen... | [
{
"created": "Wed, 1 May 2019 18:00:06 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Aug 2019 02:34:47 GMT",
"version": "v2"
}
] | 2020-07-15 | [
[
"Fortin",
"Jean-François",
""
],
[
"Skiba",
"Witold",
""
]
] | The most general operator product expansion in conformal field theory is obtained using the embedding space formalism and a new uplift for general quasi-primary operators. The uplift introduced here, based on quasi-primary operators with spinor indices only and standard projection operators, allows a unified treatment ... | 9.820338 | 10.727654 | 11.856548 | 10.041509 | 10.492489 | 10.487988 | 10.924861 | 10.402263 | 10.132502 | 12.05317 | 9.999445 | 10.146177 | 10.50937 | 10.098159 | 9.759188 | 9.724305 | 9.837766 | 9.885462 | 9.968443 | 10.55952 | 9.493597 |
1906.09053 | Aybike Ozer | Aybike \c{C}atal-\"Ozer and Se\c{c}il Tunal{\i} | Yang-Baxter Deformation as an O(d,d) Transformation | references added; revised Introduction; minor corrections; some of
the discussions clarified, section 4.3 on generalised supergravity equations
expanded, one reference added | Class. Quantum Grav. 37 (2020) 075003 | 10.1088/1361-6382/ab6f7e | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The rules for Yang-Baxter (YB) deformation for a generic Green-Schwarz string
sigma model has been obtained recently. We show that the deformation can be
described through the action of a coordinate dependent $O(d,d)$ matrix on the
target space fields both in the NS-NS and the RR sectors, generalizing previous
result... | [
{
"created": "Fri, 21 Jun 2019 10:38:06 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jul 2019 17:05:06 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Sep 2019 12:31:12 GMT",
"version": "v3"
},
{
"created": "Thu, 27 Feb 2020 08:01:43 GMT",
"version": "v4"
}
] | 2020-02-28 | [
[
"Çatal-Özer",
"Aybike",
""
],
[
"Tunalı",
"Seçil",
""
]
] | The rules for Yang-Baxter (YB) deformation for a generic Green-Schwarz string sigma model has been obtained recently. We show that the deformation can be described through the action of a coordinate dependent $O(d,d)$ matrix on the target space fields both in the NS-NS and the RR sectors, generalizing previous results.... | 7.553072 | 7.241679 | 8.592013 | 6.945851 | 7.525675 | 7.650655 | 7.82297 | 7.593658 | 7.630819 | 9.373378 | 7.188828 | 7.556213 | 7.793482 | 7.336611 | 7.654831 | 7.274196 | 7.63677 | 7.412069 | 7.616822 | 7.838547 | 7.353741 |
hep-th/0005002 | Makoto Natsuume | Masako Asano (Univ. of Tokyo, Hongo) and Makoto Natsuume (KEK) | The no-ghost theorem for string theory in curved backgrounds with a flat
timelike direction | 25 pages, AMS-LaTeX; v2: added discussion on the extension of our
results and on earlier works, minor corrections | Nucl.Phys. B588 (2000) 453-470 | 10.1016/S0550-3213(00)00495-8 | KEK-TH-688, UT-886 | hep-th | null | It is well-known that the standard no-ghost theorem can be extended
straightforwardly to the general c=26 CFT on R^{d-1,1} \times K, where 2 \leq d
\leq 26 and K is a compact unitary CFT of appropriate central charge. We prove
the no-ghost theorem for d=1, i.e., when only the timelike direction is flat.
This is done ... | [
{
"created": "Sat, 29 Apr 2000 14:52:59 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jul 2000 10:25:40 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Asano",
"Masako",
"",
"Univ. of Tokyo, Hongo"
],
[
"Natsuume",
"Makoto",
"",
"KEK"
]
] | It is well-known that the standard no-ghost theorem can be extended straightforwardly to the general c=26 CFT on R^{d-1,1} \times K, where 2 \leq d \leq 26 and K is a compact unitary CFT of appropriate central charge. We prove the no-ghost theorem for d=1, i.e., when only the timelike direction is flat. This is done us... | 7.792848 | 6.936299 | 9.336473 | 6.429266 | 6.56706 | 6.047178 | 6.592953 | 6.768777 | 6.658962 | 9.293463 | 6.244311 | 6.8922 | 7.59203 | 6.531168 | 6.617033 | 6.422709 | 6.711872 | 7.145508 | 6.667021 | 7.317123 | 6.660292 |
1807.07763 | Bruno Bertrand Dr | Bruno Bertrand and Jan Govaerts | Mass Generation in Abelian U(1) Gauge Theories: A Rich Network of
Dualities | 11 pages, 2 figures | null | 10.1063/1.5109628 | CP3-18-40 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Following a novel approach, all known basic mass generation mechanisms
consistent with an exact abelian U(1) gauge symmetry are shown to be related
through an intricate network of dualities whatever the spacetime dimension.
This equivalence which applies in the absence of any supersymmetry, is however
restricted by t... | [
{
"created": "Fri, 20 Jul 2018 10:10:09 GMT",
"version": "v1"
}
] | 2020-01-08 | [
[
"Bertrand",
"Bruno",
""
],
[
"Govaerts",
"Jan",
""
]
] | Following a novel approach, all known basic mass generation mechanisms consistent with an exact abelian U(1) gauge symmetry are shown to be related through an intricate network of dualities whatever the spacetime dimension. This equivalence which applies in the absence of any supersymmetry, is however restricted by the... | 16.442291 | 16.498692 | 17.409691 | 15.848032 | 16.78293 | 17.207684 | 15.806361 | 16.082458 | 15.149409 | 17.618465 | 15.060432 | 15.741577 | 15.639168 | 15.072214 | 15.756669 | 15.429359 | 14.782732 | 15.265178 | 15.088494 | 15.690008 | 15.107313 |
hep-th/0603225 | Juan Mateos Guilarte | M.A. Gonzalez Leon, J. Mateos Guilarte and M. de la Torre Mayado | From N=2 supersymmetric classical to quantum mechanics and back: the
SUSY WKB approximation | LaTex File, 19 Pages, 10 Figures, 3 Tables. Based on a talk given by
J. M. G. in the Workshop "Groups, Geometry and Physics", Zaragoza, Spain,
December 2005 | null | null | null | hep-th | null | Links between supersymmetric classical and quantum mechanics are explored.
Diagrammatic representations for \hbar-expansions of norms of ground states are
provided. The WKB spectra of supersymmetric non harmonic oscillators are found.
| [
{
"created": "Wed, 29 Mar 2006 09:23:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Leon",
"M. A. Gonzalez",
""
],
[
"Guilarte",
"J. Mateos",
""
],
[
"Mayado",
"M. de la Torre",
""
]
] | Links between supersymmetric classical and quantum mechanics are explored. Diagrammatic representations for \hbar-expansions of norms of ground states are provided. The WKB spectra of supersymmetric non harmonic oscillators are found. | 29.213646 | 24.172796 | 28.505924 | 22.101473 | 24.863102 | 24.476427 | 21.848156 | 25.63603 | 22.664703 | 26.576685 | 20.763367 | 19.92247 | 23.639669 | 20.427206 | 19.270138 | 20.244249 | 19.903915 | 20.05094 | 20.651855 | 22.852457 | 20.636612 |
hep-th/0009104 | Joel Giedt | Joel Giedt | Completion of standard-like embeddings | 21 pages; 10 tables; further reduction to set of 175 embeddings;
equivalence of some observable sector embeddings demonstrated | Ann.Phys.289:251,2001 | 10.1006/aphy.2001.6139 | LBNL-46839; UCB-PTH-00/28 | hep-th hep-ph math-ph math.MP | null | Inequivalent standard-like observable sector embeddings in $Z_3$ orbifolds
with two discrete Wilson lines, as determined by Casas, Mondragon and Mu\~noz,
are completed by examining all possible ways of embedding the hidden sector.
The hidden sector embeddings are relevant to twisted matter in nontrivial
representatio... | [
{
"created": "Thu, 14 Sep 2000 01:26:34 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Nov 2000 21:42:29 GMT",
"version": "v2"
},
{
"created": "Wed, 3 Jan 2001 22:08:08 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Giedt",
"Joel",
""
]
] | Inequivalent standard-like observable sector embeddings in $Z_3$ orbifolds with two discrete Wilson lines, as determined by Casas, Mondragon and Mu\~noz, are completed by examining all possible ways of embedding the hidden sector. The hidden sector embeddings are relevant to twisted matter in nontrivial representations... | 14.659046 | 17.026041 | 15.850035 | 14.538471 | 16.049112 | 15.851581 | 15.5603 | 15.693065 | 14.087519 | 16.242371 | 14.623615 | 13.788602 | 13.802392 | 13.307889 | 14.631619 | 14.057075 | 13.554739 | 13.661522 | 13.805325 | 14.401322 | 13.933642 |
0905.1445 | Shotaro Shiba | Takayuki Kobo, Yutaka Matsuo, Shotaro Shiba | Aspects of U-duality in BLG models with Lorentzian metric 3-algebras | 27 pages, v2: minor corrections | JHEP 0906:053,2009 | 10.1088/1126-6708/2009/06/053 | UT-09-11 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In our previous paper, it was shown that BLG model based on a Lorentzian
metric 3-algebra gives Dp-brane action whose worldvolume is compactified on
torus T^d (d=p-2). Here the 3-algebra was a generalized one with d+1 pairs of
Lorentzian metric generators and expressed in terms of a loop algebra with
central extensio... | [
{
"created": "Mon, 11 May 2009 15:00:49 GMT",
"version": "v1"
},
{
"created": "Thu, 14 May 2009 06:37:09 GMT",
"version": "v2"
}
] | 2009-07-28 | [
[
"Kobo",
"Takayuki",
""
],
[
"Matsuo",
"Yutaka",
""
],
[
"Shiba",
"Shotaro",
""
]
] | In our previous paper, it was shown that BLG model based on a Lorentzian metric 3-algebra gives Dp-brane action whose worldvolume is compactified on torus T^d (d=p-2). Here the 3-algebra was a generalized one with d+1 pairs of Lorentzian metric generators and expressed in terms of a loop algebra with central extensions... | 9.907608 | 9.507196 | 10.982399 | 9.251612 | 9.189858 | 9.087093 | 9.525692 | 9.559476 | 8.91547 | 12.184141 | 9.165579 | 9.373812 | 9.589664 | 9.217954 | 9.268552 | 9.157172 | 9.289969 | 9.195745 | 9.329268 | 9.804422 | 9.279238 |
hep-th/0605021 | Shigenori Seki | Shigenori Seki, Katsuyuki Sugiyama, Tatsuya Tokunaga (Kyoto Univ.) | Superconformal Symmetry in Linear Sigma Model on Supermanifolds | 24 pages, 2 figures, typos corrected and refs. added | Nucl.Phys.B753:295-312,2006 | 10.1016/j.nuclphysb.2006.07.013 | KUNS-2018, YITP-06-19 | hep-th | null | We consider a gauged linear sigma model in two dimensions with Grassmann odd
chiral superfields. We investigate the Konishi anomaly of this model and find
out the condition for realization of superconformal symmetry on the
world-sheet. When this condition is satisfied, the theory is expected to flow
into conformal th... | [
{
"created": "Tue, 2 May 2006 11:09:21 GMT",
"version": "v1"
},
{
"created": "Thu, 11 May 2006 11:29:38 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Seki",
"Shigenori",
"",
"Kyoto Univ."
],
[
"Sugiyama",
"Katsuyuki",
"",
"Kyoto Univ."
],
[
"Tokunaga",
"Tatsuya",
"",
"Kyoto Univ."
]
] | We consider a gauged linear sigma model in two dimensions with Grassmann odd chiral superfields. We investigate the Konishi anomaly of this model and find out the condition for realization of superconformal symmetry on the world-sheet. When this condition is satisfied, the theory is expected to flow into conformal theo... | 6.873127 | 6.628939 | 8.062499 | 6.008289 | 6.6268 | 6.733242 | 6.352456 | 6.348833 | 6.616211 | 7.584586 | 6.127836 | 6.386432 | 7.15474 | 6.530234 | 6.349349 | 6.580657 | 6.418232 | 6.385004 | 6.473285 | 7.402 | 6.528061 |
1509.02016 | Gabi Zafrir | Gabi Zafrir | Brane webs, $5d$ gauge theories and $6d$ $\mathcal{N}$$=(1,0)$ SCFT's | 61 pages, 51 figures; v2 typos corrected, version published in JHEP | null | 10.1007/JHEP12(2015)157 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $5d$ gauge theories that go in the UV to $6d$ $\mathcal{N}$$=(1,0)$
SCFT. We focus on these theories that can be engineered in string theory by
brane webs. Given a theory in this class, we propose a method to determine the
$6d$ SCFT it goes to. We also discuss the implication of this to the
compactification ... | [
{
"created": "Mon, 7 Sep 2015 12:46:50 GMT",
"version": "v1"
},
{
"created": "Sat, 30 Jan 2016 15:45:54 GMT",
"version": "v2"
}
] | 2016-02-02 | [
[
"Zafrir",
"Gabi",
""
]
] | We study $5d$ gauge theories that go in the UV to $6d$ $\mathcal{N}$$=(1,0)$ SCFT. We focus on these theories that can be engineered in string theory by brane webs. Given a theory in this class, we propose a method to determine the $6d$ SCFT it goes to. We also discuss the implication of this to the compactification of... | 6.074736 | 6.0784 | 7.086331 | 5.751043 | 5.696432 | 5.817903 | 5.901575 | 5.963676 | 5.69138 | 6.691088 | 5.526313 | 5.782162 | 6.225813 | 5.831782 | 5.863573 | 5.875644 | 5.729868 | 5.756513 | 5.758582 | 5.895751 | 5.732704 |
hep-th/9610018 | Jorge Russo | J.G. Russo | Supermembrane dynamics from multiple interacting strings | Small corrections. 21 pages | Nucl.Phys. B492 (1997) 205-222 | 10.1016/S0550-3213(97)80032-6 | CERN-TH/96-275 | hep-th | null | The supermembrane theory on $R^{10}x S^1$ is investigated, for membranes that
wrap once around the compact dimension. The Hamiltonian can be organized as
describing $N_s$ interacting strings, the exact supermembrane corresponding to
$N_s\to \infty$. The zero-mode part of $N_s-1$ strings turn out to be precisely
the m... | [
{
"created": "Thu, 3 Oct 1996 15:35:27 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Oct 1996 11:01:44 GMT",
"version": "v2"
},
{
"created": "Wed, 16 Oct 1996 12:39:49 GMT",
"version": "v3"
},
{
"created": "Sun, 2 Feb 1997 11:32:08 GMT",
"version": "v4"
}
] | 2015-06-26 | [
[
"Russo",
"J. G.",
""
]
] | The supermembrane theory on $R^{10}x S^1$ is investigated, for membranes that wrap once around the compact dimension. The Hamiltonian can be organized as describing $N_s$ interacting strings, the exact supermembrane corresponding to $N_s\to \infty$. The zero-mode part of $N_s-1$ strings turn out to be precisely the mod... | 9.807277 | 9.674219 | 9.983782 | 8.911906 | 9.528967 | 10.090818 | 9.940274 | 9.393893 | 8.614186 | 11.953687 | 9.138121 | 9.148053 | 9.516482 | 9.373885 | 9.537509 | 9.145723 | 9.127878 | 9.17382 | 9.394368 | 9.693363 | 9.227481 |
hep-th/9309149 | Antonio Gabriel Oliveira Moreira | C. Aragone, Pio J. Arias and A. Khoudeir | Two gravitationally Chern-Simons terms are too many | Pages 7 | null | null | SB-F/204 | hep-th | null | It is shown that topological massive gravity augmented by the triadic
gravitational Chern-Simons first order term is a curved a pure spin-2 action.
This model contains two massive spin-2 excitations. However, since its
light-front energy is not semidefinite positive, this double CS-action does not
have any physical r... | [
{
"created": "Mon, 27 Sep 1993 22:27:16 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Aragone",
"C.",
""
],
[
"Arias",
"Pio J.",
""
],
[
"Khoudeir",
"A.",
""
]
] | It is shown that topological massive gravity augmented by the triadic gravitational Chern-Simons first order term is a curved a pure spin-2 action. This model contains two massive spin-2 excitations. However, since its light-front energy is not semidefinite positive, this double CS-action does not have any physical rel... | 22.579281 | 22.176662 | 23.027069 | 20.571939 | 21.047325 | 20.026798 | 20.613337 | 21.50795 | 20.08206 | 23.397655 | 19.288055 | 19.704891 | 19.627064 | 18.92024 | 20.174469 | 20.287172 | 19.518711 | 19.871626 | 20.03367 | 20.211372 | 19.241442 |
hep-th/9205030 | Haruhiko Terao | Haruhiko Terao | Quantum Analysis of Jackiw and Teitelboim's Model for 1+1 D Gravity and
Topological Gauge Theory | 31 pages | Nucl.Phys. B395 (1993) 623-646 | 10.1016/0550-3213(93)90050-Y | DPKU-9207 | hep-th | null | We study the BRST quantization of the 1+1 dimensional gravity model proposed
by Jackiw and Teitelboim and also the topological gauge model which is
equivalent to the gravity model at least classically. The gravity model
quantized in the light-cone gauge is found to be a free theory with a nilpotent
BRST charge. We sh... | [
{
"created": "Wed, 13 May 1992 04:22:50 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Terao",
"Haruhiko",
""
]
] | We study the BRST quantization of the 1+1 dimensional gravity model proposed by Jackiw and Teitelboim and also the topological gauge model which is equivalent to the gravity model at least classically. The gravity model quantized in the light-cone gauge is found to be a free theory with a nilpotent BRST charge. We show... | 4.988197 | 4.512153 | 5.065933 | 4.40416 | 4.431312 | 4.380932 | 4.309611 | 4.454982 | 4.34897 | 5.048083 | 4.419729 | 4.651624 | 4.942961 | 4.601655 | 4.469294 | 4.601907 | 4.647174 | 4.509838 | 4.648074 | 4.824889 | 4.594432 |
hep-th/0601113 | Vincent G. J. Rodgers | V.G.J. Rodgers and Takeshi Yasuda | General Coordinate Transformations as the Origins of Dark Energy | null | Int.J.Mod.Phys.A22:749-776,2007 | 10.1142/S0217751X07035100 | null | hep-th | null | In this note we demonstrate that the algebra associated with coordinate
transformations might contain the origins of a scalar field that can behave as
an inflaton and/or a source for dark energy. We will call this particular
scalar field the diffeomorphism scalar field. In one dimension, the algebra of
coordinate tra... | [
{
"created": "Tue, 17 Jan 2006 04:13:35 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Rodgers",
"V. G. J.",
""
],
[
"Yasuda",
"Takeshi",
""
]
] | In this note we demonstrate that the algebra associated with coordinate transformations might contain the origins of a scalar field that can behave as an inflaton and/or a source for dark energy. We will call this particular scalar field the diffeomorphism scalar field. In one dimension, the algebra of coordinate trans... | 8.482494 | 8.624436 | 8.098548 | 8.035682 | 8.8272 | 8.483728 | 8.993892 | 8.123841 | 8.625806 | 8.858531 | 8.16478 | 7.974077 | 7.945435 | 7.939152 | 7.867725 | 8.014849 | 7.999709 | 7.909196 | 8.018777 | 7.833448 | 7.915663 |
hep-th/0011196 | Y. M. Cho | W. S. Bae, Y. M. Cho, D. G. Pak | Electric-Magnetic Duality in QED Effective Action | 5 pages | Phys.Rev. D64 (2001) 017303 | 10.1103/PhysRevD.64.017303 | null | hep-th | null | Recently we have obtained a non-perturbative but convergent series expression
of the one loop effective action of QED, and discussed the renormalization of
the effective action. In this paper we establish the electric-magnetic duality
in the quantum effective action.
| [
{
"created": "Wed, 22 Nov 2000 05:14:39 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bae",
"W. S.",
""
],
[
"Cho",
"Y. M.",
""
],
[
"Pak",
"D. G.",
""
]
] | Recently we have obtained a non-perturbative but convergent series expression of the one loop effective action of QED, and discussed the renormalization of the effective action. In this paper we establish the electric-magnetic duality in the quantum effective action. | 10.079337 | 6.482228 | 8.971227 | 7.056343 | 7.234565 | 7.589063 | 6.783322 | 7.201294 | 6.987859 | 8.280732 | 6.878274 | 7.513791 | 8.215369 | 7.675577 | 7.866596 | 7.630784 | 7.562353 | 7.672665 | 7.871519 | 7.885704 | 7.642159 |
1204.3893 | Hagen Triendl | Jan Louis, Paul Smyth, Hagen Triendl | Supersymmetric Vacua in N=2 Supergravity | 14 pages, v2: references added, statement on SU(3) x SU(3) structure
compactifications clarified; v3: published version with statement on moduli
space of N=2 AdS vacua corrected | JHEP 1208:039, 2012 | 10.1007/JHEP08(2012)039 | ZMP-HH/12-6; IPhT-t12/031 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the embedding tensor formalism to analyse maximally symmetric
backgrounds of N=2 gauged supergravities which have the full N=2 supersymmetry.
We state the condition for N=2 vacua and discuss some of their general
properties. We show that if the gauged isometries leave the SU(2) R-symmetry
invariant, then the N... | [
{
"created": "Tue, 17 Apr 2012 20:00:00 GMT",
"version": "v1"
},
{
"created": "Mon, 7 May 2012 12:29:16 GMT",
"version": "v2"
},
{
"created": "Mon, 19 Nov 2012 17:35:49 GMT",
"version": "v3"
}
] | 2012-11-20 | [
[
"Louis",
"Jan",
""
],
[
"Smyth",
"Paul",
""
],
[
"Triendl",
"Hagen",
""
]
] | We use the embedding tensor formalism to analyse maximally symmetric backgrounds of N=2 gauged supergravities which have the full N=2 supersymmetry. We state the condition for N=2 vacua and discuss some of their general properties. We show that if the gauged isometries leave the SU(2) R-symmetry invariant, then the N=2... | 5.718634 | 5.722791 | 6.713686 | 5.514881 | 5.881656 | 5.774714 | 5.630599 | 5.24298 | 5.542522 | 7.116162 | 5.929492 | 5.551514 | 5.824098 | 5.442775 | 5.428856 | 5.461179 | 5.55303 | 5.528553 | 5.513614 | 5.850296 | 5.337797 |
2304.04695 | Irina Aref'eva | Irina Aref'eva and Igor Volovich | Violation of the Third Law of Thermodynamics by Black Holes, Riemann
Zeta Function and Bose Gas in Negative Dimensions | 10 pages, minor improvements, reference added | null | null | null | hep-th gr-qc | http://creativecommons.org/publicdomain/zero/1.0/ | Black holes violate the third law of thermodynamics in its standard
formulation. Schwarzschild black hole entropy is inverse proportional to the
square of the temperature $S=1/(16 \pi T^2) $ and tends to infinity rather than
zero when the temperature goes to zero. We search for quantum statistical
models with such ex... | [
{
"created": "Mon, 10 Apr 2023 16:18:15 GMT",
"version": "v1"
},
{
"created": "Mon, 1 May 2023 16:24:03 GMT",
"version": "v2"
}
] | 2023-05-02 | [
[
"Aref'eva",
"Irina",
""
],
[
"Volovich",
"Igor",
""
]
] | Black holes violate the third law of thermodynamics in its standard formulation. Schwarzschild black hole entropy is inverse proportional to the square of the temperature $S=1/(16 \pi T^2) $ and tends to infinity rather than zero when the temperature goes to zero. We search for quantum statistical models with such exot... | 9.008207 | 9.814594 | 8.803267 | 8.813968 | 10.819696 | 9.218428 | 9.965465 | 8.963991 | 9.245708 | 9.406266 | 8.846101 | 8.629478 | 8.960655 | 8.363806 | 8.674797 | 8.559591 | 8.696755 | 8.277952 | 8.459105 | 8.993016 | 8.886922 |
1501.07863 | Thomas Mohaupt | Paul Dempster, David Errington and Thomas Mohaupt | Nernst branes from special geometry | 37 pages. v2: numerical pre-factors of scalar fields q_A corrected in
Section 3. No changes to conclusions. References added | null | 10.1007/JHEP05(2015)079 | LTH-1033 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct new black brane solutions in $U(1)$ gauged ${\cal N}=2$
supergravity with a general cubic prepotential, which have entropy density
$s\sim T^{1/3}$ as $T \rightarrow 0$ and thus satisfy the Nernst Law. By using
the real formulation of special geometry, we are able to obtain analytical
solutions in closed ... | [
{
"created": "Fri, 30 Jan 2015 17:53:27 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Feb 2015 10:22:43 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Dempster",
"Paul",
""
],
[
"Errington",
"David",
""
],
[
"Mohaupt",
"Thomas",
""
]
] | We construct new black brane solutions in $U(1)$ gauged ${\cal N}=2$ supergravity with a general cubic prepotential, which have entropy density $s\sim T^{1/3}$ as $T \rightarrow 0$ and thus satisfy the Nernst Law. By using the real formulation of special geometry, we are able to obtain analytical solutions in closed fo... | 5.706505 | 5.326986 | 6.567381 | 5.471567 | 5.736383 | 5.45765 | 5.903177 | 5.200777 | 5.373985 | 7.431921 | 5.268907 | 5.468853 | 5.962125 | 5.498462 | 5.450745 | 5.643428 | 5.602245 | 5.477034 | 5.434115 | 5.820376 | 5.214836 |
hep-th/0211214 | Tigran Tchrakian | A. Chakrabarti (Ecole Polytechnique) | Nonlinear transforms of momenta and Planck scale limit | 10 pages, no figures, corrected some typos | J.Math.Phys. 44 (2003) 3800-3808 | 10.1063/1.1593225 | null | hep-th gr-qc | null | Starting with the generators of the Poincar\'e group for arbitrary mass (m)
and spin (s) a nonunitary transformation is implemented to obtain momenta with
an absolute Planck scale limit. In the rest frame (for $m>0$) the transformed
energy coincides with the standard one, both being $m$. As the latter tends to
infini... | [
{
"created": "Fri, 22 Nov 2002 12:23:13 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Jan 2003 12:21:19 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Chakrabarti",
"A.",
"",
"Ecole Polytechnique"
]
] | Starting with the generators of the Poincar\'e group for arbitrary mass (m) and spin (s) a nonunitary transformation is implemented to obtain momenta with an absolute Planck scale limit. In the rest frame (for $m>0$) the transformed energy coincides with the standard one, both being $m$. As the latter tends to infinity... | 13.31248 | 16.228518 | 14.034176 | 13.402913 | 13.851701 | 15.1928 | 16.035646 | 14.019238 | 13.091317 | 14.419065 | 13.644409 | 13.171369 | 12.900056 | 13.022943 | 13.228273 | 13.500825 | 13.508034 | 13.026613 | 13.465314 | 12.630271 | 13.209379 |
1206.5140 | S. Prem Kumar | S. Prem Kumar | Heavy quark density in N=4 SYM: from hedgehog to Lifshitz spacetimes | 20 pages, 2 figures, references added | null | 10.1007/JHEP08(2012)155 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the effect of an order N^2 density of heavy quarks in strongly
coupled N=4 SUSY Yang-Mills theory in the large N limit. This is achieved in
the type IIB supergravity dual by introducing a uniformly smeared density of
macroscopic string sources stretching to the boundary of AdS_5 x S^5. The
backreacted system... | [
{
"created": "Fri, 22 Jun 2012 13:10:34 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Jul 2012 22:32:16 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Kumar",
"S. Prem",
""
]
] | We study the effect of an order N^2 density of heavy quarks in strongly coupled N=4 SUSY Yang-Mills theory in the large N limit. This is achieved in the type IIB supergravity dual by introducing a uniformly smeared density of macroscopic string sources stretching to the boundary of AdS_5 x S^5. The backreacted system e... | 8.70455 | 8.365113 | 9.328028 | 8.157343 | 8.42371 | 7.72749 | 7.913038 | 7.491508 | 7.619004 | 9.982466 | 7.341683 | 7.734118 | 9.091641 | 7.966166 | 8.260242 | 8.132025 | 7.986745 | 7.560217 | 8.189558 | 9.138183 | 7.733115 |
1808.05939 | {\DJ}or{\dj}e Radi\v{c}evi\'c | Jennifer Lin, Djordje Radicevic | Comments on Defining Entanglement Entropy | 49 pages. v2: added references | null | null | null | hep-th cond-mat.other hep-lat quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the issue of defining the entropy of a spatial region in a broad
class of quantum theories. In theories with explicit regularizations, working
within an elementary but general algebraic framework applicable to matter and
gauge theories alike, we give precise path integral expressions for three known
types ... | [
{
"created": "Fri, 17 Aug 2018 17:43:58 GMT",
"version": "v1"
},
{
"created": "Sun, 16 Sep 2018 15:17:56 GMT",
"version": "v2"
}
] | 2018-09-18 | [
[
"Lin",
"Jennifer",
""
],
[
"Radicevic",
"Djordje",
""
]
] | We revisit the issue of defining the entropy of a spatial region in a broad class of quantum theories. In theories with explicit regularizations, working within an elementary but general algebraic framework applicable to matter and gauge theories alike, we give precise path integral expressions for three known types of... | 13.06459 | 12.569155 | 14.582765 | 12.795286 | 12.468522 | 13.268987 | 12.730099 | 12.114114 | 13.46452 | 13.535839 | 12.891465 | 12.913128 | 13.223453 | 12.375851 | 12.478725 | 12.394918 | 12.596124 | 12.417946 | 13.030642 | 13.168495 | 12.319276 |
0905.0900 | Paul Hohler | Paul M. Hohler, Mikhail A. Stephanov | Holography and the speed of sound at high temperatures | 4 pages, corrected typos | Phys. Rev. D 80, 066002 (2009) | 10.1103/PhysRevD.80.066002 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that in a general class of strongly interacting theories at high
temperatures the speed of sound approaches the conformal value c_s^2=1/3
universally from_below_. This class includes theories holographically dual to a
theory of gravity coupled to a single scalar field, representing the operator
of the scale a... | [
{
"created": "Thu, 7 May 2009 19:40:55 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Sep 2009 21:05:37 GMT",
"version": "v2"
}
] | 2009-09-16 | [
[
"Hohler",
"Paul M.",
""
],
[
"Stephanov",
"Mikhail A.",
""
]
] | We show that in a general class of strongly interacting theories at high temperatures the speed of sound approaches the conformal value c_s^2=1/3 universally from_below_. This class includes theories holographically dual to a theory of gravity coupled to a single scalar field, representing the operator of the scale ano... | 13.423601 | 11.464442 | 11.763602 | 11.539361 | 12.495304 | 11.20464 | 11.59081 | 12.312431 | 10.409957 | 13.323079 | 10.41329 | 10.726202 | 11.535499 | 10.774061 | 11.183646 | 11.160851 | 11.151419 | 11.221616 | 10.745406 | 11.48095 | 10.683913 |
2312.17416 | Haifeng Tang | Haifeng Tang | Operator Krylov complexity in random matrix theory | 25 pages, 6 figures | null | null | null | hep-th cond-mat.quant-gas cond-mat.stat-mech cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Krylov complexity, as a novel measure of operator complexity under Heisenberg
evolution, exhibits many interesting universal behaviors and also bounds many
other complexity measures. In this work, we study Krylov complexity
$\mathcal{K}(t)$ in Random Matrix Theory (RMT). In large $N$ limit: (1) For
infinite temperatu... | [
{
"created": "Fri, 29 Dec 2023 01:12:51 GMT",
"version": "v1"
}
] | 2024-01-01 | [
[
"Tang",
"Haifeng",
""
]
] | Krylov complexity, as a novel measure of operator complexity under Heisenberg evolution, exhibits many interesting universal behaviors and also bounds many other complexity measures. In this work, we study Krylov complexity $\mathcal{K}(t)$ in Random Matrix Theory (RMT). In large $N$ limit: (1) For infinite temperature... | 7.743361 | 7.631242 | 7.567971 | 6.555893 | 7.487298 | 7.336822 | 7.171192 | 6.989474 | 7.149637 | 8.470928 | 6.608289 | 6.920131 | 7.117044 | 6.93407 | 7.017372 | 6.846609 | 7.033385 | 6.910433 | 6.881744 | 7.269962 | 6.799142 |
1509.03612 | Alexander Zhiboedov | Juan Maldacena, David Simmons-Duffin, Alexander Zhiboedov | Looking for a bulk point | 60 pages, 12 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Lorentzian correlators of local operators. In perturbation
theory, singularities occur when we can draw a position-space Landau diagram
with null lines. In theories with gravity duals, we can also draw Landau
diagrams in the bulk. We argue that certain singularities can arise only from
bulk diagrams, not ... | [
{
"created": "Fri, 11 Sep 2015 19:09:46 GMT",
"version": "v1"
}
] | 2015-09-14 | [
[
"Maldacena",
"Juan",
""
],
[
"Simmons-Duffin",
"David",
""
],
[
"Zhiboedov",
"Alexander",
""
]
] | We consider Lorentzian correlators of local operators. In perturbation theory, singularities occur when we can draw a position-space Landau diagram with null lines. In theories with gravity duals, we can also draw Landau diagrams in the bulk. We argue that certain singularities can arise only from bulk diagrams, not fr... | 9.846727 | 9.941341 | 10.999654 | 9.248199 | 10.434382 | 9.435089 | 9.829824 | 9.394964 | 9.769299 | 11.259782 | 8.940349 | 9.306604 | 10.463298 | 9.391948 | 9.415675 | 9.489124 | 9.203023 | 9.254086 | 9.53449 | 10.310431 | 9.455338 |
hep-th/0006111 | Shinsuke M. Nishigaki | P. H. Damgaard, S. M. Nishigaki | Distribution of the k-th smallest Dirac operator eigenvalue | REVTeX 3.1, 6 pages, 1 figure. Corrected factors in eqs. (16a) and
(16c) and very minor typos (v2) | Phys.Rev. D63 (2001) 045012 | 10.1103/PhysRevD.63.045012 | TIT-HEP-446 | hep-th cond-mat hep-lat | null | Based on the exact relationship to Random Matrix Theory, we derive the
probability distribution of the k-th smallest Dirac operator eigenvalue in the
microscopic finite-volume scaling regime of QCD and related gauge theories.
| [
{
"created": "Thu, 15 Jun 2000 15:10:02 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jul 2003 18:52:58 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Damgaard",
"P. H.",
""
],
[
"Nishigaki",
"S. M.",
""
]
] | Based on the exact relationship to Random Matrix Theory, we derive the probability distribution of the k-th smallest Dirac operator eigenvalue in the microscopic finite-volume scaling regime of QCD and related gauge theories. | 20.178125 | 19.892382 | 14.198909 | 12.493413 | 15.21452 | 14.943156 | 15.741288 | 14.030248 | 12.99645 | 16.359491 | 14.465372 | 13.443901 | 15.916552 | 14.914903 | 14.093552 | 14.513446 | 14.049412 | 13.905046 | 13.411477 | 15.720582 | 13.204807 |
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