id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9704023 | Henneaux M. | Marc Henneaux | Anomalies and Renormalization of BFYM Theory | null | Phys.Lett. B406 (1997) 66-69 | 10.1016/S0370-2693(97)00653-9 | null | hep-th | null | The (perturbative) renormalization properties of the BF formulation of
Yang-Mills gauge models are shown to be identical to those of the usual, second
order formulation. This result holds in any number of spacetime dimensions and
is a direct consequence of cohomological theorems established by G. Barnich, F.
Brandt a... | [
{
"created": "Thu, 3 Apr 1997 09:56:53 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Henneaux",
"Marc",
""
]
] | The (perturbative) renormalization properties of the BF formulation of Yang-Mills gauge models are shown to be identical to those of the usual, second order formulation. This result holds in any number of spacetime dimensions and is a direct consequence of cohomological theorems established by G. Barnich, F. Brandt and... | 6.168154 | 6.634206 | 5.596628 | 6.036401 | 6.720467 | 6.531873 | 6.353017 | 5.887807 | 6.357731 | 10.034818 | 5.96568 | 5.526768 | 6.239037 | 5.573726 | 5.570935 | 5.657162 | 5.852086 | 5.782228 | 5.618579 | 6.377473 | 5.619781 |
hep-th/0506026 | Farhang Loran | F. Loran and E. Bavarsad | Metastable de Sitter vacua from critical scalar theory | revtex4, minor corrections, 3 references added | null | null | null | hep-th | null | Studying the critical scalar theory in four dimensional Euclidean space with
the potential term $-g\phi^4$ we show that the theory can not be analytically
continued through g=0 from g<0 region to g>0 region. For g>0 although energy is
not bounded from below but there exist a classical trajectory with an AdS5
moduli s... | [
{
"created": "Thu, 2 Jun 2005 14:26:24 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Jul 2005 13:35:46 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Loran",
"F.",
""
],
[
"Bavarsad",
"E.",
""
]
] | Studying the critical scalar theory in four dimensional Euclidean space with the potential term $-g\phi^4$ we show that the theory can not be analytically continued through g=0 from g<0 region to g>0 region. For g>0 although energy is not bounded from below but there exist a classical trajectory with an AdS5 moduli spa... | 13.927176 | 14.605389 | 14.999079 | 13.715136 | 15.21835 | 14.785305 | 13.867313 | 14.241858 | 14.207335 | 17.141544 | 13.398508 | 13.934469 | 13.730978 | 13.449742 | 13.661001 | 13.389017 | 13.256382 | 13.292396 | 13.341904 | 13.528448 | 13.306201 |
hep-th/0306111 | Brandon Carter | Brandon Carter and Xavier Martin | Dynamical instability criterion for circular (vorton) string loops | 20 page TeX file (with typo corrections and added reference) of
manuscript published (with shorter title) in Annals of Physics | Annals Phys. 227 (1993) 151-171 | 10.1006/aphy.1993.1078 | null | hep-th | null | Dynamic perturbation equations are derived for a generic stationary state of
an elastic string model -- of the kind appropriate for representing a
superconducting cosmic string -- in a flat background. In the case of a
circular equilibrium (i.e. vorton) state of a closed string loop it is shown
that the fundamental a... | [
{
"created": "Thu, 12 Jun 2003 12:19:42 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Carter",
"Brandon",
""
],
[
"Martin",
"Xavier",
""
]
] | Dynamic perturbation equations are derived for a generic stationary state of an elastic string model -- of the kind appropriate for representing a superconducting cosmic string -- in a flat background. In the case of a circular equilibrium (i.e. vorton) state of a closed string loop it is shown that the fundamental axi... | 9.82456 | 10.187962 | 9.676558 | 9.179744 | 10.484911 | 9.582017 | 10.866448 | 9.854979 | 9.333017 | 9.995299 | 9.496834 | 9.556354 | 9.211121 | 9.218852 | 9.469873 | 9.544572 | 9.572546 | 9.318986 | 9.430791 | 9.423802 | 9.574669 |
hep-th/0003068 | Stefan Foerste | Stefan Forste, Debashis Ghoshal and Stefan Theisen | Wilson loop via AdS/CFT duality | 6 pages, Latex, contribution to the proceedings of the TMR network
conference in Paris 1999 | null | null | null | hep-th | null | The Wilson loop in N=4 supersymmetric Yang-Mills theory admits a dual
description as a macroscopic string configuration in the adS/CFT
correspondence. We discuss the correction to the quark anti-quark potential
arising from the fluctuations of the superstring.
| [
{
"created": "Thu, 9 Mar 2000 11:20:20 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Forste",
"Stefan",
""
],
[
"Ghoshal",
"Debashis",
""
],
[
"Theisen",
"Stefan",
""
]
] | The Wilson loop in N=4 supersymmetric Yang-Mills theory admits a dual description as a macroscopic string configuration in the adS/CFT correspondence. We discuss the correction to the quark anti-quark potential arising from the fluctuations of the superstring. | 9.878665 | 6.078829 | 7.886018 | 6.753093 | 7.423263 | 6.244894 | 6.381389 | 6.535261 | 5.896989 | 8.06673 | 7.110107 | 7.17331 | 7.427515 | 6.808222 | 7.231493 | 7.188838 | 7.335126 | 6.76685 | 7.179902 | 7.933933 | 6.949193 |
hep-th/9910242 | Sanchez | M. P. Infante, N. Sanchez | Minimal String Driven Cosmology and its Predictions | 22 pages Latex file, 2 figures | null | null | DFTUZ/99/15 | hep-th astro-ph gr-qc hep-ph | null | We present a minimal model for the Universe evolution fully extracted from
effective String Theory. By linking this model with a minimal but well
established observational information, we prove that it gives realistic
predictions on early and current energy density and its results are compatible
with General Relativi... | [
{
"created": "Fri, 29 Oct 1999 14:09:39 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Infante",
"M. P.",
""
],
[
"Sanchez",
"N.",
""
]
] | We present a minimal model for the Universe evolution fully extracted from effective String Theory. By linking this model with a minimal but well established observational information, we prove that it gives realistic predictions on early and current energy density and its results are compatible with General Relativity... | 20.224989 | 15.106133 | 20.655178 | 17.341234 | 20.669001 | 21.259081 | 22.026632 | 17.124037 | 17.463974 | 20.359564 | 17.5688 | 18.567469 | 19.53903 | 18.980875 | 19.872866 | 19.2656 | 19.36141 | 18.841639 | 19.212692 | 20.028852 | 18.937088 |
1106.3906 | Owen Pavel Fern\'andez Piedra | Owen Pavel Fern\'andez Piedra, Fidel Sosa, Jos\'e L. Bernal-Castillo
and Yulier Jimenez | Object picture, quasinormal modes and late time tails of fermion
perturbations in stringy black hole with U(1) charges | 13 pages, 10 figures | Int. J. Mod. Phys. D 21, 125004 (2012) | 10.1142/S0218271812500447 | GEA-UCF 2011/01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of the present report is to study massless fermion perturbations
outside five-dimensional stringy black holes with U(1) charges. The Dirac
equation was numerically solved to obtain the time profiles for the evolving
fermion fields, and the quasinormal frequencies at intermediate times are
computed by numerica... | [
{
"created": "Mon, 20 Jun 2011 13:59:21 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Jun 2012 14:56:21 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Piedra",
"Owen Pavel Fernández",
""
],
[
"Sosa",
"Fidel",
""
],
[
"Bernal-Castillo",
"José L.",
""
],
[
"Jimenez",
"Yulier",
""
]
] | The aim of the present report is to study massless fermion perturbations outside five-dimensional stringy black holes with U(1) charges. The Dirac equation was numerically solved to obtain the time profiles for the evolving fermion fields, and the quasinormal frequencies at intermediate times are computed by numerical ... | 12.511411 | 13.581502 | 11.268847 | 11.417095 | 13.256076 | 13.64834 | 13.289097 | 10.699942 | 12.788149 | 12.662258 | 13.022145 | 12.551181 | 12.291695 | 12.455674 | 12.523964 | 12.766916 | 12.936212 | 12.002074 | 13.081696 | 12.375299 | 11.794027 |
hep-th/0111108 | Gabriel Flores | Gabriel H. Flores and N.F. Svaiter | Quantum Properties of Solitons in $U(\phi)=\phi^2\ln^2(\phi^2)$ and
$U(\phi)=\phi^2\cos^2(\phi^2)$ Models | 18 pages, 4 figures | null | null | null | hep-th | null | Recently we constructed two new $(1+1)$-dimensional scalar field theory
models that posses solitonic solutions. They are the
$U(\phi)=\phi^2\ln^2(\phi^2)$ and the $U(\phi)=\phi^2\cos^2(\phi^2)$ models .
The first quantum corrections for these models are given by exactly solvable
Schrodinger equations. In this paper w... | [
{
"created": "Mon, 12 Nov 2001 18:50:04 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Flores",
"Gabriel H.",
""
],
[
"Svaiter",
"N. F.",
""
]
] | Recently we constructed two new $(1+1)$-dimensional scalar field theory models that posses solitonic solutions. They are the $U(\phi)=\phi^2\ln^2(\phi^2)$ and the $U(\phi)=\phi^2\cos^2(\phi^2)$ models . The first quantum corrections for these models are given by exactly solvable Schrodinger equations. In this paper we ... | 8.341852 | 7.828749 | 8.464893 | 7.694756 | 8.283663 | 8.25096 | 7.943794 | 7.757361 | 7.646063 | 8.436228 | 7.837293 | 7.54792 | 7.894345 | 7.755293 | 7.996196 | 7.78928 | 7.879673 | 7.820765 | 7.763727 | 8.043919 | 7.914166 |
hep-th/9907074 | Angel Uranga | J. Park, R. Rabadan, A. M. Uranga | N=1 Type IIA brane configurations, Chirality and T-duality | 39 pages, Latex, 7 eps figures. References added | Nucl.Phys.B570:3-37,2000 | 10.1016/S0550-3213(99)00699-9 | FTUAM-99/21, IASSNS-HEP-99/61, IFT-UAM/CSIC-99-25 | hep-th | null | We consider four-dimensional N=1 field theories realized by type IIA brane
configurations of NS-branes and D4-branes, in the presence of orientifold
six-planes and D6-branes. These configurations are known to present interesting
effects associated to the appearance of chiral symmetries and chiral matter in
the four-d... | [
{
"created": "Sat, 10 Jul 1999 17:01:51 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Jul 1999 23:09:38 GMT",
"version": "v2"
}
] | 2009-10-09 | [
[
"Park",
"J.",
""
],
[
"Rabadan",
"R.",
""
],
[
"Uranga",
"A. M.",
""
]
] | We consider four-dimensional N=1 field theories realized by type IIA brane configurations of NS-branes and D4-branes, in the presence of orientifold six-planes and D6-branes. These configurations are known to present interesting effects associated to the appearance of chiral symmetries and chiral matter in the four-dim... | 9.016143 | 8.360482 | 10.293562 | 7.985304 | 8.61056 | 8.359231 | 8.410056 | 8.038363 | 8.170693 | 10.945272 | 8.06772 | 8.52136 | 9.270141 | 8.440081 | 8.640641 | 8.526731 | 8.468361 | 8.654463 | 8.337269 | 9.524965 | 8.426985 |
hep-th/0305220 | Tobias Hurth | P.A. Grassi (SUNY Stony Brook), T. Hurth (CERN, SLAC), A. Quadri (MPI
Munich) | Super Background Field Method for N=2 SYM | 34 pages, Latex, JHEP3.cls | JHEP0307:008,2003 | 10.1088/1126-6708/2003/07/008 | YITP-2002-57, CERN-TH/2002-369, SLAC-PUB-9853, MPI-Pht-2002-81 | hep-th hep-ph | null | The implementation of the Background Field Method (BFM) for quantum field
theories is analysed within the Batalin-Vilkovisky (BV) formalism. We provide a
systematic way of constructing general splittings of the fields into classical
and quantum parts, such that the background transformations of the quantum
fields are... | [
{
"created": "Sun, 25 May 2003 15:59:25 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Grassi",
"P. A.",
"",
"SUNY Stony Brook"
],
[
"Hurth",
"T.",
"",
"CERN, SLAC"
],
[
"Quadri",
"A.",
"",
"MPI\n Munich"
]
] | The implementation of the Background Field Method (BFM) for quantum field theories is analysed within the Batalin-Vilkovisky (BV) formalism. We provide a systematic way of constructing general splittings of the fields into classical and quantum parts, such that the background transformations of the quantum fields are l... | 8.266269 | 8.046278 | 8.648341 | 7.583036 | 7.883524 | 8.035951 | 8.855237 | 7.716902 | 7.8167 | 9.254039 | 7.779618 | 7.787408 | 7.936888 | 7.703249 | 7.553652 | 7.618744 | 7.626815 | 7.586163 | 7.794967 | 7.930232 | 7.684383 |
1803.00991 | Jay Armas | Jay Armas, Jakob Gath, Akash Jain, and Andreas Vigand Pedersen | Dissipative hydrodynamics with higher-form symmetry | v2: 30 pages; presentation improved, typos fixed, to be published in
JHEP | JHEP 05 (2018) 192 | 10.1007/JHEP05(2018)192 | DCPT-18/01 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A theory of parity-invariant dissipative fluids with $q$-form symmetry is
formulated to first order in a derivative expansion. The fluid is anisotropic
with symmetry $\text{SO}(D-1-q)\times\text{SO}(q)$ and carries dissolved
$q$-dimensional charged objects that couple to a $(q+1)$-form background gauge
field. The cas... | [
{
"created": "Fri, 2 Mar 2018 18:43:06 GMT",
"version": "v1"
},
{
"created": "Tue, 29 May 2018 18:03:28 GMT",
"version": "v2"
}
] | 2018-06-05 | [
[
"Armas",
"Jay",
""
],
[
"Gath",
"Jakob",
""
],
[
"Jain",
"Akash",
""
],
[
"Pedersen",
"Andreas Vigand",
""
]
] | A theory of parity-invariant dissipative fluids with $q$-form symmetry is formulated to first order in a derivative expansion. The fluid is anisotropic with symmetry $\text{SO}(D-1-q)\times\text{SO}(q)$ and carries dissolved $q$-dimensional charged objects that couple to a $(q+1)$-form background gauge field. The case ... | 8.179185 | 8.052202 | 9.673951 | 8.010306 | 8.408914 | 9.22945 | 8.100844 | 8.407752 | 7.8819 | 9.554561 | 7.975664 | 7.80758 | 8.460873 | 7.945426 | 7.889576 | 7.914947 | 7.893074 | 7.968563 | 7.917793 | 8.624564 | 7.769207 |
1711.09966 | Humberto Gomez | Nathan Berkovits and Humberto Gomez | An Introduction to Pure Spinor Superstring Theory | Villa de Leyva Summer School 2015 proceedings, 28 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In these lecture notes presented at the 2015 Villa de Leyva Summer School, we
give an introduction to superstring theory. We begin by studying the particle
and superparticle in order to get a better understanding on the superstring
side. Afterwards, we review the pure spinor formalism and end by computing the
scatter... | [
{
"created": "Mon, 27 Nov 2017 20:17:19 GMT",
"version": "v1"
}
] | 2017-11-29 | [
[
"Berkovits",
"Nathan",
""
],
[
"Gomez",
"Humberto",
""
]
] | In these lecture notes presented at the 2015 Villa de Leyva Summer School, we give an introduction to superstring theory. We begin by studying the particle and superparticle in order to get a better understanding on the superstring side. Afterwards, we review the pure spinor formalism and end by computing the scatterin... | 9.615987 | 7.884281 | 10.737979 | 7.285555 | 7.605815 | 7.764059 | 8.553855 | 8.037851 | 7.375687 | 9.870887 | 7.654751 | 7.860171 | 9.000783 | 8.116318 | 7.568515 | 8.107479 | 7.625989 | 7.579208 | 7.861599 | 8.377225 | 7.788373 |
hep-th/0105261 | Andreas Albrecht | A. Albrecht, C.P. Burgess, F. Ravndal and C. Skordis | Exponentially Large Extra Dimensions | 15 Pages including 1 figure. V3: Final version accepted for
publication in PRD. This version has an improved discussion (in section IV-B)
of our mechanism for preserving the small radion mass. No changes have been
made to the technical content or results | Phys.Rev.D65:123506,2002 | 10.1103/PhysRevD.65.123506 | null | hep-th astro-ph hep-ph | null | We show how the presence of a very light scalar with a cubic self-interaction
in six dimensions can stabilize the extra dimensions at radii which are
naturally exponentially large, $r \sim \ell \exp [(4\pi)^3/g^2]$, where $\ell$
is a microscopic physics scale and $g$ is the (dimensionless) cubic coupling
constant. Th... | [
{
"created": "Mon, 28 May 2001 21:24:19 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Jul 2001 19:56:01 GMT",
"version": "v2"
},
{
"created": "Wed, 6 Feb 2002 23:42:39 GMT",
"version": "v3"
}
] | 2010-04-08 | [
[
"Albrecht",
"A.",
""
],
[
"Burgess",
"C. P.",
""
],
[
"Ravndal",
"F.",
""
],
[
"Skordis",
"C.",
""
]
] | We show how the presence of a very light scalar with a cubic self-interaction in six dimensions can stabilize the extra dimensions at radii which are naturally exponentially large, $r \sim \ell \exp [(4\pi)^3/g^2]$, where $\ell$ is a microscopic physics scale and $g$ is the (dimensionless) cubic coupling constant. The ... | 7.234562 | 7.674634 | 7.228703 | 6.462467 | 7.792438 | 7.127523 | 7.539562 | 6.997179 | 7.282427 | 7.661238 | 7.336601 | 6.88965 | 7.030672 | 6.782712 | 6.75924 | 6.988821 | 6.898075 | 7.01001 | 6.858408 | 7.131588 | 7.01454 |
hep-th/9712043 | Olaf Lechtenfeld | Chandrashekar Devchand, Olaf Lechtenfeld | Extended Self-Dual Yang-Mills from the N=2 String | 19 pages; typos corrected, note and reference added; published
version | Nucl.Phys. B516 (1998) 255-272 | 10.1016/S0550-3213(98)00072-8 | ITP-UH-31/97 | hep-th | null | We show that the physical degrees of freedom of the critical open string with
N=2 superconformal symmetry on the worldsheet are described by a self-dual
Yang-Mills field on a hyperspace parametrised by the coordinates of the target
space R^{2,2} together with a commuting chiral spinor. A prepotential for the
self-dua... | [
{
"created": "Thu, 4 Dec 1997 15:02:07 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Jun 1998 10:45:09 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Devchand",
"Chandrashekar",
""
],
[
"Lechtenfeld",
"Olaf",
""
]
] | We show that the physical degrees of freedom of the critical open string with N=2 superconformal symmetry on the worldsheet are described by a self-dual Yang-Mills field on a hyperspace parametrised by the coordinates of the target space R^{2,2} together with a commuting chiral spinor. A prepotential for the self-dual ... | 12.488687 | 12.759661 | 14.726149 | 11.661323 | 12.104736 | 12.003623 | 12.099484 | 12.15246 | 11.001789 | 13.9455 | 11.277382 | 11.16208 | 11.896928 | 11.30979 | 11.095218 | 11.007651 | 11.345796 | 11.362973 | 11.091295 | 12.58454 | 11.298998 |
1612.04833 | Abhishek Pathak | Abhishek Pathak, Achilleas P. Porfyriadis, Andrew Strominger, Oscar
Varela | Logarithmic corrections to black hole entropy from Kerr/CFT | null | null | 10.1007/JHEP04(2017)090 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been shown by A. Sen that logarithmic corrections to the black hole
area-entropy law are entirely determined macroscopically from the massless
particle spectrum. They therefore serve as powerful consistency checks on any
proposed enumeration of quantum black hole microstates. Sen's results include a
macroscopi... | [
{
"created": "Wed, 14 Dec 2016 21:00:25 GMT",
"version": "v1"
}
] | 2017-05-24 | [
[
"Pathak",
"Abhishek",
""
],
[
"Porfyriadis",
"Achilleas P.",
""
],
[
"Strominger",
"Andrew",
""
],
[
"Varela",
"Oscar",
""
]
] | It has been shown by A. Sen that logarithmic corrections to the black hole area-entropy law are entirely determined macroscopically from the massless particle spectrum. They therefore serve as powerful consistency checks on any proposed enumeration of quantum black hole microstates. Sen's results include a macroscopic ... | 9.914547 | 9.387222 | 8.51688 | 8.833349 | 8.725051 | 8.843359 | 8.387759 | 8.735912 | 8.498687 | 10.110106 | 7.836291 | 7.850011 | 8.518356 | 8.27495 | 8.093632 | 8.074224 | 8.495914 | 8.50342 | 8.388792 | 8.842461 | 8.410549 |
2108.08859 | Constantinos Papageorgakis | Gergely K\'antor, Vasilis Niarchos, Constantinos Papageorgakis | Solving Conformal Field Theories with Artificial Intelligence | 6 pages; v2: references added | null | 10.1103/PhysRevLett.128.041601 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this paper we deploy for the first time Reinforcement-Learning algorithms
in the context of the conformal-bootstrap programme to obtain numerical
solutions of conformal field theories (CFTs). As an illustration, we use a soft
Actor-Critic algorithm and find approximate solutions to the truncated crossing
equations... | [
{
"created": "Thu, 19 Aug 2021 18:00:57 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Sep 2021 13:46:47 GMT",
"version": "v2"
}
] | 2022-02-02 | [
[
"Kántor",
"Gergely",
""
],
[
"Niarchos",
"Vasilis",
""
],
[
"Papageorgakis",
"Constantinos",
""
]
] | In this paper we deploy for the first time Reinforcement-Learning algorithms in the context of the conformal-bootstrap programme to obtain numerical solutions of conformal field theories (CFTs). As an illustration, we use a soft Actor-Critic algorithm and find approximate solutions to the truncated crossing equations o... | 11.49905 | 9.726433 | 11.095387 | 9.322319 | 10.030694 | 10.135659 | 9.954718 | 9.150024 | 9.777575 | 11.847572 | 9.700646 | 9.71167 | 10.203015 | 9.778986 | 9.560514 | 9.685557 | 9.799571 | 9.811136 | 9.450445 | 10.762475 | 9.743312 |
hep-th/0606136 | Toshihiro Matsuo | Feng-Li Lin, Toshihiro Matsuo | Jet Quenching Parameter in Medium with Chemical Potential from AdS/CFT | 10 pages, 1 figure;v2 minor changes, references added; v3 minor
changes and final to PLB | Phys.Lett.B641:45-49,2006 | 10.1016/j.physletb.2006.08.024 | null | hep-th hep-ph nucl-th | null | We calculate the jet quenching parameter in medium with chemical potential
from AdS/CFT correspondence. Our result is summarized in a plot. Moreover, we
extract the explicit form of the jet quenching parameter of medium with small
chemical potential for phases of dual SYM corresponding to large and small
black holes.... | [
{
"created": "Thu, 15 Jun 2006 14:30:21 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Jun 2006 02:12:23 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Aug 2006 03:21:53 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Lin",
"Feng-Li",
""
],
[
"Matsuo",
"Toshihiro",
""
]
] | We calculate the jet quenching parameter in medium with chemical potential from AdS/CFT correspondence. Our result is summarized in a plot. Moreover, we extract the explicit form of the jet quenching parameter of medium with small chemical potential for phases of dual SYM corresponding to large and small black holes. F... | 10.765157 | 10.462887 | 11.315656 | 9.510107 | 10.71704 | 10.457402 | 10.365553 | 10.246057 | 10.343431 | 11.551516 | 10.200583 | 10.651978 | 11.556832 | 10.693682 | 10.426233 | 10.941609 | 10.270142 | 10.08899 | 10.56123 | 10.751901 | 10.656597 |
1701.06553 | Lukas Witkowski | Arthur Hebecker, Philipp Henkenjohann, Lukas T. Witkowski | What is the Magnetic Weak Gravity Conjecture for Axions? | 29 pages, 7 figures; v2: Comment on topologically inflating monopoles
added; v3: References added | null | 10.1002/prop.201700011 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The electric Weak Gravity Conjecture demands that axions with large decay
constant $f$ couple to light instantons. The resulting large instantonic
corrections pose problems for natural inflation. We explore an alternative
argument based on the magnetic Weak Gravity Conjecture for axions, which we try
to make more pre... | [
{
"created": "Mon, 23 Jan 2017 18:51:08 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Feb 2017 17:45:18 GMT",
"version": "v2"
},
{
"created": "Tue, 28 Mar 2017 16:58:53 GMT",
"version": "v3"
}
] | 2017-04-26 | [
[
"Hebecker",
"Arthur",
""
],
[
"Henkenjohann",
"Philipp",
""
],
[
"Witkowski",
"Lukas T.",
""
]
] | The electric Weak Gravity Conjecture demands that axions with large decay constant $f$ couple to light instantons. The resulting large instantonic corrections pose problems for natural inflation. We explore an alternative argument based on the magnetic Weak Gravity Conjecture for axions, which we try to make more preci... | 12.936276 | 13.596084 | 14.841074 | 13.468877 | 13.892603 | 14.551989 | 14.51797 | 14.295674 | 13.588698 | 14.596557 | 13.240629 | 13.377256 | 13.493887 | 12.931851 | 12.896781 | 13.103762 | 12.92266 | 13.317461 | 13.102468 | 13.328592 | 12.635605 |
hep-th/9912116 | Andrei Ivanov | M.Faber, A.I. Ivanov, A. Mueller and N.I. Troitskaya | On the dual-vector field condensation in the dual Monopole
Nambu-Jona-Lasinio model with dual Dirac strings | 19 pages, no figers, Latex | null | null | null | hep-th | null | The condensation of a dual-vector field is investigated in the dual Monopole
Nambu-Jona-Lasinio model with dual Dirac strings. The condensate of a
dual-vector field is calculated as a functional of a shape of a dual Dirac
string. The obtained result is compared with the gluon condensate calculated in
a QCD sum rules ... | [
{
"created": "Tue, 14 Dec 1999 15:02:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Faber",
"M.",
""
],
[
"Ivanov",
"A. I.",
""
],
[
"Mueller",
"A.",
""
],
[
"Troitskaya",
"N. I.",
""
]
] | The condensation of a dual-vector field is investigated in the dual Monopole Nambu-Jona-Lasinio model with dual Dirac strings. The condensate of a dual-vector field is calculated as a functional of a shape of a dual Dirac string. The obtained result is compared with the gluon condensate calculated in a QCD sum rules ap... | 10.260503 | 7.766853 | 9.049083 | 7.591993 | 9.072552 | 8.30307 | 8.168214 | 7.884661 | 8.091537 | 10.966778 | 8.613484 | 8.709266 | 8.512867 | 8.345485 | 8.541438 | 8.742857 | 8.362814 | 8.385478 | 8.354801 | 9.097802 | 8.93657 |
hep-th/0105249 | Youm Donam | Donam Youm | The Cardy-Verlinde Formula and Charged Topological AdS Black Holes | 10 pages, LaTeX, references added | Mod.Phys.Lett. A16 (2001) 1327-1334 | 10.1142/S0217732301004510 | IC/2001/39 | hep-th | null | We consider the brane universe in the bulk background of the charged
topological AdS black holes. The evolution of the brane universe is described
by the Friedmann equations for a flat or an open FRW-universe containing
radiation and stiff matter. We find that the temperature and entropy of the
dual CFT are simply ex... | [
{
"created": "Thu, 24 May 2001 13:47:52 GMT",
"version": "v1"
},
{
"created": "Mon, 28 May 2001 13:47:48 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Youm",
"Donam",
""
]
] | We consider the brane universe in the bulk background of the charged topological AdS black holes. The evolution of the brane universe is described by the Friedmann equations for a flat or an open FRW-universe containing radiation and stiff matter. We find that the temperature and entropy of the dual CFT are simply expr... | 7.211056 | 5.399063 | 7.059043 | 5.947899 | 5.082518 | 5.196258 | 5.679462 | 5.706442 | 6.180565 | 7.133907 | 5.727668 | 6.714378 | 6.814445 | 6.481183 | 6.439603 | 6.394746 | 6.467389 | 6.552125 | 6.607123 | 6.808124 | 6.634686 |
2106.14971 | Mithat Unsal | Mithat \"Unsal | TQFT at work for IR-renormalons, resurgence and Lefschetz decomposition | 7 pages, 1 figure | null | null | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the implications of coupling a topological quantum field
theory (TQFT) to Yang-Mills theory with $SU(N)$ gauge group in the context of
the IR-renormalon problem. Coupling a TQFT to QFT does not change the local
dynamics and perturbation theory, but it does change the bundle topology.
Crucially, the con... | [
{
"created": "Mon, 28 Jun 2021 20:34:04 GMT",
"version": "v1"
}
] | 2021-07-02 | [
[
"Ünsal",
"Mithat",
""
]
] | We investigate the implications of coupling a topological quantum field theory (TQFT) to Yang-Mills theory with $SU(N)$ gauge group in the context of the IR-renormalon problem. Coupling a TQFT to QFT does not change the local dynamics and perturbation theory, but it does change the bundle topology. Crucially, the confi... | 14.441 | 12.467568 | 16.208225 | 13.635789 | 13.878963 | 14.422829 | 13.947942 | 13.593999 | 13.710709 | 17.528217 | 13.187264 | 14.228395 | 14.247503 | 13.948533 | 13.781561 | 13.330228 | 13.695951 | 13.696944 | 13.94425 | 14.505002 | 13.909038 |
1301.0508 | Eiji Konishi | Eiji Konishi | Time and a Temporally Statistical Quantum Geometrodynamics | Review, 89 pages, version to be published, v3 | Int.J.Mod.Phys.A.28:1330015,2013 | 10.1142/S0217751X13300159 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper is an exposition of the author's recent work (arXiv:1001.3382
[hep-th], arXiv:1005.5430 [cond-mat.dis-nn], arXiv:1212.4956 [quant-ph]) on
modeling M-theory vacua and quantum mechanical observers in the framework of a
temporally statistical description of quantum geometrodynamics, including
measurement proc... | [
{
"created": "Thu, 3 Jan 2013 17:08:41 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Feb 2013 14:54:05 GMT",
"version": "v2"
},
{
"created": "Sun, 31 Mar 2013 14:53:01 GMT",
"version": "v3"
}
] | 2015-06-12 | [
[
"Konishi",
"Eiji",
""
]
] | This paper is an exposition of the author's recent work (arXiv:1001.3382 [hep-th], arXiv:1005.5430 [cond-mat.dis-nn], arXiv:1212.4956 [quant-ph]) on modeling M-theory vacua and quantum mechanical observers in the framework of a temporally statistical description of quantum geometrodynamics, including measurement proces... | 11.97107 | 13.633724 | 12.325133 | 12.030432 | 12.33115 | 12.399405 | 13.497639 | 11.895952 | 12.742621 | 13.33134 | 12.044182 | 12.489636 | 12.313951 | 12.124672 | 12.264845 | 12.234034 | 11.975475 | 12.169645 | 11.771273 | 12.19873 | 12.150771 |
hep-th/0108050 | Marco Cavaglia | Marco Cavaglia, Alessandro Fabbri | Quantum gravitational corrections to black hole geometries | 15 pages, 6 figures. Revised version: Introduction and conclusion
expanded, section II reshaped, references added. Accepted for publication in
Phys. Rev. D | Phys.Rev. D65 (2002) 044012 | 10.1103/PhysRevD.65.044012 | MIT-CTP-3172 | hep-th gr-qc | null | We calculate perturbative quantum gravity corrections to eternal
two-dimensional black holes. We estimate the leading corrections to the AdS_2
black hole entropy and determine the quantum modification of N-dimensional
Schwarzschild spacetime.
| [
{
"created": "Wed, 8 Aug 2001 14:20:46 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Oct 2001 13:55:04 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Cavaglia",
"Marco",
""
],
[
"Fabbri",
"Alessandro",
""
]
] | We calculate perturbative quantum gravity corrections to eternal two-dimensional black holes. We estimate the leading corrections to the AdS_2 black hole entropy and determine the quantum modification of N-dimensional Schwarzschild spacetime. | 18.348919 | 15.610271 | 18.662605 | 15.233477 | 15.427383 | 16.57065 | 15.734385 | 15.503436 | 14.233823 | 18.977015 | 16.79652 | 17.268562 | 16.282654 | 16.587685 | 17.364557 | 17.804552 | 16.53553 | 17.552744 | 15.496427 | 15.655549 | 16.272655 |
hep-th/0501010 | Kluson Josef | J.Kluson | Non-BPS Dp-Brane in Dk-Brane Background | 23 pages,typos fixed,discussion in section devoted to the time
dependent tachyon condensation corrected | JHEP 0503 (2005) 044 | 10.1088/1126-6708/2005/03/044 | null | hep-th | null | In this paper we will study the dynamics of a non-BPS Dp-brane in the
background of N BPS Dk-branes.
| [
{
"created": "Mon, 3 Jan 2005 12:12:43 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jan 2005 09:50:34 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Kluson",
"J.",
""
]
] | In this paper we will study the dynamics of a non-BPS Dp-brane in the background of N BPS Dk-branes. | 9.189463 | 4.793505 | 8.230009 | 5.058659 | 5.128629 | 5.185067 | 5.115793 | 4.613815 | 5.431426 | 7.349479 | 5.296585 | 5.618212 | 7.278157 | 5.996169 | 6.221564 | 5.667662 | 5.404874 | 5.609767 | 5.995129 | 7.081914 | 6.178763 |
2303.12028 | Junchen Rong | Junchen Rong | Scalar CFTs from structural phase transitions | 35 pages, 16 figures | null | null | null | hep-th cond-mat.stat-mech | http://creativecommons.org/licenses/by/4.0/ | We discuss scalar conformal field theories (CFTs) that can be realized in
structural phase transitions. The Landau condition and Lifshitz condition are
reviewed, which are necessary conditions for a structural phase transition to
be second order. We also review the perturbative analysis in $4-\epsilon$
expansion of t... | [
{
"created": "Tue, 21 Mar 2023 17:12:42 GMT",
"version": "v1"
}
] | 2023-03-22 | [
[
"Rong",
"Junchen",
""
]
] | We discuss scalar conformal field theories (CFTs) that can be realized in structural phase transitions. The Landau condition and Lifshitz condition are reviewed, which are necessary conditions for a structural phase transition to be second order. We also review the perturbative analysis in $4-\epsilon$ expansion of the... | 9.034347 | 8.969107 | 9.853219 | 8.270041 | 10.063691 | 10.115581 | 8.990899 | 9.054273 | 8.513725 | 9.918604 | 8.255529 | 8.654824 | 9.52276 | 8.772446 | 8.687099 | 8.942267 | 8.849196 | 8.817434 | 8.839291 | 8.791099 | 8.547872 |
1103.4179 | Yeuan-Ming Sheu | H. M. Fried (Brown), T. Grandou (INLN), Y.-M. Sheu (INLN) | A Non-Perturbative Gauge-Invariant QCD: Ideal vs. Realistic QCD | 21 pages, 3 figures, the third piece of a series (Eur. Phys. J. C65,
395 (2010) and arXiv:1003.2936[hep-th]). Additional proof has been added
along with 2 appendices for more details in the main text | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A basic distinction, long overlooked, between the conventional, "idealistic"
formulation of QCD, and a more "realistic" formulation is brought into focus by
a rigorous, non-perturbative, gauge-invariant evaluation of the Schwinger
solution for the QCD generating functional in terms of exact Fradkin
representations fo... | [
{
"created": "Tue, 22 Mar 2011 00:34:04 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jun 2011 02:53:53 GMT",
"version": "v2"
}
] | 2011-06-07 | [
[
"Fried",
"H. M.",
"",
"Brown"
],
[
"Grandou",
"T.",
"",
"INLN"
],
[
"Sheu",
"Y. -M.",
"",
"INLN"
]
] | A basic distinction, long overlooked, between the conventional, "idealistic" formulation of QCD, and a more "realistic" formulation is brought into focus by a rigorous, non-perturbative, gauge-invariant evaluation of the Schwinger solution for the QCD generating functional in terms of exact Fradkin representations for ... | 14.412874 | 16.235701 | 15.092036 | 13.896926 | 14.99796 | 14.835999 | 15.506198 | 15.124288 | 14.566683 | 15.157918 | 14.798495 | 14.58962 | 14.592994 | 14.058459 | 14.44007 | 14.390594 | 14.360751 | 13.829376 | 14.426681 | 14.074828 | 14.35115 |
2009.05787 | Katarzyna Ole\'s | C. Adam, C. Naya, K. Oles, T. Romanczukiewicz, J. Sanchez-Guillen, and
A. Wereszczynski | Incompressible topological solitons | reference added | Phys. Rev. D 102, 105007 (2020) | 10.1103/PhysRevD.102.105007 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discover a new class of topological solitons. These solitons can exist in
a space of infinite volume like, e.g., $\mathbb{R}^n$, but they cannot be
placed in any finite volume, because the resulting formal solutions have
infinite energy. These objects are, therefore, interpreted as totally
incompressible solitons.... | [
{
"created": "Sat, 12 Sep 2020 13:21:16 GMT",
"version": "v1"
},
{
"created": "Sun, 20 Sep 2020 19:00:00 GMT",
"version": "v2"
}
] | 2020-11-18 | [
[
"Adam",
"C.",
""
],
[
"Naya",
"C.",
""
],
[
"Oles",
"K.",
""
],
[
"Romanczukiewicz",
"T.",
""
],
[
"Sanchez-Guillen",
"J.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | We discover a new class of topological solitons. These solitons can exist in a space of infinite volume like, e.g., $\mathbb{R}^n$, but they cannot be placed in any finite volume, because the resulting formal solutions have infinite energy. These objects are, therefore, interpreted as totally incompressible solitons. A... | 10.274824 | 10.020432 | 10.755738 | 9.869062 | 9.7152 | 9.295678 | 10.966987 | 9.682519 | 9.91181 | 11.580122 | 9.814828 | 9.905303 | 10.078205 | 9.927954 | 10.016897 | 10.337628 | 9.870253 | 10.254454 | 10.036995 | 9.824616 | 10.097449 |
hep-th/0410217 | Cecilia Albertsson | Cecilia Albertsson, Ulf Lindstrom and Maxim Zabzine | T-duality for the sigma model with boundaries | 48 pages, LaTeX, v2: typos corrected, references added | JHEP0412:056,2004 | 10.1088/1126-6708/2004/12/056 | ITP-UH-24/04, UUITP-24/04, HIP-2004-54/TH | hep-th | null | We derive the most general local boundary conditions necessary for T-duality
to be compatible with superconformal invariance of the two-dimensional N=1
supersymmetric nonlinear sigma model with boundaries. To this end, we construct
a consistent gauge invariant parent action by gauging a U(1) isometry, with and
withou... | [
{
"created": "Thu, 21 Oct 2004 07:51:18 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jan 2005 16:43:32 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Albertsson",
"Cecilia",
""
],
[
"Lindstrom",
"Ulf",
""
],
[
"Zabzine",
"Maxim",
""
]
] | We derive the most general local boundary conditions necessary for T-duality to be compatible with superconformal invariance of the two-dimensional N=1 supersymmetric nonlinear sigma model with boundaries. To this end, we construct a consistent gauge invariant parent action by gauging a U(1) isometry, with and without ... | 7.467427 | 7.098839 | 8.332824 | 7.118101 | 8.323511 | 7.466398 | 8.084296 | 6.588814 | 7.051356 | 9.313745 | 6.983994 | 6.950502 | 7.905493 | 7.264962 | 7.078611 | 6.964316 | 6.942893 | 7.056443 | 6.966167 | 7.40142 | 7.033765 |
hep-th/0407080 | Chryssomalis Chryssomalakos | C. Chryssomalakos and E. Okon | Linear Form of 3-scale Relativity Algebra and the Relevance of Stability | 5 pages | Int.J.Mod.Phys. D13 (2004) 1817-1822 | 10.1142/S0218271804005225 | null | hep-th | null | We show that the algebra of the recently proposed Triply Special Relativity
can be brought to a linear (ie, Lie) form by a correct identification of its
generators. The resulting Lie algebra is the stable form proposed by Vilela
Mendes a decade ago, itself a reapparition of Yang's algebra, dating from 1947.
As a coro... | [
{
"created": "Sun, 11 Jul 2004 07:35:31 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Chryssomalakos",
"C.",
""
],
[
"Okon",
"E.",
""
]
] | We show that the algebra of the recently proposed Triply Special Relativity can be brought to a linear (ie, Lie) form by a correct identification of its generators. The resulting Lie algebra is the stable form proposed by Vilela Mendes a decade ago, itself a reapparition of Yang's algebra, dating from 1947. As a coroll... | 15.24025 | 16.071077 | 15.52133 | 13.872413 | 15.801075 | 14.91007 | 14.315544 | 15.064516 | 13.831484 | 17.039291 | 13.371337 | 13.823025 | 14.402042 | 13.623154 | 13.385742 | 13.422469 | 13.116777 | 13.780273 | 13.914368 | 13.322984 | 14.266239 |
2307.00554 | Olivera Miskovic | Olivera Miskovic, Rodrigo Olea, Eleftherios Papantonopoulos, Yoel
Parra-Cisterna | Asymptotic Black Holes and Conformal Mass in AdS Quadratic Curvature
Gravity | 38 pages, no figures; in v2, one reference added | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We explore the consistent truncation of conserved charges in Quadratic
Curvature Gravity (QCG) with anti-de Sitter asymptotics to the linear order in
the Weyl tensor. The QCG action is given by the most general curvature-squared
corrections to Einstein gravity, and it is suitably rendered finite by the
addition of ex... | [
{
"created": "Sun, 2 Jul 2023 12:33:40 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Aug 2023 12:58:52 GMT",
"version": "v2"
}
] | 2023-08-29 | [
[
"Miskovic",
"Olivera",
""
],
[
"Olea",
"Rodrigo",
""
],
[
"Papantonopoulos",
"Eleftherios",
""
],
[
"Parra-Cisterna",
"Yoel",
""
]
] | We explore the consistent truncation of conserved charges in Quadratic Curvature Gravity (QCG) with anti-de Sitter asymptotics to the linear order in the Weyl tensor. The QCG action is given by the most general curvature-squared corrections to Einstein gravity, and it is suitably rendered finite by the addition of extr... | 12.139119 | 11.405731 | 11.8811 | 11.023409 | 11.279794 | 11.532957 | 10.973589 | 10.752326 | 11.301517 | 13.376896 | 11.049058 | 11.509318 | 11.398288 | 11.499365 | 11.431581 | 11.114253 | 11.540469 | 11.314092 | 11.732512 | 11.883205 | 11.475835 |
1510.03954 | Dmitri Vassilevich | Dmitri Vassilevich | Can Spectral Action be a Window to Very High Energies? | A talk at "Integrable systems and quantum symmetries", Prague, 2015.
To be published in the Proceedings | null | 10.1088/1742-6596/670/1/012050 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The principles of noncommutative geometry impose severe restrictions on the
structure of (almost) commutative field theories. The Standard Model fits
surprisingly well into the noncommutative framework. Here we overview some
universal predictions of the spectral action principle for the behavior of
bosonic theories a... | [
{
"created": "Wed, 14 Oct 2015 03:17:36 GMT",
"version": "v1"
}
] | 2016-02-17 | [
[
"Vassilevich",
"Dmitri",
""
]
] | The principles of noncommutative geometry impose severe restrictions on the structure of (almost) commutative field theories. The Standard Model fits surprisingly well into the noncommutative framework. Here we overview some universal predictions of the spectral action principle for the behavior of bosonic theories at ... | 12.00855 | 9.513688 | 10.780639 | 9.796845 | 10.805335 | 11.821769 | 11.742475 | 10.129176 | 10.673436 | 12.913211 | 10.401744 | 11.138202 | 12.355912 | 11.49129 | 10.828207 | 11.271477 | 11.336673 | 10.955416 | 11.598144 | 11.664986 | 11.270958 |
1807.01578 | Timothy Andersen | Timothy D. Andersen | Quantization of Fields by Averaging Classical Evolution Equations | 20 pages, 4 feynman diagrams, accepted for publication in Physical
Review D | Phys. Rev. D 99, 016012 (2019) | 10.1103/PhysRevD.99.016012 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | This paper extends the formalism for quantizing field theories via a
microcanonical quantum field theory and Hamilton's principle to classical
evolution equations. These are based on the well-known correspondence under a
Wick rotation between quantum field theories and 4-D statistical mechanical
theories. By placing ... | [
{
"created": "Tue, 3 Jul 2018 16:04:39 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jan 2019 15:50:09 GMT",
"version": "v2"
}
] | 2019-01-23 | [
[
"Andersen",
"Timothy D.",
""
]
] | This paper extends the formalism for quantizing field theories via a microcanonical quantum field theory and Hamilton's principle to classical evolution equations. These are based on the well-known correspondence under a Wick rotation between quantum field theories and 4-D statistical mechanical theories. By placing qu... | 19.201414 | 20.800266 | 20.609337 | 20.36503 | 20.912203 | 22.567383 | 21.166403 | 21.249027 | 20.74913 | 22.357109 | 19.430836 | 19.296459 | 18.73546 | 18.752451 | 19.072676 | 18.909193 | 18.958008 | 18.458786 | 18.759642 | 19.068394 | 18.443512 |
hep-th/0507260 | Peter Shepard | Peter G. Shepard (UC Berkeley) | Black Hole Statistics from Holography | 21 pages, 4 figures; References added | JHEP 0510 (2005) 072 | 10.1088/1126-6708/2005/10/072 | null | hep-th | null | We study the microstates of the ``small'' black hole in the $\half$-BPS
sector of AdS$_5\times S^5$, the superstar of Myers and Tafjord, using the
powerful holographic description provided by LLM. The system demonstrates the
inherently statistical nature of black holes, with the geometry of Myer and
Tafjord emerging ... | [
{
"created": "Wed, 27 Jul 2005 19:40:39 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Aug 2005 19:30:30 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Shepard",
"Peter G.",
"",
"UC Berkeley"
]
] | We study the microstates of the ``small'' black hole in the $\half$-BPS sector of AdS$_5\times S^5$, the superstar of Myers and Tafjord, using the powerful holographic description provided by LLM. The system demonstrates the inherently statistical nature of black holes, with the geometry of Myer and Tafjord emerging on... | 14.796124 | 14.295677 | 17.857901 | 14.288715 | 14.548658 | 12.985239 | 14.274885 | 14.642521 | 14.097645 | 19.49966 | 14.471107 | 14.179862 | 16.251028 | 14.339117 | 14.521349 | 13.784334 | 13.782094 | 14.216628 | 14.168214 | 15.353498 | 13.886148 |
0712.1116 | Liuba Mazzanti | Liuba Mazzanti | Topics in noncommutative integrable theories and holographic brane-world
cosmology | Ph.D. Thesis, 256 pages, 6 figures, references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This thesis follows two main lines of research, both related to relevant
aspects of string theory and its phenomenological/cosmological applications. We
study two different generalizations of the integrable SG model to NC geometry,
after discussing general properties and issues of integrable theories and NC
field the... | [
{
"created": "Fri, 7 Dec 2007 11:27:00 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 2008 17:51:12 GMT",
"version": "v2"
}
] | 2008-08-06 | [
[
"Mazzanti",
"Liuba",
""
]
] | This thesis follows two main lines of research, both related to relevant aspects of string theory and its phenomenological/cosmological applications. We study two different generalizations of the integrable SG model to NC geometry, after discussing general properties and issues of integrable theories and NC field theor... | 11.474741 | 12.083912 | 12.462061 | 11.306558 | 11.671007 | 11.849385 | 11.945336 | 11.528337 | 11.849996 | 12.477631 | 11.269897 | 11.381063 | 11.634735 | 11.413456 | 11.570858 | 11.434295 | 11.252891 | 11.297394 | 11.328908 | 11.778897 | 11.364016 |
hep-th/0008225 | Francesco Fucito | Ugo Bruzzo, Francesco Fucito, Alessandro Tanzini and Gabriele
Travaglini | On the Multi-Instanton Measure for Super Yang--Mills Theories | 28 pages, latex file | Nucl.Phys. B611 (2001) 205-226 | 10.1016/S0550-3213(01)00349-2 | ROM2F/2000/25, SISSA 74/2000/fm | hep-th | null | In this paper we revisit the arguments that have led to the proposal of a
multi-instanton measure for supersymmetric Yang-Mills theories. We then recall
how the moduli space of gauge connections on $\real^4$ can be built from a
hyperk\"ahler quotient construction which we generalize to supermanifolds. The
measure we ... | [
{
"created": "Tue, 29 Aug 2000 16:12:41 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bruzzo",
"Ugo",
""
],
[
"Fucito",
"Francesco",
""
],
[
"Tanzini",
"Alessandro",
""
],
[
"Travaglini",
"Gabriele",
""
]
] | In this paper we revisit the arguments that have led to the proposal of a multi-instanton measure for supersymmetric Yang-Mills theories. We then recall how the moduli space of gauge connections on $\real^4$ can be built from a hyperk\"ahler quotient construction which we generalize to supermanifolds. The measure we ar... | 8.732778 | 7.990814 | 9.408516 | 7.437701 | 7.756153 | 8.865102 | 8.318037 | 8.008708 | 7.779383 | 10.317663 | 7.734747 | 7.733347 | 8.291422 | 7.845414 | 7.811067 | 7.904227 | 7.827067 | 7.95509 | 7.90342 | 8.153596 | 7.715322 |
1103.1169 | Jonathan L. Bougie | Jonathan Bougie, Asim Gangopadhyaya, and Jeffry V. Mallow | Method for Generating Additive Shape Invariant Potentials from an Euler
Equation | 1 figure, 4 tables, 18 pages | J. Phys. A: Math. Theor. 44 (2011) 275307 | 10.1088/1751-8113/44/27/275307 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the supersymmetric quantum mechanics formalism, the shape invariance
condition provides a sufficient constraint to make a quantum mechanical problem
solvable; i.e., we can determine its eigenvalues and eigenfunctions
algebraically. Since shape invariance relates superpotentials and their
derivatives at two differe... | [
{
"created": "Sun, 6 Mar 2011 22:29:52 GMT",
"version": "v1"
}
] | 2011-11-10 | [
[
"Bougie",
"Jonathan",
""
],
[
"Gangopadhyaya",
"Asim",
""
],
[
"Mallow",
"Jeffry V.",
""
]
] | In the supersymmetric quantum mechanics formalism, the shape invariance condition provides a sufficient constraint to make a quantum mechanical problem solvable; i.e., we can determine its eigenvalues and eigenfunctions algebraically. Since shape invariance relates superpotentials and their derivatives at two different... | 8.24652 | 7.83407 | 10.12517 | 8.09438 | 9.721172 | 8.362866 | 8.236141 | 8.402488 | 7.846845 | 10.493224 | 7.830121 | 8.288554 | 8.97382 | 7.992706 | 8.447266 | 8.07291 | 8.089643 | 7.929988 | 8.376673 | 8.572722 | 7.893718 |
hep-th/0604004 | Leonid Lantsman | Leonid Lantsman | Dirac fundamental quantization of gauge theories is natural way of
reference frames in modern physics | v5; the specific approach to the mass gab problem in the Minkowskian
BPS monopole model quantized by Dirac was pointed (see p.37 of the present
issue); some references are added | Fizika B18:99-140,2009 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyse two principal approaches to the quantization of physical models
worked out to date. There are the Faddeev-Popov "heuristic" approach, based on
fixing a gauge in the FP path integrals formalism, and the "fundamental"
approach by Dirac based on the constraint-shell reduction of Hamiltonians with
deleting unp... | [
{
"created": "Sun, 2 Apr 2006 10:12:06 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Apr 2006 13:57:36 GMT",
"version": "v2"
},
{
"created": "Tue, 16 May 2006 14:07:01 GMT",
"version": "v3"
},
{
"created": "Sun, 19 Nov 2006 11:55:11 GMT",
"version": "v4"
},
{
"cre... | 2014-11-18 | [
[
"Lantsman",
"Leonid",
""
]
] | We analyse two principal approaches to the quantization of physical models worked out to date. There are the Faddeev-Popov "heuristic" approach, based on fixing a gauge in the FP path integrals formalism, and the "fundamental" approach by Dirac based on the constraint-shell reduction of Hamiltonians with deleting unphy... | 16.191196 | 18.433701 | 17.146614 | 16.682854 | 18.326338 | 18.356775 | 17.403227 | 16.409424 | 16.972137 | 19.420544 | 16.711296 | 16.454588 | 16.72366 | 16.153831 | 16.627348 | 16.288574 | 16.213911 | 16.20882 | 16.375946 | 16.82044 | 16.364744 |
1905.03780 | Jordan Cotler | Jordan Cotler, Kristan Jensen, Alexander Maloney | Low-dimensional de Sitter quantum gravity | 106 pages, 13 figures; v2: published version, subsection on complex
metrics added | null | 10.1007/JHEP06(2020)048 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study aspects of Jackiw-Teitelboim (JT) quantum gravity in two-dimensional
nearly de Sitter (dS) spacetime, as well as pure de Sitter quantum gravity in
three dimensions. These are each theories of boundary modes, which include a
reparameterization field on each connected component of the boundary as well as
topol... | [
{
"created": "Thu, 9 May 2019 17:59:57 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Jun 2020 16:55:19 GMT",
"version": "v2"
}
] | 2020-07-15 | [
[
"Cotler",
"Jordan",
""
],
[
"Jensen",
"Kristan",
""
],
[
"Maloney",
"Alexander",
""
]
] | We study aspects of Jackiw-Teitelboim (JT) quantum gravity in two-dimensional nearly de Sitter (dS) spacetime, as well as pure de Sitter quantum gravity in three dimensions. These are each theories of boundary modes, which include a reparameterization field on each connected component of the boundary as well as topolog... | 6.398051 | 5.948775 | 7.144681 | 5.83854 | 6.14471 | 6.128041 | 6.117426 | 5.853092 | 5.934156 | 7.369576 | 6.083746 | 6.389565 | 6.415564 | 6.299951 | 6.352131 | 6.102044 | 6.277166 | 6.130083 | 6.196728 | 6.482428 | 6.01699 |
2203.15744 | Richard Szabo | Richard J. Szabo | The $L_{\infty}$-structure of noncommutative gravity | 22 pages; v2: typos corrected; Contribution to the Proceedings of the
Humboldt Kolleg on "Quantum Gravity and Fundamental Interactions", Corfu
Summer Institute on Elementary Particle Physics and Gravity, 29 August-9
October 2021, Corfu, Greece | null | null | EMPG-22-06 | hep-th gr-qc math-ph math.MP math.QA | http://creativecommons.org/licenses/by/4.0/ | We summarise recent perspectives on symmetries of noncommutative field
theories based on homotopy algebras. We show how these viewpoints naturally
lead to a new class of noncommutative field theories which possess braided
gauge symmetries, and explain in detail their uses in gravity. We review how
these consideration... | [
{
"created": "Tue, 29 Mar 2022 16:52:43 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Mar 2022 09:12:32 GMT",
"version": "v2"
}
] | 2022-04-01 | [
[
"Szabo",
"Richard J.",
""
]
] | We summarise recent perspectives on symmetries of noncommutative field theories based on homotopy algebras. We show how these viewpoints naturally lead to a new class of noncommutative field theories which possess braided gauge symmetries, and explain in detail their uses in gravity. We review how these considerations ... | 9.684092 | 8.102623 | 8.542778 | 7.939998 | 7.971525 | 7.654997 | 7.885411 | 8.010994 | 7.546568 | 9.27299 | 7.423045 | 8.258152 | 8.269102 | 8.10743 | 7.876135 | 8.181173 | 8.087105 | 8.008718 | 7.814854 | 8.086258 | 7.649203 |
1412.7541 | Balt van Rees | Christopher Beem, Madalena Lemos, Pedro Liendo, Leonardo Rastelli,
Balt C. van Rees | The ${\mathcal N}=2$ superconformal bootstrap | 92 pages (64 pages + 5 appendices), 27 figures; v2: minor
improvements, results unchanged | JHEP 1603 (2016) 183 | 10.1007/JHEP03(2016)183 | YITP-SB-14-54, CERN-PH-TH-2014-269, HU-EP-14/61 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we initiate the conformal bootstrap program for ${\mathcal N}=2$
superconformal field theories in four dimensions. We promote an abstract
operator-algebraic viewpoint in order to unify the description of Lagrangian
and non-Lagrangian theories, and formulate various conjectures concerning the
landscape of... | [
{
"created": "Tue, 23 Dec 2014 21:00:06 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Dec 2015 17:36:54 GMT",
"version": "v2"
}
] | 2019-03-25 | [
[
"Beem",
"Christopher",
""
],
[
"Lemos",
"Madalena",
""
],
[
"Liendo",
"Pedro",
""
],
[
"Rastelli",
"Leonardo",
""
],
[
"van Rees",
"Balt C.",
""
]
] | In this work we initiate the conformal bootstrap program for ${\mathcal N}=2$ superconformal field theories in four dimensions. We promote an abstract operator-algebraic viewpoint in order to unify the description of Lagrangian and non-Lagrangian theories, and formulate various conjectures concerning the landscape of t... | 5.151763 | 5.468086 | 6.059782 | 5.177271 | 5.461109 | 5.186201 | 5.456997 | 5.169722 | 5.370921 | 6.064829 | 5.284861 | 5.244111 | 5.39028 | 5.081357 | 5.224144 | 5.153711 | 5.256263 | 5.032208 | 5.152215 | 5.422901 | 5.161449 |
hep-th/9301117 | John Gracey | J.A. Gracey | Analysis of Abelian Gauge Theory with Four Fermi Interaction at
$O(1/N^2)$ in Arbitrary Dimensions | latex, 13 pages, 4 figures available on request from the author,
LTH-297 | J.Phys. A26 (1993) 1431-1440 | 10.1088/0305-4470/26/6/024 | null | hep-th | null | An arbitrary dimensional expression is given for the anomalous dimension of
the fermion field in a model with a four point interaction and a $U(1)$ gauge
field, at $O(1/N^2)$ within a large flavour expansion in the Landau gauge.
| [
{
"created": "Thu, 28 Jan 1993 08:58:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Gracey",
"J. A.",
""
]
] | An arbitrary dimensional expression is given for the anomalous dimension of the fermion field in a model with a four point interaction and a $U(1)$ gauge field, at $O(1/N^2)$ within a large flavour expansion in the Landau gauge. | 13.333385 | 8.970258 | 12.409981 | 10.374785 | 9.965947 | 10.573741 | 11.916027 | 9.486691 | 10.299129 | 11.87919 | 10.230466 | 10.899807 | 11.551659 | 10.551542 | 10.885345 | 10.976195 | 10.745105 | 11.009013 | 10.85934 | 11.658693 | 10.416382 |
2010.00897 | Arkadii Kozhevnikov | A. A. Kozhevnikov | Shape and dynamics of nonrelativistic vortex strings in parity-breaking
media | 8 pages, 1 figure. Copy-paste errors in Eqs. (2.14), (3.2), and (5.4)
are corrected | Phys. Rev. D 103, 025025 (2021) | 10.1103/PhysRevD.103.025025 | null | hep-th cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The shape and dynamics of the nonrelativistic gauge vortex string in the
parity-broken media is considered, upon reducing the problem to finding the
extremum of the Abelian Higgs model effective action with the fixed B-type
helicity of the gauge field. It is shown that in contrast with the case of the
fixed A-type he... | [
{
"created": "Fri, 2 Oct 2020 09:52:08 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Feb 2021 04:55:46 GMT",
"version": "v2"
},
{
"created": "Mon, 24 May 2021 04:30:52 GMT",
"version": "v3"
}
] | 2021-05-25 | [
[
"Kozhevnikov",
"A. A.",
""
]
] | The shape and dynamics of the nonrelativistic gauge vortex string in the parity-broken media is considered, upon reducing the problem to finding the extremum of the Abelian Higgs model effective action with the fixed B-type helicity of the gauge field. It is shown that in contrast with the case of the fixed A-type heli... | 12.981085 | 12.855004 | 13.539519 | 12.995605 | 13.671737 | 13.53799 | 13.999815 | 12.858342 | 12.849423 | 15.442626 | 12.345861 | 12.489857 | 12.410812 | 12.235755 | 12.043365 | 12.653635 | 12.671505 | 12.393042 | 12.325251 | 12.989543 | 12.297352 |
2108.04469 | Hun Jang | Hun Jang and Massimo Porrati | Component Actions of Liberated $\mathcal{N} = 1$ Supergravity and New
Fayet-Iliopoulos Terms in Superconformal Tensor Calculus | 37 pages | JHEP 11 (2021) 075 | 10.1007/JHEP11(2021)075 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly compute the component action of certain recently discovered new
$\mathcal{N} = 1$ supergravity actions which enlarge the space of scalar
potentials allowed by supersymmetry and also contain fermionic interaction
terms that become singular when supersymmetry is unbroken. They are the
"Liberated Supergrav... | [
{
"created": "Tue, 10 Aug 2021 06:29:51 GMT",
"version": "v1"
}
] | 2021-11-23 | [
[
"Jang",
"Hun",
""
],
[
"Porrati",
"Massimo",
""
]
] | We explicitly compute the component action of certain recently discovered new $\mathcal{N} = 1$ supergravity actions which enlarge the space of scalar potentials allowed by supersymmetry and also contain fermionic interaction terms that become singular when supersymmetry is unbroken. They are the "Liberated Supergravit... | 9.632096 | 10.818914 | 12.560895 | 10.895 | 11.829597 | 11.949122 | 12.882884 | 11.389337 | 10.608719 | 12.800021 | 10.694104 | 8.695989 | 9.676085 | 9.182265 | 9.366881 | 8.942428 | 9.177982 | 8.931273 | 9.252042 | 9.857981 | 9.170285 |
1907.03571 | Bojan Nikoli\'c | B. Nikoli\'c and B. Sazdovi\'c | Advantage of the second-order formalism in double space T-dualization of
type II superstring | null | Eur. Phys. J. C (2019) 79:819 | 10.1140/epjc/s10052-019-7338-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we present bosonic T-dualization in double space of the type
II superstring theory in pure spinor formulation. We use the action with
constant background fields obtained from the general case under some physically
and mathematically justified assumptions. Unlike Ref.\cite{bnbstip2}, where we
used the ... | [
{
"created": "Mon, 8 Jul 2019 12:57:31 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Oct 2019 11:33:29 GMT",
"version": "v2"
}
] | 2019-10-08 | [
[
"Nikolić",
"B.",
""
],
[
"Sazdović",
"B.",
""
]
] | In this article we present bosonic T-dualization in double space of the type II superstring theory in pure spinor formulation. We use the action with constant background fields obtained from the general case under some physically and mathematically justified assumptions. Unlike Ref.\cite{bnbstip2}, where we used the fi... | 8.194521 | 7.713565 | 8.78631 | 7.79542 | 8.699582 | 8.351131 | 8.336492 | 7.646763 | 7.742721 | 9.29532 | 8.143683 | 7.707031 | 8.362849 | 7.931625 | 8.016457 | 7.964173 | 8.141627 | 7.944067 | 7.970947 | 8.300649 | 7.781941 |
0903.1400 | Zhan-Yun Wang | Zhan-Yun Wang, Xiao-Ning Xie, Jun Feng, Yao-Xiong Wang, Yu Zeng and
Kang-Jie Shi | Solution Transformations for GS String in AdS_5 x S^5 by Conserved
Quantities | 34 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For Light-cone gauge of Green-Schwarz superstring in AdS_5 x S^5 background,
we fix two bosonic variables x^{+}=\tau and y^{9}=\sigma, and then perform the
partial Legendre transformation of the remaining bosonic variables. We then
obtain a Lagrangian which is linear in velocity after eliminating the metric of
world ... | [
{
"created": "Sun, 8 Mar 2009 09:22:40 GMT",
"version": "v1"
}
] | 2009-03-10 | [
[
"Wang",
"Zhan-Yun",
""
],
[
"Xie",
"Xiao-Ning",
""
],
[
"Feng",
"Jun",
""
],
[
"Wang",
"Yao-Xiong",
""
],
[
"Zeng",
"Yu",
""
],
[
"Shi",
"Kang-Jie",
""
]
] | For Light-cone gauge of Green-Schwarz superstring in AdS_5 x S^5 background, we fix two bosonic variables x^{+}=\tau and y^{9}=\sigma, and then perform the partial Legendre transformation of the remaining bosonic variables. We then obtain a Lagrangian which is linear in velocity after eliminating the metric of world sh... | 13.93233 | 14.951539 | 16.913477 | 13.563457 | 14.147546 | 15.689193 | 16.573923 | 13.74622 | 13.357955 | 18.733379 | 14.380677 | 13.137127 | 14.901463 | 13.046614 | 13.064511 | 13.347421 | 12.788912 | 13.169098 | 13.039745 | 14.894392 | 13.355328 |
1711.08403 | Jose M. Carmona | J.M. Carmona, J.L. Cortes, J.J. Relancio | Spacetime from locality of interactions in deformations of special
relativity: the example of $\kappa$-Poincar\'e Hopf algebra | 14 pages | Phys. Rev. D 97, 064025 (2018) | 10.1103/PhysRevD.97.064025 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new proposal for the notion of spacetime in a relativistic generalization
of special relativity based on a modification of the composition law of momenta
is presented. Locality of interactions is the principle which defines the
spacetime structure for a system of particles. The formulation based on
$\kappa$-Poincar... | [
{
"created": "Wed, 22 Nov 2017 17:26:22 GMT",
"version": "v1"
}
] | 2018-03-28 | [
[
"Carmona",
"J. M.",
""
],
[
"Cortes",
"J. L.",
""
],
[
"Relancio",
"J. J.",
""
]
] | A new proposal for the notion of spacetime in a relativistic generalization of special relativity based on a modification of the composition law of momenta is presented. Locality of interactions is the principle which defines the spacetime structure for a system of particles. The formulation based on $\kappa$-Poincar\'... | 9.186063 | 7.005372 | 6.879816 | 6.851255 | 7.227818 | 7.400393 | 7.414391 | 6.537674 | 7.336571 | 7.356087 | 7.033536 | 7.174038 | 7.427786 | 7.277335 | 7.179734 | 7.047823 | 7.210356 | 7.101883 | 7.401542 | 7.095074 | 6.95181 |
hep-th/9508077 | David Lamb | A.Z. Capri, M. Kobayashi, and D.J. Lamb | Two observers calculate the trace anomaly | RevTeX, 13 pages, some typos corrected and an appendix added, this is
the version to appear in Class. and Quantum Gavity | Class.Quant.Grav. 13 (1996) 179-188 | 10.1088/0264-9381/13/2/006 | Alberta Thy 17-95 | hep-th gr-qc | null | We adapt a calculation due to Massacand and Schmid to the coordinate
independent definition of time and vacuum given by Capri and Roy in order to
compute the trace anomaly for a massless scalar field in a curved spacetime in
1+1 dimensions. The computation which requires only a simple regulator and
normal ordering yi... | [
{
"created": "Wed, 16 Aug 1995 19:48:51 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Jan 1996 16:03:56 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Capri",
"A. Z.",
""
],
[
"Kobayashi",
"M.",
""
],
[
"Lamb",
"D. J.",
""
]
] | We adapt a calculation due to Massacand and Schmid to the coordinate independent definition of time and vacuum given by Capri and Roy in order to compute the trace anomaly for a massless scalar field in a curved spacetime in 1+1 dimensions. The computation which requires only a simple regulator and normal ordering yiel... | 19.880682 | 16.349623 | 20.569845 | 18.502626 | 18.423954 | 17.193535 | 21.440863 | 18.707312 | 19.869522 | 22.047674 | 18.593477 | 17.556139 | 19.341105 | 18.032282 | 17.402472 | 18.440786 | 18.074974 | 16.184204 | 18.338774 | 17.395279 | 17.590292 |
1710.08418 | Ying-Hsuan Lin | Chi-Ming Chang, Martin Fluder, Ying-Hsuan Lin, Yifan Wang | Spheres, Charges, Instantons, and Bootstrap: A Five-Dimensional Odyssey | 90 pages, 12 figures, 11 tables; v2: references added; v3: minor
corrections | null | 10.1007/JHEP03(2018)123 | CALT-TH 2017-030, PUPT-2539 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We combine supersymmetric localization and the conformal bootstrap to study
five-dimensional superconformal field theories. To begin, we classify the
admissible counter-terms and derive a general relation between the five-sphere
partition function and the conformal and flavor central charges. Along the way,
we discov... | [
{
"created": "Mon, 23 Oct 2017 18:00:00 GMT",
"version": "v1"
},
{
"created": "Sun, 21 Jan 2018 00:15:36 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Mar 2018 06:53:07 GMT",
"version": "v3"
}
] | 2018-03-28 | [
[
"Chang",
"Chi-Ming",
""
],
[
"Fluder",
"Martin",
""
],
[
"Lin",
"Ying-Hsuan",
""
],
[
"Wang",
"Yifan",
""
]
] | We combine supersymmetric localization and the conformal bootstrap to study five-dimensional superconformal field theories. To begin, we classify the admissible counter-terms and derive a general relation between the five-sphere partition function and the conformal and flavor central charges. Along the way, we discover... | 8.601352 | 8.773906 | 10.139573 | 7.753387 | 8.423828 | 8.035192 | 8.708074 | 8.156954 | 7.684649 | 9.99078 | 7.665066 | 7.603354 | 8.824717 | 8.197171 | 7.855006 | 7.686708 | 7.800395 | 7.951434 | 8.181497 | 8.848743 | 7.619634 |
1811.11572 | Nicol\`o Petri | Giuseppe Dibitetto, Nicol\`o Petri | AdS$_{\textbf{2}}$ solutions and their massive IIA origin | 21 pages, uses jheppub.sty. arXiv admin note: text overlap with
arXiv:1807.07768 | null | 10.1007/JHEP05(2019)107 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider warped $\mathrm{AdS}_2\times \mathcal M_4$ backgrounds within
$F(4)$ gauged supergravity in six dimensions. In particular, we are able to
find supersymmetric solutions of the aforementioned type characterized by
$\textrm{AdS}_{6}$ asymptotics and an $\mathcal M_4$ given by a three-sphere
warped over a seg... | [
{
"created": "Tue, 27 Nov 2018 09:40:24 GMT",
"version": "v1"
}
] | 2019-06-26 | [
[
"Dibitetto",
"Giuseppe",
""
],
[
"Petri",
"Nicolò",
""
]
] | We consider warped $\mathrm{AdS}_2\times \mathcal M_4$ backgrounds within $F(4)$ gauged supergravity in six dimensions. In particular, we are able to find supersymmetric solutions of the aforementioned type characterized by $\textrm{AdS}_{6}$ asymptotics and an $\mathcal M_4$ given by a three-sphere warped over a segme... | 6.868532 | 6.528841 | 7.878129 | 6.398847 | 6.116212 | 6.508023 | 6.562206 | 6.599559 | 6.174447 | 8.348125 | 6.409346 | 6.55197 | 7.367126 | 6.498594 | 6.506893 | 6.563047 | 6.690107 | 6.674507 | 6.518098 | 7.547752 | 6.482098 |
hep-th/9907034 | Sascha Vongehr | Sascha Vongehr | Nature: "I have Two Times" | 8 pages, two formulas corrected | null | null | null | hep-th | null | This is a slightly extended version of a seminar given the 8th of June at the
TASI 99 at Colorado University in Boulder. The motivations behind two time
theory are explained and the theory is introduced via one of the theory's
easier gauges of a particle on a black hole background. Important results that
should be in... | [
{
"created": "Wed, 7 Jul 1999 01:25:52 GMT",
"version": "v1"
},
{
"created": "Sun, 11 Jul 1999 19:33:44 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Vongehr",
"Sascha",
""
]
] | This is a slightly extended version of a seminar given the 8th of June at the TASI 99 at Colorado University in Boulder. The motivations behind two time theory are explained and the theory is introduced via one of the theory's easier gauges of a particle on a black hole background. Important results that should be inte... | 34.529461 | 34.339306 | 30.79059 | 31.110748 | 34.792606 | 30.534359 | 31.828152 | 29.07198 | 29.485447 | 33.934727 | 28.813269 | 28.351753 | 31.372955 | 29.72805 | 29.61146 | 27.676796 | 29.655481 | 29.38406 | 31.18313 | 32.850506 | 28.883589 |
hep-th/0506069 | Bin Wang | Bin Wang, Yungui Gong and Elcio Abdalla | Transition of the dark energy equation of state in an interacting
holographic dark energy model | revised version, references added. Accepted for publication in PLB | Phys.Lett. B624 (2005) 141-146 | 10.1016/j.physletb.2005.08.008 | null | hep-th astro-ph gr-qc | null | A model of holographic dark energy with an interaction with matter fields has
been investigated. Choosing the future event horizon as an IR cutoff, we have
shown that the ratio of energy densities can vary with time. With the
interaction between the two different constituents of the universe, we observed
the evolutio... | [
{
"created": "Thu, 9 Jun 2005 07:15:09 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Aug 2005 13:02:57 GMT",
"version": "v2"
},
{
"created": "Sun, 7 Aug 2005 07:55:39 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Wang",
"Bin",
""
],
[
"Gong",
"Yungui",
""
],
[
"Abdalla",
"Elcio",
""
]
] | A model of holographic dark energy with an interaction with matter fields has been investigated. Choosing the future event horizon as an IR cutoff, we have shown that the ratio of energy densities can vary with time. With the interaction between the two different constituents of the universe, we observed the evolution ... | 9.062676 | 9.954497 | 8.266739 | 7.683919 | 8.931535 | 8.917288 | 8.404013 | 8.719394 | 8.394047 | 8.904245 | 8.182823 | 8.047321 | 8.067146 | 7.896012 | 7.959581 | 8.287181 | 7.996537 | 7.945598 | 8.327889 | 7.952085 | 8.136311 |
hep-th/0205047 | Giovanni Amelino-Camelia | Giovanni Amelino-Camelia, Michele Arzano, Luisa Doplicher | Field Theories on Canonical and Lie-Algebra Noncommutative Spacetimes | 13 pages, LaTex, invited talk given by G. Amelino-Camelia at the 25th
Johns Hopkins Workshop on Current Problems in Particle Theory | null | 10.1142/9789812791368_0027 | null | hep-th | null | Field theories on canonical noncommutative spacetimes, which are being
studied also in connection with string theory, and on $\kappa$-Minkowski
spacetime, which is a popular example of Lie-algebra noncommutative spacetime,
can be naturally constructed by introducing a suitable generating functional
for Green function... | [
{
"created": "Mon, 6 May 2002 16:34:47 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Amelino-Camelia",
"Giovanni",
""
],
[
"Arzano",
"Michele",
""
],
[
"Doplicher",
"Luisa",
""
]
] | Field theories on canonical noncommutative spacetimes, which are being studied also in connection with string theory, and on $\kappa$-Minkowski spacetime, which is a popular example of Lie-algebra noncommutative spacetime, can be naturally constructed by introducing a suitable generating functional for Green functions ... | 10.319516 | 9.804523 | 10.500657 | 9.825347 | 10.162314 | 10.008492 | 10.313753 | 10.425268 | 9.641816 | 10.509967 | 9.397888 | 9.66482 | 9.565503 | 9.49201 | 9.394395 | 9.873273 | 9.504927 | 10.099916 | 9.43307 | 9.513343 | 9.801218 |
1402.2312 | Vyacheslav P. Spiridonov | V.P. Spiridonov and G.S. Vartanov | Vanishing superconformal indices and the chiral symmetry breaking | 26 pp | J. High Energy Phys. 06 (2014) 062 | 10.1007/JHEP06(2014)062 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Superconformal indices of 4d \N=1 SYM theories with SU(N) and SP(2N) gauge
groups are investigated for N_f=N and N_f=N+1 flavors, respectively. These
indices vanish for generic values of the flavor fugacities. However, for a
singular submanifold of fugacities they behave like the Dirac delta functions
and describe th... | [
{
"created": "Mon, 10 Feb 2014 21:36:53 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Jun 2014 11:50:17 GMT",
"version": "v2"
}
] | 2015-06-18 | [
[
"Spiridonov",
"V. P.",
""
],
[
"Vartanov",
"G. S.",
""
]
] | Superconformal indices of 4d \N=1 SYM theories with SU(N) and SP(2N) gauge groups are investigated for N_f=N and N_f=N+1 flavors, respectively. These indices vanish for generic values of the flavor fugacities. However, for a singular submanifold of fugacities they behave like the Dirac delta functions and describe the ... | 8.280867 | 7.427081 | 8.709864 | 7.490312 | 8.31101 | 8.736856 | 7.881774 | 7.720447 | 7.989715 | 8.641807 | 7.426196 | 7.325591 | 7.774693 | 7.155686 | 7.888401 | 7.720917 | 7.487715 | 7.29104 | 7.218508 | 8.463624 | 6.846191 |
hep-th/0409219 | Joaquim Gomis | Joaquim Gomis, Kiyoshi Kamimura and Paul K. Townsend | Non-Relativistic Superbranes | 19 pages, Latex. Small changes, version to appear on JHEP | JHEP0411:051,2004 | 10.1088/1126-6708/2004/11/051 | UB-ECM-PF-04/26, Toho-CP-0476, DAMTP-2004-94 | hep-th | null | Subtleties arising in the non-relativistic limit of relativistic branes are
resolved, and a reparametrization-invariant and kappa-symmetric
non-relativistic super p-brane action is obtained as a limit of the action for
a relativistic super p-brane in a Minkowski vacuum. We give explicit results
for the D0-brane, whic... | [
{
"created": "Wed, 22 Sep 2004 08:46:51 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Oct 2004 12:52:16 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Nov 2004 17:04:47 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Gomis",
"Joaquim",
""
],
[
"Kamimura",
"Kiyoshi",
""
],
[
"Townsend",
"Paul K.",
""
]
] | Subtleties arising in the non-relativistic limit of relativistic branes are resolved, and a reparametrization-invariant and kappa-symmetric non-relativistic super p-brane action is obtained as a limit of the action for a relativistic super p-brane in a Minkowski vacuum. We give explicit results for the D0-brane, which ... | 7.612827 | 6.312435 | 8.132635 | 6.126759 | 7.948366 | 6.17402 | 6.365216 | 5.944703 | 5.942777 | 8.021599 | 6.859069 | 6.190444 | 7.035188 | 6.660703 | 6.429613 | 6.232651 | 6.193444 | 6.031781 | 6.445487 | 6.873151 | 6.459351 |
hep-th/0108239 | Steven S. Gubser | Steven S. Gubser and Indrajit Mitra | Some interesting violations of the Breitenlohner-Freedman bound | 16 pages, latex. v2: minor corrections | JHEP 0207 (2002) 044 | 10.1088/1126-6708/2002/07/044 | CALT-68-2345, CITUSC/01-030, PUPT-2005 | hep-th | null | We demonstrate that AdS_5 x T^{pq} is unstable, in the sense of Breitenlohner
and Freedman, for unequal p and q. This settles, negatively, the long-standing
question of whether the T^{pq} manifolds for unequal p and q might correspond
to non-supersymmetric fixed points of the renormalization group. We also show
that ... | [
{
"created": "Fri, 31 Aug 2001 16:35:14 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jun 2002 19:20:59 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Gubser",
"Steven S.",
""
],
[
"Mitra",
"Indrajit",
""
]
] | We demonstrate that AdS_5 x T^{pq} is unstable, in the sense of Breitenlohner and Freedman, for unequal p and q. This settles, negatively, the long-standing question of whether the T^{pq} manifolds for unequal p and q might correspond to non-supersymmetric fixed points of the renormalization group. We also show that th... | 7.852046 | 7.600677 | 7.788942 | 7.290646 | 7.793926 | 7.540448 | 7.106511 | 7.255558 | 7.43813 | 9.013813 | 7.130929 | 7.190598 | 8.226531 | 7.682177 | 7.687223 | 7.248861 | 7.34577 | 7.173576 | 7.436163 | 7.508097 | 6.846982 |
hep-th/0212218 | Eric R. Sharpe | S. Katz, T. Pantev, E. Sharpe | D-branes, orbifolds, and Ext groups | 51 pages, 3 figures; v2: material on Freed-Witten added; v3: more
typos fixed | Nucl.Phys. B673 (2003) 263-300 | 10.1016/j.nuclphysb.2003.09.022 | ILL-(TH)-02-10 | hep-th | null | In this note we extend previous work on massless Ramond spectra of open
strings connecting D-branes wrapped on complex manifolds, to consider D-branes
wrapped on smooth complex orbifolds. Using standard methods, we calculate the
massless boundary Ramond sector spectra directly in BCFT, and find that the
states in the... | [
{
"created": "Wed, 18 Dec 2002 17:10:41 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 2003 16:12:37 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Dec 2003 02:25:40 GMT",
"version": "v3"
}
] | 2010-04-05 | [
[
"Katz",
"S.",
""
],
[
"Pantev",
"T.",
""
],
[
"Sharpe",
"E.",
""
]
] | In this note we extend previous work on massless Ramond spectra of open strings connecting D-branes wrapped on complex manifolds, to consider D-branes wrapped on smooth complex orbifolds. Using standard methods, we calculate the massless boundary Ramond sector spectra directly in BCFT, and find that the states in the s... | 12.5319 | 11.069308 | 15.377008 | 11.50014 | 12.405656 | 11.598989 | 11.305614 | 11.429966 | 11.562799 | 14.625072 | 11.141551 | 11.776898 | 12.763321 | 11.250766 | 11.284407 | 11.202861 | 11.795189 | 11.882092 | 11.419161 | 12.038317 | 11.554199 |
1006.5849 | Akbar Jahan | A. Jahan | On the String Pair Creation in Dp-Dp' Brane System | Accepted for publication in Mod. Phys. Lett. A | Mod.Phys.Lett.A26:215-222,2011 | 10.1142/S0217732311034748 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We address the bosonic string pair creation in a system of parallel Dp-Dp'
(p<p') branes by applying the path integral formalism. We drive the string pair
creation rate by calculating the one loop vacuum amplitude of the setup in
presence of the background electric field defined over the Dp'-brane. It is
pointed out ... | [
{
"created": "Wed, 30 Jun 2010 13:26:15 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Nov 2010 08:24:20 GMT",
"version": "v2"
}
] | 2011-03-04 | [
[
"Jahan",
"A.",
""
]
] | We address the bosonic string pair creation in a system of parallel Dp-Dp' (p<p') branes by applying the path integral formalism. We drive the string pair creation rate by calculating the one loop vacuum amplitude of the setup in presence of the background electric field defined over the Dp'-brane. It is pointed out th... | 11.934909 | 9.799118 | 12.568264 | 10.218209 | 10.747036 | 9.545141 | 9.283818 | 9.64655 | 9.576538 | 13.341385 | 10.267715 | 11.058061 | 11.673627 | 10.639121 | 10.685436 | 10.713172 | 10.946076 | 11.149667 | 10.661012 | 11.99018 | 11.450273 |
hep-th/0607179 | A. Tureanu | M. Chaichian, A. Tureanu, G. Zet | Twist as a Symmetry Principle and the Noncommutative Gauge Theory
Formulation | 13 pages, more accurate motivation added | Phys.Lett.B651:319-323,2007 | 10.1016/j.physletb.2007.06.026 | HIP-2006-32/TH | hep-th math-ph math.MP | null | Based on the analysis of the most natural and general ansatz, we conclude
that the concept of twist symmetry, originally obtained for the noncommutative
space-time, cannot be extended to include internal gauge symmetry. The case is
reminiscent of the Coleman-Mandula theorem. Invoking the supersymmetry may
reverse the... | [
{
"created": "Mon, 24 Jul 2006 18:46:48 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Nov 2006 18:04:02 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Jun 2007 09:28:49 GMT",
"version": "v3"
},
{
"created": "Sun, 24 Jun 2007 13:46:04 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Chaichian",
"M.",
""
],
[
"Tureanu",
"A.",
""
],
[
"Zet",
"G.",
""
]
] | Based on the analysis of the most natural and general ansatz, we conclude that the concept of twist symmetry, originally obtained for the noncommutative space-time, cannot be extended to include internal gauge symmetry. The case is reminiscent of the Coleman-Mandula theorem. Invoking the supersymmetry may reverse the s... | 21.029999 | 16.944494 | 17.629807 | 16.262486 | 16.685366 | 16.033104 | 18.279898 | 15.500428 | 16.703691 | 18.276268 | 15.317822 | 16.234783 | 17.772968 | 16.641588 | 16.775066 | 16.595804 | 16.817787 | 16.527771 | 16.975513 | 17.476681 | 16.056814 |
1712.02603 | Santiago Codesido Sanchez | Santiago Codesido, Marcos Marino, Ricardo Schiappa | Non-Perturbative Quantum Mechanics from Non-Perturbative Strings | 56 pages, 9 figures | null | null | NSF-ITP-17-152 | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work develops a new method to calculate non-perturbative corrections in
one-dimensional Quantum Mechanics, based on trans-series solutions to the
refined holomorphic anomaly equations of topological string theory. The method
can be applied to traditional spectral problems governed by the Schr\"odinger
equation, ... | [
{
"created": "Thu, 7 Dec 2017 13:02:30 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Oct 2018 13:48:17 GMT",
"version": "v2"
}
] | 2018-10-15 | [
[
"Codesido",
"Santiago",
""
],
[
"Marino",
"Marcos",
""
],
[
"Schiappa",
"Ricardo",
""
]
] | This work develops a new method to calculate non-perturbative corrections in one-dimensional Quantum Mechanics, based on trans-series solutions to the refined holomorphic anomaly equations of topological string theory. The method can be applied to traditional spectral problems governed by the Schr\"odinger equation, wh... | 5.629722 | 5.497554 | 6.718626 | 5.333867 | 5.401569 | 5.279293 | 5.202671 | 5.466451 | 5.334948 | 7.355412 | 5.111611 | 5.326293 | 5.781328 | 5.36479 | 5.393723 | 5.399294 | 5.356466 | 5.37785 | 5.401266 | 5.847972 | 5.276248 |
1409.8295 | James Halverson | Antonella Grassi, James Halverson, Julius Shaneson, and Washington
Taylor | Non-Higgsable QCD and the Standard Model Spectrum in F-theory | v1: 29 pages + references | null | 10.1007/JHEP01(2015)086 | NSF-KITP-14-100, MIT-CTP-4581 | hep-th hep-ph math.AG math.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many four-dimensional supersymmetric compactifications of F-theory contain
gauge groups that cannot be spontaneously broken through geometric
deformations. These "non-Higgsable clusters" include realizations of $SU(3)$,
$SU(2)$, and $SU(3) \times SU(2)$, but no $SU(n)$ gauge groups or factors with
$n> 3$. We study po... | [
{
"created": "Mon, 29 Sep 2014 20:00:17 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Grassi",
"Antonella",
""
],
[
"Halverson",
"James",
""
],
[
"Shaneson",
"Julius",
""
],
[
"Taylor",
"Washington",
""
]
] | Many four-dimensional supersymmetric compactifications of F-theory contain gauge groups that cannot be spontaneously broken through geometric deformations. These "non-Higgsable clusters" include realizations of $SU(3)$, $SU(2)$, and $SU(3) \times SU(2)$, but no $SU(n)$ gauge groups or factors with $n> 3$. We study poss... | 7.290915 | 7.671712 | 7.898055 | 6.922969 | 7.70423 | 7.985816 | 7.785233 | 7.712195 | 7.372129 | 8.497372 | 7.324987 | 6.867451 | 6.905067 | 6.859992 | 7.18064 | 7.173579 | 7.165704 | 6.866409 | 7.065989 | 7.283478 | 7.055812 |
hep-th/9310028 | A. Leonidov | A. Leonidov | Resummed Effective Action in Inhomogeneous External Field at Zero and
Finite Temperature | BI-TP 93/53, Plain LaTeX | null | null | null | hep-th | null | The two ways of resumming the efffective action for the massless test
particles in inhomogeneous external field at zero and finite temperature
providing the infrared finite answer are discussed. The case of the massive
test particles having a mass which is parametrically small with respect to a
scale set by the inhom... | [
{
"created": "Wed, 6 Oct 1993 12:37:57 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Leonidov",
"A.",
""
]
] | The two ways of resumming the efffective action for the massless test particles in inhomogeneous external field at zero and finite temperature providing the infrared finite answer are discussed. The case of the massive test particles having a mass which is parametrically small with respect to a scale set by the inhomog... | 14.982998 | 15.696496 | 14.941158 | 13.928156 | 15.659028 | 13.836685 | 13.967149 | 14.624686 | 12.644663 | 15.538398 | 12.954579 | 13.23848 | 13.722162 | 13.06817 | 13.516731 | 13.392229 | 13.371956 | 13.480976 | 13.911472 | 13.517374 | 13.497114 |
1007.2651 | Rafael Ferraro | Rafael Ferraro | Born-Infeld electrostatics in the complex plane | 15 pages, 4 figures | JHEP 1012:028,2010 | 10.1007/JHEP12(2010)028 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complex method to obtain 2-dimensional Born-Infeld electrostatic
solutions is presented in a renewed form. The solutions are generated by a
holomorphic seed that makes contact with the Coulombian complex potential. The
procedure is exemplified by solving the Born-Infeld multipolar configurations.
Besides, it is s... | [
{
"created": "Thu, 15 Jul 2010 20:42:15 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Nov 2010 16:39:10 GMT",
"version": "v2"
},
{
"created": "Fri, 10 Dec 2010 16:04:07 GMT",
"version": "v3"
}
] | 2011-04-06 | [
[
"Ferraro",
"Rafael",
""
]
] | The complex method to obtain 2-dimensional Born-Infeld electrostatic solutions is presented in a renewed form. The solutions are generated by a holomorphic seed that makes contact with the Coulombian complex potential. The procedure is exemplified by solving the Born-Infeld multipolar configurations. Besides, it is sho... | 14.774691 | 14.328497 | 14.413427 | 13.459716 | 14.335467 | 14.301804 | 14.061553 | 13.384208 | 14.725381 | 14.845938 | 14.136453 | 13.564053 | 14.316022 | 14.620854 | 14.493819 | 14.069253 | 14.476423 | 13.780599 | 14.450175 | 14.52462 | 14.28502 |
2408.03673 | George Georgiou | George Georgiou | The massless S-matrix of integrable $\sigma$-models | 32 pages | null | null | null | hep-th hep-ph nlin.SI | http://creativecommons.org/licenses/by/4.0/ | In contradistinction to the case of massive excitations, the connection
between integrability and the tree-level massless scattering matrix of
integrable $\sigma$-models is lost. Namely, in well-known 2-d integrable models
the tree-level massless S-matrix exhibits particle production and fails to
factorise. This is c... | [
{
"created": "Wed, 7 Aug 2024 10:30:49 GMT",
"version": "v1"
}
] | 2024-08-08 | [
[
"Georgiou",
"George",
""
]
] | In contradistinction to the case of massive excitations, the connection between integrability and the tree-level massless scattering matrix of integrable $\sigma$-models is lost. Namely, in well-known 2-d integrable models the tree-level massless S-matrix exhibits particle production and fails to factorise. This is con... | 8.365048 | 7.630409 | 7.922048 | 6.947968 | 7.158585 | 7.328797 | 6.67421 | 6.702483 | 7.127288 | 8.566787 | 6.958154 | 7.207651 | 7.45505 | 7.18622 | 7.1798 | 7.339981 | 6.981889 | 7.027694 | 7.078542 | 7.319949 | 7.139605 |
hep-th/9301041 | null | Ansar Fayyazuddin | On the origin of multi-component anyon wave functions | 20, Latex, USITP-92-15 | Nucl.Phys. B401 (1993) 644-662 | 10.1016/0550-3213(93)90317-I | null | hep-th | null | In this paper I discuss how the component structure of anyon wave functions
arises in theories with non-relativistic matter coupled to a Chern-Simons gauge
field on the torus. It is shown that there exists a singular gauge
transformation which brings the Hamiltonian to free form. The gauge
transformation removes a de... | [
{
"created": "Tue, 12 Jan 1993 11:28:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Fayyazuddin",
"Ansar",
""
]
] | In this paper I discuss how the component structure of anyon wave functions arises in theories with non-relativistic matter coupled to a Chern-Simons gauge field on the torus. It is shown that there exists a singular gauge transformation which brings the Hamiltonian to free form. The gauge transformation removes a degr... | 8.323239 | 7.321733 | 7.984943 | 7.163651 | 7.878544 | 7.590217 | 6.719638 | 7.318769 | 6.897145 | 7.812225 | 7.108725 | 7.562854 | 7.849741 | 7.344361 | 7.568055 | 7.564499 | 7.458842 | 7.491879 | 7.535297 | 7.591241 | 7.452824 |
hep-th/0406027 | Clovis Wotzasek | Patricio Gaete, Clovis Wotzasek | Fractional statistics and confinement | Four pages, Latex file | Europhys.Lett. 69 (2005) 341-345 | 10.1209/epl/i2004-10370-7 | USM-TH-154 | hep-th | null | It is shown that a pointlike composite having charge and magnetic moment
displays a confining potential for the static interaction while simultaneously
obeying fractional statistics in a pure gauge theory in three dimensions,
without a Chern-Simons term. This result is distinct from the
Maxwell-Chern-Simons theory th... | [
{
"created": "Wed, 2 Jun 2004 20:59:52 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Gaete",
"Patricio",
""
],
[
"Wotzasek",
"Clovis",
""
]
] | It is shown that a pointlike composite having charge and magnetic moment displays a confining potential for the static interaction while simultaneously obeying fractional statistics in a pure gauge theory in three dimensions, without a Chern-Simons term. This result is distinct from the Maxwell-Chern-Simons theory that... | 22.330202 | 18.271502 | 21.069696 | 18.886749 | 18.235699 | 18.957476 | 18.171284 | 18.211033 | 17.503319 | 21.871578 | 18.194807 | 17.589161 | 19.469761 | 17.916639 | 18.120281 | 17.497849 | 17.171364 | 18.101412 | 18.083984 | 18.637812 | 18.643986 |
0809.3287 | Yu. M. Zinoviev | Yu. M. Zinoviev | Toward frame-like gauge invariant formulation for massive mixed symmetry
bosonic fields | 18 pages, 9 LaTeX pictures | Nucl.Phys.B812:46-63,2009 | 10.1016/j.nuclphysb.2008.12.003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, as a first step toward frame-like gauge invariant formulation
for massive mixed symmetry bosonic fields, we consider mixed tensors,
corresponding to Young tableau with two rows with k >= 2 boxes in the first row
and only one box in the second one. We construct complete Lagrangian and gauge
transformati... | [
{
"created": "Fri, 19 Sep 2008 15:12:43 GMT",
"version": "v1"
}
] | 2009-02-12 | [
[
"Zinoviev",
"Yu. M.",
""
]
] | In this paper, as a first step toward frame-like gauge invariant formulation for massive mixed symmetry bosonic fields, we consider mixed tensors, corresponding to Young tableau with two rows with k >= 2 boxes in the first row and only one box in the second one. We construct complete Lagrangian and gauge transformation... | 12.370759 | 7.822642 | 13.399786 | 9.055134 | 9.304193 | 7.549041 | 8.864264 | 8.241468 | 8.881866 | 14.195227 | 10.07655 | 9.841723 | 12.140399 | 10.0015 | 10.029156 | 9.840862 | 9.5883 | 9.621443 | 9.985617 | 11.41774 | 10.661724 |
hep-th/9705180 | G. Mussardo | D.C. Cabra, A. Honecker, G. Mussardo, P. Pujol | A Non-Perturbative Approach to the Random-Bond Ising Model | 17 pages LaTeX, 1 PostScript figure included using psfig.sty | J.Phys.A30:8415-8426,1997 | 10.1088/0305-4470/30/24/008 | IC/97/37, SISSA 54/97/EP | hep-th cond-mat | null | We study the N -> 0 limit of the O(N) Gross-Neveu model in the framework of
the massless form-factor approach. This model is related to the continuum limit
of the Ising model with random bonds via the replica method. We discuss how
this method may be useful in calculating correlation functions of physical
operators. ... | [
{
"created": "Fri, 23 May 1997 09:41:51 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cabra",
"D. C.",
""
],
[
"Honecker",
"A.",
""
],
[
"Mussardo",
"G.",
""
],
[
"Pujol",
"P.",
""
]
] | We study the N -> 0 limit of the O(N) Gross-Neveu model in the framework of the massless form-factor approach. This model is related to the continuum limit of the Ising model with random bonds via the replica method. We discuss how this method may be useful in calculating correlation functions of physical operators. Th... | 9.407839 | 9.216611 | 9.747445 | 7.98174 | 8.878163 | 8.603774 | 8.227096 | 8.733567 | 8.676143 | 10.783184 | 8.471041 | 8.852273 | 9.312316 | 9.013168 | 8.724677 | 8.542686 | 8.675185 | 8.829741 | 8.903369 | 9.619981 | 8.730736 |
hep-th/0511086 | John Baez | John C. Baez | Calabi-Yau Manifolds and the Standard Model | 4 pages | null | null | null | hep-th | null | For any subgroup G of O(n), define a "G-manifold" to be an n-dimensional
Riemannian manifold whose holonomy group is contained in G. Then a G-manifold
where G is the Standard Model gauge group is precisely a Calabi-Yau manifold of
10 real dimensions whose tangent spaces split into orthogonal 4- and
6-dimensional subs... | [
{
"created": "Tue, 8 Nov 2005 06:14:07 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Nov 2005 04:18:15 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Baez",
"John C.",
""
]
] | For any subgroup G of O(n), define a "G-manifold" to be an n-dimensional Riemannian manifold whose holonomy group is contained in G. Then a G-manifold where G is the Standard Model gauge group is precisely a Calabi-Yau manifold of 10 real dimensions whose tangent spaces split into orthogonal 4- and 6-dimensional subspa... | 6.032058 | 6.577161 | 7.031108 | 5.734203 | 6.079544 | 6.539179 | 5.695226 | 6.351451 | 6.33969 | 7.084428 | 6.284092 | 5.5195 | 5.898588 | 5.753101 | 5.632886 | 5.439703 | 5.486557 | 5.525486 | 5.530581 | 5.607294 | 5.47369 |
2101.02512 | Anna Pachol | Stjepan Meljanac, Anna Pacho{\l} | Heisenberg doubles for Snyder type models | 19 pages, no figures, 1 Appendix; version accepted for publication | Symmetry 2021, 13(6), 1055 | 10.3390/sym13061055 | null | hep-th gr-qc math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A Snyder model generated by the noncommutative coordinates and Lorentz
generators close a Lie algebra. The application of the Heisenberg double
construction is investigated for the Snyder coordinates and momenta generators.
It leads to the phase space of the Snyder model. Further, the extended Snyder
algebra is const... | [
{
"created": "Thu, 7 Jan 2021 12:24:36 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Jan 2021 09:25:43 GMT",
"version": "v2"
},
{
"created": "Thu, 3 Jun 2021 15:34:35 GMT",
"version": "v3"
}
] | 2021-06-17 | [
[
"Meljanac",
"Stjepan",
""
],
[
"Pachoł",
"Anna",
""
]
] | A Snyder model generated by the noncommutative coordinates and Lorentz generators close a Lie algebra. The application of the Heisenberg double construction is investigated for the Snyder coordinates and momenta generators. It leads to the phase space of the Snyder model. Further, the extended Snyder algebra is constru... | 13.03632 | 11.879741 | 13.750949 | 10.961267 | 11.518515 | 11.353777 | 12.173009 | 11.241301 | 11.298802 | 15.063227 | 11.23879 | 11.279399 | 11.981585 | 10.877541 | 11.098376 | 11.550261 | 11.207384 | 11.309825 | 11.154607 | 11.898953 | 10.824501 |
1705.05425 | Olaf Lechtenfeld | Francisco Correa, Olaf Lechtenfeld | ${\cal PT}$ deformation of angular Calogero models | 1+41 pages, 12 figures | null | 10.1007/JHEP11(2017)122 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The rational Calogero model based on an arbitrary rank-$n$ Coxeter root
system is spherically reduced to a superintegrable angular model of a particle
moving on $S^{n-1}$ subject to a very particular potential singular at the
reflection hyperplanes. It is outlined how to find conserved charges and to
construct intert... | [
{
"created": "Mon, 15 May 2017 19:56:48 GMT",
"version": "v1"
}
] | 2018-01-17 | [
[
"Correa",
"Francisco",
""
],
[
"Lechtenfeld",
"Olaf",
""
]
] | The rational Calogero model based on an arbitrary rank-$n$ Coxeter root system is spherically reduced to a superintegrable angular model of a particle moving on $S^{n-1}$ subject to a very particular potential singular at the reflection hyperplanes. It is outlined how to find conserved charges and to construct intertwi... | 10.506492 | 10.661335 | 11.530371 | 10.802599 | 10.350183 | 10.183197 | 10.896691 | 9.721076 | 10.639055 | 12.895718 | 9.896284 | 9.888659 | 10.339521 | 10.116128 | 10.114098 | 10.133632 | 9.63446 | 9.971519 | 9.888819 | 10.06269 | 9.944811 |
hep-th/9409070 | null | A. Shafei Deh Abad, V. Milani | $Q$-Meromorphic Functions, Quantums sets and Homomorphisms of the
Quantum Plane | 15 pages | null | null | (ISTPM) IPM-94-049 | hep-th math.QA | null | In this paper which is the completion of [1], we construct the
$A_0(q)$-algebra of $Q$-meromorphic functions on the quantum plane. This is the
largest non-commutative, associative, $A_0(q)$-algebra of functions constructed
on the quantum plane. We also define the notion of quantum subsets of R$^2$
which is a generali... | [
{
"created": "Mon, 12 Sep 1994 20:15:31 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Abad",
"A. Shafei Deh",
""
],
[
"Milani",
"V.",
""
]
] | In this paper which is the completion of [1], we construct the $A_0(q)$-algebra of $Q$-meromorphic functions on the quantum plane. This is the largest non-commutative, associative, $A_0(q)$-algebra of functions constructed on the quantum plane. We also define the notion of quantum subsets of R$^2$ which is a generaliza... | 8.216392 | 7.9405 | 7.704545 | 7.930448 | 7.451451 | 7.58176 | 8.142073 | 7.893292 | 7.573385 | 8.855983 | 7.840438 | 7.827554 | 7.949184 | 7.693244 | 7.641547 | 7.857025 | 7.790079 | 7.936396 | 7.435231 | 7.847329 | 7.47992 |
2207.11261 | Luca Delacr\'etaz | Luca V. Delacretaz, A. Liam Fitzpatrick, Emanuel Katz, Matthew T.
Walters | Thermalization and chaos in a 1+1d QFT | 17 pages, 18 figures; v2: added Fig.10 on quantum scars, published
version | null | 10.1007/JHEP02(2023)045 | EFI 22-7 | hep-th cond-mat.stat-mech cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study aspects of chaos and thermodynamics at strong coupling in a scalar
model using LCT numerical methods. We find that our eigenstate spectrum
satisfies Wigner-Dyson statistics and that the coefficients describing
eigenstates in our basis satisfy Random Matrix Theory (RMT) statistics. At weak
coupling, though th... | [
{
"created": "Fri, 22 Jul 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Feb 2023 16:12:06 GMT",
"version": "v2"
}
] | 2023-02-22 | [
[
"Delacretaz",
"Luca V.",
""
],
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Katz",
"Emanuel",
""
],
[
"Walters",
"Matthew T.",
""
]
] | We study aspects of chaos and thermodynamics at strong coupling in a scalar model using LCT numerical methods. We find that our eigenstate spectrum satisfies Wigner-Dyson statistics and that the coefficients describing eigenstates in our basis satisfy Random Matrix Theory (RMT) statistics. At weak coupling, though the ... | 10.656097 | 9.923631 | 10.960277 | 10.084347 | 11.604505 | 11.775522 | 11.596542 | 10.989628 | 10.432614 | 11.983538 | 10.777419 | 10.406428 | 10.47379 | 10.445272 | 10.28946 | 10.207466 | 10.586555 | 10.527595 | 10.454094 | 10.563258 | 10.09769 |
0805.4217 | Robert Brandenberger | Robert Brandenberger (McGill University) and Walter Craig (McMaster
University) | Towards a New Proof of Anderson Localization | null | null | 10.1140/epjc/s10052-012-1881-9 | null | hep-th cond-mat.stat-mech math-ph math.DS math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The wave function of a non-relativistic particle in a periodic potential
admits oscillatory solutions, the Bloch waves. In the presence of a random
noise contribution to the potential the wave function is localized. We outline
a new proof of this Anderson localization phenomenon in one spatial dimension,
extending th... | [
{
"created": "Tue, 27 May 2008 20:55:05 GMT",
"version": "v1"
}
] | 2015-05-13 | [
[
"Brandenberger",
"Robert",
"",
"McGill University"
],
[
"Craig",
"Walter",
"",
"McMaster\n University"
]
] | The wave function of a non-relativistic particle in a periodic potential admits oscillatory solutions, the Bloch waves. In the presence of a random noise contribution to the potential the wave function is localized. We outline a new proof of this Anderson localization phenomenon in one spatial dimension, extending the ... | 9.284213 | 9.353601 | 8.880168 | 9.151582 | 9.761785 | 9.858999 | 10.094147 | 9.316013 | 9.04608 | 9.609107 | 8.853956 | 9.593379 | 8.8871 | 9.115832 | 8.974545 | 9.338758 | 8.87577 | 9.145932 | 9.066324 | 9.041873 | 9.057261 |
hep-th/0203033 | George Tsoupros | George Tsoupros | Perturbative Evaluation of the Effective Action for a Self-Interacting
Conformal Field on a Manifold with Boundary | 12 pages, 5 figures LaTeX2e. Talk delivered in the third (ACGRG3)
conference of the ASGRG, Perth-Australia. To appear in proceedings | Gen.Rel.Grav. 34 (2002) 1739-1750 | null | null | hep-th | null | In a series of three projects a new technique which allows for higher-loop
renormalisation on a manifold with boundary has been developed and used in
order to assess the effects of the boundary on the dynamical behaviour of the
theory. Commencing with a conceptual approach to the theoretical underpinnings
of the, und... | [
{
"created": "Tue, 5 Mar 2002 11:51:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Tsoupros",
"George",
""
]
] | In a series of three projects a new technique which allows for higher-loop renormalisation on a manifold with boundary has been developed and used in order to assess the effects of the boundary on the dynamical behaviour of the theory. Commencing with a conceptual approach to the theoretical underpinnings of the, under... | 23.254295 | 18.594296 | 21.451048 | 19.359613 | 19.400232 | 19.441925 | 20.587616 | 19.842094 | 20.249384 | 20.810234 | 19.793428 | 19.025661 | 21.039879 | 19.818567 | 19.290138 | 18.882784 | 19.268368 | 18.55414 | 19.226572 | 20.194141 | 19.138695 |
2201.10333 | Gianmassimo Tasinato | Gianmassimo Tasinato | Stochastic approach to gravitational waves from inflation | 27 pages, 2 figures | Phys.Rev.D 105 (2022) 2, 023521 | 10.1103/PhysRevD.105.023521 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a coarse-graining procedure for describing the superhorizon
dynamics of inflationary tensor modes. Our aim is to formulate a stochastic
description for the statistics of spin-2 modes which seed the background of
gravitational waves from inflation. Using basic principles of quantum
mechanics, we determine a... | [
{
"created": "Tue, 25 Jan 2022 14:13:20 GMT",
"version": "v1"
}
] | 2022-02-03 | [
[
"Tasinato",
"Gianmassimo",
""
]
] | We propose a coarse-graining procedure for describing the superhorizon dynamics of inflationary tensor modes. Our aim is to formulate a stochastic description for the statistics of spin-2 modes which seed the background of gravitational waves from inflation. Using basic principles of quantum mechanics, we determine a p... | 11.010095 | 12.597253 | 11.207205 | 10.555993 | 11.691932 | 12.116049 | 11.325948 | 10.830649 | 11.829395 | 12.044669 | 11.412632 | 11.499537 | 10.838698 | 11.163105 | 11.335203 | 11.335843 | 11.344801 | 10.906423 | 11.389565 | 11.059477 | 11.013507 |
hep-th/0602227 | Shane Magee | Conor Houghton and Shane Magee | The effect of pion mass on Skyrme configurations | 6 pages, 3 figures; new data added, clarifications and typo
corrections made; version to appear in Europhysics Letters | Europhys.Lett.77:11001,2007 | 10.1209/0295-5075/77/11001 | TCD-MATH 06-02 | hep-th | null | In the Skyrme model, atomic nuclei are identified with solitonic
configurations. If the pion mass is set to zero, these configurations are
spherical shells of energy with a fullerene-like appearance and are well
approximated by a simple rational map ansatz. Using simulated annealing, we
have calculated minimum energy... | [
{
"created": "Wed, 22 Feb 2006 16:16:12 GMT",
"version": "v1"
},
{
"created": "Sat, 25 Feb 2006 13:30:09 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Nov 2006 16:35:49 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Houghton",
"Conor",
""
],
[
"Magee",
"Shane",
""
]
] | In the Skyrme model, atomic nuclei are identified with solitonic configurations. If the pion mass is set to zero, these configurations are spherical shells of energy with a fullerene-like appearance and are well approximated by a simple rational map ansatz. Using simulated annealing, we have calculated minimum energy c... | 9.194356 | 7.514072 | 8.83808 | 7.743673 | 8.053773 | 7.014969 | 7.773179 | 7.846153 | 7.760056 | 9.678131 | 7.589231 | 7.813059 | 8.374613 | 7.892877 | 7.906931 | 7.812293 | 7.791362 | 8.139807 | 7.903098 | 8.355602 | 8.068874 |
2302.03998 | Kilian Hersent | Kilian Hersent | Quantum properties of $U(1)$-like gauge theory on $\kappa$-Minkowski | 6+4 pages. From a talk given at the "Workshop on Noncommutative and
generalized geometry in string theory, gauge theory and related physical
models", Corfu, Sep 18 - Sep 25, 2022 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the 5-dimensional twisted $U(1)$-like gauge theory on $\kappa$-Minkowski,
the one-loop one-point (tadpole) function was computed in arXiv:2107.14462.
This article summarizes the construction of such a gauge theory and discusses
the non-vanishing of the tadpole.
| [
{
"created": "Wed, 8 Feb 2023 11:16:51 GMT",
"version": "v1"
}
] | 2023-03-06 | [
[
"Hersent",
"Kilian",
""
]
] | In the 5-dimensional twisted $U(1)$-like gauge theory on $\kappa$-Minkowski, the one-loop one-point (tadpole) function was computed in arXiv:2107.14462. This article summarizes the construction of such a gauge theory and discusses the non-vanishing of the tadpole. | 11.557955 | 9.998617 | 10.687449 | 9.651279 | 10.333641 | 10.432256 | 10.63349 | 9.215939 | 9.219396 | 11.788778 | 10.225866 | 9.670278 | 10.040925 | 9.224743 | 9.833043 | 9.366776 | 9.725987 | 9.680762 | 9.556431 | 10.318328 | 9.684116 |
hep-th/9401060 | null | Lev Rozansky | Witten's Invariant of 3-Dimensional Manifolds: Loop Expansion and
Surgery Calculus | 29 pages, "\draft" declaration has been removed | null | null | UTTG-12-93 | hep-th math.QA | null | We review two different methods of calculating Witten's invariant: a
stationary phase approximation and a surgery calculus. We give a detailed
description of the 1-loop approximation formula for Witten's invariant and of
the technics involved in deriving its exact value through a surgery
construction of a manifold. F... | [
{
"created": "Fri, 14 Jan 1994 01:38:34 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Jan 1994 21:53:42 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Rozansky",
"Lev",
""
]
] | We review two different methods of calculating Witten's invariant: a stationary phase approximation and a surgery calculus. We give a detailed description of the 1-loop approximation formula for Witten's invariant and of the technics involved in deriving its exact value through a surgery construction of a manifold. Fin... | 14.023509 | 13.467011 | 13.248481 | 13.31743 | 12.612889 | 12.624267 | 12.406913 | 12.983913 | 12.616967 | 14.18371 | 12.429569 | 12.824361 | 12.62959 | 12.811238 | 12.979327 | 12.156837 | 12.743724 | 12.520241 | 12.716385 | 13.422922 | 12.164462 |
hep-th/0210014 | Bert Schellekens | N. Sousa and A.N. Schellekens | Orientation matters for NIMreps | 34 pages, plain TeX + phyzzx; typos corrected,a few clarifications
and references added | Nucl.Phys. B653 (2003) 339-368 | 10.1016/S0550-3213(02)01124-0 | NIKHEF/02-009 | hep-th | null | The problem of finding boundary states in CFT, often rephrased in terms of
"NIMreps" of the fusion algebra, has a natural extension to CFT on
non-orientable surfaces. This provides extra information that turns out to be
quite useful to give the proper interpretation to a NIMrep. We illustrate this
with several exampl... | [
{
"created": "Wed, 2 Oct 2002 15:21:50 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Oct 2002 14:04:35 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Sousa",
"N.",
""
],
[
"Schellekens",
"A. N.",
""
]
] | The problem of finding boundary states in CFT, often rephrased in terms of "NIMreps" of the fusion algebra, has a natural extension to CFT on non-orientable surfaces. This provides extra information that turns out to be quite useful to give the proper interpretation to a NIMrep. We illustrate this with several examples... | 11.695024 | 11.859812 | 12.697327 | 10.913493 | 12.260027 | 12.349598 | 11.352507 | 11.505499 | 10.470263 | 13.879165 | 11.460789 | 11.041434 | 11.909423 | 11.008246 | 10.74032 | 11.051124 | 10.824426 | 11.212432 | 11.009267 | 11.705672 | 10.91087 |
1808.04135 | Shun'ya Mizoguchi | Shin Fukuchi, Naoto Kan, Shun'ya Mizoguchi and Hitomi Tashiro | A dessin on the base: a description of mutually non-local 7-branes
without using branch cuts | 27 pages, 9 figures. v3: Title changed, section 3 added to explain
the notion of a "dessin d'enfant", sections 4,6 and 7 in v2 removed | Phys. Rev. D 100, 126025 (2019) | 10.1103/PhysRevD.100.126025 | KEK-TH-2069 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the special roles of the zero loci of the Weierstrass invariants
$g_2(\tau(z))$, $g_3(\tau(z))$ in F-theory on an elliptic fibration over $P^1$
or a further fibration thereof. They are defined as the zero loci of the
coefficient functions $f(z)$ and $g(z)$ of a Weierstrass equation. They are
thought of as... | [
{
"created": "Mon, 13 Aug 2018 10:17:35 GMT",
"version": "v1"
},
{
"created": "Tue, 28 May 2019 09:48:50 GMT",
"version": "v2"
},
{
"created": "Mon, 21 Oct 2019 06:30:28 GMT",
"version": "v3"
}
] | 2020-01-08 | [
[
"Fukuchi",
"Shin",
""
],
[
"Kan",
"Naoto",
""
],
[
"Mizoguchi",
"Shun'ya",
""
],
[
"Tashiro",
"Hitomi",
""
]
] | We consider the special roles of the zero loci of the Weierstrass invariants $g_2(\tau(z))$, $g_3(\tau(z))$ in F-theory on an elliptic fibration over $P^1$ or a further fibration thereof. They are defined as the zero loci of the coefficient functions $f(z)$ and $g(z)$ of a Weierstrass equation. They are thought of as c... | 12.15661 | 12.912891 | 12.841005 | 11.930551 | 12.344266 | 13.083576 | 12.605981 | 12.576327 | 12.13725 | 13.890731 | 11.521478 | 11.829989 | 11.543986 | 11.304868 | 11.434758 | 11.560595 | 11.978045 | 11.665958 | 11.64105 | 11.989563 | 11.421623 |
hep-th/9208009 | null | Jonathan M. Evans and Philip A. Tuckey | A Geometrical Approach to Time-Dependent Gauge-Fixing | 15 pages, OUTP-92-11P | Int.J.Mod.Phys. A8 (1993) 4055-4069 | 10.1142/S0217751X93001661 | null | hep-th gr-qc | null | When a Hamiltonian system is subject to constraints which depend explicitly
on time, difficulties can arise in attempting to reduce the system to its
physical phase space. Specifically, it is non-trivial to restrict the system in
such a way that one can find a Hamiltonian time-evolution equation involving
the Dirac b... | [
{
"created": "Mon, 3 Aug 1992 13:15:00 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Evans",
"Jonathan M.",
""
],
[
"Tuckey",
"Philip A.",
""
]
] | When a Hamiltonian system is subject to constraints which depend explicitly on time, difficulties can arise in attempting to reduce the system to its physical phase space. Specifically, it is non-trivial to restrict the system in such a way that one can find a Hamiltonian time-evolution equation involving the Dirac bra... | 9.458003 | 8.327755 | 8.500319 | 7.923778 | 8.784596 | 9.066037 | 7.820078 | 8.022774 | 8.339511 | 8.881591 | 8.162784 | 7.930277 | 8.177172 | 8.10535 | 8.168982 | 8.124934 | 8.071917 | 8.217622 | 8.171558 | 8.079974 | 7.861526 |
hep-th/9108019 | Igor Klebanov | Igor R. Klebanov | String Theory in Two Dimensions | 76 pages, Phyzzx, lectures at the 1991 ICTP Spring School; v2:
postscript figures included | null | null | PUPT-1271 | hep-th | null | I review some of the recent progress in two-dimensional string theory, which
is formulated as a sum over surfaces embedded in one dimension.
| [
{
"created": "Mon, 26 Aug 1991 15:55:27 GMT",
"version": "v1"
},
{
"created": "Sun, 25 May 2003 23:14:09 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Klebanov",
"Igor R.",
""
]
] | I review some of the recent progress in two-dimensional string theory, which is formulated as a sum over surfaces embedded in one dimension. | 18.090725 | 10.72581 | 13.594742 | 11.278118 | 10.433765 | 12.069123 | 9.413776 | 10.713397 | 12.653321 | 14.952582 | 11.260899 | 10.472927 | 12.971466 | 11.185425 | 11.659318 | 10.648266 | 11.350723 | 9.151168 | 10.78771 | 10.067627 | 10.209941 |
hep-th/0503016 | Miguel Vazquez-Mozo | Luis Alvarez-Gaume, Miguel A. Vazquez-Mozo | On nonanticommutative N=2 sigma-models in two dimensions | 29 pages. Typos corrected and references added | JHEP 0504 (2005) 007 | 10.1088/1126-6708/2005/04/007 | CERN-PH-TH/033-2005 | hep-th | null | We study nonanticommutative deformations of N=2 two-dimensional Euclidean
sigma models. We find that these theories are described by simple deformations
of Zumino's Lagrangian and the holomorphic superpotential. Geometrically, this
deformation can be interpreted as a fuzziness in target space controlled by the
vacuum... | [
{
"created": "Wed, 2 Mar 2005 14:00:53 GMT",
"version": "v1"
},
{
"created": "Wed, 25 May 2005 13:22:48 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Alvarez-Gaume",
"Luis",
""
],
[
"Vazquez-Mozo",
"Miguel A.",
""
]
] | We study nonanticommutative deformations of N=2 two-dimensional Euclidean sigma models. We find that these theories are described by simple deformations of Zumino's Lagrangian and the holomorphic superpotential. Geometrically, this deformation can be interpreted as a fuzziness in target space controlled by the vacuum e... | 8.040674 | 7.804566 | 9.902359 | 7.792442 | 8.273872 | 8.503533 | 8.770563 | 7.916493 | 7.66398 | 9.118784 | 7.480628 | 7.551246 | 8.305431 | 7.72924 | 7.485173 | 7.872052 | 7.693844 | 7.897115 | 7.824315 | 8.498148 | 7.777055 |
1904.12786 | Jos\'e Manuel Izquierdo | Jos\'e A. de Azc\'arraga, Diego G\'utiez and Jos\'e M. Izquierdo | Extended $D=3$ Bargmann supergravity from a Lie algebra expansion | 17 pages | null | 10.1016/j.nuclphysb.2019.114706 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we show how the method of Lie algebra expansions may be used to
obtain, in a simple way, both the extended Bargmann Lie superalgebra and the
Chern-Simons action associated to it in three dimensions, starting from $D=3$,
$\mathcal{N}=2$ superPoincar\'e and its corresponding Chern-Simons
supergravity.
| [
{
"created": "Mon, 29 Apr 2019 15:58:24 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Jul 2019 10:05:48 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"de Azcárraga",
"José A.",
""
],
[
"Gútiez",
"Diego",
""
],
[
"Izquierdo",
"José M.",
""
]
] | In this paper we show how the method of Lie algebra expansions may be used to obtain, in a simple way, both the extended Bargmann Lie superalgebra and the Chern-Simons action associated to it in three dimensions, starting from $D=3$, $\mathcal{N}=2$ superPoincar\'e and its corresponding Chern-Simons supergravity. | 7.569637 | 5.775496 | 7.931949 | 5.978341 | 6.094432 | 5.970774 | 5.309978 | 5.252344 | 5.565515 | 8.096971 | 5.845591 | 6.321431 | 7.214502 | 6.19361 | 6.168162 | 6.653086 | 6.201976 | 6.092369 | 6.335566 | 7.311662 | 6.203064 |
1910.07019 | Victoria Volkova | S. Mironov, V. Rubakov, V. Volkova | Subluminal cosmological bounce beyond Horndeski | 24 pages, 12 figures. In v3: Major revision. A section on (the
absence of) superluminality in the presence of additional matter added.
Journal version, to appear in JCAP | null | 10.1088/1475-7516/2020/05/024 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We address the issue of potential superluminal propagation of gravitational
waves in backgrounds neighboring the previously suggested bounce
[arXiv:1807.08361] in beyond Horndeski theory. We find that the bouncing
solution lies right at the boundary of the region where the gravitational waves
propagate at speed excee... | [
{
"created": "Tue, 15 Oct 2019 19:39:22 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Oct 2019 12:12:42 GMT",
"version": "v2"
},
{
"created": "Sat, 25 Apr 2020 08:27:14 GMT",
"version": "v3"
}
] | 2020-05-20 | [
[
"Mironov",
"S.",
""
],
[
"Rubakov",
"V.",
""
],
[
"Volkova",
"V.",
""
]
] | We address the issue of potential superluminal propagation of gravitational waves in backgrounds neighboring the previously suggested bounce [arXiv:1807.08361] in beyond Horndeski theory. We find that the bouncing solution lies right at the boundary of the region where the gravitational waves propagate at speed exceedi... | 11.770512 | 12.90525 | 11.135881 | 11.510388 | 11.901505 | 11.85361 | 11.932127 | 11.55691 | 11.166006 | 12.035148 | 10.831225 | 11.013358 | 11.469905 | 11.249878 | 11.132801 | 11.183214 | 11.067893 | 10.919999 | 10.859406 | 10.954073 | 10.997065 |
1909.09027 | Mohamed Anber | Mohamed M. Anber, Erich Poppitz | On the baryon-color-flavor (BCF) anomaly in vector-like theories | 14 pages, typos corrected, matches the published version | null | 10.1007/JHEP11(2019)063 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the most general fractional background fluxes in the color,
flavor, and baryon number directions, compatible with the faithful action of
the global symmetry of a given theory. We call the obstruction to gauging
symmetries revealed by such backgrounds the baryon-color-flavor (BCF) 't Hooft
anomaly. We appl... | [
{
"created": "Thu, 19 Sep 2019 14:52:33 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Nov 2019 11:02:22 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Anber",
"Mohamed M.",
""
],
[
"Poppitz",
"Erich",
""
]
] | We consider the most general fractional background fluxes in the color, flavor, and baryon number directions, compatible with the faithful action of the global symmetry of a given theory. We call the obstruction to gauging symmetries revealed by such backgrounds the baryon-color-flavor (BCF) 't Hooft anomaly. We apply ... | 9.510459 | 9.632939 | 10.88525 | 9.214521 | 9.78472 | 10.460981 | 10.024172 | 9.915308 | 9.509544 | 11.634792 | 9.090933 | 9.795222 | 10.133434 | 9.454988 | 9.663401 | 9.81072 | 9.783676 | 9.800887 | 9.612516 | 9.887065 | 9.809075 |
hep-th/9111038 | null | Michael D. McGuigan, Chiara R. Nappi and Scott A. Yost | Charged Black Holes in Two-Dimensional String Theory | 39 pages | Nucl.Phys.B375:421-452,1992 | 10.1016/0550-3213(92)90039-E | null | hep-th | null | We discuss two dimensional string theories containing gauge fields introduced
either via coupling to open strings, in which case we get a Born-Infeld type
action, or via heterotic compactification. The solutions to the modified
background field equations are charged black holes which exhibit interesting
space-time ge... | [
{
"created": "Wed, 20 Nov 1991 16:54:00 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"McGuigan",
"Michael D.",
""
],
[
"Nappi",
"Chiara R.",
""
],
[
"Yost",
"Scott A.",
""
]
] | We discuss two dimensional string theories containing gauge fields introduced either via coupling to open strings, in which case we get a Born-Infeld type action, or via heterotic compactification. The solutions to the modified background field equations are charged black holes which exhibit interesting space-time geom... | 18.188267 | 14.595412 | 17.010246 | 14.530083 | 16.976059 | 14.338078 | 15.805893 | 15.082125 | 14.726058 | 17.458862 | 14.322827 | 15.962805 | 17.4088 | 16.437582 | 16.004776 | 16.493948 | 15.225863 | 15.806444 | 15.381981 | 17.026833 | 15.142689 |
hep-th/9506157 | Yao-zhong Zhang | Takeo Inami, Satoru Odake and Yao-Zhong Zhang | Supersymmetric extension of the sine-Gordon theory with integrable
boundary interactions | Latex 9 pages, submitted to Phys. Lett. B | Phys.Lett. B359 (1995) 118-124 | 10.1016/0370-2693(95)01072-X | Kyoto University and Shinshu University preprint YITP/K-1109,
DPSU-95-2 | hep-th cond-mat | null | Integrability and supersymmetry of the supersymmetric extension of the
sine-Gordon theory on a half-line are examined and the boundary potential which
preserves both the integrability and supersymmetry on the bulk is derived. It
appears that unlike the boundary bosonic sine-Gordon theory, integrability and
supersymme... | [
{
"created": "Fri, 23 Jun 1995 06:36:53 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Inami",
"Takeo",
""
],
[
"Odake",
"Satoru",
""
],
[
"Zhang",
"Yao-Zhong",
""
]
] | Integrability and supersymmetry of the supersymmetric extension of the sine-Gordon theory on a half-line are examined and the boundary potential which preserves both the integrability and supersymmetry on the bulk is derived. It appears that unlike the boundary bosonic sine-Gordon theory, integrability and supersymmetr... | 9.132339 | 7.783592 | 9.421111 | 7.731089 | 7.66369 | 7.233134 | 7.508669 | 7.196709 | 7.075275 | 10.664996 | 7.631314 | 7.551752 | 8.660915 | 7.953655 | 7.832544 | 7.986117 | 7.679222 | 7.810953 | 7.917714 | 8.560663 | 7.921266 |
2404.07173 | Seyed Morteza Hosseini | Edoardo Colombo, Seyed Morteza Hosseini, Dario Martelli, Antonio
Pittelli, Alberto Zaffaroni | Microstates of accelerating and supersymmetric AdS$_4$ black holes from
the spindle index | 6 pages, v2: references added | Phys. Rev. Lett. 133, 031603 (2024) | 10.1103/PhysRevLett.133.031603 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a first principles derivation of the microscopic entropy of a very
general class of supersymmetric, rotating and accelerating black holes in
AdS$_4$. This is achieved by analysing the large-$N$ limit of the spindle index
and completes the construction of the first example of a holographic duality
involving... | [
{
"created": "Wed, 10 Apr 2024 17:12:45 GMT",
"version": "v1"
},
{
"created": "Sun, 21 Jul 2024 17:41:20 GMT",
"version": "v2"
}
] | 2024-07-23 | [
[
"Colombo",
"Edoardo",
""
],
[
"Hosseini",
"Seyed Morteza",
""
],
[
"Martelli",
"Dario",
""
],
[
"Pittelli",
"Antonio",
""
],
[
"Zaffaroni",
"Alberto",
""
]
] | We provide a first principles derivation of the microscopic entropy of a very general class of supersymmetric, rotating and accelerating black holes in AdS$_4$. This is achieved by analysing the large-$N$ limit of the spindle index and completes the construction of the first example of a holographic duality involving s... | 11.139458 | 8.746566 | 11.719246 | 8.366456 | 8.4924 | 8.140176 | 7.995348 | 7.616561 | 8.447382 | 10.630534 | 8.247776 | 8.622981 | 10.543479 | 8.555909 | 8.765525 | 8.855509 | 8.850039 | 8.740148 | 8.699898 | 10.586252 | 8.692142 |
hep-th/9704101 | Vincent G. J. Rodgers | S. James Gates, Jr and V.G.J. Rodgers | Type -B/ -O Bosonic String Sigma-Models | 13 pages Latex, minor revisions including references | Phys.Lett. B405 (1997) 71-78 | 10.1016/S0370-2693(97)00620-5 | null | hep-th | null | We provide world sheet non-supersymmetrical actions that describe the
coupling of a bosonic string to the tachyon and massless states of both the
type-B and type-O theories. The type-B theory is derived as a truncation and
chiral doubling of the Ramond-Ramond sector in our previous model that
connected the (1,0) hete... | [
{
"created": "Mon, 14 Apr 1997 05:11:04 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Apr 1997 21:35:03 GMT",
"version": "v2"
}
] | 2012-08-27 | [
[
"Gates,",
"S. James",
"Jr"
],
[
"Rodgers",
"V. G. J.",
""
]
] | We provide world sheet non-supersymmetrical actions that describe the coupling of a bosonic string to the tachyon and massless states of both the type-B and type-O theories. The type-B theory is derived as a truncation and chiral doubling of the Ramond-Ramond sector in our previous model that connected the (1,0) hetero... | 12.894764 | 12.015886 | 14.329634 | 11.79315 | 12.632884 | 11.509456 | 11.873528 | 10.758988 | 10.950903 | 15.669566 | 11.672791 | 11.868399 | 12.433469 | 11.466503 | 11.837655 | 11.82794 | 11.460731 | 11.362036 | 11.427931 | 12.80863 | 11.365916 |
1007.5509 | Pablo G. Camara | G. Aldazabal, E. Andres, P. G. Camara and M. Gra\~na | U-dual fluxes and Generalized Geometry | 58 pages, 6 tables | JHEP 1011:083,2010 | 10.1007/JHEP11(2010)083 | CERN-PH-TH-2010-172, IPhT-T10/093 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform a systematic analysis of generic string flux compactifications,
making use of Exceptional Generalized Geometry (EGG) as an organizing
principle. In particular, we establish the precise map between fluxes, gaugings
of maximal 4d supergravity and EGG, identifying the complete set of gaugings
that admit an up... | [
{
"created": "Fri, 30 Jul 2010 18:09:04 GMT",
"version": "v1"
}
] | 2010-11-23 | [
[
"Aldazabal",
"G.",
""
],
[
"Andres",
"E.",
""
],
[
"Camara",
"P. G.",
""
],
[
"Graña",
"M.",
""
]
] | We perform a systematic analysis of generic string flux compactifications, making use of Exceptional Generalized Geometry (EGG) as an organizing principle. In particular, we establish the precise map between fluxes, gaugings of maximal 4d supergravity and EGG, identifying the complete set of gaugings that admit an upli... | 7.680011 | 7.474548 | 8.081546 | 7.108493 | 7.348364 | 7.416036 | 7.213887 | 7.101737 | 6.95004 | 8.678948 | 7.133232 | 7.665123 | 7.697397 | 7.382676 | 7.315007 | 7.369169 | 7.496603 | 7.471527 | 7.22625 | 7.655121 | 7.308309 |
1601.04732 | Mahdi Kord Zangeneh | M. Kord Zangeneh, A. Dehyadegari, A. Sheykhi and M. H. Dehghani | Thermodynamics and gauge/gravity duality for Lifshitz black holes in the
presence of exponential electrodynamics | 31 pages, 16 figures (some figures include two subfigures). V2: some
typos corrected, some references added | JHEP 1603, 037 (2016) | 10.1007/JHEP03(2016)037 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we construct a new class of topological black hole Lifshitz
solutions in the presence of nonlinear exponential electrodynamics for
Einstein-dilaton gravity. We show that the reality of Lifshitz supporting
Maxwell matter fields exclude the negative horizon curvature solutions except
for the asymptotic A... | [
{
"created": "Mon, 18 Jan 2016 21:43:37 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Mar 2016 01:29:50 GMT",
"version": "v2"
}
] | 2016-03-15 | [
[
"Zangeneh",
"M. Kord",
""
],
[
"Dehyadegari",
"A.",
""
],
[
"Sheykhi",
"A.",
""
],
[
"Dehghani",
"M. H.",
""
]
] | In this paper, we construct a new class of topological black hole Lifshitz solutions in the presence of nonlinear exponential electrodynamics for Einstein-dilaton gravity. We show that the reality of Lifshitz supporting Maxwell matter fields exclude the negative horizon curvature solutions except for the asymptotic AdS... | 8.474648 | 8.13109 | 8.624375 | 7.583659 | 8.431629 | 7.724607 | 8.318075 | 8.087255 | 7.920962 | 8.934319 | 8.047977 | 8.499143 | 8.131957 | 8.11171 | 8.242412 | 8.162564 | 8.327157 | 7.998572 | 7.947375 | 8.327544 | 8.086937 |
hep-th/0410160 | Hans Peter Nilles | Hans Peter Nilles | Five golden rules for superstring phenomenology | Based on talks given at the conference on ``String Phenomenology
2004, Ann Arbor, and ``Pascos04-NathFest Symposium'', Boston, August 2004 | null | 10.1142/9789812701756_0094 | null | hep-th hep-ph | null | Recent measurements of the values of gauge coupling constants as well as
neutrino properties support the idea of a grand unified (GUT) description of
particle physics at a large scale of $M_{GUT}\sim 10^{16}$ GeV. We discuss a
strategy to incorporate this picture in the framework of superstring theory. In
such a sche... | [
{
"created": "Thu, 14 Oct 2004 07:37:04 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Nilles",
"Hans Peter",
""
]
] | Recent measurements of the values of gauge coupling constants as well as neutrino properties support the idea of a grand unified (GUT) description of particle physics at a large scale of $M_{GUT}\sim 10^{16}$ GeV. We discuss a strategy to incorporate this picture in the framework of superstring theory. In such a scheme... | 7.183301 | 7.568972 | 6.884517 | 6.357296 | 7.702155 | 7.268842 | 6.788455 | 7.011233 | 6.956712 | 7.628246 | 6.905345 | 6.74207 | 6.670883 | 6.678816 | 6.8969 | 6.763669 | 6.785261 | 6.795223 | 6.639927 | 6.721016 | 6.930149 |
0704.0296 | Itzhak Bars | Itzhak Bars and Bora Orcal | Generalized Twistor Transform And Dualities, With A New Description of
Particles With Spin, Beyond Free and Massless | 33 pages | Phys.Rev.D75:104015,2007 | 10.1103/PhysRevD.75.104015 | USC-07/HEP-B3 | hep-th | null | A generalized twistor transform for spinning particles in 3+1 dimensions is
constructed that beautifully unifies many types of spinning systems by mapping
them to the same twistor, thus predicting an infinite set of duality relations
among spinning systems with different Hamiltonians. Usual 1T-physics is not
equipped... | [
{
"created": "Tue, 3 Apr 2007 01:01:13 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Apr 2007 13:56:25 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bars",
"Itzhak",
""
],
[
"Orcal",
"Bora",
""
]
] | A generalized twistor transform for spinning particles in 3+1 dimensions is constructed that beautifully unifies many types of spinning systems by mapping them to the same twistor, thus predicting an infinite set of duality relations among spinning systems with different Hamiltonians. Usual 1T-physics is not equipped t... | 13.300352 | 12.003469 | 14.176674 | 12.515418 | 13.366123 | 13.489689 | 13.068273 | 13.662164 | 12.50166 | 14.416531 | 12.641909 | 12.550953 | 13.356127 | 12.536631 | 12.985162 | 12.731644 | 12.642111 | 12.393874 | 12.235585 | 13.533371 | 12.638331 |
hep-th/0605037 | John Gracey | J. A. Gracey | Practicalities of renormalizing quantum field theories | 24 latex pages, talk presented at Renormalization and Universality in
Mathematical Physics Workshop, Toronto, 18-22 Oct, 2005 | null | null | LTH-701 | hep-th | null | We review the techniques used to renormalize quantum field theories at
several loop orders. This includes the techniques to systematically extract the
infinities in a Feynman integral and the implementation of the algorithm within
computer algebra. To illustrate the method we discuss the renormalization of
phi^4 theo... | [
{
"created": "Wed, 3 May 2006 10:30:11 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gracey",
"J. A.",
""
]
] | We review the techniques used to renormalize quantum field theories at several loop orders. This includes the techniques to systematically extract the infinities in a Feynman integral and the implementation of the algorithm within computer algebra. To illustrate the method we discuss the renormalization of phi^4 theory... | 9.768826 | 8.41232 | 9.016889 | 9.132834 | 8.457014 | 9.201035 | 8.140808 | 9.72721 | 8.992109 | 9.785099 | 8.684965 | 8.663357 | 9.08827 | 8.617962 | 8.657519 | 8.451378 | 8.556475 | 9.134512 | 8.923455 | 9.43328 | 8.674224 |
1804.05396 | Alessandro Pini | Thomas Bourton, Alessandro Pini and Elli Pomoni | 4d $\mathcal{N}=3$ indices via discrete gauging | 34 pages | null | 10.1007/JHEP10(2018)131 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A class of 4d $\mathcal{N}=3$ SCFTs can be obtained from gauging a discrete
subgroup of the global symmetry group of $\mathcal{N}=4$ Super Yang-Mills
theory. This discrete subgroup contains elements of both the $SU(4)$ R-symmetry
group and the $SL(2,\mathbb{Z})$ S-duality group of $\mathcal{N}=4$ SYM. We
give a presc... | [
{
"created": "Sun, 15 Apr 2018 18:00:01 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Dec 2020 07:45:37 GMT",
"version": "v2"
}
] | 2020-12-11 | [
[
"Bourton",
"Thomas",
""
],
[
"Pini",
"Alessandro",
""
],
[
"Pomoni",
"Elli",
""
]
] | A class of 4d $\mathcal{N}=3$ SCFTs can be obtained from gauging a discrete subgroup of the global symmetry group of $\mathcal{N}=4$ Super Yang-Mills theory. This discrete subgroup contains elements of both the $SU(4)$ R-symmetry group and the $SL(2,\mathbb{Z})$ S-duality group of $\mathcal{N}=4$ SYM. We give a prescri... | 5.004683 | 4.398913 | 5.415349 | 4.456847 | 4.688301 | 4.849029 | 4.562378 | 4.404589 | 4.522642 | 5.951497 | 4.521618 | 4.51869 | 5.113625 | 4.458917 | 4.594758 | 4.523788 | 4.567971 | 4.747284 | 4.495868 | 5.068091 | 4.601388 |
0905.0957 | Yun Soo Myung | Yun Soo Myung | Thermodynamics of black holes in the deformed Ho\v{r}ava-Lifshitz
gravity | 10 pages, 3 figures, final version to appear in PLB | null | 10.1016/j.physletb.2009.06.013 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study thermodynamics of black holes in the deformed Ho\v{r}ava-Lifshitz
gravity with coupling constant $\lambda$.
For $\lambda=1$, the black hole behaves the
Reissner-Norstr\"om black hole. Hence, this is different from the
Schwarzschild black hole of Einstein gravity. A connection to the generalized
uncertain... | [
{
"created": "Thu, 7 May 2009 07:21:22 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jun 2009 03:00:50 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"Myung",
"Yun Soo",
""
]
] | We study thermodynamics of black holes in the deformed Ho\v{r}ava-Lifshitz gravity with coupling constant $\lambda$. For $\lambda=1$, the black hole behaves the Reissner-Norstr\"om black hole. Hence, this is different from the Schwarzschild black hole of Einstein gravity. A connection to the generalized uncertainty pri... | 6.317796 | 5.264405 | 5.117296 | 4.676854 | 5.115116 | 5.019656 | 5.726294 | 4.6396 | 4.979702 | 5.170695 | 5.615936 | 5.516411 | 5.362164 | 5.244331 | 5.600028 | 5.552017 | 5.473832 | 5.117103 | 5.561423 | 5.21741 | 5.53485 |
1811.06228 | Bengt E. W. Nilsson | B.E.W. Nilsson, A. Padellaro and C.N. Pope | The role of singletons in $S^7$ compactifications | 24 pages including appendix with 12 figure, v2 minor typos corrected | null | 10.1007/JHEP07(2019)124 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the isometry irrep content of squashed seven-sphere
compactifications of eleven-dimensional supergravity, i.e., the left-squashed
($LS^7$) with ${\mathcal N}=1$ and right-squashed ($RS^7$) with ${\mathcal
N}=0$ supersymmetry, in a manner completely independent of the round sphere.
Then we compare this resul... | [
{
"created": "Thu, 15 Nov 2018 08:27:04 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Feb 2019 13:46:54 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"Nilsson",
"B. E. W.",
""
],
[
"Padellaro",
"A.",
""
],
[
"Pope",
"C. N.",
""
]
] | We derive the isometry irrep content of squashed seven-sphere compactifications of eleven-dimensional supergravity, i.e., the left-squashed ($LS^7$) with ${\mathcal N}=1$ and right-squashed ($RS^7$) with ${\mathcal N}=0$ supersymmetry, in a manner completely independent of the round sphere. Then we compare this result ... | 7.091109 | 6.646304 | 7.753413 | 6.721636 | 6.963146 | 7.229918 | 6.84364 | 6.799962 | 6.399355 | 8.570348 | 6.785567 | 6.716776 | 7.16583 | 6.702687 | 6.737806 | 6.58722 | 6.887731 | 6.851465 | 6.787793 | 6.8118 | 6.661421 |
hep-th/0108092 | Ysmyung | Y. S. Myung (Inje Univ) | Quintessence with a localized scalar field on the brane | 12page, version to appear in MPLA | Mod.Phys.Lett. A16 (2001) 1963-1972 | 10.1142/S0217732301005308 | INJE-TP-01-07 | hep-th | null | We study issues of the quintessence in the brane cosmology. The initial bulk
spacetime consists of two 5D topological anti de Sitter black hole joined by
the brane (moving domain wall). Here we do not introduce any conventional
radiation and matter. Instead we include a localized scalar on the brane as a
stress-energ... | [
{
"created": "Tue, 14 Aug 2001 02:32:23 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Sep 2001 02:10:55 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Oct 2001 07:18:47 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Myung",
"Y. S.",
"",
"Inje Univ"
]
] | We study issues of the quintessence in the brane cosmology. The initial bulk spacetime consists of two 5D topological anti de Sitter black hole joined by the brane (moving domain wall). Here we do not introduce any conventional radiation and matter. Instead we include a localized scalar on the brane as a stress-energy ... | 14.446341 | 14.954687 | 14.22388 | 13.686997 | 14.138616 | 13.406182 | 14.175773 | 12.976604 | 13.730772 | 15.735892 | 12.917337 | 13.779488 | 14.292978 | 13.540484 | 13.793415 | 13.96989 | 13.484065 | 14.001046 | 13.863638 | 14.172143 | 13.669644 |
0804.4096 | Gabor Takacs | G. Takacs | Finite temperature expectation values of boundary operators | 26 pages, 4 eps figures, latex2e file. v2: A formula added, some
typos are corrected | Nucl.Phys.B805:391-417,2008 | 10.1016/j.nuclphysb.2008.06.014 | ITP-Budapest Report No. 639 | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A conjecture is presented for the thermal one-point function of boundary
operators in integrable boundary quantum field theories in terms of form
factors. It is expected to have applications in studying boundary critical
phenomena and boundary flows, which are relevant in the context of condensed
matter and string th... | [
{
"created": "Fri, 25 Apr 2008 12:05:58 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Jun 2008 06:24:06 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Takacs",
"G.",
""
]
] | A conjecture is presented for the thermal one-point function of boundary operators in integrable boundary quantum field theories in terms of form factors. It is expected to have applications in studying boundary critical phenomena and boundary flows, which are relevant in the context of condensed matter and string theo... | 10.418021 | 8.738418 | 10.160012 | 8.20644 | 7.662475 | 8.306149 | 8.5611 | 8.656233 | 7.804924 | 11.650493 | 8.649341 | 8.02835 | 10.037878 | 8.379865 | 7.977707 | 8.273961 | 8.166516 | 8.146629 | 8.211117 | 9.855467 | 8.432016 |
1405.2325 | Falk Hassler | Falk Hassler and Dieter Lust and Stefano Massai | On Inflation and de Sitter in Non-Geometric String Backgrounds | 21 pages, 2 figures, references added, typos corrected, note added | null | null | LMU-ASC 35/14, MPP-2014-222 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the problem of obtaining de Sitter and inflationary vacua from
dimensional reduction of double field theory (DFT) on nongeometric string
backgrounds. In this context, we consider a new class of effective potentials
that admit Minkowski and de Sitter minima. We then construct a simple model of
chaotic inflati... | [
{
"created": "Fri, 9 May 2014 19:30:40 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Jun 2014 18:55:34 GMT",
"version": "v2"
},
{
"created": "Wed, 4 May 2016 19:49:47 GMT",
"version": "v3"
}
] | 2016-05-05 | [
[
"Hassler",
"Falk",
""
],
[
"Lust",
"Dieter",
""
],
[
"Massai",
"Stefano",
""
]
] | We study the problem of obtaining de Sitter and inflationary vacua from dimensional reduction of double field theory (DFT) on nongeometric string backgrounds. In this context, we consider a new class of effective potentials that admit Minkowski and de Sitter minima. We then construct a simple model of chaotic inflation... | 9.751244 | 8.550698 | 12.012718 | 8.327425 | 8.966003 | 9.125347 | 8.793326 | 9.265357 | 8.215427 | 10.939727 | 8.768471 | 9.032955 | 9.739487 | 9.061966 | 9.082575 | 9.437151 | 9.262232 | 9.443679 | 8.8188 | 10.032296 | 9.096022 |
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