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/0505020 | Qing-Guo Huang | Qing-Guo Huang, Ke Ke and Miao Li | One conjecture and two observations on de Sitter space | 12 pages, harvmac; references added; version for publication in JHEP | JHEP0602:045,2006 | 10.1088/1126-6708/2006/02/045 | null | hep-th | null | We propose that the state represented by the Nariai black hole inside de
Sitter space is the ground state of the de Sitter gravity, while the pure de
Sitter space is the maximal energy state. With this point of view, we
investigate thermodynamics of de Sitter space, we find that if there is a dual
field theory, this ... | [
{
"created": "Tue, 3 May 2005 08:25:34 GMT",
"version": "v1"
},
{
"created": "Mon, 9 May 2005 08:38:59 GMT",
"version": "v2"
},
{
"created": "Thu, 3 Nov 2005 02:39:54 GMT",
"version": "v3"
},
{
"created": "Fri, 17 Feb 2006 09:33:52 GMT",
"version": "v4"
},
{
"crea... | 2009-11-11 | [
[
"Huang",
"Qing-Guo",
""
],
[
"Ke",
"Ke",
""
],
[
"Li",
"Miao",
""
]
] | We propose that the state represented by the Nariai black hole inside de Sitter space is the ground state of the de Sitter gravity, while the pure de Sitter space is the maximal energy state. With this point of view, we investigate thermodynamics of de Sitter space, we find that if there is a dual field theory, this th... | 9.039042 | 9.204991 | 8.989501 | 8.648421 | 9.260368 | 8.629858 | 8.719028 | 8.637793 | 8.445702 | 9.747686 | 8.534072 | 8.407013 | 8.430593 | 8.363959 | 8.472119 | 8.497179 | 8.429735 | 8.515331 | 8.536137 | 8.443003 | 8.345874 |
0905.0709 | Neil Turok | Ben Craps, Thomas Hertog, Neil Turok | A multitrace deformation of ABJM theory | 14 pages, 4 figures; v3. Clarification of precise relation to
$O(N)\times O(N)$ model and other minor comments added | Phys.Rev.D80:086007,2009 | 10.1103/PhysRevD.80.086007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the study of big crunch singularities in asymptotically $AdS_4$
spacetimes, we consider a marginal triple trace deformation of ABJM theory. The
deformation corresponds to adding a potential which is unbounded below. In a 't
Hooft large N limit, the beta function for the triple trace deformation
vanishes,... | [
{
"created": "Tue, 5 May 2009 21:34:47 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Jul 2009 22:19:41 GMT",
"version": "v2"
},
{
"created": "Sun, 13 Sep 2009 22:26:11 GMT",
"version": "v3"
}
] | 2009-10-29 | [
[
"Craps",
"Ben",
""
],
[
"Hertog",
"Thomas",
""
],
[
"Turok",
"Neil",
""
]
] | Motivated by the study of big crunch singularities in asymptotically $AdS_4$ spacetimes, we consider a marginal triple trace deformation of ABJM theory. The deformation corresponds to adding a potential which is unbounded below. In a 't Hooft large N limit, the beta function for the triple trace deformation vanishes, w... | 7.033259 | 7.270418 | 7.458125 | 6.806034 | 6.474049 | 6.6121 | 6.885638 | 6.626944 | 6.602083 | 8.425963 | 6.66403 | 6.962189 | 7.093576 | 6.667788 | 6.577057 | 6.656158 | 6.652555 | 6.464314 | 6.742367 | 7.132807 | 6.663081 |
2003.13700 | Jeffrey Harvey | Jeffrey A. Harvey and Gregory W. Moore | Moonshine, Superconformal Symmetry, and Quantum Error Correction | only 53 pages | null | 10.1007/JHEP05(2020)146 | null | hep-th math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Special conformal field theories can have symmetry groups which are
interesting sporadic finite simple groups. Famous examples include the Monster
symmetry group of a $c=24$ two-dimensional conformal field theory (CFT)
constructed by Frenkel, Lepowsky and Meurman, and the Conway symmetry group of
a $c=12$ CFT explore... | [
{
"created": "Mon, 30 Mar 2020 18:00:02 GMT",
"version": "v1"
}
] | 2020-06-24 | [
[
"Harvey",
"Jeffrey A.",
""
],
[
"Moore",
"Gregory W.",
""
]
] | Special conformal field theories can have symmetry groups which are interesting sporadic finite simple groups. Famous examples include the Monster symmetry group of a $c=24$ two-dimensional conformal field theory (CFT) constructed by Frenkel, Lepowsky and Meurman, and the Conway symmetry group of a $c=12$ CFT explored ... | 6.422597 | 7.520758 | 8.329735 | 6.859862 | 8.281477 | 8.115987 | 7.746806 | 7.276021 | 7.031992 | 8.851378 | 7.315851 | 6.458265 | 6.923825 | 6.445853 | 6.571877 | 6.520325 | 6.569206 | 6.407964 | 6.478483 | 6.703895 | 6.436538 |
1110.6494 | Jos\'e Alejandro Rosabal Rodr\'iguez | Jos\'e A. Rosabal | Coleman de Luccia geometry reconsidered and ADS/CFT | 10 pages, minor corrections made | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reconsidered the Coleman de Luccia solution building an AdS4 bubble
expanding into a false flat vacuum. In this construction when junction
conditions are imposed we find an upper bound to the radius of the AdS4 and a
domain wall whose tension is a function of the minimum of the scalar potential.
We prove that this... | [
{
"created": "Sat, 29 Oct 2011 02:49:29 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Nov 2011 00:00:51 GMT",
"version": "v2"
}
] | 2011-11-14 | [
[
"Rosabal",
"José A.",
""
]
] | We reconsidered the Coleman de Luccia solution building an AdS4 bubble expanding into a false flat vacuum. In this construction when junction conditions are imposed we find an upper bound to the radius of the AdS4 and a domain wall whose tension is a function of the minimum of the scalar potential. We prove that this s... | 13.5637 | 11.101666 | 11.407243 | 10.856919 | 12.079366 | 11.155178 | 11.509162 | 11.381977 | 11.454333 | 12.33934 | 11.335097 | 11.081608 | 11.613873 | 11.445281 | 11.428986 | 11.244522 | 11.580368 | 11.365287 | 11.17614 | 11.458283 | 11.085962 |
2308.03848 | Alessandro Pini | Alessandro Pini, Paolo Vallarino | Wilson loop correlators at strong coupling in $\mathcal{N}=2$ quiver
gauge theories | null | JHEP 11 (2023) 003 | 10.1007/JHEP11(2023)003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider 4-dimensional $\mathcal{N} = 2$ superconformal quiver theories
with $SU(N)^M$ gauge group and bi-fundamental matter and we evaluate
correlation functions of $n$ coincident Wilson loops in the planar limit of the
theory. Exploiting specific untwisted/twisted combinations of these operators
and using supers... | [
{
"created": "Mon, 7 Aug 2023 18:01:09 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Nov 2023 12:41:08 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Dec 2023 13:01:07 GMT",
"version": "v3"
}
] | 2023-12-06 | [
[
"Pini",
"Alessandro",
""
],
[
"Vallarino",
"Paolo",
""
]
] | We consider 4-dimensional $\mathcal{N} = 2$ superconformal quiver theories with $SU(N)^M$ gauge group and bi-fundamental matter and we evaluate correlation functions of $n$ coincident Wilson loops in the planar limit of the theory. Exploiting specific untwisted/twisted combinations of these operators and using supersym... | 6.582957 | 6.089017 | 6.855031 | 5.959291 | 5.824553 | 5.893894 | 5.958513 | 5.929521 | 5.854313 | 7.210634 | 6.000732 | 6.171215 | 6.415693 | 6.086003 | 6.13996 | 6.080117 | 5.972023 | 6.145521 | 6.096674 | 6.290421 | 5.936533 |
1111.6567 | Phillip Szepietowski | Nick Halmagyi, James T. Liu and Phillip Szepietowski | On N = 2 Truncations of IIB on T^{1,1} | 32 pages, v2:references added | null | 10.1007/JHEP07(2012)098 | MCTP-11-41 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the N=4 gauged supergravity theory which arises from the consistent
truncation of IIB supergravity on the coset T^{1,1}. We analyze three N=2
subsectors and in particular we clarify the relationship between true
superpotentials for gauged supergravity and certain fake superpotentials which
have been widely u... | [
{
"created": "Mon, 28 Nov 2011 19:57:11 GMT",
"version": "v1"
},
{
"created": "Sat, 10 Mar 2012 16:49:43 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Halmagyi",
"Nick",
""
],
[
"Liu",
"James T.",
""
],
[
"Szepietowski",
"Phillip",
""
]
] | We study the N=4 gauged supergravity theory which arises from the consistent truncation of IIB supergravity on the coset T^{1,1}. We analyze three N=2 subsectors and in particular we clarify the relationship between true superpotentials for gauged supergravity and certain fake superpotentials which have been widely use... | 7.702097 | 7.967911 | 8.763659 | 7.208633 | 8.137011 | 7.687896 | 7.781054 | 7.060117 | 6.97181 | 9.282048 | 7.532483 | 7.734911 | 7.920488 | 7.553697 | 7.500578 | 7.713199 | 7.283089 | 7.591986 | 7.336134 | 7.953653 | 7.4248 |
1711.08370 | Rudnei O. Ramos | Robert Brandenberger, Qiuyue Liang, Rudnei O. Ramos and Siyi Zhou | Fluctuations through a Vibrating Bounce | 17 pages, 5 figures | Phys. Rev. D 97, 043504 (2018) | 10.1103/PhysRevD.97.043504 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the evolution of cosmological perturbations in a non-singular
bouncing cosmology with a bounce phase which has superimposed oscillations of
the scale factor. We identify length scales for which the final spectrum of
fluctuations obtains imprints of the non-trivial bounce dynamics. These
imprints in the spect... | [
{
"created": "Wed, 22 Nov 2017 16:21:28 GMT",
"version": "v1"
}
] | 2018-02-14 | [
[
"Brandenberger",
"Robert",
""
],
[
"Liang",
"Qiuyue",
""
],
[
"Ramos",
"Rudnei O.",
""
],
[
"Zhou",
"Siyi",
""
]
] | We study the evolution of cosmological perturbations in a non-singular bouncing cosmology with a bounce phase which has superimposed oscillations of the scale factor. We identify length scales for which the final spectrum of fluctuations obtains imprints of the non-trivial bounce dynamics. These imprints in the spectru... | 12.409031 | 12.799713 | 11.747632 | 11.324509 | 12.280727 | 12.978003 | 11.477824 | 11.995592 | 12.694534 | 13.016052 | 12.703366 | 11.519312 | 12.126892 | 12.519668 | 12.066166 | 11.839061 | 12.186503 | 11.532444 | 12.090355 | 12.094291 | 11.760768 |
1401.2409 | Pietro Menotti | Pietro Menotti | On the monodromy problem for the four-punctured sphere | 14 pages LaTeX, 1 figure. Notation improved; Sec.4 extended to
include the complete second order computation | null | 10.1088/1751-8113/47/41/415201 | IFUP-TH/2014-1 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the monodromy problem for the four-punctured sphere in which the
character of one composite monodromy is fixed, by looking at the expansion of
the accessory parameter in the modulus $x$ directly, without taking the limit
of the quantum conformal blocks for infinite central charge. The integrals
which appe... | [
{
"created": "Fri, 10 Jan 2014 17:34:09 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jan 2014 09:04:25 GMT",
"version": "v2"
},
{
"created": "Sun, 6 Apr 2014 14:33:09 GMT",
"version": "v3"
}
] | 2015-06-18 | [
[
"Menotti",
"Pietro",
""
]
] | We consider the monodromy problem for the four-punctured sphere in which the character of one composite monodromy is fixed, by looking at the expansion of the accessory parameter in the modulus $x$ directly, without taking the limit of the quantum conformal blocks for infinite central charge. The integrals which appear... | 9.340147 | 10.136661 | 10.038403 | 9.081758 | 9.39029 | 10.175472 | 9.17453 | 9.155899 | 8.657493 | 11.268501 | 8.783244 | 9.216413 | 9.130978 | 9.434197 | 9.403289 | 9.309509 | 9.637298 | 8.853174 | 9.019163 | 9.046125 | 9.064416 |
0801.3583 | Bibhas Majhi Ranjan | Rabin Banerjee, Bibhas Ranjan Majhi and Saurav Samanta | Noncommutative Black Hole Thermodynamics | LaTex, 17 pages, 2 figures, minor changes, references added, to
appear in Phys. Rev. D | Phys.Rev.D77:124035,2008 | 10.1103/PhysRevD.77.124035 | null | hep-th gr-qc | null | We give a general derivation, for any static spherically symmetric metric, of
the relation $T_h=\frac{\cal K}{2\pi}$ connecting the black hole temperature
($T_h$) with the surface gravity ($\cal K$), following the tunneling
interpretation of Hawking radiation. This derivation is valid even beyond the
semi classical r... | [
{
"created": "Wed, 23 Jan 2008 14:24:20 GMT",
"version": "v1"
},
{
"created": "Tue, 6 May 2008 08:42:18 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Banerjee",
"Rabin",
""
],
[
"Majhi",
"Bibhas Ranjan",
""
],
[
"Samanta",
"Saurav",
""
]
] | We give a general derivation, for any static spherically symmetric metric, of the relation $T_h=\frac{\cal K}{2\pi}$ connecting the black hole temperature ($T_h$) with the surface gravity ($\cal K$), following the tunneling interpretation of Hawking radiation. This derivation is valid even beyond the semi classical reg... | 7.658444 | 7.056038 | 6.905334 | 6.966572 | 6.747396 | 6.917147 | 7.363422 | 6.410132 | 6.627496 | 6.843832 | 6.898461 | 7.330739 | 7.097862 | 6.981696 | 7.032237 | 7.027687 | 7.216514 | 7.107808 | 7.20132 | 7.381038 | 7.239239 |
0904.2932 | Katrin Becker | Katrin Becker, Chris Bertinato, Yu-Chieh Chung and Guangyu Guo | Supersymmetry breaking, heterotic strings and fluxes | 26 pages, corrected typos, added references | Nucl.Phys.B823:428-447,2009 | 10.1016/j.nuclphysb.2009.07.025 | MIFP-09-14, NSF-KITP-09-30 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we consider compactifications of heterotic strings in the
presence of background flux. The background metric is a T^2 fibration over a K3
base times four-dimensional Minkowski space. Depending on the choice of
three-form flux different amounts of supersymmetry are preserved (N=2,1,0). For
supersymmetric... | [
{
"created": "Sun, 19 Apr 2009 20:28:13 GMT",
"version": "v1"
},
{
"created": "Mon, 4 May 2009 19:41:24 GMT",
"version": "v2"
}
] | 2011-04-14 | [
[
"Becker",
"Katrin",
""
],
[
"Bertinato",
"Chris",
""
],
[
"Chung",
"Yu-Chieh",
""
],
[
"Guo",
"Guangyu",
""
]
] | In this paper we consider compactifications of heterotic strings in the presence of background flux. The background metric is a T^2 fibration over a K3 base times four-dimensional Minkowski space. Depending on the choice of three-form flux different amounts of supersymmetry are preserved (N=2,1,0). For supersymmetric s... | 7.623302 | 6.256827 | 7.387499 | 6.761608 | 6.945346 | 6.759475 | 6.815741 | 6.203959 | 6.488428 | 7.989279 | 6.370535 | 6.556067 | 7.273883 | 6.767305 | 6.830554 | 6.659263 | 6.665837 | 6.563719 | 6.625834 | 7.064816 | 6.770603 |
1006.3510 | M. Hossein Dehghani | M. H. Dehghani and R. B. Mann | Thermodynamics of Lovelock-Lifshitz Black Branes | 16 pages, no figure, typos fixed | Phys.Rev.D82:064019,2010 | 10.1103/PhysRevD.82.064019 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the thermodynamics of Lovelock-Lifshitz black branes. We begin
by introducing the finite action of third order Lovelock gravity in the
presence of a massive vector field for a flat boundary, and use it to compute
the energy density of these black branes. Using the field equations, we find a
conserved q... | [
{
"created": "Thu, 17 Jun 2010 16:35:05 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Sep 2010 13:00:32 GMT",
"version": "v2"
}
] | 2014-11-21 | [
[
"Dehghani",
"M. H.",
""
],
[
"Mann",
"R. B.",
""
]
] | We investigate the thermodynamics of Lovelock-Lifshitz black branes. We begin by introducing the finite action of third order Lovelock gravity in the presence of a massive vector field for a flat boundary, and use it to compute the energy density of these black branes. Using the field equations, we find a conserved qua... | 6.296943 | 6.593052 | 6.81814 | 5.915446 | 6.461424 | 6.368757 | 6.475914 | 5.980315 | 6.11498 | 6.998861 | 6.28376 | 6.310862 | 6.131753 | 6.027279 | 6.143171 | 6.24755 | 6.131071 | 6.314313 | 6.051873 | 6.28353 | 6.106396 |
0707.0957 | Andrea Fuster | A. Coley, A. Fuster and S. Hervik | Supergravity solutions with constant scalar invariants | 12 pages; to appear in IJMPA | null | null | NIKHEF/2007-016 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a class of constant scalar invariant (CSI) spacetimes, which belong
to the higher-dimensional Kundt class, that are solutions of supergravity. We
review the known CSI supergravity solutions in this class and we explicitly
present a number of new exact CSI supergravity solutions, some of which are
Einstein.
| [
{
"created": "Fri, 6 Jul 2007 12:29:38 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Dec 2008 08:27:00 GMT",
"version": "v2"
}
] | 2008-12-17 | [
[
"Coley",
"A.",
""
],
[
"Fuster",
"A.",
""
],
[
"Hervik",
"S.",
""
]
] | We study a class of constant scalar invariant (CSI) spacetimes, which belong to the higher-dimensional Kundt class, that are solutions of supergravity. We review the known CSI supergravity solutions in this class and we explicitly present a number of new exact CSI supergravity solutions, some of which are Einstein. | 11.229074 | 10.781896 | 10.044196 | 8.982009 | 10.635074 | 10.030626 | 10.581093 | 8.326534 | 9.832093 | 9.953039 | 10.247887 | 9.955411 | 9.821666 | 9.309481 | 10.245546 | 9.605502 | 9.971302 | 9.363702 | 10.178675 | 9.642432 | 9.503117 |
1807.07871 | Isobel Kolb\'e | Sylvain Mogliacci, Isobel Kolb\'e, W. A. Horowitz | Geometrically confined thermal field theory: Finite size corrections and
phase transitions | 47 pages, 15 figures | Phys. Rev. D 102, 116017 (2020) | 10.1103/PhysRevD.102.116017 | INT-PUB-20-045 | hep-th cond-mat.quant-gas cond-mat.stat-mech hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the recent shocking results from RHIC and LHC that show
quark-gluon plasma signatures in small systems, we study a simple model of a
massless, noninteracting scalar field confined with Dirichlet boundary
conditions. We use this system to investigate the finite size corrections to
thermal field theoretica... | [
{
"created": "Thu, 19 Jul 2018 17:44:23 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jan 2021 19:04:55 GMT",
"version": "v2"
}
] | 2021-01-06 | [
[
"Mogliacci",
"Sylvain",
""
],
[
"Kolbé",
"Isobel",
""
],
[
"Horowitz",
"W. A.",
""
]
] | Motivated by the recent shocking results from RHIC and LHC that show quark-gluon plasma signatures in small systems, we study a simple model of a massless, noninteracting scalar field confined with Dirichlet boundary conditions. We use this system to investigate the finite size corrections to thermal field theoreticall... | 10.761994 | 12.194973 | 11.235087 | 10.515927 | 11.837946 | 12.18544 | 11.708854 | 11.228374 | 10.501208 | 11.427806 | 10.656656 | 11.015898 | 10.876698 | 10.440569 | 10.923846 | 11.174773 | 11.138412 | 10.923487 | 10.543766 | 10.869859 | 10.659567 |
2312.11238 | Sascha Gehrmann | Holger Frahm, Sascha Gehrmann and Gleb A. Kotousov | Scaling limit of the staggered six-vertex model with
$U_q\big(\mathfrak{sl}(2)\big)$ invariant boundary conditions | 35 pages, minor revisions made, SciPost style used | SciPost Phys. 16, 149 (2024) | 10.21468/SciPostPhys.16.6.149 | null | hep-th cond-mat.stat-mech math-ph math.MP | http://creativecommons.org/licenses/by-sa/4.0/ | We study the scaling limit of a statistical system, which is a special case
of the integrable inhomogeneous six-vertex model. It possesses
$U_q\big(\mathfrak{sl}(2)\big)$ invariance due to the choice of open boundary
conditions imposed. An interesting feature of the lattice theory is that the
spectrum of scaling dime... | [
{
"created": "Mon, 18 Dec 2023 14:36:51 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Dec 2023 17:00:17 GMT",
"version": "v2"
},
{
"created": "Thu, 4 Apr 2024 09:41:20 GMT",
"version": "v3"
}
] | 2024-06-05 | [
[
"Frahm",
"Holger",
""
],
[
"Gehrmann",
"Sascha",
""
],
[
"Kotousov",
"Gleb A.",
""
]
] | We study the scaling limit of a statistical system, which is a special case of the integrable inhomogeneous six-vertex model. It possesses $U_q\big(\mathfrak{sl}(2)\big)$ invariance due to the choice of open boundary conditions imposed. An interesting feature of the lattice theory is that the spectrum of scaling dimens... | 8.109924 | 7.63385 | 9.154727 | 7.149469 | 7.525014 | 7.887378 | 7.687212 | 7.526366 | 7.354227 | 9.287624 | 7.146099 | 7.573072 | 8.318514 | 7.656355 | 7.85104 | 7.411932 | 7.687687 | 7.584859 | 7.657822 | 8.120681 | 7.402949 |
2404.05918 | Azadeh Mohammadi | Jo\'as Ven\^ancio, Lameque Filho, Herondy Mota and Azadeh Mohammadi | Thermal Casimir effect for a Dirac field on flat space with a nontrivial
circular boundary condition | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | This work investigates the thermal Casimir effect associated with a massive
spinor field defined on a four-dimensional flat space with a circularly
compactified spatial dimension whose periodicity is oriented along a vector in
$xy$-plane. We employ the generalized zeta function method to establish a
finite definition... | [
{
"created": "Tue, 9 Apr 2024 00:37:23 GMT",
"version": "v1"
}
] | 2024-04-10 | [
[
"Venâncio",
"Joás",
""
],
[
"Filho",
"Lameque",
""
],
[
"Mota",
"Herondy",
""
],
[
"Mohammadi",
"Azadeh",
""
]
] | This work investigates the thermal Casimir effect associated with a massive spinor field defined on a four-dimensional flat space with a circularly compactified spatial dimension whose periodicity is oriented along a vector in $xy$-plane. We employ the generalized zeta function method to establish a finite definition f... | 13.712415 | 12.976846 | 12.561413 | 12.522999 | 13.783989 | 13.632778 | 14.237755 | 12.958129 | 13.478691 | 14.12579 | 12.937773 | 12.647305 | 13.444177 | 13.031101 | 12.679864 | 12.646274 | 12.85425 | 13.005982 | 13.107742 | 13.800365 | 12.930578 |
hep-th/9502089 | null | G. Bonelli, P.A. Marchetti and M. Matone | Algebraic-geometrical formulation of two-dimensional quantum gravity | 10 pages, Latex file | Lett.Math.Phys. 36 (1996) 189-196 | 10.1007/BF00714381 | DFPD 95/TH/05 | hep-th alg-geom gr-qc math.AG math.QA nlin.SI q-alg solv-int | null | We find a volume form on moduli space of double punctured Riemann surfaces
whose integral satisfies the Painlev\'e I recursion relations of the genus
expansion of the specific heat of 2D gravity. This allows us to express the
asymptotic expansion of the specific heat as an integral on an infinite
dimensional moduli s... | [
{
"created": "Tue, 14 Feb 1995 16:30:26 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Bonelli",
"G.",
""
],
[
"Marchetti",
"P. A.",
""
],
[
"Matone",
"M.",
""
]
] | We find a volume form on moduli space of double punctured Riemann surfaces whose integral satisfies the Painlev\'e I recursion relations of the genus expansion of the specific heat of 2D gravity. This allows us to express the asymptotic expansion of the specific heat as an integral on an infinite dimensional moduli spa... | 11.735818 | 10.928683 | 12.16964 | 9.954971 | 11.81662 | 9.714355 | 10.619469 | 9.542374 | 10.161309 | 11.184883 | 9.633849 | 10.114744 | 10.158652 | 9.862575 | 9.718469 | 9.660254 | 9.707756 | 10.289579 | 9.876562 | 10.091163 | 9.341344 |
2012.12021 | Rudra Prakash Malik | A. K. Rao, A. Tripathi, R. P. Malik | Supervariable and BRST Approaches to a Reparameterization Invariant
Non-Relativistic System | LaTeX file, 31 pages, Version to appear in AHEP (2021) | Advances in High Energy Physics, vol. 2021, Article ID 5593434, 20
pages, 2021 | 10.1155/2021/5593434. | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We exploit the theoretical strength of the supervariable and
Becchi-Rouet-Stora-Tyutin (BRST) formalisms to derive the proper (i.e.
off-shell nilpotent and absolutely anticommuting) (anti-)BRST symmetry
transformations for the reparameterization invariant model of a
non-relativistic (NR) free particle whose space $(x... | [
{
"created": "Tue, 22 Dec 2020 14:13:02 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Jun 2021 14:19:29 GMT",
"version": "v2"
}
] | 2021-07-27 | [
[
"Rao",
"A. K.",
""
],
[
"Tripathi",
"A.",
""
],
[
"Malik",
"R. P.",
""
]
] | We exploit the theoretical strength of the supervariable and Becchi-Rouet-Stora-Tyutin (BRST) formalisms to derive the proper (i.e. off-shell nilpotent and absolutely anticommuting) (anti-)BRST symmetry transformations for the reparameterization invariant model of a non-relativistic (NR) free particle whose space $(x)$... | 5.358125 | 4.263794 | 6.691855 | 4.486187 | 4.87499 | 4.34877 | 4.511581 | 4.380122 | 4.379425 | 6.969772 | 4.387888 | 4.819547 | 5.503727 | 5.021152 | 5.146717 | 5.01534 | 5.205204 | 4.881303 | 5.122869 | 5.586287 | 4.904511 |
hep-th/9812244 | Olaf Lechtenfeld | Olaf Lechtenfeld and Boris Zupnik | Manifestly invariant actions for harmonic self-dual gauge theory | 16 pages, no figures | null | null | ITP-UH-36/98, JINR E2-98-382 | hep-th | null | We discuss alternative descriptions of four-dimensional self-dual Yang-Mills
fields in harmonic space with additional commuting spinor coordinates. In
particular, the linear analyticity equation and nonlinear covariant
harmonic-field equations are studied. A covariant harmonic field can be treated
as an infinite set ... | [
{
"created": "Wed, 30 Dec 1998 17:41:25 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Lechtenfeld",
"Olaf",
""
],
[
"Zupnik",
"Boris",
""
]
] | We discuss alternative descriptions of four-dimensional self-dual Yang-Mills fields in harmonic space with additional commuting spinor coordinates. In particular, the linear analyticity equation and nonlinear covariant harmonic-field equations are studied. A covariant harmonic field can be treated as an infinite set of... | 18.005564 | 15.58761 | 18.721586 | 17.124649 | 16.712265 | 16.719194 | 16.625198 | 15.475366 | 16.840549 | 22.644936 | 15.85045 | 16.638296 | 18.379635 | 16.231222 | 17.288673 | 16.868212 | 15.85146 | 17.317726 | 16.487698 | 18.042213 | 16.753683 |
2305.10712 | Brett McInnes | Brett McInnes | Slow Complexification | 23 pages, 4 figures, references added, some discussions simplified,
added a discussion of the possible relation of complexity with quantum
teleportation. Version to appear in Nuclear Physics B | Nuclear Physics B, Volume 998, January 2024, 116401 | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The fact that AdS black hole interior geometries are time-dependent presents
two challenges: first, to holographic duality (the boundary matter tends to
equilibrate, often very quickly), and, second, to the idea that wormholes can
be traversable (the wormhole geometry is dynamic, and the wormhole is apt to
collapse t... | [
{
"created": "Thu, 18 May 2023 05:17:30 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Jul 2023 04:26:13 GMT",
"version": "v2"
},
{
"created": "Wed, 22 Nov 2023 05:04:37 GMT",
"version": "v3"
}
] | 2023-11-23 | [
[
"McInnes",
"Brett",
""
]
] | The fact that AdS black hole interior geometries are time-dependent presents two challenges: first, to holographic duality (the boundary matter tends to equilibrate, often very quickly), and, second, to the idea that wormholes can be traversable (the wormhole geometry is dynamic, and the wormhole is apt to collapse too... | 11.461322 | 12.478386 | 11.764573 | 11.328943 | 12.916075 | 12.210247 | 12.131684 | 11.544083 | 11.532287 | 13.78724 | 11.454787 | 12.015956 | 11.72996 | 11.421716 | 11.777606 | 11.478503 | 11.728607 | 11.334341 | 11.82616 | 11.684143 | 11.285257 |
hep-th/9409123 | null | M. Sakamoto and M. Tachibana | Topological Terms in String Theory on Orbifolds | 15pages,LaTex,KOBE-TH-94-05 | Prog.Theor.Phys. 93 (1995) 471-482 | 10.1143/PTP.93.471 | null | hep-th | null | We study toroidal orbifold models with topologically invariant terms in the
path integral formalism and give physical interpretations of the terms from an
operator formalism point of view. We briefly discuss a possibility of a new
class of modular invariant orbifold models.
| [
{
"created": "Wed, 21 Sep 1994 09:39:25 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Sakamoto",
"M.",
""
],
[
"Tachibana",
"M.",
""
]
] | We study toroidal orbifold models with topologically invariant terms in the path integral formalism and give physical interpretations of the terms from an operator formalism point of view. We briefly discuss a possibility of a new class of modular invariant orbifold models. | 18.569696 | 14.294897 | 20.754795 | 13.72309 | 12.637617 | 15.104555 | 15.217999 | 15.412689 | 14.850554 | 19.674519 | 14.008359 | 14.791091 | 18.387318 | 15.171596 | 13.883493 | 14.703669 | 14.190756 | 14.638701 | 14.701425 | 18.583935 | 15.209666 |
1309.4362 | Marc Henneaux | Marc Henneaux, Alfredo Perez, David Tempo, Ricardo Troncoso | Chemical potentials in three-dimensional higher spin anti-de Sitter
gravity | Minor misprints corrected | null | 10.1007/JHEP12(2013)048 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We indicate how to introduce chemical potentials for higher spin charges in
higher spin anti-de Sitter gravity in a manner that manifestly preserves the
original asymptotic W-symmetry. This is done by switching on a non-vanishing
component of the connection along the temporal (thermal) circles. We first
recall the pr... | [
{
"created": "Tue, 17 Sep 2013 15:59:43 GMT",
"version": "v1"
},
{
"created": "Sat, 21 Sep 2013 21:30:54 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Feb 2014 07:14:52 GMT",
"version": "v3"
}
] | 2015-06-17 | [
[
"Henneaux",
"Marc",
""
],
[
"Perez",
"Alfredo",
""
],
[
"Tempo",
"David",
""
],
[
"Troncoso",
"Ricardo",
""
]
] | We indicate how to introduce chemical potentials for higher spin charges in higher spin anti-de Sitter gravity in a manner that manifestly preserves the original asymptotic W-symmetry. This is done by switching on a non-vanishing component of the connection along the temporal (thermal) circles. We first recall the proc... | 10.072104 | 8.266587 | 10.406551 | 8.898897 | 8.988691 | 9.72396 | 8.975248 | 9.010197 | 8.731594 | 11.571195 | 9.185472 | 8.835144 | 10.0164 | 8.722739 | 8.919927 | 8.725016 | 8.761546 | 8.910664 | 8.832659 | 10.288521 | 8.743191 |
0907.2296 | Marc Bellon | Marc Bellon (LPTHE) | Approximate Differential Equations for Renormalization Group Functions
in Models Free of Vertex Divergencies | Clarification of the presentation of results. Equations and results
unchanged. Match the published version. 12 pages | Nucl.Phys.B826:522-531,2010 | 10.1016/j.nuclphysb.2009.11.002 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I introduce an approximation scheme that allows to deduce differential
equations for the renormalization group $\beta$-function from a
Schwinger--Dyson equation for the propagator. This approximation is proven to
give the dominant asymptotic behavior of the perturbative solution. In the
supersymmetric Wess--Zumino mo... | [
{
"created": "Tue, 14 Jul 2009 07:12:03 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Oct 2009 08:41:02 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Nov 2009 12:24:14 GMT",
"version": "v3"
}
] | 2009-11-23 | [
[
"Bellon",
"Marc",
"",
"LPTHE"
]
] | I introduce an approximation scheme that allows to deduce differential equations for the renormalization group $\beta$-function from a Schwinger--Dyson equation for the propagator. This approximation is proven to give the dominant asymptotic behavior of the perturbative solution. In the supersymmetric Wess--Zumino mode... | 8.825159 | 7.960499 | 8.026579 | 8.346557 | 8.157094 | 8.055763 | 8.546702 | 8.224945 | 8.00071 | 9.123676 | 8.103813 | 7.90972 | 8.314865 | 7.774045 | 7.880452 | 7.904164 | 7.892148 | 7.816221 | 7.895882 | 8.364906 | 7.905131 |
hep-th/0302067 | Sean Carroll | Sean M. Carroll and Monica M. Guica | Sidestepping the Cosmological Constant with Football-Shaped Extra
Dimensions | null | null | null | EFI-2003-05 | hep-th astro-ph gr-qc hep-ph | null | We present an exact solution for a factorizable brane-world spacetime with
two extra dimensions and explicit brane sources. The compactification manifold
has the topology of a two-sphere, and is stabilized by a bulk cosmological
constant and magnetic flux. The geometry of the sphere is locally round except
for conica... | [
{
"created": "Tue, 11 Feb 2003 02:29:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Carroll",
"Sean M.",
""
],
[
"Guica",
"Monica M.",
""
]
] | We present an exact solution for a factorizable brane-world spacetime with two extra dimensions and explicit brane sources. The compactification manifold has the topology of a two-sphere, and is stabilized by a bulk cosmological constant and magnetic flux. The geometry of the sphere is locally round except for conical ... | 8.174581 | 8.126973 | 8.974195 | 8.09514 | 7.711276 | 7.381052 | 8.016556 | 7.527416 | 7.762285 | 9.345523 | 8.13978 | 7.820731 | 8.143513 | 7.855206 | 7.83438 | 7.906765 | 7.955654 | 7.950803 | 7.914323 | 7.992298 | 7.852497 |
hep-th/0205048 | Horatiu Stefan Nastase | David Berenstein and Horatiu Nastase | On lightcone string field theory from Super Yang-Mills and holography | 40 pages, 17 figures, latex; v2: typos corrected, references added,
Comments on extra diagrams added (page 30) | null | null | null | hep-th | null | We investigate the issues of holography and string interactions in the
duality between SYM and the pp wave background. We argue that the Penrose
diagram of the maximally supersymmetric pp-wave has a one dimensional boundary.
This fact suggests that the holographic dual of the pp-wave can be described by
a quantum mec... | [
{
"created": "Tue, 7 May 2002 17:02:09 GMT",
"version": "v1"
},
{
"created": "Wed, 15 May 2002 17:39:19 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Berenstein",
"David",
""
],
[
"Nastase",
"Horatiu",
""
]
] | We investigate the issues of holography and string interactions in the duality between SYM and the pp wave background. We argue that the Penrose diagram of the maximally supersymmetric pp-wave has a one dimensional boundary. This fact suggests that the holographic dual of the pp-wave can be described by a quantum mecha... | 9.046751 | 9.408992 | 10.30615 | 9.073543 | 9.878926 | 9.560254 | 9.912422 | 9.038526 | 9.247045 | 11.127808 | 9.141446 | 9.124114 | 9.795208 | 9.19943 | 9.399106 | 9.704056 | 9.265384 | 9.159624 | 9.082267 | 9.620885 | 8.835453 |
hep-th/0508116 | Michael Creutz | Michael Creutz | Hidden symmetries in two dimensional field theory | 15 pages. Revision adds numerous references and puts things in better
historical context | Annals Phys. 321 (2006) 2782-2792 | 10.1016/j.aop.2006.01.003 | null | hep-th hep-lat | null | The bosonization process elegantly shows the equivalence of massless scalar
and fermion fields in two space-time dimensions. However, with multiple
fermions the technique often obscures global symmetries. Witten's non-Abelian
bosonization makes these symmetries explicit, but at the expense of a somewhat
complicated b... | [
{
"created": "Tue, 16 Aug 2005 13:30:25 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Jan 2006 16:05:02 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Creutz",
"Michael",
""
]
] | The bosonization process elegantly shows the equivalence of massless scalar and fermion fields in two space-time dimensions. However, with multiple fermions the technique often obscures global symmetries. Witten's non-Abelian bosonization makes these symmetries explicit, but at the expense of a somewhat complicated bos... | 10.465555 | 9.911895 | 11.238954 | 10.289408 | 9.917795 | 11.010591 | 9.907417 | 10.01136 | 9.939315 | 10.902328 | 10.17675 | 9.995264 | 10.629779 | 10.249147 | 10.131779 | 10.015724 | 10.082264 | 9.961543 | 9.921118 | 10.304364 | 10.117435 |
hep-th/0406165 | Kazuyuki Furuuchi | Kazuyuki Furuuchi | Holomorphically Covariant Matrix Models | 12 pages | null | null | IHES/P/04/30 | hep-th | null | We present a method to construct matrix models on arbitrary simply connected
oriented real two dimensional Riemannian manifolds. The actions and the path
integral measure are invariant under holomorphic transformations of matrix
coordinates.
| [
{
"created": "Mon, 21 Jun 2004 09:21:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Furuuchi",
"Kazuyuki",
""
]
] | We present a method to construct matrix models on arbitrary simply connected oriented real two dimensional Riemannian manifolds. The actions and the path integral measure are invariant under holomorphic transformations of matrix coordinates. | 13.938601 | 12.472018 | 13.350113 | 11.242472 | 12.083946 | 12.15726 | 11.161677 | 11.086262 | 11.458136 | 16.014767 | 11.455645 | 11.242057 | 13.362564 | 11.085222 | 11.582964 | 11.033508 | 11.254197 | 11.154716 | 11.635873 | 13.518437 | 11.593529 |
2003.07958 | Nick Early | Freddy Cachazo, Nick Early | Minimal Kinematics: An All $k$ and $n$ Peek into ${\rm Trop}^+{\rm
G}(k,n)$ | null | SIGMA 17 (2021), 078, 22 pages | 10.3842/SIGMA.2021.078 | null | hep-th math.CO | http://creativecommons.org/licenses/by-sa/4.0/ | In this note we present a formula for the Cachazo-Early-Guevara-Mizera (CEGM)
generalized biadjoint amplitudes for all $k$ and $n$ on what we call the
minimal kinematics. We prove that on the minimal kinematics, the scattering
equations on the configuration space of $n$ points on $\mathbb{CP}^{k-1}$ has a
unique solu... | [
{
"created": "Tue, 17 Mar 2020 21:43:46 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Dec 2020 19:20:09 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Aug 2021 05:25:18 GMT",
"version": "v3"
}
] | 2021-08-26 | [
[
"Cachazo",
"Freddy",
""
],
[
"Early",
"Nick",
""
]
] | In this note we present a formula for the Cachazo-Early-Guevara-Mizera (CEGM) generalized biadjoint amplitudes for all $k$ and $n$ on what we call the minimal kinematics. We prove that on the minimal kinematics, the scattering equations on the configuration space of $n$ points on $\mathbb{CP}^{k-1}$ has a unique soluti... | 6.515419 | 6.140184 | 7.541489 | 6.275951 | 6.192771 | 6.230373 | 6.4496 | 5.906597 | 6.039162 | 8.047048 | 6.0691 | 6.34859 | 6.769109 | 6.391922 | 6.429112 | 6.502051 | 6.291678 | 6.524928 | 6.326237 | 6.707701 | 6.298982 |
1610.00326 | Chen Zhang | Chen Zhang | Instability of Chern-Simons Theory with Fermions at Large N | null | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the (in)stability around the dynamical gap solution of the $U(N)$
Chern-Simons gauge theory with fundamental fermions (massless or massive)
coupled in $D=3$ at large $N$. Explicit analyses on both the Auxiliary-Field
(AF) and the Cornwall-Jackiw-Tomboulis (CJT) effective potentials are given. In
both approac... | [
{
"created": "Sun, 2 Oct 2016 18:05:59 GMT",
"version": "v1"
}
] | 2016-10-04 | [
[
"Zhang",
"Chen",
""
]
] | We study the (in)stability around the dynamical gap solution of the $U(N)$ Chern-Simons gauge theory with fundamental fermions (massless or massive) coupled in $D=3$ at large $N$. Explicit analyses on both the Auxiliary-Field (AF) and the Cornwall-Jackiw-Tomboulis (CJT) effective potentials are given. In both approache... | 12.561291 | 12.055368 | 11.658323 | 10.57093 | 12.083364 | 10.591929 | 10.894613 | 11.02334 | 10.755849 | 13.263299 | 10.512613 | 10.934297 | 11.670579 | 10.800112 | 10.766843 | 10.627088 | 10.847056 | 11.439296 | 10.59061 | 11.313317 | 10.693556 |
hep-th/0406041 | Marek Rogatko | Marek Rogatko | Uniqueness Theorem for Generalized Maxwell Electric and Magnetic Black
Holes in Higher Dimensions | 7 pages, RevTex, to be published in Phys.Rev.D15 | Phys.Rev. D70 (2004) 044023 | 10.1103/PhysRevD.70.044023 | null | hep-th gr-qc | null | Based on the conformal energy theorem we prove the uniqueness theorem for
static higher dimensional electrically and magnetically charged black holes
being the solution of Einstein (n-2)-gauge forms equations of motion. Black
hole spacetime contains an asymptotically flat spacelike hypersurface with
compact interior ... | [
{
"created": "Fri, 4 Jun 2004 07:17:57 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Rogatko",
"Marek",
""
]
] | Based on the conformal energy theorem we prove the uniqueness theorem for static higher dimensional electrically and magnetically charged black holes being the solution of Einstein (n-2)-gauge forms equations of motion. Black hole spacetime contains an asymptotically flat spacelike hypersurface with compact interior an... | 15.706057 | 7.192713 | 13.351148 | 9.764502 | 9.10039 | 8.57285 | 8.605331 | 8.427722 | 9.841515 | 16.078375 | 9.871096 | 12.002097 | 13.249431 | 12.763426 | 11.358544 | 11.656109 | 11.837122 | 11.847445 | 12.713896 | 14.953506 | 13.305325 |
1910.02404 | Anurag Kaushal | Parijat Banerjee, Adwait Gaikwad, Anurag Kaushal and Gautam Mandal | Quantum quench and thermalization to GGE in arbitrary dimensions and the
odd-even effect | 27+12 pages, 6 figures | null | 10.1007/JHEP09(2020)027 | TIFR/TH/19-34 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In many quantum quench experiments involving cold atom systems the
post-quench system can be described by a quantum field theory of free scalars
or fermions, typically in a box or in an external potential. We work with free
scalars in arbitrary dimensions generalizing the techniques employed in our
earlier work \cite... | [
{
"created": "Sun, 6 Oct 2019 09:39:35 GMT",
"version": "v1"
}
] | 2023-08-29 | [
[
"Banerjee",
"Parijat",
""
],
[
"Gaikwad",
"Adwait",
""
],
[
"Kaushal",
"Anurag",
""
],
[
"Mandal",
"Gautam",
""
]
] | In many quantum quench experiments involving cold atom systems the post-quench system can be described by a quantum field theory of free scalars or fermions, typically in a box or in an external potential. We work with free scalars in arbitrary dimensions generalizing the techniques employed in our earlier work \cite{M... | 8.351154 | 8.696451 | 9.220846 | 8.448389 | 9.241499 | 8.848345 | 9.489279 | 8.935624 | 8.539104 | 9.957355 | 8.404141 | 8.371975 | 8.438515 | 8.30152 | 8.473938 | 8.296449 | 8.334926 | 8.140973 | 8.27313 | 8.560427 | 8.332802 |
1012.5044 | Kirsten Schn\"ulle | Burkhard Kleihaus, Jutta Kunz and Kirsten Schn\"ulle | Charged Balanced Black Rings in Five Dimensions | 7 pages, 7 figures | null | 10.1016/j.physletb.2011.03.072 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present balanced black ring solutions of pure Einstein-Maxwell theory in
five dimensions. The solutions are asymptotically flat, and their tension and
gravitational self-attraction are balanced by the repulsion due to rotation and
electrical charge. Hence the solutions are free of conical singularities and
possess... | [
{
"created": "Wed, 22 Dec 2010 17:22:20 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Kleihaus",
"Burkhard",
""
],
[
"Kunz",
"Jutta",
""
],
[
"Schnülle",
"Kirsten",
""
]
] | We present balanced black ring solutions of pure Einstein-Maxwell theory in five dimensions. The solutions are asymptotically flat, and their tension and gravitational self-attraction are balanced by the repulsion due to rotation and electrical charge. Hence the solutions are free of conical singularities and possess a... | 9.278061 | 8.746707 | 7.618005 | 6.966738 | 7.794376 | 7.980276 | 7.503549 | 7.40361 | 8.132959 | 8.086735 | 8.213775 | 7.761792 | 7.873989 | 7.793675 | 7.995052 | 8.088573 | 7.913193 | 7.973473 | 7.965506 | 7.948026 | 7.821087 |
1403.1449 | Per Sundin | Per Sundin | Worldsheet two- and four-point functions at one loop in AdS(3) / CFT(2) | 11 pages, FeynMP. Version 2; footnote added and typos fixed,
published version | null | 10.1016/j.physletb.2014.04.022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we study worldsheet two- and four-point functions at the
one-loop level for the type IIA superstring in AdS(3) x S(3) x M(4) . We first
address the regularization ambiguity that appears in the dispersion relation
derived from integrability. We demonstrate that only the regulator treating all
fields equal... | [
{
"created": "Thu, 6 Mar 2014 14:21:49 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Apr 2014 10:00:27 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Sundin",
"Per",
""
]
] | In this note we study worldsheet two- and four-point functions at the one-loop level for the type IIA superstring in AdS(3) x S(3) x M(4) . We first address the regularization ambiguity that appears in the dispersion relation derived from integrability. We demonstrate that only the regulator treating all fields equally... | 13.129834 | 12.666787 | 16.333422 | 12.058468 | 12.248345 | 12.466468 | 11.712207 | 12.271029 | 12.067208 | 17.644876 | 12.258293 | 12.241882 | 14.176333 | 12.283366 | 12.953056 | 12.249084 | 12.58888 | 12.171032 | 12.681104 | 14.172956 | 12.321564 |
1305.3547 | Richard Eager | Richard Eager and Johannes Schmude | Superconformal Indices and M2-Branes | 40 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the superconformal index of the world-volume theory on M2-branes
probing the cone over an arbitrary Sasaki-Einstein seven-manifold. The index is
expressed in terms of the cohomology groups of the cone. We match our
supergravity results with known results from gauge theory. Along the way we
derive the spectr... | [
{
"created": "Wed, 15 May 2013 17:09:19 GMT",
"version": "v1"
}
] | 2013-05-16 | [
[
"Eager",
"Richard",
""
],
[
"Schmude",
"Johannes",
""
]
] | We derive the superconformal index of the world-volume theory on M2-branes probing the cone over an arbitrary Sasaki-Einstein seven-manifold. The index is expressed in terms of the cohomology groups of the cone. We match our supergravity results with known results from gauge theory. Along the way we derive the spectrum... | 5.319972 | 4.699772 | 6.700354 | 4.746254 | 4.688512 | 4.682536 | 4.375192 | 4.690662 | 4.445793 | 7.2106 | 4.628204 | 4.69216 | 5.479903 | 4.718351 | 4.763855 | 4.761607 | 4.737988 | 4.687726 | 4.731648 | 5.574582 | 4.591749 |
1910.07727 | Sridip Pal | Sridip Pal, Zhengdi Sun | Tauberian-Cardy formula with spin | Multiple figures and inequalities! v2: ref updated, Eq 1.30 modified | JHEP 01 (2020) 135 | 10.1007/JHEP01(2020)135 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove a $2$ dimensional Tauberian theorem in context of $2$ dimensional
conformal field theory. The asymptotic density of states with conformal weight
$(h,\bar{h})\to (\infty,\infty)$ for any arbitrary spin is derived using the
theorem. We further rigorously show that the error term is controlled by the
twist para... | [
{
"created": "Thu, 17 Oct 2019 06:15:46 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Jan 2020 14:49:08 GMT",
"version": "v2"
}
] | 2020-05-21 | [
[
"Pal",
"Sridip",
""
],
[
"Sun",
"Zhengdi",
""
]
] | We prove a $2$ dimensional Tauberian theorem in context of $2$ dimensional conformal field theory. The asymptotic density of states with conformal weight $(h,\bar{h})\to (\infty,\infty)$ for any arbitrary spin is derived using the theorem. We further rigorously show that the error term is controlled by the twist parame... | 12.450435 | 13.08782 | 13.727031 | 11.448478 | 12.861806 | 13.016518 | 13.581232 | 12.806612 | 11.638428 | 14.74735 | 11.842071 | 11.781698 | 11.925253 | 11.692119 | 11.32066 | 11.941037 | 11.757099 | 11.846696 | 11.65493 | 12.32722 | 11.538667 |
hep-th/0009092 | Peter Horvathy | M. Hassa\"ine and P. A. Horv\'athy | Symmetries of fluid dynamics with polytropic exponent | 10 pages, LaTex, no figures. Revised version: A new proof of the
Schrodinger symmetry and two more references added. To appear in Phys. Lett.
A | Phys.Lett. A279 (2001) 215-222 | 10.1016/S0375-9601(00)00834-3 | null | hep-th | null | The symmetries of the general Euler equations of fluid dynamics with
polytropic exponent are determined using the Kaluza-Klein type framework of
Duval et $\it{al}$. In the standard polytropic case the recent results of
O'Raifeartaigh and Sreedhar are confirmed and generalized. Similar results are
proved for polytropi... | [
{
"created": "Tue, 12 Sep 2000 12:48:24 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Sep 2000 09:58:13 GMT",
"version": "v2"
},
{
"created": "Fri, 29 Sep 2000 10:24:26 GMT",
"version": "v3"
},
{
"created": "Tue, 28 Nov 2000 13:04:25 GMT",
"version": "v4"
},
{
"c... | 2016-08-15 | [
[
"Hassaïne",
"M.",
""
],
[
"Horváthy",
"P. A.",
""
]
] | The symmetries of the general Euler equations of fluid dynamics with polytropic exponent are determined using the Kaluza-Klein type framework of Duval et $\it{al}$. In the standard polytropic case the recent results of O'Raifeartaigh and Sreedhar are confirmed and generalized. Similar results are proved for polytropic ... | 16.005241 | 15.33042 | 19.637821 | 15.196679 | 17.571611 | 17.66218 | 16.194632 | 15.251707 | 14.745729 | 18.486259 | 14.624064 | 13.64789 | 14.949942 | 14.589602 | 15.07538 | 14.153952 | 14.152521 | 14.640636 | 14.011548 | 14.799335 | 13.456862 |
0707.3055 | Tim Jones | Ian Jack, D.R. Timothy Jones, Philipp Kant, Luminita Mihaila | The four-loop DRED gauge beta-function and fermion mass anomalous
dimension for general gauge groups | 44 pages, added references (v2) minor changes (v3) | JHEP 0709:058,2007 | 10.1088/1126-6708/2007/09/058 | LTH751, TTP/07-17, SFB/CPP-07-40, NSF-KITP-07-153 | hep-th | null | We present four-loop results for the gauge beta-function and the fermion mass
anomalous dimension for a gauge theory with a general gauge group and a
multiplet of fermions transforming according to an arbitrary representation,
calculated using the dimensional reduction scheme. In the special case of a
supersymmetric ... | [
{
"created": "Fri, 20 Jul 2007 12:04:38 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Jul 2007 15:54:54 GMT",
"version": "v2"
},
{
"created": "Thu, 23 Aug 2007 15:35:16 GMT",
"version": "v3"
}
] | 2009-11-18 | [
[
"Jack",
"Ian",
""
],
[
"Jones",
"D. R. Timothy",
""
],
[
"Kant",
"Philipp",
""
],
[
"Mihaila",
"Luminita",
""
]
] | We present four-loop results for the gauge beta-function and the fermion mass anomalous dimension for a gauge theory with a general gauge group and a multiplet of fermions transforming according to an arbitrary representation, calculated using the dimensional reduction scheme. In the special case of a supersymmetric th... | 6.166803 | 6.905278 | 5.793979 | 5.789752 | 5.969846 | 7.089175 | 5.830081 | 6.796272 | 5.31215 | 5.632644 | 6.186411 | 6.144775 | 5.953329 | 5.467514 | 5.709862 | 6.243871 | 5.587652 | 6.531906 | 5.679765 | 5.603624 | 6.052676 |
2201.10163 | Michael Ponds | Michael Ponds | Models for (super)conformal higher-spin fields on curved backgrounds | PhD thesis, 302 pages. Based on arXiv:1806.06643, arXiv:1812.05331,
arXiv:1902.08010, arXiv:1910.10440, arXiv:1912.00652, arXiv:2005.08657,
arXiv:2011.11300, 2101.05524, arXiv:2103.11673 and arXiv:2107.12201 | null | null | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by-sa/4.0/ | This thesis is devoted to the construction of theories describing the
consistent propagation of (super)conformal higher-spin fields on curved three-
and four-dimensional (super)spaces. In the first half of this thesis we
systematically derive models for conformal fields of arbitrary rank on various
types of curved sp... | [
{
"created": "Tue, 25 Jan 2022 08:08:02 GMT",
"version": "v1"
}
] | 2022-01-26 | [
[
"Ponds",
"Michael",
""
]
] | This thesis is devoted to the construction of theories describing the consistent propagation of (super)conformal higher-spin fields on curved three- and four-dimensional (super)spaces. In the first half of this thesis we systematically derive models for conformal fields of arbitrary rank on various types of curved spac... | 7.275115 | 7.067729 | 7.677009 | 7.085255 | 7.214877 | 6.954368 | 7.685448 | 7.089182 | 7.087976 | 8.09281 | 7.048253 | 7.0231 | 7.20457 | 7.074568 | 6.958207 | 6.905993 | 7.098708 | 7.031112 | 6.912169 | 7.321422 | 6.846496 |
0806.4348 | Nele Vandersickel | David Dudal, John Gracey, Silvio Paolo Sorella, Nele Vandersickel,
Henri Verschelde | A refinement of the Gribov-Zwanziger approach in the Landau gauge:
infrared propagators in harmony with the lattice results | 38 pages, 9 figures, the content of section V has been extended and
adapted | Phys.Rev.D78:065047,2008 | 10.1103/PhysRevD.78.065047 | LTH-789 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent lattice data have reported an infrared suppressed, positivity
violating gluon propagator which is nonvanishing at zero momentum and a ghost
propagator which is no longer enhanced. This paper discusses how to obtain
analytical results which are in qualitative agreement with these lattice data
within the Gribov-... | [
{
"created": "Thu, 26 Jun 2008 15:43:19 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Aug 2008 14:13:25 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Dudal",
"David",
""
],
[
"Gracey",
"John",
""
],
[
"Sorella",
"Silvio Paolo",
""
],
[
"Vandersickel",
"Nele",
""
],
[
"Verschelde",
"Henri",
""
]
] | Recent lattice data have reported an infrared suppressed, positivity violating gluon propagator which is nonvanishing at zero momentum and a ghost propagator which is no longer enhanced. This paper discusses how to obtain analytical results which are in qualitative agreement with these lattice data within the Gribov-Zw... | 8.786834 | 7.634778 | 10.123076 | 7.991759 | 8.256728 | 7.833411 | 7.71082 | 7.940117 | 7.62391 | 8.5548 | 8.001619 | 8.04938 | 8.422126 | 8.02269 | 8.040922 | 7.759392 | 7.798662 | 8.143288 | 7.80615 | 8.255874 | 8.562186 |
2104.04788 | Zbigniew Haba | Z. Haba | The impact of a random metric upon a diffusing particle | 8 pages | null | null | null | hep-th gr-qc math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | We show that if the singularity of the quantized gravity propagator is $\vert
{\bf x}\vert^{-2\gamma}$ then the mean value of the fourth power of the
distance achieved in time $t$ by a diffusing particle behaves as
$t^{2(1-\gamma)}$ for a small $t$.
| [
{
"created": "Sat, 10 Apr 2021 15:10:41 GMT",
"version": "v1"
},
{
"created": "Fri, 21 May 2021 15:03:14 GMT",
"version": "v2"
}
] | 2021-05-24 | [
[
"Haba",
"Z.",
""
]
] | We show that if the singularity of the quantized gravity propagator is $\vert {\bf x}\vert^{-2\gamma}$ then the mean value of the fourth power of the distance achieved in time $t$ by a diffusing particle behaves as $t^{2(1-\gamma)}$ for a small $t$. | 11.661777 | 13.633928 | 10.788653 | 8.972724 | 10.97548 | 8.248311 | 9.166893 | 9.37641 | 10.445332 | 12.038703 | 9.507765 | 10.073979 | 10.182932 | 9.982739 | 9.269632 | 9.278574 | 9.123588 | 9.473487 | 10.530861 | 10.744617 | 9.364213 |
2304.04684 | Juntao Wang | Wei Cui, Hongfei Shu, Wei Song, Juntao Wang | Correlation Functions in the TsT/$T{\bar T}$ Correspondence | 35 pages; references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the proposed holographic duality between the TsT
transformation of IIB string theory on AdS$_3\times {\cal N}$ with NS-NS flux
and a single-trace $T\bar{T}$ deformation of the symmetric orbifold CFT. We
present a non-perturbative calculation of two-point correlation functions using
string theory and de... | [
{
"created": "Mon, 10 Apr 2023 16:00:59 GMT",
"version": "v1"
},
{
"created": "Wed, 10 May 2023 14:27:27 GMT",
"version": "v2"
}
] | 2023-05-11 | [
[
"Cui",
"Wei",
""
],
[
"Shu",
"Hongfei",
""
],
[
"Song",
"Wei",
""
],
[
"Wang",
"Juntao",
""
]
] | We investigate the proposed holographic duality between the TsT transformation of IIB string theory on AdS$_3\times {\cal N}$ with NS-NS flux and a single-trace $T\bar{T}$ deformation of the symmetric orbifold CFT. We present a non-perturbative calculation of two-point correlation functions using string theory and demo... | 5.539929 | 5.256818 | 6.678809 | 5.323032 | 5.690426 | 5.34779 | 5.345428 | 5.161942 | 5.380177 | 7.182345 | 5.488692 | 5.195405 | 5.776827 | 5.287866 | 5.296925 | 5.333439 | 5.278203 | 5.227416 | 5.545126 | 5.627295 | 5.521448 |
hep-th/9201075 | Saburo Higuchi o-2082 | K.Amano and S.Higuchi | Topology change in ISO(2,1) Chern-Simons gravity | 24 pages and 4 figures (not included) | Nucl.Phys. B377 (1992) 218-235 | 10.1016/0550-3213(92)90022-4 | null | hep-th | null | In 2+1 dimensional gravity, a dreibein and the compatible spin connection can
represent a space-time containing a closed spacelike surface $\Sigma$ only if
the associated SO(2,1) bundle restricted to $\Sigma$ has the same
non-triviality (Euler class) as that of the tangent bundle of $\Sigma.$ We
impose this bundle co... | [
{
"created": "Thu, 30 Jan 1992 09:52:29 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Amano",
"K.",
""
],
[
"Higuchi",
"S.",
""
]
] | In 2+1 dimensional gravity, a dreibein and the compatible spin connection can represent a space-time containing a closed spacelike surface $\Sigma$ only if the associated SO(2,1) bundle restricted to $\Sigma$ has the same non-triviality (Euler class) as that of the tangent bundle of $\Sigma.$ We impose this bundle cond... | 12.818807 | 13.893715 | 12.322754 | 11.915008 | 12.35494 | 13.631849 | 14.031751 | 11.920966 | 12.284078 | 14.388981 | 13.172803 | 12.201569 | 12.233403 | 11.908973 | 11.888067 | 12.3404 | 12.26848 | 12.043283 | 11.827522 | 11.720604 | 11.884678 |
hep-th/9402044 | Nathan Seiberg | Nathan Seiberg | Exact Results on the Space of Vacua of Four Dimensional SUSY Gauge
Theories | 19 pages, RU-94-18 | Phys.Rev.D49:6857-6863,1994 | 10.1103/PhysRevD.49.6857 | null | hep-th hep-ph | null | We consider four dimensional quantum field theories which have a continuous
manifold of inequivalent exact ground states -- a moduli space of vacua.
Classically, the singular points on the moduli space are associated with extra
massless particles. Quantum mechanically these singularities can be smoothed
out. Alternat... | [
{
"created": "Tue, 8 Feb 1994 19:34:40 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Seiberg",
"Nathan",
""
]
] | We consider four dimensional quantum field theories which have a continuous manifold of inequivalent exact ground states -- a moduli space of vacua. Classically, the singular points on the moduli space are associated with extra massless particles. Quantum mechanically these singularities can be smoothed out. Alternativ... | 10.103611 | 9.485542 | 11.766267 | 8.92383 | 10.025089 | 9.594003 | 9.955029 | 8.485771 | 8.497429 | 12.865414 | 9.263446 | 8.93374 | 10.862449 | 9.089879 | 9.065224 | 8.820543 | 8.72344 | 9.018651 | 9.13342 | 10.267489 | 8.742008 |
2308.04092 | Davoud Kamani | Niloufar Barghi-Janyar and Davoud Kamani | Pair Production of the Open Superstrings from the Parallel-dressed
D3-branes in the Compact Spacetime | 14 pages, LaTeX2e, no figure | Eur. Phys. J. C (2023) 83:716 | 10.1140/epjc/s10052-023-11890-4 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We employ the boundary state formalism to compute the pair creation rate of
the open superstrings from the interaction of two parallel D3-branes. The
branes live in the partially compact spacetime. In addition, they have been
dressed with the internal gauge potentials and the Kalb-Ramond field.
| [
{
"created": "Tue, 8 Aug 2023 07:16:19 GMT",
"version": "v1"
}
] | 2023-08-14 | [
[
"Barghi-Janyar",
"Niloufar",
""
],
[
"Kamani",
"Davoud",
""
]
] | We employ the boundary state formalism to compute the pair creation rate of the open superstrings from the interaction of two parallel D3-branes. The branes live in the partially compact spacetime. In addition, they have been dressed with the internal gauge potentials and the Kalb-Ramond field. | 17.02223 | 8.729158 | 14.078949 | 9.685306 | 10.973973 | 10.219932 | 9.507337 | 9.576249 | 10.103674 | 16.050522 | 9.867124 | 11.925144 | 13.82146 | 12.824022 | 12.503339 | 12.524969 | 11.844861 | 12.462551 | 12.545772 | 14.128457 | 12.605474 |
hep-th/0409241 | Axel Krause | Axel Krause and Siew-Phang Ng | Ghost Cosmology: Exact Solutions, Transitions Between Standard
Cosmologies and Ghost Dark Energy/Matter Evolution | 31 pages, 9 figures; added references, clarified a few minor points | Int.J.Mod.Phys.A21:1091-1122,2006 | 10.1142/S0217751X0602516X | UMD-PP-05-019, BA-04-10 | hep-th astro-ph gr-qc hep-ph | null | The recently proposed infrared modification of gravity through the
introduction of a ghost scalar field results in a number of interesting
cosmological and phenomenological implications. In this paper, we derive the
exact cosmological solutions for a number of scenarios where at late stages,
the ghost behaves like da... | [
{
"created": "Fri, 24 Sep 2004 19:57:39 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Sep 2004 01:19:26 GMT",
"version": "v2"
}
] | 2011-05-12 | [
[
"Krause",
"Axel",
""
],
[
"Ng",
"Siew-Phang",
""
]
] | The recently proposed infrared modification of gravity through the introduction of a ghost scalar field results in a number of interesting cosmological and phenomenological implications. In this paper, we derive the exact cosmological solutions for a number of scenarios where at late stages, the ghost behaves like dark... | 10.727918 | 12.0535 | 10.649116 | 10.210939 | 12.032199 | 11.532472 | 11.162639 | 11.009451 | 10.545267 | 11.084774 | 10.696312 | 10.344295 | 10.526174 | 10.247527 | 10.584402 | 10.381263 | 10.417102 | 10.686748 | 10.316601 | 10.422018 | 10.641281 |
hep-th/9603029 | Me | Adriano Di Giacomo | Mechanisms of colour confinement | 30 pages. Lectures delivered at the CXXX Course of the International
School of Physics E. Fermi on ''SELECTED TOPICS IN NONPERTURBATIVE QCD''.
Varenna 27 June - 7 July 1995 | null | null | null | hep-th | null | The dual superconductivity of QCD vacuum as a mechanism for colour
confinement is reviewed. Recent evidence from lattice of monopole condensation
is presented.
| [
{
"created": "Wed, 6 Mar 1996 13:03:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Di Giacomo",
"Adriano",
""
]
] | The dual superconductivity of QCD vacuum as a mechanism for colour confinement is reviewed. Recent evidence from lattice of monopole condensation is presented. | 22.658794 | 9.8016 | 9.379264 | 10.16897 | 10.298658 | 13.996768 | 9.644398 | 9.988941 | 8.700066 | 11.850623 | 10.132212 | 10.946499 | 11.036753 | 10.560396 | 11.423766 | 11.435066 | 10.612086 | 12.05244 | 10.524881 | 9.984239 | 12.211714 |
hep-th/0703040 | Kazuya Koyama | Kazuya Koyama and David Wands | Ekpyrotic collapse with multiple fields | 13 pages, 1 figure | JCAP 0704:008,2007 | 10.1088/1475-7516/2007/04/008 | null | hep-th astro-ph | null | A scale invariant spectrum of isocurvature perturbations is generated during
collapse in the scaling solution in models where two or more fields have steep
negative exponential potentials. The scale invariance of the spectrum is
realised by a tachyonic instability in the isocurvature field. We show that
this instabil... | [
{
"created": "Mon, 5 Mar 2007 13:20:09 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Mar 2007 17:08:54 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Koyama",
"Kazuya",
""
],
[
"Wands",
"David",
""
]
] | A scale invariant spectrum of isocurvature perturbations is generated during collapse in the scaling solution in models where two or more fields have steep negative exponential potentials. The scale invariance of the spectrum is realised by a tachyonic instability in the isocurvature field. We show that this instabilit... | 12.07518 | 10.822939 | 11.562728 | 11.118357 | 11.850128 | 11.751666 | 12.430487 | 10.945023 | 11.23003 | 11.77616 | 10.431541 | 11.317545 | 11.202746 | 10.907642 | 11.097701 | 11.453101 | 11.072774 | 11.573904 | 10.687204 | 11.734078 | 11.059258 |
hep-th/0612229 | Arutyunov Gleb E | Gleb Arutyunov, Sergey Frolov, Marija Zamaklar | The Zamolodchikov-Faddeev Algebra for AdS_5 x S^5 Superstring | 40 pages, v2: derivation of symmetries from the S-matrix and the Hopf
algebra interpretation added, typos corrected, references added | JHEP 0704:002,2007 | 10.1088/1126-6708/2007/04/002 | AEI-2006-099, ITP-UU-06-58, SPIN-06-48, TCDMATH 06-18 | hep-th nlin.SI | null | We discuss the Zamolodchikov-Faddeev algebra for the superstring sigma-model
on AdS_5 x S^5. We find the canonical su(2|2)^2 invariant S-matrix satisfying
the standard Yang-Baxter and crossing symmetry equations. Its near-plane-wave
expansion matches exactly the leading order term recently obtained by the
direct pert... | [
{
"created": "Wed, 20 Dec 2006 20:39:20 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Jan 2007 15:40:25 GMT",
"version": "v2"
},
{
"created": "Tue, 20 Mar 2007 17:16:45 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Arutyunov",
"Gleb",
""
],
[
"Frolov",
"Sergey",
""
],
[
"Zamaklar",
"Marija",
""
]
] | We discuss the Zamolodchikov-Faddeev algebra for the superstring sigma-model on AdS_5 x S^5. We find the canonical su(2|2)^2 invariant S-matrix satisfying the standard Yang-Baxter and crossing symmetry equations. Its near-plane-wave expansion matches exactly the leading order term recently obtained by the direct pertur... | 7.577981 | 7.165212 | 8.785131 | 6.968878 | 6.808931 | 7.075134 | 7.346217 | 7.016416 | 7.260538 | 9.121171 | 6.97211 | 7.223423 | 7.611493 | 7.103459 | 7.035655 | 6.886575 | 7.157346 | 6.830964 | 7.06878 | 7.747674 | 7.165411 |
2107.12796 | Loriano Bonora | L. Bonora and R.P. Malik | BRST and superfield formalism. A review | 56 pages, typos corrected, bibliography completed, to appear in
"Universe" | Universe 2021, 7, 280 | 10.3390/universe708028 | SISSA 17/2021/FISI | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article, which is a review with substantial original material, is meant
to offer a comprehensive description of the superfield representations of the
BRST and anti-BRST algebras and their applications to some field-theoretic
topics. After a review of the superfield formalism for gauge theories we
present the sam... | [
{
"created": "Tue, 27 Jul 2021 13:11:17 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jul 2021 13:49:37 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Aug 2021 17:05:13 GMT",
"version": "v3"
}
] | 2021-08-12 | [
[
"Bonora",
"L.",
""
],
[
"Malik",
"R. P.",
""
]
] | This article, which is a review with substantial original material, is meant to offer a comprehensive description of the superfield representations of the BRST and anti-BRST algebras and their applications to some field-theoretic topics. After a review of the superfield formalism for gauge theories we present the same ... | 10.735796 | 10.089245 | 10.628839 | 10.228322 | 9.889729 | 10.055831 | 10.626823 | 10.087804 | 9.535345 | 11.575485 | 10.309576 | 9.828428 | 10.240869 | 9.939027 | 9.923824 | 10.029137 | 10.113722 | 10.399979 | 9.976027 | 10.299599 | 9.841017 |
0710.3040 | Christian Brouder | Christian Brouder and Michael Duetsch | Relating on-shell and off-shell formalism in perturbative quantum field
theory | The case of gauge fields was added. 16 pages | J.Math.Phys.49:052303,2008 | 10.1063/1.2918137 | null | hep-th | null | In the on-shell formalism (mostly used in perturbative quantum field theory)
the entries of the time ordered product T are on-shell fields (i.e. the basic
fields satisfy the free field equations). With that, (multi)linearity of T is
incompatible with the Action Ward identity. This can be circumvented by using
the off... | [
{
"created": "Tue, 16 Oct 2007 13:00:56 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Feb 2008 10:40:42 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Brouder",
"Christian",
""
],
[
"Duetsch",
"Michael",
""
]
] | In the on-shell formalism (mostly used in perturbative quantum field theory) the entries of the time ordered product T are on-shell fields (i.e. the basic fields satisfy the free field equations). With that, (multi)linearity of T is incompatible with the Action Ward identity. This can be circumvented by using the off-s... | 9.295723 | 8.973221 | 9.103868 | 8.403955 | 9.604686 | 9.711287 | 9.841064 | 9.330957 | 8.946563 | 9.811302 | 8.620017 | 8.338984 | 8.463505 | 8.317756 | 8.516673 | 8.484178 | 8.314051 | 8.20339 | 8.167029 | 8.394151 | 8.254188 |
hep-th/9610082 | Gabriele Ferretti | Ulf H. Danielsson and Gabriele Ferretti | The Heterotic Life of the D-particle | 20 pages, LaTeX | Int.J.Mod.Phys. A12 (1997) 4581-4596 | 10.1142/S0217751X97002474 | UUITP-24/96 | hep-th | null | We study the dynamics of D-particles (D0-branes) in type I' string theory and
of the corresponding states in the dual heterotic description. We account for
the presence of the two 8-orientifolds (8 dimensional orientifold planes) and
sixteen D8-branes by deriving the appropriate quantum mechanical system. We
recover ... | [
{
"created": "Fri, 11 Oct 1996 12:52:42 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Danielsson",
"Ulf H.",
""
],
[
"Ferretti",
"Gabriele",
""
]
] | We study the dynamics of D-particles (D0-branes) in type I' string theory and of the corresponding states in the dual heterotic description. We account for the presence of the two 8-orientifolds (8 dimensional orientifold planes) and sixteen D8-branes by deriving the appropriate quantum mechanical system. We recover th... | 10.766142 | 10.809712 | 12.307729 | 10.85285 | 10.619299 | 10.811323 | 10.763987 | 10.459748 | 10.568988 | 12.923233 | 10.594827 | 10.482929 | 11.045753 | 10.330305 | 10.424751 | 10.356458 | 10.456228 | 10.513169 | 10.087191 | 11.143637 | 10.196173 |
hep-th/9712004 | Paul K. Townsend | P.K. Townsend | M-theory from its superalgebra | 43 pp. Cargese lectures 1997. Minor errors corrected, as in previous
revisions | null | null | null | hep-th | null | These lectures explore what can be learnt about M-theory from its
superalgebra. The first three lectures introduce the 'basic' branes of
M-theory, and type II superstring theories, and show how the duality relations
between them are encoded in the respective spacetime superalgebras. The fourth
lecture introduces bran... | [
{
"created": "Mon, 1 Dec 1997 17:13:12 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Dec 1997 16:49:13 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Jan 1998 14:15:55 GMT",
"version": "v3"
},
{
"created": "Thu, 26 Feb 1998 00:29:19 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Townsend",
"P. K.",
""
]
] | These lectures explore what can be learnt about M-theory from its superalgebra. The first three lectures introduce the 'basic' branes of M-theory, and type II superstring theories, and show how the duality relations between them are encoded in the respective spacetime superalgebras. The fourth lecture introduces brane ... | 7.545462 | 7.131998 | 9.335873 | 6.757215 | 6.827196 | 7.141901 | 7.190671 | 6.854521 | 6.89044 | 8.873059 | 6.825177 | 6.553752 | 7.44664 | 6.532637 | 6.842479 | 6.631753 | 6.807464 | 6.478426 | 6.594605 | 7.388453 | 6.4449 |
1610.00475 | Hideo Suganuma | Kohei Matsumoto, Yuya Nakagawa and Hideo Suganuma (Kyoto U.) | A Study of the H-dibaryon in Holographic QCD | 5 pages, 2 figures | null | 10.7566/JPSCP.13.020014 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the H-dibaryon (uuddss) in holographic QCD for the first time.
Holographic QCD is derived from a QCD-equivalent D-brane system
($S^1$-compactified D4/D8/$\overline{\rm D8}$) in the superstring theory via
the gauge/gravity correspondence. In holographic QCD, all baryons appear as
topological chiral solitons o... | [
{
"created": "Mon, 3 Oct 2016 10:14:27 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Oct 2016 17:13:31 GMT",
"version": "v2"
},
{
"created": "Thu, 3 Nov 2016 17:10:25 GMT",
"version": "v3"
},
{
"created": "Thu, 17 Nov 2016 22:50:53 GMT",
"version": "v4"
}
] | 2017-03-08 | [
[
"Matsumoto",
"Kohei",
"",
"Kyoto U."
],
[
"Nakagawa",
"Yuya",
"",
"Kyoto U."
],
[
"Suganuma",
"Hideo",
"",
"Kyoto U."
]
] | We study the H-dibaryon (uuddss) in holographic QCD for the first time. Holographic QCD is derived from a QCD-equivalent D-brane system ($S^1$-compactified D4/D8/$\overline{\rm D8}$) in the superstring theory via the gauge/gravity correspondence. In holographic QCD, all baryons appear as topological chiral solitons of ... | 4.877288 | 4.339095 | 5.548502 | 4.659409 | 5.399395 | 4.474368 | 4.338802 | 4.276155 | 4.737007 | 5.8036 | 4.492972 | 4.851179 | 5.096166 | 4.681686 | 4.930355 | 5.101746 | 4.740517 | 4.612625 | 4.798184 | 4.891105 | 4.536869 |
hep-th/0501017 | Sebastian Nowak | Sebastian Nowak | Lorentz invariance of scalar field action on $\kappa$-Minkowski
space-time | 11 pages | null | null | null | hep-th | null | We construct field theory on noncommutative $\kappa$-Minkowski space-time.
Having the Lorentz action on the noncommutative space-time coordinates we show
that the field lagrangian is invariant. We show that noncommutativity requires
replacing the Leibnitz rule with the coproduct one.
| [
{
"created": "Tue, 4 Jan 2005 15:09:16 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nowak",
"Sebastian",
""
]
] | We construct field theory on noncommutative $\kappa$-Minkowski space-time. Having the Lorentz action on the noncommutative space-time coordinates we show that the field lagrangian is invariant. We show that noncommutativity requires replacing the Leibnitz rule with the coproduct one. | 9.641271 | 8.143637 | 8.092692 | 7.948199 | 7.768295 | 7.913377 | 8.316697 | 7.372915 | 7.372418 | 9.167743 | 8.228836 | 8.402036 | 8.235477 | 8.079355 | 8.585148 | 8.701829 | 8.105007 | 8.261007 | 8.13677 | 8.763393 | 8.305659 |
2106.04535 | David Rosa Junior | D. R. Junior, L. E. Oxman, and G. M. Sim\~oes | From center-vortex ensembles to the confining flux tube | null | Universe 2021, 7(8), 253 | 10.3390/universe7080253 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this review, we discuss the present status of the description of confining
flux tubes in SU(N) pure Yang-Mills theory in terms of ensembles of percolating
center vortices. This is based on three main pillars: modelling in the
continuum the ensemble components detected in the lattice, the derivation of
effective fi... | [
{
"created": "Tue, 8 Jun 2021 17:18:35 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Aug 2021 12:26:09 GMT",
"version": "v2"
}
] | 2021-08-11 | [
[
"Junior",
"D. R.",
""
],
[
"Oxman",
"L. E.",
""
],
[
"Simões",
"G. M.",
""
]
] | In this review, we discuss the present status of the description of confining flux tubes in SU(N) pure Yang-Mills theory in terms of ensembles of percolating center vortices. This is based on three main pillars: modelling in the continuum the ensemble components detected in the lattice, the derivation of effective fiel... | 16.659695 | 18.195473 | 17.76255 | 15.781316 | 15.856438 | 17.142345 | 17.221737 | 15.459038 | 16.475475 | 17.736406 | 15.792879 | 14.790855 | 15.875521 | 15.631377 | 15.223486 | 14.988997 | 15.804752 | 15.053591 | 15.231897 | 16.235886 | 14.775681 |
0810.4519 | Amihay Hanany | Davide Forcella, Amihay Hanany, Alberto Zaffaroni | Master Space, Hilbert Series and Seiberg Duality | 32 pages, 7 figures, 7 tables; minor corrections | JHEP 0907:018,2009 | 10.1088/1126-6708/2009/07/018 | Bicocca-FT-08-16, CERN-PH-TH/2008-200, Imperial/TP/08/AH/09 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the action of Toric (Seiberg) duality on the combined mesonic and
baryonic moduli space of quiver gauge theories obtained from D3 branes at
Calabi-Yau singularities. We analyze in particular the structure of the master
space, the complete moduli space for one brane, for different toric phases of a
given si... | [
{
"created": "Fri, 24 Oct 2008 18:25:39 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Apr 2009 14:17:32 GMT",
"version": "v2"
}
] | 2009-07-22 | [
[
"Forcella",
"Davide",
""
],
[
"Hanany",
"Amihay",
""
],
[
"Zaffaroni",
"Alberto",
""
]
] | We analyze the action of Toric (Seiberg) duality on the combined mesonic and baryonic moduli space of quiver gauge theories obtained from D3 branes at Calabi-Yau singularities. We analyze in particular the structure of the master space, the complete moduli space for one brane, for different toric phases of a given sing... | 7.681408 | 6.573418 | 8.615005 | 7.015014 | 7.242898 | 6.701041 | 7.078815 | 7.442318 | 6.757473 | 8.038265 | 6.633536 | 7.04481 | 7.798748 | 7.111162 | 7.000619 | 7.180061 | 7.141898 | 7.198273 | 7.193418 | 7.410151 | 6.93461 |
2007.10367 | Daniel Grumiller | C. Ecker, D. Grumiller, H. Soltanpanahi and P. Stanzer | QNEC2 in deformed holographic CFTs | 55pp, 18 figs; v2: added reference; v3: major revision: added
clarifying remarks, corrected critical exponent in section 4, and added table
1 with data showing the universality of the critical exponent (4.6) | null | 10.1007/JHEP03(2021)213 | TUW-20-01 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We use the quantum null energy condition in strongly coupled two-dimensional
field theories (QNEC2) as diagnostic tool to study a variety of phase
structures, including crossover, second and first order phase transitions. We
find a universal QNEC2 constraint for first order phase transitions with kinked
entanglement ... | [
{
"created": "Mon, 20 Jul 2020 18:00:27 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Jul 2020 07:08:49 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Feb 2021 08:30:00 GMT",
"version": "v3"
}
] | 2021-04-07 | [
[
"Ecker",
"C.",
""
],
[
"Grumiller",
"D.",
""
],
[
"Soltanpanahi",
"H.",
""
],
[
"Stanzer",
"P.",
""
]
] | We use the quantum null energy condition in strongly coupled two-dimensional field theories (QNEC2) as diagnostic tool to study a variety of phase structures, including crossover, second and first order phase transitions. We find a universal QNEC2 constraint for first order phase transitions with kinked entanglement en... | 10.299803 | 9.450526 | 11.809011 | 9.30719 | 10.589051 | 9.981409 | 9.963614 | 9.307788 | 9.387266 | 12.404541 | 9.226568 | 9.357861 | 10.376434 | 9.813986 | 9.573863 | 9.28871 | 9.317835 | 9.527379 | 9.406226 | 10.911481 | 9.768118 |
1906.05501 | Hayato Hirai | Hayato Hirai | Shrinking of Operators in Quantum Error Correction and AdS/CFT | 40 pages, 1 figure, v2: published version | null | 10.1007/JHEP12(2019)128 | OU-HET-1020 | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We first show that a class of operators acting on a given bipartite pure
state on $\mathcal{H}_{A}\otimes\mathcal{H}_{B}$ can shrink its supports on
$\mathcal{H}_{A}\otimes\mathcal{H}_{B}$ to only $\mathcal{H}_{A}$ or
$\mathcal{H}_{B}$ while keeping its mappings. Using this result, we show how to
systematically const... | [
{
"created": "Thu, 13 Jun 2019 06:32:39 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Feb 2020 09:00:03 GMT",
"version": "v2"
}
] | 2020-02-28 | [
[
"Hirai",
"Hayato",
""
]
] | We first show that a class of operators acting on a given bipartite pure state on $\mathcal{H}_{A}\otimes\mathcal{H}_{B}$ can shrink its supports on $\mathcal{H}_{A}\otimes\mathcal{H}_{B}$ to only $\mathcal{H}_{A}$ or $\mathcal{H}_{B}$ while keeping its mappings. Using this result, we show how to systematically constru... | 8.416545 | 8.716345 | 8.796268 | 7.919236 | 7.964967 | 8.571171 | 8.372376 | 8.339732 | 8.298148 | 9.053307 | 7.623577 | 7.874419 | 7.981787 | 7.723955 | 7.917578 | 8.148372 | 7.837578 | 7.828888 | 7.921126 | 8.302927 | 8.026995 |
2311.11671 | Mohammad Naghdi | M. Naghdi | Higgs-like (pseudo)Scalars in AdS$_4$, Marginal and Irrelevant
Deformations in CFT_3 and Instantons on S^3 | 27 Pages, Minor changes, Typos fixed | Chin. Phys. C 48, 043104 (2024) | 10.1088/1674-1137/ad205f | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | With a 4-form ansatz of 11-dimensional supergravity over non-dynamical AdS$_4
\times S^7/Z_k$ background, with the internal space as a $S^1$ Hopf fibration
on CP$^3$, we get a consistent truncation. The (pseudo)scalars, in the
resulting scalar equations in Euclidean AdS_4 space, may be viewed as arising
from (anti)M-... | [
{
"created": "Mon, 20 Nov 2023 11:11:59 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jan 2024 15:17:25 GMT",
"version": "v2"
}
] | 2024-03-18 | [
[
"Naghdi",
"M.",
""
]
] | With a 4-form ansatz of 11-dimensional supergravity over non-dynamical AdS$_4 \times S^7/Z_k$ background, with the internal space as a $S^1$ Hopf fibration on CP$^3$, we get a consistent truncation. The (pseudo)scalars, in the resulting scalar equations in Euclidean AdS_4 space, may be viewed as arising from (anti)M-br... | 16.530815 | 15.140141 | 18.676123 | 14.676308 | 16.356726 | 15.182037 | 15.432137 | 16.194658 | 16.00185 | 19.518385 | 15.248885 | 15.294876 | 16.623823 | 15.223112 | 15.139491 | 15.641133 | 16.112953 | 15.660082 | 15.444114 | 16.122841 | 15.284345 |
hep-th/9311142 | Andrei Mironov | A.Morozov | Bosonization of Coordinate Ring of $U_q(SL(N))$. The Cases of $N=2$ and
$N=3$ | ITEP-M-7/93 (11 pages) | JETP Lett. 60 (1994) 225-234 | null | null | hep-th | null | Non-abelian coordinate ring of $U_q(SL(N))$ (quantum deformation of the
algebra of functions) for $N=2,3$ is represented in terms of conventional
creation and annihilation operators. This allows to construct explicitly
representations of this algebra, which were earlier described in somewhat more
abstract algebraic f... | [
{
"created": "Tue, 23 Nov 1993 19:17:15 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Morozov",
"A.",
""
]
] | Non-abelian coordinate ring of $U_q(SL(N))$ (quantum deformation of the algebra of functions) for $N=2,3$ is represented in terms of conventional creation and annihilation operators. This allows to construct explicitly representations of this algebra, which were earlier described in somewhat more abstract algebraic fas... | 11.413513 | 9.666105 | 11.097138 | 9.519442 | 9.88554 | 10.292647 | 9.950475 | 9.368155 | 9.104868 | 11.857773 | 9.169732 | 9.312249 | 10.619021 | 8.979669 | 9.281997 | 9.308195 | 9.223504 | 8.943523 | 9.273461 | 10.48054 | 9.385986 |
hep-th/0101227 | Jens Mund | Jens Mund | The Bisognano-Wichmann Theorem for Massive Theories | 16 pages; improved and corrected formulations | Annales Henri Poincare 2 (2001) 907-926 | 10.1007/s00023-001-8598-x | null | hep-th math-ph math.MP | null | The geometric action of modular groups for wedge regions (Bisognano-Wichmann
property) is derived from the principles of local quantum physics for a large
class of Poincare covariant models in d=4. As a consequence, the CPT theorem
holds for this class. The models must have a complete interpretation in terms
of massi... | [
{
"created": "Wed, 31 Jan 2001 15:58:04 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Feb 2001 16:15:32 GMT",
"version": "v2"
}
] | 2015-06-25 | [
[
"Mund",
"Jens",
""
]
] | The geometric action of modular groups for wedge regions (Bisognano-Wichmann property) is derived from the principles of local quantum physics for a large class of Poincare covariant models in d=4. As a consequence, the CPT theorem holds for this class. The models must have a complete interpretation in terms of massive... | 14.311115 | 12.592367 | 17.304543 | 12.715478 | 14.06111 | 12.551183 | 14.821818 | 12.507648 | 11.769253 | 19.017216 | 13.091486 | 11.956887 | 13.471906 | 12.453287 | 12.428107 | 12.79304 | 12.856521 | 12.927686 | 12.044282 | 13.446809 | 13.32598 |
hep-th/9912044 | Anton Kapustin | Anton Kapustin | On The Universality Class Of Little String Theories | 25 pages, latex | Phys.Rev. D63 (2001) 086005 | 10.1103/PhysRevD.63.086005 | IASSNS-HEP-99/111 | hep-th | null | We propose that Little String Theories in six dimensions are quasilocal
quantum field theories. Such field theories obey a modification of Wightman
axioms which allows Wightman functions (i.e. vacuum expectation values of
products of fundamental fields) to grow exponentially in momentum space.
Wightman functions of q... | [
{
"created": "Mon, 6 Dec 1999 21:36:27 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Apr 2000 22:04:27 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Kapustin",
"Anton",
""
]
] | We propose that Little String Theories in six dimensions are quasilocal quantum field theories. Such field theories obey a modification of Wightman axioms which allows Wightman functions (i.e. vacuum expectation values of products of fundamental fields) to grow exponentially in momentum space. Wightman functions of qua... | 10.426641 | 9.523178 | 12.423954 | 10.624169 | 10.885988 | 11.532141 | 11.718651 | 10.857649 | 10.139972 | 12.56563 | 9.835726 | 10.174022 | 10.538484 | 10.306931 | 10.205205 | 10.354551 | 10.104048 | 10.15469 | 9.933883 | 10.780352 | 9.746085 |
hep-th/0604141 | Yui Noma | Yui Noma | Supersymmetric Gauge Theories with Matters, Toric Geometries and Random
Partitions | 26 pages, 11 figures; v2 typos corrected | Prog.Theor.Phys.116:1131-1157,2007 | 10.1143/PTP.116.1131 | OU-HET 559 | hep-th | null | We derive the relation between the Hilbert space of certain geometries under
the Bohr-Sommerfeld quantization and the perturbative prepotentials for the
supersymmetric five-dimensional SU(N) gauge theories with massive fundamental
matters and with one massive adjoint matter. The gauge theory with one adjoint
matter s... | [
{
"created": "Thu, 20 Apr 2006 09:32:54 GMT",
"version": "v1"
},
{
"created": "Thu, 25 May 2006 09:34:15 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Noma",
"Yui",
""
]
] | We derive the relation between the Hilbert space of certain geometries under the Bohr-Sommerfeld quantization and the perturbative prepotentials for the supersymmetric five-dimensional SU(N) gauge theories with massive fundamental matters and with one massive adjoint matter. The gauge theory with one adjoint matter sho... | 11.548704 | 10.186303 | 12.561728 | 10.568748 | 10.634483 | 11.11175 | 9.878394 | 11.435058 | 10.617899 | 13.001214 | 10.552083 | 11.077617 | 11.375562 | 11.643545 | 11.088731 | 11.24472 | 10.680238 | 11.320437 | 11.355263 | 11.120252 | 11.363235 |
hep-th/0212206 | Adam Falkowski | Adam Falkowski, Hans-Peter Nilles, Marek Olechowski and Stefan
Pokorski | Deconstructing 5D supersymmetric U(1) gauge theories on orbifolds | Discussion of mixed anomalies and some clarifying commments added.
Version to appear in Phys.Lett. B | Phys.Lett.B566:248-257,2003 | 10.1016/S0370-2693(03)00843-8 | null | hep-th | null | We investigate deconstruction of five dimensional supersymmetric abelian
gauge theories compactified on $S_1/Z_2$, with various sets of bulk and matter
multiplets. The problem of anomalies, chirality and stability in the
deconstructed theories is discussed. We find that for most of the 5d brane/bulk
matter assignment... | [
{
"created": "Tue, 17 Dec 2002 18:16:17 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Jun 2003 15:49:46 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Falkowski",
"Adam",
""
],
[
"Nilles",
"Hans-Peter",
""
],
[
"Olechowski",
"Marek",
""
],
[
"Pokorski",
"Stefan",
""
]
] | We investigate deconstruction of five dimensional supersymmetric abelian gauge theories compactified on $S_1/Z_2$, with various sets of bulk and matter multiplets. The problem of anomalies, chirality and stability in the deconstructed theories is discussed. We find that for most of the 5d brane/bulk matter assignments ... | 12.245047 | 10.984085 | 10.415535 | 9.799032 | 10.571793 | 11.045286 | 10.394707 | 10.646772 | 10.154768 | 10.866899 | 9.599192 | 10.96603 | 10.535685 | 10.285277 | 9.823872 | 10.763635 | 10.035143 | 10.508864 | 10.270254 | 10.607275 | 10.29234 |
hep-th/0507048 | Ian McArthur | D. Grasso and I.N. McArthur | The SU(N) Matrix Model at Two Loops | 30 pages, 1 figure; v2 - typos corrected, references updated | JHEP 0509 (2005) 075 | 10.1088/1126-6708/2005/09/075 | null | hep-th | null | Multi-loop calculations of the effective action for the matrix model are
important for carrying out tests of the conjectured relationship of the matrix
model to the low energy description of M-theory. In particular, comparison with
N-graviton scattering amplitudes in eleven-dimensional supergravity requires
the calcu... | [
{
"created": "Wed, 6 Jul 2005 05:50:10 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Aug 2005 07:48:09 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Grasso",
"D.",
""
],
[
"McArthur",
"I. N.",
""
]
] | Multi-loop calculations of the effective action for the matrix model are important for carrying out tests of the conjectured relationship of the matrix model to the low energy description of M-theory. In particular, comparison with N-graviton scattering amplitudes in eleven-dimensional supergravity requires the calcula... | 6.531273 | 5.775344 | 6.457605 | 5.852945 | 6.05236 | 5.988301 | 5.863606 | 5.735887 | 5.515911 | 6.336165 | 5.985845 | 5.662746 | 6.018724 | 5.654091 | 5.752607 | 5.837105 | 5.648532 | 5.634906 | 5.682658 | 6.019725 | 5.921794 |
1810.03976 | Douglas A. Singleton | Michael Bishop, Erick Aiken, and Douglas Singleton | Modified commutation relationships from the Berry-Keating program | 14 pages, 0 figures revtex4. Version published in PRD | Phys. Rev. D 99, 026012 (2019) | 10.1103/PhysRevD.99.026012 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Current approaches to quantum gravity suggest there should be a modification
of the standard quantum mechanical commutator, $[{\hat x} , {\hat p}] = i
\hbar$. Typical modifications are phenomenological and designed to result in a
minimal length scale. As a motivating principle for the modification of the
position and... | [
{
"created": "Sun, 30 Sep 2018 17:56:10 GMT",
"version": "v1"
},
{
"created": "Sun, 13 Jan 2019 00:30:17 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Jan 2019 18:35:02 GMT",
"version": "v3"
}
] | 2019-01-28 | [
[
"Bishop",
"Michael",
""
],
[
"Aiken",
"Erick",
""
],
[
"Singleton",
"Douglas",
""
]
] | Current approaches to quantum gravity suggest there should be a modification of the standard quantum mechanical commutator, $[{\hat x} , {\hat p}] = i \hbar$. Typical modifications are phenomenological and designed to result in a minimal length scale. As a motivating principle for the modification of the position and m... | 7.222838 | 8.125741 | 7.56646 | 7.492967 | 7.810912 | 7.387983 | 7.948417 | 7.252561 | 7.646674 | 8.97977 | 7.63109 | 7.204064 | 6.729279 | 6.822173 | 6.914499 | 6.975707 | 6.95952 | 7.06681 | 7.059755 | 6.819222 | 7.02606 |
hep-th/0407036 | Gonzalo A. Palma | Gonzalo A. Palma, Anne-Christine Davis (DAMTP, University of
Cambridge) | Moduli-Space Approximation for BPS Brane-Worlds | 10 pages, 1 figure | Phys.Rev. D70 (2004) 106003 | 10.1103/PhysRevD.70.106003 | null | hep-th astro-ph hep-ph | null | We develop the moduli-space approximation for the low energy regime of
BPS-branes with a bulk scalar field to obtain an effective four-dimensional
action describing the system. An arbitrary BPS potential is used and account is
taken of the presence of matter in the branes and small supersymmetry breaking
terms. The r... | [
{
"created": "Tue, 6 Jul 2004 12:14:49 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Palma",
"Gonzalo A.",
"",
"DAMTP, University of\n Cambridge"
],
[
"Davis",
"Anne-Christine",
"",
"DAMTP, University of\n Cambridge"
]
] | We develop the moduli-space approximation for the low energy regime of BPS-branes with a bulk scalar field to obtain an effective four-dimensional action describing the system. An arbitrary BPS potential is used and account is taken of the presence of matter in the branes and small supersymmetry breaking terms. The res... | 17.385395 | 15.319539 | 13.979528 | 15.094093 | 15.272772 | 16.51993 | 15.472529 | 15.054004 | 15.511682 | 15.786826 | 15.342231 | 15.242876 | 13.995796 | 15.268017 | 15.775204 | 15.542941 | 16.085106 | 14.458811 | 15.034179 | 14.600493 | 14.686844 |
hep-th/9304149 | Patrick Dorey | Patrick Dorey | A remark on the coupling-dependence in affine Toda field theories | 12 pages (harvmac), CERN-TH.6873/93 | Phys.Lett. B312 (1993) 291-298 | 10.1016/0370-2693(93)91083-Y | null | hep-th | null | The affine Toda field theories based on the non simply-laced Lie algebras are
discussed. By rewriting the S-matrix formulae found by Delius et al, a
universal form for the coupling-constant dependence of these models is
obtained, and related to various general properties of the classical couplings.
This is illustrate... | [
{
"created": "Wed, 28 Apr 1993 21:47:21 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dorey",
"Patrick",
""
]
] | The affine Toda field theories based on the non simply-laced Lie algebras are discussed. By rewriting the S-matrix formulae found by Delius et al, a universal form for the coupling-constant dependence of these models is obtained, and related to various general properties of the classical couplings. This is illustrated ... | 9.394709 | 7.71879 | 10.645981 | 7.517047 | 8.273938 | 7.800122 | 7.663664 | 7.760644 | 7.378124 | 11.222481 | 7.503561 | 7.979194 | 9.825204 | 8.515627 | 8.371137 | 8.465158 | 8.018411 | 8.124112 | 8.358003 | 9.989778 | 8.115727 |
hep-th/9911096 | Igor R. Klebanov | Igor R. Klebanov and Nikita A. Nekrasov | Gravity Duals of Fractional Branes and Logarithmic RG Flow | 15 pages, harvmac; v2: typos corrected; v3: minor corrections,
references added | Nucl.Phys. B574 (2000) 263-274 | 10.1016/S0550-3213(00)00016-X | PUPT-1897, ITEP-TH-61/99 | hep-th | null | We study fractional branes in ${\CN}=2$ orbifold and ${\CN}=1$ conifold
theories. Placing a large number $N$ of regular D3-branes at the singularity
produces the dual ${\bf AdS}_5\times X^5$ geometry, and we describe the
fractional branes as small perturbations to this background. For the orbifolds,
$X^5={\bf S}^5/\G... | [
{
"created": "Fri, 12 Nov 1999 18:00:01 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Nov 1999 21:31:49 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Nov 1999 01:53:38 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Klebanov",
"Igor R.",
""
],
[
"Nekrasov",
"Nikita A.",
""
]
] | We study fractional branes in ${\CN}=2$ orbifold and ${\CN}=1$ conifold theories. Placing a large number $N$ of regular D3-branes at the singularity produces the dual ${\bf AdS}_5\times X^5$ geometry, and we describe the fractional branes as small perturbations to this background. For the orbifolds, $X^5={\bf S}^5/\Gam... | 6.256 | 5.808627 | 7.634932 | 5.876774 | 5.98054 | 6.203697 | 5.827369 | 5.675299 | 5.907884 | 8.565361 | 5.576057 | 5.92205 | 6.704366 | 6.066683 | 5.976914 | 5.998084 | 6.130169 | 6.172815 | 5.961243 | 6.515187 | 5.98771 |
hep-th/9803158 | Arne Lykke Larsen | M. Christensen, V.P. Frolov and A.L. Larsen | Soap Bubbles in Outer Space: Interaction of a Domain Wall with a Black
Hole | 15 pages, Latex, 4 figures included | Phys.Rev. D58 (1998) 085008 | 10.1103/PhysRevD.58.085008 | null | hep-th gr-qc | null | We discuss the generalized Plateau problem in the 3+1 dimensional
Schwarzschild background. This represents the physical situation, which could
for instance have appeared in the early universe, where a cosmic membrane (thin
domain wall) is located near a black hole. Considering stationary axially
symmetric membranes,... | [
{
"created": "Thu, 19 Mar 1998 16:31:41 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Christensen",
"M.",
""
],
[
"Frolov",
"V. P.",
""
],
[
"Larsen",
"A. L.",
""
]
] | We discuss the generalized Plateau problem in the 3+1 dimensional Schwarzschild background. This represents the physical situation, which could for instance have appeared in the early universe, where a cosmic membrane (thin domain wall) is located near a black hole. Considering stationary axially symmetric membranes, t... | 7.022934 | 7.588602 | 7.412848 | 6.826756 | 7.524158 | 7.406041 | 7.464396 | 6.886703 | 6.881752 | 7.511131 | 6.894503 | 6.801921 | 6.833558 | 6.610219 | 6.760512 | 6.750315 | 6.929666 | 6.730853 | 6.838027 | 6.894794 | 6.757894 |
1403.5549 | Sayantan Choudhury | Sayantan Choudhury, Anupam Mazumdar | Reconstructing inflationary potential from BICEP2 and running of tensor
modes | 22 pages, 5 figures, A new set of consistency relationships have been
added in the discussion, new citations added. arXiv admin note: text overlap
with arXiv:1306.4496 | null | null | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we will analyse the constraints on a sub-Planckian excursion of
a single inflaton field, which would yield a large tensor to scalar ratio,
while explaining the temperature anisotropy of the cosmic microwave background
(CMB) radiation. In particular, our attempt will be to reconstruct the
inflationary po... | [
{
"created": "Fri, 21 Mar 2014 19:28:34 GMT",
"version": "v1"
},
{
"created": "Sun, 30 Mar 2014 18:07:53 GMT",
"version": "v2"
}
] | 2014-04-01 | [
[
"Choudhury",
"Sayantan",
""
],
[
"Mazumdar",
"Anupam",
""
]
] | In this paper we will analyse the constraints on a sub-Planckian excursion of a single inflaton field, which would yield a large tensor to scalar ratio, while explaining the temperature anisotropy of the cosmic microwave background (CMB) radiation. In particular, our attempt will be to reconstruct the inflationary pote... | 4.674646 | 5.084278 | 4.924972 | 4.849351 | 5.114382 | 5.154404 | 5.137354 | 4.825605 | 4.841786 | 5.321401 | 4.708841 | 4.724336 | 4.653799 | 4.660366 | 4.736289 | 4.760857 | 4.708468 | 4.660956 | 4.60143 | 4.727385 | 4.672573 |
2101.00239 | Joselen Pena | Pedro D. Alvarez, Maria Pilar Garcia del Moral, Joselen M. Pe\~na and
Reginaldo Prado | Rotating Central Charge Membranes | 6 pages, 1 figure. Section 4 re-worked, conclusions modified.
Submitted to Journal of Physics: Conference Series Proceedings Chilean
Physics Symposium 2020 (SOCHIFI 2020) | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we obtain dynamical solutions of the bosonic sector of the
supermembrane theory with central charges formulated on $M_9\times T^2$,
denoted by MIM2. The theory with this condition corresponds to a supermembrane
with a $C_-$ flux. This sector of the M2-brane is very interesting since
classically is stable... | [
{
"created": "Fri, 1 Jan 2021 14:09:02 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Apr 2021 23:42:44 GMT",
"version": "v2"
}
] | 2021-04-14 | [
[
"Alvarez",
"Pedro D.",
""
],
[
"del Moral",
"Maria Pilar Garcia",
""
],
[
"Peña",
"Joselen M.",
""
],
[
"Prado",
"Reginaldo",
""
]
] | In this work we obtain dynamical solutions of the bosonic sector of the supermembrane theory with central charges formulated on $M_9\times T^2$, denoted by MIM2. The theory with this condition corresponds to a supermembrane with a $C_-$ flux. This sector of the M2-brane is very interesting since classically is stable a... | 14.99528 | 13.392507 | 17.524073 | 13.154055 | 13.47312 | 13.16287 | 13.67534 | 13.795986 | 13.021689 | 18.611071 | 12.66298 | 13.314001 | 14.540247 | 14.24031 | 13.446629 | 13.43806 | 13.607112 | 13.245871 | 14.102715 | 15.055792 | 13.532884 |
1005.0464 | Olaf Lechtenfeld | Olaf Lechtenfeld, Armen Nersessian, Vahagn Yeghikyan | Action-angle variables for dihedral systems on the circle | 8 pages; v2: references added, typos fixed, version for PLA | Phys.Lett.A374:4647-4652,2010 | 10.1016/j.physleta.2010.09.047 | null | hep-th math-ph math.DS math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A nonrelativistic particle on a circle and subject to a cos^{-2}(k phi)
potential is related to the two-dimensional (dihedral) Coxeter system I_2(k),
for k in N. For such `dihedral systems' we construct the action-angle variables
and establish a local equivalence with a free particle on the circle. We
perform the qua... | [
{
"created": "Tue, 4 May 2010 08:35:43 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Oct 2010 12:55:08 GMT",
"version": "v2"
}
] | 2011-01-18 | [
[
"Lechtenfeld",
"Olaf",
""
],
[
"Nersessian",
"Armen",
""
],
[
"Yeghikyan",
"Vahagn",
""
]
] | A nonrelativistic particle on a circle and subject to a cos^{-2}(k phi) potential is related to the two-dimensional (dihedral) Coxeter system I_2(k), for k in N. For such `dihedral systems' we construct the action-angle variables and establish a local equivalence with a free particle on the circle. We perform the quant... | 14.248897 | 13.682142 | 15.513712 | 12.153719 | 12.295267 | 12.154106 | 12.765324 | 12.676736 | 12.559604 | 17.2223 | 12.355467 | 12.281017 | 13.161722 | 12.332021 | 12.579889 | 12.769799 | 12.326189 | 12.275388 | 12.054218 | 13.085442 | 12.553104 |
hep-th/9409200 | Valeri Dvoeglazov | Valeri V. Dvoeglazov (Zacatecas University, M\'exico) | ADDENDUM to the papers on the Weinberg Theory | LaTeX file, 6pp. Preprint EFUAZ FT-94-09 | null | null | null | hep-th | null | The Weinberg-Tucker-Hammer equations are shown to substitute the common-used
$j=1$ massless equations. Meantime, the old equations preserve their
significance as a particular case.
Possible consequences are discussed.
| [
{
"created": "Mon, 3 Oct 1994 02:27:39 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dvoeglazov",
"Valeri V.",
"",
"Zacatecas University, México"
]
] | The Weinberg-Tucker-Hammer equations are shown to substitute the common-used $j=1$ massless equations. Meantime, the old equations preserve their significance as a particular case. Possible consequences are discussed. | 56.1091 | 41.309902 | 40.003139 | 37.927998 | 41.488041 | 39.115822 | 36.05751 | 41.82896 | 39.092514 | 66.101768 | 36.502468 | 40.537952 | 39.744652 | 35.91906 | 37.259621 | 36.852489 | 37.688499 | 39.495842 | 38.417965 | 40.987049 | 38.254681 |
1404.2095 | Niall MacKay | Alejandro De La Rosa Gomez and Niall J. MacKay | Twisted Yangian symmetry of the open Hubbard model | 13 pages. Minor revisions and additional references | null | 10.1088/1751-8113/47/30/305203 | null | hep-th cond-mat.str-el math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that, in the open Hubbard model with integrable boundary conditions,
the bulk Yangian symmetry is broken to a twisted Yangian. We prove that the
associated charges commute with the Hamiltonian and the reflection matrix, and
that they form a coideal subalgebra.
| [
{
"created": "Tue, 8 Apr 2014 11:48:16 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Jun 2014 17:05:12 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Gomez",
"Alejandro De La Rosa",
""
],
[
"MacKay",
"Niall J.",
""
]
] | We show that, in the open Hubbard model with integrable boundary conditions, the bulk Yangian symmetry is broken to a twisted Yangian. We prove that the associated charges commute with the Hamiltonian and the reflection matrix, and that they form a coideal subalgebra. | 9.24949 | 7.074733 | 10.56497 | 7.541718 | 7.114459 | 7.051404 | 6.643296 | 6.858581 | 7.414099 | 11.543375 | 7.225695 | 8.235548 | 10.291735 | 8.606665 | 8.0028 | 8.496104 | 8.304339 | 8.23666 | 8.780139 | 9.949829 | 8.291147 |
1607.05273 | Wilke van der Schee | Jorge Casalderrey-Solana, David Mateos, Wilke van der Schee, Miquel
Triana | Holographic heavy ion collisions with baryon charge | 18 pages, 10 figures | JHEP 1609 (2016) 108 | 10.1007/JHEP09(2016)108 | ICCUB-16-027, MIT-CTP/4819 | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We numerically simulate collisions of charged shockwaves in Einstein-Maxwell
theory in anti-de Sitter space as a toy model of heavy ion collisions with
non-zero baryon charge. The stress tensor and the baryon current become well
described by charged hydrodynamics at roughly the same time. The effect of the
charge den... | [
{
"created": "Mon, 18 Jul 2016 20:00:00 GMT",
"version": "v1"
}
] | 2017-07-05 | [
[
"Casalderrey-Solana",
"Jorge",
""
],
[
"Mateos",
"David",
""
],
[
"van der Schee",
"Wilke",
""
],
[
"Triana",
"Miquel",
""
]
] | We numerically simulate collisions of charged shockwaves in Einstein-Maxwell theory in anti-de Sitter space as a toy model of heavy ion collisions with non-zero baryon charge. The stress tensor and the baryon current become well described by charged hydrodynamics at roughly the same time. The effect of the charge densi... | 11.406416 | 10.465366 | 11.179301 | 10.075007 | 10.232222 | 9.9388 | 9.643397 | 9.983575 | 9.67057 | 11.62968 | 9.457146 | 10.025849 | 10.521781 | 10.10431 | 10.202792 | 10.023956 | 10.034042 | 9.780061 | 9.929482 | 10.473786 | 9.916835 |
hep-th/9910168 | Ilya Shapiro | G. de Berredo-Peixoto, J.A. Helayel-Neto, I.L. Shapiro | On the Consistency of a Fermion-Torsion Effective Theory | LaTeX, 26 pages, 4 figures | JHEP 0002 (2000) 003 | 10.1088/1126-6708/2000/02/003 | DF/UFJF-99/16, CBPF-NF-061/99 | hep-th | null | We discuss the possibility to construct an effective quantum field theory for
an axial vector coupled to a Dirac spinor field. A massive axial vector
describes antisymmetric torsion. The consistency conditions include unitarity
and renormalizability in the low-energy region. The investigation of the Ward
identities a... | [
{
"created": "Thu, 21 Oct 1999 11:56:28 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Mar 2001 17:53:45 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"de Berredo-Peixoto",
"G.",
""
],
[
"Helayel-Neto",
"J. A.",
""
],
[
"Shapiro",
"I. L.",
""
]
] | We discuss the possibility to construct an effective quantum field theory for an axial vector coupled to a Dirac spinor field. A massive axial vector describes antisymmetric torsion. The consistency conditions include unitarity and renormalizability in the low-energy region. The investigation of the Ward identities and... | 12.573712 | 10.542553 | 11.305209 | 11.528111 | 11.721222 | 10.69488 | 10.436 | 10.904241 | 11.371118 | 12.829135 | 10.562282 | 11.035784 | 11.855552 | 11.609652 | 11.458641 | 11.159685 | 11.552871 | 11.055746 | 11.468838 | 11.545167 | 10.785112 |
1803.07500 | Luca Mattiello | Luca Mattiello, Ivo Sachs | $\mathbb{Z}_2$ boundary twist fields and the moduli space of D-branes | 36 pages, 3 figures, section 3 revised, typos corrected | JHEP 07 (2018) 099 | 10.1007/JHEP07(2018)099 | LMU-ASC 14/18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the boundary conformal field theory of twist fields. Based on the
equivalence between twisted bosons on a circle and the orbifold theory at the
critical radius, we provide a bosonized representation of boundary twist fields
and thus a free field representation of the latter. One advantage of this
formulati... | [
{
"created": "Tue, 20 Mar 2018 15:59:21 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Apr 2018 09:24:40 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Jul 2018 15:14:47 GMT",
"version": "v3"
}
] | 2018-07-20 | [
[
"Mattiello",
"Luca",
""
],
[
"Sachs",
"Ivo",
""
]
] | We revisit the boundary conformal field theory of twist fields. Based on the equivalence between twisted bosons on a circle and the orbifold theory at the critical radius, we provide a bosonized representation of boundary twist fields and thus a free field representation of the latter. One advantage of this formulation... | 10.419938 | 9.137599 | 11.397902 | 9.564013 | 10.106269 | 9.559359 | 10.487686 | 9.222178 | 9.017547 | 12.129627 | 9.456347 | 9.234982 | 10.733981 | 9.716838 | 9.556406 | 9.534 | 9.674117 | 9.566486 | 9.997102 | 10.187838 | 9.680366 |
0704.1651 | Orest Hrycyna | Orest Hrycyna, Marek Szydlowski | Route to Lambda in conformally coupled phantom cosmology | revtex4, 7 pages, 3 figures; (v2) refs. added, typos corrected; (v3)
published version | Phys.Lett.B651:8-14,2007 | 10.1016/j.physletb.2007.05.057 | null | hep-th astro-ph | null | In this letter we investigate acceleration in the flat cosmological model
with a conformally coupled phantom field and we show that acceleration is its
generic feature. We reduce the dynamics of the model to a 3-dimensional
dynamical system and analyze it on a invariant 2-dimensional submanifold. Then
the concordance... | [
{
"created": "Thu, 12 Apr 2007 19:47:11 GMT",
"version": "v1"
},
{
"created": "Sun, 22 Apr 2007 17:26:12 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Jul 2007 19:45:23 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Hrycyna",
"Orest",
""
],
[
"Szydlowski",
"Marek",
""
]
] | In this letter we investigate acceleration in the flat cosmological model with a conformally coupled phantom field and we show that acceleration is its generic feature. We reduce the dynamics of the model to a 3-dimensional dynamical system and analyze it on a invariant 2-dimensional submanifold. Then the concordance F... | 10.711755 | 11.512246 | 10.568968 | 10.485859 | 10.690296 | 11.187387 | 11.518655 | 10.914247 | 10.943587 | 12.115498 | 10.629444 | 10.991168 | 10.120749 | 10.413355 | 10.66311 | 10.526295 | 10.706865 | 10.509768 | 10.757033 | 10.205692 | 10.431348 |
2005.12831 | I\~naki Garc\'ia-Etxebarria | Federica Albertini and Michele Del Zotto and I\~naki Garc\'ia
Etxebarria and Saghar S. Hosseini | Higher Form Symmetries and M-theory | 48 pages. v2: Added references and fixed typos | null | 10.1007/JHEP12(2020)203 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the geometric origin of discrete higher form symmetries of quantum
field theories in terms of defect groups from geometric engineering in
M-theory. The flux non-commutativity in M-theory gives rise to (mixed) 't Hooft
anomalies for the defect group which constrains the corresponding global
structures of th... | [
{
"created": "Tue, 26 May 2020 16:10:46 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jun 2020 17:42:23 GMT",
"version": "v2"
}
] | 2021-02-03 | [
[
"Albertini",
"Federica",
""
],
[
"Del Zotto",
"Michele",
""
],
[
"Etxebarria",
"Iñaki García",
""
],
[
"Hosseini",
"Saghar S.",
""
]
] | We discuss the geometric origin of discrete higher form symmetries of quantum field theories in terms of defect groups from geometric engineering in M-theory. The flux non-commutativity in M-theory gives rise to (mixed) 't Hooft anomalies for the defect group which constrains the corresponding global structures of the ... | 7.43084 | 7.372535 | 8.410832 | 7.033257 | 7.682199 | 7.095653 | 7.613207 | 7.541329 | 7.402051 | 8.436292 | 7.313223 | 7.484779 | 7.49725 | 7.049916 | 7.125625 | 7.212881 | 7.330378 | 7.20767 | 7.012189 | 7.558442 | 7.25046 |
1404.5151 | Fernando Quevedo | Fernando Quevedo | Local String Models and Moduli Stabilisation | 23 pages, 4 figures, invited contribution to 'Perspectives in String
Phenomenology' book B. Acharya, et al (eds). Minor rewordings and references
added | null | 10.1142/S0217732315300049 | DAMTP-2014-26 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A brief overview is presented of the progress made during the past few years
on the general structure of local models of particle physics from string theory
including: moduli stabilisation, supersymmetry breaking, global embedding in
compact Calabi-Yau compactifications and potential cosmological implications.
Type I... | [
{
"created": "Mon, 21 Apr 2014 09:51:27 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Apr 2014 15:44:41 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Quevedo",
"Fernando",
""
]
] | A brief overview is presented of the progress made during the past few years on the general structure of local models of particle physics from string theory including: moduli stabilisation, supersymmetry breaking, global embedding in compact Calabi-Yau compactifications and potential cosmological implications. Type IIB... | 9.614783 | 7.553115 | 9.362298 | 8.305228 | 9.471226 | 8.339813 | 8.411545 | 8.217057 | 8.067543 | 10.570084 | 8.179355 | 8.442224 | 8.981182 | 8.358253 | 8.348058 | 8.66021 | 8.461542 | 8.639812 | 8.392619 | 8.680707 | 8.582723 |
1308.4608 | Satoshi Okuda | Satoshi Okuda and Yutaka Yoshida | G/G gauged WZW-matter model, Bethe Ansatz for q-boson model and
Commutative Frobenius algebra | 41 pages, 7 figures, Published version | null | 10.1007/JHEP03(2014)003 | KEK-TH-1658, RUP-13-8 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the correspondence between two dimensional topological gauge
theories and quantum integrable systems discovered by Moore, Nekrasov,
Shatashvili. This correspondence means that the hidden quantum integrable
structure exists in the topological gauge theories. We showed the
correspondence between the G/G ... | [
{
"created": "Wed, 21 Aug 2013 15:06:39 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Mar 2014 09:29:42 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Okuda",
"Satoshi",
""
],
[
"Yoshida",
"Yutaka",
""
]
] | We investigate the correspondence between two dimensional topological gauge theories and quantum integrable systems discovered by Moore, Nekrasov, Shatashvili. This correspondence means that the hidden quantum integrable structure exists in the topological gauge theories. We showed the correspondence between the G/G ga... | 7.118606 | 6.686365 | 7.600625 | 6.259274 | 6.480621 | 6.463607 | 6.085015 | 6.436755 | 6.725935 | 7.963924 | 6.592439 | 6.461048 | 7.462196 | 6.641098 | 6.241486 | 6.578729 | 6.278641 | 6.705113 | 6.758802 | 7.179442 | 6.664855 |
hep-th/0602204 | Kazuyuki Fujii | Kazuyuki Fujii, Hiroshi Oike and Tatsuo Suzuki | Universal Yang-Mills Action on Four Dimensional Manifolds | Latex file ; 14 pages ; 1 figure ; minor changes | Int.J.Geom.Meth.Mod.Phys.3:1331-1340,2006 | null | null | hep-th math-ph math.MP quant-ph | null | The usual action of Yang-Mills theory is given by the quadratic form of
curvatures of a principal G bundle defined on four dimensional manifolds. The
non-linear generalization which is known as the Born-Infeld action has been
given. In this paper we give another non-linear generalization on four
dimensional manifolds... | [
{
"created": "Tue, 21 Feb 2006 02:20:56 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Feb 2006 23:47:30 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Fujii",
"Kazuyuki",
""
],
[
"Oike",
"Hiroshi",
""
],
[
"Suzuki",
"Tatsuo",
""
]
] | The usual action of Yang-Mills theory is given by the quadratic form of curvatures of a principal G bundle defined on four dimensional manifolds. The non-linear generalization which is known as the Born-Infeld action has been given. In this paper we give another non-linear generalization on four dimensional manifolds a... | 9.758697 | 9.515786 | 9.215752 | 8.579277 | 9.016037 | 9.666907 | 8.981331 | 8.85415 | 8.845567 | 10.318682 | 8.874248 | 8.898043 | 9.190468 | 8.817789 | 8.723939 | 8.827329 | 8.866694 | 8.930922 | 8.957971 | 9.354693 | 8.714355 |
hep-th/0502089 | Hitoshi Nishino | Hitoshi Nishino and Subhash Rajpoot | Dual Vector Multiplet Coupled to Dual N=1 Supergravity in 10D | 20 pages, no figures | Phys.Rev. D71 (2005) 085011 | 10.1103/PhysRevD.71.085011 | CSULB-PA-04-7 | hep-th | null | We couple in superspace a `dual' vector multiplet (C_{m_1... m_7}, \l^\alpha)
to the dual version of N=1 supergravity (e_m{}^a, \psi_m{}^\alpha, M_{m_1...
m_6}, \chi_\a,\Phi) in ten-dimensions. Our new 7-form field C has its 8-form
field strength H dual to the 2-form field strength F of the conventional vector
multip... | [
{
"created": "Wed, 9 Feb 2005 07:28:26 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Nishino",
"Hitoshi",
""
],
[
"Rajpoot",
"Subhash",
""
]
] | We couple in superspace a `dual' vector multiplet (C_{m_1... m_7}, \l^\alpha) to the dual version of N=1 supergravity (e_m{}^a, \psi_m{}^\alpha, M_{m_1... m_6}, \chi_\a,\Phi) in ten-dimensions. Our new 7-form field C has its 8-form field strength H dual to the 2-form field strength F of the conventional vector multiple... | 8.964898 | 8.417332 | 10.036361 | 7.514991 | 8.334407 | 8.469557 | 8.125234 | 7.651022 | 7.780195 | 10.460025 | 7.508034 | 7.906128 | 8.66506 | 7.719395 | 8.12619 | 8.012487 | 7.826438 | 8.30681 | 7.989671 | 8.562652 | 7.796616 |
hep-th/0206209 | Yu. M. Zinoviev | Yu. M. Zinoviev | Massive Spin-2 Supermultiplets | 23 pages, plain LaTeX, no figures | null | null | null | hep-th | null | In this paper we construct explicit Lagrangian formulation for the massive
spin-2 supermultiplets with N = k supersymmetries k = 1,2,3,4. Such multiplets
contain 2k particles with spin-3/2, so there must exist N = 2k local
supersymmetries in the full nonlinear theories spontaneously broken so that
only N = k global s... | [
{
"created": "Sun, 23 Jun 2002 16:22:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Zinoviev",
"Yu. M.",
""
]
] | In this paper we construct explicit Lagrangian formulation for the massive spin-2 supermultiplets with N = k supersymmetries k = 1,2,3,4. Such multiplets contain 2k particles with spin-3/2, so there must exist N = 2k local supersymmetries in the full nonlinear theories spontaneously broken so that only N = k global sup... | 9.912734 | 9.702766 | 10.645612 | 9.315141 | 10.11126 | 10.069043 | 9.850529 | 9.559849 | 9.361399 | 11.204897 | 9.682851 | 9.240902 | 9.881418 | 9.462329 | 9.608743 | 9.349092 | 9.457004 | 9.391314 | 9.778263 | 10.07253 | 9.453215 |
hep-th/9712152 | Sergei Ketov | Sergei V. Ketov (ITP, University of Hannover) | The hypermultiplet low-energy effective action, N=2 supersymmetry
breaking and confinement | 7 pages, LaTeX, macros included (Talk given at the 31st International
Ahrenshoop Symposium on the Theory of Elementary Particles, 2-6 September
1997, in Buckow, Germany, and the String Workshop, 14-15 November 1997, in
Wittenberg, Germany) | null | null | ITP-UH-34/97 | hep-th | null | Some exact solutions to the hypermultiplet low-energy effective action in N=2
supersymmetric four-dimensional gauge field theories with massive `quark'
hypermultiplets are discussed. The need for a spontaneous N=2 supersymmetry
breaking is emphasized, because of its possible relevance in the search for an
ultimate th... | [
{
"created": "Tue, 16 Dec 1997 13:26:26 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ketov",
"Sergei V.",
"",
"ITP, University of Hannover"
]
] | Some exact solutions to the hypermultiplet low-energy effective action in N=2 supersymmetric four-dimensional gauge field theories with massive `quark' hypermultiplets are discussed. The need for a spontaneous N=2 supersymmetry breaking is emphasized, because of its possible relevance in the search for an ultimate theo... | 14.027162 | 11.191734 | 12.761544 | 11.468461 | 11.377522 | 11.613813 | 11.307738 | 10.113235 | 11.149478 | 13.717984 | 10.847529 | 12.210208 | 11.865904 | 11.632252 | 11.719193 | 12.055644 | 11.531077 | 11.667173 | 11.875965 | 13.263455 | 11.2799 |
hep-th/0212326 | Namil Park | Yoonbai Kim, Chae Young Oh, Namil Park (Sungkyunkwan U.) | Classical Geometry of De Sitter Spacetime : An Introductory Review | 40 pages, 12 figures (ps or eps) | null | null | null | hep-th astro-ph gr-qc hep-ph | null | Classical geometry of de Sitter spacetime is reviewed in arbitrary
dimensions. Topics include coordinate systems, geodesic motions, and Penrose
diagrams with detailed calculations.
| [
{
"created": "Sun, 29 Dec 2002 16:48:50 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kim",
"Yoonbai",
"",
"Sungkyunkwan U."
],
[
"Oh",
"Chae Young",
"",
"Sungkyunkwan U."
],
[
"Park",
"Namil",
"",
"Sungkyunkwan U."
]
] | Classical geometry of de Sitter spacetime is reviewed in arbitrary dimensions. Topics include coordinate systems, geodesic motions, and Penrose diagrams with detailed calculations. | 18.110287 | 14.996536 | 11.25606 | 13.102205 | 10.705247 | 12.098521 | 11.827459 | 11.763784 | 14.769335 | 14.747343 | 12.767224 | 14.201543 | 13.164891 | 13.323136 | 13.704365 | 14.678477 | 13.465387 | 13.34607 | 13.863803 | 13.130354 | 13.345925 |
1312.1279 | Giampiero Esposito Dr. | Elisabetta Di Grezia, Giampiero Esposito, Patrizia Vitale | Self-dual road to noncommutative gravity with twist: a new analysis | 37 pages, Revtex. Appendix A is a recollection of mathematical tools
used in the paper. In the final version, Appendix C and some valuable
References have been added. arXiv admin note: text overlap with
arXiv:hep-th/0703014 by other authors. Misprints in Eq. (10.23) and (10.25)
have been amended, as well as the... | Phys.Rev. D89 (2014) 064039, Erratum-ibid. D90 (2014) 129901 | 10.1103/PhysRevD.89.064039 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The field equations of noncommutative gravity can be obtained by replacing
all exterior products by twist-deformed exterior products in the action
functional of general relativity, and are here studied by requiring that the
torsion 2-form should vanish, and that the Lorentz-Lie-algebra- valued part of
the full connec... | [
{
"created": "Wed, 4 Dec 2013 18:53:47 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Feb 2014 17:42:19 GMT",
"version": "v2"
},
{
"created": "Sat, 11 Oct 2014 14:54:14 GMT",
"version": "v3"
},
{
"created": "Sun, 23 Nov 2014 18:07:04 GMT",
"version": "v4"
}
] | 2015-06-18 | [
[
"Di Grezia",
"Elisabetta",
""
],
[
"Esposito",
"Giampiero",
""
],
[
"Vitale",
"Patrizia",
""
]
] | The field equations of noncommutative gravity can be obtained by replacing all exterior products by twist-deformed exterior products in the action functional of general relativity, and are here studied by requiring that the torsion 2-form should vanish, and that the Lorentz-Lie-algebra- valued part of the full connecti... | 11.234843 | 11.803558 | 11.708094 | 10.977348 | 12.012049 | 12.067618 | 11.802584 | 11.215617 | 10.880916 | 12.300844 | 11.218575 | 11.539424 | 11.097479 | 11.075021 | 10.829939 | 11.120019 | 11.223106 | 11.044643 | 10.985387 | 11.40308 | 10.876755 |
hep-th/9708052 | Elisha Atzmon | Yuval Ne'eman | A Superconnection for Riemannian Gravity as Spontaneously Broken SL(4,R)
Gauge Theory | 11 pages, latex | Phys.Lett.B427:19-25,1998 | 10.1016/S0370-2693(98)00326-8 | null | hep-th | null | A superconnection is a supermatrix whose even part contains the
gauge-potential one-forms of a local gauge group, while the odd parts contain
the (0-form) Higgs fields; the combined grading is thus odd everywhere. We
demonstrate that the simple supergroup ${\bar P}(4,R)$ (rank=3) in Kac'
classification (even subgroup... | [
{
"created": "Sun, 10 Aug 1997 11:09:30 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Ne'eman",
"Yuval",
""
]
] | A superconnection is a supermatrix whose even part contains the gauge-potential one-forms of a local gauge group, while the odd parts contain the (0-form) Higgs fields; the combined grading is thus odd everywhere. We demonstrate that the simple supergroup ${\bar P}(4,R)$ (rank=3) in Kac' classification (even subgroup $... | 18.909349 | 20.159328 | 22.223318 | 18.732187 | 21.303146 | 23.342888 | 19.264046 | 17.98307 | 22.086618 | 20.072321 | 19.102526 | 17.806284 | 17.062996 | 17.207502 | 17.611666 | 17.883167 | 18.482197 | 17.471153 | 17.222179 | 17.260664 | 16.571537 |
hep-th/0507062 | Olaf Lechtenfeld | Chong-Sun Chu, Olaf Lechtenfeld | Time-Space Noncommutative Abelian Solitons | 1+10 pages | Phys.Lett. B625 (2005) 145-155 | 10.1016/j.physletb.2005.08.054 | null | hep-th | null | We demonstrate the construction of solitons for a time-space Moyal-deformed
integrable U(n) sigma model (the Ward model) in 2+1 dimensions. These solitons
cannot travel parallel to the noncommutative spatial direction. For the U(1)
case, the rank-one single-soliton configuration is constructed explicitly and
is singu... | [
{
"created": "Wed, 6 Jul 2005 19:49:22 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Chu",
"Chong-Sun",
""
],
[
"Lechtenfeld",
"Olaf",
""
]
] | We demonstrate the construction of solitons for a time-space Moyal-deformed integrable U(n) sigma model (the Ward model) in 2+1 dimensions. These solitons cannot travel parallel to the noncommutative spatial direction. For the U(1) case, the rank-one single-soliton configuration is constructed explicitly and is singula... | 10.911934 | 9.917642 | 12.656895 | 9.930068 | 10.797478 | 10.950616 | 10.138891 | 10.082403 | 10.51436 | 15.087831 | 9.895418 | 10.503291 | 11.598995 | 10.488599 | 10.263931 | 10.497397 | 10.368044 | 10.515255 | 10.594145 | 11.407561 | 10.534916 |
1305.4777 | Krzysztof Andrzejewski | K. Andrzejewski, J. Gonera | Unitary representations of N-conformal Galilei group | References updated | null | 10.1103/PhysRevD.88.065011 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | All unitary irreducible representations of centrally extended (N-odd)
N-conformal Galilei group are constructed. The "on-shell" action of the group
is derived and shown to coincide, in special but most important case, with that
obtained in: J. Gomis, K. Kamimura, Phys. Rev. {\bf D85} (2012), 045023.
| [
{
"created": "Tue, 21 May 2013 10:31:25 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jun 2013 09:05:10 GMT",
"version": "v2"
}
] | 2013-09-18 | [
[
"Andrzejewski",
"K.",
""
],
[
"Gonera",
"J.",
""
]
] | All unitary irreducible representations of centrally extended (N-odd) N-conformal Galilei group are constructed. The "on-shell" action of the group is derived and shown to coincide, in special but most important case, with that obtained in: J. Gomis, K. Kamimura, Phys. Rev. {\bf D85} (2012), 045023. | 12.08281 | 10.059011 | 12.812481 | 9.591677 | 9.413758 | 9.578854 | 10.279916 | 8.694878 | 9.540074 | 11.563721 | 9.06765 | 9.19264 | 9.49089 | 8.496305 | 9.023308 | 8.418008 | 8.783357 | 9.140001 | 8.630664 | 10.153039 | 8.625857 |
0903.1353 | Amos Yarom | Amos Yarom | Fourth sound of holographic superfluids | 20 pages, 6 figures; removed a discussion on a variant of fourth
sound | JHEP 0907:070,2009 | 10.1088/1126-6708/2009/07/070 | PUPT-2293 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute fourth sound for superfluids dual to a charged scalar and a gauge
field in an AdS_4 background. For holographic superfluids with condensates that
have a large scaling dimension (greater than approximately two), we find that
fourth sound approaches first sound at low temperatures. For condensates that a
hav... | [
{
"created": "Mon, 9 Mar 2009 18:36:09 GMT",
"version": "v1"
},
{
"created": "Fri, 8 May 2009 13:57:26 GMT",
"version": "v2"
}
] | 2009-07-24 | [
[
"Yarom",
"Amos",
""
]
] | We compute fourth sound for superfluids dual to a charged scalar and a gauge field in an AdS_4 background. For holographic superfluids with condensates that have a large scaling dimension (greater than approximately two), we find that fourth sound approaches first sound at low temperatures. For condensates that a have ... | 9.254471 | 8.802378 | 10.447371 | 8.728351 | 8.565475 | 9.442161 | 9.090466 | 9.177407 | 8.67139 | 10.993892 | 8.21286 | 8.744324 | 8.776749 | 8.376579 | 8.436841 | 8.31937 | 8.191429 | 8.411616 | 8.35275 | 8.837215 | 8.22291 |
1902.01912 | Musema Sinamuli Mr | Musema Sinamuli and Robert B. Mann | Holographic Complexity and Charged Scalar Fields | 9 pages, 2 figures, typos corrected from earlier version, reference
added | Phys. Rev. D 99, 106013 (2019) | 10.1103/PhysRevD.99.106013 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a time-dependent expression of the computational complexity of a
quantum system which consists of two conformal complex scalar field theories in
d dimensions coupled to constant electric potentials and defined on the
boundaries of a charged AdS black hole in (d+1) dimensions. Using a suitable
choice of t... | [
{
"created": "Tue, 5 Feb 2019 21:18:23 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Feb 2019 17:39:43 GMT",
"version": "v2"
},
{
"created": "Fri, 10 May 2019 20:15:36 GMT",
"version": "v3"
},
{
"created": "Wed, 15 May 2019 01:18:28 GMT",
"version": "v4"
}
] | 2019-05-29 | [
[
"Sinamuli",
"Musema",
""
],
[
"Mann",
"Robert B.",
""
]
] | We construct a time-dependent expression of the computational complexity of a quantum system which consists of two conformal complex scalar field theories in d dimensions coupled to constant electric potentials and defined on the boundaries of a charged AdS black hole in (d+1) dimensions. Using a suitable choice of the... | 14.649725 | 13.362544 | 13.688831 | 12.174773 | 12.195257 | 12.948261 | 13.302004 | 11.945494 | 12.316024 | 13.886503 | 13.089062 | 12.913038 | 13.536341 | 12.545047 | 12.148651 | 12.39524 | 12.478824 | 12.502838 | 12.595943 | 13.593384 | 12.858069 |
1710.11235 | Yi-Nan Wang | Washington Taylor, Yi-Nan Wang | Scanning the skeleton of the 4D F-theory landscape | 41 pages, 12 figures | null | 10.1007/JHEP01(2018)111 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using a one-way Monte Carlo algorithm from several different starting points,
we get an approximation to the distribution of toric threefold bases that can
be used in four-dimensional F-theory compactification. We separate the
threefold bases into "resolvable" ones where the Weierstrass polynomials
$(f,g)$ can vanish... | [
{
"created": "Mon, 30 Oct 2017 20:51:23 GMT",
"version": "v1"
}
] | 2018-03-14 | [
[
"Taylor",
"Washington",
""
],
[
"Wang",
"Yi-Nan",
""
]
] | Using a one-way Monte Carlo algorithm from several different starting points, we get an approximation to the distribution of toric threefold bases that can be used in four-dimensional F-theory compactification. We separate the threefold bases into "resolvable" ones where the Weierstrass polynomials $(f,g)$ can vanish t... | 8.901081 | 9.5005 | 10.355281 | 9.022759 | 9.986157 | 9.952543 | 9.524309 | 9.208669 | 9.112075 | 11.558191 | 8.845311 | 8.569363 | 9.140681 | 8.762012 | 8.621996 | 8.900975 | 8.726338 | 8.873032 | 8.697392 | 9.216971 | 8.630892 |
1010.4302 | Bartosz Fornal | Jonathan M. Arnold, Bartosz Fornal, Mark B. Wise | Standard Model Vacua for Two-dimensional Compactifications | 7 pages, 2 figures; v2: published in JHEP | JHEP 1012:083,2010 | 10.1007/JHEP12(2010)083 | CALT 68-2805 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the structure of lower-dimensional standard model vacua for
two-dimensional compactifications (on a 2D torus and on a 2D sphere). In the
case of the torus we find a new standard model vacuum for a large range of
neutrino masses consistent with experiment. Quantum effects play a crucial role
in the existenc... | [
{
"created": "Wed, 20 Oct 2010 20:00:01 GMT",
"version": "v1"
},
{
"created": "Sat, 1 Jan 2011 21:00:01 GMT",
"version": "v2"
}
] | 2011-01-04 | [
[
"Arnold",
"Jonathan M.",
""
],
[
"Fornal",
"Bartosz",
""
],
[
"Wise",
"Mark B.",
""
]
] | We examine the structure of lower-dimensional standard model vacua for two-dimensional compactifications (on a 2D torus and on a 2D sphere). In the case of the torus we find a new standard model vacuum for a large range of neutrino masses consistent with experiment. Quantum effects play a crucial role in the existence ... | 8.859668 | 8.68683 | 8.481127 | 8.334748 | 9.079483 | 8.7196 | 8.372263 | 8.673018 | 8.477362 | 8.690227 | 8.711294 | 8.56644 | 8.737874 | 8.820935 | 8.711259 | 8.80164 | 8.544512 | 8.649296 | 8.665545 | 8.52993 | 8.733544 |
1408.0655 | Changhyun Ahn | Changhyun Ahn | Higher Spin Currents in Wolf Space: Part II | 176 pages | null | 10.1088/0264-9381/32/1/015023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The 16 lowest higher spin currents of spins (1, 3/2, 3/2, 2), (3/2, 2, 2, 5/2
), (3/2, 2, 2, 5/2) and (2, 5/2, 5/2, 3) in terms of N=2 WZW affine currents
were obtained in the N=4 superconformal Wolf space coset SU(5)/[SU(3) x SU(2) x
U(1)] previously. By calculating the operator product expansions (OPEs) between
the... | [
{
"created": "Mon, 4 Aug 2014 12:17:04 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Ahn",
"Changhyun",
""
]
] | The 16 lowest higher spin currents of spins (1, 3/2, 3/2, 2), (3/2, 2, 2, 5/2 ), (3/2, 2, 2, 5/2) and (2, 5/2, 5/2, 3) in terms of N=2 WZW affine currents were obtained in the N=4 superconformal Wolf space coset SU(5)/[SU(3) x SU(2) x U(1)] previously. By calculating the operator product expansions (OPEs) between the a... | 4.098927 | 3.312531 | 4.519521 | 3.476413 | 3.827031 | 3.499605 | 3.541229 | 3.301696 | 3.561471 | 4.695261 | 3.448887 | 3.635606 | 4.140671 | 3.739165 | 3.806414 | 3.716236 | 3.738216 | 3.691703 | 3.698753 | 4.149967 | 3.745549 |
1906.10894 | Yusef Maleki | Yusef Maleki and Alireza Maleki | Speed limit of quantum dynamics near the event horizon of black holes | 6 pages, 5 figures | null | 10.1016/j.physletb.2020.135700 | null | hep-th gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum mechanics imposes a fundamental bound on the minimum time required
for the quantum systems to evolve between two states of interest. This bound
introduces a limit on the speed of the dynamical evolution of the systems,
known as the quantum speed limit. We show that black holes can drastically
affect the speed... | [
{
"created": "Wed, 26 Jun 2019 07:54:11 GMT",
"version": "v1"
}
] | 2020-08-19 | [
[
"Maleki",
"Yusef",
""
],
[
"Maleki",
"Alireza",
""
]
] | Quantum mechanics imposes a fundamental bound on the minimum time required for the quantum systems to evolve between two states of interest. This bound introduces a limit on the speed of the dynamical evolution of the systems, known as the quantum speed limit. We show that black holes can drastically affect the speed l... | 8.96516 | 9.089443 | 8.216847 | 8.261065 | 9.464208 | 10.205741 | 9.417368 | 9.384627 | 8.166323 | 7.60439 | 9.367076 | 8.838394 | 8.542552 | 8.464127 | 9.047415 | 8.695565 | 8.774435 | 8.557766 | 8.893447 | 8.446563 | 8.906316 |
hep-th/0508244 | Danilo Mauro | P. Carta, E. Gozzi, D. Mauro | Koopman-von Neumann Formulation of Classical Yang-Mills Theories: I | 46 pages, Latex | Annalen Phys. 15 (2006) 177-215 | 10.1002/andp.200510177 | null | hep-th | null | In this paper we present the Koopman-von Neumann (KvN) formulation of
classical non-Abelian gauge field theories. In particular we shall explore the
functional (or classical path integral) counterpart of the KvN method. In the
quantum path integral quantization of Yang-Mills theories concepts like
gauge-fixing and Fa... | [
{
"created": "Wed, 31 Aug 2005 13:14:42 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Carta",
"P.",
""
],
[
"Gozzi",
"E.",
""
],
[
"Mauro",
"D.",
""
]
] | In this paper we present the Koopman-von Neumann (KvN) formulation of classical non-Abelian gauge field theories. In particular we shall explore the functional (or classical path integral) counterpart of the KvN method. In the quantum path integral quantization of Yang-Mills theories concepts like gauge-fixing and Fadd... | 11.261545 | 11.299932 | 11.253062 | 10.467904 | 10.516828 | 10.083656 | 10.283964 | 10.01895 | 9.823262 | 11.773158 | 10.53421 | 9.678833 | 10.451963 | 10.387636 | 10.077903 | 10.240593 | 10.482262 | 10.155099 | 10.19459 | 10.726678 | 10.620968 |
hep-th/0608224 | Shankaranarayanan S | L. Sriramkumar (HRI, Allahabad), S. Shankaranarayanan (ICTP, Trieste;
AEI, Golm) | Path integral duality and Planck scale corrections to the primordial
spectrum in exponential inflation | 12 pages, 1 figure, RevTex4 format | JHEP 0612:050,2006 | 10.1088/1126-6708/2006/12/050 | AEI-2006-069 | hep-th astro-ph gr-qc | null | The enormous red-shifting of the modes during the inflationary epoch suggests
that physics at the Planck scale may modify the standard, nearly,
scale-invariant, primordial, density perturbation spectrum. Under the principle
of path-integral duality, the space-time behaves as though it has a minimal
length $L_{_{\rm P... | [
{
"created": "Thu, 31 Aug 2006 13:19:17 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Sriramkumar",
"L.",
"",
"HRI, Allahabad"
],
[
"Shankaranarayanan",
"S.",
"",
"ICTP, Trieste;\n AEI, Golm"
]
] | The enormous red-shifting of the modes during the inflationary epoch suggests that physics at the Planck scale may modify the standard, nearly, scale-invariant, primordial, density perturbation spectrum. Under the principle of path-integral duality, the space-time behaves as though it has a minimal length $L_{_{\rm P}}... | 6.737144 | 6.649639 | 6.813396 | 6.508198 | 6.81987 | 6.31111 | 7.236337 | 6.026709 | 6.329884 | 7.03901 | 6.325479 | 6.587875 | 6.508918 | 6.47234 | 6.53374 | 6.633651 | 6.50649 | 6.364658 | 6.552921 | 6.547051 | 6.532489 |
hep-th/0411232 | Stefano Bellucci | S. Bellucci, A.V. Galajinsky, E. Latini | New insight into WDVV equation | 16 pages, no figures, LaTeX file, PACS: 04.60.Ds; 11.30.Pb | Phys.Rev. D71 (2005) 044023 | 10.1103/PhysRevD.71.044023 | null | hep-th | null | We show that Witten-Dijkgraaf-Verlinde-Verlinde equation underlies the
construction of N=4 superconformal multi--particle mechanics in one dimension,
including a N=4 superconformal Calogero model.
| [
{
"created": "Thu, 25 Nov 2004 10:02:46 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Bellucci",
"S.",
""
],
[
"Galajinsky",
"A. V.",
""
],
[
"Latini",
"E.",
""
]
] | We show that Witten-Dijkgraaf-Verlinde-Verlinde equation underlies the construction of N=4 superconformal multi--particle mechanics in one dimension, including a N=4 superconformal Calogero model. | 7.874284 | 6.413802 | 9.415037 | 7.22029 | 6.557975 | 6.592013 | 6.683278 | 6.718185 | 7.12199 | 11.487423 | 6.493873 | 7.248134 | 8.080518 | 7.242161 | 6.656676 | 6.611466 | 6.514243 | 6.773516 | 7.293733 | 8.04487 | 6.601674 |
hep-th/0603026 | Lorenzo Sorbo | Marco Peloso, Lorenzo Sorbo, Gianmassimo Tasinato | Standard 4d gravity on a brane in six dimensional flux compactifications | 24 pages, 1 figure; corrected typos, added references; final version | Phys.Rev.D73:104025,2006 | 10.1103/PhysRevD.73.104025 | null | hep-th gr-qc hep-ph | null | We consider a six dimensional space-time, in which two of the dimensions are
compactified by a flux. Matter can be localized on a codimension one brane
coupled to the bulk gauge field and wrapped around an axis of symmetry of the
internal space. By studying the linear perturbations around this background, we
show tha... | [
{
"created": "Sun, 5 Mar 2006 18:31:01 GMT",
"version": "v1"
},
{
"created": "Mon, 22 May 2006 12:26:17 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Peloso",
"Marco",
""
],
[
"Sorbo",
"Lorenzo",
""
],
[
"Tasinato",
"Gianmassimo",
""
]
] | We consider a six dimensional space-time, in which two of the dimensions are compactified by a flux. Matter can be localized on a codimension one brane coupled to the bulk gauge field and wrapped around an axis of symmetry of the internal space. By studying the linear perturbations around this background, we show that ... | 8.568112 | 7.554408 | 9.159328 | 8.065088 | 8.368736 | 7.930005 | 8.202003 | 8.663513 | 7.841965 | 9.462053 | 7.716593 | 8.117809 | 8.505791 | 8.218705 | 8.539929 | 8.356116 | 8.407521 | 8.235865 | 8.031346 | 8.16258 | 7.94434 |
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