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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1403.4664 | Alexander Kovner | Ibrahim B. Ilhan and Alex Kovner | Conformal Gravity Redux: Ghost-turned-Tachyon | 10 pages | Phys. Rev. D 89, 104015 (2014) | 10.1103/PhysRevD.89.104015 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze conformal gravity in translationally invariant approximation,
where the metric is taken to depend on time but not on spatial coordinates. We
find that the field mode which in perturbation theory has a ghostlike kinetic
term, turns into a tachyon when nonlinear interaction is accounted for. The
kinetic term... | [
{
"created": "Wed, 19 Mar 2014 01:58:13 GMT",
"version": "v1"
}
] | 2014-05-14 | [
[
"Ilhan",
"Ibrahim B.",
""
],
[
"Kovner",
"Alex",
""
]
] | We analyze conformal gravity in translationally invariant approximation, where the metric is taken to depend on time but not on spatial coordinates. We find that the field mode which in perturbation theory has a ghostlike kinetic term, turns into a tachyon when nonlinear interaction is accounted for. The kinetic term a... | 12.028389 | 11.559536 | 12.000552 | 12.181794 | 12.252062 | 12.199108 | 11.411249 | 11.26324 | 10.833756 | 11.09857 | 10.590117 | 11.188441 | 11.644381 | 11.406846 | 10.990343 | 10.92788 | 11.530764 | 11.471644 | 11.320292 | 11.718167 | 10.865985 |
hep-th/0701082 | Justin F. Vazquez-Poritz | W. Chen, M. Cvetic, H. Lu, C.N. Pope, J.F. Vazquez-Poritz | Resolved Calabi-Yau Cones and Flows from L^{abc} Superconformal Field
Theories | 35 pages, 2 figures, additional comments and references | Nucl.Phys.B785:74-97,2007 | 10.1016/j.nuclphysb.2007.06.018 | null | hep-th | null | We discuss D3-branes on cohomogeneity-three resolved Calabi-Yau cones over
L^{abc} spaces, for which a 2-cycle or 4-cycle has been blown up. In terms of
the dual quiver gauge theory, this corresponds to motion along the non-mesonic,
or baryonic, directions in the moduli space of vacua. In particular, a
dimension-two ... | [
{
"created": "Tue, 9 Jan 2007 21:12:58 GMT",
"version": "v1"
},
{
"created": "Mon, 28 May 2007 20:31:04 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Chen",
"W.",
""
],
[
"Cvetic",
"M.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Vazquez-Poritz",
"J. F.",
""
]
] | We discuss D3-branes on cohomogeneity-three resolved Calabi-Yau cones over L^{abc} spaces, for which a 2-cycle or 4-cycle has been blown up. In terms of the dual quiver gauge theory, this corresponds to motion along the non-mesonic, or baryonic, directions in the moduli space of vacua. In particular, a dimension-two an... | 11.228584 | 11.305107 | 13.978959 | 11.255924 | 11.558037 | 12.024069 | 11.629921 | 12.046969 | 10.907808 | 14.588972 | 10.847214 | 10.496707 | 11.89894 | 11.15243 | 10.633089 | 11.204025 | 11.190149 | 10.999165 | 10.925362 | 12.439749 | 10.693173 |
1101.0120 | Raffaele Marotta | P. Di Vecchia, R. Marotta, I. Pesando and F. Pezzella | Open strings in the system D5/D9 | 54 pages, Latex | null | 10.1088/1751-8113/44/24/245401 | DFTT/9/2010, NORDITA-2010-115 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the six-dimensional Lagrangian for the massless twisted open
strings with one end-point ending on a stack of D5 and the other on a stack of
D9 branes, interacting with the gauge multiplets living respectively on the D5
and D9 branes. It is first obtained by uplifting to six dimensions the
four-dimensiona... | [
{
"created": "Thu, 30 Dec 2010 17:51:39 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Di Vecchia",
"P.",
""
],
[
"Marotta",
"R.",
""
],
[
"Pesando",
"I.",
""
],
[
"Pezzella",
"F.",
""
]
] | We construct the six-dimensional Lagrangian for the massless twisted open strings with one end-point ending on a stack of D5 and the other on a stack of D9 branes, interacting with the gauge multiplets living respectively on the D5 and D9 branes. It is first obtained by uplifting to six dimensions the four-dimensional ... | 7.451776 | 7.293005 | 7.7223 | 7.078547 | 7.190785 | 6.979824 | 7.116432 | 7.344557 | 7.053852 | 8.151616 | 6.995601 | 6.909397 | 7.078842 | 6.972347 | 7.044525 | 7.140422 | 6.951318 | 6.874733 | 7.050077 | 7.12339 | 6.958146 |
2306.04687 | Alessandro Dondarini | Alessandro Dondarini | Causality Bounds in Quadratic Inflation from Purely Virtual Particles | null | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The "$\phi^2$" slow roll inflation combined with General Relativity is
largely excluded by Planck data. In this paper, we consider the same potential
combined with the $R+C^2$ gravity of purely virtual particles (or fakeons),
where the would-be ghost introduced by the Weyl tensor term, $C^2$, is
quantized with the fa... | [
{
"created": "Wed, 7 Jun 2023 18:00:04 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Oct 2023 15:53:05 GMT",
"version": "v2"
}
] | 2023-10-23 | [
[
"Dondarini",
"Alessandro",
""
]
] | The "$\phi^2$" slow roll inflation combined with General Relativity is largely excluded by Planck data. In this paper, we consider the same potential combined with the $R+C^2$ gravity of purely virtual particles (or fakeons), where the would-be ghost introduced by the Weyl tensor term, $C^2$, is quantized with the fake... | 17.579538 | 16.259474 | 13.666767 | 12.644727 | 14.377075 | 14.736443 | 14.993716 | 12.864929 | 13.359567 | 15.239519 | 13.960756 | 15.344999 | 13.292902 | 14.52422 | 14.485231 | 15.299501 | 16.436943 | 15.24485 | 13.998713 | 13.590143 | 15.573609 |
1004.5388 | Eric R. Sharpe | E. Sharpe | GLSM's, gerbes, and Kuznetsov's homological projective duality | LaTeX, 8 pages, contribution to the proceedings of Quantum Theory and
Symmetries 6 (Lexington, Kentucky, July 2009) | null | null | VT-IPNAS 10-04 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this short note we give an overview of recent work on string propagation
on stacks and applications to gauged linear sigma models. We begin by outlining
noneffective orbifolds (orbifolds in which a subgroup acts trivially) and
related phenomena in two-dimensional gauge theories, which realize string
propagation on... | [
{
"created": "Thu, 29 Apr 2010 20:17:31 GMT",
"version": "v1"
}
] | 2010-05-03 | [
[
"Sharpe",
"E.",
""
]
] | In this short note we give an overview of recent work on string propagation on stacks and applications to gauged linear sigma models. We begin by outlining noneffective orbifolds (orbifolds in which a subgroup acts trivially) and related phenomena in two-dimensional gauge theories, which realize string propagation on g... | 10.201892 | 11.255542 | 13.547302 | 10.30938 | 10.65874 | 10.736457 | 11.610633 | 10.3711 | 9.99123 | 13.936834 | 10.393854 | 10.352518 | 10.788107 | 10.074893 | 10.582533 | 10.250572 | 10.527813 | 10.17211 | 9.977828 | 11.258118 | 10.052568 |
2010.11192 | Cheng Peng | Cheng Peng | Ensemble averages, Poisson processes and Microstates | 36 pages, 2 figures | Phys. Rev. D 103, 061901 (2021) | 10.1103/PhysRevD.103.L061901 | null | hep-th cond-mat.dis-nn math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider ensemble averaged theories with discrete random variables. We
propose a suitable measure to do the ensemble average. We also provide a
mathematical description of such ensemble averages of theories in terms of
Poisson point processes. Moreover, we demonstrate that averaging theories of
this type has an eq... | [
{
"created": "Wed, 21 Oct 2020 18:00:00 GMT",
"version": "v1"
}
] | 2021-03-31 | [
[
"Peng",
"Cheng",
""
]
] | We consider ensemble averaged theories with discrete random variables. We propose a suitable measure to do the ensemble average. We also provide a mathematical description of such ensemble averages of theories in terms of Poisson point processes. Moreover, we demonstrate that averaging theories of this type has an equi... | 23.281794 | 22.110437 | 21.948605 | 21.096851 | 22.283319 | 22.263681 | 22.042351 | 20.36738 | 20.977589 | 26.330755 | 19.376787 | 21.267117 | 20.457766 | 20.324644 | 20.31568 | 20.958651 | 21.225462 | 21.14418 | 20.576681 | 21.397474 | 20.952526 |
0711.4878 | Raphael Flauger | Elena Caceres, Raphael Flauger, Matthias Ihl, Timm Wrase | New Supergravity Backgrounds Dual to N=1 SQCD-like Theories with
N_f=2N_c | 22+24 pages, 17 figures, Figure 12 replaced | JHEP 0803:020,2008 | 10.1088/1126-6708/2008/03/020 | UTTG-09-07 | hep-th | null | We present new supergravity backgrounds generated by N_c D5-branes, wrapping
the S^2 of the resolved conifold, in the presence of N_f = 2 N_c smeared flavor
D5-branes. The smearing allows us to take their backreaction on the geometry
into account. We discuss the consistency, stability, and supersymmetry of these
type... | [
{
"created": "Fri, 30 Nov 2007 06:31:15 GMT",
"version": "v1"
},
{
"created": "Sat, 1 Dec 2007 23:25:08 GMT",
"version": "v2"
}
] | 2009-11-19 | [
[
"Caceres",
"Elena",
""
],
[
"Flauger",
"Raphael",
""
],
[
"Ihl",
"Matthias",
""
],
[
"Wrase",
"Timm",
""
]
] | We present new supergravity backgrounds generated by N_c D5-branes, wrapping the S^2 of the resolved conifold, in the presence of N_f = 2 N_c smeared flavor D5-branes. The smearing allows us to take their backreaction on the geometry into account. We discuss the consistency, stability, and supersymmetry of these types ... | 9.961736 | 8.806276 | 11.003707 | 8.840524 | 9.282603 | 9.288167 | 8.540062 | 9.257082 | 8.606577 | 11.810248 | 8.544001 | 9.33594 | 10.384336 | 9.648057 | 9.774618 | 9.420853 | 9.620411 | 9.707369 | 9.62762 | 10.583986 | 9.435369 |
0707.0424 | Linda I. Uruchurtu | Linda I. Uruchurtu | AdS/CFT for Four-Point Amplitudes involving Gravitino Exchange | 32 pages, 1 figure. Published Version. Minor changes | JHEP0709:086,2007 | 10.1088/1126-6708/2007/09/086 | DAMTP-2007-65 | hep-th | null | In this paper we compute the tree-level four-point scattering amplitude of
two dilatini and two axion-dilaton fields in type IIB supergravity in AdS5 x
S5. A special feature of this process is that there is an "exotic" channel in
which there are no singleparticle poles. Another novelty is that this process
involves t... | [
{
"created": "Tue, 3 Jul 2007 14:28:26 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Aug 2007 12:38:39 GMT",
"version": "v2"
},
{
"created": "Fri, 14 Dec 2007 10:06:50 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Uruchurtu",
"Linda I.",
""
]
] | In this paper we compute the tree-level four-point scattering amplitude of two dilatini and two axion-dilaton fields in type IIB supergravity in AdS5 x S5. A special feature of this process is that there is an "exotic" channel in which there are no singleparticle poles. Another novelty is that this process involves the... | 7.514711 | 7.928432 | 8.287204 | 7.115685 | 7.957596 | 7.473906 | 7.110052 | 7.511631 | 6.970365 | 9.16332 | 7.202035 | 7.143604 | 7.258574 | 6.827519 | 6.977986 | 7.154068 | 6.968175 | 7.110136 | 7.005641 | 7.180364 | 6.958946 |
1406.6389 | Tomas Andrade | Tomas Andrade, Yang Lei, Simon F. Ross | Scattering amplitudes in Lifshitz spacetime | 14 pages, 8 figures | null | 10.1088/0264-9381/31/21/215002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the calculation of scattering amplitudes in field theories dual
to Lifshitz spacetimes. These amplitudes provide an interesting probe of the IR
structure of the field theory; our aim is to use them to explore the observable
consequences of the singularity in the spacetime. We assume the amplitudes can
be ... | [
{
"created": "Tue, 24 Jun 2014 20:47:06 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Andrade",
"Tomas",
""
],
[
"Lei",
"Yang",
""
],
[
"Ross",
"Simon F.",
""
]
] | We consider the calculation of scattering amplitudes in field theories dual to Lifshitz spacetimes. These amplitudes provide an interesting probe of the IR structure of the field theory; our aim is to use them to explore the observable consequences of the singularity in the spacetime. We assume the amplitudes can be re... | 9.027157 | 8.338373 | 9.80317 | 8.559893 | 8.855049 | 8.824429 | 8.371724 | 8.322142 | 8.176291 | 9.698727 | 7.94103 | 8.409163 | 9.140388 | 8.105237 | 8.122962 | 8.246013 | 8.339157 | 8.461804 | 8.137197 | 9.016822 | 8.041865 |
hep-th/0201198 | Boris Noyvert | Boris Noyvert (Weizmann Institute) | Unitary minimal models of SW(3/2,3/2,2) superconformal algebra and
manifolds of G_2 holonomy | 34 pages, 2 figures, latex; v2: added examples in appendix D; v3:
published version, corrected typos | JHEP 0203 (2002) 030 | 10.1088/1126-6708/2002/03/030 | WIS/06/02-JAN-DPP | hep-th math-ph math.MP | null | The SW(3/2,3/2,2) superconformal algebra is a W algebra with two free
parameters. It consists of 3 superconformal currents of spins 3/2, 3/2 and 2.
The algebra is proved to be the symmetry algebra of the coset
(su(2)+su(2)+su(2))/su(2). At the central charge c=21/2 the algebra coincides
with the superconformal algebr... | [
{
"created": "Thu, 24 Jan 2002 20:45:30 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Feb 2002 14:46:37 GMT",
"version": "v2"
},
{
"created": "Mon, 1 Apr 2002 10:50:30 GMT",
"version": "v3"
}
] | 2009-01-20 | [
[
"Noyvert",
"Boris",
"",
"Weizmann Institute"
]
] | The SW(3/2,3/2,2) superconformal algebra is a W algebra with two free parameters. It consists of 3 superconformal currents of spins 3/2, 3/2 and 2. The algebra is proved to be the symmetry algebra of the coset (su(2)+su(2)+su(2))/su(2). At the central charge c=21/2 the algebra coincides with the superconformal algebra ... | 4.995366 | 4.295159 | 6.074671 | 4.377934 | 4.269298 | 4.311814 | 4.579751 | 4.348479 | 4.181942 | 5.86825 | 4.618481 | 4.718355 | 5.251858 | 4.64057 | 4.670889 | 4.658562 | 4.661545 | 4.675761 | 4.600701 | 5.181708 | 4.564385 |
1604.07263 | Sergio Gonz\'alez Mart\'in | Enrique \'Alvarez, Sergio Gonz\'alez-Mart\'in, Carmelo P. Mart\'in | A note on the Gauge Symmetries of Unimodular Gravity | 4 pages, v2: acknowledgments corrected | Phys. Rev. D 93, 123018 (2016) | 10.1103/PhysRevD.93.123018 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The symmetries of Unimodular Gravity are clarified somewhat.
| [
{
"created": "Mon, 25 Apr 2016 14:00:01 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Apr 2016 15:10:46 GMT",
"version": "v2"
}
] | 2018-02-15 | [
[
"Álvarez",
"Enrique",
""
],
[
"González-Martín",
"Sergio",
""
],
[
"Martín",
"Carmelo P.",
""
]
] | The symmetries of Unimodular Gravity are clarified somewhat. | 62.375824 | 19.15094 | 22.517067 | 18.966955 | 18.687252 | 19.914442 | 21.549303 | 21.143499 | 19.402985 | 26.212473 | 22.189674 | 26.665846 | 35.978115 | 28.206861 | 27.271473 | 27.045893 | 28.263786 | 27.399969 | 31.451014 | 34.05542 | 27.222172 |
1505.03119 | Alessandro Codello | Alessandro Codello, Roberto Percacci, Leslaw Rachwal and Alberto
Tonero | Computing the Effective Action with the Functional Renormalization Group | 40 pages | null | 10.1140/epjc/s10052-016-4063-3 | CP^3-Origins-2015-18 DNRF90 & DIAS-2015-18 | hep-th gr-qc hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The "exact" or "functional" renormalization group equation describes the
renormalization group flow of the effective average action $\Gamma_k$. The
ordinary effective action $\Gamma_0$ can be obtained by integrating the flow
equation from an ultraviolet scale $k=\Lambda$ down to $k=0$. We give several
examples of suc... | [
{
"created": "Tue, 12 May 2015 18:59:27 GMT",
"version": "v1"
}
] | 2016-05-25 | [
[
"Codello",
"Alessandro",
""
],
[
"Percacci",
"Roberto",
""
],
[
"Rachwal",
"Leslaw",
""
],
[
"Tonero",
"Alberto",
""
]
] | The "exact" or "functional" renormalization group equation describes the renormalization group flow of the effective average action $\Gamma_k$. The ordinary effective action $\Gamma_0$ can be obtained by integrating the flow equation from an ultraviolet scale $k=\Lambda$ down to $k=0$. We give several examples of such ... | 4.977189 | 5.83519 | 5.944695 | 4.855462 | 5.552998 | 5.982822 | 5.7778 | 5.883027 | 5.388504 | 6.5175 | 5.274114 | 5.245982 | 4.933173 | 5.020873 | 4.967109 | 5.141456 | 5.264488 | 5.11684 | 4.928657 | 5.085841 | 4.936014 |
1307.2221 | Kewang Jin | Matthias R. Gaberdiel, Kewang Jin, Eric Perlmutter | Probing higher spin black holes from CFT | 34 pages, 1 figure | JHEP 1310:045,2013 | 10.1007/JHEP10(2013)045 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a class of 2D CFTs with higher spin symmetry, we compute thermal two-point
functions of certain scalar primary operators in the presence of nonzero
chemical potential for higher spin charge. These are shown to agree with the
same quantity calculated holographically using scalar fields propagating in a
charged blac... | [
{
"created": "Mon, 8 Jul 2013 19:50:36 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Jin",
"Kewang",
""
],
[
"Perlmutter",
"Eric",
""
]
] | In a class of 2D CFTs with higher spin symmetry, we compute thermal two-point functions of certain scalar primary operators in the presence of nonzero chemical potential for higher spin charge. These are shown to agree with the same quantity calculated holographically using scalar fields propagating in a charged black ... | 7.333544 | 5.679958 | 8.081898 | 5.798433 | 6.060151 | 5.682731 | 5.621416 | 5.64348 | 5.897329 | 8.764298 | 5.835219 | 6.062963 | 6.817654 | 6.267712 | 6.017027 | 6.020008 | 6.063262 | 6.201873 | 6.152103 | 6.673495 | 6.183984 |
0906.2430 | Guglielmo Fucci Dr. | Guglielmo Fucci | Non-Perturbative One-Loop Effective Action for Electrodynamics in Curved
Spacetime | LaTeX, 23 pages | J. Math. Phys 50, 102301 (2009) | 10.1063/1.3231787 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we explicitly evaluate the one-loop effective action in four
dimensions for scalar and spinor fields under the influence of a strong,
covariantly constant, magnetic field in curved spacetime. In the framework of
zeta function regularization, we find the one-loop effective action to all
orders in the mag... | [
{
"created": "Fri, 12 Jun 2009 21:51:08 GMT",
"version": "v1"
}
] | 2009-10-02 | [
[
"Fucci",
"Guglielmo",
""
]
] | In this paper we explicitly evaluate the one-loop effective action in four dimensions for scalar and spinor fields under the influence of a strong, covariantly constant, magnetic field in curved spacetime. In the framework of zeta function regularization, we find the one-loop effective action to all orders in the magne... | 8.1557 | 6.456679 | 7.525825 | 7.214591 | 7.51919 | 8.022635 | 7.274843 | 6.791831 | 7.308095 | 8.311412 | 7.079962 | 7.436114 | 7.747869 | 7.381165 | 7.44462 | 7.477783 | 7.442377 | 7.215561 | 7.405375 | 7.836112 | 7.282149 |
1507.04053 | Lilia Anguelova | Lilia Anguelova, Peter Suranyi, L.C. Rohana Wijewardhana | Toward a Gravity Dual of Glueball Inflation | 11 pages, contribution to the proceedings of the memorial "Matey
Mateev Symposium", Sofia, April 2015 | Bulg. J. Phys. 42 (2015) 277 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We summarize and extend our work on nonsupersymmetric solutions of a 5d
consistent truncation of type IIB supergravity, that is relevant for
gauge/gravity duality. The fields in this 5d theory are the five-dimensional
metric and a set of scalars. We find solutions of the 5d equations of motion,
which represent dS_4 f... | [
{
"created": "Wed, 15 Jul 2015 00:04:28 GMT",
"version": "v1"
}
] | 2016-01-08 | [
[
"Anguelova",
"Lilia",
""
],
[
"Suranyi",
"Peter",
""
],
[
"Wijewardhana",
"L. C. Rohana",
""
]
] | We summarize and extend our work on nonsupersymmetric solutions of a 5d consistent truncation of type IIB supergravity, that is relevant for gauge/gravity duality. The fields in this 5d theory are the five-dimensional metric and a set of scalars. We find solutions of the 5d equations of motion, which represent dS_4 fol... | 8.084943 | 6.6434 | 8.3894 | 7.46627 | 7.447073 | 6.9983 | 7.467431 | 7.152946 | 7.182443 | 9.080959 | 7.055436 | 7.360881 | 7.570332 | 7.235001 | 7.675471 | 7.526648 | 7.375385 | 7.612754 | 7.180774 | 7.787269 | 7.327445 |
2110.08276 | Pieter Bomans | Pieter Bomans, Davide Cassani, Giuseppe Dibitetto and Nicolo Petri | Bubble instability of mIIA on $\mathrm{AdS}_4\times S^6$ | 27 pages, 6 figures. Published version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider compactifications of massive IIA supergravity on a six-sphere.
This setup is known to give rise to non-supersymmetric AdS$_4$ vacua preserving
SO$(7)$ as well as G$_2$ residual symmetry. Both solutions have a round $S^6$
metric and are supported by the Romans' mass and internal $F_6$ flux. While the
SO$(7... | [
{
"created": "Fri, 15 Oct 2021 18:00:01 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Apr 2022 10:22:30 GMT",
"version": "v2"
}
] | 2022-04-06 | [
[
"Bomans",
"Pieter",
""
],
[
"Cassani",
"Davide",
""
],
[
"Dibitetto",
"Giuseppe",
""
],
[
"Petri",
"Nicolo",
""
]
] | We consider compactifications of massive IIA supergravity on a six-sphere. This setup is known to give rise to non-supersymmetric AdS$_4$ vacua preserving SO$(7)$ as well as G$_2$ residual symmetry. Both solutions have a round $S^6$ metric and are supported by the Romans' mass and internal $F_6$ flux. While the SO$(7)$... | 6.948184 | 5.800689 | 7.718473 | 6.002466 | 6.151967 | 6.250507 | 6.079886 | 6.007042 | 5.977247 | 7.43424 | 6.18952 | 6.300733 | 6.905267 | 6.330116 | 6.34468 | 6.35181 | 6.500544 | 6.55045 | 6.269936 | 6.896438 | 6.389477 |
1804.03834 | Tim Morris Prof | Tim R. Morris | Perturbatively renormalizable quantum gravity | 5 pages; Received Honourable mention in Gravity Research Foundation
essay competition-2018 | Int.J.Mod.Phys. D27 (2018) 1847003 | 10.1142/S021827181847003X | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Wilsonian renormalization group (RG) requires Euclidean signature. The
conformal factor of the metric then has a wrong-sign kinetic term, which has a
profound effect on its RG properties. In particular around the Gaussian fixed
point, it supports a Hilbert space of renormalizable interactions involving
arbitraril... | [
{
"created": "Wed, 11 Apr 2018 06:52:42 GMT",
"version": "v1"
},
{
"created": "Wed, 16 May 2018 12:09:20 GMT",
"version": "v2"
}
] | 2018-12-04 | [
[
"Morris",
"Tim R.",
""
]
] | The Wilsonian renormalization group (RG) requires Euclidean signature. The conformal factor of the metric then has a wrong-sign kinetic term, which has a profound effect on its RG properties. In particular around the Gaussian fixed point, it supports a Hilbert space of renormalizable interactions involving arbitrarily ... | 9.180788 | 8.853308 | 9.723395 | 8.065831 | 8.364438 | 9.041483 | 8.229758 | 8.894952 | 8.163746 | 10.717011 | 8.275395 | 8.108234 | 9.189633 | 8.682169 | 8.738176 | 8.293763 | 8.801729 | 8.432555 | 8.712507 | 9.38634 | 8.55883 |
hep-th/0209168 | Elena Poletaeva | Elena Poletaeva | Superconformal algebras and Lie superalgebras of the Hodge theory | Published by JNMP at http://www.sm.luth.se/math/JNMP/ | J.Nonlin.Math.Phys. 10 (2003) 141-147 | 10.2991/jnmp.2003.10.2.2 | null | hep-th | null | We observe a correspondence between the zero modes of superconformal algebras
$S'(2, 1)$ and W(4) and the Lie superalgebras formed by classical operators
appearing in the K{\"a}hler and hyper-K{\"a}hler geometry.
| [
{
"created": "Fri, 20 Sep 2002 09:55:05 GMT",
"version": "v1"
},
{
"created": "Wed, 14 May 2003 09:54:35 GMT",
"version": "v2"
},
{
"created": "Fri, 24 Oct 2003 23:18:48 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Poletaeva",
"Elena",
""
]
] | We observe a correspondence between the zero modes of superconformal algebras $S'(2, 1)$ and W(4) and the Lie superalgebras formed by classical operators appearing in the K{\"a}hler and hyper-K{\"a}hler geometry. | 13.085995 | 11.295879 | 13.496625 | 11.942255 | 12.564483 | 12.790652 | 11.48739 | 11.866586 | 10.461953 | 16.311663 | 11.872525 | 11.407463 | 13.431784 | 12.025949 | 11.881488 | 11.768295 | 11.481933 | 11.574591 | 11.924568 | 12.842263 | 11.916129 |
hep-th/9312138 | A. Leonidov | E.I.Guendelman, A.Leonidov, V.Nechitailo and D.A.Owen | On the Heat Kernel in Covariant Background Gauge | 6 pages, plain LaTeX, BI-TP 93/54, BGUPHYS-93/10-2 | Phys.Lett.B324:160-163,1994 | 10.1016/0370-2693(94)90402-2 | null | hep-th hep-ph | null | The first three coefficients in an expansion of the heat kernel of a
nonminimal nonabelian kinetic operator taken in an arbitrary background gauge
in arbitrary space-time dimension are calculated
| [
{
"created": "Wed, 15 Dec 1993 16:55:42 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Guendelman",
"E. I.",
""
],
[
"Leonidov",
"A.",
""
],
[
"Nechitailo",
"V.",
""
],
[
"Owen",
"D. A.",
""
]
] | The first three coefficients in an expansion of the heat kernel of a nonminimal nonabelian kinetic operator taken in an arbitrary background gauge in arbitrary space-time dimension are calculated | 29.060593 | 15.388573 | 17.492702 | 13.560019 | 21.301161 | 14.716718 | 13.876829 | 13.576975 | 15.315459 | 22.809345 | 13.944833 | 16.304699 | 19.984438 | 18.724279 | 18.050407 | 16.294716 | 17.286858 | 18.804192 | 18.174194 | 21.346714 | 18.566521 |
1212.4111 | Alberto Palomo-Lozano | Alberto Palomo-Lozano | Killing Spinors -- Beyond Supergravity | Ph.D. thesis, IFT UAM/CSIC, June 2012 (v2: minor changes) | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a doctoral thesis on the application of techniques originally
developed in the programme of characterisation of supersymmetric solutions to
Supergravity theories, to finding alternative backgrounds. We start by
discussing the concept of a Killing spinor, and how these are paramount to the
process of classifyi... | [
{
"created": "Mon, 17 Dec 2012 19:22:53 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Mar 2013 19:16:31 GMT",
"version": "v2"
}
] | 2013-03-07 | [
[
"Palomo-Lozano",
"Alberto",
""
]
] | This is a doctoral thesis on the application of techniques originally developed in the programme of characterisation of supersymmetric solutions to Supergravity theories, to finding alternative backgrounds. We start by discussing the concept of a Killing spinor, and how these are paramount to the process of classifying... | 17.433849 | 19.044458 | 17.896299 | 16.561405 | 17.819288 | 18.73588 | 20.648537 | 15.757912 | 18.22777 | 18.402121 | 17.947989 | 16.80615 | 16.563671 | 15.980447 | 16.730272 | 16.771599 | 16.510208 | 16.314642 | 16.359175 | 17.046635 | 16.211708 |
hep-th/9702003 | Shoichi Ichinose | Shoichi Ichinose and Noriaki Ikeda | Graphical Classification of Global SO(n) Invariants and Independent
General Invariants | LaTex, epsf, 60 pages, many figures | J.Math.Phys. 38 (1997) 6475-6521 | 10.1063/1.532183 | DAMTP/97-3 | hep-th | null | This paper treats some basic points in general relativity and in its
perturbative analysis. Firstly a systematic classification of global SO(n)
invariants, which appear in the weak-field expansion of n-dimensional
gravitational theories, is presented. Through the analysis, we explain the
following points: a) a graphi... | [
{
"created": "Fri, 31 Jan 1997 15:40:25 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Feb 1997 11:00:42 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Ichinose",
"Shoichi",
""
],
[
"Ikeda",
"Noriaki",
""
]
] | This paper treats some basic points in general relativity and in its perturbative analysis. Firstly a systematic classification of global SO(n) invariants, which appear in the weak-field expansion of n-dimensional gravitational theories, is presented. Through the analysis, we explain the following points: a) a graphica... | 16.003632 | 16.362625 | 15.941198 | 15.724503 | 17.478189 | 17.423441 | 17.009026 | 16.352373 | 15.679594 | 17.840904 | 15.862918 | 15.444324 | 15.527137 | 15.346544 | 15.370367 | 15.761342 | 15.499904 | 15.43611 | 15.221093 | 15.850337 | 15.599838 |
2301.00663 | Jiakang Bao | Jiakang Bao | A Survey of Toric Quivers and BPS Algebras | 40 pages; v4: minor corrections | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note, we discuss some properties of the quiver BPS algebras. We
consider how they would transform under different operations on the toric
quivers, such as dualities and higgsing. We also give free field realizations
of the algebras, in particular for the chiral quivers.
| [
{
"created": "Mon, 2 Jan 2023 13:34:35 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Feb 2023 10:32:58 GMT",
"version": "v2"
},
{
"created": "Thu, 16 Mar 2023 15:34:18 GMT",
"version": "v3"
},
{
"created": "Mon, 10 Apr 2023 13:39:08 GMT",
"version": "v4"
}
] | 2023-04-11 | [
[
"Bao",
"Jiakang",
""
]
] | In this note, we discuss some properties of the quiver BPS algebras. We consider how they would transform under different operations on the toric quivers, such as dualities and higgsing. We also give free field realizations of the algebras, in particular for the chiral quivers. | 12.18573 | 8.851877 | 11.074595 | 8.873705 | 8.977037 | 8.137445 | 8.67722 | 9.301214 | 9.608129 | 13.761913 | 8.602851 | 9.476397 | 11.027559 | 9.559874 | 9.638249 | 9.499323 | 9.50643 | 9.604192 | 9.496757 | 11.129071 | 9.005319 |
hep-th/9806228 | Frank Wilczek | Frank Wilczek | Projective Statistics and Spinors in Hilbert Space | LaTeX, 3 pages | null | null | IASSNS-HEP98-61 | hep-th cond-mat | null | In quantum mechanics, symmetry groups can be realized by projective, as well
as by ordinary unitary, representations. For the permutation symmetry relevant
to quantum statistics of N indistinguishable particles, the simplest properly
projective representation is highly non-trivial, of dimension $2^{(N-1)/2}$,
and is ... | [
{
"created": "Mon, 29 Jun 1998 14:06:26 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Wilczek",
"Frank",
""
]
] | In quantum mechanics, symmetry groups can be realized by projective, as well as by ordinary unitary, representations. For the permutation symmetry relevant to quantum statistics of N indistinguishable particles, the simplest properly projective representation is highly non-trivial, of dimension $2^{(N-1)/2}$, and is mo... | 12.735875 | 14.995882 | 13.800688 | 12.774504 | 15.715156 | 13.087642 | 13.67424 | 12.968458 | 12.824471 | 15.508265 | 12.853043 | 11.662196 | 12.072376 | 11.316573 | 11.491603 | 11.240266 | 11.026229 | 11.308754 | 11.817924 | 12.383832 | 11.914686 |
1610.01647 | Prabal Adhikari | Prabal Adhikari and Jens O. Andersen | Chiral density wave versus pion condensation in the 1+1 dimensional NJL
model | 14 pages and 11 figs | Phys. Rev. D 95, 054020 (2017) | 10.1103/PhysRevD.95.054020 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the possibility of an inhomogeneous quark condensate
in the 1+1 dimensional Nambu-Jona-Lasinio model in the large-$N_c$ limit at
finite temperature $T$ and quark chemical potential $\mu$ using dimensional
regularization. The phase diagram in the $\mu$--$T$ plane is mapped out. At
zero temperat... | [
{
"created": "Sat, 24 Sep 2016 12:33:52 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Jun 2017 13:32:44 GMT",
"version": "v2"
}
] | 2017-06-06 | [
[
"Adhikari",
"Prabal",
""
],
[
"Andersen",
"Jens O.",
""
]
] | In this paper, we study the possibility of an inhomogeneous quark condensate in the 1+1 dimensional Nambu-Jona-Lasinio model in the large-$N_c$ limit at finite temperature $T$ and quark chemical potential $\mu$ using dimensional regularization. The phase diagram in the $\mu$--$T$ plane is mapped out. At zero temperatur... | 4.00553 | 4.110352 | 3.529872 | 3.770295 | 3.901402 | 4.081003 | 3.940407 | 4.343009 | 3.669439 | 3.832704 | 3.885751 | 3.724134 | 3.850476 | 3.753133 | 3.779691 | 3.92832 | 3.823878 | 3.902978 | 3.706507 | 3.806853 | 3.936083 |
2212.13165 | Stefan Evans | Johann Rafelski, Stefan Evans, Lance Labun | Study of QED singular properties for variable gyromagnetic ratio
$g\simeq 2$ | 12 pages, 3 figures. This paper builds on the work in
arXiv:1205.1835, motivated by recent advances in the Dirac-Pauli-based QED
effective action, and with extended author list | Physical Review D 107, No. 7 (2023) 107.076002 | 10.1103/PhysRevD.107.076002 | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Using the external field method, {\it i.e.\/} evaluating the effective action
$V_{\mathrm{eff}}$ for an arbitrarily strong constant and homogeneous field, we
explore nonperturbative properties of QED allowing arbitrary gyromagnetic ratio
$g$. We find a cusp at $g = 2$ in: a) The QED $b_0$-renormalization group
coeffi... | [
{
"created": "Mon, 26 Dec 2022 13:54:29 GMT",
"version": "v1"
}
] | 2023-04-06 | [
[
"Rafelski",
"Johann",
""
],
[
"Evans",
"Stefan",
""
],
[
"Labun",
"Lance",
""
]
] | Using the external field method, {\it i.e.\/} evaluating the effective action $V_{\mathrm{eff}}$ for an arbitrarily strong constant and homogeneous field, we explore nonperturbative properties of QED allowing arbitrary gyromagnetic ratio $g$. We find a cusp at $g = 2$ in: a) The QED $b_0$-renormalization group coeffici... | 13.902824 | 14.749316 | 12.053454 | 11.885685 | 13.994745 | 13.990118 | 13.314769 | 13.079188 | 11.839061 | 13.194806 | 12.894642 | 12.922318 | 12.644676 | 12.733361 | 12.927872 | 13.070852 | 12.976332 | 12.713332 | 12.602572 | 13.021772 | 12.605732 |
1112.4713 | Stefano Bellucci | Stefano Bellucci, Armen Nersessian and Vahagn Yeghikyan | Action-angle variables for the particle near extreme Kerr throat | 8 pages, PACS numbers: 04.70.Bw, 45.10.Na; we corrected a mistake | Mod.Phys.Lett. A27:1250191,2012 | 10.1142/S021773231250191X | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the action-angle variables for the spherical part of conformal
mechanics describing the motion of a particle near extreme Kerr throat. We
indicate the existence of the critical point $|p_\varphi|=mc R_{\rm Sch}$ (with
$m$ being the mass of the particle, $c$ denoting the speed of light, $R_{\rm
Sch}=2\gam... | [
{
"created": "Tue, 20 Dec 2011 14:56:50 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Jun 2012 10:01:56 GMT",
"version": "v2"
}
] | 2014-12-01 | [
[
"Bellucci",
"Stefano",
""
],
[
"Nersessian",
"Armen",
""
],
[
"Yeghikyan",
"Vahagn",
""
]
] | We construct the action-angle variables for the spherical part of conformal mechanics describing the motion of a particle near extreme Kerr throat. We indicate the existence of the critical point $|p_\varphi|=mc R_{\rm Sch}$ (with $m$ being the mass of the particle, $c$ denoting the speed of light, $R_{\rm Sch}=2\gamma... | 7.157991 | 7.063861 | 7.825649 | 6.963088 | 7.77646 | 6.933823 | 7.079476 | 6.839511 | 6.779945 | 8.163542 | 7.147691 | 6.930026 | 7.332572 | 6.934014 | 6.747781 | 6.803992 | 7.121097 | 6.910965 | 6.997051 | 7.405248 | 7.002203 |
0706.2493 | Christian Saemann | Denjoe O'Connor and Christian Saemann | Fuzzy Scalar Field Theory as a Multitrace Matrix Model | 1+25 pages, replaced with published version, minor improvements | JHEP 0708:066,2007 | 10.1088/1126-6708/2007/08/066 | null | hep-th | null | We develop an analytical approach to scalar field theory on the fuzzy sphere
based on considering a perturbative expansion of the kinetic term. This
expansion allows us to integrate out the angular degrees of freedom in the
hermitian matrices encoding the scalar field. The remaining model depends only
on the eigenval... | [
{
"created": "Sun, 17 Jun 2007 17:24:40 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Sep 2007 09:59:26 GMT",
"version": "v2"
}
] | 2009-11-18 | [
[
"O'Connor",
"Denjoe",
""
],
[
"Saemann",
"Christian",
""
]
] | We develop an analytical approach to scalar field theory on the fuzzy sphere based on considering a perturbative expansion of the kinetic term. This expansion allows us to integrate out the angular degrees of freedom in the hermitian matrices encoding the scalar field. The remaining model depends only on the eigenvalue... | 7.852643 | 7.118894 | 8.851862 | 6.740311 | 7.587039 | 7.17937 | 6.937022 | 7.214038 | 7.303088 | 9.244573 | 7.067448 | 7.29778 | 7.63661 | 7.260531 | 7.334761 | 7.269596 | 7.16362 | 7.019895 | 7.427982 | 8.144289 | 7.431479 |
1806.08292 | Matteo Bertolini | Riccardo Argurio, Matteo Bertolini, Francesco Bigazzi, Aldo L.
Cotrone, Pierluigi Niro | QCD domain walls, Chern-Simons theories and holography | 25 pages, 2 figures. v2: refs added, typos corrected, some
clarifications in section 3. v3: minor improvements, ref added | null | 10.1007/JHEP09(2018)090 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Massive QCD at $\theta=\pi$ breaks CP spontaneously and admits domain walls
whose dynamics and phases depend on the number of flavors and their masses. We
discuss these issues within the Witten-Sakai-Sugimoto model of holographic QCD.
Besides showing that this model reproduces all QCD expectations, we address two
int... | [
{
"created": "Thu, 21 Jun 2018 15:34:16 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Jul 2018 13:41:58 GMT",
"version": "v2"
},
{
"created": "Thu, 13 Sep 2018 15:13:12 GMT",
"version": "v3"
}
] | 2018-10-17 | [
[
"Argurio",
"Riccardo",
""
],
[
"Bertolini",
"Matteo",
""
],
[
"Bigazzi",
"Francesco",
""
],
[
"Cotrone",
"Aldo L.",
""
],
[
"Niro",
"Pierluigi",
""
]
] | Massive QCD at $\theta=\pi$ breaks CP spontaneously and admits domain walls whose dynamics and phases depend on the number of flavors and their masses. We discuss these issues within the Witten-Sakai-Sugimoto model of holographic QCD. Besides showing that this model reproduces all QCD expectations, we address two inter... | 12.066578 | 9.516798 | 11.591493 | 10.968843 | 10.331273 | 10.25111 | 10.786725 | 10.136771 | 10.049417 | 12.312667 | 10.047984 | 9.898602 | 10.712457 | 10.728342 | 10.716946 | 10.427115 | 9.884685 | 10.096365 | 10.19428 | 11.302902 | 10.01352 |
hep-th/9709201 | null | E Rodulfo, R Delbourgo (University of Tasmania) | One-loop effective multi-gluon Lagrangian in arbitrary dimensions | 16 pages, LaTeX | Int.J.Mod.Phys.A14:4457-4472,1999 | 10.1142/S0217751X99002086 | UTAS-PHYS-97-14 | hep-th | null | We exhibit the one-loop multi-gluon effective Lagrangian in any dimension for
a field theory with a quasilocal background, using the background-field
formalism. Specific results, including counter terms (up to 12 spacetime
dimensions), have been derived, applied to the Yang-Mills theory and found to
be in agreement w... | [
{
"created": "Mon, 29 Sep 1997 05:02:50 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Rodulfo",
"E",
"",
"University of Tasmania"
],
[
"Delbourgo",
"R",
"",
"University of Tasmania"
]
] | We exhibit the one-loop multi-gluon effective Lagrangian in any dimension for a field theory with a quasilocal background, using the background-field formalism. Specific results, including counter terms (up to 12 spacetime dimensions), have been derived, applied to the Yang-Mills theory and found to be in agreement wit... | 19.64957 | 16.030165 | 19.200357 | 16.771122 | 18.070976 | 18.052963 | 20.015476 | 16.325428 | 15.477736 | 19.932951 | 16.787485 | 17.906055 | 17.631819 | 16.862711 | 17.31245 | 16.983347 | 17.713558 | 16.927216 | 17.18424 | 18.707991 | 17.354008 |
hep-th/0506067 | Sergei Sibiryakov | D.S. Gorbunov, S.M. Sibiryakov | Ultra-large distance modification of gravity from Lorentz symmetry
breaking at the Planck scale | 28 pages | JHEP 0509 (2005) 082 | 10.1088/1126-6708/2005/09/082 | null | hep-th | null | We present an extension of the Randall--Sundrum model in which, due to
spontaneous Lorentz symmetry breaking, graviton mixes with bulk vector fields
and becomes quasilocalized. The masses of KK modes comprising the
four-dimensional graviton are naturally exponentially small. This allows to
push the Lorentz breaking s... | [
{
"created": "Wed, 8 Jun 2005 18:56:19 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Gorbunov",
"D. S.",
""
],
[
"Sibiryakov",
"S. M.",
""
]
] | We present an extension of the Randall--Sundrum model in which, due to spontaneous Lorentz symmetry breaking, graviton mixes with bulk vector fields and becomes quasilocalized. The masses of KK modes comprising the four-dimensional graviton are naturally exponentially small. This allows to push the Lorentz breaking sca... | 7.822832 | 8.492037 | 8.068768 | 7.942266 | 7.547221 | 8.050494 | 7.43313 | 8.074391 | 8.25661 | 8.75106 | 7.841896 | 7.478891 | 7.607354 | 7.615195 | 7.7717 | 7.663562 | 7.799754 | 7.69878 | 7.565866 | 7.909103 | 7.643905 |
hep-th/0612241 | Wolfgang Schleifenbaum | D. Epple, H. Reinhardt, W. Schleifenbaum | Confining Solution of the Dyson-Schwinger Equations in Coulomb Gauge | 9 pages, 3 figures, references added. | Phys.Rev.D75:045011,2007 | 10.1103/PhysRevD.75.045011 | null | hep-th hep-lat hep-ph | null | The Dyson-Schwinger equations arising from minimizing the vacuum energy
density in the Hamiltonian approach to Yang-Mills theory in Coulomb gauge are
solved numerically. A new solution is presented which gives rise to a strictly
linearly rising static quark potential and whose existence was previously
observed in the... | [
{
"created": "Thu, 21 Dec 2006 18:26:13 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Apr 2007 10:31:20 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Epple",
"D.",
""
],
[
"Reinhardt",
"H.",
""
],
[
"Schleifenbaum",
"W.",
""
]
] | The Dyson-Schwinger equations arising from minimizing the vacuum energy density in the Hamiltonian approach to Yang-Mills theory in Coulomb gauge are solved numerically. A new solution is presented which gives rise to a strictly linearly rising static quark potential and whose existence was previously observed in the i... | 8.190063 | 7.582872 | 7.744653 | 7.187712 | 7.643693 | 7.601853 | 7.504277 | 6.698482 | 6.586559 | 8.301041 | 6.849439 | 7.371313 | 7.683689 | 7.53163 | 7.814809 | 7.429899 | 7.75924 | 7.488392 | 7.629048 | 7.772432 | 7.323884 |
1307.6263 | Kevin Morand | Xavier Bekaert and Kevin Morand | Embedding nonrelativistic physics inside a gravitational wave | 56 pages, 9 figures, v3:Minor corrections | Phys. Rev. D 88, 063008 (2013) | 10.1103/PhysRevD.88.063008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gravitational waves with parallel rays are known to have remarkable
properties: Their orbit space of null rays possesses the structure of a
non-relativistic spacetime of codimension-one. Their geodesics are in
one-to-one correspondence with dynamical trajectories of a non-relativistic
system. Similarly, the null dime... | [
{
"created": "Tue, 23 Jul 2013 22:39:05 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Sep 2013 17:44:25 GMT",
"version": "v2"
},
{
"created": "Sun, 28 Dec 2014 21:19:31 GMT",
"version": "v3"
}
] | 2016-02-22 | [
[
"Bekaert",
"Xavier",
""
],
[
"Morand",
"Kevin",
""
]
] | Gravitational waves with parallel rays are known to have remarkable properties: Their orbit space of null rays possesses the structure of a non-relativistic spacetime of codimension-one. Their geodesics are in one-to-one correspondence with dynamical trajectories of a non-relativistic system. Similarly, the null dimens... | 11.73785 | 11.828803 | 10.894359 | 10.987577 | 10.9159 | 12.252964 | 12.239732 | 11.395358 | 11.42339 | 12.252032 | 11.173457 | 10.969016 | 10.949013 | 10.936015 | 11.468328 | 10.796346 | 11.382558 | 11.108206 | 10.962287 | 10.924059 | 10.92788 |
1212.0093 | Romain Vasseur | Azat M. Gainutdinov, Jesper Lykke Jacobsen, Hubert Saleur and Romain
Vasseur | A physical approach to the classification of indecomposable Virasoro
representations from the blob algebra | 65 pages, 19 figures. New appendix | Nuclear Physics B 873 (3), 614--681 (2013) | 10.1016/j.nuclphysb.2013.04.017 | null | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of Conformal Field Theory (CFT), many results can be obtained
from the representation theory of the Virasoro algebra. While the interest in
Logarithmic CFTs has been growing recently, the Virasoro representations
corresponding to these quantum field theories remain dauntingly complicated,
thus hinderin... | [
{
"created": "Sat, 1 Dec 2012 11:08:57 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Jan 2013 08:44:05 GMT",
"version": "v2"
},
{
"created": "Wed, 23 Jan 2013 14:28:39 GMT",
"version": "v3"
},
{
"created": "Sat, 23 Mar 2013 10:36:32 GMT",
"version": "v4"
}
] | 2013-06-12 | [
[
"Gainutdinov",
"Azat M.",
""
],
[
"Jacobsen",
"Jesper Lykke",
""
],
[
"Saleur",
"Hubert",
""
],
[
"Vasseur",
"Romain",
""
]
] | In the context of Conformal Field Theory (CFT), many results can be obtained from the representation theory of the Virasoro algebra. While the interest in Logarithmic CFTs has been growing recently, the Virasoro representations corresponding to these quantum field theories remain dauntingly complicated, thus hindering ... | 10.43497 | 10.920718 | 12.726575 | 10.499445 | 11.963286 | 10.836062 | 11.486835 | 10.69702 | 10.772869 | 12.397409 | 10.259794 | 10.148424 | 10.946903 | 10.152906 | 10.245231 | 10.087976 | 10.242231 | 9.970563 | 10.225908 | 10.901125 | 9.915385 |
hep-th/9604108 | Claudia Daboul | Claudia Daboul (Universitaet Hamburg, GERMANY) | Algebraic Proof of the Symmetric Space Theorem | 13 pages. Latex2e. To be published in Journal of Mathematical Physics | J.Math.Phys. 37 (1996) 3576-3586 | 10.1063/1.531583 | null | hep-th | null | I give a relatively elementary proof of the symmetric space theorem, due to
Goddard, Nahm and Olive \cite{GNO}. Unlike their original proof, which involves
the quark-model construction, I only use elementary algebraic techniques.
| [
{
"created": "Thu, 18 Apr 1996 23:24:47 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Daboul",
"Claudia",
"",
"Universitaet Hamburg, GERMANY"
]
] | I give a relatively elementary proof of the symmetric space theorem, due to Goddard, Nahm and Olive \cite{GNO}. Unlike their original proof, which involves the quark-model construction, I only use elementary algebraic techniques. | 16.386616 | 13.096169 | 16.253935 | 12.868356 | 14.021765 | 12.484831 | 10.437959 | 14.952434 | 12.868116 | 15.868684 | 12.616002 | 12.585185 | 12.723684 | 11.744414 | 12.517459 | 12.506595 | 11.8883 | 11.746856 | 12.50596 | 13.188868 | 12.182108 |
hep-th/9809154 | Erhard Seiler | Adrian Patrascioiu, Erhard Seiler | Nonlinear $\sigma$-model, form factors and universality | 10 pages, 5 figures | Phys.Lett. B445 (1998) 160-164 | 10.1016/S0370-2693(98)01425-7 | AZPH-TH 98-07, MPI-PhT/98-40 | hep-th hep-lat | null | We report the results of a very high statistics Monte Carlo study of the
continuum limit of the two dimensional O(3) non-linear $\sigma$ model. We find
a significant discrepancy between the continuum extrapolation of our data and
the form factor prediction of Balog and Niedermaier, inspired by the
Zamolodchikovs' S-m... | [
{
"created": "Mon, 21 Sep 1998 15:56:28 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Patrascioiu",
"Adrian",
""
],
[
"Seiler",
"Erhard",
""
]
] | We report the results of a very high statistics Monte Carlo study of the continuum limit of the two dimensional O(3) non-linear $\sigma$ model. We find a significant discrepancy between the continuum extrapolation of our data and the form factor prediction of Balog and Niedermaier, inspired by the Zamolodchikovs' S-mat... | 7.488626 | 7.687868 | 7.693507 | 6.959782 | 7.55957 | 7.258943 | 7.672394 | 7.470722 | 6.947398 | 7.636529 | 7.534054 | 6.596313 | 7.061611 | 6.963402 | 7.109158 | 6.807033 | 7.015802 | 6.58733 | 7.232218 | 6.852468 | 6.611753 |
hep-th/9701059 | Chand Devchand | C. Devchand and Jeremy Schiff | Hidden Symmetries of the Principal Chiral Model and a Nonstandard Loop
Algebra | 5 pages, latex; changed title and slight textual revisions; to be
published in Phys. Lett. B | null | 10.1016/S0370-2693(97)01420-2 | null | hep-th | null | We examine the precise structure of the loop algebra of `dressing' symmetries
of the Principal Chiral Model, and discuss a new infinite set of abelian
symmetries of the field equations which preserve a symplectic form on the space
of solutions.
| [
{
"created": "Tue, 14 Jan 1997 08:59:42 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Nov 1997 19:17:34 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Devchand",
"C.",
""
],
[
"Schiff",
"Jeremy",
""
]
] | We examine the precise structure of the loop algebra of `dressing' symmetries of the Principal Chiral Model, and discuss a new infinite set of abelian symmetries of the field equations which preserve a symplectic form on the space of solutions. | 12.807754 | 11.019036 | 12.009274 | 10.120485 | 10.085739 | 10.23102 | 10.450618 | 9.944091 | 10.478758 | 10.45089 | 9.652621 | 11.029416 | 12.875469 | 11.433736 | 11.369282 | 10.771231 | 11.066513 | 10.628592 | 11.114804 | 12.175343 | 10.513613 |
hep-th/0008131 | Shyamoli Chaudhuri | Shyamoli Chaudhuri | Deconfinement and the Hagedorn Transition in String Theory | Superseded and extended in hep-th/0105110 and hep-th/0208112 | Phys.Rev.Lett. 86 (2001) 1943; Erratum-ibid. 87 (2001) 199901 | 10.1103/PhysRevLett.86.1943 | null | hep-th hep-lat hep-ph | null | Superseded and extended in hep-th/0105110 and hep-th/0208112.
| [
{
"created": "Wed, 16 Aug 2000 19:54:19 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Sep 2000 09:16:31 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Dec 2000 23:45:28 GMT",
"version": "v3"
},
{
"created": "Tue, 27 Feb 2001 21:21:22 GMT",
"version": "v4"
},
{
"cr... | 2009-10-31 | [
[
"Chaudhuri",
"Shyamoli",
""
]
] | Superseded and extended in hep-th/0105110 and hep-th/0208112. | 36.734116 | 22.178629 | 18.153776 | 16.314514 | 26.672052 | 17.049845 | 19.583532 | 22.484192 | 17.671734 | 32.33548 | 24.63027 | 21.851446 | 29.535612 | 21.767294 | 21.752476 | 23.620667 | 21.510395 | 21.988779 | 21.223444 | 30.252254 | 19.895338 |
hep-th/0403035 | Sebastian de Haro | Jan de Boer, Sebastian de Haro | The Off-shell M5-brane and Non-Perturbative Gauge Theory | 30 pages | Nucl.Phys.B696:174-204,2004 | 10.1016/j.nuclphysb.2004.06.050 | AEI-2003-108, UCLA/03/TEP/41, ITFA-2004-09 | hep-th | null | M5-branes wrapping a holomorphic curve in a Calabi-Yau manifold can be used
to construct four-dimensional N=1 gauge theories. In this paper we will
consider M5-brane configurations corresponding to N=2 theories broken to N=1 by
a superpotential for the adjoint scalar field. These M5-brane configurations
can be obtain... | [
{
"created": "Tue, 2 Mar 2004 13:29:53 GMT",
"version": "v1"
}
] | 2010-12-03 | [
[
"de Boer",
"Jan",
""
],
[
"de Haro",
"Sebastian",
""
]
] | M5-branes wrapping a holomorphic curve in a Calabi-Yau manifold can be used to construct four-dimensional N=1 gauge theories. In this paper we will consider M5-brane configurations corresponding to N=2 theories broken to N=1 by a superpotential for the adjoint scalar field. These M5-brane configurations can be obtained... | 5.183807 | 4.726995 | 6.069342 | 4.724111 | 4.866736 | 4.841742 | 4.712991 | 4.673406 | 4.943536 | 6.210824 | 4.767852 | 4.792826 | 5.311522 | 4.875245 | 4.815135 | 4.84141 | 4.935662 | 4.818343 | 4.807721 | 5.299965 | 4.891597 |
2105.09603 | Takeshi Morita | Takeshi Morita | Extracting classical Lyapunov exponent from one-dimensional quantum
mechanics | 15 pages, 5 figures. Appendix moved to the main text,the version
published in PRD | Phys.Rev.D 106 (2022) 10, 106001 | 10.1103/PhysRevD.106.106001 | null | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The commutator $[x(t),p]$ in an inverted harmonic oscillator (IHO) in
one-dimensional quantum mechanics exhibits remarkable properties. It reduces to
a c-number and does not show any quantum fluctuations for arbitrary states.
Related to this nature, the quantum Lyapunov exponent computed through the
out-of-time-order... | [
{
"created": "Thu, 20 May 2021 08:57:30 GMT",
"version": "v1"
},
{
"created": "Mon, 31 May 2021 05:28:46 GMT",
"version": "v2"
},
{
"created": "Tue, 22 Nov 2022 00:53:36 GMT",
"version": "v3"
}
] | 2022-11-23 | [
[
"Morita",
"Takeshi",
""
]
] | The commutator $[x(t),p]$ in an inverted harmonic oscillator (IHO) in one-dimensional quantum mechanics exhibits remarkable properties. It reduces to a c-number and does not show any quantum fluctuations for arbitrary states. Related to this nature, the quantum Lyapunov exponent computed through the out-of-time-order c... | 8.442242 | 8.868542 | 8.697057 | 7.85615 | 8.175733 | 8.947765 | 8.615715 | 8.085331 | 8.618821 | 9.583967 | 7.709061 | 8.293592 | 8.488436 | 8.091748 | 8.036834 | 8.107442 | 8.020888 | 8.006442 | 8.453736 | 8.571716 | 8.187477 |
hep-th/9508150 | null | Kurt Lechner and Mario Tonin | Seven--Superform Gauge Fields in N=1, D=10 Supergravity and Duality | 12 pages, Plain TeX, no figures | Phys.Lett. B366 (1996) 149 | 10.1016/0370-2693(95)01375-X | DFPD/95/TH/44, August 1995 | hep-th | null | We present a formulation of $N=1,D=10$ Supergravity--Super--Maxwell theory in
superspace in which the graviphoton can be described by a 2--form $B_2$ or a
6--form $B_6$, the photon by a 1--form $A_1$ or a 7--form $A_7$ and the dilaton
by a scalar $\varphi$ or an 8--form $\varphi_8$, the supercurvatures of these
field... | [
{
"created": "Mon, 28 Aug 1995 16:19:39 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Lechner",
"Kurt",
""
],
[
"Tonin",
"Mario",
""
]
] | We present a formulation of $N=1,D=10$ Supergravity--Super--Maxwell theory in superspace in which the graviphoton can be described by a 2--form $B_2$ or a 6--form $B_6$, the photon by a 1--form $A_1$ or a 7--form $A_7$ and the dilaton by a scalar $\varphi$ or an 8--form $\varphi_8$, the supercurvatures of these fields ... | 6.120432 | 5.995348 | 7.265642 | 5.449189 | 6.033123 | 6.058218 | 5.705661 | 5.614646 | 5.85896 | 7.41081 | 5.852557 | 5.994123 | 6.188382 | 5.75835 | 6.063859 | 6.078933 | 5.93922 | 5.943511 | 5.903108 | 6.202152 | 6.090398 |
hep-th/9905176 | Johanna Erdmenger | Johanna Erdmenger | Gravitational Axial Anomaly for Four Dimensional Conformal Field
Theories | 15 pages, LaTex, no figures. Discussion of photon triangle anomaly
extended, references added. To appear in Nuclear Physics B | Nucl.Phys. B562 (1999) 315-329 | 10.1016/S0550-3213(99)00561-1 | null | hep-th | null | We construct the three point function involving an axial vector current and
two energy-momentum tensors for four dimensional conformal field theories.
Conformal symmetry determines the form of this three point function uniquely up
to a constant factor if the necessary conservation conditions are imposed. The
gravitat... | [
{
"created": "Mon, 24 May 1999 18:52:17 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Oct 1999 13:41:33 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Erdmenger",
"Johanna",
""
]
] | We construct the three point function involving an axial vector current and two energy-momentum tensors for four dimensional conformal field theories. Conformal symmetry determines the form of this three point function uniquely up to a constant factor if the necessary conservation conditions are imposed. The gravitatio... | 9.152246 | 9.494262 | 9.043706 | 8.298797 | 8.925296 | 10.01041 | 8.88709 | 8.802816 | 8.247609 | 10.001691 | 7.983123 | 8.538295 | 8.902301 | 8.571342 | 8.695572 | 8.609205 | 8.438018 | 8.639732 | 8.551454 | 8.799117 | 8.337181 |
hep-th/0403297 | Saharian | Aram A. Saharian, Anna S. Kotanjyan | Radiation from an oscillator uniformly moving along the axis of a
dielectric cylinder | 16 pages, 8 EPS figures | Nucl.Instrum.Meth. B226 (2004) 351-364 | 10.1016/j.nimb.2004.06.036 | null | hep-th cond-mat.other | null | The radiation generated by a charged longitudinal oscillator moving with a
constant drift velocity along the axis of a dielectric cylinder immersed in a
homogeneous medium is investigated. For an arbitrary oscillation law a formula
is derived for the spectral-angular distribution of this radiation. Under the
Cherenko... | [
{
"created": "Wed, 31 Mar 2004 09:14:38 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Saharian",
"Aram A.",
""
],
[
"Kotanjyan",
"Anna S.",
""
]
] | The radiation generated by a charged longitudinal oscillator moving with a constant drift velocity along the axis of a dielectric cylinder immersed in a homogeneous medium is investigated. For an arbitrary oscillation law a formula is derived for the spectral-angular distribution of this radiation. Under the Cherenkov ... | 7.223289 | 6.232402 | 6.861046 | 6.686544 | 6.522356 | 6.017293 | 6.083713 | 6.792597 | 6.694145 | 7.007102 | 6.609231 | 6.567586 | 7.006784 | 6.834732 | 6.716708 | 6.822627 | 6.951092 | 7.091824 | 6.665501 | 7.071263 | 6.861266 |
2104.08332 | Ashok Kapoor | A K Kapoor | A New Approach to Axial Vector Gauge Theories | Latex 8 pages | Int. J. Mod. Phys. A 36 (2021) 2150104 | 10.1142/S0217751X21501049 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In an earlier paper it has been shown that the ultra violet divergence
structure of anomalous U(1) axial vector gauge model in the stochastic
quantization scheme is different from that in the conventional quantum field
theory. Also it has been shown that the model is expected to be renormalizable.
Based on the operat... | [
{
"created": "Tue, 30 Mar 2021 03:26:48 GMT",
"version": "v1"
}
] | 2021-07-19 | [
[
"Kapoor",
"A K",
""
]
] | In an earlier paper it has been shown that the ultra violet divergence structure of anomalous U(1) axial vector gauge model in the stochastic quantization scheme is different from that in the conventional quantum field theory. Also it has been shown that the model is expected to be renormalizable. Based on the operator... | 9.848773 | 9.46201 | 8.852774 | 8.749383 | 8.91726 | 9.149652 | 9.057552 | 8.822028 | 8.90274 | 9.459762 | 9.075304 | 8.578711 | 8.64465 | 8.63826 | 8.494109 | 8.745756 | 8.669576 | 8.815641 | 8.720452 | 8.773759 | 8.898107 |
1706.01397 | Gianni Tallarita | Gianni Tallarita and Fabrizio Canfora | Multi-Skyrmions on $AdS_2 \times S_2$, Rational maps and Popcorn
Transitions | 20 pages, 4 figures, to appear in Nuclear Physics B | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By combining two different techniques to construct multi-soliton solutions of
the (3+1)-dimensional Skyrme model, the generalized hedgehog and the rational
map ansatz, we find multi-Skyrmion configurations in $AdS_{2}\times S_{2}$. We
construct Skyrmionic multi-layered configurations such that the total Baryon
charge... | [
{
"created": "Mon, 5 Jun 2017 16:08:48 GMT",
"version": "v1"
}
] | 2017-06-06 | [
[
"Tallarita",
"Gianni",
""
],
[
"Canfora",
"Fabrizio",
""
]
] | By combining two different techniques to construct multi-soliton solutions of the (3+1)-dimensional Skyrme model, the generalized hedgehog and the rational map ansatz, we find multi-Skyrmion configurations in $AdS_{2}\times S_{2}$. We construct Skyrmionic multi-layered configurations such that the total Baryon charge i... | 6.672014 | 6.829699 | 6.240725 | 5.95397 | 6.369604 | 6.350845 | 6.288761 | 5.79354 | 6.298992 | 6.805964 | 5.794961 | 6.238165 | 6.503257 | 6.289427 | 6.207278 | 6.240222 | 6.18745 | 6.159024 | 6.339314 | 6.55269 | 6.336678 |
hep-th/9508153 | null | S. James Gates, Jr | Why Auxiliary Fields Matter: The Strange Case of the 4D, N = 1
Supersymmetric QCD Effective Action | 14 pages, UMDEPP 96-19 | Phys.Lett.B365:132-140,1996 | 10.1016/0370-2693(95)01309-1 | null | hep-th | null | Within a four dimensional manifestly N = 1 supersymmetric action, we show
that Wess-Zumino-Novikov-Witten (WZNW) terms can be embedded in an
extraordinarily simple manner into a purely chiral superaction. In order to
achieve this result it is necessary to assign spin-0 and spin-1/2 degrees of
freedom both to chiral s... | [
{
"created": "Mon, 28 Aug 1995 20:40:15 GMT",
"version": "v1"
}
] | 2012-08-27 | [
[
"Gates,",
"S. James",
"Jr"
]
] | Within a four dimensional manifestly N = 1 supersymmetric action, we show that Wess-Zumino-Novikov-Witten (WZNW) terms can be embedded in an extraordinarily simple manner into a purely chiral superaction. In order to achieve this result it is necessary to assign spin-0 and spin-1/2 degrees of freedom both to chiral sup... | 8.485901 | 7.571171 | 8.225239 | 7.487853 | 7.293881 | 7.888275 | 7.389511 | 7.641335 | 7.285101 | 9.118002 | 7.392836 | 7.208173 | 8.171356 | 7.499194 | 7.625981 | 7.260268 | 7.448339 | 7.615121 | 7.585156 | 8.013681 | 7.518031 |
hep-th/0211275 | Olkhov | O. A. Olkhov (Institute of Chemical Physics, Moscow) | Topological interpretation of Dirac equation and geometrization of
physical interactions | LaTex, 10 pages, Proc.XXV Workshop on Fundamental Problems of High
Energy Physics and Field Theory. Geometrical and topological ideas in modern
physics, Protvino, Russia, 25 - 28 June 2002 (to be published} | null | null | null | hep-th | null | Earlier we have shown that interacting electron-positron and electromagnetic
fields can be considered as a certain microscopic distortion of
pseudo-Euclidean properties of the Minkovsky 4-space-time. The known Dirac and
Maxwell equations prove to be group-theoretical relations describing this
distortion (nonmetrized ... | [
{
"created": "Thu, 28 Nov 2002 11:11:25 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Olkhov",
"O. A.",
"",
"Institute of Chemical Physics, Moscow"
]
] | Earlier we have shown that interacting electron-positron and electromagnetic fields can be considered as a certain microscopic distortion of pseudo-Euclidean properties of the Minkovsky 4-space-time. The known Dirac and Maxwell equations prove to be group-theoretical relations describing this distortion (nonmetrized cl... | 21.817356 | 22.851122 | 22.876492 | 20.991652 | 24.489853 | 21.771753 | 23.002174 | 21.712088 | 21.868887 | 28.746246 | 20.748997 | 21.513805 | 19.943893 | 20.280151 | 20.339531 | 21.578609 | 21.86005 | 20.097326 | 21.086336 | 20.187815 | 20.848932 |
2112.05168 | Brian McPeak | Johan Henriksson, Ashish Kakkar, Brian McPeak | Classical Codes and Chiral CFTs at Higher Genus | 48pp | null | 10.1007/JHEP05(2022)159 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Higher genus modular invariance of two-dimensional conformal field theories
(CFTs) is a largely unexplored area. In this paper, we derive explicit
expressions for the higher genus partition functions of a specific class of
CFTs: code CFTs, which are constructed using classical error-correcting codes.
In this setting,... | [
{
"created": "Thu, 9 Dec 2021 19:00:04 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Apr 2022 18:12:58 GMT",
"version": "v2"
}
] | 2022-06-08 | [
[
"Henriksson",
"Johan",
""
],
[
"Kakkar",
"Ashish",
""
],
[
"McPeak",
"Brian",
""
]
] | Higher genus modular invariance of two-dimensional conformal field theories (CFTs) is a largely unexplored area. In this paper, we derive explicit expressions for the higher genus partition functions of a specific class of CFTs: code CFTs, which are constructed using classical error-correcting codes. In this setting, t... | 7.284384 | 6.653212 | 7.068164 | 6.444197 | 7.024672 | 6.738675 | 6.432896 | 6.643686 | 6.604462 | 7.1758 | 6.759786 | 6.805837 | 7.036732 | 6.663855 | 6.84548 | 6.853621 | 6.589766 | 6.676432 | 6.831027 | 7.375967 | 6.785662 |
hep-th/0610160 | Sergey Paston | V.A. Franke, S.A. Paston, E.V. Prokhvatilov | QED(1+1) on the Light Front and its implications for
semiphenomenological methods in QCD(3+1) | LaTeX 2e, 9 pages, 2 figures. Proceedings of "Quarks-2006",
St-Petersburg 2006 | null | null | SPbU-IP-06-04 | hep-th | null | A possibility of semiphenomenological description of vacuum effects in QCD
quantized on the Light Front (LF) is discussed. A modification of the canonical
LF Hamiltonian for QCD is proposed, basing on the detailed study of the exact
description of vacuum condensate in QED(1+1) that uses correct form of LF
Hamiltonian... | [
{
"created": "Fri, 13 Oct 2006 14:07:23 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Franke",
"V. A.",
""
],
[
"Paston",
"S. A.",
""
],
[
"Prokhvatilov",
"E. V.",
""
]
] | A possibility of semiphenomenological description of vacuum effects in QCD quantized on the Light Front (LF) is discussed. A modification of the canonical LF Hamiltonian for QCD is proposed, basing on the detailed study of the exact description of vacuum condensate in QED(1+1) that uses correct form of LF Hamiltonian. | 14.335302 | 14.776911 | 14.302621 | 13.273317 | 13.704767 | 13.848712 | 14.206091 | 12.688946 | 13.385557 | 15.222454 | 13.723516 | 13.021443 | 14.079937 | 12.869828 | 13.353287 | 12.957344 | 12.376854 | 12.316412 | 13.01625 | 13.5595 | 12.79104 |
hep-th/0412154 | James T. Liu | A. Batrachenko, James T. Liu, Oscar Varela and W. Y. Wen | Higher Order Integrability in Generalized Holonomy | 19 pages, Latex | Nucl.Phys. B760 (2007) 89-103 | 10.1016/j.nuclphysb.2006.10.017 | MCTP-04-69, FTUV-04-1214, IFIC-04-71 | hep-th | null | Supersymmetric backgrounds in M-theory often involve four-form flux in
addition to pure geometry. In such cases, the classification of supersymmetric
vacua involves the notion of generalized holonomy taking values in SL(32,R),
the Clifford group for eleven-dimensional spinors. Although previous
investigations of gene... | [
{
"created": "Tue, 14 Dec 2004 21:01:41 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Batrachenko",
"A.",
""
],
[
"Liu",
"James T.",
""
],
[
"Varela",
"Oscar",
""
],
[
"Wen",
"W. Y.",
""
]
] | Supersymmetric backgrounds in M-theory often involve four-form flux in addition to pure geometry. In such cases, the classification of supersymmetric vacua involves the notion of generalized holonomy taking values in SL(32,R), the Clifford group for eleven-dimensional spinors. Although previous investigations of genera... | 10.693285 | 11.641081 | 12.10295 | 10.517308 | 11.072386 | 10.765472 | 11.579211 | 10.841115 | 9.782733 | 12.540063 | 9.497448 | 9.853521 | 10.922971 | 9.429713 | 9.697263 | 9.931517 | 9.543998 | 9.873052 | 9.83425 | 10.385521 | 9.934368 |
hep-th/0304017 | Asher Peres | Netanel H. Lindner, Asher Peres, and Daniel R. Terno | Wigner's little group and Berry's phase for massless particles | 4 pages revtex | J.Phys. A36 (2003) L449 | 10.1088/0305-4470/36/29/101 | null | hep-th quant-ph | null | The ``little group'' for massless particles (namely, the Lorentz
transformations $\Lambda$ that leave a null vector invariant) is isomorphic to
the Euclidean group E2: translations and rotations in a plane. We show how to
obtain explicitly the rotation angle of E2 as a function of $\Lambda$ and we
relate that angle t... | [
{
"created": "Wed, 2 Apr 2003 19:01:00 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Lindner",
"Netanel H.",
""
],
[
"Peres",
"Asher",
""
],
[
"Terno",
"Daniel R.",
""
]
] | The ``little group'' for massless particles (namely, the Lorentz transformations $\Lambda$ that leave a null vector invariant) is isomorphic to the Euclidean group E2: translations and rotations in a plane. We show how to obtain explicitly the rotation angle of E2 as a function of $\Lambda$ and we relate that angle to ... | 10.466853 | 9.908334 | 10.386402 | 9.583182 | 9.887282 | 10.244332 | 10.119899 | 10.890598 | 9.54789 | 11.091793 | 9.471703 | 9.53398 | 9.84853 | 9.61617 | 9.237523 | 9.554688 | 9.561233 | 9.640997 | 9.729487 | 9.512969 | 9.811599 |
1812.10970 | Carlos Mafra | Carlos R. Mafra, Oliver Schlotterer | Towards the n-point one-loop superstring amplitude II: Worldsheet
functions and their duality to kinematics | 72 pages, v2: published version | JHEP 1908 (2019) 091 | 10.1007/JHEP08(2019)091 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is the second installment of a series of three papers in which we
describe a method to determine higher-point correlation functions in one-loop
open-superstring amplitudes from first principles. In this second part, we
study worldsheet functions defined on a genus-one surface built from the
coefficient functions... | [
{
"created": "Fri, 28 Dec 2018 12:12:50 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Sep 2019 16:52:38 GMT",
"version": "v2"
}
] | 2019-09-11 | [
[
"Mafra",
"Carlos R.",
""
],
[
"Schlotterer",
"Oliver",
""
]
] | This is the second installment of a series of three papers in which we describe a method to determine higher-point correlation functions in one-loop open-superstring amplitudes from first principles. In this second part, we study worldsheet functions defined on a genus-one surface built from the coefficient functions o... | 12.051403 | 11.309175 | 13.336248 | 11.602253 | 11.754995 | 12.544132 | 13.072336 | 12.346915 | 11.428667 | 14.063943 | 11.849221 | 11.885284 | 11.987613 | 11.614508 | 11.636142 | 11.650135 | 11.909307 | 12.050348 | 11.829166 | 12.098885 | 11.75821 |
1911.03205 | Alberto G. Martin-Caro | Luis J. Garay, Alberto Garc\'ia Mart\'in-Caro and Mercedes
Mart\'in-Benito | Unitary quantization of a charged scalar field and Schwinger effect | 27 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum field theory in curved spacetimes suffers in general from an infinite
ambiguity in the choice of Fock representation and associated vacuum. In
cosmological backgrounds, the requirement of a unitary implementation of the
field dynamics in the physical Hilbert space of the theory is a good criterion
to ameliora... | [
{
"created": "Fri, 8 Nov 2019 12:04:05 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Apr 2020 15:10:36 GMT",
"version": "v2"
}
] | 2020-04-20 | [
[
"Garay",
"Luis J.",
""
],
[
"Martín-Caro",
"Alberto García",
""
],
[
"Martín-Benito",
"Mercedes",
""
]
] | Quantum field theory in curved spacetimes suffers in general from an infinite ambiguity in the choice of Fock representation and associated vacuum. In cosmological backgrounds, the requirement of a unitary implementation of the field dynamics in the physical Hilbert space of the theory is a good criterion to ameliorate... | 8.234543 | 8.698779 | 7.413341 | 7.362854 | 8.144408 | 7.994532 | 8.389473 | 7.471642 | 8.099695 | 8.372768 | 7.978727 | 7.672244 | 7.552993 | 7.69662 | 7.751339 | 7.780891 | 7.673647 | 7.545044 | 7.836517 | 7.950947 | 7.692876 |
hep-th/0303038 | Boris Blankleider | A. N. Kvinikhidze and B. Blankleider | Gauge invariant reduction to the light-front | 12 pages, revtex4 | Phys.Rev.D68:025021,2003 | 10.1103/PhysRevD.68.025021 | null | hep-th hep-ph nucl-th | null | The problem of constructing gauge invariant currents in terms of light-cone
bound-state wave functions is solved by utilising the gauging of equations
method. In particular, it is shown how to construct perturbative expansions of
the electromagnetic current in the light-cone formalism, such that current
conservation ... | [
{
"created": "Wed, 5 Mar 2003 17:38:47 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Kvinikhidze",
"A. N.",
""
],
[
"Blankleider",
"B.",
""
]
] | The problem of constructing gauge invariant currents in terms of light-cone bound-state wave functions is solved by utilising the gauging of equations method. In particular, it is shown how to construct perturbative expansions of the electromagnetic current in the light-cone formalism, such that current conservation is... | 9.996797 | 9.606949 | 9.256386 | 7.949137 | 8.971273 | 9.357394 | 9.579199 | 10.172852 | 9.634853 | 9.455457 | 9.825429 | 9.883337 | 9.36526 | 9.484715 | 9.513953 | 9.727505 | 9.651319 | 9.774315 | 9.518866 | 8.431406 | 9.564787 |
hep-th/0307275 | Soo-Jong Rey | Oleg Lunin, Soo-Jong Rey | Renormalizability of Non(anti)commutative Gauge Theories with N=1/2
Supersymmetry | 21 pages, Latex, 2 figs; v2. minor corrections | JHEP 0309 (2003) 045 | 10.1088/1126-6708/2003/09/045 | SNUST 030702 | hep-th | null | Non(anti)commutative gauge theories are supersymmetric Yang-Mills and matter
system defined on a deformed superspace whose coordinates obey
non(anti)commutative algebra. We prove that these theories in four dimensions
with N=1/2 supersymmetry are renormalizable to all orders in perturbation
theory. Our proof is based... | [
{
"created": "Tue, 29 Jul 2003 18:27:03 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Aug 2003 18:37:55 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Lunin",
"Oleg",
""
],
[
"Rey",
"Soo-Jong",
""
]
] | Non(anti)commutative gauge theories are supersymmetric Yang-Mills and matter system defined on a deformed superspace whose coordinates obey non(anti)commutative algebra. We prove that these theories in four dimensions with N=1/2 supersymmetry are renormalizable to all orders in perturbation theory. Our proof is based o... | 7.914052 | 7.591872 | 7.649582 | 6.985096 | 7.518678 | 7.62861 | 7.550567 | 7.257338 | 7.067219 | 8.098828 | 7.002852 | 7.128424 | 7.2289 | 6.859842 | 7.196193 | 7.126105 | 6.980814 | 6.897285 | 6.825001 | 7.25595 | 7.101433 |
hep-th/0601082 | Sera Cremonini | Sera Cremonini and Scott Watson | Dilaton Dynamics from Production of Tensionless Membranes | 39 pages, 7 figures, minor corrections and reference added | Phys.Rev.D73:086007,2006 | 10.1103/PhysRevD.73.086007 | null | hep-th astro-ph gr-qc hep-ph | null | In this paper we consider classical and quantum corrections to cosmological
solutions of 11D SUGRA coming from dynamics of membrane states. We first
consider the supermembrane spectrum following the approach of Russo and
Tseytlin for consistent quantization. We calculate the production rate of BPS
membrane bound stat... | [
{
"created": "Fri, 13 Jan 2006 20:56:24 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jan 2006 21:19:42 GMT",
"version": "v2"
},
{
"created": "Tue, 24 Jan 2006 04:07:38 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Cremonini",
"Sera",
""
],
[
"Watson",
"Scott",
""
]
] | In this paper we consider classical and quantum corrections to cosmological solutions of 11D SUGRA coming from dynamics of membrane states. We first consider the supermembrane spectrum following the approach of Russo and Tseytlin for consistent quantization. We calculate the production rate of BPS membrane bound states... | 13.038974 | 13.556671 | 12.975902 | 12.876475 | 13.497021 | 13.887939 | 12.544057 | 13.81105 | 12.458145 | 14.513206 | 13.279025 | 12.241488 | 12.703942 | 12.539034 | 12.68111 | 12.433881 | 12.386732 | 12.410372 | 12.255903 | 13.076897 | 12.387148 |
0710.4034 | Delsate T\'erence | Y. Brihaye, T. Delsate, E. Radu | On the stability of AdS black strings | 8 pages, 4 figures ; reference added | Phys.Lett.B662:264-269,2008 | 10.1016/j.physletb.2008.03.008 | null | hep-th | null | We explore via linearized perturbation theory the Gregory-Laflamme
instability of the black string solutions of Einstein's equations with negative
cosmological constant recently discussed in literature. Our results indicate
that the black strings whose conformal infinity is the product of time and
$S^{d-3}\times S^1$... | [
{
"created": "Mon, 22 Oct 2007 12:23:22 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Nov 2007 10:01:32 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Brihaye",
"Y.",
""
],
[
"Delsate",
"T.",
""
],
[
"Radu",
"E.",
""
]
] | We explore via linearized perturbation theory the Gregory-Laflamme instability of the black string solutions of Einstein's equations with negative cosmological constant recently discussed in literature. Our results indicate that the black strings whose conformal infinity is the product of time and $S^{d-3}\times S^1$ a... | 8.830858 | 7.402451 | 8.586308 | 7.116706 | 6.529671 | 6.820131 | 7.512331 | 7.74605 | 7.475924 | 8.980093 | 7.468919 | 7.711187 | 8.356389 | 7.927115 | 7.850129 | 7.774786 | 7.907172 | 7.75637 | 8.169583 | 8.161049 | 7.947707 |
1311.4619 | In Yong Park | I. Y. Park | Reduction of BTZ spacetime to hypersurfaces of foliation | 16 pages, minor corrections, version that will appear in JHEP | null | 10.1007/JHEP01(2014)102 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reduce the BTZ spacetime to two kinds of hypersurfaces of foliation: one
having a fixed radial coordinate and the other a fixed angular coordinate. The
radial reduction leads to a Liouville type theory, and confirms, from the first
principle, the expectation laid out in the literature. In the other endeavor,
the a... | [
{
"created": "Tue, 19 Nov 2013 04:42:22 GMT",
"version": "v1"
},
{
"created": "Sun, 24 Nov 2013 16:05:08 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Dec 2013 09:30:44 GMT",
"version": "v3"
},
{
"created": "Thu, 16 Jan 2014 14:23:51 GMT",
"version": "v4"
}
] | 2015-06-17 | [
[
"Park",
"I. Y.",
""
]
] | We reduce the BTZ spacetime to two kinds of hypersurfaces of foliation: one having a fixed radial coordinate and the other a fixed angular coordinate. The radial reduction leads to a Liouville type theory, and confirms, from the first principle, the expectation laid out in the literature. In the other endeavor, the ang... | 13.647717 | 12.581153 | 12.303347 | 11.985209 | 12.676029 | 12.256005 | 11.895609 | 12.54907 | 12.464658 | 13.308279 | 11.559764 | 12.093345 | 13.083982 | 11.967654 | 12.629208 | 12.096061 | 12.3009 | 12.098204 | 12.412866 | 12.598893 | 12.260293 |
hep-th/9409142 | Timothy Hollowood | Jonathan M. Evans and Timothy J. Hollowood | The Exact Mass-Gap of the Supersymmetric CP^{n-1} Sigam Model | Plain TeX (macro included), CERN-TH.7426/94, SWAT/93-94/42 | Phys.Lett. B343 (1995) 198-206 | 10.1016/0370-2693(94)01478-U | null | hep-th | null | A formula for the mass-gap of the supersymmetric $\CP^{n-1}$ sigma model ($n
> 1$) in two dimensions is derived: $m/\Lambda_{\overline{\rm
MS}}=\sin(\pi\Delta)/(\pi\Delta)$ where $\Delta=1/n$ and $m$ is the mass of the
fundamental particle multiplet. This result is obtained by comparing two
expressions for the free-e... | [
{
"created": "Fri, 23 Sep 1994 09:55:12 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Evans",
"Jonathan M.",
""
],
[
"Hollowood",
"Timothy J.",
""
]
] | A formula for the mass-gap of the supersymmetric $\CP^{n-1}$ sigma model ($n > 1$) in two dimensions is derived: $m/\Lambda_{\overline{\rm MS}}=\sin(\pi\Delta)/(\pi\Delta)$ where $\Delta=1/n$ and $m$ is the mass of the fundamental particle multiplet. This result is obtained by comparing two expressions for the free-ene... | 6.354531 | 5.081308 | 7.812214 | 5.989575 | 5.23788 | 5.025115 | 5.707617 | 5.842353 | 5.664083 | 8.307313 | 6.359028 | 5.837289 | 7.161419 | 6.16304 | 5.993318 | 5.960758 | 5.736462 | 6.133662 | 6.2614 | 6.701686 | 6.142168 |
hep-th/0511051 | Dongsu Bak | Dongsu Bak, Kyungyu Kim and Nobuyoshi Ohta | M-theory Supertubes with Three and Four Charges | 24 pages, references added and typos corrected | JHEP0601:072,2006 | 10.1088/1126-6708/2006/01/072 | UOSTP 5101, OU-HET 544 | hep-th | null | Using the covariant M5-brane action, we construct configurations
corresponding to supertubes with three and four charges. We derive the BPS
equations and study the full structure of the solutions. In particular, we find
new solutions involving arbitrariness in field strengths.
| [
{
"created": "Fri, 4 Nov 2005 06:14:41 GMT",
"version": "v1"
},
{
"created": "Sun, 6 Nov 2005 14:11:46 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Nov 2005 14:34:56 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Bak",
"Dongsu",
""
],
[
"Kim",
"Kyungyu",
""
],
[
"Ohta",
"Nobuyoshi",
""
]
] | Using the covariant M5-brane action, we construct configurations corresponding to supertubes with three and four charges. We derive the BPS equations and study the full structure of the solutions. In particular, we find new solutions involving arbitrariness in field strengths. | 12.478374 | 10.004276 | 13.95629 | 9.445777 | 9.096896 | 9.314073 | 9.841881 | 9.638269 | 9.023488 | 12.183877 | 9.154657 | 9.802695 | 11.111564 | 10.213248 | 9.702693 | 9.590936 | 10.242739 | 10.11077 | 10.196307 | 11.400195 | 10.142411 |
2205.07817 | Stephen Ebert | Stephen Ebert, Christian Ferko, Hao-Yu Sun, Zhengdi Sun | $T\bar{T}$ in JT Gravity and BF Gauge Theory | 92 pages | SciPost Phys. 13, 096 (2022) | 10.21468/SciPostPhys.13.4.096 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | JT gravity has a first-order formulation as a two-dimensional BF theory,
which can be viewed as the dimensional reduction of the Chern-Simons
description of $3d$ gravity. We consider $T\bar{T}$-type deformations of the
$(0+1)$-dimensional dual to this $2d$ BF theory and interpret the deformation
as a modification of ... | [
{
"created": "Mon, 16 May 2022 17:17:07 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Jun 2022 07:39:28 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Aug 2022 09:46:07 GMT",
"version": "v3"
}
] | 2022-10-19 | [
[
"Ebert",
"Stephen",
""
],
[
"Ferko",
"Christian",
""
],
[
"Sun",
"Hao-Yu",
""
],
[
"Sun",
"Zhengdi",
""
]
] | JT gravity has a first-order formulation as a two-dimensional BF theory, which can be viewed as the dimensional reduction of the Chern-Simons description of $3d$ gravity. We consider $T\bar{T}$-type deformations of the $(0+1)$-dimensional dual to this $2d$ BF theory and interpret the deformation as a modification of th... | 6.707385 | 6.672915 | 7.82955 | 6.208614 | 6.649206 | 6.320286 | 6.083798 | 6.257073 | 6.431189 | 7.757424 | 6.572761 | 6.343399 | 6.481623 | 6.237215 | 6.327024 | 6.360286 | 6.280962 | 6.194011 | 6.324744 | 6.874542 | 6.413043 |
hep-th/9408157 | Li Jian-ming | Jianming Li | Matrix Realization of Gauge Theory on Discrete Group $Z_2$ | Latex file, 10 pages, ASITP-94-9 | null | null | null | hep-th | null | We construct a $2\times 2$ matrix algebra as representation of functions on
discrete group $Z_2$ and develop the gauge theory on discrete group proposed by
Starz in the matrix algebra. Accordingly, we show that the non-commutative
geometry model built by R.Conquereax, G.Esposito-Farese and G.Vaillant results
from thi... | [
{
"created": "Mon, 29 Aug 1994 21:03:53 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Li",
"Jianming",
""
]
] | We construct a $2\times 2$ matrix algebra as representation of functions on discrete group $Z_2$ and develop the gauge theory on discrete group proposed by Starz in the matrix algebra. Accordingly, we show that the non-commutative geometry model built by R.Conquereax, G.Esposito-Farese and G.Vaillant results from this ... | 23.758286 | 26.020451 | 21.252102 | 21.903597 | 25.02253 | 28.825453 | 33.000957 | 23.921103 | 20.809381 | 25.321749 | 22.37812 | 21.860682 | 22.322771 | 20.749229 | 21.395992 | 22.448608 | 20.976053 | 20.156017 | 20.348129 | 22.173311 | 20.304424 |
0807.3453 | David Richards | David M. Richards | The One-Loop H^2R^3 and H^2(DH)^2R Terms in the Effective Action | 20 pages, 3 figures; corrected typos | JHEP 0810:043,2008 | 10.1088/1126-6708/2008/10/043 | DAMTP-2008-61 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the one-loop B^2h^3 and B^4h amplitudes in type II string theory,
where B is the NS-NS two-form and h the graviton, and expand to lowest order in
alpha'. After subtracting diagrams due to quartic terms in the effective
action, we determine the presence and structure of both an H^2R^3 and
H^2(DH)^2R term. ... | [
{
"created": "Tue, 22 Jul 2008 11:08:07 GMT",
"version": "v1"
},
{
"created": "Sun, 1 Mar 2009 14:42:32 GMT",
"version": "v2"
}
] | 2011-08-04 | [
[
"Richards",
"David M.",
""
]
] | We consider the one-loop B^2h^3 and B^4h amplitudes in type II string theory, where B is the NS-NS two-form and h the graviton, and expand to lowest order in alpha'. After subtracting diagrams due to quartic terms in the effective action, we determine the presence and structure of both an H^2R^3 and H^2(DH)^2R term. We... | 10.392739 | 8.942812 | 11.426487 | 8.414916 | 9.934171 | 10.934029 | 10.40557 | 9.951462 | 8.779827 | 12.624674 | 9.820895 | 9.820342 | 9.922893 | 9.201764 | 10.37242 | 10.834836 | 10.447787 | 10.158409 | 9.381789 | 10.576736 | 10.364612 |
hep-th/0612067 | Takuya Okuda | Mina Aganagic, Takuya Okuda, Hirosi Ooguri | Quantum Entanglement of Baby Universes | 42 pages; v.2 typos corrected | Nucl.Phys.B778:36-68,2007 | 10.1016/j.nuclphysb.2007.04.006 | CALT-68-2622, NSF-KITP-06-118 | hep-th gr-qc quant-ph | null | We study quantum entanglements of baby universes which appear in
non-perturbative corrections to the OSV formula for the entropy of extremal
black holes in Type IIA string theory compactified on the local Calabi-Yau
manifold defined as a rank 2 vector bundle over an arbitrary genus G Riemann
surface. This generalizes... | [
{
"created": "Thu, 7 Dec 2006 22:21:47 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jun 2007 20:55:38 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Aganagic",
"Mina",
""
],
[
"Okuda",
"Takuya",
""
],
[
"Ooguri",
"Hirosi",
""
]
] | We study quantum entanglements of baby universes which appear in non-perturbative corrections to the OSV formula for the entropy of extremal black holes in Type IIA string theory compactified on the local Calabi-Yau manifold defined as a rank 2 vector bundle over an arbitrary genus G Riemann surface. This generalizes t... | 7.806211 | 9.446746 | 9.897888 | 8.307287 | 9.19379 | 9.089871 | 9.992267 | 8.722779 | 8.652835 | 9.687047 | 8.331604 | 8.095214 | 8.126197 | 7.627314 | 7.957886 | 7.89554 | 7.923157 | 7.849146 | 7.945035 | 8.157377 | 7.808272 |
hep-th/0605293 | Michael T. Anderson | Michael T. Anderson | On the uniqueness and global dynamics of AdS spacetimes | 18pp, significant revision of v1 | Class.Quant.Grav.23:6935-6954,2006 | 10.1088/0264-9381/23/23/021 | null | hep-th gr-qc math.DG | null | We study global aspects of complete, non-singular asymptotically locally AdS
spacetimes solving the vacuum Einstein equations whose conformal infinity is an
arbitrary globally stationary spacetime. It is proved that any such solution
which is asymptotically stationary to the past and future is itself globally
station... | [
{
"created": "Wed, 31 May 2006 16:32:25 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Jun 2006 17:11:09 GMT",
"version": "v2"
},
{
"created": "Thu, 10 Aug 2006 19:34:33 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Anderson",
"Michael T.",
""
]
] | We study global aspects of complete, non-singular asymptotically locally AdS spacetimes solving the vacuum Einstein equations whose conformal infinity is an arbitrary globally stationary spacetime. It is proved that any such solution which is asymptotically stationary to the past and future is itself globally stationar... | 10.972705 | 11.987524 | 10.724359 | 11.01806 | 11.304962 | 12.992846 | 12.798621 | 10.451364 | 12.729798 | 12.930803 | 11.624827 | 11.92046 | 11.265609 | 10.775513 | 10.676859 | 10.364671 | 11.014151 | 10.630884 | 11.471447 | 11.127232 | 11.31202 |
2407.13556 | Javier Peraza | Silvia Nagy, Javier Peraza, Giorgio Pizzolo | Infinite-dimensional hierarchy of recursive extensions for all
sub$^n$-leading soft effects in Yang-Mills | 51 Pages, 4 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Building on our proposal in arXiv:2405.06629, we present in detail the
construction of the extended phase space for Yang-Mills at null infinity,
containing the asymptotic symmetries and the charges responsible for
sub$^n$-leading soft theorems at all orders. The generality of the procedure
allows it to be directly ap... | [
{
"created": "Thu, 18 Jul 2024 14:29:05 GMT",
"version": "v1"
}
] | 2024-07-19 | [
[
"Nagy",
"Silvia",
""
],
[
"Peraza",
"Javier",
""
],
[
"Pizzolo",
"Giorgio",
""
]
] | Building on our proposal in arXiv:2405.06629, we present in detail the construction of the extended phase space for Yang-Mills at null infinity, containing the asymptotic symmetries and the charges responsible for sub$^n$-leading soft theorems at all orders. The generality of the procedure allows it to be directly appl... | 13.930646 | 13.535165 | 14.70011 | 13.045037 | 13.5139 | 13.788204 | 13.378308 | 13.158381 | 13.144455 | 14.149499 | 13.690476 | 13.407235 | 13.614852 | 13.666965 | 13.325974 | 13.181619 | 13.253602 | 13.167657 | 13.12619 | 13.944575 | 13.029254 |
hep-th/0007132 | Norman Dombey | N Dombey, P Kennedy and A Calogeracos | Supercriticality and Transmission Resonances in the Dirac equation | Submitted to Physical Review Letters | Phys.Rev.Lett. 85 (2000) 1787-1790 | 10.1103/PhysRevLett.85.1787 | SUSX-TH/00-011 | hep-th math-ph math.MP quant-ph | null | It is shown that a Dirac particle of mass $m$ and arbitrarily small momentum
will tunnel without reflection through a potential barrier $V=U_c(x)$ of finite
range provided that the potential well $V=-U_c(x)$ supports a bound state of
energy $E=-m.$ This is called a supercritical potential well.
| [
{
"created": "Mon, 17 Jul 2000 13:24:43 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Dombey",
"N",
""
],
[
"Kennedy",
"P",
""
],
[
"Calogeracos",
"A",
""
]
] | It is shown that a Dirac particle of mass $m$ and arbitrarily small momentum will tunnel without reflection through a potential barrier $V=U_c(x)$ of finite range provided that the potential well $V=-U_c(x)$ supports a bound state of energy $E=-m.$ This is called a supercritical potential well. | 10.395967 | 10.80721 | 10.333599 | 9.043419 | 9.560565 | 10.460883 | 9.211907 | 10.195413 | 10.113676 | 10.306406 | 9.722853 | 10.150056 | 9.62551 | 9.515664 | 9.931515 | 9.727105 | 10.038457 | 9.743671 | 9.714051 | 8.627559 | 9.572541 |
hep-th/9702195 | Juergen Fuchs | J. Fuchs | Universal simple current vertex operators | 17 pages, LaTeX2e | Annals Phys. 266 (1998) 254-273 | 10.1006/aphy.1998.9999 | DESY 97-023 | hep-th | null | We construct a vertex operator realization for the simple current primary
fields of WZW theories which are based on simply laced affine Lie algebras g.
This is achieved by employing an embedding of the integrable highest weight
modules of g into the Fock space for a bosonic string compactified on the
weight lattice o... | [
{
"created": "Thu, 27 Feb 1997 15:40:40 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Fuchs",
"J.",
""
]
] | We construct a vertex operator realization for the simple current primary fields of WZW theories which are based on simply laced affine Lie algebras g. This is achieved by employing an embedding of the integrable highest weight modules of g into the Fock space for a bosonic string compactified on the weight lattice of ... | 8.186451 | 7.661532 | 9.834119 | 7.334496 | 7.454861 | 7.093232 | 8.260508 | 7.269268 | 6.808278 | 9.831008 | 6.825659 | 7.780952 | 7.851566 | 7.804953 | 7.924207 | 7.557501 | 7.633639 | 7.701411 | 7.747907 | 7.942906 | 7.544233 |
1801.10174 | Konstantinos Siampos | Eftychia Sagkrioti, Konstantinos Sfetsos, Konstantinos Siampos | RG flows for $\lambda$-deformed CFTs | v1: 1+19 pages, Latex; v2: NPB version; v3: Mild simplifications of
the conventions in section 2.1.2 | null | 10.1016/j.nuclphysb.2018.03.013 | CERN-TH-2018-017 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the renormalization group equations of the fully anisotropic
$\lambda$-deformed CFTs involving the direct product of two current algebras at
different levels $k_{1,2}$ for general semi-simple groups. The exact, in the
deformation parameters, $\beta$-function is found via the effective action of
the quantum f... | [
{
"created": "Tue, 30 Jan 2018 19:00:39 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Mar 2018 10:01:46 GMT",
"version": "v2"
},
{
"created": "Tue, 15 May 2018 12:18:12 GMT",
"version": "v3"
}
] | 2018-05-16 | [
[
"Sagkrioti",
"Eftychia",
""
],
[
"Sfetsos",
"Konstantinos",
""
],
[
"Siampos",
"Konstantinos",
""
]
] | We study the renormalization group equations of the fully anisotropic $\lambda$-deformed CFTs involving the direct product of two current algebras at different levels $k_{1,2}$ for general semi-simple groups. The exact, in the deformation parameters, $\beta$-function is found via the effective action of the quantum flu... | 16.91004 | 15.751027 | 17.646753 | 15.829378 | 15.907966 | 16.801582 | 16.099632 | 15.740193 | 15.372048 | 17.667786 | 15.2228 | 16.225025 | 16.186754 | 15.920201 | 16.601105 | 15.992419 | 15.511015 | 16.037024 | 16.066364 | 17.127214 | 15.251675 |
2006.11326 | Luciano Abreu | L. M. Abreu, M. de Montigny and P. P. A. Ouimet | An effective field theory approach to monopolium | 14 pages, 9 figures, 2 tables; accepted for publication in The
European Physical Journal Plus | Eur. Phys. J. Plus 135, 543 (2020) | 10.1140/epjp/s13360-020-00550-1 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we investigate the interaction between spin-zero and spin-one
monopoles by making use of an effective field theory based on two-body and
four-body interaction parts. In particular, we analyze the formation of bound
state of monopole-antimonopole (i.e. monopolium). The magnetic-charge
conjugation symmetry... | [
{
"created": "Fri, 19 Jun 2020 19:01:29 GMT",
"version": "v1"
}
] | 2020-07-08 | [
[
"Abreu",
"L. M.",
""
],
[
"de Montigny",
"M.",
""
],
[
"Ouimet",
"P. P. A.",
""
]
] | In this work we investigate the interaction between spin-zero and spin-one monopoles by making use of an effective field theory based on two-body and four-body interaction parts. In particular, we analyze the formation of bound state of monopole-antimonopole (i.e. monopolium). The magnetic-charge conjugation symmetry i... | 12.835752 | 13.007968 | 12.666826 | 12.008235 | 12.151472 | 13.324686 | 12.434323 | 12.544715 | 11.747817 | 13.442241 | 12.789205 | 12.401551 | 11.810257 | 11.932027 | 11.894132 | 12.786634 | 11.859551 | 12.609227 | 11.933757 | 11.848834 | 12.556837 |
1510.09060 | Sang Kwan Choi | Sang Kwan Choi, Chaiho Rim, Hong Zhang | Irregular conformal block, spectral curve and flow equations | 35 pages; v2: 38 pages, section 4 and references added, minor changes | JHEP03(2016)118 | 10.1007/JHEP03(2016)118 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Irregular conformal block is motivated by the Argyres-Douglas type of N=2
super conformal gauge theory. We investigate the classical/NS limit of the
irregular conformal block using spectral curve on a Riemann surface with
irregular punctures, which is equivalent to the loop equation of irregular
matrix model. The spe... | [
{
"created": "Fri, 30 Oct 2015 12:43:04 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Mar 2016 10:08:51 GMT",
"version": "v2"
}
] | 2016-04-20 | [
[
"Choi",
"Sang Kwan",
""
],
[
"Rim",
"Chaiho",
""
],
[
"Zhang",
"Hong",
""
]
] | Irregular conformal block is motivated by the Argyres-Douglas type of N=2 super conformal gauge theory. We investigate the classical/NS limit of the irregular conformal block using spectral curve on a Riemann surface with irregular punctures, which is equivalent to the loop equation of irregular matrix model. The spect... | 7.533718 | 7.999485 | 10.032691 | 7.856062 | 8.004979 | 8.332492 | 8.784654 | 7.974741 | 8.050943 | 10.256058 | 8.192347 | 7.321154 | 8.461514 | 7.536404 | 7.651535 | 7.769453 | 7.834246 | 7.238025 | 7.472077 | 8.084793 | 7.915717 |
1702.03383 | Joseph C. V\'arilly | Jos\'e M. Gracia-Bond\'ia, Jens Mund and Joseph C. V\'arilly | The chirality theorem | Latex, 31 pages. v2: minor changes, 3 references added, author order
now alphabetical. v3: substantial rewrite to improve presentation,
conclusions unchanged. v4: minor edits to match published version, one
reference added. To appear in Annales Henri Poincar\'e | Annales Henri Poincar\'e 19 (2018) 843-874 | 10.1007/s00023-017-0637-3 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how chirality of the weak interactions stems from string independence
in the string-local formalism of quantum field theory.
| [
{
"created": "Sat, 11 Feb 2017 05:16:18 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Mar 2017 00:58:35 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Nov 2017 04:00:04 GMT",
"version": "v3"
},
{
"created": "Sat, 23 Dec 2017 17:00:12 GMT",
"version": "v4"
}
] | 2018-09-05 | [
[
"Gracia-Bondía",
"José M.",
""
],
[
"Mund",
"Jens",
""
],
[
"Várilly",
"Joseph C.",
""
]
] | We show how chirality of the weak interactions stems from string independence in the string-local formalism of quantum field theory. | 28.380442 | 29.444975 | 22.375692 | 29.755081 | 37.344151 | 30.806438 | 25.391346 | 23.682186 | 22.757568 | 30.488441 | 29.803415 | 30.044689 | 26.532986 | 27.118469 | 33.224903 | 30.564732 | 28.668623 | 29.415281 | 26.54871 | 27.684834 | 26.536057 |
1012.1697 | Taotao Qiu | Taotao Qiu and Kwei-Chou Yang | Non-Gaussianities of Single Field Inflation with Non-minimal Coupling | 19 pages, 6 figures, one more section added, analytical results
simplified | Phys.Rev.D83:084022,2011 | 10.1103/PhysRevD.83.084022 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the non-Gaussianities of inflation driven by a single scalar
field coupling non-minimally to the Einstein Gravity. We assume that the form
of the scalar field is very general with an arbitrary sound speed. For
convenience to study, we take the subclass that the non-minimal coupling term
is linear to th... | [
{
"created": "Wed, 8 Dec 2010 07:50:20 GMT",
"version": "v1"
},
{
"created": "Thu, 26 May 2011 06:13:27 GMT",
"version": "v2"
}
] | 2011-05-27 | [
[
"Qiu",
"Taotao",
""
],
[
"Yang",
"Kwei-Chou",
""
]
] | We investigate the non-Gaussianities of inflation driven by a single scalar field coupling non-minimally to the Einstein Gravity. We assume that the form of the scalar field is very general with an arbitrary sound speed. For convenience to study, we take the subclass that the non-minimal coupling term is linear to the ... | 7.69278 | 7.711745 | 7.786547 | 7.237224 | 7.809351 | 7.360998 | 8.36804 | 7.532732 | 7.506209 | 8.023401 | 7.789161 | 7.506865 | 7.661415 | 7.377885 | 7.318018 | 7.367274 | 7.696677 | 7.540092 | 7.429946 | 7.306511 | 7.234692 |
1812.08941 | Enrico Herrmann | Samuel Abreu, Lance J. Dixon, Enrico Herrmann, Ben Page, Mao Zeng | The two-loop five-point amplitude in $\mathcal{N} =4$ super-Yang-Mills
theory | 6pages, 1 figure, 1 table; v2: references added, fixed typos, flipped
overall sign of amplitude in ancillary files; v3: references and typos fixed | Phys. Rev. Lett. 122, 121603 (2019) | 10.1103/PhysRevLett.122.121603 | CP3-18-31, IPhT-18/170, SLAC-PUB-17369 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the symbol of the two-loop five-point scattering amplitude in
$\mathcal{N}$ = 4 super-Yang-Mills theory, including its full color dependence.
This requires constructing the symbol of all two-loop five-point nonplanar
massless master integrals, for which we give explicit results.
| [
{
"created": "Fri, 21 Dec 2018 04:32:39 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Jan 2019 20:41:36 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Mar 2019 02:42:06 GMT",
"version": "v3"
}
] | 2019-04-03 | [
[
"Abreu",
"Samuel",
""
],
[
"Dixon",
"Lance J.",
""
],
[
"Herrmann",
"Enrico",
""
],
[
"Page",
"Ben",
""
],
[
"Zeng",
"Mao",
""
]
] | We compute the symbol of the two-loop five-point scattering amplitude in $\mathcal{N}$ = 4 super-Yang-Mills theory, including its full color dependence. This requires constructing the symbol of all two-loop five-point nonplanar massless master integrals, for which we give explicit results. | 6.934533 | 4.61025 | 6.868544 | 5.227801 | 5.885 | 5.466803 | 5.367704 | 4.957297 | 5.228305 | 7.010184 | 5.791019 | 5.785251 | 5.641489 | 5.565464 | 5.770789 | 6.062529 | 5.703437 | 6.276132 | 5.227331 | 6.290085 | 5.578831 |
hep-th/9904162 | Alessandro Fabbri | R. Balbinot, A. Fabbri and I. Shapiro | Vacuum polarization in Schwarzschild space-time by anomaly induced
effective actions | 20 pages, latex; misprints corrected and references added | Nucl.Phys. B559 (1999) 301-319 | 10.1016/S0550-3213(99)00424-1 | SU-ITP-99-17 | hep-th gr-qc | null | The characteristic features of $<T_{\mu\nu}>$ in the Boulware, Unruh and
Hartle-Hawking states for a conformal massless scalar field propagating in the
Schwarzschild space-time are obtained by means of effective actions deduced by
the trace anomaly. The actions are made local by the introduction of auxiliary
fields a... | [
{
"created": "Mon, 26 Apr 1999 22:37:33 GMT",
"version": "v1"
},
{
"created": "Fri, 21 May 1999 22:41:23 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Balbinot",
"R.",
""
],
[
"Fabbri",
"A.",
""
],
[
"Shapiro",
"I.",
""
]
] | The characteristic features of $<T_{\mu\nu}>$ in the Boulware, Unruh and Hartle-Hawking states for a conformal massless scalar field propagating in the Schwarzschild space-time are obtained by means of effective actions deduced by the trace anomaly. The actions are made local by the introduction of auxiliary fields and... | 9.851195 | 8.087824 | 7.852551 | 6.994234 | 7.826757 | 6.884985 | 7.960855 | 6.511622 | 7.496071 | 8.759963 | 7.94081 | 7.784594 | 7.866007 | 7.801878 | 7.901474 | 7.767786 | 7.636137 | 7.43605 | 7.807259 | 7.888798 | 8.292647 |
2104.00601 | Jordan Cotler | Jordan Cotler, Kristan Jensen | Wormholes and black hole microstates in AdS/CFT | 64 pages, 6 figures; v2: modified discussion of brane nucleation in
wormholes with torus boundary, added references | null | 10.1007/JHEP09(2021)001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has long been known that the coarse-grained approximation to the black
hole density of states can be computed using classical Euclidean gravity. In
this work we argue for another entry in the dictionary between Euclidean
gravity and black hole physics, namely that Euclidean wormholes describe a
coarse-grained appr... | [
{
"created": "Thu, 1 Apr 2021 16:35:10 GMT",
"version": "v1"
},
{
"created": "Wed, 5 May 2021 22:08:37 GMT",
"version": "v2"
}
] | 2023-02-22 | [
[
"Cotler",
"Jordan",
""
],
[
"Jensen",
"Kristan",
""
]
] | It has long been known that the coarse-grained approximation to the black hole density of states can be computed using classical Euclidean gravity. In this work we argue for another entry in the dictionary between Euclidean gravity and black hole physics, namely that Euclidean wormholes describe a coarse-grained approx... | 8.696239 | 9.160838 | 9.928524 | 8.754714 | 9.370223 | 8.808169 | 8.685332 | 8.798238 | 8.539333 | 10.828382 | 8.785004 | 8.978164 | 9.035027 | 8.67076 | 8.762497 | 8.896246 | 8.806294 | 8.536797 | 8.728725 | 9.219273 | 8.679001 |
1606.08443 | Y\=uki Nakaguchi | Yuki Nakaguchi, Tatsuma Nishioka | A Holographic Proof of R\'enyi Entropic Inequalities | 29 pages, 1 figure; v3: references added, our assumption for the
proof clarified | null | 10.1007/JHEP12(2016)129 | IPMU-16-0090, UT-16-26 | hep-th cond-mat.str-el gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove R\'enyi entropic inequalities in a holographic setup based on the
recent proposal for the holographic formula of R\'enyi entropies when the bulk
is stable against any perturbation. Regarding the R\'enyi parameter as an
inverse temperature, we reformulate the entropies in analogy with statistical
mechanics, w... | [
{
"created": "Mon, 27 Jun 2016 20:00:02 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jul 2016 06:53:08 GMT",
"version": "v2"
},
{
"created": "Thu, 22 Dec 2016 07:01:59 GMT",
"version": "v3"
}
] | 2017-02-01 | [
[
"Nakaguchi",
"Yuki",
""
],
[
"Nishioka",
"Tatsuma",
""
]
] | We prove R\'enyi entropic inequalities in a holographic setup based on the recent proposal for the holographic formula of R\'enyi entropies when the bulk is stable against any perturbation. Regarding the R\'enyi parameter as an inverse temperature, we reformulate the entropies in analogy with statistical mechanics, whi... | 11.796677 | 10.692304 | 12.708605 | 9.900964 | 11.40118 | 10.450563 | 11.396681 | 11.124898 | 11.091562 | 13.337642 | 10.571308 | 10.304341 | 11.414362 | 10.356614 | 10.56028 | 10.256166 | 10.387779 | 10.481594 | 10.598682 | 11.63268 | 10.182185 |
hep-th/9910067 | Maximilian Kreuzer | M. Kreuzer and Jian-Ge Zhou | Killing gauge for the 0-brane on $AdS_2 \times S^2$ coset superspace | 14 pages, LaTeX2e | Phys.Lett. B472 (2000) 309-315 | 10.1016/S0370-2693(99)01443-4 | TUW-99/23 | hep-th | null | How to gauge fix $\k$-symmetry for the super 0-brane action on $AdS_2 \times
S^2$ in Killing gauge properly is discussed in order to find the superconformal
mechanics which describes super 0-brane probes moving on $AdS_2 \times S^2$.
The dependence on the coordinate frame for the proper Killing gauge is
considered an... | [
{
"created": "Thu, 7 Oct 1999 15:24:08 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Kreuzer",
"M.",
""
],
[
"Zhou",
"Jian-Ge",
""
]
] | How to gauge fix $\k$-symmetry for the super 0-brane action on $AdS_2 \times S^2$ in Killing gauge properly is discussed in order to find the superconformal mechanics which describes super 0-brane probes moving on $AdS_2 \times S^2$. The dependence on the coordinate frame for the proper Killing gauge is considered and ... | 12.346439 | 10.860168 | 12.434527 | 9.849923 | 11.140951 | 11.064432 | 11.170623 | 9.935342 | 10.219496 | 12.22173 | 10.037225 | 9.869502 | 10.540242 | 9.730655 | 9.520949 | 9.720378 | 9.398047 | 9.496528 | 9.756462 | 10.522957 | 9.759186 |
hep-th/0001148 | Liangzhong | L.Z. Hu (Peking University) | U(1) gauge theory over discrete space-time and phase transitions | 12 pages | null | null | IMH-99-08 | hep-th | null | We first apply Connes' noncommutative geometry to a finite point space. The
explicit form of the action functional of U(1) gauge field on this n-point
space is obtained. We then consider the case when the n-point space is replaced
by {space-time}\times{n-point space}. This action is shown to relate the
Hamiltonian of... | [
{
"created": "Sat, 22 Jan 2000 09:03:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Hu",
"L. Z.",
"",
"Peking University"
]
] | We first apply Connes' noncommutative geometry to a finite point space. The explicit form of the action functional of U(1) gauge field on this n-point space is obtained. We then consider the case when the n-point space is replaced by {space-time}\times{n-point space}. This action is shown to relate the Hamiltonian of t... | 14.704499 | 14.900408 | 15.338058 | 13.250823 | 14.476835 | 15.210519 | 13.606496 | 14.713316 | 13.224117 | 15.016013 | 12.965823 | 13.933287 | 14.01061 | 13.660616 | 13.57828 | 13.812703 | 13.704515 | 13.918906 | 14.381068 | 13.614634 | 13.678734 |
2108.12090 | Yosuke Imamura | Yosuke Imamura | Finite-$N$ superconformal index via the AdS/CFT correspondence | 31 pages, 7 figures | null | null | TIT/HEP-686 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We propose a prescription to calculate the superconformal index of the ${\cal
N}=4$ $U(N)$ supersymmetric Yang-Mills theory with finite $N$ on the AdS side.
The finite $N$ corrections are included as contributions of D3-branes wrapped
around three-cycles in $\boldsymbol{S}^5$, which are calculated as the index of
the... | [
{
"created": "Fri, 27 Aug 2021 02:26:03 GMT",
"version": "v1"
}
] | 2021-08-30 | [
[
"Imamura",
"Yosuke",
""
]
] | We propose a prescription to calculate the superconformal index of the ${\cal N}=4$ $U(N)$ supersymmetric Yang-Mills theory with finite $N$ on the AdS side. The finite $N$ corrections are included as contributions of D3-branes wrapped around three-cycles in $\boldsymbol{S}^5$, which are calculated as the index of the g... | 7.22731 | 6.193594 | 7.702416 | 6.405134 | 6.044897 | 6.547244 | 6.270475 | 6.61634 | 6.213047 | 7.804778 | 6.146171 | 6.528354 | 7.517715 | 6.560543 | 6.329748 | 6.290107 | 6.365194 | 6.537748 | 6.688197 | 7.231251 | 6.573779 |
1310.4821 | Alexander Zamolodchikov | Alexander Zamolodchikov | Ising Spectroscopy II: Particles and poles at T>Tc | null | null | null | RUNHETC-2013-20 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I discuss particle content of the Ising field theory (the scaling limit of
the Ising model in a magnetic field), in particular the evolution of its mass
spectrum under the change of the scaling parameter. I consider both real and
pure imaginary magnetic field. Here I address the high-temperature regime,
where the spe... | [
{
"created": "Thu, 17 Oct 2013 19:52:42 GMT",
"version": "v1"
}
] | 2013-10-18 | [
[
"Zamolodchikov",
"Alexander",
""
]
] | I discuss particle content of the Ising field theory (the scaling limit of the Ising model in a magnetic field), in particular the evolution of its mass spectrum under the change of the scaling parameter. I consider both real and pure imaginary magnetic field. Here I address the high-temperature regime, where the spect... | 12.413369 | 13.904012 | 13.657496 | 12.364609 | 12.832372 | 15.016247 | 13.103446 | 11.666507 | 12.34923 | 15.868485 | 11.825711 | 12.044839 | 12.145573 | 11.763176 | 12.160509 | 11.929731 | 11.569963 | 11.654822 | 12.18893 | 12.280514 | 11.819429 |
hep-th/0207119 | Ira Wasserman | Gary Shiu, S.-H. Henry Tye and Ira Wasserman | Rolling Tachyon in Brane World Cosmology from Superstring Field Theory | 4 pages, one figure. This version quantifies constraints on various
phenomenological models for tachyon decay | Phys.Rev. D67 (2003) 083517 | 10.1103/PhysRevD.67.083517 | null | hep-th gr-qc | null | The pressureless tachyonic matter recently found in superstring field theory
has an over-abundance problem in cosmology. We argue that this problem is
naturally solved in the brane inflationary scenario if almost all of the
tachyon energy is drained (via its coupling to the inflaton and matter fields)
to heating the ... | [
{
"created": "Fri, 12 Jul 2002 15:54:55 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jul 2002 17:39:58 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Jul 2002 17:54:03 GMT",
"version": "v3"
},
{
"created": "Tue, 8 Oct 2002 16:40:46 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Shiu",
"Gary",
""
],
[
"Tye",
"S. -H. Henry",
""
],
[
"Wasserman",
"Ira",
""
]
] | The pressureless tachyonic matter recently found in superstring field theory has an over-abundance problem in cosmology. We argue that this problem is naturally solved in the brane inflationary scenario if almost all of the tachyon energy is drained (via its coupling to the inflaton and matter fields) to heating the un... | 11.560103 | 11.085846 | 12.03842 | 10.206486 | 10.305312 | 10.823093 | 10.296991 | 10.166596 | 9.759745 | 11.68579 | 9.862246 | 9.515918 | 11.346503 | 10.057455 | 9.943863 | 10.018172 | 9.450753 | 9.575249 | 9.879378 | 10.742522 | 9.922674 |
0903.0511 | Vladimir Dobrev | V.K. Dobrev | Note on Centrally Extended su(2/2) and Serre Relations | 6 pages, LATEX, v2: added references; v3: small changes and added
reference | Fortsch.Phys.57:542-545,2009 | 10.1002/prop.200900052 | null | hep-th math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We point out that the nontrivial central extension of the superalgebra
$su(2/2)$ is related to the some not so well-known Serre relations.
| [
{
"created": "Tue, 3 Mar 2009 12:02:53 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Mar 2009 15:32:31 GMT",
"version": "v2"
},
{
"created": "Wed, 11 Mar 2009 17:01:51 GMT",
"version": "v3"
}
] | 2009-08-03 | [
[
"Dobrev",
"V. K.",
""
]
] | We point out that the nontrivial central extension of the superalgebra $su(2/2)$ is related to the some not so well-known Serre relations. | 14.954619 | 9.511835 | 15.026101 | 9.373154 | 10.79452 | 10.341774 | 10.953564 | 10.478384 | 9.772013 | 13.144925 | 10.665448 | 10.837461 | 14.080198 | 11.474864 | 11.626266 | 11.413481 | 10.680884 | 11.226289 | 10.749235 | 12.911576 | 11.355566 |
1308.5828 | Dmitriy Pak | L.P. Zou, P.M. Zhang and D.G. Pak | Monopoles without magnetic charges: Finite energy monopole-antimonopole
configurations in CP1 model and restricted QCD | 8 pages, 8 figures, 1 table, final version accepted by Phys. Lett. B | Physics Letters B 728C (2014), pp. 650-657 | 10.1016/j.physletb.2013.12.043 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new type of regular monopole-like field configuration in quantum
chromodynamics (QCD) and CP^1 model. The monopole configuration can be treated
as a monopole-antimonopole pair without localized magnetic charges. An exact
numeric solution for a simple monopole-antimonopole solution has been obtained
in CP... | [
{
"created": "Tue, 27 Aug 2013 11:38:13 GMT",
"version": "v1"
},
{
"created": "Sat, 31 Aug 2013 13:26:10 GMT",
"version": "v2"
},
{
"created": "Mon, 30 Dec 2013 03:46:07 GMT",
"version": "v3"
}
] | 2014-01-07 | [
[
"Zou",
"L. P.",
""
],
[
"Zhang",
"P. M.",
""
],
[
"Pak",
"D. G.",
""
]
] | We propose a new type of regular monopole-like field configuration in quantum chromodynamics (QCD) and CP^1 model. The monopole configuration can be treated as a monopole-antimonopole pair without localized magnetic charges. An exact numeric solution for a simple monopole-antimonopole solution has been obtained in CP^1... | 8.977845 | 7.565198 | 8.8859 | 7.46771 | 7.930466 | 7.509272 | 7.506242 | 7.980183 | 7.779672 | 9.601353 | 8.163896 | 8.153179 | 9.173135 | 8.323442 | 7.965385 | 8.230395 | 8.1719 | 8.337467 | 8.262382 | 8.92038 | 8.3269 |
2104.04536 | Elizabeth Wildenhain | Ning Bao and Elizabeth Wildenhain | Black Hole Cannibalism | 6 pages, 2 figures; Essay written for the Gravity Research Foundation
2021 Awards for Essays on Gravitation | null | 10.1142/S0218271821420190 | null | hep-th gr-qc quant-ph | http://creativecommons.org/licenses/by/4.0/ | We consider a version of the Hayden-Preskill thought experiment in which the
message thrown into the black hole is itself a smaller black hole. We then
discuss the implications of the existence of a recovery channel for this black
hole message at asymptotic infinity, resulting in a sharpening of the black
hole inform... | [
{
"created": "Fri, 9 Apr 2021 18:00:10 GMT",
"version": "v1"
}
] | 2022-01-26 | [
[
"Bao",
"Ning",
""
],
[
"Wildenhain",
"Elizabeth",
""
]
] | We consider a version of the Hayden-Preskill thought experiment in which the message thrown into the black hole is itself a smaller black hole. We then discuss the implications of the existence of a recovery channel for this black hole message at asymptotic infinity, resulting in a sharpening of the black hole informat... | 11.557381 | 11.398513 | 12.278049 | 10.268002 | 12.608488 | 11.60139 | 12.371193 | 11.542533 | 11.466684 | 11.746688 | 10.688846 | 10.661993 | 10.924697 | 11.013463 | 11.311459 | 11.433226 | 10.843328 | 11.755779 | 10.952885 | 11.497246 | 10.970125 |
0812.3595 | Ivan Gonzalez | Ivan Gonzalez, Ivan Schmidt | Modular application of an Integration by Fractional Expansion (IBFE)
method to multiloop Feynman diagrams II | 18 pages, 10 figures, 1 table | Phys.Rev.D79:126014,2009 | 10.1103/PhysRevD.79.126014 | USM-TH-242 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A modular application of the integration by fractional expansion (IBFE)
method for evaluating Feynman diagrams is extended to diagrams that contain
loop triangle subdiagrams in their geometry. The technique is based in the
replacement of this module or subdiagram by its corresponding multiregion
expansion (MRE), whic... | [
{
"created": "Thu, 18 Dec 2008 19:09:05 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jun 2009 13:31:03 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Jun 2009 17:30:37 GMT",
"version": "v3"
}
] | 2009-07-09 | [
[
"Gonzalez",
"Ivan",
""
],
[
"Schmidt",
"Ivan",
""
]
] | A modular application of the integration by fractional expansion (IBFE) method for evaluating Feynman diagrams is extended to diagrams that contain loop triangle subdiagrams in their geometry. The technique is based in the replacement of this module or subdiagram by its corresponding multiregion expansion (MRE), which ... | 15.654354 | 16.132158 | 16.840473 | 13.544017 | 14.653991 | 14.521705 | 13.985653 | 14.415571 | 14.427871 | 17.418568 | 14.534781 | 15.346562 | 14.989454 | 14.385095 | 14.995381 | 14.752593 | 14.545712 | 15.009596 | 14.65675 | 14.756969 | 14.954918 |
hep-th/9911069 | Sukanta Bose | Sukanta Bose (Cardiff Univ.), Naresh Dadhich (IUCAA), and Sayan Kar
(IIT-Kharagpur) | New classes of black hole spacetimes in 2+1 gravity | 8 pages | Phys.Lett. B477 (2000) 451-456 | 10.1016/S0370-2693(00)00191-X | IUCAA-40/99 | hep-th gr-qc | null | The electrogravity transformation is applied to the three-dimensional
Einstein field equations to obtain new multi-parameter families of black hole
solutions. The Ba\~{n}ados-Teitelboim-Zanelli black hole is shown to be a
special case of one of these families. The causal structure, associated matter,
as well as the m... | [
{
"created": "Wed, 10 Nov 1999 20:00:49 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bose",
"Sukanta",
"",
"Cardiff Univ."
],
[
"Dadhich",
"Naresh",
"",
"IUCAA"
],
[
"Kar",
"Sayan",
"",
"IIT-Kharagpur"
]
] | The electrogravity transformation is applied to the three-dimensional Einstein field equations to obtain new multi-parameter families of black hole solutions. The Ba\~{n}ados-Teitelboim-Zanelli black hole is shown to be a special case of one of these families. The causal structure, associated matter, as well as the mec... | 8.119283 | 7.644335 | 7.040941 | 6.699738 | 7.115586 | 6.758139 | 7.163219 | 6.996917 | 7.194309 | 7.641236 | 7.527521 | 7.39155 | 7.051996 | 6.996301 | 7.097038 | 7.079572 | 7.347391 | 6.880063 | 7.446175 | 7.282659 | 7.184528 |
1001.1444 | Borun Chowdhury | Borun D. Chowdhury, Amitabh Virmani | Modave Lectures on Fuzzballs and Emission from the D1-D5 System | 54 pages, 20 figures; notes of lectures presented at the 5th Modave
Summer School; to appear in proceedings of the Solvay Institutes; v3 minor
typos corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | These lecture notes present an introduction to the fuzzball proposal and
emission from the D1-D5 system which is geared to an audience of graduate
students and others with little background in the subject. The presentation
begins with a discussion of the Penrose process and Hawking radiation. The
fuzzball proposal is... | [
{
"created": "Sun, 10 Jan 2010 12:57:58 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jan 2010 22:29:15 GMT",
"version": "v2"
},
{
"created": "Wed, 8 Sep 2010 11:59:04 GMT",
"version": "v3"
}
] | 2010-09-09 | [
[
"Chowdhury",
"Borun D.",
""
],
[
"Virmani",
"Amitabh",
""
]
] | These lecture notes present an introduction to the fuzzball proposal and emission from the D1-D5 system which is geared to an audience of graduate students and others with little background in the subject. The presentation begins with a discussion of the Penrose process and Hawking radiation. The fuzzball proposal is t... | 7.629454 | 8.008972 | 7.75823 | 7.226853 | 7.384611 | 8.301023 | 7.997808 | 7.296668 | 7.760141 | 9.114269 | 7.651354 | 7.36615 | 7.906283 | 7.400285 | 7.429638 | 7.292516 | 7.396891 | 7.193923 | 7.440281 | 7.83543 | 7.100725 |
1907.06353 | Robert Brandenberger | Robert Brandenberger, Juerg Froehlich and Ryo Namba (McGill and ETH
Zuerich) | Unified Dark Matter, Dark Energy and Baryogenesis via a "Cosmological
Wetting Transition'' | 8 pages, 1 figure, matches version accepted in JCAP, a couple of
minor clarifications compared to the initial version | null | 10.1088/1475-7516/2019/09/069 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a recent publication \cite{us}, a cosmological scenario featuring a scalar
field, $\varphi$, that is a source for Dark Matter and Dark Energy has been
proposed. In this paper, a concrete realization of that scenario is presented.
As in many models of scalar-field driven Dark Energy, the effective Lagrangian
of the... | [
{
"created": "Mon, 15 Jul 2019 07:50:43 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Sep 2019 17:42:58 GMT",
"version": "v2"
}
] | 2019-10-09 | [
[
"Brandenberger",
"Robert",
"",
"McGill and ETH\n Zuerich"
],
[
"Froehlich",
"Juerg",
"",
"McGill and ETH\n Zuerich"
],
[
"Namba",
"Ryo",
"",
"McGill and ETH\n Zuerich"
]
] | In a recent publication \cite{us}, a cosmological scenario featuring a scalar field, $\varphi$, that is a source for Dark Matter and Dark Energy has been proposed. In this paper, a concrete realization of that scenario is presented. As in many models of scalar-field driven Dark Energy, the effective Lagrangian of the f... | 6.862611 | 7.558338 | 6.73663 | 6.757669 | 7.012618 | 7.135735 | 6.875896 | 7.027782 | 6.882133 | 6.957142 | 6.790713 | 6.507074 | 6.517795 | 6.505351 | 6.472692 | 6.600482 | 6.578216 | 6.490426 | 6.576395 | 6.586949 | 6.562449 |
1411.6670 | Gian Paolo Vacca | J. Bartels, C. Contreras and G. P. Vacca | Renormalization group analysis of reggeon field theory: flow equations | 4 pages, 1 figure, To appear in the Proceedings of conference:
Diffraction 2014 - International Workshop on Diffraction in High-Energy
Physics | null | 10.1063/1.4915993 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Can large distance high energy QCD be described by Reggeon Field Theory as an
effective emergent theory? We start to investigate the issue employing
functional renormalisation group techniques.
| [
{
"created": "Mon, 24 Nov 2014 22:15:21 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Bartels",
"J.",
""
],
[
"Contreras",
"C.",
""
],
[
"Vacca",
"G. P.",
""
]
] | Can large distance high energy QCD be described by Reggeon Field Theory as an effective emergent theory? We start to investigate the issue employing functional renormalisation group techniques. | 24.080147 | 25.343632 | 18.85487 | 20.500597 | 23.096342 | 24.541864 | 27.639708 | 20.714624 | 22.000811 | 18.525232 | 20.413219 | 18.546286 | 16.892199 | 17.351297 | 17.46213 | 18.364216 | 17.786999 | 17.375473 | 17.507488 | 15.814425 | 22.523315 |
hep-th/9401121 | Wolfgang Lerche | W. Lerche | Chiral Rings and Integrable Systems for Models of Topological Gravity | 19p, plain tex, 1 uuencoded PostScript figure | null | null | null | hep-th | null | (Talk given at Strings '93, Berkeley, and at XXVII. Internationales Symposium
\"uber Elementarteilchentheorie, Wendisch-Rietz, 1993) We review the
superconformal properties of matter coupled to $2d$ gravity, and $W$-extensions
thereof. We show in particular how the \nex2 structure provides a direct link
between certa... | [
{
"created": "Tue, 25 Jan 1994 10:38:44 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Lerche",
"W.",
""
]
] | (Talk given at Strings '93, Berkeley, and at XXVII. Internationales Symposium \"uber Elementarteilchentheorie, Wendisch-Rietz, 1993) We review the superconformal properties of matter coupled to $2d$ gravity, and $W$-extensions thereof. We show in particular how the \nex2 structure provides a direct link between certain... | 11.547528 | 9.858999 | 12.891173 | 9.321848 | 10.322299 | 10.506227 | 10.960055 | 9.788176 | 10.321974 | 12.908484 | 9.515388 | 9.958583 | 10.565201 | 10.18189 | 10.174706 | 9.89559 | 10.071977 | 9.783956 | 9.762576 | 11.085543 | 9.859178 |
hep-th/9902095 | null | A.A. Tseytlin and K. Zarembo | Effective potential in non-supersymmetric SU(N) x SU(N) gauge theory and
interactions of type 0 D3-branes | 14 pages, latex, v2: minor corrections, v3: a comment and references
added at the end of section 5 | Phys.Lett.B457:77-86,1999 | 10.1016/S0370-2693(99)00471-2 | ITEP-TH-4/99, Imperial/TP/98-99/41 | hep-th | null | We study some aspects of short-distance interaction between parallel
D3-branes in type 0 string theory as described by the corresponding
world-volume gauge theory. We compute the one-loop effective potential in the
non-supersymmetric SU(N) x SU(N) gauge theory (which is a Z_2 projection of the
U(2N) n=4 SYM theory) r... | [
{
"created": "Fri, 12 Feb 1999 22:54:19 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Feb 1999 16:12:04 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Feb 1999 10:59:34 GMT",
"version": "v3"
}
] | 2009-09-17 | [
[
"Tseytlin",
"A. A.",
""
],
[
"Zarembo",
"K.",
""
]
] | We study some aspects of short-distance interaction between parallel D3-branes in type 0 string theory as described by the corresponding world-volume gauge theory. We compute the one-loop effective potential in the non-supersymmetric SU(N) x SU(N) gauge theory (which is a Z_2 projection of the U(2N) n=4 SYM theory) rep... | 7.895728 | 7.576031 | 8.808056 | 7.315262 | 7.827827 | 8.339974 | 7.632308 | 7.528744 | 7.560313 | 9.766159 | 7.474219 | 7.560531 | 8.000282 | 7.845049 | 7.5377 | 7.638035 | 7.546347 | 7.720757 | 7.507409 | 8.1352 | 7.412991 |
1004.1841 | Leszek Hadasz | Leszek Hadasz, Zbigniew Jaskolski and Paulina Suchanek | Proving the AGT relation for N_f = 0,1,2 antifundamentals | LaTeX, 20+1 pages, version 2: added references and typos corrected | JHEP 1006:046,2010 | 10.1007/JHEP06(2010)046 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using recursive relations satisfied by Nekrasov partition functions and by
irregular conformal blocks we prove the AGT correspondence in the case of N=2
superconformal SU(2) quiver gauge theories with N_f = 0,1,2 antifundamental
hypermultiplets
| [
{
"created": "Sun, 11 Apr 2010 20:52:50 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Jun 2010 15:44:06 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Hadasz",
"Leszek",
""
],
[
"Jaskolski",
"Zbigniew",
""
],
[
"Suchanek",
"Paulina",
""
]
] | Using recursive relations satisfied by Nekrasov partition functions and by irregular conformal blocks we prove the AGT correspondence in the case of N=2 superconformal SU(2) quiver gauge theories with N_f = 0,1,2 antifundamental hypermultiplets | 6.107667 | 5.241498 | 8.551961 | 4.630731 | 4.554911 | 4.766519 | 4.593204 | 4.780665 | 4.660334 | 8.553162 | 4.663043 | 4.809565 | 6.022992 | 4.985626 | 4.814227 | 4.926523 | 4.916265 | 4.840365 | 4.828931 | 6.773887 | 4.75822 |
hep-th/0008201 | Matteo Bertolini | M. Bertolini, M. Trigiante | Microscopic entropy of the most general four-dimensional BPS black hole | 15 pages, latex. Misprints corrected, few points clarified and a
reference added | JHEP 0010:002,2000 | 10.1088/1126-6708/2000/10/002 | NORDITA-2000/59 HE, SWAT/265 | hep-th gr-qc | null | In a recent paper we have given the macroscopic and microscopic description
of the generating solution of toroidally compactified string theory BPS black
holes. In this note we compute its corresponding microscopic entropy. Since by
definition the generating solution is the most general solution modulo
U-duality tran... | [
{
"created": "Fri, 25 Aug 2000 16:52:38 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Sep 2000 14:36:28 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Bertolini",
"M.",
""
],
[
"Trigiante",
"M.",
""
]
] | In a recent paper we have given the macroscopic and microscopic description of the generating solution of toroidally compactified string theory BPS black holes. In this note we compute its corresponding microscopic entropy. Since by definition the generating solution is the most general solution modulo U-duality transf... | 12.200312 | 9.081934 | 9.937175 | 9.213566 | 9.105258 | 9.426668 | 9.091767 | 9.597118 | 9.233658 | 11.973857 | 9.622982 | 9.137816 | 9.955545 | 9.217914 | 8.980202 | 9.144479 | 9.023723 | 8.86999 | 9.02997 | 9.979396 | 8.919782 |
hep-th/0506128 | Umut Gursoy | Daniel Z. Freedman and Umut Gursoy | Comments on the beta-deformed N=4 SYM Theory | 18 pages, 1 figure. 2nd version: typos corrected, one reference added | JHEP 0511:042,2005 | 10.1088/1126-6708/2005/11/042 | null | hep-th | null | Several calculations of 2- and 3-point correlation functions in the deformed
theory are presented. The central charge in the Lunin-Maldacena gravity dual is
shown to be independent of the deformation parameter. Calculations show that 2-
and 3-point functions of chiral primary operators have no radiative corrections
t... | [
{
"created": "Wed, 15 Jun 2005 20:17:37 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Jun 2005 20:10:15 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Freedman",
"Daniel Z.",
""
],
[
"Gursoy",
"Umut",
""
]
] | Several calculations of 2- and 3-point correlation functions in the deformed theory are presented. The central charge in the Lunin-Maldacena gravity dual is shown to be independent of the deformation parameter. Calculations show that 2- and 3-point functions of chiral primary operators have no radiative corrections to ... | 8.889334 | 8.005899 | 9.249011 | 7.477417 | 7.994755 | 7.762891 | 7.623477 | 7.402593 | 7.238986 | 9.71769 | 7.175597 | 7.63535 | 9.041693 | 7.759321 | 8.073585 | 7.653556 | 7.908285 | 7.684453 | 7.89051 | 9.01478 | 7.789594 |
2101.12494 | Neven Bili\'c | Neven Bili\'c and Julio C. Fabris | Analog dual to a 2+1-dimensional holographic superconductor | 20 pages, 3 figures, typos corrected, Introduction and Section 3.2
expanded, one figure removed, references added, matches the accepted version
in CQG | Class. Quantum Grav. 38 (2021) 165007 | 10.1088/1361-6382/ac1207 | RBI-ThPhys-2021-7 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We study an analog hydrodynamic model that mimics a 3+1 AdS planar BH
spacetime dual to a 2+1-dimensional superconductor. We demonstrate that the
AdS$_4$ bulk and its holographic dual could be realized in nature in an analog
gravity model based on fluid dynamics. In particular we mimic the metric of an
$O_2$ holograp... | [
{
"created": "Fri, 29 Jan 2021 10:01:23 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Mar 2021 15:05:41 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Apr 2021 07:52:54 GMT",
"version": "v3"
},
{
"created": "Sun, 25 Jul 2021 13:19:44 GMT",
"version": "v4"
}
] | 2021-07-27 | [
[
"Bilić",
"Neven",
""
],
[
"Fabris",
"Julio C.",
""
]
] | We study an analog hydrodynamic model that mimics a 3+1 AdS planar BH spacetime dual to a 2+1-dimensional superconductor. We demonstrate that the AdS$_4$ bulk and its holographic dual could be realized in nature in an analog gravity model based on fluid dynamics. In particular we mimic the metric of an $O_2$ holographi... | 13.613862 | 11.801233 | 12.562566 | 12.810387 | 12.576255 | 13.041656 | 14.040139 | 11.572565 | 13.403236 | 15.839514 | 12.378746 | 12.565349 | 12.79675 | 11.475075 | 12.270355 | 12.064759 | 12.793865 | 11.6052 | 12.16438 | 12.187723 | 12.737041 |
hep-th/0508225 | Karl-Georg Schlesinger | Harald Grosse, Karl-Georg Schlesinger | On deformation theory of quantum vertex algebras | 22 pages | null | null | null | hep-th | null | We study an algebraic deformation problem which captures the data of the
general deformation problem for a quantum vertex algebra. We derive a system of
coupled equations which is the counterpart of the Maurer-Cartan equation on the
usual Hochschild complex of an assocative algebra. We show that this system of
equati... | [
{
"created": "Tue, 30 Aug 2005 12:00:28 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Grosse",
"Harald",
""
],
[
"Schlesinger",
"Karl-Georg",
""
]
] | We study an algebraic deformation problem which captures the data of the general deformation problem for a quantum vertex algebra. We derive a system of coupled equations which is the counterpart of the Maurer-Cartan equation on the usual Hochschild complex of an assocative algebra. We show that this system of equation... | 10.062973 | 9.741969 | 10.756892 | 9.198457 | 8.756473 | 10.422053 | 9.953505 | 9.479548 | 10.089532 | 12.458838 | 9.538444 | 8.850204 | 9.624219 | 8.941943 | 8.762763 | 8.807257 | 8.850298 | 8.978819 | 8.758894 | 9.628737 | 8.99294 |
1004.0752 | Shih-Hung Chen | Itzhak Bars and Shih-Hung Chen | The Big Bang and Inflation United by an Analytic Solution | V2 improve computation with better agreement with WMAP 7 years data,
and also point out an exact solution for cyclic cosmology | Phys.Rev.D83:043522,2011 | 10.1103/PhysRevD.83.043522 | USC-HEP-10B2 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Exact analytic solutions for a class of scalar-tensor gravity theories with a
hyperbolic scalar potential are presented. Using an exact solution we have
successfully constructed a model of inflation that produces the spectral index,
the running of the spectral index and the amplitude of scalar perturbations
within th... | [
{
"created": "Tue, 6 Apr 2010 01:58:13 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Dec 2010 05:22:49 GMT",
"version": "v2"
}
] | 2011-03-23 | [
[
"Bars",
"Itzhak",
""
],
[
"Chen",
"Shih-Hung",
""
]
] | Exact analytic solutions for a class of scalar-tensor gravity theories with a hyperbolic scalar potential are presented. Using an exact solution we have successfully constructed a model of inflation that produces the spectral index, the running of the spectral index and the amplitude of scalar perturbations within the ... | 12.288955 | 12.486548 | 13.125505 | 12.042151 | 12.937881 | 12.961484 | 13.123183 | 12.155599 | 12.188162 | 13.461121 | 12.319828 | 12.71175 | 12.219729 | 12.360741 | 12.828058 | 12.790266 | 12.708186 | 12.220576 | 12.090563 | 12.568986 | 12.116485 |
0801.3909 | N. I. Stoilova | N.I. Stoilova and J. Van der Jeugt | Parafermions, parabosons and representations of so(\infty) and
osp(1|\infty) | null | Int.J.Math.20:693-715,2009 | 10.1142/S0129167X09005467 | null | hep-th math-ph math.GR math.MP math.RT quant-ph | null | The goal of this paper is to give an explicit construction of the Fock spaces
of the parafermion and the paraboson algebra, for an infinite set of
generators. This is equivalent to constructing certain unitary irreducible
lowest weight representations of the (infinite rank) Lie algebra so(\infty) and
of the Lie super... | [
{
"created": "Fri, 25 Jan 2008 10:43:12 GMT",
"version": "v1"
}
] | 2009-08-24 | [
[
"Stoilova",
"N. I.",
""
],
[
"Van der Jeugt",
"J.",
""
]
] | The goal of this paper is to give an explicit construction of the Fock spaces of the parafermion and the paraboson algebra, for an infinite set of generators. This is equivalent to constructing certain unitary irreducible lowest weight representations of the (infinite rank) Lie algebra so(\infty) and of the Lie superal... | 7.80179 | 7.715822 | 8.552654 | 6.776473 | 7.495551 | 7.73488 | 7.124737 | 7.849436 | 7.28003 | 9.056985 | 7.365384 | 7.156782 | 7.81333 | 7.374329 | 7.12568 | 7.331694 | 7.259614 | 7.292361 | 7.206702 | 8.022527 | 7.223314 |
1810.01847 | Sasha Haco | Sasha Haco, Stephen W. Hawking, Malcolm J. Perry and Andrew Strominger | Black Hole Entropy and Soft Hair | Accepted for publication by JHEP on 05/12/18 | null | 10.1007/JHEP12(2018)098 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A set of infinitesimal ${\rm Virasoro_{\,L}}\otimes{\rm Virasoro_{\,R}}$
diffeomorphisms are presented which act non-trivially on the horizon of a
generic Kerr black hole with spin J. The covariant phase space formalism
provides a formula for the Virasoro charges as surface integrals on the
horizon. Integrability and... | [
{
"created": "Wed, 3 Oct 2018 17:16:36 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Oct 2018 10:07:22 GMT",
"version": "v2"
},
{
"created": "Tue, 16 Oct 2018 14:13:45 GMT",
"version": "v3"
},
{
"created": "Thu, 13 Dec 2018 12:07:17 GMT",
"version": "v4"
}
] | 2019-01-30 | [
[
"Haco",
"Sasha",
""
],
[
"Hawking",
"Stephen W.",
""
],
[
"Perry",
"Malcolm J.",
""
],
[
"Strominger",
"Andrew",
""
]
] | A set of infinitesimal ${\rm Virasoro_{\,L}}\otimes{\rm Virasoro_{\,R}}$ diffeomorphisms are presented which act non-trivially on the horizon of a generic Kerr black hole with spin J. The covariant phase space formalism provides a formula for the Virasoro charges as surface integrals on the horizon. Integrability and a... | 7.481291 | 6.906567 | 8.314627 | 6.844759 | 7.516674 | 7.239578 | 7.175864 | 6.856106 | 7.190251 | 9.646858 | 6.864921 | 6.797657 | 7.275922 | 7.094675 | 7.400315 | 6.952637 | 7.014959 | 7.155068 | 7.433324 | 7.799456 | 7.063859 |
hep-th/0504196 | Hanno Klemm | H. Klemm | BPS branes in discrete torsion orbifolds | 20 pages, LaTeX | JHEP 0507 (2005) 010 | 10.1088/1126-6708/2005/07/010 | null | hep-th | null | We investigate D-branes in a Z_3xZ_3 orbifold with discrete torsion. For this
class of orbifolds the only known objects which couple to twisted RR potentials
have been non-BPS branes. By using more general gluing conditions we construct
here a D-brane which is BPS and couples to RR potentials in the twisted and in
th... | [
{
"created": "Mon, 25 Apr 2005 07:56:32 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Klemm",
"H.",
""
]
] | We investigate D-branes in a Z_3xZ_3 orbifold with discrete torsion. For this class of orbifolds the only known objects which couple to twisted RR potentials have been non-BPS branes. By using more general gluing conditions we construct here a D-brane which is BPS and couples to RR potentials in the twisted and in the ... | 8.60677 | 7.091622 | 10.572637 | 7.321213 | 7.941831 | 6.964567 | 7.560266 | 7.189014 | 7.688277 | 10.354966 | 6.941674 | 7.955989 | 9.117938 | 7.966826 | 8.135798 | 7.9688 | 7.40424 | 8.018683 | 7.833601 | 9.011402 | 7.837026 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.