id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0406152 | Michael Faux | Michael Faux, David Kagan and Donald Spector | Central Charges and Extra Dimensions in Supersymmetric Quantum Mechanics | 30 pages, LaTeX, references and commentary added | null | null | null | hep-th | null | We systematically include central charges into supersymmetric quantum
mechanics formulated on curved Euclidean spaces, and explain how the background
geometry manifests itself on states of the theory. In particular, we show in
detail how, from the point of view of non-relativistic d=1 world-line physics,
one can infe... | [
{
"created": "Fri, 18 Jun 2004 17:27:28 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Jul 2004 07:42:33 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Faux",
"Michael",
""
],
[
"Kagan",
"David",
""
],
[
"Spector",
"Donald",
""
]
] | We systematically include central charges into supersymmetric quantum mechanics formulated on curved Euclidean spaces, and explain how the background geometry manifests itself on states of the theory. In particular, we show in detail how, from the point of view of non-relativistic d=1 world-line physics, one can infer ... | 13.231718 | 12.652502 | 12.364343 | 12.004213 | 12.608599 | 11.776036 | 12.193083 | 11.189817 | 11.727998 | 15.422408 | 11.657892 | 11.966217 | 12.040972 | 11.654538 | 12.212587 | 11.719635 | 11.425635 | 11.662949 | 11.799633 | 12.252187 | 11.592794 |
1006.1214 | Wei He | Wei He, Yan-Gang Miao | Magnetic expansion of Nekrasov theory: the SU(2) pure gauge theory | 17 pages, submitted to PRD; v2, typos corrected, references added;
v3, published version | Phys.Rev.D82:025020,2010 | 10.1103/PhysRevD.82.025020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is recently claimed by Nekrasov and Shatashvili that the $\mathcal {N}=2$
gauge theories in the $\Omega$ background with $\epsilon_1=\hbar, \epsilon_2=0$
are related to the quantization of certain algebraic integrable systems. We
study the special case of SU(2) pure gauge theory, the corresponding integrable
model... | [
{
"created": "Mon, 7 Jun 2010 09:39:32 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Jun 2010 14:07:42 GMT",
"version": "v2"
},
{
"created": "Sat, 31 Jul 2010 08:21:27 GMT",
"version": "v3"
}
] | 2014-11-21 | [
[
"He",
"Wei",
""
],
[
"Miao",
"Yan-Gang",
""
]
] | It is recently claimed by Nekrasov and Shatashvili that the $\mathcal {N}=2$ gauge theories in the $\Omega$ background with $\epsilon_1=\hbar, \epsilon_2=0$ are related to the quantization of certain algebraic integrable systems. We study the special case of SU(2) pure gauge theory, the corresponding integrable model i... | 6.923282 | 6.729746 | 8.083344 | 6.911957 | 7.71155 | 7.203135 | 6.930307 | 6.76638 | 6.847956 | 8.523461 | 6.928697 | 6.782222 | 6.816988 | 6.65575 | 6.635462 | 6.659099 | 6.696924 | 6.79776 | 6.680388 | 6.723109 | 6.63664 |
0907.2989 | Lee Peng Teo | L.P. Teo | Casimir Effect in Spacetime with Extra Dimensions -- From Kaluza-Klein
to Randall-Sundrum Models | 9 pages, 3 figure. Final version accepted by Phys. Lett. B | Phys.Lett.B682:259-265,2009 | 10.1016/j.physletb.2009.11.011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article, we derive the finite temperature Casimir force acting on a
pair of parallel plates due to a massless scalar field propagating in the bulk
of a higher dimensional brane model. In contrast to previous works which used
approximations for the effective masses in deriving the Casimir force, the
formulas o... | [
{
"created": "Fri, 17 Jul 2009 06:40:25 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jul 2009 00:53:55 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Nov 2009 00:48:37 GMT",
"version": "v3"
}
] | 2009-11-23 | [
[
"Teo",
"L. P.",
""
]
] | In this article, we derive the finite temperature Casimir force acting on a pair of parallel plates due to a massless scalar field propagating in the bulk of a higher dimensional brane model. In contrast to previous works which used approximations for the effective masses in deriving the Casimir force, the formulas of ... | 8.909229 | 7.437004 | 8.319163 | 7.433366 | 7.882468 | 7.618624 | 7.763433 | 7.516391 | 7.652536 | 9.199165 | 7.584608 | 7.919321 | 8.096814 | 7.94028 | 7.954635 | 7.759875 | 7.726017 | 8.024993 | 7.773375 | 8.200109 | 7.91687 |
1501.07562 | Konstantinos Koutrolikos | Fotis Farakos, Alex Kehagias, Konstantinos Koutrolikos | Linearized Non-Minimal Higher Curvature Supergravity | null | null | 10.1016/j.nuclphysb.2015.03.010 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the framework of linearized non-minimal supergravity (20/20), we present
the embedding of the $R + R^2$ model and we analyze its field spectrum. As
usual, the auxiliary fields of the Einstein theory now become propagating,
giving rise to additional degrees of freedom, which organize themselves into
on-shell irredu... | [
{
"created": "Thu, 29 Jan 2015 19:53:53 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Farakos",
"Fotis",
""
],
[
"Kehagias",
"Alex",
""
],
[
"Koutrolikos",
"Konstantinos",
""
]
] | In the framework of linearized non-minimal supergravity (20/20), we present the embedding of the $R + R^2$ model and we analyze its field spectrum. As usual, the auxiliary fields of the Einstein theory now become propagating, giving rise to additional degrees of freedom, which organize themselves into on-shell irreduci... | 11.693184 | 10.960457 | 12.290071 | 11.490602 | 11.712763 | 11.056795 | 10.476633 | 10.904156 | 10.538338 | 12.89406 | 10.643456 | 10.685864 | 12.345415 | 11.418435 | 11.365585 | 10.637481 | 11.147524 | 11.301437 | 11.028682 | 12.018772 | 10.693913 |
hep-th/9508044 | Bas Peeters | Dileep P. Jatkar and Bas Peeters | String Theory near a Conifold Singularity | 10 pages, harvmac. Some changes to manuscript and a reference added | Phys.Lett. B362 (1995) 73-77 | 10.1016/0370-2693(95)01155-J | ITP-SB-95-24 | hep-th | null | We demonstrate that type II string theory compactified on a singular
Calabi-Yau manifold is related to $c=1$ string theory compactified at the
self-dual radius. We establish this result in two ways. First we show that
complex structure deformations of the conifold correspond, on the mirror
manifold, to the problem of... | [
{
"created": "Wed, 9 Aug 1995 20:57:40 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Aug 1995 16:44:05 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Jatkar",
"Dileep P.",
""
],
[
"Peeters",
"Bas",
""
]
] | We demonstrate that type II string theory compactified on a singular Calabi-Yau manifold is related to $c=1$ string theory compactified at the self-dual radius. We establish this result in two ways. First we show that complex structure deformations of the conifold correspond, on the mirror manifold, to the problem of m... | 4.843641 | 4.446458 | 5.66341 | 4.671599 | 4.812387 | 4.794359 | 4.528577 | 4.629081 | 4.59871 | 5.835285 | 4.478611 | 4.657302 | 4.88072 | 4.629891 | 4.570785 | 4.588458 | 4.541838 | 4.654651 | 4.721535 | 4.878197 | 4.54544 |
1805.12413 | Vuong-Viet Tran | Vuong-Viet Tran | Perturbative Correlation Functions and Scattering Amplitudes in Planar
$\mathcal{N}=4$ Supersymmetric Yang-Mills | PhD thesis, Durham University, 2018, v2 minor aesthetic corrections,
http://etheses.dur.ac.uk/12642 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this thesis, we study the integrands of a special four-point correlation
function formed of protected half-BPS operators and scattering amplitudes in
planar supersymmetric $\mathcal{N}=4$ Yang-Mills. We use the `soft-collinear
bootstrap' method to construct integrands of the aforementioned correlator and
four-poin... | [
{
"created": "Thu, 31 May 2018 10:37:10 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jun 2018 00:43:10 GMT",
"version": "v2"
}
] | 2018-06-07 | [
[
"Tran",
"Vuong-Viet",
""
]
] | In this thesis, we study the integrands of a special four-point correlation function formed of protected half-BPS operators and scattering amplitudes in planar supersymmetric $\mathcal{N}=4$ Yang-Mills. We use the `soft-collinear bootstrap' method to construct integrands of the aforementioned correlator and four-point ... | 12.349362 | 11.847653 | 13.194686 | 11.217906 | 12.54789 | 11.608954 | 12.885633 | 11.726303 | 11.537539 | 13.317454 | 11.891296 | 12.263172 | 12.397235 | 11.511843 | 11.730042 | 11.838062 | 11.794263 | 11.795313 | 11.83809 | 12.097523 | 11.492738 |
1705.02322 | Jia-ju Zhang | Marco Lietti, Andrea Mauri, Silvia Penati and Jia-ju Zhang | String theory duals of Wilson loops from Higgsing | 52 pages, 4 figures; V2, 61 pages, 4 figures, supercharges in gravity
and field theory identified, conclusion unchanged, published version | JHEP 1708 (2017) 030 | 10.1007/JHEP08(2017)030 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For three-dimensional ABJ(M) theories and $\mathcal N=4$ Chern-Simons-matter
quiver theories, we construct two sets of 1/2 BPS Wilson loop operators by
applying the Higgsing procedure along independent directions of the moduli
space, and choosing different massive modes. For theories whose dual M-theory
description i... | [
{
"created": "Fri, 5 May 2017 17:46:30 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Aug 2017 17:54:22 GMT",
"version": "v2"
}
] | 2017-08-10 | [
[
"Lietti",
"Marco",
""
],
[
"Mauri",
"Andrea",
""
],
[
"Penati",
"Silvia",
""
],
[
"Zhang",
"Jia-ju",
""
]
] | For three-dimensional ABJ(M) theories and $\mathcal N=4$ Chern-Simons-matter quiver theories, we construct two sets of 1/2 BPS Wilson loop operators by applying the Higgsing procedure along independent directions of the moduli space, and choosing different massive modes. For theories whose dual M-theory description is ... | 7.591368 | 7.497735 | 8.794199 | 7.35087 | 7.874774 | 7.591488 | 7.873334 | 7.47328 | 7.58357 | 8.930933 | 7.545142 | 7.390437 | 7.74962 | 7.43957 | 7.549555 | 7.663926 | 7.492771 | 7.540207 | 7.504054 | 7.69157 | 7.345447 |
hep-th/0003243 | Buchholz | Hans-Juergen Borchers, Detlev Buchholz and Bert Schroer | Polarization-Free Generators and the S-Matrix | Dedicated to the memory of Harry Lehmann, 19 pages; revised version
(proof of Lemma 3.4 corrected) | Commun.Math.Phys. 219 (2001) 125-140 | 10.1007/s002200100411 | null | hep-th | null | Polarization-free generators, i.e. ``interacting'' Heisenberg operators which
are localized in wedge-shaped regions of Minkowski space and generate single
particle states from the vacuum, are a novel tool in the analysis and synthesis
of two-dimensional integrable quantum field theories. In the present article,
the s... | [
{
"created": "Mon, 27 Mar 2000 13:30:57 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Apr 2000 10:07:26 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Borchers",
"Hans-Juergen",
""
],
[
"Buchholz",
"Detlev",
""
],
[
"Schroer",
"Bert",
""
]
] | Polarization-free generators, i.e. ``interacting'' Heisenberg operators which are localized in wedge-shaped regions of Minkowski space and generate single particle states from the vacuum, are a novel tool in the analysis and synthesis of two-dimensional integrable quantum field theories. In the present article, the sta... | 11.063087 | 11.089581 | 11.68973 | 10.807061 | 11.442105 | 10.714056 | 11.269676 | 10.727148 | 10.5357 | 12.019566 | 10.247549 | 9.906971 | 10.219596 | 10.2736 | 9.934908 | 10.0853 | 9.797165 | 9.975092 | 10.198746 | 10.517522 | 10.111648 |
hep-th/0112167 | Pedro D. Fonseca | P. Fonseca, A. Zamolodchikov | Ising field theory in a magnetic field: analytic properties of the free
energy | 65 pages, 23 eps figures; uses harvmac.tex | null | null | RUNHETC-2001-37 | hep-th cond-mat | null | We study the analytic properties of the scaling function associated with the
2D Ising model free energy in the critical domain $T \to T_c$, $H \to 0$. The
analysis is based on numerical data obtained through the Truncated Free Fermion
Space Approach. We determine the discontinuities across the Yang-Lee and Langer
bra... | [
{
"created": "Wed, 19 Dec 2001 19:22:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Fonseca",
"P.",
""
],
[
"Zamolodchikov",
"A.",
""
]
] | We study the analytic properties of the scaling function associated with the 2D Ising model free energy in the critical domain $T \to T_c$, $H \to 0$. The analysis is based on numerical data obtained through the Truncated Free Fermion Space Approach. We determine the discontinuities across the Yang-Lee and Langer branc... | 13.844592 | 10.688911 | 13.168301 | 9.965689 | 12.067236 | 9.192484 | 10.120526 | 10.393189 | 9.683839 | 15.738235 | 10.403689 | 10.725373 | 11.404871 | 11.001443 | 10.730154 | 10.513024 | 10.755018 | 11.344985 | 10.818208 | 11.180237 | 10.916283 |
1405.5532 | Austin Joyce | Garrett Goon, Austin Joyce and Mark Trodden | Spontaneously Broken Gauge Theories and the Coset Construction | 28 pages. v2: added references | Phys. Rev. D 90, 025022 (2014) | 10.1103/PhysRevD.90.025022 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The methods of non-linear realizations have proven to be powerful in studying
the low energy physics resulting from spontaneously broken internal and
spacetime symmetries. In this paper, we reconsider how these techniques may be
applied to the case of spontaneously broken gauge theories, concentrating on
Yang-Mills t... | [
{
"created": "Wed, 21 May 2014 20:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Jun 2014 18:47:04 GMT",
"version": "v2"
}
] | 2014-07-22 | [
[
"Goon",
"Garrett",
""
],
[
"Joyce",
"Austin",
""
],
[
"Trodden",
"Mark",
""
]
] | The methods of non-linear realizations have proven to be powerful in studying the low energy physics resulting from spontaneously broken internal and spacetime symmetries. In this paper, we reconsider how these techniques may be applied to the case of spontaneously broken gauge theories, concentrating on Yang-Mills the... | 9.883047 | 8.596304 | 9.586588 | 8.436095 | 8.494864 | 8.886618 | 9.135973 | 8.462306 | 8.448567 | 9.271613 | 8.462246 | 8.590705 | 8.7906 | 8.735533 | 8.656155 | 8.385203 | 8.734523 | 8.701918 | 8.795478 | 8.701118 | 8.697716 |
0810.4750 | Hironobu Kihara | Hironobu Kihara | Finite Energy Monopoles in Non-Abelian Gauge Theories on Odd-dimensional
Spaces | 19 pages, 2 figures, 1 table | Phys.Rev.D79:045021,2009 | 10.1103/PhysRevD.79.045021 | KIAS-P08064 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In higher dimensional gauge theory, we need energies with higher power terms
of field strength in order to realize point-wise monopoles. We consider new
models with higher power terms of field strength and extraordinary kinetic term
of scalar field. Monopole charges are computed as integrals over spheres and
they are... | [
{
"created": "Mon, 27 Oct 2008 07:41:30 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Dec 2008 03:21:16 GMT",
"version": "v2"
}
] | 2009-03-12 | [
[
"Kihara",
"Hironobu",
""
]
] | In higher dimensional gauge theory, we need energies with higher power terms of field strength in order to realize point-wise monopoles. We consider new models with higher power terms of field strength and extraordinary kinetic term of scalar field. Monopole charges are computed as integrals over spheres and they are r... | 22.021046 | 22.049177 | 21.257915 | 21.85894 | 24.514664 | 22.067696 | 23.655045 | 23.946278 | 23.566957 | 25.4123 | 21.441477 | 21.106218 | 20.969738 | 20.630545 | 20.081816 | 20.915422 | 21.10725 | 20.766129 | 21.317013 | 21.738897 | 21.487667 |
hep-th/0410057 | Roman Konoplya | Roman Konoplya | Quasinormal modes of the charged black hole in Gauss-Bonnet gravity | 16 pages, 4 figures, 3 tables; misprints corrected | Phys.Rev. D71 (2005) 024038 | 10.1103/PhysRevD.71.024038 | null | hep-th | null | The d-dimensional string generated gravity models lead to Einstein-Maxwell
equations with quadratic order correction term called the Gauss-Bonnet term. We
calculate the quasinormal modes for the d-dimensional charged black hole in the
framework of this model. The quasinormal spectrum essentially depends upon the
Gaus... | [
{
"created": "Wed, 6 Oct 2004 08:46:47 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Oct 2004 14:09:41 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Oct 2004 19:40:58 GMT",
"version": "v3"
},
{
"created": "Sun, 6 Feb 2005 16:24:01 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Konoplya",
"Roman",
""
]
] | The d-dimensional string generated gravity models lead to Einstein-Maxwell equations with quadratic order correction term called the Gauss-Bonnet term. We calculate the quasinormal modes for the d-dimensional charged black hole in the framework of this model. The quasinormal spectrum essentially depends upon the Gauss-... | 11.457554 | 10.647495 | 10.05721 | 9.819432 | 10.749986 | 10.111327 | 10.464338 | 9.644119 | 10.340332 | 10.611342 | 10.645457 | 10.134777 | 10.011129 | 10.678613 | 10.55817 | 10.835179 | 10.645719 | 10.052321 | 10.471528 | 10.546195 | 10.293362 |
hep-th/0503127 | Bernard Piette | V.B. Kopeliovich, B. Piette and W.J. Zakrzewski | Mass terms in the Skyrme Model | 28 pages, 5 figures, 6 tables | Phys.Rev. D73 (2006) 014006 | 10.1103/PhysRevD.73.014006 | null | hep-th | null | We consider various forms of the mass term that can be used in the Skyrme
model and their implications on the properties of baryonic states. We show
that, with an appropriate choice for the mass term, without changing the
asymptotic behaviour of the profile functions at large $r$, we can considerably
reduce or increa... | [
{
"created": "Wed, 16 Mar 2005 08:18:58 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Kopeliovich",
"V. B.",
""
],
[
"Piette",
"B.",
""
],
[
"Zakrzewski",
"W. J.",
""
]
] | We consider various forms of the mass term that can be used in the Skyrme model and their implications on the properties of baryonic states. We show that, with an appropriate choice for the mass term, without changing the asymptotic behaviour of the profile functions at large $r$, we can considerably reduce or increase... | 8.485919 | 7.763008 | 8.014758 | 7.482765 | 7.768125 | 8.161263 | 8.033378 | 7.315346 | 7.681073 | 7.910797 | 7.58587 | 7.902001 | 7.84854 | 7.658983 | 8.111277 | 8.004563 | 7.823783 | 8.086816 | 7.790991 | 7.905156 | 7.733552 |
1810.05115 | Timothy Adamo | Tim Adamo, Eduardo Casali, Lionel Mason, Stefan Nekovar | Plane wave backgrounds and colour-kinematics duality | 29 pages, 4 figures | null | 10.1007/JHEP02(2019)198 | IMPERIAL-TP-TA-2018-04 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain the detailed Feynman rules for perturbative gauge theory on a fixed
Yang-Mills plane wave background. Using these rules, the tree-level 4-point
gluon amplitude is computed and some 1-loop Feynman diagrams are considered. As
an application, we test the extent to which colour-kinematics duality, the
relation ... | [
{
"created": "Thu, 11 Oct 2018 16:47:00 GMT",
"version": "v1"
}
] | 2019-03-27 | [
[
"Adamo",
"Tim",
""
],
[
"Casali",
"Eduardo",
""
],
[
"Mason",
"Lionel",
""
],
[
"Nekovar",
"Stefan",
""
]
] | We obtain the detailed Feynman rules for perturbative gauge theory on a fixed Yang-Mills plane wave background. Using these rules, the tree-level 4-point gluon amplitude is computed and some 1-loop Feynman diagrams are considered. As an application, we test the extent to which colour-kinematics duality, the relation be... | 8.791433 | 9.109545 | 10.04713 | 8.860047 | 9.140437 | 9.279211 | 9.462653 | 8.538929 | 8.692202 | 10.603786 | 8.318252 | 8.817063 | 9.646925 | 8.72653 | 8.848655 | 8.855911 | 8.492022 | 8.941579 | 9.053041 | 8.694881 | 8.434721 |
1902.05547 | Arjun Kar | Vishnu Jejjala, Arjun Kar, Onkar Parrikar | Deep Learning the Hyperbolic Volume of a Knot | 18 pages, 9 figures, updated figures | null | 10.1016/j.physletb.2019.135033 | null | hep-th math.GT math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An important conjecture in knot theory relates the large-$N$, double scaling
limit of the colored Jones polynomial $J_{K,N}(q)$ of a knot $K$ to the
hyperbolic volume of the knot complement, $\text{Vol}(K)$. A less studied
question is whether $\text{Vol}(K)$ can be recovered directly from the original
Jones polynomia... | [
{
"created": "Thu, 14 Feb 2019 18:59:07 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Feb 2019 16:28:47 GMT",
"version": "v2"
},
{
"created": "Mon, 16 Sep 2019 14:22:09 GMT",
"version": "v3"
}
] | 2019-10-30 | [
[
"Jejjala",
"Vishnu",
""
],
[
"Kar",
"Arjun",
""
],
[
"Parrikar",
"Onkar",
""
]
] | An important conjecture in knot theory relates the large-$N$, double scaling limit of the colored Jones polynomial $J_{K,N}(q)$ of a knot $K$ to the hyperbolic volume of the knot complement, $\text{Vol}(K)$. A less studied question is whether $\text{Vol}(K)$ can be recovered directly from the original Jones polynomial ... | 4.716452 | 5.079103 | 5.098852 | 4.918561 | 5.32442 | 4.88808 | 4.983257 | 4.960544 | 4.814181 | 5.768748 | 4.841486 | 4.693094 | 4.859622 | 4.815061 | 4.756921 | 4.69955 | 4.852385 | 4.836953 | 4.87284 | 4.926063 | 4.668487 |
0910.1828 | Jonathan Mark Evans | Jonathan M. Evans | Trialities and Exceptional Lie Algebras: DECONSTRUCTING the Magic Square | 34 pages, plain TeX, 2 figures | null | null | DAMTP-2009-62 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A construction of the magic square, and hence of exceptional Lie algebras, is
carried out using trialities rather than division algebras. By way of
preparation, a comprehensive discussion of trialities is given, incorporating a
number of novel results and proofs. Many of the techniques are closely related
to, or deri... | [
{
"created": "Fri, 9 Oct 2009 19:54:03 GMT",
"version": "v1"
}
] | 2009-10-12 | [
[
"Evans",
"Jonathan M.",
""
]
] | A construction of the magic square, and hence of exceptional Lie algebras, is carried out using trialities rather than division algebras. By way of preparation, a comprehensive discussion of trialities is given, incorporating a number of novel results and proofs. Many of the techniques are closely related to, or derive... | 14.806701 | 13.560548 | 14.42384 | 13.440644 | 13.771392 | 14.122418 | 13.550948 | 13.090997 | 13.672004 | 14.343512 | 13.008972 | 12.619194 | 13.110953 | 12.585245 | 12.439809 | 12.026658 | 12.197377 | 12.456221 | 13.0077 | 12.960498 | 12.473351 |
1102.5343 | Daniel Baumann | Daniel Baumann and Daniel Green | Equilateral Non-Gaussianity and New Physics on the Horizon | 45 pages, 4 figures; v2: references added | null | 10.1088/1475-7516/2011/09/014 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the effective theory of single-field inflation in the limit where
the scalar perturbations propagate with a small speed of sound. In this case
the non-linearly realized time-translation symmetry of the Lagrangian implies
large interactions, giving rise to primordial non-Gaussianities. When the
non-Gaussian... | [
{
"created": "Fri, 25 Feb 2011 21:01:49 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Mar 2011 15:19:38 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Baumann",
"Daniel",
""
],
[
"Green",
"Daniel",
""
]
] | We examine the effective theory of single-field inflation in the limit where the scalar perturbations propagate with a small speed of sound. In this case the non-linearly realized time-translation symmetry of the Lagrangian implies large interactions, giving rise to primordial non-Gaussianities. When the non-Gaussianit... | 7.797569 | 7.404388 | 7.594835 | 7.214119 | 8.135319 | 7.61377 | 8.206213 | 7.357145 | 7.071722 | 8.322009 | 7.129843 | 7.978157 | 7.849644 | 7.628532 | 7.405156 | 7.641431 | 7.531838 | 7.683665 | 7.715503 | 7.953073 | 7.582167 |
1708.06339 | Carlos Andres Cardona Giraldo | Carlos Cardona | Mellin-(Schwinger) representation of One-loop Witten diagrams in AdS | 27 pages, 6 figures. References added, typos corrected | null | null | NCTS-TH/1713 | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this paper we consider Witten diagrams at one loop in AdS space for scalar
$\phi^3+\phi^4$ theory. After using Schwinger parametrization to trivialize the
space-time loop integration, we extract the Mellin-Barnes representation for
the one-loop corrections to the four-particle scattering up to an integration
over ... | [
{
"created": "Mon, 21 Aug 2017 17:54:46 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Aug 2017 12:48:13 GMT",
"version": "v2"
}
] | 2017-08-31 | [
[
"Cardona",
"Carlos",
""
]
] | In this paper we consider Witten diagrams at one loop in AdS space for scalar $\phi^3+\phi^4$ theory. After using Schwinger parametrization to trivialize the space-time loop integration, we extract the Mellin-Barnes representation for the one-loop corrections to the four-particle scattering up to an integration over th... | 10.216782 | 9.902643 | 10.090008 | 9.038612 | 8.13265 | 8.897552 | 9.147878 | 8.902089 | 9.210346 | 10.221935 | 8.462687 | 8.700793 | 8.325261 | 8.828048 | 8.853478 | 9.029706 | 8.976781 | 8.673014 | 8.783442 | 8.606037 | 8.789063 |
2303.02821 | Peter Kazinski | P.O. Kazinski, T.V. Solovyev | Susceptibility of a single photon wave packet | 15 pp., 1 fig; some misprints corrected | Phys. Rev. D 108, 016004 (2023) | 10.1103/PhysRevD.108.016004 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The explicit compact expression for the susceptibility tensor of a single
photon wave packet on the photon mass-shell is derived. It is assumed that the
probe photon is hard, the test photon is soft, and their total energy is below
the electron-positron pair creation threshold. It turns out that a single
photon wave ... | [
{
"created": "Mon, 6 Mar 2023 01:25:21 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Mar 2023 01:48:30 GMT",
"version": "v2"
},
{
"created": "Sun, 2 Jul 2023 04:50:29 GMT",
"version": "v3"
}
] | 2023-07-18 | [
[
"Kazinski",
"P. O.",
""
],
[
"Solovyev",
"T. V.",
""
]
] | The explicit compact expression for the susceptibility tensor of a single photon wave packet on the photon mass-shell is derived. It is assumed that the probe photon is hard, the test photon is soft, and their total energy is below the electron-positron pair creation threshold. It turns out that a single photon wave pa... | 8.260544 | 9.373632 | 8.218654 | 7.855251 | 9.029652 | 9.241299 | 9.294084 | 8.822996 | 7.41584 | 8.475239 | 8.75458 | 7.995491 | 8.016258 | 7.987561 | 8.05397 | 8.256508 | 8.375763 | 8.321451 | 7.796545 | 8.210086 | 7.987886 |
1307.5997 | Giulio Bonelli | Giulio Bonelli, Antonio Sciarappa, Alessandro Tanzini and Petr Vasko | Vortex partition functions, wall crossing and equivariant Gromov-Witten
invariants | 44 pages, no figures: v2 version to appear in Comm. Math. Phys., a
new section added | Commun. Math. Phys. (2015) 333: 717 | 10.1007/s00220-014-2193-8 | SISSA 34/2013/MATE-FISI | hep-th math-ph math.AG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we identify the problem of equivariant vortex counting in a
$(2,2)$ supersymmetric two dimensional quiver gauged linear sigma model with
that of computing the equivariant Gromov-Witten invariants of the GIT quotient
target space determined by the quiver. We provide new contour integral formulae
for the ... | [
{
"created": "Tue, 23 Jul 2013 09:44:55 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Nov 2014 12:26:12 GMT",
"version": "v2"
}
] | 2019-12-06 | [
[
"Bonelli",
"Giulio",
""
],
[
"Sciarappa",
"Antonio",
""
],
[
"Tanzini",
"Alessandro",
""
],
[
"Vasko",
"Petr",
""
]
] | In this paper we identify the problem of equivariant vortex counting in a $(2,2)$ supersymmetric two dimensional quiver gauged linear sigma model with that of computing the equivariant Gromov-Witten invariants of the GIT quotient target space determined by the quiver. We provide new contour integral formulae for the ${... | 6.134279 | 7.04825 | 7.619727 | 6.756762 | 6.763594 | 7.173367 | 6.763776 | 6.813718 | 6.870393 | 8.039601 | 6.649864 | 6.06289 | 6.904118 | 6.112253 | 6.464958 | 6.035101 | 6.172917 | 6.083503 | 6.269623 | 6.824505 | 6.207233 |
0807.2773 | Bojan Pomori\v{s}ac | B. Pomori\v{s}ac | In search of the true vacuum: natural ordering, $\gamma$ condensate and
the last renormalization | 18 pages, 6 figures, minor revision | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | With the idea of canceling the leading divergence in vacuum energy of
$\varphi^4$ field theory a parameter is introduced that interpolates between
free Hamiltonian with or without normal ordering. This leads to a condensate
ground state having an arbitrary number of particle-particle pairs. In addition
to the usual s... | [
{
"created": "Thu, 17 Jul 2008 15:58:31 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Jul 2008 15:41:35 GMT",
"version": "v2"
}
] | 2008-07-18 | [
[
"Pomorišac",
"B.",
""
]
] | With the idea of canceling the leading divergence in vacuum energy of $\varphi^4$ field theory a parameter is introduced that interpolates between free Hamiltonian with or without normal ordering. This leads to a condensate ground state having an arbitrary number of particle-particle pairs. In addition to the usual sta... | 14.332761 | 12.65062 | 13.147573 | 12.684315 | 13.409724 | 12.884791 | 13.227189 | 13.434087 | 12.925708 | 14.033627 | 12.887197 | 13.25722 | 12.698746 | 12.630101 | 12.54826 | 12.768602 | 12.733948 | 12.640275 | 12.768825 | 12.756227 | 12.461431 |
0909.3153 | Maximilian Schmidt-Sommerfeld | Maximilian Schmidt-Sommerfeld | One-loop and D-instanton corrections to the effective action of open
string models | This article is essentially the main part of the author's PhD thesis | null | null | MPP-2009-161 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One-loop corrections to the gauge coupling and the gauge kinetic function in
certain classes of four-dimensional D-brane models are computed. It is
described how to determine D-instanton corrections to the superpotential and
the gauge kinetic function in such models. The Affleck-Dine-Seiberg
superpotential is rederiv... | [
{
"created": "Thu, 17 Sep 2009 07:27:15 GMT",
"version": "v1"
}
] | 2009-09-18 | [
[
"Schmidt-Sommerfeld",
"Maximilian",
""
]
] | One-loop corrections to the gauge coupling and the gauge kinetic function in certain classes of four-dimensional D-brane models are computed. It is described how to determine D-instanton corrections to the superpotential and the gauge kinetic function in such models. The Affleck-Dine-Seiberg superpotential is rederived... | 7.783694 | 6.820985 | 9.481454 | 6.836073 | 7.401077 | 6.731001 | 7.274744 | 6.765288 | 6.758681 | 8.512209 | 6.65168 | 6.669769 | 8.231825 | 6.886451 | 6.9265 | 6.71126 | 6.665842 | 6.66908 | 6.701192 | 7.784 | 6.946736 |
hep-th/9811077 | null | Richard Battye and Paul Sutcliffe | Solitons, Links and Knots | 24 pages plus 14 figures in GIF format | Proc.Roy.Soc.Lond. A455 (1999) 4305-4331 | 10.1098/rspa.1999.0502 | null | hep-th | null | Using numerical simulations of the full nonlinear equations of motion we
investigate topological solitons of a modified O(3) sigma model in three space
dimensions, in which the solitons are stabilized by the Hopf charge. We find
that for solitons up to charge five the solutions have the structure of closed
strings, w... | [
{
"created": "Mon, 9 Nov 1998 13:01:12 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Battye",
"Richard",
""
],
[
"Sutcliffe",
"Paul",
""
]
] | Using numerical simulations of the full nonlinear equations of motion we investigate topological solitons of a modified O(3) sigma model in three space dimensions, in which the solitons are stabilized by the Hopf charge. We find that for solitons up to charge five the solutions have the structure of closed strings, whi... | 10.033423 | 8.656661 | 9.416713 | 8.43414 | 8.707684 | 8.805186 | 9.501764 | 8.719564 | 8.159402 | 10.327159 | 8.459219 | 9.135174 | 8.997344 | 8.731433 | 8.862431 | 9.055048 | 8.465515 | 8.777453 | 8.7129 | 9.040111 | 8.580865 |
2004.12135 | Aradhita Chattopadhyaya | Aradhita Chattopadhyaya | Gravitational couplings in ${\cal N}=2$ heterotic compactifications with
Wilson lines | 37 pages, 1 figure, some typos fixed | null | 10.1007/JHEP07(2020)185 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we compute the gravitational couplings of the heterotic string
compactified on $(K3\times T^2)/\mathbb{Z}_N$ and $E_8\times E_8$ and predict
the Gopakumar Vafa invariants of the dual Calabi Yau manifold in presence of
Wilson lines. Here $\mathbb{Z}_N$ acts as an automorphism on $K3$ associated
with the ... | [
{
"created": "Sat, 25 Apr 2020 13:06:51 GMT",
"version": "v1"
},
{
"created": "Wed, 13 May 2020 13:22:20 GMT",
"version": "v2"
}
] | 2020-08-26 | [
[
"Chattopadhyaya",
"Aradhita",
""
]
] | In this paper we compute the gravitational couplings of the heterotic string compactified on $(K3\times T^2)/\mathbb{Z}_N$ and $E_8\times E_8$ and predict the Gopakumar Vafa invariants of the dual Calabi Yau manifold in presence of Wilson lines. Here $\mathbb{Z}_N$ acts as an automorphism on $K3$ associated with the co... | 5.842285 | 5.243511 | 6.561299 | 5.227665 | 5.650127 | 5.69829 | 5.201852 | 5.296153 | 5.281447 | 7.481723 | 5.309327 | 5.577131 | 5.884945 | 5.605773 | 5.496374 | 5.600698 | 5.498466 | 5.523179 | 5.539354 | 5.754582 | 5.597217 |
1703.07776 | Kenan Sogut | Kenan Sogut, Hilmi Yanar and Ali Havare | Production of Dirac Particles in External Electromagnetic Fields | Accepted for publication in Acta Physica Polonica B | null | 10.5506/APhysPolB.48.1493 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Pair creation of spin- 1/2 particles in Minkowski spacetime is investigated
by obtaining exact solu- tions of the Dirac equation in the presence of
electromagnetic fields and using them for determining the Bogoliubov
coefficients. The resulting particle creation number density depends on the
strength of the electric ... | [
{
"created": "Wed, 22 Mar 2017 14:02:02 GMT",
"version": "v1"
},
{
"created": "Wed, 3 May 2017 08:49:44 GMT",
"version": "v2"
},
{
"created": "Fri, 29 Sep 2017 13:11:52 GMT",
"version": "v3"
}
] | 2017-11-22 | [
[
"Sogut",
"Kenan",
""
],
[
"Yanar",
"Hilmi",
""
],
[
"Havare",
"Ali",
""
]
] | Pair creation of spin- 1/2 particles in Minkowski spacetime is investigated by obtaining exact solu- tions of the Dirac equation in the presence of electromagnetic fields and using them for determining the Bogoliubov coefficients. The resulting particle creation number density depends on the strength of the electric an... | 7.953236 | 6.780793 | 6.691167 | 6.959109 | 6.906299 | 7.54098 | 7.42997 | 6.641974 | 6.982292 | 7.079618 | 6.791894 | 6.857784 | 6.900661 | 6.859975 | 6.914509 | 6.765711 | 6.949711 | 6.818095 | 6.825161 | 6.859301 | 7.017203 |
hep-th/9908037 | Andrey Bytsenko | A.A. Bytsenko, A.E. Goncalves and F.L. Williams | Chern-Simons Invariants of Closed Hyperbolic 3-Manifolds | 10 pages, 2 diagrams | Mod.Phys.Lett. A15 (2000) 1031-1036 | 10.1142/S0217732300001298 | Preprint No. UEL/DF-990501 | hep-th | null | The Chern-Simons invariants of irreducible U(n)- flat connections on compact
hyperbolic 3-manifolds of the form {\Gamma}\H^3 are derived. The explicit
formula for the Chern-Simons functional is given in terms of Selberg type zeta
functions related to the twisted eta invariants of Atiyah-Patodi-Singer.
| [
{
"created": "Wed, 4 Aug 1999 18:12:58 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bytsenko",
"A. A.",
""
],
[
"Goncalves",
"A. E.",
""
],
[
"Williams",
"F. L.",
""
]
] | The Chern-Simons invariants of irreducible U(n)- flat connections on compact hyperbolic 3-manifolds of the form {\Gamma}\H^3 are derived. The explicit formula for the Chern-Simons functional is given in terms of Selberg type zeta functions related to the twisted eta invariants of Atiyah-Patodi-Singer. | 8.585267 | 6.5468 | 10.197826 | 7.358814 | 7.784115 | 7.123088 | 7.017588 | 6.906656 | 6.383525 | 10.588749 | 7.322453 | 7.818922 | 9.434281 | 8.188824 | 8.022018 | 7.829033 | 8.095729 | 8.256059 | 8.180636 | 9.265226 | 7.965282 |
1110.0867 | Marcelo Botta Cantcheff | Marcelo Botta Cantcheff | Emergent spacetime, and a model for unitary gravitational collapse in
AdS | 19 pages, 1 figure | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a CFT unitary description of the gravitational collapse. The
starting point is the model of a black hole in AdS proposed by Maldacena in
arXiv: 0106112 [hep-th]. We show that by proposing a two-copies version of the
AdS/CFT conjecture, the process of formation of black holes so as other
spacetimes with hor... | [
{
"created": "Tue, 4 Oct 2011 23:25:28 GMT",
"version": "v1"
}
] | 2011-10-06 | [
[
"Cantcheff",
"Marcelo Botta",
""
]
] | We propose a CFT unitary description of the gravitational collapse. The starting point is the model of a black hole in AdS proposed by Maldacena in arXiv: 0106112 [hep-th]. We show that by proposing a two-copies version of the AdS/CFT conjecture, the process of formation of black holes so as other spacetimes with horiz... | 12.120004 | 13.458984 | 13.375103 | 12.510158 | 12.34394 | 13.042161 | 12.529471 | 11.82258 | 12.29108 | 14.107722 | 11.84854 | 12.26248 | 11.844447 | 11.671322 | 11.627137 | 11.697344 | 11.725154 | 11.709149 | 11.737483 | 11.956512 | 11.69358 |
0708.3386 | Spyros Avramis | Spyros D. Avramis, Alex Kehagias, Constantina Mattheopoulou | Three-dimensional AdS gravity and extremal CFTs at c=8m | 17 pages, harvmac; v2: references added, version accepted in JHEP | JHEP 0711:022,2007 | 10.1088/1126-6708/2007/11/022 | null | hep-th | null | We note that Witten's proposed duality between extremal c=24k CFTs and
three-dimensional anti-de Sitter gravity may possibly be extended to central
charges that are multiples of 8, for which extremal self-dual CFTs are known to
exist up to c=40. All CFTs of this type with central charge 24 or higher,
provided that th... | [
{
"created": "Fri, 24 Aug 2007 19:29:38 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Oct 2007 19:59:25 GMT",
"version": "v2"
}
] | 2009-06-10 | [
[
"Avramis",
"Spyros D.",
""
],
[
"Kehagias",
"Alex",
""
],
[
"Mattheopoulou",
"Constantina",
""
]
] | We note that Witten's proposed duality between extremal c=24k CFTs and three-dimensional anti-de Sitter gravity may possibly be extended to central charges that are multiples of 8, for which extremal self-dual CFTs are known to exist up to c=40. All CFTs of this type with central charge 24 or higher, provided that they... | 9.448462 | 8.833779 | 10.359616 | 9.220491 | 9.448534 | 9.129314 | 9.657773 | 9.057494 | 8.610851 | 10.438769 | 8.666829 | 8.701181 | 9.474824 | 8.690063 | 8.806864 | 8.543673 | 8.736545 | 8.997874 | 8.716877 | 9.1315 | 8.787322 |
0904.2205 | Daniel Ferrante | D. D. Ferrante | Symmetry Breaking: A New Paradigm for Non-Perturbative QFT and
Topological Transitions | 103 pages, 56 figures, author's Ph.D. thesis | null | null | null | hep-th gr-qc hep-lat math-ph math.MP | http://creativecommons.org/licenses/by-nc-sa/3.0/ | Symmetry Breaking is used as an "underlying principle", bringing different
features of QFT to the foreground. However, the understanding of Symmetry
Breaking that is used here is quite different from what is done in the
mainstream: Symmetry Breaking is understood as the solution set of a given QFT,
its vacuum manifol... | [
{
"created": "Tue, 14 Apr 2009 20:39:25 GMT",
"version": "v1"
}
] | 2009-04-16 | [
[
"Ferrante",
"D. D.",
""
]
] | Symmetry Breaking is used as an "underlying principle", bringing different features of QFT to the foreground. However, the understanding of Symmetry Breaking that is used here is quite different from what is done in the mainstream: Symmetry Breaking is understood as the solution set of a given QFT, its vacuum manifold,... | 15.789751 | 16.979673 | 17.06069 | 16.196806 | 16.015827 | 17.025799 | 16.700733 | 16.60158 | 16.84318 | 16.794422 | 16.211637 | 15.577271 | 16.139587 | 15.572347 | 15.610888 | 15.537138 | 15.40843 | 15.701582 | 15.375388 | 16.109497 | 15.452095 |
hep-th/0201099 | Shahin Rouhani | S. Moghimi-Araghi, S. Rouhani and M. Saadat | Use of Nilpotent weights in Logarithmic Conformal Field Theories | 21 pages. Talk delivered in School and Workshop on Logarithmic
Conformal Field Theory, Tehran, Iran, September 2001 | Int.J.Mod.Phys. A18 (2003) 4747-4770 | 10.1142/S0217751X03016914 | null | hep-th | null | We show that logarithmic conformal field theories may be derived using
nilpotent scale transformation. Using such nilpotent weights we derive
properties of LCFT's, such as two and three point correlation functions solely
from symmetry arguments. Singular vectors and the Kac determinant may also be
obtained using thes... | [
{
"created": "Tue, 15 Jan 2002 08:42:58 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Moghimi-Araghi",
"S.",
""
],
[
"Rouhani",
"S.",
""
],
[
"Saadat",
"M.",
""
]
] | We show that logarithmic conformal field theories may be derived using nilpotent scale transformation. Using such nilpotent weights we derive properties of LCFT's, such as two and three point correlation functions solely from symmetry arguments. Singular vectors and the Kac determinant may also be obtained using these ... | 13.660137 | 12.635536 | 14.608958 | 12.351341 | 13.443727 | 13.696637 | 12.133873 | 12.535865 | 13.145897 | 16.219608 | 12.670478 | 13.032994 | 14.556272 | 13.107745 | 12.82253 | 13.161339 | 12.78833 | 12.937825 | 13.384186 | 14.175161 | 12.661639 |
0709.4163 | Ali Alavi | S. A. Alavi | On statistical mechanics in noncommutative spaces | 9 pages, no figures | Prob.Atomic Sci.Technol.3:301-304,2007 | null | null | hep-th | null | We study the formulation of quantum statistical mechanics in noncommutative
spaces. We construct microcanonical and canonical ensemble theory in
noncommutative spaces. We consider for illustration some basic and important
examples in the framework of noncommutative statistical mechanics : (i). An
electron in a magnet... | [
{
"created": "Wed, 26 Sep 2007 13:58:05 GMT",
"version": "v1"
}
] | 2009-06-10 | [
[
"Alavi",
"S. A.",
""
]
] | We study the formulation of quantum statistical mechanics in noncommutative spaces. We construct microcanonical and canonical ensemble theory in noncommutative spaces. We consider for illustration some basic and important examples in the framework of noncommutative statistical mechanics : (i). An electron in a magnetic... | 7.087946 | 6.581923 | 7.09525 | 6.345049 | 6.81558 | 6.880076 | 6.671629 | 6.697651 | 6.718965 | 7.192889 | 6.775284 | 6.482647 | 6.7693 | 6.628304 | 6.620378 | 6.582701 | 6.550192 | 6.553271 | 6.622208 | 7.116833 | 6.539104 |
1901.10492 | Niklas Mueller | Niklas Mueller and Raju Venugopalan | Constructing phase space distributions with internal symmetries | 13 pages, references added, typo corrected, accepted for publication
in Phys. Rev. D | Phys. Rev. D 99, 056003 (2019) | 10.1103/PhysRevD.99.056003 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss an ab initio world-line approach to constructing phase space
distributions in systems with internal symmetries. Starting from the
Schwinger-Keldysh real time path integral in quantum field theory, we derive
the most general extension of the Wigner phase space distribution to include
color and spin degrees ... | [
{
"created": "Tue, 29 Jan 2019 19:00:03 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Feb 2019 16:11:10 GMT",
"version": "v2"
}
] | 2019-03-13 | [
[
"Mueller",
"Niklas",
""
],
[
"Venugopalan",
"Raju",
""
]
] | We discuss an ab initio world-line approach to constructing phase space distributions in systems with internal symmetries. Starting from the Schwinger-Keldysh real time path integral in quantum field theory, we derive the most general extension of the Wigner phase space distribution to include color and spin degrees of... | 9.063455 | 10.085512 | 9.251673 | 8.897816 | 10.031545 | 9.105484 | 10.022717 | 9.423477 | 9.117477 | 10.33436 | 8.945308 | 9.044627 | 9.113463 | 8.98898 | 9.243381 | 9.187254 | 9.179746 | 8.985811 | 9.150965 | 9.14089 | 8.856928 |
hep-th/9903078 | Marco M. Caldarelli | Marco M. Caldarelli and Dietmar Klemm | M-Theory and Stringy Corrections to Anti-de Sitter Black Holes and
Conformal Field Theories | 29 pages, revtex, 6 figures using epsfig, typos corrected, 1
reference added, final version to appear in Nucl. Phys. B | Nucl.Phys. B555 (1999) 157-182 | 10.1016/S0550-3213(99)00342-9 | UTF 431 | hep-th | null | We consider black holes in anti-de Sitter space AdS_{p+2} (p = 2,3,5), which
have hyperbolic, flat or spherical event horizons. The $O(\alpha'^3)$
corrections (or the leading corrections in powers of the eleven-dimensional
Planck length) to the black hole metrics are computed for the various
topologies and dimensions... | [
{
"created": "Tue, 9 Mar 1999 20:43:15 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 1999 18:29:51 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Jul 1999 17:14:50 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Caldarelli",
"Marco M.",
""
],
[
"Klemm",
"Dietmar",
""
]
] | We consider black holes in anti-de Sitter space AdS_{p+2} (p = 2,3,5), which have hyperbolic, flat or spherical event horizons. The $O(\alpha'^3)$ corrections (or the leading corrections in powers of the eleven-dimensional Planck length) to the black hole metrics are computed for the various topologies and dimensions. ... | 6.709529 | 7.014661 | 6.989898 | 6.547778 | 6.94569 | 7.279841 | 7.149417 | 6.566154 | 6.855913 | 7.518255 | 6.492075 | 6.942693 | 6.841827 | 6.580849 | 6.772838 | 6.688106 | 6.788801 | 6.659401 | 6.684831 | 6.955852 | 6.618741 |
2007.00855 | Chen-Te Ma | Chen-Te Ma and Chih-Hung Wu | Quantum Entanglement and Spectral Form Factor | 21 pages, 8 figures, minor changes | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We replace a Hamiltonian with a modular Hamiltonian in the spectral form
factor and the level spacing distribution function. This study establishes a
connection between quantities within Quantum Entanglement and Quantum Chaos. To
have a universal study for Quantum Entanglement, we consider the Gaussian
random 2-qubit... | [
{
"created": "Thu, 2 Jul 2020 03:40:28 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Nov 2021 05:18:19 GMT",
"version": "v2"
},
{
"created": "Mon, 14 Nov 2022 00:02:48 GMT",
"version": "v3"
}
] | 2022-11-15 | [
[
"Ma",
"Chen-Te",
""
],
[
"Wu",
"Chih-Hung",
""
]
] | We replace a Hamiltonian with a modular Hamiltonian in the spectral form factor and the level spacing distribution function. This study establishes a connection between quantities within Quantum Entanglement and Quantum Chaos. To have a universal study for Quantum Entanglement, we consider the Gaussian random 2-qubit m... | 12.780042 | 12.191421 | 14.535504 | 11.928491 | 13.332746 | 12.744976 | 11.748323 | 12.247151 | 11.734935 | 14.238909 | 11.739142 | 11.843386 | 12.710331 | 11.788635 | 12.075369 | 11.869143 | 11.905315 | 11.8458 | 11.867785 | 12.141253 | 11.705051 |
hep-th/0609016 | Harikumar E | E. Harikumar, Amilcar R. Queiroz, P. Teotonio-Sobrinho | Index Theorem for the $q$-Deformed Fuzzy Sphere | 15 pages, minor changes | J.Phys.A40:3671-3682,2007 | 10.1088/1751-8113/40/13/023 | null | hep-th | null | We calculate the index of the Dirac operator defined on the q-deformed fuzzy
sphere. The index of the Dirac operator is related to its net chiral zero modes
and thus to the trace of the chirality operator. We show that for the
q-deformed fuzzy sphere, a $\uq$ invariant trace of the chirality operator
gives the q-dime... | [
{
"created": "Sat, 2 Sep 2006 06:18:35 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Oct 2006 03:36:59 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Harikumar",
"E.",
""
],
[
"Queiroz",
"Amilcar R.",
""
],
[
"Teotonio-Sobrinho",
"P.",
""
]
] | We calculate the index of the Dirac operator defined on the q-deformed fuzzy sphere. The index of the Dirac operator is related to its net chiral zero modes and thus to the trace of the chirality operator. We show that for the q-deformed fuzzy sphere, a $\uq$ invariant trace of the chirality operator gives the q-dimens... | 7.00928 | 6.882317 | 7.01019 | 6.53538 | 7.380044 | 7.075453 | 7.718685 | 6.593866 | 6.822517 | 8.017833 | 6.828557 | 6.965805 | 6.588496 | 6.759859 | 6.83185 | 7.10538 | 6.848902 | 6.799206 | 6.863931 | 6.685763 | 6.808163 |
1106.1602 | Anastasia Doikou | Anastasia Doikou | Defects in the discrete non-linear Schrodinger model | 18 pages, Latex. Comments and clarifications introduced. One
reference added | Nucl.Phys.B854:153-165,2012 | 10.1016/j.nuclphysb.2011.08.015 | null | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The discrete non-linear Schrodinger (NLS) model in the presence of an
integrable defect is examined. The problem is viewed from a purely algebraic
point of view, starting from the fundamental algebraic relations that rule the
model. The first charges in involution are explicitly constructed, as well as
the correspond... | [
{
"created": "Wed, 8 Jun 2011 17:33:38 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Sep 2011 11:36:18 GMT",
"version": "v2"
}
] | 2011-10-20 | [
[
"Doikou",
"Anastasia",
""
]
] | The discrete non-linear Schrodinger (NLS) model in the presence of an integrable defect is examined. The problem is viewed from a purely algebraic point of view, starting from the fundamental algebraic relations that rule the model. The first charges in involution are explicitly constructed, as well as the correspondin... | 13.439443 | 11.329443 | 14.738657 | 11.642158 | 11.43979 | 12.370609 | 13.095261 | 10.990414 | 10.816307 | 14.204661 | 10.937098 | 11.957067 | 14.350079 | 13.020637 | 12.663584 | 11.774622 | 12.501825 | 12.30988 | 12.317161 | 14.017934 | 11.522775 |
hep-th/0306297 | Alberto Iglesias | Alberto Iglesias and Zurab Kakushadze | A Novel Approach to the Cosmological Constant Problem | 20 pages, revtex | Int.J.Mod.Phys. A19 (2004) 4621-4640 | 10.1142/S0217751X04019901 | YITP-SB-06-33 | hep-th | null | We propose a novel infinite-volume brane world scenario where we live on a
non-inflating spherical 3-brane, whose radius is somewhat larger than the
present Hubble size, embedded in higher dimensional bulk. Once we include
higher curvature terms in the bulk, we find completely smooth solutions with
the property that ... | [
{
"created": "Mon, 30 Jun 2003 17:37:43 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Iglesias",
"Alberto",
""
],
[
"Kakushadze",
"Zurab",
""
]
] | We propose a novel infinite-volume brane world scenario where we live on a non-inflating spherical 3-brane, whose radius is somewhat larger than the present Hubble size, embedded in higher dimensional bulk. Once we include higher curvature terms in the bulk, we find completely smooth solutions with the property that th... | 11.724958 | 11.370206 | 11.97628 | 10.967453 | 11.797439 | 11.392033 | 11.28663 | 11.236914 | 10.985048 | 12.224924 | 11.187718 | 11.333433 | 11.020807 | 10.761411 | 10.673447 | 11.43018 | 11.141819 | 10.942199 | 11.006966 | 10.86412 | 10.748827 |
hep-th/9903126 | Mauro Negrao | M. S. Goes-Negrao, M. R. Negrao, A. B. Penna-Firme | (2,0)-Super-Yang-Mills Coupled to Non-Linear Sigma-Model | 18 pages, no figures, revised version | Int.J.Mod.Phys. A16 (2001) 189-200 | 10.1142/S0217751X01002804 | null | hep-th | null | Considering a class of (2,0)-super-Yang-Mills multiplets that accommodate a
pair of independent gauge potentials in connection with a single symmetry
group, we present here their coupling to ordinary matter and to non-linear
$\sigma$-models in (2,0)-superspace. The dynamics and the couplings of the
gauge potentials a... | [
{
"created": "Mon, 15 Mar 1999 19:08:43 GMT",
"version": "v1"
},
{
"created": "Mon, 3 May 1999 19:01:08 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Jul 1999 22:29:23 GMT",
"version": "v3"
},
{
"created": "Mon, 19 Jul 1999 17:35:30 GMT",
"version": "v4"
},
{
"cr... | 2015-06-26 | [
[
"Goes-Negrao",
"M. S.",
""
],
[
"Negrao",
"M. R.",
""
],
[
"Penna-Firme",
"A. B.",
""
]
] | Considering a class of (2,0)-super-Yang-Mills multiplets that accommodate a pair of independent gauge potentials in connection with a single symmetry group, we present here their coupling to ordinary matter and to non-linear $\sigma$-models in (2,0)-superspace. The dynamics and the couplings of the gauge potentials are... | 12.249891 | 11.737581 | 12.665809 | 11.056547 | 10.685006 | 11.722767 | 10.281093 | 11.598652 | 10.519141 | 13.181832 | 10.172467 | 10.277615 | 11.200339 | 10.742624 | 10.485756 | 10.616733 | 10.824157 | 10.525678 | 10.677279 | 11.579537 | 10.40055 |
hep-th/9212075 | Christof Schmidhuber | Christof Schmidhuber (Caltech) | Exactly Marginal Operators and Running Coupling Constants in 2D Gravity | 22 pages, plain Tex, CALT-68-1817 (Some modifications but same
results. Figures will be faxed upon request.) | Nucl.Phys. B404 (1993) 342-358 | 10.1016/0550-3213(93)90483-6 | null | hep-th | null | The Liouville action for two--dimensional quantum gravity coupled to
interacting matter contains terms that have not been considered previously.
They are crucial for understanding the renormalization group flow and can be
observed in recent matrix model results for the phase diagram of the
Sine--Gordon model coupled ... | [
{
"created": "Fri, 11 Dec 1992 07:12:41 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Dec 1992 07:59:55 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Feb 1993 04:37:33 GMT",
"version": "v3"
}
] | 2009-10-22 | [
[
"Schmidhuber",
"Christof",
"",
"Caltech"
]
] | The Liouville action for two--dimensional quantum gravity coupled to interacting matter contains terms that have not been considered previously. They are crucial for understanding the renormalization group flow and can be observed in recent matrix model results for the phase diagram of the Sine--Gordon model coupled to... | 14.468663 | 11.559156 | 12.277291 | 11.245635 | 12.450324 | 11.228932 | 10.720401 | 11.56759 | 11.653872 | 11.996548 | 12.037519 | 11.3595 | 11.869843 | 11.460603 | 11.747873 | 11.790164 | 11.727276 | 11.348277 | 11.940989 | 12.066051 | 11.421367 |
hep-th/0305194 | John McGreevy | John McGreevy, Joerg Teschner, and Herman Verlinde | Classical and Quantum D-branes in 2D String Theory | 28 pages, 2 figures. v2: discussion of descent relation clarified,
added refs | JHEP 0401 (2004) 039 | 10.1088/1126-6708/2004/01/039 | PUPT-2087 | hep-th | null | We investigate two classes of D-branes in 2-d string theory, corresponding to
extended and localized branes, respectively. We compute the string emission
during tachyon condensation and reinterpret the results within the $c=1$ matrix
model. As in hep-th/0304224, we find that the extended branes describe
classical eig... | [
{
"created": "Thu, 22 May 2003 19:50:22 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Dec 2003 22:09:09 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"McGreevy",
"John",
""
],
[
"Teschner",
"Joerg",
""
],
[
"Verlinde",
"Herman",
""
]
] | We investigate two classes of D-branes in 2-d string theory, corresponding to extended and localized branes, respectively. We compute the string emission during tachyon condensation and reinterpret the results within the $c=1$ matrix model. As in hep-th/0304224, we find that the extended branes describe classical eigen... | 12.355594 | 11.781349 | 14.94811 | 10.736126 | 11.700416 | 11.93176 | 11.017915 | 10.690372 | 11.136551 | 14.512017 | 10.625739 | 11.77285 | 12.633637 | 11.431019 | 11.673919 | 11.585231 | 11.46036 | 11.719153 | 12.007914 | 13.068042 | 11.762483 |
1701.06572 | Gokce Basar | Gokce Basar, Gerald V. Dunne, and Mithat Unsal | Quantum Geometry of Resurgent Perturbative/Nonperturbative Relations | 50 pages, 3 figures | null | 10.1007/JHEP05(2017)087 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For a wide variety of quantum potentials, including the textbook `instanton'
examples of the periodic cosine and symmetric double-well potentials, the
perturbative data coming from fluctuations about the vacuum saddle encodes all
non-perturbative data in all higher non-perturbative sectors. Here we unify
these exampl... | [
{
"created": "Mon, 23 Jan 2017 19:00:02 GMT",
"version": "v1"
}
] | 2017-06-23 | [
[
"Basar",
"Gokce",
""
],
[
"Dunne",
"Gerald V.",
""
],
[
"Unsal",
"Mithat",
""
]
] | For a wide variety of quantum potentials, including the textbook `instanton' examples of the periodic cosine and symmetric double-well potentials, the perturbative data coming from fluctuations about the vacuum saddle encodes all non-perturbative data in all higher non-perturbative sectors. Here we unify these examples... | 13.414476 | 15.024515 | 17.306705 | 14.419996 | 13.680583 | 15.034971 | 15.194708 | 14.766842 | 14.312521 | 16.44783 | 14.072383 | 13.672435 | 13.41503 | 13.38513 | 13.308843 | 13.150797 | 13.313061 | 13.252562 | 12.926133 | 13.742454 | 13.013557 |
1604.01556 | Elena Melkumova | D.V.Gal'tsov, E.Yu.Melkumova and P.Spirin | Domain Walls: Momentum Conservation in Absence of Asymptotic States | 6 pages, ws-procs975x65 style, to be published as Proceeding of the
14th Marcel Grossmann Meeting, Rome, 12-18 July, 2015 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gravitational potentials of the domain walls in the linearized gravity are
growing with distance, so the particle scattering by the wall can not be
described in terms of free asymptotic states. In the non-relativistic case this
problem is solved using the concept of the potential energy. We show that in
the relativis... | [
{
"created": "Wed, 6 Apr 2016 09:40:30 GMT",
"version": "v1"
}
] | 2016-04-07 | [
[
"Gal'tsov",
"D. V.",
""
],
[
"Melkumova",
"E. Yu.",
""
],
[
"Spirin",
"P.",
""
]
] | Gravitational potentials of the domain walls in the linearized gravity are growing with distance, so the particle scattering by the wall can not be described in terms of free asymptotic states. In the non-relativistic case this problem is solved using the concept of the potential energy. We show that in the relativisti... | 16.105007 | 17.051947 | 15.300594 | 14.257126 | 17.157867 | 16.347282 | 17.542665 | 15.082209 | 14.972881 | 16.501627 | 14.080282 | 14.343553 | 15.031097 | 14.684799 | 14.827974 | 14.538628 | 14.76221 | 14.990434 | 14.710516 | 15.504663 | 14.04884 |
1004.3772 | Alexander Zhidenko | R. A. Konoplya and A. Zhidenko | Long life of Gauss-Bonnet corrected black holes | 13 pages, 14 figures | Phys.Rev.D82:084003,2010 | 10.1103/PhysRevD.82.084003 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dictated by the string theory and various higher dimensional scenarios, black
holes in $D>4$-dimensional space-times must have higher curvature corrections.
The first and dominant term is quadratic in curvature, and called the
Gauss-Bonnet (GB) term. We shall show that although the Gauss-Bonnet correction
changes bla... | [
{
"created": "Wed, 21 Apr 2010 18:53:06 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Apr 2010 13:40:44 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Apr 2010 20:08:56 GMT",
"version": "v3"
},
{
"created": "Wed, 1 Sep 2010 22:19:31 GMT",
"version": "v4"
},
{
"cr... | 2011-12-15 | [
[
"Konoplya",
"R. A.",
""
],
[
"Zhidenko",
"A.",
""
]
] | Dictated by the string theory and various higher dimensional scenarios, black holes in $D>4$-dimensional space-times must have higher curvature corrections. The first and dominant term is quadratic in curvature, and called the Gauss-Bonnet (GB) term. We shall show that although the Gauss-Bonnet correction changes black... | 10.186382 | 12.039886 | 10.898606 | 10.658913 | 11.461224 | 10.985576 | 11.131032 | 10.474707 | 10.266322 | 11.758659 | 10.546436 | 10.000852 | 9.969339 | 9.749523 | 9.905336 | 9.758481 | 9.809602 | 9.834548 | 9.803726 | 9.464293 | 9.986851 |
hep-th/0402090 | Arjan Keurentjes | Arjan Keurentjes | E_11: Sign of the times | 20 pages, LaTeX, 1 figure; v2. typo's corrected, references added | Nucl.Phys. B697 (2004) 302-318 | 10.1016/j.nuclphysb.2004.06.058 | null | hep-th | null | We discuss the signature of space-time in the context of the E_11
-conjecture. In this setting, the space-time signature depends on the choice of
basis for the ``gravitational sub-algebra'' A_10, and Weyl transformations
connect interpretations with different signatures of space-time. Also the sign
of the 4-form gaug... | [
{
"created": "Thu, 12 Feb 2004 11:33:09 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 2004 18:32:20 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Keurentjes",
"Arjan",
""
]
] | We discuss the signature of space-time in the context of the E_11 -conjecture. In this setting, the space-time signature depends on the choice of basis for the ``gravitational sub-algebra'' A_10, and Weyl transformations connect interpretations with different signatures of space-time. Also the sign of the 4-form gauge ... | 11.764441 | 11.883247 | 13.012716 | 11.673072 | 12.48869 | 13.070067 | 12.514335 | 11.922287 | 12.449443 | 14.950426 | 11.649854 | 11.27631 | 12.120261 | 11.774108 | 12.313074 | 11.275484 | 11.66026 | 11.291232 | 11.375133 | 12.33137 | 11.222957 |
hep-th/0309152 | Takashi Torii | Kei-ichi Maeda, and Takashi Torii | Covariant Gravitational Equations on Brane World with Gauss-Bonnet term | 14 pages, no figure | Phys.Rev. D69 (2004) 024002 | 10.1103/PhysRevD.69.024002 | WU-AP/173/03 | hep-th gr-qc | null | We present the covariant gravitational equations to describe a
four-dimensional brane world in the case with the Gauss-Bonnet term in a bulk
spacetime, assuming that gravity is confined on the $Z_2$ symmetric brane. It
contains some components of five-dimensional Weyl curvature ($E_{\mu\nu}$)
which describes all effe... | [
{
"created": "Tue, 16 Sep 2003 03:56:49 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Maeda",
"Kei-ichi",
""
],
[
"Torii",
"Takashi",
""
]
] | We present the covariant gravitational equations to describe a four-dimensional brane world in the case with the Gauss-Bonnet term in a bulk spacetime, assuming that gravity is confined on the $Z_2$ symmetric brane. It contains some components of five-dimensional Weyl curvature ($E_{\mu\nu}$) which describes all effect... | 9.978868 | 9.860994 | 8.734783 | 8.273324 | 9.062391 | 9.166447 | 9.196837 | 8.565219 | 9.311726 | 9.116097 | 9.879456 | 9.475594 | 9.391168 | 9.24161 | 9.114109 | 9.277318 | 9.303936 | 9.008008 | 9.66746 | 9.799908 | 9.404228 |
1912.05865 | Nina Javerzat | Nina Javerzat, Marco Picco, Raoul Santachiara | Three- and four-point connectivities of two-dimensional critical $Q-$
Potts random clusters on the torus | 30 pages, 9 figures. Figure captions have been added, the notation in
section 3.2 has been slightly changed, and typos in equations (4.21) and
(5.3) have been corrected | null | 10.1088/1742-5468/ab7c5e | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a recent paper, we considered the effects of the torus lattice topology on
the two-point connectivity of $Q-$ Potts clusters. These effects are universal
and probe non-trivial structure constants of the theory. We complete here this
work by considering the torus corrections to the three- and four-point
connectivit... | [
{
"created": "Thu, 12 Dec 2019 10:20:27 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Apr 2020 15:40:04 GMT",
"version": "v2"
}
] | 2020-06-24 | [
[
"Javerzat",
"Nina",
""
],
[
"Picco",
"Marco",
""
],
[
"Santachiara",
"Raoul",
""
]
] | In a recent paper, we considered the effects of the torus lattice topology on the two-point connectivity of $Q-$ Potts clusters. These effects are universal and probe non-trivial structure constants of the theory. We complete here this work by considering the torus corrections to the three- and four-point connectivitie... | 11.155646 | 12.312369 | 12.031019 | 12.344611 | 12.18148 | 13.666829 | 11.757358 | 11.298802 | 11.351113 | 14.54051 | 11.118216 | 11.020539 | 11.647782 | 10.587336 | 10.821526 | 10.820541 | 10.214484 | 10.864017 | 10.485114 | 11.226289 | 10.842472 |
1403.8087 | Aleksandra Anokhina | A.Anokhina and A.Morozov | Towards R-matrix construction of Khovanov-Rozansky polynomials. I.
Primary $T$-deformation of HOMFLY | 146 pages; some points clarified, some typos corrected | JHEP07(2014)063 | 10.1007/JHEP07(2014)063 | ITEP/TH-07/14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We elaborate on the simple alternative from arXiv:1308.5759 to the
matrix-factorization construction of Khovanov-Rozansky (KR) polynomials for
arbitrary knots and links in the fundamental representation of arbitrary SL(N).
Construction consists of 2 steps: first, with every link diagram with m
vertices one associates... | [
{
"created": "Mon, 31 Mar 2014 16:58:33 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Jun 2014 17:01:40 GMT",
"version": "v2"
}
] | 2014-10-14 | [
[
"Anokhina",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | We elaborate on the simple alternative from arXiv:1308.5759 to the matrix-factorization construction of Khovanov-Rozansky (KR) polynomials for arbitrary knots and links in the fundamental representation of arbitrary SL(N). Construction consists of 2 steps: first, with every link diagram with m vertices one associates a... | 13.435556 | 13.744322 | 16.254097 | 13.262923 | 14.423124 | 14.147138 | 14.160112 | 13.792546 | 13.460072 | 16.151894 | 13.306756 | 13.052719 | 13.216266 | 12.661712 | 13.248919 | 12.955494 | 12.849862 | 13.062628 | 13.14769 | 13.639566 | 12.795274 |
1009.4915 | Francisco A. Brito | F.A. Brito and E. Passos | Spectral dimension of Horava-Snyder spacetime and the $AdS_2\times S^2$
momentum space | 5 pages, revtex, 1 figure, version to appear in EPL | null | 10.1209/0295-5075/99/60003 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the UV-regime at the Lifshitz point $z=3$ is equivalent to work
with a momenta manifold whose topology is the same as that of an $AdS_2\times
S^2$ space. According to Snyder's theory, curved momentum space is related to
non-commutative quantized spacetime. In this sense, our analysis suggests an
equivale... | [
{
"created": "Fri, 24 Sep 2010 19:35:06 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Aug 2012 19:36:42 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Brito",
"F. A.",
""
],
[
"Passos",
"E.",
""
]
] | We show that the UV-regime at the Lifshitz point $z=3$ is equivalent to work with a momenta manifold whose topology is the same as that of an $AdS_2\times S^2$ space. According to Snyder's theory, curved momentum space is related to non-commutative quantized spacetime. In this sense, our analysis suggests an equivalenc... | 11.704031 | 11.222795 | 11.042846 | 10.529757 | 10.284637 | 11.121962 | 11.376471 | 10.415419 | 10.128808 | 11.31452 | 10.704918 | 10.716579 | 10.673326 | 10.942029 | 11.18829 | 10.916853 | 11.17423 | 10.499863 | 10.515737 | 10.688759 | 10.464664 |
2207.06435 | Stefano Baiguera | Stefano Baiguera, Lorenzo Cederle and Silvia Penati | Supersymmetric Galilean Electrodynamics | 38+18 pages, 12 figures; v2: reference added | JHEP 09 (2022) 237 | 10.1007/JHEP09(2022)237 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In 2+1 dimensions, we propose a renormalizable non-linear sigma model action
which describes the $\mathcal{N}=2$ supersymmetric generalization of Galilean
Electrodynamics. We first start with the simplest model obtained by null
reduction of the relativistic Abelian $\mathcal{N}=1$ supersymmetric QED in 3+1
dimensions... | [
{
"created": "Wed, 13 Jul 2022 18:00:03 GMT",
"version": "v1"
},
{
"created": "Sat, 1 Oct 2022 12:16:14 GMT",
"version": "v2"
}
] | 2022-10-19 | [
[
"Baiguera",
"Stefano",
""
],
[
"Cederle",
"Lorenzo",
""
],
[
"Penati",
"Silvia",
""
]
] | In 2+1 dimensions, we propose a renormalizable non-linear sigma model action which describes the $\mathcal{N}=2$ supersymmetric generalization of Galilean Electrodynamics. We first start with the simplest model obtained by null reduction of the relativistic Abelian $\mathcal{N}=1$ supersymmetric QED in 3+1 dimensions a... | 8.737939 | 8.434581 | 9.598103 | 8.34804 | 9.243813 | 8.506 | 8.866138 | 8.379653 | 8.029057 | 10.337204 | 8.049459 | 8.525716 | 8.583822 | 8.294771 | 8.238074 | 8.367996 | 8.282065 | 8.344287 | 8.174771 | 8.787121 | 8.329157 |
1708.01779 | Yan-Gang Miao | Yan-Gang Miao, Long Zhao | Complexity/Action duality of shock wave geometry in a massive gravity
theory | v1: 19 pages, 2 figures; v2: clarifications added, the final version
to appear in Physical Review D | Phys. Rev. D 97, 024035 (2018) | 10.1103/PhysRevD.97.024035 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | On the holographic complexity dual to the bulk action, we investigate the
action growth for a shock wave geometry in a massive gravity theory within the
Wheeler-De Witt (WDW) patch at the late time limit. For a global shock wave,
the graviton mass does not affect the action growth in the bulk, i.e. the
complexity on ... | [
{
"created": "Sat, 5 Aug 2017 15:24:03 GMT",
"version": "v1"
},
{
"created": "Sat, 30 Dec 2017 07:37:04 GMT",
"version": "v2"
}
] | 2018-02-13 | [
[
"Miao",
"Yan-Gang",
""
],
[
"Zhao",
"Long",
""
]
] | On the holographic complexity dual to the bulk action, we investigate the action growth for a shock wave geometry in a massive gravity theory within the Wheeler-De Witt (WDW) patch at the late time limit. For a global shock wave, the graviton mass does not affect the action growth in the bulk, i.e. the complexity on th... | 6.723229 | 5.869487 | 6.741208 | 5.894003 | 6.09155 | 5.957756 | 6.010145 | 6.441177 | 5.991118 | 6.880617 | 6.153596 | 5.823375 | 6.16866 | 6.064363 | 5.99517 | 5.904796 | 6.041262 | 5.946424 | 6.010945 | 6.412819 | 6.009118 |
1007.0191 | Vladimir Zhukovsky | D. Ebert, V.Ch. Zhukovsky, and A.V. Tyukov | Dynamical Fermion Masses Under the Influence of Kaluza-Klein Fermions
and a Bulk Abelian Gauge Field | 9 pages, 4 figures | Mod.Phys.Lett.A25:2933-2945,2010 | 10.1142/S0217732310034249 | HU-EP-10/31 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dynamical fermion mass generation on a 3-brane in the 5D space-time is
discussed in a model with bulk fermions in interaction with fermions on the
brane assuming the presence of a constant abelian gauge field component $A_5$
in the bulk. We calculate the effective potential as a function of the fermion
masses and... | [
{
"created": "Thu, 1 Jul 2010 15:08:07 GMT",
"version": "v1"
}
] | 2010-11-03 | [
[
"Ebert",
"D.",
""
],
[
"Zhukovsky",
"V. Ch.",
""
],
[
"Tyukov",
"A. V.",
""
]
] | The dynamical fermion mass generation on a 3-brane in the 5D space-time is discussed in a model with bulk fermions in interaction with fermions on the brane assuming the presence of a constant abelian gauge field component $A_5$ in the bulk. We calculate the effective potential as a function of the fermion masses and t... | 6.435681 | 5.621422 | 5.55017 | 5.65561 | 6.038134 | 6.298894 | 5.938661 | 5.950745 | 5.515462 | 5.731808 | 5.671842 | 5.86977 | 6.004189 | 5.89597 | 6.011325 | 6.031801 | 5.991151 | 6.045283 | 5.961334 | 5.846271 | 5.915765 |
1505.07353 | Anna Kotanjyan | A. S. Kotanjyan, A. A. Saharian, H. A. Nersisyan | Electromagnetic Casimir effect for conducting plates in de Sitter
spacetime | 14 pages, 1 figure | Phys. Scr. 90 (2015) 065304 | 10.1088/0031-8949/90/6/065304 | null | hep-th astro-ph.CO quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Two-point functions, the mean field squared and the vacuum expectation value
(VEV) of the energy-momentum tensor are investigated for the electromagnetic
field in the geometry of parallel plates on background of $(D+1)$% -dimensional
dS spacetime. We assume that the field is prepared in the Bunch-Davies vacuum
state ... | [
{
"created": "Wed, 27 May 2015 14:45:13 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Kotanjyan",
"A. S.",
""
],
[
"Saharian",
"A. A.",
""
],
[
"Nersisyan",
"H. A.",
""
]
] | Two-point functions, the mean field squared and the vacuum expectation value (VEV) of the energy-momentum tensor are investigated for the electromagnetic field in the geometry of parallel plates on background of $(D+1)$% -dimensional dS spacetime. We assume that the field is prepared in the Bunch-Davies vacuum state an... | 5.502302 | 3.90484 | 5.930592 | 4.276335 | 4.132872 | 4.499409 | 4.143036 | 4.016612 | 4.017058 | 6.015143 | 4.207103 | 4.683106 | 5.378351 | 4.930149 | 4.796167 | 4.745174 | 4.72937 | 4.794388 | 4.831377 | 5.352363 | 4.810093 |
hep-th/0607236 | Matteo Beccaria | Matteo Beccaria, Luigi Del Debbio | Bethe Ansatz solutions for highest states in ${\cal N}=4$ SYM and
AdS/CFT duality | 42 pages, JHEP style LaTeX | JHEP 0609:025,2006 | 10.1088/1126-6708/2006/09/025 | null | hep-th | null | We consider the operators with highest anomalous dimension $\Delta$ in the
compact rank-one sectors $\mathfrak{su}(1|1)$ and $\mathfrak{su}(2)$ of ${\cal
N}=4$ super Yang-Mills. We study the flow of $\Delta$ from weak to strong 't
Hooft coupling $\lambda$ by solving (i) the all-loop gauge Bethe Ansatz, (ii)
the quant... | [
{
"created": "Fri, 28 Jul 2006 11:11:21 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Beccaria",
"Matteo",
""
],
[
"Del Debbio",
"Luigi",
""
]
] | We consider the operators with highest anomalous dimension $\Delta$ in the compact rank-one sectors $\mathfrak{su}(1|1)$ and $\mathfrak{su}(2)$ of ${\cal N}=4$ super Yang-Mills. We study the flow of $\Delta$ from weak to strong 't Hooft coupling $\lambda$ by solving (i) the all-loop gauge Bethe Ansatz, (ii) the quantum... | 6.117506 | 5.888708 | 7.034518 | 5.836674 | 5.667877 | 5.899224 | 5.601334 | 6.050684 | 6.013037 | 7.131916 | 5.55105 | 5.822952 | 6.267323 | 5.673942 | 5.867126 | 5.84797 | 5.799451 | 5.695008 | 5.805069 | 6.531197 | 5.735348 |
2007.01551 | Taegyu Kim | Taegyu Kim and Phillial Oh | A Vanishingly Small Vector Mass from Anisotropy of Higher Dimensional
Spacetime | References are added | null | 10.3938/jkps.77.463 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider five-dimensional massive vector-gravity theory which is based on
the foliation preserving diffeomorphism and anisotropic conformal invariance.
It does not have an intrinsic scale and the only relevant parameter is the
anisotropic factor $z$ which characterizes the degree of anisotropy between the
four-dim... | [
{
"created": "Fri, 3 Jul 2020 08:32:19 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jul 2020 04:56:35 GMT",
"version": "v2"
}
] | 2020-10-28 | [
[
"Kim",
"Taegyu",
""
],
[
"Oh",
"Phillial",
""
]
] | We consider five-dimensional massive vector-gravity theory which is based on the foliation preserving diffeomorphism and anisotropic conformal invariance. It does not have an intrinsic scale and the only relevant parameter is the anisotropic factor $z$ which characterizes the degree of anisotropy between the four-dimen... | 8.294528 | 8.222437 | 8.225521 | 7.690415 | 7.639771 | 8.243023 | 8.435265 | 7.83185 | 8.002075 | 8.420632 | 7.627573 | 7.580936 | 8.158799 | 7.685946 | 7.891939 | 7.773304 | 7.878411 | 7.642502 | 7.613571 | 7.681038 | 7.537984 |
hep-th/9608089 | Guido Cognola | A.A. Bytsenko, Guido Cognola and Sergio Zerbini | Determinant of Laplacian on a non-compact 3-dimensional hyperbolic
manifold with finite volume | 10 pages, LaTex. The contribution of hyperbolic elements has been
added | J.Phys.A30:3543-3552,1997 | 10.1088/0305-4470/30/10/028 | University of Trento, UTF 382 | hep-th | null | The functional determinant of Laplace-type operators on the 3-dimensional
non-compact hyperbolic manifold with invariant fundamental domain of finite
volume is computed by quadratures and making use of the related terms of the
Selberg trace formula.
| [
{
"created": "Wed, 14 Aug 1996 08:09:46 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Oct 1996 15:21:39 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bytsenko",
"A. A.",
""
],
[
"Cognola",
"Guido",
""
],
[
"Zerbini",
"Sergio",
""
]
] | The functional determinant of Laplace-type operators on the 3-dimensional non-compact hyperbolic manifold with invariant fundamental domain of finite volume is computed by quadratures and making use of the related terms of the Selberg trace formula. | 17.809523 | 12.397495 | 16.294867 | 12.038297 | 16.604414 | 17.357244 | 13.120771 | 15.080284 | 12.393207 | 15.168992 | 13.270786 | 14.25596 | 14.925232 | 13.918306 | 15.145112 | 14.300678 | 14.975203 | 14.911734 | 13.57781 | 14.232012 | 14.860952 |
hep-th/9207064 | David Kutasov | David Kutasov | Irreversibility of the Renormalization Group Flow in Two Dimensional
Quantum Gravity | 14 pages, PUPT-1334 | Mod.Phys.Lett. A7 (1992) 2943-2956 | 10.1142/S0217732392002317 | null | hep-th | null | We argue that the torus partition sum in $2d$ (super) gravity, which counts
physical states in the theory, is a decreasing function of the renormalization
group scale. As an application we chart the space of $(\hat c\leq1)$ $c\leq1$
models coupled to (super) gravity, confirming and extending ideas due to A.
Zamolodch... | [
{
"created": "Mon, 20 Jul 1992 14:58:49 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Kutasov",
"David",
""
]
] | We argue that the torus partition sum in $2d$ (super) gravity, which counts physical states in the theory, is a decreasing function of the renormalization group scale. As an application we chart the space of $(\hat c\leq1)$ $c\leq1$ models coupled to (super) gravity, confirming and extending ideas due to A. Zamolodchik... | 12.706135 | 11.072475 | 13.208076 | 10.069295 | 11.163184 | 10.68722 | 11.145177 | 10.65394 | 10.048385 | 14.720062 | 10.233498 | 10.438548 | 12.631516 | 10.754144 | 10.807404 | 10.650334 | 10.023144 | 10.532448 | 10.394815 | 11.78235 | 10.711688 |
hep-th/9909107 | Koushik Ray | Subir Mukhopadhyay and Koushik Ray | D-branes on Fourfolds with Discrete Torsion | Two references added | Nucl.Phys. B576 (2000) 152-176 | 10.1016/S0550-3213(00)00166-8 | ROM2F-99-30, MRI-PHY/P990927 | hep-th | null | We study D1-branes on the fourfold $\C^4/(\Z_2\times\Z_2\times\Z_2)$, in the
presence of discrete torsion. Discrete torsion is incorporated in the gauge
theory of the D1-branes by considering a projective representation of the
finite group $\Z_2\times\Z_2\times\Z_2$. The corresponding orbifold is then
deformed by per... | [
{
"created": "Wed, 15 Sep 1999 16:41:33 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Oct 1999 10:44:46 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Mukhopadhyay",
"Subir",
""
],
[
"Ray",
"Koushik",
""
]
] | We study D1-branes on the fourfold $\C^4/(\Z_2\times\Z_2\times\Z_2)$, in the presence of discrete torsion. Discrete torsion is incorporated in the gauge theory of the D1-branes by considering a projective representation of the finite group $\Z_2\times\Z_2\times\Z_2$. The corresponding orbifold is then deformed by pertu... | 5.068213 | 5.139597 | 6.102127 | 4.89341 | 5.209786 | 4.91187 | 4.966736 | 4.726047 | 4.829784 | 5.907689 | 4.917188 | 5.008296 | 5.320039 | 4.801373 | 4.736168 | 4.898338 | 4.856424 | 4.957396 | 4.940087 | 5.15243 | 4.78487 |
1307.4769 | Andrew Tolley | Nicholas A. Ondo, Andrew J. Tolley | Complete Decoupling Limit of Ghost-free Massive Gravity | 20 pages, typos corrected, references added | null | 10.1007/JHEP11(2013)059 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the complete form of the decoupling limit of ghost-free massive
gravity with a Minkowski reference metric, including the full interactions of
the helicity-1 and helicity-0 modes of the massive spin-2 field. While in the
metric language the square root structure of the mass terms makes it difficult
to find ... | [
{
"created": "Wed, 17 Jul 2013 20:09:14 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Jul 2013 19:58:48 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Ondo",
"Nicholas A.",
""
],
[
"Tolley",
"Andrew J.",
""
]
] | We present the complete form of the decoupling limit of ghost-free massive gravity with a Minkowski reference metric, including the full interactions of the helicity-1 and helicity-0 modes of the massive spin-2 field. While in the metric language the square root structure of the mass terms makes it difficult to find a ... | 6.80434 | 6.337179 | 7.086488 | 6.206916 | 6.691845 | 6.637785 | 6.194044 | 6.093697 | 6.201649 | 7.910398 | 6.219951 | 6.651225 | 6.597618 | 6.13606 | 6.50451 | 6.488316 | 6.444492 | 6.311253 | 6.288334 | 6.669686 | 6.220346 |
1010.2760 | Todd Springer | Todd Springer, Charles Gale, and Sangyong Jeon | Bulk spectral functions in single and multi-scalar gravity duals | 10 pages + appendices, 2 figures. v2: typos fixed and some text
modified in Sec. V; conclusions unchanged. v3: Minor modifications, matches
published version | Phys.Rev.D82:126011,2010 | 10.1103/PhysRevD.82.126011 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine two point correlation functions involving the trace of the energy
momentum tensor in five dimensional gravity dual theories supported by one or
more scalar fields. A prescription for determining bulk channel spectral
functions is developed. This prescription generalizes previous work which
centered on one ... | [
{
"created": "Wed, 13 Oct 2010 20:08:50 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Oct 2010 17:29:01 GMT",
"version": "v2"
},
{
"created": "Wed, 22 Dec 2010 17:54:59 GMT",
"version": "v3"
}
] | 2011-01-20 | [
[
"Springer",
"Todd",
""
],
[
"Gale",
"Charles",
""
],
[
"Jeon",
"Sangyong",
""
]
] | We examine two point correlation functions involving the trace of the energy momentum tensor in five dimensional gravity dual theories supported by one or more scalar fields. A prescription for determining bulk channel spectral functions is developed. This prescription generalizes previous work which centered on one sc... | 10.939857 | 9.288214 | 10.564914 | 9.37287 | 9.730882 | 9.840302 | 9.755748 | 9.55034 | 9.757269 | 9.960225 | 9.426392 | 9.907528 | 10.078085 | 9.789783 | 10.07348 | 9.732274 | 9.877892 | 9.610889 | 9.746928 | 9.909371 | 10.027951 |
1506.05930 | Yi Yang | Yi Yang and Pei-Hung Yuan | Confinement-Deconfinment Phase Transition for Heavy Quarks | 23 pages, 14 figures, published in JHEP. arXiv admin note: text
overlap with arXiv:1301.0385 | Journal of High Energy Physics, 2015(12), 1-22 | 10.1007/JHEP12(2015)161 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study confinement-deconfinement phase transition for heavy quarks in a
bottom-up holographic QCD model. We consider a black hole background in an
Einstein-Maxwell-scalar system and add probe open strings to the background.
Combining the various configurations of the open strings and the phase
structure of the blac... | [
{
"created": "Fri, 19 Jun 2015 09:30:27 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Jan 2016 01:55:17 GMT",
"version": "v2"
}
] | 2016-01-11 | [
[
"Yang",
"Yi",
""
],
[
"Yuan",
"Pei-Hung",
""
]
] | We study confinement-deconfinement phase transition for heavy quarks in a bottom-up holographic QCD model. We consider a black hole background in an Einstein-Maxwell-scalar system and add probe open strings to the background. Combining the various configurations of the open strings and the phase structure of the black ... | 5.892466 | 5.189425 | 5.340316 | 4.785492 | 5.065964 | 5.082469 | 4.498674 | 5.051574 | 5.09044 | 5.374765 | 5.046589 | 5.090233 | 5.185363 | 5.103812 | 4.909459 | 5.094313 | 5.006843 | 5.144967 | 5.041499 | 5.139036 | 5.047827 |
hep-th/0204195 | Adam Falkowski | Philippe Brax, Adam Falkowski, Zygmunt Lalak and Stefan Pokorski | Custodial supersymmetry in non-supersymmetric quiver theories | 10 pages, latex, references added, discussion of custodial susy in
the zero-mode sector extended | Phys.Lett. B538 (2002) 426-434 | 10.1016/S0370-2693(02)02006-3 | null | hep-th | null | We consider non-supersymmetric quiver theories obtained by orbifolding the
N=4 supersymmetric U(K) gauge theory by a discrete Z_\Gamma group embedded in
the SU(4) R-symmetry group. We explicitly find that in such theories there are
no one-loop quadratic divergences in the effective potential.
Moreover, when the gau... | [
{
"created": "Tue, 23 Apr 2002 16:21:53 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 2002 14:27:00 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Brax",
"Philippe",
""
],
[
"Falkowski",
"Adam",
""
],
[
"Lalak",
"Zygmunt",
""
],
[
"Pokorski",
"Stefan",
""
]
] | We consider non-supersymmetric quiver theories obtained by orbifolding the N=4 supersymmetric U(K) gauge theory by a discrete Z_\Gamma group embedded in the SU(4) R-symmetry group. We explicitly find that in such theories there are no one-loop quadratic divergences in the effective potential. Moreover, when the gauge g... | 7.438075 | 6.131687 | 7.881171 | 7.227631 | 6.621666 | 6.81346 | 7.134349 | 7.398145 | 6.629465 | 8.653423 | 6.704918 | 7.054588 | 7.449806 | 7.102115 | 6.955773 | 7.176752 | 6.7949 | 6.842027 | 7.2112 | 7.487512 | 6.75002 |
1204.3043 | Philipp Fleig | Philipp Fleig, Axel Kleinschmidt | Eisenstein series for infinite-dimensional U-duality groups | 69 pages. v2: Added references and small additions, to be published
in JHEP | null | 10.1007/JHEP06(2012)054 | AEI-2012-035 | hep-th math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Eisenstein series appearing as coefficients of curvature
corrections in the low-energy expansion of type II string theory four-graviton
scattering amplitudes. We define these Eisenstein series over all groups in the
E_n series of string duality groups, and in particular for the
infinite-dimensional Kac-Mo... | [
{
"created": "Fri, 13 Apr 2012 16:35:53 GMT",
"version": "v1"
},
{
"created": "Tue, 29 May 2012 16:14:47 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Fleig",
"Philipp",
""
],
[
"Kleinschmidt",
"Axel",
""
]
] | We consider Eisenstein series appearing as coefficients of curvature corrections in the low-energy expansion of type II string theory four-graviton scattering amplitudes. We define these Eisenstein series over all groups in the E_n series of string duality groups, and in particular for the infinite-dimensional Kac-Mood... | 7.962454 | 8.455226 | 10.19652 | 8.447232 | 8.273645 | 8.631635 | 8.442175 | 8.194416 | 8.519717 | 10.173197 | 7.92809 | 7.770263 | 9.067252 | 8.105165 | 7.997304 | 8.045045 | 7.889823 | 7.876493 | 8.09205 | 8.757875 | 7.861087 |
0707.0388 | Ingo Runkel | Matthias R. Gaberdiel, Ingo Runkel | From boundary to bulk in logarithmic CFT | 35 pages, 2 figures; v2: minor corrections, version to appear in
J.Phys.A | J. Phys. A41 (2008) 075402 | 10.1088/1751-8113/41/7/075402 | null | hep-th math.QA | null | The analogue of the charge-conjugation modular invariant for rational
logarithmic conformal field theories is constructed. This is done by
reconstructing the bulk spectrum from a simple boundary condition (the analogue
of the Cardy `identity brane'). We apply the general method to the c_1,p
triplet models and reprodu... | [
{
"created": "Tue, 3 Jul 2007 10:45:44 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Jan 2008 11:51:32 GMT",
"version": "v2"
}
] | 2008-05-01 | [
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Runkel",
"Ingo",
""
]
] | The analogue of the charge-conjugation modular invariant for rational logarithmic conformal field theories is constructed. This is done by reconstructing the bulk spectrum from a simple boundary condition (the analogue of the Cardy `identity brane'). We apply the general method to the c_1,p triplet models and reproduce... | 10.896456 | 9.192794 | 15.392612 | 10.481832 | 10.880072 | 10.127604 | 9.578829 | 9.61501 | 10.116755 | 16.238342 | 9.568977 | 10.564694 | 12.662183 | 10.182323 | 10.789514 | 10.476402 | 9.998234 | 10.316925 | 10.399501 | 11.925671 | 10.376601 |
1108.3555 | Osvaldo Chandia | Osvaldo Chandia, William D. Linch III, and Brenno Carlini Vallilo | Compactification of the Heterotic Pure Spinor Superstring II | Title changed. Added one reference | null | 10.1007/JHEP10(2011)098 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study compactifications of the heterotic pure spinor superstring to six
and four dimensions focusing on two simple Calabi-Yau orbifolds. We show that
the correct spectrum can be reproduced only if, in the twisted sector, there
remain exactly 5 and 2 pure spinor components untwisted, respectively. This
naturally de... | [
{
"created": "Wed, 17 Aug 2011 19:23:21 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Sep 2011 16:53:20 GMT",
"version": "v2"
}
] | 2015-05-30 | [
[
"Chandia",
"Osvaldo",
""
],
[
"Linch",
"William D.",
"III"
],
[
"Vallilo",
"Brenno Carlini",
""
]
] | We study compactifications of the heterotic pure spinor superstring to six and four dimensions focusing on two simple Calabi-Yau orbifolds. We show that the correct spectrum can be reproduced only if, in the twisted sector, there remain exactly 5 and 2 pure spinor components untwisted, respectively. This naturally defi... | 9.994637 | 10.34391 | 11.676842 | 8.876296 | 10.025824 | 9.909835 | 9.790125 | 9.075775 | 9.857685 | 10.234828 | 9.087548 | 9.225699 | 9.476349 | 9.047072 | 8.936128 | 9.137788 | 8.99212 | 9.029449 | 9.169333 | 9.58802 | 8.984488 |
2112.03976 | Rafael A. Porto | Gihyuk Cho, Gregor K\"alin and Rafael A. Porto | From Boundary Data to Bound States III: Radiative Effects | 43 pages. 3 Figures. 1 ancillary file. v2: Paper and ancillary file
updated to correct an error (using by mistake non-canonical variables) in the
derivation of the spin-dependent radiated energy/angular-momentum in Eqs.
5.18, 5.20, 5.21 and 5.23. The B2B map remains unaltered. Published version | null | 10.1007/JHEP04(2022)154 | DESY 21-212 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We extend the "boundary-to-bound" (B2B) correspondence to incorporate
radiative as well as conservative radiation-reaction effects. We start by
deriving a map between the total change in observables due to gravitational
wave emission during hyperbolic-like motion and in one period of an
elliptic-like orbit, which is ... | [
{
"created": "Tue, 7 Dec 2021 20:37:21 GMT",
"version": "v1"
},
{
"created": "Fri, 27 May 2022 14:19:44 GMT",
"version": "v2"
}
] | 2022-05-30 | [
[
"Cho",
"Gihyuk",
""
],
[
"Kälin",
"Gregor",
""
],
[
"Porto",
"Rafael A.",
""
]
] | We extend the "boundary-to-bound" (B2B) correspondence to incorporate radiative as well as conservative radiation-reaction effects. We start by deriving a map between the total change in observables due to gravitational wave emission during hyperbolic-like motion and in one period of an elliptic-like orbit, which is va... | 13.532201 | 13.20391 | 12.604608 | 11.545921 | 12.904545 | 12.504004 | 12.998413 | 11.663847 | 12.355715 | 14.267685 | 11.70527 | 12.466454 | 12.861813 | 12.292198 | 12.320741 | 12.596706 | 12.27744 | 12.070117 | 12.267896 | 12.578481 | 12.493931 |
1806.01115 | Urs Schreiber | Vincent Braunack-Mayer, Hisham Sati, Urs Schreiber | Gauge enhancement of super M-branes via parametrized stable homotopy
theory | 57 pages, various figures, v2: minor corrections, v3: published
version | Communications in Mathematical Physics 2019 | 10.1007/s00220-019-03441-4 | null | hep-th math-ph math.AT math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A key open problem in M-theory is the mechanism of "gauge enhancement", which
supposedly makes M-branes exhibit the nonabelian gauge degrees of freedom that
are seen perturbatively in the limit of 10d string theory. In fact, since only
the twisted K-theory classes represented by nonabelian Chan-Paton gauge fields
on ... | [
{
"created": "Mon, 4 Jun 2018 13:50:31 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Jul 2018 14:13:28 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Mar 2019 10:41:23 GMT",
"version": "v3"
}
] | 2019-05-24 | [
[
"Braunack-Mayer",
"Vincent",
""
],
[
"Sati",
"Hisham",
""
],
[
"Schreiber",
"Urs",
""
]
] | A key open problem in M-theory is the mechanism of "gauge enhancement", which supposedly makes M-branes exhibit the nonabelian gauge degrees of freedom that are seen perturbatively in the limit of 10d string theory. In fact, since only the twisted K-theory classes represented by nonabelian Chan-Paton gauge fields on D-... | 9.223176 | 11.558827 | 12.609002 | 10.032165 | 11.563205 | 11.229273 | 11.266015 | 10.470432 | 9.849308 | 12.994353 | 9.989801 | 9.299964 | 10.224154 | 9.449967 | 9.679583 | 9.326206 | 9.363762 | 9.292138 | 9.480853 | 10.204505 | 9.150302 |
hep-th/0404006 | Oleg Lunin | Oleg Lunin | Adding momentum to D1-D5 system | 28 pages, LATEX, references added, typo fixed | JHEP0404:054,2004 | 10.1088/1126-6708/2004/04/054 | null | hep-th | null | We construct the first example of asymptotically flat solution which carries
three charges (D1,D5 and momentum) and which is completely regular everywhere.
The construction utilizes the relation between gravity solutions and spectral
flow in the dual CFT. We show that the solution has the right properties to
describe... | [
{
"created": "Thu, 1 Apr 2004 19:41:29 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Apr 2004 01:42:21 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Apr 2004 23:33:19 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Lunin",
"Oleg",
""
]
] | We construct the first example of asymptotically flat solution which carries three charges (D1,D5 and momentum) and which is completely regular everywhere. The construction utilizes the relation between gravity solutions and spectral flow in the dual CFT. We show that the solution has the right properties to describe o... | 10.763368 | 8.185178 | 10.735407 | 7.983851 | 9.151596 | 8.507001 | 8.440473 | 7.685924 | 7.834234 | 10.053286 | 8.13262 | 8.226245 | 10.051363 | 8.565449 | 8.786947 | 9.125215 | 8.141168 | 8.742188 | 8.666383 | 9.609097 | 8.54759 |
2401.07707 | Horatiu Stefan Nastase | Horatiu Nastase and Jacob Sonnenschein | Novel knotted non-abelian gauge fields | 33 pages, 1 figure; references added; summary of main points added in
Introduction | null | null | null | hep-th hep-lat hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In analogy to null electromagnetic fields we define null YM fields. We show
that the null non-abelian $SU(N)$ gauge fields admit a set of $2 N^2$ conserved
"helicities". We derive null YM solutions that carry finite helicities by
uplifting the abelian Hopfion solution and their generalizations. Another
method that we... | [
{
"created": "Mon, 15 Jan 2024 14:23:10 GMT",
"version": "v1"
},
{
"created": "Mon, 6 May 2024 17:06:24 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Aug 2024 18:13:10 GMT",
"version": "v3"
}
] | 2024-08-13 | [
[
"Nastase",
"Horatiu",
""
],
[
"Sonnenschein",
"Jacob",
""
]
] | In analogy to null electromagnetic fields we define null YM fields. We show that the null non-abelian $SU(N)$ gauge fields admit a set of $2 N^2$ conserved "helicities". We derive null YM solutions that carry finite helicities by uplifting the abelian Hopfion solution and their generalizations. Another method that we i... | 11.518089 | 12.127094 | 11.869407 | 11.036676 | 11.577056 | 12.989704 | 11.615555 | 10.966041 | 11.760094 | 13.354923 | 11.45563 | 10.988457 | 10.75936 | 10.791129 | 10.436206 | 10.902832 | 10.486044 | 11.44481 | 10.804283 | 10.857688 | 10.43042 |
2203.07914 | Xian-Hui Ge | Qing-Bing Wang, Ming-Hui Yu and Xian-Hui Ge | Scrambling time for analogue black holes embedded in AdS space | 1+18 pages, 3 figures, published version | Eur. Phys. J. C 82 (2022) 468 | 10.1140/epjc/s10052-022-10438-2 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We propose a gedanken experiment on realizing thermofield double state (TFD)
by using analog black holes and provide an approach to test the scrambling
time. Through this approach, we demonstrate clearly how shock wave changes the
TFD state as time evolves. As the whole system evolves forward in time, the
perturbatio... | [
{
"created": "Tue, 15 Mar 2022 13:54:27 GMT",
"version": "v1"
},
{
"created": "Sat, 30 Apr 2022 16:00:03 GMT",
"version": "v2"
},
{
"created": "Tue, 24 May 2022 13:46:44 GMT",
"version": "v3"
}
] | 2022-05-25 | [
[
"Wang",
"Qing-Bing",
""
],
[
"Yu",
"Ming-Hui",
""
],
[
"Ge",
"Xian-Hui",
""
]
] | We propose a gedanken experiment on realizing thermofield double state (TFD) by using analog black holes and provide an approach to test the scrambling time. Through this approach, we demonstrate clearly how shock wave changes the TFD state as time evolves. As the whole system evolves forward in time, the perturbation ... | 12.886097 | 11.91519 | 12.66115 | 11.359154 | 12.422779 | 12.605966 | 12.748574 | 11.303102 | 11.216104 | 13.877761 | 11.611787 | 12.063148 | 12.108148 | 11.720721 | 11.644836 | 11.8848 | 11.745668 | 11.703835 | 11.258359 | 12.277633 | 11.581829 |
2204.04927 | Hosein Mohammadzadeh | H. Babaei-Aghbolagh, Hosein Mohammadzadeh, Davood Mahdavian Yekta and
Komeil Babaei Velni | Thermodynamic geometry and complexity of black holes in theories with
broken translational invariance | 14 pages, 10 figures | null | 10.1103/PhysRevD.106.024044 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The relationship between thermodynamics and the Lloyd bound on the
holographic complexity for a black hole has been of interest. We consider $D$
dimensional anti-de Sitter black holes with hyperbolic geometry as well as
black holes with momentum relaxation that have a minimum for temperature and
mass. We show that th... | [
{
"created": "Mon, 11 Apr 2022 07:56:57 GMT",
"version": "v1"
}
] | 2022-08-03 | [
[
"Babaei-Aghbolagh",
"H.",
""
],
[
"Mohammadzadeh",
"Hosein",
""
],
[
"Yekta",
"Davood Mahdavian",
""
],
[
"Velni",
"Komeil Babaei",
""
]
] | The relationship between thermodynamics and the Lloyd bound on the holographic complexity for a black hole has been of interest. We consider $D$ dimensional anti-de Sitter black holes with hyperbolic geometry as well as black holes with momentum relaxation that have a minimum for temperature and mass. We show that the ... | 11.022116 | 9.965609 | 10.968059 | 9.914634 | 10.90743 | 10.081505 | 10.320549 | 10.234601 | 9.671114 | 11.686121 | 10.186752 | 9.987074 | 10.523582 | 10.243309 | 10.127772 | 10.790728 | 10.401026 | 10.393487 | 10.12958 | 10.654563 | 10.096866 |
2107.07035 | Hugo Garcia-Compean | H. Garc\'ia-Compe\'an, D. Mata-Pacheco | Lorentzian Vacuum Transitions for Anisotropic Universes | 33 pages, 2 figures, sec. 3 was imporved, typos corrected, references
added | null | 10.1103/PhysRevD.104.106014 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The vacuum transition probabilities for anisotropic universes in the presence
of a scalar field potential in the Wentzel-Kramers-Brillouin approximation are
studied. We follow the work by Cespedes et al [Phys. Rev. D 104, 026013
(2021)], which discuss these transitions in the isotropic context using the
Wheeler-DeWit... | [
{
"created": "Wed, 14 Jul 2021 23:16:19 GMT",
"version": "v1"
},
{
"created": "Sat, 16 Oct 2021 07:03:18 GMT",
"version": "v2"
}
] | 2021-12-01 | [
[
"García-Compeán",
"H.",
""
],
[
"Mata-Pacheco",
"D.",
""
]
] | The vacuum transition probabilities for anisotropic universes in the presence of a scalar field potential in the Wentzel-Kramers-Brillouin approximation are studied. We follow the work by Cespedes et al [Phys. Rev. D 104, 026013 (2021)], which discuss these transitions in the isotropic context using the Wheeler-DeWitt ... | 8.903902 | 9.968795 | 8.612001 | 8.652633 | 9.008382 | 9.502431 | 9.577244 | 9.239252 | 8.955135 | 9.586369 | 8.622126 | 8.648201 | 8.659156 | 8.64484 | 8.722359 | 8.606205 | 8.596987 | 8.492584 | 8.701532 | 8.690046 | 8.735933 |
hep-th/9706031 | Cezary Juszczak | Giovanni Amelino-Camelia, Jerzy Lukierski, and Anatol Nowicki | kappa-Deformed Covariant Phase Space and Quantum-Gravity Uncertainty
Relations | 9 pages, LaTeX | Phys.Atom.Nucl.61:1811-1815,1998; Yad.Fiz.61:1925-1929,1998 | null | OUTP-97-24P | hep-th gr-qc math.QA q-alg | null | We describe the deformed covariant phase space corresponding to the so-called
kappa-deformation of D=4 relativistic symmetries, with quantum ``time''
coordinate and Heisenberg algebra obtained according to the Heisenberg double
construction. The associated modified uncertainty relations are analyzed, and
in particula... | [
{
"created": "Wed, 4 Jun 1997 14:39:11 GMT",
"version": "v1"
}
] | 2011-04-15 | [
[
"Amelino-Camelia",
"Giovanni",
""
],
[
"Lukierski",
"Jerzy",
""
],
[
"Nowicki",
"Anatol",
""
]
] | We describe the deformed covariant phase space corresponding to the so-called kappa-deformation of D=4 relativistic symmetries, with quantum ``time'' coordinate and Heisenberg algebra obtained according to the Heisenberg double construction. The associated modified uncertainty relations are analyzed, and in particular ... | 12.039045 | 11.293143 | 11.435729 | 9.664589 | 10.397478 | 10.683083 | 10.342704 | 10.798614 | 10.772497 | 12.509989 | 10.913138 | 10.70021 | 11.706927 | 11.086235 | 11.069719 | 10.87124 | 10.782406 | 10.490917 | 11.28002 | 12.419358 | 11.001354 |
hep-th/0508021 | Nobuyuki Motoyui | Nobuyuki Motoyui and Mitsuru Yamada | Operator ordering and Classical soliton path in Two-dimensional N=2
supersymmetry with Kahler potential | 13 pages, typos corrected | Int.J.Mod.Phys. A21 (2006) 109-120 | 10.1142/S0217751X06025018 | IU-MSTP/72 | hep-th | null | We investigate a 2-dimensional N=2 supersymmetric model which consists of n
chiral superfields with Kahler potential. When we define quantum observables,
we are always plagued by operator ordering problem. Among various ways to fix
the operator order, we rely upon the supersymmetry. We demonstrate that the
correct op... | [
{
"created": "Wed, 3 Aug 2005 02:45:36 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Oct 2005 07:17:59 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Motoyui",
"Nobuyuki",
""
],
[
"Yamada",
"Mitsuru",
""
]
] | We investigate a 2-dimensional N=2 supersymmetric model which consists of n chiral superfields with Kahler potential. When we define quantum observables, we are always plagued by operator ordering problem. Among various ways to fix the operator order, we rely upon the supersymmetry. We demonstrate that the correct oper... | 12.731246 | 13.031241 | 14.124105 | 13.394693 | 14.717164 | 14.187878 | 14.118002 | 12.946838 | 13.612057 | 15.603123 | 12.685102 | 13.120087 | 12.754081 | 12.306755 | 13.009713 | 13.167493 | 13.003769 | 12.579767 | 12.765936 | 13.05246 | 12.53767 |
1103.3348 | Giampiero Esposito Dr. | Paolo Aschieri, Elisabetta Di Grezia, Giampiero Esposito | Non-commutative Einstein equations and Seiberg-Witten map | 6 and 1/2 pages, based on talk prepared for the Friedmann Seminar,
May-June 2011. In the final version, the presentation has been improved,
including a better notation | null | 10.1142/S2010194511001231 | DSF preprint 2011/3 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Seiberg--Witten map is a powerful tool in non-commutative field theory,
and it has been recently obtained in the literature for gravity itself, to
first order in non-commutativity. This paper, relying upon the pure-gravity
form of the action functional considered in Ref. 2, studies the expansion to
first order of... | [
{
"created": "Thu, 17 Mar 2011 07:18:25 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Jun 2011 10:03:14 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Aschieri",
"Paolo",
""
],
[
"Di Grezia",
"Elisabetta",
""
],
[
"Esposito",
"Giampiero",
""
]
] | The Seiberg--Witten map is a powerful tool in non-commutative field theory, and it has been recently obtained in the literature for gravity itself, to first order in non-commutativity. This paper, relying upon the pure-gravity form of the action functional considered in Ref. 2, studies the expansion to first order of t... | 11.444302 | 10.390928 | 9.822926 | 9.149981 | 10.154455 | 9.975328 | 9.639106 | 9.642985 | 9.417875 | 10.620879 | 9.288524 | 9.260414 | 9.649384 | 9.362523 | 9.486933 | 9.515793 | 9.643821 | 9.689426 | 9.642959 | 9.475732 | 9.561541 |
1502.07737 | Arash Arabi Ardehali | Arash Arabi Ardehali, James T. Liu, Phillip Szepietowski | High-Temperature Expansion of Supersymmetric Partition Functions | 15 pages plus appendices; v2: minor modifications and a "Note added";
v3: presentation improved and minor errors in app B corrected | JHEP 1507 (2015) 113 | 10.1007/JHEP07(2015)113 | MCTP-15-06, ITP-UU-15/03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Di Pietro and Komargodski have recently demonstrated a four-dimensional
counterpart of Cardy's formula, which gives the leading high-temperature
($\beta\rightarrow{0}$) behavior of supersymmetric partition functions
$Z^{SUSY}(\beta)$. Focusing on superconformal theories, we elaborate on the
subleading contributions t... | [
{
"created": "Thu, 26 Feb 2015 20:56:45 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Mar 2015 23:32:35 GMT",
"version": "v2"
},
{
"created": "Tue, 7 Jul 2015 00:39:54 GMT",
"version": "v3"
}
] | 2015-11-13 | [
[
"Ardehali",
"Arash Arabi",
""
],
[
"Liu",
"James T.",
""
],
[
"Szepietowski",
"Phillip",
""
]
] | Di Pietro and Komargodski have recently demonstrated a four-dimensional counterpart of Cardy's formula, which gives the leading high-temperature ($\beta\rightarrow{0}$) behavior of supersymmetric partition functions $Z^{SUSY}(\beta)$. Focusing on superconformal theories, we elaborate on the subleading contributions to ... | 7.123923 | 6.686494 | 7.354135 | 6.707152 | 6.632353 | 6.814691 | 6.561159 | 6.639384 | 6.716771 | 8.250199 | 7.033149 | 6.407391 | 6.842666 | 6.508787 | 6.420206 | 6.314167 | 6.457908 | 6.273732 | 6.507417 | 6.613479 | 6.905545 |
hep-th/9502109 | Emil Mottola | Emil Mottola | Functional Integration Over Geometries | 68 pages, Latex document using Revtex Macro package, Contribution to
the special issue of the Journal of Mathematical Physics on Functional
Integration, to be published July, 1995. | J.Math.Phys. 36 (1995) 2470-2511 | 10.1063/1.531359 | LA-UR-95-80 | hep-th gr-qc | null | The geometric construction of the functional integral over coset spaces
${\cal M}/{\cal G}$ is reviewed. The inner product on the cotangent space of
infinitesimal deformations of $\cal M$ defines an invariant distance and volume
form, or functional integration measure on the full configuration space. Then,
by a simpl... | [
{
"created": "Fri, 17 Feb 1995 01:05:30 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Mottola",
"Emil",
""
]
] | The geometric construction of the functional integral over coset spaces ${\cal M}/{\cal G}$ is reviewed. The inner product on the cotangent space of infinitesimal deformations of $\cal M$ defines an invariant distance and volume form, or functional integration measure on the full configuration space. Then, by a simple ... | 7.183977 | 8.324305 | 8.093905 | 7.714474 | 8.198834 | 7.903045 | 8.149654 | 7.901647 | 7.950847 | 8.579534 | 7.67869 | 7.440255 | 7.262819 | 7.307772 | 7.490756 | 7.297587 | 7.52498 | 7.269989 | 7.228637 | 7.582154 | 7.420056 |
1108.3557 | Gregory Korchemsky | Burkhard Eden, Paul Heslop, Gregory P. Korchemsky and Emery Sokatchev | Hidden symmetry of four-point correlation functions and amplitudes in
N=4 SYM | 46 pages, 10 figures; v2: minor typos corrected | null | 10.1016/j.nuclphysb.2012.04.007 | CERN-PH-TH/2011-208; DCPT-11/33; IPhT-T11/91; LAPTH-030/11 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the four-point correlation function of stress-tensor supermultiplets
in N=4 SYM using the method of Lagrangian insertions. We argue that, as a
corollary of N=4 superconformal symmetry, the resulting all-loop integrand
possesses an unexpected complete symmetry under the exchange of the four
external and all t... | [
{
"created": "Wed, 17 Aug 2011 19:39:59 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Apr 2012 22:43:05 GMT",
"version": "v2"
},
{
"created": "Wed, 9 May 2012 06:57:10 GMT",
"version": "v3"
}
] | 2015-05-30 | [
[
"Eden",
"Burkhard",
""
],
[
"Heslop",
"Paul",
""
],
[
"Korchemsky",
"Gregory P.",
""
],
[
"Sokatchev",
"Emery",
""
]
] | We study the four-point correlation function of stress-tensor supermultiplets in N=4 SYM using the method of Lagrangian insertions. We argue that, as a corollary of N=4 superconformal symmetry, the resulting all-loop integrand possesses an unexpected complete symmetry under the exchange of the four external and all the... | 4.33754 | 5.070009 | 6.017495 | 5.0193 | 4.972884 | 4.997087 | 5.140759 | 4.936629 | 5.12457 | 5.856774 | 4.931097 | 4.732886 | 5.220801 | 4.747774 | 4.73929 | 4.682139 | 4.809237 | 4.835814 | 4.806218 | 5.20594 | 4.785436 |
1902.02578 | Shuichi Yokoyama | Sinya Aoki, Shuichi Yokoyama, and Kentaroh Yoshida | Holographic geometry for non-relativistic systems emerging from
generalized flow equations | 32 pages, no figure, v2: the definition of the metric operator
changed, typos fixed, comments and references added, published version | Phys. Rev. D 99, 126002 (2019) | 10.1103/PhysRevD.99.126002 | YITP-19-04, KUNS-2747 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An intriguing result presented by two of the present authors is that an anti
de Sitter space can be derived from a conformal field theory by considering a
flow equation. A natural expectation is that given a certain data on the
boundary system, the associated geometry would be able to emerge from a flow,
even beyond ... | [
{
"created": "Thu, 7 Feb 2019 11:51:53 GMT",
"version": "v1"
},
{
"created": "Thu, 23 May 2019 13:05:38 GMT",
"version": "v2"
}
] | 2019-06-12 | [
[
"Aoki",
"Sinya",
""
],
[
"Yokoyama",
"Shuichi",
""
],
[
"Yoshida",
"Kentaroh",
""
]
] | An intriguing result presented by two of the present authors is that an anti de Sitter space can be derived from a conformal field theory by considering a flow equation. A natural expectation is that given a certain data on the boundary system, the associated geometry would be able to emerge from a flow, even beyond th... | 12.431854 | 11.604344 | 12.562682 | 10.649296 | 11.56967 | 10.568993 | 11.490924 | 11.15128 | 10.642019 | 13.132332 | 11.003143 | 10.486756 | 11.096183 | 10.642682 | 10.625604 | 10.517311 | 10.846723 | 10.783789 | 10.676065 | 11.539765 | 10.707392 |
hep-th/9211056 | Jerome Gauntlett | Jerome P. Gauntlett, Jeffrey A. Harvey and James T. Liu | Magnetic Monopoles in String Theory | 24 pages (Corrected title) | Nucl.Phys.B409:363-381,1993 | 10.1016/0550-3213(93)90584-C | EFI-92-67, IFP-434-UNC | hep-th | null | Magnetic monopole solutions to heterotic string theory are discussed in
toroidal compactifications to four spacetime dimensions. Particular emphasis is
placed on the relation to previously studied fivebrane solutions in ten
dimensions and on the possibility of constructing exact monopole solutions
related to symmetri... | [
{
"created": "Thu, 12 Nov 1992 19:14:48 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Nov 1992 14:39:21 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Gauntlett",
"Jerome P.",
""
],
[
"Harvey",
"Jeffrey A.",
""
],
[
"Liu",
"James T.",
""
]
] | Magnetic monopole solutions to heterotic string theory are discussed in toroidal compactifications to four spacetime dimensions. Particular emphasis is placed on the relation to previously studied fivebrane solutions in ten dimensions and on the possibility of constructing exact monopole solutions related to symmetric ... | 9.680901 | 7.264633 | 9.071293 | 7.643514 | 7.711961 | 7.288851 | 7.023335 | 7.245368 | 7.721374 | 9.104405 | 7.341658 | 7.464396 | 8.381158 | 7.681762 | 7.114614 | 7.236861 | 7.255962 | 7.286922 | 7.589434 | 8.286262 | 7.247942 |
1012.1818 | Murat Gunaydin | M. Gunaydin, H. Samtleben and E. Sezgin | On the Magical Supergravities in Six Dimensions | 42 pages, Latex file; References added, typos corrected, minor
clarifications in the introduction and conclusion sections added. Version to
be published in Nuclear Physics B | Nucl.Phys.B848:62-89,2011 | 10.1016/j.nuclphysb.2011.02.010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Magical supergravities are a very special class of supergravity theories
whose symmetries and matter content in various dimensions correspond to
symmetries and underlying algebraic structures of the remarkable geometries of
the Magic Square of Freudenthal, Rozenfeld and Tits. These symmetry groups
include the excepti... | [
{
"created": "Wed, 8 Dec 2010 17:57:42 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Dec 2010 00:54:12 GMT",
"version": "v2"
},
{
"created": "Mon, 21 Feb 2011 15:58:41 GMT",
"version": "v3"
}
] | 2011-04-04 | [
[
"Gunaydin",
"M.",
""
],
[
"Samtleben",
"H.",
""
],
[
"Sezgin",
"E.",
""
]
] | Magical supergravities are a very special class of supergravity theories whose symmetries and matter content in various dimensions correspond to symmetries and underlying algebraic structures of the remarkable geometries of the Magic Square of Freudenthal, Rozenfeld and Tits. These symmetry groups include the exception... | 9.816459 | 9.498995 | 11.488332 | 10.339533 | 10.735384 | 11.120289 | 10.604837 | 9.56201 | 9.625086 | 11.67947 | 9.678842 | 8.763939 | 9.101223 | 8.964082 | 8.985353 | 8.997148 | 8.899418 | 9.025089 | 9.494308 | 9.149935 | 9.247946 |
hep-th/0010192 | Michael Gutperle | Michael Gutperle (Harvard University) and Michal Spalinski (Harvard
University) | Supergravity Instantons for N=2 Hypermultiplets | 29 pages, harvmac(b), no figures, v4: typos corrected, version to
appear in NPB | Nucl.Phys. B598 (2001) 509-529 | 10.1016/S0550-3213(00)00756-2 | HUTP-00/A043 | hep-th | null | The dimensional reduction of eleven dimensional supergravity on a Calabi-Yau
manifold gives N=2 supergravity in five dimensions with $h_{1,1}$ vector and
$h_{2,1}+1$ hypermultiplets. In this paper instanton solutions are constructed
which are responsible for nonperturbtative corrections to the hypermultiplet
moduli s... | [
{
"created": "Mon, 23 Oct 2000 22:12:20 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Nov 2000 22:31:06 GMT",
"version": "v2"
},
{
"created": "Fri, 17 Nov 2000 21:23:52 GMT",
"version": "v3"
},
{
"created": "Sat, 17 Feb 2001 20:38:31 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Gutperle",
"Michael",
"",
"Harvard University"
],
[
"Spalinski",
"Michal",
"",
"Harvard\n University"
]
] | The dimensional reduction of eleven dimensional supergravity on a Calabi-Yau manifold gives N=2 supergravity in five dimensions with $h_{1,1}$ vector and $h_{2,1}+1$ hypermultiplets. In this paper instanton solutions are constructed which are responsible for nonperturbtative corrections to the hypermultiplet moduli spa... | 6.519009 | 5.769798 | 7.483973 | 5.461161 | 6.031644 | 5.5279 | 5.796136 | 5.550191 | 5.445825 | 8.077456 | 5.715025 | 5.905454 | 6.310083 | 5.980809 | 6.108672 | 5.814239 | 5.68119 | 5.947094 | 6.155098 | 6.440591 | 5.926232 |
hep-th/9906140 | Maslowski Tomasz | Tomasz Mas{\l}owski and Stanis{\l}aw D. G{\l}azek | This manuscript (hep-th/9906140v1) is incomplete | Please read instead S. D. G{\l}azek, T. Mas{\l}owski, Renormalized
Poincar\'e algebra for effective particles in quantum field theory, Phys.Rev.
D65 (2002) 065011, (hep-th/0110185) | null | null | null | hep-th | null | This manuscript (hep-th/9906140v1) is incomplete. Please read instead S. D.
G{\l}azek, T. Mas{\l}owski, Renormalized Poincar\'e algebra for effective
particles in quantum field theory, Phys.Rev. D65 (2002) 065011,
(hep-th/0110185).
| [
{
"created": "Fri, 18 Jun 1999 08:27:22 GMT",
"version": "v1"
},
{
"created": "Sun, 1 Jul 2007 12:23:56 GMT",
"version": "v2"
}
] | 2007-07-01 | [
[
"Masłowski",
"Tomasz",
""
],
[
"Głazek",
"Stanisław D.",
""
]
] | This manuscript (hep-th/9906140v1) is incomplete. Please read instead S. D. G{\l}azek, T. Mas{\l}owski, Renormalized Poincar\'e algebra for effective particles in quantum field theory, Phys.Rev. D65 (2002) 065011, (hep-th/0110185). | 13.624521 | 10.956601 | 15.757811 | 10.880931 | 12.666968 | 10.98377 | 12.198189 | 12.065347 | 10.769377 | 12.530427 | 11.13952 | 11.248816 | 11.182902 | 11.422954 | 11.363337 | 11.3464 | 11.072111 | 11.395877 | 10.771491 | 10.933134 | 10.817512 |
1110.1636 | Ahmad Borzou | Ahmad Borzou, Kai Lin, and Anzhong Wang | Static electromagnetic fields and charged black holes in general
covariant theory of Horava-Lifshitz gravity | 8 pages, To appear in JCAP | JCAP 02 (2012) 025 | 10.1088/1475-7516/2012/02/025 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study electromeganetic static spacetimes in the
nonrelativisitc general covariant theory of the Horava-Lifshitz (HL) gravity,
proposed recently by Horava and Melby-Thompson, and present all the electric
static solutions, which represent the generalization of the Reissner-Nordstrom
solution found in ... | [
{
"created": "Fri, 7 Oct 2011 20:00:33 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Jan 2012 17:20:20 GMT",
"version": "v2"
}
] | 2012-04-02 | [
[
"Borzou",
"Ahmad",
""
],
[
"Lin",
"Kai",
""
],
[
"Wang",
"Anzhong",
""
]
] | In this paper, we study electromeganetic static spacetimes in the nonrelativisitc general covariant theory of the Horava-Lifshitz (HL) gravity, proposed recently by Horava and Melby-Thompson, and present all the electric static solutions, which represent the generalization of the Reissner-Nordstrom solution found in Ei... | 9.307452 | 9.323915 | 9.379698 | 8.296324 | 7.941358 | 8.90947 | 8.711724 | 8.798248 | 8.483829 | 10.718472 | 8.235477 | 8.48679 | 8.664656 | 8.477529 | 8.3112 | 8.514799 | 8.491342 | 8.503222 | 8.362462 | 8.957888 | 8.341059 |
hep-th/9707117 | Marcos Alvarez | Marcos Alvarez | Physical states of dyons | 9 pages, no figures | null | null | SWAT-97-156 | hep-th | null | It is shown that physical states of a non-abelian Yang-Mills-Higgs dyon are
invariant under large gauge transformations that do not commute with its
magnetic field. This result is established within an enlarged Hamiltonian
formalism where surface terms are kept as dynamical variables. These additional
variables are p... | [
{
"created": "Fri, 11 Jul 1997 16:05:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Alvarez",
"Marcos",
""
]
] | It is shown that physical states of a non-abelian Yang-Mills-Higgs dyon are invariant under large gauge transformations that do not commute with its magnetic field. This result is established within an enlarged Hamiltonian formalism where surface terms are kept as dynamical variables. These additional variables are par... | 11.630434 | 12.275277 | 10.872311 | 11.125287 | 12.374863 | 10.836724 | 11.595262 | 10.403049 | 11.026896 | 11.734612 | 10.865058 | 10.858962 | 10.538136 | 10.713018 | 10.726948 | 10.458318 | 10.385286 | 10.878212 | 10.779043 | 11.0263 | 10.465663 |
0904.0449 | Diego Trancanelli | Diego Trancanelli | Emergent geometry in N=6 Chern-Simons-matter theory | 6 pages. Talk given at the "BIRS Workshop on Gauge Fields, Cosmology,
and Mathematical String Theory", Banff (Canada), Feb. 1 - 6, 2009; v2:
reference added | null | null | NSF-KITP-09-60 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a strong coupling expansion of N=6 superconformal Chern-Simons
theory obtained from the semiclassical analysis of low energy, effective
degrees of freedom given by the eigenvalues of a certain matrix model. We show
how the orbifolded sphere S^7/Z_k of the dual geometry emerges dynamically from
the dist... | [
{
"created": "Thu, 2 Apr 2009 19:44:38 GMT",
"version": "v1"
},
{
"created": "Wed, 13 May 2009 16:54:22 GMT",
"version": "v2"
}
] | 2009-05-13 | [
[
"Trancanelli",
"Diego",
""
]
] | We investigate a strong coupling expansion of N=6 superconformal Chern-Simons theory obtained from the semiclassical analysis of low energy, effective degrees of freedom given by the eigenvalues of a certain matrix model. We show how the orbifolded sphere S^7/Z_k of the dual geometry emerges dynamically from the distri... | 11.566307 | 9.731903 | 11.88503 | 10.2483 | 11.067857 | 10.536536 | 10.974369 | 9.904517 | 9.931322 | 12.763729 | 9.64117 | 9.794715 | 10.540443 | 10.108086 | 10.290529 | 9.970585 | 10.393048 | 10.132456 | 10.695381 | 10.926573 | 10.41114 |
2210.14705 | Davide De Biasio | Davide De Biasio, Julian Freigang, Dieter Lust and Toby Wiseman | Gradient flow of Einstein-Maxwell theory and Reissner-Nordstr\"om black
holes | 46 pages, 12 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Ricci flow is a natural gradient flow of the Einstein-Hilbert action. Here we
consider the analog for the Einstein-Maxwell action, which gives Ricci flow
with a stress tensor contribution coupled to a Yang-Mills flow for the Maxwell
field. We argue that this flow is well-posed for static spacetimes with pure
electric... | [
{
"created": "Wed, 26 Oct 2022 13:33:37 GMT",
"version": "v1"
}
] | 2022-10-27 | [
[
"De Biasio",
"Davide",
""
],
[
"Freigang",
"Julian",
""
],
[
"Lust",
"Dieter",
""
],
[
"Wiseman",
"Toby",
""
]
] | Ricci flow is a natural gradient flow of the Einstein-Hilbert action. Here we consider the analog for the Einstein-Maxwell action, which gives Ricci flow with a stress tensor contribution coupled to a Yang-Mills flow for the Maxwell field. We argue that this flow is well-posed for static spacetimes with pure electric o... | 8.139091 | 8.617337 | 8.199881 | 8.407135 | 8.842174 | 8.541964 | 8.968478 | 8.162642 | 8.318761 | 8.626816 | 8.393362 | 8.118168 | 8.069 | 7.742609 | 7.900157 | 7.863443 | 7.988039 | 7.861125 | 8.007102 | 8.186347 | 7.779941 |
2201.07807 | David Tennyson | Alex S. Arvanitakis, Emanuel Malek and David Tennyson | Romans massive QP manifolds | V2 - References and discussion added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce QP manifolds that capture the generalised geometry of type IIA
string backgrounds with Ramond-Ramond fluxes and Romans mass. Each of these is
associated to a BPS brane in type IIA: a D2, D4, or NS5-brane. We explain how
these probe branes are related to their associated QP-manifolds via the AKSZ
topologi... | [
{
"created": "Wed, 19 Jan 2022 19:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Feb 2022 12:11:41 GMT",
"version": "v2"
}
] | 2022-02-15 | [
[
"Arvanitakis",
"Alex S.",
""
],
[
"Malek",
"Emanuel",
""
],
[
"Tennyson",
"David",
""
]
] | We introduce QP manifolds that capture the generalised geometry of type IIA string backgrounds with Ramond-Ramond fluxes and Romans mass. Each of these is associated to a BPS brane in type IIA: a D2, D4, or NS5-brane. We explain how these probe branes are related to their associated QP-manifolds via the AKSZ topologica... | 9.445289 | 9.23807 | 12.10278 | 8.53575 | 8.873334 | 8.751841 | 8.998254 | 9.382957 | 8.933132 | 11.05808 | 8.806001 | 8.738955 | 9.480866 | 8.884706 | 8.790688 | 8.737172 | 8.965518 | 8.621271 | 8.734616 | 9.960684 | 8.931725 |
hep-th/9310185 | null | David McMullan and Izumi Tsutsui | BPST instanton and Spin from inequivalent quantizations | 11 pages, plain TeX, PLY-MS-93-04, DIAS-STP-93-21 (This version
should now TeX) | Phys.Lett. B320 (1994) 287-293 | 10.1016/0370-2693(94)90658-0 | null | hep-th | null | We present a simple alternative to Mackey's account of the (infinite)
inequivalent quantizations possible on a coset space G/H. Our reformulation is
based on the reduction ${\rm G \rightarrow G/H}$ and employs a generalized form
of Dirac's approach to the quantization of constrained systems. When applied to
the four-... | [
{
"created": "Thu, 28 Oct 1993 14:01:52 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Nov 1993 10:00:22 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"McMullan",
"David",
""
],
[
"Tsutsui",
"Izumi",
""
]
] | We present a simple alternative to Mackey's account of the (infinite) inequivalent quantizations possible on a coset space G/H. Our reformulation is based on the reduction ${\rm G \rightarrow G/H}$ and employs a generalized form of Dirac's approach to the quantization of constrained systems. When applied to the four-sp... | 12.336343 | 11.714594 | 11.205722 | 10.387088 | 11.420103 | 10.883149 | 10.770756 | 10.671642 | 10.599087 | 14.026265 | 11.276643 | 10.82288 | 11.040302 | 10.667926 | 10.135517 | 10.571374 | 10.909593 | 10.827407 | 10.980438 | 11.272939 | 11.159807 |
0802.1753 | Allan Joseph Michael Medved | A.J.M. Medved | A Comment or two on Holographic Dark Energy | 18 pages; (v2) an oversight in Section 2.1 is rectified and a few
citations added | Gen.Rel.Grav.41:287-303,2009 | 10.1007/s10714-008-0674-9 | null | hep-th gr-qc | null | It has, quite recently, become fashionable to study a certain class of
holographic-inspired models for the dark energy. These investigations have,
indeed, managed to make some significant advances towards explaining the
empirical data. Nonetheless, surprisingly little thought has been given to
conceptual issues such ... | [
{
"created": "Wed, 13 Feb 2008 11:33:55 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Feb 2008 20:45:17 GMT",
"version": "v2"
}
] | 2009-02-18 | [
[
"Medved",
"A. J. M.",
""
]
] | It has, quite recently, become fashionable to study a certain class of holographic-inspired models for the dark energy. These investigations have, indeed, managed to make some significant advances towards explaining the empirical data. Nonetheless, surprisingly little thought has been given to conceptual issues such as... | 17.749153 | 15.030462 | 15.526149 | 15.941932 | 15.319791 | 15.933765 | 15.125899 | 16.048372 | 15.031029 | 16.990191 | 15.032864 | 15.166815 | 15.687727 | 15.341422 | 15.548756 | 15.457718 | 15.379682 | 15.016321 | 15.652518 | 15.377749 | 15.75123 |
1805.05497 | James Gray | Lara. B. Anderson, James Gray and Brian Hammack | Fibrations in Non-simply Connected Calabi-Yau Quotients | 18 pages, 3 figures | null | 10.1007/JHEP08(2018)128 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study genus one fibrations in Calabi-Yau three-folds with a
non-trivial first fundamental group. The manifolds under consideration are
constructed as smooth quotients of complete intersection Calabi-Yau three-folds
(CICYs) by a freely acting, discrete automorphism. By probing the compatibility
of symm... | [
{
"created": "Tue, 15 May 2018 00:08:57 GMT",
"version": "v1"
}
] | 2018-09-26 | [
[
"Anderson",
"Lara. B.",
""
],
[
"Gray",
"James",
""
],
[
"Hammack",
"Brian",
""
]
] | In this work we study genus one fibrations in Calabi-Yau three-folds with a non-trivial first fundamental group. The manifolds under consideration are constructed as smooth quotients of complete intersection Calabi-Yau three-folds (CICYs) by a freely acting, discrete automorphism. By probing the compatibility of symmet... | 10.111856 | 10.561537 | 12.338712 | 9.769126 | 10.13097 | 10.051152 | 10.56063 | 9.85206 | 9.444399 | 11.802434 | 9.962268 | 9.605849 | 10.270494 | 9.688257 | 9.319077 | 9.653468 | 9.597527 | 9.613995 | 9.692889 | 10.124687 | 9.762355 |
2010.10877 | Emil Akhmedov | E.T. Akhmedov, P.A. Anempodistov, K.V. Bazarov, D.V. Diakonov, U.
Moschella | Heating up an environment around black holes and inside de Sitter space | 24 pages, 4 figures; The version to appear in PRD, the title has been
changed again according to the agreement with the editor | Phys. Rev. D 103, 025023 (2021) | 10.1103/PhysRevD.103.025023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study quantum fields on spacetimes having a bifurcate Killing horizon by
allowing the possibility that left- and right- (in-going and out-going) modes
have different temperatures. We consider in particular the Rindler for both
massless and massive fields, the static de Sitter and Schwarzschild black hole
backgroun... | [
{
"created": "Wed, 21 Oct 2020 10:08:46 GMT",
"version": "v1"
},
{
"created": "Sun, 3 Jan 2021 08:07:21 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Jan 2021 07:36:02 GMT",
"version": "v3"
}
] | 2021-02-03 | [
[
"Akhmedov",
"E. T.",
""
],
[
"Anempodistov",
"P. A.",
""
],
[
"Bazarov",
"K. V.",
""
],
[
"Diakonov",
"D. V.",
""
],
[
"Moschella",
"U.",
""
]
] | We study quantum fields on spacetimes having a bifurcate Killing horizon by allowing the possibility that left- and right- (in-going and out-going) modes have different temperatures. We consider in particular the Rindler for both massless and massive fields, the static de Sitter and Schwarzschild black hole backgrounds... | 8.828139 | 8.672297 | 7.809462 | 8.167359 | 7.961749 | 8.50226 | 8.149823 | 7.621545 | 7.740885 | 8.304557 | 8.353718 | 8.488977 | 8.419005 | 8.263511 | 7.960385 | 8.297194 | 8.508135 | 7.978054 | 8.435628 | 8.377544 | 8.288394 |
hep-th/0412036 | Artyom Yurov | A.V. Yurov, V.A. Yurov | The nonsingular brane solutions via the Darboux transformation | 13 pages, 4 figures, RevTex, submitted to Phys.Rev. D | Phys.Rev. D72 (2005) 026003 | 10.1103/PhysRevD.72.026003 | null | hep-th | null | We consider the Darboux transformation as a method of construction of exact
nonsingular solutions describing the three-dimensional brane that interacts
with five-dimensional gravity and the bulk scalar field. To make it work, the
five-dimensional Einstein's equations and the Israel's conditions are being
reduced to t... | [
{
"created": "Fri, 3 Dec 2004 12:59:39 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Apr 2005 10:18:33 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Yurov",
"A. V.",
""
],
[
"Yurov",
"V. A.",
""
]
] | We consider the Darboux transformation as a method of construction of exact nonsingular solutions describing the three-dimensional brane that interacts with five-dimensional gravity and the bulk scalar field. To make it work, the five-dimensional Einstein's equations and the Israel's conditions are being reduced to the... | 14.993919 | 13.676885 | 14.823475 | 14.580652 | 15.161095 | 14.884072 | 15.604177 | 13.517721 | 14.256164 | 14.706476 | 13.918824 | 13.913386 | 14.142399 | 13.451503 | 13.474957 | 14.03073 | 14.18745 | 13.437662 | 13.505419 | 13.57082 | 13.859447 |
hep-th/0210175 | Yonatan Zunger | Yonatan Zunger | Constructing exotic D-branes with infinite matrices in type IIA string
theory | 9 pages, revtex | null | null | SU-ITP/02-39 | hep-th | null | We examine the set of objects which can be built in type IIA string theory by
matrix methods using an infinite number of D0-branes. In addition to stacks of
ordinary Dp-branes and branes in background fields, we find exotic states which
cannot be constructed by other means. These states exhibit strongly
noncommutativ... | [
{
"created": "Fri, 18 Oct 2002 06:41:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Zunger",
"Yonatan",
""
]
] | We examine the set of objects which can be built in type IIA string theory by matrix methods using an infinite number of D0-branes. In addition to stacks of ordinary Dp-branes and branes in background fields, we find exotic states which cannot be constructed by other means. These states exhibit strongly noncommutative ... | 12.620051 | 12.68371 | 13.568196 | 12.362998 | 14.858249 | 13.375929 | 14.023335 | 12.661511 | 12.407605 | 15.244698 | 12.30346 | 11.751506 | 11.906957 | 11.548718 | 11.599565 | 11.742287 | 11.842917 | 11.558412 | 11.652679 | 12.848533 | 11.351925 |
2008.01269 | Jingyi Chao | Jingyi Chao and Thomas Schaefer | Multiplicative noise and the diffusion of conserved densities | add an appendix, updated the references, 17 pages, 5 figures | null | 10.1007/JHEP01(2021)071 | null | hep-th cond-mat.quant-gas nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Stochastic fluid dynamics governs the long time tails of hydrodynamic
correlation functions, and the critical slowing down of relaxation phenomena in
the vicinity of a critical point in the phase diagram. In this work we study
the role of multiplicative noise in stochastic fluid dynamics. Multiplicative
noise arises ... | [
{
"created": "Tue, 4 Aug 2020 01:53:01 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Nov 2020 04:10:42 GMT",
"version": "v2"
}
] | 2021-02-03 | [
[
"Chao",
"Jingyi",
""
],
[
"Schaefer",
"Thomas",
""
]
] | Stochastic fluid dynamics governs the long time tails of hydrodynamic correlation functions, and the critical slowing down of relaxation phenomena in the vicinity of a critical point in the phase diagram. In this work we study the role of multiplicative noise in stochastic fluid dynamics. Multiplicative noise arises fr... | 7.384143 | 8.431742 | 7.526556 | 7.292233 | 7.995411 | 8.564769 | 9.341548 | 8.413067 | 7.854828 | 8.315354 | 8.126524 | 7.017903 | 7.31556 | 7.130337 | 7.061856 | 7.551406 | 7.372274 | 7.25056 | 7.149023 | 7.504397 | 7.468341 |
0904.3144 | Uwe Trittmann | U. Trittmann, S. Pinsky | Effects of a fundamental mass term in two-dimensional super Yang-Mills
theory | 17 pp., 10 figs; substantially revised version to be published in
Phys. Rev. D | Phys.Rev.D80:065005,2009 | 10.1103/PhysRevD.80.065005 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that adding a vacuum expectation value to a gauge field left over
from a dimensional reduction of three-dimensional pure supersymmetric
Yang-Mills theory generates mass terms for the fundamental fields in the
two-dimensional theory while supersymmetry stays intact. This is similar to the
adjoint mass term tha... | [
{
"created": "Tue, 21 Apr 2009 00:02:47 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Jun 2009 15:30:19 GMT",
"version": "v2"
},
{
"created": "Thu, 27 Aug 2009 20:28:10 GMT",
"version": "v3"
}
] | 2009-09-24 | [
[
"Trittmann",
"U.",
""
],
[
"Pinsky",
"S.",
""
]
] | We show that adding a vacuum expectation value to a gauge field left over from a dimensional reduction of three-dimensional pure supersymmetric Yang-Mills theory generates mass terms for the fundamental fields in the two-dimensional theory while supersymmetry stays intact. This is similar to the adjoint mass term that ... | 9.724168 | 10.586013 | 10.264744 | 9.323959 | 10.214426 | 9.36387 | 11.20129 | 9.649918 | 9.715508 | 10.051991 | 9.622337 | 9.526501 | 9.799191 | 9.629509 | 9.706812 | 9.614976 | 9.637366 | 9.781476 | 9.529272 | 9.685664 | 9.246877 |
2210.10794 | Daniel Grumiller | Arjun Bagchi, Daniel Grumiller, and M.M. Sheikh-Jabbari | Horizon Strings as 3d Black Hole Microstates | 24pp; v2: considerably extended version with details and text added
but otherwise same content, v3: converted to SciPost style | SciPost Phys. 15, 210 (2023) | 10.21468/SciPostPhys.15.5.210 | TUW-22-05 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We propose that 3d black holes are an ensemble of tensionless null string
states. These microstates typically have non-zero winding. We evaluate their
partition function in the limit of large excitation numbers and show that their
combinatorics reproduces the Bekenstein-Hawking entropy and its semiclassical
logarithm... | [
{
"created": "Wed, 19 Oct 2022 18:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 23 May 2023 09:08:11 GMT",
"version": "v2"
},
{
"created": "Sat, 7 Oct 2023 17:31:19 GMT",
"version": "v3"
}
] | 2023-11-29 | [
[
"Bagchi",
"Arjun",
""
],
[
"Grumiller",
"Daniel",
""
],
[
"Sheikh-Jabbari",
"M. M.",
""
]
] | We propose that 3d black holes are an ensemble of tensionless null string states. These microstates typically have non-zero winding. We evaluate their partition function in the limit of large excitation numbers and show that their combinatorics reproduces the Bekenstein-Hawking entropy and its semiclassical logarithmic... | 16.518965 | 13.585501 | 15.241182 | 12.891318 | 14.072975 | 13.755841 | 12.882488 | 13.328748 | 14.004906 | 15.888885 | 12.743587 | 13.866331 | 15.663068 | 14.312518 | 14.18504 | 13.842007 | 13.992603 | 13.940903 | 14.488208 | 16.361534 | 13.949727 |
2104.08070 | Cheng-Yong Zhang | Peng Liu, Chao Niu, Zi-Jian Shi, Cheng-Yong Zhang | Entanglement Wedge Minimum Cross-section in Holographic Massive Gravity
Theory | 27 pages, 15 figures | null | 10.1007/JHEP08(2021)113 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the entanglement wedge cross-section (EWCS) in holographic massive
gravity theory, in which a first and second-order phase transition can occur.
We find that the mixed state entanglement measures, the EWCS and mutual
information (MI) can characterize the phase transitions. The EWCS and MI show
exactly the op... | [
{
"created": "Fri, 16 Apr 2021 12:34:42 GMT",
"version": "v1"
},
{
"created": "Thu, 20 May 2021 14:58:00 GMT",
"version": "v2"
}
] | 2021-09-15 | [
[
"Liu",
"Peng",
""
],
[
"Niu",
"Chao",
""
],
[
"Shi",
"Zi-Jian",
""
],
[
"Zhang",
"Cheng-Yong",
""
]
] | We study the entanglement wedge cross-section (EWCS) in holographic massive gravity theory, in which a first and second-order phase transition can occur. We find that the mixed state entanglement measures, the EWCS and mutual information (MI) can characterize the phase transitions. The EWCS and MI show exactly the oppo... | 8.610833 | 8.176724 | 9.035942 | 7.877697 | 8.194793 | 8.486765 | 7.64571 | 7.957541 | 7.962762 | 9.928597 | 7.852461 | 8.018508 | 8.402664 | 8.256084 | 8.081959 | 8.248858 | 8.167688 | 7.762128 | 7.921679 | 8.884217 | 7.929289 |
1001.5343 | Shingo Takeuchi | Youngman Kim, Yoshinori Matsuo, Woojoo Sim, Shingo Takeuchi, Takuya
Tsukioka | Quark Number Susceptibility with Finite Chemical Potential in
Holographic QCD | 25 pages, 3 figures, published version | JHEP 1005:038,2010 | 10.1007/JHEP05(2010)038 | APCTP-Pre2010-001, HRI/ST/1002 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the quark number susceptibility in holographic QCD with a finite
chemical potential or under an external magnetic field at finite temperature.
We first consider the quark number susceptibility with the chemical potential.
We observe that approaching the critical temperature from high temperature
regime, the ... | [
{
"created": "Fri, 29 Jan 2010 07:46:50 GMT",
"version": "v1"
},
{
"created": "Sun, 23 May 2010 14:56:17 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Kim",
"Youngman",
""
],
[
"Matsuo",
"Yoshinori",
""
],
[
"Sim",
"Woojoo",
""
],
[
"Takeuchi",
"Shingo",
""
],
[
"Tsukioka",
"Takuya",
""
]
] | We study the quark number susceptibility in holographic QCD with a finite chemical potential or under an external magnetic field at finite temperature. We first consider the quark number susceptibility with the chemical potential. We observe that approaching the critical temperature from high temperature regime, the qu... | 6.256004 | 6.372617 | 6.292571 | 5.74126 | 6.270852 | 6.427254 | 6.257529 | 6.646447 | 6.058196 | 6.209513 | 6.085104 | 6.011715 | 6.120765 | 6.106889 | 5.992446 | 5.987404 | 6.074839 | 6.008215 | 6.084455 | 6.218545 | 5.998344 |
1303.0622 | Boris A. Arbuzov | Boris A. Arbuzov and Ivan V. Zaitsev | Elimination of the Landau pole in QCD with the spontaneously generated
anomalous three-gluon interaction | 9 pages, 5 figures. arXiv admin note: text overlap with
arXiv:1103.3951, arXiv:0901.3997, arXiv:1107.5164, arXiv:hep-ph/0703237 | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply the Bogoliubov compensation principle to QCD. The non-trivial
solution of compensation equations for a spontaneous generation of the
anomalous three-gluon interaction leads to the determination of parameters of
the theory, including behavior of the gauge coupling $\alpha_s(Q^2)$ without
the Landau singularit... | [
{
"created": "Mon, 4 Mar 2013 07:10:22 GMT",
"version": "v1"
}
] | 2013-03-05 | [
[
"Arbuzov",
"Boris A.",
""
],
[
"Zaitsev",
"Ivan V.",
""
]
] | We apply the Bogoliubov compensation principle to QCD. The non-trivial solution of compensation equations for a spontaneous generation of the anomalous three-gluon interaction leads to the determination of parameters of the theory, including behavior of the gauge coupling $\alpha_s(Q^2)$ without the Landau singularity,... | 8.160954 | 8.874589 | 6.416996 | 6.321206 | 7.905329 | 8.724306 | 7.751674 | 8.254006 | 6.454368 | 6.337414 | 8.348796 | 7.751214 | 7.172414 | 7.176247 | 7.768003 | 7.898959 | 7.547502 | 7.524705 | 7.402616 | 7.524601 | 7.895397 |
hep-th/0303230 | David Berenstein | David Berenstein | D-brane realizations of runaway behavior and moduli stabilization | 15 pages, 3 figures | null | null | null | hep-th | null | In this paper we find examples of moduli stabilization and runaway behavior
which can be treated exactly. This is shown for supersymmetric field theories
which can be realized on the world volume of D-branes. From a geometric point
of view, these field theories lift moduli spaces of vacua by deforming lines of
singul... | [
{
"created": "Wed, 26 Mar 2003 17:50:58 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Berenstein",
"David",
""
]
] | In this paper we find examples of moduli stabilization and runaway behavior which can be treated exactly. This is shown for supersymmetric field theories which can be realized on the world volume of D-branes. From a geometric point of view, these field theories lift moduli spaces of vacua by deforming lines of singular... | 16.778261 | 16.953842 | 16.791096 | 16.079973 | 17.028948 | 16.65221 | 18.160147 | 17.699537 | 16.316078 | 18.578669 | 16.105762 | 15.197879 | 15.991663 | 15.207597 | 14.094413 | 15.389699 | 14.908499 | 14.840269 | 14.94543 | 16.497353 | 14.486499 |
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