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
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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1808.04380 | Victor Gorbenko | Victor Gorbenko, Slava Rychkov, Bernardo Zan | Walking, Weak first-order transitions, and Complex CFTs II.
Two-dimensional Potts model at $Q>4$ | 34 pages, 13 figures. v2: refs added; v3 refs added, typos corrected,
presentation of several arguments clarified | SciPost Phys. 5, 050 (2018) | 10.21468/SciPostPhys.5.5.050 | null | hep-th cond-mat.stat-mech cond-mat.str-el hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study complex CFTs describing fixed points of the two-dimensional
$Q$-state Potts model with $Q>4$. Their existence is closely related to the
weak first-order phase transition and walking RG behavior present in the real
Potts model at $Q>4$. The Potts model, apart from its own significance, serves
as an ideal play... | [
{
"created": "Mon, 13 Aug 2018 18:00:12 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Aug 2018 12:06:20 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Oct 2018 23:48:22 GMT",
"version": "v3"
}
] | 2018-11-28 | [
[
"Gorbenko",
"Victor",
""
],
[
"Rychkov",
"Slava",
""
],
[
"Zan",
"Bernardo",
""
]
] | We study complex CFTs describing fixed points of the two-dimensional $Q$-state Potts model with $Q>4$. Their existence is closely related to the weak first-order phase transition and walking RG behavior present in the real Potts model at $Q>4$. The Potts model, apart from its own significance, serves as an ideal playgr... | 9.198307 | 10.799664 | 11.112626 | 9.606903 | 10.678896 | 11.09822 | 10.479473 | 10.98568 | 10.304128 | 10.660089 | 9.963033 | 9.472303 | 9.351949 | 9.230497 | 9.084874 | 8.967362 | 9.177768 | 9.1771 | 8.988551 | 9.364521 | 9.046824 |
1203.1442 | Rio Saitou | Rio Saitou, Shin'ichi Nojiri | Stable phantom-divide crossing in two scalar models with matter | 12 pages, 1 figure | null | 10.1140/epjc/s10052-012-1946-9 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct cosmological models with two scalar fields, which has the
structure as in the ghost condensation model or k-essence model. The models can
describe the stable phantom crossing, which should be contrasted with one
scalar tensor models, where the infinite instability occurs at the crossing the
phantom divid... | [
{
"created": "Wed, 7 Mar 2012 11:24:17 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Mar 2012 04:49:25 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Saitou",
"Rio",
""
],
[
"Nojiri",
"Shin'ichi",
""
]
] | We construct cosmological models with two scalar fields, which has the structure as in the ghost condensation model or k-essence model. The models can describe the stable phantom crossing, which should be contrasted with one scalar tensor models, where the infinite instability occurs at the crossing the phantom divide.... | 13.506266 | 13.635454 | 13.9527 | 13.589265 | 13.810308 | 14.194864 | 14.206765 | 12.70901 | 13.603901 | 14.868147 | 13.736177 | 13.696787 | 13.179277 | 12.96052 | 13.24415 | 13.3445 | 13.414062 | 13.42395 | 13.725996 | 13.765963 | 13.328369 |
1209.5403 | Christoph Adam | C. Adam, J. Sanchez-Guillen, A. Wereszczynski, W. J. Zakrzewski | Topological duality between vortices and planar skyrmions in BPS
theories with APD symmetries | Latex, 18 pages, references added, typos corrected | null | 10.1103/PhysRevD.87.027703 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The BPS baby Skyrme models are submodels of baby Skyrme models, where the
nonlinear sigma model term is suppressed. They have skyrmion solutions
saturating a BPS bound, and the corresponding static energy functional is
invariant under area-preserving diffeomorphisms (APDs). Here we show that the
solitons in the BPS b... | [
{
"created": "Mon, 24 Sep 2012 20:02:31 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Oct 2012 18:53:09 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Adam",
"C.",
""
],
[
"Sanchez-Guillen",
"J.",
""
],
[
"Wereszczynski",
"A.",
""
],
[
"Zakrzewski",
"W. J.",
""
]
] | The BPS baby Skyrme models are submodels of baby Skyrme models, where the nonlinear sigma model term is suppressed. They have skyrmion solutions saturating a BPS bound, and the corresponding static energy functional is invariant under area-preserving diffeomorphisms (APDs). Here we show that the solitons in the BPS bab... | 5.211313 | 4.663787 | 5.126135 | 4.539104 | 5.07394 | 4.699394 | 4.610454 | 4.589476 | 4.471361 | 5.713327 | 4.497485 | 4.549667 | 4.901454 | 4.698439 | 4.757928 | 4.696493 | 4.645278 | 4.756599 | 4.586101 | 4.82228 | 4.519919 |
2305.11209 | Marco Meineri | Marco Meineri, Joao Penedones, Taro Spirig | Renormalization group flows in AdS and the bootstrap program | 43+27 pages, 10 figures, a few typos removed, a couple of references
added, matches published version | null | 10.1007/JHEP07(2024)229 | null | hep-th | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We study correlation functions of the bulk stress tensor and boundary
operators in Quantum Field Theories (QFT) in Anti-de Sitter (AdS) space. In
particular, we derive new sum rules from the two-point function of the stress
tensor and its three-point function with two boundary operators. In AdS2, this
leads to a boot... | [
{
"created": "Thu, 18 May 2023 18:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Jul 2024 09:03:24 GMT",
"version": "v2"
}
] | 2024-07-31 | [
[
"Meineri",
"Marco",
""
],
[
"Penedones",
"Joao",
""
],
[
"Spirig",
"Taro",
""
]
] | We study correlation functions of the bulk stress tensor and boundary operators in Quantum Field Theories (QFT) in Anti-de Sitter (AdS) space. In particular, we derive new sum rules from the two-point function of the stress tensor and its three-point function with two boundary operators. In AdS2, this leads to a bootst... | 9.282848 | 8.744303 | 9.832371 | 8.102418 | 8.702852 | 8.823021 | 8.796844 | 8.492617 | 7.886902 | 9.793569 | 8.3751 | 8.524469 | 9.046591 | 8.441791 | 8.550381 | 8.626245 | 8.191914 | 8.347882 | 8.399083 | 8.836035 | 8.289362 |
hep-th/0207235 | Johannes Walcher | Alex Buchel, Peter Langfelder and Johannes Walcher | Does the Tachyon Matter? | 15 pages, 1 figure, v2: refs added, v3: two more refs added | Annals Phys. 302 (2002) 78-87 | 10.1006/aphy.2002.6306 | NSF-ITP-02-65, YITP-SB-02-38 | hep-th | null | We study time-dependent solutions of Einstein-Maxwell gravity in four
dimensions coupled to tachyon matter--the Dirac-Born-Infeld Lagrangian that
provides an effective description of a decaying tachyon on an unstable D-brane
in string theory. Asymptotically, the solutions are similar to the recently
studied space-lik... | [
{
"created": "Thu, 25 Jul 2002 23:43:51 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Aug 2002 17:28:58 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Aug 2002 20:46:13 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Buchel",
"Alex",
""
],
[
"Langfelder",
"Peter",
""
],
[
"Walcher",
"Johannes",
""
]
] | We study time-dependent solutions of Einstein-Maxwell gravity in four dimensions coupled to tachyon matter--the Dirac-Born-Infeld Lagrangian that provides an effective description of a decaying tachyon on an unstable D-brane in string theory. Asymptotically, the solutions are similar to the recently studied space-like ... | 7.649881 | 7.5139 | 7.955068 | 6.893321 | 7.457915 | 6.961782 | 7.020814 | 7.288079 | 7.240469 | 8.342999 | 7.288457 | 7.279643 | 7.601721 | 7.189111 | 6.927568 | 7.213849 | 7.130504 | 6.931327 | 7.268298 | 7.756551 | 7.085289 |
hep-th/0110117 | Alan Coley | A. Coley | No Chaos in Brane-World Cosmology | Updated Refs. Final version to appear in Class. Quantum Grav | Class.Quant.Grav.19:L45-L56,2002 | 10.1088/0264-9381/19/8/102 | null | hep-th gr-qc | null | We discuss the asymptotic dynamical evolution of spatially homogeneous
brane-world cosmological models close to the initial singularity. We find that
generically the cosmological singularity is isotropic in Bianchi type IX
brane-world models and consequently these models do not exhibit Mixmaster or
chaotic-like behav... | [
{
"created": "Fri, 12 Oct 2001 19:38:42 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Feb 2002 16:51:35 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Coley",
"A.",
""
]
] | We discuss the asymptotic dynamical evolution of spatially homogeneous brane-world cosmological models close to the initial singularity. We find that generically the cosmological singularity is isotropic in Bianchi type IX brane-world models and consequently these models do not exhibit Mixmaster or chaotic-like behavio... | 7.633899 | 7.42932 | 5.84951 | 6.00909 | 6.784515 | 6.133974 | 7.981604 | 5.90778 | 7.781813 | 6.312017 | 7.111307 | 7.235238 | 6.899668 | 6.902969 | 7.193575 | 7.116717 | 7.313948 | 6.941909 | 7.632025 | 7.015058 | 7.184213 |
hep-th/9310033 | Ramy Brustein | R. Brustein, M. Faux and B. Ovrut | Effective d=2 supersymmetric Lagrangians from d=1 supermatrix models | 59 pages. Contains 5 postscript figures included with epsf macro.
Figures obtained upon request, preprint CERN-TH.7017/93 | Nucl.Phys. B421 (1994) 293-342 | 10.1016/0550-3213(94)90330-1 | null | hep-th | null | We discuss $d=1, {\cal N}=2$ supersymmetric matrix models and exhibit the
associated $d=2$ collective field theory in the limit of dense eigenvalues.
From this theory we construct, by the addition of several new fields, a $d=2$
supersymmetric effective field theory, which reduces to the collective field
theory when t... | [
{
"created": "Wed, 6 Oct 1993 19:51:07 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Brustein",
"R.",
""
],
[
"Faux",
"M.",
""
],
[
"Ovrut",
"B.",
""
]
] | We discuss $d=1, {\cal N}=2$ supersymmetric matrix models and exhibit the associated $d=2$ collective field theory in the limit of dense eigenvalues. From this theory we construct, by the addition of several new fields, a $d=2$ supersymmetric effective field theory, which reduces to the collective field theory when the... | 8.566987 | 6.436759 | 8.787567 | 7.492126 | 6.478925 | 6.105385 | 6.329961 | 7.017119 | 7.024666 | 10.21017 | 7.382814 | 7.718804 | 8.610436 | 7.982917 | 7.583118 | 7.282795 | 7.663056 | 7.854094 | 7.967709 | 8.503773 | 7.769659 |
0907.2677 | Miloslav Znojil | Miloslav Znojil | Fundamental length in quantum theories with PT-symmetric Hamiltonians | 31 pp, 3 figures | Phys.Rev.D80:045022,2009 | 10.1103/PhysRevD.80.045022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The direct observability of coordinates x is often lost in PT-symmetric
quantum theories. A manifestly non-local Hilbert-space metric $\Theta$ enters
the double-integral normalization of wave functions $\psi(x)$ there. In the
context of scattering, the (necessary) return to the asymptotically fully local
metric has b... | [
{
"created": "Wed, 15 Jul 2009 18:19:08 GMT",
"version": "v1"
}
] | 2009-09-02 | [
[
"Znojil",
"Miloslav",
""
]
] | The direct observability of coordinates x is often lost in PT-symmetric quantum theories. A manifestly non-local Hilbert-space metric $\Theta$ enters the double-integral normalization of wave functions $\psi(x)$ there. In the context of scattering, the (necessary) return to the asymptotically fully local metric has bee... | 20.009338 | 24.399775 | 24.573093 | 21.286037 | 21.748619 | 23.814486 | 24.437126 | 22.011423 | 21.338058 | 24.994041 | 23.415129 | 21.112793 | 20.293192 | 19.268051 | 20.666006 | 20.710999 | 21.363857 | 19.783213 | 20.031239 | 20.741201 | 20.120697 |
1909.10916 | Kazuo Fujikawa | Shinichi Deguchi, Kazuo Fujikawa | A new magnetic monopole inspired by Berry's phase | 17 pages, 3 figures. The presentation has been subtantially modified
by creating a new subsection and reducing the number of figures, by
concentrating more on the monopole aspect then on Berry's phase. The present
version is going to be published in Phys. Lett. B. arXiv admin note: text
overlap with arXiv:1905.... | null | 10.1016/j.physletb.2020.135210 | RIKEN-iTHEMS-Report-19 | hep-th cond-mat.mes-hall hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new static and azimuthally symmetric magnetic monopolelike object, which
looks like a Dirac monopole when seen from far away but smoothly changes to a
dipole near the monopole position and vanishes at the origin, is discussed.
This monopolelike object is inspired by an analysis of an exactly solvable
model of Berry... | [
{
"created": "Mon, 23 Sep 2019 08:50:58 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jan 2020 08:12:07 GMT",
"version": "v2"
}
] | 2020-03-18 | [
[
"Deguchi",
"Shinichi",
""
],
[
"Fujikawa",
"Kazuo",
""
]
] | A new static and azimuthally symmetric magnetic monopolelike object, which looks like a Dirac monopole when seen from far away but smoothly changes to a dipole near the monopole position and vanishes at the origin, is discussed. This monopolelike object is inspired by an analysis of an exactly solvable model of Berry's... | 7.196941 | 7.417962 | 7.422307 | 6.750477 | 7.209325 | 7.293396 | 7.2387 | 6.731453 | 6.984863 | 7.662694 | 6.646397 | 6.764811 | 6.978367 | 6.773585 | 6.649599 | 6.685587 | 6.990854 | 6.797078 | 6.60543 | 7.058876 | 6.693453 |
1412.5181 | Konstantinos Siampos | Konstantinos Sfetsos, Konstantinos Siampos | The anisotropic \lambda-deformed SU(2) model is integrable | 1+17 pages, Latex, v2: few minor changes, PLB version, v3: Correcting
an erroneous mistake on the diagonalizability of the coupling matrix, v4: We
corrected the multiplicative factor in 2.16 | J. Phys. Lett. B 743 (2015) 160-165 | 10.1016/j.physletb.2015.02.040 | null | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The all-loop anisotropic Thirring model interpolates between the WZW model
and the non-Abelian T-dual of the anisotropic principal chiral model. We focus
on the SU(2) case and we prove that it is classically integrable by providing
its Lax pair formulation. We derive its underlying symmetry current algebra and
use it... | [
{
"created": "Tue, 16 Dec 2014 21:00:13 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Feb 2015 16:16:17 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Jun 2015 09:27:36 GMT",
"version": "v3"
},
{
"created": "Tue, 20 Feb 2018 06:55:32 GMT",
"version": "v4"
}
] | 2018-02-21 | [
[
"Sfetsos",
"Konstantinos",
""
],
[
"Siampos",
"Konstantinos",
""
]
] | The all-loop anisotropic Thirring model interpolates between the WZW model and the non-Abelian T-dual of the anisotropic principal chiral model. We focus on the SU(2) case and we prove that it is classically integrable by providing its Lax pair formulation. We derive its underlying symmetry current algebra and use it t... | 8.618967 | 7.405755 | 10.861097 | 7.638819 | 8.726412 | 7.883977 | 8.094983 | 7.950573 | 7.817503 | 10.641422 | 8.119375 | 8.193671 | 9.033888 | 7.988523 | 8.604387 | 8.343797 | 8.392513 | 7.942502 | 8.267513 | 9.380549 | 8.1235 |
hep-th/0104251 | Chengbo Guan | Z. Chang (1), C.B. Guan (1), H.Y. Guo (2) ((1) IHEP, Academia Sinica,
(2) ITP, Academia Sinica) | AdS Dynamics for Massive Scalar Field: exact solutions vs. bulk-boundary
propagator | LaTeX, 18 pages, 3 eps figures | Int.J.Mod.Phys. A18 (2003) 1657-1670 | 10.1142/S0217751X03013739 | null | hep-th | null | AdS dynamics for massive scalar field is studied both by solving exactly the
equation of motion and by constructing bulk-boundary propagator. A
Robertson-Walker-like metric is deduced from the familiar SO(2,n) invariant
metric. The metric allows us to present a time-like Killing vector, which is
not only invariant un... | [
{
"created": "Sun, 29 Apr 2001 07:26:07 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Chang",
"Z.",
""
],
[
"Guan",
"C. B.",
""
],
[
"Guo",
"H. Y.",
""
]
] | AdS dynamics for massive scalar field is studied both by solving exactly the equation of motion and by constructing bulk-boundary propagator. A Robertson-Walker-like metric is deduced from the familiar SO(2,n) invariant metric. The metric allows us to present a time-like Killing vector, which is not only invariant unde... | 13.149643 | 12.597373 | 13.438732 | 13.076082 | 13.242846 | 13.302588 | 12.736122 | 13.013263 | 12.490623 | 13.281738 | 12.46078 | 11.666687 | 11.674829 | 11.573909 | 11.858191 | 12.320536 | 11.844284 | 11.436163 | 11.746481 | 11.827459 | 11.876087 |
hep-th/0308035 | Kimball A. Milton | Kimball A. Milton | Anomalies in PT-Symmetric Quantum Field Theory | 7 pages, uses czjphys.cls, to appear in proceedings of Workshop on
Pseudo-Hermitian Hamiltonians in Quantum Physics | Czech.J.Phys. 54 (2004) 85-91 | 10.1023/B:CJOP.0000014372.21537.c0 | null | hep-th quant-ph | null | It is shown that a version of PT-symmetric electrodynamics based on an
axial-vector current coupling massless fermions to the photon possesses
anomalies and so is rendered nonrenormalizable. An alternative theory is
proposed based on the conventional vector current constructed from massive
Dirac fields, but in which ... | [
{
"created": "Tue, 5 Aug 2003 18:09:49 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Milton",
"Kimball A.",
""
]
] | It is shown that a version of PT-symmetric electrodynamics based on an axial-vector current coupling massless fermions to the photon possesses anomalies and so is rendered nonrenormalizable. An alternative theory is proposed based on the conventional vector current constructed from massive Dirac fields, but in which th... | 17.538177 | 17.578005 | 13.993585 | 15.170926 | 16.602049 | 16.33993 | 16.610151 | 15.381874 | 15.936383 | 16.796312 | 15.186897 | 15.023458 | 15.444559 | 15.803313 | 16.296692 | 15.199738 | 15.743882 | 15.731478 | 15.353447 | 16.399651 | 15.494117 |
hep-th/0208158 | null | N. Alonso-Alberca, E. Lozano-Tellechea and T. Ortin | Geometric Construction of Killing Spinors and Supersymmetry Algebras in
Homogeneous Spacetimes | misprints corrected and references added. Version to appear in
Classical and Quantum Gravity | Class.Quant.Grav. 19 (2002) 6009-6024 | 10.1088/0264-9381/19/23/309 | IFT-UAM/CSIC-02-35 | hep-th gr-qc | null | We show how the Killing spinors of some maximally supersymmetric supergravity
solutions whose metrics describe symmetric spacetimes (including $AdS,AdS\times
S$ and H$pp$-waves) can be easily constructed using purely geometrical and
group-theoretical methods. The calculation of the supersymmetry algebras is
extremely... | [
{
"created": "Wed, 21 Aug 2002 19:25:52 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Nov 2002 18:07:22 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Alonso-Alberca",
"N.",
""
],
[
"Lozano-Tellechea",
"E.",
""
],
[
"Ortin",
"T.",
""
]
] | We show how the Killing spinors of some maximally supersymmetric supergravity solutions whose metrics describe symmetric spacetimes (including $AdS,AdS\times S$ and H$pp$-waves) can be easily constructed using purely geometrical and group-theoretical methods. The calculation of the supersymmetry algebras is extremely s... | 11.561598 | 11.657011 | 12.242623 | 10.405408 | 11.975172 | 11.042619 | 10.208936 | 10.660397 | 10.503944 | 13.283278 | 9.783764 | 10.623295 | 11.535747 | 10.815735 | 10.962921 | 10.629796 | 10.739199 | 10.373539 | 10.744925 | 10.548453 | 10.211229 |
hep-th/9705087 | V. P. Nair | Dimitra Karabali, Chanju Kim, V.P. Nair | Planar Yang-Mills theory: Hamiltonian, regulators and mass gap | 41 pages, Plain TeX, discussion added, typos corrected | Nucl.Phys.B524:661-694,1998 | 10.1016/S0550-3213(98)00309-5 | CCNY-HEP 97/5, RU-97-3-B, SNUTP 97-054 | hep-th | null | We carry out the Hamiltonian analysis of non-Abelian gauge theories in (2+1)
dimensions in a gauge-invariant matrix parametrization of the fields. A
detailed discussion of regularization issues and the construction of the
renormalized Laplace operator on the configuration space, which is proportional
to the kinetic e... | [
{
"created": "Tue, 13 May 1997 16:05:07 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Apr 1998 14:50:58 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Karabali",
"Dimitra",
""
],
[
"Kim",
"Chanju",
""
],
[
"Nair",
"V. P.",
""
]
] | We carry out the Hamiltonian analysis of non-Abelian gauge theories in (2+1) dimensions in a gauge-invariant matrix parametrization of the fields. A detailed discussion of regularization issues and the construction of the renormalized Laplace operator on the configuration space, which is proportional to the kinetic ene... | 12.00269 | 10.808857 | 12.062861 | 10.970949 | 10.729683 | 11.475368 | 11.305484 | 10.461906 | 9.703387 | 11.524536 | 10.32899 | 10.340508 | 11.129593 | 10.527504 | 10.780393 | 10.352318 | 10.164495 | 10.682143 | 10.531837 | 11.151995 | 10.225891 |
hep-th/0411121 | Robert McNees | Joshua L. Davis, Robert McNees | Boundary Counterterms and the Thermodynamics of 2-D Black Holes | 27 pages, uses utarticle.cls; corrected typos and added references | JHEP0509:072,2005 | 10.1088/1126-6708/2005/09/072 | MCTP-04-65 | hep-th gr-qc | null | We utilize a novel method to study the thermodynamics of two dimensional type
0A black holes with constant RR flux. Our approach is based on the
Hamilton-Jacobi method of deriving boundary counterterms. We demonstrate this
approach by recovering the standard results for a well understood example,
Witten's black hole.... | [
{
"created": "Thu, 11 Nov 2004 20:39:00 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jul 2005 15:01:12 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Davis",
"Joshua L.",
""
],
[
"McNees",
"Robert",
""
]
] | We utilize a novel method to study the thermodynamics of two dimensional type 0A black holes with constant RR flux. Our approach is based on the Hamilton-Jacobi method of deriving boundary counterterms. We demonstrate this approach by recovering the standard results for a well understood example, Witten's black hole. B... | 10.113064 | 9.041746 | 10.522875 | 8.671502 | 8.837495 | 8.72756 | 8.611501 | 8.947232 | 9.227635 | 10.631199 | 8.677299 | 9.182196 | 9.856931 | 8.839556 | 9.134148 | 9.221178 | 9.410659 | 9.052186 | 9.207642 | 10.10003 | 9.141047 |
hep-th/0005216 | Dragovich | G.S.Djordjevic, B.Dragovich and LJ. Nesic | p-Adic and Adelic Free Relativistic Particle | 9 pages | Mod.Phys.Lett. A14 (1999) 317-325 | 10.1142/S0217732399000365 | null | hep-th math-ph math.MP | null | We consider spectral problem for a free relativistic particle in p-adic and
adelic quantum mechanics. In particular, we found p-adic and adelic
eigenfunctions. Within adelic approach there exist quantum states that exhibit
discrete structure of spacetime at the Planck scale.
| [
{
"created": "Wed, 24 May 2000 09:04:14 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Djordjevic",
"G. S.",
""
],
[
"Dragovich",
"B.",
""
],
[
"Nesic",
"LJ.",
""
]
] | We consider spectral problem for a free relativistic particle in p-adic and adelic quantum mechanics. In particular, we found p-adic and adelic eigenfunctions. Within adelic approach there exist quantum states that exhibit discrete structure of spacetime at the Planck scale. | 14.455099 | 11.541615 | 12.182616 | 9.89676 | 11.36962 | 11.940458 | 11.786053 | 9.754817 | 10.505139 | 14.190874 | 11.027402 | 12.337329 | 12.053699 | 10.587423 | 11.501835 | 11.417003 | 11.365656 | 11.699977 | 10.804621 | 12.888504 | 11.726457 |
hep-th/0312080 | Katsusada Morita | Katsusada Morita | A New Gauge-Invariant Regularization Scheme Based on Lorentz-Invariant
Noncommutative Quantum Field Theory | 27 pages, platex | Prog.Theor.Phys. 111 (2004) 881-905 | 10.1143/PTP.111.881 | null | hep-th | null | The IR/UV mixing in the non-commutative (NC) field theory is investigated in
Carlson-Carone-Zobin (CCZ) formalism of Lorentz-invariant NC field theory
provided that the fields are `independent' of the `internal' coordinates
$\theta^{\mu\nu}$. A new regularization scheme called NC regularizatioon is
then proposed, whi... | [
{
"created": "Mon, 8 Dec 2003 09:02:45 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Jan 2004 06:57:02 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Morita",
"Katsusada",
""
]
] | The IR/UV mixing in the non-commutative (NC) field theory is investigated in Carlson-Carone-Zobin (CCZ) formalism of Lorentz-invariant NC field theory provided that the fields are `independent' of the `internal' coordinates $\theta^{\mu\nu}$. A new regularization scheme called NC regularizatioon is then proposed, which... | 7.918059 | 8.009336 | 8.308918 | 7.514019 | 8.609253 | 7.771278 | 8.165354 | 7.995439 | 7.728811 | 8.842605 | 7.518468 | 7.811404 | 7.705775 | 7.599032 | 7.487569 | 7.760715 | 7.534834 | 7.712344 | 7.645846 | 7.857594 | 7.603943 |
2302.13371 | Shi Cheng | Shi Cheng, Piotr Su{\l}kowski | 3d $\mathcal{N}=2$ theories and plumbing graphs: adding matter, gauging,
and new dualities | 66 pages, many figures | null | 10.1007/JHEP08(2023)136 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Recently, a large class of 3d $\mathcal{N} = 2$ gauge theories with mixed
Chern-Simons levels, corresponding to plumbing 3-manifolds, has been
identified. In this paper we generalize these theories by including in their
content chiral multiples, and analyze their properties. We find that the
content of such theories ... | [
{
"created": "Sun, 26 Feb 2023 18:11:58 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Aug 2023 06:52:05 GMT",
"version": "v2"
}
] | 2023-08-25 | [
[
"Cheng",
"Shi",
""
],
[
"Sułkowski",
"Piotr",
""
]
] | Recently, a large class of 3d $\mathcal{N} = 2$ gauge theories with mixed Chern-Simons levels, corresponding to plumbing 3-manifolds, has been identified. In this paper we generalize these theories by including in their content chiral multiples, and analyze their properties. We find that the content of such theories ca... | 9.530803 | 9.170559 | 10.662481 | 8.585955 | 9.626166 | 9.18911 | 9.474363 | 8.807704 | 8.91592 | 11.846518 | 8.758318 | 8.809785 | 9.636011 | 8.71467 | 9.067085 | 8.916012 | 8.895616 | 8.65344 | 8.817358 | 9.564156 | 8.642938 |
2211.13667 | Jose Ramon Espinosa | J.R. Espinosa and J.-F. Fortin | Vacuum Decay Actions from Tunneling Potentials for General Spacetime
Dimension | 17 pages plus appendices | null | 10.1088/1475-7516/2023/02/023 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The tunneling potential method to calculate the action for vacuum decay is an
alternative to the Euclidean bounce method that has a number of attractive
features. In this paper we extend the formalism to general spacetime dimension
$d>2$ and use it to give simple proofs of several results. For Minkowski or
Anti de Si... | [
{
"created": "Thu, 24 Nov 2022 15:34:11 GMT",
"version": "v1"
}
] | 2023-02-22 | [
[
"Espinosa",
"J. R.",
""
],
[
"Fortin",
"J. -F.",
""
]
] | The tunneling potential method to calculate the action for vacuum decay is an alternative to the Euclidean bounce method that has a number of attractive features. In this paper we extend the formalism to general spacetime dimension $d>2$ and use it to give simple proofs of several results. For Minkowski or Anti de Sitt... | 13.671453 | 11.353771 | 13.271461 | 11.713531 | 12.008181 | 11.664064 | 12.079571 | 11.483992 | 12.088626 | 14.105579 | 11.798105 | 12.675089 | 12.793474 | 12.307911 | 13.176906 | 12.799253 | 12.642011 | 12.383508 | 12.257359 | 13.304547 | 12.39009 |
1706.05061 | Antony Speranza | Antony J. Speranza | Local phase space and edge modes for diffeomorphism-invariant theories | 29+12 pages, references added and minor typos fixed | null | 10.1007/JHEP02(2018)021 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss an approach to characterizing local degrees of freedom of a
subregion in diffeomorphism-invariant theories using the extended phase space
of Donnelly and Freidel, [JHEP 2016 (2016) 102]. Such a characterization is
important for defining local observables and entanglement entropy in
gravitational theories. ... | [
{
"created": "Thu, 15 Jun 2017 19:59:53 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jul 2017 15:12:50 GMT",
"version": "v2"
}
] | 2018-02-09 | [
[
"Speranza",
"Antony J.",
""
]
] | We discuss an approach to characterizing local degrees of freedom of a subregion in diffeomorphism-invariant theories using the extended phase space of Donnelly and Freidel, [JHEP 2016 (2016) 102]. Such a characterization is important for defining local observables and entanglement entropy in gravitational theories. Tr... | 7.179054 | 7.389667 | 7.22626 | 7.011455 | 7.264117 | 7.307209 | 7.158771 | 6.889306 | 7.118316 | 7.668546 | 7.092224 | 7.021997 | 7.124217 | 6.884121 | 7.080037 | 7.067468 | 7.257131 | 7.048278 | 7.117354 | 7.093881 | 7.030789 |
1504.04176 | Andelka Andrasi | A. Andrasi, J. C. Taylor | Finiteness of the Coulomb gauge QCD perturbative effective action | Accepted in Annals of Physics | Annals of Physics, 356 (2015) 352-368 | 10.1016/j.aop.2015.03.014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | At 2-loop order in the Coulomb gauge, individual Feynman graphs contributing
to the effective action have energy divergences. It is proved that these cancel
in suitable combinations of graphs. This has previously been shown only for
transverse external fields. The calculation results in a generalization of the
Christ... | [
{
"created": "Thu, 16 Apr 2015 10:33:39 GMT",
"version": "v1"
}
] | 2015-08-14 | [
[
"Andrasi",
"A.",
""
],
[
"Taylor",
"J. C.",
""
]
] | At 2-loop order in the Coulomb gauge, individual Feynman graphs contributing to the effective action have energy divergences. It is proved that these cancel in suitable combinations of graphs. This has previously been shown only for transverse external fields. The calculation results in a generalization of the Christ-L... | 14.085893 | 12.057085 | 15.322348 | 12.732724 | 14.221456 | 13.328508 | 12.472298 | 11.841519 | 12.070027 | 14.977951 | 12.32293 | 11.881633 | 13.486081 | 12.526607 | 11.660417 | 11.377153 | 11.709099 | 11.332873 | 11.919627 | 13.571874 | 12.229473 |
2304.00679 | Josh Kirklin | Josh Kirklin | Probes, purviews, purgatories, parable, paradox? | 12 pages, 5 figures. Essay written for the Gravity Research
Foundation 2023 Awards for Essays on Gravitation | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I discuss some general information-theoretic properties of quantum mechanical
probes in semiclassical gravity: their purview, i.e. what they can see and act
on (in terms of a generalised entanglement wedge), their spontaneous
evaporation into a cloud of highly entropic particles when one tries to make
them see too mu... | [
{
"created": "Mon, 3 Apr 2023 01:45:20 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Apr 2023 08:51:33 GMT",
"version": "v2"
}
] | 2023-04-14 | [
[
"Kirklin",
"Josh",
""
]
] | I discuss some general information-theoretic properties of quantum mechanical probes in semiclassical gravity: their purview, i.e. what they can see and act on (in terms of a generalised entanglement wedge), their spontaneous evaporation into a cloud of highly entropic particles when one tries to make them see too much... | 26.738876 | 24.501617 | 25.835278 | 23.36656 | 23.110622 | 24.683784 | 27.386286 | 24.265049 | 23.433855 | 29.479115 | 21.936108 | 23.419958 | 23.569351 | 24.72447 | 23.67679 | 24.323692 | 22.712605 | 23.870687 | 23.75193 | 24.481384 | 23.426334 |
hep-th/9602139 | Steven Brumby | S. P. Brumby, R. Foot, and R. R. Volkas | Quaternionic Formulation of the Exact Parity Model | 30 pages, standard LaTeX, submitted to Phys. Rev. D | null | null | University of Melbourne UM-P-96/11 RCHEP 96/01 | hep-th hep-ph | null | The exact parity model (EPM) is a simple extension of the Standard Model
which reinstates parity invariance as an unbroken symmetry of nature. The
mirror matter sector of the model can interact with ordinary matter through
gauge boson mixing, Higgs boson mixing and, if neutrinos are massive, through
neutrino mixing. ... | [
{
"created": "Tue, 27 Feb 1996 06:32:21 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Brumby",
"S. P.",
""
],
[
"Foot",
"R.",
""
],
[
"Volkas",
"R. R.",
""
]
] | The exact parity model (EPM) is a simple extension of the Standard Model which reinstates parity invariance as an unbroken symmetry of nature. The mirror matter sector of the model can interact with ordinary matter through gauge boson mixing, Higgs boson mixing and, if neutrinos are massive, through neutrino mixing. Th... | 7.246683 | 7.809186 | 6.509264 | 7.155705 | 7.924689 | 7.845285 | 6.754838 | 7.281076 | 6.948485 | 7.072677 | 7.793223 | 7.083447 | 7.221488 | 7.063433 | 7.135235 | 7.214383 | 7.440227 | 7.166625 | 7.081984 | 7.141047 | 6.661833 |
1110.4803 | Sang-Woo Kim | Sang-Woo Kim, Jun Nishimura, Asato Tsuchiya | Expanding universe as a classical solution in the Lorentzian matrix
model for nonperturbative superstring theory | 4 pages, 2 figures | null | 10.1103/PhysRevD.86.027901 | KEK-TH-1503, OU-HET-729-2011 | hep-th astro-ph.CO gr-qc hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently we have shown by Monte Carlo simulation that expanding
(3+1)-dimensional universe appears dynamically from a Lorentzian matrix model
for type IIB superstring theory in (9+1)-dimensions. The mechanism for the
spontaneous breaking of rotational symmetry relies crucially on the
noncommutative nature of the spac... | [
{
"created": "Fri, 21 Oct 2011 14:30:30 GMT",
"version": "v1"
}
] | 2015-05-30 | [
[
"Kim",
"Sang-Woo",
""
],
[
"Nishimura",
"Jun",
""
],
[
"Tsuchiya",
"Asato",
""
]
] | Recently we have shown by Monte Carlo simulation that expanding (3+1)-dimensional universe appears dynamically from a Lorentzian matrix model for type IIB superstring theory in (9+1)-dimensions. The mechanism for the spontaneous breaking of rotational symmetry relies crucially on the noncommutative nature of the space.... | 8.561278 | 7.434268 | 8.9819 | 7.55397 | 7.991805 | 7.956693 | 7.578202 | 7.199771 | 7.481114 | 9.297002 | 7.563125 | 8.089967 | 8.224121 | 7.842156 | 7.841173 | 7.833285 | 7.931894 | 7.931614 | 7.982702 | 8.437646 | 7.774732 |
1812.00026 | Christian Saemann | Andreas Deser and Christian Saemann | Extended Riemannian Geometry III: Global Double Field Theory with
Nilmanifolds | 36 pages, typos fixed, references added, presentation improved and
discussion added, published version | JHEP 05 (2019) 209 | 10.1007/JHEP05(2019)209 | EMPG-18-24 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe the global geometry, symmetries and tensors for Double Field
Theory over pairs of nilmanifolds with fluxes or gerbes. This is achieved by a
rather straightforward application of a formalism we developed previously. This
formalism constructs the analogue of a Courant algebroid over the
correspondence space... | [
{
"created": "Fri, 30 Nov 2018 19:20:25 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jun 2019 10:44:18 GMT",
"version": "v2"
}
] | 2019-06-19 | [
[
"Deser",
"Andreas",
""
],
[
"Saemann",
"Christian",
""
]
] | We describe the global geometry, symmetries and tensors for Double Field Theory over pairs of nilmanifolds with fluxes or gerbes. This is achieved by a rather straightforward application of a formalism we developed previously. This formalism constructs the analogue of a Courant algebroid over the correspondence space o... | 12.703206 | 11.133892 | 14.67761 | 12.252967 | 13.667323 | 12.831108 | 12.852773 | 12.919973 | 12.127429 | 15.972079 | 12.114036 | 12.800831 | 13.075428 | 12.569186 | 11.899802 | 12.111665 | 11.889003 | 12.040466 | 12.260947 | 12.998633 | 12.033443 |
2007.11538 | Jean Felipe | L. C. T. Brito, J. C. C. Felipe, J. R. Nascimento, A. Yu Petrov and A.
P. Ba\^eta Scarpelli | Higher-order one-loop renormalization in the spinor sector of minimal LV
extended QED | 14 pages, 2 figures | Phys. Rev. D 102, 075017 (2020) | 10.1103/PhysRevD.102.075017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate contributions to the one-loop renormalization in the spinor
sector of the minimal Lorentz-violating extended QED in the second order in
Lorentz-breaking parameters. From the renormalizability viewpoint, we show that
the inclusion of some of the Lorentz-breaking terms in the model is linked to
the presenc... | [
{
"created": "Wed, 22 Jul 2020 16:58:15 GMT",
"version": "v1"
}
] | 2020-10-19 | [
[
"Brito",
"L. C. T.",
""
],
[
"Felipe",
"J. C. C.",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu",
""
],
[
"Scarpelli",
"A. P. Baêta",
""
]
] | We calculate contributions to the one-loop renormalization in the spinor sector of the minimal Lorentz-violating extended QED in the second order in Lorentz-breaking parameters. From the renormalizability viewpoint, we show that the inclusion of some of the Lorentz-breaking terms in the model is linked to the presence ... | 8.7995 | 7.999438 | 8.57865 | 7.420739 | 6.870038 | 7.634067 | 6.034264 | 7.450394 | 7.394805 | 8.232074 | 7.185404 | 7.62843 | 8.02963 | 7.91236 | 7.655735 | 7.242333 | 7.491033 | 7.739196 | 7.568896 | 7.885945 | 7.38654 |
1906.07192 | Toby Wiseman | Krai Cheamsawat, Gary Gibbons and Toby Wiseman | A new energy upper bound for AdS black holes inspired by free field
theory | 21 pages, 1 figure. v2: journal version, minor changes | null | 10.1088/1361-6382/ab56f3 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the toroidally compactified planar AdS-Schwarzschild solution to
4-dimensional gravity with negative cosmological constant. This has a flat
torus conformal boundary metric. We show that if the spatial part of the
boundary metric is deformed, keeping it static and the temperature and area
fixed, then assum... | [
{
"created": "Mon, 17 Jun 2019 18:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jan 2020 15:44:12 GMT",
"version": "v2"
}
] | 2020-01-10 | [
[
"Cheamsawat",
"Krai",
""
],
[
"Gibbons",
"Gary",
""
],
[
"Wiseman",
"Toby",
""
]
] | We consider the toroidally compactified planar AdS-Schwarzschild solution to 4-dimensional gravity with negative cosmological constant. This has a flat torus conformal boundary metric. We show that if the spatial part of the boundary metric is deformed, keeping it static and the temperature and area fixed, then assumin... | 8.26583 | 7.71386 | 9.028208 | 7.786521 | 8.380277 | 7.778633 | 8.255994 | 7.755547 | 7.927062 | 9.942646 | 7.948032 | 7.720128 | 8.112735 | 7.926501 | 7.930716 | 7.777406 | 7.972278 | 7.852476 | 7.94042 | 7.989351 | 7.762173 |
2203.15449 | Niccol\`o Cribiori | Niccol\`o Cribiori | De Sitter, gravitino mass and the swampland | 17 pages. Contribution to the proceedings for Corfu Summer Institute
2021 "School and Workshops on Elementary Particle Physics and Gravity"
(CORFU2021) 29 August - 9 October 2021 Corfu, Greece | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this contribution, we review a general argument showing that de Sitter
critical points of extended supergravity are in tension with the magnetic weak
gravity conjecture if the gravitino mass is vanishing. Motivated by this
assumption, we review then the gravitino conjecture, which states that the
limit of vanishin... | [
{
"created": "Tue, 29 Mar 2022 11:38:49 GMT",
"version": "v1"
}
] | 2022-03-30 | [
[
"Cribiori",
"Niccolò",
""
]
] | In this contribution, we review a general argument showing that de Sitter critical points of extended supergravity are in tension with the magnetic weak gravity conjecture if the gravitino mass is vanishing. Motivated by this assumption, we review then the gravitino conjecture, which states that the limit of vanishing ... | 11.538772 | 9.783023 | 10.935178 | 9.505364 | 9.337758 | 9.639612 | 9.596579 | 9.597121 | 9.341083 | 11.347977 | 9.492178 | 9.884053 | 10.397627 | 9.862382 | 10.611835 | 10.070301 | 10.238776 | 9.733145 | 10.208866 | 10.449287 | 9.986417 |
hep-th/9207058 | null | Sudhakar Panda and Shibaji Roy | Remarks on the Additional Symmetries and W-Constraints in the
Generalized KdV Hierarchy | 10 pages, Plain Tex | Phys.Lett. B296 (1992) 23-27 | 10.1016/0370-2693(92)90798-9 | IC-92-145 | hep-th | null | Additional symmetries of the $p$-reduced KP hierarchy are generated by the
Lax operator $L$ and another operator $M$, satisfying $res (M^n L^{m+n/p})$ = 0
for $1 \leq n \leq p-1$ and $m \geq -1$ with the condition that ${\partial L
\over {\partial t_{kp}}}$ = 0, $k$ = 1, 2,..... We show explicitly that the
generators... | [
{
"created": "Thu, 16 Jul 1992 14:16:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Panda",
"Sudhakar",
""
],
[
"Roy",
"Shibaji",
""
]
] | Additional symmetries of the $p$-reduced KP hierarchy are generated by the Lax operator $L$ and another operator $M$, satisfying $res (M^n L^{m+n/p})$ = 0 for $1 \leq n \leq p-1$ and $m \geq -1$ with the condition that ${\partial L \over {\partial t_{kp}}}$ = 0, $k$ = 1, 2,..... We show explicitly that the generators o... | 6.628611 | 6.093791 | 7.619738 | 6.351796 | 6.757664 | 6.013527 | 6.24151 | 6.092616 | 6.242825 | 7.151693 | 6.107101 | 6.173497 | 6.746737 | 6.17581 | 6.6899 | 6.438354 | 6.153382 | 6.192962 | 6.530235 | 6.645598 | 6.193347 |
hep-th/9302132 | Jisuke Kubo | T. Fujiwara, Y. Igarashi and J. Kubo | Unrecognizable Black Holes in Two Dimensions | 14 pages, KANAZAWA-93-01 | Phys.Lett. B316 (1993) 66-73 | 10.1016/0370-2693(93)90659-6 | null | hep-th | null | The classical 2D cosmological model of Callan, Giddings, Harvey and
Strominger possesses a global symmetry that is responsible for decoupling of
matter fields. The model is quantized on the basis of the extended phase space
method to allow an exhaustive, algebraic analysis to find potential anomalies.
Under a certain... | [
{
"created": "Fri, 26 Feb 1993 06:55:53 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Fujiwara",
"T.",
""
],
[
"Igarashi",
"Y.",
""
],
[
"Kubo",
"J.",
""
]
] | The classical 2D cosmological model of Callan, Giddings, Harvey and Strominger possesses a global symmetry that is responsible for decoupling of matter fields. The model is quantized on the basis of the extended phase space method to allow an exhaustive, algebraic analysis to find potential anomalies. Under a certain s... | 16.314764 | 13.802587 | 14.995747 | 13.596297 | 13.268508 | 14.599916 | 14.467946 | 14.910504 | 13.364317 | 16.258862 | 14.044351 | 13.222204 | 15.010758 | 14.501544 | 14.362805 | 14.035973 | 14.47885 | 14.364739 | 14.329463 | 15.666332 | 13.908885 |
2101.00024 | Georgios K. Karananas Dr. | Georgios K. Karananas, Alex Kehagias, John Taskas | Islands in Linear Dilaton Black Holes | Journal version---discussion extended, typos corrected, references
added | J. High Energ. Phys. 2021, 253 (2021) | 10.1007/JHEP03(2021)253 | LMU-ASC 67/20 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a novel four-dimensional black hole with planar horizon that
asymptotes to the linear dilaton background. The usual growth of its
entanglement entropy before Page's time is established. After that, emergent
islands modify to a large extent the entropy, which becomes finite and is
saturated by its Bekenstein... | [
{
"created": "Thu, 31 Dec 2020 19:00:05 GMT",
"version": "v1"
},
{
"created": "Sun, 28 Mar 2021 15:43:20 GMT",
"version": "v2"
}
] | 2021-03-30 | [
[
"Karananas",
"Georgios K.",
""
],
[
"Kehagias",
"Alex",
""
],
[
"Taskas",
"John",
""
]
] | We derive a novel four-dimensional black hole with planar horizon that asymptotes to the linear dilaton background. The usual growth of its entanglement entropy before Page's time is established. After that, emergent islands modify to a large extent the entropy, which becomes finite and is saturated by its Bekenstein-H... | 10.291557 | 10.041744 | 10.564617 | 9.62178 | 10.66296 | 9.602786 | 9.678228 | 9.886134 | 9.467336 | 11.184384 | 9.453742 | 9.600888 | 9.998747 | 9.870912 | 9.622273 | 9.762795 | 9.999936 | 9.818954 | 9.851312 | 10.370264 | 9.704396 |
2012.09286 | Paul K. Townsend | Igor Bandos, Kurt Lechner, Dmitri Sorokin and Paul K. Townsend | On p-form gauge theories and their conformal limits | 46 pp. Minor corrections plus Note Added with additional references
in v2 | null | 10.1007/JHEP03(2021)022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Relations between the various formulations of nonlinear p-form
electrodynamics with conformal-invariant weak-field and strong-field limits are
clarified, with a focus on duality invariant (2n-1)-form electrodynamics and
chiral 2n-form electrodynamics in Minkowski spacetime of dimension D=4n and
D=4n+2, respectively. ... | [
{
"created": "Wed, 16 Dec 2020 21:59:41 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Mar 2021 13:09:55 GMT",
"version": "v2"
}
] | 2021-03-17 | [
[
"Bandos",
"Igor",
""
],
[
"Lechner",
"Kurt",
""
],
[
"Sorokin",
"Dmitri",
""
],
[
"Townsend",
"Paul K.",
""
]
] | Relations between the various formulations of nonlinear p-form electrodynamics with conformal-invariant weak-field and strong-field limits are clarified, with a focus on duality invariant (2n-1)-form electrodynamics and chiral 2n-form electrodynamics in Minkowski spacetime of dimension D=4n and D=4n+2, respectively. We... | 7.15941 | 6.647122 | 7.231081 | 6.505936 | 6.92549 | 7.143982 | 6.971408 | 6.639 | 6.719861 | 7.722052 | 6.439329 | 7.158308 | 6.892025 | 6.599332 | 7.018835 | 7.03385 | 6.789932 | 6.751958 | 6.750733 | 7.071811 | 6.823921 |
hep-th/9802017 | Francesco Sannino | N. Kitazawa and F. Sannino (Yale Univ.) | Higgs Lagrangian from Gauge Theories | 4 pages, two-column RevTeX | null | null | YCTP-1-98 | hep-th hep-ph | null | We explore a novel way of deriving the effective Higgs Lagrangian from
strongly interacting vector-like gauge theories. We consider the N=1
supersymmetric extension of gauge theories and interpret the auxiliary field
associated with the low energy effective "meson" superfield as the Higgs field.
By introducing an exp... | [
{
"created": "Tue, 3 Feb 1998 23:06:02 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kitazawa",
"N.",
"",
"Yale Univ."
],
[
"Sannino",
"F.",
"",
"Yale Univ."
]
] | We explore a novel way of deriving the effective Higgs Lagrangian from strongly interacting vector-like gauge theories. We consider the N=1 supersymmetric extension of gauge theories and interpret the auxiliary field associated with the low energy effective "meson" superfield as the Higgs field. By introducing an expli... | 8.008329 | 8.283966 | 7.902075 | 7.714314 | 7.854495 | 7.313713 | 7.720603 | 7.655111 | 7.787471 | 8.536036 | 7.317289 | 7.871829 | 8.220128 | 8.102538 | 8.179881 | 8.244456 | 7.93013 | 8.159953 | 8.016539 | 8.364697 | 7.731441 |
hep-th/9612152 | Franco Ferrari | Franco Ferrari | Topologically Nontrivial Sectors of the Maxwell Field Theory on
Algebraic Curves | 24 pages, latex file + 3 ps figures | J.Geom.Phys.25:91-103,1998 | 10.1016/S0393-0440(97)00023-5 | preprint UTF 379, PAR-LPTHE 96-30 | hep-th | null | In this paper the Maxwell field theory is considered on the $Z_n$ symmetric
algebraic curves. As a first result, a large family of nondegenerate metrics is
derived for general curves. This allows to treat many differential equations
arising in quantum mechanics and field theory on Riemann surfaces as
differential equ... | [
{
"created": "Fri, 13 Dec 1996 12:25:05 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Ferrari",
"Franco",
""
]
] | In this paper the Maxwell field theory is considered on the $Z_n$ symmetric algebraic curves. As a first result, a large family of nondegenerate metrics is derived for general curves. This allows to treat many differential equations arising in quantum mechanics and field theory on Riemann surfaces as differential equat... | 10.147277 | 9.98118 | 10.16256 | 10.074647 | 10.808303 | 10.398576 | 10.600636 | 9.588734 | 10.343794 | 10.867112 | 9.746488 | 9.733179 | 9.305138 | 9.585176 | 9.679278 | 9.541303 | 9.552747 | 9.989582 | 9.59821 | 9.698014 | 9.71321 |
hep-th/0401011 | Shoichi Ichinose | Shoichi Ichinose and Akihiro Murayama | Quantum Dynamics of a Bulk-Boundary System | 57 pages,10 figures, final version 2 | Nucl.Phys. B710 (2005) 255-308 | 10.1016/j.nuclphysb.2004.12.023 | US-03-08 | hep-th | null | The quantum dynamics of a bulk-boundary theory is closely examined by the use
of the background field method. As an example we take the Mirabelli-Peskin
model, which is composed of 5D super Yang-Mills (bulk) and 4D Wess-Zumino
(boundary). Singular interaction terms play an important role of canceling the
divergences ... | [
{
"created": "Sun, 4 Jan 2004 06:11:40 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Jul 2004 05:56:01 GMT",
"version": "v2"
},
{
"created": "Sat, 30 Oct 2004 03:49:36 GMT",
"version": "v3"
},
{
"created": "Fri, 26 Nov 2004 02:12:23 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Ichinose",
"Shoichi",
""
],
[
"Murayama",
"Akihiro",
""
]
] | The quantum dynamics of a bulk-boundary theory is closely examined by the use of the background field method. As an example we take the Mirabelli-Peskin model, which is composed of 5D super Yang-Mills (bulk) and 4D Wess-Zumino (boundary). Singular interaction terms play an important role of canceling the divergences co... | 12.187752 | 12.571312 | 12.443647 | 11.781484 | 12.189912 | 12.165236 | 11.449397 | 11.206729 | 11.624586 | 13.838622 | 11.411005 | 12.0775 | 12.063045 | 12.161976 | 12.183055 | 12.090621 | 12.112932 | 11.900065 | 12.035892 | 12.273085 | 11.905154 |
1706.07025 | Frans Klinkhamer | K.J.B. Ghosh, F.R. Klinkhamer | Anomalous Lorentz and CPT violation from a local Chern-Simons-like term
in the effective gauge-field action | 48 pages, v7: published version | Nucl. Phys. B 926 (2018) 335-369 | 10.1016/j.nuclphysb.2017.11.010 | KA-TP-25-2017 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider four-dimensional chiral gauge theories defined over a spacetime
manifold with topology $\mathbb{R}^3 \times S^1$ and periodic boundary
conditions over the compact dimension. The effective gauge-field action is
calculated for Abelian $U(1)$ gauge fields $A_{\mu}(x)$ which depend on all
four spacetime coord... | [
{
"created": "Wed, 21 Jun 2017 17:35:45 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Jun 2017 17:22:47 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Jun 2017 17:29:31 GMT",
"version": "v3"
},
{
"created": "Thu, 20 Jul 2017 16:58:36 GMT",
"version": "v4"
},
{
"c... | 2018-03-14 | [
[
"Ghosh",
"K. J. B.",
""
],
[
"Klinkhamer",
"F. R.",
""
]
] | We consider four-dimensional chiral gauge theories defined over a spacetime manifold with topology $\mathbb{R}^3 \times S^1$ and periodic boundary conditions over the compact dimension. The effective gauge-field action is calculated for Abelian $U(1)$ gauge fields $A_{\mu}(x)$ which depend on all four spacetime coordin... | 4.853426 | 4.766945 | 5.048427 | 4.584968 | 4.822588 | 4.87223 | 4.652647 | 4.8283 | 4.710665 | 5.548901 | 4.767501 | 4.689558 | 4.621262 | 4.590293 | 4.630864 | 4.732734 | 4.593254 | 4.548661 | 4.700087 | 4.670106 | 4.525244 |
hep-th/9804145 | Sachindeo Vaidya | A. P. Balachandran, G. Bimonte, T. R. Govindarajan, K. S. Gupta, V.
John and S. Vaidya | Current Oscillations, Interacting Hall Discs and Boundary CFTs | 32 pages, LateX. Uses amstex, amssymb. Typos corrected. To appear in
Int. J. Mod. Phys. A | Int.J.Mod.Phys. A14 (1999) 1061-1086 | 10.1142/S0217751X99000531 | SU-4240-675, DSF-9/98, IMSc 98/03/10, SINP-TNP/98-01, IC/98/37 | hep-th cond-mat.mes-hall | null | In this paper, we discuss the behavior of conformal field theories
interacting at a single point. The edge states of the quantum Hall effect (QHE)
system give rise to a particular representation of a chiral Kac-Moody current
algebra. We show that in the case of QHE systems interacting at one point we
obtain a ``twist... | [
{
"created": "Tue, 21 Apr 1998 22:51:32 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Jul 1998 14:13:47 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Balachandran",
"A. P.",
""
],
[
"Bimonte",
"G.",
""
],
[
"Govindarajan",
"T. R.",
""
],
[
"Gupta",
"K. S.",
""
],
[
"John",
"V.",
""
],
[
"Vaidya",
"S.",
""
]
] | In this paper, we discuss the behavior of conformal field theories interacting at a single point. The edge states of the quantum Hall effect (QHE) system give rise to a particular representation of a chiral Kac-Moody current algebra. We show that in the case of QHE systems interacting at one point we obtain a ``twisted... | 8.024101 | 8.10432 | 8.532967 | 8.148106 | 8.613981 | 8.254117 | 8.772087 | 8.347074 | 7.996583 | 9.203807 | 7.990683 | 8.154756 | 8.313612 | 7.944988 | 8.072229 | 8.002889 | 7.942298 | 7.960515 | 8.044474 | 8.528606 | 7.910254 |
1812.05428 | A. Yu. Petrov | M. B. Cruz, E. R. Bezerra de Mello, and A. Yu. Petrov | Fermionic Casimir effect in a field theory model with Lorentz symmetry
violation | Version accepted for publication in PRD, metadata corrected | Phys. Rev. D 99, 085012 (2019) | 10.1103/PhysRevD.99.085012 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we evaluate the Casimir energy and pressure for a massive
fermionic field confined in the region between two parallel plates. In order to
implement this confinement we impose the standard MIT bag boundary on the
plates for the fermionic field. In this paper we consider a quantum field
theory model with... | [
{
"created": "Thu, 13 Dec 2018 13:52:34 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Apr 2019 16:16:45 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Apr 2019 12:04:56 GMT",
"version": "v3"
}
] | 2019-04-29 | [
[
"Cruz",
"M. B.",
""
],
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Petrov",
"A. Yu.",
""
]
] | In this paper, we evaluate the Casimir energy and pressure for a massive fermionic field confined in the region between two parallel plates. In order to implement this confinement we impose the standard MIT bag boundary on the plates for the fermionic field. In this paper we consider a quantum field theory model with a... | 7.703452 | 5.749588 | 7.78196 | 6.415474 | 6.586185 | 5.83655 | 5.824978 | 5.952714 | 6.709346 | 8.375993 | 6.529846 | 6.288366 | 7.290784 | 6.481015 | 6.649752 | 6.729669 | 6.41555 | 6.73411 | 6.660741 | 7.68948 | 6.997218 |
1406.2991 | H. Casini | Horacio Casini, Marina Huerta | Entanglement entropy for a Maxwell field: Numerical calculation on a two
dimensional lattice | 27 pages, 15 figures | null | 10.1103/PhysRevD.90.105013 | null | hep-th hep-lat quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study entanglement entropy (EE) for a Maxwell field in 2+1 dimensions. We
do numerical calculations in two dimensional lattices. This gives a concrete
example of the general results of our recent work on entropy for lattice gauge
fields using an algebraic approach. To evaluate the entropies we extend the
standard ... | [
{
"created": "Wed, 11 Jun 2014 18:41:14 GMT",
"version": "v1"
}
] | 2015-06-19 | [
[
"Casini",
"Horacio",
""
],
[
"Huerta",
"Marina",
""
]
] | We study entanglement entropy (EE) for a Maxwell field in 2+1 dimensions. We do numerical calculations in two dimensional lattices. This gives a concrete example of the general results of our recent work on entropy for lattice gauge fields using an algebraic approach. To evaluate the entropies we extend the standard ca... | 12.278746 | 12.736665 | 12.256043 | 11.57758 | 12.224301 | 11.657815 | 12.389231 | 11.884318 | 11.756016 | 13.989549 | 11.581705 | 11.804909 | 12.07037 | 11.463505 | 12.017591 | 11.328271 | 11.865293 | 11.754709 | 11.856823 | 12.128103 | 11.899314 |
2403.15531 | Francesco Giacosa | Leonardo Tinti, Arthur Vereijken, Shahriyar Jafarzade, Francesco
Giacosa | Scalar field with a time-independent classical source, not trivial after
all: from vacuum decay to scattering | 33 pages, 3 figures | null | null | null | hep-th hep-ph nucl-th quant-ph | http://creativecommons.org/licenses/by/4.0/ | Historically it has been believed that a time-independent classical source
has no effect on the scattering of relativistic uncharged field, in contrast
with single particle quantum mechanics. In this work we show that the dynamics
is not trivial. We solve exactly for the scattering amplitudes and find that a
key ingr... | [
{
"created": "Fri, 22 Mar 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-03-26 | [
[
"Tinti",
"Leonardo",
""
],
[
"Vereijken",
"Arthur",
""
],
[
"Jafarzade",
"Shahriyar",
""
],
[
"Giacosa",
"Francesco",
""
]
] | Historically it has been believed that a time-independent classical source has no effect on the scattering of relativistic uncharged field, in contrast with single particle quantum mechanics. In this work we show that the dynamics is not trivial. We solve exactly for the scattering amplitudes and find that a key ingred... | 13.272034 | 13.59223 | 12.953918 | 12.348986 | 14.22458 | 13.385714 | 13.390568 | 13.79064 | 12.441482 | 14.238851 | 12.600035 | 12.18058 | 12.60354 | 12.412324 | 12.90605 | 12.514197 | 12.843562 | 12.117279 | 12.147061 | 12.601534 | 12.604136 |
1404.7224 | Daniel S. Freed | Daniel S. Freed | Anomalies and Invertible Field Theories | 21 pages, based talk at String-Math 2013; small corrections in v2 | null | null | null | hep-th math-ph math.AT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a modern geometric viewpoint on anomalies in quantum field theory and
illustrate it in a 1-dimensional theory: supersymmetric quantum mechanics. This
is background for the resolution of worldsheet anomalies in orientifold
superstring theory.
| [
{
"created": "Tue, 29 Apr 2014 03:35:12 GMT",
"version": "v1"
},
{
"created": "Sat, 21 Jun 2014 02:48:05 GMT",
"version": "v2"
}
] | 2014-06-24 | [
[
"Freed",
"Daniel S.",
""
]
] | We give a modern geometric viewpoint on anomalies in quantum field theory and illustrate it in a 1-dimensional theory: supersymmetric quantum mechanics. This is background for the resolution of worldsheet anomalies in orientifold superstring theory. | 24.2911 | 18.056837 | 21.057167 | 19.152323 | 18.676128 | 18.338673 | 18.374132 | 17.834631 | 19.735815 | 25.07601 | 18.964622 | 20.169687 | 21.796423 | 19.197369 | 19.265369 | 20.52887 | 19.684128 | 20.093674 | 20.057882 | 22.411562 | 20.566587 |
1806.09146 | Tianshu Liu | Thomas Creutzig, Shashank Kanade, Tianshu Liu and David Ridout | Cosets, characters and fusion for admissible-level $\mathfrak{osp}(1
\vert 2)$ minimal models | 26 pages, minor revision | null | 10.1016/j.nuclphysb.2018.10.022 | null | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the minimal models associated to $\mathfrak{osp}(1 \vert 2)$,
otherwise known as the fractional-level Wess-Zumino-Witten models of
$\mathfrak{osp}(1 \vert 2)$. Since these minimal models are extensions of the
tensor product of certain Virasoro and $\mathfrak{sl}_2$ minimal models, we can
induce the known str... | [
{
"created": "Sun, 24 Jun 2018 13:51:34 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Nov 2018 06:33:27 GMT",
"version": "v2"
}
] | 2018-12-05 | [
[
"Creutzig",
"Thomas",
""
],
[
"Kanade",
"Shashank",
""
],
[
"Liu",
"Tianshu",
""
],
[
"Ridout",
"David",
""
]
] | We study the minimal models associated to $\mathfrak{osp}(1 \vert 2)$, otherwise known as the fractional-level Wess-Zumino-Witten models of $\mathfrak{osp}(1 \vert 2)$. Since these minimal models are extensions of the tensor product of certain Virasoro and $\mathfrak{sl}_2$ minimal models, we can induce the known struc... | 5.206327 | 5.38336 | 7.769449 | 5.233054 | 5.318791 | 5.743834 | 5.423177 | 5.360832 | 4.969779 | 6.761163 | 5.28147 | 5.356065 | 6.410656 | 5.147863 | 5.315915 | 5.328102 | 5.052774 | 5.310145 | 5.045149 | 5.996012 | 5.131376 |
hep-th/0301103 | Sergei Khlebnikov | S. Khlebnikov | A dual description of decoherence in de Sitter space | 11 pages, latex; a reference added | JHEP 0303:059,2003 | 10.1088/1126-6708/2003/03/059 | null | hep-th gr-qc | null | Decoherence associated with super-Hubble modes in de Sitter space may have a
dual description, in which it is attributed to interaction of sub-Hubble modes
with an ``environment'' residing just inside the observer's horizon. We present
a version of such description, together with some consistency checks, which it
is ... | [
{
"created": "Wed, 15 Jan 2003 19:45:44 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Jan 2003 19:28:41 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Khlebnikov",
"S.",
""
]
] | Decoherence associated with super-Hubble modes in de Sitter space may have a dual description, in which it is attributed to interaction of sub-Hubble modes with an ``environment'' residing just inside the observer's horizon. We present a version of such description, together with some consistency checks, which it is sh... | 17.739418 | 12.253972 | 14.612741 | 13.204473 | 13.117156 | 14.735621 | 13.385991 | 12.645346 | 12.932332 | 16.962345 | 14.794995 | 13.142995 | 13.428669 | 12.775311 | 12.311782 | 12.672734 | 13.120483 | 12.618577 | 12.604331 | 13.091155 | 13.536476 |
1105.5848 | E. T. Tomboulis | E. T. Tomboulis | General Relativity as the effective theory of GL(4,R) spontaneous
symmetry breaking | 15 pages | Phys. Rev. D 84, 084018 (2011) | 10.1103/PhysRevD.84.084018 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We assume a GL(4,R) space-time symmetry which is spontaneously broken to
SO(3,1). We carry out the coset construction of the effective theory for the
non-linearly realized broken symmetry in terms of the Goldstone fields and
matter fields transforming linearly under the unbroken Lorentz subgroup. We
then identify fun... | [
{
"created": "Mon, 30 May 2011 02:21:59 GMT",
"version": "v1"
}
] | 2013-05-29 | [
[
"Tomboulis",
"E. T.",
""
]
] | We assume a GL(4,R) space-time symmetry which is spontaneously broken to SO(3,1). We carry out the coset construction of the effective theory for the non-linearly realized broken symmetry in terms of the Goldstone fields and matter fields transforming linearly under the unbroken Lorentz subgroup. We then identify funct... | 7.629556 | 7.635602 | 7.443379 | 7.036441 | 7.506863 | 7.412624 | 7.426679 | 7.13671 | 7.130547 | 8.007431 | 7.465683 | 7.290219 | 7.395029 | 7.270966 | 7.205758 | 7.284999 | 7.227943 | 7.700192 | 7.250413 | 7.549417 | 7.214489 |
1111.3040 | Daniel Green | Daniel Baumann and Daniel Green | A Field Range Bound for General Single-Field Inflation | 16 pages | null | 10.1088/1475-7516/2012/05/017 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the consequences of a detection of primordial tensor fluctuations
for general single-field models of inflation. Using the effective theory of
inflation, we propose a generalization of the Lyth bound. Our bound applies to
all single-field models with two-derivative kinetic terms for the scalar
fluctuations ... | [
{
"created": "Sun, 13 Nov 2011 18:00:25 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Baumann",
"Daniel",
""
],
[
"Green",
"Daniel",
""
]
] | We explore the consequences of a detection of primordial tensor fluctuations for general single-field models of inflation. Using the effective theory of inflation, we propose a generalization of the Lyth bound. Our bound applies to all single-field models with two-derivative kinetic terms for the scalar fluctuations an... | 8.816555 | 8.546111 | 9.072499 | 8.420335 | 8.793339 | 8.705815 | 8.379581 | 8.878911 | 7.661691 | 9.617285 | 8.487973 | 8.851883 | 8.944876 | 8.585062 | 8.602256 | 8.225607 | 8.444468 | 8.674286 | 8.683893 | 8.939428 | 8.507352 |
0905.3047 | Carlos A. R. Herdeiro | Jai Grover, Jan B. Gutowski, Carlos A. R. Herdeiro, Patrick Meessen,
Alberto Palomo-Lozano and Wafic A. Sabra | Gauduchon-Tod structures, Sim holonomy and De Sitter supergravity | 1+21 pages, no figures; v2 minor changes, typos corrected, matches
published version in JHEP | JHEP 0907:069,2009 | 10.1088/1126-6708/2009/07/069 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Solutions of five-dimensional De Sitter supergravity admitting Killing
spinors are considered, using spinorial geometry techniques. It is shown that
the "null" solutions are defined in terms of a one parameter family of
3-dimensional constrained Einstein-Weyl spaces called Gauduchon-Tod structures.
They admit a geode... | [
{
"created": "Tue, 19 May 2009 09:10:54 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Aug 2009 16:08:15 GMT",
"version": "v2"
}
] | 2009-08-26 | [
[
"Grover",
"Jai",
""
],
[
"Gutowski",
"Jan B.",
""
],
[
"Herdeiro",
"Carlos A. R.",
""
],
[
"Meessen",
"Patrick",
""
],
[
"Palomo-Lozano",
"Alberto",
""
],
[
"Sabra",
"Wafic A.",
""
]
] | Solutions of five-dimensional De Sitter supergravity admitting Killing spinors are considered, using spinorial geometry techniques. It is shown that the "null" solutions are defined in terms of a one parameter family of 3-dimensional constrained Einstein-Weyl spaces called Gauduchon-Tod structures. They admit a geodesi... | 8.153563 | 8.118491 | 8.523081 | 7.422742 | 8.23872 | 8.199434 | 8.985471 | 7.043623 | 7.74869 | 9.305022 | 7.858844 | 8.145282 | 8.155427 | 7.616752 | 7.796474 | 8.122985 | 7.812251 | 7.641021 | 8.008386 | 7.889148 | 8.052669 |
1406.4142 | David Berenstein | David Berenstein, Alexandra Miller | Conformal perturbation theory, dimensional regularization and AdS/CFT | 18 pages | Phys. Rev. D 90, 086011 (2014) | 10.1103/PhysRevD.90.086011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study relevant deformations of conformal field theory on a cylinder using
conformal perturbation theory, and in particular the one point function of the
deformation operator and the energy in a system after a quench. We do the one
point function calculation in both AdS and the conformal field theory and we
show th... | [
{
"created": "Mon, 16 Jun 2014 20:00:09 GMT",
"version": "v1"
}
] | 2014-11-05 | [
[
"Berenstein",
"David",
""
],
[
"Miller",
"Alexandra",
""
]
] | We study relevant deformations of conformal field theory on a cylinder using conformal perturbation theory, and in particular the one point function of the deformation operator and the energy in a system after a quench. We do the one point function calculation in both AdS and the conformal field theory and we show that... | 11.258797 | 10.523527 | 13.803801 | 10.052611 | 10.888856 | 10.75678 | 9.655319 | 10.53414 | 9.726352 | 13.011857 | 10.421357 | 10.27638 | 11.699121 | 10.555563 | 10.66425 | 10.481057 | 10.144198 | 10.319642 | 10.346117 | 11.823589 | 10.210443 |
1212.6173 | Ronald Reid-Edwards | L. J. Mason and R. A. Reid-Edwards | The supersymmetric Penrose transform in six dimensions | 20 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a supersymmetric extension to the six-dimensional Penrose transform
and give an integral formula for the on-shell (0, 2) supermultiplet. The
relationship between super fields on space-time and twistor space is clarified
and the space-time superfield constraint equations are derived from the
geometry of supert... | [
{
"created": "Wed, 26 Dec 2012 13:15:14 GMT",
"version": "v1"
}
] | 2012-12-27 | [
[
"Mason",
"L. J.",
""
],
[
"Reid-Edwards",
"R. A.",
""
]
] | We give a supersymmetric extension to the six-dimensional Penrose transform and give an integral formula for the on-shell (0, 2) supermultiplet. The relationship between super fields on space-time and twistor space is clarified and the space-time superfield constraint equations are derived from the geometry of supertwi... | 10.502643 | 8.920053 | 11.713386 | 9.024573 | 8.992375 | 8.747252 | 8.702254 | 8.763379 | 8.758514 | 12.45228 | 8.758713 | 8.770393 | 11.113615 | 8.965366 | 9.198763 | 9.181084 | 9.457042 | 9.276608 | 9.315527 | 10.956873 | 9.167762 |
1007.0195 | David Skinner | David Skinner | A Direct Proof of BCFW Recursion for Twistor-Strings | 23 pages, 5 figures | JHEP 1101:072,2011 | 10.1007/JHEP01(2011)072 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper gives a direct proof that the leading trace part of the genus zero
twistor-string path integral obeys the BCFW recursion relation. This is the
first complete proof that the twistor-string correctly computes all tree
amplitudes in maximally supersymmetric Yang-Mills theory. The recursion has a
beautiful geo... | [
{
"created": "Thu, 1 Jul 2010 15:37:36 GMT",
"version": "v1"
}
] | 2011-03-07 | [
[
"Skinner",
"David",
""
]
] | This paper gives a direct proof that the leading trace part of the genus zero twistor-string path integral obeys the BCFW recursion relation. This is the first complete proof that the twistor-string correctly computes all tree amplitudes in maximally supersymmetric Yang-Mills theory. The recursion has a beautiful geome... | 6.964118 | 7.190251 | 7.457688 | 6.432089 | 6.710047 | 7.139006 | 7.217704 | 6.457292 | 6.491611 | 7.741163 | 6.689281 | 6.547238 | 7.070522 | 6.431387 | 6.606436 | 6.322294 | 6.746382 | 6.548603 | 6.439332 | 6.934475 | 6.373143 |
0911.4709 | Wei Chao | Wei Chao | Horava-Lifshitz Type Quantum Field Theory and Hierarchy Problem | 8 pages, 2 figures | Commun. Theor. Phys. 65(2016) 743-746 | 10.1088/0253-6102/65/6/743 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Lifshitz type extension of the standard model (SM) at UV, with
dynamical critical exponent z=3. One loop radiative corrections to the Higgs
mass in such a model is calculated. Our result shows that, the Hierarchy
problem, which has initiated many excellent extension of the minimal SM, can be
weakened in ... | [
{
"created": "Tue, 24 Nov 2009 20:55:28 GMT",
"version": "v1"
},
{
"created": "Fri, 27 May 2016 23:55:56 GMT",
"version": "v2"
},
{
"created": "Fri, 24 Jun 2016 18:41:57 GMT",
"version": "v3"
}
] | 2016-06-27 | [
[
"Chao",
"Wei",
""
]
] | We study the Lifshitz type extension of the standard model (SM) at UV, with dynamical critical exponent z=3. One loop radiative corrections to the Higgs mass in such a model is calculated. Our result shows that, the Hierarchy problem, which has initiated many excellent extension of the minimal SM, can be weakened in th... | 12.413225 | 11.425288 | 10.854171 | 10.652816 | 10.266347 | 11.318948 | 10.81549 | 10.339374 | 9.695636 | 11.400687 | 10.519897 | 10.367432 | 11.560208 | 11.178051 | 11.003578 | 11.049611 | 10.63408 | 11.038892 | 10.880596 | 10.843385 | 11.184917 |
hep-th/9210100 | null | Krzysztof Gaw\c{e}dzki | Quantum Group Symmetries in Conformal Field Theory | 13 pages, Talk given at Oji Seminar on Quantum Analysis, Kyoto, June
25-29, 1992 | null | null | IHES/P/92/80 | hep-th | null | Quantum groups play the role of hidden symmetries of some two-dimensional
field theories. We discuss how they appear in this role in the
Wess-Zumino-Witten model of conformal field theory.
| [
{
"created": "Mon, 19 Oct 1992 10:24:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gawȩdzki",
"Krzysztof",
""
]
] | Quantum groups play the role of hidden symmetries of some two-dimensional field theories. We discuss how they appear in this role in the Wess-Zumino-Witten model of conformal field theory. | 9.560154 | 5.579331 | 6.765316 | 5.631749 | 5.574864 | 5.133645 | 5.069007 | 5.754356 | 5.241658 | 5.856383 | 5.329562 | 5.796277 | 6.753879 | 5.879818 | 5.785871 | 5.959083 | 5.734153 | 6.04541 | 5.864619 | 6.414658 | 5.807346 |
hep-th/0611114 | David Dudal | D. Dudal, M.A.L. Capri, J.A. Gracey, V.E.R. Lemes, R.F. Sobreiro, S.P.
Sorella, H. Verschelde | Dimension two gluon condensates in a variety of gauges and a gauge
invariant Yang-Mills action with a mass | 4 pages. espcrc2.sty is used. Talk given at "13th International
Conference In QCD (QCD 06), 3-7 Jul 2006, Montpellier, France" | Nucl.Phys.Proc.Suppl.174:201-204,2007 | 10.1016/j.nuclphysbps.2007.08.124 | LTH-727 | hep-th | null | We give a short overview of our work concerning the dimension two operator
A^2 in the Landau gauge and its generalizations to other gauges. We conclude by
discussing recent work that leads to a renormalizable gauge invariant action
containing a mass parameter, based on the operator F 1/D^2 F.
| [
{
"created": "Fri, 10 Nov 2006 08:35:47 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Dudal",
"D.",
""
],
[
"Capri",
"M. A. L.",
""
],
[
"Gracey",
"J. A.",
""
],
[
"Lemes",
"V. E. R.",
""
],
[
"Sobreiro",
"R. F.",
""
],
[
"Sorella",
"S. P.",
""
],
[
"Verschelde",
"H.",
""
]
] | We give a short overview of our work concerning the dimension two operator A^2 in the Landau gauge and its generalizations to other gauges. We conclude by discussing recent work that leads to a renormalizable gauge invariant action containing a mass parameter, based on the operator F 1/D^2 F. | 19.704609 | 10.553771 | 15.810295 | 14.538693 | 13.559193 | 12.331509 | 11.85114 | 12.096783 | 12.175851 | 15.875403 | 14.116645 | 15.099899 | 16.080179 | 14.96534 | 14.69017 | 14.843212 | 14.67762 | 14.324729 | 15.028535 | 16.528181 | 15.300164 |
hep-th/0011167 | Chris Pope | M. Cvetic, M.J. Duff, James T. Liu, H. Lu, C.N. Pope and K.S. Stelle | Randall-Sundrum Brane Tensions | Latex, 21 pages, 2 figures | Nucl.Phys.B605:141-158,2001 | 10.1016/S0550-3213(01)00205-X | null | hep-th | null | We show that the singular sources in the energy-momentum tensor for the
Randall-Sundrum brane world, viewed as a solution of type IIB supergravity, are
composed of two elements. One of these is a D3-brane source with tension
opposite in sign to the RS tension in five dimensions; the other arises from
patching two reg... | [
{
"created": "Mon, 20 Nov 2000 23:13:33 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Cvetic",
"M.",
""
],
[
"Duff",
"M. J.",
""
],
[
"Liu",
"James T.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Stelle",
"K. S.",
""
]
] | We show that the singular sources in the energy-momentum tensor for the Randall-Sundrum brane world, viewed as a solution of type IIB supergravity, are composed of two elements. One of these is a D3-brane source with tension opposite in sign to the RS tension in five dimensions; the other arises from patching two regio... | 10.012289 | 8.856846 | 10.343856 | 9.013985 | 9.350124 | 9.585794 | 9.182843 | 9.527482 | 9.649446 | 11.739566 | 9.193547 | 9.927379 | 9.775182 | 9.854708 | 9.493617 | 9.508894 | 9.704974 | 9.351072 | 10.287261 | 9.929439 | 9.73726 |
1312.2972 | Daniele Marmiroli | Daniele Marmiroli (NORDITA) | Notes on BPS Wilson Loops and the Cusp Anomalous Dimension in ABJM
theory | 31 pages | null | null | NORDITA preprint number 2013-100 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a new purely bosonic, $\frac{1}{6}$ BPS Wilson loop for ABJM
theory on $S^3$ that couples scalar fields to a latitude at an angle $\theta$
on $S^2\in\mathbb{C}P^3$. Through localization of this operator, we relate the
expansion of the cusp anomalous dimension at small cusp angles to the
logarithmic deriv... | [
{
"created": "Tue, 10 Dec 2013 21:32:17 GMT",
"version": "v1"
}
] | 2013-12-12 | [
[
"Marmiroli",
"Daniele",
"",
"NORDITA"
]
] | We introduce a new purely bosonic, $\frac{1}{6}$ BPS Wilson loop for ABJM theory on $S^3$ that couples scalar fields to a latitude at an angle $\theta$ on $S^2\in\mathbb{C}P^3$. Through localization of this operator, we relate the expansion of the cusp anomalous dimension at small cusp angles to the logarithmic derivat... | 8.452946 | 8.151975 | 8.939156 | 8.08111 | 8.098116 | 9.207349 | 8.146123 | 8.293856 | 8.179201 | 10.154012 | 7.766364 | 7.940019 | 8.739809 | 8.130448 | 7.836945 | 7.99393 | 8.026185 | 7.939949 | 7.831093 | 8.724674 | 7.823229 |
0712.2118 | Mohammad Sami | Mofazzal Azam, M. Sami, C. S. Unnikrishnan, T. Shiromizu | Proposal for an experiment to search for Randall-Sundrum type
corrections to Newton's law of gravitation | 4 pages and 5 figures, figures improved, minor clarifications and few
references added, final version to appear in PRD (rapid communications) | Phys.Rev.D77:101101,2008 | 10.1103/PhysRevD.77.101101 | null | hep-th astro-ph gr-qc hep-ph | null | String theory, as well as the string inspired brane-world models such as the
Randall-Sundrum (RS) one, suggest a modification of Newton's law of gravitation
at small distance scales. Search for modifications of standard gravity is an
active field of research in this context. It is well known that short range
correcti... | [
{
"created": "Thu, 13 Dec 2007 10:13:19 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Apr 2008 07:18:41 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Azam",
"Mofazzal",
""
],
[
"Sami",
"M.",
""
],
[
"Unnikrishnan",
"C. S.",
""
],
[
"Shiromizu",
"T.",
""
]
] | String theory, as well as the string inspired brane-world models such as the Randall-Sundrum (RS) one, suggest a modification of Newton's law of gravitation at small distance scales. Search for modifications of standard gravity is an active field of research in this context. It is well known that short range correction... | 10.212089 | 11.473887 | 10.047827 | 9.719214 | 10.266883 | 9.894083 | 11.900673 | 10.296419 | 10.035909 | 11.619159 | 10.379172 | 10.306704 | 9.708011 | 9.757194 | 9.934785 | 10.245626 | 10.139263 | 9.977421 | 9.78908 | 10.143594 | 9.953358 |
1802.08107 | Tom\'a\v{s} Brauner | Mark P. Bogers and Tomas Brauner | Geometry of Multi-Flavor Galileon-Like Theories | 8 pages; v2: substantially rewritten and extended, matches version to
appear in PRL | Phys. Rev. Lett. 121, 171602 (2018) | 10.1103/PhysRevLett.121.171602 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use Lie-algebraic arguments to classify Lorentz-invariant theories of
massless interacting scalars that feature coordinate-dependent redundant
symmetries of the Galileon type. We show that such theories are determined, up
to a set of low-energy effective couplings, by specifying an affine
representation of the Lie... | [
{
"created": "Thu, 22 Feb 2018 15:43:02 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Oct 2018 08:23:43 GMT",
"version": "v2"
}
] | 2018-10-31 | [
[
"Bogers",
"Mark P.",
""
],
[
"Brauner",
"Tomas",
""
]
] | We use Lie-algebraic arguments to classify Lorentz-invariant theories of massless interacting scalars that feature coordinate-dependent redundant symmetries of the Galileon type. We show that such theories are determined, up to a set of low-energy effective couplings, by specifying an affine representation of the Lie a... | 12.780432 | 12.242323 | 13.114122 | 11.136353 | 11.706779 | 11.14505 | 11.972303 | 12.522267 | 12.417229 | 14.97773 | 11.015417 | 11.737872 | 12.180116 | 11.752616 | 12.260088 | 12.622973 | 11.53593 | 12.60743 | 11.876353 | 12.320551 | 11.672581 |
hep-th/0002060 | Yan-Gang Miao | Yan-Gang Miao, R. Manvelyan and H.J.W. Mueller-Kirsten | Self-Duality beyond Chiral p-Form Actions | Latex, 13 pages, no figures, minor typos corrected | Phys.Lett. B482 (2000) 264 | 10.1016/S0370-2693(00)00502-5 | null | hep-th | null | The self-duality of chiral p-forms was originally investigated by Pasti,
Sorokin and Tonin in a manifestly Lorentz covariant action with non-polynomial
auxiliary fields. The investigation was then extended to other chiral p-form
actions. In this paper we point out that the self-duality appears in a wider
context of t... | [
{
"created": "Tue, 8 Feb 2000 10:34:44 GMT",
"version": "v1"
},
{
"created": "Tue, 30 May 2000 15:24:56 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Miao",
"Yan-Gang",
""
],
[
"Manvelyan",
"R.",
""
],
[
"Mueller-Kirsten",
"H. J. W.",
""
]
] | The self-duality of chiral p-forms was originally investigated by Pasti, Sorokin and Tonin in a manifestly Lorentz covariant action with non-polynomial auxiliary fields. The investigation was then extended to other chiral p-form actions. In this paper we point out that the self-duality appears in a wider context of the... | 2.45893 | 6.219064 | 8.624186 | 6.444974 | 6.04485 | 6.448329 | 6.277125 | 6.077017 | 6.14501 | 8.501637 | 6.279947 | 5.638986 | 6.581296 | 6.204499 | 6.146132 | 5.831149 | 6.165674 | 5.810705 | 6.239686 | 6.807567 | 6.077592 |
1510.08055 | Andrea Puhm | Iosif Bena, Lucien Heurtier and Andrea Puhm | AdS_3: the NHEK generation | 25 pages | null | null | IPhT-T15/184,CPHT-RR043.1015,ULB-TH/15-20 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was argued in arXiv:1203.4227 that the five-dimensional near-horizon
extremal Kerr (NHEK) geometry can be embedded in String Theory as the infrared
region of an infinite family of non-supersymmetric geometries that have D1, D5,
momentum and KK monopole charges. We show that there exists a method to embed
these geo... | [
{
"created": "Tue, 27 Oct 2015 20:04:44 GMT",
"version": "v1"
}
] | 2015-10-29 | [
[
"Bena",
"Iosif",
""
],
[
"Heurtier",
"Lucien",
""
],
[
"Puhm",
"Andrea",
""
]
] | It was argued in arXiv:1203.4227 that the five-dimensional near-horizon extremal Kerr (NHEK) geometry can be embedded in String Theory as the infrared region of an infinite family of non-supersymmetric geometries that have D1, D5, momentum and KK monopole charges. We show that there exists a method to embed these geome... | 8.432883 | 7.656947 | 8.920962 | 7.270095 | 7.257938 | 7.69594 | 7.890768 | 8.12101 | 7.42681 | 10.687273 | 7.703143 | 7.355311 | 8.180254 | 7.490538 | 7.606377 | 7.387825 | 7.516423 | 7.327446 | 7.73316 | 8.293365 | 7.653145 |
hep-th/0609177 | Stefan Zohren | S. Zohren | Analytic Results in 2D Causal Dynamical Triangulations: A Review | 66 pages, 17 figures. Based on the author's thesis for the Master of
Science in Theoretical Physics, supervised by R. Loll and co-supervised by J.
Ambjorn, J. Jersak, July 2005 | null | null | null | hep-th | null | We describe the motivation behind the recent formulation of a nonperturbative
path integral for Lorentzian quantum gravity defined through Causal Dynamical
Triangulations (CDT). In the case of two dimensions the model is analytically
solvable, leading to a genuine continuum theory of quantum gravity whose ground
stat... | [
{
"created": "Mon, 25 Sep 2006 22:26:24 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Zohren",
"S.",
""
]
] | We describe the motivation behind the recent formulation of a nonperturbative path integral for Lorentzian quantum gravity defined through Causal Dynamical Triangulations (CDT). In the case of two dimensions the model is analytically solvable, leading to a genuine continuum theory of quantum gravity whose ground state ... | 7.737618 | 7.692309 | 7.830699 | 7.504301 | 7.718528 | 7.829666 | 7.662232 | 7.418381 | 7.461697 | 8.397219 | 7.270461 | 7.384581 | 7.535768 | 7.276527 | 7.635162 | 7.652683 | 7.465261 | 7.474297 | 7.384654 | 7.687146 | 7.433484 |
hep-th/9712170 | Argurio Riccardo | R. Argurio | Intersection Rules and Open Branes | 12 pages, Latex, uses crckapb.sty. To appear in the proceedings of
the Cargese '97 summer school | null | null | ULB-TH-97/21 | hep-th | null | A general rule determining how extremal branes can intersect in a
configuration with zero binding energy is presented. It is derived in a model
independent way and without explicit use of supersymmetry, solving a set of
classical equations of motion. When specializing to M and type II theories, it
is shown that some ... | [
{
"created": "Wed, 17 Dec 1997 11:54:18 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Argurio",
"R.",
""
]
] | A general rule determining how extremal branes can intersect in a configuration with zero binding energy is presented. It is derived in a model independent way and without explicit use of supersymmetry, solving a set of classical equations of motion. When specializing to M and type II theories, it is shown that some in... | 17.41181 | 14.054319 | 16.50647 | 13.166557 | 14.645838 | 15.217077 | 12.607185 | 12.909849 | 13.886436 | 18.559324 | 13.971313 | 13.216316 | 15.060318 | 13.954817 | 13.759905 | 13.242619 | 13.649076 | 13.078012 | 13.508408 | 15.99801 | 13.553834 |
0801.3402 | Bhupendra Nath Tiwari | Bhupendra Nath Tiwari | On Generalized Uncertainty Principle | 29 pages, Latex | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study generalized uncertainty principle through the basic concepts of
limit and Fourier transformation and analyze both the quantum theory of gravity
and string theory from the perspective of complex function theory. Motivated
from the noncommutative nature of string theory, we have proposed a UV/IR
mixing depende... | [
{
"created": "Tue, 22 Jan 2008 16:23:03 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Sep 2011 21:57:00 GMT",
"version": "v2"
}
] | 2011-09-22 | [
[
"Tiwari",
"Bhupendra Nath",
""
]
] | We study generalized uncertainty principle through the basic concepts of limit and Fourier transformation and analyze both the quantum theory of gravity and string theory from the perspective of complex function theory. Motivated from the noncommutative nature of string theory, we have proposed a UV/IR mixing dependent... | 9.218943 | 9.908794 | 9.506432 | 9.152266 | 9.766886 | 9.193477 | 8.889338 | 9.645754 | 9.00996 | 9.977359 | 9.006625 | 9.197536 | 9.205487 | 9.076139 | 9.050351 | 9.078544 | 9.215735 | 9.071644 | 9.311399 | 9.162278 | 8.921069 |
1408.1514 | Christopher Pope | H. Lu, C.N. Pope and Qiang Wen | Thermodynamics of AdS Black Holes in Einstein-Scalar Gravity | 42 pages, 2 figures. Version published in JHEP, plus a "Note Added"
expanding on our definition of "mass" via the first law | JHEP 1503 (2015) 165 | null | MIFPA-14-23 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the thermodynamics of $n$-dimensional static asymptotically AdS
black holes in Einstein gravity coupled to a scalar field with a potential
admitting a stationary point with an AdS vacuum. Such black holes with
non-trivial scalar hair can exist provided that the mass-squared of the scalar
field is negative, a... | [
{
"created": "Thu, 7 Aug 2014 08:41:50 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Jul 2015 08:13:19 GMT",
"version": "v2"
}
] | 2015-07-09 | [
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Wen",
"Qiang",
""
]
] | We study the thermodynamics of $n$-dimensional static asymptotically AdS black holes in Einstein gravity coupled to a scalar field with a potential admitting a stationary point with an AdS vacuum. Such black holes with non-trivial scalar hair can exist provided that the mass-squared of the scalar field is negative, and... | 6.47545 | 6.878478 | 7.814494 | 6.902217 | 7.340501 | 6.745026 | 7.034964 | 6.777087 | 6.478929 | 8.57475 | 6.694412 | 6.478184 | 6.884172 | 6.694198 | 6.758268 | 6.762837 | 6.574439 | 6.749837 | 6.572509 | 7.038013 | 6.605479 |
0807.3664 | Jesper Grimstrup | Johannes Aastrup, Jesper M. Grimstrup, Ryszard Nest | A new spectral triple over a space of connections | 14 pages, 5 figures | Commun.Math.Phys.290:389-398,2009 | 10.1007/s00220-009-0758-8 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new construction of a semifinite spectral triple on an algebra of holonomy
loops is presented. The construction is canonically associated to quantum
gravity and is an alternative version of the spectral triple presented in
hep-th/08021784.
| [
{
"created": "Wed, 23 Jul 2008 13:37:54 GMT",
"version": "v1"
}
] | 2011-03-02 | [
[
"Aastrup",
"Johannes",
""
],
[
"Grimstrup",
"Jesper M.",
""
],
[
"Nest",
"Ryszard",
""
]
] | A new construction of a semifinite spectral triple on an algebra of holonomy loops is presented. The construction is canonically associated to quantum gravity and is an alternative version of the spectral triple presented in hep-th/08021784. | 20.069946 | 14.730745 | 19.600395 | 17.243322 | 16.120623 | 19.027861 | 19.211792 | 16.30393 | 14.041673 | 34.731441 | 13.822432 | 14.183365 | 15.558553 | 16.069942 | 15.096621 | 14.664877 | 15.477019 | 15.336387 | 15.672174 | 17.941927 | 14.282722 |
hep-th/9506091 | Per Berglund | P. Berglund, S. Katz and A. Klemm | Mirror Symmetry and the Moduli Space for Generic Hypersurfaces in Toric
Varieties | 54 pages, use harvmac and epsf, one uuencoded figure | Nucl.Phys.B456:153-204,1995 | 10.1016/0550-3213(95)00434-2 | CERN-TH-7528/95; IASSNS-HEP-94/106; OSU Math 1994-3 | hep-th alg-geom math.AG | null | The moduli dependence of $(2,2)$ superstring compactifications based on
Calabi--Yau hypersurfaces in weighted projective space has so far only been
investigated for Fermat-type polynomial constraints. These correspond to
Landau-Ginzburg orbifolds with $c=9$ whose potential is a sum of $A$-type
singularities. Here we ... | [
{
"created": "Wed, 14 Jun 1995 05:43:04 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Berglund",
"P.",
""
],
[
"Katz",
"S.",
""
],
[
"Klemm",
"A.",
""
]
] | The moduli dependence of $(2,2)$ superstring compactifications based on Calabi--Yau hypersurfaces in weighted projective space has so far only been investigated for Fermat-type polynomial constraints. These correspond to Landau-Ginzburg orbifolds with $c=9$ whose potential is a sum of $A$-type singularities. Here we co... | 7.817693 | 8.706071 | 9.85398 | 8.25246 | 8.259428 | 8.081003 | 8.412811 | 7.706865 | 7.662973 | 10.875582 | 7.628921 | 7.54842 | 8.604344 | 7.414578 | 7.747419 | 7.862685 | 7.77266 | 7.712134 | 7.724948 | 8.557129 | 7.781161 |
2302.12776 | Jungwon Lim | Johannes M. Henn, Jungwon Lim, William J. Torres Bobadilla | First look at the evaluation of three-loop non-planar Feynman diagrams
for Higgs plus jet production | 13 pages, 4 figures, 630 integrals | null | 10.1007/JHEP05(2023)026 | MPP-2023-35 | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | We present new computations for Feynman integrals relevant to Higgs plus jet
production at three loops, including first results for a non-planar class of
integrals. The results are expressed in terms of generalised polylogarithms up
to transcendental weight six. We also provide the full canonical differential
equatio... | [
{
"created": "Fri, 24 Feb 2023 17:45:25 GMT",
"version": "v1"
}
] | 2023-05-24 | [
[
"Henn",
"Johannes M.",
""
],
[
"Lim",
"Jungwon",
""
],
[
"Bobadilla",
"William J. Torres",
""
]
] | We present new computations for Feynman integrals relevant to Higgs plus jet production at three loops, including first results for a non-planar class of integrals. The results are expressed in terms of generalised polylogarithms up to transcendental weight six. We also provide the full canonical differential equations... | 11.601498 | 11.526858 | 11.657462 | 10.794052 | 10.762278 | 11.870061 | 12.262096 | 11.740842 | 11.138144 | 12.037071 | 11.29947 | 11.369742 | 10.920528 | 11.035382 | 11.170823 | 11.680378 | 11.04802 | 11.259113 | 10.860339 | 11.383346 | 11.302518 |
2101.05117 | Edoardo Vescovi | Edoardo Vescovi | The four-point function of determinant operators in $\mathcal{N}=4$ SYM | 9 pages, 1 figure, matching published version | Phys. Rev. D 103, 106001 (2021) | 10.1103/PhysRevD.103.106001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the four-point function of $1/2$-BPS determinant operators in
$\mathcal{N}=4$ SYM at next-to-leading order at weak coupling. We use two
complementary methods recently developed for a class of determinant three-point
functions: one is based on Feynman diagrams and it extracts perturbative data
at finite $... | [
{
"created": "Wed, 13 Jan 2021 15:12:59 GMT",
"version": "v1"
},
{
"created": "Tue, 4 May 2021 23:10:18 GMT",
"version": "v2"
}
] | 2021-05-12 | [
[
"Vescovi",
"Edoardo",
""
]
] | We calculate the four-point function of $1/2$-BPS determinant operators in $\mathcal{N}=4$ SYM at next-to-leading order at weak coupling. We use two complementary methods recently developed for a class of determinant three-point functions: one is based on Feynman diagrams and it extracts perturbative data at finite $N$... | 9.799745 | 8.996489 | 11.087348 | 8.945344 | 9.027723 | 8.138802 | 8.805424 | 9.287035 | 8.338549 | 11.623597 | 8.255898 | 8.805964 | 9.985769 | 9.068887 | 9.23044 | 9.145257 | 9.316424 | 9.182535 | 8.970523 | 9.83144 | 9.346757 |
hep-th/9407163 | null | W.A. Sabra, O.A. Soloviev and S. Thomas | Towards c=0 Flows | LaTex file, 11 pages, QMW Preprint, QMW 94-21 | Phys.Lett. B338 (1994) 169-174 | 10.1016/0370-2693(94)91362-5 | null | hep-th | null | We discuss some implications of the gravitational dressing of the
renormalization group for conformal field theories perturbed by relevant
operators. The renormalization group flows are defined with respect to the
dilatation operator associated with the $J_0^{(0)}$ mode of the $SL(2,R)$
affine algebra. We discuss the... | [
{
"created": "Mon, 25 Jul 1994 20:07:21 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Sabra",
"W. A.",
""
],
[
"Soloviev",
"O. A.",
""
],
[
"Thomas",
"S.",
""
]
] | We discuss some implications of the gravitational dressing of the renormalization group for conformal field theories perturbed by relevant operators. The renormalization group flows are defined with respect to the dilatation operator associated with the $J_0^{(0)}$ mode of the $SL(2,R)$ affine algebra. We discuss the p... | 9.425283 | 9.190619 | 11.233014 | 8.969667 | 9.652517 | 9.442019 | 9.054636 | 8.676578 | 8.17658 | 12.340673 | 8.486688 | 8.786228 | 9.759281 | 9.097739 | 9.344486 | 9.322948 | 8.890516 | 9.188146 | 8.918554 | 9.678141 | 8.935399 |
0907.4503 | Paul Chesler | Paul M. Chesler | Gauge/gravity duality and jets in strongly coupled plasma | 8 pages, 4 figures - Minor formatting adjustments. To appear in the
conference proceedings for Quark Matter 2009, March 30 - April 4, Knoxville,
Tennessee | Nucl.Phys.A830:115c-122c,2009 | 10.1016/j.nuclphysa.2009.10.088 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss jets in strongly coupled N = 4 supersymmetric Yang-Mills plasma
and their dual gravitational description.
| [
{
"created": "Sun, 26 Jul 2009 18:00:23 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Oct 2009 16:34:52 GMT",
"version": "v2"
}
] | 2009-11-18 | [
[
"Chesler",
"Paul M.",
""
]
] | We discuss jets in strongly coupled N = 4 supersymmetric Yang-Mills plasma and their dual gravitational description. | 12.062498 | 7.610977 | 8.131267 | 7.689676 | 7.458858 | 6.687496 | 6.319109 | 6.846018 | 7.376037 | 10.768768 | 7.844888 | 9.887494 | 10.514493 | 9.180249 | 9.33628 | 9.331411 | 9.019656 | 9.159057 | 9.090209 | 10.240134 | 9.686137 |
1905.13361 | Clay C\'ordova | Clay Cordova, Daniel S. Freed, Ho Tat Lam, Nathan Seiberg | Anomalies in the Space of Coupling Constants and Their Dynamical
Applications II | 43 pages, 4 tables. v2 minor corrections and additional references.
v3 published version | SciPost Phys. 8, 002 (2020) | 10.21468/SciPostPhys.8.1.002 | null | hep-th cond-mat.str-el math-ph math.AT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend our earlier work on anomalies in the space of coupling constants to
four-dimensional gauge theories. Pure Yang-Mills theory (without matter) with a
simple and simply connected gauge group has a mixed anomaly between its
one-form global symmetry (associated with the center) and the periodicity of
the $\theta... | [
{
"created": "Fri, 31 May 2019 00:15:56 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Jul 2019 02:10:14 GMT",
"version": "v2"
},
{
"created": "Wed, 30 Oct 2019 05:57:18 GMT",
"version": "v3"
}
] | 2020-01-08 | [
[
"Cordova",
"Clay",
""
],
[
"Freed",
"Daniel S.",
""
],
[
"Lam",
"Ho Tat",
""
],
[
"Seiberg",
"Nathan",
""
]
] | We extend our earlier work on anomalies in the space of coupling constants to four-dimensional gauge theories. Pure Yang-Mills theory (without matter) with a simple and simply connected gauge group has a mixed anomaly between its one-form global symmetry (associated with the center) and the periodicity of the $\theta$-... | 7.962109 | 7.798345 | 9.679236 | 7.413869 | 7.913655 | 8.059651 | 7.67486 | 8.020702 | 7.575513 | 9.197892 | 7.525536 | 7.55101 | 8.298896 | 7.555037 | 7.685384 | 7.238324 | 7.542816 | 7.312841 | 7.310793 | 8.535419 | 7.504429 |
hep-th/9407124 | Jean-Yves Thibon | Israel Gelfand, D. Krob, Alain Lascoux, B. Leclerc, V. S. Retakh,
J.-Y. Thibon | Noncommutative symmetric functions | 111 pages | null | null | LITP 94.39 | hep-th math.QA | null | This paper presents a noncommutative theory of symmetric functions, based on
the notion of quasi-determinant. We begin with a formal theory, corresponding
to the case of symmetric functions in an infinite number of independent
variables. This allows us to endow the resulting algebra with a Hopf structure,
which leads... | [
{
"created": "Wed, 20 Jul 1994 10:45:23 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Gelfand",
"Israel",
""
],
[
"Krob",
"D.",
""
],
[
"Lascoux",
"Alain",
""
],
[
"Leclerc",
"B.",
""
],
[
"Retakh",
"V. S.",
""
],
[
"Thibon",
"J. -Y.",
""
]
] | This paper presents a noncommutative theory of symmetric functions, based on the notion of quasi-determinant. We begin with a formal theory, corresponding to the case of symmetric functions in an infinite number of independent variables. This allows us to endow the resulting algebra with a Hopf structure, which leads t... | 7.956145 | 8.722413 | 8.987561 | 8.37194 | 9.206157 | 9.499356 | 9.253553 | 8.471183 | 8.563713 | 9.194928 | 8.356826 | 8.000853 | 8.393985 | 8.489568 | 8.274425 | 8.35875 | 8.564606 | 8.391351 | 8.252501 | 8.715794 | 8.086345 |
1105.3740 | Matthew Roberts | Sergei Dubovsky, Albion Lawrence, and Matthew M. Roberts | Axion monodromy in a model of holographic gluodynamics | 43 pages, 10 figures. v2: references updated | null | 10.1007/JHEP02(2012)053 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The low energy field theory for N type IIA D4-branes at strong 't Hooft
coupling, wrapped on a circle with antiperiodic boundary conditions for
fermions, is known to have a vacuum energy which depends on the $\theta$ angle
for the gauge fields, and which is a multivalued function of this angle. This
gives a field-the... | [
{
"created": "Wed, 18 May 2011 20:08:40 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Nov 2011 16:23:14 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Dubovsky",
"Sergei",
""
],
[
"Lawrence",
"Albion",
""
],
[
"Roberts",
"Matthew M.",
""
]
] | The low energy field theory for N type IIA D4-branes at strong 't Hooft coupling, wrapped on a circle with antiperiodic boundary conditions for fermions, is known to have a vacuum energy which depends on the $\theta$ angle for the gauge fields, and which is a multivalued function of this angle. This gives a field-theor... | 8.583576 | 9.735637 | 9.596027 | 8.621125 | 8.725245 | 9.457195 | 8.790654 | 8.746638 | 8.435025 | 10.351278 | 8.507199 | 8.213755 | 8.440772 | 8.272375 | 8.439068 | 8.416301 | 8.282276 | 8.361049 | 8.219904 | 8.442677 | 8.348624 |
1901.10493 | Gabriele Lo Monaco | Ivan Garozzo, Gabriele Lo Monaco and Noppadol Mekareeya | Variations on S-fold CFTs | v2: minor corrections and references added | null | 10.1007/JHEP03(2019)171 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A local SL(2,Z) transformation on the Type IIB brane configuration gives rise
to an interesting class of superconformal field theories, known as the S-fold
CFTs. Previously it has been proposed that the corresponding quiver theory has
a link involving the T(U(N)) theory. In this paper, we generalise the preceding
res... | [
{
"created": "Tue, 29 Jan 2019 19:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Feb 2019 09:43:20 GMT",
"version": "v2"
}
] | 2019-05-01 | [
[
"Garozzo",
"Ivan",
""
],
[
"Monaco",
"Gabriele Lo",
""
],
[
"Mekareeya",
"Noppadol",
""
]
] | A local SL(2,Z) transformation on the Type IIB brane configuration gives rise to an interesting class of superconformal field theories, known as the S-fold CFTs. Previously it has been proposed that the corresponding quiver theory has a link involving the T(U(N)) theory. In this paper, we generalise the preceding resul... | 9.822867 | 8.447565 | 10.08076 | 8.490054 | 8.545528 | 8.645809 | 8.726007 | 8.677052 | 8.244831 | 11.079154 | 8.517465 | 9.097616 | 9.343596 | 8.65155 | 9.027306 | 8.619444 | 8.823462 | 8.892757 | 8.867418 | 9.486766 | 9.017594 |
0911.4408 | David Turton | Yusuke Kimura, Sanjaye Ramgoolam, David Turton | Free particles from Brauer algebras in complex matrix models | 64 pages, v2: Exposition improved, minor corrections; v3: Typos
corrected, published version | JHEP 1005:052,2010 | 10.1007/JHEP05(2010)052 | QMUL-PH-09-20 | hep-th cond-mat.stat-mech math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The gauge invariant degrees of freedom of matrix models based on an N x N
complex matrix, with U(N) gauge symmetry, contain hidden free particle
structures. These are exhibited using triangular matrix variables via the Schur
decomposition. The Brauer algebra basis for complex matrix models developed
earlier is useful... | [
{
"created": "Mon, 23 Nov 2009 17:02:04 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Apr 2010 20:22:28 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Jun 2010 19:26:49 GMT",
"version": "v3"
}
] | 2010-06-02 | [
[
"Kimura",
"Yusuke",
""
],
[
"Ramgoolam",
"Sanjaye",
""
],
[
"Turton",
"David",
""
]
] | The gauge invariant degrees of freedom of matrix models based on an N x N complex matrix, with U(N) gauge symmetry, contain hidden free particle structures. These are exhibited using triangular matrix variables via the Schur decomposition. The Brauer algebra basis for complex matrix models developed earlier is useful i... | 14.66328 | 15.340233 | 17.059982 | 14.088983 | 15.18257 | 14.236556 | 15.292306 | 14.935403 | 14.616288 | 18.368608 | 13.986613 | 14.163657 | 14.727463 | 14.251009 | 13.82399 | 13.578616 | 14.124618 | 14.001457 | 14.263427 | 14.80035 | 14.04083 |
1306.2058 | Sever Amit | Benjamin Basso, Amit Sever and Pedro Vieira | Space-time S-matrix and Flux tube S-matrix II. Extracting and Matching
Data | 73 pages, 42 figures. v2,v3: typos corrected | null | 10.1007/JHEP01(2014)008 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We elaborate on a non-perturbative formulation of scattering amplitudes/null
polygonal Wilson loops in planar N=4 Super-Yang-Mills theory. The construction
is based on a decomposition of the Wilson loop into elementary building blocks
named pentagon transitions. Our discussion expands on a previous letter of the
auth... | [
{
"created": "Sun, 9 Jun 2013 19:57:34 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Nov 2013 15:29:05 GMT",
"version": "v2"
},
{
"created": "Fri, 14 Feb 2014 23:02:39 GMT",
"version": "v3"
}
] | 2015-06-16 | [
[
"Basso",
"Benjamin",
""
],
[
"Sever",
"Amit",
""
],
[
"Vieira",
"Pedro",
""
]
] | We elaborate on a non-perturbative formulation of scattering amplitudes/null polygonal Wilson loops in planar N=4 Super-Yang-Mills theory. The construction is based on a decomposition of the Wilson loop into elementary building blocks named pentagon transitions. Our discussion expands on a previous letter of the author... | 9.375544 | 9.409357 | 11.346013 | 8.54358 | 9.714663 | 8.603995 | 8.961683 | 8.966469 | 9.0652 | 11.541799 | 8.731044 | 8.817909 | 9.583555 | 8.782254 | 8.88035 | 8.632127 | 9.015111 | 8.928271 | 8.767525 | 9.3362 | 8.889557 |
hep-th/9901123 | Andrea Gregori | A. Gregori, C. Kounnas and J. Rizos | Classification of the N=2, Z2 X Z2-symmetric type II orbifolds and their
type II asymmetric duals | Latex, 47 pages, no figures | Nucl.Phys. B549 (1999) 16-62 | 10.1016/S0550-3213(99)00135-2 | null | hep-th | null | Using free world-sheet fermions, we construct and classify all the N=2, Z2 X
Z2 four-dimensional orbifolds of the type IIA/B strings for which the orbifold
projections act symmetrically on the left and right movers. We study the
deformations of these models out of the fermionic point, deriving the partition
functions... | [
{
"created": "Mon, 25 Jan 1999 21:30:17 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Gregori",
"A.",
""
],
[
"Kounnas",
"C.",
""
],
[
"Rizos",
"J.",
""
]
] | Using free world-sheet fermions, we construct and classify all the N=2, Z2 X Z2 four-dimensional orbifolds of the type IIA/B strings for which the orbifold projections act symmetrically on the left and right movers. We study the deformations of these models out of the fermionic point, deriving the partition functions a... | 8.928546 | 8.829132 | 9.976276 | 8.232323 | 8.157066 | 8.335786 | 8.373348 | 8.662444 | 8.235065 | 10.795311 | 8.233005 | 8.494289 | 9.453405 | 8.250758 | 8.322399 | 8.455821 | 8.092448 | 8.349138 | 8.28313 | 9.222594 | 8.23018 |
1710.01972 | Alessia Platania | Alessia Platania, Frank Saueressig | Functional Renormalization Group flows on
Friedman-Lema\^{\i}tre-Robertson-Walker backgrounds | 14 pages, 2 figures | null | 10.1007/s10701-018-0181-0 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reanalyze the construction of the gravitational functional renormalization
group equation tailored to the Arnowitt-Deser-Misner formulation emphasizing
its connection to the covariant formulation. The results obtained from
projecting the renormalization group flow onto the Einstein-Hilbert action are
reviewed in d... | [
{
"created": "Thu, 5 Oct 2017 11:38:51 GMT",
"version": "v1"
}
] | 2018-07-04 | [
[
"Platania",
"Alessia",
""
],
[
"Saueressig",
"Frank",
""
]
] | We reanalyze the construction of the gravitational functional renormalization group equation tailored to the Arnowitt-Deser-Misner formulation emphasizing its connection to the covariant formulation. The results obtained from projecting the renormalization group flow onto the Einstein-Hilbert action are reviewed in det... | 9.794603 | 8.256303 | 8.693698 | 8.01466 | 9.058542 | 8.250567 | 7.572095 | 8.318026 | 9.200103 | 9.360262 | 8.200857 | 8.633437 | 8.728962 | 8.412547 | 8.625286 | 8.6182 | 8.651791 | 8.311668 | 8.672739 | 8.795235 | 8.729734 |
1706.09344 | Chandrasekhar Bhamidipati | Chandrasekhar Bhamidipati and Pavan Kumar Yerra | A Note on Gauss-Bonnet Black Holes at Criticality | 14 pages, 17 figures | null | 10.1016/j.physletb.2017.07.052 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | With in the extended thermodynamics, we give a comparative study of critical
heat engines for Gauss-Bonnet and charged black holes in AdS in five
dimensions, in the limit of large Gauss-Bonnet parameter $\alpha$ and charge
$q$, respectively. We show that the approach of efficiency of heat engines to
Carnot limit in G... | [
{
"created": "Wed, 28 Jun 2017 16:10:13 GMT",
"version": "v1"
}
] | 2017-10-11 | [
[
"Bhamidipati",
"Chandrasekhar",
""
],
[
"Yerra",
"Pavan Kumar",
""
]
] | With in the extended thermodynamics, we give a comparative study of critical heat engines for Gauss-Bonnet and charged black holes in AdS in five dimensions, in the limit of large Gauss-Bonnet parameter $\alpha$ and charge $q$, respectively. We show that the approach of efficiency of heat engines to Carnot limit in Gau... | 13.215166 | 9.835409 | 11.364059 | 9.94843 | 10.99519 | 10.697373 | 10.669744 | 9.312902 | 9.393403 | 14.580287 | 10.28592 | 11.232141 | 12.070775 | 11.703356 | 11.405312 | 11.540269 | 11.04198 | 10.828377 | 12.091361 | 12.142093 | 11.5905 |
hep-th/9811228 | Wolfgang Lerche | W. Lerche, S. Stieberger and N.P. Warner | Quartic Gauge Couplings from K3 Geometry | 32 p, harvmac; One footnote on page 11 extended; results unchanged;
Version subm. to ATMP | Adv.Theor.Math.Phys.3:1575-1611,1999 | null | CERN-TH/98-378 | hep-th | null | We show how certain F^4 couplings in eight dimensions can be computed using
the mirror map and K3 data. They perfectly match with the corresponding
heterotic one-loop couplings, and therefore this amounts to a successful test
of the conjectured duality between the heterotic string on T^2 and F-theory on
K3. The under... | [
{
"created": "Thu, 26 Nov 1998 17:30:54 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Dec 1999 23:55:43 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Dec 1999 21:54:26 GMT",
"version": "v3"
}
] | 2010-11-26 | [
[
"Lerche",
"W.",
""
],
[
"Stieberger",
"S.",
""
],
[
"Warner",
"N. P.",
""
]
] | We show how certain F^4 couplings in eight dimensions can be computed using the mirror map and K3 data. They perfectly match with the corresponding heterotic one-loop couplings, and therefore this amounts to a successful test of the conjectured duality between the heterotic string on T^2 and F-theory on K3. The underly... | 13.262262 | 11.582506 | 16.479649 | 11.48621 | 12.617783 | 11.63335 | 12.11769 | 11.648966 | 11.622495 | 15.316468 | 11.470993 | 11.323184 | 13.040333 | 11.745369 | 11.701371 | 11.473365 | 11.387626 | 11.736898 | 11.669463 | 13.407532 | 11.583452 |
1009.1212 | Takuya Saka | Katsushi Ito, Hiroaki Nakajima, Takuya Saka and Shin Sasaki | N=2 Instanton Effective Action in Omega-background and D3/D(-1)-brane
System in R-R Background | 35 pages, no figures, references added | JHEP1011 (2010) 093 | 10.1007/JHEP11(2010)093 | TIT/HEP-606, KIAS-P10027 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the relation between the ADHM construction of instantons in the
Omega-background and the fractional D3/D(-1)-branes at the orbifold singularity
of C \times C^2/Z_2 in Ramond-Ramond (R-R) 3-form field strength background. We
calculate disk amplitudes of open strings connecting the D3/D(-1)-branes in
certain R... | [
{
"created": "Tue, 7 Sep 2010 07:29:17 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Mar 2011 06:57:24 GMT",
"version": "v2"
}
] | 2015-05-19 | [
[
"Ito",
"Katsushi",
""
],
[
"Nakajima",
"Hiroaki",
""
],
[
"Saka",
"Takuya",
""
],
[
"Sasaki",
"Shin",
""
]
] | We study the relation between the ADHM construction of instantons in the Omega-background and the fractional D3/D(-1)-branes at the orbifold singularity of C \times C^2/Z_2 in Ramond-Ramond (R-R) 3-form field strength background. We calculate disk amplitudes of open strings connecting the D3/D(-1)-branes in certain R-R... | 5.267033 | 4.536764 | 6.29741 | 4.619531 | 4.548217 | 4.545402 | 4.202239 | 4.697227 | 4.603913 | 6.339539 | 4.637242 | 4.995937 | 5.451137 | 4.903847 | 5.050578 | 4.955575 | 4.990903 | 4.931097 | 4.94628 | 5.351031 | 4.857547 |
hep-th/0702098 | Masato Minamitsuji | Emilio Elizalde, Masato Minamitsuji and Wade Naylor | Casimir effect in rugby-ball type flux compactifications | 13 pages, 6 figures, accepted for publication in PRD | Phys.Rev.D75:064032,2007 | 10.1103/PhysRevD.75.064032 | null | hep-th astro-ph gr-qc | null | As a continuation of the work in \cite{mns}, we discuss the Casimir effect
for a massless bulk scalar field in a 4D toy model of a 6D warped flux
compactification model,to stabilize the volume modulus. The one-loop effective
potential for the volume modulus has a form similar to the Coleman-Weinberg
potential. The st... | [
{
"created": "Tue, 13 Feb 2007 10:05:53 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Feb 2007 19:22:49 GMT",
"version": "v2"
},
{
"created": "Sat, 24 Mar 2007 15:53:13 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Elizalde",
"Emilio",
""
],
[
"Minamitsuji",
"Masato",
""
],
[
"Naylor",
"Wade",
""
]
] | As a continuation of the work in \cite{mns}, we discuss the Casimir effect for a massless bulk scalar field in a 4D toy model of a 6D warped flux compactification model,to stabilize the volume modulus. The one-loop effective potential for the volume modulus has a form similar to the Coleman-Weinberg potential. The stab... | 12.274677 | 11.634491 | 12.117652 | 11.702549 | 12.613605 | 12.574205 | 11.815028 | 11.266598 | 11.117198 | 12.899539 | 11.871261 | 11.745052 | 11.906199 | 11.676881 | 11.537683 | 11.532034 | 11.515678 | 11.539798 | 11.575623 | 11.91518 | 11.782392 |
1103.0692 | Andelka Andrasi | A. Andrasi | Linear energy divergences in Coulomb gauge QCD | 6 pages, 1 figure | null | 10.1142/S0217732311036231 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The structure of linear energy divergences is analysed on the example of one
graph to 3-loop order. Such dangerous divergences do cancel when all graphs are
added, but next to leading divergences do not cancel out.
| [
{
"created": "Thu, 3 Mar 2011 14:22:45 GMT",
"version": "v1"
}
] | 2015-05-27 | [
[
"Andrasi",
"A.",
""
]
] | The structure of linear energy divergences is analysed on the example of one graph to 3-loop order. Such dangerous divergences do cancel when all graphs are added, but next to leading divergences do not cancel out. | 25.364208 | 20.59601 | 19.172447 | 17.800138 | 18.868324 | 21.436831 | 20.651514 | 17.090429 | 16.37816 | 22.136711 | 20.445488 | 20.305052 | 17.753939 | 17.754997 | 18.488556 | 20.965588 | 19.838669 | 20.899805 | 18.151754 | 18.283712 | 21.734219 |
2212.07370 | James Bonifacio | James Bonifacio, Harry Goodhew, Austin Joyce, Enrico Pajer, David
Stefanyszyn | The graviton four-point function in de Sitter space | 46 pages | null | 10.1007/JHEP06(2023)212 | null | hep-th astro-ph.CO gr-qc | http://creativecommons.org/licenses/by/4.0/ | We compute the tree-level late-time graviton four-point correlation function,
and the related quartic wavefunction coefficient, for Einstein gravity in de
Sitter spacetime. We derive this result in several ways: by direct calculation,
using the in-in formalism and the wavefunction of the universe; by a heuristic
deri... | [
{
"created": "Wed, 14 Dec 2022 17:47:11 GMT",
"version": "v1"
}
] | 2023-07-26 | [
[
"Bonifacio",
"James",
""
],
[
"Goodhew",
"Harry",
""
],
[
"Joyce",
"Austin",
""
],
[
"Pajer",
"Enrico",
""
],
[
"Stefanyszyn",
"David",
""
]
] | We compute the tree-level late-time graviton four-point correlation function, and the related quartic wavefunction coefficient, for Einstein gravity in de Sitter spacetime. We derive this result in several ways: by direct calculation, using the in-in formalism and the wavefunction of the universe; by a heuristic deriva... | 14.097077 | 10.10279 | 15.576584 | 10.84059 | 10.917958 | 10.707998 | 11.409795 | 11.374973 | 10.33746 | 15.304659 | 11.612503 | 12.018193 | 13.737376 | 12.852997 | 12.13073 | 12.644706 | 12.399638 | 12.934299 | 12.519366 | 13.035766 | 11.563967 |
hep-th/9811161 | Tekin Dereli | A.H.Bilge (ITU), T.Dereli (METU), S.Kocak (Anadolu U.) | Monopole equations on 8-manifolds with Spin(7) holonomy | 14 pages, LATEX (No figures) | Commun.Math.Phys. 203 (1999) 21-30 | 10.1007/s002200050024 | null | hep-th | null | We construct a consistent set of monopole equations on eight-manifolds with
Spin(7) holonomy. These equations are elliptic and admit non-trivial solutions
including all the 4-dimensional Seiberg-Witten solutions as a special case.
| [
{
"created": "Tue, 17 Nov 1998 09:18:22 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bilge",
"A. H.",
"",
"ITU"
],
[
"Dereli",
"T.",
"",
"METU"
],
[
"Kocak",
"S.",
"",
"Anadolu U."
]
] | We construct a consistent set of monopole equations on eight-manifolds with Spin(7) holonomy. These equations are elliptic and admit non-trivial solutions including all the 4-dimensional Seiberg-Witten solutions as a special case. | 7.858535 | 6.681818 | 10.053202 | 6.654954 | 6.57144 | 6.574668 | 6.085097 | 6.35499 | 6.444286 | 9.71224 | 6.722883 | 6.705958 | 6.9978 | 6.739815 | 6.722729 | 6.913061 | 6.573514 | 6.484694 | 6.765839 | 7.291936 | 6.718125 |
hep-th/0007189 | Noah Graham | E. Farhi, N. Graham, R. L. Jaffe, and H. Weigel | Fractional and Integer Charges from Levinson's Theorem | 16 pages, uses RevTex, 1 figure; v2: minor corrections | Nucl.Phys. B595 (2001) 536-550 | 10.1016/S0550-3213(00)00665-9 | MIT-CTP-3004 | hep-th | null | We compute fractional and integer fermion quantum numbers of static
background field configurations using phase shifts and Levinson's theorem. By
extending fermionic scattering theory to arbitrary dimensions, we implement
dimensional regularization in a 1+1 dimensional gauge theory. We demonstrate
that this regulariz... | [
{
"created": "Mon, 24 Jul 2000 18:54:06 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Dec 2000 18:51:08 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Farhi",
"E.",
""
],
[
"Graham",
"N.",
""
],
[
"Jaffe",
"R. L.",
""
],
[
"Weigel",
"H.",
""
]
] | We compute fractional and integer fermion quantum numbers of static background field configurations using phase shifts and Levinson's theorem. By extending fermionic scattering theory to arbitrary dimensions, we implement dimensional regularization in a 1+1 dimensional gauge theory. We demonstrate that this regularizat... | 18.650488 | 14.775498 | 19.306067 | 16.50008 | 16.531916 | 16.207136 | 15.966265 | 15.531427 | 16.414629 | 22.41194 | 15.648369 | 16.612602 | 18.740503 | 17.645168 | 17.453331 | 17.188669 | 16.914234 | 16.819708 | 17.826065 | 18.388435 | 16.478733 |
hep-th/9605104 | Gerard Watts | H.G.Kausch (1), G.Takacs (2) and G.M.T.Watts (1) ((1) King's College
London, (2) ELTE Budapest) | On the relation between Phi(1,2) and Phi(1,5) perturbed minimal models | LaTeX, 23 pages, 12 figures. Substantial revision of introductory
section, new discussion of complex eigenvalues and non-unitary S-matrices | Nucl.Phys. B489 (1997) 557-579 | 10.1016/S0550-3213(97)00056-4 | KCL-TH-96-7 | hep-th | null | We consider the RSOS S-matrices of the Phi(1,5) perturbed minimal models
which have recently been found in the companion paper [hep-th/9604098]. These
S-matrices have some interesting properties, in particular, unitarity may be
broken in a stronger sense than seen before, while one of the three classes of
Phi(1,5) pe... | [
{
"created": "Wed, 15 May 1996 12:11:32 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Dec 1996 11:23:36 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Kausch",
"H. G.",
""
],
[
"Takacs",
"G.",
""
],
[
"Watts",
"G. M. T.",
""
]
] | We consider the RSOS S-matrices of the Phi(1,5) perturbed minimal models which have recently been found in the companion paper [hep-th/9604098]. These S-matrices have some interesting properties, in particular, unitarity may be broken in a stronger sense than seen before, while one of the three classes of Phi(1,5) pert... | 12.042694 | 12.142568 | 14.514547 | 11.228307 | 11.781645 | 13.125935 | 11.78403 | 12.612441 | 11.853333 | 15.274152 | 11.348377 | 12.080821 | 13.05063 | 11.718324 | 12.3903 | 12.015838 | 11.907306 | 11.863081 | 11.891212 | 12.746302 | 11.50939 |
hep-th/9403136 | Ivan Cherednik | Ivan Cherednik | Elliptic quantum many-body problem and double affine
Knizhnik-Zamolodchikov equation | 23 pages | Commun.Math.Phys. 169 (1995) 441-462 | 10.1007/BF02099480 | null | hep-th math.QA | null | The elliptic-matrix quantum Olshanetsky-Perelomov problem is introduced for
arbitrary root systems by means of an elliptic generalization of the Dunkl
operators. Its equivalence with the double affine generalization of the
Knizhnik-Zamolodchikov equation (in the induced representations) is
established.
| [
{
"created": "Tue, 22 Mar 1994 22:37:31 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Cherednik",
"Ivan",
""
]
] | The elliptic-matrix quantum Olshanetsky-Perelomov problem is introduced for arbitrary root systems by means of an elliptic generalization of the Dunkl operators. Its equivalence with the double affine generalization of the Knizhnik-Zamolodchikov equation (in the induced representations) is established. | 10.761382 | 10.630693 | 12.744483 | 8.450707 | 9.886379 | 9.850262 | 10.930581 | 9.639214 | 9.361992 | 11.914135 | 9.980526 | 9.710945 | 10.96609 | 10.090717 | 10.050644 | 10.38904 | 9.856178 | 9.355916 | 9.990592 | 10.587133 | 9.707892 |
hep-th/0010229 | Carmen Molina Paris | Diego D. Dalvit, Francisco D. Mazzitelli and Carmen Molina-Paris | One-loop graviton corrections to Maxwell's equations | 15 pages, revtex | Phys.Rev.D63:084023,2001 | 10.1103/PhysRevD.63.084023 | null | hep-th gr-qc | null | We compute the graviton induced corrections to Maxwell's equations in the
one-loop and weak field approximations. The corrected equations are analogous
to the classical equations in anisotropic and inhomogeneous media. We analyze
in particular the corrections to the dispersion relations. When the wavelength
of the el... | [
{
"created": "Wed, 25 Oct 2000 11:47:08 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Dalvit",
"Diego D.",
""
],
[
"Mazzitelli",
"Francisco D.",
""
],
[
"Molina-Paris",
"Carmen",
""
]
] | We compute the graviton induced corrections to Maxwell's equations in the one-loop and weak field approximations. The corrected equations are analogous to the classical equations in anisotropic and inhomogeneous media. We analyze in particular the corrections to the dispersion relations. When the wavelength of the elec... | 6.230017 | 6.611762 | 5.830249 | 5.814825 | 6.229337 | 6.454656 | 6.043864 | 6.058044 | 5.843356 | 6.027251 | 6.055607 | 6.060589 | 5.870236 | 5.879448 | 6.018648 | 5.953732 | 5.991006 | 6.078495 | 5.848681 | 6.057893 | 6.046187 |
hep-th/9308079 | Boris Feigin | Boris Feigin and A. V. Stoyanovsky | Quasi-particles models for the representations of Lie algebras and
geometry of flag manifold | 35 pages | Funct. Anal. Appl. 28(1994), No. 1, 68--90 | null | null | hep-th math.QA | null | We give a new interpretation and proof of the "quasi-particle" type character
formulas for integrable representations of the simply-laced affine Kac-Moody
algebras through a new "semi-infinite" construction of such representations. We
compare formulas of this kind to other formulas obtained using the geometry of
the ... | [
{
"created": "Tue, 17 Aug 1993 08:26:47 GMT",
"version": "v1"
}
] | 2009-10-14 | [
[
"Feigin",
"Boris",
""
],
[
"Stoyanovsky",
"A. V.",
""
]
] | We give a new interpretation and proof of the "quasi-particle" type character formulas for integrable representations of the simply-laced affine Kac-Moody algebras through a new "semi-infinite" construction of such representations. We compare formulas of this kind to other formulas obtained using the geometry of the co... | 13.039879 | 12.786942 | 16.039314 | 12.768501 | 12.784543 | 13.186664 | 11.910863 | 12.8573 | 11.090779 | 16.360247 | 12.59101 | 11.944694 | 13.959505 | 12.058832 | 11.64703 | 11.662246 | 11.681533 | 11.795104 | 11.879724 | 14.186068 | 11.84516 |
1412.7709 | Mikhail Khramtsov A. | Dmitri Gal'tsov, Mikhail Khramtsov, Dmitri Orlov | "Triangular" extremal dilatonic dyons | An error in Sec IV and misprints throughout the paper are corrected,
one figure added, other figures replaced | null | 10.1016/j.physletb.2015.02.017 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Explicit dyonic dilaton black holes of the four-dimensional
Einstein-Maxwell-dilaton theory are known only for two particular values of the
dilaton coupling constant $a =1,\sqrt{3}$, while for other $a$ numerical
evidence was presented earlier about existence of extremal dyons in theories
with the discrete sequence o... | [
{
"created": "Wed, 24 Dec 2014 16:43:03 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Dec 2014 19:49:24 GMT",
"version": "v2"
}
] | 2015-06-23 | [
[
"Gal'tsov",
"Dmitri",
""
],
[
"Khramtsov",
"Mikhail",
""
],
[
"Orlov",
"Dmitri",
""
]
] | Explicit dyonic dilaton black holes of the four-dimensional Einstein-Maxwell-dilaton theory are known only for two particular values of the dilaton coupling constant $a =1,\sqrt{3}$, while for other $a$ numerical evidence was presented earlier about existence of extremal dyons in theories with the discrete sequence of ... | 8.058658 | 8.482268 | 7.908683 | 7.718201 | 8.910213 | 8.458139 | 9.047081 | 8.705056 | 8.186052 | 9.233437 | 7.920815 | 8.147225 | 7.965846 | 7.851962 | 8.040318 | 8.107829 | 8.105463 | 8.11819 | 8.093845 | 8.220692 | 8.01984 |
0711.4972 | Adolfo Malbouisson | C.A. Linhares, A.P.C. Malbouisson, I. Roditi | Existence of Asymptotic Expansions in Noncommutative Quantum Field
Theories | 15 pages, LATEX, no figures | Rev.Math.Phys.20:933-949,2008 | 10.1142/S0129055X0800347X | null | hep-th math-ph math.MP | null | Starting from the complete Mellin representation of Feynman amplitudes for
noncommutative vulcanized scalar quantum field theory, introduced in a previous
publication, we generalize to this theory the study of asymptotic behaviours
under scaling of arbitrary subsets of external invariants of any Feynman
amplitude. Th... | [
{
"created": "Fri, 30 Nov 2007 16:46:26 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"Linhares",
"C. A.",
""
],
[
"Malbouisson",
"A. P. C.",
""
],
[
"Roditi",
"I.",
""
]
] | Starting from the complete Mellin representation of Feynman amplitudes for noncommutative vulcanized scalar quantum field theory, introduced in a previous publication, we generalize to this theory the study of asymptotic behaviours under scaling of arbitrary subsets of external invariants of any Feynman amplitude. This... | 13.744275 | 11.509033 | 16.104984 | 11.648199 | 11.79999 | 12.192981 | 12.610727 | 13.286058 | 11.6757 | 14.730907 | 13.089065 | 11.473125 | 12.615998 | 12.571351 | 12.053209 | 12.354118 | 11.814831 | 11.682628 | 11.888408 | 12.773495 | 12.269562 |
1202.1528 | Waldemar Schulgin | Melanie Becker, Waldemar Schulgin | Boundary Terms, Spinors and Kerr/CFT | 15 pages | Journal of High Energy Physics, Volume 2012, Number 4 (2012), 63 | 10.1007/JHEP04(2012)063 | MIFPA-12-03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Similarly as in AdS/CFT, the requirement that the action for spinors be
stationary for solutions to the Dirac equation with fixed boundary conditions
determines the form of the boundary term that needs to be added to the standard
Dirac action in Kerr/CFT. We determine this boundary term and make use of it to
calculat... | [
{
"created": "Tue, 7 Feb 2012 21:00:03 GMT",
"version": "v1"
}
] | 2012-04-25 | [
[
"Becker",
"Melanie",
""
],
[
"Schulgin",
"Waldemar",
""
]
] | Similarly as in AdS/CFT, the requirement that the action for spinors be stationary for solutions to the Dirac equation with fixed boundary conditions determines the form of the boundary term that needs to be added to the standard Dirac action in Kerr/CFT. We determine this boundary term and make use of it to calculate ... | 8.527246 | 8.767941 | 8.096878 | 7.980092 | 8.804462 | 8.879795 | 8.257307 | 7.638544 | 8.833091 | 8.534637 | 7.494817 | 7.432868 | 7.965332 | 7.576841 | 7.769099 | 7.524222 | 7.380281 | 7.485529 | 7.696967 | 7.467682 | 7.422089 |
1401.0288 | Sabine Hossenfelder | S. Hossenfelder | Disentangling the Black Hole Vacuum | 16 pages, 2 figures | Phys. Rev. D 91, 044015 (2015) | 10.1103/PhysRevD.91.044015 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the question whether disentanglement of Hawking radiation can be
achieved with any local operation. We assume that the operation we look for is
unitary and can be described by a Bogoliubov transformation. This allows to
formulate requirements on the operation of disentanglement. We then show that
these requi... | [
{
"created": "Wed, 1 Jan 2014 14:08:20 GMT",
"version": "v1"
}
] | 2015-02-26 | [
[
"Hossenfelder",
"S.",
""
]
] | We study the question whether disentanglement of Hawking radiation can be achieved with any local operation. We assume that the operation we look for is unitary and can be described by a Bogoliubov transformation. This allows to formulate requirements on the operation of disentanglement. We then show that these require... | 10.788871 | 10.539618 | 10.535537 | 10.168715 | 11.608337 | 10.894919 | 10.461936 | 9.492736 | 9.974774 | 10.735386 | 9.593445 | 9.893715 | 10.262972 | 9.973647 | 10.189555 | 10.685913 | 9.908639 | 9.956492 | 10.081271 | 10.106936 | 9.917148 |
1012.6040 | Sudipta Sarkar | Saugata Chatterjee, Maulik Parikh and Sudipta Sarkar | The Black Hole Membrane Paradigm in f(R) Gravity | null | null | 10.1088/0264-9381/29/3/035014 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | To an outside observer, a black hole's event horizon appears to behave
exactly like a dynamical fluid membrane. We extend this membrane paradigm to
black holes in general $f(R)$ theories of gravity. We derive the stress tensor
and various transport coefficients of the fluid and find that the membrane
behaves as a non... | [
{
"created": "Wed, 29 Dec 2010 20:55:04 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Chatterjee",
"Saugata",
""
],
[
"Parikh",
"Maulik",
""
],
[
"Sarkar",
"Sudipta",
""
]
] | To an outside observer, a black hole's event horizon appears to behave exactly like a dynamical fluid membrane. We extend this membrane paradigm to black holes in general $f(R)$ theories of gravity. We derive the stress tensor and various transport coefficients of the fluid and find that the membrane behaves as a non-N... | 9.843669 | 8.075579 | 7.982377 | 7.724898 | 8.207244 | 8.744779 | 8.890845 | 7.688435 | 8.228337 | 7.787186 | 8.058367 | 7.938643 | 8.196874 | 8.192316 | 8.21214 | 8.366165 | 7.925395 | 8.005262 | 7.853637 | 8.545588 | 7.743884 |
hep-th/0608006 | Norma Mankoc Borstnik | Norma Susana Mankoc Borstnik, Holger Bech Nielsen | Fermions with no fundamental charges call for extra dimensions | 11 pages, revtex | null | 10.1016/j.physletb.2006.11.029 | null | hep-th | null | We call attention to that if assuming no conserved charges in the fundamental
theory with fermions, which carry only a spin and interact with only the
gravity, the dimensions $4, 12, 20,.....,$ as well as all odd dimensions, are
excluded under the requirement of mass protection. If more than one family is
required, t... | [
{
"created": "Tue, 1 Aug 2006 08:40:42 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Borstnik",
"Norma Susana Mankoc",
""
],
[
"Nielsen",
"Holger Bech",
""
]
] | We call attention to that if assuming no conserved charges in the fundamental theory with fermions, which carry only a spin and interact with only the gravity, the dimensions $4, 12, 20,.....,$ as well as all odd dimensions, are excluded under the requirement of mass protection. If more than one family is required, tha... | 35.063381 | 36.733807 | 31.034845 | 31.653704 | 34.555229 | 41.6367 | 39.665024 | 37.961975 | 36.85659 | 32.764004 | 34.914993 | 33.054321 | 30.83128 | 30.647669 | 30.699183 | 30.862404 | 30.248352 | 33.400845 | 32.174103 | 28.61809 | 31.119101 |
1912.04857 | Fyodor Tkachov | A.A. Radionov and F.V. Tkachov | Breaking the 2-loop barrier for generalized IBP reduction | 17 pages, presented at the Bogolyubov-2019 Conference, 11-13 Sep.
2019, JINR, Dubna, Russia | Physics of Particles and Nuclei, 2020, Vol. 51, No. 4, pp. 604-608 | null | INR-TH-2019-020 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the problem of constructing differential operators for the
generalized IBP reduction algorithms at the 2-loop level. A deeply optimized
software allows one to efficiently construct such operators for the first
non-degenerate 2-loop cases. The most efficient approach is found to be via the
so-called partial... | [
{
"created": "Tue, 10 Dec 2019 17:54:51 GMT",
"version": "v1"
}
] | 2020-07-07 | [
[
"Radionov",
"A. A.",
""
],
[
"Tkachov",
"F. V.",
""
]
] | We discuss the problem of constructing differential operators for the generalized IBP reduction algorithms at the 2-loop level. A deeply optimized software allows one to efficiently construct such operators for the first non-degenerate 2-loop cases. The most efficient approach is found to be via the so-called partial o... | 24.662865 | 23.563143 | 22.851128 | 20.18577 | 21.621693 | 20.7101 | 25.836578 | 20.137131 | 23.59234 | 32.31739 | 23.73214 | 21.208551 | 22.912037 | 23.224648 | 23.504549 | 23.165756 | 24.129841 | 21.974133 | 22.757948 | 24.543116 | 22.261421 |
2406.08485 | Jonathan Heckman | Jonathan J. Heckman and Max H\"ubner | Celestial Topology, Symmetry Theories, and Evidence for a Non-SUSY
D3-Brane CFT | 12 pages + references, 7 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Symmetry Theories (SymThs) provide a flexible framework for analyzing the
global categorical symmetries of a $D$-dimensional QFT$_{D}$ in terms of a
$(D+1)$-dimensional bulk system SymTh$_{D+1}$. In QFTs realized via local
string backgrounds, these SymThs naturally arise from dimensional reduction of
the linking boun... | [
{
"created": "Wed, 12 Jun 2024 17:59:36 GMT",
"version": "v1"
}
] | 2024-06-13 | [
[
"Heckman",
"Jonathan J.",
""
],
[
"Hübner",
"Max",
""
]
] | Symmetry Theories (SymThs) provide a flexible framework for analyzing the global categorical symmetries of a $D$-dimensional QFT$_{D}$ in terms of a $(D+1)$-dimensional bulk system SymTh$_{D+1}$. In QFTs realized via local string backgrounds, these SymThs naturally arise from dimensional reduction of the linking bounda... | 12.46524 | 11.650607 | 13.290022 | 11.905869 | 12.055328 | 12.022234 | 12.317164 | 12.382298 | 11.855874 | 13.59246 | 11.581182 | 12.156109 | 11.875909 | 11.660283 | 11.783142 | 11.508687 | 11.60111 | 11.137289 | 11.600923 | 11.864656 | 11.896185 |
1611.10194 | Olivera Miskovic | Xiao-Mei Kuang and Olivera Miskovic | Thermal phase transitions of dimensionally continued AdS black holes | 18 pages, 2 figures; introduction extended, references added | Phys. Rev. D 95, 046009 (2017) | 10.1103/PhysRevD.95.046009 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the thermal phase transitions of charged black holes in
dimensionally continued gravity in anti-de Sitter space. We find the van der
Waals-like phase transition in the temperature-entropy plane of the black holes
with spherical horizons in even dimensions, and there is no such phase
transition of the black h... | [
{
"created": "Wed, 30 Nov 2016 14:55:49 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Feb 2017 05:02:20 GMT",
"version": "v2"
}
] | 2017-02-24 | [
[
"Kuang",
"Xiao-Mei",
""
],
[
"Miskovic",
"Olivera",
""
]
] | We study the thermal phase transitions of charged black holes in dimensionally continued gravity in anti-de Sitter space. We find the van der Waals-like phase transition in the temperature-entropy plane of the black holes with spherical horizons in even dimensions, and there is no such phase transition of the black hol... | 6.592938 | 6.437804 | 6.297228 | 6.031488 | 6.750349 | 6.720199 | 6.666456 | 6.02325 | 6.367987 | 6.485114 | 6.415731 | 6.129587 | 6.227223 | 6.055552 | 6.211215 | 6.343446 | 6.414757 | 6.124157 | 6.244782 | 6.444583 | 6.318495 |
1210.3365 | Mohammed Mia | Mohammed Mia and Fang Chen | Non extremal geometries and holographic phase transitions | There was an algebraic mistake in the earlier version, which has been
corrected. This alters some factors in the critical horizon calculation but
the physics remains unchanged | null | 10.1007/JHEP01(2013)083 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the low energy limit of type IIB superstring theory, we obtain the
non-extremal limit of deformed conifold geometry which is dual to the IR limit
of large N thermal QCD.At low temperatures, the extremal geometry without black
hole is favored while at high temperatures, the field theory is described by
non-extre... | [
{
"created": "Thu, 11 Oct 2012 20:07:45 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Oct 2012 20:05:54 GMT",
"version": "v2"
},
{
"created": "Wed, 5 Dec 2012 03:25:53 GMT",
"version": "v3"
},
{
"created": "Wed, 8 May 2013 19:28:53 GMT",
"version": "v4"
}
] | 2015-06-11 | [
[
"Mia",
"Mohammed",
""
],
[
"Chen",
"Fang",
""
]
] | Using the low energy limit of type IIB superstring theory, we obtain the non-extremal limit of deformed conifold geometry which is dual to the IR limit of large N thermal QCD.At low temperatures, the extremal geometry without black hole is favored while at high temperatures, the field theory is described by non-extrema... | 6.796621 | 7.23367 | 7.934368 | 6.52298 | 7.116396 | 7.038606 | 7.047766 | 6.751389 | 7.262321 | 7.943563 | 6.88288 | 6.5991 | 7.098614 | 6.638124 | 6.711135 | 6.666334 | 6.716365 | 6.490344 | 6.586389 | 7.029719 | 6.558678 |
2304.03743 | Adam Solomon | Maria J. Rodriguez, Luca Santoni, Adam R. Solomon, and Luis Fernando
Temoche | Love Numbers for Rotating Black Holes in Higher Dimensions | 23+5 pages, 2 figures. v2: minor updates | Phys.Rev.D 108 (2023) 8, 084011 | 10.1103/PhysRevD.108.084011 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We compute the tidal Love numbers and static response coefficients associated
to several rotating black holes in higher dimensions, including Myers-Perry
black holes, black rings, and black strings. These coefficients exhibit a rich
and complex structure as a function of the black hole parameters and
multipoles. Our ... | [
{
"created": "Fri, 7 Apr 2023 17:27:12 GMT",
"version": "v1"
},
{
"created": "Wed, 31 May 2023 16:14:45 GMT",
"version": "v2"
}
] | 2023-11-08 | [
[
"Rodriguez",
"Maria J.",
""
],
[
"Santoni",
"Luca",
""
],
[
"Solomon",
"Adam R.",
""
],
[
"Temoche",
"Luis Fernando",
""
]
] | We compute the tidal Love numbers and static response coefficients associated to several rotating black holes in higher dimensions, including Myers-Perry black holes, black rings, and black strings. These coefficients exhibit a rich and complex structure as a function of the black hole parameters and multipoles. Our re... | 8.881919 | 8.192105 | 8.082767 | 7.528147 | 7.685504 | 8.588717 | 7.282229 | 7.453789 | 7.717464 | 8.521998 | 7.896675 | 8.391997 | 8.180788 | 8.058185 | 8.065806 | 7.615581 | 8.293301 | 8.200871 | 7.911385 | 8.239585 | 8.094913 |
2112.05390 | Mohammad Vahid Takook | M.V. Takook | "Krein" regularization method | 10 pages, a reference added, explanations added, typos corrected,
accepted for publication in Modern Physics Letters A | Mod. Phys. Lett. A, 37 (2022) 2250059 | 10.1142/S0217732322500596 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The "Krein" regularization method of quantum field theory is studied,
inspired by the Krein space quantization and quantum metric fluctuations. It
was previously considered in the one-loop approximation, and this paper is
generalized to all orders of perturbation theory. We directly recover the
physical results previ... | [
{
"created": "Fri, 10 Dec 2021 08:51:39 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Mar 2022 09:11:56 GMT",
"version": "v2"
}
] | 2022-08-18 | [
[
"Takook",
"M. V.",
""
]
] | The "Krein" regularization method of quantum field theory is studied, inspired by the Krein space quantization and quantum metric fluctuations. It was previously considered in the one-loop approximation, and this paper is generalized to all orders of perturbation theory. We directly recover the physical results previou... | 11.662994 | 10.886356 | 9.794038 | 9.979826 | 11.465506 | 10.189698 | 10.611815 | 10.350532 | 10.454947 | 10.625405 | 11.133009 | 10.897383 | 10.513686 | 10.647326 | 10.929902 | 10.654533 | 10.844811 | 11.003819 | 11.03158 | 10.184659 | 10.648824 |
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