id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1806.07445 | Vitor Emanuel Rodino Lemes | R. L. P. G. Amaral, V. E. R. Lemes, O. S. Ventura and L.C.Q.Vilar | Confining Potentials | 16 pages, no figures | null | 10.1007/s13538-019-00675-4 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the t'Hoft-Wilson method for the generation of static fermions
potential in order to derive a class of confining potentials which can describe
the quark confinement. A general pattern for the construction of propagators
through the localization of non-local actions is uncovered.
| [
{
"created": "Tue, 19 Jun 2018 19:49:01 GMT",
"version": "v1"
}
] | 2019-07-24 | [
[
"Amaral",
"R. L. P. G.",
""
],
[
"Lemes",
"V. E. R.",
""
],
[
"Ventura",
"O. S.",
""
],
[
"Vilar",
"L. C. Q.",
""
]
] | We use the t'Hoft-Wilson method for the generation of static fermions potential in order to derive a class of confining potentials which can describe the quark confinement. A general pattern for the construction of propagators through the localization of non-local actions is uncovered. | 38.864655 | 26.387661 | 38.560608 | 29.57243 | 24.248411 | 31.236362 | 29.062881 | 27.887398 | 36.442303 | 36.417297 | 28.967249 | 29.741539 | 28.19775 | 26.441961 | 26.099848 | 28.327971 | 24.962748 | 27.614574 | 25.146524 | 28.174726 | 27.137234 |
hep-th/0607149 | Rajamani Narayanan | R. Narayanan, H. Neuberger | Large N gauge theories -- Numerical results | 7 pages, 5 figures, Talk presented at CAQCD06 | null | 10.1142/9789812708267_0052 | null | hep-th hep-lat hep-ph | null | Some physical results in four dimensional large N gauge theories on a
periodic torus are summarized.
| [
{
"created": "Thu, 20 Jul 2006 15:54:08 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Narayanan",
"R.",
""
],
[
"Neuberger",
"H.",
""
]
] | Some physical results in four dimensional large N gauge theories on a periodic torus are summarized. | 52.894981 | 33.663189 | 35.084538 | 32.164303 | 34.06427 | 32.430977 | 31.123434 | 33.806103 | 27.704067 | 36.544991 | 34.074455 | 32.890827 | 32.224865 | 32.092312 | 32.532448 | 30.500082 | 30.767101 | 30.579994 | 31.440886 | 33.312576 | 29.778145 |
1809.03522 | George Georgiou | George Georgiou and Konstantinos Sfetsos | Novel all loop actions of interacting CFTs: Construction, integrability
and RG flows | 33 pages, 4 figures, typos corrected in version 2, version published
in Nucl. Phys. B | null | 10.1016/j.nuclphysb.2018.10.018 | null | hep-th nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the all loop effective action representing, for small couplings,
simultaneously self and mutually interacting current algebra CFTs realized by
WZW models. This non-trivially generalizes our previous works where such
interactions were, at the linear level, not simultaneously present. For the two
coupling ... | [
{
"created": "Mon, 10 Sep 2018 18:01:03 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Nov 2018 11:07:52 GMT",
"version": "v2"
}
] | 2018-11-14 | [
[
"Georgiou",
"George",
""
],
[
"Sfetsos",
"Konstantinos",
""
]
] | We construct the all loop effective action representing, for small couplings, simultaneously self and mutually interacting current algebra CFTs realized by WZW models. This non-trivially generalizes our previous works where such interactions were, at the linear level, not simultaneously present. For the two coupling ca... | 21.608635 | 20.254194 | 23.381767 | 18.950443 | 20.630039 | 19.515816 | 20.183813 | 19.629427 | 19.953949 | 26.764688 | 17.789362 | 18.929148 | 20.937626 | 19.759441 | 19.883121 | 18.680153 | 19.151785 | 19.647644 | 19.379412 | 20.416061 | 18.967331 |
2303.15372 | Akash Singh | Roshan Kaundinya, Omkar Nippanikar, Akash Singh and K. P. Yogendran | Revisiting the Thermal AdS partition function | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We rewrite the worldsheet torus partition function of the Thermal AdS CFT by
isolating the boundary parameters. Using this, we show that the spectrum of the
Euclidean BTZ black hole and Lorentzian AdS3 can be extracted -- the latter as
a zero temperature limit. A similar procedure recovers the Lorentzian BTZ
spectrum... | [
{
"created": "Mon, 27 Mar 2023 16:46:28 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Mar 2023 11:07:54 GMT",
"version": "v2"
}
] | 2023-03-29 | [
[
"Kaundinya",
"Roshan",
""
],
[
"Nippanikar",
"Omkar",
""
],
[
"Singh",
"Akash",
""
],
[
"Yogendran",
"K. P.",
""
]
] | We rewrite the worldsheet torus partition function of the Thermal AdS CFT by isolating the boundary parameters. Using this, we show that the spectrum of the Euclidean BTZ black hole and Lorentzian AdS3 can be extracted -- the latter as a zero temperature limit. A similar procedure recovers the Lorentzian BTZ spectrum p... | 15.765769 | 11.469366 | 14.824043 | 12.681605 | 12.196153 | 12.769291 | 11.762049 | 11.53439 | 12.17112 | 15.206382 | 12.108411 | 12.912728 | 13.927196 | 12.851831 | 13.121482 | 12.989697 | 13.433167 | 12.955854 | 12.914877 | 13.644302 | 13.252666 |
1309.0690 | Vladimir Efremov | Vladimir N. Efremov, Alfonso M. Hernandez Magdaleno, Fernando I.
Becerra Lopez | The Universe as a Set of Topological Fluids with Hierarchy and Fine
Tuning of Coupling Constants in Terms of Graph Manifolds | 46 pages, LaTeX; added interpretation in terms of Julia-Toulouse
approach in section 3; added 6 references | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The hierarchy and fine tuning of the gauge coupling constants are described
on the base of topological invariants (Chern classes interpreted as filling
factors) characterizing a collection of fractional topological fluids emerging
from three dimensional graph manifolds, which play the role of internal spaces
in the K... | [
{
"created": "Tue, 3 Sep 2013 14:19:57 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Mar 2014 15:42:43 GMT",
"version": "v2"
}
] | 2014-03-11 | [
[
"Efremov",
"Vladimir N.",
""
],
[
"Magdaleno",
"Alfonso M. Hernandez",
""
],
[
"Lopez",
"Fernando I. Becerra",
""
]
] | The hierarchy and fine tuning of the gauge coupling constants are described on the base of topological invariants (Chern classes interpreted as filling factors) characterizing a collection of fractional topological fluids emerging from three dimensional graph manifolds, which play the role of internal spaces in the Kal... | 16.42366 | 18.303837 | 17.151098 | 15.018101 | 17.883038 | 18.201475 | 16.994299 | 17.182171 | 17.303711 | 18.222942 | 16.286663 | 15.290727 | 15.733878 | 15.44326 | 15.325033 | 15.609838 | 15.416199 | 15.517744 | 15.866799 | 15.801614 | 15.106327 |
1008.3327 | John Joseph Carrasco | Z. Bern, J. J. M. Carrasco, L. J. Dixon, H. Johansson and R. Roiban | The Complete Four-Loop Four-Point Amplitude in N=4 Super-Yang-Mills
Theory | 108 pages, 37 figures | Phys.Rev.D82:125040,2010 | 10.1103/PhysRevD.82.125040 | UCLA/10/TEP/105 , Saclay--IPhT--T10/075 , SLAC--PUB--14137 ,
CERN-TH/2010-186 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the complete four-loop four-point amplitude in N=4
super-Yang-Mills theory, for a general gauge group and general D-dimensional
covariant kinematics, and including all non-planar contributions. We use the
method of maximal cuts --- an efficient application of the unitarity method ---
to construct the resul... | [
{
"created": "Thu, 19 Aug 2010 15:40:05 GMT",
"version": "v1"
}
] | 2011-03-03 | [
[
"Bern",
"Z.",
""
],
[
"Carrasco",
"J. J. M.",
""
],
[
"Dixon",
"L. J.",
""
],
[
"Johansson",
"H.",
""
],
[
"Roiban",
"R.",
""
]
] | We present the complete four-loop four-point amplitude in N=4 super-Yang-Mills theory, for a general gauge group and general D-dimensional covariant kinematics, and including all non-planar contributions. We use the method of maximal cuts --- an efficient application of the unitarity method --- to construct the result ... | 8.252975 | 8.325597 | 9.539997 | 7.931866 | 8.67213 | 8.516618 | 8.271204 | 8.83697 | 7.82201 | 9.733896 | 8.020409 | 7.89496 | 8.116966 | 7.70275 | 7.914495 | 7.797041 | 8.004972 | 7.852472 | 7.805571 | 8.121867 | 7.821171 |
0803.1378 | Nele Vandersickel | D. Dudal, J.A. Gracey, S.P. Sorella, N. Vandersickel, H. Verschelde | A gauge invariant infrared stabilization of 3D Yang-Mills gauge theories | 16 pages, 14 figures. v2: version to appear in JPhysA | J.Phys.A42:085402,2009 | 10.1088/1751-8113/42/8/085402 | LTH-782 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate that the inversion method can be a very useful tool in
providing an infrared stabilization of 3D gauge theories, in combination with
the mass operator $A^2$ in the Landau gauge. The numerical results will be
unambiguous, since the corresponding theory is ultraviolet finite in
dimensional regularization... | [
{
"created": "Mon, 10 Mar 2008 10:06:24 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Dec 2008 16:12:28 GMT",
"version": "v2"
}
] | 2009-02-02 | [
[
"Dudal",
"D.",
""
],
[
"Gracey",
"J. A.",
""
],
[
"Sorella",
"S. P.",
""
],
[
"Vandersickel",
"N.",
""
],
[
"Verschelde",
"H.",
""
]
] | We demonstrate that the inversion method can be a very useful tool in providing an infrared stabilization of 3D gauge theories, in combination with the mass operator $A^2$ in the Landau gauge. The numerical results will be unambiguous, since the corresponding theory is ultraviolet finite in dimensional regularization, ... | 12.423265 | 11.040564 | 11.304759 | 10.314616 | 10.818397 | 11.186832 | 11.096059 | 11.21058 | 10.50582 | 12.365924 | 9.955054 | 11.136081 | 11.029647 | 10.766362 | 10.983239 | 10.657586 | 10.820991 | 11.042029 | 10.831414 | 10.935486 | 10.507113 |
1301.0518 | Young-Hwan Hyun | Young-Hwan Hyun, Yoonbai Kim, O-Kab Kwon, D. D. Tolla | Abelian Projections of the Mass-deformed ABJM theory and Weakly Curved
Dual Geometry | 31 pages, 5 figures, more analysis for gravitational invariants was
added, published version | null | 10.1103/PhysRevD.87.085011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct ${\cal N}=2,4$ supersymmetric abelian projections of the ${\cal
N}=6$ mass-deformed ABJM theory. There are well-defined dual background
geometries for the ${\cal N}=2$ abelian theory, while those geometries are
unclear for the ${\cal N}=4$ abelian theory. The ${\cal N}=2$ theory is built
on the supersymm... | [
{
"created": "Thu, 3 Jan 2013 17:36:57 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Jan 2013 11:11:29 GMT",
"version": "v2"
},
{
"created": "Mon, 18 Feb 2013 10:21:33 GMT",
"version": "v3"
},
{
"created": "Fri, 29 Mar 2013 10:48:02 GMT",
"version": "v4"
}
] | 2013-04-10 | [
[
"Hyun",
"Young-Hwan",
""
],
[
"Kim",
"Yoonbai",
""
],
[
"Kwon",
"O-Kab",
""
],
[
"Tolla",
"D. D.",
""
]
] | We construct ${\cal N}=2,4$ supersymmetric abelian projections of the ${\cal N}=6$ mass-deformed ABJM theory. There are well-defined dual background geometries for the ${\cal N}=2$ abelian theory, while those geometries are unclear for the ${\cal N}=4$ abelian theory. The ${\cal N}=2$ theory is built on the supersymmet... | 5.468624 | 5.434954 | 6.717062 | 5.235917 | 5.30338 | 5.331616 | 5.284023 | 5.27657 | 5.043426 | 6.501833 | 5.316385 | 5.454267 | 5.645291 | 5.351284 | 5.372753 | 5.388061 | 5.506332 | 5.407578 | 5.397176 | 5.522954 | 5.398399 |
1507.01068 | Sudarshan Ananth | Sudarshan Ananth, Lars Brink and Mahendra Mali | Yang-Mills theories and quadratic forms | 12 pages | JHEP 1508 (2015) 153 | 10.1007/JHEP08(2015)153 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the Hamiltonian of (N=1;d=10) super Yang-Mills can be expressed
as a quadratic form in a very similar manner to that of the (N=4;d=4) theory.
We find a similar quadratic form structure for pure Yang-Mills theory but this
feature, in the non-supersymmetric case, seems to be unique to four dimensions.
We d... | [
{
"created": "Sat, 4 Jul 2015 05:29:03 GMT",
"version": "v1"
}
] | 2020-02-25 | [
[
"Ananth",
"Sudarshan",
""
],
[
"Brink",
"Lars",
""
],
[
"Mali",
"Mahendra",
""
]
] | We show that the Hamiltonian of (N=1;d=10) super Yang-Mills can be expressed as a quadratic form in a very similar manner to that of the (N=4;d=4) theory. We find a similar quadratic form structure for pure Yang-Mills theory but this feature, in the non-supersymmetric case, seems to be unique to four dimensions. We dis... | 8.457417 | 6.664135 | 8.017361 | 6.671004 | 7.148911 | 7.02716 | 7.010219 | 6.717885 | 6.401 | 7.788099 | 6.473645 | 7.230363 | 7.766755 | 7.366994 | 7.438358 | 7.284944 | 7.093531 | 7.189094 | 7.548351 | 7.883916 | 7.016652 |
hep-th/0601065 | Shao-You Zhao | Shao-You Zhao, Wen-Li Yang, and Yao-Zhong Zhang | On the Construction of Correlation Functions for the Integrable
Supersymmetric Fermion Models | Latex file, 42 pages. Invited review article for Int. J. Mod. Phys.
B; V2: Two references added, mionor typos corrected | Int.J.Mod.Phys.B20:505-550,2006 | 10.1142/S0217979206033383 | null | hep-th cond-mat.str-el cond-mat.supr-con math-ph math.MP nlin.SI | null | We review the recent progress on the construction of the determinant
representations of the correlation functions for the integrable supersymmetric
fermion models. The factorizing $F$-matrices (or the so-called $F$-basis) play
an important role in the construction. In the $F$-basis, the creation (and the
annihilation... | [
{
"created": "Wed, 11 Jan 2006 03:28:29 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Apr 2006 01:10:41 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Zhao",
"Shao-You",
""
],
[
"Yang",
"Wen-Li",
""
],
[
"Zhang",
"Yao-Zhong",
""
]
] | We review the recent progress on the construction of the determinant representations of the correlation functions for the integrable supersymmetric fermion models. The factorizing $F$-matrices (or the so-called $F$-basis) play an important role in the construction. In the $F$-basis, the creation (and the annihilation) ... | 5.989323 | 6.231863 | 6.948538 | 5.95822 | 6.110956 | 6.651445 | 5.871681 | 5.994344 | 6.13033 | 6.469496 | 6.277447 | 5.89735 | 5.897136 | 5.746624 | 5.72661 | 5.763134 | 5.649222 | 5.765827 | 5.642136 | 5.825196 | 5.647774 |
hep-th/0402060 | Ulvi Yurtsever | Ulvi Yurtsever and George Hockney | Signaling and the Black Hole Final State | 3 pages, RevTeX | null | null | null | hep-th gr-qc quant-ph | null | In an attempt to restore the unitarity of the evaporation process, Horowitz
and Maldacena recently proposed a boundary-condition constraint for the final
quantum state of an evaporating black hole at its singularity. Gottesman and
Preskill have argued that the proposed constraint must lead to nonlinear
evolution of t... | [
{
"created": "Fri, 6 Feb 2004 23:37:29 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Jun 2004 07:25:07 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Yurtsever",
"Ulvi",
""
],
[
"Hockney",
"George",
""
]
] | In an attempt to restore the unitarity of the evaporation process, Horowitz and Maldacena recently proposed a boundary-condition constraint for the final quantum state of an evaporating black hole at its singularity. Gottesman and Preskill have argued that the proposed constraint must lead to nonlinear evolution of the... | 13.112137 | 12.182552 | 12.833323 | 13.250413 | 12.900257 | 11.868464 | 13.204681 | 11.985723 | 13.09143 | 15.417246 | 12.372399 | 12.096451 | 12.326485 | 12.550259 | 12.448202 | 12.332932 | 12.254354 | 12.098695 | 12.374272 | 12.764664 | 12.225942 |
hep-th/0401114 | Richard Garavuso | Richard S. Garavuso | SO(10) heterotic M-theory vacua | 9 pages. Invited talk presented at the String Phenomenology 2003
Workshop, IPPP, Durham UK, 29 July - 4 August 2003 | null | null | OUTP-04-03P | hep-th hep-ph | null | This talk adapts the available formalism to study a class of heterotic
M-theory vacua with SO(10) grand unification group. Compactification to four
dimensions with N = 1 supersymmetry is achieved on a torus fibered Calabi-Yau
3-fold Z = X / tau_{X} with first homotopy group pi_{1}(Z) = Z_{2}. Here X is
an ellipticall... | [
{
"created": "Fri, 16 Jan 2004 20:04:46 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Jan 2004 13:05:19 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Garavuso",
"Richard S.",
""
]
] | This talk adapts the available formalism to study a class of heterotic M-theory vacua with SO(10) grand unification group. Compactification to four dimensions with N = 1 supersymmetry is achieved on a torus fibered Calabi-Yau 3-fold Z = X / tau_{X} with first homotopy group pi_{1}(Z) = Z_{2}. Here X is an elliptically ... | 6.769798 | 5.90204 | 8.124484 | 6.243588 | 7.620466 | 6.948743 | 6.99391 | 5.196725 | 5.973327 | 8.227088 | 5.986446 | 6.2779 | 7.003781 | 6.517232 | 6.858399 | 6.82033 | 6.736311 | 6.469179 | 6.500495 | 6.969188 | 6.576929 |
1801.01077 | Dionisio Bazeia | D. Bazeia, L. Losano, M.A. Marques, R. Menezes | Analytic vortex solutions in generalized models of the Maxwell-Higgs
type | 9 pages, 10 figures. To appear in PLB | Phys. Lett. B 778 (2018) 22 | 10.1016/j.physletb.2018.01.004 | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work deals with the presence of analytical vortex configurations in
generalized models of the Maxwell-Higgs type in the three-dimensional
spacetime. We implement a procedure that allows to decouple the first order
equations, which we use to solve the model analytically. The approach is
exemplified with three dis... | [
{
"created": "Wed, 3 Jan 2018 17:00:28 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jan 2018 19:44:27 GMT",
"version": "v2"
}
] | 2018-01-16 | [
[
"Bazeia",
"D.",
""
],
[
"Losano",
"L.",
""
],
[
"Marques",
"M. A.",
""
],
[
"Menezes",
"R.",
""
]
] | This work deals with the presence of analytical vortex configurations in generalized models of the Maxwell-Higgs type in the three-dimensional spacetime. We implement a procedure that allows to decouple the first order equations, which we use to solve the model analytically. The approach is exemplified with three disti... | 15.662019 | 8.440817 | 13.231091 | 10.402305 | 9.910403 | 9.494473 | 9.765451 | 8.293512 | 9.694831 | 14.499804 | 10.345607 | 11.698535 | 13.448578 | 12.394738 | 12.306012 | 11.957726 | 12.111847 | 12.458395 | 12.260576 | 13.309341 | 12.420566 |
1310.0858 | Jun Bourdier | Jun Bourdier and Elias Kiritsis | Holographic RG flows and nearly-marginal operators | Latex, 23 pages. Minor corrections. Version to be published in
Classical and Quantum Gravity | null | 10.1088/0264-9381/31/3/035011 | CCTP-2013-16, CCQCN-2013-11, CERN-PH-TH/2013-265, KCL-MTH-13-10 | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The holographic renormalization group flows associated with marginally
relevant operators are analyzed. The associated perturbative and
non-perturbative beta-functions are calculated and the consistent scalar
potentials are identified. The presence of a Zamolodchikov metric in the
multiscalar case is shown to affect ... | [
{
"created": "Wed, 2 Oct 2013 22:16:31 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Dec 2013 12:20:48 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Bourdier",
"Jun",
""
],
[
"Kiritsis",
"Elias",
""
]
] | The holographic renormalization group flows associated with marginally relevant operators are analyzed. The associated perturbative and non-perturbative beta-functions are calculated and the consistent scalar potentials are identified. The presence of a Zamolodchikov metric in the multiscalar case is shown to affect be... | 11.889609 | 10.090771 | 11.41802 | 10.737337 | 11.690156 | 9.729453 | 9.740889 | 10.041574 | 9.762912 | 12.687121 | 9.45179 | 10.166371 | 11.53532 | 10.795575 | 10.355282 | 10.698688 | 10.447671 | 10.520724 | 10.687663 | 11.606207 | 9.841032 |
0809.3744 | Diego Blas | D. Blas | Aspects of Infrared Modifications of Gravity | Ph.D. Thesis, 168 pages, 12 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the first part of the thesis, and after an introduction to certain models
of modified gravity, we study consistent Lagrangians for Lorentz invariant
(massive and massless) spin-2 and spin-3/2 particles in flat space. The second
part of the dissertation is devoted to non-linear extensions for the spin-2
case, focus... | [
{
"created": "Mon, 22 Sep 2008 18:12:03 GMT",
"version": "v1"
}
] | 2008-09-23 | [
[
"Blas",
"D.",
""
]
] | In the first part of the thesis, and after an introduction to certain models of modified gravity, we study consistent Lagrangians for Lorentz invariant (massive and massless) spin-2 and spin-3/2 particles in flat space. The second part of the dissertation is devoted to non-linear extensions for the spin-2 case, focusin... | 10.075601 | 9.686181 | 9.017837 | 8.769038 | 8.977374 | 9.033329 | 8.926001 | 9.191515 | 9.259638 | 9.599771 | 8.901536 | 8.961232 | 8.758541 | 8.91877 | 8.933665 | 9.018382 | 9.11689 | 8.835789 | 9.374589 | 9.237037 | 9.305763 |
2309.03934 | Arthur Platschorre | Prateek Agrawal and Arthur Platschorre | The Monodromic Axion-Photon Coupling | 20 pages, 1 figure; v2: typos corrected, references added | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | We consider the general form of the axion coupling to photons in the
axion-Maxwell theory. On general grounds this coupling takes the form of a
monodromic function of the axion, which we call $g(a)$, multiplying the
Chern-Pontryagin density $F \widetilde{F}$ of the photon. We show that the
non-linearity of $g(a)$ is ... | [
{
"created": "Thu, 7 Sep 2023 18:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Oct 2023 13:09:09 GMT",
"version": "v2"
}
] | 2023-10-11 | [
[
"Agrawal",
"Prateek",
""
],
[
"Platschorre",
"Arthur",
""
]
] | We consider the general form of the axion coupling to photons in the axion-Maxwell theory. On general grounds this coupling takes the form of a monodromic function of the axion, which we call $g(a)$, multiplying the Chern-Pontryagin density $F \widetilde{F}$ of the photon. We show that the non-linearity of $g(a)$ is a ... | 7.438562 | 7.407028 | 7.324423 | 6.980319 | 7.920078 | 7.483109 | 7.688147 | 7.365029 | 6.916131 | 7.645088 | 7.116699 | 7.204978 | 7.020738 | 6.90699 | 7.014067 | 7.210144 | 7.155478 | 7.187034 | 7.035955 | 7.279475 | 7.051863 |
hep-th/0206096 | Amir-Kian Kashani-Poor | T.Banks, W.Fischler, A.Kashani-Poor, R.McNees, S.Paban | Entropy of the Stiffest Stars | 16 pages, 5 figures | Class.Quant.Grav. 19 (2002) 4717-4728 | 10.1088/0264-9381/19/18/307 | null | hep-th | null | We analyze the properties of stars whose interior is described by the
stiffest equation of state consistent with causality. We note the remarkable
fact that the entropy of such stars scales like the area.
| [
{
"created": "Wed, 12 Jun 2002 18:45:58 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Banks",
"T.",
""
],
[
"Fischler",
"W.",
""
],
[
"Kashani-Poor",
"A.",
""
],
[
"McNees",
"R.",
""
],
[
"Paban",
"S.",
""
]
] | We analyze the properties of stars whose interior is described by the stiffest equation of state consistent with causality. We note the remarkable fact that the entropy of such stars scales like the area. | 17.897631 | 12.904892 | 11.496861 | 9.901289 | 10.105835 | 11.517309 | 11.290895 | 11.309518 | 11.47325 | 10.582873 | 13.035234 | 12.624589 | 11.599268 | 11.240713 | 11.851261 | 11.635228 | 11.747125 | 12.075093 | 11.807884 | 11.085693 | 11.894157 |
2305.18530 | Robert Saskowski | Evan Deddo, James T. Liu, Leopoldo A. Pando Zayas, Robert J. Saskowski | $c$-functions in Higher-derivative Flows Across Dimensions | 37 pages; references added | JHEP08(2023)147 | 10.1007/JHEP08(2023)147 | LCTP-23-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of gravitational theories describing renormalization group
flows across dimensions via AdS/CFT, we study the role of higher-derivative
corrections to Einstein gravity. We use the Null Energy Condition to derive
monotonicity properties of candidate holographic central charges formed by
combinations of m... | [
{
"created": "Mon, 29 May 2023 18:01:18 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jul 2023 17:14:11 GMT",
"version": "v2"
},
{
"created": "Mon, 31 Jul 2023 17:44:21 GMT",
"version": "v3"
}
] | 2023-08-25 | [
[
"Deddo",
"Evan",
""
],
[
"Liu",
"James T.",
""
],
[
"Zayas",
"Leopoldo A. Pando",
""
],
[
"Saskowski",
"Robert J.",
""
]
] | In the context of gravitational theories describing renormalization group flows across dimensions via AdS/CFT, we study the role of higher-derivative corrections to Einstein gravity. We use the Null Energy Condition to derive monotonicity properties of candidate holographic central charges formed by combinations of met... | 12.215808 | 11.306633 | 12.892152 | 11.122828 | 11.681328 | 11.59226 | 11.37928 | 10.739887 | 10.82782 | 14.741082 | 10.843637 | 11.426618 | 11.887571 | 11.405127 | 10.834206 | 11.498273 | 11.255394 | 11.681946 | 11.168671 | 11.886594 | 11.186275 |
0712.2456 | Mukund Rangamani | Sayantani Bhattacharyya, Veronika E Hubeny, Shiraz Minwalla, Mukund
Rangamani | Nonlinear Fluid Dynamics from Gravity | 46 pages, latex. v2: added refs and new section discussing second
order hydrodynamics. v3: typos corrected. v4: typos corrected | JHEP 0802:045,2008 | 10.1088/1126-6708/2008/02/045 | null | hep-th gr-qc nucl-th | null | Black branes in AdS5 appear in a four parameter family labeled by their
velocity and temperature. Promoting these parameters to Goldstone modes or
collective coordinate fields -- arbitrary functions of the coordinates on the
boundary of AdS5 -- we use Einstein's equations together with regularity
requirements and bou... | [
{
"created": "Fri, 14 Dec 2007 21:01:02 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jan 2008 10:33:34 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Feb 2008 11:02:40 GMT",
"version": "v3"
},
{
"created": "Wed, 2 Apr 2008 17:04:59 GMT",
"version": "v4"
}
] | 2009-07-09 | [
[
"Bhattacharyya",
"Sayantani",
""
],
[
"Hubeny",
"Veronika E",
""
],
[
"Minwalla",
"Shiraz",
""
],
[
"Rangamani",
"Mukund",
""
]
] | Black branes in AdS5 appear in a four parameter family labeled by their velocity and temperature. Promoting these parameters to Goldstone modes or collective coordinate fields -- arbitrary functions of the coordinates on the boundary of AdS5 -- we use Einstein's equations together with regularity requirements and bound... | 11.726216 | 9.874085 | 11.772698 | 10.837048 | 11.888573 | 10.789858 | 11.274949 | 10.498585 | 10.757334 | 11.7631 | 10.590052 | 10.08446 | 10.889866 | 10.18126 | 10.467667 | 10.081118 | 10.142612 | 10.133669 | 10.304725 | 11.196049 | 10.646481 |
hep-th/9408116 | Neil Marcus | Neil Marcus and Shimon Yankielowicz | The B model as a twisted spinning particle | 25/17 Pages big/little (LaTeX), TAUP-2192-94, CERN-TH.7402/94 | Nucl.Phys.B432:225-245,1994 | 10.1016/0550-3213(94)90601-7 | null | hep-th | null | The B-twisted topological sigma model coupled to topological gravity is
supposed to be described by an ordinary field theory: a type of holomorphic
Chern-Simons theory for the open string, and the Kodaira-Spencer theory for the
closed string. We show that the B model can be represented as a PARTICLE
theory, obtained ... | [
{
"created": "Sun, 21 Aug 1994 18:54:31 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Marcus",
"Neil",
""
],
[
"Yankielowicz",
"Shimon",
""
]
] | The B-twisted topological sigma model coupled to topological gravity is supposed to be described by an ordinary field theory: a type of holomorphic Chern-Simons theory for the open string, and the Kodaira-Spencer theory for the closed string. We show that the B model can be represented as a PARTICLE theory, obtained by... | 7.260917 | 6.66971 | 7.69919 | 6.497464 | 7.332307 | 6.994019 | 6.62887 | 6.748178 | 6.964583 | 7.827323 | 6.714702 | 6.651707 | 7.463654 | 6.817405 | 6.8985 | 6.775081 | 6.913852 | 6.762761 | 6.960324 | 7.506793 | 6.802201 |
2001.10534 | Himanshu Parihar | Jaydeep Kumar Basak, Himanshu Parihar, Boudhayan Paul and Gautam
Sengupta | Holographic entanglement negativity for disjoint subsystems in
$\mathrm{AdS_{d+1}/CFT_d}$ | 20 pages, 5 figures, v3: minor modifications | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a construction to compute the holographic entanglement negativity
for bipartite mixed state configurations of two disjoint subsystems in higher
dimensional conformal field theories (CFT$_d$s) dual to bulk AdS$_{d+1}$
geometries. Our proposal follows from the corresponding AdS$_3$/CFT$_2$
scenario and invol... | [
{
"created": "Tue, 28 Jan 2020 15:23:24 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Feb 2020 08:08:40 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Mar 2024 04:42:11 GMT",
"version": "v3"
}
] | 2024-03-05 | [
[
"Basak",
"Jaydeep Kumar",
""
],
[
"Parihar",
"Himanshu",
""
],
[
"Paul",
"Boudhayan",
""
],
[
"Sengupta",
"Gautam",
""
]
] | We propose a construction to compute the holographic entanglement negativity for bipartite mixed state configurations of two disjoint subsystems in higher dimensional conformal field theories (CFT$_d$s) dual to bulk AdS$_{d+1}$ geometries. Our proposal follows from the corresponding AdS$_3$/CFT$_2$ scenario and involve... | 5.710926 | 4.19811 | 6.197154 | 4.401096 | 4.383154 | 4.308188 | 4.505903 | 4.257354 | 4.56692 | 6.64362 | 4.509377 | 4.883004 | 5.744667 | 5.017407 | 4.978138 | 5.013937 | 4.933417 | 5.017325 | 5.004986 | 5.824871 | 5.086703 |
1811.06987 | Clay C\'ordova | Clay Cordova, G. Bruno De Luca, Alessandro Tomasiello | AdS$_8$ Solutions in Type II Supergravity | 28 pages, 3 figures. v2 additional comments | null | 10.1007/JHEP07(2019)127 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find non-supersymmetric AdS$_8$ solutions of type IIA supergravity. The
internal space is topologically an $S^2$ with a U(1) isometry. The only
non-zero flux is $F_0$; an O8 sourcing it is present at the equator of the
$S^2$. The warping function and dilaton are non-constant. It is also possible
to add D8-branes o... | [
{
"created": "Fri, 16 Nov 2018 19:00:06 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Feb 2019 17:15:18 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"Cordova",
"Clay",
""
],
[
"De Luca",
"G. Bruno",
""
],
[
"Tomasiello",
"Alessandro",
""
]
] | We find non-supersymmetric AdS$_8$ solutions of type IIA supergravity. The internal space is topologically an $S^2$ with a U(1) isometry. The only non-zero flux is $F_0$; an O8 sourcing it is present at the equator of the $S^2$. The warping function and dilaton are non-constant. It is also possible to add D8-branes on ... | 8.391425 | 7.579664 | 10.252843 | 6.762418 | 7.644568 | 8.234652 | 8.11779 | 7.536377 | 7.640242 | 10.203793 | 7.306363 | 7.474996 | 8.584841 | 7.788931 | 7.624185 | 7.756547 | 7.745022 | 7.69454 | 7.659721 | 8.324954 | 7.889497 |
1412.8751 | Rampei Kimura | Gregory Gabadadze, Rampei Kimura, David Pirtskhalava | Vainshtein Solutions Without Superluminal Modes | 30 pages, 1 figure | Phys. Rev. D 91, 124024 (2015) | 10.1103/PhysRevD.91.124024 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Vainshtein mechanism suppresses the fifth force at astrophysical
distances, while enabling it to compete with gravity at cosmological scales.
Typically, Vainshtein solutions exhibit superluminal perturbations. However, a
restricted class of solutions with special boundary conditions were shown to be
devoid of the... | [
{
"created": "Tue, 30 Dec 2014 20:14:36 GMT",
"version": "v1"
}
] | 2015-06-17 | [
[
"Gabadadze",
"Gregory",
""
],
[
"Kimura",
"Rampei",
""
],
[
"Pirtskhalava",
"David",
""
]
] | The Vainshtein mechanism suppresses the fifth force at astrophysical distances, while enabling it to compete with gravity at cosmological scales. Typically, Vainshtein solutions exhibit superluminal perturbations. However, a restricted class of solutions with special boundary conditions were shown to be devoid of the f... | 9.409284 | 10.545896 | 9.591649 | 8.874276 | 9.753798 | 10.201909 | 9.818877 | 9.403921 | 9.875692 | 10.44262 | 9.790447 | 9.249927 | 9.037199 | 8.944543 | 8.827838 | 9.145307 | 9.030323 | 8.890167 | 9.089426 | 9.253057 | 9.019302 |
hep-th/0105258 | Marco Billo' | M. Billo', L. Gallot and A. Liccardo | Classical geometry and gauge duals for fractional branes on ALE
orbifolds | LaTeX 2e, 27 pages, 4 figures | Nucl.Phys. B614 (2001) 254-278 | 10.1016/S0550-3213(01)00399-6 | DFTT 14/2001 | hep-th | null | We investigate the classical geometry corresponding to a collection of
fractional D3 branes in the orbifold limit of an ALE space. We discuss its
interpretation in terms of the world-volume gauge theory on the branes, which
is in general a non conformal N=2 Yang-Mills theory with matter. The twisted
fields reproduce ... | [
{
"created": "Fri, 25 May 2001 16:26:50 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Billo'",
"M.",
""
],
[
"Gallot",
"L.",
""
],
[
"Liccardo",
"A.",
""
]
] | We investigate the classical geometry corresponding to a collection of fractional D3 branes in the orbifold limit of an ALE space. We discuss its interpretation in terms of the world-volume gauge theory on the branes, which is in general a non conformal N=2 Yang-Mills theory with matter. The twisted fields reproduce th... | 11.248834 | 9.804316 | 10.421131 | 8.427541 | 9.481772 | 9.585735 | 9.329696 | 8.782465 | 9.061622 | 12.818101 | 9.249357 | 9.155406 | 10.389426 | 9.480342 | 9.388165 | 9.836166 | 9.504959 | 9.523085 | 9.485594 | 10.737465 | 9.48265 |
2401.02760 | Yi-Xiao Tao | Pratik Chattopadhyay, Yi-Xiao Tao | Celestial self-dual Yang-Mills theory: a new formula and the OPE limit | JHEP version | null | 10.1007/JHEP03(2024)100 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Celestial holography is a new way to understand flat-space amplitudes.
Self-dual theories, due to their nice properties, are good subjects to study
celestial holography. In this paper, we developed a new formula to calculate
the celestial color-ordered self-dual Yang-Mills amplitudes based on celestial
Berends-Giele ... | [
{
"created": "Fri, 5 Jan 2024 11:24:03 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jan 2024 16:44:20 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Mar 2024 03:36:59 GMT",
"version": "v3"
}
] | 2024-03-20 | [
[
"Chattopadhyay",
"Pratik",
""
],
[
"Tao",
"Yi-Xiao",
""
]
] | Celestial holography is a new way to understand flat-space amplitudes. Self-dual theories, due to their nice properties, are good subjects to study celestial holography. In this paper, we developed a new formula to calculate the celestial color-ordered self-dual Yang-Mills amplitudes based on celestial Berends-Giele cu... | 11.069311 | 8.22549 | 11.953277 | 7.82761 | 8.31041 | 9.825497 | 8.410403 | 7.922888 | 7.912436 | 13.259951 | 8.060539 | 8.273746 | 9.381794 | 8.274263 | 8.397668 | 8.338523 | 8.600745 | 8.321034 | 8.255009 | 9.182424 | 8.343223 |
hep-th/0402035 | Stefano Arnone | Stefano Arnone, Francesco Guerrieri and Kensuke Yoshida | N=1* model and glueball superpotential from
Renormalization-Group-improved perturbation theory | 19 pages, no figures; added references; note added at the end of the
paper; version to appear in JHEP | JHEP 0405:031,2004 | 10.1088/1126-6708/2004/05/031 | null | hep-th | null | A method for computing the low-energy non-perturbative properties of SUSY
GFT, starting from the microscopic lagrangian model, is presented. The method
relies on covariant SUSY Feynman graph techniques, adapted to low energy, and
Renormalization-Group-improved perturbation theory. We apply the method to
calculate the... | [
{
"created": "Wed, 4 Feb 2004 18:50:58 GMT",
"version": "v1"
},
{
"created": "Fri, 14 May 2004 09:51:03 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Arnone",
"Stefano",
""
],
[
"Guerrieri",
"Francesco",
""
],
[
"Yoshida",
"Kensuke",
""
]
] | A method for computing the low-energy non-perturbative properties of SUSY GFT, starting from the microscopic lagrangian model, is presented. The method relies on covariant SUSY Feynman graph techniques, adapted to low energy, and Renormalization-Group-improved perturbation theory. We apply the method to calculate the g... | 12.673644 | 11.034868 | 12.332732 | 11.338575 | 10.960525 | 10.778115 | 10.780235 | 10.572748 | 9.541951 | 13.881166 | 10.73496 | 10.51777 | 12.276998 | 10.884654 | 11.087894 | 10.540079 | 10.534029 | 10.684851 | 10.681923 | 11.93747 | 10.548572 |
1811.12658 | Josef Kluson | J. Kluson | Note About T-duality of Non-Relativistic String | 12 pages, references added | null | 10.1007/JHEP08(2019)074 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we perform canonical analysis of T-duality for non-relativistic
string in stringy Newton-Cartan background. We confirm recent result that
T-duality along longitudinal spatial direction of stringy Newton-Cartan
geometry maps non-relativistic string to the relativistic string that
propagates on the backgro... | [
{
"created": "Fri, 30 Nov 2018 07:58:41 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Dec 2018 10:10:38 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"Kluson",
"J.",
""
]
] | In this note we perform canonical analysis of T-duality for non-relativistic string in stringy Newton-Cartan background. We confirm recent result that T-duality along longitudinal spatial direction of stringy Newton-Cartan geometry maps non-relativistic string to the relativistic string that propagates on the backgroun... | 8.070498 | 5.732015 | 8.274433 | 6.620478 | 6.348176 | 5.844122 | 6.421417 | 6.553902 | 6.378556 | 8.939822 | 6.590157 | 6.315048 | 8.161274 | 7.167099 | 6.980938 | 6.327779 | 6.780203 | 6.723689 | 6.975358 | 8.279492 | 6.417476 |
1708.04335 | Ignacio Salazar | Ra\'ul E. Arias and Ignacio Salazar Landea | Thermoelectric Transport Coefficients from Charged Solv and Nil Black
Holes | 19 pages, 9 figures. v2: refs and details on computations added.
arXiv admin note: text overlap with arXiv:1503.01716 by other authors | null | 10.1007/JHEP12(2017)087 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present work we study charged black hole solutions of the
Einstein-Maxwell action that have Thurston geometries on its near horizon
region. In particular we find solutions with charged Solv and Nil geometry
horizons. We also find Nil black holes with hyperscaling violation. For all our
solutions we compute the... | [
{
"created": "Mon, 14 Aug 2017 21:31:28 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Dec 2017 20:01:43 GMT",
"version": "v2"
}
] | 2018-01-17 | [
[
"Arias",
"Raúl E.",
""
],
[
"Landea",
"Ignacio Salazar",
""
]
] | In the present work we study charged black hole solutions of the Einstein-Maxwell action that have Thurston geometries on its near horizon region. In particular we find solutions with charged Solv and Nil geometry horizons. We also find Nil black holes with hyperscaling violation. For all our solutions we compute the t... | 7.760289 | 6.614348 | 8.053826 | 6.28138 | 6.964315 | 6.995424 | 7.144839 | 6.757523 | 6.754838 | 8.897196 | 6.349824 | 6.548813 | 7.558838 | 6.931231 | 6.991095 | 7.09008 | 6.670092 | 6.739815 | 6.929869 | 7.302065 | 6.632776 |
2208.08803 | Teng Ji | Teng Ji, Li Li and Hao-Tian Sun | Thermoelectric Transport in Holographic Quantum Matter under Shear
Strain | 35 pages, 13 figures | null | 10.1088/1572-9494/aca0e1 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the thermoelectric transport under shear strain in two spatial
dimensional quantum matter using the holographic duality. General analytic
formulae for the DC thermoelectric conductivities subjected to finite shear
strain are obtained in terms of the black hole horizon data. Off-diagonal terms
in the conducti... | [
{
"created": "Thu, 18 Aug 2022 12:43:52 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Dec 2022 04:17:35 GMT",
"version": "v2"
}
] | 2022-12-28 | [
[
"Ji",
"Teng",
""
],
[
"Li",
"Li",
""
],
[
"Sun",
"Hao-Tian",
""
]
] | We study the thermoelectric transport under shear strain in two spatial dimensional quantum matter using the holographic duality. General analytic formulae for the DC thermoelectric conductivities subjected to finite shear strain are obtained in terms of the black hole horizon data. Off-diagonal terms in the conductivi... | 10.432226 | 11.034605 | 11.523277 | 9.611824 | 10.608985 | 10.413807 | 10.49082 | 10.249597 | 10.136314 | 11.501245 | 9.801354 | 10.102448 | 10.937809 | 10.040459 | 10.367064 | 9.943393 | 10.31621 | 10.127396 | 10.20224 | 10.464785 | 10.018139 |
1411.1785 | Jan Holland | Jan Holland, Stefan Hollands and Christoph Kopper | The operator product expansion converges in massless
$\varphi_4^4$-theory | 57 pages, 10 figures | null | 10.1007/s00220-015-2486-6 | CPHT-RR050.0914 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been shown recently that the mathematical status of the operator
product expansion (OPE) is better than was expected before: namely considering
massive Euclidean $\varphi^4$-theory in the perturbative loop expansion, the
OPE converges at any loop order when considering (as is usually done) composite
operator i... | [
{
"created": "Thu, 6 Nov 2014 22:36:04 GMT",
"version": "v1"
}
] | 2016-01-13 | [
[
"Holland",
"Jan",
""
],
[
"Hollands",
"Stefan",
""
],
[
"Kopper",
"Christoph",
""
]
] | It has been shown recently that the mathematical status of the operator product expansion (OPE) is better than was expected before: namely considering massive Euclidean $\varphi^4$-theory in the perturbative loop expansion, the OPE converges at any loop order when considering (as is usually done) composite operator ins... | 10.517113 | 10.929877 | 11.260555 | 10.536119 | 11.153932 | 12.084361 | 10.907773 | 10.627572 | 10.334289 | 11.034614 | 11.099733 | 10.52383 | 10.01799 | 9.887648 | 10.210881 | 10.427146 | 10.383201 | 10.145165 | 10.32543 | 10.259606 | 10.418893 |
1108.2659 | Michele Cicoli | Michele Cicoli and Fernando Quevedo | String moduli inflation: an overview | 20 pages, 1 figure, invited contribution for a special CQG issue on
String Cosmology. Typos corrected and references added | Class.Quant.Grav.28:204001,2011 | 10.1088/0264-9381/28/20/204001 | DESY 11-088 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an overview of inflationary models derived from string theory
focusing mostly on closed string moduli as inflatons. After a detailed
discussion of the eta-problem and different approaches to address it, we
describe possible ways to obtain a de Sitter vacuum with all closed string
moduli stabilised. We then... | [
{
"created": "Fri, 12 Aug 2011 17:10:16 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Sep 2011 14:14:40 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Cicoli",
"Michele",
""
],
[
"Quevedo",
"Fernando",
""
]
] | We present an overview of inflationary models derived from string theory focusing mostly on closed string moduli as inflatons. After a detailed discussion of the eta-problem and different approaches to address it, we describe possible ways to obtain a de Sitter vacuum with all closed string moduli stabilised. We then l... | 10.165445 | 10.371585 | 10.496279 | 9.945162 | 10.335452 | 10.190604 | 9.876147 | 10.669831 | 10.068051 | 10.823624 | 10.115207 | 10.045714 | 10.517836 | 9.948468 | 9.966409 | 10.316665 | 9.975989 | 10.265372 | 10.122649 | 10.41438 | 10.11467 |
1109.4834 | Hisham Sati | Hisham Sati | Topological aspects of the NS5-brane | 17 pages, arguments and presentation sharpened | null | null | null | hep-th math.AT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we investigate certain topological aspects of the effective
action of the NS5-brane in type IIA string theory. To facilitate the study of
the corresponding partition function, we define a cohomology class whose
vanishing is a necessary condition for this function to be well-defined. This
leads to various... | [
{
"created": "Thu, 22 Sep 2011 14:52:45 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Apr 2013 23:42:31 GMT",
"version": "v2"
},
{
"created": "Fri, 31 Oct 2014 21:12:25 GMT",
"version": "v3"
}
] | 2014-11-04 | [
[
"Sati",
"Hisham",
""
]
] | In this note we investigate certain topological aspects of the effective action of the NS5-brane in type IIA string theory. To facilitate the study of the corresponding partition function, we define a cohomology class whose vanishing is a necessary condition for this function to be well-defined. This leads to various t... | 9.505124 | 9.063841 | 10.786795 | 9.60705 | 9.644175 | 9.825064 | 9.120249 | 8.920841 | 8.752659 | 10.373417 | 8.802124 | 8.651069 | 9.547893 | 8.465117 | 8.918177 | 8.434991 | 8.88638 | 8.741354 | 8.692993 | 9.543907 | 8.6747 |
1305.5547 | Jun Nishimura | Jun Nishimura, Asato Tsuchiya | Realizing chiral fermions in the type IIB matrix model at finite N | 4 pages, 2 figures; (v2) analysis in section 3 improved | null | 10.1007/JHEP12(2013)002 | KEK-TH-1635 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss how chiral fermions can appear in the type IIB matrix model, which
is considered to be a nonperturbative formulation of superstring theory. In
particular, we are concerned with a constructive definition of the theory, in
which we start with a finite-N configuration and take the large-N limit later
on. We p... | [
{
"created": "Thu, 23 May 2013 20:02:22 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Dec 2013 09:03:37 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Nishimura",
"Jun",
""
],
[
"Tsuchiya",
"Asato",
""
]
] | We discuss how chiral fermions can appear in the type IIB matrix model, which is considered to be a nonperturbative formulation of superstring theory. In particular, we are concerned with a constructive definition of the theory, in which we start with a finite-N configuration and take the large-N limit later on. We poi... | 7.920841 | 6.719576 | 8.29037 | 7.257532 | 7.316422 | 7.023771 | 6.905001 | 6.651484 | 7.102889 | 8.470404 | 7.197031 | 7.433336 | 8.086039 | 7.639049 | 7.379107 | 7.287004 | 7.195954 | 7.469697 | 7.356067 | 8.152804 | 7.43189 |
hep-th/9803251 | null | Mans Henningson and Konstadinos Sfetsos | Spinors and the AdS/CFT correspondence | 9 pages, harvmac; minor changes, added references | Phys.Lett. B431 (1998) 63-68 | 10.1016/S0370-2693(98)00559-0 | CERN-TH/98-78 | hep-th | null | We consider a free massive spinor field in Euclidean Anti-de Sitter space.
The usual Dirac action in bulk is supplemented by a certain boundary term. The
boundary conditions of the field are parametrized by a spinor on the boundary,
subject to a projection. We calculate the dependence of the partition function
on thi... | [
{
"created": "Mon, 30 Mar 1998 20:41:17 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Apr 1998 09:10:18 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Henningson",
"Mans",
""
],
[
"Sfetsos",
"Konstadinos",
""
]
] | We consider a free massive spinor field in Euclidean Anti-de Sitter space. The usual Dirac action in bulk is supplemented by a certain boundary term. The boundary conditions of the field are parametrized by a spinor on the boundary, subject to a projection. We calculate the dependence of the partition function on this ... | 7.217866 | 6.444004 | 7.79168 | 6.593047 | 7.191935 | 6.686751 | 6.552564 | 6.372073 | 6.276747 | 7.753574 | 6.697724 | 6.345509 | 7.18625 | 6.65597 | 6.503002 | 6.254332 | 6.468478 | 6.662741 | 6.744281 | 6.974736 | 6.841204 |
1908.01785 | Ander Retolaza | Iosif Bena, Mariana Gra\~na, Nicolas Kovensky and Ander Retolaza | K\"ahler moduli stabilization from ten dimensions | 21 pages. v2: version published in JHEP with minor modifications | JHEP 1910 (2019) 200 | 10.1007/JHEP10(2019)200 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe the back-reaction of gaugino condensates in supersymmetric
AdS$_4$ Type II String Theory compactifications with fluxes. We use generalized
complex geometry to capture the modification of the ten-dimensional
supersymmetry equations and show that the cosmological constant prevents the
cycle wrapped by the b... | [
{
"created": "Mon, 5 Aug 2019 18:01:14 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Nov 2019 17:10:58 GMT",
"version": "v2"
}
] | 2019-11-19 | [
[
"Bena",
"Iosif",
""
],
[
"Graña",
"Mariana",
""
],
[
"Kovensky",
"Nicolas",
""
],
[
"Retolaza",
"Ander",
""
]
] | We describe the back-reaction of gaugino condensates in supersymmetric AdS$_4$ Type II String Theory compactifications with fluxes. We use generalized complex geometry to capture the modification of the ten-dimensional supersymmetry equations and show that the cosmological constant prevents the cycle wrapped by the bra... | 7.706831 | 7.857934 | 8.240054 | 7.234183 | 7.625693 | 8.159852 | 7.378932 | 7.366465 | 7.970367 | 9.630869 | 7.491706 | 7.396803 | 7.998057 | 7.297998 | 7.389029 | 7.281449 | 7.240799 | 7.097205 | 7.149528 | 7.867862 | 7.386294 |
hep-th/0507221 | Maxim Chernodub | M. N. Chernodub | Liquid crystal defects and confinement in Yang-Mills theory | 9 pages, 5 figures, RevTeX style | JETP Lett. 83 (2006) 268-272 | 10.1134/S0021364006070022 | ITEP-LAT/2005-13 | hep-th cond-mat.soft hep-lat hep-ph | null | We show that in the Landau gauge of the SU(2) Yang-Mills theory the residual
global symmetry supports existence of the topological vortices which resemble
disclination defects in the nematic liquid crystals and the Alice
(half-quantum) vortices in the superfluid heluim 3 in the A-phase. The theory
also possesses half... | [
{
"created": "Fri, 22 Jul 2005 00:01:37 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Chernodub",
"M. N.",
""
]
] | We show that in the Landau gauge of the SU(2) Yang-Mills theory the residual global symmetry supports existence of the topological vortices which resemble disclination defects in the nematic liquid crystals and the Alice (half-quantum) vortices in the superfluid heluim 3 in the A-phase. The theory also possesses half-i... | 7.012172 | 7.83058 | 6.934558 | 6.786494 | 7.621264 | 7.236068 | 6.834991 | 6.719376 | 6.690529 | 6.950394 | 6.986607 | 6.697988 | 6.610298 | 6.578581 | 6.7817 | 6.527239 | 6.615696 | 6.671121 | 6.776525 | 6.62807 | 6.587997 |
0708.0596 | Christopher Beem | Mina Aganagic, Christopher Beem, Ben Freivogel | Geometric Metastability, Quivers and Holography | v2: 56 pages, 4 figures, harvmac, abstract corrected | Nucl.Phys.B795:291-333,2008 | 10.1016/j.nuclphysb.2007.11.031 | null | hep-th | null | We use large N duality to study brane/anti-brane configurations on a class of
Calabi-Yau manifolds. With only branes present, the Calabi-Yau manifolds in
question give rise to N=2 ADE quiver theories deformed by superpotential terms.
We show that the large N duality conjecture of hep-th/0610249 reproduces
correctly t... | [
{
"created": "Mon, 6 Aug 2007 15:31:23 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Sep 2007 18:34:23 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Aganagic",
"Mina",
""
],
[
"Beem",
"Christopher",
""
],
[
"Freivogel",
"Ben",
""
]
] | We use large N duality to study brane/anti-brane configurations on a class of Calabi-Yau manifolds. With only branes present, the Calabi-Yau manifolds in question give rise to N=2 ADE quiver theories deformed by superpotential terms. We show that the large N duality conjecture of hep-th/0610249 reproduces correctly the... | 7.062502 | 6.638065 | 9.260803 | 6.560483 | 7.05441 | 6.298544 | 6.395524 | 6.386366 | 6.379983 | 8.308399 | 6.592061 | 6.390163 | 7.672957 | 6.667377 | 6.645439 | 6.593874 | 6.613936 | 6.517029 | 6.510767 | 7.544697 | 6.622863 |
hep-th/0503014 | Nuno M. Rom\~ao | Nuno M. Rom\~ao | Gauged vortices in a background | Final version: 22 pages, LaTeX, 1 eps figure | J.Phys.A38:9127-9144,2005 | 10.1088/0305-4470/38/41/020 | null | hep-th cond-mat.stat-mech math-ph math.MP | null | We discuss the statistical mechanics of a gas of gauged vortices in the
canonical formalism. At critical self-coupling, and for low temperatures, it
has been argued that the configuration space for vortex dynamics in each
topological class of the abelian Higgs model approximately truncates to a
finite-dimensional mod... | [
{
"created": "Wed, 2 Mar 2005 11:54:03 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Sep 2005 08:53:50 GMT",
"version": "v2"
}
] | 2011-04-08 | [
[
"Romão",
"Nuno M.",
""
]
] | We discuss the statistical mechanics of a gas of gauged vortices in the canonical formalism. At critical self-coupling, and for low temperatures, it has been argued that the configuration space for vortex dynamics in each topological class of the abelian Higgs model approximately truncates to a finite-dimensional modul... | 12.230946 | 11.688523 | 12.772408 | 11.5826 | 11.894747 | 11.886554 | 11.882757 | 11.687316 | 11.275267 | 14.066264 | 11.162708 | 11.989456 | 12.903111 | 11.817842 | 12.015947 | 12.21002 | 11.54375 | 11.647877 | 12.243649 | 12.579805 | 11.69907 |
1106.1870 | Ofer Aharony | Ofer Aharony, Leon Berdichevsky, Micha Berkooz and Itamar Shamir | Near-horizon solutions for D3-branes ending on 5-branes | 32 pages, 5 figures. v2: minor changes, added reference. v3: removed
discussion of extra solutions with no brane interpretation. Discussion of
solutions for D3-branes ending on 5-branes is unchanged | null | 10.1103/PhysRevD.84.126003 | WIS/5/11-MAY-DPPA | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the type IIB supergravity solutions describing D3-branes ending
on 5-branes, in the near-horizon limit of the D3-branes. Our solutions are
holographically dual to the 4d N=4 SU(N) super-Yang-Mills (SYM) theory on a
half-line, at large N and large 't Hooft coupling, with various boundary
conditions that p... | [
{
"created": "Thu, 9 Jun 2011 17:50:24 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jun 2011 19:13:20 GMT",
"version": "v2"
},
{
"created": "Wed, 6 Jul 2011 07:11:33 GMT",
"version": "v3"
}
] | 2013-05-29 | [
[
"Aharony",
"Ofer",
""
],
[
"Berdichevsky",
"Leon",
""
],
[
"Berkooz",
"Micha",
""
],
[
"Shamir",
"Itamar",
""
]
] | We construct the type IIB supergravity solutions describing D3-branes ending on 5-branes, in the near-horizon limit of the D3-branes. Our solutions are holographically dual to the 4d N=4 SU(N) super-Yang-Mills (SYM) theory on a half-line, at large N and large 't Hooft coupling, with various boundary conditions that pre... | 3.87516 | 4.024397 | 4.631243 | 3.74798 | 3.822232 | 3.876844 | 3.896653 | 3.798946 | 3.703347 | 5.098476 | 3.735781 | 3.745239 | 4.156605 | 3.746313 | 3.756338 | 3.712632 | 3.801057 | 3.771275 | 3.79143 | 4.048438 | 3.834721 |
hep-th/9707205 | Katsuyuki Sugiyama | Yuji Sugawara, Katsuyuki Sugiyama | D-brane Analyses for BPS Mass Spectra and U-duality | 44 pages, Latex, 9 figures (eps. files), Analyses based on M-theory
are added. final version to appear in Nucl. Phys. B | Nucl.Phys. B522 (1998) 158-192 | 10.1016/S0550-3213(98)00265-X | UT-781, KUCP-0109 | hep-th | null | We give a confirmation of U-duality of type II superstring by discussing mass
spectrum of the BPS states. We first evaluate the mass spectrum of BPS solitons
with one kind of R-R charges. Our analysis is based on the 1-loop effective
action of D-brane, which is known as ``Dirac-Born-Infeld (DBI) action'', and
the fac... | [
{
"created": "Thu, 24 Jul 1997 15:10:59 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Apr 1998 08:52:40 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Sugawara",
"Yuji",
""
],
[
"Sugiyama",
"Katsuyuki",
""
]
] | We give a confirmation of U-duality of type II superstring by discussing mass spectrum of the BPS states. We first evaluate the mass spectrum of BPS solitons with one kind of R-R charges. Our analysis is based on the 1-loop effective action of D-brane, which is known as ``Dirac-Born-Infeld (DBI) action'', and the fact ... | 7.668022 | 7.552101 | 7.840666 | 7.387444 | 7.607298 | 7.951875 | 7.499716 | 7.453113 | 7.602346 | 8.805162 | 7.435666 | 7.445915 | 7.604744 | 7.431603 | 7.344556 | 7.349221 | 7.416296 | 7.286769 | 7.427857 | 7.682508 | 7.306631 |
hep-th/9408112 | null | O. A. Soloviev | Conformal Invariance of Interacting WZNW Models | LaTex file, 17 pages, QMW 94-26 | null | null | null | hep-th | null | We consider two level $k$ WZNW models coupled to each other through a
generalized Thirring-like current-current interaction. It is shown that in the
large $k$ limit, this interacting system can be presented as a two-parameter
perturbation around a nonunitary WZNW model. The perturbation operators are the
sigma model ... | [
{
"created": "Fri, 19 Aug 1994 18:21:43 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Soloviev",
"O. A.",
""
]
] | We consider two level $k$ WZNW models coupled to each other through a generalized Thirring-like current-current interaction. It is shown that in the large $k$ limit, this interacting system can be presented as a two-parameter perturbation around a nonunitary WZNW model. The perturbation operators are the sigma model ki... | 9.233775 | 8.038571 | 9.609743 | 8.165548 | 8.54952 | 8.579611 | 7.988498 | 8.251018 | 8.596386 | 10.63421 | 8.326792 | 8.47913 | 9.253835 | 8.521661 | 8.447758 | 8.369076 | 8.299228 | 8.475486 | 8.416842 | 9.521272 | 8.502797 |
1001.4509 | David Berenstein | David Berenstein, Yuichiro Nakada | The shape of emergent quantum geometry from an N=4 SYM minisuperspace
approximation | 33 pages, 13 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study numerically various wave functions in a gauged matrix quantum
mechanics of six commuting hermitian $N\times N$ matrices. Our simulations span
ranges of $N$ up to 10000. This system is a truncated and quenched version of
N=4 SYM that serves as a minisuperspace approximation to the full ${\cal N}=4$
SYM system... | [
{
"created": "Mon, 25 Jan 2010 19:08:27 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Mar 2010 23:17:21 GMT",
"version": "v2"
}
] | 2010-03-04 | [
[
"Berenstein",
"David",
""
],
[
"Nakada",
"Yuichiro",
""
]
] | We study numerically various wave functions in a gauged matrix quantum mechanics of six commuting hermitian $N\times N$ matrices. Our simulations span ranges of $N$ up to 10000. This system is a truncated and quenched version of N=4 SYM that serves as a minisuperspace approximation to the full ${\cal N}=4$ SYM system. ... | 8.81288 | 9.854919 | 9.891007 | 8.953879 | 9.264085 | 9.993115 | 9.264202 | 9.383892 | 8.848716 | 9.955396 | 9.008392 | 8.782532 | 9.212579 | 8.758616 | 8.988914 | 9.04079 | 8.705441 | 8.770688 | 8.82921 | 9.186067 | 8.758535 |
2312.06743 | Kurt Hinterbichler | James Bonifacio, Kurt Hinterbichler | Fermionic Shift Symmetries in (Anti) de Sitter Space | 40 pages, 2 figures | JHEP 2024, 100 (2024) | 10.1007/JHEP04(2024)100 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study extended shift symmetries that arise for fermionic fields on anti-de
Sitter (AdS) space and de Sitter (dS) space for particular values of the mass
relative to the curvature scale. We classify these symmetries for general
mixed-symmetry fermionic fields in arbitrary dimension and describe how fields
with thes... | [
{
"created": "Mon, 11 Dec 2023 19:00:00 GMT",
"version": "v1"
}
] | 2024-08-15 | [
[
"Bonifacio",
"James",
""
],
[
"Hinterbichler",
"Kurt",
""
]
] | We study extended shift symmetries that arise for fermionic fields on anti-de Sitter (AdS) space and de Sitter (dS) space for particular values of the mass relative to the curvature scale. We classify these symmetries for general mixed-symmetry fermionic fields in arbitrary dimension and describe how fields with these ... | 8.606989 | 7.515724 | 8.541709 | 7.439895 | 7.933964 | 7.486328 | 7.568613 | 7.695697 | 7.866682 | 8.981125 | 7.506926 | 7.672712 | 8.093377 | 7.784502 | 7.70102 | 7.619198 | 7.542989 | 7.674533 | 7.719631 | 8.199108 | 7.648159 |
2103.04638 | Yang Zhang | Christoph Dlapa, Xiaodi Li, Yang Zhang | Leading singularities in Baikov representation and Feynman integrals
with uniform transcendental weight | 27 pages, 3 figures | null | 10.1007/JHEP07(2021)227 | MPP-2021-23, PCFT-21-10, USTC-ICTS-21-10 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a leading singularity analysis protocol in Baikov representation,
for the searching of Feynman integrals with uniform transcendental (UT) weight.
This approach is powered by the recent developments in rationalizing square
roots and syzygy computations, and is particularly suitable for finding UT
integrals ... | [
{
"created": "Mon, 8 Mar 2021 09:54:11 GMT",
"version": "v1"
}
] | 2021-08-18 | [
[
"Dlapa",
"Christoph",
""
],
[
"Li",
"Xiaodi",
""
],
[
"Zhang",
"Yang",
""
]
] | We provide a leading singularity analysis protocol in Baikov representation, for the searching of Feynman integrals with uniform transcendental (UT) weight. This approach is powered by the recent developments in rationalizing square roots and syzygy computations, and is particularly suitable for finding UT integrals wi... | 15.45397 | 11.661278 | 15.134641 | 11.670115 | 14.168488 | 13.208331 | 12.207788 | 12.752654 | 11.373444 | 14.49965 | 13.442801 | 13.992924 | 14.127921 | 13.594196 | 14.582268 | 14.507009 | 13.269404 | 13.451753 | 14.130805 | 13.719502 | 14.032396 |
hep-th/9504028 | null | A.G.Mirzabekian and G.A.Vilkovisky | The one-loop form factors in the effective action, and production of
coherent gravitons from the vacuum | 49 pages, latex | Class.Quant.Grav.12:2173-2200,1995 | 10.1088/0264-9381/12/9/006 | DSFT-17/95 | hep-th gr-qc | null | We present the solution of the problem of the $1/\Box, \Box \to 0,$
asymptotic terms discovered in the one-loop form factors of the gravitational
effective action. Owing to certain constraints among their coefficients, which
we establish, these terms cancel in the vacuum stress tensor and do not violate
the asymptoti... | [
{
"created": "Thu, 6 Apr 1995 11:46:45 GMT",
"version": "v1"
}
] | 2010-04-06 | [
[
"Mirzabekian",
"A. G.",
""
],
[
"Vilkovisky",
"G. A.",
""
]
] | We present the solution of the problem of the $1/\Box, \Box \to 0,$ asymptotic terms discovered in the one-loop form factors of the gravitational effective action. Owing to certain constraints among their coefficients, which we establish, these terms cancel in the vacuum stress tensor and do not violate the asymptotic ... | 14.273435 | 16.534292 | 13.676041 | 14.415843 | 16.370579 | 18.036034 | 16.503967 | 15.100267 | 14.614024 | 15.214737 | 14.951774 | 14.545195 | 13.44311 | 14.065731 | 14.258682 | 14.355033 | 14.704681 | 14.025107 | 14.054119 | 14.209052 | 13.987203 |
hep-th/9307162 | null | Z.Lalak, J.Pawelczyk, S.Pokorski | Phase Transitions in NJL and super-NJL models | LATEX, 1 figure available upon request, 11 pages, TUM-TH-157/93,
MPI-Ph/93-42, UW-IFT-10/93 | null | null | null | hep-th hep-ph | null | An elementary method of determination of the character of the hot phase
transition in 4d four-fermion NJL-type models is applied to non-supersymmetric
and supersymmetric versions of simple NJL model. We find that in the non-susy
case the transition is usually of the second order. It is weakly first order
only in the ... | [
{
"created": "Tue, 27 Jul 1993 11:44:27 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Lalak",
"Z.",
""
],
[
"Pawelczyk",
"J.",
""
],
[
"Pokorski",
"S.",
""
]
] | An elementary method of determination of the character of the hot phase transition in 4d four-fermion NJL-type models is applied to non-supersymmetric and supersymmetric versions of simple NJL model. We find that in the non-susy case the transition is usually of the second order. It is weakly first order only in the re... | 8.592557 | 8.7836 | 7.687731 | 7.469735 | 8.183864 | 8.376498 | 7.857287 | 7.394262 | 7.317656 | 7.654831 | 7.769492 | 7.874466 | 7.505678 | 7.699955 | 7.671737 | 7.825953 | 8.010795 | 7.99122 | 7.597099 | 7.809407 | 7.760331 |
2210.10712 | Boris Pioline | Pierrick Bousseau, Pierre Descombes, Bruno Le Floch, Boris Pioline | BPS Dendroscopy on Local $P^2$ | 61+23 pages, 32 figures; v3: final version to appear in Comm. Math.
Phys | Communications in Mathematical Physics 405, 108 (2024) | 10.1007/s00220-024-04938-3 | null | hep-th math.AG | http://creativecommons.org/licenses/by/4.0/ | The spectrum of BPS states in type IIA string theory compactified on a
Calabi-Yau threefold famously jumps across codimension-one walls in
complexified K\"ahler moduli space, leading to an intricate chamber structure.
The Split Attractor Flow Conjecture posits that the BPS index
$\Omega_z(\gamma)$ for given charge $\... | [
{
"created": "Wed, 19 Oct 2022 16:44:26 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Jan 2023 07:30:44 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Mar 2024 04:21:09 GMT",
"version": "v3"
}
] | 2024-05-14 | [
[
"Bousseau",
"Pierrick",
""
],
[
"Descombes",
"Pierre",
""
],
[
"Floch",
"Bruno Le",
""
],
[
"Pioline",
"Boris",
""
]
] | The spectrum of BPS states in type IIA string theory compactified on a Calabi-Yau threefold famously jumps across codimension-one walls in complexified K\"ahler moduli space, leading to an intricate chamber structure. The Split Attractor Flow Conjecture posits that the BPS index $\Omega_z(\gamma)$ for given charge $\ga... | 6.913285 | 7.792765 | 8.625204 | 7.132672 | 8.101101 | 8.297493 | 8.041483 | 7.12869 | 7.346733 | 8.458146 | 7.063463 | 6.923447 | 7.265973 | 6.770243 | 6.878215 | 7.030142 | 6.969083 | 6.892408 | 6.815324 | 7.160715 | 6.766663 |
hep-th/0010185 | Dzhunushaliev Vladimir | V. Dzhunushaliev | Nonperturbative Quantization of the Cylindrically Symmetric Strongly
Oscillating Field | grammar errors are corrected | Phys.Lett. B498 (2001) 218-222 | 10.1016/S0370-2693(00)01394-0 | null | hep-th cond-mat hep-ph | null | A recent investigation of SU(2) Yang-Mills theory found several classical
solutions with bad behaviour at infinity : one of the potential components
oscillated and another tended to infinity. In this paper we apply an idea due
to Heisenberg about the quantization of strongly interacting nonlinear fields
to these clas... | [
{
"created": "Sun, 22 Oct 2000 05:34:24 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Nov 2000 13:17:46 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Dzhunushaliev",
"V.",
""
]
] | A recent investigation of SU(2) Yang-Mills theory found several classical solutions with bad behaviour at infinity : one of the potential components oscillated and another tended to infinity. In this paper we apply an idea due to Heisenberg about the quantization of strongly interacting nonlinear fields to these classi... | 15.941506 | 14.415031 | 14.556553 | 12.709641 | 14.673884 | 12.637877 | 13.227617 | 12.527446 | 13.836286 | 13.966466 | 13.763298 | 13.638187 | 14.608572 | 13.681999 | 13.829278 | 14.370187 | 14.066566 | 13.654481 | 14.216811 | 14.210485 | 14.128658 |
1706.01001 | Adriano Lana Cherchiglia | J. S. Porto, A. R. Vieira, A. L. Cherchiglia, Marcos Sampaio, and
Brigitte Hiller | On the Bose symmetry and the left- and right-chiral anomalies | References added, comply with published version | Eur. Phys. J. C (2018) 78: 160 | 10.1140/epjc/s10052-018-5648-9 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is generally assumed that in order to preserve Bose symmetry in the left-
(or right-chiral) current it is necessary to equally distribute the chiral
anomaly between the vectorial and the axial Ward identities, requiring the use
of counterterms to restore consistency. In this work, we show how to calculate
the quan... | [
{
"created": "Sat, 3 Jun 2017 20:42:55 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Feb 2018 22:17:46 GMT",
"version": "v2"
}
] | 2018-02-27 | [
[
"Porto",
"J. S.",
""
],
[
"Vieira",
"A. R.",
""
],
[
"Cherchiglia",
"A. L.",
""
],
[
"Sampaio",
"Marcos",
""
],
[
"Hiller",
"Brigitte",
""
]
] | It is generally assumed that in order to preserve Bose symmetry in the left- (or right-chiral) current it is necessary to equally distribute the chiral anomaly between the vectorial and the axial Ward identities, requiring the use of counterterms to restore consistency. In this work, we show how to calculate the quantu... | 12.663127 | 11.948183 | 11.797254 | 12.034242 | 12.768761 | 13.079999 | 12.726997 | 11.703609 | 12.219418 | 13.812449 | 11.612963 | 11.943088 | 11.934688 | 11.457447 | 11.347097 | 11.88885 | 11.414472 | 12.063462 | 11.470227 | 12.512486 | 11.485703 |
hep-th/9604017 | Antonio Gonzalez-Arroyo | A. Gonzalez-Arroyo and A. Montero | Do classical configurations produce Confinement? | Uuencoded, Z-compressed and tarred file of the TeX file submit.tex
and PostScript files Stnt.eps and Stst.eps. 11 pages of text and two figures | Phys.Lett.B387:823-828,1996 | 10.1016/0370-2693(96)01107-0 | FTUAM/96-13 | hep-th hep-lat | null | We show that certain classical SU(2) pure gauge configurations give rise to a
non-zero string tension. We then investigate cooled configurations generated by
Monte Carlo simulations on the lattice and find similar properties. We infer
evidence in favour of a classical model of Confinement.
| [
{
"created": "Wed, 3 Apr 1996 13:42:36 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gonzalez-Arroyo",
"A.",
""
],
[
"Montero",
"A.",
""
]
] | We show that certain classical SU(2) pure gauge configurations give rise to a non-zero string tension. We then investigate cooled configurations generated by Monte Carlo simulations on the lattice and find similar properties. We infer evidence in favour of a classical model of Confinement. | 22.102501 | 18.568478 | 18.601736 | 17.165543 | 19.934196 | 16.441681 | 16.961927 | 18.617056 | 16.339615 | 18.203909 | 18.125639 | 17.208973 | 18.745455 | 18.22336 | 18.008604 | 18.587692 | 17.618444 | 18.283482 | 17.975513 | 19.229017 | 18.231428 |
hep-th/0405058 | David Kutasov | D. Kutasov | D-Brane Dynamics Near NS5-Branes | 22 pages, harvmac; added references | null | null | EFI-04-16 | hep-th | null | We use the Dirac-Born-Infeld action to study the real time dynamics of a
$Dp$-brane propagating in the vicinity of $NS5$-branes. This problem is closely
related to tachyon condensation on an unstable D-brane, with the role of the
tachyon played by the radial mode on the D-brane. As the D-brane approaches the
fivebran... | [
{
"created": "Fri, 7 May 2004 15:00:45 GMT",
"version": "v1"
},
{
"created": "Sun, 9 May 2004 12:45:49 GMT",
"version": "v2"
},
{
"created": "Wed, 19 May 2004 20:03:35 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Kutasov",
"D.",
""
]
] | We use the Dirac-Born-Infeld action to study the real time dynamics of a $Dp$-brane propagating in the vicinity of $NS5$-branes. This problem is closely related to tachyon condensation on an unstable D-brane, with the role of the tachyon played by the radial mode on the D-brane. As the D-brane approaches the fivebranes... | 5.81059 | 4.956306 | 6.528019 | 5.151865 | 4.865977 | 5.337475 | 5.152723 | 5.385582 | 5.312211 | 6.754008 | 5.129275 | 5.454686 | 5.834691 | 5.481984 | 5.477087 | 5.453029 | 5.441967 | 5.503488 | 5.408709 | 5.802144 | 5.441141 |
0903.1141 | Haitao Liu | Haitao Liu | Dimension of Conformal Blocks in Five Dimensional Kaehler-Chern-Simons
Theory | 17 pages, typos corrected and minor corrections; the version to
appear in Journal of Mathematical Physics | J.Math.Phys.51:043513,2010 | 10.1063/1.3359006 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We briefly review the Kaehler-Chern-Simon theory on 5-manifolds which are
trivial circle bundles over 4-dimensional Kaehler manifolds and present a
detailed calculation of the path integral, using the method of Blau and
Thompson.
| [
{
"created": "Fri, 6 Mar 2009 02:00:23 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Jun 2009 02:54:25 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Aug 2009 23:03:29 GMT",
"version": "v3"
},
{
"created": "Sun, 7 Mar 2010 20:02:55 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Liu",
"Haitao",
""
]
] | We briefly review the Kaehler-Chern-Simon theory on 5-manifolds which are trivial circle bundles over 4-dimensional Kaehler manifolds and present a detailed calculation of the path integral, using the method of Blau and Thompson. | 10.217727 | 8.510338 | 11.23338 | 8.23667 | 7.824323 | 8.953276 | 8.131616 | 7.931822 | 8.166928 | 10.82275 | 8.332155 | 9.134895 | 10.334909 | 8.728016 | 8.987997 | 8.781687 | 8.154171 | 8.901359 | 9.299203 | 10.385259 | 9.220028 |
hep-th/0305203 | Andrei Ivanov | M. Faber, A. N. Ivanov | Dynamical breaking of conformal symmetry in the massless Thirring model | 9 pages, Latex, no figures | null | null | null | hep-th | null | We discuss conformal invariance of the massless Thirring model. We show that
conformal symmetry of the massless Thirring model is dynamically broken due to
the constant of motion caused by the equations of motion. This confirms the
existence of the chirally broken phase in the massless Thirring model (Eur.
Phys. J. C... | [
{
"created": "Thu, 22 May 2003 15:57:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Faber",
"M.",
""
],
[
"Ivanov",
"A. N.",
""
]
] | We discuss conformal invariance of the massless Thirring model. We show that conformal symmetry of the massless Thirring model is dynamically broken due to the constant of motion caused by the equations of motion. This confirms the existence of the chirally broken phase in the massless Thirring model (Eur. Phys. J. C20... | 6.178544 | 4.847575 | 6.506675 | 5.401678 | 5.894535 | 5.834338 | 5.44132 | 5.651221 | 5.486371 | 7.567476 | 5.087661 | 5.56157 | 6.265274 | 5.958302 | 5.964492 | 5.885946 | 5.956642 | 5.932189 | 5.9677 | 6.013414 | 5.796408 |
hep-th/0205012 | Stefan Groot Nibbelink | S. Groot Nibbelink, H.P. Nilles, M. Olechowski | Instabilities of bulk fields and anomalies on orbifolds | 29 pages, LaTeX, with figures | Nucl.Phys.B640:171-201,2002 | 10.1016/S0550-3213(02)00564-3 | null | hep-th hep-ph | null | Bulk matter modes of higher dimensional models generically become unstable in
the presence of additional matter multiplets at the branes. This quantum
instability is driven by localized Fayet-Iliopoulos terms that attract the bulk
zero modes towards the boundary branes. We study this mechanism in the
framework of a 5... | [
{
"created": "Wed, 1 May 2002 16:47:49 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Nibbelink",
"S. Groot",
""
],
[
"Nilles",
"H. P.",
""
],
[
"Olechowski",
"M.",
""
]
] | Bulk matter modes of higher dimensional models generically become unstable in the presence of additional matter multiplets at the branes. This quantum instability is driven by localized Fayet-Iliopoulos terms that attract the bulk zero modes towards the boundary branes. We study this mechanism in the framework of a 5 d... | 13.51952 | 12.749858 | 13.20909 | 12.42524 | 13.00677 | 13.038756 | 12.612597 | 13.123262 | 11.987553 | 13.049357 | 12.365287 | 12.655368 | 12.32663 | 12.292188 | 12.540146 | 12.477274 | 12.12608 | 12.910576 | 12.426478 | 12.702347 | 12.521474 |
1105.3202 | Tameem Albash | Tameem Albash, Clifford V. Johnson | Thermal Dynamics of Quarks and Mesons in N=2* Yang-Mills Theory | 17 pages, 6 figures | JHEP 1107:063,2011 | 10.1007/JHEP07(2011)063 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the dynamics of quenched fundamental matter in $\mathcal{N}=2^\ast$
supersymmetric large $N_c$ $SU(N_c)$ Yang-Mills theory, extending our earlier
work to finite temperature. We use probe D7-branes in the holographically dual
thermalized generalization of the $\mathcal{N}=2^\ast$ Pilch-Warner
gravitational ba... | [
{
"created": "Mon, 16 May 2011 20:01:42 GMT",
"version": "v1"
}
] | 2011-08-04 | [
[
"Albash",
"Tameem",
""
],
[
"Johnson",
"Clifford V.",
""
]
] | We study the dynamics of quenched fundamental matter in $\mathcal{N}=2^\ast$ supersymmetric large $N_c$ $SU(N_c)$ Yang-Mills theory, extending our earlier work to finite temperature. We use probe D7-branes in the holographically dual thermalized generalization of the $\mathcal{N}=2^\ast$ Pilch-Warner gravitational back... | 6.422347 | 5.958852 | 7.070648 | 6.173911 | 6.252511 | 6.119281 | 6.517578 | 6.094683 | 6.546196 | 7.763974 | 6.060911 | 6.160804 | 6.5473 | 6.177536 | 6.114446 | 6.235158 | 6.122829 | 6.195771 | 6.163817 | 6.288774 | 6.168771 |
hep-th/0403216 | Paolo Di Vecchia pdv | P. Di Vecchia | N=1 super Yang-Mills from D branes | 13 pages, latex | null | null | NORDITA-2004-20 | hep-th | null | We use fractional and wrapped branes to describe perturbative and
non-perturbative properties of N=1 super Yang-Mills living on their
world-volume. (Talk given at the 1st Nordstrom Symposium, Helsinki, August
2003.)
| [
{
"created": "Mon, 22 Mar 2004 14:22:27 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Di Vecchia",
"P.",
""
]
] | We use fractional and wrapped branes to describe perturbative and non-perturbative properties of N=1 super Yang-Mills living on their world-volume. (Talk given at the 1st Nordstrom Symposium, Helsinki, August 2003.) | 16.163912 | 10.101025 | 13.32937 | 10.39741 | 12.435085 | 11.831511 | 8.91773 | 8.849264 | 11.503215 | 16.396856 | 10.24217 | 11.518125 | 13.793876 | 11.991229 | 11.934402 | 12.584123 | 11.708162 | 11.40131 | 11.500561 | 14.101336 | 12.622973 |
hep-th/0603144 | Saharian | A.A. Saharian, A.S. Tarloyan | Scalar Casimir densities for cylindrically symmetric Robin boundaries | 22 pages, 5 figures | J.Phys.A39:13371-13392,2006; J.Phys.A39:13371,2006 | 10.1088/0305-4470/39/42/011 | null | hep-th quant-ph | null | Wightman function, the vacuum expectation values of the field square and the
energy-momentum tensor are investigated for a massive scalar field with general
curvature coupling parameter in the region between two coaxial cylindrical
boundaries. It is assumed that the field obeys general Robin boundary
conditions on bo... | [
{
"created": "Mon, 20 Mar 2006 14:03:07 GMT",
"version": "v1"
},
{
"created": "Wed, 3 May 2006 18:42:46 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Saharian",
"A. A.",
""
],
[
"Tarloyan",
"A. S.",
""
]
] | Wightman function, the vacuum expectation values of the field square and the energy-momentum tensor are investigated for a massive scalar field with general curvature coupling parameter in the region between two coaxial cylindrical boundaries. It is assumed that the field obeys general Robin boundary conditions on boun... | 7.272427 | 3.207396 | 8.005766 | 4.020999 | 3.727876 | 3.550354 | 3.583798 | 3.768305 | 4.033535 | 8.444512 | 3.961031 | 5.241806 | 7.220915 | 6.121892 | 5.804049 | 5.392405 | 5.192531 | 5.556808 | 5.774891 | 7.33362 | 5.720955 |
1406.6661 | Vladimir Belavin | A.A. Belavin and V.A. Belavin | Frobenius manifolds, Integrable Hierarchies and Minimal Liouville
Gravity | 17 pages; v2: typos removed, some comments added, minor corrections | null | 10.1007/JHEP09(2014)151 | FIAN-TD-2014-10 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the connection between the Frobrenius manifold and the Douglas string
equation to further investigate Minimal Liouville gravity. We search a solution
of the Douglas string equation and simultaneously a proper transformation from
the KdV to the Liouville frame which ensure the fulfilment of the conformal and
fu... | [
{
"created": "Wed, 25 Jun 2014 18:47:53 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Oct 2014 16:33:05 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Belavin",
"A. A.",
""
],
[
"Belavin",
"V. A.",
""
]
] | We use the connection between the Frobrenius manifold and the Douglas string equation to further investigate Minimal Liouville gravity. We search a solution of the Douglas string equation and simultaneously a proper transformation from the KdV to the Liouville frame which ensure the fulfilment of the conformal and fusi... | 14.533353 | 11.501353 | 14.760664 | 11.929117 | 13.507032 | 12.632349 | 13.08868 | 11.875196 | 11.903153 | 15.577156 | 12.738782 | 12.323591 | 14.271492 | 12.702552 | 12.745782 | 12.359969 | 12.215249 | 12.374429 | 12.461989 | 14.076472 | 12.645537 |
2109.14238 | Victor Chernyak | Victor L. Chernyak | Phase transitions between confinement and higgs phases in ${\cal
N}=1\,\, SU(N_c)$ SQCD with $1\leq N_F\leq N_c-1$ quark flavors | 13 pages. Most important: added at page 9 the critique of the
QCD-like model with scalar quarks used in the paper of Fradkin and Shenker
[10]. Besides, there are small improvements in the text and corrected some
typos. Results unchanged | null | null | null | hep-th hep-lat hep-ph | http://creativecommons.org/licenses/by/4.0/ | Considered is 4-dimensional ${\cal N}=1$ supersymmetric $SU(N_c)$ QCD (SQCD)
with $1\leq N_F\leq N_c-1$ equal mass quark flavors in the fundamental
representation. The gauge invariant order parameter $\rho$ is introduced
distinguishing confinement (with $\rho=0$) and higgs (with $\rho\neq 0$)
phases.
Using a number... | [
{
"created": "Wed, 29 Sep 2021 07:25:48 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Nov 2021 12:27:26 GMT",
"version": "v2"
},
{
"created": "Tue, 24 May 2022 13:15:27 GMT",
"version": "v3"
},
{
"created": "Wed, 20 Jul 2022 11:58:17 GMT",
"version": "v4"
},
{
"c... | 2023-09-14 | [
[
"Chernyak",
"Victor L.",
""
]
] | Considered is 4-dimensional ${\cal N}=1$ supersymmetric $SU(N_c)$ QCD (SQCD) with $1\leq N_F\leq N_c-1$ equal mass quark flavors in the fundamental representation. The gauge invariant order parameter $\rho$ is introduced distinguishing confinement (with $\rho=0$) and higgs (with $\rho\neq 0$) phases. Using a number of ... | 6.316154 | 5.816645 | 6.65882 | 5.737961 | 6.312557 | 6.177246 | 6.155558 | 5.737107 | 5.650172 | 6.361909 | 5.991124 | 5.771502 | 6.014933 | 5.646944 | 5.822281 | 5.902576 | 5.929708 | 5.805868 | 5.759046 | 5.985251 | 5.994833 |
2302.11630 | Tomas Ortin | Romina Ballesteros, Carmen G\'omez-Fayr\'en, Tom\'as Ort\'in and
Matteo Zatti | On scalar charges and black-hole thermodynamics | Misprints corrected and a few comments and references added. Version
to be published in JHEP | null | 10.1007/JHEP05(2023)158 | IFT-UAM/CSIC-23-018 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the first law of black hole thermodynamics in 4-dimensional
theories containing scalar and Abelian vector fields coupled to gravity using
Wald's formalism and a new definition of scalar charge as an integral over a
2-surface which satisfies a Gauss law in stationary black-hole spacetimes. We
focus on ungau... | [
{
"created": "Wed, 22 Feb 2023 20:12:40 GMT",
"version": "v1"
},
{
"created": "Tue, 16 May 2023 10:47:45 GMT",
"version": "v2"
}
] | 2023-06-07 | [
[
"Ballesteros",
"Romina",
""
],
[
"Gómez-Fayrén",
"Carmen",
""
],
[
"Ortín",
"Tomás",
""
],
[
"Zatti",
"Matteo",
""
]
] | We revisit the first law of black hole thermodynamics in 4-dimensional theories containing scalar and Abelian vector fields coupled to gravity using Wald's formalism and a new definition of scalar charge as an integral over a 2-surface which satisfies a Gauss law in stationary black-hole spacetimes. We focus on ungauge... | 11.362288 | 12.960177 | 12.965746 | 11.360464 | 12.781123 | 12.671623 | 12.201196 | 11.366661 | 11.229391 | 13.760453 | 12.134093 | 11.802114 | 11.220765 | 11.313987 | 11.286988 | 11.284241 | 11.844192 | 11.284266 | 11.624736 | 11.24708 | 11.279977 |
1906.11226 | Alfredo Perez | Emilio Ojeda and Alfredo P\'erez | Boundary conditions for General Relativity in three-dimensional
spacetimes, integrable systems and the KdV/mKdV hierarchies | 23 pages. Minor changes. Matches published version in JHEP | null | 10.1007/JHEP08(2019)079 | CECS-PHY-19/02 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a new set of boundary conditions for General Relativity on
AdS$_3$, where the dynamics of the boundary degrees of freedom are described by
two independent left and right members of the Gardner hierarchy of integrable
equations, also known as the "mixed KdV-mKdV" hierarchy. This integrable system
has the ve... | [
{
"created": "Wed, 26 Jun 2019 17:39:15 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Jul 2019 16:59:16 GMT",
"version": "v2"
},
{
"created": "Tue, 13 Aug 2019 15:45:06 GMT",
"version": "v3"
}
] | 2019-09-04 | [
[
"Ojeda",
"Emilio",
""
],
[
"Pérez",
"Alfredo",
""
]
] | We present a new set of boundary conditions for General Relativity on AdS$_3$, where the dynamics of the boundary degrees of freedom are described by two independent left and right members of the Gardner hierarchy of integrable equations, also known as the "mixed KdV-mKdV" hierarchy. This integrable system has the very... | 6.464547 | 5.876971 | 6.784127 | 6.11864 | 5.815469 | 5.980297 | 5.902526 | 6.056701 | 5.820501 | 7.505625 | 6.085412 | 6.111118 | 6.450675 | 6.171056 | 6.085651 | 6.298192 | 6.213874 | 6.140594 | 6.150253 | 6.456192 | 6.382646 |
hep-th/0610067 | Dongsu Bak | Dongsu Bak, Sang-Ok Hahn, Joohan Lee, and Phillial Oh | Supersymmetric Q-Lumps in the Grassmannian nonlinear sigma models | 11 pages, References added, Small corrections and a reference added | Phys.Rev.D75:025004,2007 | 10.1103/PhysRevD.75.025004 | UOSPT 06004 | hep-th | null | We construct the N=2 supersymmetric Grassmannian nonlinear sigma model for
the massless case and extend it to massive N=2 model by adding an appropriate
superpotential. We then study their BPS equations leading to supersymmetric
Q-lumps carrying both topological and Noether charges. These solutions are
shown to be al... | [
{
"created": "Thu, 5 Oct 2006 19:13:10 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Oct 2006 17:55:09 GMT",
"version": "v2"
},
{
"created": "Thu, 14 Dec 2006 19:33:08 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Bak",
"Dongsu",
""
],
[
"Hahn",
"Sang-Ok",
""
],
[
"Lee",
"Joohan",
""
],
[
"Oh",
"Phillial",
""
]
] | We construct the N=2 supersymmetric Grassmannian nonlinear sigma model for the massless case and extend it to massive N=2 model by adding an appropriate superpotential. We then study their BPS equations leading to supersymmetric Q-lumps carrying both topological and Noether charges. These solutions are shown to be alwa... | 17.122335 | 16.738674 | 18.675446 | 14.301445 | 13.29766 | 14.872231 | 13.975737 | 14.879424 | 14.77986 | 21.311666 | 14.118782 | 15.458168 | 16.143007 | 15.247969 | 14.625624 | 15.662494 | 15.825121 | 15.791998 | 16.149542 | 16.311243 | 15.001883 |
1712.01608 | Marek Rogatko | Marek Rogatko, Karol.I.Wysokinski | Holographic calcualtion of the magneto-transport coefficients in Dirac
semimetals | 26 pages, 7 figures | JHEP 01 (2018) 078 | 10.1007/JHEP01(2018)078 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on the gauge/gravity correspondence we have calculated the
thermoelectric kinetic and transport characteristics of the strongly
interacting materials in the presence of perpendicular magnetic field. The 3+1
dimensional system with Dirac-like spectrum is considered as a strongly
interacting one if it is close to... | [
{
"created": "Tue, 5 Dec 2017 13:04:56 GMT",
"version": "v1"
}
] | 2018-02-14 | [
[
"Rogatko",
"Marek",
""
],
[
"Wysokinski",
"Karol. I.",
""
]
] | Based on the gauge/gravity correspondence we have calculated the thermoelectric kinetic and transport characteristics of the strongly interacting materials in the presence of perpendicular magnetic field. The 3+1 dimensional system with Dirac-like spectrum is considered as a strongly interacting one if it is close to t... | 14.096052 | 12.768106 | 14.643586 | 11.317151 | 11.981935 | 13.102928 | 12.278464 | 11.490427 | 11.889071 | 16.169865 | 12.294863 | 12.526529 | 13.549956 | 12.283571 | 11.915121 | 12.284499 | 12.151618 | 12.322072 | 12.092991 | 13.473859 | 12.420308 |
hep-th/0505077 | Diego Trancanelli | Simone Giombi, Riccardo Ricci, Daniel Robles-Llana, Diego Trancanelli | Instantons and Matter in N=1/2 Supersymmetric Gauge Theory | 33 pages, harvmac; v2: minor changes, added references; v3: added
analysis of the instanton measure in section 9 | JHEP 0510 (2005) 021 | 10.1088/1126-6708/2005/10/021 | YITP-SB-05-12 | hep-th | null | We extend the instanton calculus for N=1/2 U(2) supersymmetric gauge theory
by including one massless flavor. We write the equations of motion at leading
order in the coupling constant and we solve them exactly in the
non(anti)commutativity parameter C. The profile of the matter superfield is
deformed through linear ... | [
{
"created": "Mon, 9 May 2005 19:53:24 GMT",
"version": "v1"
},
{
"created": "Thu, 12 May 2005 19:10:49 GMT",
"version": "v2"
},
{
"created": "Tue, 27 Sep 2005 19:45:32 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Giombi",
"Simone",
""
],
[
"Ricci",
"Riccardo",
""
],
[
"Robles-Llana",
"Daniel",
""
],
[
"Trancanelli",
"Diego",
""
]
] | We extend the instanton calculus for N=1/2 U(2) supersymmetric gauge theory by including one massless flavor. We write the equations of motion at leading order in the coupling constant and we solve them exactly in the non(anti)commutativity parameter C. The profile of the matter superfield is deformed through linear an... | 8.524494 | 7.557674 | 7.853708 | 7.749228 | 7.559392 | 7.561827 | 7.285446 | 7.283062 | 7.302568 | 8.608512 | 7.711121 | 7.953099 | 8.164782 | 7.725158 | 7.947427 | 8.05187 | 7.948383 | 7.866262 | 7.649289 | 8.351608 | 7.791929 |
0911.3378 | Michael R. Douglas | Michael R. Douglas | Effective potential and warp factor dynamics | 32 pages, JHEP3.cls. v4: added reference to hep-th/0507158 | JHEP 1003:071,2010 | 10.1007/JHEP03(2010)071 | null | hep-th | http://creativecommons.org/licenses/by/3.0/ | We define an effective potential describing all massless and massive modes in
the supergravity limit of string/M theory compactification which is valid
off-shell, i.e. without imposing the equations of motion. If we neglect the
warp factor, it is unbounded below, as is the case for the action in Euclidean
quantum gra... | [
{
"created": "Tue, 17 Nov 2009 19:19:21 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Nov 2009 16:29:10 GMT",
"version": "v2"
},
{
"created": "Sun, 6 Dec 2009 16:55:08 GMT",
"version": "v3"
},
{
"created": "Sat, 26 Dec 2009 18:21:51 GMT",
"version": "v4"
}
] | 2010-05-18 | [
[
"Douglas",
"Michael R.",
""
]
] | We define an effective potential describing all massless and massive modes in the supergravity limit of string/M theory compactification which is valid off-shell, i.e. without imposing the equations of motion. If we neglect the warp factor, it is unbounded below, as is the case for the action in Euclidean quantum gravi... | 14.549648 | 13.854507 | 15.311999 | 13.476756 | 13.615807 | 13.179667 | 14.281519 | 14.204557 | 13.802005 | 15.823426 | 13.953256 | 13.307352 | 13.874378 | 13.425944 | 14.172243 | 13.563551 | 13.339868 | 14.166619 | 13.167207 | 14.046146 | 13.441889 |
2303.04701 | David K. Kolchmeyer | David K. Kolchmeyer | von Neumann algebras in JT gravity | 35 pages + appendices. v2: typos fixed, appendix added | null | 10.1007/JHEP06(2023)067 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We quantize JT gravity with matter on the spatial interval with two
asymptotically AdS boundaries. We consider the von Neumann algebra generated by
the right Hamiltonian and the gravitationally dressed matter operators on the
right boundary. We prove that the commutant of this algebra is the analogously
defined left ... | [
{
"created": "Wed, 8 Mar 2023 16:42:02 GMT",
"version": "v1"
},
{
"created": "Fri, 7 Apr 2023 15:01:22 GMT",
"version": "v2"
}
] | 2023-06-28 | [
[
"Kolchmeyer",
"David K.",
""
]
] | We quantize JT gravity with matter on the spatial interval with two asymptotically AdS boundaries. We consider the von Neumann algebra generated by the right Hamiltonian and the gravitationally dressed matter operators on the right boundary. We prove that the commutant of this algebra is the analogously defined left bo... | 8.442155 | 7.424186 | 8.752768 | 6.956292 | 7.409356 | 7.471543 | 7.101226 | 6.913929 | 7.07838 | 9.314466 | 7.089264 | 7.164133 | 8.191876 | 7.265983 | 7.316794 | 7.206695 | 6.932153 | 7.072064 | 7.299563 | 8.016786 | 6.981553 |
hep-th/0409198 | Allemandi Gianluca | Gianluca Allemandi, Monica Capone, Salvatore Capozziello, Mauro
Francaviglia | Conformal aspects of Palatini approach in Extended Theories of Gravity | null | Gen.Rel.Grav.38:33-60,2006 | 10.1007/s10714-005-0208-7 | null | hep-th | null | The debate on the physical relevance of conformal transformations can be
faced by taking the Palatini approach into account to gravitational theories.
We show that conformal transformations are not only a mathematical tool to
disentangle gravitational and matter degrees of freedom (passing from the
Jordan frame to th... | [
{
"created": "Mon, 20 Sep 2004 13:15:39 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Allemandi",
"Gianluca",
""
],
[
"Capone",
"Monica",
""
],
[
"Capozziello",
"Salvatore",
""
],
[
"Francaviglia",
"Mauro",
""
]
] | The debate on the physical relevance of conformal transformations can be faced by taking the Palatini approach into account to gravitational theories. We show that conformal transformations are not only a mathematical tool to disentangle gravitational and matter degrees of freedom (passing from the Jordan frame to the ... | 10.117457 | 11.169681 | 9.498752 | 9.462773 | 10.169343 | 9.635834 | 10.246388 | 9.315908 | 9.918331 | 9.890273 | 9.80855 | 9.590716 | 8.995663 | 9.005951 | 9.604629 | 9.496651 | 9.728924 | 9.252816 | 9.859063 | 9.094173 | 10.046453 |
2309.04425 | Federico Faedo | Edoardo Colombo, Federico Faedo, Dario Martelli, Alberto Zaffaroni | Equivariant volume extremization and holography | 62 pages. v2: minor changes, subsection and appendix added,
references added. v3: minor changes, published version | null | null | null | hep-th math-ph math.DG math.MP | http://creativecommons.org/licenses/by/4.0/ | In a previous paper two of us (D.M. and A.Z.) proposed that a vast class of
gravitational extremization problems in holography can be formulated in terms
of the equivariant volume of the internal geometry, or of the cone over it. We
substantiate this claim by analysing supergravity solutions corresponding to
branes p... | [
{
"created": "Fri, 8 Sep 2023 16:38:50 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Oct 2023 17:12:47 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Jan 2024 08:15:16 GMT",
"version": "v3"
}
] | 2024-01-24 | [
[
"Colombo",
"Edoardo",
""
],
[
"Faedo",
"Federico",
""
],
[
"Martelli",
"Dario",
""
],
[
"Zaffaroni",
"Alberto",
""
]
] | In a previous paper two of us (D.M. and A.Z.) proposed that a vast class of gravitational extremization problems in holography can be formulated in terms of the equivariant volume of the internal geometry, or of the cone over it. We substantiate this claim by analysing supergravity solutions corresponding to branes par... | 12.05866 | 11.674747 | 12.989466 | 11.421007 | 12.248579 | 11.62765 | 11.623265 | 12.041465 | 10.88746 | 14.743526 | 11.549966 | 11.521063 | 11.960403 | 11.33295 | 11.053946 | 11.564011 | 11.208717 | 11.562012 | 11.244399 | 12.252733 | 10.986282 |
hep-th/9511040 | Terry Gannon | Terry Gannon | The level 2 and 3 modular invariants of SU(n) | plain tex, 8 pages | Lett.Math.Phys.39:289-298,1997 | 10.1023/A:1007369013693 | null | hep-th | null | In this paper we explicitly classify all modular invariant partition
functions for su(n) at level 2 and 3. Previously, these were known only for
level 1. The level 2 exceptionals exist at n=10, 16, and 28; the level 3
exceptionals exist at n=5, 9, and 21. One of these is new, but the others were
all anticipated by th... | [
{
"created": "Mon, 6 Nov 1995 20:34:14 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Gannon",
"Terry",
""
]
] | In this paper we explicitly classify all modular invariant partition functions for su(n) at level 2 and 3. Previously, these were known only for level 1. The level 2 exceptionals exist at n=10, 16, and 28; the level 3 exceptionals exist at n=5, 9, and 21. One of these is new, but the others were all anticipated by the ... | 10.766905 | 11.000061 | 12.014856 | 9.88916 | 10.725434 | 12.114968 | 10.293953 | 10.023302 | 10.604574 | 12.621216 | 10.054247 | 10.118794 | 11.008504 | 10.310963 | 10.608749 | 9.913268 | 10.614864 | 10.104472 | 10.266383 | 10.948634 | 9.869771 |
hep-th/0008253 | Kirill Krasnov | Kirill Krasnov (UCSB) | 3D Gravity, Point Particles and Liouville Theory | 17 pages, 3 figures, references added | Class.Quant.Grav. 18 (2001) 1291-1304 | 10.1088/0264-9381/18/7/311 | null | hep-th gr-qc | null | This paper elaborates on the bulk/boundary relation between negative
cosmological constant 3D gravity and Liouville field theory (LFT). We develop
an interpretation of LFT non-normalizable states in terms of particles moving
in the bulk. This interpretation is suggested by the fact that ``heavy'' vertex
operators of ... | [
{
"created": "Thu, 31 Aug 2000 22:05:55 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Sep 2000 23:57:28 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Krasnov",
"Kirill",
"",
"UCSB"
]
] | This paper elaborates on the bulk/boundary relation between negative cosmological constant 3D gravity and Liouville field theory (LFT). We develop an interpretation of LFT non-normalizable states in terms of particles moving in the bulk. This interpretation is suggested by the fact that ``heavy'' vertex operators of LF... | 10.387101 | 9.0363 | 10.682408 | 9.013613 | 9.248204 | 9.423883 | 8.947838 | 8.765539 | 8.873197 | 10.541662 | 8.843246 | 8.549651 | 10.296294 | 8.696953 | 8.814836 | 8.638591 | 8.590075 | 8.546486 | 8.581258 | 10.040513 | 9.159794 |
hep-th/0611075 | Masato Ito | Masato Ito | Cosmological solutions for model with a $1/H^{2}$ term | 10 pages, 2 figures, version to appear in JCAP | JCAP 0703:009,2007 | 10.1088/1475-7516/2007/03/009 | AUE-06-01 | hep-th astro-ph gr-qc hep-ph | null | We drive the cosmological solutions of five-dimensional model with $1/H^{2}$
term $(H^{2}\equiv H_{MNPQ}H^{MNPQ})$, where $H_{MNPQ}$ is 4-form field
strength. The behaviors of the scale factors and the scalar potential in
effective theory are examined.As a consequence, we show that the universe
changes from decelerat... | [
{
"created": "Tue, 7 Nov 2006 09:41:48 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Jan 2007 11:01:31 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Mar 2007 02:46:34 GMT",
"version": "v3"
},
{
"created": "Wed, 14 Mar 2007 05:21:22 GMT",
"version": "v4"
}
] | 2010-10-27 | [
[
"Ito",
"Masato",
""
]
] | We drive the cosmological solutions of five-dimensional model with $1/H^{2}$ term $(H^{2}\equiv H_{MNPQ}H^{MNPQ})$, where $H_{MNPQ}$ is 4-form field strength. The behaviors of the scale factors and the scalar potential in effective theory are examined.As a consequence, we show that the universe changes from decelerated... | 11.935658 | 8.782974 | 10.163591 | 8.584446 | 10.319986 | 9.716731 | 9.283347 | 9.206921 | 8.839367 | 10.750865 | 9.062022 | 9.197848 | 10.503722 | 9.537825 | 10.229119 | 10.435185 | 10.202418 | 9.975533 | 10.026268 | 10.366759 | 9.559434 |
hep-th/0607077 | Yann Mambrini | E. Dudas, Y. Mambrini | Moduli stabilization with positive vacuum energy | 20 pages, 1 figure | JHEP0610:044,2006 | 10.1088/1126-6708/2006/10/044 | null | hep-th hep-ph | null | We study the effect of anomalous U(1) gauge groups in string theory
compactification with fluxes. We find that, in a gauge invariant formulation,
consistent AdS vacua appear breaking spontaneously supergravity. Non vanishing
D-terms from the anomalous symmetry act as an uplifting potential and could
allow for de Sitt... | [
{
"created": "Wed, 12 Jul 2006 14:06:27 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Dudas",
"E.",
""
],
[
"Mambrini",
"Y.",
""
]
] | We study the effect of anomalous U(1) gauge groups in string theory compactification with fluxes. We find that, in a gauge invariant formulation, consistent AdS vacua appear breaking spontaneously supergravity. Non vanishing D-terms from the anomalous symmetry act as an uplifting potential and could allow for de Sitter... | 9.119134 | 8.705288 | 9.114852 | 8.33671 | 8.293612 | 8.974811 | 8.936259 | 8.718049 | 7.772586 | 8.543053 | 8.582887 | 8.295688 | 8.398615 | 8.518612 | 8.563729 | 8.939396 | 8.375645 | 8.56521 | 8.324079 | 8.821679 | 8.717315 |
2311.18290 | Pratik Rath | Xi Dong, Donald Marolf and Pratik Rath | Constrained HRT Surfaces and their Entropic Interpretation | 16 pages, 3 figures, minor edits in v2 | null | null | null | hep-th gr-qc quant-ph | http://creativecommons.org/licenses/by/4.0/ | Consider two boundary subregions $A$ and $B$ that lie in a common boundary
Cauchy surface, and consider also the associated HRT surface $\gamma_B$ for
$B$. In that context, the constrained HRT surface $\gamma_{A:B}$ can be defined
as the codimension-2 bulk surface anchored to $A$ that is obtained by a maximin
constru... | [
{
"created": "Thu, 30 Nov 2023 06:50:40 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Dec 2023 16:00:53 GMT",
"version": "v2"
},
{
"created": "Wed, 31 Jan 2024 20:18:39 GMT",
"version": "v3"
}
] | 2024-02-02 | [
[
"Dong",
"Xi",
""
],
[
"Marolf",
"Donald",
""
],
[
"Rath",
"Pratik",
""
]
] | Consider two boundary subregions $A$ and $B$ that lie in a common boundary Cauchy surface, and consider also the associated HRT surface $\gamma_B$ for $B$. In that context, the constrained HRT surface $\gamma_{A:B}$ can be defined as the codimension-2 bulk surface anchored to $A$ that is obtained by a maximin construct... | 4.735158 | 4.523174 | 5.024076 | 4.526038 | 4.962245 | 4.75837 | 4.765043 | 4.684839 | 4.536259 | 5.38903 | 4.4167 | 4.490676 | 4.66712 | 4.376172 | 4.450255 | 4.544991 | 4.546756 | 4.474039 | 4.438714 | 4.599533 | 4.460427 |
hep-th/9610102 | Alexander Sevrin | Alexander Sevrin and Jan Troost | Off-Shell Formulation of N=2 Non-Linear Sigma-Models | 22 pages, LaTeX | Nucl.Phys. B492 (1997) 623-646 | 10.1016/S0550-3213(97)00103-X | VUB/TENA/96/06 | hep-th | null | We study d=2, N=(2,2) non-linear sigma-models in (2,2) superspace. By
analyzing the most general constraints on a superfield, we show that through an
appropriate choice of coordinates, there are no other superfields than chiral,
twisted chiral and semi-chiral ones. We study the resulting sigma-models and we
speculate... | [
{
"created": "Tue, 15 Oct 1996 09:57:41 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Sevrin",
"Alexander",
""
],
[
"Troost",
"Jan",
""
]
] | We study d=2, N=(2,2) non-linear sigma-models in (2,2) superspace. By analyzing the most general constraints on a superfield, we show that through an appropriate choice of coordinates, there are no other superfields than chiral, twisted chiral and semi-chiral ones. We study the resulting sigma-models and we speculate o... | 5.690876 | 5.24305 | 6.071129 | 5.033395 | 5.14408 | 5.063474 | 4.919671 | 5.1017 | 5.047773 | 6.520109 | 5.229218 | 5.083675 | 5.773462 | 5.149358 | 5.137753 | 5.372178 | 5.202506 | 5.136153 | 5.208872 | 5.707618 | 5.254935 |
1309.4185 | Luis F. Urrutia | C.A. Escobar and L. F. Urrutia | The invariants of the electromagnetic field | 6 pages, no figures, revtex4, New sections I and II. New references
added. The construction in sections III,IV,V and in the Appendix is the same
as in version 1 | Journal of Mathematical Physics 55, 032902 (2014) | 10.1063/1.4868478 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a constructive proof that all gauge invariant Lorentz scalars in
Electrodynamics can be expressed as a function of the quadratic ones.
| [
{
"created": "Tue, 17 Sep 2013 05:21:28 GMT",
"version": "v1"
},
{
"created": "Sun, 20 Apr 2014 01:42:29 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Escobar",
"C. A.",
""
],
[
"Urrutia",
"L. F.",
""
]
] | We present a constructive proof that all gauge invariant Lorentz scalars in Electrodynamics can be expressed as a function of the quadratic ones. | 21.608311 | 14.109676 | 12.479263 | 10.928173 | 16.664045 | 13.043983 | 13.185682 | 12.809155 | 14.13047 | 9.517136 | 13.202336 | 14.914547 | 13.311122 | 13.559251 | 13.744662 | 14.931825 | 14.91067 | 14.481861 | 13.538748 | 13.632911 | 13.218916 |
1706.05221 | Zoltan Bajnok | Ines Aniceto, Zoltan Bajnok, Tamas Gombor, Minkyoo Kim, Laszlo Palla | On integrable boundaries in the 2 dimensional $O(N)$ $\sigma$-models | Dedicated to the memory of Petr Kulish, 31 pages, 1 figure, v2:
conformality and integrability of the boundary conditions are distinguished | null | 10.1088/1751-8121/aa8205 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We make an attempt to map the integrable boundary conditions for 2
dimensional non-linear O(N) $\sigma$-models. We do it at various levels:
classically, by demanding the existence of infinitely many conserved local
charges and also by constructing the double row transfer matrix from the Lax
connection, which leads to... | [
{
"created": "Fri, 16 Jun 2017 11:24:58 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Jul 2017 14:46:52 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Aniceto",
"Ines",
""
],
[
"Bajnok",
"Zoltan",
""
],
[
"Gombor",
"Tamas",
""
],
[
"Kim",
"Minkyoo",
""
],
[
"Palla",
"Laszlo",
""
]
] | We make an attempt to map the integrable boundary conditions for 2 dimensional non-linear O(N) $\sigma$-models. We do it at various levels: classically, by demanding the existence of infinitely many conserved local charges and also by constructing the double row transfer matrix from the Lax connection, which leads to t... | 8.970542 | 8.011933 | 9.937556 | 7.875656 | 9.035825 | 8.623775 | 9.038382 | 7.985432 | 7.835413 | 8.97022 | 8.014811 | 8.122047 | 10.116621 | 7.938674 | 8.333211 | 8.216689 | 7.907363 | 8.042628 | 8.233562 | 8.906893 | 8.078317 |
0708.2287 | Eric Bergshoeff | Eric Bergshoeff, Jelle Hartong and Dmitri Sorokin | Q7-branes and their coupling to IIB supergravity | 31 pages, Latex file | JHEP 0712:079,2007 | 10.1088/1126-6708/2007/12/079 | null | hep-th | null | We show how, by making use of a new basis of the IIB supergravity
axion-dilaton coset, SL(2,R)/SO(2), 7-branes that belong to different conjugacy
classes of the duality group SL(2,R) naturally couple to IIB supergravity with
appropriate source terms characterized by an SL(2,R) charge matrix Q. The
conjugacy classes a... | [
{
"created": "Fri, 17 Aug 2007 15:21:47 GMT",
"version": "v1"
}
] | 2009-11-18 | [
[
"Bergshoeff",
"Eric",
""
],
[
"Hartong",
"Jelle",
""
],
[
"Sorokin",
"Dmitri",
""
]
] | We show how, by making use of a new basis of the IIB supergravity axion-dilaton coset, SL(2,R)/SO(2), 7-branes that belong to different conjugacy classes of the duality group SL(2,R) naturally couple to IIB supergravity with appropriate source terms characterized by an SL(2,R) charge matrix Q. The conjugacy classes are... | 5.78066 | 6.082091 | 6.44775 | 5.73427 | 6.537462 | 6.25913 | 6.473015 | 5.89852 | 5.805787 | 7.407054 | 5.743268 | 5.733323 | 6.143576 | 5.625174 | 6.020534 | 5.704072 | 5.794538 | 5.773458 | 5.703985 | 6.188035 | 5.708019 |
2307.08742 | Xiaoyang Shen | Chi-Ming Chang, Xiaoyang Shen | Disordered $\mathcal{N} = (2, 2)$ Supersymmetric Field Theories | 43 pages, 6 figures | SciPost Phys. 16, 140 (2024) | 10.21468/SciPostPhys.16.5.140 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a large class of $\mathcal{N} = (2, 2)$ supersymmetric field
theories in two dimensions, which contains the Murugan-Stanford-Witten model,
and can be naturally regarded as a disordered generalization of the
two-dimensional Landau-Ginzburg models. We analyze the two and four-point
functions of chiral su... | [
{
"created": "Mon, 17 Jul 2023 18:00:02 GMT",
"version": "v1"
}
] | 2024-06-05 | [
[
"Chang",
"Chi-Ming",
""
],
[
"Shen",
"Xiaoyang",
""
]
] | We investigate a large class of $\mathcal{N} = (2, 2)$ supersymmetric field theories in two dimensions, which contains the Murugan-Stanford-Witten model, and can be naturally regarded as a disordered generalization of the two-dimensional Landau-Ginzburg models. We analyze the two and four-point functions of chiral supe... | 7.203748 | 7.292463 | 8.776031 | 6.917909 | 6.918153 | 6.942303 | 7.223752 | 7.033412 | 6.78236 | 9.575655 | 6.742131 | 6.85354 | 7.69942 | 6.775109 | 6.847591 | 6.885674 | 7.030566 | 6.707381 | 6.830557 | 7.432101 | 6.960156 |
2401.09307 | Leihua Liu | Tao Li and Lei-Hua Liu | Inflationary Krylov complexity | matching the publishing version | JHEP04(2024)123 | 10.1007/JHEP04(2024)123 | null | hep-th astro-ph.CO gr-qc hep-ph quant-ph | http://creativecommons.org/licenses/by/4.0/ | In this work, we have systematically investigated the Krylov complexity of
curvature perturbation for the modified dispersion relation in inflation, using
the algorithm in closed system and open system. Our analysis could be applied
to the most inflationary models. Following the Lanczos algorithm, we find the
very ea... | [
{
"created": "Wed, 17 Jan 2024 16:17:51 GMT",
"version": "v1"
},
{
"created": "Sat, 20 Jan 2024 16:37:49 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Feb 2024 08:00:47 GMT",
"version": "v3"
},
{
"created": "Thu, 23 May 2024 08:06:31 GMT",
"version": "v4"
}
] | 2024-05-24 | [
[
"Li",
"Tao",
""
],
[
"Liu",
"Lei-Hua",
""
]
] | In this work, we have systematically investigated the Krylov complexity of curvature perturbation for the modified dispersion relation in inflation, using the algorithm in closed system and open system. Our analysis could be applied to the most inflationary models. Following the Lanczos algorithm, we find the very earl... | 13.366854 | 13.478341 | 13.286695 | 12.618665 | 13.164273 | 13.702571 | 13.24608 | 12.754585 | 13.230683 | 14.272618 | 12.655594 | 12.434288 | 13.191004 | 12.462489 | 12.823281 | 12.456895 | 12.879629 | 12.30565 | 12.62978 | 12.895924 | 12.586745 |
hep-th/0001025 | Calin Iuliu Lazaroiu | Brian R. Greene, C. I. Lazaroiu | Collapsing D-Branes in Calabi-Yau Moduli Space: I | 77 pages, 15 figures | Nucl.Phys. B604 (2001) 181-255 | 10.1016/S0550-3213(01)00154-7 | CU-TP 963 | hep-th math.AG | null | We study the quantum volume of D-branes wrapped around various cycles in
Calabi-Yau manifolds, as the manifold's moduli are varied. In particular, we
focus on the behaviour of these D-branes near phase transitions between
distinct low energy physical descriptions of the resulting string theory.
Whereas previous studi... | [
{
"created": "Thu, 6 Jan 2000 22:56:57 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Feb 2000 05:33:37 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Greene",
"Brian R.",
""
],
[
"Lazaroiu",
"C. I.",
""
]
] | We study the quantum volume of D-branes wrapped around various cycles in Calabi-Yau manifolds, as the manifold's moduli are varied. In particular, we focus on the behaviour of these D-branes near phase transitions between distinct low energy physical descriptions of the resulting string theory. Whereas previous studies... | 11.858593 | 10.891307 | 12.235574 | 10.167892 | 11.513537 | 11.233257 | 10.422083 | 11.387588 | 10.379271 | 13.330811 | 10.593124 | 10.538385 | 11.643904 | 10.782819 | 10.569141 | 10.422711 | 10.481808 | 10.677574 | 10.57333 | 11.198439 | 10.637144 |
0812.1311 | Irina Radinschi | I. Radinschi, F. Rahaman, M. Kalam and K. Chakraborty | Classical electron model with non static conformal symmetry | Title changed, LaTex | Fizika B, 19(3), 125-134, (2010) | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Lorentz proposed a classical model of electron in which electron was assumed
to have only 'electromagnetic mass'. We modeled electron as charged anisotropic
perfect fluid sphere admitting non static conformal symmetry. It is noticed
that the pressure and density fail to be regular at the origin but effective
gravitat... | [
{
"created": "Sat, 6 Dec 2008 20:00:44 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Dec 2010 14:40:37 GMT",
"version": "v2"
}
] | 2011-10-11 | [
[
"Radinschi",
"I.",
""
],
[
"Rahaman",
"F.",
""
],
[
"Kalam",
"M.",
""
],
[
"Chakraborty",
"K.",
""
]
] | Lorentz proposed a classical model of electron in which electron was assumed to have only 'electromagnetic mass'. We modeled electron as charged anisotropic perfect fluid sphere admitting non static conformal symmetry. It is noticed that the pressure and density fail to be regular at the origin but effective gravitatio... | 13.319861 | 14.978269 | 13.821868 | 12.965365 | 12.396014 | 12.854361 | 14.880705 | 12.602688 | 14.864514 | 14.400907 | 14.381123 | 13.047292 | 12.904917 | 12.615434 | 12.187726 | 12.031333 | 12.335611 | 12.787638 | 12.944057 | 12.447154 | 13.137297 |
1702.02164 | Edoardo Vescovi | V. Forini, A.A. Tseytlin, E. Vescovi | Perturbative computation of string one-loop corrections to Wilson loop
minimal surfaces in $AdS_5 \times S^5$ | 32 pages, one reference added, typos corrected | null | 10.1007/JHEP03(2017)003 | HU-EP-17/02, Imperial-TP-AAT-2017-03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the computation of the 1-loop string correction to the "latitude"
minimal surface in $AdS_5 \times S^5$ representing 1/4 BPS Wilson loop in
planar $\cal N$=4 SYM theory previously addressed in arXiv:1512.00841 and
arXiv:1601.04708. We resolve the problem of matching with the subleading term
in the strong c... | [
{
"created": "Tue, 7 Feb 2017 19:08:09 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Feb 2017 19:36:31 GMT",
"version": "v2"
}
] | 2017-04-05 | [
[
"Forini",
"V.",
""
],
[
"Tseytlin",
"A. A.",
""
],
[
"Vescovi",
"E.",
""
]
] | We revisit the computation of the 1-loop string correction to the "latitude" minimal surface in $AdS_5 \times S^5$ representing 1/4 BPS Wilson loop in planar $\cal N$=4 SYM theory previously addressed in arXiv:1512.00841 and arXiv:1601.04708. We resolve the problem of matching with the subleading term in the strong cou... | 7.215276 | 7.476333 | 8.880562 | 7.293383 | 7.11838 | 7.326511 | 6.896492 | 6.488808 | 7.036872 | 9.159904 | 6.943648 | 7.017994 | 7.884323 | 7.380887 | 7.25616 | 7.092734 | 7.31636 | 7.142061 | 7.287122 | 7.618752 | 6.966678 |
1410.7985 | Diego Chialva | Diego Chialva | On UltraViolet effects in protected inflationary models | 4 pages plus bibliography | null | null | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inflationary models are usually UV sensitive. Several mechanism have been
proposed to protect the necessary features of the potential, and most notably
(softly broken) global symmetries as shift-symmetry. We show that, even in
presence of these protecting mechanisms, the models maintain a serious
UV-dependence. Via a... | [
{
"created": "Wed, 29 Oct 2014 13:56:11 GMT",
"version": "v1"
}
] | 2014-11-03 | [
[
"Chialva",
"Diego",
""
]
] | Inflationary models are usually UV sensitive. Several mechanism have been proposed to protect the necessary features of the potential, and most notably (softly broken) global symmetries as shift-symmetry. We show that, even in presence of these protecting mechanisms, the models maintain a serious UV-dependence. Via an ... | 21.008301 | 19.12759 | 18.457941 | 18.17429 | 20.499434 | 18.924788 | 20.612526 | 20.143435 | 17.687666 | 19.960957 | 17.775503 | 18.213299 | 17.79841 | 16.983187 | 17.825687 | 18.087072 | 18.222147 | 17.679554 | 17.06484 | 18.133587 | 17.213682 |
1805.00233 | Hisham Sati | Hisham Sati, Urs Schreiber | Higher T-duality in M-theory via local supersymmetry | 7 pages, concise physics letter companion to the mathematically
rigorous treatment arXiv:1803.05634; to appear in Phys. Lett. B | null | 10.1016/j.physletb.2018.04.058 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By analyzing super-torsion and brane super-cocycles, we derive a new duality
in M-theory, which takes the form of a higher version of T-duality in string
theory. This involves a new topology change mechanism abelianizing the 3-sphere
associated with the C-field topology to the 517-torus associated with
exceptional-ge... | [
{
"created": "Tue, 1 May 2018 08:24:23 GMT",
"version": "v1"
}
] | 2018-05-23 | [
[
"Sati",
"Hisham",
""
],
[
"Schreiber",
"Urs",
""
]
] | By analyzing super-torsion and brane super-cocycles, we derive a new duality in M-theory, which takes the form of a higher version of T-duality in string theory. This involves a new topology change mechanism abelianizing the 3-sphere associated with the C-field topology to the 517-torus associated with exceptional-gene... | 20.403366 | 19.686441 | 24.185167 | 19.916965 | 20.987928 | 20.414085 | 20.414347 | 20.029402 | 18.675329 | 23.18602 | 18.228371 | 18.125435 | 22.360909 | 19.103617 | 19.943832 | 19.562571 | 18.32283 | 18.412552 | 18.74032 | 22.475965 | 19.028751 |
1511.04784 | M. P. Garcia del Moral | Maria Pikar Garcia del Moral and Alvaro Restuccia | 10D Massive Type IIA Supergravities as the uplift of Parabolic M2-brane
Torus bundles | latex, 4pg, Contribution to the proceedings of "The String Theory
Universe" workshop in Leuven, 7-11 Sept 2015 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We remark that the two 10D massive deformations of the $N=2$ maximal type IIA
supergravity (Romans and HLW supergravity) are associated to the low energy
limit of the uplift to 10D of M2-brane torus bundles with parabolic monodromy
linearly and non-linearly realized respectively. Romans supergravity
corresponds to M2... | [
{
"created": "Sun, 15 Nov 2015 23:46:48 GMT",
"version": "v1"
}
] | 2015-11-17 | [
[
"del Moral",
"Maria Pikar Garcia",
""
],
[
"Restuccia",
"Alvaro",
""
]
] | We remark that the two 10D massive deformations of the $N=2$ maximal type IIA supergravity (Romans and HLW supergravity) are associated to the low energy limit of the uplift to 10D of M2-brane torus bundles with parabolic monodromy linearly and non-linearly realized respectively. Romans supergravity corresponds to M2-b... | 13.789578 | 15.328666 | 16.959356 | 12.59962 | 14.603 | 13.934484 | 13.964441 | 13.517206 | 12.997972 | 19.160215 | 12.599112 | 12.965975 | 13.681013 | 12.761411 | 12.152377 | 12.614944 | 12.442596 | 12.552802 | 12.728612 | 12.846242 | 11.974035 |
1705.04124 | Malin G\"oteman | Malin G\"oteman | The complex world of superstrings: On semichiral sigma models | PhD thesis: Digital Comprehensive Summaries of Uppsala Dissertations
from the Faculty of Science and Technology 989. 139 pp. Uppsala | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Non-linear sigma models with extended supersymmetry have constrained target
space geometries, and can serve as effective tools for investigating and
constructing new geometries. Analyzing the geometrical and topological
properties of sigma models is necessary to understand the underlying structures
of string theory. ... | [
{
"created": "Thu, 11 May 2017 12:08:29 GMT",
"version": "v1"
}
] | 2017-05-12 | [
[
"Göteman",
"Malin",
""
]
] | Non-linear sigma models with extended supersymmetry have constrained target space geometries, and can serve as effective tools for investigating and constructing new geometries. Analyzing the geometrical and topological properties of sigma models is necessary to understand the underlying structures of string theory. Th... | 5.368088 | 5.597589 | 6.033254 | 5.328922 | 5.565562 | 5.355645 | 5.094535 | 5.376301 | 5.332142 | 6.255743 | 5.231953 | 5.266626 | 5.715441 | 5.424253 | 5.411272 | 5.408645 | 5.348899 | 5.44009 | 5.44096 | 5.657267 | 5.348081 |
2004.02735 | Shun-Qing Zhang | Congkao Wen, Shun-Qing Zhang | D3-Brane Loop Amplitudes from M5-Brane Tree Amplitudes | 36 pages, 6 figures; v2: minor changes to match accepted version in
JHEP, references added | null | 10.1007/JHEP07(2020)098 | QMUL-PH-20-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study loop corrections to scattering amplitudes in the world-volume theory
of a probe D3-brane, which is described by the supersymmetric Dirac-Born-Infeld
theory. We show that the D3-brane loop superamplitudes can be obtained from the
tree-level superamplitudes in the world-volume theory of a probe M5-brane (or
D5... | [
{
"created": "Mon, 6 Apr 2020 15:30:11 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Jul 2020 11:47:13 GMT",
"version": "v2"
}
] | 2020-08-26 | [
[
"Wen",
"Congkao",
""
],
[
"Zhang",
"Shun-Qing",
""
]
] | We study loop corrections to scattering amplitudes in the world-volume theory of a probe D3-brane, which is described by the supersymmetric Dirac-Born-Infeld theory. We show that the D3-brane loop superamplitudes can be obtained from the tree-level superamplitudes in the world-volume theory of a probe M5-brane (or D5-b... | 5.067316 | 4.867974 | 5.657676 | 4.928572 | 5.108352 | 4.962916 | 4.820626 | 4.759969 | 4.737755 | 5.59914 | 4.70914 | 4.905251 | 5.116411 | 4.859735 | 4.905593 | 4.978747 | 4.912097 | 4.794387 | 4.822907 | 4.989451 | 4.818312 |
1005.3519 | Erich Poppitz | Erich Poppitz, Mithat Unsal | AdS/CFT and large-N volume independence | 4 pages, 2 figures; references and comments added | Phys.Rev.D82:066002,2010 | 10.1103/PhysRevD.82.066002 | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Eguchi-Kawai reduction in the strong-coupling domain of gauge
theories via the gravity dual of N=4 super-Yang-Mills on R^3xS^1. We show that
D-branes geometrize volume independence in the center-symmetric vacuum and give
supergravity predictions for the range of validity of reduced large-N models at
stro... | [
{
"created": "Wed, 19 May 2010 18:54:31 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Jun 2010 19:51:35 GMT",
"version": "v2"
}
] | 2014-11-21 | [
[
"Poppitz",
"Erich",
""
],
[
"Unsal",
"Mithat",
""
]
] | We study the Eguchi-Kawai reduction in the strong-coupling domain of gauge theories via the gravity dual of N=4 super-Yang-Mills on R^3xS^1. We show that D-branes geometrize volume independence in the center-symmetric vacuum and give supergravity predictions for the range of validity of reduced large-N models at strong... | 11.460106 | 12.027366 | 15.864101 | 11.964713 | 10.140411 | 11.054995 | 11.657262 | 10.372121 | 10.65561 | 13.721845 | 10.951459 | 10.961056 | 11.490819 | 11.252829 | 11.809173 | 11.933615 | 11.288325 | 12.052362 | 10.868934 | 12.084586 | 10.73339 |
1006.1986 | Hrvoje Nikolic | H. Nikolic | Superluminal velocities and nonlocality in relativistic mechanics with
scalar potential | 16 pages, Sec. 4.3 and Appendix revised | null | null | null | hep-th hep-ph physics.class-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Even though the usual form of relativistic mechanics does not allow
superluminal particle velocities and nonlocal interactions, these features are
not forbidden by relativity itself. To understand this on a deeper level, we
study a generalized form of relativistic mechanics in which the particle is
influenced not onl... | [
{
"created": "Thu, 10 Jun 2010 09:47:55 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jun 2010 12:22:12 GMT",
"version": "v2"
},
{
"created": "Fri, 18 Jun 2010 11:22:57 GMT",
"version": "v3"
}
] | 2011-09-28 | [
[
"Nikolic",
"H.",
""
]
] | Even though the usual form of relativistic mechanics does not allow superluminal particle velocities and nonlocal interactions, these features are not forbidden by relativity itself. To understand this on a deeper level, we study a generalized form of relativistic mechanics in which the particle is influenced not only ... | 8.543011 | 9.227407 | 8.291962 | 8.263265 | 9.683271 | 9.138795 | 8.39614 | 8.604514 | 8.549665 | 8.899935 | 8.918367 | 7.822979 | 7.926714 | 8.006098 | 8.090767 | 8.119668 | 8.531329 | 7.989115 | 8.164434 | 8.259934 | 8.044628 |
0910.5122 | Stefan Hohenegger | Matthias R. Gaberdiel and Stefan Hohenegger | Manifestly Supersymmetric RG Flows | 22 pages; references added, minor changes | JHEP 1002:052,2010 | 10.1007/JHEP02(2010)052 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Renormalisation group (RG) equations in two-dimensional N=1 supersymmetric
field theories with boundary are studied. It is explained how a manifestly N=1
supersymmetric scheme can be chosen, and within this scheme the RG equations
are determined to next-to-leading order. We also use these results to revisit
the quest... | [
{
"created": "Tue, 27 Oct 2009 14:01:34 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Jan 2010 08:40:00 GMT",
"version": "v2"
}
] | 2010-03-12 | [
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Hohenegger",
"Stefan",
""
]
] | Renormalisation group (RG) equations in two-dimensional N=1 supersymmetric field theories with boundary are studied. It is explained how a manifestly N=1 supersymmetric scheme can be chosen, and within this scheme the RG equations are determined to next-to-leading order. We also use these results to revisit the questio... | 10.88049 | 8.88954 | 10.372169 | 8.459857 | 9.385695 | 9.342047 | 8.88064 | 8.674029 | 8.391245 | 11.309941 | 8.769867 | 9.690741 | 11.42726 | 9.50587 | 9.68034 | 10.010241 | 9.732594 | 9.446032 | 9.648728 | 10.765483 | 9.372643 |
hep-th/0405251 | El Hassan Saidi | Malika Ait Ben Haddou, El Hassan Saidi | Hyperbolic Invariance | 41 pages, 5 figures | null | null | Lab/UFR-HEP0401/GNPHE0401 | hep-th | null | Motivated by the study of duality cascades in supersymmetric quiver gauge
theories beyond affine models, we develop in this paper the analysis of a class
of simply laced hyperbolic Lie algebras. These are specific generalizations of
affine ADE symmetries which form a particular subclass of the so-called
Indefinite Li... | [
{
"created": "Thu, 27 May 2004 18:30:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Haddou",
"Malika Ait Ben",
""
],
[
"Saidi",
"El Hassan",
""
]
] | Motivated by the study of duality cascades in supersymmetric quiver gauge theories beyond affine models, we develop in this paper the analysis of a class of simply laced hyperbolic Lie algebras. These are specific generalizations of affine ADE symmetries which form a particular subclass of the so-called Indefinite Lie ... | 12.402078 | 12.164583 | 12.445956 | 11.748478 | 12.516528 | 12.880406 | 13.636292 | 12.427936 | 11.832348 | 14.230895 | 11.754689 | 11.948695 | 12.359666 | 11.555527 | 12.090497 | 11.622705 | 11.7379 | 11.85181 | 11.765942 | 12.21008 | 11.807641 |
0812.3273 | Ed Threlfall | Nick Evans and Ed Threlfall | Chemical Potential in the Gravity Dual of a 2+1 Dimensional System | 10 pages, 10 eps figures, version for publication | null | 10.1103/PhysRevD.79.066008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study probe D5 branes in D3 brane AdS_5 and AdS_5-Schwarzschild
backgrounds as a prototype dual description of strongly coupled 2+1 dimensional
quasi-particles. We introduce a chemical potential through the U(1)_R symmetry
group, U(1) baryon number and a U(1) of isospin in the multi-flavour case. We
find the appro... | [
{
"created": "Wed, 17 Dec 2008 12:13:58 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Feb 2009 12:07:18 GMT",
"version": "v2"
}
] | 2009-11-13 | [
[
"Evans",
"Nick",
""
],
[
"Threlfall",
"Ed",
""
]
] | We study probe D5 branes in D3 brane AdS_5 and AdS_5-Schwarzschild backgrounds as a prototype dual description of strongly coupled 2+1 dimensional quasi-particles. We introduce a chemical potential through the U(1)_R symmetry group, U(1) baryon number and a U(1) of isospin in the multi-flavour case. We find the appropr... | 10.461886 | 8.32006 | 11.447603 | 7.791067 | 9.323233 | 8.117514 | 7.777684 | 7.4817 | 7.707294 | 10.911119 | 8.47874 | 8.871564 | 10.414609 | 9.33302 | 9.305671 | 9.075988 | 9.254009 | 8.854773 | 8.7334 | 10.180277 | 9.16792 |
1202.3692 | Pierre Vanhove | Piotr Tourkine, Pierre Vanhove | An R^4 non-renormalisation theorem in N=4 supergravity | v2: added comments about one-loop UV divergences. Assorted stylistic
corrections. Added references. v3: Eq. III.21 corrected and assorted minor
corrections and clarifications. Version to be published. v4: minor
corrections. 18 pages. one figure | null | 10.1088/0264-9381/29/11/115006 | IHES/P/12/02; IPHT-t11/189 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the four-graviton amplitudes in CHL constructions providing
four-dimensional N=4 models with various numbers of vector multiplets. We show
that in these models the two-loop amplitude has a prefactor of d^2R^4. This
implies a non-renormalisation theorem for the R^4 term, which forbids the
appearance of a t... | [
{
"created": "Thu, 16 Feb 2012 20:52:34 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Mar 2012 08:10:04 GMT",
"version": "v2"
},
{
"created": "Wed, 2 May 2012 08:26:09 GMT",
"version": "v3"
},
{
"created": "Mon, 6 Aug 2012 19:47:04 GMT",
"version": "v4"
}
] | 2015-06-04 | [
[
"Tourkine",
"Piotr",
""
],
[
"Vanhove",
"Pierre",
""
]
] | We consider the four-graviton amplitudes in CHL constructions providing four-dimensional N=4 models with various numbers of vector multiplets. We show that in these models the two-loop amplitude has a prefactor of d^2R^4. This implies a non-renormalisation theorem for the R^4 term, which forbids the appearance of a thr... | 9.265655 | 9.323286 | 9.017148 | 8.1342 | 9.095915 | 9.462329 | 8.24537 | 7.894685 | 7.955268 | 10.42417 | 8.758552 | 8.581356 | 9.013959 | 8.190328 | 8.739035 | 8.156063 | 8.524277 | 8.688779 | 8.424562 | 9.079899 | 8.338805 |
hep-th/0603169 | Martin Land | Martin Land | Duality in Off-Shell Electromagnetism | 18 pages | Found.Phys.35:1245,2005 | 10.1007/s10701-005-6408-x | null | hep-th | null | In this paper, we examine the Dirac monopole in the framework of Off-Shell
Electromagnetism, the five dimensional U(1) gauge theory associated with
Stueckelberg-Schrodinger relativistic quantum theory. After reviewing the Dirac
model in four dimensions, we show that the structure of the five dimensional
theory preven... | [
{
"created": "Tue, 21 Mar 2006 14:24:43 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Land",
"Martin",
""
]
] | In this paper, we examine the Dirac monopole in the framework of Off-Shell Electromagnetism, the five dimensional U(1) gauge theory associated with Stueckelberg-Schrodinger relativistic quantum theory. After reviewing the Dirac model in four dimensions, we show that the structure of the five dimensional theory prevents... | 7.638084 | 7.387124 | 7.560005 | 7.332514 | 7.950109 | 8.389812 | 7.754615 | 7.392027 | 7.199135 | 8.395706 | 7.726121 | 7.363394 | 7.397921 | 7.193846 | 7.351614 | 7.400713 | 7.329805 | 7.268566 | 7.207708 | 7.187052 | 7.170772 |
hep-th/9509165 | Cobi Sonnenschein | Ofer Aharony, Michael E. Peskin, Jacob Sonnenschein, Shimon
Yankielowicz | Duality and other Exotic Gauge Dynamics in Softly Broken Supersymmetric
QCD | 13 pages | null | null | TAUP-2291-95 | hep-th hep-lat hep-ph | null | We analyze the theory of softly broken supersymmetric $QCD$. Exotic behavior
like spontaneously broken baryon number, massless composite fermions and
Seiberg's duality seems to persist also in the presence of (small) soft
supersymmetry breaking. We argue that certain, specially tailored, lattice
simulations may be ab... | [
{
"created": "Thu, 28 Sep 1995 13:58:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Aharony",
"Ofer",
""
],
[
"Peskin",
"Michael E.",
""
],
[
"Sonnenschein",
"Jacob",
""
],
[
"Yankielowicz",
"Shimon",
""
]
] | We analyze the theory of softly broken supersymmetric $QCD$. Exotic behavior like spontaneously broken baryon number, massless composite fermions and Seiberg's duality seems to persist also in the presence of (small) soft supersymmetry breaking. We argue that certain, specially tailored, lattice simulations may be able... | 13.35857 | 9.484676 | 12.442778 | 11.6928 | 9.547432 | 10.13608 | 9.710252 | 10.231012 | 10.618031 | 14.052674 | 10.355707 | 11.456442 | 12.315379 | 11.537452 | 11.45376 | 11.766845 | 11.62237 | 12.503985 | 11.558078 | 12.682675 | 11.765145 |
hep-th/0505067 | P. S. Howe | P.S. Howe, U. Lindstrom, L. Wulff | Superstrings with boundary fermions | 26 pages. Typographical errors corrected. References added | JHEP 0508 (2005) 041 | 10.1088/1126-6708/2005/08/041 | KCL-TH-05-03, UUITP-08/05, HIP-2005-17/TH, USITP-05-01 | hep-th | null | The Green-Schwarz action for an open superstring with additional boundary
fermions, representing Chan-Paton factors, is studied at the classical level.
The boundary geometry is described by a bundle, with fermionic fibres, over the
super worldvolume of a D-brane together with a map from the total space into
the type ... | [
{
"created": "Mon, 9 May 2005 15:43:05 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jun 2005 14:32:43 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Howe",
"P. S.",
""
],
[
"Lindstrom",
"U.",
""
],
[
"Wulff",
"L.",
""
]
] | The Green-Schwarz action for an open superstring with additional boundary fermions, representing Chan-Paton factors, is studied at the classical level. The boundary geometry is described by a bundle, with fermionic fibres, over the super worldvolume of a D-brane together with a map from the total space into the type II... | 7.687315 | 7.918924 | 8.359974 | 7.406196 | 7.286941 | 7.275432 | 7.802114 | 7.669652 | 7.408713 | 9.482363 | 6.984211 | 7.421822 | 8.118347 | 7.356572 | 7.444549 | 7.339643 | 7.415973 | 7.619743 | 7.387569 | 8.09359 | 7.321065 |
1912.05746 | Dominik Neuenfeld | Sean Cooper, Dominik Neuenfeld, Moshe Rozali, David Wakeham | Brane dynamics from the first law of entanglement | 19 pages plus appendices | null | 10.1007/JHEP03(2020)023 | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | In this note, we study the first law of entanglement in a boundary conformal
field theory (BCFT) dual to warped AdS cut off by a brane. Exploiting the
symmetry of boundary-centered half-balls in the BCFT, and using Wald's
covariant phase space formalism in the presence of boundaries, we derive
constraints from the fi... | [
{
"created": "Thu, 12 Dec 2019 03:09:22 GMT",
"version": "v1"
}
] | 2020-04-22 | [
[
"Cooper",
"Sean",
""
],
[
"Neuenfeld",
"Dominik",
""
],
[
"Rozali",
"Moshe",
""
],
[
"Wakeham",
"David",
""
]
] | In this note, we study the first law of entanglement in a boundary conformal field theory (BCFT) dual to warped AdS cut off by a brane. Exploiting the symmetry of boundary-centered half-balls in the BCFT, and using Wald's covariant phase space formalism in the presence of boundaries, we derive constraints from the firs... | 9.931659 | 9.263174 | 11.628665 | 8.937438 | 10.218955 | 10.060066 | 9.231668 | 9.13848 | 8.631383 | 11.278799 | 8.751457 | 9.373449 | 10.003341 | 9.075884 | 9.56356 | 9.21967 | 9.407791 | 9.079232 | 9.231818 | 9.520397 | 8.87094 |
2008.13159 | Vakhid Gani | Petr A. Blinov, Tatiana V. Gani, Vakhid A. Gani | Deformations of Kink Tails | 14 pages, 6 figures; v2: final/published version | Ann. Phys. (N. Y.) 437, 168739 (2022) | 10.1016/j.aop.2021.168739 | null | hep-th math-ph math.MP nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the asymptotic properties of kinks in connection with the
deformation procedure. We show that, upon deformation of the field-theoretic
model, the asymptotics of kinks can change or remain unchanged, depending on
the properties of the deforming function. The cases of both explicit and
implicit kinks are consi... | [
{
"created": "Sun, 30 Aug 2020 13:03:20 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jan 2022 21:48:14 GMT",
"version": "v2"
}
] | 2022-04-20 | [
[
"Blinov",
"Petr A.",
""
],
[
"Gani",
"Tatiana V.",
""
],
[
"Gani",
"Vakhid A.",
""
]
] | We study the asymptotic properties of kinks in connection with the deformation procedure. We show that, upon deformation of the field-theoretic model, the asymptotics of kinks can change or remain unchanged, depending on the properties of the deforming function. The cases of both explicit and implicit kinks are conside... | 8.435345 | 8.057912 | 8.34845 | 7.715771 | 8.160593 | 7.606371 | 7.944258 | 7.788981 | 7.454716 | 8.454913 | 7.905523 | 7.881672 | 8.096577 | 7.880436 | 7.920542 | 7.993752 | 8.067533 | 7.895252 | 7.915582 | 8.209876 | 7.737215 |
1112.0325 | Witold Skiba | Walter D. Goldberger, Witold Skiba, and Minho Son | Superembedding methods for 4d N=1 SCFTs | 33 pages, clarification of constraints, version to appear in PRD | null | 10.1103/PhysRevD.86.025019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend SO(4,2) covariant lightcone embedding methods of four-dimensional
CFTs to N=1 superconformal field theory (SCFT). Manifest superconformal
SU(2,2|1) invariance is achieved by realizing 4D superconformal space as a
surface embedded in the projective superspace spanned by certain complex chiral
supermatrices. ... | [
{
"created": "Thu, 1 Dec 2011 21:01:04 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Jan 2012 19:36:30 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Jun 2012 20:31:19 GMT",
"version": "v3"
}
] | 2013-05-30 | [
[
"Goldberger",
"Walter D.",
""
],
[
"Skiba",
"Witold",
""
],
[
"Son",
"Minho",
""
]
] | We extend SO(4,2) covariant lightcone embedding methods of four-dimensional CFTs to N=1 superconformal field theory (SCFT). Manifest superconformal SU(2,2|1) invariance is achieved by realizing 4D superconformal space as a surface embedded in the projective superspace spanned by certain complex chiral supermatrices. Be... | 6.76037 | 6.546981 | 7.681559 | 6.488367 | 6.986207 | 6.712666 | 6.641524 | 6.929372 | 6.557988 | 8.04256 | 6.729766 | 6.396094 | 7.136978 | 6.534558 | 6.498999 | 6.655158 | 6.363335 | 6.524947 | 6.747778 | 7.070978 | 6.447063 |
1602.09057 | Eva Llabr\'es | Alejandra Castro, Nabil Iqbal, and Eva Llabr\'es | Eternal Higher Spin Black Holes: a Thermofield Interpretation | 53 pages, 9 figures | null | 10.1007/JHEP08(2016)022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study Lorentzian eternal black holes in the Chern-Simons sector of AdS$_3$
higher spin gravity. We probe such black holes using bulk Wilson lines and
motivate new regularity conditions that must be obeyed by the bulk connections
in order for the geometry to be consistent with an interpretation as a
thermofield sta... | [
{
"created": "Mon, 29 Feb 2016 17:27:07 GMT",
"version": "v1"
}
] | 2016-08-24 | [
[
"Castro",
"Alejandra",
""
],
[
"Iqbal",
"Nabil",
""
],
[
"Llabrés",
"Eva",
""
]
] | We study Lorentzian eternal black holes in the Chern-Simons sector of AdS$_3$ higher spin gravity. We probe such black holes using bulk Wilson lines and motivate new regularity conditions that must be obeyed by the bulk connections in order for the geometry to be consistent with an interpretation as a thermofield state... | 8.330273 | 8.371785 | 8.874238 | 8.832124 | 8.594523 | 8.702509 | 9.143011 | 8.522978 | 8.77123 | 10.74451 | 8.505058 | 8.27337 | 8.250773 | 8.01824 | 8.183937 | 8.180392 | 8.047137 | 8.111876 | 7.912702 | 8.435745 | 7.869575 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.