id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9411221 | null | Alex Deckmyn, Ruud Siebelink, Walter Troost and Alexander Sevrin | On the Lagrangian Realization of Non-Critical ${\cal W}$-Strings | 19 pages, LaTeX (REVTEX macro's) | Phys. Rev. D 51, 6970 (1995) | 10.1103/PhysRevD.51.6970 | Preprint-KUL-TF-94/38 and CERN-TH.7477/94 | hep-th | null | A large class of non-critical string theories with extended worldsheet gauge
symmetry are described by two coupled, gauged Wess-Zumino-Witten Models. We
give a detailed analysis of the gauge invariant action and in particular the
gauge fixing procedure and the resulting BRST symmetries. The results are
applied to the... | [
{
"created": "Tue, 29 Nov 1994 18:56:23 GMT",
"version": "v1"
}
] | 2016-08-24 | [
[
"Deckmyn",
"Alex",
""
],
[
"Siebelink",
"Ruud",
""
],
[
"Troost",
"Walter",
""
],
[
"Sevrin",
"Alexander",
""
]
] | A large class of non-critical string theories with extended worldsheet gauge symmetry are described by two coupled, gauged Wess-Zumino-Witten Models. We give a detailed analysis of the gauge invariant action and in particular the gauge fixing procedure and the resulting BRST symmetries. The results are applied to the e... | 9.43546 | 7.107136 | 9.76107 | 6.68313 | 7.670411 | 7.323517 | 7.636912 | 7.168791 | 7.208655 | 9.250826 | 7.024963 | 6.987114 | 8.022097 | 7.42734 | 7.297087 | 7.244931 | 7.058135 | 7.143432 | 7.45919 | 7.720048 | 7.300318 |
1110.6355 | Jacopo Viti | Gesualdo Delfino and Jacopo Viti | Crossing probability and number of crossing clusters in off-critical
percolation | 13 pages, 5 figures. Published version with references, appendix and
comparison with numerics added | J. Phys. A: Math. Theor. 45 (2012) 032005 | 10.1088/1751-8113/45/3/032005 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider two-dimensional percolation in the scaling limit close to
criticality and use integrable field theory to obtain universal predictions for
the probability that at least one cluster crosses between opposite sides of a
rectangle of sides much larger than the correlation length and for the mean
number of such... | [
{
"created": "Fri, 28 Oct 2011 14:46:59 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Dec 2011 17:43:25 GMT",
"version": "v2"
}
] | 2014-10-09 | [
[
"Delfino",
"Gesualdo",
""
],
[
"Viti",
"Jacopo",
""
]
] | We consider two-dimensional percolation in the scaling limit close to criticality and use integrable field theory to obtain universal predictions for the probability that at least one cluster crosses between opposite sides of a rectangle of sides much larger than the correlation length and for the mean number of such c... | 9.818931 | 9.755333 | 11.075607 | 9.689536 | 9.894927 | 10.321489 | 8.729986 | 9.456997 | 9.586575 | 13.277572 | 10.047285 | 9.182069 | 10.384165 | 9.360952 | 8.591944 | 9.1223 | 8.524921 | 9.648236 | 9.418691 | 10.516802 | 9.002758 |
hep-th/9806084 | Tatsuo Suzuki | Kazuyuki Fujii, Yasushi Homma and Tatsuo Suzuki | Nonlinear Grassmann Sigma Models in Any Dimension and An Infinite Number
of Conserved Currents | 11 pages, AMSLaTex | Phys.Lett. B438 (1998) 290-294 | 10.1016/S0370-2693(98)00981-2 | null | hep-th | null | We first consider nonlinear Grassmann sigma models in any dimension and next
construct their submodels. For these models we construct an infinite number of
nontrivial conserved currents. Our result is independent of time-space
dimensions and, therfore, is a full generalization of that of authors (Alvarez,
Ferreira an... | [
{
"created": "Thu, 11 Jun 1998 09:03:30 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Fujii",
"Kazuyuki",
""
],
[
"Homma",
"Yasushi",
""
],
[
"Suzuki",
"Tatsuo",
""
]
] | We first consider nonlinear Grassmann sigma models in any dimension and next construct their submodels. For these models we construct an infinite number of nontrivial conserved currents. Our result is independent of time-space dimensions and, therfore, is a full generalization of that of authors (Alvarez, Ferreira and ... | 14.694382 | 12.04624 | 15.404893 | 12.650176 | 12.175558 | 11.202094 | 12.658129 | 12.407721 | 12.313831 | 17.211771 | 12.419026 | 12.834097 | 14.638392 | 13.78027 | 12.848285 | 13.131613 | 12.468557 | 12.728822 | 13.879601 | 14.151422 | 13.396655 |
1708.05323 | Fei Yan | Andrew Neitzke, Fei Yan | Line defect Schur indices, Verlinde algebras and $U(1)_r$ fixed points | 64 pages, 21 figures. v2 published version, references updated | JHEP11(2017)035 | 10.1007/JHEP11(2017)035 | UTTG-05-17 | hep-th math.AG math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given an $\mathcal{N}=2$ superconformal field theory, we reconsider the Schur
index $\mathcal{I}_L(q)$ in the presence of a half line defect $L$. Recently
Cordova-Gaiotto-Shao found that $\mathcal{I}_L(q)$ admits an expansion in terms
of characters of the chiral algebra $\mathcal{A}$ introduced by Beem et al.,
with s... | [
{
"created": "Thu, 17 Aug 2017 14:56:41 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Dec 2017 18:59:09 GMT",
"version": "v2"
}
] | 2017-12-13 | [
[
"Neitzke",
"Andrew",
""
],
[
"Yan",
"Fei",
""
]
] | Given an $\mathcal{N}=2$ superconformal field theory, we reconsider the Schur index $\mathcal{I}_L(q)$ in the presence of a half line defect $L$. Recently Cordova-Gaiotto-Shao found that $\mathcal{I}_L(q)$ admits an expansion in terms of characters of the chiral algebra $\mathcal{A}$ introduced by Beem et al., with sim... | 5.108862 | 5.327438 | 6.49421 | 5.06654 | 5.466817 | 5.272567 | 5.28573 | 4.84837 | 5.095561 | 6.475612 | 5.180242 | 4.987263 | 5.331282 | 4.994173 | 4.857617 | 4.951837 | 5.003873 | 4.983676 | 4.953042 | 5.415512 | 5.032682 |
1106.0213 | Glenn Barnich | Glenn Barnich and Cedric Troessaert | BMS charge algebra | 25 pages Latex file, extended discussions in sections 3 and 5 | null | 10.1007/JHEP12(2011)105 | ULB-TH/11-10 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The surface charges associated with the symmetries of asymptotically flat
four dimensional spacetimes at null infinity are constructed. They realize the
symmetry algebra in general only up to a field-dependent central extension that
satisfies a suitably generalized cocycle condition. This extension vanishes
when usin... | [
{
"created": "Wed, 1 Jun 2011 15:58:36 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Oct 2011 15:30:14 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Barnich",
"Glenn",
""
],
[
"Troessaert",
"Cedric",
""
]
] | The surface charges associated with the symmetries of asymptotically flat four dimensional spacetimes at null infinity are constructed. They realize the symmetry algebra in general only up to a field-dependent central extension that satisfies a suitably generalized cocycle condition. This extension vanishes when using ... | 11.982689 | 10.08747 | 10.715788 | 9.709969 | 10.528815 | 10.897214 | 10.34809 | 9.377542 | 10.829309 | 12.909388 | 10.011995 | 10.675101 | 10.663981 | 10.186096 | 10.596881 | 10.508244 | 10.767626 | 10.154274 | 10.350718 | 10.905209 | 10.322892 |
1310.2772 | Emil Nissimov | Eduardo Guendelman, Emil Nissimov, Svetlana Pacheva, Mahary Vasihoun | Dynamical Volume Element in Scale-Invariant and Supergravity Theories | 6 pages, invited talk at Second Bulgarian National Congress in
Physics, Sept. 2013; v.2 - important key word added in abstract, minor typos
corrected | Bulgarian Journal of Physics 40 (2013) 121-126 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The use in the action integral of a volume element of the form $\Phi d^{D}x$,
where $\Phi$ is a metric-independent measure density, can yield new interesting
results in all types of known generally coordinate-invariant theories: (1) 4-D
theories of gravity plus matter fields; (2) reparametrization invariant
theories ... | [
{
"created": "Thu, 10 Oct 2013 11:10:56 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Oct 2013 19:04:01 GMT",
"version": "v2"
}
] | 2013-11-15 | [
[
"Guendelman",
"Eduardo",
""
],
[
"Nissimov",
"Emil",
""
],
[
"Pacheva",
"Svetlana",
""
],
[
"Vasihoun",
"Mahary",
""
]
] | The use in the action integral of a volume element of the form $\Phi d^{D}x$, where $\Phi$ is a metric-independent measure density, can yield new interesting results in all types of known generally coordinate-invariant theories: (1) 4-D theories of gravity plus matter fields; (2) reparametrization invariant theories of... | 11.306668 | 8.394299 | 10.130132 | 9.16783 | 8.490078 | 8.887669 | 8.881011 | 8.461736 | 9.313518 | 11.354072 | 9.572954 | 10.026263 | 10.315484 | 10.363728 | 10.134671 | 10.258701 | 10.117713 | 9.961444 | 10.04274 | 10.615479 | 10.397264 |
1511.08955 | Michael Gutperle | Michael Gutperle and John D. Miller | Entanglement entropy at holographic interfaces | 15 pages, 2 figures, pdflatex. v2: reference added, typos corrected | Phys. Rev. D 93, 026006 (2016) | 10.1103/PhysRevD.93.026006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we calculate the holographic entanglement entropy in the
presence of a conformal interface for a geometric configuration in which the
entangling region ${\cal A}$ lies on one side of the interface. For the
supersymmetric Janus solution we find exact agreement between the holographic
and CFT calculation o... | [
{
"created": "Sun, 29 Nov 2015 01:50:53 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jan 2016 19:32:53 GMT",
"version": "v2"
}
] | 2016-01-20 | [
[
"Gutperle",
"Michael",
""
],
[
"Miller",
"John D.",
""
]
] | In this note we calculate the holographic entanglement entropy in the presence of a conformal interface for a geometric configuration in which the entangling region ${\cal A}$ lies on one side of the interface. For the supersymmetric Janus solution we find exact agreement between the holographic and CFT calculation of ... | 6.049926 | 5.17899 | 6.782648 | 5.11523 | 5.266128 | 4.92437 | 4.880111 | 4.919729 | 5.319763 | 8.410796 | 4.978243 | 5.081159 | 6.379156 | 5.508392 | 5.305538 | 5.252625 | 5.375082 | 5.154762 | 5.18031 | 6.337161 | 5.060572 |
hep-th/9903133 | Osamu Abe | Osamu Abe | A New Basis Function Approach to 't Hooft-Bergknoff-Eller Equations | 16 pages, 3 figures | Phys. Rev. D 60, 105040 (1999) | 10.1103/PhysRevD.60.105040 | HUEAP-012 | hep-th | null | We analytically and numerically investigate the 't Hooft-Bergknoff-Eller
equations, the lowest order mesonic Light-Front Tamm-Dancoff equations for
U(N_C) and SU(N_C) gauge theories. We find the wavefunction can be well
approximated by new basis functions and obtain an analytic formula for the mass
of the lightest bo... | [
{
"created": "Tue, 16 Mar 1999 04:40:27 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Mar 1999 01:38:53 GMT",
"version": "v2"
},
{
"created": "Thu, 24 Jun 1999 23:52:48 GMT",
"version": "v3"
}
] | 2016-08-25 | [
[
"Abe",
"Osamu",
""
]
] | We analytically and numerically investigate the 't Hooft-Bergknoff-Eller equations, the lowest order mesonic Light-Front Tamm-Dancoff equations for U(N_C) and SU(N_C) gauge theories. We find the wavefunction can be well approximated by new basis functions and obtain an analytic formula for the mass of the lightest boun... | 15.048659 | 11.628201 | 16.164637 | 12.840252 | 12.746402 | 10.70312 | 13.198147 | 11.762063 | 10.157644 | 16.178139 | 12.137372 | 13.242417 | 14.549332 | 13.770092 | 14.443665 | 14.22424 | 13.397929 | 13.937208 | 13.500522 | 15.160355 | 13.576221 |
hep-th/9502078 | Won-Tae Kim | Won T. Kim and Julian Lee | ADM, Bondi mass, and energy conservation in two-dimensional dilaton
gravities | 11 pages, latex, no figures | Int.J.Mod.Phys. A11 (1996) 553-562 | 10.1142/S0217751X96000250 | SNUTP 95-005 | hep-th | null | We show how a stress-energy pseudotensor can be constructed in
two-dimensional dilatonic gravity theories (classical, CGHS and RST) and derive
the expression for the ADM mass in these theories from it. We define the Bondi
mass for these theories by using the pseudotensor formalism. The resulting
expression is the gen... | [
{
"created": "Tue, 14 Feb 1995 06:02:41 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Kim",
"Won T.",
""
],
[
"Lee",
"Julian",
""
]
] | We show how a stress-energy pseudotensor can be constructed in two-dimensional dilatonic gravity theories (classical, CGHS and RST) and derive the expression for the ADM mass in these theories from it. We define the Bondi mass for these theories by using the pseudotensor formalism. The resulting expression is the gener... | 9.828642 | 9.533151 | 9.251049 | 8.005039 | 8.534798 | 8.858764 | 9.532206 | 9.493035 | 8.480149 | 10.107218 | 8.371881 | 8.865263 | 9.328166 | 8.856672 | 9.119355 | 9.080206 | 8.892806 | 8.951982 | 8.995002 | 9.653079 | 8.820344 |
2304.01259 | Dong-Yu Hong | Dong-Yu Hong, Zhuo-Hui Wang and Shuang-Yong Zhou | Causality bounds on scalar-tensor EFTs | 76 pages, 15 figures; to appear in JHEP | null | null | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the causality/positivity bounds on the Wilson coefficients of
scalar-tensor effective field theories. Two-sided bounds are obtained by
extracting IR information from UV physics via dispersion relations of
scattering amplitudes, making use of the full crossing symmetry. The graviton
$t$-channel pole is care... | [
{
"created": "Mon, 3 Apr 2023 18:00:05 GMT",
"version": "v1"
},
{
"created": "Sat, 21 Oct 2023 10:27:16 GMT",
"version": "v2"
}
] | 2023-10-24 | [
[
"Hong",
"Dong-Yu",
""
],
[
"Wang",
"Zhuo-Hui",
""
],
[
"Zhou",
"Shuang-Yong",
""
]
] | We compute the causality/positivity bounds on the Wilson coefficients of scalar-tensor effective field theories. Two-sided bounds are obtained by extracting IR information from UV physics via dispersion relations of scattering amplitudes, making use of the full crossing symmetry. The graviton $t$-channel pole is carefu... | 15.71891 | 14.622023 | 15.871222 | 14.910301 | 14.275089 | 13.867132 | 13.581562 | 15.075356 | 14.742213 | 18.315046 | 14.475036 | 14.416946 | 15.40236 | 14.777129 | 14.291806 | 14.630988 | 14.578864 | 14.968181 | 14.67917 | 15.260396 | 14.607604 |
2112.06335 | Ilya Kochergin | I. V. Kochergin | On Calabi-Yau manifolds in weighted projective spaces and their mirror
GLSMs | 20 pages, improved the display of references | null | 10.1103/PhysRevD.105.066008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The goal of the present paper is to calculate the complex structure moduli
space K\"ahler potentials for hypersurfaces in weighted projective spaces and
compare with the partition functions of their mirror GLSMs. We explicitly
perform the K\"ahler potential computation and show that the corresponding
formula is well-... | [
{
"created": "Sun, 12 Dec 2021 22:11:04 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Dec 2021 22:23:12 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Jan 2022 19:54:21 GMT",
"version": "v3"
},
{
"created": "Thu, 20 Jan 2022 02:42:25 GMT",
"version": "v4"
}
] | 2022-04-06 | [
[
"Kochergin",
"I. V.",
""
]
] | The goal of the present paper is to calculate the complex structure moduli space K\"ahler potentials for hypersurfaces in weighted projective spaces and compare with the partition functions of their mirror GLSMs. We explicitly perform the K\"ahler potential computation and show that the corresponding formula is well-de... | 7.878398 | 7.943362 | 8.21587 | 8.006442 | 8.154632 | 8.081349 | 7.373682 | 7.613585 | 7.389958 | 9.562737 | 7.714957 | 7.751544 | 8.244916 | 7.6693 | 7.466119 | 7.64579 | 7.559298 | 7.662093 | 7.383161 | 8.218778 | 7.428523 |
1211.1983 | D. S. Berman | Joel Berkeley, David S. Berman | The Navier-Stokes equation and solution generating symmetries from
holography | LateX, 24 pages, v2 references added and some improved discussion, v3
improved discussion and typos fixed | null | 10.1007/JHEP04(2013)092 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The fluid-gravity correspondence provides us with explicit spacetime metrics
that are holographically dual to (non-)relativistic nonlinear hydrodynamics.
The vacuum Einstein equations, in the presence of a Killing vector, possess
solution-generating symmetries known as spacetime Ehlers transformations. These
form a s... | [
{
"created": "Thu, 8 Nov 2012 21:05:44 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Dec 2012 09:25:20 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Feb 2013 09:13:32 GMT",
"version": "v3"
}
] | 2015-06-12 | [
[
"Berkeley",
"Joel",
""
],
[
"Berman",
"David S.",
""
]
] | The fluid-gravity correspondence provides us with explicit spacetime metrics that are holographically dual to (non-)relativistic nonlinear hydrodynamics. The vacuum Einstein equations, in the presence of a Killing vector, possess solution-generating symmetries known as spacetime Ehlers transformations. These form a sub... | 11.819296 | 12.285967 | 11.384841 | 11.683817 | 12.243444 | 11.784895 | 11.39271 | 11.695776 | 11.372033 | 12.350367 | 11.254025 | 11.017873 | 11.533678 | 11.219099 | 10.784627 | 11.219843 | 10.828233 | 10.879895 | 11.291105 | 11.486472 | 11.238122 |
1503.08207 | Steven B. Giddings | Steven B. Giddings | Hilbert space structure in quantum gravity: an algebraic perspective | 24 pages, harvmac. v2: added refs | null | 10.1007/JHEP12(2015)099 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | If quantum gravity respects the principles of quantum mechanics, suitably
generalized, it may be that a more viable approach to the theory is through
identifying the relevant quantum structures rather than by quantizing classical
spacetime. This viewpoint is supported by difficulties of such quantization,
and by the ... | [
{
"created": "Fri, 27 Mar 2015 20:00:17 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Aug 2015 21:52:01 GMT",
"version": "v2"
}
] | 2016-01-27 | [
[
"Giddings",
"Steven B.",
""
]
] | If quantum gravity respects the principles of quantum mechanics, suitably generalized, it may be that a more viable approach to the theory is through identifying the relevant quantum structures rather than by quantizing classical spacetime. This viewpoint is supported by difficulties of such quantization, and by the ap... | 12.042688 | 13.502067 | 13.199199 | 12.173172 | 12.250607 | 13.75426 | 12.995687 | 12.351547 | 12.58712 | 14.134663 | 12.320225 | 11.684809 | 11.921014 | 11.61781 | 11.88389 | 11.970665 | 11.636832 | 11.773737 | 11.811217 | 12.287385 | 11.600883 |
hep-th/9909159 | A. Demichev | Masud Chaichian and Kazuhiko Nishijima | The Goto-Imamura-Schwinger Term and Renormalization Group | LaTeX, 14 pages | Fiz.Elem.Chast.Atom.Yadra 31N7B:56-69,2000 | null | HIP-1999-61/TH | hep-th | null | In connection with the question of color confinement the origin of the
Goto-Imamura-Schwinger term has been studied with the help of renormalization
group. An emphasis has been laid on the difference between theories with and
without a cut-off.
| [
{
"created": "Wed, 22 Sep 1999 16:56:52 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Chaichian",
"Masud",
""
],
[
"Nishijima",
"Kazuhiko",
""
]
] | In connection with the question of color confinement the origin of the Goto-Imamura-Schwinger term has been studied with the help of renormalization group. An emphasis has been laid on the difference between theories with and without a cut-off. | 16.976564 | 14.468091 | 15.559418 | 14.790848 | 13.009692 | 14.754479 | 14.008549 | 13.738513 | 14.190594 | 14.964473 | 14.223508 | 15.087322 | 14.276767 | 13.225527 | 13.996664 | 14.122085 | 14.038844 | 14.586232 | 14.359473 | 14.331431 | 14.042989 |
2011.03337 | Myungbo Shim | Jung-Wook Kim, Myungbo Shim | Quantum corrections to tidal Love number for Schwarzschild black holes | 5 pages, no figure; Published Version; any comments welcome | Phys. Rev. D 104, 046022 (2021) | 10.1103/PhysRevD.104.046022 | QMUL-PH-20-31 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | A sum rule for tidal Love number is derived from quantum field theory
computations, which relates tidal susceptibility of a spinless body to
transition rates of its single graviton emission processes. An analogous sum
rule for electromagnetism is given as an example, which is substantiated by
comparing to the solved ... | [
{
"created": "Fri, 6 Nov 2020 13:23:16 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Mar 2021 08:49:11 GMT",
"version": "v2"
},
{
"created": "Sat, 21 Aug 2021 13:34:42 GMT",
"version": "v3"
}
] | 2021-08-24 | [
[
"Kim",
"Jung-Wook",
""
],
[
"Shim",
"Myungbo",
""
]
] | A sum rule for tidal Love number is derived from quantum field theory computations, which relates tidal susceptibility of a spinless body to transition rates of its single graviton emission processes. An analogous sum rule for electromagnetism is given as an example, which is substantiated by comparing to the solved pr... | 15.64092 | 15.898126 | 14.695506 | 14.194521 | 14.700387 | 15.259111 | 14.94821 | 15.393516 | 12.831125 | 13.85325 | 15.299782 | 14.695265 | 14.352552 | 14.782591 | 14.397749 | 15.23521 | 14.14788 | 13.936128 | 14.306903 | 15.205468 | 14.079711 |
1803.11302 | Yong Zhang | Song He, Gongwang Yan, Chi Zhang and Yong Zhang | Scattering Forms, Worldsheet Forms and Amplitudes from Subspaces | 25+4 pages, a dozen figures, lots of polytopes | null | 10.1007/JHEP08(2018)040 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a general construction of two types of differential forms, based
on any $(n{-}3)$-dimensional subspace in the kinematic space of $n$ massless
particles. The first type is the so-called projective, scattering forms in
kinematic space, while the second is defined in the moduli space of
$n$-punctured Riemann ... | [
{
"created": "Fri, 30 Mar 2018 01:18:51 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Jul 2018 17:42:27 GMT",
"version": "v2"
}
] | 2018-08-29 | [
[
"He",
"Song",
""
],
[
"Yan",
"Gongwang",
""
],
[
"Zhang",
"Chi",
""
],
[
"Zhang",
"Yong",
""
]
] | We present a general construction of two types of differential forms, based on any $(n{-}3)$-dimensional subspace in the kinematic space of $n$ massless particles. The first type is the so-called projective, scattering forms in kinematic space, while the second is defined in the moduli space of $n$-punctured Riemann sp... | 8.785198 | 8.226213 | 9.658439 | 8.290699 | 8.752294 | 8.811844 | 8.583473 | 8.355923 | 8.002044 | 11.280932 | 8.61471 | 8.662008 | 8.799851 | 8.568624 | 8.663313 | 8.682523 | 8.697216 | 8.586903 | 8.607652 | 9.207399 | 8.477244 |
2107.08005 | Eduardo Guendelman I | Eduardo Guendelman | Light Like Segment Compactification and Braneworlds with Dynamical
String Tension | 17 pages. References added. This version has been accepted for
publication in European Physics Journal C. arXiv admin note: substantial text
overlap with arXiv:2105.02279, arXiv:2104.08875 | null | 10.1140/epjc/s10052-021-09646-z | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Braneworld scenarios appear in dynamical string tension theories, where
string tension is positive between two surfaces separated by a short distance
and at the two surfaces themselves the string tensions become infinite,
therefore producing an effective confinement of the strings and therefore of
all matter and grav... | [
{
"created": "Fri, 16 Jul 2021 16:51:51 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Sep 2021 16:21:10 GMT",
"version": "v2"
}
] | 2021-10-27 | [
[
"Guendelman",
"Eduardo",
""
]
] | Braneworld scenarios appear in dynamical string tension theories, where string tension is positive between two surfaces separated by a short distance and at the two surfaces themselves the string tensions become infinite, therefore producing an effective confinement of the strings and therefore of all matter and gravit... | 18.931232 | 15.934856 | 20.880959 | 17.143559 | 18.658068 | 17.56679 | 16.867754 | 17.113295 | 17.794737 | 21.928991 | 17.132324 | 17.608583 | 18.901426 | 18.438583 | 18.315981 | 18.314932 | 17.660202 | 18.144533 | 18.154858 | 18.652271 | 17.706835 |
2010.15610 | Per Berglund | Per Berglund, Tristan H\"ubsch and Djordje Minic | String Theory, the Dark Sector and the Hierarchy Problem | 10 pages, typo fixed, reference added | LHEP 2021 (2021) 186 | 10.31526/lhep.2021.186 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss dark energy, dark matter and the hierarchy problem in the context
of a general non-commutative formulation of string theory. In this framework
dark energy is generated by the dynamical geometry of the dual spacetime while
dark matter, on the other hand, comes from the degrees of freedom dual to the
visible... | [
{
"created": "Thu, 29 Oct 2020 13:58:50 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Jan 2021 18:25:17 GMT",
"version": "v2"
}
] | 2021-02-05 | [
[
"Berglund",
"Per",
""
],
[
"Hübsch",
"Tristan",
""
],
[
"Minic",
"Djordje",
""
]
] | We discuss dark energy, dark matter and the hierarchy problem in the context of a general non-commutative formulation of string theory. In this framework dark energy is generated by the dynamical geometry of the dual spacetime while dark matter, on the other hand, comes from the degrees of freedom dual to the visible m... | 8.205828 | 8.561088 | 8.940873 | 8.023807 | 8.628254 | 8.183104 | 8.102493 | 8.435105 | 8.006065 | 8.535901 | 8.022003 | 8.008028 | 8.281129 | 8.160425 | 8.040602 | 8.09162 | 8.036739 | 7.979452 | 8.158825 | 8.070378 | 7.776909 |
hep-th/0003094 | Luka Sustersic | Marijan Ribaric and Luka Sustersic | Realistic regularization of the QED Green functions | null | null | null | null | hep-th | null | Generalizing the 't Hooft and Veltman method of unitary regulators, we
demonstrate for the first time the existence of local, Lorentz-invariant,
physically motivated Lagrangians of quantum-electrodynamic phenomena such that:
(i) Feynman diagrams are finite and equal the diagrams of QED but with
regularized propagator... | [
{
"created": "Mon, 13 Mar 2000 13:44:52 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Jul 2001 07:02:27 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Ribaric",
"Marijan",
""
],
[
"Sustersic",
"Luka",
""
]
] | Generalizing the 't Hooft and Veltman method of unitary regulators, we demonstrate for the first time the existence of local, Lorentz-invariant, physically motivated Lagrangians of quantum-electrodynamic phenomena such that: (i) Feynman diagrams are finite and equal the diagrams of QED but with regularized propagators.... | 11.396804 | 6.965285 | 9.664534 | 7.959444 | 6.656658 | 7.003779 | 6.557921 | 7.338418 | 7.8982 | 11.397856 | 8.407494 | 9.325391 | 10.096609 | 9.209792 | 9.155704 | 9.28744 | 9.648857 | 9.018688 | 9.569215 | 10.54798 | 9.799473 |
hep-th/9404033 | Nakano | Hiroaki Nakano | Scalar Mass and Cosmological Constant induced by ``Anomalous" $U(1)$
$D$-term | 8p, KUNS-1257,HETH-94/05 | null | null | null | hep-th | null | When the supersymmetric theory contains the ``anomalous" $U(1)$ gauge
symmetry with Green-Schwarz anomaly cancellation mechanism in 4 dimensions, its
Fayet-Iliopoulos $D$-term generates non-universal scalar masses and the
positive cosmological constant after the supersymmetry breaking. Both give the
new contributions... | [
{
"created": "Wed, 6 Apr 1994 13:56:26 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nakano",
"Hiroaki",
""
]
] | When the supersymmetric theory contains the ``anomalous" $U(1)$ gauge symmetry with Green-Schwarz anomaly cancellation mechanism in 4 dimensions, its Fayet-Iliopoulos $D$-term generates non-universal scalar masses and the positive cosmological constant after the supersymmetry breaking. Both give the new contributions t... | 9.520409 | 8.2715 | 8.302648 | 7.93374 | 8.443164 | 8.52689 | 8.548055 | 8.509244 | 7.953766 | 8.675698 | 8.641267 | 8.680511 | 8.176846 | 8.25587 | 8.603487 | 8.917603 | 8.204439 | 8.504263 | 8.288321 | 8.360771 | 9.03218 |
1205.0120 | Zahra Rezaei | Zahra Rezaei | Boundary Super-Deformations, Boundary States, and Tachyon Condensation | 18 pages, no figure | Phys. Rev. D 85, 086011 (2012) | 10.1103/PhysRevD.85.086011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The open string tachyon and U(1) gauge field as longitudinal fluctuations and
the velocity as transverse fluctuation of an arbitrary dimensional D-brane are
considered as boundary deformations of a closed superstring free action. The
path integral approach will be applied to calculate the corresponding
generalized bo... | [
{
"created": "Tue, 1 May 2012 09:05:05 GMT",
"version": "v1"
}
] | 2013-12-31 | [
[
"Rezaei",
"Zahra",
""
]
] | The open string tachyon and U(1) gauge field as longitudinal fluctuations and the velocity as transverse fluctuation of an arbitrary dimensional D-brane are considered as boundary deformations of a closed superstring free action. The path integral approach will be applied to calculate the corresponding generalized boun... | 18.183952 | 14.45258 | 21.123203 | 14.392573 | 16.688391 | 16.255531 | 14.716718 | 13.608076 | 15.215205 | 22.507164 | 15.234698 | 15.56973 | 17.706108 | 15.358927 | 15.004582 | 15.677781 | 15.200518 | 15.042812 | 15.331196 | 17.12915 | 15.156942 |
hep-th/0106163 | Benjamin Grinstein | Benjamin Grinstein (UCSD) and Detlef R. Nolte (IAS) | Bulk Observers in Non-Factorizable Geometries | 11 pages, dedicated to the memory of Detlef Nolte | Phys.Rev. D64 (2001) 085017 | 10.1103/PhysRevD.64.085017 | UCSD/PTH 01-11 | hep-th | null | We consider five dimensional non-factorizable geometries where the transverse
dimension is bounded and the remaining (parallel) dimensions are not. We study
the construction of effective theories at distances much longer than the
transverse size. An observer unable to resolve the transverse direction can
only measure... | [
{
"created": "Mon, 18 Jun 2001 23:18:48 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Grinstein",
"Benjamin",
"",
"UCSD"
],
[
"Nolte",
"Detlef R.",
"",
"IAS"
]
] | We consider five dimensional non-factorizable geometries where the transverse dimension is bounded and the remaining (parallel) dimensions are not. We study the construction of effective theories at distances much longer than the transverse size. An observer unable to resolve the transverse direction can only measure d... | 9.474826 | 9.491367 | 9.543373 | 8.794436 | 10.472103 | 9.367875 | 9.524652 | 9.307179 | 9.491901 | 10.935898 | 9.269716 | 9.0471 | 9.446115 | 9.161319 | 8.824612 | 8.718507 | 9.177678 | 8.769403 | 9.04978 | 9.227019 | 8.604888 |
0705.4006 | Anton Zabrodin | A. Zabrodin | Backlund transformations for difference Hirota equation and
supersymmetric Bethe ansatz | 22 pages, 2 figures, based on the talk given at the Workshop
"Classical and Quantum Integrable Systems", Dubna, January 2007 | null | 10.1007/s11232-008-0047-2 | ITEP-TH-21/07 | hep-th nlin.SI | null | We consider GL(K|M)-invariant integrable supersymmetric spin chains with
twisted boundary conditions and elucidate the role of Backlund transformations
in solving the difference Hirota equation for eigenvalues of their transfer
matrices. The nested Bethe ansatz technique is shown to be equivalent to a
chain of succes... | [
{
"created": "Mon, 28 May 2007 14:05:11 GMT",
"version": "v1"
}
] | 2009-11-13 | [
[
"Zabrodin",
"A.",
""
]
] | We consider GL(K|M)-invariant integrable supersymmetric spin chains with twisted boundary conditions and elucidate the role of Backlund transformations in solving the difference Hirota equation for eigenvalues of their transfer matrices. The nested Bethe ansatz technique is shown to be equivalent to a chain of successi... | 12.293905 | 12.246562 | 13.74362 | 10.442815 | 11.25297 | 11.486719 | 10.720717 | 11.605698 | 11.65123 | 15.472694 | 10.472727 | 10.84333 | 12.239799 | 11.302385 | 12.000565 | 11.57277 | 11.698916 | 11.397709 | 11.594278 | 13.664278 | 10.845169 |
hep-th/0602178 | Allan Adams | Allan Adams, Nima Arkani-Hamed, Sergei Dubovsky, Alberto Nicolis,
Riccardo Rattazzi | Causality, Analyticity and an IR Obstruction to UV Completion | 34 pages, 10 figures; v2: analyticity arguments improved, discussion
on non-commutative theories and minor clarifications added | JHEP 0610:014,2006 | 10.1088/1126-6708/2006/10/014 | null | hep-th hep-ph | null | We argue that certain apparently consistent low-energy effective field
theories described by local, Lorentz-invariant Lagrangians, secretly exhibit
macroscopic non-locality and cannot be embedded in any UV theory whose S-matrix
satisfies canonical analyticity constraints. The obstruction involves the signs
of a set o... | [
{
"created": "Mon, 20 Feb 2006 20:30:07 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Mar 2006 22:47:25 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Adams",
"Allan",
""
],
[
"Arkani-Hamed",
"Nima",
""
],
[
"Dubovsky",
"Sergei",
""
],
[
"Nicolis",
"Alberto",
""
],
[
"Rattazzi",
"Riccardo",
""
]
] | We argue that certain apparently consistent low-energy effective field theories described by local, Lorentz-invariant Lagrangians, secretly exhibit macroscopic non-locality and cannot be embedded in any UV theory whose S-matrix satisfies canonical analyticity constraints. The obstruction involves the signs of a set of ... | 11.168365 | 11.835584 | 11.181634 | 11.347124 | 12.51939 | 11.740803 | 11.628673 | 11.681341 | 10.831274 | 12.15386 | 11.127651 | 11.093027 | 11.109146 | 10.973055 | 11.084306 | 11.313539 | 11.209476 | 10.894021 | 10.885467 | 11.108285 | 10.85854 |
1401.5721 | Kurt Lechner | Francesco Azzurli, Kurt Lechner | Electromagnetic fields and potentials generated by massless charged
particles | 34 pages, no figures | null | 10.1016/j.aop.2014.06.005 | DFPD/2013/TH22 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide for the first time the exact solution of Maxwell's equations for a
massless charged particle moving on a generic trajectory at the speed of light.
In particular we furnish explicit expressions for the vector potential and the
electromagnetic field, which were both previously unknown, finding that they
enta... | [
{
"created": "Wed, 22 Jan 2014 16:29:59 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Azzurli",
"Francesco",
""
],
[
"Lechner",
"Kurt",
""
]
] | We provide for the first time the exact solution of Maxwell's equations for a massless charged particle moving on a generic trajectory at the speed of light. In particular we furnish explicit expressions for the vector potential and the electromagnetic field, which were both previously unknown, finding that they entail... | 11.071446 | 11.867177 | 11.933859 | 11.131806 | 12.248317 | 13.225833 | 11.773355 | 10.451542 | 10.896218 | 11.219666 | 10.896078 | 11.345588 | 10.967746 | 10.651503 | 10.743647 | 11.157139 | 10.998895 | 10.875286 | 11.054621 | 10.62892 | 10.934647 |
2306.13714 | Anamaria Hell | Anamaria Hell, Dieter Lust, George Zoupanos | On the Ghost Problem of Conformal Gravity | 24 pages | J. High Energ. Phys. 2023, 168 (2023) | 10.1007/JHEP08(2023)168 | CERN-TH-2023-116, LMU-ASC 21/23, MPP-2023-134 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the metric perturbations around the de Sitter and Minkowski
backgrounds in Conformal Gravity. We confirm the presence of ghosts in both
cases. In the de Sitter case, by applying the Maldacena boundary conditions -
the Neumann boundary condition and the positive-frequency mode condition - to
the metric, we sh... | [
{
"created": "Fri, 23 Jun 2023 18:00:11 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Aug 2023 11:02:54 GMT",
"version": "v2"
}
] | 2023-08-30 | [
[
"Hell",
"Anamaria",
""
],
[
"Lust",
"Dieter",
""
],
[
"Zoupanos",
"George",
""
]
] | We study the metric perturbations around the de Sitter and Minkowski backgrounds in Conformal Gravity. We confirm the presence of ghosts in both cases. In the de Sitter case, by applying the Maldacena boundary conditions - the Neumann boundary condition and the positive-frequency mode condition - to the metric, we show... | 8.13716 | 8.223269 | 7.955777 | 7.660099 | 8.066741 | 8.635167 | 8.258679 | 7.828108 | 7.987109 | 8.57655 | 8.259452 | 7.977385 | 8.099701 | 7.82788 | 7.893379 | 7.73129 | 7.760796 | 7.588831 | 7.630313 | 8.121706 | 7.782123 |
hep-th/0703053 | Farvah Mahmoudi | Alexandre Arbey, Farvah Mahmoudi | One-loop quantum corrections to cosmological scalar field potentials | 11 pages, 1 figure, accepted for publication in Phys. Rev. D | Phys.Rev.D75:063513,2007 | 10.1103/PhysRevD.75.063513 | MTA-PHYS-0701 | hep-th astro-ph gr-qc | null | We study the loop corrections to potentials of complex or coupled real scalar
fields used in cosmology to account for dark energy, dark matter or dark fluid.
We show that the SUGRA quintessence and dark matter scalar field potentials are
stable against the quantum fluctuations, and we propose solutions to the
instabi... | [
{
"created": "Tue, 6 Mar 2007 16:59:39 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Arbey",
"Alexandre",
""
],
[
"Mahmoudi",
"Farvah",
""
]
] | We study the loop corrections to potentials of complex or coupled real scalar fields used in cosmology to account for dark energy, dark matter or dark fluid. We show that the SUGRA quintessence and dark matter scalar field potentials are stable against the quantum fluctuations, and we propose solutions to the instabili... | 14.02113 | 15.240714 | 15.073747 | 15.153231 | 15.497242 | 14.632899 | 16.642454 | 15.97674 | 15.617698 | 16.658882 | 13.147517 | 13.947861 | 13.961306 | 14.0093 | 13.667823 | 14.427348 | 14.142439 | 13.905056 | 14.075687 | 14.365842 | 13.862157 |
hep-th/0103201 | Elena Poletaeva | Elena Poletaeva | Contact superconformal algebras and their representations | 6 pages, LaTeX2e, submitted to W. Siegel et al., editors, Concise
Encyclopedia of Supersymmetry, to be published by Kluwer Academic Publishers,
Dordrecht, 2001 | null | null | null | hep-th | null | This is a brief overview of my work on the realization of contact
superconformal algebras in terms of pseudodifferential symbols on a
supercircle. Also the 2-cocycles on K'(4) are given for this realization.
| [
{
"created": "Fri, 23 Mar 2001 13:47:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Poletaeva",
"Elena",
""
]
] | This is a brief overview of my work on the realization of contact superconformal algebras in terms of pseudodifferential symbols on a supercircle. Also the 2-cocycles on K'(4) are given for this realization. | 20.235498 | 13.295637 | 21.4373 | 14.246695 | 15.109137 | 15.474281 | 13.426465 | 14.803643 | 12.708825 | 21.42115 | 13.902264 | 14.77011 | 18.313679 | 15.121591 | 14.950127 | 14.552576 | 14.907948 | 14.752836 | 15.902289 | 18.763144 | 15.009925 |
1405.0997 | Haruki Watanabe | Haruki Watanabe, Hitoshi Murayama | Englert-Brout-Higgs Mechanism in Nonrelativistic Systems | 5 + 2 pages, including Supplemental Materials; v3: discussions
clarified | Phys. Rev. D 90, 121703(R) (2014) | 10.1103/PhysRevD.90.121703 | IPMU14-0109, UCB-PTH-14/30 | hep-th cond-mat.other cond-mat.quant-gas cond-mat.supr-con hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the general theory of Englert-Brout-Higgs mechanism without assuming
Lorentz invariance. In the presence of a finite expectation value of
non-Abelian matter charges, gauging those symmetries always results in
spontaneous breaking of spatial rotation. If we impose the charge neutrality by
assuming a backgroun... | [
{
"created": "Mon, 5 May 2014 19:12:52 GMT",
"version": "v1"
},
{
"created": "Tue, 13 May 2014 19:56:54 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Jul 2014 23:18:23 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Watanabe",
"Haruki",
""
],
[
"Murayama",
"Hitoshi",
""
]
] | We study the general theory of Englert-Brout-Higgs mechanism without assuming Lorentz invariance. In the presence of a finite expectation value of non-Abelian matter charges, gauging those symmetries always results in spontaneous breaking of spatial rotation. If we impose the charge neutrality by assuming a background ... | 12.805303 | 13.461515 | 13.325268 | 12.790662 | 14.188059 | 11.720626 | 11.69087 | 13.194428 | 11.867426 | 12.192638 | 12.421161 | 11.275682 | 12.466072 | 12.131037 | 11.974653 | 12.331956 | 11.678144 | 12.994658 | 12.136105 | 12.110166 | 11.76068 |
hep-th/9912124 | Andrei Marshakov | A.Marshakov | Duality in Integrable Systems and Generating Functions for New
Hamiltonians | Latex, 7 pp; minor corrections | Phys.Lett. B476 (2000) 420-426 | 10.1016/S0370-2693(00)00076-9 | FIAN/TD-26/99, ITEP/TH-78/99 | hep-th nlin.SI solv-int | null | Duality in the integrable systems arising in the context of Seiberg-Witten
theory shows that their tau-functions indeed can be seen as generating
functions for the mutually Poisson-commuting hamiltonians of the {\em dual}
systems. We demonstrate that the $\Theta$-function coefficients of their
expansion can be expres... | [
{
"created": "Tue, 14 Dec 1999 23:47:53 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Dec 1999 16:59:54 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Marshakov",
"A.",
""
]
] | Duality in the integrable systems arising in the context of Seiberg-Witten theory shows that their tau-functions indeed can be seen as generating functions for the mutually Poisson-commuting hamiltonians of the {\em dual} systems. We demonstrate that the $\Theta$-function coefficients of their expansion can be expresse... | 13.365686 | 11.584538 | 14.715276 | 11.835316 | 12.396865 | 12.808161 | 12.403964 | 11.886262 | 11.286244 | 15.757172 | 11.01547 | 11.310431 | 12.349309 | 11.637681 | 11.699673 | 11.091168 | 11.428362 | 11.498852 | 11.649246 | 12.790638 | 11.227129 |
hep-th/0009165 | Subir Ghosh | Subir Ghosh | Unified Study of Planar Field Theories | Accepted for publication in Annals of Physics (N.Y.) | Annals Phys. 291 (2001) 1-13 | 10.1006/aphy.2001.6141 | null | hep-th | null | A "Master" gauge theory is constructed in 2+1-dimensions through which
various gauge invariant and gauge non-invariant theories can be studied. In
particular, Maxwell-Chern-Simons, Maxwell-Proca and Maxwell-Chern-Simons -Proca
models are considered here. The Master theory in an enlarged phase space is
constructed bot... | [
{
"created": "Thu, 21 Sep 2000 12:32:08 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Jun 2001 07:29:44 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Ghosh",
"Subir",
""
]
] | A "Master" gauge theory is constructed in 2+1-dimensions through which various gauge invariant and gauge non-invariant theories can be studied. In particular, Maxwell-Chern-Simons, Maxwell-Proca and Maxwell-Chern-Simons -Proca models are considered here. The Master theory in an enlarged phase space is constructed both ... | 8.098655 | 7.317244 | 8.649713 | 6.82977 | 7.455839 | 7.143024 | 8.080246 | 7.18502 | 7.068274 | 8.900561 | 7.092738 | 7.045766 | 7.729687 | 7.198955 | 7.226712 | 7.323463 | 7.106867 | 7.091409 | 6.961307 | 7.681751 | 7.051354 |
hep-th/0003117 | Jonathan Bagger | Richard Altendorfer, Jonathan Bagger and Dennis Nemeschansky | Supersymmetric Randall-Sundrum Scenario | Latex, 9 pages. Published version | Phys.Rev. D63 (2001) 125025 | 10.1103/PhysRevD.63.125025 | null | hep-th hep-ph | null | We present the supersymmetric version of the minimal Randall-Sundrum model
with two opposite tension branes.
| [
{
"created": "Tue, 14 Mar 2000 22:14:36 GMT",
"version": "v1"
},
{
"created": "Tue, 23 May 2000 16:06:39 GMT",
"version": "v2"
},
{
"created": "Fri, 11 May 2001 13:49:34 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Altendorfer",
"Richard",
""
],
[
"Bagger",
"Jonathan",
""
],
[
"Nemeschansky",
"Dennis",
""
]
] | We present the supersymmetric version of the minimal Randall-Sundrum model with two opposite tension branes. | 15.820455 | 10.011986 | 11.408538 | 7.1776 | 8.239364 | 8.199523 | 7.446832 | 7.552033 | 8.980688 | 10.323508 | 10.052286 | 11.371237 | 11.266001 | 11.229578 | 11.659324 | 12.100667 | 11.889425 | 11.855597 | 10.260268 | 11.308145 | 12.596303 |
1209.3030 | Aram Saharian | E. R. Bezerra de Mello, A. A. Saharian, S. V. Abajyan | Fermionic vacuum polarization by a flat boundary in cosmic string
spacetime | 22 pages, 3 figures | Class. Quantum Grav. 30 (2013) 015002 | 10.1088/0264-9381/30/1/015002 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate the fermionic condensate and the renormalized
vacuum expectation value (VEV) of the energy-momentum tensor for a massive
fermionic field induced by a flat boundary in the cosmic string spacetime. In
this analysis we assume that the field operator obeys MIT bag boundary
condition on the bo... | [
{
"created": "Wed, 12 Sep 2012 17:18:03 GMT",
"version": "v1"
}
] | 2012-12-06 | [
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Saharian",
"A. A.",
""
],
[
"Abajyan",
"S. V.",
""
]
] | In this paper we investigate the fermionic condensate and the renormalized vacuum expectation value (VEV) of the energy-momentum tensor for a massive fermionic field induced by a flat boundary in the cosmic string spacetime. In this analysis we assume that the field operator obeys MIT bag boundary condition on the boun... | 5.033166 | 3.650182 | 5.557628 | 4.112638 | 3.935086 | 3.944975 | 3.908566 | 3.690419 | 3.630504 | 5.549415 | 3.646751 | 4.349617 | 5.080536 | 4.687936 | 4.636024 | 4.543287 | 4.540237 | 4.508821 | 4.649942 | 5.210968 | 4.535002 |
hep-th/9510037 | Mario Belloni | Mario Belloni, Lusheng Chen, and Kurt Haller (University of
Connecticut) | Implementing Gauss's law in Yang-Mills theory and QCD | 11 pages | Phys.Lett. B373 (1996) 185-192 | 10.1016/0370-2693(96)00112-8 | UCONN-95-05 | hep-th hep-ph | null | We construct a transformation that transforms perturbative states into states
that implement Gauss's law for `pure gluonic' Yang-Mills theory and QCD. The
fact that this transformation is not and cannot be unitary has special
significance. Previous work has shown that only states that are unitarily
equivalent to pert... | [
{
"created": "Sat, 7 Oct 1995 00:54:55 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Belloni",
"Mario",
"",
"University of\n Connecticut"
],
[
"Chen",
"Lusheng",
"",
"University of\n Connecticut"
],
[
"Haller",
"Kurt",
"",
"University of\n Connecticut"
]
] | We construct a transformation that transforms perturbative states into states that implement Gauss's law for `pure gluonic' Yang-Mills theory and QCD. The fact that this transformation is not and cannot be unitary has special significance. Previous work has shown that only states that are unitarily equivalent to pertur... | 14.403314 | 13.07401 | 13.762842 | 13.08897 | 12.979612 | 14.470326 | 13.301953 | 12.970242 | 12.458544 | 13.419474 | 13.600104 | 12.687717 | 12.852574 | 12.842539 | 13.237278 | 12.566721 | 13.824274 | 12.643464 | 12.922071 | 12.243041 | 12.812186 |
0907.1488 | Sang-Woo Kim | Goro Ishiki, Sang-Woo Kim, Jun Nishimura, Asato Tsuchiya | Testing a novel large-N reduction for N=4 super Yang-Mills theory on
RxS^3 | 24 pages, 4 figures | JHEP 0909:029,2009 | 10.1088/1126-6708/2009/09/029 | OU-HET 623, KEK-TH-1317 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently a novel large-N reduction has been proposed as a maximally
supersymmetric regularization of N=4 super Yang-Mills theory on RxS^3 in the
planar limit. This proposal, if it works, will enable us to study the theory
non-perturbatively on a computer, and hence to test the AdS/CFT correspondence
analogously to th... | [
{
"created": "Thu, 9 Jul 2009 10:18:41 GMT",
"version": "v1"
}
] | 2009-10-09 | [
[
"Ishiki",
"Goro",
""
],
[
"Kim",
"Sang-Woo",
""
],
[
"Nishimura",
"Jun",
""
],
[
"Tsuchiya",
"Asato",
""
]
] | Recently a novel large-N reduction has been proposed as a maximally supersymmetric regularization of N=4 super Yang-Mills theory on RxS^3 in the planar limit. This proposal, if it works, will enable us to study the theory non-perturbatively on a computer, and hence to test the AdS/CFT correspondence analogously to the ... | 6.758783 | 5.854841 | 8.12051 | 6.086419 | 6.172935 | 5.833162 | 5.422787 | 6.254102 | 6.151519 | 8.729449 | 6.147918 | 6.095548 | 7.04514 | 6.440181 | 6.50538 | 6.264105 | 6.252408 | 6.182762 | 6.502247 | 7.046392 | 6.389122 |
hep-th/9511187 | Itzhak Bars | Itzhak Bars | Solution of the SL(2,R) string in curved spacetime | LaTeX, 18 pages | null | null | USC-95/HEP-B3 | hep-th | null | The SL(2,R) WZW model, one of the simplest models for strings propagating in
curved space time, was believed to be non-unitary in the algebraic treatment
involving affine current algebra. It is shown that this was an error that
resulted from neglecting a zero mode that must be included to describe the
correct physics... | [
{
"created": "Mon, 27 Nov 1995 09:32:06 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bars",
"Itzhak",
""
]
] | The SL(2,R) WZW model, one of the simplest models for strings propagating in curved space time, was believed to be non-unitary in the algebraic treatment involving affine current algebra. It is shown that this was an error that resulted from neglecting a zero mode that must be included to describe the correct physics o... | 11.596056 | 11.072817 | 12.079317 | 10.872187 | 12.063128 | 11.528234 | 11.648949 | 11.173526 | 10.233809 | 13.359391 | 10.685645 | 10.809963 | 11.270012 | 10.704152 | 10.99992 | 10.643107 | 10.804263 | 11.16472 | 10.672662 | 11.55664 | 10.522245 |
hep-th/9511206 | Masao Jinzenji | Masao Jinzenji | On Quantum Cohomology Rings for Hypersurfaces in $CP^{N-1}$ | 32 pages, Revised version | J.Math.Phys. 38 (1997) 6613-6638 | 10.1063/1.532228 | UT-HEP-734-95 | hep-th | null | Using the torus action method, we construct one variable polynomial
representation of quantum cohomology ring for degree $k$ hypersurface in
$CP^{N-1}$ . The results interpolate the well-known result of $CP^{N-2}$ model
and the one of Calabi-Yau hypersuface in $CP^{N-1}$. We find in $k\leq N-2$
case, principal relati... | [
{
"created": "Wed, 29 Nov 1995 09:03:14 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Apr 1996 10:33:19 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Jinzenji",
"Masao",
""
]
] | Using the torus action method, we construct one variable polynomial representation of quantum cohomology ring for degree $k$ hypersurface in $CP^{N-1}$ . The results interpolate the well-known result of $CP^{N-2}$ model and the one of Calabi-Yau hypersuface in $CP^{N-1}$. We find in $k\leq N-2$ case, principal relation... | 8.885187 | 8.194369 | 10.042331 | 7.78385 | 7.911172 | 8.360883 | 8.319802 | 7.491605 | 7.925372 | 10.66467 | 8.081837 | 7.686562 | 8.940533 | 7.703226 | 7.986639 | 7.992622 | 8.112283 | 8.01141 | 7.668951 | 9.120467 | 7.944067 |
1409.1651 | Rosy Chooi Gim Teh | Amin Soltanian, Rosy Teh, Khai-Ming Wong | Multiple bifurcations and transitions for electrically charged
monopole-antimonopole chain and vortex-ring solutions | 31 pages, 16 Figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dependence of physical properties of the electrically charged two-poles
monopole-antimonopole pair (MAP) solutions in the Higgs self-coupling constant
is previously investigated. In this paper we study the three-poles
monopole-antimonopole chain (MAC) solutions. The study includes $\phi$-winding
number $n=2,3,4$,... | [
{
"created": "Fri, 5 Sep 2014 03:06:57 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Oct 2014 06:15:30 GMT",
"version": "v2"
},
{
"created": "Thu, 11 Dec 2014 07:47:18 GMT",
"version": "v3"
}
] | 2014-12-12 | [
[
"Soltanian",
"Amin",
""
],
[
"Teh",
"Rosy",
""
],
[
"Wong",
"Khai-Ming",
""
]
] | The dependence of physical properties of the electrically charged two-poles monopole-antimonopole pair (MAP) solutions in the Higgs self-coupling constant is previously investigated. In this paper we study the three-poles monopole-antimonopole chain (MAC) solutions. The study includes $\phi$-winding number $n=2,3,4$, a... | 5.227893 | 5.528167 | 5.355037 | 4.951128 | 5.463046 | 5.421737 | 5.371005 | 5.201893 | 5.269887 | 5.788904 | 5.357674 | 5.107574 | 5.267703 | 5.057375 | 5.175241 | 5.160636 | 5.142236 | 5.216459 | 5.176237 | 5.29952 | 5.109521 |
2405.10362 | David Osten | Eric Lescano and David Osten | Non-Relativistic Limits of Bosonic and Heterotic Double Field Theory | V2: 21 pages + references, relation to known results on NR-limit of
bosonic DFT in introduction and section 3 clarified, new section 3.4 added | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The known stringy non-relativistic (NR) limit of the universal NS-NS sector
of supergravity has a finite Lagrangian due to non-trivial cancellations of
divergent parts coming from the metric and the $B$-field. We demonstrate that
in Double Field Theory (DFT) and generalised geometry these cancellations
already happen... | [
{
"created": "Thu, 16 May 2024 18:00:02 GMT",
"version": "v1"
},
{
"created": "Thu, 23 May 2024 14:00:58 GMT",
"version": "v2"
}
] | 2024-05-24 | [
[
"Lescano",
"Eric",
""
],
[
"Osten",
"David",
""
]
] | The known stringy non-relativistic (NR) limit of the universal NS-NS sector of supergravity has a finite Lagrangian due to non-trivial cancellations of divergent parts coming from the metric and the $B$-field. We demonstrate that in Double Field Theory (DFT) and generalised geometry these cancellations already happen a... | 8.075278 | 8.426515 | 9.325207 | 7.610562 | 8.668507 | 7.976489 | 8.697193 | 7.515674 | 8.235772 | 9.079555 | 7.79482 | 8.135226 | 7.998027 | 7.747879 | 7.738705 | 7.970003 | 7.859674 | 7.966934 | 7.75978 | 8.024346 | 7.763227 |
hep-th/0610125 | Toshiharu Maeda | Hajime Aoki (1), Satoshi Iso (2) and Toshiharu Maeda (1) ((1) Saga
Univ., (2) KEK) | Ginsparg-Wilson Dirac operator in the monopole backgrounds on the fuzzy
2-sphere | Latex2e, 37 pages, 3 figures | Phys.Rev.D75:085021,2007 | 10.1103/PhysRevD.75.085021 | SAGA-HE-230, KEK-TH-1110 | hep-th | null | In the previous papers, we studied the 't Hooft-Polyakov (TP) monopole
configurations in the U(2) gauge theory on the fuzzy 2-sphere,and showed that
they have nonzero topological charge in the formalism based on the
Ginsparg-Wilson (GW) relation. In this paper, we will show an index theorem in
the TP monopole backgro... | [
{
"created": "Wed, 11 Oct 2006 08:09:31 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Mar 2007 05:57:20 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Aoki",
"Hajime",
""
],
[
"Iso",
"Satoshi",
""
],
[
"Maeda",
"Toshiharu",
""
]
] | In the previous papers, we studied the 't Hooft-Polyakov (TP) monopole configurations in the U(2) gauge theory on the fuzzy 2-sphere,and showed that they have nonzero topological charge in the formalism based on the Ginsparg-Wilson (GW) relation. In this paper, we will show an index theorem in the TP monopole backgroun... | 7.373949 | 6.539155 | 7.575717 | 6.411422 | 7.312732 | 6.1846 | 6.366624 | 6.682201 | 6.462128 | 8.53806 | 6.509031 | 6.766102 | 7.025004 | 6.820907 | 6.736587 | 6.843723 | 6.780617 | 6.860236 | 6.666269 | 7.26978 | 6.86143 |
1511.09309 | Daniele Binosi | D. Binosi, A. Quadri | The Cosmological Slavnov-Taylor Identity from BRST Symmetry in
Single-Field Inflation | 38 pages, no figures. Corrected an error in the bispectrum relations,
so that original Maldacena's results are now recovered. Added new sections on
the extended discussions of the in-in formalism in the BRST approach and
higher order corrections in the squeezed limit (special conformal
transformations). Revised... | null | 10.1088/1475-7516/2016/03/045 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The cosmological Slavnov-Taylor (ST) identity of the Einstein-Hilbert action
coupled to a single inflaton field is obtained from the
Becchi-Rouet-Stora-Tyutin (BRST) symmetry associated with diffeomorphism
invariance in the Arnowitt-Deser-Misner (ADM) formalism. The consistency
conditions between the correlators of t... | [
{
"created": "Mon, 30 Nov 2015 13:55:40 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Mar 2016 15:30:44 GMT",
"version": "v2"
}
] | 2016-04-06 | [
[
"Binosi",
"D.",
""
],
[
"Quadri",
"A.",
""
]
] | The cosmological Slavnov-Taylor (ST) identity of the Einstein-Hilbert action coupled to a single inflaton field is obtained from the Becchi-Rouet-Stora-Tyutin (BRST) symmetry associated with diffeomorphism invariance in the Arnowitt-Deser-Misner (ADM) formalism. The consistency conditions between the correlators of the... | 5.981674 | 5.55723 | 5.660859 | 5.438453 | 5.942132 | 5.63967 | 5.674976 | 5.545018 | 5.560331 | 5.648091 | 5.930853 | 5.498445 | 5.399156 | 5.519032 | 5.531992 | 5.518446 | 5.6583 | 5.604912 | 5.540032 | 5.239464 | 5.61876 |
0906.0582 | Nicol\'as Grandi | Marcelo Botta-Cantcheff, Nicolas Grandi, Mauricio Sturla | Wormhole solutions to Horava gravity | 17 pages, 1 figure. Replaced by revised version. Includes an appendix
with the proof of the matching condition. References added. Accepted for
publication in Phys.Rev.D | Phys.Rev.D82:124034,2010 | 10.1103/PhysRevD.82.124034 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present wormhole solutions to Horava non-relativistic gravity theory in
vacuum. We show that, if the parameter $\lambda$ is set to one, transversable
wormholes connecting two asymptotically de Sitter or anti-de Sitter regions
exist. In the case of arbitrary $\lambda$, the asymptotic regions have a more
complicated... | [
{
"created": "Tue, 2 Jun 2009 20:05:23 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Jun 2009 11:23:46 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Nov 2010 14:57:46 GMT",
"version": "v3"
}
] | 2011-01-17 | [
[
"Botta-Cantcheff",
"Marcelo",
""
],
[
"Grandi",
"Nicolas",
""
],
[
"Sturla",
"Mauricio",
""
]
] | We present wormhole solutions to Horava non-relativistic gravity theory in vacuum. We show that, if the parameter $\lambda$ is set to one, transversable wormholes connecting two asymptotically de Sitter or anti-de Sitter regions exist. In the case of arbitrary $\lambda$, the asymptotic regions have a more complicated m... | 7.475675 | 7.335226 | 7.973847 | 7.137848 | 7.546903 | 6.834025 | 7.329861 | 7.342609 | 7.468446 | 8.051502 | 7.39545 | 7.386938 | 7.839969 | 7.489231 | 7.319388 | 7.256465 | 7.08299 | 7.011511 | 7.473987 | 7.654791 | 7.51946 |
hep-th/9304055 | null | P. Mayr and S. Stieberger | Dilaton, Antisymmetric Tensor and Gauge Fields in String Effective
Theories at the One--loop Level | Latex, 20 pages, 3 figures (available upon request), MPI--Ph/93--19 | Nucl.Phys. B412 (1994) 502-522 | 10.1016/0550-3213(94)90390-5 | null | hep-th | null | We investigate the dependence of the gauge couplings on the dilaton field in
string effective theories at the one--loop level. First we resolve the
discrepancies between statements based on symmetry considerations and explicit
calculations in string effective theories on this subject. A calculation of the
relevant on... | [
{
"created": "Tue, 13 Apr 1993 21:23:34 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Mayr",
"P.",
""
],
[
"Stieberger",
"S.",
""
]
] | We investigate the dependence of the gauge couplings on the dilaton field in string effective theories at the one--loop level. First we resolve the discrepancies between statements based on symmetry considerations and explicit calculations in string effective theories on this subject. A calculation of the relevant one-... | 9.898592 | 9.337636 | 10.067199 | 9.69022 | 9.851548 | 9.784936 | 9.828588 | 10.321785 | 9.82605 | 10.911798 | 9.380544 | 9.428084 | 9.650822 | 9.447667 | 9.69506 | 9.646166 | 9.806421 | 9.577629 | 9.363411 | 10.011179 | 9.475174 |
1606.08012 | Julien Serreau | U. Reinosa, J. Serreau, M. Tissier, A. Tresmontant | Yang-Mills correlators across the deconfinement phase transition | 28 pages, 17 figures; published version | Phys. Rev. D 95, 045014 (2017) | 10.1103/PhysRevD.95.045014 | null | hep-th hep-lat hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the finite temperature ghost and gluon propagators of Yang-Mills
theory in the Landau-DeWitt gauge. The background field that enters the
definition of the latter is intimately related with the (gauge-invariant)
Polyakov loop and serves as an equivalent order parameter for the deconfinement
transition. We u... | [
{
"created": "Sun, 26 Jun 2016 08:59:21 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Mar 2017 19:25:18 GMT",
"version": "v2"
}
] | 2017-03-03 | [
[
"Reinosa",
"U.",
""
],
[
"Serreau",
"J.",
""
],
[
"Tissier",
"M.",
""
],
[
"Tresmontant",
"A.",
""
]
] | We compute the finite temperature ghost and gluon propagators of Yang-Mills theory in the Landau-DeWitt gauge. The background field that enters the definition of the latter is intimately related with the (gauge-invariant) Polyakov loop and serves as an equivalent order parameter for the deconfinement transition. We use... | 6.945311 | 6.995419 | 7.397686 | 6.479982 | 7.358602 | 7.22913 | 6.610153 | 7.15798 | 6.896559 | 7.330516 | 6.829463 | 7.041952 | 6.732282 | 6.804091 | 6.970784 | 7.007702 | 7.100909 | 6.939514 | 6.704223 | 6.875689 | 7.06338 |
hep-th/0511049 | Calin Iuliu Lazaroiu | C. I. Lazaroiu | Non-commutative moduli spaces of topological D-branes | null | Fortsch.Phys. 54 (2006) 430-434 | 10.1002/prop.200510287 | null | hep-th | null | We give a general construction of extended moduli spaces of topological
D-branes as non-commutative algebraic varieties. This shows that noncommutative
symplectic geometry in the sense of Kontsevich arises naturally in String
Theory.
| [
{
"created": "Fri, 4 Nov 2005 01:39:53 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Lazaroiu",
"C. I.",
""
]
] | We give a general construction of extended moduli spaces of topological D-branes as non-commutative algebraic varieties. This shows that noncommutative symplectic geometry in the sense of Kontsevich arises naturally in String Theory. | 7.46932 | 6.568053 | 8.875586 | 5.96939 | 6.45365 | 7.120205 | 6.321453 | 6.685241 | 6.285624 | 8.951555 | 6.714239 | 6.669781 | 8.704307 | 6.813989 | 6.448413 | 6.876762 | 6.935155 | 6.591283 | 6.786444 | 8.745313 | 6.373542 |
0902.0035 | Hyun Seok Yang | Hyun Seok Yang | Dark Energy and Emergent Spacetime | 6 pages, A contribution for the Proceedings of the Workshop on
Cosmology and Particle Astrophysics 2008, October 28 - November 1, APCTP,
Korea | Int. J. Mod. Phys. CS1:266-271, 2011 | 10.1142/S2010194511000389 | KIAS-P09006 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A natural geometric framework of noncommutative spacetime is symplectic
geometry rather than Riemannian geometry. The Darboux theorem in symplectic
geometry then admits a novel form of the equivalence principle such that the
electromagnetism in noncommutative spacetime can be regarded as a theory of
gravity. Remarkab... | [
{
"created": "Mon, 2 Feb 2009 16:48:42 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Feb 2009 01:55:01 GMT",
"version": "v2"
},
{
"created": "Thu, 30 Apr 2009 01:53:22 GMT",
"version": "v3"
}
] | 2011-10-05 | [
[
"Yang",
"Hyun Seok",
""
]
] | A natural geometric framework of noncommutative spacetime is symplectic geometry rather than Riemannian geometry. The Darboux theorem in symplectic geometry then admits a novel form of the equivalence principle such that the electromagnetism in noncommutative spacetime can be regarded as a theory of gravity. Remarkably... | 9.973611 | 9.366673 | 9.677506 | 9.379825 | 9.599208 | 10.041749 | 9.456789 | 9.63949 | 9.043046 | 9.903807 | 9.053889 | 9.071455 | 9.175628 | 9.211071 | 8.907735 | 9.240256 | 9.32118 | 9.05744 | 9.247192 | 9.485352 | 9.14681 |
2002.04050 | Erik Plauschinn | Martin Enriquez-Rojo, Erik Plauschinn | Swampland conjectures for type IIB orientifolds with closed-string U(1)s | 26+3 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the weak gravity conjecture, the swampland distance conjecture and
the emergence proposal for $\mathcal{N}=1$ orientifold compactifications of
type IIB string theory with O3-/O7-planes. We allow for orientifold projections
with $h^{2,1}_+\neq 0$ which gives rise to closed-string $U(1)$ gauge fields,
and our ... | [
{
"created": "Mon, 10 Feb 2020 19:07:26 GMT",
"version": "v1"
}
] | 2020-02-12 | [
[
"Enriquez-Rojo",
"Martin",
""
],
[
"Plauschinn",
"Erik",
""
]
] | We study the weak gravity conjecture, the swampland distance conjecture and the emergence proposal for $\mathcal{N}=1$ orientifold compactifications of type IIB string theory with O3-/O7-planes. We allow for orientifold projections with $h^{2,1}_+\neq 0$ which gives rise to closed-string $U(1)$ gauge fields, and our fi... | 7.243832 | 6.350719 | 7.901423 | 6.294197 | 7.206982 | 6.62488 | 6.601419 | 6.250022 | 6.102993 | 8.351961 | 6.318234 | 6.921044 | 7.251472 | 6.642967 | 6.848644 | 6.824408 | 6.954657 | 6.732127 | 6.733482 | 7.312444 | 6.592367 |
hep-th/0103192 | Yusuke Kimura | Yusuke Kimura | Noncommutative Gauge Theories on Fuzzy Sphere and Fuzzy Torus from
Matrix Model | 30 Pages, references added and some comments corrected | Prog.Theor.Phys. 106 (2001) 445-469 | 10.1143/PTP.106.445 | KEK-TH-752, TIT/HEP-465 | hep-th | null | We consider a reduced model of four-dimensional Yang-Mills theory with a mass
term. This matrix model has two classical solutions, two-dimensional fuzzy
sphere and two-dimensional fuzzy torus. These classical solutions are
constructed by embedding them into three or four dimensional flat space. They
exist for finite ... | [
{
"created": "Thu, 22 Mar 2001 17:22:07 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Apr 2001 11:04:21 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Kimura",
"Yusuke",
""
]
] | We consider a reduced model of four-dimensional Yang-Mills theory with a mass term. This matrix model has two classical solutions, two-dimensional fuzzy sphere and two-dimensional fuzzy torus. These classical solutions are constructed by embedding them into three or four dimensional flat space. They exist for finite si... | 10.305143 | 9.163132 | 10.938161 | 8.809854 | 10.554273 | 9.305271 | 8.686158 | 9.513631 | 9.285829 | 12.001183 | 8.785902 | 9.835236 | 11.051092 | 9.473844 | 9.363626 | 9.229646 | 9.427018 | 9.491852 | 9.396355 | 10.578078 | 9.703806 |
hep-th/0603128 | Subir Ghosh | Subir Ghosh (Indian Statistical Institute) | Study of the "Non-Abelian" Current Algebra of a Non-linear
$\sigma$-Model | Revised version, To appear in Phys.Lett.B | null | 10.1016/j.physletb.2006.07.032 | null | hep-th math-ph math.MP nlin.SI quant-ph | null | A particular form of non-linear $\sigma$-model, having a global gauge
invariance, is studied. The detailed discussion on current algebra structures
reveals the non-abelian nature of the invariance, with {\it{field dependent
structure functions}}. Reduction of the field theory to a point particle
framework yields a no... | [
{
"created": "Thu, 16 Mar 2006 12:12:14 GMT",
"version": "v1"
},
{
"created": "Sun, 16 Jul 2006 20:15:29 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Ghosh",
"Subir",
"",
"Indian Statistical Institute"
]
] | A particular form of non-linear $\sigma$-model, having a global gauge invariance, is studied. The detailed discussion on current algebra structures reveals the non-abelian nature of the invariance, with {\it{field dependent structure functions}}. Reduction of the field theory to a point particle framework yields a non-... | 14.756245 | 12.902895 | 14.096234 | 12.7161 | 12.401395 | 12.699361 | 12.844027 | 12.315666 | 12.552311 | 15.666313 | 13.654075 | 13.403435 | 13.480989 | 12.816056 | 13.03513 | 12.817753 | 12.988149 | 12.76948 | 12.863361 | 13.623443 | 13.06634 |
1711.03469 | Nava Gaddam | Panagiotis Betzios and Nava Gaddam and Olga Papadoulaki | Antipodal correlation on the meron wormhole and a bang-crunch universe | 5 pages; v2 - discussion on semi-classical stability added, published | Phys. Rev. D 97, 126006 (2018) | 10.1103/PhysRevD.97.126006 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a covariant euclidean wormhole solution to Einstein Yang-Mills
system and study scalar perturbations analytically. The fluctuation operator
has a positive definite spectrum. We compute the Euclidean Green's function,
which displays maximal antipodal correlation on the smallest three sphere. Upon
analytic c... | [
{
"created": "Thu, 9 Nov 2017 16:51:48 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Jun 2018 06:11:55 GMT",
"version": "v2"
}
] | 2018-06-20 | [
[
"Betzios",
"Panagiotis",
""
],
[
"Gaddam",
"Nava",
""
],
[
"Papadoulaki",
"Olga",
""
]
] | We present a covariant euclidean wormhole solution to Einstein Yang-Mills system and study scalar perturbations analytically. The fluctuation operator has a positive definite spectrum. We compute the Euclidean Green's function, which displays maximal antipodal correlation on the smallest three sphere. Upon analytic con... | 16.443493 | 16.631826 | 15.710263 | 14.143138 | 16.316715 | 15.977091 | 15.983366 | 16.309481 | 13.897429 | 16.670801 | 14.639213 | 14.807784 | 14.784015 | 15.587027 | 15.544604 | 14.497191 | 14.914895 | 14.429715 | 15.008881 | 15.039564 | 15.277095 |
2208.07842 | David Tong | Avner Karasik, Kaan \"Onder and David Tong | Chiral Gauge Dynamics: Candidates for Non-Supersymmetric Dualities | 41 pages. v2: minor typo fixed | null | 10.1007/JHEP11(2022)122 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study the dynamics of chiral SU(N) gauge theories. These contain Weyl
fermions in the symmetric or anti-symmetric representation of the gauge group,
together with further fermions in the fundamental and anti-fundamental. We
revisit an old proposal of Bars and Yankielowicz who match the 't Hooft
anomalies of this t... | [
{
"created": "Tue, 16 Aug 2022 16:55:24 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Oct 2022 12:41:51 GMT",
"version": "v2"
}
] | 2022-11-28 | [
[
"Karasik",
"Avner",
""
],
[
"Önder",
"Kaan",
""
],
[
"Tong",
"David",
""
]
] | We study the dynamics of chiral SU(N) gauge theories. These contain Weyl fermions in the symmetric or anti-symmetric representation of the gauge group, together with further fermions in the fundamental and anti-fundamental. We revisit an old proposal of Bars and Yankielowicz who match the 't Hooft anomalies of this the... | 7.685585 | 7.591166 | 7.964345 | 7.252257 | 7.797383 | 7.676037 | 7.359527 | 6.901725 | 7.235676 | 8.520745 | 6.956359 | 7.416397 | 7.739322 | 7.512748 | 7.246656 | 7.483792 | 7.56567 | 7.450497 | 7.518604 | 7.855362 | 7.551363 |
1106.4796 | David M. Schmidtt | David M. Schmidtt | Integrability vs Supersymmetry: Poisson Structures of The Pohlmeyer
Reduction | 33 pages, Published version | JHEP11(2011)067 | 10.1007/JHEP11(2011)067 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct recursively an infinite number of Poisson structures for the
supersymmetric integrable hierarchy governing the Pohlmeyer reduction of
superstring sigma models on the target spaces AdS_{n}\times S^n, n=2,3,5. These
Poisson structures are all non-local and not relativistic except one, which is
the canonica... | [
{
"created": "Thu, 23 Jun 2011 19:21:25 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Jul 2011 17:16:32 GMT",
"version": "v2"
},
{
"created": "Thu, 17 Nov 2011 15:13:51 GMT",
"version": "v3"
}
] | 2011-11-18 | [
[
"Schmidtt",
"David M.",
""
]
] | We construct recursively an infinite number of Poisson structures for the supersymmetric integrable hierarchy governing the Pohlmeyer reduction of superstring sigma models on the target spaces AdS_{n}\times S^n, n=2,3,5. These Poisson structures are all non-local and not relativistic except one, which is the canonical ... | 10.133877 | 10.414552 | 12.223149 | 10.084876 | 11.277882 | 9.744854 | 9.988687 | 9.834496 | 10.280279 | 13.37005 | 9.852641 | 9.64813 | 10.974567 | 9.84446 | 9.494771 | 9.530288 | 9.616044 | 9.535821 | 9.6926 | 10.62013 | 9.443355 |
hep-th/9710154 | Jerzy Plebanski | Hugo Garcia-Compean, Jerzy F. Plebanski, Maciej Przanowski | The Geometry of Deformation Quantization and Self-Dual Gravity | LaTeX, mprocl.sty, 3 pages, no figures, version to appear in the
Eighth Marcel Grossmann Meeting | null | null | CINVESTAV-FIS 27/97 | hep-th | null | A geometric formulation of the Moyal deformation for the Self-dual Yang-Mills
theory and the Chiral Model approach to Self-dual gravity is given. We find in
Fedosov's geometrical construction of deformation quantization the natural
geometrical framework associated to the Moyal deformation of Self-dual gravity.
| [
{
"created": "Mon, 20 Oct 1997 15:46:04 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Garcia-Compean",
"Hugo",
""
],
[
"Plebanski",
"Jerzy F.",
""
],
[
"Przanowski",
"Maciej",
""
]
] | A geometric formulation of the Moyal deformation for the Self-dual Yang-Mills theory and the Chiral Model approach to Self-dual gravity is given. We find in Fedosov's geometrical construction of deformation quantization the natural geometrical framework associated to the Moyal deformation of Self-dual gravity. | 13.063643 | 7.91049 | 12.206236 | 8.314121 | 7.833639 | 8.10222 | 7.602695 | 8.129508 | 9.436582 | 14.148449 | 9.04255 | 10.171334 | 12.458499 | 10.837935 | 9.978149 | 10.192698 | 10.027085 | 11.066324 | 10.640583 | 11.832859 | 10.377924 |
1207.3355 | Don N. Page | Don N. Page | Generalized Jarzynski Equality | 6 pages, LaTeX | null | null | Alberta-Thy-11-12 | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Jarzynski equality equates the mean of the exponential of the negative of
the work (per fixed temperature) done by a changing Hamiltonian on a system,
initially in thermal equilibrium at that temperature, to the ratio of the final
to the initial equilibrium partition functions of the system at that fixed
temperat... | [
{
"created": "Fri, 13 Jul 2012 20:00:04 GMT",
"version": "v1"
}
] | 2012-07-17 | [
[
"Page",
"Don N.",
""
]
] | The Jarzynski equality equates the mean of the exponential of the negative of the work (per fixed temperature) done by a changing Hamiltonian on a system, initially in thermal equilibrium at that temperature, to the ratio of the final to the initial equilibrium partition functions of the system at that fixed temperatur... | 7.374657 | 7.566047 | 9.56123 | 7.075083 | 7.753136 | 9.18364 | 9.298137 | 7.534081 | 8.235456 | 9.775342 | 6.873423 | 7.272805 | 6.555264 | 7.031505 | 6.844053 | 6.849098 | 6.710141 | 6.600719 | 7.505031 | 7.147918 | 7.330524 |
1905.12014 | Makoto Natsuume | Makoto Natsuume, Takashi Okamura | Holographic chaos, pole-skipping, and regularity | 19 pages, PTEPHY; v2: a few clarifications, published version | Prog Theor Exp Phys (2020) | 10.1093/ptep/ptz155 | KEK-TH-2128 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the "pole-skipping" phenomenon in holographic chaos. According
to the pole-skipping, the energy-density Green's function is not unique at a
special point in complex momentum plane. This arises because the bulk field
equation has two regular near-horizon solutions at the special point. We study
the regu... | [
{
"created": "Tue, 28 May 2019 18:19:22 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Feb 2020 07:32:15 GMT",
"version": "v2"
}
] | 2020-02-12 | [
[
"Natsuume",
"Makoto",
""
],
[
"Okamura",
"Takashi",
""
]
] | We investigate the "pole-skipping" phenomenon in holographic chaos. According to the pole-skipping, the energy-density Green's function is not unique at a special point in complex momentum plane. This arises because the bulk field equation has two regular near-horizon solutions at the special point. We study the regula... | 11.711554 | 9.705298 | 13.198416 | 9.474925 | 10.499949 | 9.894149 | 9.829959 | 9.484626 | 10.10643 | 13.820098 | 9.695596 | 10.434373 | 11.660945 | 10.70184 | 10.637167 | 10.797625 | 10.964314 | 10.709438 | 10.997936 | 11.886937 | 10.42636 |
hep-th/0603037 | Jamila Douari | Jamila Douari | Neumann Boundary Conditions from D1-Brane Description at the Presence of
Electric Field | 10 pages, v2: some equations are corrected and some points have been
clarified | Phys.Lett.B644:83-87,2007 | 10.1016/j.physletb.2006.11.017 | null | hep-th | null | We study the fluctuations of D1$\bot$D3 branes from D1-Brane description in
the presence of world volume electric field. The fluctuations are found to obey
Neumann boundary conditions separating the system into two regions depending on
electric field $E$.
| [
{
"created": "Mon, 6 Mar 2006 13:50:52 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Sep 2006 18:48:31 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Douari",
"Jamila",
""
]
] | We study the fluctuations of D1$\bot$D3 branes from D1-Brane description in the presence of world volume electric field. The fluctuations are found to obey Neumann boundary conditions separating the system into two regions depending on electric field $E$. | 19.468025 | 12.565304 | 19.079535 | 12.256268 | 13.929311 | 13.177503 | 13.270404 | 12.313745 | 13.729443 | 22.49991 | 11.596194 | 13.439151 | 19.244146 | 14.995707 | 14.211911 | 14.122862 | 14.262542 | 14.228327 | 14.961777 | 17.816343 | 14.022109 |
hep-th/9509162 | Kanehisa Takasaki | Toshio Nakatsu (Ritsumeikan University) and Kanehisa Takasaki (Kyoto
University) | Whitham-Toda hierarchy and N = 2 supersymmetric Yang-Mills theory | 13 pages, LaTeX | Mod.Phys.Lett. A11 (1996) 157-168 | 10.1142/S0217732396000187 | KUCP-0083 | hep-th | null | The exact solution of $N=2$ supersymmetric $SU(N)$ Yang-Mills theory is
studied in the framework of the Whitham hierarchies. The solution is identified
with a homogeneous solution of a Whitham hierarchy. This integrable hierarchy
(Whitham-Toda hierarchy) describes modulation of a quasi-periodic solution of
the (gener... | [
{
"created": "Thu, 28 Sep 1995 03:47:51 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Nakatsu",
"Toshio",
"",
"Ritsumeikan University"
],
[
"Takasaki",
"Kanehisa",
"",
"Kyoto\n University"
]
] | The exact solution of $N=2$ supersymmetric $SU(N)$ Yang-Mills theory is studied in the framework of the Whitham hierarchies. The solution is identified with a homogeneous solution of a Whitham hierarchy. This integrable hierarchy (Whitham-Toda hierarchy) describes modulation of a quasi-periodic solution of the (general... | 6.35382 | 5.451662 | 6.674027 | 5.811746 | 5.768589 | 5.470803 | 5.532753 | 5.179692 | 5.233379 | 7.578522 | 5.405794 | 5.6403 | 6.249378 | 5.528411 | 5.654033 | 5.710781 | 5.563266 | 5.590595 | 5.666779 | 6.294062 | 5.533188 |
hep-th/9410098 | null | H. Boschi-Filho, C. Farina and A. de Souza Dutra | The Partition Function for an Anyon-Like Oscillator | LaTex, 9 pages, preprint IF/UFRJ | J.Phys. A28 (1995) L7-L12 | 10.1088/0022-3727/28/1/003 | null | hep-th | null | We compute the partition function of an anyon-like harmonic oscillator. The
well known results for both the bosonic and fermionic oscillators are then
reobtained as particular cases as ours. The technique we employ is a
non-relativistic version of the Green function method used in the computation
of one-loop effectiv... | [
{
"created": "Thu, 13 Oct 1994 20:00:44 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Boschi-Filho",
"H.",
""
],
[
"Farina",
"C.",
""
],
[
"Dutra",
"A. de Souza",
""
]
] | We compute the partition function of an anyon-like harmonic oscillator. The well known results for both the bosonic and fermionic oscillators are then reobtained as particular cases as ours. The technique we employ is a non-relativistic version of the Green function method used in the computation of one-loop effective ... | 10.939724 | 9.575287 | 10.830595 | 9.837623 | 9.713099 | 10.466781 | 9.372902 | 9.700334 | 10.059639 | 11.316226 | 9.859058 | 10.450292 | 10.801787 | 10.576931 | 10.588007 | 10.190921 | 10.255392 | 10.533012 | 10.579851 | 10.964412 | 10.124612 |
1912.06025 | Marc Geiller | Marc Geiller, Puttarak Jai-akson | Extended actions, dynamics of edge modes, and entanglement entropy | 50 pages, 1 figure, published version | J. High Energ. Phys. 2020, 134 (2020) | 10.1007/JHEP09(2020)134 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we propose a simple and systematic framework for including edge
modes in gauge theories on manifolds with boundaries. We argue that this is
necessary in order to achieve the factorizability of the path integral, the
Hilbert space and the phase space, and that it explains how edge modes acquire
a boundary... | [
{
"created": "Thu, 12 Dec 2019 15:24:14 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Sep 2020 21:44:58 GMT",
"version": "v2"
}
] | 2020-10-01 | [
[
"Geiller",
"Marc",
""
],
[
"Jai-akson",
"Puttarak",
""
]
] | In this work we propose a simple and systematic framework for including edge modes in gauge theories on manifolds with boundaries. We argue that this is necessary in order to achieve the factorizability of the path integral, the Hilbert space and the phase space, and that it explains how edge modes acquire a boundary d... | 9.607471 | 8.976715 | 9.31256 | 9.230953 | 9.451446 | 9.24808 | 9.073657 | 8.912243 | 9.215747 | 10.65454 | 9.074975 | 9.149174 | 9.13791 | 8.902452 | 9.104709 | 8.887442 | 8.899964 | 8.885617 | 9.0123 | 8.992042 | 9.064848 |
hep-th/9611163 | Juan Maldacena | Juan M. Maldacena | N=2 Extremal Black Holes and Intersecting Branes | 4 pages, no figures. Typos corrected | Phys.Lett. B403 (1997) 20-22 | 10.1016/S0370-2693(97)00412-7 | RU-96-103 | hep-th | null | Using a simple hypothesis about the degrees of freedom of intersecting branes
we find a microscopic counting argument that reproduces the entropy of a class
of BPS black holes of type IIA string theory on general Calabi Yau three folds.
| [
{
"created": "Thu, 21 Nov 1996 00:47:11 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Mar 1997 16:04:54 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Maldacena",
"Juan M.",
""
]
] | Using a simple hypothesis about the degrees of freedom of intersecting branes we find a microscopic counting argument that reproduces the entropy of a class of BPS black holes of type IIA string theory on general Calabi Yau three folds. | 11.663803 | 8.368038 | 11.715935 | 8.315957 | 8.240166 | 9.266994 | 8.231276 | 8.309873 | 9.232203 | 13.182014 | 8.32297 | 8.734414 | 10.554385 | 8.506036 | 8.783016 | 8.642971 | 9.037638 | 8.801282 | 8.44826 | 11.133595 | 8.496373 |
1412.4275 | Nikolaos Brouzakis | Petros Asimakis, Nikolaos Brouzakis, Aris Katsis and Nikolaos Tetradis | Quantum Corrections in Classicalon Theories | 8 pages, 1 figure, citation added | null | 10.1016/j.physletb.2015.02.031 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the heat kernel in order to compute the one-loop effective action on a
classicalon background. We find that the UV divergences are suppressed relative
to the predictions of standard perturbation theory in the interior of the
classicalon. There is a strong analogy with the suppression of quantum
fluctuations in... | [
{
"created": "Sat, 13 Dec 2014 20:28:24 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Dec 2014 16:39:44 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Feb 2015 20:00:59 GMT",
"version": "v3"
}
] | 2015-06-23 | [
[
"Asimakis",
"Petros",
""
],
[
"Brouzakis",
"Nikolaos",
""
],
[
"Katsis",
"Aris",
""
],
[
"Tetradis",
"Nikolaos",
""
]
] | We use the heat kernel in order to compute the one-loop effective action on a classicalon background. We find that the UV divergences are suppressed relative to the predictions of standard perturbation theory in the interior of the classicalon. There is a strong analogy with the suppression of quantum fluctuations in G... | 13.975117 | 11.030121 | 11.377746 | 10.802726 | 11.552037 | 13.00654 | 11.318222 | 11.176122 | 11.205399 | 12.245257 | 11.038629 | 11.20077 | 11.817988 | 10.907838 | 11.600502 | 11.680514 | 11.50681 | 11.136877 | 11.381993 | 12.39686 | 11.497958 |
1604.06025 | Everton Murilo Carvalho Abreu | Everton M. C. Abreu, Jorge A. Neto, Rafael L. Fernandes and Albert C.
R. Mendes | Gauge-invariant extensions of the Proca model in a noncommutative
space-time | 14 pages | null | 10.1142/S0217751X16501505 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The gauge invariance analysis of theories described in noncommutative (NC)
space-times can lead us to interesting results since noncommutativity is one of
the possible paths to investigate quantum effects in classical theories such as
general relativity, for example. This theoretical possibility has motivated us
to a... | [
{
"created": "Wed, 20 Apr 2016 16:29:33 GMT",
"version": "v1"
}
] | 2016-10-12 | [
[
"Abreu",
"Everton M. C.",
""
],
[
"Neto",
"Jorge A.",
""
],
[
"Fernandes",
"Rafael L.",
""
],
[
"Mendes",
"Albert C. R.",
""
]
] | The gauge invariance analysis of theories described in noncommutative (NC) space-times can lead us to interesting results since noncommutativity is one of the possible paths to investigate quantum effects in classical theories such as general relativity, for example. This theoretical possibility has motivated us to ana... | 10.921487 | 9.877819 | 11.342548 | 9.580581 | 10.481865 | 10.024911 | 10.38361 | 9.55315 | 9.703052 | 11.750619 | 9.404369 | 9.979767 | 10.916983 | 10.225038 | 10.292146 | 10.227078 | 9.788818 | 10.068107 | 10.190773 | 10.764771 | 9.981379 |
1110.2174 | Fabio Zwirner | Francesca Catino, Giovanni Villadoro, Fabio Zwirner | On Fayet-Iliopoulos terms and de Sitter vacua in supergravity: some easy
pieces | 17 pages, no figures; v3: added sentence at the end of section 3.2 | JHEP01 (2012) 002 | 10.1007/JHEP01(2012)002 | DFPD-2011/TH/15; SLAC-PUB-14627 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We clarify a number of issues on Fayet-Iliopoulos (FI) terms in supergravity,
keeping the formalism at a minumum and making use of explicit examples. We
explain why, if the U(1) vector is massive everywhere in field space, FI terms
are not genuine and can always be redefined away or introduced when they are
not prese... | [
{
"created": "Mon, 10 Oct 2011 20:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Oct 2011 16:47:05 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Dec 2011 16:13:48 GMT",
"version": "v3"
}
] | 2012-01-12 | [
[
"Catino",
"Francesca",
""
],
[
"Villadoro",
"Giovanni",
""
],
[
"Zwirner",
"Fabio",
""
]
] | We clarify a number of issues on Fayet-Iliopoulos (FI) terms in supergravity, keeping the formalism at a minumum and making use of explicit examples. We explain why, if the U(1) vector is massive everywhere in field space, FI terms are not genuine and can always be redefined away or introduced when they are not present... | 9.584908 | 9.440244 | 9.81076 | 8.9491 | 8.56712 | 9.627101 | 9.135247 | 8.461542 | 8.672603 | 9.782885 | 8.542636 | 9.105617 | 9.261292 | 8.817742 | 9.027213 | 8.727648 | 9.065099 | 9.119823 | 8.845781 | 9.750382 | 8.720392 |
1003.0745 | Shesansu Pal | Shesansu Sekhar Pal | Weak Gravity Conjecture, Central Charges and $\eta/s$ | 1+14 pages; v2 A note and few references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We correlate the weak gravity conjecture (WGC), the KSS conjecture with
chemical potential at extremality and the central charges by going through a
particular example in five dimensional AdS spacetime with two unknown
coefficients $c_1, c_2$, assuming WGC exists in AdS spacetime. The result that
follows from this ex... | [
{
"created": "Wed, 3 Mar 2010 08:02:33 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Mar 2010 09:27:54 GMT",
"version": "v2"
}
] | 2010-03-16 | [
[
"Pal",
"Shesansu Sekhar",
""
]
] | We correlate the weak gravity conjecture (WGC), the KSS conjecture with chemical potential at extremality and the central charges by going through a particular example in five dimensional AdS spacetime with two unknown coefficients $c_1, c_2$, assuming WGC exists in AdS spacetime. The result that follows from this exam... | 8.597181 | 9.188201 | 8.4011 | 8.29507 | 8.323953 | 9.186415 | 8.351105 | 8.36323 | 8.535205 | 9.033195 | 8.034312 | 8.273593 | 8.423815 | 8.570098 | 8.492588 | 8.573152 | 8.44453 | 8.501333 | 8.716347 | 8.658799 | 8.398513 |
2006.09390 | Valentin Reys | Nikolay Bobev, Anthony M. Charles, Kiril Hristov, Valentin Reys | The Unreasonable Effectiveness of Higher-Derivative Supergravity in
AdS$_4$ Holography | 6 pages | Phys. Rev. Lett. 125, 131601 (2020) | 10.1103/PhysRevLett.125.131601 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study four-derivative corrections to four-dimensional $\mathcal{N}=2$
minimal gauged supergravity and show that they are controlled by two real
constants. The solutions of the equations of motion in the two-derivative
theory are not modified by the higher-derivative corrections. We use this to
derive a general for... | [
{
"created": "Tue, 16 Jun 2020 18:00:02 GMT",
"version": "v1"
}
] | 2020-09-30 | [
[
"Bobev",
"Nikolay",
""
],
[
"Charles",
"Anthony M.",
""
],
[
"Hristov",
"Kiril",
""
],
[
"Reys",
"Valentin",
""
]
] | We study four-derivative corrections to four-dimensional $\mathcal{N}=2$ minimal gauged supergravity and show that they are controlled by two real constants. The solutions of the equations of motion in the two-derivative theory are not modified by the higher-derivative corrections. We use this to derive a general formu... | 4.600126 | 4.500709 | 5.193008 | 4.212576 | 4.365733 | 4.264216 | 4.193026 | 4.348341 | 4.318241 | 5.292351 | 4.346598 | 4.377439 | 4.914433 | 4.419833 | 4.491187 | 4.343764 | 4.422242 | 4.437049 | 4.33568 | 4.732425 | 4.469584 |
1810.12528 | Kedar Kolekar | Kedar S. Kolekar, K. Narayan | On $AdS_2$ holography from redux, renormalization group flows and
$c$-functions | Latex, 40pgs incl appendices; v2: minor tweaks, figure added; v3:
minor clarifications added, matches version to be published | null | 10.1007/JHEP02(2019)039 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Extremal black branes upon compactification in the near horizon throat region
are known to give rise to $AdS_2$ dilaton-gravity-matter theories. Away from
the throat region, the background has nontrivial profile. We interpret this as
holographic renormalization group flow in the 2-dim dilaton-gravity-matter
theories ... | [
{
"created": "Tue, 30 Oct 2018 04:52:11 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Nov 2018 11:05:50 GMT",
"version": "v2"
},
{
"created": "Mon, 28 Jan 2019 06:26:18 GMT",
"version": "v3"
}
] | 2019-02-20 | [
[
"Kolekar",
"Kedar S.",
""
],
[
"Narayan",
"K.",
""
]
] | Extremal black branes upon compactification in the near horizon throat region are known to give rise to $AdS_2$ dilaton-gravity-matter theories. Away from the throat region, the background has nontrivial profile. We interpret this as holographic renormalization group flow in the 2-dim dilaton-gravity-matter theories ar... | 10.302447 | 10.188593 | 11.207251 | 10.089861 | 9.699754 | 10.15625 | 10.285596 | 9.792581 | 9.431238 | 11.717394 | 9.726925 | 9.993834 | 9.898002 | 9.583749 | 9.767388 | 9.46651 | 9.719319 | 9.479223 | 9.925147 | 10.111771 | 9.561349 |
2405.05168 | Hai-Qing Zhang | Tian-Chi Ma, Han-Qing Shi, Hai-Qing Zhang | Asymmetric Symmetry Breaking: Unequal Probabilities of Vacuum Selection | 5+2 pages, 3+2 figures, context improved, references added | null | null | null | hep-th cond-mat.supr-con gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Spontaneous symmetry breaking is a fundamental notion in modern physics,
ranging from high energy to condensed matter. However, the usual spontaneous
symmetry breaking only considers the equal probability to select the vacua. In
this work, we conceive a model to realize the unequal probability of the
symmetry breakin... | [
{
"created": "Wed, 8 May 2024 16:06:22 GMT",
"version": "v1"
},
{
"created": "Sat, 25 May 2024 06:35:10 GMT",
"version": "v2"
}
] | 2024-05-28 | [
[
"Ma",
"Tian-Chi",
""
],
[
"Shi",
"Han-Qing",
""
],
[
"Zhang",
"Hai-Qing",
""
]
] | Spontaneous symmetry breaking is a fundamental notion in modern physics, ranging from high energy to condensed matter. However, the usual spontaneous symmetry breaking only considers the equal probability to select the vacua. In this work, we conceive a model to realize the unequal probability of the symmetry breaking,... | 8.382137 | 8.58881 | 8.158844 | 8.299881 | 8.565772 | 8.164918 | 8.608477 | 8.158397 | 8.681937 | 8.695499 | 7.960002 | 8.144864 | 8.134202 | 7.927447 | 8.008143 | 7.990753 | 8.119956 | 7.886325 | 7.929181 | 8.185623 | 7.832386 |
0907.5555 | Wen-Yu Wen | Hsien-Chung Kao, Wen-Yu Wen | Absorption cross section in warped AdS_3 black hole revisited | 16+1 pages, typos corrected, references and footnotes added | JHEP 0909:102,2009 | 10.1088/1126-6708/2009/09/102 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the absorption cross section for minimal-coupled scalars in
the warped AdS_3 black hole. According to our calculation, the cross section
reduces to the horizon area in the low energy limit as usually expected in
contrast to what was previously found. We also calculate the greybody factor
and find that ... | [
{
"created": "Fri, 31 Jul 2009 15:31:16 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Sep 2009 14:49:54 GMT",
"version": "v2"
}
] | 2009-10-16 | [
[
"Kao",
"Hsien-Chung",
""
],
[
"Wen",
"Wen-Yu",
""
]
] | We investigate the absorption cross section for minimal-coupled scalars in the warped AdS_3 black hole. According to our calculation, the cross section reduces to the horizon area in the low energy limit as usually expected in contrast to what was previously found. We also calculate the greybody factor and find that th... | 12.329727 | 10.222734 | 12.587151 | 10.197412 | 10.443891 | 10.479396 | 10.719677 | 10.149712 | 10.105047 | 12.454244 | 10.251925 | 10.0079 | 11.407115 | 10.068521 | 9.820741 | 10.146796 | 10.202905 | 10.089262 | 9.783465 | 11.469495 | 10.017048 |
1805.00991 | Adalto R. Gomes | Adalto R. Gomes, F. C. Simas, K. Z. Nobrega, P. P. Avelino | False vacuum decay in kink scattering | 16 pages, 17 figures | null | 10.1007/JHEP10(2018)192 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we consider kink-antikink and antikink-kink collisions in a
modified $\phi^4$ model with a false vacuum characterized by a dimensionless
parameter $\epsilon$. The usual $\phi^4$ model is recovered for $\epsilon=0$.
We investigate the $\epsilon<<1$ regime where the kink in the presence of false
vacuum can... | [
{
"created": "Wed, 2 May 2018 19:32:18 GMT",
"version": "v1"
}
] | 2018-11-14 | [
[
"Gomes",
"Adalto R.",
""
],
[
"Simas",
"F. C.",
""
],
[
"Nobrega",
"K. Z.",
""
],
[
"Avelino",
"P. P.",
""
]
] | In this work we consider kink-antikink and antikink-kink collisions in a modified $\phi^4$ model with a false vacuum characterized by a dimensionless parameter $\epsilon$. The usual $\phi^4$ model is recovered for $\epsilon=0$. We investigate the $\epsilon<<1$ regime where the kink in the presence of false vacuum can b... | 6.609666 | 5.585647 | 6.303977 | 5.504754 | 5.517191 | 5.727696 | 5.857158 | 5.553873 | 5.553617 | 6.849787 | 5.544677 | 5.761642 | 6.100507 | 5.87366 | 5.97612 | 5.956217 | 5.78912 | 5.984219 | 5.943963 | 5.911421 | 5.953824 |
1011.5147 | Abolfazl Jafari | Abolfazl Jafari | The photo-balls and static solutions in NCQED with time attended | 4 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We drive the potential of photon interaction from Feynman diagrams
amplitudes, and we show that the photo-balls, can be produced in noncommutative
electrodynamics with time attended but for the static and localized fields, the
static solutions (the lumps) can not be exited.
| [
{
"created": "Mon, 22 Nov 2010 14:52:33 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Mar 2011 12:51:52 GMT",
"version": "v2"
},
{
"created": "Thu, 26 May 2011 07:11:38 GMT",
"version": "v3"
}
] | 2011-05-27 | [
[
"Jafari",
"Abolfazl",
""
]
] | We drive the potential of photon interaction from Feynman diagrams amplitudes, and we show that the photo-balls, can be produced in noncommutative electrodynamics with time attended but for the static and localized fields, the static solutions (the lumps) can not be exited. | 68.900513 | 51.032234 | 56.346111 | 50.674698 | 61.599228 | 55.391109 | 62.862251 | 55.627686 | 56.200249 | 65.35247 | 52.789291 | 46.658859 | 60.220219 | 56.474415 | 52.853428 | 49.453362 | 53.936298 | 47.456455 | 58.79538 | 59.622654 | 51.173725 |
2312.05904 | Kaberi Goswami | Kaberi Goswami, K. Narayan | Small Schwarzschild de Sitter black holes, the future boundary and
islands | Latex, 34pgs, 1 fig, v2: references, clarifications added, matches
published version. arXiv admin note: text overlap with arXiv:2207.10724 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue the study of 4-dimensional Schwarzschild de Sitter black holes in
the regime where the black hole mass is small compared with the de Sitter
scale, following arXiv:2207.10724 [hep-th]. The de Sitter temperature is very
low compared with that of the black hole. We consider the future boundary as
the locatio... | [
{
"created": "Sun, 10 Dec 2023 15:00:17 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Apr 2024 06:53:18 GMT",
"version": "v2"
}
] | 2024-04-15 | [
[
"Goswami",
"Kaberi",
""
],
[
"Narayan",
"K.",
""
]
] | We continue the study of 4-dimensional Schwarzschild de Sitter black holes in the regime where the black hole mass is small compared with the de Sitter scale, following arXiv:2207.10724 [hep-th]. The de Sitter temperature is very low compared with that of the black hole. We consider the future boundary as the location ... | 12.643252 | 10.954039 | 13.148991 | 11.545955 | 11.836098 | 12.125446 | 11.751414 | 12.061861 | 10.589708 | 14.063823 | 11.367864 | 11.655611 | 12.677086 | 11.593013 | 11.81015 | 11.721185 | 11.607377 | 11.953829 | 11.439526 | 12.656302 | 11.323251 |
1406.5290 | Mahmut Elbistan | Mahmut Elbistan | Topological Concepts for the Weyl Hamiltonians with the Berry Gauge
Field | 13 pages | null | null | null | hep-th cond-mat.mes-hall math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The winding numbers for the even d+1 spacetime dimensional Weyl Hamiltonians
are calculated in terms of the related Green's functions. It is shown that
these winding numbers result in the divergence of the Dirac monopole fields,
hence they are equal to the unit topological charge. It is demonstrated that
the winding ... | [
{
"created": "Fri, 20 Jun 2014 07:07:48 GMT",
"version": "v1"
}
] | 2014-06-23 | [
[
"Elbistan",
"Mahmut",
""
]
] | The winding numbers for the even d+1 spacetime dimensional Weyl Hamiltonians are calculated in terms of the related Green's functions. It is shown that these winding numbers result in the divergence of the Dirac monopole fields, hence they are equal to the unit topological charge. It is demonstrated that the winding nu... | 10.192085 | 10.265286 | 11.061135 | 9.715225 | 9.623058 | 9.218222 | 10.264291 | 9.571937 | 9.424995 | 10.149784 | 8.872706 | 9.479933 | 10.132278 | 9.698394 | 9.754312 | 9.631755 | 9.560888 | 9.34675 | 9.663396 | 10.130031 | 9.575899 |
hep-th/0605099 | Steven Thomas | Steven Thomas and John Ward | Non-Abelian (p,q) Strings in the Warped Deformed Conifold | 18 pages, Latex, 1 figure; Added a discussion of the case when the
warp factor parameter $b\neq 1$ and typos corrected | JHEP0612:057,2006 | 10.1088/1126-6708/2006/12/057 | QMUL-PH-06-06 | hep-th | null | We calculate the tension of $(p,q)$-strings in the warped deformed conifold
using the non-Abelian DBI action. In the large flux limit, we find exact
agreement with the recent expression obtained by Firouzjahi, Leblond and
Henry-Tye up to and including order $1/M^2$ terms if $q$ is also taken to be
large. Furthermore ... | [
{
"created": "Tue, 9 May 2006 15:23:46 GMT",
"version": "v1"
},
{
"created": "Wed, 17 May 2006 17:31:58 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Thomas",
"Steven",
""
],
[
"Ward",
"John",
""
]
] | We calculate the tension of $(p,q)$-strings in the warped deformed conifold using the non-Abelian DBI action. In the large flux limit, we find exact agreement with the recent expression obtained by Firouzjahi, Leblond and Henry-Tye up to and including order $1/M^2$ terms if $q$ is also taken to be large. Furthermore us... | 12.284197 | 11.977353 | 13.460928 | 11.494338 | 12.167095 | 12.242486 | 10.797425 | 11.137663 | 10.88151 | 14.201191 | 11.026573 | 10.895208 | 12.156636 | 10.965617 | 11.436184 | 11.142046 | 11.015868 | 10.897812 | 10.782048 | 11.783982 | 10.673457 |
1005.4408 | Barak Kol | Barak Kol | On Conformal Deformations II | 16 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The conformal index counts the number of exactly marginal deformations. In 4d
the index is given by the number of chiral primary operators of dimension 3
moded out by the complexified global group, where the quotient is defined as
usual by imposing a D-term. Here we show its consistency with the
Leigh-Strassler metho... | [
{
"created": "Mon, 24 May 2010 20:00:05 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Jun 2010 14:34:17 GMT",
"version": "v2"
}
] | 2010-06-04 | [
[
"Kol",
"Barak",
""
]
] | The conformal index counts the number of exactly marginal deformations. In 4d the index is given by the number of chiral primary operators of dimension 3 moded out by the complexified global group, where the quotient is defined as usual by imposing a D-term. Here we show its consistency with the Leigh-Strassler method ... | 16.547709 | 15.668308 | 17.394985 | 16.305426 | 19.021444 | 16.475908 | 17.985857 | 16.871658 | 15.195456 | 18.298338 | 16.194042 | 14.997863 | 16.59749 | 15.478277 | 16.018478 | 15.833329 | 15.751842 | 15.489962 | 15.840613 | 16.731308 | 15.280909 |
1706.10016 | Guozhen Wu | Sen Hu, Guozhen Wu | Entanglement Entropy of $AdS_5 \times S^5$ with massive flavors | null | Mod. Phys. Lett. A, Vol. 33, No. 3 (2018) 1850008 | 10.1142/S0217732318500086 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider backreacted $AdS_5 \times S^5$ coupled with $N_f$ massive flavors
introduced by D7-branes. The backreacted geometry is in the Veneziano limit
with fixed $N_f/N_c$. By dividing one of the directions into a line segment
with length $l$, we get two subspaces. Then we calculate the entanglement
entropy betwee... | [
{
"created": "Fri, 30 Jun 2017 04:30:08 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Jul 2017 13:44:01 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Aug 2017 03:23:23 GMT",
"version": "v3"
}
] | 2018-01-25 | [
[
"Hu",
"Sen",
""
],
[
"Wu",
"Guozhen",
""
]
] | We consider backreacted $AdS_5 \times S^5$ coupled with $N_f$ massive flavors introduced by D7-branes. The backreacted geometry is in the Veneziano limit with fixed $N_f/N_c$. By dividing one of the directions into a line segment with length $l$, we get two subspaces. Then we calculate the entanglement entropy between ... | 8.098096 | 7.118161 | 8.837211 | 6.883677 | 6.984007 | 7.062404 | 7.149919 | 7.130958 | 7.108155 | 9.291229 | 7.126894 | 7.396224 | 7.602462 | 7.832727 | 7.266773 | 7.404328 | 7.039552 | 7.564427 | 7.568933 | 8.194799 | 7.382286 |
0805.3517 | A. Yu. Petrov | M. A. Anacleto, C. Furtado, J. R. Nascimento, A. Yu. Petrov | On the dual equivalence between self-dual and Maxwell-Chern-Simons
models with Lorentz symmetry breaking | 14 pages, minor corrections, version accepted to Physical Review D | Phys.Rev.D78:065014,2008 | 10.1103/PhysRevD.78.065014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we use gauge embedding procedure and master action approach to
establish the equivalence between the self-dual and Maxwell-Chern-Simons models
with Lorentz symmetry breaking. As a result, new kinds of Lorentz-breaking
terms arise.
| [
{
"created": "Thu, 22 May 2008 17:56:27 GMT",
"version": "v1"
},
{
"created": "Mon, 26 May 2008 13:11:51 GMT",
"version": "v2"
},
{
"created": "Tue, 10 Jun 2008 16:58:30 GMT",
"version": "v3"
},
{
"created": "Wed, 13 Aug 2008 19:18:23 GMT",
"version": "v4"
}
] | 2008-12-18 | [
[
"Anacleto",
"M. A.",
""
],
[
"Furtado",
"C.",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
]
] | In this paper, we use gauge embedding procedure and master action approach to establish the equivalence between the self-dual and Maxwell-Chern-Simons models with Lorentz symmetry breaking. As a result, new kinds of Lorentz-breaking terms arise. | 11.672942 | 7.39548 | 11.762913 | 7.544165 | 7.340211 | 6.77058 | 7.268258 | 6.913137 | 7.222719 | 12.929036 | 7.088699 | 8.196835 | 9.996844 | 8.601052 | 8.490586 | 8.276887 | 8.292778 | 8.23602 | 8.757468 | 9.82949 | 8.516582 |
2407.18866 | Amr Ahmadain | Amr Ahmadain, Vasudev Shyam, Zihan Yan | A Comment on Deriving the Gibbons-Hawking-York Term From the String
Worldsheet | 11 pages | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | In this note, we show that the noncovariant metric boundary term obtained
from the nonlinear sigma model worldsheet derivation of the bulk off-shell
sphere partition function is closely related to the Einstein boundary term in
the Gamma-Gamma noncovariant action. In fact, when expressed in terms of the
trace of the e... | [
{
"created": "Fri, 26 Jul 2024 16:53:23 GMT",
"version": "v1"
}
] | 2024-07-29 | [
[
"Ahmadain",
"Amr",
""
],
[
"Shyam",
"Vasudev",
""
],
[
"Yan",
"Zihan",
""
]
] | In this note, we show that the noncovariant metric boundary term obtained from the nonlinear sigma model worldsheet derivation of the bulk off-shell sphere partition function is closely related to the Einstein boundary term in the Gamma-Gamma noncovariant action. In fact, when expressed in terms of the trace of the ext... | 12.152408 | 12.653729 | 11.833515 | 10.194892 | 10.707669 | 10.65301 | 10.532928 | 10.634129 | 12.391343 | 12.009537 | 11.756497 | 10.715101 | 10.682874 | 10.692411 | 10.489137 | 10.503073 | 10.474887 | 10.264556 | 10.896553 | 11.670566 | 10.885308 |
0902.4814 | Patrick Meessen | P. Meessen, A. Palomo-Lozano | Cosmological solutions from fake N=2 EYM supergravity | 30 pages. Comments and references added, typos corrected | JHEP 0905:042,2009 | 10.1088/1126-6708/2009/05/042 | IFT-UAM/CSIC-09-08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We characterise the (fake) supersymmetric solutions of Wick-rotated N=2 d=4
gauged supergravity coupled to non-Abelian vector multiplets. In the time-like
case we obtain generalisations of Kastor & Traschen's cosmological black holes:
they have a specific time-dependence and the base-space must be 3-dimensional
hyper... | [
{
"created": "Fri, 27 Feb 2009 12:11:43 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Mar 2009 15:10:40 GMT",
"version": "v2"
},
{
"created": "Fri, 13 Mar 2009 11:53:14 GMT",
"version": "v3"
}
] | 2010-01-15 | [
[
"Meessen",
"P.",
""
],
[
"Palomo-Lozano",
"A.",
""
]
] | We characterise the (fake) supersymmetric solutions of Wick-rotated N=2 d=4 gauged supergravity coupled to non-Abelian vector multiplets. In the time-like case we obtain generalisations of Kastor & Traschen's cosmological black holes: they have a specific time-dependence and the base-space must be 3-dimensional hyperCR... | 10.570585 | 8.641817 | 12.491972 | 8.99404 | 9.080702 | 9.528066 | 9.587351 | 9.500321 | 8.688394 | 12.854452 | 8.717686 | 10.172348 | 11.485777 | 9.54827 | 10.07051 | 10.136225 | 9.788335 | 10.109606 | 9.874487 | 12.011209 | 9.515518 |
hep-th/9401109 | Simon Philip Adrian Gill | S.W. Hawking | The Superscattering Matrix for Two Dimensional Black Holes | 12 pages (R/94/4) | Phys.Rev. D50 (1994) 3982-3986 | 10.1103/PhysRevD.50.3982 | null | hep-th | null | A consistent Euclidean semi classical calculation is given for the
superscattering operator $\$ $ in the RST model for states with a constant flux
of energy. The $\$ $ operator is CPT invariant. There is no loss of quantum
coherence when the energy flux is less than a critical rate and complete loss
when the energy f... | [
{
"created": "Fri, 21 Jan 1994 18:44:43 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Hawking",
"S. W.",
""
]
] | A consistent Euclidean semi classical calculation is given for the superscattering operator $\$ $ in the RST model for states with a constant flux of energy. The $\$ $ operator is CPT invariant. There is no loss of quantum coherence when the energy flux is less than a critical rate and complete loss when the energy flu... | 27.168133 | 18.306198 | 20.340082 | 18.851196 | 22.211946 | 19.406279 | 20.271208 | 16.796301 | 18.026285 | 24.719259 | 19.7826 | 18.395531 | 19.470341 | 19.086014 | 19.0366 | 19.330381 | 19.12179 | 19.097275 | 19.346209 | 20.885668 | 19.420679 |
2207.01161 | Harold Blas | H. Blas, J.J. Monsalve, R. Quica\~no and J.R.V. Pereira | Majorana zero mode-soliton duality and in-gap and BIC bound states in
modified Toda model coupled to fermion | 68 pages, 25 figures, LaTex. New sections present a formula of the
Atiyah-Patodi-Singer-type, for non-zero and zero modes. Figs with numerical
kinks and bound states added | null | 10.1007/JHEP09(2022)082 | null | hep-th cond-mat.supr-con math-ph math.MP nlin.SI | http://creativecommons.org/licenses/by/4.0/ | A two-dimensional field theory of a fermion chirally coupled to Toda field
plus a scalar self-coupling potential is considered. Using techniques of
integrable systems we obtain analytical zero modes, in-gap states and bound
states in the continuum (BIC) for topological configurations of the scalar
field. Fermion-soli... | [
{
"created": "Mon, 4 Jul 2022 02:07:24 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Aug 2022 19:40:18 GMT",
"version": "v2"
}
] | 2022-09-28 | [
[
"Blas",
"H.",
""
],
[
"Monsalve",
"J. J.",
""
],
[
"Quicaño",
"R.",
""
],
[
"Pereira",
"J. R. V.",
""
]
] | A two-dimensional field theory of a fermion chirally coupled to Toda field plus a scalar self-coupling potential is considered. Using techniques of integrable systems we obtain analytical zero modes, in-gap states and bound states in the continuum (BIC) for topological configurations of the scalar field. Fermion-solito... | 12.26314 | 12.232481 | 12.953956 | 11.37324 | 11.916502 | 12.173784 | 12.036867 | 12.120625 | 11.856991 | 13.590034 | 11.851597 | 11.897896 | 11.912919 | 11.785204 | 11.706029 | 11.696554 | 11.931814 | 11.307649 | 11.694793 | 12.098516 | 11.601995 |
0912.5191 | Stepanyantz Konstantin | A.B.Pimenov, E.S.Shevtsova, K.V.Stepanyantz | Calculation of two-loop beta-function for general N=1 supersymmetric
Yang--Mills theory with the higher covariant derivative regularization | 9 pages, no figures, some references added | Phys.Lett.B686:293-297,2010 | 10.1016/j.physletb.2010.02.047 | null | hep-th | http://creativecommons.org/licenses/by/3.0/ | For the general renormalizable N=1 supersymmetric Yang--Mills theory,
regularized by higher covariant derivatives, a two-loop beta-function is
calculated. It is shown that all integrals, needed for obtaining this function,
can be easily calculated, because they are integrals of total derivatives.
| [
{
"created": "Mon, 28 Dec 2009 16:56:14 GMT",
"version": "v1"
},
{
"created": "Sun, 24 Jan 2010 18:08:30 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Pimenov",
"A. B.",
""
],
[
"Shevtsova",
"E. S.",
""
],
[
"Stepanyantz",
"K. V.",
""
]
] | For the general renormalizable N=1 supersymmetric Yang--Mills theory, regularized by higher covariant derivatives, a two-loop beta-function is calculated. It is shown that all integrals, needed for obtaining this function, can be easily calculated, because they are integrals of total derivatives. | 8.549963 | 5.041694 | 6.765544 | 5.388942 | 5.698119 | 5.021421 | 5.262622 | 5.196963 | 5.527947 | 7.42379 | 5.747009 | 6.021349 | 7.053202 | 6.302118 | 6.141081 | 6.195443 | 6.202192 | 6.003617 | 6.280634 | 6.944012 | 6.190693 |
hep-th/0008105 | Arkady Segal | A. Yu. Segal | Point particle in general background fields and generalized equivalence
principle | 21 pages, reference added, typos corrected | null | null | FIAN/TD/12/00 | hep-th | null | The model of point particle in general external fields is considered and the
generalized equivalence principle is suggested identifying all backgrounds
which give rise to equivalent particle dynamics. The equivalence
transformations for external fields are interpreted as gauge ones. The gauge
group appears to be a se... | [
{
"created": "Sat, 12 Aug 2000 10:30:31 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Aug 2000 11:30:32 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Segal",
"A. Yu.",
""
]
] | The model of point particle in general external fields is considered and the generalized equivalence principle is suggested identifying all backgrounds which give rise to equivalent particle dynamics. The equivalence transformations for external fields are interpreted as gauge ones. The gauge group appears to be a semi... | 21.261393 | 21.770132 | 23.420399 | 18.450171 | 19.947985 | 23.471395 | 19.925053 | 21.010675 | 21.186625 | 27.504847 | 19.848501 | 18.871643 | 21.238649 | 19.675081 | 19.742767 | 19.303017 | 18.860628 | 19.477604 | 19.683714 | 21.766567 | 19.259892 |
1902.05175 | Tadashi Okazaki | Davide Gaiotto, Tadashi Okazaki | Dualities of Corner Configurations and Supersymmetric Indices | 108 pages, 22 figures, v3: published version in JHEP | JHEP 1911 (2019) 056 | 10.1007/JHEP11(2019)056 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute supersymmetric indices which count local operators at certain
half-BPS interfaces and quarter-BPS junctions of interfaces in four-dimensional
$\mathcal{N}=4$ Super Yang-Mills theory. We use the indices as very stringent
tests of a variety of string theory-inspired conjectures about the action of
S-duality ... | [
{
"created": "Thu, 14 Feb 2019 00:51:28 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Mar 2019 23:15:43 GMT",
"version": "v2"
},
{
"created": "Sun, 17 Nov 2019 02:13:26 GMT",
"version": "v3"
}
] | 2019-11-19 | [
[
"Gaiotto",
"Davide",
""
],
[
"Okazaki",
"Tadashi",
""
]
] | We compute supersymmetric indices which count local operators at certain half-BPS interfaces and quarter-BPS junctions of interfaces in four-dimensional $\mathcal{N}=4$ Super Yang-Mills theory. We use the indices as very stringent tests of a variety of string theory-inspired conjectures about the action of S-duality on... | 11.604219 | 8.776594 | 12.57448 | 8.950102 | 9.43586 | 9.449681 | 10.055999 | 9.355171 | 8.967001 | 15.807458 | 10.029448 | 9.815989 | 12.143415 | 10.345489 | 10.279263 | 9.801408 | 10.222573 | 9.679634 | 9.769797 | 12.815907 | 10.360844 |
1610.02038 | Josiah Couch | Josiah Couch, Willy Fischler, Phuc H. Nguyen | Noether charge, black hole volume, and complexity | v4: Changed to match published version | JHEP 1703 (2017) 119 | 10.1007/JHEP03(2017)119 | UTTG-16-16 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the physical significance of the thermodynamic
volumes of AdS black holes using the Noether charge formalism of Iyer and Wald.
After applying this formalism to study the extended thermodynamics of a few
examples, we discuss how the extended thermodynamics interacts with the recent
complexity =... | [
{
"created": "Thu, 6 Oct 2016 20:00:02 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Nov 2016 20:34:46 GMT",
"version": "v2"
},
{
"created": "Mon, 6 Feb 2017 21:54:20 GMT",
"version": "v3"
},
{
"created": "Wed, 12 Apr 2017 01:01:37 GMT",
"version": "v4"
}
] | 2017-04-13 | [
[
"Couch",
"Josiah",
""
],
[
"Fischler",
"Willy",
""
],
[
"Nguyen",
"Phuc H.",
""
]
] | In this paper, we study the physical significance of the thermodynamic volumes of AdS black holes using the Noether charge formalism of Iyer and Wald. After applying this formalism to study the extended thermodynamics of a few examples, we discuss how the extended thermodynamics interacts with the recent complexity = a... | 7.76087 | 7.602377 | 8.408434 | 7.22826 | 7.420421 | 7.249316 | 7.93527 | 7.417184 | 7.187624 | 8.554922 | 7.758247 | 7.586539 | 7.741421 | 7.326621 | 7.100405 | 7.428735 | 7.143445 | 7.41688 | 7.234755 | 7.611411 | 7.339879 |
hep-th/9905022 | Alexandre Grezzi de Miranda Schmidt | Alfredo T. Suzuki and Alexandre G. M. Schmidt | Prescriptionless light-cone integrals | 6 pages, no figures, Revtex style, reference [2] corrected | Eur.Phys.J.C12:361-365,2000 | 10.1007/s100529900229 | null | hep-th | null | Perturbative quantum gauge field theory seen within the perspective of
physical gauge choices such as the light-cone entails the emergence of
troublesome poles of the type $(k\cdot n)^{-\alpha}$ in the Feynman integrals,
and these come from the boson field propagator, where $\alpha = 1,2,...$ and
$n^{\mu}$ is the ext... | [
{
"created": "Tue, 4 May 1999 13:28:45 GMT",
"version": "v1"
},
{
"created": "Tue, 11 May 1999 13:39:04 GMT",
"version": "v2"
}
] | 2011-09-13 | [
[
"Suzuki",
"Alfredo T.",
""
],
[
"Schmidt",
"Alexandre G. M.",
""
]
] | Perturbative quantum gauge field theory seen within the perspective of physical gauge choices such as the light-cone entails the emergence of troublesome poles of the type $(k\cdot n)^{-\alpha}$ in the Feynman integrals, and these come from the boson field propagator, where $\alpha = 1,2,...$ and $n^{\mu}$ is the exter... | 11.489034 | 12.762904 | 12.006622 | 11.285559 | 13.316245 | 12.535184 | 12.472865 | 12.258201 | 11.466178 | 12.534443 | 11.985852 | 11.323081 | 11.108102 | 11.017084 | 11.29758 | 11.599064 | 11.485313 | 11.149691 | 11.183691 | 11.356486 | 11.456404 |
2202.09846 | George Savvidy K | George Savvidy | Maximally Chaotic Dynamical Systems and Fundamental Interactions | 79 pages, 17 figures. Based on lectures at the International
Bogolyubov Conference "Problems of Theoretical and MathematicalPhysics" at
the Steklov Mathematical Institute, Moscow-Dubna, September 9-13, 2019
[arXiv:2001.01785] and seminars at the Niels Bohr Institute, at the CERN
Theory Department and A. Alikhan... | null | 10.1142/S0217751X22300010 | NRCPS-HE-69-2021 | hep-th astro-ph.GA math-ph math.MP nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a general review on the application of Ergodic theory to the
investigation of dynamics of the Yang-Mills gauge fields and of the
gravitational systems, as well as its application in the Monte Carlo method and
fluid dynamics. In ergodic theory the maximally chaotic dynamical systems
(MCDS) can be defined as dy... | [
{
"created": "Sun, 20 Feb 2022 16:05:18 GMT",
"version": "v1"
}
] | 2022-05-25 | [
[
"Savvidy",
"George",
""
]
] | We give a general review on the application of Ergodic theory to the investigation of dynamics of the Yang-Mills gauge fields and of the gravitational systems, as well as its application in the Monte Carlo method and fluid dynamics. In ergodic theory the maximally chaotic dynamical systems (MCDS) can be defined as dyna... | 8.237276 | 9.26365 | 8.899749 | 8.379465 | 8.419168 | 9.029175 | 8.205028 | 8.509461 | 8.089293 | 9.337362 | 8.445478 | 8.16027 | 8.399196 | 8.227482 | 8.190447 | 8.495189 | 8.261108 | 8.191376 | 8.246928 | 8.188701 | 8.147954 |
hep-th/0608226 | Alain Connes | Alain Connes | Noncommutative Geometry and the standard model with neutrino mixing | Typos removed, to appear in JHEP | JHEP0611:081,2006 | 10.1088/1126-6708/2006/11/081 | null | hep-th | null | We show that allowing the metric dimension of a space to be independent of
its KO-dimension and turning the finite noncommutative geometry F-- whose
product with classical 4-dimensional space-time gives the standard model
coupled with gravity--into a space of KO-dimension 6 by changing the grading on
the antiparticle... | [
{
"created": "Thu, 31 Aug 2006 14:00:09 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Nov 2006 16:15:58 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Connes",
"Alain",
""
]
] | We show that allowing the metric dimension of a space to be independent of its KO-dimension and turning the finite noncommutative geometry F-- whose product with classical 4-dimensional space-time gives the standard model coupled with gravity--into a space of KO-dimension 6 by changing the grading on the antiparticle s... | 13.801126 | 17.035681 | 16.171938 | 14.846968 | 13.826643 | 14.405478 | 15.576205 | 14.411159 | 14.793799 | 18.084963 | 13.817383 | 14.149917 | 14.517776 | 13.991686 | 14.357381 | 14.708001 | 14.159693 | 13.824945 | 14.043996 | 15.378171 | 13.605422 |
1410.8860 | Ivan K. Kostov | Yunfeng Jiang, Ivan Kostov, Andrei Petrovskii, Didina Serban | String Bits and the Spin Vertex | 34 pages, 6 figures, a sign correction in eq. (3.1) and appendix
added | null | 10.1016/j.nuclphysb.2015.05.029 | t14/231 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate a novel formalism for computing correlation functions of trace
operators in the planar N=4 SYM theory. The central object in our formalism is
the spin vertex, which is the weak coupling analogy of the string vertex in
string field theory. We construct the spin vertex explicitly for all sectors at
the lead... | [
{
"created": "Fri, 31 Oct 2014 19:33:43 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Dec 2014 08:29:13 GMT",
"version": "v2"
},
{
"created": "Fri, 15 May 2015 22:47:43 GMT",
"version": "v3"
}
] | 2015-12-09 | [
[
"Jiang",
"Yunfeng",
""
],
[
"Kostov",
"Ivan",
""
],
[
"Petrovskii",
"Andrei",
""
],
[
"Serban",
"Didina",
""
]
] | We initiate a novel formalism for computing correlation functions of trace operators in the planar N=4 SYM theory. The central object in our formalism is the spin vertex, which is the weak coupling analogy of the string vertex in string field theory. We construct the spin vertex explicitly for all sectors at the leadin... | 7.035841 | 7.112582 | 8.302864 | 6.986728 | 6.833029 | 6.853881 | 7.363323 | 6.634949 | 6.937001 | 9.082382 | 7.117428 | 6.864297 | 7.531385 | 6.929799 | 6.6947 | 7.119911 | 6.862467 | 6.92572 | 6.823143 | 7.301871 | 6.824719 |
hep-th/0008210 | Guy Bonneau | Guy Bonneau (LPTHE, Paris) | Regularisation : many recipes, but a unique principle : Ward identities
and Normalisation conditions. The case of CPT violation in QED | 14 pages, Latex file | Nucl.Phys. B593 (2001) 398-412 | 10.1016/S0550-3213(00)00625-8 | PAR/LPTHE/00-08 | hep-th hep-ph | null | We analyse the recent controversy on a possible Chern-Simons like term
generated through radiative corrections in QED with a CPT violating term : we
prove that, if the theory is correctly defined through Ward identities and
normalisation conditions, no Chern-Simons term appears, without any ambiguity.
This is related... | [
{
"created": "Mon, 28 Aug 2000 15:07:43 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bonneau",
"Guy",
"",
"LPTHE, Paris"
]
] | We analyse the recent controversy on a possible Chern-Simons like term generated through radiative corrections in QED with a CPT violating term : we prove that, if the theory is correctly defined through Ward identities and normalisation conditions, no Chern-Simons term appears, without any ambiguity. This is related t... | 15.795206 | 14.80125 | 15.939054 | 14.22283 | 13.630415 | 15.12391 | 14.565269 | 15.129997 | 13.550538 | 16.683039 | 14.114188 | 15.192677 | 15.428609 | 15.072823 | 15.636267 | 15.158467 | 15.270674 | 15.365993 | 14.851372 | 15.48532 | 14.681617 |
hep-th/9307063 | null | Jan Ambjorn and Charlotte F. Kristjansen | From 1-matrix model to Kontsevich model | 17 pages, Latex | Mod.Phys.Lett. A8 (1993) 2875-2890 | 10.1142/S0217732393003263 | nbi-he-93-30 | hep-th | null | Loop equations of matrix models express the invariance of the models under
field redefinitions. We use loop equations to prove that it is possible to
define continuum times for the generic hermitian {1-matrix} model such that all
correlation functions in the double scaling limit agree with the corresponding
correlati... | [
{
"created": "Fri, 9 Jul 1993 11:50:49 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ambjorn",
"Jan",
""
],
[
"Kristjansen",
"Charlotte F.",
""
]
] | Loop equations of matrix models express the invariance of the models under field redefinitions. We use loop equations to prove that it is possible to define continuum times for the generic hermitian {1-matrix} model such that all correlation functions in the double scaling limit agree with the corresponding correlation... | 9.009444 | 8.244655 | 10.000567 | 7.839788 | 8.864722 | 7.945306 | 8.21276 | 8.358383 | 7.885998 | 9.493137 | 8.026974 | 8.08919 | 7.924233 | 7.875196 | 8.024683 | 8.256604 | 7.57267 | 8.327713 | 7.971947 | 8.300586 | 8.054963 |
1503.04594 | Daisuke Kawai | Yuhma Asano, Daisuke Kawai and Kentaroh Yoshida | Chaos in the BMN matrix model | 23 pages, 15 figures, v2: further clarifications and references added | null | null | KUNS-2546 | hep-th math-ph math.MP nlin.CD nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study classical chaotic motions in the Berenstein-Maldacena-Nastase (BMN)
matrix model. For this purpose, it is convenient to focus upon a reduced system
composed of two-coupled anharmonic oscillators by supposing an ansatz. We
examine three ans\"atze: 1) two pulsating fuzzy spheres, 2) a single
Coulomb-type poten... | [
{
"created": "Mon, 16 Mar 2015 10:30:33 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Jun 2015 16:47:13 GMT",
"version": "v2"
}
] | 2015-06-10 | [
[
"Asano",
"Yuhma",
""
],
[
"Kawai",
"Daisuke",
""
],
[
"Yoshida",
"Kentaroh",
""
]
] | We study classical chaotic motions in the Berenstein-Maldacena-Nastase (BMN) matrix model. For this purpose, it is convenient to focus upon a reduced system composed of two-coupled anharmonic oscillators by supposing an ansatz. We examine three ans\"atze: 1) two pulsating fuzzy spheres, 2) a single Coulomb-type potenti... | 6.703874 | 5.720097 | 6.990947 | 5.965751 | 6.034028 | 5.96709 | 5.684644 | 5.720794 | 6.019294 | 6.625557 | 5.964869 | 6.30016 | 6.259181 | 6.174072 | 6.299204 | 6.209294 | 6.092905 | 6.165019 | 6.212979 | 6.143951 | 6.103418 |
hep-th/9402056 | Eduardo Ramos | Eduardo Ramos and Sonia Stanciu | On the Supersymmetric BKP-Hierarchy | 15 pages, Plain TeX, QMW-PH-94-3 | Nucl.Phys. B427 (1994) 338-350 | 10.1016/0550-3213(94)90280-1 | null | hep-th | null | We prove that the supersymmetric BKP-hierarchy of Yu (SBKP_2) is hamiltonian
with respect to a nonlinear extension of the N=1 Super-Virasoro algebra
(W_SBKP) by fields of spin k, where k>3/2 and 2k = 0,3 mod 4. Moreover, we show
how to associate in a similar manner an N=1 W-superalgebra with every
integrable hierarch... | [
{
"created": "Thu, 10 Feb 1994 00:08:39 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ramos",
"Eduardo",
""
],
[
"Stanciu",
"Sonia",
""
]
] | We prove that the supersymmetric BKP-hierarchy of Yu (SBKP_2) is hamiltonian with respect to a nonlinear extension of the N=1 Super-Virasoro algebra (W_SBKP) by fields of spin k, where k>3/2 and 2k = 0,3 mod 4. Moreover, we show how to associate in a similar manner an N=1 W-superalgebra with every integrable hierarchy ... | 9.677245 | 10.750104 | 13.878853 | 9.553141 | 9.645366 | 10.879973 | 10.656484 | 11.541799 | 10.171089 | 12.568321 | 11.403289 | 9.971345 | 10.695862 | 10.572682 | 11.286801 | 10.601437 | 10.453957 | 10.813251 | 10.477212 | 10.325497 | 10.407517 |
hep-th/9506117 | null | S.D. Odintsov and A. Wipf | Running surface couplings | 11 pages, Latex file | Phys.Lett.B356:26-31,1995 | 10.1016/0370-2693(95)00806-V | preprint uni-jena- TPI 1/95 | hep-th | null | We discuss the renormalization group improved effective action and running
surface couplings in curved spacetime with boundary. Using scalar
self-interacting theory as an example, we study the influence of the boundary
effects to effective equations of motion in spherical cap and the relevance of
surface running coup... | [
{
"created": "Mon, 19 Jun 1995 12:00:57 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Odintsov",
"S. D.",
""
],
[
"Wipf",
"A.",
""
]
] | We discuss the renormalization group improved effective action and running surface couplings in curved spacetime with boundary. Using scalar self-interacting theory as an example, we study the influence of the boundary effects to effective equations of motion in spherical cap and the relevance of surface running coupli... | 16.95611 | 15.381794 | 17.241016 | 14.516685 | 16.532995 | 15.256485 | 17.44623 | 14.596662 | 15.41328 | 19.249407 | 13.475491 | 16.148863 | 15.742478 | 15.787158 | 16.731464 | 16.599205 | 15.316036 | 15.558513 | 16.106981 | 15.82515 | 15.707337 |
hep-th/0512129 | Matthias Schmidt | S. Charzy\'nski, G. Rudolph, M. Schmidt | On the Topology of the Reduced Classical Configuration Space of Lattice
QCD | 33 pages, 3 figures | J.Geom.Phys.58:1607-1623,2008 | 10.1016/j.geomphys.2008.07.005 | null | hep-th math-ph math.MP | null | We study the topological structure of the quotient of $SU(3)\times SU(3)$ by
diagonal conjugation. This is the simplest nontrivial example for the classical
reduced configuration space of chromodynamics on a spatial lattice in the
Hamiltonian approach. We construct a cell complex structure of the quotient in
such a w... | [
{
"created": "Mon, 12 Dec 2005 14:39:56 GMT",
"version": "v1"
},
{
"created": "Mon, 31 Mar 2008 09:24:49 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Charzyński",
"S.",
""
],
[
"Rudolph",
"G.",
""
],
[
"Schmidt",
"M.",
""
]
] | We study the topological structure of the quotient of $SU(3)\times SU(3)$ by diagonal conjugation. This is the simplest nontrivial example for the classical reduced configuration space of chromodynamics on a spatial lattice in the Hamiltonian approach. We construct a cell complex structure of the quotient in such a way... | 8.2894 | 8.534745 | 8.182965 | 8.11767 | 9.165418 | 8.91712 | 9.332106 | 8.564301 | 9.340192 | 8.914153 | 8.581033 | 8.882661 | 7.78311 | 8.25001 | 8.467269 | 8.532993 | 8.96553 | 8.457217 | 8.275559 | 8.822704 | 8.382527 |
2108.08694 | Bobby Eka Gunara | Emir Syahreza Fadhilla, Bobby Eka Gunara, and Ardian Nata Atmaja | BPS Skyrmions of Generalized Skyrme Model In Higher Dimensions | 37 pages, 3 figures. Major revisions: discussion about submodels and
the case of $B \ge 1% and appendices added, and some references added.
Discussion and analysis improved. Accepted in JHEP | null | null | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | In this work we consider the higher dimensional Skyrme model, with spatial
dimension $d > 3$, focusing on its BPS submodels and their corresponding
features. To accommodate the cases with a higher topological degree, \(B\geq
1\), a modified generalized hedgehog ansatz is used where we assign an integer
\(n_i\) for ea... | [
{
"created": "Thu, 19 Aug 2021 14:02:00 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Nov 2021 14:30:30 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Aug 2022 14:06:47 GMT",
"version": "v3"
}
] | 2022-08-03 | [
[
"Fadhilla",
"Emir Syahreza",
""
],
[
"Gunara",
"Bobby Eka",
""
],
[
"Atmaja",
"Ardian Nata",
""
]
] | In this work we consider the higher dimensional Skyrme model, with spatial dimension $d > 3$, focusing on its BPS submodels and their corresponding features. To accommodate the cases with a higher topological degree, \(B\geq 1\), a modified generalized hedgehog ansatz is used where we assign an integer \(n_i\) for each... | 9.05399 | 8.450624 | 9.665956 | 8.399844 | 9.061127 | 8.586575 | 8.533581 | 8.441564 | 8.458736 | 9.94519 | 8.891941 | 8.541874 | 8.695874 | 8.56841 | 8.482424 | 8.549322 | 8.448074 | 8.439347 | 8.507098 | 8.841672 | 8.501457 |
1901.11292 | Josef Kluson | J. Kluson | (m,n)-String and D1-Brane in Stringy Newton-Cartan Background | 19 pages | null | 10.1007/JHEP04(2019)163 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper is devoted to the analysis of (m,n)-string in stringy
Newton-Cartan background. We start with the Hamiltonian constraint for
(m,n)-string in general background and perform limiting procedure on metric and
NSNS and Ramond-Ramond two form background that leads to stringy Newton-Cartan
gravity. We also analyz... | [
{
"created": "Thu, 31 Jan 2019 09:59:30 GMT",
"version": "v1"
}
] | 2019-05-22 | [
[
"Kluson",
"J.",
""
]
] | This paper is devoted to the analysis of (m,n)-string in stringy Newton-Cartan background. We start with the Hamiltonian constraint for (m,n)-string in general background and perform limiting procedure on metric and NSNS and Ramond-Ramond two form background that leads to stringy Newton-Cartan gravity. We also analyze ... | 10.472829 | 8.071497 | 10.802705 | 8.226774 | 8.27908 | 8.010733 | 8.378501 | 9.108758 | 7.852139 | 11.420686 | 8.533022 | 8.096136 | 9.604569 | 8.497769 | 8.272545 | 8.232528 | 8.228732 | 8.271802 | 8.239513 | 9.287376 | 8.736349 |
2007.08913 | Ioannis Lavdas | Ioannis Lavdas, Dieter Lust | Massive gravitons on the Landscape and the AdS Distance Conjecture | null | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work regards IIB string theory embeddings of massive and bi-metric
$AdS_{4}$ gravity where the spectrum of the theory includes multiple massive
gravitons. The corresponding geometry consists of multiple
$AdS_{4}\times_{w}\mathcal{M}_{6}$ spacetimes coupled by Janus throats of
different radii. In the second part ... | [
{
"created": "Fri, 17 Jul 2020 11:42:33 GMT",
"version": "v1"
}
] | 2020-07-20 | [
[
"Lavdas",
"Ioannis",
""
],
[
"Lust",
"Dieter",
""
]
] | This work regards IIB string theory embeddings of massive and bi-metric $AdS_{4}$ gravity where the spectrum of the theory includes multiple massive gravitons. The corresponding geometry consists of multiple $AdS_{4}\times_{w}\mathcal{M}_{6}$ spacetimes coupled by Janus throats of different radii. In the second part of... | 12.020804 | 11.494395 | 13.761517 | 10.072433 | 10.988302 | 10.376507 | 11.445467 | 11.077287 | 11.222226 | 14.020457 | 10.898225 | 10.818784 | 11.076145 | 11.122463 | 11.031465 | 11.349471 | 10.910847 | 10.561275 | 10.985105 | 11.697268 | 11.135613 |
hep-th/9503043 | Hidetoshi Awata | H. Awata, Y. Matsuo, S. Odake and J. Shiraishi | Excited States of Calogero-Sutherland Model and Singular Vectors of the
$W_N$ Algebra | LaTeX, 29 pages, 2 figures, New sections for skew-Jack polynomial and
example of singular vectors added | Nucl.Phys. B449 (1995) 347-374 | 10.1016/0550-3213(95)00286-2 | RIMS-1009, YITP/U-95-3, SULDP-1995-2 | hep-th cond-mat | null | Using the collective field method, we find a relation between the Jack
symmetric polynomials, which describe the excited states of the
Calogero-Sutherland model, and the singular vectors of the $W_N$ algebra. Based
on this relation, we obtain their integral representations. We also give a
direct algebraic method whic... | [
{
"created": "Tue, 7 Mar 1995 17:45:13 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Mar 1995 05:48:54 GMT",
"version": "v2"
},
{
"created": "Thu, 9 Mar 1995 13:35:42 GMT",
"version": "v3"
},
{
"created": "Thu, 11 May 1995 08:21:23 GMT",
"version": "v4"
}
] | 2009-10-28 | [
[
"Awata",
"H.",
""
],
[
"Matsuo",
"Y.",
""
],
[
"Odake",
"S.",
""
],
[
"Shiraishi",
"J.",
""
]
] | Using the collective field method, we find a relation between the Jack symmetric polynomials, which describe the excited states of the Calogero-Sutherland model, and the singular vectors of the $W_N$ algebra. Based on this relation, we obtain their integral representations. We also give a direct algebraic method which ... | 9.804968 | 6.374598 | 11.847004 | 6.538424 | 6.296596 | 6.156139 | 6.601641 | 6.180663 | 6.577462 | 9.562402 | 6.880541 | 6.932434 | 9.401543 | 7.595758 | 7.462969 | 7.477799 | 7.320022 | 7.49537 | 7.302027 | 9.174994 | 7.038795 |
0801.3274 | Zohar Komargodski | Zohar Komargodski | On collinear factorization of Wilson loops and MHV amplitudes in N=4 SYM | 26 pages, 7 figures, JHEP format. v2: minor corrections. v3: minor
improvements | JHEP 0805:019,2008 | 10.1088/1126-6708/2008/05/019 | WIS/01/08-JAN-DPP | hep-th | null | We consider the (multi) Splitting function of Wilson loops and MHV gluon
scattering S matrix elements in N=4 SYM. At strong coupling, one can utilize
the methods of Alday and Maldacena and at weak coupling (one loop) the
correspondence to light like Wilson loops is used. In both cases, the (multi)
Splitting function ... | [
{
"created": "Mon, 21 Jan 2008 21:05:36 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2008 21:24:57 GMT",
"version": "v2"
},
{
"created": "Thu, 17 Apr 2008 12:24:48 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Komargodski",
"Zohar",
""
]
] | We consider the (multi) Splitting function of Wilson loops and MHV gluon scattering S matrix elements in N=4 SYM. At strong coupling, one can utilize the methods of Alday and Maldacena and at weak coupling (one loop) the correspondence to light like Wilson loops is used. In both cases, the (multi) Splitting function co... | 12.805308 | 15.208641 | 14.559752 | 12.582905 | 12.887459 | 13.225152 | 13.451412 | 12.893955 | 12.883757 | 15.654664 | 12.654619 | 12.738533 | 12.885444 | 12.065919 | 12.78903 | 12.367699 | 12.698725 | 12.632318 | 12.362507 | 13.179551 | 12.48168 |
1912.05780 | Leo Rodriguez | Sathwik Bharadwaj, L. R. Ram-Mohan, Leo Rodriguez, Shanshan Rodriguez | Exploration of The Duality Between Generalized Geometry and
Extraordinary Magnetoresistance | 13 pages and 6 figures. Revised/edited for clarity and purpose.
Several references added. Updated title based on suggestions and comments
received. Version accepted for publication in Phys.Rev.B | Phys. Rev. B 101, 174417 (2020) | 10.1103/PhysRevB.101.174417 | null | hep-th cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We outline the duality between the extraordinary magnetoresistance (EMR),
observed in semiconductor-metal hybrids, and non-symmetric gravity coupled to a
diffusive $U(1)$ gauge field. The corresponding gravity theory may be
interpreted as the generalized complex geometry of the semi-direct product of
the symmetric me... | [
{
"created": "Thu, 12 Dec 2019 05:47:41 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Apr 2020 06:06:12 GMT",
"version": "v2"
}
] | 2023-05-24 | [
[
"Bharadwaj",
"Sathwik",
""
],
[
"Ram-Mohan",
"L. R.",
""
],
[
"Rodriguez",
"Leo",
""
],
[
"Rodriguez",
"Shanshan",
""
]
] | We outline the duality between the extraordinary magnetoresistance (EMR), observed in semiconductor-metal hybrids, and non-symmetric gravity coupled to a diffusive $U(1)$ gauge field. The corresponding gravity theory may be interpreted as the generalized complex geometry of the semi-direct product of the symmetric metr... | 16.707037 | 19.187181 | 18.285826 | 17.27755 | 17.697977 | 17.349184 | 17.590567 | 18.519844 | 17.588829 | 20.103632 | 16.158464 | 16.036419 | 16.234632 | 15.537368 | 15.887309 | 15.397336 | 15.90125 | 15.603629 | 16.657745 | 17.290991 | 15.77494 |
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