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values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0703018 | Voja Radovanovic | Dusko Latas, Voja Radovanovic and Josip Trampetic | Non-commutative SU(N) gauge theories and asymptotic freedom | 16 pages, no figures | Phys.Rev.D76:085006,2007 | 10.1103/PhysRevD.76.085006 | null | hep-th | null | In this paper we analyze the one-loop renormalization of the
$\theta$-expanded $\rm SU(N)$ Yang-Mills theory. We show that the {\it freedom
parameter} $a$, key to renormalization, originates from higher order
non-commutative gauge interaction, represented by a higher derivative term $ b
h \theta^{\mu\nu}\hat F_{\mu\n... | [
{
"created": "Fri, 2 Mar 2007 10:01:40 GMT",
"version": "v1"
},
{
"created": "Sat, 21 Apr 2007 14:33:23 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Latas",
"Dusko",
""
],
[
"Radovanovic",
"Voja",
""
],
[
"Trampetic",
"Josip",
""
]
] | In this paper we analyze the one-loop renormalization of the $\theta$-expanded $\rm SU(N)$ Yang-Mills theory. We show that the {\it freedom parameter} $a$, key to renormalization, originates from higher order non-commutative gauge interaction, represented by a higher derivative term $ b h \theta^{\mu\nu}\hat F_{\mu\nu}... | 6.233776 | 6.5281 | 6.422888 | 5.83285 | 6.249457 | 5.99952 | 6.040088 | 6.085397 | 5.725836 | 6.251058 | 5.805078 | 5.841558 | 6.029087 | 5.871886 | 5.922267 | 5.835401 | 5.866621 | 5.809708 | 5.823256 | 6.356679 | 5.861869 |
1307.5340 | Carlos M. Reyes | Carlos M. Reyes | Unitarity in higher-order Lorentz-invariance violating QED | 7 pages, 2 figures, to appear in Phys. Rev.D | Phys.Rev.D87:125028,2013 | 10.1103/PhysRevD.87.125028 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The unitarity in Lorentz invariance violating QED consisting of standard
fermions and higher-order photons of the Myers-Pospelov theory is studied. We
find ghost states associated to the higher-order character of the theory which
could render the $S$ matrix nonunitary. An explicit calculation to check
perturbative un... | [
{
"created": "Fri, 19 Jul 2013 21:21:59 GMT",
"version": "v1"
}
] | 2013-07-24 | [
[
"Reyes",
"Carlos M.",
""
]
] | The unitarity in Lorentz invariance violating QED consisting of standard fermions and higher-order photons of the Myers-Pospelov theory is studied. We find ghost states associated to the higher-order character of the theory which could render the $S$ matrix nonunitary. An explicit calculation to check perturbative unit... | 12.265336 | 10.227688 | 10.691292 | 10.814138 | 10.686232 | 9.179654 | 10.228734 | 9.532081 | 10.283606 | 10.389956 | 10.89598 | 10.933367 | 10.703313 | 10.480437 | 10.784269 | 10.559676 | 11.165468 | 10.546163 | 9.923997 | 10.372935 | 10.726728 |
hep-th/9910141 | Helmut Kroger | H. Jirari, H. Kr\"oger, X.Q. Luo, K.J.M. Moriarty, and S.G. Rubin | Closed Path Integrals and Renormalisation in Quantum Mechanics | Revised text, 1 figure added; Text (LaTeX file), 1 Figure (ps file) | Phys.Rev.Lett. 86 (2001) 187-191 | 10.1103/PhysRevLett.86.187 | null | hep-th quant-ph | null | We suggest a closed form expression for the path integral of quantum
transition amplitudes. We introduce a quantum action with renormalized
parameters. We present numerical results for the $V \sim x^{4}$ potential. The
renormalized action is relevant for quantum chaos and quantum instantons.
| [
{
"created": "Mon, 18 Oct 1999 13:50:02 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Apr 2000 15:14:18 GMT",
"version": "v2"
}
] | 2016-08-15 | [
[
"Jirari",
"H.",
""
],
[
"Kröger",
"H.",
""
],
[
"Luo",
"X. Q.",
""
],
[
"Moriarty",
"K. J. M.",
""
],
[
"Rubin",
"S. G.",
""
]
] | We suggest a closed form expression for the path integral of quantum transition amplitudes. We introduce a quantum action with renormalized parameters. We present numerical results for the $V \sim x^{4}$ potential. The renormalized action is relevant for quantum chaos and quantum instantons. | 14.869636 | 15.47014 | 16.239618 | 14.383815 | 14.345386 | 13.783724 | 15.462086 | 13.549843 | 15.102294 | 16.126225 | 13.955578 | 14.884132 | 16.146656 | 15.252892 | 15.207139 | 14.659676 | 15.199495 | 14.775974 | 15.537334 | 16.26903 | 14.036539 |
1811.04040 | Sebastian Waeber | Sebastian Waeber | Quasinormal modes of magnetic black branes at finite 't Hooft coupling | 33 pages, corrected typos, included cautionary remark in section 3.6 | null | 10.1007/JHEP08(2019)006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of this work is to extend the knowledge about Quasinormal Modes
(QNMs) and the equilibration of strongly coupled systems, specifically of a
quark gluon plasma (which we consider to be in a strong magnetic background
field) by using the duality between $\mathcal{N}=4$ Super Yang-Mills (SYM)
theory and type IIb... | [
{
"created": "Fri, 9 Nov 2018 17:44:21 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Nov 2018 09:06:57 GMT",
"version": "v2"
},
{
"created": "Thu, 29 Nov 2018 10:57:08 GMT",
"version": "v3"
}
] | 2019-08-06 | [
[
"Waeber",
"Sebastian",
""
]
] | The aim of this work is to extend the knowledge about Quasinormal Modes (QNMs) and the equilibration of strongly coupled systems, specifically of a quark gluon plasma (which we consider to be in a strong magnetic background field) by using the duality between $\mathcal{N}=4$ Super Yang-Mills (SYM) theory and type IIb S... | 8.251693 | 8.176719 | 8.470238 | 8.311945 | 7.788953 | 8.707156 | 8.386045 | 7.875168 | 8.410419 | 9.132225 | 7.783087 | 7.643362 | 7.932768 | 7.640769 | 8.049263 | 8.035489 | 7.81502 | 7.871416 | 7.959518 | 8.082629 | 7.673922 |
2207.01665 | Alexander Belavin | A. Artemev and A. Belavin | Five-point correlation numbers in minimal Liouville gravity and matrix
models | null | null | 10.1016/j.nuclphysb.2022.116019 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this article, we will show how to use Zamolodchikov's higher equations of
motion in Liouville field theory to explicitly calculate $N$-point correlation
numbers in minimal Liouville gravity for $N>4$. We find the explicit expression
for the 5-point correlation numbers and compare it with calculations in the
one-ma... | [
{
"created": "Mon, 4 Jul 2022 18:32:07 GMT",
"version": "v1"
}
] | 2022-11-30 | [
[
"Artemev",
"A.",
""
],
[
"Belavin",
"A.",
""
]
] | In this article, we will show how to use Zamolodchikov's higher equations of motion in Liouville field theory to explicitly calculate $N$-point correlation numbers in minimal Liouville gravity for $N>4$. We find the explicit expression for the 5-point correlation numbers and compare it with calculations in the one-matr... | 8.78655 | 6.233779 | 7.921544 | 7.111348 | 7.082876 | 6.050848 | 6.388185 | 6.373348 | 7.064982 | 9.5794 | 7.036181 | 7.65305 | 7.757588 | 7.692773 | 7.437703 | 7.197147 | 7.542016 | 7.141624 | 7.608343 | 7.604702 | 7.357052 |
1811.12653 | Yi-Jian Du | Linghui Hou, Yi-Jian Du | A graphic approach to gauge invariance induced identity | 75 pages, 35figures, 4 tables | null | 10.1007/JHEP05(2019)012 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | All tree-level amplitudes in Einstein-Yang-Mills (EYM) theory and gravity
(GR) can be expanded in terms of color ordered Yang-Mills (YM) ones whose
coefficients are polynomial functions of Lorentz inner products and are
constructed by a graphic rule. Once the gauge invariance condition of any
graviton is imposed, the... | [
{
"created": "Fri, 30 Nov 2018 07:42:12 GMT",
"version": "v1"
}
] | 2019-05-22 | [
[
"Hou",
"Linghui",
""
],
[
"Du",
"Yi-Jian",
""
]
] | All tree-level amplitudes in Einstein-Yang-Mills (EYM) theory and gravity (GR) can be expanded in terms of color ordered Yang-Mills (YM) ones whose coefficients are polynomial functions of Lorentz inner products and are constructed by a graphic rule. Once the gauge invariance condition of any graviton is imposed, the e... | 6.762592 | 6.444415 | 7.446146 | 6.081201 | 6.461135 | 6.084794 | 6.090107 | 6.132808 | 6.276378 | 7.819386 | 6.052115 | 6.239533 | 6.414665 | 6.094386 | 6.163306 | 6.288105 | 6.102835 | 6.199116 | 6.12684 | 6.561845 | 6.078187 |
2308.13704 | Gabriel Menezes | John F. Donoghue, Gabriel Menezes | Higher Derivative Sigma Models | 19 pages, 1 figure | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the nature of running couplings in the higher derivative linear
and nonlinear sigma models and show that the results in dimensional
regularization for the physical running couplings do not always match the
values quoted in the literature. Heat kernel methods identify divergences
correctly, but not all of t... | [
{
"created": "Fri, 25 Aug 2023 23:28:20 GMT",
"version": "v1"
}
] | 2023-08-29 | [
[
"Donoghue",
"John F.",
""
],
[
"Menezes",
"Gabriel",
""
]
] | We explore the nature of running couplings in the higher derivative linear and nonlinear sigma models and show that the results in dimensional regularization for the physical running couplings do not always match the values quoted in the literature. Heat kernel methods identify divergences correctly, but not all of the... | 12.88028 | 12.539129 | 11.932656 | 12.284728 | 12.597277 | 12.32585 | 12.215324 | 11.962616 | 11.855741 | 12.58523 | 11.528604 | 11.835124 | 11.745518 | 11.614948 | 11.467717 | 11.995684 | 11.562251 | 12.048588 | 11.635017 | 11.805402 | 11.733513 |
hep-th/0502127 | Petr Horava | Petr Horava, Peter G. Shepard | Topology Changing Transitions in Bubbling Geometries | 24 pages, 8 figures | JHEP 0502 (2005) 063 | 10.1088/1126-6708/2005/02/063 | null | hep-th | null | Topological transitions in bubbling half-BPS Type IIB geometries with SO(4) x
SO(4) symmetry can be decomposed into a sequence of n elementary transitions.
The half-BPS solution that describes the elementary transition is seeded by a
phase space distribution of fermions filling two diagonal quadrants. We study
the ge... | [
{
"created": "Tue, 15 Feb 2005 02:23:44 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Horava",
"Petr",
""
],
[
"Shepard",
"Peter G.",
""
]
] | Topological transitions in bubbling half-BPS Type IIB geometries with SO(4) x SO(4) symmetry can be decomposed into a sequence of n elementary transitions. The half-BPS solution that describes the elementary transition is seeded by a phase space distribution of fermions filling two diagonal quadrants. We study the geom... | 11.059434 | 10.774225 | 12.457047 | 10.218005 | 10.450451 | 10.540408 | 10.932324 | 10.263598 | 9.721681 | 11.744394 | 10.21112 | 10.41442 | 10.63014 | 10.160899 | 10.549928 | 10.539908 | 10.438349 | 10.276336 | 10.123057 | 10.668137 | 10.293127 |
1108.4326 | Takahiro Nishinaka | Takahiro Nishinaka and Yutaka Yoshida | A note on statistical model for BPS D4-D2-D0 states | 14 pages, 7 figures | null | 10.1016/j.physletb.2012.03.071 | KEK-TH-1488 | hep-th math.AG math.CO math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a statistical model that reproduces the BPS partition function
of D4-D2-D0 bound states on a class of toric Calabi-Yau three-folds. The
Calabi-Yau three-folds we consider are obtained by adding a compact two-cycle
to $A_{N-1}$-ALE $\times \mathbb{C}$. We show that in the small radii limit of
the Calabi-Y... | [
{
"created": "Mon, 22 Aug 2011 14:18:23 GMT",
"version": "v1"
}
] | 2015-05-30 | [
[
"Nishinaka",
"Takahiro",
""
],
[
"Yoshida",
"Yutaka",
""
]
] | We construct a statistical model that reproduces the BPS partition function of D4-D2-D0 bound states on a class of toric Calabi-Yau three-folds. The Calabi-Yau three-folds we consider are obtained by adding a compact two-cycle to $A_{N-1}$-ALE $\times \mathbb{C}$. We show that in the small radii limit of the Calabi-Yau... | 7.101393 | 6.716686 | 8.59931 | 6.208561 | 6.72969 | 5.972135 | 6.637922 | 6.192479 | 6.641887 | 8.313321 | 6.174275 | 6.330222 | 7.436493 | 6.333592 | 6.314163 | 6.336125 | 6.547499 | 6.273037 | 6.528098 | 7.812695 | 6.380857 |
hep-th/0303047 | Alexei Yung | K. Evlampiev and A. Yung | Flux Tubes on Higgs Branches in SUSY Gauge Theories | LATEX file, 35 p., no figures | Nucl.Phys.B662:120-146,2003 | 10.1016/S0550-3213(03)00302-X | PNPI-TH-2512/03, ITEP-TH-19/03 | hep-th | null | We study flux tubes on Higgs branches with curved geometry in supersymmetric
gauge theories. As a first example we consider N=1 QED with one flavor of
charges and with Higgs branch curved by adding a Fayet-Iliopoulos (FI) term. We
show that in a generic vacuum on the Higgs branch flux tubes exist but become
``thick''... | [
{
"created": "Thu, 6 Mar 2003 16:45:32 GMT",
"version": "v1"
}
] | 2010-05-27 | [
[
"Evlampiev",
"K.",
""
],
[
"Yung",
"A.",
""
]
] | We study flux tubes on Higgs branches with curved geometry in supersymmetric gauge theories. As a first example we consider N=1 QED with one flavor of charges and with Higgs branch curved by adding a Fayet-Iliopoulos (FI) term. We show that in a generic vacuum on the Higgs branch flux tubes exist but become ``thick''. ... | 9.156834 | 9.025014 | 10.215968 | 9.055981 | 9.38931 | 9.333049 | 8.899464 | 8.709971 | 8.635953 | 9.968464 | 8.338543 | 8.720313 | 8.779457 | 8.903498 | 8.90501 | 8.928489 | 8.477622 | 8.829842 | 8.589955 | 9.096557 | 8.748954 |
2207.14167 | Patricio Salgado-Rebolledo | Andrea Campoleoni, Marc Henneaux, Simon Pekar, Alfredo P\'erez,
Patricio Salgado-Rebolledo | Magnetic Carrollian gravity from the Carroll algebra | 24 pages | null | 10.1007/JHEP09(2022)127 | null | hep-th gr-qc | http://creativecommons.org/publicdomain/zero/1.0/ | We explicitly establish the equivalence between the magnetic Carrollian limit
of Einstein gravity defined through the Hamiltonian formalism and the
Carrollian theory of gravity defined through a gauging of the Carroll algebra
along the lines of standard Poincar\'e (or (A)dS) gaugings.
| [
{
"created": "Thu, 28 Jul 2022 15:27:51 GMT",
"version": "v1"
}
] | 2022-09-28 | [
[
"Campoleoni",
"Andrea",
""
],
[
"Henneaux",
"Marc",
""
],
[
"Pekar",
"Simon",
""
],
[
"Pérez",
"Alfredo",
""
],
[
"Salgado-Rebolledo",
"Patricio",
""
]
] | We explicitly establish the equivalence between the magnetic Carrollian limit of Einstein gravity defined through the Hamiltonian formalism and the Carrollian theory of gravity defined through a gauging of the Carroll algebra along the lines of standard Poincar\'e (or (A)dS) gaugings. | 12.045833 | 10.028781 | 10.245199 | 8.561723 | 9.973531 | 9.059308 | 10.22193 | 9.426908 | 8.918976 | 18.230167 | 9.740643 | 9.535042 | 9.428966 | 9.224012 | 8.758974 | 9.333251 | 9.060414 | 9.298905 | 9.456954 | 10.226701 | 8.835833 |
2110.14481 | Giacomo Piccinini | Neil B. Copland, Giacomo Piccinini, Daniel C. Thompson | The Duality Symmetric String at Two-loops | 28 pages, 2 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The Tseytlin duality symmetric string makes manifest the $O(n,n)$ T-duality
symmetry on the worldsheet at the expense of manifest Lorentz invariance. Here
we consider the two-loop renormalisation of this model in the context of
"cosmological" spacetimes consisting of an internal $n$-dimensional torus
fibred over a on... | [
{
"created": "Wed, 27 Oct 2021 14:53:18 GMT",
"version": "v1"
}
] | 2021-10-28 | [
[
"Copland",
"Neil B.",
""
],
[
"Piccinini",
"Giacomo",
""
],
[
"Thompson",
"Daniel C.",
""
]
] | The Tseytlin duality symmetric string makes manifest the $O(n,n)$ T-duality symmetry on the worldsheet at the expense of manifest Lorentz invariance. Here we consider the two-loop renormalisation of this model in the context of "cosmological" spacetimes consisting of an internal $n$-dimensional torus fibred over a one-... | 9.513651 | 9.26553 | 11.753983 | 9.410228 | 9.52643 | 10.221435 | 9.482041 | 9.281926 | 8.730867 | 10.378395 | 8.976435 | 9.422684 | 10.45631 | 9.78682 | 9.762774 | 9.651321 | 9.39425 | 9.52634 | 9.913377 | 11.065959 | 9.270079 |
0807.1104 | Ben Freivogel | Ben Freivogel and Matthew Lippert | Evidence for a bound on the lifetime of de Sitter space | 28 pages | JHEP 0812:096,2008 | 10.1088/1126-6708/2008/12/096 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent work has suggested a surprising new upper bound on the lifetime of de
Sitter vacua in string theory. The bound is parametrically longer than the
Hubble time but parametrically shorter than the recurrence time. We investigate
whether the bound is satisfied in a particular class of de Sitter solutions,
the KKLT ... | [
{
"created": "Tue, 8 Jul 2008 16:10:19 GMT",
"version": "v1"
}
] | 2009-01-16 | [
[
"Freivogel",
"Ben",
""
],
[
"Lippert",
"Matthew",
""
]
] | Recent work has suggested a surprising new upper bound on the lifetime of de Sitter vacua in string theory. The bound is parametrically longer than the Hubble time but parametrically shorter than the recurrence time. We investigate whether the bound is satisfied in a particular class of de Sitter solutions, the KKLT va... | 6.740931 | 7.133436 | 6.792095 | 6.140173 | 6.385504 | 6.668351 | 5.701395 | 5.990194 | 6.074975 | 7.371306 | 6.432322 | 5.559398 | 6.384654 | 5.955487 | 5.944288 | 6.027134 | 5.956158 | 5.844515 | 6.019362 | 6.403222 | 6.249338 |
hep-th/0612235 | Olaf Hohm | Olaf Hohm | Massive Kaluza-Klein Theories and their Spontaneously Broken Symmetries | 112 pages, 3 figures, based on the author's Ph.D. thesis | null | null | null | hep-th | null | In this thesis we investigate the effective actions for massive Kaluza-Klein
states, focusing on the massive modes of spin-3/2 and spin-2 fields. To this
end we determine the spontaneously broken gauge symmetries associated to these
`higher spin' states and construct the unbroken phase of the Kaluza-Klein
theory. We ... | [
{
"created": "Thu, 21 Dec 2006 13:52:48 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Hohm",
"Olaf",
""
]
] | In this thesis we investigate the effective actions for massive Kaluza-Klein states, focusing on the massive modes of spin-3/2 and spin-2 fields. To this end we determine the spontaneously broken gauge symmetries associated to these `higher spin' states and construct the unbroken phase of the Kaluza-Klein theory. We sh... | 6.366577 | 6.558763 | 7.005413 | 6.372239 | 6.625149 | 6.680538 | 6.535981 | 6.248893 | 6.339447 | 7.299935 | 6.294333 | 6.241677 | 6.626297 | 6.290154 | 6.35846 | 6.376645 | 6.397728 | 6.219923 | 6.392388 | 6.512333 | 6.268855 |
0708.4116 | Jason Kumar | Jason Kumar | Dynamical SUSY Breaking in Intersecting Brane Models | 10 pages, LaTeX, References added | Phys.Rev.D77:046010,2008 | 10.1103/PhysRevD.77.046010 | null | hep-th hep-ph | null | We present a simple mechanism by which supersymmetry can be dynamically
broken in intersecting brane models, naturally generating an exponentially
small scale. Rather than utilize either non-Abelian gauge dynamics or
D-instantons, our mechanism uses worldsheet instantons to generate the small
scale in a hidden sector... | [
{
"created": "Thu, 30 Aug 2007 18:35:45 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Sep 2007 06:07:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Kumar",
"Jason",
""
]
] | We present a simple mechanism by which supersymmetry can be dynamically broken in intersecting brane models, naturally generating an exponentially small scale. Rather than utilize either non-Abelian gauge dynamics or D-instantons, our mechanism uses worldsheet instantons to generate the small scale in a hidden sector. | 10.037396 | 7.915267 | 8.73987 | 8.199263 | 8.134774 | 8.565482 | 8.346641 | 8.567798 | 7.800401 | 9.122557 | 8.900638 | 8.827842 | 9.282402 | 8.464419 | 8.823861 | 9.060896 | 8.858018 | 8.931569 | 8.657744 | 9.059356 | 8.943056 |
2109.06546 | Arkajyoti Manna | Sourav Ballav and Arkajyoti Manna | Recursion relations for scattering amplitudes with massive particles II:
massive vector bosons | Changes in the abstract, the presentation in the text and notation.
Matched with the published version | Nuclear Physics B, Volume 983,October 2022, 115935 | 10.1016/j.nuclphysb.2022.115935 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Using the recently introduced recursion relations with covariant
massive-massless shift, we study tree-level scattering amplitudes involving a
pair of massive vector bosons and an arbitrary number of gluons in the massive
spinor-helicity formalism. In particular, we derive compact expressions for
cases in which i) al... | [
{
"created": "Tue, 14 Sep 2021 09:38:57 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Nov 2021 12:44:44 GMT",
"version": "v2"
},
{
"created": "Wed, 16 Feb 2022 16:21:59 GMT",
"version": "v3"
},
{
"created": "Tue, 23 Aug 2022 17:05:20 GMT",
"version": "v4"
}
] | 2022-08-24 | [
[
"Ballav",
"Sourav",
""
],
[
"Manna",
"Arkajyoti",
""
]
] | Using the recently introduced recursion relations with covariant massive-massless shift, we study tree-level scattering amplitudes involving a pair of massive vector bosons and an arbitrary number of gluons in the massive spinor-helicity formalism. In particular, we derive compact expressions for cases in which i) all ... | 8.201059 | 7.403571 | 8.105112 | 6.925416 | 7.577215 | 7.588019 | 7.074925 | 6.689886 | 6.793014 | 8.313195 | 7.544411 | 7.263289 | 7.757257 | 7.117555 | 7.500374 | 7.44206 | 7.141953 | 7.49268 | 7.069 | 7.699107 | 7.267869 |
1501.02322 | Shan Hu | Shan Hu, Tianjun Li | Group manifold approach to higher spin theory | 35 pages,v2: revised version, v3: 38 pages, improved discussion on
global HS symmetry, clarifications added in appendix B, journal version | JHEP 1510 (2015) 019 | 10.1007/JHEP10(2015)019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the group manifold approach to higher spin theory. The deformed
local higher spin transformation is realized as the diffeomorphism
transformation in the group manifold $\textbf{M}$. With the suitable rheonomy
condition and the torsion constraint imposed, the unfolded equation can be
obtained from the Bian... | [
{
"created": "Sat, 10 Jan 2015 09:14:08 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Feb 2015 14:02:11 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Sep 2015 03:06:36 GMT",
"version": "v3"
}
] | 2015-10-15 | [
[
"Hu",
"Shan",
""
],
[
"Li",
"Tianjun",
""
]
] | We consider the group manifold approach to higher spin theory. The deformed local higher spin transformation is realized as the diffeomorphism transformation in the group manifold $\textbf{M}$. With the suitable rheonomy condition and the torsion constraint imposed, the unfolded equation can be obtained from the Bianch... | 9.316271 | 9.628336 | 9.171322 | 8.797493 | 9.826434 | 9.718756 | 9.319444 | 9.341248 | 9.015401 | 10.927444 | 9.402142 | 9.241735 | 9.120891 | 8.932197 | 8.993038 | 9.032952 | 8.839577 | 9.024014 | 8.949545 | 9.075908 | 8.845546 |
1009.5553 | Futoshi Yagi | Kazunobu Maruyoshi, Futoshi Yagi | Seiberg-Witten curve via generalized matrix model | 22 pages, 3 figures; v2: references added, typos corrected; v3: minor
corrections, references added | JHEP 1101:042,2011 | 10.1007/JHEP01(2011)042 | YITP-10-84, IHES/P/10/34 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the generalized matrix model which corresponds to the n-point toric
Virasoro conformal block. This describes four-dimensional N=2 SU(2)^n gauge
theory with circular quiver diagram by the AGT relation. We first verify that
it is obtained from the perturbative calculation of the Liouville correlation
function.... | [
{
"created": "Tue, 28 Sep 2010 12:54:23 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Oct 2010 13:32:43 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Dec 2010 20:48:37 GMT",
"version": "v3"
}
] | 2011-01-17 | [
[
"Maruyoshi",
"Kazunobu",
""
],
[
"Yagi",
"Futoshi",
""
]
] | We study the generalized matrix model which corresponds to the n-point toric Virasoro conformal block. This describes four-dimensional N=2 SU(2)^n gauge theory with circular quiver diagram by the AGT relation. We first verify that it is obtained from the perturbative calculation of the Liouville correlation function. W... | 7.676838 | 6.93017 | 10.287917 | 6.874094 | 6.476143 | 6.364883 | 6.147826 | 6.641893 | 6.527962 | 9.96203 | 6.461025 | 7.028212 | 8.609682 | 7.135452 | 6.903769 | 7.278852 | 6.998529 | 7.138635 | 7.605802 | 8.525512 | 6.963742 |
2407.10203 | Raphael Dulac | Iosif Bena and Rapha\"el Dulac | On the supersymmetries of branes with fluxes | 14 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Dirac-Born-Infled action that describes the dynamics of D branes also
allows one to compute the supersymmetries they preserve using the
Kappa-symmetry projector. The ''Lagrangian'' expression of this projector
depends on the velocity and electric fields of the branes, but not on the
corresponding conserved charge... | [
{
"created": "Sun, 14 Jul 2024 13:47:53 GMT",
"version": "v1"
}
] | 2024-07-16 | [
[
"Bena",
"Iosif",
""
],
[
"Dulac",
"Raphaël",
""
]
] | The Dirac-Born-Infled action that describes the dynamics of D branes also allows one to compute the supersymmetries they preserve using the Kappa-symmetry projector. The ''Lagrangian'' expression of this projector depends on the velocity and electric fields of the branes, but not on the corresponding conserved charges.... | 13.173877 | 14.435492 | 14.899538 | 13.405435 | 14.461111 | 14.930347 | 12.761116 | 12.597872 | 13.537844 | 14.890306 | 12.990702 | 12.528153 | 12.92891 | 12.004341 | 12.96703 | 12.816374 | 12.882181 | 12.25361 | 12.917705 | 12.991198 | 12.469634 |
1802.04445 | Yifan Wang | Chi-Ming Chang, Ying-Hsuan Lin, Shu-Heng Shao, Yifan Wang, Xi Yin | Topological Defect Lines and Renormalization Group Flows in Two
Dimensions | 101 pages, 63 figures, 2 tables; v3: minor changes, added footnotes
and references, published version | null | 10.1007/JHEP01(2019)026 | CALT-TH 2017-067, PUPT-2546 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider topological defect lines (TDLs) in two-dimensional conformal
field theories. Generalizing and encompassing both global symmetries and
Verlinde lines, TDLs together with their attached defect operators provide
models of fusion categories without braiding. We study the crossing relations
of TDLs, discuss th... | [
{
"created": "Tue, 13 Feb 2018 02:51:54 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Apr 2018 22:33:35 GMT",
"version": "v2"
},
{
"created": "Sat, 12 Jan 2019 09:42:13 GMT",
"version": "v3"
}
] | 2019-01-30 | [
[
"Chang",
"Chi-Ming",
""
],
[
"Lin",
"Ying-Hsuan",
""
],
[
"Shao",
"Shu-Heng",
""
],
[
"Wang",
"Yifan",
""
],
[
"Yin",
"Xi",
""
]
] | We consider topological defect lines (TDLs) in two-dimensional conformal field theories. Generalizing and encompassing both global symmetries and Verlinde lines, TDLs together with their attached defect operators provide models of fusion categories without braiding. We study the crossing relations of TDLs, discuss thei... | 8.529997 | 7.545872 | 10.908188 | 7.621496 | 7.314503 | 7.735709 | 7.654853 | 7.822505 | 7.431801 | 11.657824 | 7.549321 | 7.772623 | 9.642123 | 8.335484 | 8.023561 | 8.254513 | 8.211305 | 8.102571 | 8.383356 | 9.329472 | 7.958323 |
1805.07377 | Ahmad Sheykhi | Mahya Mohammadi, Ahmad Sheykhi and Mahdi Kord Zangeneh | Analytical and numerical study of backreacting one-dimensional
holographic superconductors in the presence of Born-Infeld electrodynamics | 7 pages, two columns | Eur. Phys. J. C (2018) 78:654 | 10.1140/epjc/s10052-018-6138-9 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We analytically as well as numerically study the effects of Born-Infeld
nonlinear electrodynamics on the properties of $(1+1)$-dimensional s-wave
holographic superconductors. We relax the probe limit and further assume the
scalar and gauge fields affect on the background spacetime. We thus explore the
effects of back... | [
{
"created": "Sun, 6 May 2018 19:27:54 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Jun 2018 16:28:23 GMT",
"version": "v2"
}
] | 2018-09-26 | [
[
"Mohammadi",
"Mahya",
""
],
[
"Sheykhi",
"Ahmad",
""
],
[
"Zangeneh",
"Mahdi Kord",
""
]
] | We analytically as well as numerically study the effects of Born-Infeld nonlinear electrodynamics on the properties of $(1+1)$-dimensional s-wave holographic superconductors. We relax the probe limit and further assume the scalar and gauge fields affect on the background spacetime. We thus explore the effects of backre... | 7.113913 | 6.016955 | 6.859574 | 5.797943 | 5.989241 | 5.92233 | 5.884205 | 5.335731 | 5.884953 | 6.602305 | 5.907507 | 6.399696 | 6.933621 | 6.638974 | 6.779761 | 6.478506 | 6.508595 | 6.6041 | 6.647239 | 6.9635 | 6.530004 |
1206.0175 | Stefano Bellucci | S. Bellucci, N. Kozyrev, S. Krivonos and A. Sutulin | Symmetries of N=4 supersymmetric CP(n) mechanics | 10 pages, PACS numbers: 11.30.Pb, 03.65.-w; minor changes in
Introduction, references added | null | 10.1088/1751-8113/46/27/275305 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly constructed the generators of $SU(n+1)$ group which commute
with the supercharges of N=4 supersymmetric $\mathbb{CP}^n$ mechanics in the
background U(n) gauge fields. The corresponding Hamiltonian can be represented
as a direct sum of two Casimir operators: one Casimir operator on $SU(n+1)$
group contai... | [
{
"created": "Fri, 1 Jun 2012 13:22:18 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Jan 2013 14:14:35 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Bellucci",
"S.",
""
],
[
"Kozyrev",
"N.",
""
],
[
"Krivonos",
"S.",
""
],
[
"Sutulin",
"A.",
""
]
] | We explicitly constructed the generators of $SU(n+1)$ group which commute with the supercharges of N=4 supersymmetric $\mathbb{CP}^n$ mechanics in the background U(n) gauge fields. The corresponding Hamiltonian can be represented as a direct sum of two Casimir operators: one Casimir operator on $SU(n+1)$ group contains... | 8.961603 | 9.55698 | 9.825356 | 8.511984 | 10.017683 | 9.578611 | 10.0818 | 9.127856 | 8.925752 | 10.557941 | 8.331889 | 8.687243 | 8.7509 | 8.957036 | 9.492015 | 8.753045 | 8.687167 | 8.741018 | 8.696688 | 9.564484 | 8.500776 |
hep-th/9803062 | Kwei-Chou Yang | A. N. Mitra | 3D-4D Interlinkage Of qqq Wave Functions Under 3D Support For Pairwise
Bethe-Salpeter Kernels | 20 pages, Latex, submitted via the account of K.-C. Yang | null | 10.1142/S0217751X99002256 | null | hep-th | null | Using the method of Green's functions within a Bethe-Salpeter framework
characterized by a pairwise qq interaction with a Lorentz-covariant 3D support
to its kernel, the 4D BS wave function for a system of 3 identical relativistic
spinless quarks is reconstructed from the corresponding 3D form which satisfies
a fully... | [
{
"created": "Sat, 7 Mar 1998 07:51:01 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Mitra",
"A. N.",
""
]
] | Using the method of Green's functions within a Bethe-Salpeter framework characterized by a pairwise qq interaction with a Lorentz-covariant 3D support to its kernel, the 4D BS wave function for a system of 3 identical relativistic spinless quarks is reconstructed from the corresponding 3D form which satisfies a fully c... | 16.720083 | 14.714887 | 17.098801 | 14.509398 | 16.588408 | 15.702085 | 15.097963 | 14.815518 | 14.922756 | 17.735189 | 16.032568 | 15.893056 | 16.718369 | 16.009872 | 15.547626 | 15.837557 | 15.69116 | 15.890618 | 15.705687 | 16.834082 | 15.884978 |
hep-th/9905083 | Robert Marnelius | Igor Batalin, Robert Marnelius | General quantum antibrackets | 21 pages,Latexfile | Theor.Math.Phys. 120 (1999) 1115-1132; Teor.Mat.Fiz. 120 (1999)
358-379 | 10.1007/BF02557237 | ITP-Goteborg 99-04 | hep-th | null | The recently introduced quantum antibracket is further generalized allowing
for the defining odd operator Q to be arbitrary. We give exact formulas for
higher quantum antibrackets of arbitrary orders and their generalized Jacobi
identities. Their applications to BV-quantization and BFV-BRST quantization are
then revi... | [
{
"created": "Wed, 12 May 1999 12:47:30 GMT",
"version": "v1"
}
] | 2019-08-17 | [
[
"Batalin",
"Igor",
""
],
[
"Marnelius",
"Robert",
""
]
] | The recently introduced quantum antibracket is further generalized allowing for the defining odd operator Q to be arbitrary. We give exact formulas for higher quantum antibrackets of arbitrary orders and their generalized Jacobi identities. Their applications to BV-quantization and BFV-BRST quantization are then review... | 19.395243 | 15.379032 | 21.141573 | 15.66233 | 13.796409 | 15.51177 | 15.058606 | 13.734504 | 15.637781 | 20.493359 | 16.33374 | 16.77247 | 18.534363 | 16.138275 | 16.598389 | 16.481403 | 15.918498 | 16.346155 | 17.256742 | 18.719328 | 16.136105 |
1805.07904 | Jian-Pin Wu | Xiao-Mei Kuang, Jian-Pin Wu and Zhenhua Zhou | Holographic transports from Born-Infeld electrodynamics with momentum
dissipation | 21 pages,8 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the Einstein-axions AdS black hole from Born-Infeld
electrodynamics. Various DC transport coefficients of the dual boundary theory
are computed. The DC electric conductivity depends on the temperature, which is
a novel property comparing to that in RN-AdS black hole. The DC electric
conductivity are posi... | [
{
"created": "Mon, 21 May 2018 06:12:34 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jun 2018 23:29:23 GMT",
"version": "v2"
}
] | 2018-06-19 | [
[
"Kuang",
"Xiao-Mei",
""
],
[
"Wu",
"Jian-Pin",
""
],
[
"Zhou",
"Zhenhua",
""
]
] | We construct the Einstein-axions AdS black hole from Born-Infeld electrodynamics. Various DC transport coefficients of the dual boundary theory are computed. The DC electric conductivity depends on the temperature, which is a novel property comparing to that in RN-AdS black hole. The DC electric conductivity are positi... | 9.823534 | 9.566126 | 9.80837 | 9.136315 | 9.798181 | 9.103611 | 9.644062 | 9.460788 | 9.393269 | 11.302272 | 9.178468 | 9.544142 | 9.732198 | 9.46241 | 9.692723 | 9.641037 | 9.483638 | 9.196998 | 9.548676 | 10.089082 | 9.205576 |
hep-th/0512210 | Yidun Wan | Yidun Wan | 2D Ising Model with non-local links - a study of non-locality | 4 pages (2 columns), 6 figures | null | null | null | hep-th cond-mat.stat-mech | null | Markopoulou and Smolin have argued that the low energy limit of LQG may
suffer from a conflict between locality, as defined by the connectivity of spin
networks, and an averaged notion of locality that emerges at low energy from a
superposition of spin network states. This raises the issue of how much
non-locality, r... | [
{
"created": "Fri, 16 Dec 2005 20:43:15 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Jan 2006 03:27:25 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Wan",
"Yidun",
""
]
] | Markopoulou and Smolin have argued that the low energy limit of LQG may suffer from a conflict between locality, as defined by the connectivity of spin networks, and an averaged notion of locality that emerges at low energy from a superposition of spin network states. This raises the issue of how much non-locality, rel... | 9.082018 | 9.859304 | 9.460348 | 9.003877 | 9.427237 | 9.651922 | 9.929831 | 9.199245 | 9.801415 | 9.312185 | 9.341763 | 8.80942 | 9.034718 | 8.943074 | 8.778389 | 8.912608 | 8.955624 | 8.671618 | 8.942461 | 8.803308 | 9.286725 |
2212.11811 | Harold Erbin | Harold Erbin, Vincent Lahoche, Dine Ousmane Samary | Renormalization in the neural network-quantum field theory
correspondence | A shorter version of this paper has been accepted in the NeurIPS 2022
workshop: Machine learning and the physical sciences
(https://ml4physicalsciences.github.io/2022/) | null | null | null | hep-th cond-mat.dis-nn cs.LG stat.ML | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A statistical ensemble of neural networks can be described in terms of a
quantum field theory (NN-QFT correspondence). The infinite-width limit is
mapped to a free field theory, while finite N corrections are mapped to
interactions. After reviewing the correspondence, we will describe how to
implement renormalization... | [
{
"created": "Thu, 22 Dec 2022 15:41:13 GMT",
"version": "v1"
}
] | 2022-12-23 | [
[
"Erbin",
"Harold",
""
],
[
"Lahoche",
"Vincent",
""
],
[
"Samary",
"Dine Ousmane",
""
]
] | A statistical ensemble of neural networks can be described in terms of a quantum field theory (NN-QFT correspondence). The infinite-width limit is mapped to a free field theory, while finite N corrections are mapped to interactions. After reviewing the correspondence, we will describe how to implement renormalization i... | 14.995485 | 13.173749 | 14.103444 | 11.676577 | 12.604629 | 12.899268 | 13.421002 | 11.938275 | 13.584188 | 15.123272 | 12.185288 | 12.352133 | 14.643107 | 12.816264 | 13.392925 | 12.467494 | 13.000777 | 12.954309 | 13.003995 | 14.4615 | 13.089312 |
hep-th/0310116 | Lutz Moeller | Marija Dimitrijevic, Frank Meyer, Lutz M\"oller, Julius Wess | Gauge theories on the kappa-Minkowski spacetime | 17 pages, few minor revisions | Eur.Phys.J. C36 (2004) 117-126 | 10.1140/epjc/s2004-01887-0 | null | hep-th | null | This study of gauge field theories on kappa-deformed Minkowski spacetime
extends previous work on field theories on this example of a noncommutative
spacetime. We construct deformed gauge theories for arbitrary compact Lie
groups using the concept of enveloping algebra-valued gauge transformations and
the Seiberg-Wit... | [
{
"created": "Mon, 13 Oct 2003 16:07:42 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Aug 2004 12:30:49 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Dimitrijevic",
"Marija",
""
],
[
"Meyer",
"Frank",
""
],
[
"Möller",
"Lutz",
""
],
[
"Wess",
"Julius",
""
]
] | This study of gauge field theories on kappa-deformed Minkowski spacetime extends previous work on field theories on this example of a noncommutative spacetime. We construct deformed gauge theories for arbitrary compact Lie groups using the concept of enveloping algebra-valued gauge transformations and the Seiberg-Witte... | 7.875906 | 8.144029 | 8.729636 | 7.750665 | 8.415319 | 8.130719 | 8.383378 | 8.095645 | 7.724915 | 9.256849 | 7.408538 | 7.66836 | 8.040348 | 7.846385 | 8.048809 | 8.050851 | 7.766334 | 7.788697 | 7.95097 | 8.252021 | 7.717802 |
2007.08227 | Yan-Gang Miao | Yang Guo, Yan-Gang Miao | Null geodesics, quasinormal modes and the correspondence with shadows in
high-dimensional Einstein-Yang-Mills spacetimes | v1: 10 pages, 6 figures; v2: clarifications added and references
adjusted; v3: 14 pages, clarifications, 6 tables and one reference added,
final version to appear in Physical Review D | Phys. Rev. D 102, 084057 (2020) | 10.1103/PhysRevD.102.084057 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Null geodesics, quasinormal modes of a massless scalar field perturbation and
the correspondence with shadow radii are investigated in the background
spacetime of high-dimensional Einstein-Yang-Mills black holes. Based on the
properties of null geodesics, we obtain the connection between the radius of a
photon sphere... | [
{
"created": "Thu, 16 Jul 2020 09:52:03 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Jul 2020 08:43:54 GMT",
"version": "v2"
},
{
"created": "Sat, 3 Oct 2020 01:33:50 GMT",
"version": "v3"
}
] | 2020-10-27 | [
[
"Guo",
"Yang",
""
],
[
"Miao",
"Yan-Gang",
""
]
] | Null geodesics, quasinormal modes of a massless scalar field perturbation and the correspondence with shadow radii are investigated in the background spacetime of high-dimensional Einstein-Yang-Mills black holes. Based on the properties of null geodesics, we obtain the connection between the radius of a photon sphere a... | 7.049499 | 7.326226 | 6.006515 | 5.989207 | 6.571394 | 6.543861 | 6.496818 | 5.937149 | 6.831028 | 6.516343 | 6.615556 | 6.832739 | 6.317238 | 6.441111 | 6.401643 | 6.404619 | 7.05358 | 6.273666 | 6.649972 | 6.494719 | 6.559616 |
hep-th/0611013 | Martin Wolf | Martin Wolf | On supertwistor geometry and integrability in super gauge theory | Ph.D. thesis | null | null | null | hep-th math-ph math.MP | null | In this thesis, we report on different aspects of integrability in
supersymmetric gauge theories. The main tool of investigation is twistor
geometry. In trying to be self-contained, we first present a brief review about
the basics of twistor geometry. We then focus on the twistor description of
various gauge theories... | [
{
"created": "Wed, 1 Nov 2006 14:51:13 GMT",
"version": "v1"
}
] | 2007-06-14 | [
[
"Wolf",
"Martin",
""
]
] | In this thesis, we report on different aspects of integrability in supersymmetric gauge theories. The main tool of investigation is twistor geometry. In trying to be self-contained, we first present a brief review about the basics of twistor geometry. We then focus on the twistor description of various gauge theories i... | 7.760976 | 7.694818 | 8.524386 | 7.624144 | 7.769553 | 7.656213 | 7.648357 | 7.461197 | 7.486495 | 8.958099 | 7.369214 | 7.768414 | 7.670998 | 7.642305 | 7.724164 | 7.775793 | 7.713377 | 7.545293 | 7.53101 | 7.892664 | 7.499645 |
hep-th/9507121 | Edward Witten | Edward Witten | Some Comments On String Dynamics | 26 pages | null | null | IASSNS-HEP-95-63 | hep-th | null | Three subjects are considered here: a self-dual non-critical string that
appears in Type IIB superstring theory at points in ${\rm K3}$ moduli space
where the Type IIA theory has extended gauge symmetry; a conformal field theory
singularity at such points which may signal quantum effects that persist even
at weak cou... | [
{
"created": "Sun, 23 Jul 1995 14:01:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Witten",
"Edward",
""
]
] | Three subjects are considered here: a self-dual non-critical string that appears in Type IIB superstring theory at points in ${\rm K3}$ moduli space where the Type IIA theory has extended gauge symmetry; a conformal field theory singularity at such points which may signal quantum effects that persist even at weak coupl... | 15.408512 | 15.520629 | 18.346558 | 15.401556 | 15.931826 | 16.427208 | 17.054922 | 16.258921 | 15.037066 | 18.756758 | 15.68408 | 14.691831 | 15.280773 | 14.436214 | 14.451184 | 15.339016 | 14.603755 | 14.81904 | 14.565384 | 15.489954 | 15.119501 |
hep-th/0008150 | Eric R. Sharpe | Tomas Gomez, Eric R. Sharpe | D-Branes and Scheme Theory | 10 pages, LaTeX | null | null | DUKE-CGTP-2000-12 | hep-th | null | In this highly speculative note we conjecture that it may be possible to
understand features of coincident D-branes, such as the appearance of enhanced
non-abelian gauge symmetry, in a purely geometric fashion, using a form of
geometry known as scheme theory. We give a very brief introduction to some
relevant ideas f... | [
{
"created": "Fri, 18 Aug 2000 17:24:45 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Aug 2000 19:15:17 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Gomez",
"Tomas",
""
],
[
"Sharpe",
"Eric R.",
""
]
] | In this highly speculative note we conjecture that it may be possible to understand features of coincident D-branes, such as the appearance of enhanced non-abelian gauge symmetry, in a purely geometric fashion, using a form of geometry known as scheme theory. We give a very brief introduction to some relevant ideas fro... | 11.538008 | 9.72549 | 10.65418 | 9.328383 | 9.003566 | 9.998589 | 8.982208 | 8.94815 | 9.263055 | 9.980319 | 9.021824 | 8.781619 | 10.170926 | 9.259024 | 9.204908 | 8.937528 | 8.920547 | 9.122698 | 9.344705 | 9.954739 | 9.356554 |
hep-th/0005259 | Paul Wiegmann | I.K.Kostov, I.Krichever, M.Mineev-Weinstein, P.Wiegmann, A.Zabrodin | $\tau$-function for analytic curves | 13 pages, no figures, prepared for Proccedings of MSRI Workshop
``Matrix Models and Painlev\'e Equations'', Berkeley (USA) 1999 | Random matrices and their applications, MSRI publications,vol.40,
285,2001, Cambridge University Press | null | null | hep-th | null | We review the concept of $\tau$-function for simple analytic curves. The
$\tau$-function gives a formal solution to the 2D inverse potential problem and
appears as the $\tau$-function of the integrable hierarchy which describes
conformal maps of simply-connected domains bounded by analytic curves to the
unit disk. Th... | [
{
"created": "Fri, 26 May 2000 21:25:23 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kostov",
"I. K.",
""
],
[
"Krichever",
"I.",
""
],
[
"Mineev-Weinstein",
"M.",
""
],
[
"Wiegmann",
"P.",
""
],
[
"Zabrodin",
"A.",
""
]
] | We review the concept of $\tau$-function for simple analytic curves. The $\tau$-function gives a formal solution to the 2D inverse potential problem and appears as the $\tau$-function of the integrable hierarchy which describes conformal maps of simply-connected domains bounded by analytic curves to the unit disk. The ... | 9.788778 | 9.491989 | 11.463204 | 9.077634 | 10.094707 | 9.23645 | 9.527459 | 8.838186 | 9.804949 | 11.812488 | 9.11658 | 8.888864 | 9.341176 | 8.842464 | 8.951506 | 8.975773 | 8.445415 | 8.658487 | 8.868629 | 9.029398 | 8.461821 |
hep-th/9705013 | Igor V. Volovich | I.V.Volovich | Planckian Energy Scattering of D-branes and M(atrix) Theory in Curved
Space | 5 pages, Latex | null | 10.1007/BFb0105235 | SMI-12-97/5 | hep-th gr-qc | null | We argue that black p-branes will occur in the collision of D0-branes at
Planckian energies. This extents the Amati, Ciafaloni and Veneziano and 't
Hooft conjecture that black holes occur in the collision of two light particles
at Planckian energies. We discuss a possible scenario for such a process by
using collidin... | [
{
"created": "Sun, 4 May 1997 13:55:40 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Volovich",
"I. V.",
""
]
] | We argue that black p-branes will occur in the collision of D0-branes at Planckian energies. This extents the Amati, Ciafaloni and Veneziano and 't Hooft conjecture that black holes occur in the collision of two light particles at Planckian energies. We discuss a possible scenario for such a process by using colliding ... | 11.263952 | 10.103985 | 11.799931 | 9.550467 | 9.014718 | 10.285059 | 9.249587 | 9.453291 | 9.544399 | 11.474916 | 9.836483 | 10.215576 | 10.768984 | 10.036717 | 10.105536 | 9.935029 | 10.253507 | 10.806085 | 9.942078 | 11.012909 | 9.826151 |
hep-th/0001130 | Oren Bergman | O. Bergman (Caltech), M.R. Gaberdiel (Cambridge) | On the Consistency of Orbifolds | 10 pages, LaTex. The sign ambiguities in the GSO-projection are
clarified in the abstract and the introduction, and revised in sections 3 and
4. In particular we clarify that modular invariance fixes all the ambiguities
in principle, but in practice this is hard to do. The final conclusion
regarding the spectru... | Phys.Lett. B481 (2000) 379-385 | 10.1016/S0370-2693(00)00446-9 | CALT-68-2256, CITUSC/00-002, DAMTP-2000-4 | hep-th | null | Modular invariance is a necessary condition for the consistency of any closed
string theory. In particular, it imposes stringent constraints on the spectrum
of orbifold theories, and in principle determines their spectrum uniquely up to
discrete torsion classes. In practice, however, there are often ambiguities in
th... | [
{
"created": "Thu, 20 Jan 2000 18:56:21 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Mar 2000 23:54:48 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Bergman",
"O.",
"",
"Caltech"
],
[
"Gaberdiel",
"M. R.",
"",
"Cambridge"
]
] | Modular invariance is a necessary condition for the consistency of any closed string theory. In particular, it imposes stringent constraints on the spectrum of orbifold theories, and in principle determines their spectrum uniquely up to discrete torsion classes. In practice, however, there are often ambiguities in the ... | 5.691211 | 5.214666 | 6.044888 | 5.159568 | 5.618846 | 5.43251 | 5.659802 | 5.666067 | 5.27611 | 5.687928 | 5.308061 | 5.239166 | 5.549037 | 5.285835 | 5.175671 | 5.244293 | 5.383254 | 5.329686 | 5.25959 | 5.36753 | 5.116316 |
1411.1320 | Pierre Martinetti | Agostino Devastato and Pierre Martinetti | Twisted spectral triple for the Standard Model and spontaneous breaking
of the Grand Symmetry | References updated, misprint corrected. One paragraph added at the
end of the paper to discuss results in the literature since the first version
of the paper. 39 pages in Mathematical Physics, Analysis and Geometry (2016) | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Grand symmetry models in noncommutative geometry have been introduced to
explain how to generate minimally (i.e. without adding new fermions) an extra
scalar field beyond the standard model, which both stabilizes the electroweak
vacuum and makes the computation of the mass of the Higgs compatible with its
experimenta... | [
{
"created": "Wed, 5 Nov 2014 16:52:58 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Jan 2015 00:38:03 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Dec 2016 16:31:18 GMT",
"version": "v3"
}
] | 2016-12-19 | [
[
"Devastato",
"Agostino",
""
],
[
"Martinetti",
"Pierre",
""
]
] | Grand symmetry models in noncommutative geometry have been introduced to explain how to generate minimally (i.e. without adding new fermions) an extra scalar field beyond the standard model, which both stabilizes the electroweak vacuum and makes the computation of the mass of the Higgs compatible with its experimental ... | 11.318241 | 11.545029 | 11.488691 | 10.501899 | 10.59165 | 10.797954 | 11.009633 | 10.569031 | 10.735079 | 13.023232 | 9.885455 | 10.940618 | 11.087274 | 10.883556 | 10.925034 | 10.643752 | 10.584003 | 10.808767 | 10.808453 | 11.363287 | 10.392689 |
0708.1016 | Derrick Kiley | Derrick Kiley | Rotating Black Holes on Codimension-2 Branes | 7 pages, uses revtex | Phys.Rev.D76:126002,2007 | 10.1103/PhysRevD.76.126002 | null | hep-th astro-ph gr-qc hep-ph | null | It has recently been demonstrated that certain types of non-tensional
stress-energy can live on tensional codimension-2 branes, including
gravitational shockwaves and small Schwarzschild black holes. In this note we
generalize the earlier Schwarzschild results, and construct the exact
gravitational fields of small ro... | [
{
"created": "Tue, 7 Aug 2007 23:23:50 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kiley",
"Derrick",
""
]
] | It has recently been demonstrated that certain types of non-tensional stress-energy can live on tensional codimension-2 branes, including gravitational shockwaves and small Schwarzschild black holes. In this note we generalize the earlier Schwarzschild results, and construct the exact gravitational fields of small rota... | 9.670445 | 10.500341 | 9.701939 | 9.27676 | 9.669621 | 9.826812 | 10.108543 | 9.190827 | 10.069146 | 10.99055 | 8.947996 | 8.803731 | 9.1493 | 9.050267 | 9.184523 | 9.392317 | 9.329705 | 8.916822 | 9.091151 | 9.380758 | 9.113746 |
hep-th/9401161 | null | Joaquim Gomis and Jordi Par\'is | Anomalies and Wess-Zumino Terms in an Extended, Regularized
Field-Antifield Formalism | 30 pages, Latex file, KUL-TF-93/50, UB-ECM-PF 93/14, UTTG-16-93.
(shortened version, to appear in Nucl. Phys. B) | Nucl.Phys. B431 (1994) 378-412 | 10.1016/0550-3213(94)90110-4 | null | hep-th | null | Quantization of anomalous gauge theories with closed, irreducible gauge
algebra within the extended Field-Antifield formalism is further pursued. Using
a Pauli-Villars (PV) regularization of the generating functional at one loop
level, an alternative form for the anomaly is found which involves only the
regulator. Th... | [
{
"created": "Mon, 31 Jan 1994 10:39:01 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Sep 1994 15:12:07 GMT",
"version": "v2"
}
] | 2016-08-14 | [
[
"Gomis",
"Joaquim",
""
],
[
"París",
"Jordi",
""
]
] | Quantization of anomalous gauge theories with closed, irreducible gauge algebra within the extended Field-Antifield formalism is further pursued. Using a Pauli-Villars (PV) regularization of the generating functional at one loop level, an alternative form for the anomaly is found which involves only the regulator. The ... | 14.501495 | 11.95944 | 14.52869 | 11.826695 | 12.807171 | 11.593878 | 12.618291 | 12.175212 | 12.046365 | 15.507536 | 11.956629 | 12.790732 | 13.177835 | 12.513907 | 12.383142 | 12.329268 | 12.418606 | 12.518447 | 12.512443 | 13.013719 | 12.477764 |
1710.06439 | Alexander Tyukov | Alexander Tyukov and Nicholas P. Warner | BPS equations and Non-trivial Compactifications | 32 pages, no figures | null | 10.1007/JHEP05(2018)022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the problem of finding exact, eleven-dimensional, BPS
supergravity solutions in which the compactification involves a non-trivial
Calabi-Yau manifold, ${\cal Y}$, as opposed to simply a $T^6$. Since there are
no explicitly-known metrics on non-trivial, compact Calabi-Yau manifolds, we
use a non-compact "l... | [
{
"created": "Tue, 17 Oct 2017 18:00:07 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Nov 2017 20:48:11 GMT",
"version": "v2"
}
] | 2018-05-23 | [
[
"Tyukov",
"Alexander",
""
],
[
"Warner",
"Nicholas P.",
""
]
] | We consider the problem of finding exact, eleven-dimensional, BPS supergravity solutions in which the compactification involves a non-trivial Calabi-Yau manifold, ${\cal Y}$, as opposed to simply a $T^6$. Since there are no explicitly-known metrics on non-trivial, compact Calabi-Yau manifolds, we use a non-compact "loc... | 8.04731 | 8.963506 | 8.917515 | 8.077205 | 8.569114 | 8.41277 | 8.339821 | 8.212812 | 8.217301 | 9.125177 | 8.127851 | 8.037975 | 8.038449 | 7.905725 | 7.890141 | 7.894209 | 8.022443 | 7.716826 | 7.860857 | 8.194408 | 7.877658 |
1207.6948 | Badr Mohammed Mr | Badr Awad Elseid Mohammed | Nonplanar Integrability and Parity in ABJ Theory | 1+12 pages, Corrected typos, more clarifications, figure and appendix
added | IJMPA Vol. 28 (2013) 1350043 | 10.1142/S0217751X13500437 | WITS-CTP-101 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we study the action of the non-planar two-loop dilatation
operator in an SU(2)*SU(2) sub-sector of the ABJ Chern-Simons-matter theory.
The gauge invariant operators we consider are the restricted Schur polynomials.
As in ABJM theory, there is a limit in which the spectrum reduces to a set of
decoupled... | [
{
"created": "Mon, 30 Jul 2012 14:38:19 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Aug 2012 10:13:01 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Oct 2012 14:02:24 GMT",
"version": "v3"
},
{
"created": "Wed, 31 Oct 2012 11:57:50 GMT",
"version": "v4"
}
] | 2013-04-16 | [
[
"Mohammed",
"Badr Awad Elseid",
""
]
] | In this article we study the action of the non-planar two-loop dilatation operator in an SU(2)*SU(2) sub-sector of the ABJ Chern-Simons-matter theory. The gauge invariant operators we consider are the restricted Schur polynomials. As in ABJM theory, there is a limit in which the spectrum reduces to a set of decoupled h... | 9.089387 | 8.071654 | 10.7551 | 7.998312 | 9.356721 | 8.772597 | 8.252715 | 8.173049 | 8.163615 | 11.709599 | 7.74609 | 8.408026 | 8.94249 | 8.498712 | 8.348402 | 8.549824 | 8.382255 | 8.60574 | 8.162119 | 9.686123 | 8.575723 |
1506.05784 | Konstantinos Siampos | Konstantinos Sfetsos, Konstantinos Siampos, Daniel C. Thompson | Generalised integrable $\lambda$- and $\eta$-deformations and their
relation | 33 pages, Latex, v2: 35 pages, Latex, clarifying comments, v3: few
minor changes, NPB version | null | 10.1016/j.nuclphysb.2015.08.015 | null | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct two-parameter families of integrable $\lambda$-deformations of
two-dimensional field theories. These interpolate between a CFT (a WZW/gauged
WZW model) and the non-Abelian T-dual of a principal chiral model on a
group/symmetric coset space. In examples based on the $SU(2)$ WZW model and the
$SU(2)/U(1)$ ... | [
{
"created": "Thu, 18 Jun 2015 19:38:13 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Jun 2015 19:42:19 GMT",
"version": "v2"
},
{
"created": "Mon, 31 Aug 2015 08:50:57 GMT",
"version": "v3"
}
] | 2015-09-01 | [
[
"Sfetsos",
"Konstantinos",
""
],
[
"Siampos",
"Konstantinos",
""
],
[
"Thompson",
"Daniel C.",
""
]
] | We construct two-parameter families of integrable $\lambda$-deformations of two-dimensional field theories. These interpolate between a CFT (a WZW/gauged WZW model) and the non-Abelian T-dual of a principal chiral model on a group/symmetric coset space. In examples based on the $SU(2)$ WZW model and the $SU(2)/U(1)$ ex... | 6.661178 | 6.326826 | 8.934361 | 6.166132 | 6.316309 | 5.947326 | 6.411467 | 6.162491 | 5.982852 | 9.472938 | 6.589798 | 6.600436 | 7.429558 | 6.434378 | 6.459015 | 6.43289 | 6.245738 | 6.430341 | 6.575509 | 7.255 | 6.363508 |
1307.3517 | Joanna L. Karczmarek | Joanna L. Karczmarek and Charles Rabideau | Holographic entanglement entropy in nonlocal theories | 26 pages, 9 figures | null | 10.1007/JHEP10(2013)078 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute holographic entanglement entropy in two strongly coupled nonlocal
field theories: the dipole and the noncommutative deformations of SYM theory.
We find that entanglement entropy in the dipole theory follows a volume law for
regions smaller than the length scale of nonlocality and has a smooth
cross-over to... | [
{
"created": "Fri, 12 Jul 2013 17:21:26 GMT",
"version": "v1"
}
] | 2014-04-15 | [
[
"Karczmarek",
"Joanna L.",
""
],
[
"Rabideau",
"Charles",
""
]
] | We compute holographic entanglement entropy in two strongly coupled nonlocal field theories: the dipole and the noncommutative deformations of SYM theory. We find that entanglement entropy in the dipole theory follows a volume law for regions smaller than the length scale of nonlocality and has a smooth cross-over to a... | 5.739472 | 5.244056 | 6.369665 | 5.590089 | 5.851006 | 5.474988 | 5.784477 | 5.863442 | 5.806375 | 6.347466 | 5.527735 | 5.643742 | 5.865061 | 5.593079 | 5.572466 | 5.808874 | 5.621787 | 5.535824 | 5.671105 | 5.834999 | 5.451204 |
2107.13130 | Phil Saad | Phil Saad, Stephen Shenker, and Shunyu Yao | Comments on wormholes and factorization | 89 pages + appendices | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In AdS/CFT partition functions of decoupled copies of the CFT factorize. In
bulk computations of such quantities contributions from spacetime wormholes
which link separate asymptotic boundaries threaten to spoil this property,
leading to a "factorization puzzle." Certain simple models like JT gravity have
wormholes, ... | [
{
"created": "Wed, 28 Jul 2021 02:13:46 GMT",
"version": "v1"
}
] | 2021-07-29 | [
[
"Saad",
"Phil",
""
],
[
"Shenker",
"Stephen",
""
],
[
"Yao",
"Shunyu",
""
]
] | In AdS/CFT partition functions of decoupled copies of the CFT factorize. In bulk computations of such quantities contributions from spacetime wormholes which link separate asymptotic boundaries threaten to spoil this property, leading to a "factorization puzzle." Certain simple models like JT gravity have wormholes, bu... | 10.994183 | 11.349196 | 13.447475 | 11.019336 | 11.845563 | 12.373792 | 11.956735 | 11.125391 | 11.102889 | 13.839207 | 11.174395 | 10.770076 | 11.566106 | 10.804938 | 10.761861 | 10.750701 | 10.832071 | 11.073995 | 10.755661 | 11.267062 | 10.896731 |
1012.3154 | Antonio Amariti | A. Amariti | Dynamical SUSY Breaking and the Beta-Deformation | 12 pages, 4 figures, JHEP3.cls, references added, final version
published on JHEP | null | 10.1007/JHEP09(2011)111 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study supersymmetry breaking metastable vacua arising from beta deformed
quiver gauge theories. The relation between the bounds on metastability and the
deformation are discussed. Metastable supersymmetry breaking vacua are found in
the IR of beta deformed cascading quivers with vector-like field content.
Furtherm... | [
{
"created": "Tue, 14 Dec 2010 20:08:31 GMT",
"version": "v1"
},
{
"created": "Wed, 30 May 2012 20:52:02 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Amariti",
"A.",
""
]
] | We study supersymmetry breaking metastable vacua arising from beta deformed quiver gauge theories. The relation between the bounds on metastability and the deformation are discussed. Metastable supersymmetry breaking vacua are found in the IR of beta deformed cascading quivers with vector-like field content. Furthermor... | 12.124776 | 10.719762 | 12.95461 | 10.886543 | 10.730547 | 11.27364 | 11.427863 | 11.5784 | 10.804884 | 13.488441 | 10.608064 | 11.377967 | 12.169469 | 11.474614 | 11.222708 | 11.33146 | 11.170942 | 10.934229 | 11.140964 | 12.755826 | 11.250347 |
0709.1411 | Anton Zeitlin | Anton M. Zeitlin | BV Yang-Mills as a Homotopy Chern-Simons via SFT | LaTeX2e, 22 pages, minor revisions, typos corrected, references
added, Int. J. Mod. Physics A, published version | Int.J.Mod.Phys. A24 (2009) 1309 - 1331 | 10.1142/S0217751X09043031 | null | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show explicitly how BV Yang-Mills action emerges as a homotopy
generalization of Chern-Simons theory from the algebraic constructions arising
from String Field Theory.
| [
{
"created": "Mon, 10 Sep 2007 15:02:56 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Nov 2007 18:38:26 GMT",
"version": "v2"
},
{
"created": "Wed, 10 Dec 2008 04:12:25 GMT",
"version": "v3"
},
{
"created": "Tue, 31 Mar 2009 19:39:26 GMT",
"version": "v4"
}
] | 2009-03-31 | [
[
"Zeitlin",
"Anton M.",
""
]
] | We show explicitly how BV Yang-Mills action emerges as a homotopy generalization of Chern-Simons theory from the algebraic constructions arising from String Field Theory. | 27.580431 | 15.039352 | 20.027491 | 18.060966 | 19.914406 | 15.866613 | 18.764933 | 15.752615 | 15.735248 | 28.304138 | 17.83185 | 20.552025 | 20.716181 | 19.971544 | 19.713215 | 19.831617 | 19.20487 | 18.575052 | 19.726576 | 22.808784 | 19.038094 |
hep-th/9302061 | null | Arlen Anderson | Quantum Canonical Transformations and Integrability: Beyond Unitary
Transformations | 15 pages, LaTeX, Imperial-TP-92-93-19 [Revision consists of new
material on observables and an explanation of how the proposed definition of
integrability allows for systems which have fewer commuting integrals of the
motion than degrees of freedom.] | Phys.Lett.B319:157-162,1993 | 10.1016/0370-2693(93)90796-K | null | hep-th | null | Quantum canonical transformations are defined in analogy to classical
canonical transformations as changes of the phase space variables which
preserve the Dirac bracket structure. In themselves, they are neither unitary
nor non-unitary. A definition of quantum integrability in terms of canonical
transformations is pr... | [
{
"created": "Mon, 15 Feb 1993 00:13:01 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Sep 1993 13:56:42 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Anderson",
"Arlen",
""
]
] | Quantum canonical transformations are defined in analogy to classical canonical transformations as changes of the phase space variables which preserve the Dirac bracket structure. In themselves, they are neither unitary nor non-unitary. A definition of quantum integrability in terms of canonical transformations is prop... | 8.35094 | 8.863803 | 8.650174 | 7.744863 | 7.693489 | 7.157415 | 7.841619 | 8.074828 | 7.45677 | 9.696814 | 8.434627 | 7.764477 | 7.956562 | 7.87461 | 7.70224 | 7.967119 | 7.649838 | 7.789262 | 7.934591 | 8.548153 | 8.070117 |
hep-th/9910199 | Jeong-Hyuck Park | Jeong-Hyuck Park | Superconformal Symmetry in Three-dimensions | 1+46 pages, No figure, LaTeX, References added | J.Math.Phys. 41 (2000) 7129-7161 | 10.1063/1.1290056 | KIAS-99101 | hep-th | null | Three-dimensional N-extended superconformal symmetry is studied within the
superspace formalism. A superconformal Killing equation is derived and its
solutions are classified in terms of supertranslations, dilations, Lorentz
transformations, R-symmetry transformations and special superconformal
transformations. Super... | [
{
"created": "Tue, 26 Oct 1999 08:12:31 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Nov 1999 03:33:06 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Park",
"Jeong-Hyuck",
""
]
] | Three-dimensional N-extended superconformal symmetry is studied within the superspace formalism. A superconformal Killing equation is derived and its solutions are classified in terms of supertranslations, dilations, Lorentz transformations, R-symmetry transformations and special superconformal transformations. Superco... | 5.975622 | 5.078488 | 6.482305 | 5.187358 | 5.296149 | 5.443901 | 5.139021 | 5.086145 | 5.172829 | 6.673626 | 5.263567 | 5.81309 | 5.989784 | 5.613149 | 5.701823 | 5.6724 | 5.45274 | 5.633129 | 5.625661 | 6.030264 | 5.623408 |
hep-th/9112063 | David Senechal | P. Di Francesco, P. Mathieu and D. Senechal | Integrability of the quantum KdV equation at c = -2 | 9 pages | Mod.Phys.Lett. A7 (1992) 701-708 | 10.1142/S0217732392000677 | null | hep-th | null | We present a simple a direct proof of the complete integrability of the
quantum KdV equation at $c=-2$, with an explicit description of all the
conservation laws.
| [
{
"created": "Fri, 20 Dec 1991 18:57:42 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Di Francesco",
"P.",
""
],
[
"Mathieu",
"P.",
""
],
[
"Senechal",
"D.",
""
]
] | We present a simple a direct proof of the complete integrability of the quantum KdV equation at $c=-2$, with an explicit description of all the conservation laws. | 13.518521 | 11.574323 | 14.133174 | 11.491222 | 11.41578 | 11.284663 | 10.699827 | 12.504827 | 12.516657 | 15.288806 | 10.615114 | 11.102196 | 15.251245 | 12.318756 | 11.337706 | 10.475549 | 11.678888 | 11.263987 | 12.387361 | 14.052718 | 10.536899 |
hep-th/9612229 | Donam Youm | Mirjam Cvetic and Donam Youm | Rotating Intersecting M-Branes | 28 pages, uses RevTex, the revised version to appear in Nuclear
Physics B | Nucl.Phys.B499:253-282,1997 | 10.1016/S0550-3213(97)00302-7 | IASSNS-HEP-96/123,UPR-728-T | hep-th gr-qc | null | We present intersecting p-brane solutions of eleven-dimensional supergravity
(M-branes) which upon toroidal compactification reduce to non-extreme
``rotating'' black holes. We identify harmonic functions, associated with each
M-brane, and non-extremality functions, specifying a deviation from the BPS
limit. These fun... | [
{
"created": "Tue, 24 Dec 1996 00:50:08 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Jun 1997 18:18:45 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Cvetic",
"Mirjam",
""
],
[
"Youm",
"Donam",
""
]
] | We present intersecting p-brane solutions of eleven-dimensional supergravity (M-branes) which upon toroidal compactification reduce to non-extreme ``rotating'' black holes. We identify harmonic functions, associated with each M-brane, and non-extremality functions, specifying a deviation from the BPS limit. These funct... | 12.498159 | 11.071179 | 12.761009 | 11.074204 | 12.932339 | 12.544144 | 11.690121 | 10.387447 | 11.267621 | 12.866911 | 12.124033 | 11.745748 | 12.084704 | 11.302781 | 11.567504 | 10.873104 | 11.026114 | 11.821743 | 11.632436 | 11.983227 | 11.195921 |
1807.09712 | Javier Tarrio | Anton F. Faedo, David Mateos, Christiana Pantelidou, Javier Tarrio | A Supersymmetric Color Superconductor from Holography | 11 pages, 2 figures. v2: comments and references added, published
text | null | 10.1007/JHEP05(2019)106 | ICCUB-18-016 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use holography to study $d=4$, $\mathcal{N}=4$, SU($N_{\rm \tiny{c}}$)
super Yang-Mills coupled to $N_{\rm \tiny{F}} \ll N_{\rm \tiny{c}}$ quark
flavors. We place the theory at finite isospin density $n_{\rm \tiny{I}}$ by
turning on an isospin chemical potential $\mu_{\rm \tiny{I}}=M_{\rm \tiny{q}}$,
with $M_{\rm ... | [
{
"created": "Wed, 25 Jul 2018 16:37:59 GMT",
"version": "v1"
},
{
"created": "Mon, 27 May 2019 09:12:22 GMT",
"version": "v2"
}
] | 2019-06-26 | [
[
"Faedo",
"Anton F.",
""
],
[
"Mateos",
"David",
""
],
[
"Pantelidou",
"Christiana",
""
],
[
"Tarrio",
"Javier",
""
]
] | We use holography to study $d=4$, $\mathcal{N}=4$, SU($N_{\rm \tiny{c}}$) super Yang-Mills coupled to $N_{\rm \tiny{F}} \ll N_{\rm \tiny{c}}$ quark flavors. We place the theory at finite isospin density $n_{\rm \tiny{I}}$ by turning on an isospin chemical potential $\mu_{\rm \tiny{I}}=M_{\rm \tiny{q}}$, with $M_{\rm \t... | 4.46089 | 4.274465 | 4.66908 | 4.068072 | 4.120316 | 4.125159 | 4.526542 | 4.111554 | 4.216084 | 4.831975 | 4.10504 | 4.273044 | 4.417404 | 4.224628 | 4.277531 | 4.277262 | 4.1714 | 4.169331 | 4.270764 | 4.448492 | 4.284004 |
1504.03723 | Andrew Hickling | Andrew Hickling | Bulk Duals for Generic Static, Scale-Invariant Holographic CFT States | null | null | 10.1088/0264-9381/32/17/175011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Near horizon geometries have been widely studied, and have found many
applications. Certain static, near horizon geometries are now understood to be
bulk duals to CFTs with static scale-invariant sources under the AdS/CFT
correspondence. However, static near-horizon geometries aren't just
scale-invariant, they have e... | [
{
"created": "Tue, 14 Apr 2015 21:00:56 GMT",
"version": "v1"
}
] | 2015-08-26 | [
[
"Hickling",
"Andrew",
""
]
] | Near horizon geometries have been widely studied, and have found many applications. Certain static, near horizon geometries are now understood to be bulk duals to CFTs with static scale-invariant sources under the AdS/CFT correspondence. However, static near-horizon geometries aren't just scale-invariant, they have ext... | 8.574074 | 8.405077 | 8.748826 | 8.130113 | 8.333588 | 8.785573 | 8.62361 | 8.410087 | 8.339294 | 9.294784 | 8.435399 | 7.975627 | 7.965221 | 7.827466 | 7.854841 | 8.213392 | 7.93311 | 8.176662 | 7.951192 | 8.175736 | 7.927663 |
hep-th/0401160 | T. Damour | Thibault Damour | The entropy of black holes: a primer | 51 pages, 4 figures, talk given at the "Poincare seminar" (Paris, 6
December 2003), to appear in Poincare Seminar 2003 (Birkhauser) | null | 10.1007/978-3-0348-7932-3_10 | null | hep-th astro-ph gr-qc | null | After recalling the definition of black holes, and reviewing their energetics
and their classical thermodynamics, one expounds the conjecture of Bekenstein,
attributing an entropy to black holes, and the calculation by Hawking of the
semi-classical radiation spectrum of a black hole, involving a thermal
(Planckian) f... | [
{
"created": "Thu, 22 Jan 2004 16:54:38 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Damour",
"Thibault",
""
]
] | After recalling the definition of black holes, and reviewing their energetics and their classical thermodynamics, one expounds the conjecture of Bekenstein, attributing an entropy to black holes, and the calculation by Hawking of the semi-classical radiation spectrum of a black hole, involving a thermal (Planckian) fac... | 7.821803 | 7.737988 | 8.117694 | 7.595015 | 7.568013 | 7.362501 | 7.822465 | 7.391523 | 8.097127 | 8.936432 | 7.613662 | 7.33681 | 7.702823 | 7.447229 | 7.566904 | 7.661815 | 7.496573 | 7.491904 | 7.621131 | 7.452085 | 7.494021 |
1406.2699 | Francesco Benini | Francesco Benini, Daniel S. Park, Peng Zhao | Cluster algebras from dualities of 2d N=(2,2) quiver gauge theories | 49 pages + appendices, 8 figures | Commun.Math.Phys. 340 (2015) 1, 47-104 | 10.1007/s00220-015-2452-3 | null | hep-th math.RA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We interpret certain Seiberg-like dualities of two-dimensional N=(2,2) quiver
gauge theories with unitary groups as cluster mutations in cluster algebras,
originally formulated by Fomin and Zelevinsky. In particular, we show how the
complexified Fayet-Iliopoulos parameters of the gauge group factors transform
under t... | [
{
"created": "Tue, 10 Jun 2014 20:00:17 GMT",
"version": "v1"
}
] | 2015-09-15 | [
[
"Benini",
"Francesco",
""
],
[
"Park",
"Daniel S.",
""
],
[
"Zhao",
"Peng",
""
]
] | We interpret certain Seiberg-like dualities of two-dimensional N=(2,2) quiver gauge theories with unitary groups as cluster mutations in cluster algebras, originally formulated by Fomin and Zelevinsky. In particular, we show how the complexified Fayet-Iliopoulos parameters of the gauge group factors transform under tho... | 7.504366 | 7.895318 | 9.194052 | 6.866284 | 8.290009 | 8.087162 | 7.616545 | 6.775454 | 7.18291 | 10.298361 | 6.97362 | 7.275065 | 7.680741 | 7.063262 | 7.054574 | 7.139524 | 7.559795 | 7.030132 | 6.961788 | 7.458386 | 7.009605 |
1507.02327 | Anatoly Shabad | Tiago C. Adorno (1), Dmitry M. Gitman (1,2,3), Anatoly E. Shabad (2,3)
((1) Instituto de Fisica, Universidade de Sao Paulo, CEP 05508-090, Sao
Paulo, S. P., Brazil (2) P. N. Lebedev Physics Institute, Leninsky Prospekt
53, Moscow 117924, Russia (3) Tomsk State University, Lenin Prospekt 36,
Tomsk 634050, Russia... | When electric charge becomes also magnetic | Four pages, no figures | Phys. Rev. D 92, 041702 (2015) | 10.1103/PhysRevD.92.041702 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In nonlinear electrodynamics, QED included, we find a static solution to the
field equations with an electric charge as its source, which is comprised of
homogeneous parallel magnetic and electric fields, and a radial
spherically-nonsymmetric long-range magnetic field, whose magnetic charge is
proportional to the ele... | [
{
"created": "Wed, 8 Jul 2015 22:29:13 GMT",
"version": "v1"
}
] | 2015-09-09 | [
[
"Adorno",
"Tiago C.",
""
],
[
"Gitman",
"Dmitry M.",
""
],
[
"Shabad",
"Anatoly E.",
""
]
] | In nonlinear electrodynamics, QED included, we find a static solution to the field equations with an electric charge as its source, which is comprised of homogeneous parallel magnetic and electric fields, and a radial spherically-nonsymmetric long-range magnetic field, whose magnetic charge is proportional to the elect... | 17.3165 | 15.875438 | 15.894648 | 16.076477 | 17.762703 | 13.861142 | 16.205362 | 13.625587 | 16.593672 | 16.498117 | 14.42732 | 15.508275 | 15.699389 | 15.562241 | 15.833258 | 16.610384 | 15.629949 | 16.926304 | 15.407751 | 15.926691 | 15.147958 |
1910.12981 | Kostas Filippas | Kostas Filippas | Non-integrability on AdS$_3$ supergravity backgrounds | 22 pages plus appendices. Added references, corrected typos,
corrected/added comments, improved title | null | 10.1007/JHEP02(2020)027 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate classical integrability on two recently discovered classes of
backgrounds in massive IIA supergravity. These vacua are of the form
AdS$_3\times\,$S$^2\times\mathbb{R}\times\,$CY$_2$, they preserve small
$\mathcal{N}=(0,4)$ supersymmetry and are associated with D8$-$D6$-$D4$-$D2
Hanany-Witten brane set-... | [
{
"created": "Mon, 28 Oct 2019 21:47:52 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Nov 2019 12:09:17 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Jan 2020 15:44:50 GMT",
"version": "v3"
}
] | 2020-03-18 | [
[
"Filippas",
"Kostas",
""
]
] | We investigate classical integrability on two recently discovered classes of backgrounds in massive IIA supergravity. These vacua are of the form AdS$_3\times\,$S$^2\times\mathbb{R}\times\,$CY$_2$, they preserve small $\mathcal{N}=(0,4)$ supersymmetry and are associated with D8$-$D6$-$D4$-$D2 Hanany-Witten brane set-up... | 7.562894 | 7.365505 | 9.070409 | 7.356118 | 7.842556 | 8.055249 | 7.802442 | 7.363246 | 8.166664 | 9.768716 | 7.48206 | 7.468047 | 8.402456 | 7.39724 | 7.639443 | 7.387538 | 7.464378 | 7.296831 | 7.442102 | 7.940664 | 7.436082 |
hep-th/9201063 | Marc Kamionkowski | Marc Kamionkowski and John March-Russell | Are Textures Natural? | 9pp | Phys.Rev.Lett. 69 (1992) 1485-1488 | 10.1103/PhysRevLett.69.1485 | null | hep-th | null | We make the simple observation that, because of global symmetry violating
higher-dimension operators expected to be induced by Planck-scale physics,
textures are generically much too short-lived to be of use for large-scale
structure formation.
| [
{
"created": "Tue, 28 Jan 1992 22:05:04 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jan 1992 23:12:26 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Kamionkowski",
"Marc",
""
],
[
"March-Russell",
"John",
""
]
] | We make the simple observation that, because of global symmetry violating higher-dimension operators expected to be induced by Planck-scale physics, textures are generically much too short-lived to be of use for large-scale structure formation. | 20.700367 | 16.268291 | 14.857347 | 16.606825 | 16.064388 | 18.778858 | 16.195927 | 15.413795 | 15.548322 | 13.453905 | 16.758053 | 17.483454 | 17.003641 | 14.8521 | 16.480156 | 15.5978 | 16.987696 | 17.198919 | 15.064078 | 16.143833 | 16.185511 |
hep-th/0611265 | Parthasarathi Mitra | P. Mitra | Hawking temperature from tunnelling formalism | REVTeX, 3 pages; version accepted in Phys. Letters B | Phys.Lett.B648:240-242,2007 | 10.1016/j.physletb.2007.03.002 | null | hep-th gr-qc | null | It has recently been suggested that the attempt to understand Hawking
radiation as tunnelling across black hole horizons produces a Hawking
temperature double the standard value. It is explained here how one can obtain
the standard value in the same tunnelling approach.
| [
{
"created": "Fri, 24 Nov 2006 11:09:23 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Nov 2006 11:13:43 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Mar 2007 05:25:48 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Mitra",
"P.",
""
]
] | It has recently been suggested that the attempt to understand Hawking radiation as tunnelling across black hole horizons produces a Hawking temperature double the standard value. It is explained here how one can obtain the standard value in the same tunnelling approach. | 9.739616 | 8.017957 | 7.763186 | 7.784255 | 8.307795 | 8.526217 | 7.855572 | 6.785101 | 7.701648 | 8.739279 | 8.22393 | 9.61623 | 8.577349 | 8.623522 | 8.219032 | 8.689013 | 8.520152 | 8.627441 | 8.415016 | 9.11937 | 8.867772 |
hep-th/0610163 | Pedro J. Silva | Pedro J. Silva | Phase transitions and statistical mechanics for BPS Black Holes in
AdS/CFT | 14 pages, 5 figures, corrected typos and references added | JHEP 0703:015,2007 | 10.1088/1126-6708/2007/03/015 | null | hep-th | null | Using the general framework developed in hep-th/0607056, we study in detail
the phase space of BPS Black Holes in AdS, for the case where all three
electric charges are equal. Although these solitons are supersymmetric with
zero Hawking temperature, it turns out that these Black Holes have rich phase
structure with s... | [
{
"created": "Sun, 15 Oct 2006 11:15:20 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Nov 2006 15:36:09 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Silva",
"Pedro J.",
""
]
] | Using the general framework developed in hep-th/0607056, we study in detail the phase space of BPS Black Holes in AdS, for the case where all three electric charges are equal. Although these solitons are supersymmetric with zero Hawking temperature, it turns out that these Black Holes have rich phase structure with sha... | 16.468004 | 16.094221 | 17.322128 | 15.208155 | 16.055761 | 16.464512 | 17.465902 | 16.420969 | 15.628682 | 18.923492 | 15.226844 | 15.700728 | 16.548716 | 15.755561 | 15.734464 | 15.455832 | 16.117273 | 15.948824 | 15.625814 | 16.121042 | 15.672899 |
1704.04148 | Igor Samsonov | I.B. Samsonov | Low-energy effective action in two-dimensional SQED: A two-loop analysis | 40 pages; v2: references added, typos corrected | null | 10.1007/JHEP07(2017)146 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study two-loop quantum corrections to the low-energy effective actions in
N=(2,2) and N=(4,4) SQED in the Coulomb branch. In the latter model, the
low-energy effective action is described by a generalized Kahler potential
which depends on both chiral and twisted chiral superfields. We demonstrate
that this general... | [
{
"created": "Thu, 13 Apr 2017 14:23:03 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Apr 2017 07:18:20 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Samsonov",
"I. B.",
""
]
] | We study two-loop quantum corrections to the low-energy effective actions in N=(2,2) and N=(4,4) SQED in the Coulomb branch. In the latter model, the low-energy effective action is described by a generalized Kahler potential which depends on both chiral and twisted chiral superfields. We demonstrate that this generaliz... | 5.131227 | 4.873754 | 6.123656 | 4.891982 | 5.107902 | 4.947176 | 5.143934 | 4.897168 | 4.687255 | 6.354043 | 5.156214 | 5.128148 | 5.452147 | 4.883247 | 4.926976 | 4.845876 | 4.792112 | 4.977781 | 4.941905 | 5.201469 | 4.989343 |
hep-th/9712075 | Chris Hull | C.M. Hull | U-Duality and BPS Spectrum of Super Yang-Mills Theory and M-Theory | 18 Pages, Tex, Phyzzx Macro. References added, minor corrections | JHEP 9807:018,1998 | 10.1088/1126-6708/1998/07/018 | QMW-97-39, LPTENS 97/59 | hep-th | null | It is shown that the BPS spectrum of Super-Yang-Mills theory on $T^d\times
\R$, which fits into representations of the U-duality group for M-theory
compactified on $T^{d}$, in accordance with the matrix-theory conjecture, in
fact fits into representations of the U-duality group for M-theory on
$T^{d+1}$, the extra du... | [
{
"created": "Sun, 7 Dec 1997 14:43:52 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Hull",
"C. M.",
""
]
] | It is shown that the BPS spectrum of Super-Yang-Mills theory on $T^d\times \R$, which fits into representations of the U-duality group for M-theory compactified on $T^{d}$, in accordance with the matrix-theory conjecture, in fact fits into representations of the U-duality group for M-theory on $T^{d+1}$, the extra dual... | 10.14397 | 9.606239 | 11.802035 | 9.789633 | 8.451818 | 9.216637 | 10.813589 | 9.683546 | 9.115277 | 11.836411 | 9.549771 | 9.304277 | 10.859529 | 9.290936 | 9.10078 | 9.077594 | 9.035165 | 8.868969 | 9.060011 | 9.9923 | 8.900438 |
hep-th/0201004 | Robert Mann | A.M. Ghezelbash, D. Ida, R.B. Mann and T. Shiromizu | Slicing and Brane Dependence of the (A)dS/CFT Correspondence | latex, 6 pages, minor changes in wording, reference added | Phys.Lett. B535 (2002) 315-320 | 10.1016/S0370-2693(02)01773-2 | WATPHYS-TH02/01 | hep-th | null | We investigate the slicing dependence of the relationship between conserved
quantities in the (A)dS/CFT correspondence. Specifically, we show that the
Casimir energy depends upon the topology and geometry of spacetime foliations
of the bulk near the conformal boundary. We point out that the determination of
the brane... | [
{
"created": "Wed, 2 Jan 2002 14:40:35 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Jan 2002 21:19:46 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Mar 2002 20:58:38 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Ghezelbash",
"A. M.",
""
],
[
"Ida",
"D.",
""
],
[
"Mann",
"R. B.",
""
],
[
"Shiromizu",
"T.",
""
]
] | We investigate the slicing dependence of the relationship between conserved quantities in the (A)dS/CFT correspondence. Specifically, we show that the Casimir energy depends upon the topology and geometry of spacetime foliations of the bulk near the conformal boundary. We point out that the determination of the brane l... | 10.006409 | 9.639774 | 9.312201 | 9.308327 | 9.316742 | 8.914749 | 9.867829 | 9.134317 | 9.120325 | 10.026553 | 8.467509 | 8.659065 | 8.766837 | 8.691586 | 8.524502 | 8.701437 | 8.706892 | 8.667585 | 8.649491 | 9.062735 | 8.351573 |
hep-th/0504137 | Qing-Guo Huang | Qing-Guo Huang and Ke Ke | Non-Gaussianity in KKLMMT model | 13 pages, 2 figuers, harvmac; references added | Phys.Lett. B633 (2006) 447-452 | 10.1016/j.physletb.2005.12.038 | null | hep-th astro-ph gr-qc hep-ph | null | We investigate the non-Gaussianity of the brane inflation which happens in
the same throat in the framework of the generalized KKLMMT model. When we take
the constraints from non-Gaussianity into account, various consequences are
discussed including the bound on the string coupling, such as the string
coupling is lar... | [
{
"created": "Sat, 16 Apr 2005 11:50:22 GMT",
"version": "v1"
},
{
"created": "Mon, 2 May 2005 06:22:50 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Huang",
"Qing-Guo",
""
],
[
"Ke",
"Ke",
""
]
] | We investigate the non-Gaussianity of the brane inflation which happens in the same throat in the framework of the generalized KKLMMT model. When we take the constraints from non-Gaussianity into account, various consequences are discussed including the bound on the string coupling, such as the string coupling is large... | 9.926832 | 10.051016 | 10.315713 | 8.65972 | 9.674293 | 9.564034 | 9.502462 | 9.390141 | 8.989323 | 11.803057 | 8.488098 | 9.347632 | 9.076619 | 8.937148 | 9.184433 | 9.20748 | 9.207226 | 9.116912 | 9.274584 | 9.672242 | 8.854409 |
hep-th/9706211 | Tomasz Taylor | I. Antoniadis, H. Partouche, T.R. Taylor | Lectures on Heterotic-Type I Duality | 14 pages, LaTeX, espcrc2.sty | Nucl.Phys.Proc.Suppl. 61A (1998) 58-71; Nucl.Phys.Proc.Suppl. 67
(1998) 3-16 | 10.1016/S0920-5632(98)00114-5 | CERN--TH/97-136; CPTH--5370.0697 | hep-th | null | We present a review of heterotic-type I string duality. In particular, we
discuss the effective field theory of six- and four-dimensional
compactifications with N>1 supersymmetries. We then describe various duality
tests by comparing gauge couplings, N=2 prepotentials, as well as
higher-derivative F-terms. Based on i... | [
{
"created": "Sat, 28 Jun 1997 17:28:35 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Antoniadis",
"I.",
""
],
[
"Partouche",
"H.",
""
],
[
"Taylor",
"T. R.",
""
]
] | We present a review of heterotic-type I string duality. In particular, we discuss the effective field theory of six- and four-dimensional compactifications with N>1 supersymmetries. We then describe various duality tests by comparing gauge couplings, N=2 prepotentials, as well as higher-derivative F-terms. Based on inv... | 5.12766 | 4.662292 | 5.917409 | 4.730914 | 4.850471 | 4.46799 | 4.667771 | 4.763654 | 4.882607 | 7.010766 | 4.91569 | 4.66736 | 5.80175 | 4.958244 | 4.905277 | 5.123377 | 4.907423 | 4.840633 | 4.888613 | 5.602894 | 4.798604 |
hep-th/9404122 | Junichi Shiraishi | Jun'ichi Shiraishi | A trial to find an elliptic quantum algebra for $sl_2$ using the
Heisenberg and Clifford algebra | 4 pages | Mod.Phys.Lett. A9 (1994) 2301-2304 | 10.1142/S0217732394002161 | null | hep-th | null | A Heisenberg-Clifford realization of a deformed $U(sl_{2})$ by two parameters
$p$ and $q$ is discussed. The commutation relations for this deformed algebra
have interesting connection with the theta functions.
| [
{
"created": "Wed, 20 Apr 1994 12:18:26 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Shiraishi",
"Jun'ichi",
""
]
] | A Heisenberg-Clifford realization of a deformed $U(sl_{2})$ by two parameters $p$ and $q$ is discussed. The commutation relations for this deformed algebra have interesting connection with the theta functions. | 14.08718 | 11.82673 | 13.675871 | 10.494182 | 10.107828 | 12.250159 | 10.592047 | 10.600924 | 10.62688 | 13.135557 | 11.454877 | 10.724916 | 12.228846 | 10.848011 | 11.33362 | 11.156716 | 10.865962 | 11.65369 | 11.199431 | 11.253848 | 10.264952 |
1009.3277 | Matthew Kleban | Simeon Hellerman and Matthew Kleban | Dynamical Cobordisms in General Relativity and String Theory | 35 pages, 5 figures, LaTeX v2: reference added | JHEP 1102:022,2011 | 10.1007/JHEP02(2011)022 | IPMU-10-0156 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a class of time-dependent solutions in string- or M-theory that
are exact with respect to alpha-prime and curvature corrections and interpolate
in physical space between regions in which the low energy physics is
well-approximated by different string theories and string compactifications.
The regions are ... | [
{
"created": "Thu, 16 Sep 2010 20:13:09 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Nov 2010 19:31:35 GMT",
"version": "v2"
}
] | 2011-02-15 | [
[
"Hellerman",
"Simeon",
""
],
[
"Kleban",
"Matthew",
""
]
] | We describe a class of time-dependent solutions in string- or M-theory that are exact with respect to alpha-prime and curvature corrections and interpolate in physical space between regions in which the low energy physics is well-approximated by different string theories and string compactifications. The regions are co... | 11.46923 | 11.52647 | 12.340593 | 11.127309 | 11.388437 | 11.154067 | 12.294376 | 10.239438 | 11.483572 | 13.996995 | 11.275607 | 11.035276 | 11.65848 | 10.797805 | 11.004313 | 10.668953 | 10.820692 | 10.803529 | 10.808011 | 10.985887 | 10.508451 |
1105.4862 | Ant\'on F. Faedo | Irene Amado and Anton F. Faedo | Lifshitz black holes in string theory | 19 pages, 7 figures. v2 references added | JHEP 1107:004,2011 | 10.1007/JHEP07(2011)004 | SISSA 21/2011/EP | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide the first black hole solutions with Lifshitz asymptotics found in
string theory. These are expected to be dual to models enjoying anisotropic
scale invariance with dynamical exponent z=2 at finite temperature. We employ a
consistent truncation of type IIB supergravity to four dimensions with an
arbitrary 5... | [
{
"created": "Tue, 24 May 2011 19:29:07 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Jun 2011 10:38:17 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Amado",
"Irene",
""
],
[
"Faedo",
"Anton F.",
""
]
] | We provide the first black hole solutions with Lifshitz asymptotics found in string theory. These are expected to be dual to models enjoying anisotropic scale invariance with dynamical exponent z=2 at finite temperature. We employ a consistent truncation of type IIB supergravity to four dimensions with an arbitrary 5-d... | 8.677372 | 7.962368 | 9.456776 | 8.075255 | 8.51517 | 8.240078 | 7.872509 | 7.787339 | 7.332901 | 9.673369 | 7.628496 | 8.150449 | 8.368431 | 8.135132 | 8.572618 | 8.021416 | 8.147172 | 8.497911 | 8.168218 | 8.6654 | 8.081127 |
hep-th/0508179 | Jorgen Rasmussen | Jorgen Rasmussen | Affine Jordan cells, logarithmic correlators, and hamiltonian reduction | 31 pages, v2: reference corrected, v3: version to be published | Nucl.Phys.B736:225-258,2006 | 10.1016/j.nuclphysb.2005.12.009 | null | hep-th | null | We study a particular type of logarithmic extension of SL(2,R)
Wess-Zumino-Witten models. It is based on the introduction of affine Jordan
cells constructed as multiplets of quasi-primary fields organized in
indecomposable representations of the Lie algebra sl(2). We solve the
simultaneously imposed set of conformal ... | [
{
"created": "Wed, 24 Aug 2005 15:34:47 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Sep 2005 01:40:15 GMT",
"version": "v2"
},
{
"created": "Tue, 3 Jan 2006 01:54:11 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Rasmussen",
"Jorgen",
""
]
] | We study a particular type of logarithmic extension of SL(2,R) Wess-Zumino-Witten models. It is based on the introduction of affine Jordan cells constructed as multiplets of quasi-primary fields organized in indecomposable representations of the Lie algebra sl(2). We solve the simultaneously imposed set of conformal an... | 11.271923 | 11.131172 | 13.799721 | 10.613632 | 11.892555 | 11.305134 | 11.31369 | 11.166488 | 10.420732 | 13.777078 | 11.652082 | 10.98989 | 11.687004 | 10.806713 | 10.419365 | 10.375669 | 10.785089 | 10.772217 | 10.761379 | 11.737612 | 10.7236 |
hep-th/0101141 | Jose Manuel velhinho | J. M. Velhinho | Some properties of generalized connections in quantum gravity | LaTeX, 11 pages. Submitted to the on-line proceedings of the Ninth
Marcel Grossmann Meeting (Rome, July 2000). Talk based on hep-th/0011200 | null | 10.1142/9789812777386_0220 | null | hep-th | null | The quantum completion of the space of connections in a manifold can be seen
as the set of all morphisms from the groupoid of the edges of the manifold to
the (compact) gauge group. This algebraic construction generalizes the
analogous description of the gauge-invariant quantum configuration space of
Ashtekar and Ish... | [
{
"created": "Mon, 22 Jan 2001 15:34:30 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Velhinho",
"J. M.",
""
]
] | The quantum completion of the space of connections in a manifold can be seen as the set of all morphisms from the groupoid of the edges of the manifold to the (compact) gauge group. This algebraic construction generalizes the analogous description of the gauge-invariant quantum configuration space of Ashtekar and Isham... | 9.456471 | 8.841445 | 9.161728 | 8.545096 | 8.89322 | 8.529391 | 10.670017 | 8.657555 | 10.152699 | 9.9199 | 9.298898 | 9.394863 | 8.669942 | 8.647666 | 8.867525 | 8.79236 | 8.837885 | 8.517405 | 8.973135 | 8.871953 | 8.822645 |
1112.4599 | Huiquan Li | Huiquan Li | Strings from geometric tachyon in Rindler space and black hole
thermodynamics | 12 pages | null | 10.1007/JHEP03(2012)003 | USTC-ICTS-11-14 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dynamics of a probe particle or wrapped brane moving in the
two-dimensional Rindler space can be described by a time-dependent tachyon
field theory. Using knowledge of tachyon condensation, we learn that the
infalling brane gets thermalised and produces open string pairs at the Hagedorn
temperature when entering ... | [
{
"created": "Tue, 20 Dec 2011 08:05:04 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Mar 2012 02:19:06 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Li",
"Huiquan",
""
]
] | The dynamics of a probe particle or wrapped brane moving in the two-dimensional Rindler space can be described by a time-dependent tachyon field theory. Using knowledge of tachyon condensation, we learn that the infalling brane gets thermalised and produces open string pairs at the Hagedorn temperature when entering in... | 11.306274 | 9.329861 | 10.905251 | 9.929311 | 10.726695 | 10.581963 | 9.989568 | 10.175918 | 9.954084 | 11.190426 | 9.951023 | 10.37248 | 10.396655 | 9.969268 | 10.061827 | 10.006845 | 10.119719 | 10.051421 | 10.27748 | 10.476505 | 10.458467 |
hep-th/9208014 | null | S.P. Gavrilov, D.M. Gitman | Quantization of systems with time-dependent constraints. Example of
relativistic particle in plane wave | 16 pg. , IFUSP/P-980-APRIL-1992 | Class.Quant.Grav.10:57-67,1993 | 10.1088/0264-9381/10/1/008 | null | hep-th | null | A modification of the canonical quantization procedure for systems with
time-dependent second-class constraints is discussed and applied to the
quantization of the relativistic particle in a plane wave. The time dependence
of constraints appears in the problem in two ways. The Lagrangian depends on
time explicitly by... | [
{
"created": "Tue, 4 Aug 1992 17:35:25 GMT",
"version": "v1"
}
] | 2010-04-06 | [
[
"Gavrilov",
"S. P.",
""
],
[
"Gitman",
"D. M.",
""
]
] | A modification of the canonical quantization procedure for systems with time-dependent second-class constraints is discussed and applied to the quantization of the relativistic particle in a plane wave. The time dependence of constraints appears in the problem in two ways. The Lagrangian depends on time explicitly by o... | 10.161002 | 11.931865 | 11.12441 | 10.740345 | 9.925197 | 11.00642 | 10.855956 | 9.830372 | 10.116787 | 11.329327 | 9.828986 | 9.806926 | 10.380835 | 9.693853 | 9.44451 | 9.632394 | 9.657001 | 9.895415 | 9.673432 | 10.477039 | 9.790667 |
hep-th/0702108 | Ram Brustein | Ram Brustein | Cosmological Entropy Bounds | 50 pages, 4 figures, To appear in ``String theory and fundamental
interactions" published in celebration of the 65 birthday of Gabriele
Veneziano | Lect.NotesPhys.737:619-659,2008 | null | null | hep-th gr-qc | null | I review some basic facts about entropy bounds in general and about
cosmological entropy bounds. Then I review the Causal Entropy Bound, the
conditions for its validity and its application to the study of cosmological
singularities. This article is based on joint work with Gabriele Veneziano and
subsequent related re... | [
{
"created": "Wed, 14 Feb 2007 15:02:48 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Brustein",
"Ram",
""
]
] | I review some basic facts about entropy bounds in general and about cosmological entropy bounds. Then I review the Causal Entropy Bound, the conditions for its validity and its application to the study of cosmological singularities. This article is based on joint work with Gabriele Veneziano and subsequent related rese... | 11.923313 | 9.462943 | 9.753071 | 8.954061 | 9.698876 | 9.514121 | 10.010668 | 8.619793 | 9.088781 | 11.027184 | 9.293943 | 9.355202 | 10.381542 | 9.523739 | 10.413332 | 10.211168 | 9.728831 | 9.666663 | 9.889708 | 10.454293 | 9.863105 |
1612.01730 | Arjun Bagchi | Arjun Bagchi, Mirah Gary, Zodinmawia | The BMS Bootstrap | 5 pages | Phys. Rev. D 96, 025007 (2017) | 10.1103/PhysRevD.96.025007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate a study of the bootstrap programme for field theories with BMS
symmetry. Specifically, we look at two-dimensional field theories with BMS3
symmetry and, using highest weight representations, we construct the BMS
bootstrap equation by formulating the notion of crossing symmetry in the
four-point functions ... | [
{
"created": "Tue, 6 Dec 2016 10:03:32 GMT",
"version": "v1"
}
] | 2017-07-19 | [
[
"Bagchi",
"Arjun",
""
],
[
"Gary",
"Mirah",
""
],
[
"Zodinmawia",
"",
""
]
] | We initiate a study of the bootstrap programme for field theories with BMS symmetry. Specifically, we look at two-dimensional field theories with BMS3 symmetry and, using highest weight representations, we construct the BMS bootstrap equation by formulating the notion of crossing symmetry in the four-point functions of... | 7.600879 | 6.385629 | 7.815102 | 6.930341 | 7.873197 | 6.769169 | 7.199471 | 6.518281 | 7.003288 | 7.981768 | 7.020519 | 6.990612 | 7.404272 | 6.811543 | 6.850592 | 6.70448 | 6.689065 | 6.683009 | 6.695929 | 7.387676 | 6.868508 |
hep-th/9202022 | Konstantinos Anagnostopoulos | Lee Smolin | Recent Developments in Non-Perturbative Quantum Gravity | 82 pages | null | null | null | hep-th | null | New results from the new variables/loop representation program of
nonperturbative quantum gravity are presented, with a focus on results of
Ashtekar, Rovelli and the author which greatly clarify the physical
interpretation of the quantum states in the loop representation. These include:
1) The construction of a class... | [
{
"created": "Fri, 7 Feb 1992 01:00:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Smolin",
"Lee",
""
]
] | New results from the new variables/loop representation program of nonperturbative quantum gravity are presented, with a focus on results of Ashtekar, Rovelli and the author which greatly clarify the physical interpretation of the quantum states in the loop representation. These include: 1) The construction of a class o... | 7.934035 | 8.434957 | 7.954792 | 7.005013 | 7.751812 | 7.752763 | 8.392424 | 7.499228 | 8.182176 | 8.492892 | 7.492527 | 7.32249 | 7.551071 | 7.302959 | 7.386169 | 7.298919 | 7.271869 | 7.195562 | 7.480433 | 7.442208 | 7.3483 |
hep-th/0604041 | Kristjan Runar Kristjansson | Andrei V. Frolov, Kristjan R. Kristjansson, Larus Thorlacius | Global geometry of two-dimensional charged black holes | REVTeX, 13 pages, 12 figures; Reference added | Phys.Rev.D73:124036,2006 | 10.1103/PhysRevD.73.124036 | SU-ITP-06-11, NORDITA-2006-7, RH-09-2006 | hep-th gr-qc | null | The semiclassical geometry of charged black holes is studied in the context
of a two-dimensional dilaton gravity model where effects due to pair-creation
of charged particles can be included in a systematic way. The classical
mass-inflation instability of the Cauchy horizon is amplified and we find that
gravitational... | [
{
"created": "Thu, 6 Apr 2006 13:15:49 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Apr 2006 08:15:39 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Frolov",
"Andrei V.",
""
],
[
"Kristjansson",
"Kristjan R.",
""
],
[
"Thorlacius",
"Larus",
""
]
] | The semiclassical geometry of charged black holes is studied in the context of a two-dimensional dilaton gravity model where effects due to pair-creation of charged particles can be included in a systematic way. The classical mass-inflation instability of the Cauchy horizon is amplified and we find that gravitational c... | 6.841564 | 7.680564 | 7.205976 | 6.908196 | 7.624177 | 7.773942 | 7.464423 | 7.394949 | 7.545685 | 7.726908 | 7.221634 | 6.920606 | 6.974298 | 6.867497 | 6.891327 | 6.937884 | 7.101502 | 6.925755 | 7.075537 | 6.864077 | 6.951717 |
hep-th/0111050 | Gabriele Ferretti | G. Ferretti, P. Salomonson and D. Tsimpis | D-brane probes on G2 Orbifolds | 16 pages; v2: References added; v3: Erroneous interpretation of
twisted moduli corrected, acknowledgments added | JHEP 0203:004,2002 | 10.1088/1126-6708/2002/03/004 | null | hep-th | null | We consider type IIB string theory on a seven dimensional orbifold with
holonomy in G2. The motivation is to use D1-branes as probes of the geometry.
The low energy theory on the D1-brane is a sigma-model with two real
supercharges (N = (1,1) in two dimensional language). We study in detail the
closed and open string... | [
{
"created": "Tue, 6 Nov 2001 18:09:24 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Nov 2001 10:38:40 GMT",
"version": "v2"
},
{
"created": "Wed, 30 Jan 2002 14:18:47 GMT",
"version": "v3"
}
] | 2010-12-03 | [
[
"Ferretti",
"G.",
""
],
[
"Salomonson",
"P.",
""
],
[
"Tsimpis",
"D.",
""
]
] | We consider type IIB string theory on a seven dimensional orbifold with holonomy in G2. The motivation is to use D1-branes as probes of the geometry. The low energy theory on the D1-brane is a sigma-model with two real supercharges (N = (1,1) in two dimensional language). We study in detail the closed and open string s... | 10.608067 | 10.56468 | 11.781363 | 10.31635 | 10.833448 | 10.308347 | 10.487003 | 9.583748 | 10.362776 | 13.175253 | 10.645202 | 10.064288 | 11.276672 | 10.492534 | 10.475057 | 9.975633 | 9.952991 | 10.226789 | 10.134325 | 11.055227 | 10.16592 |
2011.02708 | Fabien Besnard | Fabien Besnard | Extensions of the noncommutative Standard Model and the weak order one
condition | 13 pages | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the derivation of the Standard Model from the axioms of Noncommutative
Geometry, the scalar sector is given by a finite Dirac operator which has to
satisfy the so-called \emph{first-order condition}. However, the general
solution to this constraint still has unphysical terms which must be fine-tuned
to zero. Moreo... | [
{
"created": "Thu, 5 Nov 2020 08:56:26 GMT",
"version": "v1"
}
] | 2020-11-06 | [
[
"Besnard",
"Fabien",
""
]
] | In the derivation of the Standard Model from the axioms of Noncommutative Geometry, the scalar sector is given by a finite Dirac operator which has to satisfy the so-called \emph{first-order condition}. However, the general solution to this constraint still has unphysical terms which must be fine-tuned to zero. Moreove... | 7.188766 | 7.097241 | 7.211374 | 6.544289 | 7.339973 | 6.772735 | 6.690976 | 6.976436 | 6.804717 | 7.196404 | 6.772386 | 6.843976 | 6.84085 | 6.644634 | 6.935834 | 6.932203 | 6.866694 | 6.94614 | 6.916956 | 6.959288 | 6.845618 |
hep-th/0612017 | Bobby Eka Gunara | Bobby E. Gunara, Freddy P. Zen, and Arianto | BPS Domain Walls and Vacuum Structure of N=1 Supergravity Coupled to a
Chiral Multiplet | 17 pages, a typo corrected in section 2 | J.Math.Phys.48:053505,2007 | 10.1063/1.2728889 | null | hep-th math-ph math.DS math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study BPS domain walls of N=1 supergravity coupled to a chiral multiplet
and their Lorentz invariant vacua which can be viewed as critical points of BPS
equations and the scalar potential. Supersymmetry further implies that gradient
flows of BPS equations controlled by a holomorphic superpotential and the
Kaehler ... | [
{
"created": "Sat, 2 Dec 2006 03:41:51 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Dec 2006 01:06:17 GMT",
"version": "v2"
},
{
"created": "Fri, 4 May 2007 03:45:54 GMT",
"version": "v3"
},
{
"created": "Wed, 14 Nov 2007 08:46:26 GMT",
"version": "v4"
},
{
"crea... | 2008-11-26 | [
[
"Gunara",
"Bobby E.",
""
],
[
"Zen",
"Freddy P.",
""
],
[
"Arianto",
"",
""
]
] | We study BPS domain walls of N=1 supergravity coupled to a chiral multiplet and their Lorentz invariant vacua which can be viewed as critical points of BPS equations and the scalar potential. Supersymmetry further implies that gradient flows of BPS equations controlled by a holomorphic superpotential and the Kaehler ge... | 11.779145 | 10.735489 | 15.809945 | 11.09718 | 10.983697 | 11.414373 | 11.562869 | 10.284206 | 11.007257 | 16.22176 | 11.221614 | 11.123163 | 12.961772 | 11.067719 | 11.50666 | 11.099287 | 11.652535 | 11.144024 | 10.693176 | 13.318659 | 11.084136 |
0805.0150 | Skenderis Kostas | Kostas Skenderis and Balt C. van Rees | Real-time gauge/gravity duality | 5 pages, 3 figures; v2: typos corrected, PRL version | Phys.Rev.Lett.101:081601,2008 | 10.1103/PhysRevLett.101.081601 | ITFA-2008-15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a general prescription for the holographic computation of
real-time n-point functions in non-trivial states. In QFT such real-time
computations involve a choice of a time contour in the complex time plane. The
holographic prescription amounts to ``filling in'' this contour with bulk
solutions: real segment... | [
{
"created": "Fri, 2 May 2008 14:04:46 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Jul 2008 14:48:09 GMT",
"version": "v2"
}
] | 2010-05-12 | [
[
"Skenderis",
"Kostas",
""
],
[
"van Rees",
"Balt C.",
""
]
] | We present a general prescription for the holographic computation of real-time n-point functions in non-trivial states. In QFT such real-time computations involve a choice of a time contour in the complex time plane. The holographic prescription amounts to ``filling in'' this contour with bulk solutions: real segments ... | 8.001877 | 8.966388 | 8.479233 | 7.685682 | 8.009725 | 8.263876 | 8.211949 | 7.835996 | 7.979808 | 8.925383 | 8.218072 | 7.834976 | 8.043691 | 7.70936 | 7.89 | 7.636704 | 8.090435 | 7.849596 | 7.670861 | 8.220149 | 7.613873 |
2405.00847 | Antony Speranza | Thomas Faulkner, Antony J. Speranza | Gravitational algebras and the generalized second law | 62 pages + appendices and references, 4 figures; v2 minor edits,
references added | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the generalized second law (GSL) for arbitrary cuts of Killing
horizons from the perspective of crossed-product gravitational algebras, making
use of a recent proposal by one of us for the construction of local
gravitational algebras. This construction relies on the existence of a state
whose modular flow i... | [
{
"created": "Wed, 1 May 2024 20:23:37 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Aug 2024 20:16:27 GMT",
"version": "v2"
}
] | 2024-08-14 | [
[
"Faulkner",
"Thomas",
""
],
[
"Speranza",
"Antony J.",
""
]
] | We derive the generalized second law (GSL) for arbitrary cuts of Killing horizons from the perspective of crossed-product gravitational algebras, making use of a recent proposal by one of us for the construction of local gravitational algebras. This construction relies on the existence of a state whose modular flow is ... | 12.707359 | 13.254766 | 12.753463 | 11.636446 | 12.723114 | 12.318142 | 12.625932 | 12.032623 | 11.712056 | 14.630176 | 12.107642 | 12.15156 | 12.552536 | 12.000475 | 12.501994 | 12.366254 | 12.184618 | 11.942609 | 12.434216 | 12.115188 | 12.234579 |
1108.4081 | Denis Bashkirov | Denis Bashkirov | A note on ${\cal N}\ge 6$ Superconformal Quantum Field Theories in three
dimensions | 7 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on the structure of the three-dimensional superconformal algebra we
show that every irreducible ${\mathcal N}=6$ three-dimensional superconformal
theory containes exactly one conserved U(1)-symmetry current in the stress
tensor supermultiplet and that superconformal symmetry of every ${\mathcal
N}=7$ superconfo... | [
{
"created": "Sat, 20 Aug 2011 02:13:24 GMT",
"version": "v1"
}
] | 2011-08-23 | [
[
"Bashkirov",
"Denis",
""
]
] | Based on the structure of the three-dimensional superconformal algebra we show that every irreducible ${\mathcal N}=6$ three-dimensional superconformal theory containes exactly one conserved U(1)-symmetry current in the stress tensor supermultiplet and that superconformal symmetry of every ${\mathcal N}=7$ superconform... | 5.457899 | 4.710521 | 5.636157 | 5.148174 | 4.999369 | 5.071607 | 4.901771 | 5.119067 | 5.163911 | 6.296318 | 4.985445 | 5.038069 | 5.224534 | 5.014765 | 4.949654 | 5.070239 | 5.09652 | 4.8729 | 4.985761 | 5.225869 | 4.934479 |
hep-th/0306182 | Malik Rudra Prakash | R. P. Malik (as-Ictp) | Superfield Approach to (Non-)local Symmetries for One-Form Abelian Gauge
Theory | LaTeX file, 23 pages | J.Phys.A37:1059-1078,2004 | 10.1088/0305-4470/37/3/034 | null | hep-th | null | We exploit the geometrical superfield formalism to derive the local,
covariant and continuous Becchi-Rouet-Stora-Tyutin (BRST) symmetry
transformations and the non-local, non-covariant and continuous dual-BRST
symmetry transformations for the free Abelian one-form gauge theory in four $(3
+ 1)$-dimensions (4D) of spa... | [
{
"created": "Thu, 19 Jun 2003 19:04:40 GMT",
"version": "v1"
},
{
"created": "Sat, 28 Jun 2003 09:33:24 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Oct 2003 16:12:25 GMT",
"version": "v3"
},
{
"created": "Wed, 31 Dec 2003 10:01:53 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Malik",
"R. P.",
"",
"as-Ictp"
]
] | We exploit the geometrical superfield formalism to derive the local, covariant and continuous Becchi-Rouet-Stora-Tyutin (BRST) symmetry transformations and the non-local, non-covariant and continuous dual-BRST symmetry transformations for the free Abelian one-form gauge theory in four $(3 + 1)$-dimensions (4D) of space... | 6.760544 | 4.260861 | 7.582523 | 4.479351 | 4.818533 | 4.564934 | 4.654152 | 4.369276 | 4.900672 | 8.128923 | 4.548538 | 5.351439 | 6.655667 | 5.847992 | 5.828283 | 5.448096 | 5.576906 | 5.652763 | 5.943631 | 6.638463 | 5.670118 |
0806.0603 | Samuel V\'azquez | Samuel E. Vazquez | Constraining Modified Gravity with Large non-Gaussianities | 17 pages, 7 figures, RevTeX format | Phys.Rev.D79:043520,2009 | 10.1103/PhysRevD.79.043520 | null | hep-th astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In writing a covariant effective action for single field inflation, one is
allowed to add a Gauss-Bonnet and axion-type curvature couplings. These
couplings represent modifications of gravity, and are the unique
higher-curvature terms that lead to second order equations of motion in four
dimensions. In this paper we ... | [
{
"created": "Tue, 3 Jun 2008 17:57:03 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jun 2008 14:56:34 GMT",
"version": "v2"
}
] | 2009-03-12 | [
[
"Vazquez",
"Samuel E.",
""
]
] | In writing a covariant effective action for single field inflation, one is allowed to add a Gauss-Bonnet and axion-type curvature couplings. These couplings represent modifications of gravity, and are the unique higher-curvature terms that lead to second order equations of motion in four dimensions. In this paper we st... | 5.960816 | 5.852243 | 6.150075 | 5.867857 | 5.915436 | 5.702569 | 5.808684 | 5.835358 | 5.864836 | 6.36889 | 5.894493 | 5.991423 | 5.933318 | 5.803556 | 5.890632 | 5.922155 | 5.866807 | 6.024122 | 5.86127 | 6.152957 | 5.884899 |
1611.02772 | Christian Saemann | Andreas Deser and Christian Saemann | Extended Riemannian Geometry I: Local Double Field Theory | v2: 50 pages, typos corrected, published version | Ann. Henri Poincare (2018) | 10.1007/s00023-018-0694-2 | ITP-UH-22/16, EMPG-16-18 | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an extended version of Riemannian geometry suitable for the
description of current formulations of double field theory (DFT). This
framework is based on graded manifolds and it yields extended notions of
symmetries, dynamical data and constraints. In special cases, we recover
general relativity with and wi... | [
{
"created": "Tue, 8 Nov 2016 23:27:31 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Jul 2018 12:34:49 GMT",
"version": "v2"
}
] | 2018-07-03 | [
[
"Deser",
"Andreas",
""
],
[
"Saemann",
"Christian",
""
]
] | We present an extended version of Riemannian geometry suitable for the description of current formulations of double field theory (DFT). This framework is based on graded manifolds and it yields extended notions of symmetries, dynamical data and constraints. In special cases, we recover general relativity with and with... | 9.455989 | 8.860445 | 9.687326 | 8.841809 | 9.155458 | 8.697676 | 9.606857 | 8.774315 | 9.284883 | 9.71841 | 8.814298 | 8.742988 | 9.21756 | 8.83169 | 8.930517 | 8.840529 | 8.705905 | 8.994706 | 8.996963 | 9.336897 | 8.657226 |
hep-th/0111243 | Henrik Aratyn | Henrik Aratyn and Johan van de Leur | Integrable Structure behind WDVV Equations | 14 pgs, contribution to Needs 2001 conference proceedings | Theor.Math.Phys. 134 (2003) 14-26; Teor.Mat.Fiz. 134 (2003) 18-31 | null | null | hep-th math-ph math.MP nlin.SI | null | An integrable structure behind Witten--Dijkgraaf--Verlinde--Verlinde (WDVV)
equations is identified with reduction of a Riemann-Hilbert problem for a
homogeneous GL(N, C) loop group. Reduction requires the dressing matrices to be
fixed points of a loop group automorphism of order two resulting in a
sub-hierarchy of g... | [
{
"created": "Tue, 27 Nov 2001 15:12:32 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Aratyn",
"Henrik",
""
],
[
"van de Leur",
"Johan",
""
]
] | An integrable structure behind Witten--Dijkgraaf--Verlinde--Verlinde (WDVV) equations is identified with reduction of a Riemann-Hilbert problem for a homogeneous GL(N, C) loop group. Reduction requires the dressing matrices to be fixed points of a loop group automorphism of order two resulting in a sub-hierarchy of gl(... | 13.530416 | 14.706171 | 16.634434 | 12.863696 | 15.564663 | 14.074463 | 14.788347 | 12.960739 | 13.392031 | 17.039576 | 12.566532 | 11.864736 | 12.625936 | 12.261684 | 11.875119 | 12.930205 | 11.719506 | 12.757685 | 12.274727 | 12.265737 | 11.919857 |
hep-th/0103023 | Garnik G. Alexanian | G.Alexanian, A.P.Balachandran, G.Immirzi and B.Ydri | Fuzzy CP2 | 32 pages,LaTeX; References added and several typos corrected | J.Geom.Phys.42:28-53,2002 | 10.1016/S0393-0440(01)00070-5 | SU-4240-730 | hep-th gr-qc hep-lat math.QA | null | Regularization of quantum field theories (QFT's) can be achieved by
quantizing the underlying manifold (spacetime or spatial slice) thereby
replacing it by a non-commutative matrix model or a ``fuzzy manifold''. Such
discretization by quantization is remarkably successful in preserving
symmetries and topological feat... | [
{
"created": "Mon, 5 Mar 2001 00:53:24 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Apr 2001 22:23:45 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Alexanian",
"G.",
""
],
[
"Balachandran",
"A. P.",
""
],
[
"Immirzi",
"G.",
""
],
[
"Ydri",
"B.",
""
]
] | Regularization of quantum field theories (QFT's) can be achieved by quantizing the underlying manifold (spacetime or spatial slice) thereby replacing it by a non-commutative matrix model or a ``fuzzy manifold''. Such discretization by quantization is remarkably successful in preserving symmetries and topological featur... | 13.651034 | 10.34837 | 14.627284 | 11.79107 | 10.285065 | 10.269151 | 9.577044 | 11.70335 | 10.723924 | 14.726272 | 12.92417 | 11.850572 | 12.33764 | 12.149054 | 11.288931 | 11.776218 | 12.347705 | 12.565493 | 11.591008 | 12.869536 | 12.205362 |
1403.3823 | Seckin Kurkcuoglu | F. Balli, A. Behtash, S. Kurkcuoglu, G. Unal | Quantum Hall Effect on the Grassmannians $\mathbf{Gr}_2(\mathbb{C}^N)$ | 34 pages, revtex 4-1, Minor Corrections | Phys. Rev. D 89, 105031 (2014) | 10.1103/PhysRevD.89.105031 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum Hall Effects (QHEs) on the complex Grassmann manifolds
$\mathbf{Gr}_2(\mathbb{C}^N)$ are formulated. We set up the Landau problem in
$\mathbf{Gr}_2(\mathbb{C}^N)$ and solve it using group theoretical techniques
and provide the energy spectrum and the eigenstates in terms of the $SU(N)$
Wigner ${\cal D}$-funct... | [
{
"created": "Sat, 15 Mar 2014 16:38:45 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Apr 2014 15:30:09 GMT",
"version": "v2"
}
] | 2014-06-11 | [
[
"Balli",
"F.",
""
],
[
"Behtash",
"A.",
""
],
[
"Kurkcuoglu",
"S.",
""
],
[
"Unal",
"G.",
""
]
] | Quantum Hall Effects (QHEs) on the complex Grassmann manifolds $\mathbf{Gr}_2(\mathbb{C}^N)$ are formulated. We set up the Landau problem in $\mathbf{Gr}_2(\mathbb{C}^N)$ and solve it using group theoretical techniques and provide the energy spectrum and the eigenstates in terms of the $SU(N)$ Wigner ${\cal D}$-functio... | 4.635381 | 4.806944 | 5.138936 | 4.43175 | 4.833614 | 5.013209 | 5.018228 | 4.644889 | 4.664019 | 5.361164 | 4.599574 | 4.459308 | 4.680256 | 4.476425 | 4.454905 | 4.426542 | 4.466715 | 4.450788 | 4.477059 | 4.745578 | 4.429851 |
1401.3664 | Kunihito Uzawa | Kunihito Uzawa, Kentaroh Yoshida | Probe brane dynamics on cosmological brane backgrounds | 14 pages, LaTeX, typos corrected, Journal version | Phys.Lett. B738 (2014) 493-498 | 10.1016/j.physletb.2014.10.030 | KUNS-2472 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the dynamics of a single probe brane on various cosmological
brane backgrounds. The on-shell condition of the static probe brane leads to
the supersymmetric intersection rules for static BPS configurations, though the
cosmological backgrounds do not preserve any supersymmetries. This is a
remarkable featu... | [
{
"created": "Wed, 15 Jan 2014 16:55:38 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Oct 2014 05:05:05 GMT",
"version": "v2"
}
] | 2014-10-24 | [
[
"Uzawa",
"Kunihito",
""
],
[
"Yoshida",
"Kentaroh",
""
]
] | We consider the dynamics of a single probe brane on various cosmological brane backgrounds. The on-shell condition of the static probe brane leads to the supersymmetric intersection rules for static BPS configurations, though the cosmological backgrounds do not preserve any supersymmetries. This is a remarkable feature... | 11.048474 | 10.939159 | 11.384703 | 9.786872 | 9.483966 | 9.261642 | 10.058458 | 9.940081 | 9.906969 | 11.343922 | 9.579571 | 9.976094 | 10.185361 | 9.879155 | 9.444663 | 9.706485 | 10.001073 | 9.982918 | 9.931067 | 10.585412 | 9.659425 |
0707.4669 | David Berenstein | David Berenstein, Samuel E. Vazquez | Giant magnon bound states from strongly coupled N=4 SYM | 19 pages, uses revtex | Phys.Rev.D77:026005,2008 | 10.1103/PhysRevD.77.026005 | null | hep-th | null | We calculate in a very simple way the spectrum of giant magnon bound states
at strong coupling in N=4 SYM, by utilizing the description of the field theory
vacuum in terms of a condensate of eigenvalues of commuting matrices. We
further show that these calculations can be understood in terms of the central
charge ext... | [
{
"created": "Tue, 31 Jul 2007 18:21:53 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Berenstein",
"David",
""
],
[
"Vazquez",
"Samuel E.",
""
]
] | We calculate in a very simple way the spectrum of giant magnon bound states at strong coupling in N=4 SYM, by utilizing the description of the field theory vacuum in terms of a condensate of eigenvalues of commuting matrices. We further show that these calculations can be understood in terms of the central charge exten... | 10.607604 | 9.081332 | 10.68961 | 9.170596 | 9.951322 | 9.325244 | 10.149489 | 9.640278 | 9.096129 | 12.095202 | 9.07739 | 9.134113 | 10.096681 | 9.459624 | 9.75655 | 9.60965 | 9.720201 | 9.500162 | 9.207649 | 9.827814 | 9.568466 |
hep-th/0208154 | Calin Iuliu Lazaroiu | L. Anguelova, C.I. Lazaroiu | Domain walls of N=2 supergravity in five dimensions from hypermultiplet
moduli spaces | 39 pages, numerous figures; v4: two references added | JHEP 0209:053,2002 | 10.1088/1126-6708/2002/09/053 | YITP-SB-02-45 | hep-th hep-ph | null | We study domain wall solutions in d=5, N=2 supergravity coupled to a single
hypermultiplet whose moduli space is described by certain inhomogeneous, toric
ESD manifolds constructed recently by Calderbank and Singer. Upon gauging a
generic U(1) isometry of these spaces, we obtain an infinite family of models
whose "su... | [
{
"created": "Wed, 21 Aug 2002 12:23:40 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Aug 2002 01:04:50 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Aug 2002 15:43:47 GMT",
"version": "v3"
},
{
"created": "Fri, 4 Oct 2002 20:51:57 GMT",
"version": "v4"
}
] | 2010-12-03 | [
[
"Anguelova",
"L.",
""
],
[
"Lazaroiu",
"C. I.",
""
]
] | We study domain wall solutions in d=5, N=2 supergravity coupled to a single hypermultiplet whose moduli space is described by certain inhomogeneous, toric ESD manifolds constructed recently by Calderbank and Singer. Upon gauging a generic U(1) isometry of these spaces, we obtain an infinite family of models whose "supe... | 11.279736 | 11.456772 | 13.29624 | 11.073711 | 11.916905 | 12.261374 | 12.89532 | 11.730711 | 11.146344 | 15.256762 | 11.235162 | 10.673705 | 11.501306 | 10.791677 | 10.335713 | 10.38617 | 10.303415 | 10.344828 | 10.81098 | 11.482266 | 10.428576 |
hep-th/9910113 | Shin'ichi Nojiri | Shin'ichi Nojiri and Sergei D. Odintsov | Weyl anomaly from Weyl gravity | LaTeX file, 8 pages | Mod.Phys.Lett.A15:1043-1050,2000 | 10.1142/S0217732300001225 | null | hep-th | null | We calculate the conformal anomaly from 5d Weyl gravity (with broken
conformal symmetry) which is conjectured to be supergravity dual to ${\cal
N}=2$ superconformal field theory via AdS/CFT correspondence. Its comparison
with ${\cal N}=2$ SCFT conformal anomaly (UV calculation) suggests that such
duality may exist su... | [
{
"created": "Fri, 15 Oct 1999 13:27:26 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Nojiri",
"Shin'ichi",
""
],
[
"Odintsov",
"Sergei D.",
""
]
] | We calculate the conformal anomaly from 5d Weyl gravity (with broken conformal symmetry) which is conjectured to be supergravity dual to ${\cal N}=2$ superconformal field theory via AdS/CFT correspondence. Its comparison with ${\cal N}=2$ SCFT conformal anomaly (UV calculation) suggests that such duality may exist subj... | 11.999983 | 10.167804 | 10.700886 | 10.188705 | 10.460111 | 9.425488 | 10.911474 | 10.144534 | 9.814622 | 11.29974 | 9.861012 | 10.260237 | 11.147812 | 11.016859 | 10.952608 | 10.582644 | 10.373311 | 10.235865 | 10.419934 | 10.87044 | 10.401587 |
hep-th/9407154 | Giovanni Felder | Giovanni Felder | Conformal field theory and integrable systems associated with elliptic
curves | 11 pages, LaTeX | Proc. of the ICM 94, 1247-1255, Birkhaeuser 1994 | null | null | hep-th | null | An elliptic version of quantum groups is proposed. It comes form the
quantization of the Knizhnik-Zamolodchikov- Bernard equation on the torus. The
relation with elliptic IRF models is explained.
| [
{
"created": "Sat, 23 Jul 1994 09:37:06 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Felder",
"Giovanni",
""
]
] | An elliptic version of quantum groups is proposed. It comes form the quantization of the Knizhnik-Zamolodchikov- Bernard equation on the torus. The relation with elliptic IRF models is explained. | 11.321669 | 6.935268 | 12.914015 | 7.746743 | 7.588304 | 7.887292 | 7.491972 | 7.513459 | 7.503075 | 10.924588 | 7.918684 | 7.987267 | 10.541296 | 8.437957 | 8.761867 | 9.032843 | 7.902902 | 8.40501 | 8.048803 | 9.787583 | 8.412719 |
hep-th/9509111 | Geza Fulop | G\'eza F\"ul\"op | Gauge fixing, co-BRST and time evolution in QED | Latex, 24 pages, included some new references and comments | Int.J.Mod.Phys. A11 (1996) 4785 | 10.1142/S0217751X96002194 | Goteborg ITP 95-21 | hep-th | null | We consider BRST-invariant inner product states for quantum electrodynamics
constructed from trivial BRST-invariant states and a gauge regulator. The
trivial states are products of matter and ghost states and are annihilated by
hermitian operators. The co-BRST operator and some further gauge-fixing
regulators are fou... | [
{
"created": "Thu, 21 Sep 1995 08:59:49 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Feb 1996 18:08:13 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Fülöp",
"Géza",
""
]
] | We consider BRST-invariant inner product states for quantum electrodynamics constructed from trivial BRST-invariant states and a gauge regulator. The trivial states are products of matter and ghost states and are annihilated by hermitian operators. The co-BRST operator and some further gauge-fixing regulators are found... | 19.706131 | 22.295607 | 19.151373 | 15.9104 | 18.316427 | 17.213547 | 20.709982 | 17.324953 | 18.668777 | 18.223433 | 17.45249 | 19.129948 | 18.811148 | 17.710888 | 18.356476 | 19.571341 | 18.419044 | 19.197752 | 18.076815 | 19.651543 | 17.485851 |
0705.0022 | Michael Gutperle | Eric D'Hoker, John Estes and Michael Gutperle | Exact half-BPS Type IIB interface solutions I: Local solution and
supersymmetric Janus | LaTeX, 69 pages, 3 figures, v2: references added | JHEP 0706:021,2007 | 10.1088/1126-6708/2007/06/021 | UCLA/07/TEP/09 | hep-th | null | The complete Type IIB supergravity solutions with 16 supersymmetries are
obtained on the manifold $AdS_4 \times S^2 \times S^2 \times \Sigma$ with
$SO(2,3) \times SO(3) \times SO(3)$ symmetry in terms of two holomorphic
functions on a Riemann surface $\Sigma$, which generally has a boundary. This
is achieved by reduc... | [
{
"created": "Tue, 1 May 2007 00:15:23 GMT",
"version": "v1"
},
{
"created": "Mon, 21 May 2007 18:26:57 GMT",
"version": "v2"
}
] | 2009-11-13 | [
[
"D'Hoker",
"Eric",
""
],
[
"Estes",
"John",
""
],
[
"Gutperle",
"Michael",
""
]
] | The complete Type IIB supergravity solutions with 16 supersymmetries are obtained on the manifold $AdS_4 \times S^2 \times S^2 \times \Sigma$ with $SO(2,3) \times SO(3) \times SO(3)$ symmetry in terms of two holomorphic functions on a Riemann surface $\Sigma$, which generally has a boundary. This is achieved by reducin... | 6.601133 | 6.162376 | 7.812227 | 6.456155 | 6.301312 | 6.164627 | 6.806648 | 6.311885 | 6.14369 | 8.32335 | 6.108799 | 6.3188 | 7.222137 | 6.238809 | 6.434829 | 6.531115 | 6.414237 | 6.393091 | 6.368367 | 6.745343 | 6.364491 |
1511.05918 | Andre Lehum | A. C. Lehum | Lorentz-violating quantum electrodynamics in two-dimensional
aether-superspace | 9 pages | null | 10.1209/0295-5075/112/51001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The two-dimensional aether-superspace is constructed and the superfield
techniques are applied to the study of dynamical generation of mass in the
Lorentz-violating supersymmetric quantum electrodynamics in two dimensions of
spacetime. It is shown that such model presents a dynamical generation of mass
to the gauge a... | [
{
"created": "Tue, 17 Nov 2015 12:43:34 GMT",
"version": "v1"
}
] | 2016-01-20 | [
[
"Lehum",
"A. C.",
""
]
] | The two-dimensional aether-superspace is constructed and the superfield techniques are applied to the study of dynamical generation of mass in the Lorentz-violating supersymmetric quantum electrodynamics in two dimensions of spacetime. It is shown that such model presents a dynamical generation of mass to the gauge aet... | 11.83217 | 10.723706 | 11.995729 | 8.934185 | 10.675559 | 9.692048 | 9.36049 | 10.190768 | 9.778391 | 13.470052 | 9.806049 | 9.484159 | 11.143663 | 10.185637 | 9.821651 | 9.68682 | 9.221112 | 9.99871 | 9.896526 | 10.914227 | 9.586894 |
1308.1054 | Hoda Farahani | J. Sadeghi and H. Farahani | Thermodynamics of a charged hairy black hole in (2+1) dimensions | 18 pages, 12 figures. References added | null | 10.1007/s10773-014-2122-9 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study thermodynamics, statistics and spectroscopic aspects
of a charged black hole with a scalar hair coupled to the gravity in (2+1)
dimensions. We obtained effects of the black hole charge and scalar field on
the thermodynamical and statistical quantities. We find that scalar charge may
increase en... | [
{
"created": "Mon, 5 Aug 2013 18:11:25 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Aug 2013 18:15:18 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Sadeghi",
"J.",
""
],
[
"Farahani",
"H.",
""
]
] | In this paper we study thermodynamics, statistics and spectroscopic aspects of a charged black hole with a scalar hair coupled to the gravity in (2+1) dimensions. We obtained effects of the black hole charge and scalar field on the thermodynamical and statistical quantities. We find that scalar charge may increase entr... | 10.77881 | 10.565488 | 9.528311 | 9.432536 | 10.303345 | 10.114583 | 9.367188 | 9.416479 | 10.010795 | 10.326316 | 9.785859 | 9.830618 | 10.235636 | 9.940836 | 9.344353 | 9.846188 | 9.752199 | 9.367402 | 9.843007 | 10.138803 | 9.755378 |
hep-th/0104094 | Sergey Alexandrov | Sergei Alexandrov and Vladimir Kazakov | Correlators in 2D string theory with vortex condensation | 20 pages | Nucl.Phys.B610:77,2001; Nucl.Phys.B610:77-96,2001 | 10.1016/S0550-3213(01)00298-X | LPTENS-01/18, SPhT-t01/036 | hep-th | null | We calculate one- and two-point correlators of winding operators in the
matrix model of 2D string theory compactified on a circle, recently proposed
for the description of string dynamics on the 2D black hole background.
| [
{
"created": "Tue, 10 Apr 2001 14:48:02 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Alexandrov",
"Sergei",
""
],
[
"Kazakov",
"Vladimir",
""
]
] | We calculate one- and two-point correlators of winding operators in the matrix model of 2D string theory compactified on a circle, recently proposed for the description of string dynamics on the 2D black hole background. | 9.462908 | 8.121596 | 8.298106 | 7.315704 | 7.783289 | 7.643998 | 7.578531 | 7.067266 | 7.115961 | 9.255585 | 7.108886 | 7.670452 | 8.693103 | 7.680192 | 7.65929 | 7.661662 | 7.772278 | 7.05514 | 7.591338 | 9.051394 | 7.632695 |
1410.0621 | Timothy Olson | Henriette Elvang, Yu-tin Huang, Cynthia Keeler, Thomas Lam, Timothy M.
Olson, Samuel B. Roland, David E. Speyer | Grassmannians for scattering amplitudes in 4d $\mathcal{N}=4$ SYM and 3d
ABJM | 52 pages, 5 figures | null | 10.1007/JHEP12(2014)181 | MCTP-14-36 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Scattering amplitudes in 4d $\mathcal{N}=4$ super Yang-Mills theory (SYM) can
be described by Grassmannian contour integrals whose form depends on whether
the external data is encoded in momentum space, twistor space, or momentum
twistor space. After a pedagogical review, we present a new, streamlined proof
of the eq... | [
{
"created": "Thu, 2 Oct 2014 17:45:50 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Elvang",
"Henriette",
""
],
[
"Huang",
"Yu-tin",
""
],
[
"Keeler",
"Cynthia",
""
],
[
"Lam",
"Thomas",
""
],
[
"Olson",
"Timothy M.",
""
],
[
"Roland",
"Samuel B.",
""
],
[
"Speyer",
"David E.",
""
]
] | Scattering amplitudes in 4d $\mathcal{N}=4$ super Yang-Mills theory (SYM) can be described by Grassmannian contour integrals whose form depends on whether the external data is encoded in momentum space, twistor space, or momentum twistor space. After a pedagogical review, we present a new, streamlined proof of the equi... | 5.880039 | 5.564158 | 6.594725 | 5.604303 | 5.827286 | 5.546672 | 5.717213 | 5.886097 | 5.797432 | 6.677889 | 5.380355 | 5.783937 | 6.002801 | 5.635096 | 5.555518 | 5.749084 | 5.661366 | 5.647445 | 5.564033 | 6.182537 | 5.609796 |
hep-th/0208076 | George Papadopoulos | W. Machin and G. Papadopoulos | Supersymmetric Gauge Theories, Vortices and Equivariant Cohomology | 45 pages, Latex | Class.Quant.Grav.20:1233-1266,2003 | 10.1088/0264-9381/20/7/302 | null | hep-th | null | We construct actions for (p,0)- and (p,1)- supersymmetric, 1 <= p <= 4,
two-dimensional gauge theories coupled to non-linear sigma model matter with a
Wess-Zumino term. We derive the scalar potential for a large class of these
models. We then show that the Euclidean actions of the (2,0) and
(4,0)-supersymmetric model... | [
{
"created": "Sat, 10 Aug 2002 15:45:19 GMT",
"version": "v1"
}
] | 2009-10-09 | [
[
"Machin",
"W.",
""
],
[
"Papadopoulos",
"G.",
""
]
] | We construct actions for (p,0)- and (p,1)- supersymmetric, 1 <= p <= 4, two-dimensional gauge theories coupled to non-linear sigma model matter with a Wess-Zumino term. We derive the scalar potential for a large class of these models. We then show that the Euclidean actions of the (2,0) and (4,0)-supersymmetric models ... | 7.931919 | 6.229336 | 8.015495 | 6.704019 | 6.320659 | 6.135474 | 6.590336 | 6.33972 | 6.377613 | 9.704765 | 6.502821 | 6.892838 | 7.687162 | 7.2349 | 7.125782 | 7.229798 | 7.002904 | 7.011492 | 7.163356 | 7.576511 | 7.094121 |
1011.5872 | Luis Castro | Luis B. Castro and Luis E. Arroyo Meza | Fermion localization on branes with generalized dynamics | 6 pages, 3 figures | EPL 102 (2013) 21001 | 10.1209/0295-5075/102/21001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this letter we consider a specific model of braneworld with nonstandard
dynamics diffused in the literature, specifically we focus our attention on the
matter energy density, the energy of system, the Ricci scalar and the thin
brane limit. As the model is classically stable and capable of localize
gravity, as a na... | [
{
"created": "Fri, 26 Nov 2010 20:41:01 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Mar 2011 17:58:06 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Mar 2013 12:25:58 GMT",
"version": "v3"
}
] | 2015-02-24 | [
[
"Castro",
"Luis B.",
""
],
[
"Meza",
"Luis E. Arroyo",
""
]
] | In this letter we consider a specific model of braneworld with nonstandard dynamics diffused in the literature, specifically we focus our attention on the matter energy density, the energy of system, the Ricci scalar and the thin brane limit. As the model is classically stable and capable of localize gravity, as a natu... | 11.131251 | 8.496868 | 11.318521 | 9.82559 | 9.534483 | 9.665669 | 9.577979 | 9.061522 | 8.689231 | 10.665273 | 9.2663 | 9.852401 | 10.84883 | 10.024356 | 9.804797 | 9.531542 | 10.053329 | 10.022671 | 10.078382 | 10.324371 | 10.44404 |
hep-th/0011200 | Jose Manuel velhinho | J. M. Velhinho | A groupoid approach to spaces of generalized connections | 20 pages, LaTeX, added references | J.Geom.Phys. 41 (2002) 166-180 | 10.1016/S0393-0440(01)00051-1 | null | hep-th | null | The quantum completion of the space of connections in a manifold can be seen
as the set of all morphisms from the groupoid of the edges of the manifold to
the (compact) gauge group. This algebraic construction generalizes an analogous
description of the gauge-invariant quantum configuration space of Ashtekar and
Isha... | [
{
"created": "Wed, 22 Nov 2000 16:01:22 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Jan 2001 12:07:47 GMT",
"version": "v2"
}
] | 2015-06-25 | [
[
"Velhinho",
"J. M.",
""
]
] | The quantum completion of the space of connections in a manifold can be seen as the set of all morphisms from the groupoid of the edges of the manifold to the (compact) gauge group. This algebraic construction generalizes an analogous description of the gauge-invariant quantum configuration space of Ashtekar and Isham,... | 9.673419 | 9.114697 | 9.443179 | 8.505733 | 8.719374 | 8.596298 | 10.490102 | 9.015958 | 10.171895 | 9.950786 | 9.469094 | 9.364429 | 8.909845 | 8.822975 | 9.20421 | 8.933298 | 9.0208 | 8.70749 | 9.084218 | 8.932004 | 8.97095 |
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