id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1302.7310 | Silviu Pufu | Daniel Z. Freedman and Silviu S. Pufu | The Holography of F-maximization | 48 pages; v2 minor improvements | null | 10.1007/JHEP03(2014)135 | SU-ITP-13/01, MIT-CTP-4443 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find new supersymmetric backgrounds of ${\cal N} = 8$ gauged supergravity
in four Euclidean dimensions that are dual to deformations of ABJM theory on
$S^3$. The deformations encode the most general choice of $U(1)_R$ symmetry
used to define the theory on $S^3$. We work within an ${\cal N} = 2$ truncation
of the $... | [
{
"created": "Thu, 28 Feb 2013 20:42:40 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Jan 2014 23:45:28 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"Freedman",
"Daniel Z.",
""
],
[
"Pufu",
"Silviu S.",
""
]
] | We find new supersymmetric backgrounds of ${\cal N} = 8$ gauged supergravity in four Euclidean dimensions that are dual to deformations of ABJM theory on $S^3$. The deformations encode the most general choice of $U(1)_R$ symmetry used to define the theory on $S^3$. We work within an ${\cal N} = 2$ truncation of the ${\... | 5.89232 | 4.794251 | 6.903981 | 4.979492 | 4.481407 | 4.595974 | 4.811185 | 4.614571 | 4.77647 | 6.822477 | 5.011512 | 5.129507 | 5.765416 | 5.037374 | 5.002036 | 5.06269 | 4.941017 | 5.05771 | 5.220634 | 5.683825 | 5.127002 |
1512.01705 | Dirk Kreimer | Spencer Bloch and Dirk Kreimer | Cutkosky Rules and Outer Space | 46 pages, 8 figures | null | null | MaPhy-AvH/2015-17 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive Cutkosky's theorem starting from Pham's classical work. We
emphasize structural relations to Outer Space.
| [
{
"created": "Sat, 5 Dec 2015 21:53:45 GMT",
"version": "v1"
}
] | 2015-12-08 | [
[
"Bloch",
"Spencer",
""
],
[
"Kreimer",
"Dirk",
""
]
] | We derive Cutkosky's theorem starting from Pham's classical work. We emphasize structural relations to Outer Space. | 120.542648 | 101.168358 | 173.731369 | 89.596008 | 119.372055 | 100.761299 | 137.357422 | 104.447151 | 135.698975 | 136.834824 | 94.41198 | 101.860603 | 126.752106 | 102.006805 | 108.76561 | 102.18129 | 94.117477 | 104.807755 | 105.124832 | 129.722305 | 90.28611 |
2203.07957 | Raffaele Marotta | Raffaele Marotta | Soft-Theorems for Scalar Particles: The Dilatons Story | 17 pages, 1 figure; article prepared for Symmetry, Special Issue
"Advances in Theoretical High Energy Physics - Solving Quantum Field Theory" | Symmetry 2022, 14(3), 574 | 10.3390/sym14030574 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We summarize recent results regarding single and double soft theorems of two
different particles named dilatons, the Nambu-Goldstone boson of the
spontaneously broken conformal field theories and the massless scalar particle
of the closed string theories. Similarities and differences between the soft
theorems of thes... | [
{
"created": "Tue, 15 Mar 2022 14:40:51 GMT",
"version": "v1"
}
] | 2022-03-16 | [
[
"Marotta",
"Raffaele",
""
]
] | We summarize recent results regarding single and double soft theorems of two different particles named dilatons, the Nambu-Goldstone boson of the spontaneously broken conformal field theories and the massless scalar particle of the closed string theories. Similarities and differences between the soft theorems of these ... | 7.954059 | 7.479684 | 8.302215 | 7.177988 | 6.550973 | 6.769576 | 7.480071 | 7.613229 | 6.654666 | 9.122791 | 7.427263 | 7.930673 | 7.761601 | 7.472713 | 7.424894 | 8.126381 | 7.618354 | 7.893229 | 7.568962 | 8.181502 | 7.414238 |
1606.06632 | Thomas Mertens | Thomas G. Mertens, Henri Verschelde, Valentin I. Zakharov | String Theory in Polar Coordinates and the Vanishing of the One-Loop
Rindler Entropy | 58 pages + appendices, v2: typos corrected, matches published version | JHEP 1608 (2016) 113 | 10.1007/JHEP08(2016)113 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the string spectrum of flat space in polar coordinates, following
the small curvature limit of the $SL(2,\mathbb{R})/U(1)$ cigar CFT. We first
analyze the partition function of the cigar itself, making some clarifications
of the structure of the spectrum that have escaped attention up to this point.
The su... | [
{
"created": "Tue, 21 Jun 2016 15:56:13 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Aug 2016 16:21:10 GMT",
"version": "v2"
}
] | 2016-08-26 | [
[
"Mertens",
"Thomas G.",
""
],
[
"Verschelde",
"Henri",
""
],
[
"Zakharov",
"Valentin I.",
""
]
] | We analyze the string spectrum of flat space in polar coordinates, following the small curvature limit of the $SL(2,\mathbb{R})/U(1)$ cigar CFT. We first analyze the partition function of the cigar itself, making some clarifications of the structure of the spectrum that have escaped attention up to this point. The supe... | 15.06721 | 16.099169 | 15.207143 | 15.389153 | 15.327152 | 16.044546 | 15.466617 | 15.595298 | 15.427914 | 16.914024 | 15.093356 | 14.204594 | 14.977673 | 14.432787 | 14.253004 | 14.258659 | 14.413059 | 14.391629 | 14.483805 | 14.697224 | 14.27484 |
1405.6651 | Chanju Kim | Chanju Kim | Some Exact Solutions of the Semilocal Popov Equations with Many Flavors | 12 pages | null | 10.3938/jkps.65.12 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In 2+1 dimensional nonrelativistic Chern-Simons gauge theories on $S^2$ which
has a global $SU(M)$ symmetry, the semilocal Popov vortex equations are
obtained as Bogomolny equations by minimizing the energy in the presence of a
uniform external magnetic field. We study the equations with many flavors and
find several... | [
{
"created": "Mon, 26 May 2014 17:25:23 GMT",
"version": "v1"
}
] | 2015-06-19 | [
[
"Kim",
"Chanju",
""
]
] | In 2+1 dimensional nonrelativistic Chern-Simons gauge theories on $S^2$ which has a global $SU(M)$ symmetry, the semilocal Popov vortex equations are obtained as Bogomolny equations by minimizing the energy in the presence of a uniform external magnetic field. We study the equations with many flavors and find several f... | 8.19621 | 6.802728 | 8.520602 | 7.012361 | 7.002965 | 7.318736 | 7.837451 | 6.926283 | 7.133139 | 8.181257 | 7.123388 | 7.464083 | 7.635947 | 7.234503 | 7.392894 | 7.191434 | 7.266209 | 7.466669 | 7.340295 | 7.789227 | 7.503964 |
0811.2305 | Umpei Miyamoto | Kei-ichi Maeda (Waseda Univ.), Umpei Miyamoto (Hebrew Univ.) | Black hole-black string phase transitions from hydrodynamics | 22 pages, 6 figures, 2 tables; v3: Appendix B added | JHEP03(2009)066 | 10.1088/1126-6708/2009/03/066 | WU-AP/294/08 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the phase transitions between three states of a plasma fluid
(plasma ball, uniform plasma tube, and non-uniform plasma tube), which are dual
to the corresponding finite energy black objects (black hole, uniform black
string, and non-uniform black string) localized in an asymptotically locally
AdS space. Ad... | [
{
"created": "Fri, 14 Nov 2008 19:06:39 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Dec 2008 17:54:39 GMT",
"version": "v2"
},
{
"created": "Tue, 24 Feb 2009 08:44:51 GMT",
"version": "v3"
}
] | 2009-11-13 | [
[
"Maeda",
"Kei-ichi",
"",
"Waseda Univ."
],
[
"Miyamoto",
"Umpei",
"",
"Hebrew Univ."
]
] | We discuss the phase transitions between three states of a plasma fluid (plasma ball, uniform plasma tube, and non-uniform plasma tube), which are dual to the corresponding finite energy black objects (black hole, uniform black string, and non-uniform black string) localized in an asymptotically locally AdS space. Adop... | 6.633116 | 6.19333 | 6.972028 | 6.484348 | 6.720439 | 6.439965 | 6.514015 | 6.629172 | 6.115967 | 7.793969 | 6.477971 | 6.424312 | 6.696499 | 6.47718 | 6.516447 | 6.434985 | 6.595778 | 6.467586 | 6.569759 | 6.706741 | 6.361799 |
1905.07413 | Bartlomiej Czech | Bartlomiej Czech, Yaithd D. Olivas, Zi-zhi Wang | Holographic integral geometry with time dependence | 21 pages plus references, 6 figures | null | 10.1007/JHEP12(2020)063 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We write down Crofton formulas--expressions that compute lengths of spacelike
curves in asymptotically AdS$_3$ geometries as integrals over kinematic
space--which apply when the curve and/or the background spacetime is
time-dependent. Relative to their static predecessor, the time-dependent
Crofton formulas display s... | [
{
"created": "Fri, 17 May 2019 18:00:00 GMT",
"version": "v1"
}
] | 2020-12-30 | [
[
"Czech",
"Bartlomiej",
""
],
[
"Olivas",
"Yaithd D.",
""
],
[
"Wang",
"Zi-zhi",
""
]
] | We write down Crofton formulas--expressions that compute lengths of spacelike curves in asymptotically AdS$_3$ geometries as integrals over kinematic space--which apply when the curve and/or the background spacetime is time-dependent. Relative to their static predecessor, the time-dependent Crofton formulas display sev... | 11.620732 | 11.569374 | 13.864573 | 10.21111 | 11.519745 | 11.574409 | 12.546116 | 10.722205 | 9.941393 | 14.136136 | 10.09424 | 10.421777 | 10.751898 | 10.110537 | 10.171855 | 10.308305 | 10.504107 | 10.754406 | 10.042665 | 11.722835 | 9.841249 |
hep-th/0412188 | Matthias Staudacher | Matthias Staudacher | The Factorized S-Matrix of CFT/AdS | 38 pages, LaTeX, JHEP3.cls | JHEP 0505:054,2005 | 10.1088/1126-6708/2005/05/054 | AEI-2004-107, NSF-KITP-04-122 | hep-th | null | We argue that the recently discovered integrability in the large-N CFT/AdS
system is equivalent to diffractionless scattering of the corresponding hidden
elementary excitations. This suggests that, perhaps, the key tool for finding
the spectrum of this system is neither the gauge theory's dilatation operator
nor the ... | [
{
"created": "Fri, 17 Dec 2004 17:43:54 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Staudacher",
"Matthias",
""
]
] | We argue that the recently discovered integrability in the large-N CFT/AdS system is equivalent to diffractionless scattering of the corresponding hidden elementary excitations. This suggests that, perhaps, the key tool for finding the spectrum of this system is neither the gauge theory's dilatation operator nor the st... | 7.328629 | 7.478586 | 8.44842 | 7.084428 | 7.556987 | 7.300436 | 7.129611 | 6.975279 | 7.230547 | 9.543869 | 6.936248 | 7.305554 | 7.636055 | 7.093546 | 7.229263 | 7.053788 | 7.191126 | 7.291126 | 7.103485 | 7.436217 | 6.925158 |
2212.02511 | Giuseppe Bruno De Luca | G. Bruno De Luca, Nicol\`o De Ponti, Andrea Mondino, Alessandro
Tomasiello | Gravity from thermodynamics: optimal transport and negative effective
dimensions | 57 pages + 4 appendices, 4 figures. v2: expanded introduction and
comments on the Casimir vacuum. v3: clarification on the agreement of the
Casimir vacuum with conjectured bounds | SciPost Phys. 15, 039 (2023) | 10.21468/SciPostPhys.15.2.039 | null | hep-th gr-qc math-ph math.DG math.MG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove an equivalence between the classical equations of motion governing
vacuum gravity compactifications (and more general warped-product spacetimes)
and a concavity property of entropy under time evolution. This is obtained by
linking the theory of optimal transport to the Raychaudhuri equation in the
internal s... | [
{
"created": "Mon, 5 Dec 2022 19:00:00 GMT",
"version": "v1"
},
{
"created": "Fri, 12 May 2023 19:19:25 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Dec 2023 22:25:56 GMT",
"version": "v3"
}
] | 2023-12-19 | [
[
"De Luca",
"G. Bruno",
""
],
[
"De Ponti",
"Nicolò",
""
],
[
"Mondino",
"Andrea",
""
],
[
"Tomasiello",
"Alessandro",
""
]
] | We prove an equivalence between the classical equations of motion governing vacuum gravity compactifications (and more general warped-product spacetimes) and a concavity property of entropy under time evolution. This is obtained by linking the theory of optimal transport to the Raychaudhuri equation in the internal spa... | 15.789392 | 17.841185 | 17.36623 | 16.379293 | 17.992128 | 18.278831 | 18.335251 | 16.061857 | 17.718128 | 20.12668 | 15.454254 | 16.260462 | 17.336693 | 16.009459 | 15.949734 | 15.998246 | 15.899615 | 16.188047 | 16.208485 | 16.572006 | 15.219687 |
1005.1700 | Hisham Sati | Hisham Sati | Geometry of Spin and Spin^c structures in the M-theory partition
function | 86 pages, minor changes and improvements, published version (112
pages) | Rev. Math. Phys. 24 (2012) 1250005 | 10.1142/S0129055X12500055 | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the effects of having multiple Spin structures on the partition
function of the spacetime fields in M-theory. This leads to a potential anomaly
which appears in the eta-invariants upon variation of the Spin structure. The
main source of such spaces are manifolds with nontrivial fundamental group,
which are a... | [
{
"created": "Tue, 11 May 2010 01:29:24 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Jun 2010 10:34:19 GMT",
"version": "v2"
},
{
"created": "Sun, 1 Apr 2012 11:13:44 GMT",
"version": "v3"
}
] | 2012-04-03 | [
[
"Sati",
"Hisham",
""
]
] | We study the effects of having multiple Spin structures on the partition function of the spacetime fields in M-theory. This leads to a potential anomaly which appears in the eta-invariants upon variation of the Spin structure. The main source of such spaces are manifolds with nontrivial fundamental group, which are als... | 12.355644 | 13.536724 | 14.633161 | 12.069366 | 13.774916 | 13.455747 | 12.98271 | 13.018854 | 13.029107 | 15.09333 | 11.975635 | 12.681657 | 13.364466 | 12.444715 | 12.293131 | 12.707393 | 12.17455 | 12.464527 | 12.352748 | 13.23647 | 12.144987 |
hep-th/9712116 | Peter Cho | Peter Cho | Moduli in Exceptional SUSY Gauge Theories | 20 pages, harvmac and tables macros | Phys.Rev. D57 (1998) 5214-5223 | 10.1103/PhysRevD.57.5214 | HUTP-97/A099 | hep-th hep-ph | null | The low energy structures of N=1 supersymmetric models with E_6, F_4 and E_7
gauge groups and fundamental irrep matter contents are studied herein. We
identify sets of gauge invariant composites which label all flat directions in
the confining/Higgs phases of these theories. The impossibility of mapping
several of th... | [
{
"created": "Thu, 11 Dec 1997 18:27:47 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Cho",
"Peter",
""
]
] | The low energy structures of N=1 supersymmetric models with E_6, F_4 and E_7 gauge groups and fundamental irrep matter contents are studied herein. We identify sets of gauge invariant composites which label all flat directions in the confining/Higgs phases of these theories. The impossibility of mapping several of thes... | 35.304188 | 28.259508 | 34.10643 | 26.975615 | 30.772486 | 31.171995 | 28.942949 | 34.2477 | 25.784575 | 36.816631 | 28.142334 | 29.440027 | 31.938391 | 29.947012 | 28.817583 | 28.732109 | 28.78557 | 29.40679 | 30.522699 | 32.472034 | 30.015921 |
2005.01731 | Mark Hertzberg | Mark P. Hertzberg, Jacob A. Litterer | Symmetries from Locality. I. Electromagnetism and Charge Conservation | 7 pages in double column format. V2: Further clarifications. Updated
towards version accepted for publication in Phys. Rev. D. V3: Update to
journal title format | Phys. Rev. D 102, 025022 (2020) | 10.1103/PhysRevD.102.025022 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well known that a theory of the (i) Lorentz invariant and (ii) locally
interacting (iii) two degrees of freedom of a massless spin 1 particle, the
photon, leads uniquely to electromagnetism at large distances. In this work, we
remove the assumption of (i) Lorentz boost invariance, but we still demand (ii)
and (... | [
{
"created": "Mon, 4 May 2020 18:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Jul 2020 21:46:46 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Aug 2020 01:23:36 GMT",
"version": "v3"
}
] | 2020-08-12 | [
[
"Hertzberg",
"Mark P.",
""
],
[
"Litterer",
"Jacob A.",
""
]
] | It is well known that a theory of the (i) Lorentz invariant and (ii) locally interacting (iii) two degrees of freedom of a massless spin 1 particle, the photon, leads uniquely to electromagnetism at large distances. In this work, we remove the assumption of (i) Lorentz boost invariance, but we still demand (ii) and (ii... | 11.48747 | 11.744773 | 11.602386 | 11.042706 | 11.631234 | 11.803352 | 11.484113 | 11.412798 | 11.301234 | 13.670387 | 11.345255 | 11.034705 | 10.821974 | 10.733979 | 10.675462 | 10.69885 | 10.960745 | 10.782226 | 10.930072 | 11.288365 | 11.034476 |
hep-th/0205171 | Frank Ferrari | Frank Ferrari (Princeton and Neuchatel Universities) | Four dimensional non-critical strings | 27 pages, 2 figures. Based on a talk given in Les Houches. v2: one
erroneous formula corrected. v3: typos corrected | null | null | PUPT-2027, NEIP-02-003, LPTENS-02/18 | hep-th | null | This is a set of lectures on the gauge/string duality and non-critical
strings, with a particular emphasis on the discretized, or matrix model,
approach. After a general discussion of various points of view, I describe the
recent generalization to four dimensional non-critical (or five dimensional
critical) string th... | [
{
"created": "Thu, 16 May 2002 14:44:45 GMT",
"version": "v1"
},
{
"created": "Fri, 17 May 2002 09:36:56 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Aug 2002 08:57:30 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Ferrari",
"Frank",
"",
"Princeton and Neuchatel Universities"
]
] | This is a set of lectures on the gauge/string duality and non-critical strings, with a particular emphasis on the discretized, or matrix model, approach. After a general discussion of various points of view, I describe the recent generalization to four dimensional non-critical (or five dimensional critical) string theo... | 10.476663 | 10.374565 | 11.471546 | 9.767217 | 10.446039 | 10.656195 | 10.526033 | 10.150626 | 9.807292 | 11.773181 | 9.765288 | 10.490031 | 10.358759 | 10.299007 | 10.457953 | 10.348076 | 10.252146 | 10.440031 | 10.512104 | 10.66581 | 10.088081 |
hep-th/0104215 | Stefan Vandoren | Bernard de Wit, Martin Rocek and Stefan Vandoren | Gauging Isometries on Hyperkahler Cones and Quaternion-Kahler Manifolds | 15 pages | Phys.Lett. B511 (2001) 302-310 | 10.1016/S0370-2693(01)00636-0 | null | hep-th | null | We extend our previous results on the relation between quaternion-Kahler
manifolds and hyperkahler cones and we describe how isometries, moment maps and
scalar potentials descend from the cone to the quaternion-Kahler space. As an
example of the general construction, we discuss the gauging and the
corresponding scala... | [
{
"created": "Tue, 24 Apr 2001 20:18:59 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"de Wit",
"Bernard",
""
],
[
"Rocek",
"Martin",
""
],
[
"Vandoren",
"Stefan",
""
]
] | We extend our previous results on the relation between quaternion-Kahler manifolds and hyperkahler cones and we describe how isometries, moment maps and scalar potentials descend from the cone to the quaternion-Kahler space. As an example of the general construction, we discuss the gauging and the corresponding scalar ... | 10.804276 | 8.550051 | 11.662132 | 8.414478 | 8.197194 | 8.540815 | 7.905674 | 8.948564 | 8.961888 | 12.199349 | 7.721094 | 8.173975 | 9.7807 | 8.563044 | 8.656358 | 8.472433 | 8.200038 | 8.281011 | 8.876985 | 8.950059 | 8.515749 |
2405.20366 | Anatoly Dymarsky | Anatoly Dymarsky and Alfred Shapere | Bulk derivation of TQFT gravity | 28 pages, 2 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We outline a general derivation of holographic duality between "TQFT gravity"
- the path integral of a 3d TQFT summed over different topologies - and an
ensemble of boundary 2d CFTs. The key idea is to place the boundary ensemble on
a Riemann surface of very high genus, where the duality trivializes. The
duality rela... | [
{
"created": "Thu, 30 May 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-06-03 | [
[
"Dymarsky",
"Anatoly",
""
],
[
"Shapere",
"Alfred",
""
]
] | We outline a general derivation of holographic duality between "TQFT gravity" - the path integral of a 3d TQFT summed over different topologies - and an ensemble of boundary 2d CFTs. The key idea is to place the boundary ensemble on a Riemann surface of very high genus, where the duality trivializes. The duality relati... | 10.376131 | 10.038699 | 11.753574 | 9.883485 | 10.458238 | 10.329103 | 10.700294 | 9.752476 | 9.712143 | 12.852037 | 9.274858 | 9.411067 | 9.98315 | 9.628389 | 9.604494 | 9.853538 | 9.303008 | 9.403984 | 9.466224 | 10.287058 | 9.586027 |
2212.13653 | Max Guillen | Max Guillen | Taming the 11D pure spinor b-ghost | 23 pages | null | 10.1007/JHEP03(2023)135 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide an alternative compact expression for the 11D pure spinor b-ghost
by introducing a new set of negative ghost number operators made out of
non-minimal pure spinor variables. Using the algebraic properties satisfied by
these operators, it will be straightforwardly shown that $\{Q, b\}={P^2\over
2}$, as well ... | [
{
"created": "Wed, 28 Dec 2022 00:29:29 GMT",
"version": "v1"
}
] | 2023-04-05 | [
[
"Guillen",
"Max",
""
]
] | We provide an alternative compact expression for the 11D pure spinor b-ghost by introducing a new set of negative ghost number operators made out of non-minimal pure spinor variables. Using the algebraic properties satisfied by these operators, it will be straightforwardly shown that $\{Q, b\}={P^2\over 2}$, as well as... | 12.627778 | 11.011155 | 14.694077 | 11.381321 | 11.451764 | 12.274967 | 11.399184 | 10.741761 | 10.665074 | 15.007892 | 10.897752 | 11.983749 | 13.059667 | 11.474973 | 11.600582 | 11.871238 | 11.81464 | 11.546346 | 11.359775 | 12.453682 | 11.32937 |
2006.10007 | Jose Edelstein | Jose D. Edelstein, David V\'azquez Rodr\'iguez, Alejandro Vilar
L\'opez | Aspects of Geometric Inflation | 20 pages, 3 figures; v2: minor amendments and additions | null | 10.1088/1475-7516/2020/12/040 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the recently proposed mechanism of Geometric Inflation. On general
grounds, we show that obtaining the right amount of inflation demands an
exceedingly large initial energy density. We introduce a scalar field and study
the combined action of both mechanisms. Besides fixing the aforementioned
issue, a casc... | [
{
"created": "Wed, 17 Jun 2020 17:13:11 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Oct 2020 10:12:15 GMT",
"version": "v2"
}
] | 2021-01-06 | [
[
"Edelstein",
"Jose D.",
""
],
[
"Rodríguez",
"David Vázquez",
""
],
[
"López",
"Alejandro Vilar",
""
]
] | We revisit the recently proposed mechanism of Geometric Inflation. On general grounds, we show that obtaining the right amount of inflation demands an exceedingly large initial energy density. We introduce a scalar field and study the combined action of both mechanisms. Besides fixing the aforementioned issue, a cascad... | 16.240784 | 17.455378 | 14.94373 | 14.547379 | 17.306202 | 14.690392 | 17.607836 | 16.805273 | 16.340168 | 16.476046 | 15.536391 | 15.424964 | 15.340636 | 15.657117 | 15.561904 | 15.578483 | 15.741499 | 15.379938 | 15.962481 | 15.387051 | 15.635239 |
1510.02099 | Netta Engelhardt | Raphael Bousso and Netta Engelhardt | Generalized Second Law for Cosmology | 14 pages, 5 figures | Phys. Rev. D 93, 024025 (2016) | 10.1103/PhysRevD.93.024025 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We conjecture a novel Generalized Second Law that can be applied in
cosmology, regardless of whether an event horizon is present: the generalized
entropy increases monotonically outside of certain hypersurfaces we call past
Q-screens. A past Q-screen is foliated by surfaces whose generalized entropy
(sum of area and ... | [
{
"created": "Wed, 7 Oct 2015 20:10:35 GMT",
"version": "v1"
}
] | 2016-01-20 | [
[
"Bousso",
"Raphael",
""
],
[
"Engelhardt",
"Netta",
""
]
] | We conjecture a novel Generalized Second Law that can be applied in cosmology, regardless of whether an event horizon is present: the generalized entropy increases monotonically outside of certain hypersurfaces we call past Q-screens. A past Q-screen is foliated by surfaces whose generalized entropy (sum of area and en... | 9.165778 | 8.847471 | 9.38835 | 8.376753 | 8.144248 | 8.018225 | 9.178794 | 8.579795 | 8.154047 | 11.405684 | 8.872173 | 8.667493 | 8.910542 | 9.09673 | 8.568004 | 8.982107 | 9.225066 | 8.45005 | 8.726722 | 8.840791 | 8.647621 |
hep-th/0010291 | Kurt Lechner | K. Lechner and P.A. Marchetti | Spin-statistics transmutation in relativistic quantum field theories of
dyons | 32 pages, LaTeX, no figures | JHEP 0012 (2000) 028 | 10.1088/1126-6708/2000/12/028 | DFPD/00/TH/33, October 2000 | hep-th | null | We analyse spin and statistics of quantum dyon fields, i.e. fields carrying
both electric and magnetic charge, in 3+1 space-time dimensions. It has been
shown long time ago that, at the quantum mechanical level, a composite dyon
made out of a magnetic pole of charge g and a particle of electric charge e
possesses hal... | [
{
"created": "Tue, 31 Oct 2000 17:36:27 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Lechner",
"K.",
""
],
[
"Marchetti",
"P. A.",
""
]
] | We analyse spin and statistics of quantum dyon fields, i.e. fields carrying both electric and magnetic charge, in 3+1 space-time dimensions. It has been shown long time ago that, at the quantum mechanical level, a composite dyon made out of a magnetic pole of charge g and a particle of electric charge e possesses half-... | 8.771111 | 8.825527 | 9.54335 | 8.956945 | 9.875288 | 9.553319 | 10.15175 | 9.217997 | 8.945083 | 10.029627 | 8.823617 | 9.043634 | 8.725698 | 8.615511 | 8.719036 | 8.70771 | 8.926045 | 8.627432 | 8.738101 | 8.699561 | 8.741187 |
hep-th/9304120 | Reinhard Werner | R.F. Werner | The Free Quon Gas Suffers Gibbs' Paradox | number-of-pages, LaTeX with REVTEX | Phys.Rev. D48 (1993) 2929-2934 | 10.1103/PhysRevD.48.2929 | null | hep-th | null | We consider the Statistical Mechanics of systems of particles satisfying the
$q$-commutation relations recently proposed by Greenberg and others. We show
that although the commutation relations approach Bose (resp.\ Fermi) relations
for $q\to1$ (resp.\ $q\to-1$), the partition functions of free gases are
independent ... | [
{
"created": "Mon, 26 Apr 1993 08:55:50 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Werner",
"R. F.",
""
]
] | We consider the Statistical Mechanics of systems of particles satisfying the $q$-commutation relations recently proposed by Greenberg and others. We show that although the commutation relations approach Bose (resp.\ Fermi) relations for $q\to1$ (resp.\ $q\to-1$), the partition functions of free gases are independent of... | 8.521801 | 9.694685 | 9.885884 | 9.305437 | 10.710365 | 10.164108 | 8.767964 | 9.095445 | 8.770398 | 10.607224 | 8.316021 | 8.19038 | 8.775273 | 8.550956 | 8.482575 | 8.387881 | 8.479094 | 8.442497 | 8.365874 | 8.765341 | 8.44586 |
2202.10499 | Nathan Moynihan | William T. Emond and Nathan Moynihan | Scattering Amplitudes and The Cotton Double Copy | null | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We construct classical curvature spinors in topologically massive gauge
theory and topologically massive gravity, expressed in terms of massive
three-particle amplitudes. We show that when the amplitudes double copy, the
curvature spinors satisfy the Cotton double copy, the three-dimensional cousin
of the Weyl double... | [
{
"created": "Mon, 21 Feb 2022 19:16:25 GMT",
"version": "v1"
}
] | 2022-02-23 | [
[
"Emond",
"William T.",
""
],
[
"Moynihan",
"Nathan",
""
]
] | We construct classical curvature spinors in topologically massive gauge theory and topologically massive gravity, expressed in terms of massive three-particle amplitudes. We show that when the amplitudes double copy, the curvature spinors satisfy the Cotton double copy, the three-dimensional cousin of the Weyl double c... | 9.395135 | 9.787898 | 10.530614 | 8.433595 | 10.645141 | 9.419813 | 8.909128 | 8.861267 | 9.281052 | 12.23278 | 8.874964 | 9.007523 | 9.620986 | 8.929668 | 9.171051 | 8.914584 | 9.650058 | 8.854494 | 8.917392 | 9.666649 | 8.493979 |
1109.3224 | Gonzalo A. Palma | Vicente Atal, Luis E. Campusano, Gonzalo A. Palma | Bigravitational inflation | 5 pages, v2: discussion changed, published version | Phys. Rev. D 86, 123521 (2012) | 10.1103/PhysRevD.86.123521 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the realization of cosmic inflation in bigravity theories. By
analyzing the evolution of scalar, vector, and tensor perturbations in de
Sitter-like spacetimes, we find strong stability constraints on the class of
viable vacua offered by these theories. More specifically, the only stable de
Sitter vacua conta... | [
{
"created": "Wed, 14 Sep 2011 23:03:21 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Dec 2012 03:51:27 GMT",
"version": "v2"
}
] | 2012-12-21 | [
[
"Atal",
"Vicente",
""
],
[
"Campusano",
"Luis E.",
""
],
[
"Palma",
"Gonzalo A.",
""
]
] | We study the realization of cosmic inflation in bigravity theories. By analyzing the evolution of scalar, vector, and tensor perturbations in de Sitter-like spacetimes, we find strong stability constraints on the class of viable vacua offered by these theories. More specifically, the only stable de Sitter vacua contain... | 7.650173 | 8.450929 | 7.265917 | 7.154648 | 8.275271 | 7.77812 | 8.274342 | 8.013514 | 7.943624 | 8.371269 | 7.868792 | 7.558379 | 7.341735 | 7.44213 | 7.440758 | 7.729487 | 7.719848 | 7.396895 | 7.393751 | 7.135516 | 7.656863 |
hep-th/0101122 | Niels Obers | N.A. Obers (Spinoza, ITF), B. Pioline (Harvard, LPTHE) | Exact Thresholds and Instanton Effects in String Theory | 24 pages, latex, contribution to the proceedings of the First
Workshop of the RTN Network "The Quantum Structure of Spacetime and the
Geometric Nature of Fundamental Interactions", Berlin, Germany, 4-10 October
2000 | Fortsch.Phys. 49 (2001) 359-375 | 10.1002/1521-3978(200105)49:4/6<359::AID-PROP359>3.3.CO;2-U | SPIN-01/01, ITP-UU-01/01, HUTP-00/A053, LPTHE-01-51 | hep-th | null | In this lecture we summarize some recent work on the understanding of
instanton effects in string theories with 16 supersymmetries. In particular, we
consider F^4 couplings using the duality between the heterotic string on T^4
and type IIA on K_3 at an orbifold point, as well as higher and lower
dimensional versions ... | [
{
"created": "Thu, 18 Jan 2001 14:03:56 GMT",
"version": "v1"
}
] | 2015-06-25 | [
[
"Obers",
"N. A.",
"",
"Spinoza, ITF"
],
[
"Pioline",
"B.",
"",
"Harvard, LPTHE"
]
] | In this lecture we summarize some recent work on the understanding of instanton effects in string theories with 16 supersymmetries. In particular, we consider F^4 couplings using the duality between the heterotic string on T^4 and type IIA on K_3 at an orbifold point, as well as higher and lower dimensional versions of... | 6.467788 | 5.421067 | 7.790095 | 5.593271 | 5.594689 | 5.823458 | 6.066472 | 5.755116 | 5.639959 | 7.287131 | 5.826755 | 5.665405 | 6.305034 | 5.957391 | 5.932942 | 5.92782 | 5.902224 | 6.037661 | 5.836983 | 6.423182 | 5.832289 |
2109.00073 | Prahar Mitra | Daniel Kapec and Prahar Mitra | Shadows and Soft Exchange in Celestial CFT | 43 pages, 1 figure | null | 10.1103/PhysRevD.105.026009 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study exponentiated soft exchange in $d+2$ dimensional gauge and
gravitational theories using the celestial CFT formalism. These models exhibit
spontaneously broken asymptotic symmetries generated by gauge transformations
with non-compact support, and the effective dynamics of the associated
Goldstone "edge" mode ... | [
{
"created": "Tue, 31 Aug 2021 20:47:13 GMT",
"version": "v1"
}
] | 2022-01-19 | [
[
"Kapec",
"Daniel",
""
],
[
"Mitra",
"Prahar",
""
]
] | We study exponentiated soft exchange in $d+2$ dimensional gauge and gravitational theories using the celestial CFT formalism. These models exhibit spontaneously broken asymptotic symmetries generated by gauge transformations with non-compact support, and the effective dynamics of the associated Goldstone "edge" mode is... | 9.768758 | 9.229859 | 10.850555 | 9.178485 | 9.420238 | 9.276376 | 9.418515 | 9.6032 | 8.959845 | 10.72679 | 9.23116 | 9.556538 | 10.146624 | 9.473742 | 9.642956 | 9.486377 | 9.355905 | 9.294482 | 9.403787 | 10.134582 | 9.596487 |
hep-th/0212014 | Brett McInnes | Brett McInnes | The Covariant Entropy Bound, Brane Cosmology, and the Null Energy
Condition | 21 pages, 3 figures, version 2:corrected and greatly improved
discussion of the Bousso-Randall consistency check, references added;
version3: more references added, JHEP version | JHEP 0212:053,2002 | 10.1088/1126-6708/2002/12/053 | null | hep-th astro-ph gr-qc | null | In discussions of Bousso's Covariant Entropy Bound, the Null Energy Condition
is always assumed, as a sufficient {\em but not necessary} condition which
helps to ensure that the entropy on any lightsheet shall necessarily be finite.
The spectacular failure of the Strong Energy Condition in cosmology has,
however, l... | [
{
"created": "Mon, 2 Dec 2002 13:20:41 GMT",
"version": "v1"
},
{
"created": "Sat, 14 Dec 2002 08:28:21 GMT",
"version": "v2"
},
{
"created": "Sat, 21 Dec 2002 08:33:48 GMT",
"version": "v3"
}
] | 2010-12-23 | [
[
"McInnes",
"Brett",
""
]
] | In discussions of Bousso's Covariant Entropy Bound, the Null Energy Condition is always assumed, as a sufficient {\em but not necessary} condition which helps to ensure that the entropy on any lightsheet shall necessarily be finite. The spectacular failure of the Strong Energy Condition in cosmology has, however, led m... | 9.07366 | 9.041164 | 9.436171 | 9.20423 | 9.462437 | 8.927882 | 9.618532 | 9.384147 | 9.480837 | 10.284584 | 9.323223 | 8.751887 | 8.949191 | 8.796183 | 8.645996 | 8.743631 | 8.855289 | 8.556111 | 8.80788 | 9.077647 | 8.766894 |
1805.04504 | Arthur Lipstein | Joseph A. Farrow and Arthur E. Lipstein | New Worldsheet Formulae for Conformal Supergravity Amplitudes | v3. minor changes, published in JHEP | null | 10.1007/JHEP07(2018)074 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use 4d ambitwistor string theory to derive new worldsheet formulae for
tree-level conformal supergravity amplitudes supported on refined scattering
equations. Unlike the worldsheet formulae for super-Yang-Mills or supergravity,
the scattering equations for conformal supergravity are not in general refined
by MHV d... | [
{
"created": "Fri, 11 May 2018 17:43:08 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jun 2018 13:59:20 GMT",
"version": "v2"
},
{
"created": "Wed, 11 Jul 2018 16:07:49 GMT",
"version": "v3"
}
] | 2018-07-12 | [
[
"Farrow",
"Joseph A.",
""
],
[
"Lipstein",
"Arthur E.",
""
]
] | We use 4d ambitwistor string theory to derive new worldsheet formulae for tree-level conformal supergravity amplitudes supported on refined scattering equations. Unlike the worldsheet formulae for super-Yang-Mills or supergravity, the scattering equations for conformal supergravity are not in general refined by MHV deg... | 10.388181 | 10.484306 | 12.771925 | 9.317615 | 9.816195 | 9.903738 | 9.58486 | 9.141627 | 9.626656 | 12.701898 | 9.531433 | 9.548899 | 10.216492 | 9.367319 | 9.286898 | 9.297688 | 9.38922 | 9.521519 | 9.325604 | 10.812646 | 9.60538 |
1801.03245 | Arjun Bagchi | Arjun Bagchi, Rudranil Basu, St\'ephane Detournay, and Pulastya Parekh | Flatspace Chiral Supergravity | 30 pages | Phys. Rev. D 97, 106020 (2018) | 10.1103/PhysRevD.97.106020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a holographic duality between a 2 dimensional (2d) chiral
superconformal field theory and a certain theory of supergravity in 3d with
flatspace boundary conditions that is obtained as a double scaling limit of a
parity breaking theory of supergravity. We show how the asymptotic symmetries
of the bulk theor... | [
{
"created": "Wed, 10 Jan 2018 06:00:33 GMT",
"version": "v1"
}
] | 2018-05-30 | [
[
"Bagchi",
"Arjun",
""
],
[
"Basu",
"Rudranil",
""
],
[
"Detournay",
"Stéphane",
""
],
[
"Parekh",
"Pulastya",
""
]
] | We propose a holographic duality between a 2 dimensional (2d) chiral superconformal field theory and a certain theory of supergravity in 3d with flatspace boundary conditions that is obtained as a double scaling limit of a parity breaking theory of supergravity. We show how the asymptotic symmetries of the bulk theory ... | 8.410734 | 8.703397 | 10.442135 | 8.782959 | 8.554358 | 9.163825 | 8.519242 | 9.059388 | 8.743757 | 11.718885 | 9.014866 | 8.3645 | 10.126287 | 8.307278 | 9.124138 | 8.833804 | 8.32283 | 8.688273 | 8.570276 | 9.305485 | 8.491046 |
0807.5113 | Maxim Zabzine | Giulio Bonelli, Alessandro Tanzini and Maxim Zabzine | Topological branes, p-algebras and generalized Nahm equations | 20 pages | Phys.Lett.B672:390-395,2009 | 10.1016/j.physletb.2009.01.051 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inspired by the recent advances in multiple M2-brane theory, we consider the
generalizations of Nahm equations for arbitrary p-algebras. We construct the
topological p-algebra quantum mechanics associated to them and we show that
this can be obtained as a truncation of the topological p-brane theory
previously studie... | [
{
"created": "Thu, 31 Jul 2008 17:13:33 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Aug 2008 13:15:12 GMT",
"version": "v2"
}
] | 2009-02-24 | [
[
"Bonelli",
"Giulio",
""
],
[
"Tanzini",
"Alessandro",
""
],
[
"Zabzine",
"Maxim",
""
]
] | Inspired by the recent advances in multiple M2-brane theory, we consider the generalizations of Nahm equations for arbitrary p-algebras. We construct the topological p-algebra quantum mechanics associated to them and we show that this can be obtained as a truncation of the topological p-brane theory previously studied ... | 6.797599 | 6.224219 | 8.291481 | 5.866171 | 6.057057 | 6.076983 | 6.322603 | 5.984034 | 6.01033 | 7.136436 | 6.18144 | 5.820664 | 6.611038 | 6.002858 | 5.969771 | 6.026492 | 6.102739 | 5.933875 | 6.113877 | 6.768795 | 6.122243 |
hep-th/0310151 | Muhammad Sharif | M. Sharif | Energy of a Regular Black Hole | Latex, 10 pages, 2 figures | Nuovo Cim. B119 (2004) 463-469 | 10.1393/ncb/i2004-10012-3 | null | hep-th gr-qc | null | We use Einstein, Landau-Lifshitz, Papapetrou and Weinberg energy-momentum
complexes to evaluate energy distribution of a regular black hole. It is shown
that for a regular black hole, these energy-momentum complexes give the same
energy distribution. This supports Cooperstock hypothesis and also
Aguirregabbiria et al... | [
{
"created": "Thu, 16 Oct 2003 07:40:33 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Sharif",
"M.",
""
]
] | We use Einstein, Landau-Lifshitz, Papapetrou and Weinberg energy-momentum complexes to evaluate energy distribution of a regular black hole. It is shown that for a regular black hole, these energy-momentum complexes give the same energy distribution. This supports Cooperstock hypothesis and also Aguirregabbiria et al. ... | 10.81412 | 13.257634 | 7.179715 | 7.752225 | 9.008348 | 9.367424 | 14.587602 | 7.728743 | 11.459638 | 7.706839 | 10.289575 | 11.238316 | 8.660141 | 9.170165 | 10.205967 | 10.33852 | 12.212986 | 9.04795 | 10.550257 | 9.097828 | 10.559112 |
0808.0351 | Don N. Page | Don N. Page | Cosmological Measures without Volume Weighting | 15 pages, LaTeX, added references for constant-H hypersurfaces and
also an idea for minimal-flux hypersurfaces | JCAP 0810:025,2008 | 10.1088/1475-7516/2008/10/025 | Alberta-Thy-16-08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many cosmologists (myself included) have advocated volume weighting for the
cosmological measure problem, weighting spatial hypersurfaces by their volume.
However, this often leads to the Boltzmann brain problem, that almost all
observations would be by momentary Boltzmann brains that arise very briefly as
quantum fl... | [
{
"created": "Sun, 3 Aug 2008 21:00:01 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Aug 2008 16:20:16 GMT",
"version": "v2"
},
{
"created": "Wed, 10 Sep 2008 23:56:03 GMT",
"version": "v3"
},
{
"created": "Tue, 16 Sep 2008 23:19:12 GMT",
"version": "v4"
}
] | 2009-03-27 | [
[
"Page",
"Don N.",
""
]
] | Many cosmologists (myself included) have advocated volume weighting for the cosmological measure problem, weighting spatial hypersurfaces by their volume. However, this often leads to the Boltzmann brain problem, that almost all observations would be by momentary Boltzmann brains that arise very briefly as quantum fluc... | 14.074321 | 15.648395 | 18.196255 | 13.609902 | 16.630022 | 15.327902 | 15.499929 | 13.878767 | 13.083115 | 17.371489 | 13.865974 | 14.461139 | 13.940992 | 14.271369 | 14.137325 | 13.587832 | 13.242009 | 13.423204 | 13.853699 | 14.873278 | 13.873487 |
hep-th/0008191 | Eric R. Sharpe | Eric R. Sharpe | Recent Developments in Discrete Torsion | 12 pages, LaTeX, 2 figures | Phys.Lett. B498 (2001) 104-110 | 10.1016/S0370-2693(00)01376-9 | DUKE-CGTP-2000-16 | hep-th | null | In this short note we briefly review some recent developments in
understanding discrete torsion. Specifically, we give a short overview of the
highlights of a group of recent papers which give the basic understanding of
discrete torsion. Briefly, those papers observe that discrete torsion can be
completely understood... | [
{
"created": "Thu, 24 Aug 2000 13:55:20 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Sharpe",
"Eric R.",
""
]
] | In this short note we briefly review some recent developments in understanding discrete torsion. Specifically, we give a short overview of the highlights of a group of recent papers which give the basic understanding of discrete torsion. Briefly, those papers observe that discrete torsion can be completely understood s... | 11.528119 | 10.926826 | 11.90517 | 10.319511 | 10.618119 | 10.825066 | 10.281397 | 10.874352 | 9.802202 | 11.921833 | 9.996403 | 10.435863 | 11.086888 | 10.521478 | 10.386531 | 10.711162 | 10.433946 | 10.270576 | 10.509733 | 10.369021 | 10.281293 |
1512.06805 | Andreas Nink | Andreas Nink and Martin Reuter | The unitary conformal field theory behind 2D Asymptotic Safety | 64 pages | JHEP 1602 (2016) 167 | 10.1007/JHEP02(2016)167 | MITP/15-113 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Being interested in the compatibility of Asymptotic Safety with Hilbert space
positivity (unitarity), we consider a local truncation of the functional RG
flow which describes quantum gravity in $d>2$ dimensions and construct its
limit of exactly two dimensions. We find that in this limit the flow displays a
nontrivia... | [
{
"created": "Mon, 21 Dec 2015 20:29:48 GMT",
"version": "v1"
}
] | 2016-03-09 | [
[
"Nink",
"Andreas",
""
],
[
"Reuter",
"Martin",
""
]
] | Being interested in the compatibility of Asymptotic Safety with Hilbert space positivity (unitarity), we consider a local truncation of the functional RG flow which describes quantum gravity in $d>2$ dimensions and construct its limit of exactly two dimensions. We find that in this limit the flow displays a nontrivial ... | 6.626189 | 7.695837 | 7.539255 | 7.016236 | 7.164741 | 7.409186 | 7.158955 | 7.414231 | 7.146103 | 8.608842 | 7.245924 | 6.475701 | 6.803942 | 6.58641 | 6.552713 | 6.77962 | 6.647736 | 6.653728 | 6.631583 | 6.683867 | 6.674747 |
1907.09482 | Washington Taylor | Yu-Chien Huang and Washington Taylor | Fibration structure in toric hypersurface Calabi-Yau threefolds | 14 pages, 4 figures; v2: minor changes, comments added | null | 10.1007/JHEP03(2020)172 | MIT-CTP-5132 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find through a systematic analysis that all but 29,223 of the 473.8
million 4D reflexive polytopes found by Kreuzer and Skarke have a 2D reflexive
subpolytope. Such a subpolytope is generally associated with the presence of an
elliptic or genus one fibration in the corresponding birational equivalence
class of Cal... | [
{
"created": "Mon, 22 Jul 2019 18:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Sep 2019 14:25:37 GMT",
"version": "v2"
}
] | 2020-04-22 | [
[
"Huang",
"Yu-Chien",
""
],
[
"Taylor",
"Washington",
""
]
] | We find through a systematic analysis that all but 29,223 of the 473.8 million 4D reflexive polytopes found by Kreuzer and Skarke have a 2D reflexive subpolytope. Such a subpolytope is generally associated with the presence of an elliptic or genus one fibration in the corresponding birational equivalence class of Calab... | 9.747377 | 6.872142 | 10.607654 | 7.464455 | 7.122708 | 7.859691 | 7.474153 | 7.415768 | 7.046533 | 12.717312 | 7.333723 | 7.40212 | 9.226385 | 7.741776 | 7.533702 | 7.61754 | 7.530538 | 7.29197 | 7.683837 | 9.352682 | 7.466316 |
2109.11556 | Martin Wolfgang Winkler | Katherine Freese, Aliki Litsa, Martin Wolfgang Winkler | Natural Chain Inflation | 7 pages, 4 figures | null | 10.1016/j.physletb.2022.137081 | UTTG-18-2021, NORDITA-2021-078 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In Chain Inflation the universe tunnels along a series of false vacua of
ever-decreasing energy. The main goal of this paper is to embed Chain Inflation
in high energy fundamental physics. We begin by illustrating a simple effective
formalism for calculating Cosmic Microwave Background (CMB) observables in
Chain Infl... | [
{
"created": "Thu, 23 Sep 2021 18:00:01 GMT",
"version": "v1"
}
] | 2022-04-20 | [
[
"Freese",
"Katherine",
""
],
[
"Litsa",
"Aliki",
""
],
[
"Winkler",
"Martin Wolfgang",
""
]
] | In Chain Inflation the universe tunnels along a series of false vacua of ever-decreasing energy. The main goal of this paper is to embed Chain Inflation in high energy fundamental physics. We begin by illustrating a simple effective formalism for calculating Cosmic Microwave Background (CMB) observables in Chain Inflat... | 9.62829 | 9.561089 | 9.166189 | 8.957627 | 9.663589 | 9.177208 | 9.25779 | 9.101206 | 9.014107 | 9.983115 | 9.457592 | 8.948572 | 9.32646 | 8.954452 | 9.176342 | 8.924974 | 8.974977 | 9.288921 | 9.022942 | 9.472434 | 9.022523 |
hep-th/9706117 | Tomas Ortin Miguel | Eric Bergshoeff, Bert Janssen, Tomas Ortin | Kaluza-Klein Monopoles and Gauged Sigma-Models | Latex file. References added. Version to be published in Physics
Letters B | Phys.Lett.B410:131-141,1997 | 10.1016/S0370-2693(97)00946-5 | CERN-TH/97-125, UG-5/97 | hep-th | null | We propose an effective action for the eleven-dimensional (bosonic)
Kaluza-Klein monopole solution. The construction of the action requires that
the background fields admit an Abelian isometry group. The corresponding
sigma-model is gauged with respect to this isometry. The gauged sigma-model is
the source for the mo... | [
{
"created": "Sun, 15 Jun 1997 16:05:21 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Jul 1997 13:29:01 GMT",
"version": "v2"
},
{
"created": "Thu, 31 Jul 1997 13:32:01 GMT",
"version": "v3"
}
] | 2008-12-18 | [
[
"Bergshoeff",
"Eric",
""
],
[
"Janssen",
"Bert",
""
],
[
"Ortin",
"Tomas",
""
]
] | We propose an effective action for the eleven-dimensional (bosonic) Kaluza-Klein monopole solution. The construction of the action requires that the background fields admit an Abelian isometry group. The corresponding sigma-model is gauged with respect to this isometry. The gauged sigma-model is the source for the mono... | 6.107273 | 5.806162 | 6.611985 | 5.798544 | 5.787276 | 5.493543 | 5.638298 | 5.488487 | 5.518663 | 6.611782 | 5.592948 | 5.748045 | 6.201317 | 5.796437 | 5.798639 | 5.465826 | 5.771981 | 5.682473 | 5.846542 | 6.131912 | 5.746185 |
2111.07107 | Akihiro Miyata | Norihiro Iizuka, Akihiro Miyata, Tomonori Ugajin | A comment on a fine-grained description of evaporating black holes with
baby universes | 27 Pages, 5 figures; v2: typos corrected, references added | null | 10.1007/JHEP09(2022)158 | OU-HET-1119, UT-Komaba/21-6, YITP-21-133 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We study a partially fine-grained description of an evaporating black hole by
introducing an open baby universe with a boundary. Since the Page's calculation
of the entropy of Hawking radiation involves an ensemble average over a class
of states, one can formally obtain a fine-grained state by purifying this
setup. F... | [
{
"created": "Sat, 13 Nov 2021 12:41:42 GMT",
"version": "v1"
},
{
"created": "Mon, 16 May 2022 05:00:28 GMT",
"version": "v2"
}
] | 2022-10-19 | [
[
"Iizuka",
"Norihiro",
""
],
[
"Miyata",
"Akihiro",
""
],
[
"Ugajin",
"Tomonori",
""
]
] | We study a partially fine-grained description of an evaporating black hole by introducing an open baby universe with a boundary. Since the Page's calculation of the entropy of Hawking radiation involves an ensemble average over a class of states, one can formally obtain a fine-grained state by purifying this setup. For... | 14.201241 | 13.454412 | 15.791068 | 12.833451 | 13.543365 | 12.527622 | 14.723412 | 13.105277 | 13.57278 | 14.36062 | 12.865812 | 13.006004 | 14.737104 | 13.474216 | 14.441809 | 14.689803 | 13.933513 | 13.733411 | 13.597451 | 14.996439 | 14.251506 |
2302.00655 | Lucas Pinol | Denis Werth, Lucas Pinol, S\'ebastien Renaux-Petel | Cosmological Flow of Primordial Correlators | v2: minor modifications, 6 pages, 3 figures | null | null | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Correlation functions of primordial density fluctuations provide an exciting
probe of the physics governing the earliest moments of our Universe. However,
the standard approach to compute them is technically challenging. Theoretical
predictions are therefore available only in restricted classes of theories. In
this L... | [
{
"created": "Wed, 1 Feb 2023 18:30:34 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jun 2023 15:56:02 GMT",
"version": "v2"
}
] | 2023-06-14 | [
[
"Werth",
"Denis",
""
],
[
"Pinol",
"Lucas",
""
],
[
"Renaux-Petel",
"Sébastien",
""
]
] | Correlation functions of primordial density fluctuations provide an exciting probe of the physics governing the earliest moments of our Universe. However, the standard approach to compute them is technically challenging. Theoretical predictions are therefore available only in restricted classes of theories. In this Let... | 11.902986 | 12.13276 | 12.209294 | 10.962883 | 11.655027 | 11.9522 | 11.253647 | 10.836995 | 11.130947 | 12.355538 | 10.940185 | 10.923663 | 11.047359 | 10.986594 | 10.943851 | 11.114407 | 11.214439 | 10.926873 | 11.001925 | 11.284606 | 10.897079 |
hep-th/0610335 | Anirban Basu | Anirban Basu | The D^{10} R^4 term in type IIB string theory | 12 pages, LaTeX | Phys.Lett.B648:378-382,2007 | 10.1016/j.physletb.2007.03.024 | null | hep-th | null | The modular invariant coefficient of the D^{2k} {\cal{R}}^4 term in the
effective action of type IIB superstring theory is expected to satisfy Poisson
equation on the fundamental domain of SL(2,Z). Under certain assumptions, we
obtain the equation satisfied by D^{10} {\cal{R}}^4 using the tree level and
one loop resu... | [
{
"created": "Tue, 31 Oct 2006 20:47:42 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Nov 2006 23:35:56 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Basu",
"Anirban",
""
]
] | The modular invariant coefficient of the D^{2k} {\cal{R}}^4 term in the effective action of type IIB superstring theory is expected to satisfy Poisson equation on the fundamental domain of SL(2,Z). Under certain assumptions, we obtain the equation satisfied by D^{10} {\cal{R}}^4 using the tree level and one loop result... | 7.343295 | 5.839265 | 7.491026 | 6.135328 | 6.238673 | 5.856891 | 5.873238 | 6.039909 | 5.787597 | 7.882817 | 5.640234 | 6.704874 | 7.696578 | 6.83442 | 6.762037 | 6.689732 | 6.743767 | 7.000603 | 6.897292 | 7.675497 | 6.78236 |
1901.04501 | Christoph Adam | C. Adam, Jose M. Queiruga, A. Wereszczynski | BPS soliton-impurity models and supersymmetry | LaTex file, 25 pages | null | 10.1007/JHEP07(2019)164 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find supersymmetric extensions of the half-BPS soliton-impurity models in
(1+1) dimensions which preserve half of the $\mathcal{N}=1$ supersymmetry. This
is related to the fact that in the bosonic sector (i.e., the half-BPS
soliton-impurity model), only one soliton (for example, the kink) is a BPS
configuration wh... | [
{
"created": "Mon, 14 Jan 2019 19:00:02 GMT",
"version": "v1"
}
] | 2019-09-04 | [
[
"Adam",
"C.",
""
],
[
"Queiruga",
"Jose M.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | We find supersymmetric extensions of the half-BPS soliton-impurity models in (1+1) dimensions which preserve half of the $\mathcal{N}=1$ supersymmetry. This is related to the fact that in the bosonic sector (i.e., the half-BPS soliton-impurity model), only one soliton (for example, the kink) is a BPS configuration whic... | 5.289197 | 5.529874 | 5.730767 | 5.448963 | 5.385453 | 5.604886 | 5.507775 | 5.286128 | 5.424931 | 6.578259 | 5.145347 | 5.336903 | 5.414101 | 5.169713 | 5.173988 | 5.067336 | 5.244013 | 5.208908 | 5.163792 | 5.371588 | 5.097248 |
2112.13564 | Yoshihisa Kitazawa | Yoshihisa Kitazawa | de Sitter Duality and Holographic Renormalization | 10 pages, Contribution to the proceedings of EAJS at Osaka City
University, | null | null | KEK-TH-2382 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We perform the resummation of the infrared logarithms in the inflationary
universe. Applying the renormalization group, we derive the stochastic
equations as the effective theory at the horizon. We focus on the conformal
zero mode to respect local Lorentz symmetry.
Under Gaussian approximation, we derive the fundam... | [
{
"created": "Mon, 27 Dec 2021 08:23:53 GMT",
"version": "v1"
}
] | 2021-12-28 | [
[
"Kitazawa",
"Yoshihisa",
""
]
] | We perform the resummation of the infrared logarithms in the inflationary universe. Applying the renormalization group, we derive the stochastic equations as the effective theory at the horizon. We focus on the conformal zero mode to respect local Lorentz symmetry. Under Gaussian approximation, we derive the fundamenta... | 19.21056 | 22.233707 | 20.152716 | 19.109646 | 19.647921 | 19.509508 | 18.714848 | 19.199062 | 19.38479 | 21.90357 | 18.677633 | 18.78063 | 18.325682 | 18.639246 | 19.265732 | 19.077593 | 18.326855 | 18.931362 | 19.148558 | 18.876976 | 18.630135 |
1804.04592 | Junho Hong | Junho Hong, James T. Liu | The topologically twisted index of $\mathcal N=4$ super-Yang-Mills on
$T^2\times S^2$ and the elliptic genus | 29 pages, 1 figure; v2: restricted to real chemical potentials in
section 4 and added a comment on the index where $c_r(\mathfrak n_a)<0$ in
section 5 | null | 10.1007/JHEP07(2018)018 | LCTP-18-12 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the topologically twisted index of $\mathcal N=4$ super-Yang-Mills
with gauge group $SU(N)$ on $T^2\times S^2$, and demonstrate that it receives
contributions from multiple sectors corresponding to the freely acting
orbifolds $T^2/\mathbb Z_m\times\mathbb Z_n$ where $N=mn$. After summing over
these sectors... | [
{
"created": "Thu, 12 Apr 2018 16:03:48 GMT",
"version": "v1"
},
{
"created": "Fri, 4 May 2018 17:48:47 GMT",
"version": "v2"
}
] | 2018-08-01 | [
[
"Hong",
"Junho",
""
],
[
"Liu",
"James T.",
""
]
] | We examine the topologically twisted index of $\mathcal N=4$ super-Yang-Mills with gauge group $SU(N)$ on $T^2\times S^2$, and demonstrate that it receives contributions from multiple sectors corresponding to the freely acting orbifolds $T^2/\mathbb Z_m\times\mathbb Z_n$ where $N=mn$. After summing over these sectors, ... | 4.858231 | 4.512288 | 5.532282 | 4.259058 | 4.352147 | 4.518019 | 4.404824 | 4.294879 | 4.361265 | 5.462908 | 4.268235 | 4.437743 | 4.846817 | 4.414463 | 4.371945 | 4.447673 | 4.362058 | 4.478018 | 4.524014 | 5.002517 | 4.423764 |
2110.02872 | Marieke van Beest | Marieke van Beest, Simone Giacomelli | Connecting 5d Higgs Branches via Fayet-Iliopoulos Deformations | 47 pages, many figures | null | 10.1007/JHEP12(2021)202 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe how the geometry of the Higgs branch of 5d superconformal field
theories is transformed under movement along the extended Coulomb branch.
Working directly with the (unitary) magnetic quiver, we demonstrate a
correspondence between Fayet-Iliopoulos deformations in 3d and 5d mass
deformations. When the Higg... | [
{
"created": "Wed, 6 Oct 2021 15:58:39 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Dec 2021 13:54:18 GMT",
"version": "v2"
}
] | 2022-01-19 | [
[
"van Beest",
"Marieke",
""
],
[
"Giacomelli",
"Simone",
""
]
] | We describe how the geometry of the Higgs branch of 5d superconformal field theories is transformed under movement along the extended Coulomb branch. Working directly with the (unitary) magnetic quiver, we demonstrate a correspondence between Fayet-Iliopoulos deformations in 3d and 5d mass deformations. When the Higgs ... | 11.184979 | 11.043659 | 13.552573 | 10.473412 | 10.010458 | 10.670672 | 10.986236 | 10.755113 | 10.300095 | 13.400545 | 10.7925 | 11.101743 | 11.480709 | 10.814998 | 10.23864 | 11.040942 | 10.833358 | 11.174933 | 10.85865 | 11.872948 | 10.561297 |
0706.0595 | Christoph Stephan A. | Christoph A. Stephan | Almost-Commutative Geometries Beyond the Standard Model II: New Colours | Revised version for publication in J.Phys.A with corrected Higgs
masses | J.Phys.A40:9941,2007 | 10.1088/1751-8113/40/32/017 | null | hep-th | null | We will present an extension of the standard model of particle physics in its
almost-commutative formulation. This extension is guided by the minimal
approach to almost-commutative geometries employed in [13], although the model
presented here is not minimal itself.
The corresponding almost-commutative geometry lea... | [
{
"created": "Tue, 5 Jun 2007 08:02:58 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Jul 2007 14:27:30 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Stephan",
"Christoph A.",
""
]
] | We will present an extension of the standard model of particle physics in its almost-commutative formulation. This extension is guided by the minimal approach to almost-commutative geometries employed in [13], although the model presented here is not minimal itself. The corresponding almost-commutative geometry leads t... | 13.336525 | 10.43044 | 14.254006 | 11.139086 | 12.181455 | 11.880981 | 13.276287 | 11.56342 | 10.965374 | 14.610894 | 11.994785 | 12.1074 | 12.590074 | 12.00279 | 12.374199 | 12.203015 | 12.430028 | 12.115589 | 12.4871 | 12.414412 | 11.949014 |
0912.3374 | K. Narayan | K. Narayan | On nonsupersymmetric $\BC^4/\BZ_N$, tachyons, terminal singularities and
flips | Latex, 43pgs incl. appendices, 2 eps figs, v2. minor clarifications
added, to appear in JHEP | null | 10.1007/JHEP03(2010)019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate nonsupersymmetric $\BC^4/\BZ_N$ orbifold singularities using
their description in terms of the string worldsheet conformal field theory and
its close relation with the toric geometry description of these singularities
and their possible resolutions. Analytic and numerical study strongly suggest
the abs... | [
{
"created": "Thu, 17 Dec 2009 11:28:56 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Feb 2010 07:14:20 GMT",
"version": "v2"
}
] | 2015-05-14 | [
[
"Narayan",
"K.",
""
]
] | We investigate nonsupersymmetric $\BC^4/\BZ_N$ orbifold singularities using their description in terms of the string worldsheet conformal field theory and its close relation with the toric geometry description of these singularities and their possible resolutions. Analytic and numerical study strongly suggest the absen... | 13.106555 | 12.727006 | 15.684843 | 12.747411 | 14.297641 | 12.943394 | 13.677308 | 12.581308 | 12.589548 | 16.080406 | 12.012215 | 12.579926 | 14.519669 | 12.570979 | 12.538322 | 12.087562 | 12.388017 | 12.275517 | 12.822704 | 15.719959 | 12.594268 |
1412.2373 | Elena Gubankova | E. Gubankova, M. Cubrovic, J. Zaanen | Exciton-driven quantum phase transitions in holography | 44 pages, 16 figures; published version | Phys. Rev. D 92, 086004 (2015) | 10.1103/PhysRevD.92.086004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study phase transitions driven by fermionic double-trace deformations in
gauge-gravity duality. Both the strength of the double trace deformation and
the infrared conformal dimension/self-energy scaling of the quasiparticle can
be used to decrease the critical temperature to zero, leading to a line of
quantum crit... | [
{
"created": "Sun, 7 Dec 2014 17:13:17 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Dec 2014 15:14:58 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Oct 2015 15:09:39 GMT",
"version": "v3"
}
] | 2015-11-04 | [
[
"Gubankova",
"E.",
""
],
[
"Cubrovic",
"M.",
""
],
[
"Zaanen",
"J.",
""
]
] | We study phase transitions driven by fermionic double-trace deformations in gauge-gravity duality. Both the strength of the double trace deformation and the infrared conformal dimension/self-energy scaling of the quasiparticle can be used to decrease the critical temperature to zero, leading to a line of quantum critic... | 10.964406 | 12.175232 | 12.485163 | 10.750775 | 11.838564 | 11.058917 | 11.796521 | 11.282707 | 11.441079 | 12.975846 | 10.738558 | 10.675599 | 11.507386 | 11.131454 | 10.56095 | 10.891024 | 10.683518 | 10.960206 | 10.793552 | 11.492367 | 10.655653 |
hep-th/0610204 | Sangmin Lee | Sangmin Lee | Superconformal field theories from crystal lattices | 4 pages, 4 figures, revtex; v2. references added, minor corrections | Phys.Rev.D75:101901,2007 | 10.1103/PhysRevD.75.101901 | SNUST-061001 | hep-th | null | We propose a brane configuration for the (2+1)d, $\mathcal{N}=2$
superconformal theories (CFT$_3$) arising from M2-branes probing toric
Calabi-Yau 4-fold cones, using a T-duality transformation of M-theory. We
obtain intersections of M5-branes on a three-torus which form a 3d bipartite
crystal lattice in a way simila... | [
{
"created": "Wed, 18 Oct 2006 06:37:36 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Oct 2006 12:44:32 GMT",
"version": "v2"
}
] | 2017-09-07 | [
[
"Lee",
"Sangmin",
""
]
] | We propose a brane configuration for the (2+1)d, $\mathcal{N}=2$ superconformal theories (CFT$_3$) arising from M2-branes probing toric Calabi-Yau 4-fold cones, using a T-duality transformation of M-theory. We obtain intersections of M5-branes on a three-torus which form a 3d bipartite crystal lattice in a way similar ... | 8.296729 | 8.06916 | 9.159816 | 7.679348 | 7.738729 | 7.966163 | 8.023281 | 7.840771 | 7.085133 | 10.274018 | 7.103034 | 7.484046 | 8.434574 | 7.555233 | 7.235477 | 7.443862 | 7.515399 | 7.214475 | 7.405926 | 8.389889 | 7.585888 |
hep-th/9812119 | Sergei Frolov | G.Arutyunov, S.Frolov and A.Polishchuk | On Lorentz invariance and supersymmetry of four particle scattering
amplitudes in $S^N\R^8$ orbifold sigma model | Latex, 23 pages | Phys. Rev. D 60, 066003 (1999) | 10.1103/PhysRevD.60.066003 | null | hep-th | null | The $S^N\R^8$ supersymmetric orbifold sigma model is expected to describe the
IR limit of the Matrix string theory. In the framework of the model the type
IIA string interaction is governed by a vertex which was recently proposed by
R.Dijkgraaf, E.Verlinde and H.Verlinde. By using this interaction vertex we
derive al... | [
{
"created": "Mon, 14 Dec 1998 21:59:12 GMT",
"version": "v1"
}
] | 2016-08-25 | [
[
"Arutyunov",
"G.",
""
],
[
"Frolov",
"S.",
""
],
[
"Polishchuk",
"A.",
""
]
] | The $S^N\R^8$ supersymmetric orbifold sigma model is expected to describe the IR limit of the Matrix string theory. In the framework of the model the type IIA string interaction is governed by a vertex which was recently proposed by R.Dijkgraaf, E.Verlinde and H.Verlinde. By using this interaction vertex we derive all ... | 11.804225 | 8.586432 | 12.803968 | 8.551546 | 8.870244 | 8.140937 | 8.814436 | 8.785108 | 8.781512 | 12.61274 | 9.011329 | 9.075828 | 10.914885 | 9.24617 | 9.27995 | 9.618855 | 8.930634 | 8.973467 | 8.862825 | 10.767392 | 9.011114 |
hep-th/0111093 | Cai Rong-gen | Rong-Gen Cai | Cardy-Verlinde Formula and Asymptotically de Sitter Spaces | Latex, 12 pages, v2: references corrected | Phys.Lett. B525 (2002) 331-336 | 10.1016/S0370-2693(01)01457-5 | null | hep-th | null | In this paper we discuss the question of whether the entropy of cosmological
horizon in some asymptotically de Sitter spaces can be described by the
Cardy-Verlinde formula, which is supposed to be an entropy formula of conformal
field theory in any dimension. For the Schwarzschild-de Sitter solution,
although the gra... | [
{
"created": "Sun, 11 Nov 2001 07:07:41 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Nov 2001 06:59:39 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Cai",
"Rong-Gen",
""
]
] | In this paper we discuss the question of whether the entropy of cosmological horizon in some asymptotically de Sitter spaces can be described by the Cardy-Verlinde formula, which is supposed to be an entropy formula of conformal field theory in any dimension. For the Schwarzschild-de Sitter solution, although the gravi... | 5.029387 | 4.659348 | 5.273935 | 4.526542 | 4.583917 | 4.375457 | 4.533551 | 4.50605 | 4.335028 | 5.30409 | 4.495863 | 4.517264 | 4.992657 | 4.557084 | 4.718489 | 4.603287 | 4.530288 | 4.67918 | 4.672012 | 4.873409 | 4.508914 |
hep-th/9605148 | Lawrence Horwitz | Oskar Pelc and L. P. Horwitz | Construction of a Complete Set of States in Relativistic Scattering
Theory | 30 pages, Latex | J.Math.Phys.38:115-138,1997 | 10.1063/1.531845 | IASSNS-96/40, TAUP 2312-95 | hep-th | null | The space of physical states in relativistic scattering theory is
constructed, using a rigorous version of the Dirac formalism, where the Hilbert
space structure is extended to a Gel'fand triple. This extension enables the
construction of ``a complete set of states'', the basic concept of the original
Dirac formalism... | [
{
"created": "Tue, 21 May 1996 16:28:03 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Pelc",
"Oskar",
""
],
[
"Horwitz",
"L. P.",
""
]
] | The space of physical states in relativistic scattering theory is constructed, using a rigorous version of the Dirac formalism, where the Hilbert space structure is extended to a Gel'fand triple. This extension enables the construction of ``a complete set of states'', the basic concept of the original Dirac formalism, ... | 9.327455 | 9.629682 | 9.857107 | 8.890362 | 10.450234 | 9.424455 | 9.582072 | 9.888633 | 9.242462 | 10.080861 | 8.66133 | 9.187548 | 9.090647 | 9.024199 | 9.167135 | 9.254036 | 8.963412 | 9.052796 | 9.246725 | 9.347802 | 9.237182 |
1909.04077 | Till Bargheer | Till Bargheer, Frank Coronado, Pedro Vieira | Octagons II: Strong Coupling | 43 pages, 14 figures, comments welcome | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The octagon function is the fundamental building block yielding correlation
functions of four large BPS operators in N=4 super Yang-Mills theory at any
value of the 't Hooft coupling and at any genus order. Here we compute the
octagon at strong coupling, and discuss various interesting limits and
implications, both a... | [
{
"created": "Mon, 9 Sep 2019 18:08:47 GMT",
"version": "v1"
}
] | 2019-09-11 | [
[
"Bargheer",
"Till",
""
],
[
"Coronado",
"Frank",
""
],
[
"Vieira",
"Pedro",
""
]
] | The octagon function is the fundamental building block yielding correlation functions of four large BPS operators in N=4 super Yang-Mills theory at any value of the 't Hooft coupling and at any genus order. Here we compute the octagon at strong coupling, and discuss various interesting limits and implications, both at ... | 11.267484 | 8.64859 | 12.17871 | 8.474261 | 8.945481 | 8.007685 | 8.753429 | 8.269889 | 8.450128 | 12.052712 | 9.133183 | 8.75226 | 10.407269 | 8.454174 | 8.862243 | 9.079672 | 8.771454 | 8.633296 | 8.631645 | 10.948493 | 9.350414 |
hep-th/9608097 | Paul Mansfield | Paul Mansfield | A Large Distance Expansion for Quantum Field Theory | 5 pages, latex, invited talk at the Second International Sakharov
Conference on Physics, May 1996 | null | null | DTP 96/33 | hep-th | null | Using analyticity of the vacuum wave-functional under complex scalings, the
vacuum of a quantum field theory may be reconstructed from a derivative
expansion valid for slowly varying fields. This enables the eigenvalue problem
for the Hamiltonian to be reduced to algebraic equations. Applied to Yang-Mills
theory this... | [
{
"created": "Thu, 15 Aug 1996 14:42:25 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Mansfield",
"Paul",
""
]
] | Using analyticity of the vacuum wave-functional under complex scalings, the vacuum of a quantum field theory may be reconstructed from a derivative expansion valid for slowly varying fields. This enables the eigenvalue problem for the Hamiltonian to be reduced to algebraic equations. Applied to Yang-Mills theory this e... | 15.204003 | 12.876411 | 12.873177 | 11.268532 | 12.700575 | 12.134223 | 12.18956 | 11.195347 | 11.714005 | 14.850419 | 12.324895 | 12.370048 | 12.761162 | 12.177444 | 12.3852 | 13.340543 | 12.536786 | 13.348043 | 12.6536 | 13.898142 | 12.465134 |
1603.07982 | Vitaly Vanchurin | Vitaly Vanchurin | Dual Field Theories of Quantum Computation | 19 pages, 1 figure | JHEP 1606 (2016) 001 | 10.1007/JHEP06(2016)001 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given two quantum states of N q-bits we are interested to find the shortest
quantum circuit consisting of only one- and two- q-bit gates that would
transfer one state into another. We call it the quantum maze problem for the
reasons described in the paper. We argue that in a large N limit the quantum
maze problem is ... | [
{
"created": "Fri, 25 Mar 2016 18:46:20 GMT",
"version": "v1"
},
{
"created": "Wed, 18 May 2016 19:46:16 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Dec 2016 16:03:19 GMT",
"version": "v3"
}
] | 2019-01-15 | [
[
"Vanchurin",
"Vitaly",
""
]
] | Given two quantum states of N q-bits we are interested to find the shortest quantum circuit consisting of only one- and two- q-bit gates that would transfer one state into another. We call it the quantum maze problem for the reasons described in the paper. We argue that in a large N limit the quantum maze problem is eq... | 8.901754 | 10.827633 | 10.702517 | 10.450624 | 10.899469 | 10.596628 | 10.587517 | 11.319371 | 9.917532 | 10.705472 | 9.48164 | 10.015727 | 9.386786 | 9.402804 | 9.816917 | 9.572053 | 9.707913 | 9.672938 | 9.597135 | 9.365104 | 9.483864 |
hep-th/9308024 | Yuji Kobayashi 0426-77-1111x3377 | Yuji Kobayashi | The Improved Bounce Solution of SU(2)-Higgs Model | Plain TeX, 12 pages plus 3 figures available upon request,
TMUP-HEL-9304 | null | 10.1143/ptp/90.4.885 | null | hep-th | null | We further develop the reduced action formalism of the SU(2)-Higgs model
originally given by Aoyama et.al.. Our new ansatz for the sphaleron solution
makes it possible to apply this formalism to all range of the Higgs self
coupling constant. Based on the formalism, we construct a bounce solution
oscillating around th... | [
{
"created": "Fri, 6 Aug 1993 05:59:42 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Aug 1993 06:59:54 GMT",
"version": "v2"
}
] | 2017-02-01 | [
[
"Kobayashi",
"Yuji",
""
]
] | We further develop the reduced action formalism of the SU(2)-Higgs model originally given by Aoyama et.al.. Our new ansatz for the sphaleron solution makes it possible to apply this formalism to all range of the Higgs self coupling constant. Based on the formalism, we construct a bounce solution oscillating around the ... | 11.598381 | 8.058946 | 9.594812 | 8.6514 | 9.60241 | 9.234581 | 9.007406 | 9.850766 | 8.972796 | 10.315425 | 9.674565 | 9.868225 | 10.58731 | 10.218516 | 9.825453 | 9.369391 | 10.021586 | 9.722413 | 10.14323 | 9.842836 | 9.699522 |
1309.0785 | Arkady Tseytlin | A.A. Tseytlin | On partition function and Weyl anomaly of conformal higher spin fields | 36 pages. v2: misprints corrected, references added; v3: comments on
D greater than 4 generalization and appendix B on conformal higher derivative
scalar operator added; v4: a minor comment in section 3.1 and references
added | null | 10.1016/j.nuclphysb.2013.10.009 | Imperial-TP-AT-2013-4 | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study 4-dimensional higher-derivative conformal higher spin (CHS) fields
generalising Weyl graviton and conformal gravitino. They appear, in particular,
as "induced" theories in the AdS/CFT context. We consider their partition
function on curved Einstein-space backgrounds like (A)dS or sphere and
Ricci-flat spaces... | [
{
"created": "Tue, 3 Sep 2013 19:26:50 GMT",
"version": "v1"
},
{
"created": "Sat, 7 Sep 2013 21:16:37 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Sep 2013 18:34:33 GMT",
"version": "v3"
},
{
"created": "Mon, 28 Oct 2013 19:55:07 GMT",
"version": "v4"
}
] | 2015-06-17 | [
[
"Tseytlin",
"A. A.",
""
]
] | We study 4-dimensional higher-derivative conformal higher spin (CHS) fields generalising Weyl graviton and conformal gravitino. They appear, in particular, as "induced" theories in the AdS/CFT context. We consider their partition function on curved Einstein-space backgrounds like (A)dS or sphere and Ricci-flat spaces. ... | 6.983221 | 7.056091 | 7.538436 | 6.775329 | 6.878052 | 6.847503 | 6.754964 | 6.769507 | 6.624036 | 8.247381 | 6.579936 | 6.756311 | 6.992946 | 6.647168 | 6.759131 | 6.84223 | 6.727083 | 6.591295 | 6.705052 | 7.086083 | 6.655196 |
2212.10214 | Massimo Giovannini | Massimo Giovannini | The hypermagnetic power spectra and the phases of Sakharov oscillations | 40 pages, 11 figures | null | 10.1103/PhysRevD.107.043525 | null | hep-th astro-ph.CO gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | If the gauge fields are amplified from the inflationary vacuum, the quantum
mechanical initial data correspond to travelling waves that turn asymptotically
into standing waves whose phases only depend on the evolution of the gauge
coupling. We point out that these gauge analogs of the Sakharov oscillations
are exchan... | [
{
"created": "Tue, 20 Dec 2022 12:47:52 GMT",
"version": "v1"
}
] | 2023-03-08 | [
[
"Giovannini",
"Massimo",
""
]
] | If the gauge fields are amplified from the inflationary vacuum, the quantum mechanical initial data correspond to travelling waves that turn asymptotically into standing waves whose phases only depend on the evolution of the gauge coupling. We point out that these gauge analogs of the Sakharov oscillations are exchange... | 17.280016 | 18.735714 | 16.966866 | 16.630693 | 17.931887 | 18.747633 | 17.400724 | 16.679583 | 17.714756 | 17.370764 | 17.556858 | 17.063477 | 16.593819 | 16.118496 | 16.478292 | 16.556679 | 16.896818 | 16.81531 | 16.574509 | 16.644382 | 16.762005 |
hep-th/0412267 | Paul Korbel | Paul Korbel | Quantum Basis of Lorentz Symmetry | 21 pages | null | null | null | hep-th | null | An unconventional outlook on relationship between the quantum mechanics and
special relativity is proposed. We show that the two fundamental postulates of
quantum mechanics of Planck and de Broglie combined with the idea of comparison
scale (explained in the paper), are enough to introduce relativistic
description. W... | [
{
"created": "Tue, 21 Dec 2004 23:35:53 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Korbel",
"Paul",
""
]
] | An unconventional outlook on relationship between the quantum mechanics and special relativity is proposed. We show that the two fundamental postulates of quantum mechanics of Planck and de Broglie combined with the idea of comparison scale (explained in the paper), are enough to introduce relativistic description. We ... | 19.244772 | 18.77302 | 19.286795 | 19.203196 | 18.969772 | 19.779831 | 19.859217 | 18.68046 | 17.371853 | 20.069105 | 19.742121 | 18.793436 | 19.541765 | 19.119219 | 19.316072 | 19.636843 | 19.742714 | 18.582455 | 19.062866 | 18.768888 | 18.890163 |
1612.08858 | Gordon Semenoff | Gianluca Grignani, Gordon W. Semenoff | Scattering and momentum space entanglement | null | null | 10.1016/j.physletb.2017.07.030 | null | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a formula for the entanglement entropy of two regions in momentum
space that is generated by the scattering of weakly interacting scalar
particles. We discuss an example where weak interactions entangle momentum
scales above and below an infrared cutoff.
| [
{
"created": "Wed, 28 Dec 2016 11:40:40 GMT",
"version": "v1"
}
] | 2017-09-13 | [
[
"Grignani",
"Gianluca",
""
],
[
"Semenoff",
"Gordon W.",
""
]
] | We derive a formula for the entanglement entropy of two regions in momentum space that is generated by the scattering of weakly interacting scalar particles. We discuss an example where weak interactions entangle momentum scales above and below an infrared cutoff. | 17.073015 | 16.051853 | 13.212381 | 13.29339 | 15.98228 | 13.232769 | 13.088547 | 13.830343 | 12.6777 | 14.14342 | 14.753068 | 15.243846 | 14.562613 | 14.824242 | 14.841648 | 14.783561 | 14.978441 | 15.226422 | 14.28535 | 16.30267 | 14.674454 |
1304.0822 | Mikhail Shifman | M. Shifman, A. Yung | Detailing N=1 Seiberg's Duality through the Seiberg-Witten Solution of
N=2 | 30 pp., 3 figs; v2. One reference added | null | 10.1103/PhysRevD.87.106009 | FTPI-MINN-13/10, UMN-TH-3142/13 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Starting from the Seiberg-Witten solution of N=2 SQCD with the U(N) gauge
group and N_f quark flavors we construct the so-called \mu-dual N=1 theory in
the r vacua in the regime analogous to that existing to the left of the left
edge of the Seiberg conformal window (here r is the number of condensed
quarks). The stro... | [
{
"created": "Wed, 3 Apr 2013 02:10:47 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Apr 2013 16:02:16 GMT",
"version": "v2"
}
] | 2013-06-05 | [
[
"Shifman",
"M.",
""
],
[
"Yung",
"A.",
""
]
] | Starting from the Seiberg-Witten solution of N=2 SQCD with the U(N) gauge group and N_f quark flavors we construct the so-called \mu-dual N=1 theory in the r vacua in the regime analogous to that existing to the left of the left edge of the Seiberg conformal window (here r is the number of condensed quarks). The strong... | 10.486311 | 9.687016 | 11.69329 | 8.59377 | 9.446061 | 8.702244 | 8.862606 | 8.778839 | 8.209125 | 11.062947 | 9.203207 | 9.029297 | 9.943344 | 9.164443 | 9.4114 | 8.961184 | 9.213512 | 9.255351 | 8.908545 | 10.147882 | 8.73546 |
1611.03101 | Yifan Wang | Jaume Gomis, Zohar Komargodski, Hirosi Ooguri, Nathan Seiberg, and
Yifan Wang | Shortening Anomalies in Supersymmetric Theories | 31 pages. v2: reference added | null | 10.1007/JHEP01(2017)067 | CALT-TH-2016-031, IPMU 16-016, PUPT-2513 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present new anomalies in two-dimensional ${\mathcal N} =(2, 2)$
superconformal theories. They obstruct the shortening conditions of chiral and
twisted chiral multiplets at coincident points. This implies that marginal
couplings cannot be promoted to background superfields in short
representations. Therefore, stand... | [
{
"created": "Wed, 9 Nov 2016 21:35:13 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Dec 2016 17:25:11 GMT",
"version": "v2"
}
] | 2017-03-08 | [
[
"Gomis",
"Jaume",
""
],
[
"Komargodski",
"Zohar",
""
],
[
"Ooguri",
"Hirosi",
""
],
[
"Seiberg",
"Nathan",
""
],
[
"Wang",
"Yifan",
""
]
] | We present new anomalies in two-dimensional ${\mathcal N} =(2, 2)$ superconformal theories. They obstruct the shortening conditions of chiral and twisted chiral multiplets at coincident points. This implies that marginal couplings cannot be promoted to background superfields in short representations. Therefore, standar... | 5.606719 | 5.851733 | 7.014786 | 5.918914 | 6.037894 | 6.13187 | 5.663717 | 5.917345 | 5.813774 | 7.351686 | 5.779566 | 5.535866 | 5.951598 | 5.449302 | 5.44125 | 5.545769 | 5.453009 | 5.565107 | 5.50399 | 5.734274 | 5.5288 |
hep-th/0410164 | Yoshishige Kobayashi | Yoshishige Kobayashi, Shin Sasaki | Lorentz invariant and supersymmetric interpretation of noncommutative
quantum field theory | 15 pages, LaTeX. v3:One section added, typos corrected, to appear in
Int. J. Mod. Phys. A | Int.J.Mod.Phys. A20 (2005) 7175-7188 | 10.1142/S0217751X05022421 | null | hep-th | null | In this paper, using a Hopf-algebraic method, we construct deformed
Poincar\'e SUSY algebra in terms of twisted (Hopf) algebra. By adapting this
twist deformed super-Poincar\'e algrebra as our fundamental symmetry, we can
see the consistency between the algebra and non(anti)commutative relation among
(super)coordinat... | [
{
"created": "Thu, 14 Oct 2004 10:13:21 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Nov 2004 13:49:44 GMT",
"version": "v2"
},
{
"created": "Mon, 7 Mar 2005 10:25:34 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Kobayashi",
"Yoshishige",
""
],
[
"Sasaki",
"Shin",
""
]
] | In this paper, using a Hopf-algebraic method, we construct deformed Poincar\'e SUSY algebra in terms of twisted (Hopf) algebra. By adapting this twist deformed super-Poincar\'e algrebra as our fundamental symmetry, we can see the consistency between the algebra and non(anti)commutative relation among (super)coordinates... | 12.054877 | 11.673652 | 13.292243 | 10.90694 | 12.000587 | 12.563338 | 11.701165 | 10.913079 | 11.100543 | 13.332914 | 11.644354 | 11.254132 | 12.165737 | 11.0591 | 11.227739 | 11.180457 | 11.203424 | 11.275645 | 11.308267 | 11.744391 | 11.07548 |
1503.01044 | Tomas Ortin | Pablo Bueno, Pedro Fernandez-Ramirez, Patrick Meessen and Tomas Ortin | Resolution of SU(2) monopole singularities by oxidation | 13 pages, LaTeX file, no figures | null | 10.1016/j.physletb.2015.04.065 | University of Oviedo preprint FPAUO-15/07 and IFT-UAM/CSIC preprint
IFT-UAM/CSIC-15-019 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how "colored" SU(2) BPS monopoles (that is: SU(2) monopoles
satisfying the Bogomol'nyi equation whose Higgs field and magnetic charge
vanish at infinity and which are singular at the origin) can be obtained from
the BPST instanton by a singular dimensional reduction, explaining the origin
of the singularity a... | [
{
"created": "Tue, 3 Mar 2015 18:29:37 GMT",
"version": "v1"
}
] | 2015-05-06 | [
[
"Bueno",
"Pablo",
""
],
[
"Fernandez-Ramirez",
"Pedro",
""
],
[
"Meessen",
"Patrick",
""
],
[
"Ortin",
"Tomas",
""
]
] | We show how "colored" SU(2) BPS monopoles (that is: SU(2) monopoles satisfying the Bogomol'nyi equation whose Higgs field and magnetic charge vanish at infinity and which are singular at the origin) can be obtained from the BPST instanton by a singular dimensional reduction, explaining the origin of the singularity and... | 9.922246 | 10.496431 | 9.959766 | 9.378486 | 11.288548 | 11.212331 | 10.669935 | 8.985535 | 10.000277 | 10.410192 | 9.784886 | 9.612188 | 9.884998 | 9.614715 | 9.877944 | 9.680532 | 9.618186 | 9.793305 | 9.480642 | 9.648668 | 9.643466 |
0711.2742 | Mykola Shpot | M. A. Shpot | A massive Feynman integral and some reduction relations for Appell
functions | 19 pages. To appear in Journal of Mathematical Physics | J.Math.Phys.48:123512,2007 | 10.1063/1.2821256 | null | hep-th math-ph math.CA math.MP | null | New explicit expressions are derived for the one-loop two-point Feynman
integral with arbitrary external momentum and masses $m_1^2$ and $m_2^2$ in D
dimensions. The results are given in terms of Appell functions, manifestly
symmetric with respect to the masses $m_i^2$. Equating our expressions with
previously known ... | [
{
"created": "Sat, 17 Nov 2007 15:03:38 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Shpot",
"M. A.",
""
]
] | New explicit expressions are derived for the one-loop two-point Feynman integral with arbitrary external momentum and masses $m_1^2$ and $m_2^2$ in D dimensions. The results are given in terms of Appell functions, manifestly symmetric with respect to the masses $m_i^2$. Equating our expressions with previously known re... | 8.373005 | 9.249915 | 7.773848 | 7.945306 | 9.163639 | 8.217184 | 8.722154 | 8.468937 | 7.834715 | 7.661642 | 7.770205 | 7.564452 | 8.162966 | 7.566447 | 8.092769 | 7.893334 | 8.029841 | 7.867692 | 7.652063 | 7.869289 | 7.888777 |
2407.08638 | Renann Lipinski Jusinskas | Renann Lipinski Jusinskas | Strings as particle arrays | 13 pages. v2: small improvements, references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | These notes discuss the emergence of the Polyakov action from the low-energy
limit of an array of relativistic particles with harmonic interactions, which
is suggestive of a ``microscopic'' description of string theory.
| [
{
"created": "Thu, 11 Jul 2024 16:19:05 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jul 2024 18:35:37 GMT",
"version": "v2"
}
] | 2024-07-16 | [
[
"Jusinskas",
"Renann Lipinski",
""
]
] | These notes discuss the emergence of the Polyakov action from the low-energy limit of an array of relativistic particles with harmonic interactions, which is suggestive of a ``microscopic'' description of string theory. | 18.15085 | 12.121882 | 14.77999 | 11.455237 | 12.632387 | 12.631141 | 11.867728 | 11.101197 | 12.062027 | 16.057495 | 11.197162 | 11.957473 | 15.707761 | 12.454968 | 11.937838 | 11.441748 | 11.600939 | 11.775006 | 12.972995 | 14.889608 | 10.910958 |
hep-th/9809125 | Marco Matone | Alon E. Faraggi and Marco Matone | Equivalence Principle, Planck Length and Quantum Hamilton-Jacobi
Equation | 1+7 pages, LaTeX. Typos corrected, to appear in Phys. Lett. B | Phys.Lett. B445 (1998) 77-81 | 10.1016/S0370-2693(98)01484-1 | UMN-TH-1722-98-TPI-MINN-98/19, DFPD97/TH/51 | hep-th gr-qc hep-ph math-ph math.MP nlin.SI quant-ph solv-int | null | The Quantum Stationary HJ Equation (QSHJE) that we derived from the
equivalence principle, gives rise to initial conditions which cannot be seen in
the Schroedinger equation. Existence of the classical limit leads to a
dependence of the integration constant $\ell=\ell_1+i\ell_2$ on the Planck
length. Solutions of the... | [
{
"created": "Thu, 17 Sep 1998 15:59:08 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Sep 1998 21:59:55 GMT",
"version": "v2"
},
{
"created": "Fri, 20 Nov 1998 15:38:33 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Faraggi",
"Alon E.",
""
],
[
"Matone",
"Marco",
""
]
] | The Quantum Stationary HJ Equation (QSHJE) that we derived from the equivalence principle, gives rise to initial conditions which cannot be seen in the Schroedinger equation. Existence of the classical limit leads to a dependence of the integration constant $\ell=\ell_1+i\ell_2$ on the Planck length. Solutions of the Q... | 15.502975 | 14.423655 | 15.619854 | 14.277053 | 14.953363 | 15.432747 | 15.30258 | 13.596842 | 14.053026 | 15.096653 | 13.833618 | 14.708654 | 14.904374 | 14.290555 | 13.811916 | 13.945168 | 13.880277 | 14.624882 | 14.294103 | 14.301731 | 14.030078 |
hep-th/9510028 | Ioannis Bakas | E. Alvarez, L. Alvarez-Gaume and I. Bakas | Supersymmetry and Dualities | 19 pages, latex, no figures | Nucl.Phys.Proc.Suppl. 46 (1996) 16-29 | 10.1016/0920-5632(96)00003-5 | CERN-TH/95-258, FTUAM/95-34 | hep-th | null | Duality transformations with respect to rotational isometries relate
supersymmetric with non-supersymmetric backgrounds in string theory. We find
that non-local world-sheet effects have to be taken into account in order to
restore supersymmetry at the string level. The underlying superconformal
algebra remains the sa... | [
{
"created": "Fri, 6 Oct 1995 15:43:40 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Alvarez",
"E.",
""
],
[
"Alvarez-Gaume",
"L.",
""
],
[
"Bakas",
"I.",
""
]
] | Duality transformations with respect to rotational isometries relate supersymmetric with non-supersymmetric backgrounds in string theory. We find that non-local world-sheet effects have to be taken into account in order to restore supersymmetry at the string level. The underlying superconformal algebra remains the same... | 10.084229 | 8.251564 | 10.257258 | 7.837551 | 7.898999 | 7.883169 | 7.281553 | 8.124368 | 7.679367 | 11.189804 | 8.250219 | 8.236582 | 9.503734 | 7.965358 | 8.152375 | 8.28081 | 8.22197 | 8.147 | 8.010944 | 9.177238 | 8.128377 |
1601.07530 | Ahmad Ghodsi | Ahmad Ghodsi, Mohammad R. Garousi and Ghadir Jafari | On T-duality of $R^2$-corrections to DBI action at all orders of gauge
field | 13 pages | JHEP 1604 (2016) 081 (2016-04-14) | 10.1007/JHEP04(2016)081 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, it has been observed that in a T-duality invariant world-volume
theory in flat spacetime, all orders of gauge field strength and all orders of
the D-brane velocity appear in two specific matrices. Using these two matrices,
we construct the world-volume couplings of two massless NSNS states at order
$\alpha'... | [
{
"created": "Wed, 27 Jan 2016 20:18:38 GMT",
"version": "v1"
}
] | 2016-10-18 | [
[
"Ghodsi",
"Ahmad",
""
],
[
"Garousi",
"Mohammad R.",
""
],
[
"Jafari",
"Ghadir",
""
]
] | Recently, it has been observed that in a T-duality invariant world-volume theory in flat spacetime, all orders of gauge field strength and all orders of the D-brane velocity appear in two specific matrices. Using these two matrices, we construct the world-volume couplings of two massless NSNS states at order $\alpha'^2... | 10.162612 | 8.231801 | 11.089426 | 8.71173 | 9.526564 | 9.045668 | 8.837895 | 9.131529 | 8.643705 | 11.305447 | 9.229519 | 9.665338 | 10.647793 | 9.450787 | 9.401913 | 9.337436 | 9.546994 | 9.418376 | 9.626169 | 10.590527 | 9.438803 |
hep-th/9708079 | Joern Haeuser | J.M. Hauser, W. Cassing, S. Leupold, and M.H. Thoma (Institut fuer
Theoretische Physik, Universitaet Giessen) | Convergence properties of the equal-time connected Green function
approach for temporal gauge SU(2)_{2+1} Yang-Mills theory | 43 pages, LaTeX, 15 PS figures | Annals Phys. 265 (1998) 155-197 | 10.1006/aphy.1997.5820 | UGI-97-11 | hep-th hep-ph | null | The hierarchy of equations of motion for equal-time Green functions in
temporal gauge SU(N) Yang-Mills theory is truncated using an expansion in terms
of connected Green functions. A second hierarchy of constraint equations arises
from Gauss law and can be truncated in a similar way. Within this approximation
scheme ... | [
{
"created": "Thu, 14 Aug 1997 16:04:30 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Hauser",
"J. M.",
"",
"Institut fuer\n Theoretische Physik, Universitaet Giessen"
],
[
"Cassing",
"W.",
"",
"Institut fuer\n Theoretische Physik, Universitaet Giessen"
],
[
"Leupold",
"S.",
"",
"Institut fuer\n Theoretische Physik, Universitaet Giessen"
... | The hierarchy of equations of motion for equal-time Green functions in temporal gauge SU(N) Yang-Mills theory is truncated using an expansion in terms of connected Green functions. A second hierarchy of constraint equations arises from Gauss law and can be truncated in a similar way. Within this approximation scheme we... | 11.829154 | 11.915632 | 12.432569 | 11.202457 | 12.228498 | 12.284218 | 12.157779 | 10.878778 | 11.90138 | 13.617062 | 11.258871 | 11.865005 | 11.958094 | 11.675887 | 11.934698 | 12.294065 | 12.073959 | 12.147293 | 11.828546 | 12.258082 | 11.803453 |
0807.0923 | Partha Mukhopadhyay | Partha Mukhopadhyay | On the Conformal Field Theories for Bosonic Strings in PP-Waves | 19 pages | JHEP0811:034,2008 | 10.1088/1126-6708/2008/11/034 | UK/08-06 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently Kazama and Yokoi (arXiv:0801.1561 [hep-th]) have used a phase-space
method to study the Virasoro algebra of type IIB superstring theory in the
maximally supersymmetric R-R plane wave background in a semi-light-cone gauge.
Two types of normal ordering have been considered, namely "phase space normal
ordering"... | [
{
"created": "Sun, 6 Jul 2008 18:07:36 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Mukhopadhyay",
"Partha",
""
]
] | Recently Kazama and Yokoi (arXiv:0801.1561 [hep-th]) have used a phase-space method to study the Virasoro algebra of type IIB superstring theory in the maximally supersymmetric R-R plane wave background in a semi-light-cone gauge. Two types of normal ordering have been considered, namely "phase space normal ordering" (... | 9.493947 | 9.203385 | 10.419065 | 8.987435 | 9.191494 | 9.094035 | 9.298657 | 9.478843 | 9.360335 | 11.098673 | 9.694427 | 9.008573 | 9.548209 | 9.166034 | 8.855968 | 9.259474 | 9.24188 | 9.271553 | 9.260845 | 9.756308 | 9.242603 |
1203.2948 | Aalok Misra | Aalok Misra | Local D3/D7 mu-Split SUSY, 125 GeV Higgs and Large Volume Ricci-Flat
Swiss-Cheese Metrics: A Brief Review | 1+14 pages, LaTeX, invited review for MPLA. arXiv admin note: text
overlap with arXiv:1105.0365 | null | 10.1142/S0217732312300133 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article, we review briefly recent progress made in realizing
local(ized around a mobile space-time filling D3-brane in) D3/D7 mu-Split
Supersymmetry in (the large volume limit of Type IIB) String Theory
(compactified on Swiss-Cheese Calabi-Yau orientifolds) as well as obtaining a
125 GeV (light) Higgs in the ... | [
{
"created": "Tue, 13 Mar 2012 20:47:20 GMT",
"version": "v1"
}
] | 2015-06-04 | [
[
"Misra",
"Aalok",
""
]
] | In this article, we review briefly recent progress made in realizing local(ized around a mobile space-time filling D3-brane in) D3/D7 mu-Split Supersymmetry in (the large volume limit of Type IIB) String Theory (compactified on Swiss-Cheese Calabi-Yau orientifolds) as well as obtaining a 125 GeV (light) Higgs in the sa... | 16.216757 | 14.666608 | 16.64237 | 13.341532 | 13.231109 | 13.846906 | 14.07795 | 14.248866 | 13.377986 | 17.558445 | 13.477354 | 13.845298 | 14.883707 | 14.005857 | 13.787349 | 14.076462 | 13.955016 | 14.348104 | 14.29411 | 14.9198 | 14.285273 |
2111.07989 | Shai Chester | Shai M. Chester, Ross Dempsey, and Silviu S. Pufu | Bootstrapping $\mathcal{N}=4$ super-Yang-Mills on the conformal manifold | 31 pages plus appendices, 13 figures, v3 expanded discussion of
integration region | null | null | PUPT-2627 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We combine supersymmetric localization results with numerical bootstrap
techniques to compute upper bounds on the low-lying CFT data of ${\cal N} = 4$
super-Yang-Mills theory as a function of the complexified gauge coupling
$\tau$. In particular, from the stress tensor multiplet four-point function, we
extract the sc... | [
{
"created": "Mon, 15 Nov 2021 18:50:45 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Nov 2021 15:06:26 GMT",
"version": "v2"
},
{
"created": "Sat, 8 Oct 2022 14:14:40 GMT",
"version": "v3"
}
] | 2022-10-11 | [
[
"Chester",
"Shai M.",
""
],
[
"Dempsey",
"Ross",
""
],
[
"Pufu",
"Silviu S.",
""
]
] | We combine supersymmetric localization results with numerical bootstrap techniques to compute upper bounds on the low-lying CFT data of ${\cal N} = 4$ super-Yang-Mills theory as a function of the complexified gauge coupling $\tau$. In particular, from the stress tensor multiplet four-point function, we extract the scal... | 5.778707 | 5.357494 | 7.451947 | 5.456393 | 5.363287 | 5.353109 | 5.955782 | 5.380055 | 5.429136 | 7.185 | 5.46691 | 5.387906 | 6.354122 | 5.744841 | 5.520229 | 5.391851 | 5.489749 | 5.325714 | 5.573243 | 6.582594 | 5.58562 |
1007.0736 | Delsate T\'erence | Yves Brihaye, T\'erence Delsate, Nobuyuki Sawado, Yuta Kodama | Inflating baby-Skyrme branes in six dimensions | 24 pages, 16 figures | Phys.Rev.D82:106002,2010 | 10.1103/PhysRevD.82.106002 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a six dimensional brane world model, where the brane is described
by a localized solution to the baby-Skyrme model extending in the
extradimensions. The branes have a cosmological constant modeled by inflating
four dimensional slices and we further consider a bulk cosmological constant.
We construct solut... | [
{
"created": "Mon, 5 Jul 2010 18:07:50 GMT",
"version": "v1"
}
] | 2010-11-11 | [
[
"Brihaye",
"Yves",
""
],
[
"Delsate",
"Térence",
""
],
[
"Sawado",
"Nobuyuki",
""
],
[
"Kodama",
"Yuta",
""
]
] | We consider a six dimensional brane world model, where the brane is described by a localized solution to the baby-Skyrme model extending in the extradimensions. The branes have a cosmological constant modeled by inflating four dimensional slices and we further consider a bulk cosmological constant. We construct solutio... | 11.530556 | 12.211569 | 10.967306 | 11.123052 | 12.485948 | 10.962114 | 12.416833 | 10.243999 | 11.765307 | 10.887169 | 11.452384 | 11.466283 | 10.959517 | 11.143477 | 11.318408 | 11.3532 | 11.238495 | 11.220118 | 11.319445 | 10.801955 | 11.036221 |
hep-th/0305163 | Tom Banks | T.Banks (SCIPP-U.C. Santa Cruz, Runhetc-Rutgers U.) | SUSY and the Holographic Screens | null | null | null | SCIPP-03/05, RUNHETC-2003-15 | hep-th gr-qc | null | The Cartan-Penrose (CP) equation is interpreted as a connection between a
spinor at a point in spacetime, and a pair of holographic screens on which the
information at that point may be projected. Local SUSY is thus given a physical
interpretation in terms of the ambiguity of the choice of holographic screen
implicit... | [
{
"created": "Mon, 19 May 2003 18:14:57 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Banks",
"T.",
"",
"SCIPP-U.C. Santa Cruz, Runhetc-Rutgers U."
]
] | The Cartan-Penrose (CP) equation is interpreted as a connection between a spinor at a point in spacetime, and a pair of holographic screens on which the information at that point may be projected. Local SUSY is thus given a physical interpretation in terms of the ambiguity of the choice of holographic screen implicit i... | 15.239748 | 16.898123 | 15.927575 | 14.885257 | 14.054049 | 14.563502 | 15.135442 | 16.757429 | 16.041569 | 16.901972 | 14.438734 | 14.734205 | 14.368093 | 14.103354 | 13.978199 | 14.072439 | 13.939856 | 14.903315 | 14.631525 | 15.324902 | 14.171562 |
hep-th/0410158 | Rong-Gen Cai | Rong-Gen Cai, Da-Wei Pang and Anzhong Wang | Born-Infeld Black Holes in (A)dS Spaces | Latex, 18 pages with 4 eps figures, v2: Revtex, 11 pages with 4 eps
figures, to appear in PRD | Phys.Rev.D70:124034,2004 | 10.1103/PhysRevD.70.124034 | null | hep-th gr-qc | null | We study some exact solutions in a $D(\ge4)$-dimensional Einstein-Born-Infeld
theory with a cosmological constant. These solutions are asymptotically de
Sitter or anti-de Sitter, depending on the sign of the cosmological constant.
Black hole horizon and cosmological horizon in these spacetimes can be a
positive, zero... | [
{
"created": "Thu, 14 Oct 2004 02:42:42 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Dec 2004 02:15:17 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Cai",
"Rong-Gen",
""
],
[
"Pang",
"Da-Wei",
""
],
[
"Wang",
"Anzhong",
""
]
] | We study some exact solutions in a $D(\ge4)$-dimensional Einstein-Born-Infeld theory with a cosmological constant. These solutions are asymptotically de Sitter or anti-de Sitter, depending on the sign of the cosmological constant. Black hole horizon and cosmological horizon in these spacetimes can be a positive, zero o... | 4.100624 | 4.032678 | 4.021363 | 3.811575 | 3.880681 | 3.96051 | 3.75239 | 3.701519 | 3.746573 | 4.069696 | 3.922739 | 3.936722 | 3.976012 | 3.842208 | 3.883087 | 3.987607 | 3.853262 | 3.77641 | 3.921782 | 3.982691 | 3.800357 |
0904.4869 | Gregory Giecold | G. C. Giecold | Fermionic Schwinger-Keldysh Propagators from AdS/CFT | 16 pages, 2 figures. v3: refs added, confusing typos fixed, note on
sqrt(V,-U) and Dirac eqn added | JHEP 0910:057,2009 | 10.1088/1126-6708/2009/10/057 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Herzog and Son prescription for computing real-time Green functions for
finite temperature gauge theories from their gravity dual is generalized to
fermions. These notes explain how such an extension involves properties of
spinors in a curved, complexified space-time.
| [
{
"created": "Thu, 30 Apr 2009 16:11:30 GMT",
"version": "v1"
},
{
"created": "Fri, 1 May 2009 12:04:36 GMT",
"version": "v2"
},
{
"created": "Wed, 6 May 2009 15:09:21 GMT",
"version": "v3"
},
{
"created": "Thu, 25 Jun 2009 16:18:35 GMT",
"version": "v4"
}
] | 2009-11-09 | [
[
"Giecold",
"G. C.",
""
]
] | The Herzog and Son prescription for computing real-time Green functions for finite temperature gauge theories from their gravity dual is generalized to fermions. These notes explain how such an extension involves properties of spinors in a curved, complexified space-time. | 58.581409 | 22.002329 | 32.492256 | 19.774841 | 28.027533 | 19.343756 | 25.956879 | 24.471729 | 23.173779 | 38.708576 | 25.804836 | 24.450233 | 24.73262 | 22.750238 | 26.451796 | 26.076735 | 25.498522 | 22.433228 | 24.412745 | 22.722591 | 30.42687 |
2112.10658 | Roman Mauch | Roman Mauch and Lorenzo Ruggeri | Index of the Transversally Elliptic Complex in Pestunization | 26 pages + appendices; version to be published in J.Phys.A | null | 10.1088/1751-8121/ac7921 | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | In this note we present a formula for the equivariant index of the
cohomological complex obtained from localization of $\mathcal{N}=2$ SYM on
simply-connected compact four-manifolds with a $T^2$-action. Knowledge of said
index is essential to compute the perturbative part of the partition function
for the theory. In ... | [
{
"created": "Mon, 20 Dec 2021 16:34:22 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Mar 2022 16:50:15 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Jun 2022 13:55:22 GMT",
"version": "v3"
}
] | 2022-09-20 | [
[
"Mauch",
"Roman",
""
],
[
"Ruggeri",
"Lorenzo",
""
]
] | In this note we present a formula for the equivariant index of the cohomological complex obtained from localization of $\mathcal{N}=2$ SYM on simply-connected compact four-manifolds with a $T^2$-action. Knowledge of said index is essential to compute the perturbative part of the partition function for the theory. In th... | 8.09015 | 8.542033 | 9.070037 | 8.027071 | 8.261718 | 8.428038 | 8.468989 | 7.790736 | 7.903141 | 10.225511 | 7.591754 | 7.749442 | 8.157132 | 7.63076 | 7.831426 | 7.664203 | 7.662062 | 7.804834 | 7.733067 | 8.001289 | 7.563305 |
2211.07810 | Paul Ryan | Andrea Cavagli\`a, Simon Ekhammar, Nikolay Gromov, Paul Ryan | Exploring the Quantum Spectral Curve for AdS${}_3$/CFT${}_2$ | null | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Despite the rich and fruitful history of the integrability approach to string
theory on the $AdS_3\times S^3\times T^4$ background, it has not been possible
to extract many concrete predictions from integrability, except in a strict
asymptotic regime of large quantum numbers, due to the severity of wrapping
effects. ... | [
{
"created": "Tue, 15 Nov 2022 00:32:39 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Feb 2023 08:04:11 GMT",
"version": "v2"
}
] | 2023-02-24 | [
[
"Cavaglià",
"Andrea",
""
],
[
"Ekhammar",
"Simon",
""
],
[
"Gromov",
"Nikolay",
""
],
[
"Ryan",
"Paul",
""
]
] | Despite the rich and fruitful history of the integrability approach to string theory on the $AdS_3\times S^3\times T^4$ background, it has not been possible to extract many concrete predictions from integrability, except in a strict asymptotic regime of large quantum numbers, due to the severity of wrapping effects. Th... | 11.352546 | 10.529123 | 12.842155 | 9.981492 | 10.6312 | 10.569207 | 10.503123 | 10.24473 | 10.066009 | 12.920341 | 10.052202 | 10.633051 | 11.044926 | 10.290421 | 10.430151 | 10.506519 | 10.381498 | 10.564634 | 10.123475 | 10.757018 | 10.429578 |
2004.03779 | Sinya Aoki | Sinya Aoki, Tetsuya Onogi, Shuichi Yokoyama | What does a quantum black hole look like? | 15 pages, 4 figures. v2: 16 pages, 4 figures, comment on entropy and
a reference added, a figure and discussion improved. v3: published version in
PLB | null | 10.1016/j.physletb.2021.136104 | YITP-20-24, OU-HET-1044 | hep-th gr-qc hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We take a first step towards a holographic description of a black hole by
means of a flow equation. We consider a free theory of multiple scalar fields
at finite temperature and study its holographic geometry defined through a free
flow of the scalar fields. We find that the holographic metric has the
following prope... | [
{
"created": "Wed, 8 Apr 2020 02:42:57 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jun 2020 06:52:42 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Jan 2021 08:13:38 GMT",
"version": "v3"
}
] | 2021-02-03 | [
[
"Aoki",
"Sinya",
""
],
[
"Onogi",
"Tetsuya",
""
],
[
"Yokoyama",
"Shuichi",
""
]
] | We take a first step towards a holographic description of a black hole by means of a flow equation. We consider a free theory of multiple scalar fields at finite temperature and study its holographic geometry defined through a free flow of the scalar fields. We find that the holographic metric has the following propert... | 10.273867 | 10.167544 | 10.417509 | 10.034497 | 9.90061 | 10.129574 | 10.389803 | 9.8915 | 10.120944 | 10.796773 | 9.328248 | 9.72594 | 10.291331 | 9.812516 | 10.121366 | 9.660465 | 9.711825 | 9.830734 | 10.094028 | 10.137633 | 9.390375 |
hep-th/0201245 | Giovanni Amelino-Camelia | Giovanni Amelino-Camelia, Dario Benedetti, Francesco D'Andrea, Andrea
Procaccini | Comparison of relativity theories with observer-independent scales of
both velocity and length/mass | 21 pages, LaTex. v2: Andrea Procaccini (contributing some results
from hia Laurea thesis) is added to the list of authors and the paper
provides further elements of comparison between DSR1 and DSR2, including the
observation that both lead to the same formula for the dependence of momentum
on rapidity | Class.Quant.Grav.20:5353-5370,2003 | 10.1088/0264-9381/20/24/008 | null | hep-th gr-qc | null | We consider the two most studied proposals of relativity theories with
observer-independent scales of both velocity and length/mass: the one discussed
by Amelino-Camelia as illustrative example for the original proposal
(gr-qc/0012051) of theories with two relativistic invariants, and an
alternative more recently pro... | [
{
"created": "Wed, 30 Jan 2002 07:10:32 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Oct 2003 13:44:59 GMT",
"version": "v2"
}
] | 2011-09-13 | [
[
"Amelino-Camelia",
"Giovanni",
""
],
[
"Benedetti",
"Dario",
""
],
[
"D'Andrea",
"Francesco",
""
],
[
"Procaccini",
"Andrea",
""
]
] | We consider the two most studied proposals of relativity theories with observer-independent scales of both velocity and length/mass: the one discussed by Amelino-Camelia as illustrative example for the original proposal (gr-qc/0012051) of theories with two relativistic invariants, and an alternative more recently propo... | 9.260837 | 10.207904 | 10.009422 | 9.149196 | 9.65325 | 10.156579 | 10.9776 | 9.095043 | 9.868195 | 10.22414 | 9.684144 | 9.440691 | 9.436776 | 9.295413 | 9.562938 | 9.725121 | 9.708862 | 9.510075 | 9.04374 | 9.047428 | 9.283051 |
1912.10688 | Andrea Santi | Andrea Santi | Remarks on highly supersymmetric backgrounds of 11-dimensional
supergravity | 23 pages (v2: a couple of typos fixed, to appear on the Proceedings
of the Abel Symposium 2019 "Geometry, Lie Theory and Applications") | Proceedings of the Abel Symposium 2019 Geometry, Lie Theory and
Applications, Springer series Abel Symposia (2022), 253-277 | null | null | hep-th math.DG math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This note focuses on some properties and uses of filtered deformations in the
context of D=11 supergravity. We define the concept of abstract symbol and give
a strong version of the Reconstruction Theorem, namely a bijective
correspondence from the space of highly supersymmetric supergravity backgrounds
to the space ... | [
{
"created": "Mon, 23 Dec 2019 08:53:15 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Jun 2020 09:46:05 GMT",
"version": "v2"
}
] | 2022-08-23 | [
[
"Santi",
"Andrea",
""
]
] | This note focuses on some properties and uses of filtered deformations in the context of D=11 supergravity. We define the concept of abstract symbol and give a strong version of the Reconstruction Theorem, namely a bijective correspondence from the space of highly supersymmetric supergravity backgrounds to the space of... | 11.424695 | 11.798592 | 14.552218 | 11.78089 | 13.151385 | 12.980368 | 12.454065 | 12.157593 | 12.342028 | 15.175159 | 11.056463 | 10.728416 | 11.968422 | 10.976645 | 11.810587 | 11.554361 | 11.14653 | 10.934191 | 10.680712 | 12.022381 | 11.331015 |
hep-th/0602071 | Steven Thomas | Steven Thomas and John Ward | Electrified Fuzzy Spheres and Funnels in Curved Backgrounds | 38 pages, Latex; references added | JHEP 0611:019,2006 | 10.1088/1126-6708/2006/11/019 | QMUL-PH-06-02 | hep-th | null | We use the non-Abelian DBI action to study the dynamics of $N$ coincident
$Dp$-branes in an arbitrary curved background, with the presence of a
homogenous world-volume electric field. The solutions are natural extensions of
those without electric fields, and imply that the spheres will collapse toward
zero size. We t... | [
{
"created": "Tue, 7 Feb 2006 17:10:20 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Feb 2006 14:54:36 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Thomas",
"Steven",
""
],
[
"Ward",
"John",
""
]
] | We use the non-Abelian DBI action to study the dynamics of $N$ coincident $Dp$-branes in an arbitrary curved background, with the presence of a homogenous world-volume electric field. The solutions are natural extensions of those without electric fields, and imply that the spheres will collapse toward zero size. We the... | 10.352315 | 10.098284 | 11.21981 | 10.021983 | 10.289649 | 10.994458 | 10.496137 | 9.752882 | 9.991392 | 11.316555 | 9.704231 | 10.068966 | 10.687322 | 10.133545 | 10.207325 | 10.013523 | 10.030099 | 9.983358 | 10.140433 | 10.306816 | 9.932907 |
0902.2700 | Ralf Hofmann | Ralf Hofmann | Low-frequency line temperatures of the CMB | v2: 9 pages, 1 figure, extended discussion of why prsent photon mass
bounds are not in contradiction to a low-temperature, low-frequency Meissner
mass responsible for UEGE, matches journal version | Annalen Phys.18:634-639,2009 | 10.1002/andp.200910361 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on SU(2) Yang-Mills thermodynamics we interprete Aracde2's and the
results of earlier radio-surveys on low-frequency CMB line temperatures as a
phase-boundary effect. We explain the excess at low frequencies by evanescent,
nonthermal photon fields of the CMB whose intensity is nulled by that of Planck
distribut... | [
{
"created": "Mon, 16 Feb 2009 14:34:59 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Jul 2009 12:38:39 GMT",
"version": "v2"
}
] | 2009-12-04 | [
[
"Hofmann",
"Ralf",
""
]
] | Based on SU(2) Yang-Mills thermodynamics we interprete Aracde2's and the results of earlier radio-surveys on low-frequency CMB line temperatures as a phase-boundary effect. We explain the excess at low frequencies by evanescent, nonthermal photon fields of the CMB whose intensity is nulled by that of Planck distributed... | 43.554554 | 53.211582 | 43.416286 | 41.912727 | 46.360428 | 46.506329 | 46.388092 | 54.815685 | 43.225719 | 47.681976 | 40.785213 | 41.927086 | 45.466187 | 43.602036 | 46.977924 | 44.361752 | 41.30616 | 42.901596 | 42.55167 | 42.263172 | 42.299732 |
1005.5051 | Petya Nedkova | Petya G. Nedkova, Stoytcho S. Yazadjiev | Rotating black ring on Kaluza-Klein bubbles | 26 pages, 4 figures; v2: a new limit case added; references and
comments added | Phys.Rev.D82:044010,2010 | 10.1103/PhysRevD.82.044010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a new exact solution to the 5D Einstein equations describing
rotating black ring with a single angular momentum surrounded by two
Kaluza-Klein bubbles. The solution is generated by 2-soliton B\"{a}cklund
transformation. Its physical properties are computed and analyzed. The
corresponding static solution,... | [
{
"created": "Thu, 27 May 2010 12:47:35 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Jun 2010 15:53:29 GMT",
"version": "v2"
}
] | 2015-03-17 | [
[
"Nedkova",
"Petya G.",
""
],
[
"Yazadjiev",
"Stoytcho S.",
""
]
] | We construct a new exact solution to the 5D Einstein equations describing rotating black ring with a single angular momentum surrounded by two Kaluza-Klein bubbles. The solution is generated by 2-soliton B\"{a}cklund transformation. Its physical properties are computed and analyzed. The corresponding static solution, t... | 10.950613 | 8.249866 | 8.33144 | 8.054705 | 9.132867 | 8.006896 | 8.653158 | 8.75813 | 8.052649 | 9.8283 | 9.537626 | 9.620576 | 9.735465 | 9.570585 | 9.434974 | 9.686625 | 9.733413 | 9.062637 | 9.36217 | 9.6342 | 9.609963 |
1908.10996 | Raghu Mahajan | Ahmed Almheiri, Raghu Mahajan, Juan Maldacena, Ying Zhao | The Page curve of Hawking radiation from semiclassical geometry | 21 pages, 12 figures | null | 10.1007/JHEP03(2020)149 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a gravity theory coupled to matter, where the matter has a
higher-dimensional holographic dual. In such a theory, finding quantum extremal
surfaces becomes equivalent to finding the RT/HRT surfaces in the
higher-dimensional theory. Using this we compute the entropy of Hawking
radiation and argue that it f... | [
{
"created": "Thu, 29 Aug 2019 00:37:46 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Nov 2019 16:40:19 GMT",
"version": "v2"
}
] | 2020-04-22 | [
[
"Almheiri",
"Ahmed",
""
],
[
"Mahajan",
"Raghu",
""
],
[
"Maldacena",
"Juan",
""
],
[
"Zhao",
"Ying",
""
]
] | We consider a gravity theory coupled to matter, where the matter has a higher-dimensional holographic dual. In such a theory, finding quantum extremal surfaces becomes equivalent to finding the RT/HRT surfaces in the higher-dimensional theory. Using this we compute the entropy of Hawking radiation and argue that it fol... | 9.500908 | 8.778879 | 10.75635 | 8.445273 | 9.009945 | 9.082947 | 8.441624 | 9.832129 | 8.865911 | 11.821576 | 8.591768 | 9.117264 | 9.824568 | 9.014436 | 8.979123 | 8.786529 | 8.696944 | 8.931437 | 8.949944 | 9.806376 | 8.638441 |
1503.07584 | Alexi Morin-Duchesne | Alexi Morin-Duchesne, Jorgen Rasmussen, David Ridout | Boundary algebras and Kac modules for logarithmic minimal models | 71 pages. v3: version published in Nucl. Phys. B | null | 10.1016/j.nuclphysb.2015.08.017 | null | hep-th cond-mat.stat-mech math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Virasoro Kac modules were initially introduced indirectly as representations
whose characters arise in the continuum scaling limits of certain transfer
matrices in logarithmic minimal models, described using Temperley-Lieb
algebras. The lattice transfer operators include seams on the boundary that use
Wenzl-Jones pro... | [
{
"created": "Wed, 25 Mar 2015 23:55:03 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Apr 2015 10:41:23 GMT",
"version": "v2"
},
{
"created": "Wed, 16 Sep 2015 11:05:30 GMT",
"version": "v3"
}
] | 2015-12-09 | [
[
"Morin-Duchesne",
"Alexi",
""
],
[
"Rasmussen",
"Jorgen",
""
],
[
"Ridout",
"David",
""
]
] | Virasoro Kac modules were initially introduced indirectly as representations whose characters arise in the continuum scaling limits of certain transfer matrices in logarithmic minimal models, described using Temperley-Lieb algebras. The lattice transfer operators include seams on the boundary that use Wenzl-Jones proje... | 9.156009 | 10.047727 | 11.063614 | 9.311737 | 10.398125 | 9.019567 | 9.878218 | 9.41647 | 9.634392 | 12.423934 | 9.329926 | 9.419505 | 9.508615 | 8.892499 | 9.47817 | 9.500962 | 9.318066 | 9.039078 | 9.266294 | 9.722531 | 9.015439 |
hep-th/0105053 | Kazunori Takenaga | K. Takenaga (Dublin Inst.) | Dynamics of Nonintegrable Phases in Softly Broken Supersymmetric Gauge
Theory with Massless Adjoint Matter | 19 pages, 2 figures, corrected some typos | Phys.Rev. D64 (2001) 066001 | 10.1103/PhysRevD.64.066001 | DIAS-STP-01-05 | hep-th | null | We study SU(N) supersymmetric Yang-Mills theory with massless adjoint matter
defined on $M^3\otimes S^1$. The SU(N) gauge symmetry is broken maximally to
$U(1)^{N-1}$, independent of the number of flavor and the boundary conditions
of the fields associated with the Scherk-Schwarz mechanism of supersymmetry
breaking. ... | [
{
"created": "Sun, 6 May 2001 14:15:48 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Jul 2001 14:10:57 GMT",
"version": "v2"
},
{
"created": "Sun, 15 Jul 2001 11:25:12 GMT",
"version": "v3"
},
{
"created": "Thu, 9 Aug 2001 12:49:44 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Takenaga",
"K.",
"",
"Dublin Inst."
]
] | We study SU(N) supersymmetric Yang-Mills theory with massless adjoint matter defined on $M^3\otimes S^1$. The SU(N) gauge symmetry is broken maximally to $U(1)^{N-1}$, independent of the number of flavor and the boundary conditions of the fields associated with the Scherk-Schwarz mechanism of supersymmetry breaking. Th... | 8.037188 | 7.385998 | 7.486283 | 7.071898 | 7.08067 | 7.262616 | 7.465643 | 6.606925 | 7.182524 | 7.942414 | 7.332223 | 7.149261 | 7.184517 | 7.06334 | 7.173899 | 7.267325 | 7.380588 | 7.408683 | 7.158957 | 7.626561 | 7.4223 |
0803.3085 | Eva Silverstein | Eva Silverstein and Alexander Westphal | Monodromy in the CMB: Gravity Waves and String Inflation | 43 pages, latex. 4 figures | Phys.Rev.D78:106003,2008 | 10.1103/PhysRevD.78.106003 | SU-ITP-08/07, SLAC-PUB-13183 | hep-th astro-ph hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a simple mechanism for obtaining large-field inflation, and hence
a gravitational wave signature, from string theory compactified on twisted
tori. For Nil manifolds, we obtain a leading inflationary potential
proportional to phi^(2/3) in terms of the canonically normalized field phi,
yielding predictions f... | [
{
"created": "Fri, 21 Mar 2008 16:26:35 GMT",
"version": "v1"
},
{
"created": "Sun, 23 Mar 2008 20:25:21 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Silverstein",
"Eva",
""
],
[
"Westphal",
"Alexander",
""
]
] | We present a simple mechanism for obtaining large-field inflation, and hence a gravitational wave signature, from string theory compactified on twisted tori. For Nil manifolds, we obtain a leading inflationary potential proportional to phi^(2/3) in terms of the canonically normalized field phi, yielding predictions for... | 9.256026 | 9.707147 | 10.838653 | 9.343432 | 9.039772 | 9.86464 | 10.175128 | 9.186009 | 9.776843 | 11.086222 | 9.474704 | 9.671908 | 9.683151 | 9.054754 | 9.398208 | 9.037317 | 9.512597 | 9.107794 | 9.094929 | 9.287471 | 8.752308 |
0811.0218 | Sergei Kuzenko | Sergei M. Kuzenko, Joseph Novak | Chiral formulation for hyperkaehler sigma-models on cotangent bundles of
symmetric spaces | 11 pages, LaTeX, no figues | JHEP 0812:072,2008 | 10.1088/1126-6708/2008/12/072 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Starting with the projective-superspace off-shell formulation for
four-dimensional N = 2 supersymmetric sigma-models on cotangent bundles of
arbitrary Hermitian symmetric spaces, their on-shell description in terms of N
= 1 chiral superfields is developed. In particular, we derive a universal
representation for the h... | [
{
"created": "Mon, 3 Nov 2008 11:32:10 GMT",
"version": "v1"
}
] | 2009-02-10 | [
[
"Kuzenko",
"Sergei M.",
""
],
[
"Novak",
"Joseph",
""
]
] | Starting with the projective-superspace off-shell formulation for four-dimensional N = 2 supersymmetric sigma-models on cotangent bundles of arbitrary Hermitian symmetric spaces, their on-shell description in terms of N = 1 chiral superfields is developed. In particular, we derive a universal representation for the hyp... | 8.338181 | 6.557458 | 8.601588 | 6.983137 | 6.203872 | 7.0637 | 7.372757 | 6.747102 | 6.814859 | 10.187712 | 6.890465 | 7.424452 | 8.216379 | 7.540696 | 7.593899 | 7.814675 | 7.686106 | 7.326442 | 7.501934 | 8.583103 | 7.505052 |
2111.01106 | Sylvain Ribault | Linnea Grans-Samuelsson, Rongvoram Nivesvivat, Jesper Lykke Jacobsen,
Sylvain Ribault, Hubert Saleur | Global symmetry and conformal bootstrap in the two-dimensional $O(n)$
model | 49 pages, v3: improved explanations on a few points | SciPost Phys. 12, 147 (2022) | 10.21468/SciPostPhys.12.5.147 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define the two-dimensional $O(n)$ conformal field theory as a theory that
includes the critical dilute and dense $O(n)$ models as special cases, and
depends analytically on the central charge. For generic values of
$n\in\mathbb{C}$, we write a conjecture for the decomposition of the spectrum
into irreducible repre... | [
{
"created": "Mon, 1 Nov 2021 17:20:53 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jan 2022 09:26:45 GMT",
"version": "v2"
},
{
"created": "Tue, 22 Mar 2022 13:10:21 GMT",
"version": "v3"
}
] | 2022-05-11 | [
[
"Grans-Samuelsson",
"Linnea",
""
],
[
"Nivesvivat",
"Rongvoram",
""
],
[
"Jacobsen",
"Jesper Lykke",
""
],
[
"Ribault",
"Sylvain",
""
],
[
"Saleur",
"Hubert",
""
]
] | We define the two-dimensional $O(n)$ conformal field theory as a theory that includes the critical dilute and dense $O(n)$ models as special cases, and depends analytically on the central charge. For generic values of $n\in\mathbb{C}$, we write a conjecture for the decomposition of the spectrum into irreducible represe... | 7.129375 | 7.26458 | 8.188514 | 7.341918 | 7.039321 | 6.975529 | 7.549293 | 6.854977 | 7.106276 | 8.690919 | 7.154447 | 6.85009 | 7.787226 | 6.948553 | 7.1594 | 7.247694 | 7.092764 | 7.04087 | 6.900727 | 7.873507 | 7.079686 |
1107.3139 | Marco Stefano Bianchi | Marco S. Bianchi, Matias Leoni, Andrea Mauri, Silvia Penati and
Alberto Santambrogio | Scattering Amplitudes/Wilson Loop Duality In ABJM Theory | 1+16 pages, 2 figures, minor modifications and references added | null | 10.1007/JHEP01(2012)056 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For N=6 superconformal Chern-Simons-matter theories in three dimensions, by a
direct superspace Feynman diagram approach, we compute the two-loop four-point
scattering amplitude with external chiral matter fields. We find that the
result is in perfect agreement with the two-loop result for a light-like
four-polygon W... | [
{
"created": "Fri, 15 Jul 2011 19:50:03 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Oct 2011 13:36:07 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Bianchi",
"Marco S.",
""
],
[
"Leoni",
"Matias",
""
],
[
"Mauri",
"Andrea",
""
],
[
"Penati",
"Silvia",
""
],
[
"Santambrogio",
"Alberto",
""
]
] | For N=6 superconformal Chern-Simons-matter theories in three dimensions, by a direct superspace Feynman diagram approach, we compute the two-loop four-point scattering amplitude with external chiral matter fields. We find that the result is in perfect agreement with the two-loop result for a light-like four-polygon Wil... | 7.30614 | 7.027937 | 8.547862 | 6.784501 | 6.225804 | 6.458105 | 6.229785 | 6.269108 | 6.535965 | 9.198255 | 6.685674 | 6.907289 | 7.08091 | 6.869719 | 6.819813 | 6.926672 | 6.949391 | 6.813028 | 6.816132 | 7.031831 | 6.638257 |
2012.00030 | Stephen G. Naculich | Stephen G. Naculich | All-loop-orders relation between Regge limits of ${\cal N}=4$ SYM and
${\cal N}=8$ supergravity four-point amplitudes | 34 pages; v2: clarification added, minor typos corrected, published
version | null | 10.1007/JHEP02(2021)044 | BOW-PH-169 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine in detail the structure of the Regge limit of the (nonplanar)
${\cal N}=4$ SYM four-point amplitude. We begin by developing a basis of color
factors $C_{ik}$ suitable for the Regge limit of the amplitude at any loop
order, and then calculate explicitly the coefficients of the amplitude in that
basis throug... | [
{
"created": "Mon, 30 Nov 2020 19:00:08 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Feb 2021 21:31:27 GMT",
"version": "v2"
}
] | 2021-02-24 | [
[
"Naculich",
"Stephen G.",
""
]
] | We examine in detail the structure of the Regge limit of the (nonplanar) ${\cal N}=4$ SYM four-point amplitude. We begin by developing a basis of color factors $C_{ik}$ suitable for the Regge limit of the amplitude at any loop order, and then calculate explicitly the coefficients of the amplitude in that basis through ... | 6.085396 | 6.978952 | 6.588517 | 6.264813 | 6.505142 | 6.962136 | 6.779428 | 6.921292 | 6.309198 | 6.734338 | 6.344419 | 5.956608 | 5.912491 | 5.900009 | 6.083227 | 5.943329 | 6.318236 | 6.002593 | 5.868961 | 5.893189 | 6.167859 |
1612.03915 | Adam Bzowski | Adam Bzowski | Dimensional renormalization in AdS/CFT | 60 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we present a dimensional renormalization scheme suitable for
holographic theories. We use the bulk physics in the supergravity limit as a
definition of the dual CFT. Similar to the perturbative quantization of a QFT,
one is free to choose a convenient renormalization scheme, and the holographic
renormal... | [
{
"created": "Mon, 12 Dec 2016 21:00:04 GMT",
"version": "v1"
}
] | 2016-12-14 | [
[
"Bzowski",
"Adam",
""
]
] | In this paper we present a dimensional renormalization scheme suitable for holographic theories. We use the bulk physics in the supergravity limit as a definition of the dual CFT. Similar to the perturbative quantization of a QFT, one is free to choose a convenient renormalization scheme, and the holographic renormaliz... | 8.247924 | 8.429713 | 8.995993 | 8.092306 | 8.871124 | 8.281929 | 8.203169 | 8.475531 | 7.572964 | 9.222339 | 8.089828 | 7.998616 | 8.259412 | 7.95055 | 7.76616 | 8.147341 | 7.820302 | 8.170736 | 7.772273 | 8.068342 | 7.889874 |
1012.2554 | Ali Imaanpur | A. Imaanpur and M. Naghdi | Dual Instantons in Anti-membranes Theory | 14 pages, minor changes, added refs | Phys.Rev.D83:085025,2011 | 10.1103/PhysRevD.83.085025 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce two ansatzs for the 3-form potential of Euclidean 11d
supergravity on skew-whiffed AdS_4 X S^7 background which results in two scalar
modes with m^2=-2 on AdS_4. Being conformally coupled with a quartic
interaction it is possible to find the exact solutions of the scalar equation
on this background. Thes... | [
{
"created": "Sun, 12 Dec 2010 16:29:54 GMT",
"version": "v1"
},
{
"created": "Sun, 24 Apr 2011 09:43:34 GMT",
"version": "v2"
}
] | 2011-05-12 | [
[
"Imaanpur",
"A.",
""
],
[
"Naghdi",
"M.",
""
]
] | We introduce two ansatzs for the 3-form potential of Euclidean 11d supergravity on skew-whiffed AdS_4 X S^7 background which results in two scalar modes with m^2=-2 on AdS_4. Being conformally coupled with a quartic interaction it is possible to find the exact solutions of the scalar equation on this background. These ... | 10.528802 | 10.724627 | 12.020267 | 9.930946 | 10.288662 | 9.766781 | 9.604645 | 9.94699 | 10.097709 | 12.947965 | 9.979874 | 10.228354 | 10.386172 | 10.093801 | 10.454693 | 9.831484 | 10.164573 | 10.118304 | 10.001929 | 10.32131 | 9.942277 |
1508.04764 | Massimo Taronna | E.D. Skvortsov and Massimo Taronna | On Locality, Holography and Unfolding | 36 pages, LaTex. References added, typos corrected. Final version to
appear in JHEP | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the functional class and locality problems in the context of
higher-spin theories and Vasiliev's equations. A locality criterion that is
sufficient to make higher-spin theories well-defined as field theories on
Anti-de-Sitter space is proposed. This criterion identifies admissible
pseudo-local field redefini... | [
{
"created": "Wed, 19 Aug 2015 20:03:30 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Nov 2015 17:26:18 GMT",
"version": "v2"
}
] | 2015-11-04 | [
[
"Skvortsov",
"E. D.",
""
],
[
"Taronna",
"Massimo",
""
]
] | We study the functional class and locality problems in the context of higher-spin theories and Vasiliev's equations. A locality criterion that is sufficient to make higher-spin theories well-defined as field theories on Anti-de-Sitter space is proposed. This criterion identifies admissible pseudo-local field redefiniti... | 16.586201 | 17.239073 | 17.311741 | 14.896937 | 15.686642 | 14.523993 | 16.980362 | 14.401402 | 15.197078 | 19.750271 | 14.419271 | 15.537334 | 17.109093 | 14.918047 | 14.784441 | 15.211066 | 14.355115 | 15.219233 | 15.068845 | 16.458158 | 14.398417 |
0811.4177 | Noriaki Ogawa | Tatsuo Azeyanagi, Noriaki Ogawa and Seiji Terashima | Holographic Duals of Kaluza-Klein Black Holes | 21 pages, LaTeX; v2: metadata corrected, v3: minor corrections,
references added, v4: minor corrections (mainly on boundary conditions), v5:
minor corrections, references added, published in JHEP | JHEP 0904:061,2009 | 10.1088/1126-6708/2009/04/061 | KUNS-2169, YITP-08-88 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply Brown-Henneaux's method to the 5D extremal rotating Kaluza-Klein
black holes essentially following the calculation of the Kerr/CFT
correspondence, which is not based on supersymmetry nor string theory. We find
that there are two completely different Virasoro algebras that can be obtained
as the asymptotic sy... | [
{
"created": "Wed, 26 Nov 2008 20:54:44 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Nov 2008 00:31:29 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Dec 2008 12:34:31 GMT",
"version": "v3"
},
{
"created": "Mon, 29 Dec 2008 18:04:24 GMT",
"version": "v4"
},
{
"c... | 2009-04-19 | [
[
"Azeyanagi",
"Tatsuo",
""
],
[
"Ogawa",
"Noriaki",
""
],
[
"Terashima",
"Seiji",
""
]
] | We apply Brown-Henneaux's method to the 5D extremal rotating Kaluza-Klein black holes essentially following the calculation of the Kerr/CFT correspondence, which is not based on supersymmetry nor string theory. We find that there are two completely different Virasoro algebras that can be obtained as the asymptotic symm... | 7.098433 | 6.691896 | 7.228068 | 6.319956 | 7.149005 | 6.57626 | 6.985653 | 6.547406 | 6.39901 | 7.544388 | 6.503543 | 6.682117 | 7.005738 | 6.712487 | 6.778421 | 6.619764 | 6.65169 | 6.555924 | 6.620312 | 6.885588 | 6.526931 |
hep-th/9804190 | Norbert Scheu | Norbert Scheu | On the Computation of Mass Spectra and Structure Functions in a
Relativistic Hamiltonian Formalism: A Lattice Point of View | LaTeX2e. Macros: amssymb,amsmath,amscd,psfig,makeidx,pifont,
tabularx,cite,floatflt,multirow, Abstract modified | null | null | ULaval-Laphyt-April-98 | hep-th hep-lat hep-ph | null | Herein we propose a new numerical technique for solving field theories: the
large momentum frame (LMF). This technique combines several advantages of
lattice gauge theory with the simplicity of front form quantisation. We apply
the LMF on QED(1+1) and on the $\phi^4(3+1)$ theory. We demonstrate both
analytically and ... | [
{
"created": "Wed, 29 Apr 1998 04:05:33 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Apr 1998 19:07:37 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Scheu",
"Norbert",
""
]
] | Herein we propose a new numerical technique for solving field theories: the large momentum frame (LMF). This technique combines several advantages of lattice gauge theory with the simplicity of front form quantisation. We apply the LMF on QED(1+1) and on the $\phi^4(3+1)$ theory. We demonstrate both analytically and in... | 8.993012 | 9.41984 | 9.128969 | 9.058507 | 9.671122 | 10.138386 | 9.166908 | 9.619156 | 8.782652 | 9.575401 | 8.957119 | 8.972178 | 8.511945 | 8.531079 | 8.676926 | 9.007243 | 8.957241 | 8.709172 | 8.502913 | 8.762947 | 8.688375 |
hep-th/0212167 | Andreas Gustavsson | Andreas Gustavsson | Classical self-dual strings in d=6, (2,0) theory from afar | 13 pages, clarifications and added references | JHEP 0301 (2003) 019 | 10.1088/1126-6708/2003/01/019 | null | hep-th | null | We show how one can get solitonic strings in a six-dimensional (2,0)
supersymmetric theory by incorporating a nonlinear interaction term. We derive
a zero force condition between parallel strings, and compute a metric on a
moduli space which is $R^4$ when the strings are far apart. When compactifying
the strings on a... | [
{
"created": "Mon, 16 Dec 2002 08:32:17 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Dec 2002 11:42:09 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Gustavsson",
"Andreas",
""
]
] | We show how one can get solitonic strings in a six-dimensional (2,0) supersymmetric theory by incorporating a nonlinear interaction term. We derive a zero force condition between parallel strings, and compute a metric on a moduli space which is $R^4$ when the strings are far apart. When compactifying the strings on a t... | 11.52186 | 9.953773 | 12.884383 | 10.258625 | 10.523321 | 10.067672 | 9.644984 | 10.113056 | 10.30064 | 12.312909 | 9.80735 | 10.128939 | 11.024237 | 10.605083 | 10.226283 | 10.232057 | 10.006454 | 10.575049 | 10.61369 | 11.505949 | 10.043839 |
1707.00512 | Johar Muhammad Ashfaque | Johar M. Ashfaque | Free-Fermionic $SO(8)$ And tri$(\mathbb{O})$ | 15 pages. arXiv admin note: text overlap with arXiv:1309.0546 by
other authors | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note, we speculate about the fundamental role being played by the
$SO(8)$ group representations displaying the triality structure that
necessarily arise in models constructed under the free fermionic methodology as
being remnants of the higher-dimensional triality algebra tri$(\mathbb{O}) =
\mathfrak{so}(8)$.... | [
{
"created": "Fri, 16 Jun 2017 11:05:16 GMT",
"version": "v1"
}
] | 2017-07-04 | [
[
"Ashfaque",
"Johar M.",
""
]
] | In this note, we speculate about the fundamental role being played by the $SO(8)$ group representations displaying the triality structure that necessarily arise in models constructed under the free fermionic methodology as being remnants of the higher-dimensional triality algebra tri$(\mathbb{O}) = \mathfrak{so}(8)$. | 29.211153 | 23.829496 | 25.578983 | 23.793652 | 27.214634 | 23.407883 | 23.959768 | 25.805414 | 24.054348 | 29.700102 | 23.311342 | 24.717865 | 23.671461 | 23.652134 | 23.519993 | 23.62253 | 23.696856 | 24.826265 | 24.524935 | 23.829054 | 23.842743 |
1805.07279 | Joris Raeymaekers | Pan Kessel and Joris Raeymaekers | Simple Unfolded Equations for Massive Higher Spins in AdS$_3$ | 21 pages plus appendices. V2: typos corrected, references added,
published version | JHEP 1808 (2018) 076 | 10.1007/JHEP08(2018)076 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a simple unfolded description of free massive higher spin
particles in anti-de-Sitter spacetime. While our unfolded equation of motion
has the standard form of a covariant constancy condition, our formulation
differs from the standard one in that our field takes values in a different
internal space, which ... | [
{
"created": "Fri, 18 May 2018 15:20:16 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Aug 2018 17:23:32 GMT",
"version": "v2"
}
] | 2018-08-29 | [
[
"Kessel",
"Pan",
""
],
[
"Raeymaekers",
"Joris",
""
]
] | We propose a simple unfolded description of free massive higher spin particles in anti-de-Sitter spacetime. While our unfolded equation of motion has the standard form of a covariant constancy condition, our formulation differs from the standard one in that our field takes values in a different internal space, which fo... | 9.085552 | 8.6397 | 9.410264 | 8.234474 | 8.162123 | 8.78191 | 8.391641 | 8.262859 | 8.622445 | 9.960558 | 8.710149 | 8.140583 | 9.043785 | 8.206898 | 8.17361 | 8.287137 | 8.397962 | 8.228144 | 8.245898 | 9.364318 | 8.146575 |
hep-th/0312169 | Ricardo Moritz Cavalcanti | F. A. Barone, R. M. Cavalcanti and C. Farina | Radiative corrections to the Casimir energy in the $\lambda|\phi|^{4}$
model under quasi-periodic boundary conditions | 6 pages, 2 figures. Work presented at the XXIV Brazilian National
Meeting on Particles and Fields (Caxambu, Brazil, 30 Sep - 4 Oct 2003) | null | null | null | hep-th | null | We compute the first radiative correction to the Casimir energy in the
$(d+1)$-dimensional $\lambda|\phi|^{4}$ model submitted to quasi-periodic
boundary conditions in one spatial direction. Our results agree with the ones
found in the literature for periodic and anti-periodic boundary conditions,
special cases of th... | [
{
"created": "Mon, 15 Dec 2003 19:53:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Barone",
"F. A.",
""
],
[
"Cavalcanti",
"R. M.",
""
],
[
"Farina",
"C.",
""
]
] | We compute the first radiative correction to the Casimir energy in the $(d+1)$-dimensional $\lambda|\phi|^{4}$ model submitted to quasi-periodic boundary conditions in one spatial direction. Our results agree with the ones found in the literature for periodic and anti-periodic boundary conditions, special cases of the ... | 6.892203 | 4.464453 | 6.467528 | 4.916605 | 4.898613 | 4.640429 | 4.54543 | 4.542091 | 4.845217 | 5.618586 | 4.908016 | 5.485945 | 6.114486 | 5.638249 | 5.523882 | 5.330717 | 5.262893 | 5.256675 | 5.559995 | 6.093711 | 5.343187 |
1906.10715 | Sam van Leuven | Shinji Hirano, Yang Lei, Sam van Leuven | Information Transfer and Black Hole Evaporation via Traversable BTZ
Wormholes | 27+5 pages, 11 figures, v2: added ref + corrected typos in section 2 | null | 10.1007/JHEP09(2019)070 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study traversable wormholes by considering the duality between BTZ black
holes and two-dimensional conformal field theory on the thermofield double
state. The BTZ black holes can be rendered traversable by a negative energy
shock wave. Following Gao, Jafferis and Wall [1], we show that the negative
energy shock wa... | [
{
"created": "Tue, 25 Jun 2019 18:22:05 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Jul 2019 08:50:19 GMT",
"version": "v2"
}
] | 2019-09-30 | [
[
"Hirano",
"Shinji",
""
],
[
"Lei",
"Yang",
""
],
[
"van Leuven",
"Sam",
""
]
] | We study traversable wormholes by considering the duality between BTZ black holes and two-dimensional conformal field theory on the thermofield double state. The BTZ black holes can be rendered traversable by a negative energy shock wave. Following Gao, Jafferis and Wall [1], we show that the negative energy shock wave... | 8.52852 | 8.551983 | 10.186726 | 8.036673 | 8.177533 | 8.498306 | 8.240215 | 8.085544 | 7.532012 | 11.092636 | 8.09221 | 7.947009 | 8.96775 | 8.322096 | 8.245283 | 7.97153 | 8.158705 | 8.283475 | 7.986483 | 9.265686 | 7.858406 |
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