id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1110.5075 | Paul McGuirk | Paul McGuirk | Hidden-sector current-current correlators in holographic gauge mediation | 46 pages. Typographical errors corrected and clarifications added.
Version to appear in PRD | Phys. Rev. D 85, 045025 (2012) | 10.1103/PhysRevD.85.045025 | MAD-TH-11-08 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss gauge mediation in the case where the hidden sector is strongly
coupled but, via the gauge-gravity correspondence, admits a weakly-coupled
description in terms of a warped higher-dimensional spacetime. In this
framework, known as holographic gauge mediation, the visible-sector gauge group
is realized in th... | [
{
"created": "Sun, 23 Oct 2011 19:12:37 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Oct 2011 17:02:34 GMT",
"version": "v2"
},
{
"created": "Fri, 13 Jan 2012 16:47:59 GMT",
"version": "v3"
}
] | 2012-02-17 | [
[
"McGuirk",
"Paul",
""
]
] | We discuss gauge mediation in the case where the hidden sector is strongly coupled but, via the gauge-gravity correspondence, admits a weakly-coupled description in terms of a warped higher-dimensional spacetime. In this framework, known as holographic gauge mediation, the visible-sector gauge group is realized in the ... | 9.449625 | 10.966598 | 10.504578 | 9.698409 | 10.218636 | 10.730836 | 10.856468 | 10.399275 | 9.611666 | 10.712644 | 9.475491 | 9.146155 | 9.937708 | 9.412311 | 9.680845 | 9.44986 | 9.738929 | 9.464898 | 9.663347 | 10.14699 | 9.576175 |
hep-th/0403093 | Brett D. Altschul | B. Altschul | Nonpolynomial Normal Modes of the Renormalization Group in the Presence
of a Constant Vector Potential Background | 12 pages | Nucl.Phys. B705 (2005) 593-604 | 10.1016/j.nuclphysb.2004.10.054 | IUHET-467 | hep-th | null | We examine the renormalization group flow in the vicinity of the free-field
fixed point for effective field theories in the presence of a constant,
nondynamical vector potential background. The interaction with this vector
potential represents the simplest possible form of Lorentz violation. We search
for any normal ... | [
{
"created": "Mon, 8 Mar 2004 20:07:41 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Altschul",
"B.",
""
]
] | We examine the renormalization group flow in the vicinity of the free-field fixed point for effective field theories in the presence of a constant, nondynamical vector potential background. The interaction with this vector potential represents the simplest possible form of Lorentz violation. We search for any normal mo... | 11.050043 | 11.61532 | 11.753417 | 10.993674 | 11.502239 | 11.428435 | 10.830193 | 10.96057 | 10.695292 | 12.008114 | 11.148108 | 10.640849 | 10.807223 | 10.905861 | 10.594074 | 10.955781 | 10.609138 | 10.582371 | 10.725966 | 10.780455 | 10.452121 |
1901.08161 | Simone Speziale | Maciej Dunajski, Miklos L{\aa}ngvik, Simone Speziale | An octahedron of complex null rays, and conformal symmetry breaking | 10 pages, 4 figures. v2: expanded introduction and conclusions | Phys. Rev. D 99, 104064 (2019) | 10.1103/PhysRevD.99.104064 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how the manifold $T^*SU(2, 2)$ arises as a symplectic reduction from
eight copies of the twistor space. Some of the constraints in the twistor space
correspond to an octahedral configuration of twelve complex light rays in the
Minkowski space. We discuss a mechanism to break the conformal symmetry down to
the... | [
{
"created": "Wed, 23 Jan 2019 22:57:42 GMT",
"version": "v1"
},
{
"created": "Thu, 16 May 2019 20:59:23 GMT",
"version": "v2"
}
] | 2019-06-05 | [
[
"Dunajski",
"Maciej",
""
],
[
"Långvik",
"Miklos",
""
],
[
"Speziale",
"Simone",
""
]
] | We show how the manifold $T^*SU(2, 2)$ arises as a symplectic reduction from eight copies of the twistor space. Some of the constraints in the twistor space correspond to an octahedral configuration of twelve complex light rays in the Minkowski space. We discuss a mechanism to break the conformal symmetry down to the t... | 10.78085 | 11.32303 | 11.860951 | 10.059408 | 11.43802 | 11.356787 | 11.041451 | 10.418555 | 10.832547 | 12.576262 | 11.112733 | 10.908545 | 10.981262 | 10.586335 | 10.657925 | 10.30399 | 10.68684 | 10.021025 | 10.281399 | 10.679642 | 9.878724 |
hep-th/0503044 | Paschalis Anastasopoulos | P. Anastasopoulos (Crete U, Ecole Polytechnique) and A. B. Hammou
(Crete U, USTO) | A Classification of Toroidal Orientifold Models | 35 pages, 3 eps figures, Latex2e | Nucl.Phys.B729:49-78,2005 | 10.1016/j.nuclphysb.2005.09.006 | null | hep-th | null | We develop the general tools for model building with orientifolds, including
SS supersymmetry breaking. In this paper, we work out the general formulae of
the tadpole conditions for a class of non supersymmetric orientifold models of
type IIB string theory compactified on $T^6$, based on the general properties
of the... | [
{
"created": "Fri, 4 Mar 2005 17:26:46 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Anastasopoulos",
"P.",
"",
"Crete U, Ecole Polytechnique"
],
[
"Hammou",
"A. B.",
"",
"Crete U, USTO"
]
] | We develop the general tools for model building with orientifolds, including SS supersymmetry breaking. In this paper, we work out the general formulae of the tadpole conditions for a class of non supersymmetric orientifold models of type IIB string theory compactified on $T^6$, based on the general properties of the o... | 10.728765 | 9.287312 | 10.503784 | 8.779323 | 9.602722 | 9.108211 | 9.712094 | 9.01146 | 9.64741 | 11.530981 | 9.519728 | 9.502415 | 10.047556 | 9.243341 | 9.415972 | 9.074252 | 9.00141 | 9.366008 | 9.040961 | 9.417729 | 9.200706 |
0708.1077 | Satoshi Nagaoka | Yoshihisa Kitazawa and Satoshi Nagaoka | Green-Schwarz superstring from type IIB matrix model | 5 pages, 3 figures, minor revisions | Phys.Rev.D77:026009,2008 | 10.1103/PhysRevD.77.026009 | KEK-TH-1168 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct Green-Schwarz (GS) light-cone closed superstring theory from
type IIB matrix model. A GS light-cone string action is derived from two
dimensional N=8 U(n) noncommutative Yang-Mills (NCYM) by identifying
noncommutative scale with string scale. Supersymmetry transformation for the
light-cone gauge action i... | [
{
"created": "Wed, 8 Aug 2007 10:44:37 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Apr 2009 07:01:05 GMT",
"version": "v2"
}
] | 2009-04-01 | [
[
"Kitazawa",
"Yoshihisa",
""
],
[
"Nagaoka",
"Satoshi",
""
]
] | We construct Green-Schwarz (GS) light-cone closed superstring theory from type IIB matrix model. A GS light-cone string action is derived from two dimensional N=8 U(n) noncommutative Yang-Mills (NCYM) by identifying noncommutative scale with string scale. Supersymmetry transformation for the light-cone gauge action is ... | 9.991526 | 8.944607 | 10.568618 | 7.89756 | 8.512592 | 8.330406 | 8.580396 | 8.28223 | 7.491356 | 12.849422 | 7.953192 | 8.373141 | 9.960437 | 8.620416 | 8.931189 | 8.526323 | 8.42651 | 8.947734 | 8.742642 | 9.713646 | 8.734579 |
2002.02993 | Takaki Matsumoto | Hiroyuki Adachi, Goro Ishiki, Takaki Matsumoto, Kaishu Saito | The matrix regularization for Riemann surfaces with magnetic fluxes | 42 pages, 1 figure; v3: some references and 1 figure with some
comments added, minor modifications | Phys. Rev. D 101, 106009 (2020) | 10.1103/PhysRevD.101.106009 | UTHEP-746, DIAS-STP-20-02 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the matrix regularization of fields on a Riemann surface which
couple to gauge fields with a nonvanishing magnetic flux. We show that such
fields are described as rectangular matrices in the matrix regularization. We
construct the matrix regularization explicitly for the case of the sphere and
torus based... | [
{
"created": "Fri, 7 Feb 2020 19:48:22 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Feb 2020 21:59:30 GMT",
"version": "v2"
},
{
"created": "Wed, 6 May 2020 17:10:37 GMT",
"version": "v3"
}
] | 2020-05-13 | [
[
"Adachi",
"Hiroyuki",
""
],
[
"Ishiki",
"Goro",
""
],
[
"Matsumoto",
"Takaki",
""
],
[
"Saito",
"Kaishu",
""
]
] | We consider the matrix regularization of fields on a Riemann surface which couple to gauge fields with a nonvanishing magnetic flux. We show that such fields are described as rectangular matrices in the matrix regularization. We construct the matrix regularization explicitly for the case of the sphere and torus based o... | 9.777088 | 7.46778 | 9.919793 | 7.461961 | 7.908822 | 7.842151 | 8.167313 | 7.116316 | 7.277993 | 11.120426 | 7.746693 | 7.752472 | 9.827615 | 8.337201 | 8.118393 | 7.948904 | 7.721361 | 8.19066 | 7.969977 | 9.441113 | 7.883317 |
1903.06633 | Fidel I. Schaposnik Massolo | Frank Ferrari and Fidel I. Schaposnik Massolo | Phases Of Melonic Quantum Mechanics | 135 pages, 50 figures, 2 tables. Minor corrections and updated list
of references in v3. Title changed to match published version | Phys. Rev. D 100, 026007 (2019) | 10.1103/PhysRevD.100.026007 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore in detail the properties of two melonic quantum mechanical
theories which can be formulated either as fermionic matrix quantum mechanics
in the new large $D$ limit, or as disordered models. Both models have a mass
parameter $m$ and the transition from the perturbative large $m$ region to the
strongly coupl... | [
{
"created": "Fri, 15 Mar 2019 16:20:09 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Apr 2019 09:34:31 GMT",
"version": "v2"
},
{
"created": "Thu, 27 Jun 2019 09:40:49 GMT",
"version": "v3"
}
] | 2019-07-24 | [
[
"Ferrari",
"Frank",
""
],
[
"Massolo",
"Fidel I. Schaposnik",
""
]
] | We explore in detail the properties of two melonic quantum mechanical theories which can be formulated either as fermionic matrix quantum mechanics in the new large $D$ limit, or as disordered models. Both models have a mass parameter $m$ and the transition from the perturbative large $m$ region to the strongly coupled... | 7.445509 | 8.131077 | 8.045959 | 7.820652 | 8.440133 | 7.873544 | 8.347036 | 8.252438 | 7.655609 | 8.342227 | 7.518172 | 7.577594 | 7.590417 | 7.341686 | 7.391979 | 7.618512 | 7.584249 | 7.719223 | 7.356177 | 7.565479 | 7.412614 |
hep-th/0601098 | Richard Andrews | R.P. Andrews and N. Dorey | Deconstruction of the Maldacena-Nunez Compactification | 50 Pages. Font size increased. Corrections made to Sections 5 and 6 | Nucl.Phys.B751:304-341,2006 | 10.1016/j.nuclphysb.2006.06.013 | SWAT/06/455 | hep-th | null | We demonstrate a classical equivalence between the large-N limit of the
Higgsed N=1* SUSY U(N) Yang-Mills theory and the Maldacena-Nunez twisted
compactification of a six dimensional gauge theory on a two-sphere. A direct
comparison of the actions and spectra of the two theories reveals them to be
identical. We also ... | [
{
"created": "Mon, 16 Jan 2006 16:08:02 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Apr 2006 15:01:48 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Andrews",
"R. P.",
""
],
[
"Dorey",
"N.",
""
]
] | We demonstrate a classical equivalence between the large-N limit of the Higgsed N=1* SUSY U(N) Yang-Mills theory and the Maldacena-Nunez twisted compactification of a six dimensional gauge theory on a two-sphere. A direct comparison of the actions and spectra of the two theories reveals them to be identical. We also pr... | 11.020466 | 9.328266 | 12.018838 | 9.103106 | 10.023991 | 8.879503 | 8.928316 | 9.353957 | 8.837352 | 12.68681 | 9.814451 | 9.185158 | 11.120103 | 9.565544 | 10.106173 | 9.656887 | 9.461835 | 9.716235 | 9.96345 | 11.053638 | 9.500299 |
hep-th/0309033 | Bo Hu | R. Arnowitt, B. Dutta, B. Hu | Yukawa Textures, Neutrino Masses and Horava-Witten M-Theory | 24 pages, 4 figures. Minor changes, references added. Some discussion
on neutrino mass generating mechanism added; no other change. Accepted for
publication in Nucl. Phys. B | Nucl.Phys.B682:347-366,2004 | 10.1016/j.nuclphysb.2004.01.029 | null | hep-th hep-ph | null | We consider the Horava-Witten based model with 5-branes situated near the
distant orbifold plane and with vanishing instanton numbers on the physical
plane. This model has a toric fibered Calabi-Yau with del Pezzo base dP_7 which
allows three generations with Standard Model gauge group at the GUT scale.
Previous anal... | [
{
"created": "Tue, 2 Sep 2003 20:39:32 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Sep 2003 19:57:33 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Jan 2004 21:56:32 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Arnowitt",
"R.",
""
],
[
"Dutta",
"B.",
""
],
[
"Hu",
"B.",
""
]
] | We consider the Horava-Witten based model with 5-branes situated near the distant orbifold plane and with vanishing instanton numbers on the physical plane. This model has a toric fibered Calabi-Yau with del Pezzo base dP_7 which allows three generations with Standard Model gauge group at the GUT scale. Previous analys... | 10.81089 | 11.691527 | 10.830156 | 10.336129 | 11.077247 | 12.851256 | 11.657329 | 11.884602 | 10.17982 | 11.437656 | 11.147405 | 10.693903 | 10.944182 | 10.627595 | 11.066326 | 11.080379 | 11.053285 | 11.210955 | 10.877488 | 11.45716 | 10.802128 |
hep-th/0106238 | P. S. Howe | P.J. Heslop and P.S. Howe | A note on composite operators in N=4 SYM | 12 pages | Phys.Lett.B516:367-375,2001 | 10.1016/S0370-2693(01)00961-3 | null | hep-th | null | We discuss composite operators in N=4 super Yang-Mills theory and their
realisations as superfields on different superspaces. The superfields that
realise various operators on analytic superspace may be different in the free,
interacting and quantum theories. In particular, in the quantum theory, there
is a restricte... | [
{
"created": "Tue, 26 Jun 2001 13:57:36 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Heslop",
"P. J.",
""
],
[
"Howe",
"P. S.",
""
]
] | We discuss composite operators in N=4 super Yang-Mills theory and their realisations as superfields on different superspaces. The superfields that realise various operators on analytic superspace may be different in the free, interacting and quantum theories. In particular, in the quantum theory, there is a restricted ... | 9.151369 | 9.600886 | 10.778383 | 9.040056 | 8.352113 | 8.45916 | 9.217036 | 9.504086 | 9.188811 | 9.997936 | 8.607158 | 8.677428 | 9.449796 | 8.91672 | 8.538136 | 9.261497 | 8.989362 | 8.685877 | 8.722971 | 9.032354 | 8.731843 |
1209.2573 | Wagner Utiel | Wagner Utiel | N-points correlator for the Gaudin's model realization of a Quantum Hall
Fluid | The paper has been withdraw by the author because a new version is
been written to better emphasize in this review the use of the off-shell
Bethe ansatz approach to obtain solutions of the KZ equation in a more easy
way than the approach used in Hou et all(arXiv:hep-th/0210173) | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Gaudin's model realization of a incompressible quantum Hall
fluid on torus. We solve the model using the so called off-shell algebraic
Bethe ansatz for a general spin representation. The n-points correlators also
was computed as a solution of the Kznihik-Zamolodchikov equations. This explore
a possible c... | [
{
"created": "Wed, 12 Sep 2012 11:34:12 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Sep 2012 12:08:35 GMT",
"version": "v2"
}
] | 2012-09-17 | [
[
"Utiel",
"Wagner",
""
]
] | We study the Gaudin's model realization of a incompressible quantum Hall fluid on torus. We solve the model using the so called off-shell algebraic Bethe ansatz for a general spin representation. The n-points correlators also was computed as a solution of the Kznihik-Zamolodchikov equations. This explore a possible con... | 25.255674 | 21.987835 | 29.187128 | 22.93187 | 24.850161 | 24.705734 | 22.023371 | 23.12405 | 21.38007 | 32.330124 | 21.454603 | 22.143045 | 24.635942 | 22.379885 | 22.974852 | 22.714527 | 23.147928 | 24.602415 | 22.150162 | 24.405413 | 22.614176 |
1904.05477 | Alexander Kovner | Candost Akkaya and Alex Kovner (University of Connecticut) | On Entanglement Entropy of Maxwell fields in 3+1 dimensions | An algebraic error corrected. Results significantly changed | null | 10.1016/j.physletb.2020.135670 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider entanglement entropy between two halves of space separated by a
plane, in the theory of free photon in 3+1 dimensions. We show how to separate
local gauge invariant quantities that belong to the two spatial regions. We
calculate the entanglement entropy by integrating over the degrees of freedom
in one ha... | [
{
"created": "Wed, 10 Apr 2019 23:28:31 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Aug 2019 08:04:27 GMT",
"version": "v2"
}
] | 2020-08-05 | [
[
"Akkaya",
"Candost",
"",
"University of Connecticut"
],
[
"Kovner",
"Alex",
"",
"University of Connecticut"
]
] | We consider entanglement entropy between two halves of space separated by a plane, in the theory of free photon in 3+1 dimensions. We show how to separate local gauge invariant quantities that belong to the two spatial regions. We calculate the entanglement entropy by integrating over the degrees of freedom in one half... | 10.687614 | 10.800184 | 10.374599 | 9.71966 | 11.259613 | 10.876384 | 10.339982 | 9.859639 | 9.824919 | 10.917474 | 9.444381 | 10.003835 | 9.891352 | 9.828691 | 9.787206 | 9.910099 | 9.889422 | 10.052958 | 9.797932 | 10.003185 | 9.636675 |
hep-th/9607161 | null | L. Frappat, A. Sciarrino, P. Sorba | Dictionary on Lie Superalgebras | 145p LaTeX Document, also available at
http://lapphp0.in2p3.fr/preplapp/psth/DICTIONARY_SUPER.ps.gz | null | null | ENSLAPP-AL-600/96 and DSF-T-30/96 | hep-th | null | The main definitions and properties of Lie superalgebras are proposed a la
facon de a short dictionary, the different items following the alphabetical
order. The main topics deal with the structure of simple Lie superalgebras and
their finite dimensional representations; rather naturally, a few pages are
devoted to s... | [
{
"created": "Thu, 18 Jul 1996 18:38:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Frappat",
"L.",
""
],
[
"Sciarrino",
"A.",
""
],
[
"Sorba",
"P.",
""
]
] | The main definitions and properties of Lie superalgebras are proposed a la facon de a short dictionary, the different items following the alphabetical order. The main topics deal with the structure of simple Lie superalgebras and their finite dimensional representations; rather naturally, a few pages are devoted to sup... | 20.093939 | 21.497952 | 19.747517 | 21.807629 | 20.050276 | 22.48148 | 22.313486 | 18.672785 | 20.019623 | 23.047977 | 19.736149 | 20.337667 | 20.607224 | 19.547567 | 20.144728 | 19.164246 | 19.391422 | 18.932983 | 18.814795 | 20.361082 | 19.223154 |
hep-th/0212323 | Christopher Pope | H. Lu, C.N. Pope and E. Sezgin | SU(2) Reduction of Six-dimensional (1,0) Supergravity | Latex, 24 pages | Nucl.Phys.B668:237-257,2003 | 10.1016/S0550-3213(03)00534-0 | null | hep-th | null | We obtain a gauged supergravity theory in three dimensions with eight real
supersymmetries by means of a Scherk-Schwarz reduction of pure N=(1,0)
supergravity in six dimension on the SU(2) group manifold. The SU(2) Yang-Mills
fields in the model propagate, since they have an ordinary kinetic term in
addition to Chern... | [
{
"created": "Sun, 29 Dec 2002 00:38:36 GMT",
"version": "v1"
}
] | 2009-10-07 | [
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Sezgin",
"E.",
""
]
] | We obtain a gauged supergravity theory in three dimensions with eight real supersymmetries by means of a Scherk-Schwarz reduction of pure N=(1,0) supergravity in six dimension on the SU(2) group manifold. The SU(2) Yang-Mills fields in the model propagate, since they have an ordinary kinetic term in addition to Chern-S... | 5.634469 | 5.472931 | 6.275769 | 5.479073 | 5.164541 | 5.273886 | 5.462121 | 5.683585 | 5.43263 | 5.976508 | 5.429872 | 5.628936 | 5.723843 | 5.351583 | 5.467284 | 5.485954 | 5.313282 | 5.525131 | 5.391374 | 5.575479 | 5.355908 |
1706.09057 | Wojciech Dybalski | Wojciech Dybalski | From Faddeev-Kulish to LSZ. Towards a non-perturbative description of
colliding electrons | 12 pages, 1 figure | Nuclear Physics B 925, 455-469 (2017) | 10.1016/j.nuclphysb.2017.10.018 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a low energy approximation of the massless Yukawa theory (Nelson model) we
derive a Faddeev-Kulish type formula for the scattering matrix of $N$ electrons
and reformulate it in LSZ terms. To this end, we perform a decomposition of the
infrared finite Dollard modifier into clouds of real and virtual photons, whose
... | [
{
"created": "Tue, 27 Jun 2017 21:44:13 GMT",
"version": "v1"
}
] | 2021-04-23 | [
[
"Dybalski",
"Wojciech",
""
]
] | In a low energy approximation of the massless Yukawa theory (Nelson model) we derive a Faddeev-Kulish type formula for the scattering matrix of $N$ electrons and reformulate it in LSZ terms. To this end, we perform a decomposition of the infrared finite Dollard modifier into clouds of real and virtual photons, whose in... | 11.174019 | 12.866647 | 13.316751 | 11.451818 | 12.607117 | 12.064495 | 13.608722 | 12.241745 | 12.275847 | 13.167986 | 11.385448 | 11.201144 | 11.460373 | 11.131687 | 11.117593 | 11.00258 | 11.285039 | 11.568138 | 10.818566 | 11.304372 | 11.378368 |
1209.4043 | Paul de Medeiros | Paul de Medeiros | Rigid supersymmetry, conformal coupling and twistor spinors | 30 pages, v2: Reference added and a few typos corrected, minor
clarifications in sections 1 and 8.1 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the relationship between conformal and spin structure on
lorentzian manifolds and see how their compatibility influences the formulation
of rigid supersymmetric field theories. In dimensions three, four, six and ten,
we show that if the Dirac current associated with a generic spinor defines a
null conf... | [
{
"created": "Tue, 18 Sep 2012 17:51:02 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Sep 2012 16:09:27 GMT",
"version": "v2"
}
] | 2012-09-28 | [
[
"de Medeiros",
"Paul",
""
]
] | We investigate the relationship between conformal and spin structure on lorentzian manifolds and see how their compatibility influences the formulation of rigid supersymmetric field theories. In dimensions three, four, six and ten, we show that if the Dirac current associated with a generic spinor defines a null confor... | 8.860435 | 9.604382 | 9.737615 | 9.234702 | 9.772365 | 9.514751 | 9.44387 | 9.30439 | 9.228691 | 10.910241 | 9.88525 | 8.885515 | 9.063298 | 8.79986 | 8.881474 | 8.668036 | 8.673738 | 8.718805 | 8.620202 | 9.463155 | 8.823964 |
0903.2477 | David Vegh | Hong Liu, John McGreevy and David Vegh | Non-Fermi liquids from holography | 10 pages, 16 figures. v2: added references, corrected figures, some
minor changes. v3: figure 5 replaced | Phys.Rev.D83:065029,2011 | 10.1103/PhysRevD.83.065029 | MIT-CTP/4023 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report on a potentially new class of non-Fermi liquids in
(2+1)-dimensions. They are identified via the response functions of composite
fermionic operators in a class of strongly interacting quantum field theories
at finite density, computed using the AdS/CFT correspondence. We find strong
evidence of Fermi surfac... | [
{
"created": "Mon, 16 Mar 2009 19:50:48 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Mar 2009 19:59:32 GMT",
"version": "v2"
},
{
"created": "Thu, 16 Jul 2009 18:18:54 GMT",
"version": "v3"
}
] | 2011-05-10 | [
[
"Liu",
"Hong",
""
],
[
"McGreevy",
"John",
""
],
[
"Vegh",
"David",
""
]
] | We report on a potentially new class of non-Fermi liquids in (2+1)-dimensions. They are identified via the response functions of composite fermionic operators in a class of strongly interacting quantum field theories at finite density, computed using the AdS/CFT correspondence. We find strong evidence of Fermi surfaces... | 10.316144 | 10.069425 | 10.823942 | 9.147152 | 9.499723 | 9.202272 | 9.894954 | 8.956053 | 9.240891 | 11.308331 | 8.882441 | 9.200131 | 10.756207 | 9.635206 | 9.372314 | 9.70013 | 9.697711 | 9.866195 | 9.559548 | 10.725654 | 9.145676 |
1509.00640 | Suddhasattwa Brahma | Martin Bojowald and Suddhasattwa Brahma | Minisuperspace models as infrared contributions | 31 pages | Phys. Rev. D 93, 125001 (2016) | 10.1103/PhysRevD.93.125001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A direct correspondence of quantum mechanics as a minisuperspace model for a
self-interacting scalar quantum-field theory is established by computing, in
several models, the infrared contributions to 1-loop effective potentials of
Coleman--Weinberg type. A minisuperspace approximation rather than truncation
is thereb... | [
{
"created": "Wed, 2 Sep 2015 10:59:34 GMT",
"version": "v1"
}
] | 2016-06-08 | [
[
"Bojowald",
"Martin",
""
],
[
"Brahma",
"Suddhasattwa",
""
]
] | A direct correspondence of quantum mechanics as a minisuperspace model for a self-interacting scalar quantum-field theory is established by computing, in several models, the infrared contributions to 1-loop effective potentials of Coleman--Weinberg type. A minisuperspace approximation rather than truncation is thereby ... | 13.609191 | 14.042918 | 13.702327 | 12.871007 | 13.772593 | 14.656596 | 14.648118 | 12.628581 | 13.166439 | 14.271569 | 13.703173 | 13.053521 | 13.043718 | 12.928657 | 13.095295 | 13.143674 | 13.143784 | 12.866035 | 13.11789 | 13.056201 | 13.031086 |
hep-th/0501032 | Robert Brandenberger | Yeuk-Kwan E. Cheung, Scott Watson, and Robert Brandenberger | Moduli Stabilization with Long Winding Strings | title changed, improved presentation; reference added. 18 pages, JHEP
style | JHEP 0605 (2006) 025 | 10.1088/1126-6708/2006/05/025 | BROWN-HET-1436, CMS 06004, MCGILL-01-05 | hep-th | null | Stabilizing all of the modulus fields coming from compactifications of string
theory on internal manifolds is one of the outstanding challenges for string
cosmology. Here, in a simple example of toroidal compactification, we study the
dynamics of the moduli fields corresponding to the size and shape of the torus
alon... | [
{
"created": "Thu, 6 Jan 2005 13:52:16 GMT",
"version": "v1"
},
{
"created": "Mon, 8 May 2006 09:07:38 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Cheung",
"Yeuk-Kwan E.",
""
],
[
"Watson",
"Scott",
""
],
[
"Brandenberger",
"Robert",
""
]
] | Stabilizing all of the modulus fields coming from compactifications of string theory on internal manifolds is one of the outstanding challenges for string cosmology. Here, in a simple example of toroidal compactification, we study the dynamics of the moduli fields corresponding to the size and shape of the torus along ... | 10.860285 | 9.615735 | 10.548149 | 9.349374 | 9.765286 | 9.980638 | 9.013628 | 9.707883 | 9.382451 | 10.796909 | 9.110887 | 9.366158 | 9.753635 | 9.343946 | 9.243096 | 9.369571 | 9.046587 | 9.405991 | 9.4815 | 10.061597 | 9.298995 |
2111.02576 | Chia-Kai Kuo | Song He, Chia-Kai Kuo, Yao-Qi Zhang | The momentum amplituhedron of SYM and ABJM from twistor-string maps | typos corrected, JHEP published version | null | 10.1007/JHEP02(2022)148 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study remarkable connections between twistor-string formulas for tree
amplitudes in ${\cal N}=4$ SYM and ${\cal N}=6$ ABJM, and the corresponding
momentum amplituhedron in the kinematic space of $D=4$ and $D=3$, respectively.
Based on the Veronese map to positive Grassmannians, we define a twistor-string
map from ... | [
{
"created": "Thu, 4 Nov 2021 01:21:07 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Apr 2022 10:38:36 GMT",
"version": "v2"
}
] | 2022-04-29 | [
[
"He",
"Song",
""
],
[
"Kuo",
"Chia-Kai",
""
],
[
"Zhang",
"Yao-Qi",
""
]
] | We study remarkable connections between twistor-string formulas for tree amplitudes in ${\cal N}=4$ SYM and ${\cal N}=6$ ABJM, and the corresponding momentum amplituhedron in the kinematic space of $D=4$ and $D=3$, respectively. Based on the Veronese map to positive Grassmannians, we define a twistor-string map from $G... | 5.542936 | 5.5765 | 6.399446 | 5.482028 | 5.573573 | 5.544722 | 5.756368 | 5.567328 | 5.347679 | 6.498801 | 5.23989 | 5.308475 | 5.761012 | 5.491014 | 5.518435 | 5.362116 | 5.421424 | 5.495379 | 5.392723 | 5.71732 | 5.258898 |
2210.12349 | Anwesha Chakraborty Ms | Rabin Banerjee and Anwesha Chakraborty | Shift symmetries and duality web in gauge theories | 41 Pages, 6 Tables | Nucl. Phys. B, Volume 996, 2023 | 10.1016/j.nuclphysb.2023.116354 | 116354 | hep-th cond-mat.str-el | http://creativecommons.org/licenses/by/4.0/ | Using a generalised Noether prescription we are able to extract all the
currents and their conservation laws in space dependent shift symmetric
theories. Various identities among the currents in the matter sector are found
that form the basis for revealing a dual picture when the full interacting
theory is considered... | [
{
"created": "Sat, 22 Oct 2022 04:27:17 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Sep 2023 18:37:46 GMT",
"version": "v2"
}
] | 2023-09-27 | [
[
"Banerjee",
"Rabin",
""
],
[
"Chakraborty",
"Anwesha",
""
]
] | Using a generalised Noether prescription we are able to extract all the currents and their conservation laws in space dependent shift symmetric theories. Various identities among the currents in the matter sector are found that form the basis for revealing a dual picture when the full interacting theory is considered b... | 18.003693 | 17.309851 | 18.486938 | 16.41721 | 18.727734 | 18.333994 | 17.566902 | 16.991022 | 16.933287 | 20.77705 | 16.992847 | 17.175394 | 17.392633 | 16.845379 | 16.939445 | 16.864637 | 16.554722 | 16.639086 | 16.684713 | 17.79278 | 16.866413 |
1307.6856 | David Poland | Filip Kos, David Poland, David Simmons-Duffin | Bootstrapping the O(N) Vector Models | 26 pages, 5 figures; V2: typos corrected | JHEP 1406 (2014) 091 | 10.1007/JHEP06(2014)091 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the conformal bootstrap for 3D CFTs with O(N) global symmetry. We
obtain rigorous upper bounds on the scaling dimensions of the first O(N)
singlet and symmetric tensor operators appearing in the $\phi_i \times \phi_j$
OPE, where $\phi_i$ is a fundamental of O(N). Comparing these bounds to
previous determinat... | [
{
"created": "Thu, 25 Jul 2013 20:00:01 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Oct 2015 18:35:14 GMT",
"version": "v2"
}
] | 2015-10-16 | [
[
"Kos",
"Filip",
""
],
[
"Poland",
"David",
""
],
[
"Simmons-Duffin",
"David",
""
]
] | We study the conformal bootstrap for 3D CFTs with O(N) global symmetry. We obtain rigorous upper bounds on the scaling dimensions of the first O(N) singlet and symmetric tensor operators appearing in the $\phi_i \times \phi_j$ OPE, where $\phi_i$ is a fundamental of O(N). Comparing these bounds to previous determinatio... | 3.358565 | 3.969955 | 5.532468 | 4.068518 | 5.069751 | 4.149335 | 4.398041 | 4.403075 | 4.393348 | 5.576295 | 3.996868 | 3.835462 | 4.557828 | 3.966765 | 4.086641 | 4.009168 | 4.139649 | 3.908698 | 3.807183 | 4.75204 | 4.071553 |
1312.3506 | Ilarion Melnikov | Jock McOrist, Ilarion V. Melnikov, and Brian Wecht | Global Symmetries and N=2 SUSY | 14 pages | null | null | DMUS-MP-13/20, MIFPA 13-34, QMUL-PH-13-13 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove that N=2 theories that arise by taking n free hypermultiplets and
gauging a subgroup of Sp(n), the non-R global symmetry of the free theory, have
a remaining global symmetry which is a direct sum of unitary, symplectic, and
special orthogonal factors. This implies that theories that have SU(N) but not
U(N) g... | [
{
"created": "Thu, 12 Dec 2013 14:48:54 GMT",
"version": "v1"
}
] | 2013-12-13 | [
[
"McOrist",
"Jock",
""
],
[
"Melnikov",
"Ilarion V.",
""
],
[
"Wecht",
"Brian",
""
]
] | We prove that N=2 theories that arise by taking n free hypermultiplets and gauging a subgroup of Sp(n), the non-R global symmetry of the free theory, have a remaining global symmetry which is a direct sum of unitary, symplectic, and special orthogonal factors. This implies that theories that have SU(N) but not U(N) glo... | 8.155869 | 8.35631 | 9.462295 | 7.27882 | 7.911057 | 7.931196 | 7.965726 | 6.971031 | 7.271814 | 9.719435 | 7.56843 | 7.310787 | 7.962764 | 7.328726 | 7.428916 | 7.321993 | 7.389597 | 7.339968 | 7.476013 | 8.217386 | 7.456009 |
0705.1225 | S. Q. Wu | Jun-Jin Peng, Shuang-Qing Wu | Hawking radiation from the Schwarzschild black hole with a global
monopole via gravitational anomaly | 4 pages, no figure, 3nd revsion with one reference added | Chin.Phys.B17:825-828,2008 | 10.1088/1674-1056/17/3/016 | null | hep-th gr-qc | null | Hawking flux from the Schwarzschild black hole with a global monopole is
obtained by using Robinson and Wilczek's method. Adopting a dimension reduction
technique, the effective quantum field in the (3+1)--dimensional global
monopole background can be described by an infinite collection of the
(1+1)--dimensional mass... | [
{
"created": "Wed, 9 May 2007 08:24:08 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Jun 2007 11:11:27 GMT",
"version": "v2"
},
{
"created": "Wed, 11 Jul 2007 12:03:54 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Peng",
"Jun-Jin",
""
],
[
"Wu",
"Shuang-Qing",
""
]
] | Hawking flux from the Schwarzschild black hole with a global monopole is obtained by using Robinson and Wilczek's method. Adopting a dimension reduction technique, the effective quantum field in the (3+1)--dimensional global monopole background can be described by an infinite collection of the (1+1)--dimensional massle... | 8.953858 | 6.944011 | 8.037081 | 6.974938 | 7.045076 | 6.787861 | 7.304608 | 6.598592 | 7.06514 | 8.313539 | 6.902036 | 7.146605 | 7.863828 | 7.26051 | 7.319636 | 7.031068 | 7.339829 | 6.930563 | 7.286979 | 7.634001 | 7.159181 |
hep-th/9306083 | Don N. Page | Don N. Page | Information in Black Hole Radiation | 12 pages, 1 PostScript figure, LaTeX, Alberta-Thy-24-93 (In response
to Phys. Rev. Lett. referees' comments, the connection between expansions in
inverse mass and in 1/N are spelled out, and a figure is added. An argument
against perturbatively predicting even late-time information is also
provided, as well as ... | Phys.Rev.Lett. 71 (1993) 3743-3746 | 10.1103/PhysRevLett.71.3743 | null | hep-th gr-qc | null | If black hole formation and evaporation can be described by an $S$ matrix,
information would be expected to come out in black hole radiation. An estimate
shows that it may come out initially so slowly, or else be so spread out, that
it would never show up in an analysis perturbative in $M_{Planck}/M$, or in 1/N
for t... | [
{
"created": "Fri, 18 Jun 1993 01:10:14 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Aug 1993 22:59:01 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Page",
"Don N.",
""
]
] | If black hole formation and evaporation can be described by an $S$ matrix, information would be expected to come out in black hole radiation. An estimate shows that it may come out initially so slowly, or else be so spread out, that it would never show up in an analysis perturbative in $M_{Planck}/M$, or in 1/N for two... | 13.52383 | 10.556862 | 11.619205 | 10.444234 | 13.073327 | 10.634334 | 11.020295 | 10.585907 | 11.386926 | 11.966413 | 10.474822 | 10.705686 | 10.498143 | 9.895638 | 10.108264 | 10.391594 | 10.082904 | 10.342593 | 10.108739 | 10.194595 | 9.763696 |
2312.09291 | Matilda Delgado | Matilda Delgado | The Bubble of Nothing under T-duality | 23 pages + refs + 2 figures | null | null | IFT-UAM/CSIC-23-146 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The bubble of nothing is a solution to Einstein's equations where a circle
shrinks and pinches off smoothly. As such, it is one of the simplest examples
of a dynamical cobordism to nothing. We take a first step in studying how this
solution transforms under T-duality in bosonic string theory. Applying
Buscher's rules... | [
{
"created": "Thu, 14 Dec 2023 19:00:18 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 2024 15:02:49 GMT",
"version": "v2"
}
] | 2024-05-08 | [
[
"Delgado",
"Matilda",
""
]
] | The bubble of nothing is a solution to Einstein's equations where a circle shrinks and pinches off smoothly. As such, it is one of the simplest examples of a dynamical cobordism to nothing. We take a first step in studying how this solution transforms under T-duality in bosonic string theory. Applying Buscher's rules r... | 11.977762 | 10.721852 | 12.159288 | 9.631302 | 10.215084 | 10.341417 | 10.745537 | 10.158483 | 10.257021 | 12.385636 | 10.268942 | 10.193519 | 10.897118 | 10.030737 | 10.491275 | 10.144033 | 10.089957 | 10.247087 | 10.619952 | 11.206809 | 10.039443 |
1608.07237 | Arvind Rajaraman | Arvind Rajaraman | de Sitter Space is Unstable in Quantum Gravity | 13 pages, references added | Phys. Rev. D 94, 125025 (2016) | 10.1103/PhysRevD.94.125025 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Graviton loop corrections to observables in de Sitter space often lead to
infrared divergences. We show that these infrared divergences are resolved by
the spontaneous breaking of de Sitter invariance.
| [
{
"created": "Thu, 25 Aug 2016 18:22:47 GMT",
"version": "v1"
},
{
"created": "Sat, 17 Sep 2016 05:01:57 GMT",
"version": "v2"
}
] | 2017-01-04 | [
[
"Rajaraman",
"Arvind",
""
]
] | Graviton loop corrections to observables in de Sitter space often lead to infrared divergences. We show that these infrared divergences are resolved by the spontaneous breaking of de Sitter invariance. | 7.800702 | 4.52025 | 5.022171 | 4.421295 | 4.43555 | 4.013825 | 4.498322 | 4.166581 | 4.559114 | 5.14934 | 4.641616 | 4.920033 | 4.956062 | 4.886829 | 4.829369 | 4.993847 | 4.793868 | 4.783089 | 5.00956 | 5.344628 | 4.676157 |
2407.15575 | Kiarash Naderi | Kiarash Naderi | Space-time symmetry from the world-sheet | 41 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The tensionless string on AdS$_3$ is a laboratory to study different aspects
of the AdS/CFT correspondence. A particular question addressed in this paper is
how the space-time symmetry algebra is encoded on the world-sheet. A natural
prescription for calculating the space-time OPEs from the world-sheet is
presented i... | [
{
"created": "Mon, 22 Jul 2024 12:05:55 GMT",
"version": "v1"
}
] | 2024-07-23 | [
[
"Naderi",
"Kiarash",
""
]
] | The tensionless string on AdS$_3$ is a laboratory to study different aspects of the AdS/CFT correspondence. A particular question addressed in this paper is how the space-time symmetry algebra is encoded on the world-sheet. A natural prescription for calculating the space-time OPEs from the world-sheet is presented in ... | 10.491398 | 7.677404 | 11.165742 | 8.143856 | 7.752949 | 7.848282 | 7.741246 | 8.195498 | 7.878248 | 11.599824 | 8.021423 | 8.463895 | 10.165365 | 9.23024 | 8.438386 | 8.361457 | 8.476569 | 8.445783 | 8.613014 | 10.561546 | 8.310199 |
hep-th/9701146 | null | A. Buonanno, M. Gasperini, M. Maggiore and C. Ungarelli | Expanding and contracting universes in third quantized string cosmology | 11 pages, LATEX, to apper in Class. Quantum Grav. An updated
collection of papers on the pre-big bang scenario in string cosmology is a
available at http://www.to.infn.it/teorici/gasperini | Class.Quant.Grav.14:L97-L103,1997 | 10.1088/0264-9381/14/5/005 | CERN-TH/96-322 | hep-th gr-qc | null | We discuss the possibility of quantum transitions from the string
perturbative vacuum to cosmological configurations characterized by isotropic
contraction and decreasing dilaton. When the dilaton potential preserves the
sign of the Hubble factor throughout the evolution, such transitions can be
represented as an ant... | [
{
"created": "Mon, 27 Jan 1997 16:37:34 GMT",
"version": "v1"
}
] | 2019-08-17 | [
[
"Buonanno",
"A.",
""
],
[
"Gasperini",
"M.",
""
],
[
"Maggiore",
"M.",
""
],
[
"Ungarelli",
"C.",
""
]
] | We discuss the possibility of quantum transitions from the string perturbative vacuum to cosmological configurations characterized by isotropic contraction and decreasing dilaton. When the dilaton potential preserves the sign of the Hubble factor throughout the evolution, such transitions can be represented as an anti-... | 14.079826 | 13.185475 | 13.33141 | 11.377096 | 12.558445 | 13.425355 | 12.553135 | 13.067628 | 12.22121 | 14.687569 | 12.746332 | 12.296792 | 12.717783 | 12.487576 | 12.223933 | 12.265059 | 11.972848 | 12.228764 | 12.932208 | 12.89874 | 12.721737 |
2004.02890 | Carlo Alberto Cremonini | R.Catenacci, C.A.Cremonini, P.A.Grassi, S.Noja | On Forms, Cohomology, and BV Laplacians in Odd Symplectic Geometry | 23 pages | null | 10.1007/s11005-021-01384-3 | null | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the cohomology of the complexes of differential, integral and pseudo
forms on odd symplectic manifolds taking the wedge product with the symplectic
form as differential. We show that the cohomology classes are in correspondence
with inequivalent Lagrangian submanifolds and that they all define
semidensities ... | [
{
"created": "Mon, 6 Apr 2020 18:00:01 GMT",
"version": "v1"
}
] | 2021-04-21 | [
[
"Catenacci",
"R.",
""
],
[
"Cremonini",
"C. A.",
""
],
[
"Grassi",
"P. A.",
""
],
[
"Noja",
"S.",
""
]
] | We study the cohomology of the complexes of differential, integral and pseudo forms on odd symplectic manifolds taking the wedge product with the symplectic form as differential. We show that the cohomology classes are in correspondence with inequivalent Lagrangian submanifolds and that they all define semidensities on... | 7.967988 | 8.904462 | 8.69558 | 7.747583 | 7.87934 | 8.573483 | 8.391565 | 7.892589 | 7.873313 | 9.970175 | 7.710095 | 7.633648 | 8.155101 | 7.564279 | 7.739451 | 7.607236 | 7.738805 | 7.805193 | 7.405208 | 7.915559 | 7.555038 |
2107.05832 | Juan Manuel Romero | Juan M. Romero and Leonardo Ort\'iz | Snyder and their representation with creation and annihilation operators | 12 pages, non figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Inspired by the Schwinger's representation of angular momentum, we propose a
representation of certain operators where we use the algebra of the
annihilation and creation operators. In particular, we propose a representation
of the Snyder space-time with the help of the annihilation and creation
operators, which crea... | [
{
"created": "Tue, 13 Jul 2021 03:37:35 GMT",
"version": "v1"
}
] | 2021-07-14 | [
[
"Romero",
"Juan M.",
""
],
[
"Ortíz",
"Leonardo",
""
]
] | Inspired by the Schwinger's representation of angular momentum, we propose a representation of certain operators where we use the algebra of the annihilation and creation operators. In particular, we propose a representation of the Snyder space-time with the help of the annihilation and creation operators, which create... | 8.230317 | 8.095314 | 7.689491 | 7.597611 | 8.106159 | 8.489229 | 7.916432 | 7.748775 | 7.742505 | 7.906241 | 8.132397 | 7.877964 | 8.193494 | 8.024964 | 8.000063 | 7.838223 | 7.756591 | 7.658913 | 8.203498 | 7.986028 | 7.850234 |
hep-th/0010119 | Kazuyuki Furuuchi | Kazuyuki Furuuchi | Dp-D(p+4) in Noncommutative Yang-Mills | 16 pages. v2 eq.(3.28) and typos corrected, ref. added v3 extended to
25 pages including various examples and explanations v4 misleading comments
on the instanton position are corrected | JHEP 0103:033,2001 | 10.1088/1126-6708/2001/03/033 | KEK-TH 720 | hep-th | null | An anti-self-dual instanton solution in Yang-Mills theory on noncommutative
${\R}^4$ with an anti-self-dual noncommutative parameter is constructed. The
solution is constructed by the ADHM construction and it can be treated in the
framework of the IIB matrix model. In the IIB matrix model, this solution is
interprete... | [
{
"created": "Mon, 16 Oct 2000 14:56:25 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Oct 2000 04:48:31 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Feb 2001 13:27:24 GMT",
"version": "v3"
},
{
"created": "Sat, 24 Feb 2001 14:44:13 GMT",
"version": "v4"
}
] | 2018-09-14 | [
[
"Furuuchi",
"Kazuyuki",
""
]
] | An anti-self-dual instanton solution in Yang-Mills theory on noncommutative ${\R}^4$ with an anti-self-dual noncommutative parameter is constructed. The solution is constructed by the ADHM construction and it can be treated in the framework of the IIB matrix model. In the IIB matrix model, this solution is interpreted ... | 4.405754 | 4.135804 | 4.729663 | 4.154285 | 4.156306 | 4.277795 | 4.18206 | 4.157419 | 3.945199 | 4.815039 | 4.219926 | 4.125926 | 4.246445 | 4.157503 | 4.192468 | 4.167254 | 4.136167 | 4.088793 | 4.207373 | 4.317384 | 4.117123 |
hep-th/9908076 | Lisa Randall | Joseph Lykken and Lisa Randall | The Shape of Gravity | 8 pages, 1 figure | JHEP 0006:014,2000 | 10.1088/1126-6708/2000/06/014 | PUPT-1883,MIT-CTP-2892,NSF-ITP-99-092 | hep-th | null | In a nontrivial background geometry with extra dimensions, gravitational
effects will depend on the shape of the Kaluza-Klein excitations of the
graviton. We investigate a consistent scenario of this type with two positive
tension three-branes separated in a five-dimensional Anti-de Sitter geometry.
The graviton is l... | [
{
"created": "Tue, 10 Aug 1999 02:04:20 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Lykken",
"Joseph",
""
],
[
"Randall",
"Lisa",
""
]
] | In a nontrivial background geometry with extra dimensions, gravitational effects will depend on the shape of the Kaluza-Klein excitations of the graviton. We investigate a consistent scenario of this type with two positive tension three-branes separated in a five-dimensional Anti-de Sitter geometry. The graviton is loc... | 13.586881 | 14.63902 | 13.588397 | 12.780337 | 13.771626 | 13.840031 | 15.466097 | 12.958861 | 13.57467 | 14.729423 | 13.253156 | 12.980018 | 13.221605 | 12.286555 | 12.91605 | 13.072146 | 12.823967 | 13.084406 | 12.613373 | 13.140043 | 12.728696 |
hep-th/0111099 | Dmitri Gal'tsov | V.V. Dyadichev, D.V. Gal'tsov, A.G. Zorin, and M.Yu. Zotov | Non-Abelian Born--Infeld cosmology | Latex2e, 7 figures | Phys.Rev. D65 (2002) 084007 | 10.1103/PhysRevD.65.084007 | DTP-MSU/01-14 | hep-th | null | We investigate homogeneous and isotropic cosmological solutions supported by
the SU(2) gauge field governed by the Born-Infeld lagrangian. In the framework
of the Friedmann-Robertson-Walker cosmology, with or without cosmological
constant $\lambda$, we derive dynamical systems that give rather complete
description of... | [
{
"created": "Mon, 12 Nov 2001 06:49:16 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Dyadichev",
"V. V.",
""
],
[
"Gal'tsov",
"D. V.",
""
],
[
"Zorin",
"A. G.",
""
],
[
"Zotov",
"M. Yu.",
""
]
] | We investigate homogeneous and isotropic cosmological solutions supported by the SU(2) gauge field governed by the Born-Infeld lagrangian. In the framework of the Friedmann-Robertson-Walker cosmology, with or without cosmological constant $\lambda$, we derive dynamical systems that give rather complete description of t... | 6.836387 | 6.771613 | 6.419907 | 6.443184 | 6.691057 | 6.15836 | 7.118095 | 6.41566 | 6.584046 | 7.049044 | 6.326474 | 6.384117 | 6.498841 | 6.224923 | 6.536401 | 6.447536 | 6.304607 | 6.384764 | 6.489992 | 6.554197 | 6.287636 |
1806.02384 | Zheng Sun | Zheng Sun, Xingyue Wei | Runaway directions in O'Raifeartaigh models | 8 pages | Commun.Theor.Phys. 70 (2018) 6, 677 | 10.1088/0253-6102/70/6/677 | CTP-SCU/2018021 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | R-symmetries, which are needed for supersymmetry (SUSY) breaking in
O'Raifeartaigh models, often lead to SUSY runaway directions trough a
complexified R-transformation. Non-R symmetries also lead to runaway directions
in a similar way. This work investigates the occurrence of runaway directions
of both SUSY and SUSY ... | [
{
"created": "Wed, 6 Jun 2018 18:55:51 GMT",
"version": "v1"
}
] | 2019-04-23 | [
[
"Sun",
"Zheng",
""
],
[
"Wei",
"Xingyue",
""
]
] | R-symmetries, which are needed for supersymmetry (SUSY) breaking in O'Raifeartaigh models, often lead to SUSY runaway directions trough a complexified R-transformation. Non-R symmetries also lead to runaway directions in a similar way. This work investigates the occurrence of runaway directions of both SUSY and SUSY br... | 10.639739 | 10.992104 | 10.811771 | 9.871413 | 10.905541 | 10.512861 | 10.107548 | 9.974251 | 10.474315 | 11.029602 | 10.481592 | 9.529642 | 9.907484 | 9.490174 | 9.358425 | 9.899805 | 9.455622 | 9.993879 | 9.491166 | 9.897947 | 9.718626 |
hep-th/0204005 | Jose M. M. Senovilla | J. M. M. Senovilla | Trapped surfaces, horizons and exact solutions in higher dimensions | 7 pages, no figures, final version to appear in Class. Quantum Grav | Class.Quant.Grav. 19 (2002) L113 | 10.1088/0264-9381/19/12/101 | null | hep-th gr-qc | null | A very simple criterion to ascertain if (D-2)-surfaces are trapped in
arbitrary D-dimensional Lorentzian manifolds is given. The result is purely
geometric, independent of the particular gravitational theory, of any field
equations or of any other conditions. Many physical applications arise, a few
shown here: a defi... | [
{
"created": "Sat, 30 Mar 2002 19:05:49 GMT",
"version": "v1"
},
{
"created": "Sat, 18 May 2002 19:19:58 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Senovilla",
"J. M. M.",
""
]
] | A very simple criterion to ascertain if (D-2)-surfaces are trapped in arbitrary D-dimensional Lorentzian manifolds is given. The result is purely geometric, independent of the particular gravitational theory, of any field equations or of any other conditions. Many physical applications arise, a few shown here: a defini... | 15.851961 | 15.05984 | 13.850597 | 13.124392 | 14.776376 | 15.127238 | 16.909908 | 13.11235 | 14.983312 | 16.147493 | 14.243458 | 14.402779 | 14.014001 | 13.631621 | 13.461458 | 13.047102 | 14.025462 | 13.439869 | 13.775398 | 13.976703 | 13.890989 |
hep-th/0403269 | Mark Laidlaw | Mark Laidlaw and Madoka Nishimura | Comments on Higher Derivative Terms for the Tachyon Action | 21 pages | null | null | null | hep-th | null | We consider the open string tachyon action in a world-sheet sigma model
approach. We present explicit calculations up to order 8 in derivatives for the
bosonic string, and mimic these to order 6 for the superstring, including terms
with multiple derivatives acting on the tachyon field. We reproduce lower
derivative t... | [
{
"created": "Fri, 26 Mar 2004 20:19:59 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Laidlaw",
"Mark",
""
],
[
"Nishimura",
"Madoka",
""
]
] | We consider the open string tachyon action in a world-sheet sigma model approach. We present explicit calculations up to order 8 in derivatives for the bosonic string, and mimic these to order 6 for the superstring, including terms with multiple derivatives acting on the tachyon field. We reproduce lower derivative ter... | 10.563907 | 9.866094 | 11.873839 | 9.938814 | 9.809096 | 9.80532 | 9.998782 | 9.694473 | 9.634982 | 12.390404 | 10.214968 | 9.809576 | 10.260663 | 9.763768 | 9.793071 | 9.954031 | 10.123437 | 9.344199 | 9.719018 | 10.029551 | 9.782362 |
hep-th/9512087 | Marco Picco | Vladimir Dotsenko, Marco Picco and Pierre Pujol | Randomly coupled minimal models | 12 pages, latex, 1 eps figures; new results added | null | 10.1016/0370-2693(96)00759-9 | PAR--LPTHE 95/63 | hep-th cond-mat | null | Using 1-loop renormalisation group equations, we analyze the effect of
randomness on multi-critical unitary minimal conformal models. We study the
case of two randomly coupled $M_p$ models and found that they flow in two
decoupled $M_{p-1}$ models, in the infra-red limit. This result is then extend
to the case with $... | [
{
"created": "Tue, 12 Dec 1995 20:01:52 GMT",
"version": "v1"
},
{
"created": "Sun, 21 Apr 1996 16:16:07 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Dotsenko",
"Vladimir",
""
],
[
"Picco",
"Marco",
""
],
[
"Pujol",
"Pierre",
""
]
] | Using 1-loop renormalisation group equations, we analyze the effect of randomness on multi-critical unitary minimal conformal models. We study the case of two randomly coupled $M_p$ models and found that they flow in two decoupled $M_{p-1}$ models, in the infra-red limit. This result is then extend to the case with $M$... | 8.93335 | 7.243671 | 8.397267 | 6.747174 | 7.190495 | 7.559209 | 7.336494 | 7.748224 | 6.920748 | 10.30303 | 7.021703 | 7.16893 | 8.64012 | 7.605924 | 7.4773 | 7.571227 | 7.623465 | 7.526476 | 7.642444 | 9.072734 | 7.285934 |
hep-th/9911035 | Sebastian Silva | B. Julia and S. Silva | On first order formulations of supergravities | LaTex, 30 Pages. Expanded introduction and added references | JHEP 0001 (2000) 026 | 10.1088/1126-6708/2000/01/026 | null | hep-th | null | Supergravities are usually presented in a so-called 1.5 order formulation.
Here we present a general scheme to derive pure 1^{st} order formulations of
supergravities from the 1.5 order ones. The example of N_4=1 supergravity will
be rederived and new results for N_4=2 and N_11=1 will be presented. It seems
that beyo... | [
{
"created": "Fri, 5 Nov 1999 16:49:29 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Dec 1999 14:16:04 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Julia",
"B.",
""
],
[
"Silva",
"S.",
""
]
] | Supergravities are usually presented in a so-called 1.5 order formulation. Here we present a general scheme to derive pure 1^{st} order formulations of supergravities from the 1.5 order ones. The example of N_4=1 supergravity will be rederived and new results for N_4=2 and N_11=1 will be presented. It seems that beyond... | 13.850608 | 14.828303 | 15.465407 | 13.266076 | 14.147748 | 14.13192 | 14.288259 | 14.505272 | 14.353322 | 15.937406 | 13.572913 | 14.169646 | 14.200462 | 13.697711 | 13.668438 | 13.530204 | 13.810319 | 13.649173 | 13.788039 | 13.652102 | 13.818823 |
hep-th/9505108 | Hoi-Kwong Lo | Kai-Ming Lee and Hoi-Kwong Lo | Wavefunctions for Non-Abelian Vortices | Reference added | null | null | IASSNS-HEP-95/34 ; OUTP-95-20P | hep-th | null | We construct exact wavefunctions of two vortices on a plane, a single vortex
on the cylinder and a vortex on the torus. In each case, the physics is shown
to be equivalent to a particle moving in a covering space, something simple to
solve in those examples. We describe how our solutions fit into the general
theory o... | [
{
"created": "Wed, 17 May 1995 16:04:14 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Jan 1997 18:56:06 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Lee",
"Kai-Ming",
""
],
[
"Lo",
"Hoi-Kwong",
""
]
] | We construct exact wavefunctions of two vortices on a plane, a single vortex on the cylinder and a vortex on the torus. In each case, the physics is shown to be equivalent to a particle moving in a covering space, something simple to solve in those examples. We describe how our solutions fit into the general theory of ... | 13.500551 | 13.654413 | 14.631162 | 12.522919 | 13.927703 | 14.754071 | 13.565628 | 14.138721 | 13.425288 | 14.425119 | 13.509731 | 12.395882 | 13.664614 | 13.063004 | 13.192821 | 13.1018 | 12.915505 | 12.389062 | 12.513783 | 13.804173 | 12.66207 |
hep-th/0307274 | Muneto Nitta | Masato Arai, Muneto Nitta, Norisuke Sakai | Vacua of Massive Hyper-Kahler Sigma Models with Non-Abelian Quotient | 37 pages, one figure, final version to appear in Prog. Theor. Phys | Prog.Theor.Phys. 113 (2005) 657-685 | 10.1143/PTP.113.657 | TIT/HEP-504 | hep-th hep-ph math-ph math.MP | null | The Higgs branch of N=2 supersymmetric gauge theories with non-Abelian gauge
groups are described by hyper-Kahler (HK) nonlinear sigma models with potential
terms. With the non-Abelian HK quotient by U(M) and SU(M) gauge groups, we give
the massive HK sigma models that are not toric in the N=1 superfield formalism
an... | [
{
"created": "Mon, 28 Jul 2003 19:49:15 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Sep 2003 23:55:06 GMT",
"version": "v2"
},
{
"created": "Thu, 13 Jan 2005 15:14:48 GMT",
"version": "v3"
},
{
"created": "Tue, 1 Mar 2005 08:38:50 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Arai",
"Masato",
""
],
[
"Nitta",
"Muneto",
""
],
[
"Sakai",
"Norisuke",
""
]
] | The Higgs branch of N=2 supersymmetric gauge theories with non-Abelian gauge groups are described by hyper-Kahler (HK) nonlinear sigma models with potential terms. With the non-Abelian HK quotient by U(M) and SU(M) gauge groups, we give the massive HK sigma models that are not toric in the N=1 superfield formalism and ... | 9.833301 | 8.838608 | 10.590749 | 8.417111 | 9.756084 | 9.448812 | 8.988974 | 8.904443 | 8.545453 | 12.003709 | 8.754139 | 8.597944 | 9.321325 | 8.789881 | 8.911115 | 8.870887 | 8.719709 | 8.757673 | 9.054727 | 8.553034 | 8.933068 |
0903.2293 | Dennis D. Dietrich | Dennis D. Dietrich | On invariants for particle propagation in non-Abelian fields | 4 pages, no figures, to be published in PRD | Phys.Rev.D80:067701,2009 | 10.1103/PhysRevD.80.067701 | CP3-Origins: 2009-5 | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Characterising the propagation of particles in an external non-Abelian field
only in terms of invariants constructed from its field tensor is not always
sufficient, especially, in many analytically tractable and phenomenologically
interesting cases.
| [
{
"created": "Thu, 12 Mar 2009 23:43:16 GMT",
"version": "v1"
},
{
"created": "Sat, 29 Aug 2009 17:41:43 GMT",
"version": "v2"
}
] | 2009-09-24 | [
[
"Dietrich",
"Dennis D.",
""
]
] | Characterising the propagation of particles in an external non-Abelian field only in terms of invariants constructed from its field tensor is not always sufficient, especially, in many analytically tractable and phenomenologically interesting cases. | 25.131981 | 17.095617 | 14.848699 | 15.265156 | 15.50167 | 19.046011 | 16.406139 | 15.222106 | 12.793818 | 15.053206 | 15.458038 | 15.788737 | 14.998717 | 14.466412 | 15.002157 | 15.034563 | 14.614846 | 16.263868 | 13.769197 | 14.21388 | 15.944251 |
2109.10382 | Soumangsu Chakraborty Dr | Soumangsu Chakraborty and Akikazu Hashimoto | Weighed average over Narain moduli space as $T \bar T$ deformation of
CFT target space | 15 pages | null | 10.1103/PhysRevD.105.086018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the weighted average of a two dimensional CFT, whose target space
is $T^2$, over its Narain moduli space. We take as the weighing function the
integral kernel which gives rise to $T \bar T$ deformation when applied to the
world sheet moduli data of the partition function viewed as vacuum amplitude
when th... | [
{
"created": "Tue, 21 Sep 2021 18:08:43 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Jul 2022 13:24:09 GMT",
"version": "v2"
}
] | 2022-07-20 | [
[
"Chakraborty",
"Soumangsu",
""
],
[
"Hashimoto",
"Akikazu",
""
]
] | We consider the weighted average of a two dimensional CFT, whose target space is $T^2$, over its Narain moduli space. We take as the weighing function the integral kernel which gives rise to $T \bar T$ deformation when applied to the world sheet moduli data of the partition function viewed as vacuum amplitude when the ... | 11.341026 | 10.980698 | 11.339241 | 10.410528 | 10.593365 | 9.444586 | 11.067294 | 9.650709 | 10.104536 | 13.430074 | 10.277527 | 9.682006 | 10.915192 | 10.166567 | 10.22937 | 10.094307 | 10.156189 | 9.709782 | 10.239607 | 11.170679 | 10.648509 |
1312.3542 | Riccardo Borsato | Gleb Arutyunov, Riccardo Borsato and Sergey Frolov | S-matrix for strings on $\eta$-deformed AdS5 x S5 | 23 pages, 1 figure. Misprint in (3.18) corrected | JHEP (2014) 002 | 10.1007/JHEP04(2014)002 | ITP-UU-13-31, SPIN-13-23, HU-Mathematik-2013-24, TCD-MATH-13-16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We determine the bosonic part of the superstring sigma model Lagrangian on
$\eta$-deformed AdS5 x S5, and use it to compute the perturbative world-sheet
scattering matrix of bosonic particles of the model. We then compare it with
the large string tension limit of the q-deformed S-matrix and find exact
agreement.
| [
{
"created": "Thu, 12 Dec 2013 16:41:53 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Apr 2014 08:54:00 GMT",
"version": "v2"
},
{
"created": "Thu, 27 Aug 2015 15:23:13 GMT",
"version": "v3"
}
] | 2015-08-28 | [
[
"Arutyunov",
"Gleb",
""
],
[
"Borsato",
"Riccardo",
""
],
[
"Frolov",
"Sergey",
""
]
] | We determine the bosonic part of the superstring sigma model Lagrangian on $\eta$-deformed AdS5 x S5, and use it to compute the perturbative world-sheet scattering matrix of bosonic particles of the model. We then compare it with the large string tension limit of the q-deformed S-matrix and find exact agreement. | 8.946592 | 7.207925 | 11.402666 | 7.143857 | 7.444983 | 7.832628 | 7.599856 | 7.682568 | 7.148372 | 11.427661 | 7.478691 | 7.658948 | 9.522667 | 7.430581 | 7.59219 | 7.76082 | 7.699109 | 7.68533 | 7.581056 | 8.769722 | 7.513153 |
0711.0155 | Arkady Tseytlin | M. Grigoriev and A.A. Tseytlin | Pohlmeyer reduction of AdS_5 x S^5 superstring sigma model | 56 pages. v2: section 6.4 expanded with comments on mass spectrum and
the corresponding S-matrix; v3,v4: minor corrections and clarifications added | Nucl.Phys.B800:450-501,2008 | 10.1016/j.nuclphysb.2008.01.006 | Imperial-TP-AT-2007-4, NI07093 | hep-th | null | Motivated by a desire to find a useful 2d Lorentz-invariant reformulation of
the AdS_5 x S^5 superstring world-sheet theory in terms of physical degrees of
freedom we construct the Pohlmeyer-reduced version of the corresponding sigma
model. The Pohlmeyer reduction procedure involves several steps. Starting with
a cos... | [
{
"created": "Thu, 1 Nov 2007 19:57:01 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Nov 2007 19:52:08 GMT",
"version": "v2"
},
{
"created": "Mon, 12 Nov 2007 20:52:24 GMT",
"version": "v3"
},
{
"created": "Mon, 7 Jan 2008 17:07:38 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Grigoriev",
"M.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | Motivated by a desire to find a useful 2d Lorentz-invariant reformulation of the AdS_5 x S^5 superstring world-sheet theory in terms of physical degrees of freedom we construct the Pohlmeyer-reduced version of the corresponding sigma model. The Pohlmeyer reduction procedure involves several steps. Starting with a coset... | 6.116408 | 5.63896 | 7.021881 | 6.058212 | 6.602156 | 6.433528 | 6.065456 | 6.006113 | 5.824224 | 6.872818 | 6.008473 | 6.103641 | 6.283198 | 6.059289 | 6.115121 | 6.143711 | 6.06882 | 5.966946 | 5.979036 | 6.259891 | 6.002409 |
0810.4778 | Yuri Makeenko | Yuri Makeenko and Poul Olesen | Implementation of the Duality between Wilson loops and Scattering
Amplitudes in QCD | REVTex, 6 pages, 1 figure; v3: refs added; v4pp. to appear in PRL | Phys.Rev.Lett.102:071602,2009 | 10.1103/PhysRevLett.102.071602 | ITEP-TH-47/08 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize modern ideas about the duality between Wilson loops and
scattering amplitudes in ${\cal N}$=4 SYM to large-N (or quenched) QCD. We show
that the area-law behavior of asymptotically large Wilson loops is dual to the
Regge-Veneziano behavior of scattering amplitudes at high energies and fixed
momentum tra... | [
{
"created": "Mon, 27 Oct 2008 15:10:45 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Oct 2008 20:43:52 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Nov 2008 09:34:36 GMT",
"version": "v3"
},
{
"created": "Tue, 27 Jan 2009 11:09:01 GMT",
"version": "v4"
}
] | 2009-02-27 | [
[
"Makeenko",
"Yuri",
""
],
[
"Olesen",
"Poul",
""
]
] | We generalize modern ideas about the duality between Wilson loops and scattering amplitudes in ${\cal N}$=4 SYM to large-N (or quenched) QCD. We show that the area-law behavior of asymptotically large Wilson loops is dual to the Regge-Veneziano behavior of scattering amplitudes at high energies and fixed momentum trans... | 9.650061 | 8.756965 | 9.177989 | 8.56115 | 8.420044 | 8.766233 | 8.036217 | 8.701756 | 8.527927 | 10.266952 | 7.864618 | 8.484416 | 8.658438 | 8.306959 | 8.312077 | 8.107867 | 8.56479 | 8.784666 | 8.523683 | 8.903416 | 8.273993 |
2403.15893 | Ugo Moschella | Ugo Moschella | Plane waves, harmonic analysis in de Sitter and anti de Sitter Quantum
Field Theory and the spectral condition | THE FRIEDMANN COSMOLOGY: A CENTURY LATER. Invited paper | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We review the role of the spectral condition as a characteristic feature
unifying Minkowski, de Sitter and anti de Sitter Quantum Field Theory. In this
context, we highlight the role of an important class of plane waves which are
either de Sitter or anti de Sitter covariant and are compatible with the
relevant analyt... | [
{
"created": "Sat, 23 Mar 2024 17:19:31 GMT",
"version": "v1"
}
] | 2024-03-26 | [
[
"Moschella",
"Ugo",
""
]
] | We review the role of the spectral condition as a characteristic feature unifying Minkowski, de Sitter and anti de Sitter Quantum Field Theory. In this context, we highlight the role of an important class of plane waves which are either de Sitter or anti de Sitter covariant and are compatible with the relevant analytic... | 14.635753 | 13.342943 | 13.254041 | 11.999166 | 13.73015 | 12.903665 | 14.86006 | 12.751086 | 13.269765 | 14.627904 | 13.200149 | 14.070162 | 13.247406 | 13.088578 | 13.628222 | 13.376369 | 13.675473 | 13.129912 | 13.809206 | 13.76682 | 13.201272 |
1202.2494 | Yushu Song | Yushu Song and Shu-Qing Guo | Fermi Surface under Magnetism Instability | 17pages,2 figures, discussions added; terminology corrected | null | 10.1007/JHEP07(2012)165 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the fermionic excitations near the quantum
criticality using gauge/gravity duality. This is motivated by exploring the
Fermi surface evolution near the quantum criticality. We construct the gravity
dual of "paramagnetic-nematic" phase transition in a continuum limit and study
the Fermi surface... | [
{
"created": "Sun, 12 Feb 2012 07:34:29 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Feb 2012 08:23:32 GMT",
"version": "v2"
},
{
"created": "Tue, 3 Apr 2012 13:38:49 GMT",
"version": "v3"
},
{
"created": "Thu, 26 Jul 2012 11:34:24 GMT",
"version": "v4"
}
] | 2017-08-23 | [
[
"Song",
"Yushu",
""
],
[
"Guo",
"Shu-Qing",
""
]
] | In this paper, we study the fermionic excitations near the quantum criticality using gauge/gravity duality. This is motivated by exploring the Fermi surface evolution near the quantum criticality. We construct the gravity dual of "paramagnetic-nematic" phase transition in a continuum limit and study the Fermi surface e... | 6.698788 | 5.893699 | 6.052499 | 5.675811 | 6.014463 | 5.737792 | 5.962244 | 5.867778 | 5.578408 | 5.919085 | 5.586072 | 5.786252 | 5.717206 | 5.634803 | 5.525765 | 5.721718 | 5.536849 | 5.656023 | 5.501796 | 5.695753 | 6.025402 |
1907.08862 | Junho Hong | Junho Hong, Finn Larsen, and James T. Liu | The Scales of Black Holes with nAdS$_2$ Geometry | 42 pages; v2: minor revisions; v3: discussion section added | null | 10.1007/JHEP10(2019)260 | LCTP-19-14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study nearly extreme black holes with nearly AdS$_2$ horizon geometry in
various settings inspired by string theory. Our focus is on the scales of the
nAdS$_2$ region and their relation to microscopic theory. These scales are
determined by a generalization of the attractor mechanism for extremal black
holes and re... | [
{
"created": "Sat, 20 Jul 2019 20:01:33 GMT",
"version": "v1"
},
{
"created": "Sat, 10 Aug 2019 12:35:02 GMT",
"version": "v2"
},
{
"created": "Mon, 21 Oct 2019 18:44:11 GMT",
"version": "v3"
}
] | 2020-01-08 | [
[
"Hong",
"Junho",
""
],
[
"Larsen",
"Finn",
""
],
[
"Liu",
"James T.",
""
]
] | We study nearly extreme black holes with nearly AdS$_2$ horizon geometry in various settings inspired by string theory. Our focus is on the scales of the nAdS$_2$ region and their relation to microscopic theory. These scales are determined by a generalization of the attractor mechanism for extremal black holes and real... | 12.904476 | 12.332747 | 13.017604 | 11.527514 | 12.410629 | 12.859783 | 12.428137 | 11.775522 | 12.323838 | 13.940358 | 11.862034 | 11.840305 | 12.017979 | 11.550687 | 11.674492 | 12.087873 | 12.493917 | 11.431488 | 11.759455 | 11.866676 | 11.563999 |
1501.04651 | Roberto Tateo Prof. | Andrea Cavagli\`a, Martina Cornagliotto, Massimo Mattelliano, Roberto
Tateo | A Riemann-Hilbert formulation for the finite temperature Hubbard model | 43 pages, 13 figures. v2: References added, typos corrected, minor
changes to the text. v3: JHEP published version; typos corrected, references
added and text improved in Section 8 | null | null | null | hep-th cond-mat.str-el math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inspired by recent results in the context of AdS/CFT integrability, we
reconsider the Thermodynamic Bethe Ansatz equations describing the 1D fermionic
Hubbard model at finite temperature. We prove that the infinite set of TBA
equations are equivalent to a simple nonlinear Riemann-Hilbert problem for a
finite number o... | [
{
"created": "Mon, 19 Jan 2015 21:32:04 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Feb 2015 20:16:13 GMT",
"version": "v2"
},
{
"created": "Wed, 3 Jun 2015 16:32:26 GMT",
"version": "v3"
}
] | 2015-06-04 | [
[
"Cavaglià",
"Andrea",
""
],
[
"Cornagliotto",
"Martina",
""
],
[
"Mattelliano",
"Massimo",
""
],
[
"Tateo",
"Roberto",
""
]
] | Inspired by recent results in the context of AdS/CFT integrability, we reconsider the Thermodynamic Bethe Ansatz equations describing the 1D fermionic Hubbard model at finite temperature. We prove that the infinite set of TBA equations are equivalent to a simple nonlinear Riemann-Hilbert problem for a finite number of ... | 6.10535 | 6.683339 | 7.033579 | 6.25112 | 6.328775 | 5.979982 | 6.209314 | 6.227961 | 6.446854 | 7.285995 | 5.958013 | 6.109716 | 6.502671 | 6.043491 | 5.953222 | 6.084 | 6.350315 | 6.055866 | 6.178101 | 6.031711 | 5.976062 |
1201.0768 | Wei Xue | Wei Xue, Xian Gao and Robert Brandenberger | IR Divergences in Inflation and Entropy Perturbations | 28 pages, minor changes in Sec 3.3, reference added | null | 10.1088/1475-7516/2012/06/035 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study leading order perturbative corrections to the two point correlation
function of the scalar field describing the curvature perturbation in a
slow-roll inflationary background, paying particular attention to the
contribution of entropy mode loops. We find that the infrared divergences are
worse than in pure de... | [
{
"created": "Tue, 3 Jan 2012 21:08:44 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Jan 2012 03:45:14 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Xue",
"Wei",
""
],
[
"Gao",
"Xian",
""
],
[
"Brandenberger",
"Robert",
""
]
] | We study leading order perturbative corrections to the two point correlation function of the scalar field describing the curvature perturbation in a slow-roll inflationary background, paying particular attention to the contribution of entropy mode loops. We find that the infrared divergences are worse than in pure de S... | 7.99746 | 7.857943 | 7.799739 | 7.754519 | 7.455323 | 8.071925 | 8.099451 | 7.80878 | 7.768084 | 8.433427 | 8.009544 | 7.622741 | 7.684033 | 7.681773 | 7.719015 | 7.977685 | 7.740216 | 7.812207 | 7.618948 | 7.753617 | 7.536973 |
1810.10540 | Max Zimet | Shamit Kachru, Arnav Tripathy, Max Zimet | K3 metrics from little string theory | 36 pages. v2: added references. v3: updated joke | null | null | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Certain six-dimensional (1,0) supersymmetric little string theories, when
compactified on $T^3$, have moduli spaces of vacua given by smooth K3 surfaces.
Using ideas of Gaiotto-Moore-Neitzke, we show that this provides a systematic
procedure for determining the Ricci-flat metric on a smooth K3 surface in terms
of BPS... | [
{
"created": "Wed, 24 Oct 2018 18:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Dec 2019 20:38:10 GMT",
"version": "v2"
},
{
"created": "Sun, 11 Oct 2020 03:33:34 GMT",
"version": "v3"
}
] | 2020-10-13 | [
[
"Kachru",
"Shamit",
""
],
[
"Tripathy",
"Arnav",
""
],
[
"Zimet",
"Max",
""
]
] | Certain six-dimensional (1,0) supersymmetric little string theories, when compactified on $T^3$, have moduli spaces of vacua given by smooth K3 surfaces. Using ideas of Gaiotto-Moore-Neitzke, we show that this provides a systematic procedure for determining the Ricci-flat metric on a smooth K3 surface in terms of BPS d... | 7.357784 | 6.027686 | 8.631248 | 5.654752 | 6.371143 | 6.368369 | 5.672091 | 5.808713 | 6.216386 | 8.562715 | 5.887444 | 6.272213 | 7.491349 | 6.321787 | 6.383449 | 6.122973 | 6.287524 | 6.459089 | 6.500342 | 7.658681 | 6.442789 |
hep-th/9306038 | null | Katsuyuki Sugiyama | BRST analysis of N=2 superconformal minimal unitary models in Coulomb
gas formalism | 34 pages, 2 eps figures | Int.J.Mod.Phys.A9:5821-5850,1994 | 10.1142/S0217751X94002417 | UT-646 | hep-th | null | We perform a BRST analysis of the N=2 superconformal minimal unitary models.
A bosonic as well as fermionic BRST operators are used to construct irreducible
representations of the N=2 superconformal algebra on the Fock space as BRST
cohomology classes of the BRST operators. Also a character formula is rederived
by us... | [
{
"created": "Mon, 7 Jun 1993 08:50:20 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Sugiyama",
"Katsuyuki",
""
]
] | We perform a BRST analysis of the N=2 superconformal minimal unitary models. A bosonic as well as fermionic BRST operators are used to construct irreducible representations of the N=2 superconformal algebra on the Fock space as BRST cohomology classes of the BRST operators. Also a character formula is rederived by usin... | 7.398396 | 7.149947 | 8.943788 | 6.176942 | 5.967709 | 7.100384 | 7.109988 | 6.845394 | 6.742435 | 8.375721 | 6.113946 | 6.514499 | 7.718435 | 6.60233 | 6.468527 | 6.758677 | 6.365779 | 6.455173 | 6.543854 | 8.03759 | 6.406305 |
hep-th/9503188 | R. Kantowski | H. T. Cho and R. Kantowski | Zeta-Functions for Non-Minimal Operators | 26 pages, additional references | Phys.Rev. D52 (1995) 4588-4599 | 10.1103/PhysRevD.52.4588 | OKHEP-95-02 | hep-th | null | We evaluate zeta-functions $\zeta(s)$ at $s=0$ for invariant non-minimal
2nd-order vector and tensor operators defined on maximally symmetric even
dimensional spaces. We decompose the operators into their irreducible parts and
obtain their corresponding eigenvalues. Using these eigenvalues, we are able to
explicitly ... | [
{
"created": "Mon, 27 Mar 1995 19:39:54 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jul 1995 17:22:31 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Cho",
"H. T.",
""
],
[
"Kantowski",
"R.",
""
]
] | We evaluate zeta-functions $\zeta(s)$ at $s=0$ for invariant non-minimal 2nd-order vector and tensor operators defined on maximally symmetric even dimensional spaces. We decompose the operators into their irreducible parts and obtain their corresponding eigenvalues. Using these eigenvalues, we are able to explicitly ca... | 7.419161 | 7.585161 | 7.088288 | 6.481092 | 7.60489 | 6.766955 | 8.26385 | 6.916697 | 6.6716 | 7.727018 | 6.819773 | 7.137243 | 7.133973 | 6.704771 | 6.964588 | 6.778409 | 6.805621 | 6.864927 | 6.70203 | 7.111247 | 6.605302 |
hep-th/0004055 | Mark Walton | S. E. Irvine, M. A. Walton | Schubert Calculus and Threshold Polynomials of Affine Fusion | 20 pages, 0 figures, harvmac, typos corrected, references added | Nucl.Phys. B584 (2000) 795-809 | 10.1016/S0550-3213(00)00404-1 | null | hep-th math.QA | null | We show how the threshold level of affine fusion, the fusion of
Wess-Zumino-Witten (WZW) conformal field theories, fits into the Schubert
calculus introduced by Gepner. The Pieri rule can be modified in a simple way
to include the threshold level, so that calculations may be done for all
(non-negative integer) levels... | [
{
"created": "Fri, 7 Apr 2000 19:11:15 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Apr 2000 17:50:56 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Irvine",
"S. E.",
""
],
[
"Walton",
"M. A.",
""
]
] | We show how the threshold level of affine fusion, the fusion of Wess-Zumino-Witten (WZW) conformal field theories, fits into the Schubert calculus introduced by Gepner. The Pieri rule can be modified in a simple way to include the threshold level, so that calculations may be done for all (non-negative integer) levels a... | 11.023228 | 10.397003 | 11.943155 | 10.944192 | 11.030425 | 11.253276 | 11.93833 | 11.5198 | 11.165444 | 14.261315 | 10.539627 | 10.889666 | 10.953083 | 10.829239 | 10.708208 | 10.651274 | 10.579543 | 10.620454 | 10.862201 | 11.368317 | 10.487964 |
0704.0262 | Matteo Bertolini | Riccardo Argurio, Matteo Bertolini, Gabriele Ferretti, Alberto Lerda
and Christoffer Petersson | Stringy Instantons at Orbifold Singularities | Latex, 29 pages, 6 figures. v3: typos corrected, one comment and refs
added, published version | JHEP 0706:067,2007 | 10.1088/1126-6708/2007/06/067 | null | hep-th | null | We study the effects produced by D-brane instantons on the holomorphic
quantities of a D-brane gauge theory at an orbifold singularity. These effects
are not limited to reproducing the well known contributions of the gauge theory
instantons but also generate extra terms in the superpotential or the
prepotential. On t... | [
{
"created": "Tue, 3 Apr 2007 16:07:41 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Apr 2007 12:25:27 GMT",
"version": "v2"
},
{
"created": "Mon, 18 Jun 2007 09:53:05 GMT",
"version": "v3"
}
] | 2009-11-13 | [
[
"Argurio",
"Riccardo",
""
],
[
"Bertolini",
"Matteo",
""
],
[
"Ferretti",
"Gabriele",
""
],
[
"Lerda",
"Alberto",
""
],
[
"Petersson",
"Christoffer",
""
]
] | We study the effects produced by D-brane instantons on the holomorphic quantities of a D-brane gauge theory at an orbifold singularity. These effects are not limited to reproducing the well known contributions of the gauge theory instantons but also generate extra terms in the superpotential or the prepotential. On the... | 11.032054 | 12.58731 | 12.896889 | 10.844337 | 12.044767 | 11.635695 | 11.649319 | 11.638 | 11.367929 | 13.111869 | 11.755345 | 10.877541 | 11.65837 | 10.933758 | 11.066084 | 11.132555 | 11.305315 | 10.913383 | 10.611459 | 11.436609 | 10.850631 |
1411.1795 | Rafael Augusto Couceiro Correa | R. A. C. Correa and A. de Souza Dutra | On the study of oscillons in scalar field theories: A new approach | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study configurations in one-dimensional scalar field theory,
which are time-dependent, localized in space and extremely long-lived called
oscillons. It is investigated how the action of changing the minimum value of
the field configuration representing the oscillon affects its behavior. We find
that o... | [
{
"created": "Thu, 6 Nov 2014 23:23:09 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Feb 2016 14:43:50 GMT",
"version": "v2"
}
] | 2016-02-03 | [
[
"Correa",
"R. A. C.",
""
],
[
"Dutra",
"A. de Souza",
""
]
] | In this work we study configurations in one-dimensional scalar field theory, which are time-dependent, localized in space and extremely long-lived called oscillons. It is investigated how the action of changing the minimum value of the field configuration representing the oscillon affects its behavior. We find that one... | 14.060436 | 11.138654 | 12.506866 | 11.069961 | 10.725578 | 11.058485 | 10.737354 | 10.809609 | 10.678249 | 11.503061 | 10.889575 | 11.160669 | 11.925313 | 11.183081 | 11.367244 | 11.326877 | 11.211732 | 11.331833 | 11.440453 | 11.829062 | 11.544658 |
1409.6851 | Hoang Nam Cao | Cao H. Nam | Gauge theory of quantum gravity | 11 pages, discussions and references added, a mistake of Eq. (10)
corrected, results unchanged | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The gravity is classically formulated as the geometric curvature of the
space-time in general relativity which is completely different from the other
well-known physical forces. Since seeking a quantum framework for the gravity
is a great challenge in physics. Here we present an alternative construction of
quantum gr... | [
{
"created": "Wed, 24 Sep 2014 07:41:17 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Sep 2014 09:42:07 GMT",
"version": "v2"
}
] | 2014-09-29 | [
[
"Nam",
"Cao H.",
""
]
] | The gravity is classically formulated as the geometric curvature of the space-time in general relativity which is completely different from the other well-known physical forces. Since seeking a quantum framework for the gravity is a great challenge in physics. Here we present an alternative construction of quantum grav... | 11.754143 | 13.079372 | 11.749892 | 11.783223 | 12.447643 | 12.067921 | 12.963665 | 11.676237 | 11.957806 | 11.136906 | 12.211752 | 11.901013 | 11.405396 | 11.529098 | 11.522234 | 11.669894 | 11.714313 | 11.268559 | 11.889159 | 11.680133 | 11.563216 |
hep-th/0502145 | Sergiu Vacaru I. | Sergiu I. Vacaru | Clifford Algebroids and Nonholonomic Spinor Deformations of Taub-NUT
Spacetimes | 30 pages | null | null | null | hep-th gr-qc math-ph math.DG math.MP | null | In this paper we examine a new class of five dimensional (5D) exact solutions
in extra dimension gravity possessing Lie algebroid symmetry. The constructions
provide a motivation for the theory of Clifford nonholonomic algebroids
elaborated in Ref. hep-th/0501217. Such Einstein-Dirac spacetimes are
parametrized by ge... | [
{
"created": "Wed, 16 Feb 2005 14:11:33 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Vacaru",
"Sergiu I.",
""
]
] | In this paper we examine a new class of five dimensional (5D) exact solutions in extra dimension gravity possessing Lie algebroid symmetry. The constructions provide a motivation for the theory of Clifford nonholonomic algebroids elaborated in Ref. hep-th/0501217. Such Einstein-Dirac spacetimes are parametrized by gene... | 13.89089 | 14.873043 | 12.381068 | 13.017411 | 17.027243 | 13.748786 | 14.230213 | 13.715802 | 13.553389 | 15.355167 | 14.567465 | 13.693832 | 12.73652 | 12.767257 | 13.492545 | 13.398087 | 14.42831 | 13.150538 | 13.823111 | 13.458493 | 13.895792 |
hep-th/9909219 | Ken Intriligator | Kenneth Intriligator | Compactified Little String Theories and Compact Moduli Spaces of Vacua | 12 pages, harvmac; v2:added reference | Phys.Rev.D61:106005,2000 | 10.1103/PhysRevD.61.106005 | UCSD/PTH 99-12, IASSNS-HEP-99/86 | hep-th | null | It is emphasized that compactified little string theories have compact moduli
spaces of vacua, which globally probe compact string geometry. Compactifying
various little string theories on T^3 leads to 3d theories with exact, quantum
Coulomb branch given by: an arbitrary T^4 of volume M_s^2, an arbitrary K3 of
volume... | [
{
"created": "Wed, 29 Sep 1999 21:03:20 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Oct 1999 20:18:45 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Intriligator",
"Kenneth",
""
]
] | It is emphasized that compactified little string theories have compact moduli spaces of vacua, which globally probe compact string geometry. Compactifying various little string theories on T^3 leads to 3d theories with exact, quantum Coulomb branch given by: an arbitrary T^4 of volume M_s^2, an arbitrary K3 of volume M... | 12.899718 | 11.756573 | 13.381192 | 11.912496 | 14.00682 | 11.300205 | 11.874553 | 11.8964 | 10.952529 | 13.416741 | 11.075129 | 10.797632 | 12.321922 | 11.38707 | 11.609232 | 11.533913 | 11.24353 | 11.077548 | 11.438005 | 12.294804 | 11.431021 |
hep-th/9503183 | null | E.Celeghini, M.Rasetti and G.Vitiello (Phys. Dept. Univ.ty of
Florence, Italy) | IDENTICAL PARTICLES AND PERMUTATION GROUP | 8 pages, tex, J. of Phys. A:Math. and General, in print | J.Phys.A28:L239-L244,1995 | 10.1088/0305-4470/28/8/003 | null | hep-th | null | Second quantization is revisited and creation and annihilation operators are
shown to be related, on the same footing both to the algebra ${\it h}(1)$,
${\underline {and}}$ to the superalgebra ${\it osp}(1|2)$ that are shown to be
both compatible with Bose ${\underline {and}}$ Fermi statistics. The two
algebras are c... | [
{
"created": "Mon, 27 Mar 1995 13:39:29 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Celeghini",
"E.",
"",
"Phys. Dept. Univ.ty of\n Florence, Italy"
],
[
"Rasetti",
"M.",
"",
"Phys. Dept. Univ.ty of\n Florence, Italy"
],
[
"Vitiello",
"G.",
"",
"Phys. Dept. Univ.ty of\n Florence, Italy"
]
] | Second quantization is revisited and creation and annihilation operators are shown to be related, on the same footing both to the algebra ${\it h}(1)$, ${\underline {and}}$ to the superalgebra ${\it osp}(1|2)$ that are shown to be both compatible with Bose ${\underline {and}}$ Fermi statistics. The two algebras are com... | 11.129968 | 8.746981 | 10.943694 | 9.235067 | 8.074554 | 8.210902 | 7.484001 | 8.606314 | 8.353498 | 11.142205 | 9.339576 | 9.165664 | 10.829185 | 9.279127 | 9.197011 | 9.508792 | 8.971918 | 9.424178 | 9.36036 | 10.365205 | 9.484128 |
1812.01135 | Tomonori Ugajin | Tomonori Ugajin | Perturbative expansions of R\'enyi relative divergences and holography | 23+11 pages, 2 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we develop a novel way to perturbatively calculate R\'enyi
relative divergences $D_{\gamma}(\rho|| \sigma) ={\rm tr} \rho^{\gamma}
\sigma^{1-\gamma}$ and related quantities without using replica trick as well
as analytic continuation. We explicitly determine the form of the perturbative
term at any ord... | [
{
"created": "Mon, 3 Dec 2018 23:49:21 GMT",
"version": "v1"
}
] | 2018-12-05 | [
[
"Ugajin",
"Tomonori",
""
]
] | In this paper, we develop a novel way to perturbatively calculate R\'enyi relative divergences $D_{\gamma}(\rho|| \sigma) ={\rm tr} \rho^{\gamma} \sigma^{1-\gamma}$ and related quantities without using replica trick as well as analytic continuation. We explicitly determine the form of the perturbative term at any order... | 10.415343 | 9.492615 | 11.007207 | 8.966405 | 10.66239 | 10.414931 | 9.81429 | 10.106112 | 9.347185 | 12.607892 | 9.032247 | 9.389501 | 9.88769 | 9.670061 | 9.253636 | 9.127495 | 9.291023 | 9.741364 | 9.393157 | 10.233266 | 9.766937 |
1904.02871 | Parinya Karndumri | Parinya Karndumri and Patharadanai Nuchino | Supersymmetric domain walls in 7D maximal gauged supergravity | 38 pages, no figures, typos corrected and references added | Eur. Phys. J. C 79 (2019) 648 | 10.1140/epjc/s10052-019-7168-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a large class of supersymmetric domain walls in maximal
seven-dimensional gauged supergravity with various types of gauge groups.
Gaugings are described by components of the embedding tensor transforming in
representations $\mathbf{15}$ and $\overline{\mathbf{40}}$ of the global
symmetry $SL(5)$. The embeddin... | [
{
"created": "Fri, 5 Apr 2019 05:14:22 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Apr 2019 13:35:43 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Aug 2019 17:42:26 GMT",
"version": "v3"
}
] | 2019-08-27 | [
[
"Karndumri",
"Parinya",
""
],
[
"Nuchino",
"Patharadanai",
""
]
] | We give a large class of supersymmetric domain walls in maximal seven-dimensional gauged supergravity with various types of gauge groups. Gaugings are described by components of the embedding tensor transforming in representations $\mathbf{15}$ and $\overline{\mathbf{40}}$ of the global symmetry $SL(5)$. The embedding ... | 3.705285 | 3.353079 | 4.656379 | 3.402982 | 3.774548 | 3.564595 | 3.629719 | 3.324057 | 3.548563 | 4.465511 | 3.438603 | 3.588305 | 3.978355 | 3.565203 | 3.726314 | 3.629467 | 3.557227 | 3.632815 | 3.617661 | 4.077444 | 3.579684 |
hep-th/9301111 | Leon Takhtajan | Leon Takhtajan | On Foundation of the Generalized Nambu Mechanics | 27 pages | Commun.Math.Phys. 160 (1994) 295-316 | 10.1007/BF02103278 | null | hep-th math.SG | null | We outline the basic principles of canonical formalism for the Nambu
mechanics---a generalization of Hamiltonian mechanics proposed by Yoichiro
Nambu in 1973. It is based on the notion of Nambu bracket which generalizes the
Poisson bracket to the multiple operation of higher order $n \geq 3$ on
classical observables ... | [
{
"created": "Tue, 26 Jan 1993 20:45:26 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Takhtajan",
"Leon",
""
]
] | We outline the basic principles of canonical formalism for the Nambu mechanics---a generalization of Hamiltonian mechanics proposed by Yoichiro Nambu in 1973. It is based on the notion of Nambu bracket which generalizes the Poisson bracket to the multiple operation of higher order $n \geq 3$ on classical observables an... | 9.150675 | 9.25946 | 11.012641 | 9.59335 | 10.305919 | 10.470268 | 9.714588 | 9.955572 | 9.13691 | 11.856849 | 9.59124 | 8.904316 | 10.482854 | 9.143953 | 9.144374 | 9.21473 | 9.012796 | 8.905987 | 8.982463 | 9.556934 | 8.91726 |
hep-th/9606011 | null | T.D. Palev, N.I. Stoilova | Many-Body Wigner Quantum Systems | 20 pages, PlainTex | J.Math.Phys. 38 (1997) 2506-2523 | 10.1063/1.531991 | IC/96/82 | hep-th | null | We present examples of many-body Wigner quantum systems. The position and the
momentum operators ${\bf R}_A$ and ${\bf P}_A,\; A=1,\ldots,n+1$, of the
particles are noncanonical and are chosen so that the Heisenberg and the
Hamiltonian equations are identical. The spectrum of the energy with respect to
the centre of ... | [
{
"created": "Tue, 4 Jun 1996 10:58:11 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Palev",
"T. D.",
""
],
[
"Stoilova",
"N. I.",
""
]
] | We present examples of many-body Wigner quantum systems. The position and the momentum operators ${\bf R}_A$ and ${\bf P}_A,\; A=1,\ldots,n+1$, of the particles are noncanonical and are chosen so that the Heisenberg and the Hamiltonian equations are identical. The spectrum of the energy with respect to the centre of ma... | 11.99819 | 10.871193 | 11.816862 | 10.334492 | 10.618122 | 10.327421 | 9.746299 | 10.638924 | 11.198027 | 12.992157 | 10.586068 | 10.471514 | 10.966535 | 10.665771 | 10.219242 | 10.803815 | 11.042251 | 10.739283 | 10.794646 | 11.161082 | 10.332261 |
1307.1460 | Carlos Eduardo Pellicer de Oliveira | E. Abdalla, Jeferson de Oliveira, A. B. Pavan, C. E. Pellicer | Holographic Phase Transitions in (2+1)-dimensional black hole spacetimes
in NMG | 19 pages, 36 figures | Braz J Phys 54, 50 (2024) | 10.1007/s13538-024-01429-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we aim at the question of holographic phase transitions in two
dimensional systems with Lifshitz scaling. We consider the gravity side
candidate for a dual description as the black hole solution of New Massive
Gravity (NMG) with Lifshitz scaling. We discuss the effects due to the Lifshitz
scaling in the ... | [
{
"created": "Thu, 4 Jul 2013 19:47:22 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jul 2013 17:52:00 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Jul 2021 12:13:02 GMT",
"version": "v3"
},
{
"created": "Thu, 15 Jul 2021 17:20:25 GMT",
"version": "v4"
},
{
"cr... | 2024-02-06 | [
[
"Abdalla",
"E.",
""
],
[
"de Oliveira",
"Jeferson",
""
],
[
"Pavan",
"A. B.",
""
],
[
"Pellicer",
"C. E.",
""
]
] | In this work we aim at the question of holographic phase transitions in two dimensional systems with Lifshitz scaling. We consider the gravity side candidate for a dual description as the black hole solution of New Massive Gravity (NMG) with Lifshitz scaling. We discuss the effects due to the Lifshitz scaling in the AG... | 10.33649 | 12.114449 | 10.930332 | 11.028842 | 11.343922 | 12.889895 | 12.035108 | 10.970481 | 11.522692 | 14.065288 | 11.245678 | 10.32478 | 10.300417 | 9.10716 | 9.673359 | 10.420283 | 10.159521 | 9.703743 | 9.516755 | 10.521829 | 10.308479 |
2112.07587 | Fran\c{c}ois Rondeau | Ignatios Antoniadis, Fran\c{c}ois Rondeau | Minimal embedding of the Standard Model into intersecting D-brane
configurations with a bulk leptonic $U(1)$ | 20 pages. Published version | Eur. Phys. J. C 82, 701 (2022) | 10.1140/epjc/s10052-022-10660-y | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been recently shown that the discrepancy between the theoretical and
experimental values of the anomalous magnetic moment of the muon can be fully
accommodated by considering the contribution of few Kaluza-Klein (KK) states of
the gauged lepton number with masses lighter than the LEP energy, consistently
with ... | [
{
"created": "Tue, 14 Dec 2021 17:44:39 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Aug 2022 13:29:03 GMT",
"version": "v2"
}
] | 2022-08-16 | [
[
"Antoniadis",
"Ignatios",
""
],
[
"Rondeau",
"François",
""
]
] | It has been recently shown that the discrepancy between the theoretical and experimental values of the anomalous magnetic moment of the muon can be fully accommodated by considering the contribution of few Kaluza-Klein (KK) states of the gauged lepton number with masses lighter than the LEP energy, consistently with pr... | 6.357088 | 7.857623 | 6.686125 | 6.577328 | 7.249099 | 7.593421 | 7.09404 | 7.191932 | 6.505188 | 6.908766 | 6.576444 | 6.584671 | 6.293581 | 6.206863 | 6.370112 | 6.474302 | 6.361385 | 6.512506 | 6.398837 | 6.492941 | 6.273018 |
hep-th/9302034 | Stepanenko Alexander | S.E. Derkachov, N.A. Kivel, A.S. Stepanenko, A.N. Vasiliev | On Calculation of 1/n Expansions of Critical Exponents in the
Gross-Neveu Model with the Conformal Technique | null | null | null | null | hep-th | null | A proof of critical conformal invariance of Green's functions for a quite
wide class of models possessing critical scale invariance is given. A simple
method for establishing critical conformal invariance of a composite operator,
which has a certain critical dimension, is also presented. The method is
illustrated wit... | [
{
"created": "Tue, 9 Feb 1993 15:46:08 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Mar 1993 12:58:44 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Derkachov",
"S. E.",
""
],
[
"Kivel",
"N. A.",
""
],
[
"Stepanenko",
"A. S.",
""
],
[
"Vasiliev",
"A. N.",
""
]
] | A proof of critical conformal invariance of Green's functions for a quite wide class of models possessing critical scale invariance is given. A simple method for establishing critical conformal invariance of a composite operator, which has a certain critical dimension, is also presented. The method is illustrated with ... | 10.03392 | 10.648857 | 10.903043 | 9.588591 | 9.850233 | 10.820116 | 11.359162 | 10.438485 | 10.25805 | 10.36139 | 10.023618 | 9.360744 | 9.51269 | 9.394518 | 9.661119 | 9.498167 | 9.542759 | 9.377104 | 9.27492 | 9.205408 | 9.368749 |
1209.1068 | Itzhak Bars | Itzhak Bars | Traversing Cosmological Singularities, Complete Journeys Through
Spacetime Including Antigravity | 14 pages, 9 figures, minor corrections in v2 | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A unique description of the Big Crunch-Big Bang transition is given at the
classical gravity level, along with a complete set of homogeneous, isotropic,
analytic solutions in scalar-tensor cosmology, with radiation and curvature.
All solutions repeat cyclically; they have been obtained by using conformal
gauge symmet... | [
{
"created": "Wed, 5 Sep 2012 18:17:44 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Sep 2012 14:17:19 GMT",
"version": "v2"
}
] | 2012-09-07 | [
[
"Bars",
"Itzhak",
""
]
] | A unique description of the Big Crunch-Big Bang transition is given at the classical gravity level, along with a complete set of homogeneous, isotropic, analytic solutions in scalar-tensor cosmology, with radiation and curvature. All solutions repeat cyclically; they have been obtained by using conformal gauge symmetry... | 13.55564 | 15.008336 | 13.971528 | 13.08075 | 13.080962 | 13.85289 | 13.749946 | 13.034943 | 13.040096 | 14.245781 | 13.410853 | 12.719325 | 12.840497 | 12.670798 | 12.692969 | 12.716897 | 12.498544 | 12.447921 | 12.689442 | 13.167914 | 12.613977 |
1110.0201 | S. Mignemi | S. Mignemi | Classical and quantum mechanics of the nonrelativistic Snyder model in
curved space | 21 pages; discussion of three-dimensional quantum mechanics added,
error in quantum commutators corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Snyder-de Sitter (SdS) model is a generalization of the Snyder model to a
spacetime background of constant curvature. It is an example of noncommutative
spacetime admitting two fundamental scales besides the speed of light, and is
invariant under the action of the de Sitter group. Here we consider its
nonrelativi... | [
{
"created": "Sun, 2 Oct 2011 16:32:22 GMT",
"version": "v1"
},
{
"created": "Sat, 21 Jul 2012 09:53:05 GMT",
"version": "v2"
}
] | 2012-07-24 | [
[
"Mignemi",
"S.",
""
]
] | The Snyder-de Sitter (SdS) model is a generalization of the Snyder model to a spacetime background of constant curvature. It is an example of noncommutative spacetime admitting two fundamental scales besides the speed of light, and is invariant under the action of the de Sitter group. Here we consider its nonrelativist... | 5.726184 | 5.463097 | 5.519831 | 5.308354 | 5.436744 | 5.536427 | 5.739759 | 5.299055 | 5.362093 | 5.695936 | 5.318691 | 5.276541 | 5.396246 | 5.184531 | 5.308225 | 5.241997 | 5.177678 | 5.272292 | 5.291672 | 5.334323 | 5.186397 |
1906.02206 | Ben Heidenreich | Ben Heidenreich, Matthew Reece, Tom Rudelius | Repulsive Forces and the Weak Gravity Conjecture | 57 pages, 6 figures; v2: matches published version | JHEP 10 (2019) 055 | 10.1007/JHEP10(2019)055 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Weak Gravity Conjecture is a nontrivial conjecture about quantum gravity
that makes sharp, falsifiable predictions which can be checked in a broad range
of string theory examples. However, in the presence of massless scalar fields
(moduli), there are (at least) two inequivalent forms of the conjecture, one
based ... | [
{
"created": "Wed, 5 Jun 2019 18:00:04 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Oct 2020 21:19:14 GMT",
"version": "v2"
}
] | 2020-11-02 | [
[
"Heidenreich",
"Ben",
""
],
[
"Reece",
"Matthew",
""
],
[
"Rudelius",
"Tom",
""
]
] | The Weak Gravity Conjecture is a nontrivial conjecture about quantum gravity that makes sharp, falsifiable predictions which can be checked in a broad range of string theory examples. However, in the presence of massless scalar fields (moduli), there are (at least) two inequivalent forms of the conjecture, one based on... | 7.532588 | 6.99282 | 7.551791 | 6.5004 | 7.232259 | 6.928012 | 6.846575 | 6.994481 | 6.713375 | 7.813633 | 7.021433 | 7.166904 | 7.1436 | 6.694448 | 6.822232 | 6.773996 | 7.024079 | 7.012355 | 6.811468 | 6.899794 | 6.83742 |
hep-th/0305162 | Zappala' Dario | P. Castorina, M. Mazza, D. Zappala' | Renormalization group analysis of the three-dimensional Gross-Neveu
model at finite temperature and density | Latex file, 12 pages, 2 eps figures, minor changes, added references,
published version | Phys.Lett. B567 (2003) 31-38 | 10.1016/j.physletb.2003.06.005 | null | hep-th | null | The Renormalization Group flow equations obtained by means of a proper time
regulator are used to analyze the restoration of the discrete chiral symmetry
at non-zero density and temperature in the Gross-Neveu model in d=2+1
dimensions. The effects of the wave function renormalization of the auxiliary
scalar field on ... | [
{
"created": "Mon, 19 May 2003 17:30:34 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Dec 2003 11:17:59 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Castorina",
"P.",
""
],
[
"Mazza",
"M.",
""
],
[
"Zappala'",
"D.",
""
]
] | The Renormalization Group flow equations obtained by means of a proper time regulator are used to analyze the restoration of the discrete chiral symmetry at non-zero density and temperature in the Gross-Neveu model in d=2+1 dimensions. The effects of the wave function renormalization of the auxiliary scalar field on th... | 7.933887 | 6.212293 | 6.855255 | 6.222497 | 6.693949 | 7.059338 | 6.46249 | 6.707929 | 6.452721 | 7.238509 | 6.614457 | 6.69108 | 7.081895 | 6.840784 | 6.699406 | 7.275731 | 7.010355 | 6.87249 | 6.877031 | 7.031507 | 6.820311 |
2008.13573 | Mikhail Volkov | Romain Gervalle and Mikhail S. Volkov | Asymptotically flat hairy black holes in massive bigravity | 57 pages, many figures, matches the published version | Phys. Rev. D 102, 124040 (2020) | 10.1103/PhysRevD.102.124040 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study asymptotically flat black holes with massive graviton hair within
the ghost-free bigravity theory. There have been contradictory statements in
the literature about their existence -- such solutions were reported some time
ago, but later a different group claimed the Schwarzschild solution to be the
only asym... | [
{
"created": "Mon, 31 Aug 2020 12:57:35 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Sep 2020 12:15:34 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Nov 2020 14:10:14 GMT",
"version": "v3"
},
{
"created": "Wed, 23 Dec 2020 17:25:09 GMT",
"version": "v4"
}
] | 2021-01-04 | [
[
"Gervalle",
"Romain",
""
],
[
"Volkov",
"Mikhail S.",
""
]
] | We study asymptotically flat black holes with massive graviton hair within the ghost-free bigravity theory. There have been contradictory statements in the literature about their existence -- such solutions were reported some time ago, but later a different group claimed the Schwarzschild solution to be the only asympt... | 9.612155 | 9.570953 | 9.742579 | 9.183838 | 9.818874 | 10.080382 | 9.479449 | 9.441629 | 9.649747 | 10.338013 | 9.196136 | 9.308531 | 9.426907 | 9.257704 | 9.582049 | 9.378828 | 9.198011 | 9.255733 | 9.43869 | 9.466794 | 9.189382 |
hep-th/0301129 | Christian Armendariz-Picon | C. Armendariz-Picon and Patrick B. Greene | Spinors, Inflation, and Non-Singular Cyclic Cosmologies | 12 two-column pages, 3 figures; uses RevTeX4 | Gen.Rel.Grav.35:1637-1658,2003 | 10.1023/A:1025783118888 | FERMILAB-Pub-03/014-A | hep-th astro-ph gr-qc | null | We consider toy cosmological models in which a classical, homogeneous, spinor
field provides a dominant or sub-dominant contribution to the energy-momentum
tensor of a flat Friedmann-Robertson-Walker universe. We find that, if such a
field were to exist, appropriate choices of the spinor self-interaction would
genera... | [
{
"created": "Mon, 20 Jan 2003 20:56:13 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Armendariz-Picon",
"C.",
""
],
[
"Greene",
"Patrick B.",
""
]
] | We consider toy cosmological models in which a classical, homogeneous, spinor field provides a dominant or sub-dominant contribution to the energy-momentum tensor of a flat Friedmann-Robertson-Walker universe. We find that, if such a field were to exist, appropriate choices of the spinor self-interaction would generate... | 9.185463 | 9.138835 | 8.977348 | 9.137398 | 9.70143 | 10.134963 | 9.63718 | 8.958563 | 9.511021 | 9.686162 | 9.520004 | 9.3093 | 9.211901 | 8.907926 | 9.038345 | 9.093402 | 8.987656 | 9.202817 | 8.960355 | 9.413954 | 9.249613 |
hep-th/0008019 | Hiroyuki T. Takata | Hiroyuki Takata (Matscience, Chennai) | Electric-Magnetic Duality in IIB Matrix Model with D-brane | Latex, 15 pages, 1 figure, talk at Lattice 2000, 17-22 August 2000,
Bangalore, India | null | null | null | hep-th | null | We consider electric-magnetic duality(S-duality) in IIB matrix model with a
D3-brane background. We propose the duality transformation by considering that
of noncommutative Yang-Mills theory(NCYM) in four dimension. NCYM derived from
the matrix model has a Yang-Mills coupling related to the noncommutativity of
the sp... | [
{
"created": "Wed, 2 Aug 2000 20:34:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Takata",
"Hiroyuki",
"",
"Matscience, Chennai"
]
] | We consider electric-magnetic duality(S-duality) in IIB matrix model with a D3-brane background. We propose the duality transformation by considering that of noncommutative Yang-Mills theory(NCYM) in four dimension. NCYM derived from the matrix model has a Yang-Mills coupling related to the noncommutativity of the spac... | 15.125951 | 13.780927 | 15.797575 | 13.402837 | 15.455157 | 15.231982 | 15.328611 | 14.171974 | 13.129775 | 17.110632 | 13.778693 | 13.934995 | 15.979217 | 13.985052 | 14.196698 | 14.477739 | 14.305517 | 13.812203 | 14.043882 | 15.235305 | 13.707273 |
1612.03840 | Georgios Pastras | Georgios Pastras | Revisiting the O(3) Non-linear Sigma Model and Its Pohlmeyer Reduction | 27 pages, 3 figures | Fortsch.Phys. 66 (2018) no.1, 1700067 | 10.1002/prop.201700067 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well known that sigma models in symmetric spaces accept equivalent
descriptions in terms of integrable systems such as the sine-Gordon equation
through Pohlmeyer reduction. In this paper, we study the mapping between known
solutions of the Euclidean O(3) non-linear sigma model, such as instantons,
merons and el... | [
{
"created": "Mon, 12 Dec 2016 18:39:37 GMT",
"version": "v1"
}
] | 2018-01-10 | [
[
"Pastras",
"Georgios",
""
]
] | It is well known that sigma models in symmetric spaces accept equivalent descriptions in terms of integrable systems such as the sine-Gordon equation through Pohlmeyer reduction. In this paper, we study the mapping between known solutions of the Euclidean O(3) non-linear sigma model, such as instantons, merons and elli... | 7.710981 | 8.233342 | 9.140929 | 7.763667 | 7.79434 | 7.435538 | 7.549973 | 8.117249 | 7.66647 | 9.704846 | 7.267024 | 7.51753 | 7.731919 | 7.656434 | 7.635487 | 7.578357 | 7.720393 | 7.624991 | 7.208247 | 7.91694 | 7.312689 |
1905.02039 | Ljubica Davidovic | Ljubica Davidovi\'c and Branislav Sazdovi\'c | Effective theories of two T-dual theories are also T-dual | null | Eur. Phys. J. C (2019) 79: 770 | 10.1140/epjc/s10052-019-7266-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate how T-duality and solving the boundary conditions of the open
bosonic string are related. We start by considering the T-dualization of the
open string moving in the constant background. We take that the coordinates of
the initial theory satisfy either Neumann or Dirichlet boundary conditions. It
follow... | [
{
"created": "Mon, 6 May 2019 13:36:23 GMT",
"version": "v1"
}
] | 2019-10-21 | [
[
"Davidović",
"Ljubica",
""
],
[
"Sazdović",
"Branislav",
""
]
] | We investigate how T-duality and solving the boundary conditions of the open bosonic string are related. We start by considering the T-dualization of the open string moving in the constant background. We take that the coordinates of the initial theory satisfy either Neumann or Dirichlet boundary conditions. It follows ... | 8.809638 | 9.071574 | 10.556537 | 8.486447 | 9.005658 | 8.587279 | 8.323521 | 8.390328 | 8.65709 | 10.502484 | 8.47508 | 8.236508 | 9.075685 | 8.490752 | 8.56328 | 8.603641 | 8.356556 | 8.540872 | 8.550609 | 9.007494 | 8.55769 |
1711.07787 | Tim De Jonckheere | Tim De Jonckheere | Modave lectures on bulk reconstruction in AdS/CFT | 35 pages, 8 figures, lecture notes, v4: a few minor improvements upon
the published proceedings version (version 3 of these lecture notes in arXiv)
have been implemented | PoS Modave2017 (2018) 005 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | These lecture notes are based on a series of lectures given at the XIII
Modave summer school in mathematical physics. We review the construction due to
Hamilton, Kabat, Lifschytz and Lowe for reconstructing local bulk operators
from CFT operators in the context of AdS/CFT and show how to recover bulk
correlation func... | [
{
"created": "Tue, 21 Nov 2017 13:55:29 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Dec 2017 13:01:07 GMT",
"version": "v2"
},
{
"created": "Thu, 29 Mar 2018 10:04:13 GMT",
"version": "v3"
},
{
"created": "Wed, 27 Jun 2018 16:37:39 GMT",
"version": "v4"
}
] | 2018-06-28 | [
[
"De Jonckheere",
"Tim",
""
]
] | These lecture notes are based on a series of lectures given at the XIII Modave summer school in mathematical physics. We review the construction due to Hamilton, Kabat, Lifschytz and Lowe for reconstructing local bulk operators from CFT operators in the context of AdS/CFT and show how to recover bulk correlation functi... | 9.452649 | 8.546914 | 12.445765 | 8.115237 | 8.432851 | 8.95305 | 8.349463 | 8.455268 | 7.962254 | 11.751452 | 7.915374 | 8.147909 | 9.148487 | 8.421768 | 8.111942 | 8.308024 | 7.818175 | 8.323104 | 8.090126 | 8.704081 | 8.22751 |
0711.2898 | Giuliano Niccoli G. | G. Cristofano, V. Marotta, P. Minnhagen, A. Naddeo and G. Niccoli | New Results on the Phase Diagram of the FFXY Model: A Twisted CFT
Approach | 7 pages; talk given by G. Niccoli at "Path Integrals - New Trends and
Perspectives International Conference", Max-Planck-Institut, Dresden,
Germany, September 23 - 28, 2007 | null | 10.1142/9789812837271_0076 | null | hep-th | null | The issue of the number, nature and sequence of phase transitions in the
fully frustrated XY (FFXY) model is a highly non trivial one due to the complex
interplay between its continuous and discrete degrees of freedom. In this
contribution we attack such a problem by means of a twisted conformal field
theory (CFT) ap... | [
{
"created": "Mon, 19 Nov 2007 11:26:57 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Cristofano",
"G.",
""
],
[
"Marotta",
"V.",
""
],
[
"Minnhagen",
"P.",
""
],
[
"Naddeo",
"A.",
""
],
[
"Niccoli",
"G.",
""
]
] | The issue of the number, nature and sequence of phase transitions in the fully frustrated XY (FFXY) model is a highly non trivial one due to the complex interplay between its continuous and discrete degrees of freedom. In this contribution we attack such a problem by means of a twisted conformal field theory (CFT) appr... | 8.690731 | 9.086022 | 8.95984 | 8.582989 | 8.594677 | 9.047523 | 8.447835 | 8.603384 | 9.177032 | 9.066607 | 8.207494 | 8.378629 | 8.751756 | 8.533128 | 8.405997 | 8.306036 | 8.293003 | 8.203963 | 8.933346 | 8.911799 | 8.249205 |
hep-th/0009160 | Shinpei Kobayashi | Shinpei Kobayashi, Kazuya Koyama and Jiro Soda | Quantum Fluctuations of Bulk Inflaton in Inflationary Brane World | 14 pages, 2 figures | Phys.Lett. B501 (2001) 157-164 | 10.1016/S0370-2693(01)00137-X | KUCP0168 | hep-th astro-ph gr-qc | null | The inflationary scenario for the brane world driven by the bulk inflaton is
proposed. The quantum fluctuations of the inflaton is calculated and compared
to those of the conventional 4-dimensional inflationary scenario. It is shown
that the deviation of the primordial spectrum of this model from that of the
conventi... | [
{
"created": "Thu, 21 Sep 2000 02:06:34 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Kobayashi",
"Shinpei",
""
],
[
"Koyama",
"Kazuya",
""
],
[
"Soda",
"Jiro",
""
]
] | The inflationary scenario for the brane world driven by the bulk inflaton is proposed. The quantum fluctuations of the inflaton is calculated and compared to those of the conventional 4-dimensional inflationary scenario. It is shown that the deviation of the primordial spectrum of this model from that of the convention... | 7.705369 | 6.462989 | 6.327795 | 6.18518 | 6.692549 | 6.202496 | 6.304057 | 6.031694 | 6.829816 | 7.295258 | 6.719213 | 6.86918 | 6.804341 | 6.784367 | 6.580376 | 6.632598 | 6.880619 | 6.777489 | 6.812846 | 6.775797 | 6.93495 |
hep-th/9304141 | Andreas Fring | A. Fring and R. K\"oberle | Factorized Scattering in the Presence of Reflecting Boundaries | 18p., USP-IFQSC/TH/93-06 | Nucl.Phys.B421:159-172,1994 | 10.1016/0550-3213(94)90229-1 | null | hep-th | null | We formulate a general set of consistency requirements, which are expected to
be satisfied by the scattering matrices in the presence of reflecting
boundaries. In particular we derive an equivalent to the boostrap equation
involving the W-matrix, which encodes the reflection of a particle off a wall.
This set of equa... | [
{
"created": "Tue, 27 Apr 1993 19:06:00 GMT",
"version": "v1"
}
] | 2011-05-05 | [
[
"Fring",
"A.",
""
],
[
"Köberle",
"R.",
""
]
] | We formulate a general set of consistency requirements, which are expected to be satisfied by the scattering matrices in the presence of reflecting boundaries. In particular we derive an equivalent to the boostrap equation involving the W-matrix, which encodes the reflection of a particle off a wall. This set of equati... | 16.136835 | 10.73219 | 15.253827 | 11.411396 | 11.337073 | 10.882258 | 12.692692 | 12.155518 | 10.703394 | 15.632961 | 12.046752 | 10.795187 | 14.881379 | 11.670579 | 10.923567 | 11.183393 | 11.024509 | 11.607654 | 11.681698 | 14.030576 | 11.45899 |
hep-th/9408019 | Eduardo Ramos | E. Ramos and J. Roca | W-symmetry and the rigid particle | 14 pages, plain TeX (macros included). QMW-PH-94-23 | Nucl.Phys. B436 (1995) 529-544 | 10.1016/0550-3213(94)00507-B | null | hep-th | null | We prove that $\W_3$ is the gauge symmetry of the scale-invariant rigid
particle, whose action is given by the integrated extrinsic curvature of its
world line. This is achieved by showing that its equations of motion can be
written in terms of the Boussinesq operator. The $\W_3$ generators $T$ and $W$
then appear re... | [
{
"created": "Wed, 3 Aug 1994 16:24:12 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ramos",
"E.",
""
],
[
"Roca",
"J.",
""
]
] | We prove that $\W_3$ is the gauge symmetry of the scale-invariant rigid particle, whose action is given by the integrated extrinsic curvature of its world line. This is achieved by showing that its equations of motion can be written in terms of the Boussinesq operator. The $\W_3$ generators $T$ and $W$ then appear resp... | 8.723063 | 9.015874 | 9.075025 | 8.206689 | 8.964222 | 9.121402 | 8.415685 | 8.699013 | 8.320374 | 10.406091 | 8.403419 | 8.695037 | 8.255427 | 8.311234 | 8.470775 | 8.649349 | 8.433696 | 8.440742 | 8.248176 | 8.678559 | 8.2448 |
1911.12388 | Pietro Ferrero | Pietro Ferrero, Kausik Ghosh, Aninda Sinha, Ahmadullah Zahed | Crossing symmetry, transcendentality and the Regge behaviour of 1d CFTs | 90 pages, 6 figures | null | 10.1007/JHEP07(2020)170 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop the technology for Polyakov-Mellin (PM) bootstrap in
one-dimensional conformal field theories (CFT$_1$). By adding appropriate
contact terms, we bootstrap various effective field theories in AdS$_2$ and
analytically compute the CFT data to one loop. The computation can be extended
to higher orders in pertu... | [
{
"created": "Wed, 27 Nov 2019 19:26:39 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Apr 2020 20:28:32 GMT",
"version": "v2"
}
] | 2020-08-26 | [
[
"Ferrero",
"Pietro",
""
],
[
"Ghosh",
"Kausik",
""
],
[
"Sinha",
"Aninda",
""
],
[
"Zahed",
"Ahmadullah",
""
]
] | We develop the technology for Polyakov-Mellin (PM) bootstrap in one-dimensional conformal field theories (CFT$_1$). By adding appropriate contact terms, we bootstrap various effective field theories in AdS$_2$ and analytically compute the CFT data to one loop. The computation can be extended to higher orders in perturb... | 11.181969 | 10.921728 | 12.432583 | 10.930466 | 11.774088 | 11.102619 | 11.041556 | 10.512119 | 10.796602 | 12.556553 | 10.566979 | 10.421871 | 11.043383 | 10.378746 | 10.604343 | 10.312551 | 10.654068 | 10.400065 | 10.367803 | 10.809066 | 10.539692 |
hep-th/9202017 | Sheldon Katz | Sheldon Katz | Rational Curves on Calabi-Yau Threefolds | 10 pages. This is a survey talk given at the May 1991 Workshop on
Mirror Symmetry at MSRI | null | null | null | hep-th math.AG | null | By considering mirror symmetry applied to conformal field theories
corresponding to strings propagating in quintic hypersurfaces in projective
4-space, Candelas, de la Ossa, Green and Parkes calculated the ``number of
rational curves on the hypersurface'' by comparing three point functions.
Actually, the number of cu... | [
{
"created": "Wed, 5 Feb 1992 17:52:58 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Katz",
"Sheldon",
""
]
] | By considering mirror symmetry applied to conformal field theories corresponding to strings propagating in quintic hypersurfaces in projective 4-space, Candelas, de la Ossa, Green and Parkes calculated the ``number of rational curves on the hypersurface'' by comparing three point functions. Actually, the number of curv... | 12.351541 | 13.209733 | 16.816347 | 11.542905 | 13.030648 | 13.544082 | 13.487251 | 11.796322 | 12.655464 | 16.487684 | 12.836765 | 11.871422 | 14.170592 | 11.897067 | 11.862226 | 12.220612 | 11.974761 | 12.216239 | 11.769078 | 13.52217 | 11.50989 |
hep-th/0005278 | Ryu Sasaki | S.P. Khastgir and R. Sasaki | Liouville Integrability of Classical Calogero-Moser Models | 8 pages, LaTeX2e, no figures | Phys.Lett. A279 (2001) 189-193 | 10.1016/S0375-9601(00)00842-2 | YITP-00-31 | hep-th cond-mat math-ph math.MP nlin.SI quant-ph | null | Liouville integrability of classical Calogero-Moser models is proved for
models based on any root systems, including the non-crystallographic ones. It
applies to all types of elliptic potentials, i.e. untwisted and twisted
together with their degenerations (hyperbolic, trigonometric and rational),
except for the rati... | [
{
"created": "Tue, 30 May 2000 10:20:29 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Khastgir",
"S. P.",
""
],
[
"Sasaki",
"R.",
""
]
] | Liouville integrability of classical Calogero-Moser models is proved for models based on any root systems, including the non-crystallographic ones. It applies to all types of elliptic potentials, i.e. untwisted and twisted together with their degenerations (hyperbolic, trigonometric and rational), except for the ration... | 9.943649 | 8.762219 | 11.792356 | 9.080875 | 8.419807 | 8.429272 | 8.039993 | 7.659863 | 7.761528 | 10.715691 | 8.252069 | 9.350967 | 9.276019 | 8.474009 | 8.670094 | 9.149662 | 8.499195 | 8.970256 | 8.518363 | 8.577772 | 8.755084 |
2102.10970 | Luigi Alfonsi | Luigi Alfonsi | Towards an extended/higher correspondence -- Generalised geometry,
bundle gerbes and global Double Field Theory | Prepared for submission to Complex Manifolds, special issue:
Generalized Geometry. 35 pages, 2 figures. Published version | Complex Manifolds, vol. 8, special issue "Generalized Geometry"
(2021), pp. 302-328 | 10.1515/coma-2020-0121 | QMUL-PH-21-11 | hep-th math.DG | http://creativecommons.org/licenses/by/4.0/ | In this short paper, we will review the proposal of a correspondence between
the doubled geometry of Double Field Theory and the higher geometry of bundle
gerbes. Double Field Theory is T-duality covariant formulation of the
supergravity limit of String Theory, which generalises Kaluza-Klein theory by
unifying metric... | [
{
"created": "Mon, 22 Feb 2021 13:20:26 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Feb 2021 15:39:06 GMT",
"version": "v2"
},
{
"created": "Wed, 6 Oct 2021 12:24:17 GMT",
"version": "v3"
}
] | 2021-10-27 | [
[
"Alfonsi",
"Luigi",
""
]
] | In this short paper, we will review the proposal of a correspondence between the doubled geometry of Double Field Theory and the higher geometry of bundle gerbes. Double Field Theory is T-duality covariant formulation of the supergravity limit of String Theory, which generalises Kaluza-Klein theory by unifying metric a... | 6.633135 | 6.217554 | 7.158299 | 6.175958 | 6.367023 | 6.476732 | 6.377646 | 5.982405 | 6.392864 | 7.281317 | 6.046977 | 6.376039 | 6.373116 | 6.119384 | 6.120956 | 6.111874 | 6.256669 | 6.136544 | 6.170891 | 6.603185 | 6.0673 |
hep-th/0010132 | J. Bijtebier | J. Bijtebier | Towards a 3D reduction of the N-body Bethe-Salpeter equation | 4 pages. Poster presented at the XVIIth conference on few-body
problems in physics, Evora 2000 | null | null | null | hep-th | null | Starting with the homogeneous Bethe-Salpeter equation for two fermions, we
perform a 3D reduction using a series expansion around an unspecified
positive-energy instantaneous approximation of the kernel. A second series
expansion is made, at the 3D level, in order to get an "hermitian" potential.
The combination of b... | [
{
"created": "Tue, 17 Oct 2000 08:10:21 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bijtebier",
"J.",
""
]
] | Starting with the homogeneous Bethe-Salpeter equation for two fermions, we perform a 3D reduction using a series expansion around an unspecified positive-energy instantaneous approximation of the kernel. A second series expansion is made, at the 3D level, in order to get an "hermitian" potential. The combination of bot... | 14.059702 | 13.877233 | 12.303487 | 11.660425 | 13.914424 | 13.879632 | 12.464293 | 12.217894 | 11.810431 | 14.296999 | 12.283902 | 13.095803 | 12.329719 | 12.584552 | 12.952787 | 12.412215 | 12.838182 | 13.161468 | 12.414313 | 12.585809 | 13.112034 |
1109.4940 | Andreas Stergiou | Jean-Fran\c{c}ois Fortin, Kenneth Intriligator, Andreas Stergiou | Superconformally Covariant OPE and General Gauge Mediation | 33 pages, 4 figures | JHEP12(2011)064 | 10.1007/JHEP12(2011)064 | UCSD-PTH-11-09 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider using broken superconformal symmetry and the super operator
product expansion (sOPE) to constrain and analyze hidden sector theories that
couple to our gauge forces and are not necessarily weakly coupled. Conformal
and supersymmetry breaking are IR effects, associated with field or spurion
expectation val... | [
{
"created": "Thu, 22 Sep 2011 20:00:01 GMT",
"version": "v1"
}
] | 2011-12-20 | [
[
"Fortin",
"Jean-François",
""
],
[
"Intriligator",
"Kenneth",
""
],
[
"Stergiou",
"Andreas",
""
]
] | We consider using broken superconformal symmetry and the super operator product expansion (sOPE) to constrain and analyze hidden sector theories that couple to our gauge forces and are not necessarily weakly coupled. Conformal and supersymmetry breaking are IR effects, associated with field or spurion expectation value... | 9.904756 | 11.633487 | 10.801636 | 9.954907 | 10.831289 | 11.298618 | 10.719079 | 10.634466 | 9.526294 | 11.391298 | 10.019923 | 9.907179 | 10.231481 | 9.809731 | 9.920424 | 9.893784 | 9.639439 | 9.917743 | 9.867595 | 10.290004 | 9.9066 |
1608.00399 | Robert de Mello Koch | Robert de Mello Koch, David Gossman, Lwazi Nkumane, Laila Tribelhorn | Eigenvalue Dynamics for Multimatrix Models | 28+1 pages | Phys. Rev. D 96, 026011 (2017) | 10.1103/PhysRevD.96.026011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By performing explicit computations of correlation functions, we find
evidence that there is a sector of the two matrix model defined by the $SU(2)$
sector of ${\cal N}=4$ super Yang-Mills theory, that can be reduced to
eigenvalue dynamics. There is an interesting generalization of the usual Van
der Monde determinant... | [
{
"created": "Mon, 1 Aug 2016 12:17:39 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Aug 2016 12:28:02 GMT",
"version": "v2"
}
] | 2017-07-19 | [
[
"Koch",
"Robert de Mello",
""
],
[
"Gossman",
"David",
""
],
[
"Nkumane",
"Lwazi",
""
],
[
"Tribelhorn",
"Laila",
""
]
] | By performing explicit computations of correlation functions, we find evidence that there is a sector of the two matrix model defined by the $SU(2)$ sector of ${\cal N}=4$ super Yang-Mills theory, that can be reduced to eigenvalue dynamics. There is an interesting generalization of the usual Van der Monde determinant t... | 9.724165 | 9.146077 | 9.948805 | 8.822304 | 9.391124 | 10.240064 | 9.69558 | 9.041903 | 8.678232 | 11.214276 | 8.50389 | 8.639829 | 9.374806 | 8.610436 | 8.715275 | 8.362031 | 8.950909 | 8.658428 | 8.756935 | 9.559347 | 8.692712 |
1911.08392 | Andre Alves Lima | A.A. Lima, U. Camara da Silva, G.M. Sotkov | Conformal Scale Factor Inversion for Domain Walls and Holography | V2 - improved and extended version; 12 figures; 40 pgs; few
references added. V3 - 55 pages, 7 figures; extended and corrected version;
accepted for publication in Physical Review D | Phys. Rev. D 102, 046009 (2020) | 10.1103/PhysRevD.102.046009 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a correspondence between domain wall solutions of Einstein
gravity with a single scalar field and self-interaction potential. The
correspondence we call 'conformal scale factor inversion (CSFI)' is a map
comprising the inversion of the scale factor in conformal coordinates, and a
transformation of the fie... | [
{
"created": "Tue, 19 Nov 2019 16:51:30 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Jan 2020 06:26:54 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Aug 2020 21:46:16 GMT",
"version": "v3"
}
] | 2020-08-19 | [
[
"Lima",
"A. A.",
""
],
[
"da Silva",
"U. Camara",
""
],
[
"Sotkov",
"G. M.",
""
]
] | We describe a correspondence between domain wall solutions of Einstein gravity with a single scalar field and self-interaction potential. The correspondence we call 'conformal scale factor inversion (CSFI)' is a map comprising the inversion of the scale factor in conformal coordinates, and a transformation of the field... | 11.033629 | 11.302762 | 11.07993 | 10.375062 | 11.081897 | 11.50632 | 11.609801 | 10.810733 | 10.405138 | 12.446344 | 9.984336 | 10.511596 | 10.648645 | 10.307184 | 10.704431 | 10.435222 | 10.788662 | 10.590799 | 10.305167 | 10.83727 | 10.309349 |
1910.04197 | Peter Weck | Ibrahima Bah, Ross Dempsey, and Peter Weck | Kerr-Schild Double Copy and Complex Worldlines | To be published in JHEP. Version updated in include clarifications in
wording, new sentences making a few additional remarks, and typo corrections | J. High Energ. Phys. 2020, 180 (2020) | 10.1007/JHEP02(2020)180 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the classical double copy to identify a necessary condition for
Maxwell theory sources to constitute single copies of Kerr-Schild solutions to
Einstein's equations. In the case of four-dimensional Kerr-Schild spacetimes on
Minkowski backgrounds, we extend this condition to a parameterization of the
correspondi... | [
{
"created": "Wed, 9 Oct 2019 18:37:40 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Feb 2020 19:00:26 GMT",
"version": "v2"
}
] | 2020-03-10 | [
[
"Bah",
"Ibrahima",
""
],
[
"Dempsey",
"Ross",
""
],
[
"Weck",
"Peter",
""
]
] | We use the classical double copy to identify a necessary condition for Maxwell theory sources to constitute single copies of Kerr-Schild solutions to Einstein's equations. In the case of four-dimensional Kerr-Schild spacetimes on Minkowski backgrounds, we extend this condition to a parameterization of the corresponding... | 12.929881 | 12.546941 | 12.91407 | 11.939414 | 11.801858 | 12.028324 | 11.925269 | 12.463933 | 12.28834 | 13.178049 | 11.153687 | 11.283267 | 11.964371 | 11.529166 | 11.79134 | 11.137658 | 11.510789 | 11.676037 | 11.362605 | 12.43611 | 11.185636 |
1807.10512 | Dennis Stock | Jan M. Pawlowski, Dennis Stock | Quantum Improved Schwarzschild-(A)dS and Kerr-(A)dS Space-times | 21 pages, 25 figures | Phys. Rev. D 98, 106008 (2018) | 10.1103/PhysRevD.98.106008 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss quantum black holes in asymptotically safe quantum gravity with a
scale identification based on the Kretschmann scalar. After comparing this
scenario with other scale identifications, we investigate in detail the
Kerr-(A)dS and Schwarzschild-(A)dS space-times. The global structure of these
geometries is st... | [
{
"created": "Fri, 27 Jul 2018 09:46:43 GMT",
"version": "v1"
}
] | 2019-02-11 | [
[
"Pawlowski",
"Jan M.",
""
],
[
"Stock",
"Dennis",
""
]
] | We discuss quantum black holes in asymptotically safe quantum gravity with a scale identification based on the Kretschmann scalar. After comparing this scenario with other scale identifications, we investigate in detail the Kerr-(A)dS and Schwarzschild-(A)dS space-times. The global structure of these geometries is stud... | 10.178675 | 9.56905 | 8.780112 | 9.508085 | 8.875463 | 9.065737 | 10.712546 | 9.147601 | 9.433421 | 9.627967 | 9.452662 | 9.782372 | 9.641664 | 9.67275 | 9.205462 | 9.443343 | 9.290911 | 8.98484 | 9.46408 | 9.385939 | 9.459256 |
1410.5047 | Junjie Rao | Junjie Rao | Soft Theorem of N=4 SYM in Grassmannian Formulation | 17 pages, 2 appendices | JHEP 1502 (2015) 087 | 10.1007/JHEP02(2015)087 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inspired by the new soft theorem in gravity by Cachazo and Strominger, the
soft theorem for color-ordered Yang-Mills amplitudes has also been identified
by Casali. In this note, the same content of N=4 SYM using the Grassmannian
formulation is studied. Explicitly, in the holomorphic soft limit, we reduce
the n-partic... | [
{
"created": "Sun, 19 Oct 2014 08:11:35 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Nov 2014 02:10:09 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Feb 2015 04:59:46 GMT",
"version": "v3"
}
] | 2015-02-23 | [
[
"Rao",
"Junjie",
""
]
] | Inspired by the new soft theorem in gravity by Cachazo and Strominger, the soft theorem for color-ordered Yang-Mills amplitudes has also been identified by Casali. In this note, the same content of N=4 SYM using the Grassmannian formulation is studied. Explicitly, in the holomorphic soft limit, we reduce the n-particle... | 12.665749 | 11.635622 | 15.453893 | 10.826224 | 10.926654 | 12.1433 | 10.786815 | 11.117839 | 10.440312 | 13.222572 | 10.710248 | 10.843084 | 12.766737 | 11.606771 | 11.671729 | 11.674356 | 11.435461 | 11.747352 | 11.616654 | 12.271022 | 11.485338 |
1211.5839 | Aaron Warren | Aaron R. Warren | The K-Theoretic Formulation of D-Brane Aharonov-Bohm Phases | 14 pages, 2 figures | null | null | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The topological calculation of Aharonov-Bohm phases associated with D-branes
in the absence of a Neveu-Schwarz B-field is explored. The K-theoretic
classification of Ramond-Ramond fields in Type II and Type I theories is used
to produce formulae for the Aharonov-Bohm phase associated with a torsion flux.
A topologica... | [
{
"created": "Mon, 26 Nov 2012 01:49:41 GMT",
"version": "v1"
}
] | 2012-11-27 | [
[
"Warren",
"Aaron R.",
""
]
] | The topological calculation of Aharonov-Bohm phases associated with D-branes in the absence of a Neveu-Schwarz B-field is explored. The K-theoretic classification of Ramond-Ramond fields in Type II and Type I theories is used to produce formulae for the Aharonov-Bohm phase associated with a torsion flux. A topological ... | 10.262194 | 10.297858 | 11.210439 | 10.125631 | 9.89489 | 10.132204 | 10.951671 | 9.735195 | 10.441628 | 12.731342 | 9.988765 | 9.759561 | 10.059111 | 9.911366 | 9.994359 | 9.785085 | 9.7597 | 9.895476 | 10.121825 | 10.15772 | 9.764532 |
hep-th/0202111 | Jose M. Figueroa-O'Farrill | Matthias Blau, Jos\'e Figueroa-O'Farrill and George Papadopoulos | Penrose limits, supergravity and brane dynamics | 67 pages | Class.Quant.Grav.19:4753,2002 | 10.1088/0264-9381/19/18/310 | EMPG-02-04 | hep-th gr-qc math.DG | null | We investigate the Penrose limits of classical string and M-theory
backgrounds. We prove that the number of (super)symmetries of a supergravity
background never decreases in the limit. We classify all the possible Penrose
limits of AdS x S spacetimes and of supergravity brane solutions. We also
present the Penrose li... | [
{
"created": "Mon, 18 Feb 2002 15:34:11 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Feb 2002 22:48:26 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Blau",
"Matthias",
""
],
[
"Figueroa-O'Farrill",
"José",
""
],
[
"Papadopoulos",
"George",
""
]
] | We investigate the Penrose limits of classical string and M-theory backgrounds. We prove that the number of (super)symmetries of a supergravity background never decreases in the limit. We classify all the possible Penrose limits of AdS x S spacetimes and of supergravity brane solutions. We also present the Penrose limi... | 8.66049 | 9.234332 | 9.511356 | 9.117206 | 8.262621 | 8.376821 | 8.389114 | 8.586061 | 8.837132 | 10.717226 | 8.627174 | 8.57556 | 9.167582 | 8.526291 | 8.676737 | 8.781654 | 8.527346 | 8.495872 | 8.569568 | 8.598209 | 8.740201 |
2010.14297 | Andrei Zotov | K. Atalikov, A. Zotov | Field theory generalizations of two-body Calogero-Moser models in the
form of Landau-Lifshitz equations | 18 pages, minor changes | J. Geom. Phys., 164 (2021) 104161 | 10.1016/j.geomphys.2021.104161 | null | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give detailed description for continuous version of the classical
IRF-Vertex relation, where on the IRF side we deal with the
Calogero-Moser-Sutherland models. Our study is based on constructing
modifications of the Higgs bundles of infinite rank over elliptic curve and its
degenerations. In this way the previousl... | [
{
"created": "Tue, 27 Oct 2020 13:56:42 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Dec 2020 16:56:29 GMT",
"version": "v2"
}
] | 2021-03-02 | [
[
"Atalikov",
"K.",
""
],
[
"Zotov",
"A.",
""
]
] | We give detailed description for continuous version of the classical IRF-Vertex relation, where on the IRF side we deal with the Calogero-Moser-Sutherland models. Our study is based on constructing modifications of the Higgs bundles of infinite rank over elliptic curve and its degenerations. In this way the previously ... | 12.758018 | 14.423365 | 16.958292 | 12.802823 | 14.808491 | 14.001627 | 13.241438 | 13.571929 | 13.881894 | 17.474041 | 12.009399 | 12.893374 | 14.296016 | 12.795359 | 13.383681 | 13.08237 | 13.229759 | 12.902055 | 11.974561 | 14.558933 | 12.225123 |
2205.10935 | Daniel Kapec | Daniel Kapec, Y.T. Albert Law, Sruthi A. Narayanan | Soft Scalars and the Geometry of the Space of Celestial CFTs | 21 pages | null | 10.1103/PhysRevD.107.046024 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Known examples of the holographic dictionary in asymptotically Anti-de Sitter
spacetimes equate moduli spaces of bulk vacua with conformal manifolds in the
dual quantum field theory. We demonstrate that the same identification holds
for gravity in asymptotically flat spacetimes in any dimension, in accord with
expect... | [
{
"created": "Sun, 22 May 2022 21:37:33 GMT",
"version": "v1"
}
] | 2023-03-15 | [
[
"Kapec",
"Daniel",
""
],
[
"Law",
"Y. T. Albert",
""
],
[
"Narayanan",
"Sruthi A.",
""
]
] | Known examples of the holographic dictionary in asymptotically Anti-de Sitter spacetimes equate moduli spaces of bulk vacua with conformal manifolds in the dual quantum field theory. We demonstrate that the same identification holds for gravity in asymptotically flat spacetimes in any dimension, in accord with expectat... | 12.980722 | 11.568823 | 14.519953 | 11.636632 | 13.891115 | 12.254205 | 11.843284 | 11.805962 | 11.758401 | 16.454561 | 12.435139 | 11.984529 | 12.128775 | 11.763851 | 11.935695 | 12.09455 | 12.226545 | 12.181878 | 12.019342 | 12.82198 | 11.588618 |
1007.0236 | Olaf Lechtenfeld | Olaf Lechtenfeld, Christoph N\"olle, Alexander D. Popov | Heterotic compactifications on nearly K\"ahler manifolds | 1+16 pages | JHEP 1009:074,2010 | 10.1007/JHEP09(2010)074 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider compactifications of heterotic supergravity on anti-de Sitter
space, with a six-dimensional nearly K"ahler manifold as the internal space.
Completing the model proposed by Frey and Lippert with the particular choice of
SU(3)/U(1)xU(1) for the internal manifold, we show that it satisfies not only
the super... | [
{
"created": "Thu, 1 Jul 2010 19:32:05 GMT",
"version": "v1"
}
] | 2014-11-21 | [
[
"Lechtenfeld",
"Olaf",
""
],
[
"Nölle",
"Christoph",
""
],
[
"Popov",
"Alexander D.",
""
]
] | We consider compactifications of heterotic supergravity on anti-de Sitter space, with a six-dimensional nearly K"ahler manifold as the internal space. Completing the model proposed by Frey and Lippert with the particular choice of SU(3)/U(1)xU(1) for the internal manifold, we show that it satisfies not only the supersy... | 9.562265 | 8.360253 | 9.762918 | 7.978923 | 8.69727 | 8.594245 | 8.678527 | 8.41613 | 8.613678 | 10.908711 | 8.883846 | 8.231716 | 9.069565 | 8.589558 | 8.541495 | 8.664896 | 8.201945 | 8.979928 | 8.242988 | 9.010605 | 8.22668 |
1508.01502 | Cristopher David Gonz\'alez D\'iaz | Cristopher Gonz\'alez and Benjamin Koch | Improved Reissner-Nordstr\"om-(A)dS Black Hole in Asymptotic Safety | V1:23 pages, 9 figures. V2:28 pages, 12 figures. Incorporation of
references in introduction section and consideration of another analysis in
section 5, without changes in the conclusions. V3:28 pages, 12 figures. Some
redaction corrections. Accepted in International Journal of Modern Physics A | null | 10.1142/S0217751X16501414 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper studies the quantum modifications of the
Reissner-Nordstr\"{o}m-(A)dS black hole within Quantum Einstein Gravity,
coupled to an electromagnetic sector. Quantum effects are introduced on the
level of the improvements of the classical solution, where the originally
constant couplings ($G_0$, $\Lambda_0$, and... | [
{
"created": "Thu, 6 Aug 2015 19:27:02 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Mar 2016 16:07:28 GMT",
"version": "v2"
},
{
"created": "Thu, 1 Sep 2016 22:08:36 GMT",
"version": "v3"
}
] | 2016-09-05 | [
[
"González",
"Cristopher",
""
],
[
"Koch",
"Benjamin",
""
]
] | This paper studies the quantum modifications of the Reissner-Nordstr\"{o}m-(A)dS black hole within Quantum Einstein Gravity, coupled to an electromagnetic sector. Quantum effects are introduced on the level of the improvements of the classical solution, where the originally constant couplings ($G_0$, $\Lambda_0$, and $... | 11.481476 | 11.621477 | 11.705603 | 11.187368 | 12.222202 | 10.821299 | 11.985464 | 11.310833 | 11.391298 | 12.400173 | 11.407457 | 11.318886 | 10.827884 | 10.670863 | 10.707147 | 11.322838 | 11.360635 | 10.943974 | 10.836866 | 10.874307 | 11.544646 |
1412.3337 | Augusto Sagnotti Prof. | S. Ferrara, M. Porrati, A. Sagnotti, R. Stora, A. Yeranyan | Generalized Born--Infeld Actions and Projective Cubic Curves | 17 pages, LaTeX, 1 eps figure. Comments added and misprints
corrected. Final version to appear in Fortschritte der Physik - Progress of
Physics | null | 10.1002/prop.201400087 | CERN-PH-TH/2014-250 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate $U(1)^{\,n}$ supersymmetric Born-Infeld Lagrangians with a
second non-linearly realized supersymmetry. The resulting non-linear structure
is more complex than the square root present in the standard Born-Infeld
action, and nonetheless the quadratic constraints determining these models can
be solved exa... | [
{
"created": "Wed, 10 Dec 2014 15:23:00 GMT",
"version": "v1"
},
{
"created": "Wed, 31 Dec 2014 07:28:55 GMT",
"version": "v2"
}
] | 2016-01-20 | [
[
"Ferrara",
"S.",
""
],
[
"Porrati",
"M.",
""
],
[
"Sagnotti",
"A.",
""
],
[
"Stora",
"R.",
""
],
[
"Yeranyan",
"A.",
""
]
] | We investigate $U(1)^{\,n}$ supersymmetric Born-Infeld Lagrangians with a second non-linearly realized supersymmetry. The resulting non-linear structure is more complex than the square root present in the standard Born-Infeld action, and nonetheless the quadratic constraints determining these models can be solved exact... | 15.602647 | 13.809571 | 19.142756 | 14.395722 | 14.37274 | 15.65696 | 15.318926 | 14.937286 | 13.683766 | 19.333235 | 12.860372 | 14.21311 | 17.447222 | 15.316077 | 15.251586 | 14.696421 | 14.459935 | 14.394817 | 15.263208 | 17.853167 | 13.787204 |
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