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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1204.4482 | Max Atkin | Max R. Atkin, Stefan Zohren | FZZT Brane Relations in the Presence of Boundary Magnetic Fields | 23 pages, 5 figures (3 new). Two new sections added giving examples
of the construction. Explanations clarified. Minor changes to the conclusion
but main results unchanged. Matches published version | JHEP 1211 (2012) 163 | 10.1007/JHEP11(2012)163 | null | hep-th cond-mat.stat-mech math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how a boundary state different from the (1,1) Cardy state may be
realised in the (m,m+1) minimal string by the introduction of an auxiliary
matrix into the standard two hermitian matrix model. This boundary is a natural
generalisation of the free spin boundary state in the Ising model. The
resolvent for the a... | [
{
"created": "Thu, 19 Apr 2012 21:49:54 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Oct 2012 09:49:18 GMT",
"version": "v2"
}
] | 2012-12-18 | [
[
"Atkin",
"Max R.",
""
],
[
"Zohren",
"Stefan",
""
]
] | We show how a boundary state different from the (1,1) Cardy state may be realised in the (m,m+1) minimal string by the introduction of an auxiliary matrix into the standard two hermitian matrix model. This boundary is a natural generalisation of the free spin boundary state in the Ising model. The resolvent for the aux... | 9.425816 | 9.608599 | 10.750955 | 9.237244 | 9.887367 | 10.015111 | 9.782141 | 9.169666 | 9.527077 | 11.751756 | 9.362351 | 9.265812 | 9.837438 | 9.09071 | 9.094718 | 9.439519 | 9.105773 | 9.113976 | 9.113839 | 9.670785 | 9.092741 |
1104.4804 | Elena M. Murchikova | E. M. Murchikova | Splitting of folded strings in AdS_3 | 18 pages, 2 figures; v2: typos corrected | Phys.Rev.D84:026002,2011 | 10.1103/PhysRevD.84.026002 | Imperial-TP-EM-2011-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we present semiclassical computations of the splitting of
folded spinning strings in AdS_3, which may be of interest in the context of
AdS/CFT duality. We start with a classical closed string and assume that it can
split on two closed string fragments, if at a given time two points on it
coincide in tar... | [
{
"created": "Mon, 25 Apr 2011 20:34:48 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Jun 2011 09:53:10 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Murchikova",
"E. M.",
""
]
] | In this paper we present semiclassical computations of the splitting of folded spinning strings in AdS_3, which may be of interest in the context of AdS/CFT duality. We start with a classical closed string and assume that it can split on two closed string fragments, if at a given time two points on it coincide in targe... | 10.170074 | 10.850729 | 10.762416 | 10.049283 | 10.109826 | 9.650288 | 10.582444 | 9.921886 | 9.955931 | 11.535628 | 9.558228 | 9.573927 | 9.606586 | 9.719788 | 9.743254 | 9.57421 | 9.603095 | 9.518825 | 9.40637 | 9.860038 | 9.694198 |
1908.08514 | Ibrahim Akal | Ibrahim Akal | Reflections on Virasoro circuit complexity and Berry phase | 32 pages | null | null | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, the notion of circuit complexity defined in symmetry group
manifolds has been related to geometric actions which generally arise in the
coadjoint orbit method in representation theory and play an important role in
geometric quantization. On the other hand, it is known that there exists a
precise relation be... | [
{
"created": "Thu, 22 Aug 2019 17:46:13 GMT",
"version": "v1"
}
] | 2019-08-23 | [
[
"Akal",
"Ibrahim",
""
]
] | Recently, the notion of circuit complexity defined in symmetry group manifolds has been related to geometric actions which generally arise in the coadjoint orbit method in representation theory and play an important role in geometric quantization. On the other hand, it is known that there exists a precise relation betw... | 9.397686 | 9.705975 | 10.298398 | 9.591757 | 9.988906 | 9.689375 | 10.295098 | 9.021955 | 9.38672 | 11.165668 | 9.482097 | 9.165115 | 9.457159 | 8.98898 | 9.12322 | 9.397507 | 9.20785 | 8.800894 | 8.951009 | 9.411798 | 9.024755 |
1108.6331 | David Turton | Stefano Giusto, Rodolfo Russo, David Turton | New D1-D5-P geometries from string amplitudes | 48 pages, 2 figures, v2: typos corrected | JHEP11(2011)062 | 10.1007/JHEP11(2011)062 | DFPD-11-TH-14, QMUL-PH-11-12 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the long range supergravity fields sourced by a D1-D5-P bound state
from disk amplitudes for massless closed string emission. We suggest that since
the parameter controlling the string perturbation expansion for this
calculation decreases with distance from the bound state, the resulting
asymptotic fields a... | [
{
"created": "Wed, 31 Aug 2011 19:59:41 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Nov 2011 16:18:58 GMT",
"version": "v2"
}
] | 2011-11-28 | [
[
"Giusto",
"Stefano",
""
],
[
"Russo",
"Rodolfo",
""
],
[
"Turton",
"David",
""
]
] | We derive the long range supergravity fields sourced by a D1-D5-P bound state from disk amplitudes for massless closed string emission. We suggest that since the parameter controlling the string perturbation expansion for this calculation decreases with distance from the bound state, the resulting asymptotic fields are... | 9.350424 | 7.975633 | 10.8164 | 8.102337 | 9.043111 | 8.498592 | 8.25737 | 8.647986 | 8.493291 | 10.906135 | 8.409851 | 8.681546 | 9.41973 | 8.546123 | 8.787882 | 8.576124 | 8.780738 | 8.404359 | 8.422401 | 9.402887 | 8.814672 |
2011.08231 | Raquel Santos | Enrique Alvarez, Jesus Anero and Raquel Santos-Garcia | Weighing the Vacuum Energy | 32 pages. Minor corrections | Phys. Rev. D 103, 084032 (2021) | 10.1103/PhysRevD.103.084032 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the weight of vacuum energy in various contexts. First, we compute
the vacuum energy for flat spacetimes of the form $\mathbb{T}^3 \times
\mathbb{R}$, where $\mathbb{T}^3$ stands for a general 3-torus. We discover a
quite simple relationship between energy at radius $R$ and energy at radius
$\frac{l_s^2}{ ... | [
{
"created": "Mon, 16 Nov 2020 19:20:28 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Nov 2020 16:39:37 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Jan 2021 15:22:58 GMT",
"version": "v3"
}
] | 2021-04-28 | [
[
"Alvarez",
"Enrique",
""
],
[
"Anero",
"Jesus",
""
],
[
"Santos-Garcia",
"Raquel",
""
]
] | We discuss the weight of vacuum energy in various contexts. First, we compute the vacuum energy for flat spacetimes of the form $\mathbb{T}^3 \times \mathbb{R}$, where $\mathbb{T}^3$ stands for a general 3-torus. We discover a quite simple relationship between energy at radius $R$ and energy at radius $\frac{l_s^2}{ R}... | 8.492085 | 8.839368 | 8.742358 | 8.358617 | 8.342932 | 9.258097 | 9.488433 | 8.39675 | 8.452084 | 9.258334 | 8.395872 | 8.288495 | 8.42804 | 8.249153 | 7.995206 | 8.328424 | 8.500733 | 8.464672 | 8.284789 | 8.422017 | 8.151814 |
hep-th/9601030 | Hagen Kleinert | H. Kleinert
(http://www.physik.fu-berlin.de/~kleinert/institution.html) and A.M.
Chervyakov | Evidence for Negative Stiffness of QCD Strings | LaTeX and figure files tarred and gzipped. New Version contains a
number of improvements | null | null | null | hep-th | null | QCD strings are color-electric flux tubes between quarks with a finite
thickness and thus a finite curvature stiffness. Contrary to an earlier
rigid-string by Polyakov and Kleinert, and motivated by the properties of a
magnetic flux tubes in type-II superconductors we put forward the hypothesis
that QCD strings have ... | [
{
"created": "Tue, 9 Jan 1996 10:02:40 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Apr 1996 07:10:17 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Apr 1996 05:34:54 GMT",
"version": "v3"
}
] | 2008-02-03 | [
[
"Kleinert",
"H.",
"",
"http://www.physik.fu-berlin.de/~kleinert/institution.html"
],
[
"Chervyakov",
"A. M.",
""
]
] | QCD strings are color-electric flux tubes between quarks with a finite thickness and thus a finite curvature stiffness. Contrary to an earlier rigid-string by Polyakov and Kleinert, and motivated by the properties of a magnetic flux tubes in type-II superconductors we put forward the hypothesis that QCD strings have a ... | 16.324047 | 17.229662 | 17.667664 | 14.529937 | 19.465334 | 16.739595 | 16.689823 | 15.613416 | 15.606489 | 18.681913 | 16.014969 | 14.830287 | 15.427623 | 15.08916 | 15.34972 | 14.638057 | 15.355717 | 14.847396 | 15.383405 | 14.950868 | 15.065417 |
hep-th/0401131 | Luca Lusanna | Luca Lusanna (INFN, Firenze) | On the Anticipatory Aspects of the Four Interactions: what the Known
Classical and Semi-Classical Solutions Teach us | 12 pages, Talk and "best contribution" at The Sixth International
Conference on Computing Anticipatory Systems CASYS'03, Liege August 11-16,
2003 | null | 10.1063/1.1787316 | null | hep-th | null | The four (electro-magnetic, weak, strong and gravitational) interactions are
described by singular Lagrangians and by Dirac-Bergmann theory of Hamiltonian
constraints. As a consequence a subset of the original configuration variables
are {\it gauge variables}, not determined by the equations of motion. Only at
the Ha... | [
{
"created": "Tue, 20 Jan 2004 13:25:40 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Lusanna",
"Luca",
"",
"INFN, Firenze"
]
] | The four (electro-magnetic, weak, strong and gravitational) interactions are described by singular Lagrangians and by Dirac-Bergmann theory of Hamiltonian constraints. As a consequence a subset of the original configuration variables are {\it gauge variables}, not determined by the equations of motion. Only at the Hami... | 10.118528 | 11.18891 | 10.390529 | 9.740251 | 10.51048 | 10.647052 | 10.679479 | 10.060886 | 10.261287 | 10.98464 | 9.906612 | 9.773378 | 10.094339 | 9.724346 | 9.548853 | 9.872632 | 9.863502 | 10.094717 | 9.47003 | 9.733887 | 9.962418 |
hep-th/0008197 | Uzawa | K.Uzawa, J.Soda | Self-Tuning Dark Energy in Brane World Cosmology | 11pages, LaTex | Mod.Phys.Lett. A16 (2001) 1089-1100 | 10.1142/S0217732301004273 | null | hep-th astro-ph gr-qc hep-ph | null | Recently, the self-tuning mechanism of cancellation of vacuum energy has been
proposed in which our universe is a flat 3-brane in a 5-dimensional spacetime.
In this letter, the self-tuning mechanism of dark energy is proposed by
considering the cosmological matter in the brane world. In our model, the bulk
scalar fie... | [
{
"created": "Fri, 25 Aug 2000 10:36:43 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Uzawa",
"K.",
""
],
[
"Soda",
"J.",
""
]
] | Recently, the self-tuning mechanism of cancellation of vacuum energy has been proposed in which our universe is a flat 3-brane in a 5-dimensional spacetime. In this letter, the self-tuning mechanism of dark energy is proposed by considering the cosmological matter in the brane world. In our model, the bulk scalar field... | 9.08862 | 7.584894 | 7.644323 | 7.417684 | 7.180163 | 7.236818 | 7.202574 | 7.770533 | 7.47848 | 8.088773 | 7.015053 | 7.636978 | 7.738633 | 7.303061 | 7.51574 | 7.331191 | 7.515656 | 7.418733 | 7.52856 | 7.553025 | 7.563194 |
2306.07318 | Diego Delmastro | Marieke van Beest, Philip Boyle Smith, Diego Delmastro, Zohar
Komargodski, David Tong | Monopoles, Scattering, and Generalized Symmetries | 60 pages | null | null | null | hep-th cond-mat.str-el | http://creativecommons.org/licenses/by/4.0/ | We reconsider the problem of electrically charged, massless fermions
scattering off magnetic monopoles. The interpretation of the outgoing states
has long been a puzzle as, in certain circumstances, they necessarily carry
fractional quantum numbers. We argue that consistency requires such outgoing
particles to be att... | [
{
"created": "Mon, 12 Jun 2023 18:00:01 GMT",
"version": "v1"
}
] | 2023-06-14 | [
[
"van Beest",
"Marieke",
""
],
[
"Smith",
"Philip Boyle",
""
],
[
"Delmastro",
"Diego",
""
],
[
"Komargodski",
"Zohar",
""
],
[
"Tong",
"David",
""
]
] | We reconsider the problem of electrically charged, massless fermions scattering off magnetic monopoles. The interpretation of the outgoing states has long been a puzzle as, in certain circumstances, they necessarily carry fractional quantum numbers. We argue that consistency requires such outgoing particles to be attac... | 13.481292 | 13.46364 | 14.350654 | 12.880986 | 13.518991 | 14.148041 | 13.238913 | 12.79445 | 12.690145 | 16.72303 | 12.742716 | 12.961797 | 13.118617 | 12.628362 | 13.266288 | 12.902899 | 13.14369 | 12.72178 | 13.199066 | 13.778055 | 12.980991 |
0704.3920 | Seong Chan Park | Seong Chan Park (Seoul National University) | Orbifold GUT inflation | 12 pages, 6 figures, JCAP accepted version | JCAP0711:001,2007 | 10.1088/1475-7516/2007/11/001 | null | hep-th astro-ph gr-qc hep-ph | null | We consider a scenario of cosmological inflation coming from a grand unified
theory in higher dimensional orbifold. Flatness of the potential is
automatically guaranteed in this orbifold setup thanks to the nonlocality of
the Wilson line on higher dimensions and the local quantum gravitational
corrections are exponen... | [
{
"created": "Mon, 30 Apr 2007 12:17:25 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Oct 2007 16:53:47 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Park",
"Seong Chan",
"",
"Seoul National University"
]
] | We consider a scenario of cosmological inflation coming from a grand unified theory in higher dimensional orbifold. Flatness of the potential is automatically guaranteed in this orbifold setup thanks to the nonlocality of the Wilson line on higher dimensions and the local quantum gravitational corrections are exponenti... | 12.933217 | 13.188855 | 12.891871 | 12.347613 | 14.587821 | 13.840097 | 14.193182 | 13.337527 | 11.932024 | 15.392734 | 13.153236 | 12.376527 | 12.60765 | 12.050245 | 12.032156 | 12.239098 | 12.293005 | 12.818981 | 12.344543 | 12.564015 | 12.448528 |
hep-th/9809141 | Taro Kashiwa | Taro Kashiwa (Kyushu University) | The Auxiliary Field Method as a Powerful Tool for Nonperturbative Study | 18 pages, 5 figures | Phys.Rev. D59 (1999) 085002 | 10.1103/PhysRevD.59.085002 | KYUSHU-HET-42 | hep-th | null | The auxiliary field method, defined through introducing an auxiliary (also
called as the Hubbard-Stratonovich or the Mean-) field and utilizing a
loop-expansion, gives an excellent result for a wide range of a coupling
constant. The analysis is made for Anharmonic-Oscillator and Double-Well
examples in 0-(a simple in... | [
{
"created": "Sat, 19 Sep 1998 09:19:33 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Kashiwa",
"Taro",
"",
"Kyushu University"
]
] | The auxiliary field method, defined through introducing an auxiliary (also called as the Hubbard-Stratonovich or the Mean-) field and utilizing a loop-expansion, gives an excellent result for a wide range of a coupling constant. The analysis is made for Anharmonic-Oscillator and Double-Well examples in 0-(a simple inte... | 13.2859 | 13.949404 | 15.882749 | 13.168865 | 12.692104 | 14.042085 | 15.178304 | 14.050306 | 13.219496 | 14.938063 | 12.969833 | 13.036895 | 13.289558 | 13.222162 | 13.341875 | 12.549277 | 12.860626 | 12.998694 | 13.316124 | 13.621462 | 13.349983 |
hep-th/9809075 | George Siopsis | George Siopsis | Newtonian versus black-hole scattering | 11 pages, ReVTeX | Phys. Rev. D 59, 044015 (1999) | 10.1103/PhysRevD.59.044015 | null | hep-th | null | We discuss non-relativistic scattering by a Newtonian potential. We show that
the gray-body factors associated with scattering by a black hole exhibit the
same functional dependence as scattering amplitudes in the Newtonian limit,
which should be the weak-field limit of any quantum theory of gravity. This
behavior ar... | [
{
"created": "Thu, 10 Sep 1998 21:58:23 GMT",
"version": "v1"
}
] | 2016-08-25 | [
[
"Siopsis",
"George",
""
]
] | We discuss non-relativistic scattering by a Newtonian potential. We show that the gray-body factors associated with scattering by a black hole exhibit the same functional dependence as scattering amplitudes in the Newtonian limit, which should be the weak-field limit of any quantum theory of gravity. This behavior aris... | 9.028227 | 6.137825 | 8.158752 | 6.587119 | 6.681269 | 6.752693 | 6.557852 | 7.030021 | 6.968974 | 8.633678 | 6.853196 | 7.469546 | 7.889964 | 7.540182 | 7.407118 | 7.644556 | 7.658095 | 7.484358 | 7.47142 | 7.991646 | 7.295956 |
1904.00922 | Alesandro Santos | S. C. Ulhoa, A. F. Santos, T. F. Furtado and F. C. Khanna | On Gravitational Casimir Effect and Stefan-Boltzmann Law at Finite
Temperature | 12 pages, accepted for publication in Advances in High Energy Physics | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gravitons are described by the propagator in Teleparallel gravity in nearly
flat space-time. Finite temperature is introduced by using Thermo Field
Dynamics formalism. The Gravitational Casimir effect and Stefan-Boltzmann law
are calculated as a function of temperature. Then an equation of state for
gravitons is dete... | [
{
"created": "Mon, 1 Apr 2019 15:51:03 GMT",
"version": "v1"
}
] | 2019-04-02 | [
[
"Ulhoa",
"S. C.",
""
],
[
"Santos",
"A. F.",
""
],
[
"Furtado",
"T. F.",
""
],
[
"Khanna",
"F. C.",
""
]
] | Gravitons are described by the propagator in Teleparallel gravity in nearly flat space-time. Finite temperature is introduced by using Thermo Field Dynamics formalism. The Gravitational Casimir effect and Stefan-Boltzmann law are calculated as a function of temperature. Then an equation of state for gravitons is determ... | 11.167031 | 8.26405 | 9.670621 | 8.755103 | 9.300975 | 9.122431 | 8.60657 | 8.326633 | 9.187053 | 8.935244 | 9.133872 | 8.916681 | 9.933549 | 9.857144 | 9.796523 | 9.410291 | 9.768095 | 9.66041 | 9.872602 | 9.665764 | 9.114917 |
1004.4567 | Delia Schwartz-Perlov | Delia Schwartz-Perlov and Alexander Vilenkin | Measures for a Transdimensional Multiverse | 30 pages, 1 figure Minor revisions, reference added | JCAP 1006:024,2010 | 10.1088/1475-7516/2010/06/024 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The multiverse/landscape paradigm that has emerged from eternal inflation and
string theory, describes a large-scale multiverse populated by "pocket
universes" which come in a huge variety of different types, including different
dimensionalities. In order to make predictions in the multiverse, we need a
probability m... | [
{
"created": "Mon, 26 Apr 2010 16:29:30 GMT",
"version": "v1"
},
{
"created": "Tue, 25 May 2010 14:44:44 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Schwartz-Perlov",
"Delia",
""
],
[
"Vilenkin",
"Alexander",
""
]
] | The multiverse/landscape paradigm that has emerged from eternal inflation and string theory, describes a large-scale multiverse populated by "pocket universes" which come in a huge variety of different types, including different dimensionalities. In order to make predictions in the multiverse, we need a probability mea... | 9.254189 | 8.890417 | 10.379573 | 8.852499 | 9.677942 | 9.061382 | 9.18257 | 8.990154 | 8.552427 | 9.497481 | 8.358077 | 8.556169 | 8.81066 | 8.454972 | 8.825011 | 8.736526 | 8.82364 | 8.384439 | 8.606529 | 9.067135 | 8.414629 |
1510.09020 | Javier Molina Dr | Javier Molina-Vilaplana | Entanglement Renormalization and Two Dimensional String Theory | 20 pages. v3 minor corrections. Accepted for publication in Physics
Letters B | Phys.Lett. B755 (2016) 421-425 | 10.1016/j.physletb.2016.02.050 | null | hep-th cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The entanglement renormalization flow of a (1+1) free boson is formulated as
a path integral over some auxiliary scalar fields. The resulting effective
theory for these fields amounts to the dilaton term of non-critical string
theory in two spacetime dimensions. A connection between the scalar fields in
the two theor... | [
{
"created": "Fri, 30 Oct 2015 09:24:28 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Dec 2015 11:14:44 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Feb 2016 09:22:46 GMT",
"version": "v3"
}
] | 2016-03-29 | [
[
"Molina-Vilaplana",
"Javier",
""
]
] | The entanglement renormalization flow of a (1+1) free boson is formulated as a path integral over some auxiliary scalar fields. The resulting effective theory for these fields amounts to the dilaton term of non-critical string theory in two spacetime dimensions. A connection between the scalar fields in the two theorie... | 11.019671 | 10.857691 | 12.874328 | 10.550463 | 10.424789 | 11.608995 | 11.34732 | 11.240872 | 10.493782 | 12.000555 | 10.782925 | 10.498684 | 10.802252 | 10.259173 | 10.313402 | 10.288986 | 10.27333 | 9.61543 | 10.932175 | 11.021089 | 10.415334 |
1911.06305 | Raphael Bousso | Raphael Bousso, Marija Tomasevic | Unitarity From a Smooth Horizon? | 28 pages, 5 figures; v2: minor updates | Phys. Rev. D 102, 106019 (2020) | 10.1103/PhysRevD.102.106019 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Under semiclassical evolution, black holes retain a smooth horizon but fail
to return information. Yet, the Ryu-Takayanagi prescription computes the
boundary entropy expected from unitary CFT evolution. We demonstrate this in a
novel setting with an asymptotic bulk detector, eliminating an assumption about
the entang... | [
{
"created": "Thu, 14 Nov 2019 18:47:51 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Mar 2020 16:14:50 GMT",
"version": "v2"
}
] | 2020-11-25 | [
[
"Bousso",
"Raphael",
""
],
[
"Tomasevic",
"Marija",
""
]
] | Under semiclassical evolution, black holes retain a smooth horizon but fail to return information. Yet, the Ryu-Takayanagi prescription computes the boundary entropy expected from unitary CFT evolution. We demonstrate this in a novel setting with an asymptotic bulk detector, eliminating an assumption about the entangle... | 11.766385 | 12.491156 | 13.737013 | 12.064273 | 12.994121 | 13.282647 | 13.63401 | 12.640522 | 12.360718 | 14.087355 | 12.13552 | 11.869534 | 11.996624 | 11.675876 | 11.830009 | 11.580973 | 11.818259 | 12.104349 | 11.714252 | 12.554027 | 11.575127 |
0911.0012 | I\~naki Garc\'ia-Etxebarria | Mirjam Cveti\v{c}, I\~naki Garc\'ia-Etxebarria and Robert Richter | Branes and instantons at angles and the F-theory lift of O(1) instantons | 15 pages, 1 figure. Based in part on talks given at various
conferences | AIP Conf.Proc.1200:246-260,2010 | 10.1063/1.3327564 | ROM2F/2009/21, UPR-1214-T | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the physics of D-branes and D-brane instantons intersecting at
angles, focusing on the (non)generation of a superpotential in the worldvolume
theory of the branes. This is a short review of the results in arXiv:0905.1694,
where we further emphasize both the macroscopic and microscopic structure of
the mani... | [
{
"created": "Mon, 2 Nov 2009 04:22:15 GMT",
"version": "v1"
}
] | 2015-05-14 | [
[
"Cvetič",
"Mirjam",
""
],
[
"García-Etxebarria",
"Iñaki",
""
],
[
"Richter",
"Robert",
""
]
] | We discuss the physics of D-branes and D-brane instantons intersecting at angles, focusing on the (non)generation of a superpotential in the worldvolume theory of the branes. This is a short review of the results in arXiv:0905.1694, where we further emphasize both the macroscopic and microscopic structure of the manife... | 10.192726 | 9.340406 | 10.166788 | 9.158437 | 10.048106 | 10.054314 | 9.982686 | 9.390034 | 9.582226 | 10.544158 | 8.881381 | 9.216554 | 10.784253 | 9.725065 | 9.423998 | 9.858795 | 9.33179 | 9.616491 | 9.649694 | 10.663511 | 9.102771 |
1104.0706 | Evgeny Ivanov | M. Goykhman, E. Ivanov | Worldsheet Supersymmetry of Pohlmeyer-Reduced AdS_n x S^n Superstrings | 1+18 pages, minor corrections, published version | JHEP 1109:078,2011 | 10.1007/JHEP09(2011)078 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As was observed by Grigoriev and Tseytlin, the Pohlmeyer-reduced AdS_2 x S^2
superstring theory possesses N=(2,2) worldsheet supersymmetry. We show, at the
classical level, that the AdS_3 x S^3 and AdS_5 x S^5 superstring theories in
the Pohlmeyer-reduced form reveal hidden N=(4,4) and N=(8,8) worldsheet
supersymmetr... | [
{
"created": "Mon, 4 Apr 2011 22:59:39 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Apr 2011 20:09:15 GMT",
"version": "v2"
},
{
"created": "Wed, 16 Nov 2011 20:28:34 GMT",
"version": "v3"
}
] | 2011-11-17 | [
[
"Goykhman",
"M.",
""
],
[
"Ivanov",
"E.",
""
]
] | As was observed by Grigoriev and Tseytlin, the Pohlmeyer-reduced AdS_2 x S^2 superstring theory possesses N=(2,2) worldsheet supersymmetry. We show, at the classical level, that the AdS_3 x S^3 and AdS_5 x S^5 superstring theories in the Pohlmeyer-reduced form reveal hidden N=(4,4) and N=(8,8) worldsheet supersymmetrie... | 5.375167 | 4.885279 | 5.682014 | 4.881744 | 4.762872 | 5.030942 | 5.135704 | 4.841953 | 4.494036 | 6.384895 | 4.937409 | 4.887358 | 5.255616 | 4.719294 | 4.722634 | 4.906675 | 4.900667 | 4.76158 | 4.856441 | 5.20921 | 5.05319 |
2107.14227 | Miguel Montero | Arun Debray, Markus Dierigl, Jonathan J. Heckman, Miguel Montero | The anomaly that was not meant IIB | 40 pages + appendices, 4 figures, 331776 bordism classes. v2: Added
references, expanded discussion on quadratic refinement | null | 10.1002/prop.202100168 | LMU-ASC 24/21 | hep-th math.AT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Type IIB supergravity enjoys a discrete non-Abelian duality group, which has
potential quantum anomalies. In this paper we explicitly compute these, and
present the bordism group that controls them, modulo some physically motivated
assumptions. Quite surprisingly, we find that they do not vanish, which naively
would ... | [
{
"created": "Thu, 29 Jul 2021 17:58:14 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Nov 2021 14:02:14 GMT",
"version": "v2"
}
] | 2022-02-09 | [
[
"Debray",
"Arun",
""
],
[
"Dierigl",
"Markus",
""
],
[
"Heckman",
"Jonathan J.",
""
],
[
"Montero",
"Miguel",
""
]
] | Type IIB supergravity enjoys a discrete non-Abelian duality group, which has potential quantum anomalies. In this paper we explicitly compute these, and present the bordism group that controls them, modulo some physically motivated assumptions. Quite surprisingly, we find that they do not vanish, which naively would si... | 11.053042 | 9.560467 | 11.698092 | 9.759195 | 10.088305 | 10.131856 | 10.491635 | 10.689801 | 10.018745 | 12.526546 | 9.928037 | 10.244425 | 10.570306 | 10.171383 | 10.076662 | 10.131148 | 9.977288 | 10.399865 | 10.121045 | 10.617767 | 9.744482 |
1505.02647 | Enrico Brehm | Enrico M. Brehm and Ilka Brunner | Entanglement entropy through conformal interfaces in the 2D Ising model | 27 pages, 3 figures, v2: additional references and minor corrections | null | null | LMU-ASC 23/15 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the entanglement entropy for the 2D Ising model at the conformal
fixed point in the presence of interfaces. More precisely, we investigate the
situation where the two subsystems are separated by a defect line that
preserves conformal invariance. Using the replica trick, we compute the
entanglement entropy... | [
{
"created": "Mon, 11 May 2015 14:47:32 GMT",
"version": "v1"
},
{
"created": "Fri, 22 May 2015 12:23:33 GMT",
"version": "v2"
}
] | 2015-05-25 | [
[
"Brehm",
"Enrico M.",
""
],
[
"Brunner",
"Ilka",
""
]
] | We consider the entanglement entropy for the 2D Ising model at the conformal fixed point in the presence of interfaces. More precisely, we investigate the situation where the two subsystems are separated by a defect line that preserves conformal invariance. Using the replica trick, we compute the entanglement entropy b... | 5.093686 | 4.708346 | 5.30508 | 4.611866 | 4.983107 | 4.910858 | 4.401205 | 4.731304 | 4.671038 | 5.306509 | 4.635591 | 4.79128 | 5.06458 | 4.841105 | 4.810211 | 4.911323 | 4.894405 | 4.843237 | 4.879658 | 4.980916 | 4.724624 |
1105.0591 | Mark Goodsell | P.Anastasopoulos, I.Antoniadis, K.Benakli, M.D.Goodsell and A.Vichi | One-loop adjoint masses for non-supersymmetric intersecting branes | 40 pages | null | 10.1007/JHEP08(2011)120 | CERN-PH-TH/2011-095; DESY 11-069; TUW-11-09 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider breaking of supersymmetry in intersecting D-brane configurations
by slight deviation of the angles from their supersymmetric values. We compute
the masses generated by radiative corrections for the adjoint scalars on the
brane world-volumes. In the open string channel, the string two-point function
receiv... | [
{
"created": "Tue, 3 May 2011 14:20:50 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Anastasopoulos",
"P.",
""
],
[
"Antoniadis",
"I.",
""
],
[
"Benakli",
"K.",
""
],
[
"Goodsell",
"M. D.",
""
],
[
"Vichi",
"A.",
""
]
] | We consider breaking of supersymmetry in intersecting D-brane configurations by slight deviation of the angles from their supersymmetric values. We compute the masses generated by radiative corrections for the adjoint scalars on the brane world-volumes. In the open string channel, the string two-point function receives... | 9.287066 | 8.405708 | 10.358438 | 8.582291 | 8.428699 | 8.473312 | 8.022847 | 8.88114 | 8.284492 | 10.494285 | 8.331456 | 9.084558 | 9.65787 | 8.927452 | 8.798974 | 8.695522 | 8.858223 | 8.866797 | 8.826708 | 9.598253 | 8.97864 |
hep-th/9608140 | Kechkin O. V. | O.Kechkin and M.Yurova | U(1,1)--Invariant Generation of Charges for
Einstein--Maxwell--Dilaton--Axion Theory | 14 pages, RevTex, no figuries | Gen.Rel.Grav. 29 (1997) 1283-1293 | 10.1023/A:1018815930628 | null | hep-th | null | The action of the isometry subgroup which preserves the trivial values of the
fields is studied for the stationary D=4 Einstein--Maxwell--Dilaton--Axion
theory. The technique for generation of charges and the corresponding procedure
for construction of new solutions is formulated. A solution describing the
double rot... | [
{
"created": "Wed, 21 Aug 1996 17:02:18 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Kechkin",
"O.",
""
],
[
"Yurova",
"M.",
""
]
] | The action of the isometry subgroup which preserves the trivial values of the fields is studied for the stationary D=4 Einstein--Maxwell--Dilaton--Axion theory. The technique for generation of charges and the corresponding procedure for construction of new solutions is formulated. A solution describing the double rotat... | 18.377926 | 17.058977 | 16.220133 | 15.200764 | 16.972721 | 16.560074 | 15.103969 | 14.25882 | 16.447567 | 18.266422 | 15.84451 | 15.919848 | 16.693989 | 15.505081 | 15.983735 | 16.181198 | 15.49063 | 16.180437 | 15.652675 | 17.289585 | 15.02994 |
1803.01379 | Shai Chester | Shai M. Chester | AdS$_4$/CFT$_3$ for Unprotected Operators | 22 pages, 1 figure, v4, fixed typos | Journal of High Energy Physics, 2018, 1-30 | 10.1007/JHEP07(2018)030 | PUPT-2553 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the four-point function of the lowest scalar in the stress-energy
tensor multiplet in $\mathcal{N}=8$ ABJ(M) theory \cite{Aharony:2008ug,
Aharony:2008gk}. At large central charge $c_T\sim N^{3/2}$, this correlator is
given by the corresponding holographic correlation function in 11d supergravity
on $AdS_4... | [
{
"created": "Sun, 4 Mar 2018 16:50:53 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jun 2018 20:36:06 GMT",
"version": "v2"
},
{
"created": "Thu, 2 Aug 2018 23:44:48 GMT",
"version": "v3"
},
{
"created": "Mon, 17 Jun 2019 15:50:11 GMT",
"version": "v4"
}
] | 2019-06-18 | [
[
"Chester",
"Shai M.",
""
]
] | We consider the four-point function of the lowest scalar in the stress-energy tensor multiplet in $\mathcal{N}=8$ ABJ(M) theory \cite{Aharony:2008ug, Aharony:2008gk}. At large central charge $c_T\sim N^{3/2}$, this correlator is given by the corresponding holographic correlation function in 11d supergravity on $AdS_4\t... | 5.083865 | 5.109689 | 6.740543 | 4.806859 | 5.430315 | 5.549294 | 5.870341 | 4.720838 | 5.19803 | 7.4477 | 4.924234 | 4.796683 | 5.662628 | 4.848404 | 4.875391 | 4.821085 | 4.965435 | 4.963969 | 4.861779 | 5.481987 | 4.905198 |
0806.4777 | Paul K. Townsend | Igor A. Bandos and Paul K. Townsend | Light-cone M5 and multiple M2-branes | 21 pages, revised to clarify some points, to include a discussion of
SDiff gauge invariance, and to add two references | Class.Quant.Grav.25:245003,2008 | 10.1088/0264-9381/25/24/245003 | IFIC-08-33, FTUV-08-2506, DAMTP-2008-53 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the light-cone gauge fixed Lagrangian for the M5-brane; it has a
residual `exotic' gauge invariance with the group of 5-volume preserving
diffeomorphisms, SDiff(5), as gauge group. For an M5-brane of topology R2 x M3,
for closed 3-manifold M3, we find an infinite tension limit that yields an
SO(8)-invarian... | [
{
"created": "Sun, 29 Jun 2008 18:41:20 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Jul 2008 22:23:07 GMT",
"version": "v2"
}
] | 2008-12-18 | [
[
"Bandos",
"Igor A.",
""
],
[
"Townsend",
"Paul K.",
""
]
] | We present the light-cone gauge fixed Lagrangian for the M5-brane; it has a residual `exotic' gauge invariance with the group of 5-volume preserving diffeomorphisms, SDiff(5), as gauge group. For an M5-brane of topology R2 x M3, for closed 3-manifold M3, we find an infinite tension limit that yields an SO(8)-invariant ... | 7.542453 | 7.671595 | 8.69969 | 6.902166 | 7.428833 | 7.046586 | 7.000479 | 6.87247 | 6.740937 | 9.08692 | 7.158169 | 7.202256 | 7.781281 | 7.11593 | 7.005722 | 7.200788 | 6.99755 | 7.140913 | 7.093183 | 8.047892 | 7.193214 |
hep-th/0408032 | Bin Wang | Bin Wang, Yungui Gong and Ru-Keng Su | Probing the curvature of the Universe from supernova measurement | 8 pages, 3 figures, revised version, accepted for publication in
Physics Letters B | Phys.Lett. B605 (2005) 9-14 | 10.1016/j.physletb.2004.11.027 | null | hep-th astro-ph gr-qc | null | We study the possibility to probe the spatial geometry of the Universe by
supernova measurement of the cubic correction to the luminosity distance. We
illustrate with an accelerating universe model with infinite-volume extra
dimensions, for which the 1$\sigma$ level supernova results indicate that the
Universe is clo... | [
{
"created": "Wed, 4 Aug 2004 08:17:26 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Nov 2004 02:34:55 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Wang",
"Bin",
""
],
[
"Gong",
"Yungui",
""
],
[
"Su",
"Ru-Keng",
""
]
] | We study the possibility to probe the spatial geometry of the Universe by supernova measurement of the cubic correction to the luminosity distance. We illustrate with an accelerating universe model with infinite-volume extra dimensions, for which the 1$\sigma$ level supernova results indicate that the Universe is close... | 19.99579 | 19.120979 | 20.695484 | 18.421917 | 17.724218 | 20.186522 | 18.629082 | 19.045362 | 19.554802 | 19.095644 | 19.60605 | 21.06362 | 17.569563 | 17.147404 | 17.050041 | 18.002645 | 17.594185 | 18.335445 | 17.274158 | 17.175316 | 19.091206 |
1608.02957 | Thomas T. Dumitrescu | Thomas T. Dumitrescu | An introduction to supersymmetric field theories in curved space | This is a contribution to the review volume `Localization techniques
in quantum field theories' (eds. V. Pestun and M. Zabzine) which contains 17
Chapters. The complete volume is summarized in arXiv:1608.02952 and it can be
downloaded at https://arxiv.org/src/1608.02952/anc/LocQFT.pdf or
http://pestun.ihes.fr/p... | null | 10.1088/1751-8121/aa62f5 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this review, we give a pedagogical introduction to a systematic framework
for constructing and analyzing supersymmetric field theories on curved
spacetime manifolds. The framework is based on the use of off-shell
supergravity background fields. We present the general principles, which
broadly apply to theories wit... | [
{
"created": "Tue, 9 Aug 2016 20:01:42 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Aug 2016 14:22:07 GMT",
"version": "v2"
},
{
"created": "Sat, 15 Oct 2016 18:05:10 GMT",
"version": "v3"
}
] | 2017-10-25 | [
[
"Dumitrescu",
"Thomas T.",
""
]
] | In this review, we give a pedagogical introduction to a systematic framework for constructing and analyzing supersymmetric field theories on curved spacetime manifolds. The framework is based on the use of off-shell supergravity background fields. We present the general principles, which broadly apply to theories with ... | 6.290746 | 5.230212 | 6.885642 | 5.957861 | 5.514607 | 5.110347 | 5.191606 | 5.497336 | 5.564203 | 7.046628 | 5.127507 | 5.411639 | 6.005885 | 5.600476 | 5.548538 | 5.58725 | 5.617017 | 5.5026 | 5.652398 | 5.952538 | 5.562416 |
1501.07842 | Mario Trigiante | Laura Andrianopoli, Riccardo D'Auria, Sergio Ferrara and Mario
Trigiante | Observations on the Partial Breaking of $N=2$ Rigid Supersymmetry | 7 pages, LaTeX source | null | 10.1016/j.physletb.2015.03.032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the partial breaking of $N=2$ rigid supersymmetry for a generic
rigid special geometry of $n$ abelian vector multiplets in the presence of
Fayet-Iliopoulos terms induced by the Hyper-K\"ahler momentum map. By
exhibiting the symplectic structure of the problem we give invariant conditions
for the breaking to ... | [
{
"created": "Fri, 30 Jan 2015 17:02:03 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Andrianopoli",
"Laura",
""
],
[
"D'Auria",
"Riccardo",
""
],
[
"Ferrara",
"Sergio",
""
],
[
"Trigiante",
"Mario",
""
]
] | We study the partial breaking of $N=2$ rigid supersymmetry for a generic rigid special geometry of $n$ abelian vector multiplets in the presence of Fayet-Iliopoulos terms induced by the Hyper-K\"ahler momentum map. By exhibiting the symplectic structure of the problem we give invariant conditions for the breaking to oc... | 10.230593 | 9.230619 | 9.803062 | 8.800663 | 8.341997 | 9.076578 | 8.872228 | 9.041408 | 9.053804 | 10.773992 | 8.622801 | 8.757109 | 9.590631 | 9.251807 | 9.114841 | 8.96754 | 8.943361 | 9.040076 | 9.396676 | 9.734126 | 8.893413 |
1212.3532 | Kurt Lechner | Francesco Azzurli, Kurt Lechner | The Lienard-Wiechert field of accelerated massless charges | 9 pages, no figures | null | 10.1016/j.physleta.2013.02.046 | DFPD/2012/TH25 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We determine for the first time the electromagnetic field generated by a
generic massless accelerated charge, solving exactly Maxwell's equations. This
result may shed new light on the possible existence of such particles in
nature.
| [
{
"created": "Fri, 14 Dec 2012 17:16:40 GMT",
"version": "v1"
}
] | 2015-06-12 | [
[
"Azzurli",
"Francesco",
""
],
[
"Lechner",
"Kurt",
""
]
] | We determine for the first time the electromagnetic field generated by a generic massless accelerated charge, solving exactly Maxwell's equations. This result may shed new light on the possible existence of such particles in nature. | 15.926602 | 14.330269 | 13.13676 | 11.142231 | 12.399893 | 12.778699 | 13.699409 | 10.941672 | 13.153731 | 10.869222 | 14.164556 | 13.211342 | 12.533779 | 12.833741 | 12.834021 | 13.145298 | 13.061912 | 11.96414 | 13.067864 | 13.615238 | 13.819901 |
1608.02965 | Leonardo Rastelli | Leonardo Rastelli and Shlomo S. Razamat | The supersymmetric index in four dimensions | This is a contribution to the review volume `Localization techniques
in quantum field theories' (eds. V. Pestun and M. Zabzine) which contains 17
Chapters. The complete volume is summarized in arXiv:1608.02952 and it can be
downloaded at https://arxiv.org/src/1608.02952/anc/LocQFT.pdf or
http://pestun.ihes.fr/p... | null | 10.1088/1751-8121/aa76a6 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the calculation and properties of the supersymmetric index for four
dimensional N=1 theories, illustrating its physical significance in several
examples.
| [
{
"created": "Tue, 9 Aug 2016 20:01:50 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Aug 2016 14:22:45 GMT",
"version": "v2"
},
{
"created": "Sat, 15 Oct 2016 17:48:01 GMT",
"version": "v3"
}
] | 2017-10-25 | [
[
"Rastelli",
"Leonardo",
""
],
[
"Razamat",
"Shlomo S.",
""
]
] | We review the calculation and properties of the supersymmetric index for four dimensional N=1 theories, illustrating its physical significance in several examples. | 16.164047 | 9.411155 | 13.101376 | 10.007573 | 9.15412 | 9.107411 | 9.777048 | 9.7623 | 9.234493 | 13.684687 | 9.501876 | 11.932757 | 15.289553 | 11.76706 | 10.853437 | 11.286944 | 10.601081 | 11.580913 | 11.398554 | 13.743538 | 11.193505 |
hep-th/9703129 | Daniele Guido | Daniele Guido (U. Roma "Tor Vergata"), Roberto Longo (U. Roma "Tor
Vergata"), Hans-Werner Wiesbrock (Freie Universitaet Berlin) | Extensions of Conformal Nets and Superselection Structures | 34 pages, Latex2e. Some points have been clarified and some
references have been added. To appear in Communications in Mathematical
Physics | Commun.Math.Phys.192:217-244,1998 | 10.1007/s002200050297 | null | hep-th funct-an math.FA | null | Starting with a conformal Quantum Field Theory on the real line, we show that
the dual net is still conformal with respect to a new representation of the
Moebius group. We infer from this that every conformal net is normal and
conormal, namely the local von Neumann algebra associated with an interval
coincides with i... | [
{
"created": "Tue, 18 Mar 1997 18:50:07 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jul 1997 11:04:46 GMT",
"version": "v2"
}
] | 2011-04-06 | [
[
"Guido",
"Daniele",
"",
"U. Roma \"Tor Vergata\""
],
[
"Longo",
"Roberto",
"",
"U. Roma \"Tor\n Vergata\""
],
[
"Wiesbrock",
"Hans-Werner",
"",
"Freie Universitaet Berlin"
]
] | Starting with a conformal Quantum Field Theory on the real line, we show that the dual net is still conformal with respect to a new representation of the Moebius group. We infer from this that every conformal net is normal and conormal, namely the local von Neumann algebra associated with an interval coincides with its... | 13.985553 | 16.115702 | 16.720562 | 15.05535 | 15.38956 | 15.720124 | 18.484413 | 14.895563 | 13.860302 | 17.346685 | 14.524208 | 14.08096 | 14.470137 | 14.257215 | 13.805292 | 14.449207 | 14.017877 | 14.434088 | 13.953991 | 14.681221 | 13.489573 |
hep-th/0507028 | Kourosh Nozari | Kourosh Nozari and Mojdeh Karami | Minimal Length and Generalized Dirac Equation | 10 pages, no figure | Mod.Phys.Lett. A20 (2005) 3095-3104 | 10.1142/S0217732305018517 | null | hep-th | null | Existence of a minimal observable length which has been indicated by string
theory and quantum gravity, leads to a modification of Dirac equation. In this
letter we find this modified Dirac equation and solve its eigenvalue problem
for a free particle. We will show that due to background spacetime fluctuation,
it is ... | [
{
"created": "Sun, 3 Jul 2005 03:35:42 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Nozari",
"Kourosh",
""
],
[
"Karami",
"Mojdeh",
""
]
] | Existence of a minimal observable length which has been indicated by string theory and quantum gravity, leads to a modification of Dirac equation. In this letter we find this modified Dirac equation and solve its eigenvalue problem for a free particle. We will show that due to background spacetime fluctuation, it is im... | 11.291652 | 8.452084 | 9.414745 | 8.476597 | 8.782801 | 8.438072 | 7.917697 | 7.973462 | 9.403583 | 9.463357 | 8.896356 | 8.780763 | 9.09479 | 8.913481 | 8.828734 | 8.739033 | 8.874766 | 8.761388 | 8.750844 | 9.590726 | 9.311236 |
1604.05195 | Marc Geiller | Bianca Dittrich, Marc Geiller | Quantum gravity kinematics from extended TQFTs | 81 pages | New J. Phys. 19 (2017) 013003 | 10.1088/1367-2630/aa54e2 | null | hep-th cond-mat.str-el gr-qc math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how extended topological quantum field theories (TQFTs) can be used
to obtain a kinematical setup for quantum gravity, i.e. a kinematical Hilbert
space together with a representation of the observable algebra including
operators of quantum geometry. In particular, we consider the holonomy-flux
algebra of (2+1... | [
{
"created": "Mon, 18 Apr 2016 15:07:27 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Jan 2017 23:40:55 GMT",
"version": "v2"
}
] | 2017-01-10 | [
[
"Dittrich",
"Bianca",
""
],
[
"Geiller",
"Marc",
""
]
] | We show how extended topological quantum field theories (TQFTs) can be used to obtain a kinematical setup for quantum gravity, i.e. a kinematical Hilbert space together with a representation of the observable algebra including operators of quantum geometry. In particular, we consider the holonomy-flux algebra of (2+1)-... | 8.585353 | 9.581604 | 8.863513 | 8.9178 | 10.026199 | 9.279922 | 10.577483 | 8.77624 | 9.596229 | 9.500162 | 9.484716 | 8.953942 | 8.499872 | 8.390133 | 8.694364 | 8.660979 | 8.782555 | 8.687004 | 8.490359 | 8.663072 | 8.720419 |
1608.03919 | Seok Kim | Hee-Cheol Kim, Seok Kim, Jaemo Park | 6d strings from new chiral gauge theories | 54 pages, no figures | null | null | SNUTP16-002 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the 6d $\mathcal{N}=(1,0)$ superconformal field theory with smallest
non-Higgsable gauge symmetry $SU(3)$. In particular, we propose new 2d gauge
theory descriptions of its self-dual strings in the tensor branch. We use our
gauge theories to compute the elliptic genera of the self-dual strings, which
complet... | [
{
"created": "Fri, 12 Aug 2016 22:25:32 GMT",
"version": "v1"
}
] | 2016-08-16 | [
[
"Kim",
"Hee-Cheol",
""
],
[
"Kim",
"Seok",
""
],
[
"Park",
"Jaemo",
""
]
] | We study the 6d $\mathcal{N}=(1,0)$ superconformal field theory with smallest non-Higgsable gauge symmetry $SU(3)$. In particular, we propose new 2d gauge theory descriptions of its self-dual strings in the tensor branch. We use our gauge theories to compute the elliptic genera of the self-dual strings, which completel... | 7.037291 | 6.129078 | 8.924315 | 5.948109 | 6.240785 | 6.189236 | 6.214952 | 6.023289 | 6.181597 | 8.627413 | 5.884062 | 6.212303 | 7.338852 | 6.105403 | 6.338462 | 6.42268 | 6.157321 | 6.315501 | 6.218609 | 6.981585 | 6.422166 |
1903.09309 | Ichiro Oda | Ichiro Oda | Planck and Electroweak Scales Emerging from Weyl Conformal Gravity | 12 pages; Contribution to the Proceedings of the Corfu Summer
Institute 2018, Aug-Sep 2018, Corfu, Greece | null | null | DPUR/TH/63 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the Planck mass scale can be generated from conformal gravity in
the Weyl conformal geometry via the Coleman-Weinberg mechanism of dimensional
transmutation where quantum corrections stemming from the gravitational field
and the Weyl gauge field trigger the symmetry breakdown of a local Weyl
symmetry. It... | [
{
"created": "Fri, 22 Mar 2019 02:01:16 GMT",
"version": "v1"
}
] | 2019-03-25 | [
[
"Oda",
"Ichiro",
""
]
] | We show that the Planck mass scale can be generated from conformal gravity in the Weyl conformal geometry via the Coleman-Weinberg mechanism of dimensional transmutation where quantum corrections stemming from the gravitational field and the Weyl gauge field trigger the symmetry breakdown of a local Weyl symmetry. It i... | 9.257754 | 7.714427 | 8.431437 | 7.89869 | 9.318891 | 8.984421 | 9.104071 | 7.427804 | 8.284838 | 8.576979 | 8.275652 | 8.810707 | 8.585955 | 8.407453 | 8.767105 | 8.51862 | 8.779121 | 8.612283 | 8.688749 | 8.375351 | 8.750823 |
1810.03768 | Toshiaki Fujimori | Toshiaki Fujimori, Syo Kamata, Tatsuhiro Misumi, Muneto Nitta,
Norisuke Sakai | Bion non-perturbative contributions versus infrared renormalons in
two-dimensional $\mathbb C P^{N-1}$ models | 42 pages, | JHEP 02 (2019) 190 | 10.1007/JHEP02(2019)190 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the semiclassical contributions from the real and complex bions in
the two-dimensional $\mathbb C P^{N-1}$ sigma model on ${\mathbb R} \times
S^{1}$ with a twisted boundary condition. The bion configurations are saddle
points of the complexified Euclidean action, which can be viewed as bound
states of a pai... | [
{
"created": "Tue, 9 Oct 2018 01:44:24 GMT",
"version": "v1"
}
] | 2019-03-04 | [
[
"Fujimori",
"Toshiaki",
""
],
[
"Kamata",
"Syo",
""
],
[
"Misumi",
"Tatsuhiro",
""
],
[
"Nitta",
"Muneto",
""
],
[
"Sakai",
"Norisuke",
""
]
] | We derive the semiclassical contributions from the real and complex bions in the two-dimensional $\mathbb C P^{N-1}$ sigma model on ${\mathbb R} \times S^{1}$ with a twisted boundary condition. The bion configurations are saddle points of the complexified Euclidean action, which can be viewed as bound states of a pair ... | 5.48726 | 5.176441 | 5.710406 | 5.07157 | 5.303367 | 5.254063 | 5.313024 | 5.153457 | 5.23469 | 6.330059 | 4.969503 | 5.332184 | 5.479068 | 5.358207 | 5.368275 | 5.213372 | 5.280982 | 5.260784 | 5.325615 | 5.573246 | 5.318578 |
1709.04897 | Andrei Mironov | G. Aminov, A. Mironov and A. Morozov | Modular properties of 6d (DELL) systems | 23 pages | JHEP, 23 (2017) 2017 | 10.1007/JHEP11(2017)023 | FIAN/TD-22/17; IITP/TH-15/17; ITEP/TH-24/17 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | If super-Yang-Mills theory possesses the exact conformal invariance, there is
an additional modular invariance under the change of the complex bare charge
$\tau = \frac{\theta}{2\pi}+ \frac{4\pi\imath}{g^2}\longrightarrow
-\frac{1}{\tau}$. The low-energy Seiberg-Witten prepotential ${\cal F}(a)$,
however, is not expl... | [
{
"created": "Thu, 14 Sep 2017 17:37:30 GMT",
"version": "v1"
}
] | 2017-11-17 | [
[
"Aminov",
"G.",
""
],
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | If super-Yang-Mills theory possesses the exact conformal invariance, there is an additional modular invariance under the change of the complex bare charge $\tau = \frac{\theta}{2\pi}+ \frac{4\pi\imath}{g^2}\longrightarrow -\frac{1}{\tau}$. The low-energy Seiberg-Witten prepotential ${\cal F}(a)$, however, is not explic... | 8.403319 | 8.558406 | 9.759367 | 8.363417 | 8.359709 | 8.696086 | 8.938288 | 8.336103 | 7.718118 | 9.715742 | 8.338997 | 7.901641 | 8.156267 | 7.948157 | 8.017342 | 7.852476 | 7.710829 | 7.809273 | 7.96808 | 8.121023 | 7.749911 |
0712.2717 | Pantelis Manousselis | A. Chatzistavrakidis, P. Manousselis, N. Prezas, G. Zoupanos | Coset Space Dimensional Reduction of Einstein--Yang--Mills theory | 15 pages, Contribution to the workshop "Challenges Beyond the
Standard Model", September 2-9, 2007, Kladovo, Serbia. To appear in
Fortsch.Phys | Fortsch.Phys.56:389-399,2008 | 10.1002/prop.200710510 | null | hep-th | null | In the present contribution we extend our previous work by considering the
coset space dimensional reduction of higher-dimensional Einstein--Yang--Mills
theories including scalar fluctuations as well as Kaluza--Klein excitations of
the compactification metric and we describe the gravity-modified rules for the
reducti... | [
{
"created": "Mon, 17 Dec 2007 13:30:33 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Chatzistavrakidis",
"A.",
""
],
[
"Manousselis",
"P.",
""
],
[
"Prezas",
"N.",
""
],
[
"Zoupanos",
"G.",
""
]
] | In the present contribution we extend our previous work by considering the coset space dimensional reduction of higher-dimensional Einstein--Yang--Mills theories including scalar fluctuations as well as Kaluza--Klein excitations of the compactification metric and we describe the gravity-modified rules for the reduction... | 14.416345 | 12.491529 | 11.66861 | 11.17464 | 12.234025 | 13.318092 | 12.912417 | 12.89989 | 13.182203 | 12.814361 | 11.527942 | 12.117664 | 11.533087 | 12.427183 | 13.045373 | 12.311882 | 12.113489 | 11.91899 | 12.349532 | 12.318663 | 12.112956 |
hep-th/0506003 | Jerzy Kr\'ol | Jerzy Kr\'ol | Model theory and the AdS/CFT correspondence | 17 pages, presented at the IPM String School and Workshop, Queshm
Island, Iran, 05-14. 01. 2005. Some bibliographical corrections included | null | null | null | hep-th | null | We give arguments that exotic smooth structures on compact and noncompact
4-manifolds are essential for some approaches to quantum gravity. We rely on
the recently developed model-theoretic approach to exotic smoothness in
dimension four. It is possible to conjecture that exotic $R^4$'s play
fundamental role in quant... | [
{
"created": "Wed, 1 Jun 2005 08:23:35 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Jun 2005 10:46:25 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Król",
"Jerzy",
""
]
] | We give arguments that exotic smooth structures on compact and noncompact 4-manifolds are essential for some approaches to quantum gravity. We rely on the recently developed model-theoretic approach to exotic smoothness in dimension four. It is possible to conjecture that exotic $R^4$'s play fundamental role in quantum... | 14.505341 | 16.212296 | 13.786103 | 13.941923 | 14.526615 | 13.978385 | 15.802533 | 13.71838 | 13.668989 | 14.478933 | 13.972454 | 13.26346 | 14.337125 | 13.233813 | 13.95819 | 13.596246 | 13.882921 | 13.510536 | 13.86418 | 14.537585 | 14.183662 |
1805.04194 | Sean A. Hartnoll | Luca V. Delacr\'etaz, Thomas Hartman, Sean A. Hartnoll and Aitor
Lewkowycz | Thermalization, Viscosity and the Averaged Null Energy Condition | 28 pages, 3 figures | null | 10.1007/JHEP10(2018)028 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the implications of the averaged null energy condition for thermal
states of relativistic quantum field theories. A key property of such thermal
states is the thermalization length. This lengthscale generalizes the notion of
a mean free path beyond weak coupling, and allows finite size regions to
independe... | [
{
"created": "Thu, 10 May 2018 22:18:17 GMT",
"version": "v1"
}
] | 2018-11-14 | [
[
"Delacrétaz",
"Luca V.",
""
],
[
"Hartman",
"Thomas",
""
],
[
"Hartnoll",
"Sean A.",
""
],
[
"Lewkowycz",
"Aitor",
""
]
] | We explore the implications of the averaged null energy condition for thermal states of relativistic quantum field theories. A key property of such thermal states is the thermalization length. This lengthscale generalizes the notion of a mean free path beyond weak coupling, and allows finite size regions to independent... | 9.679381 | 10.665123 | 10.557463 | 9.71571 | 11.06968 | 11.387536 | 11.23202 | 10.487501 | 9.327343 | 10.071168 | 9.32123 | 9.584373 | 9.857595 | 9.809873 | 9.573627 | 9.46503 | 9.938707 | 9.675257 | 9.986129 | 10.278053 | 9.496218 |
hep-th/9803054 | Angel Uranga | Angel M. Uranga | Towards Mass Deformed N=4 SO(n) and Sp(k) gauge configurations | 48 pages, 6 figures (included). One reference corrected | Nucl.Phys.B526:241-277,1998 | 10.1016/S0550-3213(98)00370-8 | IASSNS-HEP-98/8 | hep-th | null | We study the introduction of orientifold six-planes in the type IIA brane
configurations known as elliptic models. The N=4 SO(n) and $Sp(k)$ theories
softly broken to N=2 through a mass for the adjoint hypermultiplet can be
realized in this framework in the presence of two orientifold planes with
opposite RR charge. ... | [
{
"created": "Fri, 6 Mar 1998 03:19:35 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Mar 1998 23:22:12 GMT",
"version": "v2"
}
] | 2009-10-09 | [
[
"Uranga",
"Angel M.",
""
]
] | We study the introduction of orientifold six-planes in the type IIA brane configurations known as elliptic models. The N=4 SO(n) and $Sp(k)$ theories softly broken to N=2 through a mass for the adjoint hypermultiplet can be realized in this framework in the presence of two orientifold planes with opposite RR charge. A ... | 9.691762 | 9.102458 | 10.902338 | 8.603202 | 8.969058 | 9.187473 | 9.343292 | 9.42591 | 9.279846 | 11.640623 | 8.549954 | 8.948615 | 9.407837 | 9.065843 | 9.150849 | 9.036633 | 8.73388 | 9.028057 | 8.931044 | 9.858249 | 9.033368 |
1009.5386 | I\~naki Garc\'ia-Etxebarria | Mirjam Cveti\v{c}, I\~naki Garc\'ia-Etxebarria and James Halverson | On the computation of non-perturbative effective potentials in the
string theory landscape -- IIB/F-theory perspective | 52 pages. v2: Added refs, fixed typos | null | 10.1002/prop.201000093 | UPR-1219-T, NSF-KITP-10-124 | hep-th hep-ph math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss a number of issues arising when computing non-perturbative effects
systematically across the string theory landscape. In particular, we cast the
study of fairly generic physical properties into the language of
computability/number theory and show that this amounts to solving systems of
diophantine equation... | [
{
"created": "Mon, 27 Sep 2010 20:06:43 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Nov 2010 16:28:57 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Cvetič",
"Mirjam",
""
],
[
"García-Etxebarria",
"Iñaki",
""
],
[
"Halverson",
"James",
""
]
] | We discuss a number of issues arising when computing non-perturbative effects systematically across the string theory landscape. In particular, we cast the study of fairly generic physical properties into the language of computability/number theory and show that this amounts to solving systems of diophantine equations.... | 10.396206 | 10.543113 | 11.212587 | 10.680059 | 11.146307 | 11.579775 | 10.640152 | 10.57918 | 10.66882 | 12.147293 | 10.033438 | 10.248477 | 10.542444 | 9.959178 | 10.070608 | 10.252921 | 10.146612 | 9.962016 | 10.108177 | 10.529161 | 10.034545 |
0711.1045 | Shinsuke Kawai | Shinsuke Kawai, Yuji Sugawara | Mirrorfolds with K3 Fibrations | Eqns (2.61) and (3.17) corrected | JHEP0802:065,2008 | 10.1088/1126-6708/2008/02/065 | UT-07-36, HIP-07-59/TH | hep-th | null | We study a class of non-geometric string vacua realized as completely soluble
superconformal field theory (SCFT). These models are defined as `interpolating
orbifolds' of $K3 \times S^1$ by the mirror transformation acting on the $K3$
fiber combined with the half-shift on the $S^1$-base. They are variants of the
T-fo... | [
{
"created": "Wed, 7 Nov 2007 09:49:51 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Feb 2008 17:10:51 GMT",
"version": "v2"
},
{
"created": "Tue, 6 May 2008 22:16:35 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Kawai",
"Shinsuke",
""
],
[
"Sugawara",
"Yuji",
""
]
] | We study a class of non-geometric string vacua realized as completely soluble superconformal field theory (SCFT). These models are defined as `interpolating orbifolds' of $K3 \times S^1$ by the mirror transformation acting on the $K3$ fiber combined with the half-shift on the $S^1$-base. They are variants of the T-fold... | 8.063956 | 8.38469 | 9.790049 | 8.012501 | 8.587379 | 8.687588 | 8.117717 | 8.252966 | 7.868774 | 9.769418 | 7.914427 | 8.023776 | 7.961451 | 7.806755 | 7.894625 | 8.015465 | 8.000145 | 7.851784 | 7.89481 | 8.098369 | 7.709643 |
hep-th/0208130 | Klaus Kirsten | Peter Gilkey, Klaus Kirsten and Dmitri Vassilevich | Heat trace asymptotics defined by transfer boundary conditions | 7 pages | Lett.Math.Phys. 63 (2003) 29-37 | null | null | hep-th | null | We compute the first 5 terms in the short-time heat trace asymptotics
expansion for an operator of Laplace type with transfer boundary conditions
using the functorial properties of these invariants.
| [
{
"created": "Mon, 19 Aug 2002 08:27:44 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gilkey",
"Peter",
""
],
[
"Kirsten",
"Klaus",
""
],
[
"Vassilevich",
"Dmitri",
""
]
] | We compute the first 5 terms in the short-time heat trace asymptotics expansion for an operator of Laplace type with transfer boundary conditions using the functorial properties of these invariants. | 22.981131 | 20.378771 | 30.621435 | 22.069832 | 22.000137 | 24.362223 | 26.744383 | 24.481285 | 18.993565 | 33.850201 | 19.922997 | 22.873169 | 23.363947 | 23.801817 | 22.179253 | 21.379633 | 21.532808 | 23.42658 | 21.709904 | 25.267902 | 21.95186 |
0912.1489 | Antonio Capolupo Dr | Massimo Blasone, Antonio Capolupo and Giuseppe Vitiello | Particle mixing, flavor condensate and dark energy | 3 pages, Presented at the Conference Neutrinos in Cosmology, Astro-,
Particle- and Nuclear Physics, Erice School on Nuclear Physics, Erice, Italy,
16-24 Sep 2009 | Prog.Part.Nucl.Phys.64:451-453,2010 | 10.1016/j.ppnp.2009.12.073 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The mixing of neutrinos and quarks generate a vacuum condensate that, at the
present epoch, behaves as a cosmological constant. The value of the dark energy
is constrained today by the very small breaking of the Lorentz invariance.
| [
{
"created": "Tue, 8 Dec 2009 13:20:13 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Blasone",
"Massimo",
""
],
[
"Capolupo",
"Antonio",
""
],
[
"Vitiello",
"Giuseppe",
""
]
] | The mixing of neutrinos and quarks generate a vacuum condensate that, at the present epoch, behaves as a cosmological constant. The value of the dark energy is constrained today by the very small breaking of the Lorentz invariance. | 14.71555 | 11.540544 | 13.073239 | 11.734834 | 11.965138 | 13.335464 | 13.762753 | 12.199934 | 13.097812 | 14.229515 | 11.365463 | 12.858384 | 13.271287 | 13.473875 | 12.617052 | 12.320965 | 12.617756 | 13.229154 | 12.798474 | 12.82515 | 12.402651 |
1907.13491 | David Pirtskhalava | Gregory Gabadadze, Daniel Older, David Pirtskhalava | Resolving the vDVZ and Strong Coupling Problems in Massive Gravity and
Bigravity | 29 + 14 pages | Phys. Rev. D 100, 124017 (2019) | 10.1103/PhysRevD.100.124017 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As is well known, both massive gravity and bigravity exhibit the linear van
Dam-Veltman-Zakharov (vDVZ) discontinuity that is cured classically by the
nonlinear Vainshtein mechanism due to certain low scale strongly coupled
interactions. Here we show how both the vDVZ and strong coupling problems can
be removed by em... | [
{
"created": "Wed, 31 Jul 2019 13:24:39 GMT",
"version": "v1"
}
] | 2019-12-11 | [
[
"Gabadadze",
"Gregory",
""
],
[
"Older",
"Daniel",
""
],
[
"Pirtskhalava",
"David",
""
]
] | As is well known, both massive gravity and bigravity exhibit the linear van Dam-Veltman-Zakharov (vDVZ) discontinuity that is cured classically by the nonlinear Vainshtein mechanism due to certain low scale strongly coupled interactions. Here we show how both the vDVZ and strong coupling problems can be removed by embe... | 7.637027 | 7.863551 | 8.026335 | 7.353775 | 7.558739 | 7.875384 | 7.891199 | 7.897504 | 7.761668 | 7.984655 | 7.481487 | 7.362366 | 7.695899 | 7.315411 | 7.348553 | 7.205054 | 7.240902 | 7.414649 | 7.318861 | 7.474874 | 7.372623 |
1309.0821 | Alessio Marrani | L.G.C. Gentile, P.A. Grassi, A. Marrani, and A. Mezzalira | Fermions, Wigs, and Attractors | v2 : 1+11 pages; paper reorganized in Sections; Sec. 5 added, with
detailed treatment of the axion-dilaton model; some typos fixed and
references added | null | 10.1016/j.physletb.2014.03.046 | DFPD-13/TH/16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the modifications to the attractor mechanism due to fermionic
corrections. In N=2, D=4 supergravity, at the fourth order, we find a new
contribution to the horizon values of the scalar fields of the vector
multiplets.
| [
{
"created": "Tue, 3 Sep 2013 20:00:10 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Jun 2014 13:50:18 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Gentile",
"L. G. C.",
""
],
[
"Grassi",
"P. A.",
""
],
[
"Marrani",
"A.",
""
],
[
"Mezzalira",
"A.",
""
]
] | We compute the modifications to the attractor mechanism due to fermionic corrections. In N=2, D=4 supergravity, at the fourth order, we find a new contribution to the horizon values of the scalar fields of the vector multiplets. | 11.457977 | 7.503474 | 12.744991 | 7.862981 | 8.495904 | 8.351995 | 9.020728 | 9.264369 | 8.101756 | 13.456953 | 8.245863 | 8.703522 | 10.008658 | 8.85699 | 9.136076 | 9.090044 | 8.653415 | 8.724938 | 9.045517 | 9.993318 | 8.631519 |
0909.0503 | Neil Barnaby | Neil Barnaby, J. Richard Bond, Zhiqi Huang and Lev Kofman | Preheating After Modular Inflation | 34 pages, 10 figures. Accepted for publication in JCAP | JCAP 0912:021,2009 | 10.1088/1475-7516/2009/12/021 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study (p)reheating in modular (closed string) inflationary scenarios, with
a special emphasis on Kahler moduli/Roulette models. It is usually assumed that
reheating in such models occurs through perturbative decays. However, we find
that there are very strong non-perturbative preheating decay channels related
to t... | [
{
"created": "Wed, 2 Sep 2009 20:18:05 GMT",
"version": "v1"
},
{
"created": "Sun, 13 Dec 2009 18:10:32 GMT",
"version": "v2"
}
] | 2010-01-15 | [
[
"Barnaby",
"Neil",
""
],
[
"Bond",
"J. Richard",
""
],
[
"Huang",
"Zhiqi",
""
],
[
"Kofman",
"Lev",
""
]
] | We study (p)reheating in modular (closed string) inflationary scenarios, with a special emphasis on Kahler moduli/Roulette models. It is usually assumed that reheating in such models occurs through perturbative decays. However, we find that there are very strong non-perturbative preheating decay channels related to the... | 8.610359 | 8.952744 | 9.322563 | 9.144049 | 9.278304 | 9.435365 | 10.135572 | 9.339783 | 8.285849 | 9.544991 | 8.669735 | 8.686173 | 8.689034 | 8.484126 | 8.515528 | 8.4064 | 8.655373 | 8.607518 | 8.54444 | 8.763818 | 8.541375 |
hep-th/9206082 | null | J. A. Dixon | BRS Operators and Covariant Derivatives in Loop Space for P-Branes
Coupled to Yang-Mills | 21 pages, CTP-TAMU-50/92 | Nucl.Phys.B407:73-87,1993 | 10.1016/0550-3213(93)90274-S | null | hep-th | null | Canonical forms are given for the nilpotent BRS operator $\d$ and the
covariant `loop space' derivative ${\cal D}_{\m}$ for the p-brane fields for
all odd p. The defining characteristic of ${\cal D}_{\m}$ is that it is a
functional derivative operator which generalizes the ordinary functional
derivative and also comm... | [
{
"created": "Mon, 22 Jun 1992 19:58:15 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Dixon",
"J. A.",
""
]
] | Canonical forms are given for the nilpotent BRS operator $\d$ and the covariant `loop space' derivative ${\cal D}_{\m}$ for the p-brane fields for all odd p. The defining characteristic of ${\cal D}_{\m}$ is that it is a functional derivative operator which generalizes the ordinary functional derivative and also commut... | 12.541001 | 9.797648 | 11.137737 | 10.445711 | 11.597988 | 10.857688 | 10.769349 | 11.140966 | 10.760879 | 13.62749 | 10.648063 | 10.465299 | 11.383649 | 10.790344 | 10.521421 | 10.303047 | 10.659392 | 10.548901 | 10.363688 | 11.761188 | 11.075707 |
hep-th/9801149 | Andrei Mironov | A.Mironov | On N=2 SUSY gauge theories and integrable systems | LaTeX, 7 pages; contribution to the 31st Ahrenshoop Symposium,
Buckow, Germany, 2-6 September 1997 | null | null | FIAN/TD-02/98; ITEP/TH-4/98 | hep-th | null | This note gives a brief review of the integrable structures presented in the
Seiberg-Witten approach to the N=2 SUSY gauge theories with emphasize on the
case of the gauge theories with matter hypermultiplets included (described by
spin chains). The web of different N=2 SUSY theories is discussed.
| [
{
"created": "Thu, 22 Jan 1998 15:17:27 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Mironov",
"A.",
""
]
] | This note gives a brief review of the integrable structures presented in the Seiberg-Witten approach to the N=2 SUSY gauge theories with emphasize on the case of the gauge theories with matter hypermultiplets included (described by spin chains). The web of different N=2 SUSY theories is discussed. | 13.142961 | 11.609599 | 13.232437 | 11.232506 | 10.498633 | 11.811567 | 10.709145 | 10.393653 | 10.627138 | 16.60536 | 11.592033 | 10.773542 | 12.009509 | 11.396294 | 12.268153 | 11.552974 | 11.110836 | 10.845422 | 11.364756 | 12.442722 | 11.097127 |
1207.1109 | Sergei Alexandrov | Sergei Alexandrov, Jan Manschot, Boris Pioline | D3-instantons, Mock Theta Series and Twistors | 42 pages; discussion of isometries is amended; misprints corrected | JHEP 1304 (2013) 002 | 10.1007/JHEP04(2013)002 | L2C:12-090; Bonn-TH-2012-13; CERN-PH-TH/2012-157 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The D-instanton corrected hypermultiplet moduli space of type II string
theory compactified on a Calabi-Yau threefold is known in the type IIA picture
to be determined in terms of the generalized Donaldson-Thomas invariants,
through a twistorial construction. At the same time, in the mirror type IIB
picture, and in t... | [
{
"created": "Wed, 4 Jul 2012 20:03:45 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Aug 2012 10:19:24 GMT",
"version": "v2"
},
{
"created": "Fri, 17 Feb 2017 19:08:40 GMT",
"version": "v3"
}
] | 2017-02-21 | [
[
"Alexandrov",
"Sergei",
""
],
[
"Manschot",
"Jan",
""
],
[
"Pioline",
"Boris",
""
]
] | The D-instanton corrected hypermultiplet moduli space of type II string theory compactified on a Calabi-Yau threefold is known in the type IIA picture to be determined in terms of the generalized Donaldson-Thomas invariants, through a twistorial construction. At the same time, in the mirror type IIB picture, and in the... | 5.929512 | 5.570212 | 7.893645 | 5.667911 | 5.594209 | 5.725657 | 5.187613 | 5.476338 | 5.732674 | 8.588188 | 5.541857 | 5.796794 | 6.522103 | 5.792336 | 5.728411 | 5.657626 | 5.637921 | 5.861236 | 5.900974 | 6.307243 | 5.689516 |
hep-th/0504145 | Subodh Patil | Subodh P. Patil | Moduli (Dilaton, Volume and Shape) Stabilization via Massless F and D
String Modes | 22 pages, 2 appendices, 2 EPS figs | null | null | null | hep-th astro-ph | null | Finding a consistent way to stabilize the various moduli fields which
generically appear in string theory compactifications, is essential if string
theory is to make contact with the physics we see around us. We present, in
this paper, a mechanism to stabilize the dilaton within a framework that has
already proven it... | [
{
"created": "Mon, 18 Apr 2005 19:29:37 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Feb 2006 10:27:12 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Patil",
"Subodh P.",
""
]
] | Finding a consistent way to stabilize the various moduli fields which generically appear in string theory compactifications, is essential if string theory is to make contact with the physics we see around us. We present, in this paper, a mechanism to stabilize the dilaton within a framework that has already proven itse... | 9.623406 | 9.996566 | 8.920144 | 8.479393 | 9.762579 | 9.966452 | 9.846843 | 9.35578 | 8.867201 | 9.092812 | 9.253595 | 8.925548 | 8.652099 | 8.620635 | 8.945338 | 8.871422 | 8.890228 | 8.478576 | 8.752052 | 8.862125 | 9.117887 |
1902.04307 | Sosuke Imai | Sosuke Imai, Yoshiyuki Tatsuta | Wavefunctions on $S^2$ with flux and branes | 31 pages, 7 figures | null | 10.1007/JHEP07(2019)005 | WU-HEP-19-03, DESY 19-018 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formulate a six dimensional $U(1)$ gauge theory compactified on a (two
dimensional) sphere $S^2$ with flux and localized brane sources. Profiles of
the lowest Kaluza-Klein (KK) wavefunctions and their masses are derived
analytically. In contrast to ordinary sphere compactifications, the above setup
can lead to the... | [
{
"created": "Tue, 12 Feb 2019 09:56:00 GMT",
"version": "v1"
}
] | 2020-01-08 | [
[
"Imai",
"Sosuke",
""
],
[
"Tatsuta",
"Yoshiyuki",
""
]
] | We formulate a six dimensional $U(1)$ gauge theory compactified on a (two dimensional) sphere $S^2$ with flux and localized brane sources. Profiles of the lowest Kaluza-Klein (KK) wavefunctions and their masses are derived analytically. In contrast to ordinary sphere compactifications, the above setup can lead to the d... | 11.852547 | 12.302818 | 9.70336 | 9.618692 | 10.255255 | 11.789683 | 11.154577 | 11.244975 | 10.083098 | 10.398058 | 10.822539 | 10.724573 | 9.927637 | 10.516541 | 10.521108 | 10.897427 | 10.906085 | 11.023039 | 10.339598 | 10.449068 | 10.598782 |
hep-th/9605041 | Steffen Meissner | B.-D. Doerfel and St. Meissner (HU Berlin) | Ground State Structure and Low Temperature Behaviour of an Integrable
Chain with Alternating Spins | 22 pages, LaTeX, uses ioplppt.sty and PicTeX macros | J.Phys.A29:6471-6487,1996 | 10.1088/0305-4470/29/20/006 | SFB 288 preprint | hep-th | null | In this paper we continue the investigation of an anisotropic integrable spin
chain, consisting of spins $s=1$ and $s=\frac{1}{2}$, started in our paper
\cite{meissner}. The thermodynamic Bethe ansatz is analysed especially for the
case, when the signs of the two couplings $\bar{c}$ and $\tilde{c}$ differ. For
the co... | [
{
"created": "Tue, 7 May 1996 09:41:10 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Doerfel",
"B. -D.",
"",
"HU Berlin"
],
[
"Meissner",
"St.",
"",
"HU Berlin"
]
] | In this paper we continue the investigation of an anisotropic integrable spin chain, consisting of spins $s=1$ and $s=\frac{1}{2}$, started in our paper \cite{meissner}. The thermodynamic Bethe ansatz is analysed especially for the case, when the signs of the two couplings $\bar{c}$ and $\tilde{c}$ differ. For the conf... | 7.987037 | 6.836781 | 8.110677 | 7.084391 | 7.408051 | 7.789547 | 7.157307 | 6.947704 | 6.828275 | 9.036248 | 7.159089 | 6.988877 | 7.787286 | 7.081949 | 6.984155 | 7.299561 | 7.153428 | 7.098757 | 7.342506 | 7.710742 | 7.056478 |
1408.6057 | Kellogg S. Stelle | K.S. Stelle | Symmetry Orbits of Supergravity Black Holes - In Honor of Andrei
Slavnov's 75th Birthday | 13 pages, 1 figure | null | null | Imperial/TP/14/KSS/01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Black hole solutions of supergravity theories form families that realizing
the deep nonlinear "duality" symmetries of these theories. They form orbits
under the action of these symmetry groups, with extremal (i.e. BPS) solutions
at the limits of such orbits. An important technique in the analysis of such
solution fam... | [
{
"created": "Tue, 26 Aug 2014 09:04:36 GMT",
"version": "v1"
}
] | 2014-08-27 | [
[
"Stelle",
"K. S.",
""
]
] | Black hole solutions of supergravity theories form families that realizing the deep nonlinear "duality" symmetries of these theories. They form orbits under the action of these symmetry groups, with extremal (i.e. BPS) solutions at the limits of such orbits. An important technique in the analysis of such solution famil... | 17.418783 | 15.32215 | 18.041828 | 15.885021 | 17.925756 | 15.844363 | 18.524557 | 18.237017 | 16.950483 | 20.02931 | 15.993757 | 15.62324 | 16.111675 | 14.617748 | 16.02096 | 15.454578 | 15.481308 | 15.172731 | 14.798347 | 15.647799 | 15.22076 |
hep-th/9909025 | Heiyoung Shin | Heiyoung Shin | Glueball Mass Spectrum in KK Monopole Background | 4 pages Latex | null | null | null | hep-th | null | We consider typeIIA supergravity solution of D2-branes and D3-branes
localized within D6-branes in the near-core region of D6-branes. With these
solutions we can calculate the spectrum of the glueball mass in QCD3 and QCD4.
The equation of motion describing the dilaton has the same eigenvalues and the
same glueball m... | [
{
"created": "Sat, 4 Sep 1999 09:22:17 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Shin",
"Heiyoung",
""
]
] | We consider typeIIA supergravity solution of D2-branes and D3-branes localized within D6-branes in the near-core region of D6-branes. With these solutions we can calculate the spectrum of the glueball mass in QCD3 and QCD4. The equation of motion describing the dilaton has the same eigenvalues and the same glueball mas... | 7.922242 | 8.401703 | 8.442364 | 7.687326 | 7.867956 | 7.814755 | 7.966237 | 7.800665 | 7.730443 | 9.238157 | 7.250218 | 7.484187 | 7.730168 | 7.294191 | 7.28459 | 7.498459 | 7.363415 | 7.148217 | 7.107163 | 7.70595 | 6.943222 |
hep-th/0007140 | Hyun Seok Yang | Bum-Hoon Lee, Kimyeong Lee, and Hyun Seok Yang | The CP(n) Model on Noncommutative Plane | v3: 14 pages, Latex, Published version in Phys. Lett. B | Phys.Lett. B498 (2001) 277-284 | 10.1016/S0370-2693(01)00006-5 | KIAS-P00045, NBI-HE-00-32, SOGANG-HEP 274/00 | hep-th | null | We construct the consistent CP(n) model on noncommutative plane. The
Bogomolny bound on the energy is saturated by (anti-)self-dual solitons with
integer topological charge, which is independent of their scaling and
orientation. This integer quantization is satisfied for our general solutions,
which turns out regular... | [
{
"created": "Tue, 18 Jul 2000 09:17:20 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Sep 2000 03:32:51 GMT",
"version": "v2"
},
{
"created": "Sun, 18 Mar 2001 17:31:41 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Lee",
"Bum-Hoon",
""
],
[
"Lee",
"Kimyeong",
""
],
[
"Yang",
"Hyun Seok",
""
]
] | We construct the consistent CP(n) model on noncommutative plane. The Bogomolny bound on the energy is saturated by (anti-)self-dual solitons with integer topological charge, which is independent of their scaling and orientation. This integer quantization is satisfied for our general solutions, which turns out regular e... | 13.769521 | 11.053069 | 12.754886 | 10.748645 | 10.87429 | 10.959969 | 10.715929 | 10.276429 | 11.079696 | 14.035939 | 10.871728 | 12.446968 | 13.845272 | 12.130445 | 12.173326 | 12.469402 | 11.584846 | 12.3213 | 12.275265 | 13.238746 | 12.167208 |
2209.12696 | Sunjin Choi | Sunjin Choi, Seok Kim, Eunwoo Lee, Jaemo Park | The shape of non-graviton operators for $SU(2)$ | 8 pages | null | null | KIAS-P22052 | hep-th | http://creativecommons.org/licenses/by/4.0/ | The BPS spectrum of AdS/CFT exhibits multi-gravitons at low energies, while
having black hole states at higher energies. This can be studied concretely in
AdS$_5$/CFT$_4$ in terms of classical cohomologies, even in the quantum regimes
at finite $1/N$. Recently, Chang and Lin found a threshold for non-graviton
states ... | [
{
"created": "Mon, 26 Sep 2022 13:45:23 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Sep 2022 16:11:19 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Jun 2023 07:00:33 GMT",
"version": "v3"
},
{
"created": "Mon, 1 Jul 2024 17:32:38 GMT",
"version": "v4"
}
] | 2024-07-02 | [
[
"Choi",
"Sunjin",
""
],
[
"Kim",
"Seok",
""
],
[
"Lee",
"Eunwoo",
""
],
[
"Park",
"Jaemo",
""
]
] | The BPS spectrum of AdS/CFT exhibits multi-gravitons at low energies, while having black hole states at higher energies. This can be studied concretely in AdS$_5$/CFT$_4$ in terms of classical cohomologies, even in the quantum regimes at finite $1/N$. Recently, Chang and Lin found a threshold for non-graviton states in... | 17.396692 | 14.323792 | 18.994106 | 13.772081 | 14.047338 | 15.385399 | 14.739153 | 13.314571 | 14.17294 | 19.497713 | 14.488346 | 14.379807 | 16.408747 | 15.116847 | 14.952807 | 14.361773 | 15.221634 | 14.65949 | 14.598276 | 16.316801 | 14.098486 |
1007.3843 | Kang Sin Choi | Kang-Sin Choi | SU(3) x SU(2) x U(1) Vacua in F-Theory | 40 pages, 1 figure | Nucl.Phys.B842:1-32,2011 | 10.1016/j.nuclphysb.2010.08.012 | KUNS-2282 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Standard Model group and matter spectrum is obtained in vacua of
F-theory, without resorting to an intermediate unification group. The group
SU(3) x SU(2) x U(1)_Y is the commutant to SU(5)_t \times U(1)_Y structure
group of a Higgs bundle in E_8 and is geometrically realized as a deformation
of I_5 singularity. ... | [
{
"created": "Thu, 22 Jul 2010 10:01:54 GMT",
"version": "v1"
}
] | 2014-11-21 | [
[
"Choi",
"Kang-Sin",
""
]
] | The Standard Model group and matter spectrum is obtained in vacua of F-theory, without resorting to an intermediate unification group. The group SU(3) x SU(2) x U(1)_Y is the commutant to SU(5)_t \times U(1)_Y structure group of a Higgs bundle in E_8 and is geometrically realized as a deformation of I_5 singularity. Ly... | 13.136435 | 13.888794 | 14.17662 | 11.884425 | 15.674006 | 13.434852 | 13.481738 | 13.283594 | 12.578951 | 14.365096 | 12.75314 | 12.452126 | 13.01662 | 12.382447 | 13.086452 | 12.699584 | 13.072728 | 12.382081 | 12.77694 | 13.538974 | 12.380827 |
hep-th/9911003 | Justin David | Justin R. David | String Theory and Black Holes | 106 pages, PhD thesis at TIFR | null | null | null | hep-th | null | This thesis aims to make precise the microscopic understanding of Hawking
radiation from the D1/D5 black hole. We present an explict construction of all
the shortmultiplets of the ${\cal N}=(4,4)$ SCFT on the symmetric product
$\tilde{T}^4/S(Q_1Q_5)$. An investigation of the symmerties of this SCFT
enables us to make... | [
{
"created": "Tue, 2 Nov 1999 05:56:02 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"David",
"Justin R.",
""
]
] | This thesis aims to make precise the microscopic understanding of Hawking radiation from the D1/D5 black hole. We present an explict construction of all the shortmultiplets of the ${\cal N}=(4,4)$ SCFT on the symmetric product $\tilde{T}^4/S(Q_1Q_5)$. An investigation of the symmerties of this SCFT enables us to make a... | 10.815364 | 10.605208 | 11.571584 | 10.249707 | 10.311373 | 10.818425 | 10.754795 | 10.41982 | 10.464723 | 13.153563 | 10.46719 | 10.00518 | 10.74072 | 10.059188 | 10.506527 | 10.325735 | 10.283363 | 10.249066 | 10.178189 | 11.300784 | 10.464678 |
1912.11422 | Gang Yang | Qingjun Jin and Gang Yang | Hidden Analytic Structure of Higgs Amplitudes and Maximal
Transcendentality Principle | 11 pages, 2 figures; Proceedings of the 14th International Symposium
on Radiative Corrections (RADCOR2019) 9-13 September 2019, Avignon, France | PoS(RADCOR2019)071 | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the computation of two-loop Higgs plus three-parton amplitudes
with dimension-seven operators in Higgs effective field theory. The computation
is based on the combination of unitarity cut and integration by parts methods
in an unconventional way. The analytic results take remarkably simple form. In
particu... | [
{
"created": "Tue, 24 Dec 2019 15:59:06 GMT",
"version": "v1"
}
] | 2019-12-25 | [
[
"Jin",
"Qingjun",
""
],
[
"Yang",
"Gang",
""
]
] | We present the computation of two-loop Higgs plus three-parton amplitudes with dimension-seven operators in Higgs effective field theory. The computation is based on the combination of unitarity cut and integration by parts methods in an unconventional way. The analytic results take remarkably simple form. In particula... | 12.424793 | 12.562983 | 12.017697 | 11.481823 | 13.259208 | 11.285962 | 11.73278 | 10.632916 | 11.139355 | 15.001113 | 11.655258 | 12.620337 | 12.06702 | 11.59016 | 12.391685 | 12.571141 | 12.474148 | 11.703144 | 12.274735 | 12.102612 | 12.150012 |
2211.14021 | Nikolay Kozyrev | Nikolay Kozyrev, Sergey Krivonos | Generalized Schwarzians | 12 pages, 0 figures | null | 10.1103/PhysRevD.107.026018 | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | In this paper we demonstrate that the different generalizations of the
Schwarzians, supersymmetric or purely bosonic, can be easily constructed by
using the nonlinear realizations technique.
| [
{
"created": "Fri, 25 Nov 2022 10:52:38 GMT",
"version": "v1"
}
] | 2023-02-01 | [
[
"Kozyrev",
"Nikolay",
""
],
[
"Krivonos",
"Sergey",
""
]
] | In this paper we demonstrate that the different generalizations of the Schwarzians, supersymmetric or purely bosonic, can be easily constructed by using the nonlinear realizations technique. | 20.030861 | 10.726905 | 17.261557 | 13.423858 | 12.113455 | 13.705951 | 12.313573 | 13.328255 | 11.894324 | 18.88376 | 12.706338 | 14.711138 | 17.496622 | 15.512568 | 14.795338 | 14.591304 | 15.523273 | 13.944552 | 15.00488 | 15.567614 | 15.165498 |
hep-th/0308201 | Sayed Fawad Hassan | S. F. Hassan | N=1 Worldsheet Boundary Couplings and Covariance of non-Abelian
Worldvolume Theory | 30 pages, LaTeX | null | null | USITP-03-07 | hep-th | null | A systematic construction is given for N=1 open string boundary coupling to
Abelian and non-Abelian Dp-brane worldvolume fields, in general curved
backgrounds. The basic ingredient is a set of four ``boundary vectors'' that
provide a unified description of boundary conditions and boundary couplings. We
then turn to t... | [
{
"created": "Thu, 28 Aug 2003 20:54:44 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Hassan",
"S. F.",
""
]
] | A systematic construction is given for N=1 open string boundary coupling to Abelian and non-Abelian Dp-brane worldvolume fields, in general curved backgrounds. The basic ingredient is a set of four ``boundary vectors'' that provide a unified description of boundary conditions and boundary couplings. We then turn to the... | 10.114651 | 10.120719 | 11.047483 | 8.984551 | 11.01439 | 10.550737 | 10.127077 | 9.457286 | 9.542738 | 11.197109 | 9.086606 | 9.678498 | 9.633836 | 9.231256 | 9.490225 | 9.599085 | 9.420581 | 9.310966 | 9.179137 | 9.683283 | 9.119516 |
hep-th/0610189 | Ying-Qiu Gu | Ying-Qiu Gu | Test of Einstein's Mass-Energy Relation | 6 pages, 1 figure | Applied Physics Research, Vol. 10, No. 1, 1-4(2018) | 10.5539/apr.v10n1p1 | null | hep-th hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Einstein's mass-energy relation $E=mc^2$ is one of the most fundamental
formulae in physics, but it has not been seriously tested by an elaborated
experiment, and only some indirect evidences in nuclear reaction suggested that
it holds to high precision. Manifestly, for a particle, different self
potential leads ... | [
{
"created": "Tue, 17 Oct 2006 08:56:47 GMT",
"version": "v1"
},
{
"created": "Sun, 16 Jan 2011 16:48:58 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Jun 2017 03:10:24 GMT",
"version": "v3"
}
] | 2018-01-09 | [
[
"Gu",
"Ying-Qiu",
""
]
] | The Einstein's mass-energy relation $E=mc^2$ is one of the most fundamental formulae in physics, but it has not been seriously tested by an elaborated experiment, and only some indirect evidences in nuclear reaction suggested that it holds to high precision. Manifestly, for a particle, different self potential leads to... | 13.490978 | 12.915475 | 12.6134 | 12.18239 | 12.832647 | 12.999519 | 13.745252 | 11.746411 | 13.450787 | 11.856483 | 12.96221 | 12.562686 | 11.99152 | 11.879488 | 11.890026 | 12.606239 | 12.258554 | 12.092382 | 12.127343 | 11.374409 | 12.386602 |
hep-th/0006229 | Gerald V. Dunne | I. J. R. Aitchison and G. V. Dunne | Nontopological Finite Temperature Induced Fermion Number | 7 pp, 2 figs; refs + comments added; to appear in PRL | Phys.Rev.Lett. 86 (2001) 1690-1693 | 10.1103/PhysRevLett.86.1690 | null | hep-th cond-mat.soft hep-ph | null | We show that while the zero temperature induced fermion number in a chiral
sigma model background depends only on the asymptotic values of the chiral
field, at finite temperature the induced fermion number depends also on the
detailed shape of the chiral background. We resum the leading low temperature
terms to all o... | [
{
"created": "Thu, 29 Jun 2000 02:10:18 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Feb 2001 13:47:04 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Aitchison",
"I. J. R.",
""
],
[
"Dunne",
"G. V.",
""
]
] | We show that while the zero temperature induced fermion number in a chiral sigma model background depends only on the asymptotic values of the chiral field, at finite temperature the induced fermion number depends also on the detailed shape of the chiral background. We resum the leading low temperature terms to all ord... | 9.058801 | 8.982887 | 9.469464 | 8.541515 | 9.325533 | 9.920543 | 8.644923 | 8.771799 | 8.361473 | 10.468778 | 9.200325 | 8.537814 | 9.144844 | 8.429418 | 8.794285 | 8.573425 | 8.944999 | 8.720944 | 8.96382 | 8.92755 | 8.633138 |
2103.02998 | Reza Pirmoradian | Reza Pirmoradian and Mohammad Reza Tanhayi | Non-local Probes of Entanglement in the Scale Invariant Gravity | 14 pages, 3 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the generic action for the scale-invariant theory of
gravity and then by making use of the holographic methods, we compute some
specific holographic measures of entanglement. Precisely, we calculate the
entanglement entropy, mutual and tripartite information and show that the
mutual informatio... | [
{
"created": "Thu, 4 Mar 2021 12:46:01 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Apr 2021 09:13:46 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Apr 2021 07:08:46 GMT",
"version": "v3"
}
] | 2021-04-19 | [
[
"Pirmoradian",
"Reza",
""
],
[
"Tanhayi",
"Mohammad Reza",
""
]
] | In this paper, we study the generic action for the scale-invariant theory of gravity and then by making use of the holographic methods, we compute some specific holographic measures of entanglement. Precisely, we calculate the entanglement entropy, mutual and tripartite information and show that the mutual information ... | 9.364401 | 8.161741 | 7.890474 | 7.737199 | 7.736512 | 7.733541 | 7.177831 | 7.076861 | 7.717967 | 9.863057 | 7.793001 | 8.015572 | 7.991376 | 7.576155 | 7.677953 | 7.705225 | 7.722996 | 7.697098 | 7.834141 | 7.978356 | 7.867637 |
1504.05745 | Razvan-Gheorghe Gurau | Thibault Delepouve, Razvan Gurau | Phase Transition in Tensor Models | null | JHEP 06 (2015) 178 | 10.1007/JHEP06(2015)178 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Generalizing matrix models, tensor models generate dynamical triangulations
in any dimension and support a $1/N$ expansion. Using the intermediate field
representation we explicitly rewrite a quartic tensor model as a field theory
for a fluctuation field around a vacuum state corresponding to the resummation
of the e... | [
{
"created": "Wed, 22 Apr 2015 11:42:29 GMT",
"version": "v1"
}
] | 2015-07-09 | [
[
"Delepouve",
"Thibault",
""
],
[
"Gurau",
"Razvan",
""
]
] | Generalizing matrix models, tensor models generate dynamical triangulations in any dimension and support a $1/N$ expansion. Using the intermediate field representation we explicitly rewrite a quartic tensor model as a field theory for a fluctuation field around a vacuum state corresponding to the resummation of the ent... | 13.624594 | 12.453373 | 12.493731 | 10.58673 | 12.609224 | 12.53542 | 13.629525 | 10.324025 | 11.720967 | 15.18958 | 11.394217 | 11.865353 | 12.016419 | 11.009717 | 12.0143 | 11.596896 | 11.900344 | 11.453356 | 11.528328 | 11.60061 | 11.095916 |
hep-th/0604124 | Nadav Drukker | Nadav Drukker and Shoichi Kawamoto | Small deformations of supersymmetric Wilson loops and open spin-chains | 40 pages, amstex, 4 figures. V2: Corrected eqn (2.14) and some
equations in section 5. Version to appear in JHEP | JHEP0607:024,2006 | 10.1088/1126-6708/2006/07/024 | null | hep-th | null | We study insertions of composite operators into Wilson loops in N=4
supersymmetric Yang-Mills theory in four dimensions. The loops follow a
circular or straight path and the composite insertions transform in the adjoint
representation of the gauge group. This provides a gauge invariant way to
define the correlator of... | [
{
"created": "Tue, 18 Apr 2006 20:00:28 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jul 2006 14:42:14 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Drukker",
"Nadav",
""
],
[
"Kawamoto",
"Shoichi",
""
]
] | We study insertions of composite operators into Wilson loops in N=4 supersymmetric Yang-Mills theory in four dimensions. The loops follow a circular or straight path and the composite insertions transform in the adjoint representation of the gauge group. This provides a gauge invariant way to define the correlator of n... | 8.37293 | 7.960985 | 10.027477 | 8.04282 | 8.391438 | 8.301291 | 8.0764 | 8.395107 | 8.221022 | 10.921234 | 7.917032 | 8.17846 | 8.906201 | 7.899746 | 8.055713 | 8.143233 | 7.994257 | 8.114565 | 8.045388 | 8.674468 | 7.879048 |
1507.08659 | Jun Bourdier | Jun Bourdier, Nadav Drukker and Jan Felix | The exact Schur index of $\mathcal{N}=4$ SYM | 11 pages; v2: typos corrected | null | 10.1007/JHEP11(2015)210 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Witten index counts the difference in the number of bosonic and fermionic
states of a quantum mechanical system. The Schur index, which can be defined
for theories with at least $\mathcal{N}=2$ supersymmetry in four dimensions is
a particular refinement of the index, dependent on one parameter $q$ serving as
the ... | [
{
"created": "Thu, 30 Jul 2015 20:05:15 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Oct 2015 13:47:42 GMT",
"version": "v2"
}
] | 2016-01-27 | [
[
"Bourdier",
"Jun",
""
],
[
"Drukker",
"Nadav",
""
],
[
"Felix",
"Jan",
""
]
] | The Witten index counts the difference in the number of bosonic and fermionic states of a quantum mechanical system. The Schur index, which can be defined for theories with at least $\mathcal{N}=2$ supersymmetry in four dimensions is a particular refinement of the index, dependent on one parameter $q$ serving as the fu... | 7.333411 | 6.197529 | 7.744885 | 6.379921 | 7.034371 | 6.926212 | 6.821114 | 6.545921 | 6.388857 | 9.122315 | 6.336773 | 6.913399 | 6.927835 | 6.576869 | 6.917273 | 6.880555 | 6.572079 | 6.579892 | 6.62797 | 7.289323 | 6.601212 |
hep-th/0105293 | Nicholas Jones | Eanna Flanagan, Richard J. Hill, Nicholas Jones, S.-H. Henry Tye, Ira
Wasserman | Probe Brane Dynamics and the Cosmological Constant | 13 pages, 1 figure, REVTEX | Phys.Lett. B515 (2001) 161-169 | 10.1016/S0370-2693(01)00837-1 | CLNS 01/1738 | hep-th | null | Recently a brane world perspective on the cosmological constant and the
hierarchy problems was presented. Here, we elaborate on some aspects of that
particular scenario and discuss the stability of the stationary brane solution
and the dynamics of a probe brane. Even though the brane is unstable under a
small perturb... | [
{
"created": "Tue, 29 May 2001 16:44:04 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Flanagan",
"Eanna",
""
],
[
"Hill",
"Richard J.",
""
],
[
"Jones",
"Nicholas",
""
],
[
"Tye",
"S. -H. Henry",
""
],
[
"Wasserman",
"Ira",
""
]
] | Recently a brane world perspective on the cosmological constant and the hierarchy problems was presented. Here, we elaborate on some aspects of that particular scenario and discuss the stability of the stationary brane solution and the dynamics of a probe brane. Even though the brane is unstable under a small perturbat... | 10.476336 | 9.063791 | 9.55927 | 9.149785 | 9.857817 | 9.900652 | 9.488471 | 8.843239 | 8.990118 | 9.743425 | 8.94045 | 9.33972 | 9.912648 | 9.68712 | 9.854517 | 9.950093 | 9.586987 | 9.729014 | 9.429563 | 10.274594 | 9.761773 |
2406.03764 | Shuo Zhang | Shuo Zhang | More on spin-2 operators in holographic quantum mechanics | 18 pages, 3 figures, v2: added references | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study the spectrum, unitarity bound and holographic central charge of
spin-2 operators in a warped $\text{AdS}_2 \times \text{S}^2 \times \text{T}^4
\times \mathcal{I}_\psi \times \mathcal{I}_\rho$ background in the Type IIB
theory. We were able to identify a class of solutions that is completely
independent of th... | [
{
"created": "Thu, 6 Jun 2024 05:59:15 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Jun 2024 09:01:46 GMT",
"version": "v2"
}
] | 2024-06-13 | [
[
"Zhang",
"Shuo",
""
]
] | We study the spectrum, unitarity bound and holographic central charge of spin-2 operators in a warped $\text{AdS}_2 \times \text{S}^2 \times \text{T}^4 \times \mathcal{I}_\psi \times \mathcal{I}_\rho$ background in the Type IIB theory. We were able to identify a class of solutions that is completely independent of the ... | 8.175064 | 6.395659 | 7.914274 | 6.242286 | 6.686602 | 6.756115 | 6.571442 | 6.522428 | 6.14382 | 8.215325 | 6.29557 | 6.689285 | 7.791276 | 6.792644 | 6.881014 | 7.145478 | 6.922771 | 6.803954 | 7.024983 | 7.65222 | 6.638255 |
0712.2989 | Recai Erdem | Recai Erdem | A way to get rid of cosmological constant and zero point energy problems
of quantum fields through metric reversal symmetry | Presentation and content are improved, references are added. I would
like to thank the anonymous referee for his valuable comments and suggestions
to improve the paper | J.Phys.A41:235401,2008 | 10.1088/1751-8113/41/23/235401 | IZTECH-P-07-06 | hep-th astro-ph gr-qc hep-ph | null | In this paper a framework is introduced to remove the huge discrepancy
between the empirical value of the cosmological constant and the contribution
to the cosmological constant predicted from the vacuum energy of quantum
fields. An extra dimensional space with metric reversal symmetry and $R^2$
gravity is considered... | [
{
"created": "Tue, 18 Dec 2007 16:16:52 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Apr 2008 15:50:36 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Erdem",
"Recai",
""
]
] | In this paper a framework is introduced to remove the huge discrepancy between the empirical value of the cosmological constant and the contribution to the cosmological constant predicted from the vacuum energy of quantum fields. An extra dimensional space with metric reversal symmetry and $R^2$ gravity is considered t... | 9.993431 | 8.944912 | 8.850033 | 9.260818 | 9.221712 | 9.83543 | 9.350374 | 9.463317 | 8.994601 | 8.960506 | 9.795033 | 9.287706 | 9.096012 | 8.906984 | 8.878923 | 8.96387 | 9.034136 | 8.894842 | 8.721022 | 9.003817 | 9.522951 |
1007.3301 | Christian Saemann | Christian Saemann | Constructing Self-Dual Strings | 1+19 pages, presentation improved, minor corrections, published
version | Commun.Math.Phys.305:513-532,2011 | 10.1007/s00220-011-1257-2 | HWM-10-25, EMPG-10-12 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an ADHMN-like construction which generates self-dual string
solutions to the effective M5-brane worldvolume theory from solutions to the
Basu-Harvey equation. Our construction finds a natural interpretation in terms
of gerbes, which we develop in some detail. We also comment on a possible
extension to stac... | [
{
"created": "Mon, 19 Jul 2010 22:34:24 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Aug 2010 15:01:30 GMT",
"version": "v2"
},
{
"created": "Thu, 2 Jun 2011 18:42:58 GMT",
"version": "v3"
}
] | 2011-06-03 | [
[
"Saemann",
"Christian",
""
]
] | We present an ADHMN-like construction which generates self-dual string solutions to the effective M5-brane worldvolume theory from solutions to the Basu-Harvey equation. Our construction finds a natural interpretation in terms of gerbes, which we develop in some detail. We also comment on a possible extension to stacks... | 11.261742 | 8.604346 | 12.492477 | 8.908329 | 9.059671 | 8.45697 | 9.250553 | 8.852128 | 8.637201 | 12.325992 | 8.627077 | 9.744961 | 11.357814 | 9.81777 | 10.318931 | 9.354553 | 9.583524 | 9.720967 | 10.047067 | 11.828766 | 9.866632 |
1103.6068 | Tadashi Takayanagi | Shinsei Ryu, Tadashi Takayanagi, and Tomonori Ugajin | Holographic Conductivity in Disordered Systems | 43 pages, 28 figures, latex, references added, minor corrections | null | 10.1007/JHEP04(2011)115 | IPMU11-0053 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The main purpose of this paper is to holographically study the behavior of
conductivity in 2+1 dimensional disordered systems. We analyze probe D-brane
systems in AdS/CFT with random closed string and open string background fields.
We give a prescription of calculating the DC conductivity holographically in
disordere... | [
{
"created": "Thu, 31 Mar 2011 00:27:58 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Apr 2011 21:55:04 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Ryu",
"Shinsei",
""
],
[
"Takayanagi",
"Tadashi",
""
],
[
"Ugajin",
"Tomonori",
""
]
] | The main purpose of this paper is to holographically study the behavior of conductivity in 2+1 dimensional disordered systems. We analyze probe D-brane systems in AdS/CFT with random closed string and open string background fields. We give a prescription of calculating the DC conductivity holographically in disordered ... | 11.343784 | 10.271778 | 13.913803 | 10.061632 | 10.143894 | 9.882978 | 9.664248 | 9.746203 | 10.212782 | 13.809954 | 10.139367 | 10.399676 | 12.001802 | 10.479231 | 10.682522 | 10.831411 | 10.495306 | 10.316358 | 11.078672 | 12.352242 | 11.038587 |
2302.03041 | Christian Ferko | Chih-Kai Chang, Christian Ferko, Savdeep Sethi | Holography and Irrelevant Operators | 44 pages, LaTeX; v2: references and a new section added | null | 10.1103/PhysRevD.107.126021 | EFI-21-8 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We explore the holographic proposal involving spacetimes with linear dilaton
asymptotics in three dimensions from a gravity perspective. The holographic
dual shares some properties with a symmetric product conformal field theory
deformed by a single-trace analogue of the $T \overline{T}$ deformation. We
present solut... | [
{
"created": "Mon, 6 Feb 2023 19:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Apr 2023 05:14:22 GMT",
"version": "v2"
}
] | 2023-07-05 | [
[
"Chang",
"Chih-Kai",
""
],
[
"Ferko",
"Christian",
""
],
[
"Sethi",
"Savdeep",
""
]
] | We explore the holographic proposal involving spacetimes with linear dilaton asymptotics in three dimensions from a gravity perspective. The holographic dual shares some properties with a symmetric product conformal field theory deformed by a single-trace analogue of the $T \overline{T}$ deformation. We present solutio... | 9.999407 | 9.433782 | 11.379066 | 9.201403 | 9.542091 | 8.943898 | 8.739441 | 9.300081 | 8.827153 | 10.677488 | 8.318563 | 8.917379 | 10.540403 | 9.72207 | 9.378128 | 9.38582 | 9.580384 | 9.469429 | 9.292723 | 10.413988 | 9.40567 |
2406.06704 | Hee-Cheol Kim | Hee-Cheol Kim, Cumrun Vafa | Exploring new constraints on Kahler moduli space of 6d N = 1
Supergravity | 32 pages, v2: typos fixed, references added | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We propose new constraints for 6d (1, 0) supergravity theories based on
consistency conditions on the Kahler moduli spaces of their 5d reductions. The
requirement that both the metric and the BPS string tensions in the Kahler
moduli space are positive imposes specific restrictions on the Chern-Simons
coefficients in ... | [
{
"created": "Mon, 10 Jun 2024 18:07:06 GMT",
"version": "v1"
},
{
"created": "Sat, 20 Jul 2024 19:17:12 GMT",
"version": "v2"
}
] | 2024-07-23 | [
[
"Kim",
"Hee-Cheol",
""
],
[
"Vafa",
"Cumrun",
""
]
] | We propose new constraints for 6d (1, 0) supergravity theories based on consistency conditions on the Kahler moduli spaces of their 5d reductions. The requirement that both the metric and the BPS string tensions in the Kahler moduli space are positive imposes specific restrictions on the Chern-Simons coefficients in th... | 7.91548 | 7.897183 | 9.48905 | 7.200274 | 7.247807 | 7.773691 | 7.714026 | 7.383089 | 7.577518 | 10.163039 | 7.270482 | 7.661958 | 8.516164 | 7.629676 | 7.459048 | 7.672639 | 7.26149 | 7.460594 | 7.647197 | 8.498847 | 7.4682 |
0905.4326 | Makoto Sakamoto | Makoto Sakamoto | Strong Coupling Quantum Einstein Gravity at a z=2 Lifshitz Point | 10 pages, Added references | Phys.Rev.D79:124038,2009 | 10.1103/PhysRevD.79.124038 | KOBE-TH-09-04 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We solve a renormalized Wheeler-DeWitt equation for Einstein gravity in D+1
dimensions with D= odd in the strong coupling limit, which is expected to be
suited to probe quantum geometry at short distances, in order to test Horava's
idea that quantum gravity at short distances will be described by a
nonrelativistic sy... | [
{
"created": "Wed, 27 May 2009 04:03:02 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Jun 2009 01:29:49 GMT",
"version": "v2"
}
] | 2009-07-09 | [
[
"Sakamoto",
"Makoto",
""
]
] | We solve a renormalized Wheeler-DeWitt equation for Einstein gravity in D+1 dimensions with D= odd in the strong coupling limit, which is expected to be suited to probe quantum geometry at short distances, in order to test Horava's idea that quantum gravity at short distances will be described by a nonrelativistic syst... | 9.178674 | 9.243172 | 9.626277 | 8.348324 | 9.146609 | 9.269277 | 8.878078 | 8.357832 | 8.26032 | 10.599943 | 8.225122 | 8.723056 | 8.947063 | 8.505413 | 8.719683 | 8.250542 | 8.335822 | 8.429285 | 8.623218 | 9.050284 | 8.442912 |
hep-th/9812103 | Wifredo Garcia Fuertes | W. Garcia Fuertes (Universidad de Oviedo) and J. Mateos Guilarte
(Universidad de Salamanca) | Low Energy Vortex Dynamics in Abelian Higgs Systems | 26 pages, 1 figure, to appear in The European Physical Journal C | Eur.Phys.J.C9:535-547,1999 | 10.1007/s100529900033 | FFUOV-98-18, FTUS preprint (Universidad de Salamanca) | hep-th | null | The low energy dynamics of the vortices of the Abelian Chern-Simons-Higgs
system is investigated from the adiabatic approach. The difficulties involved
in treating the field evolution as motion on the moduli space in this system
are shown. Another two generalized Abelian Higgs systems are discusssed with
respect to t... | [
{
"created": "Sat, 12 Dec 1998 19:32:58 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Fuertes",
"W. Garcia",
"",
"Universidad de Oviedo"
],
[
"Guilarte",
"J. Mateos",
"",
"Universidad de Salamanca"
]
] | The low energy dynamics of the vortices of the Abelian Chern-Simons-Higgs system is investigated from the adiabatic approach. The difficulties involved in treating the field evolution as motion on the moduli space in this system are shown. Another two generalized Abelian Higgs systems are discusssed with respect to the... | 15.132752 | 12.382088 | 16.129093 | 13.519546 | 12.779295 | 13.114291 | 13.957685 | 12.253974 | 12.187003 | 16.660549 | 12.520766 | 13.083302 | 15.100098 | 13.575085 | 13.906113 | 13.366184 | 14.02866 | 13.190903 | 13.690629 | 14.596251 | 13.296252 |
1111.5457 | Axel Maas | Axel Maas | On the structure of the residual gauge orbit | 12 pages, 6 figures, talk given at the "II International Workshop on
QCD Green"s Functions, Confinement and Phenomenology", Trento, Italy,
September 2011. Submitted to the proceedings | PoS(QCD-TNT-II)028 (2011) | null | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gauge-fixed correlation functions are a valuable tool in intermediate steps
when determining gauge-invariant physics. However, when obtaining them in
different calculations, it is necessary to use exactly the same definition of
the gauge to ensure comparability. Beyond perturbation theory, this is
complicated by the ... | [
{
"created": "Wed, 23 Nov 2011 11:08:59 GMT",
"version": "v1"
}
] | 2012-01-06 | [
[
"Maas",
"Axel",
""
]
] | Gauge-fixed correlation functions are a valuable tool in intermediate steps when determining gauge-invariant physics. However, when obtaining them in different calculations, it is necessary to use exactly the same definition of the gauge to ensure comparability. Beyond perturbation theory, this is complicated by the Gr... | 12.464849 | 14.353561 | 13.813231 | 13.369195 | 14.635272 | 14.705376 | 15.31454 | 14.702136 | 13.306679 | 14.082118 | 13.526271 | 12.908551 | 12.607403 | 12.172745 | 12.18611 | 12.344082 | 12.985246 | 12.573035 | 12.330817 | 12.878618 | 12.592545 |
hep-th/9502121 | null | S.A.Frolov | Hamiltonian lattice gauge models and the Heisenberg double | 10 pages, latex, no figures | Mod.Phys.Lett. A10 (1995) 2885-2896 | 10.1142/S0217732395003021 | LMU-TPW 95-3 | hep-th | null | Hamiltonian lattice gauge models based on the assignment of the Heisenberg
double of a Lie group to each link of the lattice are constructed in arbitrary
space-time dimensions. It is shown that the corresponding generalization of the
gauge-invariant Wilson line observables requires to attach to each vertex of
the lin... | [
{
"created": "Mon, 20 Feb 1995 12:04:03 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Frolov",
"S. A.",
""
]
] | Hamiltonian lattice gauge models based on the assignment of the Heisenberg double of a Lie group to each link of the lattice are constructed in arbitrary space-time dimensions. It is shown that the corresponding generalization of the gauge-invariant Wilson line observables requires to attach to each vertex of the line ... | 15.103172 | 12.862723 | 14.274871 | 11.824424 | 11.826149 | 12.996696 | 12.24444 | 11.446384 | 11.608813 | 15.646544 | 11.456139 | 11.496563 | 13.20685 | 11.500422 | 11.890219 | 11.382425 | 11.877019 | 12.369844 | 12.742427 | 13.209464 | 12.294802 |
0905.3474 | Hristu Culetu | Hristu Culetu | Light Dragging Phenomenon and Expanding Wormholes | 9 pages, no figures, title changed, version published in J. Korean
Phys. Soc. 57 (3), 419 - 423 (2010) | null | 10.3938/jkps.57.419 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The null geodesic congruence for the Lorentzian version of Hawking's wormhole
is studied, in spherical Rindler coordinates. One finds that the wormhole
throat expands exponentially and the "flare - out" condition is satisfied. A
time reversal is equivalent with an inversion applied to the radial coordinate.
The stres... | [
{
"created": "Thu, 21 May 2009 11:51:11 GMT",
"version": "v1"
},
{
"created": "Thu, 28 May 2009 12:38:33 GMT",
"version": "v2"
},
{
"created": "Thu, 16 Sep 2010 13:06:57 GMT",
"version": "v3"
}
] | 2015-05-13 | [
[
"Culetu",
"Hristu",
""
]
] | The null geodesic congruence for the Lorentzian version of Hawking's wormhole is studied, in spherical Rindler coordinates. One finds that the wormhole throat expands exponentially and the "flare - out" condition is satisfied. A time reversal is equivalent with an inversion applied to the radial coordinate. The stress ... | 19.863678 | 21.632128 | 17.758621 | 19.115377 | 20.439468 | 20.751633 | 21.163855 | 19.069052 | 21.083496 | 18.008314 | 19.78858 | 19.887512 | 19.281208 | 18.826237 | 18.50704 | 18.837381 | 19.245451 | 18.964558 | 19.686367 | 18.873991 | 19.035702 |
1609.01311 | Steven Abel | Steven Abel | A Dynamical Mechanism for Large Volumes with Consistent Couplings | 28 pages, 8 figures | null | 10.1007/JHEP11(2016)085 | IPPP/16/68 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A mechanism for addressing the 'decompactification problem' is proposed,
which consists of balancing the vacuum energy in Scherk-Schwarzed theories
against contributions coming from non- perturbative physics. Universality of
threshold corrections ensures that, in such situations, the stable minimum will
have consiste... | [
{
"created": "Mon, 5 Sep 2016 20:11:39 GMT",
"version": "v1"
}
] | 2016-12-21 | [
[
"Abel",
"Steven",
""
]
] | A mechanism for addressing the 'decompactification problem' is proposed, which consists of balancing the vacuum energy in Scherk-Schwarzed theories against contributions coming from non- perturbative physics. Universality of threshold corrections ensures that, in such situations, the stable minimum will have consistent... | 15.9259 | 17.511362 | 16.72142 | 16.073633 | 16.663073 | 16.140238 | 17.80966 | 16.674843 | 16.328421 | 17.97261 | 16.042496 | 15.908 | 15.520703 | 15.767077 | 15.883562 | 15.853274 | 15.734959 | 15.71436 | 15.692672 | 16.289845 | 15.785712 |
hep-th/0109113 | Zupnik B. M. | B.M. Zupnik | Static BPS-conditions in N=2 harmonic superspace | Latex file 4 pages, talk at the conference SUSY01, Dubna, June 11-17,
2001 | null | 10.1142/9789812778192_0080 | null | hep-th | null | We analyze superfield representations of BPS-conditions for the self-dual
static solutions of D=4, N=2 supersymmetric Yang-Mills theory.
| [
{
"created": "Fri, 14 Sep 2001 07:49:34 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Zupnik",
"B. M.",
""
]
] | We analyze superfield representations of BPS-conditions for the self-dual static solutions of D=4, N=2 supersymmetric Yang-Mills theory. | 13.713039 | 8.709068 | 10.209559 | 8.082168 | 8.715929 | 8.529539 | 9.643145 | 8.664135 | 7.18235 | 12.889612 | 8.018354 | 9.035044 | 12.3846 | 9.110919 | 8.736687 | 8.920572 | 9.074674 | 8.962482 | 9.448688 | 11.523105 | 8.171181 |
hep-th/0512011 | Terry Gannon | P. Bantay and T. Gannon | Conformal characters and the modular representation | 17 pages | JHEP0602:005,2006 | 10.1088/1126-6708/2006/02/005 | null | hep-th math.NT math.QA | null | A general procedure is presented to determine, given any suitable
representation of the modular group, the characters of all possible Rational
Conformal Field Theories whose associated modular representation is the given
one. The relevant ideas and methods are illustrated on two non-trivial
examples: the Yang-Lee and... | [
{
"created": "Thu, 1 Dec 2005 15:17:57 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Bantay",
"P.",
""
],
[
"Gannon",
"T.",
""
]
] | A general procedure is presented to determine, given any suitable representation of the modular group, the characters of all possible Rational Conformal Field Theories whose associated modular representation is the given one. The relevant ideas and methods are illustrated on two non-trivial examples: the Yang-Lee and t... | 13.405428 | 8.116341 | 10.308887 | 8.223254 | 8.245198 | 8.785667 | 8.226484 | 9.570696 | 7.522231 | 10.970086 | 8.62104 | 8.861979 | 9.880269 | 8.805228 | 8.915176 | 9.278665 | 8.922213 | 8.938118 | 8.874178 | 9.877888 | 9.570745 |
hep-th/0612244 | Kazuo Ghoroku | Kazuo Ghoroku, Masafumi Ishihara and Akihiro Nakamura | Flavor quarks in AdS4 and gauge/gravity correspondence | 18 pages, 8 figures | Phys.Rev.D75:046005,2007 | 10.1103/PhysRevD.75.046005 | FIT HE - 06-03 | hep-th | null | The non-perturbative properties of the gauge theories in the AdS${}_4$ are
studied in the dual supergravity by including light flavor quarks, which are
introduced by a D7 brane embedding. Contrary to the cases of Minkowski and
dS${}_4$, the dilaton does not play any important dynamical role in the
AdS${}_4$ case, and... | [
{
"created": "Fri, 22 Dec 2006 02:15:24 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Ghoroku",
"Kazuo",
""
],
[
"Ishihara",
"Masafumi",
""
],
[
"Nakamura",
"Akihiro",
""
]
] | The non-perturbative properties of the gauge theories in the AdS${}_4$ are studied in the dual supergravity by including light flavor quarks, which are introduced by a D7 brane embedding. Contrary to the cases of Minkowski and dS${}_4$, the dilaton does not play any important dynamical role in the AdS${}_4$ case, and t... | 9.297273 | 9.612002 | 10.161999 | 8.659926 | 9.358359 | 9.660929 | 9.429262 | 9.406392 | 8.81235 | 9.722119 | 8.899914 | 8.878748 | 9.279977 | 8.809156 | 8.904819 | 9.029066 | 9.136709 | 8.880616 | 8.857534 | 9.534958 | 8.653237 |
hep-th/9402153 | Juergen Fuchs | J\"urgen Fuchs, Alexander Ganchev, and Peter Vecserny\'es | Towards a classification of rational Hopf algebras | 35 pages | null | null | NIKHEF-H/94-05 and KL-TH-94/4 | hep-th math.QA | null | Rational Hopf algebras (certain quasitriangular weak quasi-Hopf
$^*$-algebras) are expected to describe the quantum symmetry of rational field
theories. In this paper methods are developped which allow for a classification
of all rational Hopf algebras that are compatible with some prescribed set of
fusion rules. The... | [
{
"created": "Mon, 28 Feb 1994 17:28:20 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Fuchs",
"Jürgen",
""
],
[
"Ganchev",
"Alexander",
""
],
[
"Vecsernyés",
"Peter",
""
]
] | Rational Hopf algebras (certain quasitriangular weak quasi-Hopf $^*$-algebras) are expected to describe the quantum symmetry of rational field theories. In this paper methods are developped which allow for a classification of all rational Hopf algebras that are compatible with some prescribed set of fusion rules. The a... | 7.271529 | 8.793695 | 8.490455 | 7.955092 | 7.294664 | 7.715077 | 7.778999 | 7.804692 | 7.376643 | 8.786867 | 7.534622 | 6.951139 | 7.354531 | 6.871325 | 6.87616 | 7.025718 | 6.920314 | 6.932247 | 6.810725 | 7.236341 | 7.200689 |
2402.12924 | Eunwoo Lee | Seunggyu Kim and Eunwoo Lee | Holographic Tests for Giant Graviton Expansion | 23+10 pages, 4 figures, 1 table, JHEP style | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | It has been proposed that the superconformal index admits a novel
reformulation, called giant graviton expansion. In this paper, we investigate
the properties of dual $AdS_5$ black holes using the giant graviton expansion
framework. First, we compute the entropy of black holes in $AdS_5\times S^5$
with fixed charges ... | [
{
"created": "Tue, 20 Feb 2024 11:19:12 GMT",
"version": "v1"
}
] | 2024-02-21 | [
[
"Kim",
"Seunggyu",
""
],
[
"Lee",
"Eunwoo",
""
]
] | It has been proposed that the superconformal index admits a novel reformulation, called giant graviton expansion. In this paper, we investigate the properties of dual $AdS_5$ black holes using the giant graviton expansion framework. First, we compute the entropy of black holes in $AdS_5\times S^5$ with fixed charges th... | 6.89493 | 6.00954 | 7.337247 | 6.333958 | 6.027362 | 6.008348 | 6.188323 | 6.194548 | 6.201474 | 8.085084 | 6.100036 | 6.492904 | 6.979987 | 6.489742 | 6.463665 | 6.492989 | 6.599156 | 6.261245 | 6.471455 | 6.983643 | 6.380114 |
1110.6720 | Ming Yu | Jian-feng Wu, Ming Yu | Calogero-Sutherland model in interacting fermion picture and explicit
construction of Jack states | 4 pages, 0 figures, abstract modified, references changed, typo
corrected | null | null | null | hep-th cond-mat.str-el math-ph math.MP | http://creativecommons.org/licenses/by/3.0/ | The 40-year-old Calogero-Sutherland (CS) model remains a source of
inspirations for understanding 1d interacting fermions. At $\beta=1,
\text{or}0$, the CS model describes a free non-relativistic fermion, or boson
theory, while for generic $\beta$, the system can be interpreted either as
interacting fermions or boson... | [
{
"created": "Mon, 31 Oct 2011 08:46:39 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Nov 2011 04:42:20 GMT",
"version": "v2"
}
] | 2011-11-07 | [
[
"Wu",
"Jian-feng",
""
],
[
"Yu",
"Ming",
""
]
] | The 40-year-old Calogero-Sutherland (CS) model remains a source of inspirations for understanding 1d interacting fermions. At $\beta=1, \text{or}0$, the CS model describes a free non-relativistic fermion, or boson theory, while for generic $\beta$, the system can be interpreted either as interacting fermions or bosons,... | 10.860682 | 11.38048 | 11.104289 | 10.231615 | 11.03971 | 11.303816 | 11.861449 | 10.872264 | 10.423909 | 11.614791 | 9.954653 | 10.439265 | 10.775394 | 10.127687 | 10.137436 | 9.979872 | 10.379854 | 10.357505 | 10.098022 | 10.536707 | 9.686402 |
hep-th/0410168 | Don Marolf | Donald Marolf | A few words on Entropy, Thermodynamics, and Horizons | 20 pages, for the Proceedings of the GR17 conference, Dublin,
Ireland, July 2004 | null | 10.1142/9789812701688_0008 | null | hep-th gr-qc quant-ph | null | We review recent progress in understanding certain aspects of the
thermodynamics of black holes and other horizons. Our discussion centers on
various ``entropy bounds'' which have been proposed in the literature and on
the current understanding of how such bounds are {\it not} required for the
semi-classical consiste... | [
{
"created": "Thu, 14 Oct 2004 18:15:49 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Oct 2004 17:52:31 GMT",
"version": "v2"
}
] | 2017-08-23 | [
[
"Marolf",
"Donald",
""
]
] | We review recent progress in understanding certain aspects of the thermodynamics of black holes and other horizons. Our discussion centers on various ``entropy bounds'' which have been proposed in the literature and on the current understanding of how such bounds are {\it not} required for the semi-classical consistenc... | 11.570993 | 12.216368 | 11.472883 | 11.239878 | 12.492707 | 12.271259 | 12.197933 | 11.90067 | 11.468529 | 12.790726 | 11.681452 | 10.894338 | 11.270983 | 10.665247 | 10.900631 | 11.102205 | 11.210051 | 10.869892 | 11.044622 | 11.091124 | 10.891723 |
1607.03897 | Diego Regalado | Pierre Corvilain, Thomas W. Grimm, Diego Regalado | Shift-symmetries and gauge coupling functions in orientifolds and
F-theory | 48 pages. v2: minor corrections | null | 10.1007/JHEP05(2017)059 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the field dependence of the gauge coupling functions of
four-dimensional Type IIB orientifold and F-theory compactifications with
space-time filling seven-branes. In particular, we analyze the constraints
imposed by holomorphicity and covariance under shift-symmetries of the bulk and
brane axions. This... | [
{
"created": "Wed, 13 Jul 2016 20:00:02 GMT",
"version": "v1"
},
{
"created": "Mon, 22 May 2017 13:21:25 GMT",
"version": "v2"
}
] | 2017-06-07 | [
[
"Corvilain",
"Pierre",
""
],
[
"Grimm",
"Thomas W.",
""
],
[
"Regalado",
"Diego",
""
]
] | We investigate the field dependence of the gauge coupling functions of four-dimensional Type IIB orientifold and F-theory compactifications with space-time filling seven-branes. In particular, we analyze the constraints imposed by holomorphicity and covariance under shift-symmetries of the bulk and brane axions. This r... | 8.869527 | 9.01996 | 10.480652 | 8.969291 | 9.313202 | 9.444483 | 9.038078 | 8.989267 | 8.646279 | 11.196546 | 8.800834 | 8.560996 | 9.389177 | 8.732175 | 8.496298 | 8.327759 | 8.60258 | 8.598758 | 8.599803 | 9.520088 | 8.485272 |
hep-th/0511092 | Holger Gies | Holger Gies and Klaus Klingmuller | Quantum energies with worldline numerics | 8 pages, 2 figures, Submitted to the Proceedings of the Seventh
Workshop QFEXT'05 (Barcelona, September 5-9, 2005), Refs updated, version to
appear in JPhysA | J.Phys.A39:6415-6422,2006 | 10.1088/0305-4470/39/21/S36 | HD-THEP-05-25 | hep-th quant-ph | null | We present new results for Casimir forces between rigid bodies which impose
Dirichlet boundary conditions on a fluctuating scalar field. As a universal
computational tool, we employ worldline numerics which builds on a combination
of the string-inspired worldline approach with Monte-Carlo techniques.
Worldline numeri... | [
{
"created": "Tue, 8 Nov 2005 14:47:45 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Mar 2006 10:45:09 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Gies",
"Holger",
""
],
[
"Klingmuller",
"Klaus",
""
]
] | We present new results for Casimir forces between rigid bodies which impose Dirichlet boundary conditions on a fluctuating scalar field. As a universal computational tool, we employ worldline numerics which builds on a combination of the string-inspired worldline approach with Monte-Carlo techniques. Worldline numerics... | 10.8647 | 9.838796 | 13.702108 | 10.005657 | 12.634975 | 10.622025 | 11.129609 | 10.623576 | 9.79005 | 13.388519 | 10.833715 | 11.016413 | 10.820462 | 10.367781 | 10.774113 | 10.72747 | 10.347878 | 10.319848 | 10.749038 | 10.841913 | 10.706712 |
2211.05147 | Andrea Olzi | Francesco Bigazzi, Aldo L. Cotrone, Andrea Olzi | Hall Droplet Sheets in Holographic QCD | minor improvements | null | 10.1007/JHEP02(2023)194 | null | hep-th hep-ph nucl-th | http://creativecommons.org/licenses/by/4.0/ | In single-flavor QCD, the low energy description of baryons as Skyrmions is
not available. In this case, it has been proposed by Komargodski that baryons
can be viewed as kinds of charged quantum Hall droplets, or "sheets". In this
paper we propose a string theory description of the sheets in single-flavor
holographi... | [
{
"created": "Wed, 9 Nov 2022 19:00:19 GMT",
"version": "v1"
},
{
"created": "Thu, 18 May 2023 10:51:38 GMT",
"version": "v2"
}
] | 2023-05-19 | [
[
"Bigazzi",
"Francesco",
""
],
[
"Cotrone",
"Aldo L.",
""
],
[
"Olzi",
"Andrea",
""
]
] | In single-flavor QCD, the low energy description of baryons as Skyrmions is not available. In this case, it has been proposed by Komargodski that baryons can be viewed as kinds of charged quantum Hall droplets, or "sheets". In this paper we propose a string theory description of the sheets in single-flavor holographic ... | 9.537898 | 8.932747 | 9.651406 | 9.196285 | 9.64889 | 9.674481 | 9.570912 | 9.596531 | 9.043588 | 10.218528 | 9.068838 | 9.167271 | 9.550392 | 9.275889 | 9.326299 | 9.229371 | 9.128279 | 8.917245 | 8.959037 | 9.347374 | 9.049113 |
1406.3038 | Shamik Banerjee | Shamik Banerjee | Note On The Dilaton Effective Action And Entanglement Entropy | Latex, 9 Pages | null | null | null | hep-th cond-mat.stat-mech cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we do the analysis of entanglement entropy more carefully when
the non-conformal theory flows to a non-trivial IR fixed point. In particular
we emphasize the role of the trace of the energy-momentum tensor in these
calculations. We also compare the current technique for evaluating the
entanglement entrop... | [
{
"created": "Wed, 11 Jun 2014 20:01:09 GMT",
"version": "v1"
}
] | 2014-07-02 | [
[
"Banerjee",
"Shamik",
""
]
] | In this note we do the analysis of entanglement entropy more carefully when the non-conformal theory flows to a non-trivial IR fixed point. In particular we emphasize the role of the trace of the energy-momentum tensor in these calculations. We also compare the current technique for evaluating the entanglement entropy,... | 10.180066 | 8.929442 | 9.737854 | 9.135481 | 9.483005 | 9.124878 | 8.977858 | 8.302587 | 8.709957 | 10.420195 | 8.583242 | 9.041127 | 9.455721 | 9.020568 | 9.181213 | 9.17712 | 9.284042 | 8.886219 | 9.326343 | 9.509381 | 8.833118 |
1307.1109 | Denis Dalmazi | D. Dalmazi | A note on the nonuniqueness of the massive Fierz-Pauli theory and
spectator fields | 9 pages, no figures | null | 10.1103/PhysRevD.88.045003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is possible to show that there are three independent families of models
describing a massive spin-2 particle via a rank-2 tensor. One of them contains
the massive Fierz-Pauli model, the only case described by a symmetric tensor.
The three families have different local symmetries in the massless limit and
can not b... | [
{
"created": "Wed, 3 Jul 2013 18:55:20 GMT",
"version": "v1"
}
] | 2013-08-14 | [
[
"Dalmazi",
"D.",
""
]
] | It is possible to show that there are three independent families of models describing a massive spin-2 particle via a rank-2 tensor. One of them contains the massive Fierz-Pauli model, the only case described by a symmetric tensor. The three families have different local symmetries in the massless limit and can not be ... | 7.976504 | 7.3645 | 8.301171 | 7.516952 | 7.772799 | 7.801484 | 7.565318 | 7.522768 | 7.32052 | 8.94768 | 7.569065 | 7.372561 | 7.816954 | 7.417465 | 7.466535 | 7.370749 | 7.361317 | 7.227871 | 7.455489 | 7.883831 | 7.214128 |
1810.13217 | Ritabrata Bhattacharya | Ritabrata Bhattacharya, Dileep P. Jatkar, Arnab Kundu | Chaotic Correlation Functions with Complex Fermions | 22 pages, 7 figures, numerical calculations improved, 2 time-fold and
3 time-fold OTO correlators computed | SciPost Phys. Core 4, 018 (2021) | 10.21468/SciPostPhysCore.4.2.018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study correlation functions in the complex fermion SYK model. We focus,
specifically, on the h = 2 mode which explicitly breaks conformal invariance
and exhibits the chaotic behaviour. We explicitly compute fermion six-point
function and extract the corresponding six-point OTOC which exhibits an
exponential growth... | [
{
"created": "Wed, 31 Oct 2018 11:10:32 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Jan 2019 05:46:02 GMT",
"version": "v2"
},
{
"created": "Sun, 6 Dec 2020 07:46:42 GMT",
"version": "v3"
},
{
"created": "Mon, 22 Feb 2021 05:53:05 GMT",
"version": "v4"
}
] | 2022-03-28 | [
[
"Bhattacharya",
"Ritabrata",
""
],
[
"Jatkar",
"Dileep P.",
""
],
[
"Kundu",
"Arnab",
""
]
] | We study correlation functions in the complex fermion SYK model. We focus, specifically, on the h = 2 mode which explicitly breaks conformal invariance and exhibits the chaotic behaviour. We explicitly compute fermion six-point function and extract the corresponding six-point OTOC which exhibits an exponential growth w... | 17.62855 | 18.386223 | 20.249702 | 16.606207 | 16.531345 | 19.582575 | 17.731033 | 16.184401 | 16.25004 | 23.54195 | 15.471861 | 16.028067 | 17.894482 | 15.871622 | 16.32449 | 15.940354 | 15.960335 | 16.568525 | 16.132088 | 17.792467 | 15.92129 |
1212.4831 | I\~naki Garc\'ia-Etxebarria | I\~naki Garc\'ia-Etxebarria, Hirotaka Hayashi, Raffaele Savelli and
Gary Shiu | On quantum corrected K\"ahler potentials in F-theory | 57 pages, 2 figures. v2: Added references, version to appear in JHEP | null | null | CERN-PH-TH/2012-359, MAD-TH-12-09, MPP-2012-185, KIAS P-12085 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We work out the exact in string coupling and perturbatively exact in \alpha'
result for the vector multiplet moduli K\"ahler potential in a specific N=2
compactification of F-theory. The well-known correction cubic in \alpha' is
absent, but there is a rich structure of corrections at all even orders in
\alpha'. Moreo... | [
{
"created": "Wed, 19 Dec 2012 21:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Mar 2013 18:49:13 GMT",
"version": "v2"
}
] | 2013-03-21 | [
[
"García-Etxebarria",
"Iñaki",
""
],
[
"Hayashi",
"Hirotaka",
""
],
[
"Savelli",
"Raffaele",
""
],
[
"Shiu",
"Gary",
""
]
] | We work out the exact in string coupling and perturbatively exact in \alpha' result for the vector multiplet moduli K\"ahler potential in a specific N=2 compactification of F-theory. The well-known correction cubic in \alpha' is absent, but there is a rich structure of corrections at all even orders in \alpha'. Moreove... | 11.287856 | 10.008949 | 10.808267 | 9.182263 | 9.801985 | 9.973915 | 9.705599 | 10.252886 | 9.218476 | 11.482802 | 9.525804 | 9.523927 | 10.158787 | 9.388184 | 9.574621 | 9.461158 | 9.407971 | 9.297696 | 9.781213 | 10.22772 | 9.490616 |
1911.06339 | Jonathan Sorce | Sean Colin-Ellerin, Veronika E. Hubeny, Benjamin E. Niehoff, Jonathan
Sorce | Large-$d$ phase transitions in holographic mutual information | 35 pages, 12 figures | JHEP 2020, 173 (2020) | 10.1007/JHEP04(2020)173 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the AdS/CFT correspondence, the entanglement entropy of subregions in the
boundary CFT is conjectured to be dual to the area of a bulk extremal surface
at leading order in $G_N$ in the holographic limit. Under this dictionary,
distantly separated regions in the CFT vacuum state have zero mutual
information at lead... | [
{
"created": "Thu, 14 Nov 2019 19:00:06 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Apr 2020 16:37:01 GMT",
"version": "v2"
},
{
"created": "Sun, 3 May 2020 17:18:54 GMT",
"version": "v3"
}
] | 2020-05-05 | [
[
"Colin-Ellerin",
"Sean",
""
],
[
"Hubeny",
"Veronika E.",
""
],
[
"Niehoff",
"Benjamin E.",
""
],
[
"Sorce",
"Jonathan",
""
]
] | In the AdS/CFT correspondence, the entanglement entropy of subregions in the boundary CFT is conjectured to be dual to the area of a bulk extremal surface at leading order in $G_N$ in the holographic limit. Under this dictionary, distantly separated regions in the CFT vacuum state have zero mutual information at leadin... | 7.900504 | 7.688415 | 8.20313 | 7.576045 | 7.82151 | 7.920078 | 7.498643 | 7.762692 | 7.683141 | 9.785202 | 7.461376 | 7.437112 | 7.756904 | 7.433072 | 7.579192 | 7.850731 | 7.652188 | 7.587675 | 7.642897 | 8.022866 | 7.561443 |
1706.01725 | Nicholas Halmagyi | Nick Halmagyi, Dan Israel, Matthieu Sarkis and Eirik Eik Svanes | Heterotic Hyper-Kahler Flux Backgrounds | 19 pages | null | 10.1007/JHEP08(2017)138 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study Heterotic supergravity on Hyper-Kahler manifolds in the presence of
non-trivial warping and three form flux with Abelian bundles in the large
charge limit. We find exact, regular solutions for multi-centered
Gibbons-Hawking spaces and Atiyah-Hitchin manifolds. In the case of
Atiyah-Hitchin, regularity requir... | [
{
"created": "Tue, 6 Jun 2017 12:19:36 GMT",
"version": "v1"
}
] | 2017-09-20 | [
[
"Halmagyi",
"Nick",
""
],
[
"Israel",
"Dan",
""
],
[
"Sarkis",
"Matthieu",
""
],
[
"Svanes",
"Eirik Eik",
""
]
] | We study Heterotic supergravity on Hyper-Kahler manifolds in the presence of non-trivial warping and three form flux with Abelian bundles in the large charge limit. We find exact, regular solutions for multi-centered Gibbons-Hawking spaces and Atiyah-Hitchin manifolds. In the case of Atiyah-Hitchin, regularity requires... | 10.830985 | 10.139948 | 12.687717 | 10.090381 | 10.476653 | 11.591805 | 10.809806 | 9.903755 | 9.59886 | 15.493368 | 10.06198 | 10.650599 | 11.321488 | 10.548767 | 10.24017 | 10.292669 | 10.633804 | 10.175229 | 10.264725 | 11.374195 | 10.277225 |
hep-th/0205276 | J. F. Vazquez-Poritz | J. Gegenberg, S. Vaidya and J.F. Vazquez-Poritz | Thurston Geometries from Eleven Dimensions | Latex, 8 pages, improved presentation in abstract, introduction and
section 2, references added | Class.Quant.Grav. 19 (2002) L199-L204 | 10.1088/0264-9381/19/23/102 | null | hep-th gr-qc math-ph math.GT math.MP | null | In three dimensions, a `master theory' for all Thurston geometries requires
imaginary flux. However, these geometries can be obtained from physical
three-dimensional theories with various additional scalar fields, which can be
interpreted as moduli in various compactifications of a higher-dimensional
`master theory'.... | [
{
"created": "Mon, 27 May 2002 10:10:25 GMT",
"version": "v1"
},
{
"created": "Fri, 7 Jun 2002 08:55:42 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Sep 2002 09:56:58 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Gegenberg",
"J.",
""
],
[
"Vaidya",
"S.",
""
],
[
"Vazquez-Poritz",
"J. F.",
""
]
] | In three dimensions, a `master theory' for all Thurston geometries requires imaginary flux. However, these geometries can be obtained from physical three-dimensional theories with various additional scalar fields, which can be interpreted as moduli in various compactifications of a higher-dimensional `master theory'. T... | 10.923635 | 10.980438 | 11.544325 | 10.207706 | 10.398347 | 10.470949 | 11.057916 | 10.423388 | 10.023199 | 12.012498 | 9.738351 | 10.201355 | 10.745509 | 10.850773 | 10.176537 | 10.330446 | 10.233809 | 10.375805 | 10.743234 | 11.16963 | 10.052245 |
1902.06571 | Hiroyuki Kitamoto | Hiroyuki Kitamoto, Yoshihisa Kitazawa | Entropy Generation at the Horizon Diffuses Cosmological Constant in 2D
de Sitter Space | 37 pages, matches published version | Phys. Rev. D 99, 085015 (2019) | 10.1103/PhysRevD.99.085015 | KEK-TH-2102, NCTS-TH/1902 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a solution of the exactly renormalized Liouville action to
foresee the fate of the two-dimensional de Sitter space. We work in the
semiclassical region with a large matter central charge $c$. Instead of de
Sitter expansion, it performs a slow-roll inflation with the parameters
$\epsilon=(1/2)\eta =6/c$... | [
{
"created": "Mon, 18 Feb 2019 13:55:36 GMT",
"version": "v1"
},
{
"created": "Wed, 1 May 2019 02:03:24 GMT",
"version": "v2"
}
] | 2019-05-02 | [
[
"Kitamoto",
"Hiroyuki",
""
],
[
"Kitazawa",
"Yoshihisa",
""
]
] | We investigate a solution of the exactly renormalized Liouville action to foresee the fate of the two-dimensional de Sitter space. We work in the semiclassical region with a large matter central charge $c$. Instead of de Sitter expansion, it performs a slow-roll inflation with the parameters $\epsilon=(1/2)\eta =6/c$. ... | 16.006094 | 16.236053 | 15.943258 | 14.719681 | 15.531802 | 16.27281 | 15.183978 | 15.815132 | 14.655017 | 18.670393 | 15.291354 | 15.542593 | 15.574033 | 15.984532 | 15.6936 | 15.972493 | 16.306278 | 15.839079 | 16.073881 | 16.343008 | 15.588837 |
hep-th/0210293 | Dmitri Antonov | D. Antonov (INFN, Pisa & Pisa U.) | Higgs- and quark-inspired modifications of the finite-temperature
properties of the Polyakov model | 4 pages, LaTeX2e, no figures, uses espcrc2.sty, submitted to Nucl.
Phys. B (Proc. Suppl.) | Nucl.Phys.Proc.Suppl.121:301-304,2003 | 10.1016/S0920-5632(03)01866-8 | IFUP-TH 2002/41 | hep-th | null | (2+1)-dimensional Georgi-Glashow model, else called the Polyakov model, is
explored at nonzero temperatures and in the regime when the Higgs boson is not
infinitely heavy. The finiteness of the Higgs-boson mass leads to the
appearance of the upper bound on the parameter of the weak-coupling
approximation, necessary t... | [
{
"created": "Wed, 30 Oct 2002 17:16:55 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Mar 2003 15:51:05 GMT",
"version": "v2"
}
] | 2010-12-09 | [
[
"Antonov",
"D.",
"",
"INFN, Pisa & Pisa U."
]
] | (2+1)-dimensional Georgi-Glashow model, else called the Polyakov model, is explored at nonzero temperatures and in the regime when the Higgs boson is not infinitely heavy. The finiteness of the Higgs-boson mass leads to the appearance of the upper bound on the parameter of the weak-coupling approximation, necessary to ... | 10.963071 | 9.592109 | 11.155642 | 9.907545 | 10.06686 | 10.222554 | 10.348001 | 10.869773 | 9.198427 | 11.280676 | 9.62879 | 9.756259 | 10.184533 | 9.838579 | 9.871733 | 10.033514 | 10.386968 | 10.119427 | 9.922615 | 10.063086 | 9.856908 |
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