id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9807206 | Renata Kallosh | Renata Kallosh | Superconformal Actions in Killing Gauge | 9 pages, Latex | null | null | SU-ITP-98-46 | hep-th | null | The classical superconformal actions of branes in adS superspaces have a
closed form depending on a matrix $M^2$ quadratic in fermions, as found in
hep-th/9805217. One can gauge-fix the local $\kappa$-symmetry using the Killing
spinors of the brane in the bulk. We show that in such gauges the
superconformal actions a... | [
{
"created": "Tue, 28 Jul 1998 23:45:19 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kallosh",
"Renata",
""
]
] | The classical superconformal actions of branes in adS superspaces have a closed form depending on a matrix $M^2$ quadratic in fermions, as found in hep-th/9805217. One can gauge-fix the local $\kappa$-symmetry using the Killing spinors of the brane in the bulk. We show that in such gauges the superconformal actions are... | 10.706853 | 9.167142 | 11.232973 | 9.657299 | 10.534836 | 9.695615 | 10.241545 | 10.255053 | 10.341881 | 12.266413 | 10.603538 | 9.396861 | 11.009934 | 9.995086 | 9.490085 | 9.831836 | 9.744247 | 9.839194 | 9.430438 | 10.805412 | 9.851039 |
hep-th/0202190 | Machiko Hatsuda | Machiko Hatsuda, Kiyoshi Kamimura and Makoto Sakaguchi | From Super-AdS_5xS^5 Algebra to Super-pp-wave Algebra | 7 pages, Latex file, references added | Nucl.Phys. B632 (2002) 114-120 | 10.1016/S0550-3213(02)00258-4 | null | hep-th | null | The isometry algebras of the maximally supersymmetric solutions of IIB
supergravity are derived by the Inonu-Wigner contractions of the
super-AdS_5xS^5 algebra. The super-AdS_5xS^5 algebra allows introducing two
contraction parameters; the one for the Penrose limit to the maximally
supersymmetric pp-wave algebra and ... | [
{
"created": "Wed, 27 Feb 2002 09:28:12 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Mar 2002 01:16:46 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Hatsuda",
"Machiko",
""
],
[
"Kamimura",
"Kiyoshi",
""
],
[
"Sakaguchi",
"Makoto",
""
]
] | The isometry algebras of the maximally supersymmetric solutions of IIB supergravity are derived by the Inonu-Wigner contractions of the super-AdS_5xS^5 algebra. The super-AdS_5xS^5 algebra allows introducing two contraction parameters; the one for the Penrose limit to the maximally supersymmetric pp-wave algebra and th... | 7.631936 | 6.536097 | 6.882115 | 6.228887 | 6.948355 | 6.137166 | 6.291881 | 6.184189 | 6.095697 | 8.214065 | 6.547074 | 6.458385 | 7.031883 | 6.387853 | 6.862831 | 6.582136 | 6.33952 | 6.414873 | 6.496666 | 6.858892 | 6.29733 |
2007.15760 | Daniel Medina Rincon | Li Botao and Daniel Medina-Rincon | On precision holography for the circular Wilson loop in $AdS_{5}\times
S^{5}$ | 7 pages, published version | null | 10.1016/j.physletb.2020.135789 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The string theory calculation of the 1/2-BPS circular Wilson loop of N=4 SYM
in the planar limit at next to leading order at strong coupling is revisited in
the ratio of its semiclassical string partition function and the one dual to a
latitude Wilson loop with trivial expectation value. After applying a conformal
tr... | [
{
"created": "Thu, 30 Jul 2020 22:24:19 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Oct 2020 17:26:28 GMT",
"version": "v2"
}
] | 2020-10-02 | [
[
"Botao",
"Li",
""
],
[
"Medina-Rincon",
"Daniel",
""
]
] | The string theory calculation of the 1/2-BPS circular Wilson loop of N=4 SYM in the planar limit at next to leading order at strong coupling is revisited in the ratio of its semiclassical string partition function and the one dual to a latitude Wilson loop with trivial expectation value. After applying a conformal tran... | 13.41007 | 13.093119 | 14.61286 | 12.380341 | 14.060316 | 13.711611 | 14.284335 | 11.598702 | 13.220271 | 15.454892 | 12.550447 | 11.910284 | 13.24781 | 12.244378 | 12.627811 | 12.464367 | 12.817187 | 12.246165 | 12.220644 | 13.244298 | 12.231202 |
2310.20698 | Andrea Leonardo Guerrieri | Adwait Gaikwad, Victor Gorbenko, Andrea L. Guerrieri | QCD Worldsheet Axion from the Bootstrap | 33 pages, 11 figures, v3: typos corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The worldsheet axion plays a crucial role in the dynamics of the Yang-Mills
confining flux tubes. According to the lattice measurements, its mass is of
order the string tension and its coupling is close to a certain critical value.
Using the S-matrix Bootstrap, we construct non-perturbative $2 \to 2$ branon
scatterin... | [
{
"created": "Tue, 31 Oct 2023 17:57:25 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Nov 2023 12:21:34 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Dec 2023 15:46:07 GMT",
"version": "v3"
}
] | 2023-12-29 | [
[
"Gaikwad",
"Adwait",
""
],
[
"Gorbenko",
"Victor",
""
],
[
"Guerrieri",
"Andrea L.",
""
]
] | The worldsheet axion plays a crucial role in the dynamics of the Yang-Mills confining flux tubes. According to the lattice measurements, its mass is of order the string tension and its coupling is close to a certain critical value. Using the S-matrix Bootstrap, we construct non-perturbative $2 \to 2$ branon scattering ... | 12.720512 | 10.406929 | 11.890253 | 11.479584 | 11.716848 | 11.723404 | 11.747663 | 11.600137 | 11.028496 | 11.649551 | 11.736955 | 11.513035 | 11.822836 | 11.538827 | 11.398372 | 11.412068 | 11.080052 | 11.855149 | 11.498233 | 11.69887 | 11.026687 |
0807.4635 | Wolfgang Schleifenbaum | H. Reinhardt, D. Campagnari, D. Epple, M. Leder, M. Pak and W.
Schleifenbaum | Coulomb gauge Yang-Mills theory in the Hamiltonian approach | 8 pages, 9 figures, Invited talk given by H. Reinhardt at the
international conference on "Selected Problems in Theoretical Physics, Dubna
23-27 June 2008" | null | null | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Within the Hamiltonian approach in Coulomb gauge the ghost and gluon
propagators are determined from a variational solution of the Yang-Mills
Schroedinger equation showing both gluon and heavy quark confinement. The
continuum results are in good agreement with lattice data. The ghost form
factor is identified as the ... | [
{
"created": "Tue, 29 Jul 2008 11:31:52 GMT",
"version": "v1"
}
] | 2008-07-31 | [
[
"Reinhardt",
"H.",
""
],
[
"Campagnari",
"D.",
""
],
[
"Epple",
"D.",
""
],
[
"Leder",
"M.",
""
],
[
"Pak",
"M.",
""
],
[
"Schleifenbaum",
"W.",
""
]
] | Within the Hamiltonian approach in Coulomb gauge the ghost and gluon propagators are determined from a variational solution of the Yang-Mills Schroedinger equation showing both gluon and heavy quark confinement. The continuum results are in good agreement with lattice data. The ghost form factor is identified as the di... | 8.159753 | 6.870107 | 7.279724 | 6.489485 | 7.711581 | 6.649123 | 6.784546 | 7.47296 | 6.467537 | 7.301073 | 6.65797 | 7.156681 | 7.352531 | 6.90828 | 7.858175 | 7.262035 | 7.227167 | 7.389997 | 7.168531 | 7.277504 | 6.909721 |
hep-th/9705178 | Physic | Fuad M. Saradzhev | Generalised chiral QED2 : Anomaly and Exotic Statistics | LATEX file, 36 pp., to appear in Phys.Rev. D | Phys.Rev. D56 (1997) 1055-1072 | 10.1103/PhysRevD.56.1055 | null | hep-th | null | We study the influence of the anomaly on the physical quantum picture of the
generalized chiral Schwinger model defined on the circle. We show that the
anomaly i) results in the background linearly rising electric field and ii)
makes the spectrum of the physical Hamiltonian nonrelativistic without a
massive boson. Th... | [
{
"created": "Fri, 23 May 1997 08:24:40 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Saradzhev",
"Fuad M.",
""
]
] | We study the influence of the anomaly on the physical quantum picture of the generalized chiral Schwinger model defined on the circle. We show that the anomaly i) results in the background linearly rising electric field and ii) makes the spectrum of the physical Hamiltonian nonrelativistic without a massive boson. The ... | 11.738312 | 8.917734 | 12.113926 | 10.735559 | 10.731468 | 10.180153 | 10.182718 | 10.048852 | 10.568032 | 12.38243 | 10.303384 | 10.295359 | 11.446061 | 10.999183 | 10.863716 | 10.585427 | 10.98278 | 10.886886 | 11.029042 | 11.731147 | 10.98254 |
2405.09608 | Carolina Figueiredo | Nima Arkani-Hamed, Carolina Figueiredo | All-order splits and multi-soft limits for particle and string
amplitudes | 59 pages, 17 figures | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The most important aspects of scattering amplitudes have long been thought to
be associated with their poles. But recently a very different sort of "split"
factorizations for a wide range of particle and string tree amplitudes have
been discovered away from poles. In this paper, we give a simple, conceptual
origin fo... | [
{
"created": "Wed, 15 May 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-05-17 | [
[
"Arkani-Hamed",
"Nima",
""
],
[
"Figueiredo",
"Carolina",
""
]
] | The most important aspects of scattering amplitudes have long been thought to be associated with their poles. But recently a very different sort of "split" factorizations for a wide range of particle and string tree amplitudes have been discovered away from poles. In this paper, we give a simple, conceptual origin for ... | 15.910404 | 14.708243 | 16.575214 | 13.626006 | 15.222085 | 14.682282 | 14.560951 | 14.74251 | 14.262069 | 17.178133 | 14.118385 | 14.063374 | 14.927229 | 14.311978 | 13.803729 | 14.234879 | 14.264266 | 14.100405 | 14.337306 | 15.475569 | 13.697535 |
hep-th/9702163 | null | A.A. Tseytlin | Composite BPS configurations of p-branes in 10 and 11 dimensions | 28 pages, harvmac. Misprints corrected, version to appear in
Classical and Quantum Gravity | Class.Quant.Grav.14:2085-2105,1997 | 10.1088/0264-9381/14/8/009 | Imperial/TP/96-97/25 | hep-th | null | We give an overview of various composite BPS configurations of string theory
and M-theory p-branes represented as classical supergravity solutions. Type II
string backgrounds can be obtained by S- and T- dualities from NS-NS string -
5-brane configurations corresponding to exact conformal sigma models. The
single-cen... | [
{
"created": "Mon, 24 Feb 1997 00:26:41 GMT",
"version": "v1"
},
{
"created": "Thu, 22 May 1997 19:53:53 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Tseytlin",
"A. A.",
""
]
] | We give an overview of various composite BPS configurations of string theory and M-theory p-branes represented as classical supergravity solutions. Type II string backgrounds can be obtained by S- and T- dualities from NS-NS string - 5-brane configurations corresponding to exact conformal sigma models. The single-cente... | 10.079388 | 9.75071 | 11.819187 | 9.538853 | 9.932693 | 9.571359 | 9.757532 | 9.351317 | 9.999986 | 12.003543 | 9.312625 | 10.024554 | 10.396548 | 9.856343 | 10.034002 | 9.667537 | 9.908689 | 9.803834 | 9.922379 | 10.508601 | 9.674927 |
2304.14938 | Nishant Gupta | Nishant Gupta and Nemani V. Suryanarayana | All chiral ${\cal W}$-algebra extensions of $\mathfrak{so}(2,3)$ | Accepted for publication in JHEP. Elaborated introduction. Some
calculations in the main text shifted to Appendix. References added | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We show that there are four chiral ${\cal W}$-algebra extensions of
$\mathfrak{so}(2,3)$ algebra and construct them explicitly. We do this by a
simple identification of each of the inequivalent embeddings of a copy of
$\mathfrak{sl}(2,{\mathbb R})$ in the $\mathfrak{so}(2,3)$ algebra and the
maximal subalgebra $\math... | [
{
"created": "Fri, 28 Apr 2023 15:49:09 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Jul 2024 14:53:36 GMT",
"version": "v2"
}
] | 2024-07-25 | [
[
"Gupta",
"Nishant",
""
],
[
"Suryanarayana",
"Nemani V.",
""
]
] | We show that there are four chiral ${\cal W}$-algebra extensions of $\mathfrak{so}(2,3)$ algebra and construct them explicitly. We do this by a simple identification of each of the inequivalent embeddings of a copy of $\mathfrak{sl}(2,{\mathbb R})$ in the $\mathfrak{so}(2,3)$ algebra and the maximal subalgebra $\mathfr... | 5.610158 | 5.53713 | 5.613247 | 5.282572 | 5.682407 | 5.437108 | 5.729593 | 5.379154 | 5.278308 | 5.737535 | 5.308069 | 5.382532 | 5.588025 | 5.322723 | 5.398894 | 5.372035 | 5.328193 | 5.290101 | 5.324295 | 5.501346 | 5.32579 |
2307.04729 | Francesco Sciotti | Teng Ma, Alex Pomarol and Francesco Sciotti | Bootstrapping the Chiral Anomaly at Large $N_c$ | 20 pages, 1 figure. v2: bound on the anomaly generalised and typos
corrected | null | null | null | hep-th hep-lat hep-ph | http://creativecommons.org/licenses/by/4.0/ | The bootstrap approach (demanding consistency conditions to scattering
amplitudes) has shown to be quite powerful to tightly constrain gauge theories
at large $N_c$. We extend previous analysis to scattering amplitudes involving
pions and external gauge bosons. These amplitudes allow us to access the chiral
anomaly a... | [
{
"created": "Mon, 10 Jul 2023 17:38:43 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Jul 2023 16:20:32 GMT",
"version": "v2"
}
] | 2023-07-31 | [
[
"Ma",
"Teng",
""
],
[
"Pomarol",
"Alex",
""
],
[
"Sciotti",
"Francesco",
""
]
] | The bootstrap approach (demanding consistency conditions to scattering amplitudes) has shown to be quite powerful to tightly constrain gauge theories at large $N_c$. We extend previous analysis to scattering amplitudes involving pions and external gauge bosons. These amplitudes allow us to access the chiral anomaly and... | 13.360153 | 12.022733 | 11.668718 | 11.002377 | 12.441529 | 12.466794 | 11.759426 | 12.408848 | 10.319671 | 12.930476 | 11.955885 | 11.626874 | 11.685441 | 11.268489 | 11.969376 | 11.899195 | 11.307927 | 11.285433 | 11.089942 | 11.37219 | 11.062235 |
hep-th/0304232 | Ari Pankiewicz | Ari Pankiewicz | An alternative formulation of light-cone string field theory on the
plane wave | 28 pages; v2: minor changes | JHEP 0306 (2003) 047 | 10.1088/1126-6708/2003/06/047 | null | hep-th | null | We construct a manifestly SO(4) x SO(4) invariant, supersymmetric extension
of the closed string cubic interaction vertex and dynamical supercharges in
light-cone string field theory on the plane wave space-time. We find that the
effective vertex for states built out of bosonic creation oscillators coincides
with the... | [
{
"created": "Mon, 28 Apr 2003 09:28:40 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jun 2003 11:54:28 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Pankiewicz",
"Ari",
""
]
] | We construct a manifestly SO(4) x SO(4) invariant, supersymmetric extension of the closed string cubic interaction vertex and dynamical supercharges in light-cone string field theory on the plane wave space-time. We find that the effective vertex for states built out of bosonic creation oscillators coincides with the o... | 11.816929 | 11.067112 | 13.484962 | 10.407607 | 11.772561 | 10.801286 | 11.87464 | 10.068973 | 11.077223 | 13.972324 | 11.107991 | 10.577637 | 11.684363 | 10.971273 | 10.565609 | 10.885218 | 11.191408 | 10.711412 | 10.628846 | 12.392865 | 10.888052 |
hep-th/9303002 | Ulf Danielsson | Ulf H. Danielsson | Super Black Holes | 8 pages, CERN-TH.6817-93 | Phys.Lett. B307 (1993) 44-48 | 10.1016/0370-2693(93)90190-S | null | hep-th | null | A quantum version of 2D super dilaton gravity containing a black hole is
constructed for $N>8$. A previous disagreement as to whether this is possible
or not is resolved.
| [
{
"created": "Mon, 1 Mar 1993 11:57:13 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Danielsson",
"Ulf H.",
""
]
] | A quantum version of 2D super dilaton gravity containing a black hole is constructed for $N>8$. A previous disagreement as to whether this is possible or not is resolved. | 37.257099 | 23.520817 | 27.918591 | 19.700983 | 20.067675 | 20.51141 | 20.085125 | 21.144644 | 21.369661 | 30.007456 | 21.856438 | 21.285851 | 28.667128 | 22.699266 | 22.602087 | 22.515402 | 23.807539 | 22.187918 | 24.374262 | 26.009439 | 22.012793 |
1807.08882 | Yu Nakayama | Yu Nakayama | Gravity Dual for Very Special Conformal Field Theories in type IIB
Supergravity | 11 pages | null | 10.1016/j.physletb.2018.09.051 | RUP-18-24 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study holographic dual descriptions of very special conformal field
theories with the T(2) symmetry. After constructing solutions in effective five
dimensional Einstein gravity coupled with massive two-form fields, we uplift
them to the ten dimensional type IIB supergravity, via a consistent truncation
ansatz, to ... | [
{
"created": "Tue, 24 Jul 2018 02:18:44 GMT",
"version": "v1"
}
] | 2018-10-03 | [
[
"Nakayama",
"Yu",
""
]
] | We study holographic dual descriptions of very special conformal field theories with the T(2) symmetry. After constructing solutions in effective five dimensional Einstein gravity coupled with massive two-form fields, we uplift them to the ten dimensional type IIB supergravity, via a consistent truncation ansatz, to de... | 10.572952 | 10.871448 | 11.271387 | 9.174582 | 11.161254 | 10.558341 | 10.345655 | 10.689292 | 10.110038 | 12.457415 | 10.091678 | 10.20429 | 10.735611 | 9.858881 | 10.211244 | 9.990153 | 10.000429 | 9.643483 | 9.945645 | 10.683989 | 9.524431 |
1504.05537 | Matthew Dodelson | Matthew Dodelson and Eva Silverstein | Longitudinal nonlocality in the string S-matrix | 40 pages, 10 figures. v2: typos fixed | null | null | SLAC-PUB-16260,SU/ITP-15/04,NSF-KITP-15-047 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze four and five-point tree-level open string S-matrix amplitudes in
the Regge limit, exhibiting some basic features which indicate longitudinal
nonlocality, as suggested by light cone gauge calculations of string spreading.
Using wavepackets to localize the asymptotic states, we compute the peak
trajectories... | [
{
"created": "Tue, 21 Apr 2015 18:27:38 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Apr 2015 16:06:24 GMT",
"version": "v2"
}
] | 2015-05-01 | [
[
"Dodelson",
"Matthew",
""
],
[
"Silverstein",
"Eva",
""
]
] | We analyze four and five-point tree-level open string S-matrix amplitudes in the Regge limit, exhibiting some basic features which indicate longitudinal nonlocality, as suggested by light cone gauge calculations of string spreading. Using wavepackets to localize the asymptotic states, we compute the peak trajectories f... | 22.704792 | 23.944572 | 24.088858 | 22.723951 | 23.326538 | 22.496058 | 24.701191 | 23.999754 | 22.389969 | 27.165535 | 21.844894 | 22.76206 | 22.157356 | 21.229652 | 22.2694 | 21.958702 | 22.600794 | 21.508112 | 21.906797 | 22.80928 | 21.555937 |
hep-th/0208021 | D. Toublan | D. Toublan and J.J.M. Verbaarschot | Dirac Spectra and Real QCD at Nonzero Chemical Potential | 26 pages, 8 Postscript figures, Invited talk at Symposium and
Workshop "Continuous Advances in QCD 2002 / Arkadyfest", May 17-23, 2002 | null | 10.1142/9789812776310_0018 | SUNY-NTG-02/27 | hep-th cond-mat hep-lat hep-ph | null | We show that QCD Dirac spectra well below Lambda_{QCD}, both at zero and at
nonzero chemical potential, can be obtained from a chiral Lagrangian. At
nonzero chemical potential Goldstone bosons with nonzero baryon number condense
beyond a critical value. Such superfluid phase transition is likely to occur in
any syste... | [
{
"created": "Fri, 2 Aug 2002 21:46:33 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Toublan",
"D.",
""
],
[
"Verbaarschot",
"J. J. M.",
""
]
] | We show that QCD Dirac spectra well below Lambda_{QCD}, both at zero and at nonzero chemical potential, can be obtained from a chiral Lagrangian. At nonzero chemical potential Goldstone bosons with nonzero baryon number condense beyond a critical value. Such superfluid phase transition is likely to occur in any system ... | 9.688474 | 9.685273 | 8.935139 | 8.540956 | 9.938596 | 10.766075 | 9.773133 | 9.513556 | 8.857904 | 10.182019 | 9.656327 | 9.63308 | 9.556413 | 9.369269 | 9.337436 | 9.597274 | 9.616003 | 9.301855 | 9.158945 | 9.565742 | 9.231682 |
2208.03481 | Riccardo Falcone | Riccardo Falcone, Claudio Conti | Minkowski-Fock states in accelerated frames | null | Phys. Rev. D 106, 045013 (2022) | 10.1103/PhysRevD.106.045013 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An explicit Wigner formulation of Minkowski particle states for non-inertial
observers is unknown. Here, we derive a general prescription to compute the
characteristic function for Minkowski-Fock states in accelerated frames. For
the special case of single-particle and two-particle states, this method
enables to deri... | [
{
"created": "Sat, 6 Aug 2022 09:35:03 GMT",
"version": "v1"
}
] | 2023-06-06 | [
[
"Falcone",
"Riccardo",
""
],
[
"Conti",
"Claudio",
""
]
] | An explicit Wigner formulation of Minkowski particle states for non-inertial observers is unknown. Here, we derive a general prescription to compute the characteristic function for Minkowski-Fock states in accelerated frames. For the special case of single-particle and two-particle states, this method enables to derive... | 9.909343 | 10.611307 | 10.36688 | 9.775582 | 9.959645 | 10.823963 | 11.151605 | 10.321321 | 10.032036 | 10.451652 | 9.915623 | 9.810137 | 10.040956 | 9.87849 | 9.53328 | 9.674782 | 9.846563 | 9.472898 | 9.791576 | 9.978654 | 9.905752 |
2008.09031 | Igor F. Justo | O. C. Junqueira, I. F. Justo, D. S. Montes, A. D. Pereira, R. F.
Sobreiro | Gauge copies and the fate of background independence in Yang-Mills
theories: a leading order analysis | 16 pages, 1 figure | Phys. Rev. D 102, 074029 (2020) | 10.1103/PhysRevD.102.074029 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we investigate the effects of the Gribov prescription to get rid
of zero-modes of the Faddeev-Popov operator, at one-loop order in perturbation
theory, in the Landau-DeWitt gauge. Quantum fluctuations are taken around a
transverse background gauge field. The one-loop effective action is explicitly
comput... | [
{
"created": "Thu, 20 Aug 2020 15:34:10 GMT",
"version": "v1"
}
] | 2020-11-04 | [
[
"Junqueira",
"O. C.",
""
],
[
"Justo",
"I. F.",
""
],
[
"Montes",
"D. S.",
""
],
[
"Pereira",
"A. D.",
""
],
[
"Sobreiro",
"R. F.",
""
]
] | In this work we investigate the effects of the Gribov prescription to get rid of zero-modes of the Faddeev-Popov operator, at one-loop order in perturbation theory, in the Landau-DeWitt gauge. Quantum fluctuations are taken around a transverse background gauge field. The one-loop effective action is explicitly computed... | 9.816397 | 9.241832 | 9.727202 | 8.923469 | 9.001466 | 9.437384 | 9.460673 | 8.770107 | 9.014109 | 10.69404 | 8.548169 | 8.863369 | 9.503559 | 9.119506 | 8.842549 | 8.954174 | 8.930302 | 9.289185 | 9.15927 | 9.661368 | 9.056628 |
hep-th/0312036 | Henryk Arodz | H. Arodz | Symmetry breaking transition and appearance of compactons in a
mechanical system | New reference added | Acta Phys.Polon. B35 (2004) 625-638 | null | TPJU-8/2003 | hep-th cond-mat.soft nlin.PS | null | Recently we have described a mechanical system which exhibits spontaneous
breaking of Z_2 symmetry and related topological kinks called compactons. The
corresponding field potential is not differentiable at its global minima.
Therefore, standard derivation of dispersion relation $\omega(k)$ for small
perturbations ar... | [
{
"created": "Wed, 3 Dec 2003 13:41:47 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Dec 2003 12:54:08 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Arodz",
"H.",
""
]
] | Recently we have described a mechanical system which exhibits spontaneous breaking of Z_2 symmetry and related topological kinks called compactons. The corresponding field potential is not differentiable at its global minima. Therefore, standard derivation of dispersion relation $\omega(k)$ for small perturbations arou... | 14.099971 | 15.05437 | 14.899041 | 13.763988 | 14.654461 | 14.797882 | 15.192532 | 13.506285 | 13.329529 | 14.637819 | 12.941425 | 12.200213 | 13.336653 | 13.081553 | 12.730708 | 12.633355 | 12.895308 | 13.664212 | 13.062226 | 13.175473 | 13.172979 |
2012.06986 | Ilyas Haouam | Ilyas Haouam | Two-dimensional pauli equation in noncommutative phase-space | arXiv admin note: text overlap with arXiv:2006.00881 | Ukrainian Journal of Physics, 2021 | 10.15407/ujpe66.9.771 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we investigated the Pauli equation in a two-dimensional
noncommutative phase-space by considering a constant magnetic field
perpendicular to the plane. We mapped the noncommutative problem to the
equivalent commutative one through a set of two-dimensional Bopp-shift
transformation. The energy spectrum ... | [
{
"created": "Sun, 13 Dec 2020 07:05:50 GMT",
"version": "v1"
},
{
"created": "Sun, 7 Feb 2021 19:47:10 GMT",
"version": "v2"
}
] | 2021-10-11 | [
[
"Haouam",
"Ilyas",
""
]
] | In this paper, we investigated the Pauli equation in a two-dimensional noncommutative phase-space by considering a constant magnetic field perpendicular to the plane. We mapped the noncommutative problem to the equivalent commutative one through a set of two-dimensional Bopp-shift transformation. The energy spectrum an... | 6.112049 | 6.181468 | 6.751055 | 6.073302 | 5.950442 | 5.984844 | 6.119745 | 5.543816 | 5.74968 | 7.274176 | 5.817725 | 6.142062 | 6.076925 | 5.877347 | 5.958666 | 6.034165 | 5.968476 | 5.905291 | 5.910878 | 5.966719 | 5.873683 |
hep-th/0611003 | Daniel Green | Daniel Green | Nothing for Branes | 17 pages, v.2: added discussion of conformal invariance, added refs | JHEP 0704:025,2007 | 10.1088/1126-6708/2007/04/025 | SU-ITP-06/30, SLAC-PUB-12179 | hep-th | null | Recent work on closed string tachyon condensation suggests the existence of a
`nothing state' where closed strings and space itself vanish. We consider the
evolution of D-branes in such backgrounds, focusing on the early stages of the
condensation process. We find evidence that the branes exist in the region;
althoug... | [
{
"created": "Tue, 31 Oct 2006 23:14:45 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Mar 2007 22:17:06 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Green",
"Daniel",
""
]
] | Recent work on closed string tachyon condensation suggests the existence of a `nothing state' where closed strings and space itself vanish. We consider the evolution of D-branes in such backgrounds, focusing on the early stages of the condensation process. We find evidence that the branes exist in the region; although,... | 11.651952 | 10.454702 | 12.454062 | 10.279452 | 12.005135 | 10.853461 | 11.325489 | 10.732686 | 11.167749 | 12.213557 | 10.858156 | 10.679362 | 11.809074 | 10.558508 | 10.453953 | 10.564637 | 10.634408 | 10.681832 | 10.842113 | 12.085315 | 10.825665 |
1111.5376 | Everton Murilo Carvalho Abreu | E. M. C. Abreu, M. V. Marcial, A. C. R. Mendes, W. Oliveira and G.
Oliveira-Neto | Noncommutative cosmological models coupled to a perfect fluid and a
cosmological constant | 27 pages. 7 figures. JHEP style.arXiv admin note: substantial text
overlap with arXiv:1104.4815 | null | 10.1007/JHEP05(2012)144 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we carry out a noncommutative analysis of several
Friedmann-Robert-Walker models, coupled to different types of perfect fluids
and in the presence of a cosmological constant. The classical field equations
are modified, by the introduction of a shift operator, in order to introduce
noncommutativity in the... | [
{
"created": "Wed, 23 Nov 2011 00:34:56 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Abreu",
"E. M. C.",
""
],
[
"Marcial",
"M. V.",
""
],
[
"Mendes",
"A. C. R.",
""
],
[
"Oliveira",
"W.",
""
],
[
"Oliveira-Neto",
"G.",
""
]
] | In this work we carry out a noncommutative analysis of several Friedmann-Robert-Walker models, coupled to different types of perfect fluids and in the presence of a cosmological constant. The classical field equations are modified, by the introduction of a shift operator, in order to introduce noncommutativity in these... | 7.357112 | 7.2047 | 6.426822 | 6.135705 | 6.421055 | 7.106288 | 6.574454 | 6.040909 | 6.749441 | 7.03271 | 6.508745 | 6.747217 | 6.396315 | 6.188784 | 6.540029 | 6.490541 | 6.60319 | 6.38271 | 6.450249 | 6.352467 | 6.610981 |
1704.02590 | Adil Belhaj | Adil Belhaj, Karim Douhou, Salah Eddine Ennadifi | D-brane Standard Model-Like and Scalar Dark Matter in Type IIA
Superstring Theory | 13 pages, latex, 4 figures. To appear in JETP (2017) | null | 10.1134/S1063776117090011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In light of the present LHC Run II at $\sqrt{s}=13$ $TeV$, string y
standard-like model is studied. Concretely, a singlet $S $ scalar-extended SM
given in terms four stacks of intersecting D6-branes in a type IIA superstring
compactification producing a large gauge symmetry is examined. The involved
scales are dealt ... | [
{
"created": "Sun, 9 Apr 2017 11:47:43 GMT",
"version": "v1"
}
] | 2017-12-06 | [
[
"Belhaj",
"Adil",
""
],
[
"Douhou",
"Karim",
""
],
[
"Ennadifi",
"Salah Eddine",
""
]
] | In light of the present LHC Run II at $\sqrt{s}=13$ $TeV$, string y standard-like model is studied. Concretely, a singlet $S $ scalar-extended SM given in terms four stacks of intersecting D6-branes in a type IIA superstring compactification producing a large gauge symmetry is examined. The involved scales are dealt wi... | 17.312429 | 17.668329 | 14.50511 | 14.368576 | 14.93552 | 16.598253 | 14.005776 | 15.985836 | 15.003746 | 16.248793 | 14.105273 | 15.575009 | 14.361689 | 14.58152 | 14.88975 | 15.241059 | 15.168753 | 15.5794 | 14.986613 | 14.965964 | 15.119342 |
0709.3573 | Hyeong-Chan Kim | Hyeong-Chan Kim, Jae-Weon Lee, and Jungjai Lee | Black hole as an Information Eraser | 12 pages, 4 figures, minor changes | Mod.Phys.Lett.A25:1581-1594,2010 | 10.1142/S0217732310033347 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the identity of black hole entropy and show that the first law of
black hole thermodynamics, in the case of a Schwarzschild black hole, can be
derived from Landauer's principle by assuming that the black hole is one of the
most efficient information erasers in systems of a given temperature. The term
"most... | [
{
"created": "Sat, 22 Sep 2007 10:21:32 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Oct 2007 13:23:38 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Dec 2007 14:58:18 GMT",
"version": "v3"
},
{
"created": "Fri, 17 Oct 2008 11:09:00 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Kim",
"Hyeong-Chan",
""
],
[
"Lee",
"Jae-Weon",
""
],
[
"Lee",
"Jungjai",
""
]
] | We discuss the identity of black hole entropy and show that the first law of black hole thermodynamics, in the case of a Schwarzschild black hole, can be derived from Landauer's principle by assuming that the black hole is one of the most efficient information erasers in systems of a given temperature. The term "most e... | 8.599947 | 9.117425 | 7.792418 | 7.527381 | 8.978643 | 8.317175 | 8.123143 | 8.735229 | 8.187837 | 9.074519 | 8.477193 | 8.595892 | 8.144053 | 8.211205 | 8.394384 | 8.501214 | 8.395322 | 8.339972 | 8.283058 | 8.361939 | 8.433696 |
1201.5754 | Ram Brustein | Ram Brustein, A. J. M. Medved | Gravitational entropy and thermodynamics away from the horizon | 13 pages, Substantial changes to presentation. Conclusions unchanged,
version to be published in PLB | null | 10.1016/j.physletb.2012.07.051 | LMU-ASC 05/12 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define, by an integral of geometric quantities over a spherical shell of
arbitrary radius, an invariant gravitational entropy. This definition relies on
defining a gravitational energy and pressure, and it reduces at the horizon of
both black branes and black holes to Wald's Noether charge entropy. We support
the ... | [
{
"created": "Fri, 27 Jan 2012 12:02:40 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Jul 2012 13:43:40 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Brustein",
"Ram",
""
],
[
"Medved",
"A. J. M.",
""
]
] | We define, by an integral of geometric quantities over a spherical shell of arbitrary radius, an invariant gravitational entropy. This definition relies on defining a gravitational energy and pressure, and it reduces at the horizon of both black branes and black holes to Wald's Noether charge entropy. We support the th... | 7.732955 | 8.664119 | 8.125322 | 7.208929 | 8.458637 | 7.683908 | 8.626826 | 8.352959 | 8.034885 | 8.885812 | 8.389331 | 8.001858 | 7.880827 | 7.532276 | 7.719846 | 7.673707 | 7.735772 | 7.961965 | 7.454937 | 8.295705 | 7.868864 |
hep-th/9807156 | Chanyong Park | Chanyong Park and Sang-Jin Sin | Notes on D-instanton correction to $AdS_5 \times S^5$ geometry | 12 pages, Major revision; Title changed, 2 figures | Phys.Lett. B444 (1998) 156-162 | 10.1016/S0370-2693(98)01369-0 | null | hep-th | null | We show that the D-instanton in the $AdS_5 \times S^5$ background is a
wormhole connecting the background $AdS_5 \times S^5$ to the flat space $\bf
R^{10}$ located at the position of the D-instanton. By a $SL(2,{\bf R})$
rotation of type IIB theory, we can make the {\it global} geometry flat in
string frame. We also ... | [
{
"created": "Tue, 21 Jul 1998 06:48:18 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Sep 1998 03:25:54 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Park",
"Chanyong",
""
],
[
"Sin",
"Sang-Jin",
""
]
] | We show that the D-instanton in the $AdS_5 \times S^5$ background is a wormhole connecting the background $AdS_5 \times S^5$ to the flat space $\bf R^{10}$ located at the position of the D-instanton. By a $SL(2,{\bf R})$ rotation of type IIB theory, we can make the {\it global} geometry flat in string frame. We also fi... | 7.385175 | 7.161003 | 7.634556 | 6.92583 | 7.231068 | 7.179999 | 7.338141 | 7.048597 | 7.152683 | 7.91771 | 7.090733 | 6.999121 | 7.202037 | 6.903079 | 7.057313 | 7.127753 | 7.084328 | 7.102267 | 6.941567 | 7.323409 | 6.880523 |
hep-th/0308049 | Soo-Jong Rey | David Berenstein, Soo-Jong Rey | Wilsonian Proof for Renormalizability of N=1/2 Supersymmetric Field
Theories | 10 pages, no figure, v2: minor correction | Phys.Rev. D68 (2003) 121701 | 10.1103/PhysRevD.68.121701 | SNUST 030801 | hep-th | null | We provide Wilsonian proof for renormalizability of four-dimensional quantum
field theories with ${\cal N}=1/2$ supersymmetry. We argue that the
non-hermiticity inherent to these theories permits assigning noncanonical
scaling dimension both for the Grassman coordinates and superfields. This
reassignment can be done ... | [
{
"created": "Thu, 7 Aug 2003 17:58:40 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Aug 2003 18:40:41 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Berenstein",
"David",
""
],
[
"Rey",
"Soo-Jong",
""
]
] | We provide Wilsonian proof for renormalizability of four-dimensional quantum field theories with ${\cal N}=1/2$ supersymmetry. We argue that the non-hermiticity inherent to these theories permits assigning noncanonical scaling dimension both for the Grassman coordinates and superfields. This reassignment can be done in... | 12.52431 | 11.758277 | 12.993703 | 11.068357 | 12.450321 | 13.380633 | 11.578793 | 11.524053 | 12.413565 | 14.715385 | 10.707792 | 11.533978 | 12.613939 | 10.844109 | 11.022452 | 11.495769 | 11.116136 | 10.967536 | 11.150828 | 12.481415 | 11.087821 |
1711.04087 | Jun-Bao Wu | Jun-Bao Wu | Notes on Integrable Boundary Interactions of Open $SU(4)$ Alternating
Spin Chains | v4,12 pages, no figures, published version. To appaer in SCIENCE
CHINA Physics, Mechanics & Astronomy | Sci. China Phys. Mech. Astron. (2018) 61: 070011 | 10.1007/s11433-018-9190-y | CJQS-2018-004 | hep-th nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In arXiv:1704.05807, it was shown that the planar flavored ABJM theory is
integrable in the scalar sector at two-loop order using coordinate Bethe
ansatz. A salient feature of this case is that the boundary reflection matrices
are anti-diagonal with respect to the chosen basis. In this paper, we relax the
coefficient... | [
{
"created": "Sat, 11 Nov 2017 06:27:21 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Nov 2017 13:10:12 GMT",
"version": "v2"
},
{
"created": "Thu, 11 Jan 2018 00:53:27 GMT",
"version": "v3"
},
{
"created": "Thu, 5 Apr 2018 02:26:56 GMT",
"version": "v4"
}
] | 2020-04-23 | [
[
"Wu",
"Jun-Bao",
""
]
] | In arXiv:1704.05807, it was shown that the planar flavored ABJM theory is integrable in the scalar sector at two-loop order using coordinate Bethe ansatz. A salient feature of this case is that the boundary reflection matrices are anti-diagonal with respect to the chosen basis. In this paper, we relax the coefficients ... | 10.515652 | 10.192255 | 11.673237 | 9.458656 | 9.845453 | 10.054915 | 9.959356 | 9.586263 | 9.19894 | 11.082945 | 9.319299 | 9.697947 | 10.522764 | 9.200514 | 9.779341 | 9.661355 | 9.663914 | 9.786333 | 9.563004 | 10.448259 | 9.819305 |
2308.00040 | Matthew Blacker | Matthew J. Blacker and Sirui Ning | Wheeler DeWitt States of a Charged AdS$_4$ Black Hole | 28 pages with references, 1 figure | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We solve the Wheeler DeWitt equation for the planar Reissner-Nordstr\"om-AdS
black hole in a minisuperspace approximation. We construct semiclassical
Wheeler DeWitt states from Gaussian wavepackets that are peaked on classical
black hole interior solutions. By using the metric component $g_{xx}$ as a
clock, these sta... | [
{
"created": "Mon, 31 Jul 2023 18:00:27 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Aug 2023 12:02:46 GMT",
"version": "v2"
}
] | 2023-08-03 | [
[
"Blacker",
"Matthew J.",
""
],
[
"Ning",
"Sirui",
""
]
] | We solve the Wheeler DeWitt equation for the planar Reissner-Nordstr\"om-AdS black hole in a minisuperspace approximation. We construct semiclassical Wheeler DeWitt states from Gaussian wavepackets that are peaked on classical black hole interior solutions. By using the metric component $g_{xx}$ as a clock, these state... | 8.626697 | 8.018547 | 7.782924 | 7.671311 | 7.929759 | 8.024679 | 9.001381 | 7.843766 | 7.868495 | 8.343956 | 7.818965 | 8.13936 | 8.350244 | 8.004317 | 8.227359 | 8.160389 | 8.146018 | 7.959845 | 8.374038 | 8.673765 | 7.971735 |
2104.06587 | Harry Goodhew | Harry Goodhew, Sadra Jazayeri, Mang Hei Gordon Lee and Enrico Pajer | Cutting Cosmological Correlators | 36 + 18 pages, 4 figures | null | 10.1088/1475-7516/2021/08/003 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The initial conditions of our universe appear to us in the form of a
classical probability distribution that we probe with cosmological
observations. In the current leading paradigm, this probability distribution
arises from a quantum mechanical wavefunction of the universe. Here we ask what
the imprint of quantum me... | [
{
"created": "Wed, 14 Apr 2021 02:14:44 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Apr 2021 09:06:51 GMT",
"version": "v2"
},
{
"created": "Thu, 24 Jun 2021 15:01:30 GMT",
"version": "v3"
}
] | 2021-08-11 | [
[
"Goodhew",
"Harry",
""
],
[
"Jazayeri",
"Sadra",
""
],
[
"Lee",
"Mang Hei Gordon",
""
],
[
"Pajer",
"Enrico",
""
]
] | The initial conditions of our universe appear to us in the form of a classical probability distribution that we probe with cosmological observations. In the current leading paradigm, this probability distribution arises from a quantum mechanical wavefunction of the universe. Here we ask what the imprint of quantum mech... | 8.653892 | 7.981953 | 9.085696 | 7.755652 | 8.419923 | 8.063833 | 8.217318 | 7.994907 | 8.033045 | 9.826214 | 7.874245 | 8.20826 | 8.552434 | 8.367857 | 8.246156 | 8.187263 | 8.171684 | 8.397479 | 8.506591 | 8.401486 | 8.468976 |
2111.00018 | Linus Wulff | Linus Wulff | Completing $R^4$ using $O(d,d)$ | 23 pages; v2: Clarifications and details of comparison to literature
added; v3: Added argument that condition imposed is also sufficient for
O(d,d). Published version | null | 10.1007/JHEP08(2022)187 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The tree-level string effective action is known to contain quartic Riemann
terms with coefficient $\zeta(3)\alpha'^3$. In the case of the type II string
this is the first $\alpha'$ correction. We use the requirement that the action
reduced on a $d$-torus should have an $O(d,d)$ symmetry to find the B-field
couplings ... | [
{
"created": "Fri, 29 Oct 2021 18:00:01 GMT",
"version": "v1"
},
{
"created": "Wed, 25 May 2022 07:19:33 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Aug 2022 06:29:47 GMT",
"version": "v3"
}
] | 2022-09-07 | [
[
"Wulff",
"Linus",
""
]
] | The tree-level string effective action is known to contain quartic Riemann terms with coefficient $\zeta(3)\alpha'^3$. In the case of the type II string this is the first $\alpha'$ correction. We use the requirement that the action reduced on a $d$-torus should have an $O(d,d)$ symmetry to find the B-field couplings up... | 10.774765 | 8.12908 | 11.302515 | 8.162484 | 8.811531 | 8.188022 | 8.594056 | 8.799113 | 8.181928 | 12.244827 | 8.493036 | 9.475248 | 9.648393 | 8.799551 | 9.337482 | 8.850491 | 9.410213 | 8.945147 | 9.170777 | 10.246531 | 9.062806 |
1205.5550 | Yasunori Nomura | Yasunori Nomura | The Static Quantum Multiverse | 27 pages, 2 figures; a typo in the abstract corrected | null | 10.1103/PhysRevD.86.083505 | UCB-PTH-12/07 | hep-th astro-ph.CO gr-qc hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the multiverse in the intrinsically quantum mechanical framework
recently proposed in Refs. [1,2]. By requiring that the principles of quantum
mechanics are universally valid and that physical predictions do not depend on
the reference frame one chooses to describe the multiverse, we find that the
multive... | [
{
"created": "Thu, 24 May 2012 19:59:41 GMT",
"version": "v1"
},
{
"created": "Sat, 26 May 2012 09:10:18 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Nomura",
"Yasunori",
""
]
] | We consider the multiverse in the intrinsically quantum mechanical framework recently proposed in Refs. [1,2]. By requiring that the principles of quantum mechanics are universally valid and that physical predictions do not depend on the reference frame one chooses to describe the multiverse, we find that the multivers... | 10.480213 | 10.234481 | 9.863544 | 9.390205 | 10.235235 | 9.732012 | 10.650487 | 9.430137 | 10.234271 | 9.998326 | 9.762053 | 9.614272 | 9.976631 | 9.7153 | 9.533817 | 9.528677 | 9.653841 | 9.5173 | 9.501774 | 10.058485 | 9.545982 |
2202.08285 | Ke Ren | Qingjun Jin, Ke Ren, Gang Yang, Rui Yu | Gluonic evanescent operators: classification and one-loop
renormalization | v2: 70 pages, 3 figures, 9 tables; reference added, minor corrections | null | 10.1007/JHEP08(2022)141 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Evanescent operators are a special class of operators that vanish classically
in four-dimensional spacetime, while in general dimensions they are non-zero
and are expected to have non-trivial physical effects at the quantum loop level
in dimensional regularization. In this paper we initiate the study of
evanescent op... | [
{
"created": "Wed, 16 Feb 2022 19:00:04 GMT",
"version": "v1"
},
{
"created": "Sun, 15 May 2022 01:53:40 GMT",
"version": "v2"
}
] | 2022-09-07 | [
[
"Jin",
"Qingjun",
""
],
[
"Ren",
"Ke",
""
],
[
"Yang",
"Gang",
""
],
[
"Yu",
"Rui",
""
]
] | Evanescent operators are a special class of operators that vanish classically in four-dimensional spacetime, while in general dimensions they are non-zero and are expected to have non-trivial physical effects at the quantum loop level in dimensional regularization. In this paper we initiate the study of evanescent oper... | 8.291268 | 6.218729 | 7.297501 | 6.303009 | 6.432459 | 6.34686 | 6.248809 | 6.174325 | 6.19557 | 7.671375 | 6.464079 | 6.561852 | 6.959279 | 6.74719 | 6.86726 | 6.697276 | 6.326518 | 6.818522 | 6.721692 | 7.088829 | 7.261121 |
hep-th/0612207 | Ling Yan Hung Miss | Ling-Yan Hung | Comments on I1-branes | 9 pages. Added comments about the near horizon limit taken | JHEP 0705:076,2007 | 10.1088/1126-6708/2007/05/076 | DAMTP-2006-121 | hep-th | null | We explore the supergravity solution of D5-branes intersecting as an
I1-brane. In a suitable near-horizon limit the geometry is in qualitative
agreement with that found in the microscopic open-string analysis as well as
the NS5-brane analysis of Itzhaki, Kutasov and Seiberg. In particular, the
ISO(1,1) Lorentz symmet... | [
{
"created": "Tue, 19 Dec 2006 15:26:04 GMT",
"version": "v1"
},
{
"created": "Sun, 31 Dec 2006 15:29:09 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Feb 2007 12:21:46 GMT",
"version": "v3"
},
{
"created": "Mon, 21 May 2007 08:28:50 GMT",
"version": "v4"
}
] | 2010-10-27 | [
[
"Hung",
"Ling-Yan",
""
]
] | We explore the supergravity solution of D5-branes intersecting as an I1-brane. In a suitable near-horizon limit the geometry is in qualitative agreement with that found in the microscopic open-string analysis as well as the NS5-brane analysis of Itzhaki, Kutasov and Seiberg. In particular, the ISO(1,1) Lorentz symmetry... | 7.339488 | 7.405318 | 8.655084 | 7.141025 | 6.802503 | 7.041092 | 7.338767 | 7.314793 | 7.191198 | 9.088538 | 7.382495 | 6.980525 | 8.17104 | 7.154742 | 7.341887 | 7.279445 | 7.160752 | 7.192329 | 6.874112 | 7.581915 | 6.895865 |
1904.01224 | Efra\'in Rojas Marcial | Efrain Rojas | Holographic relationships in Lovelock type brane gravity | 16 pages. Discussions and references added. Version that matches the
one published | Class. Quantum Grav. 36 (2019) 185006 | 10.1088/1361-6382/ab3520 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the Lovelock type brane gravity is naturally holographic by
providing a correspondence between bulk and surface terms that appear in the
Lovelock-type brane gravity action functional. We prove the existence of
relationships between the $\mathcal{L}_{\mbox{\tiny bulk}}$ and
$\mathcal{L}_{\mbox{\tiny surf}... | [
{
"created": "Tue, 2 Apr 2019 05:42:13 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Aug 2019 23:21:47 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"Rojas",
"Efrain",
""
]
] | We show that the Lovelock type brane gravity is naturally holographic by providing a correspondence between bulk and surface terms that appear in the Lovelock-type brane gravity action functional. We prove the existence of relationships between the $\mathcal{L}_{\mbox{\tiny bulk}}$ and $\mathcal{L}_{\mbox{\tiny surf}}$... | 7.07125 | 6.840523 | 7.193584 | 6.699825 | 7.311715 | 7.216826 | 7.404194 | 6.604339 | 6.90496 | 7.231413 | 7.028603 | 6.580613 | 6.818163 | 6.709983 | 6.731744 | 6.602304 | 6.696805 | 6.725492 | 6.84037 | 6.76328 | 6.579579 |
1802.08011 | Anton Galajinsky | Anton Galajinsky | Ruijsenaars-Schneider three-body models with N=2 supersymmetry | v3: 10 pages, imaginary unit missed in Eq. (22) is reinstated | null | 10.1007/JHEP04(2018)079 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Ruijsenaars-Schneider models are conventionally regarded as relativistic
generalizations of the Calogero integrable systems. Surprisingly enough, their
supersymmetric generalizations escaped attention. In this work, N=2
supersymmetric extensions of the rational and hyperbolic Ruijsenaars-Schneider
three-body mode... | [
{
"created": "Thu, 22 Feb 2018 12:33:49 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Apr 2018 06:56:23 GMT",
"version": "v2"
},
{
"created": "Wed, 5 Jun 2019 00:32:12 GMT",
"version": "v3"
}
] | 2019-06-06 | [
[
"Galajinsky",
"Anton",
""
]
] | The Ruijsenaars-Schneider models are conventionally regarded as relativistic generalizations of the Calogero integrable systems. Surprisingly enough, their supersymmetric generalizations escaped attention. In this work, N=2 supersymmetric extensions of the rational and hyperbolic Ruijsenaars-Schneider three-body models... | 7.399814 | 7.150389 | 7.845425 | 6.794653 | 7.161603 | 6.827831 | 6.697956 | 6.395791 | 7.052666 | 8.245041 | 6.650786 | 6.681603 | 7.268581 | 6.811877 | 6.978579 | 6.962897 | 6.803439 | 6.86218 | 7.167162 | 7.039332 | 6.878316 |
1902.11103 | Theodore Erler | Theodore Erler, Toru Masuda, Martin Schnabl | Rolling Near the Tachyon Vacuum | 41 pages, 12 figures | null | 10.1007/JHEP04(2020)104 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a linear dilaton background, it has been argued that an unstable D-brane
can decay to the tachyon vacuum without leaving behind a remnant of tachyon
matter. Here we address the question of how the D-brane can decay to the
tachyon vacuum when the tachyon vacuum does not support physical fluctuations.
Using the form... | [
{
"created": "Thu, 28 Feb 2019 14:36:48 GMT",
"version": "v1"
}
] | 2020-05-20 | [
[
"Erler",
"Theodore",
""
],
[
"Masuda",
"Toru",
""
],
[
"Schnabl",
"Martin",
""
]
] | In a linear dilaton background, it has been argued that an unstable D-brane can decay to the tachyon vacuum without leaving behind a remnant of tachyon matter. Here we address the question of how the D-brane can decay to the tachyon vacuum when the tachyon vacuum does not support physical fluctuations. Using the formal... | 8.261074 | 7.06035 | 8.304616 | 7.147809 | 7.842829 | 7.687223 | 7.115696 | 7.232372 | 7.47135 | 8.739142 | 7.454095 | 7.394356 | 7.825749 | 7.245241 | 7.193639 | 7.30979 | 7.621731 | 7.541304 | 7.319488 | 7.639363 | 7.490546 |
hep-th/9812039 | Marco Serone | J.F. Morales, J.C. Plefka, C.A. Scrucca, M. Serone and A.K. Waldron | Spin dependent D-brane interactions and scattering amplitudes in matrix
theory | 8 pages, no figures, talk presented at the conference "Quantum
aspects of gauge theories, supergravity and unification", Corfu, Greece, to
appear in the proceedings | Lect.Notes Phys. 525 (1999) 456-465 | 10.1007/BFb0104266 | null | hep-th | null | Spin interactions beteween two moving Dp-branes are analyzed using the
Green-Schwarz formalism of boundary states. This approach turns out to be
extremely efficient to compute all the spin effects related by supersymmetry to
the leading v^4/r^7-p term. All these terms are shown to be scale invariant,
supporting a mat... | [
{
"created": "Fri, 4 Dec 1998 11:49:41 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Morales",
"J. F.",
""
],
[
"Plefka",
"J. C.",
""
],
[
"Scrucca",
"C. A.",
""
],
[
"Serone",
"M.",
""
],
[
"Waldron",
"A. K.",
""
]
] | Spin interactions beteween two moving Dp-branes are analyzed using the Green-Schwarz formalism of boundary states. This approach turns out to be extremely efficient to compute all the spin effects related by supersymmetry to the leading v^4/r^7-p term. All these terms are shown to be scale invariant, supporting a matri... | 15.445549 | 13.504421 | 17.908178 | 12.485775 | 14.17316 | 13.623938 | 14.217378 | 11.970579 | 12.71536 | 18.415035 | 12.935104 | 14.261039 | 15.181958 | 14.190485 | 14.619164 | 14.225481 | 13.885936 | 13.845226 | 14.204726 | 15.674354 | 14.290539 |
1911.09190 | Sarthak Parikh | Sarthak Parikh | A multipoint conformal block chain in $d$ dimensions | 35 pages + appendices + references, several figures. Mathematica
notebook containing the main result included as an ancillary file | null | 10.1007/JHEP05(2020)120 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Conformal blocks play a central role in CFTs as the basic, theory-independent
building blocks. However, only limited results are available concerning
multipoint blocks associated with the global conformal group. In this paper, we
systematically work out the $d$-dimensional $n$-point global conformal blocks
(for arbit... | [
{
"created": "Wed, 20 Nov 2019 22:01:17 GMT",
"version": "v1"
}
] | 2020-06-24 | [
[
"Parikh",
"Sarthak",
""
]
] | Conformal blocks play a central role in CFTs as the basic, theory-independent building blocks. However, only limited results are available concerning multipoint blocks associated with the global conformal group. In this paper, we systematically work out the $d$-dimensional $n$-point global conformal blocks (for arbitra... | 8.446331 | 7.463869 | 8.867364 | 7.534113 | 7.068714 | 7.647903 | 7.22855 | 7.355985 | 7.274573 | 9.161772 | 6.957579 | 7.455802 | 7.64709 | 7.352489 | 7.624392 | 7.359951 | 7.529306 | 7.434362 | 7.532244 | 7.529419 | 7.38757 |
0704.0445 | Jacob Bourjaily | Jacob L. Bourjaily | Geometrically Engineering the Standard Model: Locally Unfolding Three
Families out of E8 | 10 pages, 3 figures. Corrected typos and general editing blemishes | Phys.Rev.D76:046004,2007 | 10.1103/PhysRevD.76.046004 | null | hep-th | null | This paper extends and builds upon the results of an earlier paper, in which
we described how to use the tools of geometrical engineering to deform
geometrically-engineered grand unified models into ones with lower symmetry.
This top-down unfolding has the advantage that the relative positions of
singularities giving... | [
{
"created": "Tue, 3 Apr 2007 17:28:03 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Aug 2007 20:27:24 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bourjaily",
"Jacob L.",
""
]
] | This paper extends and builds upon the results of an earlier paper, in which we described how to use the tools of geometrical engineering to deform geometrically-engineered grand unified models into ones with lower symmetry. This top-down unfolding has the advantage that the relative positions of singularities giving r... | 11.878036 | 12.579233 | 12.368712 | 11.367371 | 13.18205 | 12.43207 | 12.019801 | 12.125739 | 11.782565 | 13.31801 | 11.629809 | 11.122085 | 11.635497 | 11.190056 | 11.457368 | 11.574691 | 11.3914 | 11.548069 | 11.466829 | 11.726664 | 11.273005 |
hep-th/0107180 | Vatche Sahakian | Vatche Sahakian | The large M limit of Non-Commutative Open Strings at strong coupling | 45 pages, 7 figures | Nucl.Phys.B621:62-100,2002 | 10.1016/S0550-3213(01)00581-8 | CLNS 01/1747 | hep-th | null | Two dimensional Non-Commutative Open String (NCOS) theory, well-defined
perturbatively, may also be studied at strong coupling and for large D-string
charge by making use of the Holographic duality. We analyze the zero mode
dynamics of a closed string in the appropriate background geometry and map the
results onto a ... | [
{
"created": "Sat, 21 Jul 2001 14:39:20 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Sahakian",
"Vatche",
""
]
] | Two dimensional Non-Commutative Open String (NCOS) theory, well-defined perturbatively, may also be studied at strong coupling and for large D-string charge by making use of the Holographic duality. We analyze the zero mode dynamics of a closed string in the appropriate background geometry and map the results onto a se... | 14.58183 | 14.01529 | 16.070456 | 12.841899 | 13.796842 | 14.32395 | 13.414694 | 12.911407 | 13.726251 | 16.876583 | 13.669744 | 13.483566 | 14.646623 | 13.744918 | 13.270549 | 13.269777 | 13.497725 | 13.084805 | 13.590833 | 14.252804 | 13.563781 |
hep-th/0001010 | Andrei Belitsky | A.V. Belitsky, S. Vandoren, P. van Nieuwenhuizen | Instantons, Euclidean supersymmetry and Wick rotations | 8 pages, LaTeX, typos fixed | Phys.Lett. B477 (2000) 335-340 | 10.1016/S0370-2693(00)00183-0 | null | hep-th | null | We discuss the reality properties of the fermionic collective coordinates in
Euclidean space in an instanton background and construct hermitean actions for
N = 4 and N = 2 supersymmetric Euclidean Yang-Mills theories.
| [
{
"created": "Tue, 4 Jan 2000 01:28:58 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Feb 2000 16:20:02 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Belitsky",
"A. V.",
""
],
[
"Vandoren",
"S.",
""
],
[
"van Nieuwenhuizen",
"P.",
""
]
] | We discuss the reality properties of the fermionic collective coordinates in Euclidean space in an instanton background and construct hermitean actions for N = 4 and N = 2 supersymmetric Euclidean Yang-Mills theories. | 13.633984 | 8.886812 | 11.574407 | 9.22853 | 9.878266 | 10.489034 | 9.978302 | 9.679147 | 9.419095 | 14.699041 | 10.151582 | 10.059361 | 11.686707 | 9.450152 | 9.866411 | 9.278627 | 9.962832 | 9.938383 | 9.932923 | 11.583914 | 9.616934 |
hep-th/9812105 | Jose M. F. Labastida | J. M. F. Labastida and Esther Perez | Vassiliev Invariants in the Context of Chern-Simons Gauge Theory | Invited lecture at the Workshop on New Developments in Algebraic
Topology, Faro 1998, 17 pages, latex, epsf, 7 figures, 2 tables, figure 7 has
been improved | null | null | Universidad de Santiago de Compostela preprint USC-FT-18/98 | hep-th | null | We summarize the progress made during the last few years on the study of
Vassiliev invariants from the point of view of perturbative Chern-Simons gauge
theory. We argue that this approach is the most promising one to obtain a
combinatorial universal formula for Vassiliev invariants. The combinatorial
expressions for ... | [
{
"created": "Sun, 13 Dec 1998 17:58:14 GMT",
"version": "v1"
},
{
"created": "Sun, 20 Dec 1998 15:52:09 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Labastida",
"J. M. F.",
""
],
[
"Perez",
"Esther",
""
]
] | We summarize the progress made during the last few years on the study of Vassiliev invariants from the point of view of perturbative Chern-Simons gauge theory. We argue that this approach is the most promising one to obtain a combinatorial universal formula for Vassiliev invariants. The combinatorial expressions for th... | 6.239709 | 5.651 | 6.720689 | 5.628932 | 6.073977 | 6.256234 | 5.623415 | 5.374774 | 5.579358 | 6.700748 | 5.56778 | 5.733469 | 6.260727 | 5.928568 | 5.687638 | 5.769686 | 5.672552 | 5.687857 | 5.917372 | 6.272047 | 5.551111 |
0809.4870 | Dam Thanh Son | C. P. Herzog, P. K. Kovtun, D. T. Son | Holographic model of superfluidity | 17 pages, 4 figures; v2 ref added; v3 small corrections, published in
PRD | null | 10.1103/PhysRevD.79.066002 | PUPT-2281, INT PUB 08-45 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a holographic model of a relativistic quantum system with a global
U(1) symmetry, at non-zero temperature and density. When the temperature falls
below a critical value, we find a second-order superfluid phase transition with
mean-field critical exponents. In the symmetry-broken phase, we determine the
speed... | [
{
"created": "Sun, 28 Sep 2008 20:55:46 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Oct 2008 21:57:12 GMT",
"version": "v2"
},
{
"created": "Sun, 7 Jun 2009 09:01:55 GMT",
"version": "v3"
}
] | 2009-11-13 | [
[
"Herzog",
"C. P.",
""
],
[
"Kovtun",
"P. K.",
""
],
[
"Son",
"D. T.",
""
]
] | We study a holographic model of a relativistic quantum system with a global U(1) symmetry, at non-zero temperature and density. When the temperature falls below a critical value, we find a second-order superfluid phase transition with mean-field critical exponents. In the symmetry-broken phase, we determine the speed o... | 5.430449 | 4.874418 | 5.830387 | 5.058209 | 5.411226 | 5.725229 | 4.993853 | 4.966623 | 5.18037 | 5.408834 | 4.866096 | 5.425539 | 5.461165 | 5.336542 | 5.036071 | 5.241853 | 5.212599 | 5.065843 | 5.135538 | 5.42508 | 5.022496 |
1007.3871 | Jean Nuyts | David B. Fairlie and Jean Nuyts | Necessary conditions for Ternary Algebras | 10 pages | J.Phys.A43:465202,2010 | 10.1088/1751-8113/43/46/465202 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Ternary algebras, constructed from ternary commutators, or as we call them,
ternutators, defined as the alternating sum of products of three operators,
have been shown to satisfy cubic identities as necessary conditions for their
existence. Here we examine the situation where we permit identities not solely
construct... | [
{
"created": "Thu, 22 Jul 2010 12:51:38 GMT",
"version": "v1"
}
] | 2011-03-28 | [
[
"Fairlie",
"David B.",
""
],
[
"Nuyts",
"Jean",
""
]
] | Ternary algebras, constructed from ternary commutators, or as we call them, ternutators, defined as the alternating sum of products of three operators, have been shown to satisfy cubic identities as necessary conditions for their existence. Here we examine the situation where we permit identities not solely constructed... | 13.46811 | 12.250624 | 15.379539 | 13.094086 | 13.543509 | 11.922983 | 12.246722 | 12.503556 | 13.480542 | 15.62547 | 13.307606 | 12.366424 | 13.81082 | 12.451324 | 12.181617 | 12.077144 | 12.832628 | 12.974015 | 12.477247 | 13.458736 | 13.221737 |
hep-th/0101183 | Shahin Mamedov | Sh. Mamedov, Jian-Zu Zhang and V. Zhukovskii | Supersymmetry in Quantum Mechanics of Colored Particles | 8 pages, no figures | Mod.Phys.Lett. A16 (2001) 845-852 | 10.1142/S0217732301004066 | null | hep-th | null | The role of supercharge operators is studied in the case of a Dirac particle
moving in a constant chromomagnetic field. The Hamiltonian is factorised and
the ground state wave function in the case of unbroken supersymmetry is
determined.
| [
{
"created": "Fri, 26 Jan 2001 17:11:36 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Mamedov",
"Sh.",
""
],
[
"Zhang",
"Jian-Zu",
""
],
[
"Zhukovskii",
"V.",
""
]
] | The role of supercharge operators is studied in the case of a Dirac particle moving in a constant chromomagnetic field. The Hamiltonian is factorised and the ground state wave function in the case of unbroken supersymmetry is determined. | 10.725069 | 9.074224 | 9.583735 | 9.470402 | 9.684266 | 8.560229 | 8.92875 | 9.967561 | 9.004392 | 9.969829 | 8.753189 | 8.328051 | 9.284899 | 8.634672 | 8.158215 | 8.181325 | 8.391141 | 8.814659 | 8.683759 | 9.105577 | 8.221839 |
hep-th/9311028 | Leonid Keldish | O.V.Dodlov, S.E.Konstein, and M.A.Vasiliev | Matrix Versions of the Calogero Model | 7 pages, FIAN/TD/17--93 | null | null | null | hep-th | null | Matrix generalizations of the N-particle quantum-mechanical Calogero model
classifying according to representations of the symmetric group $S_N$ are
considered. Symmetry properties of the eigen-wave functions in the matrix
Calogero models are analyzed. Latex.
| [
{
"created": "Thu, 4 Nov 1993 21:49:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dodlov",
"O. V.",
""
],
[
"Konstein",
"S. E.",
""
],
[
"Vasiliev",
"M. A.",
""
]
] | Matrix generalizations of the N-particle quantum-mechanical Calogero model classifying according to representations of the symmetric group $S_N$ are considered. Symmetry properties of the eigen-wave functions in the matrix Calogero models are analyzed. Latex. | 19.712021 | 13.583573 | 16.512886 | 15.284039 | 14.916456 | 13.210586 | 12.838601 | 11.398521 | 13.055616 | 21.578152 | 11.410746 | 13.801393 | 15.576346 | 13.221696 | 13.695395 | 13.712344 | 12.782117 | 13.407987 | 13.161765 | 14.424026 | 12.696469 |
1407.1160 | Kouichi Nomura | Kouichi Nomura | Bimetric gravity and two-component fluid in the AdS/CFT correspondence | 25 pages, 2 figures | null | null | KUNS-2504 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study bimetric gravity through the context of the AdS/CFT correspondence,
especially, in the first order hdrodynamic limit. If we put pure general
relativity as a bulk field, the boundary field theory is interpreted as fluid
of the N = 4 supersymmetric Yang-Mills plasma. The transport coefficients of
this plasma a... | [
{
"created": "Fri, 4 Jul 2014 09:17:52 GMT",
"version": "v1"
}
] | 2014-07-07 | [
[
"Nomura",
"Kouichi",
""
]
] | We study bimetric gravity through the context of the AdS/CFT correspondence, especially, in the first order hdrodynamic limit. If we put pure general relativity as a bulk field, the boundary field theory is interpreted as fluid of the N = 4 supersymmetric Yang-Mills plasma. The transport coefficients of this plasma are... | 12.993948 | 14.166553 | 13.15504 | 13.083442 | 12.728405 | 13.336808 | 13.028722 | 13.300925 | 12.960505 | 13.956786 | 12.859136 | 12.500001 | 13.174392 | 12.673924 | 12.374368 | 12.49964 | 12.730406 | 12.832362 | 12.465357 | 12.925215 | 12.391077 |
1203.6354 | Leonardo Senatore | Leonardo Senatore and Matias Zaldarriaga | On Loops in Inflation II: IR Effects in Single Clock Inflation | 13 pages, 1 figure; v2: JHEP published version, added minor comments
and references | null | 10.1007/JHEP01(2013)109 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In single clock models of inflation the coupling between modes of very
different scales does not have any significant dynamical effect during
inflation. It leads to interesting projection effects. Larger and smaller modes
change the relation between the scale a mode of interest will appear in the
post-inflationary un... | [
{
"created": "Wed, 28 Mar 2012 20:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Feb 2013 10:47:52 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Senatore",
"Leonardo",
""
],
[
"Zaldarriaga",
"Matias",
""
]
] | In single clock models of inflation the coupling between modes of very different scales does not have any significant dynamical effect during inflation. It leads to interesting projection effects. Larger and smaller modes change the relation between the scale a mode of interest will appear in the post-inflationary univ... | 15.398644 | 16.625956 | 16.505501 | 15.436015 | 17.004456 | 16.638081 | 16.309765 | 15.835915 | 14.552173 | 15.6228 | 14.900845 | 14.147501 | 14.322539 | 14.270093 | 13.826746 | 14.618382 | 13.630315 | 14.208377 | 14.005724 | 14.915002 | 13.95498 |
1301.3519 | David Berenstein | David Berenstein | Giant gravitons: a collective coordinate approach | 29 pages + appendix. v2: small changes, added references. v3: Added
reference, fixed typos, added some clarifying remarks and made introduction
more concise | null | 10.1103/PhysRevD.87.126009 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper I describe a collective coordinate approach to the study of
giant graviton states and their excitations in various field theories. The
method simplifies considerably the understanding of emergent gauge symmetry of
these configurations, as well as the calculation of the spectrum of strings
stretched betw... | [
{
"created": "Tue, 15 Jan 2013 22:32:18 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Feb 2013 18:06:38 GMT",
"version": "v2"
},
{
"created": "Mon, 20 May 2013 19:37:08 GMT",
"version": "v3"
}
] | 2013-06-19 | [
[
"Berenstein",
"David",
""
]
] | In this paper I describe a collective coordinate approach to the study of giant graviton states and their excitations in various field theories. The method simplifies considerably the understanding of emergent gauge symmetry of these configurations, as well as the calculation of the spectrum of strings stretched betwee... | 13.084705 | 11.313779 | 14.962871 | 10.925536 | 11.587286 | 12.050696 | 11.870914 | 11.598928 | 11.089915 | 14.270025 | 11.096266 | 11.008234 | 12.069118 | 11.218481 | 11.313562 | 11.315616 | 11.141506 | 11.037216 | 11.290901 | 12.071444 | 11.738261 |
hep-th/0607103 | Tasneem Zehra Husain | Tasneem Zehra Husain | BPS M-Brane Geometries | 7 pages. Contribution to proceedings of 12th Regional Conference in
Mathematical Physics, Islamabad, March 2006 | null | null | null | hep-th | null | In the search for a classification of BPS backgrounds with flux, we look at
geometries that arise when M-branes wrap supersymmetric cycles in Calabi-Yau
manifolds. We find constraints on the differential forms in the back-reacted
manifolds and discover that the calibration corresponding to the (background
generating)... | [
{
"created": "Sun, 16 Jul 2006 18:25:01 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Husain",
"Tasneem Zehra",
""
]
] | In the search for a classification of BPS backgrounds with flux, we look at geometries that arise when M-branes wrap supersymmetric cycles in Calabi-Yau manifolds. We find constraints on the differential forms in the back-reacted manifolds and discover that the calibration corresponding to the (background generating) M... | 15.268093 | 15.250154 | 16.223152 | 13.046863 | 13.637372 | 13.955495 | 13.09404 | 12.910847 | 13.421838 | 17.733469 | 14.405876 | 14.423217 | 16.403902 | 13.623878 | 13.324782 | 13.57501 | 13.703601 | 13.174129 | 13.378678 | 15.656014 | 13.280006 |
1801.02049 | Maxim Kurkov | Maxim Kurkov and Dmitri Vassilevich | Gravitational parity anomaly with and without boundaries | 16 pages, final version, accepted for publication in JHEP | JHEP 1803 (2018) 072 | 10.1007/JHEP03(2018)072 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we consider gravitational parity anomaly in three and four
dimensions. We start with a re-computation of this anomaly on a 3D manifold
without boundaries and with a critical comparison of our results to the
previous calculations. Then we compute the anomaly on 4D manifolds with
boundaries with local bag... | [
{
"created": "Sat, 6 Jan 2018 16:57:51 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jan 2018 17:11:17 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Mar 2018 12:09:43 GMT",
"version": "v3"
}
] | 2018-11-22 | [
[
"Kurkov",
"Maxim",
""
],
[
"Vassilevich",
"Dmitri",
""
]
] | In this paper we consider gravitational parity anomaly in three and four dimensions. We start with a re-computation of this anomaly on a 3D manifold without boundaries and with a critical comparison of our results to the previous calculations. Then we compute the anomaly on 4D manifolds with boundaries with local bag b... | 8.546427 | 8.211125 | 8.410169 | 7.457425 | 8.065635 | 7.710336 | 7.611066 | 7.701413 | 8.350444 | 8.747649 | 8.012373 | 8.17759 | 8.147126 | 8.117542 | 8.080777 | 8.28581 | 8.019077 | 8.464291 | 7.964294 | 8.347172 | 7.982504 |
1502.04267 | Sinya Aoki | Sinya Aoki, Takumi Iritani, Masahiro Nozaki, Tokiro Numasawa, Noburo
Shiba, Hal Tasaki | On the definition of entanglement entropy in lattice gauge theories | 29 pages, 1 figure, a comment and more references added, some typos
corrected | null | null | YITP-2015-8 | hep-th hep-lat quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We focus on the issue of proper definition of entanglement entropy in lattice
gauge theories, and examine a naive definition where gauge invariant states are
viewed as elements of an extended Hilbert space which contains gauge
non-invariant states as well. Working in the extended Hilbert space, we can
define entangle... | [
{
"created": "Sun, 15 Feb 2015 01:21:48 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Feb 2015 03:57:54 GMT",
"version": "v2"
}
] | 2015-02-25 | [
[
"Aoki",
"Sinya",
""
],
[
"Iritani",
"Takumi",
""
],
[
"Nozaki",
"Masahiro",
""
],
[
"Numasawa",
"Tokiro",
""
],
[
"Shiba",
"Noburo",
""
],
[
"Tasaki",
"Hal",
""
]
] | We focus on the issue of proper definition of entanglement entropy in lattice gauge theories, and examine a naive definition where gauge invariant states are viewed as elements of an extended Hilbert space which contains gauge non-invariant states as well. Working in the extended Hilbert space, we can define entangleme... | 6.195415 | 6.652248 | 6.809054 | 5.754946 | 5.930161 | 5.84517 | 6.282548 | 5.95494 | 5.969487 | 7.226807 | 5.984343 | 5.888954 | 6.125622 | 5.801819 | 5.994607 | 5.805408 | 5.636293 | 5.825422 | 5.897262 | 6.066065 | 5.794777 |
hep-th/9706024 | Nathan Jacob Berkovits | Nathan Berkovits (IFT/UNESP, Sao Paulo) | Ramond-Ramond Central Charges in the Supersymmetry Algebra of the
Superstring | 10 pages harvmac tex | Phys.Rev.Lett. 79 (1997) 1813-1816 | 10.1103/PhysRevLett.79.1813 | IFT-P.038/97 | hep-th | null | The free action for the massless sector of the Type II superstring was
recently constructed using closed RNS superstring field theory. The
supersymmetry transformations of this action are shown to satisfy an N=2 D=10
SUSY algebra with Ramond-Ramond central charges.
| [
{
"created": "Tue, 3 Jun 1997 23:11:02 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Berkovits",
"Nathan",
"",
"IFT/UNESP, Sao Paulo"
]
] | The free action for the massless sector of the Type II superstring was recently constructed using closed RNS superstring field theory. The supersymmetry transformations of this action are shown to satisfy an N=2 D=10 SUSY algebra with Ramond-Ramond central charges. | 10.675355 | 8.150166 | 11.746517 | 9.402154 | 8.728145 | 9.498715 | 9.013048 | 8.478909 | 8.865515 | 15.715211 | 9.492528 | 9.484712 | 10.744569 | 9.569805 | 9.587274 | 9.939623 | 9.864966 | 9.636486 | 9.369905 | 11.360665 | 9.499678 |
hep-th/0606229 | Fabio Scardigli | Fabio Scardigli and Roberto Casadio | Reply to "Holographic principle in spacetimes with extra spatial
dimensions" and "About quantum fluctuations and holographic principle in
(4+n)-dimensional spacetime" | LaTex file, 4 pages | null | null | null | hep-th | null | We reply to the comments by P.Midodashvili about our previous paper [1]. We
argue that, contrary to the conclusions in Refs. [2,3], the Generalized
Uncertainty Principle proposed by Ng and van Dam in Ref. [4] is compatible with
the Holographic Principle in spacetimes with extra dimensions only for a very
special (and... | [
{
"created": "Fri, 23 Jun 2006 13:09:25 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Scardigli",
"Fabio",
""
],
[
"Casadio",
"Roberto",
""
]
] | We reply to the comments by P.Midodashvili about our previous paper [1]. We argue that, contrary to the conclusions in Refs. [2,3], the Generalized Uncertainty Principle proposed by Ng and van Dam in Ref. [4] is compatible with the Holographic Principle in spacetimes with extra dimensions only for a very special (and s... | 11.077424 | 8.74354 | 9.243069 | 8.616148 | 9.173181 | 9.316833 | 10.472304 | 7.963299 | 9.139799 | 8.698639 | 8.792276 | 9.174232 | 9.463673 | 8.932374 | 9.319279 | 9.484556 | 9.108189 | 9.079041 | 9.151431 | 9.16221 | 9.596407 |
hep-th/0607244 | Itamar Yaakov | Itamar Yaakov | Open and Closed String Worldsheets from Free Large N Gauge Theories with
Adjoint and Fundamental Matter | 19 pages, 3 figures; typo corrected, section 2.2 clarified | JHEP0611:065,2006 | 10.1088/1126-6708/2006/11/065 | WIS/08/06-JULY-DPP | hep-th | null | We extend Gopakumar's prescription for constructing closed string worldsheets
from free field theory diagrams with adjoint matter to open and closed string
worldsheets arising from free field theories with fundamental matter. We
describe the extension of the gluing mechanism and the electrical circuit
analogy to fund... | [
{
"created": "Sun, 30 Jul 2006 09:13:02 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Aug 2006 10:47:03 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Oct 2006 13:42:18 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Yaakov",
"Itamar",
""
]
] | We extend Gopakumar's prescription for constructing closed string worldsheets from free field theory diagrams with adjoint matter to open and closed string worldsheets arising from free field theories with fundamental matter. We describe the extension of the gluing mechanism and the electrical circuit analogy to fundam... | 14.763251 | 13.912269 | 17.520546 | 13.749031 | 14.140083 | 13.257771 | 15.512565 | 12.891479 | 14.092107 | 15.634776 | 13.67326 | 13.521393 | 14.943056 | 13.664707 | 14.226591 | 13.703814 | 13.37305 | 13.432171 | 13.626832 | 14.958934 | 13.762264 |
hep-th/9803175 | Maria A. Lledo | M.A. Lledo and V.S.V. Varadarajan | SU(2) Poisson-Lie T duality | 12 pages, 1 figure | Lett.Math.Phys. 45 (1998) 247-257 | null | UCLA/98/TEP/12 | hep-th | null | Poisson-Lie target space duality is a framework where duality transformations
are properly defined. In this letter we investigate the pair of sigma models
defined by the double SO(3,1) in the Iwasawa decomposition.
| [
{
"created": "Fri, 20 Mar 1998 23:11:23 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Mar 1998 23:47:53 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Lledo",
"M. A.",
""
],
[
"Varadarajan",
"V. S. V.",
""
]
] | Poisson-Lie target space duality is a framework where duality transformations are properly defined. In this letter we investigate the pair of sigma models defined by the double SO(3,1) in the Iwasawa decomposition. | 16.90926 | 13.321055 | 14.279922 | 12.317202 | 14.477873 | 15.591019 | 13.454329 | 15.148712 | 12.479183 | 17.235895 | 13.171491 | 13.704352 | 14.114367 | 13.717542 | 12.667587 | 13.04593 | 12.550495 | 13.267465 | 12.954901 | 13.722875 | 13.029781 |
hep-th/9306008 | Kurt Haller | K. Haller and E. Lim-Lombridas | Quantum Gauge Equivalence in QED | Contribution for a special issue of Foundations of Physics honoring
Fritz Rohrlich; edited by Larry P. Horwitz, Tel-Aviv University, and Alwyn
van der Merwe, University of Denver (Plenum Publishing, New York); 40 pages,
REVTEX, Preprint UCONN-93-3, 1 figure available upon request from authors | Found.Phys.24:217-247,1994 | 10.1007/BF02313123 | null | hep-th | null | We discuss gauge transformations in QED coupled to a charged spinor field,
and examine whether we can gauge-transform the entire formulation of the theory
from one gauge to another, so that not only the gauge and spinor fields, but
also the forms of the operator-valued Hamiltonians are transformed. The
discussion inc... | [
{
"created": "Tue, 1 Jun 1993 21:12:09 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Haller",
"K.",
""
],
[
"Lim-Lombridas",
"E.",
""
]
] | We discuss gauge transformations in QED coupled to a charged spinor field, and examine whether we can gauge-transform the entire formulation of the theory from one gauge to another, so that not only the gauge and spinor fields, but also the forms of the operator-valued Hamiltonians are transformed. The discussion inclu... | 10.362889 | 11.611496 | 10.413065 | 9.808737 | 11.349003 | 10.985023 | 10.633436 | 10.02486 | 10.712015 | 11.681943 | 10.455719 | 9.902905 | 10.327159 | 9.737803 | 9.940558 | 10.241018 | 10.18605 | 9.997802 | 9.978168 | 10.489509 | 9.7599 |
2304.01776 | Yichao Tang | Song He, Yichao Tang | Jumpstarting (elliptic) symbol integrations for loop integrals | 6 pages including an appendix, several figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive an algorithm for computing the total differentials of multi-loop
integrals expressed as one-fold integrals of multiple polylogarithms, which can
involve square roots of polynomials up to degree four and may evaluate to
(elliptic) multiple polylogarithms ((e)MPL). This gives simple algebraic rules
for comput... | [
{
"created": "Tue, 4 Apr 2023 13:06:40 GMT",
"version": "v1"
}
] | 2023-04-05 | [
[
"He",
"Song",
""
],
[
"Tang",
"Yichao",
""
]
] | We derive an algorithm for computing the total differentials of multi-loop integrals expressed as one-fold integrals of multiple polylogarithms, which can involve square roots of polynomials up to degree four and may evaluate to (elliptic) multiple polylogarithms ((e)MPL). This gives simple algebraic rules for computin... | 10.469225 | 11.186182 | 11.370607 | 10.238541 | 10.687668 | 10.931688 | 10.300589 | 10.335797 | 10.637404 | 12.929461 | 10.275433 | 10.382634 | 10.68568 | 10.015072 | 9.847503 | 9.903415 | 9.996525 | 10.275138 | 9.927251 | 10.931302 | 10.255906 |
0707.0868 | Stephen Wood | Olga V. Manko, Nicholas S. Manton and Stephen W. Wood | Light Nuclei as Quantized Skyrmions | 33 pages, 16 figures, Section 13 replaced | Phys.Rev.C76:055203,2007 | 10.1103/PhysRevC.76.055203 | DAMTP-2007-61 | hep-th nucl-th | null | We consider the rigid body quantization of Skyrmions with topological charges
1 to 8, as approximated by the rational map ansatz. Novel, general expressions
for the elements of the inertia tensors, in terms of the approximating rational
map, are presented and are used to determine the kinetic energy contribution to
t... | [
{
"created": "Thu, 5 Jul 2007 20:00:05 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jul 2007 10:54:52 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Manko",
"Olga V.",
""
],
[
"Manton",
"Nicholas S.",
""
],
[
"Wood",
"Stephen W.",
""
]
] | We consider the rigid body quantization of Skyrmions with topological charges 1 to 8, as approximated by the rational map ansatz. Novel, general expressions for the elements of the inertia tensors, in terms of the approximating rational map, are presented and are used to determine the kinetic energy contribution to the... | 9.423989 | 8.165406 | 10.221625 | 8.372618 | 9.018993 | 8.502082 | 9.409234 | 8.212601 | 8.472209 | 10.112138 | 8.537008 | 8.218574 | 9.260221 | 8.786907 | 8.509857 | 8.844076 | 8.642044 | 8.85416 | 8.446487 | 9.072067 | 8.718165 |
2106.09355 | Victoria Abakumova | V. A. Abakumova and S. L. Lyakhovich | Reducible Stueckelberg symmetry and dualities | 15 pages | null | 10.1016/j.physletb.2021.136552 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a general procedure for iterative inclusion of Stueckelberg fields
to convert the theory into gauge system being equivalent to the original one.
In so doing, we admit reducibility of the Stueckelberg gauge symmetry. In this
case, no pairing exists between Stueckelberg fields and gauge parameters,
unlike th... | [
{
"created": "Thu, 17 Jun 2021 10:17:22 GMT",
"version": "v1"
}
] | 2021-08-04 | [
[
"Abakumova",
"V. A.",
""
],
[
"Lyakhovich",
"S. L.",
""
]
] | We propose a general procedure for iterative inclusion of Stueckelberg fields to convert the theory into gauge system being equivalent to the original one. In so doing, we admit reducibility of the Stueckelberg gauge symmetry. In this case, no pairing exists between Stueckelberg fields and gauge parameters, unlike the ... | 8.805471 | 8.23387 | 9.31093 | 8.312173 | 8.22648 | 8.731213 | 8.82377 | 8.578893 | 8.483768 | 10.071898 | 7.912947 | 8.690355 | 8.669405 | 8.412956 | 8.485495 | 8.44079 | 8.610881 | 8.184782 | 8.538482 | 8.741614 | 8.395099 |
hep-th/9402014 | null | D. Bonatsos, C. Daskaloyannis, D. Ellinas and A. Faessler | Discretization of the phase space for a q-deformed harmonic oscillator
with q a root of unity | 17 pages, Latex file, FTUV/ 93-53, IFIC/ 93-34 | Phys.Lett. B331 (1994) 150-156 | 10.1016/0370-2693(94)90956-3 | null | hep-th | null | The ``position'' and ``momentum'' operators for the q-deformed oscillator
with q being a root of unity are proved to have discrete eigenvalues which are
roots of deformed Hermite polynomials. The Fourier transform connecting the
``position'' and ``momentum'' representations is also found
The phase space of this osc... | [
{
"created": "Thu, 3 Feb 1994 11:27:00 GMT",
"version": "v1"
}
] | 2019-08-15 | [
[
"Bonatsos",
"D.",
""
],
[
"Daskaloyannis",
"C.",
""
],
[
"Ellinas",
"D.",
""
],
[
"Faessler",
"A.",
""
]
] | The ``position'' and ``momentum'' operators for the q-deformed oscillator with q being a root of unity are proved to have discrete eigenvalues which are roots of deformed Hermite polynomials. The Fourier transform connecting the ``position'' and ``momentum'' representations is also found The phase space of this oscilla... | 8.833164 | 9.148646 | 9.548316 | 8.090556 | 10.573836 | 9.769116 | 9.062207 | 8.491124 | 8.555758 | 10.113056 | 8.07318 | 8.538636 | 8.954394 | 8.34315 | 8.172246 | 8.17866 | 8.610749 | 8.417966 | 8.634027 | 8.924998 | 8.520343 |
1911.08295 | Bogus{\l}aw Broda | Bogus{\l}aw Broda | Unitary toy qubit transport model for black hole evaporation | 5 pages, accepted version | Eur. Phys. J. C 80, 418 (2020) | 10.1140/epjc/s10052-020-7947-1 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a recent paper Osuga and Page have presented an explicitly unitary toy
qubit transport model for transferring information from a black hole to the
outgoing radiation. Following their idea we propose a unitary toy model which
involves (fermionic) Hawking states.
| [
{
"created": "Tue, 19 Nov 2019 14:34:04 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Nov 2019 12:08:56 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Nov 2019 15:14:53 GMT",
"version": "v3"
},
{
"created": "Thu, 5 Dec 2019 15:35:15 GMT",
"version": "v4"
},
{
"cr... | 2021-01-01 | [
[
"Broda",
"Bogusław",
""
]
] | In a recent paper Osuga and Page have presented an explicitly unitary toy qubit transport model for transferring information from a black hole to the outgoing radiation. Following their idea we propose a unitary toy model which involves (fermionic) Hawking states. | 31.82209 | 16.341862 | 29.463747 | 16.820898 | 17.254684 | 19.344347 | 15.592305 | 15.4681 | 15.913697 | 27.211908 | 19.867849 | 19.665218 | 22.224012 | 21.674606 | 21.393961 | 20.07542 | 21.084225 | 19.343359 | 22.723276 | 21.711285 | 22.749989 |
1112.2119 | Dankrad T.J. Feist | Dankrad T.J. Feist | Interactions of B = 4 Skyrmions | 21 pages, 11 figures | null | 10.1007/JHEP02(2012)100 | DAMTP-2011-105 | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is known that the interactions of single Skyrmions are asymptotically
described by a Yukawa dipole potential. Less is known about the interactions of
solutions of the Skyrme model with higher baryon number. In this paper, it is
shown that Yukawa multipole theory can be more generally applied to Skyrmion
interactio... | [
{
"created": "Fri, 9 Dec 2011 15:27:58 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Feist",
"Dankrad T. J.",
""
]
] | It is known that the interactions of single Skyrmions are asymptotically described by a Yukawa dipole potential. Less is known about the interactions of solutions of the Skyrme model with higher baryon number. In this paper, it is shown that Yukawa multipole theory can be more generally applied to Skyrmion interactions... | 8.557211 | 9.183809 | 8.402444 | 8.232716 | 8.298244 | 8.473647 | 8.54978 | 8.334627 | 7.993527 | 8.759468 | 7.781922 | 8.476266 | 8.285811 | 8.311033 | 8.066241 | 8.26156 | 8.205816 | 8.065487 | 8.136151 | 8.203856 | 8.195687 |
hep-th/9506166 | Hyeonjoon Shin | Hyeonjoon Shin, Young-Jai Park, Yongduk Kim, and Won T. Kim | On the anomaly of nonlocal symmetry in the chiral QED | 4 pages, latex, no figures | J.KoreanPhys.Soc.29:392-393,1996 | null | SOGANG-HEP-200/95 | hep-th | null | We show that the anomaly of nonlocal symmetry can be canceled by the
well-known Wess-Zumino acton which cancels the gauge anomaly in the
two-dimensional chiral electrodynamics.
| [
{
"created": "Mon, 26 Jun 1995 07:55:54 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Shin",
"Hyeonjoon",
""
],
[
"Park",
"Young-Jai",
""
],
[
"Kim",
"Yongduk",
""
],
[
"Kim",
"Won T.",
""
]
] | We show that the anomaly of nonlocal symmetry can be canceled by the well-known Wess-Zumino acton which cancels the gauge anomaly in the two-dimensional chiral electrodynamics. | 16.578129 | 13.582787 | 13.477666 | 11.549101 | 11.717497 | 11.543983 | 11.905417 | 13.255415 | 12.707316 | 13.810349 | 11.692612 | 13.704522 | 14.292953 | 14.021607 | 13.663278 | 12.345881 | 12.339803 | 12.060322 | 13.270021 | 15.421041 | 12.433846 |
hep-th/9911162 | Max Chaves | M. Chaves and H. Morales | Grand unification using a generalized Yang-Mills theory | 10 pages, no figures | Mod.Phys.Lett. A15 (2000) 197-206 | 10.1142/S0217732300000190 | null | hep-th | null | Generalized Yang-Mills theories have a covariant derivative that employs both
scalar and vector bosons. Here we show how grand unified theories of the
electroweak and strong interactions can be constructed with them. In particular
the SU(5) GUT can be obtained from SU(6) with SU(5)xU(1) as a maximal subgroup.
The cho... | [
{
"created": "Sat, 20 Nov 1999 03:39:25 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Chaves",
"M.",
""
],
[
"Morales",
"H.",
""
]
] | Generalized Yang-Mills theories have a covariant derivative that employs both scalar and vector bosons. Here we show how grand unified theories of the electroweak and strong interactions can be constructed with them. In particular the SU(5) GUT can be obtained from SU(6) with SU(5)xU(1) as a maximal subgroup. The choic... | 7.692513 | 7.135923 | 7.131159 | 6.978933 | 7.010727 | 7.581878 | 7.603891 | 7.077317 | 6.734025 | 7.213403 | 7.196981 | 7.187137 | 7.157394 | 7.106003 | 7.197991 | 7.159225 | 7.436467 | 7.173443 | 7.319582 | 7.176496 | 7.232117 |
1303.1803 | Xiao-Gang Wen | Xiao-Gang Wen | Classifying gauge anomalies through SPT orders and classifying
gravitational anomalies through topological orders | 23 pages, RevTeX4, 3 figures, 1 table | Phys. Rev. D 88, 045013 (2013) | 10.1103/PhysRevD.88.045013 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we systematically study gauge anomalies in bosonic and
fermionic weak-coupling gauge theories with gauge group G (which can be
continuous or discrete). We show a very close relation between gauge anomalies
and symmetry-protected trivial (SPT) orders [also known as symmetry-protected
topological (SPT) o... | [
{
"created": "Thu, 7 Mar 2013 20:38:08 GMT",
"version": "v1"
},
{
"created": "Sun, 28 Apr 2013 14:19:19 GMT",
"version": "v2"
},
{
"created": "Sun, 5 May 2013 18:59:02 GMT",
"version": "v3"
},
{
"created": "Tue, 30 Jul 2013 14:52:26 GMT",
"version": "v4"
}
] | 2013-11-19 | [
[
"Wen",
"Xiao-Gang",
""
]
] | In this paper, we systematically study gauge anomalies in bosonic and fermionic weak-coupling gauge theories with gauge group G (which can be continuous or discrete). We show a very close relation between gauge anomalies and symmetry-protected trivial (SPT) orders [also known as symmetry-protected topological (SPT) ord... | 6.059124 | 6.650289 | 7.089675 | 6.299531 | 7.366465 | 6.530616 | 6.752942 | 6.331208 | 6.332629 | 7.474798 | 6.372956 | 6.138487 | 6.16515 | 5.843551 | 5.983536 | 5.983057 | 5.944991 | 5.959969 | 5.996601 | 5.8784 | 5.928553 |
0805.0403 | Branko Dragovich | Branko Dragovich | Some Lagrangians with Zeta Function Nonlocality | 11 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Some nonlocal and nonpolynomial scalar field models originated from p-adic
string theory are considered. Infinite number of spacetime derivatives is
governed by the Riemann zeta function through d'Alembertian $\Box$ in its
argument. Construction of the corresponding Lagrangians begins with the exact
Lagrangian for ef... | [
{
"created": "Sun, 4 May 2008 11:28:07 GMT",
"version": "v1"
}
] | 2008-05-06 | [
[
"Dragovich",
"Branko",
""
]
] | Some nonlocal and nonpolynomial scalar field models originated from p-adic string theory are considered. Infinite number of spacetime derivatives is governed by the Riemann zeta function through d'Alembertian $\Box$ in its argument. Construction of the corresponding Lagrangians begins with the exact Lagrangian for effe... | 12.278488 | 12.346636 | 12.290648 | 11.634213 | 12.035713 | 12.219298 | 12.571842 | 11.444919 | 11.154841 | 12.348016 | 11.160049 | 10.943446 | 12.266816 | 11.343468 | 10.883938 | 11.012436 | 10.987137 | 11.186748 | 10.750379 | 11.734246 | 10.819448 |
hep-th/0412099 | Andrei Mironov | A.Alexandrov, A.Mironov and A.Morozov | Unified description of correlators in non-Gaussian phases of Hermitean
matrix model | 29 pages, LaTeX | Int.J.Mod.Phys.A21:2481-2518,2006 | 10.1142/S0217751X06029375 | null | hep-th | null | Following the program, proposed in hep-th/0310113, of systematizing known
properties of matrix model partition functions (defined as solutions to the
Virasoro-like sets of linear differential equations), we proceed to
consideration of non-Gaussian phases of the Hermitean one-matrix model. A
unified approach is propos... | [
{
"created": "Thu, 9 Dec 2004 16:48:38 GMT",
"version": "v1"
}
] | 2009-05-01 | [
[
"Alexandrov",
"A.",
""
],
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | Following the program, proposed in hep-th/0310113, of systematizing known properties of matrix model partition functions (defined as solutions to the Virasoro-like sets of linear differential equations), we proceed to consideration of non-Gaussian phases of the Hermitean one-matrix model. A unified approach is proposed... | 27.495447 | 25.376488 | 29.543684 | 24.361492 | 24.427736 | 24.671545 | 24.331417 | 22.459913 | 24.264727 | 30.531281 | 23.977558 | 23.811161 | 24.715023 | 23.111036 | 22.95727 | 23.463205 | 23.233864 | 23.124762 | 23.724329 | 25.902264 | 23.503696 |
1905.06409 | Hong Lu | Hai-Shan Liu and H. Lu | Action Growth of Dyonic Black Holes and Electromagnetic Duality | Latex, 26 pages, references added | null | 10.1007/JHEP09(2019)102 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Electromagnetic duality of Maxwell theory is a symmetry of equations but not
of the action. The usual application of the `complexity=action' conjecture
would thus loose this duality. It was recently proposed in arxiv:1901.00014
that the duality can be restored by adding some appropriate boundary term, at
the price of... | [
{
"created": "Wed, 15 May 2019 19:38:55 GMT",
"version": "v1"
},
{
"created": "Tue, 28 May 2019 02:16:40 GMT",
"version": "v2"
}
] | 2019-10-02 | [
[
"Liu",
"Hai-Shan",
""
],
[
"Lu",
"H.",
""
]
] | Electromagnetic duality of Maxwell theory is a symmetry of equations but not of the action. The usual application of the `complexity=action' conjecture would thus loose this duality. It was recently proposed in arxiv:1901.00014 that the duality can be restored by adding some appropriate boundary term, at the price of i... | 8.82413 | 8.910194 | 8.81747 | 7.62507 | 9.009971 | 8.435725 | 8.68782 | 7.91799 | 7.753798 | 9.29917 | 8.54751 | 8.581197 | 8.575411 | 8.498755 | 8.821625 | 8.30457 | 8.363802 | 8.315244 | 8.480832 | 8.794832 | 8.406219 |
2112.09597 | Arthur Lipstein | Theresa Abl, Paul Heslop, Arthur E. Lipstein | Higher-Dimensional Symmetry of AdS$_2\times$S$^2$ Correlators | v2. published in JHEP | null | 10.1007/JHEP03(2022)076 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | It was recently shown that IIB supergravity on AdS$_5\times$S$^5$ enjoys 10d
conformal symmetry and that superstring theory on this background can be
described using a 10d scalar effective field theory. In this paper we adapt
these two complementary approaches to correlators of hypermultiplets in
AdS$_2\times$S$^2$. ... | [
{
"created": "Fri, 17 Dec 2021 16:14:51 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Mar 2022 13:34:03 GMT",
"version": "v2"
}
] | 2022-03-30 | [
[
"Abl",
"Theresa",
""
],
[
"Heslop",
"Paul",
""
],
[
"Lipstein",
"Arthur E.",
""
]
] | It was recently shown that IIB supergravity on AdS$_5\times$S$^5$ enjoys 10d conformal symmetry and that superstring theory on this background can be described using a 10d scalar effective field theory. In this paper we adapt these two complementary approaches to correlators of hypermultiplets in AdS$_2\times$S$^2$. In... | 7.00135 | 6.692695 | 7.74851 | 6.58606 | 7.000985 | 6.907716 | 6.82642 | 6.678689 | 6.551661 | 7.636564 | 6.582845 | 6.484674 | 6.881224 | 6.437912 | 6.538857 | 6.578143 | 6.561118 | 6.664213 | 6.447217 | 6.819262 | 6.37885 |
2405.01433 | Leihua Liu | Tao Li and Lei-Hua Liu | Inflationary complexity of thermal state | 48 pages, 18 figures, references updated, typos corrected | null | null | null | hep-th astro-ph.CO gr-qc hep-ph quant-ph | http://creativecommons.org/licenses/by/4.0/ | In this work, we systematically investigate the inflationary complexity of
the two-mode squeezed state with thermal effect for the single field inflation,
modified dispersion relation, and non-trivial sound speed with the method of
closed system and open system, respectively. Since the various quantum
gravitational f... | [
{
"created": "Thu, 2 May 2024 16:22:59 GMT",
"version": "v1"
},
{
"created": "Mon, 6 May 2024 16:02:58 GMT",
"version": "v2"
}
] | 2024-05-07 | [
[
"Li",
"Tao",
""
],
[
"Liu",
"Lei-Hua",
""
]
] | In this work, we systematically investigate the inflationary complexity of the two-mode squeezed state with thermal effect for the single field inflation, modified dispersion relation, and non-trivial sound speed with the method of closed system and open system, respectively. Since the various quantum gravitational fra... | 11.014426 | 11.499184 | 11.214478 | 10.339747 | 11.53878 | 10.80417 | 11.240204 | 10.415261 | 10.527195 | 11.91209 | 10.208034 | 10.646996 | 10.611894 | 10.423855 | 10.520208 | 10.741323 | 10.56069 | 10.563574 | 10.364071 | 10.576345 | 10.501078 |
0902.2729 | Osvaldo Chandia | Osvaldo Chandia | A Note on T-dualities in the Pure Spinor Heterotic String | References added | JHEP 0904:104,2009 | 10.1088/1126-6708/2009/04/104 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we study the preservation of the classical pure spinor BRST
constraints under super T-duality transformations. We also determine the
invariance of the one-loop conformal invariance and of the local gauge and
Lorentz anomalies under the super T-dualities.
| [
{
"created": "Mon, 16 Feb 2009 16:32:31 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Feb 2009 14:54:52 GMT",
"version": "v2"
}
] | 2010-12-09 | [
[
"Chandia",
"Osvaldo",
""
]
] | In this note we study the preservation of the classical pure spinor BRST constraints under super T-duality transformations. We also determine the invariance of the one-loop conformal invariance and of the local gauge and Lorentz anomalies under the super T-dualities. | 11.857682 | 8.64639 | 14.527003 | 8.720664 | 7.627323 | 8.171011 | 8.111422 | 9.389149 | 8.460471 | 14.416987 | 8.423722 | 9.722075 | 10.752769 | 9.332408 | 9.234715 | 9.273748 | 9.031545 | 8.546792 | 9.160753 | 10.985887 | 8.768634 |
hep-th/0603196 | Ilka Brunner | Ilka Brunner, Matthias R. Gaberdiel, Christoph A. Keller | Matrix factorisations and D-branes on K3 | 35 pages, no figures | JHEP0606:015,2006 | 10.1088/1126-6708/2006/06/015 | null | hep-th | null | D-branes on K3 are analysed from three different points of view. For
deformations of hypersurfaces in weighted projected space we use geometrical
methods as well as matrix factorisation techniques. Furthermore, we study the
D-branes on the T^4/\Z_4 orbifold line in conformal field theory. The behaviour
of the D-brane... | [
{
"created": "Sun, 26 Mar 2006 20:04:04 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Brunner",
"Ilka",
""
],
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Keller",
"Christoph A.",
""
]
] | D-branes on K3 are analysed from three different points of view. For deformations of hypersurfaces in weighted projected space we use geometrical methods as well as matrix factorisation techniques. Furthermore, we study the D-branes on the T^4/\Z_4 orbifold line in conformal field theory. The behaviour of the D-branes ... | 11.071166 | 10.248534 | 11.860939 | 9.745723 | 10.425217 | 10.594484 | 9.807017 | 9.106628 | 9.307623 | 11.69926 | 9.281096 | 8.82754 | 10.183761 | 9.126 | 9.12257 | 8.729674 | 8.857072 | 9.054005 | 8.845565 | 9.812716 | 8.780589 |
1210.4179 | Sebastian Halter | Johanna Erdmenger, Sebastian Halter, Carlos Nunez, Gianmassimo
Tasinato | Slow-walking inflation | 16 pages + appendices; reference added | null | 10.1088/1475-7516/2013/01/006 | MPP-2012-138; LMU-ASC 74/12 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new model of slow-roll inflation in string cosmology, based on
warped throat supergravity solutions displaying `walking' dynamics, i.e. the
coupling constant of the dual gauge theory slowly varies over a range of energy
scales. The features of the throat geometry are sourced by a rich field
content, give... | [
{
"created": "Mon, 15 Oct 2012 20:05:30 GMT",
"version": "v1"
},
{
"created": "Sat, 27 Oct 2012 18:38:50 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Erdmenger",
"Johanna",
""
],
[
"Halter",
"Sebastian",
""
],
[
"Nunez",
"Carlos",
""
],
[
"Tasinato",
"Gianmassimo",
""
]
] | We propose a new model of slow-roll inflation in string cosmology, based on warped throat supergravity solutions displaying `walking' dynamics, i.e. the coupling constant of the dual gauge theory slowly varies over a range of energy scales. The features of the throat geometry are sourced by a rich field content, given ... | 10.521184 | 10.374703 | 11.065669 | 10.663801 | 10.633733 | 11.146833 | 10.57612 | 10.014361 | 9.924707 | 11.282341 | 10.211148 | 10.317356 | 10.484493 | 10.1469 | 10.485224 | 10.353603 | 10.228937 | 10.262754 | 10.440632 | 10.864472 | 10.1239 |
hep-th/0611333 | J. David Vergara | Vladimir Cuesta, Merced Montesinos, Jose David Vergara | Gauge systems with noncommutative phase space | 5 pages | null | null | null | hep-th | null | Some very simple models of gauge systems with noncanonical symplectic
structures having $sl(2,r)$ as the gauge algebra are given. The models can be
interpreted as noncommutative versions of the usual $SL(2,\mathbb{R})$ model of
Montesinos-Rovelli-Thiemann. The symplectic structures of the noncommutative
models, the f... | [
{
"created": "Wed, 29 Nov 2006 21:15:19 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Cuesta",
"Vladimir",
""
],
[
"Montesinos",
"Merced",
""
],
[
"Vergara",
"Jose David",
""
]
] | Some very simple models of gauge systems with noncanonical symplectic structures having $sl(2,r)$ as the gauge algebra are given. The models can be interpreted as noncommutative versions of the usual $SL(2,\mathbb{R})$ model of Montesinos-Rovelli-Thiemann. The symplectic structures of the noncommutative models, the fir... | 6.880062 | 6.710339 | 6.756374 | 6.3221 | 7.003025 | 6.921331 | 6.691148 | 6.496178 | 6.592056 | 7.364993 | 6.505563 | 6.578326 | 6.599203 | 6.550831 | 6.488989 | 6.407268 | 6.563761 | 6.5014 | 6.676126 | 6.614614 | 6.640476 |
0712.2557 | Wenfeng Chen WFC | W.F. Chen | A Note on the Radiatively Induced Lorentz and CPT Violated
Chern-Simons-like Term in the Extended Quantum Electrodynamics | 9 pages, RevTex 4, no figure, some misprints are corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the ambiguity for the Chern-Simons-like term induced from
quantum correction in the extended QED should have nothing to do with the
approximation on the exact fermionic propagator, contradictory to the claim in
Ref.[19]. Further, we investigate the induced Chern-Simons-like term using the
original 't Hoo... | [
{
"created": "Sun, 16 Dec 2007 06:13:00 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jul 2009 23:42:34 GMT",
"version": "v2"
}
] | 2009-07-10 | [
[
"Chen",
"W. F.",
""
]
] | We show that the ambiguity for the Chern-Simons-like term induced from quantum correction in the extended QED should have nothing to do with the approximation on the exact fermionic propagator, contradictory to the claim in Ref.[19]. Further, we investigate the induced Chern-Simons-like term using the original 't Hooft... | 15.762466 | 13.387964 | 13.212961 | 13.3193 | 13.053823 | 13.678137 | 13.137976 | 13.453709 | 12.424466 | 14.25701 | 12.903739 | 13.492793 | 13.809964 | 13.067004 | 14.126954 | 13.756753 | 13.386576 | 13.107274 | 13.425966 | 13.291134 | 13.348751 |
hep-th/0005064 | Toyohiro Tsurumaru | Toyohiro Tsurumaru, Izumi Tsutsui, Akira Fujii | Instantons, Monopoles and the Flux Quantization in the Faddeev-Niemi
Decomposition | Tex, 12 pages, 3 figures (eps), references added | Nucl.Phys. B589 (2000) 659-668 | 10.1016/S0550-3213(00)00538-1 | KEK Preprint 2000-18 | hep-th | null | We study how instantons arise in the low energy effective theory of the SU(2)
Yang-Mills theory in the context of the non-linear sigma model recently propose
by Faddeev and Niemi. We find a simple relation between the instanton number
$\nu$ and the charge m of the monopole that appears in the effective theory. It
is ... | [
{
"created": "Mon, 8 May 2000 06:11:53 GMT",
"version": "v1"
},
{
"created": "Tue, 9 May 2000 05:21:58 GMT",
"version": "v2"
},
{
"created": "Tue, 23 May 2000 04:38:35 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Tsurumaru",
"Toyohiro",
""
],
[
"Tsutsui",
"Izumi",
""
],
[
"Fujii",
"Akira",
""
]
] | We study how instantons arise in the low energy effective theory of the SU(2) Yang-Mills theory in the context of the non-linear sigma model recently propose by Faddeev and Niemi. We find a simple relation between the instanton number $\nu$ and the charge m of the monopole that appears in the effective theory. It is gi... | 6.314816 | 5.799089 | 6.514926 | 5.684145 | 5.244648 | 5.525623 | 5.785357 | 5.648068 | 5.682852 | 6.597996 | 5.521578 | 5.69188 | 6.12947 | 5.940135 | 5.814291 | 5.916423 | 5.695063 | 5.722678 | 5.834772 | 6.027804 | 5.756733 |
hep-th/0303233 | null | S.L.Dubovsky, S.M.Sibiryakov | Domain walls between gauge theories | Final version; minor corrections; to appear in Nucl.Phys.B | Nucl.Phys. B664 (2003) 407-438 | 10.1016/S0550-3213(03)00407-3 | null | hep-th | null | Noncommutative U(N) gauge theories at different N may be often thought of as
different sectors of a single theory: the U(1) theory possesses a sequence of
vacua labeled by an integer parameter N, and the theory in the vicinity of the
N-th vacuum coincides with the U(N) noncommutative gauge theory. We construct
noncom... | [
{
"created": "Wed, 26 Mar 2003 20:46:09 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Jun 2003 11:10:46 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dubovsky",
"S. L.",
""
],
[
"Sibiryakov",
"S. M.",
""
]
] | Noncommutative U(N) gauge theories at different N may be often thought of as different sectors of a single theory: the U(1) theory possesses a sequence of vacua labeled by an integer parameter N, and the theory in the vicinity of the N-th vacuum coincides with the U(N) noncommutative gauge theory. We construct noncommu... | 11.248394 | 11.067237 | 11.872987 | 10.586225 | 10.360974 | 10.490593 | 11.214234 | 11.12707 | 9.658359 | 12.429391 | 10.771793 | 10.369992 | 10.886967 | 10.234008 | 10.668167 | 10.575132 | 10.63784 | 10.330725 | 10.757147 | 10.705512 | 10.44673 |
2203.08164 | Brian McPeak | Johan Henriksson, Brian McPeak, Francesco Russo, Alessandro Vichi | Bounding Violations of the Weak Gravity Conjecture | 55 pp | null | 10.1007/JHEP08(2022)184 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The black hole weak gravity conjecture (WGC) is a set of linear inequalities
on the four-derivative corrections to Einstein--Maxwell theory. Remarkably, in
four dimensions, these combinations appear in the $2 \to 2$ photon amplitudes,
leading to the hope that the conjecture might be supported using dispersion
relatio... | [
{
"created": "Tue, 15 Mar 2022 18:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Apr 2022 18:58:30 GMT",
"version": "v2"
}
] | 2022-09-07 | [
[
"Henriksson",
"Johan",
""
],
[
"McPeak",
"Brian",
""
],
[
"Russo",
"Francesco",
""
],
[
"Vichi",
"Alessandro",
""
]
] | The black hole weak gravity conjecture (WGC) is a set of linear inequalities on the four-derivative corrections to Einstein--Maxwell theory. Remarkably, in four dimensions, these combinations appear in the $2 \to 2$ photon amplitudes, leading to the hope that the conjecture might be supported using dispersion relations... | 9.459245 | 9.886605 | 10.298025 | 8.963121 | 9.456719 | 9.540035 | 10.041938 | 9.437014 | 8.810938 | 10.874761 | 9.025269 | 9.006701 | 9.414504 | 8.967329 | 8.998563 | 9.05824 | 8.995185 | 8.880532 | 8.940053 | 9.432821 | 8.835346 |
0705.0319 | Salvatore Capozziello | A. Capolupo, S. Capozziello, G. Vitiello | Dark energy, cosmological constant and neutrino mixing | 10 pages, 2 figures | Int.J.Mod.Phys.A23:4979-4990,2009 | 10.1142/S0217751X08042857 | null | hep-th gr-qc | null | The today estimated value of dark energy can be achieved by the vacuum
condensate induced by neutrino mixing phenomenon. Such a tiny value is
recovered for a cut-off of the order of Planck scale and it is linked to the
sub eV neutrino mass scale. Contributions to dark energy from auxiliary fields
or mechanisms are no... | [
{
"created": "Wed, 2 May 2007 16:06:21 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Capolupo",
"A.",
""
],
[
"Capozziello",
"S.",
""
],
[
"Vitiello",
"G.",
""
]
] | The today estimated value of dark energy can be achieved by the vacuum condensate induced by neutrino mixing phenomenon. Such a tiny value is recovered for a cut-off of the order of Planck scale and it is linked to the sub eV neutrino mass scale. Contributions to dark energy from auxiliary fields or mechanisms are not ... | 23.396856 | 16.922354 | 16.049393 | 16.243332 | 16.10014 | 17.042562 | 15.871456 | 15.569277 | 16.342852 | 17.452799 | 18.374819 | 17.286119 | 17.398224 | 18.147665 | 17.344948 | 17.874176 | 16.853289 | 16.771547 | 17.745052 | 16.162434 | 18.499678 |
0707.1595 | Eran Palti | Eran Palti | Low Energy Supersymmetry from Non-Geometry | 36pp; v2 references added, minor clarifications, JHEP version | JHEP 0710:011,2007 | 10.1088/1126-6708/2007/10/011 | null | hep-th | null | We study a class of flux compactifications that have all the moduli
stabilised, a high (GUT) string scale and a low (TeV) gravitino mass that is
generated dynamically. These non-geometric compactifications correspond to type
II string theories on SU(3)xSU(3) structure orientifolds. The resulting
superpotentials admit... | [
{
"created": "Wed, 11 Jul 2007 11:15:51 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Oct 2007 17:10:56 GMT",
"version": "v2"
}
] | 2009-04-30 | [
[
"Palti",
"Eran",
""
]
] | We study a class of flux compactifications that have all the moduli stabilised, a high (GUT) string scale and a low (TeV) gravitino mass that is generated dynamically. These non-geometric compactifications correspond to type II string theories on SU(3)xSU(3) structure orientifolds. The resulting superpotentials admit, ... | 7.080776 | 7.195834 | 7.518533 | 6.494852 | 6.568681 | 7.027406 | 6.506703 | 6.492558 | 6.519832 | 7.790469 | 6.50348 | 6.354369 | 7.295727 | 6.606212 | 6.663494 | 6.532218 | 6.378674 | 6.581591 | 6.54633 | 7.113137 | 6.298825 |
hep-th/9710004 | Sunil Mukhi | Sunil Mukhi | Orientifolds: The Unique Personality Of Each Spacetime Dimension | harvmac, 15 pages (b), one eps figure; Review based on talks given at
Puri (Dec 1996) and Paris (Aug 1997) | null | null | TIFR/TH/97-54 | hep-th | null | I review some recent developments in our understanding of the dynamics of Z_2
orientifolds of type IIA and IIB strings and M-theory. Interesting physical
phenomena that occur in each spacetime dimension from 10 to 1 are summarized,
along with some relationships to nonperturbative effects and to M- and
F-theory. The c... | [
{
"created": "Wed, 1 Oct 1997 10:00:42 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Mukhi",
"Sunil",
""
]
] | I review some recent developments in our understanding of the dynamics of Z_2 orientifolds of type IIA and IIB strings and M-theory. Interesting physical phenomena that occur in each spacetime dimension from 10 to 1 are summarized, along with some relationships to nonperturbative effects and to M- and F-theory. The con... | 9.211644 | 9.442107 | 10.134456 | 8.520535 | 9.915431 | 9.797553 | 9.286874 | 9.050947 | 9.003331 | 10.214852 | 8.679215 | 8.526577 | 8.787618 | 8.383566 | 8.232027 | 8.276796 | 8.63185 | 8.357802 | 8.396905 | 9.124401 | 8.647256 |
1201.3471 | Emil Akhmedov | E. T. Akhmedov and A. V. Sadofyev | Comparative study of loop contributions in AdS and dS | 12 pages. Minor changes, misprints are corrected | null | 10.1016/j.physletb.2012.04.061 | ITEP-TH-2/12; AEI-2012-004 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The generic feature of non-conformal fields in Poincare patch of de Sitter
space is the presence of large IR loop corrections even for massive fields.
Moreover, in global de Sitter there are loop IR divergences for the massive
fields. Naive analytic continuation from de Sitter to Anti-de-Sitter might lead
one to conc... | [
{
"created": "Tue, 17 Jan 2012 10:16:49 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Feb 2012 11:46:55 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Akhmedov",
"E. T.",
""
],
[
"Sadofyev",
"A. V.",
""
]
] | The generic feature of non-conformal fields in Poincare patch of de Sitter space is the presence of large IR loop corrections even for massive fields. Moreover, in global de Sitter there are loop IR divergences for the massive fields. Naive analytic continuation from de Sitter to Anti-de-Sitter might lead one to conclu... | 7.284588 | 6.785964 | 7.462031 | 6.755051 | 6.76047 | 6.750766 | 7.013439 | 6.639419 | 6.648332 | 8.153152 | 6.65147 | 7.020436 | 6.915874 | 6.895372 | 6.950849 | 6.873939 | 7.15215 | 7.012289 | 6.842049 | 7.068586 | 6.880638 |
2111.05295 | Marcel Hughes | Bin Guo, Marcel R. R. Hughes, Samir D. Mathur, Madhur Mehta | Contrasting the fuzzball and wormhole paradigms for black holes | 79 pages, 20 figures; v2: some references modified and clarifications
added | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We examine an interesting set of recent proposals describing a `wormhole
paradigm' for black holes. These proposals require that in some effective
variables, semiclassical low-energy dynamics emerges at the horizon. We prove
the `effective small corrections theorem' to show that such an effective
horizon behavior is ... | [
{
"created": "Tue, 9 Nov 2021 17:56:57 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Nov 2021 16:52:36 GMT",
"version": "v2"
}
] | 2021-11-16 | [
[
"Guo",
"Bin",
""
],
[
"Hughes",
"Marcel R. R.",
""
],
[
"Mathur",
"Samir D.",
""
],
[
"Mehta",
"Madhur",
""
]
] | We examine an interesting set of recent proposals describing a `wormhole paradigm' for black holes. These proposals require that in some effective variables, semiclassical low-energy dynamics emerges at the horizon. We prove the `effective small corrections theorem' to show that such an effective horizon behavior is no... | 12.648602 | 12.587528 | 14.509056 | 12.692151 | 14.078648 | 12.978065 | 13.543516 | 13.03796 | 12.41656 | 15.396158 | 11.948545 | 12.064317 | 12.522169 | 12.417171 | 12.365528 | 12.771145 | 12.363966 | 12.585899 | 12.157842 | 12.910351 | 12.080714 |
1502.04008 | Anzor Khelashvili A. | Anzor Khelashvili and Teimuraz Nadareishvili | Singular Behavior of the Laplace Operator in Polar Spherical Coordinates
and Some of Its Consequences for the Radial Wave Function at the Origin of
Coordinates | 23 pages | Physics of Particles and Nuclei Letters. vol.12.pp11-25 (2015) | 10.1134/S1547477115010148 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Singular behavior of the Laplace operator in spherical coordinates is
investigated. It is shown that in course of transition to the reduced radial
wave function in the Schrodinger equation there appears additional term
consisting the Dirac delta function, which was unnoted during the full history
of physics and mathe... | [
{
"created": "Fri, 13 Feb 2015 14:43:21 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Khelashvili",
"Anzor",
""
],
[
"Nadareishvili",
"Teimuraz",
""
]
] | Singular behavior of the Laplace operator in spherical coordinates is investigated. It is shown that in course of transition to the reduced radial wave function in the Schrodinger equation there appears additional term consisting the Dirac delta function, which was unnoted during the full history of physics and mathema... | 14.911564 | 15.714365 | 13.239474 | 13.517715 | 13.669171 | 14.598611 | 14.85366 | 13.907167 | 14.615121 | 14.781717 | 14.44981 | 13.5396 | 13.150172 | 13.007062 | 12.858121 | 13.434819 | 12.703342 | 13.315607 | 13.1554 | 13.388509 | 13.52265 |
hep-th/0010005 | Christian Schubert | B. Eden, C. Schubert, E. Sokatchev | Four - Point Functions of Chiral Primary Operators in N=4 SYM | 7 pages, talk given by C. Schubert at "Quantization, Gauge Theory and
Strings", dedicated to the memory of E.S. Fradkin, Moscow, June 5-10, 2000 | null | null | LAPTH-Conf-814/99 | hep-th | null | We discuss recent progress in the determination of correlators of chiral
primary operators in N=4 Super-Yang-Mills theory, based on a combination of
superconformal covariance arguments in N=2 harmonic superspace, and
Intriligator's insertion formula. Applying this technique to the calculation of
the supercurrent four... | [
{
"created": "Sun, 1 Oct 2000 14:19:43 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Eden",
"B.",
""
],
[
"Schubert",
"C.",
""
],
[
"Sokatchev",
"E.",
""
]
] | We discuss recent progress in the determination of correlators of chiral primary operators in N=4 Super-Yang-Mills theory, based on a combination of superconformal covariance arguments in N=2 harmonic superspace, and Intriligator's insertion formula. Applying this technique to the calculation of the supercurrent four -... | 13.520786 | 11.538753 | 16.156319 | 11.030694 | 11.180378 | 11.402409 | 11.050837 | 10.483131 | 11.270934 | 15.766473 | 10.617117 | 11.085659 | 13.450261 | 11.67641 | 11.403732 | 11.206331 | 11.544644 | 11.515351 | 11.490222 | 13.653658 | 11.458307 |
1301.6020 | Milena Smolic | Milena Smolic | Holography and hydrodynamics for EMD theory with two Maxwell fields | 50 pages, no figures | null | 10.1007/JHEP03(2013)124 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use `generalized dimensional reduction' to relate a specific
Einstein-Maxwell-Dilaton (EMD) theory, including two gauge fields, three
neutral scalars and an axion, to higher-dimensional AdS gravity (with no
higher-dimensional Maxwell field). In general, this is a dimensional reduction
over compact Einstein spaces ... | [
{
"created": "Fri, 25 Jan 2013 11:54:28 GMT",
"version": "v1"
}
] | 2015-06-12 | [
[
"Smolic",
"Milena",
""
]
] | We use `generalized dimensional reduction' to relate a specific Einstein-Maxwell-Dilaton (EMD) theory, including two gauge fields, three neutral scalars and an axion, to higher-dimensional AdS gravity (with no higher-dimensional Maxwell field). In general, this is a dimensional reduction over compact Einstein spaces in... | 10.116871 | 10.473807 | 11.270442 | 10.018332 | 10.199888 | 10.689689 | 10.026313 | 10.417582 | 9.617133 | 11.939213 | 9.544324 | 9.887159 | 9.955132 | 9.463527 | 9.448442 | 9.716332 | 9.585753 | 9.521854 | 9.416874 | 9.911081 | 9.65317 |
1107.3157 | Sarah Folkerts | Sarah Folkerts, Alexander Pritzel and Nico Wintergerst | On ghosts in theories of self-interacting massive spin-2 particles | 13 pages, no figures; v2: references adjusted | null | null | LMU-ASC 30/11 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider general theories of a massive spin-2 particle $h_{\mu\nu}$ on a
Minkowski background. A decomposition of $h_{\mu\nu}$ in terms of helicity
eigenstates allows us to directly test whether any given theory possesses a
consistent description as a massive spin-2 representation of the Poincar\'e
group. We demon... | [
{
"created": "Fri, 15 Jul 2011 20:06:55 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Aug 2011 17:15:04 GMT",
"version": "v2"
}
] | 2011-08-03 | [
[
"Folkerts",
"Sarah",
""
],
[
"Pritzel",
"Alexander",
""
],
[
"Wintergerst",
"Nico",
""
]
] | We consider general theories of a massive spin-2 particle $h_{\mu\nu}$ on a Minkowski background. A decomposition of $h_{\mu\nu}$ in terms of helicity eigenstates allows us to directly test whether any given theory possesses a consistent description as a massive spin-2 representation of the Poincar\'e group. We demonst... | 7.079524 | 6.777813 | 6.596451 | 6.225551 | 6.89366 | 7.194974 | 6.676903 | 6.506158 | 6.202066 | 7.18421 | 6.562359 | 6.860448 | 6.210968 | 6.278671 | 6.520571 | 6.589788 | 6.50088 | 6.466935 | 6.265512 | 6.412942 | 6.356046 |
1012.3736 | Andrea Borghese | Andrea Borghese, Diederik Roest | Metastable supersymmetry breaking in extended supergravity | 27 pages. v2 correct replacement: typos corrected and clarifications
added on gauge invariance and dependence on SUSY mass terms | JHEP05(2011)102 | 10.1007/JHEP05(2011)102 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the stability of non-supersymmetric critical points of general
N=4 supergravities. A powerful method to analyse this issue based on the
sGoldstino direction has been developed for minimal supergravity. We adapt this
to the present case, and address the conceptually new features arising for
extended supers... | [
{
"created": "Thu, 16 Dec 2010 20:29:25 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Jul 2011 09:03:48 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Jul 2011 11:40:12 GMT",
"version": "v3"
}
] | 2011-07-29 | [
[
"Borghese",
"Andrea",
""
],
[
"Roest",
"Diederik",
""
]
] | We consider the stability of non-supersymmetric critical points of general N=4 supergravities. A powerful method to analyse this issue based on the sGoldstino direction has been developed for minimal supergravity. We adapt this to the present case, and address the conceptually new features arising for extended supersym... | 14.293226 | 11.94966 | 14.191998 | 12.532999 | 11.257616 | 11.368604 | 12.363612 | 11.589817 | 11.717508 | 13.931895 | 11.478149 | 12.731024 | 13.664974 | 12.631611 | 12.698809 | 13.009261 | 12.489336 | 12.616622 | 12.647977 | 12.933482 | 12.714903 |
hep-th/9903186 | Andreas Brandhuber | Mohsen Alishahiha, Andreas Brandhuber and Yaron Oz | Branes at Singularities in Type 0 String Theory | 18 pages, uses BibTeX, ssg.bst | JHEP 9905:024,1999 | 10.1088/1126-6708/1999/05/024 | CERN-TH/99-72 | hep-th | null | We consider Type 0B D3-branes placed at conical singularities and analyze in
detail the conifold singularity. We study the non supersymmetric gauge theories
on their worldvolume and their conjectured dual gravity descriptions. In the
ultraviolet the solutions exhibit a logarithmic running of the gauge coupling.
In th... | [
{
"created": "Mon, 22 Mar 1999 11:33:32 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Alishahiha",
"Mohsen",
""
],
[
"Brandhuber",
"Andreas",
""
],
[
"Oz",
"Yaron",
""
]
] | We consider Type 0B D3-branes placed at conical singularities and analyze in detail the conifold singularity. We study the non supersymmetric gauge theories on their worldvolume and their conjectured dual gravity descriptions. In the ultraviolet the solutions exhibit a logarithmic running of the gauge coupling. In the ... | 11.32199 | 7.38544 | 10.739634 | 8.243605 | 7.760528 | 7.133952 | 7.554284 | 8.491371 | 7.677356 | 12.785619 | 7.991597 | 8.533521 | 9.974897 | 8.728307 | 8.560427 | 8.24053 | 8.331606 | 8.790644 | 8.640532 | 9.562352 | 8.907618 |
2303.15590 | Amir Raz | Saba Asif Baig, Jacques Distler, Andreas Karch, Amir Raz, Hao-Yu Sun | Spacetime Subsystem Symmetries | 7 pages. V2: references added, minor error fixed | null | null | UTWI-07-2023 | hep-th cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One characteristic feature of many fractonic lattice models, and a defining
property of the exotic field theories developed to describe them, are subsystem
symmetries including a conservation of not just net electric charge but also
electric dipole moments or charges living on submanifolds. So far all such
theories w... | [
{
"created": "Mon, 27 Mar 2023 20:45:30 GMT",
"version": "v1"
},
{
"created": "Tue, 9 May 2023 16:53:56 GMT",
"version": "v2"
}
] | 2023-05-10 | [
[
"Baig",
"Saba Asif",
""
],
[
"Distler",
"Jacques",
""
],
[
"Karch",
"Andreas",
""
],
[
"Raz",
"Amir",
""
],
[
"Sun",
"Hao-Yu",
""
]
] | One characteristic feature of many fractonic lattice models, and a defining property of the exotic field theories developed to describe them, are subsystem symmetries including a conservation of not just net electric charge but also electric dipole moments or charges living on submanifolds. So far all such theories wer... | 14.740636 | 13.674814 | 15.755824 | 14.199941 | 14.267868 | 13.397879 | 15.901065 | 15.208753 | 14.092746 | 16.95047 | 12.575175 | 13.236331 | 14.384224 | 13.12619 | 13.099679 | 13.714118 | 13.299128 | 13.216272 | 13.090509 | 13.471469 | 13.799293 |
hep-th/9405014 | Anna Koubek | A. Koubek | Form-Factor Bootstrap and the Operator Content of Perturbed Minimal
Models | 30 pages; 1 section added, some parts slightly rewritten; (accepted
for publication by Nucl. Phys. B), DAMTP-HEP-94/15 | Nucl.Phys. B428 (1994) 655-680 | 10.1016/0550-3213(94)90368-9 | null | hep-th | null | The form-factor bootstrap approach is applied to the perturbed minimal models
$M_{2,2n+3}$ in the direction of the primary field $\phi_{1,3}$. These theories
are integrable and contain $n$ massive scalar particles, whose $S$--matrix is
purely elastic. The form-factor equations do not refer to a specific operator.
We ... | [
{
"created": "Tue, 3 May 1994 09:29:59 GMT",
"version": "v1"
},
{
"created": "Wed, 4 May 1994 13:41:37 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Aug 1994 13:33:22 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"Koubek",
"A.",
""
]
] | The form-factor bootstrap approach is applied to the perturbed minimal models $M_{2,2n+3}$ in the direction of the primary field $\phi_{1,3}$. These theories are integrable and contain $n$ massive scalar particles, whose $S$--matrix is purely elastic. The form-factor equations do not refer to a specific operator. We us... | 9.647632 | 7.28669 | 10.171254 | 7.4553 | 7.046007 | 6.640007 | 7.073675 | 6.855778 | 6.605632 | 11.013447 | 7.251058 | 6.923829 | 9.836179 | 7.414039 | 7.207322 | 6.951473 | 7.132017 | 6.999325 | 7.22581 | 9.476168 | 7.408693 |
2207.12448 | Denis Karateev | Hongbin Chen, A. Liam Fitzpatrick, Denis Karateev | Nonperturbative Bounds on Scattering of Massive Scalar Particles in $d
\geq 2$ | 38 pages + appendices, 23 figures | null | 10.1007/JHEP12(2022)092 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study two-to-two scattering amplitudes of a scalar particle of mass $m$.
For simplicity, we assume the presence of $\mathbb{Z}_2$ symmetry and that the
particle is $\mathbb{Z}_2$ odd. We consider two classes of amplitudes: the
fully nonperturbative ones and effective field theory (EFT) ones with a cut-off
scale $M... | [
{
"created": "Mon, 25 Jul 2022 18:03:25 GMT",
"version": "v1"
}
] | 2023-01-04 | [
[
"Chen",
"Hongbin",
""
],
[
"Fitzpatrick",
"A. Liam",
""
],
[
"Karateev",
"Denis",
""
]
] | We study two-to-two scattering amplitudes of a scalar particle of mass $m$. For simplicity, we assume the presence of $\mathbb{Z}_2$ symmetry and that the particle is $\mathbb{Z}_2$ odd. We consider two classes of amplitudes: the fully nonperturbative ones and effective field theory (EFT) ones with a cut-off scale $M$.... | 7.623201 | 7.317356 | 7.527615 | 7.101411 | 7.349758 | 7.664059 | 7.164131 | 7.199872 | 6.950066 | 7.300017 | 7.23965 | 7.092451 | 7.1705 | 6.904318 | 7.099027 | 7.144458 | 7.225447 | 7.00632 | 7.166713 | 7.232154 | 7.109659 |
hep-th/0412019 | Hyeong-Chan Kim | Hyeong-Chan Kim, Jae Hyung Yee, and Sang Pyo Kim | New variational perturbation theory based on $q-$deformed oscillator | 6pages, no figures, minor corrections | Int.J.Theor.Phys. 45 (2006) 984-993 | null | null | hep-th nucl-th quant-ph | null | A new variational perturbation theory is developed based on the $q-$deformed
oscillator. It is shown that the new variational perturbation method provides
200 or 10 times better accuracy for the ground state energy of anharmonic
oscillator than the Gaussian and the improved Gaussian approximation,
respectively.
| [
{
"created": "Thu, 2 Dec 2004 07:41:06 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Dec 2004 06:48:57 GMT",
"version": "v2"
},
{
"created": "Thu, 30 Dec 2004 02:21:31 GMT",
"version": "v3"
},
{
"created": "Tue, 12 Apr 2005 03:08:05 GMT",
"version": "v4"
},
{
"cre... | 2007-05-23 | [
[
"Kim",
"Hyeong-Chan",
""
],
[
"Yee",
"Jae Hyung",
""
],
[
"Kim",
"Sang Pyo",
""
]
] | A new variational perturbation theory is developed based on the $q-$deformed oscillator. It is shown that the new variational perturbation method provides 200 or 10 times better accuracy for the ground state energy of anharmonic oscillator than the Gaussian and the improved Gaussian approximation, respectively. | 9.831482 | 8.328472 | 9.269362 | 7.51588 | 8.930265 | 7.497878 | 8.239887 | 8.378036 | 7.74765 | 9.766017 | 7.711884 | 7.632809 | 8.18439 | 8.043796 | 7.716685 | 7.908964 | 7.881432 | 8.088514 | 7.641974 | 8.712567 | 7.63567 |
hep-th/0702076 | Andrey Martins | A. P. Balachandran, A. G. Martins and P. Teotonio-Sobrinho | Discrete Time Evolution and Energy Nonconservation in Noncommutative
Physics | 17 pages, LaTex; minor corrections | JHEP 0705:066,2007 | 10.1088/1126-6708/2007/05/066 | SU-4252-844 | hep-th gr-qc hep-ph math.QA | null | Time-space noncommutativity leads to quantisation of time and energy
nonconservation when time is conjugate to a compact spatial direction like a
circle. In this context energy is conserved only modulo some fixed unit. Such a
possibility arises for example in theories with a compact extra dimension with
which time do... | [
{
"created": "Fri, 9 Feb 2007 20:23:41 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Feb 2007 19:58:36 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Balachandran",
"A. P.",
""
],
[
"Martins",
"A. G.",
""
],
[
"Teotonio-Sobrinho",
"P.",
""
]
] | Time-space noncommutativity leads to quantisation of time and energy nonconservation when time is conjugate to a compact spatial direction like a circle. In this context energy is conserved only modulo some fixed unit. Such a possibility arises for example in theories with a compact extra dimension with which time does... | 11.974605 | 11.524237 | 11.912417 | 11.580432 | 13.233945 | 11.762652 | 11.436411 | 11.400742 | 11.192305 | 12.528372 | 11.344631 | 10.881361 | 11.457125 | 11.081327 | 11.058198 | 11.093431 | 10.626865 | 10.633492 | 10.974965 | 11.382106 | 11.449435 |
hep-th/9812009 | Marco Moriconi | A. De Martino, M. Moriconi | Boundary S-matrix for the Gross-Neveu Model | 13 pages, latex file, final version to appear in PLB | Phys.Lett. B451 (1999) 354-364 | 10.1016/S0370-2693(99)00240-3 | LPENSL-TH-12/98, IC/98/223 | hep-th | null | We study the scattering theory for the Gross-Neveu model on the half-line. We
find the reflection matrices for the elementary fermions, and by fusion we
compute the ones for the two-particle bound-states, showing that they satisfy
non-trivial bootstrap consistency conditions. We also compute more general
reflection m... | [
{
"created": "Tue, 1 Dec 1998 18:24:55 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Mar 1999 17:09:01 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"De Martino",
"A.",
""
],
[
"Moriconi",
"M.",
""
]
] | We study the scattering theory for the Gross-Neveu model on the half-line. We find the reflection matrices for the elementary fermions, and by fusion we compute the ones for the two-particle bound-states, showing that they satisfy non-trivial bootstrap consistency conditions. We also compute more general reflection mat... | 8.618207 | 7.841659 | 10.308691 | 7.617255 | 7.468125 | 7.847138 | 8.130045 | 8.172913 | 7.590489 | 9.920829 | 7.443287 | 8.188918 | 10.093126 | 8.113762 | 7.776911 | 7.985801 | 8.133502 | 8.040859 | 7.892952 | 9.355971 | 8.025272 |
2305.11280 | Michal P. Heller | Sergio E. Aguilar-Gutierrez, Michal P. Heller and Silke Van der
Schueren | Complexity = Anything Can Grow Forever in de Sitter | 7 pages, 3 figures | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Recent developments in anti-de Sitter holography point towards the
association of an infinite class of covariant objects, the simplest one being
codimension-one extremal volumes, with quantum computational complexity in the
microscopic description. One of the defining features of these gravitational
complexity propos... | [
{
"created": "Thu, 18 May 2023 19:55:45 GMT",
"version": "v1"
}
] | 2023-05-22 | [
[
"Aguilar-Gutierrez",
"Sergio E.",
""
],
[
"Heller",
"Michal P.",
""
],
[
"Van der Schueren",
"Silke",
""
]
] | Recent developments in anti-de Sitter holography point towards the association of an infinite class of covariant objects, the simplest one being codimension-one extremal volumes, with quantum computational complexity in the microscopic description. One of the defining features of these gravitational complexity proposal... | 23.94487 | 23.943478 | 26.924322 | 22.271566 | 22.519161 | 23.685726 | 25.355961 | 23.391191 | 23.386803 | 30.111172 | 21.42448 | 23.254528 | 24.463961 | 23.105307 | 24.1043 | 24.048882 | 23.622559 | 23.271545 | 23.38698 | 25.625 | 23.745268 |
hep-th/0206042 | Ian Kogan | Thibault Damour and Ian I. Kogan | Effective Lagrangians and Universality Classes of Nonlinear Bigravity | 41 pages, 4 Figures, final version to be published in Phys.Rev.D | Phys.Rev. D66 (2002) 104024 | 10.1103/PhysRevD.66.104024 | IHES/P/02/35, LPT-Orsay-02/14, OUTP-02/06P | hep-th astro-ph gr-qc hep-ph | null | We discuss the fully non-linear formulation of multigravity. The concept of
universality classes of effective Lagrangians describing bigravity, which is
the simplest form of multigravity, is introduced. We show that non-linear
multigravity theories can naturally arise in several different physical
contexts: brane con... | [
{
"created": "Wed, 5 Jun 2002 18:44:27 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Oct 2002 17:31:45 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Damour",
"Thibault",
""
],
[
"Kogan",
"Ian I.",
""
]
] | We discuss the fully non-linear formulation of multigravity. The concept of universality classes of effective Lagrangians describing bigravity, which is the simplest form of multigravity, is introduced. We show that non-linear multigravity theories can naturally arise in several different physical contexts: brane confi... | 10.928128 | 10.909484 | 10.009964 | 9.248715 | 10.556234 | 9.722761 | 10.871351 | 10.577775 | 10.252324 | 10.900515 | 10.305585 | 9.880198 | 10.161437 | 9.795155 | 10.245727 | 10.094619 | 10.467978 | 9.961857 | 10.028078 | 10.103915 | 9.804848 |
hep-th/9703006 | Juergen Berges | C. Wetterich | Non-Equilibrium Time Evolution in Quantum Field Theory | 7 pages, LaTex | Phys.Rev. E56 (1997) 2687-2690 | 10.1103/PhysRevE.56.2687 | HD-THEP-97-7 | hep-th | null | The time development of equal-time correlation functions in quantum mechanics
and quantum field theory is described by an exact evolution equation for
generating functionals. This permits a comparison between classical and quantum
evolution in non-equilibrium systems.
| [
{
"created": "Fri, 28 Feb 1997 13:17:28 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Wetterich",
"C.",
""
]
] | The time development of equal-time correlation functions in quantum mechanics and quantum field theory is described by an exact evolution equation for generating functionals. This permits a comparison between classical and quantum evolution in non-equilibrium systems. | 14.320822 | 11.463286 | 11.638133 | 9.425933 | 10.594379 | 10.361702 | 10.992854 | 9.372568 | 8.995716 | 10.808043 | 11.433709 | 10.43043 | 10.772004 | 10.638906 | 10.500437 | 10.315189 | 9.891144 | 10.293212 | 10.913197 | 10.44858 | 11.2925 |
hep-th/0412078 | Vitor Cardoso | Vitor Cardoso, Jos\'e P. S. Lemos | New instability for rotating black branes and strings | 4 pages, ReVTeX4. v2: minor improvements | Phys.Lett. B621 (2005) 219-223 | 10.1016/j.physletb.2005.06.025 | null | hep-th astro-ph gr-qc hep-ph | null | The evolution of small perturbations around rotating black branes and
strings, which are low energy solutions of string theory, are investigated. For
simplicity, we concentrate on the Kerr solution times transverse flat extra
dimensions, possibly compactified, but one can also treat other branes composed
of any rotat... | [
{
"created": "Tue, 7 Dec 2004 21:01:44 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Jul 2005 15:33:41 GMT",
"version": "v2"
}
] | 2024-02-05 | [
[
"Cardoso",
"Vitor",
""
],
[
"Lemos",
"José P. S.",
""
]
] | The evolution of small perturbations around rotating black branes and strings, which are low energy solutions of string theory, are investigated. For simplicity, we concentrate on the Kerr solution times transverse flat extra dimensions, possibly compactified, but one can also treat other branes composed of any rotatin... | 10.893816 | 11.09971 | 11.553174 | 10.750918 | 11.776484 | 11.524157 | 11.788278 | 11.520407 | 10.841169 | 11.93833 | 11.226468 | 10.611168 | 10.484596 | 10.377786 | 10.508759 | 10.565804 | 10.60207 | 10.550692 | 10.556421 | 10.938416 | 10.731564 |
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