id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9509037 | Sergei Lukyanov | S. Lukyanov | A note on the deformed Virasoro algebra | 6 pages, harvmac.tex | Phys.Lett. B367 (1996) 121-125 | 10.1016/0370-2693(95)01410-1 | CLNS-95/1360 | hep-th | null | A current of the deformed Virasoro algebra is identified with the
Zamolodchikov-Faddeev operator for the basic scalar particle in the XYZ model.
| [
{
"created": "Thu, 7 Sep 1995 18:52:59 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Lukyanov",
"S.",
""
]
] | A current of the deformed Virasoro algebra is identified with the Zamolodchikov-Faddeev operator for the basic scalar particle in the XYZ model. | 23.648998 | 14.710191 | 21.448301 | 16.041164 | 15.535975 | 13.868504 | 15.738256 | 17.284611 | 14.706441 | 22.80488 | 17.776875 | 15.132469 | 19.045258 | 15.307134 | 13.378277 | 14.24136 | 13.677019 | 13.70312 | 16.217804 | 16.206305 | 13.368921 |
hep-th/0409274 | Danielsson | Ulf H. Danielsson | Lectures on string theory and cosmology | Lectures given in January 2004 at the RTN Barcelona String School, 50
pages, 9 figures | Class.Quant.Grav. 22 (2005) S1-S40 | 10.1088/0264-9381/22/8/001 | UUITP-19/04 | hep-th | null | In these lectures I review recent attempts to apply string theory to
cosmology, including string cosmology and various models of brane cosmology. In
addition, the review includes an introduction to inflation as well as a
discussion of transplanckian signatures. I also provide a critical discussion
of the possible rol... | [
{
"created": "Mon, 27 Sep 2004 19:20:06 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Danielsson",
"Ulf H.",
""
]
] | In these lectures I review recent attempts to apply string theory to cosmology, including string cosmology and various models of brane cosmology. In addition, the review includes an introduction to inflation as well as a discussion of transplanckian signatures. I also provide a critical discussion of the possible role ... | 10.492913 | 9.119564 | 9.517245 | 8.971413 | 9.019639 | 9.482795 | 9.746705 | 9.873148 | 9.218965 | 10.182323 | 8.950285 | 9.155437 | 9.380424 | 9.113314 | 9.03406 | 9.40519 | 8.894549 | 9.03299 | 9.138719 | 9.204315 | 8.788346 |
2012.03514 | Kotaro Tamaoka | Takanori Anegawa, Norihiro Iizuka, Kotaro Tamaoka, Tomonori Ugajin | Wormholes and holographic decoherence | 34 pages, 11 figures. v2: numerical plots of section 3.1 corrected.
references added | null | 10.1007/JHEP03(2021)214 | OU-HET-1081, YITP-20-158 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a class of decoherence process which admits a 3 dimensional
holographic bulk. Starting from a thermo-field double dual to a wormhole, we
prepare another thermo-field double which plays the role of environment. By
allowing the energy flow between the original and environment thermo-field
double, the entanglem... | [
{
"created": "Mon, 7 Dec 2020 08:09:01 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Mar 2021 12:45:58 GMT",
"version": "v2"
}
] | 2021-04-07 | [
[
"Anegawa",
"Takanori",
""
],
[
"Iizuka",
"Norihiro",
""
],
[
"Tamaoka",
"Kotaro",
""
],
[
"Ugajin",
"Tomonori",
""
]
] | We study a class of decoherence process which admits a 3 dimensional holographic bulk. Starting from a thermo-field double dual to a wormhole, we prepare another thermo-field double which plays the role of environment. By allowing the energy flow between the original and environment thermo-field double, the entanglemen... | 14.322126 | 12.941711 | 15.605027 | 12.745049 | 13.059872 | 12.777732 | 13.660157 | 12.335655 | 12.783852 | 16.984459 | 12.145248 | 13.004128 | 14.674726 | 13.104855 | 13.014367 | 12.877581 | 12.390614 | 12.998106 | 12.928851 | 14.654793 | 12.777619 |
hep-th/9701093 | Michael Gutperle | Michael B.Green (DAMTP, Cambridge, U.K.) and Michael Gutperle (DAMTP,
Cambridge, U.K) | Effects of D-instantons | 31 pages, 6 figures, Latex, Reference added, corrected coefficients
in expansion of generalized Eisenstein series in equation 66 now agree with
hep-th/9704145 | Nucl.Phys. B498 (1997) 195-227 | 10.1016/S0550-3213(97)00269-1 | DAMTP-96-104 | hep-th | null | Scattering of fundamental states of type IIB supergravity and superstring
theory is discussed at low orders in perturbation theory in the background of a
D-instanton. The integration over fermionic zero modes in both the low energy
supergravity and in the string theory leads to explicit nonperturbative terms
in the e... | [
{
"created": "Mon, 20 Jan 1997 00:54:37 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Jan 1997 19:07:06 GMT",
"version": "v2"
},
{
"created": "Mon, 7 Jul 1997 19:41:06 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Green",
"Michael B.",
"",
"DAMTP, Cambridge, U.K."
],
[
"Gutperle",
"Michael",
"",
"DAMTP,\n Cambridge, U.K"
]
] | Scattering of fundamental states of type IIB supergravity and superstring theory is discussed at low orders in perturbation theory in the background of a D-instanton. The integration over fermionic zero modes in both the low energy supergravity and in the string theory leads to explicit nonperturbative terms in the eff... | 12.040989 | 11.668951 | 13.840995 | 11.675986 | 12.362079 | 12.260786 | 11.597737 | 10.825205 | 11.404681 | 14.819354 | 11.331034 | 11.489305 | 11.977988 | 11.520201 | 11.423737 | 11.551607 | 11.004405 | 11.336676 | 11.415119 | 11.650985 | 11.362258 |
1508.03190 | Sergei Kuzenko | Sergei M. Kuzenko | Complex linear Goldstino superfield and de Sitter supergravity | 8 pages; V2: typos corrected, comments and reference added; V3: title
changed, references and new section added; V4: published version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complex linear Goldstino superfield was proposed in arXiv:1102.3042 for
the cases of global and local four-dimensional N=1 supersymmetry. Here we make
use of this superfield to construct a supergravity action which is invariant
under spontaneously broken local N=1 supersymmetry and has a positive
cosmological con... | [
{
"created": "Thu, 13 Aug 2015 12:14:01 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Aug 2015 08:43:11 GMT",
"version": "v2"
},
{
"created": "Fri, 4 Sep 2015 10:25:12 GMT",
"version": "v3"
},
{
"created": "Mon, 5 Oct 2015 02:35:05 GMT",
"version": "v4"
}
] | 2015-10-06 | [
[
"Kuzenko",
"Sergei M.",
""
]
] | The complex linear Goldstino superfield was proposed in arXiv:1102.3042 for the cases of global and local four-dimensional N=1 supersymmetry. Here we make use of this superfield to construct a supergravity action which is invariant under spontaneously broken local N=1 supersymmetry and has a positive cosmological const... | 8.009594 | 5.750101 | 8.700742 | 6.641661 | 7.147037 | 5.438286 | 6.206216 | 6.074894 | 6.161362 | 8.063305 | 6.606552 | 6.820569 | 7.899208 | 7.367488 | 7.305482 | 7.103119 | 6.972173 | 7.011468 | 7.209096 | 8.139357 | 6.973416 |
2102.08396 | Zhewei Yin | Laurentiu Rodina, Zhewei Yin | Exploring the Landscape for Soft Theorems of Nonlinear Sigma Models | 46 pages + appendices, 15 figures; matched to the published version
in v2 | null | 10.1007/JHEP08(2021)096 | UUITP-10/21 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize soft theorems of the nonlinear sigma model beyond the
$\mathcal{O} (p^2)$ amplitudes and the coset of $\text{SU} (N) \times \text{SU}
(N) / \text{SU} (N) $. We first discuss the universal flavor ordering of the
amplitudes for the Nambu-Goldstone bosons, so that we can reinterpret the known
$\mathcal{O} ... | [
{
"created": "Tue, 16 Feb 2021 19:00:01 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Aug 2021 19:48:11 GMT",
"version": "v2"
}
] | 2021-09-15 | [
[
"Rodina",
"Laurentiu",
""
],
[
"Yin",
"Zhewei",
""
]
] | We generalize soft theorems of the nonlinear sigma model beyond the $\mathcal{O} (p^2)$ amplitudes and the coset of $\text{SU} (N) \times \text{SU} (N) / \text{SU} (N) $. We first discuss the universal flavor ordering of the amplitudes for the Nambu-Goldstone bosons, so that we can reinterpret the known $\mathcal{O} (p... | 5.828254 | 5.83162 | 6.028892 | 5.546017 | 5.90971 | 5.716616 | 5.749145 | 5.795554 | 5.498989 | 6.478655 | 5.443436 | 5.603849 | 5.6728 | 5.605422 | 5.512485 | 5.643013 | 5.682779 | 5.692963 | 5.558348 | 5.772797 | 5.587284 |
1211.7021 | Claire Zukowski | Raphael Bousso and Claire Zukowski | Multi-Vacuum Initial Conditions and the Arrow of Time | 14 pages, 1 figure; v2: expanded analysis of dominant eigenvector
initial conditions; v3: final version for PRD, minor edits | null | 10.1103/PhysRevD.87.103504 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Depending on the type and arrangement of metastable vacua in the theory,
initial conditions in a de Sitter vacuum with arbitrarily large entropy can be
compatible with the observed arrow of time, if the causal patch or related
measures are used to regulate divergences. An important condition, however, is
that the ini... | [
{
"created": "Thu, 29 Nov 2012 19:02:47 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Dec 2012 00:14:54 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Dec 2013 01:44:22 GMT",
"version": "v3"
}
] | 2013-12-18 | [
[
"Bousso",
"Raphael",
""
],
[
"Zukowski",
"Claire",
""
]
] | Depending on the type and arrangement of metastable vacua in the theory, initial conditions in a de Sitter vacuum with arbitrarily large entropy can be compatible with the observed arrow of time, if the causal patch or related measures are used to regulate divergences. An important condition, however, is that the initi... | 12.552689 | 14.224864 | 14.095279 | 13.52245 | 13.813625 | 14.006278 | 13.896034 | 13.04593 | 12.874391 | 15.206918 | 12.458585 | 11.763036 | 12.113524 | 12.086784 | 12.385297 | 12.548532 | 12.158567 | 12.023945 | 12.129303 | 12.645043 | 12.497349 |
0706.4307 | Steven Gubser | Steven S. Gubser, Silviu S. Pufu, and Amos Yarom | Sonic booms and diffusion wakes generated by a heavy quark in thermal
AdS/CFT | 4 pages, 1 figure, revtex4 | Phys.Rev.Lett.100:012301,2008 | 10.1103/PhysRevLett.100.012301 | PUPT-2239, LMU-ASC 42/07 | hep-th hep-ph nucl-th | null | We evaluate the Poynting vector generated by a heavy quark moving through a
thermal state of N=4 gauge theory using AdS/CFT. A significant diffusion wake
is observed as well as a Mach cone. We discuss the ratio of the energy going
into sound modes to the energy coming in from the wake.
| [
{
"created": "Thu, 28 Jun 2007 19:46:08 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gubser",
"Steven S.",
""
],
[
"Pufu",
"Silviu S.",
""
],
[
"Yarom",
"Amos",
""
]
] | We evaluate the Poynting vector generated by a heavy quark moving through a thermal state of N=4 gauge theory using AdS/CFT. A significant diffusion wake is observed as well as a Mach cone. We discuss the ratio of the energy going into sound modes to the energy coming in from the wake. | 16.027803 | 11.295074 | 13.772437 | 10.709998 | 12.605584 | 13.034753 | 10.567355 | 11.78442 | 11.37892 | 13.298843 | 11.158982 | 12.025605 | 14.700759 | 12.813478 | 12.793935 | 11.785712 | 12.100627 | 12.824428 | 12.16541 | 15.436588 | 12.052472 |
hep-th/0303179 | Vladimir Dobrev | V.K. Dobrev | New Generalized Verma Modules and Multilinear Intertwining Differential
Operators | 30 pages, plain TEX with harvmac; corrected misprints | J.Geom.Phys. 25 (1998) 1-28 | 10.1016/S0393-0440(97)00020-X | null | hep-th math-ph math.MP math.QA math.RT | null | The present paper contains two interrelated developments. First, are proposed
new generalized Verma modules. They are called k-Verma modules, k\in N, and
coincide with the usual Verma modules for k=1. As a vector space a k-Verma
module is isomorphic to the symmetric tensor product of k copies of the
universal envelop... | [
{
"created": "Thu, 20 Mar 2003 13:48:34 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Dec 2004 16:50:52 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Dobrev",
"V. K.",
""
]
] | The present paper contains two interrelated developments. First, are proposed new generalized Verma modules. They are called k-Verma modules, k\in N, and coincide with the usual Verma modules for k=1. As a vector space a k-Verma module is isomorphic to the symmetric tensor product of k copies of the universal envelopin... | 5.968676 | 6.620852 | 6.993492 | 6.454823 | 6.81841 | 6.627315 | 6.952465 | 6.656224 | 6.53987 | 7.344455 | 6.434152 | 6.002046 | 6.22599 | 6.140929 | 6.035254 | 5.95563 | 6.006881 | 5.944687 | 6.083845 | 6.247973 | 5.903577 |
1703.00349 | Merab Gogberashvili Prof | Merab Gogberashvili | Conformal (2+4)-Braneworld | The version accepted by Int. J. Mod. Phys. D | Int. J. Mod. Phys. D 26 (2017) 1750125 | 10.1142/S0218271817501255 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is considered the 6D brane model where matter is trapped on the surface of
a (2+4)-hyperboloid, as is suggested by the geometrical structure behind the 4D
conformal group. The effective dimension of the bulk space-time for matter
fields is five, with the extra space-like and time-like domains. Using the
embedding ... | [
{
"created": "Tue, 28 Feb 2017 16:54:00 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Apr 2017 06:58:41 GMT",
"version": "v2"
}
] | 2017-04-27 | [
[
"Gogberashvili",
"Merab",
""
]
] | It is considered the 6D brane model where matter is trapped on the surface of a (2+4)-hyperboloid, as is suggested by the geometrical structure behind the 4D conformal group. The effective dimension of the bulk space-time for matter fields is five, with the extra space-like and time-like domains. Using the embedding th... | 14.550817 | 12.301537 | 12.738889 | 11.824373 | 13.301011 | 12.979293 | 13.56411 | 12.461349 | 12.246017 | 14.123044 | 12.206314 | 12.127988 | 12.474055 | 12.122439 | 11.81667 | 12.218252 | 12.277208 | 11.751111 | 11.74412 | 11.995509 | 12.0415 |
hep-th/9610175 | Ian Lawrie | I.D. Lawrie and D.B. McKernan | Nonequilibrium perturbation theory for complex scalar fields | 15 pages using RevTeX; 2 figures in 1 Postscript file; Submitted to
Phys. Rev. D | Phys.Rev. D55 (1997) 2290-2297 | 10.1103/PhysRevD.55.2290 | null | hep-th gr-qc hep-ph | null | Real-time perturbation theory is formulated for complex scalar fields away
from thermal equilibrium in such a way that dissipative effects arising from
the absorptive parts of loop diagrams are approximately resummed into the
unperturbed propagators. Low order calculations of physical quantities then
involve quasipar... | [
{
"created": "Wed, 23 Oct 1996 11:43:47 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Lawrie",
"I. D.",
""
],
[
"McKernan",
"D. B.",
""
]
] | Real-time perturbation theory is formulated for complex scalar fields away from thermal equilibrium in such a way that dissipative effects arising from the absorptive parts of loop diagrams are approximately resummed into the unperturbed propagators. Low order calculations of physical quantities then involve quasiparti... | 8.400043 | 8.85805 | 8.250608 | 7.927162 | 8.512333 | 8.501277 | 8.229514 | 8.589802 | 7.809821 | 8.982163 | 8.070915 | 7.82303 | 7.775347 | 8.015705 | 7.994827 | 7.844914 | 7.922843 | 7.945643 | 7.682 | 7.960312 | 8.089526 |
hep-th/9903025 | Yuji Okawa | Yuji Okawa (University of Tokyo, Komaba) | Higher-derivative terms in one-loop effective action for general
trajectories of D-particles in Matrix theory | 18 pages, LaTeX2e, no figures, v2: a coefficient in (3.32) and the
corresponding one in (3.33) corrected and a minor change | Nucl.Phys. B552 (1999) 447-460 | 10.1016/S0550-3213(99)00266-7 | UT-Komaba/99-5 | hep-th | null | The one-loop effective action for general trajectories of D-particles in
Matrix theory is calculated in the expansion with respect to the number of
derivatives up to six, which gives the equation of motion consistently. The
result shows that the terms with six derivatives vanish for straight-line
trajectories, howeve... | [
{
"created": "Tue, 2 Mar 1999 12:29:40 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Mar 1999 05:31:50 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Okawa",
"Yuji",
"",
"University of Tokyo, Komaba"
]
] | The one-loop effective action for general trajectories of D-particles in Matrix theory is calculated in the expansion with respect to the number of derivatives up to six, which gives the equation of motion consistently. The result shows that the terms with six derivatives vanish for straight-line trajectories, however,... | 9.924385 | 8.108865 | 10.033178 | 8.351081 | 9.138498 | 9.684114 | 8.978012 | 8.886744 | 8.333513 | 10.711216 | 8.37131 | 9.103569 | 9.400967 | 9.048712 | 8.963336 | 9.146686 | 9.072753 | 8.978267 | 8.852991 | 9.777781 | 8.640812 |
1112.4662 | Sergey Solodukhin N. | Sergey N. Solodukhin | Entropy of random entangling surfaces | 18 pages; new references added, Invited Contribution to an IOP
special volume of Journal of Physics A in honor of Stuart Dowker's 75th
birthday | null | 10.1088/1751-8113/45/37/374024 | null | hep-th cond-mat.stat-mech gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the situation when a globally defined four-dimensional field
system is separated on two entangled sub-systems by a dynamical (random)
two-dimensional surface. The reduced density matrix averaged over ensemble of
random surfaces of fixed area and the corresponding average entropy are
introduced. The averag... | [
{
"created": "Tue, 20 Dec 2011 11:46:01 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Mar 2012 13:41:30 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Solodukhin",
"Sergey N.",
""
]
] | We consider the situation when a globally defined four-dimensional field system is separated on two entangled sub-systems by a dynamical (random) two-dimensional surface. The reduced density matrix averaged over ensemble of random surfaces of fixed area and the corresponding average entropy are introduced. The average ... | 9.56596 | 8.753007 | 9.199832 | 8.626903 | 9.699378 | 9.491829 | 8.904097 | 8.664612 | 9.291726 | 9.990201 | 8.860667 | 8.807198 | 9.023198 | 8.794262 | 8.782043 | 8.881843 | 8.707934 | 8.757874 | 8.85854 | 9.23339 | 8.766554 |
2110.04853 | Cristhiam Lopez-Arcos | Naser Ahmadiniaz, Filippo Maria Balli, Olindo Corradini, Cristhiam
Lopez-Arcos, Alexander Quintero Velez, Christian Schubert | Manifest colour-kinematics duality and double-copy in the string-based
formalism | 22 pages, 1 figure | null | 10.1016/j.nuclphysb.2022.115690 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The relation for the gravity polarisation tensor as the tensor product of two
gluon polarisation vectors has been well-known for a long time, but a version
of this relation for multi-particle fields is presently still not known. Here
we show that in order for this to happen we first have to ensure that the
multi-part... | [
{
"created": "Sun, 10 Oct 2021 17:02:50 GMT",
"version": "v1"
}
] | 2022-03-02 | [
[
"Ahmadiniaz",
"Naser",
""
],
[
"Balli",
"Filippo Maria",
""
],
[
"Corradini",
"Olindo",
""
],
[
"Lopez-Arcos",
"Cristhiam",
""
],
[
"Velez",
"Alexander Quintero",
""
],
[
"Schubert",
"Christian",
""
]
] | The relation for the gravity polarisation tensor as the tensor product of two gluon polarisation vectors has been well-known for a long time, but a version of this relation for multi-particle fields is presently still not known. Here we show that in order for this to happen we first have to ensure that the multi-partic... | 9.890187 | 9.950365 | 10.845432 | 9.097151 | 10.124344 | 10.008188 | 9.762941 | 9.386727 | 9.09065 | 11.845043 | 9.662166 | 9.481439 | 10.19416 | 9.31187 | 9.718125 | 9.707714 | 9.368652 | 9.394059 | 9.37357 | 9.992962 | 9.312535 |
hep-th/0703243 | Romuald A. Janik | Michal P. Heller and Romuald A. Janik | Viscous hydrodynamics relaxation time from AdS/CFT | 10 pages, Mathematica script included in the source; v2: typo in (28)
fixed, statement about electric/magnetic modes corrected | Phys.Rev.D76:025027,2007 | 10.1103/PhysRevD.76.025027 | null | hep-th gr-qc hep-ph nucl-th | null | We consider an expanding boost-invariant plasma at strong coupling using the
AdS/CFT correspondence for N=4 SYM. We determine the relaxation time in second
order viscous hydrodynamics and find that it is around thirty times shorter
than weak coupling expectations. We find that the nonsingularity of the dual
geometry ... | [
{
"created": "Tue, 27 Mar 2007 14:45:18 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Oct 2007 13:34:28 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Heller",
"Michal P.",
""
],
[
"Janik",
"Romuald A.",
""
]
] | We consider an expanding boost-invariant plasma at strong coupling using the AdS/CFT correspondence for N=4 SYM. We determine the relaxation time in second order viscous hydrodynamics and find that it is around thirty times shorter than weak coupling expectations. We find that the nonsingularity of the dual geometry in... | 12.679359 | 10.773255 | 13.04167 | 11.010846 | 11.904238 | 12.928627 | 10.580403 | 12.155084 | 10.975781 | 14.893258 | 11.881035 | 12.044265 | 12.608683 | 12.60797 | 12.953705 | 13.306625 | 12.446808 | 12.134183 | 12.788716 | 13.315705 | 12.192301 |
hep-th/0101069 | Jianxin Lu | R.-G. Cai (Osaka Univ.), J. X. Lu (Univ. of Michigan), N. Ohta (Osaka
Univ.), S. Roy (Saha Institute) and Y.-S. Wu (Univ. of Utah) | OM Theory and V-duality | 17 pages, typos corrected and references added | JHEP 0102 (2001) 024 | 10.1088/1126-6708/2001/02/024 | OU-HET 363, MCTP-00-17 | hep-th | null | We show that the (M5, M2, M2$'$, MW) bound state solution of eleven
dimensional supergravity recently constructed in hep-th/0009147 is related to
the (M5, M2) bound state one by a finite Lorentz boost along a M5-brane
direction perpendicular to the M2-brane. Given the (M5, M2) bound state as a
defining system for OM ... | [
{
"created": "Thu, 11 Jan 2001 16:18:10 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Jan 2001 16:58:06 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Cai",
"R. -G.",
"",
"Osaka Univ."
],
[
"Lu",
"J. X.",
"",
"Univ. of Michigan"
],
[
"Ohta",
"N.",
"",
"Osaka\n Univ."
],
[
"Roy",
"S.",
"",
"Saha Institute"
],
[
"Wu",
"Y. -S.",
"",
"Univ. of Utah"
]
] | We show that the (M5, M2, M2$'$, MW) bound state solution of eleven dimensional supergravity recently constructed in hep-th/0009147 is related to the (M5, M2) bound state one by a finite Lorentz boost along a M5-brane direction perpendicular to the M2-brane. Given the (M5, M2) bound state as a defining system for OM th... | 9.097698 | 8.019817 | 9.812774 | 8.034221 | 9.229626 | 8.629445 | 8.408141 | 8.014083 | 8.052851 | 9.936712 | 8.389699 | 8.602556 | 8.930503 | 8.391372 | 8.537568 | 8.706475 | 8.365056 | 8.483479 | 8.392207 | 8.861501 | 8.438056 |
1009.2942 | Robert Berman | Robert J. Berman | Kahler-Einstein metrics emerging from free fermions and statistical
mechanics | v1: 22 pages v2: 25 pages. The relation to quantum gravity has been
further developed by working over the moduli space of all complex structures.
Relations to Donaldson's program pointed out. References added | null | 10.1007/JHEP10(2011)106 | null | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a statistical mechanical derivation of Kahler-Einstein metrics,
i.e. solutions to Einstein's vacuum field equations in Euclidean signature
(with a cosmological constant) on a compact Kahler manifold X. The microscopic
theory is given by a canonical free fermion gas on X whose one-particle states
are pluric... | [
{
"created": "Wed, 15 Sep 2010 14:37:21 GMT",
"version": "v1"
},
{
"created": "Sat, 25 Jun 2011 15:12:16 GMT",
"version": "v2"
}
] | 2015-05-19 | [
[
"Berman",
"Robert J.",
""
]
] | We propose a statistical mechanical derivation of Kahler-Einstein metrics, i.e. solutions to Einstein's vacuum field equations in Euclidean signature (with a cosmological constant) on a compact Kahler manifold X. The microscopic theory is given by a canonical free fermion gas on X whose one-particle states are plurican... | 9.150975 | 10.815737 | 10.469287 | 9.792285 | 10.447249 | 10.433853 | 10.451079 | 10.360871 | 10.248531 | 11.394992 | 9.638964 | 9.180749 | 8.939051 | 8.957172 | 8.868698 | 8.984026 | 9.12481 | 8.911222 | 9.307698 | 9.085349 | 9.153548 |
0805.0665 | Marek Rogatko | Rafa{\l} Moderski and Marek Rogatko | Decay of Dirac Massive Hair in the Background of Spherical Black Hole | 8 pages, 5 figures, RevTex, to be published in Phys.Rev.D15 | Phys.Rev.D77:124007,2008 | 10.1103/PhysRevD.77.124007 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The intermediate and late-time behaviour of massive Dirac hair in the static
spherically symmetric black hole spacetime was studied. It was revealed that
the intermediate asymptotic pattern of decay of massive Dirac spinor hair is
dependent on the mass of the field under consideration as well as the multiple
number o... | [
{
"created": "Tue, 6 May 2008 08:07:30 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Moderski",
"Rafał",
""
],
[
"Rogatko",
"Marek",
""
]
] | The intermediate and late-time behaviour of massive Dirac hair in the static spherically symmetric black hole spacetime was studied. It was revealed that the intermediate asymptotic pattern of decay of massive Dirac spinor hair is dependent on the mass of the field under consideration as well as the multiple number of ... | 15.210882 | 11.302372 | 10.811721 | 11.750702 | 10.904348 | 11.120193 | 11.803726 | 10.22133 | 12.80272 | 13.923836 | 12.439477 | 13.000476 | 12.942143 | 12.090898 | 12.439337 | 12.244833 | 12.369807 | 11.733665 | 13.164724 | 13.100214 | 12.326432 |
2004.04483 | Takuya Kanazawa | Takuya Kanazawa | Color-flavor locking and 2SC pairing in random matrix theory | 9 pages. v2: results for two flavors are added in section 4 | null | null | null | hep-th hep-lat math-ph math.MP nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new non-Hermitian chiral random matrix model is proposed. For three
flavors, it is shown that in the large-$N$ limit with $N$ the matrix size, the
color $\mathrm{SU}(3)$ and the flavor $\mathrm{SU}(3)$ symmetries are
spontaneously broken to the diagonal $\mathrm{SU}(3)$ subgroup, realizing
color-flavor locking. The... | [
{
"created": "Thu, 9 Apr 2020 11:07:12 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Apr 2020 15:08:55 GMT",
"version": "v2"
}
] | 2020-04-15 | [
[
"Kanazawa",
"Takuya",
""
]
] | A new non-Hermitian chiral random matrix model is proposed. For three flavors, it is shown that in the large-$N$ limit with $N$ the matrix size, the color $\mathrm{SU}(3)$ and the flavor $\mathrm{SU}(3)$ symmetries are spontaneously broken to the diagonal $\mathrm{SU}(3)$ subgroup, realizing color-flavor locking. The n... | 4.085155 | 3.797922 | 3.821273 | 3.775359 | 3.659358 | 3.741702 | 3.899924 | 3.93516 | 3.626648 | 3.970613 | 3.913867 | 3.836785 | 3.844483 | 3.897037 | 3.869187 | 3.85614 | 3.944579 | 3.926048 | 3.825491 | 3.840291 | 3.845515 |
1810.01802 | Joan Camps | Joan Camps | Superselection Sectors of Gravitational Subregions | 17 pages. v4: minor corrections, accepted in JHEP | null | 10.1007/JHEP01(2019)182 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the problem of defining the entanglement entropy of the
graviton, we study the division of the phase space of general relativity across
subregions. Our key requirement is demanding that the separation into
subregions is imaginary---i.e., that entangling surfaces are not physical. This
translates into a c... | [
{
"created": "Wed, 3 Oct 2018 15:40:49 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Oct 2018 17:10:20 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Nov 2018 18:10:55 GMT",
"version": "v3"
},
{
"created": "Tue, 22 Jan 2019 21:39:41 GMT",
"version": "v4"
}
] | 2019-02-20 | [
[
"Camps",
"Joan",
""
]
] | Motivated by the problem of defining the entanglement entropy of the graviton, we study the division of the phase space of general relativity across subregions. Our key requirement is demanding that the separation into subregions is imaginary---i.e., that entangling surfaces are not physical. This translates into a cer... | 11.579195 | 11.723787 | 11.971523 | 10.393163 | 10.737488 | 11.581937 | 11.26522 | 10.99194 | 11.188219 | 13.762766 | 11.453001 | 11.54819 | 11.518456 | 11.213044 | 11.590044 | 11.172906 | 11.152886 | 10.847451 | 11.357104 | 11.474095 | 11.165956 |
1509.08027 | Evgeny Ivanov | Guillaume Bossard, Evgeny Ivanov and Andrei Smilga | Ultraviolet behavior of 6D supersymmetric Yang-Mills theories and
harmonic superspace | 55 pages, some signs in sections 3 and 4 are corrected without
affecting further conclusions | null | 10.1007/JHEP12(2015)085 | CPHT-RR036.0915 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the issue of higher-dimensional counterterms for the N=(1,1)
supersymmetric Yang-Mills (SYM) theory in six dimensions using the off-shell
N=(1,0) and on-shell N=(1,1) harmonic superspace approaches. The second
approach is developed in full generality and used to solve, for the first time,
the N=(1,1) SYM c... | [
{
"created": "Sat, 26 Sep 2015 21:12:52 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Dec 2015 10:55:32 GMT",
"version": "v2"
},
{
"created": "Fri, 14 May 2021 17:55:44 GMT",
"version": "v3"
}
] | 2021-05-17 | [
[
"Bossard",
"Guillaume",
""
],
[
"Ivanov",
"Evgeny",
""
],
[
"Smilga",
"Andrei",
""
]
] | We revisit the issue of higher-dimensional counterterms for the N=(1,1) supersymmetric Yang-Mills (SYM) theory in six dimensions using the off-shell N=(1,0) and on-shell N=(1,1) harmonic superspace approaches. The second approach is developed in full generality and used to solve, for the first time, the N=(1,1) SYM con... | 5.939019 | 5.739472 | 6.371491 | 5.688747 | 5.551792 | 5.68579 | 5.957717 | 5.420877 | 5.58745 | 7.457551 | 5.709644 | 5.841746 | 6.069401 | 5.820824 | 5.652211 | 5.900959 | 5.831851 | 5.766615 | 5.640229 | 6.139783 | 5.793193 |
0705.1130 | Andrea Gregori | Andrea Gregori | An Entropy-Weighted Sum over Non-Perturbative Vacua | LaTex, 198 pages, 23 figures. Version 2: added comments and
references, corrected typos and errors | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss how, in a Universe restricted to the causal region connected to
the observer, General Relativity implies the quantum nature of physical
phenomena and directly leads to a string theory scenario, whose dynamics is
ruled by a functional that weights all configurations according to their
entropy. The most favo... | [
{
"created": "Tue, 8 May 2007 18:06:52 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Feb 2009 11:40:39 GMT",
"version": "v2"
}
] | 2009-02-09 | [
[
"Gregori",
"Andrea",
""
]
] | We discuss how, in a Universe restricted to the causal region connected to the observer, General Relativity implies the quantum nature of physical phenomena and directly leads to a string theory scenario, whose dynamics is ruled by a functional that weights all configurations according to their entropy. The most favour... | 15.365952 | 17.862728 | 16.598274 | 15.725545 | 16.375725 | 17.54113 | 18.484968 | 16.752071 | 17.033997 | 18.559038 | 16.164259 | 16.066729 | 15.226668 | 15.328831 | 15.279685 | 15.944092 | 15.744287 | 15.533038 | 15.257857 | 15.311235 | 15.385942 |
0811.2225 | Hong Lu | H. Lu, Jianwei Mei and C.N. Pope | Kerr-AdS/CFT Correspondence in Diverse Dimensions | Latex, 19 pages, typos corrected and references added | JHEP 0904:054,2009 | 10.1088/1126-6708/2009/04/054 | MIFP-08-29 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was proposed recently that the near-horizon states of an extremal
four-dimensional Kerr black hole could be identified with a certain chiral
conformal field theory whose Virasoro algebra arises as an asymptotic symmetry
algebra of the near-horizon Kerr geometry. Supportive evidence for the proposed
duality came fr... | [
{
"created": "Fri, 14 Nov 2008 20:39:10 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Nov 2008 21:05:04 GMT",
"version": "v2"
},
{
"created": "Mon, 8 Dec 2008 17:40:08 GMT",
"version": "v3"
}
] | 2009-04-17 | [
[
"Lu",
"H.",
""
],
[
"Mei",
"Jianwei",
""
],
[
"Pope",
"C. N.",
""
]
] | It was proposed recently that the near-horizon states of an extremal four-dimensional Kerr black hole could be identified with a certain chiral conformal field theory whose Virasoro algebra arises as an asymptotic symmetry algebra of the near-horizon Kerr geometry. Supportive evidence for the proposed duality came from... | 4.200057 | 3.647376 | 4.189569 | 3.8718 | 3.693145 | 3.645996 | 3.772326 | 3.928584 | 3.699545 | 4.515788 | 3.79016 | 4.063766 | 3.978621 | 3.932604 | 4.00588 | 4.02916 | 3.977841 | 4.000721 | 3.951633 | 3.940909 | 4.046894 |
hep-th/0211165 | J. David Vergara | Juan M. Romero, J.A. Santiago and J. David Vergara | Newton's Second Law in a Noncommutative Space | 7 pages, References added | Phys.Lett. A310 (2003) 9-12 | 10.1016/S0375-9601(03)00191-9 | null | hep-th | null | In this work we show that corrections to the Newton's second law appears if
we assume that the phase space has a symplectic structure consistent with the
rules of commutation of noncommutative quantum mechanis. In the central field
case we find that the correction term breaks the rotational symmetry. In
particular, f... | [
{
"created": "Mon, 18 Nov 2002 16:55:42 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Nov 2002 20:17:12 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Romero",
"Juan M.",
""
],
[
"Santiago",
"J. A.",
""
],
[
"Vergara",
"J. David",
""
]
] | In this work we show that corrections to the Newton's second law appears if we assume that the phase space has a symplectic structure consistent with the rules of commutation of noncommutative quantum mechanis. In the central field case we find that the correction term breaks the rotational symmetry. In particular, for... | 11.988133 | 9.747812 | 10.603381 | 10.209462 | 10.996136 | 11.077944 | 10.649949 | 10.157561 | 9.448575 | 11.556036 | 10.3567 | 10.335804 | 11.053469 | 10.262903 | 10.653584 | 10.198567 | 10.38484 | 10.345313 | 10.29912 | 10.732082 | 10.219561 |
2204.13513 | Ashmita Das | Ashmita Das and Bibhas Ranjan Majhi | Unruh-Fulling effect in nonlocal field theory: The role of Unruh
decomposition | Minor modifications, published in Physical Review D | Physical Review D, 106, 2022, 105025 | 10.1103/PhysRevD.106.105025 | null | hep-th gr-qc quant-ph | http://creativecommons.org/licenses/by/4.0/ | We investigate the Unruh-Fulling effect in a class of nonlocal field theories
by examining both the number operator and Unruh-DeWitt detector methods. Unlike
in previous literature, we use Unruh quantization to quantize the matter field.
Such choice, as oppose to standard Minkowski decomposition, naturally
incorporat... | [
{
"created": "Thu, 28 Apr 2022 14:03:08 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Nov 2022 08:03:18 GMT",
"version": "v2"
}
] | 2022-12-01 | [
[
"Das",
"Ashmita",
""
],
[
"Majhi",
"Bibhas Ranjan",
""
]
] | We investigate the Unruh-Fulling effect in a class of nonlocal field theories by examining both the number operator and Unruh-DeWitt detector methods. Unlike in previous literature, we use Unruh quantization to quantize the matter field. Such choice, as oppose to standard Minkowski decomposition, naturally incorporates... | 7.334396 | 8.068896 | 7.525638 | 7.126894 | 8.29493 | 7.246758 | 7.550551 | 7.473216 | 7.445495 | 8.006671 | 7.22777 | 7.578259 | 7.199205 | 7.076684 | 7.32955 | 7.442338 | 7.649757 | 7.28214 | 7.229021 | 7.436394 | 7.351472 |
hep-th/9806118 | Claus Slotta | Stefan Ochs and Ulrich Heinz | Wigner functions in covariant and single-time formulations | 92 pages, to appear in Annals of Physics (N.Y.) | Annals Phys.266:351-416,1998 | 10.1006/aphy.1998.5796 | null | hep-th | null | We will establish the connection between the Lorentz covariant and so-called
single-time formulation for the quark Wigner operator. To this end we will
discuss the initial value problem for the Wigner operator of a field theory and
give a discussion of the gauge-covariant formulation for the Wigner operator
including... | [
{
"created": "Mon, 15 Jun 1998 13:25:01 GMT",
"version": "v1"
}
] | 2009-10-09 | [
[
"Ochs",
"Stefan",
""
],
[
"Heinz",
"Ulrich",
""
]
] | We will establish the connection between the Lorentz covariant and so-called single-time formulation for the quark Wigner operator. To this end we will discuss the initial value problem for the Wigner operator of a field theory and give a discussion of the gauge-covariant formulation for the Wigner operator including s... | 9.838817 | 10.777857 | 10.221296 | 10.027112 | 10.153478 | 10.221644 | 10.199708 | 10.996085 | 9.833385 | 11.587792 | 9.80735 | 10.001531 | 9.723087 | 9.496272 | 10.260374 | 9.858353 | 10.08262 | 10.020033 | 9.602177 | 9.771603 | 9.670263 |
1712.02846 | Vakhid Gani | Ekaterina Belendryasova, Vakhid A. Gani | Resonance phenomena in the $\varphi^8$ kinks scattering | 5 pages, 4 figures; Proceedings of the 3rd International Conference
on Particle Physics and Astrophysics, Moscow, 2-5 October 2017 | J. Phys.: Conf. Ser. 934, 012059 (2017) | 10.1088/1742-6596/934/1/012059 | null | hep-th cond-mat.mtrl-sci math-ph math.MP nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the scattering of the $\varphi^8$ kinks with power-law asymptotics.
We found two critical values of the initial velocity, $v_{cr}^{(1)}$ and
$v_{cr}^{(2)}$, which separate different regimes of the kink-antikink
collision. At the initial velocities $v_{in}< v_{cr}^{(1)}$ kinks can not
collide due to repulsive... | [
{
"created": "Thu, 7 Dec 2017 20:05:46 GMT",
"version": "v1"
}
] | 2018-01-09 | [
[
"Belendryasova",
"Ekaterina",
""
],
[
"Gani",
"Vakhid A.",
""
]
] | We study the scattering of the $\varphi^8$ kinks with power-law asymptotics. We found two critical values of the initial velocity, $v_{cr}^{(1)}$ and $v_{cr}^{(2)}$, which separate different regimes of the kink-antikink collision. At the initial velocities $v_{in}< v_{cr}^{(1)}$ kinks can not collide due to repulsive f... | 4.499543 | 3.457708 | 4.874034 | 4.0804 | 3.798529 | 3.85299 | 3.804321 | 3.944262 | 3.869414 | 5.428346 | 4.078401 | 4.200271 | 4.548972 | 4.450271 | 4.254603 | 4.416775 | 4.406202 | 4.342848 | 4.358767 | 4.708838 | 4.324529 |
2005.13447 | Mykola Stetsko | M. M. Stetsko | Static spherically symmetric Einstein-Yang-Mills-dilaton black hole and
its thermodynamics | 20 pages, 8 figures | null | 10.1103/PhysRevD.101.124017 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A static black hole with spherical symmetry is obtained and examined in the
framework of Einstein-Yang-Mills-dilaton theory. The obtained black hole
solution allowed us to derive and investigate entropy, temperature and heat
capacity. To better examine the thermodynamics of the black hole extended phase
space is also... | [
{
"created": "Wed, 27 May 2020 15:58:39 GMT",
"version": "v1"
}
] | 2020-07-01 | [
[
"Stetsko",
"M. M.",
""
]
] | A static black hole with spherical symmetry is obtained and examined in the framework of Einstein-Yang-Mills-dilaton theory. The obtained black hole solution allowed us to derive and investigate entropy, temperature and heat capacity. To better examine the thermodynamics of the black hole extended phase space is also u... | 10.558535 | 8.949011 | 9.402435 | 8.442392 | 9.116504 | 9.246174 | 9.598787 | 8.36738 | 9.451262 | 10.381649 | 9.40953 | 9.427859 | 9.47303 | 9.483647 | 9.630855 | 9.487046 | 9.631879 | 9.314619 | 9.66956 | 9.485909 | 9.746852 |
2102.09537 | Congkao Wen | Daniele Dorigoni, Michael B. Green, Congkao Wen | Exact properties of an integrated correlator in $\mathcal{N}=4$ $SU(N)$
SYM | 54 pages, 5 figures; v2: typos corrected, matches published version
in JHEP | null | 10.1007/JHEP05(2021)089 | QMUL-PH-21-09, DCPT-21/03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a novel expression for an integrated correlation function of four
superconformal primaries in $SU(N)$ $\mathcal{N}=4$ SYM. This integrated
correlator, which is based on supersymmetric localisation, has been the subject
of several recent developments. The correlator is re-expressed as a sum over a
two dimen... | [
{
"created": "Thu, 18 Feb 2021 18:30:21 GMT",
"version": "v1"
},
{
"created": "Mon, 10 May 2021 20:04:28 GMT",
"version": "v2"
}
] | 2021-05-26 | [
[
"Dorigoni",
"Daniele",
""
],
[
"Green",
"Michael B.",
""
],
[
"Wen",
"Congkao",
""
]
] | We present a novel expression for an integrated correlation function of four superconformal primaries in $SU(N)$ $\mathcal{N}=4$ SYM. This integrated correlator, which is based on supersymmetric localisation, has been the subject of several recent developments. The correlator is re-expressed as a sum over a two dimensi... | 5.631705 | 5.396054 | 6.051536 | 5.257881 | 5.42887 | 5.480125 | 5.536679 | 5.268047 | 5.3899 | 6.510813 | 5.167027 | 5.293206 | 5.630037 | 5.395466 | 5.469463 | 5.458025 | 5.497939 | 5.419517 | 5.335536 | 5.70774 | 5.323937 |
hep-th/0210290 | Michele Trapletti | M. Trapletti | Open string models with Scherk-Schwarz SUSY breaking | 5 pages. Talk given at SUSY02, ``The 10th International Conference on
Supersymmetry and unification of Fundamental Interactions'', DESY, Hamburg,
June 17-23, 2002 | null | null | SISSA-74/2002/EP | hep-th | null | We apply the well-known Scherk-Schwarz supersymmetry breaking mechanism in an
open string context. We construct a new Z_3\times Z_3^\prime model, containing
only D9-branes, and rederive from a more geometric perspective the known
Z_6^\prime\times Z_2^\prime model, containing D9, D5 and \bar D 5 branes. We
show recent... | [
{
"created": "Wed, 30 Oct 2002 14:28:31 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Trapletti",
"M.",
""
]
] | We apply the well-known Scherk-Schwarz supersymmetry breaking mechanism in an open string context. We construct a new Z_3\times Z_3^\prime model, containing only D9-branes, and rederive from a more geometric perspective the known Z_6^\prime\times Z_2^\prime model, containing D9, D5 and \bar D 5 branes. We show recent r... | 11.564079 | 8.007413 | 11.772 | 8.705134 | 7.805647 | 7.974986 | 8.869516 | 8.257823 | 7.84199 | 10.949895 | 8.49302 | 9.885957 | 10.242843 | 9.968609 | 10.056749 | 10.052238 | 9.555016 | 9.913513 | 10.01925 | 10.760907 | 9.890022 |
1907.06255 | Anupam A H | Anupam A H, Athira P. V | Generalized coherent states in QCD from asymptotic symmetries | v1:44pages ; v2:46pages, new references added, 2 figures added,
matches with published version | null | 10.1103/PhysRevD.101.066010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the relationship between asymptotic symmetries of QCD and
vacuum transitions induced during scattering. Starting with the Fock vacuum in
the far past, the infinity of conservation laws associated to (non-Abelian)
asymptotic symmetries in QCD can be used to determine the vacuum in the far
future. We sho... | [
{
"created": "Sun, 14 Jul 2019 17:49:25 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Nov 2020 10:30:15 GMT",
"version": "v2"
}
] | 2020-11-04 | [
[
"H",
"Anupam A",
""
],
[
"P.",
"Athira",
"V"
]
] | We investigate the relationship between asymptotic symmetries of QCD and vacuum transitions induced during scattering. Starting with the Fock vacuum in the far past, the infinity of conservation laws associated to (non-Abelian) asymptotic symmetries in QCD can be used to determine the vacuum in the far future. We show ... | 10.251104 | 9.326705 | 9.627316 | 9.653162 | 10.130984 | 9.349274 | 10.311422 | 9.552501 | 9.302749 | 10.533 | 9.754484 | 9.779856 | 9.589669 | 9.377504 | 9.164968 | 9.458256 | 9.835782 | 9.503693 | 9.4704 | 10.046564 | 9.56918 |
hep-th/0511198 | Pavel Buividovich | P. V. Buividovich, V. I. Kuvshinov | Mixed colour states in QCD confining vacuum | null | Nonlinear Phenomena In Complex Systems, No. 3, Vol. 8 (2005) | null | null | hep-th | null | We show that confinement of spinless heavy quarks in fundamental
representation of $SU(N_{c})$ gauge group can be treated as decoherence of pure
colour state into a white mixture of states. Decoherence rate is found to be
proportional to the tension of QCD string and the distance between colour
charges. The purity of... | [
{
"created": "Sun, 20 Nov 2005 12:12:02 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Aug 2006 09:16:23 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Buividovich",
"P. V.",
""
],
[
"Kuvshinov",
"V. I.",
""
]
] | We show that confinement of spinless heavy quarks in fundamental representation of $SU(N_{c})$ gauge group can be treated as decoherence of pure colour state into a white mixture of states. Decoherence rate is found to be proportional to the tension of QCD string and the distance between colour charges. The purity of c... | 11.900055 | 10.613088 | 11.016301 | 9.551857 | 10.845733 | 11.651093 | 11.512094 | 10.494995 | 10.330845 | 11.186561 | 10.516717 | 10.743619 | 10.724606 | 10.031987 | 10.181303 | 10.898147 | 10.997735 | 10.349571 | 10.288849 | 10.561892 | 10.496764 |
1209.6016 | Carlos A. S. Almeida | L. J. S. Sousa, C. A. S. Silva, C. A. S. Almeida | Brane bounce-type configurations in a string-like scenario | 15 pages, 5 figures. To appear in Physics Letters B | Physics Letters B 718 (2012) pp. 579-583 | 10.1016/j.physletb.2012.09.070 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Brane world six dimensional scenarios with string like metric has been
proposed to alleviate the problem of field localization. However, these models
have been suffering from some drawbacks related with energy conditions as well
as from difficulties to find analytical solutions. In this work, we propose a
model where... | [
{
"created": "Wed, 26 Sep 2012 17:43:07 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Sep 2012 03:40:16 GMT",
"version": "v2"
}
] | 2012-11-29 | [
[
"Sousa",
"L. J. S.",
""
],
[
"Silva",
"C. A. S.",
""
],
[
"Almeida",
"C. A. S.",
""
]
] | Brane world six dimensional scenarios with string like metric has been proposed to alleviate the problem of field localization. However, these models have been suffering from some drawbacks related with energy conditions as well as from difficulties to find analytical solutions. In this work, we propose a model where a... | 12.608519 | 13.531094 | 12.799649 | 12.365714 | 12.76131 | 13.450518 | 12.538589 | 12.764283 | 12.246608 | 12.910339 | 12.665283 | 12.554021 | 12.599556 | 12.46879 | 12.099675 | 12.314836 | 12.240151 | 12.142281 | 12.500275 | 12.42211 | 12.218598 |
2311.09219 | John Stout | Priyesh Chakraborty and John Stout | Compact Scalars at the Cosmological Collider | 40+10 pages, 4 figures, many diagrams | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the dynamics of scalar fields with compact field spaces, or axions,
in de Sitter space. We argue that the field space topology can qualitatively
affect the physics of these fields beyond just which terms are allowed in their
actions. We argue that the sharpest difference is for massless fields -- the
free ma... | [
{
"created": "Wed, 15 Nov 2023 18:59:13 GMT",
"version": "v1"
}
] | 2023-11-16 | [
[
"Chakraborty",
"Priyesh",
""
],
[
"Stout",
"John",
""
]
] | We study the dynamics of scalar fields with compact field spaces, or axions, in de Sitter space. We argue that the field space topology can qualitatively affect the physics of these fields beyond just which terms are allowed in their actions. We argue that the sharpest difference is for massless fields -- the free mass... | 8.193595 | 7.846785 | 8.371482 | 7.716384 | 8.340873 | 8.17624 | 8.16368 | 7.917893 | 7.647957 | 8.984907 | 7.690421 | 7.743055 | 7.836302 | 7.786881 | 7.646474 | 7.901071 | 7.785884 | 7.778481 | 7.758197 | 8.034337 | 7.730228 |
hep-th/0203006 | Daniel Litim | Daniel F. Litim | Critical exponents from optimised renormalisation group flows | 34 pages, 15 figures, revtex, to appear in NPB | Nucl.Phys.B631:128-158,2002 | 10.1016/S0550-3213(02)00186-4 | CERN-TH-2002-023 | hep-th cond-mat hep-ph | null | Within the exact renormalisation group, the scaling solutions for O(N)
symmetric scalar field theories are studied to leading order in the derivative
expansion. The Gaussian fixed point is examined for d>2 dimensions and
arbitrary infrared regularisation. The Wilson-Fisher fixed point in d=3 is
studied using an optim... | [
{
"created": "Fri, 1 Mar 2002 05:17:24 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Mar 2002 14:54:18 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Litim",
"Daniel F.",
""
]
] | Within the exact renormalisation group, the scaling solutions for O(N) symmetric scalar field theories are studied to leading order in the derivative expansion. The Gaussian fixed point is examined for d>2 dimensions and arbitrary infrared regularisation. The Wilson-Fisher fixed point in d=3 is studied using an optimis... | 9.727228 | 8.879602 | 9.954141 | 8.853346 | 9.428118 | 9.388178 | 8.943777 | 8.709816 | 8.558062 | 11.557427 | 8.897549 | 9.0208 | 9.354776 | 8.879857 | 9.102118 | 8.996973 | 9.107083 | 8.50092 | 8.845294 | 9.140503 | 8.867791 |
hep-th/9707251 | null | Mans Henningson and Piljin Yi | Four-dimensional BPS-spectra via M-theory | 18 pages, 3 figures, uses harvmac. References added | Phys. Rev. D 57, 1291 (1998) | 10.1103/PhysRevD.57.1291 | CERN-TH/97-175, CU-TP-852 | hep-th | null | We consider the realization of four-dimensional theories with N = 2
supersymmetry as M-theory configurations including a five-brane. Our emphasis
is on the spectrum of massive states, that are realized as two-branes ending on
the five-brane. We start with a determination of the supersymmetries that are
left unbroken ... | [
{
"created": "Wed, 30 Jul 1997 22:20:32 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Aug 1997 09:48:51 GMT",
"version": "v2"
}
] | 2016-08-25 | [
[
"Henningson",
"Mans",
""
],
[
"Yi",
"Piljin",
""
]
] | We consider the realization of four-dimensional theories with N = 2 supersymmetry as M-theory configurations including a five-brane. Our emphasis is on the spectrum of massive states, that are realized as two-branes ending on the five-brane. We start with a determination of the supersymmetries that are left unbroken by... | 6.459826 | 6.382751 | 7.398184 | 6.526291 | 6.391148 | 6.700345 | 6.37202 | 6.508406 | 6.497654 | 7.402526 | 6.357193 | 6.455733 | 6.646506 | 6.35751 | 6.54535 | 6.181342 | 6.575865 | 6.490719 | 6.523742 | 6.317991 | 6.39829 |
hep-th/0003147 | Vijay Balasubramanian | Vijay Balasubramanian, Eric Gimon and Djordje Minic | Consistency Conditions for Holographic Duality | LaTeX, 14 pages | JHEP 0005:014,2000 | 10.1088/1126-6708/2000/05/014 | HUTP-00/A007, CITUSC/00-013, CALT68-2265 | hep-th | null | We show that if the beta functions of a field theory are given by the
gradient of a certain potential on the space of couplings, a gravitational
background in one more dimension can express the renormalization group (RG)
flow of the theory. The field theory beta functions and the gradient flow
constraint together rec... | [
{
"created": "Thu, 16 Mar 2000 20:41:55 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Apr 2000 18:50:57 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Balasubramanian",
"Vijay",
""
],
[
"Gimon",
"Eric",
""
],
[
"Minic",
"Djordje",
""
]
] | We show that if the beta functions of a field theory are given by the gradient of a certain potential on the space of couplings, a gravitational background in one more dimension can express the renormalization group (RG) flow of the theory. The field theory beta functions and the gradient flow constraint together recon... | 10.426085 | 9.891033 | 10.828195 | 8.944048 | 9.240772 | 8.902825 | 9.553555 | 9.51082 | 9.500211 | 11.017262 | 9.37279 | 9.394991 | 9.599631 | 9.170526 | 9.19152 | 9.089604 | 9.23702 | 9.132006 | 9.359476 | 9.833505 | 9.343836 |
1607.06506 | Segundo Parra Mili\'an | Segundo P. Mili\'an | Supermultiplet of $\beta-$deformations from twistors | null | null | 10.1142/S0217751X17501573 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We consider the supermultiplet of linearized beta-deformation of
$\mathcal{N}=4$ Super Yang-Mills(SYM). It was previously studied on the
gravitational side. We study the supermultiplet of beta-deformations on the
field theory side and we compare two finite-dimensional representations of
$psl(4|4,\bf{R})$ algebra. We ... | [
{
"created": "Thu, 21 Jul 2016 21:22:08 GMT",
"version": "v1"
}
] | 2017-10-04 | [
[
"Milián",
"Segundo P.",
""
]
] | We consider the supermultiplet of linearized beta-deformation of $\mathcal{N}=4$ Super Yang-Mills(SYM). It was previously studied on the gravitational side. We study the supermultiplet of beta-deformations on the field theory side and we compare two finite-dimensional representations of $psl(4|4,\bf{R})$ algebra. We sh... | 9.875498 | 10.377098 | 10.326262 | 9.136127 | 9.570834 | 10.005073 | 9.974004 | 10.064974 | 8.917622 | 11.037148 | 8.47156 | 9.061147 | 9.429716 | 8.934215 | 9.27682 | 9.31253 | 9.424057 | 9.023906 | 8.999026 | 9.338817 | 9.013744 |
2111.13697 | Matthew Yu | Matthew Yu | Gauging Categorical Symmetries in 3d Topological Orders and Bulk
Reconstruction | 65 pages, comments welcome | null | null | null | hep-th cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the language of categorical condensation to give a procedure for
gauging nonabelian anyons, which are the manifestations of categorical
symmetries in three spacetime dimensions. We also describe how the condensation
procedure can be used in other contexts such as for topological cosets and
constructing modular... | [
{
"created": "Fri, 26 Nov 2021 19:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Feb 2022 02:03:53 GMT",
"version": "v2"
},
{
"created": "Mon, 10 Apr 2023 00:46:57 GMT",
"version": "v3"
}
] | 2023-04-11 | [
[
"Yu",
"Matthew",
""
]
] | We use the language of categorical condensation to give a procedure for gauging nonabelian anyons, which are the manifestations of categorical symmetries in three spacetime dimensions. We also describe how the condensation procedure can be used in other contexts such as for topological cosets and constructing modular i... | 13.798132 | 13.30028 | 15.859338 | 12.575892 | 13.492867 | 13.871635 | 13.946362 | 12.72016 | 12.788848 | 16.558338 | 12.675494 | 12.322586 | 14.002375 | 13.021996 | 12.585413 | 13.078312 | 13.042046 | 12.71737 | 12.759141 | 13.88152 | 12.824896 |
hep-th/9406095 | null | Tom Lada and Martin Markl | Strongly homotopy Lie algebras | 17 pages | null | null | null | hep-th math.QA | null | The present paper can be thought of as a continuation of the paper
"Introduction to sh Lie algebras for physicists" by T. Lada and J. Stasheff
(International Journal of Theoretical Physics Vol. 32, No. 7 (1993),
1087--1103, appeared also as preprint hep-th/9209099) which provided an
exposition of the basic ingredient... | [
{
"created": "Wed, 15 Jun 1994 08:46:25 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Lada",
"Tom",
""
],
[
"Markl",
"Martin",
""
]
] | The present paper can be thought of as a continuation of the paper "Introduction to sh Lie algebras for physicists" by T. Lada and J. Stasheff (International Journal of Theoretical Physics Vol. 32, No. 7 (1993), 1087--1103, appeared also as preprint hep-th/9209099) which provided an exposition of the basic ingredients ... | 6.595921 | 7.957782 | 7.983825 | 7.55791 | 8.517351 | 8.5456 | 8.267286 | 8.87116 | 7.512002 | 9.672151 | 7.119096 | 6.677219 | 7.066325 | 6.664219 | 6.610848 | 6.463673 | 6.558537 | 6.500083 | 6.707482 | 6.86393 | 6.560231 |
hep-th/9705122 | Svend-Egil Hjelmeland | S. E. Hjelmeland and U. Lindstr\"om | Duality for the Non-Specialist | 46 pages, Latex2e with twoside, one eps figure. References added | null | null | UIO/PHYS/97-03 | hep-th | null | This is the written version of a series of lectures reviewing the basics of
duality as applied to p-forms and sigma-models. The ideas are introduced by way
of worked examples, often quite detailed. Our approach is very pedestrian and
the presentation is aimed at non-specialists, such as e.g. graduate students.
| [
{
"created": "Fri, 16 May 1997 09:51:09 GMT",
"version": "v1"
},
{
"created": "Mon, 26 May 1997 11:57:21 GMT",
"version": "v2"
}
] | 2016-08-15 | [
[
"Hjelmeland",
"S. E.",
""
],
[
"Lindström",
"U.",
""
]
] | This is the written version of a series of lectures reviewing the basics of duality as applied to p-forms and sigma-models. The ideas are introduced by way of worked examples, often quite detailed. Our approach is very pedestrian and the presentation is aimed at non-specialists, such as e.g. graduate students. | 17.000187 | 12.179346 | 14.579132 | 11.305662 | 11.835895 | 13.959059 | 13.662575 | 13.038377 | 12.161257 | 15.393508 | 12.385185 | 12.154367 | 14.58169 | 12.507463 | 12.861804 | 12.180241 | 12.23864 | 12.074065 | 12.531584 | 14.878743 | 13.50563 |
2004.10789 | Oguz Turker | Oguz Turker, Jeroen van den Brink, Tobias Meng, Flavio S. Nogueira | Bosonization in 2+1 dimensions via Chern-Simons bosonic particle-vortex
duality | 13 pages, 4 figures; v2 matches published version | Phys. Rev. D 102, 034506 (2020) | 10.1103/PhysRevD.102.034506 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dualities provide deep insight into physics by relating two seemingly
distinct theories. Here we consider a duality between lattice fermions and
bosons in (2+1) spacetime dimensions, relating free massive Dirac fermions to
Abelian Chern-Simons Higgs (ACSH) bosons. To establish the duality we represent
the exact parti... | [
{
"created": "Wed, 22 Apr 2020 18:52:06 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Oct 2020 16:04:21 GMT",
"version": "v2"
}
] | 2020-10-28 | [
[
"Turker",
"Oguz",
""
],
[
"Brink",
"Jeroen van den",
""
],
[
"Meng",
"Tobias",
""
],
[
"Nogueira",
"Flavio S.",
""
]
] | Dualities provide deep insight into physics by relating two seemingly distinct theories. Here we consider a duality between lattice fermions and bosons in (2+1) spacetime dimensions, relating free massive Dirac fermions to Abelian Chern-Simons Higgs (ACSH) bosons. To establish the duality we represent the exact partiti... | 8.182027 | 8.645451 | 9.764915 | 8.353967 | 8.619099 | 9.169719 | 8.943948 | 8.537913 | 8.441217 | 9.784167 | 8.237756 | 8.386289 | 8.271943 | 8.029935 | 8.301494 | 8.43704 | 8.51082 | 8.278326 | 8.027909 | 8.647176 | 8.039797 |
1503.01409 | Douglas Stanford | Juan Maldacena, Stephen H. Shenker and Douglas Stanford | A bound on chaos | 16+6 pages, 2 figures | null | 10.1007/JHEP08(2016)106 | null | hep-th cond-mat.stat-mech nlin.CD quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We conjecture a sharp bound on the rate of growth of chaos in thermal quantum
systems with a large number of degrees of freedom. Chaos can be diagnosed using
an out-of-time-order correlation function closely related to the commutator of
operators separated in time. We conjecture that the influence of chaos on this
co... | [
{
"created": "Wed, 4 Mar 2015 18:37:55 GMT",
"version": "v1"
}
] | 2016-09-21 | [
[
"Maldacena",
"Juan",
""
],
[
"Shenker",
"Stephen H.",
""
],
[
"Stanford",
"Douglas",
""
]
] | We conjecture a sharp bound on the rate of growth of chaos in thermal quantum systems with a large number of degrees of freedom. Chaos can be diagnosed using an out-of-time-order correlation function closely related to the commutator of operators separated in time. We conjecture that the influence of chaos on this corr... | 5.351162 | 5.663805 | 7.107329 | 5.620503 | 6.083244 | 5.876913 | 6.172302 | 5.809303 | 5.411321 | 7.75666 | 5.785084 | 5.822555 | 6.155584 | 5.596445 | 5.757618 | 5.66811 | 5.497505 | 5.584865 | 5.759718 | 6.319885 | 5.362784 |
1305.1446 | Yang Zhou | Yunseok Seo, Sang-Jin Sin, Yang Zhou | Thermal Mass and Plasmino for Strongly Interacting Fermions | 20 pages, 14 figures | JHEP 1306:076,2013 | 10.1007/JHEP06(2013)076 | null | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate fermion self energy problem in the strongly coupled dense
medium in holographic approach. By working out bottom up models as well as top
down ones we showed that vanishing thermal mass and non-existence of
temperature generated plasmino mode is the universal feature of the strongly
interacting fermion ... | [
{
"created": "Tue, 7 May 2013 09:32:38 GMT",
"version": "v1"
}
] | 2013-06-24 | [
[
"Seo",
"Yunseok",
""
],
[
"Sin",
"Sang-Jin",
""
],
[
"Zhou",
"Yang",
""
]
] | We investigate fermion self energy problem in the strongly coupled dense medium in holographic approach. By working out bottom up models as well as top down ones we showed that vanishing thermal mass and non-existence of temperature generated plasmino mode is the universal feature of the strongly interacting fermion sy... | 24.988159 | 24.514225 | 25.02479 | 23.753965 | 24.652424 | 25.466177 | 22.852642 | 23.408144 | 24.331488 | 27.48572 | 24.324568 | 21.79702 | 23.749546 | 22.305342 | 23.08297 | 22.580816 | 21.840109 | 22.36236 | 21.463844 | 23.972025 | 21.471193 |
hep-th/9505043 | A. Khare | Avinash Khare | Chern-Simons Term and Charged Vortices in Abelian and Nonabelian Gauge
Theories | To be published in the Proceedings of Indian National Science
Academy, Part A-physical Sciences | Proc.Indian Natl.Sci.Acad.A61:161-178,1995 | null | IP-BBSR/95-3, January 95 | hep-th | null | In this article we review some of the recent advances regarding the charged
vortex solutions in abelian and nonabelian gauge theories with Chern-Simons
(CS) term in two space dimensions. Since these nontrivial results are
essentially because of the CS term, hence, we first discuss in some detail the
various propertie... | [
{
"created": "Sat, 6 May 1995 17:44:17 GMT",
"version": "v1"
}
] | 2011-03-28 | [
[
"Khare",
"Avinash",
""
]
] | In this article we review some of the recent advances regarding the charged vortex solutions in abelian and nonabelian gauge theories with Chern-Simons (CS) term in two space dimensions. Since these nontrivial results are essentially because of the CS term, hence, we first discuss in some detail the various properties ... | 7.486132 | 7.69649 | 8.640427 | 7.382568 | 8.285295 | 8.025989 | 7.995749 | 7.698603 | 7.4755 | 8.734308 | 7.830158 | 7.494107 | 7.656697 | 7.385171 | 7.709079 | 7.622025 | 7.527187 | 7.485079 | 7.658957 | 7.657222 | 7.556751 |
hep-th/0110185 | Maslowski Tomasz | Stanis{\l}aw D. G{\l}azek and Tomasz Mas{\l}owski | Renormalized Poincar\'e algebra for effective particles in quantum field
theory | 17 pages, 5 figures | Phys.Rev. D65 (2002) 065011 | 10.1103/PhysRevD.65.065011 | null | hep-th | null | Using an expansion in powers of an infinitesimally small coupling constant
$g$, all generators of the Poincar\'e group in local scalar quantum field
theory with interaction term $g \phi^3$ are expressed in terms of annihilation
and creation operators $a_\lambda$ and $a^\dagger_\lambda$ that result from a
boost-invari... | [
{
"created": "Fri, 19 Oct 2001 16:53:59 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Głazek",
"Stanisław D.",
""
],
[
"Masłowski",
"Tomasz",
""
]
] | Using an expansion in powers of an infinitesimally small coupling constant $g$, all generators of the Poincar\'e group in local scalar quantum field theory with interaction term $g \phi^3$ are expressed in terms of annihilation and creation operators $a_\lambda$ and $a^\dagger_\lambda$ that result from a boost-invarian... | 9.867018 | 9.897204 | 9.264668 | 8.777744 | 9.572733 | 9.329821 | 9.229607 | 8.740157 | 8.727023 | 10.297894 | 8.890629 | 9.182964 | 9.052578 | 8.883389 | 8.903828 | 9.185328 | 9.295688 | 9.455959 | 8.784123 | 9.111 | 9.446951 |
0708.1770 | Subhaneil Lahiri | Sayantani Bhattacharyya, Subhaneil Lahiri, R. Loganayagam and Shiraz
Minwalla | Large rotating AdS black holes from fluid mechanics | 62 pages, 1 figure. v2: references, typos | JHEP 0809:054,2008 | 10.1088/1126-6708/2008/09/054 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the AdS/CFT correspondence to argue that large rotating black holes in
global AdS(D) spaces are dual to stationary solutions of the relativistic
Navier-Stokes equations on S**(D-2). Reading off the equation of state of this
fluid from the thermodynamics of non-rotating black holes, we proceed to
construct the ... | [
{
"created": "Tue, 14 Aug 2007 17:20:08 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Jul 2008 13:02:44 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Bhattacharyya",
"Sayantani",
""
],
[
"Lahiri",
"Subhaneil",
""
],
[
"Loganayagam",
"R.",
""
],
[
"Minwalla",
"Shiraz",
""
]
] | We use the AdS/CFT correspondence to argue that large rotating black holes in global AdS(D) spaces are dual to stationary solutions of the relativistic Navier-Stokes equations on S**(D-2). Reading off the equation of state of this fluid from the thermodynamics of non-rotating black holes, we proceed to construct the no... | 6.303495 | 5.982275 | 6.739442 | 5.609896 | 6.022491 | 5.963093 | 5.937842 | 5.968235 | 5.813873 | 6.933388 | 5.41682 | 6.000909 | 6.320527 | 5.802697 | 6.009568 | 5.896111 | 5.862936 | 5.889666 | 5.782855 | 6.325584 | 5.837539 |
hep-th/9604041 | Michael Douglas | Michael R. Douglas and Miao Li | D-Brane Realization of N=2 Super Yang-Mills Theory in Four Dimensions | harvmac, 13 pp. Revised discussion of (p,q) 7-branes | null | null | BROWN-HET-1032, RU-96-16 | hep-th | null | We develop and study a D-brane realization of 4D N=2 super Yang-Mills theory.
It is a type IIB string theory compactified on R^6\times K3 and containing
parallel 7-branes. It can also be regarded as a subsector of Vafa's F-theory
compactified on K3\times K3 and is thus dual to the heterotic string on
K3\times T^2. We... | [
{
"created": "Mon, 8 Apr 1996 21:17:57 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Apr 1996 03:42:23 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Douglas",
"Michael R.",
""
],
[
"Li",
"Miao",
""
]
] | We develop and study a D-brane realization of 4D N=2 super Yang-Mills theory. It is a type IIB string theory compactified on R^6\times K3 and containing parallel 7-branes. It can also be regarded as a subsector of Vafa's F-theory compactified on K3\times K3 and is thus dual to the heterotic string on K3\times T^2. We s... | 7.252072 | 7.814898 | 8.116985 | 6.916614 | 7.011819 | 7.1663 | 7.153028 | 7.089832 | 7.232632 | 9.411919 | 6.920974 | 7.175498 | 6.935518 | 7.12503 | 7.128256 | 7.012168 | 6.93163 | 7.024232 | 6.958483 | 6.940969 | 7.026051 |
1309.3764 | Shao-Feng Wu | Yong-Zhuang Li, Shao-Feng Wu, Guo-Hong Yang | Gauss-Bonnet correction to Holographic thermalization: two-point
functions, circular Wilson loops and entanglement entropy | 19 pages, 9 figures, clarifications and references added, to appear
in Phys. Rev. D | Phys. Rev. D 88, 086006 (2013) | 10.1103/PhysRevD.88.086006 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the thermalization of a class of 4-dimensional strongly coupled
theories dual to a 5-dimensional AdS-Vaidya spacetime with Gauss-Bonnet
curvature corrections. We probe the thermalization using the two-point
functions, the expectation values of circular Wilson loops and entanglement
entropy. When boundary sep... | [
{
"created": "Sun, 15 Sep 2013 14:04:05 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Oct 2013 19:12:14 GMT",
"version": "v2"
}
] | 2013-10-30 | [
[
"Li",
"Yong-Zhuang",
""
],
[
"Wu",
"Shao-Feng",
""
],
[
"Yang",
"Guo-Hong",
""
]
] | We study the thermalization of a class of 4-dimensional strongly coupled theories dual to a 5-dimensional AdS-Vaidya spacetime with Gauss-Bonnet curvature corrections. We probe the thermalization using the two-point functions, the expectation values of circular Wilson loops and entanglement entropy. When boundary separ... | 7.86867 | 7.092661 | 8.296889 | 7.131381 | 7.253131 | 7.229975 | 6.730871 | 6.962975 | 7.105456 | 8.28644 | 7.138287 | 7.426185 | 7.857311 | 7.513287 | 7.365648 | 7.477338 | 7.619968 | 7.390101 | 7.454758 | 7.766077 | 7.287942 |
2301.13182 | Georg Stettinger | Martin Schnabl, Georg Stettinger | Open string field theory with stubs | 22 pages | null | 10.1007/JHEP07(2023)032 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | There are various reasons why adding stubs to the vertices of open string
field theory (OSFT) is interesting: Not only the stubs can tame certain
singularities and make the theory more well-behaved, but also the new theory
shares a lot of similarities with closed string field theory, which helps to
improve our unders... | [
{
"created": "Mon, 30 Jan 2023 18:50:28 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Mar 2023 16:03:44 GMT",
"version": "v2"
}
] | 2023-07-26 | [
[
"Schnabl",
"Martin",
""
],
[
"Stettinger",
"Georg",
""
]
] | There are various reasons why adding stubs to the vertices of open string field theory (OSFT) is interesting: Not only the stubs can tame certain singularities and make the theory more well-behaved, but also the new theory shares a lot of similarities with closed string field theory, which helps to improve our understa... | 15.50808 | 13.773228 | 14.980326 | 12.840547 | 14.210956 | 14.177503 | 13.404064 | 13.446773 | 13.735997 | 16.383976 | 14.540292 | 13.778509 | 13.626575 | 13.30654 | 13.620885 | 13.487502 | 13.614374 | 13.951739 | 13.44258 | 14.165653 | 14.200774 |
0808.3379 | David Dudal | D. Dudal, S.P. Sorella, N. Vandersickel, H. Verschelde | The effects of Gribov copies in 2D gauge theories | 10 pages, 1 .eps figure | Phys.Lett.B680:377-383,2009 | 10.1016/j.physletb.2009.08.055 | MIT-CTP 3974 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In previous works, we have shown that the Gribov-Zwanziger action, which
implements the restriction of the domain of integration in the path integral to
the Gribov region, generates extra dynamical effects which influence the
infrared behaviour of the gluon and ghost propagator in SU(N) Yang-Mills gauge
theories. The... | [
{
"created": "Mon, 25 Aug 2008 16:12:52 GMT",
"version": "v1"
}
] | 2009-10-06 | [
[
"Dudal",
"D.",
""
],
[
"Sorella",
"S. P.",
""
],
[
"Vandersickel",
"N.",
""
],
[
"Verschelde",
"H.",
""
]
] | In previous works, we have shown that the Gribov-Zwanziger action, which implements the restriction of the domain of integration in the path integral to the Gribov region, generates extra dynamical effects which influence the infrared behaviour of the gluon and ghost propagator in SU(N) Yang-Mills gauge theories. The l... | 5.975237 | 5.906624 | 6.030669 | 5.611289 | 5.859784 | 5.994172 | 6.110302 | 5.859653 | 5.34538 | 6.278517 | 5.616285 | 5.821185 | 5.888639 | 5.695598 | 5.768108 | 5.731884 | 5.68012 | 5.76706 | 5.631549 | 5.730716 | 5.641644 |
2406.14601 | Kwinten Fransen | Samarth Chawla, Kwinten Fransen, Cynthia Keeler | The Penrose limit of the Weyl double copy | 44+18 pages | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We embed the Penrose limit into the Weyl classical double copy. Thereby, we
provide a lift of the double copy properties of plane wave spacetimes into
black hole geometries and we open a novel avenue towards taking the classical
double copy beyond statements about algebraically special backgrounds. In
particular, the... | [
{
"created": "Thu, 20 Jun 2024 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jul 2024 18:00:01 GMT",
"version": "v2"
}
] | 2024-07-12 | [
[
"Chawla",
"Samarth",
""
],
[
"Fransen",
"Kwinten",
""
],
[
"Keeler",
"Cynthia",
""
]
] | We embed the Penrose limit into the Weyl classical double copy. Thereby, we provide a lift of the double copy properties of plane wave spacetimes into black hole geometries and we open a novel avenue towards taking the classical double copy beyond statements about algebraically special backgrounds. In particular, the P... | 10.967884 | 9.662665 | 9.68398 | 9.574922 | 9.67672 | 10.043382 | 10.312359 | 9.482636 | 10.374342 | 10.306523 | 9.395054 | 9.830856 | 9.991561 | 9.879144 | 9.699637 | 9.662985 | 10.187384 | 9.545387 | 9.710971 | 9.867823 | 9.92532 |
hep-th/9601037 | John Rizos | P.M. Petropoulos(CERN) and J. Rizos(SISSA) | Universal moduli-dependent thresholds in Z(2)xZ(2) orbifolds | 12 pages, Latex, contains two figures, final version, typos corrected | Phys.Lett.B374:49-56,1996 | 10.1016/0370-2693(96)00230-4 | CERN-TH/95-284, SISSA/170/95/EP | hep-th | null | In the context of a recently proposed method for computing exactly string
loop corrections regularized in the infra-red, we determine and calculate the
universal moduli-dependent part of the threshold corrections to the gauge
couplings for the symmetric $Z_2\times Z_2$ orbifold model. We show that these
corrections d... | [
{
"created": "Tue, 9 Jan 1996 19:01:09 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jan 1996 16:47:22 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Aug 1996 12:08:42 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Petropoulos",
"P. M.",
"",
"CERN"
],
[
"Rizos",
"J.",
"",
"SISSA"
]
] | In the context of a recently proposed method for computing exactly string loop corrections regularized in the infra-red, we determine and calculate the universal moduli-dependent part of the threshold corrections to the gauge couplings for the symmetric $Z_2\times Z_2$ orbifold model. We show that these corrections dec... | 11.456382 | 8.244949 | 9.494842 | 7.914559 | 8.15754 | 8.182636 | 8.524218 | 7.984141 | 7.900937 | 9.733281 | 7.762909 | 8.310338 | 8.150336 | 8.203905 | 8.4381 | 8.338344 | 8.451712 | 7.943223 | 8.474106 | 8.372167 | 8.469761 |
hep-th/0106226 | Brigitte Hiller | Alexander A. Osipov and Brigitte Hiller (Centro de Fisica Teorica,
Universidade de Coimbra, Portugal) | Large Mass Invariant Asymptotics of the Effective Action | 5 pages, revtex, no figures | Phys.Rev. D64 (2001) 087701 | 10.1103/PhysRevD.64.087701 | null | hep-th | null | We study the large mass asymptotics of the Dirac operator with a
nondegenerate mass matrix m={diag}(m_1,m_2,m_3) in the presence of scalar and
pseudoscalar background fields taking values in the Lie algebra of the U(3)
group. The corresponding one-loop effective action is regularized by the
Schwinger's proper-time te... | [
{
"created": "Mon, 25 Jun 2001 15:44:46 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Jun 2001 12:18:08 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Osipov",
"Alexander A.",
"",
"Centro de Fisica Teorica,\n Universidade de Coimbra, Portugal"
],
[
"Hiller",
"Brigitte",
"",
"Centro de Fisica Teorica,\n Universidade de Coimbra, Portugal"
]
] | We study the large mass asymptotics of the Dirac operator with a nondegenerate mass matrix m={diag}(m_1,m_2,m_3) in the presence of scalar and pseudoscalar background fields taking values in the Lie algebra of the U(3) group. The corresponding one-loop effective action is regularized by the Schwinger's proper-time tech... | 6.358263 | 6.281502 | 6.504981 | 5.830197 | 6.276284 | 6.569496 | 6.603432 | 5.86165 | 5.702222 | 6.534268 | 6.637761 | 6.020178 | 6.218345 | 5.853994 | 6.137014 | 6.365744 | 6.220509 | 5.999622 | 6.080649 | 6.472938 | 6.071645 |
1808.02052 | Pablo Bueno | Pablo Bueno, Pablo A. Cano, Robie A. Hennigar and Robert B. Mann | Universality of squashed-sphere partition functions | 11 pages, 2 figures; v3: minor modifications to match published
version | Phys. Rev. Lett. 122, 071602 (2019) | 10.1103/PhysRevLett.122.071602 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present several results concerning the free energy of odd-dimensional
conformal field theories (CFTs) on squashed spheres. First, we propose a
formula which computes this quantity for holographic CFTs dual to
higher-curvature gravities with second-order linearized equations of motion. As
opposed to standard on-she... | [
{
"created": "Mon, 6 Aug 2018 18:08:27 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Aug 2018 10:08:50 GMT",
"version": "v2"
},
{
"created": "Fri, 1 Mar 2019 19:54:17 GMT",
"version": "v3"
}
] | 2019-03-05 | [
[
"Bueno",
"Pablo",
""
],
[
"Cano",
"Pablo A.",
""
],
[
"Hennigar",
"Robie A.",
""
],
[
"Mann",
"Robert B.",
""
]
] | We present several results concerning the free energy of odd-dimensional conformal field theories (CFTs) on squashed spheres. First, we propose a formula which computes this quantity for holographic CFTs dual to higher-curvature gravities with second-order linearized equations of motion. As opposed to standard on-shell... | 11.299427 | 10.078155 | 12.136301 | 9.857018 | 10.948598 | 10.385427 | 11.005043 | 10.636611 | 9.891125 | 12.783906 | 9.771104 | 10.924195 | 11.507519 | 10.608486 | 10.74944 | 10.561766 | 10.614222 | 10.320754 | 10.843053 | 11.009402 | 10.625049 |
hep-th/0202176 | Yang-Hui Evariste He | Bo Feng, Yang-Hui He and Nicolas Moeller | The Spectrum of the Neumann Matrix with Zero Modes | 25+1 pages, 3 Figures; typos corrected and some comments added | JHEP 0204 (2002) 038 | 10.1088/1126-6708/2002/04/038 | MIT-CTP-3243 | hep-th | null | We calculate the spectrum of the matrix M' of Neumann coefficients of the
Witten vertex, expressed in the oscillator basis including the zero-mode a_0.
We find that in addition to the known continuous spectrum inside [-1/3,0) of
the matrix M without the zero-modes, there is also an additional eigenvalue
inside (0,1).... | [
{
"created": "Tue, 26 Feb 2002 18:12:54 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Mar 2002 23:51:57 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Feng",
"Bo",
""
],
[
"He",
"Yang-Hui",
""
],
[
"Moeller",
"Nicolas",
""
]
] | We calculate the spectrum of the matrix M' of Neumann coefficients of the Witten vertex, expressed in the oscillator basis including the zero-mode a_0. We find that in addition to the known continuous spectrum inside [-1/3,0) of the matrix M without the zero-modes, there is also an additional eigenvalue inside (0,1). F... | 13.896893 | 13.030602 | 14.752213 | 11.462786 | 13.187069 | 13.83892 | 13.624844 | 12.2918 | 12.791472 | 15.778315 | 12.458139 | 13.33225 | 13.68467 | 12.838372 | 12.977941 | 13.306975 | 12.990193 | 13.087654 | 12.553144 | 13.446308 | 12.637198 |
1209.2357 | Mir Faizal | Mir Faizal | Deformed Super-Yang-Mills in Batalin-Vilkovisky Formalism | 16 pages, 0 figures, accepted for publication in Int. J. Theor. Phys | Int. J. Theor. Phys. 52: 392, 2013 | 10.1007/s10773-012-1344-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we will analyse a three dimensional super-Yang-Mills theory on
a deformed superspace with boundaries. We show that it is possible to obtain an
undeformed theory on the boundary if the bulk superspace is deformed by
imposing a non-vanishing commutator between bosonic and fermionic coordinates.
We will al... | [
{
"created": "Tue, 11 Sep 2012 16:08:51 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Faizal",
"Mir",
""
]
] | In this paper we will analyse a three dimensional super-Yang-Mills theory on a deformed superspace with boundaries. We show that it is possible to obtain an undeformed theory on the boundary if the bulk superspace is deformed by imposing a non-vanishing commutator between bosonic and fermionic coordinates. We will also... | 6.562878 | 5.787394 | 6.404083 | 5.234764 | 5.669955 | 5.45146 | 5.115166 | 5.376136 | 5.34614 | 6.538277 | 5.457089 | 5.470022 | 5.764551 | 5.420536 | 5.772683 | 5.545491 | 5.567491 | 5.488934 | 5.646087 | 5.991467 | 5.657379 |
hep-th/0107045 | Jacob D. Bekenstein | Jacob D. Bekenstein | The Case for Discrete Energy Levels of a Black Hole | Invited talk at "2001: A Spacetime Odyssey", inaugural conference of
the Michigan Center for Theoretical Physics, May 22-25, 2001, 11 pages,
LaTeX209; to appear in the proceedings published by World Scientific
Publishing | Int.J.Mod.Phys. A17S1 (2002) 21-31 | 10.1142/S0217751X02012983 | null | hep-th astro-ph gr-qc quant-ph | null | The adiabatic invariant nature of black hole horizon area in classical
gravity suggests that in quantum theory the corresponding operator has a
discrete spectrum. I here develop further an algebraic approach to black hole
quantization which starts from very elementary assumptions, and proceeds by
exploiting symmetry.... | [
{
"created": "Fri, 6 Jul 2001 05:31:58 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bekenstein",
"Jacob D.",
""
]
] | The adiabatic invariant nature of black hole horizon area in classical gravity suggests that in quantum theory the corresponding operator has a discrete spectrum. I here develop further an algebraic approach to black hole quantization which starts from very elementary assumptions, and proceeds by exploiting symmetry. I... | 16.831356 | 17.017746 | 14.734022 | 13.827735 | 14.866528 | 17.471153 | 15.859005 | 13.77217 | 16.051878 | 14.687877 | 15.642218 | 15.739401 | 14.940759 | 14.719498 | 15.865279 | 15.478487 | 15.746029 | 14.578163 | 15.17683 | 15.450301 | 15.267817 |
hep-th/9309047 | Richard MacKenzie | R. MacKenzie, P.K. Panigrahi and S. Sakhi | Superconductivity in $2+1$ dimensions via Kosterlitz-Thouless Mechanism:
Large-N and Finite-Temperature Analyses | 27 pages + 4 figures and several diagrammatic equations, available
from authors upon request, UdeM-LPN-TH-147 | Int.J.Mod.Phys.A9:3603-3630,1994 | 10.1142/S0217751X94001448 | null | hep-th cond-mat | null | We analyse a $2+1$ dimensional model with charged, relativistic fermions
interacting through a four-Fermi term. Taking advantage of its large-$N$
renormalizability, the various phases of this model are studied at finite
temperature and beyond the leading order in $1/N$. Although the vacuum
expectation value (VEV) of ... | [
{
"created": "Wed, 8 Sep 1993 19:07:55 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"MacKenzie",
"R.",
""
],
[
"Panigrahi",
"P. K.",
""
],
[
"Sakhi",
"S.",
""
]
] | We analyse a $2+1$ dimensional model with charged, relativistic fermions interacting through a four-Fermi term. Taking advantage of its large-$N$ renormalizability, the various phases of this model are studied at finite temperature and beyond the leading order in $1/N$. Although the vacuum expectation value (VEV) of a ... | 7.366142 | 6.828697 | 7.299681 | 7.035384 | 7.420238 | 7.221103 | 7.42259 | 6.813586 | 6.626532 | 8.241569 | 7.16141 | 7.010584 | 7.278286 | 6.990815 | 7.146831 | 7.051827 | 7.019024 | 7.022758 | 6.885906 | 7.299632 | 7.010497 |
1606.01893 | David Tong | Andreas Karch and David Tong | Particle-Vortex Duality from 3d Bosonization | 21 pages. v2: references added | Phys. Rev. X 6, 031043 (2016) | 10.1103/PhysRevX.6.031043 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a simple derivation of particle-vortex duality in d=2+1
dimensions. Our starting point is a relativistic form of flux attachment,
designed to transmute the statistics of particles. From this seed, we derive a
web of new dualities. These include particle-vortex duality for bosons as well
as the recently dis... | [
{
"created": "Mon, 6 Jun 2016 20:00:00 GMT",
"version": "v1"
},
{
"created": "Sun, 19 Jun 2016 15:42:38 GMT",
"version": "v2"
}
] | 2016-09-28 | [
[
"Karch",
"Andreas",
""
],
[
"Tong",
"David",
""
]
] | We provide a simple derivation of particle-vortex duality in d=2+1 dimensions. Our starting point is a relativistic form of flux attachment, designed to transmute the statistics of particles. From this seed, we derive a web of new dualities. These include particle-vortex duality for bosons as well as the recently disco... | 9.328111 | 9.626823 | 9.345329 | 8.628886 | 8.406606 | 8.419946 | 8.552155 | 8.452233 | 8.460517 | 10.136196 | 8.727895 | 8.761042 | 9.697711 | 8.611549 | 8.689864 | 8.510676 | 8.767473 | 8.763492 | 8.660747 | 9.244285 | 8.542735 |
hep-th/0702083 | Ido Adam | Ido Adam, Amit Dekel, Luca Mazzucato, Yaron Oz | Integrability of Type II Superstrings on Ramond-Ramond Backgrounds in
Various Dimensions | LaTeX2e, 56 pages, 1 figure, JHEP style; v2: references added, typos
fixed in some equations; v3: typos fixed to match the published version | JHEP 0706:085,2007 | 10.1088/1126-6708/2007/06/085 | TAUP-2849/07 | hep-th | null | We consider type II superstrings on AdS backgrounds with Ramond-Ramond flux
in various dimensions. We realize the backgrounds as supercosets and analyze
explicitly two classes of models: non-critical superstrings on AdS_{2d} and
critical superstrings on AdS_p\times S^p\times CY. We work both in the
Green--Schwarz and... | [
{
"created": "Sun, 11 Feb 2007 21:30:38 GMT",
"version": "v1"
},
{
"created": "Sat, 12 May 2007 08:34:41 GMT",
"version": "v2"
},
{
"created": "Wed, 26 Sep 2007 14:09:53 GMT",
"version": "v3"
}
] | 2009-11-13 | [
[
"Adam",
"Ido",
""
],
[
"Dekel",
"Amit",
""
],
[
"Mazzucato",
"Luca",
""
],
[
"Oz",
"Yaron",
""
]
] | We consider type II superstrings on AdS backgrounds with Ramond-Ramond flux in various dimensions. We realize the backgrounds as supercosets and analyze explicitly two classes of models: non-critical superstrings on AdS_{2d} and critical superstrings on AdS_p\times S^p\times CY. We work both in the Green--Schwarz and i... | 7.122988 | 7.051333 | 9.02542 | 6.774834 | 6.958467 | 6.850256 | 6.873692 | 6.928973 | 6.274872 | 8.811854 | 6.591397 | 6.84488 | 7.564973 | 6.749005 | 6.892902 | 7.004426 | 7.022038 | 6.781538 | 6.848813 | 7.710864 | 6.700261 |
hep-th/9707004 | A. K. Mishra | R. P. Malik, A. K. Mishra and G. Rajasekaran | Dynamics in a noncommutative phase space | LaTeX-twice, 16 pages | Int.J.Mod.Phys.A13:4759-4776,1998 | 10.1142/S0217751X98002249 | null | hep-th math.QA q-alg | null | Dynamics has been generalized to a noncommutative phase space. The
noncommuting phase space is taken to be invariant under the quantum group
$GL_{q,p}(2)$. The $q$-deformed differential calculus on the phase space is
formulated and using this, both the Hamiltonian and Lagrangian forms of
dynamics have been constructe... | [
{
"created": "Tue, 1 Jul 1997 09:09:19 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Malik",
"R. P.",
""
],
[
"Mishra",
"A. K.",
""
],
[
"Rajasekaran",
"G.",
""
]
] | Dynamics has been generalized to a noncommutative phase space. The noncommuting phase space is taken to be invariant under the quantum group $GL_{q,p}(2)$. The $q$-deformed differential calculus on the phase space is formulated and using this, both the Hamiltonian and Lagrangian forms of dynamics have been constructed.... | 7.587513 | 6.32677 | 7.444428 | 6.200679 | 6.572388 | 6.445274 | 6.29365 | 6.340382 | 6.209306 | 8.62471 | 6.532892 | 6.463859 | 6.896472 | 6.56839 | 6.524773 | 6.357438 | 6.699375 | 6.605946 | 6.456452 | 7.032244 | 6.777559 |
1705.06163 | Timofey Snegirev | I. L. Buchbinder, T. V. Snegirev, Yu. M. Zinoviev | Lagrangian description of massive higher spin supermultiplets in AdS_3
space | 22 pages, no figures; v2: comments, references and new section added,
26 pages | null | 10.1007/JHEP08(2017)021 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the Lagrangian formulation of massive higher spin on-shell (1,0)
supermultiplets in three dimensional anti-de Sitter space. The construction is
based on description of the massive three dimensional fields in terms of
frame-like gauge invariant formalism and technique of gauge invariant
curvatures. For th... | [
{
"created": "Wed, 17 May 2017 13:52:40 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jul 2017 14:40:58 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Snegirev",
"T. V.",
""
],
[
"Zinoviev",
"Yu. M.",
""
]
] | We construct the Lagrangian formulation of massive higher spin on-shell (1,0) supermultiplets in three dimensional anti-de Sitter space. The construction is based on description of the massive three dimensional fields in terms of frame-like gauge invariant formalism and technique of gauge invariant curvatures. For the ... | 8.489458 | 6.199104 | 8.851874 | 6.597348 | 7.342061 | 6.541011 | 7.084278 | 7.218962 | 6.465509 | 9.481997 | 6.612078 | 6.880041 | 8.197615 | 7.282968 | 7.407572 | 7.220816 | 7.198925 | 6.983975 | 6.837179 | 8.115687 | 7.232783 |
hep-th/0512227 | Albrecht Klemm | Albrecht Klemm, Marcos Marino | Counting BPS states on the Enriques Calabi-Yau | 62 pages, v3: some results at genus 3 corrected, more typos corrected | Commun.Math.Phys.280:27-76,2008 | 10.1007/s00220-007-0407-z | CERN-PH-TH/2005-258, MAD-TH-05-9 | hep-th math.AG | null | We study topological string amplitudes for the FHSV model using various
techniques. This model has a type II realization involving a Calabi-Yau
threefold with Enriques fibres, which we call the Enriques Calabi-Yau. By
applying heterotic/type IIA duality, we compute the topological amplitudes in
the fibre to all gener... | [
{
"created": "Mon, 19 Dec 2005 07:29:34 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Feb 2006 06:10:53 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Dec 2006 14:08:45 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Klemm",
"Albrecht",
""
],
[
"Marino",
"Marcos",
""
]
] | We study topological string amplitudes for the FHSV model using various techniques. This model has a type II realization involving a Calabi-Yau threefold with Enriques fibres, which we call the Enriques Calabi-Yau. By applying heterotic/type IIA duality, we compute the topological amplitudes in the fibre to all genera.... | 9.270366 | 7.447173 | 9.333736 | 7.285159 | 8.255792 | 7.803212 | 7.895318 | 7.370339 | 7.38913 | 9.808865 | 7.199358 | 7.773444 | 8.14329 | 7.419692 | 7.877573 | 7.728341 | 7.775316 | 7.531728 | 7.373756 | 8.2028 | 7.433806 |
hep-th/9910162 | Joao Barcelos Neto | R. Amorim, J. Barcelos-Neto and C. Wotzasek | Partially embedding of the quantum mechanical analog of the nonlinear
sigma model | 9 pages, Revtex (multicol), revised and enlarged version | null | null | null | hep-th | null | We consider the quantum mechanical analog of the nonlinear sigma model. There
are difficulties to completely embed this theory by directly using the Batalin,
Fradkin, Fradkina, and Tyutin (BFFT) formalism. We show in this paper how the
BFFT method can be conveniently adapted in order to achieve a gauge theory that
pa... | [
{
"created": "Wed, 20 Oct 1999 16:27:49 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Jun 2000 20:33:04 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Amorim",
"R.",
""
],
[
"Barcelos-Neto",
"J.",
""
],
[
"Wotzasek",
"C.",
""
]
] | We consider the quantum mechanical analog of the nonlinear sigma model. There are difficulties to completely embed this theory by directly using the Batalin, Fradkin, Fradkina, and Tyutin (BFFT) formalism. We show in this paper how the BFFT method can be conveniently adapted in order to achieve a gauge theory that part... | 10.892853 | 9.327619 | 11.090378 | 9.225864 | 9.194446 | 10.067228 | 9.261428 | 9.20614 | 9.039573 | 12.554577 | 9.224626 | 9.406013 | 10.797202 | 9.580329 | 9.520424 | 9.558933 | 9.374167 | 9.411626 | 9.315592 | 11.503705 | 9.172198 |
1408.2185 | Kengo Kikuchi | Kengo Kikuchi, Tetsuya Onogi | Generalized Gradient Flow Equation and Its Application to Super
Yang-Mills Theory | 35 pages, v2: typos corrected and references added, v3: published
version | null | 10.1007/JHEP11(2014)094 | YITP-14-64, OU-HET-822 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the gradient flow equation for field theories with nonlinearly
realized symmetry. Applying the formalism to super Yang-Mills theory, we
construct a supersymmetric extension of the gradient flow equation. It can be
shown that the super gauge symmetry is preserved in the gradient flow.
Furthermore, choosi... | [
{
"created": "Sun, 10 Aug 2014 04:38:07 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Aug 2014 04:13:46 GMT",
"version": "v2"
},
{
"created": "Sat, 1 Nov 2014 13:04:57 GMT",
"version": "v3"
}
] | 2015-06-22 | [
[
"Kikuchi",
"Kengo",
""
],
[
"Onogi",
"Tetsuya",
""
]
] | We generalize the gradient flow equation for field theories with nonlinearly realized symmetry. Applying the formalism to super Yang-Mills theory, we construct a supersymmetric extension of the gradient flow equation. It can be shown that the super gauge symmetry is preserved in the gradient flow. Furthermore, choosing... | 9.513386 | 7.862011 | 9.163597 | 7.989627 | 8.11095 | 7.740715 | 7.352719 | 7.851998 | 7.577338 | 9.262775 | 8.320638 | 8.271974 | 8.968382 | 8.420182 | 8.533636 | 8.411345 | 8.131021 | 8.120404 | 8.885565 | 9.710691 | 8.570014 |
1410.2900 | Mikhail Shifman | M. Shifman, A. Yung | Lessons from supersymmetry: "Instead-of-Confinement" Mechanism | To be published in {\sl Quarks 50}, Murray Gell-Mann Festschrift,
(World Scientific, Singapore, 2015). 20 pp., 3 figs | null | 10.1142/S0217751X14300646 | FTPI-MINN-14/33, UMN-TH-3404/14 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review physical scenarios in different vacua of N=2 supersymmetric QCD
deformed by the mass term \mu for the adjoint matter. This deformation breaks
supersymmetry down to N=1 and, at large \mu, the theory flows to N=1 SQCD. We
focus on dynamical scenarios which can serve as prototypes of what we observe
in real-wo... | [
{
"created": "Fri, 10 Oct 2014 20:08:50 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Shifman",
"M.",
""
],
[
"Yung",
"A.",
""
]
] | We review physical scenarios in different vacua of N=2 supersymmetric QCD deformed by the mass term \mu for the adjoint matter. This deformation breaks supersymmetry down to N=1 and, at large \mu, the theory flows to N=1 SQCD. We focus on dynamical scenarios which can serve as prototypes of what we observe in real-worl... | 11.915851 | 10.315617 | 12.506377 | 10.270577 | 9.792069 | 9.72622 | 9.711658 | 10.129517 | 10.250613 | 13.438955 | 9.728723 | 10.452183 | 11.432228 | 10.537597 | 9.928444 | 10.215056 | 10.298264 | 10.254674 | 10.606294 | 11.718053 | 10.363924 |
2209.02801 | Constantinos Papageorgakis | Gergely K\'antor, Vasilis Niarchos, Constantinos Papageorgakis and
Paul Richmond | 6D (2,0) Bootstrap with soft-Actor-Critic | 30 pages, 10 figures; v2: references added | null | 10.1103/PhysRevD.107.025005 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study numerically the 6D (2,0) superconformal bootstrap using the
soft-Actor-Critic (SAC) algorithm as a stochastic optimizer. We focus on the
four-point functions of scalar superconformal primaries in the energy-momentum
multiplet. Starting from the supergravity limit, we perform searches for
adiabatically varied... | [
{
"created": "Tue, 6 Sep 2022 20:10:01 GMT",
"version": "v1"
},
{
"created": "Fri, 30 Sep 2022 08:47:25 GMT",
"version": "v2"
}
] | 2023-01-25 | [
[
"Kántor",
"Gergely",
""
],
[
"Niarchos",
"Vasilis",
""
],
[
"Papageorgakis",
"Constantinos",
""
],
[
"Richmond",
"Paul",
""
]
] | We study numerically the 6D (2,0) superconformal bootstrap using the soft-Actor-Critic (SAC) algorithm as a stochastic optimizer. We focus on the four-point functions of scalar superconformal primaries in the energy-momentum multiplet. Starting from the supergravity limit, we perform searches for adiabatically varied c... | 15.858932 | 18.636221 | 19.359558 | 15.155771 | 16.572737 | 16.00614 | 16.522739 | 15.66836 | 16.201637 | 18.857038 | 14.37047 | 15.641118 | 15.127303 | 15.02294 | 15.141495 | 15.591082 | 14.87603 | 15.151747 | 14.61194 | 16.347687 | 15.002262 |
1510.03664 | Erik Tonni | Piermarco Fonda, Domenico Seminara, Erik Tonni | On shape dependence of holographic entanglement entropy in AdS4/CFT3 | 49 pages, 11 figures | JHEP 1512 (2015) 037 | 10.1007/JHEP12(2015)037 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the finite term of the holographic entanglement entropy of finite
domains with smooth shapes and for four dimensional gravitational backgrounds.
Analytic expressions depending on the unit vectors normal to the minimal area
surface are obtained for both stationary and time dependent spacetimes. The
special ca... | [
{
"created": "Tue, 13 Oct 2015 13:32:22 GMT",
"version": "v1"
}
] | 2015-12-22 | [
[
"Fonda",
"Piermarco",
""
],
[
"Seminara",
"Domenico",
""
],
[
"Tonni",
"Erik",
""
]
] | We study the finite term of the holographic entanglement entropy of finite domains with smooth shapes and for four dimensional gravitational backgrounds. Analytic expressions depending on the unit vectors normal to the minimal area surface are obtained for both stationary and time dependent spacetimes. The special case... | 10.707432 | 9.699059 | 11.279289 | 9.408077 | 9.51051 | 9.052434 | 9.699152 | 9.402895 | 9.36203 | 11.45006 | 9.650131 | 9.481175 | 10.547184 | 9.760484 | 9.593625 | 9.537151 | 9.287581 | 9.664062 | 9.525115 | 10.232903 | 9.538212 |
2307.10378 | Kiril Hristov | Kiril Hristov and Minwoo Suh | Spindle black holes in AdS$_4 \times$SE$_7$ | 40 pages, 2 figures, 1 Mathematica file; v2: minor corrections | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct new classes of supersymmetric AdS$_2 \times {\Sigma}$ solutions
of 4d gauged supergravity in presence of charged hypermultiplet scalars, with
${\Sigma}$ the complex weighted projective space known as a spindle. These
solutions can be viewed as near-horizon geometries of asymptotically Anti
de-Sitter (AdS... | [
{
"created": "Wed, 19 Jul 2023 18:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Oct 2023 16:03:03 GMT",
"version": "v2"
}
] | 2023-10-31 | [
[
"Hristov",
"Kiril",
""
],
[
"Suh",
"Minwoo",
""
]
] | We construct new classes of supersymmetric AdS$_2 \times {\Sigma}$ solutions of 4d gauged supergravity in presence of charged hypermultiplet scalars, with ${\Sigma}$ the complex weighted projective space known as a spindle. These solutions can be viewed as near-horizon geometries of asymptotically Anti de-Sitter (AdS$_... | 8.359032 | 7.388791 | 9.043408 | 7.556584 | 7.880525 | 7.392003 | 7.631049 | 7.632345 | 7.589539 | 10.964386 | 7.711342 | 8.236346 | 8.629244 | 8.085988 | 8.557738 | 7.878644 | 8.166307 | 8.2726 | 8.007178 | 8.989541 | 7.971015 |
hep-th/0110296 | Peter Gillan | Peter Gillan | General Relativity Contains the Standard Model | 57 pages, no figures, LaTex, improved derivation for actual fine
structure constant (again), elementary tensor particles predicted, added
section on so-called Higgs boson | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Standard Model plus gravitation is derived from general relativity with
three dimensions of time. I claim that when the Lagrangian for general
relativity is calculated using three dimensions of time, the unified field
theory results. I call it 3D time, which stands for three dimensions of time.
This theory differ... | [
{
"created": "Wed, 31 Oct 2001 15:08:06 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Nov 2005 15:36:02 GMT",
"version": "v2"
},
{
"created": "Wed, 29 Sep 2010 14:23:21 GMT",
"version": "v3"
},
{
"created": "Mon, 13 Oct 2014 15:34:05 GMT",
"version": "v4"
}
] | 2014-10-14 | [
[
"Gillan",
"Peter",
""
]
] | The Standard Model plus gravitation is derived from general relativity with three dimensions of time. I claim that when the Lagrangian for general relativity is calculated using three dimensions of time, the unified field theory results. I call it 3D time, which stands for three dimensions of time. This theory differs ... | 7.920282 | 8.934346 | 8.481853 | 8.314474 | 8.551967 | 8.80581 | 8.545039 | 7.981859 | 8.124407 | 8.708483 | 7.86992 | 7.766326 | 8.03159 | 7.938134 | 7.66373 | 7.813789 | 7.827028 | 7.831477 | 7.809981 | 7.952995 | 7.71778 |
1709.02213 | Pavol Severa | Pavol \v{S}evera | On integrability of 2-dimensional $\sigma$-models of Poisson-Lie type | 7 pages | null | 10.1007/JHEP11(2017)015 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a simple procedure for constructing a Lax pair for suitable
2-dimensional $\sigma$-models appearing in Poisson-Lie T-duality
| [
{
"created": "Thu, 7 Sep 2017 12:49:39 GMT",
"version": "v1"
}
] | 2017-12-06 | [
[
"Ševera",
"Pavol",
""
]
] | We describe a simple procedure for constructing a Lax pair for suitable 2-dimensional $\sigma$-models appearing in Poisson-Lie T-duality | 15.538427 | 9.121284 | 13.726051 | 9.27686 | 10.410952 | 10.372752 | 9.190722 | 9.431069 | 9.511231 | 11.286427 | 10.180054 | 11.8675 | 12.352737 | 11.035384 | 11.441101 | 11.525778 | 11.305191 | 11.046432 | 11.606422 | 12.534969 | 11.289083 |
1004.5503 | Alfredo Perez | Ricardo Caroca, Nelson Merino, Alfredo P\'erez and Patricio Salgado | Generating Higher-Order Lie Algebras by Expanding Maurer Cartan Forms | null | Journal of Mathematical Physics 50, 123527 (2009) | 10.1063/1.3272997 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By means of a generalization of the Maurer-Cartan expansion method we
construct a procedure to obtain expanded higher-order Lie algebras. The
expanded higher order Maurer-Cartan equations for the case
$\mathcal{G}=V_{0}\oplus V_{1}$ are found. A dual formulation for the
S-expansion multialgebra procedure is also cons... | [
{
"created": "Fri, 30 Apr 2010 11:28:22 GMT",
"version": "v1"
}
] | 2015-03-17 | [
[
"Caroca",
"Ricardo",
""
],
[
"Merino",
"Nelson",
""
],
[
"Pérez",
"Alfredo",
""
],
[
"Salgado",
"Patricio",
""
]
] | By means of a generalization of the Maurer-Cartan expansion method we construct a procedure to obtain expanded higher-order Lie algebras. The expanded higher order Maurer-Cartan equations for the case $\mathcal{G}=V_{0}\oplus V_{1}$ are found. A dual formulation for the S-expansion multialgebra procedure is also consid... | 10.656146 | 10.112497 | 11.779046 | 10.244447 | 9.913967 | 10.046579 | 9.232496 | 10.422085 | 9.82205 | 12.121623 | 10.151677 | 9.70059 | 10.73653 | 10.034626 | 9.711749 | 9.825923 | 9.543029 | 10.233674 | 10.01028 | 10.720401 | 9.89941 |
hep-th/0512135 | Amanda Weltman | Brian R. Greene and Amanda Weltman | An Effect of $\alpha'$ Corrections on Racetrack Inflation | 13 pages, 4 figures. Typos corrected, references added, this version
to appear in JHEP | JHEP 0603 (2006) 035 | 10.1088/1126-6708/2006/03/035 | null | hep-th | null | We study the effects of $ \alpha '$ corrections to the K\"ahler potential on
volume stabilisation and racetrack inflation. In a region where classical
supergravity analysis is justified, stringy corrections can nevertheless be
relevant for correctly analyzing moduli stabilisation and the onset of
inflation.
| [
{
"created": "Tue, 13 Dec 2005 04:09:00 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Feb 2006 21:27:12 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Greene",
"Brian R.",
""
],
[
"Weltman",
"Amanda",
""
]
] | We study the effects of $ \alpha '$ corrections to the K\"ahler potential on volume stabilisation and racetrack inflation. In a region where classical supergravity analysis is justified, stringy corrections can nevertheless be relevant for correctly analyzing moduli stabilisation and the onset of inflation. | 16.360096 | 12.336934 | 13.92189 | 12.66137 | 13.140201 | 13.724978 | 11.775812 | 12.965681 | 11.721493 | 13.83756 | 13.12738 | 13.435832 | 15.665548 | 12.951518 | 13.38326 | 13.152716 | 13.057655 | 12.664564 | 13.71631 | 14.329864 | 12.986122 |
hep-th/0501009 | Maria Emilia Guimaraes | A. A. Bytsenko (DF/Uel), M. E. X. Guimaraes (MAT/Unb) and V. S. Mendes
(DF/Uel) | Casimir Effect for Gauge Fields in Spaces with Negative Constant
Curvature | 5 pages, no figures. To appear in The European Physical Journal C -
Particles and Fields | Eur.Phys.J. C39 (2005) 249-252 | 10.1140/epjc/s2004-02080-3 | null | hep-th | null | We consider gauge theories based on abelian $p-$forms on real compact
hyperbolic spaces. Using the zeta-function regularization method and the trace
tensor kernel formula, we determine explicitly an expression for the vacuum
energy (Casimir energy) corresponding to skew-symmetric tensor fields. It is
shown that the t... | [
{
"created": "Mon, 3 Jan 2005 11:25:10 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Bytsenko",
"A. A.",
"",
"DF/Uel"
],
[
"Guimaraes",
"M. E. X.",
"",
"MAT/Unb"
],
[
"Mendes",
"V. S.",
"",
"DF/Uel"
]
] | We consider gauge theories based on abelian $p-$forms on real compact hyperbolic spaces. Using the zeta-function regularization method and the trace tensor kernel formula, we determine explicitly an expression for the vacuum energy (Casimir energy) corresponding to skew-symmetric tensor fields. It is shown that the top... | 15.146238 | 12.477601 | 14.944269 | 12.454519 | 11.833225 | 12.709909 | 11.9143 | 12.759022 | 12.730211 | 14.624064 | 12.302058 | 13.334707 | 14.306302 | 13.665493 | 13.489773 | 13.387632 | 13.497178 | 13.883643 | 13.924639 | 14.788316 | 13.657201 |
0710.5372 | Robert de Mello Koch | David Bekker, Robert de Mello Koch and Michael Stephanou | Giant Gravitons - with Strings Attached (III) | 66 pages; v2: improved presentation | JHEP 0802:029,2008 | 10.1088/1126-6708/2008/02/029 | WITS-CTP-033 | hep-th | null | We develop techniques to compute the one-loop anomalous dimensions of
operators in the ${\cal N}=4$ super Yang-Mills theory that are dual to open
strings ending on boundstates of sphere giant gravitons. Our results, which are
applicable to excitations involving an arbitrary number of open strings,
generalize the sing... | [
{
"created": "Mon, 29 Oct 2007 10:31:40 GMT",
"version": "v1"
},
{
"created": "Sun, 13 Jan 2008 11:41:38 GMT",
"version": "v2"
}
] | 2009-05-20 | [
[
"Bekker",
"David",
""
],
[
"Koch",
"Robert de Mello",
""
],
[
"Stephanou",
"Michael",
""
]
] | We develop techniques to compute the one-loop anomalous dimensions of operators in the ${\cal N}=4$ super Yang-Mills theory that are dual to open strings ending on boundstates of sphere giant gravitons. Our results, which are applicable to excitations involving an arbitrary number of open strings, generalize the single... | 7.776505 | 6.349266 | 8.447986 | 6.919879 | 6.760695 | 6.906224 | 6.708635 | 6.660763 | 6.571868 | 9.72166 | 6.740592 | 7.064443 | 7.729777 | 6.851377 | 7.145884 | 7.20618 | 7.306048 | 6.914913 | 7.072496 | 7.790645 | 7.066957 |
hep-th/9410075 | M. Yoshimura | M.Yoshimura | Time Evolution of Pure Quantum State and Emergence of A Nearly Thermal
State | 10 pages, TU/94/468 | null | null | null | hep-th gr-qc | null | Dynamical evolution of the quantum ground state (vacuum) is analyzed for time
variant harmonic oscillators characterized by asymptotically constant
frequency. The oscillatory density matrix in the asymptotic future is uniquely
determined by a constant number of produced particles, independent of other
details of tran... | [
{
"created": "Tue, 11 Oct 1994 07:24:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Yoshimura",
"M.",
""
]
] | Dynamical evolution of the quantum ground state (vacuum) is analyzed for time variant harmonic oscillators characterized by asymptotically constant frequency. The oscillatory density matrix in the asymptotic future is uniquely determined by a constant number of produced particles, independent of other details of transi... | 19.232365 | 19.418591 | 17.161659 | 15.140927 | 16.943045 | 15.869872 | 16.399162 | 14.938323 | 15.505239 | 18.946852 | 16.599188 | 15.67312 | 16.089787 | 15.823748 | 15.756199 | 16.088144 | 15.811804 | 16.360989 | 16.006247 | 16.245977 | 16.670034 |
1702.04754 | J. David Vergara | Carlos A. Margalli and J. David Vergara | Gauge Freedom in complex holomorphic systems | 18 pages | null | null | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of this paper is to introduce and analyze a new gauge symmetry that
appears in complex holomorphic systems. This symmetry allow us to project the
system, using different gauge conditions, to several real systems which are
connect by gauge transformations in the complex space. We prove that the space
of soluti... | [
{
"created": "Wed, 15 Feb 2017 19:54:30 GMT",
"version": "v1"
}
] | 2017-02-17 | [
[
"Margalli",
"Carlos A.",
""
],
[
"Vergara",
"J. David",
""
]
] | The aim of this paper is to introduce and analyze a new gauge symmetry that appears in complex holomorphic systems. This symmetry allow us to project the system, using different gauge conditions, to several real systems which are connect by gauge transformations in the complex space. We prove that the space of solution... | 9.864811 | 9.401521 | 9.858771 | 9.304627 | 10.075354 | 9.255437 | 9.249547 | 8.978496 | 9.205747 | 11.12769 | 9.11716 | 9.364296 | 9.922786 | 9.413247 | 9.504286 | 9.388453 | 9.237525 | 9.194849 | 9.345991 | 9.839559 | 9.409977 |
hep-th/0408162 | Joe Polchinski | Nelia Mann and Joseph Polchinski | Finite Density States in Integrable Conformal Field Theories | 21 pages. To appear in "From Fields to Strings: Circumnavigating
Theoretical Physics," in memory of Ian Kogan. v. 2: added references | null | 10.1142/9789812775344_0031 | NSF-KITP-04-101 | hep-th | null | We study states of large charge density in integrable conformal coset models.
For the O(2) coset, we consider two different S-matrices, one corresponding to
a Thirring mass perturbation and the other to the continuation to O(2+epsilon).
The former leads to simplification in the conformal limit; the latter gives a
mor... | [
{
"created": "Fri, 20 Aug 2004 19:17:43 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Dec 2004 20:11:12 GMT",
"version": "v2"
}
] | 2016-11-23 | [
[
"Mann",
"Nelia",
""
],
[
"Polchinski",
"Joseph",
""
]
] | We study states of large charge density in integrable conformal coset models. For the O(2) coset, we consider two different S-matrices, one corresponding to a Thirring mass perturbation and the other to the continuation to O(2+epsilon). The former leads to simplification in the conformal limit; the latter gives a more ... | 10.877532 | 11.566135 | 11.822027 | 10.228908 | 11.8788 | 11.159954 | 12.333888 | 10.526889 | 10.593087 | 13.478363 | 10.56862 | 10.506234 | 11.43676 | 10.177127 | 10.281894 | 10.585596 | 10.460196 | 10.757652 | 10.223724 | 11.413049 | 10.33675 |
1310.6966 | Salah Haouat | S. Haouat and K. Nouicer | Influence of a Minimal Length on the Creation of Scalar Particles | significant improvement, 24 pages, 1 figure, Accepted for publication
in prd | Phys. Rev. D 89, 105030 (2014) | 10.1103/PhysRevD.89.105030 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we have studied the problem of scalar particles pair creation
by an electric field in the presence of a minimal length. Two sets of exact
solutions for the Klein Gordon equation are given in momentum space. Then the
canonical method based on Bogoliubov transformation connecting the "in" with
the "out" s... | [
{
"created": "Fri, 25 Oct 2013 15:54:49 GMT",
"version": "v1"
},
{
"created": "Tue, 20 May 2014 19:47:35 GMT",
"version": "v2"
}
] | 2014-06-11 | [
[
"Haouat",
"S.",
""
],
[
"Nouicer",
"K.",
""
]
] | In this paper we have studied the problem of scalar particles pair creation by an electric field in the presence of a minimal length. Two sets of exact solutions for the Klein Gordon equation are given in momentum space. Then the canonical method based on Bogoliubov transformation connecting the "in" with the "out" sta... | 7.626203 | 7.045013 | 6.658797 | 6.71525 | 6.643004 | 6.833127 | 7.146049 | 6.267797 | 6.656843 | 7.201429 | 6.858586 | 7.020485 | 6.998537 | 6.81083 | 6.992379 | 7.020721 | 6.93885 | 7.11249 | 6.704779 | 6.963468 | 7.10334 |
0803.2998 | Mukund Rangamani | Pau Figueras, Hari K Kunduri, James Lucietti, Mukund Rangamani | Extremal vacuum black holes in higher dimensions | 53 pages, latex, 19 eps figures. v2: added refs + one eps figure. v3:
published version | Phys.Rev.D78:044042,2008 | 10.1103/PhysRevD.78.044042 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider extremal black hole solutions to the vacuum Einstein equations in
dimensions greater than five. We prove that the near-horizon geometry of any
such black hole must possess an SO(2,1) symmetry in a special case where one
has an enhanced rotational symmetry group. We construct examples of vacuum
near-horizo... | [
{
"created": "Thu, 20 Mar 2008 13:12:43 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Apr 2008 13:19:38 GMT",
"version": "v2"
},
{
"created": "Thu, 25 Sep 2008 16:43:46 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Figueras",
"Pau",
""
],
[
"Kunduri",
"Hari K",
""
],
[
"Lucietti",
"James",
""
],
[
"Rangamani",
"Mukund",
""
]
] | We consider extremal black hole solutions to the vacuum Einstein equations in dimensions greater than five. We prove that the near-horizon geometry of any such black hole must possess an SO(2,1) symmetry in a special case where one has an enhanced rotational symmetry group. We construct examples of vacuum near-horizon ... | 7.098252 | 7.204572 | 7.127289 | 6.859892 | 7.058743 | 7.288759 | 7.311663 | 6.896976 | 7.17457 | 8.30897 | 7.208754 | 7.215321 | 6.900285 | 7.05089 | 6.913311 | 7.131958 | 7.387158 | 6.977723 | 7.144806 | 7.22383 | 6.976989 |
hep-th/9111017 | null | C. Vafa | Topological Mirrors and Quantum Rings | 24 p | null | null | null | hep-th | null | Aspects of duality and mirror symmetry in string theory are discussed. We
emphasize, through examples, the importance of loop spaces for a deeper
understanding of the geometrical origin of dualities in string theory. Moreover
we show that mirror symmetry can be reformulated in very simple terms as the
statement of eq... | [
{
"created": "Thu, 7 Nov 1991 17:19:12 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Vafa",
"C.",
""
]
] | Aspects of duality and mirror symmetry in string theory are discussed. We emphasize, through examples, the importance of loop spaces for a deeper understanding of the geometrical origin of dualities in string theory. Moreover we show that mirror symmetry can be reformulated in very simple terms as the statement of equi... | 7.802418 | 7.362818 | 8.185992 | 7.027758 | 7.610777 | 6.839766 | 7.051656 | 6.899838 | 6.990483 | 8.205078 | 6.847723 | 6.736426 | 7.427722 | 6.802553 | 6.907925 | 6.917728 | 6.74824 | 6.788671 | 6.903978 | 7.327637 | 6.790781 |
hep-th/9805056 | Michael Bershadsky | Michael Bershadsky, Tony Pantev and Vladimir Sadov | F-Theory with Quantized Fluxes | 41 pages, harvmac, 35 figures, references corrected | Adv.Theor.Math.Phys. 3 (1999) 727-773 | null | HUTP-98/A029 | hep-th | null | We present evidence that the CHL string in eight dimensions is dual to
F-theory compactified on an elliptic K3 with a $\Gamma_{0}(2)$ monodromy group.
The monodromy group $\Gamma_{0}(2)$ allows one to turn on the flux of an
antisymmetric two form along the base. The $B_{\mu \nu}$ flux is quantized and
therefore the m... | [
{
"created": "Mon, 11 May 1998 14:01:02 GMT",
"version": "v1"
},
{
"created": "Thu, 28 May 1998 17:36:59 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Bershadsky",
"Michael",
""
],
[
"Pantev",
"Tony",
""
],
[
"Sadov",
"Vladimir",
""
]
] | We present evidence that the CHL string in eight dimensions is dual to F-theory compactified on an elliptic K3 with a $\Gamma_{0}(2)$ monodromy group. The monodromy group $\Gamma_{0}(2)$ allows one to turn on the flux of an antisymmetric two form along the base. The $B_{\mu \nu}$ flux is quantized and therefore the mod... | 7.653307 | 6.771567 | 7.361232 | 6.890102 | 7.183774 | 6.601455 | 7.148407 | 7.219487 | 6.971592 | 8.579517 | 6.71231 | 7.006962 | 7.078585 | 6.897254 | 7.026051 | 6.986548 | 6.986443 | 7.119608 | 6.726661 | 7.4149 | 7.020135 |
1708.08470 | Robert Penna | Robert F. Penna | ${\rm BMS}_3$ invariant fluid dynamics at null infinity | 15 pages | null | 10.1088/1361-6382/aaa3aa | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the boundary dynamics of asymptotically flat, three dimensional
gravity. The boundary is governed by a momentum conservation equation and an
energy conservation equation, which we interpret as fluid equations, following
the membrane paradigm. We reformulate the boundary's equations of motion as
Hamiltonian... | [
{
"created": "Mon, 28 Aug 2017 18:01:19 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Jan 2018 14:28:35 GMT",
"version": "v2"
}
] | 2018-02-14 | [
[
"Penna",
"Robert F.",
""
]
] | We revisit the boundary dynamics of asymptotically flat, three dimensional gravity. The boundary is governed by a momentum conservation equation and an energy conservation equation, which we interpret as fluid equations, following the membrane paradigm. We reformulate the boundary's equations of motion as Hamiltonian f... | 7.472633 | 8.104548 | 7.948593 | 7.363751 | 8.397665 | 7.987227 | 8.216026 | 7.390055 | 7.374527 | 9.502256 | 7.574923 | 7.445204 | 7.115241 | 7.292682 | 7.364547 | 7.395969 | 7.4486 | 7.273571 | 7.344735 | 7.371822 | 7.137116 |
1509.08738 | Yuxuan Peng | Li-Ming Cao, Yuxuan Peng | Counterterms in Massive Gravity Theory | revtex4, 13pages, no figure. The form of the counterterms slightly
changed and some formulae corrected. 2 citations added. Language slightly
modified | Phys. Rev. D 92, 124052 (2015) | 10.1103/PhysRevD.92.124052 | ICTS-USTC-15-11 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derived local boundary counterterms in massive gravity theory with a
negative cosmological constant in four dimensions. With these counterterms at
hand we analyzed the properties of the boundary field theory in the context of
AdS/CFT duality by calculating the boundary stress energy tensor. The
calculation shows t... | [
{
"created": "Tue, 29 Sep 2015 13:28:24 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Nov 2015 11:31:41 GMT",
"version": "v2"
}
] | 2015-12-30 | [
[
"Cao",
"Li-Ming",
""
],
[
"Peng",
"Yuxuan",
""
]
] | We derived local boundary counterterms in massive gravity theory with a negative cosmological constant in four dimensions. With these counterterms at hand we analyzed the properties of the boundary field theory in the context of AdS/CFT duality by calculating the boundary stress energy tensor. The calculation shows tha... | 10.163651 | 9.947735 | 10.742438 | 8.909684 | 10.237417 | 9.769466 | 9.510971 | 9.4443 | 9.090371 | 10.661097 | 9.128182 | 8.920394 | 9.606053 | 9.427919 | 9.401252 | 9.108254 | 9.027527 | 9.345108 | 9.102712 | 10.044849 | 9.023688 |
2312.11660 | Ant\'onio Antunes | Ant\'onio Antunes, Sebastian Harris, Apratim Kaviraj, Volker Schomerus | Lining up a Positive Semi-Definite Six-Point Bootstrap | 45 pages + appendices, 13 figures; v2: added references, minor
clarifications and details on numerical implementation, matches JHEP version | JHEP06(2024)058 | 10.1007/JHEP06(2024)058 | DESY-23-220 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we initiate a positive semi-definite numerical bootstrap program
for multi-point correlators. Considering six-point functions of operators on a
line we reformulate the crossing symmetry equation for a pair of comb-channel
expansions as a semi-definite programming problem. We provide two alternative
formu... | [
{
"created": "Mon, 18 Dec 2023 19:13:09 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jun 2024 16:26:21 GMT",
"version": "v2"
}
] | 2024-06-19 | [
[
"Antunes",
"António",
""
],
[
"Harris",
"Sebastian",
""
],
[
"Kaviraj",
"Apratim",
""
],
[
"Schomerus",
"Volker",
""
]
] | In this work we initiate a positive semi-definite numerical bootstrap program for multi-point correlators. Considering six-point functions of operators on a line we reformulate the crossing symmetry equation for a pair of comb-channel expansions as a semi-definite programming problem. We provide two alternative formula... | 16.035662 | 13.467584 | 16.801407 | 12.446658 | 13.020926 | 12.553679 | 12.967659 | 12.010837 | 11.945579 | 18.67601 | 13.813813 | 12.715642 | 15.375095 | 13.400152 | 13.669644 | 12.944981 | 13.149225 | 13.941032 | 13.402696 | 14.958324 | 13.758193 |
2101.02209 | Yue Li | Vijay Balasubramanian, Matthew DeCross, Arjun Kar, Cathy Li, Onkar
Parrikar | Complexity Growth in Integrable and Chaotic Models | 70+13 pages, 29 figures | null | 10.1007/JHEP07(2021)011 | null | hep-th cs.CC quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the SYK family of models with $N$ Majorana fermions to study the
complexity of time evolution, formulated as the shortest geodesic length on the
unitary group manifold between the identity and the time evolution operator, in
free, integrable, and chaotic systems. Initially, the shortest geodesic follows
the ti... | [
{
"created": "Wed, 6 Jan 2021 19:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Apr 2021 02:30:47 GMT",
"version": "v2"
}
] | 2021-07-21 | [
[
"Balasubramanian",
"Vijay",
""
],
[
"DeCross",
"Matthew",
""
],
[
"Kar",
"Arjun",
""
],
[
"Li",
"Cathy",
""
],
[
"Parrikar",
"Onkar",
""
]
] | We use the SYK family of models with $N$ Majorana fermions to study the complexity of time evolution, formulated as the shortest geodesic length on the unitary group manifold between the identity and the time evolution operator, in free, integrable, and chaotic systems. Initially, the shortest geodesic follows the time... | 7.457864 | 8.022487 | 8.745176 | 7.229861 | 8.091062 | 7.559157 | 8.023107 | 7.681998 | 7.470082 | 8.677899 | 7.492188 | 7.214745 | 7.580443 | 7.220243 | 7.175111 | 7.111482 | 7.325977 | 7.087384 | 7.323015 | 7.44188 | 7.096151 |
1012.2841 | Dmitri Gal'tsov | D.V. Gal'tsov, E.Yu. Melkumova and S. Zamani-Mogaddam | Nambu-Goldstone explosion under brane perforation | 7 pages, Latex | JETP Letters, 2010. Vol 92, No. 5, pp. 276-280 | 10.1134/S0021364010170029 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that perforation of the three-brane by mass impinging upon it from
the five-dimensional bulk excites Nambu-Goldstone spherical wave propagating
outwards with the velocity of light. It is speculated that such an effect can
give rise to "`unmotivated" energy release events in the brane-world
cosmological models... | [
{
"created": "Mon, 13 Dec 2010 19:51:04 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Gal'tsov",
"D. V.",
""
],
[
"Melkumova",
"E. Yu.",
""
],
[
"Zamani-Mogaddam",
"S.",
""
]
] | We show that perforation of the three-brane by mass impinging upon it from the five-dimensional bulk excites Nambu-Goldstone spherical wave propagating outwards with the velocity of light. It is speculated that such an effect can give rise to "`unmotivated" energy release events in the brane-world cosmological models. | 22.038498 | 21.846029 | 19.834936 | 17.512264 | 19.530046 | 21.163235 | 19.326727 | 20.276501 | 18.863785 | 22.001024 | 21.072058 | 20.16864 | 19.186821 | 19.814798 | 20.050331 | 21.430513 | 20.842566 | 19.632988 | 19.307928 | 18.708727 | 20.491352 |
2001.06800 | Giulia Isabella | Adam Falkowski, Giulia Isabella | Matter Coupling in Massive Gravity | 21 pages, 1 figure | JHEP 04 (2020) 014 | 10.1007/JHEP04(2020)014 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the dRGT massive gravity interacting with spin-0, spin-1/2, or
spin-1 matter. The effective theory of a massive spin-2 particle coupled to
matter particles is constructed directly at the amplitude level. In this
setting we calculate the gravitational Compton scattering amplitudes and study
their UV propert... | [
{
"created": "Sun, 19 Jan 2020 09:57:26 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Apr 2020 10:47:31 GMT",
"version": "v2"
}
] | 2020-04-07 | [
[
"Falkowski",
"Adam",
""
],
[
"Isabella",
"Giulia",
""
]
] | We discuss the dRGT massive gravity interacting with spin-0, spin-1/2, or spin-1 matter. The effective theory of a massive spin-2 particle coupled to matter particles is constructed directly at the amplitude level. In this setting we calculate the gravitational Compton scattering amplitudes and study their UV propertie... | 6.788149 | 5.750917 | 6.338295 | 6.052243 | 6.077394 | 6.41439 | 6.312726 | 6.369604 | 5.875479 | 7.126814 | 5.949538 | 6.217707 | 6.33978 | 6.143947 | 6.285499 | 6.268826 | 6.230539 | 6.175208 | 6.345526 | 6.540124 | 6.315747 |
2210.13970 | Harvendra Singh | Harvendra Singh | Islands and Icebergs may contribute nothing to the Page curve | 13 pages, 04 figures; v2: typos corrected; v3: small corrections,
redrawn figs, footnote added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the entanglement entropy of a subsystem in contact with symmetrical
bath where the complete system lives on the boundary of AdS3 spacetime. The
system-A is taken to be in the middle of the bath system-B and the full system
is taken to be some fixed localized region of the boundary 2-dimensional CFT.
We gener... | [
{
"created": "Tue, 25 Oct 2022 12:55:22 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Nov 2022 11:03:03 GMT",
"version": "v2"
},
{
"created": "Mon, 12 Feb 2024 09:38:30 GMT",
"version": "v3"
}
] | 2024-02-13 | [
[
"Singh",
"Harvendra",
""
]
] | We study the entanglement entropy of a subsystem in contact with symmetrical bath where the complete system lives on the boundary of AdS3 spacetime. The system-A is taken to be in the middle of the bath system-B and the full system is taken to be some fixed localized region of the boundary 2-dimensional CFT. We general... | 21.826864 | 22.307352 | 23.424559 | 21.104074 | 20.676315 | 22.380159 | 22.0648 | 21.928091 | 21.074274 | 26.12875 | 20.613155 | 21.254526 | 21.395527 | 20.385923 | 21.203911 | 21.400776 | 21.043587 | 20.874907 | 20.909788 | 22.106958 | 20.934456 |
2106.00693 | Thomas Vandermeulen | Daniel Robbins, Eric Sharpe, Thomas Vandermeulen | Anomalies, Extensions and Orbifolds | 37 pages, 2 appendices, 3 figures | Phys. Rev. D 104, 085009 (2021) | 10.1103/PhysRevD.104.085009 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate gauge anomalies in the context of orbifold conformal field
theories. Such anomalies manifest as failures of modular invariance in the
constituents of the orbifold partition function. We review how this
irregularity is classified by cohomology and how extending the orbifold group
can remove it. Working ... | [
{
"created": "Tue, 1 Jun 2021 18:00:04 GMT",
"version": "v1"
}
] | 2021-10-13 | [
[
"Robbins",
"Daniel",
""
],
[
"Sharpe",
"Eric",
""
],
[
"Vandermeulen",
"Thomas",
""
]
] | We investigate gauge anomalies in the context of orbifold conformal field theories. Such anomalies manifest as failures of modular invariance in the constituents of the orbifold partition function. We review how this irregularity is classified by cohomology and how extending the orbifold group can remove it. Working wi... | 13.082771 | 12.184005 | 14.968152 | 11.874046 | 12.912278 | 11.989834 | 12.434877 | 11.752254 | 11.603902 | 14.979563 | 11.65262 | 12.908604 | 13.635632 | 12.170452 | 12.427577 | 12.344634 | 12.461749 | 11.830731 | 12.780889 | 13.008036 | 12.140675 |
hep-th/9402130 | Denis Juriev | Denis Juriev | Setting Hidden Symmetries Free by the Noncommutative Veronese Mapping | 5 pages, AMSTEX (style AMSPPT) | J.Math.Phys. 35 (1994) 5021-5024 | 10.1063/1.530895 | null | hep-th alg-geom math.AG | null | The short note is devoted to the setting free of hidden symmetries in Verma
modules over sl(2,C) by the noncommutative Veronese mappings.
| [
{
"created": "Wed, 23 Feb 1994 11:24:20 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Juriev",
"Denis",
""
]
] | The short note is devoted to the setting free of hidden symmetries in Verma modules over sl(2,C) by the noncommutative Veronese mappings. | 21.996613 | 18.854149 | 27.075733 | 20.536953 | 20.854292 | 24.739826 | 20.576368 | 23.420269 | 19.659214 | 25.869013 | 20.746815 | 22.379454 | 22.546537 | 21.439953 | 21.736027 | 20.483583 | 21.542282 | 20.340006 | 19.785595 | 20.464342 | 20.425751 |
1806.06963 | Kyung Kiu Kim | Kyung Kiu Kim and O-Kab Kwon | Janus ABJM Models with Mass Deformation | 17 pages, references added, published version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a large class of ${\cal N} = 3$ Janus ABJM models with mass
deformation, where the mass depends on a spatial (or lightcone) coordinate. We
also show that the resulting Janus model can be identified with an effective
action of M2-branes in the presence of a background self-dual 4-form field
strength varyi... | [
{
"created": "Mon, 18 Jun 2018 21:48:25 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Aug 2018 08:10:28 GMT",
"version": "v2"
}
] | 2018-08-28 | [
[
"Kim",
"Kyung Kiu",
""
],
[
"Kwon",
"O-Kab",
""
]
] | We construct a large class of ${\cal N} = 3$ Janus ABJM models with mass deformation, where the mass depends on a spatial (or lightcone) coordinate. We also show that the resulting Janus model can be identified with an effective action of M2-branes in the presence of a background self-dual 4-form field strength varying... | 10.486006 | 8.318995 | 9.769403 | 8.903286 | 8.240401 | 7.802951 | 8.159696 | 8.388026 | 8.499479 | 11.623769 | 8.218245 | 8.941451 | 9.943242 | 8.464403 | 8.426311 | 8.985389 | 8.591883 | 8.307585 | 8.411201 | 9.403045 | 8.860654 |
hep-th/0104047 | Alexander Kovner | Ian. I Kogan (Oxford U.), Alex Kovner (CERN and Plymouth U.), Bayram
Tekin (Oxford U.) | Deconfinement at N>2: SU(N) Georgi-Glashow model in 2+1 dimensions | 25 pages, Latex | JHEP 0105:062,2001 | 10.1088/1126-6708/2001/05/062 | CERN-TH/2001-103 | hep-th hep-lat hep-ph | null | We analyse the deconfining phase transition in the SU(N) Georgi-Glashow model
in 2+1 dimensions. We show that the phase transition is second order for any N,
and the universality class is different from the Z(N) invariant Villain model.
At large N the conformal theory describing the fixed point is a deformed
SU(N)_1 ... | [
{
"created": "Thu, 5 Apr 2001 09:51:54 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Kogan",
"Ian. I",
"",
"Oxford U."
],
[
"Kovner",
"Alex",
"",
"CERN and Plymouth U."
],
[
"Tekin",
"Bayram",
"",
"Oxford U."
]
] | We analyse the deconfining phase transition in the SU(N) Georgi-Glashow model in 2+1 dimensions. We show that the phase transition is second order for any N, and the universality class is different from the Z(N) invariant Villain model. At large N the conformal theory describing the fixed point is a deformed SU(N)_1 WZ... | 5.839393 | 5.360697 | 6.318347 | 5.463591 | 5.654048 | 5.340111 | 5.54795 | 5.211015 | 5.305071 | 6.591483 | 5.162279 | 5.292761 | 6.156332 | 5.392038 | 5.490637 | 5.5929 | 5.291468 | 5.525583 | 5.455227 | 6.031483 | 5.459497 |
1708.05090 | Jia-ju Zhang | Song He, Feng-Li Lin and Jia-ju Zhang | Dissimilarities of reduced density matrices and eigenstate
thermalization hypothesis | V1, 34 pages, 5 figures, see collection of complete results in the
attached Mathematica notebook; V2, 38 pages, 5 figures, published version | JHEP 1712 (2017) 073 | 10.1007/JHEP12(2017)073 | null | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate various quantities that characterize the dissimilarity of
reduced density matrices for a short interval of length $\ell$ in a
two-dimensional (2D) large central charge conformal field theory (CFT). These
quantities include the R\'enyi entropy, entanglement entropy, relative entropy,
Jensen-Shannon diverg... | [
{
"created": "Wed, 16 Aug 2017 21:56:35 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Dec 2017 05:23:05 GMT",
"version": "v2"
}
] | 2017-12-25 | [
[
"He",
"Song",
""
],
[
"Lin",
"Feng-Li",
""
],
[
"Zhang",
"Jia-ju",
""
]
] | We calculate various quantities that characterize the dissimilarity of reduced density matrices for a short interval of length $\ell$ in a two-dimensional (2D) large central charge conformal field theory (CFT). These quantities include the R\'enyi entropy, entanglement entropy, relative entropy, Jensen-Shannon divergen... | 7.910813 | 7.49021 | 9.203427 | 6.913458 | 7.188621 | 6.857631 | 7.636712 | 7.216913 | 7.079892 | 8.895697 | 6.990756 | 7.21147 | 7.799702 | 7.282776 | 7.107312 | 7.020618 | 7.253022 | 7.152678 | 7.202475 | 7.841672 | 7.096803 |
2401.17458 | Eiji Konishi | Eiji Konishi | Lorentzian holographic gravity and the time-energy uncertainty principle | 3 pages, revtex | JHAP 4, (1) (2024) 65 | 10.22128/jhap.2024.780.1068 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article, we present a heuristic derivation of the on-shell equation
of the Lorentzian classicalized holographic tensor network in the presence of a
non-zero mass in the bulk spacetime. This derivation of the on-shell equation
is based on two physical assumptions. First, the Lorentzian bulk theory is in
the gr... | [
{
"created": "Tue, 30 Jan 2024 21:41:09 GMT",
"version": "v1"
}
] | 2024-03-28 | [
[
"Konishi",
"Eiji",
""
]
] | In this article, we present a heuristic derivation of the on-shell equation of the Lorentzian classicalized holographic tensor network in the presence of a non-zero mass in the bulk spacetime. This derivation of the on-shell equation is based on two physical assumptions. First, the Lorentzian bulk theory is in the grou... | 11.023111 | 11.044937 | 11.041137 | 9.732734 | 10.1708 | 10.595093 | 9.488534 | 10.726958 | 9.649117 | 12.89473 | 10.52366 | 10.377012 | 10.137172 | 10.174063 | 9.863941 | 10.314797 | 10.506752 | 10.343942 | 10.034978 | 10.454587 | 10.814157 |
hep-th/9602055 | Lorenzo Magnea | Paolo Di Vecchia, Alberto Lerda, Lorenzo Magnea, Raffaele Marotta,
Rodolfo Russo | Renormalization constants from string theory | 15 pages. Latex, uses crckapb.sty. Proceedings Erice '95 | null | null | DFTT 82/95 | hep-th | null | We review some recent results on the calculation of renormalization constants
in Yang-Mills theory using open bosonic strings. The technology of string
amplitudes, supplemented with an appropriate continuation off the mass shell,
can be used to compute the ultraviolet divergences of dimensionally regularized
gauge th... | [
{
"created": "Mon, 12 Feb 1996 13:21:01 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Di Vecchia",
"Paolo",
""
],
[
"Lerda",
"Alberto",
""
],
[
"Magnea",
"Lorenzo",
""
],
[
"Marotta",
"Raffaele",
""
],
[
"Russo",
"Rodolfo",
""
]
] | We review some recent results on the calculation of renormalization constants in Yang-Mills theory using open bosonic strings. The technology of string amplitudes, supplemented with an appropriate continuation off the mass shell, can be used to compute the ultraviolet divergences of dimensionally regularized gauge theo... | 8.608986 | 8.015073 | 8.267137 | 7.376096 | 7.875709 | 8.62678 | 9.468788 | 7.987386 | 7.498665 | 9.335719 | 7.626877 | 7.246271 | 7.896316 | 7.329556 | 7.641482 | 7.405223 | 7.490599 | 7.232949 | 7.39447 | 7.693066 | 7.271358 |
2306.11597 | Shima Peyravi | Nematollah Riazi and Marzieh Peyravi | Fluid Dynamical Description of Sine-Gordon Solitons | null | null | null | null | hep-th nlin.PS physics.flu-dyn | http://creativecommons.org/licenses/by/4.0/ | We present a fluid dynamical description of a relativistic scalar field in
$1+1$ dimensions and apply the general results to the special case of
Sine-Gordon solitons. The results which include the local quantities pressure,
density and fluid velocity are compared to the standard quantities attributed
to the solitons.... | [
{
"created": "Tue, 20 Jun 2023 15:14:31 GMT",
"version": "v1"
}
] | 2023-07-31 | [
[
"Riazi",
"Nematollah",
""
],
[
"Peyravi",
"Marzieh",
""
]
] | We present a fluid dynamical description of a relativistic scalar field in $1+1$ dimensions and apply the general results to the special case of Sine-Gordon solitons. The results which include the local quantities pressure, density and fluid velocity are compared to the standard quantities attributed to the solitons. | 12.271464 | 10.16667 | 10.484549 | 9.511039 | 9.736917 | 9.877099 | 10.198977 | 10.117472 | 9.642009 | 10.215761 | 9.574365 | 10.314616 | 10.384233 | 9.835731 | 10.019274 | 9.905821 | 10.014812 | 9.463238 | 10.54026 | 10.204726 | 9.758378 |
1508.00926 | Pablo Pais | Alfredo Iorio and Pablo Pais | Revisiting the gauge fields of strained graphene | 24 pages, 6 figures. Comments added, text reduced and relevant
references included | Phys. Rev. D 92, 125005 (2015) | 10.1103/PhysRevD.92.125005 | null | hep-th cond-mat.mtrl-sci gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that, when graphene is only subject to strain, the spin connection
gauge field that arises plays no measurable role, but when intrinsic curvature
is present and strain is small, spin connection dictates most the physics. We
do so by showing that the Weyl field associated with strain is a pure gauge
field and ... | [
{
"created": "Tue, 4 Aug 2015 21:57:59 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Dec 2015 17:02:36 GMT",
"version": "v2"
}
] | 2015-12-14 | [
[
"Iorio",
"Alfredo",
""
],
[
"Pais",
"Pablo",
""
]
] | We show that, when graphene is only subject to strain, the spin connection gauge field that arises plays no measurable role, but when intrinsic curvature is present and strain is small, spin connection dictates most the physics. We do so by showing that the Weyl field associated with strain is a pure gauge field and no... | 11.17817 | 11.706844 | 11.362245 | 11.312875 | 11.927598 | 12.449882 | 11.898627 | 11.48953 | 11.290651 | 12.508557 | 10.846428 | 11.146836 | 10.804304 | 10.678672 | 10.755108 | 11.028609 | 10.717399 | 10.96797 | 10.689723 | 11.009157 | 10.912277 |
2202.11123 | Nicolas Wink | Jan M. Pawlowski, Coralie S. Schneider and Nicolas Wink | On Gauge Consistency In Gauge-Fixed Yang-Mills Theory | 27 pages, 19 figures | null | null | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate BRST invariance in Landau gauge Yang-Mills theory with
functional methods. To that end, we solve the coupled system of functional
renormalisation group equations for the momentum-dependent ghost and gluon
propagator, ghost-gluon, and three- and four-gluon vertex dressings. The
equations for both, trans... | [
{
"created": "Tue, 22 Feb 2022 19:05:46 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Aug 2022 11:05:40 GMT",
"version": "v2"
}
] | 2022-08-26 | [
[
"Pawlowski",
"Jan M.",
""
],
[
"Schneider",
"Coralie S.",
""
],
[
"Wink",
"Nicolas",
""
]
] | We investigate BRST invariance in Landau gauge Yang-Mills theory with functional methods. To that end, we solve the coupled system of functional renormalisation group equations for the momentum-dependent ghost and gluon propagator, ghost-gluon, and three- and four-gluon vertex dressings. The equations for both, transve... | 8.493915 | 9.001816 | 9.233955 | 8.180612 | 9.639384 | 8.768821 | 8.804059 | 9.21622 | 8.609855 | 9.297976 | 8.852986 | 8.156631 | 8.418869 | 8.551377 | 8.507104 | 8.42037 | 8.437638 | 8.703163 | 8.107509 | 8.374505 | 8.359457 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.