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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9707261 | Bernard de Wit | B. de Wit, K. Peeters and J.C. Plefka | The supermembrane with winding | Contribution to the proc. SUSY '97, Latex with espcrc2 style file | Nucl.Phys.Proc.Suppl. 62 (1998) 405-411 | 10.1016/S0920-5632(97)00681-6 | THU-97/20, NIKHEF 96-032 | hep-th | null | The supersymmetry algebra for supermembranes, quantized in the light-cone
gauge, exhibits central charges induced by wrapping the membrane around compact
dimensions. These central charges are manifestly consistent with Lorentz
symmetry. While the central charges raise the mass of the membrane states, they
still leave... | [
{
"created": "Thu, 31 Jul 1997 18:40:50 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"de Wit",
"B.",
""
],
[
"Peeters",
"K.",
""
],
[
"Plefka",
"J. C.",
""
]
] | The supersymmetry algebra for supermembranes, quantized in the light-cone gauge, exhibits central charges induced by wrapping the membrane around compact dimensions. These central charges are manifestly consistent with Lorentz symmetry. While the central charges raise the mass of the membrane states, they still leave t... | 9.476543 | 8.04353 | 9.659906 | 8.32889 | 8.666809 | 8.643708 | 8.110306 | 8.109566 | 8.54222 | 10.632929 | 8.703159 | 8.597582 | 9.336748 | 8.723363 | 8.46695 | 8.937979 | 8.394078 | 8.186267 | 8.722274 | 9.338749 | 8.249809 |
hep-th/9811041 | Antonio Gonzalez-Arroyo | A. Gonzalez-Arroyo | On Nahm's transformation with twisted boundary conditions | 18 pages | Nucl.Phys.B548:626-636,1999 | 10.1016/S0550-3213(99)00075-9 | FTUAM-98-20 and IFT-UAM/CSIC-98-25 | hep-th math-ph math.MP | null | Following two different tracks, we arrive at a definition of Nahm's
transformation valid for self-dual fields on the 4-dimensional torus with
non-zero twist tensor.The transform is again a self-dual gauge field defined on
a new torus and with non-zero twist tensor. It preserves the property of being
an involution.
| [
{
"created": "Wed, 4 Nov 1998 12:18:30 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gonzalez-Arroyo",
"A.",
""
]
] | Following two different tracks, we arrive at a definition of Nahm's transformation valid for self-dual fields on the 4-dimensional torus with non-zero twist tensor.The transform is again a self-dual gauge field defined on a new torus and with non-zero twist tensor. It preserves the property of being an involution. | 26.340136 | 20.495834 | 20.937695 | 18.251139 | 17.30109 | 21.869028 | 18.819838 | 20.886122 | 18.285965 | 26.401739 | 18.999887 | 19.207376 | 20.307512 | 19.284441 | 18.376501 | 19.035784 | 18.893349 | 18.903526 | 17.949471 | 19.596914 | 19.255405 |
2008.02713 | Shai Chester | Shai M. Chester, Michael B. Green, Silviu S. Pufu, Yifan Wang, and
Congkao Wen | New Modular Invariants in $\mathcal{N}=4$ Super-Yang-Mills Theory | 33 pages plus appendices, v2 accepted to JHEP | null | 10.1007/JHEP04(2021)212 | PUPT-2620, QMUL-PH-20-16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study modular invariants arising in the four-point functions of the stress
tensor multiplet operators of the ${\cal N} = 4$ $SU(N)$ super-Yang-Mills
theory, in the limit where $N$ is taken to be large while the complexified
Yang-Mills coupling $\tau$ is held fixed. The specific four-point functions we
consider are... | [
{
"created": "Thu, 6 Aug 2020 15:30:52 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Apr 2021 07:22:42 GMT",
"version": "v2"
}
] | 2021-05-12 | [
[
"Chester",
"Shai M.",
""
],
[
"Green",
"Michael B.",
""
],
[
"Pufu",
"Silviu S.",
""
],
[
"Wang",
"Yifan",
""
],
[
"Wen",
"Congkao",
""
]
] | We study modular invariants arising in the four-point functions of the stress tensor multiplet operators of the ${\cal N} = 4$ $SU(N)$ super-Yang-Mills theory, in the limit where $N$ is taken to be large while the complexified Yang-Mills coupling $\tau$ is held fixed. The specific four-point functions we consider are i... | 4.03868 | 3.859721 | 4.605515 | 3.912316 | 3.937113 | 4.074881 | 3.961724 | 3.896617 | 3.726563 | 5.206892 | 3.779712 | 3.917709 | 4.160535 | 3.913944 | 3.887437 | 3.959042 | 3.763721 | 3.89295 | 3.910733 | 4.2015 | 3.89046 |
1307.4740 | Anton van Niekerk | Alex Buchel, Robert C. Myers and Anton van Niekerk | Universality of Abrupt Holographic Quenches | 6 pages, 4 figures | Phys. Rev. Lett. 111, 201602 (2013) | 10.1103/PhysRevLett.111.201602 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We make an analytic investigation of rapid quenches of relevant operators in
d-dimensional holographic CFT's, which admit a dual gravity description. We
uncover a universal scaling behaviour in the response of the system, which
depends only on the conformal dimension of the quenched operator in the
vicinity of the ul... | [
{
"created": "Wed, 17 Jul 2013 19:34:27 GMT",
"version": "v1"
}
] | 2013-11-20 | [
[
"Buchel",
"Alex",
""
],
[
"Myers",
"Robert C.",
""
],
[
"van Niekerk",
"Anton",
""
]
] | We make an analytic investigation of rapid quenches of relevant operators in d-dimensional holographic CFT's, which admit a dual gravity description. We uncover a universal scaling behaviour in the response of the system, which depends only on the conformal dimension of the quenched operator in the vicinity of the ultr... | 8.968073 | 7.572796 | 8.445688 | 7.983052 | 7.963225 | 8.021853 | 8.068391 | 7.837574 | 7.783161 | 9.098665 | 7.478577 | 8.009558 | 8.470422 | 8.152785 | 7.979591 | 8.025148 | 7.877772 | 7.634229 | 8.382333 | 8.900532 | 7.91611 |
hep-th/0106177 | Mirjam Cvetic | Mirjam Cvetic (University of Pennsylvania and ITP, University of CA,
Santa Barbara), G. W. Gibbons (DAMTP, Cambridge University), H. Lu
(University of Michigan), C. N. Pope (Texas A&M University) | Resolved Branes and M-theory on Special Holonomy Spaces | 19 Pages Contribution to Strings 2001 | null | null | UPR-944-T,ITP-01-49,MCTP-01-29,CTP TAMU-23/01 | hep-th | null | We review the construction of regular p-brane solutions of M-theory and
string theory with less than maximal supersymmetry whose transverse spaces have
metrics with special holonomy, and where additional fluxes allow brane
resolutions via transgression terms. We focus on the properties of resolved
M2-branes and fract... | [
{
"created": "Tue, 19 Jun 2001 20:29:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Cvetic",
"Mirjam",
"",
"University of Pennsylvania and ITP, University of CA,\n Santa Barbara"
],
[
"Gibbons",
"G. W.",
"",
"DAMTP, Cambridge University"
],
[
"Lu",
"H.",
"",
"University of Michigan"
],
[
"Pope",
"C. N.",
"",
"Texas A&M... | We review the construction of regular p-brane solutions of M-theory and string theory with less than maximal supersymmetry whose transverse spaces have metrics with special holonomy, and where additional fluxes allow brane resolutions via transgression terms. We focus on the properties of resolved M2-branes and fractio... | 9.893262 | 6.431059 | 10.760174 | 7.326486 | 6.873303 | 6.814319 | 7.727765 | 7.102356 | 7.2523 | 11.268328 | 7.617525 | 8.813703 | 9.654495 | 8.542267 | 8.69359 | 8.839634 | 8.5764 | 8.430833 | 8.6726 | 9.687094 | 8.731758 |
hep-th/9907155 | Hwang-hyun Kwon | Michael B. Green, Michael Gutperle and Hwang-h. Kwon | Light-cone Quantum Mechanics of the Eleven-dimensional Superparticle | 31 pages, harvmac (b); A minor TeX error corrected | JHEP 9908:012,1999 | 10.1088/1126-6708/1999/08/012 | DAMTP-1999-92, PUPT-1880 | hep-th | null | The linearized interactions of eleven-dimensional supergravity are obtained
in a manifestly supersymmetric light-cone gauge formalism. These vertices are
used to calculate certain one-loop processes involving external gravitini,
antisymmetric three-form potentials and gravitons, thereby determining some
protected ter... | [
{
"created": "Mon, 19 Jul 1999 11:39:06 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Jul 1999 17:14:29 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Green",
"Michael B.",
""
],
[
"Gutperle",
"Michael",
""
],
[
"Kwon",
"Hwang-h.",
""
]
] | The linearized interactions of eleven-dimensional supergravity are obtained in a manifestly supersymmetric light-cone gauge formalism. These vertices are used to calculate certain one-loop processes involving external gravitini, antisymmetric three-form potentials and gravitons, thereby determining some protected terms... | 11.084758 | 7.818727 | 11.336621 | 7.624663 | 7.993198 | 8.20218 | 8.038242 | 8.356526 | 7.325613 | 9.684484 | 8.174323 | 8.499204 | 10.036407 | 8.376683 | 8.486909 | 8.548367 | 8.3125 | 8.494203 | 8.331949 | 9.923024 | 8.823465 |
1301.2874 | Davoud Kamani | Davoud Kamani | Some $\mathbf{Z}_2$-invariant Variables: Constructed of the Scalars
Dilaton and Axion | 11 pages, Latex, No figure. In the revised version some
interpretations have been improved | Eur. Phys. J. C (2014) 74:2846 | 10.1140/epjc/s10052-014-2846-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the dilaton scalar and axion pseudoscalar fields we construct a number
of scalars and differential forms which are symmetric under the
$\mathbf{Z}_2$-subgroup of the group $SL(2, \mathbf{R})$. These invariants
enable us to establish various 10-dimensional invariant actions. Other
invariants which are not indepe... | [
{
"created": "Mon, 14 Jan 2013 07:32:19 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Mar 2013 11:38:49 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Nov 2013 15:59:09 GMT",
"version": "v3"
}
] | 2014-04-28 | [
[
"Kamani",
"Davoud",
""
]
] | Using the dilaton scalar and axion pseudoscalar fields we construct a number of scalars and differential forms which are symmetric under the $\mathbf{Z}_2$-subgroup of the group $SL(2, \mathbf{R})$. These invariants enable us to establish various 10-dimensional invariant actions. Other invariants which are not independ... | 13.972728 | 12.661143 | 13.786461 | 12.888319 | 13.430571 | 14.362805 | 12.784736 | 12.976703 | 12.46678 | 14.017646 | 11.932978 | 12.27916 | 12.649961 | 12.357924 | 12.734949 | 12.627064 | 12.623001 | 12.41002 | 12.237537 | 12.313608 | 12.18643 |
hep-th/9807062 | Takahiro Masuda | T.Masuda and H.Suzuki (Hokkaido Univ.) | Prepotentials, Bi-linear Forms on Periods and Enhanced Gauge Symmetries
in Type-II Strings | Latex file(34pp), a reference added, typos corrected | Int.J.Mod.Phys.A14:1177-1204,1999 | 10.1142/S0217751X99000610 | EPHOU 98-009 | hep-th | null | We construct a bi-linear form on the periods of Calabi-Yau spaces. These are
used to obtain the prepotentials around conifold singularities in type-II
strings compactified on Calabi-Yau space. The explicit construction of the
bi-linear forms is achieved for the one-moduli models as well as two moduli
models with K3-f... | [
{
"created": "Thu, 9 Jul 1998 18:48:55 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Sep 1998 05:15:18 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Sep 1998 00:28:36 GMT",
"version": "v3"
},
{
"created": "Tue, 6 Oct 1998 05:25:05 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Masuda",
"T.",
"",
"Hokkaido Univ."
],
[
"Suzuki",
"H.",
"",
"Hokkaido Univ."
]
] | We construct a bi-linear form on the periods of Calabi-Yau spaces. These are used to obtain the prepotentials around conifold singularities in type-II strings compactified on Calabi-Yau space. The explicit construction of the bi-linear forms is achieved for the one-moduli models as well as two moduli models with K3-fib... | 11.047257 | 10.642273 | 12.256154 | 10.004412 | 10.90933 | 10.528857 | 9.540634 | 10.492458 | 10.760727 | 14.338536 | 9.848113 | 10.295015 | 10.864406 | 10.206558 | 10.143687 | 10.171845 | 10.266275 | 10.088959 | 10.242222 | 10.81958 | 9.958722 |
1208.5979 | Eoin \'O Colg\'ain | Eoin \'O Colg\'ain | Beyond LLM in M-theory | 1+30 pages, footnote added | JHEP 1212 (2012) 023 | 10.1007/JHEP12(2012)023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Lin, Lunin, Maldacena (LLM) ansatz in D = 11 supports two independent
Killing directions when a general Killing spinor ansatz is considered. Here we
show that these directions always commute, identify when the Killing spinors
are charged, and show that both their inner product and resulting geometry are
governed ... | [
{
"created": "Wed, 29 Aug 2012 18:20:53 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Dec 2012 13:41:13 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Feb 2013 14:03:07 GMT",
"version": "v3"
}
] | 2013-02-11 | [
[
"Colgáin",
"Eoin Ó",
""
]
] | The Lin, Lunin, Maldacena (LLM) ansatz in D = 11 supports two independent Killing directions when a general Killing spinor ansatz is considered. Here we show that these directions always commute, identify when the Killing spinors are charged, and show that both their inner product and resulting geometry are governed by... | 11.95698 | 10.761889 | 13.972648 | 11.247928 | 10.739203 | 10.797314 | 11.249091 | 10.816299 | 11.47264 | 15.488707 | 10.472455 | 10.955452 | 11.576208 | 11.642549 | 10.861585 | 11.298432 | 11.341186 | 11.239326 | 11.24784 | 11.668624 | 11.083294 |
1206.4309 | Yi Wang | Yi Wang, Robert Brandenberger | Scale-Invariant Fluctuations from Galilean Genesis | 11 pages, 3 figures | null | 10.1088/1475-7516/2012/10/021 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the spectrum of cosmological fluctuations in scenarios such as
Galilean Genesis in which a spectator scalar field acquires a scale-invariant
spectrum of perturbations during an early phase which asymptotes in the far
past to Minkowski space-time. In the case of minimal coupling to gravity and
standard scalar... | [
{
"created": "Tue, 19 Jun 2012 20:00:00 GMT",
"version": "v1"
}
] | 2015-06-05 | [
[
"Wang",
"Yi",
""
],
[
"Brandenberger",
"Robert",
""
]
] | We study the spectrum of cosmological fluctuations in scenarios such as Galilean Genesis in which a spectator scalar field acquires a scale-invariant spectrum of perturbations during an early phase which asymptotes in the far past to Minkowski space-time. In the case of minimal coupling to gravity and standard scalar f... | 8.886783 | 9.581766 | 9.723885 | 8.295887 | 8.927183 | 8.275393 | 8.1172 | 8.192074 | 8.255527 | 10.212931 | 7.724164 | 8.455956 | 8.321247 | 8.186365 | 8.412866 | 8.398663 | 8.168934 | 8.342305 | 8.622118 | 8.949541 | 8.328491 |
hep-th/9810182 | Yoichiro Nambu | Yoichiro Nambu | The Aharonov-Bohm Problem Revisited | 30 pages, LaTeX, 4 figures | Nucl.Phys. B579 (2000) 590-616 | 10.1016/S0550-3213(00)00258-3 | EFI-98-32 | hep-th | null | The properties of a nonrelativistic charged particle in two dimensions in the
presence of an arbitrary number of nonquantized magnetic fluxes are
investigated in free space as well as in a uniform magnetic field. The fluxes
are represented mathematically as branch points in one of the complex
coordinates. It is found... | [
{
"created": "Thu, 22 Oct 1998 17:16:18 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Jun 1999 16:16:23 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Nambu",
"Yoichiro",
""
]
] | The properties of a nonrelativistic charged particle in two dimensions in the presence of an arbitrary number of nonquantized magnetic fluxes are investigated in free space as well as in a uniform magnetic field. The fluxes are represented mathematically as branch points in one of the complex coordinates. It is found t... | 9.548525 | 9.723978 | 9.632175 | 9.877617 | 9.771791 | 10.019771 | 9.559097 | 8.825665 | 8.820864 | 10.355196 | 9.021836 | 9.229754 | 9.806651 | 9.430307 | 9.059345 | 9.1713 | 9.37762 | 9.206278 | 9.388954 | 9.893733 | 9.459476 |
hep-th/0006237 | Manoelito M. de Souza | Manoelito M de Souza | Conformally symmetric massive discrete fields | A new reference, a new figure and a new section are added to clarify
the meaning of conformal (and chiral) symmetry of massive discrete-fields | null | null | null | hep-th gr-qc hep-ph math-ph math.MP quant-ph | null | Conformal symmetry is taken as an attribute of theories of massless fields in
manifolds with specific dimensionalities. This paper shows that this is not an
absolute truth; it is a consequence of the mathematical representation used for
the physical interactions. It introduces a new kind of representation where the
p... | [
{
"created": "Thu, 29 Jun 2000 20:32:17 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Nov 2000 19:07:29 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Mar 2001 22:39:27 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"de Souza",
"Manoelito M",
""
]
] | Conformal symmetry is taken as an attribute of theories of massless fields in manifolds with specific dimensionalities. This paper shows that this is not an absolute truth; it is a consequence of the mathematical representation used for the physical interactions. It introduces a new kind of representation where the pro... | 18.578709 | 18.968565 | 20.235546 | 19.00057 | 19.94739 | 22.021469 | 20.776485 | 18.446344 | 19.365263 | 22.283995 | 18.768433 | 17.846575 | 18.212812 | 18.297031 | 18.724966 | 18.18539 | 17.770288 | 17.414686 | 18.045588 | 18.424206 | 18.264782 |
hep-th/0604084 | Jean Thierry-Mieg | Jean Thierry-Mieg | Chiral-Yang-Mills theory, non commutative differential geometry, and the
need for a Lie super-algebra | 17 pages, no figure | JHEP0606:038,2006 | 10.1088/1126-6708/2006/06/038 | null | hep-th | null | In Yang-Mills theory, the charges of the left and right massless Fermions are
independent of each other. We propose a new paradigm where we remove this
freedom and densify the algebraic structure of Yang-Mills theory by integrating
the scalar Higgs field into a new gauge-chiral 1-form which connects Fermions
of oppos... | [
{
"created": "Tue, 11 Apr 2006 16:35:07 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Apr 2006 21:33:04 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Thierry-Mieg",
"Jean",
""
]
] | In Yang-Mills theory, the charges of the left and right massless Fermions are independent of each other. We propose a new paradigm where we remove this freedom and densify the algebraic structure of Yang-Mills theory by integrating the scalar Higgs field into a new gauge-chiral 1-form which connects Fermions of opposit... | 13.110109 | 13.404403 | 14.642234 | 13.012431 | 13.283667 | 13.563128 | 12.797089 | 13.089374 | 13.75794 | 14.841985 | 13.662649 | 12.956133 | 13.122464 | 12.59482 | 12.628891 | 12.575695 | 12.919034 | 12.755257 | 12.875908 | 12.64067 | 13.094234 |
1708.05730 | Patricio Gaete | Patricio Gaete and Jos\'e A. Helay\"el-Neto | Remarks on a $B \wedge F$ model with topological mass from gauging spin | 5 pages | null | 10.1209/0295-5075/120/11001 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Aspects of screening and confinement are reassessed for a $B \wedge F$ model
with topological mass with the gauging of spin. Our discussion is carried out
using the gauge-invariant, but path-dependent, variables formalism. We
explicitly show that the static potential profile is the sum of a Yukawa and a
linear potent... | [
{
"created": "Fri, 18 Aug 2017 18:17:59 GMT",
"version": "v1"
}
] | 2018-01-17 | [
[
"Gaete",
"Patricio",
""
],
[
"Helayël-Neto",
"José A.",
""
]
] | Aspects of screening and confinement are reassessed for a $B \wedge F$ model with topological mass with the gauging of spin. Our discussion is carried out using the gauge-invariant, but path-dependent, variables formalism. We explicitly show that the static potential profile is the sum of a Yukawa and a linear potentia... | 15.241445 | 7.726597 | 15.144058 | 9.501751 | 8.676027 | 8.579629 | 8.295018 | 8.415743 | 9.36535 | 13.452538 | 9.115911 | 10.611448 | 13.620936 | 11.750078 | 11.021351 | 10.6888 | 10.662228 | 11.217429 | 11.287254 | 13.094286 | 11.413342 |
1108.2569 | Frederik Scholtz | Debabrata Sinha, Biswajit Chakraborty and Frederik G Scholtz | Non-commutative Quantum Mechanics in Three Dimensions and Rotational
Symmetry | 21 pages | null | 10.1088/1751-8113/45/10/105308 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the formulation of non-commutative quantum mechanics to three
dimensional non-commutative space. Particular attention is paid to the
identification of the quantum Hilbert space in which the physical states of the
system are to be represented, the construction of the representation of the
rotation group ... | [
{
"created": "Fri, 12 Aug 2011 05:54:02 GMT",
"version": "v1"
}
] | 2015-05-30 | [
[
"Sinha",
"Debabrata",
""
],
[
"Chakraborty",
"Biswajit",
""
],
[
"Scholtz",
"Frederik G",
""
]
] | We generalize the formulation of non-commutative quantum mechanics to three dimensional non-commutative space. Particular attention is paid to the identification of the quantum Hilbert space in which the physical states of the system are to be represented, the construction of the representation of the rotation group on... | 10.234382 | 9.254272 | 10.070085 | 9.424394 | 9.846938 | 9.357142 | 8.861176 | 9.291883 | 8.88612 | 10.49943 | 9.153989 | 9.177398 | 10.015516 | 9.462161 | 9.834537 | 9.064943 | 9.017675 | 9.07211 | 9.461449 | 9.719945 | 9.156261 |
2112.08683 | Yuan Zhong | Yuan Zhong | Normal modes for two-dimensional gravitating kinks | 7 pages, no figures, a Mathematica file 2dNormalModes.nb is attached | Physics Letters B 827 (2022) 136947 | 10.1016/j.physletb.2022.136947 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study small perturbations around an arbitrary static kink solution of a
two-dimensional (2D) gravity-scalar system, where the gravity part is described
by a subclass of 2D dilaton gravity theory, and the scalar matter field has
generalized dynamics. We expand the action around an arbitrary static solution
and keep... | [
{
"created": "Thu, 16 Dec 2021 08:04:16 GMT",
"version": "v1"
}
] | 2022-02-09 | [
[
"Zhong",
"Yuan",
""
]
] | We study small perturbations around an arbitrary static kink solution of a two-dimensional (2D) gravity-scalar system, where the gravity part is described by a subclass of 2D dilaton gravity theory, and the scalar matter field has generalized dynamics. We expand the action around an arbitrary static solution and keep t... | 9.699121 | 9.219826 | 9.161583 | 8.439854 | 9.067719 | 8.24307 | 9.220708 | 9.053845 | 8.381807 | 10.383649 | 9.023193 | 9.594328 | 9.058826 | 8.972194 | 9.04666 | 8.793886 | 9.101944 | 8.99342 | 9.182398 | 9.330801 | 9.163897 |
2011.13725 | Thibaut Coudarchet | Thibaut Coudarchet and Herv\'e Partouche | One-loop masses of Neumann-Dirichlet open strings and boundary-changing
vertex operators | 1+74 pages, 5 figures | null | 10.1007/JHEP12(2021)022 | CPHT-RR090.112020 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the masses acquired at one loop by massless scalars in the
Neumann-Dirichlet sector of open strings, when supersymmetry is spontaneously
broken. It is done by computing two-point functions of "boundary-changing
vertex operators" inserted on the boundaries of the annulus and M\"obius strip.
This requires the... | [
{
"created": "Fri, 27 Nov 2020 13:16:57 GMT",
"version": "v1"
}
] | 2022-01-05 | [
[
"Coudarchet",
"Thibaut",
""
],
[
"Partouche",
"Hervé",
""
]
] | We derive the masses acquired at one loop by massless scalars in the Neumann-Dirichlet sector of open strings, when supersymmetry is spontaneously broken. It is done by computing two-point functions of "boundary-changing vertex operators" inserted on the boundaries of the annulus and M\"obius strip. This requires the e... | 8.771751 | 8.591932 | 9.85183 | 8.228762 | 8.562016 | 8.427199 | 8.192521 | 8.160821 | 8.521249 | 10.576658 | 8.343433 | 8.338692 | 8.911209 | 8.422469 | 8.14375 | 8.553017 | 8.323903 | 8.392054 | 8.587337 | 8.638882 | 8.588327 |
hep-th/0205160 | Zarembo | K. Zarembo | Supersymmetric Wilson loops | 16 pages; v2: misprints corrected; v3: comments on superconformal
invariance and a reference added, version to be published in Nucl. Phys. B;
v4: discussion of N=2 supersymmetric Wilson loops corrected | Nucl.Phys. B643 (2002) 157-171 | 10.1016/S0550-3213(02)00693-4 | null | hep-th | null | I construct 1/16, 1/8 and 1/4 BPS Wilson loops in N=4 supersymmetric
Yang-Mills theory and argue that expectation values of 1/4 BPS loops do not
receive quantum corrections. At strong coupling, non-renormalization of
supersymmetric Wilson loops implies subtle cancellations in the partition
function of the AdS string ... | [
{
"created": "Wed, 15 May 2002 19:54:18 GMT",
"version": "v1"
},
{
"created": "Mon, 27 May 2002 15:25:53 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Aug 2002 14:55:01 GMT",
"version": "v3"
},
{
"created": "Tue, 27 Aug 2002 12:58:36 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Zarembo",
"K.",
""
]
] | I construct 1/16, 1/8 and 1/4 BPS Wilson loops in N=4 supersymmetric Yang-Mills theory and argue that expectation values of 1/4 BPS loops do not receive quantum corrections. At strong coupling, non-renormalization of supersymmetric Wilson loops implies subtle cancellations in the partition function of the AdS string wi... | 7.759377 | 6.284036 | 7.55253 | 5.595199 | 6.08479 | 5.822676 | 6.173971 | 5.859671 | 5.744777 | 7.787769 | 5.796988 | 5.652029 | 6.672262 | 5.857291 | 5.972867 | 5.933929 | 5.815783 | 5.9493 | 5.981025 | 6.390387 | 5.800883 |
hep-th/9312050 | Niels Obers | M.B. Halpern and N.A. Obers | Flat Connections and Non-Local Conserved Quantities in Irrational
Conformal Field Theory | 40 pages, Latex, UCB-PTH-93/33, LBL-34901, CPTH-A277.1293 | J.Math.Phys. 36 (1995) 1080-1110 | 10.1063/1.531107 | null | hep-th | null | Irrational conformal field theory (ICFT) includes rational conformal field
theory as a small subspace, and the affine-Virasoro Ward identities describe
the biconformal correlators of ICFT. We reformulate the Ward identities as an
equivalent linear partial differential system with flat connections and new
non-local co... | [
{
"created": "Tue, 7 Dec 1993 11:19:32 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Halpern",
"M. B.",
""
],
[
"Obers",
"N. A.",
""
]
] | Irrational conformal field theory (ICFT) includes rational conformal field theory as a small subspace, and the affine-Virasoro Ward identities describe the biconformal correlators of ICFT. We reformulate the Ward identities as an equivalent linear partial differential system with flat connections and new non-local cons... | 12.831252 | 11.006937 | 14.21734 | 10.846384 | 12.193453 | 11.295968 | 10.974758 | 11.21968 | 10.80535 | 16.796375 | 11.608171 | 11.616954 | 12.90628 | 11.509909 | 11.511201 | 11.652793 | 11.699477 | 10.854911 | 11.755595 | 13.288403 | 12.116526 |
2204.01982 | Yermek Aldabergenov | Yermek Aldabergenov | Gauging the R-symmetry of old-minimal $R+R^2$ supergravity | 8 pages, 1 figure (revtex 4-2). V2: corrections to numerical values
of the fermion masses | Phys.Rev.D 105 (2022) 12, 124008 | 10.1103/PhysRevD.105.124008 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Old-minimal $R+R^2$ supergravity has a $U(1)$ R-symmetry which rotates the
chiral curvature superfield. We gauge this R-symmetry and study new
interactions involving the gauge multiplet in the context of inflation and
supersymmetry breaking. We construct models where supersymmetry and the
R-symmetry are spontaneously... | [
{
"created": "Tue, 5 Apr 2022 04:37:31 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Apr 2022 11:45:12 GMT",
"version": "v2"
}
] | 2022-06-08 | [
[
"Aldabergenov",
"Yermek",
""
]
] | Old-minimal $R+R^2$ supergravity has a $U(1)$ R-symmetry which rotates the chiral curvature superfield. We gauge this R-symmetry and study new interactions involving the gauge multiplet in the context of inflation and supersymmetry breaking. We construct models where supersymmetry and the R-symmetry are spontaneously b... | 8.332633 | 7.547297 | 8.105564 | 7.043979 | 6.975847 | 7.115483 | 7.10422 | 6.980875 | 6.973217 | 8.432861 | 6.80418 | 7.094691 | 7.228583 | 6.949824 | 6.947927 | 6.953696 | 7.026483 | 7.234166 | 6.884148 | 7.205056 | 6.872314 |
2208.13309 | Carlos Henrique de Lima | Carlos Henrique de Lima, Alberto Tonero, Andres Vasquez and Rogerio
Rosenfeld | P-wave Sommerfeld enhancement near threshold: a simplified approach | references added. Title change, discussions improved, conclusions
unchanged. Version accepted at Euro Phys C | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | The calculation of P-wave Sommerfeld enhancement in processes with unstable
particles in the final state is known to be divergent. In a complete
description, where resonant (on-shell unstable particles) and non-resonant
contributions are included, it has been shown that results are finite. For most
beyond the Standar... | [
{
"created": "Sun, 28 Aug 2022 23:07:12 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Sep 2022 16:55:27 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Apr 2023 14:44:18 GMT",
"version": "v3"
},
{
"created": "Wed, 4 Oct 2023 16:59:56 GMT",
"version": "v4"
}
] | 2023-10-05 | [
[
"de Lima",
"Carlos Henrique",
""
],
[
"Tonero",
"Alberto",
""
],
[
"Vasquez",
"Andres",
""
],
[
"Rosenfeld",
"Rogerio",
""
]
] | The calculation of P-wave Sommerfeld enhancement in processes with unstable particles in the final state is known to be divergent. In a complete description, where resonant (on-shell unstable particles) and non-resonant contributions are included, it has been shown that results are finite. For most beyond the Standard ... | 9.658395 | 9.838765 | 8.670597 | 8.524094 | 9.606379 | 10.575804 | 9.24168 | 9.748752 | 8.506015 | 9.088395 | 9.482116 | 9.148733 | 8.527342 | 8.499598 | 8.45342 | 8.851003 | 8.558282 | 8.861233 | 8.517692 | 8.526072 | 8.911643 |
hep-th/0608151 | Christopher Herzog | Christopher P. Herzog | A Holographic Prediction of the Deconfinement Temperature | 4 pages, 1 figure; v2 ref added, minor changes; v3 refs added,
discussion modified, to appear in PRL | Phys.Rev.Lett.98:091601,2007 | 10.1103/PhysRevLett.98.091601 | null | hep-th hep-ph | null | We argue that deconfinement in AdS/QCD models occurs via a first order
Hawking-Page type phase transition between a low temperature thermal AdS space
and a high temperature black hole. Such a result is consistent with the
expected temperature independence, to leading order in 1/N_c, of the meson
spectrum and spatial ... | [
{
"created": "Tue, 22 Aug 2006 17:23:21 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Aug 2006 20:29:18 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Jan 2007 21:20:08 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Herzog",
"Christopher P.",
""
]
] | We argue that deconfinement in AdS/QCD models occurs via a first order Hawking-Page type phase transition between a low temperature thermal AdS space and a high temperature black hole. Such a result is consistent with the expected temperature independence, to leading order in 1/N_c, of the meson spectrum and spatial Wi... | 6.28719 | 5.329062 | 5.74167 | 5.091604 | 5.563319 | 5.14994 | 5.24407 | 5.332905 | 5.338092 | 5.482166 | 5.06984 | 5.551423 | 5.419094 | 5.512917 | 5.351339 | 5.534741 | 5.390566 | 5.424941 | 5.652456 | 5.864752 | 5.442312 |
0801.0962 | Gabor Takacs | G. Takacs | Form factors of boundary exponential operators in the sinh-Gordon model | 22 pages, LaTeX2e file | null | 10.1016/j.nuclphysb.2008.01.025 | ITP-Budapest Report No. 637 | hep-th cond-mat.other | null | Using the recently introduced boundary form factor bootstrap equations, the
form factors of boundary exponential operators in the sinh-Gordon model are
constructed. The ultraviolet scaling dimension and the normalization of these
operators are checked against previously known results. The construction
presented in th... | [
{
"created": "Mon, 7 Jan 2008 12:53:08 GMT",
"version": "v1"
}
] | 2009-11-13 | [
[
"Takacs",
"G.",
""
]
] | Using the recently introduced boundary form factor bootstrap equations, the form factors of boundary exponential operators in the sinh-Gordon model are constructed. The ultraviolet scaling dimension and the normalization of these operators are checked against previously known results. The construction presented in this... | 10.523479 | 6.463636 | 12.6894 | 7.637575 | 7.170409 | 6.717443 | 6.512172 | 7.15423 | 6.864463 | 10.79694 | 8.182273 | 8.080609 | 10.306919 | 8.333983 | 8.271283 | 8.052567 | 8.192024 | 8.207417 | 8.060682 | 11.133991 | 7.968842 |
hep-th/9708036 | Michael P. Mattis | N. Dorey (Swansea), V.V. Khoze (Durham), M.P. Mattis (Los Alamos) | Supersymmetry and the Multi-Instanton Measure | 31 pp, uses harvmac. Reference added | Nucl.Phys. B513 (1998) 681-708 | 10.1016/S0550-3213(97)00747-5 | null | hep-th | null | We propose explicit formulae for the integration measure on the moduli space
of charge-n ADHM multi-instantons in N=1 and N=2 supersymmetric gauge theories.
The form of this measure is fixed by its (super)symmetries as well as the
physical requirement of clustering in the limit of large spacetime separation
between i... | [
{
"created": "Wed, 6 Aug 1997 20:44:11 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Aug 1997 20:32:37 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Dorey",
"N.",
"",
"Swansea"
],
[
"Khoze",
"V. V.",
"",
"Durham"
],
[
"Mattis",
"M. P.",
"",
"Los Alamos"
]
] | We propose explicit formulae for the integration measure on the moduli space of charge-n ADHM multi-instantons in N=1 and N=2 supersymmetric gauge theories. The form of this measure is fixed by its (super)symmetries as well as the physical requirement of clustering in the limit of large spacetime separation between ins... | 8.943018 | 8.793153 | 9.791521 | 8.688298 | 9.700822 | 8.977455 | 8.880157 | 8.791993 | 8.914754 | 10.298264 | 8.906101 | 8.439729 | 9.244633 | 8.573402 | 8.635791 | 8.347919 | 8.461802 | 8.397628 | 8.394255 | 8.900977 | 8.469779 |
hep-th/9409093 | Montpetit Andre | Alexei Morozov and Luc Vinet | Free-Field Representation of Group Element for Simple Quantum Group | 68 pages | Int.J.Mod.Phys. A13 (1998) 1651-1708 | 10.1142/S0217751X9800072X | ITEP-M3/94 and CRM-2202 | hep-th | null | A representation of the group element (also known as ``universal ${\cal
T}$-matrix'') which satisfies $\Delta(g) = g\otimes g$, is given in the form $$
g = \left(\prod_{s=1}^{d_B}\phantom.^>\ {\cal
E}_{1/q_{i(s)}}(\chi^{(s)}T_{-i(s)})\right) q^{2\vec\phi\vec H}
\left(\prod_{s=1}^{d_B}\phantom.^<\ {\cal E}_{q_{i(s)}}(... | [
{
"created": "Fri, 16 Sep 1994 13:02:30 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Morozov",
"Alexei",
""
],
[
"Vinet",
"Luc",
""
]
] | A representation of the group element (also known as ``universal ${\cal T}$-matrix'') which satisfies $\Delta(g) = g\otimes g$, is given in the form $$ g = \left(\prod_{s=1}^{d_B}\phantom.^>\ {\cal E}_{1/q_{i(s)}}(\chi^{(s)}T_{-i(s)})\right) q^{2\vec\phi\vec H} \left(\prod_{s=1}^{d_B}\phantom.^<\ {\cal E}_{q_{i(s)}}(\p... | 3.752758 | 4.268524 | 4.287592 | 4.012689 | 4.200712 | 4.218846 | 4.276495 | 3.970879 | 4.128149 | 4.573705 | 3.825011 | 3.752785 | 3.847309 | 3.749138 | 3.793183 | 3.720748 | 3.846562 | 3.84347 | 3.784154 | 3.933715 | 3.693439 |
2210.14137 | V. Parameswaran Nair | V.P. Nair | Eductions of Edge Mode Effects | 11 pages, To be published in "Particles, Fields and Topology:
Celebrating A.P. Balachandran", a Festschrift volume for A.P. Balachandran | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Edge modes in gauge theories, whose raison d'etre is in the nature of the
test functions used for imposing the Gauss law, have implications in many
physical contexts. I discuss two such cases: 1) how edge modes are related to
the interface term in the BFK formula and how they generate the so-called
contact term for e... | [
{
"created": "Tue, 25 Oct 2022 16:36:56 GMT",
"version": "v1"
}
] | 2022-10-26 | [
[
"Nair",
"V. P.",
""
]
] | Edge modes in gauge theories, whose raison d'etre is in the nature of the test functions used for imposing the Gauss law, have implications in many physical contexts. I discuss two such cases: 1) how edge modes are related to the interface term in the BFK formula and how they generate the so-called contact term for ent... | 15.118346 | 15.570543 | 14.573249 | 13.412299 | 14.770356 | 14.766214 | 15.343913 | 14.764758 | 15.093939 | 17.141541 | 14.050641 | 13.722338 | 13.456234 | 13.373084 | 13.432366 | 14.091687 | 13.32664 | 13.17825 | 13.654488 | 13.861109 | 14.96781 |
hep-th/9606060 | null | HoSeong La | Effective Dilaton Potential in Linearized Gravity | Latex, 11 pages | null | null | MIT-CTP-2540 | hep-th gr-qc | null | Considering the linearized gravity with matter fields, the effective
potential of the ``conformal dilaton'' in the string frame is generated
semiclassically by one-loop contribution of heavy matter fields. This in turn
generates a nontrivial potential for the physical dilaton in the Einstein frame
with the trace of t... | [
{
"created": "Wed, 12 Jun 1996 01:56:06 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"La",
"HoSeong",
""
]
] | Considering the linearized gravity with matter fields, the effective potential of the ``conformal dilaton'' in the string frame is generated semiclassically by one-loop contribution of heavy matter fields. This in turn generates a nontrivial potential for the physical dilaton in the Einstein frame with the trace of the... | 13.641905 | 12.415548 | 12.280204 | 11.570784 | 13.845153 | 12.210104 | 13.122091 | 12.501782 | 11.700108 | 12.751086 | 11.277038 | 12.145943 | 12.57377 | 11.944662 | 12.295928 | 12.045694 | 12.130689 | 12.106208 | 12.363391 | 12.458799 | 11.799411 |
2209.00095 | Sachin Chauhan | Sachin Chauhan, Pichai Ramadevi | $\hat Z$- invariant for $SO(3)$ and $OSp(1|2)$ Groups | 18 pages, 2 figures; minor changes; matches the published version | Annales Henri Poincar\'e, 1-25(2023) | 10.1007/s00023-023-01332-y | null | hep-th math-ph math.GT math.MP math.QA | http://creativecommons.org/licenses/by/4.0/ | Three-manifold invariants $\hat Z$ (''$Z$-hat''), also known as homological
blocks, are $q$-series with integer coefficients. Explicit $q$-series form for
$\hat Z$ is known for $SU(2)$ group, supergroup $SU(2|1)$ and ortho-symplectic
supergroup $OSp(2|2)$. We focus on $\hat Z$ for $SO(3)$ group and
orthosymplectic su... | [
{
"created": "Wed, 31 Aug 2022 20:03:27 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jun 2023 05:49:50 GMT",
"version": "v2"
}
] | 2023-06-13 | [
[
"Chauhan",
"Sachin",
""
],
[
"Ramadevi",
"Pichai",
""
]
] | Three-manifold invariants $\hat Z$ (''$Z$-hat''), also known as homological blocks, are $q$-series with integer coefficients. Explicit $q$-series form for $\hat Z$ is known for $SU(2)$ group, supergroup $SU(2|1)$ and ortho-symplectic supergroup $OSp(2|2)$. We focus on $\hat Z$ for $SO(3)$ group and orthosymplectic supe... | 6.131422 | 5.220747 | 6.986 | 5.446741 | 5.677092 | 5.668591 | 5.225109 | 5.502266 | 5.240651 | 6.942182 | 5.286683 | 5.045546 | 6.077028 | 5.431227 | 5.493846 | 5.240073 | 5.472915 | 5.404943 | 5.212944 | 6.102811 | 5.264583 |
hep-th/9501031 | Troyan Sergei | G. S. Danilov | The calculation of Feynman diagrams in the superstring perturbation
theory | 48 pages, LATEX | Phys.Rev.D51:4359,1995; Erratum-ibid.D52:6201,1995;
Phys.Rev.D52:6201,1995 | 10.1103/PhysRevD.51.4359 10.1103/PhysRevD.52.6201 | Preprint PNPI-2023, 1994 | hep-th | null | The method of the calculation of the multi-loop superstring amplitudes is
proposed. The amplitudes are calculated from the equations that are none other
than Ward identities. They are derived from the requirement that the discussed
amplitudes are independent from a choice of gauge of both the vierbein and the
graviti... | [
{
"created": "Tue, 10 Jan 1995 15:15:08 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Danilov",
"G. S.",
""
]
] | The method of the calculation of the multi-loop superstring amplitudes is proposed. The amplitudes are calculated from the equations that are none other than Ward identities. They are derived from the requirement that the discussed amplitudes are independent from a choice of gauge of both the vierbein and the gravitino... | 8.85446 | 9.580017 | 10.242829 | 9.118407 | 9.958276 | 10.328708 | 9.974879 | 9.4809 | 9.313786 | 10.903646 | 9.34037 | 8.810369 | 9.112656 | 8.755531 | 8.838283 | 8.911041 | 8.907673 | 8.956974 | 8.891483 | 9.123462 | 8.749809 |
2007.15017 | Yi Pang | Hai-Shan Liu, H. Lu and Yi Pang | Revisiting the AdS Boson Stars: the Mass-Charge Relations | Latex, 58 pages, 26 figures. Published version | Phys. Rev. D 102, 126008 (2020) | 10.1103/PhysRevD.102.126008 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the recent progress in solving the large charge sector of
conformal field theories, we revisit the mass-charge relation of boson stars
asymptotic to global AdS. We construct and classify a large number of
electrically charged boson star solutions in a toy model and two supergravity
models arising from th... | [
{
"created": "Wed, 29 Jul 2020 18:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Aug 2020 11:52:01 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Dec 2020 01:15:31 GMT",
"version": "v3"
}
] | 2020-12-09 | [
[
"Liu",
"Hai-Shan",
""
],
[
"Lu",
"H.",
""
],
[
"Pang",
"Yi",
""
]
] | Motivated by the recent progress in solving the large charge sector of conformal field theories, we revisit the mass-charge relation of boson stars asymptotic to global AdS. We construct and classify a large number of electrically charged boson star solutions in a toy model and two supergravity models arising from the ... | 5.882543 | 5.933455 | 6.270079 | 5.725612 | 6.123674 | 6.017959 | 5.794985 | 5.593693 | 5.686611 | 6.979734 | 5.44382 | 5.641509 | 5.916368 | 5.60298 | 5.667686 | 5.605653 | 5.65706 | 5.619218 | 5.655387 | 6.012464 | 5.682505 |
2111.07998 | Paul-Konstantin Oehlmann | Finn Bjarne Kohl, Magdalena Larfors, Paul-Konstantin Oehlmann | F-theory on 6D Symmetric Toroidal Orbifolds | 39 pages plus appendix, 15 Figures, 2 Tables, V2 typos corrected | null | null | UUITP-56/21 | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this work we study F-theory on symmetric toroidal orbifolds that exhibit
roto-translations, which are point group rotations accompanied by fractional
lattice shifts. These geometries admit a rich class of effects, such as twisted
affine folded fibers, multiple fibers, and up to three distinct
torus-fibrations that... | [
{
"created": "Mon, 15 Nov 2021 18:58:52 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Nov 2021 14:46:22 GMT",
"version": "v2"
}
] | 2021-11-17 | [
[
"Kohl",
"Finn Bjarne",
""
],
[
"Larfors",
"Magdalena",
""
],
[
"Oehlmann",
"Paul-Konstantin",
""
]
] | In this work we study F-theory on symmetric toroidal orbifolds that exhibit roto-translations, which are point group rotations accompanied by fractional lattice shifts. These geometries admit a rich class of effects, such as twisted affine folded fibers, multiple fibers, and up to three distinct torus-fibrations that y... | 18.064032 | 19.278992 | 22.492718 | 18.283482 | 21.09621 | 21.207048 | 19.807953 | 18.144684 | 16.636244 | 26.010403 | 16.244711 | 16.889307 | 18.430586 | 16.867596 | 16.629551 | 17.429232 | 16.883272 | 17.224804 | 16.911245 | 18.408579 | 16.290936 |
1508.06566 | Guido Franchetti | Guido Franchetti, Bernd J. Schroers | Adiabatic dynamics of instantons on $S ^4 $ | 49 pages, 11 figures. Significant improvements in the discussion of
framing in v2 | Commun. Math. Phys. 353, 185-228 (2017) | 10.1007/s00220-016-2769-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define and compute the $L^2$ metric on the framed moduli space of circle
invariant 1-instantons on the 4-sphere. This moduli space is four dimensional
and our metric is $SO(3) \times U(1)$ symmetric. We study the behaviour of
generic geodesics and show that the metric is geodesically incomplete.
Circle-invariant i... | [
{
"created": "Wed, 26 Aug 2015 16:45:41 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Jun 2016 16:03:55 GMT",
"version": "v2"
}
] | 2017-04-25 | [
[
"Franchetti",
"Guido",
""
],
[
"Schroers",
"Bernd J.",
""
]
] | We define and compute the $L^2$ metric on the framed moduli space of circle invariant 1-instantons on the 4-sphere. This moduli space is four dimensional and our metric is $SO(3) \times U(1)$ symmetric. We study the behaviour of generic geodesics and show that the metric is geodesically incomplete. Circle-invariant ins... | 5.36769 | 5.321334 | 6.011901 | 5.278975 | 5.1429 | 5.511447 | 5.996593 | 5.460495 | 5.588408 | 6.378284 | 5.327495 | 5.166593 | 5.317803 | 5.210613 | 5.256945 | 5.172538 | 5.306946 | 5.253843 | 5.252638 | 5.321377 | 5.223706 |
1801.07172 | Shotaro Shiba | Satoshi Iso, Shotaro Shiba and Sumito Yokoo | Scale-invariant Feature Extraction of Neural Network and Renormalization
Group Flow | 32 pages, 17 figures | Phys. Rev. E 97, 053304 (2018) | 10.1103/PhysRevE.97.053304 | KEK-TH-2029 | hep-th cond-mat.stat-mech cs.LG stat.ML | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Theoretical understanding of how deep neural network (DNN) extracts features
from input images is still unclear, but it is widely believed that the
extraction is performed hierarchically through a process of coarse-graining. It
reminds us of the basic concept of renormalization group (RG) in statistical
physics. In o... | [
{
"created": "Mon, 22 Jan 2018 16:18:04 GMT",
"version": "v1"
}
] | 2018-05-16 | [
[
"Iso",
"Satoshi",
""
],
[
"Shiba",
"Shotaro",
""
],
[
"Yokoo",
"Sumito",
""
]
] | Theoretical understanding of how deep neural network (DNN) extracts features from input images is still unclear, but it is widely believed that the extraction is performed hierarchically through a process of coarse-graining. It reminds us of the basic concept of renormalization group (RG) in statistical physics. In ord... | 6.300251 | 6.890383 | 6.605399 | 6.913554 | 6.143289 | 6.706629 | 6.488507 | 6.544376 | 6.206872 | 7.125367 | 6.223027 | 6.282207 | 6.587591 | 6.340152 | 6.252271 | 6.245872 | 6.262568 | 6.377698 | 6.430059 | 6.253906 | 6.271964 |
hep-th/9510165 | Oleg K. Sheinman | O.Sheinman | Integrable Many-Body Systems of Calogero-Moser-Sutherland Type in High
Dimension | amstex, no figures | null | null | null | hep-th | null | A new series of integrable cases of the many-body problem in many-dimensional
spaces is found. That series appears as a part of the larger series of
integrable problems, which are in 1-1 correspondence with Krichever-Novikov
algebras of affine type (that is with pairs each one consisting of some finite
root system an... | [
{
"created": "Sat, 21 Oct 1995 18:20:54 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Nov 1995 16:47:06 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Sheinman",
"O.",
""
]
] | A new series of integrable cases of the many-body problem in many-dimensional spaces is found. That series appears as a part of the larger series of integrable problems, which are in 1-1 correspondence with Krichever-Novikov algebras of affine type (that is with pairs each one consisting of some finite root system and ... | 10.323421 | 12.418949 | 14.026013 | 10.713992 | 11.417294 | 11.46435 | 11.793771 | 11.345181 | 11.575422 | 15.046178 | 10.882752 | 10.019527 | 10.847519 | 9.869954 | 10.080272 | 9.638904 | 10.134852 | 10.403411 | 9.789558 | 10.815959 | 10.363784 |
hep-th/0505151 | James Cline | Aaron Berndsen, Tirthabir Biswas, and James M. Cline | Moduli Stabilization in Brane Gas Cosmology with Superpotentials | minor changes to match the journal version | JCAP 0508 (2005) 012 | 10.1088/1475-7516/2005/08/012 | null | hep-th hep-ph | null | In the context of brane gas cosmology in superstring theory, we show why it
is impossible to simultaneously stabilize the dilaton and the radion with a
general gas of strings (including massless modes) and D-branes. Although this
requires invoking a different mechanism to stabilize these moduli fields, we
find that t... | [
{
"created": "Tue, 17 May 2005 16:16:03 GMT",
"version": "v1"
},
{
"created": "Wed, 18 May 2005 03:24:26 GMT",
"version": "v2"
},
{
"created": "Thu, 9 Jun 2005 19:18:51 GMT",
"version": "v3"
},
{
"created": "Fri, 22 Jul 2005 01:17:27 GMT",
"version": "v4"
}
] | 2017-09-20 | [
[
"Berndsen",
"Aaron",
""
],
[
"Biswas",
"Tirthabir",
""
],
[
"Cline",
"James M.",
""
]
] | In the context of brane gas cosmology in superstring theory, we show why it is impossible to simultaneously stabilize the dilaton and the radion with a general gas of strings (including massless modes) and D-branes. Although this requires invoking a different mechanism to stabilize these moduli fields, we find that the... | 9.284978 | 8.305766 | 10.532723 | 8.119471 | 8.610903 | 8.701509 | 8.746259 | 7.766719 | 8.448143 | 10.118874 | 8.637265 | 8.573266 | 9.201631 | 8.682365 | 8.841733 | 9.171446 | 8.960775 | 8.992086 | 8.97854 | 9.119019 | 8.363249 |
hep-th/0601018 | Manoel Messias Ferreira Junior | Manoel M. Ferreira Jr and Fernando M.O. Moucherek (UFMA) | Influence of Lorentz- and CPT-violating terms on the Dirac equation | 13 pages, no figures, revtex4 style | Int.J.Mod.Phys. A21 (2006) 6211-6227 | 10.1142/S0217751X06033842 | null | hep-th | null | The influence of Lorentz- and CPT-violating terms (in "vector" and "axial
vector" couplings) on the Dirac equation is explicitly analyzed: plane wave
solutions, dispersion relations and eigenenergies are explicitly obtained. The
non-relativistic limit is worked out and the Lorentz-violating Hamiltonian
identified in ... | [
{
"created": "Tue, 3 Jan 2006 20:12:01 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Apr 2006 21:51:39 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Jan 2007 20:50:38 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Ferreira",
"Manoel M.",
"Jr",
"UFMA"
],
[
"Moucherek",
"Fernando M. O.",
"",
"UFMA"
]
] | The influence of Lorentz- and CPT-violating terms (in "vector" and "axial vector" couplings) on the Dirac equation is explicitly analyzed: plane wave solutions, dispersion relations and eigenenergies are explicitly obtained. The non-relativistic limit is worked out and the Lorentz-violating Hamiltonian identified in bo... | 9.348249 | 8.148562 | 9.189679 | 8.446572 | 8.52561 | 9.140573 | 8.974532 | 8.654764 | 8.396211 | 9.662338 | 8.299809 | 8.66189 | 9.239363 | 8.71275 | 8.78209 | 8.623066 | 8.372539 | 8.49272 | 8.738789 | 9.097435 | 8.578196 |
1803.10778 | Paolo Glorioso | Ping Gao, Paolo Glorioso, Hong Liu | Ghostbusters: Unitarity and Causality of Non-equilibrium Effective Field
Theories | 27 pages, 5 figures | null | null | MIT-CTP/4994; EFI-18-4 | hep-th cond-mat.stat-mech nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For a non-equilibrium physical system defined along a closed time path (CTP),
a key constraint is the so-called largest time equation, which is a consequence
of unitarity and implies causality. In this paper, we present a simple proof
that if the propagators of a non-equilibrium effective action have the proper
pole ... | [
{
"created": "Wed, 28 Mar 2018 18:00:02 GMT",
"version": "v1"
}
] | 2018-03-30 | [
[
"Gao",
"Ping",
""
],
[
"Glorioso",
"Paolo",
""
],
[
"Liu",
"Hong",
""
]
] | For a non-equilibrium physical system defined along a closed time path (CTP), a key constraint is the so-called largest time equation, which is a consequence of unitarity and implies causality. In this paper, we present a simple proof that if the propagators of a non-equilibrium effective action have the proper pole st... | 11.521874 | 11.586621 | 12.209973 | 10.006523 | 11.240595 | 11.822738 | 11.461206 | 10.881385 | 10.580104 | 10.697363 | 10.635784 | 10.5536 | 10.818768 | 10.071187 | 10.482689 | 10.474066 | 10.463747 | 10.512707 | 10.318451 | 10.884018 | 10.008768 |
hep-th/0210267 | Khazret S. Nirov | Khazret S. Nirov and Alexander V. Razumov | W-algebras for non-abelian Toda systems | LaTeX, AMS fonts, 40 pages; v3: some comments and refs added | J.Geom.Phys. 48 (2003) 505-545 | 10.1016/S0393-0440(03)00054-8 | INR-TH-02-10/2 | hep-th math-ph math.MP nlin.SI | null | We construct the classical W-algebras for some non-abelian Toda systems
associated with the Lie groups GL(2n,R) and Sp(n,R). We start with the set of
characteristic integrals and find the Poisson brackets for the corresponding
Hamiltonian counterparts. The convenient block matrix representation for the
Toda equations... | [
{
"created": "Mon, 28 Oct 2002 17:54:24 GMT",
"version": "v1"
},
{
"created": "Sun, 10 Nov 2002 13:38:29 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Mar 2003 16:22:08 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Nirov",
"Khazret S.",
""
],
[
"Razumov",
"Alexander V.",
""
]
] | We construct the classical W-algebras for some non-abelian Toda systems associated with the Lie groups GL(2n,R) and Sp(n,R). We start with the set of characteristic integrals and find the Poisson brackets for the corresponding Hamiltonian counterparts. The convenient block matrix representation for the Toda equations i... | 11.459914 | 9.617463 | 11.476978 | 8.97413 | 10.056047 | 10.250523 | 10.041811 | 9.61874 | 9.844729 | 11.159113 | 9.765991 | 9.814927 | 10.318126 | 9.842477 | 10.513959 | 10.45133 | 10.146831 | 10.119621 | 10.07001 | 10.670765 | 9.917317 |
1204.3073 | Arttu Rajantie | Arttu Rajantie | Magnetic Monopoles in Field Theory and Cosmology | 15 pages, no figures. Based on a talk given at the discussion meeting
"Emergent magnetic monopoles in frustrated magnetic systems" at the Kavli
Royal Society International Centre, 17-18 October 2011. To be published in
Philosophical Transactions of the Royal Society A | Phil. Trans. R. Soc. A. 370 (2012) 5705-5717 | 10.1098/rsta.2011.0394 | Imperial/TP/2012/AR/1 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The existence of magnetic monopoles is predicted by many theories of particle
physics beyond the Standard Model. However, in spite of extensive searches,
there is no experimental or observational sign of them. I review the role of
magnetic monopoles in quantum field theory and discuss their implications for
particle ... | [
{
"created": "Fri, 13 Apr 2012 18:40:40 GMT",
"version": "v1"
}
] | 2013-02-28 | [
[
"Rajantie",
"Arttu",
""
]
] | The existence of magnetic monopoles is predicted by many theories of particle physics beyond the Standard Model. However, in spite of extensive searches, there is no experimental or observational sign of them. I review the role of magnetic monopoles in quantum field theory and discuss their implications for particle ph... | 5.384248 | 6.234625 | 5.279534 | 5.344369 | 5.291024 | 5.005976 | 5.362387 | 5.55179 | 4.955498 | 5.692731 | 5.2282 | 5.482238 | 5.222532 | 5.144404 | 5.354084 | 5.514203 | 5.373466 | 5.385936 | 5.202022 | 5.201324 | 5.467088 |
2304.12340 | Fri{\dh}rik Freyr Gautason | Fridrik Freyr Gautason, Valentina Giangreco M. Puletti, Jesse van
Muiden | Quantized Strings and Instantons in Holography | 38 pages. v2: Minor corrections. v3: Corrections to the fermion
partition function, appendix added. v4: Minor corrections | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study worldsheet instantons in holographic type IIA backgrounds directly
in string theory. The first background is a dimensional reduction of
AdS$_7\times S^4$ and is dual to the maximally supersymmetric Yang-Mills theory
on $S^5$. The second background is AdS$_4\times \mathbf{C}P^3$ dual to ABJM in
the type IIA l... | [
{
"created": "Mon, 24 Apr 2023 18:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Jun 2023 13:58:12 GMT",
"version": "v2"
},
{
"created": "Wed, 26 Jul 2023 20:37:40 GMT",
"version": "v3"
},
{
"created": "Wed, 20 Dec 2023 11:32:30 GMT",
"version": "v4"
}
] | 2023-12-21 | [
[
"Gautason",
"Fridrik Freyr",
""
],
[
"Puletti",
"Valentina Giangreco M.",
""
],
[
"van Muiden",
"Jesse",
""
]
] | We study worldsheet instantons in holographic type IIA backgrounds directly in string theory. The first background is a dimensional reduction of AdS$_7\times S^4$ and is dual to the maximally supersymmetric Yang-Mills theory on $S^5$. The second background is AdS$_4\times \mathbf{C}P^3$ dual to ABJM in the type IIA lim... | 6.284662 | 6.269144 | 6.848392 | 6.14502 | 6.131946 | 6.139147 | 6.063148 | 5.991891 | 6.234409 | 7.373996 | 5.984635 | 6.090896 | 6.319473 | 6.070812 | 6.016242 | 6.175002 | 6.032319 | 6.035114 | 5.989509 | 6.398139 | 6.027908 |
2406.03543 | Justin Berman | Justin Berman and Henriette Elvang | Corners and Islands in the S-matrix Bootstrap of the Open Superstring | 37 pages + appendices, 21 figures | null | null | LCTP-24-10 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We bootstrap the Veneziano superstring amplitude in 10 dimensions from the
bottom-up. Starting with the most general maximally supersymmetric Yang-Mills
EFT, we input information about the lowest-lying massive states, which we
assume contribute via tree-level exchanges to the 4-point amplitude. We show
the following:... | [
{
"created": "Wed, 5 Jun 2024 18:00:03 GMT",
"version": "v1"
}
] | 2024-06-07 | [
[
"Berman",
"Justin",
""
],
[
"Elvang",
"Henriette",
""
]
] | We bootstrap the Veneziano superstring amplitude in 10 dimensions from the bottom-up. Starting with the most general maximally supersymmetric Yang-Mills EFT, we input information about the lowest-lying massive states, which we assume contribute via tree-level exchanges to the 4-point amplitude. We show the following: (... | 12.760206 | 13.43778 | 14.236674 | 12.420587 | 12.936958 | 12.94369 | 12.692701 | 12.406322 | 11.964437 | 14.502623 | 12.175458 | 12.640028 | 13.024154 | 12.627079 | 13.078 | 12.303091 | 12.583487 | 12.443501 | 12.384559 | 13.560047 | 12.544033 |
2305.10491 | Marc Klinger | David S. Berman, Marc S. Klinger and Alexander G. Stapleton | Bayesian Renormalization | 20 pages, no figures. V2: Citation format fixed, references added.
V3: Journal accepted version, new Section 4 includes fully worked
implementation of Bayesian Renormalization to a Neural Network, 30 pages, 2
tables, 5 figures | null | 10.1088/2632-2153/ad0102 | null | hep-th cond-mat.dis-nn cs.AI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we present a fully information theoretic approach to
renormalization inspired by Bayesian statistical inference, which we refer to
as Bayesian Renormalization. The main insight of Bayesian Renormalization is
that the Fisher metric defines a correlation length that plays the role of an
emergent RG scale q... | [
{
"created": "Wed, 17 May 2023 18:00:28 GMT",
"version": "v1"
},
{
"created": "Sat, 27 May 2023 18:54:26 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Oct 2023 18:14:20 GMT",
"version": "v3"
}
] | 2023-10-11 | [
[
"Berman",
"David S.",
""
],
[
"Klinger",
"Marc S.",
""
],
[
"Stapleton",
"Alexander G.",
""
]
] | In this note we present a fully information theoretic approach to renormalization inspired by Bayesian statistical inference, which we refer to as Bayesian Renormalization. The main insight of Bayesian Renormalization is that the Fisher metric defines a correlation length that plays the role of an emergent RG scale qua... | 9.21302 | 10.032303 | 9.899944 | 9.562475 | 10.143236 | 10.150854 | 10.10542 | 9.453967 | 9.432212 | 10.996049 | 8.900865 | 9.02451 | 9.288275 | 8.897228 | 8.95591 | 8.928625 | 8.88825 | 8.857411 | 9.110142 | 9.154911 | 8.818498 |
2308.03194 | Matthew Buican | Matthew Buican and Hongliang Jiang | From Free Fields to Interacting SCFTs via Representation Theory | 30 pages; | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We ask when it is possible to construct arbitrary unitary multiplets of the
superconformal algebra with eight Poincar\'e supercharges that are compatible
with locality from (continuous deformations of) representations in free field
theories. We answer this question in two, three, and five dimensions. In four
dimensio... | [
{
"created": "Sun, 6 Aug 2023 19:23:11 GMT",
"version": "v1"
}
] | 2023-08-08 | [
[
"Buican",
"Matthew",
""
],
[
"Jiang",
"Hongliang",
""
]
] | We ask when it is possible to construct arbitrary unitary multiplets of the superconformal algebra with eight Poincar\'e supercharges that are compatible with locality from (continuous deformations of) representations in free field theories. We answer this question in two, three, and five dimensions. In four dimensions... | 11.985483 | 10.322993 | 13.521867 | 10.462856 | 10.751193 | 10.795216 | 11.279361 | 10.50128 | 10.928907 | 14.249681 | 10.079029 | 11.037728 | 11.423753 | 10.512738 | 11.07725 | 10.867229 | 11.338538 | 10.748151 | 10.810109 | 11.465116 | 9.905642 |
1003.1878 | Jae-Weon Lee Prof. | Jae-Weon Lee | Zero Cosmological Constant and Nonzero Dark Energy from Holographic
Principle | Revtex 7 pages 2 figs | J. Korean Phys. Soc. 63 (2013) 1088 | 10.3938/jkps.63.1088 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that the first law of thermodynamics and the holographic
principle applied to an arbitrary large cosmic causal horizon naturally demand
the zero cosmological constant and non-zero dynamical dark energy in the form
of the holographic dark energy. Semiclassical analysis shows that the
holographic dark energ... | [
{
"created": "Tue, 9 Mar 2010 14:22:42 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Apr 2010 15:00:36 GMT",
"version": "v2"
},
{
"created": "Tue, 25 Oct 2011 09:09:02 GMT",
"version": "v3"
},
{
"created": "Sat, 13 Apr 2013 14:19:08 GMT",
"version": "v4"
}
] | 2015-03-13 | [
[
"Lee",
"Jae-Weon",
""
]
] | It is shown that the first law of thermodynamics and the holographic principle applied to an arbitrary large cosmic causal horizon naturally demand the zero cosmological constant and non-zero dynamical dark energy in the form of the holographic dark energy. Semiclassical analysis shows that the holographic dark energy ... | 9.858369 | 9.974358 | 9.467393 | 8.942605 | 9.717393 | 9.100779 | 9.684131 | 9.518518 | 9.475116 | 9.979527 | 8.996901 | 8.904969 | 9.079836 | 8.968633 | 8.913664 | 8.966433 | 9.010753 | 8.951743 | 9.115771 | 9.271751 | 8.956258 |
1012.0549 | Andrei Linde | Vittoria Demozzi, Andrei Linde and Viatcheslav Mukhanov | Supercurvaton | 17 pages, 1 figure. Non-perturbative effects related to
non-gaussianity in the curvaton scenario are discussed, some references are
added. This is the version accepted in JCAP | null | 10.1088/1475-7516/2011/04/013 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss observational consequences of the curvaton scenario, which
naturally appears in the context of the simplest model of chaotic inflation in
supergravity. The non-gaussianity parameter f_NL in this scenario can take
values in the observationally interesting range from O(10) to O(100). These
values may be diff... | [
{
"created": "Thu, 2 Dec 2010 19:38:13 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Mar 2011 04:38:14 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Apr 2011 00:33:47 GMT",
"version": "v3"
}
] | 2015-05-20 | [
[
"Demozzi",
"Vittoria",
""
],
[
"Linde",
"Andrei",
""
],
[
"Mukhanov",
"Viatcheslav",
""
]
] | We discuss observational consequences of the curvaton scenario, which naturally appears in the context of the simplest model of chaotic inflation in supergravity. The non-gaussianity parameter f_NL in this scenario can take values in the observationally interesting range from O(10) to O(100). These values may be differ... | 9.177278 | 9.096771 | 9.517754 | 8.694736 | 9.614958 | 10.114594 | 9.277864 | 9.396651 | 8.21872 | 9.99493 | 8.526839 | 9.297771 | 9.038828 | 8.612336 | 8.915827 | 9.201884 | 8.819721 | 8.946353 | 9.053146 | 8.972827 | 8.402793 |
hep-th/9508099 | G. Mussardo | R. Konik, A. LeClair and G. Mussardo | On Ising Correlation Functions with Boundary Magnetic Field | 19 pages, 5 uu-figures, macros: harvmac.tex and epsf.tex three
references added | Int. J. Mod. Phys. A11 (1996) 2765 | 10.1142/S0217751X96001346 | CLNS 95/1355, ISAS/EP/95/93 | hep-th cond-mat | null | Exact expressions of the boundary state and the form factors of the Ising
model are used to derive differential equations for the one-point functions of
the energy and magnetization operators of the model in the presence of a
boundary magnetic field. We also obtain explicit formulas for the massless
limit of the one-... | [
{
"created": "Mon, 21 Aug 1995 11:20:12 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Aug 1995 11:10:21 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Konik",
"R.",
""
],
[
"LeClair",
"A.",
""
],
[
"Mussardo",
"G.",
""
]
] | Exact expressions of the boundary state and the form factors of the Ising model are used to derive differential equations for the one-point functions of the energy and magnetization operators of the model in the presence of a boundary magnetic field. We also obtain explicit formulas for the massless limit of the one-po... | 7.04931 | 6.567177 | 7.805085 | 6.222514 | 6.454944 | 6.795937 | 6.409104 | 6.589859 | 6.109937 | 9.843325 | 6.090143 | 6.654085 | 7.879027 | 6.809434 | 6.641277 | 6.698607 | 6.667241 | 6.535348 | 6.88912 | 7.638677 | 6.723002 |
1610.08864 | Jiahua Tian | James Halverson and Jiahua Tian | The Cost of Seven-brane Gauge Symmetry in a Quadrillion F-theory
Compactifications | 11 pages | Phys. Rev. D 95, 026005 (2017) | 10.1103/PhysRevD.95.026005 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study seven-branes in $O(10^{15})$ four-dimensional F-theory
compactifications where seven-brane moduli must be tuned in order to achieve
non-abelian gauge symmetry. The associated compact spaces $B$ are the set of
all smooth weak Fano toric threefolds. By a study of fine star regular
triangulations of three dimen... | [
{
"created": "Thu, 27 Oct 2016 16:16:46 GMT",
"version": "v1"
}
] | 2017-01-11 | [
[
"Halverson",
"James",
""
],
[
"Tian",
"Jiahua",
""
]
] | We study seven-branes in $O(10^{15})$ four-dimensional F-theory compactifications where seven-brane moduli must be tuned in order to achieve non-abelian gauge symmetry. The associated compact spaces $B$ are the set of all smooth weak Fano toric threefolds. By a study of fine star regular triangulations of three dimensi... | 8.315692 | 8.161506 | 8.541412 | 7.777519 | 8.505196 | 9.269018 | 8.746574 | 8.414952 | 7.744226 | 9.797961 | 8.105779 | 7.917776 | 8.148951 | 7.647539 | 7.636166 | 7.757926 | 7.829887 | 7.962185 | 7.644361 | 8.276124 | 7.486435 |
hep-th/9909076 | null | Hisaki Hatanaka, Makoto Sakamoto, Motoi Tachibana, Kazunori Takenaga | Many-Brane Extention of the Randall-Sundrum Solution | PTPTeX 1.0(preprint style), 8 pages, no figures, references and typos
corrected | Prog.Theor.Phys. 102 (1999) 1213-1218 | 10.1143/PTP.102.1213 | KOBE-TH-99-05, YITP-99-55, IFUP-TH-50-99 | hep-th | null | Recently, Randall and Sundrum proposed a static solution to Einstein's
equations in five spacetime dimensions with two 3-branes located at the fixed
points of $S^1/Z_2$ to solve the hierarchy problem. We extend the solution and
construct static and also inflationary solutions to Einstein's equations in
five spacetime... | [
{
"created": "Mon, 13 Sep 1999 07:17:47 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Nov 1999 07:49:43 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Hatanaka",
"Hisaki",
""
],
[
"Sakamoto",
"Makoto",
""
],
[
"Tachibana",
"Motoi",
""
],
[
"Takenaga",
"Kazunori",
""
]
] | Recently, Randall and Sundrum proposed a static solution to Einstein's equations in five spacetime dimensions with two 3-branes located at the fixed points of $S^1/Z_2$ to solve the hierarchy problem. We extend the solution and construct static and also inflationary solutions to Einstein's equations in five spacetime d... | 6.421113 | 4.869563 | 5.392624 | 5.235765 | 4.922752 | 4.872298 | 5.146971 | 5.160246 | 5.263357 | 5.676338 | 5.529484 | 5.08791 | 5.153316 | 4.939661 | 5.173095 | 5.115729 | 5.374478 | 5.201025 | 5.044895 | 5.235994 | 5.132278 |
hep-th/0606219 | Juan Antonio Nieto | J. A. Nieto | The 2+2-Signature and the 1+1-Matrix-Brane | 12 pages, Latex, to appear in Mod. Phys. Lett. A | Mod.Phys.Lett.A22:2453-2461,2007 | 10.1142/S0217732307022657 | null | hep-th | null | We discuss different aspects of the 2+2-signature from the point of view of
the quatl theory. In particular, we compare two alternative approaches to such
a spacetime signature, namely the 1+1-matrix-brane and the 2+2-target spacetime
of a string. This analysis also reveals hidden discrete symmetries of the
2+2-brane... | [
{
"created": "Thu, 22 Jun 2006 18:10:26 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Nov 2006 20:05:25 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Jan 2007 18:50:33 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Nieto",
"J. A.",
""
]
] | We discuss different aspects of the 2+2-signature from the point of view of the quatl theory. In particular, we compare two alternative approaches to such a spacetime signature, namely the 1+1-matrix-brane and the 2+2-target spacetime of a string. This analysis also reveals hidden discrete symmetries of the 2+2-brane a... | 16.649971 | 14.974401 | 18.230618 | 16.505014 | 13.625343 | 16.301115 | 15.710979 | 13.851209 | 15.897429 | 16.88183 | 14.570931 | 14.430922 | 15.21358 | 15.450942 | 15.455245 | 15.29848 | 15.590636 | 14.991345 | 15.19129 | 16.089422 | 15.45704 |
1012.1832 | Ashok Das | Ashok Das and J. Frenkel | Infrared chiral anomaly at finite temperature | revtex, 5pages | Phys.Lett.B696:556-559,2011 | 10.1016/j.physletb.2011.01.017 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Schwinger model at finite temperature and show that a
temperature dependent chiral anomaly may arise from the long distance behavior
of the electric field. At high temperature this anomaly depends linearly on the
temperature $T$ and is present not only in the two point function, but also in
all even poin... | [
{
"created": "Wed, 8 Dec 2010 19:27:07 GMT",
"version": "v1"
}
] | 2011-02-16 | [
[
"Das",
"Ashok",
""
],
[
"Frenkel",
"J.",
""
]
] | We study the Schwinger model at finite temperature and show that a temperature dependent chiral anomaly may arise from the long distance behavior of the electric field. At high temperature this anomaly depends linearly on the temperature $T$ and is present not only in the two point function, but also in all even point ... | 9.193354 | 7.664649 | 8.581551 | 7.106067 | 7.765364 | 7.378585 | 7.862375 | 7.900622 | 6.82667 | 8.169581 | 7.804152 | 7.341082 | 8.067139 | 7.716517 | 7.800436 | 7.734045 | 7.395804 | 7.766884 | 7.636697 | 8.508797 | 7.719949 |
2112.05710 | Lucas Pinol | Lucas Pinol, Shuntaro Aoki, S\'ebastien Renaux-Petel, Masahide
Yamaguchi | Inflationary flavor oscillations and the cosmic spectroscopy | v2: 7 pages, 4 figures, minor modifications, version published as a
Letter in PRD | null | 10.1103/PhysRevD.107.L021301 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inflationary scenarios motivated by high-energy physics generically contain a
plethora of degrees of freedom beyond the primordial curvature perturbation.
The latter interacts in a simple way with what we name "inflationary flavor
eigenstates", which differ, in general, from freely propagating "mass
eigenstates". We ... | [
{
"created": "Fri, 10 Dec 2021 18:06:46 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Jan 2023 11:33:50 GMT",
"version": "v2"
}
] | 2023-01-23 | [
[
"Pinol",
"Lucas",
""
],
[
"Aoki",
"Shuntaro",
""
],
[
"Renaux-Petel",
"Sébastien",
""
],
[
"Yamaguchi",
"Masahide",
""
]
] | Inflationary scenarios motivated by high-energy physics generically contain a plethora of degrees of freedom beyond the primordial curvature perturbation. The latter interacts in a simple way with what we name "inflationary flavor eigenstates", which differ, in general, from freely propagating "mass eigenstates". We sh... | 11.918278 | 11.748363 | 10.391864 | 10.40909 | 12.001728 | 11.282868 | 11.759887 | 10.700603 | 10.707008 | 11.832604 | 10.293251 | 10.958378 | 11.092496 | 10.687174 | 10.864596 | 10.567592 | 10.979202 | 10.905694 | 10.632547 | 10.902021 | 10.53732 |
0704.2465 | Alberto T. Faraggi | Maximo Banados (Chile U., Catolica), Alberto T. Faraggi (Michigan U.),
Stefan Theisen (Potsdam, Max Planck Inst.) | N=2 supergravity in three dimensions and its Godel supersymmetric
background | null | Phys.Rev.D75:125015,2007 | 10.1103/PhysRevD.75.125015 | null | hep-th | null | The four dimensional Godel spacetime is known to have the structure M_3 x R.
It is also known that the three-dimensional factor M_3 is an exact solution of
three-dimensional gravity coupled to a Maxwell-Chern-Simons theory. We build in
this paper a N=2 supergravity extension for this action and prove that the
Godel b... | [
{
"created": "Thu, 19 Apr 2007 05:42:25 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Apr 2007 19:45:02 GMT",
"version": "v2"
},
{
"created": "Wed, 6 Jun 2007 04:53:42 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Banados",
"Maximo",
"",
"Chile U., Catolica"
],
[
"Faraggi",
"Alberto T.",
"",
"Michigan U."
],
[
"Theisen",
"Stefan",
"",
"Potsdam, Max Planck Inst."
]
] | The four dimensional Godel spacetime is known to have the structure M_3 x R. It is also known that the three-dimensional factor M_3 is an exact solution of three-dimensional gravity coupled to a Maxwell-Chern-Simons theory. We build in this paper a N=2 supergravity extension for this action and prove that the Godel bac... | 10.429419 | 9.007931 | 9.213108 | 8.950264 | 8.842515 | 9.249393 | 8.425144 | 8.718987 | 8.32569 | 10.429741 | 8.439584 | 8.268976 | 9.527977 | 8.617249 | 8.801514 | 8.575995 | 8.592405 | 8.347573 | 8.991492 | 9.482001 | 8.975974 |
0710.1063 | Ludmil Hadjiivanov | P. Furlan, L. Hadjiivanov, I. Todorov | Zero modes' fusion ring and braid group representations for the extended
chiral su(2) WZNW model | 36 pages, 1 figure; version 3 - improvements in Sec. 2 and 3:
definitions of the double, as well as R- (and M-)matrix changed to fit the
zero modes' ones | Lett.Math.Phys.82:117-151,2007 | 10.1007/s11005-007-0209-4 | null | hep-th math-ph math.MP math.QA | null | The zero modes' Fock space for the extended chiral $su(2)$ WZNW model gives
room to a realization of the Grothendieck fusion ring of representations of the
restricted $U_q sl(2)$ quantum universal enveloping algebra (QUEA) at an even
($2h$-th) root of unity, and of its extension by the Lusztig operators. It is
shown ... | [
{
"created": "Thu, 4 Oct 2007 18:12:55 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jan 2008 11:33:24 GMT",
"version": "v2"
},
{
"created": "Thu, 24 Apr 2008 10:10:59 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Furlan",
"P.",
""
],
[
"Hadjiivanov",
"L.",
""
],
[
"Todorov",
"I.",
""
]
] | The zero modes' Fock space for the extended chiral $su(2)$ WZNW model gives room to a realization of the Grothendieck fusion ring of representations of the restricted $U_q sl(2)$ quantum universal enveloping algebra (QUEA) at an even ($2h$-th) root of unity, and of its extension by the Lusztig operators. It is shown th... | 9.316849 | 9.405871 | 11.021903 | 9.023424 | 9.329163 | 10.0682 | 10.107495 | 9.436146 | 9.460605 | 12.620421 | 9.055175 | 8.87304 | 9.62354 | 8.891776 | 8.982499 | 8.883461 | 8.567522 | 8.88395 | 8.81197 | 9.291303 | 8.9123 |
hep-th/9809063 | Nissan Itzhaki | N. Itzhaki | D6+D0 and Five Dimensional Spinning Black Hole | 8 pages | JHEP 9809:018,1998 | 10.1088/1126-6708/1998/09/018 | UCSBTH-98-6 | hep-th | null | We study the system of D6+D0 branes at sub-stringy scale. We show that the
proper description of the system, for large background field associated with
the D0-branes, is via spinning chargeless black holes in five dimensions. The
repulsive force between the D6-branes and the D0-branes is understood through
the centri... | [
{
"created": "Wed, 9 Sep 1998 18:58:05 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Itzhaki",
"N.",
""
]
] | We study the system of D6+D0 branes at sub-stringy scale. We show that the proper description of the system, for large background field associated with the D0-branes, is via spinning chargeless black holes in five dimensions. The repulsive force between the D6-branes and the D0-branes is understood through the centrifu... | 10.947194 | 10.800866 | 12.339382 | 9.995777 | 10.051493 | 9.624412 | 10.225448 | 9.273888 | 9.537352 | 12.706022 | 9.509624 | 9.802803 | 10.70322 | 9.848707 | 9.464224 | 9.596789 | 9.462336 | 9.728776 | 9.986205 | 10.320914 | 9.648049 |
2002.12335 | Alexandria Costantino | Alexandria Costantino, Sylvain Fichet, Philip Tanedo | Effective Field Theory in AdS: Continuum Regime, Soft Bombs, and IR
Emergence | 27 pages, 3 figures; v4: Minor text improvements, references added | Phys. Rev. D 102, 115038 (2020) | 10.1103/PhysRevD.102.115038 | UCR-TR-2020-FLIP-IG-11 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a scalar field in a slice of Lorentzian five-dimensional AdS at
arbitrary energies. We show that the presence of bulk interactions separate the
behavior of the theory into two different regimes: Kaluza--Klein and continuum.
We determine the transition scale between these regimes and show that UV brane
cor... | [
{
"created": "Thu, 27 Feb 2020 18:54:24 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Jun 2020 06:23:02 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Jan 2021 03:03:02 GMT",
"version": "v3"
},
{
"created": "Fri, 12 Mar 2021 18:57:55 GMT",
"version": "v4"
}
] | 2021-03-15 | [
[
"Costantino",
"Alexandria",
""
],
[
"Fichet",
"Sylvain",
""
],
[
"Tanedo",
"Philip",
""
]
] | We consider a scalar field in a slice of Lorentzian five-dimensional AdS at arbitrary energies. We show that the presence of bulk interactions separate the behavior of the theory into two different regimes: Kaluza--Klein and continuum. We determine the transition scale between these regimes and show that UV brane corre... | 14.089927 | 14.963313 | 14.741043 | 13.493459 | 13.735205 | 14.569111 | 14.698534 | 14.274387 | 13.748478 | 14.22051 | 13.915638 | 13.659824 | 14.082024 | 13.904977 | 13.88062 | 14.461073 | 13.9496 | 13.682041 | 13.497825 | 14.243247 | 13.763988 |
1007.4380 | Alexander Reshetnyak | V. Egorushkin, N. Melnikova, A. Ponomarev and A. Reshetnyak (Institute
of Strength Physics and Material Science, Tomsk, Russia) | Anomalous thermal conductivity in multiwalled carbon nanotubes with
impurities and short-range order | 8 pages, 3 figures, contribution to the proceedings of the 2nd
International Conference on Theoretical Physics DUBNA-NANO2010, Dubna,
Russia, 5-10 July, 2010 | J.Phys.Conf.Ser.248:012005,2010 | 10.1088/1742-6596/248/1/012005 | null | hep-th cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Low-temperature thermal conductivity and thermopower of multiwalled carbon
nanotubes considered within a bundle of nanotubes are calculated taking into
account multiple scattering of electrons on the atoms of impurities (like
single carbon atoms) and short-range order regions arising due to a some
distribution of the... | [
{
"created": "Mon, 26 Jul 2010 06:19:48 GMT",
"version": "v1"
}
] | 2010-12-07 | [
[
"Egorushkin",
"V.",
"",
"Institute\n of Strength Physics and Material Science, Tomsk, Russia"
],
[
"Melnikova",
"N.",
"",
"Institute\n of Strength Physics and Material Science, Tomsk, Russia"
],
[
"Ponomarev",
"A.",
"",
"Institute\n of Strength Physics an... | Low-temperature thermal conductivity and thermopower of multiwalled carbon nanotubes considered within a bundle of nanotubes are calculated taking into account multiple scattering of electrons on the atoms of impurities (like single carbon atoms) and short-range order regions arising due to a some distribution of the i... | 15.038774 | 18.74786 | 16.139061 | 15.184956 | 15.836263 | 18.666502 | 16.497229 | 16.803322 | 16.490263 | 16.221771 | 14.767768 | 13.517212 | 13.811227 | 14.289465 | 14.567134 | 14.081568 | 14.363723 | 13.384893 | 13.568548 | 13.708695 | 13.872627 |
hep-th/0401001 | Christopher Pope | J. Kerimo, J.T. Liu, H. Lu and C.N. Pope | Variant N=(1,1) Supergravity and (Minkowski)_4 x S^2 Vacua | Latex, 17 pages. Version appearing in Classical and Quantum Gravity | Class.Quant.Grav.21:3287-3300,2004 | 10.1088/0264-9381/21/13/011 | MIFP-04-01 | hep-th | null | We construct the fermionic sector and supersymmetry transformation rules of a
variant N=(1,1) supergravity theory obtained by generalized Kaluza-Klein
reduction from seven dimensions. We show that this model admits both
(Minkowski)_4 x S^2 and (Minkowski)_3 x S^3 vacua. We perform a consistent
Kaluza-Klein reduction ... | [
{
"created": "Mon, 5 Jan 2004 20:24:49 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Aug 2004 08:05:20 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Kerimo",
"J.",
""
],
[
"Liu",
"J. T.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
]
] | We construct the fermionic sector and supersymmetry transformation rules of a variant N=(1,1) supergravity theory obtained by generalized Kaluza-Klein reduction from seven dimensions. We show that this model admits both (Minkowski)_4 x S^2 and (Minkowski)_3 x S^3 vacua. We perform a consistent Kaluza-Klein reduction on... | 5.198018 | 4.629976 | 5.176077 | 4.453071 | 4.372828 | 4.561596 | 4.933042 | 4.298378 | 4.560518 | 5.549652 | 4.745414 | 4.578654 | 4.992988 | 4.65437 | 4.827822 | 4.610958 | 4.693151 | 4.678231 | 4.720768 | 4.929988 | 4.772707 |
1802.05201 | Shota Komatsu | Simone Giombi, Shota Komatsu | Exact Correlators on the Wilson Loop in $\mathcal{N}=4$ SYM:
Localization, Defect CFT, and Integrability | 43+4 pages; v2 References added. Minor corrections. Explanation in
section 4.2 expanded; v3 Corrected statements about nonplanar corrections | null | 10.1007/JHEP05(2018)109 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute a set of correlation functions of operator insertions on the 1/8
BPS Wilson loop in $\mathcal{N}=4$ SYM by employing supersymmetric
localization, OPE and the Gram-Schmidt orthogonalization. These correlators
exhibit a simple determinant structure, are position-independent and form a
topological subsector, ... | [
{
"created": "Wed, 14 Feb 2018 16:48:58 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Feb 2018 15:31:00 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Nov 2018 03:31:22 GMT",
"version": "v3"
}
] | 2018-11-09 | [
[
"Giombi",
"Simone",
""
],
[
"Komatsu",
"Shota",
""
]
] | We compute a set of correlation functions of operator insertions on the 1/8 BPS Wilson loop in $\mathcal{N}=4$ SYM by employing supersymmetric localization, OPE and the Gram-Schmidt orthogonalization. These correlators exhibit a simple determinant structure, are position-independent and form a topological subsector, bu... | 5.806104 | 6.031329 | 7.419625 | 5.692366 | 5.813243 | 5.893214 | 5.626204 | 5.840624 | 5.91794 | 8.369529 | 5.634634 | 6.1024 | 6.441121 | 6.056575 | 5.91367 | 5.947076 | 5.982698 | 6.061965 | 5.930423 | 6.500293 | 5.904119 |
hep-th/0206046 | Dejan Stojkovic | Valeri Frolov and Dejan Stojkovic | Black Hole Radiation in the Brane World and Recoil Effect | references added, accepted for publication in Phys. Rev. D | Phys.Rev.D66:084002,2002 | 10.1103/PhysRevD.66.084002 | null | hep-th gr-qc hep-ph | null | A black hole attached to a brane in a higher dimensional space emitting
quanta into the bulk may leave the brane as a result of a recoil. We study this
effect. We consider black holes which have a size much smaller than the
characteristic size of extra dimensions. Such a black hole can be effectively
described as a m... | [
{
"created": "Thu, 6 Jun 2002 00:32:01 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Jun 2002 23:59:24 GMT",
"version": "v2"
},
{
"created": "Sat, 3 Aug 2002 18:01:15 GMT",
"version": "v3"
}
] | 2009-07-09 | [
[
"Frolov",
"Valeri",
""
],
[
"Stojkovic",
"Dejan",
""
]
] | A black hole attached to a brane in a higher dimensional space emitting quanta into the bulk may leave the brane as a result of a recoil. We study this effect. We consider black holes which have a size much smaller than the characteristic size of extra dimensions. Such a black hole can be effectively described as a mas... | 10.172515 | 8.81413 | 9.990249 | 8.93174 | 10.302657 | 9.990368 | 10.25581 | 9.026953 | 8.687457 | 10.901889 | 8.88384 | 9.470327 | 9.596703 | 9.3288 | 9.29507 | 9.430377 | 9.584227 | 9.356083 | 9.184421 | 9.691154 | 9.14185 |
2205.01119 | Stefano Andriolo | Stefano Andriolo and Gary Shiu and Pablo Soler and Thomas Van Riet | Axion wormholes with massive dilaton | 18 pages, 4 figures, published version | Class. Quant. Grav., Vol. 39, num. 21, pg. 215014, 2022 | 10.1088/1361-6382/ac8fdc | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | If Euclidean wormholes contribute meaningfully to the path integral of
quantum gravity they can have important implications for particle physics and
cosmology. The dominant effects arise from wormholes whose sizes are comparable
to the cut-off scale of effective field theory, for which ultraviolet
corrections become ... | [
{
"created": "Mon, 2 May 2022 18:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Nov 2022 19:31:07 GMT",
"version": "v2"
}
] | 2022-11-10 | [
[
"Andriolo",
"Stefano",
""
],
[
"Shiu",
"Gary",
""
],
[
"Soler",
"Pablo",
""
],
[
"Van Riet",
"Thomas",
""
]
] | If Euclidean wormholes contribute meaningfully to the path integral of quantum gravity they can have important implications for particle physics and cosmology. The dominant effects arise from wormholes whose sizes are comparable to the cut-off scale of effective field theory, for which ultraviolet corrections become re... | 12.721764 | 10.555714 | 11.118499 | 10.62517 | 10.913844 | 10.619231 | 10.69116 | 9.999364 | 10.589445 | 13.453668 | 10.14316 | 10.858609 | 11.407498 | 10.407453 | 10.480775 | 10.57175 | 10.543566 | 10.441572 | 10.990372 | 11.237907 | 10.032918 |
hep-th/9907126 | Sang Jin Sin | Mannque Rho, Sang-Jin Sin, Ismail Zahed | Elastic Parton-Parton Scattering from AdS/CFT | latex2e, 12 pages, 1 figure, missing factor i corrected. Improved
argument given | Phys.Lett. B466 (1999) 199-205 | 10.1016/S0370-2693(99)01118-1 | KIAS-P99045 | hep-th hep-ph | null | Using the AdS/CFT correspondence and the eikonal approximation, we evaluate
the elastic parton-parton scattering amplitude at large $N$ and strong coupling
$g^2N$ in N=4 SYM. We obtain a scattering amplitude with a Regge behavior that
unitarizes at large $\sqrt{s}$.
| [
{
"created": "Thu, 15 Jul 1999 14:56:30 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Aug 1999 22:52:31 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Rho",
"Mannque",
""
],
[
"Sin",
"Sang-Jin",
""
],
[
"Zahed",
"Ismail",
""
]
] | Using the AdS/CFT correspondence and the eikonal approximation, we evaluate the elastic parton-parton scattering amplitude at large $N$ and strong coupling $g^2N$ in N=4 SYM. We obtain a scattering amplitude with a Regge behavior that unitarizes at large $\sqrt{s}$. | 7.794056 | 6.434804 | 5.964402 | 5.726152 | 6.272406 | 8.018512 | 6.706548 | 6.551513 | 6.131659 | 6.707245 | 6.602815 | 7.011774 | 6.316492 | 6.184406 | 6.821765 | 6.907474 | 6.482873 | 6.793443 | 6.491681 | 6.308245 | 6.274056 |
0908.2302 | Supratik Pal Dr | Barun Kumar Pal, Supratik Pal, B. Basu | Mutated Hilltop Inflation : A Natural Choice for Early Universe | 22 pages, 7 figures, 2 tables. Matches published version in JCAP | JCAP 1001:029,2010 | 10.1088/1475-7516/2010/01/029 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a model of inflation with a suitable potential for a single scalar
field which falls in the wide class of hilltop inflation. We derive the
analytical expressions for most of the physical quantities related to inflation
and show that all of them represent the true behavior as required from a model
of inflat... | [
{
"created": "Mon, 17 Aug 2009 08:04:23 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Dec 2009 09:13:02 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Jan 2010 06:18:19 GMT",
"version": "v3"
}
] | 2010-01-28 | [
[
"Pal",
"Barun Kumar",
""
],
[
"Pal",
"Supratik",
""
],
[
"Basu",
"B.",
""
]
] | We propose a model of inflation with a suitable potential for a single scalar field which falls in the wide class of hilltop inflation. We derive the analytical expressions for most of the physical quantities related to inflation and show that all of them represent the true behavior as required from a model of inflatio... | 12.22979 | 12.645671 | 11.283522 | 10.750606 | 12.067682 | 10.489277 | 12.743836 | 10.839274 | 11.146751 | 12.018904 | 11.849439 | 11.870937 | 11.581951 | 11.518471 | 11.542768 | 11.41288 | 11.468431 | 11.341442 | 11.830537 | 11.650501 | 11.552262 |
hep-th/0203142 | Norisuke Sakai | Norisuke Sakai and Ryo Sugisaka | Winding number and non-BPS bound states of walls in nonlinear sigma
models | 20pages, 14 figures, minor misprint corrections, figures added,
explanation of winding number added | Phys.Rev. D66 (2002) 045010 | 10.1103/PhysRevD.66.045010 | TIT/HEP-475 | hep-th | null | Non-supersymmetric multi-wall configurations are generically unstable. It is
proposed that the stabilization in compact space can be achieved by introducing
a winding number into the model. A BPS-like bound is studied for the energy of
configuration with nonvanishing winding number. Winding number is implemented
in a... | [
{
"created": "Fri, 15 Mar 2002 11:12:40 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Mar 2002 10:18:49 GMT",
"version": "v2"
},
{
"created": "Mon, 13 May 2002 05:08:15 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Sakai",
"Norisuke",
""
],
[
"Sugisaka",
"Ryo",
""
]
] | Non-supersymmetric multi-wall configurations are generically unstable. It is proposed that the stabilization in compact space can be achieved by introducing a winding number into the model. A BPS-like bound is studied for the energy of configuration with nonvanishing winding number. Winding number is implemented in an ... | 13.303933 | 11.862934 | 14.744509 | 12.083627 | 12.636497 | 11.397282 | 12.086148 | 11.172581 | 11.535441 | 15.391623 | 11.019502 | 11.096125 | 13.548642 | 12.065809 | 12.322768 | 11.588044 | 12.425841 | 11.884153 | 11.443516 | 13.939438 | 11.375966 |
hep-th/9907086 | Angel Uranga | J. Park, R. Rabadan, A. M. Uranga | Orientifolding the conifold | 52 pages, Latex 7 eps figures | Nucl.Phys.B570:38-80,2000 | 10.1016/S0550-3213(99)00700-2 | FTUAM-99/22, IASSNS-HEP-99/62, IFT-UAM/CSIC-99-26 | hep-th | null | In this paper we study the N=1 supersymmetric field theories realized on the
world-volume of type IIB D3-branes sitting at orientifolds of non-orbifold
singularities (conifold and generalizations). Several chiral models belong to
this family of theories. These field theories have a T-dual realization in
terms of type... | [
{
"created": "Mon, 12 Jul 1999 17:14:58 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Aug 1999 19:03:40 GMT",
"version": "v2"
}
] | 2009-10-09 | [
[
"Park",
"J.",
""
],
[
"Rabadan",
"R.",
""
],
[
"Uranga",
"A. M.",
""
]
] | In this paper we study the N=1 supersymmetric field theories realized on the world-volume of type IIB D3-branes sitting at orientifolds of non-orbifold singularities (conifold and generalizations). Several chiral models belong to this family of theories. These field theories have a T-dual realization in terms of type I... | 6.71322 | 6.384342 | 7.604202 | 6.364423 | 6.707183 | 6.357888 | 6.229153 | 6.262249 | 6.131205 | 8.343904 | 6.416965 | 6.405153 | 6.915589 | 6.489625 | 6.674018 | 6.547591 | 6.444078 | 6.265944 | 6.425365 | 7.03628 | 6.348436 |
hep-th/9811200 | Leonid Chekhov | L. Chekhov and K. Palamarchuk | Two-logarithm matrix model with an external field | 15pp., LaTeX, no figures, reference added | Mod.Phys.Lett.A14:2229-2244,1999 | 10.1142/S0217732399002315 | null | hep-th | null | We investigate the two-logarithm matrix model with the potential
$X\Lambda+\alpha\log(1+X)+\beta\log(1-X)$ related to an exactly solvable
Kazakov-Migdal model. In the proper normalization, using Virasoro constraints,
we prove the equivalence of this model and the Kontsevich-Penner matrix model
and construct the 1/N-e... | [
{
"created": "Mon, 23 Nov 1998 16:12:06 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Feb 1999 12:33:07 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Chekhov",
"L.",
""
],
[
"Palamarchuk",
"K.",
""
]
] | We investigate the two-logarithm matrix model with the potential $X\Lambda+\alpha\log(1+X)+\beta\log(1-X)$ related to an exactly solvable Kazakov-Migdal model. In the proper normalization, using Virasoro constraints, we prove the equivalence of this model and the Kontsevich-Penner matrix model and construct the 1/N-exp... | 9.165684 | 7.812182 | 10.636226 | 8.370302 | 8.864897 | 8.056001 | 8.418653 | 8.439186 | 7.931092 | 12.457673 | 7.602473 | 8.723086 | 9.930675 | 8.778852 | 9.030766 | 8.744007 | 8.91639 | 8.584444 | 9.077165 | 9.895244 | 8.345236 |
hep-th/0507017 | Herbert Hamber | Herbert W. Hamber and Ruth M. Williams | Nonlocal Effective Gravitational Field Equations and the Running of
Newton's G | 33 pages | Phys.Rev.D72:044026,2005 | 10.1103/PhysRevD.72.044026 | DAMTP-2005-59 | hep-th astro-ph gr-qc | null | Non-perturbative studies of quantum gravity have recently suggested the
possibility that the strength of gravitational interactions might slowly
increase with distance. Here a set of generally covariant effective field
equations are proposed, which are intended to incorporate the gravitational,
vacuum-polarization in... | [
{
"created": "Fri, 1 Jul 2005 18:45:46 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Hamber",
"Herbert W.",
""
],
[
"Williams",
"Ruth M.",
""
]
] | Non-perturbative studies of quantum gravity have recently suggested the possibility that the strength of gravitational interactions might slowly increase with distance. Here a set of generally covariant effective field equations are proposed, which are intended to incorporate the gravitational, vacuum-polarization indu... | 12.887582 | 14.116311 | 12.565001 | 11.762767 | 12.740221 | 13.741874 | 14.003453 | 11.424896 | 12.143757 | 12.104857 | 12.426938 | 12.344361 | 12.417043 | 12.36498 | 12.404003 | 12.684312 | 12.722404 | 12.358628 | 12.490932 | 12.414586 | 12.049463 |
2405.20332 | Ben Heidenreich | Muldrow Etheredge, Ben Heidenreich, Tom Rudelius, Ignacio Ruiz, Irene
Valenzuela | Taxonomy of Infinite Distance Limits | 69 pages plus appendices, 30 figures | null | null | ACFI-T24-04, CERN-TH-2024-067, IFT-UAM/CSIC-23-64 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Emergent String Conjecture constrains the possible types of light towers
in infinite-distance limits in quantum gravity moduli spaces. In this paper, we
use these constraints to restrict the geometry of the scalar charge-to-mass
vectors $(-\vec{\nabla}\log m)$ of the light towers and the analogous vector
$(-\vec{... | [
{
"created": "Thu, 30 May 2024 17:59:05 GMT",
"version": "v1"
}
] | 2024-05-31 | [
[
"Etheredge",
"Muldrow",
""
],
[
"Heidenreich",
"Ben",
""
],
[
"Rudelius",
"Tom",
""
],
[
"Ruiz",
"Ignacio",
""
],
[
"Valenzuela",
"Irene",
""
]
] | The Emergent String Conjecture constrains the possible types of light towers in infinite-distance limits in quantum gravity moduli spaces. In this paper, we use these constraints to restrict the geometry of the scalar charge-to-mass vectors $(-\vec{\nabla}\log m)$ of the light towers and the analogous vector $(-\vec{\n... | 11.285398 | 9.213934 | 12.136642 | 9.422513 | 9.313964 | 8.941918 | 8.950862 | 8.780966 | 9.167002 | 12.891752 | 8.50295 | 9.563665 | 10.420628 | 9.937694 | 9.827777 | 9.813962 | 9.956004 | 9.635359 | 10.166376 | 10.783547 | 10.160173 |
0705.1645 | Domenico Orlando | R. Dijkgraaf, D. Orlando, S. Reffert | Dimer Models, Free Fermions and Super Quantum Mechanics | minor corrections, reference added | null | null | null | hep-th math.QA | null | This note relates topics in statistical mechanics, graph theory and
combinatorics, lattice quantum field theory, super quantum mechanics and string
theory. We give a precise relation between the dimer model on a graph embedded
on a torus and the massless free Majorana fermion living on the same lattice. A
loop expans... | [
{
"created": "Fri, 11 May 2007 11:32:32 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Nov 2007 13:29:06 GMT",
"version": "v2"
}
] | 2007-11-12 | [
[
"Dijkgraaf",
"R.",
""
],
[
"Orlando",
"D.",
""
],
[
"Reffert",
"S.",
""
]
] | This note relates topics in statistical mechanics, graph theory and combinatorics, lattice quantum field theory, super quantum mechanics and string theory. We give a precise relation between the dimer model on a graph embedded on a torus and the massless free Majorana fermion living on the same lattice. A loop expansio... | 10.160173 | 11.388125 | 11.832198 | 10.239052 | 10.89332 | 10.875787 | 11.430913 | 10.458951 | 9.915831 | 13.690245 | 10.1174 | 9.363151 | 10.296051 | 9.674931 | 9.454943 | 9.55431 | 9.654251 | 9.299223 | 9.385368 | 10.300685 | 9.47284 |
2204.13636 | Yuan Sun | Song He, Hao Ouyang, Yuan Sun | Note on $T\bar{T}$ deformed matrix models and JT supergravity duals | 27 pages. A replacement of v1 whose PDF cannot be opened. References
added | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this work we calculate the partition functions of $\mathcal{N}=1$ type 0A
and 0B JT supergravity (SJT) on 2D surfaces of arbitrary genus with multiple
finite cut-off boundaries, based on the $T\bar{T}$ deformed super-Schwarzian
theories. In terms of SJT/matrix model duality, we compute the corresponding
correlatio... | [
{
"created": "Thu, 28 Apr 2022 16:54:21 GMT",
"version": "v1"
},
{
"created": "Thu, 5 May 2022 14:32:02 GMT",
"version": "v2"
}
] | 2022-05-06 | [
[
"He",
"Song",
""
],
[
"Ouyang",
"Hao",
""
],
[
"Sun",
"Yuan",
""
]
] | In this work we calculate the partition functions of $\mathcal{N}=1$ type 0A and 0B JT supergravity (SJT) on 2D surfaces of arbitrary genus with multiple finite cut-off boundaries, based on the $T\bar{T}$ deformed super-Schwarzian theories. In terms of SJT/matrix model duality, we compute the corresponding correlation ... | 7.283355 | 6.726117 | 7.613538 | 5.811659 | 6.874918 | 6.535728 | 6.612738 | 6.451601 | 6.382167 | 9.184808 | 6.33654 | 6.958416 | 6.731238 | 6.456153 | 6.334416 | 6.574678 | 6.462113 | 6.537189 | 6.52361 | 6.674402 | 6.461682 |
1005.4607 | Tetsuji Kimura | Tetsuji Kimura | Non-supersymmetric Extremal RN-AdS Black Holes in N=2 Gauged
Supergravity | 23 pages, accepted version in JHEP | JHEP 1009:061,2010 | 10.1007/JHEP09(2010)061 | KEK-TH-1367 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate extremal Reissner-Nordstrom-AdS black holes in
four-dimensional N=2 abelian gauged supergravity. We find a new attractor
equation which is not reduced to the one in the asymptotically flat spacetime.
Focusing on so-called the T^3-model with a single neutral vector multiplet, we
obtain non-supersymmetri... | [
{
"created": "Tue, 25 May 2010 15:33:19 GMT",
"version": "v1"
},
{
"created": "Sat, 29 May 2010 07:12:46 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Sep 2010 19:15:12 GMT",
"version": "v3"
}
] | 2014-11-21 | [
[
"Kimura",
"Tetsuji",
""
]
] | We investigate extremal Reissner-Nordstrom-AdS black holes in four-dimensional N=2 abelian gauged supergravity. We find a new attractor equation which is not reduced to the one in the asymptotically flat spacetime. Focusing on so-called the T^3-model with a single neutral vector multiplet, we obtain non-supersymmetric ... | 6.399307 | 6.268592 | 7.427604 | 5.732039 | 6.073045 | 6.2447 | 6.059093 | 6.40046 | 5.838713 | 7.92943 | 5.756597 | 5.751426 | 6.510792 | 5.651033 | 5.923869 | 6.048862 | 5.90745 | 5.801246 | 5.860248 | 6.363513 | 5.784156 |
0906.1258 | Juan Mateos Guilarte | A. Alonso Izquierdo, M. A. Gonzalez Leon, J. Mateos Guilarte, M. J.
Senosiain | On the semiclassical mass of ${\mathbb S}^2$-kinks | RevTex file, 15 pages, 2 figures. Version to appear in Journal of
Physics A | null | 10.1088/1751-8113/42/38/385403 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One-loop mass shifts to the classical masses of stable kinks arising in a
massive non-linear ${\mathbb S}^2$-sigma model are computed. Ultraviolet
divergences are controlled using the heat kernel/zeta function regularization
method. A comparison between the results achieved from exact and
high-temperature asymptotic ... | [
{
"created": "Sat, 6 Jun 2009 09:42:18 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Aug 2009 07:14:03 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"Izquierdo",
"A. Alonso",
""
],
[
"Leon",
"M. A. Gonzalez",
""
],
[
"Guilarte",
"J. Mateos",
""
],
[
"Senosiain",
"M. J.",
""
]
] | One-loop mass shifts to the classical masses of stable kinks arising in a massive non-linear ${\mathbb S}^2$-sigma model are computed. Ultraviolet divergences are controlled using the heat kernel/zeta function regularization method. A comparison between the results achieved from exact and high-temperature asymptotic he... | 19.612646 | 12.585935 | 15.900298 | 13.172546 | 14.040143 | 12.342101 | 12.509686 | 12.206713 | 12.28266 | 15.250539 | 13.533775 | 14.627667 | 16.159935 | 14.524392 | 14.865151 | 15.08611 | 14.437523 | 14.629171 | 14.814512 | 17.732553 | 16.062075 |
1611.08601 | Alexandre Belin | Alexandre Belin, Ben Freivogel, Robert A. Jefferson, Laurens Kabir | Sub-AdS Scale Locality in AdS$_3$/CFT$_2$ | 19 pages | null | 10.1007/JHEP04(2017)147 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate sub-AdS scale locality in a weakly coupled toy model of the
AdS$_3$/CFT$_2$ correspondence. We find that this simple model has the correct
density of states at low and high energies to be dual to Einstein gravity
coupled to matter in AdS$_3$. Bulk correlation functions also have the correct
behavior at... | [
{
"created": "Fri, 25 Nov 2016 21:00:01 GMT",
"version": "v1"
}
] | 2017-05-24 | [
[
"Belin",
"Alexandre",
""
],
[
"Freivogel",
"Ben",
""
],
[
"Jefferson",
"Robert A.",
""
],
[
"Kabir",
"Laurens",
""
]
] | We investigate sub-AdS scale locality in a weakly coupled toy model of the AdS$_3$/CFT$_2$ correspondence. We find that this simple model has the correct density of states at low and high energies to be dual to Einstein gravity coupled to matter in AdS$_3$. Bulk correlation functions also have the correct behavior at l... | 6.653273 | 5.782202 | 7.320117 | 6.191608 | 5.914086 | 5.737259 | 5.929584 | 5.784201 | 6.053844 | 7.186554 | 5.98073 | 6.305604 | 6.743878 | 6.146302 | 6.497191 | 6.275237 | 6.292158 | 6.339458 | 6.440329 | 6.591027 | 6.095426 |
1305.1633 | Kenneth Intriligator | Kenneth Intriligator and Nathan Seiberg | Aspects of 3d N=2 Chern-Simons-Matter Theories | 76 pages, 1 figure. v2: added references | null | 10.1007/JHEP07(2013)079 | UCSD-PTH-12-17 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We comment on various aspects of the the dynamics of 3d N=2 Chern-Simons
gauge theories and their possible phases. Depending on the matter content, real
masses and FI parameters, there can be non-compact Higgs or Coulomb branches,
compact Higgs or Coulomb branches, and isolated vacua. We compute the Witten
index of t... | [
{
"created": "Tue, 7 May 2013 20:01:50 GMT",
"version": "v1"
},
{
"created": "Mon, 20 May 2013 20:50:00 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"Intriligator",
"Kenneth",
""
],
[
"Seiberg",
"Nathan",
""
]
] | We comment on various aspects of the the dynamics of 3d N=2 Chern-Simons gauge theories and their possible phases. Depending on the matter content, real masses and FI parameters, there can be non-compact Higgs or Coulomb branches, compact Higgs or Coulomb branches, and isolated vacua. We compute the Witten index of the... | 7.926593 | 8.270377 | 9.954354 | 7.435214 | 8.170828 | 7.443457 | 7.643483 | 7.640706 | 7.529649 | 9.44598 | 7.699548 | 7.826406 | 8.341233 | 7.656271 | 7.554464 | 7.830972 | 7.645582 | 7.589691 | 7.634932 | 8.471932 | 7.576321 |
1601.04708 | Diego Trancanelli | Alberto Faraggi, Leopoldo A. Pando Zayas, Guillermo A. Silva, Diego
Trancanelli | Toward precision holography with supersymmetric Wilson loops | 5 pages; v2: 43 pages, long version fixing a mistake and altering the
conclusions | JHEP 1604:053,2016 | 10.1007/JHEP04(2016)053 | MCTP-16-03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider certain 1/4 BPS Wilson loop operators in SU(N) ${\cal N}=4$
supersymmetric Yang-Mills theory, whose expectation value can be computed
exactly via supersymmetric localization. Holographically, these operators are
mapped to fundamental strings in AdS5 x S5. The string on-shell action
reproduces the large N ... | [
{
"created": "Mon, 18 Jan 2016 21:00:04 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Feb 2016 20:25:00 GMT",
"version": "v2"
}
] | 2016-04-12 | [
[
"Faraggi",
"Alberto",
""
],
[
"Zayas",
"Leopoldo A. Pando",
""
],
[
"Silva",
"Guillermo A.",
""
],
[
"Trancanelli",
"Diego",
""
]
] | We consider certain 1/4 BPS Wilson loop operators in SU(N) ${\cal N}=4$ supersymmetric Yang-Mills theory, whose expectation value can be computed exactly via supersymmetric localization. Holographically, these operators are mapped to fundamental strings in AdS5 x S5. The string on-shell action reproduces the large N an... | 5.38717 | 5.686173 | 6.423851 | 5.773521 | 5.727659 | 5.954918 | 5.979239 | 5.401949 | 5.430684 | 6.669485 | 5.481239 | 5.55239 | 5.824188 | 5.501949 | 5.411462 | 5.666686 | 5.619327 | 5.433675 | 5.45249 | 5.666839 | 5.441205 |
1707.04816 | Allen Stern | A. Pinzul and A. Stern | Non-commutative $AdS_2/CFT_1$ duality: the case of massless scalar
fields | 25 pages | Phys. Rev. D 96, 066019 (2017) | 10.1103/PhysRevD.96.066019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how to construct correlators for the $CFT_1$ which is dual to
non-commutative $AdS_2$ ($ncAdS_2$). We do it explicitly for the example of the
massless scalar field on Euclidean $ncAdS_2$. $ncAdS_2$ is the quantization of
$AdS_2$ that preserves all the isometries. It is described in terms of the
unitary irredu... | [
{
"created": "Sun, 16 Jul 2017 04:17:43 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Aug 2017 18:11:02 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Jan 2018 20:25:51 GMT",
"version": "v3"
}
] | 2018-01-22 | [
[
"Pinzul",
"A.",
""
],
[
"Stern",
"A.",
""
]
] | We show how to construct correlators for the $CFT_1$ which is dual to non-commutative $AdS_2$ ($ncAdS_2$). We do it explicitly for the example of the massless scalar field on Euclidean $ncAdS_2$. $ncAdS_2$ is the quantization of $AdS_2$ that preserves all the isometries. It is described in terms of the unitary irreduci... | 5.19467 | 4.866989 | 5.652632 | 4.872293 | 5.164365 | 5.23728 | 5.184243 | 4.843024 | 5.012464 | 5.365573 | 4.955096 | 4.874609 | 5.187218 | 4.942918 | 5.015848 | 5.005591 | 4.949592 | 4.880015 | 4.925479 | 5.206379 | 4.836471 |
2212.09139 | Konstantinos Rigatos | Konstantinos C. Rigatos | Spin-$2$ operators in AdS$_2$/CFT$_1$ | v1: 22 pages, 1 brane scan, 1 quiver diagram, v2: added references,
v3: added references and discussion, v4: published version | null | 10.1007/JHEP06(2023)026 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study spin-2 fluctuations around an infinite family of warped backgrounds
of the form $\text{AdS}_2 \times \text{S}^2 \times \text{T}^4 \times \text{S}^1
\times \mathcal{I}_{\rho}$ in the type IIB theory, which possesses
$\mathcal{N}=4$ supersymmetry. We find that there exists a special set of
solutions which is i... | [
{
"created": "Sun, 18 Dec 2022 18:03:45 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Dec 2022 09:48:30 GMT",
"version": "v2"
},
{
"created": "Sat, 18 Mar 2023 04:48:25 GMT",
"version": "v3"
},
{
"created": "Thu, 8 Jun 2023 00:20:34 GMT",
"version": "v4"
}
] | 2023-06-09 | [
[
"Rigatos",
"Konstantinos C.",
""
]
] | We study spin-2 fluctuations around an infinite family of warped backgrounds of the form $\text{AdS}_2 \times \text{S}^2 \times \text{T}^4 \times \text{S}^1 \times \mathcal{I}_{\rho}$ in the type IIB theory, which possesses $\mathcal{N}=4$ supersymmetry. We find that there exists a special set of solutions which is ind... | 5.291107 | 4.510405 | 5.521479 | 4.800054 | 5.0425 | 4.963753 | 5.138747 | 4.908584 | 4.829271 | 5.867545 | 4.635919 | 4.923862 | 5.322899 | 4.906502 | 5.053084 | 5.065555 | 4.865728 | 4.981859 | 5.006699 | 5.450289 | 4.900952 |
1909.10550 | Seyed Morteza Hosseini | Seyed Morteza Hosseini, Kiril Hristov, Alberto Zaffaroni | Gluing gravitational blocks for AdS black holes | 44 pages, v2: Published version, (6.17) corrected; v3: typos
corrected | JHEP12(2019)168 | 10.1007/JHEP12(2019)168 | IPMU19-0132 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a unifying entropy functional and an extremization principle for
black holes and black strings in AdS$_4\times S^7$ and AdS$_5\times S^5$ with
arbitrary rotation and generic electric and magnetic charges. This is done by
gluing gravitational blocks, basic building blocks that are directly inspired
by the h... | [
{
"created": "Mon, 23 Sep 2019 18:14:42 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Jan 2020 14:42:26 GMT",
"version": "v2"
},
{
"created": "Sat, 22 May 2021 16:25:43 GMT",
"version": "v3"
}
] | 2021-05-25 | [
[
"Hosseini",
"Seyed Morteza",
""
],
[
"Hristov",
"Kiril",
""
],
[
"Zaffaroni",
"Alberto",
""
]
] | We provide a unifying entropy functional and an extremization principle for black holes and black strings in AdS$_4\times S^7$ and AdS$_5\times S^5$ with arbitrary rotation and generic electric and magnetic charges. This is done by gluing gravitational blocks, basic building blocks that are directly inspired by the hol... | 5.783777 | 5.156265 | 6.06993 | 5.426132 | 4.943953 | 5.102593 | 5.311973 | 4.958661 | 5.27281 | 6.096323 | 5.191039 | 5.186181 | 5.799108 | 5.483847 | 5.455716 | 5.164813 | 5.358224 | 5.278528 | 5.556741 | 5.665744 | 5.36562 |
1409.2949 | KaiXi Feng | Kaixi Feng and Taotao Qiu | Curvaton with Nonminimal Derivative Coupling to Gravity II: Full
Perturbation Analysis | Published in Phys.Rev. D90 (2014) 123508 | Phys. Rev. D 90, 123508 (2014) | 10.1103/PhysRevD.90.123508 | null | hep-th astro-ph.HE gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In our previous work \cite{Feng:2013pba}, we have shown a curvaton model
where the curvaton has a nonminimal derivative coupling to gravity. Such a
coupling could bring us scale-invariance of the perturbations for wide range
constant values of the equation-of-state of the cosmic background at the early
time. In this ... | [
{
"created": "Wed, 10 Sep 2014 03:47:47 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Sep 2014 15:56:46 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Sep 2014 14:39:01 GMT",
"version": "v3"
},
{
"created": "Wed, 10 Dec 2014 08:15:08 GMT",
"version": "v4"
}
] | 2014-12-17 | [
[
"Feng",
"Kaixi",
""
],
[
"Qiu",
"Taotao",
""
]
] | In our previous work \cite{Feng:2013pba}, we have shown a curvaton model where the curvaton has a nonminimal derivative coupling to gravity. Such a coupling could bring us scale-invariance of the perturbations for wide range constant values of the equation-of-state of the cosmic background at the early time. In this pa... | 7.506433 | 8.286505 | 7.321716 | 7.273858 | 8.318414 | 8.179856 | 7.904027 | 7.49908 | 7.408713 | 7.829628 | 7.473701 | 7.328411 | 7.354681 | 7.156137 | 7.367724 | 7.229272 | 7.346718 | 7.174044 | 7.188357 | 7.17007 | 7.091824 |
1010.0700 | Massimo Siani | Massimo Siani | Holographic Superconductors and Higher Curvature Corrections | 16 pages, 6 figures; v2: published version plus one reference added | JHEP 1012:035,2010 | 10.1007/JHEP12(2010)035 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a fully backreacted holographic model of a four-dimensional
superconductor by including a higher curvature interaction in the bulk action.
We study how the critical temperature and the field theory condensate vary in
this model and conclude that positive higher curvature couplings make the
condensation harde... | [
{
"created": "Mon, 4 Oct 2010 20:35:51 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Nov 2011 10:09:20 GMT",
"version": "v2"
}
] | 2015-03-17 | [
[
"Siani",
"Massimo",
""
]
] | We study a fully backreacted holographic model of a four-dimensional superconductor by including a higher curvature interaction in the bulk action. We study how the critical temperature and the field theory condensate vary in this model and conclude that positive higher curvature couplings make the condensation harder.... | 12.014099 | 9.478378 | 11.088162 | 8.733796 | 8.722887 | 8.487044 | 9.715807 | 9.694013 | 8.620329 | 12.463033 | 8.952112 | 9.995938 | 10.997892 | 10.258716 | 9.611572 | 9.707972 | 9.609535 | 9.620677 | 9.534917 | 10.85593 | 10.077384 |
hep-th/9903041 | Piet Termonia | G. Dall'Agata, D. Fabbri, C. Fraser, P. Fre', P. Termonia, M.
Trigiante | The singleton action action from the supermembrane | 9 pages, 1 figure. Talk given by P. Termonia at the TMR meeting of
the project "Quantum Aspects of Gauge Theories, Supersymmetry and
Unification", Corfu '98, TMR contract ERBFMRX-CT96-0045 | null | 10.1007/BFb0104253 | DDFT 99/12 | hep-th | null | We derive the free Osp(8|4) singleton action by sending the M2brane to the
Minkowski boundary of an AdS_4x{\cal M}_7 background. We do this by means of
the solvable Lie algebra parametrization of the coset space. We also give some
comments on singleton actions from membranes on AdS_4xG/H backgrounds.
| [
{
"created": "Thu, 4 Mar 1999 10:45:58 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Dall'Agata",
"G.",
""
],
[
"Fabbri",
"D.",
""
],
[
"Fraser",
"C.",
""
],
[
"Fre'",
"P.",
""
],
[
"Termonia",
"P.",
""
],
[
"Trigiante",
"M.",
""
]
] | We derive the free Osp(8|4) singleton action by sending the M2brane to the Minkowski boundary of an AdS_4x{\cal M}_7 background. We do this by means of the solvable Lie algebra parametrization of the coset space. We also give some comments on singleton actions from membranes on AdS_4xG/H backgrounds. | 12.367462 | 10.645546 | 14.889311 | 10.491059 | 9.973418 | 11.172208 | 11.216178 | 11.024817 | 11.694307 | 17.223169 | 11.02584 | 11.746507 | 12.712559 | 11.275737 | 11.146355 | 11.091658 | 10.964317 | 11.050138 | 11.525866 | 13.098661 | 11.566213 |
2311.05441 | Yi-Nan Wang | Jisheng Mu, Yi-Nan Wang, Hao N. Zhang | 5d SCFTs from Isolated Complete Intersection Singularities | v2, 87 pages | null | null | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we explore the zoo of 5d superconformal field theories (SCFTs)
constructed from M-theory on Isolated Complete Intersection Singularities
(ICIS). We systematically investigate the crepant resolution of such
singularities, and obtain a classification of rank $\leqslant 10$ models with a
smooth crepant re... | [
{
"created": "Thu, 9 Nov 2023 15:26:50 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Nov 2023 13:16:13 GMT",
"version": "v2"
}
] | 2023-11-29 | [
[
"Mu",
"Jisheng",
""
],
[
"Wang",
"Yi-Nan",
""
],
[
"Zhang",
"Hao N.",
""
]
] | In this paper, we explore the zoo of 5d superconformal field theories (SCFTs) constructed from M-theory on Isolated Complete Intersection Singularities (ICIS). We systematically investigate the crepant resolution of such singularities, and obtain a classification of rank $\leqslant 10$ models with a smooth crepant reso... | 7.238785 | 6.942132 | 8.689231 | 6.777851 | 6.493023 | 6.9038 | 7.227258 | 6.564663 | 6.570673 | 8.208459 | 6.434669 | 6.588879 | 7.013593 | 6.655143 | 6.450279 | 6.547134 | 6.507218 | 6.715297 | 6.662717 | 7.118724 | 6.6863 |
hep-th/9602037 | J. C. Gallardo | Jose F. Cari\~nena and J. Nasarre | Presymplectic Geometry and Fermat's Principle for anisotropic media | LaTeX file, no figures. To appear in J. Phys. A: Math. and Gen | J.Phys.A29:1695-1702,1996 | 10.1088/0305-4470/29/8/017 | DFTUZ 96/06 | hep-th dg-ga math.DG | null | The tools of presymplectic geometry are used to study light rays trajectories
in anisotropic media.
| [
{
"created": "Thu, 8 Feb 1996 09:40:12 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cariñena",
"Jose F.",
""
],
[
"Nasarre",
"J.",
""
]
] | The tools of presymplectic geometry are used to study light rays trajectories in anisotropic media. | 25.310009 | 26.325258 | 18.084497 | 16.870596 | 17.624729 | 18.165821 | 25.665678 | 19.887423 | 22.068674 | 20.03196 | 21.061319 | 23.197222 | 22.199829 | 21.350908 | 21.212997 | 21.90048 | 21.95731 | 22.177784 | 24.040323 | 25.742638 | 22.095387 |
0712.3779 | Jean-Luc Lehners | Jean-Luc Lehners, Paul J. Steinhardt | Non-Gaussian Density Fluctuations from Entropically Generated Curvature
Perturbations in Ekpyrotic Models | 5 pages, 2 figures. Sign error corrected and results generalized | Phys.Rev.D77:063533,2008; Erratum-ibid.D79:129903,2009 | 10.1103/PhysRevD.77.063533 10.1103/PhysRevD.79.129903 | null | hep-th astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the non-gaussian density perturbations generated in
ekpyrotic/cyclic models based on heterotic M-theory. In this picture, two
scalar fields produce nearly scale-invariant entropic perturbations during an
ekpyrotic phase that are converted into curvature modes {\it after the
ekpyrotic phase is complete} and... | [
{
"created": "Fri, 21 Dec 2007 19:27:00 GMT",
"version": "v1"
},
{
"created": "Sun, 24 Feb 2008 16:06:05 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Jun 2009 15:14:49 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Lehners",
"Jean-Luc",
""
],
[
"Steinhardt",
"Paul J.",
""
]
] | We analyze the non-gaussian density perturbations generated in ekpyrotic/cyclic models based on heterotic M-theory. In this picture, two scalar fields produce nearly scale-invariant entropic perturbations during an ekpyrotic phase that are converted into curvature modes {\it after the ekpyrotic phase is complete} and j... | 6.751742 | 7.02642 | 6.957184 | 6.527557 | 7.113145 | 6.684583 | 7.226114 | 6.770107 | 6.637097 | 7.614299 | 6.513505 | 6.527569 | 6.554843 | 6.421283 | 6.597331 | 6.885195 | 6.6083 | 6.602331 | 6.694862 | 6.455305 | 6.45196 |
hep-th/9808027 | A. J. da Silva | Ashok Das and A. J. da Silva | Exact Effective Action for (1+1 Dimensional) Fermions in an Abelian
Background at Finite Temperature | A few clarifying remarks added;21 pages | Phys. Rev. D 59, 105011 (1999) | 10.1103/PhysRevD.59.105011 | null | hep-th | null | In an effort to further understand the structure of effective actions for
fermions in an external gauge background at finite temperature, we study the
example of 1+1 dimensional fermions interacting with an arbitrary Abelian gauge
field. We evaluate the effective action exactly at finite temperature. This
effective a... | [
{
"created": "Wed, 5 Aug 1998 18:35:38 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Aug 1998 18:06:30 GMT",
"version": "v2"
},
{
"created": "Mon, 10 Aug 1998 18:58:52 GMT",
"version": "v3"
}
] | 2016-08-25 | [
[
"Das",
"Ashok",
""
],
[
"da Silva",
"A. J.",
""
]
] | In an effort to further understand the structure of effective actions for fermions in an external gauge background at finite temperature, we study the example of 1+1 dimensional fermions interacting with an arbitrary Abelian gauge field. We evaluate the effective action exactly at finite temperature. This effective act... | 9.307305 | 8.228073 | 9.7883 | 8.484602 | 8.297141 | 8.52005 | 8.632664 | 8.180597 | 8.40064 | 9.187642 | 8.269684 | 8.004805 | 9.097034 | 8.566954 | 8.366076 | 8.44631 | 8.087192 | 8.532588 | 8.348195 | 8.582387 | 8.567307 |
2103.05023 | Mahsa Lezgi | Mahsa Lezgi, Mohammad Ali-Akbari | Complexity and uncomplexity during energy injection | null | Phys. Rev. D 103, 126024 (2021) | 10.1103/PhysRevD.103.126024 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a strongly coupled field theory with a critical point and nonzero
chemical potential at finite temperature, which is dual to an asymptotically
AdS charged black hole. We study the evolution of the rescaled holographic
subregion complexity near and far from the critical point. We explain two
distinct conce... | [
{
"created": "Mon, 8 Mar 2021 19:11:01 GMT",
"version": "v1"
}
] | 2021-06-30 | [
[
"Lezgi",
"Mahsa",
""
],
[
"Ali-Akbari",
"Mohammad",
""
]
] | We consider a strongly coupled field theory with a critical point and nonzero chemical potential at finite temperature, which is dual to an asymptotically AdS charged black hole. We study the evolution of the rescaled holographic subregion complexity near and far from the critical point. We explain two distinct concept... | 11.424409 | 10.917923 | 12.841618 | 11.019312 | 12.098672 | 11.581098 | 11.942304 | 11.304751 | 11.045292 | 13.010408 | 10.763912 | 10.983323 | 11.336562 | 10.772541 | 11.054565 | 10.989751 | 11.088717 | 10.749939 | 10.935911 | 11.816814 | 10.918406 |
2305.19438 | Gustavo Joaquin Turiaci | Gustavo J. Turiaci and Edward Witten | $N=2$ JT Supergravity and Matrix Models | 125 pages. v2: ref added and typos corrected. v3: two tables added in
the introduction summarizing the properties of JT supergravities and for N=2
their random matrix ensembles. v4: typos corrected in section 5.5 | null | null | null | hep-th math-ph math.AG math.MP math.SG | http://creativecommons.org/licenses/by/4.0/ | Generalizing previous results for $N=0$ and $N=1$, we analyze $N=2$ JT
supergravity on asymptotically AdS${}_2$ spaces with arbitrary topology and
show that this theory of gravity is dual, in a holographic sense, to a certain
random matrix ensemble in which supermultiplets of different $R$-charge are
statistically in... | [
{
"created": "Tue, 30 May 2023 22:14:20 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jun 2023 16:21:26 GMT",
"version": "v2"
},
{
"created": "Sun, 22 Oct 2023 19:04:12 GMT",
"version": "v3"
},
{
"created": "Wed, 22 Nov 2023 22:32:58 GMT",
"version": "v4"
}
] | 2023-11-27 | [
[
"Turiaci",
"Gustavo J.",
""
],
[
"Witten",
"Edward",
""
]
] | Generalizing previous results for $N=0$ and $N=1$, we analyze $N=2$ JT supergravity on asymptotically AdS${}_2$ spaces with arbitrary topology and show that this theory of gravity is dual, in a holographic sense, to a certain random matrix ensemble in which supermultiplets of different $R$-charge are statistically inde... | 7.627721 | 6.879491 | 8.328089 | 6.644319 | 6.495266 | 6.279418 | 7.199146 | 6.747027 | 6.522643 | 9.540567 | 6.67455 | 6.7921 | 7.036462 | 6.567369 | 6.554029 | 6.760138 | 6.507365 | 6.683109 | 6.436536 | 6.894452 | 6.504322 |
1408.4511 | Yu-Xiao Liu | Yuan Zhong, Yu-Xiao Liu | $K$-field kinks: stability, exact solutions and new features | 14 pages, 3 figures | JHEP 10 (2014) 041 | 10.1007/JHEP10(2014)041 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a class of noncanonical real scalar field models in
$(1+1)$-dimensional flat space-time. We first derive the general criterion for
the classical linear stability of an arbitrary static soliton solution of these
models. Then we construct first-order formalisms for some typical models and
derive the correspond... | [
{
"created": "Wed, 20 Aug 2014 02:54:49 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Oct 2014 02:17:22 GMT",
"version": "v2"
}
] | 2014-10-16 | [
[
"Zhong",
"Yuan",
""
],
[
"Liu",
"Yu-Xiao",
""
]
] | We study a class of noncanonical real scalar field models in $(1+1)$-dimensional flat space-time. We first derive the general criterion for the classical linear stability of an arbitrary static soliton solution of these models. Then we construct first-order formalisms for some typical models and derive the correspondin... | 10.535257 | 9.685153 | 10.226814 | 9.043725 | 9.774549 | 8.893376 | 10.030873 | 8.8328 | 8.854261 | 10.774883 | 8.654571 | 9.306223 | 10.195665 | 9.218279 | 8.969759 | 9.124723 | 9.542528 | 9.266829 | 9.174534 | 9.381941 | 8.954682 |
1201.3964 | Yong-Wan Kim | Yun Soo Myung, Yong-Wan Kim, Young-Jai Park | Spin-3 quasinormal modes of BTZ black hole | 16 pages, title changed, references added, version to appear in PRD | null | 10.1103/PhysRevD.85.084007 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the operator approach, we obtain quasinormal modes (QNMs) of BTZ black
hole in spin-3 topologically massive gravity by solving the first-order
equation of motion with the transverse-traceless condition. We find that these
are different from those obtained when solving the second-order differential
equation for ... | [
{
"created": "Thu, 19 Jan 2012 03:14:48 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Mar 2012 04:51:51 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Myung",
"Yun Soo",
""
],
[
"Kim",
"Yong-Wan",
""
],
[
"Park",
"Young-Jai",
""
]
] | Using the operator approach, we obtain quasinormal modes (QNMs) of BTZ black hole in spin-3 topologically massive gravity by solving the first-order equation of motion with the transverse-traceless condition. We find that these are different from those obtained when solving the second-order differential equation for th... | 11.622067 | 11.341044 | 11.024734 | 10.888545 | 10.494653 | 10.772761 | 11.318011 | 10.414209 | 10.616155 | 12.643277 | 10.280755 | 10.475801 | 10.795189 | 10.606918 | 10.612149 | 10.793599 | 10.971632 | 10.868231 | 10.510698 | 11.292891 | 10.095943 |
hep-th/0208065 | Elcio Abdalla | E. Abdalla, K. H. C. Castello-Branco and A. Lima-Santos | Support of dS/CFT correspondence from space-time perturbations | Modified version, appearing in Phys. Rev. D66 (2002) 104018 | Phys.Rev. D66 (2002) 104018 | 10.1103/PhysRevD.66.104018 | null | hep-th | null | We analyse the spectrum of perturbations of the de Sitter space on the one
hand, while on the other hand we compute the location of the poles in the
Conformal Field Theory (CFT) propagator at the border. The coincidence is
striking, supporting a dS/CFT correspondence. We show that the spectrum of
thermal excitations ... | [
{
"created": "Thu, 8 Aug 2002 18:32:29 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Nov 2002 12:53:26 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Abdalla",
"E.",
""
],
[
"Castello-Branco",
"K. H. C.",
""
],
[
"Lima-Santos",
"A.",
""
]
] | We analyse the spectrum of perturbations of the de Sitter space on the one hand, while on the other hand we compute the location of the poles in the Conformal Field Theory (CFT) propagator at the border. The coincidence is striking, supporting a dS/CFT correspondence. We show that the spectrum of thermal excitations of... | 9.038268 | 7.886919 | 8.622412 | 7.353216 | 8.290998 | 8.663912 | 7.967175 | 7.894648 | 7.533307 | 9.026507 | 7.415361 | 8.072178 | 8.169417 | 7.973504 | 7.86773 | 7.791403 | 8.204265 | 7.724045 | 7.853893 | 8.493098 | 7.642356 |
1612.00470 | Yan Liu | Yan Liu, Francisco Pena-Benitez | Spatially modulated instabilities of holographic gauge-gravitational
anomaly | 24 pages, 8 figures. v2: refs added, minor improvements, a new
appendix added | JHEP 1705 (2017) 111 | 10.1007/JHEP05(2017)111 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We performed a study of the perturbative instabilities in
Einstein-Maxwell-Chern-Simons theory with a gravitational Chern-Simons term,
which is dual to a strongly coupled field theory with both chiral and mixed
gauge-gravitational anomaly. With an analysis of the fluctuations in the near
horizon regime at zero temper... | [
{
"created": "Thu, 1 Dec 2016 21:10:40 GMT",
"version": "v1"
},
{
"created": "Fri, 26 May 2017 13:01:15 GMT",
"version": "v2"
}
] | 2017-08-23 | [
[
"Liu",
"Yan",
""
],
[
"Pena-Benitez",
"Francisco",
""
]
] | We performed a study of the perturbative instabilities in Einstein-Maxwell-Chern-Simons theory with a gravitational Chern-Simons term, which is dual to a strongly coupled field theory with both chiral and mixed gauge-gravitational anomaly. With an analysis of the fluctuations in the near horizon regime at zero temperat... | 8.609973 | 8.503856 | 9.422947 | 8.232445 | 8.227502 | 7.93799 | 8.445596 | 7.77563 | 7.766799 | 8.958696 | 8.245523 | 8.301872 | 8.310093 | 8.286616 | 8.014626 | 8.144614 | 8.306293 | 8.273101 | 8.230437 | 8.72656 | 8.194228 |
1311.2586 | Adam Brown | Adam R. Brown, Alex Dahlen, and Ali Masoumi | Compactifying de Sitter Naturally Selects a Small Cosmological Constant | 11 pages, 5 figures | Phys. Rev. D 90, 124048 (2014) | 10.1103/PhysRevD.90.124048 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study compactifications of $D$-dimensional de Sitter space with a $q$-form
flux down to $D-Nq$ dimensions. We show that for $(N-1)(q-1)\geq 2$ there are
double-exponentially or even infinitely many compact de Sitter vacua, and that
their effective cosmological constants accumulate at zero. This population
explosio... | [
{
"created": "Mon, 11 Nov 2013 21:00:01 GMT",
"version": "v1"
},
{
"created": "Sat, 29 Nov 2014 04:00:18 GMT",
"version": "v2"
}
] | 2014-12-24 | [
[
"Brown",
"Adam R.",
""
],
[
"Dahlen",
"Alex",
""
],
[
"Masoumi",
"Ali",
""
]
] | We study compactifications of $D$-dimensional de Sitter space with a $q$-form flux down to $D-Nq$ dimensions. We show that for $(N-1)(q-1)\geq 2$ there are double-exponentially or even infinitely many compact de Sitter vacua, and that their effective cosmological constants accumulate at zero. This population explosion ... | 12.853592 | 12.040081 | 13.238976 | 10.816209 | 11.723499 | 12.074403 | 11.345826 | 11.19609 | 11.436031 | 14.534279 | 11.27239 | 11.491647 | 12.184121 | 11.349471 | 12.043797 | 11.380116 | 11.784904 | 11.028601 | 11.532488 | 12.134585 | 10.861574 |
hep-th/9403176 | Alberto Lerda | Alberto Lerda | A Field Theory Approach to the $t$-$J$ Model and the Spin-Charge
Separation | 27 pp., TeX file (1 figure on request), DFT-US 1/94 | Nucl.Phys. B428 (1994) 629-654 | 10.1016/0550-3213(94)90367-0 | null | hep-th cond-mat | null | We analyze the $t$-$J$ model using the ${\rm CP}^1$ representation for the
slave operators (holons and spinons) which is particularly suited to study the
phenomenon of the spin-charge separation in strongly correlated electron
systems. In particular, we show that for the one-dimensional $t$-$J$ model
below half-filli... | [
{
"created": "Tue, 29 Mar 1994 17:01:21 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Lerda",
"Alberto",
""
]
] | We analyze the $t$-$J$ model using the ${\rm CP}^1$ representation for the slave operators (holons and spinons) which is particularly suited to study the phenomenon of the spin-charge separation in strongly correlated electron systems. In particular, we show that for the one-dimensional $t$-$J$ model below half-filling... | 6.238255 | 6.537961 | 6.568392 | 6.128282 | 6.660222 | 6.315678 | 6.961732 | 6.095332 | 6.218261 | 7.361613 | 6.517717 | 6.089323 | 6.395946 | 6.294194 | 6.276083 | 6.225702 | 6.212015 | 6.171117 | 6.226044 | 6.311596 | 6.076152 |
2106.00366 | Charlotte Sleight | Charlotte Sleight, Massimo Taronna | On the consistency of (partially-)massless matter couplings in de Sitter
space | 45 pages + appendices, 2 figures | null | 10.1007/JHEP10(2021)156 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the consistency of the cubic couplings of a (partially-)massless
spinning field to two scalars in $\left(d+1\right)$-dimensional de Sitter
space. Gauge invariance of observables with external (partially)-massless
spinning fields translates into Ward-Takahashi identities on the boundary.
Using the Mellin-Barn... | [
{
"created": "Tue, 1 Jun 2021 10:17:44 GMT",
"version": "v1"
}
] | 2021-11-10 | [
[
"Sleight",
"Charlotte",
""
],
[
"Taronna",
"Massimo",
""
]
] | We study the consistency of the cubic couplings of a (partially-)massless spinning field to two scalars in $\left(d+1\right)$-dimensional de Sitter space. Gauge invariance of observables with external (partially)-massless spinning fields translates into Ward-Takahashi identities on the boundary. Using the Mellin-Barnes... | 6.244474 | 5.863888 | 6.321044 | 5.605649 | 6.032716 | 5.853692 | 6.139729 | 5.764916 | 5.868629 | 7.07371 | 5.584271 | 5.922573 | 6.189617 | 5.83511 | 5.900896 | 5.761224 | 5.903872 | 5.938714 | 5.891112 | 6.159484 | 5.768713 |
hep-th/9304074 | Miroslav Doresic | Stjepan Meljanac and Marijan Milekovic | On the Clebsch-Gordan coefficients for the two-parameter quantum algebra
$SU(2)_{p,q}$ | 5 pages | J.Phys. A26 (1993) 5177-5180 | 10.1088/0305-4470/26/19/045 | null | hep-th math.QA | null | We show that the Clebsch - Gordan coefficients for the $SU(2)_{p,q}$ -
algebra depend on a single parameter Q = $\sqrt{pq}$ ,contrary to the explicit
calculation of Smirnov and Wehrhahn [J.Phys.A 25 (1992),5563].
| [
{
"created": "Mon, 19 Apr 1993 15:48:51 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Meljanac",
"Stjepan",
""
],
[
"Milekovic",
"Marijan",
""
]
] | We show that the Clebsch - Gordan coefficients for the $SU(2)_{p,q}$ - algebra depend on a single parameter Q = $\sqrt{pq}$ ,contrary to the explicit calculation of Smirnov and Wehrhahn [J.Phys.A 25 (1992),5563]. | 14.163381 | 15.051727 | 12.97448 | 12.461823 | 17.328175 | 13.841846 | 14.657417 | 12.933967 | 14.993285 | 15.220367 | 13.035526 | 12.104678 | 13.188569 | 12.703504 | 11.748153 | 12.813426 | 11.626266 | 12.927252 | 12.293846 | 14.169984 | 12.285598 |
1404.4490 | Andrea Quadri | Andrea Quadri | Quantum Local Symmetry of the D-Dimensional Non-Linear Sigma Model: A
Functional Approach | 26 pages. Invited review to Symmetry | Symmetry 2014, 6(2), 234-255 | 10.3390/sym6020234 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We summarize recent progress on the symmetric subtraction of the Non-Linear
Sigma Model in $D$ dimensions, based on the validity of a certain Local
Functional Equation (LFE) encoding the invariance of the SU(2) Haar measure
under local left transformations. The deformation of the classical non-linearly
realized symme... | [
{
"created": "Thu, 17 Apr 2014 11:16:34 GMT",
"version": "v1"
}
] | 2014-04-18 | [
[
"Quadri",
"Andrea",
""
]
] | We summarize recent progress on the symmetric subtraction of the Non-Linear Sigma Model in $D$ dimensions, based on the validity of a certain Local Functional Equation (LFE) encoding the invariance of the SU(2) Haar measure under local left transformations. The deformation of the classical non-linearly realized symmetr... | 8.401108 | 7.907785 | 8.645094 | 7.868451 | 8.471364 | 8.660735 | 8.323644 | 7.985481 | 7.901163 | 9.262141 | 7.925205 | 8.18104 | 8.742125 | 8.188389 | 8.267415 | 8.280821 | 7.812346 | 8.152729 | 8.289726 | 8.911811 | 8.174045 |
2309.07335 | Franz Richard Sattler | Friederike Ihssen, Jan M. Pawlowski, Franz R. Sattler, Nicolas Wink | Towards quantitative precision for QCD at large densities | null | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | QCD at large density reveals a rich phase structure, ranging from a potential
critical end point and inhomogeneous phases or moat regimes to color
superconducting ones with competing order effects. Resolving this region in the
phase diagram of QCD with functional approaches requires a great deal of
quantitative relia... | [
{
"created": "Wed, 13 Sep 2023 22:09:13 GMT",
"version": "v1"
}
] | 2023-09-15 | [
[
"Ihssen",
"Friederike",
""
],
[
"Pawlowski",
"Jan M.",
""
],
[
"Sattler",
"Franz R.",
""
],
[
"Wink",
"Nicolas",
""
]
] | QCD at large density reveals a rich phase structure, ranging from a potential critical end point and inhomogeneous phases or moat regimes to color superconducting ones with competing order effects. Resolving this region in the phase diagram of QCD with functional approaches requires a great deal of quantitative reliabi... | 14.897342 | 17.183659 | 15.738271 | 13.911303 | 15.618635 | 16.239519 | 16.309839 | 17.514198 | 14.171238 | 16.147404 | 15.135376 | 15.018476 | 14.343125 | 14.254009 | 14.572088 | 14.966275 | 14.850816 | 14.909213 | 14.703222 | 15.377203 | 14.395202 |
1101.2306 | Ian Jack | I. Jack and C. Luckhurst | Exact beta-functions in softly-broken N=2 Chern-Simons matter theories | 11 pages; 3 figures; references added | JHEP 1103:076,2011 | 10.1007/JHEP03(2011)076 | LTH 901 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present exact results for the beta-functions for the soft-breaking
parameters in softly-broken N=2 Chern-Simons matter theories in terms of the
anomalous dimension in the unbroken theory. We check our results explicitly up
to the two loop level.
| [
{
"created": "Wed, 12 Jan 2011 09:36:07 GMT",
"version": "v1"
},
{
"created": "Fri, 21 Jan 2011 09:02:22 GMT",
"version": "v2"
}
] | 2011-03-21 | [
[
"Jack",
"I.",
""
],
[
"Luckhurst",
"C.",
""
]
] | We present exact results for the beta-functions for the soft-breaking parameters in softly-broken N=2 Chern-Simons matter theories in terms of the anomalous dimension in the unbroken theory. We check our results explicitly up to the two loop level. | 11.20172 | 8.099963 | 7.881521 | 6.696795 | 7.951828 | 7.967003 | 7.676866 | 8.008651 | 6.797513 | 7.851454 | 7.850283 | 8.251307 | 8.767521 | 8.330121 | 8.406939 | 8.583319 | 8.575953 | 8.549335 | 8.319872 | 9.04803 | 8.504949 |
1701.03110 | Kento Watanabe | Pawel Caputa, Yuya Kusuki, Tadashi Takayanagi and Kento Watanabe | Evolution of Entanglement Entropy in Orbifold CFTs | 28 pages, 7 figures. Invited contribution to the special issue of J.
Phys. A: "John Cardy's scale-invariant journey in low dimensions: a special
issue for his 70th birthday". v2: typos corrected, refs added, sec.5
improved. v3: affiliation, ref updated | J.Phys. A50 (2017) no.24, 244001 | 10.1088/1751-8121/aa6e08 | NORDITA-2017-1, YITP-17-1, IPMU17-0003 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study the time evolution of Renyi entanglement entropy for
locally excited states created by twist operators in cyclic orbifold
$(T^2)^n/\mathbb{Z}_n$ and symmetric orbifold $(T^2)^n/S_n$. We find that when
the square of its compactification radius is rational, the second Renyi entropy
approaches a un... | [
{
"created": "Wed, 11 Jan 2017 19:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Feb 2017 05:21:39 GMT",
"version": "v2"
},
{
"created": "Mon, 29 May 2017 04:52:39 GMT",
"version": "v3"
}
] | 2017-05-30 | [
[
"Caputa",
"Pawel",
""
],
[
"Kusuki",
"Yuya",
""
],
[
"Takayanagi",
"Tadashi",
""
],
[
"Watanabe",
"Kento",
""
]
] | In this work we study the time evolution of Renyi entanglement entropy for locally excited states created by twist operators in cyclic orbifold $(T^2)^n/\mathbb{Z}_n$ and symmetric orbifold $(T^2)^n/S_n$. We find that when the square of its compactification radius is rational, the second Renyi entropy approaches a univ... | 6.086802 | 5.916225 | 7.137238 | 5.561441 | 6.131469 | 5.701812 | 5.514469 | 5.789014 | 5.650196 | 7.495413 | 5.400279 | 5.879023 | 6.089519 | 5.655129 | 5.873279 | 5.755945 | 5.721161 | 5.877574 | 5.748135 | 6.285997 | 5.719244 |
hep-th/0605231 | Saharian | E. R. Bezerra de Mello, V. B. Bezerra, A. A. Saharian, A. S. Tarloyan | Vacuum polarization induced by a cylindrical boundary in the cosmic
string spacetime | 21 pages, 5 figures | Phys.Rev. D74 (2006) 025017 | 10.1103/PhysRevD.74.025017 | null | hep-th gr-qc quant-ph | null | In this paper we investigate the Wightman function, the renormalized vacuum
expectation values of the field square, and the energy-momentum tensor for a
massive scalar field with general curvature coupling inside and outside of a
cylindrical shell in the generalized spacetime of straight cosmic string. For
the genera... | [
{
"created": "Tue, 23 May 2006 17:31:59 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Bezerra",
"V. B.",
""
],
[
"Saharian",
"A. A.",
""
],
[
"Tarloyan",
"A. S.",
""
]
] | In this paper we investigate the Wightman function, the renormalized vacuum expectation values of the field square, and the energy-momentum tensor for a massive scalar field with general curvature coupling inside and outside of a cylindrical shell in the generalized spacetime of straight cosmic string. For the general ... | 7.640088 | 5.121249 | 8.589167 | 5.018681 | 5.097192 | 4.702308 | 4.61871 | 4.747184 | 4.962437 | 9.36985 | 4.655487 | 5.628812 | 7.291576 | 6.489958 | 6.121598 | 6.085409 | 6.009389 | 6.094484 | 6.286301 | 7.290649 | 5.994325 |
2305.16046 | Miao He | Miao He, Yunfeng Jiang | Integrable Crosscap States: From Spin Chains to 1D Bose Gas | 38 pages | JHEP08(2023)079 | 10.1007/JHEP08(2023)079 | null | hep-th cond-mat.stat-mech | http://creativecommons.org/licenses/by/4.0/ | The notion of a crosscap state, a special conformal boundary state first
defined in 2d CFT, was recently generalized to 2d massive integrable quantum
field theories and integrable spin chains. It has been shown that the crosscap
states preserve integrability. In this work, we first generalize this notion to
the Lieb-... | [
{
"created": "Thu, 25 May 2023 13:23:41 GMT",
"version": "v1"
}
] | 2024-01-19 | [
[
"He",
"Miao",
""
],
[
"Jiang",
"Yunfeng",
""
]
] | The notion of a crosscap state, a special conformal boundary state first defined in 2d CFT, was recently generalized to 2d massive integrable quantum field theories and integrable spin chains. It has been shown that the crosscap states preserve integrability. In this work, we first generalize this notion to the Lieb-Li... | 6.882142 | 7.058131 | 7.268351 | 6.793577 | 7.466089 | 6.756163 | 7.22603 | 6.738033 | 6.330503 | 8.3985 | 6.52636 | 6.689929 | 6.832304 | 6.650715 | 6.784389 | 6.632189 | 6.821415 | 6.79559 | 6.587653 | 6.796463 | 6.601424 |
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