id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2011.04688 | Ricardo Zambujal Ferreira | Ricardo Z. Ferreira and Carlo Heissenberg | Super-Hawking Radiation | 46 pages, 5 figures | JHEP 02 (2021) 038 | 10.1007/JHEP02(2021)038 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss modifications to the Hawking spectrum that arise when the
asymptotic states are supertranslated or superrotated. For supertranslations we
find nontrivial off-diagonal phases in the two-point correlator although the
emission spectrum is eventually left unchanged, as previously pointed out in
the literature.... | [
{
"created": "Mon, 9 Nov 2020 19:13:14 GMT",
"version": "v1"
}
] | 2021-02-09 | [
[
"Ferreira",
"Ricardo Z.",
""
],
[
"Heissenberg",
"Carlo",
""
]
] | We discuss modifications to the Hawking spectrum that arise when the asymptotic states are supertranslated or superrotated. For supertranslations we find nontrivial off-diagonal phases in the two-point correlator although the emission spectrum is eventually left unchanged, as previously pointed out in the literature. I... | 10.456445 | 10.42915 | 10.735258 | 10.169094 | 11.606129 | 10.695055 | 10.649362 | 10.782485 | 10.5043 | 11.132271 | 10.554259 | 10.396829 | 9.970939 | 10.08614 | 10.021402 | 10.183324 | 10.095114 | 10.055793 | 9.972548 | 10.401911 | 10.214996 |
hep-th/9903094 | In Yong Park | F. Gonzalez-Rey, B. Kulik, I.Y. Park | Non-renormalization of two and three Point Correlators of N=4 SYM in N=1
Superspace | 10 pages, 20 eps figures, references added | Phys.Lett. B455 (1999) 164-170 | 10.1016/S0370-2693(99)00416-5 | null | hep-th | null | Certain two and three point functions of gauge invariant primary operators of
${\cal N}=4$ SYM are computed in ${\cal N}=1$ superspace keeping all the
$\th$-components. This allows one to read off many component descendent
correlators. Our results show the only possible $g^2_{YM}$ corrections to the
free field correl... | [
{
"created": "Thu, 11 Mar 1999 02:16:07 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Mar 1999 23:46:09 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Jun 1999 22:10:48 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Gonzalez-Rey",
"F.",
""
],
[
"Kulik",
"B.",
""
],
[
"Park",
"I. Y.",
""
]
] | Certain two and three point functions of gauge invariant primary operators of ${\cal N}=4$ SYM are computed in ${\cal N}=1$ superspace keeping all the $\th$-components. This allows one to read off many component descendent correlators. Our results show the only possible $g^2_{YM}$ corrections to the free field correlat... | 8.579534 | 8.352878 | 8.32699 | 7.540339 | 7.999655 | 7.700816 | 8.01685 | 7.549138 | 8.139343 | 9.401614 | 7.935532 | 8.071219 | 8.374347 | 8.007797 | 8.033562 | 7.89083 | 8.115718 | 7.816445 | 8.036403 | 8.573315 | 8.002526 |
1408.6040 | Konstantin Zarembo | Xinyi Chen-Lin, James Gordon and Konstantin Zarembo | N=2* Super-Yang-Mills Theory at Strong Coupling | 34 pages, 9 figures; v2: the name of one author changed | null | 10.1007/JHEP11(2014)057 | NORDITA-2014-101, UUITP-10/14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The planar N=2* Super-Yang-Mills (SYM) theory is solved at large 't Hooft
coupling using localization on S(4). The solution permits detailed
investigation of the resonance phenomena responsible for quantum phase
transitions in infinite volume, and leads to quantitative predictions for the
semiclassical string dual of... | [
{
"created": "Tue, 26 Aug 2014 07:50:11 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Sep 2014 12:37:23 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Chen-Lin",
"Xinyi",
""
],
[
"Gordon",
"James",
""
],
[
"Zarembo",
"Konstantin",
""
]
] | The planar N=2* Super-Yang-Mills (SYM) theory is solved at large 't Hooft coupling using localization on S(4). The solution permits detailed investigation of the resonance phenomena responsible for quantum phase transitions in infinite volume, and leads to quantitative predictions for the semiclassical string dual of t... | 13.617002 | 11.060342 | 16.219938 | 11.001249 | 10.720017 | 10.814646 | 11.398507 | 11.379389 | 10.522807 | 17.065878 | 11.447227 | 12.10727 | 12.824617 | 11.534066 | 11.682149 | 11.670081 | 11.76872 | 12.258902 | 11.30269 | 13.520164 | 11.575383 |
hep-th/9708021 | Oleg Soloviev | Oleg A. Soloviev (Queen Mary College) | On the Schild action for D=0 and D=1 strings | 12pp, latex file. Minor corrections | Mod.Phys.Lett.A13:2415-2426,1998 | 10.1142/S0217732398002576 | QMW-PH-97-24 | hep-th | null | It is shown that the integration measure over the matrix $Y$ in the matrix
representation of the Schild action can be fixed by comparing the Schild matrix
model with the random lattice string model for D=0. It is further checked that
the given measure is consistent with the case D=1 as well.
| [
{
"created": "Tue, 5 Aug 1997 14:08:21 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 1997 11:55:16 GMT",
"version": "v2"
},
{
"created": "Tue, 12 Aug 1997 10:21:29 GMT",
"version": "v3"
},
{
"created": "Thu, 27 Nov 1997 14:22:23 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Soloviev",
"Oleg A.",
"",
"Queen Mary College"
]
] | It is shown that the integration measure over the matrix $Y$ in the matrix representation of the Schild action can be fixed by comparing the Schild matrix model with the random lattice string model for D=0. It is further checked that the given measure is consistent with the case D=1 as well. | 17.27947 | 12.190755 | 15.467381 | 11.314059 | 10.922507 | 12.683057 | 12.47003 | 11.462887 | 12.169147 | 16.620634 | 10.744556 | 11.530195 | 12.00476 | 10.797302 | 10.961592 | 11.668675 | 11.945169 | 11.287275 | 11.33426 | 12.914932 | 11.127224 |
0808.2752 | Delsate T\'erence | T. Delsate | New stable phase of non uniform black strings in ${AdS}_d$ | Results extended. 14 pages, 5 figures | JHEP 0812:085,2008 | 10.1088/1126-6708/2008/12/085 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the non uniform $AdS$ black string equations in arbitrary number
of dimension in a perturbative approach up to order 2 and in a non
perturbative. We restrict the study in the perturbative approach to the
backreacting modes, since they provide the first relevant corrections on the
thermodynamical quantitie... | [
{
"created": "Wed, 20 Aug 2008 13:28:52 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Oct 2008 15:35:13 GMT",
"version": "v2"
}
] | 2010-05-28 | [
[
"Delsate",
"T.",
""
]
] | We consider the non uniform $AdS$ black string equations in arbitrary number of dimension in a perturbative approach up to order 2 and in a non perturbative. We restrict the study in the perturbative approach to the backreacting modes, since they provide the first relevant corrections on the thermodynamical quantities ... | 11.26735 | 11.409073 | 11.719098 | 10.541579 | 12.135948 | 11.645842 | 11.396 | 11.256227 | 10.849102 | 11.74913 | 10.667288 | 10.50176 | 10.948903 | 10.689082 | 10.681875 | 10.829904 | 10.458482 | 10.540781 | 10.421659 | 10.874548 | 10.462674 |
hep-th/9312024 | Put | Wojciech Mulak | Quantum $SU(2,2)$-Harmonic Oscillator | 10 pages, LaTex file | null | 10.1016/0034-4877(93)90051-F | null | hep-th | null | The $SU(2,2)$-harmonic oscillator on the phase space ${\cal A}(2,2)=
{SU(2,2)}/{S(U(2)\times U(2))}$ is quantized using the coherent states. The
quantum Hamiltonian is the Toeplitz operator corresponding to the square of the
distance with respect to the $SU(2,2)$-invariant K\"ahler metric on the phase
space. Its spec... | [
{
"created": "Fri, 3 Dec 1993 08:50:37 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Mulak",
"Wojciech",
""
]
] | The $SU(2,2)$-harmonic oscillator on the phase space ${\cal A}(2,2)= {SU(2,2)}/{S(U(2)\times U(2))}$ is quantized using the coherent states. The quantum Hamiltonian is the Toeplitz operator corresponding to the square of the distance with respect to the $SU(2,2)$-invariant K\"ahler metric on the phase space. Its spectr... | 4.901812 | 4.623672 | 5.150198 | 4.546109 | 4.48815 | 4.563253 | 4.846459 | 4.735864 | 4.883027 | 5.355048 | 4.676564 | 4.854049 | 4.974349 | 4.5745 | 4.731845 | 4.55995 | 4.616858 | 4.566501 | 4.756463 | 4.963765 | 4.487989 |
hep-th/9503124 | Edward Witten | Edward Witten | String Theory Dynamics In Various Dimensions | 54 pages, harvmac. Some references have been added and discussion of
five-dimensional heterotic string expanded. | Nucl.Phys.B443:85-126,1995 | 10.1016/0550-3213(95)00158-O | null | hep-th | null | The strong coupling dynamics of string theories in dimension $d\geq 4$ are
studied. It is argued, among other things, that eleven-dimensional supergravity
arises as a low energy limit of the ten-dimensional Type IIA superstring, and
that a recently conjectured duality between the heterotic string and Type IIA
superst... | [
{
"created": "Mon, 20 Mar 1995 15:17:17 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Mar 1995 15:42:49 GMT",
"version": "v2"
}
] | 2010-04-07 | [
[
"Witten",
"Edward",
""
]
] | The strong coupling dynamics of string theories in dimension $d\geq 4$ are studied. It is argued, among other things, that eleven-dimensional supergravity arises as a low energy limit of the ten-dimensional Type IIA superstring, and that a recently conjectured duality between the heterotic string and Type IIA superstri... | 7.069744 | 6.119767 | 8.026464 | 6.288356 | 6.757406 | 6.859386 | 6.330718 | 6.4357 | 6.563856 | 8.034565 | 6.471798 | 6.467356 | 7.28223 | 6.662637 | 6.377937 | 6.644039 | 6.429463 | 6.361429 | 6.561171 | 7.192493 | 6.272163 |
2303.04836 | Wen-Xin Lai | Luis Apolo, Peng-Xiang Hao, Wen-Xin Lai, Wei Song | Glue-on AdS holography for $T\bar T$-deformed CFTs | 33 pages, 1 figure; v2: clarifications and references added, matches
published version | JHEP06 (2023) 117 | 10.1007/JHEP06(2023)117 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The $T\bar T$ deformation is a solvable irrelevant deformation whose
properties depend on the sign of the deformation parameter $\mu$. In
particular, $T\bar T$-deformed CFTs with $\mu<0$ have been proposed to be
holographically dual to Einstein gravity where the metric satisfies Dirichlet
boundary conditions at a fin... | [
{
"created": "Wed, 8 Mar 2023 19:13:37 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Jun 2023 14:38:58 GMT",
"version": "v2"
}
] | 2023-06-26 | [
[
"Apolo",
"Luis",
""
],
[
"Hao",
"Peng-Xiang",
""
],
[
"Lai",
"Wen-Xin",
""
],
[
"Song",
"Wei",
""
]
] | The $T\bar T$ deformation is a solvable irrelevant deformation whose properties depend on the sign of the deformation parameter $\mu$. In particular, $T\bar T$-deformed CFTs with $\mu<0$ have been proposed to be holographically dual to Einstein gravity where the metric satisfies Dirichlet boundary conditions at a finit... | 5.23907 | 4.653525 | 6.248523 | 4.368347 | 4.305447 | 4.779366 | 4.672296 | 4.209942 | 4.581655 | 6.308382 | 4.486776 | 4.635038 | 5.201355 | 4.736651 | 4.713884 | 4.617583 | 4.555361 | 4.625164 | 4.686012 | 5.244317 | 4.749903 |
0812.1975 | Alfonso V. Ramallo | Alfonso V. Ramallo, Jonathan P. Shock and Dimitrios Zoakos | Holographic flavor in N=4 gauge theories in 3d from wrapped branes | 44 pages, 6 figures | JHEP 0902:001,2009 | 10.1088/1126-6708/2009/02/001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the addition of flavor to the gravity dual of N=4 three-dimensional
gauge theories obtained by wrapping $N_c$ D4-branes on a two-cycle of a
non-compact Calabi-Yau two-fold. In this setup the flavor is introduced by
adding another set of D4-branes that are extended along the non-compact
directions of the Cala... | [
{
"created": "Wed, 10 Dec 2008 19:59:41 GMT",
"version": "v1"
}
] | 2009-02-24 | [
[
"Ramallo",
"Alfonso V.",
""
],
[
"Shock",
"Jonathan P.",
""
],
[
"Zoakos",
"Dimitrios",
""
]
] | We study the addition of flavor to the gravity dual of N=4 three-dimensional gauge theories obtained by wrapping $N_c$ D4-branes on a two-cycle of a non-compact Calabi-Yau two-fold. In this setup the flavor is introduced by adding another set of D4-branes that are extended along the non-compact directions of the Calabi... | 6.61435 | 6.057924 | 7.366301 | 6.069974 | 6.515127 | 5.993571 | 6.124097 | 5.918558 | 6.129454 | 8.509993 | 5.955291 | 5.94762 | 6.53952 | 6.112205 | 6.150555 | 6.261356 | 6.08671 | 5.920561 | 6.191247 | 6.649134 | 6.036241 |
1502.02686 | Pascal Anastasopoulos | Pascal Anastasopoulos, Robert Richter, A. N. Schellekens | Discrete symmetries from hidden sectors | 20 pages | null | null | TUW-15-03, ZMP-HH/15-2, Nikhef/2015-004 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the presence of abelian discrete symmetries in globally consistent
orientifold compactifications based on rational conformal field theory. We
extend previous work [1] by allowing the discrete symmetries to be a linear
combination of U(1) gauge factors of the visible as well as the hidden sector.
This more ge... | [
{
"created": "Mon, 9 Feb 2015 21:11:16 GMT",
"version": "v1"
}
] | 2015-02-11 | [
[
"Anastasopoulos",
"Pascal",
""
],
[
"Richter",
"Robert",
""
],
[
"Schellekens",
"A. N.",
""
]
] | We study the presence of abelian discrete symmetries in globally consistent orientifold compactifications based on rational conformal field theory. We extend previous work [1] by allowing the discrete symmetries to be a linear combination of U(1) gauge factors of the visible as well as the hidden sector. This more gene... | 8.78368 | 8.250591 | 9.331376 | 7.572393 | 8.176873 | 9.893717 | 8.814008 | 8.59093 | 8.340718 | 10.558737 | 8.118172 | 8.406351 | 8.628001 | 8.085873 | 8.152591 | 8.345258 | 8.106499 | 8.206848 | 8.077805 | 8.97871 | 8.113547 |
2001.03172 | Wilke van der Schee | M\'ark Mezei and Wilke van der Schee | Black holes often saturate entanglement entropy the fastest | 5 pages and 5 figures + supplemental material. v2: improved text,
matches published version, v3: fixed a typo | Phys. Rev. Lett. 124, 201601 (2020) | 10.1103/PhysRevLett.124.201601 | null | hep-th cond-mat.stat-mech cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There is a simple bound on how fast the entanglement entropy of a subregion
of a many-body quantum system can saturate in a quench: $t_\text{sat}\geq
R/v_B$, where $t_\text{sat}$ is the saturation time, $R$ the radius of the
largest inscribed sphere, and $v_B$ the butterfly velocity characterizing
operator growth. By... | [
{
"created": "Thu, 9 Jan 2020 19:00:00 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jun 2020 10:54:36 GMT",
"version": "v2"
},
{
"created": "Wed, 9 Dec 2020 15:40:57 GMT",
"version": "v3"
}
] | 2020-12-10 | [
[
"Mezei",
"Márk",
""
],
[
"van der Schee",
"Wilke",
""
]
] | There is a simple bound on how fast the entanglement entropy of a subregion of a many-body quantum system can saturate in a quench: $t_\text{sat}\geq R/v_B$, where $t_\text{sat}$ is the saturation time, $R$ the radius of the largest inscribed sphere, and $v_B$ the butterfly velocity characterizing operator growth. By c... | 6.720318 | 6.186501 | 6.732579 | 6.368331 | 6.385772 | 6.760231 | 6.362041 | 6.300527 | 6.076593 | 7.923259 | 6.107146 | 6.31166 | 6.74229 | 6.550453 | 6.460757 | 6.413937 | 6.317687 | 6.350934 | 6.577839 | 6.693209 | 6.480115 |
hep-th/9208005 | Shahn Majid | S. Majid | Quantum Random Walks and Time Reversal | 32 pages, LATEX, (DAMTP/92-20) | Int.J.Mod.Phys. A8 (1993) 4521-4546 | 10.1142/S0217751X93001818 | null | hep-th | null | Classical random walks and Markov processes are easily described by Hopf
algebras. It is also known that groups and Hopf algebras (quantum groups) lead
to classical and quantum diffusions. We study here the more primitive notion of
a quantum random walk associated to a general Hopf algebra and show that it has
a simp... | [
{
"created": "Mon, 3 Aug 1992 11:30:58 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Majid",
"S.",
""
]
] | Classical random walks and Markov processes are easily described by Hopf algebras. It is also known that groups and Hopf algebras (quantum groups) lead to classical and quantum diffusions. We study here the more primitive notion of a quantum random walk associated to a general Hopf algebra and show that it has a simple... | 10.527693 | 11.394416 | 10.805984 | 10.463552 | 11.053938 | 12.220154 | 11.575516 | 11.082112 | 10.272066 | 11.158025 | 9.927582 | 10.058485 | 10.174594 | 9.93657 | 9.785775 | 10.087271 | 9.892215 | 10.034889 | 9.844542 | 10.618456 | 9.885389 |
hep-th/9407064 | Roberto Emparan | R. Emparan | Heat kernels and thermodynamics in Rindler space | 9 pages , LaTex, EHU-FT-94/5 (Revised version: the role played by
regularization is clarified) | Phys.Rev.D51:5716-5719,1995 | 10.1103/PhysRevD.51.5716 | null | hep-th gr-qc | null | We point out that using the heat kernel on a cone to compute the first
quantum correction to the entropy of Rindler space does not yield the correct
temperature dependence. In order to obtain the physics at arbitrary temperature
one must compute the heat kernel in a geometry with different topology (without
a conical... | [
{
"created": "Wed, 13 Jul 1994 09:09:00 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Aug 1994 15:33:00 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Emparan",
"R.",
""
]
] | We point out that using the heat kernel on a cone to compute the first quantum correction to the entropy of Rindler space does not yield the correct temperature dependence. In order to obtain the physics at arbitrary temperature one must compute the heat kernel in a geometry with different topology (without a conical s... | 12.523521 | 10.771852 | 11.720526 | 9.769389 | 10.682217 | 10.533478 | 10.004128 | 10.63404 | 10.013117 | 11.158115 | 9.95509 | 10.574011 | 11.126929 | 10.3147 | 10.26784 | 10.368329 | 10.180126 | 10.475302 | 10.507873 | 10.350425 | 10.226562 |
2212.03262 | Yi Pang | Liang Ma, Yi Pang, H. Lu | Negative Corrections to Black Hole Entropy from String Theory | Latex, 12 pages, 4 graphs grouped into 1 figure, correct a crucial
typo | Sci.China Phys.Mech.Astron. 66 (2023) 12, 121011 | 10.1007/s11433-023-2257-6 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report for the first time that in heterotic string compactified on 4-torus
or equivalently IIA string compactified on K3, the leading $\alpha'$
corrections to the rotating black string entropy at fixed conserved charges can
be negative. This further implies that the correction to the mass of extremal
rotating stri... | [
{
"created": "Tue, 6 Dec 2022 19:00:01 GMT",
"version": "v1"
},
{
"created": "Wed, 10 May 2023 06:58:09 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Oct 2023 01:24:11 GMT",
"version": "v3"
}
] | 2023-11-20 | [
[
"Ma",
"Liang",
""
],
[
"Pang",
"Yi",
""
],
[
"Lu",
"H.",
""
]
] | We report for the first time that in heterotic string compactified on 4-torus or equivalently IIA string compactified on K3, the leading $\alpha'$ corrections to the rotating black string entropy at fixed conserved charges can be negative. This further implies that the correction to the mass of extremal rotating string... | 16.722946 | 15.761541 | 15.392422 | 13.064366 | 16.214582 | 13.853464 | 13.678323 | 14.983187 | 13.088705 | 17.505188 | 14.113482 | 14.194674 | 14.39059 | 14.564822 | 14.060987 | 14.03688 | 14.786189 | 14.655482 | 13.526939 | 14.84982 | 14.248482 |
hep-th/9312144 | null | H.Aratyn, L.A. Ferreira and A.H. Zimerman | On Discrete Symmetries of the Multi-Boson KP Hierarchies | 11 pgs, LaTeX, IFT-P/75/93, UICHEP-TH/93-17 | Phys.Lett. B327 (1994) 266-273 | 10.1016/0370-2693(94)90727-7 | null | hep-th nlin.SI solv-int | null | We show that the multi-boson KP hierarchies possess a class of discrete
symmetries linking them to the discrete Toda systems. These discrete symmetries
are generated by the similarity transformation of the corresponding Lax
operator. This establishes a canonical nature of the discrete transformations.
The spectral eq... | [
{
"created": "Thu, 16 Dec 1993 13:43:09 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Aratyn",
"H.",
""
],
[
"Ferreira",
"L. A.",
""
],
[
"Zimerman",
"A. H.",
""
]
] | We show that the multi-boson KP hierarchies possess a class of discrete symmetries linking them to the discrete Toda systems. These discrete symmetries are generated by the similarity transformation of the corresponding Lax operator. This establishes a canonical nature of the discrete transformations. The spectral equa... | 14.215375 | 14.73135 | 16.036617 | 13.256372 | 14.049167 | 14.877505 | 13.520239 | 13.098445 | 13.069677 | 14.952819 | 12.524627 | 13.29526 | 13.713714 | 12.833077 | 13.123881 | 13.490928 | 13.357318 | 12.961267 | 13.306568 | 13.041193 | 12.494741 |
hep-th/9705054 | Harrison Sheinblatt | Harrison J. Sheinblatt | Statistical Entropy of an Extremal Black Hole with 0- and 6-Brane Charge | 13 pages using harvmac, minor correction, ref added | Phys. Rev. D 57, 2421 (1998) | 10.1103/PhysRevD.57.2421 | null | hep-th | null | A black hole solution to low energy type IIA string theory which is extremal,
non-supersymmetric, and carries 0- and 6-brane charge is presented. For large
values of the charges it is metastable and a corresponding D-brane picture can
be found. The mass and statistical entropy of the two descriptions agree at a
corre... | [
{
"created": "Thu, 8 May 1997 20:14:08 GMT",
"version": "v1"
},
{
"created": "Thu, 15 May 1997 22:58:15 GMT",
"version": "v2"
}
] | 2016-08-25 | [
[
"Sheinblatt",
"Harrison J.",
""
]
] | A black hole solution to low energy type IIA string theory which is extremal, non-supersymmetric, and carries 0- and 6-brane charge is presented. For large values of the charges it is metastable and a corresponding D-brane picture can be found. The mass and statistical entropy of the two descriptions agree at a corresp... | 11.806706 | 8.962084 | 13.083785 | 9.624285 | 10.353996 | 9.785728 | 8.218198 | 9.275834 | 9.224639 | 11.70541 | 8.958889 | 9.304706 | 11.119907 | 9.222588 | 9.959366 | 9.223049 | 9.306533 | 9.673345 | 9.030905 | 10.537906 | 9.137452 |
2306.12175 | Richard Szabo | Richard J. Szabo, Guillaume Trojani | Homotopy double copy of noncommutative gauge theories | 78 pages, 1 figure; v2: new concluding section added; Contribution to
the Special Issue of Symmetry on "Quantum Geometry and Symmetries of String
Theory" | null | null | EMPG-23-10 | hep-th math-ph math.MP math.QA | http://creativecommons.org/licenses/by/4.0/ | We discuss the double copy formulation of Moyal-Weyl type noncommutative
gauge theories from the homotopy algebraic perspective of factorisations of
$L_\infty$-algebras. We define new noncommutative scalar field theories with
rigid colour symmetries taking the role of the zeroth copy, where the deformed
colour algebr... | [
{
"created": "Wed, 21 Jun 2023 11:10:14 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Aug 2023 09:03:58 GMT",
"version": "v2"
}
] | 2023-08-02 | [
[
"Szabo",
"Richard J.",
""
],
[
"Trojani",
"Guillaume",
""
]
] | We discuss the double copy formulation of Moyal-Weyl type noncommutative gauge theories from the homotopy algebraic perspective of factorisations of $L_\infty$-algebras. We define new noncommutative scalar field theories with rigid colour symmetries taking the role of the zeroth copy, where the deformed colour algebra ... | 9.561994 | 8.635013 | 10.162709 | 8.651474 | 9.087213 | 8.82075 | 8.659044 | 8.651642 | 8.374739 | 11.354383 | 8.721795 | 8.968023 | 9.667286 | 9.002101 | 9.225345 | 8.917077 | 8.892554 | 8.844038 | 8.900825 | 9.773834 | 8.62466 |
1010.0860 | Jutta Kunz | Yves Brihaye, Burkhard Kleihaus, Jutta Kunz, Eugen Radu | Rotating black holes with equal-magnitude angular momenta in d=5
Einstein-Gauss-Bonnet theory | 25 pages, 7 figures | JHEP 1011:098,2010 | 10.1007/JHEP11(2010)098 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct rotating black hole solutions in Einstein-Gauss-Bonnet theory in
five spacetime dimensions. These black holes are asymptotically flat, and
possess a regular horizon of spherical topology and two equal-magnitude angular
momenta associated with two distinct planes of rotation. The action and global
charges... | [
{
"created": "Tue, 5 Oct 2010 12:19:58 GMT",
"version": "v1"
}
] | 2015-03-17 | [
[
"Brihaye",
"Yves",
""
],
[
"Kleihaus",
"Burkhard",
""
],
[
"Kunz",
"Jutta",
""
],
[
"Radu",
"Eugen",
""
]
] | We construct rotating black hole solutions in Einstein-Gauss-Bonnet theory in five spacetime dimensions. These black holes are asymptotically flat, and possess a regular horizon of spherical topology and two equal-magnitude angular momenta associated with two distinct planes of rotation. The action and global charges o... | 5.987724 | 6.308587 | 5.110479 | 5.100054 | 5.905954 | 5.913172 | 6.167329 | 5.22584 | 5.675093 | 5.695392 | 5.963096 | 5.89322 | 5.501451 | 5.517011 | 5.581766 | 5.519194 | 5.588531 | 5.546793 | 5.779355 | 5.854579 | 5.59764 |
2202.11111 | Ren\'e Meyer | Suting Zhao, Christian Northe, Konstantin Weisenberger, Ren\'e Meyer | Charged Moments in $W_3$ Higher Spin Holography | 28 pages, no figures, v2: accepted for publication in JHEP | null | 10.1007/JHEP05(2022)166 | null | hep-th cond-mat.stat-mech gr-qc math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | We consider the charged moments in $SL(3,\mathbb{R})$ higher spin holography,
as well as in the dual two-dimensional conformal field theory with $W_3$
symmetry. For the vacuum state and a single entangling interval, we show that
the $W_3$ algebra of the conformal field theory induces an entanglement $W_3$
algebra act... | [
{
"created": "Tue, 22 Feb 2022 19:00:05 GMT",
"version": "v1"
},
{
"created": "Tue, 3 May 2022 09:49:34 GMT",
"version": "v2"
}
] | 2022-06-15 | [
[
"Zhao",
"Suting",
""
],
[
"Northe",
"Christian",
""
],
[
"Weisenberger",
"Konstantin",
""
],
[
"Meyer",
"René",
""
]
] | We consider the charged moments in $SL(3,\mathbb{R})$ higher spin holography, as well as in the dual two-dimensional conformal field theory with $W_3$ symmetry. For the vacuum state and a single entangling interval, we show that the $W_3$ algebra of the conformal field theory induces an entanglement $W_3$ algebra actin... | 8.689684 | 9.191526 | 9.762939 | 8.92075 | 9.471321 | 9.03635 | 8.656729 | 8.679868 | 8.461992 | 11.060402 | 8.51936 | 8.741081 | 8.98236 | 8.6398 | 9.20165 | 8.797095 | 9.014421 | 8.62763 | 8.839601 | 8.84975 | 8.544544 |
hep-th/9604001 | null | Fiorenzo Bastianelli and Ulf Lindstrom | C-theorem for two dimensional chiral theories | 7 pages, uses harvmac.tex | Phys.Lett. B380 (1996) 341-345 | 10.1016/0370-2693(96)00510-2 | null | hep-th cond-mat | null | We discuss an extension of the $C$-theorem to chiral theories. We show that
two monotonically decreasing $C$-functions can be introduced. However, their
difference is a constant of the renormalization group flow. This constant
reproduces the 't Hooft anomaly matching conditions.
| [
{
"created": "Mon, 1 Apr 1996 09:48:46 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Bastianelli",
"Fiorenzo",
""
],
[
"Lindstrom",
"Ulf",
""
]
] | We discuss an extension of the $C$-theorem to chiral theories. We show that two monotonically decreasing $C$-functions can be introduced. However, their difference is a constant of the renormalization group flow. This constant reproduces the 't Hooft anomaly matching conditions. | 8.20761 | 6.7576 | 6.616696 | 6.330193 | 7.373588 | 6.623018 | 6.829032 | 6.590969 | 6.449719 | 7.719163 | 6.106011 | 7.325005 | 7.623579 | 7.000661 | 6.88316 | 7.391653 | 6.923617 | 7.168251 | 7.420334 | 7.193432 | 7.303838 |
0905.3451 | Shlomo S. Razamat | Ari Pakman, Leonardo Rastelli, and Shlomo S. Razamat | Extremal Correlators and Hurwitz Numbers in Symmetric Product Orbifolds | 36 pages, 3 figures, v2: minor improvements | Phys.Rev.D80:086009,2009 | 10.1103/PhysRevD.80.086009 | Brown-HET-1582, YITP-SB-09-12 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study correlation functions of single-cycle chiral operators in the
symmetric product orbifold of N supersymmetric four-tori. Correlators of twist
operators are evaluated on covering surfaces, generally of different genera,
where fields are single-valued. We compute some simple four-point functions and
study how t... | [
{
"created": "Thu, 21 May 2009 19:40:28 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Oct 2009 23:23:08 GMT",
"version": "v2"
}
] | 2009-11-05 | [
[
"Pakman",
"Ari",
""
],
[
"Rastelli",
"Leonardo",
""
],
[
"Razamat",
"Shlomo S.",
""
]
] | We study correlation functions of single-cycle chiral operators in the symmetric product orbifold of N supersymmetric four-tori. Correlators of twist operators are evaluated on covering surfaces, generally of different genera, where fields are single-valued. We compute some simple four-point functions and study how the... | 12.314971 | 13.069728 | 15.113124 | 12.19515 | 13.569162 | 12.175618 | 11.720031 | 10.855977 | 11.497149 | 16.338497 | 11.414572 | 12.068712 | 13.035825 | 11.103209 | 11.763888 | 11.79498 | 11.659444 | 11.720165 | 11.698546 | 13.108881 | 11.556334 |
1409.0559 | Keshav Dasgupta | Keshav Dasgupta, Charles Gale, Mohammed Mia, Michael Richard, Olivier
Trottier | Infrared Dynamics of a Large N QCD Model, the Massless String Sector and
Mesonic Spectra | 47 pages, 7 pdf figures, 24 tables, JHEP format; Detailed mathematica
file of the computations is available on request; Version 2: Text elaborated,
typos corrected, a new appendix added to discuss the regimes of validity, and
a word in the abstract changed. Results unchanged. Final version to appear in
JHEP | null | null | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A consistency check for any UV complete model for large N QCD should be,
among other things, the existence of a well-defined vector and scalar mesonic
spectra. In this paper, we use our UV complete model in type IIB string theory
to study the IR dynamics and use this to predict the mesonic spectra in the
dual type II... | [
{
"created": "Mon, 1 Sep 2014 20:27:28 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Jul 2015 00:56:03 GMT",
"version": "v2"
}
] | 2015-07-23 | [
[
"Dasgupta",
"Keshav",
""
],
[
"Gale",
"Charles",
""
],
[
"Mia",
"Mohammed",
""
],
[
"Richard",
"Michael",
""
],
[
"Trottier",
"Olivier",
""
]
] | A consistency check for any UV complete model for large N QCD should be, among other things, the existence of a well-defined vector and scalar mesonic spectra. In this paper, we use our UV complete model in type IIB string theory to study the IR dynamics and use this to predict the mesonic spectra in the dual type IIA ... | 17.888496 | 18.333572 | 17.327278 | 17.071501 | 17.596413 | 17.86891 | 18.581205 | 16.727644 | 16.027225 | 16.66151 | 16.116743 | 16.098394 | 16.971762 | 16.403851 | 16.563007 | 15.716024 | 15.448665 | 15.662646 | 15.43882 | 16.792044 | 15.776581 |
1508.03340 | Alfredo Perez | Claudio Bunster and Alfredo Perez | Space-filling branes of gravitational ancestry | Improved and final version of the manuscript previously entitled
"G-branes." Matches published version in Physical Review D | null | 10.1103/PhysRevD.92.124070 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a new kind of space-filling brane, which we term "G-brane"
because its action is a descendant of the gravitational action. The G-brane may
be thought of as the remanent of the gravitational field when the propagating
gravitons are removed. The G-brane is different from the Dirac or Nambu
space-filling br... | [
{
"created": "Thu, 13 Aug 2015 20:07:55 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jan 2016 21:09:39 GMT",
"version": "v2"
}
] | 2016-01-06 | [
[
"Bunster",
"Claudio",
""
],
[
"Perez",
"Alfredo",
""
]
] | We introduce a new kind of space-filling brane, which we term "G-brane" because its action is a descendant of the gravitational action. The G-brane may be thought of as the remanent of the gravitational field when the propagating gravitons are removed. The G-brane is different from the Dirac or Nambu space-filling bran... | 6.484169 | 5.978867 | 6.595046 | 5.999371 | 6.301578 | 6.430953 | 6.801455 | 6.044828 | 6.13813 | 6.999052 | 6.154483 | 5.931154 | 6.292735 | 5.929879 | 5.941316 | 5.889638 | 5.994378 | 5.988294 | 5.985541 | 6.155014 | 6.141215 |
1801.03199 | Napat Poovuttikul | Sa\v{s}o Grozdanov and Napat Poovuttikul | Generalised global symmetries in states with dynamical defects: the case
of the transverse sound in field theory and holography | v3: 15+5 pages, 6 figures, references and further explanations added.
Version to appear in PRD | Phys. Rev. D 97, 106005 (2018) | 10.1103/PhysRevD.97.106005 | MIT-CTP/4966 | hep-th cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we show how states with conserved numbers of dynamical defects
(strings, domain walls, etc.) can be understood as possessing generalised
global symmetries even when the microscopic origins of these symmetries are
unknown. Using this philosophy, we build an effective theory of a
$2+1$-dimensional fluid s... | [
{
"created": "Wed, 10 Jan 2018 00:37:45 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Jan 2018 17:23:24 GMT",
"version": "v2"
},
{
"created": "Tue, 24 Apr 2018 16:39:00 GMT",
"version": "v3"
}
] | 2018-05-18 | [
[
"Grozdanov",
"Sašo",
""
],
[
"Poovuttikul",
"Napat",
""
]
] | In this work, we show how states with conserved numbers of dynamical defects (strings, domain walls, etc.) can be understood as possessing generalised global symmetries even when the microscopic origins of these symmetries are unknown. Using this philosophy, we build an effective theory of a $2+1$-dimensional fluid sta... | 11.673451 | 12.886168 | 13.690319 | 12.264508 | 12.787049 | 13.594496 | 13.209371 | 12.726669 | 12.377527 | 14.010348 | 12.454599 | 12.093771 | 12.330979 | 11.97117 | 11.720235 | 11.806631 | 12.031539 | 12.141953 | 11.624113 | 12.504803 | 11.803041 |
2007.11611 | Keshav Dasgupta | Suddhasattwa Brahma, Keshav Dasgupta, Radu Tatar | de Sitter Space as a Glauber-Sudarshan State | 124 pages, 1 figure; v2: Typos corrected and references added; v3:
Some approximate results in sec 3.2 replaced by exact ones, typos corrected
and references updated; v4: sec 3.3 elaborated, typos corrected and
references updated. Final version to appear in JHEP | null | 10.1007/JHEP02(2021)104 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Glauber-Sudarshan states, sometimes simply referred to as Glauber states, or
alternatively as coherent and squeezed-coherent states, are interesting states
in the configuration spaces of any quantum field theories, that closely
resemble classical trajectories in space-time. In this paper, we identify
four-dimensional... | [
{
"created": "Wed, 22 Jul 2020 18:15:35 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Aug 2020 19:17:15 GMT",
"version": "v2"
},
{
"created": "Sat, 12 Sep 2020 05:48:02 GMT",
"version": "v3"
},
{
"created": "Tue, 12 Jan 2021 19:46:06 GMT",
"version": "v4"
}
] | 2021-03-17 | [
[
"Brahma",
"Suddhasattwa",
""
],
[
"Dasgupta",
"Keshav",
""
],
[
"Tatar",
"Radu",
""
]
] | Glauber-Sudarshan states, sometimes simply referred to as Glauber states, or alternatively as coherent and squeezed-coherent states, are interesting states in the configuration spaces of any quantum field theories, that closely resemble classical trajectories in space-time. In this paper, we identify four-dimensional d... | 14.416417 | 16.560339 | 16.910358 | 14.529497 | 16.092575 | 15.318651 | 14.469874 | 13.928477 | 14.766458 | 18.533577 | 14.559981 | 14.355448 | 14.767776 | 13.981688 | 14.154425 | 13.771737 | 13.863985 | 14.178899 | 14.286123 | 14.365014 | 14.178179 |
0710.1059 | Pietro Fre | Pietro Fr\'e and Alexander S. Sorin | The arrow of time and the Weyl group: all supergravity billiards are
integrable | 73 pages 34 figures. Research paper, not review | null | null | null | hep-th astro-ph nlin.SI | null | In this paper we show that all supergravity billiards corresponding to
sigma-models on any U/H non compact-symmetric space and obtained by
compactifying supergravity to D=3 are fully integrable. The key point in
establishing the integration algorithm is provided by an upper triangular
embedding of the solvable Lie al... | [
{
"created": "Thu, 4 Oct 2007 17:49:24 GMT",
"version": "v1"
}
] | 2008-07-09 | [
[
"Fré",
"Pietro",
""
],
[
"Sorin",
"Alexander S.",
""
]
] | In this paper we show that all supergravity billiards corresponding to sigma-models on any U/H non compact-symmetric space and obtained by compactifying supergravity to D=3 are fully integrable. The key point in establishing the integration algorithm is provided by an upper triangular embedding of the solvable Lie alge... | 15.321794 | 16.160904 | 17.608625 | 15.211255 | 15.914794 | 15.019411 | 14.33097 | 14.783663 | 14.468612 | 19.274433 | 14.166694 | 14.384271 | 14.801167 | 14.028736 | 14.734786 | 14.374548 | 14.335177 | 13.786112 | 14.39782 | 14.996197 | 13.966686 |
hep-th/0005172 | Chris Pope | P. Hoxha, R.R. Martinez-Acosta and C.N. Pope | Kaluza-Klein Consistency, Killing Vectors, and Kahler Spaces | Latex, 43 pages, references added and typos corrected | Class.Quant.Grav.17:4207-4240,2000 | 10.1088/0264-9381/17/20/305 | null | hep-th | null | We make a detailed investigation of all spaces Q_{n_1... n_N}^{q_1... q_N} of
the form of U(1) bundles over arbitrary products \prod_i CP^{n_i} of complex
projective spaces, with arbitrary winding numbers q_i over each factor in the
base. Special cases, including Q_{11}^{11} (sometimes known as T^{11}),
Q_{111}^{111}... | [
{
"created": "Thu, 18 May 2000 21:28:11 GMT",
"version": "v1"
},
{
"created": "Fri, 26 May 2000 12:46:34 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Hoxha",
"P.",
""
],
[
"Martinez-Acosta",
"R. R.",
""
],
[
"Pope",
"C. N.",
""
]
] | We make a detailed investigation of all spaces Q_{n_1... n_N}^{q_1... q_N} of the form of U(1) bundles over arbitrary products \prod_i CP^{n_i} of complex projective spaces, with arbitrary winding numbers q_i over each factor in the base. Special cases, including Q_{11}^{11} (sometimes known as T^{11}), Q_{111}^{111} a... | 7.333508 | 7.017627 | 7.743712 | 6.704161 | 6.963264 | 7.490238 | 7.057224 | 7.009089 | 6.808699 | 8.513614 | 6.465158 | 6.683477 | 6.65837 | 6.713242 | 6.7572 | 6.739987 | 6.799847 | 6.618663 | 6.665833 | 6.900148 | 6.758096 |
hep-th/0101164 | Kazuya Koyama | Kazuya Koyama and Jiro Soda | Strongly Coupled CFT in FRW Universe from AdS/CFT Correspondence | 23 pages, no figure, version to appear in JHEP | JHEP 0105:027,2001 | 10.1088/1126-6708/2001/05/027 | null | hep-th astro-ph gr-qc | null | We develop a formalism to calculate the effective action of the strongly
coupled conformal field theory (CFT) in curved spacetime. The effective action
of the CFT is obtained from AdS/CFT correspondence. The anti de-Sitter (AdS)
spacetime has various slicing which give various curved spacetime on its
boundary. We sho... | [
{
"created": "Thu, 25 Jan 2001 10:06:12 GMT",
"version": "v1"
},
{
"created": "Mon, 28 May 2001 07:11:57 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Koyama",
"Kazuya",
""
],
[
"Soda",
"Jiro",
""
]
] | We develop a formalism to calculate the effective action of the strongly coupled conformal field theory (CFT) in curved spacetime. The effective action of the CFT is obtained from AdS/CFT correspondence. The anti de-Sitter (AdS) spacetime has various slicing which give various curved spacetime on its boundary. We show ... | 6.10558 | 5.802224 | 6.10823 | 5.834566 | 6.121559 | 6.064898 | 6.087533 | 5.961187 | 5.891076 | 6.440747 | 6.002493 | 5.957983 | 5.936072 | 5.895776 | 6.018261 | 5.760941 | 5.89234 | 5.871764 | 5.975585 | 6.055035 | 5.822831 |
hep-th/9908068 | Vassili Ivanov | A.T. Filippov, V.G. Ivanov | Global Properties of Exact Solutions in Integrable Dilaton-Gravity
Models | 5 pages, LaTeX, Conf. Report, Dubna, July 13-17, 1998 | XI Intl. Conf., Problems of QFT, JINR, Dubna, July 13-17, 1998,
(publ. Dubna 1999, edited by B.M. Barbashov, G.V. Efimov, A.V. Efremov) | null | null | hep-th gr-qc | null | Global canonical transformations to free chiral fields are constructed for DG
models minimally coupled to scalar fields. The boundary terms for such
canonical transformations are shown to vanish in asymptotically static
coordinates if there is no scalar field.
| [
{
"created": "Mon, 9 Aug 1999 14:00:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Filippov",
"A. T.",
""
],
[
"Ivanov",
"V. G.",
""
]
] | Global canonical transformations to free chiral fields are constructed for DG models minimally coupled to scalar fields. The boundary terms for such canonical transformations are shown to vanish in asymptotically static coordinates if there is no scalar field. | 32.178154 | 33.776192 | 28.497908 | 30.519468 | 32.39555 | 36.021408 | 35.155651 | 30.118423 | 29.264933 | 33.672916 | 32.083248 | 27.021317 | 23.158192 | 26.678831 | 27.435858 | 26.110903 | 25.913773 | 24.180468 | 25.88232 | 24.352711 | 28.253466 |
hep-th/0607120 | John March-Russell | A. Hebecker, J. March-Russell | The Ubiquitous Throat | References added, typos fixed. LaTex, 17 pages, 1 figure | Nucl.Phys.B781:99-111,2007 | 10.1016/j.nuclphysb.2007.05.003 | HD-THEP-06-12, OUTP-DR-06 01P | hep-th hep-ph | null | We attempt to quantify the widely-held belief that large hierarchies induced
by strongly-warped geometries are common in the string theory landscape. To
this end, we focus on the arguably best-understood subset of vacua -- type IIB
Calabi-Yau orientifolds with non-perturbative Kaehler stabilization and a
SUSY-breakin... | [
{
"created": "Tue, 18 Jul 2006 16:13:50 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Aug 2006 13:01:24 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Aug 2006 13:00:16 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Hebecker",
"A.",
""
],
[
"March-Russell",
"J.",
""
]
] | We attempt to quantify the widely-held belief that large hierarchies induced by strongly-warped geometries are common in the string theory landscape. To this end, we focus on the arguably best-understood subset of vacua -- type IIB Calabi-Yau orientifolds with non-perturbative Kaehler stabilization and a SUSY-breaking ... | 8.949976 | 9.165232 | 9.452774 | 8.534316 | 9.637106 | 10.053411 | 9.489594 | 9.275544 | 8.954255 | 11.007383 | 8.958277 | 8.454055 | 8.592004 | 8.370884 | 8.550261 | 8.592972 | 8.321738 | 8.693259 | 8.38369 | 8.461124 | 8.790536 |
hep-th/9712247 | Stefano Bellucci | S. Bellucci and A. Galajinsky | On the complex structure in the Gupta-Bleuler quantization method | 12 pages, LaTeX | Phys.Lett. B423 (1998) 274-280 | 10.1016/S0370-2693(98)00168-3 | null | hep-th | null | We examine the general conditions for the existence of the complex structure
intrinsic in the Gupta-Bleuler quantization method for the specific case of
mixed first and second class fermionic constraints in an arbitrary space-time
dimension. The cases d=3 and 10 are shown to be of prime importance. The
explicit solut... | [
{
"created": "Mon, 29 Dec 1997 13:47:19 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Bellucci",
"S.",
""
],
[
"Galajinsky",
"A.",
""
]
] | We examine the general conditions for the existence of the complex structure intrinsic in the Gupta-Bleuler quantization method for the specific case of mixed first and second class fermionic constraints in an arbitrary space-time dimension. The cases d=3 and 10 are shown to be of prime importance. The explicit solutio... | 14.515505 | 15.532853 | 13.312262 | 12.421597 | 12.995918 | 12.16541 | 13.16448 | 12.650743 | 12.277621 | 13.83848 | 13.850492 | 13.655699 | 13.677735 | 13.319017 | 13.413761 | 13.131963 | 13.59015 | 13.172103 | 13.410565 | 13.745914 | 12.8922 |
1704.05856 | Shahar Hod | Shahar Hod | Onset of superradiant instabilities in rotating spacetimes of exotic
compact objects | 9 pages | Journal of High Energy Physics 06, 132 (2017) | 10.1007/JHEP06(2017)132 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Exotic compact objects, horizonless spacetimes with reflective properties,
have intriguingly been suggested by some quantum-gravity models as alternatives
to classical black-hole spacetimes. A remarkable feature of spinning
horizonless compact objects with reflective boundary conditions is the
existence of a {\it dis... | [
{
"created": "Wed, 19 Apr 2017 18:00:07 GMT",
"version": "v1"
}
] | 2017-08-02 | [
[
"Hod",
"Shahar",
""
]
] | Exotic compact objects, horizonless spacetimes with reflective properties, have intriguingly been suggested by some quantum-gravity models as alternatives to classical black-hole spacetimes. A remarkable feature of spinning horizonless compact objects with reflective boundary conditions is the existence of a {\it discr... | 4.689045 | 4.989293 | 4.032159 | 3.953826 | 4.808896 | 4.672089 | 5.405778 | 3.71611 | 4.850254 | 4.185274 | 4.905849 | 4.679476 | 4.297103 | 4.312497 | 4.4902 | 4.678485 | 4.743311 | 4.220936 | 4.574972 | 4.368418 | 4.765848 |
hep-th/0606071 | Lorenzo Salcedo L. | L.L. Salcedo | The method of covariant symbols in curved space-time | 28 pages, no figures. References added. To appear in European
Physical Journal C | Eur.Phys.J.C49:831-850,2007 | 10.1140/epjc/s10052-006-0133-2 | null | hep-th gr-qc | null | Diagonal matrix elements of pseudodifferential operators are needed in order
to compute effective Lagrangians and currents. For this purpose the method of
symbols is often used, which however lacks manifest covariance. In this work
the method of covariant symbols, introduced by Pletnev and Banin, is extended
to curve... | [
{
"created": "Thu, 8 Jun 2006 10:38:50 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Sep 2006 09:45:30 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Salcedo",
"L. L.",
""
]
] | Diagonal matrix elements of pseudodifferential operators are needed in order to compute effective Lagrangians and currents. For this purpose the method of symbols is often used, which however lacks manifest covariance. In this work the method of covariant symbols, introduced by Pletnev and Banin, is extended to curved ... | 7.206159 | 7.920886 | 9.249898 | 7.969985 | 9.00161 | 8.865956 | 8.25776 | 8.422503 | 7.7877 | 9.253588 | 7.541945 | 7.131796 | 7.674789 | 7.292598 | 7.069766 | 6.644126 | 6.713706 | 7.045546 | 7.271424 | 7.475186 | 7.096305 |
2311.17015 | Subham Dutta Chowdhury | Subham Dutta Chowdhury, Vipul Kumar, Suman Kundu, Asikur Rahaman | Regge constraints on local four-point scattering amplitudes of massive
particles with spin | References added, Scales in dRGT gravity analysis corrected | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | In this work, we classify all the possible local four-point couplings
relevant for tree-level flat space $2 \rightarrow 2$ scattering of external
massive particles of spin one and spin two which do not grow faster than $s^2$
at large $s$ and fixed t. This kinematic constraint on local growth of
tree-level S-matrices ... | [
{
"created": "Tue, 28 Nov 2023 18:09:31 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Dec 2023 18:56:38 GMT",
"version": "v2"
}
] | 2023-12-27 | [
[
"Chowdhury",
"Subham Dutta",
""
],
[
"Kumar",
"Vipul",
""
],
[
"Kundu",
"Suman",
""
],
[
"Rahaman",
"Asikur",
""
]
] | In this work, we classify all the possible local four-point couplings relevant for tree-level flat space $2 \rightarrow 2$ scattering of external massive particles of spin one and spin two which do not grow faster than $s^2$ at large $s$ and fixed t. This kinematic constraint on local growth of tree-level S-matrices is... | 11.383418 | 11.666588 | 12.185585 | 10.684298 | 11.649679 | 10.961616 | 11.488945 | 10.834293 | 10.505483 | 13.093025 | 10.387821 | 10.675062 | 11.317825 | 10.725276 | 10.90888 | 10.624207 | 11.023396 | 10.498028 | 10.723831 | 11.430425 | 10.540629 |
hep-th/0206243 | Neil Constable | Neil R. Constable and Neil D. Lambert | Calibrations, Monopoles and Fuzzy Funnels | 19 pages. Latex. v2: added references and acknowledgment | Phys.Rev. D66 (2002) 065016 | 10.1103/PhysRevD.66.065016 | null | hep-th | null | We present new non-Abelian solitonic configurations in the low energy
effective theory describing a collection of N parallel D1--branes. These
configurations preserve 1/4, 1/8, 1/16 and 1/32 of the spacetime supersymmetry.
They are solutions to a set of generalised Nahm's equations which are related
to self-duality e... | [
{
"created": "Thu, 27 Jun 2002 19:34:27 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Jul 2002 14:48:48 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Constable",
"Neil R.",
""
],
[
"Lambert",
"Neil D.",
""
]
] | We present new non-Abelian solitonic configurations in the low energy effective theory describing a collection of N parallel D1--branes. These configurations preserve 1/4, 1/8, 1/16 and 1/32 of the spacetime supersymmetry. They are solutions to a set of generalised Nahm's equations which are related to self-duality equ... | 7.268816 | 6.305589 | 8.556846 | 6.195758 | 6.551478 | 6.237038 | 6.315984 | 6.653345 | 6.057387 | 9.837675 | 6.24338 | 6.612576 | 7.579792 | 6.897525 | 6.81547 | 6.717893 | 6.612442 | 6.844188 | 6.787656 | 7.363993 | 6.78838 |
hep-th/0604179 | Meng Chwan Tan | Meng-Chwan Tan | Two-Dimensional Twisted Sigma Models And The Theory of Chiral
Differential Operators | 93 pages, no figures. Published version. See also companion paper
arXiv:0705.0790 | Adv.Theor.Math.Phys.10:759-851,2006 | null | null | hep-th math.AG math.QA | null | In this paper, we study the perturbative aspects of a twisted version of the
two-dimensional $(0,2)$ heterotic sigma model on a holomorphic gauge bundle
$\mathcal E$ over a complex, hermitian manifold $X$. We show that the model can
be naturally described in terms of the mathematical theory of ``Chiral
Differential O... | [
{
"created": "Tue, 25 Apr 2006 16:23:40 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Dec 2006 14:28:29 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Apr 2007 14:49:19 GMT",
"version": "v3"
}
] | 2009-05-28 | [
[
"Tan",
"Meng-Chwan",
""
]
] | In this paper, we study the perturbative aspects of a twisted version of the two-dimensional $(0,2)$ heterotic sigma model on a holomorphic gauge bundle $\mathcal E$ over a complex, hermitian manifold $X$. We show that the model can be naturally described in terms of the mathematical theory of ``Chiral Differential Ope... | 9.724555 | 8.810936 | 11.834563 | 8.542324 | 9.897243 | 10.104244 | 10.383078 | 9.065488 | 8.499275 | 12.229475 | 8.64432 | 9.230734 | 10.228205 | 9.307355 | 9.52327 | 9.571457 | 9.872866 | 9.533501 | 9.441609 | 10.235262 | 9.543939 |
hep-th/0401055 | Filipe Freire | Mboyo Esole and Filipe Freire | On the renormalisability of gauge invariant extensions of the squared
gauge potential | 1+13 pages. Revised version. New title and abstract. Extended
introduction and several sentences have been inserted. Final version to
appear in Physics Letters B | Phys.Lett. B593 (2004) 287-295 | 10.1016/j.physletb.2004.04.046 | null | hep-th | null | We show that gauge invariant extensions of the local functional $\cO =
\frac12\int d^4x A^2$ have long range non localities which can only be
``renormalised'' with reference to a specific gauge. Consequently, there is no
gauge independent way of claiming the perturbative renormalisability of these
extensions. In part... | [
{
"created": "Fri, 9 Jan 2004 14:17:36 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Apr 2004 11:56:23 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Esole",
"Mboyo",
""
],
[
"Freire",
"Filipe",
""
]
] | We show that gauge invariant extensions of the local functional $\cO = \frac12\int d^4x A^2$ have long range non localities which can only be ``renormalised'' with reference to a specific gauge. Consequently, there is no gauge independent way of claiming the perturbative renormalisability of these extensions. In partic... | 12.176271 | 12.895041 | 12.34663 | 11.624032 | 12.046599 | 13.575586 | 11.492064 | 12.164207 | 11.633867 | 14.133511 | 11.52865 | 11.045286 | 11.803247 | 11.280423 | 11.670115 | 11.413277 | 11.107459 | 11.854661 | 11.509796 | 11.819538 | 11.285107 |
hep-th/0112224 | Masato Ito | Masato Ito (Nagoya Univ.) | Newton's law in braneworlds with an infinite extra dimension | null | Phys.Lett. B528 (2002) 269-273 | 10.1016/S0370-2693(02)01228-5 | DPNU-01-33 | hep-th | null | We study the behavior of the four$-$dimensional Newton's law in warped
braneworlds. The setup considered here is a $(3+n)$-brane embedded in $(5+n)$
dimensions, where $n$ extra dimensions are compactified and a dimension is
infinite. We show that the wave function of gravity is described in terms of
the Bessel functi... | [
{
"created": "Sun, 23 Dec 2001 23:07:55 GMT",
"version": "v1"
},
{
"created": "Sun, 20 Jan 2002 23:50:59 GMT",
"version": "v2"
},
{
"created": "Mon, 1 Apr 2002 05:10:40 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Ito",
"Masato",
"",
"Nagoya Univ."
]
] | We study the behavior of the four$-$dimensional Newton's law in warped braneworlds. The setup considered here is a $(3+n)$-brane embedded in $(5+n)$ dimensions, where $n$ extra dimensions are compactified and a dimension is infinite. We show that the wave function of gravity is described in terms of the Bessel function... | 9.388037 | 7.268945 | 8.694343 | 8.140143 | 8.029115 | 8.230241 | 8.561818 | 7.989757 | 8.209986 | 9.492228 | 7.844151 | 7.870196 | 8.289721 | 7.956086 | 8.079121 | 8.109333 | 7.822498 | 8.388746 | 7.680161 | 7.752596 | 7.969655 |
1103.1163 | Andrea Prinsloo | Jeff Murugan and Andrea Prinsloo | ABJM Dibaryon Spectroscopy | 26 pages | null | 10.1007/JHEP05(2011)129 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the proposal for a detailed map between wrapped D-branes in Anti-de
Sitter space and baryon-like operators in the associated dual conformal field
theory provided in hep-th/0202150 to the recently formulated AdS_4 \times
CP^3/ABJM correspondence. In this example, the role of the dibaryon operator of
the 3-di... | [
{
"created": "Sun, 6 Mar 2011 21:00:07 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Mar 2011 10:18:08 GMT",
"version": "v2"
}
] | 2015-05-27 | [
[
"Murugan",
"Jeff",
""
],
[
"Prinsloo",
"Andrea",
""
]
] | We extend the proposal for a detailed map between wrapped D-branes in Anti-de Sitter space and baryon-like operators in the associated dual conformal field theory provided in hep-th/0202150 to the recently formulated AdS_4 \times CP^3/ABJM correspondence. In this example, the role of the dibaryon operator of the 3-dime... | 9.78932 | 8.201073 | 11.132549 | 8.766744 | 8.54396 | 7.719699 | 8.017732 | 8.026337 | 8.374577 | 11.641953 | 7.488249 | 8.25318 | 9.327605 | 8.27411 | 8.348948 | 8.689933 | 8.250338 | 8.231209 | 8.343894 | 9.189769 | 7.94753 |
hep-th/9604150 | null | Kayoko Maeda and Makoto Sakamoto ( Kobe univ. ) | Strong Coupling Quantum Gravity and Physics beyond the Planck Scale | 27 pages, LaTeX file. To be published in Phys. Rev. D | Phys.Rev.D54:1500-1513,1996 | 10.1103/PhysRevD.54.1500 | KOBE-TH-96-01 | hep-th | null | We propose a renormalization prescription for the Wheeler-DeWitt equation of
(3+1)-dimensional Einstein gravity and also propose a strong coupling expansion
as an approximation scheme to probe quantum geometry at length scales much
smaller than the Planck length. We solve the Wheeler-DeWitt equation to the
second ord... | [
{
"created": "Wed, 24 Apr 1996 01:39:28 GMT",
"version": "v1"
}
] | 2011-09-09 | [
[
"Maeda",
"Kayoko",
"",
"Kobe univ."
],
[
"Sakamoto",
"Makoto",
"",
"Kobe univ."
]
] | We propose a renormalization prescription for the Wheeler-DeWitt equation of (3+1)-dimensional Einstein gravity and also propose a strong coupling expansion as an approximation scheme to probe quantum geometry at length scales much smaller than the Planck length. We solve the Wheeler-DeWitt equation to the second order... | 9.461287 | 8.049759 | 8.474451 | 8.355172 | 8.722826 | 8.560473 | 9.153773 | 7.850936 | 8.173571 | 9.137559 | 8.251497 | 8.520296 | 8.652047 | 8.431183 | 8.418565 | 8.588841 | 8.513105 | 8.18923 | 8.687082 | 8.716327 | 8.270267 |
0905.4116 | Esmaeil Ebrahimi | E. Ebrahimi, N. Riazi | Expanding $(n+1)$-Dimensional Wormhole Solutions in Brans-Dicke
Cosmology | 15 pages, 16 figures, The version to appear in Phys. Rev. D | Phys.Rev.D81:024036,2010 | 10.1103/PhysRevD.81.024036 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have obtained two classes of $(n+1)$-dimensional wormhole solutions using
a traceless energy-momentum tensor in Brans-Dicke theory of gravity. The first
class contains wormhole solutions in an open geometry while the second contains
wormhole solutions in both open and closed universes. In addition to wormhole
geom... | [
{
"created": "Tue, 26 May 2009 05:16:08 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Dec 2009 12:14:03 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Ebrahimi",
"E.",
""
],
[
"Riazi",
"N.",
""
]
] | We have obtained two classes of $(n+1)$-dimensional wormhole solutions using a traceless energy-momentum tensor in Brans-Dicke theory of gravity. The first class contains wormhole solutions in an open geometry while the second contains wormhole solutions in both open and closed universes. In addition to wormhole geomet... | 6.390322 | 6.677859 | 6.26443 | 6.066778 | 6.477408 | 6.571028 | 6.766148 | 5.831078 | 6.428169 | 6.041647 | 6.052454 | 6.045786 | 5.907022 | 5.803733 | 6.008445 | 5.867785 | 5.947531 | 5.894348 | 5.963543 | 5.909838 | 5.929839 |
2303.14921 | James T. Wheeler | James T. Wheeler | Sources of torsion in Poincare gauge theory | 28 pp. Introductory Sections condensed; 2 and 3 dimensional examples
added | Eur. Phys. J. C 83, 665 (2023) | 10.1140/epjc/s10052-023-11812-4 | null | hep-th gr-qc | http://creativecommons.org/licenses/by-sa/4.0/ | We study sources for torsion in Poincare gauge theory of any dimension,
signature, and spin. We find that symmetric kinetic terms for non-Yang-Mills
bosonic fields of arbitrary rank drive torsion. Our detailed discussion of
spin-3/2 Rarita-Schwinger fields shows that they source all independent parts
of the torsion. ... | [
{
"created": "Mon, 27 Mar 2023 05:35:17 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jun 2023 21:33:51 GMT",
"version": "v2"
}
] | 2024-01-01 | [
[
"Wheeler",
"James T.",
""
]
] | We study sources for torsion in Poincare gauge theory of any dimension, signature, and spin. We find that symmetric kinetic terms for non-Yang-Mills bosonic fields of arbitrary rank drive torsion. Our detailed discussion of spin-3/2 Rarita-Schwinger fields shows that they source all independent parts of the torsion. We... | 16.507431 | 17.368988 | 17.171621 | 14.904672 | 17.672707 | 17.892126 | 18.7754 | 16.636587 | 15.754324 | 19.643393 | 16.215797 | 15.378197 | 15.842627 | 15.530005 | 15.260505 | 14.999451 | 15.300222 | 15.305805 | 15.295182 | 16.260033 | 15.160155 |
hep-th/9310026 | Gregory Moore | Gregory Moore | Symmetries of the Bosonic String S-Matrix | 37pp.,YCTP-P19-93. (Important revision: An error has been fixed and
the conclusions altered. The analysis only applies in a straightforward way
to $N$-particle scattering for $N\leq 26$.) | null | null | null | hep-th | null | The bracket operation on mutually local BRST classes may be combined with
Lorentz invariance and analyticity to write an infinite set of finite
difference relations on string scattering amplitudes. When combined with some
simple physical criteria these relations uniquely determine the genus zero
string $S$-matrix for... | [
{
"created": "Thu, 7 Oct 1993 02:45:38 GMT",
"version": "v1"
},
{
"created": "Sun, 10 Oct 1993 21:54:39 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Moore",
"Gregory",
""
]
] | The bracket operation on mutually local BRST classes may be combined with Lorentz invariance and analyticity to write an infinite set of finite difference relations on string scattering amplitudes. When combined with some simple physical criteria these relations uniquely determine the genus zero string $S$-matrix for $... | 13.976883 | 11.476993 | 14.678173 | 11.605661 | 12.386877 | 11.864835 | 12.034554 | 11.185468 | 11.426005 | 15.613941 | 12.077583 | 12.564276 | 13.272805 | 12.461374 | 12.303675 | 12.679301 | 12.061432 | 12.175424 | 11.875138 | 13.650399 | 11.611119 |
hep-th/0608152 | Mark G. Jackson | Mark G. Jackson | Cosmic Superstring Scattering in Backgrounds | 12 pages, 2 figures; v2: references added | JHEP 0609:071,2006 | 10.1088/1126-6708/2006/09/071 | FERMILAB-PUB-06-288-A | hep-th astro-ph hep-ph | null | We generalize the calculation of cosmic superstring reconnection probability
to non-trivial backgrounds. This is done by modeling cosmic strings as wound
tachyon modes in the 0B theory, and the spacetime effective action is then used
to couple this to background fields. Simple examples are given including
trivial and... | [
{
"created": "Tue, 22 Aug 2006 06:39:38 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Sep 2006 12:56:29 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Jackson",
"Mark G.",
""
]
] | We generalize the calculation of cosmic superstring reconnection probability to non-trivial backgrounds. This is done by modeling cosmic strings as wound tachyon modes in the 0B theory, and the spacetime effective action is then used to couple this to background fields. Simple examples are given including trivial and w... | 22.370714 | 18.528257 | 23.518053 | 16.648932 | 20.686039 | 19.126974 | 15.058125 | 16.827694 | 16.772867 | 27.368681 | 17.816669 | 17.694761 | 20.893902 | 17.947344 | 18.426521 | 18.242395 | 17.190784 | 18.580975 | 17.870079 | 20.140957 | 18.413223 |
2210.02966 | Kirsty Gledhill | Kirsty Gledhill and Amihay Hanany | Poisson Brackets for some Coulomb Branches | null | null | 10.1007/JHEP03(2023)154 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct Poisson bracket relations between the operators which generate
the chiral ring of the Coulomb branch of certain $3d$ $\mathcal{N}=4$ quiver
gauge theories. In the case where the Coulomb branch is a free space, $ADE$
Klein singularity, or the minimal $A_2$ nilpotent orbit, we explicitly compute
the Poisso... | [
{
"created": "Thu, 6 Oct 2022 14:59:09 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Mar 2023 12:46:58 GMT",
"version": "v2"
}
] | 2023-04-05 | [
[
"Gledhill",
"Kirsty",
""
],
[
"Hanany",
"Amihay",
""
]
] | We construct Poisson bracket relations between the operators which generate the chiral ring of the Coulomb branch of certain $3d$ $\mathcal{N}=4$ quiver gauge theories. In the case where the Coulomb branch is a free space, $ADE$ Klein singularity, or the minimal $A_2$ nilpotent orbit, we explicitly compute the Poisson ... | 14.662532 | 14.870532 | 15.477207 | 13.245622 | 13.673448 | 13.567021 | 14.535793 | 13.465815 | 13.369249 | 17.23876 | 13.121556 | 13.543283 | 14.966822 | 13.534781 | 13.538703 | 13.757357 | 13.454284 | 13.615245 | 13.298152 | 15.057148 | 13.583464 |
hep-th/0201122 | Andrea Quadri | Andrea Quadri | Algebraic Properties of BRST Coupled Doublets | Some explanations enlarged, references added | JHEP 0205 (2002) 051 | 10.1088/1126-6708/2002/05/051 | IFUM 693/FT | hep-th | null | We characterize the dependence on doublets of the cohomology of an arbitrary
nilpotent differential s (including BRST differentials and classical linearized
Slavnov-Taylor (ST) operators) in terms of the cohomology of the
doublets-independent component of s. All cohomologies are computed in the space
of local integra... | [
{
"created": "Wed, 16 Jan 2002 16:32:06 GMT",
"version": "v1"
},
{
"created": "Thu, 23 May 2002 08:23:19 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Quadri",
"Andrea",
""
]
] | We characterize the dependence on doublets of the cohomology of an arbitrary nilpotent differential s (including BRST differentials and classical linearized Slavnov-Taylor (ST) operators) in terms of the cohomology of the doublets-independent component of s. All cohomologies are computed in the space of local integrate... | 10.280313 | 8.636377 | 10.550493 | 9.248056 | 10.736296 | 9.178096 | 10.185385 | 9.090345 | 8.883955 | 11.0358 | 9.010766 | 9.656822 | 9.308558 | 8.764211 | 9.430925 | 9.435692 | 9.058619 | 9.136999 | 8.772406 | 9.467885 | 9.143864 |
1201.4697 | Daniel Puigdomenech | Jorge Alfaro, Dom\`enec Espriu, Daniel Puigdom\`enech | Spontaneous generation of geometry in four dimensions | null | Phys. Rev. D 86, 025015 (2012) | 10.1103/PhysRevD.86.025015 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the extension to 4 dimensions of an euclidean 2-dimensional model
that exhibits spontaneous generation of a metric. In this model gravitons
emerge as Goldstone bosons of a global SO(D) X GL(D) symmetry broken down to
SO(D). The microscopic theory can be formulated without having to appeal to any
particular... | [
{
"created": "Mon, 23 Jan 2012 12:13:25 GMT",
"version": "v1"
}
] | 2012-09-17 | [
[
"Alfaro",
"Jorge",
""
],
[
"Espriu",
"Domènec",
""
],
[
"Puigdomènech",
"Daniel",
""
]
] | We present the extension to 4 dimensions of an euclidean 2-dimensional model that exhibits spontaneous generation of a metric. In this model gravitons emerge as Goldstone bosons of a global SO(D) X GL(D) symmetry broken down to SO(D). The microscopic theory can be formulated without having to appeal to any particular s... | 9.425421 | 10.320709 | 9.460402 | 9.505743 | 10.138009 | 9.859648 | 10.402493 | 9.786201 | 9.467982 | 10.544141 | 9.575347 | 9.356529 | 9.127829 | 9.218247 | 8.979277 | 9.173147 | 9.238648 | 9.368711 | 9.341835 | 9.176975 | 9.329401 |
1502.07909 | Peter West | Nicolas Boulanger, Per Sundell and Peter West | Gauge fields and infinite chains of dualities | 37 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the particle states of Maxwell's theory, in $D$ dimensions, can
be represented in an infinite number of ways by using different gauge fields.
Using this result we formulate the dynamics in terms of an infinite set of
duality relations which are first order in space-time derivatives. We derive a
similar r... | [
{
"created": "Fri, 27 Feb 2015 14:26:19 GMT",
"version": "v1"
}
] | 2015-03-02 | [
[
"Boulanger",
"Nicolas",
""
],
[
"Sundell",
"Per",
""
],
[
"West",
"Peter",
""
]
] | We show that the particle states of Maxwell's theory, in $D$ dimensions, can be represented in an infinite number of ways by using different gauge fields. Using this result we formulate the dynamics in terms of an infinite set of duality relations which are first order in space-time derivatives. We derive a similar res... | 10.085979 | 9.435109 | 10.883457 | 9.402782 | 9.322573 | 9.208069 | 9.08335 | 9.445742 | 9.029715 | 10.505666 | 9.611334 | 9.475382 | 9.837021 | 9.280311 | 9.420314 | 9.349545 | 9.067928 | 9.481687 | 9.189274 | 9.809019 | 9.150286 |
1704.03395 | Raoul Letschka | Cesar Gomez and Raoul Letschka | Memory and the Infrared | null | null | 10.1007/JHEP10(2017)010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Memory effects in scattering processes are described in terms of the
asymptotic retarded fields. These fields are completely determined by the
scattering data and the zero mode part is set by the soft photon theorem. The
dressed asymptotic states defining an infrared finite S- matrix for charged
particles can be defi... | [
{
"created": "Tue, 11 Apr 2017 16:18:16 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Sep 2017 22:19:17 GMT",
"version": "v2"
},
{
"created": "Sun, 17 Sep 2017 16:20:56 GMT",
"version": "v3"
}
] | 2017-10-25 | [
[
"Gomez",
"Cesar",
""
],
[
"Letschka",
"Raoul",
""
]
] | Memory effects in scattering processes are described in terms of the asymptotic retarded fields. These fields are completely determined by the scattering data and the zero mode part is set by the soft photon theorem. The dressed asymptotic states defining an infrared finite S- matrix for charged particles can be define... | 19.165392 | 17.132919 | 18.080027 | 15.474112 | 19.929329 | 19.407732 | 19.446949 | 17.375647 | 16.544092 | 19.374575 | 16.041008 | 16.220171 | 16.43239 | 15.668252 | 16.206629 | 16.27359 | 16.711771 | 15.301192 | 15.554095 | 15.901075 | 16.732307 |
2302.02961 | Burkhard Eden | Burkhard Eden, Dennis le Plat, Anne Spiering | Double excitations in the AdS(5)/CFT(4) integrable system and the
Lagrange operator | LaTeX, 18 pp, 3 figures | null | null | HU-EP-23/05 | hep-th | http://creativecommons.org/licenses/by/4.0/ | It is argued that the integrable model for the planar spectrum of the AdS/CFT
correspondence can accommodate for the full spectrum of excitations $D^{\alpha
\dot \alpha}, \phi^{[IJ]}, \psi^I, \bar \psi_I, F^{\alpha \beta}, \tilde
F^{\dot \alpha \dot \beta}$ (with $I,J \in 1 \ldots 4$) if double excitations
are allowe... | [
{
"created": "Mon, 6 Feb 2023 17:45:30 GMT",
"version": "v1"
}
] | 2023-02-07 | [
[
"Eden",
"Burkhard",
""
],
[
"Plat",
"Dennis le",
""
],
[
"Spiering",
"Anne",
""
]
] | It is argued that the integrable model for the planar spectrum of the AdS/CFT correspondence can accommodate for the full spectrum of excitations $D^{\alpha \dot \alpha}, \phi^{[IJ]}, \psi^I, \bar \psi_I, F^{\alpha \beta}, \tilde F^{\dot \alpha \dot \beta}$ (with $I,J \in 1 \ldots 4$) if double excitations are allowed ... | 11.061246 | 12.539557 | 12.578172 | 10.93637 | 11.988285 | 12.615073 | 11.896877 | 11.353157 | 11.280835 | 13.285644 | 11.082636 | 10.998619 | 11.532227 | 10.911742 | 10.82865 | 10.790756 | 10.855606 | 11.044265 | 10.821115 | 11.183744 | 10.869498 |
hep-th/9709132 | null | Jens Hoppe | On the Construction of Zero Energy States in Supersymmetric Matrix
Models | By accident, the wrong file was submitted | null | null | null | hep-th | null | For the SU(N) invariant supersymmetric matrix model related to membranes in 4
space-time dimensions, the general solution to the equation(s)
$Q^{\dagger}\Psi=0$ $(Q\chi =0)$ is determined for N odd. For any such
(bosonic) solution of $Q^{\dagger}\Psi=0$, a (fermionic) $\Phi$ is found that
(formally) satisfies $Q^{\da... | [
{
"created": "Thu, 18 Sep 1997 14:55:03 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Sep 1997 21:10:10 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Hoppe",
"Jens",
""
]
] | For the SU(N) invariant supersymmetric matrix model related to membranes in 4 space-time dimensions, the general solution to the equation(s) $Q^{\dagger}\Psi=0$ $(Q\chi =0)$ is determined for N odd. For any such (bosonic) solution of $Q^{\dagger}\Psi=0$, a (fermionic) $\Phi$ is found that (formally) satisfies $Q^{\dagg... | 8.387743 | 6.669168 | 8.237569 | 7.004391 | 8.024706 | 7.628901 | 7.60608 | 6.865413 | 6.707648 | 8.561357 | 6.729577 | 6.686016 | 8.005262 | 7.127106 | 7.16422 | 7.404187 | 7.006662 | 6.972621 | 7.332073 | 8.130829 | 7.141201 |
1508.02401 | Kurt Hinterbichler | Kurt Hinterbichler, Mehdi Saravani | A Stueckelberg Approach to Quadratic Curvature Gravity and its
Decoupling Limits | 17 pages. v2 minus sign fixed, other small changes | Phys. Rev. D 93, 065006 (2016) | 10.1103/PhysRevD.93.065006 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Curvature squared terms, when added to the Einstein-Hilbert action and
treated non-perturbatively, generically result in the propagation of an extra
massive scalar state and an extra massive spin-2 ghost state. Using the
Stueckelberg trick, we study the high-energy limit in which the mass of the
spin-2 state is taken... | [
{
"created": "Mon, 10 Aug 2015 20:08:55 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Apr 2016 15:57:37 GMT",
"version": "v2"
}
] | 2016-04-27 | [
[
"Hinterbichler",
"Kurt",
""
],
[
"Saravani",
"Mehdi",
""
]
] | Curvature squared terms, when added to the Einstein-Hilbert action and treated non-perturbatively, generically result in the propagation of an extra massive scalar state and an extra massive spin-2 ghost state. Using the Stueckelberg trick, we study the high-energy limit in which the mass of the spin-2 state is taken t... | 10.772295 | 9.368053 | 11.004622 | 9.897448 | 11.330726 | 10.026206 | 9.760952 | 9.168807 | 9.319865 | 11.435323 | 9.778354 | 9.903029 | 9.782309 | 9.374665 | 9.48261 | 9.615116 | 9.417406 | 9.864198 | 9.27809 | 9.783398 | 9.77802 |
2402.00117 | Motoo Suzuki | Daniel Aloni, Eduardo Garc\'ia-Valdecasas, Matthew Reece, Motoo Suzuki | Spontaneously Broken $(-1)$-Form U(1) Symmetries | 42 pages; v2: minor changes, accepted for publication in SciPost | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Spontaneous breaking of symmetries leads to universal phenomena. We extend
this notion to $(-1)$-form U(1) symmetries. The spontaneous breaking is
diagnosed by a dependence of the vacuum energy on a constant background field
$\theta$, which can be probed by the topological susceptibility. This leads to
a reinterpreta... | [
{
"created": "Wed, 31 Jan 2024 19:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 31 Jul 2024 21:00:45 GMT",
"version": "v2"
}
] | 2024-08-02 | [
[
"Aloni",
"Daniel",
""
],
[
"García-Valdecasas",
"Eduardo",
""
],
[
"Reece",
"Matthew",
""
],
[
"Suzuki",
"Motoo",
""
]
] | Spontaneous breaking of symmetries leads to universal phenomena. We extend this notion to $(-1)$-form U(1) symmetries. The spontaneous breaking is diagnosed by a dependence of the vacuum energy on a constant background field $\theta$, which can be probed by the topological susceptibility. This leads to a reinterpretati... | 12.765635 | 11.128269 | 12.127751 | 11.330609 | 11.494066 | 10.444555 | 10.421102 | 11.139705 | 11.142401 | 13.120465 | 10.683375 | 10.60597 | 11.283412 | 11.407037 | 10.820622 | 11.315435 | 10.61678 | 10.703881 | 10.962054 | 11.659457 | 10.941719 |
1602.06878 | Aradhya Shukla | Aradhya Shukla, Kumar Abhinav and Prasanta K. Panigrahi | Conservation Law for Massive Scale-Invariant Photons in Weyl-Invariant
Gravity | 11 pages, title modified, minor corrections, typos fixed, references
updated, no figures | Classical and Quantum Gravity, 33 (2016) 235008 | 10.1088/0264-9381/33/23/235008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is demonstrated that a Stueckelberg-type gauge theory, coupled to the
scalar-tensor theory of gravity, is invariant under both gauge and Weyl
transformations. Unlike the pure Stueckelberg theory, this coupled Lagrangian
has a genuine Weyl symmetry, with a non-vanishing current. The above is true in
the Jordan fram... | [
{
"created": "Mon, 22 Feb 2016 18:08:57 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Feb 2016 07:21:46 GMT",
"version": "v2"
},
{
"created": "Thu, 10 Mar 2016 09:37:07 GMT",
"version": "v3"
},
{
"created": "Wed, 12 Oct 2016 18:13:36 GMT",
"version": "v4"
},
{
"c... | 2016-11-07 | [
[
"Shukla",
"Aradhya",
""
],
[
"Abhinav",
"Kumar",
""
],
[
"Panigrahi",
"Prasanta K.",
""
]
] | It is demonstrated that a Stueckelberg-type gauge theory, coupled to the scalar-tensor theory of gravity, is invariant under both gauge and Weyl transformations. Unlike the pure Stueckelberg theory, this coupled Lagrangian has a genuine Weyl symmetry, with a non-vanishing current. The above is true in the Jordan frame,... | 9.684416 | 8.909774 | 8.677043 | 8.53109 | 8.279159 | 8.700177 | 9.078868 | 8.152287 | 8.679732 | 9.112124 | 8.720658 | 9.097457 | 8.781067 | 8.745654 | 8.658064 | 8.676073 | 8.825668 | 8.435554 | 8.494838 | 8.982471 | 8.966665 |
2108.09453 | Hirohumi Sawayanagi | Hirohumi Sawayanagi | Condensates, massive gauge fields and confinement in the SU(3) gauge
theory | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | SU(3) gauge theory in the nonlinear gauge of the Curci--Ferrari type is
studied. In the low-energy region, ghost condensation and subsequent gauge
field condensation can happen. The latter condensation makes classical gauge
fields massive. If the color electric potential with string is chosen as the
classical gauge f... | [
{
"created": "Sat, 21 Aug 2021 07:36:56 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Nov 2021 01:49:31 GMT",
"version": "v2"
}
] | 2021-11-10 | [
[
"Sawayanagi",
"Hirohumi",
""
]
] | SU(3) gauge theory in the nonlinear gauge of the Curci--Ferrari type is studied. In the low-energy region, ghost condensation and subsequent gauge field condensation can happen. The latter condensation makes classical gauge fields massive. If the color electric potential with string is chosen as the classical gauge fie... | 15.213576 | 14.700745 | 14.121462 | 13.644559 | 15.807126 | 14.094302 | 14.325129 | 13.890834 | 14.343932 | 14.871381 | 14.449907 | 14.121153 | 14.464611 | 13.983643 | 14.30182 | 13.509592 | 14.063951 | 13.901304 | 13.974673 | 14.228066 | 13.914331 |
2406.08422 | Oliver Janssen | Oliver Janssen | KSW criterion in large field models | 15 pages | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We extend the analytic description of complex no-boundary solutions in the
context of inflation to large field models. We discuss the
Kontsevich-Segal-Witten (KSW) criterion and find it is satisfied in small field
models, while in large field models it depends on an integral involving
$V'(\phi)$ over the range of inf... | [
{
"created": "Wed, 12 Jun 2024 17:05:21 GMT",
"version": "v1"
}
] | 2024-06-13 | [
[
"Janssen",
"Oliver",
""
]
] | We extend the analytic description of complex no-boundary solutions in the context of inflation to large field models. We discuss the Kontsevich-Segal-Witten (KSW) criterion and find it is satisfied in small field models, while in large field models it depends on an integral involving $V'(\phi)$ over the range of infla... | 16.024157 | 15.150674 | 15.803023 | 15.294296 | 16.49402 | 15.372064 | 15.178922 | 14.653731 | 15.156822 | 18.059906 | 15.182367 | 14.962347 | 16.663465 | 15.897263 | 15.736099 | 15.349442 | 15.552913 | 15.411672 | 14.864153 | 16.693747 | 15.179161 |
2205.06274 | Matti Jarvinen | Romuald A. Janik, Matti Jarvinen, Hesam Soltanpanahi, Jacob
Sonnenschein | A perfect fluid hydrodynamic picture of domain wall velocities at strong
coupling | 7 pages, 7 figures | null | 10.1103/PhysRevLett.129.081601 | APCTP Pre2022 - 008 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that for a range of strongly coupled theories with a first order
phase transition, the domain wall or bubble velocity can be expressed in a
simple way in terms of a perfect fluid hydrodynamic formula, and thus in terms
of the equation of state. We test the predictions for the domain wall
velocities using the ... | [
{
"created": "Thu, 12 May 2022 18:00:01 GMT",
"version": "v1"
}
] | 2022-08-31 | [
[
"Janik",
"Romuald A.",
""
],
[
"Jarvinen",
"Matti",
""
],
[
"Soltanpanahi",
"Hesam",
""
],
[
"Sonnenschein",
"Jacob",
""
]
] | We show that for a range of strongly coupled theories with a first order phase transition, the domain wall or bubble velocity can be expressed in a simple way in terms of a perfect fluid hydrodynamic formula, and thus in terms of the equation of state. We test the predictions for the domain wall velocities using the ga... | 10.010261 | 8.365874 | 9.169789 | 8.197019 | 8.846357 | 8.930136 | 8.778946 | 8.523134 | 8.657678 | 9.002863 | 8.474187 | 9.029458 | 8.827964 | 8.349305 | 8.890833 | 8.545377 | 8.688462 | 8.851561 | 8.808812 | 9.107605 | 8.401693 |
1512.03362 | Irina Aref'eva | D.S. Ageev, I.Ya. Aref'eva and M.D. Tikhanovskaya | Holographic Dual to Conical Defects: I. Moving Massive Particle | Latex, 40 pages, 24 figures, comments added, some figures improved,
refs added | THEORETICAL AND MATHEMATICAL PHYSICS, 188, 2016, 1038 | 10.1134/S0040577916070060 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study correlation functions of scalar operators on the boundary of the
$AdS_3$ space deformed by moving massive particles in the context of the
AdS/CFT duality. To calculate two-point correlation functions we use the
geodesic approximation and the renormalized image method. We compare results of
the renormalized i... | [
{
"created": "Thu, 10 Dec 2015 18:34:57 GMT",
"version": "v1"
},
{
"created": "Thu, 5 May 2016 16:49:18 GMT",
"version": "v2"
}
] | 2016-12-15 | [
[
"Ageev",
"D. S.",
""
],
[
"Aref'eva",
"I. Ya.",
""
],
[
"Tikhanovskaya",
"M. D.",
""
]
] | We study correlation functions of scalar operators on the boundary of the $AdS_3$ space deformed by moving massive particles in the context of the AdS/CFT duality. To calculate two-point correlation functions we use the geodesic approximation and the renormalized image method. We compare results of the renormalized ima... | 10.411518 | 9.266042 | 10.386477 | 9.264977 | 9.325891 | 9.262034 | 9.248312 | 8.886111 | 9.081743 | 11.270695 | 9.647442 | 9.226728 | 10.227819 | 9.556114 | 9.539174 | 9.294052 | 9.226294 | 9.004441 | 9.446046 | 9.789394 | 9.459044 |
hep-th/9410167 | Chris Hull | C. M. Hull and P. K. Townsend | Unity of Superstring Dualities | 45 pages. Some minor corrections made and some references added | Nucl.Phys.B438:109-137,1995 | 10.1016/0550-3213(94)00559-W | QMW-94-30, R/94/33 | hep-th | null | The effective action for type II string theory compactified on a six torus is
$N=8$ supergravity, which is known to have an $E_{7}$ duality symmetry. We show
that this is broken by quantum effects to a discrete subgroup, $E_7(\Z)$, which
contains both the T-duality group $SO(6,6;\Z)$ and the S-duality group
$SL(2;\Z)... | [
{
"created": "Fri, 21 Oct 1994 16:53:51 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Jan 1995 18:34:49 GMT",
"version": "v2"
}
] | 2009-07-09 | [
[
"Hull",
"C. M.",
""
],
[
"Townsend",
"P. K.",
""
]
] | The effective action for type II string theory compactified on a six torus is $N=8$ supergravity, which is known to have an $E_{7}$ duality symmetry. We show that this is broken by quantum effects to a discrete subgroup, $E_7(\Z)$, which contains both the T-duality group $SO(6,6;\Z)$ and the S-duality group $SL(2;\Z)$.... | 5.259956 | 5.494946 | 6.268805 | 5.215713 | 5.447618 | 5.31846 | 5.425364 | 5.161362 | 5.219437 | 6.155225 | 5.100726 | 5.322395 | 5.537997 | 5.293083 | 5.244842 | 5.149726 | 5.204999 | 5.194442 | 5.334056 | 5.664401 | 5.13223 |
1506.01017 | Nicolas Rey-Le Lorier | Antonio Amariti, Csaba Cs\'aki, Mario Martone, and Nicolas Rey-Le
Lorier | From S-confinement to 3D Chiral Theories: Dressing the Monopoles | 6 pages + appendices and references | Phys. Rev. D 93, 105027 (2016) | 10.1103/PhysRevD.93.105027 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Monopole operators play a central role in 3 dimensional supersymmetric
dualities: a careful understanding of their spectrum is necessary to match
chiral operators on either sides of a conjectured duality. In Chern-Simons
theories ($k\neq0$), monopole operators acquire an electric charge, thus they
need to be "dressed... | [
{
"created": "Tue, 2 Jun 2015 20:00:19 GMT",
"version": "v1"
}
] | 2016-05-25 | [
[
"Amariti",
"Antonio",
""
],
[
"Csáki",
"Csaba",
""
],
[
"Martone",
"Mario",
""
],
[
"Lorier",
"Nicolas Rey-Le",
""
]
] | Monopole operators play a central role in 3 dimensional supersymmetric dualities: a careful understanding of their spectrum is necessary to match chiral operators on either sides of a conjectured duality. In Chern-Simons theories ($k\neq0$), monopole operators acquire an electric charge, thus they need to be "dressed" ... | 9.230376 | 9.059402 | 10.438247 | 8.816446 | 9.957699 | 9.773789 | 9.589631 | 9.285299 | 8.794394 | 9.968405 | 9.205527 | 8.729634 | 9.115054 | 8.683849 | 8.705937 | 8.987767 | 9.111437 | 8.745063 | 8.666459 | 8.760628 | 8.60916 |
2005.07830 | Andrea Erdas | Andrea Erdas (Department of Physics, Loyola University Maryland) | Casimir effect of a Lorentz-violating scalar in magnetic field | 10 pages, no figures | Int.J.Mod.Phys.A 35 (2020) 31, 2050209 | 10.1142/S0217751X20502097 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper I study the Casimir effect caused by a charged and massive
scalar field that breaks Lorentz invariance in a CPT-even, aether-like manner.
I investigate the case of a scalar field that satisfies Dirichlet or mixed
(Dirichlet-Neumann) boundary conditions on a pair of very large plane parallel
plates. The ... | [
{
"created": "Sat, 16 May 2020 00:02:35 GMT",
"version": "v1"
},
{
"created": "Fri, 30 Oct 2020 20:50:03 GMT",
"version": "v2"
}
] | 2020-12-02 | [
[
"Erdas",
"Andrea",
"",
"Department of Physics, Loyola University Maryland"
]
] | In this paper I study the Casimir effect caused by a charged and massive scalar field that breaks Lorentz invariance in a CPT-even, aether-like manner. I investigate the case of a scalar field that satisfies Dirichlet or mixed (Dirichlet-Neumann) boundary conditions on a pair of very large plane parallel plates. The ca... | 6.074893 | 4.993689 | 5.864304 | 5.084485 | 5.450957 | 4.973497 | 5.15472 | 4.962656 | 5.049615 | 6.585072 | 5.389411 | 5.526351 | 5.841187 | 5.573229 | 5.50868 | 5.350145 | 5.420367 | 5.572946 | 5.423925 | 5.766159 | 5.634142 |
1405.7829 | Dmitriy Uvarov | D.V. Uvarov | Conformal higher-spin symmetries in twistor string theory | 20 pages, LaTeX. v2: section 3 undergone major revision, others -
minor improvements including correction of typos. Version accepted to Nuclear
Physics B | Nucl. Phys. B v.889 (2014) pp.207-227 | 10.1016/j.nuclphysb.2014.10.013 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that similarly to massless superparticle, classical global
symmetry of the Berkovits twistor string action is infinite-dimensional. We
identify its superalgebra, whose finite-dimensional subalgebra contains
$psl(4|4,\mathbb R)$ superalgebra. In quantum theory this infinite-dimensional
symmetry breaks down... | [
{
"created": "Fri, 30 May 2014 11:58:36 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Nov 2014 09:57:47 GMT",
"version": "v2"
}
] | 2014-11-12 | [
[
"Uvarov",
"D. V.",
""
]
] | It is shown that similarly to massless superparticle, classical global symmetry of the Berkovits twistor string action is infinite-dimensional. We identify its superalgebra, whose finite-dimensional subalgebra contains $psl(4|4,\mathbb R)$ superalgebra. In quantum theory this infinite-dimensional symmetry breaks down t... | 9.629783 | 8.730699 | 11.436763 | 8.883419 | 9.723113 | 8.534939 | 8.81332 | 9.669542 | 8.654919 | 12.412114 | 8.993413 | 8.479583 | 9.912779 | 8.202913 | 8.695682 | 8.778693 | 9.17944 | 8.506622 | 8.497392 | 9.371468 | 8.673965 |
0804.3973 | Domenico Seminara | Antonio Bassetto (Padua U., INFN), Luca Griguolo (Parma U., INFN),
Fabrizio Pucci (Florence U., INFN) and Domenico Seminara (Florence U., INFN) | Supersymmetric Wilson loops at two loops | 35 pages, 14 figures, typos corrected, references added | JHEP 0806:083,2008 | 10.1088/1126-6708/2008/06/083 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the quantum properties of certain BPS Wilson loops in ${\cal N}=4$
supersymmetric Yang-Mills theory. They belong to a general family, introduced
recently, in which the addition of particular scalar couplings endows generic
loops on $S^3$ with a fraction of supersymmetry. When restricted to $S^2$,
their quant... | [
{
"created": "Thu, 24 Apr 2008 19:52:32 GMT",
"version": "v1"
},
{
"created": "Mon, 5 May 2008 18:39:13 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Bassetto",
"Antonio",
"",
"Padua U., INFN"
],
[
"Griguolo",
"Luca",
"",
"Parma U., INFN"
],
[
"Pucci",
"Fabrizio",
"",
"Florence U., INFN"
],
[
"Seminara",
"Domenico",
"",
"Florence U., INFN"
]
] | We study the quantum properties of certain BPS Wilson loops in ${\cal N}=4$ supersymmetric Yang-Mills theory. They belong to a general family, introduced recently, in which the addition of particular scalar couplings endows generic loops on $S^3$ with a fraction of supersymmetry. When restricted to $S^2$, their quantum... | 10.719176 | 9.442731 | 12.921 | 9.67954 | 10.430799 | 9.316211 | 9.940065 | 8.982078 | 9.726572 | 12.754837 | 9.158755 | 10.03073 | 11.533843 | 10.115243 | 9.903433 | 10.378734 | 9.691998 | 9.880599 | 9.828721 | 10.809519 | 9.948278 |
hep-th/0511104 | David Berenstein | David Berenstein, Diego H. Correa | Emergent geometry from q-deformations of N=4 super Yang-Mills | 22 pages, 1 figure. v2: added references. v3:final published version | JHEP0608:006,2006 | 10.1088/1126-6708/2006/08/006 | NSF-KITP-05-91, CECS-PHY-05/13 | hep-th | null | We study BPS states in a marginal deformation of super Yang-Mills on R x S^3
using a quantum mechanical system of q-commuting matrices. We focus mainly on
the case where the parameter q is a root of unity, so that the AdS dual of the
field theory can be associated to an orbifold of AdS_5x S^5. We show that in
the lar... | [
{
"created": "Wed, 9 Nov 2005 11:50:01 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Nov 2005 13:11:01 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Jun 2006 21:26:14 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Berenstein",
"David",
""
],
[
"Correa",
"Diego H.",
""
]
] | We study BPS states in a marginal deformation of super Yang-Mills on R x S^3 using a quantum mechanical system of q-commuting matrices. We focus mainly on the case where the parameter q is a root of unity, so that the AdS dual of the field theory can be associated to an orbifold of AdS_5x S^5. We show that in the large... | 9.391108 | 9.122543 | 11.337216 | 8.893126 | 10.114327 | 9.560326 | 8.877145 | 9.221958 | 9.602154 | 12.764007 | 8.926158 | 9.097598 | 10.033815 | 9.024728 | 9.372866 | 8.921621 | 9.123401 | 9.082438 | 9.240624 | 9.89279 | 9.124123 |
hep-th/9609024 | Emil Yuzbashyan | Andrei N. Leznov and Emil A. Yuzbashyan | Integrable mappings for noncommuting objects | 11 pages, language improved | Rept. Math. Phys. 43:207-214, (1999) | 10.1016/S0034-4877(99)80028-7 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We construct hierarchies of integrable systems invariant under the
two-dimensional Darboux-Toda mapping for noncommuting objects, thus
generalizing to the noncommutative case the integrable mapping approach to
nonlinear dynamical systems. Besides the usual setup with one time and two
space dimensions, we consider the... | [
{
"created": "Mon, 2 Sep 1996 10:44:48 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Sep 2023 16:14:05 GMT",
"version": "v2"
}
] | 2023-09-06 | [
[
"Leznov",
"Andrei N.",
""
],
[
"Yuzbashyan",
"Emil A.",
""
]
] | We construct hierarchies of integrable systems invariant under the two-dimensional Darboux-Toda mapping for noncommuting objects, thus generalizing to the noncommutative case the integrable mapping approach to nonlinear dynamical systems. Besides the usual setup with one time and two space dimensions, we consider the c... | 16.039951 | 15.543159 | 15.498451 | 15.531798 | 18.4701 | 14.510349 | 16.787109 | 15.37897 | 16.065071 | 20.153734 | 14.663374 | 14.6505 | 15.854864 | 14.919482 | 15.841436 | 14.663146 | 16.09149 | 15.238945 | 15.522751 | 16.230247 | 13.544484 |
1207.3220 | Song He | Bo Feng, Song He | Graphs, determinants and gravity amplitudes | 19 pages, 3 figures | null | 10.1007/JHEP10(2012)121 | AEI-2012-068 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply the matrix-tree theorem to establish a link between various
diagrammatic and determinant expressions, which naturally appear in scattering
amplitudes of gravity theories. Using this link we are able to give a general
graph-theoretical formulation for the tree-level maximally-helicity-violated
gravity amplitu... | [
{
"created": "Fri, 13 Jul 2012 12:34:06 GMT",
"version": "v1"
}
] | 2015-06-05 | [
[
"Feng",
"Bo",
""
],
[
"He",
"Song",
""
]
] | We apply the matrix-tree theorem to establish a link between various diagrammatic and determinant expressions, which naturally appear in scattering amplitudes of gravity theories. Using this link we are able to give a general graph-theoretical formulation for the tree-level maximally-helicity-violated gravity amplitude... | 10.829498 | 10.677606 | 12.222893 | 10.310378 | 9.498786 | 9.803112 | 9.569043 | 9.597787 | 9.169406 | 12.262506 | 9.429961 | 9.912271 | 9.782705 | 9.813857 | 10.202281 | 10.380364 | 9.887673 | 9.999495 | 9.99817 | 9.703713 | 9.995681 |
1812.08758 | Kallosh Renata | Murat Gunaydin and Renata Kallosh | Supersymmetry constraints on U-duality invariant deformations of $N \geq
5$ Supergravity | 24 p, 8 Tables | null | 10.1007/JHEP09(2019)105 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Candidate counterterms break E7 type U-duality symmetry of $N \geq 5$
supergravity theories in four dimensions \cite{Kallosh:2011dp}. A proposal was
made in \cite{Bossard:2011ij} to restore it, starting with a double set of
vector fields and argued that a supersymmetric extension of their proposal
should exist. We sh... | [
{
"created": "Thu, 20 Dec 2018 18:39:47 GMT",
"version": "v1"
},
{
"created": "Sun, 13 Jan 2019 04:26:48 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Aug 2019 04:01:06 GMT",
"version": "v3"
},
{
"created": "Tue, 27 Aug 2019 17:32:04 GMT",
"version": "v4"
}
] | 2019-10-02 | [
[
"Gunaydin",
"Murat",
""
],
[
"Kallosh",
"Renata",
""
]
] | Candidate counterterms break E7 type U-duality symmetry of $N \geq 5$ supergravity theories in four dimensions \cite{Kallosh:2011dp}. A proposal was made in \cite{Bossard:2011ij} to restore it, starting with a double set of vector fields and argued that a supersymmetric extension of their proposal should exist. We show... | 9.552567 | 9.815335 | 10.452948 | 9.77959 | 10.346645 | 10.724049 | 10.23495 | 9.469796 | 9.650976 | 11.635989 | 9.366006 | 9.191371 | 9.378341 | 9.129861 | 9.083395 | 9.012395 | 9.169044 | 9.227688 | 9.355097 | 9.416778 | 9.387127 |
hep-th/9802037 | Yamawaki | Koichi Yamawaki (Nagoya University) | Zero-Mode Problem on the Light Front | 63 pages, LaTex, 3 EPS figures, Lectures given at 10 th Annual Summer
School and Symposium on Nuclear Physics (NUSS 97), ``QCD, Lightcone Physics
and Hadron Phenomenology'', Seoul, Korea, June 23-28, 1997, a minor
correction on cover page | null | null | DPNU-98-07 | hep-th hep-ph nucl-th | null | A series of lectures are given to discuss the zero-mode problem on the
light-front (LF) quantization with special emphasis on the peculiar realization
of the trivial vacuum, the spontaneous symmetry breaking (SSB) and the Lorentz
invariance. We discuss Discrete Light-Cone Quantization (DLCQ) which was first
introduce... | [
{
"created": "Fri, 6 Feb 1998 16:48:37 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Feb 1998 14:20:04 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Yamawaki",
"Koichi",
"",
"Nagoya University"
]
] | A series of lectures are given to discuss the zero-mode problem on the light-front (LF) quantization with special emphasis on the peculiar realization of the trivial vacuum, the spontaneous symmetry breaking (SSB) and the Lorentz invariance. We discuss Discrete Light-Cone Quantization (DLCQ) which was first introduced ... | 11.98047 | 12.770371 | 12.436339 | 11.675674 | 12.331876 | 11.670588 | 12.271318 | 12.104584 | 11.319126 | 13.388596 | 11.93624 | 11.728442 | 11.879935 | 11.600665 | 11.493384 | 12.122889 | 11.858786 | 11.667286 | 11.896849 | 12.049463 | 11.639826 |
hep-th/9906124 | Carlos A. S. Almeida | Deusdedit M. Medeiros, R. R. Landim, C. A. S. Almeida (Departamento de
Fisica-UFC-Brazil) | Non-Chern-Simons Topological Mass Generation in (2+1) Dimensions | 8 pages, no figures, RevTEX | Europhys.Lett.48:610-615,1999 | 10.1209/epl/i1999-00527-x | null | hep-th | null | By dimensional reduction of a massive BF theory, a new topological field
theory is constructed in (2+1) dimensions. Two different topological terms, one
involving a scalar and a Kalb-Ramond fields and another one equivalent to the
four-dimensional BF term, are present. We constructed two actions with these
topologica... | [
{
"created": "Wed, 16 Jun 1999 19:43:04 GMT",
"version": "v1"
}
] | 2019-08-17 | [
[
"Medeiros",
"Deusdedit M.",
"",
"Departamento de\n Fisica-UFC-Brazil"
],
[
"Landim",
"R. R.",
"",
"Departamento de\n Fisica-UFC-Brazil"
],
[
"Almeida",
"C. A. S.",
"",
"Departamento de\n Fisica-UFC-Brazil"
]
] | By dimensional reduction of a massive BF theory, a new topological field theory is constructed in (2+1) dimensions. Two different topological terms, one involving a scalar and a Kalb-Ramond fields and another one equivalent to the four-dimensional BF term, are present. We constructed two actions with these topological ... | 10.22503 | 8.318301 | 9.816122 | 8.465289 | 8.983087 | 8.446886 | 8.584717 | 8.59795 | 8.723615 | 11.146894 | 8.500573 | 8.893983 | 9.672957 | 9.17726 | 9.133022 | 9.300453 | 9.184247 | 9.016213 | 9.032996 | 9.597437 | 9.088679 |
1101.0872 | Yutaka Yoshida | Yutaka Yoshida | Localization of Vortex Partition Functions in $\mathcal{N}=(2,2) $ Super
Yang-Mills theory | 15 pages | null | null | KEK-TH 1433 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article, we study the localizaiton of the partition function of BPS
vortices in $\mathcal{N}=(2,2)$ $U(N)$ super Yang-Mills theory with $N$-flavor
on $\R^2$. The vortex partition function for $\mathcal{N}=(2,2)$ super
Yang-Mills theory is obtained from the one in $\mathcal{N}=(4,4)$ super
Yang-Mills theory by... | [
{
"created": "Wed, 5 Jan 2011 02:43:49 GMT",
"version": "v1"
}
] | 2011-01-06 | [
[
"Yoshida",
"Yutaka",
""
]
] | In this article, we study the localizaiton of the partition function of BPS vortices in $\mathcal{N}=(2,2)$ $U(N)$ super Yang-Mills theory with $N$-flavor on $\R^2$. The vortex partition function for $\mathcal{N}=(2,2)$ super Yang-Mills theory is obtained from the one in $\mathcal{N}=(4,4)$ super Yang-Mills theory by m... | 6.076753 | 5.568409 | 6.438479 | 5.811789 | 5.915902 | 6.209596 | 5.538407 | 5.797288 | 5.547658 | 7.242571 | 5.447632 | 5.34032 | 5.775479 | 5.570248 | 5.30092 | 5.479713 | 5.414577 | 5.652521 | 5.650467 | 6.02292 | 5.419997 |
hep-th/9903242 | Amihay Hanany | Amihay Hanany and Alberto Zaffaroni | Issues on Orientifolds: On the brane construction of gauge theories with
SO(2n) global symmetry | 38 pages, 23 figures, uses bibtex and (provided) utphys.bst | JHEP 9907 (1999) 009 | 10.1088/1126-6708/1999/07/009 | CERN-TH/99-82, MIT-CTP-2845 | hep-th | null | We discuss issues related to orientifolds and the brane realization for gauge
theories with orthogonal and symplectic groups. We specifically discuss the
case of theories with (hidden) global SO(2n) symmetry, from three to six
dimensions. We analyze mirror symmetry for three dimensional N=4 gauge
theories, Brane Box ... | [
{
"created": "Mon, 29 Mar 1999 16:51:28 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Hanany",
"Amihay",
""
],
[
"Zaffaroni",
"Alberto",
""
]
] | We discuss issues related to orientifolds and the brane realization for gauge theories with orthogonal and symplectic groups. We specifically discuss the case of theories with (hidden) global SO(2n) symmetry, from three to six dimensions. We analyze mirror symmetry for three dimensional N=4 gauge theories, Brane Box Mo... | 17.864872 | 17.194408 | 21.753452 | 16.973024 | 18.29426 | 16.763027 | 16.030336 | 16.580629 | 15.767037 | 23.047489 | 15.845852 | 16.720449 | 18.67071 | 16.2715 | 17.132626 | 16.792662 | 17.055822 | 17.182577 | 16.274616 | 17.249983 | 16.462019 |
1704.02863 | Harold Steinacker | Marcus Sperling, Harold C. Steinacker | Covariant 4-dimensional fuzzy spheres, matrix models and higher spin | 41+7 pages, 4 figures | null | 10.1088/1751-8121/aa8295 | UWThPh-2017-08 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study in detail generalized 4-dimensional fuzzy spheres with twisted extra
dimensions. These spheres can be viewed as $SO(5)$-equivariant projections of
quantized coadjoint orbits of $SO(6)$. We show that they arise as solutions in
Yang-Mills matrix models, which naturally leads to higher-spin gauge theories
on $S... | [
{
"created": "Mon, 10 Apr 2017 14:11:25 GMT",
"version": "v1"
}
] | 2017-09-13 | [
[
"Sperling",
"Marcus",
""
],
[
"Steinacker",
"Harold C.",
""
]
] | We study in detail generalized 4-dimensional fuzzy spheres with twisted extra dimensions. These spheres can be viewed as $SO(5)$-equivariant projections of quantized coadjoint orbits of $SO(6)$. We show that they arise as solutions in Yang-Mills matrix models, which naturally leads to higher-spin gauge theories on $S^4... | 12.67485 | 11.529755 | 12.795075 | 11.409732 | 13.333228 | 11.227504 | 11.858865 | 11.090775 | 10.597101 | 14.323718 | 11.446545 | 10.684213 | 11.450707 | 10.66953 | 10.782745 | 10.593124 | 10.744982 | 10.851626 | 10.872977 | 11.940892 | 10.275702 |
hep-th/9311046 | Klaus Lang | Klaus Lang, Werner Ruehl | Critical O(N) - vector nonlinear sigma - models: A resume of their field
structure | 16 pages, Latex. To appear in the Proceedings of the XXII Conference
on Differential Methods in Theoretical Physics, Ixtapa, Mexico, September
20-24, 1993 | null | null | KL-TH-93/23 | hep-th | null | The classification of quasi - primary fields is outlined. It is proved that
the only conserved quasi - primary currents are the energy - momentum tensor
and the O(N) - Noether currents. Derivation of all quasi - primary fields and
the resolution of degeneracy is sketched. Finally the limits d=2 and d=4 of the
space d... | [
{
"created": "Mon, 8 Nov 1993 15:25:35 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Lang",
"Klaus",
""
],
[
"Ruehl",
"Werner",
""
]
] | The classification of quasi - primary fields is outlined. It is proved that the only conserved quasi - primary currents are the energy - momentum tensor and the O(N) - Noether currents. Derivation of all quasi - primary fields and the resolution of degeneracy is sketched. Finally the limits d=2 and d=4 of the space dim... | 7.125488 | 9.556275 | 10.161687 | 8.846172 | 10.643686 | 9.835763 | 10.176377 | 9.13295 | 8.301429 | 9.68452 | 9.316067 | 8.811697 | 9.885147 | 9.017387 | 9.07554 | 8.820478 | 9.049902 | 9.170125 | 9.139114 | 9.310604 | 8.956796 |
hep-th/0012259 | El Mostapha Sahraoui | El Mostapha Sahraoui and El Hassan Saidi | Solitons on compact and noncompact spaces in large noncommutativity | 25 pages, Latex, 1 figure (use epsfig.sty), corrected formula | Class.Quant.Grav.18:3339-3358,2001 | 10.1088/0264-9381/18/17/302 | null | hep-th | null | We study solutions at the minima of scalar field potentials for Moyal spaces
and torii in the large non-commutativity and interprete these solitons in terms
of non-BPS D-branes of string theory. We derive a mass spectrum formula linking
different D-branes together on quantum torii and suggest that it describes
genera... | [
{
"created": "Thu, 28 Dec 2000 18:58:10 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Jan 2001 17:07:51 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Sahraoui",
"El Mostapha",
""
],
[
"Saidi",
"El Hassan",
""
]
] | We study solutions at the minima of scalar field potentials for Moyal spaces and torii in the large non-commutativity and interprete these solitons in terms of non-BPS D-branes of string theory. We derive a mass spectrum formula linking different D-branes together on quantum torii and suggest that it describes general ... | 21.986992 | 20.469349 | 22.555614 | 20.807249 | 21.4352 | 21.814312 | 23.332239 | 22.303688 | 21.15494 | 26.342201 | 21.45225 | 21.118956 | 21.67886 | 20.816994 | 21.573692 | 20.919611 | 20.988453 | 21.568436 | 21.553677 | 22.424101 | 20.293671 |
hep-th/9310178 | null | Yasumasa Imamura | Supercurrents on Asymmetric Orbifolds | 7 pages, Latex, KOBE-TH-93-08 | Prog.Theor.Phys.91:591-598,1994 | 10.1143/PTP.91.591 | null | hep-th | null | We study $E_8 \times E_8$-heterotic string on asymmetric orbifolds associated
with semi-simple simply-laced Lie algebras. Using the fact that $E_6$-model
allows different twists, we present a new N=1 space-time supersymmetric model
whose supercurrent appears from twisted sectors but not untwisted sector.
| [
{
"created": "Wed, 27 Oct 1993 09:28:22 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Imamura",
"Yasumasa",
""
]
] | We study $E_8 \times E_8$-heterotic string on asymmetric orbifolds associated with semi-simple simply-laced Lie algebras. Using the fact that $E_6$-model allows different twists, we present a new N=1 space-time supersymmetric model whose supercurrent appears from twisted sectors but not untwisted sector. | 12.384236 | 9.765886 | 11.924681 | 9.100384 | 9.676897 | 10.261898 | 9.669115 | 8.752851 | 9.200001 | 12.488905 | 9.704926 | 10.604668 | 10.912207 | 10.859609 | 10.976548 | 10.443146 | 10.485411 | 10.316298 | 10.36265 | 11.19476 | 10.04073 |
1005.1911 | A. Yu. Petrov | C. Furtado, J. R. Nascimento, A. Yu. Petrov, A. F. Santos | Dynamical Chern-Simons modified gravity and Friedmann-Robertson-Walker
metric | 11 pages, revised version, new material added | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the conditions for the consistency of the Friedmann-Robertson-Walker
(FRW) metric with the dynamical Chern-Simons modified gravity. It turns out to
be that in this situation the accelerated expansion of the Universe takes
place, with the time dependence of the scale factor turns out to be similar to
the case... | [
{
"created": "Tue, 11 May 2010 19:01:58 GMT",
"version": "v1"
},
{
"created": "Fri, 21 May 2010 13:12:02 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Jul 2011 18:06:55 GMT",
"version": "v3"
}
] | 2011-07-14 | [
[
"Furtado",
"C.",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"Santos",
"A. F.",
""
]
] | We study the conditions for the consistency of the Friedmann-Robertson-Walker (FRW) metric with the dynamical Chern-Simons modified gravity. It turns out to be that in this situation the accelerated expansion of the Universe takes place, with the time dependence of the scale factor turns out to be similar to the case o... | 8.68187 | 7.735656 | 7.690237 | 7.597046 | 7.563181 | 7.321793 | 8.2981 | 7.773138 | 7.544141 | 7.744828 | 7.806241 | 7.830477 | 8.076083 | 7.658412 | 7.817461 | 7.723791 | 7.690499 | 7.616223 | 7.740226 | 7.809156 | 7.81406 |
hep-th/0512214 | Hossein Yavartanoo | Mohsen Alishahiha and Hossein Yavartanoo | On 1/2 BPS Solutions in M-theory | 19 pages, 3 figures, LaTeX, reference added | null | null | IPM/P-2005/086 | hep-th | null | We study singular 1/2 BPS solutions in M-theory using 11-dimensional
superstar solutions. The superstar solutions and their corresponding plane wave
limits could give an insight how one may deform the boundary conditions to get
singular, but still physically acceptable, solutions. Starting from M-theory
solutions wit... | [
{
"created": "Sat, 17 Dec 2005 09:20:25 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jan 2006 11:14:11 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Alishahiha",
"Mohsen",
""
],
[
"Yavartanoo",
"Hossein",
""
]
] | We study singular 1/2 BPS solutions in M-theory using 11-dimensional superstar solutions. The superstar solutions and their corresponding plane wave limits could give an insight how one may deform the boundary conditions to get singular, but still physically acceptable, solutions. Starting from M-theory solutions with ... | 15.842142 | 13.769659 | 17.211426 | 14.051938 | 13.792336 | 14.913146 | 13.49834 | 15.83136 | 12.729999 | 20.680861 | 13.77226 | 14.851548 | 15.572002 | 13.848676 | 13.96034 | 14.060979 | 13.730277 | 14.155154 | 14.020314 | 15.352204 | 13.785499 |
hep-th/0401025 | Martijn Wijnholt | Martijn Wijnholt | Five-Dimensional Gauge Theories and Unitary Matrix Models | 29 p, 4 fig, harvmac | null | null | PUPT-2106 | hep-th | null | The matrix model computations of effective superpotential terms in N=1
supersymmetric gauge theories in four dimensions have been proposed to apply
more generally to gauge theories in higher dimensions. We discuss aspects of
five-dimensional gauge theory compactified on a circle, which leads to a
unitary matrix model... | [
{
"created": "Tue, 6 Jan 2004 20:37:16 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Wijnholt",
"Martijn",
""
]
] | The matrix model computations of effective superpotential terms in N=1 supersymmetric gauge theories in four dimensions have been proposed to apply more generally to gauge theories in higher dimensions. We discuss aspects of five-dimensional gauge theory compactified on a circle, which leads to a unitary matrix model. | 11.090097 | 7.776147 | 10.403113 | 8.406301 | 8.960765 | 8.190339 | 8.447561 | 8.335399 | 7.613525 | 11.655313 | 7.887154 | 8.666289 | 10.75531 | 9.188478 | 9.028054 | 8.929632 | 9.296266 | 9.128201 | 9.029131 | 10.591756 | 8.905171 |
2208.02823 | Sam S. C. Wong | Justin Khoury, Toshifumi Noumi, Mark Trodden, Sam S. C. Wong | Stability of Hairy Black Holes in Shift-Symmetric Scalar-Tensor Theories
via the Effective Field Theory Approach | 25 pages, JCAP version | null | 10.1088/1475-7516/2023/04/035 | null | hep-th astro-ph.CO gr-qc | http://creativecommons.org/licenses/by/4.0/ | Shift-symmetric Horndeski theories admit an interesting class of
Schwarzschild-de Sitter black hole solutions exhibiting time-dependent scalar
hair. The properties of these solutions may be studied via a bottom-up
effective field theory (EFT) based on the background symmetries. This is in
part possible by making use ... | [
{
"created": "Thu, 4 Aug 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Apr 2023 03:33:59 GMT",
"version": "v2"
}
] | 2023-05-01 | [
[
"Khoury",
"Justin",
""
],
[
"Noumi",
"Toshifumi",
""
],
[
"Trodden",
"Mark",
""
],
[
"Wong",
"Sam S. C.",
""
]
] | Shift-symmetric Horndeski theories admit an interesting class of Schwarzschild-de Sitter black hole solutions exhibiting time-dependent scalar hair. The properties of these solutions may be studied via a bottom-up effective field theory (EFT) based on the background symmetries. This is in part possible by making use of... | 8.685508 | 8.267271 | 7.811042 | 7.471359 | 8.382265 | 8.089843 | 8.631577 | 7.549316 | 7.943578 | 8.421058 | 8.283761 | 7.795104 | 7.661005 | 7.640014 | 7.642522 | 7.858856 | 7.782629 | 7.471986 | 7.962006 | 7.802304 | 8.143723 |
hep-th/0509062 | Ulrich Ellwanger | Ulrich Ellwanger | Brane Universes and the Cosmological Constant | corrected typos, added references, 13 pages, accepted by MPLA as
brief review | Mod.Phys.Lett. A20 (2005) 2521-2532 | 10.1142/S0217732305018773 | LPT Orsay 05-51 | hep-th | null | The cosmological constant problem and brane universes are reviewed briefly.
We discuss how the cosmological constant problem manifests itself in various
scenarios for brane universes. We review attempts - and their difficulties -
that aim at a solution of the cosmological constant problem.
| [
{
"created": "Fri, 9 Sep 2005 12:53:08 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Sep 2005 09:21:35 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Ellwanger",
"Ulrich",
""
]
] | The cosmological constant problem and brane universes are reviewed briefly. We discuss how the cosmological constant problem manifests itself in various scenarios for brane universes. We review attempts - and their difficulties - that aim at a solution of the cosmological constant problem. | 10.021132 | 8.79483 | 9.165738 | 8.346621 | 8.474601 | 9.044344 | 7.826862 | 9.13342 | 8.269485 | 8.136875 | 9.093204 | 8.794248 | 9.414479 | 9.07146 | 8.989568 | 9.414505 | 9.102878 | 9.519853 | 9.467275 | 9.183108 | 8.909697 |
1712.02803 | ChunJun Cao | ChunJun Cao, Sean M. Carroll | Bulk Entanglement Gravity without a Boundary: Towards Finding Einstein's
Equation in Hilbert Space | 29 pages, 2 figures | Phys. Rev. D 97, 086003 (2018) | 10.1103/PhysRevD.97.086003 | CALT-TH-2017-069 | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the emergence from quantum entanglement of spacetime geometry in
a bulk region. For certain classes of quantum states in an appropriately
factorized Hilbert space, a spatial geometry can be defined by associating
areas along codimension-one surfaces with the entanglement entropy between
either side. We sh... | [
{
"created": "Thu, 7 Dec 2017 19:00:11 GMT",
"version": "v1"
}
] | 2018-04-11 | [
[
"Cao",
"ChunJun",
""
],
[
"Carroll",
"Sean M.",
""
]
] | We consider the emergence from quantum entanglement of spacetime geometry in a bulk region. For certain classes of quantum states in an appropriately factorized Hilbert space, a spatial geometry can be defined by associating areas along codimension-one surfaces with the entanglement entropy between either side. We show... | 7.456034 | 8.243416 | 8.895798 | 8.082317 | 8.528384 | 8.240808 | 8.169333 | 7.863818 | 8.254457 | 8.769779 | 8.290689 | 7.887295 | 7.874218 | 7.642568 | 7.79698 | 7.98875 | 7.780246 | 7.418906 | 7.848125 | 7.956594 | 7.515705 |
hep-th/0312254 | H{\aa}kon Enger | H. Enger and C.A. L\"utken | Non-linear Yang-Mills instantons from strings are $\pi$-stable D-branes | v3: Minor revision; 14 pages | Nucl.Phys. B695 (2004) 73-83 | 10.1016/j.nuclphysb.2004.06.051 | null | hep-th | null | We show that B-type $\Pi$-stable D-branes do not in general reduce to the
(Gieseker-) stable holomorphic vector bundles used in mathematics to construct
moduli spaces. We show that solutions of the almost Hermitian Yang--Mills
equations for the non-linear deformations of Yang--Mills instantons that appear
in the low-... | [
{
"created": "Sun, 21 Dec 2003 15:54:39 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Apr 2004 14:25:59 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Jun 2004 14:14:53 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Enger",
"H.",
""
],
[
"Lütken",
"C. A.",
""
]
] | We show that B-type $\Pi$-stable D-branes do not in general reduce to the (Gieseker-) stable holomorphic vector bundles used in mathematics to construct moduli spaces. We show that solutions of the almost Hermitian Yang--Mills equations for the non-linear deformations of Yang--Mills instantons that appear in the low-en... | 11.521212 | 13.044835 | 13.474154 | 12.495158 | 13.659284 | 12.750398 | 14.385866 | 13.613978 | 12.590755 | 16.263168 | 12.981128 | 11.442083 | 12.875967 | 11.83647 | 11.273366 | 11.248355 | 11.754959 | 11.519396 | 11.569495 | 12.206558 | 11.430517 |
2210.14196 | Gabriel Wong | Thomas G. Mertens, Joan Sim\'on, Gabriel Wong | A proposal for 3d quantum gravity and its bulk factorization | Revised introduction and summary. Journal version | null | 10.1007/JHEP06(2023)134 | null | hep-th cond-mat.str-el gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent progress in AdS/CFT has provided a good understanding of how the bulk
spacetime is encoded in the entanglement structure of the boundary CFT.
However, little is known about how spacetime emerges directly from the bulk
quantum theory. We address this question in an effective 3d quantum theory of
pure gravity, w... | [
{
"created": "Tue, 25 Oct 2022 17:41:25 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Nov 2022 15:59:34 GMT",
"version": "v2"
},
{
"created": "Sun, 12 Mar 2023 01:49:00 GMT",
"version": "v3"
},
{
"created": "Thu, 20 Jul 2023 20:19:50 GMT",
"version": "v4"
}
] | 2023-07-24 | [
[
"Mertens",
"Thomas G.",
""
],
[
"Simón",
"Joan",
""
],
[
"Wong",
"Gabriel",
""
]
] | Recent progress in AdS/CFT has provided a good understanding of how the bulk spacetime is encoded in the entanglement structure of the boundary CFT. However, little is known about how spacetime emerges directly from the bulk quantum theory. We address this question in an effective 3d quantum theory of pure gravity, whi... | 6.105901 | 5.908335 | 6.517443 | 5.928941 | 6.059059 | 5.857509 | 6.086785 | 5.969991 | 5.646842 | 7.797361 | 5.879431 | 5.804071 | 6.179551 | 5.815819 | 5.827755 | 5.930623 | 5.790474 | 6.055338 | 5.999401 | 6.259903 | 5.881331 |
2202.08127 | Xuhang Jiang | Jiaqi Chen, Xuhang Jiang, Chichuan Ma, Xiaofeng Xu, Li Lin Yang | Baikov representations, intersection theory, and canonical Feynman
integrals | v2: published version in JHEP | null | 10.1007/JHEP07(2022)066 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The method of canonical differential equations is an important tool in the
calculation of Feynman integrals in quantum field theories. It has been
realized that the canonical bases are closely related to $d$-dimensional
$d\log$-form integrands. In this work, we introduce the concept of generalized
loop-by-loop Baikov... | [
{
"created": "Wed, 16 Feb 2022 15:07:06 GMT",
"version": "v1"
},
{
"created": "Sat, 17 Sep 2022 06:18:22 GMT",
"version": "v2"
}
] | 2022-09-28 | [
[
"Chen",
"Jiaqi",
""
],
[
"Jiang",
"Xuhang",
""
],
[
"Ma",
"Chichuan",
""
],
[
"Xu",
"Xiaofeng",
""
],
[
"Yang",
"Li Lin",
""
]
] | The method of canonical differential equations is an important tool in the calculation of Feynman integrals in quantum field theories. It has been realized that the canonical bases are closely related to $d$-dimensional $d\log$-form integrands. In this work, we introduce the concept of generalized loop-by-loop Baikov r... | 7.387788 | 7.666994 | 6.834557 | 6.846309 | 7.163578 | 7.187244 | 7.033174 | 6.739799 | 6.790377 | 7.811837 | 6.817572 | 7.133958 | 6.843606 | 6.800589 | 6.856583 | 7.050832 | 6.843752 | 6.92178 | 6.861368 | 7.094538 | 6.813875 |
2004.04050 | Francesco Becattini | F. Becattini (University of Florence) | Polarization in relativistic fluids: a quantum field theoretical
derivation | 24 pages, 1 figure; version published in Lecture Notes in Physics | null | 10.1007/978-3-030-71427-7_2 | null | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the calculation of polarization in a relativistic fluid within the
framework of statistical quantum field theory. We derive the expressions of the
spin density matrix and the mean spin vector both for a single quantum
relativistic particle and for a quantum free field. After introducing the
formalism of the... | [
{
"created": "Tue, 7 Apr 2020 16:30:44 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Jun 2020 17:56:29 GMT",
"version": "v2"
},
{
"created": "Fri, 28 Jul 2023 17:13:56 GMT",
"version": "v3"
}
] | 2023-07-31 | [
[
"Becattini",
"F.",
"",
"University of Florence"
]
] | We review the calculation of polarization in a relativistic fluid within the framework of statistical quantum field theory. We derive the expressions of the spin density matrix and the mean spin vector both for a single quantum relativistic particle and for a quantum free field. After introducing the formalism of the c... | 10.643668 | 10.271562 | 10.16456 | 9.694683 | 10.67758 | 10.377531 | 11.449034 | 10.16443 | 10.778955 | 11.23293 | 10.177835 | 10.60484 | 10.680631 | 10.350139 | 10.252476 | 10.515025 | 10.386044 | 10.61632 | 10.378144 | 10.684721 | 10.614973 |
1101.1524 | Stephen G. Naculich | Stephen G. Naculich and Howard J. Schnitzer | Eikonal methods applied to gravitational scattering amplitudes | 16 pages, 3 figures; v2: title change and minor rewording (published
version); v3: typos corrected in eqs.(3.2),(4.1) | null | 10.1007/JHEP05(2011)087 | BOW-PH-148, BRX-TH-628 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply factorization and eikonal methods from gauge theories to scattering
amplitudes in gravity. We hypothesize that these amplitudes factor into an
IR-divergent soft function and an IR-finite hard function, with the former
given by the expectation value of a product of gravitational Wilson line
operators. Using t... | [
{
"created": "Fri, 7 Jan 2011 21:01:35 GMT",
"version": "v1"
},
{
"created": "Tue, 17 May 2011 17:13:53 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Jun 2013 19:37:29 GMT",
"version": "v3"
}
] | 2015-05-20 | [
[
"Naculich",
"Stephen G.",
""
],
[
"Schnitzer",
"Howard J.",
""
]
] | We apply factorization and eikonal methods from gauge theories to scattering amplitudes in gravity. We hypothesize that these amplitudes factor into an IR-divergent soft function and an IR-finite hard function, with the former given by the expectation value of a product of gravitational Wilson line operators. Using thi... | 7.126027 | 7.039156 | 6.743091 | 6.029915 | 6.224435 | 6.413216 | 6.557802 | 5.7223 | 6.170557 | 7.6135 | 6.666125 | 6.286508 | 6.605323 | 6.126828 | 5.987504 | 6.79383 | 6.217382 | 6.543488 | 6.043295 | 6.522005 | 6.398529 |
1304.5172 | Michal P. Heller | Michal P. Heller, David Mateos, Wilke van der Schee and Miquel Triana | Holographic isotropization linearized | 30 pages, 14 figures; v2: minor changes in the text, matches the
published version | JHEP 1309:026, 2013 | 10.1007/JHEP09(2013)026 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The holographic isotropization of a highly anisotropic, homogeneous, strongly
coupled, non-Abelian plasma was simplified in arXiv:1202.0981 by linearizing
Einstein's equations around the final, equilibrium state. This approximation
reproduces the expectation value of the boundary stress tensor with a 20%
accuracy. He... | [
{
"created": "Thu, 18 Apr 2013 16:04:09 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Sep 2013 08:01:46 GMT",
"version": "v2"
}
] | 2013-09-11 | [
[
"Heller",
"Michal P.",
""
],
[
"Mateos",
"David",
""
],
[
"van der Schee",
"Wilke",
""
],
[
"Triana",
"Miquel",
""
]
] | The holographic isotropization of a highly anisotropic, homogeneous, strongly coupled, non-Abelian plasma was simplified in arXiv:1202.0981 by linearizing Einstein's equations around the final, equilibrium state. This approximation reproduces the expectation value of the boundary stress tensor with a 20% accuracy. Here... | 10.590925 | 10.207318 | 11.507219 | 10.007394 | 11.041182 | 9.943689 | 9.677705 | 9.648349 | 9.77256 | 12.465579 | 9.838843 | 10.387365 | 10.919263 | 10.299151 | 10.103077 | 10.315311 | 10.887161 | 10.296717 | 10.223475 | 10.992469 | 10.473953 |
1306.3071 | Huaifan Li | Huai-Fan Li | Further studies on holographic insulator/superconductor phase
transitions from Sturm-Liouville eigenvalue problems | 16 page, 4 figures, minor corrections made and Refs. added | Journal High Energy Physics, 2013, (1107): 135 | 10.1007/JHEP07(2013)135 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We take advantage of the Sturm-Liouville eigenvalue problem to analytically
study the holographic insulator/superconductor phase transition in the probe
limit. The interesting point is that this analytical method can not only
estimate the most stable mode of the phase transition, but also the second
stable mode. We f... | [
{
"created": "Thu, 13 Jun 2013 10:40:41 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Jun 2013 09:21:50 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Jul 2013 10:13:33 GMT",
"version": "v3"
}
] | 2013-08-26 | [
[
"Li",
"Huai-Fan",
""
]
] | We take advantage of the Sturm-Liouville eigenvalue problem to analytically study the holographic insulator/superconductor phase transition in the probe limit. The interesting point is that this analytical method can not only estimate the most stable mode of the phase transition, but also the second stable mode. We fin... | 8.748509 | 7.7806 | 8.011455 | 7.491338 | 7.848059 | 7.998059 | 7.729329 | 7.933553 | 7.708702 | 8.737962 | 7.817112 | 7.851353 | 7.98846 | 7.898034 | 7.896936 | 7.881607 | 7.88247 | 7.529626 | 8.007515 | 8.101843 | 8.035414 |
2309.12869 | Daniel Baldwin Mr | Bobby Samir Acharya, Daniel Andrew Baldwin | Coulomb and Higgs Phases of $G_2$-manifolds | 22 pages | null | null | null | hep-th math.DG | http://creativecommons.org/licenses/by/4.0/ | Ricci flat manifolds of special holonomy are a rich framework as models of
the extra dimensions in string/$M$-theory. At special points in vacuum moduli
space, special kinds of singularities occur and demand a physical
interpretation. In this paper we show that the topologically distinct
$G_2$-holonomy manifolds aris... | [
{
"created": "Fri, 22 Sep 2023 13:46:46 GMT",
"version": "v1"
}
] | 2023-09-25 | [
[
"Acharya",
"Bobby Samir",
""
],
[
"Baldwin",
"Daniel Andrew",
""
]
] | Ricci flat manifolds of special holonomy are a rich framework as models of the extra dimensions in string/$M$-theory. At special points in vacuum moduli space, special kinds of singularities occur and demand a physical interpretation. In this paper we show that the topologically distinct $G_2$-holonomy manifolds arisin... | 9.982503 | 10.67308 | 11.106717 | 10.087448 | 10.235994 | 10.501333 | 10.2655 | 10.75558 | 10.044517 | 11.405633 | 9.377327 | 9.142122 | 9.738024 | 9.324808 | 9.657069 | 9.32273 | 9.244476 | 9.530697 | 9.548676 | 9.713309 | 9.293777 |
2305.06034 | Leonardo Castellani | Leonardo Castellani and Pietro Antonio Grassi | Hodge Duality and Supergravity | 30 pages, LaTeX | null | null | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | The Hodge dual operator, recently introduced for supermanifolds, is used to
reformulate super Yang-Mills and supergravity in $D=4$. We first recall the
definition of the Hodge dual operator for flat and curved supermanifolds. Then
we show how to recover the usual super-Yang-Mills equations of motion for
$N=1,2$ super... | [
{
"created": "Wed, 10 May 2023 10:35:15 GMT",
"version": "v1"
}
] | 2023-05-11 | [
[
"Castellani",
"Leonardo",
""
],
[
"Grassi",
"Pietro Antonio",
""
]
] | The Hodge dual operator, recently introduced for supermanifolds, is used to reformulate super Yang-Mills and supergravity in $D=4$. We first recall the definition of the Hodge dual operator for flat and curved supermanifolds. Then we show how to recover the usual super-Yang-Mills equations of motion for $N=1,2$ supersy... | 6.849924 | 6.128812 | 7.269944 | 6.386047 | 6.817352 | 6.187472 | 6.403456 | 6.2804 | 6.36783 | 7.07425 | 6.244109 | 6.540175 | 6.738587 | 6.583901 | 6.675992 | 6.529236 | 6.629744 | 6.491028 | 6.322673 | 6.69881 | 6.416885 |
hep-th/9612179 | Reinhold W. Gebert | R. W. Gebert (IAS, Princeton, U.S.A.) | Beyond the Frenkel-Kac-Segal construction of affine Lie algebras | 6 pages, LaTeX209 with twoside, fleqn, amsmath, amsfonts, amssymb,
amsthm style files; contribution to Proceedings of the 30th Int. Symposium
Ahrenshoop on the Theory of Elementary Particles, Buckow, Germany, August
27-31, 1996 | Nucl.Phys.Proc.Suppl. 56B (1997) 263-268 | 10.1016/S0920-5632(97)00334-4 | null | hep-th | null | This contribution reviews recent progress in constructing affine Lie algebras
at arbitrary level in terms of vertex operators. The string model describes a
completely compactified subcritical chiral bosonic string whose momentum
lattice is taken to be the (Lorentzian) affine weight lattice. The main feature
of the ne... | [
{
"created": "Tue, 17 Dec 1996 15:57:13 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Gebert",
"R. W.",
"",
"IAS, Princeton, U.S.A."
]
] | This contribution reviews recent progress in constructing affine Lie algebras at arbitrary level in terms of vertex operators. The string model describes a completely compactified subcritical chiral bosonic string whose momentum lattice is taken to be the (Lorentzian) affine weight lattice. The main feature of the new ... | 16.242752 | 13.537473 | 17.77951 | 14.177346 | 13.702363 | 14.536388 | 14.895205 | 13.168664 | 12.793029 | 18.768213 | 13.920729 | 14.269014 | 15.842781 | 13.814178 | 14.826949 | 14.474307 | 14.543464 | 13.905625 | 13.63753 | 14.382319 | 14.425381 |
1508.01116 | Stephan Stieberger | Stephan Stieberger, Tomasz R. Taylor | Subleading Terms in the Collinear Limit of Yang-Mills Amplitudes | 8 pages | null | 10.1016/j.physletb.2015.09.075 | MPP-2015-183 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For two massless particles i and j, the collinear limit is a special
kinematic configuration in which the particles propagate with parallel
four-momentum vectors, with the total momentum P distributed as p_i=xP and
p_j=(1-x)P, so that s_{ij}=(p_i+p_j)^2=P^2=0. In Yang-Mills theory, if i and j
are among N gauge bosons... | [
{
"created": "Wed, 5 Aug 2015 16:12:59 GMT",
"version": "v1"
}
] | 2015-10-14 | [
[
"Stieberger",
"Stephan",
""
],
[
"Taylor",
"Tomasz R.",
""
]
] | For two massless particles i and j, the collinear limit is a special kinematic configuration in which the particles propagate with parallel four-momentum vectors, with the total momentum P distributed as p_i=xP and p_j=(1-x)P, so that s_{ij}=(p_i+p_j)^2=P^2=0. In Yang-Mills theory, if i and j are among N gauge bosons p... | 7.505596 | 9.293163 | 8.341603 | 7.723123 | 7.810201 | 8.659662 | 8.58446 | 7.766686 | 7.653235 | 8.86956 | 7.266991 | 7.236629 | 7.258052 | 7.167587 | 7.043257 | 7.215648 | 7.354051 | 7.318699 | 7.211598 | 7.465014 | 7.035938 |
hep-th/0002044 | Daniela | Daniela Bigatti and Leonard Susskind | TASI lectures on the Holographic Principle | LaTex, 37 pages + 20 figures in .eps format (embedded in the paper) | null | 10.1142/9789812799630_0012 | SU-ITP 99-14, KUL-TF-2000/03 | hep-th | null | These TASI lectures review the Holographic principle. The first lecture
describes the puzzle of black hole information loss that led to the idea of
Black Hole Complementarity and subsequently to the Holographic Principle
itself. The second lecture discusses the holographic entropy bound in general
space-times. The fi... | [
{
"created": "Sat, 5 Feb 2000 23:36:12 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Bigatti",
"Daniela",
""
],
[
"Susskind",
"Leonard",
""
]
] | These TASI lectures review the Holographic principle. The first lecture describes the puzzle of black hole information loss that led to the idea of Black Hole Complementarity and subsequently to the Holographic Principle itself. The second lecture discusses the holographic entropy bound in general space-times. The fina... | 8.036196 | 7.104685 | 7.313946 | 7.329018 | 7.383759 | 7.450448 | 7.066199 | 6.840116 | 7.110831 | 8.42054 | 6.819264 | 7.304338 | 7.21623 | 6.893213 | 6.870398 | 7.26271 | 6.932679 | 7.007105 | 6.97105 | 7.217451 | 6.523415 |
1403.0786 | A. Yu. Petrov | J. R. Nascimento, A. Yu. Petrov, C. Wotzasek, C. A. D. Zarro | Three-dimensional Lorentz-violating action | 12 pages, accepted to PRD | Phys. Rev. D 89, 065030 (2014) | 10.1103/PhysRevD.89.065030 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate the generation of the three-dimensional Chern-Simons-like
Lorentz-breaking ``mixed" quadratic action via an appropriate Lorentz-breaking
coupling of vector and scalar fields to the spinor field and study some
features of the scalar QED with such a term. We show that the same term emerges
through a nonp... | [
{
"created": "Tue, 4 Mar 2014 13:37:53 GMT",
"version": "v1"
}
] | 2014-04-29 | [
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"Wotzasek",
"C.",
""
],
[
"Zarro",
"C. A. D.",
""
]
] | We demonstrate the generation of the three-dimensional Chern-Simons-like Lorentz-breaking ``mixed" quadratic action via an appropriate Lorentz-breaking coupling of vector and scalar fields to the spinor field and study some features of the scalar QED with such a term. We show that the same term emerges through a nonper... | 21.533543 | 11.916533 | 21.344765 | 16.561811 | 14.521012 | 14.733899 | 14.67916 | 14.671134 | 14.01779 | 23.044582 | 14.214025 | 17.639187 | 19.525009 | 18.207685 | 16.419632 | 17.210556 | 16.77347 | 16.969023 | 17.418867 | 18.860044 | 18.148941 |
hep-th/9711094 | Sunil Mukhi | Keshav Dasgupta and Sunil Mukhi | BPS Nature of 3-String Junctions | 7 pages, harvmac (b), 3 figures | Phys.Lett. B423 (1998) 261-264 | 10.1016/S0370-2693(98)00140-3 | TIFR/TH/97-58 | hep-th | null | We study BPS-saturated classical solutions for the world-sheet theory of a
D-string in the presence of a point charge. These solutions are interpreted as
describing planar 3-string junctions, which arise because the original D-string
is deformed by the presence of the inserted charge. We compute the angles of
the jun... | [
{
"created": "Thu, 13 Nov 1997 10:54:24 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Dasgupta",
"Keshav",
""
],
[
"Mukhi",
"Sunil",
""
]
] | We study BPS-saturated classical solutions for the world-sheet theory of a D-string in the presence of a point charge. These solutions are interpreted as describing planar 3-string junctions, which arise because the original D-string is deformed by the presence of the inserted charge. We compute the angles of the junct... | 11.21885 | 10.836978 | 11.794289 | 10.058368 | 9.702364 | 9.895741 | 9.339152 | 10.463859 | 10.660408 | 12.073875 | 9.812943 | 10.406173 | 11.355525 | 9.852184 | 9.972541 | 10.554153 | 10.180533 | 9.925641 | 10.223711 | 10.909531 | 9.915251 |
hep-th/0211282 | Konishi | Roberto Auzzi (Scuola Normale Superiore, Pisa), Roberto Grena (Univ.
Pisa), Kenichi Konishi (Univ. Pisa) | Almost Conformal Vacua and Confinement | 27 pages, 11 figures, LaTex file | Nucl.Phys. B653 (2003) 204-226 | 10.1016/S0550-3213(03)00046-4 | IFUP-TH 2002/46 | hep-th | null | Dynamics of confining vacua which appear as deformed superconformal theory
with a non-Abelian gauge symmetry, is studied by taking a concrete example of
the sextet vacua of ${\cal N}=2$, SU(3) gauge theory with $n_f=4$, with equal
quark masses. We show that the low-energy "matter" degrees of freedom of this
theory co... | [
{
"created": "Thu, 28 Nov 2002 17:04:33 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Auzzi",
"Roberto",
"",
"Scuola Normale Superiore, Pisa"
],
[
"Grena",
"Roberto",
"",
"Univ.\n Pisa"
],
[
"Konishi",
"Kenichi",
"",
"Univ. Pisa"
]
] | Dynamics of confining vacua which appear as deformed superconformal theory with a non-Abelian gauge symmetry, is studied by taking a concrete example of the sextet vacua of ${\cal N}=2$, SU(3) gauge theory with $n_f=4$, with equal quark masses. We show that the low-energy "matter" degrees of freedom of this theory cons... | 11.501282 | 10.946011 | 13.365753 | 11.780383 | 10.933764 | 12.958317 | 11.719408 | 10.858858 | 11.172815 | 13.003074 | 10.817826 | 10.529392 | 11.46629 | 10.5512 | 10.980174 | 10.709079 | 10.437814 | 10.995614 | 10.309735 | 11.395825 | 10.594958 |
hep-th/9608078 | Jan De Boer | Jan de Boer and Kostas Skenderis | Covariant Computation of the Low Energy Effective Action of the
Heterotic Superstring | 59 pages, LaTeX, with two figures (needs epsfig) | Nucl.Phys. B481 (1996) 129-187 | 10.1016/S0550-3213(96)90127-3 | ITP-SB-96-40 | hep-th | null | We derive the low energy effective action of the heterotic superstring in
superspace. This is achieved by coupling the covariantly quantized
Green-Schwarz superstring of Berkovits to a curved background and requiring
that the sigma model has superconformal invariance at tree level and at one
loop in $\a'$. Tree level... | [
{
"created": "Mon, 12 Aug 1996 21:29:06 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"de Boer",
"Jan",
""
],
[
"Skenderis",
"Kostas",
""
]
] | We derive the low energy effective action of the heterotic superstring in superspace. This is achieved by coupling the covariantly quantized Green-Schwarz superstring of Berkovits to a curved background and requiring that the sigma model has superconformal invariance at tree level and at one loop in $\a'$. Tree level s... | 5.964283 | 5.036836 | 7.519823 | 5.694992 | 5.291825 | 5.171805 | 5.164986 | 5.060542 | 5.14702 | 7.052267 | 5.268609 | 5.577368 | 6.144569 | 5.495947 | 5.602484 | 5.731642 | 5.642006 | 5.710351 | 5.420452 | 6.14896 | 5.464149 |
hep-th/9212112 | null | A. Brandhuber, M. Langer, M. Schweda, O. Piguet and S.P. Sorella | A short comment on the supersymmetric structure of Chern-Simons theory
in the axial gauge | 7 pages, LATEX, UGVA---DPT 1992/11--793 | Phys.Lett. B300 (1993) 92-95 | 10.1016/0370-2693(93)90753-5 | null | hep-th | null | The topological supersymmetry of the pure Chern-Simons model in three
dimensions is established in the case where the theory is defined in the axial
gauge.
| [
{
"created": "Fri, 18 Dec 1992 13:00:14 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Brandhuber",
"A.",
""
],
[
"Langer",
"M.",
""
],
[
"Schweda",
"M.",
""
],
[
"Piguet",
"O.",
""
],
[
"Sorella",
"S. P.",
""
]
] | The topological supersymmetry of the pure Chern-Simons model in three dimensions is established in the case where the theory is defined in the axial gauge. | 12.086568 | 8.746545 | 12.176292 | 10.803936 | 9.841871 | 9.611643 | 9.819151 | 9.325805 | 8.696755 | 14.377557 | 9.059837 | 9.96023 | 10.430564 | 9.525742 | 9.506222 | 9.678547 | 9.416985 | 9.298071 | 9.557317 | 10.281882 | 9.701272 |
hep-th/0106147 | Dr. Bikash Chandra Paul | B. C. Paul (North Bengal University) and S. Chakraborty (Jadavpur
University) | Inflaton Field and Primordial Blackhole | 5 pages, LaTeX, Submitted to Int. J. Mod. Phys. D | Int.J.Mod.Phys. D11 (2002) 1435-1438 | 10.1142/S0218271802002293 | null | hep-th | null | Primordial black hole formation has been studied using an inflaton field with
a variable cosmological term as the potential.
| [
{
"created": "Sun, 17 Jun 2001 04:02:46 GMT",
"version": "v1"
}
] | 2015-06-25 | [
[
"Paul",
"B. C.",
"",
"North Bengal University"
],
[
"Chakraborty",
"S.",
"",
"Jadavpur\n University"
]
] | Primordial black hole formation has been studied using an inflaton field with a variable cosmological term as the potential. | 29.088642 | 14.943292 | 13.197883 | 13.599556 | 12.848551 | 14.103148 | 16.300226 | 13.842193 | 15.550335 | 13.90974 | 16.816784 | 17.521164 | 15.05494 | 15.800672 | 16.337873 | 17.172232 | 17.315819 | 14.189869 | 18.893822 | 18.005623 | 17.141937 |
hep-th/0401197 | Akikazu Hashimoto | Akikazu Hashimoto and Leopoldo Pando Zayas | Correspondence Principle for Black Holes in Plane Waves | 20 pages, References Added | JHEP 0403:014,2004 | 10.1088/1126-6708/2004/03/014 | MAD-TH-04-1, MCTP-04-04 | hep-th | null | We compare the entropy as a function of energy of excited strings and black
strings in an asymptotically plane wave background at the level of the
correspondence principle. For the plane wave supported by the NSNS 3-form flux,
neither the entropy formula nor the cross-over scale is affected by the
presence of the flu... | [
{
"created": "Mon, 26 Jan 2004 17:32:52 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Apr 2004 22:06:42 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Hashimoto",
"Akikazu",
""
],
[
"Zayas",
"Leopoldo Pando",
""
]
] | We compare the entropy as a function of energy of excited strings and black strings in an asymptotically plane wave background at the level of the correspondence principle. For the plane wave supported by the NSNS 3-form flux, neither the entropy formula nor the cross-over scale is affected by the presence of the flux ... | 7.78681 | 6.57998 | 8.092497 | 6.423689 | 7.587214 | 7.062315 | 7.088823 | 6.442942 | 6.425655 | 9.648365 | 6.532859 | 6.706035 | 7.571826 | 6.641497 | 6.494514 | 6.187232 | 6.509012 | 6.408614 | 6.577288 | 7.398003 | 6.360424 |
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