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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0603239 | Constantinos Papageorgakis | C. Papageorgakis, S. Ramgoolam | On Time-dependent Collapsing Branes and Fuzzy Odd-dimensional Spheres | 35 pages, latex; v2: discussion in Appendix B on the large-N limit of
the associator is modified, main results of paper unchanged | Int.J.Mod.Phys.A21:6055-6086,2006 | 10.1142/S0217751X06034161 | QMUL-PH-05-15 | hep-th | null | We study the time-dependent dynamics of a collection of N
collapsing/expanding D0-branes in type IIA String Theory. We show that the
fuzzy-S^3 and S^5 provide time-dependent solutions to the Matrix Model of
D0-branes and its DBI generalisation. Some intriguing cancellations in the
calculation of the non-abelian DBI M... | [
{
"created": "Thu, 30 Mar 2006 11:06:59 GMT",
"version": "v1"
},
{
"created": "Mon, 29 May 2006 16:50:27 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Papageorgakis",
"C.",
""
],
[
"Ramgoolam",
"S.",
""
]
] | We study the time-dependent dynamics of a collection of N collapsing/expanding D0-branes in type IIA String Theory. We show that the fuzzy-S^3 and S^5 provide time-dependent solutions to the Matrix Model of D0-branes and its DBI generalisation. Some intriguing cancellations in the calculation of the non-abelian DBI Mat... | 11.799739 | 11.901039 | 13.368806 | 12.085098 | 11.475307 | 12.349436 | 12.464729 | 11.260381 | 11.675945 | 14.609571 | 11.855181 | 11.177217 | 12.217282 | 11.398739 | 11.221528 | 10.869566 | 11.196658 | 11.353728 | 11.2697 | 12.758842 | 10.973382 |
1604.01669 | El Hassan Saidi | R.Ahl Laamara, M. Miskaoui, E.H Saidi | MSSM-like from $SU_{5}\times D_{4}$ Models | 48 pages, LaTeX | NPB vol 906 (2016), 1-39 | 10.1016/j.nuclphysb.2016.02.028 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using finite discrete group characters and symmetry breaking by hyperflux as
well as constraints on top- quark family, we study minimal low energy effective
theory following from SU$_{5}\times D_{4}$ models embedded in F-theory with non
abelian flux. Matter curves spectrum of the models is obtained from
SU$_{5}\times... | [
{
"created": "Wed, 6 Apr 2016 15:50:46 GMT",
"version": "v1"
}
] | 2016-04-07 | [
[
"Laamara",
"R. Ahl",
""
],
[
"Miskaoui",
"M.",
""
],
[
"Saidi",
"E. H",
""
]
] | Using finite discrete group characters and symmetry breaking by hyperflux as well as constraints on top- quark family, we study minimal low energy effective theory following from SU$_{5}\times D_{4}$ models embedded in F-theory with non abelian flux. Matter curves spectrum of the models is obtained from SU$_{5}\times S... | 16.157736 | 16.416739 | 16.695454 | 14.731789 | 16.442078 | 17.117134 | 17.025145 | 17.254932 | 13.923531 | 17.493189 | 15.897102 | 15.06024 | 15.263146 | 15.539291 | 15.564701 | 15.298267 | 15.611395 | 15.298778 | 15.093504 | 15.403296 | 15.067827 |
2211.06355 | Gabriel Arenas-Henriquez | Gabriel Arenas-Henriquez, Felipe Diaz, Yerko Novoa | Thermal fluctuations of black holes with non-linear electrodynamics and
charged Renyi entropy | 41 pages, 6 figures. Comments are welcome. V2: minor corrections,
references added. V3: Matches accepted version in JHEP | null | 10.1007/JHEP05(2023)072 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We extend the charged Renyi entropy to a more general holographic scenario.
Coupling an arbitrary non-linear electrodynamics Lagrangian density to AdS
gravity, we analyse the thermodynamic features of non-linearly charged
hyperbolic black holes and the thermal fluctuations in the grand canonical
ensemble. We provide ... | [
{
"created": "Fri, 11 Nov 2022 17:13:59 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Nov 2022 14:26:49 GMT",
"version": "v2"
},
{
"created": "Thu, 4 May 2023 15:06:14 GMT",
"version": "v3"
}
] | 2023-05-31 | [
[
"Arenas-Henriquez",
"Gabriel",
""
],
[
"Diaz",
"Felipe",
""
],
[
"Novoa",
"Yerko",
""
]
] | We extend the charged Renyi entropy to a more general holographic scenario. Coupling an arbitrary non-linear electrodynamics Lagrangian density to AdS gravity, we analyse the thermodynamic features of non-linearly charged hyperbolic black holes and the thermal fluctuations in the grand canonical ensemble. We provide a ... | 11.477745 | 10.959859 | 12.290059 | 11.036792 | 11.253333 | 10.692421 | 11.271735 | 10.925961 | 10.61932 | 12.019238 | 10.607275 | 11.246593 | 11.772968 | 11.338949 | 11.369642 | 11.189418 | 11.017562 | 11.205535 | 11.580913 | 11.42549 | 11.105973 |
1806.09417 | Claudia de Rham | Claudia de Rham and Scott Melville | Gravitational Rainbows: LIGO and Dark Energy at its Cutoff | 6 pages, 1 figure, small edits and references added | Phys. Rev. Lett. 121, 221101 (2018) | 10.1103/PhysRevLett.121.221101 | Imperial/TP/2018/CdR/02 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The recent direct detection of a neutron star merger with optical counterpart
has been used to severely constrain models of dark energy that typically
predict a modification of the speed of gravitational waves. We point out that
the energy scales observed at LIGO, and the particular frequency of the neutron
star even... | [
{
"created": "Mon, 25 Jun 2018 12:28:32 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Dec 2018 16:19:29 GMT",
"version": "v2"
}
] | 2018-12-18 | [
[
"de Rham",
"Claudia",
""
],
[
"Melville",
"Scott",
""
]
] | The recent direct detection of a neutron star merger with optical counterpart has been used to severely constrain models of dark energy that typically predict a modification of the speed of gravitational waves. We point out that the energy scales observed at LIGO, and the particular frequency of the neutron star event,... | 11.063503 | 11.667324 | 11.657881 | 10.642415 | 11.962024 | 11.580722 | 11.645355 | 11.672271 | 10.47696 | 11.558037 | 11.0384 | 10.165581 | 10.7216 | 10.285851 | 10.471004 | 10.627265 | 10.156773 | 10.286158 | 10.346808 | 10.866389 | 10.655714 |
hep-th/9703112 | Kirill Krasnov | John C. Baez and Kirill V. Krasnov | Quantization of Diffeomorphism-Invariant Theories with Fermions | 28 pages, latex, 7 ps-files (included) are needed to process the
source file | J.Math.Phys. 39 (1998) 1251-1271 | 10.1063/1.532400 | CGPG-97/3-5 | hep-th gr-qc | null | We extend ideas developed for the loop representation of quantum gravity to
diffeomorphism-invariant gauge theories coupled to fermions. Let P -> Sigma be
a principal G-bundle over space and let F be a vector bundle associated to P
whose fiber is a sum of continuous unitary irreducible representations of the
compact ... | [
{
"created": "Sun, 16 Mar 1997 18:58:30 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Baez",
"John C.",
""
],
[
"Krasnov",
"Kirill V.",
""
]
] | We extend ideas developed for the loop representation of quantum gravity to diffeomorphism-invariant gauge theories coupled to fermions. Let P -> Sigma be a principal G-bundle over space and let F be a vector bundle associated to P whose fiber is a sum of continuous unitary irreducible representations of the compact co... | 5.894984 | 6.903641 | 6.235219 | 6.145265 | 6.637606 | 6.533302 | 6.872376 | 6.08635 | 6.121952 | 7.094849 | 6.187201 | 6.31705 | 6.007343 | 6.11497 | 6.207529 | 6.349796 | 6.262058 | 5.784147 | 6.211361 | 6.000891 | 5.897732 |
hep-th/9312030 | null | J. Navarro-Salas and C. F. Talavera | Quantum Cosmological Approach to 2d Dilaton Gravity | 19 pages, 2 figures (uuencoded) included, plain Latex, needs
amssymb.sty and psfig.sty, FTUV/93-34 & IFIC/93-34 | Nucl.Phys.B423:686-704,1994 | 10.1016/0550-3213(94)90149-X | null | hep-th | null | We study the canonical quantization of the induced 2d-gravity and the pure
gravity CGHS-model on a closed spatial section. The Wheeler-DeWitt equations
are solved in (spatially homogeneous) choices of the internal time variable and
the space of solutions is properly truncated to provide the physical Hilbert
space. We... | [
{
"created": "Fri, 3 Dec 1993 14:01:00 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Navarro-Salas",
"J.",
""
],
[
"Talavera",
"C. F.",
""
]
] | We study the canonical quantization of the induced 2d-gravity and the pure gravity CGHS-model on a closed spatial section. The Wheeler-DeWitt equations are solved in (spatially homogeneous) choices of the internal time variable and the space of solutions is properly truncated to provide the physical Hilbert space. We e... | 13.754375 | 12.082065 | 13.506114 | 12.075873 | 12.889019 | 13.041575 | 14.589571 | 12.580871 | 13.167352 | 13.422174 | 12.626052 | 13.161609 | 12.787421 | 12.732973 | 13.258452 | 13.08386 | 14.141178 | 12.600221 | 13.612298 | 13.178599 | 13.52127 |
1410.5831 | Shira Chapman Ms. | Igal Arav, Shira Chapman, Yaron Oz | Lifshitz Scale Anomalies | 58 pages, 5 appendices | JHEP 1502 (2015) 078 | 10.1007/JHEP02(2015)078 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyse scale anomalies in Lifshitz field theories, formulated as the
relative cohomology of the scaling operator with respect to foliation
preserving diffeomorphisms. We construct a detailed framework that enables us
to calculate the anomalies for any number of spatial dimensions, and for any
value of the dynamic... | [
{
"created": "Tue, 21 Oct 2014 20:00:33 GMT",
"version": "v1"
}
] | 2015-08-14 | [
[
"Arav",
"Igal",
""
],
[
"Chapman",
"Shira",
""
],
[
"Oz",
"Yaron",
""
]
] | We analyse scale anomalies in Lifshitz field theories, formulated as the relative cohomology of the scaling operator with respect to foliation preserving diffeomorphisms. We construct a detailed framework that enables us to calculate the anomalies for any number of spatial dimensions, and for any value of the dynamical... | 10.906587 | 10.090253 | 11.045648 | 9.997254 | 8.97401 | 9.599373 | 9.786933 | 10.077996 | 9.728326 | 11.355103 | 9.856218 | 9.753428 | 10.594014 | 9.910109 | 10.010871 | 9.979184 | 10.159376 | 9.946732 | 9.886009 | 10.441074 | 10.011365 |
1504.07579 | Luis Apolo | Luis Apolo and Bo Sundborg | Strings from 3D gravity: asymptotic dynamics of AdS$_3$ gravity with
free boundary conditions | 21 pages; v2: typos corrected, published version | JHEP 1506 (2015) 171 | 10.1007/JHEP06(2015)171 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Pure three-dimensional gravity in anti-de Sitter space can be formulated as
an SL(2,R) $\times $ SL(2,R) Chern-Simons theory, and the latter can be reduced
to a WZW theory at the boundary. In this paper we show that AdS$_3$ gravity
with free boundary conditions is described by a string at the boundary whose
target sp... | [
{
"created": "Tue, 28 Apr 2015 17:28:54 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Jul 2015 12:21:08 GMT",
"version": "v2"
}
] | 2015-07-02 | [
[
"Apolo",
"Luis",
""
],
[
"Sundborg",
"Bo",
""
]
] | Pure three-dimensional gravity in anti-de Sitter space can be formulated as an SL(2,R) $\times $ SL(2,R) Chern-Simons theory, and the latter can be reduced to a WZW theory at the boundary. In this paper we show that AdS$_3$ gravity with free boundary conditions is described by a string at the boundary whose target spac... | 7.96747 | 7.306208 | 7.625299 | 6.76841 | 7.397475 | 6.622674 | 7.216164 | 7.143577 | 7.332912 | 8.409769 | 6.990414 | 6.889793 | 6.793039 | 6.939704 | 7.03226 | 7.012493 | 7.001491 | 7.07623 | 7.074943 | 6.881315 | 6.765303 |
hep-th/0308043 | Richard Szabo | E. Langmann, R.J. Szabo and K. Zarembo | Exact Solution of Quantum Field Theory on Noncommutative Phase Spaces | 70 pages AMSTeX | JHEP 0401 (2004) 017 | 10.1088/1126-6708/2004/01/017 | HWM-03-9, EMPG-03-12, ITEP-TH-38/03, UUITP-14/03 | hep-th | null | We present the exact solution of a scalar field theory defined with
noncommuting position and momentum variables. The model describes charged
particles in a uniform magnetic field and with an interaction defined by the
Groenewold-Moyal star-product. Explicit results are presented for all Green's
functions in arbitrar... | [
{
"created": "Wed, 6 Aug 2003 15:40:16 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Langmann",
"E.",
""
],
[
"Szabo",
"R. J.",
""
],
[
"Zarembo",
"K.",
""
]
] | We present the exact solution of a scalar field theory defined with noncommuting position and momentum variables. The model describes charged particles in a uniform magnetic field and with an interaction defined by the Groenewold-Moyal star-product. Explicit results are presented for all Green's functions in arbitrary ... | 8.713131 | 8.039302 | 9.437199 | 8.169119 | 8.686442 | 7.698505 | 8.078027 | 8.134373 | 8.265307 | 10.508857 | 8.173517 | 8.574795 | 9.530584 | 8.689145 | 8.944749 | 8.276209 | 8.396964 | 8.578835 | 8.538414 | 9.607593 | 8.098175 |
1608.05116 | Allen Stern | B. Harms and A. Stern | Spinning $\sigma$-model solitons in $2+1$ Anti-de Sitter space | 15 pages, 6 figures | null | 10.1016/j.physletb.2016.10.075 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain numerical solutions for rotating topological solitons of the
nonlinear $\sigma$-model in three-dimensional Anti-de Sitter space. Two types
of solutions, $i)$ and $ii)$, are found. The $\sigma$-model fields are
everywhere well defined for both types of solutions, but they differ in their
space-time domains. ... | [
{
"created": "Wed, 17 Aug 2016 22:13:20 GMT",
"version": "v1"
},
{
"created": "Sat, 15 Oct 2016 21:09:08 GMT",
"version": "v2"
}
] | 2017-01-04 | [
[
"Harms",
"B.",
""
],
[
"Stern",
"A.",
""
]
] | We obtain numerical solutions for rotating topological solitons of the nonlinear $\sigma$-model in three-dimensional Anti-de Sitter space. Two types of solutions, $i)$ and $ii)$, are found. The $\sigma$-model fields are everywhere well defined for both types of solutions, but they differ in their space-time domains. An... | 9.390782 | 9.241107 | 9.054945 | 8.348907 | 9.224219 | 8.832859 | 8.927767 | 8.06711 | 8.983778 | 8.628571 | 8.635854 | 8.559549 | 8.378664 | 8.49081 | 8.371674 | 8.827282 | 8.337428 | 8.57814 | 8.7981 | 8.552024 | 8.391831 |
0706.3999 | Eugenio R. Bezerra de Mello | R. de Lima Rodrigues, A. F. de Lima, E. R. Bezerra de Mello, V. B.
Bezerra | On Matrix Superpotential and Three-Component Normal Modes | 17 pages, no figure. Paper accepted for publication in Journal of
Physics A: Mathematical and Theoretical | J.Phys.A41:025401,2008 | 10.1088/1751-8113/41/2/025401 | null | hep-th | null | We consider the supersymmetric quantum mechanics (SUSY QM) with three-
component normal modes for the Bogomol'nyi-Prasad-Sommerfield (BPS) states. An
explicit form of the SUSY QM matrix superpotential is presented and the
corresponding three-component bosonic zero-mode eigenfunction is investigated.
| [
{
"created": "Wed, 27 Jun 2007 11:23:41 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Nov 2007 11:28:13 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Rodrigues",
"R. de Lima",
""
],
[
"de Lima",
"A. F.",
""
],
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Bezerra",
"V. B.",
""
]
] | We consider the supersymmetric quantum mechanics (SUSY QM) with three- component normal modes for the Bogomol'nyi-Prasad-Sommerfield (BPS) states. An explicit form of the SUSY QM matrix superpotential is presented and the corresponding three-component bosonic zero-mode eigenfunction is investigated. | 8.095453 | 7.551136 | 8.735877 | 7.387449 | 8.058821 | 7.688829 | 6.958835 | 6.748654 | 7.035057 | 8.881804 | 6.784465 | 7.853682 | 7.915483 | 7.613115 | 7.501281 | 7.262255 | 7.283596 | 7.342683 | 7.718932 | 8.515657 | 7.28773 |
hep-th/9210109 | null | Alexios P. Polychronakos | Lattice Integrable Systems of Haldane-Shastry Type | 8 pages, NTUA 34/92 | Phys.Rev.Lett. 70 (1993) 2329-2331 | 10.1103/PhysRevLett.70.2329 | null | hep-th cond-mat | null | We present a new lattice integrable system in one dimension of the
Haldane-Shastry type. It consists of spins positioned at the static equilibrium
positions of particles in a corresponding classical Calogero system and
interacting through an exchange term with strength inversely proportional to
the square of their di... | [
{
"created": "Tue, 20 Oct 1992 14:47:38 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Polychronakos",
"Alexios P.",
""
]
] | We present a new lattice integrable system in one dimension of the Haldane-Shastry type. It consists of spins positioned at the static equilibrium positions of particles in a corresponding classical Calogero system and interacting through an exchange term with strength inversely proportional to the square of their dist... | 8.567352 | 8.822262 | 11.658507 | 8.569164 | 8.814928 | 8.766599 | 9.635012 | 8.432588 | 9.044342 | 12.214923 | 8.46222 | 9.04355 | 9.777745 | 8.844113 | 8.578572 | 8.500479 | 8.838504 | 8.409014 | 8.506263 | 9.527681 | 8.364703 |
2309.05536 | Jian-Pin Wu | Lin-Yue Bai, Jian-Pin Wu, Zhen-Hua Zhou | Transport properties of a holographic model with novel gauge-axion
coupling | 29 pages, 11 figures, Published version | Phys.Rev.D 108 (2023) 12, 126015 | 10.1103/PhysRevD.108.126015 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the transport properties within a holographic model
characterized by a novel gauge-axion coupling. A key innovation is the
introduction of the direct coupling between axion fields, the antisymmetric
tensor, and the gauge field in our bulk theory. This novel coupling term leads
to the emergence of nondi... | [
{
"created": "Mon, 11 Sep 2023 15:18:43 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Sep 2023 02:00:12 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Dec 2023 02:13:41 GMT",
"version": "v3"
}
] | 2023-12-29 | [
[
"Bai",
"Lin-Yue",
""
],
[
"Wu",
"Jian-Pin",
""
],
[
"Zhou",
"Zhen-Hua",
""
]
] | We investigate the transport properties within a holographic model characterized by a novel gauge-axion coupling. A key innovation is the introduction of the direct coupling between axion fields, the antisymmetric tensor, and the gauge field in our bulk theory. This novel coupling term leads to the emergence of nondiag... | 14.585908 | 12.090949 | 13.243456 | 11.877041 | 11.651432 | 10.860875 | 12.737731 | 12.051049 | 11.47043 | 14.23365 | 12.228335 | 12.305044 | 13.199742 | 12.031757 | 12.632295 | 12.317099 | 12.525451 | 12.135699 | 12.325674 | 13.14338 | 11.880632 |
1808.02165 | Andrew Tolley | Furqan Dar, Claudia de Rham, J. Tate Deskins, John T. Giblin Jr., and
Andrew J. Tolley | Scalar Gravitational Radiation from Binaries: Vainshtein Mechanism in
Time-dependent Systems | 27 pages, 9 figures, 1 table. Minor typos corrected and refs added | null | 10.1088/1361-6382/aaf5e8 | Imperial/TP/2018/CdR/04 | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a full four-dimensional numerical code to study scalar
gravitational radiation emitted from binary systems and probe the Vainshtein
mechanism in situations that break the static and spherical symmetry, relevant
for binary pulsars as well as black holes and neutron stars binaries. The
present study focuses ... | [
{
"created": "Tue, 7 Aug 2018 00:36:02 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Oct 2018 15:47:03 GMT",
"version": "v2"
}
] | 2019-01-09 | [
[
"Dar",
"Furqan",
""
],
[
"de Rham",
"Claudia",
""
],
[
"Deskins",
"J. Tate",
""
],
[
"Giblin",
"John T.",
"Jr."
],
[
"Tolley",
"Andrew J.",
""
]
] | We develop a full four-dimensional numerical code to study scalar gravitational radiation emitted from binary systems and probe the Vainshtein mechanism in situations that break the static and spherical symmetry, relevant for binary pulsars as well as black holes and neutron stars binaries. The present study focuses on... | 12.618617 | 13.817588 | 13.260061 | 12.346297 | 13.111549 | 12.929934 | 12.968842 | 12.81584 | 12.480436 | 14.214859 | 13.061697 | 12.67944 | 12.388176 | 12.576876 | 12.56922 | 13.002474 | 12.714935 | 12.184972 | 12.078383 | 12.58157 | 12.634271 |
1103.3636 | Steven Gubser | Steven S. Gubser | The gauge-string duality and heavy ion collisions | 21 pages | null | 10.1007/s10701-011-9613-9 | PUPT-2367 | hep-th hep-ph physics.hist-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I review at a non-technical level the use of the gauge-string duality to
study aspects of heavy ion collisions, with special emphasis on the trailing
string calculation of heavy quark energy loss. I include some brief
speculations on how variants of the trailing string construction could provide
a toy model of black ... | [
{
"created": "Fri, 18 Mar 2011 14:44:25 GMT",
"version": "v1"
}
] | 2015-05-27 | [
[
"Gubser",
"Steven S.",
""
]
] | I review at a non-technical level the use of the gauge-string duality to study aspects of heavy ion collisions, with special emphasis on the trailing string calculation of heavy quark energy loss. I include some brief speculations on how variants of the trailing string construction could provide a toy model of black ho... | 10.897856 | 7.838672 | 9.247972 | 8.164083 | 9.462024 | 8.664083 | 8.616008 | 8.128462 | 8.424648 | 11.178883 | 7.954901 | 8.799919 | 9.229285 | 9.058826 | 8.512587 | 8.200553 | 8.73035 | 8.408832 | 8.967674 | 9.157862 | 8.611285 |
hep-th/0611205 | Alikram Aliev | Alikram N. Aliev | Gyromagnetic Ratio of Charged Kerr-Anti-de Sitter Black Holes | New section added; 6 pages, RevTex | Class.Quant.Grav.24:4669-4678,2007 | 10.1088/0264-9381/24/18/008 | null | hep-th astro-ph gr-qc | null | We examine the gyromagnetic ratios of rotating and charged AdS black holes in
four and higher spacetime dimensions. We compute the gyromagnetic ratio for
Kerr-AdS black holes with an arbitrary electric charge in four dimensions and
show that it corresponds to g=2 irrespective of the AdS nature of the
spacetime. We al... | [
{
"created": "Sat, 18 Nov 2006 22:13:42 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Jun 2007 06:43:49 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Aug 2007 19:27:25 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Aliev",
"Alikram N.",
""
]
] | We examine the gyromagnetic ratios of rotating and charged AdS black holes in four and higher spacetime dimensions. We compute the gyromagnetic ratio for Kerr-AdS black holes with an arbitrary electric charge in four dimensions and show that it corresponds to g=2 irrespective of the AdS nature of the spacetime. We also... | 5.925867 | 5.413246 | 6.047872 | 5.252363 | 5.932288 | 5.235697 | 5.298599 | 5.209761 | 5.49599 | 6.032428 | 5.4628 | 5.60086 | 5.935173 | 5.476398 | 5.586091 | 5.391914 | 5.746003 | 5.392424 | 5.584334 | 5.720369 | 5.566847 |
hep-th/9208067 | Tetsuji Miwa | Michio Jimbo, Tetsuji Miwa and Yasuhiro Ohta | Structure of the space of states in RSOS models | 18 pages | Int.J.Mod.Phys. A8 (1993) 1457-1478 | 10.1142/S0217751X93000618 | RIMS-893 | hep-th nlin.SI solv-int | null | The restricted solid-on-solid models in the anti-ferromagnetic regime is
studied in the framework of quantum affine algebras. Following the line
developed recently for vertex models, a representation theoretical picture is
presented for the structure of the space of states. The local operators and the
creation/annihi... | [
{
"created": "Thu, 27 Aug 1992 02:38:25 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Jimbo",
"Michio",
""
],
[
"Miwa",
"Tetsuji",
""
],
[
"Ohta",
"Yasuhiro",
""
]
] | The restricted solid-on-solid models in the anti-ferromagnetic regime is studied in the framework of quantum affine algebras. Following the line developed recently for vertex models, a representation theoretical picture is presented for the structure of the space of states. The local operators and the creation/annihila... | 10.580648 | 9.179274 | 12.780011 | 8.241066 | 9.35745 | 9.736833 | 9.276716 | 9.739409 | 10.54295 | 13.996365 | 8.719542 | 8.600282 | 10.92898 | 9.180984 | 9.140919 | 8.932396 | 8.590228 | 9.603521 | 9.172966 | 10.417934 | 8.927525 |
1105.3851 | Gang Chen | Gang Chen and Konstantin G. Savvidy | Spinor formalism for massive fields with half-integral spin | 21 pages, 1 figures | The European Physical Journal C (2012), Volume 72, Issue 3,1952 | 10.1140/epjc/s10052-012-1952-y | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article, we extend the %Weyl-van der Waerden spinor technique for
calculating helicity amplitudes to general massive fields of half-integer
spins. We find that the little group generators can be represented as
first-order differential operators in the spinor formalism. We use the spinor
forms of the generator... | [
{
"created": "Thu, 19 May 2011 12:19:27 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Apr 2012 02:13:40 GMT",
"version": "v2"
}
] | 2012-04-09 | [
[
"Chen",
"Gang",
""
],
[
"Savvidy",
"Konstantin G.",
""
]
] | In this article, we extend the %Weyl-van der Waerden spinor technique for calculating helicity amplitudes to general massive fields of half-integer spins. We find that the little group generators can be represented as first-order differential operators in the spinor formalism. We use the spinor forms of the generators ... | 10.182175 | 9.87904 | 9.829832 | 9.061378 | 9.144721 | 10.058953 | 10.881919 | 9.513148 | 9.245536 | 10.563362 | 9.247253 | 8.988142 | 9.099264 | 8.619876 | 8.939589 | 8.81251 | 9.12428 | 8.907429 | 8.819962 | 9.028029 | 8.983644 |
1311.4882 | Chaolun Wu | Dam Thanh Son and Chaolun Wu | Holographic Spontaneous Parity Breaking and Emergent Hall Viscosity and
Angular Momentum | 55 pages, 1 figure. Version 2: angular momentum calculation revised;
referenced added | JHEP 07 (2014) 076 | 10.1007/JHEP07(2014)076 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the spontaneous parity breaking and generating of Hall viscosity and
angular momentum in holographic p+ip model, which can describe strongly-coupled
chiral superfluid states in many quantum systems. The dual gravity theory, an
SU(2) gauge field minimally coupled to Einstein gravity, is parity-invariant
but a... | [
{
"created": "Tue, 19 Nov 2013 21:00:01 GMT",
"version": "v1"
},
{
"created": "Sat, 30 Aug 2014 11:40:32 GMT",
"version": "v2"
}
] | 2014-09-02 | [
[
"Son",
"Dam Thanh",
""
],
[
"Wu",
"Chaolun",
""
]
] | We study the spontaneous parity breaking and generating of Hall viscosity and angular momentum in holographic p+ip model, which can describe strongly-coupled chiral superfluid states in many quantum systems. The dual gravity theory, an SU(2) gauge field minimally coupled to Einstein gravity, is parity-invariant but all... | 9.401845 | 9.396894 | 9.869712 | 9.097411 | 9.344413 | 9.579695 | 10.150566 | 9.843145 | 9.34176 | 10.302502 | 9.332243 | 9.336984 | 9.414003 | 9.076719 | 9.235067 | 9.256807 | 9.231591 | 8.945607 | 9.248824 | 9.395231 | 9.032938 |
0706.1667 | Alessio Marrani | S. Ferrara, A. Marrani | On the Moduli Space of non-BPS Attractors for N=2 Symmetric Manifolds | 1+11 pages, 4 Tables | Phys.Lett.B652:111-117,2007 | 10.1016/j.physletb.2007.07.001 | CERN-PH-TH/2007-094; UCLA/07/TEP/15 | hep-th | null | We study the ``flat'' directions of non-BPS extremal black hole attractors
for N=2, d=4 supergravities whose vector multiplets' scalar manifold is endowed
with homogeneous symmetric special Kahler geometry. The non-BPS attractors with
non-vanishing central charge have a moduli space described by real special
geometry... | [
{
"created": "Tue, 12 Jun 2007 12:07:16 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Ferrara",
"S.",
""
],
[
"Marrani",
"A.",
""
]
] | We study the ``flat'' directions of non-BPS extremal black hole attractors for N=2, d=4 supergravities whose vector multiplets' scalar manifold is endowed with homogeneous symmetric special Kahler geometry. The non-BPS attractors with non-vanishing central charge have a moduli space described by real special geometry (... | 8.023534 | 6.990617 | 9.349298 | 7.023894 | 6.906217 | 6.467504 | 7.127015 | 6.518333 | 6.778051 | 9.518779 | 6.844512 | 7.603557 | 8.466413 | 7.552933 | 7.440175 | 7.487229 | 7.113947 | 7.669234 | 7.550938 | 8.210581 | 7.134435 |
hep-th/0406143 | Nicholas Halmagyi | Nick Halmagyi, Christian Romelsberger, Nicholas P. Warner | Inherited Duality and Quiver Gauge Theory | 23 pages, 1 figure | Adv.Theor.Math.Phys.10:159-179,2006 | null | null | hep-th | null | We study the duality group of $\hat{A}_{n-1}$ quiver gauge theories,
primarily using their M5-brane construction. For $\mathcal{N}=2$ supersymmetry,
this duality group was first noted by Witten to be the mapping class group of a
torus with $n$ punctures. We find that it is a certain quotient of this group
that acts f... | [
{
"created": "Wed, 16 Jun 2004 21:18:17 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Mar 2005 23:17:13 GMT",
"version": "v2"
}
] | 2017-09-07 | [
[
"Halmagyi",
"Nick",
""
],
[
"Romelsberger",
"Christian",
""
],
[
"Warner",
"Nicholas P.",
""
]
] | We study the duality group of $\hat{A}_{n-1}$ quiver gauge theories, primarily using their M5-brane construction. For $\mathcal{N}=2$ supersymmetry, this duality group was first noted by Witten to be the mapping class group of a torus with $n$ punctures. We find that it is a certain quotient of this group that acts fai... | 4.845943 | 4.948102 | 5.309795 | 4.874108 | 4.820333 | 4.929882 | 4.977814 | 4.971479 | 4.881068 | 5.580167 | 4.717586 | 4.859269 | 5.014648 | 4.830585 | 4.814081 | 4.818477 | 4.779095 | 4.804095 | 4.869907 | 5.094319 | 4.844525 |
hep-th/0503235 | Juraj Bohacik | J. Bohacik and P. Presnajder | Functional integral with "phi^4" term in the action beyond standard
perturbative methods | We clarify the proofs of the formulas, add a discussions of the
mathematical steps | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose the another, in principe nonperturbative, method of the evaluatiom
of the Wiener functional integral for "phi^4" term in the action. We find the
"generalized" Gelfand-Yaglom differential equation implying the functional
integral in the continuum limit.
| [
{
"created": "Wed, 30 Mar 2005 14:07:40 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Dec 2008 11:26:06 GMT",
"version": "v2"
}
] | 2008-12-18 | [
[
"Bohacik",
"J.",
""
],
[
"Presnajder",
"P.",
""
]
] | We propose the another, in principe nonperturbative, method of the evaluatiom of the Wiener functional integral for "phi^4" term in the action. We find the "generalized" Gelfand-Yaglom differential equation implying the functional integral in the continuum limit. | 22.157705 | 24.106007 | 24.913071 | 19.371368 | 19.824612 | 21.895243 | 20.463449 | 20.261057 | 21.729488 | 21.429276 | 19.174528 | 19.385206 | 21.18075 | 19.509987 | 20.556597 | 20.017084 | 19.932846 | 20.348442 | 19.728781 | 21.199198 | 20.358467 |
0705.3847 | Justin F. Vazquez-Poritz | Mirjam Cvetic, Justin F. Vazquez-Poritz | Warped Resolved L^{a,b,c} Cones | 28 pages, 4 figures, additional references | Phys.Rev.D77:126003,2008 | 10.1103/PhysRevD.77.126003 | UPR-1181-T, MIFP-07-03 | hep-th | null | We construct supergravity solutions describing a stack of D3-branes localized
at a point on a blown-up cycle of a resolved L^{a,b,c} cone. The geometry flows
from AdS_5 x L^{a,b,c} to AdS_5 x S^5/Z_k. The corresponding quiver gauge
theory undergoes an RG flow between two superconformal fixed points, which
leads to se... | [
{
"created": "Mon, 28 May 2007 19:53:21 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Feb 2008 17:43:01 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Cvetic",
"Mirjam",
""
],
[
"Vazquez-Poritz",
"Justin F.",
""
]
] | We construct supergravity solutions describing a stack of D3-branes localized at a point on a blown-up cycle of a resolved L^{a,b,c} cone. The geometry flows from AdS_5 x L^{a,b,c} to AdS_5 x S^5/Z_k. The corresponding quiver gauge theory undergoes an RG flow between two superconformal fixed points, which leads to semi... | 9.058099 | 8.506119 | 10.831248 | 8.141404 | 9.083872 | 9.300838 | 8.428359 | 8.011125 | 8.042207 | 12.403293 | 7.959486 | 8.287876 | 9.236763 | 8.466763 | 8.126927 | 8.33676 | 8.19295 | 8.184376 | 8.369752 | 8.717654 | 8.029344 |
2102.11294 | Mike Blake | Mike Blake and Hong Liu | On systems of maximal quantum chaos | 28 pages, 3 figures, v2: minor clarification added, v3: typos
corrected | null | 10.1007/JHEP05(2021)229 | MIT-CTP/5283 | hep-th cond-mat.str-el nlin.CD nucl-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A remarkable feature of chaos in many-body quantum systems is the existence
of a bound on the quantum Lyapunov exponent. An important question is to
understand what is special about maximally chaotic systems which saturate this
bound. Here we provide further evidence for the `hydrodynamic' origin of chaos
in such sys... | [
{
"created": "Mon, 22 Feb 2021 19:00:09 GMT",
"version": "v1"
},
{
"created": "Fri, 14 May 2021 08:55:16 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Jun 2021 11:58:09 GMT",
"version": "v3"
}
] | 2023-01-11 | [
[
"Blake",
"Mike",
""
],
[
"Liu",
"Hong",
""
]
] | A remarkable feature of chaos in many-body quantum systems is the existence of a bound on the quantum Lyapunov exponent. An important question is to understand what is special about maximally chaotic systems which saturate this bound. Here we provide further evidence for the `hydrodynamic' origin of chaos in such syste... | 8.355977 | 9.111747 | 9.235975 | 8.344742 | 8.110826 | 8.335766 | 8.297238 | 8.113393 | 7.894053 | 9.152784 | 8.121253 | 7.53388 | 8.219547 | 8.056082 | 7.911648 | 7.993949 | 7.555615 | 7.851095 | 7.812907 | 8.1819 | 7.478336 |
1512.06418 | Konstantinos Siampos | Ignatios Antoniadis, Jean-Pierre Derendinger, P. Marios Petropoulos,
Konstantinos Siampos | Heisenberg symmetry and hypermultiplet manifolds | 1+24 pages, Latex; v2: few minor changes, NPB version, v3: Correcting
a typo in Eqs. (2.9), (2.10), (2.12) | null | 10.1016/j.nuclphysb.2016.02.021 | CPHT-040.1015 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the emergence of Heisenberg (Bianchi II) algebra in hyper-K\"ahler
and quaternionic spaces. This is motivated by the r\^ole these spaces with this
symmetry play in $\mathcal{N}=2$ hypermultiplet scalar manifolds. We show how
to construct related pairs of hyper-K\"ahler and quaternionic spaces under
general s... | [
{
"created": "Sun, 20 Dec 2015 18:28:44 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Mar 2016 14:37:47 GMT",
"version": "v2"
},
{
"created": "Sun, 3 Dec 2017 09:23:00 GMT",
"version": "v3"
}
] | 2017-12-05 | [
[
"Antoniadis",
"Ignatios",
""
],
[
"Derendinger",
"Jean-Pierre",
""
],
[
"Petropoulos",
"P. Marios",
""
],
[
"Siampos",
"Konstantinos",
""
]
] | We study the emergence of Heisenberg (Bianchi II) algebra in hyper-K\"ahler and quaternionic spaces. This is motivated by the r\^ole these spaces with this symmetry play in $\mathcal{N}=2$ hypermultiplet scalar manifolds. We show how to construct related pairs of hyper-K\"ahler and quaternionic spaces under general sym... | 8.631701 | 8.662452 | 9.427354 | 8.526027 | 8.952862 | 8.933987 | 9.394541 | 8.536125 | 8.610236 | 10.464655 | 8.71893 | 8.370562 | 8.509896 | 8.080594 | 8.098516 | 8.337667 | 8.578257 | 8.137845 | 8.066411 | 8.003192 | 8.114657 |
1101.2935 | Wen-Li Yang | Wen-Li Yang, Xi Chen, Jun Feng, Kun Hao, Ke Wu, Zhan-Ying Yang and
Yao-Zhong Zhang | Drinfeld twist and symmetric Bethe vectors of the open XYZ chain with
non-diagonal boundary terms | Latex file, 25 pages | null | 10.1088/0253-6102/57/1/05 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | With the help of the Drinfeld twist or factorizing F-matrix for the
eight-vertex solid-on-solid (SOS) model, we find that in the F-basis provided
by the twist the two sets of pseudo-particle creation operators simultaneously
take completely symmetric and polarization free form. This allows us to obtain
the explicit a... | [
{
"created": "Sat, 15 Jan 2011 00:55:42 GMT",
"version": "v1"
}
] | 2015-05-27 | [
[
"Yang",
"Wen-Li",
""
],
[
"Chen",
"Xi",
""
],
[
"Feng",
"Jun",
""
],
[
"Hao",
"Kun",
""
],
[
"Wu",
"Ke",
""
],
[
"Yang",
"Zhan-Ying",
""
],
[
"Zhang",
"Yao-Zhong",
""
]
] | With the help of the Drinfeld twist or factorizing F-matrix for the eight-vertex solid-on-solid (SOS) model, we find that in the F-basis provided by the twist the two sets of pseudo-particle creation operators simultaneously take completely symmetric and polarization free form. This allows us to obtain the explicit and... | 17.053854 | 9.164917 | 18.731346 | 11.149372 | 9.449313 | 9.681434 | 9.447027 | 10.090855 | 11.056278 | 18.625355 | 12.140254 | 11.919394 | 14.665163 | 12.663383 | 12.567233 | 12.392756 | 11.783077 | 12.259629 | 13.135761 | 15.037871 | 13.606048 |
hep-th/9701154 | Kalyan Rama | S. Kalyana Rama | Can String Theory Avoid Cosmological Singularities? | 14 pages. Latex file | Phys.Lett. B408 (1997) 91-97 | 10.1016/S0370-2693(97)00795-8 | MRI-PHY/97-2 | hep-th | null | We consider the effective action for strings and describe in detail the
evolution of a four dimensional homogeneous isotropic universe with matter
included. We find that the evolution, which is singular in general, becomes
singularity free if during certain Phase of the evolution, when the scale
factor increases and ... | [
{
"created": "Tue, 28 Jan 1997 07:32:10 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Rama",
"S. Kalyana",
""
]
] | We consider the effective action for strings and describe in detail the evolution of a four dimensional homogeneous isotropic universe with matter included. We find that the evolution, which is singular in general, becomes singularity free if during certain Phase of the evolution, when the scale factor increases and th... | 15.945988 | 16.66914 | 15.778179 | 14.385814 | 15.280238 | 15.199081 | 14.792587 | 14.160531 | 14.395833 | 18.152113 | 14.22873 | 14.029806 | 15.29663 | 14.206898 | 14.64316 | 15.035875 | 14.305613 | 14.312353 | 14.618401 | 15.524834 | 14.178679 |
0706.3151 | Alberto Mariotti | A.Amariti, L.Girardello, A.Mariotti | Meta-stable A_n quiver gauge theories | Minor corrections, reference added, published in JHEP | JHEP 0710:017,2007 | 10.1088/1126-6708/2007/10/017 | null | hep-th | null | We study metastable dynamical breaking of supersymmetry in A_n quiver gauge
theories. We present a general analysis and criteria for the perturbative
existence of metastable vacua in quivers of any length. Different mechanisms of
gauge mediation can be realized.
| [
{
"created": "Thu, 21 Jun 2007 19:21:35 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Oct 2007 17:03:39 GMT",
"version": "v2"
}
] | 2009-04-17 | [
[
"Amariti",
"A.",
""
],
[
"Girardello",
"L.",
""
],
[
"Mariotti",
"A.",
""
]
] | We study metastable dynamical breaking of supersymmetry in A_n quiver gauge theories. We present a general analysis and criteria for the perturbative existence of metastable vacua in quivers of any length. Different mechanisms of gauge mediation can be realized. | 15.472884 | 10.644612 | 13.810085 | 11.358867 | 10.928201 | 11.281714 | 11.57559 | 11.146746 | 10.649281 | 13.602299 | 10.025329 | 11.151322 | 13.880541 | 11.749447 | 11.77947 | 11.067189 | 11.70927 | 11.73783 | 11.712285 | 14.397679 | 11.251451 |
hep-th/9603073 | Katsushi Ito | Katsushi Ito and Sung-Kil Yang | Picard-Fuchs Equations and Prepotentials in $N=2$ Supersymmetric QCD | 14 pages, latex; (To appear in the proceedings of the Workshop
"Frontiers in Quantum Field Theory'', Osaka, Japan, December 14-17, 1995) | null | null | UTHEP-330 | hep-th | null | The Picard-Fuchs equations for $N=2$ supersymmetric $SU(N_{c})$ Yang-Mills
theories with massless hypermultiplets are obtained for $N_{c}=2$ and $3$. For
$SU(2)$ we derive the non-linear differential equations for the prepotentials
and calculate full non-perturbative corrections to the effective gauge coupling
consta... | [
{
"created": "Tue, 12 Mar 1996 11:34:47 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ito",
"Katsushi",
""
],
[
"Yang",
"Sung-Kil",
""
]
] | The Picard-Fuchs equations for $N=2$ supersymmetric $SU(N_{c})$ Yang-Mills theories with massless hypermultiplets are obtained for $N_{c}=2$ and $3$. For $SU(2)$ we derive the non-linear differential equations for the prepotentials and calculate full non-perturbative corrections to the effective gauge coupling constant... | 5.605996 | 4.713404 | 5.770229 | 4.804832 | 4.719337 | 4.583083 | 4.588218 | 4.907241 | 4.795042 | 5.813465 | 4.870557 | 4.980631 | 5.122735 | 5.071162 | 4.983914 | 5.090106 | 5.055688 | 5.057037 | 4.905947 | 5.110772 | 5.028173 |
0707.2786 | Joao M. Baptista | J. M. Baptista | Twisting gauged non-linear sigma-models | 33 pages; v2: small additions, published version | JHEP 0802:096,2008 | 10.1088/1126-6708/2008/02/096 | ITFA-2007-31 | hep-th math.DG | null | We consider gauged sigma-models from a Riemann surface into a Kaehler and
hamiltonian G-manifold X. The supersymmetric N=2 theory can always be twisted
to produce a gauged A-model. This model localizes to the moduli space of
solutions of the vortex equations and computes the Hamiltonian Gromov-Witten
invariants. When... | [
{
"created": "Wed, 18 Jul 2007 19:02:10 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Mar 2008 18:45:49 GMT",
"version": "v2"
}
] | 2009-04-30 | [
[
"Baptista",
"J. M.",
""
]
] | We consider gauged sigma-models from a Riemann surface into a Kaehler and hamiltonian G-manifold X. The supersymmetric N=2 theory can always be twisted to produce a gauged A-model. This model localizes to the moduli space of solutions of the vortex equations and computes the Hamiltonian Gromov-Witten invariants. When t... | 7.151395 | 7.881866 | 10.46879 | 7.494522 | 8.271681 | 7.101545 | 8.337661 | 8.156651 | 6.849086 | 12.274815 | 6.611349 | 7.470089 | 8.719646 | 7.402094 | 7.805669 | 7.320396 | 7.68634 | 7.654257 | 7.198153 | 8.633845 | 7.417561 |
2210.03015 | Alessia Segati | Antonio Amariti, Alessia Segati | Kerr-Newman black holes from $\mathcal{N}=1^*$ | 32 pages | null | 10.1007/JHEP06(2023)216 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The microstate counting of charged rotating AdS$_5$ supersymmetric black
holes has been reformulated in terms of an extremization problem, obtained from
the superconformal index of the 4d dual SCFT. On the gravitational side this
problem corresponds to the attractor mechanism of the theory KK reduced on
AdS$_4$. Such... | [
{
"created": "Thu, 6 Oct 2022 16:03:44 GMT",
"version": "v1"
}
] | 2023-07-26 | [
[
"Amariti",
"Antonio",
""
],
[
"Segati",
"Alessia",
""
]
] | The microstate counting of charged rotating AdS$_5$ supersymmetric black holes has been reformulated in terms of an extremization problem, obtained from the superconformal index of the 4d dual SCFT. On the gravitational side this problem corresponds to the attractor mechanism of the theory KK reduced on AdS$_4$. Such p... | 9.541887 | 9.78808 | 11.095953 | 8.884986 | 9.425136 | 8.946613 | 9.370453 | 8.722947 | 8.391449 | 11.152009 | 8.522376 | 8.647976 | 9.436366 | 8.555526 | 8.79246 | 8.906252 | 8.89464 | 8.753237 | 8.616816 | 9.294648 | 8.744466 |
hep-th/0105251 | Sergio Doplicher | Sergio Doplicher | Spacetime and Fields, a Quantum Texture | LaTeX, 15 pages. Misprints and wording corrected, references added;
change in section 3. Related references: hep-th/0303037, hep-th/0201222,
hep-th/0301100 | Proceedings of the 37th Karpacz Winter School of Theoretical
Physics, 2001, 204-213 | 10.1063/1.1419326 | null | hep-th gr-qc quant-ph | null | We report on joint work, past and in progress, with K.Fredenhagen and with
J.E,Roberts, on the quantum structure of spacetime in the small which is
dictated by the principles of Quantum Mechanics and of General Relativity; we
comment on how these principles point to a deep link between coordinates and
fields. This is... | [
{
"created": "Thu, 24 May 2001 16:21:37 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Mar 2003 18:14:18 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Doplicher",
"Sergio",
""
]
] | We report on joint work, past and in progress, with K.Fredenhagen and with J.E,Roberts, on the quantum structure of spacetime in the small which is dictated by the principles of Quantum Mechanics and of General Relativity; we comment on how these principles point to a deep link between coordinates and fields. This is a... | 12.003565 | 12.847923 | 12.686634 | 11.921156 | 12.822725 | 12.135334 | 13.054492 | 12.044549 | 11.848808 | 12.48282 | 10.993637 | 11.321483 | 12.266641 | 11.422293 | 10.721546 | 11.799933 | 11.781245 | 11.421754 | 11.876925 | 12.417113 | 11.510369 |
0903.1186 | Deger Nihat Sadik | Nihat Sadik Deger and Ali Kaya | Chern-Simons S-Brane Solutions in M-theory and Accelerating Cosmologies | 18 pages, v3: a new static solution and references added, v4:
references added, to appear in JHEP | JHEP 0904:109,2009 | 10.1088/1126-6708/2009/04/109 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct an intersecting S-brane solution of 11-dimensional supergravity
for which the contribution of the Chern-Simons term to the field equations is
non-zero. After studying some of its properties, we consider three different
compactifications (each with 3 separate subcases) of this system to
4-dimensions. Two ... | [
{
"created": "Fri, 6 Mar 2009 10:51:09 GMT",
"version": "v1"
},
{
"created": "Sat, 7 Mar 2009 11:51:59 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Mar 2009 17:57:57 GMT",
"version": "v3"
},
{
"created": "Fri, 24 Apr 2009 13:27:58 GMT",
"version": "v4"
}
] | 2009-05-01 | [
[
"Deger",
"Nihat Sadik",
""
],
[
"Kaya",
"Ali",
""
]
] | We construct an intersecting S-brane solution of 11-dimensional supergravity for which the contribution of the Chern-Simons term to the field equations is non-zero. After studying some of its properties, we consider three different compactifications (each with 3 separate subcases) of this system to 4-dimensions. Two of... | 11.900815 | 11.771683 | 13.255567 | 10.81574 | 11.877636 | 10.480437 | 10.873721 | 9.999482 | 10.613394 | 12.173801 | 10.614009 | 11.703428 | 12.307662 | 11.272176 | 11.82867 | 11.511824 | 11.423548 | 11.387162 | 10.84429 | 11.837133 | 11.087795 |
hep-th/9807143 | Eduardo Ramos | Armen Nersessian and Eduardo Ramos | Massive spinning particles and the geometry of null curves | 11 pages, LaTeX (elsart macros) | Phys.Lett. B445 (1998) 123-128 | 10.1016/S0370-2693(98)01408-7 | null | hep-th | null | We study the simplest geometrical particle model associated with null paths
in four-dimensional Minkowski space-time. The action is given by the
pseudo-arclength of the particle worldline. We show that the reduced classical
phase space of this system coincides with that of a massive spinning particle
of spin $s=\alph... | [
{
"created": "Mon, 20 Jul 1998 09:50:42 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Nersessian",
"Armen",
""
],
[
"Ramos",
"Eduardo",
""
]
] | We study the simplest geometrical particle model associated with null paths in four-dimensional Minkowski space-time. The action is given by the pseudo-arclength of the particle worldline. We show that the reduced classical phase space of this system coincides with that of a massive spinning particle of spin $s=\alpha^... | 7.256292 | 6.991133 | 7.361934 | 6.807724 | 7.448825 | 7.291996 | 7.07849 | 6.830578 | 7.095274 | 7.594763 | 6.831593 | 6.876281 | 7.295756 | 6.970714 | 7.12664 | 6.828511 | 6.982719 | 6.967649 | 6.949511 | 7.205242 | 6.921469 |
hep-th/9303109 | Fiorenzo Bastianelli | Fiorenzo Bastianelli and Ulf Lindstrom | Induced Chiral Supergravities in 2D | 28 pages, TeX, (improved text, unchanged conclusions), USITP-93-04 | Nucl.Phys. B416 (1994) 227-254 | 10.1016/0550-3213(94)90584-3 | null | hep-th | null | We analyze actions for 2D supergravities induced by chiral conformal
supermatter. The latter may be thought as described at the classical level by
superspace actions invariant under super-reparametrization, super-Weyl and
super-Lorentz transformations. Upon quantization various anomalies appear which
characterize the... | [
{
"created": "Fri, 19 Mar 1993 09:12:00 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jul 1993 10:31:49 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Bastianelli",
"Fiorenzo",
""
],
[
"Lindstrom",
"Ulf",
""
]
] | We analyze actions for 2D supergravities induced by chiral conformal supermatter. The latter may be thought as described at the classical level by superspace actions invariant under super-reparametrization, super-Weyl and super-Lorentz transformations. Upon quantization various anomalies appear which characterize the n... | 10.950927 | 9.892524 | 11.628703 | 9.953522 | 10.631178 | 10.37242 | 10.135032 | 10.232395 | 9.911623 | 12.647968 | 9.71452 | 10.392628 | 10.665878 | 10.459619 | 10.240926 | 10.689633 | 10.662642 | 10.367904 | 10.406159 | 10.828522 | 10.111663 |
1301.2017 | Ardian Nata Atmaja | Ardian Nata Atmaja | Application of Harmonic Maps $CP^{(N-1)}$ on SU(N) Bogomolny Equation
for BPS Magnetic Monopoles | Master Thesis, 48 pages, two figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this thesis we study dynamic of magnetic monopoles from Lagrangian density
in Yang-Mills-Higgs field theory. In particular, we discuss BPS (Bogomolny
Prasad Sommerfield) magnetic monopoles, described by SU(N) Bogomolny equations,
which has field equations in form of non-linear coupled matrix field equations.
One o... | [
{
"created": "Thu, 10 Jan 2013 02:40:06 GMT",
"version": "v1"
}
] | 2013-01-11 | [
[
"Atmaja",
"Ardian Nata",
""
]
] | In this thesis we study dynamic of magnetic monopoles from Lagrangian density in Yang-Mills-Higgs field theory. In particular, we discuss BPS (Bogomolny Prasad Sommerfield) magnetic monopoles, described by SU(N) Bogomolny equations, which has field equations in form of non-linear coupled matrix field equations. One of ... | 9.481119 | 9.105239 | 9.202481 | 8.412313 | 9.52921 | 10.440011 | 10.000041 | 9.494377 | 9.041028 | 9.38588 | 8.767659 | 8.616857 | 8.722968 | 8.784739 | 8.831467 | 8.920605 | 8.629577 | 8.743176 | 8.768978 | 9.36395 | 9.146853 |
2104.11661 | Alesandro Santos | G. X. A. Petronilo, R. G. G. Amorim, S. C. Ulhoa, A. F. Santos, A. E.
Santana and Faqir C. Khanna | Size-effect at finite temperature in a quark-antiquark effective model
in phase space | 20 pages, 5 figures, accepted for publication in IJMPA | null | 10.1142/S0217751X21501219 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | A quark-antiquark effective model is studied in a toroidal topology at finite
temperature. The model is described by a Schr\"odinger equation with linear
potential which is embedded in a torus. The following aspects are analysed: (i)
the nonclassicality structure using the Wigner function formalism; (ii) finite
tempe... | [
{
"created": "Fri, 23 Apr 2021 15:25:22 GMT",
"version": "v1"
}
] | 2021-07-07 | [
[
"Petronilo",
"G. X. A.",
""
],
[
"Amorim",
"R. G. G.",
""
],
[
"Ulhoa",
"S. C.",
""
],
[
"Santos",
"A. F.",
""
],
[
"Santana",
"A. E.",
""
],
[
"Khanna",
"Faqir C.",
""
]
] | A quark-antiquark effective model is studied in a toroidal topology at finite temperature. The model is described by a Schr\"odinger equation with linear potential which is embedded in a torus. The following aspects are analysed: (i) the nonclassicality structure using the Wigner function formalism; (ii) finite tempera... | 11.199958 | 11.408565 | 10.358838 | 10.312863 | 11.467173 | 11.358537 | 11.410872 | 10.882643 | 10.320613 | 10.736498 | 10.689422 | 10.009227 | 10.186936 | 10.125515 | 10.114163 | 9.974284 | 9.991306 | 9.993189 | 10.001419 | 10.101896 | 9.9733 |
0710.1833 | David Kutasov | Amit Giveon and David Kutasov | Stable and Metastable Vacua in Brane Constructions of SQCD | 28 pages, 10 figures | JHEP 0802:038,2008 | 10.1088/1126-6708/2008/02/038 | null | hep-th | null | In a recent paper [1] we showed that N=1 supersymmetric QCD in the presence
of certain superpotential deformations has a rich landscape of supersymmetric
and non-supersymmetric vacua. In this paper we embed this theory in string
theory as a low energy theory of intersecting NS and D-branes. We find that in
the region... | [
{
"created": "Tue, 9 Oct 2007 17:42:26 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Giveon",
"Amit",
""
],
[
"Kutasov",
"David",
""
]
] | In a recent paper [1] we showed that N=1 supersymmetric QCD in the presence of certain superpotential deformations has a rich landscape of supersymmetric and non-supersymmetric vacua. In this paper we embed this theory in string theory as a low energy theory of intersecting NS and D-branes. We find that in the region o... | 7.436922 | 6.326345 | 7.599097 | 6.977212 | 6.620649 | 6.482223 | 6.659675 | 6.634532 | 6.559311 | 7.103332 | 6.717258 | 7.083324 | 7.451986 | 7.009008 | 6.956498 | 6.782514 | 6.997261 | 6.829049 | 6.873133 | 7.042408 | 6.870423 |
hep-th/0505002 | Gonzalo Torroba MsC | C. D. Fosco, G. Torroba | Zero modes in non local domain walls | Latex. 10 pages, 2 figures | Phys.Lett. B620 (2005) 174-179 | 10.1016/j.physletb.2005.06.039 | null | hep-th | null | We generalize the Callan-Harvey mechanism to the case of actions with a non
local mass term for the fermions. Using a 2+1-dimensional model as a concrete
example, we show that both the existence and properties of localized zero modes
can also be consistently studied when the mass is non local. We derive some
general ... | [
{
"created": "Fri, 29 Apr 2005 23:42:42 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Fosco",
"C. D.",
""
],
[
"Torroba",
"G.",
""
]
] | We generalize the Callan-Harvey mechanism to the case of actions with a non local mass term for the fermions. Using a 2+1-dimensional model as a concrete example, we show that both the existence and properties of localized zero modes can also be consistently studied when the mass is non local. We derive some general pr... | 12.715054 | 11.434674 | 12.315432 | 11.139112 | 11.88408 | 11.832813 | 11.659939 | 12.158552 | 11.431771 | 13.48564 | 11.025081 | 10.926332 | 11.360543 | 10.835087 | 11.120214 | 11.786679 | 11.395815 | 10.283809 | 11.07838 | 11.369967 | 11.434598 |
hep-th/9309081 | null | J.-G. Demers | Hermiticity and the Cohomology Condition in Topological Yang-Mills
Theory | 19 pages, MIT-CTP 2233 | Annals Phys. 233 (1994) 281-294 | 10.1006/aphy.1994.1069 | null | hep-th | null | The symmetries of the topological Yang-Mills theory are studied in the
Hamiltonian formalism and the generators of the twisted N=2 superPoincar\'e
algebra are explicitly constructed. Noting that the twisted Lorentz generators
do not generate the Lorentz symmetry of the theory, we relate the two by
extracting from the... | [
{
"created": "Tue, 14 Sep 1993 21:45:32 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Demers",
"J. -G.",
""
]
] | The symmetries of the topological Yang-Mills theory are studied in the Hamiltonian formalism and the generators of the twisted N=2 superPoincar\'e algebra are explicitly constructed. Noting that the twisted Lorentz generators do not generate the Lorentz symmetry of the theory, we relate the two by extracting from the l... | 9.220567 | 8.301999 | 9.182885 | 8.307442 | 8.725871 | 7.97249 | 7.855171 | 7.850801 | 8.104845 | 9.634407 | 7.96861 | 8.473118 | 8.896262 | 8.335595 | 7.981326 | 8.239178 | 8.242841 | 8.314687 | 8.400299 | 8.975541 | 8.260477 |
hep-th/0507194 | Joohan Lee | Soon-Tae Hong, Joohan Lee, Tae Hoon Lee, Phillial Oh | N=4 Supersymmetric Quantum Mechanics with Magnetic Monopole | 7 pages | Phys.Lett. B628 (2005) 165-170 | 10.1016/j.physletb.2005.09.024 | null | hep-th | null | We propose an N=4 supersymmetric quantum mechanics of a charged particle on a
sphere in the background of Dirac magnetic monopole and study the system using
the CP(1) model approach. We explicitly calculate the symmetry algebra taking
the operator ordering ambiguity into consideration. We find that it is given by
the... | [
{
"created": "Wed, 20 Jul 2005 13:39:46 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Hong",
"Soon-Tae",
""
],
[
"Lee",
"Joohan",
""
],
[
"Lee",
"Tae Hoon",
""
],
[
"Oh",
"Phillial",
""
]
] | We propose an N=4 supersymmetric quantum mechanics of a charged particle on a sphere in the background of Dirac magnetic monopole and study the system using the CP(1) model approach. We explicitly calculate the symmetry algebra taking the operator ordering ambiguity into consideration. We find that it is given by the s... | 8.234628 | 7.854449 | 8.372886 | 7.021476 | 7.526706 | 7.459322 | 7.710867 | 7.454365 | 7.386229 | 9.389155 | 7.518741 | 7.460024 | 8.036859 | 7.667357 | 7.383815 | 7.59747 | 7.450488 | 7.603985 | 7.596556 | 8.085905 | 7.258322 |
hep-th/0409043 | Yutaka Sakamura | Yutaka Sakamura | Geometry mediated supersymmetry breaking | 4 pages, contribution to the Proceedings of the 12th International
Conference on Supersymmetry and Unification of the Fundamental Interactions,
June 17-23, 2004, Tsukuba, Japan | null | null | KAIST-TH 2004/12 | hep-th | null | We investigate SUSY breaking mediated through the deformation of the
spacetime geometry due to the backreaction of a nontrivial configuration of a
bulk scalar field. To illustrate its features, we work with a toy model in
which the bulk is four dimensions. Using the superconformal formulation of
SUGRA, we provide a s... | [
{
"created": "Fri, 3 Sep 2004 11:00:35 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Sakamura",
"Yutaka",
""
]
] | We investigate SUSY breaking mediated through the deformation of the spacetime geometry due to the backreaction of a nontrivial configuration of a bulk scalar field. To illustrate its features, we work with a toy model in which the bulk is four dimensions. Using the superconformal formulation of SUGRA, we provide a sys... | 10.986084 | 7.856018 | 9.344411 | 8.361433 | 7.438956 | 8.360353 | 7.744601 | 8.66928 | 8.218497 | 10.374738 | 8.635379 | 9.98089 | 10.027731 | 9.557271 | 9.840759 | 9.584956 | 9.563911 | 9.535602 | 9.890108 | 10.640583 | 9.656104 |
hep-th/9511090 | Jose Gaite | Jose Gaite and Denjoe O'Connor | Field Theory Entropy, the $H$-theorem and the Renormalization Group | 25 pages, plain TeX (macros included), 6 ps figures. Addition in
title. Entropy of cutoff Gaussian model modified in section 4 to avoid a
divergence. Therefore, last figure modified. Other minor changes to improve
readability. Version to appear in Phys. Rev. D | Phys.Rev.D54:5163-5173,1996 | 10.1103/PhysRevD.54.5163 | DIAS-STP-95-36, ITFA-94-36 | hep-th adap-org cond-mat nlin.AO | null | We consider entropy and relative entropy in Field theory and establish
relevant monotonicity properties with respect to the couplings. The relative
entropy in a field theory with a hierarchy of renormalization group fixed
points ranks the fixed points, the lowest relative entropy being assigned to
the highest multicr... | [
{
"created": "Mon, 13 Nov 1995 22:29:48 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Jul 1996 19:48:16 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Gaite",
"Jose",
""
],
[
"O'Connor",
"Denjoe",
""
]
] | We consider entropy and relative entropy in Field theory and establish relevant monotonicity properties with respect to the couplings. The relative entropy in a field theory with a hierarchy of renormalization group fixed points ranks the fixed points, the lowest relative entropy being assigned to the highest multicrit... | 16.539202 | 13.802028 | 16.926344 | 13.898719 | 14.173657 | 12.720536 | 12.414796 | 14.20558 | 13.980789 | 19.489899 | 13.841516 | 14.864606 | 16.021189 | 15.391727 | 15.06428 | 15.150919 | 14.883699 | 15.769401 | 14.579473 | 16.349247 | 14.904934 |
hep-th/9806041 | null | Changhyun Ahn, Kyungho Oh and Radu Tatar | Branes, Orbifolds and the Three Dimensional ${\cal N} = 2$ SCFT in the
Large N limit | Latex, 11 pages, final version | JHEP 9811 (1998) 024 | 10.1088/1126-6708/1998/11/024 | SNUTP-98-045, APCTP-98-018, UM-TG-209 | hep-th | null | We study the correspondence between the large $N$ limit of ${\cal N} = 2$
three dimensional superconformal field theories and M theory on orbifolds of
$AdS_4 \times {\bf S^7}$. We identify the brane configuration which gives
$C^3/Z_3$ as a background for the M theory in terms of a Brane Box Model or a
(p, q) web mode... | [
{
"created": "Thu, 4 Jun 1998 19:20:33 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jun 1998 02:51:41 GMT",
"version": "v2"
},
{
"created": "Thu, 11 Jun 1998 15:07:15 GMT",
"version": "v3"
},
{
"created": "Wed, 6 Jan 1999 23:54:28 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Ahn",
"Changhyun",
""
],
[
"Oh",
"Kyungho",
""
],
[
"Tatar",
"Radu",
""
]
] | We study the correspondence between the large $N$ limit of ${\cal N} = 2$ three dimensional superconformal field theories and M theory on orbifolds of $AdS_4 \times {\bf S^7}$. We identify the brane configuration which gives $C^3/Z_3$ as a background for the M theory in terms of a Brane Box Model or a (p, q) web model.... | 7.321101 | 6.439031 | 9.230953 | 6.037251 | 6.265051 | 6.28457 | 6.450109 | 6.160892 | 5.996134 | 8.569226 | 6.077425 | 6.567759 | 7.664348 | 6.626373 | 7.018988 | 6.705667 | 6.536942 | 6.69038 | 6.387077 | 7.634227 | 6.366416 |
hep-th/9410080 | null | L.Maiani and M.Testa | Causality in Local Quantum Field Theory | compressed uu encoded ps file, 9 pages, Roma 1044 | Phys. Lett. B356 (1995) 319 | 10.1016/0370-2693(95)00800-Z | null | hep-th hep-ph | null | The problem of causality is analyzed in the context of Local Quantum Field
Theory. Contrary to recent claims, it is shown that apparent noncausal
behaviour is due to a lack of the notion of sharp localizability for a
relativistic quantum system. (Replaced corrupted file)
| [
{
"created": "Tue, 11 Oct 1994 18:26:00 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Oct 1994 19:50:00 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Maiani",
"L.",
""
],
[
"Testa",
"M.",
""
]
] | The problem of causality is analyzed in the context of Local Quantum Field Theory. Contrary to recent claims, it is shown that apparent noncausal behaviour is due to a lack of the notion of sharp localizability for a relativistic quantum system. (Replaced corrupted file) | 16.794714 | 14.306619 | 12.325589 | 12.558305 | 15.41246 | 14.808211 | 14.069139 | 12.427113 | 13.324156 | 14.675982 | 14.014812 | 14.520721 | 13.844764 | 14.192461 | 14.842589 | 14.249592 | 14.638284 | 14.797853 | 13.845298 | 14.458149 | 14.346602 |
0706.3658 | Jerzy Kowalski-Glikman | L. Freidel, J. Kowalski-Glikman and S. Nowak | Field theory on $\kappa$--Minkowski space revisited: Noether charges and
breaking of Lorentz symmetry | 22 pages, 1 figure, formulas in sect. III corrected | Int.J.Mod.Phys.A23:2687-2718,2008 | 10.1142/S0217751X08040421 | null | hep-th | null | This paper is devoted to detailed investigations of free scalar field theory
on $\kappa$-Minkowski space. After reviewing necessary mathematical tools we
discuss in depth the Lagrangian and solutions of field equations. We analyze
the spacetime symmetries of the model and construct the conserved charges
associated wi... | [
{
"created": "Mon, 25 Jun 2007 14:39:17 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jul 2007 09:46:25 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Freidel",
"L.",
""
],
[
"Kowalski-Glikman",
"J.",
""
],
[
"Nowak",
"S.",
""
]
] | This paper is devoted to detailed investigations of free scalar field theory on $\kappa$-Minkowski space. After reviewing necessary mathematical tools we discuss in depth the Lagrangian and solutions of field equations. We analyze the spacetime symmetries of the model and construct the conserved charges associated with... | 9.041166 | 8.256742 | 9.188198 | 8.549671 | 8.403687 | 8.184694 | 8.371634 | 8.667351 | 8.502507 | 9.451959 | 8.073271 | 8.091675 | 9.016639 | 8.380629 | 8.415279 | 8.668145 | 8.454643 | 8.535925 | 8.272929 | 9.046002 | 8.191379 |
1602.01382 | Emanuel Scheidegger | Johanna Knapp, Mauricio Romo, Emanuel Scheidegger | Hemisphere Partition Function and Analytic Continuation to the Conifold
Point | 65 pages | null | null | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the hemisphere partition function for certain U(1) gauged linear
sigma models (GLSMs) with D-branes is related to a particular set of
Mellin-Barnes integrals which can be used for analytic continuation to the
singular point in the K\"ahler moduli space of an $h^{1,1}=1$ Calabi-Yau (CY)
projective hypersu... | [
{
"created": "Wed, 3 Feb 2016 17:32:31 GMT",
"version": "v1"
}
] | 2016-02-04 | [
[
"Knapp",
"Johanna",
""
],
[
"Romo",
"Mauricio",
""
],
[
"Scheidegger",
"Emanuel",
""
]
] | We show that the hemisphere partition function for certain U(1) gauged linear sigma models (GLSMs) with D-branes is related to a particular set of Mellin-Barnes integrals which can be used for analytic continuation to the singular point in the K\"ahler moduli space of an $h^{1,1}=1$ Calabi-Yau (CY) projective hypersurf... | 7.374295 | 7.684016 | 9.045383 | 7.194863 | 7.229209 | 7.558514 | 6.677962 | 7.340406 | 6.892114 | 10.027122 | 6.803791 | 6.659563 | 7.461645 | 6.886444 | 6.939867 | 6.855345 | 6.999191 | 6.72589 | 6.859013 | 7.752239 | 6.595573 |
1704.04255 | Yang Zhang | Jorrit Bosma, Mads Sogaard, Yang Zhang | Maximal Cuts in Arbitrary Dimension | typos corrected, more references added | null | 10.1007/JHEP08(2017)051 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a systematic procedure for computing maximal unitarity cuts of
multiloop Feynman integrals in arbitrary dimension. Our approach is based on
the Baikov representation in which the structure of the cuts is particularly
simple. We examine several planar and nonplanar integral topologies and
demonstrate that t... | [
{
"created": "Thu, 13 Apr 2017 19:04:52 GMT",
"version": "v1"
},
{
"created": "Sat, 27 May 2017 02:21:15 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Bosma",
"Jorrit",
""
],
[
"Sogaard",
"Mads",
""
],
[
"Zhang",
"Yang",
""
]
] | We develop a systematic procedure for computing maximal unitarity cuts of multiloop Feynman integrals in arbitrary dimension. Our approach is based on the Baikov representation in which the structure of the cuts is particularly simple. We examine several planar and nonplanar integral topologies and demonstrate that the... | 12.253396 | 12.744466 | 13.084459 | 11.71729 | 12.8004 | 12.689509 | 12.382017 | 12.524528 | 12.094821 | 13.396991 | 12.165088 | 12.51009 | 11.881663 | 11.682188 | 11.791226 | 12.26743 | 12.281507 | 12.238019 | 11.5928 | 12.298512 | 11.564845 |
hep-th/0509030 | Duoje Jia | Duoje Jia | Dual Superconductivity from Yang-Mills Theory via Connection
Decomposition | null | null | null | NWNU-PHY20050102 | hep-th | null | We derive an Abelian-Higgs-like action from SU(2) Yang-Mills theory via
monopole-condensation assumption. Abelian projection as well as
chromo-'electric-magnetic' duality are naturally realized by separating the
small off-diagonal gluon part from diagonal gluon field according to the order
of inverse coupling constan... | [
{
"created": "Sat, 3 Sep 2005 08:00:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Jia",
"Duoje",
""
]
] | We derive an Abelian-Higgs-like action from SU(2) Yang-Mills theory via monopole-condensation assumption. Abelian projection as well as chromo-'electric-magnetic' duality are naturally realized by separating the small off-diagonal gluon part from diagonal gluon field according to the order of inverse coupling constant(... | 14.689338 | 16.63434 | 17.307915 | 14.652278 | 15.701818 | 15.722107 | 16.336491 | 15.618432 | 14.796121 | 16.880199 | 14.571202 | 14.212088 | 14.721965 | 14.631978 | 14.90834 | 14.462514 | 13.930373 | 14.809097 | 14.469057 | 14.551823 | 13.763964 |
hep-th/9907112 | Marco Serone | Claudio A. Scrucca and Marco Serone | Anomaly cancellation in K3 orientifolds | 39 pages, LaTex, 1 figure; minor misprints corrected | Nucl.Phys. B564 (2000) 555-590 | 10.1016/S0550-3213(99)00643-4 | UvA-WINS-Wisk-99-10; LMU-TPW 99-13 | hep-th | null | We study in detail the pattern of anomaly cancellation in D=6 Type IIB Z_N
orientifolds, occurring through a generalized Green-Schwarz mechanism involving
several RR antisymmetric tensors and scalars fields. The starting point is a
direct string theory computation of the inflow of anomaly arising from magnetic
intera... | [
{
"created": "Wed, 14 Jul 1999 18:46:59 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Jul 1999 14:23:56 GMT",
"version": "v2"
},
{
"created": "Wed, 6 Oct 1999 11:48:08 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Scrucca",
"Claudio A.",
""
],
[
"Serone",
"Marco",
""
]
] | We study in detail the pattern of anomaly cancellation in D=6 Type IIB Z_N orientifolds, occurring through a generalized Green-Schwarz mechanism involving several RR antisymmetric tensors and scalars fields. The starting point is a direct string theory computation of the inflow of anomaly arising from magnetic interact... | 13.481976 | 12.768666 | 15.247779 | 12.299622 | 13.1547 | 12.637551 | 13.208275 | 13.082641 | 12.292764 | 15.11145 | 12.059036 | 12.009645 | 12.550268 | 11.812502 | 11.876615 | 12.030022 | 12.40899 | 12.206026 | 12.046907 | 12.933159 | 12.270457 |
2305.04730 | Ioannis Kalogerakis PhD | Ioannis Kalogerakis | A study of Bosonic and Fermionic Theories at Large Charge | doctoral thesis | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The aim of this thesis is to systematically and consistently study strongly
coupled bosonic and fermionic conformal field theories using the large quantum
number expansion. The idea behind it is to study sectors of conformal field
theories that are characterised by large quantum numbers under global
symmetries. In th... | [
{
"created": "Mon, 8 May 2023 14:29:46 GMT",
"version": "v1"
},
{
"created": "Tue, 9 May 2023 08:09:52 GMT",
"version": "v2"
}
] | 2023-05-10 | [
[
"Kalogerakis",
"Ioannis",
""
]
] | The aim of this thesis is to systematically and consistently study strongly coupled bosonic and fermionic conformal field theories using the large quantum number expansion. The idea behind it is to study sectors of conformal field theories that are characterised by large quantum numbers under global symmetries. In this... | 11.082197 | 11.146132 | 10.681747 | 9.315744 | 10.824149 | 11.123221 | 10.987857 | 11.152189 | 10.49487 | 11.495481 | 10.053468 | 9.612079 | 9.916058 | 9.691852 | 9.904324 | 9.987984 | 9.595239 | 9.890119 | 9.564671 | 10.129006 | 9.733336 |
1208.3968 | Takahisa Igata | Takahisa Igata, Hideki Ishihara, Keisuke Nishiwaki | Stationary Closed Strings in Five-dimensional Flat Spacetime | 22 pages, 17 figures | null | 10.1103/PhysRevD.86.104020 | OCU-PHYS 368, AP-GR-99 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate stationary rotating closed Nambu-Goto strings in
five-dimensional flat spacetime. The stationary string is defined as a
worldsheet that is tangent to a timelike Killing vector. Nambu-Goto equation of
motion for the stationary string is reduces to the geodesic equation on the
orbit space of the isometry... | [
{
"created": "Mon, 20 Aug 2012 10:37:42 GMT",
"version": "v1"
}
] | 2013-05-30 | [
[
"Igata",
"Takahisa",
""
],
[
"Ishihara",
"Hideki",
""
],
[
"Nishiwaki",
"Keisuke",
""
]
] | We investigate stationary rotating closed Nambu-Goto strings in five-dimensional flat spacetime. The stationary string is defined as a worldsheet that is tangent to a timelike Killing vector. Nambu-Goto equation of motion for the stationary string is reduces to the geodesic equation on the orbit space of the isometry g... | 7.043035 | 6.623612 | 6.357227 | 6.381844 | 6.897198 | 6.32095 | 6.505434 | 6.626912 | 6.112638 | 6.687003 | 6.482326 | 6.712601 | 6.613153 | 6.660236 | 6.867835 | 6.667307 | 6.747075 | 6.802186 | 6.419113 | 6.726426 | 6.526337 |
1312.4518 | I. V. Kanatchikov | I.V. Kanatchikov | On the precanonical structure of the Schr\"odinger wave functional | 19 pages. v2: a misprint in Arxiv abstract is corrected. v3: slightly
improved linguistically, accepted by ATMP | Adv. Theor. Math. Phys. 20 (2016) 1377-1396 | null | null | hep-th gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the Schr\"odinger wave functional may be obtained as the product
integral of precanonical wave functions on the space of field and space-time
variables. The functional derivative Schr\"odinger equation underlying the
canonical field quantization is derived from the partial derivative covariant
analogue o... | [
{
"created": "Mon, 16 Dec 2013 20:49:16 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Dec 2013 18:35:21 GMT",
"version": "v2"
},
{
"created": "Tue, 8 Mar 2016 04:56:16 GMT",
"version": "v3"
}
] | 2017-01-26 | [
[
"Kanatchikov",
"I. V.",
""
]
] | We show that the Schr\"odinger wave functional may be obtained as the product integral of precanonical wave functions on the space of field and space-time variables. The functional derivative Schr\"odinger equation underlying the canonical field quantization is derived from the partial derivative covariant analogue of ... | 6.57751 | 7.077916 | 7.353419 | 6.326335 | 6.860771 | 6.677924 | 6.688283 | 6.746195 | 6.81187 | 7.020857 | 6.516945 | 6.582232 | 6.657844 | 6.513261 | 6.681236 | 6.563598 | 6.667649 | 6.555334 | 6.389468 | 6.538996 | 6.290024 |
1605.09175 | Alberto Alonso-Izquierdo Dr | A. Alonso-Izquierdo, J. Mateos Guilarte and M. de la Torre Mayado | Quantum magnetic flux lines, BPS vortex zero modes, and one-loop string
tension shifts | 25 pages, 2 figures | Phys. Rev. D 94, 045008 (2016) | 10.1103/PhysRevD.94.045008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Spectral heat kernel/zeta function regularization procedures are employed in
this paper to control the divergences arising from vacuum fluctuations of
Bogomolnyi-Prasad-Sommerfield vortices in the Abelian Higgs model. Zero modes
of vortex fluctuations are the source of difficulties appearing when the
standard Gilkey-... | [
{
"created": "Mon, 30 May 2016 11:13:11 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Sep 2016 14:24:02 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Alonso-Izquierdo",
"A.",
""
],
[
"Guilarte",
"J. Mateos",
""
],
[
"Mayado",
"M. de la Torre",
""
]
] | Spectral heat kernel/zeta function regularization procedures are employed in this paper to control the divergences arising from vacuum fluctuations of Bogomolnyi-Prasad-Sommerfield vortices in the Abelian Higgs model. Zero modes of vortex fluctuations are the source of difficulties appearing when the standard Gilkey-de... | 12.949903 | 11.386557 | 12.789205 | 11.710512 | 14.410129 | 13.028445 | 12.739705 | 12.146221 | 12.780965 | 16.794987 | 11.823375 | 12.222876 | 12.262678 | 12.231129 | 12.519697 | 12.517979 | 12.038465 | 11.819466 | 12.108497 | 12.852491 | 12.284449 |
1701.02090 | Branko Dragovich | Ivan Dimitrijevic, Branko Dragovich, Jelena Stankovic, Alexey S.
Koshelev and Zoran Rakic | On Nonlocal Modified Gravity and its Cosmological Solutions | 16 pages | Springer Proceedings in Mathematics & Statistics 191 (2016) 35-51 | 10.1007/978-981-10-2636-2_3 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | During hundred years of General Relativity (GR), many significant
gravitational phenomena have been predicted and discovered. General Relativity
is still the best theory of gravity. Nevertheless, some (quantum) theoretical
and (astrophysical and cosmological) phenomenological difficulties of modern
gravity have been ... | [
{
"created": "Mon, 9 Jan 2017 08:30:17 GMT",
"version": "v1"
}
] | 2017-01-10 | [
[
"Dimitrijevic",
"Ivan",
""
],
[
"Dragovich",
"Branko",
""
],
[
"Stankovic",
"Jelena",
""
],
[
"Koshelev",
"Alexey S.",
""
],
[
"Rakic",
"Zoran",
""
]
] | During hundred years of General Relativity (GR), many significant gravitational phenomena have been predicted and discovered. General Relativity is still the best theory of gravity. Nevertheless, some (quantum) theoretical and (astrophysical and cosmological) phenomenological difficulties of modern gravity have been mo... | 9.468409 | 9.557317 | 8.780372 | 8.874254 | 8.545836 | 8.754107 | 9.531356 | 8.725702 | 9.380351 | 9.829314 | 9.187951 | 8.592231 | 8.41338 | 8.371328 | 8.458512 | 8.621277 | 8.37604 | 8.630238 | 8.506929 | 8.512808 | 8.629258 |
1909.02001 | Raphael Bousso | Raphael Bousso, Arvin Shahbazi-Moghaddam, Marija Tomasevic | Quantum Information Bound on the Energy | 47 pages, 10 figures | Phys. Rev. D 100, 126010 (2019) | 10.1103/PhysRevD.100.126010 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | According to the classical Penrose inequality, the mass at spatial infinity
is bounded from below by a function of the area of certain trapped surfaces. We
exhibit quantum field theory states that violate this relation at the
semiclassical level. We formulate a Quantum Penrose Inequality, by replacing
the area with t... | [
{
"created": "Wed, 4 Sep 2019 18:00:00 GMT",
"version": "v1"
}
] | 2019-12-18 | [
[
"Bousso",
"Raphael",
""
],
[
"Shahbazi-Moghaddam",
"Arvin",
""
],
[
"Tomasevic",
"Marija",
""
]
] | According to the classical Penrose inequality, the mass at spatial infinity is bounded from below by a function of the area of certain trapped surfaces. We exhibit quantum field theory states that violate this relation at the semiclassical level. We formulate a Quantum Penrose Inequality, by replacing the area with the... | 9.605066 | 11.512398 | 9.318644 | 9.334814 | 9.893085 | 9.829762 | 10.587934 | 9.427374 | 8.93043 | 10.01701 | 9.124007 | 9.091249 | 9.594526 | 8.827785 | 9.26769 | 9.2907 | 9.358653 | 8.863207 | 9.275949 | 9.514137 | 8.897064 |
hep-th/0502136 | Torquil MacDonald Sorensen | Torquil MacDonald Sorensen | Numerical Solution of the Ekpyrotic Scenario in the Moduli Space
Approximation | 5 pages, 7 figures, RevTeX4, fixed typos, added some small comments | Phys.Rev. D71 (2005) 107302 | 10.1103/PhysRevD.71.107302 | null | hep-th | null | A numerical solution to the equations of motion for the ekpyrotic bulk brane
scenario in the moduli space approximation is presented. The visible universe
brane has positive tension, and we use a potential that goes to zero
exponentially at large distance, and also goes to zero at small distance. In
the case consider... | [
{
"created": "Tue, 15 Feb 2005 13:11:45 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Feb 2005 12:59:45 GMT",
"version": "v2"
},
{
"created": "Wed, 25 May 2005 19:01:47 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Sorensen",
"Torquil MacDonald",
""
]
] | A numerical solution to the equations of motion for the ekpyrotic bulk brane scenario in the moduli space approximation is presented. The visible universe brane has positive tension, and we use a potential that goes to zero exponentially at large distance, and also goes to zero at small distance. In the case considered... | 10.208962 | 10.813435 | 11.154171 | 9.974607 | 9.270673 | 10.762524 | 10.367728 | 10.115663 | 10.141917 | 11.178232 | 9.76043 | 9.718277 | 9.646736 | 9.945152 | 9.829874 | 9.518368 | 9.427435 | 9.479544 | 9.484 | 9.922468 | 9.749237 |
1310.5939 | Tomoki Nosaka | Tomoki Nosaka and Seiji Terashima | Supersymmetric Gauge Theories on a Squashed Four-Sphere | 35 pages, no figures. v2: typos corrected, references added | JHEP 1312(2013) 001 | 10.1007/JHEP12(2013)001 | YITP-13-112 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define a squashed four-sphere by a dimensional reduction of a twisted S^4
x S^1, and construct explicitly a supersymmetric Yang-Mills action on it. The
action includes a non-trivial dilaton factor and a theta term with a
non-constant theta. The partition function of this theory is calculated using
the localization... | [
{
"created": "Tue, 22 Oct 2013 14:42:13 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Dec 2013 03:42:00 GMT",
"version": "v2"
}
] | 2013-12-16 | [
[
"Nosaka",
"Tomoki",
""
],
[
"Terashima",
"Seiji",
""
]
] | We define a squashed four-sphere by a dimensional reduction of a twisted S^4 x S^1, and construct explicitly a supersymmetric Yang-Mills action on it. The action includes a non-trivial dilaton factor and a theta term with a non-constant theta. The partition function of this theory is calculated using the localization t... | 9.329129 | 8.129072 | 8.854099 | 8.237661 | 7.851402 | 8.886253 | 8.209432 | 7.735912 | 7.744172 | 9.620583 | 8.189709 | 8.056548 | 8.909886 | 8.023654 | 7.776743 | 8.226135 | 8.130546 | 8.185861 | 8.301395 | 8.517085 | 8.103231 |
1106.2483 | Robert de Mello Koch | Robert de Mello Koch, Badr Awad Elseid Mohammed and Stephanie Smith | Nonplanar Integrability: Beyond the SU(2) Sector | 32 pages | null | 10.1142/S0217751X11054590 | WITS-CTP-075 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the one loop anomalous dimensions of restricted Schur polynomials
with a classical dimension \Delta\sim O(N). The operators that we consider are
labeled by Young diagrams with two long columns or two long rows. Simple
analytic expressions for the action of the dilatation operator are found. The
projection ... | [
{
"created": "Mon, 13 Jun 2011 16:29:37 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Koch",
"Robert de Mello",
""
],
[
"Mohammed",
"Badr Awad Elseid",
""
],
[
"Smith",
"Stephanie",
""
]
] | We compute the one loop anomalous dimensions of restricted Schur polynomials with a classical dimension \Delta\sim O(N). The operators that we consider are labeled by Young diagrams with two long columns or two long rows. Simple analytic expressions for the action of the dilatation operator are found. The projection op... | 7.838108 | 7.421705 | 9.528949 | 7.528166 | 8.049442 | 7.609805 | 8.012956 | 7.517939 | 7.765136 | 9.691173 | 7.254511 | 7.423732 | 8.392085 | 7.588578 | 7.610206 | 7.628072 | 7.746822 | 7.486674 | 7.930629 | 7.965261 | 7.598561 |
2405.19218 | Shani Nadir Meynet | Azeem Hasan, Shani Meynet, Daniele Migliorati | The $SL_2(\mathbb{R})$ duality and the non-invertible $U(1)$ symmetry of
Maxwell theory | v2: 19 pages, 1 figure, references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent proposals for the Symmetry Topological Field Theory (SymTFT) of
Maxwell theory admit a 0-form symmetry compatible with the classical
$SL_2(\mathbb{R})$ duality of electromagnetism. We describe how to realize
these automorphisms of the SymTFT in terms of its operators and we detail their
effects on the dynamica... | [
{
"created": "Wed, 29 May 2024 16:00:22 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Jun 2024 12:41:20 GMT",
"version": "v2"
}
] | 2024-06-12 | [
[
"Hasan",
"Azeem",
""
],
[
"Meynet",
"Shani",
""
],
[
"Migliorati",
"Daniele",
""
]
] | Recent proposals for the Symmetry Topological Field Theory (SymTFT) of Maxwell theory admit a 0-form symmetry compatible with the classical $SL_2(\mathbb{R})$ duality of electromagnetism. We describe how to realize these automorphisms of the SymTFT in terms of its operators and we detail their effects on the dynamical ... | 10.758681 | 10.332449 | 11.517051 | 9.324377 | 9.359099 | 9.488087 | 9.420168 | 9.690824 | 9.829959 | 11.963073 | 8.698678 | 9.858673 | 10.765008 | 10.068214 | 9.957098 | 9.396358 | 9.767669 | 9.809541 | 9.686768 | 10.706148 | 9.923718 |
2103.15391 | Claudio Dappiaggi | Lissa de Souza Campos, Claudio Dappiaggi and Denis Sina | On the role of boundary conditions within Ho\v{r}ava-Lifshitz gravity | 37 pages, 11 figures | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | On a class of four-dimensional Lifshitz spacetimes with critical exponent
$z=2$, including a hyperbolic and a spherical Lifshitz topological black hole,
we consider a real Klein-Gordon field. Using a mode-decomposition, we split the
equation of motion into a radial and into an angular component. As first step,
we dis... | [
{
"created": "Mon, 29 Mar 2021 07:33:42 GMT",
"version": "v1"
}
] | 2021-03-30 | [
[
"Campos",
"Lissa de Souza",
""
],
[
"Dappiaggi",
"Claudio",
""
],
[
"Sina",
"Denis",
""
]
] | On a class of four-dimensional Lifshitz spacetimes with critical exponent $z=2$, including a hyperbolic and a spherical Lifshitz topological black hole, we consider a real Klein-Gordon field. Using a mode-decomposition, we split the equation of motion into a radial and into an angular component. As first step, we discu... | 11.293508 | 11.978756 | 11.235256 | 10.432022 | 11.321834 | 10.740975 | 10.70155 | 10.357732 | 10.234518 | 12.634785 | 10.029558 | 10.158363 | 10.243679 | 10.217769 | 10.01919 | 10.060443 | 9.798014 | 10.161498 | 10.196734 | 10.534482 | 10.151176 |
hep-th/0103041 | Dionisio Bazeia | D. Bazeia, J. Menezes, M.M. Santos | Complete factorization of equations of motion in supersymmetric field
theories | Revtex, 6 pages; version to be published in Nucl. Phys. B | Nucl.Phys. B636 (2002) 132-140 | 10.1016/S0550-3213(02)00460-1 | null | hep-th hep-ph | null | We investigate bosonic sectors of supersymmetric field theories. We consider
superpotentials described by one and by two real scalar fields, and we show how
the equations of motion can be factorized into a family of first order
Bogomol'nyi equations, so that all the topological defects are of the
Bogomol'nyi-Prasad-S... | [
{
"created": "Tue, 6 Mar 2001 21:25:44 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Mar 2001 12:18:31 GMT",
"version": "v2"
},
{
"created": "Fri, 13 Jul 2001 15:25:50 GMT",
"version": "v3"
},
{
"created": "Wed, 12 Jun 2002 11:28:11 GMT",
"version": "v4"
}
] | 2015-06-25 | [
[
"Bazeia",
"D.",
""
],
[
"Menezes",
"J.",
""
],
[
"Santos",
"M. M.",
""
]
] | We investigate bosonic sectors of supersymmetric field theories. We consider superpotentials described by one and by two real scalar fields, and we show how the equations of motion can be factorized into a family of first order Bogomol'nyi equations, so that all the topological defects are of the Bogomol'nyi-Prasad-Som... | 10.585654 | 8.188846 | 10.648743 | 9.124179 | 9.081862 | 9.2374 | 9.076275 | 8.53638 | 8.907036 | 10.595138 | 8.662005 | 9.669219 | 10.287995 | 9.417388 | 9.58794 | 9.575542 | 9.439152 | 9.513785 | 9.586742 | 10.345871 | 9.482409 |
hep-th/9907180 | Ludvig Faddeev | Ludvig Faddeev and Antti J. Niemi | Decomposing the Yang-Mills Field | 5 pages, latex, no figures | Phys.Lett.B464:90-93,1999 | 10.1016/S0370-2693(99)01035-7 | null | hep-th | null | Recently we have proposed a set of variables for describing the physical
parameters of SU(N) Yang--Mills field. Here we propose an off-shell
generalization of our Ansatz. For this we envoke the Darboux theorem to
decompose arbitrary one-form with respect to some basis of one-forms. After a
partial gauge fixing we ide... | [
{
"created": "Fri, 23 Jul 1999 14:02:02 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Faddeev",
"Ludvig",
""
],
[
"Niemi",
"Antti J.",
""
]
] | Recently we have proposed a set of variables for describing the physical parameters of SU(N) Yang--Mills field. Here we propose an off-shell generalization of our Ansatz. For this we envoke the Darboux theorem to decompose arbitrary one-form with respect to some basis of one-forms. After a partial gauge fixing we ident... | 12.222654 | 12.306215 | 10.90648 | 10.905767 | 12.28861 | 12.78761 | 11.859195 | 10.782189 | 11.28336 | 13.748402 | 11.5525 | 11.208138 | 11.175277 | 11.155457 | 11.201459 | 11.263678 | 11.169707 | 11.187926 | 11.139344 | 11.119115 | 10.80693 |
hep-th/9703120 | David Delphenich | David Delphenich (Syracuse U.), Joseph Schechter (Syracuse U.) | Multiflavor Massive Schwinger Model With Non-Abelian Bosonization | To appear in Int. J. Mod. Phys. A (Footnote and reference revised
from previous version) | Int.J.Mod.Phys. A12 (1997) 5305-5324 | 10.1142/S0217751X9700284X | SU-4240-654 | hep-th hep-ph | null | We revisit the treatment of the multiflavor massive Schwinger model by
non-Abelian Bosonization. We compare three different approximations to the
low-lying spectrum: i) reading it off from the bosonized Lagrangian (neglecting
interactions), ii) semi-classical quantization of the static soliton, iii)
approximate semi-... | [
{
"created": "Mon, 17 Mar 1997 17:59:13 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Apr 1997 18:51:48 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Delphenich",
"David",
"",
"Syracuse U."
],
[
"Schechter",
"Joseph",
"",
"Syracuse U."
]
] | We revisit the treatment of the multiflavor massive Schwinger model by non-Abelian Bosonization. We compare three different approximations to the low-lying spectrum: i) reading it off from the bosonized Lagrangian (neglecting interactions), ii) semi-classical quantization of the static soliton, iii) approximate semi-cl... | 10.819698 | 10.649347 | 11.220058 | 10.001448 | 11.077226 | 11.3655 | 11.211535 | 10.132265 | 10.219237 | 11.978002 | 10.347378 | 10.218217 | 10.396677 | 10.163424 | 10.146678 | 10.258583 | 10.273768 | 10.223219 | 10.182738 | 10.339536 | 9.839842 |
hep-th/9811086 | Sheng Li | Sheng Li and Yishi Duan | SO(4) Monopole As A New Topological Invariant And Its Topological
Structure | 17 pages, Revtex, no figures | null | null | null | hep-th | null | By making use of the decomposition theory of gauge potential, the inner
structure of SU(2) and SO(4) gauge theory is discussed in detail. We find the
SO(4) monopole can be given via projecting the SO(4) gauge field onto an
antisymmetric tensor. This projection fix the coset $% SU(2)/U(1)\bigotimes
SU(2)/U(1)$ of SO(4... | [
{
"created": "Tue, 10 Nov 1998 03:17:10 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Li",
"Sheng",
""
],
[
"Duan",
"Yishi",
""
]
] | By making use of the decomposition theory of gauge potential, the inner structure of SU(2) and SO(4) gauge theory is discussed in detail. We find the SO(4) monopole can be given via projecting the SO(4) gauge field onto an antisymmetric tensor. This projection fix the coset $% SU(2)/U(1)\bigotimes SU(2)/U(1)$ of SO(4) ... | 10.411238 | 9.648314 | 10.208815 | 9.057388 | 10.372557 | 8.991887 | 9.490874 | 8.890055 | 9.254354 | 11.509637 | 9.342442 | 9.563414 | 9.497468 | 9.333901 | 9.515176 | 9.449799 | 9.124477 | 9.599654 | 9.291728 | 9.832588 | 9.399303 |
1412.6957 | A. Yu. Petrov | A. P. Baeta Scarpelli, J. R. Nascimento, A. Yu. Petrov, R. F. Ribeiro | On the duality in CPT-even Lorentz-breaking theories | 17 pages, version accepted to EPJC | Eur. Phys. J. C (2015) 75: 314 | 10.1140/epjc/s10052-015-3537-z | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we generalize the duality between self-dual and
Maxwell-Chern-Simons theories for the case of a CPT-even Lorentz-breaking
extension of these theories. The duality is demonstrated with use of the gauge
embedding procedure, both in free and coupled cases, and with the master action
approach. The physical... | [
{
"created": "Mon, 22 Dec 2014 12:36:46 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Jun 2015 14:50:54 GMT",
"version": "v2"
}
] | 2015-07-08 | [
[
"Scarpelli",
"A. P. Baeta",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"Ribeiro",
"R. F.",
""
]
] | In this paper, we generalize the duality between self-dual and Maxwell-Chern-Simons theories for the case of a CPT-even Lorentz-breaking extension of these theories. The duality is demonstrated with use of the gauge embedding procedure, both in free and coupled cases, and with the master action approach. The physical s... | 9.003139 | 8.290429 | 9.691704 | 7.574346 | 7.534618 | 7.526856 | 7.792273 | 8.227108 | 7.476555 | 10.560186 | 7.673173 | 8.104589 | 8.64423 | 7.926066 | 7.59447 | 8.113853 | 7.89675 | 8.192999 | 8.174545 | 8.475623 | 7.75029 |
hep-th/0204077 | Ghenadie N. Mardari | Ghenadie N. Mardari | Interferometric evidence for brane world cosmologies | 3 pages, no figures, Revtex. New experiment proposal added | null | null | null | hep-th physics.optics quant-ph | null | The hypothesis of brane-embedded matter appears to gain increasing
credibility in astrophysics. However, it can only be truly successful if its
implications on particle interaction are consistent with existing knowledge.
This letter focuses on the issue of optical interference, and shows that at
least one brane-world... | [
{
"created": "Tue, 9 Apr 2002 06:12:21 GMT",
"version": "v1"
},
{
"created": "Sun, 28 Apr 2002 06:25:21 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Jul 2002 22:00:06 GMT",
"version": "v3"
},
{
"created": "Thu, 23 Jan 2003 15:36:46 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Mardari",
"Ghenadie N.",
""
]
] | The hypothesis of brane-embedded matter appears to gain increasing credibility in astrophysics. However, it can only be truly successful if its implications on particle interaction are consistent with existing knowledge. This letter focuses on the issue of optical interference, and shows that at least one brane-world m... | 18.525457 | 19.77346 | 19.720341 | 18.654829 | 21.548595 | 20.595789 | 19.820557 | 19.02582 | 19.125177 | 18.532066 | 17.339916 | 17.458694 | 17.723606 | 17.531961 | 17.993742 | 17.692204 | 18.651463 | 17.344568 | 17.97946 | 17.545187 | 17.290871 |
hep-th/0403175 | Antti J. Niemi | Antti J. Niemi | Dual Superconductors and SU(2) Yang-Mills | null | JHEP 0408 (2004) 035 | 10.1088/1126-6708/2004/08/035 | null | hep-th cond-mat.supr-con hep-lat nucl-th | null | We propose that the SU(2) Yang-Mills theory can be interpreted as a two-band
dual superconductor with an interband Josephson coupling. We discuss various
consequences of this interpretation including electric flux quantization,
confinement of vortices with fractional flux, and the possibility that a closed
vortex loo... | [
{
"created": "Wed, 17 Mar 2004 12:53:22 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Mar 2004 20:53:39 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Niemi",
"Antti J.",
""
]
] | We propose that the SU(2) Yang-Mills theory can be interpreted as a two-band dual superconductor with an interband Josephson coupling. We discuss various consequences of this interpretation including electric flux quantization, confinement of vortices with fractional flux, and the possibility that a closed vortex loop ... | 12.690777 | 10.006418 | 12.038508 | 10.815043 | 11.758342 | 11.607316 | 10.437936 | 10.126768 | 10.75105 | 12.513878 | 10.266746 | 10.788148 | 12.860918 | 11.259122 | 11.099028 | 11.029545 | 11.187862 | 10.741662 | 10.904444 | 12.076073 | 11.049691 |
1401.2769 | Julien Serreau | Julien Serreau | A class of nonperturbative nonlinear covariant gauges in Yang-Mills
theories | Contribution to "QCD-TNT-III-From quarks and gluons to hadronic
matter: A bridge too far?", 2-6 Sept 2013, ECT*, Trento, Italy; 7 pages | null | null | null | hep-th hep-lat hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report on the recent proposal of a class of nonlinear covariant gauges
that can be formulated as an extremization procedure which admits a simple
discretization well-suited to numerical minimization techniques. This class of
gauges is continuously connected to the Landau gauge and, in the ultraviolet,
where one ca... | [
{
"created": "Mon, 13 Jan 2014 09:57:15 GMT",
"version": "v1"
}
] | 2014-01-14 | [
[
"Serreau",
"Julien",
""
]
] | We report on the recent proposal of a class of nonlinear covariant gauges that can be formulated as an extremization procedure which admits a simple discretization well-suited to numerical minimization techniques. This class of gauges is continuously connected to the Landau gauge and, in the ultraviolet, where one can ... | 9.25178 | 8.564154 | 11.48731 | 8.566848 | 8.653879 | 8.371798 | 8.236228 | 8.408777 | 7.880774 | 14.290347 | 8.350822 | 9.063411 | 9.785735 | 8.556158 | 9.60183 | 8.873129 | 8.990862 | 9.2615 | 8.858051 | 9.80739 | 8.538198 |
2106.13832 | Eleanor Harris | Dionysios Anninos and Eleanor Harris | Three-dimensional de Sitter horizon thermodynamics | 34 pages + appendices, 5 figures | null | 10.1007/JHEP10(2021)091 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore thermodynamic contributions to the three-dimensional de Sitter
horizon originating from metric and Chern-Simons gauge field fluctuations. In
Euclidean signature these are computed by the partition function of gravity
coupled to matter semi-classically expanded about the round three-sphere
saddle. We invest... | [
{
"created": "Fri, 25 Jun 2021 18:15:16 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jul 2021 13:53:04 GMT",
"version": "v2"
},
{
"created": "Thu, 13 Jan 2022 14:08:16 GMT",
"version": "v3"
}
] | 2022-01-14 | [
[
"Anninos",
"Dionysios",
""
],
[
"Harris",
"Eleanor",
""
]
] | We explore thermodynamic contributions to the three-dimensional de Sitter horizon originating from metric and Chern-Simons gauge field fluctuations. In Euclidean signature these are computed by the partition function of gravity coupled to matter semi-classically expanded about the round three-sphere saddle. We investig... | 8.993334 | 8.067766 | 10.111388 | 8.352742 | 8.023726 | 8.15949 | 8.22852 | 8.250878 | 8.112926 | 9.703673 | 8.000778 | 8.45298 | 8.611946 | 8.404689 | 8.368164 | 8.649403 | 8.476672 | 8.427824 | 8.788835 | 8.98616 | 8.384766 |
hep-th/0511286 | Martin Schnabl | Martin Schnabl | Analytic solution for tachyon condensation in open string field theory | 60 pages, 4 figures, v2: typos corrected, references added | Adv.Theor.Math.Phys.10:433-501,2006 | null | CERN-PH-TH/2005-220 | hep-th | null | We propose a new basis in Witten's open string field theory, in which the
star product simplifies considerably. For a convenient choice of gauge the
classical string field equation of motion yields straightforwardly an exact
analytic solution that represents the nonperturbative tachyon vacuum. The
solution is given i... | [
{
"created": "Tue, 29 Nov 2005 17:18:20 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Jun 2006 15:39:02 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Schnabl",
"Martin",
""
]
] | We propose a new basis in Witten's open string field theory, in which the star product simplifies considerably. For a convenient choice of gauge the classical string field equation of motion yields straightforwardly an exact analytic solution that represents the nonperturbative tachyon vacuum. The solution is given in ... | 9.857723 | 10.160633 | 11.495527 | 9.771749 | 10.358458 | 11.078626 | 10.19487 | 9.193444 | 9.290629 | 12.001311 | 10.522669 | 9.31739 | 10.346364 | 9.464039 | 9.537634 | 9.446473 | 9.656749 | 9.988865 | 9.501504 | 10.390162 | 9.454078 |
1605.01603 | Chethan Krishnan | Chethan Krishnan, Avinash Raju | A Neumann Boundary Term for Gravity | v3: emphasized that a covariant notion of Neumann boundary condition
inevitably leads to our boundary term. v4: more refs | null | 10.1142/S0217732317500778 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Gibbons-Hawking-York (GHY) boundary term makes the Dirichlet problem for
gravity well defined, but no such general term seems to be known for Neumann
boundary conditions. In this paper, we view Neumann {\em not} as fixing the
normal derivative of the metric ("velocity") at the boundary, but as fixing the
function... | [
{
"created": "Thu, 5 May 2016 14:08:11 GMT",
"version": "v1"
},
{
"created": "Fri, 6 May 2016 14:23:02 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Mar 2017 13:35:04 GMT",
"version": "v3"
},
{
"created": "Mon, 6 Mar 2017 06:00:21 GMT",
"version": "v4"
}
] | 2017-05-24 | [
[
"Krishnan",
"Chethan",
""
],
[
"Raju",
"Avinash",
""
]
] | The Gibbons-Hawking-York (GHY) boundary term makes the Dirichlet problem for gravity well defined, but no such general term seems to be known for Neumann boundary conditions. In this paper, we view Neumann {\em not} as fixing the normal derivative of the metric ("velocity") at the boundary, but as fixing the functional... | 7.566474 | 7.529423 | 7.937413 | 7.456602 | 7.950485 | 7.733777 | 7.740537 | 7.446866 | 7.956151 | 8.530711 | 7.402655 | 7.494845 | 7.280476 | 7.282135 | 7.582335 | 7.408181 | 7.277489 | 7.320096 | 7.300587 | 7.176282 | 7.258112 |
2209.07897 | Wen-Yuan Ai | Wen-Yuan Ai, Carl M. Bender and Sarben Sarkar | $\mathcal{P}\mathcal{T}$-symmetric $-g\varphi^4$ theory | 7 pages, 2 figures, revtex format; v2: minor typos corrected, refs
added; v3: published version; v4: two typos corrected | Phys. Rev. D 106, 125016 (2022) | 10.1103/PhysRevD.106.125016 | KCL-PH-TH-2022-25 | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The scalar field theory with potential $V(\varphi)=\textstyle{\frac{1}{2}}
m^2\varphi^2-\textstyle{\frac{1}{4}} g\varphi^4$ ($g>0$) is ill defined as a
Hermitian theory but in a non-Hermitian $\mathcal{P}\mathcal{T}$-symmetric
framework it is well defined, and it has a positive real energy spectrum for
the case of sp... | [
{
"created": "Fri, 16 Sep 2022 12:44:00 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Sep 2022 11:22:10 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Dec 2022 10:10:51 GMT",
"version": "v3"
},
{
"created": "Thu, 5 Jan 2023 08:26:09 GMT",
"version": "v4"
}
] | 2023-01-06 | [
[
"Ai",
"Wen-Yuan",
""
],
[
"Bender",
"Carl M.",
""
],
[
"Sarkar",
"Sarben",
""
]
] | The scalar field theory with potential $V(\varphi)=\textstyle{\frac{1}{2}} m^2\varphi^2-\textstyle{\frac{1}{4}} g\varphi^4$ ($g>0$) is ill defined as a Hermitian theory but in a non-Hermitian $\mathcal{P}\mathcal{T}$-symmetric framework it is well defined, and it has a positive real energy spectrum for the case of spac... | 3.302906 | 3.478549 | 3.459545 | 3.286492 | 3.475133 | 3.528491 | 3.421502 | 3.374558 | 3.34468 | 3.630881 | 3.27937 | 3.272553 | 3.274601 | 3.228196 | 3.253714 | 3.251184 | 3.281072 | 3.258803 | 3.224345 | 3.312583 | 3.236174 |
1909.10054 | Alexei Nurmagambetov | A. J. Nurmagambetov (Kharkov, KIPT), I. Y. Park (Philander Smith
Coll.) | Quantum-gravitational trans-Planckian energy of a time-dependent black
hole | 25 pages. Invited contribution to special topic of Symmetry | null | 10.3390/sym11101303 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue our recent endeavor in which a time-dependent black hole solution
of a one-loop quantum-corrected Einstein-scalar system was obtained and its
near-horizon behavior was analyzed. The energy analysis led to a
trans-Planckian scaling behavior near the event horizon. In the present work
the analysis is extend... | [
{
"created": "Sun, 22 Sep 2019 17:59:00 GMT",
"version": "v1"
}
] | 2022-02-08 | [
[
"Nurmagambetov",
"A. J.",
"",
"Kharkov, KIPT"
],
[
"Park",
"I. Y.",
"",
"Philander Smith\n Coll."
]
] | We continue our recent endeavor in which a time-dependent black hole solution of a one-loop quantum-corrected Einstein-scalar system was obtained and its near-horizon behavior was analyzed. The energy analysis led to a trans-Planckian scaling behavior near the event horizon. In the present work the analysis is extended... | 9.548177 | 8.970484 | 8.84233 | 7.854704 | 8.475771 | 8.523569 | 9.089864 | 8.124054 | 8.271732 | 9.297877 | 8.232186 | 8.614571 | 8.729391 | 8.24317 | 8.618488 | 8.792213 | 8.867084 | 8.469367 | 8.43448 | 8.63499 | 8.68926 |
0709.0873 | Charalampos Bogdanos | C. Bogdanos, A. Kehagias and K. Tamvakis | Pseudo-3-Branes in a Curved 6D Bulk | 13 pages | Phys.Lett.B656:112-118,2007 | 10.1016/j.physletb.2007.09.016 | null | hep-th | null | We consider a model involving a 4-brane in a 6D bulk which carries sigma
model fields. An axion field on the 4-brane cancels the pressure along one
direction leading to an effective codimension-2 3-brane. For a range of
parameters of the theory, we get a transverse space which is non-compact,
providing a possible sol... | [
{
"created": "Thu, 6 Sep 2007 14:39:07 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Bogdanos",
"C.",
""
],
[
"Kehagias",
"A.",
""
],
[
"Tamvakis",
"K.",
""
]
] | We consider a model involving a 4-brane in a 6D bulk which carries sigma model fields. An axion field on the 4-brane cancels the pressure along one direction leading to an effective codimension-2 3-brane. For a range of parameters of the theory, we get a transverse space which is non-compact, providing a possible solut... | 10.398901 | 10.458794 | 10.728289 | 9.653512 | 10.176554 | 10.969574 | 10.271244 | 9.936675 | 9.579062 | 11.682383 | 10.317225 | 9.629344 | 10.327306 | 9.968983 | 10.024468 | 10.081824 | 9.890762 | 9.837494 | 9.93804 | 10.526116 | 9.928442 |
hep-th/0003086 | Damien Easson | Damien A. Easson | The Interface of Cosmology with String and M(ILLENNIUM) Theory | 49 pages, 10 figures; minor revisions; accepted for publication in
IJMPA | Int.J.Mod.Phys.A16:4803-4843,2001 | 10.1142/S0217751X01005274 | BROWN-HET-1209 | hep-th astro-ph gr-qc hep-ph | null | The purpose of this review is to discuss recent developments occurring at the
interface of cosmology with string and M-theory. We begin with a short review
of 1980s string cosmology and the Brandenberger-Vafa mechanism for explaining
spacetime dimensionality. It is shown how this scenario has been modified to
include... | [
{
"created": "Sat, 11 Mar 2000 22:52:02 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Mar 2000 19:02:30 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Oct 2000 16:44:00 GMT",
"version": "v3"
},
{
"created": "Sun, 4 Mar 2001 21:57:41 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Easson",
"Damien A.",
""
]
] | The purpose of this review is to discuss recent developments occurring at the interface of cosmology with string and M-theory. We begin with a short review of 1980s string cosmology and the Brandenberger-Vafa mechanism for explaining spacetime dimensionality. It is shown how this scenario has been modified to include t... | 6.373747 | 6.655222 | 7.26148 | 6.556748 | 6.523057 | 6.02638 | 6.42058 | 6.251465 | 6.113825 | 8.628169 | 6.256112 | 6.202676 | 6.557169 | 6.178854 | 6.367589 | 6.405519 | 6.383061 | 6.395936 | 6.21498 | 6.413558 | 6.323488 |
hep-th/0109205 | Ricardo Bentin | Alfredo T. Suzuki and Ricardo Bent\'in | Obtaining a light-like planar gauge | 9 pages | Mod.Phys.Lett. A17 (2002) 205-208 | 10.1142/S0217732302006473 | null | hep-th | null | In the usual and current understanding of planar gauge choices for Abelian
and non Abelian gauge fields, the external defining vector $n_\mu$ can either
be space-like ($n^2<0$) or time-like ($n^2>0$) but not light-like ($n^2=0$). In
this work we propose a light-like planar gauge that consists in defining a
modified g... | [
{
"created": "Wed, 26 Sep 2001 19:06:15 GMT",
"version": "v1"
}
] | 2016-08-16 | [
[
"Suzuki",
"Alfredo T.",
""
],
[
"Bentín",
"Ricardo",
""
]
] | In the usual and current understanding of planar gauge choices for Abelian and non Abelian gauge fields, the external defining vector $n_\mu$ can either be space-like ($n^2<0$) or time-like ($n^2>0$) but not light-like ($n^2=0$). In this work we propose a light-like planar gauge that consists in defining a modified gau... | 8.415956 | 8.488895 | 8.154611 | 8.163695 | 9.092578 | 8.441272 | 8.449391 | 8.055217 | 7.920839 | 8.683571 | 8.338853 | 8.053093 | 8.32133 | 8.032711 | 8.117084 | 7.789509 | 7.932612 | 7.863386 | 8.053464 | 8.325784 | 8.241219 |
hep-th/0502061 | Hiroaki Kanno | Hidetoshi Awata and Hiroaki Kanno | Instanton counting, Macdonald function and the moduli space of D-branes | 33 pages, 2 figures, (v2) minor changes, references added, (v3)
Comments and more references added | JHEP 0505 (2005) 039 | 10.1088/1126-6708/2005/05/039 | null | hep-th | null | We argue the connection of Nekrasov's partition function in the \Omega
background and the moduli space of D-branes, suggested by the idea of geometric
engineering and Gopakumar-Vafa invariants. In the instanton expansion of N=2
SU(2) Yang-Mills theory the Nakrasov's partition function with equivariant
parameters \eps... | [
{
"created": "Sat, 5 Feb 2005 03:25:37 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Feb 2005 11:29:28 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Apr 2005 02:09:43 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Awata",
"Hidetoshi",
""
],
[
"Kanno",
"Hiroaki",
""
]
] | We argue the connection of Nekrasov's partition function in the \Omega background and the moduli space of D-branes, suggested by the idea of geometric engineering and Gopakumar-Vafa invariants. In the instanton expansion of N=2 SU(2) Yang-Mills theory the Nakrasov's partition function with equivariant parameters \epsil... | 7.454676 | 7.930058 | 10.389801 | 7.316806 | 8.502069 | 8.076773 | 7.740574 | 7.743847 | 7.623816 | 9.737053 | 7.428453 | 7.091727 | 7.974226 | 7.102442 | 7.224685 | 7.403776 | 7.14889 | 7.381324 | 7.181691 | 7.821696 | 7.099754 |
0905.3137 | Paul S. Aspinwall | Paul S. Aspinwall | Probing Geometry with Stability Conditions | 36 pages, refs added | null | null | DUKE-CGTP-09-01 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The notion that the geometry of spacetime is given by the moduli space of
0-branes is examined in four examples of Calabi-Yau threefolds. An important
consideration when determining the moduli space of D-branes is the stability
condition and this is key in our analysis. In the first two examples, the flop
and the orb... | [
{
"created": "Tue, 19 May 2009 15:40:12 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Jun 2009 15:53:03 GMT",
"version": "v2"
}
] | 2009-06-01 | [
[
"Aspinwall",
"Paul S.",
""
]
] | The notion that the geometry of spacetime is given by the moduli space of 0-branes is examined in four examples of Calabi-Yau threefolds. An important consideration when determining the moduli space of D-branes is the stability condition and this is key in our analysis. In the first two examples, the flop and the orbif... | 9.871187 | 9.594973 | 11.993788 | 9.301114 | 9.857471 | 9.804493 | 9.845549 | 9.484988 | 9.29397 | 12.160346 | 9.143014 | 9.437705 | 10.304305 | 9.720647 | 9.208284 | 9.390539 | 9.403934 | 9.511893 | 9.504503 | 10.146963 | 9.556027 |
1911.08456 | Sunghyuk Park | Sungbong Chun, Sergei Gukov, Sunghyuk Park, Nikita Sopenko | 3d-3d correspondence for mapping tori | 53 pages, 8 figures | J. High Energ. Phys. 2020, 152 (2020) | 10.1007/JHEP09(2020)152 | CALT-2019-048 | hep-th math.GT math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One of the main challenges in 3d-3d correspondence is that no existent
approach offers a complete description of 3d $N=2$ SCFT $T[M_3]$ --- or,
rather, a "collection of SCFTs" as we refer to it in the paper --- for all
types of 3-manifolds that include, for example, a 3-torus, Brieskorn spheres,
and hyperbolic surger... | [
{
"created": "Tue, 19 Nov 2019 18:30:57 GMT",
"version": "v1"
}
] | 2020-09-29 | [
[
"Chun",
"Sungbong",
""
],
[
"Gukov",
"Sergei",
""
],
[
"Park",
"Sunghyuk",
""
],
[
"Sopenko",
"Nikita",
""
]
] | One of the main challenges in 3d-3d correspondence is that no existent approach offers a complete description of 3d $N=2$ SCFT $T[M_3]$ --- or, rather, a "collection of SCFTs" as we refer to it in the paper --- for all types of 3-manifolds that include, for example, a 3-torus, Brieskorn spheres, and hyperbolic surgerie... | 7.44178 | 7.06265 | 8.523037 | 6.896901 | 7.302404 | 7.24901 | 7.135829 | 7.230105 | 7.027821 | 8.995742 | 7.413887 | 6.647775 | 7.420424 | 6.844723 | 6.696911 | 6.703825 | 6.905102 | 6.658492 | 6.827352 | 7.405395 | 7.164165 |
2102.05053 | Jonah Kudler-Flam | Jonah Kudler-Flam | Relative Entropy of Random States and Black Holes | 5+3 pages; v2: two appendices, discussion of implications for quantum
hypothesis testing, and references added | Phys. Rev. Lett. 126, 171603 (2021) | 10.1103/PhysRevLett.126.171603 | null | hep-th cond-mat.stat-mech cond-mat.str-el math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the relative entropy of highly excited quantum states. First, we
sample states from the Wishart ensemble and develop a large-N diagrammatic
technique for the relative entropy. The solution is exactly expressed in terms
of elementary functions. We compare the analytic results to small-N numerics,
finding prec... | [
{
"created": "Tue, 9 Feb 2021 19:00:01 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Mar 2021 14:36:27 GMT",
"version": "v2"
}
] | 2021-04-28 | [
[
"Kudler-Flam",
"Jonah",
""
]
] | We study the relative entropy of highly excited quantum states. First, we sample states from the Wishart ensemble and develop a large-N diagrammatic technique for the relative entropy. The solution is exactly expressed in terms of elementary functions. We compare the analytic results to small-N numerics, finding precis... | 8.711847 | 8.456543 | 9.488329 | 8.8333 | 9.445066 | 9.339501 | 9.15419 | 8.494492 | 8.907535 | 9.380872 | 8.423517 | 8.491323 | 9.18861 | 8.475985 | 8.652666 | 8.672646 | 8.832707 | 8.511746 | 8.551639 | 9.050088 | 8.693698 |
1410.7773 | Vasilis Niarchos | Francesco Aprile and Vasilis Niarchos | Large-N transitions of the connectivity index | 39 pages, 4 figures; v2 a new section 8 has been added to emphasise
aspects of separability in the IR effective theory and the relation with
multi-gravity, references added; v3 a proper account of the IR effects of
U(1) (singleton) degrees of freedom has been added with appropriate changes
in sections 3, 4.3, 9... | null | 10.1007/JHEP02(2015)083 | CCQCN-2014-47, CCTP-2014-22 | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The connectivity index, defined as the number of decoupled components of a
separable quantum system, can change under deformations of the Hamiltonian or
during the dynamical change of the system under renormalization group flow.
Such changes signal a rearrangement of correlations of different degrees of
freedom acros... | [
{
"created": "Tue, 28 Oct 2014 20:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Nov 2014 14:43:25 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Jan 2015 00:09:08 GMT",
"version": "v3"
}
] | 2015-06-23 | [
[
"Aprile",
"Francesco",
""
],
[
"Niarchos",
"Vasilis",
""
]
] | The connectivity index, defined as the number of decoupled components of a separable quantum system, can change under deformations of the Hamiltonian or during the dynamical change of the system under renormalization group flow. Such changes signal a rearrangement of correlations of different degrees of freedom across ... | 10.957009 | 11.266702 | 11.999102 | 11.091256 | 11.56805 | 11.869178 | 11.457668 | 11.482305 | 11.528716 | 12.808411 | 11.442061 | 10.545979 | 11.120633 | 10.642065 | 10.750711 | 10.415401 | 10.50306 | 10.426174 | 10.545579 | 11.237533 | 10.600429 |
hep-th/0304264 | Steffen Krusch | Steffen Krusch | Fermions coupled to Skyrmions on S^3 | 31 pages, 6 figures | J.Phys.A36:8141,2003 | 10.1088/0305-4470/36/29/318 | LEEDS-PURE-MATHS-2002-24 | hep-th | null | This paper discusses Skyrmions on the 3-sphere coupled to fermions. The
resulting Dirac equation commutes with a generalized angular momentum G. For G
= 0 the Dirac equation can be solved explicitly for a constant Skyrme
configuration and also for a SO(4) symmetric hedgehog configuration. We discuss
how the spectrum ... | [
{
"created": "Wed, 30 Apr 2003 14:28:32 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Krusch",
"Steffen",
""
]
] | This paper discusses Skyrmions on the 3-sphere coupled to fermions. The resulting Dirac equation commutes with a generalized angular momentum G. For G = 0 the Dirac equation can be solved explicitly for a constant Skyrme configuration and also for a SO(4) symmetric hedgehog configuration. We discuss how the spectrum ch... | 10.588951 | 10.038713 | 10.635188 | 9.767733 | 9.803233 | 10.245008 | 9.707369 | 9.626458 | 9.980512 | 10.342598 | 9.743739 | 10.322646 | 10.516835 | 9.942467 | 10.06863 | 10.162031 | 9.982356 | 10.048114 | 10.084183 | 10.411272 | 9.849162 |
hep-th/0610275 | Ta-Sheng Tai | Ta-Sheng Tai and Satoshi Yamaguchi | Correlator of Fundamental and Anti-symmetric Wilson Loops in AdS/CFT
Correspondence | 22 pages, 5 figures, v2: typos corrected, v3: final version in JHEP | JHEP 0702:035,2007 | 10.1088/1126-6708/2007/02/035 | UT-06-22, IHES/P/06/53 | hep-th | null | We study the two circular Wilson loop correlator in which one is of
anti-symmetric representation, while the other is of fundamental representation
in 4-dimensional ${\cal N}=4$ super Yang-Mills theory. This correlator has a
good AdS dual, which is a system of a D5-brane and a fundamental string. We
calculated the on... | [
{
"created": "Thu, 26 Oct 2006 08:15:21 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Nov 2006 05:39:54 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Mar 2007 10:42:13 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Tai",
"Ta-Sheng",
""
],
[
"Yamaguchi",
"Satoshi",
""
]
] | We study the two circular Wilson loop correlator in which one is of anti-symmetric representation, while the other is of fundamental representation in 4-dimensional ${\cal N}=4$ super Yang-Mills theory. This correlator has a good AdS dual, which is a system of a D5-brane and a fundamental string. We calculated the on-s... | 8.447505 | 7.592686 | 8.435506 | 7.032469 | 6.611691 | 7.276147 | 7.391592 | 6.965107 | 6.756553 | 9.206229 | 7.393485 | 7.356815 | 7.640553 | 7.402129 | 7.122309 | 7.292363 | 7.405513 | 7.299552 | 7.289863 | 7.644146 | 7.341268 |
1903.04511 | Federico Galli | Alice Bernamonti, Federico Galli, Juan Hernandez, Robert C. Myers,
Shan-Ming Ruan, Joan Sim\'on | The First Law of Complexity | 7 pages + supplemental material, 2 figures; v2: clarifications and
reference added, published version | Phys. Rev. Lett. 123, 081601 (2019) | 10.1103/PhysRevLett.123.081601 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the variation of holographic complexity for two nearby target
states. Based on Nielsen's geometric approach, we find the variation only
depends on the end point of the optimal trajectory, a result which we designate
the first law of complexity. As an example, we examine the complexity=action
conjecture... | [
{
"created": "Mon, 11 Mar 2019 18:01:08 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Feb 2020 13:34:25 GMT",
"version": "v2"
}
] | 2020-02-28 | [
[
"Bernamonti",
"Alice",
""
],
[
"Galli",
"Federico",
""
],
[
"Hernandez",
"Juan",
""
],
[
"Myers",
"Robert C.",
""
],
[
"Ruan",
"Shan-Ming",
""
],
[
"Simón",
"Joan",
""
]
] | We investigate the variation of holographic complexity for two nearby target states. Based on Nielsen's geometric approach, we find the variation only depends on the end point of the optimal trajectory, a result which we designate the first law of complexity. As an example, we examine the complexity=action conjecture w... | 13.287937 | 12.681909 | 15.073775 | 11.499345 | 13.843305 | 12.848624 | 14.026339 | 11.754787 | 13.028887 | 18.513786 | 11.757418 | 12.703918 | 14.238963 | 12.804062 | 12.930902 | 13.25063 | 12.900825 | 12.94257 | 13.284446 | 13.870381 | 12.675415 |
hep-th/9807164 | Steven S. Gubser | Steven S. Gubser | Einstein manifolds and conformal field theories | 13 pages, latex, no figures, minor changes and references added | Phys. Rev. D 59, 025006 (1998) | 10.1103/PhysRevD.59.025006 | PUPT-1805 | hep-th | null | In light of the AdS/CFT correspondence, it is natural to try to define a
conformal field theory in a large N, strong coupling limit via a supergravity
compactification on the product of an Einstein manifold and anti-de Sitter
space. We consider the five-dimensional manifolds T^{pq} which are coset spaces
(SU(2) x SU(... | [
{
"created": "Tue, 21 Jul 1998 22:28:37 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Aug 1998 19:51:45 GMT",
"version": "v2"
}
] | 2016-08-25 | [
[
"Gubser",
"Steven S.",
""
]
] | In light of the AdS/CFT correspondence, it is natural to try to define a conformal field theory in a large N, strong coupling limit via a supergravity compactification on the product of an Einstein manifold and anti-de Sitter space. We consider the five-dimensional manifolds T^{pq} which are coset spaces (SU(2) x SU(2)... | 7.449461 | 6.917572 | 8.625197 | 6.666447 | 7.669787 | 6.914259 | 6.67478 | 6.968349 | 6.687623 | 8.269217 | 6.841715 | 7.013862 | 7.488845 | 6.993505 | 6.860894 | 6.879248 | 7.104101 | 7.013122 | 7.013353 | 7.5093 | 6.877383 |
1303.3044 | Julien Garaud | Julien Garaud, Eugen Radu and Mikhail S. Volkov | Stable Cosmic Vortons | 8 pages, 5 figures, improved and extended as compared to the first
version, published | Phys. Rev. Lett. 111, 171602 (2013) | 10.1103/PhysRevLett.111.171602 | null | hep-th astro-ph.CO cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present for the first time solutions in the gauged $U(1)\times U(1)$ model
of Witten describing vortons -- spinning flux loops stabilized against
contraction by the centrifugal force. Vortons were heuristically described many
years ago, however, the corresponding field theory solutions were not obtained
and so the... | [
{
"created": "Tue, 5 Mar 2013 13:00:05 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Oct 2013 12:33:20 GMT",
"version": "v2"
}
] | 2013-10-29 | [
[
"Garaud",
"Julien",
""
],
[
"Radu",
"Eugen",
""
],
[
"Volkov",
"Mikhail S.",
""
]
] | We present for the first time solutions in the gauged $U(1)\times U(1)$ model of Witten describing vortons -- spinning flux loops stabilized against contraction by the centrifugal force. Vortons were heuristically described many years ago, however, the corresponding field theory solutions were not obtained and so the s... | 11.657718 | 13.110827 | 12.638865 | 10.892756 | 11.205212 | 11.362987 | 11.862739 | 10.927238 | 11.257162 | 12.631529 | 10.796842 | 11.10422 | 10.939867 | 10.645202 | 11.416338 | 11.123985 | 10.832121 | 11.051554 | 10.865216 | 11.448786 | 10.83635 |
1808.07883 | Alessandro Strumia | Alberto Salvio, Alessandro Strumia and Hardi Veermae | New infra-red enhancements in 4-derivative gravity | 20 pages, 3 figures | null | 10.1140/epjc/s10052-018-6311-1 | CERN-TH-2018-195 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | 4-derivative gravity provides a renormalizable theory of quantum gravity at
the price of introducing a physical ghost, which could admit a sensible
positive-energy quantization. To understand its physics, we compute
ghost-mediated scatterings among matter particles at tree-level, finding a new
power-like infra-red en... | [
{
"created": "Thu, 23 Aug 2018 18:00:13 GMT",
"version": "v1"
}
] | 2018-11-14 | [
[
"Salvio",
"Alberto",
""
],
[
"Strumia",
"Alessandro",
""
],
[
"Veermae",
"Hardi",
""
]
] | 4-derivative gravity provides a renormalizable theory of quantum gravity at the price of introducing a physical ghost, which could admit a sensible positive-energy quantization. To understand its physics, we compute ghost-mediated scatterings among matter particles at tree-level, finding a new power-like infra-red enha... | 18.95874 | 19.06076 | 17.197577 | 16.00193 | 19.587034 | 19.107386 | 18.72168 | 17.814568 | 15.825464 | 18.625671 | 18.258839 | 15.95887 | 16.749592 | 15.892688 | 16.080671 | 15.434205 | 16.278128 | 16.296511 | 16.446348 | 16.086008 | 16.521841 |
hep-th/0302062 | Michael Maziashvili | Michael Maziashvili | Particle production related to the tunneling in false vacuum decay | LaTeX, 6 pages | Mod.Phys.Lett. A18 (2003) 993 | 10.1142/S0217732303010806 | null | hep-th | null | Motivated by the work of Mersini, the particle production related to the
tunneling in false vacuum decay is carefully investigated in the thin-wall
approximation. It is shown that in this case the particle production is
exponentially suppressed even when the momentum is comparable to the curvature
scale of the bubble... | [
{
"created": "Mon, 10 Feb 2003 08:26:24 GMT",
"version": "v1"
},
{
"created": "Sat, 15 Feb 2003 11:42:50 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Maziashvili",
"Michael",
""
]
] | Motivated by the work of Mersini, the particle production related to the tunneling in false vacuum decay is carefully investigated in the thin-wall approximation. It is shown that in this case the particle production is exponentially suppressed even when the momentum is comparable to the curvature scale of the bubble. ... | 12.068755 | 8.596485 | 10.200993 | 8.721377 | 9.003117 | 9.376485 | 9.753029 | 8.561982 | 9.053697 | 10.640421 | 8.786758 | 10.078363 | 10.282165 | 10.089151 | 10.313844 | 10.24741 | 10.526259 | 10.072823 | 9.953486 | 10.812202 | 9.994013 |
2106.03522 | Michael Thies | Michael Thies | Twisted kink dynamics in multiflavor chiral Gross-Neveu model | 20 pages, no figure; v2: A remark and a reference added | null | 10.1088/1751-8121/ac3cde | null | hep-th cond-mat.str-el hep-ph | http://creativecommons.org/licenses/by/4.0/ | The Gross-Neveu model with ${\rm U}_L(N_f)\times{\rm U}_R(N_f)$ chiral
symmetry is reconsidered in the large $N_c$ limit. The known analytical
solution for the time dependent interaction of any number of twisted kinks and
breathers is cast into a more revealing form. The ($x,t$)-dependent factors are
isolated from co... | [
{
"created": "Mon, 7 Jun 2021 11:28:40 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jun 2021 15:17:32 GMT",
"version": "v2"
}
] | 2021-12-22 | [
[
"Thies",
"Michael",
""
]
] | The Gross-Neveu model with ${\rm U}_L(N_f)\times{\rm U}_R(N_f)$ chiral symmetry is reconsidered in the large $N_c$ limit. The known analytical solution for the time dependent interaction of any number of twisted kinks and breathers is cast into a more revealing form. The ($x,t$)-dependent factors are isolated from cons... | 11.580244 | 11.291892 | 12.296584 | 10.467627 | 11.952918 | 10.973979 | 10.943007 | 10.207291 | 10.628672 | 13.014839 | 10.533257 | 10.767724 | 10.613318 | 10.277808 | 10.484066 | 10.555339 | 11.140006 | 10.216575 | 10.475669 | 11.015847 | 10.640438 |
0911.2152 | Piotr Korcyl | Piotr Korcyl | Exact solutions to D=2 Supersymmetric Yang-Mills Quantum Mechanics with
SU(3) gauge group | Proceedings of the XLIX Cracow School of Theoretical Physics, 2009 | Acta Phys. Polon. Supp.2:623, 2009 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we present the cut Fock space approach to the D=d+1=2,
Supersymmetric Yang-Mills Quantum Mechanics (SYMQM). We start by briefly
introducing the main features of the framework. We concentrate on those
properties of the method which make it a convenient set up not only for
numerical calculations but als... | [
{
"created": "Wed, 11 Nov 2009 14:42:26 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Korcyl",
"Piotr",
""
]
] | In this article we present the cut Fock space approach to the D=d+1=2, Supersymmetric Yang-Mills Quantum Mechanics (SYMQM). We start by briefly introducing the main features of the framework. We concentrate on those properties of the method which make it a convenient set up not only for numerical calculations but also ... | 9.780522 | 9.687268 | 10.856314 | 9.009813 | 9.671802 | 9.038806 | 9.962373 | 9.320065 | 9.34456 | 10.399679 | 9.491361 | 9.577673 | 9.728495 | 9.375096 | 9.262274 | 9.311647 | 9.968678 | 9.313334 | 9.315971 | 10.003015 | 9.045173 |
hep-th/9608102 | Horacio A. Falomir | Horacio Alberto Falomir, Ricardo Enrique Gamboa Saravi, Mar\'{\I}a
Amelia Muschietti, Eve Mariel Santangelo and Jorge Eduardo Solomin | On the relation between determinants and Green functions of elliptic
operators with local boundary conditions | standard LaTeX, 14 pages | null | null | null | hep-th funct-an math.FA | null | A formula relating quotients of determinants of elliptic differential
operators sharing their principal symbol, with local boundary conditions, to
the corresponding Green function is given.
| [
{
"created": "Thu, 15 Aug 1996 18:33:25 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Falomir",
"Horacio Alberto",
""
],
[
"Saravi",
"Ricardo Enrique Gamboa",
""
],
[
"Muschietti",
"Mar\\'{\\I}a Amelia",
""
],
[
"Santangelo",
"Eve Mariel",
""
],
[
"Solomin",
"Jorge Eduardo",
""
]
] | A formula relating quotients of determinants of elliptic differential operators sharing their principal symbol, with local boundary conditions, to the corresponding Green function is given. | 24.351603 | 21.260435 | 23.183609 | 18.922441 | 20.458254 | 25.905031 | 19.983246 | 20.999512 | 26.397585 | 28.303106 | 20.909145 | 21.570683 | 22.789783 | 24.452118 | 20.46278 | 20.528593 | 21.55377 | 22.050224 | 21.188559 | 23.070953 | 24.459534 |
hep-th/9508006 | Adi Armoni | A. Armoni and J. Sonnenschein | Mesonic Spectra of Bosonized QCD_2 Models | 17 pages, Latex | Nucl.Phys. B457 (1995) 81-95 | 10.1016/0550-3213(95)00505-6 | TAUP-2285-95 | hep-th | null | We discuss bosonized two-dimensional QCD with massless fermions in the
adjoint and multi-flavor fundamental representations. We evaluate the massive
mesonic spectra of several models by using the light-front quantization and
diagonalizing the mass operator $M^2=2P^+P^- $. We recover previous results in
the case of on... | [
{
"created": "Wed, 2 Aug 1995 10:55:17 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Armoni",
"A.",
""
],
[
"Sonnenschein",
"J.",
""
]
] | We discuss bosonized two-dimensional QCD with massless fermions in the adjoint and multi-flavor fundamental representations. We evaluate the massive mesonic spectra of several models by using the light-front quantization and diagonalizing the mass operator $M^2=2P^+P^- $. We recover previous results in the case of one ... | 10.180029 | 7.272189 | 9.602124 | 7.656127 | 8.47513 | 9.145201 | 7.707381 | 7.378695 | 8.5323 | 9.263303 | 8.002174 | 8.200648 | 8.650376 | 8.107106 | 8.486289 | 8.351418 | 8.612811 | 7.794169 | 8.914293 | 9.11893 | 8.097231 |
hep-th/0510189 | Mohammad M. Sheikh-Jabbari | Darius Sadri, M. M. Sheikh-Jabbari | Integrable Spin Chains on the Conformal Moose | 53 pages, 14 eps figures; Added references | JHEP 0603:024,2006 | 10.1088/1126-6708/2006/03/024 | IPM/P-2005/037, SU-ITP-05/30 | hep-th | null | We consider N=1, D=4 superconformal U(N)^{pq} Yang-Mills theories dual to
AdS_5xS^5/Z_pxZ_q orbifolds. We construct the dilatation operator of this
superconformal gauge theory at one-loop planar level. We demonstrate that a
specific sector of this dilatation operator can be thought of as the transfer
matrix for a two... | [
{
"created": "Sat, 22 Oct 2005 22:14:41 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Nov 2005 07:15:54 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Sadri",
"Darius",
""
],
[
"Sheikh-Jabbari",
"M. M.",
""
]
] | We consider N=1, D=4 superconformal U(N)^{pq} Yang-Mills theories dual to AdS_5xS^5/Z_pxZ_q orbifolds. We construct the dilatation operator of this superconformal gauge theory at one-loop planar level. We demonstrate that a specific sector of this dilatation operator can be thought of as the transfer matrix for a two-d... | 9.707288 | 9.492325 | 11.294188 | 9.353489 | 9.451278 | 10.010439 | 10.403665 | 9.469599 | 9.060952 | 11.65518 | 9.47751 | 9.636773 | 10.055263 | 9.40132 | 9.097858 | 9.415022 | 9.350142 | 9.366332 | 9.213989 | 9.949448 | 9.222871 |
1011.0574 | Ion Vasile Vancea | R. Nardi, M. A. Santos and I. V. Vancea | Thermal magnetized D-branes on $R^{1,p}\times T^{d-p-1}$ in the
generalized Thermo Field Dynamics approach | Minor error and misprints corrected. 22 pages | J.Phys.A44:235403,2011 | 10.1088/1751-8113/44/23/235403 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the D-brane states at finite temperature in thermal equilibrium
in the $\mathbb{R}^{1,p}\times{\mathbb{T}}^{d-p-1}$ spacetime in the presence
of cold (unthermalized) Kalb-Ramond (KR) and U(1) gauge potential background.
To this end, we first generalize the Thermo Field Dynamics (TFD) to wrapped
closed st... | [
{
"created": "Tue, 2 Nov 2010 11:23:10 GMT",
"version": "v1"
},
{
"created": "Mon, 9 May 2011 12:40:13 GMT",
"version": "v2"
}
] | 2011-05-13 | [
[
"Nardi",
"R.",
""
],
[
"Santos",
"M. A.",
""
],
[
"Vancea",
"I. V.",
""
]
] | We construct the D-brane states at finite temperature in thermal equilibrium in the $\mathbb{R}^{1,p}\times{\mathbb{T}}^{d-p-1}$ spacetime in the presence of cold (unthermalized) Kalb-Ramond (KR) and U(1) gauge potential background. To this end, we first generalize the Thermo Field Dynamics (TFD) to wrapped closed stri... | 6.740129 | 6.509372 | 6.962895 | 6.685016 | 7.038781 | 6.363455 | 6.617145 | 6.47019 | 6.095745 | 7.328858 | 6.294291 | 6.32093 | 6.773306 | 6.393027 | 6.45266 | 6.427239 | 6.43117 | 6.367095 | 6.269297 | 6.721193 | 6.263385 |
0910.3596 | Rodrigo Ferreira Sobreiro | A. J. Gomez, M. S. Guimaraes, R. F. Sobreiro, S. P. Sorella | Equivalence between Zwanziger's horizon function and Gribov's no-pole
ghost form factor | 9 pp. No figures. Final version to appear in Physics Letters B | Phys.Lett.B683:217-221,2010 | 10.1016/j.physletb.2009.12.001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The ghost form factor entering the Gribov no-pole condition is evaluated till
the third order in the gauge fields. The resulting expression turns out to
coincide with Zwanziger's horizon function implementing the restriction to the
Gribov region in the functional integral.
| [
{
"created": "Mon, 19 Oct 2009 18:10:42 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Dec 2009 18:22:30 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Gomez",
"A. J.",
""
],
[
"Guimaraes",
"M. S.",
""
],
[
"Sobreiro",
"R. F.",
""
],
[
"Sorella",
"S. P.",
""
]
] | The ghost form factor entering the Gribov no-pole condition is evaluated till the third order in the gauge fields. The resulting expression turns out to coincide with Zwanziger's horizon function implementing the restriction to the Gribov region in the functional integral. | 19.042791 | 12.495945 | 15.48673 | 13.028455 | 12.247829 | 10.256865 | 13.887705 | 12.345691 | 10.274396 | 20.066616 | 13.10469 | 14.003644 | 19.073248 | 15.658468 | 15.568668 | 13.464556 | 15.195999 | 15.474256 | 14.456423 | 16.386467 | 14.958858 |
hep-th/0412150 | Anamaria Font | A. Font, L.E. Ibanez | SUSY-breaking Soft Terms in a MSSM Magnetized D7-brane Model | Latex, 27 pages, v2: added references | JHEP 0503:040,2005 | 10.1088/1126-6708/2005/03/040 | IFT-UAM/CSIC-04-62 | hep-th hep-ph | null | We compute the SUSY-breaking soft terms in a magnetized D7-brane model with
MSSM-like spectrum, under the general assumption of non-vanishing auxiliary
fields of the dilaton and Kahler moduli. As a particular scenario we discuss
SUSY breaking triggered by ISD or IASD 3-form fluxes.
| [
{
"created": "Tue, 14 Dec 2004 17:20:03 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Dec 2004 15:40:54 GMT",
"version": "v2"
}
] | 2010-12-03 | [
[
"Font",
"A.",
""
],
[
"Ibanez",
"L. E.",
""
]
] | We compute the SUSY-breaking soft terms in a magnetized D7-brane model with MSSM-like spectrum, under the general assumption of non-vanishing auxiliary fields of the dilaton and Kahler moduli. As a particular scenario we discuss SUSY breaking triggered by ISD or IASD 3-form fluxes. | 8.718035 | 8.03893 | 10.507441 | 7.376438 | 8.538968 | 8.432447 | 8.816122 | 8.757224 | 8.87238 | 11.083407 | 8.592698 | 8.564028 | 8.525057 | 8.344053 | 8.511038 | 8.512767 | 8.15827 | 8.069839 | 8.041127 | 8.154405 | 8.295834 |
hep-th/9507050 | Edward Witten | Cumrun Vafa and Edward Witten | Dual String Pairs With N=1 And N=2 Supersymmetry In Four Dimensions | 40 pages | Nucl.Phys.Proc.Suppl.46:225-247,1996 | 10.1016/0920-5632(96)00025-4 | HUTP-95/A023, IASSNS-HEP-95-58 | hep-th | null | Based on a simple adiabatic argument and by considering the heterotic string
counterpart of certain symmetries of Type II superstrings such as $(-1)^{F_L}$
and orientation reversal, we construct orbifold candidates for dual pairs of
heterotic and Type II string theories with $N=2$ and $N=1$ supersymmetry. We
also ana... | [
{
"created": "Fri, 7 Jul 1995 19:15:01 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Jul 1995 20:12:57 GMT",
"version": "v2"
}
] | 2010-04-07 | [
[
"Vafa",
"Cumrun",
""
],
[
"Witten",
"Edward",
""
]
] | Based on a simple adiabatic argument and by considering the heterotic string counterpart of certain symmetries of Type II superstrings such as $(-1)^{F_L}$ and orientation reversal, we construct orbifold candidates for dual pairs of heterotic and Type II string theories with $N=2$ and $N=1$ supersymmetry. We also analy... | 8.367767 | 8.288357 | 9.325582 | 8.058319 | 8.593778 | 8.542953 | 8.771945 | 8.576997 | 7.71904 | 9.075287 | 8.652637 | 8.344103 | 8.786713 | 8.103796 | 8.203485 | 8.397351 | 8.118716 | 8.138259 | 8.144292 | 8.625588 | 7.957452 |
0903.4638 | Joyce Myers | Joyce C. Myers, Michael C. Ogilvie | Phase diagrams of SU(N) gauge theories with fermions in various
representations | 39 pages, 26 figures, JHEP3; references added, small corrections made | JHEP 0907:095,2009 | 10.1088/1126-6708/2009/07/095 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We minimize the one-loop effective potential for SU(N) gauge theories
including fermions with finite mass in the fundamental (F), adjoint (Adj),
symmetric (S), and antisymmetric (AS) representations. We calculate the phase
diagram on S^1 x R^3 as a function of the length of the compact dimension,
beta, and the fermio... | [
{
"created": "Thu, 26 Mar 2009 17:04:07 GMT",
"version": "v1"
},
{
"created": "Tue, 5 May 2009 12:54:50 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Jul 2009 18:47:09 GMT",
"version": "v3"
}
] | 2009-08-05 | [
[
"Myers",
"Joyce C.",
""
],
[
"Ogilvie",
"Michael C.",
""
]
] | We minimize the one-loop effective potential for SU(N) gauge theories including fermions with finite mass in the fundamental (F), adjoint (Adj), symmetric (S), and antisymmetric (AS) representations. We calculate the phase diagram on S^1 x R^3 as a function of the length of the compact dimension, beta, and the fermion ... | 7.330485 | 8.099639 | 7.969672 | 7.390025 | 8.089007 | 8.550487 | 7.934576 | 7.765103 | 7.520754 | 8.237181 | 7.527429 | 7.247071 | 7.209935 | 7.08954 | 7.205897 | 7.256083 | 7.356205 | 7.040747 | 7.209218 | 7.378065 | 6.971478 |
0902.2833 | Masaaki Watanabe | Masa-aki Watanabe, Sugumi Kanno, and Jiro Soda | Inflationary Universe with Anisotropic Hair | 10 pages, 2 figures; an error in abstract corrected; (v2) replaced
with version accepted by PRL, title changed from "Hairy Inflation" | Phys.Rev.Lett.102:191302,2009 | 10.1103/PhysRevLett.102.191302 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study an inflationary scenario with a vector field coupled with an
inflaton field and show that the inflationary universe is endowed with
anisotropy for a wide range of coupling functions. This anisotropic inflation
is a tracking solution where the energy density of the vector field follows
that of the inflaton fi... | [
{
"created": "Tue, 17 Feb 2009 04:55:47 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Apr 2009 07:52:45 GMT",
"version": "v2"
}
] | 2009-06-30 | [
[
"Watanabe",
"Masa-aki",
""
],
[
"Kanno",
"Sugumi",
""
],
[
"Soda",
"Jiro",
""
]
] | We study an inflationary scenario with a vector field coupled with an inflaton field and show that the inflationary universe is endowed with anisotropy for a wide range of coupling functions. This anisotropic inflation is a tracking solution where the energy density of the vector field follows that of the inflaton fiel... | 7.518921 | 6.241614 | 6.974634 | 6.143463 | 6.502855 | 6.511158 | 6.504725 | 6.553688 | 6.224233 | 6.604284 | 6.535056 | 6.870827 | 6.817602 | 6.79608 | 6.740899 | 6.907692 | 6.941915 | 6.675406 | 7.10361 | 6.60471 | 7.066449 |
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