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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9212002 | Haruhiko Terao | Haruhiko Terao | Two Dimensional Black Hole Evapolation in the Light-Cone Gauge | 10 pages, KANAZAWA-92-19 | Prog.Theor.Phys.Suppl.114:175-184,1993 | 10.1143/PTPS.114.175 | null | hep-th | null | Quantization of the pure $1+1$ dimensional dilaton gravity is examined in the
light-cone gauge. It is found that the total action including ghosts generates
a $c=0$ free conformal field theory without modification of the classical
action, which is required in the conformal gauge. We also study semiclassical
equations... | [
{
"created": "Tue, 1 Dec 1992 11:56:57 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Terao",
"Haruhiko",
""
]
] | Quantization of the pure $1+1$ dimensional dilaton gravity is examined in the light-cone gauge. It is found that the total action including ghosts generates a $c=0$ free conformal field theory without modification of the classical action, which is required in the conformal gauge. We also study semiclassical equations o... | 8.5727 | 7.158363 | 8.512 | 7.536923 | 7.762228 | 7.702118 | 7.628543 | 7.452473 | 7.470376 | 7.585465 | 7.367627 | 7.496981 | 7.997525 | 7.349448 | 7.882498 | 7.507159 | 7.480094 | 7.725966 | 7.329859 | 8.084621 | 7.940901 |
0709.4392 | Ruslan Metsaev | R. R. Metsaev | Ordinary-derivative formulation of conformal totally symmetric arbitrary
spin bosonic fields | 51 pages, v2: Results and conclusions of v1 unchanged. In Sec.3,
brief review of higher-derivative approaches added. In Sec.4, new
representations for Lagrangian, modified de Donder gauge, and de
Donder-Stueckelberg gauge added. In Sec.5, discussion of interrelations
between the ordinary-derivative and higher-d... | null | 10.1007/JHEP06(2012)062 | FIAN-TD-2007-11 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Conformal totally symmetric arbitrary spin bosonic fields in flat space-time
of even dimension greater than or equal to four are studied. Second-derivative
(ordinary-derivative) formulation for such fields is developed. We obtain gauge
invariant Lagrangian and the corresponding gauge transformations. Gauge
symmetries... | [
{
"created": "Thu, 27 Sep 2007 13:42:14 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Apr 2012 18:12:10 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"Metsaev",
"R. R.",
""
]
] | Conformal totally symmetric arbitrary spin bosonic fields in flat space-time of even dimension greater than or equal to four are studied. Second-derivative (ordinary-derivative) formulation for such fields is developed. We obtain gauge invariant Lagrangian and the corresponding gauge transformations. Gauge symmetries a... | 7.695971 | 4.815691 | 8.766788 | 5.437923 | 5.222806 | 4.789767 | 4.575065 | 5.289011 | 5.297013 | 8.777236 | 5.350995 | 6.161775 | 7.530159 | 6.374799 | 6.259488 | 6.337412 | 6.110681 | 6.413546 | 6.597374 | 7.421098 | 6.536263 |
2005.05028 | Naoki Yamamoto | Naoki Yamamoto | Magnetic monopoles and fermion number violation in chiral matter | 5 pages | null | null | null | hep-th astro-ph.CO cond-mat.mes-hall hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the presence of a magnetic monopole in position space gives rise
to a violation of the fermion number conservation in chiral matter. Using the
chiral kinetic theory, we derive a model-independent expression of such a
violation in nonequilibrium many-body systems of chiral fermions. In local
thermal equil... | [
{
"created": "Mon, 11 May 2020 12:03:10 GMT",
"version": "v1"
}
] | 2020-05-12 | [
[
"Yamamoto",
"Naoki",
""
]
] | We show that the presence of a magnetic monopole in position space gives rise to a violation of the fermion number conservation in chiral matter. Using the chiral kinetic theory, we derive a model-independent expression of such a violation in nonequilibrium many-body systems of chiral fermions. In local thermal equilib... | 6.714559 | 7.128492 | 7.009614 | 6.491628 | 7.117722 | 6.985813 | 7.238812 | 6.754386 | 6.470223 | 6.915978 | 6.361576 | 6.473297 | 6.552664 | 6.335931 | 6.484145 | 6.505924 | 6.532377 | 6.389174 | 6.344395 | 6.463645 | 6.378765 |
0806.1954 | Marco Caldarelli | Marco M. Caldarelli, Roberto Emparan, Maria J. Rodriguez | Black Rings in (Anti)-deSitter space | 38 pages, 6 figures. v2: changes in terminology, refs added. v3:
minor improvements, refs added, published version | JHEP 0811:011,2008 | 10.1088/1126-6708/2008/11/011 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct solutions for thin black rings in Anti-deSitter and deSitter
spacetimes using approximate methods. Black rings in AdS exist with arbitrarily
large radius and satisfy a bound |J| \leq LM, which they saturate as their
radius becomes infinitely large. For angular momentum near the maximum, they
have larger ... | [
{
"created": "Thu, 12 Jun 2008 16:24:37 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jun 2008 17:37:33 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Jan 2009 18:18:12 GMT",
"version": "v3"
}
] | 2009-12-10 | [
[
"Caldarelli",
"Marco M.",
""
],
[
"Emparan",
"Roberto",
""
],
[
"Rodriguez",
"Maria J.",
""
]
] | We construct solutions for thin black rings in Anti-deSitter and deSitter spacetimes using approximate methods. Black rings in AdS exist with arbitrarily large radius and satisfy a bound |J| \leq LM, which they saturate as their radius becomes infinitely large. For angular momentum near the maximum, they have larger ar... | 12.894785 | 13.90544 | 12.237082 | 12.216423 | 12.016316 | 12.511733 | 12.792492 | 12.602696 | 12.620021 | 14.210775 | 11.611055 | 12.132957 | 11.995967 | 12.106421 | 11.996193 | 12.052742 | 12.020124 | 11.962157 | 12.023003 | 12.435559 | 12.109828 |
1606.09479 | Jiri Prochazka PhD | Jiri Prochazka, Vojtech Kundrat | Eikonal model analysis of elastic proton-proton collisions at 52.8 GeV
and 8 TeV | 31 pages, 37 figures, 2 tables | Eur. Phys. J. C (2020) 80: 779 | 10.1140/epjc/s10052-020-8334-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Under the influence of standardly used description of Coulomb-hadronic
interference proposed by West and Yennie the protons have been interpreted as
transparent objects; elastic events have been interpreted as more central than
inelastic ones. It will be shown that using eikonal model the protons may be
interpreted i... | [
{
"created": "Thu, 30 Jun 2016 13:26:55 GMT",
"version": "v1"
},
{
"created": "Thu, 18 May 2017 16:05:16 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Sep 2017 14:34:52 GMT",
"version": "v3"
},
{
"created": "Tue, 16 Apr 2019 15:15:26 GMT",
"version": "v4"
},
{
"c... | 2022-03-14 | [
[
"Prochazka",
"Jiri",
""
],
[
"Kundrat",
"Vojtech",
""
]
] | Under the influence of standardly used description of Coulomb-hadronic interference proposed by West and Yennie the protons have been interpreted as transparent objects; elastic events have been interpreted as more central than inelastic ones. It will be shown that using eikonal model the protons may be interpreted in ... | 17.543791 | 21.344963 | 13.865072 | 14.754085 | 20.686552 | 23.086464 | 18.170071 | 20.786152 | 17.728428 | 17.52293 | 19.226126 | 19.077465 | 16.185789 | 16.217712 | 17.259817 | 18.32682 | 16.715263 | 17.897051 | 16.618628 | 16.365498 | 18.01413 |
hep-th/0011214 | Jerzy Lukierski | J. Lukierski (Wroclaw, Poland), P.C. Stichel (Bielefeld, Germany) and
W.J. Zakrzewski (Durham, UK) | Chern-Simons Particles with Nonstandard Gravitational Interaction | LaTeX, 1 figure (included), 14 pages | Eur.Phys.J.C20:759-765,2001 | 10.1007/s100520100683 | null | hep-th | null | The model of nonrelativistic particles coupled to nonstandard (2+1)-gravity
[1] is extended to include Abelian or non-Abelian charges coupled to
Chern-Simons gauge fields. Equivalently, the model may be viewed as describing
the (Abelian or non-Abelian) anyonic dynamics of Chern-Simons particles
coupled, in a reparame... | [
{
"created": "Thu, 23 Nov 2000 16:25:58 GMT",
"version": "v1"
}
] | 2009-01-07 | [
[
"Lukierski",
"J.",
"",
"Wroclaw, Poland"
],
[
"Stichel",
"P. C.",
"",
"Bielefeld, Germany"
],
[
"Zakrzewski",
"W. J.",
"",
"Durham, UK"
]
] | The model of nonrelativistic particles coupled to nonstandard (2+1)-gravity [1] is extended to include Abelian or non-Abelian charges coupled to Chern-Simons gauge fields. Equivalently, the model may be viewed as describing the (Abelian or non-Abelian) anyonic dynamics of Chern-Simons particles coupled, in a reparametr... | 9.629682 | 8.366981 | 9.674595 | 8.359374 | 9.087916 | 8.744914 | 8.890203 | 8.49563 | 8.699582 | 9.701134 | 8.507808 | 8.602086 | 9.669502 | 8.66543 | 8.927978 | 8.934594 | 8.792994 | 8.635834 | 8.966864 | 9.175717 | 9.054052 |
2008.02190 | Eric Perlmutter | Justin Kaidi, Eric Perlmutter | Discreteness and Integrality in Conformal Field Theory | 76 pages; v3: references added, minor changes | null | 10.1007/JHEP02(2021)064 | CALT-TH 2020-033 | hep-th math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Various observables in compact CFTs are required to obey positivity,
discreteness, and integrality. Positivity forms the crux of the conformal
bootstrap, but understanding of the abstract implications of discreteness and
integrality for the space of CFTs is lacking. We systematically study these
constraints in two-di... | [
{
"created": "Wed, 5 Aug 2020 15:38:15 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Aug 2020 16:33:00 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Oct 2020 00:38:36 GMT",
"version": "v3"
}
] | 2021-02-24 | [
[
"Kaidi",
"Justin",
""
],
[
"Perlmutter",
"Eric",
""
]
] | Various observables in compact CFTs are required to obey positivity, discreteness, and integrality. Positivity forms the crux of the conformal bootstrap, but understanding of the abstract implications of discreteness and integrality for the space of CFTs is lacking. We systematically study these constraints in two-dime... | 9.174099 | 10.099375 | 10.453892 | 9.303084 | 10.040145 | 9.673803 | 9.64957 | 9.012687 | 9.363164 | 11.195817 | 8.98466 | 9.191768 | 9.48672 | 9.359907 | 9.358498 | 9.221154 | 9.371572 | 9.243765 | 9.04756 | 9.788636 | 9.076609 |
1912.04581 | Toshihide Shibasaki | Masaki Honda, Toshihide Shibasaki | Wilson-line Scalar as a Nambu-Goldstone Boson in Flux Compactifications
and Higher-loop Corrections | 16 pages, 5 figures, version published in JHEP | JHEP 03 (2020) 031 | 10.1007/JHEP03(2020)031 | WU-HEP-19-09 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a scalar zero mode originated from extradimensional components of a
gauge field in a six-dimensional theory compactified on a magnetized torus. We
confirm it is a Nambu-Goldstone boson of the translational symmetry on the
torus which is breaking spontaneously due to magnetic flux. We also show
explicitly it ... | [
{
"created": "Tue, 10 Dec 2019 08:56:15 GMT",
"version": "v1"
},
{
"created": "Sun, 8 Mar 2020 05:57:46 GMT",
"version": "v2"
}
] | 2020-03-10 | [
[
"Honda",
"Masaki",
""
],
[
"Shibasaki",
"Toshihide",
""
]
] | We study a scalar zero mode originated from extradimensional components of a gauge field in a six-dimensional theory compactified on a magnetized torus. We confirm it is a Nambu-Goldstone boson of the translational symmetry on the torus which is breaking spontaneously due to magnetic flux. We also show explicitly it is... | 11.6214 | 10.794271 | 10.635374 | 10.076122 | 10.814732 | 10.106635 | 10.350978 | 10.865983 | 9.658867 | 10.07857 | 10.900434 | 10.492124 | 10.468758 | 10.124151 | 10.483204 | 10.289153 | 10.238928 | 10.423897 | 10.411473 | 10.534451 | 10.268474 |
hep-th/0311110 | Kasper Peeters | Kasper Peeters and Marija Zamaklar | Anti-de-Sitter vacua require fermionic brane charges | 10 pages | Phys.Rev. D69 (2004) 066009 | 10.1103/PhysRevD.69.066009 | AEI-2003-092 | hep-th | null | We argue that a modification of the super-AdS algebras which accounts for the
presence of D-branes requires not only the inclusion of bosonic brane charges,
but also the inclusion of new fermionic ones. We show that such fermionic brane
charges are indeed present in the matrix model and the supermembrane in the
pp-wa... | [
{
"created": "Thu, 13 Nov 2003 15:07:09 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Peeters",
"Kasper",
""
],
[
"Zamaklar",
"Marija",
""
]
] | We argue that a modification of the super-AdS algebras which accounts for the presence of D-branes requires not only the inclusion of bosonic brane charges, but also the inclusion of new fermionic ones. We show that such fermionic brane charges are indeed present in the matrix model and the supermembrane in the pp-wave... | 10.764258 | 8.952705 | 11.328954 | 9.333225 | 9.44469 | 9.674724 | 9.724944 | 8.853188 | 9.051423 | 11.223492 | 8.805964 | 9.114858 | 10.04725 | 9.214323 | 9.161405 | 8.746539 | 8.970998 | 8.699864 | 8.957033 | 10.517512 | 9.126581 |
hep-th/0608063 | Alberto Mariotti | A. Amariti, L. Girardello, A. Mariotti | Non-supersymmetric Meta-Stable vacua in SU(N) SQCD with adjoint matter | 14 pages, 2 figures | JHEP0612:058,2006 | 10.1088/1126-6708/2006/12/058 | null | hep-th | null | We investigate models of SU(N) SQCD with adjoint matter and non trivial
mesonic deformations. We apply standard methods in the dual magnetic theory and
we find meta-stable supersymmetry breaking vacua with arbitrary large lifetime.
We comment on the difference with known models.
| [
{
"created": "Wed, 9 Aug 2006 19:50:40 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Amariti",
"A.",
""
],
[
"Girardello",
"L.",
""
],
[
"Mariotti",
"A.",
""
]
] | We investigate models of SU(N) SQCD with adjoint matter and non trivial mesonic deformations. We apply standard methods in the dual magnetic theory and we find meta-stable supersymmetry breaking vacua with arbitrary large lifetime. We comment on the difference with known models. | 17.54423 | 12.240344 | 16.961834 | 13.88361 | 14.590447 | 13.789126 | 14.129787 | 13.752569 | 15.211876 | 18.601896 | 14.491079 | 14.372176 | 16.585825 | 14.916155 | 15.354035 | 15.582409 | 14.092312 | 15.087139 | 15.181847 | 17.425406 | 15.375484 |
hep-th/0410061 | Sugumi Kanno | Sugumi Kanno, Jiro Soda | On the Validity of a Factorizable Metric Ansatz in String Cosmology | 5 pages, Typos corrected. Published version | Phys.Rev. D71 (2005) 044031 | 10.1103/PhysRevD.71.044031 | KUNS-1936 | hep-th gr-qc | null | To support the validity of a factorizable metric ansatz used in string
cosmology, we investigate a toy problem in RSI model. For this purpose, we
revise the gradient expansion method to conform to the factorizable metric
ansatz. By solving the 5-dimensional equations of motion and substituting the
results into the ac... | [
{
"created": "Wed, 6 Oct 2004 10:23:17 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Apr 2005 08:36:10 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Kanno",
"Sugumi",
""
],
[
"Soda",
"Jiro",
""
]
] | To support the validity of a factorizable metric ansatz used in string cosmology, we investigate a toy problem in RSI model. For this purpose, we revise the gradient expansion method to conform to the factorizable metric ansatz. By solving the 5-dimensional equations of motion and substituting the results into the acti... | 9.37942 | 8.21925 | 8.842419 | 8.158587 | 8.172597 | 8.282815 | 7.601016 | 8.273273 | 7.694934 | 8.590418 | 8.76852 | 7.69709 | 8.479749 | 7.978851 | 7.927246 | 7.688893 | 7.570832 | 7.704864 | 8.323759 | 8.436039 | 8.072251 |
1203.0303 | Christopher Beem | Ibrahima Bah, Christopher Beem, Nikolay Bobev, Brian Wecht | Four-Dimensional SCFTs from M5-Branes | 45 pages, 11 figures | JHEP 06 (2012) 005 | 10.1007/JHEP06(2012)005 | MCTP-12-05; QMUL-PH-12-05 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We engineer a large new set of four-dimensional N=1 superconformal field
theories by wrapping M5-branes on complex curves. We present new supersymmetric
AdS_5 M-theory backgrounds which describe these fixed points at large N, and
then directly construct the dual four-dimensional CFTs for a certain subset of
these sol... | [
{
"created": "Thu, 1 Mar 2012 21:00:01 GMT",
"version": "v1"
}
] | 2012-06-05 | [
[
"Bah",
"Ibrahima",
""
],
[
"Beem",
"Christopher",
""
],
[
"Bobev",
"Nikolay",
""
],
[
"Wecht",
"Brian",
""
]
] | We engineer a large new set of four-dimensional N=1 superconformal field theories by wrapping M5-branes on complex curves. We present new supersymmetric AdS_5 M-theory backgrounds which describe these fixed points at large N, and then directly construct the dual four-dimensional CFTs for a certain subset of these solut... | 10.32353 | 8.204062 | 10.385885 | 8.484642 | 9.062955 | 8.293178 | 8.793592 | 8.019346 | 8.431014 | 10.972354 | 8.187259 | 8.527387 | 9.77125 | 8.599667 | 8.633942 | 8.268209 | 8.640613 | 8.537706 | 8.30248 | 9.856258 | 8.806647 |
0711.4967 | Dr. H. F. Jones | H. F. Jones | Equivalent Hamiltonian for Lee Model | 9 pages, no figures | Phys.Rev.D77:065023,2008 | 10.1103/PhysRevD.77.065023 | null | hep-th | null | Using the techniques of quasi-Hermitian quantum mechanics and quantum field
theory we use a similarity transformation to construct an equivalent Hermitian
Hamiltonian for the Lee model. In the field theory confined to the $V/N\theta$
sector it effectively decouples $V$, replacing the three-point interaction of
the or... | [
{
"created": "Fri, 30 Nov 2007 16:15:59 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Jones",
"H. F.",
""
]
] | Using the techniques of quasi-Hermitian quantum mechanics and quantum field theory we use a similarity transformation to construct an equivalent Hermitian Hamiltonian for the Lee model. In the field theory confined to the $V/N\theta$ sector it effectively decouples $V$, replacing the three-point interaction of the orig... | 11.220565 | 10.765817 | 11.514062 | 10.466527 | 11.765631 | 11.584649 | 11.300917 | 11.401128 | 10.553122 | 12.488097 | 10.833769 | 10.739968 | 10.592525 | 10.09034 | 10.713823 | 11.026133 | 10.802674 | 10.234139 | 10.63863 | 10.151923 | 10.192095 |
2206.03509 | Clifford V. Johnson | Clifford V. Johnson | Wigner meets 't Hooft near the black hole horizon | A quick read at 10 double-spaced pages (plus bibliography). Essay
written for the Gravity Research Foundation 2022 Awards for Essays on
Gravitation. (Honorable Mention awarded.) | null | 10.1142/S0218271822420032 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent work on Euclidean quantum gravity, black hole thermodynamics, and the
holographic principle has seen the return of random matrix models as a powerful
tool. It is explained how they allow for the study of the physics well beyond
the perturbative expansion. In fact, a fully non-perturbative treatment
naturally u... | [
{
"created": "Tue, 7 Jun 2022 18:00:04 GMT",
"version": "v1"
}
] | 2022-12-07 | [
[
"Johnson",
"Clifford V.",
""
]
] | Recent work on Euclidean quantum gravity, black hole thermodynamics, and the holographic principle has seen the return of random matrix models as a powerful tool. It is explained how they allow for the study of the physics well beyond the perturbative expansion. In fact, a fully non-perturbative treatment naturally uni... | 13.962844 | 13.272698 | 13.648776 | 12.350367 | 13.406746 | 13.019344 | 13.810853 | 13.62382 | 12.372128 | 14.131044 | 13.472692 | 13.03818 | 13.72509 | 13.097856 | 13.403648 | 13.760962 | 12.86995 | 13.322803 | 13.218894 | 13.771058 | 13.219872 |
hep-th/9511026 | Ashoke Sen | Ashoke Sen | U-duality and Intersecting D-branes | LaTeX file, 7 pages | Phys.Rev.D53:2874-2894,1996 | 10.1103/PhysRevD.53.2874 | MRI-PHY/27/95 | hep-th | null | Spectrum of elementary string states in type II string theory compactified on
a torus contains short multiplets which are invariant under only one quarter of
the space-time supersymmetry generators. $U$-duality transformation converts
these states into bound states of Dirichlet branes which wrap around
intersecting c... | [
{
"created": "Sat, 4 Nov 1995 15:32:47 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Sen",
"Ashoke",
""
]
] | Spectrum of elementary string states in type II string theory compactified on a torus contains short multiplets which are invariant under only one quarter of the space-time supersymmetry generators. $U$-duality transformation converts these states into bound states of Dirichlet branes which wrap around intersecting cyc... | 8.328658 | 6.291317 | 8.36722 | 6.392444 | 7.30767 | 6.070464 | 6.581537 | 5.824617 | 6.289688 | 10.937366 | 6.574827 | 6.793849 | 7.375499 | 6.874967 | 7.348549 | 6.716934 | 6.829923 | 6.835923 | 7.023518 | 7.75507 | 7.355395 |
2007.07892 | Ben Heidenreich | Ben Heidenreich and Tom Rudelius | Infinite Distance and Zero Gauge Coupling in 5d Supergravity | 6 pages | null | 10.1103/PhysRevD.104.106016 | ACFI-T20-08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note, we prove that for all five-dimensional supergravities arising
from M-theory compactified on a Calabi-Yau threefold, points of vanishing gauge
coupling lie at infinite distance in the moduli space. Conversely, any point at
infinite distance in the vector multiplet moduli space is a point of vanishing
gau... | [
{
"created": "Wed, 15 Jul 2020 18:00:00 GMT",
"version": "v1"
}
] | 2021-12-08 | [
[
"Heidenreich",
"Ben",
""
],
[
"Rudelius",
"Tom",
""
]
] | In this note, we prove that for all five-dimensional supergravities arising from M-theory compactified on a Calabi-Yau threefold, points of vanishing gauge coupling lie at infinite distance in the moduli space. Conversely, any point at infinite distance in the vector multiplet moduli space is a point of vanishing gauge... | 6.321338 | 4.794323 | 7.117146 | 4.994767 | 5.317989 | 4.949538 | 5.272137 | 4.771407 | 4.891201 | 8.31612 | 5.130314 | 5.341603 | 6.008812 | 5.733722 | 5.479604 | 5.603059 | 5.601104 | 5.688123 | 5.624788 | 6.007904 | 5.728572 |
1005.3848 | Gonzalo A. Palma | Ana Ach\'ucarro, Jinn-Ouk Gong, Sjoerd Hardeman, Gonzalo A. Palma and
Subodh P. Patil | Mass hierarchies and non-decoupling in multi-scalar field dynamics | 16 pages, 2 figures, typeset in PRD style. v2: Minor changes
throughout to emphasize that the analysis also applies to sharp and/or
prolonged turns. References added | Phys.Rev.D84:043502,2011 | 10.1103/PhysRevD.84.043502 | CPHT-RR 039.0510,LPTENS-10/20 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study the effects of field space curvature on scalar field
perturbations around an arbitrary background field trajectory evolving in time.
Non-trivial imprints of the 'heavy' directions on the low energy dynamics arise
when the vacuum manifold of the potential does not coincide with the span of
geodes... | [
{
"created": "Thu, 20 May 2010 21:59:18 GMT",
"version": "v1"
},
{
"created": "Wed, 25 May 2011 21:11:33 GMT",
"version": "v2"
}
] | 2011-08-10 | [
[
"Achúcarro",
"Ana",
""
],
[
"Gong",
"Jinn-Ouk",
""
],
[
"Hardeman",
"Sjoerd",
""
],
[
"Palma",
"Gonzalo A.",
""
],
[
"Patil",
"Subodh P.",
""
]
] | In this work we study the effects of field space curvature on scalar field perturbations around an arbitrary background field trajectory evolving in time. Non-trivial imprints of the 'heavy' directions on the low energy dynamics arise when the vacuum manifold of the potential does not coincide with the span of geodesic... | 11.88005 | 12.626789 | 12.331568 | 11.309998 | 12.404222 | 11.834608 | 11.925534 | 12.193348 | 12.096978 | 12.723473 | 11.304935 | 11.165278 | 11.434647 | 11.084708 | 11.336761 | 11.116999 | 11.122402 | 11.262263 | 10.783172 | 11.547474 | 10.821161 |
hep-th/0012184 | Kluson Josef | J. Kluson | Matrix model and noncommutative Chern-Simons theory | 10 pages, corrected some typos and reference added, to be published
in Phys. Lett. B | Phys.Lett. B505 (2001) 243-248 | 10.1016/S0370-2693(01)00337-9 | null | hep-th | null | In this short paper we would like to present a simple topological matrix
model which has close relation with the noncommutative Chern-Simons theory.
| [
{
"created": "Wed, 20 Dec 2000 07:49:21 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Mar 2001 07:30:37 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Kluson",
"J.",
""
]
] | In this short paper we would like to present a simple topological matrix model which has close relation with the noncommutative Chern-Simons theory. | 10.18385 | 5.871359 | 8.489912 | 6.351406 | 5.734101 | 6.135636 | 6.196589 | 6.210743 | 6.589209 | 7.870278 | 6.654101 | 6.54004 | 8.590873 | 7.111316 | 6.500654 | 6.608617 | 6.368815 | 6.834181 | 6.832278 | 8.597805 | 6.807168 |
1004.0745 | Hyun Seok Yang | Jungjai Lee and Hyun Seok Yang | Quantum Gravity from Noncommutative Spacetime | 97 pages, to be published in J. Korean Phys. Soc | J. Korean Phys. Soc. 65 (2014) 1754-1798 | 10.3938/jkps.65.1754 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review a novel and authentic way to quantize gravity. This novel approach
is based on the fact that Einstein gravity can be formulated in terms of a
symplectic geometry rather than a Riemannian geometry in the context of
emergent gravity. An essential step for emergent gravity is to realize the
equivalence princip... | [
{
"created": "Tue, 6 Apr 2010 01:08:18 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Aug 2010 16:28:53 GMT",
"version": "v2"
},
{
"created": "Tue, 31 Aug 2010 07:46:46 GMT",
"version": "v3"
},
{
"created": "Tue, 25 Nov 2014 14:28:22 GMT",
"version": "v4"
}
] | 2014-12-30 | [
[
"Lee",
"Jungjai",
""
],
[
"Yang",
"Hyun Seok",
""
]
] | We review a novel and authentic way to quantize gravity. This novel approach is based on the fact that Einstein gravity can be formulated in terms of a symplectic geometry rather than a Riemannian geometry in the context of emergent gravity. An essential step for emergent gravity is to realize the equivalence principle... | 6.944469 | 7.731419 | 7.669166 | 7.34661 | 7.702798 | 7.646608 | 7.695929 | 7.671223 | 7.788441 | 8.151589 | 7.253274 | 6.96761 | 7.272371 | 7.052507 | 7.112179 | 7.113147 | 6.99773 | 7.133485 | 7.058239 | 7.181715 | 7.022304 |
1906.00467 | Christian Ferko | Chih-Kai Chang, Christian Ferko, Savdeep Sethi, Alessandro Sfondrini,
Gabriele Tartaglino-Mazzucchelli | $T\bar{T}$ Flows and (2,2) Supersymmetry | 39 pages | Phys. Rev. D 101, 026008 (2020) | 10.1103/PhysRevD.101.026008 | EFI-19-5 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a solvable deformation of two-dimensional theories with $(2,2)$
supersymmetry using an irrelevant operator which is a bilinear in the
supercurrents. This supercurrent-squared operator is manifestly supersymmetric,
and equivalent to $T\bar{T}$ after using conservation laws. As illustrative
examples, we de... | [
{
"created": "Sun, 2 Jun 2019 18:38:41 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jul 2019 13:07:19 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Dec 2019 23:00:46 GMT",
"version": "v3"
}
] | 2020-01-15 | [
[
"Chang",
"Chih-Kai",
""
],
[
"Ferko",
"Christian",
""
],
[
"Sethi",
"Savdeep",
""
],
[
"Sfondrini",
"Alessandro",
""
],
[
"Tartaglino-Mazzucchelli",
"Gabriele",
""
]
] | We construct a solvable deformation of two-dimensional theories with $(2,2)$ supersymmetry using an irrelevant operator which is a bilinear in the supercurrents. This supercurrent-squared operator is manifestly supersymmetric, and equivalent to $T\bar{T}$ after using conservation laws. As illustrative examples, we defo... | 9.092111 | 9.065749 | 10.695355 | 8.696919 | 9.387029 | 9.392384 | 9.243676 | 8.673214 | 8.685374 | 11.721571 | 8.603022 | 8.868062 | 10.083476 | 8.702514 | 8.523459 | 8.944522 | 8.659606 | 8.83162 | 8.573241 | 9.592935 | 8.486215 |
2112.14089 | Vinay Malvimat | Vinay Malvimat, Rohan R. Poojary | Fast Scrambling due to Rotating Shockwaves in BTZ | 28 pages, 1 figure | null | 10.1103/PhysRevD.105.126019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the perturbation due to rotating shockwaves in BTZ geometries at
late times and analyse the change in Mutual Information between the two
subsystems belonging to the dual CFT$_L$ and CFT$_R$. We find that the
scrambling of Mutual Information is in general governed by the Lyapunov index
$\lambda_L$ which is bo... | [
{
"created": "Tue, 28 Dec 2021 11:00:26 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Mar 2022 11:47:52 GMT",
"version": "v2"
},
{
"created": "Sun, 3 Jul 2022 14:59:06 GMT",
"version": "v3"
}
] | 2022-07-13 | [
[
"Malvimat",
"Vinay",
""
],
[
"Poojary",
"Rohan R.",
""
]
] | We study the perturbation due to rotating shockwaves in BTZ geometries at late times and analyse the change in Mutual Information between the two subsystems belonging to the dual CFT$_L$ and CFT$_R$. We find that the scrambling of Mutual Information is in general governed by the Lyapunov index $\lambda_L$ which is boun... | 7.046306 | 6.757659 | 7.703642 | 6.148564 | 5.981718 | 5.933771 | 6.061774 | 5.983679 | 6.020528 | 8.088655 | 6.017807 | 6.335217 | 6.953821 | 6.613358 | 6.348768 | 6.433081 | 6.358611 | 6.746067 | 6.587775 | 6.984371 | 6.523938 |
1508.03367 | Stefano Kovacs | Stefano Kovacs, Yuki Sato and Hidehiko Shimada | On membrane interactions and a three-dimensional analog of Riemann
surfaces | 64 pages, 17 figures. V2: An appendix, a figure and references added;
various minor changes and improvements | null | 10.1007/JHEP02(2016)050 | DIAS-STP-15-05, WITS-MITP-018, OIQP-15-4 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Membranes in M-theory are expected to interact via splitting and joining
processes. We study these effects in the pp-wave matrix model, in which they
are associated with transitions between states in sectors built on vacua with
different numbers of membranes. Transition amplitudes between such states
receive contribu... | [
{
"created": "Thu, 13 Aug 2015 21:43:39 GMT",
"version": "v1"
},
{
"created": "Fri, 30 Oct 2015 21:47:47 GMT",
"version": "v2"
}
] | 2016-03-23 | [
[
"Kovacs",
"Stefano",
""
],
[
"Sato",
"Yuki",
""
],
[
"Shimada",
"Hidehiko",
""
]
] | Membranes in M-theory are expected to interact via splitting and joining processes. We study these effects in the pp-wave matrix model, in which they are associated with transitions between states in sectors built on vacua with different numbers of membranes. Transition amplitudes between such states receive contributi... | 8.695406 | 8.846395 | 9.597341 | 8.381612 | 9.214995 | 8.556538 | 9.103337 | 8.62009 | 8.407002 | 9.587609 | 8.256248 | 8.030358 | 8.498412 | 7.948713 | 8.179086 | 8.455657 | 8.16748 | 8.154685 | 8.016124 | 8.480614 | 8.149384 |
0812.3337 | Davide Campagnari | H. Reinhardt, G . Burgio, D. Campagnari, D. Epple, M. Leder, M. Pak,
M. Quandt and W. Schleifenbaum | Recent results from the Hamiltonian approach to Yang-Mills theory in
Coulomb gauge | 5 pages, 7 figures, Talk presented at the 8th Conference Quark
Confinement and the Hadron Spectrum, September 1-6, 2008, Mainz, Germany | PoS Confinement8:061,2008 | null | UNITU-THEP-02-2008 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Within the Hamiltonian approach to Yang-Mills theory in Coulomb gauge the
ghost and gluon propagators are determined from a variational solution of the
Yang-Mills Schroedinger equation showing both gluon and heavy quark
confinement. The continuum results are in good agreement with lattice data. The
ghost form factor ... | [
{
"created": "Wed, 17 Dec 2008 16:41:03 GMT",
"version": "v1"
}
] | 2009-06-25 | [
[
"Reinhardt",
"H.",
""
],
[
"Burgio",
"G .",
""
],
[
"Campagnari",
"D.",
""
],
[
"Epple",
"D.",
""
],
[
"Leder",
"M.",
""
],
[
"Pak",
"M.",
""
],
[
"Quandt",
"M.",
""
],
[
"Schleifenbaum",
"W.",
... | Within the Hamiltonian approach to Yang-Mills theory in Coulomb gauge the ghost and gluon propagators are determined from a variational solution of the Yang-Mills Schroedinger equation showing both gluon and heavy quark confinement. The continuum results are in good agreement with lattice data. The ghost form factor is... | 7.618707 | 6.202505 | 7.208601 | 6.29304 | 7.546142 | 6.39045 | 6.402692 | 6.814933 | 6.484519 | 7.664242 | 6.4763 | 6.774434 | 7.046244 | 6.65479 | 7.228382 | 6.915307 | 6.807635 | 6.948576 | 6.617022 | 6.930548 | 6.751007 |
1504.07710 | Tomoki Nosaka | Sanefumi Moriyama and Tomoki Nosaka | Superconformal Chern-Simons Partition Functions of Affine D-type Quiver
from Fermi Gas | 23 pages, 4 figures; v2: section 4.2 added, one figure added | null | 10.1007/JHEP09(2015)054 | OCU-PHYS 425, YITP-15-18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the partition function of the superconformal Chern-Simons
theories with the quiver diagram being the affine D-type Dynkin diagram.
Rewriting the partition function into that of a Fermi gas system, we show that
the perturbative expansions in 1/N are summed up to an Airy function, as in the
ABJM theory or m... | [
{
"created": "Wed, 29 Apr 2015 02:56:59 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jun 2015 03:55:28 GMT",
"version": "v2"
}
] | 2015-10-28 | [
[
"Moriyama",
"Sanefumi",
""
],
[
"Nosaka",
"Tomoki",
""
]
] | We consider the partition function of the superconformal Chern-Simons theories with the quiver diagram being the affine D-type Dynkin diagram. Rewriting the partition function into that of a Fermi gas system, we show that the perturbative expansions in 1/N are summed up to an Airy function, as in the ABJM theory or mor... | 9.121778 | 8.022975 | 11.72627 | 7.994862 | 8.911337 | 7.706942 | 7.876882 | 8.098021 | 7.746776 | 11.503942 | 8.048223 | 8.724637 | 10.008212 | 8.686057 | 9.193017 | 9.097596 | 8.807653 | 9.054107 | 8.747763 | 9.814175 | 8.933183 |
hep-th/9805014 | Edward Teo | Edward Teo | Black hole absorption cross-sections and the anti-de Sitter -- conformal
field theory correspondence | 10 pages, harvmac | Phys.Lett. B436 (1998) 269-274 | 10.1016/S0370-2693(98)00849-1 | DAMTP R98/21 | hep-th | null | Recent work has uncovered a correspondence between theories in anti-de Sitter
space, and those on its boundary. This has important implications for black
holes in string theory which have near-horizon AdS geometries. Using the
effective coupling to the boundary conformal field theory, I compute the
low-energy, s-wave... | [
{
"created": "Mon, 4 May 1998 15:23:22 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Teo",
"Edward",
""
]
] | Recent work has uncovered a correspondence between theories in anti-de Sitter space, and those on its boundary. This has important implications for black holes in string theory which have near-horizon AdS geometries. Using the effective coupling to the boundary conformal field theory, I compute the low-energy, s-wave a... | 9.225348 | 7.942757 | 9.246327 | 7.908196 | 7.72651 | 7.672942 | 7.672826 | 7.458424 | 7.731624 | 9.918569 | 8.09468 | 7.754365 | 8.629477 | 7.986603 | 8.232841 | 7.627335 | 7.877465 | 7.6681 | 7.938217 | 8.492707 | 7.942497 |
1310.3122 | Richard Szabo | Georgios Giasemidis, Richard J. Szabo and Miguel Tierz | Supersymmetric gauge theories, Coulomb gases and Chern-Simons matrix
models | 17 pages; v2: reference added | Phys. Rev. D 89, 025016 (2014) | 10.1103/PhysRevD.89.025016 | EMPG-13-16 | hep-th cond-mat.stat-mech cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop Coulomb gas pictures of strong and weak coupling regimes of
supersymmetric Yang-Mills theory in five and four dimensions. By relating them
to the matrix models that arise in Chern-Simons theory, we compute their free
energies in the large N limit and establish relationships between the
respective gauge the... | [
{
"created": "Fri, 11 Oct 2013 13:43:31 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Oct 2013 01:04:21 GMT",
"version": "v2"
}
] | 2014-02-05 | [
[
"Giasemidis",
"Georgios",
""
],
[
"Szabo",
"Richard J.",
""
],
[
"Tierz",
"Miguel",
""
]
] | We develop Coulomb gas pictures of strong and weak coupling regimes of supersymmetric Yang-Mills theory in five and four dimensions. By relating them to the matrix models that arise in Chern-Simons theory, we compute their free energies in the large N limit and establish relationships between the respective gauge theor... | 7.747984 | 7.74039 | 8.158702 | 7.049213 | 7.637944 | 7.654848 | 7.264601 | 7.215458 | 7.028343 | 8.861588 | 7.356435 | 7.762498 | 7.816598 | 7.515604 | 7.687294 | 7.782119 | 7.829481 | 7.258779 | 7.230014 | 7.435513 | 7.213435 |
hep-th/0312030 | M. Hossein Dehghani | M. H. Dehghani | Magnetic Branes in Gauss-Bonnet Gravity | 17 pages, No figure, The version to be published in Phys. Rev. D | Phys.Rev. D69 (2004) 064024 | 10.1103/PhysRevD.69.064024 | null | hep-th | null | We present two new classes of magnetic brane solutions in
Einstein-Maxwell-Gauss-Bonnet gravity with a negative cosmological constant.
The first class of solutions yields an $(n+1)$-dimensional spacetime with a
longitudinal magnetic field generated by a static magnetic brane. We also
generalize this solution to the c... | [
{
"created": "Tue, 2 Dec 2003 15:13:41 GMT",
"version": "v1"
},
{
"created": "Sun, 7 Mar 2004 07:15:38 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dehghani",
"M. H.",
""
]
] | We present two new classes of magnetic brane solutions in Einstein-Maxwell-Gauss-Bonnet gravity with a negative cosmological constant. The first class of solutions yields an $(n+1)$-dimensional spacetime with a longitudinal magnetic field generated by a static magnetic brane. We also generalize this solution to the cas... | 4.363445 | 3.146263 | 4.374615 | 3.720497 | 3.804347 | 3.822154 | 3.794716 | 3.451396 | 3.658668 | 4.78919 | 3.625584 | 3.921776 | 4.395528 | 4.157304 | 4.197665 | 4.114747 | 4.20351 | 4.022984 | 4.130501 | 4.368964 | 4.087472 |
hep-th/0404148 | A. Joel Saavedra | Sergio del Campo, Ramon Herrera and Joel Saavedra | Open inflationary universes in a brane world cosmology | 8 pages, 4 Figures, accepted in Physical Review D | Phys.Rev. D70 (2004) 023507 | 10.1103/PhysRevD.70.023507 | GACG-04/07 | hep-th | null | In this paper, we study a type of one-field model for open inflationary
universe models in the context of the brane world models. In the scenario of a
one-bubble universe model, we determine and characterize the existence of the
Coleman-De Lucia instanton, together with the period of inflation after
tunneling has occ... | [
{
"created": "Tue, 20 Apr 2004 14:55:42 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"del Campo",
"Sergio",
""
],
[
"Herrera",
"Ramon",
""
],
[
"Saavedra",
"Joel",
""
]
] | In this paper, we study a type of one-field model for open inflationary universe models in the context of the brane world models. In the scenario of a one-bubble universe model, we determine and characterize the existence of the Coleman-De Lucia instanton, together with the period of inflation after tunneling has occur... | 15.941453 | 14.924475 | 9.880141 | 11.088524 | 11.760489 | 10.835309 | 15.473624 | 12.376224 | 14.470398 | 15.541025 | 15.415813 | 14.598597 | 12.99002 | 12.630461 | 13.204908 | 13.289558 | 14.853879 | 13.485746 | 14.394152 | 14.877036 | 13.860723 |
2302.06469 | Pulkit Agarwal | Pulkit Agarwal, Richard C. Brower, Timothy G. Raben, and Chung-I Tan | Embedding Space Approach to Lorentzian CFT Amplitudes and Causal
Spherical Functions | 65 pages, 8 figures; Note added at the end of Introduction, updated
references, corrected typos, added appendix B5 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Conformal Field Theory in a Minkowski setting is discussed in an embedding
space approach, paying special attention to causality constraints for
four-point amplitudes. The physics of dilatation and Lorentz boost is
emphasized in specifying the non-compact Maximal Abelian subgroup (MASG) of
$SO(d,2)$. Reduction of a C... | [
{
"created": "Mon, 13 Feb 2023 15:45:29 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Mar 2023 05:47:29 GMT",
"version": "v2"
}
] | 2023-03-20 | [
[
"Agarwal",
"Pulkit",
""
],
[
"Brower",
"Richard C.",
""
],
[
"Raben",
"Timothy G.",
""
],
[
"Tan",
"Chung-I",
""
]
] | Conformal Field Theory in a Minkowski setting is discussed in an embedding space approach, paying special attention to causality constraints for four-point amplitudes. The physics of dilatation and Lorentz boost is emphasized in specifying the non-compact Maximal Abelian subgroup (MASG) of $SO(d,2)$. Reduction of a Con... | 12.875997 | 13.57626 | 12.482552 | 12.500691 | 12.084918 | 12.275754 | 13.540797 | 13.125903 | 11.885908 | 14.183433 | 11.853355 | 11.290804 | 11.811834 | 11.481859 | 11.562739 | 11.380699 | 11.847278 | 10.921543 | 11.375792 | 12.297112 | 11.681411 |
0708.1701 | Sven Faller | Sven Faller | Effective Field Theory of Gravity: Leading Quantum Gravitational
Corrections to Newtons and Coulombs Law | 14 pages, 12 figures | Phys.Rev.D77:124039,2008 | 10.1103/PhysRevD.77.124039 | SI-HEP-2007-13 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we consider general relativity and its combination with scalar
quantum electrodynamics (QED) as an effective quantum field theory at energies
well below the Planck scale. This enables us to compute the one-loop quantum
corrections to the Newton and Coulomb potential induced by the combination of
gravito... | [
{
"created": "Mon, 13 Aug 2007 12:22:01 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Oct 2007 09:35:52 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Jun 2008 07:40:37 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Faller",
"Sven",
""
]
] | In this paper we consider general relativity and its combination with scalar quantum electrodynamics (QED) as an effective quantum field theory at energies well below the Planck scale. This enables us to compute the one-loop quantum corrections to the Newton and Coulomb potential induced by the combination of graviton ... | 6.198653 | 6.915417 | 6.322076 | 5.666757 | 6.061129 | 6.665298 | 7.004431 | 5.991609 | 5.89654 | 7.075611 | 6.253284 | 5.965102 | 6.061913 | 5.85304 | 6.03573 | 5.853364 | 6.158799 | 5.770236 | 6.003031 | 6.103973 | 6.130388 |
1505.03850 | Thomas T. Dumitrescu | Clay Cordova, Thomas T. Dumitrescu, Xi Yin | Higher Derivative Terms, Toroidal Compactification, and Weyl Anomalies
in Six-Dimensional (2,0) Theories | 48 pages + appendix, 3 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We systematically analyze the effective action on the moduli space of (2,0)
superconformal field theories in six dimensions, as well as their toroidal
compactification to maximally supersymmetric Yang-Mills theories in five and
four dimensions. We present a streamlined approach to non-renormalization
theorems that co... | [
{
"created": "Thu, 14 May 2015 19:44:16 GMT",
"version": "v1"
}
] | 2015-05-15 | [
[
"Cordova",
"Clay",
""
],
[
"Dumitrescu",
"Thomas T.",
""
],
[
"Yin",
"Xi",
""
]
] | We systematically analyze the effective action on the moduli space of (2,0) superconformal field theories in six dimensions, as well as their toroidal compactification to maximally supersymmetric Yang-Mills theories in five and four dimensions. We present a streamlined approach to non-renormalization theorems that cons... | 6.337353 | 5.860641 | 7.079051 | 5.659161 | 5.407154 | 5.567427 | 5.634815 | 5.775373 | 5.655534 | 7.333299 | 5.77138 | 5.946036 | 6.198837 | 5.769867 | 5.915979 | 5.795766 | 5.87375 | 5.980973 | 5.784565 | 6.282838 | 5.802293 |
hep-th/0605265 | Ishwaree Neupane | Ishwaree P Neupane | Towards Inflation and Accelerating Cosmologies in String-Generated
Gravity Models | 8 pages, 3 figures; Based on a Talk given at the XL Rencontre de
Moriond | null | null | null | hep-th astro-ph gr-qc | null | The string $\alpha^\prime$-correction to the usual Einstein action comprises
a Gauss-Bonnet integrand multiplied by non-trivial functions of the modulus
field $\chi$ and/or the dilaton field $\phi$. We discuss how the presence of
such terms in the four dimensional effective action can explain several novel
phenomena,... | [
{
"created": "Mon, 29 May 2006 08:06:13 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Neupane",
"Ishwaree P",
""
]
] | The string $\alpha^\prime$-correction to the usual Einstein action comprises a Gauss-Bonnet integrand multiplied by non-trivial functions of the modulus field $\chi$ and/or the dilaton field $\phi$. We discuss how the presence of such terms in the four dimensional effective action can explain several novel phenomena, s... | 10.491407 | 9.724504 | 9.850278 | 9.436686 | 9.347897 | 9.654681 | 9.612722 | 9.799197 | 9.533642 | 10.533022 | 9.568393 | 9.390823 | 9.020839 | 9.00405 | 9.140139 | 9.326443 | 9.180453 | 8.965167 | 8.964099 | 9.587868 | 9.114259 |
1211.4512 | Changrim Ahn | Changrim Ahn, Diego Bombardelli | Exact S-matrices for AdS_3/CFT_2 | 14 pages, 4 figures | null | 10.1142/S0217751X13501686 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose exact $S$-matrices for the AdS_3/CFT_2 duality between Type IIB
strings on AdS_3 x S^3 x M_4 with M_4=S^3 x S^1 or T^4 and the corresponding
two-dimensional conformal field theories. We fix the complete two-particle
S-matrices for both those cases of AdS_3/CFT_2, on the basis of the symmetries
su(1|1) and ... | [
{
"created": "Mon, 19 Nov 2012 17:28:56 GMT",
"version": "v1"
}
] | 2015-06-12 | [
[
"Ahn",
"Changrim",
""
],
[
"Bombardelli",
"Diego",
""
]
] | We propose exact $S$-matrices for the AdS_3/CFT_2 duality between Type IIB strings on AdS_3 x S^3 x M_4 with M_4=S^3 x S^1 or T^4 and the corresponding two-dimensional conformal field theories. We fix the complete two-particle S-matrices for both those cases of AdS_3/CFT_2, on the basis of the symmetries su(1|1) and su... | 6.477843 | 5.968403 | 7.814116 | 5.761755 | 5.760172 | 5.958963 | 5.864171 | 5.304264 | 6.109084 | 8.495389 | 5.8003 | 6.183633 | 6.73441 | 5.753627 | 5.68624 | 5.631916 | 5.737631 | 5.73245 | 5.721721 | 6.756088 | 5.858356 |
hep-th/0504168 | Jerome Martin | Philippe Brax and Jerome Martin | Shift Symmetry and Inflation in Supergravity | 29 pages, 13 figures | Phys.Rev. D72 (2005) 023518 | 10.1103/PhysRevD.72.023518 | null | hep-th astro-ph gr-qc hep-ph | null | We consider models of inflation in supergravity with a shift symmetry. We
focus on models with one moduli and one inflaton field. The presence of this
symmetry guarantees the existence of a flat direction for the inflaton field.
Mildly breaking the shift symmetry using a superpotential which depends not
only on the m... | [
{
"created": "Wed, 20 Apr 2005 12:53:43 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Brax",
"Philippe",
""
],
[
"Martin",
"Jerome",
""
]
] | We consider models of inflation in supergravity with a shift symmetry. We focus on models with one moduli and one inflaton field. The presence of this symmetry guarantees the existence of a flat direction for the inflaton field. Mildly breaking the shift symmetry using a superpotential which depends not only on the mod... | 7.716696 | 8.831078 | 8.057737 | 7.797556 | 7.939451 | 8.389327 | 7.7771 | 7.828275 | 7.856993 | 8.679096 | 7.67319 | 7.64793 | 7.551255 | 7.46664 | 7.246678 | 7.319068 | 7.293797 | 7.547594 | 7.309874 | 7.447114 | 7.326374 |
hep-th/9704177 | Christophe Grojean | E. Dudas and C. Grojean | Four-dimensional M-theory and supersymmetry breaking | 23 pages, LaTex, 1 figure | Nucl.Phys.B507:553-570,1997 | 10.1016/S0550-3213(97)00590-7 | CERN-TH/97-79, LPTHE_ORSAY 97/17, Saclay T97/038 | hep-th hep-ph | null | We investigate compactifications of M-theory from $11\to 5\to 4$ dimensions
and discuss geometrical properties of 4-d moduli fields related to the
structure of 5-d theory. We study supersymmetry breaking by compactification of
the fifth dimension and find that an universal superpotential is generated for
the axion-di... | [
{
"created": "Thu, 24 Apr 1997 21:32:37 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Dudas",
"E.",
""
],
[
"Grojean",
"C.",
""
]
] | We investigate compactifications of M-theory from $11\to 5\to 4$ dimensions and discuss geometrical properties of 4-d moduli fields related to the structure of 5-d theory. We study supersymmetry breaking by compactification of the fifth dimension and find that an universal superpotential is generated for the axion-dila... | 8.159721 | 7.214869 | 8.093064 | 7.38555 | 8.113386 | 7.523399 | 8.34127 | 8.012656 | 7.284939 | 8.75478 | 7.533414 | 7.577331 | 7.697041 | 7.51979 | 7.97522 | 7.635688 | 7.785437 | 7.780874 | 7.717824 | 7.931393 | 7.453681 |
hep-th/0104156 | Dieter Luest H. | Gabriel Lopes Cardoso, Gianguido Dall'Agata, Dieter Lust | Curved BPS domain wall solutions in five-dimensional gauged supergravity | 13 pages, latex, error corrected plus substantial revision (title
changed) | JHEP 0107:026,2001 | 10.1088/1126-6708/2001/07/026 | HU-EP-01/17 | hep-th | null | We analyze the possibility of constructing supersymmetric curved domain wall
solutions in five-dimensional ${\cal N}=2$ gauged supergravity, which are
supported by non-constant scalar fields belonging either to vector multiplets
only or to vector and hypermultiplets. We show that the BPS equations for the
warp factor... | [
{
"created": "Wed, 18 Apr 2001 14:50:29 GMT",
"version": "v1"
},
{
"created": "Fri, 18 May 2001 14:03:23 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Cardoso",
"Gabriel Lopes",
""
],
[
"Dall'Agata",
"Gianguido",
""
],
[
"Lust",
"Dieter",
""
]
] | We analyze the possibility of constructing supersymmetric curved domain wall solutions in five-dimensional ${\cal N}=2$ gauged supergravity, which are supported by non-constant scalar fields belonging either to vector multiplets only or to vector and hypermultiplets. We show that the BPS equations for the warp factor a... | 6.375842 | 6.26964 | 7.30359 | 5.974713 | 6.401832 | 6.116026 | 5.890121 | 5.79437 | 6.126721 | 8.187589 | 6.016803 | 6.047108 | 6.486197 | 6.156499 | 6.335291 | 6.369683 | 5.996945 | 5.887084 | 6.061131 | 6.905052 | 6.172774 |
hep-th/9310148 | Robert Coquereaux | R. Coquereaux, R. Haussling, F. Scheck | Algebraic connections on parallel universes | 10 pages, CPT-93/PE 2947 | Int.J.Mod.Phys. A10 (1995) 89-98 | 10.1142/S0217751X95000048 | null | hep-th | null | For any manifold $M$, we introduce a $\ZZ $-graded differential algebra
$\Xi$, which, in particular, is a bi-module over the associative algebra
$C(M\cup M)$. We then introduce the corresponding covariant differentials and
show how this construction can be interpreted in terms of Yang-Mills and Higgs
fields. This is ... | [
{
"created": "Fri, 22 Oct 1993 08:15:35 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Coquereaux",
"R.",
""
],
[
"Haussling",
"R.",
""
],
[
"Scheck",
"F.",
""
]
] | For any manifold $M$, we introduce a $\ZZ $-graded differential algebra $\Xi$, which, in particular, is a bi-module over the associative algebra $C(M\cup M)$. We then introduce the corresponding covariant differentials and show how this construction can be interpreted in terms of Yang-Mills and Higgs fields. This is a ... | 11.699818 | 10.936477 | 11.929106 | 10.174177 | 10.362168 | 11.820426 | 10.801072 | 10.360666 | 10.160367 | 14.563093 | 10.269789 | 9.883616 | 10.363781 | 10.389196 | 9.871926 | 10.067221 | 10.256455 | 10.480033 | 10.404766 | 10.940303 | 10.171094 |
1711.09104 | Oliver Schlotterer | Carlos R. Mafra and Oliver Schlotterer | Double-Copy Structure of One-Loop Open-String Amplitudes | 5 pages, v2: modifications in the structure to match published
version | Phys. Rev. Lett. 121, 011601 (2018) | 10.1103/PhysRevLett.121.011601 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this Letter, we provide evidence for a new double-copy structure in
one-loop amplitudes of the open superstring. Their integrands with respect to
the moduli space of genus-one surfaces are cast into a form where
gauge-invariant kinematic factors and certain functions of the punctures --
so-called generalized ellip... | [
{
"created": "Fri, 24 Nov 2017 19:00:15 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Jun 2018 16:28:04 GMT",
"version": "v2"
}
] | 2018-07-11 | [
[
"Mafra",
"Carlos R.",
""
],
[
"Schlotterer",
"Oliver",
""
]
] | In this Letter, we provide evidence for a new double-copy structure in one-loop amplitudes of the open superstring. Their integrands with respect to the moduli space of genus-one surfaces are cast into a form where gauge-invariant kinematic factors and certain functions of the punctures -- so-called generalized ellipti... | 13.102709 | 11.661575 | 13.212079 | 11.71167 | 12.094357 | 14.047067 | 12.009844 | 11.406754 | 11.217726 | 14.491845 | 10.601167 | 11.920279 | 12.279384 | 11.905466 | 12.160623 | 11.444956 | 11.752772 | 11.961775 | 11.997748 | 12.196354 | 11.802949 |
1105.3577 | Matteo Beccaria | Matteo Beccaria, Guido Macorini, CarloAlberto Ratti | Wrapping corrections, reciprocity and BFKL beyond the sl(2) subsector in
N=4 SYM | 18 pages | JHEP 1106:071,2011 | 10.1007/JHEP06(2011)071 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider N=4 SYM and a class of spin N, length-3, twist operators beyond
the well studied sl(2) subsector. They can be identified at one-loop with three
gluon operators. At strong coupling, they are associated with spinning strings
with two spins in AdS5. We exploit the Y-system to compute the leading
weak-couplin... | [
{
"created": "Wed, 18 May 2011 09:59:24 GMT",
"version": "v1"
}
] | 2011-06-20 | [
[
"Beccaria",
"Matteo",
""
],
[
"Macorini",
"Guido",
""
],
[
"Ratti",
"CarloAlberto",
""
]
] | We consider N=4 SYM and a class of spin N, length-3, twist operators beyond the well studied sl(2) subsector. They can be identified at one-loop with three gluon operators. At strong coupling, they are associated with spinning strings with two spins in AdS5. We exploit the Y-system to compute the leading weak-coupling ... | 14.145081 | 8.737988 | 15.702694 | 11.218874 | 14.314476 | 13.433744 | 12.134067 | 9.941819 | 11.316031 | 17.418224 | 11.137175 | 12.233254 | 14.483379 | 12.53072 | 13.141443 | 13.230705 | 13.384332 | 12.907948 | 12.740194 | 14.321605 | 13.21172 |
hep-th/9506001 | Keith Dienes | Keith R. Dienes (IAS, Princeton), Moshe Moshe (Technion), Robert C.
Myers (McGill) | SUPERTRACES IN STRING THEORY | 6 pages, LaTeX, one encapsulated figure | null | null | IASSNS-HEP-95/42; McGill/95-28 (June 1995) | hep-th | null | We demonstrate that the spectrum of any consistent string theory in $D$
dimensions must satisfy a number of supertrace constraints: $ Str~M^{2n}=0 $
for $0 \leq n < D/2-1$, integer $n$. These results hold for a large class of
string theories, including critical heterotic strings. For strings lacking
spacetime supersy... | [
{
"created": "Thu, 1 Jun 1995 06:14:38 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dienes",
"Keith R.",
"",
"IAS, Princeton"
],
[
"Moshe",
"Moshe",
"",
"Technion"
],
[
"Myers",
"Robert C.",
"",
"McGill"
]
] | We demonstrate that the spectrum of any consistent string theory in $D$ dimensions must satisfy a number of supertrace constraints: $ Str~M^{2n}=0 $ for $0 \leq n < D/2-1$, integer $n$. These results hold for a large class of string theories, including critical heterotic strings. For strings lacking spacetime supersymm... | 10.14514 | 8.694228 | 9.059304 | 8.074947 | 9.274178 | 8.458483 | 8.692447 | 9.201751 | 9.051014 | 10.867278 | 8.534509 | 8.952994 | 9.316413 | 8.866451 | 8.757366 | 9.161177 | 8.819709 | 8.88306 | 8.443891 | 9.156015 | 8.718211 |
1310.0206 | S. Prem Kumar | Anton F. Faedo, Benjo Fraser, and S. Prem Kumar | Supersymmetric Lifshitz-like backgrounds from N=4 SYM with heavy quark
density | 24 pages, 2 figures, references added, version published in JHEP,
Feb. 2014 | JHEP 1402 (2014) 066 | 10.1007/JHEP02(2014)066 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine a class of gravity backgrounds obtained by considering the
backreaction of a spatially uniform density of mutually BPS Wilson lines or
heavy quarks in N=4 SUSY Yang-Mills theory. The configurations preserve eight
supercharges and an SO(5) subgroup of the SO(6) R-symmetry. They are obtained
by considering t... | [
{
"created": "Tue, 1 Oct 2013 09:30:43 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Dec 2014 21:54:20 GMT",
"version": "v2"
}
] | 2014-12-24 | [
[
"Faedo",
"Anton F.",
""
],
[
"Fraser",
"Benjo",
""
],
[
"Kumar",
"S. Prem",
""
]
] | We examine a class of gravity backgrounds obtained by considering the backreaction of a spatially uniform density of mutually BPS Wilson lines or heavy quarks in N=4 SUSY Yang-Mills theory. The configurations preserve eight supercharges and an SO(5) subgroup of the SO(6) R-symmetry. They are obtained by considering the... | 7.266654 | 6.288559 | 8.49136 | 6.730732 | 6.694046 | 6.563231 | 6.908537 | 6.377018 | 6.581522 | 8.695945 | 6.543997 | 6.690198 | 7.545291 | 7.03058 | 6.918267 | 7.051735 | 6.852269 | 6.82818 | 7.112545 | 7.65968 | 6.809025 |
hep-th/0003050 | Adi Armoni | Carlo Angelantonj (ENS) and Adi Armoni (Ecole Polytechnique) | RG Flow, Wilson Loops and the Dilaton Tadpole | 12 pages, Latex. v2: minor changes, refs. added | Phys.Lett. B482 (2000) 329-336 | 10.1016/S0370-2693(00)00475-5 | CPHT-S004.0300, LPTENS 00/07 | hep-th hep-ph | null | We discuss the role of the dilaton tadpole in the holographic description of
non-supersymmetric gauge theories that are conformal in the planar limit. On
the string theory side, the presence of the dilaton tadpole modifies the AdS
background inducing a logarithmic running for the radius and the dilaton. Using
the hol... | [
{
"created": "Tue, 7 Mar 2000 18:25:13 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Mar 2000 12:58:11 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Angelantonj",
"Carlo",
"",
"ENS"
],
[
"Armoni",
"Adi",
"",
"Ecole Polytechnique"
]
] | We discuss the role of the dilaton tadpole in the holographic description of non-supersymmetric gauge theories that are conformal in the planar limit. On the string theory side, the presence of the dilaton tadpole modifies the AdS background inducing a logarithmic running for the radius and the dilaton. Using the holog... | 8.325515 | 7.333779 | 8.251923 | 7.195039 | 7.217003 | 7.891887 | 7.786738 | 7.558359 | 7.318942 | 9.194669 | 7.534329 | 7.918904 | 8.587787 | 8.209579 | 7.556217 | 7.508966 | 7.567661 | 7.695321 | 8.085023 | 8.893949 | 7.737701 |
2102.06097 | Jung Hun Lee | Chanyong Park, Jung Hun Lee | Quantum correlation in quark-gluon medium | 18 pages, 2 figures, reference added, minor changes | null | 10.1007/s40042-022-00669-7 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study thermodynamics and quantum correlations of the string cloud geometry
whose field theory dual is the quark-gluon medium. We found the novel
universality of the entanglement entropy first law in the high quark density
limit. We also showed that a correlation function generally decreases as the
entanglement ent... | [
{
"created": "Thu, 11 Feb 2021 16:22:22 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Aug 2022 06:26:58 GMT",
"version": "v2"
}
] | 2022-12-14 | [
[
"Park",
"Chanyong",
""
],
[
"Lee",
"Jung Hun",
""
]
] | We study thermodynamics and quantum correlations of the string cloud geometry whose field theory dual is the quark-gluon medium. We found the novel universality of the entanglement entropy first law in the high quark density limit. We also showed that a correlation function generally decreases as the entanglement entro... | 14.144735 | 12.488797 | 14.874249 | 12.8633 | 12.902231 | 13.933002 | 13.890032 | 12.771873 | 13.03489 | 17.329428 | 13.235962 | 13.423089 | 14.001895 | 13.470329 | 12.836919 | 13.617475 | 13.375677 | 13.070478 | 13.224042 | 13.932346 | 13.107262 |
hep-th/9807187 | Klaus Behrndt | K. Behrndt, A.H. Chamseddine and W.A. Sabra | BPS black holes in N=2 five dimensional AdS supergravity | 8 pages, 1 figure, LaTeX, corrected the potential | Phys.Lett. B442 (1998) 97-101 | 10.1016/S0370-2693(98)01208-8 | null | hep-th gr-qc | null | BPS black hole solutions of U(1) gauged five-dimensional supergravity are
obtained by solving the Killing spinor equations. These extremal static black
holes live in an asymptotic AdS_5 space time. Unlike black holes in asymptotic
flat space time none of them possess a regular horizon. We also calculate the
influence... | [
{
"created": "Fri, 24 Jul 1998 15:16:34 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Aug 1998 14:26:14 GMT",
"version": "v2"
},
{
"created": "Tue, 18 Aug 1998 15:51:41 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Behrndt",
"K.",
""
],
[
"Chamseddine",
"A. H.",
""
],
[
"Sabra",
"W. A.",
""
]
] | BPS black hole solutions of U(1) gauged five-dimensional supergravity are obtained by solving the Killing spinor equations. These extremal static black holes live in an asymptotic AdS_5 space time. Unlike black holes in asymptotic flat space time none of them possess a regular horizon. We also calculate the influence, ... | 11.473179 | 8.833438 | 11.090919 | 8.965877 | 8.679164 | 9.211014 | 8.466307 | 9.642612 | 8.699769 | 12.805958 | 8.838816 | 9.369328 | 9.394348 | 9.230791 | 8.789113 | 9.333127 | 9.106567 | 9.149731 | 9.337235 | 10.381832 | 9.042971 |
1601.04758 | Stefano Bolognesi | Stefano Bolognesi, Eliezer Rabinovici, Gianni Tallarita | String pair production in non homogeneous backgrounds | 36 pages; v3: added comments on perturbative vs. non-perturbative
behaviour | null | 10.1007/JHEP04(2016)174 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider string pair production in non homogeneous electric backgrounds.
We study several particular configurations which can be addressed with the
Euclidean world-sheet instanton technique, the analogue of the world-line
instanton for particles. In the first case the string is suspended between two
D-branes in fl... | [
{
"created": "Mon, 18 Jan 2016 23:39:14 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Jan 2016 16:04:00 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Mar 2016 18:54:16 GMT",
"version": "v3"
}
] | 2016-05-25 | [
[
"Bolognesi",
"Stefano",
""
],
[
"Rabinovici",
"Eliezer",
""
],
[
"Tallarita",
"Gianni",
""
]
] | We consider string pair production in non homogeneous electric backgrounds. We study several particular configurations which can be addressed with the Euclidean world-sheet instanton technique, the analogue of the world-line instanton for particles. In the first case the string is suspended between two D-branes in flat... | 8.443405 | 9.432255 | 9.330253 | 8.760711 | 9.072426 | 9.175791 | 9.079262 | 8.432702 | 8.270052 | 9.897285 | 8.579371 | 8.191492 | 8.336274 | 8.205668 | 8.215756 | 8.417882 | 8.310021 | 8.153626 | 8.213682 | 8.439555 | 8.085927 |
1402.4691 | Gianni Tallarita | Gianni Tallarita | Holographic Lifshitz Superconductors with an Axion Field | 19 pages, 9 figures | Phys. Rev. D 89, 106005 (2014) | 10.1103/PhysRevD.89.106005 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use a Yang-Mills field coupled to an axion as probes of a black hole with
arbitrary Lifshitz scaling to investigate, via holography, superconducting
phase transitions of the dual theory with a $p_x+ip_y$ condensate. In the
relativistic case with no axion, this phase is known to be unstable, the stable
phase corres... | [
{
"created": "Wed, 19 Feb 2014 15:18:06 GMT",
"version": "v1"
}
] | 2014-05-21 | [
[
"Tallarita",
"Gianni",
""
]
] | We use a Yang-Mills field coupled to an axion as probes of a black hole with arbitrary Lifshitz scaling to investigate, via holography, superconducting phase transitions of the dual theory with a $p_x+ip_y$ condensate. In the relativistic case with no axion, this phase is known to be unstable, the stable phase correspo... | 11.717271 | 11.919513 | 13.384609 | 10.820145 | 12.099191 | 12.457521 | 11.879015 | 11.746928 | 10.804876 | 14.45839 | 10.757126 | 11.610452 | 12.018106 | 11.170253 | 10.983365 | 10.423219 | 10.963278 | 11.251618 | 10.960057 | 11.44747 | 10.67178 |
hep-th/0610280 | J. M. Drummond | J.M.Drummond, L.Gallot, E.Sokatchev | Superconformal Invariants or How to Relate Four-point AdS Amplitudes | 11 pages | Phys.Lett.B645:95-100,2007 | 10.1016/j.physletb.2006.12.015 | LAPTH-1165/06 | hep-th | null | Using the form of N=2 superconformal invariants we derive the explicit
relation between the bottom and top components of the correlator of four
stress-tensor multiplets in N=4 Super Yang-Mills. The result is given in terms
of an eighth order differential operator acting on the function of two
variables which characte... | [
{
"created": "Thu, 26 Oct 2006 15:30:10 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Drummond",
"J. M.",
""
],
[
"Gallot",
"L.",
""
],
[
"Sokatchev",
"E.",
""
]
] | Using the form of N=2 superconformal invariants we derive the explicit relation between the bottom and top components of the correlator of four stress-tensor multiplets in N=4 Super Yang-Mills. The result is given in terms of an eighth order differential operator acting on the function of two variables which characteri... | 8.298067 | 7.083166 | 8.546095 | 6.964378 | 7.663439 | 7.660701 | 7.932306 | 6.837176 | 7.406862 | 9.321954 | 7.08848 | 7.429574 | 8.483257 | 7.48213 | 7.7076 | 7.587632 | 7.706271 | 7.368126 | 7.271179 | 8.822605 | 7.465576 |
1810.11803 | K V Pavan Kumar | Rishabh Jha, Chethan Krishnan, K.V. Pavan Kumar | Massive Scattering Amplitudes in Six Dimensions | 37 pages; v2: minor improvements, JHEP version | null | 10.1007/JHEP03(2019)198 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that a natural spinor-helicity formalism that can describe massive
scattering amplitudes exists in $D=6$ dimensions. This is arranged by having
helicity spinors carry an index in the Dirac spinor {\bf 4} of the massive
little group, $SO(5) \sim Sp(4)$. In the high energy limit, two separate kinds
of massless ... | [
{
"created": "Sun, 28 Oct 2018 12:02:11 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Mar 2019 11:48:15 GMT",
"version": "v2"
}
] | 2019-05-01 | [
[
"Jha",
"Rishabh",
""
],
[
"Krishnan",
"Chethan",
""
],
[
"Kumar",
"K. V. Pavan",
""
]
] | We show that a natural spinor-helicity formalism that can describe massive scattering amplitudes exists in $D=6$ dimensions. This is arranged by having helicity spinors carry an index in the Dirac spinor {\bf 4} of the massive little group, $SO(5) \sim Sp(4)$. In the high energy limit, two separate kinds of massless he... | 9.852023 | 10.713402 | 10.276417 | 9.734059 | 9.858298 | 10.178728 | 10.491193 | 10.316749 | 10.164434 | 10.937533 | 9.924791 | 9.442236 | 9.609435 | 9.451084 | 9.366178 | 9.537381 | 9.423347 | 9.429628 | 9.489658 | 10.115559 | 9.380818 |
hep-th/0101118 | Samir Mathur | Samir D. Mathur | Gravity on $AdS_3$ and flat connections in the boundary CFT | 35 pages, harvmac, references added | null | null | OHSTPY-HEP-T-00-033 | hep-th | null | We consider the CFT that arises from the D1-D5 system in the presence of a
constant background gauge potential which couples to the R-charge of the
theory: this potential effectively changes the periodicities of the fermions.
By the AdS/CFT correspondence, the effect of this connnection should be
obtained by finding ... | [
{
"created": "Wed, 17 Jan 2001 23:12:46 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Jul 2001 18:22:49 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Mathur",
"Samir D.",
""
]
] | We consider the CFT that arises from the D1-D5 system in the presence of a constant background gauge potential which couples to the R-charge of the theory: this potential effectively changes the periodicities of the fermions. By the AdS/CFT correspondence, the effect of this connnection should be obtained by finding a ... | 15.137174 | 16.01383 | 14.84986 | 14.421708 | 16.776934 | 15.786236 | 15.918873 | 14.603832 | 15.377952 | 16.402641 | 15.199097 | 15.629968 | 15.586699 | 14.317924 | 14.191222 | 14.304688 | 15.082108 | 14.609954 | 14.274711 | 14.778144 | 14.262198 |
1504.07985 | Sean A. Hartnoll | Sean A. Hartnoll and Edward Mazenc | Entanglement entropy in two dimensional string theory | 1+15 pages | Phys. Rev. Lett. 115, 121602 (2015) | 10.1103/PhysRevLett.115.121602 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | To understand an emergent spacetime is to understand the emergence of
locality. Entanglement entropy is a powerful diagnostic of locality, because
locality leads to a large amount of short distance entanglement. Two
dimensional string theory is among the very simplest instances of an emergent
spatial dimension. We co... | [
{
"created": "Wed, 29 Apr 2015 20:00:25 GMT",
"version": "v1"
}
] | 2015-09-23 | [
[
"Hartnoll",
"Sean A.",
""
],
[
"Mazenc",
"Edward",
""
]
] | To understand an emergent spacetime is to understand the emergence of locality. Entanglement entropy is a powerful diagnostic of locality, because locality leads to a large amount of short distance entanglement. Two dimensional string theory is among the very simplest instances of an emergent spatial dimension. We comp... | 8.395224 | 7.787331 | 8.636437 | 7.732387 | 7.865469 | 8.277606 | 7.505592 | 7.424984 | 7.690356 | 8.731566 | 7.869166 | 7.333436 | 8.107502 | 7.72569 | 7.531648 | 7.689139 | 7.377509 | 7.394779 | 7.528007 | 7.785259 | 7.811313 |
1512.01819 | Jun Zhang | Jaume Garriga, Alexander Vilenkin and Jun Zhang | Black holes and the multiverse | 49 pages, 15 figures, matches version to appear in JCAP | null | 10.1088/1475-7516/2016/02/064 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Vacuum bubbles may nucleate and expand during the inflationary epoch in the
early universe. After inflation ends, the bubbles quickly dissipate their
kinetic energy; they come to rest with respect to the Hubble flow and
eventually form black holes. The fate of the bubble itself depends on the
resulting black hole mas... | [
{
"created": "Sun, 6 Dec 2015 19:01:39 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Dec 2015 17:14:00 GMT",
"version": "v2"
},
{
"created": "Sun, 20 Dec 2015 22:08:06 GMT",
"version": "v3"
},
{
"created": "Thu, 25 Feb 2016 18:36:50 GMT",
"version": "v4"
}
] | 2016-03-16 | [
[
"Garriga",
"Jaume",
""
],
[
"Vilenkin",
"Alexander",
""
],
[
"Zhang",
"Jun",
""
]
] | Vacuum bubbles may nucleate and expand during the inflationary epoch in the early universe. After inflation ends, the bubbles quickly dissipate their kinetic energy; they come to rest with respect to the Hubble flow and eventually form black holes. The fate of the bubble itself depends on the resulting black hole mass.... | 6.161797 | 7.11772 | 6.30901 | 6.154836 | 6.520778 | 6.735852 | 6.36844 | 6.042785 | 6.642249 | 5.929118 | 6.268024 | 5.995353 | 5.905863 | 5.793447 | 5.755811 | 5.878554 | 5.890974 | 5.82655 | 5.848692 | 5.924292 | 5.907635 |
hep-th/0609058 | Margarita Garcia-Perez | Margarita Garcia Perez and Antonio Gonzalez-Arroyo | Gluino zero-modes for non-trivial holonomy calorons | 17 pages, 3 Postscript figures, latex | JHEP0611:091,2006 | 10.1088/1126-6708/2006/11/091 | IFT-UAM/CSIC-06-027, FTUAM-2006-15 | hep-th hep-lat math-ph math.MP | null | We couple fermion fields in the adjoint representation (gluinos) to the SU(2)
gauge field of unit charge calorons defined on R^3 x S_1. We compute
corresponding zero-modes of the Dirac equation. These are relevant in
semiclassical studies of N=1 Super-symmetric Yang-Mills theory. Our formulas,
show that, up to a term... | [
{
"created": "Fri, 8 Sep 2006 10:09:47 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Perez",
"Margarita Garcia",
""
],
[
"Gonzalez-Arroyo",
"Antonio",
""
]
] | We couple fermion fields in the adjoint representation (gluinos) to the SU(2) gauge field of unit charge calorons defined on R^3 x S_1. We compute corresponding zero-modes of the Dirac equation. These are relevant in semiclassical studies of N=1 Super-symmetric Yang-Mills theory. Our formulas, show that, up to a term p... | 17.454088 | 15.202782 | 17.506445 | 14.704537 | 16.34185 | 17.719179 | 16.441587 | 15.176824 | 14.57883 | 18.869196 | 15.017825 | 16.106621 | 16.248779 | 16.452677 | 16.711369 | 17.407385 | 15.74642 | 17.191391 | 15.626417 | 17.742798 | 15.616459 |
2304.13075 | Andre LeClair | Andr\'e LeClair | Comment on the cosmological constant for $\lambda \phi^4$ theory in $d$
spacetime dimensions | Only 7 pages, can be viewed as an addendum to our previous article
arXiv:2301.09019, accepted for publication in JHEP; This version accepted for
publication in the journal Universe | Universe (2023) 310 | 10.3390/universe9070310 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | In a recent article we showed that the analog of the cosmological constant in
two spacetime dimensions for a wide variety of integrable quantum field
theories has the form $\rho_{\rm vac} = - m^2 /2 \mathfrak{g} $ where $m$ is a
physical mass and $\mathfrak{g} $ is a generalized coupling, where in the free
field limi... | [
{
"created": "Tue, 25 Apr 2023 18:18:24 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jun 2023 23:20:47 GMT",
"version": "v2"
}
] | 2024-03-04 | [
[
"LeClair",
"André",
""
]
] | In a recent article we showed that the analog of the cosmological constant in two spacetime dimensions for a wide variety of integrable quantum field theories has the form $\rho_{\rm vac} = - m^2 /2 \mathfrak{g} $ where $m$ is a physical mass and $\mathfrak{g} $ is a generalized coupling, where in the free field limit ... | 5.519545 | 5.396212 | 5.392504 | 5.058745 | 5.214969 | 5.416179 | 5.430718 | 5.115043 | 5.193941 | 5.811624 | 5.234091 | 5.373441 | 5.38907 | 5.219023 | 5.226187 | 5.342899 | 5.238161 | 5.198153 | 5.28702 | 5.430208 | 5.336619 |
hep-th/0204136 | Rajesh Venkatachalapathy | Samik Dasgupta (Department of Physics, University of Colorado,
Boulder), Rajesh Venkatachalapathy (Institute of Mathematical Sciences,
CHENNAI, India), S. Kalyana Rama (Institute of Mathematical Sciences,
CHENNAI, India) | No Go Theorem for Self Tuning Solutions With Gauss-Bonnet Terms | 17 pages, 3 figures | JHEP 0207 (2002) 061 | 10.1088/1126-6708/2002/07/061 | IMSc/2002/03/07 | hep-th | null | We consider self tuning solutions for a brane embedded in an anti de Sitter
spacetime. We include the higher derivative Gauss-Bonnet terms in the action
and study singularity free solutions with finite effective Newton's constant.
Using the methods of Csaki et al, we prove that such solutions, when exist,
always requ... | [
{
"created": "Wed, 17 Apr 2002 03:10:56 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Jun 2002 16:30:10 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Jun 2002 04:08:39 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Dasgupta",
"Samik",
"",
"Department of Physics, University of Colorado,\n Boulder"
],
[
"Venkatachalapathy",
"Rajesh",
"",
"Institute of Mathematical Sciences,\n CHENNAI, India"
],
[
"Rama",
"S. Kalyana",
"",
"Institute of Mathematical Sciences,\n CHENNA... | We consider self tuning solutions for a brane embedded in an anti de Sitter spacetime. We include the higher derivative Gauss-Bonnet terms in the action and study singularity free solutions with finite effective Newton's constant. Using the methods of Csaki et al, we prove that such solutions, when exist, always requir... | 11.084786 | 8.841537 | 9.643081 | 8.240016 | 8.848486 | 8.470641 | 8.630801 | 8.429452 | 8.427909 | 8.801196 | 8.472267 | 8.646279 | 8.908097 | 8.671606 | 9.413412 | 8.890689 | 8.981803 | 8.750727 | 8.943111 | 9.002696 | 9.195374 |
1804.10550 | Michele Arzano | Michele Arzano and Jerzy Kowalski-Glikman | Horizon temperature on the real line | 4 pages, no figures; v2: extensive revision, references updated,
matches published version | Physics Letters B 788C (2019) pp. 82-86 | 10.1016/j.physletb.2018.10.019 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We illustrate the analogue of the Unruh effect for a quantum system on the
real line. Our derivation relies solely on basic elements of representation
theory of the group of affine transformations without a notion of time or
metric. Our result shows that a thermal distribution naturally emerges in
connecting quantum ... | [
{
"created": "Fri, 27 Apr 2018 15:09:45 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Nov 2018 12:41:36 GMT",
"version": "v2"
}
] | 2018-11-30 | [
[
"Arzano",
"Michele",
""
],
[
"Kowalski-Glikman",
"Jerzy",
""
]
] | We illustrate the analogue of the Unruh effect for a quantum system on the real line. Our derivation relies solely on basic elements of representation theory of the group of affine transformations without a notion of time or metric. Our result shows that a thermal distribution naturally emerges in connecting quantum st... | 21.159264 | 16.964794 | 18.226023 | 17.144623 | 17.482424 | 18.312157 | 19.127357 | 17.689741 | 18.41609 | 19.064987 | 17.47879 | 17.750587 | 17.839251 | 18.241638 | 16.554142 | 18.466305 | 17.686729 | 18.282152 | 17.58128 | 18.143835 | 18.593782 |
hep-th/0108115 | Matthew Schwartz | Lisa Randall and Matthew D. Schwartz | Unification and the Hierarchy from AdS5 | 5 pages, 2 figures | Phys.Rev.Lett.88:081801,2002 | 10.1103/PhysRevLett.88.081801 | MIT-CTP 3175 | hep-th hep-ph | null | In AdS5, the coupling for bulk gauge bosons runs logarithmically, not as a
power law. For this reason, one can preserve perturbative unification of
couplings. Depending on the cutoff, this can occur at a high scale. We discuss
subtleties in the calculation and present a regularization scheme motivated by
the holograp... | [
{
"created": "Thu, 16 Aug 2001 20:36:31 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Randall",
"Lisa",
""
],
[
"Schwartz",
"Matthew D.",
""
]
] | In AdS5, the coupling for bulk gauge bosons runs logarithmically, not as a power law. For this reason, one can preserve perturbative unification of couplings. Depending on the cutoff, this can occur at a high scale. We discuss subtleties in the calculation and present a regularization scheme motivated by the holographi... | 11.252423 | 12.651074 | 11.347775 | 11.082494 | 11.637478 | 11.04396 | 11.295941 | 11.460488 | 11.417253 | 12.300021 | 11.239992 | 10.708018 | 10.913885 | 10.948783 | 10.701733 | 10.299562 | 10.975717 | 10.919981 | 10.445698 | 10.915298 | 10.924546 |
1507.08859 | Benjamin Knorr | Holger Gies, Benjamin Knorr and Stefan Lippoldt | Generalized Parametrization Dependence in Quantum Gravity | 18 pages, 8 figures | Phys. Rev. D 92, 084020 (2015) | 10.1103/PhysRevD.92.084020 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We critically examine the gauge, and field-parametrization dependence of
renormalization group flows in the vicinity of non-Gau\ss{}ian fixed points in
quantum gravity. While physical observables are independent of such
calculational specifications, the construction of quantum gravity field
theories typically relies ... | [
{
"created": "Fri, 31 Jul 2015 12:52:50 GMT",
"version": "v1"
}
] | 2015-10-14 | [
[
"Gies",
"Holger",
""
],
[
"Knorr",
"Benjamin",
""
],
[
"Lippoldt",
"Stefan",
""
]
] | We critically examine the gauge, and field-parametrization dependence of renormalization group flows in the vicinity of non-Gau\ss{}ian fixed points in quantum gravity. While physical observables are independent of such calculational specifications, the construction of quantum gravity field theories typically relies on... | 13.088842 | 15.722261 | 14.506677 | 13.266601 | 14.870491 | 13.983313 | 15.200934 | 14.41029 | 14.128073 | 16.212114 | 13.399866 | 13.345686 | 13.407854 | 13.190535 | 13.947023 | 13.607972 | 13.516232 | 13.648227 | 13.548554 | 13.699694 | 13.250245 |
2104.13163 | Marco Bochicchio | Marco Bochicchio, Mauro Papinutto, Francesco Scardino | $n$-point correlators of twist-$2$ operators in $SU(N)$ Yang-Mills
theory to the lowest perturbative order | 77 pages, no figures, paper expanded by including the generating
functionals of the correlators both in the coordinate and momentum
representation | JHEP08(2021)142 | 10.1007/JHEP08(2021)142 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute, to the lowest perturbative order in $SU(N)$ Yang-Mills theory,
$n$-point correlators in the coordinate and momentum representation of the
gauge-invariant twist-$2$ operators with maximal spin along the $p_+$
direction, both in Minkowskian and -- by analytic continuation -- Euclidean
space-time. We also co... | [
{
"created": "Tue, 27 Apr 2021 13:18:18 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Jul 2021 22:25:52 GMT",
"version": "v2"
}
] | 2021-08-31 | [
[
"Bochicchio",
"Marco",
""
],
[
"Papinutto",
"Mauro",
""
],
[
"Scardino",
"Francesco",
""
]
] | We compute, to the lowest perturbative order in $SU(N)$ Yang-Mills theory, $n$-point correlators in the coordinate and momentum representation of the gauge-invariant twist-$2$ operators with maximal spin along the $p_+$ direction, both in Minkowskian and -- by analytic continuation -- Euclidean space-time. We also cons... | 11.00245 | 9.81564 | 11.661398 | 10.76392 | 10.827378 | 11.452214 | 12.333778 | 10.79694 | 10.591949 | 12.816013 | 10.09201 | 10.711948 | 10.998264 | 10.195945 | 10.483901 | 10.315278 | 10.458652 | 10.642275 | 10.281463 | 10.883828 | 9.901859 |
1109.3230 | Sayed Fawad Hassan | S. F. Hassan, Rachel A. Rosen, Angnis Schmidt-May | Ghost-free Massive Gravity with a General Reference Metric | v2: references, comments and a new subsection 3.5 added, discussion
of the secondary constraint updated | null | 10.1007/JHEP02(2012)026 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Theories of massive gravity inevitably include an auxiliary reference metric.
Generically, they also contain an inconsistency known as the Boulware-Deser
ghost. Recently, a family of non-linear massive gravity actions, formulated
with a flat reference metric, were proposed and shown to be ghost free at the
complete n... | [
{
"created": "Thu, 15 Sep 2011 00:13:45 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Dec 2011 02:23:22 GMT",
"version": "v2"
}
] | 2015-05-30 | [
[
"Hassan",
"S. F.",
""
],
[
"Rosen",
"Rachel A.",
""
],
[
"Schmidt-May",
"Angnis",
""
]
] | Theories of massive gravity inevitably include an auxiliary reference metric. Generically, they also contain an inconsistency known as the Boulware-Deser ghost. Recently, a family of non-linear massive gravity actions, formulated with a flat reference metric, were proposed and shown to be ghost free at the complete non... | 5.764877 | 5.843995 | 5.939259 | 5.608813 | 5.904979 | 5.680252 | 5.586732 | 5.504264 | 5.61556 | 6.286073 | 5.528273 | 5.776491 | 5.473455 | 5.475513 | 5.620576 | 5.545768 | 5.63062 | 5.544153 | 5.539032 | 5.736129 | 5.42485 |
hep-th/9401086 | null | M. Cavicchi | A Bilocal Field Approach to the Large-N Expansion of Two-Dimensional
(Gauge) Theories | 36 pages + 7 uuencoded postcript figures, Latex, Preprint DFUB-93-17 | Int.J.Mod.Phys. A10 (1995) 167-198 | 10.1142/S0217751X95000097 | null | hep-th | null | We consider a wide class of two-dimensional models as gauge theories,
Gross-Neveu model, $O(N)$ and $CP^{N-1}$-like models using a formalism based on
the introduction of bilocal fields that permits to perform easily the large-N
expansion of this set of models in a unified and general way. We mainly discuss
the $SU(N)... | [
{
"created": "Wed, 19 Jan 1994 15:22:27 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Cavicchi",
"M.",
""
]
] | We consider a wide class of two-dimensional models as gauge theories, Gross-Neveu model, $O(N)$ and $CP^{N-1}$-like models using a formalism based on the introduction of bilocal fields that permits to perform easily the large-N expansion of this set of models in a unified and general way. We mainly discuss the $SU(N)$ ... | 11.627683 | 10.755131 | 12.426546 | 10.893572 | 11.709353 | 10.765141 | 11.120825 | 10.559653 | 10.665935 | 13.392072 | 10.80712 | 10.931037 | 11.942355 | 10.929533 | 10.71956 | 11.18742 | 10.579971 | 10.532699 | 10.996431 | 10.847786 | 10.920879 |
2206.07653 | John Klauder | John R. Klauder | A Valid Quantization of a Half-Harmonic Oscillator Field Theory | 9 pages, a valid quantization of a novel model | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The usual full- and half-harmonic oscillators are turned into field theories,
and that behavior is examined using canonical and affine quantization. The
result leads to a valid affine quantization of the half harmonic oscillator
field theory, which points toward further valid quantizations of more realistic
field the... | [
{
"created": "Sat, 4 Jun 2022 14:05:48 GMT",
"version": "v1"
}
] | 2022-06-16 | [
[
"Klauder",
"John R.",
""
]
] | The usual full- and half-harmonic oscillators are turned into field theories, and that behavior is examined using canonical and affine quantization. The result leads to a valid affine quantization of the half harmonic oscillator field theory, which points toward further valid quantizations of more realistic field theor... | 28.459421 | 22.777321 | 23.18786 | 25.058302 | 25.990242 | 21.537943 | 23.23332 | 20.181219 | 23.471111 | 25.705296 | 21.836693 | 23.415485 | 23.858438 | 23.392754 | 22.633417 | 22.728205 | 21.815857 | 22.388456 | 23.72645 | 22.96616 | 21.740499 |
1008.4567 | Jean-Luc Lehners | Jean-Luc Lehners and Paul J. Steinhardt | Dynamical Selection of the Primordial Density Fluctuation Amplitude | 4 pages; v2: version to be published in PRL | Phys.Rev.Lett.106:081301,2011 | 10.1103/PhysRevLett.106.081301 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In inflationary models, the predicted amplitude of primordial density
perturbations Q is much larger than the observed value (~10^{-5}) for natural
choices of parameters. To explain the requisite exponential fine-tuning,
anthropic selection is often invoked, especially in cases where microphysics is
expected to produ... | [
{
"created": "Thu, 26 Aug 2010 19:20:58 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Feb 2011 14:42:10 GMT",
"version": "v2"
}
] | 2011-03-02 | [
[
"Lehners",
"Jean-Luc",
""
],
[
"Steinhardt",
"Paul J.",
""
]
] | In inflationary models, the predicted amplitude of primordial density perturbations Q is much larger than the observed value (~10^{-5}) for natural choices of parameters. To explain the requisite exponential fine-tuning, anthropic selection is often invoked, especially in cases where microphysics is expected to produce... | 12.058134 | 12.355285 | 11.48802 | 10.917909 | 11.069717 | 11.845069 | 11.153293 | 11.37208 | 11.650671 | 13.360416 | 11.509063 | 11.203157 | 10.872821 | 11.15294 | 10.835507 | 11.260617 | 10.592415 | 11.105246 | 10.627756 | 11.474948 | 10.90054 |
hep-th/9907149 | Guy Bonneau | Guy Bonneau | Non linear $\sigma$ models : renormalisability versus geometry | 10 pages, latex file, Talk given in Cortona, Italy, at the 1st June
meeting in honnor of Carlo Becchi 60th birthday | null | null | PAR/LPTHE/99-27 | hep-th | null | After some recalls on the standard (non)-linear $\sigma$ model, we discuss
the interest of B.R.S. symmetry in non-linear $\sigma$ models renormalisation.
We also emphasise the importance of a correct definition of a theory through
physical constraints rather than as given by a particular Lagrangian and
discuss some w... | [
{
"created": "Sat, 17 Jul 1999 15:27:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bonneau",
"Guy",
""
]
] | After some recalls on the standard (non)-linear $\sigma$ model, we discuss the interest of B.R.S. symmetry in non-linear $\sigma$ models renormalisation. We also emphasise the importance of a correct definition of a theory through physical constraints rather than as given by a particular Lagrangian and discuss some way... | 20.095285 | 16.836708 | 15.414673 | 14.60086 | 15.620927 | 15.567588 | 16.122477 | 14.438025 | 13.013595 | 15.162971 | 16.028151 | 15.528461 | 15.345168 | 14.351229 | 15.286922 | 14.891983 | 15.395637 | 15.324167 | 14.820302 | 14.055537 | 14.94563 |
hep-th/0411143 | Noriko Nakayama | Noriko Nakayama, Katsuyuki Sugiyama | Construction of Supergravity Backgrounds with a Dilaton Field | 13 pages, minor corrections | Phys.Lett. B607 (2005) 306-316 | 10.1016/j.physletb.2004.12.070 | KUNS 1944 | hep-th | null | A new class of non-compact Kahler backgrounds accompanied by a non-constant
dilaton field is constructed as a supergravity solution. It is interpreted as a
complex line bundle over a base manifold comprising of a combination of
arbitrary coset spaces, and also includes the case of Calabi-Yau manifolds. The
resulting ... | [
{
"created": "Mon, 15 Nov 2004 17:39:05 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Dec 2004 12:29:32 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Nakayama",
"Noriko",
""
],
[
"Sugiyama",
"Katsuyuki",
""
]
] | A new class of non-compact Kahler backgrounds accompanied by a non-constant dilaton field is constructed as a supergravity solution. It is interpreted as a complex line bundle over a base manifold comprising of a combination of arbitrary coset spaces, and also includes the case of Calabi-Yau manifolds. The resulting ba... | 10.643393 | 9.050855 | 10.627871 | 9.578884 | 9.332871 | 9.422879 | 9.959503 | 8.916089 | 9.521624 | 10.908014 | 8.832539 | 9.294787 | 10.472185 | 9.221204 | 9.389006 | 9.496668 | 9.523532 | 9.542258 | 9.482044 | 10.071833 | 9.41136 |
hep-th/0410074 | S. Stieberger | D. Lust, S. Reffert, S. Stieberger | MSSM with Soft SUSY Breaking Terms from D7-Branes with Fluxes | 41 pages, harvmac. Typos removed and more general twisted matter
field metric used | Nucl.Phys.B727:264-300,2005 | 10.1016/j.nuclphysb.2005.08.009 | null | hep-th hep-ph | null | We discuss the structure of the soft supersymmetry breaking terms in a MSSM
like model, which can be derived from D7-branes with chiral matter fields from
2-form f-fluxes and supersymmetry breaking from 3-form G-fluxes.
| [
{
"created": "Thu, 7 Oct 2004 13:31:50 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Dec 2004 16:37:09 GMT",
"version": "v2"
},
{
"created": "Sun, 3 Jul 2005 17:27:03 GMT",
"version": "v3"
}
] | 2009-10-07 | [
[
"Lust",
"D.",
""
],
[
"Reffert",
"S.",
""
],
[
"Stieberger",
"S.",
""
]
] | We discuss the structure of the soft supersymmetry breaking terms in a MSSM like model, which can be derived from D7-branes with chiral matter fields from 2-form f-fluxes and supersymmetry breaking from 3-form G-fluxes. | 11.379384 | 10.12326 | 9.724694 | 8.114108 | 9.840388 | 9.276616 | 9.344112 | 9.491984 | 8.169521 | 10.226335 | 8.727772 | 9.192887 | 9.262207 | 8.850444 | 8.866846 | 9.31568 | 9.117549 | 9.885005 | 9.296379 | 9.39615 | 9.183726 |
hep-th/9806200 | M. R. Pennington | M.R. Pennington | Mass production requires precision engineering | 12 pages, 6 epsi figures. To be published in the Proceedings of the
Workshop on Methods in Non-perturbative Field Theories, CSSM/NITP, Adelaide,
February 1998 | null | null | DTP-98/42 | hep-th | null | This talk is in two parts both entitled mass production requires precision
engineering. The first is about the dynamical generation of mass for matter
particles in gauge theories. I will explain how the details of this depend on a
precision knowledge of the interactions. The second is about tests of the
mechanism of ... | [
{
"created": "Wed, 24 Jun 1998 12:11:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Pennington",
"M. R.",
""
]
] | This talk is in two parts both entitled mass production requires precision engineering. The first is about the dynamical generation of mass for matter particles in gauge theories. I will explain how the details of this depend on a precision knowledge of the interactions. The second is about tests of the mechanism of ch... | 16.740072 | 17.478611 | 14.609237 | 14.396399 | 15.972296 | 17.224401 | 16.252157 | 16.450254 | 15.341177 | 16.77704 | 14.733625 | 16.560774 | 15.912305 | 14.701299 | 15.443083 | 15.824904 | 15.756503 | 16.294338 | 15.167042 | 15.470411 | 16.257206 |
hep-th/0702077 | Jonathan Heckman | Jonathan J. Heckman, Jihye Seo, Cumrun Vafa | Phase Structure of a Brane/Anti-Brane System at Large N | v3: 55 pages, 11 figures, typos corrected | JHEP0707:073,2007 | 10.1088/1126-6708/2007/07/073 | HUTP-07/A0002 | hep-th | null | We further analyze a class of recently studied metastable string vacua
obtained by wrapping D5-branes and anti-D5-branes over rigid homologous S^2's
of a non-compact Calabi-Yau threefold. The large N dual description is
characterized by a potential for the glueball fields which is determined by an
auxiliary matrix mo... | [
{
"created": "Mon, 12 Feb 2007 19:30:51 GMT",
"version": "v1"
},
{
"created": "Tue, 22 May 2007 20:38:48 GMT",
"version": "v2"
},
{
"created": "Fri, 27 Jul 2007 20:26:40 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Heckman",
"Jonathan J.",
""
],
[
"Seo",
"Jihye",
""
],
[
"Vafa",
"Cumrun",
""
]
] | We further analyze a class of recently studied metastable string vacua obtained by wrapping D5-branes and anti-D5-branes over rigid homologous S^2's of a non-compact Calabi-Yau threefold. The large N dual description is characterized by a potential for the glueball fields which is determined by an auxiliary matrix mode... | 10.411292 | 8.977295 | 10.805093 | 8.724375 | 9.10513 | 9.164924 | 9.07899 | 8.941584 | 9.102957 | 12.201767 | 8.661502 | 9.18422 | 10.284923 | 9.271694 | 9.074058 | 9.299937 | 9.156536 | 9.080446 | 9.250427 | 10.173093 | 9.117717 |
1908.01913 | Stuart Raby | Herbert Clemens and Stuart Raby | Heterotic-$\mathbf{F}$-theory Duality with Wilson Line Symmetry-breaking | 51 pages, corrected some typos | null | 10.1007/JHEP12(2019)016 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We begin with an $E_{8}\times E_{8}$ Heterotic model broken to an
$SU(5)_{gauge}$ and a mirror $SU(5)_{gauge}$, where one $SU(5)$ and its
spectrum is identified as the visible sector while the other can be identified
as a hidden mirror world. In both cases we obtain the minimal supersymmetric
standard model spectrum ... | [
{
"created": "Tue, 6 Aug 2019 00:43:22 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Nov 2019 20:33:39 GMT",
"version": "v2"
}
] | 2020-01-29 | [
[
"Clemens",
"Herbert",
""
],
[
"Raby",
"Stuart",
""
]
] | We begin with an $E_{8}\times E_{8}$ Heterotic model broken to an $SU(5)_{gauge}$ and a mirror $SU(5)_{gauge}$, where one $SU(5)$ and its spectrum is identified as the visible sector while the other can be identified as a hidden mirror world. In both cases we obtain the minimal supersymmetric standard model spectrum af... | 9.101766 | 9.730053 | 10.059919 | 9.811077 | 10.40788 | 10.263682 | 10.173731 | 9.611731 | 9.351472 | 10.949297 | 9.2133 | 8.958249 | 9.195094 | 9.084602 | 9.387301 | 9.179738 | 9.173513 | 9.155216 | 9.020417 | 9.572341 | 8.986818 |
1007.4485 | Adil Belhaj Rogani | A. Belhaj, N-E. Fahssi, E.H. Saidi, A. Segui | Embedding Fractional Quantum Hall Solitons in M-theory Compactifications | Latex, 14 pages. Modified version, to appear in IJGMMP | null | 10.1142/S0219887811005762 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We engineer U(1)^n Chern-Simons type theories describing fractional quantum
Hall solitons (QHS) in 1+2 dimensions from M-theory compactified on eight
dimensional hyper-K\"{a}hler manifolds as target space of N=4 sigma model.
Based on M-theory/Type IIA duality, the systems can be modeled by considering
D6-branes wrapp... | [
{
"created": "Mon, 26 Jul 2010 15:25:50 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Mar 2011 15:06:40 GMT",
"version": "v2"
}
] | 2015-05-19 | [
[
"Belhaj",
"A.",
""
],
[
"Fahssi",
"N-E.",
""
],
[
"Saidi",
"E. H.",
""
],
[
"Segui",
"A.",
""
]
] | We engineer U(1)^n Chern-Simons type theories describing fractional quantum Hall solitons (QHS) in 1+2 dimensions from M-theory compactified on eight dimensional hyper-K\"{a}hler manifolds as target space of N=4 sigma model. Based on M-theory/Type IIA duality, the systems can be modeled by considering D6-branes wrappin... | 13.74361 | 12.116262 | 14.613557 | 11.288465 | 11.833008 | 12.756553 | 11.533935 | 10.9638 | 10.935265 | 17.893568 | 11.16076 | 10.995457 | 12.869469 | 11.414721 | 11.628237 | 11.950162 | 11.573114 | 11.603913 | 11.678027 | 13.202885 | 11.339114 |
0911.4999 | Anindya Mukherjee | Pallab Basu, Jianyang He, Anindya Mukherjee and Hsien-Hang Shieh | Hard-gapped Holographic Superconductors | 9 pages, latex, 6 figures | Phys.Lett.B689:45-50,2010 | 10.1016/j.physletb.2010.04.042 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we discuss the zero temperature limit of a "p-wave" holographic
superconductor. The bulk description consists of a non-Abelian SU(2) gauge
fields minimally coupled to gravity. We numerically construct the zero
temperature solution which is the gravity dual of the superconducting ground
state of the "p-wa... | [
{
"created": "Thu, 26 Nov 2009 11:02:56 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Nov 2009 07:55:38 GMT",
"version": "v2"
},
{
"created": "Sat, 5 Dec 2009 03:00:29 GMT",
"version": "v3"
}
] | 2010-05-25 | [
[
"Basu",
"Pallab",
""
],
[
"He",
"Jianyang",
""
],
[
"Mukherjee",
"Anindya",
""
],
[
"Shieh",
"Hsien-Hang",
""
]
] | In this work we discuss the zero temperature limit of a "p-wave" holographic superconductor. The bulk description consists of a non-Abelian SU(2) gauge fields minimally coupled to gravity. We numerically construct the zero temperature solution which is the gravity dual of the superconducting ground state of the "p-wave... | 8.416561 | 7.398611 | 9.176297 | 7.5451 | 7.897842 | 7.910821 | 7.922848 | 7.163054 | 7.437621 | 9.558299 | 7.284477 | 7.57629 | 8.274318 | 7.713983 | 7.573215 | 7.444806 | 7.751088 | 7.625677 | 7.978446 | 8.316023 | 7.5768 |
2403.14446 | Sergey Fedoruk | I.L. Buchbinder, S.A. Fedoruk, A.P. Isaev, V.A. Krykhtin | BRST construction for infinite spin field on $AdS_4$ | 1 + 16 pages; v4: published version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the first class constraints that describe the infinite spin
irreducible $4D$ Poincar\'{e} group representation in flat space to new first
class constraints in $AdS_4$ space. The constraints are realized as operators
acting in Fock space spanned by the creation and annihilation operators with
two-compone... | [
{
"created": "Thu, 21 Mar 2024 14:52:49 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Apr 2024 11:55:11 GMT",
"version": "v2"
},
{
"created": "Mon, 13 May 2024 10:58:03 GMT",
"version": "v3"
},
{
"created": "Wed, 17 Jul 2024 07:34:14 GMT",
"version": "v4"
}
] | 2024-07-18 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Fedoruk",
"S. A.",
""
],
[
"Isaev",
"A. P.",
""
],
[
"Krykhtin",
"V. A.",
""
]
] | We generalize the first class constraints that describe the infinite spin irreducible $4D$ Poincar\'{e} group representation in flat space to new first class constraints in $AdS_4$ space. The constraints are realized as operators acting in Fock space spanned by the creation and annihilation operators with two-component... | 8.402496 | 6.135777 | 8.808361 | 6.605098 | 7.088938 | 6.608744 | 6.305886 | 6.099554 | 6.538381 | 8.675569 | 6.581497 | 6.944328 | 7.589385 | 6.840828 | 6.698895 | 6.735013 | 6.842452 | 6.923276 | 6.84384 | 7.419945 | 6.85844 |
hep-th/9701058 | Joao Barcelos Neto | J. Barcelos-Neto and W. Oliveira | Transformation of second-class into first-class constraints in
supersymmetric theories | 22 pages, Latex | Int.J.Mod.Phys. A12 (1997) 5209-5222 | 10.1142/S0217751X97002796 | null | hep-th | null | We use the method due to Batalin, Fradkin, Fradkina, and Tyutin (BFFT) in
order to convert second-class into first-class constraints for some quantum
mechanics supersymmetric theories. The main point to be considered is that the
extended theory, where new auxiliary variables are introduced, has to be
supersymmetric t... | [
{
"created": "Tue, 14 Jan 1997 19:37:47 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Barcelos-Neto",
"J.",
""
],
[
"Oliveira",
"W.",
""
]
] | We use the method due to Batalin, Fradkin, Fradkina, and Tyutin (BFFT) in order to convert second-class into first-class constraints for some quantum mechanics supersymmetric theories. The main point to be considered is that the extended theory, where new auxiliary variables are introduced, has to be supersymmetric too... | 9.227218 | 7.554779 | 8.21932 | 6.996469 | 7.02921 | 6.816725 | 6.503516 | 7.430328 | 7.013006 | 10.887309 | 7.725688 | 7.558181 | 8.284366 | 7.350421 | 7.735757 | 7.561735 | 7.492303 | 7.631124 | 7.544965 | 8.67666 | 7.47161 |
1812.00389 | Anirban Basu | Anirban Basu | Eigenvalue equation for genus two modular graphs | 67 pages, LaTex; 27 figures | null | 10.1007/JHEP02(2019)046 | null | hep-th math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain a second order differential equation on moduli space satisfied by
certain modular graph functions at genus two, each of which has two links. This
eigenvalue equation is obtained by analyzing the variations of these graphs
under the variation of the Beltrami differentials. This equation involves seven
distin... | [
{
"created": "Sun, 2 Dec 2018 13:34:49 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Feb 2019 07:46:46 GMT",
"version": "v2"
}
] | 2019-02-20 | [
[
"Basu",
"Anirban",
""
]
] | We obtain a second order differential equation on moduli space satisfied by certain modular graph functions at genus two, each of which has two links. This eigenvalue equation is obtained by analyzing the variations of these graphs under the variation of the Beltrami differentials. This equation involves seven distinct... | 9.120649 | 6.957536 | 12.362513 | 6.847993 | 7.583854 | 7.103658 | 7.271587 | 7.349037 | 7.40964 | 12.557412 | 7.472441 | 7.826531 | 8.904972 | 7.745193 | 8.055501 | 7.734595 | 7.87535 | 7.658676 | 8.065677 | 8.745452 | 7.898957 |
2007.10156 | Davoud Kamani | Davoud Kamani | Brane with Transverse Rotation and Background Fields: Boundary State and
Tachyon Condensation | 15 pages, LaTeX2e, no figure | Eur. Phys. J. C (2020) 80:624 | 10.1140/epjc/s10052-020-8212-3 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The boundary state corresponding to the D$p$-brane with a transverse rotation
in the presence of the Kalb-Ramond and tachyon background fields and a $U(1)$
internal field will be constructed. We shall investigate effects of the open
string tachyon condensation on this brane via its boundary state. We
demonstrate that... | [
{
"created": "Mon, 20 Jul 2020 14:27:55 GMT",
"version": "v1"
}
] | 2020-07-24 | [
[
"Kamani",
"Davoud",
""
]
] | The boundary state corresponding to the D$p$-brane with a transverse rotation in the presence of the Kalb-Ramond and tachyon background fields and a $U(1)$ internal field will be constructed. We shall investigate effects of the open string tachyon condensation on this brane via its boundary state. We demonstrate that t... | 10.055073 | 7.077309 | 9.765458 | 7.666197 | 8.192108 | 6.856901 | 6.934028 | 7.232924 | 7.086791 | 10.810081 | 7.73372 | 8.918106 | 9.222473 | 8.503732 | 8.782931 | 8.516159 | 8.602289 | 8.694133 | 8.66113 | 9.94917 | 8.677316 |
2112.09614 | Alesandro Santos | L. H. A. R. Ferreira, A. F. Santos and Faqir C. Khanna | TFD formalism: applications to the scalar field in a Lorentz-violating
theory | 16 pages, accepted for publication in PLB | null | 10.1016/j.physletb.2021.136845 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The Thermofield Dynamics (TFD) formalism is considered. In this context, a
Lorentz-breaking scalar field theory is introduced. In contrast to the
Matsubara formalism, the best-known approach to introducing the temperature
effect, TFD is a real-time formalism and is a topological field theory. While
in Matsubara the t... | [
{
"created": "Fri, 17 Dec 2021 16:43:09 GMT",
"version": "v1"
}
] | 2022-01-05 | [
[
"Ferreira",
"L. H. A. R.",
""
],
[
"Santos",
"A. F.",
""
],
[
"Khanna",
"Faqir C.",
""
]
] | The Thermofield Dynamics (TFD) formalism is considered. In this context, a Lorentz-breaking scalar field theory is introduced. In contrast to the Matsubara formalism, the best-known approach to introducing the temperature effect, TFD is a real-time formalism and is a topological field theory. While in Matsubara the tem... | 8.220592 | 7.33289 | 8.60956 | 7.484615 | 7.760966 | 7.626695 | 7.666122 | 7.391673 | 7.825796 | 9.141398 | 7.351424 | 7.748378 | 8.104963 | 7.729163 | 7.608089 | 7.780978 | 7.654552 | 7.887019 | 7.662182 | 8.24269 | 7.452359 |
hep-th/0506005 | Jean Iliopoulos | Jean Iliopoulos (LPTENS) | Gauge Theories and Non-Commutative Geometry | null | Fortsch.Phys. 54 (2006) 139-145 | 10.1002/prop.200510262 | null | hep-th | null | It is shown that a $d$-dimensional classical SU(N) Yang-Mills theory can be
formulated in a $d+2$-dimensional space, with the extra two dimensions forming
a surface with non-commutative geometry.
| [
{
"created": "Wed, 1 Jun 2005 11:59:28 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Iliopoulos",
"Jean",
"",
"LPTENS"
]
] | It is shown that a $d$-dimensional classical SU(N) Yang-Mills theory can be formulated in a $d+2$-dimensional space, with the extra two dimensions forming a surface with non-commutative geometry. | 6.3456 | 3.888601 | 5.630642 | 4.45477 | 4.030309 | 3.855571 | 4.058803 | 3.79678 | 4.913118 | 6.188547 | 4.422697 | 4.742468 | 5.466265 | 5.153244 | 4.862464 | 4.873942 | 4.91985 | 4.951746 | 4.941428 | 5.629173 | 4.670504 |
hep-th/9910264 | Dubin Andrey Yurievich | Andrey Dubin | Nonabelian Duality and Solvable Large N Lattice Systems | TeX, 46 pages | Nucl.Phys. B584 (2000) 749-783 | 10.1016/S0550-3213(00)00351-5 | null | hep-th hep-lat | null | We introduce the basics of the nonabelian duality transformation of SU(N) or
U(N) vector-field models defined on a lattice. The dual degrees of freedom are
certain species of the integer-valued fields complemented by the symmetric
groups' \otimes_{n} S(n) variables. While the former parametrize relevant
irreducible r... | [
{
"created": "Mon, 1 Nov 1999 15:28:14 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Dubin",
"Andrey",
""
]
] | We introduce the basics of the nonabelian duality transformation of SU(N) or U(N) vector-field models defined on a lattice. The dual degrees of freedom are certain species of the integer-valued fields complemented by the symmetric groups' \otimes_{n} S(n) variables. While the former parametrize relevant irreducible rep... | 17.165703 | 17.57143 | 19.530283 | 15.030684 | 18.654879 | 17.012865 | 17.221512 | 16.803526 | 16.530781 | 21.084099 | 16.246687 | 16.43679 | 16.767561 | 16.020975 | 16.567068 | 17.348158 | 16.967731 | 16.815079 | 15.866719 | 17.701681 | 16.442858 |
1506.00035 | Mario Neves Junior | Everton M. C. Abreu and M. J. Neves | The Yang-Mills gauge theory in DFR noncommutative space-time | 26 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Doplicher-Fredenhagen-Roberts (DFR) framework for noncommutative (NC)
space-times is considered as an alternative approach to describe the physics of
quantum gravity, for instance. In this formalism, the NC parameter, {\it i.e.}
$\theta^{\mu\nu}$, is promoted to a coordinate of a new extended space-time.
Conseque... | [
{
"created": "Fri, 29 May 2015 21:35:01 GMT",
"version": "v1"
}
] | 2015-06-02 | [
[
"Abreu",
"Everton M. C.",
""
],
[
"Neves",
"M. J.",
""
]
] | The Doplicher-Fredenhagen-Roberts (DFR) framework for noncommutative (NC) space-times is considered as an alternative approach to describe the physics of quantum gravity, for instance. In this formalism, the NC parameter, {\it i.e.} $\theta^{\mu\nu}$, is promoted to a coordinate of a new extended space-time. Consequent... | 8.044889 | 7.296346 | 8.606066 | 7.171862 | 7.436532 | 7.313286 | 7.420318 | 7.314983 | 7.119779 | 8.16135 | 7.442645 | 7.241935 | 7.741185 | 7.335212 | 7.352758 | 7.307505 | 7.055324 | 7.236714 | 7.240048 | 7.974058 | 7.472592 |
1011.6388 | Andres Collinucci | Andres Collinucci and Raffaele Savelli | On Flux Quantization in F-Theory | 46 pages | null | 10.1007/JHEP02(2012)015 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the problem of four-form flux quantization in F-theory
compactifications. We prove that for smooth, elliptically fibered Calabi-Yau
fourfolds with a Weierstrass representation, the flux is always integrally
quantized. This implies that any possible half-integral quantization effects
must come from 7-branes, ... | [
{
"created": "Mon, 29 Nov 2010 21:06:55 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Mar 2012 20:03:01 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Collinucci",
"Andres",
""
],
[
"Savelli",
"Raffaele",
""
]
] | We study the problem of four-form flux quantization in F-theory compactifications. We prove that for smooth, elliptically fibered Calabi-Yau fourfolds with a Weierstrass representation, the flux is always integrally quantized. This implies that any possible half-integral quantization effects must come from 7-branes, i.... | 9.011221 | 9.47004 | 10.279933 | 8.851119 | 8.299855 | 9.308573 | 9.954421 | 8.749516 | 9.294544 | 11.197311 | 8.472142 | 8.493544 | 9.328336 | 8.595112 | 8.855015 | 8.858143 | 8.841784 | 8.687132 | 8.641879 | 8.957526 | 8.8065 |
hep-th/9409183 | Yong Wan Kim | Yong-Wan Kim, Young-Jai Park, Kee Yong Kim and Yongduk Kim | Batalin-Tyutin Quantization of the Self-Dual Massive Theory in Three
Dimensions | 17 pages, SOGANG-HEP 191/94 | Phys.Rev. D51 (1995) 2943-2949 | 10.1103/PhysRevD.51.2943 | null | hep-th | null | We quantize the self-dual massive theory by using the Batalin-Tyutin
Hamiltonian method, which systematically embeds second class constraint system
into first class one in the extended phase space by introducing the new fields.
Through this analysis we obtain simultaneously the St\"uckelberg scalar term
related to th... | [
{
"created": "Thu, 29 Sep 1994 14:53:19 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Kim",
"Yong-Wan",
""
],
[
"Park",
"Young-Jai",
""
],
[
"Kim",
"Kee Yong",
""
],
[
"Kim",
"Yongduk",
""
]
] | We quantize the self-dual massive theory by using the Batalin-Tyutin Hamiltonian method, which systematically embeds second class constraint system into first class one in the extended phase space by introducing the new fields. Through this analysis we obtain simultaneously the St\"uckelberg scalar term related to the ... | 15.393006 | 7.427582 | 14.47885 | 10.061996 | 8.008085 | 8.058287 | 8.191712 | 8.807792 | 8.788795 | 15.708267 | 9.660272 | 11.315366 | 13.748501 | 11.785592 | 11.577009 | 11.783564 | 11.640286 | 12.061008 | 11.515901 | 13.405499 | 11.500602 |
2005.02761 | Keita Nii | Keita Nii | Coulomb branch in 3d $\mathcal{N}=2$ $SU(N)_k$ Chern-Simons gauge
theories with chiral matter content | 56 pages: refs added, typos corrected, refined argument | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We elaborate on quantum moduli spaces in 3d $\mathcal{N}=2$ $SU(N)_k$
Chern-Simons gauge theories with $F$ fundamental and $\bar{F}$ anti-fundamental
matter fields. The quantum flat direction on the Coulomb branch differs so much
from the classical one and from the one of the vector-like theories. In many
cases, the ... | [
{
"created": "Wed, 6 May 2020 12:23:16 GMT",
"version": "v1"
},
{
"created": "Mon, 11 May 2020 03:56:19 GMT",
"version": "v2"
}
] | 2020-05-12 | [
[
"Nii",
"Keita",
""
]
] | We elaborate on quantum moduli spaces in 3d $\mathcal{N}=2$ $SU(N)_k$ Chern-Simons gauge theories with $F$ fundamental and $\bar{F}$ anti-fundamental matter fields. The quantum flat direction on the Coulomb branch differs so much from the classical one and from the one of the vector-like theories. In many cases, the Co... | 7.257286 | 7.689379 | 8.838819 | 6.746528 | 7.233567 | 7.615864 | 7.589582 | 7.330688 | 7.279011 | 10.484806 | 7.043631 | 7.190554 | 7.723547 | 6.960384 | 6.826757 | 6.953176 | 7.077175 | 7.237797 | 6.797127 | 7.655789 | 6.971548 |
hep-th/0501030 | Anirban Saha | Rabin Banerjee, Pradip Mukherjee, Anirban Saha | Bosonic p-brane and A--D--M decomposition | LaTeX, 14 pages, Title changed, paper extended, references added,
this version is to appear in Phys. Rev. D | Phys.Rev. D72 (2005) 066015 | 10.1103/PhysRevD.72.066015 | null | hep-th | null | A master action for the bosonic p-brane, interpolating between the
Nambu--Goto and Polyakov formalisms, is discussed. The fundamental
arbitrariness of extended structures (p-brane) embeded in space time manifold
has been exploited to build an independent metric in the brane world volume.
The cosmological term for the... | [
{
"created": "Thu, 6 Jan 2005 11:11:54 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Sep 2005 10:27:46 GMT",
"version": "v2"
},
{
"created": "Thu, 22 Sep 2005 10:38:24 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Banerjee",
"Rabin",
""
],
[
"Mukherjee",
"Pradip",
""
],
[
"Saha",
"Anirban",
""
]
] | A master action for the bosonic p-brane, interpolating between the Nambu--Goto and Polyakov formalisms, is discussed. The fundamental arbitrariness of extended structures (p-brane) embeded in space time manifold has been exploited to build an independent metric in the brane world volume. The cosmological term for the g... | 19.809416 | 14.141125 | 16.800264 | 14.078278 | 14.590771 | 14.527439 | 15.237361 | 14.67886 | 14.686203 | 20.416431 | 14.579566 | 15.561681 | 16.030291 | 15.180561 | 14.491052 | 14.911581 | 14.91885 | 15.037305 | 15.441051 | 15.004941 | 15.366461 |
1812.11756 | Daniel Brattan K | Daniel K. Brattan | The curious behaviour of the scale invariant $(2+1)$-dimensional
Lifshitz scalar | 9 pages, 3 figures + 3 pages supplementary material, 2 supplementary
figures | null | null | null | hep-th cond-mat.quant-gas math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate the existence of an exactly marginal deformation, with
derivative coupling, about the free theory of a $(2+1)$-dimensional charged,
Lifshitz scalar with dynamic critical exponent $z=4$ and particle-hole
asymmetry. We show that the other classically scale invariant interactions
(consistent with translat... | [
{
"created": "Mon, 31 Dec 2018 10:51:41 GMT",
"version": "v1"
}
] | 2019-01-01 | [
[
"Brattan",
"Daniel K.",
""
]
] | We demonstrate the existence of an exactly marginal deformation, with derivative coupling, about the free theory of a $(2+1)$-dimensional charged, Lifshitz scalar with dynamic critical exponent $z=4$ and particle-hole asymmetry. We show that the other classically scale invariant interactions (consistent with translatio... | 11.008422 | 11.038958 | 12.441938 | 10.564111 | 10.845207 | 10.903313 | 10.814803 | 10.33282 | 10.247996 | 11.855012 | 10.406495 | 10.477355 | 10.995487 | 10.51429 | 10.862732 | 10.542919 | 10.578055 | 10.604208 | 10.60531 | 11.207813 | 10.366433 |
hep-th/9509004 | Barry McCoy | Barry M. McCoy and William P. Orrick | Analyticity and Integrabiity in the Chiral Potts Model | 31 pages in harvmac including 9 tables, several misprints eliminated | J.Statist.Phys. 83 (1996) 839 | 10.1007/BF02179547 | ITPSB 95-14 | hep-th | null | We study the perturbation theory for the general non-integrable chiral Potts
model depending on two chiral angles and a strength parameter and show how the
analyticity of the ground state energy and correlation functions dramatically
increases when the angles and the strength parameter satisfy the integrability
condi... | [
{
"created": "Fri, 1 Sep 1995 17:53:11 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Sep 1995 15:42:13 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"McCoy",
"Barry M.",
""
],
[
"Orrick",
"William P.",
""
]
] | We study the perturbation theory for the general non-integrable chiral Potts model depending on two chiral angles and a strength parameter and show how the analyticity of the ground state energy and correlation functions dramatically increases when the angles and the strength parameter satisfy the integrability conditi... | 13.702415 | 11.74491 | 16.16663 | 12.36658 | 12.346498 | 12.574492 | 11.897317 | 11.851323 | 11.183779 | 16.80258 | 11.574067 | 12.253712 | 13.959275 | 12.295528 | 12.319496 | 12.313238 | 12.429975 | 12.674541 | 12.441642 | 13.592259 | 11.653674 |
1906.09361 | Chong-Sun Chu | Chong-Sun Chu and Yoji Koyama | Memory Effect in Anti-de Sitter Spacetime | v2: 33 pages, 2 figures. Add comments in introduction section
clarifying our results in comparsion with those of the literature | Phys. Rev. D 100, 104034 (2019) | 10.1103/PhysRevD.100.104034 | NCTS-TH/1903 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The geodesic deviation of a pair of test particles is an natural observable
for the gravitational memory effect. Nevertheless in curved spacetime, this
observable is plagued with various issues that need to be clarified before one
can extract the essential part that is related to the gravitational radiation.
In this ... | [
{
"created": "Sat, 22 Jun 2019 01:20:33 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Sep 2019 14:26:33 GMT",
"version": "v2"
}
] | 2019-11-27 | [
[
"Chu",
"Chong-Sun",
""
],
[
"Koyama",
"Yoji",
""
]
] | The geodesic deviation of a pair of test particles is an natural observable for the gravitational memory effect. Nevertheless in curved spacetime, this observable is plagued with various issues that need to be clarified before one can extract the essential part that is related to the gravitational radiation. In this pa... | 8.677599 | 8.754706 | 8.362027 | 8.451366 | 8.709268 | 8.783724 | 8.89947 | 8.675116 | 7.978706 | 8.711134 | 8.649049 | 8.238181 | 8.381274 | 8.222467 | 8.294111 | 8.435061 | 8.161902 | 8.161473 | 8.153551 | 8.329206 | 8.177729 |
2111.12845 | Yasuaki Hikida | Thomas Creutzig and Yasuaki Hikida | FZZ-triality and large $\mathcal{N}=4$ super Liouville theory | 41 pages, minor modifications, references added, published version | null | 10.1016/j.nuclphysb.2022.115734 | YITP-21-144 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We examine dualities of two dimensional conformal field theories by applying
the methods developed in previous works. We first derive the duality between
$SL(2|1)_k/(SL(2)_k \otimes U(1))$ coset and Witten's cigar model or
sine-Liouville theory. The latter two models are
Fateev-Zamolodchikov-Zamolodchikov (FZZ-)dual ... | [
{
"created": "Wed, 24 Nov 2021 23:36:36 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Mar 2022 02:55:17 GMT",
"version": "v2"
}
] | 2022-04-06 | [
[
"Creutzig",
"Thomas",
""
],
[
"Hikida",
"Yasuaki",
""
]
] | We examine dualities of two dimensional conformal field theories by applying the methods developed in previous works. We first derive the duality between $SL(2|1)_k/(SL(2)_k \otimes U(1))$ coset and Witten's cigar model or sine-Liouville theory. The latter two models are Fateev-Zamolodchikov-Zamolodchikov (FZZ-)dual to... | 6.241972 | 6.347749 | 7.041284 | 5.942322 | 6.470212 | 6.145594 | 6.115241 | 6.162258 | 5.773779 | 7.20804 | 5.879545 | 5.883407 | 6.325495 | 5.983129 | 6.018589 | 5.966388 | 6.010776 | 6.025791 | 6.045322 | 6.529837 | 6.032335 |
hep-th/0310275 | Bodo Geyer | D. M"ulsch and B. Geyer | Cohomological extension of Spin(7)-invariant super Yang-Mills theory in
eight dimensions | 15 pages, Latex | Nucl.Phys. B684 (2004) 351-368 | 10.1016/j.nuclphysb.2004.02.011 | null | hep-th | null | It is shown that the Spin(7)-invariant super Yang-Mills theory in euight
dimensions, which relies on the existence of the Caley invariant, permits the
construction of a cohomological extension, which relies on the existence of the
eight-dimensional analogue of the Pontryagin invariant arising from a quartic
chiral pr... | [
{
"created": "Thu, 30 Oct 2003 08:29:26 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"M\"ulsch",
"D.",
""
],
[
"Geyer",
"B.",
""
]
] | It is shown that the Spin(7)-invariant super Yang-Mills theory in euight dimensions, which relies on the existence of the Caley invariant, permits the construction of a cohomological extension, which relies on the existence of the eight-dimensional analogue of the Pontryagin invariant arising from a quartic chiral prim... | 18.965837 | 19.909149 | 19.787327 | 17.258228 | 18.169104 | 17.44775 | 20.812616 | 19.014877 | 18.327837 | 22.889404 | 17.639351 | 17.432436 | 18.14579 | 16.739519 | 17.769747 | 16.943659 | 17.865234 | 17.258364 | 18.317732 | 17.332079 | 16.575718 |
hep-th/0502039 | Tonguc Rador | Tongu\c{c} Rador | Vibrating Winding Branes, Wrapping Democracy and Stabilization of Extra
Dimensions in Dilaton Gravity | Added a section discussing the linear and non-linear stability of the
equilibrium point of the scale factors of the extra dimensions. Corrected a
typo in the original field equations and other typos. Added and changed
references. Final version appeared in JHEP | JHEP0506:001,2005 | 10.1088/1126-6708/2005/06/001 | null | hep-th gr-qc | null | We show that, in the context of dilaton gravity, a recently proposed
democratic principle for intersection possibilities of branes winding around
extra dimensions yield stabilization, even with the inclusion of momentum modes
of the wrapped branes on top of the winding modes. The constraints for
stabilization massage... | [
{
"created": "Thu, 3 Feb 2005 11:27:19 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Feb 2005 14:15:53 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Jun 2005 12:50:50 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Rador",
"Tonguç",
""
]
] | We show that, in the context of dilaton gravity, a recently proposed democratic principle for intersection possibilities of branes winding around extra dimensions yield stabilization, even with the inclusion of momentum modes of the wrapped branes on top of the winding modes. The constraints for stabilization massaged ... | 32.6534 | 31.51898 | 30.069685 | 27.544098 | 32.056133 | 29.568052 | 29.795389 | 29.790352 | 28.285332 | 34.258568 | 29.110405 | 30.683027 | 29.235302 | 29.593201 | 29.598301 | 29.030144 | 29.988216 | 30.561882 | 29.083334 | 30.519257 | 29.898613 |
hep-th/0608170 | Haji Ahmedov | H. Ahmedov and I. H. Duru | Casimir Energy due to a Semi-Infinite Plane Boundary | 4 pages, Latex | null | null | null | hep-th | null | Following the derivation of the Green function for the massless scalar field
satisfying the Dirichlet boundary condition on the Plane (x > 0, y = 0), we
calculate the Casimir energy.
| [
{
"created": "Thu, 24 Aug 2006 14:11:21 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Aug 2006 11:45:36 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Ahmedov",
"H.",
""
],
[
"Duru",
"I. H.",
""
]
] | Following the derivation of the Green function for the massless scalar field satisfying the Dirichlet boundary condition on the Plane (x > 0, y = 0), we calculate the Casimir energy. | 10.058406 | 8.884128 | 10.230227 | 9.198162 | 10.008798 | 10.151899 | 8.535716 | 8.287773 | 8.3115 | 9.119839 | 9.711405 | 9.409039 | 9.598606 | 9.254045 | 9.180536 | 8.942285 | 8.711528 | 8.775981 | 9.224853 | 9.658266 | 8.9816 |
hep-th/9312012 | null | V. V. Dodonov and V. I. Man'ko | New relations for two-dimensional Hermite polynomials | 17 pages | J.Math.Phys. 35 (1994) 4277-4294 | 10.1063/1.530853 | Naples University INFN-NA-IV-93/33; DSF-T-93/33 | hep-th math.CA | null | The effective formulas reducing the two-dimensional Hermite polynomials to
the classical (one-dimensional) orthogonal polynomials are given. New
one-parameter generating functions for these polynomials are derived.
Asymptotical formulas for large values of indices are found. The applications
to the squeezed one-mode ... | [
{
"created": "Thu, 2 Dec 1993 18:16:31 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dodonov",
"V. V.",
""
],
[
"Man'ko",
"V. I.",
""
]
] | The effective formulas reducing the two-dimensional Hermite polynomials to the classical (one-dimensional) orthogonal polynomials are given. New one-parameter generating functions for these polynomials are derived. Asymptotical formulas for large values of indices are found. The applications to the squeezed one-mode st... | 11.525943 | 12.72039 | 13.170728 | 10.04145 | 11.30611 | 12.599599 | 12.579965 | 10.975229 | 10.032751 | 13.294782 | 10.979318 | 11.166823 | 11.530907 | 10.851327 | 10.880816 | 10.861124 | 11.278517 | 11.200113 | 10.702103 | 11.609139 | 11.032872 |
hep-th/0002105 | Cesar D. Fosco | I. J. R. Aitchison and C. D. Fosco | On the chiral and deconfinement phase transitions in parity-conserving
QED_3 at finite temperature | 1 reference added | Nucl.Phys. B578 (2000) 199-214 | 10.1016/S0550-3213(00)00197-8 | null | hep-th | null | We present some results about the interplay between the chiral and
deconfinement phase transitions in parity-conserving QED3 (with N flavours of
massless 4 component fermions) at finite temperature. Following Grignani et al
(Phys. Rev. D53, 7157 (1996), Nucl. Phys. B473, 143 (1996)), confinement is
discussed in terms... | [
{
"created": "Sun, 13 Feb 2000 22:32:12 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Feb 2000 19:31:18 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Aitchison",
"I. J. R.",
""
],
[
"Fosco",
"C. D.",
""
]
] | We present some results about the interplay between the chiral and deconfinement phase transitions in parity-conserving QED3 (with N flavours of massless 4 component fermions) at finite temperature. Following Grignani et al (Phys. Rev. D53, 7157 (1996), Nucl. Phys. B473, 143 (1996)), confinement is discussed in terms o... | 8.706388 | 9.526391 | 9.195255 | 8.642128 | 9.838868 | 9.031392 | 9.57644 | 8.592402 | 8.558718 | 10.398333 | 8.619761 | 8.635875 | 8.652166 | 8.38695 | 8.493396 | 8.536552 | 8.755095 | 8.608259 | 8.495733 | 8.5207 | 8.541011 |
1401.1833 | Robert Finkelstein J | Robert J. Finkelstein | The Preon Sector of the SLq(2) Model and the Binding Problem | arXiv admin note: text overlap with arXiv:1301.6440 | null | 10.1142/S0217751X14500924 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There are suggestive experimental indications that the leptons, neutrinos,
and quarks are composite and that their structure is described by the quantum
group SLq(2). Since the hypothetical preons must be very heavy relative to the
masses of the leptons, neutrinos, and quarks, there must be a very strong
binding fiel... | [
{
"created": "Wed, 8 Jan 2014 21:28:20 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Finkelstein",
"Robert J.",
""
]
] | There are suggestive experimental indications that the leptons, neutrinos, and quarks are composite and that their structure is described by the quantum group SLq(2). Since the hypothetical preons must be very heavy relative to the masses of the leptons, neutrinos, and quarks, there must be a very strong binding field ... | 10.615388 | 11.047997 | 11.127951 | 10.703691 | 10.824057 | 11.182761 | 10.695165 | 10.86852 | 10.667265 | 12.512735 | 10.672151 | 10.118547 | 10.620864 | 10.24166 | 10.51239 | 10.224881 | 10.186748 | 10.55876 | 10.185652 | 10.737944 | 10.181136 |
hep-th/9308043 | null | Bergfinnur Durhuus and Thordur Jonsson | Classification and construction of unitary topological field theories in
two dimensions | 12 pages, latex | J.Math.Phys. 35 (1994) 5306-5313 | 10.1063/1.530752 | null | hep-th | null | We prove that unitary two-dimensional topological field theories are uniquely
characterized by $n$ positive real numbers $\lambda _1,\ldots \lambda _n$ which
can be regarded as the eigenvalues of a hermitean handle creation operator. The
number $n$ is the dimension of the Hilbert space associated with the circle and
... | [
{
"created": "Mon, 9 Aug 1993 18:10:05 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Durhuus",
"Bergfinnur",
""
],
[
"Jonsson",
"Thordur",
""
]
] | We prove that unitary two-dimensional topological field theories are uniquely characterized by $n$ positive real numbers $\lambda _1,\ldots \lambda _n$ which can be regarded as the eigenvalues of a hermitean handle creation operator. The number $n$ is the dimension of the Hilbert space associated with the circle and th... | 6.743734 | 6.886005 | 7.58314 | 6.921394 | 7.404283 | 6.739234 | 6.990653 | 6.561654 | 6.70907 | 8.543271 | 6.429261 | 6.31041 | 6.840516 | 6.56331 | 6.667925 | 6.601822 | 6.502528 | 6.768851 | 6.702516 | 7.032383 | 6.338695 |
hep-th/9810101 | Mikhail Plyushchay | Mikhail Plyushchay | Comment on "The relativistic particle with curvature and torsion of
world trajectory" | 5 pages, LaTeX | null | null | null | hep-th | null | Gogilidze and Surovtsev have claimed recently (hep-th/9809191) that the
tachyonic sector can be removed from the spectrum of the relativistic particle
with curvature and torsion by a proper gauge choice. We show that the mass-spin
dependence obtained by them is incorrect and point out that their gauge surface
does no... | [
{
"created": "Wed, 14 Oct 1998 15:01:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Plyushchay",
"Mikhail",
""
]
] | Gogilidze and Surovtsev have claimed recently (hep-th/9809191) that the tachyonic sector can be removed from the spectrum of the relativistic particle with curvature and torsion by a proper gauge choice. We show that the mass-spin dependence obtained by them is incorrect and point out that their gauge surface does not ... | 13.069856 | 9.412641 | 10.442198 | 9.879793 | 10.397899 | 9.810877 | 10.958548 | 10.51845 | 10.520642 | 12.709464 | 10.10252 | 9.235207 | 9.984634 | 9.470016 | 8.785857 | 9.179162 | 9.521496 | 9.107221 | 9.32584 | 9.880486 | 9.367895 |
hep-th/0504006 | Muraari Vasudevan | Terry Gannon and Muraari Vasudevan | Charges of Exceptionally Twisted Branes | 19 pages, 2 figures, LaTex2e, complete proofs of all statements,
updated bibliography | JHEP0507:035,2005 | 10.1088/1126-6708/2005/07/035 | Alberta Thy 05-05 | hep-th | null | The charges of the exceptionally twisted (D4 with triality and E6 with charge
conjugation) D-branes of WZW models are determined from the microscopic/CFT
point of view. The branes are labeled by twisted representations of the affine
algebra, and their charge is determined to be the ground state multiplicity of
the tw... | [
{
"created": "Fri, 1 Apr 2005 11:03:29 GMT",
"version": "v1"
},
{
"created": "Tue, 3 May 2005 18:12:39 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Jun 2005 18:21:50 GMT",
"version": "v3"
},
{
"created": "Wed, 22 Jun 2005 09:30:12 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Gannon",
"Terry",
""
],
[
"Vasudevan",
"Muraari",
""
]
] | The charges of the exceptionally twisted (D4 with triality and E6 with charge conjugation) D-branes of WZW models are determined from the microscopic/CFT point of view. The branes are labeled by twisted representations of the affine algebra, and their charge is determined to be the ground state multiplicity of the twis... | 14.273476 | 13.712533 | 14.710218 | 11.867331 | 13.307993 | 13.425817 | 13.822813 | 12.895957 | 11.486872 | 16.231853 | 12.60817 | 12.997811 | 13.885294 | 12.716075 | 13.027204 | 13.211808 | 12.860676 | 12.47198 | 12.953056 | 14.363189 | 13.243595 |
hep-th/9210021 | null | Xenia C. de la Ossa and Fernando Quevedo | Duality Symmetries from Non--Abelian Isometries in String Theories | 18 pages, preprint NEIPH92-004, to be published in Nuclear Physics B.
(corrected minor typos and references, other minor changes) | Nucl.Phys. B403 (1993) 377-394 | 10.1016/0550-3213(93)90041-M | null | hep-th gr-qc | null | In string theory it is known that abelian isometries in the sigma model lead
to target space duality. We generalize this duality to backgrounds with
non--abelian isometries. The procedure we follow consists of gauging the
isometries of the original action and constraining the field strength $F$ to
vanish. This new ac... | [
{
"created": "Mon, 5 Oct 1992 14:08:30 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Feb 1993 13:06:34 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"de la Ossa",
"Xenia C.",
""
],
[
"Quevedo",
"Fernando",
""
]
] | In string theory it is known that abelian isometries in the sigma model lead to target space duality. We generalize this duality to backgrounds with non--abelian isometries. The procedure we follow consists of gauging the isometries of the original action and constraining the field strength $F$ to vanish. This new acti... | 6.954678 | 6.826173 | 6.842352 | 6.574876 | 6.594778 | 6.571524 | 6.69884 | 6.535468 | 6.62515 | 7.723256 | 6.561887 | 6.679377 | 6.812807 | 6.680154 | 6.499314 | 6.709117 | 6.811475 | 6.753417 | 6.701155 | 6.8779 | 6.697891 |
hep-th/0411228 | J. M. C. Malbouisson | H. Queiroz, J. C. da Silva, F. C. Khanna, J. M. C. Malbouisson, M.
Revzen, A. E. Santana | Thermofield Dynamics and Casimir Effect for Fermions | 21 pages, 3 figures, to appear in Annals of Physics | Annals Phys. 317 (2005) 220-237; Erratum-ibid. 321 (2006)
1274-1275 | 10.1016/j.aop.2004.11.011 | null | hep-th | null | A generalization of the Bogoliubov transformation is developed to describe a
space compactified fermionic field. The method is the fermionic counterpart of
the formalism introduced earlier for bosons (J. C. da Silva, A. Matos Neto, F.
C. Khanna and A. E. Santana, Phys. Rev. A 66 (2002) 052101), and is based on
the th... | [
{
"created": "Wed, 24 Nov 2004 23:01:21 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Queiroz",
"H.",
""
],
[
"da Silva",
"J. C.",
""
],
[
"Khanna",
"F. C.",
""
],
[
"Malbouisson",
"J. M. C.",
""
],
[
"Revzen",
"M.",
""
],
[
"Santana",
"A. E.",
""
]
] | A generalization of the Bogoliubov transformation is developed to describe a space compactified fermionic field. The method is the fermionic counterpart of the formalism introduced earlier for bosons (J. C. da Silva, A. Matos Neto, F. C. Khanna and A. E. Santana, Phys. Rev. A 66 (2002) 052101), and is based on the ther... | 7.170714 | 8.293466 | 8.40761 | 7.732244 | 7.787481 | 8.932083 | 8.519853 | 8.414942 | 8.022047 | 8.679992 | 7.683817 | 7.392154 | 7.475099 | 6.987391 | 6.989995 | 7.012379 | 7.061036 | 7.296187 | 7.076621 | 7.360689 | 7.151846 |
hep-th/0001053 | Hirosi Ooguri | Juan Maldacena and Hirosi Ooguri | Strings in AdS_3 and the SL(2,R) WZW Model. Part 1: The Spectrum | 44 pages, 7 figures, LaTeX; minor changes, references added | J.Math.Phys.42:2929-2960,2001 | 10.1063/1.1377273 | CALT-68-2245, CITUSC/99-010, HUTP-99/A027, LBNL-44375, UCB-PTH-99/48 | hep-th | null | In this paper we study the spectrum of bosonic string theory on AdS_3. We
study classical solutions of the SL(2,R) WZW model, including solutions for
long strings with non-zero winding number. We show that the model has a
symmetry relating string configurations with different winding numbers. We then
study the Hilber... | [
{
"created": "Mon, 10 Jan 2000 19:32:52 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jan 2000 00:46:35 GMT",
"version": "v2"
},
{
"created": "Fri, 19 May 2000 19:09:17 GMT",
"version": "v3"
}
] | 2009-09-17 | [
[
"Maldacena",
"Juan",
""
],
[
"Ooguri",
"Hirosi",
""
]
] | In this paper we study the spectrum of bosonic string theory on AdS_3. We study classical solutions of the SL(2,R) WZW model, including solutions for long strings with non-zero winding number. We show that the model has a symmetry relating string configurations with different winding numbers. We then study the Hilbert ... | 8.277282 | 7.528594 | 8.815434 | 7.196981 | 7.421371 | 7.520323 | 7.58598 | 7.114042 | 7.379068 | 8.570468 | 7.386946 | 7.351684 | 8.198709 | 7.560246 | 7.658764 | 7.589653 | 7.162302 | 7.35611 | 7.578068 | 7.843342 | 7.520456 |
1912.05188 | Cheng-Yang Lee | Cheng-Yang Lee | Spin-half mass dimension one fermions and their higher-spin
generalizations | 24 pages, submitted to the EPJ Special Topic on Elko and mass
dimension one fermions | null | 10.1140/epjst/e2020-900277-x | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A self-contained review on spin-half mass dimension one fermions and their
higher-spin generalizations is presented. Starting from the two-component
left-handed Weyl spinors, the Dirac spinors and Elko (eigenspinors of the
charge conjugation operator) are constructed. After elaborating on their
similarities and diffe... | [
{
"created": "Wed, 11 Dec 2019 09:07:57 GMT",
"version": "v1"
}
] | 2020-10-28 | [
[
"Lee",
"Cheng-Yang",
""
]
] | A self-contained review on spin-half mass dimension one fermions and their higher-spin generalizations is presented. Starting from the two-component left-handed Weyl spinors, the Dirac spinors and Elko (eigenspinors of the charge conjugation operator) are constructed. After elaborating on their similarities and differe... | 7.752668 | 7.573683 | 8.419313 | 7.254623 | 7.105517 | 7.543131 | 6.743728 | 7.04724 | 7.398517 | 8.152564 | 7.514501 | 7.355806 | 7.76486 | 7.59323 | 7.541068 | 7.532531 | 7.608618 | 7.586212 | 7.358756 | 7.838657 | 7.720474 |
hep-th/0402018 | Yun Soo Myung | Hungsoo Kim, Gil Sang Lee, Yun Soo Myung | Noncommutative spacetime effect on the slow-roll period of inflation | 13 pages | Mod.Phys.Lett. A20 (2005) 271-284 | 10.1142/S0217732305016518 | INJE-TP-04-01 | hep-th astro-ph | null | We study how the noncommutative spacetime affects on inflation. First we
obtain the noncommutative power spectrum of the curvature perturbations
produced during inflation in the slow-roll approximation. This is the explicit
$k$-dependent power spectrum up to first order in slow-roll parameters
$\epsilon_1 \delta_1$ i... | [
{
"created": "Tue, 3 Feb 2004 03:16:13 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Kim",
"Hungsoo",
""
],
[
"Lee",
"Gil Sang",
""
],
[
"Myung",
"Yun Soo",
""
]
] | We study how the noncommutative spacetime affects on inflation. First we obtain the noncommutative power spectrum of the curvature perturbations produced during inflation in the slow-roll approximation. This is the explicit $k$-dependent power spectrum up to first order in slow-roll parameters $\epsilon_1 \delta_1$ inc... | 7.830733 | 7.413961 | 7.68243 | 7.362935 | 8.666594 | 7.291051 | 7.709454 | 7.401139 | 7.154303 | 8.254282 | 6.976268 | 7.103307 | 7.668146 | 7.229169 | 7.337011 | 7.352357 | 7.153617 | 7.121392 | 7.385541 | 7.587945 | 7.127849 |
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