id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9111011 | Thordur Jonsson | Thordur Jonsson | Intrinsic and extrinsic geometry of random surfaces | 9 pages | Phys.Lett. B278 (1992) 89-93 | 10.1016/0370-2693(92)90716-H | null | hep-th | null | We prove that the extrinsic Hausdorff dimension is always greater than or
equal to the intrinsic Hausdorff dimension in models of triangulated random
surfaces with action which is quadratic in the separation of vertices. We
furthermore derive a few naive scaling relations which relate the intrinsic
Hausdorff dimensio... | [
{
"created": "Tue, 5 Nov 1991 09:01:35 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Jonsson",
"Thordur",
""
]
] | We prove that the extrinsic Hausdorff dimension is always greater than or equal to the intrinsic Hausdorff dimension in models of triangulated random surfaces with action which is quadratic in the separation of vertices. We furthermore derive a few naive scaling relations which relate the intrinsic Hausdorff dimension ... | 8.659559 | 7.128525 | 8.846575 | 7.62841 | 7.325154 | 7.459184 | 7.78975 | 7.403608 | 7.762452 | 9.140186 | 7.283419 | 7.544909 | 8.036127 | 7.746718 | 7.754818 | 7.514289 | 7.657715 | 7.720139 | 7.515781 | 8.056158 | 7.418376 |
hep-th/0406122 | Vadim Kaplunovsky | Edoardo Di Napoli, Vadim S. Kaplunovsky, Jacob Sonnenschein | Chiral Rings of Deconstructive [SU(n_c)]^N Quivers | 93 pages, LaTeX, PSTricks macros; 1 reference added in v2 | JHEP 0406 (2004) 060 | 10.1088/1126-6708/2004/06/060 | UTTG-03-04, TAUP-2772-04 | hep-th | null | Dimensional deconstruction of 5D SQCD with general n_c, n_f and k_CS gives
rise to 4D N=1 gauge theories with large quivers of SU(n_c) gauge factors. We
construct the chiral rings of such [SU(n_c)]^N theories, off-shell and
on-shell. Our results are broadly similar to the chiral rings of single U(n_c)
theories with b... | [
{
"created": "Tue, 15 Jun 2004 14:04:24 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Sep 2004 22:35:22 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Di Napoli",
"Edoardo",
""
],
[
"Kaplunovsky",
"Vadim S.",
""
],
[
"Sonnenschein",
"Jacob",
""
]
] | Dimensional deconstruction of 5D SQCD with general n_c, n_f and k_CS gives rise to 4D N=1 gauge theories with large quivers of SU(n_c) gauge factors. We construct the chiral rings of such [SU(n_c)]^N theories, off-shell and on-shell. Our results are broadly similar to the chiral rings of single U(n_c) theories with bot... | 9.517928 | 9.150616 | 9.916248 | 8.592059 | 9.142528 | 9.158279 | 8.81135 | 8.370373 | 8.532598 | 10.615509 | 8.576287 | 9.182216 | 9.005935 | 8.537642 | 8.712015 | 8.789887 | 8.699018 | 8.918445 | 8.76246 | 9.046824 | 9.000979 |
hep-th/0407184 | Sugumi Kanno | Sugumi Kanno, Jiro Soda | A Unified View of RS Braneworlds | 10 pages, to appear in QG issue of TSPU Vestnik | TSPU Vestnik 44N7 (2004) 15-24 | null | KUNS-1930 | hep-th gr-qc | null | There are various different descriptions of Randall-Sundrum (RS) braneworlds.
Here we present a unified view of the braneworld based on the gradient
expansion approach. In the case of the single-brane model, we reveal the
relation between the geometrical and the AdS/CFT approach. It turns out that
the high energy and... | [
{
"created": "Wed, 21 Jul 2004 10:13:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kanno",
"Sugumi",
""
],
[
"Soda",
"Jiro",
""
]
] | There are various different descriptions of Randall-Sundrum (RS) braneworlds. Here we present a unified view of the braneworld based on the gradient expansion approach. In the case of the single-brane model, we reveal the relation between the geometrical and the AdS/CFT approach. It turns out that the high energy and t... | 7.939495 | 6.593446 | 6.799044 | 6.47077 | 6.310428 | 6.563724 | 6.526083 | 6.029186 | 6.533886 | 7.041218 | 6.716159 | 6.594953 | 6.839658 | 6.647116 | 6.676484 | 6.873094 | 6.848463 | 6.858174 | 6.873592 | 7.094887 | 6.710272 |
hep-th/0511112 | Archil Kobakhidze | R. Holman and L. Mersini-Houghton | A Fly in the SOUP | 5 pages | Phys.Rev. D74 (2006) 043511 | 10.1103/PhysRevD.74.043511 | null | hep-th astro-ph gr-qc hep-ph | null | We investigate the Selection of Original Universe Proposal (SOUP) of Tye et
al. and show that as it stands, this proposal is flawed. The corrections to the
Euclidean gravity action that were to select a Universe with a sufficiently
large value of the cosmological constant $\Lambda$ to allow for an inflationary
phase,... | [
{
"created": "Wed, 9 Nov 2005 18:58:54 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Holman",
"R.",
""
],
[
"Mersini-Houghton",
"L.",
""
]
] | We investigate the Selection of Original Universe Proposal (SOUP) of Tye et al. and show that as it stands, this proposal is flawed. The corrections to the Euclidean gravity action that were to select a Universe with a sufficiently large value of the cosmological constant $\Lambda$ to allow for an inflationary phase, o... | 12.106641 | 11.164291 | 10.646206 | 10.079664 | 12.096767 | 11.549426 | 11.144894 | 10.35333 | 11.234238 | 12.319167 | 11.15403 | 10.381865 | 10.75085 | 10.521852 | 11.229092 | 10.533538 | 10.301682 | 10.655165 | 10.527861 | 10.875892 | 10.884693 |
hep-th/0611129 | Zbigniew Hasiewicz | Marcin Daszkiewicz (IFT UWr), Zbigniew Hasiewicz (IFT UwB), Tomasz
Nikiciuk (IFT UwB), Cezary J. Walczyk (IFT UwB) | High spin particles with spin-mass coupling II | 12 pages, 1 figure, the paper accepted for publication in Advances in
Applied Clifford Algebra | Adv.Appl.CliffordAlgebras18:43-56,2008 | 10.1007/s00006-007-0062-7 | IFT UwB 03/2006 | hep-th | null | The classical and quantum model of high spin particles with spin-mass
coupling is presented in this paper. The mass spectrum of the model is
symmetric with respect to particle-antiparticle exchange. The quantum model
contains elementary particles and the cluster states generating infinite
degeneracy of the mass spect... | [
{
"created": "Sat, 11 Nov 2006 11:17:49 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Aug 2007 08:36:55 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Daszkiewicz",
"Marcin",
"",
"IFT UWr"
],
[
"Hasiewicz",
"Zbigniew",
"",
"IFT UwB"
],
[
"Nikiciuk",
"Tomasz",
"",
"IFT UwB"
],
[
"Walczyk",
"Cezary J.",
"",
"IFT UwB"
]
] | The classical and quantum model of high spin particles with spin-mass coupling is presented in this paper. The mass spectrum of the model is symmetric with respect to particle-antiparticle exchange. The quantum model contains elementary particles and the cluster states generating infinite degeneracy of the mass spectru... | 16.489113 | 10.702756 | 14.252751 | 12.265517 | 13.310079 | 13.896551 | 12.237132 | 12.069224 | 12.357718 | 12.736128 | 12.434406 | 12.903191 | 13.507367 | 12.975945 | 13.311452 | 13.488672 | 13.121789 | 13.016148 | 12.731555 | 13.633214 | 12.504793 |
0904.4556 | Sarben Sarkar | Sarben Sarkar | The Omega Effect for Neutral Mesons | Accepted for publication in Journal of Physics: Conference Series,
Discrete '08, Symposium on Prospects in the Physics of Discrete Symmetries,
Valencia, December 2008 | J.Phys.Conf.Ser.171:012040,2009 | 10.1088/1742-6596/171/1/012040 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The possible role of decoherence due to space-time foam is discussed within
the context of two models, one based on string/brane theory. and the other
based on properties of black hole horizons in general relativity. It is argued
that the density matrix satisfies a dissipative master equation, primarily from
the stud... | [
{
"created": "Wed, 29 Apr 2009 08:56:29 GMT",
"version": "v1"
}
] | 2009-08-03 | [
[
"Sarkar",
"Sarben",
""
]
] | The possible role of decoherence due to space-time foam is discussed within the context of two models, one based on string/brane theory. and the other based on properties of black hole horizons in general relativity. It is argued that the density matrix satisfies a dissipative master equation, primarily from the study ... | 12.433057 | 13.268968 | 11.011079 | 11.809981 | 12.316198 | 13.411365 | 12.800159 | 12.089499 | 11.506292 | 12.592985 | 12.455532 | 12.412407 | 12.115176 | 12.072341 | 12.07104 | 12.026236 | 12.312282 | 12.421464 | 12.249032 | 12.304599 | 12.247873 |
1510.08926 | Henning Samtleben | A. Baguet, C.N. Pope, H. Samtleben | Consistent Pauli reduction on group manifolds | 16 pages | null | 10.1016/j.physletb.2015.11.062 | MI-TH-1536 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove an old conjecture by Duff, Nilsson, Pope and Warner asserting that
the NS-NS sector of supergravity (and more general the bosonic string) allows
for a consistent Pauli reduction on any d-dimensional group manifold G, keeping
the full set of gauge bosons of the G x G isometry group of the bi-invariant
metric ... | [
{
"created": "Thu, 29 Oct 2015 22:10:43 GMT",
"version": "v1"
}
] | 2015-12-02 | [
[
"Baguet",
"A.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Samtleben",
"H.",
""
]
] | We prove an old conjecture by Duff, Nilsson, Pope and Warner asserting that the NS-NS sector of supergravity (and more general the bosonic string) allows for a consistent Pauli reduction on any d-dimensional group manifold G, keeping the full set of gauge bosons of the G x G isometry group of the bi-invariant metric on... | 13.973288 | 10.77343 | 14.656667 | 11.303102 | 11.395192 | 11.052367 | 10.860632 | 10.716725 | 11.749228 | 17.662128 | 10.988764 | 12.181643 | 12.512673 | 11.106569 | 11.63468 | 11.456638 | 11.200332 | 10.912459 | 11.505684 | 12.322201 | 11.363819 |
hep-th/9406024 | null | F. Illuminati, M. Patriarca, and P. Sodano | Classical and quantum dissipation in non homogeneous environments | 17 pages, plain LaTeX [12pt,A4wide], DFPD 94/TH/24 | Physica A211 (1994) 449 | 10.1016/0378-4371(94)00171-5 | null | hep-th cond-mat | null | We generalize the oscillator model of a particle interacting with a thermal
reservoir by introducing arbitrary nonlinear couplings in the particle
coordinates.The equilibrium positions of the heat bath oscillators are promoted
to space-time functions, which are shown to represent a modulation of the
internal noise by... | [
{
"created": "Sat, 4 Jun 1994 19:40:00 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Illuminati",
"F.",
""
],
[
"Patriarca",
"M.",
""
],
[
"Sodano",
"P.",
""
]
] | We generalize the oscillator model of a particle interacting with a thermal reservoir by introducing arbitrary nonlinear couplings in the particle coordinates.The equilibrium positions of the heat bath oscillators are promoted to space-time functions, which are shown to represent a modulation of the internal noise by t... | 12.926582 | 14.750711 | 13.522163 | 13.062861 | 14.152106 | 14.397447 | 13.82203 | 13.276188 | 13.307564 | 14.193514 | 13.347561 | 13.365715 | 13.274496 | 12.931787 | 13.58418 | 13.108552 | 13.169644 | 13.055037 | 12.655708 | 12.919419 | 12.877081 |
2407.08793 | Alek Bedroya | Alek Bedroya, Qianshu Lu, Paul Steinhardt | TCC in the interior of moduli space and its implications for the string
landscape and cosmology | 35 pages, 11 figures | null | null | null | hep-th astro-ph.CO gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We consider the classical Friedmann-Robertson-Walker solutions that describe
a universe undergoing a transition from an accelerating expansion phase in the
past to an eternal decelerating expansion phase in the future, driven by a
scalar field evolving in a potential energy landscape. We show that any
solution for wh... | [
{
"created": "Thu, 11 Jul 2024 18:08:05 GMT",
"version": "v1"
}
] | 2024-07-15 | [
[
"Bedroya",
"Alek",
""
],
[
"Lu",
"Qianshu",
""
],
[
"Steinhardt",
"Paul",
""
]
] | We consider the classical Friedmann-Robertson-Walker solutions that describe a universe undergoing a transition from an accelerating expansion phase in the past to an eternal decelerating expansion phase in the future, driven by a scalar field evolving in a potential energy landscape. We show that any solution for whic... | 12.057507 | 11.153974 | 11.654455 | 10.85944 | 12.050437 | 11.503588 | 12.135853 | 11.416031 | 11.732992 | 12.666389 | 10.961003 | 11.541758 | 11.612512 | 11.287189 | 11.652707 | 11.762834 | 11.341269 | 10.867744 | 11.472306 | 12.017629 | 11.606213 |
1803.04414 | Sebastian Fischetti | Sebastian Fischetti, Lucas Wallis, and Toby Wiseman | What spatial geometry does the (2+1)-dimensional QFT vacuum prefer? | 5+2 pages; v2: addressed referee comments, fixed table 1 | Phys. Rev. Lett. 120, 261601 (2018) | 10.1103/PhysRevLett.120.261601 | null | hep-th cond-mat.mtrl-sci cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider relativistic (2+1)-QFTs on a product of time with a two-space and
study the vacuum free energy as a functional of the temperature and spatial
geometry. We focus on free scalar and Dirac fields on arbitrary perturbations
of flat space, finding that the free energy difference from flat space is
finite and a... | [
{
"created": "Mon, 12 Mar 2018 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 29 May 2019 16:00:18 GMT",
"version": "v2"
}
] | 2019-05-30 | [
[
"Fischetti",
"Sebastian",
""
],
[
"Wallis",
"Lucas",
""
],
[
"Wiseman",
"Toby",
""
]
] | We consider relativistic (2+1)-QFTs on a product of time with a two-space and study the vacuum free energy as a functional of the temperature and spatial geometry. We focus on free scalar and Dirac fields on arbitrary perturbations of flat space, finding that the free energy difference from flat space is finite and alw... | 10.475721 | 10.766281 | 11.440299 | 9.764983 | 10.498153 | 10.713543 | 11.349844 | 10.260502 | 9.821991 | 12.295581 | 10.192059 | 10.149061 | 10.293653 | 9.857986 | 10.007378 | 10.290072 | 10.167615 | 10.063772 | 9.979286 | 10.438058 | 10.081914 |
1012.2734 | Yun-Song Piao | Yun-Song Piao | Adiabatic Spectra During Slowly Evolving | 3 pages, 1 figure, arguments, discussions and Refs. added, to publish
in PLB | null | 10.1016/j.physletb.2011.06.047 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In general, for single field, the scale invariant spectrum of curvature
perturbation can be given by either its constant mode or its increasing mode.
We show that during slowly expanding or contracting, the spectrum of curvature
perturbation given by its increasing mode can be scale invariance. The
perturbation mode ... | [
{
"created": "Mon, 13 Dec 2010 14:25:49 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jun 2011 09:42:55 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Piao",
"Yun-Song",
""
]
] | In general, for single field, the scale invariant spectrum of curvature perturbation can be given by either its constant mode or its increasing mode. We show that during slowly expanding or contracting, the spectrum of curvature perturbation given by its increasing mode can be scale invariance. The perturbation mode ca... | 14.467729 | 11.31074 | 11.597947 | 10.319767 | 11.168256 | 11.555372 | 13.635525 | 11.664204 | 11.722918 | 11.779056 | 11.881137 | 12.832378 | 11.600256 | 11.591346 | 12.042171 | 12.06423 | 12.310142 | 11.546753 | 12.103111 | 11.80257 | 12.064418 |
2406.13461 | Di Wu | Wentao Liu, Di Wu, Jieci Wang | Static neutral black holes in Kalb-Ramond gravity | 22 pages, 2 figures, 1 table, JHEP3.cls | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Kalb-Ramond (KR) gravity theory, a modified gravity theory that
nonminimally couples a KR field with a nonzero vacuum expectation value for the
gravitational field, can spontaneously break the Lorentz symmetry of gravity.
In a recent work, Yang et al. [Phys. Rev. D 108, 124004 (2023)] successfully
derived Schwarz... | [
{
"created": "Wed, 19 Jun 2024 11:38:05 GMT",
"version": "v1"
}
] | 2024-06-21 | [
[
"Liu",
"Wentao",
""
],
[
"Wu",
"Di",
""
],
[
"Wang",
"Jieci",
""
]
] | The Kalb-Ramond (KR) gravity theory, a modified gravity theory that nonminimally couples a KR field with a nonzero vacuum expectation value for the gravitational field, can spontaneously break the Lorentz symmetry of gravity. In a recent work, Yang et al. [Phys. Rev. D 108, 124004 (2023)] successfully derived Schwarzsc... | 5.434484 | 5.068494 | 4.790864 | 4.76716 | 5.052904 | 5.308894 | 5.162715 | 4.66719 | 5.038054 | 5.298899 | 4.943305 | 5.096721 | 4.901528 | 4.946494 | 4.948354 | 5.123371 | 5.075943 | 4.952261 | 5.100991 | 5.010314 | 5.078119 |
hep-th/9706023 | Kimyeong Lee | Kimyeong Lee, Piljin Yi | A Family of N=2 Gauge Theories with Exact S-Duality | 28 pages, Latex, a single figure, minor corrections in text and
references | Nucl.Phys. B520 (1998) 157-178 | 10.1016/S0550-3213(98)00078-9 | CU-TP-842 | hep-th | null | We study an infinite family of N=2 $Sp(2n)$ gauge theories that naturally
arise from the D3-brane probe dynamics in F-theory. The matter sector consists
of four fundamental and one antisymmetric tensor hyper multiplets. We propose
that, in the limit of vanishing bare masses, the theory has exact
$SO(8)\sdtimes SL(2,Z... | [
{
"created": "Tue, 3 Jun 1997 21:59:11 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Jun 1997 20:51:36 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Lee",
"Kimyeong",
""
],
[
"Yi",
"Piljin",
""
]
] | We study an infinite family of N=2 $Sp(2n)$ gauge theories that naturally arise from the D3-brane probe dynamics in F-theory. The matter sector consists of four fundamental and one antisymmetric tensor hyper multiplets. We propose that, in the limit of vanishing bare masses, the theory has exact $SO(8)\sdtimes SL(2,Z)$... | 9.958822 | 11.272608 | 12.165451 | 9.202552 | 8.375858 | 9.163822 | 9.207406 | 9.800373 | 8.858974 | 12.857045 | 8.951839 | 8.978057 | 9.793487 | 8.561988 | 9.154158 | 8.481303 | 8.878199 | 8.65799 | 9.124643 | 10.291471 | 8.788424 |
hep-th/9712061 | Gleb E. Arutyunov | G.E.Arutyunov and S.A.Frolov | Four graviton scattering amplitude from $S^N\large{{\bf R}}^{8}$
supersymmetric orbifold sigma model | latex, 35 pages, misprints are corrected, the final version to appear
in Nucl.Phys.B | Nucl.Phys. B524 (1998) 159-206 | 10.1016/S0550-3213(98)00326-5 | null | hep-th | null | In the IR limit the Matrix string theory is expected to be described by the
$S^N\R^{8}$ supersymmetric orbifold sigma model. Recently Dijkgraaf, Verlinde
and Verlinde proposed a vertex that may describe the type IIA string
interaction. In this paper using this interaction vertex we derive the four
graviton scattering... | [
{
"created": "Fri, 5 Dec 1997 17:31:56 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Apr 1998 10:00:57 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Arutyunov",
"G. E.",
""
],
[
"Frolov",
"S. A.",
""
]
] | In the IR limit the Matrix string theory is expected to be described by the $S^N\R^{8}$ supersymmetric orbifold sigma model. Recently Dijkgraaf, Verlinde and Verlinde proposed a vertex that may describe the type IIA string interaction. In this paper using this interaction vertex we derive the four graviton scattering a... | 13.232224 | 7.832302 | 12.478431 | 8.516602 | 7.919345 | 8.322867 | 7.902877 | 8.188801 | 7.513182 | 13.670218 | 8.352747 | 8.614722 | 10.506176 | 9.023378 | 8.718456 | 8.880607 | 8.57693 | 8.365634 | 8.634144 | 10.837941 | 8.946466 |
1302.7136 | Shahin Rouhani | Malte Henkel and Shahin Rouhani | Logarithmic correlators or responses in non-relativistic analogues of
conformal invariance | 29 pages, 3 figures | J. Phys. A: Math. Theor. 46, 494004 (2013) | 10.1088/1751-8113/46/49/494004 | null | hep-th cond-mat.stat-mech math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent developments on emergence of logarithmic terms in correlators or
response functions of models which exhibit dynamical symmetries analogous to
conformal invariance in not necessarily relativistic systems are reviewed. The
main examples of these are logarithmic Schr\"odinger-invariance and logarithmic
conformal ... | [
{
"created": "Thu, 28 Feb 2013 10:11:19 GMT",
"version": "v1"
}
] | 2013-11-22 | [
[
"Henkel",
"Malte",
""
],
[
"Rouhani",
"Shahin",
""
]
] | Recent developments on emergence of logarithmic terms in correlators or response functions of models which exhibit dynamical symmetries analogous to conformal invariance in not necessarily relativistic systems are reviewed. The main examples of these are logarithmic Schr\"odinger-invariance and logarithmic conformal Ga... | 10.551034 | 10.901979 | 12.311334 | 9.662151 | 10.84559 | 10.566884 | 9.285931 | 9.871425 | 9.200165 | 13.733411 | 9.125748 | 9.426478 | 9.841595 | 9.226152 | 9.038052 | 8.983912 | 8.83609 | 9.162715 | 9.206359 | 9.404782 | 8.808426 |
1107.0380 | Davoud Kamani | Zahra Rezaei and Davoud Kamani | Moving Branes with Background Massless and Tachyon Fields in the Compact
Spacetime | 13 pages, Latex, no figure | Braz. J. Phys. 41, 177 (2011) | 10.1007/s13538-011-0030-5 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we shall obtain the boundary state associated with a moving
$Dp$-brane in the presence of the Kalb-Ramond field $B_{\mu\nu}$, an internal
U(1) gauge field $A_{\alpha}$ and a tachyon field, in the compact spacetime.
According to this state, properties of the brane and a closed string, with
mixed bounda... | [
{
"created": "Sat, 2 Jul 2011 13:34:13 GMT",
"version": "v1"
}
] | 2020-08-21 | [
[
"Rezaei",
"Zahra",
""
],
[
"Kamani",
"Davoud",
""
]
] | In this article we shall obtain the boundary state associated with a moving $Dp$-brane in the presence of the Kalb-Ramond field $B_{\mu\nu}$, an internal U(1) gauge field $A_{\alpha}$ and a tachyon field, in the compact spacetime. According to this state, properties of the brane and a closed string, with mixed boundary... | 8.50532 | 5.466751 | 8.238474 | 5.972279 | 6.094232 | 5.736598 | 5.805763 | 6.226113 | 5.756828 | 9.12431 | 6.293169 | 6.995993 | 8.249269 | 7.434091 | 7.693147 | 7.273299 | 7.048509 | 7.203414 | 7.209633 | 8.144332 | 7.444838 |
hep-th/9505149 | null | A. V. Ramallo and J. M. Sanchez de Santos | TOPOLOGICAL MATTER, MIRROR SYMMETRY AND NON-CRITICAL (SUPER)STRINGS | 45 pages, phyzzx, no figures | Nucl.Phys. B456 (1995) 405-441 | 10.1016/0550-3213(95)00485-8 | US-FT-5/95 | hep-th | null | We study the realization of the (super) conformal topological symmetry in
two-dimensional field theories. The mirror automorphism of the topological
algebra is represented as a reflection in the space of fields. As a
consequence, a double BRST structure for topological matter theories is found.
It is shown that the i... | [
{
"created": "Wed, 24 May 1995 05:37:39 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ramallo",
"A. V.",
""
],
[
"de Santos",
"J. M. Sanchez",
""
]
] | We study the realization of the (super) conformal topological symmetry in two-dimensional field theories. The mirror automorphism of the topological algebra is represented as a reflection in the space of fields. As a consequence, a double BRST structure for topological matter theories is found. It is shown that the imp... | 11.654899 | 10.093665 | 12.776879 | 9.143637 | 10.271319 | 9.310161 | 10.023883 | 9.684495 | 10.431209 | 12.560331 | 9.607467 | 10.883608 | 11.350225 | 10.835645 | 10.580156 | 10.886317 | 10.901577 | 10.632351 | 10.57829 | 11.906556 | 10.49079 |
hep-th/0212327 | Lev Kofman | Andrei Frolov and Lev Kofman | Inflation and de Sitter Thermodynamics | 19 pages, 5 figures | JCAP 0305 (2003) 009 | 10.1088/1475-7516/2003/05/009 | CITA-2002-46 | hep-th astro-ph gr-qc hep-ph | null | We consider the quasi-de Sitter geometry of the inflationary universe. We
calculate the energy flux of the slowly rolling background scalar field through
the quasi-de Sitter apparent horizon and set it equal to the change of the
entropy (1/4 of the area) multiplied by the temperature, dE=TdS. Remarkably,
this thermod... | [
{
"created": "Mon, 30 Dec 2002 20:14:01 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Frolov",
"Andrei",
""
],
[
"Kofman",
"Lev",
""
]
] | We consider the quasi-de Sitter geometry of the inflationary universe. We calculate the energy flux of the slowly rolling background scalar field through the quasi-de Sitter apparent horizon and set it equal to the change of the entropy (1/4 of the area) multiplied by the temperature, dE=TdS. Remarkably, this thermodyn... | 11.343813 | 11.822839 | 11.954565 | 11.10151 | 12.197503 | 11.728331 | 11.902503 | 11.201968 | 11.155902 | 12.629639 | 11.086457 | 11.108335 | 11.327412 | 10.881737 | 11.138825 | 11.113688 | 11.330031 | 10.878993 | 10.839155 | 10.743813 | 10.793637 |
0902.3898 | Ralf Hofmann | Josef Ludescher and Ralf Hofmann | CMB dipole revisited | 9 pages, 5 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We re-evaluate the build-up of a horizon-sized temperature profile of
amplitude $\delta T/T \sim 10^{-3}$ at $z\sim 1$ in light of an improved
determination of the black-body anomaly, based on a pure SU(2) Yang-Mills
theory, and the correction of a mistake in deriving the evolution equation for
$\delta T$. Our presen... | [
{
"created": "Mon, 23 Feb 2009 12:03:18 GMT",
"version": "v1"
}
] | 2009-02-24 | [
[
"Ludescher",
"Josef",
""
],
[
"Hofmann",
"Ralf",
""
]
] | We re-evaluate the build-up of a horizon-sized temperature profile of amplitude $\delta T/T \sim 10^{-3}$ at $z\sim 1$ in light of an improved determination of the black-body anomaly, based on a pure SU(2) Yang-Mills theory, and the correction of a mistake in deriving the evolution equation for $\delta T$. Our present ... | 14.540292 | 15.749754 | 13.882835 | 11.750739 | 15.6495 | 15.106706 | 14.552198 | 12.600563 | 13.397955 | 14.424184 | 13.799181 | 13.568885 | 13.575231 | 13.40546 | 13.547423 | 14.19835 | 13.614937 | 13.963593 | 13.637359 | 13.547339 | 14.088912 |
1011.4264 | J. M. Drummond | J.M.Drummond, L.Ferro, E.Ragoucy | Yangian symmetry of light-like Wilson loops | 15 pages, 5 figures | JHEP 1111 (2011) 049 | 10.1007/JHEP11(2011)049 | CERN-PH-TH/2010-275; HU-EP-10/81 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that a certain class of light-like Wilson loops exhibits a Yangian
symmetry at one loop, or equivalently, in an Abelian theory. The Wilson loops
we discuss are equivalent to one-loop MHV amplitudes in N=4 super Yang-Mills
theory in a certain kinematical regime. The fact that we find a Yangian
symmetry constra... | [
{
"created": "Thu, 18 Nov 2010 19:44:21 GMT",
"version": "v1"
},
{
"created": "Sat, 4 Dec 2010 16:41:10 GMT",
"version": "v2"
}
] | 2015-05-20 | [
[
"Drummond",
"J. M.",
""
],
[
"Ferro",
"L.",
""
],
[
"Ragoucy",
"E.",
""
]
] | We show that a certain class of light-like Wilson loops exhibits a Yangian symmetry at one loop, or equivalently, in an Abelian theory. The Wilson loops we discuss are equivalent to one-loop MHV amplitudes in N=4 super Yang-Mills theory in a certain kinematical regime. The fact that we find a Yangian symmetry constrain... | 9.003791 | 8.281094 | 9.950676 | 8.267159 | 8.01911 | 8.666038 | 8.016844 | 7.626622 | 8.439308 | 10.664198 | 7.835309 | 8.23246 | 9.135727 | 8.171325 | 8.056986 | 8.030401 | 8.109032 | 8.045929 | 7.914359 | 9.205635 | 8.0806 |
1009.1854 | David Skinner | Mathew Bullimore, Lionel Mason and David Skinner | MHV Diagrams in Momentum Twistor Space | 36 pages, 13 figures | JHEP 1012:032,2010 | 10.1007/JHEP12(2010)032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that there are remarkable simplifications when the MHV diagram
formalism for N=4 super Yang-Mills is reformulated in momentum twistor space.
The vertices are replaced by unity while each propagator becomes a dual
superconformal `R-invariant' whose arguments may be read off from the diagram.
The momentum twist... | [
{
"created": "Thu, 9 Sep 2010 18:48:56 GMT",
"version": "v1"
}
] | 2010-12-14 | [
[
"Bullimore",
"Mathew",
""
],
[
"Mason",
"Lionel",
""
],
[
"Skinner",
"David",
""
]
] | We show that there are remarkable simplifications when the MHV diagram formalism for N=4 super Yang-Mills is reformulated in momentum twistor space. The vertices are replaced by unity while each propagator becomes a dual superconformal `R-invariant' whose arguments may be read off from the diagram. The momentum twistor... | 7.510569 | 7.051304 | 8.484436 | 7.213472 | 6.776497 | 7.440806 | 7.481586 | 7.280751 | 6.769282 | 9.178937 | 6.966606 | 7.644218 | 7.999484 | 7.34597 | 7.315485 | 7.729448 | 7.661019 | 7.395711 | 7.342897 | 8.21101 | 7.242579 |
2206.03414 | Jeevan Chandra Namburi | Jeevan Chandra and Thomas Hartman | Coarse graining pure states in AdS/CFT | 46 pages + 4 appendices (correction to section 6.2.3 in v2) | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct new Euclidean wormhole solutions in AdS(d+1) and discuss their
role in UV-complete theories, without ensemble averaging. The geometries are
interpreted as overlaps of GHZ-like entangled states, which arise naturally
from coarse graining the density matrix of a pure state in the dual CFT. In
several examp... | [
{
"created": "Tue, 7 Jun 2022 16:04:17 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Jun 2022 06:32:56 GMT",
"version": "v2"
}
] | 2022-06-09 | [
[
"Chandra",
"Jeevan",
""
],
[
"Hartman",
"Thomas",
""
]
] | We construct new Euclidean wormhole solutions in AdS(d+1) and discuss their role in UV-complete theories, without ensemble averaging. The geometries are interpreted as overlaps of GHZ-like entangled states, which arise naturally from coarse graining the density matrix of a pure state in the dual CFT. In several example... | 14.143104 | 12.34258 | 15.155063 | 11.802773 | 13.301113 | 12.542275 | 12.894804 | 12.185893 | 12.11016 | 15.240685 | 12.614453 | 13.414922 | 14.153068 | 13.553359 | 13.22974 | 13.252682 | 12.523143 | 13.192295 | 12.875583 | 14.225075 | 13.250989 |
hep-th/9803052 | Barvinski | A.O.Barvinsky and A.Yu.Kamenshchik | Effective equations of motion and initial conditions for inflation in
quantum cosmology | 23 pages, LaTeX | Nucl.Phys.B532:339-360,1998 | 10.1016/S0550-3213(98)00484-2 | FIAN/TD/98-10 | hep-th | null | We obtain effective equations of inflationary dynamics for the mean inflaton
and metric fields in the no-boundary and tunneling quantum states of the
Universe. In the slow roll approximation (taking the form of the local
Schwiger-DeWitt expansion) effective equations follow from the Euclidean
effective action on the ... | [
{
"created": "Thu, 5 Mar 1998 23:10:48 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Barvinsky",
"A. O.",
""
],
[
"Kamenshchik",
"A. Yu.",
""
]
] | We obtain effective equations of inflationary dynamics for the mean inflaton and metric fields in the no-boundary and tunneling quantum states of the Universe. In the slow roll approximation (taking the form of the local Schwiger-DeWitt expansion) effective equations follow from the Euclidean effective action on the De... | 13.034 | 12.593502 | 12.131819 | 12.10053 | 13.090824 | 12.432675 | 12.987094 | 11.457191 | 12.863994 | 13.36201 | 12.211914 | 12.853036 | 12.158596 | 12.509406 | 12.969296 | 12.882107 | 12.598163 | 12.491402 | 12.744475 | 12.773157 | 12.789632 |
hep-th/9902122 | Nobuyoshi Ohta | Kazuyuki Furuuchi, Nobuyoshi Ohta and Jian-Ge Zhou | Spacetime Superalgebra in AdS_4 \times S^7 via Supermembrane Probe | 8 pages, Latex, minor corrections, final version to appear in Phys.
Rev.D | Phys. Rev. D 60, 047901 (1999) | 10.1103/PhysRevD.60.047901 | OU-HET 313 | hep-th | null | The spacetime superalgebra via the supermembrane probe in the background of
AdS_4 \times S^7 is discussed to the lowest order in the spinor coordinate
$\t$. To obtain the correct spacetime superalgebras, all $\t^2$ order
corrections for supervielbein and super 3-form gauge potential have to be
included. The central e... | [
{
"created": "Wed, 17 Feb 1999 07:15:38 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Feb 1999 04:55:10 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Apr 1999 06:24:19 GMT",
"version": "v3"
}
] | 2016-08-25 | [
[
"Furuuchi",
"Kazuyuki",
""
],
[
"Ohta",
"Nobuyoshi",
""
],
[
"Zhou",
"Jian-Ge",
""
]
] | The spacetime superalgebra via the supermembrane probe in the background of AdS_4 \times S^7 is discussed to the lowest order in the spinor coordinate $\t$. To obtain the correct spacetime superalgebras, all $\t^2$ order corrections for supervielbein and super 3-form gauge potential have to be included. The central ext... | 9.645527 | 8.031189 | 10.177496 | 7.819333 | 8.775694 | 8.664413 | 7.765467 | 8.6545 | 7.390976 | 9.711504 | 8.513006 | 8.214091 | 9.633009 | 8.299109 | 8.084959 | 8.270232 | 7.847309 | 8.167012 | 8.126251 | 9.829258 | 8.147572 |
1007.2820 | Manuel Calixto | V. Aldaya, M. Calixto and F.F. L\'opez-Ruiz | Non-Canonical Perturbation Theory of Non-Linear Sigma Models | 11 pages, 1 figure, LaTeX | Mod.Phys.Lett.A26:127-138,2011 | 10.1142/S0217732311034670 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the O(N)-invariant Non-Linear Sigma Model (NLSM) in a different
perturbative regime from the usual relativistic-free-field one, by using
non-canonical basic commutation relations adapted to the underlying O(N)
symmetry of the system, which also account for the non-trivial (non-flat)
geometry and topology o... | [
{
"created": "Fri, 16 Jul 2010 17:33:11 GMT",
"version": "v1"
}
] | 2011-01-20 | [
[
"Aldaya",
"V.",
""
],
[
"Calixto",
"M.",
""
],
[
"López-Ruiz",
"F. F.",
""
]
] | We explore the O(N)-invariant Non-Linear Sigma Model (NLSM) in a different perturbative regime from the usual relativistic-free-field one, by using non-canonical basic commutation relations adapted to the underlying O(N) symmetry of the system, which also account for the non-trivial (non-flat) geometry and topology of ... | 13.537808 | 10.778194 | 12.342444 | 11.338455 | 12.511664 | 11.482607 | 12.309408 | 11.632125 | 10.967296 | 12.385979 | 11.271934 | 11.889964 | 11.929779 | 11.546518 | 11.901493 | 11.742763 | 12.19304 | 11.72199 | 11.463937 | 11.794002 | 12.157867 |
hep-th/9307045 | Nobuyuki Ishibashi | Nobuyuki Ishibashi and Hikaru Kawai | String Field Theory of Noncritical Strings | 13 pages ( LaTex file ), KEK-TH-364, UT-649 | Phys.Lett. B314 (1993) 190-196 | 10.1016/0370-2693(93)90448-Q | null | hep-th | null | We construct the Hamiltonian operator of the string field theory for $c=0$
string theory. It describes how strings evolve in the coordinate frame, which
is defined by using the geodesic distance on the worldsheet. The Hamiltonian
consists of three-string interaction terms and a tadpole term. We show that one
can deri... | [
{
"created": "Wed, 7 Jul 1993 06:13:47 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ishibashi",
"Nobuyuki",
""
],
[
"Kawai",
"Hikaru",
""
]
] | We construct the Hamiltonian operator of the string field theory for $c=0$ string theory. It describes how strings evolve in the coordinate frame, which is defined by using the geodesic distance on the worldsheet. The Hamiltonian consists of three-string interaction terms and a tadpole term. We show that one can derive... | 8.969535 | 7.842818 | 8.463882 | 7.540655 | 7.559193 | 6.989839 | 8.06406 | 7.520738 | 8.101263 | 9.236277 | 7.412734 | 7.521372 | 7.907729 | 7.75835 | 7.769362 | 8.110671 | 7.64132 | 7.928005 | 8.018037 | 7.842027 | 7.714454 |
hep-th/0309257 | J. M. Maillard | D. Altschuler, A. Coste, J-M. Maillard | Representation Theory of Twisted Group Double | 15 pages, no figure | Annales Fond.Broglie 29 (2004) 681-694 | null | null | hep-th | null | This text collects useful results concerning the quasi-Hopf algebra $\D $. We
give a review of issues related to its use in conformal theories and physical
mathematics. Existence of such algebras based on 3-cocycles with values in $
{R} / {Z} $ which mimic for finite groups Chern-Simons terms of gauge theories,
open ... | [
{
"created": "Mon, 29 Sep 2003 12:43:46 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Oct 2003 14:30:04 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Altschuler",
"D.",
""
],
[
"Coste",
"A.",
""
],
[
"Maillard",
"J-M.",
""
]
] | This text collects useful results concerning the quasi-Hopf algebra $\D $. We give a review of issues related to its use in conformal theories and physical mathematics. Existence of such algebras based on 3-cocycles with values in $ {R} / {Z} $ which mimic for finite groups Chern-Simons terms of gauge theories, open wi... | 25.594038 | 28.663162 | 27.360435 | 24.854212 | 26.55739 | 28.786402 | 27.162626 | 26.611952 | 24.781599 | 32.22464 | 22.938 | 23.990183 | 26.650137 | 24.004854 | 25.928179 | 25.166061 | 24.457521 | 23.856516 | 23.410423 | 26.046936 | 23.771856 |
hep-th/9209082 | null | Alexander Turbiner | Lie-algebraic approach to the theory of polynomial solutions. III.
Differential equations in two real variables and general outlook | 28pp | null | null | ETH-TH/92-34 | hep-th alg-geom funct-an math.AG math.FA | null | Classification theorems for linear differential equations in two real
variables, possessing eigenfunctions in the form of the polynomials (the
generalized Bochner problem) are given. The main result is based on the
consideration of the eigenvalue problem for a polynomial elements of the
universal enveloping algebras ... | [
{
"created": "Tue, 22 Sep 1992 14:56:53 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Turbiner",
"Alexander",
""
]
] | Classification theorems for linear differential equations in two real variables, possessing eigenfunctions in the form of the polynomials (the generalized Bochner problem) are given. The main result is based on the consideration of the eigenvalue problem for a polynomial elements of the universal enveloping algebras of... | 9.970502 | 9.899567 | 11.180159 | 9.244498 | 9.575527 | 10.592194 | 10.437588 | 9.611451 | 10.529302 | 11.781195 | 9.475255 | 9.421709 | 9.340297 | 9.315096 | 9.635736 | 9.646097 | 9.619165 | 9.440831 | 9.671677 | 9.443373 | 9.845314 |
1003.5361 | Larus Thorlacius | E.J. Brynjolfsson, U.H. Danielsson, L. Thorlacius, T. Zingg | Black Hole Thermodynamics and Heavy Fermion Metals | 17 pages, 4 figures; v2: added references; v3: matches published
version | JHEP 1008:027,2010 | 10.1007/JHEP08(2010)027 | NORDITA-2010-15, UUITP-09/10 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Heavy fermion alloys at critical doping typically exhibit non-Fermi-liquid
behavior at low temperatures, including a logarithmic or power law rise in the
ratio of specific heat to temperature as the temperature is lowered. Anomalous
specific heat of this type is also observed in a simple class of gravitational
dual m... | [
{
"created": "Sun, 28 Mar 2010 11:46:31 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Apr 2010 20:13:20 GMT",
"version": "v2"
},
{
"created": "Tue, 10 Aug 2010 07:13:33 GMT",
"version": "v3"
}
] | 2015-03-13 | [
[
"Brynjolfsson",
"E. J.",
""
],
[
"Danielsson",
"U. H.",
""
],
[
"Thorlacius",
"L.",
""
],
[
"Zingg",
"T.",
""
]
] | Heavy fermion alloys at critical doping typically exhibit non-Fermi-liquid behavior at low temperatures, including a logarithmic or power law rise in the ratio of specific heat to temperature as the temperature is lowered. Anomalous specific heat of this type is also observed in a simple class of gravitational dual mod... | 9.972853 | 7.857106 | 11.434761 | 8.301423 | 8.804749 | 8.090041 | 8.297363 | 8.245065 | 9.35646 | 9.573356 | 8.323304 | 8.310742 | 10.367825 | 8.772573 | 8.586573 | 8.509441 | 8.348201 | 8.435592 | 9.072405 | 10.808228 | 8.783267 |
1112.3979 | Simon Gentle A | Simon A. Gentle, Mukund Rangamani, Benjamin Withers | A soliton menagerie in AdS | 62 pages, 21 figures. v2: added refs and comments and updated
appendices | null | 10.1007/JHEP05(2012)106 | DCPT-11/55 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the behaviour of charged scalar solitons in asymptotically global
AdS4 spacetimes. This is motivated in part by attempting to identify under what
circumstances such objects can become large relative to the AdS length scale.
We demonstrate that such solitons generically do get large and in fact in the
plana... | [
{
"created": "Fri, 16 Dec 2011 21:44:53 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Jan 2012 16:30:28 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Gentle",
"Simon A.",
""
],
[
"Rangamani",
"Mukund",
""
],
[
"Withers",
"Benjamin",
""
]
] | We explore the behaviour of charged scalar solitons in asymptotically global AdS4 spacetimes. This is motivated in part by attempting to identify under what circumstances such objects can become large relative to the AdS length scale. We demonstrate that such solitons generically do get large and in fact in the planar ... | 11.493198 | 11.472028 | 13.176914 | 10.871499 | 11.818442 | 12.010775 | 11.830133 | 12.264462 | 12.459923 | 11.950006 | 11.208111 | 11.14445 | 11.542522 | 11.120893 | 11.112897 | 11.344755 | 11.046085 | 11.050201 | 11.035344 | 11.169933 | 11.078242 |
2009.03806 | Euclides Silva | J. E. G. Silva | A field theory in Randers-Finsler spacetime | 12 pages. arXiv admin note: substantial text overlap with
arXiv:1602.07345 | EPL 133 21002 (2021) | 10.1209/0295-5075/133/21002 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Finsler geometry is a natural arena to investigate the physics of spacetimes
with local Lorentz violating. The directional dependence of the Finsler metric
provides a way to encode the Lorentz violating effects into the geometric
structure of spacetime. Here, a classical field theory is proposed in a special
Finsler ... | [
{
"created": "Fri, 4 Sep 2020 20:32:29 GMT",
"version": "v1"
}
] | 2021-04-29 | [
[
"Silva",
"J. E. G.",
""
]
] | Finsler geometry is a natural arena to investigate the physics of spacetimes with local Lorentz violating. The directional dependence of the Finsler metric provides a way to encode the Lorentz violating effects into the geometric structure of spacetime. Here, a classical field theory is proposed in a special Finsler ge... | 9.206576 | 8.260137 | 8.231216 | 7.705514 | 8.179285 | 8.70791 | 8.533239 | 7.850825 | 8.213931 | 8.786633 | 7.821325 | 7.990383 | 8.21524 | 8.12264 | 8.124521 | 8.14149 | 8.19602 | 8.102327 | 8.105911 | 8.053149 | 7.922905 |
hep-th/9803162 | Reza Abbaspur | R. Abbaspur, H. Arfaei | Distributed Systems of Intersecting Branes at Arbitrary Angles | Latex file, 58 pages, no figures, 5 tables, This revision contains
some minor changes of the original version including those of the title,
abstract and referrences. Some comments are added | Nucl.Phys. B541 (1999) 386-440 | 10.1016/S0550-3213(98)00746-9 | IPM-98-284 | hep-th | null | A `reduced' action formulation for a general class of the supergravity
solutions, corresponding to the `marginally' bound `distributed' systems of
various types of branes at arbitrary angles, is developed. It turns out that
all the information regarding the classical features of such solutions is
encoded in a first o... | [
{
"created": "Thu, 19 Mar 1998 18:24:30 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Jun 1998 13:17:03 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Abbaspur",
"R.",
""
],
[
"Arfaei",
"H.",
""
]
] | A `reduced' action formulation for a general class of the supergravity solutions, corresponding to the `marginally' bound `distributed' systems of various types of branes at arbitrary angles, is developed. It turns out that all the information regarding the classical features of such solutions is encoded in a first ord... | 9.993555 | 9.820265 | 10.624703 | 9.510833 | 9.95201 | 9.820096 | 10.102833 | 9.735437 | 9.91898 | 10.764515 | 9.743416 | 9.641282 | 9.772632 | 9.405929 | 9.383393 | 9.161313 | 9.576757 | 9.515634 | 9.524584 | 9.735261 | 9.534333 |
hep-th/9704005 | Seungjoon Hyun | S. Hyun | U-duality between Three and Higher Dimensional Black Holes | 9 pages, TeX, harvmac(b) | J.KoreanPhys.Soc.33:S532-S536,1998 | null | null | hep-th | null | We show that the D-brane configurations for the five and four-dimensional
black holes give the geometry of two and three-dimensional ones as well. The
emergence of these lower dimensional black holes from the D-brane
configurations for those of higher dimensions comes from the choice of the
integration constant of ha... | [
{
"created": "Tue, 1 Apr 1997 16:29:09 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Hyun",
"S.",
""
]
] | We show that the D-brane configurations for the five and four-dimensional black holes give the geometry of two and three-dimensional ones as well. The emergence of these lower dimensional black holes from the D-brane configurations for those of higher dimensions comes from the choice of the integration constant of harm... | 10.704877 | 10.158887 | 10.363982 | 9.576112 | 10.474827 | 10.306314 | 10.235723 | 9.164726 | 9.746699 | 11.075047 | 10.056792 | 9.917273 | 10.316724 | 10.146853 | 10.050097 | 10.17416 | 10.519904 | 10.103654 | 10.066847 | 10.183005 | 9.877008 |
1811.01717 | Patricio Salgado | G. Rubio and P. Salgado | Modified newtonian dynamics and non-relativistic ChSAS gravity | null | Physics Letter B 787 (2018) 30 | 10.1016/j.physletb.2018.10.028 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of the non-relativistic theories, a generalization of the
Chern--Weil-theorem allows us to show that extended Chern--Simons actions for
gravity in d=4 invariant under some specific non-relativistic groups lead to
modified Poisson equations. In some particular cases, these modified equations
have the fo... | [
{
"created": "Mon, 5 Nov 2018 14:25:08 GMT",
"version": "v1"
}
] | 2018-11-06 | [
[
"Rubio",
"G.",
""
],
[
"Salgado",
"P.",
""
]
] | In the context of the non-relativistic theories, a generalization of the Chern--Weil-theorem allows us to show that extended Chern--Simons actions for gravity in d=4 invariant under some specific non-relativistic groups lead to modified Poisson equations. In some particular cases, these modified equations have the form... | 12.614555 | 12.354124 | 11.545803 | 11.27149 | 12.415951 | 12.541749 | 10.964976 | 11.422827 | 11.641816 | 12.013498 | 11.866305 | 11.656302 | 12.111918 | 11.598746 | 12.271422 | 11.855116 | 11.18957 | 11.425684 | 11.828588 | 12.263464 | 11.408171 |
hep-th/9405099 | Masako Asano | Masako Asano and Saburo Higuchi | On three-dimensional topological field theories constructed from
$D^\omega(G)$ for finite group | 13 pages, 3 PS figures included | Mod.Phys.Lett.A9:2359-2370,1994 | 10.1142/S0217732394002239 | TIT/HEP-255 | hep-th hep-lat math.QA | null | We investigate the 3d lattice topological field theories defined by Chung,
Fukuma and Shapere. We concentrate on the model defined by taking a deformation
$\D{G}$ of the quantum double of a finite commutative group $G$ as the
underlying Hopf algebra. It is suggested that Chung-Fukuma-Shapere partition
function is rel... | [
{
"created": "Mon, 16 May 1994 12:31:46 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Asano",
"Masako",
""
],
[
"Higuchi",
"Saburo",
""
]
] | We investigate the 3d lattice topological field theories defined by Chung, Fukuma and Shapere. We concentrate on the model defined by taking a deformation $\D{G}$ of the quantum double of a finite commutative group $G$ as the underlying Hopf algebra. It is suggested that Chung-Fukuma-Shapere partition function is relat... | 10.555098 | 9.379618 | 13.402475 | 9.569694 | 10.554987 | 9.922479 | 10.165763 | 10.093692 | 10.495987 | 11.886044 | 8.920098 | 9.78171 | 10.722073 | 10.465853 | 9.828733 | 9.891195 | 10.030347 | 10.035718 | 9.840243 | 10.342388 | 9.480657 |
0807.1107 | Meng-Chwan Tan | Meng-Chwan Tan | Five-Branes in M-Theory and a Two-Dimensional Geometric Langlands
Duality | 43 pages. Technical refinement of section 4.3. Minor correction of
sections 5.2 and 5.3: level 2k changed to k | Adv.Theor.Math.Phys.14:179-224,2010 | null | null | hep-th math.AG math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A recent attempt to extend the geometric Langlands duality to affine
Kac-Moody groups, has led Braverman and Finkelberg [arXiv:0711.2083] to
conjecture a mathematical relation between the intersection cohomology of the
moduli space of G-bundles on certain singular complex surfaces, and the
integrable representations ... | [
{
"created": "Tue, 8 Jul 2008 16:22:57 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Jul 2008 03:31:23 GMT",
"version": "v2"
},
{
"created": "Sat, 2 Aug 2008 06:02:27 GMT",
"version": "v3"
},
{
"created": "Sat, 4 Jul 2009 16:45:04 GMT",
"version": "v4"
},
{
"crea... | 2013-01-04 | [
[
"Tan",
"Meng-Chwan",
""
]
] | A recent attempt to extend the geometric Langlands duality to affine Kac-Moody groups, has led Braverman and Finkelberg [arXiv:0711.2083] to conjecture a mathematical relation between the intersection cohomology of the moduli space of G-bundles on certain singular complex surfaces, and the integrable representations of... | 8.736993 | 10.009551 | 10.412374 | 8.671608 | 9.828229 | 9.276436 | 9.104498 | 8.896626 | 8.41067 | 11.544523 | 8.6841 | 8.718683 | 8.953274 | 8.452315 | 8.880269 | 8.83893 | 8.669347 | 8.742829 | 8.534964 | 9.343515 | 8.198633 |
2303.10534 | Kanade Nishikawa | Kanade Nishikawa | Conformal bootstrap in momentum space at finite volume | 83 pages, 14 figures | null | 10.1007/JHEP06(2023)152 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we Fourier transform the Wightman function concerning energy
and angular momentum on the $S^{D-1}$ spatial slice in radial quantization in
$D=2,3$ dimensions. In each case, we use the conformal Ward Identities to solve
systematically for the Fourier components. We then use these Fourier components
to b... | [
{
"created": "Sun, 19 Mar 2023 02:25:57 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Mar 2023 11:59:24 GMT",
"version": "v2"
},
{
"created": "Tue, 13 Jun 2023 13:35:25 GMT",
"version": "v3"
}
] | 2023-06-28 | [
[
"Nishikawa",
"Kanade",
""
]
] | In this paper, we Fourier transform the Wightman function concerning energy and angular momentum on the $S^{D-1}$ spatial slice in radial quantization in $D=2,3$ dimensions. In each case, we use the conformal Ward Identities to solve systematically for the Fourier components. We then use these Fourier components to bui... | 12.457082 | 12.555984 | 11.431286 | 11.127717 | 12.451004 | 12.187964 | 13.094586 | 12.537569 | 11.612997 | 12.210855 | 12.084944 | 11.088428 | 11.03364 | 10.900592 | 11.400035 | 11.388989 | 11.372505 | 11.466397 | 11.242665 | 11.108315 | 11.326515 |
hep-th/9505095 | null | R. Amorim and J. Barcelos-Neto | BV QUANTIZATION OF A VECTOR-TENSOR GAUGE THEORY WITH TOPOLOGICAL
COUPLING | 10 pages, Latex | Mod.Phys.Lett. A10 (1995) 917-924 | 10.1142/S0217732395001009 | null | hep-th | null | We use the BV quantization method for a theory with coupled tensor and vector
gauge fields through a topological term. We consider in details the
reducibility of the tensorial sector as well as the appearance of a mass term
in the effective vectorial theory .
| [
{
"created": "Tue, 16 May 1995 15:23:41 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Amorim",
"R.",
""
],
[
"Barcelos-Neto",
"J.",
""
]
] | We use the BV quantization method for a theory with coupled tensor and vector gauge fields through a topological term. We consider in details the reducibility of the tensorial sector as well as the appearance of a mass term in the effective vectorial theory . | 20.10265 | 15.69464 | 18.914358 | 17.071163 | 15.677979 | 17.458078 | 13.287997 | 16.049707 | 16.554859 | 19.000765 | 13.959738 | 16.943125 | 19.224543 | 18.513601 | 17.517187 | 18.284828 | 18.484224 | 18.046366 | 18.559643 | 18.130867 | 17.377657 |
hep-th/9903207 | Alastair Paulin-Campbell | Robert de Mello Koch, Alastair Paulin-Campbell and Joao P. Rodrigues | Monopole Dynamics in N=2 super Yang-Mills Theory From a Threebrane Probe | 26 pages, harvmac, some equations corrected in section 3. No
conclusions changed, references added. Apologies to those not previously
referenced, final version to appear in Nucl. Phys. B | Nucl.Phys. B559 (1999) 143-164 | 10.1016/S0550-3213(99)00422-8 | CNLS-99-03, BROWN-HET-1177 | hep-th | null | The BPS states of N=2 super Yang-Mills theory with gauge group SU(2) are
constructed as non-trivial finite-energy solutions of the worldvolume theory of
a threebrane probe in F theory. The solutions preserve 1/2 of N=2 supersymmetry
and provide a worldvolume realization of strings stretching from the probe to a
seven... | [
{
"created": "Wed, 24 Mar 1999 15:10:28 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Apr 1999 19:13:58 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Aug 1999 06:04:42 GMT",
"version": "v3"
},
{
"created": "Wed, 25 Aug 1999 10:20:31 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Koch",
"Robert de Mello",
""
],
[
"Paulin-Campbell",
"Alastair",
""
],
[
"Rodrigues",
"Joao P.",
""
]
] | The BPS states of N=2 super Yang-Mills theory with gauge group SU(2) are constructed as non-trivial finite-energy solutions of the worldvolume theory of a threebrane probe in F theory. The solutions preserve 1/2 of N=2 supersymmetry and provide a worldvolume realization of strings stretching from the probe to a sevenbr... | 7.929406 | 7.135415 | 8.918153 | 6.968235 | 7.398868 | 7.265228 | 7.24764 | 6.458461 | 6.406979 | 9.571446 | 6.746039 | 6.687219 | 7.963677 | 7.075031 | 6.804448 | 6.843218 | 6.743191 | 6.92987 | 7.181267 | 8.189716 | 7.024035 |
hep-th/0002133 | Yungui Gong | Yungui Gong | Ramond-Ramond Field Transformation | 8 pages, no figures. correct some minor mistakes, add one section of
examples, add one reference | null | null | UTEXAS-HEP-00-1 | hep-th | null | We find that the mixture of Ramond-Ramond fields and Neveu-Schwarz two form
are transformed as Majorana spinors under the T-duality group $O(d,d)$. The
Ramond-Ramond field transformation under the group $O(d,d)$ is realized in a
simple form by using the spinor representation. The Ramond-Ramond field
transformation ru... | [
{
"created": "Wed, 16 Feb 2000 20:48:30 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Mar 2000 23:18:37 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Gong",
"Yungui",
""
]
] | We find that the mixture of Ramond-Ramond fields and Neveu-Schwarz two form are transformed as Majorana spinors under the T-duality group $O(d,d)$. The Ramond-Ramond field transformation under the group $O(d,d)$ is realized in a simple form by using the spinor representation. The Ramond-Ramond field transformation rule... | 8.139917 | 7.321177 | 8.382481 | 6.936194 | 7.284678 | 7.62308 | 7.30694 | 7.195223 | 6.839942 | 7.584533 | 6.909429 | 7.410594 | 7.392335 | 6.95691 | 7.101705 | 7.184927 | 7.106323 | 7.248389 | 6.8701 | 7.516108 | 7.242093 |
1212.6876 | Ahmad Ghodsi | Ahmad Ghodsi and Davood Mahdavian Yekta | Stability of vacua in New Massive Gravity in different gauges | 30 pages, 10 figures. v3: Improved version. To appear in JHEP | null | 10.1007/JHEP08(2013)095 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider AdS3 and warped AdS3 vacua in new massive gravity and study the
highest weight modes and general propagating modes as a set of solutions for
the linearized equations of motion. We observed that depending on the choice of
gauge there are two types of solutions. We show that for warped AdS3 vacuum,
the mass... | [
{
"created": "Mon, 31 Dec 2012 12:23:56 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Mar 2013 10:52:08 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Jul 2013 05:42:58 GMT",
"version": "v3"
}
] | 2013-08-20 | [
[
"Ghodsi",
"Ahmad",
""
],
[
"Yekta",
"Davood Mahdavian",
""
]
] | We consider AdS3 and warped AdS3 vacua in new massive gravity and study the highest weight modes and general propagating modes as a set of solutions for the linearized equations of motion. We observed that depending on the choice of gauge there are two types of solutions. We show that for warped AdS3 vacuum, the massle... | 13.100729 | 11.441527 | 13.324458 | 11.835009 | 11.996342 | 12.818819 | 11.919474 | 11.973028 | 11.322193 | 13.598266 | 11.337854 | 11.792737 | 12.910339 | 12.433851 | 11.749206 | 11.495134 | 11.712082 | 11.908887 | 12.271544 | 12.399901 | 11.911184 |
1304.6944 | Luigi Delle Rose | Claudio Coriano, Luigi Delle Rose, Emil Mottola and Mirko Serino | Solving the Conformal Constraints for Scalar Operators in Momentum Space
and the Evaluation of Feynman's Master Integrals | 28 pages, extended final version, to appear on JHEP | null | 10.1007/JHEP07(2013)011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the structure of the constraints on three-point correlation
functions emerging when conformal invariance is imposed in momentum space and
in arbitrary space-time dimensions, presenting a derivation of their solutions
for arbitrary scalar operators. We show that the differential equations
generated by t... | [
{
"created": "Thu, 25 Apr 2013 15:53:47 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Jun 2013 10:13:53 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"Coriano",
"Claudio",
""
],
[
"Rose",
"Luigi Delle",
""
],
[
"Mottola",
"Emil",
""
],
[
"Serino",
"Mirko",
""
]
] | We investigate the structure of the constraints on three-point correlation functions emerging when conformal invariance is imposed in momentum space and in arbitrary space-time dimensions, presenting a derivation of their solutions for arbitrary scalar operators. We show that the differential equations generated by the... | 10.962422 | 10.856112 | 11.967127 | 10.885393 | 11.341451 | 10.932405 | 11.228111 | 11.119016 | 9.947425 | 11.211887 | 10.462342 | 10.547003 | 10.36797 | 10.23605 | 10.468778 | 10.841865 | 10.547093 | 10.522347 | 9.996112 | 10.30529 | 9.844056 |
1208.4801 | Wissam Chemissany | W. Chemissany, S. Ferrara, R. Kallosh, and C. S. Shahbazi | N=2 Supergravity Counterterms, Off and On Shell | 20 pages, 3 tables. Acknowledgments added. arXiv admin note: text
overlap with arXiv:1010.2150 by other authors | null | 10.1007/JHEP12(2012)089 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study N=2 supergravity deformed by a genuine supersymmetric completion of
the $\lambda R^4$ term, using the underlying off shell N=2 superconformal
framework. The gauge-fixed superconformal model has unbroken local
supersymmetry of N=2 supergravity with higher derivative deformation.
Elimination of auxiliary field... | [
{
"created": "Thu, 23 Aug 2012 17:08:13 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Dec 2012 15:37:15 GMT",
"version": "v2"
},
{
"created": "Sat, 19 Jan 2013 15:35:59 GMT",
"version": "v3"
}
] | 2015-06-11 | [
[
"Chemissany",
"W.",
""
],
[
"Ferrara",
"S.",
""
],
[
"Kallosh",
"R.",
""
],
[
"Shahbazi",
"C. S.",
""
]
] | We study N=2 supergravity deformed by a genuine supersymmetric completion of the $\lambda R^4$ term, using the underlying off shell N=2 superconformal framework. The gauge-fixed superconformal model has unbroken local supersymmetry of N=2 supergravity with higher derivative deformation. Elimination of auxiliary fields ... | 10.701667 | 11.34171 | 12.059229 | 10.085777 | 11.079778 | 11.729226 | 10.695866 | 10.799893 | 10.610027 | 13.471005 | 10.256163 | 10.785876 | 11.164822 | 10.460001 | 10.208778 | 10.336793 | 10.606559 | 10.383815 | 10.276608 | 11.42101 | 10.379449 |
hep-th/9110009 | null | John Ellis, Yitzhak Frishman and Marek Karliner | Constituent Quarks as Solitons | 14 pages | Phys.Lett.B272:333-338,1991 | 10.1016/0370-2693(91)91839-N | null | hep-th | null | We exhibit soliton solutions of QCD in two dimensions that have the quantum
numbers of quarks. They exist only for quarks heavier than the dimensional
gauge coupling, and have infinite energy, corresponding to the presence of a
string carrying the non-singlet color flux off to spatial infinity. The quark
solitons als... | [
{
"created": "Wed, 2 Oct 1991 16:56:00 GMT",
"version": "v1"
}
] | 2009-09-11 | [
[
"Ellis",
"John",
""
],
[
"Frishman",
"Yitzhak",
""
],
[
"Karliner",
"Marek",
""
]
] | We exhibit soliton solutions of QCD in two dimensions that have the quantum numbers of quarks. They exist only for quarks heavier than the dimensional gauge coupling, and have infinite energy, corresponding to the presence of a string carrying the non-singlet color flux off to spatial infinity. The quark solitons also ... | 13.223831 | 15.124136 | 12.227508 | 12.131498 | 13.502347 | 14.235571 | 15.087229 | 14.83493 | 11.621902 | 14.862265 | 12.906988 | 12.658243 | 12.019666 | 12.074198 | 12.539742 | 12.24848 | 11.832086 | 11.883676 | 12.093279 | 12.414594 | 12.655491 |
0802.2040 | Ulf Gran | U. Gran, J. Gutowski, G. Papadopoulos | Invariant Killing spinors in 11D and type II supergravities | 22 pages, typos corrected | Class.Quant.Grav.26:155004,2009 | 10.1088/0264-9381/26/15/155004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present all isotropy groups and associated $\Sigma$ groups, up to discrete
identifications of the component connected to the identity, of spinors of
eleven-dimensional and type II supergravities. The $\Sigma$ groups are products
of a Spin group and an R-symmetry group of a suitable lower dimensional
supergravity t... | [
{
"created": "Thu, 14 Feb 2008 15:59:11 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Jul 2009 08:39:34 GMT",
"version": "v2"
}
] | 2009-07-22 | [
[
"Gran",
"U.",
""
],
[
"Gutowski",
"J.",
""
],
[
"Papadopoulos",
"G.",
""
]
] | We present all isotropy groups and associated $\Sigma$ groups, up to discrete identifications of the component connected to the identity, of spinors of eleven-dimensional and type II supergravities. The $\Sigma$ groups are products of a Spin group and an R-symmetry group of a suitable lower dimensional supergravity the... | 11.719143 | 11.519489 | 13.340444 | 11.324503 | 12.0451 | 11.17234 | 11.314132 | 10.215902 | 11.114341 | 12.676464 | 10.573933 | 10.325674 | 11.410069 | 10.239441 | 10.261448 | 10.063976 | 9.990799 | 10.388688 | 10.422306 | 11.314154 | 10.397968 |
0707.2671 | Hiroyuki Abe | Hiroyuki Abe, Tetsutaro Higaki, Tatsuo Kobayashi | More about F-term uplifting | 22 pages; a sign error in the evaluation of F^X and the related part
corrected, references added | Phys.Rev.D76:105003,2007 | 10.1103/PhysRevD.76.105003 | YITP-07-43, TU-794, KUNS-2087 | hep-th hep-ph | null | We study moduli stabilization and a realization of de Sitter vacua in
generalized F-term uplifting scenarios of the KKLT-type anti-de Sitter vacuum,
where the uplifting sector X directly couples to the light K\"ahler modulus T
in the superpotential through, e.g., stringy instanton effects. F-term
uplifting can be ach... | [
{
"created": "Wed, 18 Jul 2007 08:43:02 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Jul 2007 09:58:54 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Abe",
"Hiroyuki",
""
],
[
"Higaki",
"Tetsutaro",
""
],
[
"Kobayashi",
"Tatsuo",
""
]
] | We study moduli stabilization and a realization of de Sitter vacua in generalized F-term uplifting scenarios of the KKLT-type anti-de Sitter vacuum, where the uplifting sector X directly couples to the light K\"ahler modulus T in the superpotential through, e.g., stringy instanton effects. F-term uplifting can be achie... | 5.687917 | 5.735126 | 6.140129 | 5.604784 | 5.994895 | 5.754415 | 5.674432 | 5.657053 | 5.435358 | 6.016444 | 5.474738 | 5.638592 | 5.52409 | 5.625893 | 5.572852 | 5.541138 | 5.632357 | 5.505482 | 5.482666 | 5.663933 | 5.459859 |
hep-th/9802124 | W. Kim Baskerville | Kim Baskerville and Robin Michaels | Classification of Normal Modes for Multiskyrmions | 4 pages latex, 1 figure added, typos corrected: in particular
concerning B=4 and B=7 representations. Text otherwise unchanged | null | null | DTP 98-11 | hep-th | null | The normal mode spectra of multiskyrmions play a key role in their
quantisation. We present a general method capable of predicting all the
low-lying vibrational modes of known minimal energy multiskyrmions. In
particular, we explain the origin of the higher multipole breathing modes,
previously observed but not under... | [
{
"created": "Wed, 18 Feb 1998 17:48:35 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Feb 1998 16:35:29 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Baskerville",
"Kim",
""
],
[
"Michaels",
"Robin",
""
]
] | The normal mode spectra of multiskyrmions play a key role in their quantisation. We present a general method capable of predicting all the low-lying vibrational modes of known minimal energy multiskyrmions. In particular, we explain the origin of the higher multipole breathing modes, previously observed but not underst... | 10.84345 | 9.188816 | 11.002508 | 8.779147 | 9.663128 | 8.767229 | 9.568542 | 9.406872 | 9.1373 | 9.907687 | 8.951118 | 9.241167 | 9.755201 | 9.3296 | 9.028335 | 9.385265 | 9.425527 | 8.898303 | 9.276061 | 9.751015 | 9.155127 |
1607.05187 | Sunandan Gangopadhyay | Debabrata Ghorai, Sunandan Gangopadhyay | Holographic free energy and thermodynamic geometry | 13 pages Latex | Eur. Phys. J. C 76 (2016) 702 | 10.1140/epjc/s10052-016-4555-1 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analytically obtain the free energy and thermodynamic geometry of
holographic superconductors in $2+1$-dimensions. The gravitational theory in
the bulk dual to this $2+1$-dimensional strongly coupled theory lives in the
$3+1$-dimensions and is that of a charged $AdS$ black hole together with a
massive charged scal... | [
{
"created": "Thu, 14 Jul 2016 16:31:01 GMT",
"version": "v1"
}
] | 2016-12-23 | [
[
"Ghorai",
"Debabrata",
""
],
[
"Gangopadhyay",
"Sunandan",
""
]
] | We analytically obtain the free energy and thermodynamic geometry of holographic superconductors in $2+1$-dimensions. The gravitational theory in the bulk dual to this $2+1$-dimensional strongly coupled theory lives in the $3+1$-dimensions and is that of a charged $AdS$ black hole together with a massive charged scalar... | 6.491852 | 6.450641 | 6.690924 | 6.275975 | 6.327971 | 6.291017 | 6.760863 | 6.5506 | 6.296474 | 6.813913 | 6.01845 | 6.477796 | 6.380621 | 6.249591 | 6.535769 | 6.638134 | 6.624462 | 6.391487 | 6.301271 | 6.540653 | 6.211654 |
hep-th/9110007 | Peter Bouwknegt | P. Bouwknegt, J. McCarthy, and K. Pilch | Some aspects of free field resolutions in 2D CFT with application to the
quantum Drinfeld-Sokolov reduction | 15 pages | null | null | null | hep-th | null | We review some aspects of the free field approach to two-dimensional
conformal field theories. Specifically, we discuss the construction of free
field resolutions for the integrable highest weight modules of untwisted affine
Kac-Moody algebras, and extend the construction to a certain class of
admissible highest weig... | [
{
"created": "Wed, 2 Oct 1991 09:23:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bouwknegt",
"P.",
""
],
[
"McCarthy",
"J.",
""
],
[
"Pilch",
"K.",
""
]
] | We review some aspects of the free field approach to two-dimensional conformal field theories. Specifically, we discuss the construction of free field resolutions for the integrable highest weight modules of untwisted affine Kac-Moody algebras, and extend the construction to a certain class of admissible highest weight... | 5.237344 | 4.705394 | 7.00247 | 4.801403 | 4.875551 | 4.740269 | 5.060807 | 4.902587 | 4.999194 | 6.682069 | 4.878095 | 4.899916 | 5.609637 | 4.915518 | 4.878816 | 4.785947 | 5.020298 | 4.856262 | 4.968859 | 5.439131 | 4.864112 |
2011.12192 | Konstantin Zarembo | Charlotte Kristjansen, Dennis M\"uller and Konstantin Zarembo | Overlaps and Fermionic Dualities for Integrable Super Spin Chains | 34 pages, 8 figures; v2: a few clarifications added | null | null | NORDITA 2020-109 | hep-th | http://creativecommons.org/licenses/by/4.0/ | The psu(2,2|4) integrable super spin chain underlying the AdS/CFT
correspondence has integrable boundary states which describe set-ups where k
D3-branes get dissolved in a probe D5-brane. Overlaps between Bethe eigenstates
and these boundary states encode the one-point functions of conformal operators
and are express... | [
{
"created": "Tue, 24 Nov 2020 16:36:42 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jan 2021 16:01:27 GMT",
"version": "v2"
}
] | 2021-01-18 | [
[
"Kristjansen",
"Charlotte",
""
],
[
"Müller",
"Dennis",
""
],
[
"Zarembo",
"Konstantin",
""
]
] | The psu(2,2|4) integrable super spin chain underlying the AdS/CFT correspondence has integrable boundary states which describe set-ups where k D3-branes get dissolved in a probe D5-brane. Overlaps between Bethe eigenstates and these boundary states encode the one-point functions of conformal operators and are expressed... | 10.402867 | 9.707967 | 12.316697 | 8.832878 | 10.596335 | 10.471828 | 10.517082 | 9.758302 | 9.716472 | 14.18302 | 9.983387 | 10.208982 | 10.675803 | 9.818729 | 9.405152 | 9.937036 | 9.869476 | 9.653307 | 9.867107 | 10.668892 | 9.380067 |
hep-th/9712168 | Moshe Rozali | Robert G. Leigh and Moshe Rozali | A Note on Six-Dimensional Gauge Theories | Minor changes, Final version to appear in Physics Letters B | Phys.Lett.B433:43-48,1998 | 10.1016/S0370-2693(98)00594-2 | ILL-(TH)-97-09 | hep-th | null | We study the new ``gauge'' theories in 5+1 dimensions, and their
non-commutative generalizations. We argue that the $\theta$-term and the
non-commutative torus parameters appear on an equal footing in the non-critical
string theories which define the gauge theories. The use of these theories as a
Matrix description o... | [
{
"created": "Tue, 16 Dec 1997 22:56:46 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Apr 1998 15:46:03 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Leigh",
"Robert G.",
""
],
[
"Rozali",
"Moshe",
""
]
] | We study the new ``gauge'' theories in 5+1 dimensions, and their non-commutative generalizations. We argue that the $\theta$-term and the non-commutative torus parameters appear on an equal footing in the non-critical string theories which define the gauge theories. The use of these theories as a Matrix description of ... | 10.146443 | 9.22359 | 11.38825 | 9.540053 | 9.845049 | 9.495929 | 10.029259 | 9.879756 | 9.448741 | 11.298292 | 9.440401 | 9.506757 | 10.696501 | 9.732828 | 9.634405 | 9.598032 | 9.545018 | 9.328854 | 9.371253 | 10.745522 | 9.649237 |
2211.01186 | Alessandro Torrielli | Alessandro Torrielli | LonTI Lectures on Sine-Gordon and Thirring | 40 pages, pdfLaTeX; many figures; comments are welcome | null | null | DMUS-MP-22/20 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is the extended write-up of a series of lectures on the duality between
the Sine-Gordon model and the Thirring model. Prepared for the London Theory
Institute (LonTI) - Fall 2022: a PhD-level mini-course, with exercises and a
guide to the literature.
| [
{
"created": "Wed, 2 Nov 2022 15:02:23 GMT",
"version": "v1"
}
] | 2022-11-03 | [
[
"Torrielli",
"Alessandro",
""
]
] | This is the extended write-up of a series of lectures on the duality between the Sine-Gordon model and the Thirring model. Prepared for the London Theory Institute (LonTI) - Fall 2022: a PhD-level mini-course, with exercises and a guide to the literature. | 20.113691 | 16.713682 | 17.170988 | 15.550531 | 17.855177 | 18.736189 | 15.925501 | 15.264002 | 12.819455 | 19.074785 | 16.504755 | 15.363992 | 14.954625 | 14.42383 | 14.810803 | 15.487901 | 15.979937 | 15.504463 | 15.171509 | 15.346049 | 15.044477 |
2305.16940 | Ricardo Schiappa | Bertrand Eynard, Elba Garcia-Failde, Paolo Gregori, Danilo Lewanski,
Ricardo Schiappa | Resurgent Asymptotics of Jackiw-Teitelboim Gravity and the
Nonperturbative Topological Recursion | 63 pages, 52 plots in 16 figures, jheppub-nosort.sty; v2: minor
corrections/typos | null | null | CERN-TH-2021-097 | hep-th math-ph math.AG math.MP math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Jackiw-Teitelboim dilaton-quantum-gravity localizes on a double-scaled
random-matrix model, whose perturbative free energy is an asymptotic series.
Understanding the resurgent properties of this asymptotic series, including its
completion into a full transseries, requires understanding the nonperturbative
instanton s... | [
{
"created": "Fri, 26 May 2023 13:56:48 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Dec 2023 14:11:12 GMT",
"version": "v2"
}
] | 2023-12-19 | [
[
"Eynard",
"Bertrand",
""
],
[
"Garcia-Failde",
"Elba",
""
],
[
"Gregori",
"Paolo",
""
],
[
"Lewanski",
"Danilo",
""
],
[
"Schiappa",
"Ricardo",
""
]
] | Jackiw-Teitelboim dilaton-quantum-gravity localizes on a double-scaled random-matrix model, whose perturbative free energy is an asymptotic series. Understanding the resurgent properties of this asymptotic series, including its completion into a full transseries, requires understanding the nonperturbative instanton sec... | 11.537295 | 11.159012 | 14.788461 | 10.494055 | 10.721423 | 11.442915 | 10.160895 | 10.214894 | 10.351032 | 13.848577 | 9.902038 | 11.028019 | 11.667389 | 11.187286 | 11.412641 | 11.249113 | 10.665341 | 10.854553 | 10.756233 | 11.487209 | 10.843992 |
hep-th/0404054 | Paolo Aschieri | Paolo Aschieri | Non-Commutative GUTs, Standard Model and C,P,T properties from
Seiberg-Witten map | 9 pages. Presented at the Balkan Workshop 2003, Vrnjacka Banja,
29.8-2.9.2003 and at the 9th Adriatic Meeting, Dubrovnik, 4-14.9.2003 | SpringerProc.Phys.98:285-292,2005 | 10.1007/3-540-26798-0_27 | null | hep-th hep-ph | null | Noncommutative generalizations of Yang-Mills theories using Seiberg-Witten
map are in general not unique. We study these ambiguities and see that SO(10)
GUT, at first order in the noncommutativity parameter \theta, is unique and
therefore is a truly unified theory, while SU(5) is not. We then present the
noncommutati... | [
{
"created": "Tue, 6 Apr 2004 18:27:17 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Aschieri",
"Paolo",
""
]
] | Noncommutative generalizations of Yang-Mills theories using Seiberg-Witten map are in general not unique. We study these ambiguities and see that SO(10) GUT, at first order in the noncommutativity parameter \theta, is unique and therefore is a truly unified theory, while SU(5) is not. We then present the noncommutative... | 8.406043 | 7.529893 | 8.27373 | 8.01252 | 8.178998 | 8.363183 | 8.33906 | 7.576704 | 7.740757 | 9.072234 | 7.64507 | 7.641072 | 7.915663 | 7.354694 | 7.790664 | 8.207499 | 7.424286 | 7.619558 | 7.524025 | 7.889148 | 7.594676 |
hep-th/9801122 | Herbert Liebl | W. Kummer, H. Liebl (Vienna, Tech. U.), D.V. Vassilevich (St.
Petersburg University) | Comment on: ``Trace anomaly of dilaton coupled scalars in two
dimensions'' | 2 pages | Phys. Rev. D 58, 108501 (1998) | 10.1103/PhysRevD.58.108501 | TUW-98-03 | hep-th gr-qc | null | The trace anomaly for nonminimally coupled scalars in spherically reduced
gravity obtained by Bousso and Hawking (hep-th/9705236) is incorrect. We
explain the reasons for the deviations from our correct (published) result
which is supported by several other recent papers.
| [
{
"created": "Sun, 18 Jan 1998 16:31:10 GMT",
"version": "v1"
}
] | 2016-08-25 | [
[
"Kummer",
"W.",
"",
"Vienna, Tech. U."
],
[
"Liebl",
"H.",
"",
"Vienna, Tech. U."
],
[
"Vassilevich",
"D. V.",
"",
"St.\n Petersburg University"
]
] | The trace anomaly for nonminimally coupled scalars in spherically reduced gravity obtained by Bousso and Hawking (hep-th/9705236) is incorrect. We explain the reasons for the deviations from our correct (published) result which is supported by several other recent papers. | 16.104094 | 14.379406 | 15.589138 | 11.867712 | 13.936769 | 15.621158 | 15.788456 | 14.439134 | 15.217441 | 18.340837 | 12.953263 | 12.426955 | 15.357249 | 14.691828 | 12.458938 | 12.990233 | 13.468787 | 14.030769 | 13.506533 | 14.78704 | 12.646313 |
1201.0449 | Wout Merbis | Eric A. Bergshoeff, Sjoerd de Haan, Wout Merbis, Massimo Porrati and
Jan Rosseel | Unitary Truncations and Critical Gravity: a Toy Model | 23 pages. As accepted for publication in JHEP | JHEP 1204 (2012), 134 | 10.1007/JHEP04(2012)134 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a higher-derivative scalar field model in a fixed d+1
dimensional AdS background as a toy model for a gravitational dual to a
higher-rank logarithmic CFT. The holographic two-point correlation functions on
the boundary agree with higher-rank LCFT correlation functions. For odd rank,
the theory allows f... | [
{
"created": "Mon, 2 Jan 2012 10:27:57 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Apr 2012 12:01:42 GMT",
"version": "v2"
},
{
"created": "Mon, 7 May 2012 12:35:26 GMT",
"version": "v3"
}
] | 2012-05-08 | [
[
"Bergshoeff",
"Eric A.",
""
],
[
"de Haan",
"Sjoerd",
""
],
[
"Merbis",
"Wout",
""
],
[
"Porrati",
"Massimo",
""
],
[
"Rosseel",
"Jan",
""
]
] | We investigate a higher-derivative scalar field model in a fixed d+1 dimensional AdS background as a toy model for a gravitational dual to a higher-rank logarithmic CFT. The holographic two-point correlation functions on the boundary agree with higher-rank LCFT correlation functions. For odd rank, the theory allows for... | 12.593358 | 11.579844 | 13.003325 | 10.763683 | 10.92745 | 11.801188 | 10.859269 | 11.285814 | 11.252778 | 14.684852 | 10.930176 | 11.182135 | 12.22975 | 11.405119 | 11.453498 | 11.640687 | 11.479907 | 11.350187 | 10.885162 | 11.769718 | 11.136896 |
1409.0571 | Gianluca Zoccarato | Hirotaka Hayashi, Gianluca Zoccarato | Exact partition functions of Higgsed 5d $T_N$ theories | 54 pages, 13 figures, v2. added an appendix and minor changes in the
main text, version accepted on JHEP | null | 10.1007/JHEP01(2015)093 | IFT-UAM/CSIC-14-089 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a general prescription by which we can systematically compute
exact partition functions of five-dimensional supersymmetric theories which
arise in Higgs branches of the $T_N$ theory. The theories may be realized by
webs of 5-branes whose dual geometries are non-toric. We have checked our
method by calculat... | [
{
"created": "Mon, 1 Sep 2014 22:07:22 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Jan 2015 10:45:27 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Hayashi",
"Hirotaka",
""
],
[
"Zoccarato",
"Gianluca",
""
]
] | We present a general prescription by which we can systematically compute exact partition functions of five-dimensional supersymmetric theories which arise in Higgs branches of the $T_N$ theory. The theories may be realized by webs of 5-branes whose dual geometries are non-toric. We have checked our method by calculatin... | 6.453619 | 5.353121 | 7.382922 | 5.528012 | 5.928221 | 5.835231 | 5.886068 | 5.758665 | 5.732626 | 7.387918 | 5.689671 | 5.447313 | 6.544995 | 5.729399 | 5.563851 | 5.562236 | 5.836042 | 5.640442 | 5.586688 | 6.178755 | 5.615118 |
hep-th/9809213 | Dmitri Sorokin | Paolo Pasti, Dmitri Sorokin and Mario Tonin | On gauge-fixed superbrane actions in AdS superbackgrounds | LaTeX file, 10 pages. Minor corrections, version to appear in PLB | Phys.Lett. B447 (1999) 251-256 | 10.1016/S0370-2693(98)01597-4 | HUB EP-98/66, DFPB 98/TH/45 | hep-th | null | To construct actions for describing superbranes propagating in AdS x S
superbackgrounds we propose a coset space realization of these superbackgrounds
which results in a short polynomial fermionic dependence (up to the sixth power
in Grassmann coordinates) of target superspace supervielbeins and
superconnections. Gau... | [
{
"created": "Wed, 30 Sep 1998 18:11:10 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Oct 1998 19:07:54 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Jan 1999 17:41:54 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Pasti",
"Paolo",
""
],
[
"Sorokin",
"Dmitri",
""
],
[
"Tonin",
"Mario",
""
]
] | To construct actions for describing superbranes propagating in AdS x S superbackgrounds we propose a coset space realization of these superbackgrounds which results in a short polynomial fermionic dependence (up to the sixth power in Grassmann coordinates) of target superspace supervielbeins and superconnections. Gauge... | 13.507725 | 10.370215 | 14.686942 | 10.869003 | 11.86602 | 11.254996 | 11.132109 | 10.809965 | 11.075301 | 15.557801 | 11.042517 | 10.641405 | 13.223559 | 11.527396 | 11.099697 | 10.752851 | 11.362886 | 11.259951 | 11.558191 | 12.972027 | 11.070327 |
hep-th/9801059 | Valeri Dvoeglazov | Valeri V. Dvoeglazov (Universidad Autonoma de Zacatecas) | More about the S=1 relativistic oscillator | ReVTeX file, 7pp., no figures | Int.J.Theor.Phys. 39 (2000) 2011-2017 | null | EFUAZ FT-96-40-REV | hep-th math-ph math.MP | null | Following to the lines drawn in my previous paper about the S=0 relativistic
oscillator I build up an oscillatorlike system which can be named as the S=1
Proca oscillator. The Proca field function is obtained in the framework of the
Bargmann-Wigner prescription and the interaction is introduced similarly to the
S=1/2... | [
{
"created": "Sun, 11 Jan 1998 00:09:49 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dvoeglazov",
"Valeri V.",
"",
"Universidad Autonoma de Zacatecas"
]
] | Following to the lines drawn in my previous paper about the S=0 relativistic oscillator I build up an oscillatorlike system which can be named as the S=1 Proca oscillator. The Proca field function is obtained in the framework of the Bargmann-Wigner prescription and the interaction is introduced similarly to the S=1/2 D... | 11.317329 | 11.81948 | 11.986173 | 10.668185 | 11.009244 | 11.393036 | 11.730556 | 12.417108 | 11.527438 | 12.157616 | 11.301022 | 11.08804 | 11.341323 | 10.479381 | 10.595039 | 11.029469 | 11.138176 | 10.844007 | 10.756016 | 10.900693 | 10.919123 |
1511.01659 | Gennady Stepanovich Danilov | G. S. Danilov | Calculation of multi-loop superstring amplitudes | 47 pages, LATEX | null | 10.1088/0264-9381/33/23/235012 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Multi-loop interaction amplitudes in the theory of the closed, oriented
superstrings are obtained by the integration of local amplitudes which are
represented by a sum of the spinning string local amplitudes. The last local
amplitudes are given explicitly through super-Schottky group parameters and
interaction vertex... | [
{
"created": "Thu, 5 Nov 2015 09:04:43 GMT",
"version": "v1"
}
] | 2016-11-15 | [
[
"Danilov",
"G. S.",
""
]
] | Multi-loop interaction amplitudes in the theory of the closed, oriented superstrings are obtained by the integration of local amplitudes which are represented by a sum of the spinning string local amplitudes. The last local amplitudes are given explicitly through super-Schottky group parameters and interaction vertex c... | 16.45207 | 15.094306 | 19.227049 | 14.810843 | 17.182795 | 16.659338 | 17.171114 | 15.812572 | 14.733437 | 20.596699 | 15.138328 | 15.242237 | 16.736336 | 16.196779 | 15.343731 | 15.618268 | 15.645624 | 15.401464 | 15.484707 | 16.629639 | 15.33639 |
1911.10343 | Damiano Anselmi | Damiano Anselmi | Fakeons, quantum gravity and the correspondence principle | Proceedings of the conference "Progress and Visions in Quantum Theory
in View of Gravity: Bridging foundations of physics and mathematics", Max
Planck Institute for Mathematics in the Sciences, Leipzig, October 2018 - to
appear in a book with the same title edited by F. Finster, D. Giulini, J.
Kleiner and J. To... | null | null | null | hep-th gr-qc hep-ph physics.hist-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The correspondence principle made of unitarity, locality and
renormalizability has been very successful in quantum field theory. Among the
other things, it helped us build the standard model. However, it also showed
important limitations. For example, it failed to restrict the gauge group and
the matter sector in a p... | [
{
"created": "Sat, 23 Nov 2019 10:11:28 GMT",
"version": "v1"
}
] | 2019-11-27 | [
[
"Anselmi",
"Damiano",
""
]
] | The correspondence principle made of unitarity, locality and renormalizability has been very successful in quantum field theory. Among the other things, it helped us build the standard model. However, it also showed important limitations. For example, it failed to restrict the gauge group and the matter sector in a pow... | 5.146401 | 10.488672 | 11.512642 | 9.930078 | 10.044188 | 9.474844 | 10.109534 | 9.800478 | 10.22998 | 11.305644 | 9.46498 | 8.484369 | 8.402711 | 7.51683 | 7.200187 | 7.888948 | 7.616181 | 7.917443 | 7.815521 | 8.132541 | 7.572653 |
1107.4886 | Juan Mateos Guilarte | M. A. Gonzalez Leon, M. de la Torre Mayado, J. Mateos Guilarte, and
M.J. Senosiain | On the Supersymmetric Spectra of two Planar Integrable Quantum Systems | LaTex file, 39 pages, 18 Figures. Expanded version of lectures given
by JMG at Benasque, Spain, July 2010, and the Jairo Charris Seminar in Santa
Marta, Colombia, August 2010 | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Two planar supersymmetric quantum mechanical systems built around the quantum
integrable Kepler/Coulomb and Euler/Coulomb problems are analyzed in depth. The
supersymmetric spectra of both systems are unveiled, profiting from symmetry
operators not related to invariance with respect to rotations. It is shown
analytic... | [
{
"created": "Mon, 25 Jul 2011 10:33:35 GMT",
"version": "v1"
}
] | 2011-07-26 | [
[
"Leon",
"M. A. Gonzalez",
""
],
[
"Mayado",
"M. de la Torre",
""
],
[
"Guilarte",
"J. Mateos",
""
],
[
"Senosiain",
"M. J.",
""
]
] | Two planar supersymmetric quantum mechanical systems built around the quantum integrable Kepler/Coulomb and Euler/Coulomb problems are analyzed in depth. The supersymmetric spectra of both systems are unveiled, profiting from symmetry operators not related to invariance with respect to rotations. It is shown analytical... | 13.491715 | 14.535692 | 14.651832 | 12.932768 | 15.797745 | 14.650887 | 14.603759 | 14.255878 | 13.427971 | 16.799805 | 12.345732 | 12.940586 | 12.839001 | 12.699557 | 13.394052 | 12.90435 | 11.945292 | 12.616131 | 12.910663 | 13.4815 | 12.459933 |
hep-th/9801119 | Arthur Jaffe | Arthur Jaffe | Quantum Invariants | 13 pages, Latex | Commun.Math.Phys.209:1-12,2000 | 10.1007/PL00005524 | HUTMP 97/B370 | hep-th | null | In super-symmetric quantum theory, or in string theory, (including
generalizations of these theories to underlying quantum spaces) we study a
certain partition function Z(Q,A,g). Here Q denotes a supercharge, A denotes an
observable with the property A^2 = I, and g denotes an element of a symmetry
group of Q. The sup... | [
{
"created": "Sat, 17 Jan 1998 23:35:06 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Jaffe",
"Arthur",
""
]
] | In super-symmetric quantum theory, or in string theory, (including generalizations of these theories to underlying quantum spaces) we study a certain partition function Z(Q,A,g). Here Q denotes a supercharge, A denotes an observable with the property A^2 = I, and g denotes an element of a symmetry group of Q. The super... | 13.58425 | 14.097245 | 14.340533 | 12.317496 | 12.791165 | 13.9146 | 13.640018 | 13.004498 | 13.023204 | 16.571583 | 12.151606 | 12.526401 | 13.057592 | 12.19797 | 11.721995 | 11.881737 | 12.029892 | 12.028295 | 12.390583 | 13.109408 | 11.947376 |
1611.02179 | Jyotirmoy Bhattacharya | Jyotirmoy Bhattacharya and Arthur E. Lipstein | 6d Dual Conformal Symmetry and Minimal Volumes in AdS | v1: 17+5 pages, 9 figures, v2: Published version; new references
added | Journal of High Energy Physics, 2016(12), 1-24 | 10.1007/JHEP12(2016)105 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The S-matrix of a theory often exhibits symmetries which are not manifest
from the viewpoint of its Lagrangian. For instance, powerful constraints on
scattering amplitudes are imposed by the dual conformal symmetry of planar 4d
$\mathcal{N}=4$ super Yang-Mills theory and the ABJM theory. Motivated by this,
we investi... | [
{
"created": "Mon, 7 Nov 2016 17:21:00 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Dec 2016 15:06:27 GMT",
"version": "v2"
}
] | 2016-12-30 | [
[
"Bhattacharya",
"Jyotirmoy",
""
],
[
"Lipstein",
"Arthur E.",
""
]
] | The S-matrix of a theory often exhibits symmetries which are not manifest from the viewpoint of its Lagrangian. For instance, powerful constraints on scattering amplitudes are imposed by the dual conformal symmetry of planar 4d $\mathcal{N}=4$ super Yang-Mills theory and the ABJM theory. Motivated by this, we investiga... | 6.368114 | 7.131765 | 8.085755 | 6.972307 | 7.003779 | 7.067645 | 6.779067 | 7.027892 | 6.948225 | 8.287684 | 6.707871 | 6.48995 | 6.954095 | 6.742255 | 6.615864 | 6.682214 | 6.616466 | 6.590958 | 6.688864 | 6.994565 | 6.524054 |
hep-th/0606275 | Riccardo Sturani | J. L. Cornou, E. Pajer, R. Sturani | Graviton production from D-string recombination and annihilation | 28 pages, 3 figures | Nucl.Phys.B756:16-37,2006 | 10.1016/j.nuclphysb.2006.08.018 | null | hep-th gr-qc | null | Fundamental superstrings (F-strings) and D-strings may be produced at high
temperature in the early Universe. Assuming that, we investigate if any of the
instabilities present in systems of strings and branes can give rise to a
phenomenologically interesting production of gravitons. We focus on D-strings
and find tha... | [
{
"created": "Thu, 29 Jun 2006 13:51:32 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cornou",
"J. L.",
""
],
[
"Pajer",
"E.",
""
],
[
"Sturani",
"R.",
""
]
] | Fundamental superstrings (F-strings) and D-strings may be produced at high temperature in the early Universe. Assuming that, we investigate if any of the instabilities present in systems of strings and branes can give rise to a phenomenologically interesting production of gravitons. We focus on D-strings and find that ... | 13.331372 | 13.578847 | 12.060284 | 12.66041 | 13.880507 | 12.945977 | 12.829304 | 12.866714 | 13.010163 | 12.830542 | 13.004963 | 12.847105 | 12.494967 | 12.848498 | 12.433529 | 12.827954 | 13.156335 | 13.142933 | 12.685355 | 13.298925 | 12.19591 |
hep-th/0703251 | Amitabh Virmani | Donald Marolf, Amitabh Virmani | Holographic Renormalization of Gravity in Little String Theory Duals | 29 pages; v2 refs added; v3 typos fixed | JHEP 0706:042,2007 | 10.1088/1126-6708/2007/06/042 | null | hep-th | null | We perform a holographic renormalization of gravity duals to little string
theories. In particular, we construct counterterms which yield a well-defined
type II action for NS-sector linear dilaton backgrounds. Our methods are based
on a similar recent construction in asymptotically flat spacetimes, and our
work demon... | [
{
"created": "Wed, 28 Mar 2007 08:20:21 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Apr 2007 17:00:08 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Jun 2007 18:05:09 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Marolf",
"Donald",
""
],
[
"Virmani",
"Amitabh",
""
]
] | We perform a holographic renormalization of gravity duals to little string theories. In particular, we construct counterterms which yield a well-defined type II action for NS-sector linear dilaton backgrounds. Our methods are based on a similar recent construction in asymptotically flat spacetimes, and our work demonst... | 8.192834 | 8.808029 | 8.786952 | 7.770609 | 9.076442 | 8.488485 | 8.445935 | 7.991858 | 8.152645 | 9.68661 | 7.678837 | 7.449214 | 8.235951 | 7.662506 | 7.844569 | 7.741917 | 7.728734 | 7.962203 | 7.652761 | 8.147088 | 7.525261 |
hep-th/9606068 | Fedor Smirnov | O. Babelon, D. Bernard, F.A. Smirnov | Null-vectors in Integrable Field Theory | 36 pages, Latex | Commun.Math.Phys.186:601-648,1997 | 10.1007/s002200050122 | null | hep-th | null | The form factor bootstrap approach allows to construct the space of local
fields in the massive restricted sine-Gordon model. This space has to be
isomorphic to that of the corresponding minimal model of conformal field
theory. We describe the subspaces which correspond to the Verma modules of
primary fields in terms... | [
{
"created": "Wed, 12 Jun 1996 16:03:30 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Feb 1997 12:37:31 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Babelon",
"O.",
""
],
[
"Bernard",
"D.",
""
],
[
"Smirnov",
"F. A.",
""
]
] | The form factor bootstrap approach allows to construct the space of local fields in the massive restricted sine-Gordon model. This space has to be isomorphic to that of the corresponding minimal model of conformal field theory. We describe the subspaces which correspond to the Verma modules of primary fields in terms o... | 8.851518 | 8.79253 | 9.858679 | 7.968323 | 8.364014 | 8.978519 | 9.214275 | 8.380906 | 8.822553 | 10.651985 | 8.344172 | 8.241372 | 9.459282 | 8.099902 | 8.023369 | 8.082475 | 8.129724 | 8.202497 | 8.2548 | 8.948303 | 8.033995 |
hep-th/9412055 | D'Hoker | Eric D'Hoker, Pierre Sikivie and Youli Kanev | Casimir Forces between Beads on Strings and Membranes | Plain Tex, Tables.tex macro required, 9 pages | Phys.Lett. B347 (1995) 56-62 | 10.1016/0370-2693(95)00050-U | UCLA/94/TEP/44 and UFIFT-HEP-94-17 | hep-th cond-mat | null | We develop a general formalism to calculate the force between beads attached
to a flat $d$-dimensional membrane due to the quantum fluctuations of the
membrane. The interaction potential is derived as a function of $d$ and the
membrane energy density, tension, stiffness and temperature. We find that the
induced inter... | [
{
"created": "Tue, 6 Dec 1994 04:33:35 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"D'Hoker",
"Eric",
""
],
[
"Sikivie",
"Pierre",
""
],
[
"Kanev",
"Youli",
""
]
] | We develop a general formalism to calculate the force between beads attached to a flat $d$-dimensional membrane due to the quantum fluctuations of the membrane. The interaction potential is derived as a function of $d$ and the membrane energy density, tension, stiffness and temperature. We find that the induced interac... | 10.306359 | 9.314732 | 9.575582 | 9.43944 | 10.162147 | 10.584186 | 10.357783 | 9.93843 | 9.320537 | 11.390689 | 9.169776 | 9.940418 | 9.528204 | 9.326182 | 9.250864 | 9.356398 | 9.198899 | 9.760915 | 9.848237 | 9.698667 | 9.566162 |
hep-th/0209005 | Lahouari Mesref | L. Mesref | A Map between q-deformed and ordinary Gauge Theories | Latex,15 pages, references added and some misprints corrected | New J.Phys. 5 (2003) 7 | 10.1088/1367-2630/5/1/307 | null | hep-th | null | In complete analogy with Seiberg-Witten map defined in noncommutative
geometry we introduce a new map between a q-deformed gauge theory and an
ordinary gauge theory. The construction of this map is elaborated in order to
fit the Hopf algebra structure.
| [
{
"created": "Sat, 31 Aug 2002 17:14:28 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Sep 2002 13:37:33 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Sep 2002 16:00:32 GMT",
"version": "v3"
},
{
"created": "Thu, 17 Apr 2003 14:35:36 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Mesref",
"L.",
""
]
] | In complete analogy with Seiberg-Witten map defined in noncommutative geometry we introduce a new map between a q-deformed gauge theory and an ordinary gauge theory. The construction of this map is elaborated in order to fit the Hopf algebra structure. | 11.452897 | 8.321961 | 8.886045 | 7.849667 | 8.311204 | 7.941842 | 8.73675 | 7.641194 | 8.358095 | 11.149467 | 8.147251 | 8.428847 | 9.221752 | 8.576717 | 8.257003 | 8.510421 | 8.569757 | 8.372478 | 8.906864 | 9.48687 | 9.073285 |
2206.05951 | Ma-Ke Yuan | Yilu Shao, Ma-Ke Yuan, Yang Zhou | Entanglement Negativity and Defect Extremal Surface | null | SciPost Phys. Core 7, 027 (2024) | 10.21468/SciPostPhysCore.7.2.027 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study entanglement negativity for evaporating black hole based on the
holographic model with defect brane. We introduce a defect extremal surface
formula for entanglement negativity. Based on partial reduction, we show the
equivalence between defect extremal surface formula and island formula for
entanglement nega... | [
{
"created": "Mon, 13 Jun 2022 07:46:25 GMT",
"version": "v1"
},
{
"created": "Sun, 3 Sep 2023 12:13:47 GMT",
"version": "v2"
},
{
"created": "Mon, 11 Mar 2024 12:17:42 GMT",
"version": "v3"
},
{
"created": "Sun, 14 Jul 2024 02:50:48 GMT",
"version": "v4"
}
] | 2024-07-16 | [
[
"Shao",
"Yilu",
""
],
[
"Yuan",
"Ma-Ke",
""
],
[
"Zhou",
"Yang",
""
]
] | We study entanglement negativity for evaporating black hole based on the holographic model with defect brane. We introduce a defect extremal surface formula for entanglement negativity. Based on partial reduction, we show the equivalence between defect extremal surface formula and island formula for entanglement negati... | 11.526501 | 9.644966 | 12.045551 | 9.289889 | 9.406296 | 9.625526 | 9.801011 | 9.535301 | 8.97217 | 14.341627 | 9.728992 | 9.996117 | 11.360053 | 10.014565 | 10.378672 | 10.526364 | 10.298057 | 9.761022 | 10.198076 | 11.286635 | 9.865305 |
hep-th/9612042 | Kiyoshi Kamimura | J. Gomis, K.Kamimura and R.Kuriki | Nambu-Goldstone Fields, Anomalies and WZ Terms | 19 pages, Latex | Nucl.Phys. B496 (1997) 465-485 | 10.1016/S0550-3213(97)00241-1 | UTTG-18-96, UB-ECM-PF 96/19, TOHO-FP-9654, TIT/HEP-347 | hep-th | null | We construct the Wess-Zumino terms from anomalies in case of quasigroups for
the following situations. One is effective gauge field theories of
Nambu-Goldstone fields associated with spontaneously broken global symmetries
and the other is anomalous gauge theories. The formalism that we will develop
can be seen as a g... | [
{
"created": "Wed, 4 Dec 1996 04:34:56 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Dec 1996 03:02:33 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Gomis",
"J.",
""
],
[
"Kamimura",
"K.",
""
],
[
"Kuriki",
"R.",
""
]
] | We construct the Wess-Zumino terms from anomalies in case of quasigroups for the following situations. One is effective gauge field theories of Nambu-Goldstone fields associated with spontaneously broken global symmetries and the other is anomalous gauge theories. The formalism that we will develop can be seen as a gen... | 11.811448 | 11.883349 | 13.092545 | 11.094474 | 11.820294 | 11.330553 | 11.441895 | 10.643413 | 11.03585 | 13.481573 | 10.398915 | 10.803099 | 12.13927 | 11.249354 | 10.90042 | 11.173138 | 11.159624 | 11.083783 | 11.357121 | 11.446256 | 10.851171 |
hep-th/9207010 | null | Katsushi Ito, Jens Ole Madsen and Jens Lyng Petersen | Free Field Representations and Screening Operators for the $N=4$ Doubly
Extended Superconformal Algebras | 15 pages, Latex | Phys.Lett. B292 (1992) 298-306 | 10.1016/0370-2693(92)91179-D | NBI-HE-92-43 | hep-th | null | We present explicit free field representations for the $N=4$ doubly extended
superconformal algebra, $\tilde{\cal{A}}_{\gamma}$. This algebra generalizes
and contains all previous $N=4$ superconformal algebras. We have found
$\tilde{\cal{A}}_{\gamma}$ to be obtained by hamiltonian reduction of the Lie
superalgebra $D... | [
{
"created": "Fri, 3 Jul 1992 15:21:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ito",
"Katsushi",
""
],
[
"Madsen",
"Jens Ole",
""
],
[
"Petersen",
"Jens Lyng",
""
]
] | We present explicit free field representations for the $N=4$ doubly extended superconformal algebra, $\tilde{\cal{A}}_{\gamma}$. This algebra generalizes and contains all previous $N=4$ superconformal algebras. We have found $\tilde{\cal{A}}_{\gamma}$ to be obtained by hamiltonian reduction of the Lie superalgebra $D(2... | 9.27822 | 9.379551 | 9.938556 | 8.628085 | 8.427798 | 8.30399 | 8.728665 | 8.234871 | 8.175692 | 10.709979 | 7.954043 | 8.368868 | 9.223184 | 8.375032 | 8.80329 | 8.674991 | 8.768698 | 8.158705 | 8.634624 | 8.991291 | 8.428855 |
1912.10779 | Paulo Jos\'e Ferreira Porf\'irio Da Silva | J. R. Nascimento, Gonzalo J. Olmo, P. J. Porf\'irio, A. Yu. Petrov, A.
R. Soares | Nonlinear $\sigma$-models in the Eddington-inspired Born-Infeld Gravity | 19 pages, 5 figures | Phys. Rev. D 101, 064043 (2020) | 10.1103/PhysRevD.101.064043 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we consider two different nonlinear $\sigma$-models minimally
coupled to Eddington-inspired Born-Infeld gravity. We show that the resultant
geometries represent minimal modifications with respect to those found in GR,
though with important physical consequences. In particular, wormhole structures
always... | [
{
"created": "Mon, 23 Dec 2019 13:02:01 GMT",
"version": "v1"
}
] | 2020-03-25 | [
[
"Nascimento",
"J. R.",
""
],
[
"Olmo",
"Gonzalo J.",
""
],
[
"Porfírio",
"P. J.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"Soares",
"A. R.",
""
]
] | In this paper we consider two different nonlinear $\sigma$-models minimally coupled to Eddington-inspired Born-Infeld gravity. We show that the resultant geometries represent minimal modifications with respect to those found in GR, though with important physical consequences. In particular, wormhole structures always a... | 11.983895 | 11.233528 | 10.33349 | 10.638219 | 11.544812 | 10.744984 | 11.731524 | 10.86883 | 10.944667 | 10.370121 | 11.200999 | 10.753346 | 10.33182 | 10.606504 | 10.636147 | 11.087287 | 11.098199 | 10.431937 | 10.887875 | 10.764938 | 10.822875 |
hep-th/9309022 | Hector DE Vega | H. J. de Vega and A. Gonz\'alez--Ruiz | Exact solution of the $SU_{q}(n)$ invariant quantum spin chains | 29 pages | Nucl.Phys. B417 (1994) 553-578 | 10.1016/0550-3213(94)90484-7 | LPTHE 93-38 | hep-th math.QA | null | The Nested Bethe Ansatz is generalized to open boundary conditions. This is
used to find the exact eigenvectors and eigenvalues of the $A_{n-1}$ vertex
model with fixed open boundary conditions and the corresponding $SU_{q}(n)$
invariant hamiltonian.
The Bethe Ansatz equations obtained are solved in the thermodynam... | [
{
"created": "Fri, 3 Sep 1993 14:39:36 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"de Vega",
"H. J.",
""
],
[
"González--Ruiz",
"A.",
""
]
] | The Nested Bethe Ansatz is generalized to open boundary conditions. This is used to find the exact eigenvectors and eigenvalues of the $A_{n-1}$ vertex model with fixed open boundary conditions and the corresponding $SU_{q}(n)$ invariant hamiltonian. The Bethe Ansatz equations obtained are solved in the thermodynamic l... | 8.049354 | 6.664325 | 10.676386 | 6.96863 | 7.952862 | 7.580227 | 6.866021 | 6.593346 | 6.914138 | 9.681148 | 7.288157 | 7.469135 | 8.614366 | 7.872617 | 7.933753 | 7.447036 | 7.831732 | 7.720162 | 7.642183 | 8.934417 | 7.69113 |
2101.03953 | Akimi Watanabe | Koichi Harada, Yutaka Matsuo, Go Noshita and Akimi Watanabe | $q$-Deformation of Corner Vertex Operator Algebras by Miura
Transformation | 53 pages; typos corrected, references added | null | 10.1007/JHEP04(2021)202 | null | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, Gaiotto and Rapcak proposed a generalization of $W_N$ algebra by
considering the symmetry at the corner of the brane intersection (corner vertex
operator algebra). The algebra, denoted as $Y_{L,M,N}$, is characterized by
three non-negative integers $L, M, N$. It has a manifest triality automorphism
which in... | [
{
"created": "Mon, 11 Jan 2021 15:10:22 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Jan 2021 12:42:21 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Mar 2021 14:36:10 GMT",
"version": "v3"
}
] | 2021-05-12 | [
[
"Harada",
"Koichi",
""
],
[
"Matsuo",
"Yutaka",
""
],
[
"Noshita",
"Go",
""
],
[
"Watanabe",
"Akimi",
""
]
] | Recently, Gaiotto and Rapcak proposed a generalization of $W_N$ algebra by considering the symmetry at the corner of the brane intersection (corner vertex operator algebra). The algebra, denoted as $Y_{L,M,N}$, is characterized by three non-negative integers $L, M, N$. It has a manifest triality automorphism which inte... | 6.149517 | 5.908086 | 7.344297 | 5.692109 | 6.154154 | 6.349769 | 5.861991 | 5.976508 | 6.058138 | 8.477761 | 5.97394 | 5.943481 | 6.428603 | 5.940398 | 5.977402 | 5.832914 | 5.915254 | 5.973387 | 5.934777 | 6.434101 | 5.806767 |
hep-th/9510130 | Neil Lambert | N.D. Lambert | Two Loop Renormalization of Massive (p,q) Supersymmetric Sigma Models | 43 pages phyzzx with 5 figures | Nucl.Phys. B469 (1996) 68-92 | 10.1016/0550-3213(96)00152-6 | DAMTP R/94/42 | hep-th | null | We calculate the beta-functions of the general massive (p,q) supersymmetric
sigma model to two loop order using (1,0) superfields. The conditions for
finiteness are discussed in relation to (p,q) supersymmetry. We also calculate
the effective potential using component fields to one loop order and consider
the possibi... | [
{
"created": "Wed, 18 Oct 1995 14:58:18 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Lambert",
"N. D.",
""
]
] | We calculate the beta-functions of the general massive (p,q) supersymmetric sigma model to two loop order using (1,0) superfields. The conditions for finiteness are discussed in relation to (p,q) supersymmetry. We also calculate the effective potential using component fields to one loop order and consider the possibili... | 8.337798 | 7.624622 | 8.216846 | 7.385162 | 7.449609 | 7.370739 | 7.502079 | 7.523695 | 7.433156 | 9.782036 | 7.847442 | 7.711423 | 8.875605 | 7.988467 | 8.001207 | 7.759408 | 7.618297 | 7.77725 | 7.812057 | 8.939178 | 7.843897 |
1501.00004 | Zhang-Yu Nie | Zhang-Yu Nie, Rong-Gen Cai, Xin Gao, Li Li, Hui Zeng | Phase transitions in a holographic s+p model with backreaction | 15 pages(two-column), 9 figures | Eur.Phys.J. C75 (2015) 559 | 10.1140/epjc/s10052-015-3773-2 | CCTP-2015-01,CCQCN-2015-59 | hep-th cond-mat.supr-con gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a previous paper (arXiv:1309.2204, JHEP 1311 (2013) 087), we present a
holographic s+p superconductor model with a scalar triplet charged under an
SU(2) gauge field in the bulk. We also study the competition and coexistence of
the s-wave and p-wave orders in the probe limit. In this work we continue to
study the m... | [
{
"created": "Tue, 30 Dec 2014 21:00:06 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Dec 2015 15:46:03 GMT",
"version": "v2"
}
] | 2017-12-27 | [
[
"Nie",
"Zhang-Yu",
""
],
[
"Cai",
"Rong-Gen",
""
],
[
"Gao",
"Xin",
""
],
[
"Li",
"Li",
""
],
[
"Zeng",
"Hui",
""
]
] | In a previous paper (arXiv:1309.2204, JHEP 1311 (2013) 087), we present a holographic s+p superconductor model with a scalar triplet charged under an SU(2) gauge field in the bulk. We also study the competition and coexistence of the s-wave and p-wave orders in the probe limit. In this work we continue to study the mod... | 8.730655 | 8.249138 | 8.626715 | 7.90021 | 8.436672 | 8.413121 | 7.871922 | 8.009791 | 8.00105 | 9.455924 | 8.206074 | 8.37736 | 8.652381 | 8.491161 | 8.175548 | 8.247044 | 8.118651 | 8.335617 | 8.233391 | 8.754091 | 8.30457 |
1509.07790 | Yi Yin | Yuji Hirono, Dmitri Kharzeev and Yi Yin | Self-similar inverse cascade of magnetic helicity driven by the chiral
anomaly | 21 pages, 4 figures, published version | Phys. Rev. D 92, 125031 (2015) | 10.1103/PhysRevD.92.125031 | null | hep-th cond-mat.soft hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For systems with charged chiral fermions, the imbalance of chirality in the
presence of magnetic field generates an electric current - this is the Chiral
Magnetic Effect (CME). We study the dynamical real-time evolution of
electromagnetic fields coupled by the anomaly to the chiral charge density and
the CME current ... | [
{
"created": "Fri, 25 Sep 2015 16:59:05 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Jan 2016 13:03:23 GMT",
"version": "v2"
}
] | 2016-01-29 | [
[
"Hirono",
"Yuji",
""
],
[
"Kharzeev",
"Dmitri",
""
],
[
"Yin",
"Yi",
""
]
] | For systems with charged chiral fermions, the imbalance of chirality in the presence of magnetic field generates an electric current - this is the Chiral Magnetic Effect (CME). We study the dynamical real-time evolution of electromagnetic fields coupled by the anomaly to the chiral charge density and the CME current by... | 8.849036 | 9.249834 | 8.784815 | 7.844096 | 8.719587 | 9.633865 | 8.919901 | 8.973271 | 8.376813 | 9.561107 | 8.826785 | 8.784785 | 8.857976 | 8.510581 | 8.897544 | 8.954584 | 8.929987 | 8.813465 | 8.44293 | 8.974183 | 8.300584 |
0907.1178 | Zhang Li-Jie | Li-Jie Zhang, Guo-Hong Yang | Zero Modes of Matter Fields on Scalar Flat Thick Branes | 11 pages,no figures | null | 10.1142/S0217732309030515 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Zero modes of various matters with spin 0, 1 and 1/2 on a class of scalar
flat thick branes are discussed in this paper. We show that scalar field with
spin 0 is localized on all thick branes without additional condition, while
spin 1 vector field is not localized. In addition, for spin 1/2 fermionic
field, the zero ... | [
{
"created": "Tue, 7 Jul 2009 09:47:44 GMT",
"version": "v1"
}
] | 2015-05-13 | [
[
"Zhang",
"Li-Jie",
""
],
[
"Yang",
"Guo-Hong",
""
]
] | Zero modes of various matters with spin 0, 1 and 1/2 on a class of scalar flat thick branes are discussed in this paper. We show that scalar field with spin 0 is localized on all thick branes without additional condition, while spin 1 vector field is not localized. In addition, for spin 1/2 fermionic field, the zero mo... | 10.054927 | 7.344504 | 8.199657 | 7.345843 | 8.771669 | 8.024844 | 7.926816 | 7.245594 | 7.212739 | 7.872538 | 8.372053 | 7.550201 | 8.098135 | 7.811742 | 7.487166 | 7.790594 | 7.903169 | 7.604955 | 7.802821 | 7.760781 | 8.653666 |
hep-th/0209118 | Paolo Valtancoli | Paolo Valtancoli | Noncommutative instantons on $d=2n$ planes from matrix models | 20 pages, LaTeX, no figures | Int.J.Mod.Phys. A18 (2003) 1125 | 10.1142/S0217751X03013648 | null | hep-th | null | In the case of an invertible coordinate commutator matrix $\theta_{ij}$, we
derive a general instanton solution of the noncommutative gauge theories on
$d=2n$ planes given in terms of $n$ oscillators.
| [
{
"created": "Fri, 13 Sep 2002 18:51:18 GMT",
"version": "v1"
},
{
"created": "Sun, 15 Sep 2002 20:08:59 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Sep 2002 14:23:47 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Valtancoli",
"Paolo",
""
]
] | In the case of an invertible coordinate commutator matrix $\theta_{ij}$, we derive a general instanton solution of the noncommutative gauge theories on $d=2n$ planes given in terms of $n$ oscillators. | 17.834019 | 15.16143 | 16.259407 | 14.624521 | 15.885468 | 14.913402 | 17.771887 | 16.587257 | 13.777514 | 19.489861 | 14.547914 | 13.596589 | 14.301765 | 13.371203 | 13.545438 | 13.343408 | 13.529506 | 12.887698 | 14.062626 | 14.813046 | 13.609928 |
0902.2223 | Maciej A. Nowak | Jean-Paul Blaizot and Maciej A. Nowak | Universal shocks in random matrix theory | 4 pages, no figures | Phys.Rev.E82:051115,2010 | 10.1103/PhysRevE.82.051115 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We link the appearance of universal kernels in random matrix ensembles to the
phenomenon of shock formation in some fluid dynamical equations. Such equations
are derived from Dyson's random walks after a proper rescaling of the time. In
the case of the Gaussian Unitary Ensemble, on which we focus in this letter, we
s... | [
{
"created": "Thu, 12 Feb 2009 22:06:44 GMT",
"version": "v1"
}
] | 2011-02-28 | [
[
"Blaizot",
"Jean-Paul",
""
],
[
"Nowak",
"Maciej A.",
""
]
] | We link the appearance of universal kernels in random matrix ensembles to the phenomenon of shock formation in some fluid dynamical equations. Such equations are derived from Dyson's random walks after a proper rescaling of the time. In the case of the Gaussian Unitary Ensemble, on which we focus in this letter, we sho... | 9.819041 | 11.420831 | 11.186384 | 9.445143 | 9.701397 | 10.159563 | 10.065118 | 9.954677 | 10.211712 | 11.717849 | 9.512359 | 9.377614 | 9.792439 | 9.631916 | 9.695873 | 9.418848 | 9.774503 | 9.693883 | 9.713745 | 9.90601 | 9.33677 |
2206.11806 | Stefan Prohazka | Jos\'e Figueroa-O'Farrill, Ross Grassie and Stefan Prohazka | Lifshitz symmetry: Lie algebras, spacetimes and particles | 30 pages, 2 figures. (v2: added some references and acknowledgments,
v3: various minor updates) | SciPost Phys. 14, 035 (2023) | 10.21468/SciPostPhys.14.3.035 | EMPG-22-09 | hep-th cond-mat.str-el gr-qc math.DG | http://creativecommons.org/licenses/by/4.0/ | We study and classify Lie algebras, homogeneous spacetimes and coadjoint
orbits ("particles") of Lie groups generated by spatial rotations, temporal and
spatial translations and an additional scalar generator. As a first step we
classify Lie algebras of this type in arbitrary dimension. Among them is the
prototypical... | [
{
"created": "Thu, 23 Jun 2022 16:25:17 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Jul 2022 08:15:10 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Oct 2022 14:43:50 GMT",
"version": "v3"
}
] | 2023-03-15 | [
[
"Figueroa-O'Farrill",
"José",
""
],
[
"Grassie",
"Ross",
""
],
[
"Prohazka",
"Stefan",
""
]
] | We study and classify Lie algebras, homogeneous spacetimes and coadjoint orbits ("particles") of Lie groups generated by spatial rotations, temporal and spatial translations and an additional scalar generator. As a first step we classify Lie algebras of this type in arbitrary dimension. Among them is the prototypical L... | 5.528985 | 6.30244 | 6.587275 | 6.103573 | 6.070111 | 6.188768 | 6.527776 | 6.338931 | 6.167623 | 7.078914 | 5.914922 | 5.673923 | 5.829656 | 5.540096 | 5.753938 | 5.710639 | 5.570041 | 5.613594 | 5.585288 | 5.913347 | 5.630142 |
0706.3147 | W. A. Sabra | Jan B. Gutowski and Wafic A. Sabra | Half-Supersymmetric Solutions in Five-Dimensional Supergravity | 56 pages, reference added, typos corrected | JHEP 0712:025,2007; Erratum-ibid.1004:042,2010 | 10.1088/1126-6708/2007/12/025 10.1007/JHEP04(2010)042 | null | hep-th | null | We present a systematic classification of half-supersymmetric solutions of
gauged N=2, D=5 supergravity coupled to an arbitrary number of abelian vector
multiplets for which at least one of the Killing spinors generate a time-like
Killing vector.
| [
{
"created": "Thu, 21 Jun 2007 13:37:40 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Dec 2007 15:08:44 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Gutowski",
"Jan B.",
""
],
[
"Sabra",
"Wafic A.",
""
]
] | We present a systematic classification of half-supersymmetric solutions of gauged N=2, D=5 supergravity coupled to an arbitrary number of abelian vector multiplets for which at least one of the Killing spinors generate a time-like Killing vector. | 5.872238 | 3.088832 | 6.871506 | 3.4991 | 2.883943 | 3.379347 | 3.049947 | 3.462965 | 3.579158 | 6.498455 | 3.684062 | 4.336361 | 5.530553 | 4.507782 | 4.445158 | 4.364098 | 4.364777 | 4.636488 | 4.705475 | 5.865536 | 4.536853 |
1605.05165 | Ashok Das | Ashok Das and Pushpa Kalauni | Operator description for thermal quantum field theories on an arbitrary
path in the real time formalism | 10 pages, 1 figure, figure corrected | Phys. Rev. D 93, 125028 (2016) | 10.1103/PhysRevD.93.125028 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop an operator description, much like thermofield dynamics, for
quantum field theories on a real time path with an arbitrary parameter
$\sigma\,(0\leq\sigma\leq\beta)$. We point out new features which arise when
$\sigma\neq \frac{\beta}{2}$ in that the Hilbert space develops a natural,
modified inner product ... | [
{
"created": "Tue, 17 May 2016 13:47:02 GMT",
"version": "v1"
},
{
"created": "Wed, 18 May 2016 13:35:35 GMT",
"version": "v2"
}
] | 2016-06-29 | [
[
"Das",
"Ashok",
""
],
[
"Kalauni",
"Pushpa",
""
]
] | We develop an operator description, much like thermofield dynamics, for quantum field theories on a real time path with an arbitrary parameter $\sigma\,(0\leq\sigma\leq\beta)$. We point out new features which arise when $\sigma\neq \frac{\beta}{2}$ in that the Hilbert space develops a natural, modified inner product di... | 8.317555 | 8.442385 | 8.223633 | 8.175055 | 8.782086 | 8.402777 | 8.171247 | 8.209021 | 7.9755 | 8.490653 | 8.416274 | 7.919513 | 8.467247 | 8.240103 | 7.971791 | 8.113427 | 7.963058 | 8.159673 | 8.11375 | 8.576764 | 8.036048 |
1701.03553 | Shoichi Kawamoto | Shoichi Kawamoto, Chun-Yu Wei, Wen-Yu Wen | Extremal noncommutative black holes as dark matter furnaces | 15 pages, 1 figure | Classical and Quantum Gravity, Vol. 34 (2017) 17 | 10.1088/1361-6382/aa7f56 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this letter, we consider dark matter annihilation in the gravitational
field of noncommutative black holes. At final stage of evaporation, we
hypothesize the existence of a thermal equilibrium state composed of a burning
black hole relics fueled by dark matter accretion.
| [
{
"created": "Fri, 13 Jan 2017 03:28:15 GMT",
"version": "v1"
}
] | 2017-08-02 | [
[
"Kawamoto",
"Shoichi",
""
],
[
"Wei",
"Chun-Yu",
""
],
[
"Wen",
"Wen-Yu",
""
]
] | In this letter, we consider dark matter annihilation in the gravitational field of noncommutative black holes. At final stage of evaporation, we hypothesize the existence of a thermal equilibrium state composed of a burning black hole relics fueled by dark matter accretion. | 19.398252 | 17.606119 | 13.382561 | 13.943173 | 13.964072 | 13.66748 | 14.479903 | 13.72814 | 14.74733 | 13.554047 | 15.206389 | 14.787474 | 14.696133 | 14.000556 | 14.28282 | 14.656963 | 14.690776 | 13.569312 | 14.603627 | 14.548562 | 14.585511 |
1402.0527 | Kallosh Renata | Renata Kallosh | Planck 2013 and Superconformal Symmetry | 20 p, Based on the lecture at the Les Houches School "Post-Planck
Cosmology" 2013 | null | null | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explain why the concept of a spontaneously broken superconformal symmetry
is useful to describe inflationary models favored by the Planck. Non-minimal
coupling of complex scalars to curvature, N(X, X*) R, is compulsory for
superconformal symmetry. Here N is the Kahler potential of the embedding moduli
space, inclu... | [
{
"created": "Mon, 3 Feb 2014 21:32:16 GMT",
"version": "v1"
}
] | 2014-02-05 | [
[
"Kallosh",
"Renata",
""
]
] | We explain why the concept of a spontaneously broken superconformal symmetry is useful to describe inflationary models favored by the Planck. Non-minimal coupling of complex scalars to curvature, N(X, X*) R, is compulsory for superconformal symmetry. Here N is the Kahler potential of the embedding moduli space, includi... | 11.055564 | 11.875054 | 11.982092 | 11.027864 | 12.378008 | 12.789353 | 11.933836 | 11.587309 | 11.044084 | 13.6793 | 11.326672 | 10.983137 | 11.356096 | 11.337255 | 11.361378 | 11.296071 | 11.48095 | 11.35058 | 11.171236 | 11.189679 | 10.92563 |
1103.2730 | P. S. Howe | J. Greitz and P.S. Howe | Maximal supergravity in three dimensions: supergeometry and differential
forms | 27 pages. Small changes to the text; added references | JHEP 1107:071,2011 | 10.1007/JHEP07(2011)071 | KCL-MTH-11-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The maximal supergravity theory in three dimensions, which has local SO(16)
and rigid $E_8$ symmetries, is discussed in a superspace setting starting from
an off-shell superconformal structure. The on-shell theory is obtained by
imposing further constraints. It is essentially a non-linear sigma model that
induces a P... | [
{
"created": "Mon, 14 Mar 2011 18:19:04 GMT",
"version": "v1"
},
{
"created": "Sun, 24 Apr 2011 18:06:26 GMT",
"version": "v2"
}
] | 2011-07-21 | [
[
"Greitz",
"J.",
""
],
[
"Howe",
"P. S.",
""
]
] | The maximal supergravity theory in three dimensions, which has local SO(16) and rigid $E_8$ symmetries, is discussed in a superspace setting starting from an off-shell superconformal structure. The on-shell theory is obtained by imposing further constraints. It is essentially a non-linear sigma model that induces a Poi... | 8.903927 | 7.858602 | 9.495681 | 7.893881 | 8.879996 | 8.523017 | 8.819641 | 8.66005 | 8.48003 | 8.707302 | 8.173406 | 8.500825 | 8.766616 | 8.148973 | 8.311965 | 8.397807 | 8.153757 | 8.143327 | 8.339141 | 8.437659 | 8.250787 |
hep-th/9202050 | null | J.D. Cohn and H. Dykstra | The Marinari-Parisi Model and Collective Field Theory | 14 pages | Mod.Phys.Lett. A7 (1992) 1163-1174 | 10.1142/S0217732392003621 | null | hep-th | null | We derive the supersymmetric collective field theory for the Marinari-Parisi
model. For a specific choice of the superpotential, to leading order we find a
one parameter family of ground states which can be connected via instantons. At
this level of analysis the instanton size implied by the underlying matrix
model d... | [
{
"created": "Fri, 14 Feb 1992 19:11:46 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Cohn",
"J. D.",
""
],
[
"Dykstra",
"H.",
""
]
] | We derive the supersymmetric collective field theory for the Marinari-Parisi model. For a specific choice of the superpotential, to leading order we find a one parameter family of ground states which can be connected via instantons. At this level of analysis the instanton size implied by the underlying matrix model doe... | 14.856132 | 12.415565 | 16.361082 | 12.102664 | 13.299156 | 13.183593 | 14.079091 | 12.769583 | 13.267753 | 18.884972 | 13.151423 | 13.00986 | 14.539618 | 13.914597 | 14.410871 | 13.833714 | 13.469147 | 13.367449 | 12.97761 | 15.772936 | 13.934207 |
0712.2808 | Bert Vercnocke | Bert Janssen, Paul Smyth, Thomas Van Riet, Bert Vercnocke | A first-order formalism for timelike and spacelike brane solutions | 17 pages, v2: references added, occasional typos corrected | JHEP 0804:007,2008 | 10.1088/1126-6708/2008/04/007 | null | hep-th | null | We show that the construction of BPS-type equations for non-extremal black
holes due to Miller et. al. can be extended to branes of arbitrary dimension
and, more importantly, to time-dependent solutions. We call these first-order
equations fake- or pseudo-BPS equations in light of the formalism that has been
develope... | [
{
"created": "Mon, 17 Dec 2007 20:20:19 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Jan 2008 16:15:20 GMT",
"version": "v2"
}
] | 2009-12-15 | [
[
"Janssen",
"Bert",
""
],
[
"Smyth",
"Paul",
""
],
[
"Van Riet",
"Thomas",
""
],
[
"Vercnocke",
"Bert",
""
]
] | We show that the construction of BPS-type equations for non-extremal black holes due to Miller et. al. can be extended to branes of arbitrary dimension and, more importantly, to time-dependent solutions. We call these first-order equations fake- or pseudo-BPS equations in light of the formalism that has been developed ... | 10.654181 | 8.799262 | 10.277254 | 9.641798 | 10.715018 | 8.963344 | 9.735879 | 10.036237 | 9.482539 | 11.36037 | 9.185071 | 9.783094 | 10.260196 | 9.984782 | 9.939122 | 10.017224 | 10.032112 | 10.11012 | 9.748663 | 10.305723 | 9.767209 |
1505.07379 | Andrey Sadofyev | Krishna Rajagopal, Andrey V. Sadofyev | Chiral drag force | 28 pages, small improvement to the discussion of gravitational
anomaly, references added | null | null | MIT-CTP-4676 | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a holographic evaluation of novel contributions to the drag force
acting on a heavy quark moving through strongly interacting plasma. The new
contributions are chiral in that they act in opposite directions in plasmas
containing an excess of left- or right-handed quarks and in that they are
proportional to... | [
{
"created": "Wed, 27 May 2015 15:35:45 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jul 2015 11:25:21 GMT",
"version": "v2"
}
] | 2015-07-30 | [
[
"Rajagopal",
"Krishna",
""
],
[
"Sadofyev",
"Andrey V.",
""
]
] | We provide a holographic evaluation of novel contributions to the drag force acting on a heavy quark moving through strongly interacting plasma. The new contributions are chiral in that they act in opposite directions in plasmas containing an excess of left- or right-handed quarks and in that they are proportional to t... | 6.110928 | 7.226826 | 6.642524 | 6.406452 | 6.896709 | 7.062364 | 6.964942 | 6.616094 | 6.61365 | 7.062057 | 6.618371 | 6.406965 | 6.455329 | 6.309588 | 6.380727 | 6.345336 | 6.350673 | 6.419436 | 6.370412 | 6.226737 | 6.274511 |
1608.02958 | Brian Willett | Brian Willett | Localization on three-dimensional manifolds | This is a contribution to the review volume `Localization techniques
in quantum field theories' (eds. V. Pestun and M. Zabzine) which contains 17
Chapters. The complete volume is summarized in arXiv:1608.02952 and it can be
downloaded at https://arxiv.org/src/1608.02952/anc/LocQFT.pdf or
http://pestun.ihes.fr/p... | null | 10.1088/1751-8121/aa612f | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this review article we describe the localization of three dimensional N=2
supersymmetric theories on compact manifolds, including the squashed sphere,
S^3_b, the lens space, S^3_b/Z_p, and S^2 x S^1. We describe how to write
supersymmetric actions on these spaces, and then compute the partition
functions and other... | [
{
"created": "Tue, 9 Aug 2016 20:01:43 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Aug 2016 14:22:11 GMT",
"version": "v2"
},
{
"created": "Sat, 15 Oct 2016 18:03:10 GMT",
"version": "v3"
}
] | 2017-10-25 | [
[
"Willett",
"Brian",
""
]
] | In this review article we describe the localization of three dimensional N=2 supersymmetric theories on compact manifolds, including the squashed sphere, S^3_b, the lens space, S^3_b/Z_p, and S^2 x S^1. We describe how to write supersymmetric actions on these spaces, and then compute the partition functions and other s... | 7.438581 | 6.060598 | 8.008555 | 5.511226 | 5.695119 | 6.000786 | 5.709742 | 5.832502 | 5.655448 | 8.174103 | 5.767522 | 5.297555 | 6.623349 | 5.613295 | 5.727035 | 5.567964 | 5.548727 | 5.800726 | 5.634571 | 6.07325 | 5.547944 |
1607.03461 | Evgeny Buchbinder | Stefan Blesneag, Evgeny I. Buchbinder, Andre Lukas | Holomorphic Yukawa Couplings for Complete Intersection Calabi-Yau
Manifolds | 40 pages, Latex; v2: minor corrections, references added | JHEP 1701 (2017) 119 | 10.1007/JHEP01(2017)119 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop methods to compute holomorphic Yukawa couplings for heterotic
compactifications on complete intersection Calabi-Yau manifolds, generalising
results of an earlier paper for Calabi-Yau hypersurfaces. Our methods are based
on constructing the required bundle-valued forms explicitly and evaluating the
relevant... | [
{
"created": "Tue, 12 Jul 2016 18:34:15 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Feb 2017 02:44:26 GMT",
"version": "v2"
}
] | 2017-03-08 | [
[
"Blesneag",
"Stefan",
""
],
[
"Buchbinder",
"Evgeny I.",
""
],
[
"Lukas",
"Andre",
""
]
] | We develop methods to compute holomorphic Yukawa couplings for heterotic compactifications on complete intersection Calabi-Yau manifolds, generalising results of an earlier paper for Calabi-Yau hypersurfaces. Our methods are based on constructing the required bundle-valued forms explicitly and evaluating the relevant i... | 6.116471 | 6.114839 | 7.639209 | 6.156066 | 6.600465 | 6.280512 | 6.080237 | 6.026012 | 5.761969 | 8.959714 | 5.840096 | 6.088771 | 7.109756 | 6.299677 | 6.128774 | 6.100004 | 6.039294 | 6.200773 | 6.234312 | 6.920265 | 6.068054 |
2206.04064 | Gabriel Larios | Mattia Ces\`aro and Gabriel Larios and Oscar Varela | $\mathcal{N}=1$ S-fold spectroscopy | v2: minor changes. Version to be published in JHEP | null | 10.1007/JHEP08(2022)242 | IFT-UAM/CSIC-22-60 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We analyse the spectrum of Kaluza-Klein excitations above three distinct
families of ${\cal N}=1$ AdS$_4$ solutions of type IIB supergravity of
typically non-geometric, S-fold type that have been recently found. For all
three families, we provide the complete algebraic structure of their spectra,
including the conten... | [
{
"created": "Wed, 8 Jun 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Aug 2022 19:17:43 GMT",
"version": "v2"
}
] | 2022-09-07 | [
[
"Cesàro",
"Mattia",
""
],
[
"Larios",
"Gabriel",
""
],
[
"Varela",
"Oscar",
""
]
] | We analyse the spectrum of Kaluza-Klein excitations above three distinct families of ${\cal N}=1$ AdS$_4$ solutions of type IIB supergravity of typically non-geometric, S-fold type that have been recently found. For all three families, we provide the complete algebraic structure of their spectra, including the content ... | 11.468264 | 10.103069 | 13.028912 | 10.64972 | 11.350318 | 10.57385 | 10.637777 | 10.175659 | 10.163964 | 13.980485 | 10.292159 | 10.417497 | 11.286116 | 10.484468 | 10.435555 | 10.334774 | 10.199207 | 10.755411 | 10.314675 | 11.456978 | 10.315351 |
0805.0239 | James Ettle | James H. Ettle, Tim R. Morris and Zhiguang Xiao | The MHV QCD Lagrangian | **Important New Material:** Proof that vertices are MHV amps
off-shell, **Plus** results for all MHV verts with massive quarks.
Clarifications made, esp. on the link between massless quark-gluon vertices
and known results, and the choice of massive poln. spinors. Citations
revised. 42 pages, 2 figures, 4 tables... | JHEP 0808:103,2008 | 10.1088/1126-6708/2008/08/103 | SHEP 08-20 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform a canonical change of the field variables of light-cone gauge
massless QCD to obtain a lagrangian whose terms are proportional up to
polarisation factors to MHV amplitudes and continued off shell by the CSW
prescription. We solve for this transformation as a series expansion to all
orders in the new fields... | [
{
"created": "Fri, 2 May 2008 15:09:28 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 2008 21:15:40 GMT",
"version": "v2"
}
] | 2009-12-07 | [
[
"Ettle",
"James H.",
""
],
[
"Morris",
"Tim R.",
""
],
[
"Xiao",
"Zhiguang",
""
]
] | We perform a canonical change of the field variables of light-cone gauge massless QCD to obtain a lagrangian whose terms are proportional up to polarisation factors to MHV amplitudes and continued off shell by the CSW prescription. We solve for this transformation as a series expansion to all orders in the new fields, ... | 11.34534 | 11.060012 | 12.401011 | 11.18451 | 10.896351 | 11.169025 | 10.376967 | 10.840107 | 10.500742 | 12.125611 | 10.252984 | 10.907554 | 12.011431 | 11.162915 | 10.893385 | 11.038684 | 10.478276 | 10.83028 | 11.35986 | 11.661306 | 10.944253 |
hep-th/0103061 | Gerald V. Dunne | Gerald V. Dunne and Kumar Rao | Thermal Fluctuations of Induced Fermion Number | 17 pgs, 9 figs, RevTex4 | Phys.Rev. D64 (2001) 025003 | 10.1103/PhysRevD.64.025003 | null | hep-th cond-mat hep-ph | null | We analyze the phemomenon of induced fermion number at finite temperature. At
finite temperature, the induced fermion number $<N>$ is a thermal expectation
value, and we compute the finite temperature fluctuations, $(\Delta
N)^2=<N^2>-<N>^2$. While the zero temperature induced fermion number is
topological and is a s... | [
{
"created": "Fri, 9 Mar 2001 13:23:49 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Dunne",
"Gerald V.",
""
],
[
"Rao",
"Kumar",
""
]
] | We analyze the phemomenon of induced fermion number at finite temperature. At finite temperature, the induced fermion number $<N>$ is a thermal expectation value, and we compute the finite temperature fluctuations, $(\Delta N)^2=<N^2>-<N>^2$. While the zero temperature induced fermion number is topological and is a sha... | 5.630733 | 5.269049 | 5.900408 | 5.292752 | 5.348623 | 5.471119 | 5.371823 | 5.54696 | 5.115443 | 6.107585 | 5.360395 | 5.385129 | 5.572388 | 5.36516 | 5.412405 | 5.355956 | 5.301379 | 5.422585 | 5.37513 | 5.441899 | 5.430799 |
hep-th/0604114 | Chang Jun Gao | C.J.Gao, S.N.Zhang | Phantom Black Holes | 8 pages,some references added | null | null | null | hep-th | null | The exact solutions of electrically charged phantom black holes with the
cosmological constant are constructed. They are labelled by the mass, the
electrical charge, the cosmological constant and the coupling constant between
the phantom and the Maxwell field. It is found that the phantom has important
consequences o... | [
{
"created": "Mon, 17 Apr 2006 01:02:57 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Apr 2006 01:29:46 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Gao",
"C. J.",
""
],
[
"Zhang",
"S. N.",
""
]
] | The exact solutions of electrically charged phantom black holes with the cosmological constant are constructed. They are labelled by the mass, the electrical charge, the cosmological constant and the coupling constant between the phantom and the Maxwell field. It is found that the phantom has important consequences on ... | 7.983101 | 7.305408 | 6.954261 | 6.660597 | 7.3878 | 7.486823 | 7.737739 | 6.935436 | 6.973543 | 7.226303 | 7.168209 | 7.43443 | 7.080836 | 7.027842 | 7.077389 | 6.924506 | 6.938951 | 7.142442 | 7.394695 | 7.293338 | 7.160396 |
1111.4333 | Norisuke Sakai | Akiko Miyake, Kazutoshi Ohta and Norisuke Sakai | Moduli space volume of vortex and localization | 10 pages, talk at the international conference "quantum theory and
symmetries 7" in prague, august 7-13, 2011 | null | 10.1088/1742-6596/343/1/012107 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Volume of moduli space of BPS vortices on a compact genus h Riemann surface
Sigma_h is evaluated by means of topological field theory and localization
technique. Vortex in Abelian gauge theory with a single charged scalar field
(ANO vortex) is studied first and is found that the volume of the moduli space
agrees with... | [
{
"created": "Fri, 18 Nov 2011 11:18:38 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Miyake",
"Akiko",
""
],
[
"Ohta",
"Kazutoshi",
""
],
[
"Sakai",
"Norisuke",
""
]
] | Volume of moduli space of BPS vortices on a compact genus h Riemann surface Sigma_h is evaluated by means of topological field theory and localization technique. Vortex in Abelian gauge theory with a single charged scalar field (ANO vortex) is studied first and is found that the volume of the moduli space agrees with t... | 10.243931 | 8.989285 | 12.065153 | 8.662645 | 10.33437 | 9.150982 | 10.612721 | 9.01615 | 8.796936 | 11.562028 | 9.339355 | 8.661835 | 9.050621 | 8.699093 | 8.933098 | 8.828002 | 9.083798 | 8.875657 | 8.661229 | 9.06331 | 8.862069 |
hep-th/0001003 | Gungwon Kang | Y.S. Myung and Gungwon Kang | Comment on "Metric Fluctuations in Brane Worlds" | 4 pages, revtex | null | null | INJE-TP-99-10 | hep-th gr-qc | null | Recently, Ivanov and Volovich (hep-th/9912242) claimed that the perturbation
of $h_{\mu\nu}$ with nonvanishing transverse components $h_{5\mu}$ is not
localized on the brane because $h_{\mu\nu}$ depends on the fifth coordinate $z$
linearly. Consequently, it may indicate that the effective theory is unstable.
However,... | [
{
"created": "Sat, 1 Jan 2000 06:14:51 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Myung",
"Y. S.",
""
],
[
"Kang",
"Gungwon",
""
]
] | Recently, Ivanov and Volovich (hep-th/9912242) claimed that the perturbation of $h_{\mu\nu}$ with nonvanishing transverse components $h_{5\mu}$ is not localized on the brane because $h_{\mu\nu}$ depends on the fifth coordinate $z$ linearly. Consequently, it may indicate that the effective theory is unstable. However, w... | 9.020596 | 8.95182 | 7.841226 | 7.669279 | 7.742655 | 8.27206 | 9.10805 | 8.027538 | 8.03486 | 7.867759 | 8.029416 | 8.233191 | 7.725707 | 7.676873 | 7.898726 | 7.696996 | 8.073681 | 7.817598 | 7.832688 | 7.998673 | 7.887811 |
1904.10833 | Erich Cavalcanti MSc | E. Cavalcanti, C.A. Linhares, J. A. Louren\c{c}o, A. P. C. Malbouisson | The effect of boundary conditions on dimensionally reduced
field-theoretical models at finite temperature | null | Phys. Rev. D 100, 025008 (2019) | 10.1103/PhysRevD.100.025008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Here we understand \textit{dimensional reduction} as a procedure to obtain an
effective model in $D-1$ dimensions that is related to the original model in
$D$ dimensions. To explore this concept we use both a self-interacting
fermionic model and self-interacting bosonic model. Furthermore, in both cases,
we consider ... | [
{
"created": "Wed, 24 Apr 2019 14:11:44 GMT",
"version": "v1"
}
] | 2019-07-24 | [
[
"Cavalcanti",
"E.",
""
],
[
"Linhares",
"C. A.",
""
],
[
"Lourenço",
"J. A.",
""
],
[
"Malbouisson",
"A. P. C.",
""
]
] | Here we understand \textit{dimensional reduction} as a procedure to obtain an effective model in $D-1$ dimensions that is related to the original model in $D$ dimensions. To explore this concept we use both a self-interacting fermionic model and self-interacting bosonic model. Furthermore, in both cases, we consider di... | 7.898648 | 7.762722 | 7.547806 | 7.150608 | 7.446315 | 7.709094 | 7.81262 | 7.367717 | 7.512978 | 7.978617 | 7.486269 | 7.129081 | 7.330606 | 7.102635 | 7.130927 | 7.073152 | 7.211902 | 7.287247 | 7.251147 | 7.548604 | 7.281519 |
hep-th/0406222 | Mohammad Reza Setare | M R Setare | Casimir Effect for Moving Branes in Static dS$_{4+1}$ Bulk | 9 pages, no figures | null | null | null | hep-th | null | In this paper we study the Casimir effect for conformally coupled massless
scalar fields on background of Static dS$_{4+1}$ spacetime. We will consider
the general plane--symmetric solutions of the gravitational field equations and
boundary conditions of the Dirichlet type on the branes. Then we calculate the
vacuum ... | [
{
"created": "Thu, 24 Jun 2004 13:07:24 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Setare",
"M R",
""
]
] | In this paper we study the Casimir effect for conformally coupled massless scalar fields on background of Static dS$_{4+1}$ spacetime. We will consider the general plane--symmetric solutions of the gravitational field equations and boundary conditions of the Dirichlet type on the branes. Then we calculate the vacuum en... | 7.244153 | 5.460781 | 7.81517 | 6.193594 | 6.241849 | 5.517262 | 5.735967 | 5.75725 | 6.136216 | 7.921853 | 6.218735 | 6.316443 | 7.188811 | 6.82126 | 6.422706 | 6.387762 | 6.537059 | 6.62454 | 6.541504 | 7.080515 | 6.530129 |
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