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/9909120 | Eric R. Sharpe | Eric R. Sharpe | Discrete Torsion and Gerbes II | 75 pages, must LaTeX 3x; v2: minor refinement in conclusions, other
minor upgrades | null | null | DUKE-CGTP-99-07 | hep-th math.DG | null | In a previous paper we outlined how discrete torsion can be understood
geometrically as an analogue of orbifold U(1) Wilson lines. In this paper we
shall prove the remaining details. More precisely, in this paper we describe
gerbes in terms of objects known as stacks (essentially, sheaves of
categories), and develop ... | [
{
"created": "Thu, 16 Sep 1999 20:06:33 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Aug 2000 14:00:57 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Sharpe",
"Eric R.",
""
]
] | In a previous paper we outlined how discrete torsion can be understood geometrically as an analogue of orbifold U(1) Wilson lines. In this paper we shall prove the remaining details. More precisely, in this paper we describe gerbes in terms of objects known as stacks (essentially, sheaves of categories), and develop mu... | 7.664136 | 7.786571 | 8.788428 | 7.465012 | 7.547252 | 7.664055 | 7.082387 | 6.946783 | 7.245006 | 8.56616 | 6.911725 | 7.085403 | 7.41377 | 7.225082 | 7.109968 | 7.106457 | 6.957774 | 7.217634 | 7.175145 | 7.516403 | 7.102155 |
1707.08501 | Oleg Evnin | Ben Craps, Oleg Evnin, Vincent Luyten | Maximally rotating waves in AdS and on spheres | 17 pages | JHEP 1709 (2017) 059 | 10.1007/JHEP09(2017)059 | null | hep-th gr-qc math-ph math.AP math.MP nlin.SI | http://creativecommons.org/licenses/by-nc-sa/4.0/ | We study the cubic wave equation in AdS_(d+1) (and a closely related cubic
wave equation on S^3) in a weakly nonlinear regime. Via time-averaging, these
systems are accurately described by simplified infinite-dimensional quartic
Hamiltonian systems, whose structure is mandated by the fully resonant spectrum
of linear... | [
{
"created": "Wed, 26 Jul 2017 15:36:28 GMT",
"version": "v1"
}
] | 2017-09-18 | [
[
"Craps",
"Ben",
""
],
[
"Evnin",
"Oleg",
""
],
[
"Luyten",
"Vincent",
""
]
] | We study the cubic wave equation in AdS_(d+1) (and a closely related cubic wave equation on S^3) in a weakly nonlinear regime. Via time-averaging, these systems are accurately described by simplified infinite-dimensional quartic Hamiltonian systems, whose structure is mandated by the fully resonant spectrum of lineariz... | 14.474747 | 15.628135 | 17.820669 | 14.834117 | 17.076397 | 16.734596 | 17.107506 | 15.63102 | 15.242128 | 18.204737 | 15.023032 | 14.770422 | 14.877161 | 14.747951 | 14.753797 | 14.662196 | 14.364774 | 14.593905 | 14.199165 | 15.072367 | 14.502561 |
1610.05664 | Michele Maggiore | Enis Belgacem, Giulia Cusin, Stefano Foffa, Michele Maggiore and
Michele Mancarella | Stability issues of nonlocal gravity during primordial inflation | v3: important error corrected, which changes a conclusion (RT model
viable also when initial conditions are set during inflation); v4: corrected
an error in the v3 submission (abstract in the arxiv form had not been
changed) | null | null | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the cosmological evolution of some nonlocal gravity models, when the
initial conditions are set during a phase of primordial inflation. We examine
in particular three models, the so-called RT, RR and $\Delta_4$ models,
previously introduced by our group. We find that the RR and $\Delta_4$ models
have a stabl... | [
{
"created": "Tue, 18 Oct 2016 15:08:35 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Nov 2017 10:40:16 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Nov 2018 15:02:24 GMT",
"version": "v3"
},
{
"created": "Thu, 29 Nov 2018 15:18:17 GMT",
"version": "v4"
}
] | 2018-11-30 | [
[
"Belgacem",
"Enis",
""
],
[
"Cusin",
"Giulia",
""
],
[
"Foffa",
"Stefano",
""
],
[
"Maggiore",
"Michele",
""
],
[
"Mancarella",
"Michele",
""
]
] | We study the cosmological evolution of some nonlocal gravity models, when the initial conditions are set during a phase of primordial inflation. We examine in particular three models, the so-called RT, RR and $\Delta_4$ models, previously introduced by our group. We find that the RR and $\Delta_4$ models have a stable ... | 7.332269 | 7.226307 | 6.806602 | 6.960437 | 7.427963 | 7.684356 | 7.820704 | 6.94334 | 7.231991 | 6.689192 | 7.409207 | 7.500573 | 7.284537 | 7.245022 | 7.157377 | 7.352078 | 7.358482 | 7.204741 | 7.211708 | 7.228183 | 7.115395 |
hep-th/9510125 | Yun Soo Myung | H.W. Lee, Y.S. Myung(Inje U.), Jin Young Kim(Dongseo U.) | Unstable two-dimensional extremal black holes | 9 pages 3 figures, RevTeX, to obtain figures contact author
(ysmyung@physics.inje.ac.kr) | null | null | INJE-TP-95-7 | hep-th | null | We obtain the $\epsilon<2$ new extremal ground states of a two-dimensional
(2D) charged black hole where $\epsilon$ is the dilaton coupling parameter for
the Maxwell term. The stability analysis is carried out for all these extremal
black holes. It is found that the shape of potentials to an on-coming tachyon
(as a s... | [
{
"created": "Wed, 18 Oct 1995 08:41:31 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Lee",
"H. W.",
"",
"Inje U."
],
[
"Myung",
"Y. S.",
"",
"Inje U."
],
[
"Kim",
"Jin Young",
"",
"Dongseo U."
]
] | We obtain the $\epsilon<2$ new extremal ground states of a two-dimensional (2D) charged black hole where $\epsilon$ is the dilaton coupling parameter for the Maxwell term. The stability analysis is carried out for all these extremal black holes. It is found that the shape of potentials to an on-coming tachyon (as a spe... | 16.282766 | 12.082843 | 16.710981 | 13.330507 | 12.78943 | 12.143235 | 12.123319 | 12.283503 | 13.294027 | 17.741982 | 13.251118 | 13.863937 | 14.845697 | 14.52397 | 13.915304 | 14.515727 | 13.92852 | 13.596008 | 14.874997 | 15.43537 | 13.899872 |
2111.00025 | Mauricio Romo | Jirui Guo and Mauricio Romo | Hybrid models for homological projective duals and noncommutative
resolutions | 50 pages, LaTeX; v3: references added, several improvements on the
examples and the section on complete intersections. Published version | null | 10.1007/s11005-022-01605-3 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study hybrid models arising as homological projective duals (HPD) of
certain projective embeddings $f:X\rightarrow\mathbb{P}(V)$ of Fano manifolds
$X$. More precisely, the category of B-branes of such hybrid models corresponds
to the HPD category of the embedding $f$. B-branes on these hybrid models can
be seen as... | [
{
"created": "Fri, 29 Oct 2021 18:00:21 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Dec 2021 15:27:23 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Nov 2022 10:46:06 GMT",
"version": "v3"
}
] | 2022-11-30 | [
[
"Guo",
"Jirui",
""
],
[
"Romo",
"Mauricio",
""
]
] | We study hybrid models arising as homological projective duals (HPD) of certain projective embeddings $f:X\rightarrow\mathbb{P}(V)$ of Fano manifolds $X$. More precisely, the category of B-branes of such hybrid models corresponds to the HPD category of the embedding $f$. B-branes on these hybrid models can be seen as g... | 5.191552 | 6.009477 | 6.731269 | 5.721246 | 6.007859 | 6.26073 | 5.883395 | 5.923972 | 5.60122 | 6.739336 | 5.478334 | 5.404552 | 5.592933 | 5.361825 | 5.377003 | 5.289325 | 5.421269 | 5.262833 | 5.531475 | 5.384258 | 5.147524 |
hep-th/0306217 | Luzi Bergamin | L. Bergamin and W. Kummer | The Complete Solution of 2D Superfield Supergravity from graded
Poisson-Sigma Models and the Super Pointparticle | 48 pages, 1 figure. v3: after final version, typos corrected | Phys.Rev. D68 (2003) 104005 | 10.1103/PhysRevD.68.104005 | null | hep-th | null | Recently an alternative description of 2d supergravities in terms of graded
Poisson-Sigma models (gPSM) has been given. As pointed out previously by the
present authors a certain subset of gPSMs can be interpreted as "genuine"
supergravity, fulfilling the well-known limits of supergravity, albeit deformed
by the dila... | [
{
"created": "Mon, 23 Jun 2003 11:11:54 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Oct 2003 13:28:34 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Feb 2004 11:55:23 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Bergamin",
"L.",
""
],
[
"Kummer",
"W.",
""
]
] | Recently an alternative description of 2d supergravities in terms of graded Poisson-Sigma models (gPSM) has been given. As pointed out previously by the present authors a certain subset of gPSMs can be interpreted as "genuine" supergravity, fulfilling the well-known limits of supergravity, albeit deformed by the dilato... | 13.021266 | 13.928537 | 12.714972 | 12.402675 | 12.766764 | 13.304317 | 12.83127 | 12.034262 | 11.866297 | 14.032681 | 12.236717 | 12.386543 | 12.497581 | 12.4068 | 12.25514 | 12.457593 | 12.419177 | 12.486555 | 12.029907 | 12.817093 | 12.385985 |
hep-th/0112142 | Dmitri Ryzhikh | L. Laperashvili (ITEP, Moscow, Russia), D. A. Ryzhikh (ITEP, Moscow,
Russia) | [SU(5)]^3 SUSY unification | 15 pages, 5 figures; submitted to Festschrift dedicated to the 60th
jubilee of Holger Bech Nielsen | null | null | null | hep-th | null | In the present paper we demonstrate the possibility of the [SUSY(5)]^3 SUSY
unification at the energy scale $\mu_{GUT}\approx 10^{18.3} GeV$ with the value
of GUT inverse finestructure constant $\alpha_{GUT}^{-1}\approx 34.4$, which is
very close to its critical value $\alpha_{5, crit}^{-1}\approx 34.0$, existing
at ... | [
{
"created": "Mon, 17 Dec 2001 13:39:26 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Laperashvili",
"L.",
"",
"ITEP, Moscow, Russia"
],
[
"Ryzhikh",
"D. A.",
"",
"ITEP, Moscow,\n Russia"
]
] | In the present paper we demonstrate the possibility of the [SUSY(5)]^3 SUSY unification at the energy scale $\mu_{GUT}\approx 10^{18.3} GeV$ with the value of GUT inverse finestructure constant $\alpha_{GUT}^{-1}\approx 34.4$, which is very close to its critical value $\alpha_{5, crit}^{-1}\approx 34.0$, existing at th... | 7.754646 | 8.188705 | 6.915319 | 6.318907 | 6.714125 | 8.086703 | 6.85761 | 7.922408 | 6.876537 | 7.844662 | 7.357231 | 7.010398 | 7.262703 | 6.861682 | 6.869227 | 6.799728 | 6.919176 | 6.854355 | 6.857941 | 6.97545 | 7.012963 |
hep-th/9210110 | Jorge Pullin | R. Gambini, J. Pullin | Quantum Einstein-Maxwell Fields: A Unified Viewpoint from the Loop
Representation | 13pp. no figures, Revtex, UU-HEP-92/9, IFFI 92-11 | Phys.Rev.D47:5214-5218,1993 | 10.1103/PhysRevD.47.R5214 | null | hep-th gr-qc | null | We propose a naive unification of Electromagnetism and General Relativity
based on enlarging the gauge group of Ashtekar's new variables. We construct
the connection and loop representations and analyze the space of states. In the
loop representation, the wavefunctions depend on two loops, each of them
carrying infor... | [
{
"created": "Tue, 20 Oct 1992 17:18:14 GMT",
"version": "v1"
}
] | 2009-12-30 | [
[
"Gambini",
"R.",
""
],
[
"Pullin",
"J.",
""
]
] | We propose a naive unification of Electromagnetism and General Relativity based on enlarging the gauge group of Ashtekar's new variables. We construct the connection and loop representations and analyze the space of states. In the loop representation, the wavefunctions depend on two loops, each of them carrying informa... | 10.33389 | 9.694997 | 9.898634 | 9.91836 | 10.482404 | 10.022614 | 9.503792 | 9.301416 | 10.077748 | 10.342359 | 9.307139 | 9.929902 | 9.74616 | 9.772239 | 9.551454 | 9.217415 | 9.543716 | 9.501863 | 9.861472 | 10.143098 | 9.589601 |
0708.2194 | Eugenio R. Bezerra de Mello | E. R. Bezerra de Mello | Fermionic vacuum polarization in higher-dimensional global monopole
spacetime | 21 pages, 3 figures | Phys.Rev.D76:125021,2007 | 10.1103/PhysRevD.76.125021 | null | hep-th gr-qc | null | In this paper we analyse the vacuum polarization effects associated with a
massless fermionic field in a higher-dimensional global monopole spacetime in
the "braneworld" scenario. In this context we admit that the our Universe, the
bulk, is represented by a flat $(n-1)-$dimensional brane having a global
monopole in a... | [
{
"created": "Thu, 16 Aug 2007 13:19:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"de Mello",
"E. R. Bezerra",
""
]
] | In this paper we analyse the vacuum polarization effects associated with a massless fermionic field in a higher-dimensional global monopole spacetime in the "braneworld" scenario. In this context we admit that the our Universe, the bulk, is represented by a flat $(n-1)-$dimensional brane having a global monopole in a e... | 9.406955 | 8.27459 | 9.949448 | 8.189605 | 8.507895 | 7.803187 | 7.393046 | 7.756148 | 7.44479 | 9.913388 | 8.27332 | 8.620939 | 9.382396 | 8.71485 | 8.869025 | 8.750085 | 8.130925 | 8.724278 | 9.199785 | 9.318492 | 8.745531 |
1012.5559 | Haiqing Zhang | Rong-Gen Cai, Zhang-Yu Nie and Hai-Qing Zhang | Holographic Phase Transitions of P-wave Superconductors in Gauss-Bonnet
Gravity with Back-reaction | 15 page,4 figures;Some refs added | Phys.Rev.D83:066013,2011 | 10.1103/PhysRevD.83.066013 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the phase transitions of holographic p-wave superconductors in
(4+1)-dimensional Einstein-Yang-Mills-Gauss-Bonnet theories, in a grand
canonical ensemble. Turning on the back-reaction of the Yang-Mills field, it is
found that the condensations of vector order parameter become harder if the
Gauss-Bonnet... | [
{
"created": "Mon, 27 Dec 2010 06:14:17 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Jan 2011 00:56:05 GMT",
"version": "v2"
}
] | 2015-03-17 | [
[
"Cai",
"Rong-Gen",
""
],
[
"Nie",
"Zhang-Yu",
""
],
[
"Zhang",
"Hai-Qing",
""
]
] | We investigate the phase transitions of holographic p-wave superconductors in (4+1)-dimensional Einstein-Yang-Mills-Gauss-Bonnet theories, in a grand canonical ensemble. Turning on the back-reaction of the Yang-Mills field, it is found that the condensations of vector order parameter become harder if the Gauss-Bonnet c... | 5.176767 | 4.579062 | 5.403205 | 4.601912 | 4.407616 | 4.797348 | 4.44082 | 4.737236 | 4.680616 | 5.033571 | 4.577247 | 4.898643 | 5.059137 | 4.900886 | 4.858284 | 4.910151 | 4.838315 | 4.84692 | 5.060313 | 5.078021 | 5.191182 |
hep-th/0505273 | Noah Graham | E.Farhi, N. Graham, V. Khemani, R. Markov and R. Rosales | An Oscillon in the SU(2) Gauged Higgs Model | 7 pages, 6 .eps figures, uses revtex4 and epsfig | Phys.Rev. D72 (2005) 101701 | 10.1103/PhysRevD.72.101701 | MIT-CTP-3649 | hep-th hep-ph nlin.PS | null | We study classical dynamics in the spherical ansatz for the SU(2) gauge and
Higgs fields of the electroweak Standard Model in the absence of fermions and
the photon. With the Higgs boson mass equal to twice the gauge boson mass, we
numerically demonstrate the existence of oscillons, extremely long-lived
localized con... | [
{
"created": "Tue, 31 May 2005 15:31:12 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Farhi",
"E.",
""
],
[
"Graham",
"N.",
""
],
[
"Khemani",
"V.",
""
],
[
"Markov",
"R.",
""
],
[
"Rosales",
"R.",
""
]
] | We study classical dynamics in the spherical ansatz for the SU(2) gauge and Higgs fields of the electroweak Standard Model in the absence of fermions and the photon. With the Higgs boson mass equal to twice the gauge boson mass, we numerically demonstrate the existence of oscillons, extremely long-lived localized confi... | 8.364649 | 7.091947 | 8.161739 | 7.358717 | 7.747694 | 7.509642 | 7.128498 | 7.561946 | 7.207246 | 8.38122 | 7.521891 | 7.689546 | 7.674584 | 7.639012 | 7.906394 | 7.886581 | 7.600489 | 7.642814 | 7.199145 | 7.578982 | 7.674708 |
hep-th/0701266 | Supratik Pal | Supratik Pal (IUCAA, Pune and ISI Kolkata), Sayan Kar (IIT Kharagpur) | de Sitter branes with a bulk scalar | 18 pages, 5 figures. Substantial changes and new results. To appear
in GRG | Gen.Rel.Grav.41:1165-1179,2009 | 10.1007/s10714-008-0697-2 | null | hep-th astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose new braneworld models arising from a scalar field in the bulk. In
these examples, the induced on--brane line element is de Sitter (or anti de
Sitter) and the bulk (five dimensional) Einstein equations can be exactly
solved to obtain warped spacetimes. The solutions thus derived are single and
two-brane mod... | [
{
"created": "Mon, 29 Jan 2007 17:00:30 GMT",
"version": "v1"
},
{
"created": "Wed, 16 May 2007 12:25:51 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Oct 2008 08:39:23 GMT",
"version": "v3"
}
] | 2009-05-05 | [
[
"Pal",
"Supratik",
"",
"IUCAA, Pune and ISI Kolkata"
],
[
"Kar",
"Sayan",
"",
"IIT Kharagpur"
]
] | We propose new braneworld models arising from a scalar field in the bulk. In these examples, the induced on--brane line element is de Sitter (or anti de Sitter) and the bulk (five dimensional) Einstein equations can be exactly solved to obtain warped spacetimes. The solutions thus derived are single and two-brane model... | 10.874538 | 10.037096 | 10.676332 | 9.95953 | 10.397902 | 10.23802 | 10.579649 | 10.82094 | 10.059324 | 11.190249 | 10.190522 | 10.174945 | 10.306531 | 9.907495 | 10.190486 | 10.260481 | 10.315989 | 10.281054 | 10.514465 | 10.697369 | 10.226696 |
0804.0324 | Till Bargheer | Till Bargheer, Niklas Beisert, Nikolay Gromov | Quantum Stability for the Heisenberg Ferromagnet | 82 pages, a figure a page or so | New J. Phys. 10 (2008) 103023 | 10.1088/1367-2630/10/10/103023 | AEI-2008-010, LPTENS 08/19, SPhT-t08/051 | hep-th cond-mat.stat-mech math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Highly spinning classical strings on RxS^3 are described by the
Landau-Lifshitz model or equivalently by the Heisenberg ferromagnet in the
thermodynamic limit. The spectrum of this model can be given in terms of
spectral curves. However, it is a priori not clear whether any given admissible
spectral curve can actuall... | [
{
"created": "Wed, 2 Apr 2008 10:33:15 GMT",
"version": "v1"
}
] | 2008-10-31 | [
[
"Bargheer",
"Till",
""
],
[
"Beisert",
"Niklas",
""
],
[
"Gromov",
"Nikolay",
""
]
] | Highly spinning classical strings on RxS^3 are described by the Landau-Lifshitz model or equivalently by the Heisenberg ferromagnet in the thermodynamic limit. The spectrum of this model can be given in terms of spectral curves. However, it is a priori not clear whether any given admissible spectral curve can actually ... | 10.443385 | 10.325162 | 11.375749 | 9.575011 | 10.301738 | 10.47941 | 10.616497 | 10.244711 | 9.987575 | 11.668389 | 9.7808 | 9.331558 | 10.589923 | 9.535694 | 9.538125 | 9.589864 | 9.510592 | 9.51678 | 9.857758 | 10.386461 | 9.627422 |
hep-th/0208079 | Yosuke Imamura | Yosuke Imamura | Open string - BMN operator correspondence in the weak coupling regime | 25 pages, 2 figures, PTPTeX, typos corrected | Prog.Theor.Phys. 108 (2003) 1077-1097 | 10.1143/PTP.108.1077 | UT-02-41 | hep-th | null | We reproduce the correspondence between open string states |n> and BMN
operators O_n in N=2 supersymmetric gauge theory using a worldsheet computation
with the relation <B|n>=O_n, where <B| is a boundary state of D3-branes. We
regard the NS ground states and their excitations with respect to a bosonic
oscillator as t... | [
{
"created": "Mon, 12 Aug 2002 09:09:43 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Aug 2002 09:50:40 GMT",
"version": "v2"
},
{
"created": "Tue, 12 Nov 2002 03:13:48 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Imamura",
"Yosuke",
""
]
] | We reproduce the correspondence between open string states |n> and BMN operators O_n in N=2 supersymmetric gauge theory using a worldsheet computation with the relation <B|n>=O_n, where <B| is a boundary state of D3-branes. We regard the NS ground states and their excitations with respect to a bosonic oscillator as the... | 11.3202 | 10.748733 | 12.597364 | 10.661594 | 11.107629 | 10.904517 | 10.35192 | 11.306561 | 10.380095 | 12.494548 | 10.458242 | 10.070279 | 10.560852 | 10.164272 | 10.46325 | 10.431741 | 10.424041 | 10.140939 | 10.155993 | 10.59647 | 9.565033 |
1710.10409 | Carlo Pagani | C. Pagani, H. Sonoda | On the geometry of the theory space in the ERG formalism | 23 pages | Phys. Rev. D 97, 025015 (2018) | 10.1103/PhysRevD.97.025015 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the theory space as a manifold whose coordinates are given by the
couplings appearing in the Wilson action. We discuss how to introduce
connections on this theory space. A particularly intriguing connection can be
defined directly from the solution of the exact renormalization group (ERG)
equation. We adv... | [
{
"created": "Sat, 28 Oct 2017 07:29:19 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Jan 2018 15:12:32 GMT",
"version": "v2"
}
] | 2018-01-31 | [
[
"Pagani",
"C.",
""
],
[
"Sonoda",
"H.",
""
]
] | We consider the theory space as a manifold whose coordinates are given by the couplings appearing in the Wilson action. We discuss how to introduce connections on this theory space. A particularly intriguing connection can be defined directly from the solution of the exact renormalization group (ERG) equation. We advoc... | 13.213433 | 10.324019 | 12.176753 | 10.749043 | 11.178912 | 11.547747 | 11.041256 | 10.964802 | 11.65101 | 13.253851 | 11.074804 | 11.562238 | 12.660975 | 12.488919 | 12.05265 | 11.812143 | 12.227262 | 12.289925 | 11.94346 | 12.800114 | 11.893894 |
hep-th/0303159 | Vishesh Khemani | E. Farhi, N. Graham, R.L. Jaffe, V. Khemani, H. Weigel | Heavy Fermion Quantum Effects in SU(2)_L Gauge Theory | 30 pages LaTeX, 3 eps-figures | Nucl.Phys. B665 (2003) 623-648 | 10.1016/S0550-3213(03)00487-5 | MIT-CTP-3350, UNITU-HEP-4/2003 | hep-th hep-ph nucl-th | null | We explore the effects of a heavy fermion doublet in a simplified version of
the standard electroweak theory. We integrate out the doublet and compute the
exact effective energy functional of spatially varying gauge and Higgs fields.
We perform a variational search for a local minimum of the effective energy and
do n... | [
{
"created": "Tue, 18 Mar 2003 17:26:03 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Farhi",
"E.",
""
],
[
"Graham",
"N.",
""
],
[
"Jaffe",
"R. L.",
""
],
[
"Khemani",
"V.",
""
],
[
"Weigel",
"H.",
""
]
] | We explore the effects of a heavy fermion doublet in a simplified version of the standard electroweak theory. We integrate out the doublet and compute the exact effective energy functional of spatially varying gauge and Higgs fields. We perform a variational search for a local minimum of the effective energy and do not... | 10.461405 | 9.866274 | 10.857434 | 10.013752 | 10.724338 | 10.795064 | 10.186432 | 9.826376 | 10.273923 | 11.592811 | 10.212863 | 9.953552 | 9.941031 | 9.819722 | 10.044222 | 9.79944 | 9.987494 | 9.633257 | 9.62706 | 9.991118 | 9.723779 |
1408.4808 | Hernan Piragua | Denis Klevers and Damian Kaloni Mayorga Pena and Paul-Konstantin
Oehlmann and Hernan Piragua and Jonas Reuter | F-Theory on all Toric Hypersurface Fibrations and its Higgs Branches | 129 pages, 32 figures, 44 tables v2: minor changes, references added | null | 10.1007/JHEP01(2015)142 | null | hep-th hep-ph math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider F-theory compactifications on genus-one fibered Calabi-Yau
manifolds with their fibers realized as hypersurfaces in the toric varieties
associated to the 16 reflexive 2D polyhedra. We present a base-independent
analysis of the codimension one, two and three singularities of these
fibrations. We use these ... | [
{
"created": "Wed, 20 Aug 2014 20:03:40 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Sep 2014 22:21:26 GMT",
"version": "v2"
}
] | 2015-06-22 | [
[
"Klevers",
"Denis",
""
],
[
"Pena",
"Damian Kaloni Mayorga",
""
],
[
"Oehlmann",
"Paul-Konstantin",
""
],
[
"Piragua",
"Hernan",
""
],
[
"Reuter",
"Jonas",
""
]
] | We consider F-theory compactifications on genus-one fibered Calabi-Yau manifolds with their fibers realized as hypersurfaces in the toric varieties associated to the 16 reflexive 2D polyhedra. We present a base-independent analysis of the codimension one, two and three singularities of these fibrations. We use these ge... | 6.314018 | 7.128705 | 7.701141 | 6.668134 | 6.971228 | 6.973883 | 7.279272 | 6.923761 | 6.848194 | 8.519115 | 6.592505 | 6.480509 | 6.871747 | 6.563164 | 6.499221 | 6.482358 | 6.617822 | 6.504703 | 6.555319 | 7.051098 | 6.410882 |
1204.0676 | Ulf Lindstr\"om | Ulf Lindstrom | Complex Geometry and Supersymmetry | 9 pages, Proceedings of the Corfu Summer Institute 2011 School and
Workshops on Elementary Particle Physics and Gravity September 4-18, 2011
Corfu, Greece | null | null | UUITP-08/12 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I stress how the form of sigma models with (2, 2) supersymmetry differs
depending on the number of manifest supersymmetries. The differences correspond
to different aspects/formulations of Generalized K\"ahler Geometry.
| [
{
"created": "Tue, 3 Apr 2012 12:27:09 GMT",
"version": "v1"
}
] | 2012-04-04 | [
[
"Lindstrom",
"Ulf",
""
]
] | I stress how the form of sigma models with (2, 2) supersymmetry differs depending on the number of manifest supersymmetries. The differences correspond to different aspects/formulations of Generalized K\"ahler Geometry. | 25.423124 | 14.888534 | 22.965973 | 14.701835 | 16.182413 | 14.488812 | 14.65607 | 14.508924 | 14.941225 | 16.486258 | 16.386452 | 15.566126 | 20.259922 | 16.422861 | 15.483906 | 15.286476 | 14.950419 | 15.008171 | 15.05527 | 20.368444 | 16.300797 |
hep-th/0211028 | Toby Wiseman | T. Wiseman | From Black Strings to Black Holes | 6 pages, 5 figures, RevTeX | Class.Quant.Grav. 20 (2003) 1177-1186 | 10.1088/0264-9381/20/6/309 | DAMTP-2002-134 | hep-th | null | Using recently developed numerical methods, we examine neutral compactified
non-uniform black strings which connect to the Gregory-Laflamme critical point.
By studying the geometry of the horizon we give evidence that this branch of
solutions may connect to the black hole solutions, as conjectured by Kol. We
find the... | [
{
"created": "Tue, 5 Nov 2002 12:26:03 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Wiseman",
"T.",
""
]
] | Using recently developed numerical methods, we examine neutral compactified non-uniform black strings which connect to the Gregory-Laflamme critical point. By studying the geometry of the horizon we give evidence that this branch of solutions may connect to the black hole solutions, as conjectured by Kol. We find the g... | 13.438117 | 13.69043 | 14.966264 | 13.54526 | 12.969422 | 13.344739 | 14.222551 | 13.428236 | 12.804048 | 14.368891 | 13.040308 | 11.863766 | 13.869703 | 13.087049 | 13.008029 | 12.44583 | 13.017154 | 12.553637 | 12.773837 | 14.00559 | 12.212998 |
hep-th/9506115 | null | Enrique Alvarez, J.M. Gracia-Bond\'ia and C.P. Mart\'in | Anomaly Cancellation and gauge group of the standard model in NCG | 10 pages, plain TeX.(TeX errors fixed) | Phys.Lett. B364 (1995) 33-40 | 10.1016/0370-2693(95)01051-3 | FT/UCM/7/95;FTUAM-95100 | hep-th | null | It is well known that anomaly cancellation {\it almost} determines the
hypercharges in the standard model. A related (and somewhat more stronger)
phenomenon takes place in Connes' NCG framework: unimodularity (a technical
condition on elements of the algebra) is {\it strictly} equivalent to anomaly
cancellation (in t... | [
{
"created": "Mon, 19 Jun 1995 09:08:02 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Jun 1995 09:15:50 GMT",
"version": "v2"
}
] | 2019-08-17 | [
[
"Alvarez",
"Enrique",
""
],
[
"Gracia-Bondía",
"J. M.",
""
],
[
"Martín",
"C. P.",
""
]
] | It is well known that anomaly cancellation {\it almost} determines the hypercharges in the standard model. A related (and somewhat more stronger) phenomenon takes place in Connes' NCG framework: unimodularity (a technical condition on elements of the algebra) is {\it strictly} equivalent to anomaly cancellation (in the... | 10.794299 | 9.169668 | 9.833313 | 9.341239 | 9.897072 | 8.6803 | 10.141306 | 9.240593 | 9.292965 | 12.137527 | 9.230714 | 9.524778 | 9.715647 | 9.325729 | 9.361604 | 9.264341 | 9.254409 | 9.072472 | 9.298199 | 9.655798 | 9.724105 |
2103.00257 | Hao Xu | Chen-Hao Wu, Ya-Peng Hu, Hao Xu | Hawking evaporation of Einstein-Gauss-Bonnet AdS black holes in
$D\geqslant 4$ dimensions | 14 pages, 8 figures; v2: references added, minor corrections,
submitted to journal;v3: minor corrections, published in EPJC;v4: one typo in
Eq(9) fixed | Eur. Phys. J. C 81, 351 (2021) | 10.1140/epjc/s10052-021-09140-6 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Einstein-Gauss-Bonnet theory is a string-generated gravity theory when
approaching the low energy limit. By introducing the higher order curvature
terms, this theory is supposed to help to solve the black hole singularity
problem. In this work, we investigate the evaporation of the static spherically
symmetric neutra... | [
{
"created": "Sat, 27 Feb 2021 15:56:17 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Mar 2021 09:17:50 GMT",
"version": "v2"
},
{
"created": "Sun, 25 Apr 2021 08:25:40 GMT",
"version": "v3"
},
{
"created": "Mon, 21 Nov 2022 06:30:54 GMT",
"version": "v4"
}
] | 2022-11-22 | [
[
"Wu",
"Chen-Hao",
""
],
[
"Hu",
"Ya-Peng",
""
],
[
"Xu",
"Hao",
""
]
] | Einstein-Gauss-Bonnet theory is a string-generated gravity theory when approaching the low energy limit. By introducing the higher order curvature terms, this theory is supposed to help to solve the black hole singularity problem. In this work, we investigate the evaporation of the static spherically symmetric neutral ... | 6.468991 | 6.554422 | 6.339793 | 6.076377 | 6.399849 | 6.646146 | 6.985122 | 6.283037 | 6.233832 | 7.051646 | 6.593796 | 6.192473 | 6.157358 | 6.048528 | 6.080524 | 6.166495 | 6.280054 | 6.084556 | 6.140532 | 6.224903 | 6.295465 |
1908.05330 | E. Aldo Arroyo | E. Aldo Arroyo, Mat\v{e}j Kudrna | Numerical solution for tachyon vacuum in the Schnabl gauge | 31 pages, 3 figures, appendix A added | JHEP02(2020)065 | 10.1007/JHEP02(2020)065 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on the level truncation scheme, we develop a new numerical method to
evaluate the tachyon vacuum solution in the Schnabl gauge up to level $L=24$.
We confirm the prediction that the energy associated to this numerical solution
has a local minimum at level $L=12$. Extrapolating the energy data of $L \leq
24$ to ... | [
{
"created": "Wed, 14 Aug 2019 20:02:01 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Sep 2019 17:06:24 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Nov 2019 03:21:07 GMT",
"version": "v3"
}
] | 2020-02-14 | [
[
"Arroyo",
"E. Aldo",
""
],
[
"Kudrna",
"Matěj",
""
]
] | Based on the level truncation scheme, we develop a new numerical method to evaluate the tachyon vacuum solution in the Schnabl gauge up to level $L=24$. We confirm the prediction that the energy associated to this numerical solution has a local minimum at level $L=12$. Extrapolating the energy data of $L \leq 24$ to in... | 10.744256 | 9.213359 | 11.092484 | 8.431009 | 9.255324 | 8.956493 | 8.306693 | 9.053869 | 8.298761 | 12.908184 | 8.581211 | 8.901359 | 9.404264 | 8.975415 | 8.890639 | 8.689293 | 8.734098 | 9.125483 | 8.742077 | 9.464292 | 8.749727 |
2009.06830 | Jie Jiang | Jie Jiang and Ming Zhang | Holographic Complexity in a Charged Supersymmetric Black Holes | 8 pages, 3 figures, and this paper has been accepted by PRD | Phys. Rev. D 102, 084010 (2020) | 10.1103/PhysRevD.102.084010 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For an ordinary charged system, it has been shown that by using the
"complexity equals action" (CA) conjecture, the late-time growth rate of the
holographic complexity is given by a difference between the value of $\Phi_H
Q+\Omega_H J$ on the inner and outer horizons. In this paper, we study the
influence of the chir... | [
{
"created": "Tue, 15 Sep 2020 02:14:21 GMT",
"version": "v1"
}
] | 2020-10-14 | [
[
"Jiang",
"Jie",
""
],
[
"Zhang",
"Ming",
""
]
] | For an ordinary charged system, it has been shown that by using the "complexity equals action" (CA) conjecture, the late-time growth rate of the holographic complexity is given by a difference between the value of $\Phi_H Q+\Omega_H J$ on the inner and outer horizons. In this paper, we study the influence of the chiral... | 8.072477 | 6.802792 | 8.516003 | 6.824132 | 7.244714 | 6.782945 | 6.825275 | 6.755759 | 6.806904 | 8.520907 | 6.444415 | 6.672007 | 7.369088 | 6.845474 | 6.856654 | 7.103951 | 6.92627 | 6.688288 | 6.783651 | 7.234092 | 6.765629 |
1612.00140 | Ayan Mukhopadhyay | Ayan Mukhopadhyay and Florian Preis | Semiholography for heavy ion collisions | 12 pages; 3 figures; Proceedings of Confinement XII @ Thessaloniki,
Greece -- August 28 to September 4, 2016 | null | 10.1051/epjconf/201713707015 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The formation of QGP in heavy ion collisions gives us a great opportunity for
learning about nonperturbative dynamics of QCD. Semiholography provides a new
consistent framework to combine perturbative and non-perturbative effects in a
coherent way and can be applied to obtain an effective description for heavy
ion co... | [
{
"created": "Thu, 1 Dec 2016 04:52:07 GMT",
"version": "v1"
}
] | 2017-03-27 | [
[
"Mukhopadhyay",
"Ayan",
""
],
[
"Preis",
"Florian",
""
]
] | The formation of QGP in heavy ion collisions gives us a great opportunity for learning about nonperturbative dynamics of QCD. Semiholography provides a new consistent framework to combine perturbative and non-perturbative effects in a coherent way and can be applied to obtain an effective description for heavy ion coll... | 10.882861 | 12.141944 | 11.636668 | 10.88964 | 11.071465 | 12.217498 | 11.46807 | 12.041183 | 11.288732 | 11.786718 | 11.786319 | 11.34161 | 10.754408 | 10.903436 | 11.026666 | 10.95226 | 10.535203 | 10.649517 | 10.821223 | 10.59141 | 10.604223 |
hep-th/9205015 | Ignatios Antoniadis | I. Antoniadis, P.O. Mazur and E. Mottola | Conformal Symmetry and Central Charges in 4 Dimensions | 20 pages, corrected tex version | Nucl.Phys. B388 (1992) 627-647 | 10.1016/0550-3213(92)90557-R | null | hep-th | null | The trace anomaly of matter in curved space generates an effective action for
the conformal factor of the metric tensor in $D=4$ dimensions, analogous to the
Polyakov action for $D=2$. We compute the contributions of the
reparameterization ghosts to the central charges for $D=4$, as well as the
quantum contribution o... | [
{
"created": "Thu, 7 May 1992 18:35:35 GMT",
"version": "v1"
},
{
"created": "Mon, 18 May 1992 17:55:01 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Antoniadis",
"I.",
""
],
[
"Mazur",
"P. O.",
""
],
[
"Mottola",
"E.",
""
]
] | The trace anomaly of matter in curved space generates an effective action for the conformal factor of the metric tensor in $D=4$ dimensions, analogous to the Polyakov action for $D=2$. We compute the contributions of the reparameterization ghosts to the central charges for $D=4$, as well as the quantum contribution of ... | 8.981876 | 8.395095 | 9.346755 | 8.307487 | 9.254308 | 9.176991 | 8.420415 | 8.662843 | 8.690341 | 9.378128 | 8.65714 | 8.58838 | 8.700624 | 8.640286 | 8.515581 | 8.098892 | 8.551631 | 8.40984 | 8.310843 | 8.779536 | 8.591451 |
hep-th/9909094 | Alexander Sevrin | Xavier Bekaert, Marc Henneaux and Alexander Sevrin | Deformations of Chiral Two-Forms in Six Dimensions | 7 pages, LaTeX, minor corrections, assumptions more clearly stated,
final version which will appear in Phys. Lett. B | Phys.Lett. B468 (1999) 228-232 | 10.1016/S0370-2693(99)01239-3 | ULB-TH/99-15, VUB/TENA/99/7 | hep-th | null | Motivated by a system consisting of a number of parallel M5-branes, we study
possible local deformations of a chiral two-form in six dimensions. Working to
first order in the coupling constant, this reduces to the study of the local
BRST cohomological group at ghost number zero. We obtain an exhaustive list of
all po... | [
{
"created": "Tue, 14 Sep 1999 11:48:18 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Oct 1999 08:15:04 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Bekaert",
"Xavier",
""
],
[
"Henneaux",
"Marc",
""
],
[
"Sevrin",
"Alexander",
""
]
] | Motivated by a system consisting of a number of parallel M5-branes, we study possible local deformations of a chiral two-form in six dimensions. Working to first order in the coupling constant, this reduces to the study of the local BRST cohomological group at ghost number zero. We obtain an exhaustive list of all poss... | 11.642101 | 8.240003 | 11.824077 | 10.561827 | 9.169391 | 7.934913 | 8.502372 | 8.611501 | 8.731132 | 12.79863 | 8.847853 | 9.914643 | 11.20089 | 10.061164 | 10.549623 | 10.410855 | 9.831733 | 10.279288 | 10.14185 | 11.490813 | 10.6071 |
0808.3832 | Vitaly Velizhanin | V.N. Velizhanin (St. Petersburg, INP) | The Four-Loop Konishi in N=4 SYM | 7 pages, some detailes of calculations added | JETP Lett.89:6-9,2009 | 10.1134/S0021364009010020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the result of a full direct component calculation for the planar
four-loop anomalous dimension of the Konishi operator in N =4 Supersymmetric
Yang-Mills theory. Our result confirms the results obtained from superfield
(arXiv:0712.3522, arXiv:0806.2095) and superstring (arXiv:0807.0399)
computations, which ... | [
{
"created": "Thu, 28 Aug 2008 05:49:20 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Sep 2008 16:17:00 GMT",
"version": "v2"
},
{
"created": "Fri, 21 Nov 2008 20:55:43 GMT",
"version": "v3"
}
] | 2009-12-10 | [
[
"Velizhanin",
"V. N.",
"",
"St. Petersburg, INP"
]
] | We present the result of a full direct component calculation for the planar four-loop anomalous dimension of the Konishi operator in N =4 Supersymmetric Yang-Mills theory. Our result confirms the results obtained from superfield (arXiv:0712.3522, arXiv:0806.2095) and superstring (arXiv:0807.0399) computations, which ta... | 8.407993 | 7.112418 | 10.08702 | 7.397888 | 7.501149 | 7.07083 | 7.791793 | 6.86955 | 7.198209 | 10.227957 | 7.035078 | 7.206786 | 8.416001 | 7.410572 | 7.565664 | 7.44854 | 7.453219 | 7.829303 | 7.710397 | 8.271657 | 7.426805 |
1707.01270 | Viktor Abramov | Viktor Abramov | Matrix 3-Lie superalgebras and BRST supersymmetry | 18 pages, manuscript is accepted for publication in International
Journal of Geometric Methods in Modern Physics | null | 10.1142/S0219887817501602 | null | hep-th math.RA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given a matrix Lie algebra one can construct the 3-Lie algebra by means of
the trace of a matrix. In the present paper we show that this approach can be
extended to the infinite-dimensional Lie algebra of vector fields on a manifold
if instead of the trace of a matrix we consider a differential 1-form which
satisfies... | [
{
"created": "Wed, 5 Jul 2017 09:23:43 GMT",
"version": "v1"
}
] | 2017-11-22 | [
[
"Abramov",
"Viktor",
""
]
] | Given a matrix Lie algebra one can construct the 3-Lie algebra by means of the trace of a matrix. In the present paper we show that this approach can be extended to the infinite-dimensional Lie algebra of vector fields on a manifold if instead of the trace of a matrix we consider a differential 1-form which satisfies c... | 6.125548 | 7.1275 | 7.016403 | 6.408911 | 6.734029 | 6.590992 | 6.838513 | 6.472684 | 6.758547 | 7.984558 | 6.495634 | 6.308063 | 6.34106 | 6.279267 | 6.158676 | 6.020655 | 6.041701 | 6.029778 | 6.196476 | 6.634273 | 6.170399 |
2308.10225 | Cyril Closset | Cyril Closset and Horia Magureanu | Reading between the rational sections: Global structures of 4d
$\mathcal{N}=2$ KK theories | 62 pages plus appendix; v2: added section 2.3 on non-invertible
symmetry in the SO(3) theory, fixed typos and references; v3: minor rewriting
of appendix A.5 | SciPost Phys. 16, 137 (2024) | 10.21468/SciPostPhys.16.5.137 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study how the global structure of rank-one 4d $\mathcal{N}=2$
supersymmetric field theories is encoded into global aspects of the
Seiberg-Witten elliptic fibration. Starting with the prototypical example of
the $\mathfrak{su}(2)$ gauge theory, we distinguish between relative and
absolute Seiberg-Witten curves. For... | [
{
"created": "Sun, 20 Aug 2023 10:35:36 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jan 2024 22:34:03 GMT",
"version": "v2"
},
{
"created": "Sun, 28 Jan 2024 22:34:35 GMT",
"version": "v3"
}
] | 2024-05-29 | [
[
"Closset",
"Cyril",
""
],
[
"Magureanu",
"Horia",
""
]
] | We study how the global structure of rank-one 4d $\mathcal{N}=2$ supersymmetric field theories is encoded into global aspects of the Seiberg-Witten elliptic fibration. Starting with the prototypical example of the $\mathfrak{su}(2)$ gauge theory, we distinguish between relative and absolute Seiberg-Witten curves. For i... | 5.748644 | 5.339807 | 6.560016 | 5.153876 | 5.331157 | 5.654278 | 5.401576 | 5.471371 | 5.352 | 6.85722 | 5.242571 | 5.386695 | 5.902756 | 5.487261 | 5.446085 | 5.475144 | 5.516145 | 5.431228 | 5.411672 | 5.812618 | 5.481788 |
0905.4756 | Edith Lorena Losada | C. Ccapa Ttira, C. D. Fosco and E. L. Losada | Non-superposition effects in the Dirichlet Casimir effect | 17 pages, LaTeX, no figures | J.Phys.A43:235402,2010 | 10.1088/1751-8113/43/23/235402 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study non-superposition effects in the Dirichlet Casimir interaction
energy for N boundaries in d spatial dimensions, quantifying its departure from
the case of an interaction where a superposition principle is valid. We first
derive some general results about those effects, and then show that they only
become neg... | [
{
"created": "Thu, 28 May 2009 21:52:35 GMT",
"version": "v1"
}
] | 2010-05-25 | [
[
"Ttira",
"C. Ccapa",
""
],
[
"Fosco",
"C. D.",
""
],
[
"Losada",
"E. L.",
""
]
] | We study non-superposition effects in the Dirichlet Casimir interaction energy for N boundaries in d spatial dimensions, quantifying its departure from the case of an interaction where a superposition principle is valid. We first derive some general results about those effects, and then show that they only become negli... | 16.100042 | 15.159576 | 16.605503 | 14.518077 | 15.882472 | 15.388962 | 15.389824 | 15.191735 | 14.101178 | 19.244717 | 15.006637 | 14.851581 | 14.887262 | 14.56973 | 14.548819 | 15.144679 | 15.46876 | 14.495153 | 14.996017 | 15.426987 | 14.312927 |
0907.4543 | Michael Faux | Michael G. Faux and Gregory D. Landweber | Spin Holography via Dimensional Enhancement | 13 pages, LaTeX | Phys.Lett.B681:161-165,2009 | 10.1016/j.physletb.2009.10.014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explain how all information about ambient component field spin assignments
in higher-dimensional off-shell supersymmetry is accessibly coded in
one-dimensional restrictions, known as shadows. We also explain how to
determine whether the components of a given one-dimensional supermultiplet may
assemble into represe... | [
{
"created": "Mon, 27 Jul 2009 06:52:15 GMT",
"version": "v1"
}
] | 2009-11-13 | [
[
"Faux",
"Michael G.",
""
],
[
"Landweber",
"Gregory D.",
""
]
] | We explain how all information about ambient component field spin assignments in higher-dimensional off-shell supersymmetry is accessibly coded in one-dimensional restrictions, known as shadows. We also explain how to determine whether the components of a given one-dimensional supermultiplet may assemble into represent... | 29.144329 | 25.983961 | 26.69446 | 23.402409 | 28.067146 | 28.180485 | 25.42893 | 25.246927 | 24.508791 | 31.184483 | 24.528433 | 23.964584 | 26.085409 | 23.739136 | 23.228889 | 24.508528 | 23.388258 | 24.156624 | 23.683153 | 24.834671 | 22.792835 |
1206.0416 | Sergei V. Ketov | Sergei V. Ketov and Natsuki Watanabe | Dark Energy in Modified Supergravity | LaTeX, 9 pages, 1 figure; secs. 2 and 3 extended, references updated,
title and abstract revised | Mod. Phys. Lett. A, Vol. 27, No. 39 (2012) 1250225 | 10.1142/S0217732312502252 | IPMU12-0108 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a supersymmetric extension of the dynamical dark energy function
and the corresponding scalar (super)potential in F(R) supergravity. Our model
is viable in the Einstein approximation, and also has an analytic (regular)
Wess-Zumino-type scalar superpotential. The hidden sector responsible for
spontaneous su... | [
{
"created": "Sun, 3 Jun 2012 02:09:35 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Sep 2012 03:12:10 GMT",
"version": "v2"
}
] | 2012-12-27 | [
[
"Ketov",
"Sergei V.",
""
],
[
"Watanabe",
"Natsuki",
""
]
] | We propose a supersymmetric extension of the dynamical dark energy function and the corresponding scalar (super)potential in F(R) supergravity. Our model is viable in the Einstein approximation, and also has an analytic (regular) Wess-Zumino-type scalar superpotential. The hidden sector responsible for spontaneous supe... | 19.448952 | 17.2665 | 23.305687 | 16.2801 | 16.857161 | 16.865774 | 18.647003 | 16.351702 | 17.916109 | 23.949909 | 16.200455 | 15.679213 | 19.760237 | 16.540102 | 16.184217 | 16.740183 | 16.650911 | 16.027739 | 17.367609 | 19.784241 | 16.789978 |
hep-th/0612225 | Gabriel Cardoso | G.L. Cardoso, B. de Wit and S. Mahapatra | Black hole entropy functions and attractor equations | 21 pages,LaTeX,minor changes | JHEP 0703:085,2007 | 10.1088/1126-6708/2007/03/085 | LMU-ASC 84/06, ITP-UU-06/54, SPIN-06/44 | hep-th | null | The entropy and the attractor equations for static extremal black hole
solutions follow from a variational principle based on an entropy function. In
the general case such an entropy function can be derived from the reduced
action evaluated in a near-horizon geometry. BPS black holes constitute special
solutions of t... | [
{
"created": "Wed, 20 Dec 2006 18:14:17 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Mar 2007 13:03:28 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Cardoso",
"G. L.",
""
],
[
"de Wit",
"B.",
""
],
[
"Mahapatra",
"S.",
""
]
] | The entropy and the attractor equations for static extremal black hole solutions follow from a variational principle based on an entropy function. In the general case such an entropy function can be derived from the reduced action evaluated in a near-horizon geometry. BPS black holes constitute special solutions of thi... | 8.060714 | 6.577711 | 8.72971 | 6.856636 | 7.79128 | 6.652569 | 7.318456 | 6.695049 | 7.41259 | 9.381619 | 7.149902 | 7.28274 | 8.124031 | 7.078119 | 6.980784 | 6.980803 | 7.11952 | 7.089358 | 6.947394 | 7.976622 | 7.133189 |
hep-th/9912177 | Alfonso V. Ramallo | P. M. Llatas, A. V. Ramallo and J. M. Sanchez de Santos | World-volume Solitons of the D3-brane in the Background of (p,q)
Five-branes | 22 pages, LaTeX, 1 eps file | Int.J.Mod.Phys.A15:4477-4498,2000 | 10.1142/S0217751X00001841 | US-FT-25/99 | hep-th | null | We analyze the world-volume solitons of a D3-brane probe in the background of
parallel (p,q) five-branes. The D3-brane is embedded along the directions
transverse to the five-branes of the background. By using the S-duality
invariance of the D3-brane, we find a first-order differential equation whose
solutions satura... | [
{
"created": "Mon, 20 Dec 1999 16:20:50 GMT",
"version": "v1"
}
] | 2016-12-21 | [
[
"Llatas",
"P. M.",
""
],
[
"Ramallo",
"A. V.",
""
],
[
"de Santos",
"J. M. Sanchez",
""
]
] | We analyze the world-volume solitons of a D3-brane probe in the background of parallel (p,q) five-branes. The D3-brane is embedded along the directions transverse to the five-branes of the background. By using the S-duality invariance of the D3-brane, we find a first-order differential equation whose solutions saturate... | 6.844442 | 6.183843 | 7.151647 | 6.084187 | 6.222533 | 5.726322 | 5.609434 | 5.736388 | 5.861005 | 8.505579 | 6.216094 | 6.123365 | 6.68455 | 6.33857 | 6.223938 | 6.180341 | 6.170359 | 6.155193 | 6.222447 | 6.447963 | 6.131767 |
1811.12419 | Felix Rudolph | Chrysoula Markou, Felix J. Rudolph, Angnis Schmidt-May | Gravity with antisymmetric components | 23 pages, v2: Modified discussion on causality, modified convention
in eq. 2.10 and thereafter. References added. v3: Added extended discussion
of tachyonic mass pole. v4: matches published version | null | 10.1088/1361-6382/ab0fd6 | MPP-2018-288 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work proposes a new gravitational theory formulated in terms of the
vierbein field. The vierbein contains components which can be shifted by local
Lorentz transformations and therefore do not show up in the spacetime metric.
These components are given dynamics and become physical in our setup. They
enter the mas... | [
{
"created": "Thu, 29 Nov 2018 19:00:03 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Dec 2018 16:48:13 GMT",
"version": "v2"
},
{
"created": "Fri, 18 Jan 2019 10:23:22 GMT",
"version": "v3"
},
{
"created": "Fri, 17 May 2019 09:06:35 GMT",
"version": "v4"
}
] | 2019-05-20 | [
[
"Markou",
"Chrysoula",
""
],
[
"Rudolph",
"Felix J.",
""
],
[
"Schmidt-May",
"Angnis",
""
]
] | This work proposes a new gravitational theory formulated in terms of the vierbein field. The vierbein contains components which can be shifted by local Lorentz transformations and therefore do not show up in the spacetime metric. These components are given dynamics and become physical in our setup. They enter the massl... | 8.932683 | 8.660832 | 8.578341 | 8.374651 | 8.666862 | 8.988365 | 8.59943 | 8.327432 | 8.227808 | 9.528817 | 8.21061 | 8.420475 | 8.929668 | 8.713135 | 8.917772 | 8.605865 | 8.514076 | 8.734823 | 8.626787 | 8.847686 | 8.379702 |
hep-th/9812034 | Paul Townsend | G.W. Gibbons and P.K. Townsend | Black Holes and Calogero Models | Revtex 5pp. Revision includes improved discussion of entropy and
includes an additional reference | Phys.Lett.B454:187-192,1999 | 10.1016/S0370-2693(99)00266-X | null | hep-th | null | We argue that the large $n$ limit of the $n$-particle $SU(1,1|2)$
superconformal Calogero model provides a microscopic description of the extreme
Reissner-Nordstr{\"o}m black hole in the near-horizon limit.
| [
{
"created": "Thu, 3 Dec 1998 19:13:32 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Dec 1998 15:21:33 GMT",
"version": "v2"
},
{
"created": "Fri, 5 Feb 1999 19:33:25 GMT",
"version": "v3"
},
{
"created": "Tue, 23 Feb 1999 17:36:38 GMT",
"version": "v4"
}
] | 2009-10-07 | [
[
"Gibbons",
"G. W.",
""
],
[
"Townsend",
"P. K.",
""
]
] | We argue that the large $n$ limit of the $n$-particle $SU(1,1|2)$ superconformal Calogero model provides a microscopic description of the extreme Reissner-Nordstr{\"o}m black hole in the near-horizon limit. | 5.16202 | 3.70342 | 5.594013 | 4.088177 | 3.964853 | 4.058505 | 4.685279 | 3.917942 | 3.831077 | 4.937764 | 4.246914 | 4.145678 | 4.624365 | 4.12978 | 4.245138 | 4.227339 | 4.120364 | 4.203441 | 4.095682 | 4.663704 | 4.021431 |
2101.05281 | Jakob Moritz | Federico Carta and Jakob Moritz | Resolving spacetime singularities in flux compactifications & KKLT | 42 pages, 19 figures, 1 appendix; v2: references added, minor
corrections; v3: monodromies corrected, reference added; v4: matches version
published in JHEP | null | 10.1007/JHEP08(2021)093 | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | In flux compactifications of type IIB string theory with D3 and seven-branes,
the negative induced D3 charge localized on seven-branes leads to an apparently
pathological profile of the metric sufficiently close to the source. With the
volume modulus stabilized in a KKLT de Sitter vacuum this pathological region
take... | [
{
"created": "Wed, 13 Jan 2021 19:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Jan 2021 23:46:06 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Feb 2021 16:13:27 GMT",
"version": "v3"
},
{
"created": "Tue, 24 Aug 2021 21:39:52 GMT",
"version": "v4"
}
] | 2021-09-15 | [
[
"Carta",
"Federico",
""
],
[
"Moritz",
"Jakob",
""
]
] | In flux compactifications of type IIB string theory with D3 and seven-branes, the negative induced D3 charge localized on seven-branes leads to an apparently pathological profile of the metric sufficiently close to the source. With the volume modulus stabilized in a KKLT de Sitter vacuum this pathological region takes ... | 7.400888 | 7.385117 | 8.365511 | 7.222746 | 7.325761 | 7.445094 | 7.659426 | 7.698648 | 7.35521 | 9.05262 | 7.342203 | 7.69606 | 7.462303 | 7.411686 | 7.55568 | 7.570086 | 7.540483 | 7.486967 | 7.339466 | 7.816965 | 7.450245 |
2212.06496 | Tajron Juri\'c Dr. sc. | Tajron Juri\'c and Filip Po\v{z}ar | Noncommutative correction to the entropy of charged BTZ black hole | 19 pages, typos corrected | Symmetry 2023, 15(2), 417 | 10.3390/sym15020417 | RBI-ThPhys-2022-55 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Noncommutative geometry is an established potential candidate for including
quantum phenomena in gravitation. We outline the formalism of Hopf algebras and
its connection to the algebra of infinitesimal diffeomorphisms. Using a
Drinfeld twist we deform spacetime symmetries, algebra of vector fields and
differential f... | [
{
"created": "Tue, 13 Dec 2022 11:25:32 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Dec 2022 15:10:51 GMT",
"version": "v2"
},
{
"created": "Tue, 7 Feb 2023 08:58:59 GMT",
"version": "v3"
},
{
"created": "Tue, 14 Mar 2023 12:31:18 GMT",
"version": "v4"
}
] | 2023-03-15 | [
[
"Jurić",
"Tajron",
""
],
[
"Požar",
"Filip",
""
]
] | Noncommutative geometry is an established potential candidate for including quantum phenomena in gravitation. We outline the formalism of Hopf algebras and its connection to the algebra of infinitesimal diffeomorphisms. Using a Drinfeld twist we deform spacetime symmetries, algebra of vector fields and differential for... | 9.522254 | 9.368018 | 9.276659 | 8.703144 | 9.394516 | 10.184586 | 9.407082 | 9.102344 | 9.363474 | 10.286117 | 9.341744 | 9.154766 | 9.292659 | 9.289547 | 9.370238 | 9.28742 | 9.500176 | 9.152626 | 9.378537 | 9.263389 | 9.071775 |
1907.10021 | Athira P V | Athira PV, A Manu | Classical double copy from Color Kinematics duality: A proof in the soft
limit | 47 pages, minor changes and citations added | Phys. Rev. D 101, 046014 (2020) | 10.1103/PhysRevD.101.046014 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Classical double copy is an intriguing relationship between classical
solutions to a gravity theory and solutions to classical Yang-Mills equations.
Although formally inspired by the double copy relation between (quantum)
scattering amplitudes in QCD and perturbative gravity, a direct proof of the
former from the lat... | [
{
"created": "Tue, 23 Jul 2019 17:26:57 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Aug 2019 06:14:15 GMT",
"version": "v2"
}
] | 2020-02-19 | [
[
"PV",
"Athira",
""
],
[
"Manu",
"A",
""
]
] | Classical double copy is an intriguing relationship between classical solutions to a gravity theory and solutions to classical Yang-Mills equations. Although formally inspired by the double copy relation between (quantum) scattering amplitudes in QCD and perturbative gravity, a direct proof of the former from the latte... | 7.352454 | 7.509333 | 7.186982 | 6.414305 | 7.434275 | 7.482331 | 6.984574 | 6.60426 | 6.737955 | 7.914996 | 6.622406 | 6.516602 | 6.55494 | 6.586847 | 6.785727 | 6.952071 | 6.887239 | 6.69318 | 6.625124 | 6.868257 | 6.702636 |
1609.04454 | SIbasish Banerjee | Sibasish Banerjee | Calabi-Yau compactification of type II string theories | PhD Thesis, defended on 29-09-2015 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Superstring theories are the most promising theories for unified description
of all fundamental interactions including gravity. However, these theories are
formulated consistently only in 10 spacetime dimensions. Therefore, to connect
to the observable world, it is required to compactify 6 out of those 10
dimensions ... | [
{
"created": "Wed, 14 Sep 2016 21:55:07 GMT",
"version": "v1"
}
] | 2016-09-16 | [
[
"Banerjee",
"Sibasish",
""
]
] | Superstring theories are the most promising theories for unified description of all fundamental interactions including gravity. However, these theories are formulated consistently only in 10 spacetime dimensions. Therefore, to connect to the observable world, it is required to compactify 6 out of those 10 dimensions in... | 6.535312 | 6.571545 | 7.19224 | 6.325742 | 6.585507 | 6.431877 | 6.226014 | 6.220413 | 6.310082 | 6.904646 | 6.326397 | 6.188684 | 6.416745 | 6.157972 | 6.382476 | 6.215673 | 6.327964 | 6.365756 | 6.134377 | 6.529263 | 6.304148 |
1412.8475 | Jacob Bourjaily | Nima Arkani-Hamed, Jacob L. Bourjaily, Freddy Cachazo, Alexander
Postnikov, and Jaroslav Trnka | On-Shell Structures of MHV Amplitudes Beyond the Planar Limit | 16 pages, 19 figures | null | null | CALT-TH-2014-169 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate an exploration of on-shell functions in $\mathcal{N}=4$ SYM
beyond the planar limit by providing compact, combinatorial expressions for all
leading singularities of MHV amplitudes and showing that they can always be
expressed as a positive sum of differently ordered Parke-Taylor tree
amplitudes. This is u... | [
{
"created": "Mon, 29 Dec 2014 21:00:03 GMT",
"version": "v1"
}
] | 2014-12-31 | [
[
"Arkani-Hamed",
"Nima",
""
],
[
"Bourjaily",
"Jacob L.",
""
],
[
"Cachazo",
"Freddy",
""
],
[
"Postnikov",
"Alexander",
""
],
[
"Trnka",
"Jaroslav",
""
]
] | We initiate an exploration of on-shell functions in $\mathcal{N}=4$ SYM beyond the planar limit by providing compact, combinatorial expressions for all leading singularities of MHV amplitudes and showing that they can always be expressed as a positive sum of differently ordered Parke-Taylor tree amplitudes. This is und... | 6.067554 | 6.471 | 6.591676 | 5.870406 | 5.90997 | 6.064436 | 5.721825 | 6.118795 | 6.158542 | 7.316097 | 6.033425 | 6.171481 | 6.067484 | 5.970858 | 6.145442 | 6.008224 | 6.117441 | 6.186208 | 5.923558 | 6.090137 | 5.776732 |
1403.3224 | Tehseen Rug | Stefan Hofmann and Tehseen Rug | A Quantum Bound-State Description of Black Holes | Sections on asymptotic framework for bound states and composite
operator renormalization added. Derivation of main results presented in
greater detail. References added. Submitted to Nuclear Physics B | null | null | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A relativistic framework for the description of bound states consisting of a
large number of quantum constituents is presented, and applied to black-hole
interiors. At the parton level, the constituent distribution, number and energy
density inside black holes are calculated, and gauge corrections are discussed.
A si... | [
{
"created": "Thu, 13 Mar 2014 10:28:56 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Dec 2014 10:06:06 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Oct 2015 10:39:35 GMT",
"version": "v3"
}
] | 2015-10-27 | [
[
"Hofmann",
"Stefan",
""
],
[
"Rug",
"Tehseen",
""
]
] | A relativistic framework for the description of bound states consisting of a large number of quantum constituents is presented, and applied to black-hole interiors. At the parton level, the constituent distribution, number and energy density inside black holes are calculated, and gauge corrections are discussed. A simp... | 16.31115 | 14.725613 | 13.940504 | 13.943977 | 14.031091 | 14.621792 | 12.547249 | 13.947016 | 14.110726 | 13.334818 | 14.424614 | 14.714957 | 14.256593 | 13.553281 | 14.095092 | 14.349689 | 14.147344 | 13.828233 | 13.399223 | 13.552098 | 14.860443 |
2204.13415 | Yusuke Nishida | Tatsuya Amitani and Yusuke Nishida | Torsion-induced chiral magnetic current in equilibrium | 9 pages, 4 figures; published version | Annals of Physics 448 (2023) 169181 | 10.1016/j.aop.2022.169181 | null | hep-th cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study equilibrium transport properties of massless Dirac fermions at
finite temperature and chemical potential in spacetime accompanied by torsion,
which in four dimensions couples with Dirac fermions as an axial gauge field.
In particular, we compute the current density at the linear order in the
torsion as well ... | [
{
"created": "Thu, 28 Apr 2022 11:25:18 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Dec 2022 11:50:47 GMT",
"version": "v2"
}
] | 2022-12-06 | [
[
"Amitani",
"Tatsuya",
""
],
[
"Nishida",
"Yusuke",
""
]
] | We study equilibrium transport properties of massless Dirac fermions at finite temperature and chemical potential in spacetime accompanied by torsion, which in four dimensions couples with Dirac fermions as an axial gauge field. In particular, we compute the current density at the linear order in the torsion as well as... | 10.366277 | 10.493334 | 11.276896 | 9.571222 | 10.4593 | 10.659369 | 10.488694 | 10.514975 | 9.502871 | 11.792441 | 10.200433 | 10.073173 | 10.334754 | 9.954162 | 9.91012 | 9.740357 | 10.037469 | 10.340705 | 10.117016 | 10.462597 | 10.076872 |
hep-th/0105310 | Frans Klinkhamer | F.R. Klinkhamer and C. Mayer | Torsion, topology and CPT anomaly in two-dimensional chiral U(1) gauge
theory | LaTeX with elsart.cls, 20 pages, v3: to appear in Nucl. Phys. B | Nucl.Phys. B616 (2001) 215-232 | 10.1016/S0550-3213(01)00463-1 | KA-TP-17-2001 | hep-th gr-qc | null | We consider the CPT anomaly of two-dimensional chiral U(1) gauge theory on a
torus with topologically nontrivial zweibeins corresponding to the presence of
spacetime torsion. The resulting chiral determinant can be expressed in terms
of the standard chiral determinant without torsion, but with modified spinor
boundar... | [
{
"created": "Wed, 30 May 2001 21:42:42 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Jun 2001 19:34:27 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Sep 2001 17:49:54 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Klinkhamer",
"F. R.",
""
],
[
"Mayer",
"C.",
""
]
] | We consider the CPT anomaly of two-dimensional chiral U(1) gauge theory on a torus with topologically nontrivial zweibeins corresponding to the presence of spacetime torsion. The resulting chiral determinant can be expressed in terms of the standard chiral determinant without torsion, but with modified spinor boundary ... | 8.044374 | 6.622155 | 8.271871 | 6.59854 | 6.795239 | 7.331907 | 6.428075 | 7.389269 | 6.481813 | 8.228602 | 6.828809 | 6.825099 | 7.901464 | 7.294516 | 7.698929 | 7.051743 | 7.386826 | 7.062741 | 7.452082 | 8.014696 | 7.188386 |
hep-th/9811087 | Shigeki Sugimoto | N.Sasakura and S.Sugimoto (Kyoto University) | M-theory description of 1/4 BPS states in N=4 supersymmetric Yang-Mills
theory | 16 pages, 4 Postscript figures, LaTeX | Prog.Theor.Phys. 101 (1999) 749-761 | 10.1143/PTP.101.749 | KUNS-1543 | hep-th | null | We discuss BPS states preserving 1/4 supersymmetries of N=4 supersymmetric
Yang-Mills theory as M2-branes holomorphically embedded and ending on
M5-branes. We use techniques in electrodynamics to find the M2-brane
configurations, and give some explicit examples. In case the M2-brane
worldsheet has handles, the worlds... | [
{
"created": "Tue, 10 Nov 1998 04:40:14 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Sasakura",
"N.",
"",
"Kyoto University"
],
[
"Sugimoto",
"S.",
"",
"Kyoto University"
]
] | We discuss BPS states preserving 1/4 supersymmetries of N=4 supersymmetric Yang-Mills theory as M2-branes holomorphically embedded and ending on M5-branes. We use techniques in electrodynamics to find the M2-brane configurations, and give some explicit examples. In case the M2-brane worldsheet has handles, the worldshe... | 8.444391 | 7.673146 | 9.413752 | 7.3273 | 7.875489 | 7.673671 | 7.89569 | 7.509154 | 7.872048 | 10.245434 | 7.481412 | 7.947453 | 8.927111 | 7.689944 | 7.916472 | 7.849681 | 7.833544 | 7.893031 | 7.843199 | 8.364566 | 7.766225 |
1205.6238 | George Alekseev A. | G. A. Alekseev | Monodromy transform and the integral equation method for solving the
string gravity and supergravity equations in four and higher dimensions | RevTex 7 pages, 1 figure | Phys. Rev. D88, 021503(R) (2013) | 10.1103/PhysRevD.88.021503 | null | hep-th gr-qc nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The monodromy transform and corresponding integral equation method described
here give rise to a general systematic approach for solving integrable
reductions of field equations for gravity coupled bosonic dynamics in string
gravity and supergravity in four and higher dimensions. For different types of
fields in spac... | [
{
"created": "Mon, 28 May 2012 23:45:40 GMT",
"version": "v1"
}
] | 2013-12-19 | [
[
"Alekseev",
"G. A.",
""
]
] | The monodromy transform and corresponding integral equation method described here give rise to a general systematic approach for solving integrable reductions of field equations for gravity coupled bosonic dynamics in string gravity and supergravity in four and higher dimensions. For different types of fields in space-... | 9.199203 | 10.137731 | 9.324019 | 8.69136 | 9.160315 | 9.726084 | 9.733592 | 9.161199 | 9.006683 | 10.521458 | 9.273364 | 9.100966 | 8.64543 | 8.973025 | 9.166792 | 8.9186 | 9.117532 | 9.189158 | 8.952494 | 8.994967 | 8.897156 |
hep-th/9904102 | Dr Tsou Sheung Tsun | HM Chan (Rutherford Appleton Lab), and ST Tsou (Oxford) | Nonabelian Generalization of Electric-Magnetic Duality - a Brief Review | 37 pages, Latex, 10 figures using epsfig, 4 charts in ps; invited
review to appear in Int. J. Mod. Phys | Int.J.Mod.Phys. A14 (1999) 2139-2172 | 10.1142/S0217751X99001093 | RAL-TR-1999-014 | hep-th | null | A loop space formulation of Yang-Mills theory high-lighting the significance
of monopoles for the existence of gauge potentials is used to derive a
generalization of electric-magnetic duality to the nonabelian theory. The
result implies that the gauge symmetry is doubled from SU(N) to $SU(N) \times
\widetilde{SU}(N)$... | [
{
"created": "Wed, 14 Apr 1999 15:40:07 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Chan",
"HM",
"",
"Rutherford Appleton Lab"
],
[
"Tsou",
"ST",
"",
"Oxford"
]
] | A loop space formulation of Yang-Mills theory high-lighting the significance of monopoles for the existence of gauge potentials is used to derive a generalization of electric-magnetic duality to the nonabelian theory. The result implies that the gauge symmetry is doubled from SU(N) to $SU(N) \times \widetilde{SU}(N)$, ... | 6.194491 | 5.821017 | 5.758292 | 5.35208 | 5.659567 | 5.58325 | 5.440745 | 5.740636 | 5.543586 | 6.399817 | 5.504614 | 5.560324 | 5.402377 | 5.544328 | 5.527238 | 5.464274 | 5.548879 | 5.42935 | 5.488702 | 5.669501 | 5.437039 |
hep-th/0610216 | Davoud Kamani | Davoud Kamani | Supersymmetric Form of the String Action in the Presence of the Gauge
Field | 14 pages, Latex, no figure, corrected version | Can. J. Phys. 87, 695-701 (2009) | 10.1139/P08-125 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this manuscript we study the superstring theory with an Abelian worldsheet
gauge field. The components of the gauge field appear as a space and a time
coordinates. We call them "fictitious coordinates". The worldsheet
supersymmetry and the Poincar\'e symmetry of this model will be analyzed. The
$T$-duality and qua... | [
{
"created": "Thu, 19 Oct 2006 13:24:59 GMT",
"version": "v1"
},
{
"created": "Mon, 7 May 2007 16:30:43 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Oct 2007 11:31:11 GMT",
"version": "v3"
},
{
"created": "Sat, 25 Jul 2009 12:31:10 GMT",
"version": "v4"
}
] | 2020-08-21 | [
[
"Kamani",
"Davoud",
""
]
] | In this manuscript we study the superstring theory with an Abelian worldsheet gauge field. The components of the gauge field appear as a space and a time coordinates. We call them "fictitious coordinates". The worldsheet supersymmetry and the Poincar\'e symmetry of this model will be analyzed. The $T$-duality and quant... | 11.234918 | 7.527151 | 10.190727 | 8.496386 | 9.852346 | 7.406363 | 7.316481 | 8.060252 | 8.446527 | 11.942989 | 8.470959 | 9.013143 | 10.692883 | 9.242965 | 9.653379 | 9.111741 | 9.104501 | 9.228599 | 9.716956 | 10.646115 | 9.267562 |
0910.3334 | Evgeny Skvortsov D | E.D.Skvortsov | Gauge fields in (A)dS within the unfolded approach: algebraic aspects | 59 pages, replaced with revised verion | JHEP 1001:106,2010 | 10.1007/JHEP01(2010)106 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has recently been shown that generalized connections of the (A)dS space
symmetry algebra provide an effective geometric and algebraic framework for all
types of gauge fields in (A)dS, both for massless and partially-massless. The
equations of motion are equipped with a nilpotent operator called $\sigma_-$
whose co... | [
{
"created": "Mon, 19 Oct 2009 06:36:17 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Dec 2009 09:03:23 GMT",
"version": "v2"
}
] | 2010-02-18 | [
[
"Skvortsov",
"E. D.",
""
]
] | It has recently been shown that generalized connections of the (A)dS space symmetry algebra provide an effective geometric and algebraic framework for all types of gauge fields in (A)dS, both for massless and partially-massless. The equations of motion are equipped with a nilpotent operator called $\sigma_-$ whose coho... | 11.458717 | 10.754385 | 11.70171 | 10.008922 | 10.206099 | 10.487162 | 10.86713 | 10.317612 | 10.129217 | 12.696596 | 10.450015 | 10.785661 | 11.038008 | 10.490689 | 10.150807 | 10.88021 | 10.23434 | 10.447312 | 9.997461 | 11.145428 | 10.307261 |
1501.07620 | George Papadopoulos | S. Beck, J. B. Gutowski and G. Papadopoulos | Supersymmetry of IIA warped flux AdS and flat backgrounds | 44 pages | null | 10.1007/JHEP09(2015)135 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We identify the fractions of supersymmetry preserved by the most general
warped flux AdS and flat backgrounds in both massive and standard IIA
supergravities. We find that $AdS_n\times_w M^{10-n}$ preserve $2^{[{n\over2}]}
k$ for $n\leq 4$ and $2^{[{n\over2}]+1} k$ for $4<n\leq 7$ supersymmetries,
$k\in \bN_{>0}$. In... | [
{
"created": "Thu, 29 Jan 2015 21:33:10 GMT",
"version": "v1"
}
] | 2015-10-28 | [
[
"Beck",
"S.",
""
],
[
"Gutowski",
"J. B.",
""
],
[
"Papadopoulos",
"G.",
""
]
] | We identify the fractions of supersymmetry preserved by the most general warped flux AdS and flat backgrounds in both massive and standard IIA supergravities. We find that $AdS_n\times_w M^{10-n}$ preserve $2^{[{n\over2}]} k$ for $n\leq 4$ and $2^{[{n\over2}]+1} k$ for $4<n\leq 7$ supersymmetries, $k\in \bN_{>0}$. In a... | 4.793158 | 4.291023 | 5.723691 | 4.523239 | 4.340847 | 4.215612 | 4.279335 | 4.485492 | 4.325648 | 5.887346 | 4.37389 | 4.536331 | 5.288133 | 4.646464 | 4.454478 | 4.572103 | 4.618262 | 4.477169 | 4.614178 | 5.071028 | 4.540132 |
1503.04670 | Alexander Manashov | A.N. Manashov and M. Strohmaier | Conformal constraints for anomalous dimensions of leading twist
operators | 14 pages, 6 figures | null | 10.1140/epjc/s10052-015-3595-2 | DESY 15-038 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Leading-twist operators have a remarkable property that their divergence
vanishes in a free theory. Recently it was suggested that this property can be
used for an alternative technique to calculate anomalous dimensions of
leading-twist operators and allows one to gain one order in perturbation theory
so that, i.e., ... | [
{
"created": "Mon, 16 Mar 2015 14:30:35 GMT",
"version": "v1"
}
] | 2015-09-02 | [
[
"Manashov",
"A. N.",
""
],
[
"Strohmaier",
"M.",
""
]
] | Leading-twist operators have a remarkable property that their divergence vanishes in a free theory. Recently it was suggested that this property can be used for an alternative technique to calculate anomalous dimensions of leading-twist operators and allows one to gain one order in perturbation theory so that, i.e., tw... | 8.955477 | 8.268923 | 9.195423 | 8.181176 | 9.039565 | 8.805413 | 9.308539 | 8.974784 | 8.643262 | 9.349401 | 9.028749 | 8.620129 | 8.696984 | 8.284214 | 8.144896 | 8.570325 | 8.600673 | 8.325849 | 8.400481 | 8.487602 | 8.426151 |
1612.01723 | Hrachya Babujian | H. M. Babujian, M. Karowski and A. M. Tsvelik | Multipoint Green's functions in 1+1 dimensional integrable quantum field
theories | 33 pages, 8 figures, minor corrections | null | 10.1016/j.nuclphysb.2017.02.002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the multipoint Green functions in 1+1 dimensional integrable
quantum field theories. We use the crossing formula for general models and
calculate the 3 and 4 point functions taking in to account only the lower
nontrivial intermediate states contributions. Then we apply the general results
to the examples... | [
{
"created": "Tue, 6 Dec 2016 09:45:55 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Dec 2016 09:41:27 GMT",
"version": "v2"
}
] | 2017-04-05 | [
[
"Babujian",
"H. M.",
""
],
[
"Karowski",
"M.",
""
],
[
"Tsvelik",
"A. M.",
""
]
] | We calculate the multipoint Green functions in 1+1 dimensional integrable quantum field theories. We use the crossing formula for general models and calculate the 3 and 4 point functions taking in to account only the lower nontrivial intermediate states contributions. Then we apply the general results to the examples o... | 11.528227 | 11.317529 | 11.748086 | 11.773776 | 13.293989 | 11.076106 | 12.647217 | 11.241306 | 11.93633 | 12.680513 | 11.15553 | 11.16123 | 11.931561 | 11.44748 | 11.31584 | 11.605123 | 11.137017 | 10.847558 | 11.042134 | 11.862484 | 10.929215 |
hep-th/9605130 | Shao-Ming Fei | Sergio Albeverio, Shao-Ming Fei | Symmetry, Integrable Chain Models and Stochastic Processes | 34 pages, Latex | Rev.Math.Phys. 10 (1998) 723-750 | null | null | hep-th cond-mat math.QA nlin.SI q-alg solv-int | null | A general way to construct chain models with certain Lie algebraic or quantum
Lie algebraic symmetries is presented. These symmetric models give rise to
series of integrable systems. As an example the chain models with $A_n$
symmetry and the related Temperley-Lieb algebraic structures and
representations are discusse... | [
{
"created": "Sat, 18 May 1996 10:49:40 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Albeverio",
"Sergio",
""
],
[
"Fei",
"Shao-Ming",
""
]
] | A general way to construct chain models with certain Lie algebraic or quantum Lie algebraic symmetries is presented. These symmetric models give rise to series of integrable systems. As an example the chain models with $A_n$ symmetry and the related Temperley-Lieb algebraic structures and representations are discussed.... | 9.875309 | 9.668694 | 10.039129 | 8.976552 | 8.829695 | 9.799197 | 8.959533 | 8.810518 | 8.916446 | 10.150505 | 8.436061 | 8.688221 | 9.828986 | 8.755532 | 9.380521 | 9.400633 | 8.976978 | 8.666422 | 8.713447 | 9.190663 | 8.683232 |
1611.04592 | Ethan Dyer | Ethan Dyer, Guy Gur-Ari | 2D CFT Partition Functions at Late Times | 36 pages, 7 figures | null | 10.1007/JHEP08(2017)075 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the late time behavior of the analytically continued partition
function $Z(\beta + it) Z(\beta - it)$ in holographic $2d$ CFTs. This is a
probe of information loss in such theories and in their holographic duals. We
show that each Virasoro character decays in time, and so information is not
restored at th... | [
{
"created": "Mon, 14 Nov 2016 21:00:01 GMT",
"version": "v1"
}
] | 2017-09-13 | [
[
"Dyer",
"Ethan",
""
],
[
"Gur-Ari",
"Guy",
""
]
] | We consider the late time behavior of the analytically continued partition function $Z(\beta + it) Z(\beta - it)$ in holographic $2d$ CFTs. This is a probe of information loss in such theories and in their holographic duals. We show that each Virasoro character decays in time, and so information is not restored at the ... | 8.725842 | 8.683359 | 10.505194 | 8.26146 | 8.35606 | 8.000969 | 8.719791 | 8.245254 | 8.516959 | 9.878366 | 8.303987 | 8.353436 | 8.94434 | 8.362483 | 8.441406 | 8.307701 | 8.201026 | 8.303549 | 8.369688 | 8.961239 | 8.416992 |
hep-th/9706035 | Philippe Brax | Ph. Brax (SPhT, Saclay) and Neil Turok (DAMTP, Cambridge) | Exponentially Small Couplings and the Hierarchy Problem | 8 pages, latex, 2 figures | Phys.Lett. B413 (1997) 331-335 | 10.1016/S0370-2693(97)01119-2 | Saclay preprint, 97/57, DAMTP preprint, 97/57 | hep-th | null | We propose a stringy mechanism whereby a large hierarchy between symmetry
breaking scales is generated. This mechanism is based upon the existence of a
fifth dimension compactified on a segment. We focus on a simple supersymmetric
model with one massless Higgs field in the 3 of SU(3) and another one in the
$\bar 3$ o... | [
{
"created": "Thu, 5 Jun 1997 12:12:01 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Brax",
"Ph.",
"",
"SPhT, Saclay"
],
[
"Turok",
"Neil",
"",
"DAMTP, Cambridge"
]
] | We propose a stringy mechanism whereby a large hierarchy between symmetry breaking scales is generated. This mechanism is based upon the existence of a fifth dimension compactified on a segment. We focus on a simple supersymmetric model with one massless Higgs field in the 3 of SU(3) and another one in the $\bar 3$ on ... | 7.341634 | 8.962746 | 7.646388 | 7.771539 | 8.363429 | 8.820258 | 7.966455 | 8.029381 | 7.733818 | 8.304647 | 7.939369 | 7.448293 | 7.494908 | 7.469925 | 7.345197 | 7.462809 | 7.367848 | 7.307185 | 7.401391 | 7.423935 | 7.473438 |
hep-th/0509001 | Anastasios Psinas | Anastasios Psinas | Mirage Cosmology of U(1) Gauge Field on Unstable D3 Brane Universe | ReVTeX format 20 pages; v2 1 figure added, one additional paragraph
with extra comments added, enlarged list of references, version to appear in
JHEP | JHEP 0601 (2006) 138 | 10.1088/1126-6708/2006/01/138 | null | hep-th | null | An unstable $D3$-brane universe governed by the DBI action of the tachyon
field minimally coupled to a U(1) gauge boson is examined. The cosmological
evolution of this coupled system, is further analyzed, in terms of the
expansion rate of the inflating brane, which is highly affected by the presence
of the tachyonic ... | [
{
"created": "Wed, 31 Aug 2005 22:18:15 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jan 2006 02:18:23 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Psinas",
"Anastasios",
""
]
] | An unstable $D3$-brane universe governed by the DBI action of the tachyon field minimally coupled to a U(1) gauge boson is examined. The cosmological evolution of this coupled system, is further analyzed, in terms of the expansion rate of the inflating brane, which is highly affected by the presence of the tachyonic an... | 11.546398 | 11.038426 | 11.340739 | 10.803833 | 11.18454 | 10.518503 | 10.710246 | 10.483864 | 10.583062 | 10.644214 | 10.699998 | 10.822679 | 10.931073 | 10.872425 | 10.748676 | 10.644267 | 10.673273 | 10.868356 | 10.877344 | 10.832762 | 10.637486 |
1009.2488 | Burkhard Eden | Burkhard Eden, Gregory P. Korchemsky, and Emery Sokatchev | More on the duality correlators/amplitudes | 14 pages Latex, 1 figure | null | 10.1016/j.physletb.2012.02.014 | DCPT-10/43, IPhT--T10/139, LAPTH--039/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue the study of n-point correlation functions of half-BPS protected
operators in N=4 super-Yang-Mills theory, in the limit where the positions of
the adjacent operators become light-like separated. We compute the l-loop
corrections by making l Lagrangian insertions. We argue that there exists a
simple relati... | [
{
"created": "Mon, 13 Sep 2010 19:40:14 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Feb 2012 11:31:21 GMT",
"version": "v2"
}
] | 2015-05-19 | [
[
"Eden",
"Burkhard",
""
],
[
"Korchemsky",
"Gregory P.",
""
],
[
"Sokatchev",
"Emery",
""
]
] | We continue the study of n-point correlation functions of half-BPS protected operators in N=4 super-Yang-Mills theory, in the limit where the positions of the adjacent operators become light-like separated. We compute the l-loop corrections by making l Lagrangian insertions. We argue that there exists a simple relation... | 7.770433 | 6.787645 | 8.522327 | 6.482614 | 6.331347 | 6.326045 | 6.540644 | 6.031598 | 6.041023 | 9.153799 | 6.482299 | 6.516064 | 8.018942 | 6.634886 | 6.542707 | 6.500874 | 6.565211 | 6.674755 | 6.674927 | 7.656065 | 6.597721 |
hep-th/0509164 | Gautam Mandal | Avinash Dhar, Gautam Mandal and Nemani V Suryanarayana | Exact operator bosonization of finite number of fermions in one space
dimension | 47 pages, 1 figure; (v2) typos corrected | JHEP0601:118,2006 | 10.1088/1126-6708/2006/01/118 | TIFR/TH/05-36 | hep-th cond-mat.stat-mech | null | We derive an exact operator bosonization of a finite number of fermions in
one space dimension. The fermions can be interacting or noninteracting and can
have an arbitrary hamiltonian, as long as there is a countable basis of states
in the Hilbert space. In the bosonized theory the finiteness of the number of
fermion... | [
{
"created": "Wed, 21 Sep 2005 12:47:10 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Dec 2005 06:22:18 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Dhar",
"Avinash",
""
],
[
"Mandal",
"Gautam",
""
],
[
"Suryanarayana",
"Nemani V",
""
]
] | We derive an exact operator bosonization of a finite number of fermions in one space dimension. The fermions can be interacting or noninteracting and can have an arbitrary hamiltonian, as long as there is a countable basis of states in the Hilbert space. In the bosonized theory the finiteness of the number of fermions ... | 7.077246 | 6.954413 | 7.622062 | 6.52028 | 7.0772 | 6.857672 | 6.657092 | 6.223935 | 6.847705 | 7.42533 | 6.734871 | 6.719155 | 7.024233 | 6.839567 | 6.768931 | 6.813913 | 6.664514 | 6.797167 | 6.686161 | 7.107409 | 6.743883 |
1504.06168 | C. P. Martin Professor | C.P. Martin and David G. Navarro | The hybrid Seiberg-Witten map, its $\theta$-exact expansion and the
antifield formalism | 27 pages, no figures; typos corrected | Phys. Rev. D 92, 065026 (2015) | 10.1103/PhysRevD.92.065026 | FTI/UCM 37-2015 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We deduce an evolution equation for an arbitrary hybrid Seiberg-Witten map
for compact gauge groups by using the antifield formalism. We show how this
evolution equation can be used to obtain the hybrid Seiberg-Witten map as an
expansion, which is $\theta$-exact, in the number of ordinary fields. We
compute explicitl... | [
{
"created": "Thu, 23 Apr 2015 13:12:33 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Sep 2015 12:57:21 GMT",
"version": "v2"
},
{
"created": "Fri, 18 Sep 2015 11:46:55 GMT",
"version": "v3"
}
] | 2015-09-30 | [
[
"Martin",
"C. P.",
""
],
[
"Navarro",
"David G.",
""
]
] | We deduce an evolution equation for an arbitrary hybrid Seiberg-Witten map for compact gauge groups by using the antifield formalism. We show how this evolution equation can be used to obtain the hybrid Seiberg-Witten map as an expansion, which is $\theta$-exact, in the number of ordinary fields. We compute explicitly ... | 9.886759 | 8.921879 | 9.393403 | 9.082999 | 8.380368 | 9.521157 | 8.417339 | 9.086014 | 8.623119 | 9.654573 | 8.905628 | 8.448943 | 8.886318 | 8.679373 | 8.932508 | 8.794463 | 8.540148 | 8.856358 | 8.73672 | 9.204059 | 8.599375 |
hep-th/0605016 | Wei Liao | Wei Liao | WZW action in odd dimensional gauge theories | 19 pages, text shortened, reference added. Version to appear in PRD | Phys.Rev.D74:065010,2006 | 10.1103/PhysRevD.74.065010 | null | hep-th hep-ph | null | It is shown that Wess-Zumino-Witten (WZW) type actions can be constructed in
odd dimensional space-times using Wilson line or Wilson loop. WZW action
constructed using Wilson line gives anomalous gauge variations and the WZW
action constructed using Wilson loop gives anomalous chiral transformation. We
show that pure... | [
{
"created": "Mon, 1 May 2006 19:42:36 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Aug 2006 18:28:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Liao",
"Wei",
""
]
] | It is shown that Wess-Zumino-Witten (WZW) type actions can be constructed in odd dimensional space-times using Wilson line or Wilson loop. WZW action constructed using Wilson line gives anomalous gauge variations and the WZW action constructed using Wilson loop gives anomalous chiral transformation. We show that pure g... | 9.925739 | 9.77294 | 10.435281 | 9.646951 | 9.884034 | 10.172433 | 9.874586 | 9.985765 | 9.351634 | 11.051406 | 9.589134 | 9.715716 | 9.730042 | 9.267911 | 9.702039 | 9.75899 | 9.424596 | 9.346772 | 9.284815 | 9.508512 | 9.468934 |
1608.03709 | Diederik Roest | Sergio Ferrara, Diederik Roest | General sGoldstino Inflation | 6 pages, 6 figures; v2: refs added, published version | null | 10.1088/1475-7516/2016/10/038 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove that all inflationary models, including those with dark energy after
the end of inflation, can be embedded in minimal supergravity with a single
chiral superfield. Moreover, the amount of supersymmetry breaking is
independently tunable due to a degeneracy in the choice for the superpotential.
The inflaton is... | [
{
"created": "Fri, 12 Aug 2016 08:20:38 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Oct 2016 09:38:32 GMT",
"version": "v2"
}
] | 2016-11-09 | [
[
"Ferrara",
"Sergio",
""
],
[
"Roest",
"Diederik",
""
]
] | We prove that all inflationary models, including those with dark energy after the end of inflation, can be embedded in minimal supergravity with a single chiral superfield. Moreover, the amount of supersymmetry breaking is independently tunable due to a degeneracy in the choice for the superpotential. The inflaton is a... | 8.716768 | 7.506749 | 8.768506 | 7.64813 | 8.574697 | 7.340308 | 7.703266 | 7.58477 | 7.694875 | 9.613541 | 7.197402 | 7.588509 | 8.65819 | 7.942493 | 7.70012 | 7.865103 | 8.030163 | 7.622925 | 7.972036 | 8.637937 | 7.500011 |
0706.0514 | Johannes Walcher | Katrin Becker, Melanie Becker, Johannes Walcher | Runaway in the Landscape | 26 pages | Phys.Rev.D76:106002,2007 | 10.1103/PhysRevD.76.106002 | null | hep-th | null | We consider flux compactifications of type IIB string theory on the mirror of
a rigid Calabi-Yau. In special cases, these models are dual to the type IIA
flux vacua with runaway direction in flux space. We show that new weak coupling
AdS solutions can be found for large complex structure, while Minkowski
solutions wi... | [
{
"created": "Tue, 5 Jun 2007 15:01:02 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Becker",
"Katrin",
""
],
[
"Becker",
"Melanie",
""
],
[
"Walcher",
"Johannes",
""
]
] | We consider flux compactifications of type IIB string theory on the mirror of a rigid Calabi-Yau. In special cases, these models are dual to the type IIA flux vacua with runaway direction in flux space. We show that new weak coupling AdS solutions can be found for large complex structure, while Minkowski solutions with... | 9.394391 | 9.430143 | 9.97985 | 8.917132 | 9.691713 | 10.07402 | 9.38534 | 9.39629 | 8.530351 | 11.140576 | 8.769164 | 9.007152 | 9.547676 | 9.081055 | 8.924378 | 9.219167 | 9.301845 | 9.542313 | 9.052186 | 9.65449 | 9.028307 |
2004.00965 | Kellogg S. Stelle | K.S. Stelle | Mass Gaps and Braneworlds -- In Memory of Peter Freund | 23 pages, latex; submitted to the Peter Freund Memorial Volume to be
published in J. Phys. A: Math. Theor | null | 10.1088/1751-8121/ab83ca | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Remembering the foundational contributions of Peter Freund to supergravity,
and especially to the problems of dimensional compactification, reduction is
considered with a non-compact space transverse to the lower dimensional theory.
The known problem of a continuum of Kaluza-Klein states is avoided here by the
occurr... | [
{
"created": "Thu, 2 Apr 2020 12:53:55 GMT",
"version": "v1"
}
] | 2020-04-03 | [
[
"Stelle",
"K. S.",
""
]
] | Remembering the foundational contributions of Peter Freund to supergravity, and especially to the problems of dimensional compactification, reduction is considered with a non-compact space transverse to the lower dimensional theory. The known problem of a continuum of Kaluza-Klein states is avoided here by the occurren... | 16.095852 | 13.756822 | 14.076388 | 13.451814 | 15.400491 | 13.392855 | 15.239889 | 12.66798 | 13.623729 | 15.302853 | 14.790636 | 13.557024 | 13.303618 | 12.370739 | 13.011861 | 13.191812 | 13.167685 | 13.606593 | 13.441183 | 13.742516 | 13.888066 |
hep-th/0206064 | Amer Iqbal | Amer Iqbal | A note on E-strings | 20 pages, References added | Adv.Theor.Math.Phys. 7 (2003) 1-23 | null | UTTG-05-02 | hep-th | null | We study BPS states in type IIA string compactification on a local Calabi-Yau
3-fold which are related to the BPS states of the E-string. Using
Picard-Lefshetz transformations of the 3-cycles on the mirror manifold we
determine automorphisms of the K-theory of the compact divisor of the
Calabi-Yau which maps certain ... | [
{
"created": "Mon, 10 Jun 2002 19:29:23 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jun 2002 02:04:57 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Dec 2003 21:49:45 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Iqbal",
"Amer",
""
]
] | We study BPS states in type IIA string compactification on a local Calabi-Yau 3-fold which are related to the BPS states of the E-string. Using Picard-Lefshetz transformations of the 3-cycles on the mirror manifold we determine automorphisms of the K-theory of the compact divisor of the Calabi-Yau which maps certain D-... | 7.122768 | 6.491532 | 9.708429 | 7.036094 | 8.056618 | 6.728568 | 6.646454 | 7.260354 | 7.023818 | 10.268048 | 7.204351 | 6.754874 | 8.612776 | 6.945949 | 7.214326 | 7.14466 | 7.008377 | 7.009016 | 7.128375 | 8.347829 | 6.785595 |
1809.04260 | Gabi Zafrir | Gabi Zafrir | On the torus compactifications of $Z_2$ orbifolds of E-string theories | 34 pages, 8 figures | null | 10.1007/JHEP10(2019)040 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the torus compactifications with flux of a class of $6d$ $(1,0)$
SCFTs that can be engineered as the low-energy theories on M$5$-branes near an
M$9$-plane on a $C^2/Z_2$ singularity. Specifically, we concentrate on the two
SCFTs where the $Z_2$ orbifold action acts non-trivially on the $E_8$ global
symmet... | [
{
"created": "Wed, 12 Sep 2018 05:20:45 GMT",
"version": "v1"
}
] | 2019-10-23 | [
[
"Zafrir",
"Gabi",
""
]
] | We consider the torus compactifications with flux of a class of $6d$ $(1,0)$ SCFTs that can be engineered as the low-energy theories on M$5$-branes near an M$9$-plane on a $C^2/Z_2$ singularity. Specifically, we concentrate on the two SCFTs where the $Z_2$ orbifold action acts non-trivially on the $E_8$ global symmetry... | 8.056922 | 6.420497 | 8.413773 | 6.670256 | 6.684718 | 6.99995 | 7.530858 | 6.625687 | 6.679606 | 9.486791 | 6.927014 | 7.496378 | 7.978358 | 7.253975 | 7.418118 | 7.286798 | 7.546195 | 7.214548 | 7.240077 | 7.715976 | 7.126116 |
1310.4505 | Heeyeon Kim | Heeyeon Kim, Sungjay Lee and Piljin Yi | Exact Partition Functions on RP2 and Orientifolds | 55 pages, 1 figure, published version: discussions on role of theta
angle and on r-charge dependent normalization calrified; typos corrected; one
reference added | null | 10.1007/JHEP02(2014)103 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider gauged linear sigma models (GLSM) on $\mathbb{RP}^2$, obtained
from a parity projection of $S^2$. The theories admit squashing deformation,
much like GLSM on $S^2$, which allows us to interpret the partition function as
the overlap amplitude between the vacuum state and crosscap states. From these,
we ext... | [
{
"created": "Wed, 16 Oct 2013 20:00:12 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Feb 2014 02:57:28 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Kim",
"Heeyeon",
""
],
[
"Lee",
"Sungjay",
""
],
[
"Yi",
"Piljin",
""
]
] | We consider gauged linear sigma models (GLSM) on $\mathbb{RP}^2$, obtained from a parity projection of $S^2$. The theories admit squashing deformation, much like GLSM on $S^2$, which allows us to interpret the partition function as the overlap amplitude between the vacuum state and crosscap states. From these, we extra... | 14.696726 | 12.771995 | 13.951114 | 12.712074 | 12.748894 | 13.410134 | 12.143693 | 11.92966 | 12.140836 | 16.125381 | 11.602138 | 12.623504 | 13.132236 | 12.197814 | 12.541823 | 12.62937 | 12.325319 | 12.277966 | 12.469131 | 13.166245 | 11.945276 |
1107.0368 | Karl Landsteiner | Karl Landsteiner, Eugenio Megias, Luis Melgar, Francisco Pena-Benitez | Holographic Gravitational Anomaly and Chiral Vortical Effect | 27 pages, no figures | null | 10.1007/JHEP09(2011)121 | IFT-UAM/CSIC-11-45 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze a holographic model with a pure gauge and a mixed
gauge-gravitational Chern-Simons term in the action. These are the holographic
implementations of the usual chiral and the mixed gauge-gravitational anomalies
in four dimensional field theories with chiral fermions. We discuss the
holographic renormalizatio... | [
{
"created": "Sat, 2 Jul 2011 10:36:37 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Landsteiner",
"Karl",
""
],
[
"Megias",
"Eugenio",
""
],
[
"Melgar",
"Luis",
""
],
[
"Pena-Benitez",
"Francisco",
""
]
] | We analyze a holographic model with a pure gauge and a mixed gauge-gravitational Chern-Simons term in the action. These are the holographic implementations of the usual chiral and the mixed gauge-gravitational anomalies in four dimensional field theories with chiral fermions. We discuss the holographic renormalization ... | 7.009713 | 6.944959 | 7.356821 | 6.632006 | 7.038692 | 7.128003 | 7.042684 | 6.501241 | 6.792062 | 7.925713 | 6.70088 | 6.855814 | 6.942415 | 6.750721 | 7.057277 | 6.619881 | 6.834757 | 6.901417 | 6.788572 | 6.969216 | 6.682488 |
2002.04604 | Giulia Fardelli | A. Bissi, G. Fardelli and A. Georgoudis | Towards All Loop Supergravity Amplitudes on $AdS_5 \times S^5$ | 7 pages. V2: reformatted for Phys. Rev. D, accepted version | Phys. Rev. D 104, 041901 (2021) | 10.1103/PhysRevD.104.L041901 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the four point function of the superconformal primary of the
stress-tensor multiplet in four dimensional $\mathcal{N}=4$ Super Yang Mills,
at large 't Hooft coupling and in a large $N$ expansion. This observable is
holographically dual to four graviton amplitudes in type IIB supergravity on
$AdS_5 \times S^5... | [
{
"created": "Tue, 11 Feb 2020 18:55:30 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Sep 2021 07:13:30 GMT",
"version": "v2"
}
] | 2021-09-03 | [
[
"Bissi",
"A.",
""
],
[
"Fardelli",
"G.",
""
],
[
"Georgoudis",
"A.",
""
]
] | We study the four point function of the superconformal primary of the stress-tensor multiplet in four dimensional $\mathcal{N}=4$ Super Yang Mills, at large 't Hooft coupling and in a large $N$ expansion. This observable is holographically dual to four graviton amplitudes in type IIB supergravity on $AdS_5 \times S^5$.... | 5.211329 | 5.27914 | 5.901152 | 4.991585 | 5.416895 | 5.343354 | 4.765991 | 5.024498 | 5.167506 | 6.151198 | 5.15822 | 5.112412 | 5.508279 | 5.112824 | 5.045133 | 5.008306 | 4.8522 | 4.883031 | 4.929521 | 5.396601 | 4.934248 |
1905.02632 | Koji Hashimoto | Koji Hashimoto, Wataru Sasaki, Takayuki Sumimoto | $1/N$ correction in holographic Wilson loop from quantum gravity | 15 pages, 9 figures | null | 10.1007/JHEP12(2019)138 | OU-HET-1018 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $1/N$ corrections to a Wilson loop in holographic duality. Extending
the AdS/CFT correspondence beyond the large $N$ limit is an important but a
subtle issue, as it needs quantum gravity corrections in the gravity side. To
find a physical property of the quantum corrected geometry of near-horizon
black 0-bra... | [
{
"created": "Tue, 7 May 2019 15:04:29 GMT",
"version": "v1"
}
] | 2020-01-29 | [
[
"Hashimoto",
"Koji",
""
],
[
"Sasaki",
"Wataru",
""
],
[
"Sumimoto",
"Takayuki",
""
]
] | We study $1/N$ corrections to a Wilson loop in holographic duality. Extending the AdS/CFT correspondence beyond the large $N$ limit is an important but a subtle issue, as it needs quantum gravity corrections in the gravity side. To find a physical property of the quantum corrected geometry of near-horizon black 0-brane... | 10.746588 | 11.402457 | 13.411631 | 10.464947 | 10.850354 | 11.467405 | 11.234187 | 11.024928 | 10.476064 | 12.119293 | 10.447125 | 10.411498 | 11.287548 | 10.57896 | 10.62184 | 10.540554 | 10.173485 | 10.281149 | 10.562444 | 11.725551 | 10.365551 |
1308.5264 | Urs Schreiber | Domenico Fiorenza, Hisham Sati, Urs Schreiber | Super Lie n-algebra extensions, higher WZW models, and super p-branes
with tensor multiplet fields | 28 pages, published version plus one typo fixed | International Journal of Geometric Methods in Modern Physics
Volume 12, Issue 02 (2015) 1550018 | null | null | hep-th math.AT math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formalize higher dimensional and higher gauge WZW-type sigma-model local
prequantum field theory, and discuss its rationalized/perturbative description
in (super-)Lie n-algebra homotopy theory (the true home of the "FDA"-language
used in the supergravity literature). We show generally how the intersection
laws for... | [
{
"created": "Fri, 23 Aug 2013 23:33:52 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Sep 2013 20:39:27 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Mar 2015 13:12:47 GMT",
"version": "v3"
}
] | 2015-03-18 | [
[
"Fiorenza",
"Domenico",
""
],
[
"Sati",
"Hisham",
""
],
[
"Schreiber",
"Urs",
""
]
] | We formalize higher dimensional and higher gauge WZW-type sigma-model local prequantum field theory, and discuss its rationalized/perturbative description in (super-)Lie n-algebra homotopy theory (the true home of the "FDA"-language used in the supergravity literature). We show generally how the intersection laws for s... | 7.69139 | 11.682414 | 11.973491 | 10.170299 | 11.323627 | 12.381119 | 12.053433 | 11.148101 | 10.269108 | 13.68762 | 9.868705 | 8.840125 | 9.018188 | 8.186619 | 8.46917 | 8.725949 | 8.521576 | 8.743232 | 8.471362 | 9.624384 | 8.163176 |
hep-th/9905225 | Hiroshi Suzuki | Hiroshi Suzuki (Ibaraki University) | Invariant Regularization of Supersymmetric Chiral Gauge Theory | uses PTPTeX, 16 pages, based on the invited talk in the workshop on
``Gauge Theory and Integrable Models,'' January 1999, Kyoto | Prog.Theor.Phys.Suppl.135:194-210,1999 | 10.1143/PTPS.135.194 | IU-MSTP/34 | hep-th | null | We present a regularization scheme which respects the supersymmetry and the
maximal background gauge covariance in supersymmetric chiral gauge theories.
When the anomaly cancellation condition is satisfied, the effective action in
the superfield background field method automatically restores the gauge
invariance with... | [
{
"created": "Mon, 31 May 1999 06:35:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Suzuki",
"Hiroshi",
"",
"Ibaraki University"
]
] | We present a regularization scheme which respects the supersymmetry and the maximal background gauge covariance in supersymmetric chiral gauge theories. When the anomaly cancellation condition is satisfied, the effective action in the superfield background field method automatically restores the gauge invariance withou... | 13.600849 | 13.722433 | 14.34766 | 12.434519 | 12.148124 | 13.61095 | 11.917456 | 13.113542 | 11.86518 | 14.720792 | 12.600194 | 12.796661 | 12.823325 | 12.557717 | 12.635795 | 12.98596 | 12.630285 | 13.079896 | 12.557446 | 12.844144 | 12.065501 |
hep-th/0310058 | Keshav Dasgupta | Katrin Becker, Melanie Becker, Keshav Dasgupta, Paul S. Green, Eric
Sharpe | Compactifications of Heterotic Strings on Non-Kahler Complex Manifolds:
II | 106 pages, 8 .eps figures, Harvmac; v2: Some sections expanded, typos
corrected and references updated; v3: More typos corrected, one section
expanded and references added. Final version to appear in Nucl. Phys. B | Nucl.Phys.B678:19-100,2004 | 10.1016/j.nuclphysb.2003.11.029 | UMD-PP-03-69, SU-ITP-03/24, ILL-(TH)-03-07 | hep-th | null | We continue our study of heterotic compactifications on non-Kahler complex
manifolds with torsion. We give further evidence of the consistency of the
six-dimensional manifold presented earlier and discuss the anomaly cancellation
and possible supergravity description for a generic non-Kahler complex manifold
using th... | [
{
"created": "Mon, 6 Oct 2003 22:28:38 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Oct 2003 05:58:07 GMT",
"version": "v2"
},
{
"created": "Sat, 15 Nov 2003 00:21:14 GMT",
"version": "v3"
}
] | 2010-04-06 | [
[
"Becker",
"Katrin",
""
],
[
"Becker",
"Melanie",
""
],
[
"Dasgupta",
"Keshav",
""
],
[
"Green",
"Paul S.",
""
],
[
"Sharpe",
"Eric",
""
]
] | We continue our study of heterotic compactifications on non-Kahler complex manifolds with torsion. We give further evidence of the consistency of the six-dimensional manifold presented earlier and discuss the anomaly cancellation and possible supergravity description for a generic non-Kahler complex manifold using the ... | 8.155081 | 7.749797 | 8.607617 | 7.863755 | 7.902621 | 7.675436 | 8.674631 | 7.553147 | 7.775972 | 8.780032 | 7.523069 | 7.877542 | 8.265363 | 7.977344 | 7.92757 | 7.877808 | 8.173361 | 8.112369 | 7.937802 | 8.170592 | 7.943145 |
hep-th/0007072 | Andrei Zotov | A.Zotov | On Relation Between Moyal and Kontsevich Quantum Products. Direct
Evaluation up to the $\hbar^3$-Order | LaTeX, 8 pages | Mod.Phys.Lett. A16 (2001) 615-626 | 10.1142/S0217732301003693 | null | hep-th | null | In his celebrated paper Kontsevich has proved a theorem which manifestly
gives a quantum product (deformation quantization formula) and states that
changing coordinates leads to gauge equivalent star products. To illuminate his
procedure, we make an arbitrary change of coordinates in the Moyal product and
obtain the ... | [
{
"created": "Sun, 9 Jul 2000 17:51:39 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Zotov",
"A.",
""
]
] | In his celebrated paper Kontsevich has proved a theorem which manifestly gives a quantum product (deformation quantization formula) and states that changing coordinates leads to gauge equivalent star products. To illuminate his procedure, we make an arbitrary change of coordinates in the Moyal product and obtain the de... | 14.515677 | 13.773602 | 15.615649 | 13.687307 | 15.504331 | 14.378335 | 14.479737 | 13.240298 | 13.200936 | 16.422821 | 13.700312 | 13.034918 | 14.246827 | 13.521455 | 13.41189 | 12.63141 | 13.092963 | 13.13476 | 13.303181 | 13.740707 | 13.068416 |
hep-th/0205090 | Barak Kol | Ofer Aharony, Barak Kol and Shimon Yankielowicz | On Exactly Marginal Deformations of N=4 SYM and Type IIB Supergravity on
AdS_5 * S^5 | 45 pages, 1 figure, v2 - JHEP published version | JHEP 0206:039,2002 | 10.1088/1126-6708/2002/06/039 | null | hep-th | null | N=4 supersymmetric Yang-Mills theory with gauge group SU(n) (n>=3) is
believed to have two exactly marginal deformations which break the
supersymmetry to N=1. We discuss the construction of the string theory dual to
these deformations, in the supergravity approximation, in a perturbation series
around the AdS_5 * S^5... | [
{
"created": "Thu, 9 May 2002 21:12:49 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Jun 2002 14:41:49 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Aharony",
"Ofer",
""
],
[
"Kol",
"Barak",
""
],
[
"Yankielowicz",
"Shimon",
""
]
] | N=4 supersymmetric Yang-Mills theory with gauge group SU(n) (n>=3) is believed to have two exactly marginal deformations which break the supersymmetry to N=1. We discuss the construction of the string theory dual to these deformations, in the supergravity approximation, in a perturbation series around the AdS_5 * S^5 s... | 6.777972 | 6.275921 | 6.980216 | 6.362625 | 6.489674 | 6.363043 | 6.326455 | 6.083856 | 6.277653 | 7.757762 | 6.122251 | 6.302369 | 6.672676 | 6.264044 | 6.298113 | 6.371046 | 6.121683 | 6.292377 | 6.346894 | 6.393871 | 6.299688 |
hep-th/9508138 | null | N.A. Saulina, E.M. Terentjev and M.V. Terentiev | GRAMA. A Mathematica program for analytical calculations in
10-dimensional supergravity. Version 1.0 | GRAMA user-manual and basic algorithms (LaTeX, 14 pages); Mathematica
script for the GRAMA package: files progr-a.ma, progr-b.ma, progr-c.ma,
progr-id.ma - 125 Kb total | null | null | Preprint ITEP 26-95 | hep-th | null | "GRAMA" is a Mathematica package for doing symbolic tensor computations and
complicated algebraic manipulations in 10-dimensional (D=10) simple (N=1)
supergravity. The main new ingredients of this package inside the general
Mathematica environment are the computation of complicated products of Dirac
matrices and the ... | [
{
"created": "Fri, 25 Aug 1995 17:22:16 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Aug 1995 23:45:43 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Saulina",
"N. A.",
""
],
[
"Terentjev",
"E. M.",
""
],
[
"Terentiev",
"M. V.",
""
]
] | "GRAMA" is a Mathematica package for doing symbolic tensor computations and complicated algebraic manipulations in 10-dimensional (D=10) simple (N=1) supergravity. The main new ingredients of this package inside the general Mathematica environment are the computation of complicated products of Dirac matrices and the tr... | 10.54844 | 11.433338 | 10.835648 | 10.81201 | 10.930219 | 11.757083 | 10.957711 | 11.03809 | 11.994472 | 12.019471 | 10.582903 | 10.416347 | 10.018426 | 10.272825 | 10.784265 | 10.483141 | 10.290645 | 10.775202 | 10.435335 | 10.300591 | 10.555427 |
1210.1742 | Jan Heffner | Hugo Reinhardt, Jan Heffner | The effective potential of the confinement order parameter in the
Hamilton approach | 5 pages, 3 eps figures; revised version; accepted for publication in
Physics Letters B | null | 10.1016/j.physletb.2012.10.084 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The effective potential of the order parameter for confinement is calculated
within the Hamiltonian approach by compactifying one spatial dimension and
using a background gauge fixing. Neglecting the ghost and using the
perturbative gluon energy one recovers the Weiss potential. From the full
non-perturbative potenti... | [
{
"created": "Fri, 5 Oct 2012 12:57:14 GMT",
"version": "v1"
},
{
"created": "Wed, 31 Oct 2012 16:25:48 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Reinhardt",
"Hugo",
""
],
[
"Heffner",
"Jan",
""
]
] | The effective potential of the order parameter for confinement is calculated within the Hamiltonian approach by compactifying one spatial dimension and using a background gauge fixing. Neglecting the ghost and using the perturbative gluon energy one recovers the Weiss potential. From the full non-perturbative potential... | 11.654094 | 8.087415 | 10.530624 | 7.749192 | 10.831227 | 7.588522 | 7.948993 | 7.627968 | 8.849997 | 10.036741 | 7.772449 | 9.804399 | 10.4947 | 9.89433 | 10.406043 | 10.01459 | 10.172013 | 9.605531 | 9.526233 | 10.186952 | 10.388334 |
hep-th/0404093 | Stuart Dowker | J.S.Dowker | Spherical Universe topology and the Casimir effect | 33 pages, 1 figure. Typos corrected and one reference added | Class.Quant.Grav. 21 (2004) 4247-4272 | 10.1088/0264-9381/21/17/012 | null | hep-th astro-ph gr-qc | null | The mode problem on the factored 3--sphere is applied to field theory
calculations for massless fields of spin 0, 1/2 and 1. The degeneracies on the
factors, including lens spaces, are neatly derived in a geometric fashion.
Vacuum energies are expressed in terms of the polyhedral degrees and equivalent
expressions gi... | [
{
"created": "Tue, 13 Apr 2004 20:38:43 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Apr 2004 22:22:12 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dowker",
"J. S.",
""
]
] | The mode problem on the factored 3--sphere is applied to field theory calculations for massless fields of spin 0, 1/2 and 1. The degeneracies on the factors, including lens spaces, are neatly derived in a geometric fashion. Vacuum energies are expressed in terms of the polyhedral degrees and equivalent expressions give... | 31.344439 | 28.208954 | 33.26543 | 25.602228 | 28.562889 | 29.47312 | 26.010378 | 26.602657 | 28.844446 | 38.835884 | 31.028873 | 27.532207 | 30.524197 | 29.070219 | 28.386694 | 28.247543 | 28.246378 | 27.904377 | 29.284531 | 28.361326 | 27.876932 |
hep-th/0209114 | Harvey S. Reall | Jerome P. Gauntlett, Jan B. Gutowski, Christopher M. Hull, Stathis
Pakis and Harvey S. Reall | All supersymmetric solutions of minimal supergravity in five dimensions | 63 pages; substantial additions to the analysis of maximally
supersymmetric solutions. Typos corrected and references added | Class.Quant.Grav. 20 (2003) 4587-4634 | 10.1088/0264-9381/20/21/005 | QMUL-PH-02-13 | hep-th | null | All purely bosonic supersymmetric solutions of minimal supergravity in five
dimensions are classified. The solutions preserve either one half or all of the
supersymmetry. Explicit examples of new solutions are given, including a large
family of plane-fronted waves and a maximally supersymmetric analogue of the
G\"ode... | [
{
"created": "Fri, 13 Sep 2002 16:44:04 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2003 18:26:10 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Sep 2003 18:15:10 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Gauntlett",
"Jerome P.",
""
],
[
"Gutowski",
"Jan B.",
""
],
[
"Hull",
"Christopher M.",
""
],
[
"Pakis",
"Stathis",
""
],
[
"Reall",
"Harvey S.",
""
]
] | All purely bosonic supersymmetric solutions of minimal supergravity in five dimensions are classified. The solutions preserve either one half or all of the supersymmetry. Explicit examples of new solutions are given, including a large family of plane-fronted waves and a maximally supersymmetric analogue of the G\"odel ... | 7.149254 | 5.948278 | 7.354241 | 5.92467 | 6.316705 | 6.960217 | 6.40777 | 5.837787 | 6.362287 | 7.653048 | 5.93286 | 5.81344 | 7.582169 | 5.872222 | 5.725758 | 5.937751 | 6.0156 | 6.164812 | 6.0149 | 6.630616 | 5.987648 |
1506.04548 | Dibakar Roychowdhury | Dibakar Roychowdhury | Quantum fluctuations and thermal dissipation in higher derivative
gravity | Latex, 21 pages, Version to appear in Nuclear Physics B | Nucl.Phys. B897 (2015) 678-696 | 10.1016/j.nuclphysb.2015.06.013 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, based on the $ AdS_{2}/CFT_{1} $ prescription, we explore the
low frequency behavior of quantum two point functions for a special class of
strongly coupled CFTs in one dimension whose dual gravitational counterpart
consists of \textit{extremal} black hole solutions in higher derivative
theories of grav... | [
{
"created": "Mon, 15 Jun 2015 11:01:00 GMT",
"version": "v1"
}
] | 2015-07-01 | [
[
"Roychowdhury",
"Dibakar",
""
]
] | In this paper, based on the $ AdS_{2}/CFT_{1} $ prescription, we explore the low frequency behavior of quantum two point functions for a special class of strongly coupled CFTs in one dimension whose dual gravitational counterpart consists of \textit{extremal} black hole solutions in higher derivative theories of gravit... | 10.528325 | 9.618589 | 10.57973 | 9.765477 | 9.717728 | 9.746743 | 9.740746 | 9.217134 | 9.943915 | 12.145949 | 9.962 | 10.235284 | 10.782729 | 10.135927 | 10.197084 | 9.95876 | 10.13415 | 9.878045 | 10.165591 | 11.006447 | 9.788265 |
hep-th/9604063 | Abdalla Elcio | E. Abdalla, R. Mohayaee and A. Zadra | Screening in Two-dimensional QCD | 22 pages, latex file | Int.J.Mod.Phys. A12 (1997) 4539-4558 | 10.1142/S0217751X97002450 | IC/96/51 | hep-th | null | We discuss the issue of screening and confinement of external colour charges
in bosonised two-dimensional quantum chromodynamics. Our computation relies on
the static solutions of the semi-classical equations of motion. The
significance of the different representations of the matter field is explicitly
studied. We ar... | [
{
"created": "Thu, 11 Apr 1996 14:37:00 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Abdalla",
"E.",
""
],
[
"Mohayaee",
"R.",
""
],
[
"Zadra",
"A.",
""
]
] | We discuss the issue of screening and confinement of external colour charges in bosonised two-dimensional quantum chromodynamics. Our computation relies on the static solutions of the semi-classical equations of motion. The significance of the different representations of the matter field is explicitly studied. We arri... | 14.315425 | 11.118102 | 12.858449 | 11.253182 | 11.542954 | 10.425719 | 11.384732 | 11.897118 | 11.337561 | 13.671616 | 11.360161 | 11.443799 | 12.66342 | 12.323683 | 11.698828 | 11.755071 | 12.067173 | 12.708225 | 12.002327 | 12.247376 | 11.683052 |
2107.08753 | Ryo Yokokura | Yoshimasa Hidaka, Muneto Nitta, Ryo Yokokura | Topological axion electrodynamics and 4-group symmetry | 8 pages, 2 figures; v2: minor revision, published version with more
references | Phys. Lett. B 823 (2021) 136762 | 10.1016/j.physletb.2021.136762 | KEK-TH-2331, J-PARC-TH-0243 | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study higher-form symmetries and a higher group in the low energy limit of
a $(3+1)$-dimensional axion electrodynamics with a massive axion and a massive
photon. A topological field theory describing topological excitations with the
axion-photon coupling, which we call a topological axion electrodynamics, is
obtai... | [
{
"created": "Mon, 19 Jul 2021 11:02:40 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Mar 2022 06:25:18 GMT",
"version": "v2"
}
] | 2022-03-04 | [
[
"Hidaka",
"Yoshimasa",
""
],
[
"Nitta",
"Muneto",
""
],
[
"Yokokura",
"Ryo",
""
]
] | We study higher-form symmetries and a higher group in the low energy limit of a $(3+1)$-dimensional axion electrodynamics with a massive axion and a massive photon. A topological field theory describing topological excitations with the axion-photon coupling, which we call a topological axion electrodynamics, is obtaine... | 9.147758 | 8.433999 | 9.631743 | 8.070128 | 8.473172 | 8.526277 | 8.807135 | 7.969866 | 8.20668 | 9.582827 | 7.965829 | 8.696495 | 9.135091 | 8.566848 | 8.337625 | 8.201129 | 8.655715 | 8.28406 | 8.406071 | 9.243397 | 8.309258 |
1004.3450 | Johannes Tambornino | Aristide Baratin, Bianca Dittrich, Daniele Oriti, Johannes Tambornino | Non-commutative flux representation for loop quantum gravity | 12 pages, matches published version | Class.Quant.Grav.28:175011,2011 | 10.1088/0264-9381/28/17/175011 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Hilbert space of loop quantum gravity is usually described in terms of
cylindrical functionals of the gauge connection, the electric fluxes acting as
non-commuting derivation operators. It has long been believed that this
non-commutativity prevents a dual flux (or triad) representation of loop
quantum gravity to ... | [
{
"created": "Tue, 20 Apr 2010 13:48:46 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Feb 2012 12:46:58 GMT",
"version": "v2"
}
] | 2015-05-18 | [
[
"Baratin",
"Aristide",
""
],
[
"Dittrich",
"Bianca",
""
],
[
"Oriti",
"Daniele",
""
],
[
"Tambornino",
"Johannes",
""
]
] | The Hilbert space of loop quantum gravity is usually described in terms of cylindrical functionals of the gauge connection, the electric fluxes acting as non-commuting derivation operators. It has long been believed that this non-commutativity prevents a dual flux (or triad) representation of loop quantum gravity to ex... | 6.112995 | 8.349739 | 7.641349 | 7.340106 | 7.360601 | 7.476657 | 8.794168 | 7.842848 | 7.982836 | 8.320116 | 7.199759 | 7.34147 | 6.886405 | 6.745268 | 7.068618 | 7.284475 | 6.956857 | 7.24834 | 7.012674 | 6.722577 | 6.722568 |
1210.6215 | Kirill Krasnov | Gianluca Delfino, Kirill Krasnov and Carlos Scarinci | Pure connection formalism for gravity: Feynman rules and the
graviton-graviton scattering | v2: 57 pages, figures, a missing contribution to the all plus
amplitude added, discussion improved | J. High Energ. Phys. (2015) 2015: 119 | 10.1007/JHEP03(2015)119 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue to develop the pure connection formalism for gravity. We derive
the Feynman rules for computing the connection correlation functions, as well
as the prescription for obtaining the Minkowski space graviton scattering
amplitudes from the latter. The present formalism turns out to be simpler than
the metric ... | [
{
"created": "Tue, 23 Oct 2012 12:08:55 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Oct 2014 14:13:21 GMT",
"version": "v2"
}
] | 2018-09-05 | [
[
"Delfino",
"Gianluca",
""
],
[
"Krasnov",
"Kirill",
""
],
[
"Scarinci",
"Carlos",
""
]
] | We continue to develop the pure connection formalism for gravity. We derive the Feynman rules for computing the connection correlation functions, as well as the prescription for obtaining the Minkowski space graviton scattering amplitudes from the latter. The present formalism turns out to be simpler than the metric ba... | 8.524336 | 9.748851 | 8.779237 | 8.674704 | 9.724103 | 9.340582 | 9.146639 | 8.784042 | 9.005613 | 9.74455 | 8.661024 | 8.714656 | 8.442965 | 8.557485 | 8.67002 | 8.63437 | 8.752016 | 8.401313 | 8.661977 | 8.446391 | 8.456012 |
hep-th/0603066 | Atish Dabholkar | Atish Dabholkar and Suresh Nampuri | Spectrum of Dyons and Black Holes in CHL orbifolds using Borcherds Lift | 23 pages, 1 figure | JHEP0711:077,2007 | 10.1088/1126-6708/2007/11/077 | TIFR-TH-06-07 | hep-th | null | The degeneracies of supersymmetric quarter BPS dyons in four dimensions and
of spinning black holes in five dimensions in a CHL compactification are
computed exactly using Borcherds lift. The Hodge anomaly in the construction
has a physical interpretation as the contribution of a single M-theory
Kaluza-Klein 6-brane ... | [
{
"created": "Wed, 8 Mar 2006 19:41:18 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Oct 2007 21:02:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Dabholkar",
"Atish",
""
],
[
"Nampuri",
"Suresh",
""
]
] | The degeneracies of supersymmetric quarter BPS dyons in four dimensions and of spinning black holes in five dimensions in a CHL compactification are computed exactly using Borcherds lift. The Hodge anomaly in the construction has a physical interpretation as the contribution of a single M-theory Kaluza-Klein 6-brane in... | 13.523538 | 11.14225 | 17.748533 | 10.577024 | 12.203483 | 11.582958 | 11.51485 | 11.8038 | 11.62125 | 18.334324 | 11.856351 | 12.31535 | 16.034277 | 13.135069 | 12.215313 | 12.636054 | 12.556847 | 12.400346 | 13.063652 | 14.807067 | 12.362795 |
hep-th/9305002 | Lev Vaidman | Avshalom C. Elitzur and Lev Vaidman | Quantum Mechanical Interaction-Free Measurements | (revised file with no need for macro), 12, TAUP 1865-91# | null | 10.1007/BF00736012 | null | hep-th | null | A novel manifestation of nonlocality of quantum mechanics is presented. It is
shown that it is possible to ascertain the existence of an object in a given
region of space without interacting with it. The method might have practical
applications for delicate quantum experiments.
| [
{
"created": "Mon, 3 May 1993 07:22:28 GMT",
"version": "v1"
},
{
"created": "Wed, 5 May 1993 13:59:48 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Elitzur",
"Avshalom C.",
""
],
[
"Vaidman",
"Lev",
""
]
] | A novel manifestation of nonlocality of quantum mechanics is presented. It is shown that it is possible to ascertain the existence of an object in a given region of space without interacting with it. The method might have practical applications for delicate quantum experiments. | 11.855591 | 10.112716 | 9.665861 | 8.538492 | 8.554575 | 8.724959 | 8.442863 | 9.004012 | 9.410317 | 9.186566 | 10.111342 | 8.772962 | 9.514241 | 9.272687 | 8.95306 | 8.669351 | 8.840894 | 8.796101 | 9.351334 | 9.850848 | 9.559974 |
1805.01877 | Fotis Farakos | Fotis Farakos, Alex Kehagias and Antonio Riotto | Liberated N=1 Supergravity | 27 pages, published version | null | 10.1007/JHEP06(2018)011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss a new interaction for chiral models in four-dimensional ${\cal
N}=1$ supergavity. It contains a new arbitrary function in addition to the
K\"ahler potential and superpotential. Its features include linearly realized
off-shell supersymmetry, K\"ahler-Weyl invariance and broken supersymmetry. The
correspondi... | [
{
"created": "Fri, 4 May 2018 17:46:24 GMT",
"version": "v1"
},
{
"created": "Thu, 31 May 2018 06:05:16 GMT",
"version": "v2"
}
] | 2018-07-04 | [
[
"Farakos",
"Fotis",
""
],
[
"Kehagias",
"Alex",
""
],
[
"Riotto",
"Antonio",
""
]
] | We discuss a new interaction for chiral models in four-dimensional ${\cal N}=1$ supergavity. It contains a new arbitrary function in addition to the K\"ahler potential and superpotential. Its features include linearly realized off-shell supersymmetry, K\"ahler-Weyl invariance and broken supersymmetry. The corresponding... | 10.768363 | 9.879864 | 12.02301 | 9.844148 | 9.954995 | 10.170621 | 9.488702 | 10.192753 | 10.057006 | 12.04913 | 9.773973 | 10.719966 | 10.698258 | 10.804487 | 10.706302 | 10.486212 | 10.319982 | 10.639585 | 11.009678 | 11.13155 | 10.252053 |
0809.3623 | Laura Mersini-Houghton | Laura Mersini-Houghton | Birth of the Universe from the Multiverse | Invited book chapter in the book 'Beyond Big Bang', 25 pages | null | null | null | hep-th astro-ph gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is fair to say that the deepest mystery in our understanding of nature is
the birth of our universe. Much of the dilemma over the last decades comes from
the extraordinarily small probability that the universe started with the high
energy Big Bang as compared to the chance of nucleating any other event. How
can Bi... | [
{
"created": "Mon, 22 Sep 2008 01:55:43 GMT",
"version": "v1"
}
] | 2008-09-25 | [
[
"Mersini-Houghton",
"Laura",
""
]
] | It is fair to say that the deepest mystery in our understanding of nature is the birth of our universe. Much of the dilemma over the last decades comes from the extraordinarily small probability that the universe started with the high energy Big Bang as compared to the chance of nucleating any other event. How can Big ... | 16.817598 | 18.159672 | 17.680445 | 16.950815 | 18.932777 | 18.795336 | 17.803049 | 17.686777 | 17.411861 | 17.124458 | 17.189432 | 16.045004 | 16.726316 | 16.255817 | 16.279692 | 16.297987 | 16.632732 | 16.681198 | 16.248093 | 16.421648 | 15.838929 |
hep-th/0211230 | Shinobu Hosono | Shinobu Hosono, Bong H. Lian, Keiji Oguiso, Shing-Tung Yau | c=2 Rational Toroidal Conformal Field Theories via the Gauss Product | AMS-TeX, 45 pages; title changed, minor errors corrected,
acknowledgement added | Commun.Math.Phys.241:245-286,2003 | 10.1007/s00220-003-0927-0 | null | hep-th math.AG | null | We find a concise relation between the moduli $\tau, \rho$ of a rational
Narain lattice $\Gamma(\tau,\rho)$ and the corresponding momentum lattices of
left and right chiral algebras via the Gauss product. As a byproduct, we find
an identity which counts the cardinality of a certain double coset space
defined for isom... | [
{
"created": "Sun, 24 Nov 2002 05:53:13 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Dec 2002 09:38:57 GMT",
"version": "v2"
},
{
"created": "Fri, 2 May 2003 12:32:37 GMT",
"version": "v3"
}
] | 2010-11-19 | [
[
"Hosono",
"Shinobu",
""
],
[
"Lian",
"Bong H.",
""
],
[
"Oguiso",
"Keiji",
""
],
[
"Yau",
"Shing-Tung",
""
]
] | We find a concise relation between the moduli $\tau, \rho$ of a rational Narain lattice $\Gamma(\tau,\rho)$ and the corresponding momentum lattices of left and right chiral algebras via the Gauss product. As a byproduct, we find an identity which counts the cardinality of a certain double coset space defined for isomet... | 12.557026 | 14.085994 | 14.768806 | 12.379005 | 14.202785 | 13.228377 | 15.015358 | 12.956821 | 13.323953 | 16.233747 | 11.726454 | 11.210657 | 12.551881 | 11.049995 | 11.223289 | 11.760919 | 11.690111 | 11.631102 | 11.99259 | 12.937261 | 11.205486 |
2109.02545 | Ji Hoon Lee | Davide Gaiotto, Ji Hoon Lee | The Giant Graviton Expansion | 38+35 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose and test a novel conjectural relation satisfied by the
superconformal index of maximally supersymmetric $U(N)$ gauge theory in four
dimensions. Analogous relations appear to be also valid for the superconformal
indices of a large collection of other gauge theories, as well as for a broad
class of index-lik... | [
{
"created": "Mon, 6 Sep 2021 15:33:31 GMT",
"version": "v1"
}
] | 2021-09-07 | [
[
"Gaiotto",
"Davide",
""
],
[
"Lee",
"Ji Hoon",
""
]
] | We propose and test a novel conjectural relation satisfied by the superconformal index of maximally supersymmetric $U(N)$ gauge theory in four dimensions. Analogous relations appear to be also valid for the superconformal indices of a large collection of other gauge theories, as well as for a broad class of index-like ... | 11.426 | 10.492166 | 12.469726 | 10.232061 | 11.092395 | 10.68698 | 10.243687 | 10.381416 | 9.45641 | 11.758516 | 9.875663 | 9.511891 | 10.910917 | 9.809497 | 9.892623 | 9.784277 | 10.010337 | 9.792721 | 9.919694 | 10.179677 | 9.718349 |
1908.11396 | Yuji Sugimoto | Tomohiro Furukawa, Sanefumi Moriyama, Yuji Sugimoto | Quantum Mirror Map for Del Pezzo Geometries | 22 pages, 1 eps figure; v5: minor changes, published version | J.Phys.A 53 (2020) 38, 385401 | null | NITEP 26, OCU-PHYS 508, USTC-ICTS-19-22 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Mirror maps play an important role in studying supersymmetric gauge theories.
In these theories the dynamics is often encoded in an algebraic curve where two
sets of periods enjoy the symplectic structure. The A-periods contribute to
redefinitions of chemical potentials known as mirror maps. Using the
quantization of... | [
{
"created": "Thu, 29 Aug 2019 18:00:31 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Sep 2019 02:01:42 GMT",
"version": "v2"
},
{
"created": "Wed, 23 Oct 2019 07:37:21 GMT",
"version": "v3"
},
{
"created": "Mon, 30 Mar 2020 11:51:12 GMT",
"version": "v4"
},
{
"c... | 2020-11-03 | [
[
"Furukawa",
"Tomohiro",
""
],
[
"Moriyama",
"Sanefumi",
""
],
[
"Sugimoto",
"Yuji",
""
]
] | Mirror maps play an important role in studying supersymmetric gauge theories. In these theories the dynamics is often encoded in an algebraic curve where two sets of periods enjoy the symplectic structure. The A-periods contribute to redefinitions of chemical potentials known as mirror maps. Using the quantization of t... | 12.772405 | 12.282986 | 13.498205 | 12.141484 | 12.855985 | 12.46486 | 12.826838 | 13.104405 | 12.381181 | 15.285336 | 12.187165 | 11.695561 | 12.564114 | 11.489718 | 11.54234 | 11.815811 | 11.643163 | 12.270885 | 11.790398 | 12.365973 | 11.72185 |
1505.02986 | Dietmar Klemm | Federico Faedo, Dietmar Klemm and Masato Nozawa | Hairy black holes in N=2 gauged supergravity | 25 pages, 3 figures, uses jheppub.sty. v2: Refs. and some comments
added | null | null | IFUM-1040-FT | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct black holes with scalar hair in a wide class of four-dimensional
N=2 Fayet-Iliopoulos gauged supergravity theories that are characterized by a
prepotential containing one free parameter. Considering the truncated model in
which only a single real scalar survives, the theory is reduced to an
Einstein-scal... | [
{
"created": "Tue, 12 May 2015 12:50:13 GMT",
"version": "v1"
},
{
"created": "Fri, 22 May 2015 13:34:40 GMT",
"version": "v2"
}
] | 2015-05-25 | [
[
"Faedo",
"Federico",
""
],
[
"Klemm",
"Dietmar",
""
],
[
"Nozawa",
"Masato",
""
]
] | We construct black holes with scalar hair in a wide class of four-dimensional N=2 Fayet-Iliopoulos gauged supergravity theories that are characterized by a prepotential containing one free parameter. Considering the truncated model in which only a single real scalar survives, the theory is reduced to an Einstein-scalar... | 8.297248 | 8.569499 | 9.038309 | 8.152429 | 8.684296 | 8.889766 | 8.870009 | 8.629847 | 8.70847 | 9.244168 | 8.075641 | 8.393708 | 8.224519 | 7.910338 | 8.33013 | 8.397081 | 8.283045 | 8.117638 | 8.187596 | 8.239706 | 8.073545 |
hep-th/0608165 | Mu-In Park | Mu-in Park | BTZ Black Hole with Gravitational Chern-Simons: Thermodynamics and
Statistical Entropy | Accepted in Phys. Rev. D; Shortened version, Raised a new question of
the validity of the first law (No. 5 in Sec.5), Clarified the relation with
the Euclidean action approach for $1/\hbar$ factor (below (3.2)) | Phys.Rev.D77:026011,2008 | 10.1103/PhysRevD.77.026011 | null | hep-th | null | Recently, the BTZ black hole in the presence of the gravitational
Chern-Simons (GCS) term has been studied and it has been found that the usual
thermodynamical quantities, like as the black hole mass, angular momentum, and
black hole entropy, are modified. But, for large values of the GCS coupling,
where the modifica... | [
{
"created": "Wed, 23 Aug 2006 19:13:44 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Aug 2006 16:54:59 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Aug 2006 16:48:02 GMT",
"version": "v3"
},
{
"created": "Mon, 31 Dec 2007 02:37:56 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Park",
"Mu-in",
""
]
] | Recently, the BTZ black hole in the presence of the gravitational Chern-Simons (GCS) term has been studied and it has been found that the usual thermodynamical quantities, like as the black hole mass, angular momentum, and black hole entropy, are modified. But, for large values of the GCS coupling, where the modificati... | 8.617011 | 8.069955 | 9.067551 | 8.155659 | 8.450986 | 9.181447 | 8.795256 | 8.234054 | 8.270325 | 9.237481 | 8.345879 | 8.426719 | 8.633654 | 8.43366 | 8.443593 | 8.386699 | 8.358129 | 8.40668 | 8.275995 | 8.387242 | 8.25489 |
2006.03428 | Dharmesh Jain | Sunandan Gangopadhyay, Dharmesh Jain and Ashis Saha | Universal Pieces of Holographic Entanglement Entropy and Holographic
Subregion Complexity | v1: 18 pages; v2 & v3: 19 pages, title changed, sections 1 and 2
updated, references added, journal-ref added; v4: typos corrected, minor
changes to text (published version) | Phys. Rev. D 102, 046002 (2020) | 10.1103/PhysRevD.102.046002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose that the definition of holographic subregion complexity (HSC)
needs a slight modification for supergravity solutions with warped anti-de
Sitter (AdS) factors. Such warp factors can arise due to the nontrivial dilaton
profile, for example, in $AdS_6$ solutions of type IIA supergravity. This
modified definit... | [
{
"created": "Fri, 5 Jun 2020 13:27:56 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jul 2020 16:27:21 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Aug 2020 16:05:34 GMT",
"version": "v3"
},
{
"created": "Wed, 5 Aug 2020 06:34:45 GMT",
"version": "v4"
}
] | 2020-08-06 | [
[
"Gangopadhyay",
"Sunandan",
""
],
[
"Jain",
"Dharmesh",
""
],
[
"Saha",
"Ashis",
""
]
] | We propose that the definition of holographic subregion complexity (HSC) needs a slight modification for supergravity solutions with warped anti-de Sitter (AdS) factors. Such warp factors can arise due to the nontrivial dilaton profile, for example, in $AdS_6$ solutions of type IIA supergravity. This modified definitio... | 8.100758 | 8.144523 | 9.204721 | 7.322469 | 7.88202 | 7.800107 | 7.557945 | 8.100498 | 7.525166 | 9.373521 | 7.517039 | 7.676247 | 8.083978 | 7.523991 | 7.694027 | 7.696986 | 7.763915 | 7.407248 | 7.567731 | 8.511925 | 7.762898 |
1104.3210 | Pietro Menotti | Pietro Menotti | Riemann-Hilbert treatment of Liouville theory on the torus: The general
case | 22 pages, 2 figures, LaTex, added references | J.Phys.A44:335401,2011 | 10.1088/1751-8113/44/33/335401 | IFUP-TH/2011-7-r | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the previous treatment of Liouville theory on the torus, to the
general case in which the distribution of charges is not necessarily symmetric.
This requires the concept of Fuchsian differential equation on Riemann
surfaces. We show through a group theoretic argument that the Heun parameter
and a weight con... | [
{
"created": "Sat, 16 Apr 2011 08:40:23 GMT",
"version": "v1"
},
{
"created": "Fri, 6 May 2011 07:47:55 GMT",
"version": "v2"
}
] | 2011-07-28 | [
[
"Menotti",
"Pietro",
""
]
] | We extend the previous treatment of Liouville theory on the torus, to the general case in which the distribution of charges is not necessarily symmetric. This requires the concept of Fuchsian differential equation on Riemann surfaces. We show through a group theoretic argument that the Heun parameter and a weight const... | 10.623449 | 11.919993 | 12.899934 | 11.751787 | 11.102108 | 11.425232 | 11.684018 | 11.238699 | 11.659472 | 13.060834 | 11.155841 | 11.019885 | 11.223152 | 10.746214 | 10.651358 | 11.006082 | 10.781657 | 11.1368 | 11.130004 | 10.872741 | 10.451916 |
hep-th/0106195 | null | Cesar Gomez, Pedro Resco (IFT-UAM/CSIC) | Topics in String Tachyon Dynamics | 42 pages, 8 figures, corrected some typos. Lectures at the IV SIGRAV
School and 2001 School of Algebraic Geometry and Physics | null | null | IFT-UAM/CSIC-01-21 | hep-th | null | We review some aspects of string tachyon dynamics with special emphasis on
effective actions
| [
{
"created": "Thu, 21 Jun 2001 11:23:23 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Jun 2001 11:11:03 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Gomez",
"Cesar",
"",
"IFT-UAM/CSIC"
],
[
"Resco",
"Pedro",
"",
"IFT-UAM/CSIC"
]
] | We review some aspects of string tachyon dynamics with special emphasis on effective actions | 24.606544 | 12.000442 | 16.501354 | 13.082391 | 12.246182 | 13.443583 | 11.984053 | 15.348278 | 11.511495 | 17.512293 | 13.598289 | 16.00495 | 18.056877 | 16.118187 | 16.512197 | 16.2118 | 15.745484 | 16.825291 | 16.413357 | 18.139507 | 14.930692 |
1912.03021 | Mykola Shpot Dr. | M. A. Shpot | Boundary conformal field theory at the extraordinary transition: The
layer susceptibility to $O(\varepsilon)$ | v2: optimized for submitting; corrected eq. (59) v3: journal version | JHEP 2021 55 | 10.1007/JHEP01(2021)055 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an analytic calculation of the layer (parallel) susceptibility at
the extraordinary transition in a semi-infinite system with a flat boundary.
Using the method of integral transforms put forward by McAvity and Osborn
[Nucl. Phys. B 455 (1995) 522] in the boundary CFT we derive the
coordinate-space represen... | [
{
"created": "Fri, 6 Dec 2019 08:42:28 GMT",
"version": "v1"
},
{
"created": "Mon, 18 May 2020 15:47:27 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Jan 2021 10:52:28 GMT",
"version": "v3"
}
] | 2021-01-15 | [
[
"Shpot",
"M. A.",
""
]
] | We present an analytic calculation of the layer (parallel) susceptibility at the extraordinary transition in a semi-infinite system with a flat boundary. Using the method of integral transforms put forward by McAvity and Osborn [Nucl. Phys. B 455 (1995) 522] in the boundary CFT we derive the coordinate-space representa... | 10.053194 | 11.170261 | 11.741684 | 10.484246 | 11.213285 | 11.925886 | 10.592844 | 10.82208 | 10.474015 | 12.426476 | 9.985231 | 9.976136 | 10.349717 | 10.010043 | 10.069345 | 10.389253 | 10.118092 | 10.306914 | 9.945354 | 10.696894 | 10.055781 |
1703.07274 | Miguel Vazquez-Mozo | Diego Medrano Jimenez, Agustin Sabio Vera, Miguel A. Vazquez-Mozo | Projectivity of Planar Zeros in Field and String Theory Amplitudes | 39 page, 5 figures. v2: typos corrected. It matches the version
published in Journal of High Energy Physics | JHEP 1705 (2017) 011 | 10.1007/JHEP05(2017)011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the projective properties of planar zeros of tree-level scattering
amplitudes in various theories. Whereas for pure scalar field theories we find
that the planar zeros of the five-point amplitude do not enjoy projective
invariance, coupling scalars to gauge fields gives rise to tree-level
amplitudes whose pl... | [
{
"created": "Tue, 21 Mar 2017 15:28:24 GMT",
"version": "v1"
},
{
"created": "Thu, 4 May 2017 14:56:04 GMT",
"version": "v2"
}
] | 2017-05-05 | [
[
"Jimenez",
"Diego Medrano",
""
],
[
"Vera",
"Agustin Sabio",
""
],
[
"Vazquez-Mozo",
"Miguel A.",
""
]
] | We study the projective properties of planar zeros of tree-level scattering amplitudes in various theories. Whereas for pure scalar field theories we find that the planar zeros of the five-point amplitude do not enjoy projective invariance, coupling scalars to gauge fields gives rise to tree-level amplitudes whose plan... | 10.379911 | 9.746975 | 10.331726 | 9.548388 | 10.390219 | 9.092055 | 10.127224 | 10.109968 | 10.263378 | 11.264263 | 9.641583 | 10.003102 | 10.051754 | 9.929469 | 9.865395 | 9.821111 | 9.896081 | 10.03426 | 9.874514 | 9.901324 | 9.974876 |
hep-th/0211266 | Martin Rocek | Ulf Lindstrom, Martin Rocek, and Peter van Nieuwenhuizen | Consistent Boundary Conditions for Open Strings | Latex, 25 pages (references added) (journal version) | Nucl.Phys.B662:147-169,2003 | 10.1016/S0550-3213(03)00262-1 | ITP-UU-01/12, YITP-01/18 | hep-th | null | We study boundary conditions for the bosonic, spinning (NSR) and
Green-Schwarz open string, as well as for 1+1 dimensional supergravity. We
consider boundary conditions that arise from (1) extremizing the action, (2)
BRST, rigid or local supersymmetry, or kappa(Siegel)-symmetry of the action,
(3) closure of the set o... | [
{
"created": "Wed, 27 Nov 2002 20:28:55 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Jan 2003 21:18:39 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Mar 2003 13:49:26 GMT",
"version": "v3"
}
] | 2010-12-03 | [
[
"Lindstrom",
"Ulf",
""
],
[
"Rocek",
"Martin",
""
],
[
"van Nieuwenhuizen",
"Peter",
""
]
] | We study boundary conditions for the bosonic, spinning (NSR) and Green-Schwarz open string, as well as for 1+1 dimensional supergravity. We consider boundary conditions that arise from (1) extremizing the action, (2) BRST, rigid or local supersymmetry, or kappa(Siegel)-symmetry of the action, (3) closure of the set of ... | 9.326941 | 10.263655 | 10.671699 | 9.642827 | 9.520295 | 9.907559 | 10.276122 | 10.391923 | 9.484615 | 11.495428 | 9.002316 | 9.263563 | 10.205481 | 8.940283 | 8.880185 | 9.684802 | 9.222482 | 9.086365 | 9.1632 | 9.946808 | 9.600071 |
2202.05866 | Clay C\'ordova | Clay Cordova, Kantaro Ohmori, Tom Rudelius | Generalized Symmetry Breaking Scales and Weak Gravity Conjectures | 44 pages, 1 figure | null | 10.1007/JHEP11(2022)154 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the notion of approximate global symmetries in quantum field
theory and quantum gravity. We show that a variety of conjectures about quantum
gravity, including the weak gravity conjecture, the distance conjecture, and
the magnetic and axion versions of the weak gravity conjecture can be motivated
by the as... | [
{
"created": "Fri, 11 Feb 2022 19:13:57 GMT",
"version": "v1"
}
] | 2022-12-14 | [
[
"Cordova",
"Clay",
""
],
[
"Ohmori",
"Kantaro",
""
],
[
"Rudelius",
"Tom",
""
]
] | We explore the notion of approximate global symmetries in quantum field theory and quantum gravity. We show that a variety of conjectures about quantum gravity, including the weak gravity conjecture, the distance conjecture, and the magnetic and axion versions of the weak gravity conjecture can be motivated by the assu... | 6.876041 | 6.78934 | 7.641356 | 6.090495 | 6.195504 | 7.077627 | 6.960829 | 6.677839 | 6.324382 | 7.753557 | 6.595358 | 6.406579 | 6.791018 | 6.517592 | 6.56954 | 6.582123 | 6.489204 | 6.264388 | 6.503927 | 6.86526 | 6.464166 |
1809.05535 | Alan Kostelecky | Benjamin R. Edwards and Alan Kostelecky | Riemann-Finsler Geometry and Lorentz-Violating Scalar Fields | 9 pages, version published in Physics Letters B | Phys.Lett.B786: 319-326, 2018 | 10.1016/j.physletb.2018.10.011 | null | hep-th gr-qc hep-ph math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The correspondence between Riemann-Finsler geometries and effective field
theories with spin-independent Lorentz violation is explored. We obtain the
general quadratic action for effective scalar field theories in any spacetime
dimension with Lorentz-violating operators of arbitrary mass dimension.
Classical relativi... | [
{
"created": "Fri, 14 Sep 2018 16:33:41 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Oct 2018 14:08:16 GMT",
"version": "v2"
}
] | 2018-10-18 | [
[
"Edwards",
"Benjamin R.",
""
],
[
"Kostelecky",
"Alan",
""
]
] | The correspondence between Riemann-Finsler geometries and effective field theories with spin-independent Lorentz violation is explored. We obtain the general quadratic action for effective scalar field theories in any spacetime dimension with Lorentz-violating operators of arbitrary mass dimension. Classical relativist... | 8.724734 | 8.45642 | 7.930461 | 8.029458 | 8.225076 | 8.820588 | 8.329041 | 8.732243 | 7.605301 | 8.601733 | 8.297653 | 8.400967 | 8.662768 | 8.464351 | 8.211942 | 8.136027 | 8.511127 | 8.323915 | 8.097719 | 8.66253 | 8.29226 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.