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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2111.04591 | Zimo Sun | Zimo Sun | A note on the representations of $\text{SO}(1,d+1)$ | 47+16 pages, 10 figures; references added, acknowledgement corrected | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | $\text{SO}(1, d+1)$ is the isometry group of $(d+1)$-dimensional de Sitter
spacetime $\text{dS}_{d+1}$ and the conformal group of $\mathbb{R}^{d}$. This
note gives a pedagogical introduction to the representation theory of
$\text{SO}(1, d+1)$, from the perspective of de Sitter quantum field theory and
using tools fro... | [
{
"created": "Mon, 8 Nov 2021 15:56:36 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Nov 2021 15:57:47 GMT",
"version": "v2"
}
] | 2021-11-18 | [
[
"Sun",
"Zimo",
""
]
] | $\text{SO}(1, d+1)$ is the isometry group of $(d+1)$-dimensional de Sitter spacetime $\text{dS}_{d+1}$ and the conformal group of $\mathbb{R}^{d}$. This note gives a pedagogical introduction to the representation theory of $\text{SO}(1, d+1)$, from the perspective of de Sitter quantum field theory and using tools from ... | 3.191431 | 3.071059 | 3.143451 | 2.8974 | 3.027628 | 3.091913 | 3.10371 | 2.99366 | 3.001379 | 3.214297 | 2.984329 | 2.963393 | 3.048851 | 2.983608 | 2.98311 | 2.930207 | 2.996213 | 2.950127 | 3.035198 | 3.12125 | 2.979697 |
hep-th/0506167 | Sugumi Kanno | Sugumi Kanno, Jiro Soda, David Wands | Braneworld Flux Inflation | 11 pages, 6 figures, references added | JCAP 0508 (2005) 002 | 10.1088/1475-7516/2005/08/002 | KUNS-1976 | hep-th astro-ph gr-qc | null | We propose a geometrical model of brane inflation where inflation is driven
by the flux generated by opposing brane charges and terminated by the collision
of the branes, with charge annihilation. We assume the collision process is
completely inelastic and the kinetic energy is transformed into the thermal
energy aft... | [
{
"created": "Tue, 21 Jun 2005 02:13:04 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Jun 2005 03:24:21 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Kanno",
"Sugumi",
""
],
[
"Soda",
"Jiro",
""
],
[
"Wands",
"David",
""
]
] | We propose a geometrical model of brane inflation where inflation is driven by the flux generated by opposing brane charges and terminated by the collision of the branes, with charge annihilation. We assume the collision process is completely inelastic and the kinetic energy is transformed into the thermal energy after... | 10.630166 | 10.931206 | 11.450855 | 10.698613 | 10.947426 | 10.995394 | 11.835552 | 10.59512 | 10.556708 | 12.564641 | 10.057147 | 10.014423 | 10.914945 | 10.551223 | 10.657569 | 10.458097 | 10.082343 | 10.575089 | 10.493389 | 11.551111 | 10.403234 |
hep-th/9306097 | Shin'ichi Nojiri | Shin'ich Nojiri and Ichiro Oda | Black Hole Physics from Two Dimensional Dilaton Gravity based on
$SL(2,R)/U(1)$ Coset Model | NDA-FP-12/93, OCHA-PP-33, INS-Rep.987 | Phys.Rev. D49 (1994) 4066-4077 | 10.1103/PhysRevD.49.4066 | null | hep-th | null | We analyze quantum two dimensional dilaton gravity model, which is described
by $SL(2,R)/U(1)$ gauged Wess-Zumino-Witten model deformed by $(1,1)$ operator.
We show that the curvature singularity does not appear when the central charge
$c_{\rm matter}$ of the matter fields is given by $22<c_{\rm matter}<24$. When
$22... | [
{
"created": "Mon, 21 Jun 1993 06:19:45 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Nojiri",
"Shin'ich",
""
],
[
"Oda",
"Ichiro",
""
]
] | We analyze quantum two dimensional dilaton gravity model, which is described by $SL(2,R)/U(1)$ gauged Wess-Zumino-Witten model deformed by $(1,1)$ operator. We show that the curvature singularity does not appear when the central charge $c_{\rm matter}$ of the matter fields is given by $22<c_{\rm matter}<24$. When $22<c... | 6.63358 | 6.981932 | 7.221116 | 6.676635 | 7.399685 | 7.195556 | 7.080816 | 6.760581 | 6.886148 | 7.960851 | 6.489849 | 6.690687 | 6.730791 | 6.616598 | 6.723582 | 6.785062 | 6.693485 | 6.699721 | 6.58672 | 6.740365 | 6.578927 |
hep-th/0502201 | Antonio Soares de Castro | Antonio S. de Castro | Klein-Gordon particles in mixed vector-scalar inversely linear
potentials | 17 pages, 5 figures | Phys.Lett. A338 (2005) 81-89 | 10.1016/j.physleta.2005.02.027 | null | hep-th quant-ph | null | The problem of a spinless particle subject to a general mixing of vector and
scalar inversely linear potentials in a two-dimensional world is analyzed.
Exact bounded solutions are found in closed form by imposing boundary
conditions on the eigenfunctions which ensure that the effective Hamiltonian is
Hermitian for al... | [
{
"created": "Tue, 22 Feb 2005 19:57:18 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Feb 2005 17:28:05 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"de Castro",
"Antonio S.",
""
]
] | The problem of a spinless particle subject to a general mixing of vector and scalar inversely linear potentials in a two-dimensional world is analyzed. Exact bounded solutions are found in closed form by imposing boundary conditions on the eigenfunctions which ensure that the effective Hamiltonian is Hermitian for all ... | 11.911551 | 9.925071 | 12.228657 | 10.827079 | 9.595465 | 9.623014 | 9.437594 | 9.379181 | 10.218175 | 13.494215 | 9.370138 | 10.982637 | 11.549002 | 10.433603 | 10.854072 | 10.269514 | 10.38786 | 10.156133 | 10.575072 | 12.056751 | 10.537635 |
2402.14512 | Pavel Slepov | Irina Ya. Aref'eva, Ali Hajilou, Pavel Slepov and Marina Usova | Running Coupling and Beta-Functions for HQCD with Heavy and Light
Quarks: Isotropic case | A new solution is added; 87 pages, 62 figures, 3 tables | null | null | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | We consider running coupling constant and beta-function in holographic models
supported by Einstein-dilaton-Maxwell action for heavy and light quarks. To
obtain the dependence of the running coupling constant $\alpha$ on temperature
and chemical potential we impose boundary conditions on the dilaton field that
depend... | [
{
"created": "Thu, 22 Feb 2024 13:03:01 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 2024 17:05:02 GMT",
"version": "v2"
}
] | 2024-05-08 | [
[
"Aref'eva",
"Irina Ya.",
""
],
[
"Hajilou",
"Ali",
""
],
[
"Slepov",
"Pavel",
""
],
[
"Usova",
"Marina",
""
]
] | We consider running coupling constant and beta-function in holographic models supported by Einstein-dilaton-Maxwell action for heavy and light quarks. To obtain the dependence of the running coupling constant $\alpha$ on temperature and chemical potential we impose boundary conditions on the dilaton field that depend o... | 9.488227 | 8.95736 | 9.534846 | 8.168885 | 8.931376 | 8.276305 | 8.944039 | 8.646276 | 8.056483 | 9.606651 | 8.423824 | 8.470425 | 8.970401 | 8.520846 | 8.367984 | 8.626226 | 8.143674 | 8.629737 | 8.561766 | 8.842509 | 8.417484 |
2104.07030 | Sam van Leuven | Vishnu Jejjala, Yang Lei, Sam van Leuven, Wei Li | $SL(3,\mathbb{Z})$ Modularity and New Cardy Limits of the
$\mathcal{N}=4$ Superconformal Index | 63 pages + appendices. v2: refs added, various corrections and
improvements, discussion section rewritten. v3: corrected defn normalized
partition function, added tau=sigma limit modular property in section 3.5 +
its physical interpretation in section 5.2. (published version) | null | 10.1007/JHEP11(2021)047 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The entropy of $1/16$-th BPS AdS$_5$ black holes can be microscopically
accounted for by the superconformal index of the $\mathcal{N}=4$
super-Yang-Mills theory. One way to compute this is through a Cardy-like limit
of a formula for the index obtained in [1] using the "$S$-transformation" of
the elliptic $\Gamma$ fun... | [
{
"created": "Wed, 14 Apr 2021 18:00:00 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Jul 2021 16:03:45 GMT",
"version": "v2"
},
{
"created": "Wed, 29 Sep 2021 15:56:30 GMT",
"version": "v3"
}
] | 2021-11-24 | [
[
"Jejjala",
"Vishnu",
""
],
[
"Lei",
"Yang",
""
],
[
"van Leuven",
"Sam",
""
],
[
"Li",
"Wei",
""
]
] | The entropy of $1/16$-th BPS AdS$_5$ black holes can be microscopically accounted for by the superconformal index of the $\mathcal{N}=4$ super-Yang-Mills theory. One way to compute this is through a Cardy-like limit of a formula for the index obtained in [1] using the "$S$-transformation" of the elliptic $\Gamma$ funct... | 6.08191 | 5.226427 | 6.2858 | 5.290007 | 5.675915 | 5.480066 | 5.253434 | 5.082406 | 5.262556 | 6.91609 | 5.124206 | 5.425963 | 6.191868 | 5.521105 | 5.523722 | 5.38064 | 5.689672 | 5.463645 | 5.455945 | 5.893529 | 5.502365 |
0902.4173 | Yosuke Imamura | Yosuke Imamura | Monopole operators in N=4 Chern-Simons theories and wrapped M2-branes | 18 pages, 2 figures, LaTeX. v2: references added, typos corrected | Prog.Theor.Phys.121:1173-1187,2009 | 10.1143/PTP.121.1173 | UT-09-05 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Monopole operators in Abelian N=4 Chern-Simons theories described by circular
quiver diagrams are investigated. The magnetic charges of non-diagonal U(1)
gauge symmetries form the SU(p)xSU(q) root lattice where p and q are numbers of
untwisted and twisted hypermultiplets, respectively. For monopole operators
correspo... | [
{
"created": "Tue, 24 Feb 2009 15:29:07 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Mar 2009 06:04:34 GMT",
"version": "v2"
}
] | 2011-08-23 | [
[
"Imamura",
"Yosuke",
""
]
] | Monopole operators in Abelian N=4 Chern-Simons theories described by circular quiver diagrams are investigated. The magnetic charges of non-diagonal U(1) gauge symmetries form the SU(p)xSU(q) root lattice where p and q are numbers of untwisted and twisted hypermultiplets, respectively. For monopole operators correspond... | 8.512851 | 9.23219 | 10.219751 | 7.568226 | 8.857442 | 8.630947 | 8.829041 | 8.581491 | 7.659822 | 12.178231 | 7.922261 | 8.20178 | 8.199479 | 8.018775 | 8.044738 | 7.862592 | 7.787949 | 8.049603 | 7.933992 | 8.21302 | 8.05899 |
1910.07354 | Borut Bajc | Borut Bajc, Adrian Lugo and Francesco Sannino | Safe Hologram | 6 pages | null | 10.1142/S0217732320502739 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a holographic model encapsulating the dynamics of safe quantum
field theories.
| [
{
"created": "Wed, 16 Oct 2019 14:05:13 GMT",
"version": "v1"
}
] | 2020-12-02 | [
[
"Bajc",
"Borut",
""
],
[
"Lugo",
"Adrian",
""
],
[
"Sannino",
"Francesco",
""
]
] | We introduce a holographic model encapsulating the dynamics of safe quantum field theories. | 41.661404 | 14.653802 | 22.898167 | 21.244043 | 16.947327 | 20.145649 | 16.006895 | 23.280703 | 20.626055 | 27.393353 | 23.279642 | 19.875866 | 24.60367 | 22.521385 | 21.998596 | 22.105305 | 22.072193 | 23.072752 | 22.009108 | 26.196728 | 26.453241 |
2310.15792 | Dan Xie | Yuanyuan Fang, Jing Feng, Dan Xie | Three dimensional quotient singularity and 4d $\mathcal{N}=1$ AdS/CFT
correspondence | 43 pages, 15 tables, and 13 figures | null | null | null | hep-th math.AG | http://creativecommons.org/licenses/by/4.0/ | We systematically study the AdS/CFT correspondence induced by D3 branes
probing three dimensional Gorenstein quotient singularity $\mathbb{C}^3/G$. The
field theory is given by the McKay quiver, which has a vanishing NSVZ beta
function assuming that all the chiral fields have the $U(1)_R$ charge
$\frac{2}{3}$. Variou... | [
{
"created": "Tue, 24 Oct 2023 12:42:21 GMT",
"version": "v1"
}
] | 2023-10-25 | [
[
"Fang",
"Yuanyuan",
""
],
[
"Feng",
"Jing",
""
],
[
"Xie",
"Dan",
""
]
] | We systematically study the AdS/CFT correspondence induced by D3 branes probing three dimensional Gorenstein quotient singularity $\mathbb{C}^3/G$. The field theory is given by the McKay quiver, which has a vanishing NSVZ beta function assuming that all the chiral fields have the $U(1)_R$ charge $\frac{2}{3}$. Various ... | 9.975076 | 9.265951 | 12.515349 | 9.032495 | 9.067762 | 9.900388 | 9.375517 | 9.867147 | 9.744847 | 10.892122 | 9.398616 | 9.192381 | 10.097952 | 9.036716 | 8.776692 | 9.232307 | 9.050112 | 9.204672 | 9.062581 | 9.729045 | 9.162724 |
0807.1293 | Ant\'on F. Faedo | Enrique Alvarez, Anton F. Faedo and J.J. Lopez-Villarejo | Ultraviolet behavior of transverse gravity | 22 pages | JHEP0810:023,2008 | 10.1088/1126-6708/2008/10/023 | IFT-UAM/CSIC-08-31 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The structure of the divergences for transverse theories of gravity is
studied to one-loop order. These theories are invariant only under those
diffeomorphisms that enjoy unit Jacobian determinant (TDiff), so that the
determinant of the metric transforms as a true scalar instead of a density.
Generically, the models ... | [
{
"created": "Tue, 8 Jul 2008 16:24:20 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Alvarez",
"Enrique",
""
],
[
"Faedo",
"Anton F.",
""
],
[
"Lopez-Villarejo",
"J. J.",
""
]
] | The structure of the divergences for transverse theories of gravity is studied to one-loop order. These theories are invariant only under those diffeomorphisms that enjoy unit Jacobian determinant (TDiff), so that the determinant of the metric transforms as a true scalar instead of a density. Generically, the models in... | 9.664923 | 9.223166 | 9.135498 | 8.21245 | 9.272977 | 9.238386 | 9.703707 | 8.26544 | 8.518914 | 9.436854 | 8.983761 | 8.80823 | 8.658813 | 8.650403 | 8.447047 | 8.410742 | 8.76311 | 8.418989 | 8.540941 | 8.852144 | 8.78044 |
1112.3541 | Askold Duviryak | Jurij W. Darewych and Askold Duviryak | Analysis of inter-quark interactions in classical chromodynamics | 10 pages, 1 figure, LaTex2e | Cent. Eur. J. Phys. 11(3): 336-344, 2013 | 10.2478/s11534-013-0171-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The QCD gluon equation of motion is solved approximately by means of the
Green function. This solution is used to reformulate the Lagrangian of QCD such
that the gluon propagator appears directly in the interaction terms of the
Lagrangian. The nature of the interactions is discussed. Their coordinate-space
form is pr... | [
{
"created": "Thu, 15 Dec 2011 15:46:30 GMT",
"version": "v1"
}
] | 2019-10-04 | [
[
"Darewych",
"Jurij W.",
""
],
[
"Duviryak",
"Askold",
""
]
] | The QCD gluon equation of motion is solved approximately by means of the Green function. This solution is used to reformulate the Lagrangian of QCD such that the gluon propagator appears directly in the interaction terms of the Lagrangian. The nature of the interactions is discussed. Their coordinate-space form is pres... | 9.584065 | 8.968979 | 8.879566 | 8.313393 | 8.093143 | 8.975045 | 7.774409 | 9.016871 | 7.954049 | 8.926509 | 8.490951 | 9.000685 | 8.511385 | 8.464474 | 8.429416 | 8.529013 | 8.855094 | 8.64394 | 8.565798 | 8.327261 | 8.601949 |
1712.03928 | Julio Parra-Martinez | Zvi Bern, Julio Parra-Martinez, Radu Roiban | Cancelling the U(1) Anomaly in the S-matrix of N=4 Supergravity | 6 pages, journal version | Phys. Rev. Lett. 121, 101604 (2018) | 10.1103/PhysRevLett.121.101604 | UCLA/17/TEP/107 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | ${{\cal N}=4}$ supergravity is understood to contain a $U(1)$ anomaly which
manifests itself via the nonvanishing of loop-level scattering amplitudes that
violate a tree-level charge conservation rule. In this letter we provide
detailed evidence that at one loop such anomalous amplitudes can be set to zero
by the add... | [
{
"created": "Mon, 11 Dec 2017 18:16:12 GMT",
"version": "v1"
},
{
"created": "Sat, 10 Nov 2018 23:26:37 GMT",
"version": "v2"
}
] | 2018-11-13 | [
[
"Bern",
"Zvi",
""
],
[
"Parra-Martinez",
"Julio",
""
],
[
"Roiban",
"Radu",
""
]
] | ${{\cal N}=4}$ supergravity is understood to contain a $U(1)$ anomaly which manifests itself via the nonvanishing of loop-level scattering amplitudes that violate a tree-level charge conservation rule. In this letter we provide detailed evidence that at one loop such anomalous amplitudes can be set to zero by the addit... | 8.61953 | 8.350352 | 8.688342 | 8.027052 | 8.456248 | 8.146719 | 7.877882 | 8.194986 | 8.003579 | 9.2445 | 8.335347 | 8.165445 | 8.098001 | 7.912356 | 8.33605 | 8.178975 | 8.368278 | 8.033525 | 8.069841 | 8.175528 | 7.860872 |
1802.00006 | Jorrit Kruthoff | Alexandre Belin, Jan de Boer, Jorrit Kruthoff | Comments on a state-operator correspondence for the torus | 29 pages, 8 figures | SciPost Phys. 5, 060 (2018) | 10.21468/SciPostPhys.5.6.060 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the existence of a state-operator correspondence on the torus.
This correspondence would relate states of the CFT Hilbert space living on a
spatial torus to the path integral over compact Euclidean manifolds with
operator insertions. Unlike the states on the sphere that are associated to
local operator... | [
{
"created": "Wed, 31 Jan 2018 19:00:00 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Oct 2018 01:59:35 GMT",
"version": "v2"
}
] | 2018-12-12 | [
[
"Belin",
"Alexandre",
""
],
[
"de Boer",
"Jan",
""
],
[
"Kruthoff",
"Jorrit",
""
]
] | We investigate the existence of a state-operator correspondence on the torus. This correspondence would relate states of the CFT Hilbert space living on a spatial torus to the path integral over compact Euclidean manifolds with operator insertions. Unlike the states on the sphere that are associated to local operators,... | 8.499074 | 9.114733 | 10.310901 | 8.594156 | 9.079865 | 9.158144 | 9.978361 | 8.645337 | 8.58465 | 10.107871 | 8.721927 | 8.656551 | 8.884311 | 8.21415 | 8.245592 | 8.323401 | 8.531104 | 7.981446 | 8.50092 | 8.824952 | 8.157074 |
1612.03289 | Roldao da Rocha | Nelson R. F. Braga, Roldao da Rocha | Configurational entropy of anti-de Sitter black holes | 7 pages, 4 figures | Phys. Lett. B 767 (2017) 381 | 10.1016/j.physletb.2017.02.031 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent studies indicate that the configurational entropy is an useful tool to
investigate the stability and (or) the relative dominance of states for diverse
physical systems. Recent examples comprise the connection between the variation
of this quantity and the relative fraction of light mesons and glueballs
observe... | [
{
"created": "Sat, 10 Dec 2016 13:01:40 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Feb 2017 16:57:07 GMT",
"version": "v2"
}
] | 2017-02-22 | [
[
"Braga",
"Nelson R. F.",
""
],
[
"da Rocha",
"Roldao",
""
]
] | Recent studies indicate that the configurational entropy is an useful tool to investigate the stability and (or) the relative dominance of states for diverse physical systems. Recent examples comprise the connection between the variation of this quantity and the relative fraction of light mesons and glueballs observed ... | 10.499778 | 10.715067 | 10.52705 | 9.956237 | 10.642839 | 10.394327 | 10.526862 | 9.882371 | 9.8775 | 10.954705 | 10.6436 | 10.315152 | 10.301058 | 10.205073 | 10.284169 | 10.246513 | 10.34524 | 10.393154 | 10.165036 | 10.006278 | 10.297801 |
0911.5697 | Thomas Danckaert | Thomas Danckaert and Jan Louis | Type IIA orientifold compactification on SU(2)-structure manifolds | 31 pages; v2: local report number added | JHEP 1001:105,2010 | 10.1007/JHEP01(2010)105 | ZMP-HH/09-30 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the effective theory of type IIA string theory on
six-dimensional orientifold backgrounds with SU(2)-structure. We focus on the
case of orientifolds with O6-planes, for which we compute the bosonic effective
action in the supergravity approximation. For a generic SU(2)-structure
background, we find tha... | [
{
"created": "Mon, 30 Nov 2009 17:50:57 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Dec 2009 17:03:29 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Danckaert",
"Thomas",
""
],
[
"Louis",
"Jan",
""
]
] | We investigate the effective theory of type IIA string theory on six-dimensional orientifold backgrounds with SU(2)-structure. We focus on the case of orientifolds with O6-planes, for which we compute the bosonic effective action in the supergravity approximation. For a generic SU(2)-structure background, we find that ... | 6.609661 | 6.099223 | 8.708387 | 6.770622 | 6.066543 | 6.315216 | 6.590522 | 6.238451 | 6.981016 | 8.127396 | 6.566569 | 6.593117 | 7.118877 | 6.290946 | 6.484291 | 6.461237 | 6.534172 | 6.650301 | 6.446255 | 7.336411 | 6.242146 |
hep-th/0008245 | Shoichi Ichinose | Shoichi Ichinose | Wall and Anti-Wall in the Randall-Sundrum Model and A New Infrared
Regularization | 36 pages, 29 eps figure files | Phys.Rev. D65 (2002) 084038 | 10.1103/PhysRevD.65.084038 | US-00-07 | hep-th hep-ph | null | An approach to find the field equation solution of the Randall-Sundrum model
with the $S^1/Z_2$ extra axis is presented. We closely examine the infrared
singularity. The vacuum is set by the 5 dimensional Higgs field. Both the
domain-wall and the anti-domain-wall naturally appear, at the {\it ends} of the
extra compa... | [
{
"created": "Thu, 31 Aug 2000 09:26:04 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Sep 2000 06:34:19 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Sep 2001 13:22:20 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Ichinose",
"Shoichi",
""
]
] | An approach to find the field equation solution of the Randall-Sundrum model with the $S^1/Z_2$ extra axis is presented. We closely examine the infrared singularity. The vacuum is set by the 5 dimensional Higgs field. Both the domain-wall and the anti-domain-wall naturally appear, at the {\it ends} of the extra compact... | 19.095385 | 18.164114 | 18.939453 | 17.309284 | 18.419348 | 18.112415 | 18.446882 | 18.45747 | 18.491245 | 21.716089 | 18.378815 | 18.260462 | 17.535706 | 17.435093 | 17.454924 | 17.884407 | 17.671804 | 18.026756 | 17.137009 | 17.161844 | 17.860941 |
1002.3388 | Augusto Sagnotti | A. Sagnotti (Scuola Normale Superiore and INFN, Pisa) | Higher Spins and Current Exchanges | 7 pages, LATEX. Lecture presented at the 9th Hellenic School on
Elementary Particle Physics and Gravity, Corfu 2009 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The simplest higher-spin interactions involve classical external currents and
symmetric tensors $\phi_{\m_1 ... \m_s}$, and convey three instructive lessons.
The first is a general form of the van Dam-Veltman-Zakharov discontinuity in
flat space for this class of fields. The second is the rationale for its
disappeara... | [
{
"created": "Wed, 17 Feb 2010 21:50:02 GMT",
"version": "v1"
}
] | 2010-02-19 | [
[
"Sagnotti",
"A.",
"",
"Scuola Normale Superiore and INFN, Pisa"
]
] | The simplest higher-spin interactions involve classical external currents and symmetric tensors $\phi_{\m_1 ... \m_s}$, and convey three instructive lessons. The first is a general form of the van Dam-Veltman-Zakharov discontinuity in flat space for this class of fields. The second is the rationale for its disappearanc... | 18.388336 | 17.251696 | 18.707914 | 16.230371 | 15.209167 | 18.4342 | 16.364357 | 15.40846 | 15.523235 | 19.520243 | 15.903703 | 16.220425 | 17.244108 | 16.682335 | 16.684877 | 16.454168 | 15.927218 | 15.871048 | 16.702959 | 16.91412 | 16.2628 |
1610.01835 | Mohammad Ali-Akbari | M. Rahimi, M. Ali-Akbari, M. Lezgi | Entanglement Entropy in a Non-Conformal Background | 5 pages, 3 figures, published version | null | 10.1016/j.physletb.2017.05.055 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use gauge-gravity duality to compute entanglement entropy in a
non-conformal background with an energy scale $\Lambda$. At zero temperature,
we observe that entanglement entropy decreases by raising $\Lambda$. However,
at finite temperature, we realize that both $\frac{\Lambda}{T}$ and
entanglement entropy rise to... | [
{
"created": "Thu, 6 Oct 2016 12:12:36 GMT",
"version": "v1"
},
{
"created": "Fri, 7 Oct 2016 06:28:03 GMT",
"version": "v2"
},
{
"created": "Tue, 25 Jul 2017 12:20:07 GMT",
"version": "v3"
}
] | 2017-08-02 | [
[
"Rahimi",
"M.",
""
],
[
"Ali-Akbari",
"M.",
""
],
[
"Lezgi",
"M.",
""
]
] | We use gauge-gravity duality to compute entanglement entropy in a non-conformal background with an energy scale $\Lambda$. At zero temperature, we observe that entanglement entropy decreases by raising $\Lambda$. However, at finite temperature, we realize that both $\frac{\Lambda}{T}$ and entanglement entropy rise toge... | 5.476958 | 4.971721 | 4.977445 | 5.018717 | 5.17462 | 5.073857 | 5.410158 | 4.959249 | 4.93803 | 5.474892 | 5.133049 | 5.089314 | 5.076756 | 5.207259 | 4.992705 | 5.026476 | 5.140088 | 4.925246 | 5.080715 | 5.147412 | 4.98701 |
hep-th/9802156 | I. L. Buchbinder | I.L. Buchbinder (Tomsk State Pedagogical University), B.A.Ovrut
(University of Pennsylvania) | Background Field Method and Structure of Effective Action in N=2 Super
Yang-Mills Theories | 7 pages, 1 figure. The extended talk given by I.L. Buchbinder at 31st
International Ahrenshoop Symposium on the Theory of Elementary Particles,
Buckow, Germany, 2-6 September 1997, will be published in the Proceedings | null | null | null | hep-th | null | This paper is a brief review of background field method and some of its
applications in N=2 super Yang-Mills theories with a matter within harmonic
superspace approach. A general structure of effective action is discussed, an
absence of two-loop quantum corrections to first non-leading term in effective
action is pro... | [
{
"created": "Mon, 23 Feb 1998 05:06:48 GMT",
"version": "v1"
},
{
"created": "Sat, 28 Feb 1998 06:42:39 GMT",
"version": "v2"
}
] | 2009-09-25 | [
[
"Buchbinder",
"I. L.",
"",
"Tomsk State Pedagogical University"
],
[
"Ovrut",
"B. A.",
"",
"University of Pennsylvania"
]
] | This paper is a brief review of background field method and some of its applications in N=2 super Yang-Mills theories with a matter within harmonic superspace approach. A general structure of effective action is discussed, an absence of two-loop quantum corrections to first non-leading term in effective action is prove... | 12.527485 | 10.215139 | 11.933702 | 9.51425 | 10.097836 | 9.639968 | 10.225986 | 8.573593 | 8.647817 | 14.731874 | 9.299762 | 10.40923 | 12.035948 | 10.678774 | 10.834528 | 11.087837 | 10.789099 | 10.935137 | 10.531385 | 12.742193 | 11.078081 |
2108.10669 | Robert de Mello Koch | Robert de Mello Koch, Minkyoo Kim and Hendrik J.R. Van Zyl | Complexity from Spinning Primaries | 30+1 pages; v2: refs added | null | 10.1007/JHEP12(2021)030 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define circuits given by unitary representations of Lorentzian conformal
field theory in 3 and 4 dimensions. Our circuits start from a spinning primary
state, allowing us to generalize formulas for the circuit complexity obtained
from circuits starting from scalar primary states. These results are nicely
reproduce... | [
{
"created": "Tue, 24 Aug 2021 12:16:21 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Aug 2021 09:39:20 GMT",
"version": "v2"
}
] | 2021-12-22 | [
[
"Koch",
"Robert de Mello",
""
],
[
"Kim",
"Minkyoo",
""
],
[
"Van Zyl",
"Hendrik J. R.",
""
]
] | We define circuits given by unitary representations of Lorentzian conformal field theory in 3 and 4 dimensions. Our circuits start from a spinning primary state, allowing us to generalize formulas for the circuit complexity obtained from circuits starting from scalar primary states. These results are nicely reproduced ... | 17.132401 | 15.50873 | 19.29921 | 14.91566 | 15.1091 | 14.272849 | 13.782557 | 14.88245 | 15.936193 | 18.154818 | 15.551989 | 16.821705 | 17.865995 | 15.81473 | 16.622238 | 16.180975 | 16.763208 | 16.082563 | 16.00029 | 17.776625 | 15.787793 |
1006.2709 | Aram Saharian | A.A. Saharian, M.R. Setare | Casimir effect for curved boundaries in Robertson-Walker spacetime | 11 pages, 3 figures | Class.Quant.Grav.27:225009,2010 | 10.1088/0264-9381/27/22/225009 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Vacuum expectation values of the energy-momentum tensor and the Casimir
forces are evaluated for scalar and electromagnetic fields in the geometry of
two curved boundaries on background of the Robertson-Walker spacetime with
negative spatial curvature. Robin boundary conditions are imposed in the case
of the scalar f... | [
{
"created": "Mon, 14 Jun 2010 13:42:48 GMT",
"version": "v1"
}
] | 2010-11-12 | [
[
"Saharian",
"A. A.",
""
],
[
"Setare",
"M. R.",
""
]
] | Vacuum expectation values of the energy-momentum tensor and the Casimir forces are evaluated for scalar and electromagnetic fields in the geometry of two curved boundaries on background of the Robertson-Walker spacetime with negative spatial curvature. Robin boundary conditions are imposed in the case of the scalar fie... | 6.249954 | 3.873258 | 6.82368 | 4.379653 | 4.242148 | 4.285695 | 4.331903 | 4.402675 | 4.2394 | 6.690035 | 4.688344 | 5.101882 | 6.08273 | 5.707333 | 5.400862 | 5.342732 | 5.178696 | 5.272019 | 5.483111 | 6.04024 | 5.286994 |
hep-th/9412131 | Banks Tomas | Thomas Banks (Rutgers University) | Lectures On Black Hole Evaporation and Information Loss | 65 pages, 9 figures submitted separately as a uuencoded compressed
tar file, uses epsf.tex | Nucl.Phys.Proc.Suppl. 41 (1995) 21-65 | 10.1016/0920-5632(95)00430-H | RU-94-91 | hep-th | null | Trieste Spring School Lectures describing the author's opinions about black
hole evaporation and information loss. The remnant, or cornucopion scenario for
the endpoint of Hawking evaporation is described in detail. In this picture
information can be lost to the original asymptotic observer without violating
the rule... | [
{
"created": "Thu, 15 Dec 1994 11:57:27 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Banks",
"Thomas",
"",
"Rutgers University"
]
] | Trieste Spring School Lectures describing the author's opinions about black hole evaporation and information loss. The remnant, or cornucopion scenario for the endpoint of Hawking evaporation is described in detail. In this picture information can be lost to the original asymptotic observer without violating the rules ... | 11.833528 | 12.829153 | 12.515961 | 11.028574 | 11.004554 | 12.082068 | 11.968779 | 11.391928 | 11.099192 | 13.179567 | 11.677615 | 10.637108 | 11.451414 | 10.718042 | 10.828674 | 10.926085 | 10.759611 | 10.7366 | 10.734895 | 10.990933 | 11.141492 |
hep-th/9308071 | Yoon-Bai Kim | B. K. Chung, K. G. Joo, and Soonkeon Nam | Hamiltonian formulation of SL(3) Ur-KdV equation | 12 pages, KHTP-93-03 SNUTP-93-21 | Mod.Phys.Lett.A8:2927-2936,1993 | 10.1142/S0217732393003342 | null | hep-th nlin.SI solv-int | null | We give a unified view of the relation between the $SL(2)$ KdV, the mKdV, and
the Ur-KdV equations through the Fr\'{e}chet derivatives and their inverses.
For this we introduce a new procedure of obtaining the Ur-KdV equation, where
we require that it has no non-local operators. We extend this method to the
$SL(3)$ K... | [
{
"created": "Mon, 16 Aug 1993 05:55:21 GMT",
"version": "v1"
}
] | 2010-02-05 | [
[
"Chung",
"B. K.",
""
],
[
"Joo",
"K. G.",
""
],
[
"Nam",
"Soonkeon",
""
]
] | We give a unified view of the relation between the $SL(2)$ KdV, the mKdV, and the Ur-KdV equations through the Fr\'{e}chet derivatives and their inverses. For this we introduce a new procedure of obtaining the Ur-KdV equation, where we require that it has no non-local operators. We extend this method to the $SL(3)$ KdV... | 10.012936 | 8.904507 | 10.291447 | 9.036598 | 8.707906 | 9.943974 | 8.831425 | 8.800401 | 9.673635 | 10.208423 | 9.171569 | 9.001263 | 9.824879 | 8.996113 | 9.250219 | 9.145543 | 9.261017 | 9.068389 | 9.225163 | 9.220809 | 8.965282 |
1808.09440 | Valeri Vardanyan | Yashar Akrami, Renata Kallosh, Andrei Linde, Valeri Vardanyan | The landscape, the swampland and the era of precision cosmology | 48 pages, 10 figures. v2: Improved version; discussions added, typos
fixed, structure modified, appendix added on two-field scenarios, note added
in response to arXiv:1809.00154. v3: Published version | Fortschr. Phys. 2018, 1800075 | 10.1002/prop.201800075 | null | hep-th astro-ph.CO gr-qc hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the advanced version of the KKLT construction and pure $d=4$ de
Sitter supergravity, involving a nilpotent multiplet, with regard to various
conjectures that de Sitter state cannot exist in string theory. We explain why
we consider these conjectures problematic and not well motivated, and why the
recently p... | [
{
"created": "Tue, 28 Aug 2018 17:55:08 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Sep 2018 16:42:25 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Oct 2018 11:08:20 GMT",
"version": "v3"
}
] | 2018-11-22 | [
[
"Akrami",
"Yashar",
""
],
[
"Kallosh",
"Renata",
""
],
[
"Linde",
"Andrei",
""
],
[
"Vardanyan",
"Valeri",
""
]
] | We review the advanced version of the KKLT construction and pure $d=4$ de Sitter supergravity, involving a nilpotent multiplet, with regard to various conjectures that de Sitter state cannot exist in string theory. We explain why we consider these conjectures problematic and not well motivated, and why the recently pro... | 12.113865 | 10.840086 | 12.720776 | 10.729324 | 11.596064 | 11.680561 | 12.30552 | 10.506161 | 10.512931 | 13.369524 | 10.738466 | 10.25394 | 10.306858 | 10.538378 | 10.303646 | 10.380164 | 10.43349 | 10.169574 | 10.402204 | 10.937827 | 9.886737 |
hep-th/0610105 | Piotr Korcyl | Piotr Korcyl | Classical trajectories and quantum supersymmetry | 16 pages, 12 figures, 5 tables, some misspellings corrected | Phys.Rev.D74:115012,2006 | 10.1103/PhysRevD.74.115012 | TPJU-14/2006 | hep-th | null | We analyze a supersymmetric system with four flat directions. We observe
several interesting properties, such as the coexistence of the discrete and
continuous spectrum in the same range of energies. We also solve numerically
the classical counterpart of this system. A similar analysis is then done for
an alike, but ... | [
{
"created": "Mon, 9 Oct 2006 22:30:01 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Nov 2006 20:17:34 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Korcyl",
"Piotr",
""
]
] | We analyze a supersymmetric system with four flat directions. We observe several interesting properties, such as the coexistence of the discrete and continuous spectrum in the same range of energies. We also solve numerically the classical counterpart of this system. A similar analysis is then done for an alike, but no... | 14.162918 | 13.727289 | 14.067173 | 13.413367 | 13.363262 | 14.213473 | 13.236611 | 13.265488 | 12.808389 | 13.724553 | 13.494044 | 13.789489 | 13.961918 | 13.285393 | 13.166486 | 13.184482 | 12.846943 | 13.104033 | 13.156513 | 13.494369 | 12.731936 |
hep-th/9502162 | D'Hoker | Eric D'Hoker | Invariant Effective Actions, Cohomology of Homogeneous Spaces and
Anomalies | 30 pages, Plain TeX, no figures. | Nucl.Phys. B451 (1995) 725-748 | 10.1016/0550-3213(95)00265-T | UCLA/95/TEP/5 | hep-th hep-ph | null | We construct the most general local effective actions for Goldstone boson
fields associated with spontaneous symmetry breakdown from a group $G$ to a
subgroup $H$. In a preceding paper, it was shown that any $G$-invariant term in
the action, which results from a non-invariant Lagrangian density, corresponds
to a non-... | [
{
"created": "Tue, 28 Feb 1995 02:28:40 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"D'Hoker",
"Eric",
""
]
] | We construct the most general local effective actions for Goldstone boson fields associated with spontaneous symmetry breakdown from a group $G$ to a subgroup $H$. In a preceding paper, it was shown that any $G$-invariant term in the action, which results from a non-invariant Lagrangian density, corresponds to a non-tr... | 7.37827 | 8.155447 | 8.332219 | 7.957082 | 8.119126 | 8.592793 | 8.322175 | 8.008409 | 7.467719 | 8.922072 | 7.333659 | 7.461326 | 7.597789 | 7.376754 | 7.689608 | 7.760254 | 7.453562 | 7.547502 | 7.522373 | 7.500164 | 7.463273 |
0808.1815 | Dionisio Bazeia | D. Bazeia, A.R. Gomes, L. Losano, R. Menezes | Braneworld Models of Scalar Fields with Generalized Dynamics | 10 pages, 8 figures; version to appear in PLB | Phys.Lett.B671:402-410,2009 | 10.1016/j.physletb.2008.12.039 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work deals with braneworld models driven by real scalar fields with
nonstandard dynamics. We develop the first-order formalism for models with
standard gravity but with the scalar fields having generalized dynamics. We
illustrate the results with examples of current interest, and we find
analytical and numerical... | [
{
"created": "Wed, 13 Aug 2008 12:07:37 GMT",
"version": "v1"
},
{
"created": "Sat, 4 Oct 2008 13:21:14 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Dec 2008 11:58:59 GMT",
"version": "v3"
}
] | 2009-01-29 | [
[
"Bazeia",
"D.",
""
],
[
"Gomes",
"A. R.",
""
],
[
"Losano",
"L.",
""
],
[
"Menezes",
"R.",
""
]
] | This work deals with braneworld models driven by real scalar fields with nonstandard dynamics. We develop the first-order formalism for models with standard gravity but with the scalar fields having generalized dynamics. We illustrate the results with examples of current interest, and we find analytical and numerical s... | 15.173494 | 9.121446 | 13.131584 | 10.380324 | 9.215837 | 9.185529 | 8.489347 | 8.942984 | 9.514157 | 14.199444 | 11.323804 | 12.98397 | 14.342369 | 13.352879 | 13.014935 | 12.607823 | 12.78764 | 13.795053 | 13.696575 | 14.27629 | 13.448164 |
2309.07769 | Xi Tong | David Stefanyszyn, Xi Tong, and Yuhang Zhu | Cosmological Correlators Through the Looking Glass: Reality, Parity, and
Factorisation | 67 pages, 7 figures, v2: 70 pages, 9 figures, more discussions added | null | 10.1007/JHEP05(2024)196 | null | hep-th astro-ph.CO gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We consider the evolution of quantum fields during inflation, and show that
the total-energy singularities appearing in the perturbative expansion of the
late-time Wavefunction of the Universe are purely real when the external states
are massless scalars and massless gravitons. Our proof relies on the tree-level
appr... | [
{
"created": "Thu, 14 Sep 2023 14:59:55 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jun 2024 08:37:00 GMT",
"version": "v2"
}
] | 2024-06-11 | [
[
"Stefanyszyn",
"David",
""
],
[
"Tong",
"Xi",
""
],
[
"Zhu",
"Yuhang",
""
]
] | We consider the evolution of quantum fields during inflation, and show that the total-energy singularities appearing in the perturbative expansion of the late-time Wavefunction of the Universe are purely real when the external states are massless scalars and massless gravitons. Our proof relies on the tree-level approx... | 12.453385 | 13.66269 | 13.394023 | 12.221381 | 13.250366 | 12.820653 | 12.4317 | 12.376778 | 12.279747 | 14.434594 | 12.292665 | 12.381839 | 12.763608 | 12.319399 | 12.415174 | 12.715972 | 12.542577 | 12.523157 | 12.304772 | 12.958277 | 12.045957 |
hep-th/0405025 | Claude Bervillier | C. Bervillier | The Wilson-Polchinski exact renormalization group equation | Some minor changes, a reference added, typos corrected | Phys.Lett.A332:93-100,2004 | 10.1016/j.physleta.2004.09.037 | T04/058 | hep-th cond-mat.other | null | The critical exponent $\eta $ is not well accounted for in the Polchinski
exact formulation of the renormalization group (RG). With a particular emphasis
laid on the introduction of the critical exponent $\eta $, I re-establish
(after Golner, hep-th/9801124) the explicit relation between the early Wilson
exact RG equ... | [
{
"created": "Tue, 4 May 2004 08:47:31 GMT",
"version": "v1"
},
{
"created": "Wed, 26 May 2004 14:38:58 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Bervillier",
"C.",
""
]
] | The critical exponent $\eta $ is not well accounted for in the Polchinski exact formulation of the renormalization group (RG). With a particular emphasis laid on the introduction of the critical exponent $\eta $, I re-establish (after Golner, hep-th/9801124) the explicit relation between the early Wilson exact RG equat... | 16.805157 | 16.094711 | 17.927952 | 14.773666 | 16.781971 | 15.814986 | 16.200132 | 16.299755 | 14.496065 | 19.060652 | 15.237619 | 15.345278 | 16.729988 | 15.479842 | 16.150499 | 15.349782 | 15.636848 | 15.205045 | 15.248954 | 16.352978 | 15.574456 |
2306.00865 | Ilarion Melnikov | Peng Cheng, Ilarion V. Melnikov, and Ruben Minasian | Flat F-theory and friends | 26 pages; typos fixed, comments added, discussion of T-duality
clarified | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We discuss F-theory backgrounds associated to flat torus bundles over
Ricci-flat manifolds. In this setting the F-theory background can be understood
as a IIB orientifold with a large radius limit described by a supersymmetric
compactification of IIB supergravity on a smooth, Ricci flat, but in general
non-spin geome... | [
{
"created": "Thu, 1 Jun 2023 16:24:14 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Nov 2023 15:51:24 GMT",
"version": "v2"
}
] | 2023-11-23 | [
[
"Cheng",
"Peng",
""
],
[
"Melnikov",
"Ilarion V.",
""
],
[
"Minasian",
"Ruben",
""
]
] | We discuss F-theory backgrounds associated to flat torus bundles over Ricci-flat manifolds. In this setting the F-theory background can be understood as a IIB orientifold with a large radius limit described by a supersymmetric compactification of IIB supergravity on a smooth, Ricci flat, but in general non-spin geometr... | 10.767066 | 11.071932 | 14.087121 | 9.406052 | 10.55032 | 10.178321 | 10.45474 | 10.117023 | 10.06109 | 15.173604 | 9.442335 | 9.798798 | 11.229969 | 9.721435 | 10.077332 | 10.038986 | 10.207687 | 9.735143 | 9.831522 | 10.61751 | 9.436268 |
1210.6164 | Adriano Lana Cherchiglia | A. L. Cherchiglia, L. A. Cabral, M. C. Nemes, Marcos Sampaio | (Un)determined finite regularization dependent quantum corrections: the
Higgs decay into two photons and the two photon scattering examples | Version accepted for publication at Phys. Rev. D | Phys.Rev. D87 (2013) 065011 | 10.1103/PhysRevD.87.065011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the appearance of arbitrary, regularization dependent
parameters introduced by divergent integrals in two a priori finite but
superficially divergent amplitudes: the Higgs decay into two photons and the
two photon scattering. We use a general parametrization of ultraviolet
divergences which makes expli... | [
{
"created": "Tue, 23 Oct 2012 08:43:24 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Mar 2013 10:27:32 GMT",
"version": "v2"
}
] | 2013-03-19 | [
[
"Cherchiglia",
"A. L.",
""
],
[
"Cabral",
"L. A.",
""
],
[
"Nemes",
"M. C.",
""
],
[
"Sampaio",
"Marcos",
""
]
] | We investigate the appearance of arbitrary, regularization dependent parameters introduced by divergent integrals in two a priori finite but superficially divergent amplitudes: the Higgs decay into two photons and the two photon scattering. We use a general parametrization of ultraviolet divergences which makes explici... | 11.478106 | 10.523941 | 11.03927 | 10.666348 | 10.800748 | 11.024723 | 11.216937 | 10.874336 | 10.148279 | 11.01569 | 10.493354 | 10.879159 | 11.162524 | 11.014177 | 11.222611 | 11.004405 | 11.01576 | 11.275849 | 10.872404 | 11.561391 | 11.297692 |
hep-th/0111286 | Grigorii Pivovarov | Grigorii B. Pivovarov and James P. Vary | A Non-Abelian Fourier Transform for Gauge Theories | 12 pages | Phys.Rev. D65 (2002) 125004 | 10.1103/PhysRevD.65.125004 | null | hep-th | null | We consider SU(2) gauge potentials over a space with a compactified
dimension. A non-Abelian Fourier transform of the gauge potential in the
compactified dimension is defined in such a way that the Fourier coefficients
are (almost) gauge invariant. The functional measure and the gauge field
strengths are expressed in... | [
{
"created": "Fri, 30 Nov 2001 13:31:00 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Pivovarov",
"Grigorii B.",
""
],
[
"Vary",
"James P.",
""
]
] | We consider SU(2) gauge potentials over a space with a compactified dimension. A non-Abelian Fourier transform of the gauge potential in the compactified dimension is defined in such a way that the Fourier coefficients are (almost) gauge invariant. The functional measure and the gauge field strengths are expressed in t... | 6.916317 | 7.28472 | 6.973377 | 7.257744 | 7.111747 | 7.252684 | 6.708833 | 6.66995 | 6.824924 | 7.544507 | 6.939951 | 6.934817 | 6.860134 | 6.733522 | 6.839556 | 6.754887 | 6.867571 | 6.684364 | 6.93643 | 6.863057 | 6.805407 |
2006.06022 | Max Guillen | Max Guillen | Notes on the 11D pure spinor wordline vertex operators | 16 pages. Added reference. Small modification to the published
version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The construction of the ghost number zero and one vertex operators for the
11D pure spinor superparticle will be revisited. In this sense, an alternative
way of defining the ghost number one vertex operator will be given after
introducing a ghost number -2 operator made out of physical operators defined
on the 11D no... | [
{
"created": "Wed, 10 Jun 2020 18:15:56 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Aug 2020 03:56:22 GMT",
"version": "v2"
},
{
"created": "Tue, 27 Dec 2022 23:49:33 GMT",
"version": "v3"
}
] | 2022-12-29 | [
[
"Guillen",
"Max",
""
]
] | The construction of the ghost number zero and one vertex operators for the 11D pure spinor superparticle will be revisited. In this sense, an alternative way of defining the ghost number one vertex operator will be given after introducing a ghost number -2 operator made out of physical operators defined on the 11D non-... | 11.654493 | 10.156417 | 12.423048 | 10.445212 | 10.881566 | 10.358974 | 9.962515 | 10.092711 | 10.552078 | 13.680564 | 10.002454 | 10.484877 | 12.031006 | 11.179404 | 11.013213 | 10.537144 | 10.506384 | 11.087658 | 10.893432 | 12.081746 | 10.50113 |
hep-th/9406172 | Ulrich Meyer | Ulrich Meyer | Quantum determinants | 5 pages | null | null | DAMTP/94-54 | hep-th math.QA | null | We show how to construct central and grouplike quantum determinants for FRT
algebras A(R). As an application of the general construction we give a quantum
determinant for the q-Lorentz group.
| [
{
"created": "Sun, 26 Jun 1994 14:23:04 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Meyer",
"Ulrich",
""
]
] | We show how to construct central and grouplike quantum determinants for FRT algebras A(R). As an application of the general construction we give a quantum determinant for the q-Lorentz group. | 16.129698 | 15.243814 | 19.164957 | 15.625713 | 19.304966 | 16.630363 | 18.7314 | 18.791414 | 17.108627 | 18.439257 | 15.627975 | 16.838493 | 16.704142 | 15.555152 | 17.493073 | 16.768164 | 15.675419 | 17.289322 | 15.804556 | 16.608643 | 14.874702 |
1810.10189 | Bo-Qiang Ma | Hefu Yu, Bo-Qiang Ma | Origin of fermion generations from extended noncommutative geometry | 17 latex pages, no figure. Final version for publication | Int. J. Mod. Phys. A 33 (2018) 1850168 | 10.1142/S0217751X18501683 | null | hep-th gr-qc hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a way to understand the 3 fermion generations by the algebraic
structures of noncommutative geometry, which is a promising framework to unify
the standard model and general relativity. We make the tensor product extension
and the quaternion extension on the framework. Each of the two extensions alone
keeps... | [
{
"created": "Wed, 24 Oct 2018 05:11:34 GMT",
"version": "v1"
}
] | 2018-10-30 | [
[
"Yu",
"Hefu",
""
],
[
"Ma",
"Bo-Qiang",
""
]
] | We propose a way to understand the 3 fermion generations by the algebraic structures of noncommutative geometry, which is a promising framework to unify the standard model and general relativity. We make the tensor product extension and the quaternion extension on the framework. Each of the two extensions alone keeps t... | 13.592577 | 14.828201 | 12.694654 | 12.265227 | 13.859655 | 14.704899 | 14.815868 | 13.514041 | 13.316032 | 15.156993 | 13.433814 | 14.268007 | 13.752181 | 13.332796 | 13.393525 | 13.911798 | 13.971539 | 13.501942 | 13.033401 | 13.292265 | 13.466681 |
2205.01765 | Osvaldo Chandia | Osvaldo Chandia, Brenno Carlini Vallilo | Superspaces for heterotic pure spinor string compactifications | 19 pages, latex | null | 10.1140/epjc/s10052-022-10947-0 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study supersymmetry conditions for the heterotic pure superstring
preserving and N=1 supersymmetry in four dimensions directly from the curved
superspace defined by the Berkovits-Howe constraints.
| [
{
"created": "Tue, 3 May 2022 20:19:18 GMT",
"version": "v1"
}
] | 2022-11-08 | [
[
"Chandia",
"Osvaldo",
""
],
[
"Vallilo",
"Brenno Carlini",
""
]
] | We study supersymmetry conditions for the heterotic pure superstring preserving and N=1 supersymmetry in four dimensions directly from the curved superspace defined by the Berkovits-Howe constraints. | 21.120203 | 17.129921 | 22.529144 | 16.844545 | 15.002684 | 18.01358 | 19.716475 | 18.103741 | 18.322979 | 26.68503 | 20.866167 | 18.73827 | 21.484953 | 17.998983 | 19.556881 | 17.104231 | 19.947027 | 18.501366 | 18.182503 | 20.860502 | 17.344618 |
hep-th/9810257 | Anton Kapustin | Micha Berkooz and Anton Kapustin | New IR Dualities in Supersymmetric Gauge Theory in Three Dimensions | 15 pages, harvmac, 1 embedded ps figure; a reference has been added | JHEP 9902 (1999) 009 | 10.1088/1126-6708/1999/02/009 | IASSNS-HEP-98/89 | hep-th | null | We present nontrivial examples of d=3 gauge theories with sixteen and eight
supercharges which are infrared dual at special points in the moduli space.
This duality is distinct from mirror symmetry. To demonstrate duality we
construct the gauge theories of interest using D2-branes and orientifolds and
then consider t... | [
{
"created": "Fri, 30 Oct 1998 21:48:14 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Nov 1998 14:45:51 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Berkooz",
"Micha",
""
],
[
"Kapustin",
"Anton",
""
]
] | We present nontrivial examples of d=3 gauge theories with sixteen and eight supercharges which are infrared dual at special points in the moduli space. This duality is distinct from mirror symmetry. To demonstrate duality we construct the gauge theories of interest using D2-branes and orientifolds and then consider the... | 11.16455 | 9.174403 | 13.748968 | 9.028582 | 9.174541 | 10.515679 | 10.471793 | 9.492777 | 8.901909 | 11.382067 | 9.846512 | 10.115974 | 11.216732 | 9.557782 | 10.287649 | 9.938563 | 9.829885 | 10.002294 | 9.663688 | 12.286265 | 9.918674 |
2202.08290 | Yi Pang | Liang Ma, Yi Pang, H. Lu | Improved Wald formalism and First Law of Dyonic Black Strings with Mixed
Chern-Simons Terms | Latex, 27 pages, adding discussions on attractor mechanism, to appear
in JHEP | JHEP10(2022)142 | 10.1007/JHEP10(2022)142 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the first law of thermodynamics of dyonic black strings carrying a
linear momentum in type IIA string theory compactified on K3 with leading order
$\alpha'$ corrections. The low energy effective action contains mixed
Chern-Simons terms of the form $-2B_{(2)}\wedge {\rm tr}(R(\Gamma_\pm)\wedge
R(\Gamma_\pm))$... | [
{
"created": "Wed, 16 Feb 2022 19:00:10 GMT",
"version": "v1"
},
{
"created": "Tue, 24 May 2022 23:41:08 GMT",
"version": "v2"
},
{
"created": "Mon, 10 Oct 2022 01:44:15 GMT",
"version": "v3"
}
] | 2022-10-24 | [
[
"Ma",
"Liang",
""
],
[
"Pang",
"Yi",
""
],
[
"Lu",
"H.",
""
]
] | We study the first law of thermodynamics of dyonic black strings carrying a linear momentum in type IIA string theory compactified on K3 with leading order $\alpha'$ corrections. The low energy effective action contains mixed Chern-Simons terms of the form $-2B_{(2)}\wedge {\rm tr}(R(\Gamma_\pm)\wedge R(\Gamma_\pm))$ w... | 7.059895 | 7.56673 | 7.385962 | 7.059864 | 7.349485 | 7.863817 | 7.817573 | 7.217569 | 7.016209 | 7.500061 | 6.852986 | 7.069576 | 7.128489 | 6.961809 | 6.917199 | 7.150167 | 6.841829 | 6.975417 | 6.96864 | 7.189304 | 7.008852 |
0808.1114 | Matthias Kaminski | Matthias Kaminski | Holographic quark gluon plasma with flavor | 45 figures, 166 pages | Fortsch.Phys.57:3-148,2009 | 10.1002/prop.200810571 | MPP-2008-94 | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work I explore theoretical and phenomenological implications of
chemical potentials and charge densities inside a strongly coupled thermal
plasma, using the gauge/gravity correspondence. Strong coupling effects
discovered in this model theory are interpreted geometrically and may be taken
as qualitative predi... | [
{
"created": "Thu, 7 Aug 2008 20:26:42 GMT",
"version": "v1"
}
] | 2009-07-22 | [
[
"Kaminski",
"Matthias",
""
]
] | In this work I explore theoretical and phenomenological implications of chemical potentials and charge densities inside a strongly coupled thermal plasma, using the gauge/gravity correspondence. Strong coupling effects discovered in this model theory are interpreted geometrically and may be taken as qualitative predict... | 12.714799 | 13.01972 | 11.91321 | 11.795527 | 13.084347 | 12.968392 | 13.490998 | 12.347398 | 12.08781 | 12.895798 | 12.397298 | 12.0353 | 11.539256 | 11.636992 | 12.26967 | 12.042237 | 11.968779 | 11.83602 | 11.923538 | 11.807361 | 11.732537 |
hep-th/0502162 | Gregory Jones | Dumitru Astefanesei, Gregory C. Jones | S-branes and (Anti-)Bubbles in (A)dS Space | 35 pages, 12 figures. V2: JHEP style, expanded references | JHEP 0506 (2005) 037 | 10.1088/1126-6708/2005/06/037 | HUTP-05/A0007 | hep-th | null | We describe the construction of new locally asymptotically (A)dS geometries
with relevance for the AdS/CFT and dS/CFT correspondences. Our approach is to
obtain new solutions by analytically continuing black hole solutions. A basic
consideration of the method of continuation indicates that these solutions come
in thr... | [
{
"created": "Thu, 17 Feb 2005 22:00:14 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Mar 2005 16:37:49 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Astefanesei",
"Dumitru",
""
],
[
"Jones",
"Gregory C.",
""
]
] | We describe the construction of new locally asymptotically (A)dS geometries with relevance for the AdS/CFT and dS/CFT correspondences. Our approach is to obtain new solutions by analytically continuing black hole solutions. A basic consideration of the method of continuation indicates that these solutions come in three... | 15.499415 | 14.318579 | 15.339593 | 13.24663 | 12.188737 | 12.671988 | 13.708041 | 12.579201 | 13.339699 | 16.211382 | 13.191371 | 13.575356 | 13.974544 | 13.017508 | 13.334977 | 13.303973 | 13.332638 | 13.466845 | 12.829307 | 14.466825 | 13.316683 |
2011.13870 | Jakob Salzer | Daniel Grumiller, Jelle Hartong, Stefan Prohazka, Jakob Salzer | Limits of JT gravity | 41 pages, 3 figures, 1 table; v2: Matches published version +
Footnote 11; v3: Corrected typo in Carrollian/Galilean generalized dilaton
potential | JHEP 02 (2021) 134 | 10.1007/JHEP02(2021)134 | TUW--20--05 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct various limits of JT gravity, including Newton-Cartan and
Carrollian versions of dilaton gravity in two dimensions as well as a theory on
the three-dimensional light cone. In the BF formulation our boundary conditions
relate boundary connection with boundary scalar, yielding as boundary action
the partic... | [
{
"created": "Fri, 27 Nov 2020 17:50:58 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Mar 2021 11:48:00 GMT",
"version": "v2"
},
{
"created": "Fri, 4 Feb 2022 10:47:13 GMT",
"version": "v3"
}
] | 2022-02-07 | [
[
"Grumiller",
"Daniel",
""
],
[
"Hartong",
"Jelle",
""
],
[
"Prohazka",
"Stefan",
""
],
[
"Salzer",
"Jakob",
""
]
] | We construct various limits of JT gravity, including Newton-Cartan and Carrollian versions of dilaton gravity in two dimensions as well as a theory on the three-dimensional light cone. In the BF formulation our boundary conditions relate boundary connection with boundary scalar, yielding as boundary action the particle... | 28.957142 | 26.956249 | 29.676113 | 25.112513 | 27.425007 | 25.709326 | 27.598446 | 25.093063 | 23.821573 | 34.287029 | 25.609016 | 25.620321 | 29.114202 | 27.286379 | 26.106022 | 24.785244 | 27.153872 | 25.412354 | 26.430496 | 28.516781 | 25.538465 |
1310.6006 | Mads Sogaard | Mads Sogaard, Yang Zhang | Multivariate Residues and Maximal Unitarity | 34 pages, 3 figures | JHEP 1312 (2013) 008 | 10.1007/JHEP12(2013)008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the maximal unitarity method to amplitude contributions whose cuts
define multidimensional algebraic varieties. The technique is valid to all
orders and is explicitly demonstrated at three loops in gauge theories with any
number of fermions and scalars in the adjoint representation. Deca-cuts
realized by re... | [
{
"created": "Tue, 22 Oct 2013 18:41:29 GMT",
"version": "v1"
}
] | 2014-06-20 | [
[
"Sogaard",
"Mads",
""
],
[
"Zhang",
"Yang",
""
]
] | We extend the maximal unitarity method to amplitude contributions whose cuts define multidimensional algebraic varieties. The technique is valid to all orders and is explicitly demonstrated at three loops in gauge theories with any number of fermions and scalars in the adjoint representation. Deca-cuts realized by repl... | 23.260229 | 23.906679 | 25.42499 | 19.835169 | 21.558601 | 23.830072 | 23.431849 | 22.567007 | 21.321562 | 24.460812 | 19.960991 | 21.955587 | 21.636755 | 21.547377 | 22.905695 | 22.400782 | 22.871599 | 21.016455 | 21.074446 | 22.589727 | 21.104704 |
1503.01462 | Taro Kimura | Taro Kimura | Linking loops in ABJM and refined theory | 1+24 pages; references added, typos corrected | JHEP 07 (2015) 030 | 10.1007/JHEP07(2015)030 | IPHT-T15/020, RIKEN-MP-110 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the link average of the half-BPS Wilson loop operators in N = 6
superconformal Chern-Simons-matter theory, which is called ABJM theory. We show
that this loop average is reduced to a (super)matrix integral by the
localization method, in a similar way to the bosonic U(N) Chern-Simons theory.
Using this mat... | [
{
"created": "Wed, 4 Mar 2015 21:00:10 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Jun 2015 13:00:23 GMT",
"version": "v2"
}
] | 2015-07-15 | [
[
"Kimura",
"Taro",
""
]
] | We consider the link average of the half-BPS Wilson loop operators in N = 6 superconformal Chern-Simons-matter theory, which is called ABJM theory. We show that this loop average is reduced to a (super)matrix integral by the localization method, in a similar way to the bosonic U(N) Chern-Simons theory. Using this matri... | 7.189952 | 7.675223 | 9.881159 | 7.501184 | 7.840126 | 7.473542 | 7.866088 | 7.348517 | 7.365192 | 9.588339 | 7.430072 | 7.13366 | 8.440378 | 7.338245 | 7.177837 | 6.801521 | 7.385216 | 7.037457 | 7.329275 | 8.125678 | 7.503071 |
2212.07901 | Sven Bjarke Gudnason | Johan Bijnens, Sven Bjarke Gudnason, Jiahui Yu, Tiantian Zhang | Hilbert series and higher-order Lagrangians for the $O(N)$ model | LaTeX: 26+32 pages, 17 tables; V2: published version | JHEP 2305:61, 2023 | 10.1007/JHEP05(2023)061 | LU TP 22-65 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compare the Hilbert series approach with explicit constructions of
higher-order Lagrangians for the $O(N)$ nonlinear sigma model. We use the
Hilbert series to find the number and type of operators up to mass dimension
16, for spacetime dimension $D$ up to 12 and $N$ up to 12, and further classify
the operators int... | [
{
"created": "Thu, 15 Dec 2022 15:36:26 GMT",
"version": "v1"
},
{
"created": "Wed, 10 May 2023 07:44:09 GMT",
"version": "v2"
}
] | 2023-05-12 | [
[
"Bijnens",
"Johan",
""
],
[
"Gudnason",
"Sven Bjarke",
""
],
[
"Yu",
"Jiahui",
""
],
[
"Zhang",
"Tiantian",
""
]
] | We compare the Hilbert series approach with explicit constructions of higher-order Lagrangians for the $O(N)$ nonlinear sigma model. We use the Hilbert series to find the number and type of operators up to mass dimension 16, for spacetime dimension $D$ up to 12 and $N$ up to 12, and further classify the operators into ... | 9.61209 | 11.917897 | 8.873556 | 8.827892 | 10.362106 | 10.682441 | 10.445275 | 9.565763 | 9.161446 | 10.10093 | 9.351366 | 9.834762 | 8.749803 | 8.846334 | 9.625687 | 9.370793 | 9.337551 | 9.195386 | 8.877215 | 8.540116 | 9.030974 |
hep-th/0407017 | Razvan Teodorescu | R. Teodorescu, E. Bettelheim, O. Agam, A. Zabrodin, P. Wiegmann | Semiclassical evolution of the spectral curve in the normal random
matrix ensemble as Whitham hierarchy | 14 pages | Nucl.Phys. B700 (2004) 521-532 | 10.1016/j.nuclphysb.2004.08.013 | null | hep-th cond-mat.mes-hall math-ph math.MP nlin.SI | null | We continue the analysis of the spectral curve of the normal random matrix
ensemble, introduced in an earlier paper. Evolution of the full quantum curve
is given in terms of compatibility equations of independent flows. The
semiclassical limit of these flows is expressed through canonical differential
forms of the sp... | [
{
"created": "Fri, 2 Jul 2004 16:43:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Teodorescu",
"R.",
""
],
[
"Bettelheim",
"E.",
""
],
[
"Agam",
"O.",
""
],
[
"Zabrodin",
"A.",
""
],
[
"Wiegmann",
"P.",
""
]
] | We continue the analysis of the spectral curve of the normal random matrix ensemble, introduced in an earlier paper. Evolution of the full quantum curve is given in terms of compatibility equations of independent flows. The semiclassical limit of these flows is expressed through canonical differential forms of the spec... | 13.41678 | 11.822419 | 16.868469 | 12.117172 | 13.103799 | 12.464816 | 14.141351 | 12.417496 | 12.273911 | 16.824348 | 12.901634 | 12.779911 | 13.693283 | 12.637913 | 12.988067 | 12.389727 | 12.399092 | 12.679598 | 12.962349 | 13.913824 | 12.508813 |
1508.02359 | Larry Ford | Christopher J. Fewster and L. H. Ford | Probability Distributions for Quantum Stress Tensors Measured in a
Finite Time Interval | 28 pages, 9 figures | Phys. Rev. D 92, 105008 (2015) | 10.1103/PhysRevD.92.105008 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A meaningful probability distribution for measurements of a quantum stress
tensor operator can only be obtained if the operator is averaged in time or in
spacetime. This averaging can be regarded as a description of the measurement
process. Realistic measurements can be expected to begin and end at finite
times, whic... | [
{
"created": "Mon, 10 Aug 2015 19:10:50 GMT",
"version": "v1"
}
] | 2015-11-11 | [
[
"Fewster",
"Christopher J.",
""
],
[
"Ford",
"L. H.",
""
]
] | A meaningful probability distribution for measurements of a quantum stress tensor operator can only be obtained if the operator is averaged in time or in spacetime. This averaging can be regarded as a description of the measurement process. Realistic measurements can be expected to begin and end at finite times, which ... | 9.483244 | 8.93634 | 9.478387 | 9.236672 | 9.224445 | 9.577625 | 9.789152 | 9.400548 | 9.148343 | 10.471125 | 8.917518 | 9.21024 | 9.064372 | 9.008125 | 9.29887 | 9.444942 | 9.15202 | 9.286061 | 9.23258 | 9.247996 | 8.844693 |
hep-th/9605215 | null | Francesco Fucito and Gabriele Travaglini | Instanton Calculus and Nonperturbative Relations in N=2 Supersymmetric
Gauge Theories | 18 pages, latex file, no figures | Phys.Rev. D55 (1997) 1099-1104 | 10.1103/PhysRevD.55.1099 | ROM2F-96-32 | hep-th | null | Using instanton calculus we check, in the weak coupling region, the
nonperturbative relation $$ <\Tr\phi^2>=i\pi\left(\cf-{a\over 2}
{\partial\cf\over\partial a}\right)$$ obtained for a N=2 globally
supersymmetric gauge theory. Our computations are performed for instantons of
winding number k, up to k=2 and turn out ... | [
{
"created": "Thu, 30 May 1996 14:28:28 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Fucito",
"Francesco",
""
],
[
"Travaglini",
"Gabriele",
""
]
] | Using instanton calculus we check, in the weak coupling region, the nonperturbative relation $$ <\Tr\phi^2>=i\pi\left(\cf-{a\over 2} {\partial\cf\over\partial a}\right)$$ obtained for a N=2 globally supersymmetric gauge theory. Our computations are performed for instantons of winding number k, up to k=2 and turn out to... | 12.514994 | 10.420575 | 11.596307 | 10.192719 | 10.782385 | 10.235578 | 11.743546 | 10.633982 | 10.922713 | 11.896012 | 10.308047 | 10.245456 | 11.428408 | 10.380127 | 10.426892 | 10.30513 | 10.1928 | 9.90865 | 10.454364 | 11.790991 | 10.033024 |
1410.1616 | Zheng-Wen Liu | Zheng-Wen Liu | Soft theorems in maximally supersymmetric theories | typos fixed, citations updated/added; 25+5 pages | Eur. Phys. J. C75 (2015) 105 | 10.1140/epjc/s10052-015-3304-1 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study the supersymmetric generalization of the new soft
theorem which was proposed by Cachazo and Strominger recently. At tree level,
we prove the validity of the super soft theorems in both ${\cal N}=4$
super-Yang-Mills theory and ${\cal N}=8$ supergravity using super-BCFW
recursion relations. We ve... | [
{
"created": "Tue, 7 Oct 2014 05:01:27 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Nov 2014 12:44:56 GMT",
"version": "v2"
},
{
"created": "Sun, 8 Mar 2015 14:14:59 GMT",
"version": "v3"
}
] | 2015-03-10 | [
[
"Liu",
"Zheng-Wen",
""
]
] | In this paper we study the supersymmetric generalization of the new soft theorem which was proposed by Cachazo and Strominger recently. At tree level, we prove the validity of the super soft theorems in both ${\cal N}=4$ super-Yang-Mills theory and ${\cal N}=8$ supergravity using super-BCFW recursion relations. We veri... | 5.715795 | 4.947878 | 6.698845 | 4.805453 | 4.995077 | 4.917125 | 4.821985 | 5.154278 | 4.634582 | 5.810299 | 4.830698 | 4.818159 | 5.498139 | 5.264588 | 4.951883 | 5.146156 | 5.183285 | 4.916157 | 5.110016 | 5.65045 | 5.158961 |
hep-th/0110228 | Ali Havare | K.Sogut, A.Havare, I.Acikgoz | Energy Levels and Wave Functions of Vector Bosons in Homogeneous
Magnetic Field | 13 pages, no figures | J.Math.Phys.43:3952-3962,2002 | 10.1063/1.1489502 | null | hep-th | null | We aimed to obtain the energy levels of spin-1 particles moving in a constant
magnetic field. The method used here is completely algebraic. In the process to
obtain the energy levels the wave function is choosen in terms of Laguerre
Polynomials.
| [
{
"created": "Wed, 24 Oct 2001 22:48:03 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Sogut",
"K.",
""
],
[
"Havare",
"A.",
""
],
[
"Acikgoz",
"I.",
""
]
] | We aimed to obtain the energy levels of spin-1 particles moving in a constant magnetic field. The method used here is completely algebraic. In the process to obtain the energy levels the wave function is choosen in terms of Laguerre Polynomials. | 12.805892 | 11.031435 | 11.623248 | 11.52472 | 11.204101 | 10.938313 | 10.944487 | 11.632264 | 10.532962 | 11.17335 | 11.628199 | 11.958211 | 11.810026 | 11.467717 | 11.929211 | 11.608293 | 11.343222 | 12.402897 | 11.41223 | 11.439342 | 12.133578 |
hep-th/0603040 | Alexander A. Chernitskii | Alexander A. Chernitskii | Mass, spin, charge, and magnetic moment for electromagnetic particle | 5 pages, talk given at XI Advanced Research Workshop on High Energy
Spin Physics, September 27 - October 1, 2005, Dubna, Russia | XI Advanced Research Workshop on High Energy Spin Physics
(DUBNA-SPIN-05) Proceedings, edited by A.V. Efremov and S.V. Goloskokov,
JINR, Dubna, 2006, pp. 234-239. | null | null | hep-th | null | Electromagnetic particle is considered as appropriate particle solution of
nonlinear electrodynamics. Mass, spin, charge, and dipole moment for the
electromagnetic particle are defined. Classical motion equations for massive
charged particle with spin and dipole moment are obtained from integral
conservation laws for... | [
{
"created": "Mon, 6 Mar 2006 15:14:39 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Chernitskii",
"Alexander A.",
""
]
] | Electromagnetic particle is considered as appropriate particle solution of nonlinear electrodynamics. Mass, spin, charge, and dipole moment for the electromagnetic particle are defined. Classical motion equations for massive charged particle with spin and dipole moment are obtained from integral conservation laws for t... | 16.149334 | 13.40976 | 14.118625 | 14.201854 | 12.85539 | 13.587755 | 15.640443 | 14.239448 | 14.566388 | 17.680101 | 13.477952 | 13.26779 | 15.057765 | 14.380729 | 15.439523 | 14.057877 | 14.379697 | 13.616952 | 14.575715 | 15.510254 | 12.559044 |
hep-th/0108229 | Peter Mayr | P. Mayr | N=1 Mirror Symmetry and Open/Closed String Duality | harvmac, 29 pages (b), 3 figures; v2: references added | Adv.Theor.Math.Phys.5:213-242,2002 | null | CERN-TH/2001-230 | hep-th | null | We show that the exact N=1 superpotential of a class of 4d string
compactifications is computed by the closed topological string compactified to
two dimensions. A relation to the open topological string is used to define a
special geometry for N=1 mirror symmetry. Flat coordinates, an N=1 mirror map
for chiral multip... | [
{
"created": "Thu, 30 Aug 2001 19:21:32 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Nov 2001 21:09:25 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Mayr",
"P.",
""
]
] | We show that the exact N=1 superpotential of a class of 4d string compactifications is computed by the closed topological string compactified to two dimensions. A relation to the open topological string is used to define a special geometry for N=1 mirror symmetry. Flat coordinates, an N=1 mirror map for chiral multiple... | 9.710035 | 9.753343 | 12.118268 | 9.601128 | 10.943542 | 10.189624 | 10.184197 | 9.434972 | 9.610868 | 11.207137 | 9.801045 | 9.741395 | 10.408788 | 9.49918 | 9.640069 | 9.771218 | 9.588769 | 9.310649 | 9.500776 | 9.992723 | 9.311566 |
2207.09834 | Mohammad R. Garousi | Mohammad R. Garousi, Saman Karimi | Couplings of order six in the gauge field strength and the second
fundamental form on a D$_p$-brane at order $\alpha'^2$ | 27 pages, latex file, no figure; it appears in PRD | null | 10.1103/PhysRevD.106.066016 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the assumption that the independent gauge invariant couplings on the
world-volume of the non-perturbative objects in the string theory are
independent of the background, we find the four and the six gauge field
strength and/or the second fundamental form couplings on the world volume of a
D$_p$-brane in the sup... | [
{
"created": "Wed, 20 Jul 2022 11:40:29 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Sep 2022 04:38:54 GMT",
"version": "v2"
}
] | 2022-10-05 | [
[
"Garousi",
"Mohammad R.",
""
],
[
"Karimi",
"Saman",
""
]
] | Using the assumption that the independent gauge invariant couplings on the world-volume of the non-perturbative objects in the string theory are independent of the background, we find the four and the six gauge field strength and/or the second fundamental form couplings on the world volume of a D$_p$-brane in the super... | 12.431517 | 10.983517 | 12.197151 | 11.189839 | 10.849539 | 10.594787 | 11.055453 | 10.507539 | 10.751234 | 13.594745 | 10.012977 | 11.034765 | 12.005188 | 11.207539 | 11.193933 | 10.89626 | 11.271764 | 10.952655 | 11.103559 | 11.653543 | 11.109935 |
0909.3952 | Tsunehide Kuroki | Tsunehide Kuroki and Fumihiko Sugino | Spontaneous supersymmetry breaking in large-$N$ matrix models with
slowly varying potential | 46 pages, LaTeX | null | 10.1016/j.nuclphysb.2009.12.021 | OIQP-09-10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a class of matrix models, where supersymmetry (SUSY) is
spontaneously broken at the matrix size $N$ infinite. The models are obtained
by dimensional reduction of matrix-valued SUSY quantum mechanics. The potential
of the models is slowly varying, and the large-$N$ limit is taken with the
slowly varying l... | [
{
"created": "Tue, 22 Sep 2009 10:32:58 GMT",
"version": "v1"
}
] | 2015-05-14 | [
[
"Kuroki",
"Tsunehide",
""
],
[
"Sugino",
"Fumihiko",
""
]
] | We construct a class of matrix models, where supersymmetry (SUSY) is spontaneously broken at the matrix size $N$ infinite. The models are obtained by dimensional reduction of matrix-valued SUSY quantum mechanics. The potential of the models is slowly varying, and the large-$N$ limit is taken with the slowly varying lim... | 9.068877 | 9.336506 | 9.592155 | 8.9584 | 9.581149 | 9.777027 | 9.626606 | 9.360474 | 8.908673 | 10.206099 | 9.043843 | 8.997885 | 8.65729 | 8.756775 | 8.881976 | 9.157803 | 9.105408 | 8.886378 | 8.762665 | 9.119534 | 8.777146 |
2003.01056 | Rolf Schimmrigk | Rolf Schimmrigk | Flux vacua and modularity | 24 pages; extended version, added references, typos corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Geometric modularity has recently been conjectured to be a characteristic
feature for flux vacua with $W=0$. This paper provides support for the
conjecture by computing motivic modular forms in a direct way for several
string compactifications for which such vacua are known to exist. The analysis
of some Calabi-Yau m... | [
{
"created": "Mon, 2 Mar 2020 17:42:06 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Oct 2020 05:35:58 GMT",
"version": "v2"
}
] | 2020-10-08 | [
[
"Schimmrigk",
"Rolf",
""
]
] | Geometric modularity has recently been conjectured to be a characteristic feature for flux vacua with $W=0$. This paper provides support for the conjecture by computing motivic modular forms in a direct way for several string compactifications for which such vacua are known to exist. The analysis of some Calabi-Yau man... | 10.985269 | 9.679899 | 11.63535 | 9.949422 | 9.959044 | 9.71026 | 9.523272 | 9.2019 | 9.216149 | 11.24762 | 9.402663 | 8.444141 | 9.985048 | 8.788217 | 8.934479 | 8.997145 | 9.347912 | 8.863678 | 9.066454 | 9.282555 | 10.124494 |
1504.07556 | Valentina Petkova | P. Furlan and V.B. Petkova | On some 3-point functions in the $W_4$ CFT and related braiding matrix | 27 pages, TeX with harvmac; v2: Content substantially extended, new
references added | null | 10.1007/JHEP12(2015)079 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a class of 3-point constants in the $sl(4)$ Toda conformal
theory $W_4$, extending the examples in Fateev and Litvinov. Their knowledge
allows to determine the braiding/fusing matrix transforming 4-point conformal
blocks of one fundamental, labelled by the 6-dimensional $sl(4)$
representation, and three ... | [
{
"created": "Tue, 28 Apr 2015 16:28:07 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Oct 2015 17:34:12 GMT",
"version": "v2"
}
] | 2016-01-27 | [
[
"Furlan",
"P.",
""
],
[
"Petkova",
"V. B.",
""
]
] | We construct a class of 3-point constants in the $sl(4)$ Toda conformal theory $W_4$, extending the examples in Fateev and Litvinov. Their knowledge allows to determine the braiding/fusing matrix transforming 4-point conformal blocks of one fundamental, labelled by the 6-dimensional $sl(4)$ representation, and three pa... | 14.556868 | 16.06587 | 17.42305 | 14.383922 | 14.1443 | 16.327406 | 14.207253 | 15.192466 | 14.831129 | 20.740253 | 15.057195 | 13.859834 | 15.194242 | 13.961129 | 14.718108 | 14.418682 | 14.207194 | 13.705391 | 13.943283 | 15.086297 | 14.127463 |
2202.05116 | Eugenia Colafranceschi | Eugenia Colafranceschi and Gerardo Adesso | Holographic entanglement in spin network states: a focused review | 16 pages, 15 figures | AVS Quantum Sci. 4, 025901 (2022) | 10.1116/5.0087122 | null | hep-th cond-mat.stat-mech math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the long-standing quest to reconcile gravity with quantum mechanics,
profound connections have been unveiled between concepts traditionally
pertaining to quantum information theory, such as entanglement, and
constitutive features of gravity, like holography. Developing and promoting
these connections from the conc... | [
{
"created": "Thu, 10 Feb 2022 16:06:45 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Jun 2022 13:01:37 GMT",
"version": "v2"
}
] | 2022-06-28 | [
[
"Colafranceschi",
"Eugenia",
""
],
[
"Adesso",
"Gerardo",
""
]
] | In the long-standing quest to reconcile gravity with quantum mechanics, profound connections have been unveiled between concepts traditionally pertaining to quantum information theory, such as entanglement, and constitutive features of gravity, like holography. Developing and promoting these connections from the concep... | 11.520894 | 13.141259 | 12.191577 | 11.1456 | 12.364252 | 12.892987 | 12.321661 | 11.175522 | 11.635905 | 11.937593 | 11.239175 | 11.421898 | 11.449126 | 10.960096 | 11.251573 | 11.1942 | 11.306609 | 11.269042 | 11.315838 | 11.354378 | 11.109625 |
hep-th/9909182 | Axel Krause | Axel Krause (Humboldt U., Berlin) | Testing Stability of M-Theory on an S^1/Z_2 Orbifold | 30 pages, 5 figures, several minor corrections and clarifications | JHEP 0005:046,2000 | 10.1088/1126-6708/2000/05/046 | HUB-EP-99/54 | hep-th | null | We analyse perturbatively, whether a flat background with vanishing G-flux in
Horava-Witten supergravity represents a vacuum state, which is stable with
respect to interactions between the ten-dimensional boundaries, mediated
through the D=11 supergravity bulk fields. For this, we consider fluctuations
in the gravito... | [
{
"created": "Mon, 27 Sep 1999 12:19:20 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Dec 1999 16:00:33 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Jun 2000 12:23:53 GMT",
"version": "v3"
}
] | 2010-02-03 | [
[
"Krause",
"Axel",
"",
"Humboldt U., Berlin"
]
] | We analyse perturbatively, whether a flat background with vanishing G-flux in Horava-Witten supergravity represents a vacuum state, which is stable with respect to interactions between the ten-dimensional boundaries, mediated through the D=11 supergravity bulk fields. For this, we consider fluctuations in the graviton,... | 10.078253 | 10.612253 | 11.167231 | 10.125083 | 10.05791 | 10.662697 | 10.522549 | 10.193764 | 10.28633 | 12.006909 | 9.827127 | 9.717102 | 9.886799 | 9.582267 | 9.927158 | 9.626451 | 9.970026 | 9.521964 | 9.689022 | 10.23403 | 9.501822 |
2010.09564 | Di Wang | Warren Siegel and Di Wang | M Theory from F Theory | 18 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We write down a $GL(D+1)$ (D for the dimension of string theory) manifest
fundamental brane worldvolume current algebra description of M theory, which
consists of a pair of vector field $X^m$ and dual 2-form field $X_{mn}$,
compositing together to parametrize the spacetime, with a selfduality condition
for sectioning... | [
{
"created": "Mon, 19 Oct 2020 14:48:23 GMT",
"version": "v1"
}
] | 2020-10-20 | [
[
"Siegel",
"Warren",
""
],
[
"Wang",
"Di",
""
]
] | We write down a $GL(D+1)$ (D for the dimension of string theory) manifest fundamental brane worldvolume current algebra description of M theory, which consists of a pair of vector field $X^m$ and dual 2-form field $X_{mn}$, compositing together to parametrize the spacetime, with a selfduality condition for sectioning. ... | 14.682097 | 13.287186 | 16.183254 | 14.257864 | 14.715949 | 14.879857 | 15.614016 | 15.163785 | 14.520434 | 17.849949 | 14.097992 | 14.466334 | 14.655506 | 14.211172 | 14.178969 | 14.804155 | 14.788489 | 14.093593 | 14.463218 | 14.787727 | 14.13802 |
1310.7710 | Chong-Sun Chu | Chong-Sun Chu | Non-Abelian Self-Dual Strings in Six Dimensions from Four Dimensional
1/2-BPS Monopoles | 21 pages, LaTeX. 2 figures. v3: Add a new solution that describes two
finitely separated M5-branes meeting midway in between. The solution is based
on the 't Hooft-Polyakov monopole | null | 10.1016/j.nuclphysb.2014.03.006 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explain a new construction of self-dual string solutions to the
non-abelian two-form self-duality equation proposed in \cite{CK}. This class of
self-dual strings is determined by the BPS monopoles in four-dimensions and the
self dual string charge is given by the charge of the monopole. Our
construction covers the... | [
{
"created": "Tue, 29 Oct 2013 08:48:35 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Nov 2013 14:46:44 GMT",
"version": "v2"
},
{
"created": "Tue, 18 Mar 2014 03:42:31 GMT",
"version": "v3"
}
] | 2016-11-26 | [
[
"Chu",
"Chong-Sun",
""
]
] | We explain a new construction of self-dual string solutions to the non-abelian two-form self-duality equation proposed in \cite{CK}. This class of self-dual strings is determined by the BPS monopoles in four-dimensions and the self dual string charge is given by the charge of the monopole. Our construction covers the S... | 9.105161 | 8.392072 | 10.441034 | 7.972407 | 8.667278 | 8.336042 | 8.478073 | 8.58849 | 7.853693 | 10.428797 | 8.236899 | 8.220392 | 9.095859 | 8.03665 | 8.108083 | 8.307453 | 7.990957 | 8.325661 | 8.152668 | 8.878528 | 8.131253 |
2107.12277 | Nicol\`o Petri | Yolanda Lozano, Nicol\`o Petri, Cristian Risco | New AdS$_2$ supergravity duals of 4d SCFTs with defects | 40 pages, 3 figures | null | 10.1007/JHEP10(2021)217 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct new families of $\text{AdS}_2 \times S^2 \times S^2$ solutions
with 4 supercharges in Type II supergravities. We show that subclasses of these
solutions can be interpreted in terms of defect branes embedded in 4d
$\mathcal{N} = 4 $ SYM, or orbifolds thereof. This is explicitly realised by
showing that th... | [
{
"created": "Mon, 26 Jul 2021 15:36:16 GMT",
"version": "v1"
}
] | 2021-11-17 | [
[
"Lozano",
"Yolanda",
""
],
[
"Petri",
"Nicolò",
""
],
[
"Risco",
"Cristian",
""
]
] | We construct new families of $\text{AdS}_2 \times S^2 \times S^2$ solutions with 4 supercharges in Type II supergravities. We show that subclasses of these solutions can be interpreted in terms of defect branes embedded in 4d $\mathcal{N} = 4 $ SYM, or orbifolds thereof. This is explicitly realised by showing that the ... | 6.030109 | 5.007404 | 6.75646 | 5.629928 | 5.62356 | 5.673695 | 5.202397 | 5.430305 | 5.393145 | 7.530569 | 5.420214 | 5.65119 | 6.30832 | 5.649011 | 5.749352 | 5.668582 | 5.638241 | 5.693625 | 5.632665 | 6.255946 | 5.700225 |
1503.03326 | Bruno Lima de Souza | Loriano Bonora, Antonio Duarte Pereira and Bruno Lima de Souza | Regularization of energy-momentum tensor correlators and parity-odd
terms | 40 pages, 1 figure. v2: minor changes and typos corrected | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the problem of regularizing correlators in conformal field
theories. The only way to do it in coordinate space is to interpret them as
distributions. Unfortunately except for the simplest cases we do not have
tabulated mathematical results. The way out we pursue here is to go to momentum
space and use Feyn... | [
{
"created": "Wed, 11 Mar 2015 13:38:31 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Mar 2015 16:49:38 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Bonora",
"Loriano",
""
],
[
"Pereira",
"Antonio Duarte",
""
],
[
"de Souza",
"Bruno Lima",
""
]
] | We discuss the problem of regularizing correlators in conformal field theories. The only way to do it in coordinate space is to interpret them as distributions. Unfortunately except for the simplest cases we do not have tabulated mathematical results. The way out we pursue here is to go to momentum space and use Feynma... | 9.16081 | 9.172352 | 9.073505 | 9.058254 | 8.942057 | 8.742267 | 9.509855 | 9.30437 | 8.639961 | 10.071878 | 8.592488 | 8.613794 | 8.934826 | 8.568809 | 8.675975 | 8.902822 | 8.624974 | 8.71751 | 8.799308 | 8.911615 | 8.701445 |
1312.6709 | Denis Dalmazi | H. A. Biazotti, D. Dalmazi, and G. B. de Gracia | Dimensional reduction of the massless limit of the linearized "New
Massive Gravity" | 12 pages, one more reference and text slightly modified accordingly | null | 10.1140/epjc/s10052-014-2747-0 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The so called "New Massive Gravity" in $D=2+1$ consists of the
Einstein-Hilbert action (with minus sign) plus a quadratic term in curvatures
($K$-term). Here we perform the Kaluza-Klein dimensional reduction of the
linearized $K$-term to $D=1+1$. We end up with a fourth-order massive
electrodynamics in $D=1+1$ descri... | [
{
"created": "Mon, 23 Dec 2013 21:57:16 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Jan 2014 19:24:55 GMT",
"version": "v2"
}
] | 2015-06-18 | [
[
"Biazotti",
"H. A.",
""
],
[
"Dalmazi",
"D.",
""
],
[
"de Gracia",
"G. B.",
""
]
] | The so called "New Massive Gravity" in $D=2+1$ consists of the Einstein-Hilbert action (with minus sign) plus a quadratic term in curvatures ($K$-term). Here we perform the Kaluza-Klein dimensional reduction of the linearized $K$-term to $D=1+1$. We end up with a fourth-order massive electrodynamics in $D=1+1$ describe... | 6.594196 | 5.904874 | 6.898396 | 6.021536 | 6.158976 | 5.774864 | 5.753332 | 5.861521 | 5.90202 | 6.798189 | 6.021669 | 6.008823 | 6.431967 | 6.075193 | 6.189767 | 6.126106 | 6.096595 | 6.052505 | 6.139216 | 6.644355 | 6.170314 |
hep-th/0301062 | Andrianov Alexander | A. A. Andrianov (1,2), A. V. Sokolov (2)((1)INFN, Sezione di Bologna,
Italy; (2) St.Petersburg State University) | Nonlinear supersymmetry in Quantum Mechanics: algebraic properties and
differential representation | 28 pages, Latex, minor improvements and removed misprints | Nucl.Phys. B660 (2003) 25-50 | 10.1016/S0550-3213(03)00232-3 | null | hep-th math-ph math.MP quant-ph | null | We study the Nonlinear (Polynomial, N-fold,...) Supersymmetry algebra in
one-dimensional QM. Its structure is determined by the type of conjugation
operation (Hermitian conjugation or transposition) and described with the help
of the Super-Hamiltonian projection on the zero-mode subspace of a supercharge.
We show tha... | [
{
"created": "Fri, 10 Jan 2003 14:32:20 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Jan 2003 10:48:14 GMT",
"version": "v2"
},
{
"created": "Mon, 3 Feb 2003 12:04:33 GMT",
"version": "v3"
},
{
"created": "Tue, 18 Mar 2003 17:00:58 GMT",
"version": "v4"
}
] | 2010-04-05 | [
[
"Andrianov",
"A. A.",
""
],
[
"Sokolov",
"A. V.",
""
]
] | We study the Nonlinear (Polynomial, N-fold,...) Supersymmetry algebra in one-dimensional QM. Its structure is determined by the type of conjugation operation (Hermitian conjugation or transposition) and described with the help of the Super-Hamiltonian projection on the zero-mode subspace of a supercharge. We show that ... | 11.678803 | 11.727092 | 12.53895 | 11.507661 | 13.447732 | 12.004888 | 12.578127 | 11.204936 | 11.82216 | 12.360756 | 11.202455 | 11.549191 | 11.862399 | 11.224385 | 11.859507 | 11.492411 | 11.72863 | 11.769376 | 11.292982 | 11.817857 | 11.284424 |
1107.2925 | Yoske Sumitomo | Gary Shiu, Yoske Sumitomo | Stability Constraints on Classical de Sitter Vacua | 18 pages; v2: argument improved, references added | null | 10.1007/JHEP09(2011)052 | MAD-TH-11-06, TIFR/TH/11-31 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present further no-go theorems for classical de Sitter vacua in Type II
string theory, i.e., de Sitter constructions that do not invoke
non-perturbative effects or explicit supersymmetry breaking localized sources.
By analyzing the stability of the 4D potential arising from compactification on
manfiolds with curva... | [
{
"created": "Thu, 14 Jul 2011 20:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Jul 2011 19:12:20 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Shiu",
"Gary",
""
],
[
"Sumitomo",
"Yoske",
""
]
] | We present further no-go theorems for classical de Sitter vacua in Type II string theory, i.e., de Sitter constructions that do not invoke non-perturbative effects or explicit supersymmetry breaking localized sources. By analyzing the stability of the 4D potential arising from compactification on manfiolds with curvatu... | 10.293989 | 10.40452 | 12.297185 | 9.501809 | 10.313938 | 10.071909 | 10.136374 | 9.49435 | 10.110096 | 13.262655 | 10.644921 | 9.681252 | 10.607067 | 9.688853 | 9.671421 | 9.859777 | 9.985886 | 9.867401 | 9.819118 | 10.939043 | 9.593392 |
1610.06464 | In Yong Park | I. Y. Park | Quantum gravitational effects on boundary | 31 pages, 5 figures, minor changes, version to appear in TMPh | Theor.Math.Phys. 195(1) (2018) 607-627 | 10.1134/S0040577918040128 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum gravitational effects may hold the key to some of the outstanding
problems in theoretical physics. In this work we analyze the perturbative
quantum effects on the boundary of a gravitational system and Dirichlet
boundary condtion imposed at the classical level. Our analysis reveals that for
a black hole solut... | [
{
"created": "Thu, 20 Oct 2016 15:51:29 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Nov 2016 14:01:26 GMT",
"version": "v2"
},
{
"created": "Wed, 10 May 2017 22:22:39 GMT",
"version": "v3"
}
] | 2018-05-08 | [
[
"Park",
"I. Y.",
""
]
] | Quantum gravitational effects may hold the key to some of the outstanding problems in theoretical physics. In this work we analyze the perturbative quantum effects on the boundary of a gravitational system and Dirichlet boundary condtion imposed at the classical level. Our analysis reveals that for a black hole solutio... | 8.820443 | 7.967626 | 8.712871 | 8.295774 | 8.882495 | 9.1098 | 8.373638 | 7.942523 | 8.261231 | 8.93588 | 7.826019 | 8.382375 | 8.112993 | 8.05547 | 8.238503 | 8.398707 | 8.379979 | 8.203686 | 7.978965 | 8.192271 | 8.208422 |
hep-th/9810069 | S. Kalyana Rama | S. Kalyana Rama and B. Sathiapalan | The Hagedorn Transition, Deconfinement and the AdS/CFT Correspondence | Latex file, 10 Pages | Mod.Phys.Lett. A13 (1998) 3137-3144 | 10.1142/S0217732398003338 | IMSc/98/10/51 | hep-th | null | A connection between the Hagedorn transition in string theory and the
deconfinement transition in (non-supersymmetric) Yang-Mills theory is made
using the AdS/CFT correspondence. We modify the model of zero temperature QCD
proposed by Witten by compactifying an additional space-time coordinate with
supersymmetry brea... | [
{
"created": "Sat, 10 Oct 1998 07:32:48 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Rama",
"S. Kalyana",
""
],
[
"Sathiapalan",
"B.",
""
]
] | A connection between the Hagedorn transition in string theory and the deconfinement transition in (non-supersymmetric) Yang-Mills theory is made using the AdS/CFT correspondence. We modify the model of zero temperature QCD proposed by Witten by compactifying an additional space-time coordinate with supersymmetry breaki... | 10.032875 | 8.536206 | 9.524422 | 8.318432 | 8.858362 | 9.294889 | 9.563723 | 9.159045 | 8.626526 | 11.023609 | 8.641519 | 9.138812 | 9.976209 | 8.553432 | 9.145532 | 8.950864 | 9.045985 | 8.948493 | 8.883305 | 9.528243 | 9.11151 |
2406.00712 | Amr Ahmadain | Amr Ahmadain, Rifath Khan | A Worldsheet Derivation of the Classical Off-shell Boundary Action for
the Dilaton in Half-Space | 32 pages, 4 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We use the method of images to present a worldsheet derivation of the sphere
partition function for the dilaton in half-space to leading order in $\apr$
with Neumann boundary conditions. We use Tseytlin's sphere prescription to
obtain the total (bulk and boundary) off-shell classical bosonic string action
for the dil... | [
{
"created": "Sun, 2 Jun 2024 11:31:21 GMT",
"version": "v1"
}
] | 2024-06-04 | [
[
"Ahmadain",
"Amr",
""
],
[
"Khan",
"Rifath",
""
]
] | We use the method of images to present a worldsheet derivation of the sphere partition function for the dilaton in half-space to leading order in $\apr$ with Neumann boundary conditions. We use Tseytlin's sphere prescription to obtain the total (bulk and boundary) off-shell classical bosonic string action for the dilat... | 16.386362 | 16.002785 | 17.591694 | 13.388659 | 14.759995 | 16.171127 | 18.045916 | 15.30054 | 14.088999 | 18.249907 | 13.314248 | 14.284635 | 15.17101 | 14.893682 | 14.643541 | 14.017109 | 14.220422 | 15.271785 | 14.1754 | 15.375719 | 14.274755 |
hep-th/9810076 | Yavuz Nutku | J. Kalayci and Y. Nutku | Alternative bi-Hamiltonian structures for WDVV equations of
associativity | null | J.Phys.A31:723,1998 | 10.1088/0305-4470/31/2/027 | null | hep-th | null | The WDVV equations of associativity in 2-d topological field theory are
completely integrable third order Monge-Amp\`ere equations which admit
bi-Hamiltonian structure. The time variable plays a distinguished role in the
discussion of Hamiltonian structure whereas in the theory of WDVV equations
none of the independe... | [
{
"created": "Mon, 12 Oct 1998 09:42:48 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Kalayci",
"J.",
""
],
[
"Nutku",
"Y.",
""
]
] | The WDVV equations of associativity in 2-d topological field theory are completely integrable third order Monge-Amp\`ere equations which admit bi-Hamiltonian structure. The time variable plays a distinguished role in the discussion of Hamiltonian structure whereas in the theory of WDVV equations none of the independent... | 12.192528 | 12.422124 | 14.639125 | 12.068825 | 12.877735 | 14.300183 | 12.582403 | 12.66573 | 11.037855 | 16.131504 | 11.788514 | 11.608946 | 12.575382 | 11.542041 | 12.155532 | 12.360025 | 12.034884 | 11.752331 | 12.199468 | 12.286664 | 11.838383 |
1512.02887 | Taotao Qiu | Taotao Qiu | New DBI Inflation model with Kinetic Coupling to Einstein Gravity | 6 pages, no figure | Phys. Rev. D 93, 123515 (2016) | 10.1103/PhysRevD.93.123515 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study a new class of inflation models which generalize the
Dirac-Born-Infeld (DBI) action with the addition of a nonminimal kinetic
coupling (NKC) term. We dubbed this model as the {\it new DBI inflation model}.
The NKC term does not bring new dynamical degree of freedom, so the equations
of motion r... | [
{
"created": "Wed, 9 Dec 2015 15:03:25 GMT",
"version": "v1"
},
{
"created": "Sun, 28 Feb 2016 15:40:19 GMT",
"version": "v2"
},
{
"created": "Wed, 3 Aug 2016 04:23:05 GMT",
"version": "v3"
}
] | 2016-08-04 | [
[
"Qiu",
"Taotao",
""
]
] | In this paper we study a new class of inflation models which generalize the Dirac-Born-Infeld (DBI) action with the addition of a nonminimal kinetic coupling (NKC) term. We dubbed this model as the {\it new DBI inflation model}. The NKC term does not bring new dynamical degree of freedom, so the equations of motion rem... | 7.629783 | 7.269131 | 7.215937 | 6.864781 | 7.022288 | 8.106145 | 7.431077 | 6.760592 | 7.436862 | 7.575189 | 6.979668 | 6.9861 | 7.069526 | 6.914593 | 7.224672 | 7.159736 | 7.023695 | 7.104844 | 7.118703 | 6.944785 | 6.960504 |
hep-th/0209034 | Koji Hashimoto | Gary Gibbons, Koji Hashimoto, Piljin Yi | Tachyon Condensates, Carrollian Contraction of Lorentz Group, and
Fundamental Strings | 28 pages, typos corrected | JHEP 0209:061,2002 | 10.1088/1126-6708/2002/09/061 | DAMTP-2002-101, KIAS-P02051, UT-Komaba/02-07 | hep-th | null | We study the rolling tachyon condensate in the presence of a gauge field. The
generic vacuum admits both a rolling tachyon, \dot{T}, and a uniform electric
field, \vec{E}, which together affect the effective metric governing the
fluctuations of open string modes. If one suppresses the gauge field
altogether, the ligh... | [
{
"created": "Wed, 4 Sep 2002 14:22:26 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Oct 2002 01:01:15 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Gibbons",
"Gary",
""
],
[
"Hashimoto",
"Koji",
""
],
[
"Yi",
"Piljin",
""
]
] | We study the rolling tachyon condensate in the presence of a gauge field. The generic vacuum admits both a rolling tachyon, \dot{T}, and a uniform electric field, \vec{E}, which together affect the effective metric governing the fluctuations of open string modes. If one suppresses the gauge field altogether, the light-... | 14.651584 | 15.2208 | 15.135636 | 12.760203 | 14.370097 | 15.434235 | 13.711255 | 13.785794 | 13.591416 | 15.766006 | 13.969657 | 13.984965 | 13.888446 | 13.828249 | 13.857448 | 13.543274 | 13.951223 | 13.759544 | 13.758695 | 14.139978 | 14.020779 |
1112.5406 | Petr Dunin-Barkowski | Petr Dunin-Barkowski, Alexey Sleptsov, Andrey Smirnov | Kontsevich integral for knots and Vassiliev invariants | 25 pages, 17 figures | Int. J. Mod. Phys. A 28, 1330025 (2013) | 10.1142/S0217751X13300251 | ITEP/TH-63/11 | hep-th math.CO math.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review quantum field theory approach to the knot theory. Using holomorphic
gauge we obtain the Kontsevich integral. It is explained how to calculate
Vassiliev invariants and coefficients in Kontsevich integral in a combinatorial
way which can be programmed on a computer. We discuss experimental results and
tempora... | [
{
"created": "Thu, 22 Dec 2011 18:15:04 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Dec 2011 16:31:19 GMT",
"version": "v2"
},
{
"created": "Sat, 21 Jan 2012 09:52:31 GMT",
"version": "v3"
}
] | 2014-04-03 | [
[
"Dunin-Barkowski",
"Petr",
""
],
[
"Sleptsov",
"Alexey",
""
],
[
"Smirnov",
"Andrey",
""
]
] | We review quantum field theory approach to the knot theory. Using holomorphic gauge we obtain the Kontsevich integral. It is explained how to calculate Vassiliev invariants and coefficients in Kontsevich integral in a combinatorial way which can be programmed on a computer. We discuss experimental results and temporal ... | 14.041613 | 13.644215 | 13.967981 | 13.608128 | 14.324473 | 14.311436 | 13.445224 | 13.761287 | 13.122574 | 13.940873 | 12.943866 | 12.748705 | 13.244668 | 12.459394 | 13.285039 | 13.004522 | 12.414731 | 13.030879 | 12.135736 | 13.882312 | 12.578321 |
2303.09896 | Jnanadeva Maharana | Jnanadeva Maharana | On Production of Excited Kaluza-Klein States in Large Radius
Compactification Scenario | null | null | 10.1142/S0217751X23500598 | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Production of exotic states at LHC is considered in the large radius
compactification scenario. We envisage a five dimensional theory for a scalar
field in five dimensional flat spacetime. It is compactified on a circle,
$S^1$, with radius, $R$. The radius is assumed to be in TeV scale appealing to
LRC hypothesis. Th... | [
{
"created": "Fri, 17 Mar 2023 11:22:09 GMT",
"version": "v1"
}
] | 2023-08-02 | [
[
"Maharana",
"Jnanadeva",
""
]
] | Production of exotic states at LHC is considered in the large radius compactification scenario. We envisage a five dimensional theory for a scalar field in five dimensional flat spacetime. It is compactified on a circle, $S^1$, with radius, $R$. The radius is assumed to be in TeV scale appealing to LRC hypothesis. The ... | 12.622862 | 12.539725 | 12.406718 | 12.074572 | 13.485159 | 13.755533 | 13.245236 | 12.799158 | 12.433526 | 13.433504 | 12.784096 | 12.289619 | 12.239892 | 12.173519 | 12.354312 | 12.243211 | 13.146633 | 11.749341 | 12.395905 | 12.819106 | 12.042584 |
1406.6602 | Daniela D'Ascanio | M. Asorey, C. G. Beneventano, I. Cavero-Pel\'aez, D. D'Ascanio and E.
M. Santangelo | Topological Entropy and Renormalization Group flow in 3-dimensional
spherical spaces | 35 pages, 5 figures. Minor changes; matches published version | JHEP 01 (2015) 078 | 10.1007/JHEP01(2015)078 | null | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the renormalization group (RG) flow of the temperature independent
term of the entropy in the high temperature limit \beta/a<<1 of a massive field
theory in 3-dimensional spherical spaces M_3 with constant curvature 6/a^2. For
masses lower than 2\pi/\beta, this term can be identified with the free energy
o... | [
{
"created": "Wed, 25 Jun 2014 15:11:46 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Dec 2014 21:14:49 GMT",
"version": "v2"
},
{
"created": "Sat, 17 Jan 2015 01:15:22 GMT",
"version": "v3"
}
] | 2015-01-20 | [
[
"Asorey",
"M.",
""
],
[
"Beneventano",
"C. G.",
""
],
[
"Cavero-Peláez",
"I.",
""
],
[
"D'Ascanio",
"D.",
""
],
[
"Santangelo",
"E. M.",
""
]
] | We analyze the renormalization group (RG) flow of the temperature independent term of the entropy in the high temperature limit \beta/a<<1 of a massive field theory in 3-dimensional spherical spaces M_3 with constant curvature 6/a^2. For masses lower than 2\pi/\beta, this term can be identified with the free energy of ... | 8.604528 | 8.988362 | 9.499051 | 8.45103 | 9.700746 | 9.631548 | 8.586767 | 8.822637 | 8.717505 | 9.448992 | 8.579771 | 8.146869 | 8.585623 | 8.147861 | 8.372127 | 8.49256 | 8.18111 | 8.178123 | 8.452442 | 8.824713 | 8.240792 |
2303.10958 | Rong-Xin Miao | Dongqi Li, Rong-Xin Miao | Massless Entanglement Islands in Cone Holography | 32 pages, 16 figures, minor revision published in JHEP | JHEP06(2023)056 | 10.1007/JHEP06(2023)056 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | It is controversial whether entanglement islands can exist in massless
gravity theories. Recently, it is found that the massless entanglement island
appears in wedge holography with DGP gravity on the branes. In this paper, we
generalize the discussions to the codim-n holography named cone holography. For
simplicity,... | [
{
"created": "Mon, 20 Mar 2023 09:30:49 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jun 2023 21:22:15 GMT",
"version": "v2"
}
] | 2023-06-16 | [
[
"Li",
"Dongqi",
""
],
[
"Miao",
"Rong-Xin",
""
]
] | It is controversial whether entanglement islands can exist in massless gravity theories. Recently, it is found that the massless entanglement island appears in wedge holography with DGP gravity on the branes. In this paper, we generalize the discussions to the codim-n holography named cone holography. For simplicity, w... | 7.868853 | 7.237783 | 8.560753 | 7.256747 | 7.325518 | 7.417992 | 6.992486 | 7.155469 | 7.30125 | 9.021002 | 7.390245 | 7.570538 | 8.026436 | 7.73492 | 7.818303 | 7.633703 | 7.677973 | 7.542601 | 7.64505 | 8.321183 | 7.628446 |
0811.4074 | Tao Zhu | Tao Zhu and Ji-Rong Ren | Corrections to Hawking-like Radiation for a Friedmann-Robertson-Walker
Universe | 10 pages, no figures, comments are welcome; v2: references added and
some typoes corrected, to appear in Euro.Phys.J.C; v3:a defect corrected. We
thank Dr.Elias Vagenas for pointing out a defect of our paper | Eur.Phys.J.C62:413-418,2009 | 10.1140/epjc/s10052-009-1044-9 | null | hep-th astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, a Hamilton-Jacobi method beyond semiclassical approximation in
black hole physics was developed by \emph{Banerjee} and
\emph{Majhi}\cite{beyond0}. In this paper, we generalize their analysis of
black holes to the case of Friedmann-Robertson-Walker (FRW) universe. It is
shown that all the higher order quantu... | [
{
"created": "Tue, 25 Nov 2008 12:53:08 GMT",
"version": "v1"
},
{
"created": "Wed, 13 May 2009 14:48:53 GMT",
"version": "v2"
},
{
"created": "Fri, 14 Aug 2009 06:20:04 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Zhu",
"Tao",
""
],
[
"Ren",
"Ji-Rong",
""
]
] | Recently, a Hamilton-Jacobi method beyond semiclassical approximation in black hole physics was developed by \emph{Banerjee} and \emph{Majhi}\cite{beyond0}. In this paper, we generalize their analysis of black holes to the case of Friedmann-Robertson-Walker (FRW) universe. It is shown that all the higher order quantum ... | 10.235641 | 8.075257 | 8.187565 | 8.333079 | 8.127563 | 7.690552 | 8.538875 | 7.562308 | 8.371087 | 8.758844 | 7.895916 | 8.591208 | 8.683038 | 8.299314 | 8.415636 | 8.637848 | 8.33065 | 8.343267 | 8.400232 | 8.363649 | 8.531248 |
0809.2924 | Kanghoon Lee | Kanghoon Lee, Sangmin Lee and Jeong-Hyuck Park | Topological Twisting of Multiple M2-brane Theory | 20 pages, no figure; Refs added, minor improvement, to appear in JHEP | JHEP0811:014,2008 | 10.1088/1126-6708/2008/11/014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Bagger-Lambert-Gustavsson theory with infinite dimensional gauge group has
been suggested to describe M5-brane as a condensation of multiple M2-branes.
Here we perform a topological twisting of the Bagger-Lambert-Gustavsson theory.
The original SO(8) R-symmetry is broken to SO(3)XSO(5), where the former may be
interp... | [
{
"created": "Wed, 17 Sep 2008 15:24:52 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Sep 2008 12:20:53 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Oct 2008 06:27:32 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Lee",
"Kanghoon",
""
],
[
"Lee",
"Sangmin",
""
],
[
"Park",
"Jeong-Hyuck",
""
]
] | Bagger-Lambert-Gustavsson theory with infinite dimensional gauge group has been suggested to describe M5-brane as a condensation of multiple M2-branes. Here we perform a topological twisting of the Bagger-Lambert-Gustavsson theory. The original SO(8) R-symmetry is broken to SO(3)XSO(5), where the former may be interpre... | 9.915634 | 8.728086 | 10.991588 | 9.093524 | 9.395878 | 9.287346 | 8.574818 | 8.447188 | 8.532566 | 10.897157 | 8.488323 | 8.62641 | 8.808514 | 8.353057 | 8.717423 | 8.449029 | 8.738757 | 8.492247 | 8.565925 | 9.188774 | 8.420324 |
hep-th/9307149 | Igor Musatov | B. M. Zupnik | Quantum deformations for the diagonal R-matrices | 6 pages, Talk at Workshop on Supersymmetry and Quantum Groups, Dubna,
15-20 July 1993 | null | null | NIIPF-93/07 | hep-th math.QA | null | We consider two different types of deformations for the linear group $ GL(n)$
which correspond to using of a general diagonal R-matrix. Relations between
braided and quantum deformed algebras and their coactions on a quantum plane
are discussed. We show that tensor-grading-preserving differential calculi can
be const... | [
{
"created": "Sun, 25 Jul 1993 10:43:50 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Zupnik",
"B. M.",
""
]
] | We consider two different types of deformations for the linear group $ GL(n)$ which correspond to using of a general diagonal R-matrix. Relations between braided and quantum deformed algebras and their coactions on a quantum plane are discussed. We show that tensor-grading-preserving differential calculi can be constru... | 18.306145 | 16.46018 | 17.847967 | 15.095216 | 17.58823 | 16.452438 | 19.46991 | 17.428165 | 16.657192 | 24.077522 | 17.699369 | 15.90919 | 16.413528 | 16.07432 | 16.867682 | 17.219973 | 16.390079 | 17.413639 | 17.470253 | 18.16955 | 16.23481 |
hep-th/0404063 | Graziano Vernizzi | G. Akemann, Y.V. Fyodorov and G. Vernizzi | On matrix model partition functions for QCD with chemical potential | 33 pages, 2 figures | Nucl.Phys. B694 (2004) 59-98 | 10.1016/j.nuclphysb.2004.06.017 | SPhT-T04/029 | hep-th | null | Partition functions of two different matrix models for QCD with chemical
potential are computed for an arbitrary number of quark and complex conjugate
anti-quark flavors. In the large-N limit of weak nonhermiticity complete
agreement is found between the two models. This supports the universality of
such fermionic pa... | [
{
"created": "Wed, 7 Apr 2004 14:58:39 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Akemann",
"G.",
""
],
[
"Fyodorov",
"Y. V.",
""
],
[
"Vernizzi",
"G.",
""
]
] | Partition functions of two different matrix models for QCD with chemical potential are computed for an arbitrary number of quark and complex conjugate anti-quark flavors. In the large-N limit of weak nonhermiticity complete agreement is found between the two models. This supports the universality of such fermionic part... | 8.848161 | 9.312966 | 9.48641 | 8.96589 | 9.551394 | 9.118397 | 9.54113 | 8.86436 | 8.953993 | 10.655584 | 8.757322 | 9.134719 | 8.93119 | 8.778131 | 8.625882 | 9.099383 | 8.964159 | 8.999743 | 8.997715 | 9.110922 | 8.86189 |
hep-th/0008021 | Ignatov Alexander | A. M. Ignatov, V. P. Poponin | Pulse interaction in nonlinear vacuum electrodynamics | LaTeX, 5 pages, 2 EPS figures | null | 10.1017/S0263034601194073 | null | hep-th | null | The energy-momentum conservation law is used to investigate the interaction
of pulses in the framework of nonlinear electrodynamics with Lorentz-invariant
constitutive relations. It is shown that for the pulses of the arbitrary shape
the interaction results in phase shift only.
| [
{
"created": "Wed, 2 Aug 2000 12:56:16 GMT",
"version": "v1"
}
] | 2015-06-25 | [
[
"Ignatov",
"A. M.",
""
],
[
"Poponin",
"V. P.",
""
]
] | The energy-momentum conservation law is used to investigate the interaction of pulses in the framework of nonlinear electrodynamics with Lorentz-invariant constitutive relations. It is shown that for the pulses of the arbitrary shape the interaction results in phase shift only. | 9.904243 | 9.907446 | 8.653085 | 7.468654 | 7.527171 | 7.878186 | 9.258595 | 8.773601 | 7.833575 | 8.018362 | 8.04898 | 8.67647 | 8.312564 | 8.317741 | 8.374766 | 8.862887 | 8.581438 | 8.765987 | 7.933155 | 8.131321 | 9.156362 |
1904.08530 | Seung-Joo Lee | Yang-Hui He, Seung-Joo Lee | Distinguishing Elliptic Fibrations with AI | 6 pages, 1 table, 4 figures; v2: four-fold learning vastly improved
in section III.C, four-fold statistics fixed in table I, comments added on
dataset enhancement | null | 10.1016/j.physletb.2019.134889 | CERN-TH-2019-046 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the latest techniques in machine-learning to study whether from the
landscape of Calabi-Yau manifolds one can distinguish elliptically fibred ones.
Using the dataset of complete intersections in products of projective spaces
(CICY3 and CICY4, totalling about a million manifolds) as a concrete
playground, we fi... | [
{
"created": "Wed, 17 Apr 2019 23:05:25 GMT",
"version": "v1"
},
{
"created": "Fri, 10 May 2019 20:20:28 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"He",
"Yang-Hui",
""
],
[
"Lee",
"Seung-Joo",
""
]
] | We use the latest techniques in machine-learning to study whether from the landscape of Calabi-Yau manifolds one can distinguish elliptically fibred ones. Using the dataset of complete intersections in products of projective spaces (CICY3 and CICY4, totalling about a million manifolds) as a concrete playground, we find... | 14.312849 | 11.995576 | 15.141512 | 11.002508 | 12.65801 | 12.024341 | 12.550911 | 11.648585 | 11.845266 | 15.550933 | 12.120619 | 11.774807 | 13.29676 | 12.019362 | 11.777226 | 11.985799 | 11.869081 | 12.522476 | 12.078025 | 13.586178 | 12.526102 |
1708.01411 | Yan Peng | Yan Peng, Bin Wang, Yunqi Liu | On the thermodynamics of the black hole and hairy black hole transitions
in the asymptotically flat spacetime with a box | 12 pages, 6 figures. Accepted for publication in EPJC. arXiv admin
note: text overlap with arXiv:1705.08694 | Eur. Phys. J. C (2018) 78:176 | 10.1140/epjc/s10052-018-5652-0 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the asymptotically flat quasi-local black hole/hairy black hole
model with nonzero mass of the scalar filed. We disclose effects of the scalar
mass on transitions in a grand canonical ensemble with condensation behaviors
of a parameter $\psi_{2}$, which is similar to approaches in holographic
theories. We fi... | [
{
"created": "Fri, 4 Aug 2017 08:10:26 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Sep 2017 09:43:16 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Feb 2018 08:32:01 GMT",
"version": "v3"
}
] | 2018-04-04 | [
[
"Peng",
"Yan",
""
],
[
"Wang",
"Bin",
""
],
[
"Liu",
"Yunqi",
""
]
] | We study the asymptotically flat quasi-local black hole/hairy black hole model with nonzero mass of the scalar filed. We disclose effects of the scalar mass on transitions in a grand canonical ensemble with condensation behaviors of a parameter $\psi_{2}$, which is similar to approaches in holographic theories. We find... | 15.585894 | 15.003056 | 16.056543 | 15.010977 | 14.9719 | 15.357286 | 16.723667 | 14.450788 | 15.209358 | 17.265266 | 14.503443 | 15.010389 | 15.048076 | 14.837049 | 14.850894 | 14.610965 | 14.688168 | 14.800633 | 14.85346 | 15.897751 | 15.09797 |
hep-th/0207103 | Stefano Foffa | Stefano Foffa | Pre-big bang on the brane | Final version published on PRD; one reference added | Phys.Rev. D66 (2002) 063512 | 10.1103/PhysRevD.66.063512 | null | hep-th | null | The equations of motion and junction conditions for a gravi-dilaton brane
world scenario are studied in the string frame. It is shown that they allow
Kasner-like solutions on the brane, which makes the dynamics of the brane very
similar to the low curvature phase of pre-big bang cosmology. Analogies and
differences o... | [
{
"created": "Thu, 11 Jul 2002 12:43:33 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Jul 2002 09:25:01 GMT",
"version": "v2"
},
{
"created": "Fri, 4 Oct 2002 15:09:11 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Foffa",
"Stefano",
""
]
] | The equations of motion and junction conditions for a gravi-dilaton brane world scenario are studied in the string frame. It is shown that they allow Kasner-like solutions on the brane, which makes the dynamics of the brane very similar to the low curvature phase of pre-big bang cosmology. Analogies and differences of ... | 8.950821 | 8.083073 | 8.125392 | 7.901217 | 7.804944 | 8.444398 | 8.242333 | 7.896647 | 7.881633 | 8.42173 | 8.629651 | 8.278852 | 8.349241 | 8.187473 | 8.166489 | 7.990456 | 8.126599 | 8.093937 | 8.02059 | 8.368647 | 8.095864 |
hep-th/0410240 | Clovis Wotzasek | Roberto Menezes and Clovis Wotzasek | On Duality Symmetry in Charged P-Form Theories | 7 pages, Revtex4, accepted for publication Phys. Lett. B | Phys.Lett. B604 (2004) 242-249 | 10.1016/j.physletb.2004.10.039 | null | hep-th | null | We study duality transformation and duality symmetry in the the
electromagnetic-like charged p-form theories. It is shown that the dichotomic
characterization of duality groups as $Z_2$ or SO(2) remains as the only
possibilities but are now present in all dimensions even and odd. This is a
property defined in the sym... | [
{
"created": "Mon, 25 Oct 2004 19:45:57 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Menezes",
"Roberto",
""
],
[
"Wotzasek",
"Clovis",
""
]
] | We study duality transformation and duality symmetry in the the electromagnetic-like charged p-form theories. It is shown that the dichotomic characterization of duality groups as $Z_2$ or SO(2) remains as the only possibilities but are now present in all dimensions even and odd. This is a property defined in the sympl... | 14.699018 | 13.641052 | 14.749242 | 13.189657 | 14.348201 | 13.150552 | 14.603085 | 13.438443 | 13.030956 | 14.649734 | 13.228015 | 13.818048 | 13.865138 | 13.475329 | 13.093204 | 13.714942 | 13.397035 | 13.070257 | 13.070877 | 13.77183 | 13.495138 |
2003.08351 | Mikhail Solon | Clifford Cheung and Mikhail P. Solon | Classical Gravitational Scattering at ${\cal O}(G^3)$ from Feynman
Diagrams | 10 pages + references, 2 figures, 2 ancillary files | null | 10.1007/JHEP06(2020)144 | CALT-TH-2020-006 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform a Feynman diagram calculation of the two-loop scattering amplitude
for gravitationally interacting massive particles in the classical limit.
Conveniently, we are able to sidestep the most taxing diagrams by exploiting
the test-particle limit in which the system is fully characterized by a
particle propagat... | [
{
"created": "Wed, 18 Mar 2020 17:29:57 GMT",
"version": "v1"
}
] | 2020-07-15 | [
[
"Cheung",
"Clifford",
""
],
[
"Solon",
"Mikhail P.",
""
]
] | We perform a Feynman diagram calculation of the two-loop scattering amplitude for gravitationally interacting massive particles in the classical limit. Conveniently, we are able to sidestep the most taxing diagrams by exploiting the test-particle limit in which the system is fully characterized by a particle propagatin... | 14.481425 | 16.934643 | 13.765704 | 12.763736 | 14.485835 | 15.525305 | 15.041232 | 13.738287 | 13.995179 | 16.678223 | 13.986366 | 13.471106 | 13.499979 | 13.398041 | 13.784055 | 13.732651 | 13.344572 | 13.442135 | 13.545752 | 13.731974 | 13.411724 |
hep-th/0503215 | Davide Gaiotto | D. Gaiotto | Long strings condensation and FZZT branes | 15 pages, 3 figures | null | null | HUTP-05/A0014 | hep-th | null | We propose a matrix model description of extended D-branes in 2D noncritical
string
| [
{
"created": "Mon, 28 Mar 2005 12:21:41 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gaiotto",
"D.",
""
]
] | We propose a matrix model description of extended D-branes in 2D noncritical string | 21.386852 | 12.333753 | 22.466091 | 10.939632 | 10.454415 | 10.050146 | 11.998206 | 10.267005 | 11.514212 | 27.400217 | 13.044826 | 12.791034 | 23.592693 | 13.242161 | 13.171851 | 13.151452 | 12.733001 | 13.922777 | 14.095047 | 20.933039 | 14.201225 |
hep-th/0609052 | Pallab Basu | Spenta R. Wadia | Gauge theory description of the fate of the small Schwarzschild
blackhole | 16 pages, 1 figure | null | 10.1142/9789812770523_0025 | TIFR /TH/06-27 | hep-th | null | In this talk we discuss the fate of the small Schwarzschild blackhole of
$AdS_5\times S^5$ using the AdS/CFT correspondence at finite temperature. The
third order $N = \infty$ phase transition in the gauge theory corresponds to
the blackhole-string transition. This singularity is resolved using a double
scaling limit... | [
{
"created": "Thu, 7 Sep 2006 13:10:19 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Wadia",
"Spenta R.",
""
]
] | In this talk we discuss the fate of the small Schwarzschild blackhole of $AdS_5\times S^5$ using the AdS/CFT correspondence at finite temperature. The third order $N = \infty$ phase transition in the gauge theory corresponds to the blackhole-string transition. This singularity is resolved using a double scaling limit i... | 11.575333 | 10.735292 | 14.853344 | 11.31119 | 10.664859 | 10.788729 | 10.774701 | 10.612301 | 10.755852 | 13.455035 | 10.619406 | 10.974172 | 11.773731 | 11.160372 | 10.8821 | 10.772361 | 11.210818 | 11.000866 | 11.223291 | 12.13683 | 10.997819 |
hep-th/0207238 | Francois Englert | Auttakit Chattaraputi, Francois Englert, Laurent Houart, Anne Taormina | The bosonic mother of fermionic D-branes | Latex file, 4 figures, 49 pages | JHEP 0209:037,2002 | 10.1088/1126-6708/2002/09/037 | ULB-TH-02-21, DCPT-02-45 | hep-th | null | We extend the search for fermionic subspaces of the bosonic string
compactified on E8 X SO(16) lattices to include all fermionic D-branes. This
extension constraints the truncation procedure previously proposed and relates
the fermionic strings, supersymmetric or not, to the global structure of the
SO(16) group. The ... | [
{
"created": "Fri, 26 Jul 2002 10:28:03 GMT",
"version": "v1"
}
] | 2010-04-28 | [
[
"Chattaraputi",
"Auttakit",
""
],
[
"Englert",
"Francois",
""
],
[
"Houart",
"Laurent",
""
],
[
"Taormina",
"Anne",
""
]
] | We extend the search for fermionic subspaces of the bosonic string compactified on E8 X SO(16) lattices to include all fermionic D-branes. This extension constraints the truncation procedure previously proposed and relates the fermionic strings, supersymmetric or not, to the global structure of the SO(16) group. The sp... | 17.167459 | 18.902174 | 21.034889 | 17.32255 | 18.629322 | 16.541592 | 18.265034 | 16.057278 | 18.161957 | 19.871971 | 17.564005 | 15.925563 | 18.481871 | 15.623568 | 16.410208 | 16.262312 | 16.243259 | 15.638503 | 16.616108 | 17.113977 | 15.679052 |
2212.08052 | Renata Ferrero | Renata Ferrero and Chris Ripken | Quadratic gravity potentials in de Sitter spacetime from Feynman
diagrams | 34 pages, 9 figures | JHEP 08 (2023) 199 | 10.1007/JHEP08(2023)199 | MITP-22-104 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We employ a manifestly covariant formalism to compute the tree-level
amputated Green's function of non-minimally coupled scalar fields in quadratic
gravity in a de Sitter background. We study this Green's function in the
adiabatic limit, and construct the classical Newtonian potential. At short
distances, the flat-sp... | [
{
"created": "Thu, 15 Dec 2022 18:57:00 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Aug 2023 08:10:07 GMT",
"version": "v2"
}
] | 2023-09-01 | [
[
"Ferrero",
"Renata",
""
],
[
"Ripken",
"Chris",
""
]
] | We employ a manifestly covariant formalism to compute the tree-level amputated Green's function of non-minimally coupled scalar fields in quadratic gravity in a de Sitter background. We study this Green's function in the adiabatic limit, and construct the classical Newtonian potential. At short distances, the flat-spac... | 7.90186 | 7.629179 | 7.30854 | 7.370325 | 7.961538 | 7.939943 | 8.301053 | 7.360672 | 7.030786 | 7.689192 | 7.354012 | 7.53307 | 7.326593 | 7.255738 | 7.393583 | 7.546854 | 7.194983 | 7.398865 | 7.354525 | 7.288662 | 7.413664 |
hep-th/0409007 | Dmitry Talalaev | A. Chervov, D. Talalaev | Universal G-oper and Gaudin eigenproblem | 15 pages, the status of some statements changed | null | null | ITEP-TH-34/04 | hep-th math.QA | null | This paper is devoted to the eigenvalue problem for the quantum Gaudin
system. We prove the universal correspondence between eigenvalues of Gaudin
Hamiltonians and the so-called G-opers without monodromy in general gl(n) case
modulo a hypothesys on the analytic properties of the solution of a KZ-type
equation.
Firs... | [
{
"created": "Wed, 1 Sep 2004 13:32:23 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jul 2006 11:19:56 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Chervov",
"A.",
""
],
[
"Talalaev",
"D.",
""
]
] | This paper is devoted to the eigenvalue problem for the quantum Gaudin system. We prove the universal correspondence between eigenvalues of Gaudin Hamiltonians and the so-called G-opers without monodromy in general gl(n) case modulo a hypothesys on the analytic properties of the solution of a KZ-type equation. Firstly ... | 9.780766 | 12.06066 | 12.159068 | 10.306275 | 11.220568 | 11.605979 | 11.156959 | 10.487696 | 10.695372 | 11.759407 | 10.116167 | 9.757437 | 10.495185 | 9.815654 | 9.744306 | 9.959717 | 9.66256 | 9.876846 | 9.755384 | 10.112586 | 9.519473 |
1610.01519 | Romulo Rougemont | Stefano I. Finazzo (Sao Paulo, IFT), Romulo Rougemont (Sao Paulo U.),
Maicon Zaniboni (Sao Paulo U.), Renato Critelli (Sao Paulo U.), and Jorge
Noronha (Sao Paulo U.) | Critical behavior of non-hydrodynamic quasinormal modes in a strongly
coupled plasma | 31 pages, 15 figures, version accepted for publication in JHEP | JHEP 01 (2017) 137 | 10.1007/JHEP01(2017)137 | null | hep-th gr-qc nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the behavior of quasinormal modes in a top-down holographic dual
corresponding to a strongly coupled $\mathcal{N} = 4$ super Yang-Mills plasma
charged under a $U(1)$ subgroup of the global $SU(4)$ R-symmetry. In
particular, we analyze the spectra of quasinormal modes in the external scalar
and vector diffusi... | [
{
"created": "Wed, 5 Oct 2016 16:46:35 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Jan 2017 16:34:47 GMT",
"version": "v2"
}
] | 2017-02-02 | [
[
"Finazzo",
"Stefano I.",
"",
"Sao Paulo, IFT"
],
[
"Rougemont",
"Romulo",
"",
"Sao Paulo U."
],
[
"Zaniboni",
"Maicon",
"",
"Sao Paulo U."
],
[
"Critelli",
"Renato",
"",
"Sao Paulo U."
],
[
"Noronha",
"Jorge",
"",
"Sao... | We study the behavior of quasinormal modes in a top-down holographic dual corresponding to a strongly coupled $\mathcal{N} = 4$ super Yang-Mills plasma charged under a $U(1)$ subgroup of the global $SU(4)$ R-symmetry. In particular, we analyze the spectra of quasinormal modes in the external scalar and vector diffusion... | 5.782616 | 5.565009 | 5.911973 | 5.530497 | 5.748921 | 5.357367 | 5.416902 | 5.500167 | 5.531113 | 6.172918 | 5.394962 | 5.628619 | 5.802651 | 5.60362 | 5.533693 | 5.473618 | 5.470912 | 5.572436 | 5.560165 | 5.799667 | 5.597798 |
0812.2234 | Yu Nakayama | Yu Nakayama | Emerging AdS from Extremally Rotating NS5-branes | 15 pages, v2: references added, numerical factors corrected, v3:
boundary conditions clarified, to be published in PLB | Phys.Lett.B673:272-278,2009 | 10.1016/j.physletb.2009.02.031 | UCB-PTH-08/78 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the near-horizon limit of extremally rotating NS5-branes. The
resulting geometry has SL(2,R) \times U(1)^2 isometry. The asymptotic symmetry
group contains a chiral Virasoro algebra, and we obtain two different
realizations depending on the boundary conditions we impose. When one of the
two angular mom... | [
{
"created": "Thu, 11 Dec 2008 20:09:59 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Dec 2008 18:30:57 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Feb 2009 07:07:29 GMT",
"version": "v3"
}
] | 2009-03-24 | [
[
"Nakayama",
"Yu",
""
]
] | We investigate the near-horizon limit of extremally rotating NS5-branes. The resulting geometry has SL(2,R) \times U(1)^2 isometry. The asymptotic symmetry group contains a chiral Virasoro algebra, and we obtain two different realizations depending on the boundary conditions we impose. When one of the two angular momen... | 7.996787 | 7.23012 | 8.733861 | 7.156615 | 7.375879 | 7.467796 | 7.709332 | 7.452538 | 7.391052 | 8.873419 | 7.01108 | 7.657257 | 7.789977 | 7.716666 | 7.504479 | 7.981863 | 7.633002 | 7.492878 | 7.504028 | 8.038233 | 7.58934 |
1810.09824 | Tim Morris Prof | Tim R. Morris and Roberto Percacci | Trace anomaly and infrared cutoffs | 23 pages, 2 figures; references added + extra discussion. Version to
appear in PRD | Phys. Rev. D 99, 105007 (2019) | 10.1103/PhysRevD.99.105007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Effective Average Action is a form of effective action which depends on a
cutoff scale suppressing the contribution of low momentum modes in the
functional integral. It reduces to the ordinary effective action when the
cutoff scale goes to zero. We derive the modifications of the scale Ward
identity due to this c... | [
{
"created": "Tue, 23 Oct 2018 13:00:26 GMT",
"version": "v1"
},
{
"created": "Sun, 19 May 2019 15:14:14 GMT",
"version": "v2"
}
] | 2019-05-22 | [
[
"Morris",
"Tim R.",
""
],
[
"Percacci",
"Roberto",
""
]
] | The Effective Average Action is a form of effective action which depends on a cutoff scale suppressing the contribution of low momentum modes in the functional integral. It reduces to the ordinary effective action when the cutoff scale goes to zero. We derive the modifications of the scale Ward identity due to this cut... | 12.29795 | 11.214989 | 11.482245 | 11.049896 | 10.90338 | 12.269366 | 10.770718 | 11.43721 | 9.970708 | 13.566475 | 11.54176 | 11.169128 | 11.118863 | 11.044317 | 10.631869 | 10.49945 | 11.1961 | 10.678106 | 11.333273 | 10.962789 | 10.339893 |
2305.15992 | Wenliang Li | Yongwei Guo, Wenliang Li | Solving anharmonic oscillator with null states: Hamiltonian bootstrap
and Dyson-Schwinger equations | v3: 54 pages, typos corrected, references updated, discussions
improved, Sec. 2.2 significantly expanded (high order results and comparison
to the nonperturbative null bootstrap added) | null | 10.1103/PhysRevD.108.125002 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As basic quantum mechanical models, anharmonic oscillators are recently
revisited by bootstrap methods. An effective approach is to make use of the
positivity constraints in Hermitian theories. There exists an alternative
avenue based on the null state condition, which applies to both Hermitian and
non-Hermitian theo... | [
{
"created": "Thu, 25 May 2023 12:31:00 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Sep 2023 22:07:56 GMT",
"version": "v2"
},
{
"created": "Sat, 2 Dec 2023 04:47:20 GMT",
"version": "v3"
}
] | 2023-12-05 | [
[
"Guo",
"Yongwei",
""
],
[
"Li",
"Wenliang",
""
]
] | As basic quantum mechanical models, anharmonic oscillators are recently revisited by bootstrap methods. An effective approach is to make use of the positivity constraints in Hermitian theories. There exists an alternative avenue based on the null state condition, which applies to both Hermitian and non-Hermitian theori... | 10.011293 | 9.783528 | 10.987596 | 9.962332 | 9.806064 | 9.830955 | 9.668797 | 10.014268 | 9.57336 | 11.080966 | 9.398582 | 9.502672 | 9.639152 | 9.343531 | 9.832887 | 9.485709 | 9.332007 | 9.332955 | 9.32488 | 9.933421 | 9.526789 |
hep-th/9501106 | Leonard Susskind | Leonard Susskind (Stanford University) | Trouble For Remnants | 6 pages, phyzzx | null | null | SU-ITP-95-1 | hep-th | null | An argument is presented for the inconsistency of black hole remnants which
store the information which falls into black holes. Unlike previous arguments
it is not concerned with a possible divergence in the rate of pair production.
It is argued that the existence of remnants in the thermal atmosphere of
Rindler spac... | [
{
"created": "Mon, 23 Jan 1995 22:14:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Susskind",
"Leonard",
"",
"Stanford University"
]
] | An argument is presented for the inconsistency of black hole remnants which store the information which falls into black holes. Unlike previous arguments it is not concerned with a possible divergence in the rate of pair production. It is argued that the existence of remnants in the thermal atmosphere of Rindler space ... | 17.313944 | 14.519562 | 16.651154 | 15.080166 | 14.97889 | 14.925268 | 16.072376 | 14.470881 | 14.235385 | 17.701956 | 13.570854 | 12.724943 | 15.899632 | 13.452833 | 14.278496 | 12.532016 | 13.488995 | 13.925797 | 13.960889 | 15.165972 | 13.764675 |
1801.06554 | Mario Martone | Philip C. Argyres and Mario Martone | Scaling dimensions of Coulomb branch operators of 4d N=2 superconformal
field theories | 6 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Under reasonable assumptions about the complex structure of the set of
singularities on the Coulomb branch of $\mathcal N=2$ superconformal field
theories, we present a relatively simple and elementary argument showing that
the scaling dimension, $\Delta$, of a Coulomb branch operator of a rank $r$
theory is allowed ... | [
{
"created": "Fri, 19 Jan 2018 19:09:46 GMT",
"version": "v1"
}
] | 2018-01-23 | [
[
"Argyres",
"Philip C.",
""
],
[
"Martone",
"Mario",
""
]
] | Under reasonable assumptions about the complex structure of the set of singularities on the Coulomb branch of $\mathcal N=2$ superconformal field theories, we present a relatively simple and elementary argument showing that the scaling dimension, $\Delta$, of a Coulomb branch operator of a rank $r$ theory is allowed to... | 6.404746 | 7.311516 | 7.262114 | 6.184048 | 6.893908 | 6.669462 | 6.901393 | 6.390036 | 6.265775 | 7.026521 | 5.978136 | 6.21484 | 6.39615 | 5.978402 | 6.184267 | 6.197298 | 6.041065 | 6.18013 | 6.053407 | 6.04469 | 5.883897 |
hep-th/0002056 | Chris Pope | M. Cvetic, H. Lu, C.N. Pope and A. Sadrzadeh | Consistency of Kaluza-Klein Sphere Reductions of Symmetric Potentials | Latex, 14 pages, minor corrections | Phys.Rev.D62:046005,2000 | 10.1103/PhysRevD.62.046005 | null | hep-th | null | In a recent paper, the complete (non-linear) Kaluza-Klein Ansatz for the
consistent embedding of certain scalar plus gravity subsectors of gauged
maximal supergravity in D=4, 5 and 7 was presented, in terms of sphere
reductions from D=11 or type IIB supergravity. The scalar fields included in
the truncations were the... | [
{
"created": "Mon, 7 Feb 2000 21:43:49 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Mar 2000 16:20:39 GMT",
"version": "v2"
},
{
"created": "Thu, 27 Apr 2000 22:40:31 GMT",
"version": "v3"
}
] | 2009-09-17 | [
[
"Cvetic",
"M.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Sadrzadeh",
"A.",
""
]
] | In a recent paper, the complete (non-linear) Kaluza-Klein Ansatz for the consistent embedding of certain scalar plus gravity subsectors of gauged maximal supergravity in D=4, 5 and 7 was presented, in terms of sphere reductions from D=11 or type IIB supergravity. The scalar fields included in the truncations were the d... | 8.67314 | 7.439723 | 10.857326 | 7.824175 | 8.878822 | 8.295976 | 8.047226 | 7.971568 | 7.907663 | 10.537225 | 8.021791 | 8.208669 | 9.028414 | 7.996451 | 8.042843 | 8.099467 | 8.189807 | 7.920425 | 8.027063 | 8.765352 | 8.01088 |
2011.01959 | Petr Kravchuk | Rajeev S. Erramilli, Luca V. Iliesiu, Petr Kravchuk, Walter Landry,
David Poland, David Simmons-Duffin | blocks_3d: Software for general 3d conformal blocks | 33 pages + appendices | null | 10.1007/JHEP11(2021)006 | CALT-TH 2020-048 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce the software blocks_3d for computing four-point conformal blocks
of operators with arbitrary Lorentz representations in 3d CFTs. It uses
Zamolodchikov-like recursion relations to numerically compute derivatives of
blocks around a crossing-symmetric configuration. It is implemented as a
heavily optimized,... | [
{
"created": "Tue, 3 Nov 2020 19:02:22 GMT",
"version": "v1"
}
] | 2021-11-24 | [
[
"Erramilli",
"Rajeev S.",
""
],
[
"Iliesiu",
"Luca V.",
""
],
[
"Kravchuk",
"Petr",
""
],
[
"Landry",
"Walter",
""
],
[
"Poland",
"David",
""
],
[
"Simmons-Duffin",
"David",
""
]
] | We introduce the software blocks_3d for computing four-point conformal blocks of operators with arbitrary Lorentz representations in 3d CFTs. It uses Zamolodchikov-like recursion relations to numerically compute derivatives of blocks around a crossing-symmetric configuration. It is implemented as a heavily optimized, m... | 12.71787 | 12.298683 | 13.520164 | 11.281917 | 11.489502 | 12.119019 | 11.164116 | 12.167731 | 11.243509 | 13.19811 | 12.313177 | 11.342332 | 11.410961 | 11.332169 | 11.491162 | 11.494948 | 11.172032 | 11.291687 | 11.24011 | 12.156596 | 11.793077 |
hep-th/9402084 | Timothy Hollowood | T.J. Hollowood | The exact mass-gaps of the principal chiral models | 11 pages, (macro included), CERN-TH.7164/94, SWAT/93-94/26 | Phys.Lett. B329 (1994) 450-456 | 10.1016/0370-2693(94)91089-8 | null | hep-th | null | An exact expression for the mass-gap, the ratio of the physical particle mass
to the $\Lambda$-parameter, is found for the principal chiral sigma models
associated to all the classical Lie algebras. The calculation is based on a
comparison of the free-energy in the presence of a source coupling to a
conserved charge ... | [
{
"created": "Tue, 15 Feb 1994 12:58:16 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Hollowood",
"T. J.",
""
]
] | An exact expression for the mass-gap, the ratio of the physical particle mass to the $\Lambda$-parameter, is found for the principal chiral sigma models associated to all the classical Lie algebras. The calculation is based on a comparison of the free-energy in the presence of a source coupling to a conserved charge of... | 6.562621 | 6.048615 | 7.911395 | 6.249841 | 6.057944 | 6.297787 | 6.336208 | 6.716702 | 5.970595 | 8.913249 | 6.573407 | 6.235889 | 7.087839 | 6.590636 | 6.145245 | 6.309217 | 6.155425 | 6.497076 | 6.38881 | 6.969166 | 6.529477 |
1212.0024 | Gianluca Inverso | Massimo Bianchi, Gianluca Inverso, Luca Martucci | Brane instantons and fluxes in F-theory | 61 pages; v2: references added and typos corrected | null | 10.1007/JHEP07(2013)037 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the combined effect of world-volume and background fluxes on
Euclidean D3-brane instantons in F-theory compactifications. We derive an
appropriate form of the fermionic effective action, in which the fermions are
topologically twisted and the dynamical effect of fluxes, non-trivial
axio-dilaton and warping i... | [
{
"created": "Fri, 30 Nov 2012 22:02:52 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Sep 2013 14:20:09 GMT",
"version": "v2"
}
] | 2015-06-12 | [
[
"Bianchi",
"Massimo",
""
],
[
"Inverso",
"Gianluca",
""
],
[
"Martucci",
"Luca",
""
]
] | We study the combined effect of world-volume and background fluxes on Euclidean D3-brane instantons in F-theory compactifications. We derive an appropriate form of the fermionic effective action, in which the fermions are topologically twisted and the dynamical effect of fluxes, non-trivial axio-dilaton and warping is ... | 7.831135 | 7.152421 | 8.786013 | 7.01666 | 6.835248 | 6.846539 | 7.260545 | 6.967527 | 7.009907 | 9.108974 | 6.820412 | 7.094934 | 7.980299 | 7.124744 | 7.087853 | 7.26918 | 7.267035 | 7.186947 | 7.252167 | 7.952445 | 7.090225 |
1701.07771 | Bret Underwood | S. Shajidul Haque and Bret Underwood | Consistent Cosmic Bubble Embeddings | 9 pages, 4 figures. v2: updated references. v3: matches published
version | Phys. Rev. D 95, 103513 (2017) | 10.1103/PhysRevD.95.103513 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Raychaudhuri equation for null rays is a powerful tool for finding
consistent embeddings of cosmological bubbles into a background spacetime in a
way that is largely independent of the matter content. We find that spatially
flat or positively curved thin wall bubbles surrounded by a cosmological
background must h... | [
{
"created": "Thu, 26 Jan 2017 16:53:05 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Feb 2017 23:27:18 GMT",
"version": "v2"
},
{
"created": "Wed, 31 May 2017 16:12:11 GMT",
"version": "v3"
}
] | 2017-06-01 | [
[
"Haque",
"S. Shajidul",
""
],
[
"Underwood",
"Bret",
""
]
] | The Raychaudhuri equation for null rays is a powerful tool for finding consistent embeddings of cosmological bubbles into a background spacetime in a way that is largely independent of the matter content. We find that spatially flat or positively curved thin wall bubbles surrounded by a cosmological background must hav... | 11.348454 | 13.537183 | 11.575606 | 10.98714 | 12.472286 | 12.480174 | 12.513988 | 10.708866 | 12.621985 | 11.435802 | 12.315737 | 11.359219 | 10.604934 | 10.490815 | 10.450977 | 11.197032 | 11.383364 | 10.559336 | 10.944775 | 10.77035 | 10.824273 |
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