id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1903.00773 | Andrei Mironov | A. Mironov and A. Morozov | Kerov functions for composite representations and Macdonald ideal | 26 pages | Nuclear Physics B 944 (2019) 114641 | 10.1016/j.nuclphysb.2019.114641 | FIAN/TD-01/19; IITP/TH-03/19; ITEP/TH-03/19 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Kerov functions provide an infinite-parametric deformation of the set of
Schur functions, which is a far-going generalization of the 2-parametric
Macdonald deformation. In this paper, we concentrate on a particular subject:
on Kerov functions labeled by the Young diagrams associated with the conjugate
and, more gener... | [
{
"created": "Sat, 2 Mar 2019 21:51:20 GMT",
"version": "v1"
}
] | 2019-05-28 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | Kerov functions provide an infinite-parametric deformation of the set of Schur functions, which is a far-going generalization of the 2-parametric Macdonald deformation. In this paper, we concentrate on a particular subject: on Kerov functions labeled by the Young diagrams associated with the conjugate and, more general... | 14.667566 | 14.79242 | 16.390703 | 13.46725 | 14.231167 | 14.231604 | 13.569331 | 13.78728 | 14.09164 | 15.977947 | 12.502025 | 13.025541 | 14.187996 | 13.650895 | 13.327009 | 12.556511 | 12.830655 | 13.05288 | 13.218071 | 14.301169 | 13.52079 |
2101.09820 | Tim Jones | I. Jack and D.R.T Jones | Anomalous dimensions at large charge in d=4 O(N) theory | 16 pages. 6 Figures. Typos corrected; references and an
acknowledgement added. Some minor errors corrected in a figure and equations | Phys. Rev. D 103, 085013 (2021) | 10.1103/PhysRevD.103.085013 | LTH 1252 | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Recently it was shown that the scaling dimension of the operator $\phi^n$ in
$\lambda(\phi^*\phi)^2$ theory may be computed semi-classically at the
Wilson-Fisher fixed point in $d=4-\epsilon$, for generic values of $\lambda n$
and this was verified to two loop order in perturbation theory at leading and
sub-leading $... | [
{
"created": "Sun, 24 Jan 2021 22:59:09 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Jan 2021 16:06:10 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Feb 2021 17:10:44 GMT",
"version": "v3"
},
{
"created": "Sat, 24 Apr 2021 17:35:29 GMT",
"version": "v4"
}
] | 2021-05-05 | [
[
"Jack",
"I.",
""
],
[
"Jones",
"D. R. T",
""
]
] | Recently it was shown that the scaling dimension of the operator $\phi^n$ in $\lambda(\phi^*\phi)^2$ theory may be computed semi-classically at the Wilson-Fisher fixed point in $d=4-\epsilon$, for generic values of $\lambda n$ and this was verified to two loop order in perturbation theory at leading and sub-leading $n$... | 7.677735 | 5.667058 | 7.538445 | 5.749609 | 4.870434 | 4.971314 | 5.025402 | 5.307929 | 5.764396 | 7.564371 | 5.903811 | 6.473771 | 6.769888 | 6.817988 | 6.295116 | 6.196761 | 6.210903 | 6.585371 | 6.371402 | 7.12077 | 6.311256 |
2104.12979 | Hernan Gonzalez | Hern\'an A. Gonz\'alez and Francisco Rojas | The structure of IR divergences in celestial gluon amplitudes | 28 pages, no figures (v2: minor corrections, references added) | null | 10.1007/JHEP06(2021)171 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The all-loop resummation of SU$(N)$ gauge theory amplitudes is known to
factorize into an IR-divergent (soft and collinear) factor and a finite (hard)
piece. The divergent factor is universal, whereas the hard function is a
process-dependent quantity. We prove that this factorization persists for the
corresponding ce... | [
{
"created": "Tue, 27 Apr 2021 05:01:28 GMT",
"version": "v1"
},
{
"created": "Sun, 9 May 2021 17:45:44 GMT",
"version": "v2"
}
] | 2021-07-14 | [
[
"González",
"Hernán A.",
""
],
[
"Rojas",
"Francisco",
""
]
] | The all-loop resummation of SU$(N)$ gauge theory amplitudes is known to factorize into an IR-divergent (soft and collinear) factor and a finite (hard) piece. The divergent factor is universal, whereas the hard function is a process-dependent quantity. We prove that this factorization persists for the corresponding cele... | 5.37423 | 7.949524 | 7.808577 | 7.476414 | 7.921298 | 7.380638 | 7.787557 | 7.704199 | 7.115596 | 8.123426 | 7.289584 | 6.921662 | 7.010939 | 6.89313 | 7.070285 | 6.786493 | 6.914773 | 6.829754 | 6.882676 | 6.811864 | 6.816712 |
0801.1933 | Takehisa Fujita | Takehisa Fujita | Critical Review of Path Integral Formulation | 14 pages, no figure | null | null | null | hep-th | null | The path integral formulation in quantum mechanics corresponds to the first
quantization since it is just to rewrite the quantum mechanical amplitude into
many dimensional integrations over discretized coordinates $x_n$. However, the
path integral expression cannot be connected to the dynamics of classical
mechanics,... | [
{
"created": "Sun, 13 Jan 2008 04:28:38 GMT",
"version": "v1"
}
] | 2008-01-15 | [
[
"Fujita",
"Takehisa",
""
]
] | The path integral formulation in quantum mechanics corresponds to the first quantization since it is just to rewrite the quantum mechanical amplitude into many dimensional integrations over discretized coordinates $x_n$. However, the path integral expression cannot be connected to the dynamics of classical mechanics, e... | 13.126817 | 14.023061 | 12.767537 | 13.084256 | 13.858925 | 14.846128 | 14.073349 | 14.791313 | 13.692395 | 14.833848 | 12.316604 | 12.262275 | 12.238144 | 11.997563 | 12.153808 | 12.181262 | 12.64912 | 12.260199 | 12.331388 | 12.314636 | 11.793808 |
0905.4463 | Heng-Yu Chen HYC | Heng-Yu Chen, Yu Nakayama and Gary Shiu | On D3-brane Dynamics at Strong Warping | 19 pages, No figures | Int.J.Mod.Phys.A25:2493-2513,2010 | 10.1142/S0217751X10048366 | MAD-TH-09-02, UCB-PTH-09-15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the dynamics of a D3 brane in generic IIB warped compactifications,
using the Hamiltonian formulation discussed in arXiv:0805.3700 [hep-th]. Taking
into account of both closed and open string fluctuations, we derive the warped
Kahler potential governing the motion of a probe D3 brane. By including the
backre... | [
{
"created": "Wed, 27 May 2009 18:53:05 GMT",
"version": "v1"
}
] | 2010-05-25 | [
[
"Chen",
"Heng-Yu",
""
],
[
"Nakayama",
"Yu",
""
],
[
"Shiu",
"Gary",
""
]
] | We study the dynamics of a D3 brane in generic IIB warped compactifications, using the Hamiltonian formulation discussed in arXiv:0805.3700 [hep-th]. Taking into account of both closed and open string fluctuations, we derive the warped Kahler potential governing the motion of a probe D3 brane. By including the backreac... | 9.787674 | 7.766099 | 10.600107 | 8.232118 | 8.708111 | 7.817543 | 7.601841 | 8.015027 | 8.108356 | 11.272839 | 8.661716 | 8.36257 | 9.94914 | 8.690484 | 8.743432 | 8.445306 | 8.200479 | 8.536119 | 8.424925 | 9.130309 | 8.49771 |
hep-th/0606020 | Cliff Burgess | C.P. Burgess | Strings, Branes and Cosmology: What can we hope to learn? | Some references added; Invited contribution to the 40th Rencontres de
Moriond, La Thuile, March 2006. (LaTeX 10 pages) | null | null | null | hep-th | null | This article briefly summarizes the motivations for -- and recent progress in
-- searching for cosmological configurations within string theory, with a focus
on how much we might reasonably hope to learn about fundamental physics from
precision cosmological measurements.
| [
{
"created": "Fri, 2 Jun 2006 18:16:57 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Jan 2007 02:08:46 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Burgess",
"C. P.",
""
]
] | This article briefly summarizes the motivations for -- and recent progress in -- searching for cosmological configurations within string theory, with a focus on how much we might reasonably hope to learn about fundamental physics from precision cosmological measurements. | 16.345224 | 12.933189 | 11.830988 | 11.958681 | 11.621087 | 11.788674 | 12.385137 | 12.33687 | 12.601563 | 11.510315 | 11.438213 | 12.647263 | 12.640591 | 12.631017 | 11.93778 | 12.350516 | 12.728606 | 12.679 | 13.084282 | 12.780158 | 13.028424 |
1306.3565 | Aleksey Milekhin | A. Gorsky, A. Milekhin | The CP(N-1) model on a Disc and Decay of a Non-Abelian String | null | Phys. Rev. D 88, 085017 (2013) | 10.1103/PhysRevD.88.085017 | ITEP-TH-12/13 | hep-th cond-mat.mes-hall cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the role of quantum effects in the non-perturbative decay of
non-abelian string with orientational moduli in non-supersymmetric D=4 gauge
theory. To this aim the effective action in the $CP(N-1)$ model on a disc at
large N has been calculated. It exhibits phase transition at some radius, the
"wrong sign" ... | [
{
"created": "Sat, 15 Jun 2013 11:35:51 GMT",
"version": "v1"
}
] | 2013-10-30 | [
[
"Gorsky",
"A.",
""
],
[
"Milekhin",
"A.",
""
]
] | We consider the role of quantum effects in the non-perturbative decay of non-abelian string with orientational moduli in non-supersymmetric D=4 gauge theory. To this aim the effective action in the $CP(N-1)$ model on a disc at large N has been calculated. It exhibits phase transition at some radius, the "wrong sign" Lu... | 16.14492 | 16.789591 | 17.314613 | 13.238938 | 14.514297 | 15.004598 | 16.665472 | 15.281983 | 14.176269 | 16.562349 | 14.628501 | 15.226564 | 15.857828 | 14.985556 | 15.042525 | 15.312988 | 15.122143 | 15.276803 | 14.717027 | 15.24823 | 15.208115 |
1605.04595 | Vahid Reza Shajiee | Jafar Sadeghi, Vahid Reza Shajiee | Quantum Tunneling from the Charged Non-Rotating BTZ Black Hole with GUP | 9 pages, Version accepted for publication in EPJ Plus | Eur.Phys.J.Plus 132 (2017) no.3, 132 | 10.1140/epjp/i2017-11432-x | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper, the quantum corrections to the temperature, entropy and
specific heat capacity of the charged non-rotating BTZ black hole are studied
by generalized uncertainty principle in tunneling formalism. It is shown that
quantum corrected entropy would be of the form of predicted entropy in quantum
gravi... | [
{
"created": "Sun, 15 May 2016 19:15:23 GMT",
"version": "v1"
},
{
"created": "Fri, 20 May 2016 14:36:55 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Mar 2017 21:52:14 GMT",
"version": "v3"
}
] | 2019-02-04 | [
[
"Sadeghi",
"Jafar",
""
],
[
"Shajiee",
"Vahid Reza",
""
]
] | In the present paper, the quantum corrections to the temperature, entropy and specific heat capacity of the charged non-rotating BTZ black hole are studied by generalized uncertainty principle in tunneling formalism. It is shown that quantum corrected entropy would be of the form of predicted entropy in quantum gravity... | 8.716669 | 7.769646 | 7.650755 | 7.435995 | 8.51247 | 8.623655 | 7.994373 | 8.016497 | 8.159807 | 8.872488 | 8.248285 | 7.913187 | 8.243933 | 8.044842 | 8.275437 | 8.307733 | 8.446858 | 7.922531 | 8.041062 | 8.50406 | 7.798264 |
1303.1575 | Elena-Mirela Babalic Dr | Elena-Mirela Babalic, Ioana-Alexandra Coman, Calin Iuliu Lazaroiu | A unified approach to Fierz identities | 6 pages, 5 tables, proceedings for TIM-12 Conference of Physics | AIP Conf. Proc. 1564, 57 (2013) | 10.1063/1.4832796 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We summarize a unified and computationally efficient treatment of Fierz
identities for form-valued pinor bilinears in various dimensions and
signatures, using concepts and techniques borrowed from a certain approach to
spinors known as geometric algebra. Our formulation displays the real, complex
and quaternionic str... | [
{
"created": "Thu, 7 Mar 2013 00:01:44 GMT",
"version": "v1"
}
] | 2016-11-08 | [
[
"Babalic",
"Elena-Mirela",
""
],
[
"Coman",
"Ioana-Alexandra",
""
],
[
"Lazaroiu",
"Calin Iuliu",
""
]
] | We summarize a unified and computationally efficient treatment of Fierz identities for form-valued pinor bilinears in various dimensions and signatures, using concepts and techniques borrowed from a certain approach to spinors known as geometric algebra. Our formulation displays the real, complex and quaternionic struc... | 17.394972 | 13.193938 | 17.740488 | 14.219636 | 14.901943 | 13.725266 | 13.370991 | 14.171791 | 14.10018 | 17.091778 | 14.081561 | 14.728639 | 17.053923 | 15.185198 | 15.903979 | 15.089435 | 15.037406 | 14.503584 | 15.564887 | 16.348112 | 14.857131 |
1512.04607 | Dmitri Gal'tsov | Dmitry Gal'tsov, Elena Melkumova and Pavel Spirin | Branestrahlung: radiation in the particle-brane collision | 18 pages revtex4, 3 figures, journal version | Phys. Rev. D 93, 045018 (2016) | 10.1103/PhysRevD.93.045018 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the radiation accompanying gravitational collision of the domain
wall and the point particle in five-dimensional spacetime. This process, which
can be regarded as brane-particle bremsstrahlung, here called {\it
branestrahlung}, has unusual features. Since the brane has intrinsic dynamics,
it gets excited... | [
{
"created": "Mon, 14 Dec 2015 23:52:25 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Mar 2016 10:37:55 GMT",
"version": "v2"
}
] | 2016-03-31 | [
[
"Gal'tsov",
"Dmitry",
""
],
[
"Melkumova",
"Elena",
""
],
[
"Spirin",
"Pavel",
""
]
] | We calculate the radiation accompanying gravitational collision of the domain wall and the point particle in five-dimensional spacetime. This process, which can be regarded as brane-particle bremsstrahlung, here called {\it branestrahlung}, has unusual features. Since the brane has intrinsic dynamics, it gets excited i... | 13.513771 | 14.167976 | 13.241148 | 13.355646 | 12.957467 | 12.589327 | 13.573172 | 13.22964 | 13.238338 | 15.170934 | 12.710601 | 12.854654 | 13.125522 | 13.080282 | 13.092959 | 13.141557 | 13.222364 | 12.723038 | 13.198349 | 13.288041 | 13.058567 |
2002.04341 | Mikhail Plyushchay | Luis Inzunza, Mikhail S. Plyushchay, Andreas Wipf | Hidden symmetry and (super)conformal mechanics in a monopole background | 43 pages, 4 figures | JHEP 2004 (2020) 028 | 10.1007/JHEP04(2020)028 | null | hep-th math-ph math.MP nlin.SI quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study classical and quantum hidden symmetries of a particle with electric
charge $e$ in the background of a Dirac monopole of magnetic charge $g$
subjected to an additional central potential $V(r)=U(r) +(eg)^2/2mr^{2}$ with
$U(r)=\tfrac{1}{2}m\omega^2r^2$, similar to that in the one-dimensional
conformal mechanics... | [
{
"created": "Tue, 11 Feb 2020 12:14:38 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Feb 2020 10:53:03 GMT",
"version": "v2"
},
{
"created": "Mon, 16 Mar 2020 03:50:09 GMT",
"version": "v3"
},
{
"created": "Thu, 9 Apr 2020 01:59:05 GMT",
"version": "v4"
}
] | 2020-04-13 | [
[
"Inzunza",
"Luis",
""
],
[
"Plyushchay",
"Mikhail S.",
""
],
[
"Wipf",
"Andreas",
""
]
] | We study classical and quantum hidden symmetries of a particle with electric charge $e$ in the background of a Dirac monopole of magnetic charge $g$ subjected to an additional central potential $V(r)=U(r) +(eg)^2/2mr^{2}$ with $U(r)=\tfrac{1}{2}m\omega^2r^2$, similar to that in the one-dimensional conformal mechanics m... | 6.126893 | 6.215686 | 6.396358 | 5.762737 | 6.220086 | 5.692721 | 6.259006 | 6.100252 | 5.773098 | 6.814548 | 5.712904 | 6.044211 | 6.159285 | 5.902457 | 6.054898 | 6.001409 | 6.008333 | 5.779793 | 5.993544 | 6.196964 | 5.811714 |
hep-th/9803120 | Shyamoli Chaudhuri | S.Chaudhuri and D. Minic | On the Hagedorn Transition and Collective Dynamics of D0-branes | 11 pages, plain TeX, minor comment and references added, version to
appear in Phys. Lett. B | Phys.Lett. B433 (1998) 301-306 | 10.1016/S0370-2693(98)00703-5 | null | hep-th | null | Banks, Fischler, Klebanov and Susskind have proposed a model for black hole
thermodynamics based on the principle that the entropy is of order the number
of particles at the phase transition point in a Boltzmann gas of D0-branes. We
show that the deviations from Boltzmann scaling found in $d<6$ noncompact
spatial dim... | [
{
"created": "Fri, 13 Mar 1998 23:34:25 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Apr 1998 13:32:06 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Jun 1998 18:34:32 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Chaudhuri",
"S.",
""
],
[
"Minic",
"D.",
""
]
] | Banks, Fischler, Klebanov and Susskind have proposed a model for black hole thermodynamics based on the principle that the entropy is of order the number of particles at the phase transition point in a Boltzmann gas of D0-branes. We show that the deviations from Boltzmann scaling found in $d<6$ noncompact spatial dimen... | 9.400045 | 7.54982 | 8.817876 | 7.166931 | 7.082115 | 7.58689 | 8.18001 | 7.249257 | 7.299801 | 9.529947 | 7.961452 | 7.083038 | 7.757107 | 7.209875 | 7.155041 | 7.119872 | 7.024271 | 7.446489 | 7.168424 | 7.594265 | 7.360843 |
1910.04741 | Suddhasattwa Brahma | Suddhasattwa Brahma | Trans-Planckian censorship, inflation and excited initial states for
perturbations | 15 pages, comments welcome; typos corrected, refs added & minor
revisions; v3: matches published version | Phys. Rev. D 101, 023526 (2020) | 10.1103/PhysRevD.101.023526 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The recently proposed trans-Planckian censorship conjecture (TCC) seems to
require that the energy scale of inflation is significantly lower than the
Planck scale $(H_\text{inf}<10^{-20} \Mpl)$. This, in turn, implies that the
tensor-to-scalar ratio for inflation is negligibly small, \textit{independent}
of assumptio... | [
{
"created": "Thu, 10 Oct 2019 17:51:16 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Oct 2019 20:40:00 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Feb 2020 18:17:23 GMT",
"version": "v3"
}
] | 2020-02-10 | [
[
"Brahma",
"Suddhasattwa",
""
]
] | The recently proposed trans-Planckian censorship conjecture (TCC) seems to require that the energy scale of inflation is significantly lower than the Planck scale $(H_\text{inf}<10^{-20} \Mpl)$. This, in turn, implies that the tensor-to-scalar ratio for inflation is negligibly small, \textit{independent} of assumptions... | 7.391918 | 8.098701 | 7.396328 | 6.796031 | 7.411019 | 7.20457 | 8.344181 | 7.51253 | 6.849512 | 7.275735 | 7.443463 | 7.286113 | 7.134948 | 6.915535 | 7.16729 | 7.065607 | 7.302418 | 7.082651 | 6.944151 | 6.875343 | 6.902601 |
hep-th/0302039 | Arkady A. Popov | Arkady A. Popov | Analytical approximation of the stress-energy tensor of a quantized
scalar field in static spherically symmetric spacetimes | revtex4, 17 pages; v2: three references added | Phys.Rev.D67:044021,2003 | 10.1103/PhysRevD.67.044021 | null | hep-th gr-qc | null | Analytical approximations for ${< \phi^2 >}$ and ${< T^{\mu}_{\nu} >}$ of a
quantized scalar field in static spherically symmetric spacetimes are obtained.
The field is assumed to be both massive and massless, with an arbitrary
coupling $\xi$ to the scalar curvature, and in a zero temperature vacuum state.
The expres... | [
{
"created": "Thu, 6 Feb 2003 13:33:39 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Feb 2003 20:35:40 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Popov",
"Arkady A.",
""
]
] | Analytical approximations for ${< \phi^2 >}$ and ${< T^{\mu}_{\nu} >}$ of a quantized scalar field in static spherically symmetric spacetimes are obtained. The field is assumed to be both massive and massless, with an arbitrary coupling $\xi$ to the scalar curvature, and in a zero temperature vacuum state. The expressi... | 4.261672 | 3.688214 | 3.700724 | 3.370324 | 3.422975 | 3.186546 | 3.4635 | 3.30519 | 3.651935 | 3.754416 | 3.691284 | 3.988679 | 3.801412 | 3.801062 | 3.810482 | 3.908087 | 4.010372 | 3.749576 | 3.993427 | 3.928348 | 3.882263 |
2009.00737 | Dionisio Bazeia | D. Bazeia, A. Mohammadi, D.C. Moreira | Fermions in the presence of topological structures under geometric
constrictions | 8 pages, 7 figures; v2, new results and references added. To appear
in PRD | Phys. Rev. D 103, 025003 (2021) | 10.1103/PhysRevD.103.025003 | null | hep-th cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study modifications of the spectrum of fermions interacting
with kinklike structures in two-dimensional spacetime. We consider the Yukawa
coupling between fermions and scalar fields that engender nontrivial internal
structure and investigate how the fermion spectra change in terms of the
parameters th... | [
{
"created": "Tue, 1 Sep 2020 22:52:00 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Dec 2020 17:08:37 GMT",
"version": "v2"
}
] | 2021-01-13 | [
[
"Bazeia",
"D.",
""
],
[
"Mohammadi",
"A.",
""
],
[
"Moreira",
"D. C.",
""
]
] | In this work we study modifications of the spectrum of fermions interacting with kinklike structures in two-dimensional spacetime. We consider the Yukawa coupling between fermions and scalar fields that engender nontrivial internal structure and investigate how the fermion spectra change in terms of the parameters that... | 11.873949 | 8.911027 | 10.865928 | 9.67292 | 9.521748 | 8.884776 | 8.278695 | 9.957656 | 9.189772 | 11.931944 | 9.696056 | 10.346552 | 11.090175 | 10.060229 | 10.49004 | 10.488116 | 9.843076 | 10.415399 | 10.317836 | 11.043564 | 10.330692 |
2308.16247 | Shraiyance Jain | Abhijit Gadde, Shraiyance Jain, Vineeth Krishna, Harshal Kulkarni,
Trakshu Sharma | Monotonicity conjecture for multi-party entanglement I | 40 Pages, 10 Figures | null | 10.1007/JHEP02(2024)025 | null | hep-th quant-ph | http://creativecommons.org/licenses/by/4.0/ | In this paper, we conjecture a monotonicity property that we call
monotonicity under coarse-graining for a class of multi-partite entanglement
measures. We check these properties by computing the measures for various types
of states using different methods.
| [
{
"created": "Wed, 30 Aug 2023 18:10:09 GMT",
"version": "v1"
}
] | 2024-02-07 | [
[
"Gadde",
"Abhijit",
""
],
[
"Jain",
"Shraiyance",
""
],
[
"Krishna",
"Vineeth",
""
],
[
"Kulkarni",
"Harshal",
""
],
[
"Sharma",
"Trakshu",
""
]
] | In this paper, we conjecture a monotonicity property that we call monotonicity under coarse-graining for a class of multi-partite entanglement measures. We check these properties by computing the measures for various types of states using different methods. | 11.044794 | 10.166403 | 9.424311 | 8.515369 | 9.243279 | 10.21353 | 10.470733 | 9.723042 | 9.843081 | 10.046059 | 8.973507 | 8.99922 | 9.893861 | 9.062236 | 9.565916 | 9.207496 | 9.287057 | 9.746172 | 8.941048 | 10.136379 | 9.072426 |
hep-th/9312091 | D. V. Ahluwalia, Lanl | D. V. Ahluwalia, T. Goldman, and M. B. Johnson | (J,0)+(0,j) Representation Space: Majorana-Like Construct | Los Alamos Natioanl Laboratory Preprint LA-UR-93-4316 | Acta Phys.Polon.B25:1267-1278,1994 | null | null | hep-th | null | This is second of the two invited lectures presented (by D. V. Ahluwalia) at
the ``XVII International School of Theoretical Physics: Standard Model and
Beyond' 93.'' The text is essentially based on a recent publication by the
present authors [Mod. Phys. Lett. A (in press)]. Here, after briefly reviewing
the $(j,0)\o... | [
{
"created": "Sat, 11 Dec 1993 00:36:39 GMT",
"version": "v1"
}
] | 2010-05-27 | [
[
"Ahluwalia",
"D. V.",
""
],
[
"Goldman",
"T.",
""
],
[
"Johnson",
"M. B.",
""
]
] | This is second of the two invited lectures presented (by D. V. Ahluwalia) at the ``XVII International School of Theoretical Physics: Standard Model and Beyond' 93.'' The text is essentially based on a recent publication by the present authors [Mod. Phys. Lett. A (in press)]. Here, after briefly reviewing the $(j,0)\opl... | 9.300456 | 5.960042 | 8.64399 | 6.282753 | 8.617604 | 8.488418 | 8.281512 | 6.357488 | 5.793597 | 9.537911 | 6.306065 | 7.779418 | 8.131427 | 7.206407 | 7.779919 | 8.556208 | 8.159963 | 7.69693 | 7.495828 | 8.079049 | 7.574552 |
hep-th/0605208 | W. F. Kao | W.F. Kao | Anisotropic higher derivative gravity and inflationary universe | 9 pages | Phys.Rev. D74 (2006) 043522 | 10.1103/PhysRevD.74.043522 | null | hep-th | null | Stability analysis of the Kantowski-Sachs type universe in pure higher
derivative gravity theory is studied in details. The non-redundant generalized
Friedmann equation of the system is derived by introducing a reduced one
dimensional generalized KS type action. This method greatly reduces the labor
in deriving field... | [
{
"created": "Sun, 21 May 2006 20:58:04 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Kao",
"W. F.",
""
]
] | Stability analysis of the Kantowski-Sachs type universe in pure higher derivative gravity theory is studied in details. The non-redundant generalized Friedmann equation of the system is derived by introducing a reduced one dimensional generalized KS type action. This method greatly reduces the labor in deriving field e... | 19.602139 | 14.352026 | 17.251205 | 15.886453 | 17.671509 | 17.568624 | 17.362902 | 15.257518 | 14.736771 | 18.62553 | 15.779416 | 16.809568 | 16.315409 | 16.208033 | 16.166071 | 16.556652 | 16.594374 | 15.870245 | 15.861538 | 16.455353 | 16.436617 |
1609.03651 | Chen-Te Ma | Chen-Te Ma | Discussion of Entanglement Entropy in Quantum Gravity | 10 pages, minor changes, references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study entanglement entropy in gravity theory with quantum effects. A
simplest model is a two dimensional Einstein-Hilbert action . We use an
$n$-sheet manifold to obtain an area term of entanglement entropy by summing
over all background fields. A strongly coupled conformal field theory is
expected to describe per... | [
{
"created": "Tue, 13 Sep 2016 01:15:42 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Sep 2016 10:45:31 GMT",
"version": "v2"
},
{
"created": "Sat, 9 Sep 2017 14:27:14 GMT",
"version": "v3"
}
] | 2017-09-12 | [
[
"Ma",
"Chen-Te",
""
]
] | We study entanglement entropy in gravity theory with quantum effects. A simplest model is a two dimensional Einstein-Hilbert action . We use an $n$-sheet manifold to obtain an area term of entanglement entropy by summing over all background fields. A strongly coupled conformal field theory is expected to describe pertu... | 11.140765 | 10.633794 | 12.058004 | 10.675843 | 10.837693 | 10.418018 | 10.980556 | 10.674513 | 10.573255 | 12.706996 | 10.720935 | 11.153312 | 11.551832 | 10.793298 | 10.599079 | 10.317986 | 10.918961 | 10.782097 | 10.999381 | 11.386044 | 11.142813 |
0803.2876 | Mirjam Cvetic | Mirjam Cvetic and Paul Langacker | D-Instanton Generated Dirac Neutrino Masses | 4 pages, 1 figure minor corrections, the version to be published in
Phys. Rev. D | Phys.Rev.D78:066012,2008 | 10.1103/PhysRevD.78.066012 | UPR-1193-T | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a stringy mechanism to generate Dirac neutrino masses by
D-instantons in an experimentally relevant mass scale without fine-tuning.
Within Type IIA string theory with intersecting D6-branes, we spell out
specific conditions for the emergence of such couplings and provide a class of
supersymmetric local SU(... | [
{
"created": "Wed, 19 Mar 2008 19:59:04 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Sep 2008 00:55:08 GMT",
"version": "v2"
}
] | 2009-02-23 | [
[
"Cvetic",
"Mirjam",
""
],
[
"Langacker",
"Paul",
""
]
] | We present a stringy mechanism to generate Dirac neutrino masses by D-instantons in an experimentally relevant mass scale without fine-tuning. Within Type IIA string theory with intersecting D6-branes, we spell out specific conditions for the emergence of such couplings and provide a class of supersymmetric local SU(5)... | 8.027651 | 8.568542 | 8.870876 | 8.272159 | 8.893167 | 8.335611 | 8.238498 | 8.059506 | 7.434304 | 8.514165 | 7.806803 | 7.483801 | 7.805461 | 7.607722 | 7.515624 | 7.697283 | 7.40155 | 7.56987 | 7.47674 | 8.026324 | 7.53001 |
0704.0212 | Krzysztof Turzynski | Z. Lalak, D. Langlois, S. Pokorski, K. Turzynski | Curvature and isocurvature perturbations in two-field inflation | 29 pages, 12 figures; v2: updated references, discussion extended,
matches the published version | JCAP 0707:014,2007 | 10.1088/1475-7516/2007/07/014 | null | hep-th astro-ph gr-qc | null | We study cosmological perturbations in two-field inflation, allowing for
non-standard kinetic terms. We calculate analytically the spectra of curvature
and isocurvature modes at Hubble crossing, up to first order in the slow-roll
parameters. We also compute numerically the evolution of the curvature and
isocurvature ... | [
{
"created": "Mon, 2 Apr 2007 15:12:23 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Jul 2007 19:45:32 GMT",
"version": "v2"
}
] | 2009-11-13 | [
[
"Lalak",
"Z.",
""
],
[
"Langlois",
"D.",
""
],
[
"Pokorski",
"S.",
""
],
[
"Turzynski",
"K.",
""
]
] | We study cosmological perturbations in two-field inflation, allowing for non-standard kinetic terms. We calculate analytically the spectra of curvature and isocurvature modes at Hubble crossing, up to first order in the slow-roll parameters. We also compute numerically the evolution of the curvature and isocurvature mo... | 5.631414 | 5.419532 | 5.71734 | 5.704678 | 5.647173 | 5.378848 | 5.96816 | 5.0895 | 5.747343 | 6.098997 | 5.284878 | 5.399602 | 5.400239 | 5.21294 | 5.327832 | 5.353085 | 5.467796 | 5.179064 | 5.304608 | 5.290324 | 5.183693 |
0809.0085 | Antonio Capolupo Dr | A.Capolupo, S.Capozziello, G.Vitiello | Dark energy and particle mixing | 11 pages | Phys.Lett.A373:601-610,2009 | 10.1016/j.physleta.2008.12.018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the vacuum condensate due to particle mixing is responsible of a
dynamically evolving dark energy. In particular, we show that values of the
adiabatic index close to -1 for vacuum condensates of neutrinos and quarks
imply, at the present epoch, contributions to the vacuum energy compatible with
the estim... | [
{
"created": "Sat, 30 Aug 2008 19:26:12 GMT",
"version": "v1"
}
] | 2009-02-02 | [
[
"Capolupo",
"A.",
""
],
[
"Capozziello",
"S.",
""
],
[
"Vitiello",
"G.",
""
]
] | We show that the vacuum condensate due to particle mixing is responsible of a dynamically evolving dark energy. In particular, we show that values of the adiabatic index close to -1 for vacuum condensates of neutrinos and quarks imply, at the present epoch, contributions to the vacuum energy compatible with the estimat... | 13.27824 | 10.35638 | 11.93401 | 11.908873 | 12.197371 | 12.965285 | 11.007132 | 11.628373 | 11.715284 | 12.749219 | 10.537436 | 12.608791 | 12.426611 | 11.501536 | 12.297968 | 12.240598 | 11.968844 | 12.468973 | 11.529585 | 11.001142 | 12.5582 |
1308.3844 | Fa-Min Chen | Fa-Min Chen | OSp(4|4) superconformal currents in three-dimensional N=4 Chern-Simons
quiver gauge theories | 23 pages, published in PRD | Phys. Rev. D 87, 085007 (2013) | 10.1103/PhysRevD.87.085007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove explicitly that the general D=3, N=4 Chern-Simons-matter (CSM)
theory has a complete OSp(4|4) superconformal symmetry, and construct the
corresponding conserved currents. We re-derive the OSp(5|4) superconformal
currents in the general N=5 theory as special cases of the OSp(4|4) currents by
enhancing the sup... | [
{
"created": "Sun, 18 Aug 2013 08:53:02 GMT",
"version": "v1"
}
] | 2013-08-20 | [
[
"Chen",
"Fa-Min",
""
]
] | We prove explicitly that the general D=3, N=4 Chern-Simons-matter (CSM) theory has a complete OSp(4|4) superconformal symmetry, and construct the corresponding conserved currents. We re-derive the OSp(5|4) superconformal currents in the general N=5 theory as special cases of the OSp(4|4) currents by enhancing the super... | 4.681301 | 3.997958 | 5.256481 | 4.002001 | 3.824085 | 3.800411 | 3.917551 | 4.303308 | 4.174923 | 5.636065 | 4.121244 | 4.2089 | 4.638023 | 4.317595 | 4.183346 | 4.159997 | 4.04658 | 4.230295 | 4.279257 | 4.791093 | 4.172143 |
2011.05305 | Jordan Wilson-Gerow | Jordan Wilson-Gerow, P.C.E. Stamp | Gauge Invariant Propagators and States in Quantum Electrodynamics | 24 pages, 3 figures | Annals of Physics, Volume 442, 2022, 168898 | 10.1016/j.aop.2022.168898 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study gauge invariant states in QED, where states are understood in terms
of data living on the boundary of gauge invariant path-integrals. This is done
for both scalar and spinor QED, and for boundaries that are either time slices,
or the boundaries of a 'causal diamond'. We discuss both the case where the
gauge ... | [
{
"created": "Tue, 10 Nov 2020 18:43:01 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Oct 2023 18:45:42 GMT",
"version": "v2"
}
] | 2023-10-30 | [
[
"Wilson-Gerow",
"Jordan",
""
],
[
"Stamp",
"P. C. E.",
""
]
] | We study gauge invariant states in QED, where states are understood in terms of data living on the boundary of gauge invariant path-integrals. This is done for both scalar and spinor QED, and for boundaries that are either time slices, or the boundaries of a 'causal diamond'. We discuss both the case where the gauge fi... | 11.46935 | 11.611762 | 12.383511 | 11.081542 | 11.889742 | 11.185649 | 11.659155 | 11.088172 | 10.919037 | 13.189523 | 10.87766 | 10.822229 | 11.456336 | 10.951226 | 11.157413 | 10.848099 | 10.696815 | 10.800179 | 11.053838 | 11.431011 | 10.797911 |
1210.2855 | Teruhiko Kawano | Yasutaka Fukuda, Teruhiko Kawano, Nariaki Matsumiya | 5D SYM and 2D q-Deformed YM | 32 pages; v2: one reference added and minor corrections; v3: minor
corrections | null | 10.1016/j.nuclphysb.2012.12.017 | UT-12-33 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the AGT-like conjectured relation of a four-dimensional gauge theory
on the direct product of a three-sphere and a circle to two-dimensional
q-deformed Yang-Mills theory on a Riemann surface by using a five-dimensional
N=2 supersymmetric Yang-Mills theory on the direct product of the three-sphere
and the Rie... | [
{
"created": "Wed, 10 Oct 2012 10:03:32 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Oct 2012 06:46:06 GMT",
"version": "v2"
},
{
"created": "Thu, 17 Jan 2013 02:51:50 GMT",
"version": "v3"
}
] | 2015-06-11 | [
[
"Fukuda",
"Yasutaka",
""
],
[
"Kawano",
"Teruhiko",
""
],
[
"Matsumiya",
"Nariaki",
""
]
] | We study the AGT-like conjectured relation of a four-dimensional gauge theory on the direct product of a three-sphere and a circle to two-dimensional q-deformed Yang-Mills theory on a Riemann surface by using a five-dimensional N=2 supersymmetric Yang-Mills theory on the direct product of the three-sphere and the Riema... | 5.325166 | 4.974769 | 5.569485 | 4.493223 | 5.030495 | 5.130609 | 4.842537 | 4.834737 | 4.403535 | 6.138044 | 4.798387 | 4.732473 | 5.388917 | 4.897765 | 4.837366 | 4.832685 | 4.962399 | 4.713057 | 4.872199 | 5.422116 | 4.804274 |
1501.05336 | \"Ozg\"ur Acik | \"Ozg\"ur A\c{c}{\i}k, \"Umit Ertem | Higher-degree Dirac Currents of Twistor and Killing Spinors in
Supergravity Theories | 18 pages, published version | Class. Quantum Grav. 32 (2015) 175007 | 10.1088/0264-9381/32/17/175007 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that higher degree Dirac currents of twistor and Killing spinors
correspond to the hidden symmetries of the background spacetime which are
generalizations of conformal Killing and Killing vector fields respectively.
They are the generalizations of 1-form Dirac currents to higher degrees which
are used in cons... | [
{
"created": "Wed, 21 Jan 2015 21:48:33 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Aug 2015 09:38:31 GMT",
"version": "v2"
}
] | 2015-08-17 | [
[
"Açık",
"Özgür",
""
],
[
"Ertem",
"Ümit",
""
]
] | We show that higher degree Dirac currents of twistor and Killing spinors correspond to the hidden symmetries of the background spacetime which are generalizations of conformal Killing and Killing vector fields respectively. They are the generalizations of 1-form Dirac currents to higher degrees which are used in constr... | 8.891627 | 9.615922 | 9.291646 | 9.131764 | 9.942698 | 9.893323 | 9.488392 | 9.512339 | 8.957495 | 10.072121 | 8.728786 | 8.984541 | 9.155196 | 8.880489 | 8.810826 | 8.892859 | 9.049356 | 8.878418 | 8.696764 | 9.341664 | 8.845201 |
2202.08462 | Kenta Suzuki | Kenta Suzuki, Tadashi Takayanagi | BCFT and Islands in Two Dimensions | 40 pages, 5 figures | null | 10.1007/JHEP06(2022)095 | YITP-22-14, IPMU22-0002 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | By combining the AdS/BCFT correspondence and the brane world holography, we
expect an equivalence relation between a boundary conformal field theory (BCFT)
and a gravitational system coupled to a CFT. However, it still remains unclear
how the boundary condition of the BCFT is translated in the gravitational
system. W... | [
{
"created": "Thu, 17 Feb 2022 06:23:56 GMT",
"version": "v1"
}
] | 2022-07-06 | [
[
"Suzuki",
"Kenta",
""
],
[
"Takayanagi",
"Tadashi",
""
]
] | By combining the AdS/BCFT correspondence and the brane world holography, we expect an equivalence relation between a boundary conformal field theory (BCFT) and a gravitational system coupled to a CFT. However, it still remains unclear how the boundary condition of the BCFT is translated in the gravitational system. We ... | 9.596597 | 8.896734 | 10.357747 | 8.583496 | 9.004436 | 9.026811 | 8.287603 | 8.78714 | 8.520979 | 11.615267 | 8.403872 | 8.419636 | 9.931138 | 8.837803 | 8.731317 | 8.50472 | 8.720935 | 8.714961 | 8.897024 | 9.747821 | 8.607418 |
2310.13109 | Ilya Shirokov | Ilya Shirokov, Valentina Shirokova | The four-loop $\beta$-function from vacuum supergraphs and the NSVZ
relation for ${\cal N}=1$ SQED regularized by higher derivatives | The version accepted for publication in the European Physical Journal
C | null | 10.1140/epjc/s10052-024-12587-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In ${\cal N}=1$ SQED with $N_f$ flavors regularized by higher derivatives we
obtain the four-loop beta function using a method based on calculating vacuum
supergraphs. For this purpose we use a special C++ program which obtain
contributions to the $\beta$-function from supergraphs without external legs in
the form of... | [
{
"created": "Thu, 19 Oct 2023 19:13:05 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Feb 2024 22:00:53 GMT",
"version": "v2"
}
] | 2024-03-12 | [
[
"Shirokov",
"Ilya",
""
],
[
"Shirokova",
"Valentina",
""
]
] | In ${\cal N}=1$ SQED with $N_f$ flavors regularized by higher derivatives we obtain the four-loop beta function using a method based on calculating vacuum supergraphs. For this purpose we use a special C++ program which obtain contributions to the $\beta$-function from supergraphs without external legs in the form of i... | 13.153098 | 8.597026 | 13.514622 | 9.066089 | 8.605604 | 8.521932 | 9.008061 | 8.491115 | 8.406418 | 16.641352 | 9.426805 | 10.129936 | 11.501159 | 10.900821 | 10.526827 | 10.608215 | 9.886073 | 9.966209 | 10.438334 | 11.791924 | 10.844938 |
hep-th/0611231 | Rodrigo Ferreira Sobreiro | V. E. R. Lemes, R. F. Sobreiro, S. P. Sorella | Renormalizability of the dimension two gluon operator $A^{2}$ in a class
of nonlinear covariant gauges | null | J.Phys.A40:4025-4032,2007 | 10.1088/1751-8113/40/14/017 | null | hep-th | null | In this work we discuss a class of nonlinear covariant gauges for Yang-Mills
theories which enjoy the property of being multiplicatively renormalizable to
all orders. This property follows from the validity of a linearly broken
identity, known as the ghost Ward identity. Furthermore, thanks to this
identity, it turns... | [
{
"created": "Tue, 21 Nov 2006 20:06:00 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Nov 2006 22:07:13 GMT",
"version": "v2"
},
{
"created": "Tue, 20 Mar 2007 21:30:33 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Lemes",
"V. E. R.",
""
],
[
"Sobreiro",
"R. F.",
""
],
[
"Sorella",
"S. P.",
""
]
] | In this work we discuss a class of nonlinear covariant gauges for Yang-Mills theories which enjoy the property of being multiplicatively renormalizable to all orders. This property follows from the validity of a linearly broken identity, known as the ghost Ward identity. Furthermore, thanks to this identity, it turns o... | 8.363598 | 6.025387 | 8.251101 | 7.108509 | 7.330101 | 8.01323 | 7.402758 | 7.239661 | 7.182765 | 9.185359 | 7.467175 | 7.429606 | 7.308095 | 7.460829 | 7.450051 | 7.147294 | 7.075084 | 7.30271 | 7.19334 | 7.427265 | 6.865267 |
2010.07942 | Domenico Orlando | Domenico Orlando, Vito Pellizzani, Susanne Reffert | Near-Schr\"odinger dynamics at large charge | Matches published version in PRD | Phys. Rev. D 103, 105018 (2021) | 10.1103/PhysRevD.103.105018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we discuss a non-relativistic system at large charge in a regime
where Schr\"odinger symmetry is slightly broken by an explicit mass term for
the dilaton field which non-linearly realizes non-relativistic scale
invariance. To get there, we first develop the large-charge formalism from the
linear sigma mo... | [
{
"created": "Thu, 15 Oct 2020 18:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Apr 2021 07:19:18 GMT",
"version": "v2"
}
] | 2021-05-26 | [
[
"Orlando",
"Domenico",
""
],
[
"Pellizzani",
"Vito",
""
],
[
"Reffert",
"Susanne",
""
]
] | In this note we discuss a non-relativistic system at large charge in a regime where Schr\"odinger symmetry is slightly broken by an explicit mass term for the dilaton field which non-linearly realizes non-relativistic scale invariance. To get there, we first develop the large-charge formalism from the linear sigma mode... | 12.855417 | 12.191926 | 13.547156 | 12.026548 | 12.975113 | 13.178064 | 11.676471 | 11.769258 | 11.667029 | 14.47804 | 11.878838 | 11.877829 | 12.034473 | 11.378618 | 11.708893 | 12.401672 | 12.061285 | 11.700069 | 11.984109 | 12.529591 | 11.694594 |
1611.00342 | Edwin Ireson | Adi Armoni, Edwin Ireson | Holographic Corrections to Meson Scattering Amplitudes | 29 pages, 5 figures. v2: minor edits as suggested by referee | null | 10.1016/j.nuclphysb.2017.03.004 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute meson scattering amplitudes using the holographic duality between
confining gauge theories and string theory, in order to consider holographic
corrections to the Veneziano amplitude and associated higher-point functions.
The generic nature of such computations is explained, thanks to the
well-understood na... | [
{
"created": "Tue, 1 Nov 2016 19:28:20 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Nov 2016 15:38:31 GMT",
"version": "v2"
},
{
"created": "Tue, 28 Feb 2017 18:00:48 GMT",
"version": "v3"
}
] | 2017-04-26 | [
[
"Armoni",
"Adi",
""
],
[
"Ireson",
"Edwin",
""
]
] | We compute meson scattering amplitudes using the holographic duality between confining gauge theories and string theory, in order to consider holographic corrections to the Veneziano amplitude and associated higher-point functions. The generic nature of such computations is explained, thanks to the well-understood natu... | 17.504158 | 16.804152 | 18.659647 | 17.472502 | 18.627052 | 17.76796 | 18.163399 | 16.192968 | 16.108234 | 20.730389 | 16.226147 | 16.613319 | 17.169403 | 16.142447 | 15.936551 | 16.783342 | 17.455864 | 16.654894 | 16.411615 | 17.593367 | 16.723196 |
2302.14152 | F. Saueressig | Frank Saueressig | The Functional Renormalization Group in Quantum Gravity | 44 pages, 4 figures, invited chapter for the "Handbook of Quantum
Gravity" (Eds. C. Bambi, L. Modesto and I.L. Shapiro, Springer Singapore,
expected in 2023) | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The gravitational asymptotic safety program envisions a high-energy
completion of the gravitational interactions by an interacting renormalization
group fixed point, the Reuter fixed point. The primary tool for investigating
this scenario are functional renormalization group equations, foremost the
Wetterich equation... | [
{
"created": "Mon, 27 Feb 2023 21:18:44 GMT",
"version": "v1"
}
] | 2023-03-01 | [
[
"Saueressig",
"Frank",
""
]
] | The gravitational asymptotic safety program envisions a high-energy completion of the gravitational interactions by an interacting renormalization group fixed point, the Reuter fixed point. The primary tool for investigating this scenario are functional renormalization group equations, foremost the Wetterich equation. ... | 7.337899 | 6.982352 | 8.028131 | 6.794059 | 7.247917 | 7.19523 | 6.686633 | 6.696529 | 6.83306 | 7.797598 | 6.859443 | 7.237457 | 7.19506 | 7.172172 | 7.147529 | 7.027364 | 7.131083 | 7.105323 | 6.938564 | 7.514488 | 7.001877 |
hep-th/9803155 | Fernando T. Brandt | F. T. Brandt and J. Frenkel | The structure of the graviton self-energy at finite temperature | 27 pages, 6 figures | Phys.Rev. D58 (1998) 085012 | 10.1103/PhysRevD.58.085012 | null | hep-th gr-qc hep-ph | null | We study the graviton self-energy function in a general gauge, using a hard
thermal loop expansion which includes terms proportional to T^4, T^2 and
log(T). We verify explicitly the gauge independence of the leading T^4 term and
obtain a compact expression for the sub-leading T^2 contribution. It is shown
that the lo... | [
{
"created": "Thu, 19 Mar 1998 15:45:38 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Brandt",
"F. T.",
""
],
[
"Frenkel",
"J.",
""
]
] | We study the graviton self-energy function in a general gauge, using a hard thermal loop expansion which includes terms proportional to T^4, T^2 and log(T). We verify explicitly the gauge independence of the leading T^4 term and obtain a compact expression for the sub-leading T^2 contribution. It is shown that the loga... | 8.696513 | 8.24423 | 7.552834 | 8.065939 | 7.623221 | 8.321242 | 7.390028 | 8.34829 | 7.943048 | 8.907346 | 8.101608 | 7.883868 | 8.080194 | 8.343839 | 8.541203 | 8.683684 | 8.328423 | 8.289352 | 7.975616 | 8.188465 | 8.433427 |
1101.5781 | Manuela Kulaxizi | Jan de Boer, Manuela Kulaxizi, Andrei Parnachev | Holographic Entanglement Entropy in Lovelock Gravities | harvmac, 30 pages, 1 figure, References added, typos corrected | JHEP 1107 (2011) 109 | 10.1007/JHEP07(2011)109 | ICCUB-11-018 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study entanglement entropies of simply connected surfaces in field
theories dual to Lovelock gravities. We consider Gauss-Bonnet and cubic
Lovelock gravities in detail. In the conformal case the logarithmic terms in
the entanglement entropy are governed by the conformal anomalies of the CFT; we
verify that the hol... | [
{
"created": "Sun, 30 Jan 2011 16:09:47 GMT",
"version": "v1"
},
{
"created": "Tue, 17 May 2011 14:27:00 GMT",
"version": "v2"
}
] | 2011-12-13 | [
[
"de Boer",
"Jan",
""
],
[
"Kulaxizi",
"Manuela",
""
],
[
"Parnachev",
"Andrei",
""
]
] | We study entanglement entropies of simply connected surfaces in field theories dual to Lovelock gravities. We consider Gauss-Bonnet and cubic Lovelock gravities in detail. In the conformal case the logarithmic terms in the entanglement entropy are governed by the conformal anomalies of the CFT; we verify that the holog... | 6.661562 | 5.648131 | 7.348646 | 6.339056 | 6.399069 | 6.168221 | 5.942084 | 6.20746 | 6.025721 | 8.018909 | 5.79104 | 6.247862 | 6.987344 | 6.334319 | 6.319299 | 6.201024 | 6.069017 | 6.187839 | 6.384953 | 6.881401 | 6.161791 |
hep-th/9809001 | Andreas Fring | A. G. Bytsko, A. Fring | Factorized Combinations of Virasoro Characters | 25 pages (LaTex), minor corrections, one reference added | Commun.Math.Phys. 209 (2000) 179-205 | 10.1007/s002200050019 | SFB-288-343 Berlin (1998) | hep-th math-ph math.MP | null | We investigate linear combinations of characters for minimal Virasoro models
which are representable as a products of several basic blocks. Our analysis is
based on consideration of asymptotic behaviour of the characters in the
quasi-classical limit. In particular, we introduce a notion of the secondary
effective cen... | [
{
"created": "Tue, 1 Sep 1998 11:05:36 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Oct 1998 14:46:23 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Dec 1999 14:50:05 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Bytsko",
"A. G.",
""
],
[
"Fring",
"A.",
""
]
] | We investigate linear combinations of characters for minimal Virasoro models which are representable as a products of several basic blocks. Our analysis is based on consideration of asymptotic behaviour of the characters in the quasi-classical limit. In particular, we introduce a notion of the secondary effective centr... | 12.614871 | 12.830489 | 15.381541 | 11.705965 | 12.455646 | 12.263763 | 12.286688 | 11.194552 | 12.482644 | 15.945854 | 11.236502 | 11.869211 | 12.957326 | 11.776755 | 12.223689 | 11.730827 | 11.848664 | 11.895037 | 11.878953 | 12.29917 | 11.20853 |
1508.04141 | Jerome Quintin | Jerome Quintin, Zeinab Sherkatghanad, Yi-Fu Cai, Robert H.
Brandenberger | Evolution of cosmological perturbations and the production of
non-Gaussianities through a nonsingular bounce: Indications for a no-go
theorem in single field matter bounce cosmologies | 31 pages, 2 figures; v2: minor changes, references added, matches
published version | Phys. Rev. D 92, 063532 (2015) | 10.1103/PhysRevD.92.063532 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Assuming that curvature perturbations and gravitational waves originally
arise from vacuum fluctuations in a matter-dominated phase of contraction, we
study the dynamics of the cosmological perturbations evolving through a
nonsingular bouncing phase described by a generic single scalar field
Lagrangian minimally coup... | [
{
"created": "Mon, 17 Aug 2015 20:04:57 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Sep 2015 15:13:47 GMT",
"version": "v2"
}
] | 2015-10-01 | [
[
"Quintin",
"Jerome",
""
],
[
"Sherkatghanad",
"Zeinab",
""
],
[
"Cai",
"Yi-Fu",
""
],
[
"Brandenberger",
"Robert H.",
""
]
] | Assuming that curvature perturbations and gravitational waves originally arise from vacuum fluctuations in a matter-dominated phase of contraction, we study the dynamics of the cosmological perturbations evolving through a nonsingular bouncing phase described by a generic single scalar field Lagrangian minimally couple... | 5.971464 | 6.423502 | 5.978669 | 5.71559 | 6.386119 | 6.231841 | 5.824363 | 5.965973 | 5.99247 | 6.280223 | 5.781997 | 5.807273 | 5.814251 | 5.792633 | 5.831236 | 5.750848 | 5.684764 | 5.739017 | 5.887026 | 5.954797 | 5.66462 |
1306.3211 | Andrei Linde | Renata Kallosh and Andrei Linde | Superconformal Generalization of the Chaotic Inflation Model \lambda
\phi^4/4 - \xi/ 2 \phi^2 R | 21 pages, 1 figure, references added | null | 10.1088/1475-7516/2013/06/027 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A model of chaotic inflation based on the theory of a scalar field with
potential \lambda\phi^4 perfectly matches the observational data if one adds to
it a tiny non-minimal coupling to gravity -\xi/2 \phi^2 R with \xi > 0.002. We
describe embedding of this model into the superconformal theory with
spontaneous breaki... | [
{
"created": "Thu, 13 Jun 2013 19:51:27 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jun 2013 15:47:21 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Kallosh",
"Renata",
""
],
[
"Linde",
"Andrei",
""
]
] | A model of chaotic inflation based on the theory of a scalar field with potential \lambda\phi^4 perfectly matches the observational data if one adds to it a tiny non-minimal coupling to gravity -\xi/2 \phi^2 R with \xi > 0.002. We describe embedding of this model into the superconformal theory with spontaneous breaking... | 9.283075 | 8.881135 | 9.397349 | 8.360389 | 8.984476 | 9.492971 | 9.196204 | 9.383154 | 8.664792 | 9.134862 | 9.399776 | 8.390995 | 8.573705 | 8.381944 | 8.370375 | 8.554524 | 8.264498 | 8.470104 | 8.843958 | 8.936166 | 8.299351 |
hep-th/0102202 | Ignatios Antoniadis | I. Antoniadis | String and D-brane Physics at Low Energy | 53 pages, Latex, 7 eps-figures, references and acknowledgments added.
Based on lectures given at Centre Emile Borel during the semester
"Supergravity, Superstrings and M-theory", at the "LNF-INFN Spring School in
Nuclear, Subnuclear and Astropartcle Physics", Frascati, at the Glasgow
"Workshop on Phenomenology ... | null | null | CERN-TH/2001-065; 0023/IHP | hep-th | null | 1. Preliminaries.
2. Heterotic string and motivations for large volume compactifications;
2.1 Gauge coupling unification; 2.2 Supersymmetry breaking by
compactification.
3. M-theory on S^1/Z_2 \times Calabi-Yau.
4. Type I/I' string theory and D-branes;
4.1 Low-scale strings and extra-large transverse dimens... | [
{
"created": "Wed, 28 Feb 2001 10:25:01 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Mar 2001 18:28:13 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Antoniadis",
"I.",
""
]
] | 1. Preliminaries. 2. Heterotic string and motivations for large volume compactifications; 2.1 Gauge coupling unification; 2.2 Supersymmetry breaking by compactification. 3. M-theory on S^1/Z_2 \times Calabi-Yau. 4. Type I/I' string theory and D-branes; 4.1 Low-scale strings and extra-large transverse dimensions; 4.2 Re... | 5.862731 | 6.437823 | 5.839873 | 5.675838 | 6.561077 | 6.58493 | 6.054778 | 6.012248 | 5.914218 | 6.187749 | 6.153741 | 5.899374 | 5.687415 | 5.743427 | 5.805154 | 5.87693 | 5.846348 | 5.822179 | 5.682155 | 5.852324 | 5.867255 |
0705.0663 | Matteo Beccaria | Matteo Beccaria | Universality of three gaugino anomalous dimensions in N=4 SYM | 13 pages, JHEP style | JHEP 0706:054,2007 | 10.1088/1126-6708/2007/06/054 | null | hep-th | null | We study maximal helicity three gaugino operators in N=4 Super Yang-Mills
theory. We show that the lowest anomalous dimension of scaling operators with
generic finite spin can be expressed in terms of the universal anomalous
dimension appearing at twist-2. This statement is rigourously proved at three
loops. The reas... | [
{
"created": "Fri, 4 May 2007 16:15:54 GMT",
"version": "v1"
},
{
"created": "Sat, 5 May 2007 16:28:26 GMT",
"version": "v2"
}
] | 2009-11-13 | [
[
"Beccaria",
"Matteo",
""
]
] | We study maximal helicity three gaugino operators in N=4 Super Yang-Mills theory. We show that the lowest anomalous dimension of scaling operators with generic finite spin can be expressed in terms of the universal anomalous dimension appearing at twist-2. This statement is rigourously proved at three loops. The reason... | 12.379321 | 9.846124 | 12.20236 | 10.403662 | 10.052302 | 11.086257 | 10.853399 | 10.273776 | 10.564259 | 14.4042 | 9.966159 | 10.316581 | 12.077345 | 10.9244 | 10.86312 | 10.189524 | 10.834376 | 10.568337 | 10.679609 | 12.140593 | 10.117214 |
1710.06242 | Tomasz Lukowski | Johan Henriksson and Tomasz Lukowski | Perturbative Four-Point Functions from the Analytic Conformal Bootstrap | 35 pages, 1 figure | null | 10.1007/JHEP02(2018)123 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply the analytic conformal bootstrap method to study weakly coupled
conformal gauge theories in four dimensions. We employ twist conformal blocks
to find the most general form of the one-loop four-point correlation function
of identical scalar operators, without any reference to Feynman calculations.
The method ... | [
{
"created": "Tue, 17 Oct 2017 12:53:35 GMT",
"version": "v1"
}
] | 2018-04-04 | [
[
"Henriksson",
"Johan",
""
],
[
"Lukowski",
"Tomasz",
""
]
] | We apply the analytic conformal bootstrap method to study weakly coupled conformal gauge theories in four dimensions. We employ twist conformal blocks to find the most general form of the one-loop four-point correlation function of identical scalar operators, without any reference to Feynman calculations. The method re... | 7.457361 | 7.267858 | 8.270611 | 7.276298 | 7.205226 | 7.363479 | 7.458386 | 7.845066 | 7.33908 | 8.742169 | 7.050756 | 7.302188 | 7.481511 | 7.078625 | 7.226734 | 7.311647 | 7.277816 | 7.413883 | 7.216185 | 7.352042 | 7.196352 |
1403.3302 | Michael Seifert | Michael D. Seifert | Lorentz violation and topological defects | 4 pages. Presented at the Sixth Meeting on CPT and Lorentz Symmetry,
Bloomington, Indiana, June 17-21, 2013 | null | 10.1142/9789814566438_0053 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | If Lorentz symmetry is broken, it must have occurred dynamically, via a
vector or tensor field whose potential energy forces it to take on a non-zero
background expectation value "in vacuum". If the set of minima of this
potential (the vacuum manifold) has a non-trivial topology, then there can
arise topological defe... | [
{
"created": "Thu, 13 Mar 2014 15:34:56 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Seifert",
"Michael D.",
""
]
] | If Lorentz symmetry is broken, it must have occurred dynamically, via a vector or tensor field whose potential energy forces it to take on a non-zero background expectation value "in vacuum". If the set of minima of this potential (the vacuum manifold) has a non-trivial topology, then there can arise topological defect... | 10.358159 | 10.382248 | 10.558093 | 9.539071 | 11.050064 | 10.843545 | 10.302737 | 11.10349 | 9.513958 | 10.111494 | 9.369394 | 9.058639 | 10.034894 | 9.331774 | 9.336372 | 9.674516 | 9.320354 | 9.479375 | 9.333688 | 9.486827 | 9.707378 |
hep-th/0510089 | Shahar Hod | Shahar Hod | Unruh radiation: from black holes to elementary particles | 2 pages | null | null | null | hep-th | null | We advocate the idea that Unruh's quantum radiation, whose theoretical
discovery was originally motivated by the physics of black holes, may have
important implications on the structure and dynamics of elementary particles.
To that end, we analyze the Unruh radiation effect experienced by an
accelerated particle in a... | [
{
"created": "Tue, 11 Oct 2005 16:37:39 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Nov 2005 06:38:45 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Hod",
"Shahar",
""
]
] | We advocate the idea that Unruh's quantum radiation, whose theoretical discovery was originally motivated by the physics of black holes, may have important implications on the structure and dynamics of elementary particles. To that end, we analyze the Unruh radiation effect experienced by an accelerated particle in ato... | 8.160278 | 7.777678 | 7.337821 | 7.176214 | 7.747363 | 7.593122 | 7.445793 | 6.993296 | 7.263093 | 7.461513 | 7.164679 | 7.454705 | 7.469584 | 7.478319 | 7.485205 | 7.660012 | 7.40205 | 7.221844 | 7.501192 | 7.512716 | 7.224676 |
hep-th/0603065 | Paul Frampton | Edoardo Di Napoli and Paul H. Frampton | Anomaly Cancellation and Conformality in Quiver Gauge Theories | 15 pages. minor clarifications | Phys.Lett.B638:374-381,2006 | 10.1016/j.physletb.2006.04.056 | null | hep-th | null | Abelian quiver gauge theories provide nonsupersymmetric candidates for the
conformality approach to physics beyond the standard model. Written as ${\cal
N}=0$, $U(N)^n$ gauge theories, however, they have mixed $U(1)_p U(1)_q^2$ and
$U(1)_p SU(N)_q^2$ triangle anomalies. It is shown how to construct explicitly
a compe... | [
{
"created": "Wed, 8 Mar 2006 16:47:50 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Apr 2006 22:17:04 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Di Napoli",
"Edoardo",
""
],
[
"Frampton",
"Paul H.",
""
]
] | Abelian quiver gauge theories provide nonsupersymmetric candidates for the conformality approach to physics beyond the standard model. Written as ${\cal N}=0$, $U(N)^n$ gauge theories, however, they have mixed $U(1)_p U(1)_q^2$ and $U(1)_p SU(N)_q^2$ triangle anomalies. It is shown how to construct explicitly a compens... | 7.920305 | 8.113967 | 7.984754 | 7.619778 | 8.233821 | 8.090672 | 8.801242 | 7.67028 | 7.41876 | 8.056684 | 7.685417 | 7.47282 | 7.406585 | 7.286175 | 7.29627 | 7.711956 | 7.367647 | 7.20481 | 7.346115 | 7.146824 | 7.417796 |
2201.11801 | Ben Gripaios | Ben Gripaios | Gauge anomalies of finite groups | 4 pp; v2 - added a discussion of potential further anomalies | null | 10.1103/PhysRevD.105.105008 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We show how the theory of characters can be used to analyse an anomaly
corresponding to chiral fermions carrying an arbitrary representation of a
gauge group that is finite, but otherwise arbitrary. By way of example, we do
this for some groups of relevance for the study of quark and lepton masses and
mixings.
| [
{
"created": "Thu, 27 Jan 2022 20:28:47 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Feb 2022 11:22:55 GMT",
"version": "v2"
}
] | 2022-05-25 | [
[
"Gripaios",
"Ben",
""
]
] | We show how the theory of characters can be used to analyse an anomaly corresponding to chiral fermions carrying an arbitrary representation of a gauge group that is finite, but otherwise arbitrary. By way of example, we do this for some groups of relevance for the study of quark and lepton masses and mixings. | 12.040762 | 9.794313 | 10.184276 | 9.932474 | 10.740141 | 9.774338 | 10.432552 | 10.188486 | 11.295259 | 10.190989 | 10.576672 | 10.02917 | 10.719448 | 9.851243 | 10.07934 | 10.076859 | 10.09711 | 9.819109 | 9.942021 | 10.333138 | 10.222583 |
1411.4330 | Stefano Finazzo | S. I. Finazzo and J. Noronha | Debye screening mass near deconfinement from holography | 48 pages, 16 figures, updated references | Phys. Rev. D 90, 115028 (2014) | 10.1103/PhysRevD.90.115028 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper the smallest thermal screening mass associated with the
correlator of the $CT$-odd operator, $\sim {\rm
Tr}F_{\mu\nu}\tilde{F}^{\mu\nu}$, is determined in strongly coupled non-Abelian
gauge plasmas which are holographically dual to non-conformal, bottom-up
Einstein+scalar gravity theories. These hologra... | [
{
"created": "Sun, 16 Nov 2014 23:40:39 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Jan 2015 19:48:42 GMT",
"version": "v2"
}
] | 2015-01-08 | [
[
"Finazzo",
"S. I.",
""
],
[
"Noronha",
"J.",
""
]
] | In this paper the smallest thermal screening mass associated with the correlator of the $CT$-odd operator, $\sim {\rm Tr}F_{\mu\nu}\tilde{F}^{\mu\nu}$, is determined in strongly coupled non-Abelian gauge plasmas which are holographically dual to non-conformal, bottom-up Einstein+scalar gravity theories. These holograph... | 6.39018 | 6.01252 | 5.836886 | 5.667453 | 6.031608 | 6.421863 | 5.995184 | 5.91069 | 5.585071 | 6.235609 | 6.097034 | 5.777882 | 5.795308 | 5.713493 | 5.802658 | 5.70108 | 5.75397 | 5.662082 | 5.756877 | 5.904499 | 5.843002 |
0707.0497 | Alexander Westphal | Marco Serone and Alexander Westphal | Moduli Stabilization in Meta-Stable Heterotic Supergravity Vacua | 1+31 pages, LaTeX, uses JHEP3 class, v2: references corrected and
added, version published in JHEP | JHEP0708:080,2007 | 10.1088/1126-6708/2007/08/080 | SISSA-38/2007/EP | hep-th hep-ph | null | We revisit the issue of moduli stabilization in a class of N=1 four
dimensional supergravity theories which are low energy descriptions of standard
perturbative heterotic string vacua compactified on Calabi-Yau spaces. In
particular, we show how it is possible to stabilize the universal dilaton and
Kahler moduli in a... | [
{
"created": "Tue, 3 Jul 2007 20:51:44 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Sep 2007 10:09:22 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Serone",
"Marco",
""
],
[
"Westphal",
"Alexander",
""
]
] | We revisit the issue of moduli stabilization in a class of N=1 four dimensional supergravity theories which are low energy descriptions of standard perturbative heterotic string vacua compactified on Calabi-Yau spaces. In particular, we show how it is possible to stabilize the universal dilaton and Kahler moduli in a d... | 6.327643 | 5.635313 | 5.918545 | 5.611888 | 5.370507 | 5.407131 | 5.513089 | 5.549439 | 5.2288 | 6.073053 | 5.481269 | 5.534444 | 5.828279 | 5.600654 | 5.711709 | 5.973061 | 5.781921 | 5.769392 | 5.526881 | 5.909783 | 5.831139 |
1412.7681 | Muneto Nitta | Muneto Nitta | Fractional instantons and bions in the O(N) model with twisted boundary
conditions | 43 pages, 16 figures, v2: a reference added, published version | JHEP 03 (2015) 108 | 10.1007/JHEP03(2015)108 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, multiple fractional instanton configurations with zero instanton
charge, called bions, have been revealed to play important roles in quantum
field theories on compactified spacetime. In two dimensions, fractional
instantons and bions have been extensively studied in the ${\mathbb C}P^{N-1}$
model and the Gr... | [
{
"created": "Tue, 23 Dec 2014 17:13:54 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Mar 2015 15:11:09 GMT",
"version": "v2"
}
] | 2015-03-24 | [
[
"Nitta",
"Muneto",
""
]
] | Recently, multiple fractional instanton configurations with zero instanton charge, called bions, have been revealed to play important roles in quantum field theories on compactified spacetime. In two dimensions, fractional instantons and bions have been extensively studied in the ${\mathbb C}P^{N-1}$ model and the Gras... | 4.635227 | 4.548671 | 5.001756 | 4.358244 | 4.944596 | 4.845178 | 4.794981 | 4.652177 | 4.561658 | 5.494015 | 4.556235 | 4.476924 | 4.573319 | 4.471887 | 4.543964 | 4.6309 | 4.568676 | 4.501661 | 4.483759 | 4.608305 | 4.523756 |
1707.08903 | Andrei Dubikovsky | A.I. Dubikovsky, P.K. Silaev | On the possibility of the implicit renormalization procedure for the
Casimir energy | null | Mod. Phys. Lett. A, Vol. 33, No. 22 (2018) 1850129 | 10.1142/S0217732318501298 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a procedure for the renormalization of Casimir energy, that is
based on the implicit versions of standard steps of renormalization procedure
--- regularization, subtraction and removing the regularization. The proposed
procedure is based on the calculation of a set of convergent sums, which are
related to ... | [
{
"created": "Thu, 27 Jul 2017 15:10:54 GMT",
"version": "v1"
}
] | 2018-07-06 | [
[
"Dubikovsky",
"A. I.",
""
],
[
"Silaev",
"P. K.",
""
]
] | We propose a procedure for the renormalization of Casimir energy, that is based on the implicit versions of standard steps of renormalization procedure --- regularization, subtraction and removing the regularization. The proposed procedure is based on the calculation of a set of convergent sums, which are related to th... | 9.024704 | 8.501486 | 8.442173 | 7.853992 | 8.09138 | 8.110797 | 8.759729 | 8.173262 | 8.600129 | 9.542454 | 8.362962 | 8.236758 | 8.551341 | 8.057834 | 8.149934 | 8.081378 | 8.240557 | 8.1666 | 8.502161 | 8.747462 | 8.311709 |
1603.03020 | Gustavo Joaquin Turiaci | Gustavo Turiaci and Herman Verlinde | On CFT and Quantum Chaos | 26 pages, 2 figures. References added | JHEP 1612 (2016) 110 | 10.1007/JHEP12(2016)110 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We make three observations that help clarify the relation between CFT and
quantum chaos. We show that any 1+1-D system in which conformal symmetry is
non-linearly realized exhibits two main characteristics of chaos: maximal
Lyapunov behavior and a spectrum of Ruelle resonances. We use this insight to
identify a latti... | [
{
"created": "Wed, 9 Mar 2016 20:15:53 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Mar 2016 18:38:17 GMT",
"version": "v2"
}
] | 2017-02-01 | [
[
"Turiaci",
"Gustavo",
""
],
[
"Verlinde",
"Herman",
""
]
] | We make three observations that help clarify the relation between CFT and quantum chaos. We show that any 1+1-D system in which conformal symmetry is non-linearly realized exhibits two main characteristics of chaos: maximal Lyapunov behavior and a spectrum of Ruelle resonances. We use this insight to identify a lattice... | 9.953484 | 10.690979 | 11.061124 | 9.994034 | 9.189022 | 10.982179 | 10.438884 | 10.364921 | 9.847392 | 11.580423 | 9.65201 | 10.009324 | 10.000707 | 9.597821 | 9.569798 | 9.397693 | 9.839255 | 10.122918 | 9.82646 | 9.953519 | 9.617248 |
2204.13659 | Yong Zhang | Bo Feng, Song He, Yong Zhang, and Yao-Qi Zhang | One-loop diagrams with quadratic propagators from the worldsheet | 27+11 pages,2 figures; minor changes, clarifications added, published
version | null | 10.1007/JHEP08(2022)240 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well known that forward limits of tree-level amplitudes (and those
trivalent diagrams they consist of) produce one-loop amplitudes and trivalent
diagrams with propagators linear in the loop momentum. They naturally arise
from one-loop worldsheet formulae, and an important open problem is how to
recombine them i... | [
{
"created": "Thu, 28 Apr 2022 17:20:37 GMT",
"version": "v1"
},
{
"created": "Wed, 4 May 2022 16:17:19 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Aug 2022 14:00:16 GMT",
"version": "v3"
}
] | 2022-09-07 | [
[
"Feng",
"Bo",
""
],
[
"He",
"Song",
""
],
[
"Zhang",
"Yong",
""
],
[
"Zhang",
"Yao-Qi",
""
]
] | It is well known that forward limits of tree-level amplitudes (and those trivalent diagrams they consist of) produce one-loop amplitudes and trivalent diagrams with propagators linear in the loop momentum. They naturally arise from one-loop worldsheet formulae, and an important open problem is how to recombine them int... | 14.140488 | 11.065511 | 13.499791 | 11.868444 | 12.756273 | 11.868566 | 13.029711 | 11.64037 | 11.759135 | 13.73579 | 11.934366 | 11.913933 | 12.51531 | 12.023048 | 12.193993 | 12.305998 | 12.124036 | 12.243873 | 12.153681 | 12.602029 | 12.295971 |
2012.09802 | Evan Coleman | Jeremias Aguilera-Damia, Louise M. Anderson, Evan Coleman | A substrate for brane shells from $T\bar{T}$ | 38 pages, 1 figure. Added references | null | 10.1007/JHEP05(2021)248 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | A solvable current-current deformation of the worldsheet theory of strings on
$AdS_3$ has been recently conjectured to be dual to an irrelevant deformation
of the spacetime orbifold CFT, commonly referred to as single-trace $T\bar{T}$.
These deformations give rise to a family of bulk geometries which realize a
non-tr... | [
{
"created": "Thu, 17 Dec 2020 18:09:17 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jan 2021 22:17:35 GMT",
"version": "v2"
}
] | 2023-01-11 | [
[
"Aguilera-Damia",
"Jeremias",
""
],
[
"Anderson",
"Louise M.",
""
],
[
"Coleman",
"Evan",
""
]
] | A solvable current-current deformation of the worldsheet theory of strings on $AdS_3$ has been recently conjectured to be dual to an irrelevant deformation of the spacetime orbifold CFT, commonly referred to as single-trace $T\bar{T}$. These deformations give rise to a family of bulk geometries which realize a non-triv... | 9.530994 | 9.1601 | 10.382211 | 8.69987 | 9.297596 | 8.715202 | 8.538945 | 8.196411 | 8.825573 | 11.279361 | 8.700994 | 8.822598 | 9.343801 | 8.925032 | 8.979586 | 9.011807 | 8.923121 | 8.760906 | 8.70671 | 9.219793 | 8.813337 |
2405.14056 | Gianluca Calcagni | Fabio Briscese, Gianluca Calcagni, Leonardo Modesto, Giuseppe Nardelli | Form factors, spectral and K\"all\'en-Lehmann representation in nonlocal
quantum gravity | 28 pages, 1 figure | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the conical region of convergence of exponential and
asymptotically polynomial form factors and their integral representation as the
sum of complex conjugate pairs corresponding to virtual particles that never go
on-shell. Then, we calculate the spectral representation of the propagator of
nonlocal theorie... | [
{
"created": "Wed, 22 May 2024 22:57:06 GMT",
"version": "v1"
}
] | 2024-05-24 | [
[
"Briscese",
"Fabio",
""
],
[
"Calcagni",
"Gianluca",
""
],
[
"Modesto",
"Leonardo",
""
],
[
"Nardelli",
"Giuseppe",
""
]
] | We discuss the conical region of convergence of exponential and asymptotically polynomial form factors and their integral representation as the sum of complex conjugate pairs corresponding to virtual particles that never go on-shell. Then, we calculate the spectral representation of the propagator of nonlocal theories ... | 14.274024 | 13.871405 | 14.097063 | 15.163789 | 14.945534 | 13.873187 | 14.876713 | 13.888774 | 14.547997 | 16.014507 | 14.164825 | 14.066975 | 13.321628 | 13.123287 | 13.642003 | 13.775031 | 13.558336 | 13.316051 | 13.880759 | 13.206498 | 13.414036 |
hep-th/9408159 | Chen Bin | Bin Chen, Hao-Gang Ding and Ke Wu | Gauge theory on $Z_2 \times Z_2 \ti Z_2 $ Discrete Group and a
Spontaneous $CP$ Violation Toy Model | 13pages, Latex | null | null | null | hep-th | null | In the spirit of Non-commutative differential calculus on discrete group, we
construct a toy model of spontaneous $CP$ violation (SCPV). Our model is
different from the well-known Weinberg-Branco model although it involves three
Higgs doublets and preserve neutral flavor current conservation (NFC) after
using the $Z_... | [
{
"created": "Mon, 29 Aug 1994 21:54:43 GMT",
"version": "v1"
}
] | 2019-08-17 | [
[
"Chen",
"Bin",
""
],
[
"Ding",
"Hao-Gang",
""
],
[
"Wu",
"Ke",
""
]
] | In the spirit of Non-commutative differential calculus on discrete group, we construct a toy model of spontaneous $CP$ violation (SCPV). Our model is different from the well-known Weinberg-Branco model although it involves three Higgs doublets and preserve neutral flavor current conservation (NFC) after using the $Z_2 ... | 18.974731 | 15.63758 | 14.25054 | 13.214067 | 15.47154 | 16.041348 | 14.552258 | 13.973671 | 14.111765 | 14.626966 | 13.581659 | 15.15183 | 13.533049 | 13.933589 | 14.444557 | 14.377417 | 13.990562 | 13.869796 | 13.879849 | 14.340594 | 13.721635 |
2406.10483 | Himanshu Raj | Himanshu Raj, Raju Venugopalan | QCD-Gravity double-copy in the Regge regime: shock wave propagators | 16 pages | null | null | null | hep-th gr-qc hep-ph nucl-th | http://creativecommons.org/licenses/by/4.0/ | In recent work, we demonstrated a double-copy relation between inclusive
gluon radiation in shock wave collisions of ultrarelativistic nuclei and
inclusive graviton radiation in trans-Planckian gravitational shock wave
collisions. We compute here the corresponding gravitational shock wave
propagators in general relat... | [
{
"created": "Sat, 15 Jun 2024 03:24:08 GMT",
"version": "v1"
}
] | 2024-06-18 | [
[
"Raj",
"Himanshu",
""
],
[
"Venugopalan",
"Raju",
""
]
] | In recent work, we demonstrated a double-copy relation between inclusive gluon radiation in shock wave collisions of ultrarelativistic nuclei and inclusive graviton radiation in trans-Planckian gravitational shock wave collisions. We compute here the corresponding gravitational shock wave propagators in general relativ... | 12.4263 | 13.018482 | 13.795135 | 11.896102 | 13.405918 | 14.173575 | 11.879574 | 14.067307 | 12.505894 | 13.883271 | 14.437193 | 12.982007 | 12.407297 | 12.162519 | 12.509579 | 12.450217 | 12.212136 | 12.964986 | 12.495882 | 12.435621 | 12.436808 |
hep-th/9812215 | Hendry Izaac Elim | Freddy P. Zen and Hendry I. Elim | Soliton Solution of the Integrable Coupled Nonlinear Schrodinger
Equation of Manakov Type | 11 pages | null | null | null | hep-th math.DS nlin.PS nlin.SI patt-sol solv-int | null | The soliton solution of the integrable coupled nonlinear Schrodinger equation
(NLS) of Manakov type is investigated by using Zakharov-Shabat (ZS) scheme. We
get the bright N-solitons solution by solving the integrable uncoupled NLS of
Manakov type. We also find that there is an elastic collision of the bright
N-solit... | [
{
"created": "Wed, 23 Dec 1998 09:00:19 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Dec 1998 01:08:00 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Zen",
"Freddy P.",
""
],
[
"Elim",
"Hendry I.",
""
]
] | The soliton solution of the integrable coupled nonlinear Schrodinger equation (NLS) of Manakov type is investigated by using Zakharov-Shabat (ZS) scheme. We get the bright N-solitons solution by solving the integrable uncoupled NLS of Manakov type. We also find that there is an elastic collision of the bright N-soliton... | 6.715607 | 7.52079 | 8.166913 | 7.291096 | 7.04285 | 7.096064 | 7.227301 | 6.955646 | 6.745854 | 7.365784 | 6.058678 | 6.451317 | 7.076213 | 6.538359 | 6.487478 | 6.317964 | 6.470885 | 6.570904 | 6.739819 | 7.672725 | 6.325047 |
2107.07520 | Tomasz Lukowski | Tomasz Lukowski and Jonah Stalknecht | The hypersimplex canonical forms and the momentum amplituhedron-like
logarithmic forms | 18 pages, 2 figures | null | 10.1088/1751-8121/ac62ba | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we provide a formula for the canonical differential form of the
hypersimplex $\Delta_{k,n}$ for all $n$ and $k$. We also study the
generalization of the momentum amplituhedron $\mathcal{M}_{n,k}$ to $m=2$, and
we conclude that the existing definition does not possess the desired
properties. Nevertheless... | [
{
"created": "Thu, 15 Jul 2021 18:00:01 GMT",
"version": "v1"
}
] | 2022-05-04 | [
[
"Lukowski",
"Tomasz",
""
],
[
"Stalknecht",
"Jonah",
""
]
] | In this paper we provide a formula for the canonical differential form of the hypersimplex $\Delta_{k,n}$ for all $n$ and $k$. We also study the generalization of the momentum amplituhedron $\mathcal{M}_{n,k}$ to $m=2$, and we conclude that the existing definition does not possess the desired properties. Nevertheless, ... | 8.701684 | 7.755188 | 10.43355 | 8.198895 | 8.183584 | 7.504354 | 7.852573 | 8.412689 | 7.338914 | 10.28174 | 7.4818 | 7.822442 | 8.497933 | 7.969765 | 7.863076 | 7.980586 | 7.812819 | 8.20267 | 7.757226 | 8.709356 | 7.762004 |
1306.1205 | Joseph Novak | Daniel Butter, Sergei M. Kuzenko, Joseph Novak and Gabriele
Tartaglino-Mazzucchelli | Conformal supergravity in three dimensions: Off-shell actions | 47 pages; v2: published version | JHEP 1310 (2013) 073 | 10.1007/JHEP10(2013)073 | Nikhef-2013-018 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the off-shell formulation for N-extended conformal supergravity in
three dimensions, which has recently been presented in arXiv:1305.3132, we
construct superspace actions for conformal supergravity theories with N<6. For
each of the cases considered, we work out the complete component action as well
as the gaug... | [
{
"created": "Wed, 5 Jun 2013 18:53:20 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Oct 2013 03:59:24 GMT",
"version": "v2"
}
] | 2013-10-16 | [
[
"Butter",
"Daniel",
""
],
[
"Kuzenko",
"Sergei M.",
""
],
[
"Novak",
"Joseph",
""
],
[
"Tartaglino-Mazzucchelli",
"Gabriele",
""
]
] | Using the off-shell formulation for N-extended conformal supergravity in three dimensions, which has recently been presented in arXiv:1305.3132, we construct superspace actions for conformal supergravity theories with N<6. For each of the cases considered, we work out the complete component action as well as the gauge ... | 5.953671 | 5.949461 | 6.85697 | 5.424789 | 5.428113 | 5.603663 | 5.73832 | 5.353048 | 5.549047 | 7.212392 | 5.232018 | 5.364223 | 6.263758 | 5.530689 | 5.605179 | 5.480948 | 5.341697 | 5.409421 | 5.636754 | 5.912867 | 5.37257 |
1402.1346 | Shin'ichi Nojiri | Masafumi Higuchi and Shin'ichi Nojiri | Reconstruction of Domain Wall Universe and Localization of Gravity | LaTeX, 8 pages, no figure | null | 10.1007/s10714-014-1822-z | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a four-dimensional domain wall universe by using the Brans-Dicke
type gravity with two scalar field. We give a formulation where for arbitrarily
given warp factor and scale factor, we construct an action which reproduces
both of the warp and scale factors as a solution of the Einstein equation and
the fi... | [
{
"created": "Thu, 6 Feb 2014 13:19:46 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Higuchi",
"Masafumi",
""
],
[
"Nojiri",
"Shin'ichi",
""
]
] | We construct a four-dimensional domain wall universe by using the Brans-Dicke type gravity with two scalar field. We give a formulation where for arbitrarily given warp factor and scale factor, we construct an action which reproduces both of the warp and scale factors as a solution of the Einstein equation and the fiel... | 12.401782 | 11.118773 | 12.535812 | 11.351914 | 12.790817 | 13.315248 | 12.674394 | 11.897104 | 11.278334 | 12.230946 | 11.460488 | 11.286059 | 11.879752 | 11.541372 | 11.64115 | 11.554551 | 11.401899 | 11.651057 | 11.38777 | 11.773928 | 11.156296 |
1611.02937 | Dr. Sudhaker Upadhyay | S. H. Hendi, S. Panahiyan, S. Upadhyay and B. Eslam Panah | Charged BTZ black holes in the context of massive gravity's rainbow | 23 pages with 8 captioned figures, journal version | Phys. Rev. D 95, 084036 (2017) | 10.1103/PhysRevD.95.084036 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | BTZ black holes are excellent laboratories for studying black hole
thermodynamics which is a bridge between classical general relativity and
quantum nature of gravitation. In addition, three-dimensional gravity could
have equipped us for exploring some of the ideas behind the two dimensional
conformal field theory ba... | [
{
"created": "Mon, 31 Oct 2016 20:46:50 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Apr 2017 04:36:02 GMT",
"version": "v2"
}
] | 2017-04-26 | [
[
"Hendi",
"S. H.",
""
],
[
"Panahiyan",
"S.",
""
],
[
"Upadhyay",
"S.",
""
],
[
"Panah",
"B. Eslam",
""
]
] | BTZ black holes are excellent laboratories for studying black hole thermodynamics which is a bridge between classical general relativity and quantum nature of gravitation. In addition, three-dimensional gravity could have equipped us for exploring some of the ideas behind the two dimensional conformal field theory base... | 12.755898 | 11.993005 | 13.101457 | 11.759606 | 12.48743 | 12.314075 | 12.017262 | 11.988496 | 13.023253 | 12.301402 | 12.661959 | 12.061536 | 11.973219 | 11.652065 | 11.822791 | 11.981463 | 12.101563 | 11.649282 | 11.787176 | 11.981552 | 12.170878 |
1210.8358 | Fidel Schaposnik | Fidel A. Schaposnik and Gianni Tallarita | Lifshitz holography with a probe Yang-Mills field | 12 pages, 3 figures | null | 10.1016/j.physletb.2013.02.032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Taking as a probe an SU(2) gauge field with Yang-Mills action in a 3+1
dimensional Lifshitz black hole background, we use the gauge/gravity
correspondence to discuss finite temperature effects in the dual theory defined
on the boundary. In order to test the dependence of results on the anisotropic
scaling exponent z ... | [
{
"created": "Wed, 31 Oct 2012 15:05:29 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Schaposnik",
"Fidel A.",
""
],
[
"Tallarita",
"Gianni",
""
]
] | Taking as a probe an SU(2) gauge field with Yang-Mills action in a 3+1 dimensional Lifshitz black hole background, we use the gauge/gravity correspondence to discuss finite temperature effects in the dual theory defined on the boundary. In order to test the dependence of results on the anisotropic scaling exponent z we... | 8.667652 | 7.977152 | 7.88848 | 7.499301 | 7.272603 | 7.620428 | 7.897653 | 7.705455 | 7.222077 | 8.404191 | 7.525239 | 7.668967 | 8.15745 | 7.511326 | 7.489633 | 7.599304 | 7.817131 | 7.527497 | 7.496366 | 8.131473 | 7.863239 |
2406.11557 | Si-Wen Li | Si-wen Li, Yi-peng Zhang, Hao-qian Li | Holographic spectral function of fermion in instantonic plasma | 19 pages, 5 figures | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Using the gauge-gravity duality, we investigate the fermionic correlation
function in the D(-1)-D3 brane system which describes the instantonic plasma in
holography. In this system, the charge of the D(-1) brane as the D-instanton
gives the gluon condensate. To simplify the holographic setup, we first reduce
briefly ... | [
{
"created": "Mon, 17 Jun 2024 13:55:52 GMT",
"version": "v1"
}
] | 2024-06-18 | [
[
"Li",
"Si-wen",
""
],
[
"Zhang",
"Yi-peng",
""
],
[
"Li",
"Hao-qian",
""
]
] | Using the gauge-gravity duality, we investigate the fermionic correlation function in the D(-1)-D3 brane system which describes the instantonic plasma in holography. In this system, the charge of the D(-1) brane as the D-instanton gives the gluon condensate. To simplify the holographic setup, we first reduce briefly th... | 12.102003 | 12.220323 | 12.626914 | 11.519547 | 12.364231 | 12.690556 | 12.399949 | 12.40822 | 11.673473 | 13.182524 | 11.750862 | 12.075214 | 11.799399 | 11.3914 | 11.728593 | 11.677134 | 11.402204 | 11.506084 | 11.378203 | 11.63721 | 11.146126 |
0712.1225 | Luca Vecchi | Luca Vecchi | Massive states as the relevant deformations of gravitating branes | Version published in Phys. Rev. D | Phys.Rev.D78:085029,2008 | 10.1103/PhysRevD.78.085029 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Five-dimensional theories manifesting spontaneous brane generation are
discussed in a gravitational context. Without gravity, the IR dynamics of the
brane fluctuation below the brane tension scale is described by an effective
theory for the Nambu-Goldstone modes. When gravity is properly taken into
account the long d... | [
{
"created": "Fri, 7 Dec 2007 20:53:22 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Aug 2008 15:03:51 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Dec 2008 17:47:47 GMT",
"version": "v3"
}
] | 2008-12-18 | [
[
"Vecchi",
"Luca",
""
]
] | Five-dimensional theories manifesting spontaneous brane generation are discussed in a gravitational context. Without gravity, the IR dynamics of the brane fluctuation below the brane tension scale is described by an effective theory for the Nambu-Goldstone modes. When gravity is properly taken into account the long dis... | 12.340446 | 11.250264 | 12.304713 | 11.413244 | 12.5775 | 12.07994 | 11.285405 | 11.739714 | 11.860907 | 12.619035 | 11.461668 | 11.752405 | 11.463571 | 11.466522 | 11.658421 | 11.82145 | 11.376481 | 11.931594 | 11.324221 | 12.005953 | 11.424899 |
hep-th/9809133 | Ehud Schreiber | Y. Kinar, E. Schreiber, J. Sonnenschein | Precision "Measurements" of the $Q \bar{Q}$ Potential in MQCD | Latex, 1+18 pages, 3 figures ; v2: Discussion of SUSY breaking case
corrected - results qualitatively unchanged v3: Minor corrections, reference
added | Nucl.Phys. B544 (1999) 633-649 | 10.1016/S0550-3213(99)00067-X | TAUP-2518-98 | hep-th | null | We compute the M theory corrections to the confining linear potential between
a quark and an anti-quark in N=1 Super Yang-Mills theory. We find a constant
term, and a term exponentially small with characteristic length of
$\Lambda_{QCD}^{-1}$. The potential in the MQCD setup that corresponds to
softly broken N=1 SYM ... | [
{
"created": "Thu, 17 Sep 1998 17:39:48 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Oct 1998 16:28:13 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Feb 1999 12:39:13 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Kinar",
"Y.",
""
],
[
"Schreiber",
"E.",
""
],
[
"Sonnenschein",
"J.",
""
]
] | We compute the M theory corrections to the confining linear potential between a quark and an anti-quark in N=1 Super Yang-Mills theory. We find a constant term, and a term exponentially small with characteristic length of $\Lambda_{QCD}^{-1}$. The potential in the MQCD setup that corresponds to softly broken N=1 SYM is... | 9.791676 | 8.668793 | 9.451188 | 7.920857 | 8.419434 | 8.477362 | 8.532756 | 7.559034 | 7.90847 | 9.749422 | 7.870275 | 8.233608 | 8.946208 | 9.035433 | 8.938371 | 8.611987 | 8.329669 | 8.340079 | 8.754911 | 8.665974 | 8.099473 |
1307.7738 | Anton de la Fuente | Anton de la Fuente and Raman Sundrum | Holography of the BTZ Black Hole, Inside and Out | 52 pages, 15 figures. v2: Clarifications made throughout paper.
Derivation of (new) Section 8 corrected. Results and conclusions unchanged.
References added | JHEP 09 (2014) 073 | 10.1007/JHEP09(2014)073 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a 1+1 dimensional CFT dual structure for quantum gravity and
matter on the extended 2+1 dimensional BTZ black hole, realized as a quotient
of the Poincare patch of AdS$_3$. The quotient spacetime includes regions
beyond the singularity, "whiskers", containing timelike and lightlike closed
curves, which at ... | [
{
"created": "Mon, 29 Jul 2013 20:55:08 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Jul 2014 00:54:13 GMT",
"version": "v2"
}
] | 2014-09-16 | [
[
"de la Fuente",
"Anton",
""
],
[
"Sundrum",
"Raman",
""
]
] | We propose a 1+1 dimensional CFT dual structure for quantum gravity and matter on the extended 2+1 dimensional BTZ black hole, realized as a quotient of the Poincare patch of AdS$_3$. The quotient spacetime includes regions beyond the singularity, "whiskers", containing timelike and lightlike closed curves, which at fi... | 11.339036 | 11.726982 | 12.508429 | 11.750411 | 12.475376 | 11.999951 | 12.284786 | 12.207252 | 11.550401 | 12.914594 | 10.939426 | 11.489319 | 11.427067 | 11.305943 | 11.422434 | 11.354689 | 11.196973 | 11.289008 | 11.407102 | 11.766135 | 11.387104 |
1309.7642 | Panagiota Kanti | P. Kanti, N. Pappas and K. Zuleta | On the Localisation of 4-Dimensional Brane-World Black Holes | 23 pages, Latex2e file, submitted for publication in Classical and
Quantum Gravity | null | 10.1088/0264-9381/30/23/235017 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of brane-world models, we pursue the question of the existence
of 5-dimensional solutions describing regular black holes localised close to
the brane. Employing a perturbed Vaidya-type line-element embedded in a warped
fifth dimension, we attempt to localise the extended black-string singularity,
and t... | [
{
"created": "Sun, 29 Sep 2013 19:22:50 GMT",
"version": "v1"
}
] | 2015-06-17 | [
[
"Kanti",
"P.",
""
],
[
"Pappas",
"N.",
""
],
[
"Zuleta",
"K.",
""
]
] | In the context of brane-world models, we pursue the question of the existence of 5-dimensional solutions describing regular black holes localised close to the brane. Employing a perturbed Vaidya-type line-element embedded in a warped fifth dimension, we attempt to localise the extended black-string singularity, and to ... | 9.944624 | 10.995742 | 10.843123 | 9.915986 | 10.724575 | 10.267906 | 10.63965 | 10.506279 | 10.237414 | 10.460926 | 9.818828 | 10.065828 | 9.861138 | 9.649269 | 10.037842 | 9.929605 | 10.069827 | 9.828526 | 9.642818 | 9.665186 | 9.840304 |
hep-th/9606085 | Mekhfi Mustapha | M.Mekhfi | Twisted Homotopy: A Group Theoretic Approach | 7 pages,Latex,no figures | null | null | null | hep-th | null | After summarising the physical approach leading to twisted homotopy and after
developing the cohomological approach further with respect to our previous work
we propose a third alternative approach to twisted homotopy based on group
theoretic considerations. In this approach the fundamental group $\Pi (m) $
isomorphi... | [
{
"created": "Fri, 14 Jun 1996 14:12:54 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Mekhfi",
"M.",
""
]
] | After summarising the physical approach leading to twisted homotopy and after developing the cohomological approach further with respect to our previous work we propose a third alternative approach to twisted homotopy based on group theoretic considerations. In this approach the fundamental group $\Pi (m) $ isomorphic ... | 17.880569 | 17.304741 | 18.766531 | 16.916264 | 18.650776 | 18.796259 | 17.662302 | 17.053642 | 17.443071 | 19.705526 | 16.07445 | 16.264006 | 16.386284 | 15.856067 | 16.471081 | 16.065285 | 16.314024 | 16.061264 | 16.249317 | 16.873554 | 16.277409 |
hep-th/9207034 | Steve Giddings | Steven B. Giddings and Andrew Strominger | Quantum Theories of Dilaton Gravity | 20 pages (Major additions made, including 5 pages on the relation
between conformal invariance and background independence.) | Phys.Rev.D47:2454-2460,1993 | 10.1103/PhysRevD.47.2454 | UCSBTH-92-28 | hep-th | null | Quantization of two-dimensional dilaton gravity coupled to conformal matter
is investigated. Working in conformal gauge about a fixed background metric,
the theory may be viewed as a sigma model whose target space is parameterized
by the dilaton $\phi$ and conformal factor $\rho$. A precise connection is
given betwee... | [
{
"created": "Sat, 11 Jul 1992 01:49:39 GMT",
"version": "v1"
},
{
"created": "Sat, 3 Oct 1992 23:22:20 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Giddings",
"Steven B.",
""
],
[
"Strominger",
"Andrew",
""
]
] | Quantization of two-dimensional dilaton gravity coupled to conformal matter is investigated. Working in conformal gauge about a fixed background metric, the theory may be viewed as a sigma model whose target space is parameterized by the dilaton $\phi$ and conformal factor $\rho$. A precise connection is given between ... | 8.424307 | 8.720799 | 9.511796 | 8.322487 | 8.633477 | 8.675309 | 8.21909 | 8.861283 | 8.302233 | 9.274336 | 8.138708 | 8.067256 | 8.536304 | 8.283933 | 8.153452 | 8.326762 | 8.329609 | 8.587265 | 8.113862 | 8.660161 | 8.190523 |
2207.00605 | Veronica Panizza | Veronica Panizza, Ricardo Costa de Almeida, Philipp Hauke | Entanglement Witnessing for Lattice Gauge Theories | 17+8 pages (single column), 4+2 figures; added references | null | 10.1007/JHEP09(2022)196 | null | hep-th cond-mat.quant-gas cond-mat.str-el hep-lat quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Entanglement is assuming a central role in modern quantum many-body physics.
Yet, for lattice gauge theories its certification remains extremely
challenging. A key difficulty stems from the local gauge constraints underlying
the gauge theory, which separate the full Hilbert space into a direct sum of
subspaces charac... | [
{
"created": "Fri, 1 Jul 2022 18:01:21 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Jul 2022 12:59:31 GMT",
"version": "v2"
}
] | 2022-09-26 | [
[
"Panizza",
"Veronica",
""
],
[
"de Almeida",
"Ricardo Costa",
""
],
[
"Hauke",
"Philipp",
""
]
] | Entanglement is assuming a central role in modern quantum many-body physics. Yet, for lattice gauge theories its certification remains extremely challenging. A key difficulty stems from the local gauge constraints underlying the gauge theory, which separate the full Hilbert space into a direct sum of subspaces characte... | 7.758442 | 9.058387 | 8.099822 | 7.541287 | 9.669344 | 9.251287 | 8.901126 | 8.867223 | 8.245647 | 8.594745 | 8.487432 | 8.136089 | 7.788259 | 7.659328 | 7.874492 | 7.840981 | 7.809646 | 7.83215 | 7.7978 | 7.541823 | 7.744998 |
hep-th/0103013 | null | Alexios P. Polychronakos | Quantum Hall states as matrix Chern-Simons theory | 18 pages; final version to appear in JHEP | JHEP 0104:011,2001 | 10.1088/1126-6708/2001/04/011 | CCNY-HEP-01-02, RU-01-4-B | hep-th cond-mat nlin.SI quant-ph | null | We propose a finite Chern-Simons matrix model on the plane as an effective
description of fractional quantum Hall fluids of finite extent. The
quantization of the inverse filling fraction and of the quasiparticle number is
shown to arise quantum mechanically and to agree with Laughlin theory. We also
point out the ef... | [
{
"created": "Fri, 2 Mar 2001 17:21:40 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Mar 2001 00:20:51 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Apr 2001 06:31:48 GMT",
"version": "v3"
}
] | 2010-02-03 | [
[
"Polychronakos",
"Alexios P.",
""
]
] | We propose a finite Chern-Simons matrix model on the plane as an effective description of fractional quantum Hall fluids of finite extent. The quantization of the inverse filling fraction and of the quasiparticle number is shown to arise quantum mechanically and to agree with Laughlin theory. We also point out the effe... | 11.450838 | 8.690886 | 12.831722 | 9.198024 | 10.675772 | 9.732878 | 9.432873 | 8.766042 | 8.920426 | 13.255178 | 9.197521 | 10.060018 | 11.248639 | 10.065793 | 10.193625 | 9.703896 | 9.818007 | 9.766046 | 10.102872 | 10.534899 | 10.320889 |
hep-th/9209022 | 7353 | Shinobu Hikami and Edouard Br\'ezin | Perturbative analysis of an n-Ising model on a random surface | 9pp | Phys.Lett. B295 (1992) 209-213 | 10.1016/0370-2693(92)91555-N | null | hep-th | null | Two dimensional quantum gravity coupled to a conformally invariant matter
field of central charge c=n/2, is represented, in a discretized version, by n
independent Ising spins per cell of the triangulations of a random surface. The
matrix integral representation of this model leads to a diagrammatic expansion
at larg... | [
{
"created": "Tue, 8 Sep 1992 07:37:35 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Hikami",
"Shinobu",
""
],
[
"Brézin",
"Edouard",
""
]
] | Two dimensional quantum gravity coupled to a conformally invariant matter field of central charge c=n/2, is represented, in a discretized version, by n independent Ising spins per cell of the triangulations of a random surface. The matrix integral representation of this model leads to a diagrammatic expansion at large ... | 15.334742 | 15.59422 | 19.191967 | 14.926937 | 15.733354 | 15.416467 | 15.369543 | 13.641931 | 14.269991 | 19.835518 | 15.11309 | 14.872221 | 15.232283 | 15.418059 | 15.442336 | 14.34611 | 15.730608 | 14.565756 | 15.218884 | 15.876683 | 13.989872 |
hep-th/9507057 | Jean-Bernard Zuber | Jean-Bernard Zuber | Graphs and Reflection Groups | 42 pages TEX file, harvmac and epsf macros, AMS fonts optional,
uuencoded, 8 figures included | Commun.Math.Phys. 179 (1996) 265-294 | 10.1007/BF02102590 | SPhT 95/089 | hep-th | null | It is shown that graphs that generalize the ADE Dynkin diagrams and have
appeared in various contexts of two-dimensional field theory may be regarded in
a natural way as encoding the geometry of a root system. After recalling what
are the conditions satisfied by these graphs, we define a bilinear form on a
root syste... | [
{
"created": "Mon, 10 Jul 1995 14:59:41 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Zuber",
"Jean-Bernard",
""
]
] | It is shown that graphs that generalize the ADE Dynkin diagrams and have appeared in various contexts of two-dimensional field theory may be regarded in a natural way as encoding the geometry of a root system. After recalling what are the conditions satisfied by these graphs, we define a bilinear form on a root system ... | 10.396003 | 9.947124 | 11.80743 | 9.628857 | 9.734365 | 11.272506 | 10.076124 | 10.34097 | 9.533185 | 11.319709 | 9.497076 | 9.683403 | 10.480665 | 9.609689 | 9.747245 | 9.496415 | 9.66012 | 9.87554 | 9.804739 | 10.352747 | 9.848078 |
1812.10448 | Marco Raveri | Marco Raveri, Wayne Hu and Savdeep Sethi | Swampland Conjectures and Late-Time Cosmology | 10 pages, 4 figures; more precisely worded abstract and conclusions;
references added | Phys. Rev. D 99, 083518 (2019) | 10.1103/PhysRevD.99.083518 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the cosmological implications of the string swampland conjectures
for late-time cosmology, and test them against a wide range of state of the art
cosmological observations. The refined de Sitter conjecture constrains either
the minimal slope or the curvature of the scalar potential, and depends on two
dime... | [
{
"created": "Wed, 26 Dec 2018 18:30:31 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jan 2019 19:57:30 GMT",
"version": "v2"
}
] | 2019-04-24 | [
[
"Raveri",
"Marco",
""
],
[
"Hu",
"Wayne",
""
],
[
"Sethi",
"Savdeep",
""
]
] | We discuss the cosmological implications of the string swampland conjectures for late-time cosmology, and test them against a wide range of state of the art cosmological observations. The refined de Sitter conjecture constrains either the minimal slope or the curvature of the scalar potential, and depends on two dimens... | 9.551515 | 9.913466 | 10.130589 | 9.543097 | 10.503636 | 10.334779 | 9.650279 | 9.72194 | 9.469454 | 10.690589 | 9.885147 | 9.386402 | 9.703903 | 9.090846 | 9.39696 | 9.684908 | 9.480834 | 9.108569 | 8.971177 | 9.780968 | 9.199498 |
hep-th/0511030 | Huan-Xiong Yang | Huan-Xiong Yang | Moduli Stabilization in Type IIB Flux Compactifications | 10 pages, LaTeX2e style. The paper is rewritten in ver3 with more
references added | Phys.Rev.D73:066006,2006 | 10.1103/PhysRevD.73.066006 | null | hep-th | null | In the present paper, we reexamine the moduli stabilization problem of the
Type IIB orientifolds with one complex structure modulus in a modified two-step
procedure. The full superpotential including both the 3-form fluxes and the
non-perturbative corrections is used to yield a F-term potential. This
potential is sim... | [
{
"created": "Thu, 3 Nov 2005 07:19:36 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Nov 2005 10:05:16 GMT",
"version": "v2"
},
{
"created": "Wed, 30 Nov 2005 06:52:41 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Yang",
"Huan-Xiong",
""
]
] | In the present paper, we reexamine the moduli stabilization problem of the Type IIB orientifolds with one complex structure modulus in a modified two-step procedure. The full superpotential including both the 3-form fluxes and the non-perturbative corrections is used to yield a F-term potential. This potential is simpl... | 10.87793 | 10.05667 | 10.682584 | 9.615682 | 10.458576 | 10.088918 | 10.571546 | 10.425158 | 10.489297 | 11.508564 | 10.066798 | 10.386415 | 10.58329 | 10.302355 | 10.298381 | 10.322579 | 10.306258 | 10.493792 | 10.174589 | 10.678761 | 10.149808 |
hep-th/9806075 | Tomas Ortin Miguel | E. Alvarez, C. Gomez, T. Ortin (I.F.T., Madrid) | String Representation of Wilson Loops | Latex2e file. Shortened and improved | Nucl.Phys. B545 (1999) 217-232 | 10.1016/S0550-3213(99)00103-0 | IFT-UAM/CSIC-98-1 | hep-th | null | We explore the consequences of imposing Polyakov's zig/zag-invariance in the
search for a confining string. We first find that the requirement of
zig/zag-invariance seems to be incompatible with spacetime supersymmetry. We
then try to find zig/zag-invariant string backgrounds on which to implement the
minimal-area pr... | [
{
"created": "Wed, 10 Jun 1998 09:48:09 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jun 1998 10:13:13 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Jun 1998 10:06:18 GMT",
"version": "v3"
},
{
"created": "Thu, 17 Dec 1998 16:47:34 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Alvarez",
"E.",
"",
"I.F.T., Madrid"
],
[
"Gomez",
"C.",
"",
"I.F.T., Madrid"
],
[
"Ortin",
"T.",
"",
"I.F.T., Madrid"
]
] | We explore the consequences of imposing Polyakov's zig/zag-invariance in the search for a confining string. We first find that the requirement of zig/zag-invariance seems to be incompatible with spacetime supersymmetry. We then try to find zig/zag-invariant string backgrounds on which to implement the minimal-area pres... | 15.700939 | 14.180518 | 17.558725 | 14.266575 | 14.952216 | 14.836437 | 14.408074 | 13.357114 | 13.303793 | 19.329815 | 13.429229 | 13.377523 | 16.618145 | 14.126456 | 13.486245 | 14.105553 | 13.324458 | 13.024843 | 14.28658 | 14.954233 | 13.724956 |
hep-th/9912088 | Mironov | A.Mironov, A.Morozov | Commuting Hamiltonians from Seiberg-Witten Theta-Functions | LaTeX, 9 pages; corrected a grant reference number | Phys.Lett. B475 (2000) 71-76 | 10.1016/S0370-2693(00)00075-7 | FIAN/TD-29/99, ITEP/TH-70/99 | hep-th | null | Elementary MAPLE calculations are used to support the claim of hep-th/9906240
that the ratios of theta-functions, associated with the Seiberg-Witten complex
curves, provide Poisson-commuting Hamiltonians which describe the dual of the
original Seiberg-Witten integrable system.
| [
{
"created": "Fri, 10 Dec 1999 20:03:38 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Jan 2000 12:05:39 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | Elementary MAPLE calculations are used to support the claim of hep-th/9906240 that the ratios of theta-functions, associated with the Seiberg-Witten complex curves, provide Poisson-commuting Hamiltonians which describe the dual of the original Seiberg-Witten integrable system. | 21.495676 | 14.607903 | 23.540771 | 14.190187 | 14.870395 | 15.248579 | 15.923637 | 14.982605 | 14.946374 | 19.431553 | 14.612864 | 15.386302 | 17.991026 | 16.633438 | 15.705154 | 15.241358 | 15.292801 | 15.021943 | 16.269695 | 15.884926 | 14.915915 |
1909.02170 | Carlos A. S. Almeida | F. C. E. Lima, D. M. Dantas, C. A. S. Almeida | New class of solutions of a generalized $O(3)$-sigma Chern-Simons model | 12 pages, 7 figures | null | 10.1209/0295-5075/130/10005 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we investigated the existence of compacton-like configuration
in the O(3)-sigma model. We consider a minimally coupled O(3)-sigma model with
a gauge field governed by a generalized Chern-Simons term. Contrary to that
established in the literature, we impose a new set of boundary conditions and,
we find ... | [
{
"created": "Thu, 5 Sep 2019 00:46:37 GMT",
"version": "v1"
}
] | 2020-08-26 | [
[
"Lima",
"F. C. E.",
""
],
[
"Dantas",
"D. M.",
""
],
[
"Almeida",
"C. A. S.",
""
]
] | In this work, we investigated the existence of compacton-like configuration in the O(3)-sigma model. We consider a minimally coupled O(3)-sigma model with a gauge field governed by a generalized Chern-Simons term. Contrary to that established in the literature, we impose a new set of boundary conditions and, we find so... | 11.04599 | 9.817287 | 11.405418 | 9.576714 | 9.799793 | 9.794783 | 9.25879 | 9.271054 | 9.094388 | 11.74092 | 9.463376 | 9.567412 | 10.213148 | 9.608914 | 9.249084 | 9.673276 | 9.510674 | 9.704629 | 9.530087 | 10.296702 | 9.716893 |
1605.09510 | Josef Kluson | J. Kluson | Note About Unstable D-Brane with Dynamical Tension | 21 pages | Phys. Rev. D 94, 046004 (2016) | 10.1103/PhysRevD.94.046004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose an action for unstable Dp-brane with dynamical tension. We show
that the equations of motion are equivalent to the equations of motion derived
from DBI and WZ actions for non-BPS Dp-brane. We also find Hamiltonian
formulation of this action and analyze properties of the solutions
corresponding to the tachy... | [
{
"created": "Tue, 31 May 2016 07:24:39 GMT",
"version": "v1"
}
] | 2016-08-17 | [
[
"Kluson",
"J.",
""
]
] | We propose an action for unstable Dp-brane with dynamical tension. We show that the equations of motion are equivalent to the equations of motion derived from DBI and WZ actions for non-BPS Dp-brane. We also find Hamiltonian formulation of this action and analyze properties of the solutions corresponding to the tachyon... | 7.980339 | 5.329943 | 9.97567 | 6.083674 | 6.718277 | 6.138029 | 6.034017 | 5.776858 | 6.004882 | 9.067698 | 6.22748 | 6.555303 | 8.404045 | 6.712349 | 6.503759 | 6.459789 | 6.528072 | 6.259509 | 6.873406 | 8.363537 | 6.57475 |
hep-th/9704114 | null | M. Shifman | Non-Perturbative Dynamics in Supersymmetric Gauge Theories | 121 pages, LATEX, epsfig, 4 figures. Several typos corrected and
references added. Extended version of lectures given at International School
of Physics "Enrico Fermi", Varenna, Italy, July 3-6, 1995; Institute of
Nuclear Science, UNAM, Mexico, April 11-17, 1996, and Summer School in
High-Energy Physics and Cos... | Prog.Part.Nucl.Phys.39:1-116,1997 | 10.1016/S0146-6410(97)00042-2 | TPI-MINN-97/09-T | hep-th hep-ph | null | I give an introductory review of recent, fascinating developments in
supersymmetric gauge theories. I explain pedagogically the miraculous
properties of supersymmetric gauge dynamics allowing one to obtain exact
solutions in many instances. Various dynamical regimes emerging in
supersymmetric Quantum Chromodynamics a... | [
{
"created": "Tue, 15 Apr 1997 01:14:29 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Oct 1997 20:29:54 GMT",
"version": "v2"
}
] | 2011-04-15 | [
[
"Shifman",
"M.",
""
]
] | I give an introductory review of recent, fascinating developments in supersymmetric gauge theories. I explain pedagogically the miraculous properties of supersymmetric gauge dynamics allowing one to obtain exact solutions in many instances. Various dynamical regimes emerging in supersymmetric Quantum Chromodynamics and... | 11.301523 | 11.662691 | 12.140602 | 11.001537 | 11.639826 | 12.987564 | 11.483373 | 10.948188 | 10.568968 | 12.516775 | 11.193474 | 10.505886 | 11.109249 | 10.570369 | 10.818445 | 10.701903 | 10.430179 | 10.609422 | 10.346672 | 10.963685 | 10.70974 |
hep-th/0609065 | Christian Schubert | G.V. Dunne, A. Huet (Univ. of Connnecticut), D. Rivera (UTPA), C.
Schubert (Univ. of Michoacan) | Closed-form weak-field expansion of two-loop Euler-Heisenberg
Lagrangians | 12 pages | JHEP0611:013,2006 | 10.1088/1126-6708/2006/11/013 | null | hep-th | null | We obtain closed-form expressions, in terms of the Faulhaber numbers, for the
weak-field expansion coefficients of the two-loop Euler-Heisenberg effective
Lagrangians in a magnetic or electric field. This follows from the observation
that the magnetic worldline Green's function has a natural expansion in terms
of the... | [
{
"created": "Sun, 10 Sep 2006 17:31:33 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Dunne",
"G. V.",
"",
"Univ. of Connnecticut"
],
[
"Huet",
"A.",
"",
"Univ. of Connnecticut"
],
[
"Rivera",
"D.",
"",
"UTPA"
],
[
"Schubert",
"C.",
"",
"Univ. of Michoacan"
]
] | We obtain closed-form expressions, in terms of the Faulhaber numbers, for the weak-field expansion coefficients of the two-loop Euler-Heisenberg effective Lagrangians in a magnetic or electric field. This follows from the observation that the magnetic worldline Green's function has a natural expansion in terms of the F... | 10.092322 | 8.09352 | 9.175435 | 7.801947 | 8.38507 | 7.674101 | 7.974036 | 8.741106 | 7.724548 | 10.442598 | 7.952432 | 7.78627 | 9.357042 | 8.517313 | 8.828888 | 8.417586 | 7.991584 | 8.11484 | 8.532461 | 8.869952 | 8.169106 |
2110.06038 | Ghazal Geshnizjani | Amjad Ashoorioon, Ghazal Geshnizjani, Hyung J. Kim | Non-Gaussianities in the Extended EFT of Inflation | 30 pages, 5 figures, 3 tables (updated to match the published
version) | JCAP 01 (2022) 01, 046 | 10.1088/1475-7516/2022/01/046 | null | hep-th astro-ph.CO gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | In earlier works, we studied the validity of Extended Effective Field Theory
of Inflation (EEFToI) in the regime where initial conditions are set with
dispersion relations $\omega^2 \propto k^6$. We had also evaluated and examined
the power spectrum for some interesting corners of the parameter space. In this
paper, ... | [
{
"created": "Tue, 12 Oct 2021 14:37:05 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Apr 2023 16:03:14 GMT",
"version": "v2"
}
] | 2023-04-28 | [
[
"Ashoorioon",
"Amjad",
""
],
[
"Geshnizjani",
"Ghazal",
""
],
[
"Kim",
"Hyung J.",
""
]
] | In earlier works, we studied the validity of Extended Effective Field Theory of Inflation (EEFToI) in the regime where initial conditions are set with dispersion relations $\omega^2 \propto k^6$. We had also evaluated and examined the power spectrum for some interesting corners of the parameter space. In this paper, we... | 8.467421 | 9.422743 | 8.20318 | 8.679778 | 8.721922 | 8.094172 | 8.958687 | 8.407538 | 7.75644 | 9.241149 | 8.399285 | 8.166214 | 8.494522 | 8.107581 | 8.198766 | 8.270811 | 7.98118 | 8.098668 | 8.019026 | 8.231595 | 8.076632 |
1907.06104 | H. T. Ozer | H. T. \"Ozer, Ayt\"ul Filiz | Exploring new Boundary Conditions for $\mathcal{N}=(1,1)$ Extended
Higher Spin $AdS_3$ Supergravity | 25 pages, no figures, LaTeX file, Sec.4 added, added references, a
few typos corrected | Eur. Phys. J. C (2020) 80:1072 | 10.1140/epjc/s10052-020-08613-4 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we present a candidate for $\mathcal{N}=(1,1)$ extended higher
- spin $AdS_3$ supergravity with the most general boundary conditions discussed
by Grumiller and Riegler recently. We show that the asymptotic symmetry algebra
consists of two copies of the $\mathfrak{osp}(3|2)_k$ affine algebra in the
pres... | [
{
"created": "Sat, 13 Jul 2019 16:44:07 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Jul 2019 11:41:43 GMT",
"version": "v2"
},
{
"created": "Sun, 3 May 2020 20:08:49 GMT",
"version": "v3"
},
{
"created": "Sun, 22 Nov 2020 08:45:54 GMT",
"version": "v4"
}
] | 2020-11-24 | [
[
"Özer",
"H. T.",
""
],
[
"Filiz",
"Aytül",
""
]
] | In this paper, we present a candidate for $\mathcal{N}=(1,1)$ extended higher - spin $AdS_3$ supergravity with the most general boundary conditions discussed by Grumiller and Riegler recently. We show that the asymptotic symmetry algebra consists of two copies of the $\mathfrak{osp}(3|2)_k$ affine algebra in the presen... | 6.146419 | 5.401731 | 6.851423 | 5.339838 | 5.843776 | 5.455273 | 5.838438 | 5.198024 | 5.480122 | 7.265906 | 5.448492 | 5.745213 | 5.823873 | 5.640642 | 5.885567 | 5.700911 | 5.77054 | 5.756904 | 5.662026 | 6.209167 | 5.67743 |
0804.4036 | Changrim Ahn | Changrim Ahn, Rafael Nepomechie | The Zamolodchikov-Faddeev algebra for open strings attached to giant
gravitons | 22 pages, no figure; added a reference | JHEP 0805:059,2008 | 10.1088/1126-6708/2008/05/059 | UMTG-256 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the Zamolodchikov-Faddeev algebra for the superstring sigma model
on $AdS_{5}\times S^{5}$, which was formulated by Arutyunov, Frolov and
Zamaklar, to the case of open strings attached to maximal giant gravitons,
which was recently considered by Hofman and Maldacena. We obtain boundary
$S$-matrices which sa... | [
{
"created": "Fri, 25 Apr 2008 02:14:37 GMT",
"version": "v1"
},
{
"created": "Thu, 1 May 2008 14:33:22 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Ahn",
"Changrim",
""
],
[
"Nepomechie",
"Rafael",
""
]
] | We extend the Zamolodchikov-Faddeev algebra for the superstring sigma model on $AdS_{5}\times S^{5}$, which was formulated by Arutyunov, Frolov and Zamaklar, to the case of open strings attached to maximal giant gravitons, which was recently considered by Hofman and Maldacena. We obtain boundary $S$-matrices which sati... | 4.944348 | 3.909463 | 6.303551 | 4.227851 | 4.150479 | 4.644707 | 4.501311 | 4.370216 | 4.787944 | 5.919299 | 4.346665 | 4.904802 | 5.367242 | 4.624336 | 4.603914 | 4.73433 | 4.806688 | 4.75216 | 4.707169 | 5.285861 | 4.626265 |
hep-th/9302032 | null | D. Dalmazi and E. Abdalla | Correlators in non-critical superstrings including the spinor emission
vertex | IFUSP preprint 1029, 10 pages | Phys.Lett. B312 (1993) 398-404 | 10.1016/0370-2693(93)90974-M | null | hep-th | null | We discuss the structure of correlators involving the spinor emission vertex
in non critical $N=1$ superstring theory. The technique used in the computation
is the zero mode integration to arrive at the integral representation, and
later an analysis of the pole structure of the integrals which are thus
obtained. Our ... | [
{
"created": "Tue, 9 Feb 1993 11:44:37 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dalmazi",
"D.",
""
],
[
"Abdalla",
"E.",
""
]
] | We discuss the structure of correlators involving the spinor emission vertex in non critical $N=1$ superstring theory. The technique used in the computation is the zero mode integration to arrive at the integral representation, and later an analysis of the pole structure of the integrals which are thus obtained. Our an... | 21.105125 | 19.767847 | 23.628862 | 17.745667 | 17.422409 | 20.581623 | 18.926971 | 17.143808 | 18.254639 | 23.703726 | 18.216005 | 18.361677 | 20.851368 | 17.988157 | 18.25281 | 18.71627 | 18.279341 | 17.943331 | 18.452154 | 20.738192 | 18.956856 |
hep-th/0205268 | Laurent Freidel | Laurent Freidel (PI, ENS-Lyon), Etera R. Livine (CPT Marseille) | Spin Networks for Non-Compact Groups | 43pages, many figures, some comments added | J.Math.Phys. 44 (2003) 1322-1356 | 10.1063/1.1521522 | null | hep-th gr-qc | null | Spin networks are natural generalization of Wilson loops functionals. They
have been extensively studied in the case where the gauge group is compact and
it has been shown that they naturally form a basis of gauge invariant
observables. Physically the restriction to compact gauge group is enough for
the study of Yang... | [
{
"created": "Mon, 27 May 2002 16:02:51 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jun 2002 10:06:46 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Freidel",
"Laurent",
"",
"PI, ENS-Lyon"
],
[
"Livine",
"Etera R.",
"",
"CPT Marseille"
]
] | Spin networks are natural generalization of Wilson loops functionals. They have been extensively studied in the case where the gauge group is compact and it has been shown that they naturally form a basis of gauge invariant observables. Physically the restriction to compact gauge group is enough for the study of Yang-m... | 8.970337 | 10.399092 | 9.759558 | 8.769348 | 9.611389 | 9.9225 | 9.918523 | 9.352457 | 9.42689 | 11.043341 | 9.332815 | 9.320039 | 9.086976 | 9.074571 | 9.276413 | 9.165149 | 9.035365 | 9.310058 | 9.264915 | 9.48135 | 9.063435 |
hep-th/0608111 | Antti J. Niemi | Ludvig D. Faddeev and Antti J. Niemi | Spin-Charge Separation, Conformal Covariance and the SU(2) Yang-Mills
Theory | some misprints in equations corrected | Nucl.Phys.B776:38-65,2007 | 10.1016/j.nuclphysb.2006.12.011 | null | hep-th cond-mat.str-el gr-qc hep-lat hep-ph | null | In the low energy domain of four-dimensional SU(2) Yang-Mills theory the spin
and the charge of the gauge field can become separated from each other. The
ensuing field variables describe the interacting dynamics between a version of
the O(3) nonlinear $\sigma$-model and a nonlinear Grassmannian $\sigma$-model,
both o... | [
{
"created": "Wed, 16 Aug 2006 14:17:18 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Aug 2006 19:00:58 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Faddeev",
"Ludvig D.",
""
],
[
"Niemi",
"Antti J.",
""
]
] | In the low energy domain of four-dimensional SU(2) Yang-Mills theory the spin and the charge of the gauge field can become separated from each other. The ensuing field variables describe the interacting dynamics between a version of the O(3) nonlinear $\sigma$-model and a nonlinear Grassmannian $\sigma$-model, both of ... | 9.794596 | 9.753859 | 10.008172 | 9.407763 | 10.059114 | 9.656755 | 9.423452 | 9.879333 | 9.480265 | 11.283403 | 9.765204 | 9.738341 | 9.756411 | 9.301735 | 9.650847 | 9.489523 | 9.524575 | 9.220203 | 9.280021 | 9.615288 | 9.550306 |
2008.11759 | Joshua Sandor | Simon Caron-Huot and Joshua Sandor | Conformal Regge Theory at Finite Boost | 29+5 pages, 17 figures | null | 10.1007/JHEP05(2021)059 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Operator Product Expansion is a useful tool to represent correlation
functions. In this note we extend Conformal Regge theory to provide an exact
OPE representation of Lorenzian four-point correlators in conformal field
theory, valid even away from Regge limit. The representation extends
convergence of the OPE by... | [
{
"created": "Wed, 26 Aug 2020 18:44:33 GMT",
"version": "v1"
}
] | 2021-05-26 | [
[
"Caron-Huot",
"Simon",
""
],
[
"Sandor",
"Joshua",
""
]
] | The Operator Product Expansion is a useful tool to represent correlation functions. In this note we extend Conformal Regge theory to provide an exact OPE representation of Lorenzian four-point correlators in conformal field theory, valid even away from Regge limit. The representation extends convergence of the OPE by r... | 11.580606 | 10.653626 | 15.486815 | 10.454446 | 10.709411 | 11.186678 | 11.539173 | 10.456602 | 10.648164 | 14.741996 | 10.312533 | 10.33681 | 12.373113 | 10.903087 | 10.511438 | 11.100784 | 11.494143 | 10.603083 | 10.990574 | 11.789943 | 10.67537 |
0803.0081 | Amos Yarom | Steven S. Gubser and Amos Yarom | Linearized hydrodynamics from probe-sources in the gauge-string duality | 43 pages, 3 appendices | Nucl.Phys.B813:188-219,2009 | 10.1016/j.nuclphysb.2008.12.032 | PUPT-2258, LMU-ASC 10/08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the response of an infinite, asymptotically static N=4 plasma to a
generic localized source in the probe approximation. At large distances, the
energy momentum tensor of the plasma includes a term which satisfies the
constitutive relations of linearized hydrodynamics, but it can also include a
non-hydrodynam... | [
{
"created": "Sat, 1 Mar 2008 21:06:40 GMT",
"version": "v1"
}
] | 2009-12-15 | [
[
"Gubser",
"Steven S.",
""
],
[
"Yarom",
"Amos",
""
]
] | We study the response of an infinite, asymptotically static N=4 plasma to a generic localized source in the probe approximation. At large distances, the energy momentum tensor of the plasma includes a term which satisfies the constitutive relations of linearized hydrodynamics, but it can also include a non-hydrodynamic... | 9.00428 | 9.883145 | 9.092184 | 8.821774 | 9.173412 | 10.002289 | 8.975848 | 9.239572 | 8.769213 | 9.668015 | 9.638447 | 8.976344 | 9.689063 | 8.757571 | 8.882116 | 9.137321 | 8.664617 | 8.722898 | 8.884943 | 9.179477 | 9.063088 |
0905.4633 | Stefano Bellucci | Stefano Bellucci and Sergey Krivonos | Potentials in N=4 superconformal mechanics | 12 pages, PACS number: 12.60.Jv | null | 10.1103/PhysRevD.80.065022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Proceeding from nonlinear realizations of (super)conformal symmetries, we
explicitly demonstrate that adding the harmonic oscillator potential to the
action of conformal mechanics does not break these symmetries but modifies the
transformation properties of the (super)fields. We also analyze the possibility
to introd... | [
{
"created": "Thu, 28 May 2009 12:51:54 GMT",
"version": "v1"
}
] | 2015-05-13 | [
[
"Bellucci",
"Stefano",
""
],
[
"Krivonos",
"Sergey",
""
]
] | Proceeding from nonlinear realizations of (super)conformal symmetries, we explicitly demonstrate that adding the harmonic oscillator potential to the action of conformal mechanics does not break these symmetries but modifies the transformation properties of the (super)fields. We also analyze the possibility to introduc... | 9.607158 | 9.727903 | 10.193192 | 9.030208 | 9.746083 | 8.912579 | 9.78822 | 9.08742 | 9.295572 | 10.513808 | 9.269142 | 9.070525 | 9.350604 | 8.825349 | 9.047102 | 9.140919 | 8.964539 | 9.220314 | 8.978566 | 9.409627 | 8.842781 |
1306.0145 | Andrei Mikhailov | Osvaldo Chandia, Andrei Mikhailov and Brenno C. Vallilo | A construction of integrated vertex operator in the pure spinor
sigma-model in AdS5xS5 | LaTeX 13pp; v2: correction in Section 4.1 | null | 10.1007/JHEP11(2013)124 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Vertex operators in string theory come in two varieties: integrated and
unintegrated. Understanding both types is important for the calculation of the
string theory amplitudes. The relation between them is a descent procedure
typically involving the b-ghost. In the pure spinor formalism vertex operators
can be identi... | [
{
"created": "Sat, 1 Jun 2013 20:03:48 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Sep 2013 21:51:14 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Chandia",
"Osvaldo",
""
],
[
"Mikhailov",
"Andrei",
""
],
[
"Vallilo",
"Brenno C.",
""
]
] | Vertex operators in string theory come in two varieties: integrated and unintegrated. Understanding both types is important for the calculation of the string theory amplitudes. The relation between them is a descent procedure typically involving the b-ghost. In the pure spinor formalism vertex operators can be identifi... | 10.302487 | 11.508102 | 11.213978 | 10.012621 | 11.210379 | 11.895436 | 11.275227 | 10.398005 | 9.942775 | 10.481873 | 10.443293 | 10.456687 | 10.285206 | 10.029065 | 10.305518 | 9.960021 | 10.421616 | 9.92922 | 9.961624 | 9.915118 | 10.103464 |
1704.02905 | Jan Ambjorn | J. Ambjorn and Y. Watabiki | CDT and the Big Bang | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a CDT-like model where breaking of W3 symmetry will lead to the
emergence of time and subsequently of space. Surprisingly the simplest such
models which lead to higher dimensional spacetimes are based on the four
"magical" Jordan algebras of 3x3 Hermitian matrices with real, complex,
quaternion and octoni... | [
{
"created": "Mon, 10 Apr 2017 15:25:26 GMT",
"version": "v1"
}
] | 2017-04-11 | [
[
"Ambjorn",
"J.",
""
],
[
"Watabiki",
"Y.",
""
]
] | We describe a CDT-like model where breaking of W3 symmetry will lead to the emergence of time and subsequently of space. Surprisingly the simplest such models which lead to higher dimensional spacetimes are based on the four "magical" Jordan algebras of 3x3 Hermitian matrices with real, complex, quaternion and octonion... | 11.902049 | 8.889785 | 11.762217 | 9.923327 | 9.313006 | 8.707453 | 8.5174 | 9.630958 | 9.755021 | 13.226204 | 9.885141 | 11.14758 | 11.153602 | 10.86507 | 10.626639 | 10.694416 | 10.970277 | 10.703476 | 10.724471 | 11.736518 | 10.57624 |
hep-th/0208077 | Andrei Mikhailov | Andrei Mikhailov | Nonspherical Giant Gravitons and Matrix Theory | 10 pages, LaTeX; references and explanations added; minor corrections | null | null | NSF-ITP-02-59, ITEP-TH-38/02 | hep-th | null | We consider the plane wave limit of the nonspherical giant gravitons. We
compute the Poisson brackets of the coordinate functions and find a nonlinear
algebra. We show that this algebra solves the supersymmetry conditions of the
matrix model. This is the generalization of the algebraic realization of the
spherical me... | [
{
"created": "Sat, 10 Aug 2002 17:06:00 GMT",
"version": "v1"
},
{
"created": "Sat, 5 Apr 2003 02:28:45 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Mikhailov",
"Andrei",
""
]
] | We consider the plane wave limit of the nonspherical giant gravitons. We compute the Poisson brackets of the coordinate functions and find a nonlinear algebra. We show that this algebra solves the supersymmetry conditions of the matrix model. This is the generalization of the algebraic realization of the spherical memb... | 14.026361 | 11.465347 | 14.700416 | 11.245045 | 13.610181 | 13.132661 | 12.546905 | 11.715768 | 12.443594 | 16.342985 | 12.232115 | 11.433586 | 13.560679 | 11.895268 | 11.929948 | 11.802705 | 11.767095 | 11.979073 | 12.212864 | 14.032042 | 11.791092 |
hep-th/9512064 | Shinya Wada | Hideaki Aoyama, Toshiyuki Harano, Masatoshi Sato, Shinya Wada | Valley Instanton versus Constrained Instanton | 37 pages, 8 eps figures, LaTeX, uses epsf.sty, citesort.sty and
wrapfig2.sty. Minor modifications | Nucl.Phys. B466 (1996) 127-158 | 10.1016/0550-3213(96)00066-1 | KUCP-0084, KUNS-1369 HE(TH)95/19 | hep-th | null | Based on the new valley equation, we propose the most plausible method for
constructing instanton-like configurations in the theory where the presence of
a mass scale prevents the existence of the classical solution with a finite
radius. We call the resulting instanton-like configuration as valley instanton.
The deta... | [
{
"created": "Mon, 11 Dec 1995 08:50:05 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Dec 1995 05:01:26 GMT",
"version": "v2"
},
{
"created": "Thu, 14 Dec 1995 03:06:24 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"Aoyama",
"Hideaki",
""
],
[
"Harano",
"Toshiyuki",
""
],
[
"Sato",
"Masatoshi",
""
],
[
"Wada",
"Shinya",
""
]
] | Based on the new valley equation, we propose the most plausible method for constructing instanton-like configurations in the theory where the presence of a mass scale prevents the existence of the classical solution with a finite radius. We call the resulting instanton-like configuration as valley instanton. The detail... | 14.487928 | 14.415273 | 12.535111 | 12.707017 | 13.500216 | 14.585856 | 13.614612 | 13.4779 | 13.10854 | 14.642867 | 13.541605 | 13.181741 | 12.779979 | 12.702976 | 13.303666 | 13.127646 | 13.000861 | 13.073947 | 13.090972 | 12.812937 | 13.182075 |
hep-th/9602036 | J. C. Gallardo | Jose F. Cari\~nena and J. Nasarre | On the symplectic structures arising in Optics | AmsTeX file and 2 figures (epsf required). To appear in Forsch. der
Physik. This version replaces that of (96/02/09) where postcript files
containing figures were corrupted | Fortsch.Phys. 44 (1996) 181-198 | 10.1002/prop.2190440302 | DFTUZ 96/05 | hep-th | null | Geometric optics is analysed using the techniques of Presymplectic Geometry.
We obtain the symplectic structure of the space of light rays in a medium of a
non constant refractive index by reduction from a presymplectic structure, and
using adapted coordinates, we find Darboux coordinates. The theory is
illustrated w... | [
{
"created": "Thu, 8 Feb 1996 09:40:06 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Feb 1996 18:07:11 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Cariñena",
"Jose F.",
""
],
[
"Nasarre",
"J.",
""
]
] | Geometric optics is analysed using the techniques of Presymplectic Geometry. We obtain the symplectic structure of the space of light rays in a medium of a non constant refractive index by reduction from a presymplectic structure, and using adapted coordinates, we find Darboux coordinates. The theory is illustrated wit... | 11.443919 | 10.845391 | 11.05689 | 10.096047 | 11.23961 | 11.656244 | 11.384556 | 10.768991 | 10.509172 | 11.000454 | 10.198933 | 10.892382 | 11.061138 | 10.626482 | 10.573443 | 10.797178 | 10.570596 | 11.097501 | 10.873874 | 10.264927 | 10.417026 |
hep-th/9411171 | Nicholas Landsman | N.P. Landsman | The infinite unitary group, Howe dual pairs, and the quantization of
constrained systems | LaTeX, 43 pages | null | null | null | hep-th | null | The irreducible unitary representations of the Banach Lie group $U_0(\H)$
(which is the norm-closure of the inductive limit $\cup_k U(k)$) of unitary
operators on a separable Hilbert space $\H$, which were found by Kirillov and
Ol'shanskii, are reconstructed from quantization theory. Firstly, the coadjoint
orbits of ... | [
{
"created": "Wed, 23 Nov 1994 17:34:24 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Landsman",
"N. P.",
""
]
] | The irreducible unitary representations of the Banach Lie group $U_0(\H)$ (which is the norm-closure of the inductive limit $\cup_k U(k)$) of unitary operators on a separable Hilbert space $\H$, which were found by Kirillov and Ol'shanskii, are reconstructed from quantization theory. Firstly, the coadjoint orbits of th... | 9.852958 | 11.488291 | 10.696073 | 10.432375 | 11.136776 | 11.671417 | 11.592561 | 10.990388 | 10.409601 | 12.309267 | 10.66168 | 9.450958 | 9.697247 | 9.278041 | 9.900173 | 9.703842 | 9.691566 | 9.567429 | 9.298369 | 9.898581 | 9.379443 |
0712.0850 | Sergey Cherkis | Sergey A. Cherkis and Brian Durcan | Singular Monopoles via the Nahm Transform | 10 pages, LaTeX | JHEP0804:070,2008 | 10.1088/1126-6708/2008/04/070 | TCDMATH 07-23, HMI 07-10 | hep-th | null | We present explicit expressions for the fields of a charge one BPS monopole
with two Dirac singularities. These are solutions of the nonlinear Bogomolny
equations with the gauge group U(2) or SO(3). We derive these expressions by
applying the technique of the Nahm transform. By exploring various limits we
find a numb... | [
{
"created": "Wed, 5 Dec 2007 23:37:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cherkis",
"Sergey A.",
""
],
[
"Durcan",
"Brian",
""
]
] | We present explicit expressions for the fields of a charge one BPS monopole with two Dirac singularities. These are solutions of the nonlinear Bogomolny equations with the gauge group U(2) or SO(3). We derive these expressions by applying the technique of the Nahm transform. By exploring various limits we find a number... | 10.161479 | 8.102996 | 11.064791 | 9.279466 | 8.105005 | 8.492209 | 8.5358 | 8.366259 | 8.39596 | 13.658128 | 8.035786 | 8.678601 | 10.224377 | 8.64924 | 8.968266 | 8.502761 | 8.483207 | 8.896835 | 8.795799 | 9.996694 | 8.699193 |
1402.6937 | Dmitry Ageev | D. S. Ageev and I.Ya. Aref'eva | Holography and non-local operators in the BTZ black hole with non-zero
angular momentum | LaTex, 18 pages, 10 figures | null | 10.1007/s11232-014-0186-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study quark-antiquark potential using the AdS/CFT correspondence in the
BTZ black hole with non-zero angular momentum. Using explicit form of string
configurations relevant to a calculation of the potential we find that the
potential exhibits different dependencies on angular momentum values in the
Euclidean and t... | [
{
"created": "Thu, 27 Feb 2014 15:29:52 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Ageev",
"D. S.",
""
],
[
"Aref'eva",
"I. Ya.",
""
]
] | We study quark-antiquark potential using the AdS/CFT correspondence in the BTZ black hole with non-zero angular momentum. Using explicit form of string configurations relevant to a calculation of the potential we find that the potential exhibits different dependencies on angular momentum values in the Euclidean and the... | 10.331404 | 8.857056 | 9.996701 | 9.212949 | 9.598075 | 8.996758 | 9.990296 | 9.254303 | 9.238181 | 10.428218 | 8.971528 | 8.515406 | 10.467345 | 9.071509 | 9.25302 | 9.113894 | 8.973374 | 9.546333 | 9.030114 | 10.026165 | 8.798199 |
2306.06682 | ChenWei Tong | Chen-Wei Tong, Dong-Hui Du, Jia-Rui Sun | Island of Reissner-Nordstr$\mathbf{\ddot{o}}$m anti-de Sitter black
holes in the large $d$ limit | 25 pages, 7 figures | null | 10.1103/PhysRevD.109.104053 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the information paradox of Reissner-Nordstr${\ddot{o}}$m anti-de
Sitter (RN-AdS$_{d+1}$) black holes in the large dimension limit by using the
island formula. The entanglement entropy of Hawking radiation is calculated
both for the non-extremal and the extremal cases, in which the boundary of the
radiation r... | [
{
"created": "Sun, 11 Jun 2023 13:57:08 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Jun 2024 04:18:07 GMT",
"version": "v2"
}
] | 2024-06-17 | [
[
"Tong",
"Chen-Wei",
""
],
[
"Du",
"Dong-Hui",
""
],
[
"Sun",
"Jia-Rui",
""
]
] | We study the information paradox of Reissner-Nordstr${\ddot{o}}$m anti-de Sitter (RN-AdS$_{d+1}$) black holes in the large dimension limit by using the island formula. The entanglement entropy of Hawking radiation is calculated both for the non-extremal and the extremal cases, in which the boundary of the radiation reg... | 4.863372 | 4.383706 | 4.853426 | 4.354303 | 4.177856 | 4.50339 | 4.341859 | 4.199492 | 4.34032 | 4.972074 | 4.334579 | 4.409003 | 4.673621 | 4.466395 | 4.43446 | 4.516399 | 4.359759 | 4.439684 | 4.505844 | 4.651291 | 4.52156 |
hep-th/0409134 | Marco A. RegoMonteiro | V. B. Bezerra and M. A. Rego-Monteiro | Some boundary effects in quantum field theory | 12 pages, Latex | Phys.Rev. D70 (2004) 065018 | 10.1103/PhysRevD.70.065018 | null | hep-th | null | We have constructed a quantum field theory in a finite box, with periodic
boundary conditions, using the hypothesis that particles living in a finite box
are created and/or annihilated by the creation and/or annihilation operators,
respectively, of a quantum harmonic oscillator on a circle. An expression for
the effe... | [
{
"created": "Tue, 14 Sep 2004 18:09:23 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Bezerra",
"V. B.",
""
],
[
"Rego-Monteiro",
"M. A.",
""
]
] | We have constructed a quantum field theory in a finite box, with periodic boundary conditions, using the hypothesis that particles living in a finite box are created and/or annihilated by the creation and/or annihilation operators, respectively, of a quantum harmonic oscillator on a circle. An expression for the effect... | 9.639717 | 9.138955 | 9.485022 | 8.966004 | 9.510118 | 9.690151 | 9.305755 | 8.84335 | 9.067124 | 9.604535 | 8.815527 | 8.78762 | 8.463662 | 9.080646 | 8.844092 | 8.988118 | 8.976229 | 8.794101 | 9.180808 | 8.994807 | 8.764832 |
1002.2292 | Yong-Wan Kim | Yun Soo Myung, Yong-Wan Kim | Entropic force and entanglement system | 17 pages, 2 figures, version to appear in PRD | Phys.Rev.D81:105012,2010 | 10.1103/PhysRevD.81.105012 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce the isothermal cavity, static holographic screen, and
accelerating surface as holographic screen to study the entropic force in the
presence of the Schwarzschild black hole. These may merge to provide a
consistent holographic screen to define the entropic force on the stretched
horizon near the event hor... | [
{
"created": "Thu, 11 Feb 2010 08:00:17 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Apr 2010 04:22:51 GMT",
"version": "v2"
}
] | 2010-05-19 | [
[
"Myung",
"Yun Soo",
""
],
[
"Kim",
"Yong-Wan",
""
]
] | We introduce the isothermal cavity, static holographic screen, and accelerating surface as holographic screen to study the entropic force in the presence of the Schwarzschild black hole. These may merge to provide a consistent holographic screen to define the entropic force on the stretched horizon near the event horiz... | 15.820013 | 14.870216 | 16.704229 | 13.900617 | 14.147303 | 14.262222 | 14.826734 | 15.179125 | 14.313043 | 18.002945 | 14.178534 | 15.603302 | 15.777043 | 14.88305 | 14.963767 | 14.890283 | 15.198205 | 15.839525 | 15.66641 | 16.147135 | 15.365373 |
1507.02174 | Ian Jack | J.A. Gracey, I. Jack and C. Poole | The a-function in six dimensions | 27 pages, seven figures, uses axodraw. Minor improvements in wording | null | 10.1007/JHEP01(2016)174 | LTH1045 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The a-function is a proposed quantity defined in even dimensions which has a
monotonic behaviour along RG flows, related to the beta-functions via a
gradient flow equation. We study the a-function for a general scalar theory in
six dimensions, using the beta-functions up to three-loop order for both the
MSbar and MOM... | [
{
"created": "Wed, 8 Jul 2015 14:32:37 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Oct 2015 15:20:28 GMT",
"version": "v2"
},
{
"created": "Mon, 14 Dec 2015 17:57:38 GMT",
"version": "v3"
},
{
"created": "Mon, 11 Jan 2016 14:47:56 GMT",
"version": "v4"
}
] | 2016-03-23 | [
[
"Gracey",
"J. A.",
""
],
[
"Jack",
"I.",
""
],
[
"Poole",
"C.",
""
]
] | The a-function is a proposed quantity defined in even dimensions which has a monotonic behaviour along RG flows, related to the beta-functions via a gradient flow equation. We study the a-function for a general scalar theory in six dimensions, using the beta-functions up to three-loop order for both the MSbar and MOM s... | 13.596631 | 9.450247 | 12.015779 | 9.122767 | 10.077962 | 8.705513 | 9.523605 | 8.121902 | 8.251545 | 12.229157 | 9.120625 | 11.18879 | 11.953354 | 11.431536 | 10.730723 | 10.726089 | 11.475843 | 10.712857 | 10.588758 | 12.33337 | 11.804132 |
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