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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0710.4961 | V. Parameswaran Nair | V.P. Nair | A Note on Graviton Amplitudes for New Twistor String Theories | 10 pages | Phys.Rev.D78:041501,2008 | 10.1103/PhysRevD.78.041501 | CCNY-HEP 07/5 | hep-th | null | A new class of twistor string theories were recently constructed by
Abou-Zeid, Hull and Mason. The most interesting one of these theories has the
particle content of N=8 supergravity. Arguments are given for the vanishing of
the (+ - -)-helicity amplitude for gravitons which suggest that this theory
describes a chira... | [
{
"created": "Fri, 26 Oct 2007 02:29:52 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Nair",
"V. P.",
""
]
] | A new class of twistor string theories were recently constructed by Abou-Zeid, Hull and Mason. The most interesting one of these theories has the particle content of N=8 supergravity. Arguments are given for the vanishing of the (+ - -)-helicity amplitude for gravitons which suggest that this theory describes a chiral ... | 11.967449 | 13.628004 | 15.302237 | 11.951655 | 13.035891 | 14.108886 | 12.633478 | 13.233759 | 11.377373 | 15.97799 | 12.873545 | 10.949491 | 10.400155 | 9.995167 | 10.987131 | 10.671764 | 10.609713 | 10.613065 | 10.381064 | 10.979876 | 9.855659 |
2112.07682 | Timo Weigand | Seung-Joo Lee and Timo Weigand | Elliptic K3 Surfaces at Infinite Complex Structure and their Refined
Kulikov models | 71 pages, 6 Figures | null | 10.1007/JHEP09(2022)143 | null | hep-th math.AG | http://creativecommons.org/licenses/by/4.0/ | Motivated by the Swampland Distance and the Emergent String Conjecture of
Quantum Gravity, we analyse the infinite distance degenerations in the complex
structure moduli space of elliptic K3 surfaces. All complex degenerations of K3
surfaces are known to be classified according to their associated Kulikov
models of T... | [
{
"created": "Tue, 14 Dec 2021 19:00:02 GMT",
"version": "v1"
}
] | 2022-10-19 | [
[
"Lee",
"Seung-Joo",
""
],
[
"Weigand",
"Timo",
""
]
] | Motivated by the Swampland Distance and the Emergent String Conjecture of Quantum Gravity, we analyse the infinite distance degenerations in the complex structure moduli space of elliptic K3 surfaces. All complex degenerations of K3 surfaces are known to be classified according to their associated Kulikov models of Typ... | 8.179189 | 7.983795 | 8.610072 | 7.571128 | 8.095263 | 8.3007 | 8.108544 | 8.033893 | 7.644177 | 9.529003 | 7.772697 | 8.219054 | 8.584105 | 7.895865 | 8.335591 | 8.189133 | 7.897058 | 7.935995 | 8.244712 | 8.550607 | 7.99175 |
hep-th/9401066 | null | A Kundu and Orlando Ragnisco | A Simple Lattice Version of the Nonlinear Schrodinger Equation and its
Deformation with Exact Quantum Solution | 14 pages (plain TEX) | J.Phys. A27 (1994) 6335-6348 | 10.1088/0305-4470/27/19/008 | null | hep-th | null | A lattice version of quantum nonlinear Schrodinger (NLS) equation is
considered, which has significantly simple form and fullfils most of the
criteria desirable for such lattice variants of field models. Unlike most of
the known lattice NLS, the present model belongs to a class which does not
exhibit the usual symmet... | [
{
"created": "Fri, 14 Jan 1994 12:31:01 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Feb 1994 15:35:33 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Kundu",
"A",
""
],
[
"Ragnisco",
"Orlando",
""
]
] | A lattice version of quantum nonlinear Schrodinger (NLS) equation is considered, which has significantly simple form and fullfils most of the criteria desirable for such lattice variants of field models. Unlike most of the known lattice NLS, the present model belongs to a class which does not exhibit the usual symmetry... | 14.578875 | 12.955191 | 15.166395 | 13.91589 | 13.78867 | 14.222806 | 14.283491 | 13.221998 | 13.122023 | 16.393599 | 13.188128 | 13.360827 | 14.880911 | 13.355162 | 13.214192 | 12.945841 | 13.617075 | 13.185085 | 13.414048 | 14.54344 | 12.922648 |
1910.10427 | Jeremy Mann | Matthias R. Gaberdiel and Jeremy A. Mann | Stringy CFT Duals with $\mathcal{N} = (2,2)$ Supersymmetry | 15 pages, no figures | JHEP 2001 (2020) 160 | 10.1007/JHEP01(2020)160 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was recently shown that string theory on $\mathrm{AdS}_3 \times
\mathrm{S}^3 \times \mathbb{T}^4$ with minimal NS-NS flux ($k = 1$) is exactly
dual to the symmetric orbifold of T4. Here we show that a similar statement
also holds for the $D_n$ orbifolds of these backgrounds that have $\mathcal{N}
= (2, 2)$ supersy... | [
{
"created": "Wed, 23 Oct 2019 09:25:21 GMT",
"version": "v1"
}
] | 2020-02-05 | [
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Mann",
"Jeremy A.",
""
]
] | It was recently shown that string theory on $\mathrm{AdS}_3 \times \mathrm{S}^3 \times \mathbb{T}^4$ with minimal NS-NS flux ($k = 1$) is exactly dual to the symmetric orbifold of T4. Here we show that a similar statement also holds for the $D_n$ orbifolds of these backgrounds that have $\mathcal{N} = (2, 2)$ supersymm... | 4.708581 | 3.336745 | 5.442231 | 3.770979 | 3.620195 | 3.536297 | 3.777601 | 3.509172 | 3.721972 | 5.295122 | 3.778996 | 3.912377 | 4.796018 | 4.166676 | 4.114346 | 4.197894 | 4.102479 | 4.107512 | 4.050735 | 4.822433 | 4.099668 |
1804.04409 | Stefan Lippoldt | Stefan Lippoldt | Renormalized Functional Renormalization Group | 5+1 pages | Phys.Lett. B782 (2018) 275-279 | 10.1016/j.physletb.2018.05.037 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a new version of the effective average action together with its
flow equation. The construction entails in particular the consistency of
fluctuation field and background field equations of motion, even for finite
renormalization group scales. Here we focus on the quantum gravity application,
while the ge... | [
{
"created": "Thu, 12 Apr 2018 10:20:30 GMT",
"version": "v1"
},
{
"created": "Tue, 29 May 2018 07:47:11 GMT",
"version": "v2"
}
] | 2018-05-30 | [
[
"Lippoldt",
"Stefan",
""
]
] | We construct a new version of the effective average action together with its flow equation. The construction entails in particular the consistency of fluctuation field and background field equations of motion, even for finite renormalization group scales. Here we focus on the quantum gravity application, while the gene... | 12.649108 | 13.074146 | 12.863438 | 11.761124 | 13.194123 | 12.518178 | 12.267328 | 11.648379 | 11.415219 | 11.363422 | 11.774259 | 12.069201 | 12.059654 | 11.476694 | 11.843822 | 11.544891 | 11.771509 | 11.758306 | 11.905106 | 11.876266 | 11.111112 |
1703.01337 | Davood Momeni Dr | Davood Momeni, Mir Faizal, Ratbay Myrzakulov | Holographic Cavalieri Principle as a Universal relation between
Holographic Complexity and Holographic Entanglement Entropy | 15 pages, Major revision | Int. J. Mod. Phys. D 27, no.09, 1850103 (2018) | 10.1142/S0218271818501031 | null | hep-th cond-mat.stat-mech gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we will propose a universal relation between the holographic
complexity (dual to a volume in AdS) and the holographic entanglement entropy
(dual to an area in AdS). We will explicitly demonstrate that our conjuncture
hold for all a metric asymptotic to AdS$_3$, and then argue that such a
relation shoul... | [
{
"created": "Tue, 31 Jan 2017 15:35:14 GMT",
"version": "v1"
},
{
"created": "Sun, 3 Dec 2017 16:17:21 GMT",
"version": "v2"
}
] | 2018-08-02 | [
[
"Momeni",
"Davood",
""
],
[
"Faizal",
"Mir",
""
],
[
"Myrzakulov",
"Ratbay",
""
]
] | In this paper, we will propose a universal relation between the holographic complexity (dual to a volume in AdS) and the holographic entanglement entropy (dual to an area in AdS). We will explicitly demonstrate that our conjuncture hold for all a metric asymptotic to AdS$_3$, and then argue that such a relation should ... | 9.721737 | 8.303048 | 9.955784 | 8.334761 | 9.364038 | 8.942052 | 8.943259 | 8.20751 | 8.325841 | 10.506998 | 8.57163 | 8.687495 | 9.078005 | 8.60608 | 9.020772 | 8.783518 | 8.684247 | 8.704889 | 8.90618 | 9.249421 | 8.905452 |
hep-th/9808111 | Kazutoshi Ohta | Takuhiro Kitao, Kazutoshi Ohta and Nobuyoshi Ohta | Three-Dimensional Gauge Dynamics from Brane Configurations with
(p,q)-Fivebrane | 36 pages, 9 figures, signs in table 1 are corrected | Nucl.Phys. B539 (1999) 79-106 | 10.1016/S0550-3213(98)00726-3 | UT-Komaba/98-19, YITP-98-55, OU-HET 302 | hep-th | null | We study three-dimensional gauge dynamics by using type IIB superstring brane
configurations, which can be obtained from the M-theory configuration of
M2-branes stretched between two M5-branes with relative angles. Our
construction of brane configurations includes (p,q)5-brane and gives a
systematic classification of... | [
{
"created": "Wed, 19 Aug 1998 07:58:59 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Aug 1998 06:51:20 GMT",
"version": "v2"
},
{
"created": "Mon, 26 Oct 1998 04:36:33 GMT",
"version": "v3"
},
{
"created": "Mon, 8 Feb 1999 06:13:42 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Kitao",
"Takuhiro",
""
],
[
"Ohta",
"Kazutoshi",
""
],
[
"Ohta",
"Nobuyoshi",
""
]
] | We study three-dimensional gauge dynamics by using type IIB superstring brane configurations, which can be obtained from the M-theory configuration of M2-branes stretched between two M5-branes with relative angles. Our construction of brane configurations includes (p,q)5-brane and gives a systematic classification of p... | 12.385956 | 10.401412 | 14.603362 | 11.025257 | 10.770358 | 11.452419 | 11.232693 | 11.272616 | 11.636594 | 16.64739 | 10.840592 | 11.251876 | 13.433455 | 11.873899 | 11.585532 | 11.1218 | 11.564807 | 11.502345 | 11.682984 | 13.468006 | 11.362245 |
1906.04752 | Francisco Pe\~na-Ben\'itez | Carlos Hoyos, Francisco Pe\~na-Benitez and Piotr Witkowski | Hall Viscosity in a Strongly Coupled Magnetized Plasma | 27 pages, 3 appendices and 3 figures. Published version | null | 10.1007/JHEP08(2019)146 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how a Hall viscosity induced by a magnetic field can be generated in
strongly coupled theories with a holographic dual. This is achieved by
considering parity-breaking higher derivative terms in the gravity dual. These
terms couple the Riemann curvature tensor to the field strength of a gauge
field dual to th... | [
{
"created": "Tue, 11 Jun 2019 18:00:52 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Aug 2019 13:46:34 GMT",
"version": "v2"
}
] | 2019-10-02 | [
[
"Hoyos",
"Carlos",
""
],
[
"Peña-Benitez",
"Francisco",
""
],
[
"Witkowski",
"Piotr",
""
]
] | We show how a Hall viscosity induced by a magnetic field can be generated in strongly coupled theories with a holographic dual. This is achieved by considering parity-breaking higher derivative terms in the gravity dual. These terms couple the Riemann curvature tensor to the field strength of a gauge field dual to the ... | 7.796525 | 7.800635 | 7.383166 | 7.351763 | 7.389435 | 7.606803 | 8.077529 | 7.330534 | 7.10155 | 8.388245 | 7.714768 | 7.560736 | 7.412755 | 7.469651 | 7.60911 | 7.308874 | 7.477165 | 7.439996 | 7.20923 | 7.548638 | 7.446292 |
1209.2860 | Daniel Grumiller | H. Afshar, M. Gary, D. Grumiller, R. Rashkov and M. Riegler | Non-AdS holography in 3-dimensional higher spin gravity - General recipe
and example | 23pp, v2: added Ref. [25], corrected typo in (5.4c) | JHEP11 (2012) 099 | 10.1007/JHEP11(2012)099 | TUW-12-22 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the general algorithm to establish the classical and quantum
asymptotic symmetry algebra for non-AdS higher spin gravity and implement it
for the specific example of spin-3 gravity in the non-principal embedding with
Lobachevsky (H^2xR) boundary conditions. The asymptotic symmetry algebra for
this example ... | [
{
"created": "Thu, 13 Sep 2012 11:44:38 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Nov 2012 11:19:47 GMT",
"version": "v2"
}
] | 2013-06-18 | [
[
"Afshar",
"H.",
""
],
[
"Gary",
"M.",
""
],
[
"Grumiller",
"D.",
""
],
[
"Rashkov",
"R.",
""
],
[
"Riegler",
"M.",
""
]
] | We present the general algorithm to establish the classical and quantum asymptotic symmetry algebra for non-AdS higher spin gravity and implement it for the specific example of spin-3 gravity in the non-principal embedding with Lobachevsky (H^2xR) boundary conditions. The asymptotic symmetry algebra for this example co... | 11.385291 | 10.074833 | 12.874275 | 10.616145 | 9.958176 | 10.019515 | 11.357567 | 9.403428 | 9.708019 | 13.232406 | 10.2483 | 10.284162 | 10.452118 | 10.761525 | 10.828968 | 11.451595 | 11.022836 | 10.571285 | 10.98313 | 11.448029 | 11.104715 |
hep-th/9712228 | Fernando T. Brandt | F. T. Brandt, J. Frenkel, A. Guerra | The Boltzmann Equation in Scalar Field Theory | 10 pages, using RevTeX (corrected TeX misprints) | Int.J.Mod.Phys. A13 (1998) 4281 | 10.1142/S0217751X98002067 | null | hep-th | null | We derive the classical transport equation, in scalar field theory with a
V(phi) interaction, from the equation of motion for the quantum field. We
obtain a very simple, but iterative, expression for the effective action which
generates all the n-point Green functions in the high-temperature limit. An
explicit closed... | [
{
"created": "Wed, 24 Dec 1997 13:45:02 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Jan 1998 16:17:50 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Brandt",
"F. T.",
""
],
[
"Frenkel",
"J.",
""
],
[
"Guerra",
"A.",
""
]
] | We derive the classical transport equation, in scalar field theory with a V(phi) interaction, from the equation of motion for the quantum field. We obtain a very simple, but iterative, expression for the effective action which generates all the n-point Green functions in the high-temperature limit. An explicit closed f... | 14.152225 | 13.230261 | 11.724986 | 12.279368 | 11.660973 | 13.598661 | 13.057303 | 12.55794 | 11.620014 | 13.056407 | 12.504183 | 13.12201 | 12.431981 | 12.466756 | 12.484746 | 13.21966 | 12.61951 | 12.887004 | 12.389588 | 13.281922 | 12.754007 |
hep-th/9807064 | Henrik Gustafsson | H. Gustafsson, U. Lindstrom | A Picture of D-branes at Strong Coupling II. Spinning Partons | 14 pages, Latex | Phys.Lett. B440 (1998) 43-49 | 10.1016/S0370-2693(98)01080-6 | USITP-98-13 | hep-th | null | We study the Born-Infeld D-brane action in the limit when the string coupling
goes to infinity. The resulting actions is presented in an arbitrary background
and shown to describe a foliation of the world-volume by strings. Using a
recently developed ``degenerate'' supergravity the parton picture is shown to
be appli... | [
{
"created": "Thu, 9 Jul 1998 12:56:59 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Gustafsson",
"H.",
""
],
[
"Lindstrom",
"U.",
""
]
] | We study the Born-Infeld D-brane action in the limit when the string coupling goes to infinity. The resulting actions is presented in an arbitrary background and shown to describe a foliation of the world-volume by strings. Using a recently developed ``degenerate'' supergravity the parton picture is shown to be applica... | 16.661921 | 13.401252 | 14.084372 | 14.299328 | 16.040213 | 14.414988 | 13.546362 | 14.006047 | 14.230593 | 16.396969 | 13.977269 | 14.261192 | 17.591372 | 14.290518 | 14.017563 | 15.236234 | 14.263175 | 14.057437 | 14.050373 | 16.047609 | 13.962708 |
1706.09234 | Romanczukiewicz Tomasz Ph.D. | Tomasz Roma\'nczukiewicz and Yakov Shnir | Oscillons in the presence of external potential | 24 pages, 15 figures, largely expanded version | JHEP01(2018)101 | 10.1007/JHEP01(2018)101 | null | hep-th nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss similarity between oscillons and oscillational mode in perturbed
$\phi^4$. For small depths of the perturbing potential it is difficult to
distinguish between oscillons and the mode in moderately long time evolution,
moreover one can transform one into the other by adiabatically switching on and
off the po... | [
{
"created": "Wed, 28 Jun 2017 12:09:04 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Dec 2017 11:42:00 GMT",
"version": "v2"
}
] | 2018-01-23 | [
[
"Romańczukiewicz",
"Tomasz",
""
],
[
"Shnir",
"Yakov",
""
]
] | We discuss similarity between oscillons and oscillational mode in perturbed $\phi^4$. For small depths of the perturbing potential it is difficult to distinguish between oscillons and the mode in moderately long time evolution, moreover one can transform one into the other by adiabatically switching on and off the pote... | 16.30505 | 17.624607 | 15.900814 | 14.618651 | 16.791712 | 17.894468 | 16.982986 | 14.760953 | 14.821591 | 18.017536 | 15.533101 | 15.202554 | 16.318773 | 14.319576 | 15.454829 | 15.404633 | 15.220142 | 15.455421 | 14.61877 | 14.448697 | 15.181027 |
hep-th/0106202 | Machiko Hatsuda | Machiko Hatsuda and Kiyoshi Kamimura | Classical AdS Superstring Mechanics | 16 pageg, Latex | Nucl.Phys. B611 (2001) 77-92 | 10.1016/S0550-3213(01)00338-8 | null | hep-th | null | We analyze the anti-de Sitter (AdS) superparticle and superstring systems
described in terms of supermatrix valued coordinates proposed by Roiban and
Siegel. This approach gives simple symmetry transformations and equations of
motion. We examine their kappa-transformations, infinite reducibility and
kappa-gauge fixin... | [
{
"created": "Fri, 22 Jun 2001 07:39:52 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Hatsuda",
"Machiko",
""
],
[
"Kamimura",
"Kiyoshi",
""
]
] | We analyze the anti-de Sitter (AdS) superparticle and superstring systems described in terms of supermatrix valued coordinates proposed by Roiban and Siegel. This approach gives simple symmetry transformations and equations of motion. We examine their kappa-transformations, infinite reducibility and kappa-gauge fixing ... | 12.284766 | 12.425781 | 13.852708 | 11.494877 | 11.869902 | 11.919494 | 11.260984 | 11.161106 | 11.177377 | 14.53894 | 10.908839 | 11.149951 | 12.2093 | 11.866373 | 11.360983 | 11.468713 | 11.3115 | 10.935056 | 11.788791 | 11.765577 | 11.276258 |
1907.00699 | Jun Zhang | Claudia de Rham, Jun Zhang | Perturbations of Stealth Black Holes in DHOST Theories | 18 pages, discussion and references added | Phys. Rev. D 100, 124023 (2019) | 10.1103/PhysRevD.100.124023 | Imperial/TP/2019/CdR/03 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Among the Scalar-Tensor modified theories of gravity, DHOST models could play
a special role for dark energy while being consistent with current
observations, notably those constraining the speed of gravitational waves.
Schwarzschild-de Sitter black holes were shown to be exact solutions of a
particular subclass of q... | [
{
"created": "Mon, 1 Jul 2019 12:24:07 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Aug 2019 10:02:51 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"de Rham",
"Claudia",
""
],
[
"Zhang",
"Jun",
""
]
] | Among the Scalar-Tensor modified theories of gravity, DHOST models could play a special role for dark energy while being consistent with current observations, notably those constraining the speed of gravitational waves. Schwarzschild-de Sitter black holes were shown to be exact solutions of a particular subclass of qua... | 10.861758 | 12.331312 | 10.239587 | 10.586457 | 11.049545 | 11.940914 | 11.664314 | 10.909104 | 10.84515 | 11.713742 | 10.665361 | 10.644262 | 10.389803 | 10.446308 | 10.645133 | 10.548229 | 10.9951 | 10.445835 | 10.314631 | 10.485828 | 10.405284 |
2312.10629 | N.D. Hari Dass | N.D. Hari Dass | Effective String Theories (EST) of Yang-Mills Flux Tubes | This is a preprint of Chapter 22 of the following work: N.D. Hari
Dass, Strings to Strings,2023,Springer reproduced with permission of Springer
Nature Switzerland AG 2023. The final authenticated version is available
online at the external DOI given below. In v2, typo in ref[47] has been
corrected, and a new re... | null | 10.1007/978-3-031-35358-1 | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This chapter explains the concept of \emph{Effective String Theories}(EST),
and their success in explaining the results that Yang-Mills flux tubes behave,
to a high degree of accuracy, like Bosonic Strings(BST). It describes EST's of
L\"uscher and Weisz, and their principal conclusions. It then discusses the
Polchins... | [
{
"created": "Sun, 17 Dec 2023 07:00:33 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Mar 2024 06:52:35 GMT",
"version": "v2"
}
] | 2024-03-26 | [
[
"Dass",
"N. D. Hari",
""
]
] | This chapter explains the concept of \emph{Effective String Theories}(EST), and their success in explaining the results that Yang-Mills flux tubes behave, to a high degree of accuracy, like Bosonic Strings(BST). It describes EST's of L\"uscher and Weisz, and their principal conclusions. It then discusses the Polchinski... | 15.29668 | 16.188179 | 15.55471 | 14.827013 | 15.771536 | 15.690169 | 15.309656 | 15.449999 | 14.941091 | 16.767471 | 15.493168 | 15.347013 | 14.952501 | 14.863823 | 15.369407 | 15.128778 | 15.245163 | 14.815458 | 14.691586 | 14.652792 | 15.248082 |
1510.01896 | Yegor Zenkevich | A. Morozov, Y. Zenkevich | Decomposing Nekrasov Decomposition | 29 pages, 7 figures | JHEP 1602 (2016) 098 | 10.1007/JHEP02(2016)098 | ITEP/TH-35/15, IITP/TH-15/15, INR-TH/2015-027 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | AGT relations imply that the four-point conformal block admits a
decomposition into a sum over pairs of Young diagrams of essentially rational
Nekrasov functions - this is immediately seen when conformal block is
represented in the form of a matrix model. However, the q-deformation of the
same block has a deeper deco... | [
{
"created": "Wed, 7 Oct 2015 11:19:06 GMT",
"version": "v1"
}
] | 2016-02-24 | [
[
"Morozov",
"A.",
""
],
[
"Zenkevich",
"Y.",
""
]
] | AGT relations imply that the four-point conformal block admits a decomposition into a sum over pairs of Young diagrams of essentially rational Nekrasov functions - this is immediately seen when conformal block is represented in the form of a matrix model. However, the q-deformation of the same block has a deeper decomp... | 11.758513 | 11.756492 | 14.20958 | 11.929427 | 12.231173 | 12.144006 | 12.736158 | 11.815831 | 11.715108 | 13.859781 | 12.092843 | 10.921825 | 11.733208 | 11.274009 | 11.271004 | 10.631104 | 10.862554 | 10.836422 | 11.102137 | 12.284031 | 11.25585 |
hep-th/9205011 | null | M. Dine, R.G. Leigh and D.A. MacIntire | Of CP and other Gauge Symmetries in String Theory | 8 pages | Phys.Rev.Lett. 69 (1992) 2030-2032 | 10.1103/PhysRevLett.69.2030 | null | hep-th | null | We argue that \CP is a gauge symmetry in string theory. As a consequence, \CP
cannot be explicitly broken either perturbatively or non-pertubatively; there
can be no non-perturbative \CP-violating parameters. String theory is thus an
example of a theory where all $\theta$ angles arise due to spontaneous \CP
violation... | [
{
"created": "Thu, 7 May 1992 06:38:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dine",
"M.",
""
],
[
"Leigh",
"R. G.",
""
],
[
"MacIntire",
"D. A.",
""
]
] | We argue that \CP is a gauge symmetry in string theory. As a consequence, \CP cannot be explicitly broken either perturbatively or non-pertubatively; there can be no non-perturbative \CP-violating parameters. String theory is thus an example of a theory where all $\theta$ angles arise due to spontaneous \CP violation, ... | 9.342159 | 8.424805 | 7.72607 | 7.448293 | 7.042771 | 7.498556 | 7.151085 | 7.60675 | 6.930131 | 8.239683 | 7.287174 | 7.773683 | 8.159946 | 7.666946 | 7.417704 | 7.223672 | 7.101707 | 7.200017 | 7.434505 | 7.600826 | 6.945948 |
hep-th/0112238 | Peter Lee | Calin Ciocarlie, Peter Lee, Jongwon Park | A Note on Noncommutative D-Brane Actions | 11 pages, LaTeX (v2: references added, typos fixed) | Nucl.Phys.B632:303-310,2002 | 10.1016/S0550-3213(02)00236-5 | null | hep-th | null | We use the nonabelian action of N coincident D(-1) branes in constant
background fields, in the N $\to \infty$ limit, to construct noncommutative
D-brane actions in an arbitrary noncommutative description and comment on
tachyon condensation from this perspective.
| [
{
"created": "Thu, 27 Dec 2001 20:38:57 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Jan 2002 10:59:12 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Ciocarlie",
"Calin",
""
],
[
"Lee",
"Peter",
""
],
[
"Park",
"Jongwon",
""
]
] | We use the nonabelian action of N coincident D(-1) branes in constant background fields, in the N $\to \infty$ limit, to construct noncommutative D-brane actions in an arbitrary noncommutative description and comment on tachyon condensation from this perspective. | 13.614458 | 9.383493 | 13.567542 | 10.134993 | 10.687164 | 9.570364 | 10.052209 | 9.389592 | 9.512265 | 14.634895 | 8.936082 | 10.944466 | 12.57163 | 10.727586 | 11.411364 | 11.15976 | 10.815345 | 10.484794 | 10.868605 | 12.078652 | 10.833743 |
2011.10360 | Pengfei Zhang | Pengfei Zhang | More on Complex Sachdev-Ye-Kitaev Eternal Wormholes | 22 pages, 6 figures | null | null | null | hep-th cond-mat.str-el | http://creativecommons.org/licenses/by/4.0/ | In this work, we study a generalization of the coupled Sachdev-Ye-Kitaev
(SYK) model with $U(1)$ charge conservations. The model contains two copies of
the complex SYK model at different chemical potentials, coupled by a direct
hopping term. In the zero-temperature and small coupling limit with small
averaged chemica... | [
{
"created": "Fri, 20 Nov 2020 12:03:05 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Nov 2020 21:50:00 GMT",
"version": "v2"
}
] | 2020-11-30 | [
[
"Zhang",
"Pengfei",
""
]
] | In this work, we study a generalization of the coupled Sachdev-Ye-Kitaev (SYK) model with $U(1)$ charge conservations. The model contains two copies of the complex SYK model at different chemical potentials, coupled by a direct hopping term. In the zero-temperature and small coupling limit with small averaged chemical ... | 10.783757 | 8.940385 | 12.112164 | 9.397178 | 10.272221 | 9.563063 | 9.347055 | 9.258434 | 9.190895 | 11.440589 | 9.619823 | 9.257412 | 10.163722 | 9.643043 | 9.345186 | 9.357672 | 9.447092 | 9.712034 | 9.47418 | 10.098763 | 9.561196 |
2007.01224 | Roman Pasechnik | Torbj\"orn Lundberg and Roman Pasechnik | Thermal Field Theory in real-time formalism: concepts and applications
for particle decays | 87 pages, 11 figures | null | 10.1140/epja/s10050-020-00288-5 | null | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This review represents a detailed and comprehensive discussion of the Thermal
Field Theory (TFT) concepts and key results in Yukawa-type theories. We start
with a general pedagogical introduction into the TFT in the imaginary- and
real-time formulation. As phenomenologically relevant implications, we present
a compen... | [
{
"created": "Thu, 2 Jul 2020 16:16:59 GMT",
"version": "v1"
}
] | 2021-03-17 | [
[
"Lundberg",
"Torbjörn",
""
],
[
"Pasechnik",
"Roman",
""
]
] | This review represents a detailed and comprehensive discussion of the Thermal Field Theory (TFT) concepts and key results in Yukawa-type theories. We start with a general pedagogical introduction into the TFT in the imaginary- and real-time formulation. As phenomenologically relevant implications, we present a compendi... | 11.53688 | 12.841326 | 10.42809 | 10.62232 | 11.144327 | 12.006837 | 11.556125 | 11.130278 | 10.653079 | 12.654773 | 11.823444 | 11.106974 | 10.922667 | 10.551039 | 10.844533 | 10.615752 | 10.642405 | 11.090296 | 10.492356 | 10.850554 | 11.10282 |
hep-th/0604089 | Manuel Asorey | M. Asorey, D. Garcia-Alvarez, J. M. Munoz-Castaneda | Casimir Effect and Global Theory of Boundary Conditions | 11 pages | J.Phys.A39:6127-6136,2006 | 10.1088/0305-4470/39/21/S03 | null | hep-th | null | The consistency of quantum field theories defined on domains with external
borders imposes very restrictive constraints on the type of boundary conditions
that the fields can satisfy. We analyse the global geometrical and topological
properties of the space of all possible boundary conditions for scalar quantum
field... | [
{
"created": "Wed, 12 Apr 2006 12:08:34 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Asorey",
"M.",
""
],
[
"Garcia-Alvarez",
"D.",
""
],
[
"Munoz-Castaneda",
"J. M.",
""
]
] | The consistency of quantum field theories defined on domains with external borders imposes very restrictive constraints on the type of boundary conditions that the fields can satisfy. We analyse the global geometrical and topological properties of the space of all possible boundary conditions for scalar quantum field t... | 10.70319 | 9.897741 | 10.506481 | 10.122117 | 10.822234 | 10.492651 | 10.612013 | 10.891328 | 9.900311 | 10.944057 | 10.169863 | 9.862571 | 10.332508 | 9.787432 | 10.009558 | 10.150532 | 9.931756 | 9.876968 | 9.812603 | 10.08098 | 9.757824 |
hep-th/9605056 | Claus Wilke | C. Wilke and G. Wunner | Photon splitting in strong magnetic fields: asymptotic approximation
formulae vs. accurate numerical results | 8 pages, 2 figures, Revtex. Resubmitted to Phys. Rev. D., only minor
changes | Phys.Rev. D55 (1997) 997-1000 | 10.1103/PhysRevD.55.997 | null | hep-th | null | We present the results of a numerical calculation of the photon splitting
rate below the electron-pair creation threshold ($\omega \le 2m$) in magnetic
fields $B ~{> \atop \sim}~ B_{\rm cr} = m^2 /e = 4.414 \times 10^{9}$ T. Our
results confirm asymptotic approximations derived in the low-field ($B < B_{\rm
cr}$) and... | [
{
"created": "Wed, 8 May 1996 16:15:52 GMT",
"version": "v1"
},
{
"created": "Wed, 22 May 1996 10:42:38 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Aug 1996 18:07:34 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Wilke",
"C.",
""
],
[
"Wunner",
"G.",
""
]
] | We present the results of a numerical calculation of the photon splitting rate below the electron-pair creation threshold ($\omega \le 2m$) in magnetic fields $B ~{> \atop \sim}~ B_{\rm cr} = m^2 /e = 4.414 \times 10^{9}$ T. Our results confirm asymptotic approximations derived in the low-field ($B < B_{\rm cr}$) and h... | 6.440085 | 7.262803 | 6.599613 | 5.92543 | 6.388426 | 7.329338 | 7.124542 | 7.416167 | 6.256247 | 6.525551 | 6.412835 | 6.246321 | 6.166331 | 5.992595 | 5.980333 | 6.43986 | 6.30055 | 6.446526 | 6.116077 | 6.303082 | 6.182206 |
hep-th/0105082 | Alan Kostelecky | Sean M. Carroll, Jeffrey A. Harvey, V. Alan Kostelecky, Charles D.
Lane, and Takemi Okamoto | Noncommutative Field Theory and Lorentz Violation | 4 pages | Phys.Rev.Lett.87:141601,2001 | 10.1103/PhysRevLett.87.141601 | EFI 01-12, IUHET 433, May 2001 | hep-th hep-ph | null | The role of Lorentz symmetry in noncommutative field theory is considered.
Any realistic noncommutative theory is found to be physically equivalent to a
subset of a general Lorentz-violating standard-model extension involving
ordinary fields. Some theoretical consequences are discussed. Existing
experiments bound the... | [
{
"created": "Wed, 9 May 2001 10:37:57 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Carroll",
"Sean M.",
""
],
[
"Harvey",
"Jeffrey A.",
""
],
[
"Kostelecky",
"V. Alan",
""
],
[
"Lane",
"Charles D.",
""
],
[
"Okamoto",
"Takemi",
""
]
] | The role of Lorentz symmetry in noncommutative field theory is considered. Any realistic noncommutative theory is found to be physically equivalent to a subset of a general Lorentz-violating standard-model extension involving ordinary fields. Some theoretical consequences are discussed. Existing experiments bound the s... | 11.288315 | 10.388797 | 9.094204 | 9.125484 | 11.203708 | 11.269568 | 9.676301 | 9.858978 | 9.447778 | 9.963146 | 9.979006 | 10.315205 | 9.486754 | 9.343035 | 9.619947 | 9.349782 | 10.494462 | 9.654129 | 9.653141 | 10.237776 | 9.931945 |
hep-th/0212228 | Peter Ouyang | Peter Ouyang | Semiclassical Quantization of Giant Gravitons | 21 pages, 8 figures | null | null | PUPT-2071 | hep-th | null | We study excited spherical branes (``giant gravitons'') in $AdS \times S$
spacetimes with background flux. For large excitation, these branes may be
treated semiclassically. We compute their spectra using Bohr-Sommerfeld
quantization and use the AdS/CFT correspondence to relate them to anomalous
dimensions in the dua... | [
{
"created": "Thu, 19 Dec 2002 00:32:38 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ouyang",
"Peter",
""
]
] | We study excited spherical branes (``giant gravitons'') in $AdS \times S$ spacetimes with background flux. For large excitation, these branes may be treated semiclassically. We compute their spectra using Bohr-Sommerfeld quantization and use the AdS/CFT correspondence to relate them to anomalous dimensions in the dual ... | 8.562723 | 8.711629 | 9.317118 | 7.839982 | 8.510336 | 8.099839 | 7.924563 | 8.39588 | 7.244984 | 9.5672 | 7.78285 | 7.875425 | 8.202477 | 7.624052 | 7.906013 | 8.027143 | 7.646842 | 7.737528 | 7.778769 | 8.213332 | 7.845947 |
1307.5536 | Aram Saharian | A. A. Saharian, A. S. Kotanjyan, H. A. Nersisyan | Electromagnetic two-point functions and Casimir densities for a
conducting plate in de Sitter spacetime | 12 pages, 1 figure, typo in Eq.(19) corrected, reference and
paragraph added | Phys. Lett. B 728 (2014) 141 | 10.1016/j.physletb.2013.11.041 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We evaluate the two-point function for the electromagnetic field tensor in
$(D+1)$-dimensional de Sitter spacetime assuming that the field is prepared in
Bunch-Davies vacuum state. This two-point function is used for the
investigation of the vacuum expectation values (VEVs) of the field squared and
the energy-momentu... | [
{
"created": "Sun, 21 Jul 2013 15:42:02 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Dec 2013 21:40:42 GMT",
"version": "v2"
}
] | 2013-12-13 | [
[
"Saharian",
"A. A.",
""
],
[
"Kotanjyan",
"A. S.",
""
],
[
"Nersisyan",
"H. A.",
""
]
] | We evaluate the two-point function for the electromagnetic field tensor in $(D+1)$-dimensional de Sitter spacetime assuming that the field is prepared in Bunch-Davies vacuum state. This two-point function is used for the investigation of the vacuum expectation values (VEVs) of the field squared and the energy-momentum ... | 4.025551 | 3.267285 | 4.125906 | 3.351444 | 3.422183 | 3.113935 | 3.193399 | 3.112915 | 3.396254 | 4.107331 | 3.218754 | 3.543497 | 3.826974 | 3.689864 | 3.653845 | 3.550056 | 3.539408 | 3.64028 | 3.672174 | 3.866351 | 3.620789 |
hep-th/0411178 | Andrei Mikhailov | Andrei Mikhailov | Anomalous dimension and local charges | 10 pages, LaTeX; v2: added explanations, references | JHEP0512:009,2005 | 10.1088/1126-6708/2005/12/009 | CALT-68-2531; ITEP-TH-55/04 | hep-th | null | AdS space is the universal covering of a hyperboloid. We consider the action
of the deck transformations on a classical string worldsheet in $AdS_5\times
S^5$. We argue that these transformations are generated by an infinite linear
combination of the local conserved charges. We conjecture that a similar
relation hold... | [
{
"created": "Fri, 19 Nov 2004 08:30:59 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Sep 2005 02:46:44 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Mikhailov",
"Andrei",
""
]
] | AdS space is the universal covering of a hyperboloid. We consider the action of the deck transformations on a classical string worldsheet in $AdS_5\times S^5$. We argue that these transformations are generated by an infinite linear combination of the local conserved charges. We conjecture that a similar relation holds ... | 7.25985 | 6.746104 | 7.995533 | 6.369745 | 7.126663 | 7.491026 | 6.89854 | 7.045795 | 6.968812 | 8.736658 | 7.047837 | 6.454323 | 7.106319 | 6.741745 | 6.563058 | 6.521727 | 6.66971 | 6.284791 | 6.345529 | 7.082142 | 6.969 |
1802.06751 | Dan Xie | Si Li, Dan Xie, Shing-Tung Yau | Seiberg-Witten differential via primitive forms | 24 pages | Commun. Math. Phys. (2019) | 10.1007/s00220-019-03401-y | null | hep-th math-ph math.AG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Three-fold quasi-homogeneous isolated rational singularity is argued to
define a four dimensional $\mathcal{N}=2$ SCFT. The Seiberg-Witten geometry is
built on the mini-versal deformation of the singularity. We argue in this paper
that the corresponding Seiberg-Witten differential is given by the
Gelfand-Leray form o... | [
{
"created": "Mon, 19 Feb 2018 18:37:08 GMT",
"version": "v1"
}
] | 2020-04-10 | [
[
"Li",
"Si",
""
],
[
"Xie",
"Dan",
""
],
[
"Yau",
"Shing-Tung",
""
]
] | Three-fold quasi-homogeneous isolated rational singularity is argued to define a four dimensional $\mathcal{N}=2$ SCFT. The Seiberg-Witten geometry is built on the mini-versal deformation of the singularity. We argue in this paper that the corresponding Seiberg-Witten differential is given by the Gelfand-Leray form of ... | 8.766712 | 8.048034 | 13.436191 | 7.500977 | 8.231228 | 8.857991 | 7.957428 | 7.775967 | 8.34691 | 10.479666 | 7.574584 | 7.588604 | 9.652474 | 8.010592 | 7.849543 | 8.041822 | 7.816581 | 7.505334 | 8.058493 | 8.584717 | 7.881607 |
0910.4526 | Gautam Mandal | Gautam Mandal, Manavendra Mahato and Takeshi Morita | Phases of one dimensional large N gauge theory in a 1/D expansion | 27 pages + 21 pages of Appendix; 8 figures, v2:some comments are
added in sec.4.3, minor corrections, one reference added, v3: minor
corrections, one reference added, version to be published in JHEP | JHEP 1002:034,2010 | 10.1007/JHEP02(2010)034 | TIFR/TH/09-14 | hep-th cond-mat.stat-mech hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider large N Yang Mills theory with D adjoint scalar fields in d
dimensions for d=0 or 1. We show the existence of a non-trivial saddle point of
the functional integral at large D which is characterized by a mass gap for the
adjoint scalars. We integrate out the adjoint scalars in a 1/D expansion around
the sa... | [
{
"created": "Fri, 23 Oct 2009 19:36:32 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Nov 2009 12:56:34 GMT",
"version": "v2"
},
{
"created": "Wed, 3 Feb 2010 11:49:12 GMT",
"version": "v3"
}
] | 2010-03-19 | [
[
"Mandal",
"Gautam",
""
],
[
"Mahato",
"Manavendra",
""
],
[
"Morita",
"Takeshi",
""
]
] | We consider large N Yang Mills theory with D adjoint scalar fields in d dimensions for d=0 or 1. We show the existence of a non-trivial saddle point of the functional integral at large D which is characterized by a mass gap for the adjoint scalars. We integrate out the adjoint scalars in a 1/D expansion around the sadd... | 8.94936 | 8.817986 | 9.344851 | 8.684756 | 9.352076 | 9.772699 | 9.355698 | 8.885903 | 8.145005 | 10.086566 | 8.338274 | 8.592802 | 8.869087 | 8.441966 | 8.630579 | 8.632603 | 8.709932 | 8.631215 | 8.492412 | 8.945878 | 8.26515 |
0704.1637 | Antonio J. Segui | Pablo Diaz, M. A. Per, Antonio Segui | Fischler-Susskind holographic cosmology revisited | 17 pages, 4 figures. A new example developed in subsection 3.3 and
other minor changes | Class.Quant.Grav.24:5595-5608,2007 | 10.1088/0264-9381/24/22/019 | null | hep-th gr-qc | null | When Fischler and Susskind proposed a holographic prescription based on the
Particle Horizon, they found that spatially closed cosmological models do not
verify it due to the apparently unavoidable recontraction of the Particle
Horizon area. In this article, after a short review of their original work, we
expose grap... | [
{
"created": "Thu, 12 Apr 2007 18:29:35 GMT",
"version": "v1"
},
{
"created": "Thu, 31 May 2007 17:27:45 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Diaz",
"Pablo",
""
],
[
"Per",
"M. A.",
""
],
[
"Segui",
"Antonio",
""
]
] | When Fischler and Susskind proposed a holographic prescription based on the Particle Horizon, they found that spatially closed cosmological models do not verify it due to the apparently unavoidable recontraction of the Particle Horizon area. In this article, after a short review of their original work, we expose graphi... | 12.387021 | 11.566332 | 11.151958 | 10.996398 | 11.987175 | 11.373148 | 13.034678 | 11.356489 | 11.04357 | 10.882635 | 10.908261 | 11.001346 | 10.459721 | 10.346221 | 10.628757 | 10.261543 | 10.818126 | 10.260389 | 10.939434 | 10.340926 | 10.642623 |
2112.14712 | Sebasti\'an C\'espedes | Ana Achucarro, Sebastian Cespedes, Anne-Christine Davis, Gonzalo A.
Palma | The hand-made tail: Non-perturbative tails from multifield inflation | 32 pages + appendices, 4 figures | null | 10.1007/JHEP05(2022)052 | null | hep-th astro-ph.CO | http://creativecommons.org/licenses/by/4.0/ | It is becoming increasingly clear that large but rare fluctuations of the
primordial curvature field, controlled by the tail of its probability
distribution, could have dramatic effects on the current structure of the
universe -- {\it e.g.} via primordial black-holes. However, the use of standard
perturbation theory ... | [
{
"created": "Wed, 29 Dec 2021 18:21:03 GMT",
"version": "v1"
}
] | 2022-05-25 | [
[
"Achucarro",
"Ana",
""
],
[
"Cespedes",
"Sebastian",
""
],
[
"Davis",
"Anne-Christine",
""
],
[
"Palma",
"Gonzalo A.",
""
]
] | It is becoming increasingly clear that large but rare fluctuations of the primordial curvature field, controlled by the tail of its probability distribution, could have dramatic effects on the current structure of the universe -- {\it e.g.} via primordial black-holes. However, the use of standard perturbation theory to... | 8.713928 | 8.556189 | 8.942564 | 8.041372 | 8.753592 | 8.347986 | 8.112088 | 8.329387 | 8.317734 | 9.05254 | 8.425628 | 8.145149 | 8.190392 | 8.058957 | 8.12815 | 8.102936 | 8.070893 | 7.931952 | 8.282883 | 8.317603 | 8.293863 |
hep-th/9301070 | Kanehisa Takasaki | Kanehisa Takasaki and Takashi Takebe | Quasi-classical limit of Toda hierarchy and W-infinity symmetries | 14 pages, Kyoto University KUCP-0057/93 | Lett.Math.Phys. 28 (1993) 165-176 | 10.1007/BF00745148 | null | hep-th | null | Previous results on quasi-classical limit of the KP hierarchy and its
W-infinity symmetries are extended to the Toda hierarchy. The Planck constant
$\hbar$ now emerges as the spacing unit of difference operators in the Lax
formalism. Basic notions, such as dressing operators, Baker-Akhiezer functions
and tau function... | [
{
"created": "Mon, 18 Jan 1993 08:10:29 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Jan 1993 03:54:34 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Apr 1993 01:47:56 GMT",
"version": "v3"
},
{
"created": "Mon, 24 May 1993 03:05:49 GMT",
"version": "v4"
}
] | 2009-10-22 | [
[
"Takasaki",
"Kanehisa",
""
],
[
"Takebe",
"Takashi",
""
]
] | Previous results on quasi-classical limit of the KP hierarchy and its W-infinity symmetries are extended to the Toda hierarchy. The Planck constant $\hbar$ now emerges as the spacing unit of difference operators in the Lax formalism. Basic notions, such as dressing operators, Baker-Akhiezer functions and tau function, ... | 7.967707 | 7.391139 | 9.503101 | 7.616875 | 7.931841 | 8.443617 | 8.697073 | 8.155468 | 8.098253 | 8.84694 | 7.575497 | 7.30912 | 7.667573 | 7.295705 | 7.153973 | 7.380772 | 7.141998 | 7.212932 | 7.595809 | 7.935122 | 7.54876 |
hep-th/0309105 | Ahmed Jellal | Ahmed Jellal, El Hassan El Kinani, Michael Schreiber | Two Coupled Harmonic Oscillators on Non-commutative Plane | 15 pages, 1 figure | Int.J.Mod.Phys.A20:1515-1529,2005 | 10.1142/S0217751X05020835 | null | hep-th cond-mat.stat-mech math-ph math.MP | null | We investigate a system of two coupled harmonic oscillators on the
non-commutative plane \RR^2_{\theta} by requiring that the spatial coordinates
do not commute. We show that the system can be diagonalized by a suitable
transformation, i.e. a rotation with a mixing angle \alpha. The obtained
eigenstates as well as th... | [
{
"created": "Wed, 10 Sep 2003 15:49:25 GMT",
"version": "v1"
}
] | 2010-11-05 | [
[
"Jellal",
"Ahmed",
""
],
[
"Kinani",
"El Hassan El",
""
],
[
"Schreiber",
"Michael",
""
]
] | We investigate a system of two coupled harmonic oscillators on the non-commutative plane \RR^2_{\theta} by requiring that the spatial coordinates do not commute. We show that the system can be diagonalized by a suitable transformation, i.e. a rotation with a mixing angle \alpha. The obtained eigenstates as well as the ... | 7.029537 | 7.831289 | 7.206737 | 6.865937 | 7.2631 | 7.406343 | 7.378 | 6.690438 | 7.085554 | 7.43699 | 7.020679 | 6.896435 | 6.814264 | 6.719862 | 6.732594 | 6.931009 | 6.906861 | 6.799436 | 6.878389 | 6.928601 | 6.713022 |
0804.3801 | Paul M. Saffin | Paul M. Saffin, Antonio Padilla and Edmund J. Copeland | Decay of an inhomogeneous state via resonant tunnelling | 19 pages, 22 figures | JHEP 0809:055,2008 | 10.1088/1126-6708/2008/09/055 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We recently investigated the nature of resonant tunnelling in standard scalar
Quantum Field Theory, uncovering the conditions required for resonance. It was
shown that whereas the homogeneous false vacuum may decay via bubble
nucleation, it may not decay in a resonant fashion. The no-go theorem given
there is circumv... | [
{
"created": "Thu, 24 Apr 2008 09:21:12 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Saffin",
"Paul M.",
""
],
[
"Padilla",
"Antonio",
""
],
[
"Copeland",
"Edmund J.",
""
]
] | We recently investigated the nature of resonant tunnelling in standard scalar Quantum Field Theory, uncovering the conditions required for resonance. It was shown that whereas the homogeneous false vacuum may decay via bubble nucleation, it may not decay in a resonant fashion. The no-go theorem given there is circumven... | 17.460855 | 16.558914 | 17.476614 | 15.261801 | 16.415331 | 16.470268 | 17.008352 | 16.024216 | 16.968731 | 16.684757 | 16.304945 | 15.735206 | 17.071941 | 15.684031 | 16.43096 | 16.188152 | 16.282564 | 15.639269 | 16.048468 | 16.351454 | 15.601749 |
hep-th/0611134 | Yongsung Yoon | Hyun Kyu Lee and Yongsung Yoon | Effective Potential for Uniform Magnetic Fields through Pauli
Interaction | 9 pages with 1 figure | JHEP 0703:086,2007 | 10.1088/1126-6708/2007/03/086 | null | hep-th astro-ph | null | We have calculated the explicit form of the real and imaginary parts of the
effective potential for uniform magnetic fields which interact with spin-1/2
fermions through the Pauli interaction. It is found that the non-vanishing
imaginary part develops for a magnetic field stronger than a critical field,
whose strengt... | [
{
"created": "Mon, 13 Nov 2006 10:28:44 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Nov 2006 04:56:12 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Nov 2006 06:22:23 GMT",
"version": "v3"
},
{
"created": "Sun, 14 Jan 2007 17:44:15 GMT",
"version": "v4"
}
] | 2010-10-27 | [
[
"Lee",
"Hyun Kyu",
""
],
[
"Yoon",
"Yongsung",
""
]
] | We have calculated the explicit form of the real and imaginary parts of the effective potential for uniform magnetic fields which interact with spin-1/2 fermions through the Pauli interaction. It is found that the non-vanishing imaginary part develops for a magnetic field stronger than a critical field, whose strength ... | 6.724798 | 7.500735 | 6.984456 | 6.41833 | 6.769071 | 7.411227 | 6.84553 | 6.360885 | 6.236328 | 6.636794 | 6.199963 | 6.531087 | 6.569258 | 6.532537 | 6.71537 | 6.41807 | 6.590686 | 6.504216 | 6.357031 | 6.324975 | 6.47226 |
hep-th/0402186 | M. Tierz | E. Elizalde, M. Tierz | Multiplicative anomaly and zeta factorization | 20 pages, AIP style | J.Math.Phys.45:1168-1179,2004 | 10.1063/1.1646447 | null | hep-th | null | Some aspects of the multiplicative anomaly of zeta determinants are
investigated. A rather simple approach is adopted and, in particular, the
question of zeta function factorization, together with its possible relation
with the multiplicative anomaly issue is discussed. We look primordially into
the zeta functions in... | [
{
"created": "Mon, 23 Feb 2004 21:26:02 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Elizalde",
"E.",
""
],
[
"Tierz",
"M.",
""
]
] | Some aspects of the multiplicative anomaly of zeta determinants are investigated. A rather simple approach is adopted and, in particular, the question of zeta function factorization, together with its possible relation with the multiplicative anomaly issue is discussed. We look primordially into the zeta functions inst... | 14.52435 | 15.322695 | 15.771514 | 13.475965 | 15.326982 | 13.728297 | 15.117766 | 14.158975 | 15.883051 | 17.969711 | 14.894956 | 13.949044 | 14.499467 | 13.77088 | 13.974255 | 13.646524 | 13.974667 | 13.657311 | 13.793806 | 14.795739 | 13.474298 |
2103.08653 | Jens Hoppe | Jens Hoppe | Commuting signs of infinity | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Discrete minimal surface algebras and Yang Mills algebras may be related to
(generalized) Kac Moody algebras, just as Membrane (matrix) models and the IKKT
model - including a novel construction technique for minimal surfaces.
| [
{
"created": "Wed, 10 Mar 2021 21:17:27 GMT",
"version": "v1"
},
{
"created": "Sun, 21 Mar 2021 18:17:37 GMT",
"version": "v2"
}
] | 2021-03-23 | [
[
"Hoppe",
"Jens",
""
]
] | Discrete minimal surface algebras and Yang Mills algebras may be related to (generalized) Kac Moody algebras, just as Membrane (matrix) models and the IKKT model - including a novel construction technique for minimal surfaces. | 33.984303 | 25.210358 | 37.399017 | 26.098173 | 26.857841 | 31.116972 | 28.842218 | 26.624903 | 25.96623 | 41.257668 | 23.487726 | 24.65943 | 24.959068 | 24.966818 | 25.063292 | 24.727642 | 26.014372 | 25.359226 | 27.614836 | 27.363684 | 21.991558 |
hep-th/9610015 | Amir Aghamohamadi | A. Aghamohammadi, M. Khorrami, A. Shariati | Toda theories as contraction of affine Toda theories | 6 pages, LaTeX , to appear in Phys. Lett. B | Phys.Lett. B389 (1996) 260-263 | 10.1016/S0370-2693(96)01268-3 | null | hep-th | null | Using a contraction procedure, we obtain Toda theories and their structures,
from affine Toda theories and their corresponding structures. By structures, we
mean the equation of motion, the classical Lax pair, the boundary term for half
line theories, and the quantum transfer matrix. The Lax pair and the transfer
mat... | [
{
"created": "Wed, 2 Oct 1996 19:37:39 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Aghamohammadi",
"A.",
""
],
[
"Khorrami",
"M.",
""
],
[
"Shariati",
"A.",
""
]
] | Using a contraction procedure, we obtain Toda theories and their structures, from affine Toda theories and their corresponding structures. By structures, we mean the equation of motion, the classical Lax pair, the boundary term for half line theories, and the quantum transfer matrix. The Lax pair and the transfer matri... | 14.356204 | 12.122032 | 15.899991 | 10.382575 | 13.156447 | 13.380522 | 11.444337 | 11.242498 | 11.754889 | 15.009012 | 12.645755 | 11.321588 | 13.378104 | 11.000772 | 11.145821 | 11.206112 | 12.071896 | 11.419441 | 11.187374 | 12.658298 | 11.763535 |
2403.18013 | Yiwen Zhang | Sang-Eon Bak, Cynthia Keeler, Yiwen Zhang, and Kathryn M. Zurek | Rindler Fluids from Gravitational Shockwaves | 21 pages, 1 figure | JHEP 05 (2024) 331 | 10.1007/JHEP05(2024)331 | CALT-TH 2024-016 | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We study a correspondence between gravitational shockwave geometry and its
fluid description near a Rindler horizon in Minkowski spacetime. Utilizing the
Petrov classification that describes algebraic symmetries for Lorentzian
spaces, we establish an explicit mapping between a potential fluid and the
shockwave metric... | [
{
"created": "Tue, 26 Mar 2024 18:01:58 GMT",
"version": "v1"
}
] | 2024-07-29 | [
[
"Bak",
"Sang-Eon",
""
],
[
"Keeler",
"Cynthia",
""
],
[
"Zhang",
"Yiwen",
""
],
[
"Zurek",
"Kathryn M.",
""
]
] | We study a correspondence between gravitational shockwave geometry and its fluid description near a Rindler horizon in Minkowski spacetime. Utilizing the Petrov classification that describes algebraic symmetries for Lorentzian spaces, we establish an explicit mapping between a potential fluid and the shockwave metric p... | 12.376078 | 12.331414 | 12.274765 | 11.045331 | 11.439391 | 11.910903 | 12.059505 | 11.654641 | 12.10218 | 12.002178 | 11.927414 | 12.44662 | 12.091227 | 12.00796 | 12.456301 | 12.255567 | 12.087145 | 12.324175 | 12.379877 | 12.074765 | 12.203841 |
hep-th/0411269 | Cristiano Germani | Cristiano Germani (DAMTP, University of Cambridge), Alex Kehagias
(National Technical University of Athens) | Higher-Spin Fields in Braneworlds | 26 pages, 2 figures, Revtex style. v2 references added and a sign in
the bosonic action corrected; v3 section 3 expanded, \Delta S_2 in section 5
generalized and therefore eq. 5.18 corrected, clarifications and references
added. Version accepted for publication in Nuclear Physics B | Nucl.Phys. B725 (2005) 15-44 | 10.1016/j.nuclphysb.2005.07.027 | DAMTP-2004-140 | hep-th gr-qc hep-ph | null | The dynamics of higher-spin fields in braneworlds is discussed. In
particular, we study fermionic and bosonic higher-spin fields in AdS_5 and
their localization on branes. We find that four-dimensional zero modes exist
only for spin-one fields, if there are no couplings to the boundaries. If
boundary couplings are al... | [
{
"created": "Tue, 30 Nov 2004 17:56:45 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Dec 2004 23:55:57 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Jul 2005 15:47:39 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Germani",
"Cristiano",
"",
"DAMTP, University of Cambridge"
],
[
"Kehagias",
"Alex",
"",
"National Technical University of Athens"
]
] | The dynamics of higher-spin fields in braneworlds is discussed. In particular, we study fermionic and bosonic higher-spin fields in AdS_5 and their localization on branes. We find that four-dimensional zero modes exist only for spin-one fields, if there are no couplings to the boundaries. If boundary couplings are allo... | 7.731141 | 7.854882 | 7.580788 | 7.569314 | 7.387308 | 7.775284 | 7.98479 | 7.869192 | 7.233547 | 8.100755 | 7.438302 | 7.450972 | 7.603142 | 7.40305 | 7.269253 | 7.411636 | 7.380199 | 7.363599 | 7.352957 | 7.703266 | 7.459158 |
2302.10153 | Mikhail Pavlov | Mikhail Pavlov | Global torus blocks in the necklace channel | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We continue studying of global conformal blocks on the torus in a special
(necklace) channel. Functions of such multi-point blocks are explicitly found
under special conditions on the blocks' conformal dimensions. We have verified
that these blocks satisfy the Casimir equations, which were derived in previous
studies... | [
{
"created": "Mon, 20 Feb 2023 18:37:45 GMT",
"version": "v1"
}
] | 2023-02-21 | [
[
"Pavlov",
"Mikhail",
""
]
] | We continue studying of global conformal blocks on the torus in a special (necklace) channel. Functions of such multi-point blocks are explicitly found under special conditions on the blocks' conformal dimensions. We have verified that these blocks satisfy the Casimir equations, which were derived in previous studies. | 25.427786 | 20.017071 | 25.482801 | 18.663124 | 20.359419 | 18.076242 | 18.247576 | 18.529472 | 19.605597 | 32.497776 | 18.292162 | 20.828537 | 23.242123 | 19.470211 | 20.348616 | 19.52973 | 20.970098 | 19.510523 | 20.174999 | 23.83024 | 19.284515 |
hep-th/0403066 | Stefano Ansoldi | Stefano Ansoldi | Boundary versus Bulk Dynamics of Extended Objects and the Fractal
Structure of Quantum Spacetime | 2+26+239 pages; 2 figures | null | null | PhD Thesis; Univeristy of Trieste; 2000 | hep-th | null | Subject of this thesis is the study of a closed bosonic string: the treatment
will follow an approach alternative with respect to the traditional one and
stems from a research line pursued in by Eguchi. A description of the dynamics
using Nonstandard Analysis is given in chapter 10 with prerequisites in
appendices B ... | [
{
"created": "Fri, 5 Mar 2004 10:26:42 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ansoldi",
"Stefano",
""
]
] | Subject of this thesis is the study of a closed bosonic string: the treatment will follow an approach alternative with respect to the traditional one and stems from a research line pursued in by Eguchi. A description of the dynamics using Nonstandard Analysis is given in chapter 10 with prerequisites in appendices B an... | 24.714834 | 26.915066 | 25.281242 | 23.152864 | 27.511734 | 25.92016 | 26.575451 | 22.507137 | 25.36462 | 28.962521 | 23.446411 | 22.033854 | 22.46147 | 22.316198 | 22.9541 | 22.771793 | 22.688244 | 22.643845 | 22.345922 | 23.026787 | 22.824011 |
1311.0186 | Lee Smolin | Lee Smolin | Twistor relative locality | LaTex 10 pages, no figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a version of relative locality based on the geometry of twistor
space. This can also be thought of as a new kind of deformation of twistor
theory based on the construction of a bundle of twistor spaces over momentum
space. Locality in space-time is emergent and is deformed in a precise way when
a connectio... | [
{
"created": "Fri, 1 Nov 2013 13:56:17 GMT",
"version": "v1"
}
] | 2013-11-04 | [
[
"Smolin",
"Lee",
""
]
] | We present a version of relative locality based on the geometry of twistor space. This can also be thought of as a new kind of deformation of twistor theory based on the construction of a bundle of twistor spaces over momentum space. Locality in space-time is emergent and is deformed in a precise way when a connection ... | 11.098834 | 10.461043 | 11.573306 | 10.267776 | 12.155581 | 9.845349 | 10.350855 | 11.617422 | 11.098707 | 12.672883 | 10.529111 | 10.381585 | 10.171952 | 10.156247 | 9.880966 | 10.627886 | 11.046503 | 10.433395 | 10.536067 | 10.958655 | 11.07669 |
1112.5075 | Troels Harmark | Agnese Bissi, Troels Harmark and Marta Orselli | Holographic 3-point function at one loop | 24 pages, 2 figures. v2: Typos fixed, Ref. added, figure improved.
v3: Several typos and misprints fixed, Ref. updated, figures improved, new
section 2.3 added on correction from spin-flipped coherent state,
computations on string theory side improved | null | 10.1007/JHEP02(2012)133 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the recent weak/strong coupling match of three-point functions in
the AdS/CFT correspondence for two semi-classical operators and one light
chiral primary operator found by Escobedo et al. This match is between the
tree-level three-point function with the two semi-classical operators described
by coherent ... | [
{
"created": "Wed, 21 Dec 2011 16:11:18 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jan 2012 15:16:29 GMT",
"version": "v2"
},
{
"created": "Fri, 24 Feb 2012 15:04:14 GMT",
"version": "v3"
}
] | 2015-06-03 | [
[
"Bissi",
"Agnese",
""
],
[
"Harmark",
"Troels",
""
],
[
"Orselli",
"Marta",
""
]
] | We explore the recent weak/strong coupling match of three-point functions in the AdS/CFT correspondence for two semi-classical operators and one light chiral primary operator found by Escobedo et al. This match is between the tree-level three-point function with the two semi-classical operators described by coherent st... | 7.121409 | 7.024293 | 7.434385 | 6.725931 | 6.583567 | 6.793145 | 6.532841 | 6.632184 | 6.486178 | 9.281105 | 6.561033 | 6.562231 | 7.497455 | 6.639978 | 6.660402 | 6.711679 | 6.902719 | 6.651299 | 6.999023 | 7.398611 | 6.56818 |
hep-th/0702137 | Edward Frenkel | E. Frenkel, A. Losev, and N. Nekrasov | Notes on instantons in topological field theory and beyond | 20 pages | Nucl.Phys.Proc.Suppl.171:215-230,2007 | 10.1016/j.nuclphysbps.2007.06.013 | null | hep-th math.QA | null | This is a brief summary of our studies of quantum field theories in a special
limit in which the instantons are present, the anti-instantons are absent, and
the perturbative corrections are reduced to one-loop. We analyze the
corresponding models as full-fledged quantum field theories, beyond their
topological sector... | [
{
"created": "Mon, 19 Feb 2007 20:37:50 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Frenkel",
"E.",
""
],
[
"Losev",
"A.",
""
],
[
"Nekrasov",
"N.",
""
]
] | This is a brief summary of our studies of quantum field theories in a special limit in which the instantons are present, the anti-instantons are absent, and the perturbative corrections are reduced to one-loop. We analyze the corresponding models as full-fledged quantum field theories, beyond their topological sector. ... | 8.634451 | 6.288325 | 10.249452 | 7.333705 | 7.196462 | 6.586715 | 6.654571 | 6.739285 | 7.053435 | 10.441759 | 7.371912 | 7.707969 | 8.793302 | 7.816376 | 7.940812 | 7.795874 | 7.803091 | 7.803 | 7.773802 | 8.978641 | 7.96123 |
hep-th/9903266 | Gudrun Pinter | K. Bresser, G. Pinter and D. Prange | Lorentz Invariant Renormalization in Causal Perturbation Theory | 9 pages, no figures | null | null | null | hep-th | null | In the framework of causal perturbation theory renormalization consists of
the extension of distributions. We give the explicit form of a Lorentz
invariant extension of a scalar distribution, depending on one difference of
space time coordinates.
| [
{
"created": "Wed, 31 Mar 1999 16:17:28 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Apr 1999 14:51:32 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Bresser",
"K.",
""
],
[
"Pinter",
"G.",
""
],
[
"Prange",
"D.",
""
]
] | In the framework of causal perturbation theory renormalization consists of the extension of distributions. We give the explicit form of a Lorentz invariant extension of a scalar distribution, depending on one difference of space time coordinates. | 14.476083 | 9.896958 | 11.456917 | 11.433608 | 10.740579 | 10.748853 | 10.474273 | 9.870124 | 10.821443 | 12.306682 | 9.965791 | 10.790051 | 11.764491 | 11.981878 | 11.566236 | 11.021164 | 11.40616 | 11.635168 | 11.597825 | 12.025884 | 11.056846 |
hep-th/9309156 | Francesco Belgiorno | F. Belgiorno and A.S. Cattaneo | Black Holes and Cosmological Constant in Bosonic String Theory: Some
Remarks | 17 pages; PHYZZX; IFUM 450/FT | Int.J.Mod.Phys.A10:527-540,1995 | 10.1142/S0217751X95000231 | null | hep-th | null | (some corrections in the semiclassical study and one reference added).
| [
{
"created": "Wed, 29 Sep 1993 17:35:02 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Nov 1993 16:01:43 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Belgiorno",
"F.",
""
],
[
"Cattaneo",
"A. S.",
""
]
] | (some corrections in the semiclassical study and one reference added). | 188.585419 | 80.291862 | 141.710037 | 126.393288 | 110.043457 | 82.099731 | 131.343643 | 81.165337 | 125.456276 | 159.866089 | 105.15567 | 101.891884 | 143.750687 | 136.758835 | 126.757057 | 112.130692 | 147.954437 | 139.501785 | 104.525711 | 160.055786 | 96.319092 |
hep-th/0205321 | Giancarlo Rossi | Massimo Bianchi, Burkhard Eden, Giancarlo Rossi and Yassen S. Stanev | On Operator Mixing in N=4 SYM | 32 pages, 2 figures | Nucl.Phys. B646 (2002) 69-101 | 10.1016/S0550-3213(02)00817-9 | ROM2F/2002/15 | hep-th | null | We resolve the mixing of the scalar operators of naive dimension 4 belonging
to the representation 20' of the SU(4) R-symmetry in N=4 SYM. We compute the
order g^2 corrections to their anomalous dimensions and show the absence of
instantonic contributions thereof. Ratios of the resulting expressions are
irrational nu... | [
{
"created": "Fri, 31 May 2002 15:46:06 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Bianchi",
"Massimo",
""
],
[
"Eden",
"Burkhard",
""
],
[
"Rossi",
"Giancarlo",
""
],
[
"Stanev",
"Yassen S.",
""
]
] | We resolve the mixing of the scalar operators of naive dimension 4 belonging to the representation 20' of the SU(4) R-symmetry in N=4 SYM. We compute the order g^2 corrections to their anomalous dimensions and show the absence of instantonic contributions thereof. Ratios of the resulting expressions are irrational numb... | 9.341018 | 8.300032 | 10.041665 | 8.07124 | 7.67377 | 8.235544 | 8.130951 | 7.689029 | 8.429724 | 9.487269 | 7.92518 | 8.222445 | 9.201687 | 8.673256 | 8.290208 | 8.45575 | 8.301872 | 8.333998 | 8.342832 | 9.259044 | 8.190728 |
1012.3983 | Joseph A. Minahan | Joseph A. Minahan | Review of AdS/CFT Integrability, Chapter I.1: Spin Chains in N=4 Super
Yang-Mills | 25 pages, see also overview article arXiv:1012.3982; v2: references
to other chapters updated; v3: references added, typos fixed | null | 10.1007/s11005-011-0522-9 | UUITP-38/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this chapter of "Review of AdS/CFT Integrability" we introduce N=4 Super
Yang-Mills. We discuss the global superalagebra PSU(2,2|4) and its action on
gauge invariant operators. We then discuss the computation of the correlators
of certain gauge invariant operators, the so-called single trace operators in
the large... | [
{
"created": "Fri, 17 Dec 2010 20:58:02 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Dec 2010 19:03:00 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Jul 2011 14:22:02 GMT",
"version": "v3"
}
] | 2015-05-20 | [
[
"Minahan",
"Joseph A.",
""
]
] | In this chapter of "Review of AdS/CFT Integrability" we introduce N=4 Super Yang-Mills. We discuss the global superalagebra PSU(2,2|4) and its action on gauge invariant operators. We then discuss the computation of the correlators of certain gauge invariant operators, the so-called single trace operators in the large N... | 6.54041 | 6.238186 | 8.342261 | 6.252664 | 7.158038 | 6.531666 | 6.673058 | 6.843503 | 6.580234 | 7.343603 | 6.508208 | 6.591484 | 6.620395 | 6.575442 | 7.078835 | 6.557147 | 6.434925 | 6.537819 | 6.695582 | 6.691267 | 6.487791 |
hep-th/0108006 | Daniel Kabat | Norihiro Iizuka, Daniel Kabat, Gilad Lifschytz, David A. Lowe | Probing black holes in non-perturbative gauge theory | 30 pages, LaTeX, 8 eps figures. v2: references added. v3: more
references | Phys.Rev.D65:024012,2002 | 10.1103/PhysRevD.65.024012 | BROWN-HET-1276, CU-TP-1025 | hep-th | null | We use a 0-brane to probe a ten-dimensional near-extremal black hole with N
units of 0-brane charge. We work directly in the dual strongly-coupled quantum
mechanics, using mean-field methods to describe the black hole background
non-perturbatively. We obtain the distribution of W boson masses, and find a
clear separa... | [
{
"created": "Wed, 1 Aug 2001 21:37:09 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Aug 2001 19:56:46 GMT",
"version": "v2"
},
{
"created": "Wed, 3 Oct 2001 23:54:23 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Iizuka",
"Norihiro",
""
],
[
"Kabat",
"Daniel",
""
],
[
"Lifschytz",
"Gilad",
""
],
[
"Lowe",
"David A.",
""
]
] | We use a 0-brane to probe a ten-dimensional near-extremal black hole with N units of 0-brane charge. We work directly in the dual strongly-coupled quantum mechanics, using mean-field methods to describe the black hole background non-perturbatively. We obtain the distribution of W boson masses, and find a clear separati... | 11.195436 | 11.152724 | 13.194771 | 10.369596 | 10.854012 | 10.736819 | 11.093786 | 11.014417 | 11.113332 | 13.962407 | 10.614067 | 10.544156 | 11.891914 | 10.938252 | 10.396627 | 10.366416 | 10.42135 | 10.706593 | 10.731894 | 11.3901 | 10.305819 |
1609.00513 | Kiyoharu Kawana | Kiyoharu Kawana | Possible explanations for fine-tuning of the universe | 15 pages, 5 figures | null | 10.1142/S0217751X17500488 | KUNS-2640 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Froggatt-Nielsen mechanism and the multi-local field theory are
interesting and promising candidates for solving the naturalness problem in the
universe. These theories are based on the different physical principles: The
former assumes the micro-canonical partition function $\int {\cal{D}}\phi\
\prod_i \delta (S_... | [
{
"created": "Fri, 2 Sep 2016 09:20:47 GMT",
"version": "v1"
}
] | 2017-04-19 | [
[
"Kawana",
"Kiyoharu",
""
]
] | The Froggatt-Nielsen mechanism and the multi-local field theory are interesting and promising candidates for solving the naturalness problem in the universe. These theories are based on the different physical principles: The former assumes the micro-canonical partition function $\int {\cal{D}}\phi\ \prod_i \delta (S_i^... | 6.735912 | 7.024238 | 6.89442 | 6.409259 | 6.900023 | 6.892857 | 6.536258 | 6.552682 | 6.099295 | 6.75862 | 6.493708 | 6.096195 | 6.250056 | 6.245951 | 6.282238 | 6.303139 | 6.210781 | 6.156693 | 6.14714 | 6.217153 | 6.346581 |
hep-th/9310130 | null | G. Delfino and G. Mussardo | Two-point Correlation Function in Integrable QFT with Anti-Crossing
Symmetry | 9 pages, LATEX file, ISAS/EP/93/167 (The paper contains two figures:
extract them separately with the name fig1.ps and fig2.ps and then LATEX
twice the paper) | Phys.Lett. B324 (1994) 40-44 | 10.1016/0370-2693(94)00109-X | null | hep-th | null | The two-point correlation function of the stress-energy tensor for the
$\Phi_{1,3}$ massive deformation of the non-unitary model ${\cal M}_{3,5}$ is
computed. We compare the ultraviolet CFT perturbative expansion of this
correlation function with its spectral representation given by a summation over
matrix elements o... | [
{
"created": "Wed, 20 Oct 1993 15:55:48 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Delfino",
"G.",
""
],
[
"Mussardo",
"G.",
""
]
] | The two-point correlation function of the stress-energy tensor for the $\Phi_{1,3}$ massive deformation of the non-unitary model ${\cal M}_{3,5}$ is computed. We compare the ultraviolet CFT perturbative expansion of this correlation function with its spectral representation given by a summation over matrix elements of ... | 12.751781 | 11.437225 | 12.40492 | 10.566856 | 12.036746 | 11.267059 | 10.100974 | 10.299609 | 11.186065 | 15.025833 | 10.279016 | 10.732914 | 13.086137 | 11.21386 | 11.467753 | 11.100602 | 11.349576 | 10.541574 | 11.458441 | 12.630753 | 10.879521 |
hep-th/0007144 | Alex Kaganovich | A.B. Kaganovich | Field theory model giving rise to "quintessential inflation" without the
cosmological constant and other fine tuning problems | REVTeX, shorter version (23 pages instead of 33), more convenient for
reading | Phys.Rev. D63 (2001) 025022 | 10.1103/PhysRevD.63.025022 | null | hep-th astro-ph gr-qc | null | A field theory is developed based on the idea that the effective action of
yet unknown fundamental theory, at energy scale below M_{p} has the form of
expansion in two measures: S=\intd^{4}x[\Phi L_{1}+\sqrt{-g}L_{2}] where the
new measure \Phi is defined using the third-rank antisymmetric tensor. In the
new variable... | [
{
"created": "Tue, 18 Jul 2000 12:11:18 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jul 2000 17:00:08 GMT",
"version": "v2"
},
{
"created": "Fri, 29 Dec 2000 12:31:09 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Kaganovich",
"A. B.",
""
]
] | A field theory is developed based on the idea that the effective action of yet unknown fundamental theory, at energy scale below M_{p} has the form of expansion in two measures: S=\intd^{4}x[\Phi L_{1}+\sqrt{-g}L_{2}] where the new measure \Phi is defined using the third-rank antisymmetric tensor. In the new variables ... | 13.131694 | 14.399458 | 14.329761 | 13.182631 | 14.254624 | 14.436436 | 15.203699 | 13.829219 | 13.813889 | 14.363374 | 13.786231 | 13.264431 | 13.101347 | 12.848242 | 12.84192 | 13.15776 | 13.227378 | 12.878214 | 13.148841 | 13.231665 | 13.06126 |
hep-th/0010078 | Andrei Mironov | A.Mironov | Seiberg-Witten Theories, Integrable Models and Perturbative
Prepotentials | LaTeX, 9 pages | null | null | null | hep-th | null | This is a very brief review of relations between Seiberg-Witten theories and
integrable systems with emphasis on the perturbative prepotentials presented at
the E.S.Fradkin Memorial Conference.
| [
{
"created": "Wed, 11 Oct 2000 11:27:25 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Mironov",
"A.",
""
]
] | This is a very brief review of relations between Seiberg-Witten theories and integrable systems with emphasis on the perturbative prepotentials presented at the E.S.Fradkin Memorial Conference. | 24.619486 | 10.980317 | 19.733833 | 12.073885 | 10.030888 | 8.668731 | 10.754818 | 10.746703 | 12.085459 | 20.461092 | 13.087573 | 13.962295 | 18.491575 | 14.957596 | 14.617438 | 14.328916 | 13.768174 | 14.731986 | 13.972765 | 16.136929 | 15.786935 |
2202.10483 | Damiano Anselmi | Damiano Anselmi | Purely virtual particles versus Lee-Wick ghosts: physical Pauli-Villars
fields, finite QED and quantum gravity | 32 pages; v2: PRD | Phys. Rev. D 105 125017 (2022) | 10.1103/PhysRevD.105.125017 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reconsider the Lee-Wick (LW) models and compare their properties to the
properties of the models that contain purely virtual particles. We argue
against the LW premise that unstable particles can be removed from the sets of
incoming and outgoing states in scattering processes. The removal leads to a
non-Hermitian ... | [
{
"created": "Mon, 21 Feb 2022 19:00:09 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jun 2022 14:41:58 GMT",
"version": "v2"
}
] | 2022-06-24 | [
[
"Anselmi",
"Damiano",
""
]
] | We reconsider the Lee-Wick (LW) models and compare their properties to the properties of the models that contain purely virtual particles. We argue against the LW premise that unstable particles can be removed from the sets of incoming and outgoing states in scattering processes. The removal leads to a non-Hermitian cl... | 11.093287 | 12.901293 | 12.739417 | 11.648394 | 11.148193 | 11.949541 | 12.012589 | 11.759601 | 11.365403 | 12.867189 | 10.939345 | 11.400437 | 11.263812 | 11.144814 | 11.129721 | 11.17938 | 11.196949 | 11.133439 | 11.063976 | 11.320462 | 10.85568 |
hep-th/0505167 | Eric Gimon | Per Berglund, Eric G. Gimon, and Thomas S. Levi | Supergravity Microstates for BPS Black Holes and Black Rings | 25 pages, 1 figure. Fixed minor typos, references added, extra
comment on gauge choice | JHEP0606:007,2006 | 10.1088/1126-6708/2006/06/007 | UNH-05-03, UCB-PTH-05/16, UPR-1119-T, NSF-KITP-05-29 | hep-th | null | We demonstrate a solution generating technique, modulo some constraints, for
a large class of smooth supergravity solutions with the same asymptotic charges
as a five dimensional 3-charge BPS black hole or black ring, dual to a D1/D5/P
system. These solutions are characterized by a harmonic function with both
positiv... | [
{
"created": "Wed, 18 May 2005 18:25:04 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Nov 2005 15:00:49 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Berglund",
"Per",
""
],
[
"Gimon",
"Eric G.",
""
],
[
"Levi",
"Thomas S.",
""
]
] | We demonstrate a solution generating technique, modulo some constraints, for a large class of smooth supergravity solutions with the same asymptotic charges as a five dimensional 3-charge BPS black hole or black ring, dual to a D1/D5/P system. These solutions are characterized by a harmonic function with both positive ... | 17.146561 | 13.493227 | 16.594599 | 13.852394 | 14.276151 | 15.859616 | 12.715439 | 12.75 | 14.14449 | 16.96376 | 13.884155 | 13.362431 | 15.785117 | 13.12877 | 13.717552 | 14.299059 | 13.664352 | 13.898841 | 13.913389 | 14.803562 | 13.964934 |
hep-th/9705240 | Alexander Lewis | Ian I. Kogan and Alex Lewis | Origin of Logarithmic Operators in Conformal Field Theories | 22 pages Latex. Some references added | Nucl.Phys. B509 (1998) 687-704 | 10.1016/S0550-3213(97)00666-4 | OU-TP-97-25P | hep-th | null | We study logarithmic operators in Coulomb gas models, and show that they
occur when the ``puncture'' operator of the Liouville theory is included in the
model. We also consider WZNW models for $SL(2,R)$, and for SU(2) at level 0, in
which we find logarithmic operators which form Jordan blocks for the current as
well ... | [
{
"created": "Fri, 30 May 1997 14:43:38 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Jun 1997 17:28:50 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Kogan",
"Ian I.",
""
],
[
"Lewis",
"Alex",
""
]
] | We study logarithmic operators in Coulomb gas models, and show that they occur when the ``puncture'' operator of the Liouville theory is included in the model. We also consider WZNW models for $SL(2,R)$, and for SU(2) at level 0, in which we find logarithmic operators which form Jordan blocks for the current as well as... | 10.198028 | 8.559159 | 11.108976 | 8.04458 | 7.531705 | 8.541039 | 7.854459 | 8.404988 | 8.623607 | 11.010945 | 8.796489 | 8.680519 | 10.3117 | 9.042039 | 8.763927 | 8.41497 | 8.735322 | 8.458813 | 9.085148 | 10.267213 | 8.625425 |
hep-th/9312153 | Wojtek Zakrzewski | J. Lukierski, H. Ruegg and W.J. Zakrzewski | Classical and Quantum Mechanics of Free \k Relativistic Systems | 27 pages, DTP-57/93 | Ann.Phys.243:90-116,1995 | 10.1006/aphy.1995.1092 | null | hep-th | null | We consider the Hamiltonian and Lagrangian formalism describing free
\k-relativistic particles with their four-momenta constrained to the
\k-deformed mass shell. We study the modifications of the formalism which
follow from the introduction of space coordinates with nonvanishing Poisson
brackets and from the redefini... | [
{
"created": "Fri, 17 Dec 1993 15:11:09 GMT",
"version": "v1"
}
] | 2011-05-05 | [
[
"Lukierski",
"J.",
""
],
[
"Ruegg",
"H.",
""
],
[
"Zakrzewski",
"W. J.",
""
]
] | We consider the Hamiltonian and Lagrangian formalism describing free \k-relativistic particles with their four-momenta constrained to the \k-deformed mass shell. We study the modifications of the formalism which follow from the introduction of space coordinates with nonvanishing Poisson brackets and from the redefiniti... | 8.631131 | 8.866334 | 8.546789 | 8.122876 | 8.81673 | 8.929823 | 8.816258 | 8.212379 | 8.492693 | 9.070406 | 8.196569 | 7.971327 | 8.423808 | 8.059364 | 7.757261 | 7.73908 | 8.047721 | 7.694771 | 7.91354 | 8.283398 | 7.948062 |
1912.02634 | Boris Merzlikin | I.L. Buchbinder, E.A. Ivanov, B.S. Merzlikin | Low-energy $6D$, ${\cal N}=(1,1)$ SYM effective action beyond the
leading approximation | 1+17 pages; v2: minor corrections, references added | null | 10.1016/j.nuclphysb.2020.114995 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For $6D$, ${\cal N}=(1,1)$ SYM theory formulated in ${\cal N}=(1,0)$ harmonic
superspace as a theory of interacting gauge multiplet and hypermultiplet we
construct the ${\cal N}=(1,1)$ supersymmetric Heisenberg-Euler-type superfield
effective action. The effective action is computed for the slowly varying
on-shell ba... | [
{
"created": "Thu, 5 Dec 2019 15:10:21 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Dec 2019 16:35:36 GMT",
"version": "v2"
}
] | 2020-04-22 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Ivanov",
"E. A.",
""
],
[
"Merzlikin",
"B. S.",
""
]
] | For $6D$, ${\cal N}=(1,1)$ SYM theory formulated in ${\cal N}=(1,0)$ harmonic superspace as a theory of interacting gauge multiplet and hypermultiplet we construct the ${\cal N}=(1,1)$ supersymmetric Heisenberg-Euler-type superfield effective action. The effective action is computed for the slowly varying on-shell back... | 9.523737 | 6.122486 | 8.859513 | 6.590792 | 6.259104 | 6.722293 | 6.78677 | 6.105831 | 6.810709 | 9.7175 | 6.46563 | 7.546104 | 7.644677 | 7.02298 | 7.0944 | 7.183801 | 7.159382 | 7.047771 | 7.528099 | 8.267284 | 7.463136 |
hep-th/0504112 | Marcin Ostrowski | Marcin Ostrowski | Casimir effect in external magnetic field | 12 pages, 9 figures | Acta Phys.Polon. B37 (2006) 1753-1768 | null | null | hep-th | null | In this paper we examine the Casimir effect for charged fields in presence of
external magnetic field. We consider scalar field (connected with spinless
particles) and the Dirac field (connected with 1/2-spin particles). In both
cases we describe quantum field using the canonical formalism. We obtain vacuum
energy by... | [
{
"created": "Wed, 13 Apr 2005 07:51:53 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Dec 2005 11:34:43 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Ostrowski",
"Marcin",
""
]
] | In this paper we examine the Casimir effect for charged fields in presence of external magnetic field. We consider scalar field (connected with spinless particles) and the Dirac field (connected with 1/2-spin particles). In both cases we describe quantum field using the canonical formalism. We obtain vacuum energy by d... | 8.110176 | 7.525245 | 8.603754 | 7.816279 | 7.606531 | 7.080798 | 7.270107 | 7.268572 | 7.210504 | 8.943385 | 7.437103 | 7.252467 | 7.774106 | 7.295519 | 7.404658 | 7.340574 | 7.434583 | 7.584342 | 6.991716 | 7.506235 | 7.168188 |
1601.01176 | Marco Panero | Marco Panero | The numerical approach to quantum field theory in a non-commutative
space | 15 pages, 6 figures, invited talk presented at the Humboldt Kolleg
"Open Problems in Theoretical Physics: the Issue of Quantum Space-Time", to
appear in the proceedings of the Corfu Summer Institute 2015 "School and
Workshops on Elementary Particle Physics and Gravity" (Corfu, Greece, 1-27
September 2015) | PoS CORFU2015 (2016) 099 | null | null | hep-th gr-qc hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Numerical simulation is an important non-perturbative tool to study quantum
field theories defined in non-commutative spaces. In this contribution, a
selection of results from Monte Carlo calculations for non-commutative models
is presented, and their implications are reviewed. In addition, we also discuss
how relate... | [
{
"created": "Wed, 6 Jan 2016 13:54:57 GMT",
"version": "v1"
}
] | 2016-11-21 | [
[
"Panero",
"Marco",
""
]
] | Numerical simulation is an important non-perturbative tool to study quantum field theories defined in non-commutative spaces. In this contribution, a selection of results from Monte Carlo calculations for non-commutative models is presented, and their implications are reviewed. In addition, we also discuss how related ... | 10.413456 | 9.908535 | 9.170458 | 8.892827 | 9.352319 | 9.369582 | 9.343707 | 9.340165 | 8.814645 | 9.693262 | 9.253025 | 9.100084 | 9.615863 | 9.075867 | 8.99734 | 9.32636 | 9.015403 | 9.307554 | 9.525299 | 9.302649 | 9.646904 |
1002.4636 | Soo-Jong Rey | Soo-Jong Rey, Fumihiko Sugino | A Nonperturbative Proposal for Nonabelian Tensor Gauge Theory and
Dynamical Quantum Yang-Baxter Maps | 62 pages + 14 figures | null | null | null | hep-th cond-mat.str-el hep-lat nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a nonperturbative approach to nonabelian two-form gauge theory. We
formulate the theory on a lattice in terms of plaquette as fundamental
dynamical variable, and assign U(N) Chan-Paton colors at each boundary link. We
show that, on hypercubic lattices, such colored plaquette variables constitute
Yang-Baxte... | [
{
"created": "Thu, 25 Feb 2010 20:55:24 GMT",
"version": "v1"
}
] | 2010-02-26 | [
[
"Rey",
"Soo-Jong",
""
],
[
"Sugino",
"Fumihiko",
""
]
] | We propose a nonperturbative approach to nonabelian two-form gauge theory. We formulate the theory on a lattice in terms of plaquette as fundamental dynamical variable, and assign U(N) Chan-Paton colors at each boundary link. We show that, on hypercubic lattices, such colored plaquette variables constitute Yang-Baxter ... | 13.217271 | 14.44466 | 15.095052 | 13.709638 | 13.260397 | 14.492551 | 14.636943 | 13.669126 | 13.748946 | 15.702312 | 13.248313 | 13.190922 | 13.219705 | 12.805351 | 13.379942 | 13.239964 | 12.808295 | 13.167079 | 13.0158 | 13.457418 | 12.79391 |
hep-th/9509148 | John Schwarz | John H. Schwarz | Superstring Dualities | 14 pages; latex; an error has been corrected | Nucl.Phys.Proc.Suppl. 49 (1996) 183-190 | 10.1016/0920-5632(96)00334-9 | CALT-68-2019 | hep-th | null | This talk is divided into two parts. The first part reviews some of the
duality relationships between superstring theories. These relationships are
interpreted as providing evidence for the existence of a unique underlying
fundamental theory. The second part describes my recent work on the SL(2,Z)
duality group of th... | [
{
"created": "Tue, 26 Sep 1995 18:17:46 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Oct 1995 21:44:35 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Schwarz",
"John H.",
""
]
] | This talk is divided into two parts. The first part reviews some of the duality relationships between superstring theories. These relationships are interpreted as providing evidence for the existence of a unique underlying fundamental theory. The second part describes my recent work on the SL(2,Z) duality group of the ... | 5.861035 | 4.896628 | 6.364076 | 4.817753 | 4.708243 | 4.605274 | 4.293078 | 4.834894 | 4.793141 | 5.893349 | 4.940257 | 5.067562 | 5.592864 | 5.089285 | 5.174201 | 5.14516 | 5.060315 | 5.174212 | 5.156749 | 5.454837 | 5.193206 |
2003.07126 | Kin-ya Oda | Shinya Matsuzaki, Shota Miyawaki, Kin-ya Oda, and Masatoshi Yamada | Dynamically emergent gravity from hidden local Lorentz symmetry | 7 pages; version accepted for publication in Phys. Lett. B; a table,
footnotes, references, and comments added | Phys.Lett.B 813 (2021) 135975 | 10.1016/j.physletb.2020.135975 | OU-HET-1047 | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Gravity can be regarded as a consequence of local Lorentz (LL) symmetry,
which is essential in defining a spinor field in curved spacetime. The
gravitational action may admit a zero-field limit of the metric and vierbein at
a certain ultraviolet cutoff scale such that the action becomes a linear
realization of the LL... | [
{
"created": "Mon, 16 Mar 2020 11:34:07 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Dec 2020 07:20:42 GMT",
"version": "v2"
}
] | 2020-12-23 | [
[
"Matsuzaki",
"Shinya",
""
],
[
"Miyawaki",
"Shota",
""
],
[
"Oda",
"Kin-ya",
""
],
[
"Yamada",
"Masatoshi",
""
]
] | Gravity can be regarded as a consequence of local Lorentz (LL) symmetry, which is essential in defining a spinor field in curved spacetime. The gravitational action may admit a zero-field limit of the metric and vierbein at a certain ultraviolet cutoff scale such that the action becomes a linear realization of the LL s... | 11.8309 | 12.895936 | 11.896281 | 10.960649 | 11.935367 | 11.447486 | 11.055056 | 11.793659 | 11.653947 | 12.088971 | 11.336927 | 11.4018 | 11.490105 | 11.358225 | 11.367 | 11.382756 | 11.113585 | 11.227199 | 11.194835 | 11.610945 | 10.836987 |
hep-th/0309065 | Jan-Markus Schwindt | Jan-Markus Schwindt and Christof Wetterich | Holographic Branes | 13 pages, references added | Phys.Lett.B578:409-417,2004 | 10.1016/j.physletb.2003.10.061 | HD-THEP-03-45 | hep-th | null | We discuss the properties of codimension-two branes and compare them to
codimension-one branes. In particular, we show that for deficit angle branes
the brane energy momentum tensor is uniquely related to integration constants
in the bulk solution. We investigate chiral fermions whose wave functions are
concentrated ... | [
{
"created": "Fri, 5 Sep 2003 11:05:15 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Dec 2003 15:20:38 GMT",
"version": "v2"
}
] | 2010-01-27 | [
[
"Schwindt",
"Jan-Markus",
""
],
[
"Wetterich",
"Christof",
""
]
] | We discuss the properties of codimension-two branes and compare them to codimension-one branes. In particular, we show that for deficit angle branes the brane energy momentum tensor is uniquely related to integration constants in the bulk solution. We investigate chiral fermions whose wave functions are concentrated on... | 12.980504 | 13.934237 | 11.356903 | 11.723955 | 12.227146 | 11.405271 | 13.760529 | 12.076861 | 12.185242 | 13.196134 | 12.165883 | 11.668598 | 11.434606 | 11.471379 | 11.627849 | 11.905591 | 11.614096 | 11.372942 | 11.501234 | 12.228941 | 11.599921 |
hep-th/9810041 | Philip Mark Cowdall | P.M.Cowdall (Cambridge University) | On Gauged Maximal Supergravity In Six Dimensions | 26 pages, LaTeX, no figures. Significant simplifications of final
results have been made. Also an appendix concerning the limit of D=5 N=4
SU(2)xU(1) gauged supergravity, in which the U(1) coupling constant is turned
off, has been added. Minor typos have been corrected. Complete bosonic and
fermionic Lagrangian... | JHEP 9906 (1999) 018 | 10.1088/1126-6708/1999/06/018 | DAMTP-1998-137 | hep-th | null | The maximal SO(5) gauged D=7 supergravity is dimensionally reduced to six
dimensions yielding a new SO(5) gauged D=6 model. It is shown that, unlike in
D=7, the SO(5) gauge coupling constant can be taken to zero to yield the
maximally extended supergravity in six dimensions. It is also shown that the
limit of D=5 N=4... | [
{
"created": "Tue, 6 Oct 1998 14:24:20 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Dec 1998 12:48:44 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Dec 1998 12:40:36 GMT",
"version": "v3"
},
{
"created": "Fri, 18 Jun 1999 10:08:20 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Cowdall",
"P. M.",
"",
"Cambridge University"
]
] | The maximal SO(5) gauged D=7 supergravity is dimensionally reduced to six dimensions yielding a new SO(5) gauged D=6 model. It is shown that, unlike in D=7, the SO(5) gauge coupling constant can be taken to zero to yield the maximally extended supergravity in six dimensions. It is also shown that the limit of D=5 N=4 S... | 5.922647 | 5.562936 | 6.124687 | 5.639215 | 5.292385 | 5.157816 | 5.5226 | 5.382227 | 5.266488 | 5.920835 | 5.622413 | 5.362842 | 6.000961 | 5.571545 | 5.492655 | 5.420875 | 5.310169 | 5.268611 | 5.417398 | 6.078032 | 5.360052 |
1810.11343 | Boris Pioline | Boris Pioline | String theory integrands and supergravity divergences | 40 pages; v2: after fixing a factor of 2 mistake in Eq. (2.41), all
divergent terms now agree with SUGRA predictions. Added a note at end of Sec
1 on the definition of the truncated moduli space M_{h,n}(\Lambda) | null | 10.1007/JHEP02(2019)148 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | At low energies, interactions of massless particles in type II strings
compactified on a torus $T^d$ are described by an effective Wilsonian action
$\mathcal{S}(\Lambda)$, consisting of the usual supergravity Lagrangian
supplemented by an infinite series of higher-derivative vertices, including the
much studied $\nab... | [
{
"created": "Fri, 26 Oct 2018 14:21:13 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Dec 2018 12:47:01 GMT",
"version": "v2"
}
] | 2019-03-27 | [
[
"Pioline",
"Boris",
""
]
] | At low energies, interactions of massless particles in type II strings compactified on a torus $T^d$ are described by an effective Wilsonian action $\mathcal{S}(\Lambda)$, consisting of the usual supergravity Lagrangian supplemented by an infinite series of higher-derivative vertices, including the much studied $\nabla... | 8.212658 | 7.582917 | 8.898368 | 7.252161 | 7.96664 | 7.710248 | 7.359799 | 7.416201 | 7.179854 | 8.845927 | 7.187266 | 7.622748 | 8.029368 | 7.708149 | 7.782322 | 7.791811 | 7.650175 | 7.663568 | 7.649625 | 7.9575 | 7.711679 |
hep-th/0408135 | Jorge Henrique de Oliveira Sales | A.T. Suzuki and J.H.O. Sales | The Light Front Gauge Propagator: The Status Quo | 5 pages. Talk given in Light-Cone Workshop: Hadrons and Beyond, LC03,
Grey College, University of Durham, Durham, 5-9 August, 2003 | null | null | null | hep-th | null | At the classical level, the inverse differential operator for the quadratic
term in the gauge field Lagrangian density fixed in the light front through the
multiplier (nA)^2 yields the standard two term propagator with single
unphysical pole of the type (kn)^-1. Upon canonical quantization on the
light-front, there e... | [
{
"created": "Wed, 18 Aug 2004 13:27:28 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Suzuki",
"A. T.",
""
],
[
"Sales",
"J. H. O.",
""
]
] | At the classical level, the inverse differential operator for the quadratic term in the gauge field Lagrangian density fixed in the light front through the multiplier (nA)^2 yields the standard two term propagator with single unphysical pole of the type (kn)^-1. Upon canonical quantization on the light-front, there eme... | 14.159218 | 13.522044 | 15.403813 | 13.867832 | 16.134199 | 14.440029 | 14.601799 | 13.899627 | 13.41503 | 15.418159 | 13.718461 | 12.444617 | 13.819212 | 13.436954 | 13.021772 | 13.206347 | 13.107818 | 12.690934 | 13.078897 | 13.892238 | 13.064497 |
2402.17980 | Weican Yang | Wei-Can Yang, Chuan-Yin Xia, Yu Tian, Makoto Tsubota, and Hua-Bi Zeng | Emergence of Large-Scale Structures in Holographic Superfluid Turbulence | 8 pages, 6 figures | null | null | null | hep-th cond-mat.quant-gas | http://creativecommons.org/licenses/by/4.0/ | In two-dimensional turbulence systems, the emergence of large-scale
structures holds profound physical implications, particularly as it indicates
the occurrence of inverse energy cascades, thereby garnering significant
attention. In this paper, we report a novel vortex clusters formation in the
background of near-ext... | [
{
"created": "Wed, 28 Feb 2024 01:50:31 GMT",
"version": "v1"
}
] | 2024-02-29 | [
[
"Yang",
"Wei-Can",
""
],
[
"Xia",
"Chuan-Yin",
""
],
[
"Tian",
"Yu",
""
],
[
"Tsubota",
"Makoto",
""
],
[
"Zeng",
"Hua-Bi",
""
]
] | In two-dimensional turbulence systems, the emergence of large-scale structures holds profound physical implications, particularly as it indicates the occurrence of inverse energy cascades, thereby garnering significant attention. In this paper, we report a novel vortex clusters formation in the background of near-extre... | 11.930591 | 11.149228 | 11.879267 | 10.955901 | 11.492954 | 11.238875 | 10.448009 | 10.558354 | 10.780015 | 12.085724 | 10.591667 | 10.797128 | 11.059474 | 10.789132 | 10.628392 | 10.739547 | 10.561159 | 10.332498 | 10.658925 | 11.304236 | 10.499395 |
0707.1317 | Neil Copland Dr | Neil B. Copland | Aspects of M-Theory Brane Interactions and String Theory Symmetries | 161 pages. Author's PhD thesis | null | null | null | hep-th | null | The dissertation consists of two parts. The first presents an account of the
effective worldvolume description of $N$ coincident M2-branes ending on an
M5-brane in M-theory. It reviews Basu and Harvey's recent description of the
worldvolume theory of the M2-branes in terms of a Bogomol'nyi equation, and its
solution ... | [
{
"created": "Mon, 9 Jul 2007 18:25:56 GMT",
"version": "v1"
}
] | 2011-10-27 | [
[
"Copland",
"Neil B.",
""
]
] | The dissertation consists of two parts. The first presents an account of the effective worldvolume description of $N$ coincident M2-branes ending on an M5-brane in M-theory. It reviews Basu and Harvey's recent description of the worldvolume theory of the M2-branes in terms of a Bogomol'nyi equation, and its solution vi... | 10.639611 | 11.251514 | 12.21889 | 10.809741 | 11.758412 | 10.962713 | 12.182351 | 11.253475 | 11.242528 | 12.655297 | 10.41469 | 10.442108 | 10.644633 | 10.455845 | 10.511 | 10.436923 | 10.482729 | 10.217344 | 10.672426 | 10.967413 | 10.407442 |
hep-th/0411274 | M. Hossein Dehghani | M. H. Dehghani | Magnetic Strings in Dilaton Gravity | 16 pages, no figure, references added, some minor corrections | Phys.Rev. D71 (2005) 064010 | 10.1103/PhysRevD.71.064010 | null | hep-th | null | First, I present two new classes of magnetic rotating solutions in
four-dimensional Einstein-Maxwell-dilaton gravity with Liouville-type
potential. The first class of solutions yields a 4-dimensional spacetime with a
longitudinal magnetic field generated by a static or spinning magnetic string.
I find that these solu... | [
{
"created": "Tue, 30 Nov 2004 12:46:44 GMT",
"version": "v1"
},
{
"created": "Thu, 5 May 2005 04:45:00 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dehghani",
"M. H.",
""
]
] | First, I present two new classes of magnetic rotating solutions in four-dimensional Einstein-Maxwell-dilaton gravity with Liouville-type potential. The first class of solutions yields a 4-dimensional spacetime with a longitudinal magnetic field generated by a static or spinning magnetic string. I find that these soluti... | 6.162097 | 4.46116 | 6.148863 | 5.124444 | 5.255593 | 4.917994 | 5.07225 | 4.841775 | 4.710783 | 6.149332 | 5.092863 | 5.482855 | 6.098546 | 5.781328 | 5.632479 | 5.546188 | 5.64577 | 5.586069 | 5.784369 | 5.970224 | 5.674784 |
1312.5344 | Christopher Beem | Christopher Beem, Madalena Lemos, Pedro Liendo, Wolfger Peelaers,
Leonardo Rastelli, and Balt C. van Rees | Infinite Chiral Symmetry in Four Dimensions | 75 pages. v3: minor corrections. Final version -- published in
Communications in Mathematical Physics | Commun. Math. Phys. 336 (2015) 3, 1359-1433 | 10.1007/s00220-014-2272-x | YITP-SB-13-45, CERN-PH-TH/2013-311, HU-EP-13/78 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a new correspondence between four-dimensional conformal field
theories with extended supersymmetry and two-dimensional chiral algebras. The
meromorphic correlators of the chiral algebra compute correlators in a
protected sector of the four-dimensional theory. Infinite chiral symmetry has
far-reaching cons... | [
{
"created": "Wed, 18 Dec 2013 21:28:38 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Apr 2014 20:54:27 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Sep 2015 19:43:36 GMT",
"version": "v3"
}
] | 2015-09-30 | [
[
"Beem",
"Christopher",
""
],
[
"Lemos",
"Madalena",
""
],
[
"Liendo",
"Pedro",
""
],
[
"Peelaers",
"Wolfger",
""
],
[
"Rastelli",
"Leonardo",
""
],
[
"van Rees",
"Balt C.",
""
]
] | We describe a new correspondence between four-dimensional conformal field theories with extended supersymmetry and two-dimensional chiral algebras. The meromorphic correlators of the chiral algebra compute correlators in a protected sector of the four-dimensional theory. Infinite chiral symmetry has far-reaching conseq... | 7.218142 | 6.567 | 7.18948 | 6.91901 | 6.380897 | 7.170013 | 6.704977 | 7.060678 | 6.759337 | 9.429871 | 6.833713 | 6.76707 | 7.477322 | 6.558286 | 7.074533 | 6.829533 | 6.395696 | 6.609133 | 6.687498 | 7.145458 | 7.280313 |
hep-th/9706114 | Vadim V. Tugai | V.V. Tugai, A.A. Zheltukhin | On extension of minimality principle in supersymmetric electrodynamics | 6 pages REVTeX (talk at the seminar "Supersymmetry and quantum field
theory" dedicated to the memory of Acad. Dmitrij Volkov, Kharkov, Jan. 1997)
Resubmition (27.06.97): some misprints in formulae (2) and (36) are
corrected, an omitted term in formula (15) is added. Resubmition (06.11.97):
Incorect sign in last... | null | 10.1007/BFb0105245 | null | hep-th | null | A possibility of an extension of the minimality principle for electromagnetic
interactions of charged and neutral particles having spin 1/2 is investigated.
| [
{
"created": "Sat, 14 Jun 1997 16:38:21 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Jun 1997 12:31:20 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Nov 1997 14:27:23 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Tugai",
"V. V.",
""
],
[
"Zheltukhin",
"A. A.",
""
]
] | A possibility of an extension of the minimality principle for electromagnetic interactions of charged and neutral particles having spin 1/2 is investigated. | 21.042809 | 12.835024 | 13.299997 | 12.81531 | 13.598871 | 12.202346 | 13.177816 | 12.285648 | 13.761788 | 13.523072 | 14.639844 | 14.031406 | 14.554959 | 13.41835 | 13.245761 | 13.72811 | 13.617263 | 14.207335 | 14.449662 | 14.381864 | 14.629519 |
0907.2739 | Per Kraus | James Hansen and Per Kraus | S-duality in AdS/CFT magnetohydrodynamics | 25 pages | null | 10.1088/1126-6708/2009/10/047 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the nonlinear hydrodynamics of a 2+1 dimensional charged conformal
fluid subject to slowly varying external electric and magnetic fields.
Following recent work on deriving nonlinear hydrodynamics from gravity, we
demonstrate how long wavelength perturbations of the AdS dyonic black brane
solution of 4D super... | [
{
"created": "Thu, 16 Jul 2009 03:56:20 GMT",
"version": "v1"
}
] | 2015-05-13 | [
[
"Hansen",
"James",
""
],
[
"Kraus",
"Per",
""
]
] | We study the nonlinear hydrodynamics of a 2+1 dimensional charged conformal fluid subject to slowly varying external electric and magnetic fields. Following recent work on deriving nonlinear hydrodynamics from gravity, we demonstrate how long wavelength perturbations of the AdS dyonic black brane solution of 4D supergr... | 11.455885 | 10.436858 | 12.314378 | 10.210312 | 10.280198 | 10.015121 | 9.889208 | 9.970962 | 10.468001 | 12.509069 | 10.121979 | 10.69431 | 11.262692 | 10.637123 | 10.42139 | 10.619499 | 10.393663 | 10.613199 | 10.685184 | 11.482951 | 10.444121 |
1511.01091 | Marco Stefano Bianchi | Lorenzo Bianchi and Marco S. Bianchi | On the scattering of gluons in the GKP string | 50 pages, 8 tables, 13 figures | null | 10.1007/JHEP02(2016)146 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the one-loop S-matrix for the light bosonic excitations of the GKP
string at strong coupling. These correspond, on the gauge theory side, to gluon
insertions in the GKP vacuum. We perform the calculation by Feynman diagrams in
the worldsheet theory and we compare the result to the integrability
prediction,... | [
{
"created": "Tue, 3 Nov 2015 21:00:01 GMT",
"version": "v1"
}
] | 2016-03-23 | [
[
"Bianchi",
"Lorenzo",
""
],
[
"Bianchi",
"Marco S.",
""
]
] | We compute the one-loop S-matrix for the light bosonic excitations of the GKP string at strong coupling. These correspond, on the gauge theory side, to gluon insertions in the GKP vacuum. We perform the calculation by Feynman diagrams in the worldsheet theory and we compare the result to the integrability prediction, f... | 9.813115 | 8.541912 | 10.554831 | 8.782513 | 9.212715 | 9.054305 | 9.048552 | 8.218562 | 8.537655 | 11.81104 | 8.724884 | 8.893669 | 10.089736 | 9.154531 | 8.982324 | 8.782928 | 9.07379 | 8.831665 | 9.406043 | 10.242568 | 8.763955 |
1906.08265 | Oscar J. C. Dias | Oscar J.C. Dias, Harvey S. Reall and Jorge E. Santos | The BTZ black hole violates strong cosmic censorship | 59 pages, 9 figures. Changes in v2: 1) a few discussions
added/improved, 2) added Section 5.8 discussing the non-smoothness of the
Hartle-Hawking state at the Cauchy horizon | null | 10.1007/JHEP12(2019)097 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the stability of the inner horizon of a rotating BTZ black
hole. We show that linear perturbations arising from smooth initial data are
arbitrarily differentiable at the inner horizon if the black hole is
sufficiently close to extremality. This is demonstrated for scalar fields, for
massive Chern-Simon... | [
{
"created": "Wed, 19 Jun 2019 18:00:01 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Aug 2019 11:05:48 GMT",
"version": "v2"
}
] | 2020-01-29 | [
[
"Dias",
"Oscar J. C.",
""
],
[
"Reall",
"Harvey S.",
""
],
[
"Santos",
"Jorge E.",
""
]
] | We investigate the stability of the inner horizon of a rotating BTZ black hole. We show that linear perturbations arising from smooth initial data are arbitrarily differentiable at the inner horizon if the black hole is sufficiently close to extremality. This is demonstrated for scalar fields, for massive Chern-Simons ... | 6.059976 | 6.340797 | 5.577825 | 5.630736 | 5.717602 | 6.001616 | 6.112623 | 5.422311 | 6.019014 | 5.699628 | 5.755342 | 5.786215 | 5.62308 | 5.607635 | 5.839925 | 5.768755 | 6.003431 | 5.52725 | 5.704472 | 5.702956 | 5.613369 |
hep-th/9407080 | Nieto Luis M. | M.A. del Olmo, M.A. Rodriguez and P. Winternitz | The Conformal Group SU(2,2) and Integrable Systems on a Lorentzian
Hyperboloid | 37 pages (CRM 2194) | Fortsch.Phys.44:199-233,1996 | 10.1002/prop.2190440303 | null | hep-th | null | Eleven different types of "maximally superintegrable" Hamiltonian systems on
the real hyperboloid $(s^0)^2-(s^1)^2+(s^2)^2-(s^3)^2=1$ are obtained. All of
them correspond to a free Hamiltonian system on the homogeneous space
$SU(2,2)/U(2,1)$, but to reductions by different maximal abelian subgroups of
$SU(2,2)$. Each... | [
{
"created": "Fri, 15 Jul 1994 15:01:39 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"del Olmo",
"M. A.",
""
],
[
"Rodriguez",
"M. A.",
""
],
[
"Winternitz",
"P.",
""
]
] | Eleven different types of "maximally superintegrable" Hamiltonian systems on the real hyperboloid $(s^0)^2-(s^1)^2+(s^2)^2-(s^3)^2=1$ are obtained. All of them correspond to a free Hamiltonian system on the homogeneous space $SU(2,2)/U(2,1)$, but to reductions by different maximal abelian subgroups of $SU(2,2)$. Each o... | 7.182156 | 7.135429 | 7.848407 | 6.391273 | 7.231115 | 7.13025 | 7.984513 | 6.398755 | 6.723752 | 8.697989 | 6.888495 | 6.508251 | 6.372299 | 6.220821 | 6.34154 | 6.422223 | 6.383318 | 6.134362 | 6.189821 | 6.844643 | 6.468227 |
hep-th/9912089 | Jean-Loup Gervais | Jean-Loup Gervais, Henning Samtleben | Integrable structures in classical off-shell 10D supersymmetric
Yang-Mills theory | 43 pages, 4 figures. Improved version for publication | Commun.Math.Phys. 217 (2001) 1-31 | 10.1007/s002200100364 | LPTENS-99/54 | hep-th math-ph math.MP nlin.SI solv-int | null | The superspace flatness conditions which are equivalent to the field
equations of supersymmetric Yang-Mills theory in ten dimensions have not been
useful so far to derive non trivial classical solutions. Recently, modified
flatness conditions were proposed, which are explicitly integrable
(hep-th/9811108), and are ba... | [
{
"created": "Fri, 10 Dec 1999 15:37:37 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Apr 2000 10:30:43 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Gervais",
"Jean-Loup",
""
],
[
"Samtleben",
"Henning",
""
]
] | The superspace flatness conditions which are equivalent to the field equations of supersymmetric Yang-Mills theory in ten dimensions have not been useful so far to derive non trivial classical solutions. Recently, modified flatness conditions were proposed, which are explicitly integrable (hep-th/9811108), and are base... | 13.530626 | 13.480516 | 14.837077 | 12.989859 | 14.168818 | 13.700549 | 13.704104 | 13.973337 | 12.485243 | 15.695456 | 12.875944 | 12.553419 | 13.362122 | 12.601284 | 13.534162 | 12.513816 | 12.965616 | 13.141864 | 12.865067 | 13.415084 | 13.252332 |
hep-th/0511189 | Mohab Abou Zeid Dr. | M. Abou-Zeid and C. M. Hull | A Chiral Perturbation Expansion for Gravity | 11 pages, LaTeX, no figures; v2: one reference added | JHEP0602:057,2006 | 10.1088/1126-6708/2006/02/057 | IHES/P/05/48 | hep-th | null | A formulation of Einstein gravity, analogous to that for gauge theory arising
from the Chalmers-Siegel action, leads to a perturbation theory about an
asymmetric weak coupling limit that treats positive and negative helicities
differently. We find power counting rules for amplitudes that suggest the
theory could find... | [
{
"created": "Fri, 18 Nov 2005 14:49:31 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Dec 2005 10:16:18 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Abou-Zeid",
"M.",
""
],
[
"Hull",
"C. M.",
""
]
] | A formulation of Einstein gravity, analogous to that for gauge theory arising from the Chalmers-Siegel action, leads to a perturbation theory about an asymmetric weak coupling limit that treats positive and negative helicities differently. We find power counting rules for amplitudes that suggest the theory could find a... | 15.475005 | 14.624159 | 19.300585 | 14.398713 | 13.891324 | 15.029957 | 15.370689 | 16.232941 | 13.969576 | 19.171848 | 14.849676 | 14.41676 | 15.407376 | 14.549082 | 13.979495 | 15.185507 | 14.320225 | 15.294708 | 14.595186 | 15.334086 | 13.971798 |
2203.15682 | Gabriel Luchini | G. Luchini, V. B. Zach\'e | A zero-curvature representation of electromagnetism and the conservation
of electric charge | null | null | 10.1007/s13538-022-01131-6 | null | hep-th physics.class-ph | http://creativecommons.org/licenses/by/4.0/ | We show that the laws of electromagnetism in $(D+1)$-dimensional Minkowski
space-time $\mathcal{M}$, explicitly for $D=1$, $2$ and $3$, can be obtained
from an integral representation of the zero-curvature equation in the
corresponding loop space $\mathcal{L}^{(D-1)}(\mathcal{M})$. The conservation
of the electric ch... | [
{
"created": "Tue, 29 Mar 2022 15:41:40 GMT",
"version": "v1"
}
] | 2022-06-15 | [
[
"Luchini",
"G.",
""
],
[
"Zaché",
"V. B.",
""
]
] | We show that the laws of electromagnetism in $(D+1)$-dimensional Minkowski space-time $\mathcal{M}$, explicitly for $D=1$, $2$ and $3$, can be obtained from an integral representation of the zero-curvature equation in the corresponding loop space $\mathcal{L}^{(D-1)}(\mathcal{M})$. The conservation of the electric char... | 5.557175 | 5.14654 | 6.150471 | 5.403822 | 5.346775 | 5.265623 | 5.532948 | 5.290303 | 5.250946 | 6.258072 | 5.17164 | 5.234571 | 5.715412 | 5.374964 | 5.300383 | 5.210873 | 5.391164 | 5.272396 | 5.373378 | 5.903979 | 5.236585 |
1109.4159 | Christoph Adam | C. Adam, J. M. Queiruga | An algebraic construction of twin-like models | Latex, 21 pages, no figures; typos corrected, references added | null | 10.1103/PhysRevD.84.105028 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | If the generalized dynamics of K field theories (i.e., field theories with a
non-standard kinetic term) is taken into account, then the possibility of
so-called twin-like models opens up, that is, of different field theories which
share the same topological defect solution with the same energy density. These
twin-lik... | [
{
"created": "Mon, 19 Sep 2011 20:09:36 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Oct 2011 11:44:27 GMT",
"version": "v2"
}
] | 2013-05-29 | [
[
"Adam",
"C.",
""
],
[
"Queiruga",
"J. M.",
""
]
] | If the generalized dynamics of K field theories (i.e., field theories with a non-standard kinetic term) is taken into account, then the possibility of so-called twin-like models opens up, that is, of different field theories which share the same topological defect solution with the same energy density. These twin-like ... | 7.45108 | 6.832568 | 8.069894 | 7.049265 | 7.569773 | 7.120388 | 7.07647 | 7.058055 | 7.075203 | 8.048976 | 6.998269 | 7.197181 | 7.599639 | 7.504776 | 7.379671 | 7.326455 | 7.290751 | 7.359102 | 7.54148 | 7.665336 | 7.362142 |
1709.00107 | Mir Faizal | Mushtaq B Shah, Mir Faizal, Prince A Ganai, Zaid Zaz, Anha Bhat, Syed
Masood | Boundary Effects in Super-Yang-Mills Theory | 16 pages, Accepted in EPJC | Eur. Phys. J. C 77, 309 (2017) | 10.1140/epjc/s10052-017-4861-2 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we shall analyse a three dimensional supersymmetry theory with
$\mathcal{N} = 2$. The effective Lagrangian will be given by the sum of the
gauge fixing term and the ghost term with the original classical Lagrangian. In
presence of a boundary the supersymmetry of this Lagrangian will be broken.
However,... | [
{
"created": "Thu, 31 Aug 2017 23:22:23 GMT",
"version": "v1"
}
] | 2017-09-04 | [
[
"Shah",
"Mushtaq B",
""
],
[
"Faizal",
"Mir",
""
],
[
"Ganai",
"Prince A",
""
],
[
"Zaz",
"Zaid",
""
],
[
"Bhat",
"Anha",
""
],
[
"Masood",
"Syed",
""
]
] | In this paper, we shall analyse a three dimensional supersymmetry theory with $\mathcal{N} = 2$. The effective Lagrangian will be given by the sum of the gauge fixing term and the ghost term with the original classical Lagrangian. In presence of a boundary the supersymmetry of this Lagrangian will be broken. However, i... | 5.647202 | 4.887526 | 5.396682 | 4.912849 | 4.829688 | 4.735951 | 4.782902 | 4.846941 | 5.015454 | 5.411957 | 4.915635 | 4.885871 | 5.120197 | 5.041597 | 5.019494 | 4.880513 | 4.960338 | 5.034653 | 5.024265 | 5.241844 | 5.023567 |
hep-th/9502017 | J. Mourad | A. Kehagias, J. Madore, J. Mourad and G. Zoupanos | LINEAR CONNECTIONS ON EXTENDED SPACE-TIME | 15 pages, plain TeX | J.Math.Phys. 36 (1995) 5855-5867 | 10.1063/1.531292 | LMPM 95-01 | hep-th gr-qc | null | A modification of Kaluza-Klein theory is proposed which is general enough to
admit an arbitrary finite noncommutative internal geometry. It is shown that
the existence of a non-trival extension to the total geometry of a linear
connection on space-time places severe restrictions on the structure of the
noncommutative... | [
{
"created": "Thu, 2 Feb 1995 19:03:13 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Kehagias",
"A.",
""
],
[
"Madore",
"J.",
""
],
[
"Mourad",
"J.",
""
],
[
"Zoupanos",
"G.",
""
]
] | A modification of Kaluza-Klein theory is proposed which is general enough to admit an arbitrary finite noncommutative internal geometry. It is shown that the existence of a non-trival extension to the total geometry of a linear connection on space-time places severe restrictions on the structure of the noncommutative f... | 11.858393 | 11.391265 | 12.189807 | 10.126739 | 11.818192 | 12.352092 | 10.750575 | 10.636898 | 10.508376 | 13.515266 | 11.575427 | 11.522763 | 10.875966 | 10.473501 | 11.026896 | 10.294848 | 10.710383 | 10.905055 | 10.749504 | 10.617013 | 10.857421 |
hep-th/0605257 | Oriol Pujolas | Oriol Pujolas | Quantum fluctuations in the DGP model and the size of the cross-over
scale | 16 pages, 2 figures. References added | JCAP0610:004,2006 | 10.1088/1475-7516/2006/10/004 | null | hep-th astro-ph hep-ph | null | The Dvali-Gabadadze-Porrati model introduces a parameter, the cross-over
scale $r_c$, setting the scale where higher dimensional effects are important.
In order to agree with observations and to explain the current acceleration of
the Universe, $r_c$ must be of the order of the present Hubble radius. We
discuss a mec... | [
{
"created": "Thu, 25 May 2006 20:45:39 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jun 2006 20:57:04 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Pujolas",
"Oriol",
""
]
] | The Dvali-Gabadadze-Porrati model introduces a parameter, the cross-over scale $r_c$, setting the scale where higher dimensional effects are important. In order to agree with observations and to explain the current acceleration of the Universe, $r_c$ must be of the order of the present Hubble radius. We discuss a mecha... | 7.228762 | 6.820678 | 7.312641 | 6.458193 | 7.258405 | 7.312106 | 7.431688 | 6.719023 | 7.349753 | 7.773598 | 7.179641 | 7.243444 | 6.891652 | 6.781819 | 6.960428 | 7.001905 | 6.884068 | 6.827026 | 6.856691 | 6.875314 | 7.05374 |
1303.3966 | Renann Jusinskas | Renann Lipinski Jusinskas | Nilpotency of the b ghost in the non-minimal pure spinor formalism | 27 pages; footnotes added; typos fixed; Published version | JHEP05(2013)048 | 10.1007/JHEP05(2013)048 | ICTP-SAIFR/2013-007 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The b ghost in the non minimal pure spinor formalism is not a fundamental
field. It is based on a complicated chain of operators and proving its
nilpotency is nontrivial. Chandia proved this property in arXiv:1008.1778, but
with an assumption on the non-minimal variables that is not valid in general.
In this work, th... | [
{
"created": "Sat, 16 Mar 2013 10:47:05 GMT",
"version": "v1"
},
{
"created": "Thu, 16 May 2013 18:04:43 GMT",
"version": "v2"
}
] | 2013-05-17 | [
[
"Jusinskas",
"Renann Lipinski",
""
]
] | The b ghost in the non minimal pure spinor formalism is not a fundamental field. It is based on a complicated chain of operators and proving its nilpotency is nontrivial. Chandia proved this property in arXiv:1008.1778, but with an assumption on the non-minimal variables that is not valid in general. In this work, the ... | 14.729833 | 10.728979 | 12.084707 | 9.796209 | 11.063432 | 10.109888 | 10.333954 | 10.197264 | 10.537632 | 12.730526 | 11.949049 | 11.109845 | 11.423344 | 10.701524 | 11.00826 | 10.815965 | 10.69374 | 11.185147 | 10.412841 | 11.791871 | 10.977292 |
0807.2121 | Herman Verlinde | Herman Verlinde | D2 or M2? A Note on Membrane Scattering | 11 pages,1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by a physical interpretation of its correlation functions as
membrane scattering amplitudes, we re-address whether the Lorentzian BLG theory
can be quantized such that it preserves SO(8) superconformal symmetry. We find
that this appears to be possible. While the model seems to adequately reproduce
protecte... | [
{
"created": "Mon, 14 Jul 2008 17:52:22 GMT",
"version": "v1"
}
] | 2008-07-15 | [
[
"Verlinde",
"Herman",
""
]
] | Motivated by a physical interpretation of its correlation functions as membrane scattering amplitudes, we re-address whether the Lorentzian BLG theory can be quantized such that it preserves SO(8) superconformal symmetry. We find that this appears to be possible. While the model seems to adequately reproduce protected ... | 16.427929 | 15.032487 | 18.197704 | 13.868665 | 15.309707 | 14.807456 | 13.89511 | 14.586531 | 15.083755 | 17.803284 | 14.498149 | 14.398517 | 16.21542 | 14.229453 | 14.322038 | 14.478404 | 14.033878 | 14.465694 | 14.615114 | 16.325779 | 14.596843 |
hep-th/9403046 | Evan Reidell | R. Jackiw | Topological Structures in the Standard Model at High $T$ | 8 pages in plain TeX, with PostScript figures (inside the TeX code!),
MIT-CTP-2285 | null | null | null | hep-th | null | Topological Structures in the Standard Model at high $T$ are discussed.
| [
{
"created": "Mon, 7 Mar 1994 21:49:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Jackiw",
"R.",
""
]
] | Topological Structures in the Standard Model at high $T$ are discussed. | 59.743488 | 22.25848 | 20.224226 | 22.463928 | 35.720798 | 25.888998 | 28.95817 | 24.245937 | 19.035339 | 25.801989 | 23.81209 | 23.861202 | 29.182293 | 26.289085 | 28.347935 | 23.066063 | 27.143587 | 23.878178 | 24.397245 | 22.982729 | 25.370863 |
hep-th/9309102 | David N. Yetter | Louis Crane, Louis H. Kauffman, David N. Yetter | On the Classicality of Broda's SU(2) Invariant of 4-manifolds | 4 pages (revised to state correctly Lemma 1--the correct lemma was
proved, and used throughout, but the original statement jumbled some
phrases--and add an explanatory footnote on an abuse of language) | null | null | null | hep-th math.QA | null | Recent work of Roberts has shown that the first surgical 4-manifold invariant
of Broda and (up to an unspecified normalization factor) the state-sum
invariant arising from the TQFT of Crane-Yetter are equivalent to the signature
of the 4-manifold. Subsequently Broda defined another surgical invariant in
which the 1- ... | [
{
"created": "Sat, 18 Sep 1993 19:12:44 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Sep 1993 20:56:07 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Crane",
"Louis",
""
],
[
"Kauffman",
"Louis H.",
""
],
[
"Yetter",
"David N.",
""
]
] | Recent work of Roberts has shown that the first surgical 4-manifold invariant of Broda and (up to an unspecified normalization factor) the state-sum invariant arising from the TQFT of Crane-Yetter are equivalent to the signature of the 4-manifold. Subsequently Broda defined another surgical invariant in which the 1- an... | 13.016266 | 12.042921 | 14.908333 | 13.251204 | 15.959703 | 13.180428 | 13.09409 | 12.9139 | 13.29044 | 18.623985 | 13.809542 | 12.506031 | 13.787842 | 11.863627 | 11.876781 | 12.134608 | 11.643671 | 12.388253 | 12.226918 | 13.189396 | 13.407215 |
2004.06929 | Sergio Cecotti | Sergio Cecotti | Special Geometry and the Swampland | 94 pages, 2 figures | null | 10.1007/JHEP09(2020)147 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of 4d effective gravity theories with 8 supersymmetries, we
propose to unify, strenghten, and refine the several swampland conjectures into
a single statement: the structural criterion, modelled on the structure theorem
in Hodge theory. In its most abstract form the new swampland criterion applies
to a... | [
{
"created": "Wed, 15 Apr 2020 07:54:58 GMT",
"version": "v1"
}
] | 2020-10-28 | [
[
"Cecotti",
"Sergio",
""
]
] | In the context of 4d effective gravity theories with 8 supersymmetries, we propose to unify, strenghten, and refine the several swampland conjectures into a single statement: the structural criterion, modelled on the structure theorem in Hodge theory. In its most abstract form the new swampland criterion applies to all... | 8.134528 | 8.544958 | 9.714998 | 8.389951 | 9.241495 | 8.982913 | 9.002464 | 8.543255 | 8.394625 | 9.716353 | 8.281898 | 8.207677 | 8.202266 | 7.930709 | 7.912571 | 8.074784 | 8.131907 | 7.942492 | 7.791797 | 8.236609 | 7.924514 |
1707.03520 | Masaki Yamada | Ali Masoumi, Alexander Vilenkin, Masaki Yamada | Inflation in multi-field random Gaussian landscapes | 25 pages, 5 figures; (v2) minor changes, Fig. 5 updated | null | 10.1088/1475-7516/2017/12/035 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate slow-roll inflation in a multi-field random Gaussian
landscape. The landscape is assumed to be small-field, with a correlation
length much smaller than the Planck scale. Inflation then typically occurs in
small patches of the landscape, localized near inflection or saddle points. We
find that the infla... | [
{
"created": "Wed, 12 Jul 2017 02:55:33 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Feb 2018 04:23:08 GMT",
"version": "v2"
}
] | 2018-02-13 | [
[
"Masoumi",
"Ali",
""
],
[
"Vilenkin",
"Alexander",
""
],
[
"Yamada",
"Masaki",
""
]
] | We investigate slow-roll inflation in a multi-field random Gaussian landscape. The landscape is assumed to be small-field, with a correlation length much smaller than the Planck scale. Inflation then typically occurs in small patches of the landscape, localized near inflection or saddle points. We find that the inflati... | 9.058218 | 10.135903 | 9.385292 | 8.85737 | 9.524545 | 8.936149 | 10.134403 | 9.526121 | 8.341259 | 10.044813 | 9.382343 | 8.844906 | 8.577928 | 8.278723 | 8.712931 | 8.752081 | 8.81446 | 8.499605 | 8.599833 | 8.601044 | 8.58575 |
hep-th/9811023 | Hubert Saleur | H. Saleur | The long delayed solution of the Bukhvostov Lipatov model | 9 pages | null | 10.1088/0305-4470/32/18/102 | USC-98-017 | hep-th cond-mat | null | In this paper I complete the solution of the Bukhvostov Lipatov model by
computing the physical excitations and their factorized S matrix. I also
explain the paradoxes which led in recent years to the suspicion that the model
may not be integrable.
| [
{
"created": "Tue, 3 Nov 1998 00:25:13 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Saleur",
"H.",
""
]
] | In this paper I complete the solution of the Bukhvostov Lipatov model by computing the physical excitations and their factorized S matrix. I also explain the paradoxes which led in recent years to the suspicion that the model may not be integrable. | 14.856479 | 10.712329 | 16.419048 | 11.624889 | 11.015472 | 12.06513 | 11.186896 | 11.140225 | 10.616064 | 13.613797 | 12.613093 | 12.178542 | 13.105914 | 12.000647 | 12.133824 | 12.809492 | 11.58498 | 11.818344 | 11.466954 | 12.568174 | 11.927487 |
hep-th/9611183 | Bernard Piette | B. Piette and W.J. Zakrzewski | Localized Solutions in a 2 Dimensional Landau-Lifshitz Model | plain tex : 14 pages, 9 Postscript figures, uses epsf.tex | Physica D119 (1998) 314-326 | 10.1016/S0167-2789(98)00084-0 | DTP-96/47 | hep-th | null | We demonstrate the existence of stable time dependent solutions of the
Landau-Lifshitz model with a constant external magnetic field. We find such
solutions in all topological sectors, including N=0. We discuss some of their
properties.
| [
{
"created": "Fri, 22 Nov 1996 11:01:31 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Piette",
"B.",
""
],
[
"Zakrzewski",
"W. J.",
""
]
] | We demonstrate the existence of stable time dependent solutions of the Landau-Lifshitz model with a constant external magnetic field. We find such solutions in all topological sectors, including N=0. We discuss some of their properties. | 11.417397 | 10.050563 | 9.869479 | 8.727333 | 9.730796 | 8.928325 | 9.196178 | 8.979973 | 8.104979 | 11.901206 | 9.601944 | 9.41398 | 9.306245 | 9.427916 | 9.264095 | 9.053973 | 9.247589 | 9.004479 | 8.952188 | 9.550875 | 9.309583 |
1410.2879 | Dimitrios Zoakos | Veselin G. Filev, Dimitrios Zoakos | Multiple backreacted flavour branes | 16 pages, 4 figures | null | 10.1007/JHEP12(2014)186 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a novel supergravity background holographically dual to the
flavoured N=1 Supersymmetric Yang-Mills theory. We consider flavours of
different masses that produce spherical cavities with radii corresponding to
the quark masses. The positive beta function blows at some large radial
distance corresponding t... | [
{
"created": "Fri, 10 Oct 2014 19:44:33 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Filev",
"Veselin G.",
""
],
[
"Zoakos",
"Dimitrios",
""
]
] | We construct a novel supergravity background holographically dual to the flavoured N=1 Supersymmetric Yang-Mills theory. We consider flavours of different masses that produce spherical cavities with radii corresponding to the quark masses. The positive beta function blows at some large radial distance corresponding to ... | 18.730185 | 18.978086 | 19.745293 | 17.291763 | 18.781458 | 17.708258 | 17.663969 | 16.953283 | 16.224905 | 22.415483 | 15.741652 | 18.080931 | 18.075457 | 17.92506 | 17.818264 | 16.900898 | 16.835747 | 16.277813 | 17.206514 | 17.804962 | 16.9816 |
1008.2636 | Ofer Aharony | Ofer Aharony and Matan Field | On the effective theory of long open strings | 51 pages, JHEP format. v2: added references | JHEP 1101:065,2011 | 10.1007/JHEP01(2011)065 | WIS/10/10-AUG-DPPA | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the general low-energy effective action on long open strings, such
as confining strings in pure gauge theories. Using Lorentz invariance, we find
that for a string of length R, the leading deviation from the Nambu-Goto energy
levels generically occurs at order 1/R^4 (including a correction to the ground
stat... | [
{
"created": "Mon, 16 Aug 2010 12:38:56 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Nov 2010 12:19:52 GMT",
"version": "v2"
}
] | 2011-03-07 | [
[
"Aharony",
"Ofer",
""
],
[
"Field",
"Matan",
""
]
] | We study the general low-energy effective action on long open strings, such as confining strings in pure gauge theories. Using Lorentz invariance, we find that for a string of length R, the leading deviation from the Nambu-Goto energy levels generically occurs at order 1/R^4 (including a correction to the ground state ... | 6.973697 | 6.984914 | 7.554956 | 6.757383 | 6.5299 | 6.609195 | 6.550948 | 6.876228 | 6.688818 | 7.717836 | 6.355571 | 6.629316 | 7.322608 | 6.620945 | 6.855172 | 6.616623 | 6.567102 | 6.67572 | 6.667932 | 7.180757 | 6.639998 |
1605.08337 | Gabi Zafrir | Gabi Zafrir | Compactifications of 5d SCFTs with a twist | 59 pages, 47 figures; v2 references added; v3 references added +
minor revisions, version published in JHEP | null | 10.1007/JHEP01(2017)097 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the compactification of 5d SCFTs to 4d on a circle with a twist in a
discrete global symmetry element of these SCFTs. We present evidence that this
leads to various 4d N=2 isolated SCFTs. These include many known theories as
well as seemingly new ones. The known theories include the recently discovered
rank ... | [
{
"created": "Thu, 26 May 2016 15:38:47 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Jul 2016 15:24:16 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Apr 2017 12:14:58 GMT",
"version": "v3"
}
] | 2017-04-25 | [
[
"Zafrir",
"Gabi",
""
]
] | We study the compactification of 5d SCFTs to 4d on a circle with a twist in a discrete global symmetry element of these SCFTs. We present evidence that this leads to various 4d N=2 isolated SCFTs. These include many known theories as well as seemingly new ones. The known theories include the recently discovered rank 1 ... | 9.080144 | 7.636104 | 10.390843 | 7.980103 | 8.355783 | 8.700138 | 8.00172 | 8.19346 | 7.746073 | 11.319142 | 8.027141 | 8.266924 | 8.899483 | 8.294596 | 8.258642 | 8.377826 | 8.136351 | 8.371215 | 8.429042 | 8.96324 | 8.412053 |
1503.00712 | Hyun Seok Yang | Hyun Seok Yang | Emergent Spacetime and Cosmic Inflation | 56 pages, Published in the Special Issue <Mathematical Cosmology>:
Universe 10 (2024) 3, 150 | Universe 10 (2024) 3, 150 | 10.3390/universe10030150 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a novel background-independent framework for cosmic inflation,
starting with a matrix model. In this framework, inflation is portrayed as a
dynamic process responsible for the generation of both space and time. This
stands in contrast to conventional inflation, which is characterized as a mere
(exponential... | [
{
"created": "Mon, 2 Mar 2015 20:59:44 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Mar 2015 15:12:25 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Jun 2015 08:53:19 GMT",
"version": "v3"
},
{
"created": "Fri, 9 Sep 2016 14:57:46 GMT",
"version": "v4"
},
{
"crea... | 2024-03-22 | [
[
"Yang",
"Hyun Seok",
""
]
] | We present a novel background-independent framework for cosmic inflation, starting with a matrix model. In this framework, inflation is portrayed as a dynamic process responsible for the generation of both space and time. This stands in contrast to conventional inflation, which is characterized as a mere (exponential) ... | 13.054875 | 13.1595 | 12.939315 | 12.329724 | 13.042683 | 12.794353 | 12.475242 | 12.124244 | 12.199957 | 14.853486 | 11.57644 | 12.095355 | 12.418443 | 12.155692 | 12.092653 | 12.262184 | 12.22721 | 12.272959 | 12.235126 | 12.525012 | 11.920912 |
hep-th/9603198 | null | Chien-Hao Liu (University of Miami) | Lorentz Surfaces and Lorentzian CFT --- with an appendix on quantization
of string phase space | 60 pages, 22 Postscript figures | null | null | UMTG-190 | hep-th | null | The interest in string Hamiltonian system has recently been rekindled due to
its application to target-space duality. In this article, we explore another
direction it motivates. In Sec.\ 1, conformal symmetry and some algebraic
structures of the system that are related to interacting strings are discussed.
These lead... | [
{
"created": "Fri, 29 Mar 1996 23:00:58 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Liu",
"Chien-Hao",
"",
"University of Miami"
]
] | The interest in string Hamiltonian system has recently been rekindled due to its application to target-space duality. In this article, we explore another direction it motivates. In Sec.\ 1, conformal symmetry and some algebraic structures of the system that are related to interacting strings are discussed. These lead o... | 11.886056 | 12.407079 | 11.468543 | 11.143339 | 12.088672 | 12.193391 | 12.614099 | 12.194469 | 11.667898 | 12.346766 | 11.408706 | 11.370867 | 11.310391 | 11.2963 | 11.396869 | 11.694012 | 11.477275 | 11.354488 | 11.354554 | 11.494387 | 11.207912 |
hep-th/0412104 | Juan L. Manes | Juan L. Manes | Portrait of the String as a Random Walk | 17 pages. Typos corrected, 1 reference added | JHEP 0503 (2005) 070 | 10.1088/1126-6708/2005/03/070 | null | hep-th | null | In this paper we analyze a Rutherford type experiment where light probes are
inelastically scattered by an ensemble of excited closed strings, and use the
corresponding cross section to extract density-density correlators between
different pieces of the target string. We find a wide dynamical range where the
space-ti... | [
{
"created": "Fri, 10 Dec 2004 11:35:19 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Dec 2004 12:06:16 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Apr 2005 10:33:42 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Manes",
"Juan L.",
""
]
] | In this paper we analyze a Rutherford type experiment where light probes are inelastically scattered by an ensemble of excited closed strings, and use the corresponding cross section to extract density-density correlators between different pieces of the target string. We find a wide dynamical range where the space-time... | 14.669737 | 15.134997 | 14.940089 | 13.29307 | 15.828804 | 15.422073 | 14.211893 | 14.768015 | 14.122735 | 17.057608 | 13.237028 | 12.99229 | 14.012912 | 13.580676 | 13.283062 | 13.204609 | 13.17088 | 13.300076 | 12.990417 | 14.086702 | 13.091028 |
1507.03880 | V. Parameswaran Nair | Dimitra Karabali and V.P. Nair | Boundary Conditions as Dynamical Fields | 15 pages | Phys. Rev. D 92, 125003 (2015) | 10.1103/PhysRevD.92.125003 | CCNY-HEP 15/4 | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The possibility of treating boundary conditions in terms of a bilocal
dynamical field is formalized in terms of a boundary action. This allows for a
simple path-integral perturbation theory approach to physical effects such as
radiation from a time-dependent boundary. The nature of the action which
governs the dynami... | [
{
"created": "Tue, 14 Jul 2015 15:12:59 GMT",
"version": "v1"
}
] | 2015-12-09 | [
[
"Karabali",
"Dimitra",
""
],
[
"Nair",
"V. P.",
""
]
] | The possibility of treating boundary conditions in terms of a bilocal dynamical field is formalized in terms of a boundary action. This allows for a simple path-integral perturbation theory approach to physical effects such as radiation from a time-dependent boundary. The nature of the action which governs the dynamics... | 17.660189 | 12.958323 | 14.613076 | 14.019726 | 14.15378 | 13.838354 | 15.608307 | 13.835547 | 12.905732 | 16.320213 | 13.610474 | 13.732304 | 14.480173 | 14.132116 | 13.91616 | 13.832088 | 14.308359 | 13.701512 | 14.287388 | 14.842289 | 14.078865 |
hep-th/0507200 | Dietmar Klemm | Sergio L. Cacciatori, Marco M. Caldarelli, Alex Giacomini, Dietmar
Klemm and Diego S. Mansi | Chern-Simons formulation of three-dimensional gravity with torsion and
nonmetricity | 24 pages, uses JHEP3.cls. Published version | J.Geom.Phys. 56 (2006) 2523-2543 | 10.1016/j.geomphys.2006.01.006 | IFUM-839-FT | hep-th gr-qc | null | We consider various models of three-dimensional gravity with torsion or
nonmetricity (metric affine gravity), and show that they can be written as
Chern-Simons theories with suitable gauge groups. Using the groups ISO(2,1),
SL(2,C) or SL(2,R) x SL(2,R), and the fact that they admit two independent
coupling constants,... | [
{
"created": "Wed, 20 Jul 2005 16:32:42 GMT",
"version": "v1"
},
{
"created": "Mon, 29 Jan 2007 15:43:18 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Cacciatori",
"Sergio L.",
""
],
[
"Caldarelli",
"Marco M.",
""
],
[
"Giacomini",
"Alex",
""
],
[
"Klemm",
"Dietmar",
""
],
[
"Mansi",
"Diego S.",
""
]
] | We consider various models of three-dimensional gravity with torsion or nonmetricity (metric affine gravity), and show that they can be written as Chern-Simons theories with suitable gauge groups. Using the groups ISO(2,1), SL(2,C) or SL(2,R) x SL(2,R), and the fact that they admit two independent coupling constants, w... | 6.722356 | 6.981156 | 7.014503 | 6.703224 | 7.29463 | 6.849397 | 7.294197 | 6.753997 | 6.646059 | 7.735811 | 6.739815 | 6.553267 | 6.67611 | 6.650795 | 6.548044 | 6.628273 | 6.692007 | 6.422999 | 6.592316 | 6.790886 | 6.440886 |
1605.02313 | Andrei Mironov | A. Mironov, A. Morozov, An. Morozov and A. Sleptsov | HOMFLY polynomials in representation [3,1] for 3-strand braids | 21 pages | Journal of High Energy Physics, 2016 (2016) 134 | 10.1007/JHEP09(2016)134 | FIAN/TD-08/16; IITP/TH-05/16; ITEP/TH-04/16 | hep-th math.GT math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper is a new step in the project of systematic description of colored
knot polynomials started in arXiv:1506.00339. In this paper, we managed to
explicitly find the inclusive Racah matrix, i.e. the whole set of mixing
matrices in channels R^3->Q with all possible Q, for R=[3,1]. The calculation
is made possibl... | [
{
"created": "Sun, 8 May 2016 11:53:09 GMT",
"version": "v1"
}
] | 2016-09-28 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
],
[
"Morozov",
"An.",
""
],
[
"Sleptsov",
"A.",
""
]
] | This paper is a new step in the project of systematic description of colored knot polynomials started in arXiv:1506.00339. In this paper, we managed to explicitly find the inclusive Racah matrix, i.e. the whole set of mixing matrices in channels R^3->Q with all possible Q, for R=[3,1]. The calculation is made possible ... | 20.405035 | 11.306282 | 20.917408 | 14.00546 | 12.946208 | 12.58229 | 13.44494 | 14.191118 | 15.681029 | 24.941782 | 15.086611 | 17.244802 | 20.420681 | 18.524715 | 17.884638 | 18.600983 | 18.890209 | 17.802626 | 18.585157 | 21.097731 | 18.731573 |
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