id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0212129 | Ufuk Kayserilioglu | M. Arik, S. Gun, A. Yildiz | Invariance quantum group of the fermionic oscillator | 7 A4 pages | Eur.Phys.J.C27:453-455,2003 | 10.1140/epjc/s2002-01097-x | null | hep-th | null | The fermionic oscillator defined by the algebraic relations cc^*+c^*c=1 and
c^{2}=0 admits the homogeneous group O(2) as its invariance group. We show
that, the structure of the inhomogeneous invariance group of this oscillator is
a quantum group.
| [
{
"created": "Wed, 11 Dec 2002 15:38:20 GMT",
"version": "v1"
}
] | 2011-09-13 | [
[
"Arik",
"M.",
""
],
[
"Gun",
"S.",
""
],
[
"Yildiz",
"A.",
""
]
] | The fermionic oscillator defined by the algebraic relations cc^*+c^*c=1 and c^{2}=0 admits the homogeneous group O(2) as its invariance group. We show that, the structure of the inhomogeneous invariance group of this oscillator is a quantum group. | 11.203069 | 11.558367 | 10.885863 | 10.145367 | 12.083038 | 12.21036 | 9.861536 | 11.840608 | 9.757843 | 12.933331 | 9.931604 | 10.523218 | 10.342936 | 9.950489 | 9.6251 | 9.596089 | 9.530881 | 10.375638 | 10.433836 | 10.800042 | 10.031321 |
1712.05011 | Tim Morris Prof | Kevin Falls and Tim R. Morris | Conformal anomaly from gauge fields without gauge fixing | 24 pages | Phys. Rev. D 97, 065013 (2018) | 10.1103/PhysRevD.97.065013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how the Weyl anomaly generated by gauge fields, can be computed from
manifestly gauge invariant and diffeomorphism invariant exact renormalization
group equations, without having to fix the gauge at any stage. Regularisation
is provided by covariant higher derivatives and by embedding the Maxwell field
into a... | [
{
"created": "Wed, 13 Dec 2017 21:18:49 GMT",
"version": "v1"
}
] | 2018-03-28 | [
[
"Falls",
"Kevin",
""
],
[
"Morris",
"Tim R.",
""
]
] | We show how the Weyl anomaly generated by gauge fields, can be computed from manifestly gauge invariant and diffeomorphism invariant exact renormalization group equations, without having to fix the gauge at any stage. Regularisation is provided by covariant higher derivatives and by embedding the Maxwell field into a s... | 10.071444 | 8.391725 | 11.47133 | 9.273063 | 9.38091 | 9.569561 | 9.267305 | 8.857338 | 8.482155 | 10.334232 | 8.982973 | 9.152451 | 10.052996 | 9.145947 | 9.16282 | 9.409589 | 8.904879 | 9.31429 | 9.296346 | 9.680338 | 8.933848 |
1601.02203 | Shin'ichi Nojiri | Shin'ichi Nojiri | Some solutions for one of the cosmological constant problems | LaTeX 9 pages, references are added, the version to appear in
Mod.Phys.Lett.A | null | 10.1142/S0217732316502138 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose several covariant models which may solve one of the problems in
the cosmological constant. One of the model can be regarded as an extension of
sequestering model. Other models could be regarded as extensions of the
covariant formulation of the unimodular gravity. The contributions to the
vacuum energy from... | [
{
"created": "Sun, 10 Jan 2016 12:06:42 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Jan 2016 12:56:18 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Jul 2016 11:25:44 GMT",
"version": "v3"
},
{
"created": "Sat, 15 Oct 2016 06:46:51 GMT",
"version": "v4"
},
{
"cr... | 2016-11-10 | [
[
"Nojiri",
"Shin'ichi",
""
]
] | We propose several covariant models which may solve one of the problems in the cosmological constant. One of the model can be regarded as an extension of sequestering model. Other models could be regarded as extensions of the covariant formulation of the unimodular gravity. The contributions to the vacuum energy from t... | 9.680487 | 9.410944 | 9.962931 | 8.815055 | 9.180972 | 9.278689 | 10.035013 | 8.64683 | 9.058498 | 10.561962 | 9.325689 | 9.17039 | 9.484787 | 9.093816 | 9.034253 | 8.983144 | 9.116827 | 9.261187 | 9.012147 | 9.300764 | 9.192985 |
0804.3062 | Nikolaos Prezas | Nikolaos Prezas and Konstadinos Sfetsos | Supersymmetric moduli of the SU(2) x R linear dilaton background and
NS5-branes | 38 pages, 1 figure, 1 table; version to appear in JHEP | JHEP 0806:080,2008 | 10.1088/1126-6708/2008/06/080 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study several classes of marginal deformations of the conformal field
theory SU(2) x R. This theory describes the near-horizon region of a stack of
parallel and coincident NS5-branes and is related holographically to little
string theory. We investigate the supersymmetry properties of these
deformations and we elu... | [
{
"created": "Fri, 18 Apr 2008 17:11:08 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jun 2008 16:09:25 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Prezas",
"Nikolaos",
""
],
[
"Sfetsos",
"Konstadinos",
""
]
] | We study several classes of marginal deformations of the conformal field theory SU(2) x R. This theory describes the near-horizon region of a stack of parallel and coincident NS5-branes and is related holographically to little string theory. We investigate the supersymmetry properties of these deformations and we eluci... | 8.291531 | 8.173349 | 8.917791 | 7.753792 | 8.174592 | 8.477297 | 8.040316 | 7.781315 | 7.672709 | 9.457067 | 7.809337 | 7.827 | 8.395725 | 8.05178 | 8.313643 | 8.096051 | 8.039 | 7.934947 | 7.916812 | 8.271401 | 7.873951 |
1307.2816 | Dmitri Bykov | Dmitri Bykov | The K\"ahler metric of a blow-up | 38 pages, 3 figures | null | null | NORDITA-2013-46 | hep-th gr-qc math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | After a review of the general properties of holomorphic spheres in complex
surfaces we describe the local geometry in the vicinity of a CP^1 embedded with
a negative normal bundle. As a by-product, we build (asymptotically locally
hyperbolic) Kahler-Einstein metrics on the total spaces of the line bundles
O(-m), m >=... | [
{
"created": "Wed, 10 Jul 2013 15:00:56 GMT",
"version": "v1"
}
] | 2013-07-11 | [
[
"Bykov",
"Dmitri",
""
]
] | After a review of the general properties of holomorphic spheres in complex surfaces we describe the local geometry in the vicinity of a CP^1 embedded with a negative normal bundle. As a by-product, we build (asymptotically locally hyperbolic) Kahler-Einstein metrics on the total spaces of the line bundles O(-m), m >= 3... | 11.42825 | 11.977937 | 12.344102 | 10.815569 | 9.87684 | 11.524693 | 10.393782 | 11.089204 | 11.318322 | 15.006296 | 10.440561 | 10.516054 | 11.276729 | 10.423489 | 9.887142 | 10.210818 | 10.380696 | 10.722873 | 10.499198 | 11.200479 | 10.259877 |
2310.07457 | Nabin Bhatta | Nabin Bhatta, Djordje Minic, Tatsu Takeuchi | Constraints on a Generalization of Geometric Quantum Mechanics from
Neutrino and $B^0$-$\overline{B^0}$ Oscillations | 32 pages, 11 figures | JHEP 02 (2024) 031 | 10.1007/JHEP02(2024)031 | null | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Nambu Quantum Mechanics, proposed in Phys. Lett. B536, 305 (2002), is a
deformation of canonical Quantum Mechanics in which the manifold over which the
"phase" of an energy eigenstate time evolves is modified. This generalization
affects oscillation and interference phenomena through the introduction of two
deformati... | [
{
"created": "Wed, 11 Oct 2023 13:03:10 GMT",
"version": "v1"
}
] | 2024-05-02 | [
[
"Bhatta",
"Nabin",
""
],
[
"Minic",
"Djordje",
""
],
[
"Takeuchi",
"Tatsu",
""
]
] | Nambu Quantum Mechanics, proposed in Phys. Lett. B536, 305 (2002), is a deformation of canonical Quantum Mechanics in which the manifold over which the "phase" of an energy eigenstate time evolves is modified. This generalization affects oscillation and interference phenomena through the introduction of two deformation... | 10.515047 | 10.006334 | 8.79773 | 8.402085 | 10.92244 | 11.62648 | 11.046835 | 9.806822 | 9.118847 | 8.974932 | 10.185765 | 9.561093 | 8.96979 | 9.062378 | 9.528343 | 9.344498 | 8.942208 | 9.027893 | 9.428082 | 9.286626 | 9.83736 |
0808.2650 | Carlos Alfonso Martin Ballon Bayona | C. A. Ballon Bayona, Nelson R. F. Braga, Rafael D'Andrea | T-duality for open strings in the presence of backgrounds and
noncommutativity | In this V3: more references included. Version to appear in J.Phys.A | J.Phys.A42:315201,2009 | 10.1088/1751-8113/42/31/315201 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the effect of T-duality on noncommutativity. Starting with
open strings ending on a D2-brane wrapped on a $T^2$ torus in the presence of a
Kalb Ramond field, we consider Buscher transformations on the coordinates and
background. We find that the dual system is commutative. We also study
alternative tra... | [
{
"created": "Tue, 19 Aug 2008 20:15:54 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Nov 2008 19:22:06 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Jul 2009 20:37:02 GMT",
"version": "v3"
}
] | 2010-05-28 | [
[
"Bayona",
"C. A. Ballon",
""
],
[
"Braga",
"Nelson R. F.",
""
],
[
"D'Andrea",
"Rafael",
""
]
] | We investigate the effect of T-duality on noncommutativity. Starting with open strings ending on a D2-brane wrapped on a $T^2$ torus in the presence of a Kalb Ramond field, we consider Buscher transformations on the coordinates and background. We find that the dual system is commutative. We also study alternative trans... | 8.679778 | 6.631927 | 9.879892 | 7.162725 | 7.316711 | 7.010613 | 6.999732 | 7.402113 | 6.543715 | 9.342952 | 6.610729 | 7.605876 | 8.210506 | 7.576097 | 7.509115 | 7.479866 | 7.504825 | 7.510989 | 7.426107 | 8.435419 | 7.286664 |
hep-th/0001019 | Israel Klich | I. Klich, J. Feinberg, A. Mann and M. Revzen | Casimir energy of a dilute dielectric ball with uniform velocity of
light at finite temperature | 15 pages, 1 figure | Phys.Rev. D62 (2000) 045017 | 10.1103/PhysRevD.62.045017 | null | hep-th cond-mat.stat-mech quant-ph | null | The Casimir energy, free energy and Casimir force are evaluated, at arbitrary
finite temperature, for a dilute dielectric ball with uniform velocity of light
inside the ball and in the surrounding medium. In particular, we investigate
the classical limit at high temperature. The Casimir force found is repulsive,
as i... | [
{
"created": "Wed, 5 Jan 2000 17:24:23 GMT",
"version": "v1"
},
{
"created": "Fri, 7 Jan 2000 21:44:19 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Klich",
"I.",
""
],
[
"Feinberg",
"J.",
""
],
[
"Mann",
"A.",
""
],
[
"Revzen",
"M.",
""
]
] | The Casimir energy, free energy and Casimir force are evaluated, at arbitrary finite temperature, for a dilute dielectric ball with uniform velocity of light inside the ball and in the surrounding medium. In particular, we investigate the classical limit at high temperature. The Casimir force found is repulsive, as in ... | 13.223878 | 9.261673 | 13.600075 | 9.528261 | 8.441839 | 9.255002 | 8.417643 | 8.663791 | 9.245774 | 14.915316 | 9.754083 | 10.087764 | 12.884273 | 10.95453 | 10.653519 | 9.947688 | 10.238555 | 10.451712 | 11.184718 | 12.23061 | 10.856665 |
hep-th/9205062 | null | Supriya K. Kar, S. Pratik Khastgir and Gautam Sengupta | Four Dimensional Stringy Black Membrane | 13 pages | Phys.Rev. D47 (1993) 3643-3646 | 10.1103/PhysRevD.47.3643 | IP/BBSR/92-35 | hep-th | null | An exact conformal field theory describing a four dimensional singular string
background is obtained by chiral gauging a $U(1)$ subgroup along with
translations in $R$ of an $SL(2,R)\times R$ Wess-Zumino-Witten model. It is
shown that the target space-time describes a four dimensional black membrane.
Furthermore vari... | [
{
"created": "Mon, 18 May 1992 15:53:17 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Kar",
"Supriya K.",
""
],
[
"Khastgir",
"S. Pratik",
""
],
[
"Sengupta",
"Gautam",
""
]
] | An exact conformal field theory describing a four dimensional singular string background is obtained by chiral gauging a $U(1)$ subgroup along with translations in $R$ of an $SL(2,R)\times R$ Wess-Zumino-Witten model. It is shown that the target space-time describes a four dimensional black membrane. Furthermore variou... | 13.279987 | 9.765319 | 12.510788 | 9.696685 | 10.665164 | 10.44777 | 10.434811 | 9.034239 | 9.345428 | 14.286403 | 9.990102 | 10.574689 | 11.396646 | 9.758759 | 10.42996 | 10.015149 | 10.204524 | 10.230654 | 10.305401 | 10.991866 | 10.276037 |
hep-th/0312098 | David Kutasov | D. Kutasov | New Results on the "$a$-theorem" in Four Dimensional Supersymmetric
Field Theory | 28 pages; harvmac | null | null | null | hep-th | null | In four dimensional N=1 supersymmetric field theory it is often the case that
the $U(1)_R$ current that becomes part of the superconformal algebra at the
infrared fixed point is conserved throughout the renormalization group (RG)
flow. We show that when that happens, the central charge $a$ decreases under RG
flow. Th... | [
{
"created": "Tue, 9 Dec 2003 21:23:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Kutasov",
"D.",
""
]
] | In four dimensional N=1 supersymmetric field theory it is often the case that the $U(1)_R$ current that becomes part of the superconformal algebra at the infrared fixed point is conserved throughout the renormalization group (RG) flow. We show that when that happens, the central charge $a$ decreases under RG flow. The ... | 7.264158 | 6.966465 | 7.526465 | 6.184306 | 6.118087 | 6.468096 | 6.249444 | 6.444046 | 6.56921 | 7.655935 | 6.304496 | 6.34367 | 6.865614 | 6.583194 | 6.260677 | 6.233546 | 6.39767 | 6.386532 | 6.472538 | 6.964129 | 6.376522 |
2404.03959 | Stam Nicolis | Stam Nicolis | Flavor and Fluctuations | 7 pages LaTeX, uses pos.sty and JHEP.bst. Contribution to the Corfu
Summer Institute 2023,"School and Workshops on Elementary Particle Physics
and Gravity" (CORFU2023) | null | null | null | hep-th cond-mat.stat-mech hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Parisi-Sourlas approach to supersymmetry implies that, in spacetime
dimensions greater than 1, there is a constraint on the minimal number of
flavors, in order for a field theory to define a closed system. In particular,
this number is greater than 1. This does not preclude that supersymmetry can be
broken, howev... | [
{
"created": "Fri, 5 Apr 2024 08:49:57 GMT",
"version": "v1"
}
] | 2024-04-08 | [
[
"Nicolis",
"Stam",
""
]
] | The Parisi-Sourlas approach to supersymmetry implies that, in spacetime dimensions greater than 1, there is a constraint on the minimal number of flavors, in order for a field theory to define a closed system. In particular, this number is greater than 1. This does not preclude that supersymmetry can be broken, however... | 10.728501 | 11.508307 | 11.614548 | 10.17067 | 10.396017 | 10.822217 | 11.118695 | 10.507155 | 10.040494 | 11.621142 | 10.593342 | 10.061358 | 9.959841 | 9.699845 | 9.875793 | 9.688972 | 9.521713 | 9.796917 | 9.918374 | 10.002468 | 10.189315 |
2104.02833 | Roldao da Rocha | A. J. Ferreira-Martins, R. da Rocha | Generalized Navier-Stokes equations and soft hairy horizons in
fluid/gravity correspondence | 21 pages | Nucl. Phys. B 973 (2021) 115603 | 10.1016/j.nuclphysb.2021.115603 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The fluid/gravity correspondence establishes how gravitational dynamics, as
dictated by Einstein's field equations, are related to the fluid dynamics,
governed by the relativistic Navier-Stokes equations. In this work the
correspondence is extended, where the duality between incompressible fluids and
gravitational ba... | [
{
"created": "Wed, 7 Apr 2021 00:15:32 GMT",
"version": "v1"
},
{
"created": "Sun, 7 Nov 2021 17:40:05 GMT",
"version": "v2"
}
] | 2021-11-09 | [
[
"Ferreira-Martins",
"A. J.",
""
],
[
"da Rocha",
"R.",
""
]
] | The fluid/gravity correspondence establishes how gravitational dynamics, as dictated by Einstein's field equations, are related to the fluid dynamics, governed by the relativistic Navier-Stokes equations. In this work the correspondence is extended, where the duality between incompressible fluids and gravitational back... | 10.623077 | 9.273614 | 10.883208 | 8.762698 | 9.90064 | 8.936172 | 9.978912 | 10.047903 | 8.939737 | 10.540036 | 10.095984 | 9.843529 | 10.466873 | 9.634045 | 9.863558 | 9.704012 | 9.950878 | 9.900631 | 9.90901 | 10.036153 | 9.514599 |
1905.02416 | Dmitriy Pavshinkin | D. Pavshinkin | Grassmannian and Flag sigma models on interval: phase structure and
L-dependence | 13 pages, 1 figure. The generalization of the previous results to
periodic, periodic twisted and unmixed DD, NN boundaries is discussed in
Conclusion | J. High Energ. Phys. 2019, 75 (2019) | 10.1007/JHEP12(2019)075 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the two-dimensional Grassmannian $SU(N)/S(U(N-2)\times U(2))$ and
the flag $SU(N)/S(U(N-2)\times U(1)\times U(1))$ sigma models on a finite
interval and construct analytical solutions of gap equations in the large N
limit. We show that the flag model admits a homogeneous solution for `mixed'
Dirichlet-Neum... | [
{
"created": "Tue, 7 May 2019 08:56:47 GMT",
"version": "v1"
},
{
"created": "Wed, 8 May 2019 16:01:03 GMT",
"version": "v2"
},
{
"created": "Sat, 17 Aug 2019 11:09:03 GMT",
"version": "v3"
}
] | 2019-12-17 | [
[
"Pavshinkin",
"D.",
""
]
] | We discuss the two-dimensional Grassmannian $SU(N)/S(U(N-2)\times U(2))$ and the flag $SU(N)/S(U(N-2)\times U(1)\times U(1))$ sigma models on a finite interval and construct analytical solutions of gap equations in the large N limit. We show that the flag model admits a homogeneous solution for `mixed' Dirichlet-Neuman... | 8.845781 | 9.172684 | 9.839461 | 8.913335 | 8.866546 | 9.43146 | 8.774024 | 8.733159 | 8.272321 | 9.855666 | 8.603454 | 8.429733 | 8.955355 | 8.40867 | 8.356407 | 8.460208 | 8.620078 | 8.27692 | 8.430871 | 8.880525 | 8.328012 |
1905.10800 | Mohammad R. Garousi | Mohammad R. Garousi, Hamid Razaghian | Minimal independent couplings at order $\alpha'^2$ | 17 pages, Latex file, no figure | Phys. Rev. D 100, 106007 (2019) | 10.1103/PhysRevD.100.106007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using field redefinitions and Bianchi identities on the general form of the
effective action for metric, $B$-field and dilaton, we have found that the
minimum number of independent couplings at order $\alpha'^2$ is 60. We write
these couplings in two different schemes in the string frame. In the first
scheme, each co... | [
{
"created": "Sun, 26 May 2019 13:05:13 GMT",
"version": "v1"
}
] | 2019-11-20 | [
[
"Garousi",
"Mohammad R.",
""
],
[
"Razaghian",
"Hamid",
""
]
] | Using field redefinitions and Bianchi identities on the general form of the effective action for metric, $B$-field and dilaton, we have found that the minimum number of independent couplings at order $\alpha'^2$ is 60. We write these couplings in two different schemes in the string frame. In the first scheme, each coup... | 5.920583 | 5.045753 | 6.051306 | 5.384084 | 5.410748 | 5.445373 | 5.17007 | 5.04476 | 5.030647 | 6.286309 | 5.316326 | 5.528096 | 5.725787 | 5.411257 | 5.48025 | 5.377786 | 5.553292 | 5.381325 | 5.485882 | 5.703036 | 5.549085 |
0708.4077 | Yi Wang | Miao Li, Yi Wang | Typicality, Freak Observers and the Anthropic Principle of Existence | 12 pages, 2 figures | null | null | null | hep-th astro-ph gr-qc | null | We propose an alternative anthropic probability for calculating the
probabilities in eternal inflation. This anthropic probability follows
naturally from the weak anthropic principle, and does not suffer the freak
observer or the typicality problems. The problem that our observed cosmological
constant is not at the p... | [
{
"created": "Thu, 30 Aug 2007 07:41:33 GMT",
"version": "v1"
}
] | 2007-08-31 | [
[
"Li",
"Miao",
""
],
[
"Wang",
"Yi",
""
]
] | We propose an alternative anthropic probability for calculating the probabilities in eternal inflation. This anthropic probability follows naturally from the weak anthropic principle, and does not suffer the freak observer or the typicality problems. The problem that our observed cosmological constant is not at the pea... | 14.221232 | 14.246427 | 15.461931 | 12.663223 | 13.299309 | 14.49017 | 13.762855 | 14.808794 | 13.175783 | 15.671229 | 13.938244 | 13.522421 | 13.956141 | 13.874924 | 13.654696 | 14.608404 | 13.961701 | 14.305517 | 13.599244 | 14.687713 | 13.211405 |
hep-th/9203083 | Jim Horne | James H. Horne and Gary T. Horowitz | Rotating Dilaton Black Holes | 14 pages | Phys.Rev.D46:1340-1346,1992 | 10.1103/PhysRevD.46.1340 | null | hep-th | null | It is shown that an arbitrarily small amount of angular momentum can
qualitatively change the properties of extremal charged black holes coupled to
a dilaton. In addition, the gyromagnetic ratio of these black holes is computed
and an exact rotating black string solution is presented.
| [
{
"created": "Mon, 30 Mar 1992 17:14:10 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Apr 1992 22:53:08 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Horne",
"James H.",
""
],
[
"Horowitz",
"Gary T.",
""
]
] | It is shown that an arbitrarily small amount of angular momentum can qualitatively change the properties of extremal charged black holes coupled to a dilaton. In addition, the gyromagnetic ratio of these black holes is computed and an exact rotating black string solution is presented. | 9.596044 | 7.572543 | 6.267278 | 7.025283 | 7.498728 | 6.448622 | 8.36892 | 6.206402 | 8.073208 | 6.690925 | 7.615421 | 7.540505 | 7.521577 | 7.548236 | 7.497832 | 7.512442 | 7.475199 | 7.053671 | 7.675632 | 7.535745 | 7.850412 |
2110.15256 | Pulkit Agarwal | Pulkit Agarwal, Richard C. Brower, Timothy G. Raben and Chung-I Tan | Application of Lorentzian CFT Principal Series Representation to Near
Forward Scattering | null | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | We present a discussion on recent progress in high energy diffraction from
the perspective of AdS/CFT, through which a unified treatment for both
perturbative and nonperturbative Pomeron emerges. By working with Unitary
Irreducible Representation of Conformal group, a frame is provided in extending
AdS/CFT to both fo... | [
{
"created": "Thu, 28 Oct 2021 16:14:07 GMT",
"version": "v1"
}
] | 2021-10-29 | [
[
"Agarwal",
"Pulkit",
""
],
[
"Brower",
"Richard C.",
""
],
[
"Raben",
"Timothy G.",
""
],
[
"Tan",
"Chung-I",
""
]
] | We present a discussion on recent progress in high energy diffraction from the perspective of AdS/CFT, through which a unified treatment for both perturbative and nonperturbative Pomeron emerges. By working with Unitary Irreducible Representation of Conformal group, a frame is provided in extending AdS/CFT to both forw... | 18.228539 | 22.071594 | 18.742041 | 16.895102 | 18.924297 | 20.879391 | 22.366364 | 19.57637 | 17.409012 | 18.334856 | 19.533632 | 18.406464 | 18.291229 | 17.214996 | 17.101019 | 18.527233 | 17.258623 | 17.662546 | 17.473778 | 18.468687 | 18.163967 |
2401.01617 | Tinglong Feng | Tinglong Feng | Holographic Approach to Neutron Stars | 10 pages, 3 figures | null | null | null | hep-th astro-ph.HE | http://creativecommons.org/licenses/by/4.0/ | In this article we explore the holographic approach to neutron stars in the
realm of Quantum Field Theory (QFT). We delve into the structures of neutron
stars, emphasizing the application of the AdS/CFT duality in modeling them. We
discuss both "bottom-up" and "top-down" holographic models, comparing their
prediction... | [
{
"created": "Wed, 3 Jan 2024 08:38:29 GMT",
"version": "v1"
}
] | 2024-01-04 | [
[
"Feng",
"Tinglong",
""
]
] | In this article we explore the holographic approach to neutron stars in the realm of Quantum Field Theory (QFT). We delve into the structures of neutron stars, emphasizing the application of the AdS/CFT duality in modeling them. We discuss both "bottom-up" and "top-down" holographic models, comparing their predictions ... | 9.51929 | 8.717731 | 8.005701 | 8.283047 | 9.156661 | 8.440811 | 8.57355 | 8.778613 | 8.108413 | 8.799182 | 7.669928 | 8.942273 | 8.547224 | 8.484928 | 8.432205 | 8.260519 | 8.41022 | 8.099285 | 8.271395 | 8.304136 | 8.218523 |
hep-th/9805194 | Liu Qing-Jun | Jun-Chen Su | Massive Gauge Field Theory Without Higgs Mechanism IV. Illustration of
Unitarsity | 30 pages, latex, 9 figures | null | null | null | hep-th | null | To illustrate the unitarity of the massive gauge field theory described in
the foregoing papers, we calculate the scattering amplitudes up to the fourth
order of perturbation by the optical theorem and the Landau-Cutkosky rule. In
the calculations, it is shown that for a given process, if all the diagrams are
taken i... | [
{
"created": "Thu, 28 May 1998 02:31:15 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Jan 1999 08:35:54 GMT",
"version": "v2"
},
{
"created": "Mon, 8 Mar 1999 02:57:00 GMT",
"version": "v3"
},
{
"created": "Tue, 29 Nov 2005 10:31:03 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Su",
"Jun-Chen",
""
]
] | To illustrate the unitarity of the massive gauge field theory described in the foregoing papers, we calculate the scattering amplitudes up to the fourth order of perturbation by the optical theorem and the Landau-Cutkosky rule. In the calculations, it is shown that for a given process, if all the diagrams are taken int... | 7.703494 | 7.915761 | 8.288237 | 7.824496 | 7.68535 | 7.590016 | 7.568587 | 7.176459 | 7.44971 | 8.243577 | 7.471596 | 7.287766 | 7.278334 | 7.109976 | 7.278006 | 7.400807 | 7.151541 | 7.315804 | 7.189744 | 7.31151 | 7.271328 |
0803.4273 | Toby Wiseman | Simon Catterall and Toby Wiseman | Black hole thermodynamics from simulations of lattice Yang-Mills theory | 4 pages, 4 figures | Phys.Rev.D78:041502,2008 | 10.1103/PhysRevD.78.041502 | null | hep-th gr-qc hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report on lattice simulations of 16 supercharge SU(N) Yang-Mills quantum
mechanics in the 't Hooft limit. Maldacena duality conjectures that in this
limit the theory is dual to IIA string theory, and in particular that the
behavior of the thermal theory at low temperature is equivalent to that of
certain black hol... | [
{
"created": "Sat, 29 Mar 2008 15:57:18 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Catterall",
"Simon",
""
],
[
"Wiseman",
"Toby",
""
]
] | We report on lattice simulations of 16 supercharge SU(N) Yang-Mills quantum mechanics in the 't Hooft limit. Maldacena duality conjectures that in this limit the theory is dual to IIA string theory, and in particular that the behavior of the thermal theory at low temperature is equivalent to that of certain black holes... | 8.414507 | 8.747265 | 9.840542 | 8.529002 | 9.280289 | 8.4108 | 8.882677 | 7.853467 | 8.427661 | 9.65143 | 8.08434 | 8.137069 | 8.508891 | 7.950708 | 8.342116 | 8.028962 | 8.331634 | 8.084242 | 8.027392 | 8.824389 | 8.150428 |
1812.02254 | Dalimil Mazac | Dalimil Mazac | A Crossing-Symmetric OPE Inversion Formula | Mathematica notebook included, v2: references added | null | 10.1007/JHEP06(2019)082 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a Lorentzian OPE inversion formula for the principal series of
$sl(2,\mathbb{R})$. Unlike the standard Lorentzian inversion formula in higher
dimensions, the formula described here only applies to fully crossing-symmetric
four-point functions and makes crossing symmetry manifest. In particular,
inverting a ... | [
{
"created": "Wed, 5 Dec 2018 22:27:22 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jan 2019 10:03:21 GMT",
"version": "v2"
}
] | 2019-07-24 | [
[
"Mazac",
"Dalimil",
""
]
] | We derive a Lorentzian OPE inversion formula for the principal series of $sl(2,\mathbb{R})$. Unlike the standard Lorentzian inversion formula in higher dimensions, the formula described here only applies to fully crossing-symmetric four-point functions and makes crossing symmetry manifest. In particular, inverting a si... | 9.728593 | 9.655692 | 11.880214 | 9.397739 | 9.897943 | 9.796121 | 9.74685 | 9.168658 | 9.476915 | 13.526546 | 9.309827 | 8.982516 | 10.015846 | 9.312944 | 9.56518 | 9.460844 | 9.199844 | 9.108007 | 9.217905 | 9.707515 | 8.755109 |
hep-th/9211068 | German Sierra | Cesar Gomez and German Sierra | A brief history of hidden quantum symmetries in Conformal Field Theories | 20 pages, Latex, IMAFF-92 | null | null | null | hep-th | null | We review briefly a stream of ideas concerning the role of quantum groups as
hidden symmetries in conformal field theories, paying particular attention to
the field theoretical representations of quantum groups based on Coulomb gas
methods. An extensive bibliography is also included.
| [
{
"created": "Mon, 16 Nov 1992 15:55:34 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Gomez",
"Cesar",
""
],
[
"Sierra",
"German",
""
]
] | We review briefly a stream of ideas concerning the role of quantum groups as hidden symmetries in conformal field theories, paying particular attention to the field theoretical representations of quantum groups based on Coulomb gas methods. An extensive bibliography is also included. | 15.89586 | 11.221675 | 15.402822 | 11.665758 | 11.732224 | 12.180101 | 12.583705 | 12.476375 | 11.502282 | 14.435448 | 11.920821 | 12.524526 | 14.342899 | 12.235865 | 12.430617 | 12.636639 | 11.882796 | 12.49953 | 13.147667 | 14.09735 | 12.308695 |
hep-th/9912038 | Taejin Lee | Taejin Lee | Noncommutative Dirac-Born-Infeld Action for D-brane | 13 Pages, RevTex, added references | Phys.Lett.B478:313-319,2000 | 10.1016/S0370-2693(00)00248-3 | KIAS-P99109 | hep-th | null | We derive the noncommutative Dirac-Born-Infeld action for the $D$-brane,
which governs dynamics of $D$-brane with a NS-NS $B$-field in the low energy
regime. Depending on some details of the path integral prescriptions, both
ordinary Dirac-Born-Infeld action and noncommutative one can be obtained by
evaluating the sa... | [
{
"created": "Mon, 6 Dec 1999 08:02:23 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Dec 1999 07:22:06 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Lee",
"Taejin",
""
]
] | We derive the noncommutative Dirac-Born-Infeld action for the $D$-brane, which governs dynamics of $D$-brane with a NS-NS $B$-field in the low energy regime. Depending on some details of the path integral prescriptions, both ordinary Dirac-Born-Infeld action and noncommutative one can be obtained by evaluating the same... | 5.949782 | 5.037245 | 5.752902 | 5.087462 | 5.468228 | 5.180243 | 5.200456 | 5.111015 | 5.137187 | 6.34248 | 5.098793 | 5.291231 | 5.854679 | 5.289232 | 5.454533 | 5.414152 | 5.185918 | 5.252494 | 5.329636 | 5.522743 | 5.306406 |
hep-th/0201051 | Anzhong Wang | Anzhong Wang | Thick de Sitter 3-Branes, Dynamic Black Holes and Localization of
Gravity | the study of scalar perturbations and some relevant references have
been added. The most used definition for mass in de Sitter space has been
adopted | Phys.Rev.D66:024024,2002 | 10.1103/PhysRevD.66.024024 | null | hep-th gr-qc | null | The embedding of a thick de Sitter 3-brane into a five-dimensional bulk is
studied, assuming a scalar field with potential is present in the bulk. A class
of solutions is found in closed form that can represent a thick de Sitter
3-brane interpolating either between two dynamical black holes with a $R \times
S_{4}$ to... | [
{
"created": "Tue, 8 Jan 2002 21:07:13 GMT",
"version": "v1"
},
{
"created": "Wed, 8 May 2002 15:29:03 GMT",
"version": "v2"
},
{
"created": "Thu, 9 May 2002 23:42:47 GMT",
"version": "v3"
}
] | 2009-07-07 | [
[
"Wang",
"Anzhong",
""
]
] | The embedding of a thick de Sitter 3-brane into a five-dimensional bulk is studied, assuming a scalar field with potential is present in the bulk. A class of solutions is found in closed form that can represent a thick de Sitter 3-brane interpolating either between two dynamical black holes with a $R \times S_{4}$ topo... | 8.066914 | 6.63201 | 7.348533 | 6.882359 | 7.165063 | 6.698414 | 7.346608 | 6.426125 | 6.634234 | 8.059442 | 6.691576 | 7.268041 | 7.198111 | 7.095228 | 7.037683 | 7.025618 | 7.186734 | 6.881705 | 7.087619 | 7.273194 | 6.996713 |
hep-th/0411046 | Bruno Zumino | Bruno Zumino | Constraints and Casimirs for Superpoincare and Supertranslation Algebras
in various dimensions | 9 pages, pdf, talk given at the Pran Nath Fest, Northeastern
University, Boston, August 18-19, 2004 | null | 10.1142/9789812701756_0096 | null | hep-th | null | We describe, for arbitrary dimensions the construction of a covariant and
supersymmetric constraint for the massless Super Poincare' algebra and we show
that the constraint fixes uniquely the representation of the algebra. For the
case of finite mass and in the absence of central charges we discuss a similar
construc... | [
{
"created": "Wed, 3 Nov 2004 22:59:18 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Zumino",
"Bruno",
""
]
] | We describe, for arbitrary dimensions the construction of a covariant and supersymmetric constraint for the massless Super Poincare' algebra and we show that the constraint fixes uniquely the representation of the algebra. For the case of finite mass and in the absence of central charges we discuss a similar constructi... | 13.911356 | 11.839441 | 13.309078 | 11.719874 | 14.23193 | 11.447289 | 12.024335 | 11.819538 | 12.257349 | 14.409156 | 12.046258 | 12.030886 | 12.903665 | 11.902168 | 12.36689 | 12.582848 | 12.24554 | 12.166457 | 11.566814 | 13.495904 | 11.935051 |
0704.1990 | Eugenio R. Bezerra de Mello | J. Spinelly and E. R. Bezerra de Mello | Vacuum Polarization by a Magnetic Flux Tube at Finite Temperature in the
Cosmic String Spacetime | 16 pages, 1 figure | Int.J.Mod.Phys.D18:53-70,2009 | 10.1142/S0218271809014273 | null | hep-th gr-qc | null | In this paper we analyse the effect produced by the temperature in the vacuum
polarization associated with charged massless scalar field in the presence of
magnetic flux tube in the cosmic string spacetime. Three different
configurations of magnetic fields are taken into account: $(i)$ a homogeneous
field inside the ... | [
{
"created": "Mon, 16 Apr 2007 12:02:57 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Apr 2008 17:37:47 GMT",
"version": "v2"
}
] | 2009-03-24 | [
[
"Spinelly",
"J.",
""
],
[
"de Mello",
"E. R. Bezerra",
""
]
] | In this paper we analyse the effect produced by the temperature in the vacuum polarization associated with charged massless scalar field in the presence of magnetic flux tube in the cosmic string spacetime. Three different configurations of magnetic fields are taken into account: $(i)$ a homogeneous field inside the tu... | 8.322623 | 4.529143 | 8.226786 | 6.091845 | 5.728072 | 5.34639 | 5.470573 | 5.231291 | 5.289685 | 8.519958 | 5.653829 | 6.758567 | 8.08945 | 7.369584 | 7.129083 | 7.087753 | 7.052774 | 6.943188 | 7.242923 | 8.130548 | 7.417389 |
hep-th/9701036 | Yukinori Nagatani | Yukinori Nagatani (Nagoya University) | Dynamical Symmetry Breaking in Fractal Space | 28 pages, 5 figures, LaTeX with epsf macro | Phys.Rev. D56 (1997) 1239-1249 | 10.1103/PhysRevD.56.1239 | DPNU-96-61 | hep-th | null | We formulate field theories in fractal space and show the phase diagrams of
the coupling versus the fractal dimension for the dynamical symmetry breaking.
We first consider the 4-dimensional Gross-Neveu (GN) model in the
(4-d)-dimensional randomized Cantor space where the fermions are restricted to
a fractal space by... | [
{
"created": "Thu, 9 Jan 1997 18:32:56 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Nagatani",
"Yukinori",
"",
"Nagoya University"
]
] | We formulate field theories in fractal space and show the phase diagrams of the coupling versus the fractal dimension for the dynamical symmetry breaking. We first consider the 4-dimensional Gross-Neveu (GN) model in the (4-d)-dimensional randomized Cantor space where the fermions are restricted to a fractal space by t... | 9.451344 | 10.609943 | 10.212013 | 9.800858 | 10.663377 | 11.41758 | 9.892321 | 10.371597 | 9.988503 | 9.731994 | 9.57214 | 9.735263 | 9.853862 | 9.48116 | 9.751336 | 9.398621 | 9.809075 | 9.392093 | 9.526466 | 9.649469 | 9.23486 |
hep-th/9703021 | Murat Gunaydin | Murat Gunaydin | Seven Sphere and the Exceptional Nonlinear Superconformal Algebras | Talk given at the 30th International Symposium on the Theory of
Elementary Particles, Buckow, Germany (Aug. 27-31, 1996). 11 pages, latex
file | Nucl.Phys.Proc.Suppl.56B:70-75,1997 | 10.1016/S0920-5632(97)00311-3 | PSU-TH-180 (Dec. 1996) | hep-th | null | The realizations of the exceptional non-linear (quadratically generated, or
W-type) N=8 and N=7 superconformal algebras with Spin(7) and G_2 affine
symmetry currents are reviewed. Both the N=8 and N=7 algebras admit unitary
realizations in terms of a single boson and free fermions in 8 of Spin(7) and 7
of G_2, with t... | [
{
"created": "Mon, 3 Mar 1997 20:58:59 GMT",
"version": "v1"
}
] | 2011-02-09 | [
[
"Gunaydin",
"Murat",
""
]
] | The realizations of the exceptional non-linear (quadratically generated, or W-type) N=8 and N=7 superconformal algebras with Spin(7) and G_2 affine symmetry currents are reviewed. Both the N=8 and N=7 algebras admit unitary realizations in terms of a single boson and free fermions in 8 of Spin(7) and 7 of G_2, with the... | 6.426296 | 6.910262 | 7.447371 | 6.068882 | 6.691032 | 6.712801 | 6.780093 | 6.441505 | 6.46389 | 7.896103 | 6.435926 | 6.107299 | 6.828176 | 6.122733 | 6.06999 | 5.998964 | 6.290121 | 6.091759 | 6.241025 | 6.759217 | 6.085249 |
0705.2562 | Delia Schwartz-Perlov | Ken D. Olum and Delia Schwartz-Perlov | Anthropic prediction in a large toy landscape | 13 pages | JCAP0710:010,2007 | 10.1088/1475-7516/2007/10/010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The successful anthropic prediction of the cosmological constant depends
crucially on the assumption of a flat prior distribution. However, previous
calculations in simplified landscape models showed that the prior distribution
is staggered, suggesting a conflict with anthropic predictions. Here we
analytically calcu... | [
{
"created": "Thu, 17 May 2007 16:51:27 GMT",
"version": "v1"
},
{
"created": "Thu, 17 May 2007 20:00:13 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Oct 2019 17:11:47 GMT",
"version": "v3"
}
] | 2019-10-30 | [
[
"Olum",
"Ken D.",
""
],
[
"Schwartz-Perlov",
"Delia",
""
]
] | The successful anthropic prediction of the cosmological constant depends crucially on the assumption of a flat prior distribution. However, previous calculations in simplified landscape models showed that the prior distribution is staggered, suggesting a conflict with anthropic predictions. Here we analytically calcula... | 10.161246 | 9.277265 | 9.264219 | 8.787991 | 9.356594 | 8.594223 | 10.345429 | 9.105923 | 8.712007 | 9.425654 | 9.442483 | 9.1675 | 9.527373 | 9.110548 | 9.14611 | 9.221437 | 9.276166 | 9.142397 | 9.187122 | 9.284843 | 8.817422 |
0906.4814 | Andrew K. Waldron | D. Cherney, E. Latini and A. Waldron | BRST Detour Quantization | 43 pages, LaTeX, added references | J.Math.Phys.51:062302,2010 | 10.1063/1.3372732 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the BRST cohomologies of a class of constraint (super) Lie
algebras as detour complexes. By giving physical interpretations to the
components of detour complexes as gauge invariances, Bianchi identities and
equations of motion we obtain a large class of new gauge theories. The pivotal
new machinery is a tr... | [
{
"created": "Thu, 25 Jun 2009 23:24:06 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jul 2009 16:51:02 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Cherney",
"D.",
""
],
[
"Latini",
"E.",
""
],
[
"Waldron",
"A.",
""
]
] | We present the BRST cohomologies of a class of constraint (super) Lie algebras as detour complexes. By giving physical interpretations to the components of detour complexes as gauge invariances, Bianchi identities and equations of motion we obtain a large class of new gauge theories. The pivotal new machinery is a trea... | 17.18281 | 16.798735 | 18.134245 | 15.135531 | 17.325396 | 16.004618 | 16.987015 | 15.945831 | 16.415674 | 21.101675 | 15.718963 | 14.96974 | 16.611233 | 15.782886 | 15.858865 | 15.533531 | 15.586599 | 15.385204 | 15.573922 | 17.635826 | 15.203739 |
2311.14668 | Henrik Johansson | Lucile Cangemi, Marco Chiodaroli, Henrik Johansson, Alexander Ochirov,
Paolo Pichini and Evgeny Skvortsov | From higher-spin gauge interactions to Compton amplitudes for root-Kerr | 65p + appx., 1 figure | null | null | UUITP-35/23 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We develop massive higher-spin theory as a framework for describing dynamics
of rotating compact objects, such as Kerr black holes. In this paper, we
explore gauge interactions up to quartic order and corresponding Compton
amplitudes of higher-spin massive objects coupled to electromagnetism and
Yang-Mills theory. Th... | [
{
"created": "Fri, 24 Nov 2023 18:58:34 GMT",
"version": "v1"
}
] | 2023-11-27 | [
[
"Cangemi",
"Lucile",
""
],
[
"Chiodaroli",
"Marco",
""
],
[
"Johansson",
"Henrik",
""
],
[
"Ochirov",
"Alexander",
""
],
[
"Pichini",
"Paolo",
""
],
[
"Skvortsov",
"Evgeny",
""
]
] | We develop massive higher-spin theory as a framework for describing dynamics of rotating compact objects, such as Kerr black holes. In this paper, we explore gauge interactions up to quartic order and corresponding Compton amplitudes of higher-spin massive objects coupled to electromagnetism and Yang-Mills theory. Thei... | 14.099981 | 12.51317 | 15.14118 | 12.786884 | 12.459176 | 12.773218 | 12.378973 | 12.631699 | 12.440761 | 14.696918 | 12.905449 | 12.938583 | 13.453404 | 13.006783 | 12.69209 | 13.095747 | 13.101774 | 12.604947 | 13.062724 | 13.362561 | 12.715357 |
1405.3658 | Martin Sprenger | J. Bartels, V. Schomerus, M. Sprenger | Heptagon Amplitude in the Multi-Regge Regime | 14 pages | JHEP 1410 (2014) 67 | 10.1007/JHEP10(2014)067 | DESY 14-076 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As we have shown in previous work, the high energy limit of scattering
amplitudes in N=4 supersymmetric Yang-Mills theory corresponds to the infrared
limit of the 1-dimensional quantum integrable system that solves minimal area
problems in AdS5. This insight can be developed into a systematic algorithm to
compute the... | [
{
"created": "Wed, 14 May 2014 20:00:21 GMT",
"version": "v1"
}
] | 2014-11-11 | [
[
"Bartels",
"J.",
""
],
[
"Schomerus",
"V.",
""
],
[
"Sprenger",
"M.",
""
]
] | As we have shown in previous work, the high energy limit of scattering amplitudes in N=4 supersymmetric Yang-Mills theory corresponds to the infrared limit of the 1-dimensional quantum integrable system that solves minimal area problems in AdS5. This insight can be developed into a systematic algorithm to compute the s... | 7.349713 | 7.241641 | 8.435393 | 7.036445 | 7.273821 | 7.608411 | 7.353868 | 6.923394 | 7.189941 | 8.570834 | 7.057818 | 7.099248 | 7.631888 | 6.99689 | 7.142036 | 6.908581 | 6.808507 | 6.817018 | 6.832707 | 7.153807 | 7.092934 |
2308.11583 | Surajit Biswas | Nabamita Banerjee, Arindam Bhattacharjee, Surajit Biswas, Arpita
Mitra, Debangshu Mukherjee | $W(0,b)$ algebra and the dual theory of 3D asymptotically flat higher
spin gravity | 27+5 pages; 3 appendices | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | BMS algebra in three spacetime dimensions can be deformed into a two
parameter family of algebra known as $W(a,b)$ algebra. For $a=0$, we show that
other than $W(0,-1)$, no other $W(0,b)$ algebra admits a non-degenerate
bilinear and thus one can not have a Chern-Simons gauge theory formulation with
them. However, the... | [
{
"created": "Tue, 22 Aug 2023 17:32:24 GMT",
"version": "v1"
}
] | 2023-08-23 | [
[
"Banerjee",
"Nabamita",
""
],
[
"Bhattacharjee",
"Arindam",
""
],
[
"Biswas",
"Surajit",
""
],
[
"Mitra",
"Arpita",
""
],
[
"Mukherjee",
"Debangshu",
""
]
] | BMS algebra in three spacetime dimensions can be deformed into a two parameter family of algebra known as $W(a,b)$ algebra. For $a=0$, we show that other than $W(0,-1)$, no other $W(0,b)$ algebra admits a non-degenerate bilinear and thus one can not have a Chern-Simons gauge theory formulation with them. However, they ... | 7.463586 | 7.218313 | 7.78169 | 6.788511 | 7.260899 | 7.557748 | 7.421604 | 6.51152 | 7.060037 | 8.418596 | 6.626585 | 6.889441 | 6.901213 | 6.663245 | 6.907668 | 6.785882 | 6.724367 | 6.631382 | 6.69522 | 7.179509 | 6.564714 |
1903.04127 | Zhong-Ying Fan | Zhong-Ying Fan, Minyong Guo | Holographic complexity and thermodynamics of AdS black holes | minor revisions, references added, to apperear in PRD; 31 pages, 8
figures | Phys. Rev. D 100, 026016 (2019) | 10.1103/PhysRevD.100.026016 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we relate the complexity for a holographic state to a simple
gravitational object of which the growth rate at late times is equal to
temperature times black hole entropy. We show that if this is correct, the
thermodynamics of AdS black holes implies that for generic holographic states
dual to static Ad... | [
{
"created": "Mon, 11 Mar 2019 05:09:59 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Jun 2019 04:11:22 GMT",
"version": "v2"
}
] | 2019-07-31 | [
[
"Fan",
"Zhong-Ying",
""
],
[
"Guo",
"Minyong",
""
]
] | In this paper, we relate the complexity for a holographic state to a simple gravitational object of which the growth rate at late times is equal to temperature times black hole entropy. We show that if this is correct, the thermodynamics of AdS black holes implies that for generic holographic states dual to static AdS ... | 7.07487 | 6.357048 | 7.172814 | 6.261134 | 6.634719 | 6.59089 | 6.404843 | 6.630332 | 6.161595 | 7.390781 | 6.543342 | 6.48813 | 6.668642 | 6.427625 | 6.46212 | 6.59717 | 6.385361 | 6.585766 | 6.491371 | 6.865698 | 6.500093 |
1901.00662 | Ulf Lindstr\"om | M. Abou-Zeid, C.M. Hull, U. Lindstr\"om and M. Ro\v{c}ek | T-Duality in $(2,1)$ Superspace | 45 pages, Minor Corrections | null | 10.1007/JHEP06(2019)138 | Imperial-TP-2019-CH-01, UUITP-51/18, YITP-SB-18-31 | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find the T-duality transformation rules for 2-dimensional (2,1)
supersymmetric sigma-models in (2,1) superspace. Our results clarify certain
aspects of the (2,1) sigma model geometry relevant to the discussion of
T-duality. The complexified duality transformations we find are equivalent to
the usual Buscher dualit... | [
{
"created": "Thu, 3 Jan 2019 09:47:23 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Jan 2019 13:02:47 GMT",
"version": "v2"
}
] | 2022-10-12 | [
[
"Abou-Zeid",
"M.",
""
],
[
"Hull",
"C. M.",
""
],
[
"Lindström",
"U.",
""
],
[
"Roček",
"M.",
""
]
] | We find the T-duality transformation rules for 2-dimensional (2,1) supersymmetric sigma-models in (2,1) superspace. Our results clarify certain aspects of the (2,1) sigma model geometry relevant to the discussion of T-duality. The complexified duality transformations we find are equivalent to the usual Buscher duality ... | 6.680498 | 6.808396 | 8.069512 | 6.65043 | 6.284957 | 6.948732 | 6.870121 | 6.792076 | 6.488618 | 7.867134 | 6.532792 | 6.732978 | 7.44545 | 6.514578 | 6.30107 | 6.523584 | 6.598214 | 6.397913 | 6.573706 | 7.305283 | 6.547617 |
1711.05526 | Dave Dunbar | David C. Dunbar, John H. Godwin, Guy R. Jehu and Warren B. Perkins | Loop Amplitudes in an Extended Gravity Theory | 16 pages; some corrections to formulae and comments added | null | 10.1016/j.physletb.2018.02.046 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the $S$-matrix of gravity by the addition of the minimal
three-point amplitude or equivalently adding $R^3$ terms to the Lagrangian. We
demonstrate how Unitarity can be used to simply examine the renormalisability
of this theory and determine the $R^4$ counter-terms that arise at one-loop. We
find that the ... | [
{
"created": "Wed, 15 Nov 2017 12:30:38 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Feb 2018 14:12:03 GMT",
"version": "v2"
}
] | 2018-02-28 | [
[
"Dunbar",
"David C.",
""
],
[
"Godwin",
"John H.",
""
],
[
"Jehu",
"Guy R.",
""
],
[
"Perkins",
"Warren B.",
""
]
] | We extend the $S$-matrix of gravity by the addition of the minimal three-point amplitude or equivalently adding $R^3$ terms to the Lagrangian. We demonstrate how Unitarity can be used to simply examine the renormalisability of this theory and determine the $R^4$ counter-terms that arise at one-loop. We find that the co... | 8.532853 | 7.505052 | 8.485444 | 7.658888 | 8.536239 | 8.061352 | 8.089513 | 7.858919 | 7.781469 | 9.779341 | 7.687858 | 8.511348 | 8.28104 | 8.178891 | 8.391679 | 8.310691 | 8.405232 | 8.347552 | 8.144808 | 8.093418 | 8.103928 |
1707.02072 | Leron Borsten | L. Borsten and A. Marrani | A Kind of Magic | 38 pages. Reference added and minor corrections made | null | 10.1088/1361-6382/aa8fe2 | DIAS-STP-17-05, DFPD/2015/TH-23 | hep-th math-ph math.MP math.RA math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce the extended Freudenthal-Rosenfeld-Tits magic square based on
six algebras: the reals $\mathbb{R}$, complexes $\mathbb{C}$, ternions
$\mathbb{T}$, quaternions $\mathbb{H}$, sextonions $\mathbb{S}$ and octonions
$\mathbb{O}$. The ternionic and sextonionic rows/columns of the magic square
yield non-reducti... | [
{
"created": "Fri, 7 Jul 2017 08:18:57 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Jul 2017 17:11:49 GMT",
"version": "v2"
}
] | 2017-12-06 | [
[
"Borsten",
"L.",
""
],
[
"Marrani",
"A.",
""
]
] | We introduce the extended Freudenthal-Rosenfeld-Tits magic square based on six algebras: the reals $\mathbb{R}$, complexes $\mathbb{C}$, ternions $\mathbb{T}$, quaternions $\mathbb{H}$, sextonions $\mathbb{S}$ and octonions $\mathbb{O}$. The ternionic and sextonionic rows/columns of the magic square yield non-reductive... | 3.043892 | 3.377982 | 3.408761 | 3.182487 | 3.371949 | 3.317169 | 3.257351 | 3.259974 | 3.268172 | 3.491817 | 3.287929 | 3.110486 | 3.14963 | 3.14003 | 3.124368 | 3.142973 | 3.098799 | 3.139391 | 3.064256 | 3.177588 | 3.091498 |
1406.7602 | Boris Zupnik | B.M. Zupnik | SU(4) harmonic superspace and supersymmetric gauge theory | 21 pages, v2: corrected version | null | 10.1007/s11232-015-0322-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the harmonic-superspace formalism in the $N=4$ supersymmetry
using the $SU(4)/SU(2)\times SU(2)\times U(1)$ harmonics which was earlier
applied to the abelian gauge theory. The N=4 non-abelian constraints in a
standard superspace are reformulated as the harmonic-superspace equations for
two basic analytic... | [
{
"created": "Mon, 30 Jun 2014 04:37:25 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Oct 2014 12:05:55 GMT",
"version": "v2"
}
] | 2015-10-28 | [
[
"Zupnik",
"B. M.",
""
]
] | We consider the harmonic-superspace formalism in the $N=4$ supersymmetry using the $SU(4)/SU(2)\times SU(2)\times U(1)$ harmonics which was earlier applied to the abelian gauge theory. The N=4 non-abelian constraints in a standard superspace are reformulated as the harmonic-superspace equations for two basic analytic s... | 11.814859 | 12.526445 | 13.137597 | 11.178019 | 12.465773 | 12.459111 | 11.910525 | 11.209606 | 10.931704 | 13.62522 | 10.973356 | 11.065612 | 11.547091 | 10.719092 | 10.973445 | 11.245233 | 11.057981 | 11.063968 | 10.881494 | 11.595989 | 10.881258 |
1803.05552 | Qiang Wen | Qiang Wen | Fine structure in holographic entanglement and entanglement contour | v3:Version improved, second half of the paper re-written, relate the
fine structure to the entanglement contour, references added, title changed,
calculation details added. v4:published version 21 pages, 9 figures | Phys. Rev. D 98, 106004 (2018) | 10.1103/PhysRevD.98.106004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the fine structure of the holographic entanglement entropy
proposal (the Ryu-Takayanagi formula) in AdS$_3$/CFT$_{2}$. With the guidance
from the boundary and bulk modular flows we find a natural slicing of the
entanglement wedge with the modular planes, which are co-dimension one bulk
surfaces tangent to ... | [
{
"created": "Thu, 15 Mar 2018 00:44:27 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Apr 2018 19:47:20 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Aug 2018 12:05:59 GMT",
"version": "v3"
},
{
"created": "Tue, 30 Oct 2018 11:34:50 GMT",
"version": "v4"
}
] | 2018-11-14 | [
[
"Wen",
"Qiang",
""
]
] | We explore the fine structure of the holographic entanglement entropy proposal (the Ryu-Takayanagi formula) in AdS$_3$/CFT$_{2}$. With the guidance from the boundary and bulk modular flows we find a natural slicing of the entanglement wedge with the modular planes, which are co-dimension one bulk surfaces tangent to th... | 4.219604 | 4.515889 | 4.896019 | 4.152834 | 4.423872 | 4.486888 | 4.201436 | 4.273618 | 4.200961 | 4.787951 | 4.08107 | 4.193264 | 4.275857 | 4.018411 | 4.069165 | 4.198302 | 4.140521 | 4.153553 | 4.08171 | 4.291919 | 4.108961 |
2203.04972 | Justin Kaidi | Justin Kaidi, Mario Martone, Gabi Zafrir | Exceptional moduli spaces for exceptional $\mathcal{N}=3$ theories | 33+25 pages; v2: references added | null | 10.1007/JHEP08(2022)264 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | It is expected on general grounds that the moduli space of 4d $\mathcal{N}=3$
theories is of the form $\mathbb{C}^{3r}/\Gamma$, with $r$ the rank and
$\Gamma$ a crystallographic complex reflection group (CCRG). As in the case of
Lie algebras, the space of CCRGs consists of several infinite families,
together with som... | [
{
"created": "Wed, 9 Mar 2022 19:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Aug 2022 06:36:20 GMT",
"version": "v2"
}
] | 2022-09-14 | [
[
"Kaidi",
"Justin",
""
],
[
"Martone",
"Mario",
""
],
[
"Zafrir",
"Gabi",
""
]
] | It is expected on general grounds that the moduli space of 4d $\mathcal{N}=3$ theories is of the form $\mathbb{C}^{3r}/\Gamma$, with $r$ the rank and $\Gamma$ a crystallographic complex reflection group (CCRG). As in the case of Lie algebras, the space of CCRGs consists of several infinite families, together with some ... | 5.779575 | 5.569085 | 6.207041 | 5.273641 | 5.847965 | 5.650955 | 5.504803 | 5.540924 | 5.499517 | 6.327772 | 5.345637 | 5.222058 | 5.620415 | 5.104041 | 5.362412 | 5.290507 | 5.376581 | 5.311868 | 5.272345 | 5.725452 | 5.331247 |
0910.5441 | Edi Halyo | Edi Halyo | Domain Walls on Singularities | 16 pages in phyzzx.tex | Mod.Phys.Lett.A26:1035-1045,2011 | 10.1142/S0217732311035572 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe domain walls that live on $A_2$ and $A_3$ singularities. The
walls are BPS if the singularity is resolved and non--BPS if it is deformed and
fibered. We show that these domain walls may interpolate between vacua that
support monopoles and/or vortices.
| [
{
"created": "Wed, 28 Oct 2009 17:28:58 GMT",
"version": "v1"
}
] | 2011-06-06 | [
[
"Halyo",
"Edi",
""
]
] | We describe domain walls that live on $A_2$ and $A_3$ singularities. The walls are BPS if the singularity is resolved and non--BPS if it is deformed and fibered. We show that these domain walls may interpolate between vacua that support monopoles and/or vortices. | 10.256116 | 7.893983 | 11.773763 | 8.066072 | 8.390733 | 8.717353 | 7.822385 | 7.304 | 8.730574 | 10.877556 | 7.785685 | 8.187071 | 10.737555 | 8.784894 | 8.635256 | 8.491039 | 8.854197 | 8.286709 | 8.449891 | 10.014485 | 8.049863 |
1603.05582 | Shai Chester | Shai M. Chester, Silviu S. Pufu | Anomalous dimensions of scalar operators in $QED_3$ | 33 pages, 13 figures, v2 minor improvements, refs added | Journal of High Energy Physics, 2016(8), 1-27 | 10.1007/JHEP08(2016)069 | PUPT-2501 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The infrared dynamics of $2+1$ dimensional quantum electrodynamics (QED$_3$)
with a large number $N$ of fermion flavors is governed by an interacting CFT
that can be studied in the $1/N$ expansion. We use the $1/N$ expansion to
calculate the scaling dimensions of all the lowest three scalar operators that
transform u... | [
{
"created": "Thu, 17 Mar 2016 17:28:43 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Aug 2016 23:52:07 GMT",
"version": "v2"
}
] | 2016-08-24 | [
[
"Chester",
"Shai M.",
""
],
[
"Pufu",
"Silviu S.",
""
]
] | The infrared dynamics of $2+1$ dimensional quantum electrodynamics (QED$_3$) with a large number $N$ of fermion flavors is governed by an interacting CFT that can be studied in the $1/N$ expansion. We use the $1/N$ expansion to calculate the scaling dimensions of all the lowest three scalar operators that transform und... | 5.298107 | 5.075512 | 5.420632 | 5.026476 | 5.07436 | 4.812872 | 4.843713 | 5.130118 | 4.805641 | 5.299471 | 4.724077 | 4.824683 | 4.989288 | 4.895565 | 4.705857 | 4.772051 | 4.791968 | 4.802413 | 4.824497 | 5.054328 | 4.773947 |
1504.04439 | Justin David R | Justin R. David and Surbhi Khetrapal | Thermalization of Green functions and quasinormal modes | Typos corrected, references added, 38 pages. 9 figures. Mathematica
files included in source files | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a new method to study the thermalization of time dependent
retarded Green function in conformal field theories holographically dual to
thin shell AdS Vaidya space times. The method relies on using the information
of all time derivatives of the Green function at the shell and then evolving it
for later time... | [
{
"created": "Fri, 17 Apr 2015 04:42:44 GMT",
"version": "v1"
},
{
"created": "Tue, 12 May 2015 11:20:27 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"David",
"Justin R.",
""
],
[
"Khetrapal",
"Surbhi",
""
]
] | We develop a new method to study the thermalization of time dependent retarded Green function in conformal field theories holographically dual to thin shell AdS Vaidya space times. The method relies on using the information of all time derivatives of the Green function at the shell and then evolving it for later times.... | 7.773989 | 7.606379 | 8.177165 | 7.47292 | 7.863266 | 7.415934 | 7.916204 | 7.415591 | 7.580829 | 8.633666 | 7.1723 | 7.512085 | 8.002927 | 7.718315 | 7.561228 | 7.35607 | 7.422556 | 7.645079 | 7.688675 | 8.432009 | 7.403228 |
hep-th/0508077 | Mark Van Raamsdonk | Ofer Aharony, Joseph Marsano, Shiraz Minwalla, Kyriakos Papadodimas,
Mark Van Raamsdonk, and Toby Wiseman | The Phase Structure of Low Dimensional Large N Gauge Theories on Tori | harvmac, 67 pages, 21 figures. v2: minor corrections and
clarifications | JHEP 0601:140,2006 | 10.1088/1126-6708/2006/01/140 | null | hep-th | null | In this paper we continue our study of the thermodynamics of large N gauge
theories on compact spaces. We consider toroidal compactifications of pure
SU(N) Yang-Mills theories and of maximally supersymmetric Yang-Mills theories
dimensionally reduced to 0+1 or 1+1 dimensions, and generalizations of such
theories where... | [
{
"created": "Thu, 11 Aug 2005 18:50:05 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jan 2006 13:58:19 GMT",
"version": "v2"
}
] | 2009-04-02 | [
[
"Aharony",
"Ofer",
""
],
[
"Marsano",
"Joseph",
""
],
[
"Minwalla",
"Shiraz",
""
],
[
"Papadodimas",
"Kyriakos",
""
],
[
"Van Raamsdonk",
"Mark",
""
],
[
"Wiseman",
"Toby",
""
]
] | In this paper we continue our study of the thermodynamics of large N gauge theories on compact spaces. We consider toroidal compactifications of pure SU(N) Yang-Mills theories and of maximally supersymmetric Yang-Mills theories dimensionally reduced to 0+1 or 1+1 dimensions, and generalizations of such theories where t... | 5.341905 | 5.18711 | 5.492507 | 4.991908 | 5.120207 | 5.093706 | 5.370366 | 5.070261 | 5.121629 | 6.333256 | 5.20312 | 5.12333 | 5.330123 | 5.035223 | 5.176092 | 5.074705 | 4.886128 | 5.004777 | 5.019124 | 5.243922 | 5.12575 |
1307.0077 | Gianmassimo Tasinato | Gianmassimo Tasinato (ICG, Portsmouth), Kazuya Koyama (ICG,
Portsmouth), Nima Khosravi (AIMS, Cape Town) | The role of vector fields in modified gravity scenarios | 17 pages, no figures. v2: discussion improved, JCAP version | null | 10.1088/1475-7516/2013/11/037 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gravitational vector degrees of freedom typically arise in many examples of
modified gravity models. We start to systematically explore their role in these
scenarios, studying the effects of coupling gravitational vector and scalar
degrees of freedom. We focus on set-ups that enjoy a Galilean symmetry in the
scalar s... | [
{
"created": "Sat, 29 Jun 2013 08:55:56 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Dec 2013 10:29:46 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Tasinato",
"Gianmassimo",
"",
"ICG, Portsmouth"
],
[
"Koyama",
"Kazuya",
"",
"ICG,\n Portsmouth"
],
[
"Khosravi",
"Nima",
"",
"AIMS, Cape Town"
]
] | Gravitational vector degrees of freedom typically arise in many examples of modified gravity models. We start to systematically explore their role in these scenarios, studying the effects of coupling gravitational vector and scalar degrees of freedom. We focus on set-ups that enjoy a Galilean symmetry in the scalar sec... | 7.945514 | 7.957864 | 8.212158 | 7.496377 | 7.92032 | 8.003121 | 8.15124 | 7.988886 | 7.830752 | 8.877031 | 7.652198 | 7.692204 | 7.731043 | 7.625175 | 7.459978 | 7.644088 | 7.673673 | 7.590782 | 7.517258 | 7.579504 | 7.487888 |
1402.5239 | Vasilis Oikonomou | V.K. Oikonomou | Superconducting Cosmic Strings and One Dimensional Extended
Supersymmetric Algebras | Revised Version | null | 10.1016/j.aop.2014.07.020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we study in detail the supersymmetric structures that
underlie the system of fermionic zero modes around a superconducting cosmic
string. Particularly, we extend the analysis existing in the literature on the
one dimensional $N=2$ supersymmetry and we find multiple $N=2$, $d=1$
supersymmetries. In add... | [
{
"created": "Fri, 21 Feb 2014 10:05:25 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Apr 2014 15:23:59 GMT",
"version": "v2"
}
] | 2015-06-18 | [
[
"Oikonomou",
"V. K.",
""
]
] | In this article we study in detail the supersymmetric structures that underlie the system of fermionic zero modes around a superconducting cosmic string. Particularly, we extend the analysis existing in the literature on the one dimensional $N=2$ supersymmetry and we find multiple $N=2$, $d=1$ supersymmetries. In addit... | 9.863974 | 9.058481 | 9.993178 | 8.625597 | 9.391827 | 9.058153 | 8.944394 | 8.225458 | 9.261426 | 10.440671 | 9.186994 | 9.040211 | 10.047621 | 9.348464 | 8.908161 | 9.08432 | 9.191386 | 9.277198 | 9.756252 | 9.774757 | 9.343404 |
1310.3950 | Diederik Roest | Renata Kallosh, Andrei Linde, Diederik Roest | A universal attractor for inflation at strong coupling | 5 pages, 4 figures. v2: discussion on unitarity and extra refs added,
extended version of PRL paper | PRL 112 (2014) 011303 | 10.1103/PhysRevLett.112.011303 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a novel non-minimal coupling between gravity and the inflaton
sector. Remarkably, for large values of this coupling all models asymptote to a
universal attractor. This behavior is independent of the original scalar
potential and generalizes the attractor in the phi^4 theory with non-minimal
coupling to g... | [
{
"created": "Tue, 15 Oct 2013 08:16:35 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2014 19:27:32 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Kallosh",
"Renata",
""
],
[
"Linde",
"Andrei",
""
],
[
"Roest",
"Diederik",
""
]
] | We introduce a novel non-minimal coupling between gravity and the inflaton sector. Remarkably, for large values of this coupling all models asymptote to a universal attractor. This behavior is independent of the original scalar potential and generalizes the attractor in the phi^4 theory with non-minimal coupling to gra... | 10.28386 | 10.429968 | 9.109683 | 8.703502 | 9.811688 | 9.742392 | 10.87699 | 9.652164 | 9.008602 | 10.780934 | 9.826894 | 9.79021 | 9.390727 | 9.014124 | 9.646624 | 9.475535 | 9.647689 | 9.278231 | 9.354279 | 9.096483 | 8.994205 |
1306.1745 | Stefano Giusto | Stefano Giusto, Luca Martucci, Michela Petrini, Rodolfo Russo | 6D microstate geometries from 10D structures | 59 pages, including 19 pages of Appendix; v2: corrected typos, added
references; v3: corrected typos, eq. (3.55) simplified | null | 10.1016/j.nuclphysb.2013.08.018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the formalism of Generalised Geometry to characterise in general the
supersymmetric backgrounds in type II supergravity that have a null Killing
vector. We then specify this analysis to configurations that preserve the same
supersymmetries as the D1-D5-P system compactified on a four-manifold. We give
a set of... | [
{
"created": "Fri, 7 Jun 2013 15:14:38 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Sep 2013 12:54:35 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Jul 2015 13:57:08 GMT",
"version": "v3"
}
] | 2015-07-06 | [
[
"Giusto",
"Stefano",
""
],
[
"Martucci",
"Luca",
""
],
[
"Petrini",
"Michela",
""
],
[
"Russo",
"Rodolfo",
""
]
] | We use the formalism of Generalised Geometry to characterise in general the supersymmetric backgrounds in type II supergravity that have a null Killing vector. We then specify this analysis to configurations that preserve the same supersymmetries as the D1-D5-P system compactified on a four-manifold. We give a set of e... | 6.388885 | 5.995695 | 6.837516 | 6.145147 | 6.325675 | 5.888767 | 6.130533 | 5.913969 | 6.198494 | 7.85126 | 6.202313 | 6.017882 | 6.622063 | 6.198366 | 6.221164 | 6.108843 | 5.967525 | 6.052211 | 6.153307 | 6.462657 | 6.067824 |
0901.1642 | Antoine Folacci | Yves D\'ecanini and Antoine Folacci | Quasinormal modes of the BTZ black hole are generated by surface waves
supported by its boundary at infinity | v2: Typos corrected, English "improved", one additional reference | Phys.Rev.D79:044021,2009 | 10.1103/PhysRevD.79.044021 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop the complex angular momentum method in the context of the BTZ
black hole physics. This is achieved by extending a formalism introduced a long
time ago by Arnold Sommerfeld, which allows us to define and use the Regge pole
concept in a framework where the notion of an $S$ matrix does not exist. The
Regge po... | [
{
"created": "Mon, 12 Jan 2009 20:36:28 GMT",
"version": "v1"
},
{
"created": "Sun, 8 Feb 2009 13:46:10 GMT",
"version": "v2"
}
] | 2009-02-19 | [
[
"Décanini",
"Yves",
""
],
[
"Folacci",
"Antoine",
""
]
] | We develop the complex angular momentum method in the context of the BTZ black hole physics. This is achieved by extending a formalism introduced a long time ago by Arnold Sommerfeld, which allows us to define and use the Regge pole concept in a framework where the notion of an $S$ matrix does not exist. The Regge pole... | 12.418123 | 15.213373 | 11.44234 | 11.660292 | 12.604388 | 12.912285 | 13.19435 | 11.428301 | 12.540206 | 12.139116 | 11.872868 | 11.866263 | 11.52733 | 11.461351 | 11.874652 | 12.231202 | 12.347192 | 11.518028 | 11.707195 | 11.806957 | 12.112683 |
1706.10039 | Ulf-G. Mei{\ss}ner | D. Djukanovic, J. Gegelia, Ulf-G. Mei{\ss}ner | Triviality of quantum electrodynamics revisited | 3 pages, 2 figures | Commun. Theor. Phys. 69 (2018) 263 | 10.1088/0253-6102/69/3/263 | null | hep-th hep-lat hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum electrodynamics is considered to be a trivial theory. This is based
on a number of evidences, both numerical and analytical. One of the strong
indications for triviality of QED is the existence of the Landau pole for the
running coupling. We show that by treating QED as the leading order
approximation of an e... | [
{
"created": "Fri, 30 Jun 2017 06:49:00 GMT",
"version": "v1"
}
] | 2018-02-12 | [
[
"Djukanovic",
"D.",
""
],
[
"Gegelia",
"J.",
""
],
[
"Meißner",
"Ulf-G.",
""
]
] | Quantum electrodynamics is considered to be a trivial theory. This is based on a number of evidences, both numerical and analytical. One of the strong indications for triviality of QED is the existence of the Landau pole for the running coupling. We show that by treating QED as the leading order approximation of an eff... | 7.245009 | 6.809737 | 6.364394 | 6.381264 | 6.79571 | 7.086219 | 6.639975 | 6.630335 | 6.30744 | 7.345219 | 6.496084 | 6.564839 | 6.668913 | 6.458746 | 6.497441 | 6.553556 | 6.641327 | 6.772845 | 6.309871 | 6.677284 | 6.496706 |
hep-th/0201002 | Myoung-taek Choi | Mu- in Park (CCNY) | Non-Commutative Space-Times, Black Hole, and Elementary Particle | Added footnote and references | null | null | CCNY-HEP-01/11 | hep-th | null | It is shown that elementary black hole can not be distinguished from an
elementary particle in the non-commutative space-times (space/space and
space/time) at the Planck scale. But, the non-commutative space-times can not
be ``directly'' measured in the elementary black hole system. A time-varying
non-commutative par... | [
{
"created": "Tue, 1 Jan 2002 01:55:55 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Jan 2002 15:50:56 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Park",
"Mu- in",
"",
"CCNY"
]
] | It is shown that elementary black hole can not be distinguished from an elementary particle in the non-commutative space-times (space/space and space/time) at the Planck scale. But, the non-commutative space-times can not be ``directly'' measured in the elementary black hole system. A time-varying non-commutative param... | 9.664209 | 9.081917 | 8.917313 | 8.643319 | 9.112972 | 8.749435 | 8.989628 | 8.662519 | 8.83774 | 9.474537 | 8.686078 | 8.683616 | 9.397735 | 8.762169 | 9.031052 | 8.860047 | 9.107384 | 8.613194 | 8.912336 | 9.08523 | 8.693069 |
1201.2317 | Sergey Frolov Dr. | Sergey Frolov | Scaling dimensions from the mirror TBA | null | null | 10.1088/1751-8113/45/30/305402 | TCDMATH 12-01; HMI-12-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The mirror TBA equations proposed by Arutyunov, Suzuki and the author are
solved numerically up to 't Hooft's coupling $\lambda\approx 2340$ for several
two-particle states dual to ${\cal N}=4$ SYM operators from the $\sl(2)$
sector. The data obtained for states with mode numbers $n=1,2,3,4$ is used to
propose a gene... | [
{
"created": "Wed, 11 Jan 2012 14:52:25 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Frolov",
"Sergey",
""
]
] | The mirror TBA equations proposed by Arutyunov, Suzuki and the author are solved numerically up to 't Hooft's coupling $\lambda\approx 2340$ for several two-particle states dual to ${\cal N}=4$ SYM operators from the $\sl(2)$ sector. The data obtained for states with mode numbers $n=1,2,3,4$ is used to propose a genera... | 9.282037 | 7.540788 | 9.192394 | 7.900302 | 7.83151 | 8.339332 | 7.56451 | 7.453727 | 7.647026 | 9.657792 | 7.615107 | 7.620259 | 8.512428 | 8.048638 | 7.531493 | 8.178856 | 8.05127 | 7.881423 | 7.928453 | 8.451286 | 7.994021 |
1303.1037 | Ben Hoare | B. Hoare and A. A. Tseytlin | On string theory on AdS_3 x S^3 x T^4 with mixed 3-form flux: tree-level
S-matrix | 46 pages; v2: 50 pages, new part of Appendix A added and minor
misprints corrected; v3: discussion of proposed dispersion relation in eq.
4.11 and symmetry algebra in appendix B for q not 0 modified; v4: minor
corrections and comments added; v5: misprints corrected (in particular, in
eqs. 3.18, 3.20 and 3.24) a... | null | 10.1016/j.nuclphysb.2013.05.005 | Imperial-TP-AT-2013-01, HU-EP-13/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider superstring theory on AdS_3 x S^3 x T^4 supported by a
combination of RR and NSNS 3-form fluxes (with parameter of the NSNS 3-form q).
This theory interpolates between the pure RR flux model (q=0) whose spectrum is
expected to be described by a Bethe ansatz and the pure NSNS flux model (q=1)
which is desc... | [
{
"created": "Tue, 5 Mar 2013 14:05:09 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Mar 2013 17:31:45 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Mar 2013 14:27:35 GMT",
"version": "v3"
},
{
"created": "Thu, 23 May 2013 13:12:25 GMT",
"version": "v4"
},
{
"cr... | 2018-04-09 | [
[
"Hoare",
"B.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We consider superstring theory on AdS_3 x S^3 x T^4 supported by a combination of RR and NSNS 3-form fluxes (with parameter of the NSNS 3-form q). This theory interpolates between the pure RR flux model (q=0) whose spectrum is expected to be described by a Bethe ansatz and the pure NSNS flux model (q=1) which is descri... | 5.310641 | 5.153189 | 6.266155 | 4.847524 | 5.250595 | 5.138806 | 5.177862 | 5.102395 | 4.904205 | 6.601779 | 4.883002 | 5.12025 | 5.548314 | 4.967315 | 5.069696 | 4.890663 | 5.074592 | 5.028737 | 5.139174 | 5.353483 | 5.076857 |
hep-th/0308170 | Kunihito Uzawa | Kunihito Uzawa | Dilaton Stabilization in (A)dS Spacetime with Compactified Dimensions | 43 pages, 12 figures, PTPTeX. Accepted for publication in Progress of
Theoretical Physics | Prog.Theor.Phys. 110 (2003) 457-498 | 10.1143/PTP.110.457 | null | hep-th gr-qc hep-ph | null | We investigate dilaton stabilization in a higher-dimensional theory. The
background geometry is based on an eleven-dimensional Kaluza-Klein/supergravity
model, which is assumed to be a product of four-dimensional de Sitter (dS_4)
spacetime and a seven sphere. The dilaton potential has a local minimum
resulting from c... | [
{
"created": "Tue, 26 Aug 2003 05:29:28 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Uzawa",
"Kunihito",
""
]
] | We investigate dilaton stabilization in a higher-dimensional theory. The background geometry is based on an eleven-dimensional Kaluza-Klein/supergravity model, which is assumed to be a product of four-dimensional de Sitter (dS_4) spacetime and a seven sphere. The dilaton potential has a local minimum resulting from con... | 9.587292 | 9.455931 | 8.045578 | 8.451969 | 9.765475 | 8.369083 | 9.019732 | 9.015344 | 8.401252 | 8.927171 | 9.612494 | 9.083062 | 8.403995 | 8.658592 | 8.698962 | 8.615993 | 8.841497 | 9.062825 | 8.681792 | 8.883598 | 8.777075 |
hep-th/9806095 | null | R.R. Metsaev and A.A. Tseytlin | Supersymmetric D3 brane action in AdS_5 x S^5 | 12 pages, latex. v2: misprints corrected, useful representation of
the WZ part of the action added in section 3 | Phys.Lett.B436:281-288,1998 | 10.1016/S0370-2693(98)00869-7 | Imperial/TP/97-98/53 | hep-th | null | We find the space-time supersymmetric and kappa-invariant action for a
D3-brane propagating in the AdS_5 x S^5 background. As in the previous
construction of the fundamental string action in this maximally supersymmetric
string vacuum the starting point is the corresponding superalgebra su(2,2|4).
We comment on the s... | [
{
"created": "Thu, 11 Jun 1998 23:23:38 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Jun 1998 18:06:53 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Metsaev",
"R. R.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We find the space-time supersymmetric and kappa-invariant action for a D3-brane propagating in the AdS_5 x S^5 background. As in the previous construction of the fundamental string action in this maximally supersymmetric string vacuum the starting point is the corresponding superalgebra su(2,2|4). We comment on the sup... | 8.526256 | 7.122392 | 9.302973 | 6.77975 | 6.836636 | 6.595655 | 6.98227 | 6.782367 | 6.662214 | 10.732426 | 6.125846 | 7.269138 | 8.623477 | 7.549811 | 7.476805 | 6.988724 | 7.288597 | 7.460567 | 7.326893 | 9.220668 | 7.295474 |
2103.11502 | Francisco Tello Ortiz | Alvaro Restuccia, Francisco Tello-Ortiz | Charged Throats in the Ho\v{r}ava--Lifshitz Theory | null | null | 10.1140/epjc/s10052-021-09251-0 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | A spherically symmetric solution of the field equations of the
Ho\v{r}ava--Lifshitz gravity--gauge vector interaction theory is obtained and
analyzed. It describes a charged throat. The solution exists provided a
restriction on the relation between the mass and charge is satisfied. The
restriction reduces to the Reis... | [
{
"created": "Sun, 21 Mar 2021 22:16:22 GMT",
"version": "v1"
}
] | 2023-01-11 | [
[
"Restuccia",
"Alvaro",
""
],
[
"Tello-Ortiz",
"Francisco",
""
]
] | A spherically symmetric solution of the field equations of the Ho\v{r}ava--Lifshitz gravity--gauge vector interaction theory is obtained and analyzed. It describes a charged throat. The solution exists provided a restriction on the relation between the mass and charge is satisfied. The restriction reduces to the Reissn... | 7.228134 | 7.689011 | 7.421592 | 7.416682 | 7.516889 | 7.186207 | 7.063416 | 6.980873 | 7.306513 | 7.522156 | 6.940627 | 7.157117 | 6.899447 | 6.808278 | 7.026208 | 6.973089 | 6.791803 | 6.792633 | 6.793493 | 6.823327 | 6.747625 |
2211.04333 | Ryotaku Suzuki | David Licht, Ryotaku Suzuki and Benson Way | The large D effective theory of black strings in AdS | 43pages, 18figures; v2: minor modifications, references added,
44pages | null | 10.1007/JHEP12(2022)146 | TTI-MATHPHYS-16 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study black strings/funnels and other black hole configurations in AdS
that correspond to different phases of the dual CFT in black hole backgrounds,
employing different approaches at large $D$. We assemble the phase diagram of
uniform and non-uniform black strings/funnels and study their dynamical
stability. We a... | [
{
"created": "Tue, 8 Nov 2022 15:51:01 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Nov 2022 12:29:11 GMT",
"version": "v2"
}
] | 2023-01-18 | [
[
"Licht",
"David",
""
],
[
"Suzuki",
"Ryotaku",
""
],
[
"Way",
"Benson",
""
]
] | We study black strings/funnels and other black hole configurations in AdS that correspond to different phases of the dual CFT in black hole backgrounds, employing different approaches at large $D$. We assemble the phase diagram of uniform and non-uniform black strings/funnels and study their dynamical stability. We als... | 17.655767 | 14.005049 | 17.217865 | 14.590962 | 18.311924 | 14.820913 | 15.453203 | 16.284124 | 13.932453 | 18.624418 | 14.266351 | 15.273046 | 16.141747 | 15.642016 | 15.675173 | 14.728551 | 15.593243 | 16.028147 | 15.476927 | 16.710636 | 15.393964 |
hep-th/9901057 | Poul Olesen | J. Greensite and P. Olesen | Worldsheet Fluctuations and the Heavy Quark Potential in the AdS/CFT
Approach | 16 pages, 3 figures, Latex2e. Added some remarks on the
incompatibility of the AdS/CFT and the lattice regulators, and on the
appropriate boundary conditions | JHEP 9904:001,1999 | 10.1088/1126-6708/1999/04/001 | null | hep-th hep-lat hep-ph | null | We consider contributions to the heavy quark potential, in the AdS/CFT
approach to SU(N) gauge theory, which arise from first order fluctuations of
the associated worldsheet in anti-deSitter space. The gaussian fluctuations
occur around a classical worldsheet configuration resembling an infinite square
well, with the... | [
{
"created": "Thu, 14 Jan 1999 10:01:29 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jan 1999 04:42:38 GMT",
"version": "v2"
},
{
"created": "Wed, 20 Jan 1999 09:29:42 GMT",
"version": "v3"
},
{
"created": "Wed, 7 Apr 1999 09:09:44 GMT",
"version": "v4"
}
] | 2010-02-03 | [
[
"Greensite",
"J.",
""
],
[
"Olesen",
"P.",
""
]
] | We consider contributions to the heavy quark potential, in the AdS/CFT approach to SU(N) gauge theory, which arise from first order fluctuations of the associated worldsheet in anti-deSitter space. The gaussian fluctuations occur around a classical worldsheet configuration resembling an infinite square well, with the b... | 10.505101 | 10.271062 | 10.410905 | 9.989475 | 11.014384 | 10.824547 | 10.590962 | 9.945851 | 9.817377 | 10.73274 | 9.96138 | 9.75701 | 10.294721 | 10.184629 | 10.099382 | 10.096368 | 9.85189 | 9.651929 | 9.87771 | 10.29799 | 9.743217 |
2111.06861 | Horatiu Stefan Nastase | Horatiu Nastase, Francisco Rojas and Carlos Rubio | Celestial IR divergences in general most-subleading-color gluon and
gravity amplitudes | 30 pages, no figures | null | 10.1007/JHEP01(2022)136 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gluon amplitudes at most-subleading order in the $1/N$ expansion share a
remarkable simplicity with graviton amplitudes: collinear divergences are
completely absent in both and, as a consequence, their full IR behavior arises
from soft gluon/graviton exchange among the external states. In this paper we
study the effe... | [
{
"created": "Fri, 12 Nov 2021 18:30:49 GMT",
"version": "v1"
}
] | 2022-02-09 | [
[
"Nastase",
"Horatiu",
""
],
[
"Rojas",
"Francisco",
""
],
[
"Rubio",
"Carlos",
""
]
] | Gluon amplitudes at most-subleading order in the $1/N$ expansion share a remarkable simplicity with graviton amplitudes: collinear divergences are completely absent in both and, as a consequence, their full IR behavior arises from soft gluon/graviton exchange among the external states. In this paper we study the effect... | 9.445771 | 10.157555 | 10.159027 | 9.193772 | 9.804374 | 9.118451 | 9.44199 | 9.388798 | 9.972822 | 11.030868 | 9.94754 | 9.250257 | 9.342176 | 9.188416 | 8.962379 | 9.463056 | 9.17854 | 9.19063 | 9.191956 | 9.556275 | 9.13363 |
hep-th/9701011 | Stephen Fletcher Hewson | S. Hewson | Generalised supersymmetry and p-brane actions | 29 pages, LaTex, no figures. Errors in degrees of freedom counting
corrected, leading to altered brane scan | Nucl.Phys. B501 (1997) 445-468 | 10.1016/S0550-3213(97)00370-2 | DAMTP-R-97-01 | hep-th | null | We investigate the most general N=1 graded extension of the Poincare algebra,
and find the corresponding supersymmetry transformations and the associated
superspaces. We find that the supersymmetry for which {Q,Q} = P is not special,
and in fact must be treated democratically with a whole class of
supersymmetries. We... | [
{
"created": "Sat, 4 Jan 1997 21:55:00 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Mar 1997 11:52:28 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Hewson",
"S.",
""
]
] | We investigate the most general N=1 graded extension of the Poincare algebra, and find the corresponding supersymmetry transformations and the associated superspaces. We find that the supersymmetry for which {Q,Q} = P is not special, and in fact must be treated democratically with a whole class of supersymmetries. We s... | 13.083201 | 13.453241 | 12.421425 | 12.11308 | 12.838915 | 12.389239 | 12.178927 | 12.45917 | 11.502071 | 12.539443 | 11.714352 | 12.204781 | 12.672153 | 11.658753 | 11.91349 | 11.850563 | 12.549248 | 12.044009 | 11.92087 | 12.335199 | 11.918621 |
hep-th/0302053 | Saharian | A. A. Saharian, M. R. Setare | Casimir densities for a spherical shell in the global monopole
background | 19 pages, 4 figures, discussion of zeros is added, accepted for
publication in Classical and Quantum Gravity | Class.Quant.Grav. 20 (2003) 3765-3782 | 10.1088/0264-9381/20/16/315 | null | hep-th astro-ph gr-qc quant-ph | null | We investigate the vacuum expectation values for the energy-momentum tensor
of a massive scalar field with general curvature coupling and obeying the Robin
boundary condition on a spherical shell in the $D+1$-dimensional global
monopole background. The expressions are derived for the Wightman function, the
vacuum exp... | [
{
"created": "Sat, 8 Feb 2003 07:02:43 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Jun 2003 10:01:07 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Saharian",
"A. A.",
""
],
[
"Setare",
"M. R.",
""
]
] | We investigate the vacuum expectation values for the energy-momentum tensor of a massive scalar field with general curvature coupling and obeying the Robin boundary condition on a spherical shell in the $D+1$-dimensional global monopole background. The expressions are derived for the Wightman function, the vacuum expec... | 5.563752 | 2.944608 | 7.022747 | 3.516411 | 3.489532 | 2.976204 | 3.150826 | 3.266607 | 3.739641 | 7.021388 | 3.546663 | 4.728093 | 6.13763 | 5.054991 | 4.681177 | 4.62904 | 4.484196 | 4.86077 | 4.926834 | 6.319909 | 4.801785 |
1912.04773 | Paul K. Townsend | Paul K. Townsend | Manifestly Lorentz invariant chiral boson action | 5 pp. Further minor corrections to V3 in V5 | Phys. Rev. Lett. 124, 101604 (2020) | 10.1103/PhysRevLett.124.101604 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A manifestly Lorentz invariant action is found for the Floreanini-Jackiw
chiral boson. The method involves a novel chiral reduction of the phase-space
action for a string, and can be adapted to describe chiral bosons on the
heterotic string worldsheet. A similar manifestly Lorentz invariant action is
found for an ent... | [
{
"created": "Tue, 10 Dec 2019 15:39:54 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Dec 2019 11:48:34 GMT",
"version": "v2"
},
{
"created": "Fri, 21 Feb 2020 09:10:46 GMT",
"version": "v3"
},
{
"created": "Thu, 27 Feb 2020 11:05:26 GMT",
"version": "v4"
},
{
"c... | 2020-03-18 | [
[
"Townsend",
"Paul K.",
""
]
] | A manifestly Lorentz invariant action is found for the Floreanini-Jackiw chiral boson. The method involves a novel chiral reduction of the phase-space action for a string, and can be adapted to describe chiral bosons on the heterotic string worldsheet. A similar manifestly Lorentz invariant action is found for an entir... | 7.699378 | 7.133115 | 8.124125 | 7.035546 | 7.012642 | 6.888953 | 7.105713 | 6.885405 | 7.12244 | 8.398829 | 6.901602 | 7.254423 | 7.609152 | 7.203453 | 7.336502 | 7.084454 | 7.040865 | 7.379275 | 7.155898 | 7.948322 | 7.293808 |
hep-th/0702162 | Andrew A. Semenov | A.A. Semenov, C.V. Usenko, B.I. Lev | Positive-definite states of a Klein-Gordon type particle | 10 pages | Phys.Lett.A372:4180-4183,2008 | 10.1016/j.physleta.2008.03.052 | null | hep-th math-ph math.MP quant-ph | null | A possible way for the consistent probability interpretation of the
Klein-Gordon equation is proposed. It is assumed that some states of a scalar
charged particle cannot be physically realized. The rest of quantum states are
proven to have positive-definite probability distributions.
| [
{
"created": "Tue, 20 Feb 2007 14:09:11 GMT",
"version": "v1"
},
{
"created": "Sun, 9 Dec 2007 17:37:41 GMT",
"version": "v2"
},
{
"created": "Thu, 8 May 2008 19:17:18 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Semenov",
"A. A.",
""
],
[
"Usenko",
"C. V.",
""
],
[
"Lev",
"B. I.",
""
]
] | A possible way for the consistent probability interpretation of the Klein-Gordon equation is proposed. It is assumed that some states of a scalar charged particle cannot be physically realized. The rest of quantum states are proven to have positive-definite probability distributions. | 14.836663 | 13.100567 | 13.292766 | 11.814609 | 14.13168 | 13.007559 | 13.353551 | 12.540195 | 14.798837 | 13.161201 | 13.763192 | 12.9554 | 14.198293 | 13.481278 | 13.112415 | 13.189875 | 13.270258 | 13.397309 | 14.286396 | 13.446676 | 13.474369 |
hep-th/9710119 | Hong Lu | E. Cremmer, B. Julia, H. Lu and C.N. Pope | Dualisation of Dualities, I | Latex, 82 pages, minor corrections and references added | Nucl.Phys.B523:73-144,1998 | 10.1016/S0550-3213(98)00136-9 | CTP TAMU-27/97, LPTENS-97/27, SISSARef-132/97/EP | hep-th | null | We analyse the global (rigid) symmetries that are realised on the bosonic
fields of the various supergravity actions obtained from eleven-dimensional
supergravity by toroidal compactification followed by the dualisation of some
subset of fields. In particular, we show how the global symmetries of the
action can be af... | [
{
"created": "Wed, 15 Oct 1997 12:03:53 GMT",
"version": "v1"
},
{
"created": "Sat, 22 Aug 1998 14:33:01 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Cremmer",
"E.",
""
],
[
"Julia",
"B.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
]
] | We analyse the global (rigid) symmetries that are realised on the bosonic fields of the various supergravity actions obtained from eleven-dimensional supergravity by toroidal compactification followed by the dualisation of some subset of fields. In particular, we show how the global symmetries of the action can be affe... | 11.482979 | 11.347485 | 12.823483 | 11.258048 | 12.011018 | 11.865143 | 11.94332 | 11.871521 | 11.389804 | 15.264679 | 10.960687 | 11.355517 | 11.800721 | 11.254709 | 11.14762 | 11.193127 | 10.970347 | 11.347522 | 11.310586 | 12.075689 | 10.992088 |
2008.01729 | Danilo Artigas | Danilo Artigas, Jakub Bilski, Sean Crowe, Jakub Mielczarek, Tomasz
Trze\'sniewski | General-relativistic spin system | 19 pages, 3 figures v2 rewritten parts of Secs. I-III, some
clarifications elsewhere, typos corrected, references added, 1 extra figure | Phys. Rev. D 102, 125029 (2020) | 10.1103/PhysRevD.102.125029 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The models of spin systems defined on Euclidean space provide powerful
machinery for studying a broad range of condensed matter phenomena. While the
non-relativistic effective description is sufficient for most of the
applications, it is interesting to consider special and general relativistic
extensions of such mode... | [
{
"created": "Tue, 4 Aug 2020 18:00:00 GMT",
"version": "v1"
},
{
"created": "Sat, 5 Dec 2020 08:18:32 GMT",
"version": "v2"
}
] | 2020-12-29 | [
[
"Artigas",
"Danilo",
""
],
[
"Bilski",
"Jakub",
""
],
[
"Crowe",
"Sean",
""
],
[
"Mielczarek",
"Jakub",
""
],
[
"Trześniewski",
"Tomasz",
""
]
] | The models of spin systems defined on Euclidean space provide powerful machinery for studying a broad range of condensed matter phenomena. While the non-relativistic effective description is sufficient for most of the applications, it is interesting to consider special and general relativistic extensions of such models... | 12.054552 | 12.976143 | 12.009763 | 12.103567 | 12.601284 | 12.823646 | 12.858259 | 12.292932 | 12.39183 | 12.969447 | 12.66663 | 12.087528 | 11.802058 | 11.504067 | 11.936851 | 11.807427 | 11.983829 | 11.839075 | 11.632959 | 11.667066 | 11.657523 |
2312.17725 | Leslaw Rachwal | Les{\l}aw Rachwa{\l}, P\'ublio Rwany B. R. do Vale | Generalization of conformal Hamada operators | 60 pages | null | null | null | hep-th gr-qc math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | The six-derivative conformal scalar operator was originally found by Hamada
in its critical dimension of spacetime, $d=6$. We generalize this construction
to arbitrary dimensions $d$ by adding new terms cubic in gravitational
curvatures and by changing its coefficients of expansion in various curvature
terms. The con... | [
{
"created": "Fri, 29 Dec 2023 18:25:22 GMT",
"version": "v1"
},
{
"created": "Sat, 11 May 2024 21:30:20 GMT",
"version": "v2"
}
] | 2024-05-14 | [
[
"Rachwał",
"Lesław",
""
],
[
"Vale",
"Públio Rwany B. R. do",
""
]
] | The six-derivative conformal scalar operator was originally found by Hamada in its critical dimension of spacetime, $d=6$. We generalize this construction to arbitrary dimensions $d$ by adding new terms cubic in gravitational curvatures and by changing its coefficients of expansion in various curvature terms. The conse... | 12.852859 | 12.07943 | 13.271508 | 11.412346 | 12.246337 | 11.752585 | 12.958997 | 11.740005 | 12.556592 | 15.228242 | 11.891044 | 11.58028 | 11.706523 | 11.601802 | 12.143954 | 11.72485 | 11.671881 | 11.511385 | 11.475751 | 11.841025 | 11.755743 |
hep-th/9512118 | null | Emili Bagan, Martin Lavelle and David McMullan | The Physical Propagator of a Slowly Moving Charge | 10 pages, plain TeX, 1 Figure (uuencoded needs epsfig.sty) | Phys.Lett. B370 (1996) 128-134 | 10.1016/0370-2693(96)00049-4 | UAB-FT-379, PLY-MS-95-08 | hep-th hep-ph | null | We consider an electron which is electromagnetically dressed in such a way
that it is both gauge invariant and that it has the associated electric and
magnetic fields expected of a moving charge. We study the propagator of this
dressed electron and, for small velocities, show explicitly at one loop that at
the natura... | [
{
"created": "Fri, 15 Dec 1995 18:52:40 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Bagan",
"Emili",
""
],
[
"Lavelle",
"Martin",
""
],
[
"McMullan",
"David",
""
]
] | We consider an electron which is electromagnetically dressed in such a way that it is both gauge invariant and that it has the associated electric and magnetic fields expected of a moving charge. We study the propagator of this dressed electron and, for small velocities, show explicitly at one loop that at the natural ... | 15.489626 | 17.798359 | 14.722765 | 14.564488 | 13.85577 | 16.383104 | 16.171379 | 14.905888 | 12.906532 | 15.218551 | 13.962434 | 14.487072 | 14.203059 | 14.272975 | 14.304573 | 14.182794 | 14.323195 | 14.454447 | 14.310297 | 14.764409 | 14.398366 |
hep-th/0611222 | Juan Francisco Zanella | J. Zanella, E. Calzetta | Renormalization group study of damping in nonequilibrium field theory | 50 pages, 4 figures, feynmf | null | null | null | hep-th cond-mat.other hep-ph | null | In this paper we shall study whether dissipation in a $\lambda\phi^{4}$ may
be described, in the long wavelength, low frequency limit, with a simple Ohmic
term $\kappa\dot{\phi}$, as it is usually done, for example, in studies of
defect formation in nonequilibrium phase transitions. We shall obtain an
effective theor... | [
{
"created": "Tue, 21 Nov 2006 10:31:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Zanella",
"J.",
""
],
[
"Calzetta",
"E.",
""
]
] | In this paper we shall study whether dissipation in a $\lambda\phi^{4}$ may be described, in the long wavelength, low frequency limit, with a simple Ohmic term $\kappa\dot{\phi}$, as it is usually done, for example, in studies of defect formation in nonequilibrium phase transitions. We shall obtain an effective theory ... | 7.618682 | 7.932541 | 7.160015 | 6.921667 | 7.199533 | 7.489269 | 7.351137 | 7.47462 | 6.95605 | 7.66998 | 7.710268 | 7.387936 | 7.308074 | 7.0151 | 7.075698 | 7.282899 | 7.153884 | 6.850361 | 7.140267 | 7.238631 | 7.213131 |
1602.05631 | Takuya Kanazawa | Takuya Kanazawa | Heavy-tailed chiral random matrix theory | 18 pages, 5 figures | JHEP 05 (2016) 166 | 10.1007/JHEP05(2016)166 | RIKEN-QHP-194 | hep-th hep-lat math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study an unconventional chiral random matrix model with a heavy-tailed
probabilistic weight. The model is shown to exhibit chiral symmetry breaking
with no bilinear condensate, in analogy to the Stern phase of QCD. We solve the
model analytically and obtain the microscopic spectral density and the smallest
eigenva... | [
{
"created": "Wed, 17 Feb 2016 23:43:11 GMT",
"version": "v1"
}
] | 2016-05-31 | [
[
"Kanazawa",
"Takuya",
""
]
] | We study an unconventional chiral random matrix model with a heavy-tailed probabilistic weight. The model is shown to exhibit chiral symmetry breaking with no bilinear condensate, in analogy to the Stern phase of QCD. We solve the model analytically and obtain the microscopic spectral density and the smallest eigenvalu... | 8.755858 | 7.472266 | 8.864286 | 8.176869 | 8.930986 | 8.855053 | 8.42794 | 8.054792 | 7.716458 | 9.096728 | 8.269682 | 8.592138 | 8.681759 | 8.125204 | 8.27567 | 8.352693 | 8.665449 | 8.566758 | 8.197327 | 8.802801 | 8.130857 |
hep-th/0105066 | Keshav Dasgupta | Keshav Dasgupta, Kyungho Oh, Radu Tatar | Geometric Transition, Large N Dualities and MQCD Dynamics | 18 pages, no figures, Latex; v2: a paragraph added at the end of
section 3 and a reference corrected. No other changes; v3: some comments
added at the begining of sec. 6 and references updated. Final version to
appear in Nucl. Phys. B | Nucl.Phys. B610 (2001) 331-346 | 10.1016/S0550-3213(01)00296-6 | HUTP-01/A022, HU-EP-01/20 | hep-th | null | We study Vafa's geometric transition from a brane setup in M-theory. In this
transition D5 branes wrapped on P^1 cycles of a resolved conifold disappear and
are replaced by fluxes on a deformed conifold. In the limit of small sized P^1,
we describe this mechanism as a transition from curved M5 branes to plane M5
bran... | [
{
"created": "Tue, 8 May 2001 16:22:36 GMT",
"version": "v1"
},
{
"created": "Fri, 18 May 2001 05:21:54 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Jun 2001 17:20:03 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Dasgupta",
"Keshav",
""
],
[
"Oh",
"Kyungho",
""
],
[
"Tatar",
"Radu",
""
]
] | We study Vafa's geometric transition from a brane setup in M-theory. In this transition D5 branes wrapped on P^1 cycles of a resolved conifold disappear and are replaced by fluxes on a deformed conifold. In the limit of small sized P^1, we describe this mechanism as a transition from curved M5 branes to plane M5 branes... | 11.469029 | 10.417616 | 12.554105 | 10.480338 | 11.686576 | 11.230764 | 10.689467 | 9.855974 | 10.531124 | 13.356964 | 9.985936 | 10.469821 | 11.684846 | 10.993115 | 10.946338 | 10.390603 | 10.907936 | 10.266472 | 10.627277 | 11.81591 | 10.399096 |
1906.07417 | Urs Schreiber | Domenico Fiorenza, Hisham Sati, Urs Schreiber | Twisted Cohomotopy implies level quantization of the full 6d Wess-Zumino
term of the M5-brane | 22 pages; v2 fixes a missing theta7-summand in intermediate formulas
and has two remarks added, for clarification; v3 fixes typos and makes the
slicing over the homotopy fiber space of chi_8 more explicit | Comm. Math. Phys. 2020 | 10.1007/s00220-021-03951-0 | null | hep-th math-ph math.AT math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The full 6d Hopf-Wess-Zumino term in the action functional for the M5-brane
is anomalous as traditionally defined. What has been missing is a condition
implying the higher analogue of level quantization familiar from the 2d
Wess-Zumino term. We prove that the anomaly cancellation condition is implied
by the hypothesi... | [
{
"created": "Tue, 18 Jun 2019 07:42:02 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Jan 2020 16:35:47 GMT",
"version": "v2"
},
{
"created": "Fri, 9 Oct 2020 08:38:27 GMT",
"version": "v3"
}
] | 2021-04-21 | [
[
"Fiorenza",
"Domenico",
""
],
[
"Sati",
"Hisham",
""
],
[
"Schreiber",
"Urs",
""
]
] | The full 6d Hopf-Wess-Zumino term in the action functional for the M5-brane is anomalous as traditionally defined. What has been missing is a condition implying the higher analogue of level quantization familiar from the 2d Wess-Zumino term. We prove that the anomaly cancellation condition is implied by the hypothesis ... | 6.494048 | 9.217721 | 11.288591 | 9.400767 | 10.681659 | 9.220046 | 10.078482 | 10.836866 | 9.980457 | 14.41083 | 10.136072 | 8.695114 | 10.408924 | 8.317807 | 8.539768 | 8.391261 | 9.031357 | 9.183375 | 9.486157 | 9.758234 | 8.580486 |
hep-th/0602077 | Ion I. Cot?escu | Ion I. Cot\u{a}escu, Radu Racoceanu and Cosmin Crucean | Remarks on the spherical waves of the Dirac field on de Sitter spacetime | 7 pages, no figures | Mod.Phys.Lett.A21:1313-1318,2006 | 10.1142/S0217732306020044 | null | hep-th | null | The Shishkin's solutions of the Dirac equation in spherical moving frames of
the de Sitter spacetime are investigated pointing out the set of commuting
operators whose eigenvalues determine the integration constants. It is shown
that these depend on the usual angular quantum numbers and, in addition, on the
value of ... | [
{
"created": "Wed, 8 Feb 2006 10:19:40 GMT",
"version": "v1"
}
] | 2010-11-11 | [
[
"Cotăescu",
"Ion I.",
""
],
[
"Racoceanu",
"Radu",
""
],
[
"Crucean",
"Cosmin",
""
]
] | The Shishkin's solutions of the Dirac equation in spherical moving frames of the de Sitter spacetime are investigated pointing out the set of commuting operators whose eigenvalues determine the integration constants. It is shown that these depend on the usual angular quantum numbers and, in addition, on the value of th... | 22.67207 | 26.14818 | 22.511709 | 21.220873 | 20.393581 | 23.351009 | 26.040197 | 22.902037 | 24.043333 | 25.467409 | 21.344028 | 20.733208 | 21.075329 | 21.13073 | 20.770874 | 21.210888 | 20.239349 | 20.714787 | 20.526991 | 20.977419 | 22.739365 |
hep-th/0212150 | Johannes Walcher | A. Buchel, J. Walcher | The Tachyon does Matter | 8 pages, Talk given at 35th Symposium Ahrenshoop, Contribution to the
Proceedings | Fortsch.Phys.51:885-891,2003 | 10.1002/prop.200310112 | null | hep-th | null | We review the concept of S-branes introduced by Gutperle and Strominger
hep-th/0202210. Using the effective spacetime description of the rolling
tachyon worldsheets discussed by Sen, we analyze the possibility that the
gravitational backreaction of tachyon matter is important in the time-dependent
process. We show th... | [
{
"created": "Thu, 12 Dec 2002 22:05:08 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Buchel",
"A.",
""
],
[
"Walcher",
"J.",
""
]
] | We review the concept of S-branes introduced by Gutperle and Strominger hep-th/0202210. Using the effective spacetime description of the rolling tachyon worldsheets discussed by Sen, we analyze the possibility that the gravitational backreaction of tachyon matter is important in the time-dependent process. We show that... | 9.18299 | 10.343066 | 10.89738 | 8.813627 | 9.643143 | 10.620067 | 9.52304 | 8.150002 | 8.079265 | 10.962431 | 9.170495 | 8.533569 | 8.964569 | 8.351886 | 8.197325 | 8.261886 | 8.146266 | 8.245979 | 8.333077 | 8.977999 | 7.881222 |
hep-th/0702066 | Vladimir Miransky | Alex Buchel, Junji Jia, V.A.Miransky | Dynamical stabilization of runaway potentials and landscape of vacua at
finite density | 24 pages, LaTeX; v.3: to match Nucl.Phys.B version | Nucl.Phys.B772:323-339,2007 | 10.1016/j.nuclphysb.2007.03.009 | UWO-TH-07/05 | hep-th cond-mat.supr-con hep-ph | null | We study a SU(2) gauge theory with a classical complex modulus. Introducing a
chemical potential for a conserved modulus hypercharge causes it to become
unstable and start condensing. We show that the modulus condensation in turn
generates homogeneous but anisotropic non-abelian field strength condensates.
The existe... | [
{
"created": "Fri, 9 Feb 2007 09:06:36 GMT",
"version": "v1"
},
{
"created": "Sat, 10 Feb 2007 01:01:24 GMT",
"version": "v2"
},
{
"created": "Mon, 7 May 2007 22:36:13 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Buchel",
"Alex",
""
],
[
"Jia",
"Junji",
""
],
[
"Miransky",
"V. A.",
""
]
] | We study a SU(2) gauge theory with a classical complex modulus. Introducing a chemical potential for a conserved modulus hypercharge causes it to become unstable and start condensing. We show that the modulus condensation in turn generates homogeneous but anisotropic non-abelian field strength condensates. The existenc... | 8.142062 | 8.33367 | 8.123103 | 7.791605 | 8.345438 | 8.385212 | 8.375457 | 7.521856 | 8.145891 | 8.758291 | 8.324541 | 7.840296 | 8.163449 | 7.766019 | 7.824755 | 7.88606 | 8.140748 | 7.905013 | 7.914397 | 8.039421 | 8.075835 |
hep-th/0401066 | Vasilis Niarchos | Vasilis Niarchos | Notes on Tachyon Effective Actions and Veneziano Amplitudes | harvmac, 31 pages, 15 figures; v2 minor text modifications | Phys.Rev. D69 (2004) 106009 | 10.1103/PhysRevD.69.106009 | null | hep-th | null | In a previous paper (hep-th/0304045) it has been argued that tachyonic
Dirac-Born-Infeld (DBI) actions can be obtained from open string theory in a
limit, which generalizes the usual massless DBI limit. In the present note we
review this construction focusing on a key property of the proposed tachyon
effective action... | [
{
"created": "Mon, 12 Jan 2004 19:21:15 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Jan 2004 16:23:42 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Niarchos",
"Vasilis",
""
]
] | In a previous paper (hep-th/0304045) it has been argued that tachyonic Dirac-Born-Infeld (DBI) actions can be obtained from open string theory in a limit, which generalizes the usual massless DBI limit. In the present note we review this construction focusing on a key property of the proposed tachyon effective actions:... | 8.398993 | 7.654027 | 7.853248 | 7.429222 | 7.425626 | 7.297873 | 7.506316 | 7.337063 | 7.029699 | 9.354712 | 7.40385 | 7.303423 | 7.875157 | 7.296882 | 7.394396 | 7.609692 | 7.303646 | 7.130576 | 7.421466 | 7.926075 | 7.115463 |
2406.02067 | Dijs de Neeling | Dijs de Neeling, Diederik Roest, Marcello Seri, Holger Waalkens | Bertran\v{d}s Theorem and the Double Copy of Relativistic Field Theories | 9 pages | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Which relativistic field theories give rise to Kepler dynamics in the
two-body problem? We consider a class of Hamiltonians that is the unique
relativistic extension of the Kepler problem preserving its so(4) algebra, and
have orbits related through time reparametrisation to orbits of the original
Kepler problem. For... | [
{
"created": "Tue, 4 Jun 2024 07:49:41 GMT",
"version": "v1"
}
] | 2024-06-05 | [
[
"de Neeling",
"Dijs",
""
],
[
"Roest",
"Diederik",
""
],
[
"Seri",
"Marcello",
""
],
[
"Waalkens",
"Holger",
""
]
] | Which relativistic field theories give rise to Kepler dynamics in the two-body problem? We consider a class of Hamiltonians that is the unique relativistic extension of the Kepler problem preserving its so(4) algebra, and have orbits related through time reparametrisation to orbits of the original Kepler problem. For t... | 21.190048 | 21.366907 | 22.783438 | 18.982548 | 18.519478 | 18.341606 | 21.522562 | 18.072872 | 17.899837 | 22.3577 | 18.573332 | 17.054529 | 19.861452 | 18.292698 | 17.746086 | 17.700769 | 18.013117 | 18.381939 | 17.495329 | 19.317541 | 18.88625 |
1805.12153 | Ryusuke Jinno | Ryusuke Jinno | Machine learning for bounce calculation | 8 pages, 11 figures | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the possibility of using machine learning for the calculation of the
bounce action in quantum tunneling. Adopting supervised learning, we train
neural network to give the bounce action from a given potential. It is found
that, for one-dimensional tunneling, even a simple neural network performs at a
percent ... | [
{
"created": "Wed, 30 May 2018 18:00:35 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Jun 2018 14:10:59 GMT",
"version": "v2"
},
{
"created": "Sun, 10 Jun 2018 04:51:38 GMT",
"version": "v3"
}
] | 2018-06-12 | [
[
"Jinno",
"Ryusuke",
""
]
] | We study the possibility of using machine learning for the calculation of the bounce action in quantum tunneling. Adopting supervised learning, we train neural network to give the bounce action from a given potential. It is found that, for one-dimensional tunneling, even a simple neural network performs at a percent le... | 11.417206 | 8.648991 | 9.499189 | 9.350454 | 8.920651 | 8.570375 | 8.875511 | 10.213593 | 9.642421 | 10.971357 | 9.275526 | 10.174558 | 10.36754 | 10.120273 | 9.342723 | 9.802291 | 9.545282 | 10.162505 | 9.669399 | 10.99343 | 9.19379 |
hep-th/0411043 | Paolo Grinza | P. Grinza and B. Ponsot | Form factors in the massless coset models su(2)_{k+1} \otimes su(2)_k
/su(2)_{2k+1} - Part I | 18 pages, 4 eps figures, LaTeX; v2: non-unitary case k=-1 added (this
extra result is not to be found in the published NPB version) | Nucl.Phys. B714 (2005) 357-375 | 10.1016/j.nuclphysb.2005.02.004 | null | hep-th cond-mat.stat-mech math-ph math.MP | null | Massless flows between the coset model su(2)_{k+1} \otimes su(2)_k
/su(2)_{2k+1} and the minimal model M_{k+2} are studied from the viewpoint of
form factors. These flows include in particular the flow between the
Tricritical Ising model and the Ising model. Form factors of the trace operator
with an arbitrary number... | [
{
"created": "Wed, 3 Nov 2004 11:52:17 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Feb 2005 13:26:49 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Grinza",
"P.",
""
],
[
"Ponsot",
"B.",
""
]
] | Massless flows between the coset model su(2)_{k+1} \otimes su(2)_k /su(2)_{2k+1} and the minimal model M_{k+2} are studied from the viewpoint of form factors. These flows include in particular the flow between the Tricritical Ising model and the Ising model. Form factors of the trace operator with an arbitrary number o... | 8.873829 | 7.903963 | 9.862985 | 7.872035 | 8.184321 | 8.099458 | 7.881831 | 7.956657 | 7.508676 | 11.729859 | 7.231935 | 7.68348 | 8.604273 | 7.655909 | 8.002434 | 7.619862 | 7.49997 | 7.923124 | 7.822528 | 9.097032 | 7.838469 |
hep-th/0204183 | Ian Kogan | A. Gorsky, I.I. Kogan and G. Korchemsky | High Energy QCD: Stringy Picture from Hidden Integrability | 37 pages, 3 figures | JHEP 0205:053,2002 | 10.1088/1126-6708/2002/05/053 | IHES/P/02/21,ITEP-TH-12/02,LPTHE-02-19,LPT-Orsay-02-15,OUTP-02-06 | hep-th hep-ph nlin.SI | null | We discuss the stringy properties of high-energy QCD using its hidden
integrability in the Regge limit and on the light-cone. It is shown that
multi-colour QCD in the Regge limit belongs to the same universality class as
superconformal $\cal{N}$=2 SUSY YM with $N_f=2N_c$ at the strong coupling
orbifold point. The ana... | [
{
"created": "Mon, 22 Apr 2002 17:01:28 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Gorsky",
"A.",
""
],
[
"Kogan",
"I. I.",
""
],
[
"Korchemsky",
"G.",
""
]
] | We discuss the stringy properties of high-energy QCD using its hidden integrability in the Regge limit and on the light-cone. It is shown that multi-colour QCD in the Regge limit belongs to the same universality class as superconformal $\cal{N}$=2 SUSY YM with $N_f=2N_c$ at the strong coupling orbifold point. The analo... | 9.365486 | 9.597032 | 9.975564 | 9.015298 | 9.488718 | 9.711238 | 9.614337 | 10.505813 | 9.080875 | 10.454127 | 9.37229 | 9.45357 | 9.135163 | 8.951221 | 9.255724 | 9.363307 | 9.437962 | 9.102432 | 9.17942 | 9.237692 | 8.970542 |
1102.3423 | Noriaki Ogawa | Tatsuo Azeyanagi, Noriaki Ogawa and Seiji Terashima | On Non-Chiral Extension of Kerr/CFT | 29 pages, LaTeX; v2: minor corrections, references added | JHEP 1106:081,2011 | 10.1007/JHEP06(2011)081 | KUNS-2321, YITP-1121 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss possible non-chiral extension of the Kerr/CFT correspondence. We
first consider the near horizon geometry of an extremal BTZ black hole and
study the asymptotic symmetry. In order to define it properly, we introduce a
regularization and show that the asymptotic symmetry becomes the desirable
non-chiral Vir... | [
{
"created": "Wed, 16 Feb 2011 20:44:43 GMT",
"version": "v1"
},
{
"created": "Sat, 9 Apr 2011 04:44:35 GMT",
"version": "v2"
}
] | 2011-06-24 | [
[
"Azeyanagi",
"Tatsuo",
""
],
[
"Ogawa",
"Noriaki",
""
],
[
"Terashima",
"Seiji",
""
]
] | We discuss possible non-chiral extension of the Kerr/CFT correspondence. We first consider the near horizon geometry of an extremal BTZ black hole and study the asymptotic symmetry. In order to define it properly, we introduce a regularization and show that the asymptotic symmetry becomes the desirable non-chiral Viras... | 8.097571 | 7.751668 | 7.784647 | 7.267438 | 7.541638 | 8.077281 | 7.86698 | 7.700225 | 7.833687 | 8.525094 | 7.470467 | 7.735501 | 8.24719 | 7.948782 | 7.889571 | 7.749161 | 7.731305 | 7.705169 | 7.88467 | 8.484948 | 7.673085 |
hep-th/9502007 | A. A. Kehagias | N.A. Batakis and A.A. Kehagias | Anisotropic space-times in homogeneous string cosmology | 18 pages, Latex, no figures | Nucl.Phys. B449 (1995) 248-264 | 10.1016/0550-3213(95)00249-R | CERN-TH/95-14 | hep-th gr-qc | null | The dynamics of the early universe may have been profoundly influenced by
spatial anisotropies. A search for such backgrounds in the context of string
cosmology has uncovered the existence of an entire class of (spatatially)
homogeneous but not necessarily isotropic space-times, analogous to the class
of Bianchi-type... | [
{
"created": "Wed, 1 Feb 1995 16:33:00 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Batakis",
"N. A.",
""
],
[
"Kehagias",
"A. A.",
""
]
] | The dynamics of the early universe may have been profoundly influenced by spatial anisotropies. A search for such backgrounds in the context of string cosmology has uncovered the existence of an entire class of (spatatially) homogeneous but not necessarily isotropic space-times, analogous to the class of Bianchi-types ... | 13.511825 | 14.105184 | 13.704947 | 12.657185 | 13.817989 | 13.319106 | 13.576182 | 12.814678 | 13.779048 | 13.89137 | 12.449745 | 14.090037 | 13.142644 | 13.455936 | 14.246032 | 13.945803 | 13.883437 | 13.529136 | 14.323079 | 13.67102 | 13.327372 |
2408.00866 | Matthew Buican | Mahesh Balasubramanian, Matthew Buican, and Rajath Radhakrishnan | On the Classification of Bosonic and Fermionic One-Form Symmetries in
$2+1$d and 't Hooft Anomaly Matching | 56 pages and 10 figures | null | null | null | hep-th cond-mat.str-el math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the fundamental role that bosonic and fermionic symmetries play
in physics, we study (non-invertible) one-form symmetries in $2 + 1$d
consisting of topological lines with bosonic and fermionic self-statistics. We
refer to these lines as Bose-Fermi-Braided (BFB) symmetries and argue that they
can be class... | [
{
"created": "Thu, 1 Aug 2024 18:37:24 GMT",
"version": "v1"
}
] | 2024-08-05 | [
[
"Balasubramanian",
"Mahesh",
""
],
[
"Buican",
"Matthew",
""
],
[
"Radhakrishnan",
"Rajath",
""
]
] | Motivated by the fundamental role that bosonic and fermionic symmetries play in physics, we study (non-invertible) one-form symmetries in $2 + 1$d consisting of topological lines with bosonic and fermionic self-statistics. We refer to these lines as Bose-Fermi-Braided (BFB) symmetries and argue that they can be classif... | 8.546447 | 8.309207 | 10.448625 | 7.801007 | 8.062384 | 8.353208 | 8.256909 | 8.052481 | 8.468749 | 10.427774 | 8.153436 | 8.146755 | 9.283974 | 8.291713 | 8.213451 | 8.330918 | 8.020769 | 8.323118 | 8.330186 | 9.169107 | 7.950731 |
hep-th/9205104 | J. S. Park | Jae-Suk Park | Universal Bundle, Generalized Russian Formula and Non-Abelian Anomaly in
Topological Yang-Mills Theory | 16 pages, harvmac TeX, ESENAT-92-07, (TeXnical and stupid errors are
corrected.) | null | null | null | hep-th | null | We re-examine the geometry and algebraic structure of BRST's of Topological
Yang-Mills theory based on the universal bundle formalism of Atiyah and Singer.
This enables us to find a natural generalization of the {\it Russian formula
and descent equations\/}, which can be used as algebraic method to find the
non-Abeli... | [
{
"created": "Thu, 28 May 1992 20:40:00 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Jul 1992 21:26:00 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Park",
"Jae-Suk",
""
]
] | We re-examine the geometry and algebraic structure of BRST's of Topological Yang-Mills theory based on the universal bundle formalism of Atiyah and Singer. This enables us to find a natural generalization of the {\it Russian formula and descent equations\/}, which can be used as algebraic method to find the non-Abelian... | 14.123576 | 12.338935 | 15.032401 | 12.42878 | 12.405042 | 12.713548 | 13.188013 | 11.92312 | 12.161289 | 16.09411 | 12.69646 | 12.983187 | 14.485839 | 12.72363 | 12.664788 | 13.119445 | 13.508588 | 13.021009 | 13.130817 | 14.20939 | 12.813792 |
0804.2168 | Aninda Sinha | Robert C. Myers, Aninda Sinha | The fast life of holographic mesons | 42 pages, 23 figures, v2: minor changes, references added, v3: minor
changes, references added, final version | JHEP 0806:052,2008 | 10.1088/1126-6708/2008/06/052 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use holographic techniques to study meson quasiparticles moving through a
thermal plasma in N=2 super-Yang-Mills theory, with gauge group SU(N_c) and
coupled to N_f flavours of fundamental matter. This holographic approach
reliably describes the system at large N_c, large 't Hooft coupling and
N_f/N_c<<1. The meso... | [
{
"created": "Mon, 14 Apr 2008 15:39:49 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Apr 2008 14:27:52 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Jun 2008 14:21:16 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Myers",
"Robert C.",
""
],
[
"Sinha",
"Aninda",
""
]
] | We use holographic techniques to study meson quasiparticles moving through a thermal plasma in N=2 super-Yang-Mills theory, with gauge group SU(N_c) and coupled to N_f flavours of fundamental matter. This holographic approach reliably describes the system at large N_c, large 't Hooft coupling and N_f/N_c<<1. The meson ... | 7.407171 | 7.243634 | 8.538787 | 6.988313 | 7.213185 | 7.164484 | 7.354259 | 7.314476 | 7.050452 | 8.44644 | 7.35479 | 7.354537 | 7.603874 | 7.171282 | 7.158197 | 7.359105 | 7.146442 | 7.264364 | 7.087466 | 7.527923 | 7.018632 |
hep-th/9611200 | Youjin Zhang | Boris Dubrovin and Youjin Zhang | Extended affine Weyl groups and Frobenius manifolds | 69 pages, amslatex, some references added, position of Table 1 is
corrected. Revised version for Compositio Mathematica | Compositio Mathematica 111 (1998), 167--219 | null | SISSA Ref. 67/96/FM | hep-th | null | We define certain extensions of affine Weyl groups (distinct from these
considered by K. Saito [S1] in the theory of extended affine root systems),
prove an analogue of Chevalley theorem for their invariants, and construct a
Frobenius structure on their orbit spaces. This produces solutions $F(t_1, ...,
t_n)$ of WDVV... | [
{
"created": "Sun, 24 Nov 1996 14:54:38 GMT",
"version": "v1"
},
{
"created": "Wed, 20 May 1998 09:50:20 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Dubrovin",
"Boris",
""
],
[
"Zhang",
"Youjin",
""
]
] | We define certain extensions of affine Weyl groups (distinct from these considered by K. Saito [S1] in the theory of extended affine root systems), prove an analogue of Chevalley theorem for their invariants, and construct a Frobenius structure on their orbit spaces. This produces solutions $F(t_1, ..., t_n)$ of WDVV e... | 9.170674 | 12.310435 | 12.16693 | 10.004953 | 12.78234 | 13.49418 | 11.475904 | 11.112065 | 9.962687 | 11.911773 | 10.471671 | 9.710085 | 10.163793 | 9.27289 | 9.551834 | 8.916833 | 10.154596 | 9.857784 | 9.328353 | 9.820345 | 9.290273 |
2407.01136 | Yuri Makeenko | Yuri Makeenko | The Nambu-Goto string as higher-derivative Liouville theory | 5 pages in PRL style; v2: polished | null | null | ITEP-TH-16/24 | hep-th cond-mat.stat-mech hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I propose a generalization of the Liouville action which corresponds to the
Nambu-Goto string like the usual Liouville action corresponds to the Polyakov
string. The two differ by higher-derivative terms which are negligible
classically but revive quantumly. An equivalence with the four-derivative
action suggests tha... | [
{
"created": "Mon, 1 Jul 2024 09:58:50 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Jul 2024 11:09:00 GMT",
"version": "v2"
}
] | 2024-07-09 | [
[
"Makeenko",
"Yuri",
""
]
] | I propose a generalization of the Liouville action which corresponds to the Nambu-Goto string like the usual Liouville action corresponds to the Polyakov string. The two differ by higher-derivative terms which are negligible classically but revive quantumly. An equivalence with the four-derivative action suggests that ... | 11.826989 | 10.46902 | 11.949675 | 9.884515 | 11.496681 | 10.631183 | 10.380861 | 10.866542 | 11.253778 | 11.805424 | 9.742422 | 10.311564 | 10.557501 | 10.572113 | 10.650325 | 10.721852 | 10.720291 | 10.73788 | 10.645303 | 10.775641 | 10.630795 |
1312.1350 | Marco Bochicchio | Marco Bochicchio | Yang-Mills mass gap, Floer homology, glueball spectrum, and conformal
window in large-N QCD | 68 pages, latex; some comments on Veneziano limit changed, some typos
fixed | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Morse-Smale-Floer homology associates the critical points of the action
functional of a classical field theory over a manifold to its homology. We
associate to the intersection homology of certain Lagrangian submanifolds of
R^4 the critical points of a quantum effective action of large-N SU(N) YM. For
this purpose we... | [
{
"created": "Wed, 4 Dec 2013 21:00:23 GMT",
"version": "v1"
},
{
"created": "Wed, 7 May 2014 15:55:11 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Sep 2014 04:12:31 GMT",
"version": "v3"
}
] | 2014-09-18 | [
[
"Bochicchio",
"Marco",
""
]
] | Morse-Smale-Floer homology associates the critical points of the action functional of a classical field theory over a manifold to its homology. We associate to the intersection homology of certain Lagrangian submanifolds of R^4 the critical points of a quantum effective action of large-N SU(N) YM. For this purpose we c... | 13.166498 | 13.182565 | 14.637191 | 12.58025 | 13.944972 | 13.004438 | 14.283344 | 13.00673 | 12.343239 | 15.677672 | 13.236685 | 12.35192 | 12.749083 | 12.755415 | 12.52948 | 12.771997 | 12.608044 | 12.626289 | 12.653844 | 12.801355 | 12.78394 |
hep-th/0106237 | Danny Birmingham | Danny Birmingham and Massimiliano Rinaldi | Brane World in a Topological Black Hole Bulk | Latex, 8 pages, v2: Additional references, to appear in MPLA | Mod.Phys.Lett. A16 (2001) 1887-1894 | 10.1142/S0217732301005254 | null | hep-th | null | We consider a static brane in the background of a topological black hole, in
arbitrary dimensions. For hyperbolic horizons, we find a solution only when the
black hole mass assumes its minimum negative value. In this case, the tension
of the brane vanishes, and the brane position coincides with the location of
the ho... | [
{
"created": "Tue, 26 Jun 2001 10:54:18 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Oct 2001 14:49:20 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Birmingham",
"Danny",
""
],
[
"Rinaldi",
"Massimiliano",
""
]
] | We consider a static brane in the background of a topological black hole, in arbitrary dimensions. For hyperbolic horizons, we find a solution only when the black hole mass assumes its minimum negative value. In this case, the tension of the brane vanishes, and the brane position coincides with the location of the hori... | 7.178765 | 6.551929 | 6.334241 | 6.271237 | 6.294921 | 6.442504 | 6.462411 | 5.748273 | 6.068801 | 6.692412 | 6.517114 | 6.741024 | 6.781495 | 6.575789 | 6.769763 | 6.756849 | 6.906126 | 6.556262 | 6.393905 | 7.10605 | 6.707567 |
hep-th/0209130 | Tim Morris | Stefano Arnone, Antonio Gatti, Tim R. Morris | Towards a manifestly gauge invariant and universal calculus for
Yang-Mills theory | LaTeX, 14 pages, 12 figs, merged from talks hep-th/0207154 and
hep-th/0207153, to be published in Acta Physica Slavonica | Acta Phys.Slov. 52 (2002) 621-634 | null | SHEP 02-21 | hep-th cond-mat hep-lat hep-ph | null | A manifestly gauge invariant exact renormalization group for pure SU(N)
Yang-Mills theory is proposed, along with the necessary gauge invariant
regularisation which implements the effective cutoff. The latter is naturally
incorporated by embedding the theory into a spontaneously broken SU(N|N)
super-gauge theory, whi... | [
{
"created": "Mon, 16 Sep 2002 16:10:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Arnone",
"Stefano",
""
],
[
"Gatti",
"Antonio",
""
],
[
"Morris",
"Tim R.",
""
]
] | A manifestly gauge invariant exact renormalization group for pure SU(N) Yang-Mills theory is proposed, along with the necessary gauge invariant regularisation which implements the effective cutoff. The latter is naturally incorporated by embedding the theory into a spontaneously broken SU(N|N) super-gauge theory, which... | 10.177114 | 8.216918 | 12.052959 | 8.373161 | 8.449914 | 8.364974 | 8.017557 | 8.485462 | 8.414204 | 11.451032 | 8.43775 | 9.243174 | 10.352374 | 9.529949 | 9.529862 | 9.375224 | 9.399162 | 9.526589 | 9.904212 | 9.875317 | 9.56955 |
1304.6581 | Sho Tanaka | Sho Tanaka | Where Does Black Hole Entropy Lie? Some Remarks on Area-Entropy Law,
Holographic Principle and Noncommutative Space-Time | 20 pages, punctuation errors corrected and minor modification in
English xplanation. arXiv admin note: substantial text overlap with
arXiv:1102.3448, arXiv:1006.2885, arXiv:0905.1446 | Eur.Phys.J.Plus(2014)129:11 | 10.1140/epjp/i2014-14011-9 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In confrontation with serious and fundamental problems towards ultimate
theory of quantum gravity and physics of Planck scale, we emphasize the
importance of underlying noncommutative space-time such as Snyder's or Yang's
Lorentz-covariant quantized space-time. The background of Bekenstein-Hawking's
Area-entropy law ... | [
{
"created": "Wed, 24 Apr 2013 13:29:40 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jul 2013 13:10:43 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Jul 2013 05:06:51 GMT",
"version": "v3"
},
{
"created": "Mon, 27 Jan 2014 06:28:13 GMT",
"version": "v4"
}
] | 2014-01-28 | [
[
"Tanaka",
"Sho",
""
]
] | In confrontation with serious and fundamental problems towards ultimate theory of quantum gravity and physics of Planck scale, we emphasize the importance of underlying noncommutative space-time such as Snyder's or Yang's Lorentz-covariant quantized space-time. The background of Bekenstein-Hawking's Area-entropy law an... | 10.142537 | 9.962826 | 10.86918 | 9.823174 | 9.798882 | 9.921696 | 9.766858 | 9.492908 | 9.518032 | 10.314624 | 9.822668 | 9.81112 | 10.164066 | 9.811775 | 9.88078 | 9.822729 | 9.866837 | 10.01322 | 10.005407 | 10.285363 | 9.751977 |
0911.2786 | Hael Collins | Hael Collins | Enhancing non-Gaussianities by breaking local Lorentz invariance | 10 pages, 1 figure; a talk presented at the Invisible Universe
International Conference at the Palais de l'UNESCO, Paris | AIP Conf.Proc.1241:551-560,2010 | 10.1063/1.3462684 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This talk briefly explains how the breaking of a Lorentz-invariant
description of nature at tiny space-time intervals might affect the
non-Gaussian character of the primordial fluctuations left by inflation. For
example, a model that contains irrelevant operators that only preserve the
spatial symmetries along consta... | [
{
"created": "Sat, 14 Nov 2009 16:37:41 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Collins",
"Hael",
""
]
] | This talk briefly explains how the breaking of a Lorentz-invariant description of nature at tiny space-time intervals might affect the non-Gaussian character of the primordial fluctuations left by inflation. For example, a model that contains irrelevant operators that only preserve the spatial symmetries along constant... | 17.063126 | 15.643281 | 14.387091 | 14.434445 | 17.802286 | 17.663254 | 17.423084 | 15.384615 | 15.025084 | 17.656984 | 16.006666 | 15.971758 | 15.326097 | 14.953596 | 15.814443 | 15.571772 | 15.909478 | 15.715867 | 14.894831 | 16.160248 | 15.825011 |
hep-th/9212043 | null | Ezra Getzler (Department of Mathematics, MIT) | Batalin-Vilkovisky algebras and two-dimensional topological field
theories | 23 pages (Revised in many small ways.) | Commun.Math.Phys.159:265-285,1994 | 10.1007/BF02102639 | null | hep-th | null | Batalin-Vilkovisky algebras are a new type of algebraic structure on graded
vector spaces, which first arose in the work of Batalin and Vilkovisky on gauge
fixing in quantum field theory. In this article, we show that there is a
natural structure of a Batalin-Vilkovisky algebra on the cohomology of a
topological fiel... | [
{
"created": "Mon, 7 Dec 1992 18:06:28 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Feb 1993 13:37:26 GMT",
"version": "v2"
},
{
"created": "Tue, 4 May 1993 23:21:19 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Getzler",
"Ezra",
"",
"Department of Mathematics, MIT"
]
] | Batalin-Vilkovisky algebras are a new type of algebraic structure on graded vector spaces, which first arose in the work of Batalin and Vilkovisky on gauge fixing in quantum field theory. In this article, we show that there is a natural structure of a Batalin-Vilkovisky algebra on the cohomology of a topological field ... | 4.94082 | 5.827668 | 5.577101 | 5.379532 | 5.187551 | 5.528497 | 5.67778 | 5.248028 | 5.399683 | 6.344823 | 5.152691 | 4.800612 | 5.390951 | 5.075878 | 4.766075 | 4.942161 | 4.960485 | 4.905013 | 4.903135 | 5.048343 | 4.915423 |
0908.1865 | Richard Battye | Richard A. Battye, Jonathan A. Pearson, Simon Pike and Paul M.
Sutcliffe | Formation and evolution of kinky vortons | null | JCAP 0909:039,2009 | 10.1088/1475-7516/2009/09/039 | DCPT-09/55 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present field theory simulations of a model with Z_2xU(1) symmetry in
(2+1)-dimensions. This model has two discrete vacua, allowing for domain walls,
and also a conserved Noether charge. For initial conditions in which the field
is placed in one of the vacua and given a homogeneous background charge, we
find that ... | [
{
"created": "Thu, 13 Aug 2009 10:25:11 GMT",
"version": "v1"
}
] | 2009-11-02 | [
[
"Battye",
"Richard A.",
""
],
[
"Pearson",
"Jonathan A.",
""
],
[
"Pike",
"Simon",
""
],
[
"Sutcliffe",
"Paul M.",
""
]
] | We present field theory simulations of a model with Z_2xU(1) symmetry in (2+1)-dimensions. This model has two discrete vacua, allowing for domain walls, and also a conserved Noether charge. For initial conditions in which the field is placed in one of the vacua and given a homogeneous background charge, we find that th... | 10.165917 | 10.778594 | 10.445748 | 9.914766 | 10.608822 | 10.494164 | 10.490367 | 10.031314 | 9.986197 | 10.948397 | 10.263966 | 10.248364 | 9.994606 | 10.147075 | 9.943754 | 10.058011 | 9.663062 | 9.909969 | 10.064259 | 9.735776 | 10.09575 |
1312.7197 | Hiroshi Kunitomo | Hiroshi Kunitomo | The Ramond Sector of Heterotic String Field Theory | 33 pages, 5 figures, uses PTPTeX.cls, v2:forms of general terms in
EOM and the action are modified, v3:some explanations are improved, one extra
appendix is added, published version, v4:an error is corrected,v5;typos in
appA, v6:typos | null | 10.1093/ptep/ptu032 | YITP-13-131 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We attempt to construct the full equations of motion for the Neveu-Schwarz
and the Ramond sectors of the heterotic string field theory. Although they are
non-polynomial also in the Ramond string field $\Psi$, we can construct them
order by order in $\Psi$. Their explicit forms with the gauge transformations
are given... | [
{
"created": "Fri, 27 Dec 2013 06:13:17 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jan 2014 09:07:51 GMT",
"version": "v2"
},
{
"created": "Mon, 17 Feb 2014 06:38:29 GMT",
"version": "v3"
},
{
"created": "Fri, 28 Feb 2014 07:45:43 GMT",
"version": "v4"
},
{
"cr... | 2014-05-07 | [
[
"Kunitomo",
"Hiroshi",
""
]
] | We attempt to construct the full equations of motion for the Neveu-Schwarz and the Ramond sectors of the heterotic string field theory. Although they are non-polynomial also in the Ramond string field $\Psi$, we can construct them order by order in $\Psi$. Their explicit forms with the gauge transformations are given u... | 8.487681 | 7.395137 | 9.176711 | 7.096786 | 7.976214 | 8.406871 | 7.911555 | 7.89031 | 7.214333 | 8.879158 | 7.829193 | 7.877386 | 7.840175 | 7.683914 | 7.850041 | 8.055033 | 7.724322 | 7.6175 | 7.859772 | 8.291884 | 7.752265 |
hep-th/0211245 | Hiroshi Itoyama | H. Itoyama, A. Morozov | The Dijkgraaf-Vafa prepotential in the context of general Seiberg-Witten
theory | a few changes, references added, typo corrected | Nucl.Phys.B657:53-78,2003 | 10.1016/S0550-3213(03)00172-X | OCU-PHYS-194, ITEP/TH-57/02 | hep-th | null | We consider the prepotential of Dijkgraaf and Vafa (DV) as one more (and in
fact, singular) example of the Seiberg-Witten (SW) prepotentials and discuss
its properties from this perspective. Most attention is devoted to the issue of
complete system of moduli, which should include not only the sizes of the cuts
(in ma... | [
{
"created": "Mon, 25 Nov 2002 17:00:30 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Nov 2002 08:28:34 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Itoyama",
"H.",
""
],
[
"Morozov",
"A.",
""
]
] | We consider the prepotential of Dijkgraaf and Vafa (DV) as one more (and in fact, singular) example of the Seiberg-Witten (SW) prepotentials and discuss its properties from this perspective. Most attention is devoted to the issue of complete system of moduli, which should include not only the sizes of the cuts (in matr... | 12.987735 | 14.828699 | 16.275877 | 12.743874 | 13.224549 | 13.05901 | 12.02265 | 12.047476 | 12.628638 | 15.138949 | 12.40389 | 12.196042 | 13.146405 | 12.400484 | 12.264722 | 12.205253 | 12.439764 | 12.259475 | 12.30137 | 12.745298 | 12.494075 |
1803.09911 | Dong-Gang Wang | Andrei Linde, Dong-Gang Wang, Yvette Welling, Yusuke Yamada, and Ana
Achucarro | Hypernatural inflation | 25 pages, 8 figures; v2: published version with references added and
discussion extended | JCAP 07 (2018) 035 | 10.1088/1475-7516/2018/07/035 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We constructed a model of natural inflation in the context of
$\alpha$-attractor supergravity, in which both the dilaton field and the axion
field are light during inflation, and the inflaton may be a combination of the
two. The T-model version of this theory is defined on the Poincare disk with
radius |Z| = 1. It de... | [
{
"created": "Tue, 27 Mar 2018 06:26:50 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jul 2018 09:25:39 GMT",
"version": "v2"
}
] | 2018-07-18 | [
[
"Linde",
"Andrei",
""
],
[
"Wang",
"Dong-Gang",
""
],
[
"Welling",
"Yvette",
""
],
[
"Yamada",
"Yusuke",
""
],
[
"Achucarro",
"Ana",
""
]
] | We constructed a model of natural inflation in the context of $\alpha$-attractor supergravity, in which both the dilaton field and the axion field are light during inflation, and the inflaton may be a combination of the two. The T-model version of this theory is defined on the Poincare disk with radius |Z| = 1. It desc... | 6.405282 | 6.252071 | 6.851141 | 6.108195 | 6.23741 | 6.217295 | 6.384728 | 6.270833 | 6.225742 | 7.110603 | 5.938065 | 6.196539 | 6.523188 | 6.210582 | 6.317491 | 6.117217 | 6.340022 | 6.268287 | 6.258592 | 6.43862 | 6.168828 |
hep-th/9112066 | Konstantinos Anagnostopoulos | Konstantinos N. Anagnostopoulos, Mark J. Bowick and Albert Schwarz | The Solution Space of the Unitary Matrix Model String Equation and the
Sato Grassmannian | 21 pages | Commun.Math.Phys. 148 (1992) 469-486 | 10.1007/BF02096545 | null | hep-th | null | The space of all solutions to the string equation of the symmetric unitary
one-matrix model is determined. It is shown that the string equation is
equivalent to simple conditions on points $V_1$ and $V_2$ in the big cell $\Gr$
of the Sato Grassmannian $Gr$. This is a consequence of a well-defined
continuum limit in w... | [
{
"created": "Sat, 21 Dec 1991 03:29:46 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Anagnostopoulos",
"Konstantinos N.",
""
],
[
"Bowick",
"Mark J.",
""
],
[
"Schwarz",
"Albert",
""
]
] | The space of all solutions to the string equation of the symmetric unitary one-matrix model is determined. It is shown that the string equation is equivalent to simple conditions on points $V_1$ and $V_2$ in the big cell $\Gr$ of the Sato Grassmannian $Gr$. This is a consequence of a well-defined continuum limit in whi... | 8.536574 | 9.001719 | 10.746372 | 8.584569 | 9.211984 | 9.054711 | 9.407769 | 8.532658 | 8.99754 | 10.893787 | 8.947843 | 8.357141 | 8.907597 | 8.374259 | 8.619857 | 8.730755 | 8.223915 | 8.341834 | 8.369032 | 8.683287 | 8.217672 |
0907.2773 | Matej Pavsic | Matej Pavsic | Beyond the Relativistic Point Particle: A Reciprocally Invariant System
and its Generalisation | 15 pages; Revised version, accepted for publication in Physics
Letters B | Phys.Lett.B680:526-532,2009 | 10.1016/j.physletb.2009.09.020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a reciprocally invariant system proposed by Low and Govaerts
et al., whose action contains both the orthogonal and the symplectic forms and
is invariant under global $O(2,4)\cap Sp(2,4)$ transformations. We find that
the general solution to the classical equations of motion has no linear term in
the ev... | [
{
"created": "Thu, 16 Jul 2009 12:46:20 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Sep 2009 12:00:07 GMT",
"version": "v2"
}
] | 2009-10-06 | [
[
"Pavsic",
"Matej",
""
]
] | We investigate a reciprocally invariant system proposed by Low and Govaerts et al., whose action contains both the orthogonal and the symplectic forms and is invariant under global $O(2,4)\cap Sp(2,4)$ transformations. We find that the general solution to the classical equations of motion has no linear term in the evol... | 10.104883 | 10.076086 | 10.608238 | 9.703465 | 10.851395 | 9.942611 | 10.266785 | 9.804098 | 9.751816 | 11.355011 | 9.698509 | 9.825902 | 10.003261 | 9.723858 | 9.586345 | 9.870507 | 9.758716 | 9.639026 | 9.626967 | 9.905674 | 10.06784 |
1201.2655 | Rutger H. Boels | Rutger H. Boels | Three particle superstring amplitudes with massive legs | 45 pages. v2: typos corrected, references added | null | 10.1007/JHEP06(2012)026 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | On-shell superspaces and associated spinor helicity techniques give an
efficient formulation of the Ward identities of on-shell supersymmetry for
scattering amplitudes and supply tools to construct their solutions. Based on
these techniques in this paper the general solutions of the Ward identities are
presented for ... | [
{
"created": "Thu, 12 Jan 2012 19:44:39 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Apr 2012 15:28:19 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Boels",
"Rutger H.",
""
]
] | On-shell superspaces and associated spinor helicity techniques give an efficient formulation of the Ward identities of on-shell supersymmetry for scattering amplitudes and supply tools to construct their solutions. Based on these techniques in this paper the general solutions of the Ward identities are presented for th... | 13.698018 | 13.208161 | 14.505767 | 11.944807 | 13.273078 | 13.731351 | 12.603852 | 13.342447 | 11.902052 | 14.397086 | 11.71765 | 11.909951 | 12.824697 | 12.378185 | 12.430704 | 12.188807 | 12.268088 | 12.499625 | 12.253203 | 13.887681 | 12.7604 |
hep-th/9712012 | Micha Berkooz | Micha Berkooz (IAS, Princeton) | String Dualities from Matrix Theory: A Summary | 7 pages, Talk given at STRINGS'97 | Nucl.Phys.Proc.Suppl. 68 (1998) 374-380 | 10.1016/S0920-5632(98)00172-8 | null | hep-th | null | I review the appearance, within Matrix theory, of the $SL(5,Z)$ U-duality
group of M-theory on $T^4$, and the duality between M-theory on K3 and the
Heterotic string on $T^3$. In both cases the duality is geometrical and
manifest.
| [
{
"created": "Sun, 30 Nov 1997 22:45:20 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Berkooz",
"Micha",
"",
"IAS, Princeton"
]
] | I review the appearance, within Matrix theory, of the $SL(5,Z)$ U-duality group of M-theory on $T^4$, and the duality between M-theory on K3 and the Heterotic string on $T^3$. In both cases the duality is geometrical and manifest. | 8.113771 | 5.644654 | 7.348775 | 5.872906 | 5.218609 | 4.966602 | 4.949305 | 5.1759 | 5.642594 | 8.605186 | 5.481171 | 5.771502 | 7.086053 | 6.110859 | 5.802301 | 5.640538 | 5.673867 | 5.51399 | 6.166026 | 6.505412 | 5.573425 |
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