id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2303.08852 | Gwena\"el Ferrando | Gwena\"el Ferrando, Amit Sever, Adar Sharon, and Elior Urisman | A Large Twist Limit for Any Operator | 54 pages, 16 figures | null | 10.1007/JHEP06(2023)028 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We argue that for any single-trace operator in ${\cal N}=4$ SYM theory there
is a large twist double-scaling limit in which the Feynman graphs have an
iterative structure. Such structure can be recast using a graph-building
operator. Generically, this operator mixes between single-trace operators with
different scali... | [
{
"created": "Wed, 15 Mar 2023 18:12:12 GMT",
"version": "v1"
}
] | 2023-06-21 | [
[
"Ferrando",
"Gwenaël",
""
],
[
"Sever",
"Amit",
""
],
[
"Sharon",
"Adar",
""
],
[
"Urisman",
"Elior",
""
]
] | We argue that for any single-trace operator in ${\cal N}=4$ SYM theory there is a large twist double-scaling limit in which the Feynman graphs have an iterative structure. Such structure can be recast using a graph-building operator. Generically, this operator mixes between single-trace operators with different scaling... | 11.968336 | 11.553871 | 12.353712 | 10.51604 | 11.430482 | 10.845383 | 11.294312 | 11.25898 | 10.842655 | 14.257004 | 10.626456 | 11.281899 | 11.511405 | 11.114015 | 11.11472 | 11.203069 | 11.365732 | 10.964332 | 11.28105 | 11.275129 | 10.981891 |
1406.1525 | Laura Mersini-Houghton | Laura Mersini-Houghton | Backreaction of Hawking Radiation on a Gravitationally Collapsing Star
I: Black Holes? | 8 pgs | PLB30496 Phys Lett B, 16 September 2014 | 10.1016/j.physletb.2014.09.018 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Particle creation leading to Hawking radiation is produced by the changing
gravitational field of the collapsing star. The two main initial conditions in
the far past placed on the quantum field from which particles arise, are the
Hartle Hawking vacuum and the Unruh vacuum. The former leads to a time
symmetric therma... | [
{
"created": "Thu, 5 Jun 2014 21:11:44 GMT",
"version": "v1"
}
] | 2014-09-22 | [
[
"Mersini-Houghton",
"Laura",
""
]
] | Particle creation leading to Hawking radiation is produced by the changing gravitational field of the collapsing star. The two main initial conditions in the far past placed on the quantum field from which particles arise, are the Hartle Hawking vacuum and the Unruh vacuum. The former leads to a time symmetric thermal ... | 7.874486 | 8.382986 | 7.918286 | 7.660423 | 7.811886 | 8.230202 | 8.163049 | 8.296416 | 8.198395 | 9.109479 | 7.796824 | 7.857034 | 7.439223 | 7.72668 | 7.719296 | 7.783564 | 7.782347 | 7.734576 | 7.893923 | 7.772497 | 7.894987 |
hep-th/0001117 | Sergey Afanas'ev | S. B. Afanas'ev | Quantization of the space-time based on a formless finite fundamental
element | LaTex | null | null | null | hep-th | null | The concept of the space (space-time) of the formless finite fundamental
elements (FFFE) is suggested. This space can be defined as a set of coverings
of the continual space by non-overlapping simply connected regions of any form
and arbitrary sizes with some probability measure. The average sizes of each
fundamental... | [
{
"created": "Wed, 19 Jan 2000 16:16:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Afanas'ev",
"S. B.",
""
]
] | The concept of the space (space-time) of the formless finite fundamental elements (FFFE) is suggested. This space can be defined as a set of coverings of the continual space by non-overlapping simply connected regions of any form and arbitrary sizes with some probability measure. The average sizes of each fundamental e... | 13.98684 | 15.79959 | 14.129663 | 13.410432 | 15.335633 | 14.574965 | 16.34141 | 14.764803 | 13.656572 | 15.780098 | 13.963753 | 14.035327 | 13.815717 | 13.662896 | 13.468258 | 13.768857 | 13.405781 | 14.051797 | 13.677589 | 13.979833 | 13.922007 |
hep-th/9903140 | Zarembo | G. W. Semenoff, K. Zarembo | Solitons on Branes | 15 pages, 2 figures; v2: two references added, version to be
published in Nucl.Phys. B | Nucl.Phys. B556 (1999) 247-261 | 10.1016/S0550-3213(99)00365-X | ITEP-TH-7/99 | hep-th | null | We examine the possibility that gauge field configurations on stacks of
parallel Dp branes support topological solitons. We give an exhaustive list of
possible soliton charges for p<7. We also discuss how configurations carrying
the soliton charges can be constructed from intersecting branes.
| [
{
"created": "Tue, 16 Mar 1999 15:07:44 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jul 1999 22:04:00 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Semenoff",
"G. W.",
""
],
[
"Zarembo",
"K.",
""
]
] | We examine the possibility that gauge field configurations on stacks of parallel Dp branes support topological solitons. We give an exhaustive list of possible soliton charges for p<7. We also discuss how configurations carrying the soliton charges can be constructed from intersecting branes. | 11.546962 | 10.122611 | 9.889488 | 9.207874 | 8.960545 | 9.98737 | 9.503327 | 9.765303 | 9.235528 | 11.089093 | 9.475091 | 9.940568 | 10.547168 | 9.546481 | 9.513871 | 9.648668 | 9.555786 | 9.653359 | 9.296346 | 10.368124 | 9.806001 |
2308.04490 | Dhruva K.S | Sachin Jain and Dhruva K.S | A Spin on the Bulk Locality of Slightly Broken Higher Spin Theories | 55 pages including appendices, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we investigate if it is possible to express correlation
functions in Large N Chern-Simons (CS) matter theories/ Slightly Broken Higher
Spin (SBHS) theories purely in terms of single trace twist conformal blocks
(TCBs). For this, we first develop the machinery for spinning TCBs. We do this
both by expli... | [
{
"created": "Tue, 8 Aug 2023 18:00:16 GMT",
"version": "v1"
}
] | 2023-08-10 | [
[
"Jain",
"Sachin",
""
],
[
"S",
"Dhruva K.",
""
]
] | In this paper, we investigate if it is possible to express correlation functions in Large N Chern-Simons (CS) matter theories/ Slightly Broken Higher Spin (SBHS) theories purely in terms of single trace twist conformal blocks (TCBs). For this, we first develop the machinery for spinning TCBs. We do this both by explici... | 8.47585 | 8.063718 | 8.53069 | 8.240026 | 8.245283 | 8.253357 | 8.068162 | 8.177277 | 7.922724 | 10.149583 | 7.989778 | 8.099415 | 8.461318 | 7.982704 | 8.269699 | 8.060985 | 8.243121 | 8.120963 | 8.01626 | 8.440442 | 8.099705 |
1202.4934 | Ralph Blumenhagen | Ralph Blumenhagen, Andreas Deser, Erik Plauschinn and Felix Rennecke | Palatini-Lovelock-Cartan Gravity - Bianchi Identities for Stringy Fluxes | 25 pages, notation improved, refs added | null | 10.1088/0264-9381/29/13/135004 | MPP-2012-10; ITP-UU-12/07; SPIN-12/06 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A Palatini-type action for Einstein and Gauss-Bonnet gravity with non-trivial
torsion is proposed. Three-form flux is incorporated via a deformation of the
Riemann tensor, and consistency of the Palatini variational principle requires
the flux to be covariantly constant and to satisfy a Jacobi identity. Studying
grav... | [
{
"created": "Wed, 22 Feb 2012 15:06:04 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Feb 2012 19:40:51 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Blumenhagen",
"Ralph",
""
],
[
"Deser",
"Andreas",
""
],
[
"Plauschinn",
"Erik",
""
],
[
"Rennecke",
"Felix",
""
]
] | A Palatini-type action for Einstein and Gauss-Bonnet gravity with non-trivial torsion is proposed. Three-form flux is incorporated via a deformation of the Riemann tensor, and consistency of the Palatini variational principle requires the flux to be covariantly constant and to satisfy a Jacobi identity. Studying gravit... | 10.440351 | 9.306254 | 11.905063 | 9.485655 | 10.097487 | 9.946767 | 10.491513 | 9.62538 | 8.758345 | 11.807231 | 9.982479 | 8.887048 | 9.814229 | 9.670884 | 9.292597 | 9.379691 | 9.341159 | 9.5914 | 9.348495 | 9.961149 | 9.426128 |
0912.3250 | Albrecht Klemm | Thomas W. Grimm, Tae-Won Ha, Albrecht Klemm, Denis Klevers | Five-Brane Superpotentials and Heterotic/F-theory Duality | 43 pages, v2: minor corrections | Nucl.Phys.B838:458-491,2010 | 10.1016/j.nuclphysb.2010.06.011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Under heterotic/F-theory duality it was argued that a wide class of heterotic
five-branes is mapped into the geometry of an F-theory compactification
manifold. In four-dimensional compactifications this identifies a five-brane
wrapped on a curve in the base of an elliptically fibered Calabi-Yau threefold
with a speci... | [
{
"created": "Wed, 16 Dec 2009 21:00:06 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jun 2010 17:24:33 GMT",
"version": "v2"
}
] | 2011-03-28 | [
[
"Grimm",
"Thomas W.",
""
],
[
"Ha",
"Tae-Won",
""
],
[
"Klemm",
"Albrecht",
""
],
[
"Klevers",
"Denis",
""
]
] | Under heterotic/F-theory duality it was argued that a wide class of heterotic five-branes is mapped into the geometry of an F-theory compactification manifold. In four-dimensional compactifications this identifies a five-brane wrapped on a curve in the base of an elliptically fibered Calabi-Yau threefold with a specifi... | 5.873954 | 5.858406 | 7.444398 | 5.809203 | 6.127881 | 6.229373 | 6.369616 | 6.200104 | 6.079734 | 7.587542 | 5.792195 | 5.753939 | 6.312155 | 5.750867 | 5.772083 | 5.702125 | 5.718603 | 5.733643 | 5.609766 | 6.172521 | 5.726429 |
2007.11759 | KaiXin Zhu | Kai-Xin Zhu, Fu-Wen Shu and Dong-Hui Du | Holographic complexity for nonlinearly charged Lifshitz black holes | 23 pages, 5 figures | null | 10.1088/1361-6382/aba843 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using "complexity=action" proposal we study the late time growth rate of
holographic complexity for nonlinear charged Lifshitz black hole with a single
horizon or two horizons. As a toy model, we consider two kinds of such black
holes: nonlinear charged Lifshitz black hole and nonlinear logarithmic charged
Lifshitz b... | [
{
"created": "Thu, 23 Jul 2020 02:23:18 GMT",
"version": "v1"
}
] | 2020-09-18 | [
[
"Zhu",
"Kai-Xin",
""
],
[
"Shu",
"Fu-Wen",
""
],
[
"Du",
"Dong-Hui",
""
]
] | Using "complexity=action" proposal we study the late time growth rate of holographic complexity for nonlinear charged Lifshitz black hole with a single horizon or two horizons. As a toy model, we consider two kinds of such black holes: nonlinear charged Lifshitz black hole and nonlinear logarithmic charged Lifshitz bla... | 8.04156 | 5.167359 | 6.363562 | 5.50062 | 5.749889 | 5.446989 | 4.99416 | 5.036337 | 4.984432 | 7.086668 | 5.47109 | 5.647549 | 6.393461 | 5.647467 | 5.419621 | 5.427413 | 5.545251 | 5.547268 | 5.620262 | 6.353108 | 5.604056 |
hep-th/9710188 | Carlo Ungarelli | A. Buonanno, K. Meissner, C. Ungarelli, G. Veneziano | Quantum Inhomogeneities in String Cosmology | 30 pages, RevteX, epsfig, 5 figures | JHEP 9801 (1998) 004 | 10.1088/1126-6708/1998/01/004 | null | hep-th gr-qc | null | Within two specific string cosmology scenarios --differing in the way the
pre- and post-big bang phases are joined-- we compute the size and spectral
slope of various types of cosmologically amplified quantum fluctuations that
arise in generic compactifications of heterotic string theory. By further
imposing that the... | [
{
"created": "Fri, 24 Oct 1997 16:34:12 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Buonanno",
"A.",
""
],
[
"Meissner",
"K.",
""
],
[
"Ungarelli",
"C.",
""
],
[
"Veneziano",
"G.",
""
]
] | Within two specific string cosmology scenarios --differing in the way the pre- and post-big bang phases are joined-- we compute the size and spectral slope of various types of cosmologically amplified quantum fluctuations that arise in generic compactifications of heterotic string theory. By further imposing that these... | 12.767522 | 13.692793 | 12.801038 | 11.769692 | 12.106725 | 14.16258 | 12.608822 | 12.234711 | 11.240047 | 13.596362 | 11.760921 | 12.026629 | 11.534105 | 11.373047 | 12.138075 | 11.738513 | 11.331243 | 11.93948 | 11.56071 | 11.758025 | 11.339904 |
2210.13479 | Ricardo Schiappa | Marcos Marino, Ricardo Schiappa, Maximilian Schwick | New Instantons for Matrix Models | 71 pages, 22 figures, 4 tables, jheppub-nosort.sty | null | null | null | hep-th cond-mat.stat-mech math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complete, nonperturbative content of random matrix models is described by
resurgent-transseries -- general solutions to their corresponding
string-equations. These transseries include exponentially-suppressed
multi-instanton amplitudes obtained by eigenvalue tunneling, but they also
contain exponentially-enhanced... | [
{
"created": "Mon, 24 Oct 2022 18:00:01 GMT",
"version": "v1"
}
] | 2022-10-26 | [
[
"Marino",
"Marcos",
""
],
[
"Schiappa",
"Ricardo",
""
],
[
"Schwick",
"Maximilian",
""
]
] | The complete, nonperturbative content of random matrix models is described by resurgent-transseries -- general solutions to their corresponding string-equations. These transseries include exponentially-suppressed multi-instanton amplitudes obtained by eigenvalue tunneling, but they also contain exponentially-enhanced a... | 15.560022 | 15.95661 | 18.002069 | 14.835595 | 16.197937 | 14.188208 | 14.964541 | 13.656926 | 14.2789 | 19.760693 | 14.841578 | 14.123873 | 15.124861 | 14.359449 | 14.587845 | 14.558007 | 14.194559 | 14.828798 | 15.197093 | 15.941198 | 14.025342 |
2007.05741 | Jarah Evslin | Jarah Evslin | Normal Ordering Normal Modes | 26 pages, no figures | null | 10.1140/epjc/s10052-021-08890-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a soliton sector of a quantum field theory, it is often convenient to
expand the quantum fields in terms of normal modes. Normal mode creation and
annihilation operators can be normal ordered, and their normal ordered products
have vanishing expectation values in the one-loop soliton ground state. The
Hamiltonian ... | [
{
"created": "Sat, 11 Jul 2020 10:48:45 GMT",
"version": "v1"
}
] | 2021-02-24 | [
[
"Evslin",
"Jarah",
""
]
] | In a soliton sector of a quantum field theory, it is often convenient to expand the quantum fields in terms of normal modes. Normal mode creation and annihilation operators can be normal ordered, and their normal ordered products have vanishing expectation values in the one-loop soliton ground state. The Hamiltonian of... | 9.775721 | 10.143627 | 9.987646 | 9.772693 | 9.920209 | 9.981769 | 10.035078 | 9.88418 | 9.715932 | 9.606377 | 9.776277 | 9.554982 | 8.852354 | 9.370002 | 9.195406 | 9.398367 | 9.355838 | 9.263376 | 9.398455 | 8.850423 | 9.054551 |
2008.12399 | Jamie Law-Smith | Michael Dine, Jamie A.P. Law-Smith, Shijun Sun, Duncan Wood, Yan Yu | Obstacles to Constructing de Sitter Space in String Theory | 20 pages. v2: references added; v3, v4: typos fixed | null | 10.1007/JHEP02(2021)050 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There have been many attempts to construct de Sitter space-times in string
theory. While arguably there have been some successes, this has proven
challenging, leading to the de Sitter swampland conjecture: quantum theories of
gravity do not admit stable or metastable de Sitter space. Here we explain
that, within cont... | [
{
"created": "Thu, 27 Aug 2020 22:51:50 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Sep 2020 23:59:22 GMT",
"version": "v2"
},
{
"created": "Mon, 28 Dec 2020 15:35:12 GMT",
"version": "v3"
},
{
"created": "Thu, 4 Feb 2021 18:51:34 GMT",
"version": "v4"
}
] | 2021-02-10 | [
[
"Dine",
"Michael",
""
],
[
"Law-Smith",
"Jamie A. P.",
""
],
[
"Sun",
"Shijun",
""
],
[
"Wood",
"Duncan",
""
],
[
"Yu",
"Yan",
""
]
] | There have been many attempts to construct de Sitter space-times in string theory. While arguably there have been some successes, this has proven challenging, leading to the de Sitter swampland conjecture: quantum theories of gravity do not admit stable or metastable de Sitter space. Here we explain that, within contro... | 8.503349 | 8.081429 | 8.865336 | 8.320715 | 8.54908 | 8.063087 | 8.143875 | 8.37129 | 8.06021 | 9.038754 | 7.677483 | 8.114669 | 8.097031 | 7.88712 | 8.006457 | 8.139059 | 8.057401 | 7.755521 | 7.838261 | 8.277612 | 7.912042 |
2301.10514 | Aleksandr Ivanov | A. V. Ivanov, N. V. Kharuk | Ordered Exponential and Its Features in Yang-Mills Effective Action | LaTeX, 13 pages | 2023 Commun. Theor. Phys. 75 085202 | 10.1088/1572-9494/acde4e | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we discuss some non-trivial relations for ordered exponentials
on smooth Riemannian manifolds. As an example of application, we study a
dependence of the four-dimensional quantum Yang-Mills effective action on the
background filed and gauge transformations. Also, we formulate some open
questions about a... | [
{
"created": "Wed, 25 Jan 2023 10:46:47 GMT",
"version": "v1"
}
] | 2024-01-19 | [
[
"Ivanov",
"A. V.",
""
],
[
"Kharuk",
"N. V.",
""
]
] | In this paper we discuss some non-trivial relations for ordered exponentials on smooth Riemannian manifolds. As an example of application, we study a dependence of the four-dimensional quantum Yang-Mills effective action on the background filed and gauge transformations. Also, we formulate some open questions about a s... | 16.888332 | 13.269221 | 15.454306 | 13.105748 | 13.899968 | 13.458576 | 14.932287 | 13.456433 | 12.918849 | 15.677661 | 13.614842 | 13.237145 | 14.667898 | 14.046227 | 13.362265 | 13.542254 | 13.747183 | 14.473459 | 13.505065 | 15.403021 | 14.195846 |
2011.07023 | Pavel Slepov | Irina Ya. Aref'eva, Kristina Rannu and Pavel Slepov | Holographic Anisotropic Model for Heavy Quarks in Anisotropic Hot Dense
QGP with External Magnetic Field | 38 pages, 26 figures, 2 tables, refs added, small rearrangement of
Sect.2 | JHEP 07, 161 (2021) | 10.1007/JHEP07(2021)161 | null | hep-th hep-ph | http://creativecommons.org/publicdomain/zero/1.0/ | We present a five-dimensional fully anisotropic holographic model for heavy
quarks supported by Einstein-dilaton-three-Maxwell action; one of the Maxwell
fields is related to an external magnetic field. Influence of the external
magnetic field on the 5-dim black hole solution and the
confinement/deconfinement phase d... | [
{
"created": "Fri, 13 Nov 2020 17:13:45 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Nov 2020 18:52:58 GMT",
"version": "v2"
}
] | 2022-03-24 | [
[
"Aref'eva",
"Irina Ya.",
""
],
[
"Rannu",
"Kristina",
""
],
[
"Slepov",
"Pavel",
""
]
] | We present a five-dimensional fully anisotropic holographic model for heavy quarks supported by Einstein-dilaton-three-Maxwell action; one of the Maxwell fields is related to an external magnetic field. Influence of the external magnetic field on the 5-dim black hole solution and the confinement/deconfinement phase dia... | 13.810371 | 6.589478 | 13.976179 | 9.174944 | 10.193897 | 8.121412 | 8.798438 | 8.448792 | 8.897313 | 14.248832 | 8.727025 | 12.114578 | 12.940324 | 12.037825 | 11.98757 | 11.968091 | 11.595245 | 12.367951 | 11.74582 | 12.073507 | 11.465926 |
hep-th/9311115 | Irina Ya. Aref'eva | I.Ya. Aref'eva | Regge Regime in QCD and Asymmetric Lattice Gauge Theory | LATEX, 13 pages, SMI-15-93 | Phys.Lett.B325:171-182,1994 | 10.1016/0370-2693(94)90089-2 | null | hep-th hep-lat hep-ph | null | We study the Regge regime of QCD as a special regime of lattice gauge theory
on an asymmetric lattice. This lattice has a spacing $a_0 $ in the longitudinal
direction and a spacing $a_t $ in the transversal direction. The limit
$\frac{a_{0}}{a_{t}} \to 0$ corresponds to correlation functions with small
longitudinal a... | [
{
"created": "Thu, 18 Nov 1993 14:56:16 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Aref'eva",
"I. Ya.",
""
]
] | We study the Regge regime of QCD as a special regime of lattice gauge theory on an asymmetric lattice. This lattice has a spacing $a_0 $ in the longitudinal direction and a spacing $a_t $ in the transversal direction. The limit $\frac{a_{0}}{a_{t}} \to 0$ corresponds to correlation functions with small longitudinal and... | 9.217611 | 9.636238 | 9.684241 | 9.250978 | 10.345915 | 9.124428 | 9.456939 | 9.533759 | 8.960305 | 10.016732 | 9.259227 | 8.880628 | 9.26357 | 8.871597 | 9.353242 | 8.938476 | 9.164993 | 8.700962 | 9.014499 | 9.42307 | 9.064258 |
1212.2721 | Nan Bai | Nan Bai, Yi-Hong Gao, Guan-Bu Qi, Xiao-Bao Xu | Holographic insulator/superconductor phase transition in Born-Infeld
electrodynamics | 11 pages, 6 figures typos fixed | null | null | null | hep-th | http://creativecommons.org/licenses/by/3.0/ | We studied holographic insulator/superconductor phase transition in the
framework of Born-Infeld electrodynamics both numerically and analytically.
First we numerically study the effects of the Born-Infeld electrodynamics on
the phase transition, find that the critical chemical potential is not changed
by the Born-In... | [
{
"created": "Wed, 12 Dec 2012 07:49:01 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Dec 2012 09:42:59 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Dec 2012 00:23:55 GMT",
"version": "v3"
},
{
"created": "Fri, 21 Dec 2012 12:45:40 GMT",
"version": "v4"
}
] | 2012-12-24 | [
[
"Bai",
"Nan",
""
],
[
"Gao",
"Yi-Hong",
""
],
[
"Qi",
"Guan-Bu",
""
],
[
"Xu",
"Xiao-Bao",
""
]
] | We studied holographic insulator/superconductor phase transition in the framework of Born-Infeld electrodynamics both numerically and analytically. First we numerically study the effects of the Born-Infeld electrodynamics on the phase transition, find that the critical chemical potential is not changed by the Born-Infe... | 4.434878 | 3.395267 | 3.796181 | 3.396356 | 3.471869 | 3.440233 | 3.484117 | 3.425994 | 3.392234 | 3.900741 | 3.55547 | 3.91478 | 4.191227 | 3.919791 | 4.227018 | 3.942029 | 4.098728 | 3.83693 | 4.043868 | 4.246733 | 4.022969 |
hep-th/0405194 | Keisuke Ohashi | Youichi Isozumi, Muneto Nitta, Keisuke Ohashi and Norisuke Sakai | Non-Abelian Walls in Supersymmetric Gauge Theories | 62 pages, 17 figures, the final version in PRD | Phys.Rev. D70 (2004) 125014 | 10.1103/PhysRevD.70.125014 | TIT/HEP-524 | hep-th hep-ph math.DG | null | The Bogomol'nyi-Prasad-Sommerfield (BPS) multi-wall solutions are constructed
in supersymmetric U(N_C) gauge theories in five dimensions with N_F(>N_C)
hypermultiplets in the fundamental representation. Exact solutions are obtained
with full generic moduli for infinite gauge coupling and with partial moduli
for finit... | [
{
"created": "Sat, 22 May 2004 12:21:46 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Mar 2005 07:30:10 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Isozumi",
"Youichi",
""
],
[
"Nitta",
"Muneto",
""
],
[
"Ohashi",
"Keisuke",
""
],
[
"Sakai",
"Norisuke",
""
]
] | The Bogomol'nyi-Prasad-Sommerfield (BPS) multi-wall solutions are constructed in supersymmetric U(N_C) gauge theories in five dimensions with N_F(>N_C) hypermultiplets in the fundamental representation. Exact solutions are obtained with full generic moduli for infinite gauge coupling and with partial moduli for finite ... | 7.890823 | 6.242405 | 8.235733 | 6.173253 | 6.265843 | 5.89144 | 6.018676 | 6.027299 | 6.642451 | 8.364667 | 6.06334 | 6.85009 | 7.740608 | 7.032494 | 7.06607 | 6.85678 | 6.973155 | 6.979604 | 6.968401 | 7.69475 | 6.912433 |
hep-th/0310035 | Kentaroh Yoshida | Makoto Sakaguchi, Kentaroh Yoshida (KEK) | Dirichlet Branes of the Covariant Open Supermembrane in AdS_4 x S^7 and
AdS_7 x S^4 | 16 pages, LaTeX, some clarifications and references added | Nucl.Phys. B681 (2004) 137-151 | 10.1016/j.nuclphysb.2004.01.008 | KEK-TH-904 | hep-th | null | We discuss an open supermembrane theory in the AdS_4 x S^7 and AdS_7 x S^4
backgrounds. The possible Dirichlet branes of an open supermembrane are
classified by analyzing the covariant Wess-Zumino term. All of the allowed
configurations are related to those on the pp-wave background via the Penrose
limit.
| [
{
"created": "Sat, 4 Oct 2003 07:43:59 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Oct 2003 04:58:00 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Sakaguchi",
"Makoto",
"",
"KEK"
],
[
"Yoshida",
"Kentaroh",
"",
"KEK"
]
] | We discuss an open supermembrane theory in the AdS_4 x S^7 and AdS_7 x S^4 backgrounds. The possible Dirichlet branes of an open supermembrane are classified by analyzing the covariant Wess-Zumino term. All of the allowed configurations are related to those on the pp-wave background via the Penrose limit. | 7.691212 | 5.866038 | 9.142738 | 5.763622 | 6.51694 | 6.002326 | 6.199986 | 5.683824 | 5.826991 | 9.692663 | 5.611506 | 6.334493 | 8.107265 | 6.408208 | 6.497305 | 6.387629 | 6.38363 | 6.345222 | 6.279225 | 7.672355 | 6.222879 |
1512.06924 | Joseph A. Minahan | Joseph A. Minahan | Localizing gauge theories on $S^d$ | 17 pages; v2: Typos corrected | null | 10.1007/JHEP04(2016)152 | UUITP-07/15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We conjecture the form of the one-loop determinants for localized gauge
theories with eight supersymmetries on $d$-dimensional spheres. Combining this
with results for the localized action, we investigate the strong coupling
behavior in the large $N$ limit for a continuous range of $d$. In particular,
we find the $N$... | [
{
"created": "Tue, 22 Dec 2015 01:08:15 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Apr 2016 09:47:56 GMT",
"version": "v2"
}
] | 2016-05-25 | [
[
"Minahan",
"Joseph A.",
""
]
] | We conjecture the form of the one-loop determinants for localized gauge theories with eight supersymmetries on $d$-dimensional spheres. Combining this with results for the localized action, we investigate the strong coupling behavior in the large $N$ limit for a continuous range of $d$. In particular, we find the $N$ d... | 6.846231 | 6.690567 | 7.323096 | 6.660978 | 6.421018 | 6.82994 | 6.394605 | 6.356306 | 6.297327 | 7.506473 | 6.804105 | 6.604156 | 7.100578 | 6.522516 | 6.47596 | 6.418373 | 6.541159 | 6.356202 | 6.494483 | 6.755899 | 6.334829 |
hep-th/0411187 | Michelle Cyrier | Michelle Cyrier, Monica Guica, David Mateos, and Andrew Strominger | Microscopic Entropy of the Black Ring | 5 pages; v2: References and acknowledgements added | Phys.Rev.Lett.94:191601,2005 | 10.1103/PhysRevLett.94.191601 | null | hep-th | null | A surprising new seven-parameter supersymmetric black ring solution of
five-dimensional supergravity has recently been discovered. In this paper,
M-theory is used to give an exact microscopic accounting of its entropy.
| [
{
"created": "Sat, 20 Nov 2004 22:09:30 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Dec 2004 17:46:57 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Cyrier",
"Michelle",
""
],
[
"Guica",
"Monica",
""
],
[
"Mateos",
"David",
""
],
[
"Strominger",
"Andrew",
""
]
] | A surprising new seven-parameter supersymmetric black ring solution of five-dimensional supergravity has recently been discovered. In this paper, M-theory is used to give an exact microscopic accounting of its entropy. | 15.989109 | 9.380582 | 15.392936 | 10.638528 | 9.512638 | 9.213333 | 8.545644 | 9.953362 | 9.080513 | 15.767687 | 9.680254 | 10.363377 | 14.118123 | 10.840997 | 11.074609 | 11.159156 | 10.910841 | 11.419287 | 11.220777 | 12.897052 | 10.609842 |
1106.5314 | Tomohiko Takahashi | Shoko Inatomi, Isao Kishimoto, Tomohiko Takahashi | Homotopy Operators and One-Loop Vacuum Energy at the Tachyon Vacuum | 16 pages, LaTeX with PTPTeX.cls;v2: comments and footnotes added | Prog. Theor. Phys. 126 (2011), 1077-1089 | 10.1143/PTP.126.1077 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the homotopy operators for the BRST operator in the theory
around the identity-based solutions, which are believed to represent the
tachyon vacuum in cubic bosonic open string field theory. Using the homotopy
operators, we find that the one-loop vacuum energy at the tachyon vacuum is
independent of modul... | [
{
"created": "Mon, 27 Jun 2011 06:54:49 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Jan 2012 06:26:06 GMT",
"version": "v2"
}
] | 2012-02-01 | [
[
"Inatomi",
"Shoko",
""
],
[
"Kishimoto",
"Isao",
""
],
[
"Takahashi",
"Tomohiko",
""
]
] | We construct the homotopy operators for the BRST operator in the theory around the identity-based solutions, which are believed to represent the tachyon vacuum in cubic bosonic open string field theory. Using the homotopy operators, we find that the one-loop vacuum energy at the tachyon vacuum is independent of moduli ... | 9.43232 | 9.732246 | 10.713601 | 9.181437 | 8.62877 | 9.938345 | 9.952413 | 8.727154 | 9.01484 | 12.898642 | 9.235796 | 9.296277 | 9.332014 | 9.254164 | 9.041138 | 9.226604 | 9.032495 | 9.175698 | 8.79655 | 9.477095 | 9.113817 |
2309.02180 | Evan Owen | Evan Owen | Simplicial Lattice Study of the 2d Ising CFT | PhD Thesis, Boston University 2023, 61 pages | null | null | null | hep-th hep-lat | http://creativecommons.org/licenses/by/4.0/ | I derive a formulation of the 2-dimensional critical Ising model on
non-uniform simplicial lattices. Surprisingly, the derivation leads to a set of
geometric constraints that a lattice must satisfy in order for the model to
have a well-defined continuum limit. I perform Monte Carlo simulations of the
critical Ising m... | [
{
"created": "Tue, 5 Sep 2023 12:33:41 GMT",
"version": "v1"
}
] | 2023-09-06 | [
[
"Owen",
"Evan",
""
]
] | I derive a formulation of the 2-dimensional critical Ising model on non-uniform simplicial lattices. Surprisingly, the derivation leads to a set of geometric constraints that a lattice must satisfy in order for the model to have a well-defined continuum limit. I perform Monte Carlo simulations of the critical Ising mod... | 6.853839 | 7.250316 | 6.948734 | 6.454828 | 6.767961 | 6.56671 | 6.98449 | 7.129659 | 6.733799 | 7.260423 | 6.452234 | 6.485937 | 6.828383 | 6.590793 | 6.595447 | 6.715755 | 6.706343 | 6.554254 | 6.760539 | 6.922861 | 6.429136 |
1705.09550 | Igor Bandos | Igor Bandos | An analytic superfield formalism for tree superamplitudes in D=10 and
D=11 | LaTeX, 51pp. V2: improved and completed; to be published in JHEP;
63pp | null | 10.1007/JHEP05(2018)103 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Tree amplitudes of 10D supersymmetric Yang-Mills theory (SYM) and 11D
supergravity (SUGRA) are collected in multi-particle counterparts of analytic
on-shell superfields. These have essentially the same form as their chiral 4D
counterparts describing ${\cal N}=4$ SYM and ${\cal N}=8$ SUGRA, but with
components depende... | [
{
"created": "Fri, 26 May 2017 12:34:29 GMT",
"version": "v1"
},
{
"created": "Mon, 7 May 2018 09:48:46 GMT",
"version": "v2"
}
] | 2018-06-13 | [
[
"Bandos",
"Igor",
""
]
] | Tree amplitudes of 10D supersymmetric Yang-Mills theory (SYM) and 11D supergravity (SUGRA) are collected in multi-particle counterparts of analytic on-shell superfields. These have essentially the same form as their chiral 4D counterparts describing ${\cal N}=4$ SYM and ${\cal N}=8$ SUGRA, but with components dependent... | 8.286552 | 7.697018 | 8.424604 | 7.258687 | 7.847938 | 7.358788 | 7.56935 | 7.524393 | 7.314121 | 9.562984 | 7.213168 | 7.074541 | 7.648882 | 7.387044 | 7.314302 | 7.202924 | 7.1082 | 6.919094 | 7.276008 | 7.627686 | 7.35297 |
0910.2387 | Rong-Gen Cai | Rong-Gen Cai, Li-Ming Cao, Ya-Peng Hu, Nobuyoshi Ohta | Generalized Misner-Sharp Energy in f(R) Gravity | Revtex, 17 pages, v2: some references added, to appear in PRD | Phys.Rev.D80:104016,2009 | 10.1103/PhysRevD.80.104016 | KU-TP 036 | hep-th gr-qc | http://creativecommons.org/licenses/by/3.0/ | We study generalized Misner-Sharp energy in $f(R)$ gravity in a spherically
symmetric spacetime. We find that unlike the cases of Einstein gravity and
Gauss-Bonnet gravity, the existence of the generalized Misner-Sharp energy
depends on a constraint condition in the $f(R)$ gravity. When the constraint
condition is sa... | [
{
"created": "Tue, 13 Oct 2009 13:07:57 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Oct 2009 01:08:51 GMT",
"version": "v2"
}
] | 2010-04-29 | [
[
"Cai",
"Rong-Gen",
""
],
[
"Cao",
"Li-Ming",
""
],
[
"Hu",
"Ya-Peng",
""
],
[
"Ohta",
"Nobuyoshi",
""
]
] | We study generalized Misner-Sharp energy in $f(R)$ gravity in a spherically symmetric spacetime. We find that unlike the cases of Einstein gravity and Gauss-Bonnet gravity, the existence of the generalized Misner-Sharp energy depends on a constraint condition in the $f(R)$ gravity. When the constraint condition is sati... | 5.264181 | 5.107169 | 4.974309 | 4.865756 | 4.941714 | 5.160529 | 5.165293 | 4.97219 | 5.01733 | 5.188359 | 4.810785 | 5.17429 | 4.957454 | 4.909744 | 5.019437 | 5.145102 | 4.897117 | 5.02192 | 5.062863 | 4.997964 | 4.927117 |
1605.00146 | Andreas W. Aste | Andreas Aste | Weyl, Majorana and Dirac fields from a unified perspective | 28 pages, 2 figures, one new section and two references added | Symmetry 2016, 8(9), 87 | 10.3390/sym8090087 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A self-contained derivation of the formalism describing Weyl, Majorana and
Dirac fields from a unified perspective is given based on a concise description
of the representation theory of the proper orthochronous Lorentz group.
Lagrangian methods play no role in the present exposition, which covers several
fundamental... | [
{
"created": "Sat, 30 Apr 2016 17:42:42 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Aug 2016 11:21:55 GMT",
"version": "v2"
}
] | 2016-09-01 | [
[
"Aste",
"Andreas",
""
]
] | A self-contained derivation of the formalism describing Weyl, Majorana and Dirac fields from a unified perspective is given based on a concise description of the representation theory of the proper orthochronous Lorentz group. Lagrangian methods play no role in the present exposition, which covers several fundamental a... | 10.977941 | 11.866034 | 12.215499 | 10.728419 | 12.099303 | 11.892793 | 11.506021 | 10.800065 | 10.609986 | 13.310747 | 10.626855 | 11.642247 | 11.190928 | 11.209599 | 11.053506 | 11.599589 | 11.839332 | 11.102613 | 10.657817 | 11.040251 | 10.967731 |
hep-th/9906028 | Nelson Vanegas | Nelson Vanegas | Regularization of Automorphic Functions of Manifolds with Special
K\"ahler Geometry | LaTeX2e, 31 Pages | null | null | UdeA-PE-02 | hep-th | null | In this paper we find automorphic functions of coset manifolds with special
K\"ahler geometry. We use \zeta-functions to regularize an infinite product
over integers which belong to a duality-invariant lattice, this product is
known to produce duality-invariant functions. In turn these functions
correspond to Eisenst... | [
{
"created": "Thu, 3 Jun 1999 23:46:49 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Vanegas",
"Nelson",
""
]
] | In this paper we find automorphic functions of coset manifolds with special K\"ahler geometry. We use \zeta-functions to regularize an infinite product over integers which belong to a duality-invariant lattice, this product is known to produce duality-invariant functions. In turn these functions correspond to Eisenstei... | 11.45613 | 9.760605 | 12.078136 | 10.285884 | 10.798297 | 11.133365 | 10.396964 | 11.398103 | 9.573601 | 12.885527 | 10.141478 | 10.366556 | 10.897591 | 10.452186 | 10.209414 | 10.336159 | 10.360343 | 10.035146 | 10.325391 | 11.335881 | 10.353421 |
hep-th/0201113 | Matthias R. Gaberdiel | Matthias R Gaberdiel | D-branes from conformal field theory | 19 pages, LaTeX, 4 figures; to appear in the Proceedings of the RTN
meeting `The Quantum Structure of Spacetime and the Geometric Nature of
Fundamental Interactions', Corfu, September 2001; v2: minor corrections | null | 10.1002/1521-3978(200209)50:8/9<783::AID-PROP783>3.0.CO;2-J | KCL-MTH-02-02 | hep-th | null | An introduction to the construction of D-branes using conformal field theory
methods is given. A number of examples are discussed in detail, in particular
the construction of all conformal D-branes for the theory of a single free
boson on a circle.
| [
{
"created": "Tue, 15 Jan 2002 21:17:56 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Jan 2002 11:42:52 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Gaberdiel",
"Matthias R",
""
]
] | An introduction to the construction of D-branes using conformal field theory methods is given. A number of examples are discussed in detail, in particular the construction of all conformal D-branes for the theory of a single free boson on a circle. | 6.352744 | 4.349186 | 6.457684 | 4.667898 | 5.217608 | 4.825329 | 5.276395 | 5.029283 | 4.695834 | 7.250326 | 5.168712 | 5.186769 | 6.635121 | 5.289809 | 5.279702 | 5.416543 | 5.323655 | 5.057965 | 5.301697 | 6.13886 | 5.536734 |
1110.3902 | Gyungchoon Go | Gyungchoon Go, O-Kab Kwon, D. D. Tolla | ${\cal N}=3$ Supersymmetric Effective Action of D2-branes in Massive IIA
String Theory | 22 pages, positive definite form of potential is added, some comments
are changed | null | 10.1103/PhysRevD.85.026006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain a new-type of ${\cal N}=3$ Yang-Mills Chern-Simons theory from the
Mukhi-Papageorgakis Higgsing of the ${\cal N}=3$ Gaiotto-Tomasiello theory.
This theory has ${\cal N}=1$ BPS fuzzy funnel solution which is expressed in
terms of the seven generators of SU(3), excluding $T_8$. We propose that this
is an effe... | [
{
"created": "Tue, 18 Oct 2011 08:09:43 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Dec 2011 08:09:49 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Go",
"Gyungchoon",
""
],
[
"Kwon",
"O-Kab",
""
],
[
"Tolla",
"D. D.",
""
]
] | We obtain a new-type of ${\cal N}=3$ Yang-Mills Chern-Simons theory from the Mukhi-Papageorgakis Higgsing of the ${\cal N}=3$ Gaiotto-Tomasiello theory. This theory has ${\cal N}=1$ BPS fuzzy funnel solution which is expressed in terms of the seven generators of SU(3), excluding $T_8$. We propose that this is an effect... | 8.267905 | 8.317502 | 9.67033 | 7.473285 | 7.679093 | 8.533943 | 7.876702 | 8.020037 | 7.280204 | 10.381193 | 6.996034 | 7.195328 | 8.125604 | 7.488797 | 7.174509 | 7.375485 | 7.327688 | 7.425748 | 7.437094 | 8.449197 | 7.175929 |
2101.01681 | Pietro Longhi | Pietro Longhi | On the BPS spectrum of 5d SU(2) super-Yang-Mills | 8 pages; v2 some updates due to an implicit assumption; v3 added
appendix with proof of assumption, and some clarifications | Phys. Rev. Lett. 126, 211601 (2021) | 10.1103/PhysRevLett.126.211601 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a closed-form expression for the motivic Kontsevich-Soibelman
invariant for M-theory in the background of the toric Calabi-Yau threefold
$K_{\mathbb{F}_0}$. This encodes the refined BPS spectrum of $SU(2)$ 5d ${\cal
N}=1$ Yang-Mills theory on $S^1\times \mathbb{R}^4$, corresponding to rank-zero
Donaldson-T... | [
{
"created": "Tue, 5 Jan 2021 17:55:09 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jan 2021 18:48:16 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Jan 2021 12:32:09 GMT",
"version": "v3"
}
] | 2021-06-02 | [
[
"Longhi",
"Pietro",
""
]
] | We provide a closed-form expression for the motivic Kontsevich-Soibelman invariant for M-theory in the background of the toric Calabi-Yau threefold $K_{\mathbb{F}_0}$. This encodes the refined BPS spectrum of $SU(2)$ 5d ${\cal N}=1$ Yang-Mills theory on $S^1\times \mathbb{R}^4$, corresponding to rank-zero Donaldson-Tho... | 5.881925 | 4.576403 | 6.599998 | 4.921016 | 4.999913 | 4.879022 | 5.177992 | 4.831652 | 4.729189 | 5.889193 | 4.652492 | 5.035969 | 5.51556 | 4.872255 | 5.01927 | 5.221402 | 5.144542 | 4.925585 | 4.925613 | 5.301225 | 5.055144 |
hep-th/0507007 | Nejat Yilmaz | Tekin Dereli, Nejat T. Yilmaz | Dualisation of the Symmetric Space Sigma Model with Couplings | 17 pages | Nucl.Phys.B705:60-70,2005 | 10.1016/j.nuclphysb.2004.11.006 | null | hep-th | null | The first-order formulation of the G/K symmetric space sigma model of the
scalar cosets of the supergravity theories is discussed when there is coupling
of (m-1)-form matter fields. The Lie superalgebra which enables the dualized
coset formulation is constructed for a general scalar coset G/K with matter
coupling whe... | [
{
"created": "Fri, 1 Jul 2005 10:40:19 GMT",
"version": "v1"
}
] | 2010-01-15 | [
[
"Dereli",
"Tekin",
""
],
[
"Yilmaz",
"Nejat T.",
""
]
] | The first-order formulation of the G/K symmetric space sigma model of the scalar cosets of the supergravity theories is discussed when there is coupling of (m-1)-form matter fields. The Lie superalgebra which enables the dualized coset formulation is constructed for a general scalar coset G/K with matter coupling where... | 15.146199 | 13.731682 | 16.698236 | 13.198714 | 14.204478 | 12.924056 | 14.13714 | 12.595692 | 13.693522 | 16.78688 | 12.891712 | 13.221942 | 14.137413 | 13.415244 | 13.296189 | 12.872065 | 12.590022 | 12.66783 | 13.771849 | 14.537601 | 13.048682 |
2006.16641 | Yermek Aldabergenov | Yermek Aldabergenov, Andrea Addazi, Sergei V. Ketov | Primordial black holes from modified supergravity | 30 pages, 17 figures, 4 tables. Update v3: Section 6 is revised and
main results are improved. Added two references | Eur. Phys. J. C, 80 (2020) 10, 917 | 10.1140/epjc/s10052-020-08506-6 | IPMU20-0074 | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The modified supergravity approach is applied to describe a formation of
Primordial Black Holes (PBHs) after Starobinsky inflation. Our approach
naturally leads to the two-(scalar)-field attractor-type double inflation,
whose first stage is driven by scalaron and whose second stage is driven by
another scalar field w... | [
{
"created": "Tue, 30 Jun 2020 10:07:15 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jul 2020 08:10:35 GMT",
"version": "v2"
},
{
"created": "Sat, 26 Sep 2020 09:51:06 GMT",
"version": "v3"
}
] | 2020-10-12 | [
[
"Aldabergenov",
"Yermek",
""
],
[
"Addazi",
"Andrea",
""
],
[
"Ketov",
"Sergei V.",
""
]
] | The modified supergravity approach is applied to describe a formation of Primordial Black Holes (PBHs) after Starobinsky inflation. Our approach naturally leads to the two-(scalar)-field attractor-type double inflation, whose first stage is driven by scalaron and whose second stage is driven by another scalar field whi... | 8.280359 | 7.980071 | 8.454578 | 8.123834 | 8.068972 | 8.418592 | 8.406507 | 7.944333 | 8.096081 | 8.619026 | 7.972965 | 8.176787 | 8.106975 | 7.992241 | 8.023705 | 8.122128 | 7.915098 | 7.95379 | 7.84752 | 8.26874 | 7.98661 |
1808.09136 | Bobby Ezhuthachan | Suchetan Das, Bobby Ezhuthachan | Modular Hamiltonians and large diffeomorphisms in $AdS_3$ | 17 pages | null | 10.1007/JHEP12(2018)096 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the work of Kabat and Lifshytz (arXiv:1703.06523), of
reconstructing bulk scalar fields using the intersecting modular hamiltonian
approach discussed therein, to any locally $AdS_3$ space related to $AdS_3$ by
large diffeomorphisms. We present several checks for our result including
matcing with their r... | [
{
"created": "Tue, 28 Aug 2018 06:26:06 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Sep 2018 10:13:40 GMT",
"version": "v2"
}
] | 2019-01-30 | [
[
"Das",
"Suchetan",
""
],
[
"Ezhuthachan",
"Bobby",
""
]
] | We generalize the work of Kabat and Lifshytz (arXiv:1703.06523), of reconstructing bulk scalar fields using the intersecting modular hamiltonian approach discussed therein, to any locally $AdS_3$ space related to $AdS_3$ by large diffeomorphisms. We present several checks for our result including matcing with their res... | 12.626239 | 14.428906 | 15.920835 | 13.345998 | 12.826074 | 12.272848 | 13.633565 | 12.69945 | 13.662756 | 14.230265 | 12.70642 | 11.892982 | 12.251459 | 11.442141 | 11.704703 | 11.894696 | 11.664259 | 12.078652 | 12.221066 | 12.043605 | 10.950033 |
hep-th/0111132 | Gogberashvili Merab Jakob | Merab Gogberashvili and Paul Midodashvili | Localization of Fields on a Brane in Six Dimensions | 6 pages, LaTeX, no figures, two references added, minor changes.
Version to appear in Europhysics Letters | Europhys.Lett.61:308-313,2003 | 10.1209/epl/i2003-00324-1 | null | hep-th astro-ph gr-qc hep-ph | null | Universe is considered as a brane in infinite (2+4)-space.It is shown that
zero modes of all kinds of matter fields and 4-gravity are localized on the
brane by increasing transversal gravitational potential.
| [
{
"created": "Wed, 14 Nov 2001 20:48:17 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Nov 2002 15:03:18 GMT",
"version": "v2"
}
] | 2010-12-17 | [
[
"Gogberashvili",
"Merab",
""
],
[
"Midodashvili",
"Paul",
""
]
] | Universe is considered as a brane in infinite (2+4)-space.It is shown that zero modes of all kinds of matter fields and 4-gravity are localized on the brane by increasing transversal gravitational potential. | 34.414097 | 16.504156 | 23.652195 | 16.871601 | 19.389431 | 18.134958 | 18.801754 | 19.684626 | 17.243856 | 23.354763 | 22.284866 | 20.694174 | 22.027103 | 20.817541 | 21.796007 | 22.875061 | 21.184965 | 20.89687 | 21.341955 | 23.551712 | 23.785683 |
2402.13694 | Onkar Parrikar | Ritam Basu, Anirban Ganguly, Souparna Nath, Onkar Parrikar | Complexity Growth and the Krylov-Wigner function | 30 pages, 6 figures | null | null | null | hep-th quant-ph | http://creativecommons.org/licenses/by/4.0/ | For any state in a $D$-dimensional Hilbert space with a choice of basis, one
can define a discrete version of the Wigner function -- a quasi-probability
distribution which represents the state on a discrete phase space. The Wigner
function can, in general, take on negative values, and the amount of negativity
in the ... | [
{
"created": "Wed, 21 Feb 2024 10:54:12 GMT",
"version": "v1"
}
] | 2024-02-22 | [
[
"Basu",
"Ritam",
""
],
[
"Ganguly",
"Anirban",
""
],
[
"Nath",
"Souparna",
""
],
[
"Parrikar",
"Onkar",
""
]
] | For any state in a $D$-dimensional Hilbert space with a choice of basis, one can define a discrete version of the Wigner function -- a quasi-probability distribution which represents the state on a discrete phase space. The Wigner function can, in general, take on negative values, and the amount of negativity in the Wi... | 6.322951 | 6.658552 | 6.759168 | 5.853754 | 6.428673 | 6.264738 | 6.280829 | 6.432318 | 6.43051 | 7.30422 | 6.127455 | 6.032947 | 6.150342 | 5.96083 | 5.956061 | 6.010979 | 6.126933 | 5.917111 | 6.041656 | 5.974427 | 5.9124 |
0711.2272 | Dmitry V. Belyaev | Dmitry V. Belyaev, Peter van Nieuwenhuizen | Tensor calculus for supergravity on a manifold with boundary | 20 pages, JHEP format; published version | JHEP0802:047,2008 | 10.1088/1126-6708/2008/02/047 | DESY-07-208, YITP-SB-07-33 | hep-th hep-ph | null | Using the simple setting of 3D N=1 supergravity, we show how the tensor
calculus of supergravity can be extended to manifolds with boundary. We present
an extension of the standard F-density formula which yields supersymmetric
bulk-plus-boundary actions. To construct additional separately supersymmetric
boundary acti... | [
{
"created": "Wed, 14 Nov 2007 20:51:59 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Feb 2008 15:01:59 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Belyaev",
"Dmitry V.",
""
],
[
"van Nieuwenhuizen",
"Peter",
""
]
] | Using the simple setting of 3D N=1 supergravity, we show how the tensor calculus of supergravity can be extended to manifolds with boundary. We present an extension of the standard F-density formula which yields supersymmetric bulk-plus-boundary actions. To construct additional separately supersymmetric boundary action... | 10.658445 | 11.072913 | 11.269326 | 9.612397 | 10.239721 | 9.869985 | 10.683432 | 10.378518 | 10.747679 | 13.706335 | 10.34378 | 10.256454 | 10.935922 | 10.225325 | 10.244432 | 10.097969 | 10.382639 | 10.247773 | 10.487051 | 11.115355 | 10.277179 |
hep-th/0010057 | Heinrich Saller | Heinrich Saller (MPI fuer Physik) | Residual Representations of Spacetime | 30 pages, latex, macros included | Int.J.Theor.Phys. 40 (2001) 1209-1248 | null | MPI-PTH/00-41 | hep-th | null | Spacetime is modelled by binary relations - by the classes of the
automorphisms $\GL(\C^2)$ of a complex 2-dimensional vector space with respect
to the definite unitary subgroup $\U(2)$. In extension of Feynman propagators
for particle quantum fields representing only the tangent spacetime structure,
global spacetime... | [
{
"created": "Mon, 9 Oct 2000 12:06:58 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Saller",
"Heinrich",
"",
"MPI fuer Physik"
]
] | Spacetime is modelled by binary relations - by the classes of the automorphisms $\GL(\C^2)$ of a complex 2-dimensional vector space with respect to the definite unitary subgroup $\U(2)$. In extension of Feynman propagators for particle quantum fields representing only the tangent spacetime structure, global spacetime r... | 28.567928 | 27.904211 | 29.485497 | 27.541489 | 28.016689 | 32.421242 | 29.594406 | 29.267389 | 26.553707 | 33.514202 | 26.460918 | 25.475449 | 24.998772 | 25.200157 | 25.536718 | 26.789106 | 26.173292 | 25.592073 | 25.338957 | 25.227016 | 26.443682 |
1004.0632 | Alexei Kotov | A.Kotov, T.Strobl | Generalizing Geometry - Algebroids and Sigma Models | 52 pages, Contribution to the Handbook on Pseudo-Riemannian Geometry
and Supersymmetry, ed. V. Cortes | null | null | null | hep-th math-ph math.DG math.MP math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this contribution we review some of the interplay between sigma models in
theoretical physics and novel geometrical structures such as Lie
(n-)algebroids. The first part of the article contains the mathematical
background, the definition of various algebroids as well as of Dirac
structures, a joint generalization ... | [
{
"created": "Mon, 5 Apr 2010 13:39:34 GMT",
"version": "v1"
}
] | 2010-04-06 | [
[
"Kotov",
"A.",
""
],
[
"Strobl",
"T.",
""
]
] | In this contribution we review some of the interplay between sigma models in theoretical physics and novel geometrical structures such as Lie (n-)algebroids. The first part of the article contains the mathematical background, the definition of various algebroids as well as of Dirac structures, a joint generalization of... | 9.914926 | 11.829082 | 12.252774 | 10.619591 | 11.695577 | 11.875671 | 11.94765 | 10.845427 | 10.237708 | 12.575976 | 10.456276 | 9.886061 | 10.273742 | 10.097006 | 9.907436 | 9.882988 | 10.106078 | 10.15251 | 9.866089 | 10.599241 | 9.788491 |
1809.02328 | Kentaro Hara | Kentaro Hara, Akifumi Sako, Hyun Seok Yang | Hermitian-Einstein metrics from noncommutative $U\left(1 \right)$
instantons | null | null | 10.1063/1.5063528 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that Hermitian-Einstein metrics can be locally constructed by a map
from (anti-)self-dual two-forms on Euclidean ${\mathbb R}^4$ to symmetric
two-tensors introduced in "Gravitational instantons from gauge theory," H. S.
Yang and M. Salizzoni, Phys. Rev. Lett. (2006) 201602, [hep-th/0512215]. This
corresponden... | [
{
"created": "Fri, 7 Sep 2018 07:13:02 GMT",
"version": "v1"
}
] | 2019-10-02 | [
[
"Hara",
"Kentaro",
""
],
[
"Sako",
"Akifumi",
""
],
[
"Yang",
"Hyun Seok",
""
]
] | We show that Hermitian-Einstein metrics can be locally constructed by a map from (anti-)self-dual two-forms on Euclidean ${\mathbb R}^4$ to symmetric two-tensors introduced in "Gravitational instantons from gauge theory," H. S. Yang and M. Salizzoni, Phys. Rev. Lett. (2006) 201602, [hep-th/0512215]. This correspondence... | 6.997414 | 6.961123 | 7.670916 | 6.596535 | 8.015707 | 6.994619 | 6.751793 | 7.072767 | 6.859984 | 7.398896 | 6.919499 | 6.447647 | 6.905454 | 6.592719 | 6.524928 | 6.350134 | 6.492318 | 6.535878 | 6.759515 | 6.673457 | 6.48949 |
hep-th/9602008 | Andrei Demichev | M. Chaichian (University of Helsinki) and A.P.Demichev (CBPF/CNPQ, Rio
de Janeiro) | Polynomial Algebras and Higher Spins | 8 pages, LaTeX | null | 10.1016/0375-9601(96)00631-7 | HU-SEFT R 1996-02 | hep-th | null | Polynomial relations for generators of $su(2)$ Lie algebra in arbitrary
representations are found. They generalize usual relation for Pauli operators
in spin 1/2 case and permit to construct modified Holstein-Primakoff
transformations in finite dimensional Fock spaces. The connection between
$su(2)$ Lie algebra and q... | [
{
"created": "Fri, 2 Feb 1996 20:05:00 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Chaichian",
"M.",
"",
"University of Helsinki"
],
[
"Demichev",
"A. P.",
"",
"CBPF/CNPQ, Rio\n de Janeiro"
]
] | Polynomial relations for generators of $su(2)$ Lie algebra in arbitrary representations are found. They generalize usual relation for Pauli operators in spin 1/2 case and permit to construct modified Holstein-Primakoff transformations in finite dimensional Fock spaces. The connection between $su(2)$ Lie algebra and q-o... | 11.223025 | 10.441284 | 11.147088 | 9.561477 | 10.338278 | 9.175967 | 10.347363 | 9.713122 | 9.607993 | 12.867275 | 9.581849 | 9.214934 | 9.930576 | 9.350894 | 9.261916 | 9.219396 | 9.181285 | 9.314976 | 9.250959 | 10.12145 | 9.780042 |
hep-th/9812191 | David Kastor | David Kastor and Euy Soo Na | Electric Dipole Moment of a BPS Monopole | 8 pages, references and note added | Phys.Rev.D60:025002,1999 | 10.1103/PhysRevD.60.025002 | UMHEP-457 | hep-th | null | Monopole ``superpartner'' solutions are constructed by acting with finite,
broken supersymmetry transformations on a bosonic N=2 BPS monopole. The terms
beyond first order in this construction represent the backreaction of the the
fermionic zero-mode state on the other fields. Because of the quantum nature of
the fer... | [
{
"created": "Mon, 21 Dec 1998 20:38:07 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jan 1999 21:17:12 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Kastor",
"David",
""
],
[
"Na",
"Euy Soo",
""
]
] | Monopole ``superpartner'' solutions are constructed by acting with finite, broken supersymmetry transformations on a bosonic N=2 BPS monopole. The terms beyond first order in this construction represent the backreaction of the the fermionic zero-mode state on the other fields. Because of the quantum nature of the fermi... | 11.959727 | 11.998668 | 13.070436 | 10.677116 | 12.320057 | 12.438964 | 13.078958 | 10.989985 | 12.317381 | 12.742602 | 11.253024 | 11.431984 | 11.821033 | 10.966556 | 10.944633 | 10.507794 | 10.921176 | 10.861012 | 11.268518 | 11.838923 | 11.075995 |
hep-th/0612068 | Mokhtar Hassaine | Eloy Ay\'on-Beato and Mokhtar Hassa\"ine | Higher-dimensional AdS waves and pp-waves with conformally related
sources | 13 pages | Phys.Rev.D75:064025,2007 | 10.1103/PhysRevD.75.064025 | CECS-PHY-06/26 | hep-th gr-qc | null | AdS waves and pp-waves can only be supported by pure radiation fields, for
which the only nonvanishing component of the energy-momentum tensor is the
energy density along the retarded time. We show that the nonminimal coupling of
self-gravitating scalar fields to the higher-dimensional versions of these
exact gravita... | [
{
"created": "Fri, 8 Dec 2006 01:09:27 GMT",
"version": "v1"
}
] | 2016-08-16 | [
[
"Ayón-Beato",
"Eloy",
""
],
[
"Hassaïne",
"Mokhtar",
""
]
] | AdS waves and pp-waves can only be supported by pure radiation fields, for which the only nonvanishing component of the energy-momentum tensor is the energy density along the retarded time. We show that the nonminimal coupling of self-gravitating scalar fields to the higher-dimensional versions of these exact gravitati... | 11.355891 | 11.520671 | 11.674795 | 10.35929 | 11.773425 | 11.417301 | 11.548196 | 11.347455 | 10.673159 | 11.995296 | 10.893928 | 11.070419 | 10.857739 | 10.572668 | 10.427536 | 10.371568 | 10.94765 | 10.260653 | 10.384595 | 10.782987 | 10.59212 |
hep-th/0408025 | Hidenori Sonoda | Hidenori Sonoda | Two dimensional non-linear sigma models as a limit of the linear sigma
models | 13 pages, 3 figures, LaTeX, revised with an addition of Appendix B | Prog.Theor.Phys. 113 (2005) 1377-1390 | 10.1143/PTP.113.1377 | KOBE-TH-04-03 | hep-th | null | We show how to obtain the O(N) non-linear sigma model in two dimensions as a
strong coupling limit of the corresponding linear sigma model. In taking the
strong coupling limit, the squared mass parameter must be given a specific
coupling dependence that assures the finiteness of the physical mass scale. The
relation ... | [
{
"created": "Tue, 3 Aug 2004 18:31:53 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Dec 2004 12:22:11 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Sonoda",
"Hidenori",
""
]
] | We show how to obtain the O(N) non-linear sigma model in two dimensions as a strong coupling limit of the corresponding linear sigma model. In taking the strong coupling limit, the squared mass parameter must be given a specific coupling dependence that assures the finiteness of the physical mass scale. The relation di... | 9.451765 | 8.664773 | 9.827718 | 8.614497 | 8.785797 | 9.293769 | 8.984053 | 8.510431 | 8.616919 | 10.023235 | 8.425555 | 8.22162 | 9.216112 | 8.57261 | 8.613234 | 8.48419 | 8.54723 | 8.602271 | 8.770537 | 9.130219 | 8.681559 |
2407.02554 | Alice L\"uscher | Pietro Benetti Genolini, Jerome P. Gauntlett, Yusheng Jiao, Alice
L\"uscher, James Sparks | Localization of the free energy in supergravity | 6 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We derive a general formula for the gravitational free energy of Euclidean
supersymmetric solutions to $D=4$, $\mathcal{N}=2$ gauged supergravity coupled
to vector multiplet matter. This allows one to compute the free energy without
solving any supergravity equations, just assuming the solutions exist. As well
as rec... | [
{
"created": "Tue, 2 Jul 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-07-04 | [
[
"Genolini",
"Pietro Benetti",
""
],
[
"Gauntlett",
"Jerome P.",
""
],
[
"Jiao",
"Yusheng",
""
],
[
"Lüscher",
"Alice",
""
],
[
"Sparks",
"James",
""
]
] | We derive a general formula for the gravitational free energy of Euclidean supersymmetric solutions to $D=4$, $\mathcal{N}=2$ gauged supergravity coupled to vector multiplet matter. This allows one to compute the free energy without solving any supergravity equations, just assuming the solutions exist. As well as recov... | 7.997067 | 7.104153 | 8.785998 | 7.154006 | 7.39771 | 7.231567 | 7.455512 | 6.795339 | 6.85288 | 8.958362 | 7.239566 | 7.330964 | 8.211988 | 7.442922 | 7.30404 | 7.566058 | 7.513983 | 7.675539 | 7.227437 | 8.052563 | 7.305252 |
hep-th/9201038 | null | L. Feher, L. O'Raifeartaigh, P. Ruelle and I. Tsutsui | Rational vs Polynomial Character of W$_n^l$-Algebras | 18 pages | null | 10.1016/0370-2693(92)90015-V | null | hep-th | null | The constraints proposed recently by Bershadsky to produce $W^l_n$ algebras
are a mixture of first and second class constraints and are degenerate. We show
that they admit a first-class subsystem from which they can be recovered by
gauge-fixing, and that the non-degenerate constraints can be handled by
previous metho... | [
{
"created": "Tue, 21 Jan 1992 03:18:51 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Feb 1992 20:24:11 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Feher",
"L.",
""
],
[
"O'Raifeartaigh",
"L.",
""
],
[
"Ruelle",
"P.",
""
],
[
"Tsutsui",
"I.",
""
]
] | The constraints proposed recently by Bershadsky to produce $W^l_n$ algebras are a mixture of first and second class constraints and are degenerate. We show that they admit a first-class subsystem from which they can be recovered by gauge-fixing, and that the non-degenerate constraints can be handled by previous methods... | 19.018305 | 19.343405 | 20.687031 | 17.240791 | 19.627756 | 16.59903 | 16.912384 | 18.031021 | 17.032526 | 23.706545 | 15.573123 | 16.711946 | 19.866858 | 17.638588 | 17.807554 | 16.622559 | 17.126541 | 17.237934 | 18.362963 | 19.461342 | 16.393827 |
hep-th/0312138 | Wolfgang Behr | Wolfgang Behr, Andreas Sykora | NC Wilson lines and the inverse Seiberg-Witten map for nondegenerate
star products | 8 pages | Eur.Phys.J. C35 (2004) 145-148 | 10.1140/epjc/s2004-01778-4 | MPP-2003-138 | hep-th | null | Open Wilson lines are known to be the observables of noncommutative gauge
theory with Moyal-Weyl star product. We generalize these objects to more
general star products. As an application we derive a formula for the inverse
Seiberg-Witten map for star products with invertible Poisson structures.
| [
{
"created": "Fri, 12 Dec 2003 15:08:33 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Behr",
"Wolfgang",
""
],
[
"Sykora",
"Andreas",
""
]
] | Open Wilson lines are known to be the observables of noncommutative gauge theory with Moyal-Weyl star product. We generalize these objects to more general star products. As an application we derive a formula for the inverse Seiberg-Witten map for star products with invertible Poisson structures. | 13.081549 | 8.698533 | 10.214355 | 7.731132 | 9.644768 | 8.737491 | 8.743003 | 8.665939 | 8.436353 | 12.8042 | 9.011743 | 7.333593 | 8.769185 | 7.883937 | 8.279421 | 7.93009 | 7.907766 | 8.051131 | 8.019772 | 8.657952 | 8.916295 |
1804.06727 | Behrouz Mirza | Masoumeh Tavakoli, Behrouz Mirza, Zeinab Sherkatghanad | Holographic entanglement entropy for charged accelerating AdS black
holes | 10 pages, 6 figures | Nuclear Physics B 943 (2019) 114620 | 10.1016/j.nuclphysb.2019.114620 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the holographic entanglement entropy in the Rindler-AdS
space-time to obtain an exact solution for the corresponding minimal surface.
Moreover, the holographic entanglement entropy of the charged single
accelerated AdS Black holes in four dimensions is investigated. We obtain the
volume of the codimens... | [
{
"created": "Mon, 16 Apr 2018 10:37:09 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Jul 2019 12:46:22 GMT",
"version": "v2"
}
] | 2019-07-02 | [
[
"Tavakoli",
"Masoumeh",
""
],
[
"Mirza",
"Behrouz",
""
],
[
"Sherkatghanad",
"Zeinab",
""
]
] | We investigate the holographic entanglement entropy in the Rindler-AdS space-time to obtain an exact solution for the corresponding minimal surface. Moreover, the holographic entanglement entropy of the charged single accelerated AdS Black holes in four dimensions is investigated. We obtain the volume of the codimensio... | 8.955696 | 9.171643 | 10.435525 | 8.954364 | 9.465795 | 8.840688 | 9.740657 | 9.343472 | 8.818947 | 10.436722 | 8.788675 | 9.342667 | 9.043029 | 8.976916 | 9.248619 | 9.587349 | 9.239446 | 9.257383 | 8.998612 | 9.114458 | 9.178591 |
2207.04048 | Gopal Yadav | Gopal Yadav and Aalok Misra | Entanglement entropy and Page curve from the ${\cal M}$-theory dual of
thermal QCD above $T_c$ at intermediate coupling | v4:1+77 Pages, LaTeX, 11 figures; title changed; Explanatory text
added; to appear in PRD | null | 10.1103/PhysRevD.107.106015 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Obtaining the Page curve in the context of eternal black holes associated
with top-down non-conformal holographic thermal duals at intermediate coupling,
has been entirely unexplored in the literature. We fill this gap in the context
of a doubly holographic setup relevant to the M-theory dual of thermal QCD-like
theo... | [
{
"created": "Thu, 7 Jul 2022 18:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Sep 2022 06:24:49 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Dec 2022 07:00:16 GMT",
"version": "v3"
},
{
"created": "Tue, 9 May 2023 20:13:37 GMT",
"version": "v4"
}
] | 2023-06-07 | [
[
"Yadav",
"Gopal",
""
],
[
"Misra",
"Aalok",
""
]
] | Obtaining the Page curve in the context of eternal black holes associated with top-down non-conformal holographic thermal duals at intermediate coupling, has been entirely unexplored in the literature. We fill this gap in the context of a doubly holographic setup relevant to the M-theory dual of thermal QCD-like theori... | 9.072062 | 9.68049 | 10.02607 | 9.033722 | 9.223814 | 9.510226 | 9.373525 | 9.393999 | 9.055021 | 10.354406 | 8.924426 | 8.795063 | 9.15946 | 8.676063 | 8.781159 | 8.740462 | 8.752288 | 8.698606 | 8.540683 | 8.911505 | 8.744812 |
hep-th/0402001 | Ashok Das | Ashok Das, Jorge Gamboa, Fernando M\'endez and Justo L\'opez-Sarri\'on | Chiral bosonization for non-commutative fields | 16 pages, JHEP style, version published in JHEP | JHEP0405:022,2004 | 10.1088/1126-6708/2004/05/022 | null | hep-th | null | A model of chiral bosons on a non-commutative field space is constructed and
new generalized bosonization (fermionization) rules for these fields are given.
The conformal structure of the theory is characterized by a level of the
Kac-Moody algebra equal to $(1+ \theta^2)$ where $\theta$ is the
non-commutativity param... | [
{
"created": "Mon, 2 Feb 2004 19:10:43 GMT",
"version": "v1"
},
{
"created": "Sat, 29 May 2004 11:01:24 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Das",
"Ashok",
""
],
[
"Gamboa",
"Jorge",
""
],
[
"Méndez",
"Fernando",
""
],
[
"López-Sarrión",
"Justo",
""
]
] | A model of chiral bosons on a non-commutative field space is constructed and new generalized bosonization (fermionization) rules for these fields are given. The conformal structure of the theory is characterized by a level of the Kac-Moody algebra equal to $(1+ \theta^2)$ where $\theta$ is the non-commutativity paramet... | 5.518041 | 5.475532 | 5.519718 | 5.118879 | 5.420585 | 5.280491 | 5.425765 | 5.166716 | 4.794796 | 6.100535 | 5.072269 | 5.157171 | 5.38495 | 5.046547 | 5.006074 | 4.897959 | 4.998142 | 4.973557 | 5.186262 | 5.242599 | 4.994932 |
1412.3460 | Lorenzo G. Vitale Mr. | Slava Rychkov, Lorenzo G. Vitale | Hamiltonian Truncation Study of the Phi^4 Theory in Two Dimensions | 41 pages, 27 pictures. Python code included with submission; v2:
improved discussion of the work of Coser et al; v3: exponentially suppressed
correction terms in the finite volume Hamiltonian made explicit; v4: Eq.
(4.7) corrected; v5: refs updated; v6: errors corrected in appendix on
perturbative checks | Phys. Rev. D 91, 085011 (2015) | 10.1103/PhysRevD.91.085011 | CERN-PH-TH-2014-254 | hep-th cond-mat.stat-mech cond-mat.str-el hep-lat math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We defend the Fock-space Hamiltonian truncation method, which allows to
calculate numerically the spectrum of strongly coupled quantum field theories,
by putting them in a finite volume and imposing a UV cutoff. The accuracy of
the method is improved via an analytic renormalization procedure inspired by
the usual eff... | [
{
"created": "Wed, 10 Dec 2014 21:00:12 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Dec 2014 08:35:21 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Feb 2015 16:19:14 GMT",
"version": "v3"
},
{
"created": "Thu, 3 Dec 2015 15:09:11 GMT",
"version": "v4"
},
{
"cr... | 2018-08-21 | [
[
"Rychkov",
"Slava",
""
],
[
"Vitale",
"Lorenzo G.",
""
]
] | We defend the Fock-space Hamiltonian truncation method, which allows to calculate numerically the spectrum of strongly coupled quantum field theories, by putting them in a finite volume and imposing a UV cutoff. The accuracy of the method is improved via an analytic renormalization procedure inspired by the usual effec... | 9.973409 | 8.555675 | 8.92126 | 7.999662 | 8.735149 | 9.164622 | 8.542692 | 8.425345 | 8.042065 | 9.347497 | 8.052323 | 8.460679 | 8.557057 | 8.335526 | 8.653239 | 8.535943 | 8.594855 | 8.300762 | 8.11895 | 8.551657 | 8.709098 |
hep-th/0301236 | Nejat Tevfik Yilmaz | N.T.Yilmaz | Dualisation of the General Scalar Coset in Supergravity Theories | 22 pages | Nucl.Phys.B664:357-370,2003 | 10.1016/S0550-3213(03)00461-9 | null | hep-th | null | The dualised formulation of the symmetric space sigma model is peformed for a
general scalar coset G/K where G is a maximally non-compact group and K is it's
maximal compact subgroup.By using the twisted self-duality condition the
general form of the first-order equations are obtained.The results are applied
to the e... | [
{
"created": "Wed, 29 Jan 2003 15:26:35 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Jan 2003 12:09:44 GMT",
"version": "v2"
},
{
"created": "Mon, 21 Jul 2003 13:34:58 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Yilmaz",
"N. T.",
""
]
] | The dualised formulation of the symmetric space sigma model is peformed for a general scalar coset G/K where G is a maximally non-compact group and K is it's maximal compact subgroup.By using the twisted self-duality condition the general form of the first-order equations are obtained.The results are applied to the exa... | 12.988283 | 10.419174 | 12.2297 | 9.53099 | 10.853487 | 11.140988 | 9.469167 | 10.595615 | 10.158865 | 15.054987 | 10.615923 | 10.370158 | 12.497676 | 11.238513 | 10.889121 | 11.465607 | 11.335408 | 10.869225 | 11.618468 | 11.97159 | 10.953295 |
hep-th/0508207 | Louis J. Clavelli | L. Clavelli | Properties of a future susy universe | 17 pages, 3 figures; intermediate extensions/revisions available at
http://www.bama.ua.edu/~lclavell/Susyria.pdf | Int.J.Mod.Phys. E15 (2006) 1157-1174 | 10.1142/S0218301306004818 | UAHEP053 | hep-th astro-ph hep-ph | null | In the string landscape picture, the effective potential is characterized by
an enormous number of local minima of which only a minuscule fraction are
suitable for the evolution of life. In this "multiverse", random transitions
are continually made between the various minima with the most likely
transitions being to ... | [
{
"created": "Sun, 28 Aug 2005 20:52:18 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Oct 2005 23:51:07 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Clavelli",
"L.",
""
]
] | In the string landscape picture, the effective potential is characterized by an enormous number of local minima of which only a minuscule fraction are suitable for the evolution of life. In this "multiverse", random transitions are continually made between the various minima with the most likely transitions being to mi... | 8.729653 | 8.327948 | 8.414445 | 8.14094 | 8.676029 | 8.593673 | 9.897808 | 7.903569 | 8.049778 | 9.785551 | 8.216346 | 7.767606 | 7.885641 | 7.755447 | 8.200736 | 7.737157 | 7.764655 | 7.915813 | 7.759551 | 8.139514 | 8.010261 |
hep-th/0206253 | Plamen Bojilov | P. Bozhilov | Probe Branes Dynamics in Nonconstant Background Fields | 8 pages, LaTeX, no figures. Talk at First Advanced Research Workshop
on Gravity, Astrophysics, and Strings at the Black Sea, Kiten, June 10-16,
2002, Bulgaria. To be published in the proceedings | null | null | null | hep-th | null | We consider probe p-branes dynamics in string theory backgrounds of general
type. We use an action, which interpolates between Nambu-Goto and Polyakov type
actions. This allows us to give a unified description for the tensile and
tensionless branes. Firstly, we perform our analysis in the frequently used
static gauge... | [
{
"created": "Fri, 28 Jun 2002 10:35:33 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bozhilov",
"P.",
""
]
] | We consider probe p-branes dynamics in string theory backgrounds of general type. We use an action, which interpolates between Nambu-Goto and Polyakov type actions. This allows us to give a unified description for the tensile and tensionless branes. Firstly, we perform our analysis in the frequently used static gauge. ... | 9.370951 | 8.165505 | 10.551349 | 8.700686 | 8.525364 | 8.50575 | 8.010221 | 8.61147 | 8.625084 | 10.064946 | 8.387023 | 8.597188 | 9.151944 | 8.651102 | 8.66622 | 8.399748 | 8.560566 | 8.512601 | 8.521387 | 9.337716 | 8.564359 |
1812.06843 | Hideo Suganuma | Hideo Suganuma (Kyoto U.) | Non-Abelian Higgs Theory in a Strong Magnetic Field and Confinement | 8 pages, 2 figures | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The non-abelian Higgs (NAH) theory is studied in a strong magnetic field. For
simplicity, we study the SU(2) NAH theory with the Higgs triplet in a constant
strong magnetic field $\vec B$, where the lowest-Landau-level (LLL)
approximation can be used. Without magnetic fields, charged vector fields
$A_\mu^\pm$ have a ... | [
{
"created": "Mon, 17 Dec 2018 15:36:09 GMT",
"version": "v1"
}
] | 2018-12-18 | [
[
"Suganuma",
"Hideo",
"",
"Kyoto U."
]
] | The non-abelian Higgs (NAH) theory is studied in a strong magnetic field. For simplicity, we study the SU(2) NAH theory with the Higgs triplet in a constant strong magnetic field $\vec B$, where the lowest-Landau-level (LLL) approximation can be used. Without magnetic fields, charged vector fields $A_\mu^\pm$ have a la... | 6.791175 | 7.24532 | 6.53148 | 6.298222 | 6.980634 | 7.125234 | 6.716867 | 6.987311 | 6.263211 | 6.732987 | 6.59433 | 6.633462 | 6.469262 | 6.3199 | 6.566249 | 6.50667 | 6.606064 | 6.577075 | 6.410117 | 6.709679 | 6.362949 |
0811.1583 | Robert Richter | L. E. Ibanez, R. Richter | Stringy Instantons and Yukawa Couplings in MSSM-like Orientifold Models | 33 pages, 8 figures, v2: corrected typos, added references | JHEP 0903:090,2009 | 10.1088/1126-6708/2009/03/090 | IFT-UAM/CSIC-08-74, UPR-1202-T | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Type IIA orientifold constructions with intersecting D6-branes and their IIB
duals in terms of magnetized D9/D7-branes constitute one of the most promising
avenues for the construction of semirealistic MSSM-like compactifications. One
generic problem with these constructions is, that there are many Yukawa
couplings, ... | [
{
"created": "Mon, 10 Nov 2008 23:00:11 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Dec 2008 21:12:26 GMT",
"version": "v2"
}
] | 2009-04-02 | [
[
"Ibanez",
"L. E.",
""
],
[
"Richter",
"R.",
""
]
] | Type IIA orientifold constructions with intersecting D6-branes and their IIB duals in terms of magnetized D9/D7-branes constitute one of the most promising avenues for the construction of semirealistic MSSM-like compactifications. One generic problem with these constructions is, that there are many Yukawa couplings, wh... | 9.721683 | 8.498364 | 9.188882 | 8.684206 | 9.002324 | 8.772265 | 8.976729 | 8.642149 | 8.476943 | 10.500892 | 8.375375 | 8.402012 | 8.479843 | 8.268332 | 8.404019 | 8.50404 | 8.598299 | 8.566043 | 8.506877 | 9.092649 | 8.453626 |
2205.12293 | Miguel Montero | Miguel Montero, Cumrun Vafa, Irene Valenzuela | The Dark Dimension and the Swampland | 13 pages + refs; 2 figures. v2: further details and references added;
v3: Published version | J. High Energ. Phys. 2023, 22 (2023) | 10.1007/JHEP02(2023)022 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by principles from the Swampland program, which characterize
requirements for a consistent UV completion of quantum gravity, combined with
observational data, we are led to a unique corner of the quantum gravity
landscape. In particular, using the Distance/Duality conjecture and the
smallness of dark energy... | [
{
"created": "Tue, 24 May 2022 18:03:30 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Aug 2022 15:06:34 GMT",
"version": "v2"
},
{
"created": "Fri, 3 Mar 2023 16:04:43 GMT",
"version": "v3"
}
] | 2023-03-06 | [
[
"Montero",
"Miguel",
""
],
[
"Vafa",
"Cumrun",
""
],
[
"Valenzuela",
"Irene",
""
]
] | Motivated by principles from the Swampland program, which characterize requirements for a consistent UV completion of quantum gravity, combined with observational data, we are led to a unique corner of the quantum gravity landscape. In particular, using the Distance/Duality conjecture and the smallness of dark energy, ... | 7.206938 | 7.159412 | 6.756294 | 6.532029 | 6.619964 | 6.74 | 6.631897 | 6.567561 | 6.551602 | 7.374468 | 6.489907 | 6.694362 | 6.913656 | 6.641603 | 6.675714 | 6.917572 | 6.808591 | 6.69919 | 6.660005 | 6.817832 | 6.902678 |
hep-th/0210220 | Andrei Starinets | G.Policastro, D.T.Son and A.O.Starinets | From AdS/CFT correspondence to hydrodynamics. II. Sound waves | 18 pages, 2 figures; typos in eqs. 3.4d and 3.5d corrected | JHEP 0212:054,2002 | 10.1088/1126-6708/2002/12/054 | DAMTP-2002-129, INT-PUB-02-47 | hep-th gr-qc hep-ph | null | As a non-trivial check of the non-supersymmetric gauge/gravity duality, we
use a near-extremal black brane background to compute the retarded Green's
functions of the stress-energy tensor in N=4 super-Yang-Mills (SYM) theory at
finite temperature. For the long-distance, low-frequency modes of the diagonal
components ... | [
{
"created": "Tue, 22 Oct 2002 22:12:28 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Jan 2003 01:20:09 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Jul 2005 01:21:02 GMT",
"version": "v3"
}
] | 2009-07-09 | [
[
"Policastro",
"G.",
""
],
[
"Son",
"D. T.",
""
],
[
"Starinets",
"A. O.",
""
]
] | As a non-trivial check of the non-supersymmetric gauge/gravity duality, we use a near-extremal black brane background to compute the retarded Green's functions of the stress-energy tensor in N=4 super-Yang-Mills (SYM) theory at finite temperature. For the long-distance, low-frequency modes of the diagonal components of... | 5.792833 | 4.71383 | 6.648732 | 4.948215 | 4.658339 | 4.626732 | 4.649426 | 4.710332 | 5.072239 | 6.728177 | 4.839769 | 4.821549 | 5.380141 | 5.015087 | 4.866067 | 4.940392 | 4.945086 | 5.01674 | 4.841217 | 5.438737 | 5.019727 |
hep-th/9809068 | Ryu Sasaki | A.J. Bordner (YITP, Kyoto), R. Sasaki (YITP, Kyoto) and K. Takasaki
(Dept. Fund. Sci., Kyoto) | Calogero-Moser Models II: Symmetries and Foldings | 36 pages, LaTeX2e with amsfonts.sty, no figures | Prog.Theor.Phys. 101 (1999) 487-518 | 10.1143/PTP.101.487 | YITP-98-60, KUCP-0121 | hep-th cond-mat math.DS nlin.SI solv-int | null | Universal Lax pairs (the root type and the minimal type) are presented for
Calogero-Moser models based on simply laced root systems, including E_8. They
exist with and without spectral parameter and they work for all of the four
choices of potentials: the rational, trigonometric, hyperbolic and elliptic.
For the elli... | [
{
"created": "Thu, 10 Sep 1998 08:20:14 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Oct 1998 08:40:52 GMT",
"version": "v2"
},
{
"created": "Tue, 22 Dec 1998 08:19:08 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Bordner",
"A. J.",
"",
"YITP, Kyoto"
],
[
"Sasaki",
"R.",
"",
"YITP, Kyoto"
],
[
"Takasaki",
"K.",
"",
"Dept. Fund. Sci., Kyoto"
]
] | Universal Lax pairs (the root type and the minimal type) are presented for Calogero-Moser models based on simply laced root systems, including E_8. They exist with and without spectral parameter and they work for all of the four choices of potentials: the rational, trigonometric, hyperbolic and elliptic. For the ellipt... | 8.008163 | 7.997836 | 9.993016 | 7.623032 | 8.204734 | 7.857023 | 8.085131 | 7.661547 | 7.046569 | 10.201736 | 7.58229 | 7.581518 | 8.168539 | 7.793108 | 7.638081 | 7.785825 | 7.492297 | 7.528021 | 7.657566 | 8.123165 | 7.735743 |
hep-th/9703012 | null | N. Khviengia, Z. Khviengia, H. Lu and C.N. Pope | Towards a Field Theory of F-theory | Latex, 21 pages. Typos corrected, references added, and discussion
extended | Class.Quant.Grav.15:759-773,1998 | 10.1088/0264-9381/15/4/005 | CTP-TAMU-13/97, LPTENS-97/07 | hep-th | null | We make a proposal for a bosonic field theory in twelve dimensions that
admits the bosonic sector of eleven-dimensional supergravity as a consistent
truncation. It can also be consistently truncated to a ten-dimensional
Lagrangian that contains all the BPS p-brane solitons of the type IIB theory.
The mechanism allowi... | [
{
"created": "Sun, 2 Mar 1997 18:17:45 GMT",
"version": "v1"
},
{
"created": "Sat, 8 Mar 1997 23:16:42 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Khviengia",
"N.",
""
],
[
"Khviengia",
"Z.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
]
] | We make a proposal for a bosonic field theory in twelve dimensions that admits the bosonic sector of eleven-dimensional supergravity as a consistent truncation. It can also be consistently truncated to a ten-dimensional Lagrangian that contains all the BPS p-brane solitons of the type IIB theory. The mechanism allowing... | 8.027208 | 7.694083 | 9.086646 | 7.970805 | 8.067191 | 7.588057 | 7.666652 | 7.892333 | 8.283453 | 9.578046 | 7.621887 | 7.679121 | 8.075091 | 8.010085 | 7.849521 | 7.980694 | 7.852227 | 7.627279 | 7.691273 | 7.898404 | 7.653313 |
0812.4908 | Alexander Burinskii | Alexander Burinskii | Twistor String Structure of the Kerr-Schild Geometry and Consistency of
the Dirac-Kerr System | 11 p. 2 figs. Dedicated to Jubilee of Prof. S.D.Odintsov, based on
the talk at the 5th Math. Phys. Meeting, July 2008, Belgrad | THE PROBLEMS OF MODERN COSMOLOGY. A volume in honour of Professor
S.D. Odintsov in the occasion of his 50 th birthday. pp.129-136, Tomsk, 2009 | null | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Kerr-Schild (KS) geometry of the rotating black-holes and spinning particles
is based on the associated with Kerr theorem twistor structure which is defined
by an analytic curve $F(Z)=0$ in the projective twistor space $Z \in CP^3 .$ On
the other hand, there is a complex Newman representation which describes the
sour... | [
{
"created": "Mon, 29 Dec 2008 14:08:49 GMT",
"version": "v1"
}
] | 2009-03-04 | [
[
"Burinskii",
"Alexander",
""
]
] | Kerr-Schild (KS) geometry of the rotating black-holes and spinning particles is based on the associated with Kerr theorem twistor structure which is defined by an analytic curve $F(Z)=0$ in the projective twistor space $Z \in CP^3 .$ On the other hand, there is a complex Newman representation which describes the source... | 12.955991 | 13.120803 | 13.216921 | 11.744123 | 13.145624 | 12.931722 | 13.11947 | 12.184466 | 12.264415 | 14.635729 | 11.835807 | 12.601278 | 12.659647 | 12.557687 | 12.964884 | 12.955654 | 12.518727 | 12.122186 | 12.629253 | 12.73536 | 12.230365 |
hep-th/0605167 | Rachid Ahl Laamara | R. Ahl Laamara, L.B Drissi, H. Jehjouh, E H Saidi | Pure fermionic twistor like model & target space supersymmetry | null | null | null | null | hep-th | null | Using world line fermions $\Upsilon_{\pm}^{m}=\Upsilon_{\pm}^{m}(\tau) $
valued in vector representation of $SO(d,4-d) $ with $d=2,3,4,$ we develop a
pure fermionic analog of Penrose twistor construction. First, we show that
Fermi antisymmetry requiring $(\Upsilon_{\pm}^{m}) ^{2}=0$ can be solved by
using twistor lik... | [
{
"created": "Wed, 17 May 2006 13:25:34 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Laamara",
"R. Ahl",
""
],
[
"Drissi",
"L. B",
""
],
[
"Jehjouh",
"H.",
""
],
[
"Saidi",
"E H",
""
]
] | Using world line fermions $\Upsilon_{\pm}^{m}=\Upsilon_{\pm}^{m}(\tau) $ valued in vector representation of $SO(d,4-d) $ with $d=2,3,4,$ we develop a pure fermionic analog of Penrose twistor construction. First, we show that Fermi antisymmetry requiring $(\Upsilon_{\pm}^{m}) ^{2}=0$ can be solved by using twistor like ... | 12.615948 | 11.288145 | 11.948051 | 11.235435 | 12.018534 | 11.314472 | 11.608094 | 11.532954 | 11.516131 | 13.348582 | 11.713499 | 10.906454 | 12.019786 | 10.832455 | 10.988454 | 10.925508 | 11.180567 | 11.101227 | 10.697317 | 12.298313 | 11.02055 |
0906.4926 | Balt van Rees | Kostas Skenderis, Marika Taylor, Balt C. van Rees | Topologically Massive Gravity and the AdS/CFT Correspondence | 54 pages, v2: added comments and references | JHEP 0909:045,2009 | 10.1088/1126-6708/2009/09/045 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We set up the AdS/CFT correspondence for topologically massive gravity (TMG)
in three dimensions. The first step in this procedure is to determine the
appropriate fall off conditions at infinity. These cannot be fixed a priori as
they depend on the bulk theory under consideration and are derived by solving
asymptotic... | [
{
"created": "Fri, 26 Jun 2009 13:23:52 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Aug 2009 13:41:11 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Skenderis",
"Kostas",
""
],
[
"Taylor",
"Marika",
""
],
[
"van Rees",
"Balt C.",
""
]
] | We set up the AdS/CFT correspondence for topologically massive gravity (TMG) in three dimensions. The first step in this procedure is to determine the appropriate fall off conditions at infinity. These cannot be fixed a priori as they depend on the bulk theory under consideration and are derived by solving asymptotical... | 6.533776 | 6.495568 | 7.380354 | 6.124514 | 6.814827 | 6.79621 | 6.579402 | 6.736012 | 6.330953 | 7.672785 | 6.241892 | 6.587517 | 6.696553 | 6.321455 | 6.46002 | 6.530996 | 6.468192 | 6.348241 | 6.309193 | 6.536182 | 6.264329 |
hep-th/0305136 | Anton Kapustin | Anton Kapustin, Yi Li | Topological Correlators in Landau-Ginzburg Models with Boundaries | 21 pages, latex. v2: minor typos corrected, references added. v3: a
couple minor corrections, reference added | Adv.Theor.Math.Phys.7:727-749,2004 | null | null | hep-th math.AG | null | We compute topological correlators in Landau-Ginzburg models on a Riemann
surface with arbitrary number of handles and boundaries. The boundaries may
correspond to arbitrary topological D-branes of type B. We also allow arbitrary
operator insertions on the boundary and in the bulk. The answer is given by an
explicit ... | [
{
"created": "Fri, 16 May 2003 07:01:44 GMT",
"version": "v1"
},
{
"created": "Sat, 31 May 2003 00:33:41 GMT",
"version": "v2"
},
{
"created": "Fri, 13 Jun 2003 17:50:30 GMT",
"version": "v3"
},
{
"created": "Tue, 23 Dec 2003 21:02:50 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Kapustin",
"Anton",
""
],
[
"Li",
"Yi",
""
]
] | We compute topological correlators in Landau-Ginzburg models on a Riemann surface with arbitrary number of handles and boundaries. The boundaries may correspond to arbitrary topological D-branes of type B. We also allow arbitrary operator insertions on the boundary and in the bulk. The answer is given by an explicit fo... | 6.306809 | 5.574319 | 7.606562 | 5.702844 | 5.831148 | 5.629666 | 5.700004 | 5.835021 | 6.03201 | 9.60661 | 5.678236 | 5.996008 | 7.052395 | 5.913581 | 6.017729 | 5.983318 | 6.257636 | 6.151329 | 5.863243 | 6.669421 | 5.765091 |
2306.17192 | Tal Miller | Tal Miller | The conformal manifold of three dimensional $\mathcal{N}=4$
supersymmetric star-shaped-quiver theories | Masters thesis | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this thesis we calculate the dimension of the conformal manifold (DCM) for
a class of 3d $\mathcal{N}=4$ supersymmetric theories called the
star-shaped-quiver (SSQ) theories. These theories are the mirror dual theories
of class $\mathfrak{s}$ theories, constructed as a compactification of the 4d
class $\mathcal{S}... | [
{
"created": "Wed, 28 Jun 2023 08:33:44 GMT",
"version": "v1"
}
] | 2023-07-03 | [
[
"Miller",
"Tal",
""
]
] | In this thesis we calculate the dimension of the conformal manifold (DCM) for a class of 3d $\mathcal{N}=4$ supersymmetric theories called the star-shaped-quiver (SSQ) theories. These theories are the mirror dual theories of class $\mathfrak{s}$ theories, constructed as a compactification of the 4d class $\mathcal{S}$ ... | 4.656882 | 4.714715 | 5.38101 | 4.455696 | 4.760302 | 4.557129 | 4.77054 | 4.693872 | 4.663037 | 5.308851 | 4.685171 | 4.453084 | 4.774886 | 4.568861 | 4.535609 | 4.556137 | 4.591322 | 4.433268 | 4.517136 | 4.651534 | 4.490221 |
1110.5902 | David Tong | Stefano Bolognesi and David Tong | Magnetic Catalysis in AdS4 | 22 pages, 4 figures. v2: References added, factors of 2 corrected,
extra comments added in appendix. v3: extra comments about fermion modes in a
hard wall background. v4: A final factor of 2 | null | 10.1088/0264-9381/29/19/194003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the formation of fermion condensates in Anti de Sitter space. In
particular, we describe a novel version of magnetic catalysis that arises for
fermions in asymptotically AdS4 geometries which cap off in the infra-red with
a hard wall. We show that the presence of a magnetic field induces a fermion
condensate... | [
{
"created": "Wed, 26 Oct 2011 19:58:22 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Nov 2011 10:43:23 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Jan 2012 14:01:16 GMT",
"version": "v3"
},
{
"created": "Thu, 26 Apr 2012 19:32:29 GMT",
"version": "v4"
}
] | 2015-05-30 | [
[
"Bolognesi",
"Stefano",
""
],
[
"Tong",
"David",
""
]
] | We study the formation of fermion condensates in Anti de Sitter space. In particular, we describe a novel version of magnetic catalysis that arises for fermions in asymptotically AdS4 geometries which cap off in the infra-red with a hard wall. We show that the presence of a magnetic field induces a fermion condensate i... | 7.066895 | 6.22918 | 7.309443 | 6.266444 | 6.501536 | 6.663365 | 5.997717 | 6.049128 | 6.451971 | 7.015281 | 6.417453 | 6.675477 | 6.800681 | 6.610504 | 6.532259 | 6.788908 | 6.599764 | 6.767444 | 6.386833 | 6.951637 | 6.50863 |
1408.2540 | Roberto Gobbetti | Guido D'Amico, Roberto Gobbetti, Matthew Kleban, Marjorie Schillo | D-brane scattering and annihilation | 25+7 pages, 5 figures | null | 10.1007/JHEP01(2015)050 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the dynamics of parallel brane-brane and brane-antibrane scattering
in string theory in flat spacetime, focusing on the pair production of open
strings that stretch between the branes. We are particularly interested in the
case of scattering at small impact parameter $b < l_s$, where there is a
tachyon in th... | [
{
"created": "Mon, 11 Aug 2014 20:16:19 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"D'Amico",
"Guido",
""
],
[
"Gobbetti",
"Roberto",
""
],
[
"Kleban",
"Matthew",
""
],
[
"Schillo",
"Marjorie",
""
]
] | We study the dynamics of parallel brane-brane and brane-antibrane scattering in string theory in flat spacetime, focusing on the pair production of open strings that stretch between the branes. We are particularly interested in the case of scattering at small impact parameter $b < l_s$, where there is a tachyon in the ... | 6.843804 | 7.090087 | 8.205988 | 6.646901 | 7.018368 | 6.929418 | 7.088816 | 6.43654 | 6.55067 | 7.638635 | 6.687334 | 6.401077 | 6.940567 | 6.487255 | 6.893486 | 6.564751 | 6.630337 | 6.690436 | 6.563198 | 6.818805 | 6.64171 |
0904.0381 | Gorsky Alexander | A. Gorsky and A. Zhiboedov | One-loop derivation of the Wilson polygon - MHV amplitude duality | 29 pages | J.Phys.A42:355214,2009 | 10.1088/1751-8113/42/35/355214 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the origin of the Wilson polygon - MHV amplitude duality at the
perturbative level. It is shown that the duality for the MHV amplitudes at
one-loop level can be proven upon the peculiar change of variables in Feynman
parametrization and the use of the relation between Feynman integrals at the
different spa... | [
{
"created": "Thu, 2 Apr 2009 13:04:22 GMT",
"version": "v1"
}
] | 2010-12-17 | [
[
"Gorsky",
"A.",
""
],
[
"Zhiboedov",
"A.",
""
]
] | We discuss the origin of the Wilson polygon - MHV amplitude duality at the perturbative level. It is shown that the duality for the MHV amplitudes at one-loop level can be proven upon the peculiar change of variables in Feynman parametrization and the use of the relation between Feynman integrals at the different space... | 10.961212 | 9.941596 | 11.901638 | 9.664329 | 10.873024 | 10.586058 | 11.829465 | 9.760121 | 10.129856 | 11.676079 | 9.802822 | 10.340985 | 10.870916 | 10.354897 | 10.346725 | 10.844427 | 10.67194 | 10.207505 | 10.309509 | 10.913379 | 10.55045 |
1106.4566 | Hong Lu | Haishan Liu, H. Lu and Zhao-Long Wang | Killing Spinors for the Bosonic String and the Kaluza-Klein Theory with
Scalar Potentials | Latex, 17 pages, typos corrected and further comments added | null | 10.1140/epjc/s10052-011-1853-5 | CAS-KITPC/ITP-271, KIAS-P11036 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The paper consists mainly of two parts. In the first part, we obtain
well-defined Killing spinor equations for the low-energy effective action of
the bosonic string with the conformal anomaly term. We show that the conformal
anomaly term is the only scalar potential that one can add into the action that
is consistent... | [
{
"created": "Wed, 22 Jun 2011 20:39:29 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Aug 2011 08:28:35 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Liu",
"Haishan",
""
],
[
"Lu",
"H.",
""
],
[
"Wang",
"Zhao-Long",
""
]
] | The paper consists mainly of two parts. In the first part, we obtain well-defined Killing spinor equations for the low-energy effective action of the bosonic string with the conformal anomaly term. We show that the conformal anomaly term is the only scalar potential that one can add into the action that is consistent w... | 6.658196 | 6.277251 | 6.988785 | 6.115909 | 6.449106 | 6.056177 | 6.18368 | 6.015635 | 6.363499 | 7.031885 | 6.153778 | 6.139105 | 6.586863 | 6.426971 | 6.333128 | 6.535572 | 6.207403 | 6.21722 | 6.236734 | 6.454938 | 6.258593 |
0909.4081 | Thomas S. Levi | Thomas S. Levi, Joris Raeymaekers, Dieter Van den Bleeken, Walter Van
Herck, Bert Vercnocke | Godel space from wrapped M2-branes | 21 pages+appendices, 3 figures | JHEP 1001:082,2010 | 10.1007/JHEP01(2010)082 | WITS-CTP-041, KUL-TF-09/20 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that M-theory admits a supersymmetric compactification to the Godel
universe of the form Godel3 x S2 x CY3. We interpret this geometry as coming
from the backreaction of M2-branes wrapping the S2 in an AdS3 x S2 x CY3 flux
compactification. In the black hole deconstruction proposal similar states give
rise to... | [
{
"created": "Wed, 23 Sep 2009 18:40:43 GMT",
"version": "v1"
}
] | 2010-04-28 | [
[
"Levi",
"Thomas S.",
""
],
[
"Raeymaekers",
"Joris",
""
],
[
"Bleeken",
"Dieter Van den",
""
],
[
"Van Herck",
"Walter",
""
],
[
"Vercnocke",
"Bert",
""
]
] | We show that M-theory admits a supersymmetric compactification to the Godel universe of the form Godel3 x S2 x CY3. We interpret this geometry as coming from the backreaction of M2-branes wrapping the S2 in an AdS3 x S2 x CY3 flux compactification. In the black hole deconstruction proposal similar states give rise to t... | 9.07821 | 8.117398 | 10.764689 | 8.120237 | 7.986759 | 8.762656 | 8.897277 | 8.133101 | 8.019338 | 10.607323 | 8.104553 | 8.245038 | 9.347087 | 8.494234 | 8.161918 | 8.595126 | 7.90159 | 8.426134 | 8.118384 | 9.645437 | 8.349422 |
hep-th/9703019 | Juan Carlos Perez Bueno | J. A. de Azcarraga, J. M. Izquierdo and J. C. Perez Bueno | On the generalizations of Poisson structures | Latex file. 12 pages. Trivial changes, a misprint (subindices)
corrected. To appear in J. Phys. A (letters) | J.Phys. A30 (1997) L607-L616 | 10.1088/0305-4470/30/18/001 | DAMTP/97-12 | hep-th dg-ga math.DG math.QA q-alg | null | The characterization of the Nambu-Poisson n-tensors as a subfamily of the
Generalized-Poisson ones recently introduced (and here extended to the odd
order case) is discussed. The homology and cohomology complexes of both
structures are compared, and some physical considerations are made.
| [
{
"created": "Mon, 3 Mar 1997 18:18:49 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jul 1997 16:18:09 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"de Azcarraga",
"J. A.",
""
],
[
"Izquierdo",
"J. M.",
""
],
[
"Bueno",
"J. C. Perez",
""
]
] | The characterization of the Nambu-Poisson n-tensors as a subfamily of the Generalized-Poisson ones recently introduced (and here extended to the odd order case) is discussed. The homology and cohomology complexes of both structures are compared, and some physical considerations are made. | 16.859484 | 19.485443 | 17.022306 | 15.647414 | 16.472672 | 19.384476 | 19.559502 | 16.251038 | 15.707121 | 18.795605 | 17.67725 | 16.168083 | 16.10545 | 15.525978 | 16.097668 | 16.572117 | 16.657558 | 16.076151 | 15.803418 | 16.510281 | 15.263508 |
2006.12924 | Eugenio R. Bezerra de Mello | D\^eivid R. da Silva and E. R. Bezerra de Mello | Electromagnetic Casimir effect in a Lorentz symmetry violation model | 16 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the electromagnetic Casimir effects in the context of
Lorentz symmetry violations. Two distinct approaches are considered: the first
one is based on Horava-Lifshitz methodology, which explicitly presents a
space-time anisotropy, while the second is a model that includes
higher-derivatives in t... | [
{
"created": "Tue, 23 Jun 2020 11:58:51 GMT",
"version": "v1"
}
] | 2020-06-24 | [
[
"da Silva",
"Dêivid R.",
""
],
[
"de Mello",
"E. R. Bezerra",
""
]
] | In this paper, we study the electromagnetic Casimir effects in the context of Lorentz symmetry violations. Two distinct approaches are considered: the first one is based on Horava-Lifshitz methodology, which explicitly presents a space-time anisotropy, while the second is a model that includes higher-derivatives in the... | 7.863151 | 6.382067 | 7.956131 | 6.419373 | 6.508259 | 6.490874 | 6.273286 | 6.608854 | 6.071262 | 8.007303 | 6.550499 | 6.621124 | 7.340231 | 7.020863 | 7.038873 | 6.889532 | 6.867978 | 6.747003 | 7.031606 | 7.453118 | 6.952465 |
hep-th/0311040 | David H. Lyth | David H. Lyth | Which is the best inflation model? | To appear in the proceedings of "String Phenomenoloy 03" (Durham,
2003) | null | null | null | hep-th | null | Reasonable-looking models of inflation are compared, taking into account the
possibility that the curvature perturbation might originate from some
"curvaton" field different from the inflaton.
| [
{
"created": "Wed, 5 Nov 2003 18:15:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Lyth",
"David H.",
""
]
] | Reasonable-looking models of inflation are compared, taking into account the possibility that the curvature perturbation might originate from some "curvaton" field different from the inflaton. | 19.0404 | 13.08775 | 13.292525 | 12.77013 | 16.080986 | 13.437069 | 13.645148 | 12.543349 | 13.234295 | 14.000957 | 15.251586 | 12.183464 | 12.703239 | 12.112334 | 12.017107 | 11.9861 | 11.038486 | 11.831589 | 11.655183 | 12.723335 | 16.012911 |
hep-th/0504216 | Nikolay Pletnev | I.L. Buchbinder, N.G. Pletnev | Construction of one-loop ${\cal N}=4$ SYM effective action on the mixed
branch in the harmonic superspace approach | 35 pages, JHEP style | JHEP 0509 (2005) 073 | 10.1088/1126-6708/2005/09/073 | null | hep-th | null | We develop a systematic approach to construct the one-loop ${\cal N}=4$ SYM
effective action depending on both ${\cal N}=2$ vector multiplet and
hypermultiplet background fields. Beginning with the formulation of ${\cal
N}=4$ SYM theory in terms of ${\cal N}=2$ harmonic superfields, we construct
the one-loop effectiv... | [
{
"created": "Wed, 27 Apr 2005 08:39:25 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Jul 2005 08:43:57 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Pletnev",
"N. G.",
""
]
] | We develop a systematic approach to construct the one-loop ${\cal N}=4$ SYM effective action depending on both ${\cal N}=2$ vector multiplet and hypermultiplet background fields. Beginning with the formulation of ${\cal N}=4$ SYM theory in terms of ${\cal N}=2$ harmonic superfields, we construct the one-loop effective ... | 5.762834 | 5.334203 | 6.521377 | 5.340983 | 5.338933 | 5.418535 | 5.323517 | 5.227901 | 5.564905 | 6.991657 | 5.371046 | 5.485126 | 5.868027 | 5.492856 | 5.668793 | 5.371408 | 5.661222 | 5.460018 | 5.521682 | 5.716783 | 5.558376 |
hep-th/0606145 | Alin Tirziu | J.A. Minahan, A. Tirziu and A.A. Tseytlin | Infinite spin limit of semiclassical string states | 38 pages, 3 figures; v2: comments on derivation of bound states of
magnons from discrete Bethe equations added in section 4 and appendix C,
references added, Imperial-TP-AT-6-4, HUTP-06/A0024 | JHEP 0608:049,2006 | 10.1088/1126-6708/2006/08/049 | null | hep-th | null | Motivated by recent works of Hofman and Maldacena and Dorey we consider a
special infinite spin limit of semiclassical spinning string states in AdS5 x
S5. We discuss examples of known folded and circular 2-spin string solutions
and demonstrate explicitly that the 1-loop superstring correction to the
classical expres... | [
{
"created": "Thu, 15 Jun 2006 18:49:26 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Jun 2006 16:51:10 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Minahan",
"J. A.",
""
],
[
"Tirziu",
"A.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | Motivated by recent works of Hofman and Maldacena and Dorey we consider a special infinite spin limit of semiclassical spinning string states in AdS5 x S5. We discuss examples of known folded and circular 2-spin string solutions and demonstrate explicitly that the 1-loop superstring correction to the classical expressi... | 9.681706 | 7.433882 | 10.773964 | 7.487103 | 7.975201 | 7.604335 | 7.566945 | 7.709443 | 7.979327 | 11.782594 | 7.722057 | 8.1196 | 9.351536 | 8.702236 | 8.608672 | 8.480507 | 8.263381 | 8.649289 | 8.642796 | 8.9709 | 8.847131 |
hep-th/0208181 | Yannick Meurice | Y. Meurice | Complex singularities of the critical potential in the large-N limit | 9 pages, 9 figures, uses revtex | Phys.Rev. D67 (2003) 025006 | 10.1103/PhysRevD.67.025006 | null | hep-th cond-mat.stat-mech hep-lat math-ph math.MP | null | We show with two numerical examples that the conventional expansion in powers
of the field for the critical potential of 3-dimensional O(N) models in the
large-N limit, does not converge for values of phi^2 larger than some critical
value. This can be explained by the existence of conjugated branch points in
the comp... | [
{
"created": "Sun, 25 Aug 2002 20:35:03 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Sep 2002 20:24:04 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Meurice",
"Y.",
""
]
] | We show with two numerical examples that the conventional expansion in powers of the field for the critical potential of 3-dimensional O(N) models in the large-N limit, does not converge for values of phi^2 larger than some critical value. This can be explained by the existence of conjugated branch points in the comple... | 11.116596 | 10.734491 | 12.272265 | 10.122893 | 11.803586 | 10.888117 | 10.284984 | 10.908644 | 10.466022 | 12.553128 | 10.168121 | 10.514411 | 11.314971 | 10.504402 | 10.54996 | 10.527101 | 10.249846 | 10.571024 | 10.23576 | 11.093882 | 10.361025 |
hep-th/9412233 | null | A.A. Slavnov | Generalized Pauli-Villars regularization for undoubled lattice fermions | 10 pages LATEX file | Phys.Lett. B348 (1995) 553-559 | 10.1016/0370-2693(95)00202-V | SMI-9-94 | hep-th | null | A manifestly gauge invariant formulation of chiral theories with fermions on
the lattice is developed. It combines SLAC lattice derivative \cite{DWY},
\cite{ACS}, \cite{S} and generalized Pauli-Villars regularization \cite{FS}.
The theory is free of fermion doubling, requires only local gauge invariant
counterterms a... | [
{
"created": "Thu, 29 Dec 1994 08:13:48 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Slavnov",
"A. A.",
""
]
] | A manifestly gauge invariant formulation of chiral theories with fermions on the lattice is developed. It combines SLAC lattice derivative \cite{DWY}, \cite{ACS}, \cite{S} and generalized Pauli-Villars regularization \cite{FS}. The theory is free of fermion doubling, requires only local gauge invariant counterterms and... | 13.428029 | 15.567634 | 13.445914 | 12.857269 | 14.2706 | 11.812642 | 14.331397 | 12.793791 | 14.850487 | 17.836098 | 13.122045 | 12.654031 | 13.359082 | 12.895274 | 12.308337 | 12.611542 | 12.330953 | 12.403482 | 12.350505 | 13.316381 | 12.881325 |
hep-th/0412198 | Dafni Marchioro | Nathan Berkovits, Dafni Z. Marchioro (IFT/UNESP - Sao Paulo) | Relating the Green-Schwarz and Pure Spinor Formalisms for the
Superstring | 16 pages, JHEP format, fixed typos and added 2 footnotes | JHEP 0501:018,2005 | 10.1088/1126-6708/2005/01/018 | IFT-P.058/2004 | hep-th | null | Although it is not known how to covariantly quantize the Green-Schwarz (GS)
superstring, there exists a semi-light-cone gauge choice in which the GS
superstring can be quantized in a conformally invariant manner. In this paper,
we prove that BRST quantization of the GS superstring in semi-light-cone gauge
is equivale... | [
{
"created": "Fri, 17 Dec 2004 19:40:02 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Dec 2004 13:12:19 GMT",
"version": "v2"
}
] | 2011-08-11 | [
[
"Berkovits",
"Nathan",
"",
"IFT/UNESP - Sao Paulo"
],
[
"Marchioro",
"Dafni Z.",
"",
"IFT/UNESP - Sao Paulo"
]
] | Although it is not known how to covariantly quantize the Green-Schwarz (GS) superstring, there exists a semi-light-cone gauge choice in which the GS superstring can be quantized in a conformally invariant manner. In this paper, we prove that BRST quantization of the GS superstring in semi-light-cone gauge is equivalent... | 5.243344 | 4.318396 | 5.178742 | 4.304233 | 4.175324 | 4.013389 | 4.162549 | 4.076862 | 4.427385 | 5.454254 | 4.212325 | 4.460101 | 4.872553 | 4.625395 | 4.538783 | 4.736814 | 4.51849 | 4.614058 | 4.464518 | 5.123079 | 4.748564 |
1309.2098 | Li Li | Rong-Gen Cai, Song He, Li Li, Li-Fang Li | A Holographic Study on Vector Condensate Induced by a Magnetic Field | v3: minor changes, references added, to appear in JHEP | JHEP 1312 (2013) 036 | 10.1007/JHEP12(2013)036 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a holographic model with vector condensate by coupling the anti-de
Sitter gravity to an Abelian gauge field and a charged vector field in $(3+1)$
dimensional spacetime. In this model there exists a non-minimal coupling of the
vector filed to the gauge field. We find that there is a critical temperature
below... | [
{
"created": "Mon, 9 Sep 2013 10:24:57 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Sep 2013 13:37:41 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Dec 2013 07:10:36 GMT",
"version": "v3"
}
] | 2014-01-27 | [
[
"Cai",
"Rong-Gen",
""
],
[
"He",
"Song",
""
],
[
"Li",
"Li",
""
],
[
"Li",
"Li-Fang",
""
]
] | We study a holographic model with vector condensate by coupling the anti-de Sitter gravity to an Abelian gauge field and a charged vector field in $(3+1)$ dimensional spacetime. In this model there exists a non-minimal coupling of the vector filed to the gauge field. We find that there is a critical temperature below w... | 5.975058 | 5.411651 | 6.024623 | 5.3353 | 5.630809 | 5.444281 | 5.309734 | 5.05864 | 5.20661 | 7.092309 | 5.373326 | 5.530382 | 5.914149 | 5.546775 | 5.752828 | 5.647962 | 5.535408 | 5.701886 | 5.599323 | 6.142679 | 5.798186 |
1504.00349 | Marco Matone | Marco Matone | A Surprising Relation for the Effective Coupling Constants of N=2 Super
Yang-Mills Theories | 7 pages | JHEP06(2015)109 | 10.1007/JHEP06(2015)109 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the effective coupling constants $\tau$ of supersymmetric gauge
theories described by hyperelliptic curves do not distinguish between the
lattices of the two kinds of heterotic string. In particular, the following
relation $$ \Theta_{D_{16}^+}(\tau)=\Theta_{E_8}^2(\tau) $$ holds. This is
reminiscent of t... | [
{
"created": "Wed, 1 Apr 2015 19:48:46 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Matone",
"Marco",
""
]
] | We show that the effective coupling constants $\tau$ of supersymmetric gauge theories described by hyperelliptic curves do not distinguish between the lattices of the two kinds of heterotic string. In particular, the following relation $$ \Theta_{D_{16}^+}(\tau)=\Theta_{E_8}^2(\tau) $$ holds. This is reminiscent of the... | 9.432551 | 9.306864 | 9.32186 | 9.195181 | 9.659116 | 9.282094 | 10.160173 | 8.801624 | 9.220243 | 10.234197 | 8.648537 | 8.788647 | 9.344656 | 9.519135 | 9.364137 | 9.393336 | 9.635303 | 8.935401 | 9.506743 | 10.039991 | 9.01564 |
1104.2798 | Fabio Ferrari Ruffino | Fabio Ferrari Ruffino | Classifying A-field and B-field configurations in the presence of
D-branes - Part II: Stacks of D-branes | 29 pages | Nuclear Physics, Section B 858 (2012), pp. 377-404 | 10.1016/j.nuclphysb.2012.01.013 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the paper arXiv:0810.4291 we have shown, in the context of type II
superstring theory, the classification of the allowed B-field and A-field
configurations in the presence of anomaly-free D-branes, the mathematical
framework being provided by the geometry of gerbes. Here we complete the
discussion considering in d... | [
{
"created": "Thu, 14 Apr 2011 15:13:09 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Jun 2011 17:10:31 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Nov 2011 17:28:07 GMT",
"version": "v3"
},
{
"created": "Mon, 16 Jan 2012 11:33:33 GMT",
"version": "v4"
},
{
"c... | 2012-01-30 | [
[
"Ruffino",
"Fabio Ferrari",
""
]
] | In the paper arXiv:0810.4291 we have shown, in the context of type II superstring theory, the classification of the allowed B-field and A-field configurations in the presence of anomaly-free D-branes, the mathematical framework being provided by the geometry of gerbes. Here we complete the discussion considering in det... | 9.270713 | 10.250855 | 9.792742 | 9.169041 | 10.646189 | 10.28735 | 9.580466 | 9.123168 | 8.978767 | 10.344474 | 9.202783 | 8.697119 | 8.918687 | 8.882684 | 9.033362 | 8.998443 | 8.831492 | 8.975925 | 8.811301 | 8.95461 | 8.969764 |
1203.5921 | Christian Saemann | Christian Saemann and Richard J. Szabo | Groupoid Quantization of Loop Spaces | 19 pages, Proceedings of the Corfu Summer Institute 2011 - School and
Workshops on Elementary Particle Physics and Gravity, September 4-18, 2011,
Corfu, Greece | null | null | HWM-12-02, EMPG-12-03 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the various contexts in which quantized 2-plectic manifolds are
expected to appear within closed string theory and M-theory. We then discuss
how the quantization of a 2-plectic manifold can be reduced to ordinary
quantization of its loop space, which is a symplectic manifold. We demonstrate
how the latter c... | [
{
"created": "Tue, 27 Mar 2012 10:36:16 GMT",
"version": "v1"
}
] | 2012-03-28 | [
[
"Saemann",
"Christian",
""
],
[
"Szabo",
"Richard J.",
""
]
] | We review the various contexts in which quantized 2-plectic manifolds are expected to appear within closed string theory and M-theory. We then discuss how the quantization of a 2-plectic manifold can be reduced to ordinary quantization of its loop space, which is a symplectic manifold. We demonstrate how the latter can... | 6.81869 | 5.524151 | 6.440684 | 5.585573 | 5.705326 | 5.459597 | 5.760676 | 5.797738 | 5.691549 | 7.18136 | 5.743812 | 6.272667 | 6.604855 | 6.180407 | 6.054567 | 6.025951 | 5.911193 | 6.289666 | 6.087546 | 6.446099 | 5.965425 |
1011.5672 | Alexey Koshelev | Federico Galli and Alexey S. Koshelev | Perturbative stability of SFT-based cosmological models | Version accepted for publicatin in JCAP, 19 pages, 6 figures, uses
jcappub.sty | null | 10.1088/1475-7516/2011/05/012 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the appearance of multiple scalar fields in linearized SFT based
cosmological models with a single non-local scalar field. Some of these local
fields are canonical real scalar fields and some are complex fields with
unusual coupling. These systems only admit numerical or approximate analysis.
We introduce a... | [
{
"created": "Thu, 25 Nov 2010 19:17:52 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Jun 2011 13:10:41 GMT",
"version": "v2"
}
] | 2013-12-03 | [
[
"Galli",
"Federico",
""
],
[
"Koshelev",
"Alexey S.",
""
]
] | We review the appearance of multiple scalar fields in linearized SFT based cosmological models with a single non-local scalar field. Some of these local fields are canonical real scalar fields and some are complex fields with unusual coupling. These systems only admit numerical or approximate analysis. We introduce a m... | 14.255906 | 13.36823 | 13.788812 | 13.357006 | 13.707297 | 15.280636 | 14.209796 | 12.953727 | 13.263449 | 14.561999 | 13.158214 | 13.497252 | 13.363093 | 13.251187 | 13.318855 | 13.447764 | 13.337095 | 13.067122 | 13.387593 | 13.452061 | 13.445083 |
hep-th/9406202 | Centro De Estudios Cientificos De Santia | J.Zanelli | Quantization of the Gravitational Constant in Odd-Dimensional Gravity | 9 pages, LaTeX | Phys.Rev. D51 (1995) 490-492 | 10.1103/PhysRevD.51.490 | null | hep-th gr-qc | null | It is pointed out that the action recently proposed by Ba\~nados et al. for
gravitation in odd dimensions higher (and lower) than four, provides a natural
quantization for the gravitational constant. These theories possess no
dimensionful parameters and hence they may be power counting renormalizable.
| [
{
"created": "Tue, 28 Jun 1994 21:24:33 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Zanelli",
"J.",
""
]
] | It is pointed out that the action recently proposed by Ba\~nados et al. for gravitation in odd dimensions higher (and lower) than four, provides a natural quantization for the gravitational constant. These theories possess no dimensionful parameters and hence they may be power counting renormalizable. | 18.544813 | 12.543089 | 12.020219 | 12.217736 | 13.089455 | 12.958394 | 12.910653 | 12.286963 | 12.869478 | 12.306034 | 11.789231 | 12.667738 | 12.362079 | 12.441212 | 12.254076 | 12.332323 | 12.959243 | 11.783591 | 12.688136 | 12.516321 | 11.504073 |
1708.08943 | Challenger Mishra | Andre Lukas and Challenger Mishra | Discrete Symmetries of Complete Intersection Calabi-Yau Manifolds | 23 pages; minor changes: updated a reference, removed unclear
sentence | null | 10.1007/s00220-020-03838-6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we classify non-freely acting discrete symmetries of complete
intersection Calabi- Yau manifolds and their quotients by freely-acting
symmetries. These non-freely acting symmetries can appear as symmetries of
low-energy theories resulting from string compactifications on these Calabi-Yau
manifolds, par... | [
{
"created": "Tue, 29 Aug 2017 18:03:39 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Aug 2017 11:41:43 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Oct 2017 09:30:49 GMT",
"version": "v3"
}
] | 2020-09-04 | [
[
"Lukas",
"Andre",
""
],
[
"Mishra",
"Challenger",
""
]
] | In this paper, we classify non-freely acting discrete symmetries of complete intersection Calabi- Yau manifolds and their quotients by freely-acting symmetries. These non-freely acting symmetries can appear as symmetries of low-energy theories resulting from string compactifications on these Calabi-Yau manifolds, parti... | 6.890615 | 6.744523 | 7.220288 | 6.295579 | 6.247757 | 6.760444 | 6.667097 | 6.325812 | 6.522764 | 7.503288 | 6.73618 | 6.306234 | 6.652994 | 6.400174 | 6.559724 | 6.489962 | 6.243553 | 6.374403 | 6.360984 | 6.464863 | 6.338661 |
hep-th/0504049 | Jorgen Rasmussen | Adil Belhaj, Jorgen Rasmussen, El Hassan Saidi, Abdellah Sebbar | Non-commutative ADE geometries as holomorphic wave equations | 17 pages, v2: version to be published | Nucl.Phys. B727 (2005) 499-512 | 10.1016/j.nuclphysb.2005.08.039 | GNPHE/0501-VACBT/0501 | hep-th | null | Borrowing ideas from the relation between classical and quantum mechanics, we
study a non-commutative elevation of the ADE geometries involved in building
Calabi-Yau manifolds. We derive the corresponding geometric hamiltonians and
the holomorphic wave equations representing these non-commutative geometries.
The spec... | [
{
"created": "Wed, 6 Apr 2005 16:45:38 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Sep 2005 01:19:08 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Belhaj",
"Adil",
""
],
[
"Rasmussen",
"Jorgen",
""
],
[
"Saidi",
"El Hassan",
""
],
[
"Sebbar",
"Abdellah",
""
]
] | Borrowing ideas from the relation between classical and quantum mechanics, we study a non-commutative elevation of the ADE geometries involved in building Calabi-Yau manifolds. We derive the corresponding geometric hamiltonians and the holomorphic wave equations representing these non-commutative geometries. The spectr... | 15.086798 | 13.348495 | 14.568958 | 12.113688 | 14.036368 | 13.041477 | 12.769897 | 12.824113 | 13.159296 | 15.031968 | 12.166542 | 12.690214 | 12.477966 | 12.716279 | 12.476979 | 12.796598 | 12.40259 | 12.611178 | 12.886762 | 12.847574 | 12.091868 |
2106.11786 | Carlo Alberto Cremonini | C.A.Cremonini and P.A.Grassi | Cohomology of Lie Superalgebras: Forms, Pseudoforms, and Integral Forms | null | null | null | null | hep-th math-ph math.MP math.QA math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the cohomology of Lie superalgebras for the full complex of forms:
superforms, pseudoforms and integral forms. We use the technique of spectral
sequences to abstractly compute the Chevalley-Eilenberg cohomology. We first
focus on the superalgebra $\mathfrak{osp}(2|2)$ and show that there exist
non-empty coho... | [
{
"created": "Tue, 22 Jun 2021 13:54:11 GMT",
"version": "v1"
}
] | 2021-06-25 | [
[
"Cremonini",
"C. A.",
""
],
[
"Grassi",
"P. A.",
""
]
] | We study the cohomology of Lie superalgebras for the full complex of forms: superforms, pseudoforms and integral forms. We use the technique of spectral sequences to abstractly compute the Chevalley-Eilenberg cohomology. We first focus on the superalgebra $\mathfrak{osp}(2|2)$ and show that there exist non-empty cohomo... | 8.122354 | 8.558778 | 8.77736 | 7.987856 | 8.468648 | 8.185506 | 8.67509 | 8.090213 | 8.219285 | 9.361856 | 8.334788 | 7.762541 | 8.34077 | 8.017502 | 7.823634 | 7.692729 | 7.767488 | 7.82275 | 7.934793 | 8.080966 | 7.557782 |
hep-th/9402072 | Wolfgang Bietenholz | W. Bietenholz | Goldstone Bosons in a Finite Volume: The Partition Function to Three
Loops | 59 pages, published in Helv. Phys. Acta 66(6) p.633 | Helv.Phys.Acta 66 (1993) 633-691 | null | null | hep-th hep-lat nucl-th | null | A system of Goldstone bosons - stemming from a symmetry breaking $O(N) \to
O(N-1)$ - in a finite volume at finite temperature is considered. In the
framework of dimensional regularization, the partition function is calculated
to 3 loops for 3 and 4 dimensions, where Polyakov's measure for the functional
integration i... | [
{
"created": "Fri, 11 Feb 1994 19:16:54 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Bietenholz",
"W.",
""
]
] | A system of Goldstone bosons - stemming from a symmetry breaking $O(N) \to O(N-1)$ - in a finite volume at finite temperature is considered. In the framework of dimensional regularization, the partition function is calculated to 3 loops for 3 and 4 dimensions, where Polyakov's measure for the functional integration is ... | 12.08155 | 12.495355 | 12.39844 | 11.584231 | 11.617463 | 11.688802 | 12.690816 | 11.665052 | 11.858505 | 12.901486 | 11.392814 | 11.575378 | 12.036853 | 11.507628 | 11.835982 | 11.458422 | 11.752013 | 11.283309 | 11.762472 | 11.551947 | 11.529337 |
hep-th/0503150 | Gautam Bhattacharya Professor | Gautam Bhattacharya | Criteria for Exact Solubility of Relativistic Field Theories by
Scattering Transform | 15 pages | null | null | null | hep-th | null | Scattering transform is a well known powerful tool for quantisation of field
theories in (1+1) dimensions. Conventionally only those models whose classical
counterparts admit a Lax pair (origin of which is always mysterious) have been
quantised in this way. In relativistic quantum field theories we show that the
scat... | [
{
"created": "Sat, 19 Mar 2005 15:54:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bhattacharya",
"Gautam",
""
]
] | Scattering transform is a well known powerful tool for quantisation of field theories in (1+1) dimensions. Conventionally only those models whose classical counterparts admit a Lax pair (origin of which is always mysterious) have been quantised in this way. In relativistic quantum field theories we show that the scatte... | 17.825455 | 16.780127 | 18.342194 | 16.390759 | 18.592276 | 16.925674 | 15.573684 | 16.535437 | 16.244644 | 17.945963 | 17.105312 | 14.990476 | 15.608707 | 14.940677 | 15.654642 | 15.339937 | 14.762561 | 15.247449 | 14.963507 | 16.08161 | 16.565449 |
hep-th/0603113 | Arutyunov Gleb E | G. Arutyunov, A. A. Tseytlin | On highest-energy state in the su(1|1) sector of N=4 super Yang-Mills
theory | 23 pages, Latex | JHEP 0605:033,2006 | 10.1088/1126-6708/2006/05/033 | ITP-UU-06-09, SPIN-06-07, Imperial-TP-AT-6-1 | hep-th | null | We consider the highest-energy state in the su(1|1) sector of N=4 super
Yang-Mills theory containing operators of the form tr(Z^{L-M} \psi^M) where Z
is a complex scalar and \psi is a component of gaugino. We show that this state
corresponds to the operator tr(\psi^L) and can be viewed as an analogue of the
antiferro... | [
{
"created": "Tue, 14 Mar 2006 16:51:46 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Arutyunov",
"G.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We consider the highest-energy state in the su(1|1) sector of N=4 super Yang-Mills theory containing operators of the form tr(Z^{L-M} \psi^M) where Z is a complex scalar and \psi is a component of gaugino. We show that this state corresponds to the operator tr(\psi^L) and can be viewed as an analogue of the antiferroma... | 7.179817 | 6.519964 | 8.069315 | 6.364929 | 6.347357 | 6.37141 | 6.366786 | 5.945621 | 6.203855 | 8.476842 | 5.982191 | 6.429554 | 6.708257 | 6.55975 | 6.159823 | 6.143822 | 6.449165 | 6.477541 | 6.610545 | 6.95162 | 6.246469 |
hep-th/9405077 | Victor Gurarie | V. Gurarie | Probability Density, Diagrammatic Technique, and Epsilon Expansion in
the Theory of Wave Turbulence | 26 pages, PUPT-1462 | Nucl.Phys. B441 (1995) 569-594 | 10.1016/0550-3213(95)00108-5 | null | hep-th cond-mat | null | We apply the methods of Field Theory to study the turbulent regimes of
statistical systems. First we show how one can find their probability
densities. For the case of the theory of wave turbulence with four-wave
interaction we calculate them explicitly and study their properties. Using
those densities we show how on... | [
{
"created": "Wed, 11 May 1994 22:25:32 GMT",
"version": "v1"
},
{
"created": "Tue, 31 May 1994 00:31:43 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Gurarie",
"V.",
""
]
] | We apply the methods of Field Theory to study the turbulent regimes of statistical systems. First we show how one can find their probability densities. For the case of the theory of wave turbulence with four-wave interaction we calculate them explicitly and study their properties. Using those densities we show how one ... | 8.794549 | 10.055617 | 9.475825 | 9.175836 | 9.078636 | 10.241433 | 9.54719 | 9.492653 | 9.358335 | 10.112622 | 8.798884 | 8.517243 | 8.844537 | 8.782654 | 8.726942 | 8.690581 | 8.41561 | 8.899813 | 8.651391 | 8.832513 | 8.585894 |
0805.3924 | Dmitri Gal'tsov | Dmitri V. Gal'tsov and Nikolai G. Scherbluk | Generating technique for $U(1)^3 5D$ supergravity | A typo in Sec. VII B corrected, some references added | Phys.Rev.D78:064033,2008 | 10.1103/PhysRevD.78.064033 | DTP-MSU/08-11 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop generating technique for solutions of $U(1)^3 5D$ supergravity via
dimensional reduction to three dimensions. This theory, which recently
attracted attention in connection with black rings, can be viewed as consistent
truncation of the $T^6$ compactification of the eleven-dimensional
supergravity. Its furt... | [
{
"created": "Mon, 26 May 2008 11:15:10 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Jun 2008 10:11:02 GMT",
"version": "v2"
}
] | 2009-02-20 | [
[
"Gal'tsov",
"Dmitri V.",
""
],
[
"Scherbluk",
"Nikolai G.",
""
]
] | We develop generating technique for solutions of $U(1)^3 5D$ supergravity via dimensional reduction to three dimensions. This theory, which recently attracted attention in connection with black rings, can be viewed as consistent truncation of the $T^6$ compactification of the eleven-dimensional supergravity. Its furthe... | 7.271812 | 6.627018 | 7.811556 | 6.816043 | 6.811752 | 6.608578 | 6.909474 | 6.352526 | 6.956025 | 8.637281 | 6.627836 | 7.080367 | 7.172477 | 6.898132 | 7.041373 | 6.943409 | 6.686156 | 7.002618 | 6.960883 | 7.610777 | 6.838542 |
2211.09148 | Mianqi Wang | Andreas Karch and Mianqi Wang | Universal Behavior of Entanglement Entropies in Interface CFTs from
General Holographic Spacetimes | 28 pages | null | 10.1007/JHEP06(2023)145 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In previous work universal behavior was conjectured for the behavior of the
logarithmic terms in the entanglement entropy of intervals in 1+1 dimensional
interface conformal field theories (ICFTs). These putative universal terms were
exhibited both in free field theories as well as a large class of holographic
models... | [
{
"created": "Wed, 16 Nov 2022 19:00:52 GMT",
"version": "v1"
},
{
"created": "Sun, 16 Apr 2023 22:28:31 GMT",
"version": "v2"
}
] | 2023-07-12 | [
[
"Karch",
"Andreas",
""
],
[
"Wang",
"Mianqi",
""
]
] | In previous work universal behavior was conjectured for the behavior of the logarithmic terms in the entanglement entropy of intervals in 1+1 dimensional interface conformal field theories (ICFTs). These putative universal terms were exhibited both in free field theories as well as a large class of holographic models. ... | 10.000424 | 7.723421 | 9.818069 | 8.042165 | 8.037094 | 8.382426 | 8.026086 | 7.880675 | 8.160625 | 9.758797 | 8.170598 | 8.301405 | 9.040694 | 8.153922 | 8.092225 | 8.127743 | 8.142377 | 7.976992 | 8.083654 | 8.845463 | 8.062797 |
hep-th/0108002 | Subrata Bal | Subrata Bal and Hiroyuki Takata (IMSc,india) | Interaction between two Fuzzy Spheres | Latex file, 13 pages | Int.J.Mod.Phys. A17 (2002) 2445-2458 | 10.1142/S0217751X02010728 | IMSC/2001/04/23 | hep-th | null | We have calculated interactions between two fuzzy spheres in 3 dimension. It
depends on the distance r between the spheres and the radii rho_1, rho_2. There
is no force between the spheres when they are far from each other (long
distance case). We have also studied the interaction for r=0 case. We find that
an attrac... | [
{
"created": "Wed, 1 Aug 2001 18:03:40 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Bal",
"Subrata",
"",
"IMSc,india"
],
[
"Takata",
"Hiroyuki",
"",
"IMSc,india"
]
] | We have calculated interactions between two fuzzy spheres in 3 dimension. It depends on the distance r between the spheres and the radii rho_1, rho_2. There is no force between the spheres when they are far from each other (long distance case). We have also studied the interaction for r=0 case. We find that an attracti... | 11.955676 | 11.015052 | 10.27587 | 9.766425 | 9.827934 | 9.551888 | 9.894552 | 9.404258 | 10.228517 | 11.286132 | 9.050433 | 9.760466 | 10.293199 | 9.448236 | 9.735517 | 10.028377 | 9.572546 | 9.796782 | 9.467982 | 10.268427 | 9.682165 |
1905.13058 | Sudip Karan | Sudip Karan, Gourav Banerjee and Binata Panda | Seeley-DeWitt Coefficients in $\mathcal{N}=2$ Einstein-Maxwell
Supergravity Theory and Logarithmic Corrections to $\mathcal{N}=2$ Extremal
Black Hole Entropy | V4: the Kerr-Newman results in eqs. (6.14) and (6.15) are simplified
into a topological form | Journal of High Energy Physics 08(2019)056 | 10.1007/JHEP08(2019)056 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We investigate the heat kernel method for one-loop effective action following
the Seeley-DeWitt expansion technique of heat kernel with Seeley-DeWitt
coefficients. We also review a general approach of computing the Seeley-DeWitt
coefficients in terms of background or geometric invariants. We, then consider
the Einste... | [
{
"created": "Thu, 30 May 2019 14:01:24 GMT",
"version": "v1"
},
{
"created": "Sun, 11 Aug 2019 06:23:12 GMT",
"version": "v2"
},
{
"created": "Thu, 3 Dec 2020 12:43:05 GMT",
"version": "v3"
},
{
"created": "Fri, 8 Mar 2024 12:17:06 GMT",
"version": "v4"
}
] | 2024-03-11 | [
[
"Karan",
"Sudip",
""
],
[
"Banerjee",
"Gourav",
""
],
[
"Panda",
"Binata",
""
]
] | We investigate the heat kernel method for one-loop effective action following the Seeley-DeWitt expansion technique of heat kernel with Seeley-DeWitt coefficients. We also review a general approach of computing the Seeley-DeWitt coefficients in terms of background or geometric invariants. We, then consider the Einstein... | 6.341631 | 5.14514 | 6.260364 | 5.460789 | 6.028218 | 5.58329 | 5.449703 | 5.359202 | 5.298095 | 6.306304 | 5.542907 | 5.868934 | 5.882181 | 5.748801 | 5.422213 | 5.724239 | 5.7328 | 5.64893 | 5.638095 | 5.860873 | 5.712963 |
1302.2903 | Daniel Blaschke | Daniel N. Blaschke, Harald Grosse and Jean-Christophe Wallet | Slavnov-Taylor identities, non-commutative gauge theories and infrared
divergences | 21 pages, 3 figures; v2: minor corrections and references added | JHEP 1306:038,2013 | 10.1007/JHEP06(2013)038 | LA-UR-13-20923 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we clarify some properties of the one-loop IR divergences in
non-Abelian gauge field theories on non-commutative 4-dimensional Moyal space.
Additionally, we derive the tree-level Slavnov-Taylor identities relating the
two, three and four point functions, and verify their consistency with the
divergent on... | [
{
"created": "Tue, 12 Feb 2013 20:37:17 GMT",
"version": "v1"
},
{
"created": "Thu, 30 May 2013 17:49:10 GMT",
"version": "v2"
}
] | 2013-06-17 | [
[
"Blaschke",
"Daniel N.",
""
],
[
"Grosse",
"Harald",
""
],
[
"Wallet",
"Jean-Christophe",
""
]
] | In this work we clarify some properties of the one-loop IR divergences in non-Abelian gauge field theories on non-commutative 4-dimensional Moyal space. Additionally, we derive the tree-level Slavnov-Taylor identities relating the two, three and four point functions, and verify their consistency with the divergent one-... | 9.302842 | 7.816087 | 8.333308 | 7.557838 | 8.168849 | 8.241626 | 7.549433 | 7.627665 | 7.219189 | 9.051562 | 7.785513 | 8.415169 | 8.217706 | 8.274315 | 8.359529 | 8.357927 | 8.060339 | 8.148434 | 8.435013 | 8.182866 | 8.063935 |
hep-th/0412208 | Pavel Yu. Moshin | D.M. Gitman, P.Yu. Moshin, J.L. Tomazelli | On Superfield Covariant Quantization in General Coordinates | 11 pages, no figures | Eur.Phys.J.C44:591-598,2005 | 10.1140/epjc/s2005-02375-9 | null | hep-th | null | We propose a natural extension of the BRST-antiBRST superfield covariant
scheme in general coordinates. Thus, the coordinate dependence of the basic
scalar and tensor fields of the formalism is extended from the base
supermanifold to the complete set of superfield variables.
| [
{
"created": "Fri, 17 Dec 2004 23:42:56 GMT",
"version": "v1"
}
] | 2009-01-07 | [
[
"Gitman",
"D. M.",
""
],
[
"Moshin",
"P. Yu.",
""
],
[
"Tomazelli",
"J. L.",
""
]
] | We propose a natural extension of the BRST-antiBRST superfield covariant scheme in general coordinates. Thus, the coordinate dependence of the basic scalar and tensor fields of the formalism is extended from the base supermanifold to the complete set of superfield variables. | 17.613361 | 15.570149 | 21.956772 | 15.522078 | 15.675658 | 14.865892 | 15.325108 | 14.553485 | 14.582535 | 18.401308 | 16.329159 | 16.437094 | 18.581259 | 15.531323 | 16.458002 | 16.205046 | 16.180992 | 15.264216 | 16.131243 | 17.45586 | 15.253142 |
0806.1844 | Alexander Kamenshchik | A.A. Andrianov, F. Cannata, A.Yu. Kamenshchik, D. Regoli | Two-field cosmological models and large-scale cosmic magnetic fields | 12 pages, 3 figures | JCAP 0810:019,2008 | 10.1088/1475-7516/2008/10/019 | null | hep-th astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider two different toy cosmological models based on two fields (one
normal scalar and one phantom) realizing the same evolution of the Bang-to-Rip
type. One of the fields (pseudoscalar) interacts with the magnetic field
breaking the conformal invariance of the latter. The effects of the
amplification of cosmic... | [
{
"created": "Wed, 11 Jun 2008 15:24:06 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Andrianov",
"A. A.",
""
],
[
"Cannata",
"F.",
""
],
[
"Kamenshchik",
"A. Yu.",
""
],
[
"Regoli",
"D.",
""
]
] | We consider two different toy cosmological models based on two fields (one normal scalar and one phantom) realizing the same evolution of the Bang-to-Rip type. One of the fields (pseudoscalar) interacts with the magnetic field breaking the conformal invariance of the latter. The effects of the amplification of cosmic m... | 12.384358 | 12.494953 | 10.873789 | 11.463628 | 10.447492 | 10.67604 | 11.637781 | 11.641335 | 12.33622 | 12.692626 | 12.068798 | 12.233858 | 11.591674 | 11.19005 | 11.552012 | 11.56652 | 12.687276 | 11.270122 | 11.727212 | 11.8689 | 11.48807 |
1008.0983 | Nicholas Halmagyi | Iosif Bena, Gregory Giecold, Mariana Gra\~na, Nick Halmagyi, Francesco
Orsi | Supersymmetric Consistent Truncations of IIB on T(1,1) | 23 pages, v2 minor corrections | JHEP 1104:021,2011 | 10.1007/JHEP04(2011)021 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study consistent Kaluza-Klein reductions of type IIB supergravity on
T(1,1) down to five-dimensions. We find that the most general reduction
containing singlets under the global SU(2)xSU(2) symmetry of T(1,1) is N=4
gauged supergravity coupled to three vector multiplets with a particular
gauging due to topological... | [
{
"created": "Thu, 5 Aug 2010 14:27:20 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Mar 2011 20:35:54 GMT",
"version": "v2"
}
] | 2011-04-20 | [
[
"Bena",
"Iosif",
""
],
[
"Giecold",
"Gregory",
""
],
[
"Graña",
"Mariana",
""
],
[
"Halmagyi",
"Nick",
""
],
[
"Orsi",
"Francesco",
""
]
] | We study consistent Kaluza-Klein reductions of type IIB supergravity on T(1,1) down to five-dimensions. We find that the most general reduction containing singlets under the global SU(2)xSU(2) symmetry of T(1,1) is N=4 gauged supergravity coupled to three vector multiplets with a particular gauging due to topological a... | 7.768808 | 7.192511 | 9.292043 | 7.087108 | 7.212511 | 7.218143 | 7.130827 | 7.05975 | 7.067392 | 11.097064 | 7.223431 | 7.229843 | 8.254845 | 7.188207 | 7.249486 | 7.102797 | 7.240919 | 7.430859 | 7.299937 | 8.016569 | 7.009899 |
hep-th/9907173 | Paolo Valtancoli | Paolo Valtancoli | Perturbative Analysis of the Two-body Problem in (2+1)-AdS gravity | 19 pages, no figures, LaTeX file | Int.J.Mod.Phys. A16 (2001) 2945-2964 | 10.1142/S0217751X01004232 | DFF 1/7/99 | hep-th | null | We derive a perturbative scheme to treat the interaction between point
sources and AdS-gravity. The interaction problem is equivalent to the search of
a polydromic mapping $X^A= X^A(x^\mu)$, endowed with 0(2,2) monodromies,
between the physical coordinate system and a Minkowskian 4-dimensional
coordinate system, whic... | [
{
"created": "Thu, 22 Jul 1999 09:14:14 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Valtancoli",
"Paolo",
""
]
] | We derive a perturbative scheme to treat the interaction between point sources and AdS-gravity. The interaction problem is equivalent to the search of a polydromic mapping $X^A= X^A(x^\mu)$, endowed with 0(2,2) monodromies, between the physical coordinate system and a Minkowskian 4-dimensional coordinate system, which ... | 12.327364 | 12.915489 | 12.733574 | 11.291284 | 13.638243 | 12.206456 | 12.281535 | 12.521235 | 12.096799 | 13.586386 | 12.20335 | 11.572883 | 11.915624 | 11.901286 | 11.706922 | 11.646055 | 12.466084 | 11.503374 | 12.310024 | 11.851606 | 11.7686 |
1301.1535 | Stephane Dartois | S. Dartois, V. Rivasseau and A. Tanasa | The 1/N expansion of multi-orientable random tensor models | 18 pages, 17 figures | Annales Henri Poincare Volume 15, Issue 5 (2014), Page 965-984 | 10.1007/s00023-013-0262-8 | null | hep-th gr-qc math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Multi-orientable group field theory (GFT) has been introduced in A. Tanasa,
J. Phys. A 45 (2012) 165401, arXiv:1109.0694, as a quantum field theoretical
simplification of GFT, which retains a larger class of tensor graphs than the
colored one. In this paper we define the associated multi-orientable
identically indepe... | [
{
"created": "Tue, 8 Jan 2013 13:55:37 GMT",
"version": "v1"
}
] | 2014-04-24 | [
[
"Dartois",
"S.",
""
],
[
"Rivasseau",
"V.",
""
],
[
"Tanasa",
"A.",
""
]
] | Multi-orientable group field theory (GFT) has been introduced in A. Tanasa, J. Phys. A 45 (2012) 165401, arXiv:1109.0694, as a quantum field theoretical simplification of GFT, which retains a larger class of tensor graphs than the colored one. In this paper we define the associated multi-orientable identically independ... | 7.884434 | 8.840315 | 10.960565 | 9.053683 | 9.724529 | 9.983963 | 8.716451 | 8.666218 | 9.243074 | 12.06801 | 8.708834 | 7.838377 | 8.917061 | 8.383704 | 8.160597 | 8.209839 | 8.316907 | 7.882327 | 8.33741 | 8.818866 | 7.963483 |
1012.2568 | Aleksandr Zheltukhin | A. A. Zheltukhin | Linear space of spinor monomials and realization of the Nambu-Goldstone
fermion in the Volkov-Akulov and Komargodski-Seiberg Lagrangians | 10 pages | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The analytical algorithm previously proposed by the author for matching the
Volkov-Akulov (VA) and Komargodski-Seiberg (KS) actions describing the
Nambu-Goldstone (NG) fermion, is discussed. The essence of the algotithm is
explained, its consistency is proved and the recent results obtained with
computer assistance a... | [
{
"created": "Sun, 12 Dec 2010 18:13:05 GMT",
"version": "v1"
}
] | 2010-12-14 | [
[
"Zheltukhin",
"A. A.",
""
]
] | The analytical algorithm previously proposed by the author for matching the Volkov-Akulov (VA) and Komargodski-Seiberg (KS) actions describing the Nambu-Goldstone (NG) fermion, is discussed. The essence of the algotithm is explained, its consistency is proved and the recent results obtained with computer assistance are... | 12.392179 | 11.06435 | 11.009777 | 9.953345 | 10.590743 | 11.034958 | 11.808607 | 10.810138 | 10.700042 | 13.111978 | 10.513603 | 10.220267 | 10.772394 | 10.407849 | 10.676419 | 10.506296 | 10.610962 | 10.519721 | 10.598289 | 11.099657 | 10.792644 |
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