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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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0505107 | Richard Andrews P | R. P. Andrews (Swansea U.) and N. Dorey (Cambridge U., DAMTP) | Spherical Deconstruction | 16 pages | Phys.Lett. B631 (2005) 74-82 | 10.1016/j.physletb.2005.09.078 | SWAT-05-432 | hep-th | null | We present evidence that N=1* SUSY Yang-Mills provides a deconstruction of a
six-dimensional gauge theory compactified on a two-sphere. The six-dimensional
theory is a twisted compactification of N=(1,1) SUSY Yang-Mills theory of the
type considered by Maldacena and Nunez (MN). In particular, we calculate the
full cl... | [
{
"created": "Thu, 12 May 2005 14:22:40 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Dec 2005 13:14:57 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Andrews",
"R. P.",
"",
"Swansea U."
],
[
"Dorey",
"N.",
"",
"Cambridge U., DAMTP"
]
] | We present evidence that N=1* SUSY Yang-Mills provides a deconstruction of a six-dimensional gauge theory compactified on a two-sphere. The six-dimensional theory is a twisted compactification of N=(1,1) SUSY Yang-Mills theory of the type considered by Maldacena and Nunez (MN). In particular, we calculate the full clas... | 5.485558 | 4.491577 | 6.325944 | 4.65544 | 4.521167 | 4.322691 | 4.775108 | 4.531709 | 4.693919 | 6.540432 | 4.643453 | 4.770497 | 5.416329 | 4.720282 | 4.711607 | 4.680838 | 4.625392 | 4.749587 | 4.774181 | 5.346514 | 4.722466 |
1608.03247 | Li Li | Li Li | Hyperscaling Violating Solutions in Generalised EMD Theory | 15 pages, 1 figure; v2: references added; v3: typos corrected, a
top-down example in section 4 added, to appear in Physics Letters B | null | 10.1016/j.physletb.2017.02.004 | CCTP-2016-12, CCQCN-2016-160 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This short note is devoted to deriving scaling but hyperscaling violating
solutions in a generalised Einstein-Maxwell-Dilaton theory with an arbitrary
number of scalars and vectors. We obtain analytic solutions in some special
case and discuss the physical constraints on the allowed parameter range in
order to have a... | [
{
"created": "Wed, 10 Aug 2016 18:15:49 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Sep 2016 12:43:29 GMT",
"version": "v2"
},
{
"created": "Fri, 17 Feb 2017 13:09:06 GMT",
"version": "v3"
}
] | 2017-02-20 | [
[
"Li",
"Li",
""
]
] | This short note is devoted to deriving scaling but hyperscaling violating solutions in a generalised Einstein-Maxwell-Dilaton theory with an arbitrary number of scalars and vectors. We obtain analytic solutions in some special case and discuss the physical constraints on the allowed parameter range in order to have a w... | 14.096741 | 11.110274 | 12.308524 | 10.183947 | 10.851596 | 11.605842 | 10.395105 | 11.187785 | 10.921848 | 13.281609 | 10.846779 | 11.032346 | 12.561505 | 11.390301 | 11.712983 | 10.898531 | 11.31741 | 10.868099 | 11.275731 | 12.155254 | 11.456144 |
hep-th/0509212 | Cumrun Vafa | Cumrun Vafa | The String Landscape and the Swampland | 9 pages, minor additions and corrections | null | null | HUTP-05/A043 | hep-th | null | Recent developments in string theory suggest that string theory landscape of
vacua is vast. It is natural to ask if this landscape is as vast as allowed by
consistent-looking effective field theories. We use universality ideas from
string theory to suggest that this is not the case, and that the landscape is
surround... | [
{
"created": "Wed, 28 Sep 2005 15:08:39 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Oct 2005 15:22:42 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Vafa",
"Cumrun",
""
]
] | Recent developments in string theory suggest that string theory landscape of vacua is vast. It is natural to ask if this landscape is as vast as allowed by consistent-looking effective field theories. We use universality ideas from string theory to suggest that this is not the case, and that the landscape is surrounded... | 11.954713 | 12.573105 | 13.257229 | 11.429187 | 13.065269 | 11.978521 | 11.380577 | 11.988436 | 12.248951 | 13.660277 | 11.627009 | 11.439629 | 11.832839 | 11.420269 | 11.21938 | 11.114849 | 11.344539 | 11.392487 | 11.484366 | 11.85625 | 11.843084 |
1009.3236 | Carl Bender | Carl M. Bender and R. J. Kalveks | Extending PT symmetry from Heisenberg algebra to E2 algebra | 8 pages, 7 figures | Int.J.Theor.Phys.50:955-962,2011 | 10.1007/s10773-010-0511-2 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The E2 algebra has three elements, J, u, and v, which satisfy the commutation
relations [u,J]=iv, [v,J]=-iu, [u,v]=0. We can construct the Hamiltonian
H=J^2+gu, where g is a real parameter, from these elements. This Hamiltonian is
Hermitian and consequently it has real eigenvalues. However, we can also
construct the ... | [
{
"created": "Thu, 16 Sep 2010 18:17:00 GMT",
"version": "v1"
}
] | 2011-03-17 | [
[
"Bender",
"Carl M.",
""
],
[
"Kalveks",
"R. J.",
""
]
] | The E2 algebra has three elements, J, u, and v, which satisfy the commutation relations [u,J]=iv, [v,J]=-iu, [u,v]=0. We can construct the Hamiltonian H=J^2+gu, where g is a real parameter, from these elements. This Hamiltonian is Hermitian and consequently it has real eigenvalues. However, we can also construct the PT... | 4.203492 | 4.325606 | 4.438997 | 3.993876 | 4.40236 | 4.330794 | 4.356955 | 4.253328 | 4.345218 | 4.350123 | 4.025896 | 3.890577 | 4.083413 | 4.035487 | 4.050689 | 3.962058 | 4.054301 | 3.9284 | 4.030206 | 4.112746 | 3.994614 |
2012.01717 | Keisuke Izumi | Yugo Abe, Takeo Inami and Keisuke Izumi | Perturbative $S$-matrix unitarity ($S^{\dagger}S=1$) in $R_{\mu \nu} ^2$
gravity | 11 pages, 4 figures, accepted version for publication in MPLA | null | 10.1142/S0217732321501054 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that in the quadratic curvature theory of gravity, or simply $R_{\mu
\nu} ^2$ gravity, the tree-level unitariy bound (tree unitarity) is violated in
the UV region but an analog for $S$-matrix unitarity ($SS^{\dagger} = 1$) is
satisfied. This theory is renormalizable, and hence the failure of tree
unitarity is... | [
{
"created": "Thu, 3 Dec 2020 06:02:22 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Dec 2020 04:33:11 GMT",
"version": "v2"
},
{
"created": "Sun, 21 Mar 2021 12:28:24 GMT",
"version": "v3"
},
{
"created": "Wed, 26 May 2021 06:42:35 GMT",
"version": "v4"
}
] | 2021-06-16 | [
[
"Abe",
"Yugo",
""
],
[
"Inami",
"Takeo",
""
],
[
"Izumi",
"Keisuke",
""
]
] | We show that in the quadratic curvature theory of gravity, or simply $R_{\mu \nu} ^2$ gravity, the tree-level unitariy bound (tree unitarity) is violated in the UV region but an analog for $S$-matrix unitarity ($SS^{\dagger} = 1$) is satisfied. This theory is renormalizable, and hence the failure of tree unitarity is a... | 8.028299 | 7.391026 | 7.780916 | 6.725277 | 7.995336 | 6.761507 | 6.644382 | 7.068445 | 6.893904 | 8.262362 | 7.352149 | 7.301002 | 7.864493 | 7.464818 | 7.352989 | 7.429245 | 7.403727 | 7.275863 | 7.374368 | 8.009102 | 7.40884 |
1612.02894 | Itamar Yaakov | Tatsuma Nishioka, Itamar Yaakov | Supersymmetric R\'enyi Entropy and Defect Operators | 45 pages, 1 figure | null | 10.1007/JHEP11(2017)071 | UT-16-35, IPMU16-0191 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe the defect operator interpretation of the supersymmetric Renyi
entropies of superconformal field theories in three, four and five dimensions.
The operators involved are supersymmetric codimension-two defects in an
auxiliary Z_n gauge theory coupled to n copies of the SCFT. We compute the
exact expectation... | [
{
"created": "Fri, 9 Dec 2016 02:45:16 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Sep 2017 06:53:11 GMT",
"version": "v2"
}
] | 2017-12-06 | [
[
"Nishioka",
"Tatsuma",
""
],
[
"Yaakov",
"Itamar",
""
]
] | We describe the defect operator interpretation of the supersymmetric Renyi entropies of superconformal field theories in three, four and five dimensions. The operators involved are supersymmetric codimension-two defects in an auxiliary Z_n gauge theory coupled to n copies of the SCFT. We compute the exact expectation v... | 7.994471 | 7.29629 | 9.753231 | 7.453658 | 7.725349 | 7.749981 | 7.391091 | 7.65048 | 7.177387 | 10.246662 | 6.965432 | 7.20146 | 8.62652 | 7.35476 | 7.372371 | 7.081537 | 7.165033 | 7.330688 | 7.691858 | 8.118942 | 7.203517 |
hep-th/0504100 | Govindarajan Thupil Dr | R. K. Kaul, T. R. Govindarajan, P. Ramadevi | Schwarz Type Topological Quantum Field Theories | 20 pages, Prepared for Encyclopedia of Mathematical Physics,
paragraph added minor corrections and few references added | null | null | null | hep-th | null | Topological quantum field theories can be used to probe topological
properties of low dimensional manifolds. A class of these theories known as
Schwarz type theories, comprise of Chern-Simons theories and BF theories. In
three dimensions both capture the properties of knots and links leading to
invariants characteris... | [
{
"created": "Tue, 12 Apr 2005 10:36:59 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Apr 2005 09:24:46 GMT",
"version": "v2"
},
{
"created": "Mon, 9 May 2005 11:06:41 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Kaul",
"R. K.",
""
],
[
"Govindarajan",
"T. R.",
""
],
[
"Ramadevi",
"P.",
""
]
] | Topological quantum field theories can be used to probe topological properties of low dimensional manifolds. A class of these theories known as Schwarz type theories, comprise of Chern-Simons theories and BF theories. In three dimensions both capture the properties of knots and links leading to invariants characterisin... | 8.981748 | 8.294973 | 9.854931 | 8.778455 | 8.991377 | 9.178939 | 10.121786 | 8.904309 | 8.459802 | 11.186865 | 8.34395 | 8.461586 | 9.41414 | 8.597444 | 8.210666 | 8.332577 | 8.462826 | 8.459824 | 8.607575 | 9.194606 | 8.394889 |
hep-th/9705196 | Subinit Roy | P. Mukherjee (A.B.N. Seal College, West-Bengal, India) | Magnetic Vortices in a Gauged O(3) Sigma Model with Symmetry Breaking
Self-Interaction | 8 pages, Latex | Phys.Rev. D58 (1998) 105025 | 10.1103/PhysRevD.58.105025 | null | hep-th | null | We consider a (2+1) dimensional nonlinear O(3) sigma model with its U(1)
subgroup gauged along with the inclusion of a self-interaction having symmetry
breaking minima.The gauge field dynamics is governed by the Maxwell term.The
model is shown to support topologically stable purely magnetic self-dual
vortices.
| [
{
"created": "Mon, 26 May 1997 15:48:20 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Mukherjee",
"P.",
"",
"A.B.N. Seal College, West-Bengal, India"
]
] | We consider a (2+1) dimensional nonlinear O(3) sigma model with its U(1) subgroup gauged along with the inclusion of a self-interaction having symmetry breaking minima.The gauge field dynamics is governed by the Maxwell term.The model is shown to support topologically stable purely magnetic self-dual vortices. | 11.927314 | 8.407937 | 11.291588 | 8.542896 | 7.903861 | 8.04166 | 7.946607 | 8.385478 | 8.420969 | 12.261316 | 9.172605 | 10.201369 | 11.7622 | 10.269784 | 10.296942 | 10.062416 | 10.448218 | 10.177809 | 10.484204 | 11.271928 | 10.75035 |
hep-th/0103029 | Rafael I. Nepomechie | Rafael I. Nepomechie | The boundary supersymmetric sine-Gordon model revisited | 9 pages, LaTeX; amssymb, no figures; v2: one equation and one
reference added; v3: more references and a "note added" | Phys.Lett.B509:183-188,2001 | 10.1016/S0370-2693(01)00534-2 | UMTG-227 | hep-th | null | We argue that, contrary to previous claims, the supersymmetric sine-Gordon
model with boundary has a two-parameter family of boundary interactions which
preserves both integrability and supersymmetry. We also propose the
corresponding boundary S matrix for the first supermultiplet of breathers.
| [
{
"created": "Mon, 5 Mar 2001 21:55:45 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Mar 2001 15:19:06 GMT",
"version": "v2"
},
{
"created": "Mon, 19 Mar 2001 16:13:12 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Nepomechie",
"Rafael I.",
""
]
] | We argue that, contrary to previous claims, the supersymmetric sine-Gordon model with boundary has a two-parameter family of boundary interactions which preserves both integrability and supersymmetry. We also propose the corresponding boundary S matrix for the first supermultiplet of breathers. | 12.250762 | 7.656202 | 15.292043 | 8.217745 | 7.646253 | 7.267032 | 8.064691 | 7.594658 | 8.446677 | 14.456606 | 8.41559 | 10.228814 | 13.53695 | 10.297625 | 9.789796 | 10.525846 | 9.741523 | 9.797125 | 10.502289 | 11.978273 | 10.584311 |
1903.04244 | Hiromu Shimoji | Tomohiro Inagaki, Yamato Matsuo, Hiromu Shimoji | Four-Fermion Interaction Model on $\mathcal{M}^{D-1} \otimes S^1$ | 22 pages, 13 figures | null | 10.3390/sym11040451 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Four-fermion interaction models are often used as simplified models of
interacting fermion fields with the chiral symmetry. The chiral symmetry is
dynamically broken for a larger four-fermion coupling. It is expected that the
broken symmetry is restored under extreme conditions. In this paper, the finite
size effect ... | [
{
"created": "Mon, 11 Mar 2019 12:33:01 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Apr 2019 07:41:10 GMT",
"version": "v2"
}
] | 2019-04-11 | [
[
"Inagaki",
"Tomohiro",
""
],
[
"Matsuo",
"Yamato",
""
],
[
"Shimoji",
"Hiromu",
""
]
] | Four-fermion interaction models are often used as simplified models of interacting fermion fields with the chiral symmetry. The chiral symmetry is dynamically broken for a larger four-fermion coupling. It is expected that the broken symmetry is restored under extreme conditions. In this paper, the finite size effect on... | 6.547695 | 6.182384 | 6.721586 | 6.057907 | 6.836786 | 6.47457 | 6.698709 | 6.397067 | 6.540225 | 7.176591 | 6.340314 | 6.263025 | 6.509877 | 6.293042 | 5.903477 | 6.177214 | 6.259853 | 6.352886 | 6.259982 | 6.264589 | 6.0234 |
1407.6008 | Christoph Keller | Christoph A. Keller and Alexander Maloney | Poincare Series, 3D Gravity and CFT Spectroscopy | 36 pages, 2 figures | null | 10.1007/JHEP02(2015)080 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Modular invariance strongly constrains the spectrum of states of two
dimensional conformal field theories. By summing over the images of the modular
group, we construct candidate CFT partition functions that are modular
invariant and have positive spectrum. This allows us to efficiently extract the
constraints on the... | [
{
"created": "Tue, 22 Jul 2014 20:00:24 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Keller",
"Christoph A.",
""
],
[
"Maloney",
"Alexander",
""
]
] | Modular invariance strongly constrains the spectrum of states of two dimensional conformal field theories. By summing over the images of the modular group, we construct candidate CFT partition functions that are modular invariant and have positive spectrum. This allows us to efficiently extract the constraints on the C... | 7.118062 | 7.205144 | 8.037787 | 7.005754 | 7.529249 | 7.316819 | 7.029334 | 6.813884 | 6.704988 | 8.360462 | 6.6378 | 6.366344 | 7.269703 | 6.745698 | 6.662276 | 6.702846 | 6.560727 | 6.731191 | 6.489303 | 7.395676 | 6.681165 |
0712.4070 | Mohsen Alishahiha | Mohsen Alishahiha, Farhad Ardalan, Hajar Ebrahim and Subir
Mukhopadhyay | On 5D Small Black Holes | 18 pages, Latex; V2: few comments added; V3: typos corrected | JHEP 0803:074,2008 | 10.1088/1126-6708/2008/03/074 | null | hep-th | null | Using higher order corrections we argue that five dimensional N=2 and N=4
small black holes exhibit supersymmetry enhancement in near horizon geometry
leading to eight and sixteen supercharges, respectively. Using this enhancement
at supergravity level we can identify the global supergroup of the near horizon
geometr... | [
{
"created": "Tue, 25 Dec 2007 13:22:53 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Jan 2008 15:53:13 GMT",
"version": "v2"
},
{
"created": "Mon, 26 May 2008 07:46:48 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Alishahiha",
"Mohsen",
""
],
[
"Ardalan",
"Farhad",
""
],
[
"Ebrahim",
"Hajar",
""
],
[
"Mukhopadhyay",
"Subir",
""
]
] | Using higher order corrections we argue that five dimensional N=2 and N=4 small black holes exhibit supersymmetry enhancement in near horizon geometry leading to eight and sixteen supercharges, respectively. Using this enhancement at supergravity level we can identify the global supergroup of the near horizon geometry.... | 10.87746 | 9.881969 | 13.575978 | 10.016627 | 10.1127 | 9.836637 | 10.389256 | 9.859657 | 11.0392 | 12.940839 | 9.434308 | 10.569531 | 11.842776 | 10.523515 | 10.437296 | 10.212826 | 10.408721 | 9.963778 | 10.425868 | 11.740111 | 9.85469 |
1402.1863 | Jorge L. deLyra | Jorge L. deLyra | Gaussian-Perturbative Calculations with a Homogeneous External Source | 38 pages, including 12 pages of appendices with explicit
calculations, 1 figure. V2: fixed a few typos in equations. V3: improved
introduction and conclusions. V4: further text improvements and fixes of
typos. V5: fixed a garbled equation | null | null | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the equation of the critical curve and calculate the renormalized
masses of the $SO(N)$-symmetric $\lambda\phi^{4}$ model in the presence of a
homogeneous external source. We do this using the Gaussian-Perturbative
approximation on finite lattices and explicitly taking the continuum limit. No
disabling dive... | [
{
"created": "Sat, 8 Feb 2014 16:31:40 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Feb 2014 15:54:23 GMT",
"version": "v2"
},
{
"created": "Sat, 15 Feb 2014 15:55:46 GMT",
"version": "v3"
},
{
"created": "Mon, 1 Sep 2014 16:12:39 GMT",
"version": "v4"
}
] | 2014-09-02 | [
[
"deLyra",
"Jorge L.",
""
]
] | We derive the equation of the critical curve and calculate the renormalized masses of the $SO(N)$-symmetric $\lambda\phi^{4}$ model in the presence of a homogeneous external source. We do this using the Gaussian-Perturbative approximation on finite lattices and explicitly taking the continuum limit. No disabling diverg... | 7.510849 | 7.64649 | 7.546205 | 7.377229 | 7.544454 | 7.847933 | 7.54652 | 7.84247 | 7.507992 | 7.43722 | 7.355618 | 7.422549 | 7.420442 | 7.409335 | 7.529125 | 7.306593 | 7.264549 | 7.314566 | 7.321603 | 7.71084 | 7.27839 |
hep-th/0008102 | Luis Anchordoqui | Luis Anchordoqui, and Kasper Olsen | Comments on Brane World Cosmology | Updates to match journal version | Mod.Phys.Lett.A16:1157-1169,2001 | 10.1142/S0217732301004352 | null | hep-th astro-ph gr-qc hep-ph | null | In this paper we consider some constraints on brane-world cosmologies. In the
first part we analyze different behaviors for the expansion of our universe by
imposing constraints on the speed of sound. In the second part, we study the
nature of matter on the brane world by means of the well-known energy
conditions. We... | [
{
"created": "Fri, 11 Aug 2000 21:36:27 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Aug 2000 20:51:21 GMT",
"version": "v2"
},
{
"created": "Sat, 2 Jun 2001 16:03:57 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Anchordoqui",
"Luis",
""
],
[
"Olsen",
"Kasper",
""
]
] | In this paper we consider some constraints on brane-world cosmologies. In the first part we analyze different behaviors for the expansion of our universe by imposing constraints on the speed of sound. In the second part, we study the nature of matter on the brane world by means of the well-known energy conditions. We f... | 8.930282 | 8.764951 | 7.337434 | 7.891792 | 7.883266 | 8.356025 | 8.226518 | 8.348366 | 8.133286 | 7.927544 | 7.907589 | 8.490006 | 8.170736 | 8.043566 | 8.094563 | 8.381909 | 8.323443 | 8.275914 | 8.28992 | 8.278964 | 8.164741 |
2404.14479 | Alex Radcliffe | Alex Radcliffe | Non-saturation of Bootstrap Bounds by Hyperbolic Orbifolds | 21 pages, 6 figures | null | null | null | hep-th math-ph math.MP math.SP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In recent years the conformal bootstrap has produced surprisingly tight
bounds on many non-perturbative CFTs. It is an open question whether such
bounds are indeed saturated by these CFTs. A toy version of this question
appears in a recent application of the conformal bootstrap to hyperbolic
orbifolds, where one find... | [
{
"created": "Mon, 22 Apr 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-04-24 | [
[
"Radcliffe",
"Alex",
""
]
] | In recent years the conformal bootstrap has produced surprisingly tight bounds on many non-perturbative CFTs. It is an open question whether such bounds are indeed saturated by these CFTs. A toy version of this question appears in a recent application of the conformal bootstrap to hyperbolic orbifolds, where one finds ... | 9.244177 | 9.762733 | 9.820715 | 9.129469 | 10.115412 | 9.927416 | 9.839935 | 9.653284 | 9.360318 | 10.785121 | 9.150683 | 8.618848 | 8.65326 | 8.384704 | 8.938527 | 8.420489 | 8.381018 | 8.559464 | 8.34903 | 9.075856 | 8.440463 |
1501.01727 | Hong Lu | Zhong-Ying Fan, H. Lu | Charged Black Holes in Colored Lifshitz Spacetimes | Latex, 13 pages, minor corrections and references added | null | 10.1016/j.physletb.2015.02.052 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Einstein gravities coupled to a cosmological constant and $SU(2)$
Yang-Mills fields in four and five dimensions. We find that the theories admit
colored Lifshitz solutions with dynamic exponents $z>1$. We study the wave
equations of the $SU(2)$ scalar triplet in the bulk, and find that the vacuum
color mo... | [
{
"created": "Thu, 8 Jan 2015 04:32:20 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Jan 2015 00:27:04 GMT",
"version": "v2"
}
] | 2015-06-23 | [
[
"Fan",
"Zhong-Ying",
""
],
[
"Lu",
"H.",
""
]
] | We consider Einstein gravities coupled to a cosmological constant and $SU(2)$ Yang-Mills fields in four and five dimensions. We find that the theories admit colored Lifshitz solutions with dynamic exponents $z>1$. We study the wave equations of the $SU(2)$ scalar triplet in the bulk, and find that the vacuum color modi... | 7.775392 | 6.1724 | 8.22806 | 6.471043 | 6.989881 | 6.799195 | 6.439265 | 6.459188 | 7.138441 | 8.103412 | 6.573255 | 6.946065 | 7.778939 | 7.169534 | 7.065404 | 7.263816 | 6.98862 | 7.430928 | 6.954657 | 7.58267 | 6.96124 |
1510.08598 | Hironori Mori | Hironori Mori, Takeshi Morita, and Akinori Tanaka | Single-flavor Abelian mirror symmetry on $\mathbb{RP}^{2} \times
\mathbb{S}^{1}$ | 6 pages, contribution to proceedings of IX International Symposium on
Quantum Theory and Symmetries | Phys. Atom. Nucl. 80 (2017) no.3 586-589 | 10.1134/S1063778817030218 | OU-HET 876, RIKEN-STAMP-20 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The supercoonformal index on $\mathbb{RP}^{2} \times \mathbb{S}^{1}$ can be
derived exactly by the localization technique and applied to the direct proof
of Abelian mirror symmetry. We find two sets of parity conditions compatible
with the unorientable property of $\mathbb{RP}^{2}$ and then rigorously show
two kinds ... | [
{
"created": "Thu, 29 Oct 2015 08:29:21 GMT",
"version": "v1"
}
] | 2017-09-18 | [
[
"Mori",
"Hironori",
""
],
[
"Morita",
"Takeshi",
""
],
[
"Tanaka",
"Akinori",
""
]
] | The supercoonformal index on $\mathbb{RP}^{2} \times \mathbb{S}^{1}$ can be derived exactly by the localization technique and applied to the direct proof of Abelian mirror symmetry. We find two sets of parity conditions compatible with the unorientable property of $\mathbb{RP}^{2}$ and then rigorously show two kinds of... | 8.527316 | 7.82628 | 9.022297 | 7.563044 | 7.647903 | 7.264466 | 7.696191 | 7.391692 | 7.243768 | 10.34728 | 7.334434 | 7.617614 | 8.534426 | 7.667661 | 7.5515 | 7.812521 | 7.716902 | 7.558141 | 7.622387 | 8.240234 | 7.804667 |
hep-th/9406081 | null | Reinhard Oehme and Wentao Xu | Asymptotic Limits and Sum Rules for Gauge Field Propagators | Latex, EFI 93-71 | Phys.Lett. B333 (1994) 172-177 | 10.1016/0370-2693(94)91025-1 | null | hep-th | null | For gauge field propagators, the asymptotic behavior is obtained in all
directions of the complex $k^2$-plane, and for general, linear, covariant
gauges. Asymptotically free theories are considered. Except for coefficients,
the functional form of the leading asymptotic terms is gauge-independent.
Exponents are determ... | [
{
"created": "Tue, 14 Jun 1994 13:36:42 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Oehme",
"Reinhard",
""
],
[
"Xu",
"Wentao",
""
]
] | For gauge field propagators, the asymptotic behavior is obtained in all directions of the complex $k^2$-plane, and for general, linear, covariant gauges. Asymptotically free theories are considered. Except for coefficients, the functional form of the leading asymptotic terms is gauge-independent. Exponents are determin... | 11.903049 | 10.049332 | 10.945674 | 9.861936 | 10.505548 | 10.048208 | 10.7542 | 9.55495 | 9.529794 | 10.624569 | 10.6931 | 10.498366 | 10.266807 | 9.981756 | 10.299714 | 10.750534 | 9.900147 | 10.43067 | 10.302661 | 10.31115 | 10.524307 |
hep-th/9308011 | Avinash Dhar | Avinash Dhar | Two-Dimensional Black Hole and Nonperturbative String Theory | 28p, TIFR-TH-93/34 | null | 10.1142/9789814447072_0008 | null | hep-th | null | We discuss the interpertation of the $c=1$ matrix model as two-dimensional
string theory in a dilaton-black hole background. The nonperturbative
formulation of $c=1$ matrix model in terms of an integrable model of
nonrelativistic fermions enables us to study the quantum fate of the classical
black hole singularity. W... | [
{
"created": "Wed, 4 Aug 1993 12:57:23 GMT",
"version": "v1"
}
] | 2016-11-03 | [
[
"Dhar",
"Avinash",
""
]
] | We discuss the interpertation of the $c=1$ matrix model as two-dimensional string theory in a dilaton-black hole background. The nonperturbative formulation of $c=1$ matrix model in terms of an integrable model of nonrelativistic fermions enables us to study the quantum fate of the classical black hole singularity. We ... | 7.785927 | 6.228774 | 7.373233 | 6.712497 | 6.784178 | 7.032402 | 6.560099 | 6.291134 | 6.760516 | 8.433293 | 6.952259 | 6.700586 | 7.633792 | 7.189111 | 7.052377 | 7.016695 | 6.79948 | 7.089915 | 6.904906 | 7.379912 | 6.625658 |
1401.5983 | Lorenzo G. Vitale Mr. | Florent Baume, Boaz Keren-Zur, Riccardo Rattazzi and Lorenzo Vitale | The local Callan-Symanzik equation: structure and applications | v2: Modified discussion of the amplitude; v3: typos fixed | null | 10.1007/JHEP08(2014)152 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The local Callan-Symanzik equation describes the response of a quantum field
theory to local scale transformations in the presence of background sources.
The consistency conditions associated with this anomalous equation imply
non-trivial relations among the $\beta$-function, the anomalous dimensions of
composite ope... | [
{
"created": "Thu, 23 Jan 2014 14:26:38 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Dec 2014 14:53:46 GMT",
"version": "v2"
},
{
"created": "Thu, 29 Oct 2015 16:09:35 GMT",
"version": "v3"
}
] | 2015-10-30 | [
[
"Baume",
"Florent",
""
],
[
"Keren-Zur",
"Boaz",
""
],
[
"Rattazzi",
"Riccardo",
""
],
[
"Vitale",
"Lorenzo",
""
]
] | The local Callan-Symanzik equation describes the response of a quantum field theory to local scale transformations in the presence of background sources. The consistency conditions associated with this anomalous equation imply non-trivial relations among the $\beta$-function, the anomalous dimensions of composite opera... | 9.431416 | 8.314074 | 9.899327 | 8.950926 | 8.950497 | 9.235177 | 9.440617 | 8.475186 | 8.112961 | 9.579169 | 8.998599 | 8.750689 | 8.970121 | 8.754912 | 8.605884 | 8.78753 | 8.533718 | 8.696414 | 8.746259 | 8.784277 | 8.815145 |
hep-th/9604029 | Sayan Kar | J. S. Prakash | Weyl's Character Formula for $SU(3)$ - A Generating Function Approach | RevTex 3.0, 30 pages, no figures | null | null | IP--BBSR--96/30 | hep-th math.QA q-alg | null | Using a generating function for the Wigner's $D$-matrix elements of $SU(3)$
Weyl's character formula for $SU(3)$ is derived using Schwinger's technique.
| [
{
"created": "Fri, 5 Apr 1996 15:43:12 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Prakash",
"J. S.",
""
]
] | Using a generating function for the Wigner's $D$-matrix elements of $SU(3)$ Weyl's character formula for $SU(3)$ is derived using Schwinger's technique. | 13.329815 | 9.92674 | 10.74914 | 9.229364 | 8.074183 | 11.860196 | 9.151964 | 9.153733 | 11.361131 | 18.227383 | 9.348534 | 9.552957 | 11.503448 | 8.9251 | 8.782248 | 9.201963 | 9.13691 | 9.543396 | 9.156065 | 11.969386 | 8.800361 |
hep-th/0210020 | Dr. Valeri Dvoeglazov | Valeri V. Dvoeglazov (Universidad de Zacatecas) | Theory of Antisymmetric Tensor Fields | 19 pp., RevTeX file, no figures, accepted to Turk. Phys. J | Turk.J.Phys.27:35-50,2003 | null | null | hep-th | null | It has long been claimed that the antisymmetric tensor field of the second
rank is pure longitudinal after quantization. In my opinion, such a situation
is quite unacceptable. I repeat the well-known procedure of the derivation of
the set of Proca equations. It is shown that it can be written in various
forms. Furthe... | [
{
"created": "Thu, 3 Oct 2002 01:03:01 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Dvoeglazov",
"Valeri V.",
"",
"Universidad de Zacatecas"
]
] | It has long been claimed that the antisymmetric tensor field of the second rank is pure longitudinal after quantization. In my opinion, such a situation is quite unacceptable. I repeat the well-known procedure of the derivation of the set of Proca equations. It is shown that it can be written in various forms. Furtherm... | 12.015695 | 12.941138 | 13.391823 | 11.870394 | 13.213024 | 12.761329 | 12.587337 | 12.362528 | 12.21298 | 13.582823 | 11.94264 | 12.314419 | 12.232526 | 12.009827 | 12.041933 | 12.610848 | 12.26466 | 12.338496 | 12.085423 | 12.338015 | 12.122087 |
0808.0280 | Alikram Aliev | Alikram N. Aliev and \"Ozg\"ur Delice | Superradiant Instability of Five-Dimensional Rotating Charged AdS Black
Holes | 24 pages, REVTeX; Minor changes, matching published version | Phys.Rev.D79:024013,2009 | 10.1103/PhysRevD.79.024013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the instability of small AdS black holes with two independent
rotation parameters in minimal five-dimensional gauged supergravity to massless
scalar perturbations. We analytically solve the Klein-Gordon equation for
low-frequency perturbations in two regions of the spacetime of these black
holes: namely, in ... | [
{
"created": "Sun, 3 Aug 2008 12:47:58 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Aug 2008 09:35:41 GMT",
"version": "v2"
},
{
"created": "Mon, 16 Feb 2009 18:25:24 GMT",
"version": "v3"
}
] | 2009-03-12 | [
[
"Aliev",
"Alikram N.",
""
],
[
"Delice",
"Özgür",
""
]
] | We study the instability of small AdS black holes with two independent rotation parameters in minimal five-dimensional gauged supergravity to massless scalar perturbations. We analytically solve the Klein-Gordon equation for low-frequency perturbations in two regions of the spacetime of these black holes: namely, in th... | 6.34055 | 6.57902 | 6.923504 | 6.060133 | 6.712632 | 6.411868 | 6.537767 | 6.595639 | 6.429185 | 7.36736 | 6.413578 | 6.472338 | 6.370784 | 6.407099 | 6.445843 | 6.445343 | 6.317614 | 6.25361 | 6.264154 | 6.493859 | 6.272911 |
hep-th/0012042 | Per Berglund | P. Berglund, T. Hubsch and D. Minic | Probing Naked Singularities in Non-supersymmetric String Vacua | 46 pages, Latex, 7 figures; the brane probe analysis (sections 3 and
4) has been revised, references added and typos corrected | JHEP 0102:010,2001 | 10.1088/1126-6708/2001/02/010 | CITUSC/00-061 | hep-th | null | We present a detailed analysis of non-supersymmetric spacetime varying string
vacua which can lead to an exponential hierarchy between the electroweak and
the gravitational scales. In particular, we identify a limit in which these
vacua can be interpreted as supersymmetric vacua of F-theory. Furthermore, we
study the... | [
{
"created": "Tue, 5 Dec 2000 23:40:40 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Dec 2000 22:35:56 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Berglund",
"P.",
""
],
[
"Hubsch",
"T.",
""
],
[
"Minic",
"D.",
""
]
] | We present a detailed analysis of non-supersymmetric spacetime varying string vacua which can lead to an exponential hierarchy between the electroweak and the gravitational scales. In particular, we identify a limit in which these vacua can be interpreted as supersymmetric vacua of F-theory. Furthermore, we study the p... | 8.547902 | 6.570199 | 8.398657 | 6.877085 | 7.026939 | 6.192082 | 6.719443 | 7.038018 | 6.628074 | 8.943896 | 6.998146 | 7.102201 | 7.937605 | 7.201635 | 7.178342 | 7.121916 | 7.124504 | 7.174221 | 7.111915 | 8.238198 | 7.152714 |
1806.07739 | Hyun-Sik Jeong | Hyun-Sik Jeong, Keun-Young Kim, Chao Niu | Linear-$T$ resistivity at high temperature | 21 pages, 6 figures, v2: references added | J. High Energ. Phys. 2018, 191 (2018) | 10.1007/JHEP10(2018)191 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The linear-$T$ resistivity is one of the characteristic and universal
properties of strange metals. There have been many progress in understanding it
from holographic perspective (gauge/gravity duality). In most holographic
models, the linear-$T$ resistivity is explained by the property of the infrared
geometry and v... | [
{
"created": "Wed, 20 Jun 2018 13:59:36 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Jun 2018 11:21:53 GMT",
"version": "v2"
}
] | 2024-07-01 | [
[
"Jeong",
"Hyun-Sik",
""
],
[
"Kim",
"Keun-Young",
""
],
[
"Niu",
"Chao",
""
]
] | The linear-$T$ resistivity is one of the characteristic and universal properties of strange metals. There have been many progress in understanding it from holographic perspective (gauge/gravity duality). In most holographic models, the linear-$T$ resistivity is explained by the property of the infrared geometry and val... | 6.273776 | 5.006036 | 7.202475 | 5.357085 | 5.022276 | 5.248838 | 5.263829 | 5.368925 | 5.161649 | 6.944378 | 5.203982 | 5.760371 | 6.416377 | 5.774951 | 5.716331 | 5.846354 | 5.924878 | 5.655912 | 5.928756 | 6.537652 | 5.865295 |
hep-th/0401141 | Richard Corrado | Richard Corrado, Nick Halmagyi | N=1 Field Theories and Fluxes in IIB String Theory | 37 pages, LaTeX, one figure; Corrected dimension of fixed manifolds.
Clarifications and references added. Main results unchanged | Phys.Rev.D71:046001,2005 | 10.1103/PhysRevD.71.046001 | ILL-(TH)-03-11, USC-04-01 | hep-th | null | Deformation of N=2 quiver gauge theories by adjoint masses leads to fixed
manifolds of N=1 superconformal field theories. We elaborate on the role of the
complex three-form flux in the IIB duals to these fixed point theories,
primarily using field theory techniques. We study the moduli space at a fixed
point and find... | [
{
"created": "Wed, 21 Jan 2004 05:52:19 GMT",
"version": "v1"
},
{
"created": "Sat, 28 Feb 2004 20:47:28 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Corrado",
"Richard",
""
],
[
"Halmagyi",
"Nick",
""
]
] | Deformation of N=2 quiver gauge theories by adjoint masses leads to fixed manifolds of N=1 superconformal field theories. We elaborate on the role of the complex three-form flux in the IIB duals to these fixed point theories, primarily using field theory techniques. We study the moduli space at a fixed point and find t... | 9.09206 | 9.630533 | 9.8597 | 8.472433 | 8.802287 | 9.27033 | 9.280466 | 8.902664 | 8.550031 | 11.54626 | 8.58099 | 8.667034 | 8.86278 | 8.322852 | 8.482327 | 8.803803 | 8.517049 | 8.628556 | 8.720238 | 9.161324 | 8.698071 |
2308.15743 | Wei Fan | Wei Fan | Nontrivial zeros of the Riemann zeta function on the celestial circle | null | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this short letter, we reformulate the Riemann zeta function using the
holographic framework of the celestial conformal field theory. For spacetime
dimension larger than our Minkowski spacetime $M^4$, the Riemann zeta function
is connected with the sum of the conformal primary wavefunctions evaluated over
a chain o... | [
{
"created": "Wed, 30 Aug 2023 03:49:17 GMT",
"version": "v1"
}
] | 2023-08-31 | [
[
"Fan",
"Wei",
""
]
] | In this short letter, we reformulate the Riemann zeta function using the holographic framework of the celestial conformal field theory. For spacetime dimension larger than our Minkowski spacetime $M^4$, the Riemann zeta function is connected with the sum of the conformal primary wavefunctions evaluated over a chain of ... | 11.649818 | 10.498344 | 11.438589 | 9.859429 | 10.516198 | 10.119127 | 9.231226 | 9.435909 | 9.828471 | 12.236259 | 9.992752 | 9.923831 | 10.006909 | 10.058888 | 10.301908 | 10.186087 | 9.950435 | 10.087843 | 9.948359 | 10.5131 | 9.90987 |
0803.3041 | Konstantinos Dimopoulos | Konstantinos Dimopoulos and Mindaugas Karciauskas | Non-minimally coupled vector curvaton | 4 pages, 1 figure, RevTex. Corrected mistakes and typos. Analytic
results unmodified | JHEP0807:119,2008 | 10.1088/1126-6708/2008/07/119 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that a massive Abelian vector boson field can generate the
curvature perturbation in the Universe, when coupled non-minimally to gravity,
through an RA^2 coupling. The vector boson acts as a curvaton field imposing
the curvature perturbation after the end of inflation, without generating a
large-scale ani... | [
{
"created": "Thu, 20 Mar 2008 17:56:58 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Apr 2008 14:30:05 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Dimopoulos",
"Konstantinos",
""
],
[
"Karciauskas",
"Mindaugas",
""
]
] | It is shown that a massive Abelian vector boson field can generate the curvature perturbation in the Universe, when coupled non-minimally to gravity, through an RA^2 coupling. The vector boson acts as a curvaton field imposing the curvature perturbation after the end of inflation, without generating a large-scale aniso... | 10.1901 | 10.519019 | 8.904991 | 9.379941 | 10.488219 | 10.278622 | 11.762823 | 9.725566 | 9.351687 | 9.905207 | 10.021617 | 9.739981 | 9.17544 | 9.31304 | 9.273956 | 9.418605 | 9.511982 | 9.501379 | 9.236655 | 8.990594 | 9.291551 |
1212.5224 | Karol Kampf | Karol Kampf, Jiri Novotny and Jaroslav Trnka | Recursion Relations for Tree-level Amplitudes in the SU(N) Non-linear
Sigma Model | 4 pages, 2 figures | null | 10.1103/PhysRevD.87.081701 | PUPT-2436 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well-known that the standard BCFW construction cannot be used for
on-shell amplitudes in effective field theories due to bad behavior for large
shifts. We show how to solve this problem in the case of the SU(N) non-linear
sigma model, i.e. non-renormalizable model with infinite number of interaction
vertices, u... | [
{
"created": "Thu, 20 Dec 2012 20:24:06 GMT",
"version": "v1"
}
] | 2013-04-10 | [
[
"Kampf",
"Karol",
""
],
[
"Novotny",
"Jiri",
""
],
[
"Trnka",
"Jaroslav",
""
]
] | It is well-known that the standard BCFW construction cannot be used for on-shell amplitudes in effective field theories due to bad behavior for large shifts. We show how to solve this problem in the case of the SU(N) non-linear sigma model, i.e. non-renormalizable model with infinite number of interaction vertices, usi... | 9.522065 | 7.657968 | 9.488892 | 7.866052 | 7.050044 | 7.439051 | 7.951828 | 6.970451 | 7.679533 | 8.717062 | 7.607548 | 7.873872 | 8.241791 | 8.163409 | 8.142123 | 7.799652 | 8.033042 | 8.095138 | 8.127532 | 8.725123 | 8.005756 |
hep-th/0203240 | Alireza Chenaghlou | A. Chenaghlou, H. Fakhri | On the generalized unitary parasupersymmetry algebra of Beckers-Debergh | 17 pages, LaTex2e, A new section added, To appear in IJMPA | Int.J.Mod.Phys.A18:939-956,2003 | 10.1142/S0217751X0301396X | null | hep-th | null | An appropriate generalization of the unitary parasupersymmetry algebra of
Beckers-Debergh to arbitrary order is presented in this paper. A special
representation for realizing of the even arbitrary order unitary
parasupersymmetry algebra of Beckers-Debergh is analyzed by one dimensional
shape invariance solvable mode... | [
{
"created": "Tue, 26 Mar 2002 11:15:37 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Oct 2002 09:49:52 GMT",
"version": "v2"
}
] | 2011-07-28 | [
[
"Chenaghlou",
"A.",
""
],
[
"Fakhri",
"H.",
""
]
] | An appropriate generalization of the unitary parasupersymmetry algebra of Beckers-Debergh to arbitrary order is presented in this paper. A special representation for realizing of the even arbitrary order unitary parasupersymmetry algebra of Beckers-Debergh is analyzed by one dimensional shape invariance solvable models... | 11.778055 | 14.391784 | 15.375293 | 11.849914 | 13.872492 | 14.143371 | 13.817301 | 12.893439 | 11.722214 | 15.695646 | 11.807757 | 11.387677 | 12.018064 | 11.884673 | 11.425599 | 12.33459 | 11.609145 | 11.684901 | 11.751013 | 11.188287 | 11.361066 |
1211.2618 | Fabien Vignes-Tourneret | Dine Ousmane Samary and Fabien Vignes-Tourneret | Just Renormalizable TGFT's on U(1)^d with Gauge Invariance | 33 pages, 22 figures. One added paragraph on the different notions of
connectedness, preciser formulation of the proof of the power counting
theorem, more general statements about traciality of tensor graphs | Communications in Mathematical Physics (2014) | 10.1007/s00220-014-1930-3 | 1432-0916 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the polynomial Abelian or U(1)^d Tensorial Group Field Theories
equipped with a gauge invariance condition in any dimension d. From our
analysis, we prove the just renormalizability at all orders of perturbation of
the phi^4_6 and phi^6_5 random tensor models. We also deduce that the phi^4_5
tensor model is ... | [
{
"created": "Mon, 12 Nov 2012 13:57:17 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Jan 2013 08:51:44 GMT",
"version": "v2"
}
] | 2014-03-11 | [
[
"Samary",
"Dine Ousmane",
""
],
[
"Vignes-Tourneret",
"Fabien",
""
]
] | We study the polynomial Abelian or U(1)^d Tensorial Group Field Theories equipped with a gauge invariance condition in any dimension d. From our analysis, we prove the just renormalizability at all orders of perturbation of the phi^4_6 and phi^6_5 random tensor models. We also deduce that the phi^4_5 tensor model is su... | 12.224732 | 9.272895 | 14.34428 | 9.922439 | 10.741241 | 10.36199 | 10.311703 | 10.503191 | 9.532587 | 15.582104 | 9.993755 | 10.253111 | 11.618912 | 10.554808 | 11.069144 | 10.181276 | 10.107389 | 10.599969 | 10.826627 | 12.294822 | 10.665263 |
hep-th/9606075 | null | Anna Okopi\'nska | The Effective Action for Local Composite Operators $\Phi^2(x)$ and
$\Phi^4(x)$ | 15 pages, plain Latex, 1 compressed and uuencoded Postscript figure | Int.J.Mod.Phys. A12 (1997) 585-606 | 10.1142/S0217751X97000554 | null | hep-th | null | The generating functionals for the local composite operators, $\Phi^2(x)$ and
$\Phi^4(x)$, are used to study excitations in the scalar quantum field theory
with $\lambda \Phi^4$ interaction. The effective action for the composite
operators is obtained as a series in the Planck constant $\hbar$, and the two-
and four-... | [
{
"created": "Thu, 13 Jun 1996 15:09:36 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Okopińska",
"Anna",
""
]
] | The generating functionals for the local composite operators, $\Phi^2(x)$ and $\Phi^4(x)$, are used to study excitations in the scalar quantum field theory with $\lambda \Phi^4$ interaction. The effective action for the composite operators is obtained as a series in the Planck constant $\hbar$, and the two- and four-pa... | 7.73099 | 6.52058 | 7.05212 | 6.4619 | 6.578835 | 6.407913 | 6.607124 | 6.798441 | 6.323296 | 7.251143 | 6.730531 | 6.738486 | 6.862854 | 6.833146 | 6.788308 | 6.779556 | 6.80451 | 6.810781 | 6.754092 | 7.023937 | 6.822122 |
hep-th/9911229 | Nuno Miguel Marques de Sousa | L.R. Huiszoon, A.N. Schellekens, N. Sousa | Open Descendants of Non-Diagonal Invariants | 21 pages, LaTeX | Nucl.Phys. B575 (2000) 401-415 | 10.1016/S0550-3213(00)00090-0 | null | hep-th | null | The open descendants of simple current automorphism invariants are
constructed. We consider the case where the order of the current is two or odd.
We prove that our solutions satisfy the completeness conditions, positivity and
integrality of the open and closed sectors and the Klein bottle constraint
(apart from an i... | [
{
"created": "Mon, 29 Nov 1999 13:29:45 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Huiszoon",
"L. R.",
""
],
[
"Schellekens",
"A. N.",
""
],
[
"Sousa",
"N.",
""
]
] | The open descendants of simple current automorphism invariants are constructed. We consider the case where the order of the current is two or odd. We prove that our solutions satisfy the completeness conditions, positivity and integrality of the open and closed sectors and the Klein bottle constraint (apart from an int... | 27.291773 | 16.604227 | 23.694714 | 18.483852 | 22.041157 | 19.886816 | 18.639584 | 19.821819 | 19.213348 | 28.741888 | 17.310049 | 19.538862 | 23.590939 | 21.141397 | 19.930386 | 20.127937 | 20.954704 | 20.10276 | 20.664389 | 24.726807 | 20.853073 |
2202.13741 | Deyou Chen | Chengye Yu, Deyou Chen, Chuanhong Gao | Bound on Lyapunov exponent in Einstein-Maxwell-Dilaton-Axion black holes | 17 pages | Chinese Physics C 46 (2022) 125106 | 10.1088/1674-1137/ac90af | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | In this paper, we investigate the influence of the angular momentum of a
charged particle around non-extremal and extremal
Einstein-Maxwell-Dilaton-Axion black holes on the Lyapunov exponent. The
angular momentum's ranges and spatial regions where the bound of the exponent
is violated are found for certain values of ... | [
{
"created": "Mon, 28 Feb 2022 13:08:40 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Mar 2022 12:41:31 GMT",
"version": "v2"
},
{
"created": "Sun, 22 May 2022 02:31:15 GMT",
"version": "v3"
},
{
"created": "Sat, 3 Dec 2022 13:37:56 GMT",
"version": "v4"
}
] | 2022-12-06 | [
[
"Yu",
"Chengye",
""
],
[
"Chen",
"Deyou",
""
],
[
"Gao",
"Chuanhong",
""
]
] | In this paper, we investigate the influence of the angular momentum of a charged particle around non-extremal and extremal Einstein-Maxwell-Dilaton-Axion black holes on the Lyapunov exponent. The angular momentum's ranges and spatial regions where the bound of the exponent is violated are found for certain values of th... | 7.298964 | 7.177228 | 6.649591 | 6.170895 | 7.184746 | 7.194214 | 7.231751 | 6.619778 | 6.640021 | 7.163805 | 6.756241 | 6.393118 | 6.679805 | 6.662369 | 6.384044 | 6.632805 | 6.500952 | 6.54609 | 6.839451 | 6.916456 | 6.544412 |
2002.08387 | Henry Lin | Henry W. Lin | Bootstraps to Strings: Solving Random Matrix Models with Positivity | 30 pages, 10 figures, 1 cartoon. See source for Mathematica notebook.
v2: bootstrapped more complicated model, new Appendices. v3: journal version,
v4: minor typos fixed | null | 10.1007/JHEP06(2020)090 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new approach to solving random matrix models directly in the large $N$
limit is developed. First, a set of numerical values for some low-pt
correlation functions is guessed. The large $N$ loop equations are then used to
generate values of higher-pt correlation functions based on this guess. Then
one tests whether t... | [
{
"created": "Wed, 19 Feb 2020 19:02:03 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Apr 2020 19:04:48 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Jun 2020 13:06:47 GMT",
"version": "v3"
},
{
"created": "Thu, 16 Dec 2021 17:03:17 GMT",
"version": "v4"
}
] | 2021-12-17 | [
[
"Lin",
"Henry W.",
""
]
] | A new approach to solving random matrix models directly in the large $N$ limit is developed. First, a set of numerical values for some low-pt correlation functions is guessed. The large $N$ loop equations are then used to generate values of higher-pt correlation functions based on this guess. Then one tests whether the... | 8.493007 | 9.504429 | 9.871858 | 8.288713 | 9.153125 | 9.726691 | 9.129478 | 8.971273 | 8.743323 | 10.53986 | 9.11178 | 8.617705 | 8.883357 | 8.705207 | 8.345335 | 8.65599 | 8.669537 | 8.15128 | 8.607819 | 8.760114 | 8.290757 |
hep-th/9807010 | Mario Rocca | C. G. Bollini, M. C. Rocca | The Wheeler Propagator | 20 pages latex. No figures | Int.J.Theor.Phys. 37 (1998) 2877-2893 | null | null | hep-th | null | We study the half advanced and half retarded Wheeler Green function and its
relation to Feynman propagators. First for massless equation. Then, for
Klein-Gordon equations with arbitrary mass parameters; real, imaginary or
complex. In all cases the Wheeler propagator lacks an on-shell free
propagation. The Wheeler fun... | [
{
"created": "Wed, 1 Jul 1998 20:37:11 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bollini",
"C. G.",
""
],
[
"Rocca",
"M. C.",
""
]
] | We study the half advanced and half retarded Wheeler Green function and its relation to Feynman propagators. First for massless equation. Then, for Klein-Gordon equations with arbitrary mass parameters; real, imaginary or complex. In all cases the Wheeler propagator lacks an on-shell free propagation. The Wheeler funct... | 18.148737 | 10.547335 | 17.904655 | 14.045656 | 10.835063 | 10.349542 | 10.452507 | 12.111012 | 12.457478 | 18.276686 | 13.785751 | 14.556709 | 16.309608 | 15.415474 | 14.493187 | 14.883834 | 14.472876 | 15.121771 | 15.158369 | 15.593956 | 15.302349 |
2302.08363 | Tom\'as Reis | Marcos Marino, Ramon Miravitllas, Tomas Reis | On the structure of trans-series in quantum field theory | 31 pages, 7 figures | null | null | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many observables in quantum field theory can be expressed in terms of
trans-series, in which one adds to the perturbative series a typically infinite
sum of exponentially small corrections, due to instantons or to renormalons.
Even after Borel resummation of the series in the coupling constant, one has to
sum this in... | [
{
"created": "Thu, 16 Feb 2023 15:29:15 GMT",
"version": "v1"
}
] | 2023-02-17 | [
[
"Marino",
"Marcos",
""
],
[
"Miravitllas",
"Ramon",
""
],
[
"Reis",
"Tomas",
""
]
] | Many observables in quantum field theory can be expressed in terms of trans-series, in which one adds to the perturbative series a typically infinite sum of exponentially small corrections, due to instantons or to renormalons. Even after Borel resummation of the series in the coupling constant, one has to sum this infi... | 6.737304 | 6.495793 | 6.503321 | 6.048322 | 6.582576 | 6.741812 | 6.793402 | 6.665473 | 6.151648 | 7.051766 | 6.19289 | 6.248929 | 6.35083 | 6.156549 | 6.285563 | 6.487109 | 6.461524 | 6.263954 | 6.075927 | 6.414254 | 6.164197 |
hep-th/9412047 | Svozil Karl | K. Svozil | Quantum computation and complexity theory | 51 pages, PostScript | null | null | null | hep-th quant-ph | null | The Hilbert space formalism of quantum mechanics is reviewed with emphasis on
applications to quantum computing. Standard interferomeric techniques are used
to construct a physical device capable of universal quantum computation. Some
consequences for recursion theory and complexity theory are discussed.
| [
{
"created": "Tue, 6 Dec 1994 10:30:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Svozil",
"K.",
""
]
] | The Hilbert space formalism of quantum mechanics is reviewed with emphasis on applications to quantum computing. Standard interferomeric techniques are used to construct a physical device capable of universal quantum computation. Some consequences for recursion theory and complexity theory are discussed. | 15.650134 | 16.823469 | 15.846365 | 14.402755 | 15.558769 | 13.140852 | 17.115393 | 12.844507 | 15.422323 | 16.672947 | 14.316401 | 14.543945 | 15.115607 | 13.580439 | 14.033526 | 14.168616 | 13.797174 | 14.848175 | 14.145583 | 15.511648 | 13.934257 |
2110.11663 | Tiyasa Kar | Tiyasa Kar | Emission Distribution for the quantas of Maxwell-Chern-Simon Gauge Field
coupled to External Current | null | null | 10.1142/S0217751X2250021X | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this paper, we have investigated the nature of emission distribution of
the Maxwell Chern Simon (MCS) Theory in the 2+1 dimension. The distribution of
the topologically massive quanta seems to be Poissonian in nature just like the
Maxwell field theory in 3+1 dimension but with a condition, without which the
distri... | [
{
"created": "Fri, 22 Oct 2021 08:41:16 GMT",
"version": "v1"
}
] | 2022-03-14 | [
[
"Kar",
"Tiyasa",
""
]
] | In this paper, we have investigated the nature of emission distribution of the Maxwell Chern Simon (MCS) Theory in the 2+1 dimension. The distribution of the topologically massive quanta seems to be Poissonian in nature just like the Maxwell field theory in 3+1 dimension but with a condition, without which the distribu... | 21.574282 | 15.472135 | 20.445839 | 17.721115 | 19.230406 | 17.82052 | 19.984995 | 18.760633 | 17.605511 | 21.055952 | 18.412657 | 17.063894 | 19.081659 | 17.613525 | 17.100504 | 17.162081 | 17.06185 | 17.086519 | 17.31028 | 18.906685 | 16.971041 |
hep-th/0011079 | In Yong Park | M. Mihailescu, I.Y. Park, and T.A. Tran | D-branes as Solitons of an N=1, D=10 Non-commutative Gauge Theory | 14 pages, no figure, references added, minor changes | Phys.Rev. D64 (2001) 046006 | 10.1103/PhysRevD.64.046006 | null | hep-th | null | We consider a Dp brane within a D9 brane in the presence of a B-field whose
polarization is {\em transverse} to the Dp brane. To be definite, we take a
D3-D9 system. It is observed that the system has the same pattern of
supersymmetry breaking as that of a soliton of the six dimensional
non-commutative gauge theory t... | [
{
"created": "Thu, 9 Nov 2000 23:34:53 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Nov 2000 04:57:21 GMT",
"version": "v2"
},
{
"created": "Wed, 9 May 2001 16:05:06 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Mihailescu",
"M.",
""
],
[
"Park",
"I. Y.",
""
],
[
"Tran",
"T. A.",
""
]
] | We consider a Dp brane within a D9 brane in the presence of a B-field whose polarization is {\em transverse} to the Dp brane. To be definite, we take a D3-D9 system. It is observed that the system has the same pattern of supersymmetry breaking as that of a soliton of the six dimensional non-commutative gauge theory tha... | 7.484721 | 7.133451 | 8.662355 | 6.865607 | 7.13935 | 6.901966 | 6.957911 | 6.59521 | 6.615105 | 8.100901 | 6.822491 | 6.76606 | 7.38171 | 6.808696 | 6.935092 | 6.592234 | 6.739459 | 6.719896 | 6.583309 | 7.06389 | 6.885657 |
hep-th/9507085 | Paul Montague | P.S. Montague | On the Uniqueness of the Twisted Representation in the Z_2 Orbifold
Construction of a Conformal Field Theory from a Lattice | 27 pages LaTeX. Typos corrected -- no major changes | Nucl.Phys. B455 (1995) 461-490 | 10.1016/0550-3213(95)00486-C | ADP-95/M35 | hep-th | null | Following on from recent work describing the representation content of a
meromorphic bosonic conformal field theory in terms of a certain state inside
the theory corresponding to a fixed state in the representation, and using work
of Zhu on a correspondence between the representations of the conformal field
theory an... | [
{
"created": "Mon, 17 Jul 1995 06:22:57 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jul 1995 08:19:16 GMT",
"version": "v2"
},
{
"created": "Tue, 31 Oct 1995 17:43:30 GMT",
"version": "v3"
}
] | 2015-06-26 | [
[
"Montague",
"P. S.",
""
]
] | Following on from recent work describing the representation content of a meromorphic bosonic conformal field theory in terms of a certain state inside the theory corresponding to a fixed state in the representation, and using work of Zhu on a correspondence between the representations of the conformal field theory and ... | 16.024464 | 14.433142 | 16.291803 | 13.289787 | 13.544488 | 15.033997 | 15.094302 | 13.935296 | 13.0697 | 16.441208 | 13.150078 | 14.447612 | 14.897915 | 13.807995 | 14.259706 | 13.5658 | 13.893738 | 13.73587 | 13.848619 | 14.800189 | 13.49011 |
0801.0149 | Ashoke Sen | Shamik Banerjee and Ashoke Sen | S-duality Action on Discrete T-duality Invariants | LaTeX file, 10 pages | JHEP 0804:012,2008 | 10.1088/1126-6708/2008/04/012 | null | hep-th | null | In heterotic string theory compactified on T^6, the T-duality orbits of dyons
of charge (Q,P) are characterized by O(6,22;R) invariants Q^2, P^2 and Q.P
together with a set of invariants of the discrete T-duality group O(6,22;Z). We
study the action of S-duality group on the discrete T-duality invariants and
study it... | [
{
"created": "Sun, 30 Dec 2007 17:48:19 GMT",
"version": "v1"
}
] | 2009-09-15 | [
[
"Banerjee",
"Shamik",
""
],
[
"Sen",
"Ashoke",
""
]
] | In heterotic string theory compactified on T^6, the T-duality orbits of dyons of charge (Q,P) are characterized by O(6,22;R) invariants Q^2, P^2 and Q.P together with a set of invariants of the discrete T-duality group O(6,22;Z). We study the action of S-duality group on the discrete T-duality invariants and study its ... | 6.164972 | 6.119039 | 6.851958 | 5.478077 | 5.955173 | 6.174703 | 6.106235 | 5.55636 | 5.980727 | 6.800331 | 5.666376 | 5.931092 | 6.302752 | 5.825527 | 5.706635 | 5.786294 | 5.799103 | 5.79258 | 5.821164 | 6.422606 | 5.973709 |
hep-th/0406066 | Andreas Fring | Olalla Castro-Alvaredo and Andreas Fring | Chaos in the thermodynamic Bethe ansatz | 10 pages, Latex | Phys.Lett. A334 (2005) 173 | 10.1016/j.physleta.2004.11.009 | City CMS 0304/LPENSL-TH-04 | hep-th | null | We investigate the discretized version of the thermodynamic Bethe ansatz
equation for a variety of 1+1 dimensional quantum field theories. By computing
Lyapunov exponents we establish that many systems of this type exhibit chaotic
behaviour, in the sense that their orbits through fixed points are extremely
sensitive ... | [
{
"created": "Mon, 7 Jun 2004 18:34:30 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Castro-Alvaredo",
"Olalla",
""
],
[
"Fring",
"Andreas",
""
]
] | We investigate the discretized version of the thermodynamic Bethe ansatz equation for a variety of 1+1 dimensional quantum field theories. By computing Lyapunov exponents we establish that many systems of this type exhibit chaotic behaviour, in the sense that their orbits through fixed points are extremely sensitive wi... | 11.249288 | 12.168345 | 10.062057 | 10.529412 | 10.927144 | 11.699291 | 10.193681 | 10.013074 | 10.522521 | 11.187625 | 9.997005 | 9.829419 | 10.522586 | 9.646357 | 9.749706 | 10.301256 | 9.597581 | 10.596087 | 10.16545 | 10.203164 | 10.265221 |
1112.6346 | Bayram Tekin | Metin Gurses, Tahsin Cagri Sisman, Bayram Tekin | Some exact solutions of all f(Ricci) theories in three dimensions | 25 pages, references added, presentation improved, version to appear
in Phys. Rev. D | Phys. Rev. D 86, 024001 (2012) | 10.1103/PhysRevD.86.024001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find constant scalar curvature Type-N and Type-D solutions in all higher
curvature gravity theories with actions of the form f(Ricci) that are built on
the Ricci tensor, but not on its derivatives. In our construction, these higher
derivative theories inherit some of the previously studied solutions of the
cosmolo... | [
{
"created": "Thu, 29 Dec 2011 16:50:49 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Jan 2012 15:18:36 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Jun 2012 11:38:16 GMT",
"version": "v3"
}
] | 2012-07-17 | [
[
"Gurses",
"Metin",
""
],
[
"Sisman",
"Tahsin Cagri",
""
],
[
"Tekin",
"Bayram",
""
]
] | We find constant scalar curvature Type-N and Type-D solutions in all higher curvature gravity theories with actions of the form f(Ricci) that are built on the Ricci tensor, but not on its derivatives. In our construction, these higher derivative theories inherit some of the previously studied solutions of the cosmologi... | 13.193371 | 11.238624 | 11.643831 | 10.540034 | 10.263347 | 10.107727 | 12.097307 | 9.741267 | 10.505426 | 11.597656 | 9.659514 | 10.837716 | 11.758342 | 11.080522 | 11.866235 | 10.961025 | 10.772268 | 10.990271 | 10.471244 | 12.233426 | 10.699687 |
1312.2261 | Daniel O'Keeffe | Daniel K. O'Keeffe and Amanda W. Peet | Electric hyperscaling violating solutions in Einstein-Maxwell-dilaton
gravity with R^2 corrections | 38 pages, 16 figures; v2: References added and typos corrected | Phys. Rev. D 90, 026004 (2014) | 10.1103/PhysRevD.90.026004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of holography applied to condensed matter physics, we study
Einstein-Maxwell-dilaton theory with curvature squared corrections. This theory
has three couplings eta_i for the three R^2 invariants and two theory
functions: a dilaton potential V(phi) and a dilaton-dependent gauge coupling
f(phi). We find ... | [
{
"created": "Sun, 8 Dec 2013 20:56:09 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Dec 2013 19:16:35 GMT",
"version": "v2"
}
] | 2014-07-23 | [
[
"O'Keeffe",
"Daniel K.",
""
],
[
"Peet",
"Amanda W.",
""
]
] | In the context of holography applied to condensed matter physics, we study Einstein-Maxwell-dilaton theory with curvature squared corrections. This theory has three couplings eta_i for the three R^2 invariants and two theory functions: a dilaton potential V(phi) and a dilaton-dependent gauge coupling f(phi). We find hy... | 10.999035 | 13.056189 | 12.322007 | 10.189429 | 11.555121 | 12.165714 | 11.776132 | 10.952036 | 11.652315 | 14.022149 | 10.415753 | 10.767721 | 10.960775 | 10.291077 | 10.782996 | 10.65341 | 10.9675 | 10.758714 | 10.841555 | 11.00111 | 10.621965 |
2104.02051 | Sameer Murthy | Arash Arabi Ardehali and Sameer Murthy | The 4d superconformal index near roots of unity and 3d Chern-Simons
theory | v3: minor corrections and clarifications added | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We consider the $S^3\times S^1$ superconformal index $\mathcal{I}(\tau)$ of
4d $\mathcal{N}=1$ gauge theories. The Hamiltonian index is defined in a
standard manner as the Witten index with a chemical potential $\tau$ coupled to
a combination of angular momenta on $S^3$ and the $U(1)$ R-charge. We develop
the all-ord... | [
{
"created": "Mon, 5 Apr 2021 17:59:12 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Apr 2021 16:31:07 GMT",
"version": "v2"
},
{
"created": "Wed, 14 Jul 2021 10:32:43 GMT",
"version": "v3"
}
] | 2021-07-15 | [
[
"Ardehali",
"Arash Arabi",
""
],
[
"Murthy",
"Sameer",
""
]
] | We consider the $S^3\times S^1$ superconformal index $\mathcal{I}(\tau)$ of 4d $\mathcal{N}=1$ gauge theories. The Hamiltonian index is defined in a standard manner as the Witten index with a chemical potential $\tau$ coupled to a combination of angular momenta on $S^3$ and the $U(1)$ R-charge. We develop the all-order... | 4.598102 | 4.862883 | 5.171271 | 4.560603 | 4.881603 | 5.013938 | 5.037647 | 4.65872 | 4.509721 | 5.578602 | 4.657591 | 4.643496 | 4.682786 | 4.65906 | 4.662536 | 4.714315 | 4.65941 | 4.603416 | 4.662986 | 4.724146 | 4.538648 |
1701.07445 | Ping Gao | Ping Gao and Hong Liu | Emergent Supersymmetry in Local Equilibrium Systems | 45 pages | null | 10.1007/JHEP01(2018)040 | MIT-CTP/4861 | hep-th cond-mat.stat-mech hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many physical processes we observe in nature involve variations of
macroscopic quantities over spatial and temporal scales much larger than
microscopic molecular collision scales and can be considered as in local
thermal equilibrium. In this paper we show that any classical statistical
system in local thermal equilib... | [
{
"created": "Wed, 25 Jan 2017 19:01:12 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Sep 2017 15:50:19 GMT",
"version": "v2"
}
] | 2018-02-14 | [
[
"Gao",
"Ping",
""
],
[
"Liu",
"Hong",
""
]
] | Many physical processes we observe in nature involve variations of macroscopic quantities over spatial and temporal scales much larger than microscopic molecular collision scales and can be considered as in local thermal equilibrium. In this paper we show that any classical statistical system in local thermal equilibri... | 8.975408 | 9.301028 | 9.857574 | 8.831862 | 9.313678 | 9.944493 | 8.965569 | 9.433826 | 8.961528 | 11.415614 | 8.601136 | 9.244624 | 9.085659 | 8.68962 | 9.022753 | 8.937295 | 9.039509 | 9.142175 | 8.997819 | 8.842381 | 8.838334 |
1505.01937 | Andrew Matas | Andrew Matas, Daniel M\"uller, and Glenn Starkman | Point particle motion in topologically nontrivial space-times | 24 pages, 3 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is well known that compactifying a space can break symmetries that are
present in the covering space. In this paper we study the effects of such
topological symmetry breaking on point-particle motion when the particle is
coupled to a massless field on the space. For a torus topology where Lorentz
invariance is bro... | [
{
"created": "Fri, 8 May 2015 06:24:01 GMT",
"version": "v1"
}
] | 2015-05-11 | [
[
"Matas",
"Andrew",
""
],
[
"Müller",
"Daniel",
""
],
[
"Starkman",
"Glenn",
""
]
] | It is well known that compactifying a space can break symmetries that are present in the covering space. In this paper we study the effects of such topological symmetry breaking on point-particle motion when the particle is coupled to a massless field on the space. For a torus topology where Lorentz invariance is broke... | 9.245774 | 10.499435 | 9.339279 | 9.548166 | 10.034396 | 10.436512 | 9.562254 | 9.94162 | 9.778596 | 10.296679 | 9.630937 | 8.921151 | 9.041869 | 9.072435 | 8.915027 | 9.233255 | 9.207062 | 8.889584 | 8.921111 | 9.052045 | 8.894295 |
hep-th/9510212 | Nissan Itzhaki | N. Itzhaki | Black Hole Information vs. Locality | 19 pages, final version to appear in Phys. Rev. D | Phys. Rev. D 54, 1557 (1996) | 10.1103/PhysRevD.54.1557 | TAUP-2298-95 | hep-th gr-qc | null | We discuss the limitations on space time measurement in the Schwarzchild
metric. We find that near the horizon the limitations on space time measurement
are of the order of the black hole radius. We suggest that it indicates that a
large mass black hole cannot be described by means of local field theory even
at macro... | [
{
"created": "Mon, 30 Oct 1995 08:55:36 GMT",
"version": "v1"
},
{
"created": "Thu, 9 May 1996 08:05:49 GMT",
"version": "v2"
}
] | 2016-08-24 | [
[
"Itzhaki",
"N.",
""
]
] | We discuss the limitations on space time measurement in the Schwarzchild metric. We find that near the horizon the limitations on space time measurement are of the order of the black hole radius. We suggest that it indicates that a large mass black hole cannot be described by means of local field theory even at macrosc... | 8.833014 | 7.756009 | 8.215745 | 8.1643 | 8.580127 | 7.947968 | 7.700157 | 8.008718 | 8.165389 | 9.069959 | 7.612625 | 8.336418 | 8.183172 | 8.224772 | 8.203124 | 8.383799 | 8.212006 | 8.145573 | 8.226698 | 8.43062 | 8.098955 |
hep-th/9206073 | Ted Allen | Theodore J. Allen and Andrew J. Bordner | Charged Vortex Dynamics in Ginzburg-Landau Theory of the Fractional
Quantum Hall Effect | 28 pages + 1 Figure, new phyzzx macro (included), MAD/TH-92-02 | Int.J.Mod.Phys. A10 (1995) 645-666 | 10.1142/S0217751X95000292 | null | hep-th cond-mat | null | We write a Ginzburg-Landau Hamiltonian for a charged order parameter
interacting with a background electromagnetic field in 2+1 dimensions. Using
the method of Lund we derive a collective coordinate action for vortex defects
in the order parameter and demonstrate that the vortices are charged. We
examine the classica... | [
{
"created": "Thu, 18 Jun 1992 18:39:00 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Allen",
"Theodore J.",
""
],
[
"Bordner",
"Andrew J.",
""
]
] | We write a Ginzburg-Landau Hamiltonian for a charged order parameter interacting with a background electromagnetic field in 2+1 dimensions. Using the method of Lund we derive a collective coordinate action for vortex defects in the order parameter and demonstrate that the vortices are charged. We examine the classical ... | 11.8401 | 11.194245 | 11.547658 | 10.269084 | 11.061449 | 10.852452 | 10.497169 | 10.809292 | 10.780614 | 11.625055 | 10.273386 | 10.584846 | 11.398176 | 10.585297 | 11.230172 | 10.877976 | 10.854069 | 10.592312 | 10.762501 | 11.016927 | 10.604736 |
hep-th/9604144 | Markus Pflaum | Markus J. Pflaum | A new concept of deformation quantization, I. Normal order quantization
on cotangent bundles | postscript-file, 70 pages, also available at
ftp://ftp.math.tu-berlin.de/pub/Preprints/sfb288/abstract186.html | null | null | null | hep-th math-ph math.MP | null | In this work we give a deformation theoretical approach to the problem of
quantization. First the notion of a deformation of a noncommutative ringed
space over a commutative locally ringed space is introduced within a language
coming from Algebraic Geometry and Complex Analysis. Then we define what a
Dirac quantizati... | [
{
"created": "Tue, 23 Apr 1996 12:50:30 GMT",
"version": "v1"
}
] | 2013-08-08 | [
[
"Pflaum",
"Markus J.",
""
]
] | In this work we give a deformation theoretical approach to the problem of quantization. First the notion of a deformation of a noncommutative ringed space over a commutative locally ringed space is introduced within a language coming from Algebraic Geometry and Complex Analysis. Then we define what a Dirac quantization... | 7.546191 | 7.876065 | 8.166615 | 8.13033 | 9.191965 | 8.700242 | 8.367659 | 8.331929 | 8.032384 | 8.454438 | 7.672127 | 7.187663 | 7.473773 | 7.440803 | 7.374479 | 7.356365 | 7.679292 | 7.220517 | 7.414466 | 7.672491 | 7.089308 |
hep-th/0406134 | Thomas Hertog | Thomas Hertog, Gary T. Horowitz | Towards a Big Crunch Dual | 27 pages, 3 figures;v2:minor corrections | JHEP0407:073,2004 | 10.1088/1126-6708/2004/07/073 | null | hep-th gr-qc | null | We show there exist smooth asymptotically anti-de Sitter initial data which
evolve to a big crunch singularity in a low energy supergravity limit of string
theory. This opens up the possibility of using the dual conformal field theory
to obtain a fully quantum description of the cosmological singularity. A
preliminar... | [
{
"created": "Tue, 15 Jun 2004 17:57:52 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Jul 2004 23:15:49 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Hertog",
"Thomas",
""
],
[
"Horowitz",
"Gary T.",
""
]
] | We show there exist smooth asymptotically anti-de Sitter initial data which evolve to a big crunch singularity in a low energy supergravity limit of string theory. This opens up the possibility of using the dual conformal field theory to obtain a fully quantum description of the cosmological singularity. A preliminary ... | 9.543498 | 8.947391 | 8.849296 | 8.338624 | 8.190225 | 8.806681 | 8.882906 | 8.842229 | 8.029941 | 10.562604 | 8.657635 | 8.76253 | 9.44448 | 8.715407 | 8.471882 | 8.644075 | 8.743899 | 8.404753 | 8.463508 | 9.517043 | 8.739068 |
0810.0227 | Shang-Yu Wu | Feng-Li Lin, Shang-Yu Wu | Non-relativistic Holography and Singular Black Hole | 19 pages, 1 figure, v3. minor revisions, refs. added v4. minor
revisions | Phys.Lett.B679:65-72,2009 | 10.1016/j.physletb.2009.07.002 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a framework for non-relativistic holography so that a covariant
action principle ensuring the Galilean symmetry for dual conformal field theory
is given. This framework is based on the Bargmann lift of the Newton-Cartan
gravity to the one-dimensional higher Einstein gravity, or reversely, the
null-like Kal... | [
{
"created": "Wed, 1 Oct 2008 17:58:05 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Oct 2008 14:53:11 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Dec 2008 07:57:04 GMT",
"version": "v3"
},
{
"created": "Mon, 6 Jul 2009 17:09:47 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Lin",
"Feng-Li",
""
],
[
"Wu",
"Shang-Yu",
""
]
] | We provide a framework for non-relativistic holography so that a covariant action principle ensuring the Galilean symmetry for dual conformal field theory is given. This framework is based on the Bargmann lift of the Newton-Cartan gravity to the one-dimensional higher Einstein gravity, or reversely, the null-like Kaluz... | 10.402848 | 11.490068 | 11.873103 | 10.736357 | 11.306186 | 10.702669 | 10.467251 | 10.184788 | 10.605801 | 13.073885 | 10.076055 | 10.347345 | 11.063641 | 10.560436 | 10.543007 | 10.538381 | 10.296945 | 10.441031 | 10.094832 | 11.256124 | 10.002101 |
2201.11402 | Gustavo Brito | Gustavo P. de Brito, Astrid Eichhorn | Nonvanishing gravitational contribution to matter beta functions for
vanishing dimensionful regulators | 23 pages + Appendix, 10 figures | null | 10.1140/epjc/s10052-023-11172-z | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore the effect of quantum gravity on matter within a Renormalization
Group framework. First, our results provide an explicit example of how
misleading conclusions can be drawn by analyzing the gravitational
contributions to beta functions, instead of analyzing universal quantities,
such as critical exponents, ... | [
{
"created": "Thu, 27 Jan 2022 09:34:41 GMT",
"version": "v1"
}
] | 2023-03-22 | [
[
"de Brito",
"Gustavo P.",
""
],
[
"Eichhorn",
"Astrid",
""
]
] | We explore the effect of quantum gravity on matter within a Renormalization Group framework. First, our results provide an explicit example of how misleading conclusions can be drawn by analyzing the gravitational contributions to beta functions, instead of analyzing universal quantities, such as critical exponents, th... | 14.699294 | 14.851637 | 14.831192 | 13.530307 | 14.930137 | 14.634563 | 14.16539 | 15.032598 | 14.188093 | 15.538891 | 13.381208 | 14.258561 | 14.744045 | 14.283502 | 14.610358 | 14.086733 | 14.603784 | 13.966809 | 14.043699 | 14.547698 | 14.044665 |
2209.09248 | Mario Martone | Philip C. Argyres and Mario Martone | The rank 2 classification problem I: scale invariant geometries | Tables and references updated | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this first of a series of three papers we outline an approach to
classifying 4d $\mathcal{N}{=}2$ superconformal field theories at rank 2. The
classification of allowed scale invariant $\mathcal{N}=2$ Coulomb branch
geometries of dimension (or rank) greater than one is a famous open problem
whose solution will gre... | [
{
"created": "Mon, 19 Sep 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Sep 2022 07:25:29 GMT",
"version": "v2"
}
] | 2022-09-28 | [
[
"Argyres",
"Philip C.",
""
],
[
"Martone",
"Mario",
""
]
] | In this first of a series of three papers we outline an approach to classifying 4d $\mathcal{N}{=}2$ superconformal field theories at rank 2. The classification of allowed scale invariant $\mathcal{N}=2$ Coulomb branch geometries of dimension (or rank) greater than one is a famous open problem whose solution will great... | 8.888806 | 8.443689 | 9.484878 | 7.76544 | 8.437191 | 8.40547 | 8.559141 | 8.250648 | 7.752953 | 10.212844 | 7.935657 | 8.237072 | 8.229387 | 8.002567 | 8.271829 | 8.136057 | 8.006286 | 7.954878 | 8.06729 | 8.400846 | 8.006272 |
hep-th/9506176 | M. Yoshimura | M.Yoshimura | Catastrophic Particle Production under Periodic Perturbation | 33 pages | Prog.Theor.Phys. 94 (1995) 873-898 | 10.1143/PTP.94.873 | TU/95/484 | hep-th gr-qc hep-ph | null | We develop a formalism to investigate the behavior of quantum field and
quantum ground state when the field is coupled to perturbation that
periodically oscillates. Working in the Schroedinger picture of quantum field
theory, we confirm that the phenomenon of parametric resonance in the classical
theory implies an in... | [
{
"created": "Tue, 27 Jun 1995 05:27:01 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Yoshimura",
"M.",
""
]
] | We develop a formalism to investigate the behavior of quantum field and quantum ground state when the field is coupled to perturbation that periodically oscillates. Working in the Schroedinger picture of quantum field theory, we confirm that the phenomenon of parametric resonance in the classical theory implies an inst... | 14.30754 | 17.174969 | 14.886336 | 14.642019 | 15.672022 | 15.797501 | 16.267586 | 15.488506 | 14.553762 | 15.877152 | 15.368088 | 14.770722 | 14.029482 | 14.047452 | 14.371666 | 14.269045 | 14.576362 | 14.4624 | 14.020678 | 14.27723 | 14.539331 |
2011.07071 | Damian Van De Heisteeg | Christopher Couzens, Eric Marcus, Koen Stemerdink, Damian van de
Heisteeg | The Near-Horizon Geometry of Supersymmetric Rotating AdS$_4$ Black Holes
in M-theory | 31 pages plus appendix | null | 10.1007/JHEP05(2021)194 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We classify the necessary and sufficient conditions to obtain the
near-horizon geometry of extremal supersymmetric rotating black holes embedded
in 11d supergravity. Such rotating black holes admit an AdS$_2$ near-horizon
geometry which is fibered by the transverse spacetime directions. Despite their
clear interest t... | [
{
"created": "Fri, 13 Nov 2020 19:00:00 GMT",
"version": "v1"
}
] | 2023-01-11 | [
[
"Couzens",
"Christopher",
""
],
[
"Marcus",
"Eric",
""
],
[
"Stemerdink",
"Koen",
""
],
[
"van de Heisteeg",
"Damian",
""
]
] | We classify the necessary and sufficient conditions to obtain the near-horizon geometry of extremal supersymmetric rotating black holes embedded in 11d supergravity. Such rotating black holes admit an AdS$_2$ near-horizon geometry which is fibered by the transverse spacetime directions. Despite their clear interest to ... | 8.444599 | 8.525188 | 9.747605 | 8.142895 | 8.507967 | 8.131738 | 8.389801 | 7.991045 | 8.374374 | 9.921194 | 8.315446 | 8.190701 | 8.47685 | 8.036366 | 8.145561 | 8.241885 | 8.045984 | 8.201641 | 8.06135 | 8.242048 | 8.036325 |
hep-th/0402175 | Yue-Liang Wu | Yue-Liang Wu (ITP, Cas) | Conformal Scaling Gauge Symmetry and Inflationary Universe | 12 pages, RevTex, no figures | Int.J.Mod.Phys. A20 (2005) 811-820 | 10.1142/S0217751X0502080X | null | hep-th | null | Considering the conformal scaling gauge symmetry as a fundamental symmetry of
nature in the presence of gravity, a scalar field is required and used to
describe the scale behavior of universe. In order for the scalar field to be a
physical field, a gauge field is necessary to be introduced. A gauge invariant
potentia... | [
{
"created": "Mon, 23 Feb 2004 02:15:15 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Wu",
"Yue-Liang",
"",
"ITP, Cas"
]
] | Considering the conformal scaling gauge symmetry as a fundamental symmetry of nature in the presence of gravity, a scalar field is required and used to describe the scale behavior of universe. In order for the scalar field to be a physical field, a gauge field is necessary to be introduced. A gauge invariant potential ... | 11.839523 | 12.223202 | 11.520858 | 10.8788 | 12.878225 | 11.613732 | 12.861576 | 11.286054 | 11.358699 | 12.271292 | 12.155297 | 11.500484 | 11.433425 | 11.273753 | 11.479578 | 11.494869 | 11.498751 | 11.343644 | 11.233786 | 11.356603 | 11.577477 |
2012.09354 | Francisco Tello Ortiz | Alvaro Restuccia and Francisco Tello-Ortiz | Gravitational-gauge vector interaction in the Ho\v{r}ava-Lifshitz
framework | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | An anisotropic model describing gravity--vector gauge coupling at all energy
scales is presented. The starting point is the 4+1 dimensional non--projectable
Ho\v{r}ava--Lifshitz gravity theory subject to a geometrical restriction.
Renormalizability arguments require all possible interactions in the potential
up to te... | [
{
"created": "Thu, 17 Dec 2020 02:01:16 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jan 2023 23:20:26 GMT",
"version": "v2"
}
] | 2023-01-23 | [
[
"Restuccia",
"Alvaro",
""
],
[
"Tello-Ortiz",
"Francisco",
""
]
] | An anisotropic model describing gravity--vector gauge coupling at all energy scales is presented. The starting point is the 4+1 dimensional non--projectable Ho\v{r}ava--Lifshitz gravity theory subject to a geometrical restriction. Renormalizability arguments require all possible interactions in the potential up to term... | 11.302409 | 10.367189 | 12.436698 | 11.320781 | 11.495991 | 11.32793 | 10.905638 | 10.59891 | 10.716576 | 12.916641 | 10.897533 | 10.368138 | 11.301804 | 10.952381 | 10.928998 | 11.021935 | 11.105557 | 10.84042 | 10.677658 | 11.556635 | 10.635036 |
hep-th/0204174 | Mohammad Sheikh-Jabbari | Mohsen Alishahiha, Mohammad M. Sheikh-Jabbari | Strings in PP-Waves and Worldsheet Deconstruction | Latex file, 15 pages, no figures. v2: a reference added | Phys.Lett.B538:180-188,2002 | 10.1016/S0370-2693(02)01994-9 | IPM/P-2002/012, SU-ITP-2/13 | hep-th | null | Based on the observation that $AdS_5\times S^5/Z_k$ orbifolds have a maximal
supersymmetric PP-wave limit, the description of strings in PP-waves in terms
of ${\cal N}=2$ quiver gauge theories is presented. We consider two different,
small and large $k$, cases and show that the operators in the gauge theory
which cor... | [
{
"created": "Sun, 21 Apr 2002 20:46:35 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Apr 2002 23:21:10 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Alishahiha",
"Mohsen",
""
],
[
"Sheikh-Jabbari",
"Mohammad M.",
""
]
] | Based on the observation that $AdS_5\times S^5/Z_k$ orbifolds have a maximal supersymmetric PP-wave limit, the description of strings in PP-waves in terms of ${\cal N}=2$ quiver gauge theories is presented. We consider two different, small and large $k$, cases and show that the operators in the gauge theory which corre... | 8.16964 | 7.141152 | 8.998029 | 6.979742 | 7.185375 | 7.042989 | 7.784276 | 7.233285 | 6.970268 | 8.922323 | 7.155854 | 6.893902 | 8.044533 | 7.049938 | 7.326914 | 7.291393 | 7.104775 | 7.100172 | 6.995533 | 7.808322 | 6.976201 |
hep-th/0311048 | Mikhail Altaisky | M.V.Altaisky | Wavelet based regularization for Euclidean field theory and stochastic
quantization | LaTeX, 12 pages; 2 eps figures; To appear in "Progress in Field
Theory Research" by Nova Science Publishers, Inc | null | null | null | hep-th | null | It is shown that Euclidean field theory with polynomial interaction, can be
regularized using the wavelet representation of the fields. The connections
between wavelet based regularization and stochastic quantization are considered
with $\phi^3$ field theory taken as an example.
| [
{
"created": "Thu, 6 Nov 2003 11:22:29 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Altaisky",
"M. V.",
""
]
] | It is shown that Euclidean field theory with polynomial interaction, can be regularized using the wavelet representation of the fields. The connections between wavelet based regularization and stochastic quantization are considered with $\phi^3$ field theory taken as an example. | 14.802172 | 12.408901 | 12.820127 | 11.817941 | 12.075824 | 10.885534 | 12.103201 | 11.70253 | 11.600942 | 11.798226 | 11.352894 | 11.852719 | 12.75276 | 12.08874 | 11.820289 | 12.224252 | 11.843708 | 11.327482 | 12.119727 | 12.811584 | 11.371521 |
hep-th/9703124 | Mees de Roo | M. de Roo | Intersecting branes and Supersymmetry | 6 pages, Latex, Presented at Supersymmetry and Quantum Field Theory,
International Seminar dedicated to the memory of D. V. Volkov, Kharkov, 1997 | null | 10.1007/BFb0105225 | null | hep-th | null | We consider intersecting M-brane solutions of supergravity in eleven
dimensions. Supersymmetry turns out to be a powerful tool in obtaining such
solutions and their generalizations.
| [
{
"created": "Tue, 18 Mar 1997 08:57:39 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"de Roo",
"M.",
""
]
] | We consider intersecting M-brane solutions of supergravity in eleven dimensions. Supersymmetry turns out to be a powerful tool in obtaining such solutions and their generalizations. | 9.727913 | 6.637045 | 11.393881 | 6.770544 | 6.990253 | 7.007253 | 7.211512 | 7.222172 | 6.906772 | 7.981905 | 6.864977 | 7.901918 | 8.762823 | 8.10439 | 7.996311 | 8.392203 | 8.055779 | 7.788532 | 7.47938 | 8.441416 | 7.687702 |
2202.05490 | Dirk Kreimer | Dirk Kreimer | Bananas: multi-edge graphs and their Feynman integrals | 43 pages, 7 figures, minor corrections | Lett Math Phys 113, 38 (2023) | 10.1007/s11005-023-01660-4 | MaPhy-AvH/2022-01 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We consider multi-edge or banana graphs $b_n$ on $n$ internal edges $e_i$
with different masses $m_i$. We focus on the cut banana graphs
$\Im(\Phi_R(b_n))$ from which the full result $\Phi_R(b_n)$ can be derived
through dispersion. We give a recursive definition of $\Im(\Phi_R(b_n))$
through iterated integrals. We di... | [
{
"created": "Fri, 11 Feb 2022 08:02:32 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Jun 2022 10:08:24 GMT",
"version": "v2"
}
] | 2023-04-04 | [
[
"Kreimer",
"Dirk",
""
]
] | We consider multi-edge or banana graphs $b_n$ on $n$ internal edges $e_i$ with different masses $m_i$. We focus on the cut banana graphs $\Im(\Phi_R(b_n))$ from which the full result $\Phi_R(b_n)$ can be derived through dispersion. We give a recursive definition of $\Im(\Phi_R(b_n))$ through iterated integrals. We disc... | 18.784302 | 15.128486 | 13.109186 | 12.446038 | 13.661619 | 13.258408 | 14.276654 | 15.081051 | 12.035952 | 14.910252 | 14.78317 | 12.660655 | 12.801669 | 12.515347 | 12.387431 | 12.761258 | 13.068898 | 13.547379 | 12.532219 | 12.760979 | 14.029659 |
hep-th/0607025 | Giuseppe Mussardo | Giuseppe Mussardo | Neutral Bound States in Kink-like Theories | 68 pages, 30 figures | Nucl.Phys.B779:101-154,2007 | 10.1016/j.nuclphysb.2007.03.053 | null | hep-th cond-mat.other hep-lat | null | In this paper we present an elementary derivation of the semi-classical
spectrum of neutral particles in a field theory with kink excitations. In the
non-integrable cases, we show that each vacuum state cannot generically support
more than two stable particles, since all other neutral exitations are
resonances, which... | [
{
"created": "Wed, 5 Jul 2006 14:13:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Mussardo",
"Giuseppe",
""
]
] | In this paper we present an elementary derivation of the semi-classical spectrum of neutral particles in a field theory with kink excitations. In the non-integrable cases, we show that each vacuum state cannot generically support more than two stable particles, since all other neutral exitations are resonances, which w... | 13.125829 | 12.414122 | 13.854081 | 11.910679 | 12.432983 | 12.367179 | 12.053489 | 11.938193 | 12.269069 | 14.054883 | 11.363637 | 11.998936 | 13.095041 | 12.685298 | 12.523276 | 12.038291 | 12.392681 | 12.52391 | 12.554203 | 13.589262 | 12.143859 |
0711.1870 | Takuya Okuda | Nick Halmagyi (EFI, U. Chicago) and Takuya Okuda (KITP, UC Santa
Barbara) | Bubbling Calabi-Yau geometry from matrix models | 30 pages; v.2 reference added, minor corrections | JHEP0803:028,2008 | 10.1088/1126-6708/2008/03/028 | EFI-07-32, NSF-KITP-07-192 | hep-th | null | We study bubbling geometry in topological string theory. Specifically, we
analyse Chern-Simons theory on both the 3-sphere and lens spaces in the
presence of a Wilson loop insertion of an arbitrary representation. For each of
these three manifolds we formulate a multi-matrix model whose partition
function is the vev ... | [
{
"created": "Mon, 12 Nov 2007 21:34:47 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Feb 2008 09:02:21 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Halmagyi",
"Nick",
"",
"EFI, U. Chicago"
],
[
"Okuda",
"Takuya",
"",
"KITP, UC Santa\n Barbara"
]
] | We study bubbling geometry in topological string theory. Specifically, we analyse Chern-Simons theory on both the 3-sphere and lens spaces in the presence of a Wilson loop insertion of an arbitrary representation. For each of these three manifolds we formulate a multi-matrix model whose partition function is the vev of... | 8.308914 | 7.424206 | 8.956094 | 7.125143 | 7.480208 | 7.223296 | 8.168422 | 7.640717 | 7.262322 | 9.264441 | 7.297621 | 7.034077 | 7.644869 | 7.088324 | 7.282111 | 7.089345 | 7.080521 | 7.121135 | 7.235868 | 8.203773 | 7.322189 |
hep-th/0406218 | Aaron Bergman | Aaron Bergman and Uday Varadarajan | Loop Groups, Kaluza-Klein Reduction and M-Theory | 26 pages, LaTeX, utarticle.cls, v2:clarifications and refs added | JHEP0506:043,2005 | 10.1088/1126-6708/2005/06/043 | UTTG-06-04 | hep-th | null | We show that the data of a principal G-bundle over a principal circle bundle
is equivalent to that of a \hat{LG} = U(1) |x LG bundle over the base of the
circle bundle. We apply this to the Kaluza-Klein reduction of M-theory to IIA
and show that certain generalized characteristic classes of the loop group
bundle enco... | [
{
"created": "Thu, 24 Jun 2004 05:51:05 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Jul 2004 20:31:54 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Bergman",
"Aaron",
""
],
[
"Varadarajan",
"Uday",
""
]
] | We show that the data of a principal G-bundle over a principal circle bundle is equivalent to that of a \hat{LG} = U(1) |x LG bundle over the base of the circle bundle. We apply this to the Kaluza-Klein reduction of M-theory to IIA and show that certain generalized characteristic classes of the loop group bundle encode... | 8.94357 | 8.911077 | 10.528312 | 9.306456 | 8.526321 | 9.266501 | 8.947734 | 8.707966 | 9.002106 | 12.922879 | 8.493832 | 8.58739 | 9.828403 | 9.259556 | 8.680158 | 8.500786 | 8.826198 | 8.510967 | 8.873918 | 10.362417 | 8.408605 |
1309.0146 | Tarek Anous | Dionysios Anninos, Tarek Anous, Frederik Denef, Lucas Peeters | Holographic Vitrification | 100 pages, 25 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish the existence of stable and metastable stationary black hole
bound states at finite temperature and chemical potentials in global and planar
four-dimensional asymptotically anti-de Sitter space. We determine a number of
features of their holographic duals and argue they represent structural
glasses. We m... | [
{
"created": "Sat, 31 Aug 2013 19:13:30 GMT",
"version": "v1"
}
] | 2013-09-03 | [
[
"Anninos",
"Dionysios",
""
],
[
"Anous",
"Tarek",
""
],
[
"Denef",
"Frederik",
""
],
[
"Peeters",
"Lucas",
""
]
] | We establish the existence of stable and metastable stationary black hole bound states at finite temperature and chemical potentials in global and planar four-dimensional asymptotically anti-de Sitter space. We determine a number of features of their holographic duals and argue they represent structural glasses. We map... | 17.073154 | 14.724277 | 17.749588 | 14.81709 | 15.942475 | 16.247833 | 15.468225 | 15.849494 | 13.615692 | 17.762907 | 14.758736 | 14.144288 | 15.923903 | 13.997822 | 14.015645 | 14.616571 | 14.234869 | 14.385543 | 14.505489 | 16.608963 | 14.109997 |
hep-th/0311113 | Alexandre C. Tort | D Pinheiro, F C Santos, and A. C. Tort | An alternative calculation of the Casimir energy for kappa-deformed
electrodynamics | Four pages, latex file. Submitted for the Proceedings of the XXIV
Brazilian National Meeting on Particles and Fields held in Caxambu MG,
Brazil, September 30 -- October 4, 2003 | null | null | null | hep-th | null | A simple, but effcient way of calculating regularized Casimir energies
suitable for non-trivial frequency spectra is briefly described and applied to
the case of a kappa-deformed scalar field theory. The results are consistent
with the ones obtained by other means.
| [
{
"created": "Thu, 13 Nov 2003 19:43:19 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Pinheiro",
"D",
""
],
[
"Santos",
"F C",
""
],
[
"Tort",
"A. C.",
""
]
] | A simple, but effcient way of calculating regularized Casimir energies suitable for non-trivial frequency spectra is briefly described and applied to the case of a kappa-deformed scalar field theory. The results are consistent with the ones obtained by other means. | 17.700031 | 14.364031 | 14.702021 | 12.237587 | 13.253194 | 13.940155 | 14.641414 | 12.327908 | 13.68029 | 15.783743 | 13.19739 | 13.728336 | 14.085191 | 13.21736 | 13.176783 | 13.325144 | 13.281948 | 13.345524 | 13.148618 | 13.757462 | 12.845442 |
1906.12252 | Carlos Mafra | Elliot Bridges and Carlos R. Mafra | Algorithmic construction of SYM multiparticle superfields in the BCJ
gauge | 43 pages | null | 10.1007/JHEP10(2019)022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We write down closed formulas for all necessary steps to obtain multiparticle
super Yang--Mills superfields in the so-called BCJ gauge. The superfields in
this gauge have obvious applications in the quest for finding BCJ-satisfying
representations of amplitudes. As a benefit of having these closed formulas, we
identi... | [
{
"created": "Fri, 28 Jun 2019 14:58:06 GMT",
"version": "v1"
}
] | 2019-10-23 | [
[
"Bridges",
"Elliot",
""
],
[
"Mafra",
"Carlos R.",
""
]
] | We write down closed formulas for all necessary steps to obtain multiparticle super Yang--Mills superfields in the so-called BCJ gauge. The superfields in this gauge have obvious applications in the quest for finding BCJ-satisfying representations of amplitudes. As a benefit of having these closed formulas, we identify... | 20.943935 | 19.250502 | 22.673557 | 19.576893 | 21.638128 | 22.17964 | 19.81776 | 18.778982 | 19.279329 | 24.602364 | 18.026056 | 19.956942 | 20.764832 | 19.340519 | 20.433514 | 19.649818 | 20.04845 | 19.310192 | 19.67366 | 19.741335 | 19.132456 |
1702.03497 | Yu-Xiao Liu | Feng-Wei Chen, Bao-Min Gu, Yu-Xiao Liu | Stability of braneworlds with non-minimally coupled multi-scalar fields | 13 pages, 3 figures | Eur.Phys.J. C78 (2018) 131 | 10.1140/epjc/s10052-018-5613-7 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Linear stability of braneworld models constructed with multi-scalar fields is
very different from that of single-scalar field models. It is well known that
both the tensor and scalar perturbation equations of the later can always be
written as a supersymmetric Schr\"{o}dinger equation, so it can be shown that
the per... | [
{
"created": "Sun, 12 Feb 2017 07:25:57 GMT",
"version": "v1"
},
{
"created": "Sat, 17 Jun 2017 16:30:46 GMT",
"version": "v2"
},
{
"created": "Sun, 25 Feb 2018 07:51:31 GMT",
"version": "v3"
}
] | 2018-02-27 | [
[
"Chen",
"Feng-Wei",
""
],
[
"Gu",
"Bao-Min",
""
],
[
"Liu",
"Yu-Xiao",
""
]
] | Linear stability of braneworld models constructed with multi-scalar fields is very different from that of single-scalar field models. It is well known that both the tensor and scalar perturbation equations of the later can always be written as a supersymmetric Schr\"{o}dinger equation, so it can be shown that the pertu... | 5.767403 | 5.936878 | 6.009596 | 5.68308 | 6.102497 | 6.040192 | 6.055084 | 5.816287 | 5.772401 | 6.196265 | 5.534893 | 5.754644 | 5.927648 | 5.724908 | 5.760334 | 5.712216 | 5.615099 | 5.705959 | 5.59598 | 5.732525 | 5.61665 |
hep-th/0412332 | Gregory Gabadadze | Gregory Gabadadze and Luca Grisa | Lorentz-violating massive gauge and gravitational fields | 14 LaTex pages, 3 refs with comments added; PLB version | Phys.Lett.B617:124-132,2005 | 10.1016/j.physletb.2005.04.064 | NYU-TH-04/12/13 | hep-th | null | We study nonlinear dynamics in models of Lorentz-violating massive gravity.
The Boulware-Deser instability restricts severely the class of acceptable
theories. We identify a model that is stable. It exhibits the following bizarre
but interesting property: there are only two massive propagating degrees of
freedom in t... | [
{
"created": "Fri, 31 Dec 2004 17:57:23 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Apr 2005 19:20:20 GMT",
"version": "v2"
}
] | 2011-07-19 | [
[
"Gabadadze",
"Gregory",
""
],
[
"Grisa",
"Luca",
""
]
] | We study nonlinear dynamics in models of Lorentz-violating massive gravity. The Boulware-Deser instability restricts severely the class of acceptable theories. We identify a model that is stable. It exhibits the following bizarre but interesting property: there are only two massive propagating degrees of freedom in the... | 12.35446 | 10.901205 | 12.253667 | 10.905773 | 11.014075 | 11.235181 | 11.491472 | 12.240204 | 11.193682 | 12.309276 | 10.888618 | 10.977532 | 11.473075 | 11.482563 | 10.960724 | 11.089561 | 10.914576 | 11.521143 | 11.393571 | 11.704578 | 11.181372 |
2106.10576 | Surjeet Rajendran | David E. Kaplan and Surjeet Rajendran | A Causal Framework for Non-Linear Quantum Mechanics | 22 pages, 0 figures, Journal Version | Phys Rev D 105 055002 (2022) | 10.1103/PhysRevD.105.055002 | null | hep-th gr-qc hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We add non-linear and state-dependent terms to quantum field theory. We show
that the resulting low-energy theory, non-linear quantum mechanics, is causal,
preserves probability and permits a consistent description of the process of
measurement. We explore the consequences of such terms and show that non-linear
quant... | [
{
"created": "Sat, 19 Jun 2021 21:52:27 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Mar 2022 13:50:55 GMT",
"version": "v2"
}
] | 2022-03-10 | [
[
"Kaplan",
"David E.",
""
],
[
"Rajendran",
"Surjeet",
""
]
] | We add non-linear and state-dependent terms to quantum field theory. We show that the resulting low-energy theory, non-linear quantum mechanics, is causal, preserves probability and permits a consistent description of the process of measurement. We explore the consequences of such terms and show that non-linear quantum... | 14.657148 | 17.490353 | 15.496227 | 14.615821 | 16.460148 | 17.282955 | 17.010132 | 15.759305 | 15.32335 | 16.939672 | 15.357726 | 14.639977 | 14.453935 | 14.535041 | 14.451316 | 14.212961 | 14.493714 | 14.797688 | 13.982052 | 14.369936 | 14.2676 |
hep-th/0606274 | Mariano Cadoni | Mariano Cadoni | Conformal symmetry of gravity and the cosmological constant problem | Some references have been added. Some points have been clarified | Phys.Lett. B642 (2006) 525-529 | 10.1016/j.physletb.2006.10.009 | null | hep-th astro-ph gr-qc | null | In absence of matter Einstein gravity with a cosmological constant $\La$ can
be formulated as a scale-free theory depending only on the dimensionless
coupling constant G \Lambda where G is Newton constant. We derive the conformal
field theory (CFT) and its improved stress-energy tensor that describe the
dynamics of c... | [
{
"created": "Thu, 29 Jun 2006 13:52:15 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Sep 2006 14:58:33 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Cadoni",
"Mariano",
""
]
] | In absence of matter Einstein gravity with a cosmological constant $\La$ can be formulated as a scale-free theory depending only on the dimensionless coupling constant G \Lambda where G is Newton constant. We derive the conformal field theory (CFT) and its improved stress-energy tensor that describe the dynamics of con... | 9.907822 | 10.578094 | 9.416925 | 9.525799 | 9.872625 | 10.311919 | 10.317669 | 9.596394 | 9.932327 | 10.431224 | 9.215341 | 8.807138 | 9.270377 | 8.978885 | 8.53954 | 9.084069 | 9.149228 | 8.857552 | 8.839143 | 9.238196 | 8.833443 |
hep-th/0103107 | Miao Li | Miao Li | Dimensional Reduction via Noncommutative Spacetime: Bootstrap and
Holography | 15 pages, harvmac. v2: typos corrected and some changes made | JHEP 0205 (2002) 033 | 10.1088/1126-6708/2002/05/033 | null | hep-th gr-qc quant-ph | null | Unlike noncommutative space, when space and time are noncommutative, it seems
necessary to modify the usual scheme of quantum mechanics. We propose in this
paper a simple generalization of the time evolution equation in quantum
mechanics to incorporate the feature of a noncommutative spacetime. This
equation is much ... | [
{
"created": "Wed, 14 Mar 2001 14:16:19 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Mar 2001 06:38:32 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Li",
"Miao",
""
]
] | Unlike noncommutative space, when space and time are noncommutative, it seems necessary to modify the usual scheme of quantum mechanics. We propose in this paper a simple generalization of the time evolution equation in quantum mechanics to incorporate the feature of a noncommutative spacetime. This equation is much mo... | 12.864484 | 11.838858 | 12.724534 | 11.383747 | 13.050823 | 12.298856 | 12.981986 | 11.580738 | 12.547634 | 13.021325 | 11.455527 | 11.882647 | 12.163377 | 11.622688 | 11.515994 | 11.679193 | 11.703944 | 11.410177 | 11.763439 | 12.033949 | 11.927752 |
hep-th/0204058 | Larus Thorlacius | K.R. Kristjansson and L. Thorlacius | Cosmological Models and Renormalization Group Flow | 26 pages, 11 figures, v2: improved discussion of entropy bounds,
references added, v3: minor changes, reference added | JHEP 0205 (2002) 011 | 10.1088/1126-6708/2002/05/011 | RH-05-2002 | hep-th gr-qc | null | We study cosmological solutions of Einstein gravity with a positive
cosmological constant in diverse dimensions. These include big-bang models that
re-collapse, big-bang models that approach de Sitter acceleration at late
times, and bounce models that are both past and future asymptotically de
Sitter. The re-collapsi... | [
{
"created": "Sat, 6 Apr 2002 00:34:27 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Apr 2002 16:44:22 GMT",
"version": "v2"
},
{
"created": "Mon, 13 May 2002 13:31:30 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Kristjansson",
"K. R.",
""
],
[
"Thorlacius",
"L.",
""
]
] | We study cosmological solutions of Einstein gravity with a positive cosmological constant in diverse dimensions. These include big-bang models that re-collapse, big-bang models that approach de Sitter acceleration at late times, and bounce models that are both past and future asymptotically de Sitter. The re-collapsing... | 8.643985 | 9.077875 | 9.592253 | 8.349092 | 10.221666 | 8.997705 | 9.152237 | 8.552155 | 8.59135 | 9.928455 | 8.630951 | 8.44743 | 8.865666 | 8.59275 | 8.476181 | 8.420226 | 8.296235 | 8.400687 | 8.555603 | 8.798572 | 8.22338 |
hep-th/9602051 | Gary Horowitz | Gary Horowitz and Andrew Strominger | Counting States of Near-Extremal Black Holes | 11 pages, references corrected | Phys.Rev.Lett.77:2368-2371,1996 | 10.1103/PhysRevLett.77.2368 | null | hep-th gr-qc | null | A six-dimensional black string is considered and its Bekenstein-Hawking
entropy computed. It is shown that to leading order above extremality, this
entropy precisely counts the number of string states with the given energy and
charges. This identification implies that Hawking decay of the near-extremal
black string c... | [
{
"created": "Sat, 10 Feb 1996 01:08:48 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Feb 1996 01:05:14 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Horowitz",
"Gary",
""
],
[
"Strominger",
"Andrew",
""
]
] | A six-dimensional black string is considered and its Bekenstein-Hawking entropy computed. It is shown that to leading order above extremality, this entropy precisely counts the number of string states with the given energy and charges. This identification implies that Hawking decay of the near-extremal black string can... | 10.541492 | 8.898832 | 10.552493 | 8.98486 | 9.707552 | 9.075858 | 9.237195 | 9.171881 | 9.128307 | 10.718167 | 8.497115 | 8.925828 | 9.527811 | 9.209667 | 9.146402 | 9.585906 | 8.798095 | 8.87113 | 9.056753 | 9.782213 | 8.851828 |
0706.0717 | Michael Kroyter | Ehud Fuchs and Michael Kroyter | Marginal deformation for the photon in superstring field theory | v1. 17 pages; v2. 21 pages. Presentation expanded, fig. added, refs.
added, typos corrected | JHEP 0711:005,2007 | 10.1088/1126-6708/2007/11/005 | AEI-2007-042 | hep-th | null | We find solutions of supersymmetric string field theory that correspond to
the photon marginal deformation in the boundary conformal field theory. We
revisit the bosonic string marginal deformation and generate a real solution
for it. We find a map between the solutions of bosonic and supersymmetric
string field theo... | [
{
"created": "Tue, 5 Jun 2007 18:35:00 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Nov 2007 09:15:51 GMT",
"version": "v2"
}
] | 2009-04-17 | [
[
"Fuchs",
"Ehud",
""
],
[
"Kroyter",
"Michael",
""
]
] | We find solutions of supersymmetric string field theory that correspond to the photon marginal deformation in the boundary conformal field theory. We revisit the bosonic string marginal deformation and generate a real solution for it. We find a map between the solutions of bosonic and supersymmetric string field theori... | 15.310462 | 14.615427 | 14.099625 | 14.785595 | 14.316194 | 14.496825 | 14.23035 | 13.41925 | 14.366665 | 16.98395 | 14.157729 | 14.841702 | 14.201779 | 13.857864 | 15.136239 | 13.725793 | 13.732343 | 13.933888 | 13.641427 | 15.281152 | 14.495346 |
1912.08039 | Madad Ali Valuyan | M. A. Valuyan | Radiative Correction of the Casimir Energy for the Scalar Field with the
Mixed Boundary Condition in 3 + 1 Dimensions | 15 Pages, In Persian language, 5 figures | Journal of Research on Many-body Systems, 9(3), 187-201 (2019) | 10.22055/JRMBS.2019.14916 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present study, the zeroth- and first-order radiative correction of the
Casimir energy for massive and massless scalar fields, confined with mixed
boundary conditions (Dirichlet- Neumann) between two parallel plates in
$\phi^4$ theory, were computed. Two issues in performing calculations in this
work are essent... | [
{
"created": "Tue, 17 Dec 2019 14:39:21 GMT",
"version": "v1"
}
] | 2019-12-18 | [
[
"Valuyan",
"M. A.",
""
]
] | In the present study, the zeroth- and first-order radiative correction of the Casimir energy for massive and massless scalar fields, confined with mixed boundary conditions (Dirichlet- Neumann) between two parallel plates in $\phi^4$ theory, were computed. Two issues in performing calculations in this work are essentia... | 11.687723 | 9.914861 | 11.878919 | 10.257765 | 10.177746 | 9.604973 | 9.617936 | 10.014956 | 10.736562 | 13.12779 | 10.359501 | 10.982807 | 11.880904 | 11.260381 | 11.115496 | 10.952756 | 11.218219 | 10.859301 | 11.146653 | 11.727875 | 10.98385 |
2307.02743 | Pujian Mao | Song He, Pujian Mao, Xin-Cheng Mao | Loop corrections versus marginal deformation in celestial holography | v2: 9 pages + appendices, interpretations significantly improved,
sections reorganized, main results unchanged, new section about moduli spaces
of bulk vacua added, sections of deformed soft graviton theorem and shifted
stress tensor moved to appendix, refs. added | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | Four-dimensional all-loop amplitudes in QED and gravity exhibit universal
Infrared (IR) singularities with a factorization structure. This structure is
governed by tree amplitudes and a universal IR-divergent factor representing
the exchange of soft particles between external lines. This letter offers a
precise dual ... | [
{
"created": "Thu, 6 Jul 2023 03:06:41 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Oct 2023 16:17:45 GMT",
"version": "v2"
}
] | 2023-10-30 | [
[
"He",
"Song",
""
],
[
"Mao",
"Pujian",
""
],
[
"Mao",
"Xin-Cheng",
""
]
] | Four-dimensional all-loop amplitudes in QED and gravity exhibit universal Infrared (IR) singularities with a factorization structure. This structure is governed by tree amplitudes and a universal IR-divergent factor representing the exchange of soft particles between external lines. This letter offers a precise dual in... | 14.704184 | 12.595679 | 14.888562 | 11.775225 | 12.306717 | 12.799787 | 11.949541 | 11.792199 | 12.332305 | 15.83704 | 12.102468 | 13.051669 | 13.600246 | 12.810041 | 12.753287 | 13.369425 | 13.19034 | 12.897775 | 13.0159 | 14.102126 | 12.987332 |
hep-th/0212291 | Peter West | P. West | Very Extended $E_8$ and $A_8$ at low levels, Gravity and Supergravity | 16 pages, plain tex (equation 3.3 modified and one reference
expanded) | Class.Quant.Grav.20:2393-2406,2003 | 10.1088/0264-9381/20/11/328 | KCL-MTH-02-31 | hep-th | null | We define a level for a large class of Lorentzian Kac-Moody algebras. Using
this we find the representation content of very extended $A_{D-3}$ and $E_8$
(i.e. $E_{11}$) at low levels in terms of $A_{D-1}$ and $A_{10}$
representations respectively. The results are consistent with the conjectured
very extended $A_8$ an... | [
{
"created": "Mon, 23 Dec 2002 18:42:02 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jan 2003 15:10:58 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"West",
"P.",
""
]
] | We define a level for a large class of Lorentzian Kac-Moody algebras. Using this we find the representation content of very extended $A_{D-3}$ and $E_8$ (i.e. $E_{11}$) at low levels in terms of $A_{D-1}$ and $A_{10}$ representations respectively. The results are consistent with the conjectured very extended $A_8$ and ... | 7.486001 | 6.909267 | 8.546168 | 6.617458 | 7.506586 | 8.266151 | 7.036352 | 6.410701 | 6.726182 | 8.338201 | 6.579333 | 6.755804 | 7.077354 | 6.648903 | 6.730432 | 6.567348 | 6.997788 | 6.370187 | 6.833171 | 7.727927 | 6.639186 |
2110.02255 | Davide Gaiotto | Davide Gaiotto | Vertex Algebra constructions for (analytic) Geometric Langlands in genus
zero | 30 pages | null | null | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We employ two-dimensional chiral algebra techniques to produce solutions of
certain differential and integral equations which occur in the context of the
Analytic Geometric Langlands Program.
| [
{
"created": "Tue, 5 Oct 2021 18:06:24 GMT",
"version": "v1"
}
] | 2021-10-07 | [
[
"Gaiotto",
"Davide",
""
]
] | We employ two-dimensional chiral algebra techniques to produce solutions of certain differential and integral equations which occur in the context of the Analytic Geometric Langlands Program. | 27.341373 | 17.977537 | 28.281191 | 17.837675 | 14.09341 | 19.306873 | 20.077906 | 19.707941 | 16.757925 | 30.159447 | 15.923273 | 18.193457 | 26.446211 | 19.075199 | 19.842644 | 18.776098 | 18.491703 | 18.052185 | 20.097662 | 22.358799 | 19.060888 |
hep-th/0303048 | Ulrich Theis | Ulrich Theis and Stefan Vandoren | N=2 Supersymmetric Scalar-Tensor Couplings | 23 pages, LaTeX2e with amsmath.sty; v2: corrected typos and added
reference | JHEP 0304 (2003) 042 | 10.1088/1126-6708/2003/04/042 | ITP-UU-03/06, SPIN-03/04, TUW-03-07 | hep-th | null | We determine the general coupling of a system of scalars and antisymmetric
tensors, with at most two derivatives and undeformed gauge transformations, for
both rigid and local N=2 supersymmetry in four-dimensional spacetime. Our
results cover interactions of hyper, tensor and double-tensor multiplets and
apply among ... | [
{
"created": "Thu, 6 Mar 2003 18:25:05 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Apr 2003 12:52:51 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Theis",
"Ulrich",
""
],
[
"Vandoren",
"Stefan",
""
]
] | We determine the general coupling of a system of scalars and antisymmetric tensors, with at most two derivatives and undeformed gauge transformations, for both rigid and local N=2 supersymmetry in four-dimensional spacetime. Our results cover interactions of hyper, tensor and double-tensor multiplets and apply among ot... | 9.374406 | 7.520999 | 10.430592 | 8.513153 | 7.891191 | 8.284583 | 7.883156 | 7.950036 | 7.662398 | 10.841916 | 8.072556 | 8.535769 | 9.708573 | 8.346172 | 8.206196 | 8.091619 | 8.293555 | 8.515814 | 8.571532 | 9.509193 | 8.495383 |
hep-th/0011047 | Partha Mukhopadhyay | Partha Mukhopadhyay | Unstable Non-BPS D-Branes of Type-II String Theories in Light-Cone
Green-Schwarz Formalism | LaTeX file, 37 pages | Nucl.Phys. B600 (2001) 285-314 | 10.1016/S0550-3213(01)00072-4 | MRI-P-001101 | hep-th | null | The problem of describing the boundary states of unstable non-BPS D-branes of
type-II string theories in light-cone Green-Schwarz (GS) formalism is
addressed. Regarding the type II theories in light-cone gauge as different
realizations of the $\hat{SO}(8)_{k=1}$ Kac-Moody algebra, the non-BPS D-brane
boundary states ... | [
{
"created": "Wed, 8 Nov 2000 10:00:56 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Mukhopadhyay",
"Partha",
""
]
] | The problem of describing the boundary states of unstable non-BPS D-branes of type-II string theories in light-cone Green-Schwarz (GS) formalism is addressed. Regarding the type II theories in light-cone gauge as different realizations of the $\hat{SO}(8)_{k=1}$ Kac-Moody algebra, the non-BPS D-brane boundary states of... | 7.654859 | 7.233655 | 8.723847 | 6.844728 | 7.692177 | 7.496083 | 6.984688 | 6.69819 | 7.238851 | 8.958613 | 7.421553 | 7.327613 | 7.599431 | 7.051206 | 7.143613 | 7.115577 | 7.044196 | 7.302117 | 7.227102 | 7.619167 | 7.185677 |
2104.06435 | Paul Romatschke | Paul Romatschke | Shear Viscosity at Infinite Coupling: A Field Theory Calculation | 6 pages, 1 figure plus supplemental material; v2: fixed typos and
buggy code for (84) in v1, corrected eta/s values; v3: typo in (9) corrected,
Fig.1 updated (no change in results) | Phys. Rev. Lett. 127, 111603 (2021) | 10.1103/PhysRevLett.127.111603 | null | hep-th cond-mat.str-el hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I derive an exact integral expression for the ratio of shear viscosity over
entropy density $\frac{\eta}{s}$ for the massless (critical) O(N) model at
large N with quartic interactions. The calculation is set up and performed
entirely from the field theory side using a non-perturbative resummation scheme
that capture... | [
{
"created": "Tue, 13 Apr 2021 18:20:51 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Jun 2021 15:01:30 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Dec 2021 19:19:20 GMT",
"version": "v3"
}
] | 2021-12-23 | [
[
"Romatschke",
"Paul",
""
]
] | I derive an exact integral expression for the ratio of shear viscosity over entropy density $\frac{\eta}{s}$ for the massless (critical) O(N) model at large N with quartic interactions. The calculation is set up and performed entirely from the field theory side using a non-perturbative resummation scheme that captures ... | 7.433882 | 7.334864 | 7.35267 | 6.395656 | 7.047901 | 6.864169 | 6.499018 | 7.074154 | 6.980169 | 8.556369 | 6.621475 | 6.8392 | 7.217363 | 6.895268 | 6.916355 | 6.763239 | 6.843396 | 6.726963 | 6.840899 | 7.207611 | 6.868997 |
2209.14342 | Christos Litos | Elias Kiritsis, Christos Litos | Holographic RG flows on Squashed $S^3$ | 41 pages + appendices (v2) Several numerical errors corrected in
equations (F.15-16) on page 68, (F.93-F.96) on page 79, ,(F.128-132) on page
83, (F.143-F.146) on page 85 , and (F.192) and (F.196) on page 91. These
changes do not affect the results of the paper | null | 10.1007/JHEP12(2022)161 | CCTP-2022-6, ITCP-2022/6 | hep-th | http://creativecommons.org/licenses/by-nc-nd/4.0/ | Holographic RG flows dual to QFTs on a squashed $S^3$ are considered in the
framework of Einstein dilaton gravity in four dimensions. A general dilaton
potential is used and flows are driven by a scalar relevant operator. The
general properties of such flows are analysed and the UV and IR asymptotics are
computed. Ex... | [
{
"created": "Wed, 28 Sep 2022 18:11:16 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Jun 2023 18:02:27 GMT",
"version": "v2"
}
] | 2023-06-27 | [
[
"Kiritsis",
"Elias",
""
],
[
"Litos",
"Christos",
""
]
] | Holographic RG flows dual to QFTs on a squashed $S^3$ are considered in the framework of Einstein dilaton gravity in four dimensions. A general dilaton potential is used and flows are driven by a scalar relevant operator. The general properties of such flows are analysed and the UV and IR asymptotics are computed. Exot... | 9.389446 | 6.473358 | 7.818011 | 6.89754 | 6.917212 | 6.283966 | 6.131074 | 7.231134 | 7.225831 | 9.179691 | 6.649366 | 6.676354 | 7.410462 | 6.858459 | 6.821646 | 6.940382 | 6.754419 | 7.015463 | 7.031945 | 7.49677 | 7.183665 |
hep-th/9508008 | Rodriguez Romo Suemi-FESC | Suemi Rodr\'iguez-Romo | Real Space Renormalization-Group for Configurational Random Walk Models
on a Hierarchical Lattice. The Asymptotic End-to-End Distance of a Weakly
SARW in Dimension Four | 39 pages + 4 figures, LaTex | null | null | CIT-FESC-UNAM 95/2 | hep-th chem-ph cond-mat hep-lat | null | We present a real space renormalization-group map for probabilities of random
walks on a hierarchical lattice. From this, we study the asymptotic behavior of
the end-to-end distance of a weakly self- avoiding random walk (SARW) that
penalizes the (self-)intersection of two random walks in dimension four on the
hierar... | [
{
"created": "Wed, 2 Aug 1995 23:48:19 GMT",
"version": "v1"
}
] | 2016-08-15 | [
[
"Rodríguez-Romo",
"Suemi",
""
]
] | We present a real space renormalization-group map for probabilities of random walks on a hierarchical lattice. From this, we study the asymptotic behavior of the end-to-end distance of a weakly self- avoiding random walk (SARW) that penalizes the (self-)intersection of two random walks in dimension four on the hierarch... | 12.412049 | 14.173906 | 15.111334 | 12.26899 | 13.624444 | 12.698621 | 12.845313 | 12.35013 | 13.40023 | 15.000037 | 12.330221 | 12.263029 | 13.375085 | 12.547683 | 12.138955 | 11.789498 | 11.809787 | 12.276723 | 12.164218 | 14.695478 | 12.800437 |
hep-th/0612023 | Ram Sriharsha | Ram Sriharsha | The moduli space of hyper-K{\"a}hler four-fold compactifications | 42 pages, discussion of ${\cal N}=3$ supersymmetry preserving fluxes
added, acknowledegement added | JHEP 0703:095,2007 | 10.1088/1126-6708/2007/03/095 | null | hep-th | null | I discuss some aspects of the moduli space of hyper-K{\"a}hler four-fold
compactifications of type II and ${\cal M}$- theories. The dimension of the
moduli space of these theories is strictly bounded from above. As an example I
study Hilb$^2(K3)$ and the generalized Kummer variety $K^2(T^4)$. In both cases
RR-flux (o... | [
{
"created": "Mon, 4 Dec 2006 20:13:59 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Dec 2006 19:48:55 GMT",
"version": "v2"
},
{
"created": "Fri, 5 Jan 2007 01:01:01 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Sriharsha",
"Ram",
""
]
] | I discuss some aspects of the moduli space of hyper-K{\"a}hler four-fold compactifications of type II and ${\cal M}$- theories. The dimension of the moduli space of these theories is strictly bounded from above. As an example I study Hilb$^2(K3)$ and the generalized Kummer variety $K^2(T^4)$. In both cases RR-flux (or ... | 7.893292 | 8.663641 | 9.398465 | 8.414966 | 8.772562 | 8.540783 | 8.907834 | 8.709072 | 8.314722 | 10.347491 | 8.125974 | 7.950773 | 7.998576 | 7.730495 | 7.512102 | 7.821027 | 7.570317 | 7.616426 | 7.759468 | 7.908982 | 7.414596 |
0905.2970 | Shamit Kachru | Shamit Kachru, Dusan Simic and Sandip P. Trivedi | Stable Non-Supersymmetric Throats in String Theory | 28 pages,2 figures | JHEP 1005:067,2010 | 10.1007/JHEP05(2010)067 | NSF-KITP-09-55, SITP-09/17, SLAC-PUB-13593 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a large class of non-supersymmetric AdS-like throat geometries
in string theory by taking non-supersymmetric orbifolds of supersymmetric
backgrounds. The scale of SUSY breaking is the AdS radius, and the dual field
theory has explicitly broken supersymmetry. The large hierarchy of energy
scales in these ... | [
{
"created": "Tue, 19 May 2009 16:08:07 GMT",
"version": "v1"
}
] | 2010-05-27 | [
[
"Kachru",
"Shamit",
""
],
[
"Simic",
"Dusan",
""
],
[
"Trivedi",
"Sandip P.",
""
]
] | We construct a large class of non-supersymmetric AdS-like throat geometries in string theory by taking non-supersymmetric orbifolds of supersymmetric backgrounds. The scale of SUSY breaking is the AdS radius, and the dual field theory has explicitly broken supersymmetry. The large hierarchy of energy scales in these ge... | 7.90778 | 8.591838 | 8.819108 | 7.942722 | 8.76986 | 8.111886 | 8.819189 | 7.9468 | 7.839855 | 8.955532 | 8.044677 | 7.914715 | 8.129125 | 7.687421 | 7.741217 | 7.992125 | 7.904909 | 7.986121 | 7.770385 | 8.186671 | 7.677344 |
hep-th/9411045 | Marek Grabowski | M. P. Grabowski and P. Mathieu | Structure of the conservation laws in integrable spin chains with short
range interactions | 79 pages in plain TeX plus 4 uuencoded figures; (uses harvmac and
epsf) | Annals Phys. 243 (1995) 299-371 | 10.1006/aphy.1995.1101 | LAVAL-PHY-21/94 | hep-th cond-mat | null | We present a detailed analysis of the structure of the conservation laws in
quantum integrable chains of the XYZ-type and in the Hubbard model. With the
use of the boost operator, we establish the general form of the XYZ conserved
charges in terms of simple polynomials in spin variables and derive recursion
relations... | [
{
"created": "Mon, 7 Nov 1994 11:42:05 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Grabowski",
"M. P.",
""
],
[
"Mathieu",
"P.",
""
]
] | We present a detailed analysis of the structure of the conservation laws in quantum integrable chains of the XYZ-type and in the Hubbard model. With the use of the boost operator, we establish the general form of the XYZ conserved charges in terms of simple polynomials in spin variables and derive recursion relations f... | 10.750642 | 11.20363 | 11.577365 | 10.840032 | 11.673276 | 11.319442 | 12.037564 | 10.771727 | 10.723537 | 12.620163 | 10.949801 | 10.660064 | 10.890413 | 10.715523 | 10.424995 | 10.559122 | 10.746529 | 10.654385 | 10.28209 | 10.67307 | 10.515511 |
hep-th/0006041 | Martin Schvellinger | Martin Schvellinger (Oxford U.) | Confining strings, Wilson loops and extra dimensions | 17 pages, Latex, 5 eps figures, a discussion about the naked
singularity is included and three references added | Phys.Lett. B493 (2000) 402-410 | 10.1016/S0370-2693(00)01152-7 | OUTP-00-24-P | hep-th | null | We study solutions of the one-loop beta-functions of the critical bosonic
string theory in the framework of the Renormalization Group (RG) approach to
string theory, considering explicitly the effects of the 21 extra dimensions.
In the RG approach the 26-dimensional manifold is given in terms of a four
dimensional Mi... | [
{
"created": "Tue, 6 Jun 2000 10:36:36 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Nov 2000 18:07:23 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Schvellinger",
"Martin",
"",
"Oxford U."
]
] | We study solutions of the one-loop beta-functions of the critical bosonic string theory in the framework of the Renormalization Group (RG) approach to string theory, considering explicitly the effects of the 21 extra dimensions. In the RG approach the 26-dimensional manifold is given in terms of a four dimensional Mink... | 12.392605 | 13.294705 | 13.844661 | 12.637084 | 14.750702 | 13.738431 | 14.603306 | 13.103796 | 12.311876 | 14.371824 | 12.555454 | 12.541306 | 12.150939 | 12.019035 | 12.437543 | 12.435358 | 12.464836 | 12.197234 | 12.366722 | 12.218476 | 11.948763 |
0706.2015 | Evgeny Buchbinder | Evgeny I. Buchbinder | Infrared Limit of Gluon Amplitudes at Strong Coupling | 10 pages, 2 figures; minor corrections, references added; typos
corrected | Phys.Lett.B654:46-50,2007 | 10.1016/j.physletb.2007.08.028 | null | hep-th | null | In this note, we propose that the infrared structure of gluon amplitudes at
strong coupling can be fully extracted from a local consideration near cusps.
This is consistent with field theory and correctly reproduces the infrared
divergences of the four-gluon amplitude at strong coupling calculated recently
by Alday a... | [
{
"created": "Thu, 14 Jun 2007 00:24:04 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Jul 2007 05:20:10 GMT",
"version": "v2"
},
{
"created": "Fri, 27 Jul 2007 06:39:24 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Buchbinder",
"Evgeny I.",
""
]
] | In this note, we propose that the infrared structure of gluon amplitudes at strong coupling can be fully extracted from a local consideration near cusps. This is consistent with field theory and correctly reproduces the infrared divergences of the four-gluon amplitude at strong coupling calculated recently by Alday and... | 8.603612 | 7.852651 | 7.790623 | 7.592851 | 7.403412 | 7.32243 | 7.946778 | 7.658824 | 7.046567 | 8.854456 | 7.500288 | 7.853338 | 7.65604 | 7.352078 | 7.402293 | 7.741115 | 7.49928 | 8.028358 | 7.741909 | 7.497718 | 7.834459 |
hep-th/0604106 | Ahmad Ghodsi | Ahmad Ghodsi | R^4 Corrections to D1D5p Black Hole Entropy from Entropy Function
Formalism | 15 pages, minor corrections, typos corrected | Phys.Rev.D74:124026,2006 | 10.1103/PhysRevD.74.124026 | IPM/P-2006/022, CPHT RR020. 0406 | hep-th gr-qc | null | We show that in IIB string theory and for D1D5p black holes in ten dimensions
the method of entropy function works. Despite the more complicated Wald formula
for the entropy of D1D5p black holes in ten dimensions, their entropy is given
by entropy function at its extremum point. We use this method for computing the
e... | [
{
"created": "Fri, 14 Apr 2006 15:36:24 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Apr 2006 13:40:08 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Ghodsi",
"Ahmad",
""
]
] | We show that in IIB string theory and for D1D5p black holes in ten dimensions the method of entropy function works. Despite the more complicated Wald formula for the entropy of D1D5p black holes in ten dimensions, their entropy is given by entropy function at its extremum point. We use this method for computing the ent... | 13.77669 | 12.213516 | 16.070368 | 12.339344 | 12.659608 | 13.29857 | 10.69605 | 11.545657 | 11.36111 | 19.50676 | 10.864607 | 12.999891 | 13.068913 | 12.996241 | 12.950475 | 12.386449 | 12.139278 | 12.747936 | 12.869257 | 14.267845 | 12.728661 |
1708.05658 | Stephen Pietromonaco | Stephen Pietromonaco | Emergent Geometry Through Holomorphic Matrix Models | Masters Thesis in Physics, University of British Columbia, August
2017, 68 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Over the years, deep insights into string theory and supersymmetric gauge
theories have come from studying geometry emerging from matrix models. In this
thesis, I study the N=1* and N=2* theories from which an elliptic curve is
known to emerge, alongside an elliptic function called the generalized
resolvent into whic... | [
{
"created": "Tue, 15 Aug 2017 19:23:03 GMT",
"version": "v1"
}
] | 2017-08-21 | [
[
"Pietromonaco",
"Stephen",
""
]
] | Over the years, deep insights into string theory and supersymmetric gauge theories have come from studying geometry emerging from matrix models. In this thesis, I study the N=1* and N=2* theories from which an elliptic curve is known to emerge, alongside an elliptic function called the generalized resolvent into which ... | 10.286964 | 10.878432 | 11.598649 | 10.090325 | 11.382634 | 11.034648 | 11.166412 | 10.488819 | 10.450914 | 11.946502 | 10.397142 | 10.087855 | 10.628901 | 10.126872 | 10.304912 | 10.118063 | 10.259051 | 10.37184 | 10.306239 | 10.542504 | 10.547957 |
hep-th/9508029 | Jun Koga | Jun-ichirou Koga and Kei-ichi Maeda | Evaporation and Fate of Dilatonic Black Holes | 33 pages, LaTex, 14 postscript figure files (appended as a uuencoded
compressed tar file) | Phys.Rev. D52 (1995) 7066-7079 | 10.1103/PhysRevD.52.7066 | WU-AP/46/95 | hep-th gr-qc | null | We study both spherically symmetric and rotating black holes with dilaton
coupling and discuss the evaporation of these black holes via Hawking's quantum
radiation and their fates. We find that the dilaton coupling constant $\alpha$
drastically affects the emission rates, and therefore the fates of the black
holes. W... | [
{
"created": "Mon, 7 Aug 1995 09:27:17 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Koga",
"Jun-ichirou",
""
],
[
"Maeda",
"Kei-ichi",
""
]
] | We study both spherically symmetric and rotating black holes with dilaton coupling and discuss the evaporation of these black holes via Hawking's quantum radiation and their fates. We find that the dilaton coupling constant $\alpha$ drastically affects the emission rates, and therefore the fates of the black holes. Whe... | 7.461444 | 7.998711 | 8.296553 | 7.443357 | 7.647668 | 7.607612 | 7.797688 | 7.632556 | 7.385732 | 8.136689 | 7.605691 | 7.460679 | 7.610578 | 7.41854 | 7.466069 | 7.679695 | 7.409447 | 7.487905 | 7.327863 | 7.525584 | 7.378932 |
hep-th/9910148 | Terry Gannon | T. Gannon | Integers in the open string | 8 pp, plain tex | Phys.Lett. B473 (2000) 80-85 | 10.1016/S0370-2693(99)01468-9 | null | hep-th | null | We show that the $Y_{ab}^c$ of Pradisi-Sagnotti-Stanev are indeed integers,
and we prove a conjecture of Borisov-Halpern-Schweigert. We indicate some of
the special features which arise when the order of the modular matrix T is odd.
Our arguments are general, applying to arbitrary ``parent'' RCFT assuming only
that T... | [
{
"created": "Mon, 18 Oct 1999 21:23:15 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Gannon",
"T.",
""
]
] | We show that the $Y_{ab}^c$ of Pradisi-Sagnotti-Stanev are indeed integers, and we prove a conjecture of Borisov-Halpern-Schweigert. We indicate some of the special features which arise when the order of the modular matrix T is odd. Our arguments are general, applying to arbitrary ``parent'' RCFT assuming only that T h... | 20.076143 | 17.279509 | 26.516886 | 18.020819 | 19.122744 | 20.946993 | 20.438519 | 15.983495 | 18.505213 | 28.819887 | 18.129536 | 16.908587 | 20.018744 | 18.404041 | 19.468874 | 18.68564 | 18.201982 | 17.377214 | 17.942787 | 21.001959 | 18.314087 |
hep-th/9702068 | Charles Thorn | O. Bergman (Brandeis, Harvard) and C.B. Thorn (University of Florida) | The Size of a Polymer of String-Bits: A Numerical Investigation | 14 pages, LaTeX, 9 postscript figures | Nucl.Phys. B502 (1997) 309-324 | 10.1016/S0550-3213(97)00475-6 | null | hep-th | null | In string-bit models, string is described as a polymer of point-like
constituents. We attempt to use string-bit ideas to investigate how the size of
string is affected by string interactions in a non-perturbative context.
Lacking adequate methods to deal with the full complications of bit
rearrangement interactions, ... | [
{
"created": "Sat, 8 Feb 1997 20:08:55 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Bergman",
"O.",
"",
"Brandeis, Harvard"
],
[
"Thorn",
"C. B.",
"",
"University of Florida"
]
] | In string-bit models, string is described as a polymer of point-like constituents. We attempt to use string-bit ideas to investigate how the size of string is affected by string interactions in a non-perturbative context. Lacking adequate methods to deal with the full complications of bit rearrangement interactions, we... | 21.679495 | 19.193037 | 18.769672 | 17.856998 | 19.538141 | 17.238846 | 17.825274 | 18.237928 | 18.603289 | 22.715654 | 16.695633 | 16.961199 | 18.580921 | 16.896214 | 17.041157 | 17.375656 | 16.721188 | 16.717951 | 17.160183 | 18.430809 | 17.114237 |
1009.1615 | Juan Jottar | Ibrahima Bah, Alberto Faraggi, Juan I. Jottar and Robert G. Leigh | Fermions and Type IIB Supergravity On Squashed Sasaki-Einstein Manifolds | 43 pages, 2 figures, PDFLaTeX; v2: added references, typos corrected,
minor changes | JHEP 1101:100,2011 | 10.1007/JHEP01(2011)100 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the dimensional reduction of fermionic modes in a recently found
class of consistent truncations of type IIB supergravity compactified on
squashed five-dimensional Sasaki-Einstein manifolds. We derive the lower
dimensional equations of motion and effective action, and comment on the
supersymmetry of the re... | [
{
"created": "Wed, 8 Sep 2010 19:55:11 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Dec 2010 19:51:59 GMT",
"version": "v2"
}
] | 2011-01-27 | [
[
"Bah",
"Ibrahima",
""
],
[
"Faraggi",
"Alberto",
""
],
[
"Jottar",
"Juan I.",
""
],
[
"Leigh",
"Robert G.",
""
]
] | We discuss the dimensional reduction of fermionic modes in a recently found class of consistent truncations of type IIB supergravity compactified on squashed five-dimensional Sasaki-Einstein manifolds. We derive the lower dimensional equations of motion and effective action, and comment on the supersymmetry of the resu... | 7.12907 | 6.406162 | 7.657542 | 6.23315 | 6.579243 | 6.794298 | 6.403716 | 6.158291 | 6.498034 | 7.92011 | 6.59746 | 6.662342 | 7.058585 | 6.802829 | 6.777857 | 6.91501 | 6.682443 | 6.767004 | 6.77596 | 6.983632 | 6.648698 |
hep-th/0412088 | Nesic Ljubisa | Goran S. Djordjevic and Ljubisa Nesic | Towards Adelic Noncommutative Quantum Mechanics | 8 pages, Talk presented at the 8th Adriatic Meeting, "Particle
Physics in the new Millennium", (Dubrovnik, Croatia) | CRM Springer Lecture Notes in Physics, 616 (2003) 25-32, Editors:
J. Trampetic and J. Wess | null | null | hep-th math-ph math.MP | null | A motivation of using noncommutative and nonarchimedean geometry on very
short distances is given. Besides some mathematical preliminaries, we give a
short introduction in adelic quantum mechanics. We also recall to basic ideas
and tools embedded in q-deformed and noncommutative quantum mechanics. A rather
fundamenta... | [
{
"created": "Wed, 8 Dec 2004 15:50:11 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Djordjevic",
"Goran S.",
""
],
[
"Nesic",
"Ljubisa",
""
]
] | A motivation of using noncommutative and nonarchimedean geometry on very short distances is given. Besides some mathematical preliminaries, we give a short introduction in adelic quantum mechanics. We also recall to basic ideas and tools embedded in q-deformed and noncommutative quantum mechanics. A rather fundamental ... | 16.61969 | 16.142254 | 15.75795 | 15.315434 | 15.626022 | 15.917128 | 15.743394 | 14.899793 | 15.824536 | 16.859097 | 15.793791 | 15.679732 | 15.824208 | 15.519202 | 16.025318 | 16.107883 | 15.812146 | 15.797447 | 15.898338 | 15.349801 | 15.073577 |
hep-th/9704021 | M. Abouzeid | M. Abou Zeid and C. M. Hull | Intrinsic Geometry of D-Branes | 10 pages, LaTeX, no figures. Minor correction; version to appear in
Physics Letters B | Phys.Lett. B404 (1997) 264-270 | 10.1016/S0370-2693(97)00570-4 | QMW-PH-97-12 | hep-th | null | We obtain forms of Born-Infeld and D-brane actions that are quadratic in
derivatives of $X$ and linear in $F_{\mu \nu}$ by introducing an auxiliary
`metric' which has both symmetric and anti-symmetric parts, generalising the
simplification of the Nambu-Goto action for $p$-branes using a symmetric
metric. The abelian ... | [
{
"created": "Wed, 2 Apr 1997 21:01:25 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Apr 1997 19:58:12 GMT",
"version": "v2"
},
{
"created": "Tue, 20 May 1997 16:05:53 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Zeid",
"M. Abou",
""
],
[
"Hull",
"C. M.",
""
]
] | We obtain forms of Born-Infeld and D-brane actions that are quadratic in derivatives of $X$ and linear in $F_{\mu \nu}$ by introducing an auxiliary `metric' which has both symmetric and anti-symmetric parts, generalising the simplification of the Nambu-Goto action for $p$-branes using a symmetric metric. The abelian ga... | 9.776676 | 8.79746 | 10.225752 | 9.229432 | 9.173044 | 8.939326 | 8.688793 | 8.905787 | 9.134465 | 10.399024 | 8.767949 | 9.352034 | 9.642457 | 9.01002 | 8.899591 | 8.977939 | 9.093051 | 9.119205 | 9.269567 | 9.4866 | 8.987667 |
0810.4648 | Pedro J. Silva | Pedro J. Silva | The M2/M5 BPS Partition Functions from Supergravity | 9 pages, 2 columns, 4 figures, revtex, typos corrected, reference
added | JHEP 0901:083,2009 | 10.1088/1126-6708/2009/01/083 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the framework of the AdS/CFT duality, we calculate the supersymmetric
partition function of the superconformal field theories living in the world
volume of either $N$ $M2$-branes or $N$ $M5$-branes. We used the dual
supergravity partition function in a saddle point approximation over
supersymmetric Black Holes. Si... | [
{
"created": "Sat, 25 Oct 2008 21:39:45 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Nov 2008 11:25:39 GMT",
"version": "v2"
}
] | 2009-02-09 | [
[
"Silva",
"Pedro J.",
""
]
] | In the framework of the AdS/CFT duality, we calculate the supersymmetric partition function of the superconformal field theories living in the world volume of either $N$ $M2$-branes or $N$ $M5$-branes. We used the dual supergravity partition function in a saddle point approximation over supersymmetric Black Holes. Sinc... | 10.75906 | 11.003469 | 13.26145 | 10.340273 | 11.185892 | 11.158468 | 11.37509 | 10.651462 | 10.662941 | 14.556628 | 10.224663 | 10.310382 | 11.504931 | 10.687887 | 10.56957 | 10.753872 | 10.63988 | 10.226457 | 10.411602 | 11.336392 | 10.456044 |
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