id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2006.00299 | Madad Ali Valuyan | M. A. Valuyan | Radiative Correction to the Casimir Energy for Lorentz-violating Scalar
Field in d+1 Dimensions | 18 pages, 9 figures, 1 table, accepted for publication in MPLA | null | 10.1142/S0217732320501497 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The renormalization program in every renormalized theory should be run
consistently with the type of boundary condition imposed on quantum fields. To
maintain this consistency, the counterterms usually appear in the
position-dependent form. In the present study, using such counterterms, we
calculated the radiative co... | [
{
"created": "Sat, 30 May 2020 15:45:15 GMT",
"version": "v1"
}
] | 2020-06-02 | [
[
"Valuyan",
"M. A.",
""
]
] | The renormalization program in every renormalized theory should be run consistently with the type of boundary condition imposed on quantum fields. To maintain this consistency, the counterterms usually appear in the position-dependent form. In the present study, using such counterterms, we calculated the radiative corr... | 14.401816 | 12.752676 | 14.597597 | 13.660316 | 14.076969 | 13.03717 | 13.2652 | 12.712953 | 13.45434 | 15.72775 | 12.970922 | 13.6833 | 14.56401 | 13.906348 | 13.910854 | 13.616115 | 14.25749 | 13.947049 | 13.694518 | 14.802115 | 14.201353 |
1405.2046 | Francisco A. Brito | M. A. Anacleto, F. A. Brito, E. Passos and W. P. Santos | The entropy of the noncommutative acoustic black hole based on
generalized uncertainty principle | 9 pages, no figures; version to appear in PLB. arXiv admin note:
substantial text overlap with arXiv:1210.7739 | null | 10.1016/j.physletb.2014.08.018 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate statistical entropy of a 3-dimensional rotating
acoustic black hole based on generalized uncertainty principle. In our results
we obtain an area entropy and a correction term associated with the
noncommutative acoustic black hole when $\lambda$ introduced in the generalized
uncertainty pr... | [
{
"created": "Thu, 8 May 2014 18:59:51 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Aug 2014 17:31:42 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Anacleto",
"M. A.",
""
],
[
"Brito",
"F. A.",
""
],
[
"Passos",
"E.",
""
],
[
"Santos",
"W. P.",
""
]
] | In this paper we investigate statistical entropy of a 3-dimensional rotating acoustic black hole based on generalized uncertainty principle. In our results we obtain an area entropy and a correction term associated with the noncommutative acoustic black hole when $\lambda$ introduced in the generalized uncertainty prin... | 14.163864 | 11.222234 | 11.230513 | 11.855254 | 13.328906 | 12.512911 | 12.125253 | 12.181733 | 11.081888 | 13.753722 | 12.304995 | 11.451395 | 11.866713 | 11.338441 | 11.783291 | 11.909364 | 12.183107 | 11.283009 | 11.592042 | 12.231691 | 11.723466 |
hep-th/0304163 | Masako Fujita | Masako Fujita and Hiroyuki Hata (Kyoto U.) | Time Dependent Solution in Cubic String Field Theory | 22 pages, 12 figures, LaTeX2e, v3:minor corrections | JHEP 0305 (2003) 043 | 10.1088/1126-6708/2003/05/043 | KUNS-1835 | hep-th | null | We study time dependent solutions in cubic open string field theory which are
expected to describe the configuration of the rolling tachyon. We consider the
truncated system consisting of component fields of level zero and two, which
are expanded in terms of cosh n x^0 modes. For studying the large time behavior
of t... | [
{
"created": "Fri, 18 Apr 2003 07:51:21 GMT",
"version": "v1"
},
{
"created": "Fri, 23 May 2003 01:24:57 GMT",
"version": "v2"
},
{
"created": "Fri, 30 May 2003 05:37:41 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Fujita",
"Masako",
"",
"Kyoto U."
],
[
"Hata",
"Hiroyuki",
"",
"Kyoto U."
]
] | We study time dependent solutions in cubic open string field theory which are expected to describe the configuration of the rolling tachyon. We consider the truncated system consisting of component fields of level zero and two, which are expanded in terms of cosh n x^0 modes. For studying the large time behavior of the... | 13.269761 | 14.057953 | 14.493781 | 11.88514 | 12.990404 | 13.307524 | 13.18292 | 13.879595 | 11.872791 | 15.336394 | 12.423093 | 11.90686 | 12.123993 | 11.947698 | 11.285548 | 11.808839 | 12.026566 | 12.059505 | 11.66209 | 12.250779 | 11.666909 |
hep-th/9504113 | Ofer Aharony | O. Aharony, J. Sonnenschein and S. Yankielowicz | Flows and Duality Symmetries in N=1 Supersymmetric Gauge Theories | 31 pages, uses harvmac.tex and tables.tex Minor changes - version
accepted to Nucl. Phys. B | Nucl.Phys.B449:509-534,1995 | 10.1016/0550-3213(95)00332-M | TAUP-2246-95, CERN-TH/95-91 | hep-th | null | We present more examples of dual N=1 SUSY gauge theories. This set of
theories is connected by flows to both Seiberg's and Kutasov's dual theories.
This provides a unifying picture of the various dual theories. We investigate
the dual theories, their flat directions and mass perturbations.
| [
{
"created": "Sun, 23 Apr 1995 15:52:34 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Jul 1995 15:27:52 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Aharony",
"O.",
""
],
[
"Sonnenschein",
"J.",
""
],
[
"Yankielowicz",
"S.",
""
]
] | We present more examples of dual N=1 SUSY gauge theories. This set of theories is connected by flows to both Seiberg's and Kutasov's dual theories. This provides a unifying picture of the various dual theories. We investigate the dual theories, their flat directions and mass perturbations. | 14.304699 | 12.02267 | 14.284083 | 11.911529 | 12.715327 | 11.383166 | 10.633756 | 10.795979 | 11.25443 | 14.235405 | 11.338768 | 12.09576 | 13.444808 | 12.526428 | 12.619618 | 12.220856 | 11.689 | 12.418589 | 12.395855 | 13.541899 | 11.789926 |
1807.07950 | Keshav Dasgupta | Alina Czajka, Keshav Dasgupta, Charles Gale, Sangyong Jeon, Aalok
Misra, Michael Richard, Karunava Sil | On Bulk Viscosity at Weak and Strong 't Hooft Couplings | 18 pages, 3 figures, Companion paper | null | null | null | hep-th cond-mat.str-el hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Bulk viscosity is an important transport coefficient that exists in the
hydrodynamical limit only when the underlying theory is non-conformal. One
example being thermal QCD with large number of colors. We study bulk viscosity
in such a theory at low energies and at weak and strong 't Hooft couplings when
the temperat... | [
{
"created": "Fri, 20 Jul 2018 17:44:18 GMT",
"version": "v1"
}
] | 2018-07-23 | [
[
"Czajka",
"Alina",
""
],
[
"Dasgupta",
"Keshav",
""
],
[
"Gale",
"Charles",
""
],
[
"Jeon",
"Sangyong",
""
],
[
"Misra",
"Aalok",
""
],
[
"Richard",
"Michael",
""
],
[
"Sil",
"Karunava",
""
]
] | Bulk viscosity is an important transport coefficient that exists in the hydrodynamical limit only when the underlying theory is non-conformal. One example being thermal QCD with large number of colors. We study bulk viscosity in such a theory at low energies and at weak and strong 't Hooft couplings when the temperatur... | 9.874285 | 9.352479 | 9.978807 | 9.290129 | 9.677479 | 9.136475 | 9.264855 | 8.853943 | 8.863982 | 10.39398 | 9.145474 | 9.057591 | 9.772591 | 9.417207 | 9.54999 | 9.19508 | 9.546642 | 9.27803 | 9.237915 | 9.818641 | 9.08312 |
1011.6109 | K.B. Alkalaev | K.B. Alkalaev | FV-type action for AdS(5) mixed-symmetry fields | 48 pages; v2: typos corrected, comments and references added | JHEP 1103:031,2011 | 10.1007/JHEP03(2011)031 | FIAN-TD-2010-09 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formulate Fradkin-Vasiliev type theory of massless higher spin fields in
AdS(5). The corresponding action functional describes cubic order approximation
to gravitational interactions of bosonic mixed-symmetry fields of a particular
"hook" symmetry type and totally symmetric bosonic and fermionic fields.
| [
{
"created": "Mon, 29 Nov 2010 00:11:59 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jan 2011 13:03:57 GMT",
"version": "v2"
}
] | 2011-03-18 | [
[
"Alkalaev",
"K. B.",
""
]
] | We formulate Fradkin-Vasiliev type theory of massless higher spin fields in AdS(5). The corresponding action functional describes cubic order approximation to gravitational interactions of bosonic mixed-symmetry fields of a particular "hook" symmetry type and totally symmetric bosonic and fermionic fields. | 19.66785 | 14.389255 | 23.553717 | 14.564798 | 19.021357 | 15.425111 | 17.148478 | 12.443528 | 14.337538 | 26.605963 | 13.474556 | 14.197677 | 19.871014 | 14.506295 | 15.339092 | 14.646449 | 13.74073 | 15.453186 | 14.664552 | 19.952097 | 13.539086 |
1703.00278 | Simon Caron-Huot | Simon Caron-Huot | Analyticity in Spin in Conformal Theories | 33+12 pages, 6 figures. Typos fixed, published version | null | 10.1007/JHEP09(2017)078 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Conformal theory correlators are characterized by the spectrum and three-
point functions of local operators. We present a formula which extracts this
data as an analytic function of spin. In analogy with a classic formula due to
Froissart and Gribov, it is sensitive only to an "imaginary part" which appears
after an... | [
{
"created": "Wed, 1 Mar 2017 13:06:18 GMT",
"version": "v1"
},
{
"created": "Sat, 3 Mar 2018 22:37:26 GMT",
"version": "v2"
}
] | 2018-03-06 | [
[
"Caron-Huot",
"Simon",
""
]
] | Conformal theory correlators are characterized by the spectrum and three- point functions of local operators. We present a formula which extracts this data as an analytic function of spin. In analogy with a classic formula due to Froissart and Gribov, it is sensitive only to an "imaginary part" which appears after anal... | 16.405195 | 18.467321 | 19.274729 | 15.274096 | 16.243723 | 16.458939 | 16.039427 | 16.034157 | 15.187389 | 20.355738 | 14.719627 | 15.179255 | 16.146765 | 15.609523 | 15.410966 | 15.353226 | 14.971375 | 15.544238 | 14.98875 | 16.381729 | 14.945904 |
hep-th/0302225 | Santiago Esteban Perez Bergliaffa | M. Novello, S. E. Perez Bergliaffa, and R. P. Neves | Causality and charged spin-2 fields in an electromagnetic background | 6 pages, RevTex4, minor changes following hep-th/0304050 and
gr-qc/0304041, conclusions unchanged | null | null | null | hep-th | null | We show that, contrary to common belief, the propagation of a spin-2 field in
an electromagnetic background is {\em causal}. The proof will be given in the
Fierz formalism which, as we shall see, is free of the ambiguity present in the
more usual Einstein representation. We shall also review the proof in this
latter ... | [
{
"created": "Fri, 28 Feb 2003 14:07:56 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Apr 2003 17:25:35 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Novello",
"M.",
""
],
[
"Bergliaffa",
"S. E. Perez",
""
],
[
"Neves",
"R. P.",
""
]
] | We show that, contrary to common belief, the propagation of a spin-2 field in an electromagnetic background is {\em causal}. The proof will be given in the Fierz formalism which, as we shall see, is free of the ambiguity present in the more usual Einstein representation. We shall also review the proof in this latter re... | 14.087852 | 12.931925 | 9.82229 | 10.22047 | 10.379375 | 11.415241 | 12.088297 | 11.387064 | 10.453085 | 11.665564 | 11.857366 | 12.283806 | 11.096108 | 11.049424 | 12.049294 | 11.700206 | 12.033599 | 11.27582 | 11.72412 | 10.793802 | 11.431796 |
1202.2458 | Sumit Das | Sumit R. Das and K. Sengupta | Non-equilibrium Dynamics of O(N) Nonlinear Sigma models: a Large-N
approach | 22 pages, 9 figures. Typos corrected, references rearranged and
added.v3 : sections rearranged, abstract modified, comment about Kibble-Zurek
scaling corrected | null | 10.1007/JHEP09(2012)072 | UK-12-02 | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the time evolution of the mass gap of the O(N) non-linear sigma
model in 2+1 dimensions due to a time-dependent coupling in the large-$N$
limit. Using the Schwinger-Keldysh approach, we derive a set of equations at
large $N$ which determine the time dependent gap in terms of the coupling.
These equations lea... | [
{
"created": "Sat, 11 Feb 2012 18:30:29 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Feb 2012 20:07:03 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Aug 2012 17:34:32 GMT",
"version": "v3"
}
] | 2015-06-04 | [
[
"Das",
"Sumit R.",
""
],
[
"Sengupta",
"K.",
""
]
] | We study the time evolution of the mass gap of the O(N) non-linear sigma model in 2+1 dimensions due to a time-dependent coupling in the large-$N$ limit. Using the Schwinger-Keldysh approach, we derive a set of equations at large $N$ which determine the time dependent gap in terms of the coupling. These equations lead ... | 6.467838 | 6.63926 | 7.016782 | 6.551882 | 6.801669 | 6.883314 | 6.941602 | 6.625096 | 6.671122 | 7.148083 | 6.355172 | 6.195279 | 6.41994 | 6.251812 | 6.426005 | 6.363007 | 6.261314 | 6.250442 | 6.279737 | 6.404072 | 6.32992 |
1403.7567 | Pierre Martinetti | Agostino Devastato, Fedele Lizzi, Pierre Martinetti | Higgs mass in Noncommutative Geometry | Proceedings of the Corfou Workshop on noncommutative field theory and
gravity, september 2013 | Fortschritte der Physik 2014 | 10.1002/prop.201400013 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the noncommutative geometry approach to the standard model, an extra
scalar field - initially suggested by particle physicist to stabilize the
electroweak vacuum - makes the computation of the Higgs mass compatible with
the 126 GeV experimental value. We give a brief account on how to generate this
field from the ... | [
{
"created": "Fri, 28 Mar 2014 23:17:45 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Apr 2014 23:02:32 GMT",
"version": "v2"
}
] | 2016-01-20 | [
[
"Devastato",
"Agostino",
""
],
[
"Lizzi",
"Fedele",
""
],
[
"Martinetti",
"Pierre",
""
]
] | In the noncommutative geometry approach to the standard model, an extra scalar field - initially suggested by particle physicist to stabilize the electroweak vacuum - makes the computation of the Higgs mass compatible with the 126 GeV experimental value. We give a brief account on how to generate this field from the Ma... | 9.889321 | 8.181717 | 10.396708 | 8.654436 | 8.364639 | 6.936805 | 8.177896 | 8.993885 | 8.640818 | 9.871543 | 8.087822 | 8.718045 | 9.483928 | 8.594272 | 8.751415 | 8.379397 | 8.699739 | 8.778419 | 9.098236 | 9.135983 | 8.464181 |
hep-th/9707247 | null | Soonkeon Nam, Kyungho Oh, Sang-Jin Sin | Superpotentials of N=1 Supersymmetric Gauge Theories from M-theory | 15pages, latex, typos corrected, a line regarding M\"obius
transformation in page 4 and angle dependence in page 12 corrected | Phys.Lett.B416:319-326,1998 | 10.1016/S0370-2693(97)01250-1 | SNUTP/97-106 | hep-th | null | We consider brane configurations in M-theory describing N=1 supersymmetric
gauge theories and using the parametric representation of the brane
configurations, we calculate the superpotentials for various cases including
multiple gauge groups or fermions. For SU(n) N=1 SQCD with $N_f$ fermion case
($N_f < N_c)$, we fi... | [
{
"created": "Wed, 30 Jul 1997 14:24:05 GMT",
"version": "v1"
},
{
"created": "Sun, 31 Aug 1997 07:31:29 GMT",
"version": "v2"
}
] | 2010-02-05 | [
[
"Nam",
"Soonkeon",
""
],
[
"Oh",
"Kyungho",
""
],
[
"Sin",
"Sang-Jin",
""
]
] | We consider brane configurations in M-theory describing N=1 supersymmetric gauge theories and using the parametric representation of the brane configurations, we calculate the superpotentials for various cases including multiple gauge groups or fermions. For SU(n) N=1 SQCD with $N_f$ fermion case ($N_f < N_c)$, we find... | 10.772995 | 10.334556 | 11.385118 | 10.165644 | 10.133847 | 10.003921 | 11.287512 | 10.099144 | 10.251564 | 12.99239 | 10.060387 | 10.590956 | 11.043712 | 10.594625 | 10.704119 | 10.807344 | 10.271714 | 10.634656 | 10.798326 | 10.882415 | 10.012707 |
1711.00450 | Volodymyr Gorkavenko | Yurii A. Sitenko, Volodymyr M. Gorkavenko | Non-Euclidean geometry, nontrivial topology and quantum vacuum effects | 13 pages, minor changes, misprints eliminated | Universe 2018, 4, 23 | 10.3390/universe4020023 | null | hep-th cond-mat.mtrl-sci cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Space out of a topological defect of the Abrikosov-Nielsen-Olesen vortex type
is locally flat but non-Euclidean. If a spinor field is quantized in such a
space, then a variety of quantum effects is induced in the vacuum. Basing on
the continuum model for long-wavelength electronic excitations, originating in
the tigh... | [
{
"created": "Wed, 1 Nov 2017 17:31:06 GMT",
"version": "v1"
},
{
"created": "Sat, 27 Jan 2018 17:14:36 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Apr 2018 08:46:04 GMT",
"version": "v3"
},
{
"created": "Thu, 24 May 2018 12:39:44 GMT",
"version": "v4"
}
] | 2018-05-25 | [
[
"Sitenko",
"Yurii A.",
""
],
[
"Gorkavenko",
"Volodymyr M.",
""
]
] | Space out of a topological defect of the Abrikosov-Nielsen-Olesen vortex type is locally flat but non-Euclidean. If a spinor field is quantized in such a space, then a variety of quantum effects is induced in the vacuum. Basing on the continuum model for long-wavelength electronic excitations, originating in the tight-... | 10.555457 | 11.072811 | 10.347942 | 10.353693 | 11.332833 | 11.199031 | 11.275476 | 11.13122 | 10.622337 | 11.627863 | 10.465206 | 10.390249 | 10.410036 | 10.167959 | 10.686232 | 10.239719 | 10.279154 | 10.600537 | 10.106813 | 10.250516 | 10.024549 |
1612.00042 | Andrzej Rostworowski | Andrzej Rostworowski | Comment on "AdS nonlinear instability: moving beyond spherical symmetry"
[Class. Quantum Grav. 33 23LT01 (2016)] | 1 page, v2: missing $\theta$ dependence in eqs. (3,4) added | Class. Quantum Grav. 34 (2017) 128001 | 10.1088/1361-6382/aa71cc | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that if the degeneracy of the spectrum of linear perturbations of
AdS is properly taken into account, there are globally regular, time-periodic,
asymptotically AdS solutions (geons) bifurcating from each linear
eigenfrequency of AdS.
| [
{
"created": "Wed, 30 Nov 2016 21:35:16 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Mar 2017 10:32:21 GMT",
"version": "v2"
}
] | 2017-06-02 | [
[
"Rostworowski",
"Andrzej",
""
]
] | We argue that if the degeneracy of the spectrum of linear perturbations of AdS is properly taken into account, there are globally regular, time-periodic, asymptotically AdS solutions (geons) bifurcating from each linear eigenfrequency of AdS. | 10.181476 | 8.69056 | 9.101711 | 8.075055 | 9.387089 | 9.008864 | 8.704425 | 8.326019 | 9.288634 | 9.742275 | 9.342958 | 8.834184 | 9.025414 | 8.54942 | 8.980127 | 8.53895 | 8.611447 | 8.801 | 9.304763 | 9.363882 | 8.651865 |
1104.5397 | James Allen | James P Allen and Douglas J Smith | Coupling M2-branes to background fields | 20 pages, no figures | JHEP 1108:078,2011 | 10.1007/JHEP08(2011)078 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss some of the issues arising in trying to extend the ABJM action to
include couplings to background fields. This is analogous to the
Myers-Chern-Simons terms of the multiple Dp-brane action. We review and extend
previous results to include terms which are quadratic in the background fields.
These are fixed b... | [
{
"created": "Thu, 28 Apr 2011 14:08:12 GMT",
"version": "v1"
}
] | 2011-08-25 | [
[
"Allen",
"James P",
""
],
[
"Smith",
"Douglas J",
""
]
] | We discuss some of the issues arising in trying to extend the ABJM action to include couplings to background fields. This is analogous to the Myers-Chern-Simons terms of the multiple Dp-brane action. We review and extend previous results to include terms which are quadratic in the background fields. These are fixed by ... | 11.505365 | 10.15555 | 12.283574 | 9.881614 | 11.796209 | 10.008911 | 10.143526 | 10.909827 | 9.573802 | 13.323124 | 10.076886 | 10.006201 | 10.768099 | 9.921723 | 10.080795 | 9.986364 | 9.82012 | 9.913324 | 9.852302 | 10.934756 | 10.182627 |
hep-th/9402156 | null | Makoto Natsuume and Joseph Polchinski | Gravitational Scattering in the c = 1 Matrix Model | 20 pages + 2 figures (included as a uufile), LaTeX | Nucl.Phys.B424:137-154,1994 | 10.1016/0550-3213(94)90092-2 | NSF-ITP-94-19 | hep-th | null | The $c=1$ matrix model is equivalent to $1+1$ dimensional string theory.
However, the tachyon self-interaction in the former is local, while in the
latter it is nonlocal due to the gravitational, dilaton and higher string
fields. By studying scattering of classical pulses we show that the appropriate
nonlocal field r... | [
{
"created": "Mon, 28 Feb 1994 23:50:00 GMT",
"version": "v1"
}
] | 2009-10-09 | [
[
"Natsuume",
"Makoto",
""
],
[
"Polchinski",
"Joseph",
""
]
] | The $c=1$ matrix model is equivalent to $1+1$ dimensional string theory. However, the tachyon self-interaction in the former is local, while in the latter it is nonlocal due to the gravitational, dilaton and higher string fields. By studying scattering of classical pulses we show that the appropriate nonlocal field red... | 11.649652 | 9.174701 | 10.825458 | 9.139293 | 9.700502 | 8.735524 | 9.20628 | 8.82788 | 8.761342 | 10.662934 | 8.574081 | 9.049035 | 10.51018 | 9.244421 | 9.083661 | 8.883808 | 8.796447 | 9.220393 | 9.376851 | 10.048476 | 8.887691 |
hep-th/0407087 | Michael T. Anderson | Michael T. Anderson | On the structure of asymptotically de Sitter and anti-de Sitter spaces | 22pp, minor changes, references added | null | null | null | hep-th gr-qc math.DG | null | We discuss several aspects of the relation between asymptotically AdS and
asymptotically dS spacetimes including: the continuation between these types of
spaces, the global stability of asymptotically dS spaces and the structure of
limits within this class, holographic renormalization, and the maximal mass
conjecture... | [
{
"created": "Mon, 12 Jul 2004 14:10:58 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Jun 2005 12:23:44 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Anderson",
"Michael T.",
""
]
] | We discuss several aspects of the relation between asymptotically AdS and asymptotically dS spacetimes including: the continuation between these types of spaces, the global stability of asymptotically dS spaces and the structure of limits within this class, holographic renormalization, and the maximal mass conjecture o... | 11.679511 | 12.29764 | 15.209747 | 10.066426 | 10.314474 | 12.219805 | 12.671891 | 12.318709 | 11.237538 | 12.778113 | 11.137506 | 11.530553 | 12.243721 | 11.472563 | 11.59949 | 11.227386 | 12.084759 | 11.29637 | 11.241163 | 12.291367 | 11.158278 |
hep-th/0211101 | Angelos Fotopoulos | A. Fotopoulos and A.A. Tseytlin | On gravitational couplings in D-brane action | 15 pages, 1 figure, LaTex JHEP style; v2: reference added, typos
corrected; v3: section 2 rewritten due to an error in gauge fixing, appendix
added, conclusions unchanged | JHEP 0212:001,2002 | 10.1088/1126-6708/2002/12/001 | Imperial/TP/02 -3/3, CPHT-RR 076.1102 | hep-th | null | We compute the two closed string graviton - two open string scalar scattering
amplitude on the disc to show that there is no second-derivative curvature -
scalar coupling term R X^2 in the low-energy effective action of a D-brane in
curved space in type II superstring theory.
| [
{
"created": "Tue, 12 Nov 2002 12:40:49 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Dec 2002 18:36:44 GMT",
"version": "v2"
},
{
"created": "Tue, 26 Oct 2004 14:38:22 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Fotopoulos",
"A.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We compute the two closed string graviton - two open string scalar scattering amplitude on the disc to show that there is no second-derivative curvature - scalar coupling term R X^2 in the low-energy effective action of a D-brane in curved space in type II superstring theory. | 14.831022 | 13.31181 | 15.21645 | 11.014821 | 15.066069 | 11.61827 | 14.116426 | 12.683983 | 12.285496 | 14.647479 | 11.491386 | 12.268421 | 12.673853 | 11.714372 | 12.363666 | 12.782522 | 12.139612 | 12.584171 | 12.125695 | 12.204911 | 12.271687 |
1512.05376 | Bert Vercnocke | Iosif Bena, Daniel R. Mayerson, Andrea Puhm and Bert Vercnocke | Tunneling into Microstate Geometries: Quantum Effects Stop Gravitational
Collapse | 26 pages + appendix | null | 10.1007/JHEP07(2016)031 | IPhT-T15/217, MCTP-15-32 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Collapsing shells form horizons, and when the curvature is small classical
general relativity is believed to describe this process arbitrarily well. On
the other hand, quantum information theory based (fuzzball/firewall) arguments
suggest the existence of some structure at the black hole horizon. This
structure can o... | [
{
"created": "Wed, 16 Dec 2015 21:12:20 GMT",
"version": "v1"
}
] | 2016-08-03 | [
[
"Bena",
"Iosif",
""
],
[
"Mayerson",
"Daniel R.",
""
],
[
"Puhm",
"Andrea",
""
],
[
"Vercnocke",
"Bert",
""
]
] | Collapsing shells form horizons, and when the curvature is small classical general relativity is believed to describe this process arbitrarily well. On the other hand, quantum information theory based (fuzzball/firewall) arguments suggest the existence of some structure at the black hole horizon. This structure can onl... | 9.317157 | 9.172468 | 9.266636 | 8.413455 | 9.091544 | 9.210748 | 9.326478 | 8.706336 | 8.662381 | 10.484837 | 8.433636 | 8.45923 | 8.755136 | 8.453176 | 8.367212 | 8.465174 | 8.223007 | 8.528852 | 8.327578 | 9.019629 | 8.47881 |
1506.03723 | Carlo Maccaferri | Carlo Maccaferri, Martin Schnabl | Large BCFT moduli in open string field theory | 14 pages, 3 figures. v2: minor notation improvements, version
published in JHEP | JHEP 1508:149,2015 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the recently constructed solution for marginal deformations by one of
the authors, to analytically relate the BCFT modulus (lambda_BCFT) to the
coefficient of the boundary marginal field in the solution (lambda_SFT). We
explicitly find that the relation is not one to one and the same value of
lambda_SFT corres... | [
{
"created": "Thu, 11 Jun 2015 16:02:35 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Sep 2015 13:35:23 GMT",
"version": "v2"
}
] | 2015-09-04 | [
[
"Maccaferri",
"Carlo",
""
],
[
"Schnabl",
"Martin",
""
]
] | We use the recently constructed solution for marginal deformations by one of the authors, to analytically relate the BCFT modulus (lambda_BCFT) to the coefficient of the boundary marginal field in the solution (lambda_SFT). We explicitly find that the relation is not one to one and the same value of lambda_SFT correspo... | 10.576735 | 9.742972 | 11.450816 | 9.9917 | 10.075625 | 9.638331 | 9.746983 | 10.384288 | 8.780838 | 11.621142 | 9.373997 | 9.287911 | 10.372057 | 9.533857 | 9.117314 | 9.279484 | 9.23346 | 9.40345 | 9.40903 | 10.438749 | 8.966977 |
0911.0043 | Joao Penedones | Lorenzo Cornalba, Miguel S. Costa, Joao Penedones | Deep Inelastic Scattering in Conformal QCD | 44+16 pages, 7 figures. Some corrections | JHEP 1003:133,2010 | 10.1007/JHEP03(2010)133 | CERN-PH-TH/2009-185, NSF-KITP-09-193 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the Regge limit of a CFT correlation function of two vector and
two scalar operators, as appropriate to study small-x deep inelastic scattering
in N=4 SYM or in QCD assuming approximate conformal symmetry. After clarifying
the nature of the Regge limit for a CFT correlator, we use its conformal
partial wa... | [
{
"created": "Sun, 1 Nov 2009 02:24:12 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jan 2010 22:19:36 GMT",
"version": "v2"
}
] | 2010-04-08 | [
[
"Cornalba",
"Lorenzo",
""
],
[
"Costa",
"Miguel S.",
""
],
[
"Penedones",
"Joao",
""
]
] | We consider the Regge limit of a CFT correlation function of two vector and two scalar operators, as appropriate to study small-x deep inelastic scattering in N=4 SYM or in QCD assuming approximate conformal symmetry. After clarifying the nature of the Regge limit for a CFT correlator, we use its conformal partial wave... | 6.159592 | 7.249469 | 7.199494 | 6.534959 | 7.421436 | 7.64373 | 7.368334 | 7.354406 | 6.365016 | 7.318773 | 6.999232 | 6.779308 | 6.696159 | 6.616282 | 6.812767 | 6.873461 | 6.646087 | 6.824597 | 6.454616 | 6.686241 | 6.533811 |
1607.01922 | David Berenstein | David Berenstein, Alexandra Miller | Logarithmic enhancements in conformal perturbation theory and their real
time interpretation | 20 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study various corrections of correlation functions to leading order in
conformal perturbation theory, both on the cylinder and on the plane. Many
problems on the cylinder are mathematically equivalent to those in the plane if
we give the perturbations a position dependent scaling profile. The integrals
to be done ... | [
{
"created": "Thu, 7 Jul 2016 08:52:03 GMT",
"version": "v1"
}
] | 2016-07-08 | [
[
"Berenstein",
"David",
""
],
[
"Miller",
"Alexandra",
""
]
] | We study various corrections of correlation functions to leading order in conformal perturbation theory, both on the cylinder and on the plane. Many problems on the cylinder are mathematically equivalent to those in the plane if we give the perturbations a position dependent scaling profile. The integrals to be done ar... | 13.060466 | 13.07372 | 13.750486 | 13.140693 | 12.573161 | 13.009443 | 13.26874 | 13.599329 | 13.25448 | 16.011131 | 12.691639 | 12.530504 | 13.225148 | 12.362348 | 12.435056 | 12.304502 | 12.524753 | 12.386738 | 12.471087 | 13.423707 | 12.273708 |
hep-th/9612244 | Chaiho Rim | Chaiho Rim | Fermion Ground State of Three Particles in a Harmonic Potential Well and
Its Anyon Interpolation | RevTex, 11pages | J.KoreanPhys.Soc.29:559-562,1996 | null | SNUTP/96-052 | hep-th | null | We examine the detail of the analytic structure of an exact analytic solution
of three anyons, which interpolates to the fermion ground state in a harmonic
potential well. The analysis is done on the fundamental domain with appropriate
boundary conditions. Some remarks on the hard-core conditions and
self-adjointness... | [
{
"created": "Sat, 28 Dec 1996 04:07:54 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Rim",
"Chaiho",
""
]
] | We examine the detail of the analytic structure of an exact analytic solution of three anyons, which interpolates to the fermion ground state in a harmonic potential well. The analysis is done on the fundamental domain with appropriate boundary conditions. Some remarks on the hard-core conditions and self-adjointness a... | 22.11408 | 16.267683 | 20.41227 | 16.319832 | 17.024324 | 17.115005 | 16.693958 | 15.721534 | 15.528898 | 20.549398 | 17.802332 | 17.972551 | 19.814594 | 17.70697 | 18.142353 | 19.228306 | 18.093782 | 17.959547 | 18.065304 | 20.420847 | 18.607327 |
hep-th/9405079 | Piotr Podles | P. Kondratowicz and P. Podles | On representation theory of quantum $SL_q(2)$ groups at roots of unity | 31 pages, Section 2.7 added and other minor changes | Banach Center Publ. 40 (1997) 223-248 | null | null | hep-th math.QA | null | Irreducible representations of quantum groups $SL_q(2)$ (in Woronowicz'
approach) were classified in J.Wang, B.Parshall, Memoirs AMS 439 in the~case of
$q$ being an~odd root of unity. Here we find the~irreducible representations
for all roots of unity (also of an~even degree), as well as describe
"the~diagonal part" ... | [
{
"created": "Thu, 12 May 1994 12:26:42 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Jun 1994 11:11:46 GMT",
"version": "v2"
},
{
"created": "Sun, 21 Jan 1996 03:31:14 GMT",
"version": "v3"
}
] | 2008-02-03 | [
[
"Kondratowicz",
"P.",
""
],
[
"Podles",
"P.",
""
]
] | Irreducible representations of quantum groups $SL_q(2)$ (in Woronowicz' approach) were classified in J.Wang, B.Parshall, Memoirs AMS 439 in the~case of $q$ being an~odd root of unity. Here we find the~irreducible representations for all roots of unity (also of an~even degree), as well as describe "the~diagonal part" of... | 10.474182 | 11.974467 | 12.495441 | 11.125949 | 12.457768 | 12.452152 | 11.330953 | 13.032484 | 10.426721 | 13.47329 | 10.929465 | 10.447203 | 10.765506 | 9.994919 | 10.208057 | 9.9807 | 10.025379 | 10.156257 | 9.864635 | 10.379092 | 10.14825 |
1108.4158 | S. Q. Wu | Shuang-Qing Wu | Two-charged non-extremal rotating black holes in seven-dimensional
gauged supergravity: The single-rotation case | 13 pages, elsarticle.cls, revised version with two typos removed and
three references added | Phys. Lett. B 705 (2011) 383-387 | 10.1016/j.physletb.2011.10.026 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the solution for non-extremal charged rotating black holes in
seven-dimensional gauged supergravity, in the case with only one rotation
parameter and two independent charges. Using the Boyer-Lindquist coordinates,
the metric is expressed in a generalized form of the ansatz previously
presented in [S.Q. W... | [
{
"created": "Sun, 21 Aug 2011 02:57:06 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Aug 2011 01:49:27 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Oct 2011 04:34:43 GMT",
"version": "v3"
}
] | 2011-11-01 | [
[
"Wu",
"Shuang-Qing",
""
]
] | We construct the solution for non-extremal charged rotating black holes in seven-dimensional gauged supergravity, in the case with only one rotation parameter and two independent charges. Using the Boyer-Lindquist coordinates, the metric is expressed in a generalized form of the ansatz previously presented in [S.Q. Wu,... | 7.730879 | 7.173748 | 7.799767 | 6.671453 | 8.138706 | 7.486701 | 7.974719 | 7.139633 | 6.951282 | 8.468616 | 7.453555 | 7.521986 | 7.735136 | 7.457897 | 7.641684 | 7.515471 | 7.815133 | 7.680099 | 7.838433 | 7.871579 | 7.639851 |
1407.4275 | Javier Matulich | Glenn Barnich, Laura Donnay, Javier Matulich, Ricardo Troncoso | Asymptotic symmetries and dynamics of three-dimensional flat
supergravity | 13 pages, no figures | null | 10.1007/JHEP08(2014)071 | CECS-PHY-14/02 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A consistent set of asymptotic conditions for the simplest supergravity
theory without cosmological constant in three dimensions is proposed. The
canonical generators associated to the asymptotic symmetries are shown to span
a supersymmetric extension of the BMS$_3$ algebra with an appropriate central
charge. The ene... | [
{
"created": "Wed, 16 Jul 2014 12:20:24 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Barnich",
"Glenn",
""
],
[
"Donnay",
"Laura",
""
],
[
"Matulich",
"Javier",
""
],
[
"Troncoso",
"Ricardo",
""
]
] | A consistent set of asymptotic conditions for the simplest supergravity theory without cosmological constant in three dimensions is proposed. The canonical generators associated to the asymptotic symmetries are shown to span a supersymmetric extension of the BMS$_3$ algebra with an appropriate central charge. The energ... | 8.037251 | 6.445305 | 7.745663 | 6.69143 | 6.74437 | 6.956247 | 6.875592 | 6.845807 | 6.758116 | 7.764401 | 6.74084 | 6.852121 | 7.402256 | 6.94487 | 7.282 | 6.813725 | 6.94597 | 7.025347 | 7.158674 | 7.22154 | 6.972885 |
hep-th/0312181 | Kenichiro Aoki | Kenichiro Aoki, Eric D'Hoker and D.H. Phong | Two-Loop Superstrings on Orbifold Compactifications | Corrected typos; added refs | Nucl.Phys. B688 (2004) 3-69 | 10.1016/j.nuclphysb.2004.04.001 | null | hep-th math.CV | null | The two-loop chiral measure for superstring theories compactified on $\bZ_2$
reflection orbifolds is constructed from first principles for even spin
structures. This is achieved by a careful implementation of the chiral
splitting procedure in the twisted sectors and the identification of a subtle
worldsheet supersymm... | [
{
"created": "Tue, 16 Dec 2003 10:51:10 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Mar 2004 02:50:17 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Aoki",
"Kenichiro",
""
],
[
"D'Hoker",
"Eric",
""
],
[
"Phong",
"D. H.",
""
]
] | The two-loop chiral measure for superstring theories compactified on $\bZ_2$ reflection orbifolds is constructed from first principles for even spin structures. This is achieved by a careful implementation of the chiral splitting procedure in the twisted sectors and the identification of a subtle worldsheet supersymmet... | 11.0804 | 11.039526 | 12.229446 | 11.176866 | 11.025194 | 10.657279 | 11.832103 | 11.064752 | 11.00641 | 14.117691 | 11.042806 | 10.753315 | 11.667583 | 10.960964 | 10.695497 | 10.909156 | 11.016449 | 10.835379 | 11.16853 | 11.344994 | 10.688435 |
hep-th/0408003 | A. D. Alhaidari | A. D. Alhaidari | Spinor superalgebra: Towards a theory for higher spin particles | 16 pages | null | null | null | hep-th | null | We define a superalgebra S2(N/2) as a Z2 graded algebra of dimension 2N+3,
where N is a positive, odd integer. The even component is a three-dimensional
abelian subalgebra, while the odd component is made up of two N-dimensional,
mutually conjugate algebras. For N = 1, two of the three even elements become
identical,... | [
{
"created": "Sat, 31 Jul 2004 17:18:48 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Alhaidari",
"A. D.",
""
]
] | We define a superalgebra S2(N/2) as a Z2 graded algebra of dimension 2N+3, where N is a positive, odd integer. The even component is a three-dimensional abelian subalgebra, while the odd component is made up of two N-dimensional, mutually conjugate algebras. For N = 1, two of the three even elements become identical, r... | 7.373872 | 7.895125 | 7.847814 | 7.612413 | 7.964307 | 7.640274 | 8.159553 | 7.501442 | 7.581614 | 7.865467 | 7.069003 | 7.302303 | 7.310431 | 7.024055 | 7.159404 | 7.025128 | 7.170611 | 7.030322 | 7.082328 | 7.178947 | 7.113953 |
2103.06666 | Meer Ashwinkumar | Meer Ashwinkumar, Lennart Schmidt, Meng-Chwan Tan | Matrix Quantization of Classical Nambu Brackets and Super $p$-Branes | 36 pages. Updated title and refined presentation. Published in JHEP | JHEP 07 (2021) 172 | 10.1007/JHEP07(2021)172 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an explicit matrix algebra quantization of the algebra of
volume-preserving diffeomorphisms of the $n$-torus. That is, we approximate the
corresponding classical Nambu brackets using
$\mathfrak{sl}(N^{\lceil\frac{n}{2}\rceil},\mathbb{C})$-matrices equipped with
the finite bracket given by the completely an... | [
{
"created": "Thu, 11 Mar 2021 13:44:57 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Jul 2021 12:29:03 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Jan 2022 18:11:05 GMT",
"version": "v3"
}
] | 2022-08-02 | [
[
"Ashwinkumar",
"Meer",
""
],
[
"Schmidt",
"Lennart",
""
],
[
"Tan",
"Meng-Chwan",
""
]
] | We present an explicit matrix algebra quantization of the algebra of volume-preserving diffeomorphisms of the $n$-torus. That is, we approximate the corresponding classical Nambu brackets using $\mathfrak{sl}(N^{\lceil\frac{n}{2}\rceil},\mathbb{C})$-matrices equipped with the finite bracket given by the completely anti... | 7.057048 | 8.280361 | 8.120901 | 7.465287 | 7.509999 | 6.863031 | 7.526286 | 7.168893 | 6.957523 | 8.621832 | 6.875762 | 6.631478 | 7.151558 | 6.641405 | 6.723285 | 6.744722 | 6.517046 | 6.567426 | 6.792521 | 7.172047 | 6.58187 |
hep-th/0111147 | Chung | Ding-Yu Chung | The Periodic Table of Elementary Particles and the Composition of
Hadrons | 32 pages, 13 tables, 6 figures | null | null | null | hep-th | null | All leptons, quarks, and gauge bosons can be placed in the periodic table of
elementary particles. As the periodic table of elements derived from atomic
orbital, the periodic table of elementary particles is derived from the two
sets of seven orbitals: principal dimensional orbital and auxiliary dimensional
orbital. ... | [
{
"created": "Thu, 15 Nov 2001 22:55:27 GMT",
"version": "v1"
},
{
"created": "Sat, 17 Nov 2001 12:22:28 GMT",
"version": "v2"
},
{
"created": "Tue, 27 Nov 2001 21:33:17 GMT",
"version": "v3"
},
{
"created": "Thu, 15 May 2003 02:08:30 GMT",
"version": "v4"
},
{
"c... | 2016-09-06 | [
[
"Chung",
"Ding-Yu",
""
]
] | All leptons, quarks, and gauge bosons can be placed in the periodic table of elementary particles. As the periodic table of elements derived from atomic orbital, the periodic table of elementary particles is derived from the two sets of seven orbitals: principal dimensional orbital and auxiliary dimensional orbital. (S... | 8.005638 | 9.226218 | 8.503391 | 8.528391 | 8.709079 | 10.177901 | 9.777185 | 8.744599 | 8.72022 | 8.787458 | 8.981765 | 8.262383 | 8.165147 | 8.191781 | 8.054209 | 8.125335 | 8.253971 | 8.108189 | 8.204749 | 8.209706 | 8.217565 |
hep-th/0503025 | Sonia P. Paban | C. Krishnan, S. Paban and M. Zanic | Evolution of Gravitationally Unstable de Sitter Compactifications | 11 pages, 8 figures; references added, typos corrected and figure 5
replaced | JHEP 0505 (2005) 045 | 10.1088/1126-6708/2005/05/045 | UTTG-03-05 | hep-th | null | We study the time evolution of unstable $dS_p$ \times $S^q$ configurations
with flux in theories of gravity with a cosmological constant. For certain
values of the flux, we identify a stable configuration to which these unstable
solutions flow. For other values of the flux the sphere wants to decompactify,
regardless... | [
{
"created": "Wed, 2 Mar 2005 21:26:56 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Apr 2005 17:38:21 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Krishnan",
"C.",
""
],
[
"Paban",
"S.",
""
],
[
"Zanic",
"M.",
""
]
] | We study the time evolution of unstable $dS_p$ \times $S^q$ configurations with flux in theories of gravity with a cosmological constant. For certain values of the flux, we identify a stable configuration to which these unstable solutions flow. For other values of the flux the sphere wants to decompactify, regardless o... | 15.084446 | 13.704496 | 15.533327 | 13.217394 | 12.922339 | 14.895481 | 11.786016 | 12.418268 | 12.294403 | 16.608709 | 12.3172 | 12.714999 | 14.459231 | 13.006249 | 13.352383 | 13.103484 | 12.643576 | 12.079124 | 13.165121 | 14.978076 | 11.877888 |
1103.2454 | Ryo Saotome | Ratindranath Akhoury, David Garfinkle, Ryo Saotome and Alexander
Vikman | Non-Stationary Dark Energy Around a Black Hole | 8 pages, 10 figures | Phys.Rev.D83:084034,2011 | 10.1103/PhysRevD.83.084034 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Numerical simulations of the accretion of test scalar fields with
non-standard kinetic terms (of the k-essence type) onto a Schwarzschild black
hole are performed. We find a full dynamical solution for the spherical
accretion of a Dirac-Born-Infeld type scalar field. The simulations show that
the accretion eventually... | [
{
"created": "Sat, 12 Mar 2011 15:54:15 GMT",
"version": "v1"
}
] | 2011-07-22 | [
[
"Akhoury",
"Ratindranath",
""
],
[
"Garfinkle",
"David",
""
],
[
"Saotome",
"Ryo",
""
],
[
"Vikman",
"Alexander",
""
]
] | Numerical simulations of the accretion of test scalar fields with non-standard kinetic terms (of the k-essence type) onto a Schwarzschild black hole are performed. We find a full dynamical solution for the spherical accretion of a Dirac-Born-Infeld type scalar field. The simulations show that the accretion eventually s... | 8.634977 | 8.069029 | 7.429914 | 7.996119 | 8.546264 | 8.606016 | 9.242459 | 8.184739 | 8.00236 | 8.453977 | 8.539483 | 8.171052 | 7.808266 | 7.758809 | 7.623539 | 8.061278 | 8.159369 | 8.201775 | 7.850791 | 7.992201 | 8.149613 |
1001.3046 | Adel Rezaei-Aghdam | S. Hajizadeh and A. Rezaei-Aghdam | Poisson-Lie sigma models over low dimensional real Poisson-Lie groups | 12 pages, 1 tables | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Poisson-Lie sigma models over nonsemisimple low dimensional real
Poisson-Lie groups are investigated. We find two sided models on two, three and
some four dimensional Poisson-Lie groups where the Poisson-Lie sigma models
over Poisson-Lie groups G and its dual $\tilde{G}$ are topological sigma models
or BF gauge m... | [
{
"created": "Mon, 18 Jan 2010 12:56:07 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Jul 2010 13:16:49 GMT",
"version": "v2"
},
{
"created": "Tue, 18 Oct 2011 08:52:15 GMT",
"version": "v3"
}
] | 2011-10-19 | [
[
"Hajizadeh",
"S.",
""
],
[
"Rezaei-Aghdam",
"A.",
""
]
] | The Poisson-Lie sigma models over nonsemisimple low dimensional real Poisson-Lie groups are investigated. We find two sided models on two, three and some four dimensional Poisson-Lie groups where the Poisson-Lie sigma models over Poisson-Lie groups G and its dual $\tilde{G}$ are topological sigma models or BF gauge mod... | 13.820622 | 12.976184 | 13.216244 | 11.282273 | 12.718716 | 15.202565 | 12.299909 | 14.093347 | 11.936768 | 18.472563 | 12.786403 | 13.619439 | 12.952161 | 13.109496 | 13.350377 | 13.582489 | 14.028894 | 12.760264 | 12.909031 | 12.839789 | 12.34166 |
1606.06601 | Silvio Paolo Sorella | M. A. L. Capri, D. Fiorentini, M. S. Guimaraes, B. W. Mintz, L. F.
Palhares, S. P. Sorella | A local and renormalizable framework for the gauge-invariant operator
$A^2_{\min}$ in Euclidean Yang-Mills theories in linear covariant gauges | 35 pages; v2: ref. added | Phys. Rev. D 94, 065009 (2016) | 10.1103/PhysRevD.94.065009 | null | hep-th hep-lat hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We address the issue of the renormalizability of the gauge-invariant
non-local dimension-two operator $A^2_{\rm min}$, whose minimization is defined
along the gauge orbit. Despite its non-local character, we show that the
operator $A^2_{\rm min}$ can be cast in local form through the introduction of
an auxiliary Stue... | [
{
"created": "Tue, 21 Jun 2016 14:39:31 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jun 2016 23:36:42 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Jul 2016 12:29:27 GMT",
"version": "v3"
}
] | 2016-09-14 | [
[
"Capri",
"M. A. L.",
""
],
[
"Fiorentini",
"D.",
""
],
[
"Guimaraes",
"M. S.",
""
],
[
"Mintz",
"B. W.",
""
],
[
"Palhares",
"L. F.",
""
],
[
"Sorella",
"S. P.",
""
]
] | We address the issue of the renormalizability of the gauge-invariant non-local dimension-two operator $A^2_{\rm min}$, whose minimization is defined along the gauge orbit. Despite its non-local character, we show that the operator $A^2_{\rm min}$ can be cast in local form through the introduction of an auxiliary Stueck... | 4.771987 | 4.75019 | 4.751058 | 4.739887 | 4.671643 | 4.634403 | 4.522121 | 4.61548 | 4.559311 | 5.022575 | 4.453161 | 4.53699 | 4.734134 | 4.470077 | 4.505303 | 4.366203 | 4.397904 | 4.375138 | 4.581728 | 4.7898 | 4.448986 |
0705.0983 | Masaki Shigemori | Joseph Marsano, Kyriakos Papadodimas and Masaki Shigemori | Nonsupersymmetric Brane/Antibrane Configurations in Type IIA and M
Theory | 84 pages (57 pages + 4 appendices), 18 figures | Nucl.Phys.B789:294-361,2008 | 10.1016/j.nuclphysb.2007.08.010 | CALT-68-2644, ITFA-2007-15 | hep-th | null | We study metastable nonsupersymmetric configurations in type IIA string
theory, obtained by suspending D4-branes and anti-D4-branes between
holomorphically curved NS5's, which are related to those of hep-th/0610249 by
T-duality. When the numbers of branes and antibranes are the same, we are able
to obtain an exact M ... | [
{
"created": "Mon, 7 May 2007 21:13:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Marsano",
"Joseph",
""
],
[
"Papadodimas",
"Kyriakos",
""
],
[
"Shigemori",
"Masaki",
""
]
] | We study metastable nonsupersymmetric configurations in type IIA string theory, obtained by suspending D4-branes and anti-D4-branes between holomorphically curved NS5's, which are related to those of hep-th/0610249 by T-duality. When the numbers of branes and antibranes are the same, we are able to obtain an exact M th... | 11.141381 | 11.427342 | 12.472108 | 10.28935 | 11.124624 | 10.687654 | 11.528801 | 10.585924 | 10.260201 | 13.146699 | 10.607621 | 10.981231 | 11.156567 | 10.66266 | 10.854408 | 10.688879 | 10.681007 | 10.780734 | 10.535522 | 11.433949 | 10.57592 |
hep-th/0201162 | Vitor Cardoso | Vitor Cardoso, Jose' P. S. Lemos | Scalar Synchrotron Radiation in the Schwarzschild-anti-de Sitter
Geometry | 13 pages, 6 figures, published version. References added | Phys.Rev. D65 (2002) 104033 | 10.1103/PhysRevD.65.104033 | null | hep-th astro-ph gr-qc hep-ph | null | We present a complete relativistic analysis for the scalar radiation emitted
by a particle in circular orbit around a Schwarzschild-anti-de Sitter black
hole. If the black hole is large, then the radiation is concentrated in narrow
angles- high multipolar distribution- i.e., the radiation is synchrotronic.
However, s... | [
{
"created": "Mon, 21 Jan 2002 10:55:50 GMT",
"version": "v1"
},
{
"created": "Sat, 18 May 2002 14:02:27 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Cardoso",
"Vitor",
""
],
[
"Lemos",
"Jose' P. S.",
""
]
] | We present a complete relativistic analysis for the scalar radiation emitted by a particle in circular orbit around a Schwarzschild-anti-de Sitter black hole. If the black hole is large, then the radiation is concentrated in narrow angles- high multipolar distribution- i.e., the radiation is synchrotronic. However, sma... | 8.494077 | 9.17805 | 7.963228 | 7.836872 | 8.962759 | 8.255607 | 8.446292 | 7.767653 | 8.26491 | 9.289179 | 8.000698 | 8.130388 | 7.563275 | 7.787806 | 7.907408 | 7.966877 | 7.790454 | 7.665155 | 7.726296 | 7.610769 | 7.696072 |
hep-th/0010265 | Fedor Gubarev | M.N.Chernodub, F.V.Gubarev, M.I.Polikarpov, V.I.Zakharov | Towards Abelian-like formulation of the dual gluodynamics | 28+1 pp., Latex2e, 1 figure | Nucl.Phys. B600 (2001) 163-184 | 10.1016/S0550-3213(01)00011-6 | ITEP-TH-28/00 | hep-th hep-lat hep-ph | null | We consider gluodynamics in case when both color and magnetic charges are
present. We discuss first short distance physics, where only the fundamental
|Q|=1 monopoles introduced via the `t Hooft loop can be considered
consistently. We show that at short distances the external monopoles interact
as pure Abelian object... | [
{
"created": "Sat, 28 Oct 2000 08:43:12 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Chernodub",
"M. N.",
""
],
[
"Gubarev",
"F. V.",
""
],
[
"Polikarpov",
"M. I.",
""
],
[
"Zakharov",
"V. I.",
""
]
] | We consider gluodynamics in case when both color and magnetic charges are present. We discuss first short distance physics, where only the fundamental |Q|=1 monopoles introduced via the `t Hooft loop can be considered consistently. We show that at short distances the external monopoles interact as pure Abelian objects.... | 14.154394 | 14.489307 | 13.703856 | 13.354748 | 15.365088 | 14.596916 | 13.701523 | 15.559369 | 12.787704 | 14.838799 | 13.854768 | 13.949015 | 13.689801 | 13.911562 | 14.144315 | 13.645643 | 13.605082 | 14.305937 | 13.45218 | 14.054444 | 13.69621 |
2207.02831 | Eduardo Garc\'ia-Valdecasas Tenreiro | Jeremias Aguilera Damia, Riccardo Argurio, Eduardo Garcia-Valdecasas | Non-Invertible Defects in 5d, Boundaries and Holography | v3: Journal Version | SciPost Phys. 14, 067 (2023) | 10.21468/SciPostPhys.14.4.067 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that very simple theories of abelian gauge fields with a cubic
Chern-Simons term in 5d have an infinite number of non-invertible co-dimension
two defects. They arise by dressing the symmetry operators of the broken
electric 1-form symmetry with a suitable topological field theory, for any
rational angle. We f... | [
{
"created": "Wed, 6 Jul 2022 17:40:00 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Sep 2022 16:59:15 GMT",
"version": "v2"
},
{
"created": "Tue, 10 Jan 2023 11:58:52 GMT",
"version": "v3"
}
] | 2023-04-12 | [
[
"Damia",
"Jeremias Aguilera",
""
],
[
"Argurio",
"Riccardo",
""
],
[
"Garcia-Valdecasas",
"Eduardo",
""
]
] | We show that very simple theories of abelian gauge fields with a cubic Chern-Simons term in 5d have an infinite number of non-invertible co-dimension two defects. They arise by dressing the symmetry operators of the broken electric 1-form symmetry with a suitable topological field theory, for any rational angle. We fur... | 12.274475 | 12.303536 | 13.929427 | 11.521085 | 12.44781 | 11.592504 | 11.758875 | 10.54875 | 10.919999 | 15.159168 | 11.460483 | 11.324206 | 12.526538 | 11.092223 | 11.298034 | 10.995013 | 11.117895 | 11.94692 | 11.412545 | 12.659388 | 11.127468 |
hep-th/0001205 | Ken Intriligator | Kenneth Intriligator | Anomaly Matching and a Hopf-Wess-Zumino Term in 6d, N=(2,0) Field
Theories | 19 pages; v2:expanded discussion of skyrmionic strings | Nucl.Phys. B581 (2000) 257-273 | 10.1016/S0550-3213(00)00148-6 | UCSD/PTH 00-02 | hep-th | null | We point out that the low energy theory of 6d, N=(2,0) field theories, when
away from the origin of the moduli space of vacua, necessarily includes a new
kind of Wess-Zumino term. The form of this term is related to the Hopf
invariant associated with \pi_7 (S^4). The coefficient of the Wess-Zumino term
is fixed by an... | [
{
"created": "Fri, 28 Jan 2000 23:34:35 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Mar 2000 20:08:04 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Intriligator",
"Kenneth",
""
]
] | We point out that the low energy theory of 6d, N=(2,0) field theories, when away from the origin of the moduli space of vacua, necessarily includes a new kind of Wess-Zumino term. The form of this term is related to the Hopf invariant associated with \pi_7 (S^4). The coefficient of the Wess-Zumino term is fixed by an a... | 8.572103 | 8.687014 | 9.471833 | 7.991086 | 8.407557 | 8.40836 | 8.374739 | 8.397301 | 8.475829 | 10.201242 | 7.995325 | 8.049066 | 8.429363 | 8.213404 | 8.089611 | 8.124918 | 8.119844 | 8.465556 | 8.006536 | 8.767305 | 7.817008 |
0909.5430 | Raman Sundrum | Raman Sundrum | SUSY Splits, But Then Returns | 29 pages. Flavor and CP constraints on left-right symmetric structure
briefly discussed. References added | JHEP 1101:062,2011 | 10.1007/JHEP01(2011)062 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the phenomenon of accidental or "emergent" supersymmetry within
gauge theory and connect it to the scenarios of Split Supersymmetry and Higgs
compositeness. Combining these elements leads to a significant refinement and
extension of the proposal of Partial Supersymmetry, in which supersymmetry is
broken at v... | [
{
"created": "Tue, 29 Sep 2009 20:08:41 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Nov 2010 13:41:49 GMT",
"version": "v2"
}
] | 2011-03-04 | [
[
"Sundrum",
"Raman",
""
]
] | We study the phenomenon of accidental or "emergent" supersymmetry within gauge theory and connect it to the scenarios of Split Supersymmetry and Higgs compositeness. Combining these elements leads to a significant refinement and extension of the proposal of Partial Supersymmetry, in which supersymmetry is broken at ver... | 11.77054 | 13.129531 | 11.907465 | 11.640664 | 11.736526 | 13.292782 | 12.456642 | 12.661645 | 11.627078 | 11.972716 | 11.852921 | 11.489134 | 11.520165 | 11.489467 | 11.787733 | 11.887218 | 11.407697 | 11.472325 | 11.32227 | 11.576779 | 11.463879 |
1507.03005 | Martin Heinze | Martin Heinze | Spectrum and Quantum Symmetries of the ${\rm AdS}_5 \times {\rm S}^5$
Superstring | 168 pages, PhD thesis of the author; v2: typos corrected, references
updated | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The the duality between ${\cal N}=4$ SYM and the AdS$_5\times\;$S$^5$
superstring appears to enjoy quantum integrability in the planar limit, which
allowed to devise powerful methods ostensibly solving the spectral problem.
However, quantization of the AdS$_5\times\;$S$^5$ superstring from first
principles is still a... | [
{
"created": "Fri, 10 Jul 2015 19:50:45 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Nov 2016 10:59:23 GMT",
"version": "v2"
}
] | 2016-11-08 | [
[
"Heinze",
"Martin",
""
]
] | The the duality between ${\cal N}=4$ SYM and the AdS$_5\times\;$S$^5$ superstring appears to enjoy quantum integrability in the planar limit, which allowed to devise powerful methods ostensibly solving the spectral problem. However, quantization of the AdS$_5\times\;$S$^5$ superstring from first principles is still an ... | 8.205338 | 8.387409 | 8.886058 | 7.96841 | 8.107586 | 8.701366 | 8.387619 | 8.228267 | 8.143873 | 9.471032 | 8.216544 | 8.107214 | 8.518242 | 8.048235 | 8.207221 | 8.157675 | 8.208941 | 8.112841 | 8.033243 | 8.638118 | 8.199511 |
0912.0616 | Giuseppe De Risi | G. De Risi | Induced cosmology on a codimension-2 brane in a conical bulk | 14 pages, 1 figure. Corrections and clarifications troughout the
text. Match the published version on NPB | Nucl.Phys.B845:246-256,2011 | 10.1016/j.nuclphysb.2010.12.006 | BA-TH 620-09 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the cosmology of a 5-dimensional brane, which represents a
regularization of a 4-dimensional codimension-2 brane, embedded in a conical
bulk. The brane is assumed to be tensional, and to contain a curvature term.
Cosmology is obtained by letting the brane move trough the bulk, and
implementing dynamical junc... | [
{
"created": "Thu, 3 Dec 2009 10:11:47 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jan 2011 11:19:27 GMT",
"version": "v2"
}
] | 2011-01-17 | [
[
"De Risi",
"G.",
""
]
] | We study the cosmology of a 5-dimensional brane, which represents a regularization of a 4-dimensional codimension-2 brane, embedded in a conical bulk. The brane is assumed to be tensional, and to contain a curvature term. Cosmology is obtained by letting the brane move trough the bulk, and implementing dynamical juncti... | 9.506206 | 7.724412 | 9.361744 | 8.654834 | 9.329398 | 8.719052 | 8.790803 | 7.794822 | 8.688176 | 10.408363 | 8.77134 | 8.657661 | 8.921249 | 8.578097 | 9.065873 | 8.756926 | 9.141995 | 8.414725 | 9.017639 | 8.791459 | 8.602305 |
1302.3630 | Tomer Shacham | Tomer Shacham | A Non-Renormalization Theorem in Gapped Quantum Field Theory | 9 pages, v2: typos corrected, discussion added | null | 10.1007/JHEP05(2013)147 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the two-point functions of the U(1) current and energy-momentum
tensor in certain gapped three-dimensional field theories, and show that the
parity-odd part in both of these correlation functions is one-loop exact. In
particular, we find a new and simplified derivation of the Coleman-Hill theorem
that also... | [
{
"created": "Thu, 14 Feb 2013 21:14:03 GMT",
"version": "v1"
},
{
"created": "Sun, 26 May 2013 08:25:12 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"Shacham",
"Tomer",
""
]
] | We discuss the two-point functions of the U(1) current and energy-momentum tensor in certain gapped three-dimensional field theories, and show that the parity-odd part in both of these correlation functions is one-loop exact. In particular, we find a new and simplified derivation of the Coleman-Hill theorem that also c... | 8.232568 | 7.105273 | 8.502025 | 7.147029 | 7.290503 | 7.389213 | 7.776586 | 7.038249 | 7.066022 | 8.903497 | 7.741567 | 7.827127 | 8.508707 | 7.515079 | 7.900321 | 7.975295 | 7.72073 | 7.853895 | 7.663249 | 8.12213 | 7.896786 |
1503.07410 | Ruggero Ferrari | Ruggero Ferrari | Managing $\gamma_5$ in Dimensional Regularization II: the Trace with
more $\gamma_5$ | 21 pages LaTex, no figures | null | 10.1007/s10773-016-3211-8 | MIT-CTP4643 March 2015 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper we evaluate the anomaly for the abelian axial current in
a non abelian chiral gauge theory, by using dimensional regularization. This
amount to formulate a procedure for managing traces with more than one
$\gamma_5$. \par The suggested procedure obeys Lorentz covariance and
cyclicity, at variance... | [
{
"created": "Wed, 25 Mar 2015 15:04:32 GMT",
"version": "v1"
}
] | 2016-12-21 | [
[
"Ferrari",
"Ruggero",
""
]
] | In the present paper we evaluate the anomaly for the abelian axial current in a non abelian chiral gauge theory, by using dimensional regularization. This amount to formulate a procedure for managing traces with more than one $\gamma_5$. \par The suggested procedure obeys Lorentz covariance and cyclicity, at variance w... | 11.655441 | 11.905622 | 11.86252 | 11.092577 | 13.036232 | 12.217996 | 11.978905 | 11.896477 | 11.447374 | 12.455069 | 11.037508 | 11.375396 | 11.470613 | 11.040423 | 11.288147 | 11.52517 | 11.477285 | 11.17099 | 11.275242 | 11.680243 | 11.155793 |
1002.0062 | Ioannis Bakas | Ioannis Bakas, Francois Bourliot, Dieter Lust, Marios Petropoulos | Geometric flows in Horava-Lifshitz gravity | 67 pages, 16 figures; more solutions found, 1 extra figure, 1 more
reference added in v2; minor typos corrected in v3 (to appear in JHEP); an
acknowledgement added in v4 | null | 10.1007/JHEP04(2010)131 | CPHT-RR078.0709, MPP-2009-179, LMU-ASC 47/09 | hep-th gr-qc math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider instanton solutions of Euclidean Horava-Lifshitz gravity in four
dimensions satisfying the detailed balance condition. They are described by
geometric flows in three dimensions driven by certain combinations of the
Cotton and Ricci tensors as well as the cosmological-constant term. The
deformation curvatu... | [
{
"created": "Sat, 30 Jan 2010 11:56:00 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Feb 2010 20:20:12 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Apr 2010 17:01:12 GMT",
"version": "v3"
},
{
"created": "Thu, 7 Apr 2011 08:53:57 GMT",
"version": "v4"
}
] | 2015-05-18 | [
[
"Bakas",
"Ioannis",
""
],
[
"Bourliot",
"Francois",
""
],
[
"Lust",
"Dieter",
""
],
[
"Petropoulos",
"Marios",
""
]
] | We consider instanton solutions of Euclidean Horava-Lifshitz gravity in four dimensions satisfying the detailed balance condition. They are described by geometric flows in three dimensions driven by certain combinations of the Cotton and Ricci tensors as well as the cosmological-constant term. The deformation curvature... | 10.280695 | 10.836621 | 11.345829 | 9.820197 | 10.874966 | 11.016769 | 10.404679 | 10.009713 | 10.582484 | 12.565943 | 10.061743 | 10.297502 | 10.744023 | 10.068793 | 10.065327 | 10.423457 | 10.055555 | 10.167944 | 10.20098 | 10.81247 | 10.208006 |
hep-th/9912262 | Katsumi Itoh | Yuji Igarashi, Katsumi Itoh and Hiroto So | Exact Symmetries realized on the Renormalized Group Flow | Latex, 10 pages | Phys.Lett. B479 (2000) 336-342 | 10.1016/S0370-2693(00)00305-1 | NIIG-DP-99-2 | hep-th | null | We show that symmetries are preserved exactly along the (Wilsonian)
renormalization group flow, though the IR cutoff deforms concrete forms of the
transformations. For a gauge theory the cutoff dependent Ward-Takahashi
identity is written as the master equation in the antifield formalism: one may
read off the renorma... | [
{
"created": "Tue, 28 Dec 1999 09:59:02 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Jan 2000 13:02:02 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Igarashi",
"Yuji",
""
],
[
"Itoh",
"Katsumi",
""
],
[
"So",
"Hiroto",
""
]
] | We show that symmetries are preserved exactly along the (Wilsonian) renormalization group flow, though the IR cutoff deforms concrete forms of the transformations. For a gauge theory the cutoff dependent Ward-Takahashi identity is written as the master equation in the antifield formalism: one may read off the renormali... | 12.930226 | 12.624294 | 14.610275 | 12.075096 | 12.319214 | 12.807741 | 12.57172 | 11.564765 | 11.671824 | 13.889331 | 12.08197 | 12.5461 | 12.751459 | 12.268567 | 12.324584 | 12.03479 | 12.783549 | 12.046002 | 12.559224 | 13.280149 | 12.174309 |
1107.3334 | Giovanni Amelino-Camelia | Giovanni Amelino-Camelia, Leonardo Barcaroli, Niccol\'o Loret | Modeling transverse relative locality | LaTex, 13 pages | null | 10.1007/s10773-012-1216-5 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate some aspects of relativistic classical theories with "relative
locality", in which pairs of events established to be coincident by nearby
observers may be described as non-coincident by distant observers. While
previous studies focused mainly on the case of longitudinal relative locality,
where the eff... | [
{
"created": "Sun, 17 Jul 2011 21:01:25 GMT",
"version": "v1"
}
] | 2012-09-20 | [
[
"Amelino-Camelia",
"Giovanni",
""
],
[
"Barcaroli",
"Leonardo",
""
],
[
"Loret",
"Niccoló",
""
]
] | We investigate some aspects of relativistic classical theories with "relative locality", in which pairs of events established to be coincident by nearby observers may be described as non-coincident by distant observers. While previous studies focused mainly on the case of longitudinal relative locality, where the effec... | 8.00952 | 9.295916 | 9.421633 | 8.184206 | 9.037459 | 9.289487 | 9.554548 | 8.690011 | 8.791097 | 9.506505 | 8.62138 | 8.31895 | 8.522346 | 8.115967 | 8.103143 | 8.363491 | 8.087712 | 8.348245 | 8.308335 | 8.768119 | 8.029058 |
hep-th/9601015 | Dirk Schlingemann | Dirk Schlingemann | On the Algebraic Theory of Soliton and Antisoliton Sectors | 33pp, latex2e. to appear in Rev. Math. Phys | Rev.Math.Phys. 8 (1996) 301-326 | 10.1142/S0129055X96000111 | DESY 95-012 | hep-th | null | We consider the properties of massive one particle states on a translation
covariant Haag-Kastler net in Minkowski space. In two dimensional theories,
these states can be interpreted as soliton states and we are interested in the
existence of antisolitons. It is shown that for each soliton state there are
three diffe... | [
{
"created": "Fri, 5 Jan 1996 09:51:34 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Schlingemann",
"Dirk",
""
]
] | We consider the properties of massive one particle states on a translation covariant Haag-Kastler net in Minkowski space. In two dimensional theories, these states can be interpreted as soliton states and we are interested in the existence of antisolitons. It is shown that for each soliton state there are three differe... | 9.67073 | 11.041619 | 10.212079 | 9.395265 | 8.603924 | 9.951113 | 10.150009 | 10.194267 | 9.156595 | 11.710381 | 10.416925 | 9.748202 | 10.064329 | 9.477582 | 9.425845 | 9.649341 | 9.266961 | 9.782849 | 9.827529 | 9.95687 | 9.469966 |
2005.08471 | Takuya Kanazawa | Takuya Kanazawa | Chiral random matrix theory for colorful quark-antiquark condensates | 9 pages, 1 figure | Phys. Rev. D 102, 014002 (2020) | 10.1103/PhysRevD.102.014002 | null | hep-th hep-lat hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In QCD at high density, the color-octet quark-antiquark condensate
$\langle\overline\psi\gamma_0(\lambda^A)_C (\lambda^A)_F\psi\rangle$ is
generally nonzero and dynamically breaks the $\mathrm{SU}(3)_C\times
\mathrm{SU}(3)_L\times\mathrm{SU}(3)_R$ symmetry down to the diagonal
$\mathrm{SU}(3)_V$. We evaluate this con... | [
{
"created": "Mon, 18 May 2020 06:17:30 GMT",
"version": "v1"
}
] | 2020-07-02 | [
[
"Kanazawa",
"Takuya",
""
]
] | In QCD at high density, the color-octet quark-antiquark condensate $\langle\overline\psi\gamma_0(\lambda^A)_C (\lambda^A)_F\psi\rangle$ is generally nonzero and dynamically breaks the $\mathrm{SU}(3)_C\times \mathrm{SU}(3)_L\times\mathrm{SU}(3)_R$ symmetry down to the diagonal $\mathrm{SU}(3)_V$. We evaluate this conde... | 5.364846 | 6.141619 | 5.437672 | 5.260558 | 6.350271 | 6.131685 | 5.959954 | 5.394194 | 5.064045 | 5.857337 | 5.679507 | 5.476147 | 5.200481 | 5.304698 | 5.551461 | 5.541589 | 5.646799 | 5.373683 | 5.368206 | 5.400099 | 5.199012 |
1511.05991 | Catherine Whiting A | Leopoldo A. Pando Zayas, Vincent G. J. Rodgers and Catherine A.
Whiting | Supergravity Solutions with $AdS_4$ from Non-Abelian T-Dualities | 50 pages | null | null | MCTP-15-19 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a large class of new backgrounds that are solutions of type II
supergravity with a warped AdS${}_4$ factor, non-trivial axion-dilaton,
B-field, and three- and five-form Ramond-Ramond fluxes. We obtain these
solutions by applying non-Abelian T-dualities with respect to SU(2) or
SU(2)/U(1) isometries to redu... | [
{
"created": "Wed, 18 Nov 2015 21:46:12 GMT",
"version": "v1"
},
{
"created": "Sat, 5 Dec 2015 14:54:51 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Jan 2016 20:39:44 GMT",
"version": "v3"
}
] | 2016-01-28 | [
[
"Zayas",
"Leopoldo A. Pando",
""
],
[
"Rodgers",
"Vincent G. J.",
""
],
[
"Whiting",
"Catherine A.",
""
]
] | We present a large class of new backgrounds that are solutions of type II supergravity with a warped AdS${}_4$ factor, non-trivial axion-dilaton, B-field, and three- and five-form Ramond-Ramond fluxes. We obtain these solutions by applying non-Abelian T-dualities with respect to SU(2) or SU(2)/U(1) isometries to reduct... | 5.14641 | 5.247174 | 6.704399 | 4.794408 | 5.258158 | 5.10427 | 5.015116 | 5.159578 | 5.089734 | 7.105027 | 5.037909 | 4.870319 | 5.579676 | 4.912069 | 4.840552 | 4.972779 | 4.865234 | 5.02142 | 4.898486 | 5.827198 | 4.919673 |
hep-th/9411144 | Vyjayanthi Chari | V. Chari | Minimal Affinizations of Representations of quantum groups: the
U_q(g)--module structure | 17 pages | null | null | null | hep-th math.QA q-alg | null | We describe the underlying U_q(g)--module structure of representations of
quantum affine algebras.
| [
{
"created": "Fri, 18 Nov 1994 21:23:52 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Chari",
"V.",
""
]
] | We describe the underlying U_q(g)--module structure of representations of quantum affine algebras. | 35.493073 | 15.672201 | 37.436432 | 19.110086 | 21.517136 | 13.501681 | 19.404726 | 12.232097 | 19.203302 | 36.753239 | 17.338966 | 16.496899 | 39.188053 | 21.56698 | 17.894114 | 18.748102 | 18.471813 | 18.909557 | 21.118383 | 35.045929 | 18.385214 |
hep-th/9912261 | Takao Suyama | Takao Suyama | Intersecting Branes and Generalized Vortices | 10 pages | null | null | OU-HET-339 | hep-th | null | We construct the effective theory of intersecting branes and investigate the
BPS monopoles in the theory. The monopoles obtained are the generalization of
Nielsen-Olesen vortex. We study the properties of the solutions and interpret
them as the D0-branes on the brane-intersections.
| [
{
"created": "Tue, 28 Dec 1999 09:46:59 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Suyama",
"Takao",
""
]
] | We construct the effective theory of intersecting branes and investigate the BPS monopoles in the theory. The monopoles obtained are the generalization of Nielsen-Olesen vortex. We study the properties of the solutions and interpret them as the D0-branes on the brane-intersections. | 10.178514 | 8.410148 | 9.933947 | 7.887541 | 8.057656 | 7.070889 | 7.874603 | 8.486207 | 7.821344 | 11.365715 | 8.036613 | 8.218042 | 9.269506 | 8.512081 | 8.420921 | 8.167168 | 8.113557 | 8.58596 | 8.33787 | 9.201095 | 8.084597 |
1706.04925 | Radu Tatar | Radu Tatar | From N=2 in four dimensions to (0,2) in two dimensions | 18 Pages, Latex, v2 references added | Phys. Rev. D 96, 066022 (2017) | 10.1103/PhysRevD.96.066022 | LTH/1135 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider N=2 four dimensional field theories compactified on a two torus
in the presence of a U(1) magnetic field. We discuss the restrictions leading
to theories with (2,2) supersymmetry or (0,2) supersymmetry in two dimensions.
The field theories live on D5 branes wrapped on four cycles of Calabi-Yau
3-folds or ... | [
{
"created": "Thu, 15 Jun 2017 15:26:07 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jul 2017 10:23:04 GMT",
"version": "v2"
}
] | 2017-09-27 | [
[
"Tatar",
"Radu",
""
]
] | We consider N=2 four dimensional field theories compactified on a two torus in the presence of a U(1) magnetic field. We discuss the restrictions leading to theories with (2,2) supersymmetry or (0,2) supersymmetry in two dimensions. The field theories live on D5 branes wrapped on four cycles of Calabi-Yau 3-folds or 4-... | 6.366398 | 5.858123 | 7.440588 | 5.630999 | 5.722639 | 5.823383 | 6.142088 | 6.083687 | 5.826528 | 7.763221 | 6.069453 | 6.022295 | 6.915316 | 5.983333 | 6.099049 | 5.931619 | 5.934153 | 6.06456 | 6.036714 | 6.84143 | 5.894825 |
hep-th/0509158 | Michael Ratz | Oscar Loaiza-Brito, Johannes Martin, Hans Peter Nilles, Michael Ratz | log(M_Pl/m_3/2) | Based on talks given at PLANCK05, Trieste, Italy and PASCOS05,
Gyeongju, Korea | null | 10.1063/1.2149698 | null | hep-th hep-ph | null | Flux compactifications of string theory seem to require the presence of a
fine-tuned constant in the superpotential. We discuss a scheme where this
constant is replaced by a dynamical quantity which we argue to be a `continuous
Chern--Simons term'. In such a scheme, the gaugino condensate generates the
hierarchically... | [
{
"created": "Tue, 20 Sep 2005 20:08:27 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Loaiza-Brito",
"Oscar",
""
],
[
"Martin",
"Johannes",
""
],
[
"Nilles",
"Hans Peter",
""
],
[
"Ratz",
"Michael",
""
]
] | Flux compactifications of string theory seem to require the presence of a fine-tuned constant in the superpotential. We discuss a scheme where this constant is replaced by a dynamical quantity which we argue to be a `continuous Chern--Simons term'. In such a scheme, the gaugino condensate generates the hierarchically s... | 7.295578 | 7.763672 | 7.31425 | 6.847628 | 7.030557 | 7.490863 | 7.358551 | 7.362221 | 6.699443 | 7.311321 | 6.790303 | 6.857533 | 6.781843 | 6.932374 | 6.843277 | 6.978254 | 6.870717 | 6.924078 | 6.837431 | 7.329126 | 6.909659 |
2201.03931 | Ladislav Hlavaty | Ladislav Hlavaty | Compatibility of Poisson--Lie transformations with symmetries of
Generalized Supergravity Equations | Published version | Eur. Phys. J. C (2022) 82:1070 | 10.1140/epjc/s10052-022-11042-0 | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | We investigate two types of transformations that keep NS-NS Generalized
Supergravity Equations satisfied : $\chi$-symmetry that shifts dilaton and
gauge transformations that change both dilaton and vector field $J$. Due to
these symmetries there is a large set of dilatons and vector fields $J$ that
(for a fixed metri... | [
{
"created": "Tue, 11 Jan 2022 13:15:54 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Dec 2022 11:36:00 GMT",
"version": "v2"
}
] | 2022-12-12 | [
[
"Hlavaty",
"Ladislav",
""
]
] | We investigate two types of transformations that keep NS-NS Generalized Supergravity Equations satisfied : $\chi$-symmetry that shifts dilaton and gauge transformations that change both dilaton and vector field $J$. Due to these symmetries there is a large set of dilatons and vector fields $J$ that (for a fixed metric ... | 14.759408 | 14.353503 | 15.629148 | 13.18353 | 14.984619 | 14.162334 | 16.11237 | 13.297032 | 13.390936 | 14.859851 | 14.338428 | 14.318101 | 13.774734 | 14.206738 | 15.204309 | 14.558389 | 13.664014 | 13.731989 | 14.178202 | 14.153547 | 14.066067 |
hep-th/0112192 | Laura Andrianopoli | L. Andrianopoli, R. D'Auria, S. Ferrara | Consistent reduction of N=2 -> N=1 four dimensional supergravity coupled
to matter | LaTeX, 16 pages | Nucl.Phys. B628 (2002) 387-403 | 10.1016/S0550-3213(02)00090-1 | null | hep-th | null | We analyze the constraints which follow both on the geometry and on the gauge
sector for a consistent supergravity reduction of a general matter-coupled N=2
supergravity theory in four dimensions. These constraints can be derived in an
elegant way by looking at the fermionic sector of the theory.
| [
{
"created": "Thu, 20 Dec 2001 13:21:05 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Andrianopoli",
"L.",
""
],
[
"D'Auria",
"R.",
""
],
[
"Ferrara",
"S.",
""
]
] | We analyze the constraints which follow both on the geometry and on the gauge sector for a consistent supergravity reduction of a general matter-coupled N=2 supergravity theory in four dimensions. These constraints can be derived in an elegant way by looking at the fermionic sector of the theory. | 10.037756 | 8.205956 | 9.56772 | 8.784484 | 8.898011 | 8.100736 | 8.44376 | 8.777215 | 8.779825 | 9.584446 | 8.601272 | 9.009483 | 9.579363 | 9.012524 | 9.240961 | 9.102233 | 9.169535 | 9.204794 | 8.653068 | 9.152695 | 8.977545 |
1612.01306 | Johannes Kriel Dr. | J.N. Kriel, H.W. Groenewald and F.G. Scholtz | Scattering in three-dimensional fuzzy space | 12 pages, 6 figures | null | 10.1103/PhysRevD.95.025003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop scattering theory in a non-commutative space defined by a $su(2)$
coordinate algebra. By introducing a positive operator valued measure as a
replacement for strong position measurements, we are able to derive explicit
expressions for the probability current, differential and total cross-sections.
We show t... | [
{
"created": "Mon, 5 Dec 2016 11:03:04 GMT",
"version": "v1"
}
] | 2017-02-01 | [
[
"Kriel",
"J. N.",
""
],
[
"Groenewald",
"H. W.",
""
],
[
"Scholtz",
"F. G.",
""
]
] | We develop scattering theory in a non-commutative space defined by a $su(2)$ coordinate algebra. By introducing a positive operator valued measure as a replacement for strong position measurements, we are able to derive explicit expressions for the probability current, differential and total cross-sections. We show tha... | 8.028947 | 9.190654 | 8.566609 | 7.432175 | 8.655812 | 8.53643 | 8.317349 | 8.554854 | 7.481858 | 8.773882 | 8.08844 | 7.502653 | 7.630487 | 7.681573 | 7.649351 | 7.547705 | 7.506322 | 7.660049 | 7.6156 | 7.82882 | 7.361567 |
hep-th/9811058 | Marco Cavagli\`a | Marco Cavaglia | Geometrodynamical Formulation of Two-Dimensional Dilaton Gravity and the
Quantum Birkhoff Theorem | 6 pages, LATEX, invited talk at the 11th International Conference on
Problems of Quantum Field Theory, July 13-17, 1998, Dubna, Russia | null | null | null | hep-th gr-qc | null | General two-dimensional pure dilaton-gravity can be discussed in a unitary
way by introducing suitable field redefinitions. The new fields are directly
related to the original spacetime geometry and in the canonical picture they
generalize the well-known geometrodynamical variables used in the discussion of
the vacuu... | [
{
"created": "Fri, 6 Nov 1998 09:56:59 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Cavaglia",
"Marco",
""
]
] | General two-dimensional pure dilaton-gravity can be discussed in a unitary way by introducing suitable field redefinitions. The new fields are directly related to the original spacetime geometry and in the canonical picture they generalize the well-known geometrodynamical variables used in the discussion of the vacuum ... | 13.482149 | 9.794918 | 11.832639 | 10.403689 | 9.392707 | 9.499431 | 9.981175 | 10.424364 | 10.457427 | 11.855461 | 10.831458 | 11.625285 | 11.664954 | 11.109732 | 11.140279 | 11.62296 | 11.451783 | 11.317877 | 11.419319 | 11.365044 | 11.615899 |
1208.1699 | Ramond | Dmitry Belyaev, Patrick Hearin, and Pierre Ramond | The $\mathcal {OSP}(2,2|16)$ superconformal theory is free! | 14 pages | null | 10.1007/JHEP11(2012)078 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The SuperConformal theory in three space-time dimensions with SO(16)
$R$-symmetry, 128 bosons, and 128 fermions, cannot sustain interactions. This
result is obtained using both light-cone superspace techniques which rely on
algebraic consistency, and covariant methods which rely on SO(16) Fierz
identities which fail ... | [
{
"created": "Wed, 8 Aug 2012 15:59:40 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Belyaev",
"Dmitry",
""
],
[
"Hearin",
"Patrick",
""
],
[
"Ramond",
"Pierre",
""
]
] | The SuperConformal theory in three space-time dimensions with SO(16) $R$-symmetry, 128 bosons, and 128 fermions, cannot sustain interactions. This result is obtained using both light-cone superspace techniques which rely on algebraic consistency, and covariant methods which rely on SO(16) Fierz identities which fail to... | 17.215258 | 15.012119 | 18.144411 | 14.021918 | 15.929193 | 15.121364 | 14.213679 | 13.079466 | 13.21984 | 18.53606 | 12.898854 | 14.699568 | 15.327215 | 14.326584 | 15.868188 | 15.26777 | 15.232015 | 14.343152 | 14.097051 | 16.020731 | 14.052631 |
1001.4458 | Jos\'e Roberto Vidal Madrid | Enrique \'Alvarez, Roberto Vidal | Weyl transverse gravity (WTDiff) and the cosmological constant | 11 pages | Phys.Rev.D81:084057,2010 | 10.1103/PhysRevD.81.084057 | IFT-UAM/CSIC-10-01 FTUAM-10-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Scale invariant (transverse) gravitational theories are introduced. They are
invariant under pure metric rescalings (i.e. the matter fields are inert under
those). This symmetry forbids the presence of a cosmological constant. Those
theories are not invariant under the full set of diffeomorphisms, but only with
respe... | [
{
"created": "Mon, 25 Jan 2010 15:24:15 GMT",
"version": "v1"
}
] | 2011-01-24 | [
[
"Álvarez",
"Enrique",
""
],
[
"Vidal",
"Roberto",
""
]
] | Scale invariant (transverse) gravitational theories are introduced. They are invariant under pure metric rescalings (i.e. the matter fields are inert under those). This symmetry forbids the presence of a cosmological constant. Those theories are not invariant under the full set of diffeomorphisms, but only with respect... | 12.947999 | 10.959886 | 10.939958 | 10.893587 | 10.34448 | 12.481819 | 10.839283 | 11.549583 | 10.383743 | 12.00192 | 11.668501 | 10.615226 | 10.921786 | 10.904668 | 10.678437 | 10.770193 | 11.459193 | 10.67065 | 11.312659 | 11.050895 | 10.948708 |
1802.02968 | Loriano Bonora | L.Bonora, M. Cvitan, P. Dominis Prester, S. Giaccari, M. Paulisic, T.
Stemberga | Worldline quantization of field theory, effective actions and $L_\infty$
structure | 23 pages, several minor corrections added | null | null | SISSA/03/2018/FISI | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formulate the worldline quantization of a massive fermion model coupled to
external higher spin sources. We use the relations obtained in this way to show
that its regularized effective action is endowed with an $L_\infty$ symmetry.
The same result holds also for a massive scalar model.
| [
{
"created": "Thu, 8 Feb 2018 17:20:49 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Feb 2018 04:17:29 GMT",
"version": "v2"
},
{
"created": "Fri, 11 May 2018 07:25:21 GMT",
"version": "v3"
}
] | 2018-05-14 | [
[
"Bonora",
"L.",
""
],
[
"Cvitan",
"M.",
""
],
[
"Prester",
"P. Dominis",
""
],
[
"Giaccari",
"S.",
""
],
[
"Paulisic",
"M.",
""
],
[
"Stemberga",
"T.",
""
]
] | We formulate the worldline quantization of a massive fermion model coupled to external higher spin sources. We use the relations obtained in this way to show that its regularized effective action is endowed with an $L_\infty$ symmetry. The same result holds also for a massive scalar model. | 17.800762 | 12.57851 | 16.02062 | 13.547644 | 14.111537 | 13.772203 | 13.438655 | 12.437501 | 13.556478 | 17.648024 | 13.488618 | 13.673015 | 15.000101 | 13.819901 | 13.357547 | 13.329386 | 13.197679 | 13.398329 | 13.71509 | 14.99177 | 13.622569 |
hep-th/0506247 | Micha{\l} Spali\'nski | Michal Spalinski | Some half-BPS solutions of M-theory | Typos fixed, reference added | Phys.Lett. B634 (2006) 315-318 | 10.1016/j.physletb.2006.01.068 | null | hep-th | null | It was recently shown that half BPS-solutions of M-theory can be expressed in
terms of a single function satisfying the 3-d continuum Toda equation. In this
note half-BPS solutions corresponding to separable solutions of the Toda
equations are examined.
| [
{
"created": "Wed, 29 Jun 2005 16:01:46 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Feb 2006 12:35:24 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Spalinski",
"Michal",
""
]
] | It was recently shown that half BPS-solutions of M-theory can be expressed in terms of a single function satisfying the 3-d continuum Toda equation. In this note half-BPS solutions corresponding to separable solutions of the Toda equations are examined. | 13.253756 | 9.620994 | 13.369486 | 9.793554 | 10.680567 | 9.454357 | 8.868123 | 9.370493 | 9.522231 | 13.571259 | 9.427232 | 10.159754 | 10.535996 | 10.449594 | 9.770303 | 9.383086 | 9.469005 | 9.734165 | 10.396976 | 11.036489 | 9.760096 |
hep-th/0401038 | Keiichi Nagao | Takehiro Azuma, Subrata Bal (Kyoto U.), Keiichi Nagao, Jun Nishimura
(KEK, Tsukuba) | Nonperturbative studies of fuzzy spheres in a matrix model with the
Chern-Simons term | Latex 37 pages, 13 figures, discussion on instabilities refined,
references added, typo corrected, the final version to appear in JHEP | JHEP 0405 (2004) 005 | 10.1088/1126-6708/2004/05/005 | KUNS-1883, KEK-TH-929 | hep-th hep-lat | null | Fuzzy spheres appear as classical solutions in a matrix model obtained via
dimensional reduction of 3-dimensional Yang-Mills theory with the Chern-Simons
term. Well-defined perturbative expansion around these solutions can be
formulated even for finite matrix size, and in the case of $k$ coincident fuzzy
spheres it g... | [
{
"created": "Wed, 7 Jan 2004 16:50:45 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Feb 2004 08:50:47 GMT",
"version": "v2"
},
{
"created": "Wed, 19 May 2004 14:46:04 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Azuma",
"Takehiro",
"",
"Kyoto U."
],
[
"Bal",
"Subrata",
"",
"Kyoto U."
],
[
"Nagao",
"Keiichi",
"",
"KEK, Tsukuba"
],
[
"Nishimura",
"Jun",
"",
"KEK, Tsukuba"
]
] | Fuzzy spheres appear as classical solutions in a matrix model obtained via dimensional reduction of 3-dimensional Yang-Mills theory with the Chern-Simons term. Well-defined perturbative expansion around these solutions can be formulated even for finite matrix size, and in the case of $k$ coincident fuzzy spheres it giv... | 6.080796 | 5.809243 | 6.407943 | 5.628915 | 5.951835 | 5.766352 | 5.89211 | 5.550179 | 5.731663 | 6.949569 | 5.975139 | 5.731084 | 5.815974 | 5.626837 | 5.655381 | 5.635563 | 5.679581 | 5.616045 | 5.648068 | 5.788017 | 5.828948 |
hep-th/0006200 | Myriam Mondragon | G. German (1), A. de la Macorra (2) and M. Mondragon (2) ((1) Centro
de Ciencias Fisicas, Nat. Univ. Mexico, (2) Inst. Fisica, Nat. Univ. Mexico) | Low-scale supergravity inflation with R-symmetry | 11 pages, 3 figures; added discussion and references in section 2;
corrected Eqs. 24 and 26; minor corrections in the table and figures; one
fig. added in section 1. Accepted for publication in Physics Letters B | Phys.Lett. B494 (2000) 311-317 | 10.1016/S0370-2693(00)01212-0 | IFUNAM-FT00-02 | hep-th | null | We study a supergravity model of inflation with R-symmetry and a single
scalar field, the inflaton, slowly rolling away from the origin. The scales of
inflation can be as low as the supersymmetry breaking scale of 10^10 GeV or
even the electroweak scale of 10^3 GeV which could be relevant in the context
of theories w... | [
{
"created": "Mon, 26 Jun 2000 18:06:22 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Nov 2000 19:00:01 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"German",
"G.",
""
],
[
"de la Macorra",
"A.",
""
],
[
"Mondragon",
"M.",
""
]
] | We study a supergravity model of inflation with R-symmetry and a single scalar field, the inflaton, slowly rolling away from the origin. The scales of inflation can be as low as the supersymmetry breaking scale of 10^10 GeV or even the electroweak scale of 10^3 GeV which could be relevant in the context of theories wit... | 9.005117 | 7.393446 | 8.794171 | 7.844928 | 7.797794 | 8.263825 | 8.297001 | 8.199133 | 8.0178 | 8.251858 | 8.237956 | 8.51385 | 8.404284 | 8.329874 | 8.076013 | 8.92322 | 8.363403 | 8.189306 | 8.339397 | 8.978637 | 8.141942 |
hep-th/9703178 | Dmitri Fursaev | V.P. Frolov and D.V. Fursaev | Mechanism of Generation of Black Hole Entropy in Sakharov's Induced
Gravity | 28 pages, Latex file | Phys.Rev.D56:2212-2225,1997 | 10.1103/PhysRevD.56.2212 | Alberta-Thy 07-97 | hep-th | null | The mechanism of generation of the Bekenstein-Hawking entropy $S^{BH}$ of a
black hole in the Sakharov's induced gravity is proposed. It is suggested that
the "physical" degrees of freedom, which explain the entropy $S^{BH}$, form
only a finite subset of the standard Rindler-like modes defined outside the
black hole ... | [
{
"created": "Tue, 25 Mar 1997 21:07:15 GMT",
"version": "v1"
}
] | 2011-09-09 | [
[
"Frolov",
"V. P.",
""
],
[
"Fursaev",
"D. V.",
""
]
] | The mechanism of generation of the Bekenstein-Hawking entropy $S^{BH}$ of a black hole in the Sakharov's induced gravity is proposed. It is suggested that the "physical" degrees of freedom, which explain the entropy $S^{BH}$, form only a finite subset of the standard Rindler-like modes defined outside the black hole ho... | 6.136557 | 6.502512 | 6.016072 | 5.941888 | 6.335491 | 6.345035 | 6.147092 | 6.23938 | 5.864632 | 6.658744 | 5.95787 | 6.167349 | 5.936626 | 5.926147 | 5.980007 | 6.012142 | 6.068582 | 6.028726 | 5.978071 | 6.031806 | 5.994008 |
1311.2940 | Gim Seng Ng | Tatsuo Azeyanagi, R. Loganayagam, Gim Seng Ng and Maria J. Rodriguez | Holographic Thermal Helicity | 20 pages + 47 pages of appendices ; v2: minor corrections | null | 10.1007/JHEP08(2014)040 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the thermal helicity, defined in arXiv:1211.3850, of a conformal
field theory with anomalies in the context of AdS$_{2n+1}$/CFT$_{2n}$. To do
so, we consider large charged rotating AdS black holes in the
Einstein-Maxwell-Chern-Simons theory with a negative cosmological constant
using fluid/gravity expansion.... | [
{
"created": "Tue, 12 Nov 2013 21:00:06 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jul 2014 18:37:21 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Azeyanagi",
"Tatsuo",
""
],
[
"Loganayagam",
"R.",
""
],
[
"Ng",
"Gim Seng",
""
],
[
"Rodriguez",
"Maria J.",
""
]
] | We study the thermal helicity, defined in arXiv:1211.3850, of a conformal field theory with anomalies in the context of AdS$_{2n+1}$/CFT$_{2n}$. To do so, we consider large charged rotating AdS black holes in the Einstein-Maxwell-Chern-Simons theory with a negative cosmological constant using fluid/gravity expansion. W... | 10.231163 | 9.923382 | 11.130198 | 8.879154 | 9.23357 | 9.155499 | 8.431693 | 9.014197 | 8.708794 | 11.056431 | 8.613265 | 9.068162 | 9.937904 | 9.208914 | 9.031327 | 9.285167 | 9.126464 | 9.158895 | 9.022037 | 10.483796 | 8.820417 |
2403.05241 | Wolfgang M\"uck | Wolfgang M\"uck | Black Holes and Marchenko-Pastur Distribution | 24 pages, 3 figures, v2, v3: references added, small changes | Phys. Rev. D 109, 126001 (2024) | 10.1103/PhysRevD.109.126001 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The universal eigenvalue distribution characterizing the Gram matrix of
semiclassical ensembles of black hole microstates is recognized as the
Marchenko-Pastur distribution, which plays a prominent role as the universal
limit distribution in a large class of random matrix and vector models. It is
proposed that this d... | [
{
"created": "Fri, 8 Mar 2024 12:03:12 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Mar 2024 12:03:32 GMT",
"version": "v2"
},
{
"created": "Tue, 2 Apr 2024 09:13:32 GMT",
"version": "v3"
}
] | 2024-06-06 | [
[
"Mück",
"Wolfgang",
""
]
] | The universal eigenvalue distribution characterizing the Gram matrix of semiclassical ensembles of black hole microstates is recognized as the Marchenko-Pastur distribution, which plays a prominent role as the universal limit distribution in a large class of random matrix and vector models. It is proposed that this dis... | 13.4693 | 12.195101 | 13.8002 | 11.692721 | 11.687517 | 11.598821 | 11.266222 | 11.66303 | 11.166126 | 14.494452 | 11.274761 | 12.052498 | 13.148273 | 12.307521 | 11.776269 | 11.862345 | 12.136853 | 12.419994 | 12.102944 | 11.925243 | 11.577334 |
hep-th/0107082 | Paola Mosconi | P. Mosconi, G. Mussardo, V. Riva | Boundary Quantum Field Theories with Infinite Resonance States | 18 pages, 11 figures, LATEX file | Nucl.Phys. B621 (2002) 571-586 | 10.1016/S0550-3213(01)00599-5 | SISSA/54/2001/FM | hep-th | null | We extend a recent work by Mussardo and Penati on integrable quantum field
theories with a single stable particle and an infinite number of unstable
resonance states, including the presence of a boundary. The corresponding
scattering and reflection amplitudes are expressed in terms of Jacobian
elliptic functions, and... | [
{
"created": "Tue, 10 Jul 2001 16:09:32 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Mosconi",
"P.",
""
],
[
"Mussardo",
"G.",
""
],
[
"Riva",
"V.",
""
]
] | We extend a recent work by Mussardo and Penati on integrable quantum field theories with a single stable particle and an infinite number of unstable resonance states, including the presence of a boundary. The corresponding scattering and reflection amplitudes are expressed in terms of Jacobian elliptic functions, and g... | 10.02195 | 9.823733 | 11.973802 | 9.896246 | 10.936497 | 10.039264 | 9.942509 | 10.083615 | 9.716722 | 12.657426 | 10.127427 | 10.096897 | 10.239646 | 9.814224 | 10.176857 | 9.791792 | 9.708136 | 9.729864 | 9.68138 | 10.318894 | 9.711413 |
0911.1435 | Emmanuil Saridakis | Sourish Dutta, Emmanuel N. Saridakis | Observational constraints on Horava-Lifshitz cosmology | 11 pages, 6 figures, version published in JCAP | null | 10.1088/1475-7516/2010/01/013 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use observational data from Type Ia Supernovae (SNIa), Baryon Acoustic
Oscillations (BAO), and Cosmic Microwave Background (CMB), along with
requirements of Big Bang Nucleosynthesis (BBN), to constrain the cosmological
scenarios governed by Horava-Lifshitz gravity. We consider both the detailed
and non-detailed ba... | [
{
"created": "Mon, 9 Nov 2009 20:09:45 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Dec 2009 15:53:48 GMT",
"version": "v2"
}
] | 2015-05-14 | [
[
"Dutta",
"Sourish",
""
],
[
"Saridakis",
"Emmanuel N.",
""
]
] | We use observational data from Type Ia Supernovae (SNIa), Baryon Acoustic Oscillations (BAO), and Cosmic Microwave Background (CMB), along with requirements of Big Bang Nucleosynthesis (BBN), to constrain the cosmological scenarios governed by Horava-Lifshitz gravity. We consider both the detailed and non-detailed bala... | 7.264594 | 6.558616 | 6.743271 | 6.321085 | 6.818763 | 6.579597 | 6.798329 | 6.241541 | 6.500336 | 6.783806 | 6.637098 | 6.711717 | 6.563853 | 6.534036 | 6.690495 | 6.592521 | 6.733786 | 6.41718 | 6.722727 | 6.52452 | 6.752964 |
1507.05534 | David Kastor | David Kastor and Jennie Traschen | Melvin Magnetic Fluxtube/Cosmology Correspondence | 19 pages, 3 figures; v2 - references added | null | 10.1088/0264-9381/32/23/235027 | ACFI-T15-06 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore a correspondence between Melvin magnetic fluxtubes and anisotropic
cosmological solutions, which we call `Melvin cosmologies'. The correspondence
via analytic continuation provides useful information in both directions.
Solution generating techniques known on the fluxtube side can also be used for
generati... | [
{
"created": "Mon, 20 Jul 2015 15:29:31 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Aug 2015 14:52:47 GMT",
"version": "v2"
}
] | 2015-12-09 | [
[
"Kastor",
"David",
""
],
[
"Traschen",
"Jennie",
""
]
] | We explore a correspondence between Melvin magnetic fluxtubes and anisotropic cosmological solutions, which we call `Melvin cosmologies'. The correspondence via analytic continuation provides useful information in both directions. Solution generating techniques known on the fluxtube side can also be used for generating... | 11.558687 | 9.456724 | 10.902302 | 9.395161 | 10.145804 | 9.969268 | 9.902655 | 9.252869 | 9.43682 | 11.742696 | 9.618426 | 9.455822 | 10.136389 | 9.579432 | 9.656327 | 9.451891 | 9.431663 | 9.605293 | 9.719926 | 9.857695 | 9.696613 |
hep-th/0212248 | Asad Naqvi | Finn Larsen, Asad Naqvi and Seiji Terashima | Rolling Tachyons and Decaying Branes | 24 pages | JHEP 0302 (2003) 039 | 10.1088/1126-6708/2003/02/039 | MCTP-02-70, UPR-1026-T, ITFA-2002-60 | hep-th | null | We present new rolling tachyon solutions describing the classical decay of
D-branes. Our methods are simpler than those appearing in recent works, yet our
results are exact in classical string theory. The role of pressure in the decay
is studied using tachyon profiles with spatial variation. In this case the
final st... | [
{
"created": "Thu, 19 Dec 2002 20:24:26 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Feb 2003 20:43:15 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Larsen",
"Finn",
""
],
[
"Naqvi",
"Asad",
""
],
[
"Terashima",
"Seiji",
""
]
] | We present new rolling tachyon solutions describing the classical decay of D-branes. Our methods are simpler than those appearing in recent works, yet our results are exact in classical string theory. The role of pressure in the decay is studied using tachyon profiles with spatial variation. In this case the final stat... | 17.104879 | 16.359413 | 17.033735 | 14.661542 | 16.383055 | 14.610752 | 14.438539 | 14.766483 | 15.826506 | 17.620205 | 13.432332 | 15.564285 | 16.574606 | 15.420629 | 15.554559 | 15.378618 | 15.568067 | 15.036294 | 15.337969 | 16.719305 | 14.599672 |
hep-th/0207218 | Kirill A. Kazakov | Kirill A. Kazakov | Quantum Fluctuations of Effective Fields and the Correspondence
Principle | 15 pages, 3 figures, REVTeX | null | null | null | hep-th quant-ph | null | The question of Bohr correspondence in quantum field theory is considered
from a dynamical point of view. It is shown that the classical description of
particle interactions is inapplicable even in the limit of large particles'
masses because of finite quantum fluctuations of the fields produced. In
particular, it is... | [
{
"created": "Wed, 24 Jul 2002 10:18:17 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Kazakov",
"Kirill A.",
""
]
] | The question of Bohr correspondence in quantum field theory is considered from a dynamical point of view. It is shown that the classical description of particle interactions is inapplicable even in the limit of large particles' masses because of finite quantum fluctuations of the fields produced. In particular, it is f... | 7.572364 | 7.044794 | 7.364147 | 7.197758 | 6.926392 | 7.065482 | 7.459429 | 6.827558 | 6.758401 | 8.005013 | 7.273733 | 7.258208 | 7.465446 | 7.485936 | 7.275378 | 7.41237 | 7.446015 | 7.357415 | 7.298354 | 7.512087 | 7.305401 |
1002.3132 | Samir Mathur | Steven G. Avery, Borun D. Chowdhury and Samir D. Mathur | Deforming the D1D5 CFT away from the orbifold point | 30 pages, 4 figures, Latex | JHEP 1006:031,2010 | 10.1007/JHEP06(2010)031 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The D1D5 brane bound state is believed to have an `orbifold point' in its
moduli space which is the analogue of the free Yang Mills theory for the D3
brane bound state. The supergravity geometry generated by D1 and D5 branes is
described by a different point in moduli space, and in moving towards this
point we have t... | [
{
"created": "Tue, 16 Feb 2010 18:44:34 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Feb 2010 20:12:28 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Avery",
"Steven G.",
""
],
[
"Chowdhury",
"Borun D.",
""
],
[
"Mathur",
"Samir D.",
""
]
] | The D1D5 brane bound state is believed to have an `orbifold point' in its moduli space which is the analogue of the free Yang Mills theory for the D3 brane bound state. The supergravity geometry generated by D1 and D5 branes is described by a different point in moduli space, and in moving towards this point we have to ... | 10.651472 | 9.637929 | 11.614708 | 9.37581 | 10.194527 | 10.040882 | 9.975723 | 9.62986 | 9.907196 | 12.909227 | 9.888902 | 9.76404 | 10.55125 | 10.055728 | 9.878599 | 9.588135 | 10.106982 | 9.661741 | 10.040583 | 10.517259 | 10.163097 |
1809.09107 | Jesse Cresswell | Jesse C. Cresswell, Ian T. Jardine, and Amanda W. Peet | Holographic relations for OPE blocks in excited states | 22 pages. As published in JHEP | JHEP03(2019)058 | 10.1007/JHEP03(2019)058 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the holographic duality between boundary OPE blocks and geodesic
integrated bulk fields in quotients of AdS$_3$ dual to excited CFT states. The
quotient geometries exhibit non-minimal geodesics between pairs of spacelike
separated boundary points which modify the OPE block duality. We decompose OPE
blocks in... | [
{
"created": "Mon, 24 Sep 2018 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Mar 2019 14:18:20 GMT",
"version": "v2"
}
] | 2019-03-14 | [
[
"Cresswell",
"Jesse C.",
""
],
[
"Jardine",
"Ian T.",
""
],
[
"Peet",
"Amanda W.",
""
]
] | We study the holographic duality between boundary OPE blocks and geodesic integrated bulk fields in quotients of AdS$_3$ dual to excited CFT states. The quotient geometries exhibit non-minimal geodesics between pairs of spacelike separated boundary points which modify the OPE block duality. We decompose OPE blocks into... | 11.866702 | 10.046409 | 13.788608 | 10.033011 | 10.327035 | 10.738041 | 9.31359 | 10.186415 | 9.834696 | 15.662258 | 10.393433 | 10.416575 | 12.683813 | 11.391541 | 10.964082 | 11.13435 | 11.143647 | 10.994246 | 10.997113 | 12.128592 | 10.99157 |
hep-th/9406139 | Desmond Johnston | D. Johnston | A Remark on the Renormalization Group Equation for the Penner Model | LaTeX, 5 pages, LPTHE-Orsay-94-59 | Phys.Rev. D51 (1995) 2014-2017 | 10.1103/PhysRevD.51.2014 | null | hep-th | null | It is possible to extract values for critical couplings and gamma_string in
matrix models by deriving a renormalization group equation for the variation of
the of the free energy as the size N of the matrices in the theory is varied.
In this paper we derive a ``renormalization group equation'' for the Penner
model by... | [
{
"created": "Tue, 21 Jun 1994 16:59:10 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Johnston",
"D.",
""
]
] | It is possible to extract values for critical couplings and gamma_string in matrix models by deriving a renormalization group equation for the variation of the of the free energy as the size N of the matrices in the theory is varied. In this paper we derive a ``renormalization group equation'' for the Penner model by d... | 12.584455 | 10.461482 | 11.391352 | 10.126676 | 11.822944 | 10.963756 | 10.560255 | 10.085917 | 9.298036 | 11.690165 | 10.143301 | 10.151652 | 10.85283 | 9.567683 | 10.093122 | 10.211529 | 10.13519 | 10.579685 | 10.168807 | 10.537735 | 9.968637 |
hep-th/0611107 | Jerzy Lukierski | Jerzy Lukierski, (Inst. Theor. Phys. University of Wroclaw) | Quantum $\kappa$-deformations of D=4 relativistic supersymmetries | LaTeX 4 pages, aipproc style - included. To appear in Proc. of 14th
Int. Conf. on Supersymmetry and Unification of Fundamental Interactions
(SUSY'06), UC Irvine, California, June 2006; Ed. J. Feng, AIP Proc. Ser.
(2007) | AIPConf.Proc.903:546-549,2007 | 10.1063/1.2735244 | null | hep-th | null | We describe the quantum $\kappa$-deformation of super-Poincar\'{e} algebra,
with fundamental mass-like deformation parameter $\kappa$. We shall describe
the result in graded bicrossproduct basis, with classical Lorentz superalgebra
sector which includes half of the supercharges.
| [
{
"created": "Thu, 9 Nov 2006 15:02:25 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Lukierski",
"Jerzy",
""
]
] | We describe the quantum $\kappa$-deformation of super-Poincar\'{e} algebra, with fundamental mass-like deformation parameter $\kappa$. We shall describe the result in graded bicrossproduct basis, with classical Lorentz superalgebra sector which includes half of the supercharges. | 15.734163 | 12.614895 | 17.523849 | 12.240745 | 14.288999 | 13.882729 | 12.252865 | 11.158892 | 12.258563 | 16.537731 | 12.254135 | 12.908751 | 15.314741 | 13.392817 | 14.022269 | 13.603975 | 12.952612 | 13.016434 | 13.254016 | 14.80934 | 13.33692 |
1308.1222 | Rajesh Gupta | S. de Alwis, R. K. Gupta, E. Hatefi and F. Quevedo | Stability, Tunneling and Flux Changing de Sitter Transitions in the
Large Volume String Scenario | An error (equation 5.5) is corrected and references added. The main
conclusion is unchanged | JHEP11(2013)179 | 10.1007/JHEP11(2013)179 | DAMTP-2013-42 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the non-perturbative stability of the Large Volume Scenario (LVS) of
IIB string compactifications, by analysing transitions mediated by the
Brown-Teitelboim (BT) brane nucleations and by Coleman De Luccia tunneling
(CDL). We find that, as long as the effective field theory description holds,
the LVS AdS mini... | [
{
"created": "Tue, 6 Aug 2013 09:59:28 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Aug 2013 17:54:27 GMT",
"version": "v2"
},
{
"created": "Tue, 12 Nov 2013 16:23:38 GMT",
"version": "v3"
},
{
"created": "Fri, 12 May 2017 17:42:10 GMT",
"version": "v4"
}
] | 2017-05-15 | [
[
"de Alwis",
"S.",
""
],
[
"Gupta",
"R. K.",
""
],
[
"Hatefi",
"E.",
""
],
[
"Quevedo",
"F.",
""
]
] | We study the non-perturbative stability of the Large Volume Scenario (LVS) of IIB string compactifications, by analysing transitions mediated by the Brown-Teitelboim (BT) brane nucleations and by Coleman De Luccia tunneling (CDL). We find that, as long as the effective field theory description holds, the LVS AdS minima... | 10.934668 | 11.035547 | 11.385194 | 10.583247 | 11.852666 | 10.974552 | 10.908451 | 10.684733 | 10.076576 | 12.673234 | 10.463895 | 10.870937 | 10.992194 | 10.551024 | 10.96094 | 10.287559 | 10.709173 | 10.385858 | 10.81378 | 11.201352 | 10.59894 |
0907.5259 | Yuji Satoh | Kazuhiro Sakai, Yuji Satoh | A note on string solutions in AdS_3 | 17 pages, 1 figure; (v2) added 1 figure and discussion on solutions
with 6 null boundaries; (v3) corrected equation numbers; (v4) added comments | JHEP 0910:001,2009 | 10.1088/1126-6708/2009/10/001 | UTHEP-588 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We systematically search for classical open string solutions in AdS_3 within
the general class expressed by elliptic functions (i.e., the genus-one
finite-gap solutions). By explicitly solving the reality and Virasoro
conditions, we give a classification of the allowed solutions. When the
elliptic modulus degenerates... | [
{
"created": "Thu, 30 Jul 2009 08:09:44 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Sep 2009 04:26:33 GMT",
"version": "v2"
},
{
"created": "Thu, 1 Oct 2009 12:02:37 GMT",
"version": "v3"
},
{
"created": "Tue, 19 Jan 2010 11:24:13 GMT",
"version": "v4"
}
] | 2010-01-22 | [
[
"Sakai",
"Kazuhiro",
""
],
[
"Satoh",
"Yuji",
""
]
] | We systematically search for classical open string solutions in AdS_3 within the general class expressed by elliptic functions (i.e., the genus-one finite-gap solutions). By explicitly solving the reality and Virasoro conditions, we give a classification of the allowed solutions. When the elliptic modulus degenerates, ... | 17.19058 | 16.261738 | 18.588774 | 14.609638 | 15.260312 | 15.614176 | 15.447815 | 15.165777 | 15.570187 | 19.367264 | 14.893102 | 14.979152 | 17.028275 | 15.018749 | 14.923422 | 15.81278 | 14.79944 | 14.976459 | 15.079519 | 16.967089 | 14.850153 |
2011.07596 | Martin Bojowald | Martin Bojowald, Suddhasattwa Brahma, Umut Buyukcam, Martijn van
Kuppeveld | The ground state of non-associative hydrogen and upper bounds on the
magnetic charge of elementary particles | 25 pages | Phys. Rev. D 104 (2021) 105009 | 10.1103/PhysRevD.104.105009 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Formulations of magnetic monopoles in a Hilbert-space formulation of quantum
mechanics require Dirac's quantization condition of magnetic charge, which
implies a large value that can easily be ruled out for elementary particles by
standard atomic spectroscopy. However, an algebraic formulation of
non-associative quan... | [
{
"created": "Sun, 15 Nov 2020 18:20:02 GMT",
"version": "v1"
}
] | 2022-05-03 | [
[
"Bojowald",
"Martin",
""
],
[
"Brahma",
"Suddhasattwa",
""
],
[
"Buyukcam",
"Umut",
""
],
[
"van Kuppeveld",
"Martijn",
""
]
] | Formulations of magnetic monopoles in a Hilbert-space formulation of quantum mechanics require Dirac's quantization condition of magnetic charge, which implies a large value that can easily be ruled out for elementary particles by standard atomic spectroscopy. However, an algebraic formulation of non-associative quantu... | 12.546641 | 10.843178 | 12.502653 | 11.747725 | 12.088502 | 12.21757 | 11.603385 | 12.760409 | 11.944687 | 12.589038 | 11.629684 | 11.435162 | 11.566892 | 11.553864 | 11.417824 | 11.366517 | 11.383782 | 11.422211 | 11.655742 | 11.807825 | 11.558585 |
1305.2578 | Ming-Fan Li | Ming-Fan Li and Mingxing Luo | Intermediate effective interactions and dynamical fermion mass
generation of QCD | 6 pages, 5 figures, revtex4 | Phys. Rev. D 88, 085019 (2013) | 10.1103/PhysRevD.88.085019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The functional renormalization group equation is expanded to a two-loop form.
This two-loop form equation involves one-loop effective action. An intermediate
effective action perspective is adopted toward the one-loop effective action.
That is to say, the intermediate effective action could not be of the same form
of... | [
{
"created": "Sun, 12 May 2013 11:38:03 GMT",
"version": "v1"
}
] | 2013-10-30 | [
[
"Li",
"Ming-Fan",
""
],
[
"Luo",
"Mingxing",
""
]
] | The functional renormalization group equation is expanded to a two-loop form. This two-loop form equation involves one-loop effective action. An intermediate effective action perspective is adopted toward the one-loop effective action. That is to say, the intermediate effective action could not be of the same form of t... | 16.201889 | 18.099068 | 16.555878 | 15.958801 | 18.329441 | 17.936491 | 16.771406 | 17.636204 | 16.257416 | 17.000725 | 16.59763 | 15.461639 | 16.258524 | 15.744817 | 16.420061 | 17.031393 | 15.857836 | 16.187468 | 15.455097 | 15.797007 | 15.996243 |
hep-th/0301217 | Radu Roiban | Radu Roiban, Radu Tatar, Johannes Walcher | Massless Flavor in Geometry and Matrix Models | 33 pages, 1 figure | Nucl.Phys.B665:211-235,2003 | 10.1016/S0550-3213(03)00451-6 | null | hep-th | null | The proper inclusion of flavor in the Dijkgraaf-Vafa proposal for the
solution of N=1 gauge theories through matrix models has been subject of debate
in the recent literature. We here reexamine this issue by geometrically
engineering fundamental matter with type IIB branes wrapped on non-compact
cycles in the resolve... | [
{
"created": "Mon, 27 Jan 2003 19:17:47 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Roiban",
"Radu",
""
],
[
"Tatar",
"Radu",
""
],
[
"Walcher",
"Johannes",
""
]
] | The proper inclusion of flavor in the Dijkgraaf-Vafa proposal for the solution of N=1 gauge theories through matrix models has been subject of debate in the recent literature. We here reexamine this issue by geometrically engineering fundamental matter with type IIB branes wrapped on non-compact cycles in the resolved ... | 12.810349 | 10.477627 | 15.10614 | 10.263525 | 11.097294 | 10.798347 | 10.597462 | 10.695387 | 10.942818 | 14.830339 | 11.346433 | 10.477257 | 11.976508 | 11.446086 | 10.908648 | 10.653068 | 10.623781 | 10.630615 | 11.440517 | 11.589108 | 10.931944 |
1906.03102 | Peng-Xiang Hao | Bin Chen, Peng-Xiang Hao, Zhe-fei Yu | 2d Galilean Field Theories with Anisotropic Scaling | 39 pages; v2: 40 pages, note and references added, typos corrected;
v3: reference added, typos corrected; v4: minor revision on section4 and
section 7 | Phys. Rev. D 101, 066029 (2020) | 10.1103/PhysRevD.101.066029 | null | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we study two-dimensional Galilean field theories with global
translations and anisotropic scaling symmetries. We show that such theories
have enhanced local symmetries, generated by the infinite dimensional spin-l
Galilean algebra with possible central extensions, under the assumption that
the dilation ... | [
{
"created": "Fri, 7 Jun 2019 13:52:20 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Jun 2019 03:24:50 GMT",
"version": "v2"
},
{
"created": "Wed, 19 Jun 2019 14:25:25 GMT",
"version": "v3"
},
{
"created": "Thu, 26 Sep 2019 11:13:07 GMT",
"version": "v4"
}
] | 2020-04-08 | [
[
"Chen",
"Bin",
""
],
[
"Hao",
"Peng-Xiang",
""
],
[
"Yu",
"Zhe-fei",
""
]
] | In this work, we study two-dimensional Galilean field theories with global translations and anisotropic scaling symmetries. We show that such theories have enhanced local symmetries, generated by the infinite dimensional spin-l Galilean algebra with possible central extensions, under the assumption that the dilation op... | 9.500315 | 8.433484 | 10.156206 | 8.0322 | 8.845604 | 8.737637 | 8.919209 | 8.044332 | 8.882828 | 10.539775 | 8.528366 | 8.43309 | 9.293223 | 8.628881 | 8.811804 | 9.237259 | 8.872439 | 8.933089 | 9.067599 | 9.218358 | 8.598137 |
2107.04535 | Khai Ming Wong | Dan Zhu, Khai-Ming Wong, Timothy Tie, Guo-Quan Wong | Bifurcating Branches of Multiple Charged One-Plus-Half Monopole In SU(2)
Yang-Mills-Higgs Theory | 7 pages, 4 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study on the one-plus-half monopole configuration in SU(2)
Yang-Mills-Higgs theory when the $\phi$-winding number, $n$, runs from 2 to 4
and for a range of Higgs coupling constant, $\lambda_b \leq \lambda \leq 40$,
where $\lambda_b$ is the lower bound, below which no solution can be found.
Bifurcati... | [
{
"created": "Fri, 9 Jul 2021 16:40:33 GMT",
"version": "v1"
}
] | 2021-07-12 | [
[
"Zhu",
"Dan",
""
],
[
"Wong",
"Khai-Ming",
""
],
[
"Tie",
"Timothy",
""
],
[
"Wong",
"Guo-Quan",
""
]
] | In this paper, we study on the one-plus-half monopole configuration in SU(2) Yang-Mills-Higgs theory when the $\phi$-winding number, $n$, runs from 2 to 4 and for a range of Higgs coupling constant, $\lambda_b \leq \lambda \leq 40$, where $\lambda_b$ is the lower bound, below which no solution can be found. Bifurcation... | 8.23481 | 8.005945 | 9.207544 | 7.993999 | 7.885374 | 7.976759 | 7.181371 | 7.650826 | 7.910964 | 8.85563 | 7.829369 | 7.48239 | 8.054658 | 7.787939 | 7.737124 | 7.626648 | 7.445864 | 7.631701 | 7.665377 | 7.941796 | 7.862006 |
hep-th/0103112 | Massimo Bianchi | Massimo Bianchi (DAMTP University of Cambridge and Universita` di Roma
``Tor Vergata'') | (Non-)perturbative tests of the AdS/CFT correspondence | 9 pages, Latex, style file espcrc2.sty. Typos corrected, references
added. Talk given at the D.V. Volkov Memorial Conference ``Supersymmetry and
Quantum Field Theory'', 25-30 July 2000, Kharkov, to be published in Nuclear
Physics B Conference Supplements. Summary of the lectures delivered at the
school ``Latest... | Nucl.Phys.Proc.Suppl. 102 (2001) 56-64 | 10.1016/S0920-5632(01)01536-5 | DAMTP-01-24 | hep-th | null | I summarize perturbative and non-perturbative field theory tests of the
holographic correspondence between type IIB superstring on AdS_5xS^5 and N=4
SYM theory. The holographic duality between D-instantons and YM instantons is
briefly described. Non renormalization of two- and three-point functions of
CPO's and their... | [
{
"created": "Wed, 14 Mar 2001 17:02:27 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Apr 2001 11:00:03 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Bianchi",
"Massimo",
"",
"DAMTP University of Cambridge and Universita` di Roma\n ``Tor Vergata''"
]
] | I summarize perturbative and non-perturbative field theory tests of the holographic correspondence between type IIB superstring on AdS_5xS^5 and N=4 SYM theory. The holographic duality between D-instantons and YM instantons is briefly described. Non renormalization of two- and three-point functions of CPO's and their e... | 8.104832 | 6.679173 | 8.786824 | 6.844859 | 6.677854 | 6.765091 | 6.930559 | 6.692538 | 7.125151 | 9.19383 | 6.940246 | 6.828336 | 7.737628 | 7.145889 | 7.150283 | 6.757091 | 6.968345 | 6.878718 | 7.147479 | 8.017621 | 6.862717 |
1104.3155 | Hans Jockers | Allan Adams, Hans Jockers, Vijay Kumar, Joshua M. Lapan | N=1 Sigma Models in AdS_4 | 32 pages; v2: minor changes and references added; v3: discussion in
sect. 5 extended, version published in JHEP | null | 10.1007/JHEP12(2011)042 | MIT-CTP-4246; SU-ITP-11/21; NSF-KITP-11-053 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study sigma models in AdS_4 with global N=1 supersymmetry and find that
they differ significantly from their flat-space cousins -- the target space is
constrained to be a Kahler manifold with an exact Kahler form, the
superpotential transforms under Kahler transformations, the space of
supersymmetric vacua is gene... | [
{
"created": "Fri, 15 Apr 2011 20:37:24 GMT",
"version": "v1"
},
{
"created": "Sun, 10 Jul 2011 17:00:01 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Dec 2011 13:06:01 GMT",
"version": "v3"
}
] | 2015-05-27 | [
[
"Adams",
"Allan",
""
],
[
"Jockers",
"Hans",
""
],
[
"Kumar",
"Vijay",
""
],
[
"Lapan",
"Joshua M.",
""
]
] | We study sigma models in AdS_4 with global N=1 supersymmetry and find that they differ significantly from their flat-space cousins -- the target space is constrained to be a Kahler manifold with an exact Kahler form, the superpotential transforms under Kahler transformations, the space of supersymmetric vacua is generi... | 8.301281 | 7.999825 | 9.864546 | 8.470468 | 8.417182 | 8.511036 | 8.711145 | 8.362786 | 8.272632 | 10.702919 | 7.842236 | 7.980365 | 8.88045 | 8.136249 | 8.298273 | 8.136935 | 8.152492 | 8.035805 | 8.118598 | 8.91729 | 8.059487 |
2009.00033 | Yasunori Lee | Yasunori Lee, Kantaro Ohmori, Yuji Tachikawa | Revisiting Wess-Zumino-Witten terms | 59 pages; v2: minor changes | SciPost Phys. 10, 061 (2021) | 10.21468/SciPostPhys.10.3.061 | IPMU-20-0093 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit various topological issues concerning four-dimensional ungauged
and gauged Wess-Zumino-Witten (WZW) terms for $SU$ and $SO$ quantum
chromodynamics (QCD), from the modern bordism point of view. We explain, for
example, why the definition of the $4d$ WZW terms requires the spin structure.
We also discuss how... | [
{
"created": "Mon, 31 Aug 2020 18:02:55 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Sep 2020 15:00:01 GMT",
"version": "v2"
}
] | 2021-03-10 | [
[
"Lee",
"Yasunori",
""
],
[
"Ohmori",
"Kantaro",
""
],
[
"Tachikawa",
"Yuji",
""
]
] | We revisit various topological issues concerning four-dimensional ungauged and gauged Wess-Zumino-Witten (WZW) terms for $SU$ and $SO$ quantum chromodynamics (QCD), from the modern bordism point of view. We explain, for example, why the definition of the $4d$ WZW terms requires the spin structure. We also discuss how t... | 10.396389 | 8.744449 | 9.348716 | 8.365787 | 8.716574 | 8.247952 | 8.503083 | 8.093826 | 8.523234 | 11.11171 | 7.959414 | 9.05244 | 9.546422 | 8.737564 | 9.333316 | 8.939782 | 8.997077 | 8.432467 | 8.883622 | 9.213829 | 9.185432 |
hep-th/0604217 | Yoshinobu Habara | Yoshinobu Habara | Gauge Theory and a Dirac Operator on a Noncommutative Space | 2 figures, final version | Prog.Theor.Phys.116:771-781,2007 | 10.1143/PTP.116.771 | null | hep-th | null | As a tool to carry out the quantization of gauge theory on a noncommutative
space, we present a Dirac operator that behaves as a line element of the
canonical noncommutative space. Utilizing this operator, we construct the
Dixmier trace, which is the regularized trace for infinite-dimensional
matrices. We propose the... | [
{
"created": "Fri, 28 Apr 2006 16:31:56 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Oct 2006 15:26:09 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Habara",
"Yoshinobu",
""
]
] | As a tool to carry out the quantization of gauge theory on a noncommutative space, we present a Dirac operator that behaves as a line element of the canonical noncommutative space. Utilizing this operator, we construct the Dixmier trace, which is the regularized trace for infinite-dimensional matrices. We propose the p... | 10.152991 | 9.074951 | 9.190716 | 8.188008 | 8.421714 | 8.681649 | 9.110602 | 8.85064 | 7.92905 | 10.006118 | 8.263355 | 8.275128 | 8.74833 | 8.730663 | 8.541971 | 8.445576 | 8.654814 | 8.391275 | 8.526433 | 8.845015 | 8.447351 |
hep-th/9409100 | Philippe Zaugg | Philippe Zaugg | The quantum Poincare group from quantum group contraction | 19 pages, mit-2353, harvmac | null | 10.1088/0305-4470/28/9/018 | null | hep-th | null | We propose a contraction of the de Sitter quantum group leading to the
quantum Poincare group in any dimensions. The method relies on the coaction of
the de Sitter quantum group on a non--commutative space, and the deformation
parameter $q$ is sent to one. The bicrossproduct structure of the quantum
Poincar\'e group ... | [
{
"created": "Sun, 18 Sep 1994 22:33:03 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Zaugg",
"Philippe",
""
]
] | We propose a contraction of the de Sitter quantum group leading to the quantum Poincare group in any dimensions. The method relies on the coaction of the de Sitter quantum group on a non--commutative space, and the deformation parameter $q$ is sent to one. The bicrossproduct structure of the quantum Poincar\'e group is... | 6.677845 | 5.903417 | 5.686288 | 5.305818 | 5.535274 | 5.459599 | 5.828139 | 5.307373 | 5.473759 | 6.805131 | 5.958162 | 5.571509 | 6.000768 | 5.803077 | 5.565929 | 5.5206 | 5.581437 | 5.718547 | 5.740679 | 6.147851 | 6.015256 |
hep-th/0112226 | Allan Joseph Medved | A.J.M. Medved (University of Alberta) | A Holographic Interpretation of Asymptotically de Sitter Spacetimes | 23 page, Latex; references added and some discussion (but no
equations) modified | Class.Quant.Grav. 19 (2002) 2883-2896 | 10.1088/0264-9381/19/11/309 | null | hep-th | null | One of the remarkable outcomes of the AdS/CFT correspondence has been the
generalization of Cardy's entropy formula for arbitrary dimensionality, as well
as a variety of anti-de Sitter scenarios. More recently, related work has been
done in the realm of asymptotically de Sitter backgrounds. Such studies presume
a wel... | [
{
"created": "Mon, 24 Dec 2001 20:46:25 GMT",
"version": "v1"
},
{
"created": "Mon, 31 Dec 2001 20:37:11 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Medved",
"A. J. M.",
"",
"University of Alberta"
]
] | One of the remarkable outcomes of the AdS/CFT correspondence has been the generalization of Cardy's entropy formula for arbitrary dimensionality, as well as a variety of anti-de Sitter scenarios. More recently, related work has been done in the realm of asymptotically de Sitter backgrounds. Such studies presume a well-... | 8.053905 | 7.37693 | 7.688708 | 7.107747 | 7.34454 | 7.237079 | 7.30261 | 7.257107 | 7.612362 | 8.650309 | 7.225964 | 7.329558 | 7.201671 | 7.602535 | 7.276752 | 7.384694 | 7.261983 | 7.306633 | 7.296852 | 7.40361 | 7.346295 |
1605.02030 | Christopher D. Carone | Christopher D. Carone | Unitarity and microscopic acausality in a nonlocal theory | 26 pages LaTeX, 4 eps figures (latest version: discussion added) | Phys. Rev. D 95, 045009 (2017) | 10.1103/PhysRevD.95.045009 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider unitarity and causality in a higher-derivative theory of infinite
order, where propagators fall off more quickly in the ultraviolet due to the
presence of a transcendental entire function of the momentum. Like Lee-Wick
theories, these field theories might provide new avenues for addressing the
hierarchy p... | [
{
"created": "Fri, 6 May 2016 18:44:25 GMT",
"version": "v1"
},
{
"created": "Fri, 13 May 2016 21:27:20 GMT",
"version": "v2"
},
{
"created": "Tue, 7 Feb 2017 16:47:34 GMT",
"version": "v3"
}
] | 2017-03-01 | [
[
"Carone",
"Christopher D.",
""
]
] | We consider unitarity and causality in a higher-derivative theory of infinite order, where propagators fall off more quickly in the ultraviolet due to the presence of a transcendental entire function of the momentum. Like Lee-Wick theories, these field theories might provide new avenues for addressing the hierarchy pro... | 13.705973 | 14.336059 | 14.223823 | 12.994235 | 13.761069 | 14.471065 | 15.178444 | 14.041365 | 13.417812 | 15.913017 | 12.95178 | 13.709905 | 13.398149 | 12.936837 | 13.229481 | 13.660203 | 13.146439 | 13.030107 | 13.339573 | 13.569396 | 12.976598 |
1101.1748 | Sun ChengYi | Cheng-Yi Sun and Rui-Hong Yue | Inflation and New Agegraphic Dark Energy | 5 pages,no figures, detials is added | Phys.Rev.D83:107302,2011 | 10.1103/PhysRevD.83.107302 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the note, we extend the discussion of the new agegraphic dark energy
(NADE) model to include the inflation stage. Usually, in the inflation models,
for convenience the conformal time $\eta$ is set to be zero at the end of
inflation. This is incompatible with the NADE model since $\eta=0$ indicates
the divergence o... | [
{
"created": "Mon, 10 Jan 2011 09:44:12 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Apr 2011 08:20:33 GMT",
"version": "v2"
}
] | 2011-06-02 | [
[
"Sun",
"Cheng-Yi",
""
],
[
"Yue",
"Rui-Hong",
""
]
] | In the note, we extend the discussion of the new agegraphic dark energy (NADE) model to include the inflation stage. Usually, in the inflation models, for convenience the conformal time $\eta$ is set to be zero at the end of inflation. This is incompatible with the NADE model since $\eta=0$ indicates the divergence of ... | 9.242962 | 9.237343 | 8.261155 | 8.208163 | 9.197978 | 8.923194 | 9.516192 | 8.255953 | 8.775874 | 8.560259 | 8.297115 | 8.478579 | 8.135273 | 8.367336 | 8.392345 | 8.706594 | 8.232239 | 8.24628 | 8.199907 | 7.76791 | 8.685297 |
1402.0872 | Jorge Eduardo Santos | Sean A. Hartnoll and Jorge E. Santos | Disordered horizons: Holography of randomly disordered fixed points | v2: typos fixed, refs added, 19 pages, 5 figures | Phys. Rev. Lett. 112, 231601 (2014) | 10.1103/PhysRevLett.112.231601 | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We deform conformal field theories with classical gravity duals by marginally
relevant random disorder. We show that the disorder generates a flow to IR
fixed points with a finite amount of disorder. The randomly disordered fixed
points are characterized by a dynamical critical exponent $z>1$ that we obtain
both anal... | [
{
"created": "Tue, 4 Feb 2014 21:00:17 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Feb 2014 18:29:11 GMT",
"version": "v2"
}
] | 2014-06-18 | [
[
"Hartnoll",
"Sean A.",
""
],
[
"Santos",
"Jorge E.",
""
]
] | We deform conformal field theories with classical gravity duals by marginally relevant random disorder. We show that the disorder generates a flow to IR fixed points with a finite amount of disorder. The randomly disordered fixed points are characterized by a dynamical critical exponent $z>1$ that we obtain both analyt... | 7.965366 | 7.279872 | 8.314171 | 7.472081 | 6.959517 | 7.574414 | 8.208057 | 7.515405 | 7.758191 | 8.540921 | 7.094975 | 6.953754 | 7.957524 | 7.323902 | 7.309455 | 7.226018 | 7.2082 | 7.282986 | 7.343196 | 7.701454 | 7.109286 |
2309.15892 | Danai Roumelioti | Spyros Konitopoulos, Danai Roumelioti, George Zoupanos | Unification of Gravity and Internal Interactions | null | Fortschr. Phys. 2023, 2300226 | 10.1002/prop.202300226 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the gauge theoretic approach of gravity, General Relativity is described
by gauging the symmetry of the tangent manifold in four dimensions. Usually the
dimension of the tangent space is considered to be equal to the dimension of
the curved manifold. However, the tangent group of a manifold of dimension $d$
is not... | [
{
"created": "Wed, 27 Sep 2023 17:16:50 GMT",
"version": "v1"
}
] | 2023-11-16 | [
[
"Konitopoulos",
"Spyros",
""
],
[
"Roumelioti",
"Danai",
""
],
[
"Zoupanos",
"George",
""
]
] | In the gauge theoretic approach of gravity, General Relativity is described by gauging the symmetry of the tangent manifold in four dimensions. Usually the dimension of the tangent space is considered to be equal to the dimension of the curved manifold. However, the tangent group of a manifold of dimension $d$ is not n... | 8.700332 | 9.818486 | 9.105678 | 8.872926 | 9.249457 | 8.590045 | 9.559026 | 8.385937 | 8.937666 | 9.561541 | 8.782169 | 8.579455 | 8.456264 | 8.342831 | 8.49964 | 8.617481 | 8.52117 | 8.428753 | 8.416212 | 8.521173 | 8.618019 |
1003.3190 | Alexander Schenkel | Alexander Schenkel, Christoph F. Uhlemann | Field Theory on Curved Noncommutative Spacetimes | SIGMA Special Issue on Noncommutative Spaces and Fields | SIGMA 6 (2010), 061, 19 pages | 10.3842/SIGMA.2010.061 | null | hep-th gr-qc math-ph math.MP | http://creativecommons.org/licenses/by-nc-sa/3.0/ | We study classical scalar field theories on noncommutative curved spacetimes.
Following the approach of Wess et al. [Classical Quantum Gravity 22 (2005),
3511 and Classical Quantum Gravity 23 (2006), 1883], we describe noncommutative
spacetimes by using (Abelian) Drinfel'd twists and the associated *-products
and *-d... | [
{
"created": "Tue, 16 Mar 2010 17:03:39 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Aug 2010 06:18:22 GMT",
"version": "v2"
}
] | 2010-08-04 | [
[
"Schenkel",
"Alexander",
""
],
[
"Uhlemann",
"Christoph F.",
""
]
] | We study classical scalar field theories on noncommutative curved spacetimes. Following the approach of Wess et al. [Classical Quantum Gravity 22 (2005), 3511 and Classical Quantum Gravity 23 (2006), 1883], we describe noncommutative spacetimes by using (Abelian) Drinfel'd twists and the associated *-products and *-dif... | 4.89537 | 5.62238 | 6.207682 | 5.145776 | 5.154093 | 5.8624 | 5.619521 | 5.279426 | 5.047136 | 6.081207 | 5.10974 | 5.225593 | 5.356809 | 5.118661 | 5.041649 | 5.071829 | 5.229973 | 5.008493 | 5.000721 | 5.247143 | 4.988397 |
hep-th/0407093 | Juan Antonio Nieto | J. A. Nieto | Chirotope Concept in Various Scenarios of Physics | 19 pages, Latex | Rev.Mex.Fis. E51 (2005) 5-12 | null | null | hep-th | null | We argue that the chirotope concept of oriented matroid theory may be found
in different scenarios of physics, including classical mechanics, quantum
mechanics, gauge field theory, p-branes formalism, two time physics and Matrix
theory. Our observations may motivate the interest of possible applications of
matroid th... | [
{
"created": "Mon, 12 Jul 2004 18:49:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nieto",
"J. A.",
""
]
] | We argue that the chirotope concept of oriented matroid theory may be found in different scenarios of physics, including classical mechanics, quantum mechanics, gauge field theory, p-branes formalism, two time physics and Matrix theory. Our observations may motivate the interest of possible applications of matroid theo... | 20.393663 | 13.540559 | 24.417553 | 14.011922 | 15.860309 | 12.943283 | 14.344226 | 13.797789 | 15.441725 | 24.672562 | 14.561794 | 16.339096 | 20.475634 | 17.480492 | 17.773926 | 15.874916 | 16.658869 | 17.225986 | 17.745598 | 20.281094 | 17.170734 |
hep-th/9407056 | Robert Perry | Robert J. Perry (The Ohio State University) | Hamiltonian Light-Front Field Theory and Quantum Chromodynamics | corrected version of 1994 lectures, 84 pages, LATEX. Published in
"Hadron Physics 94," Proceedings, Gramado, Brazil (World Scientific, 1995) | null | null | null | hep-th hep-ph nucl-th | null | Light-front coordinates offer a scenario in which a constituent picture of
hadron structure can emerge from QCD, after several difficulties are addressed.
Field theoretic difficulties force us to introduce cutoffs that violate Lorentz
covariance and gauge invariance, and a new renormalization group formalism
based on... | [
{
"created": "Mon, 11 Jul 1994 18:27:51 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Jul 1997 02:21:02 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Perry",
"Robert J.",
"",
"The Ohio State University"
]
] | Light-front coordinates offer a scenario in which a constituent picture of hadron structure can emerge from QCD, after several difficulties are addressed. Field theoretic difficulties force us to introduce cutoffs that violate Lorentz covariance and gauge invariance, and a new renormalization group formalism based on a... | 16.236595 | 12.09408 | 17.233852 | 13.951686 | 14.418555 | 12.890676 | 12.831352 | 13.935925 | 14.185583 | 16.751249 | 14.23828 | 15.072969 | 16.095043 | 15.645858 | 15.317413 | 15.478056 | 14.928585 | 15.633493 | 15.629654 | 16.653381 | 15.59651 |
hep-th/9406012 | M. B. Green | Michael B. Green and Joe Polchinski | Summing Over World-Sheet Boundaries | 10 pages | Phys.Lett.B335:377-382,1994 | 10.1016/0370-2693(94)90367-0 | DAMTP/94-38;NSF-ITP-94-52 | hep-th | null | The moduli associated with boundaries in a Riemann surface are parametrized
by the positions and strengths of electric charges. This suggests a method for
summing over orientable Riemann surfaces with Dirichlet boundary conditions on
the embedding coordinates. A light-cone parameterization of such boundaries is
also ... | [
{
"created": "Fri, 3 Jun 1994 08:16:10 GMT",
"version": "v1"
}
] | 2009-10-09 | [
[
"Green",
"Michael B.",
""
],
[
"Polchinski",
"Joe",
""
]
] | The moduli associated with boundaries in a Riemann surface are parametrized by the positions and strengths of electric charges. This suggests a method for summing over orientable Riemann surfaces with Dirichlet boundary conditions on the embedding coordinates. A light-cone parameterization of such boundaries is also di... | 17.874701 | 16.374239 | 17.142288 | 15.128738 | 15.81378 | 15.191434 | 15.275765 | 14.414431 | 14.378233 | 18.652098 | 14.489403 | 13.74363 | 14.556275 | 13.770518 | 15.083521 | 14.364401 | 15.41646 | 14.120389 | 14.067833 | 15.485431 | 14.012424 |
1308.4400 | Theodore Erler | Theodore Erler | Analytic Solution for Tachyon Condensation in Berkovits' Open
Superstring Field Theory | v2: 43 pages, 6 figures. Minor corrections, references added | JHEP 1311 (2013) 007 | 10.1007/JHEP11(2013)007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an analytic solution for tachyon condensation on a non-BPS D-brane
in Berkovits' open superstring field theory. The solution is presented as a
product of $2\times 2$ matrices in two distinct $GL_2$ subgroups of the open
string star algebra. All string fields needed for computation of the
nonpolynomial acti... | [
{
"created": "Tue, 20 Aug 2013 20:00:00 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Sep 2013 13:45:43 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Erler",
"Theodore",
""
]
] | We present an analytic solution for tachyon condensation on a non-BPS D-brane in Berkovits' open superstring field theory. The solution is presented as a product of $2\times 2$ matrices in two distinct $GL_2$ subgroups of the open string star algebra. All string fields needed for computation of the nonpolynomial action... | 7.606067 | 7.030129 | 10.403501 | 7.209967 | 7.191328 | 8.022598 | 7.42437 | 7.049821 | 7.097719 | 11.927655 | 7.370019 | 7.412432 | 8.424983 | 7.124961 | 7.367031 | 7.309179 | 7.243413 | 7.422985 | 7.169224 | 8.086677 | 7.290968 |
1808.06744 | Brian Willett | P. Marcos Crichigno, Dharmesh Jain, and Brian Willett | 5d Partition Functions with A Twist | Corrected typos, updated references, and added clarifying comments in
Section 5 | JHEP 1811 (2018) 058 | 10.1007/JHEP11(2018)058 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the partition function of 5d ${\cal N}=1$ gauge theories on the
manifold $S^3_b \times \Sigma_{\frak g}$ with a partial topological twist along
the Riemann surface, $\Sigma_{\frak g}$. This setup is a higher dimensional
uplift of the two-dimensional A-twist, and the result can be expressed as a sum
over sol... | [
{
"created": "Tue, 21 Aug 2018 03:07:35 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Sep 2018 16:45:16 GMT",
"version": "v2"
}
] | 2018-12-05 | [
[
"Crichigno",
"P. Marcos",
""
],
[
"Jain",
"Dharmesh",
""
],
[
"Willett",
"Brian",
""
]
] | We derive the partition function of 5d ${\cal N}=1$ gauge theories on the manifold $S^3_b \times \Sigma_{\frak g}$ with a partial topological twist along the Riemann surface, $\Sigma_{\frak g}$. This setup is a higher dimensional uplift of the two-dimensional A-twist, and the result can be expressed as a sum over solut... | 5.141912 | 4.663703 | 5.795557 | 4.804863 | 4.841352 | 5.017765 | 4.918708 | 4.721807 | 4.572123 | 5.974346 | 4.739393 | 4.866036 | 5.330337 | 4.908395 | 4.938678 | 4.910311 | 5.054194 | 4.829996 | 4.740744 | 5.179913 | 4.861039 |
0907.1973 | Mohamed Chakhad | Mohamed Chakhad | Kundt spacetimes of massive gravity in three dimensions | 31 pages, 7 figures | null | null | UTTG-07-07 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study Kundt solutions of topologically massive gravity (TMG) and the new
theory of massive gravity (NMG), proposed recently in arXiv:0901.1766. For
topologically massive gravity, only the CSI Kundt solutions (i.e., solutions
with constant scalar polynomial curvature invariants) were found very recently
in arXiv:09... | [
{
"created": "Sat, 11 Jul 2009 16:14:21 GMT",
"version": "v1"
}
] | 2009-07-15 | [
[
"Chakhad",
"Mohamed",
""
]
] | We study Kundt solutions of topologically massive gravity (TMG) and the new theory of massive gravity (NMG), proposed recently in arXiv:0901.1766. For topologically massive gravity, only the CSI Kundt solutions (i.e., solutions with constant scalar polynomial curvature invariants) were found very recently in arXiv:0906... | 9.311457 | 9.689622 | 9.975079 | 8.907662 | 9.178963 | 9.326652 | 10.06216 | 9.648409 | 9.546224 | 9.833001 | 9.566052 | 9.197762 | 9.164526 | 8.914669 | 9.219846 | 8.964461 | 8.654531 | 9.103116 | 9.119884 | 9.643785 | 8.671481 |
2009.03369 | Rafael Bravo | Rafael Bravo and Gonzalo A. Palma | Unifying attractor and non-attractor models of inflation under a single
soft theorem | 13 pages; v5: matches published version in Phys Rev D. We included a
discussion regarding adiabaticity during USR-SR transitions | null | 10.1103/PhysRevD.107.043524 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the generation of local non-Gaussianity in models of canonical
single field inflation when their backgrounds are either attractor or
non-attractor. We show that the invariance of inflation under space-time
diffeomorphisms can be exploited to make powerful statements about the squeezed
limit of the primordial... | [
{
"created": "Mon, 7 Sep 2020 18:46:16 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Nov 2020 15:48:15 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Feb 2021 23:54:28 GMT",
"version": "v3"
},
{
"created": "Thu, 2 Sep 2021 15:52:38 GMT",
"version": "v4"
},
{
"cre... | 2023-04-13 | [
[
"Bravo",
"Rafael",
""
],
[
"Palma",
"Gonzalo A.",
""
]
] | We study the generation of local non-Gaussianity in models of canonical single field inflation when their backgrounds are either attractor or non-attractor. We show that the invariance of inflation under space-time diffeomorphisms can be exploited to make powerful statements about the squeezed limit of the primordial b... | 6.723342 | 7.717588 | 7.13774 | 6.702415 | 7.137336 | 7.776345 | 7.39113 | 6.919711 | 6.710304 | 7.437387 | 7.03007 | 6.823063 | 6.695558 | 6.729271 | 6.938621 | 6.913485 | 6.695146 | 6.775661 | 6.697543 | 6.995959 | 6.675344 |
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