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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9905218 | Bogdan Morariu | Daniel Brace, Bogdan Morariu, Bruno Zumino | Duality Invariant Born-Infeld Theory | 10 pages, LaTeX file; to appear in the Yuri Golfand memorial volume;
typos corrected, references added | null | 10.1142/9789812793850_0009 | LBNL-43404 | hep-th | null | We present an Sp(2n,R) duality invariant Born-Infeld U(1)^2n gauge theory
with scalar fields. To implement this duality we had to introduce complex gauge
fields and as a result the rank of the duality group is only half as large as
that of the corresponding Maxwell gauge theory with the same number of gauge
fields. T... | [
{
"created": "Sat, 29 May 1999 19:18:48 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Jul 1999 00:46:48 GMT",
"version": "v2"
}
] | 2016-11-23 | [
[
"Brace",
"Daniel",
""
],
[
"Morariu",
"Bogdan",
""
],
[
"Zumino",
"Bruno",
""
]
] | We present an Sp(2n,R) duality invariant Born-Infeld U(1)^2n gauge theory with scalar fields. To implement this duality we had to introduce complex gauge fields and as a result the rank of the duality group is only half as large as that of the corresponding Maxwell gauge theory with the same number of gauge fields. The... | 8.635507 | 7.815394 | 8.971334 | 8.013172 | 8.793748 | 8.644247 | 8.033636 | 7.803208 | 8.225064 | 8.864039 | 8.133809 | 8.289463 | 8.208576 | 8.11152 | 8.005541 | 8.060133 | 8.080105 | 8.000229 | 8.117471 | 8.445799 | 8.160872 |
hep-th/0101076 | Tassos Petkou | D. Klemm, A. C. Petkou and G. Siopsis | Entropy bounds, monotonicity properties and scaling in CFTs | 19p, LaTeX, v2 minor clarifications and added references, v3 version
to appear in NPB | Nucl.Phys. B601 (2001) 380-394 | 10.1016/S0550-3213(01)00085-2 | IFUM-679-FT, UTHET-01-0101 | hep-th gr-qc | null | We study the ratio of the entropy to the total energy in conformal field
theories at finite temperature. For the free field realizations of {\cal N}=4
super Yang-Mills theory in D=4 and the (2,0) tensor multiplet in D=6, the ratio
is bounded from above. The corresponding bounds are less stringent than the
recently pr... | [
{
"created": "Fri, 12 Jan 2001 10:32:47 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Jan 2001 14:36:39 GMT",
"version": "v2"
},
{
"created": "Tue, 20 Mar 2001 08:51:27 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Klemm",
"D.",
""
],
[
"Petkou",
"A. C.",
""
],
[
"Siopsis",
"G.",
""
]
] | We study the ratio of the entropy to the total energy in conformal field theories at finite temperature. For the free field realizations of {\cal N}=4 super Yang-Mills theory in D=4 and the (2,0) tensor multiplet in D=6, the ratio is bounded from above. The corresponding bounds are less stringent than the recently prop... | 6.887165 | 5.120147 | 7.414488 | 6.006186 | 6.193452 | 6.389513 | 6.096695 | 5.709911 | 6.216671 | 7.427618 | 5.824326 | 6.201474 | 7.018559 | 6.625764 | 6.616778 | 6.599998 | 6.691453 | 6.2278 | 6.492504 | 7.090662 | 6.380846 |
0801.1508 | James Gray | James Gray, Yang-Hui He, Anton Ilderton and Andr\'e Lukas | STRINGVACUA: A Mathematica Package for Studying Vacuum Configurations in
String Phenomenology | 21 pages, 9 figures | Comput.Phys.Commun.180:107-119,2009 | 10.1016/j.cpc.2008.08.009 | null | hep-th | null | We give a simple tutorial introduction to the Mathematica package
STRINGVACUA, which is designed to find vacua of string-derived or inspired
four-dimensional N=1 supergravities. The package uses powerful
algebro-geometric methods, as implemented in the free computer algebra system
Singular, but requires no knowledge ... | [
{
"created": "Wed, 9 Jan 2008 21:26:56 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"Gray",
"James",
""
],
[
"He",
"Yang-Hui",
""
],
[
"Ilderton",
"Anton",
""
],
[
"Lukas",
"André",
""
]
] | We give a simple tutorial introduction to the Mathematica package STRINGVACUA, which is designed to find vacua of string-derived or inspired four-dimensional N=1 supergravities. The package uses powerful algebro-geometric methods, as implemented in the free computer algebra system Singular, but requires no knowledge of... | 10.025716 | 11.34525 | 11.902384 | 9.936321 | 9.394189 | 10.446495 | 11.974527 | 10.436313 | 9.265728 | 12.684751 | 9.736726 | 9.603097 | 9.557169 | 9.735549 | 9.58928 | 9.854133 | 9.956481 | 9.66715 | 9.539531 | 9.597329 | 9.540625 |
1711.00914 | Igor Bandos | Igor Bandos | Spinor frame formalism for amplitudes and constrained superamplitudes of
10D SYM and 11D supergravity | 73 pages, no figures. V2: revised. Discussion improved and extended,
78 pages. V3. Published version, 82 pages | null | 10.1007/JHEP11(2018)017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that 10D spinor helicity formalism can be understood as spinor moving
frame approach to supersymmetric particles extended to the description of
amplitudes. This allows us to develop the spinor helicity formalism for 11D
supergravity and a new constrained superfield formalism for 10D SYM and 11D
SUGRA amplitud... | [
{
"created": "Thu, 2 Nov 2017 20:15:24 GMT",
"version": "v1"
},
{
"created": "Mon, 21 May 2018 13:38:50 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Oct 2018 17:43:47 GMT",
"version": "v3"
}
] | 2018-12-05 | [
[
"Bandos",
"Igor",
""
]
] | We show that 10D spinor helicity formalism can be understood as spinor moving frame approach to supersymmetric particles extended to the description of amplitudes. This allows us to develop the spinor helicity formalism for 11D supergravity and a new constrained superfield formalism for 10D SYM and 11D SUGRA amplitudes... | 11.532562 | 11.011449 | 12.575947 | 11.294034 | 11.194064 | 11.084549 | 11.98343 | 10.928268 | 11.281301 | 12.897476 | 11.065339 | 11.334811 | 11.827822 | 11.394901 | 11.690033 | 11.706924 | 11.660475 | 11.220203 | 11.234738 | 11.38461 | 11.148458 |
1905.01884 | Muneto Nitta | Chandrasekhar Chatterjee, Muneto Nitta | Aharonov-Bohm defects | 25 pages, 5 figures | Phys. Rev. D 101, 085002 (2020) | 10.1103/PhysRevD.101.085002 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss what happens when a field receiving an Aharonov-Bohm (AB) phase
develops a vacuum expectation value (VEV), with an example of an Alice string
in a $U(1) \times SU(2)$ gauge theory coupled with complex triplet scalar
fields. We introduce scalar fields belonging to the doublet representation of
$SU(2)$, char... | [
{
"created": "Mon, 6 May 2019 08:56:24 GMT",
"version": "v1"
}
] | 2020-04-08 | [
[
"Chatterjee",
"Chandrasekhar",
""
],
[
"Nitta",
"Muneto",
""
]
] | We discuss what happens when a field receiving an Aharonov-Bohm (AB) phase develops a vacuum expectation value (VEV), with an example of an Alice string in a $U(1) \times SU(2)$ gauge theory coupled with complex triplet scalar fields. We introduce scalar fields belonging to the doublet representation of $SU(2)$, charge... | 8.715911 | 8.204513 | 8.432013 | 8.209195 | 8.861649 | 8.641877 | 8.256967 | 8.295165 | 8.081708 | 9.184814 | 8.167486 | 8.23409 | 8.263267 | 7.81545 | 8.155149 | 8.205757 | 8.06217 | 8.223833 | 7.885283 | 8.112291 | 8.210612 |
hep-th/0406094 | Rosy Chooi Gim Teh | Rosy Teh and Khai-Ming Wong | Static Monopoles and Their Anti-Configurations | 20 pages with 4 figures | Int.J.Mod.Phys. A20 (2005) 4291 | 10.1142/S0217751X05023918 | null | hep-th | null | Recently, we have reported on the existence of some monopoles, multimonopole,
and antimonopoles configurations. In this paper we would like to present more
monopoles, multimonopole, and antimonopoles configurations of the magnetic
ansatz of Ref.\cite{kn:9} when the parameters $p$ and $b$ of the solutions
takes differ... | [
{
"created": "Fri, 11 Jun 2004 08:08:05 GMT",
"version": "v1"
},
{
"created": "Mon, 9 May 2005 08:41:14 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Teh",
"Rosy",
""
],
[
"Wong",
"Khai-Ming",
""
]
] | Recently, we have reported on the existence of some monopoles, multimonopole, and antimonopoles configurations. In this paper we would like to present more monopoles, multimonopole, and antimonopoles configurations of the magnetic ansatz of Ref.\cite{kn:9} when the parameters $p$ and $b$ of the solutions takes differen... | 11.680528 | 12.188776 | 12.325662 | 10.925924 | 11.445146 | 11.455843 | 11.738871 | 10.383872 | 10.835852 | 12.097166 | 11.333538 | 11.173423 | 11.230671 | 11.053482 | 11.041108 | 10.999751 | 11.17472 | 11.080993 | 11.09343 | 11.163743 | 10.725084 |
hep-th/9806192 | Zbigniew Walczak | Dieter Mayer, Alexander Ushveridze, Zbigniew Walczak | On time-dependent quasi-exactly solvable models | LaTeX, 12 pages | Mod.Phys.Lett. A15 (2000) 1243-1252 | 10.1142/S0217732300001572 | null | hep-th | null | In this paper we demonstrate that there exists a close relationship between
quasi-exactly solvable quantum models and two special classes of classical
dynamical systems. One of these systems can be considered a natural
generalization of the multi-particle Calogero-Moser model and the second one is
a classical matrix ... | [
{
"created": "Tue, 23 Jun 1998 15:17:52 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Mayer",
"Dieter",
""
],
[
"Ushveridze",
"Alexander",
""
],
[
"Walczak",
"Zbigniew",
""
]
] | In this paper we demonstrate that there exists a close relationship between quasi-exactly solvable quantum models and two special classes of classical dynamical systems. One of these systems can be considered a natural generalization of the multi-particle Calogero-Moser model and the second one is a classical matrix mo... | 7.416666 | 6.460689 | 7.890368 | 5.978472 | 6.93854 | 6.144742 | 6.149873 | 6.439776 | 6.27632 | 7.695057 | 6.384909 | 6.322314 | 6.999657 | 6.475904 | 6.323395 | 6.47468 | 6.183016 | 6.601201 | 6.385478 | 7.103593 | 6.408369 |
1302.2130 | Dirk Rathlev | Dirk Rathlev | Constraints from de Sitter metastability in heterotic string
compactifications | 32 pages, 1 figure; v2: a few references added, minor clarifications
added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the possibility of obtaining metastable de Sitter vacua of heterotic
string theory compactified on a Calabi-Yau threefold which are classical and
simple in the K\"ahler moduli sector of the theory. For this, we exploit a
known necessary condition on the K\"ahler potential in N=1-supergravity, which
we, under... | [
{
"created": "Fri, 8 Feb 2013 19:55:23 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 2013 16:38:48 GMT",
"version": "v2"
}
] | 2013-05-08 | [
[
"Rathlev",
"Dirk",
""
]
] | We study the possibility of obtaining metastable de Sitter vacua of heterotic string theory compactified on a Calabi-Yau threefold which are classical and simple in the K\"ahler moduli sector of the theory. For this, we exploit a known necessary condition on the K\"ahler potential in N=1-supergravity, which we, under t... | 8.647924 | 8.730301 | 8.960351 | 8.112007 | 8.149722 | 8.80514 | 8.959321 | 8.446589 | 7.957082 | 9.308719 | 7.938726 | 8.03291 | 8.346663 | 7.878822 | 8.030089 | 8.413378 | 8.043869 | 8.004035 | 8.11282 | 8.137477 | 7.899379 |
2406.04622 | Kang Zhou | Fang-Stars Wei, Kang Zhou | On soft factors and transmutation operators | 28 pages, 1 figure | null | null | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | The well known soft theorems state the specific factorizations of tree level
gravitational (GR) amplitudes at leading, sub-leading and sub-sub-leading
orders, with universal soft factors. For Yang-Mills (YM) amplitudes, similar
factorizations and universal soft factors are found at leading and sub-leading
orders. The... | [
{
"created": "Fri, 7 Jun 2024 04:06:20 GMT",
"version": "v1"
}
] | 2024-06-10 | [
[
"Wei",
"Fang-Stars",
""
],
[
"Zhou",
"Kang",
""
]
] | The well known soft theorems state the specific factorizations of tree level gravitational (GR) amplitudes at leading, sub-leading and sub-sub-leading orders, with universal soft factors. For Yang-Mills (YM) amplitudes, similar factorizations and universal soft factors are found at leading and sub-leading orders. Then ... | 8.365241 | 7.746872 | 8.735587 | 7.408105 | 7.914742 | 7.110451 | 7.651786 | 7.297336 | 7.476343 | 9.097908 | 7.42441 | 7.138038 | 8.16855 | 7.762784 | 7.797928 | 7.548461 | 7.752509 | 7.416745 | 7.419519 | 7.903147 | 7.628792 |
hep-th/0409099 | Horatiu Stefan Nastase | Kyungsik Kang and Horatiu Nastase | Planckian scattering effects and black hole production in low $M_{Pl}$
scenarios | 40 pages, latex, typos corrected, references added | Phys.Rev. D71 (2005) 124035 | 10.1103/PhysRevD.71.124035 | null | hep-th hep-ph | null | We reanalyze the question of black hole creation in high energy scattering
via shockwave collisions. We find that string corrections tend to increase the
scattering cross-section. We analyze corrections in a more physical setting, of
Randall-Sundrum type and of higher dimensionality. We also analyze the
scattering in... | [
{
"created": "Wed, 8 Sep 2004 15:37:39 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Sep 2004 17:42:10 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Kang",
"Kyungsik",
""
],
[
"Nastase",
"Horatiu",
""
]
] | We reanalyze the question of black hole creation in high energy scattering via shockwave collisions. We find that string corrections tend to increase the scattering cross-section. We analyze corrections in a more physical setting, of Randall-Sundrum type and of higher dimensionality. We also analyze the scattering insi... | 22.82892 | 21.257378 | 22.310308 | 19.973066 | 21.762951 | 21.60343 | 22.870018 | 21.508142 | 24.214355 | 19.605528 | 20.537594 | 21.429026 | 20.573959 | 21.212526 | 20.769773 | 21.328104 | 20.877966 | 19.736113 | 21.322121 | 20.983671 | 19.5821 |
1504.01700 | Imtak Jeon | Rajesh Kumar Gupta, Yuto Ito, Imtak Jeon | Supersymmetric Localization for BPS Black Hole Entropy: 1-loop Partition
Function from Vector Multiplets | 28+16 pages, improved discussion on the boundary mode in the 4.2 and
conclusion section | null | 10.1007/JHEP11(2015)197 | KIAS-P14053 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the techniques of supersymmetric localization to compute the BPS black
hole entropy in N=2 supergravity. We focus on the n_v+1 vector multiplets on
the black hole near horizon background which is AdS_2 x S^2 space. We find the
localizing saddle point of the vector multiplets by solving the localization
equatio... | [
{
"created": "Tue, 7 Apr 2015 18:25:41 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Aug 2015 09:16:01 GMT",
"version": "v2"
}
] | 2016-01-27 | [
[
"Gupta",
"Rajesh Kumar",
""
],
[
"Ito",
"Yuto",
""
],
[
"Jeon",
"Imtak",
""
]
] | We use the techniques of supersymmetric localization to compute the BPS black hole entropy in N=2 supergravity. We focus on the n_v+1 vector multiplets on the black hole near horizon background which is AdS_2 x S^2 space. We find the localizing saddle point of the vector multiplets by solving the localization equations... | 7.071283 | 6.805892 | 7.880412 | 7.127759 | 6.91408 | 7.159308 | 7.019753 | 7.368477 | 7.179312 | 8.632305 | 6.745316 | 6.642382 | 7.544569 | 6.821819 | 6.623802 | 6.590663 | 6.852257 | 6.783192 | 6.900003 | 7.717172 | 6.723055 |
hep-th/0004160 | Akihiro Ishibashi | Hideo Kodama, Akihiro Ishibashi and Osamu Seto | Brane World Cosmology - Gauge-Invariant Formalism for Perturbation | 25 pages, no figures, typos corrected, to appear in Phys.Rev.D | Phys.Rev. D62 (2000) 064022 | 10.1103/PhysRevD.62.064022 | YITP-00-21 | hep-th astro-ph gr-qc | null | In the present paper the gauge-invariant formalism is developed for
perturbations of the brane-world model in which our universe is realized as a
boundary of a higher-dimensional spacetime. For the background model in which
the bulk spacetime is $(n+m)$-dimensional and has the spatial symmetry
corresponding to the is... | [
{
"created": "Mon, 24 Apr 2000 09:45:19 GMT",
"version": "v1"
},
{
"created": "Mon, 8 May 2000 09:17:20 GMT",
"version": "v2"
},
{
"created": "Mon, 7 Aug 2000 06:18:36 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Kodama",
"Hideo",
""
],
[
"Ishibashi",
"Akihiro",
""
],
[
"Seto",
"Osamu",
""
]
] | In the present paper the gauge-invariant formalism is developed for perturbations of the brane-world model in which our universe is realized as a boundary of a higher-dimensional spacetime. For the background model in which the bulk spacetime is $(n+m)$-dimensional and has the spatial symmetry corresponding to the isom... | 6.986616 | 8.34182 | 7.280464 | 7.154787 | 7.450595 | 7.931695 | 8.097749 | 7.475122 | 7.545782 | 7.950077 | 7.406463 | 7.024595 | 6.786087 | 6.880169 | 7.071097 | 6.820298 | 7.032159 | 6.950209 | 7.152178 | 7.130868 | 6.96668 |
0912.4211 | Diego S\'aez-G\'omez | Diego S\'aez-G\'omez | Reconstructing cosmological solutions in F(R) gravity. Towards a unified
model of the Universe evolution | 4 pages. Contribution to the Proceedings of the Spanish Relativity
Meeting (ERE) 2009, Bilbao, Spain | J.Phys.Conf.Ser.229:012066,2010 | 10.1088/1742-6596/229/1/012066 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is accepted by the majority of scientific community that the Universe is
currently in an accelerated epoch. In order to explain this shock of late 90's,
a lot of dark energy candidates have been proposed. We study in the context of
f (R) gravity, how some modifications on General Relativity could reproduce
such be... | [
{
"created": "Mon, 21 Dec 2009 17:10:49 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Sáez-Gómez",
"Diego",
""
]
] | It is accepted by the majority of scientific community that the Universe is currently in an accelerated epoch. In order to explain this shock of late 90's, a lot of dark energy candidates have been proposed. We study in the context of f (R) gravity, how some modifications on General Relativity could reproduce such beha... | 12.544847 | 12.570993 | 11.955241 | 12.890826 | 13.455894 | 13.126766 | 13.849817 | 12.123617 | 13.182961 | 13.749678 | 13.348096 | 12.450439 | 12.017087 | 12.362538 | 12.440512 | 12.604208 | 12.349156 | 11.777368 | 12.875251 | 11.891807 | 12.524187 |
1307.5877 | Dan Xie | Dan Xie | M5 brane and four dimensional N=1 theories I | 30 pages, 18 figures | null | 10.1007/JHEP04(2014)154 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Four dimensional N=1 theories are engineered by compactifying six dimensional
(2,0) theory on a Riemann surface with regular punctures. A generalized
Hitchin's equation involving two Higgs fields is proposed as the BPS equation
for N=1 compactification. The puncture is interpreted as the singular boundary
condition o... | [
{
"created": "Mon, 22 Jul 2013 20:36:03 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Xie",
"Dan",
""
]
] | Four dimensional N=1 theories are engineered by compactifying six dimensional (2,0) theory on a Riemann surface with regular punctures. A generalized Hitchin's equation involving two Higgs fields is proposed as the BPS equation for N=1 compactification. The puncture is interpreted as the singular boundary condition of ... | 8.05513 | 7.59112 | 10.646668 | 7.766121 | 7.697187 | 7.894315 | 7.855369 | 7.453926 | 7.564534 | 10.597532 | 7.43099 | 7.666192 | 8.837731 | 7.452512 | 7.543749 | 7.712042 | 7.605435 | 7.649395 | 7.485054 | 8.54952 | 7.474561 |
2005.09851 | Yu. M. Zinoviev | M. V. Khabarov and Yu. M. Zinoviev | Massless higher spin cubic vertices in flat four dimmensional space | 21 pages, no figures. Some comments and new references added. Version
to appear in JHEP | JHEP 08 (2020) 112 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we construct a number of cubic interaction vertices for
massless bosonic and fermionic higher spin fields in flat four dimensional
space. First of all, we construct these cubic vertices in AdS_4 space using a
so-called Fradkin-Vasiliev approach, which works only for the non-zero
cosmological constant. T... | [
{
"created": "Wed, 20 May 2020 05:48:50 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Aug 2020 07:11:28 GMT",
"version": "v2"
}
] | 2020-08-31 | [
[
"Khabarov",
"M. V.",
""
],
[
"Zinoviev",
"Yu. M.",
""
]
] | In this paper we construct a number of cubic interaction vertices for massless bosonic and fermionic higher spin fields in flat four dimensional space. First of all, we construct these cubic vertices in AdS_4 space using a so-called Fradkin-Vasiliev approach, which works only for the non-zero cosmological constant. The... | 10.875951 | 8.600023 | 11.020626 | 8.329669 | 9.591917 | 8.251527 | 8.399466 | 8.558406 | 8.462996 | 12.866686 | 8.768499 | 9.313227 | 9.898866 | 9.063828 | 9.209674 | 9.261488 | 9.029637 | 8.843431 | 9.095098 | 10.191895 | 9.075976 |
2202.03048 | Mahya Mohammadi | Mahya Mohammadi and Ahmad Sheykhi | Gauss-Bonnet holographic superconductors in lower-dimensions | 15 pages. arXiv admin note: substantial text overlap with
arXiv:1908.07992 | Eur. Phys. J. Plus 137, 852 (2022) | 10.1140/epjp/s13360-022-03056-0 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We disclose the effect of Gauss-Bonnet gravity on the properties of
holographic $s$-wave and $p$-wave superconductors with higher order corrections
in lower-dimensional spacetime. We employ shooting method to solve equations of
motion numerically and obtain the effect of different values of mass, nonlinear
gauge fiel... | [
{
"created": "Mon, 7 Feb 2022 10:27:30 GMT",
"version": "v1"
},
{
"created": "Sun, 21 Aug 2022 16:15:04 GMT",
"version": "v2"
}
] | 2022-09-29 | [
[
"Mohammadi",
"Mahya",
""
],
[
"Sheykhi",
"Ahmad",
""
]
] | We disclose the effect of Gauss-Bonnet gravity on the properties of holographic $s$-wave and $p$-wave superconductors with higher order corrections in lower-dimensional spacetime. We employ shooting method to solve equations of motion numerically and obtain the effect of different values of mass, nonlinear gauge field ... | 7.639361 | 6.967191 | 8.126284 | 7.039267 | 7.184804 | 7.123196 | 7.071781 | 7.054677 | 7.5075 | 8.862309 | 7.124847 | 7.406806 | 7.794629 | 7.448696 | 7.390882 | 7.605443 | 7.53805 | 7.497083 | 7.363901 | 7.806271 | 7.356296 |
hep-th/9412129 | Jouko Mickelsson | Edwin Langmann and Jouko Mickelsson | Elementary Derivation of the Chiral Anomaly | Minor errors and misprints corrected, a reference added. AmsTex file,
12 output pages. If you do not have preloaded AmsTex you have to \input
amstex.tex | Lett. Math. Phys. 36 (1996) 45 | 10.1007/BF00403250 | null | hep-th | null | An elementary derivation of the chiral gauge anomaly in all even dimensions
is given in terms of noncommutative traces of pseudo-differential operators.
| [
{
"created": "Thu, 15 Dec 1994 12:24:42 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Jan 1995 12:18:45 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Langmann",
"Edwin",
""
],
[
"Mickelsson",
"Jouko",
""
]
] | An elementary derivation of the chiral gauge anomaly in all even dimensions is given in terms of noncommutative traces of pseudo-differential operators. | 14.998248 | 9.682597 | 12.66901 | 9.371747 | 10.024564 | 8.50763 | 8.390093 | 9.445284 | 8.559286 | 13.77595 | 9.580791 | 9.469543 | 12.149277 | 9.882589 | 10.12629 | 9.698766 | 9.611089 | 9.874902 | 10.023794 | 11.737416 | 10.209903 |
0707.3858 | Sachindeo Vaidya | Sachindeo Vaidya | The quantum sinh-Gordon model in noncommutative (1+1) dimensions | 7 pages, 2 figures, LaTex. References added | Phys.Lett.B655:294-297,2007 | 10.1016/j.physletb.2007.08.089 | IISc/CHEP/10/07 | hep-th | null | Using twisted commutation relations we show that the quantum sinh-Gordon
model on noncommutative space is integrable, and compute the exact two-particle
scattering matrix. The model possesses a strong-weak duality, just like its
commutative counterpart.
| [
{
"created": "Thu, 26 Jul 2007 05:56:10 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Aug 2007 06:12:38 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Vaidya",
"Sachindeo",
""
]
] | Using twisted commutation relations we show that the quantum sinh-Gordon model on noncommutative space is integrable, and compute the exact two-particle scattering matrix. The model possesses a strong-weak duality, just like its commutative counterpart. | 9.135023 | 6.027495 | 9.942405 | 6.476271 | 6.034019 | 5.486239 | 6.523564 | 6.848883 | 6.589614 | 8.613657 | 6.090785 | 6.802417 | 8.287119 | 6.79068 | 7.220629 | 7.141115 | 6.52883 | 6.809785 | 6.739512 | 8.025537 | 6.809207 |
1911.00589 | Sahand Seifnashri | J.P. Ang, Konstantinos Roumpedakis, Sahand Seifnashri | Line Operators of Gauge Theories on Non-Spin Manifolds | 53 | null | 10.1007/JHEP04(2020)087 | YITP-SB-19-39 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study four-dimensional gauge theories on oriented and non-spin spacetime
manifolds. On such manifolds, each line operator arises only either as a boson
or a fermion. Based on physical arguments, a method of systematically assigning
spin labels to line operators is proposed, and several consistency checks are
perfo... | [
{
"created": "Fri, 1 Nov 2019 21:02:40 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Feb 2020 22:16:25 GMT",
"version": "v2"
}
] | 2020-05-20 | [
[
"Ang",
"J. P.",
""
],
[
"Roumpedakis",
"Konstantinos",
""
],
[
"Seifnashri",
"Sahand",
""
]
] | We study four-dimensional gauge theories on oriented and non-spin spacetime manifolds. On such manifolds, each line operator arises only either as a boson or a fermion. Based on physical arguments, a method of systematically assigning spin labels to line operators is proposed, and several consistency checks are perform... | 8.657305 | 8.869155 | 9.144528 | 7.968921 | 8.633645 | 8.820213 | 8.944389 | 7.82664 | 8.56455 | 10.545634 | 8.392152 | 8.331891 | 8.876688 | 8.080637 | 8.422783 | 8.247863 | 8.386212 | 8.467415 | 8.289034 | 9.086617 | 7.917576 |
hep-th/9812089 | Igor Klebanov | Igor R. Klebanov and Arkady A. Tseytlin | Asymptotic Freedom and Infrared Behavior in the Type 0 String Approach
to Gauge Theory | 15 pages, harvmac; v2: a reference added; v3: last section revised;
v4: numerical coefficients corrected | Nucl.Phys.B547:143-156,1999 | 10.1016/S0550-3213(99)00084-X | PUPT-1825, Imperial/TP/98-99/20 | hep-th | null | In a recent paper we considered the type 0 string theories, obtained from the
ten-dimensional closed NSR string by a GSO projection which excludes space-time
fermions, and studied the low-energy dynamics of N coincident D-branes. This
led us to conjecture that the four-dimensional SU(N) gauge theory coupled to 6
adjo... | [
{
"created": "Thu, 10 Dec 1998 19:47:21 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Dec 1998 20:47:11 GMT",
"version": "v2"
},
{
"created": "Thu, 21 Jan 1999 20:42:51 GMT",
"version": "v3"
},
{
"created": "Wed, 3 Feb 1999 21:03:04 GMT",
"version": "v4"
}
] | 2009-09-17 | [
[
"Klebanov",
"Igor R.",
""
],
[
"Tseytlin",
"Arkady A.",
""
]
] | In a recent paper we considered the type 0 string theories, obtained from the ten-dimensional closed NSR string by a GSO projection which excludes space-time fermions, and studied the low-energy dynamics of N coincident D-branes. This led us to conjecture that the four-dimensional SU(N) gauge theory coupled to 6 adjoin... | 8.089024 | 7.646969 | 9.554105 | 6.890331 | 8.455409 | 7.520198 | 7.383542 | 6.997878 | 7.235005 | 8.92814 | 7.355052 | 7.217555 | 7.758801 | 7.469961 | 7.356403 | 7.493837 | 7.377678 | 7.50073 | 7.239461 | 7.763037 | 7.502424 |
1704.01967 | Florian Loebbert | Dmitry Chicherin, Vladimir Kazakov, Florian Loebbert, Dennis M\"uller,
De-liang Zhong | Yangian Symmetry for Bi-Scalar Loop Amplitudes | 40 pages, 20 figures | JHEP05(2018)003 | 10.1007/JHEP05(2018)003 | HU-EP-17/09, LPTENS/17/07, MITP/17-022 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish an all-loop conformal Yangian symmetry for the full set of
planar amplitudes in the recently proposed integrable bi-scalar field theory in
four dimensions. This chiral theory is a particular double scaling limit of
gamma-twisted weakly coupled N=4 SYM theory. Each amplitude with a certain
order of scalar... | [
{
"created": "Thu, 6 Apr 2017 18:00:00 GMT",
"version": "v1"
}
] | 2018-05-08 | [
[
"Chicherin",
"Dmitry",
""
],
[
"Kazakov",
"Vladimir",
""
],
[
"Loebbert",
"Florian",
""
],
[
"Müller",
"Dennis",
""
],
[
"Zhong",
"De-liang",
""
]
] | We establish an all-loop conformal Yangian symmetry for the full set of planar amplitudes in the recently proposed integrable bi-scalar field theory in four dimensions. This chiral theory is a particular double scaling limit of gamma-twisted weakly coupled N=4 SYM theory. Each amplitude with a certain order of scalar p... | 10.612942 | 10.198979 | 12.289614 | 9.918478 | 11.348865 | 11.762744 | 10.867148 | 9.899099 | 10.668307 | 14.029977 | 10.012728 | 10.256121 | 10.999219 | 10.486006 | 10.745509 | 10.781915 | 10.704082 | 10.304182 | 10.129424 | 10.442665 | 10.101641 |
hep-th/0006107 | null | R. D'Auria, S. Ferrara and S. Vaul\`a | Matter Coupled F(4) Supergravity and the AdS_6/CFT_5 Correspondence | 21 pages, latex, minor corrections and reference added | JHEP 0010:013,2000 | 10.1088/1126-6708/2000/10/013 | CERN-TH/2000-167 | hep-th | null | F(4) supergravity, the gauge theory of the exceptional six-dimensional
Anti-de Sitter superalgebra, is coupled to an arbitrary number of vector
multiplets whose scalar components parametrize the quaternionic manifold
$SO(4,n)/SO(4)\times SO(n)$. By gauging the compact subgroup $SU(2)_d \otimes
\cG$, where SU(2)_d is ... | [
{
"created": "Thu, 15 Jun 2000 12:06:06 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Jul 2000 13:35:55 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"D'Auria",
"R.",
""
],
[
"Ferrara",
"S.",
""
],
[
"Vaulà",
"S.",
""
]
] | F(4) supergravity, the gauge theory of the exceptional six-dimensional Anti-de Sitter superalgebra, is coupled to an arbitrary number of vector multiplets whose scalar components parametrize the quaternionic manifold $SO(4,n)/SO(4)\times SO(n)$. By gauging the compact subgroup $SU(2)_d \otimes \cG$, where SU(2)_d is th... | 7.699032 | 6.06736 | 9.16332 | 6.515495 | 7.569861 | 5.997357 | 6.191794 | 5.958798 | 6.665748 | 8.976526 | 6.525167 | 6.838456 | 7.831937 | 7.014225 | 7.24982 | 6.892284 | 6.825441 | 6.846756 | 7.015181 | 7.625472 | 7.035786 |
1408.0094 | Anirban Basu | Anirban Basu | Constraining non--BPS interactions from counterterms in three loop
maximal supergravity | 31 pages, LaTeX, 8 figures | null | 10.1088/0264-9381/32/4/045012 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The structure of one, two and three loop counterterms imposes strong
constraints on several non--BPS interactions in the low momentum expansion of
the three loop four graviton amplitude in maximal supergravity. The constraints
are imposed by demanding consistency with string amplitudes. We analyze these
constraints i... | [
{
"created": "Fri, 1 Aug 2014 07:33:19 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Mar 2015 18:30:40 GMT",
"version": "v2"
},
{
"created": "Sat, 10 Oct 2015 11:31:22 GMT",
"version": "v3"
}
] | 2015-10-13 | [
[
"Basu",
"Anirban",
""
]
] | The structure of one, two and three loop counterterms imposes strong constraints on several non--BPS interactions in the low momentum expansion of the three loop four graviton amplitude in maximal supergravity. The constraints are imposed by demanding consistency with string amplitudes. We analyze these constraints imp... | 12.949997 | 10.168051 | 14.480062 | 10.909897 | 10.246638 | 10.926445 | 9.808618 | 9.459829 | 9.777981 | 15.335107 | 10.616644 | 11.589762 | 13.571503 | 11.673983 | 11.016461 | 11.629981 | 11.144691 | 11.713341 | 11.675687 | 13.52759 | 12.111968 |
hep-th/0607193 | Eric Bergshoeff | Eric A. Bergshoeff, Gary W. Gibbons and Paul K. Townsend | Open M5-branes | 4 pages, 3 figures, version to appear in PRL | Phys.Rev.Lett.97:231601,2006 | 10.1103/PhysRevLett.97.231601 | DAMTP-2006-42; UG-06-06 | hep-th | null | We show how, in heterotic M-theory, an M5-brane in the 11-dimensional bulk
may end on an ``M9-brane'' boundary, the M5-brane boundary being a Yang
monopole 4-brane. This possibility suggests various novel 5-brane
configurations of heterotic M-theory, in particular a static M5-brane suspended
between the two M9-brane ... | [
{
"created": "Tue, 25 Jul 2006 13:26:12 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Dec 2006 10:25:57 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bergshoeff",
"Eric A.",
""
],
[
"Gibbons",
"Gary W.",
""
],
[
"Townsend",
"Paul K.",
""
]
] | We show how, in heterotic M-theory, an M5-brane in the 11-dimensional bulk may end on an ``M9-brane'' boundary, the M5-brane boundary being a Yang monopole 4-brane. This possibility suggests various novel 5-brane configurations of heterotic M-theory, in particular a static M5-brane suspended between the two M9-brane bo... | 9.352319 | 8.381168 | 9.963959 | 7.957537 | 8.095307 | 8.176463 | 8.90543 | 7.944476 | 8.109704 | 10.000689 | 7.988719 | 8.242245 | 8.86526 | 7.935992 | 7.967953 | 8.21759 | 7.752293 | 8.352009 | 8.027379 | 9.035415 | 8.333771 |
1208.0354 | Gianluca Calcagni | Gianluca Calcagni, Daniele Oriti, Johannes Th\"urigen | Laplacians on discrete and quantum geometries | 43 pages, 2 multiple figures. v2: discussion improved, references
added, minor typos corrected | Class. Quantum Grav. 30 (2013) 125006 | 10.1088/0264-9381/30/12/125006 | AEI-2012-078 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend discrete calculus for arbitrary ($p$-form) fields on embedded
lattices to abstract discrete geometries based on combinatorial complexes. We
then provide a general definition of discrete Laplacian using both the primal
cellular complex and its combinatorial dual. The precise implementation of
geometric volum... | [
{
"created": "Wed, 1 Aug 2012 20:44:38 GMT",
"version": "v1"
},
{
"created": "Fri, 17 May 2013 08:15:05 GMT",
"version": "v2"
}
] | 2013-05-20 | [
[
"Calcagni",
"Gianluca",
""
],
[
"Oriti",
"Daniele",
""
],
[
"Thürigen",
"Johannes",
""
]
] | We extend discrete calculus for arbitrary ($p$-form) fields on embedded lattices to abstract discrete geometries based on combinatorial complexes. We then provide a general definition of discrete Laplacian using both the primal cellular complex and its combinatorial dual. The precise implementation of geometric volume ... | 12.058825 | 14.484447 | 12.903496 | 12.371069 | 14.652698 | 12.968087 | 13.167704 | 12.731335 | 12.658461 | 14.14968 | 11.939613 | 12.257548 | 12.490256 | 12.046706 | 12.487356 | 12.274792 | 12.746034 | 12.361692 | 12.250764 | 12.433187 | 12.148573 |
2201.01630 | Sabrina Pasterski | Sabrina Pasterski and Herman Verlinde | Chaos in Celestial CFT | 29 pages, 6 figures | null | 10.1007/JHEP08(2022)106 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Celestial holography proposes a duality between gravitational scattering in
asymptotically flat space-time and a conformal field theory living on the
celestial sphere. Its dictionary relates the infinite dimensional space-time
symmetry group to Ward identities of the CFT. The spontaneous breaking of these
asymptotic ... | [
{
"created": "Wed, 5 Jan 2022 14:21:21 GMT",
"version": "v1"
}
] | 2022-08-24 | [
[
"Pasterski",
"Sabrina",
""
],
[
"Verlinde",
"Herman",
""
]
] | Celestial holography proposes a duality between gravitational scattering in asymptotically flat space-time and a conformal field theory living on the celestial sphere. Its dictionary relates the infinite dimensional space-time symmetry group to Ward identities of the CFT. The spontaneous breaking of these asymptotic sy... | 9.874514 | 9.173012 | 10.52152 | 8.769604 | 9.316318 | 9.046144 | 9.091206 | 8.736589 | 8.647207 | 11.379259 | 8.560719 | 8.540583 | 8.92931 | 8.612496 | 8.964146 | 8.733215 | 8.584082 | 8.62535 | 8.716902 | 9.122927 | 8.783775 |
2108.11621 | Qi-Feng Wu | Qi-Feng Wu | Sectional curvatures distribution of complexity geometry | 23 pages, 4 figures | JHEP08(2022)197 | 10.1007/JHEP08(2022)197 | null | hep-th quant-ph | http://creativecommons.org/licenses/by/4.0/ | In the geometric approach to define complexity, operator complexity is
defined as the distance on the operator space. In this paper, based on the
analogy with the circuit complexity, the operator size is adopted as the metric
of the operator space where path length is the complexity. The typical
sectional curvatures ... | [
{
"created": "Thu, 26 Aug 2021 07:23:03 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Nov 2021 09:38:27 GMT",
"version": "v2"
},
{
"created": "Sun, 21 Aug 2022 02:15:48 GMT",
"version": "v3"
}
] | 2022-08-23 | [
[
"Wu",
"Qi-Feng",
""
]
] | In the geometric approach to define complexity, operator complexity is defined as the distance on the operator space. In this paper, based on the analogy with the circuit complexity, the operator size is adopted as the metric of the operator space where path length is the complexity. The typical sectional curvatures of... | 11.70592 | 11.425611 | 11.94892 | 10.061728 | 11.207183 | 11.277759 | 10.927868 | 10.651698 | 10.24824 | 11.934955 | 10.864239 | 10.61596 | 10.212055 | 10.448961 | 10.599502 | 10.522535 | 10.420796 | 10.800341 | 10.631974 | 10.319843 | 10.614376 |
0901.0130 | Sergei Parkhomenko | S.E.Parkhomenko | Gepner-like models and Landau-Ginzburg/sigma-model correspondence | null | J.Phys.A42:304023,2009 | 10.1088/1751-8113/42/30/304023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Gepner-like models of $k^{K}$-type is considered. When $k+2$ is multiple
of $K$ the elliptic genus and the Euler characteristic is calculated. Using
free-field representation we relate these models with $\sigma$-models on
hypersurfaces in the total space of anticanonical bundle over the projective
space $\mathbb{... | [
{
"created": "Wed, 31 Dec 2008 19:10:26 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Jan 2009 14:03:53 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Jan 2009 16:29:51 GMT",
"version": "v3"
},
{
"created": "Thu, 5 Mar 2009 13:33:40 GMT",
"version": "v4"
},
{
"cr... | 2010-02-13 | [
[
"Parkhomenko",
"S. E.",
""
]
] | The Gepner-like models of $k^{K}$-type is considered. When $k+2$ is multiple of $K$ the elliptic genus and the Euler characteristic is calculated. Using free-field representation we relate these models with $\sigma$-models on hypersurfaces in the total space of anticanonical bundle over the projective space $\mathbb{P}... | 11.430727 | 9.891003 | 10.658669 | 9.685052 | 9.673672 | 9.670554 | 10.075942 | 9.666089 | 9.397223 | 11.211186 | 9.622289 | 9.146901 | 10.864465 | 9.546268 | 9.824654 | 9.733274 | 9.540111 | 9.560045 | 9.454342 | 10.267426 | 9.597876 |
hep-th/9601092 | Slavnov | T.D.Bakeyev, A.A.Slavnov | Higher covariant derivative regularization revisited | 14 pages, latex, 1 figure | Mod.Phys.Lett. A11 (1996) 1539-1554 | 10.1142/S0217732396001533 | SMI-02-96 | hep-th | null | The method of higher covariant derivative regularization of gauge theories is
reviewed. The objections raised in the literature last years are discussed and
the consistency of the method is proven. New approach to regularization of
overlapping divergencies is developped.
| [
{
"created": "Thu, 18 Jan 1996 11:16:16 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Bakeyev",
"T. D.",
""
],
[
"Slavnov",
"A. A.",
""
]
] | The method of higher covariant derivative regularization of gauge theories is reviewed. The objections raised in the literature last years are discussed and the consistency of the method is proven. New approach to regularization of overlapping divergencies is developped. | 15.074479 | 12.447875 | 12.664416 | 10.769395 | 11.529428 | 11.30851 | 12.328519 | 12.617887 | 10.753354 | 12.080562 | 10.810926 | 12.378873 | 12.617415 | 11.526416 | 12.573027 | 12.422811 | 11.847541 | 13.08958 | 11.986701 | 12.459105 | 12.406793 |
2201.01657 | Jonas Sommerfeldt | J. Sommerfeldt, V. A. Yerokhin, R. A. M\"uller, V. A. Zaytsev, A. V.
Volotka and A. Surzhykov | Calculations of Delbr\"uck scattering to all orders in $\alpha Z$ | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a theoretical method to calculate Delbr\"uck scattering
amplitudes. Our formalism is based on the exact analytical Dirac-Coulomb
Green's function and, therefore, accounts for the interaction of the virtual
electron-positron pair with the nucleus to all orders, including the Coulomb
corrections. The numeric... | [
{
"created": "Wed, 5 Jan 2022 15:24:53 GMT",
"version": "v1"
}
] | 2022-01-06 | [
[
"Sommerfeldt",
"J.",
""
],
[
"Yerokhin",
"V. A.",
""
],
[
"Müller",
"R. A.",
""
],
[
"Zaytsev",
"V. A.",
""
],
[
"Volotka",
"A. V.",
""
],
[
"Surzhykov",
"A.",
""
]
] | We present a theoretical method to calculate Delbr\"uck scattering amplitudes. Our formalism is based on the exact analytical Dirac-Coulomb Green's function and, therefore, accounts for the interaction of the virtual electron-positron pair with the nucleus to all orders, including the Coulomb corrections. The numerical... | 6.9892 | 8.452045 | 7.302357 | 7.186107 | 7.36202 | 8.630359 | 7.908413 | 8.409593 | 6.984621 | 7.793668 | 7.516471 | 7.763313 | 7.29941 | 6.779686 | 7.355678 | 7.594795 | 7.337481 | 7.559808 | 6.6428 | 7.186339 | 7.33332 |
hep-th/9806163 | Roberto Soldati | Michele Morara and Roberto Soldati | Consistent perturbative light-front formulation of quantum
electrodynamics | PlainTeX, 29 pages, 5 Postscript figures | Phys.Rev. D58 (1998) 105011 | 10.1103/PhysRevD.58.105011 | DFUB-97-17 | hep-th | null | A new light-front formulation of Q.E.D. is developed, within the framework of
standard perturbation theory, in which $x^+$ plays the role of the evolution
parameter and the gauge choice is $A_+=0$ (light-front "temporal" gauge). It is
shown that this formulation leads to the Mandelstam-Leibbrandt causal
prescription ... | [
{
"created": "Fri, 19 Jun 1998 09:01:48 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Morara",
"Michele",
""
],
[
"Soldati",
"Roberto",
""
]
] | A new light-front formulation of Q.E.D. is developed, within the framework of standard perturbation theory, in which $x^+$ plays the role of the evolution parameter and the gauge choice is $A_+=0$ (light-front "temporal" gauge). It is shown that this formulation leads to the Mandelstam-Leibbrandt causal prescription fo... | 8.099365 | 7.592251 | 7.881111 | 7.475323 | 8.049467 | 7.55573 | 8.158556 | 7.398849 | 7.655713 | 8.597241 | 7.307071 | 6.928771 | 7.732864 | 7.734974 | 7.501354 | 7.010335 | 7.419823 | 7.409333 | 7.312908 | 7.87324 | 7.165466 |
hep-th/0012047 | John F. Donoghue | John F. Donoghue | Random values of the physical parameters | 3 pages, talk presented at the Division of Particles and Fields
Meeting, DPF 2000, Columbus, Ohio, Aug. 2000 | Int.J.Mod.Phys. A16S1C (2001) 902-904 | 10.1142/S0217751X01008448 | null | hep-th hep-ph | null | I briefly describe two motivations, two mechanisms and two possible tests of
the hypothesis that the physical parameters of the ground state of a theory can
vary in different regions of the universe.
| [
{
"created": "Wed, 6 Dec 2000 19:17:26 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Donoghue",
"John F.",
""
]
] | I briefly describe two motivations, two mechanisms and two possible tests of the hypothesis that the physical parameters of the ground state of a theory can vary in different regions of the universe. | 23.39929 | 19.408922 | 15.497816 | 16.048643 | 14.787773 | 17.031498 | 15.908273 | 16.512568 | 15.511941 | 20.142935 | 16.885227 | 16.810663 | 16.041397 | 15.83171 | 15.736857 | 16.115513 | 16.023664 | 17.241276 | 16.889492 | 16.548431 | 17.993811 |
0708.0240 | Reza Fraeghbal | H. Arfaei, R. Fareghbal | Double Horizon Limit, AdS Geometry and Entropy Function | 19 pages- minor correction - published version | Nucl.Phys.B802:405-420,2008 | 10.1016/j.nuclphysb.2008.04.017 | IPM/P-2007/050, SUT-P-07-2b | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We start from a generic metric which describes four dimensional stationary
black holes in an arbitrary theory of gravity and show that the AdS_2 part of
the near horizon geometry is a consequence of the double-horizon limit and
finiteness . We also show that the field configurations of the near horizon are
determined... | [
{
"created": "Wed, 1 Aug 2007 23:02:01 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Nov 2007 11:01:04 GMT",
"version": "v2"
},
{
"created": "Sat, 12 Jul 2008 08:11:30 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Arfaei",
"H.",
""
],
[
"Fareghbal",
"R.",
""
]
] | We start from a generic metric which describes four dimensional stationary black holes in an arbitrary theory of gravity and show that the AdS_2 part of the near horizon geometry is a consequence of the double-horizon limit and finiteness . We also show that the field configurations of the near horizon are determined i... | 9.270121 | 8.813938 | 9.587496 | 8.826518 | 8.911108 | 8.798412 | 9.182294 | 8.522102 | 8.636106 | 9.092753 | 8.575398 | 8.975463 | 8.865842 | 8.742248 | 8.92407 | 9.051185 | 8.703522 | 8.92467 | 8.695558 | 9.083817 | 8.659437 |
hep-th/0510068 | Pietro Fre | Pietro Fre' | M-theory FDA, Twisted Tori and Chevalley Cohomology | LaTeX, 40 pages, article. Few typos corrected, one formula improved | Nucl.Phys.B742:86-123,2006 | 10.1016/j.nuclphysb.2006.02.008 | DFTT/05/33 | hep-th | null | The FDA algebras emerging from twisted tori compactifications of M-theory
with fluxes are discussed within the general classification scheme provided by
Sullivan's theorems and by Chevalley cohomology. It is shown that the
generalized Maurer Cartan equations which have appeared in the literature, in
spite of their co... | [
{
"created": "Sun, 9 Oct 2005 14:00:47 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Oct 2005 16:09:38 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Fre'",
"Pietro",
""
]
] | The FDA algebras emerging from twisted tori compactifications of M-theory with fluxes are discussed within the general classification scheme provided by Sullivan's theorems and by Chevalley cohomology. It is shown that the generalized Maurer Cartan equations which have appeared in the literature, in spite of their comp... | 17.064583 | 18.146692 | 18.570948 | 16.194366 | 17.291502 | 16.378038 | 15.961651 | 16.262863 | 15.844254 | 19.498322 | 14.639079 | 15.624961 | 16.205853 | 15.10883 | 15.682376 | 15.835979 | 15.105906 | 15.291484 | 15.517983 | 16.344118 | 15.779025 |
2006.12452 | Chris Blair | Chris D. A. Blair, Daniel C. Thompson, Sofia Zhidkova | Exploring Exceptional Drinfeld Geometries | 24 pages + appendices + refs. v2: published version | JHEP 09 (2020) 151 | 10.1007/JHEP09(2020)151 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore geometries that give rise to a novel algebraic structure, the
Exceptional Drinfeld Algebra, which has recently been proposed as an approach
to study generalised U-dualities, similar to the non-Abelian and Poisson-Lie
generalisations of T-duality. This algebra is generically not a Lie algebra but
a Leibniz ... | [
{
"created": "Mon, 22 Jun 2020 17:35:47 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Oct 2020 18:15:11 GMT",
"version": "v2"
}
] | 2020-10-14 | [
[
"Blair",
"Chris D. A.",
""
],
[
"Thompson",
"Daniel C.",
""
],
[
"Zhidkova",
"Sofia",
""
]
] | We explore geometries that give rise to a novel algebraic structure, the Exceptional Drinfeld Algebra, which has recently been proposed as an approach to study generalised U-dualities, similar to the non-Abelian and Poisson-Lie generalisations of T-duality. This algebra is generically not a Lie algebra but a Leibniz al... | 9.597332 | 8.419817 | 11.55966 | 8.136926 | 8.340246 | 8.847393 | 8.316199 | 8.763381 | 8.717444 | 13.787217 | 8.167507 | 8.816965 | 9.558326 | 8.928263 | 8.818102 | 8.882151 | 9.120049 | 8.781843 | 9.064734 | 10.028289 | 8.937218 |
2210.16597 | Poula Tadros | Poula Tadros and Iiro Vilja | Low energy models of string theory | Derived from MSc thesis | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | String theory is the prime candidate for the theory of everything. However,
it must be defined in ten dimensions to be consistent. To get 4D physics, the 6
other dimensions should be curled up in a small compact manifold, this
procedure is called string compactification. In this review, we will review
different compa... | [
{
"created": "Sat, 29 Oct 2022 13:33:57 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Nov 2022 08:41:18 GMT",
"version": "v2"
}
] | 2022-11-02 | [
[
"Tadros",
"Poula",
""
],
[
"Vilja",
"Iiro",
""
]
] | String theory is the prime candidate for the theory of everything. However, it must be defined in ten dimensions to be consistent. To get 4D physics, the 6 other dimensions should be curled up in a small compact manifold, this procedure is called string compactification. In this review, we will review different compact... | 8.658539 | 9.379535 | 9.539465 | 8.942406 | 8.941605 | 8.982984 | 8.847673 | 8.854917 | 8.491084 | 10.076649 | 8.474303 | 8.584266 | 8.617105 | 8.343873 | 8.028392 | 8.17439 | 8.243292 | 8.254825 | 8.379336 | 8.589745 | 8.134523 |
hep-th/9910227 | Vasiliy A. Dolgushev | V.A. Dolgushev | Polynomial Gauge Invariants of a Bosonic String | 4 pages, Latexfile, Talk presented at the QFTHEP'99, Moscow, 27 May -
2 June | null | null | null | hep-th | null | An open bosonic string is considered with the aim to construct a general
gauge invariant, being a polynomial of Fubini-Veneziano (FV) fields. The FV
fields are transformed as 1-forms on $S^1$, that allows to formulate the
problem in geometric terms. We introduce a most general anzats for these
invariants and explicit... | [
{
"created": "Thu, 28 Oct 1999 11:59:11 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dolgushev",
"V. A.",
""
]
] | An open bosonic string is considered with the aim to construct a general gauge invariant, being a polynomial of Fubini-Veneziano (FV) fields. The FV fields are transformed as 1-forms on $S^1$, that allows to formulate the problem in geometric terms. We introduce a most general anzats for these invariants and explicitly... | 13.512141 | 14.283587 | 14.07822 | 13.0132 | 14.248716 | 13.605507 | 13.067883 | 12.911358 | 13.299122 | 14.682178 | 12.733429 | 12.626417 | 13.104671 | 12.623882 | 12.631542 | 12.811083 | 12.82128 | 13.010967 | 13.037419 | 13.294214 | 12.527837 |
hep-th/0310210 | M. Meyer | Howard J. Schnitzer | Gauged Vector Models and Higher-Spin Representations in AdS_5 | 18 pages, LaTex, 1 figure, v. 2, references added; a minor correction | Nucl.Phys. B695 (2004) 283-300 | 10.1016/j.nuclphysb.2004.06.055 | BRX TH-524 | hep-th | null | Motivated by the work of Klebanov and Polyakov [hep-th/0210114] on the
relationship of the large N O(N) vector model in three-dimensions to AdS_4 and
higher spin representations, we attempt to find analogous connections for
AdS_5. Since the usual O(N) vector model in four-dimensions is inconsistent, we
consider the (... | [
{
"created": "Wed, 22 Oct 2003 19:13:44 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Nov 2003 18:49:30 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Schnitzer",
"Howard J.",
""
]
] | Motivated by the work of Klebanov and Polyakov [hep-th/0210114] on the relationship of the large N O(N) vector model in three-dimensions to AdS_4 and higher spin representations, we attempt to find analogous connections for AdS_5. Since the usual O(N) vector model in four-dimensions is inconsistent, we consider the (co... | 8.488333 | 8.997048 | 10.76261 | 7.788832 | 8.419614 | 8.296591 | 8.749181 | 8.818969 | 8.304161 | 10.788535 | 8.736693 | 8.164055 | 8.50404 | 8.24958 | 8.231018 | 8.067241 | 8.380727 | 8.027249 | 8.003858 | 8.45939 | 8.148873 |
0904.0188 | Antonio De Felice | Antonio De Felice, Christophe Ringeval | Charged seven-dimensional spacetimes with spherically symmetric
extra-dimensions | 14 pages, 8 figures, uses RevTeX. Physical discussion clarified,
wormhole solutions added. References added | Phys.Rev.D79:123525,2009 | 10.1103/PhysRevD.79.123525 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive exact solutions of the seven-dimensional Einstein-Maxwell equations
for a spacetime exhibiting Poincare invariance along four-dimensions and
spherical symmetry in the extra-dimensions. Such topology generically arises in
the context of braneworld models. Our solutions generalise previous results on
Ricci-fl... | [
{
"created": "Wed, 1 Apr 2009 15:38:44 GMT",
"version": "v1"
},
{
"created": "Thu, 14 May 2009 15:22:34 GMT",
"version": "v2"
}
] | 2009-07-09 | [
[
"De Felice",
"Antonio",
""
],
[
"Ringeval",
"Christophe",
""
]
] | We derive exact solutions of the seven-dimensional Einstein-Maxwell equations for a spacetime exhibiting Poincare invariance along four-dimensions and spherical symmetry in the extra-dimensions. Such topology generically arises in the context of braneworld models. Our solutions generalise previous results on Ricci-flat... | 11.85112 | 11.077028 | 10.984714 | 10.155487 | 11.036031 | 11.408908 | 11.195464 | 10.732006 | 10.262331 | 11.668729 | 10.875875 | 11.021285 | 11.143156 | 10.732917 | 11.013888 | 10.906849 | 10.845497 | 11.157771 | 10.719532 | 11.598965 | 10.55695 |
2404.10127 | Cielo Ramirez De Arellano Torres | Mariano Chernicoff, Gaston Giribet, Javier Moreno, Julio Oliva, Raul
Rojas, Cielo Ramirez de Arellano Torres | Quantum backreactions in (A)dS3 massive gravity and logarithmic
asymptotic behavior | 16 pages | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We study the interplay between higher curvature terms and the backreaction of
quantum fluctuations in 3-dimensional massive gravity in asymptotically
(Anti-)de Sitter space. We focus on the theory at the special point of the
parameter space where the two maximally symmetric vacua coincide. In the case
of positive cos... | [
{
"created": "Mon, 15 Apr 2024 20:30:37 GMT",
"version": "v1"
}
] | 2024-04-17 | [
[
"Chernicoff",
"Mariano",
""
],
[
"Giribet",
"Gaston",
""
],
[
"Moreno",
"Javier",
""
],
[
"Oliva",
"Julio",
""
],
[
"Rojas",
"Raul",
""
],
[
"Torres",
"Cielo Ramirez de Arellano",
""
]
] | We study the interplay between higher curvature terms and the backreaction of quantum fluctuations in 3-dimensional massive gravity in asymptotically (Anti-)de Sitter space. We focus on the theory at the special point of the parameter space where the two maximally symmetric vacua coincide. In the case of positive cosmo... | 8.325914 | 7.785233 | 8.270756 | 7.568685 | 8.231536 | 7.75988 | 7.621711 | 7.843019 | 7.65549 | 8.94191 | 7.510485 | 7.914105 | 8.459321 | 8.064508 | 8.170664 | 8.008914 | 7.695881 | 7.897161 | 8.146013 | 8.306893 | 7.979039 |
0812.0620 | Klaus Kirsten | Gerald Dunne and Klaus Kirsten | Simplified Vacuum Energy Expressions for Radial Backgrounds and Domain
Walls | 30 pages | J.Phys.A42:075402,2009 | 10.1088/1751-8113/42/7/075402 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend our previous results of simplified expressions for functional
determinants for radial Schr\"odinger operators to the computation of vacuum
energy, or mass corrections, for static but spatially radial backgrounds, and
for domain wall configurations. Our method is based on the zeta function
approach to the Ge... | [
{
"created": "Tue, 2 Dec 2008 23:41:57 GMT",
"version": "v1"
}
] | 2009-03-12 | [
[
"Dunne",
"Gerald",
""
],
[
"Kirsten",
"Klaus",
""
]
] | We extend our previous results of simplified expressions for functional determinants for radial Schr\"odinger operators to the computation of vacuum energy, or mass corrections, for static but spatially radial backgrounds, and for domain wall configurations. Our method is based on the zeta function approach to the Gel'... | 14.805708 | 12.645324 | 14.894044 | 13.195848 | 13.421057 | 13.352651 | 15.163066 | 13.555217 | 13.432571 | 14.336461 | 13.184673 | 13.259515 | 13.444539 | 12.902357 | 13.672092 | 13.635716 | 13.611661 | 13.491718 | 13.182291 | 13.291159 | 13.288877 |
hep-th/9511225 | Peter Johnson | Edwin J. Beggs, Peter R. Johnson (Wales, Swansea) | The generic soliton of the $A_n$ affine Toda field theories | 14 pages, 5 .eps figures, compressed tar file, print out plot4.eps
and plot5.eps separately | null | null | null | hep-th | null | In this note we show that the single soliton solutions known previously in
the $1+1$ dimensional affine Toda field theories from a variety of different
methods \cite{H1,MM,OTUa,OTUb}, are in fact not the most general single soliton
solutions. We exhibit single soliton solutions with additional small parameters
which ... | [
{
"created": "Thu, 30 Nov 1995 20:11:50 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Beggs",
"Edwin J.",
"",
"Wales, Swansea"
],
[
"Johnson",
"Peter R.",
"",
"Wales, Swansea"
]
] | In this note we show that the single soliton solutions known previously in the $1+1$ dimensional affine Toda field theories from a variety of different methods \cite{H1,MM,OTUa,OTUb}, are in fact not the most general single soliton solutions. We exhibit single soliton solutions with additional small parameters which re... | 8.242643 | 9.243216 | 8.898346 | 7.92298 | 9.009719 | 8.514927 | 8.217319 | 8.237972 | 8.093087 | 10.097993 | 8.216284 | 8.372992 | 8.80989 | 8.390553 | 8.481955 | 8.463859 | 8.538875 | 8.316897 | 8.387678 | 8.309755 | 8.030131 |
hep-th/0310199 | Manuel Barros | Josu Arroyo, Manuel Barros and Oscar J. Garay | Models of relativistic particle with curvature and torsion revisited | 13 pages | Gen.Rel.Grav. 36 (2004) 1441-1451 | 10.1023/B:GERG.0000022580.08717.40 | null | hep-th | null | Models, describing relativistic particles, where Lagrangian densities depend
linearly on both the curvature and the torsion of the trajectories, are
revisited in D=3 space forms. The moduli spaces of trajectories are completely
and explicitly determined using the Lancret program. The moduli subspaces of
closed solito... | [
{
"created": "Tue, 21 Oct 2003 09:22:25 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Arroyo",
"Josu",
""
],
[
"Barros",
"Manuel",
""
],
[
"Garay",
"Oscar J.",
""
]
] | Models, describing relativistic particles, where Lagrangian densities depend linearly on both the curvature and the torsion of the trajectories, are revisited in D=3 space forms. The moduli spaces of trajectories are completely and explicitly determined using the Lancret program. The moduli subspaces of closed solitons... | 24.467489 | 20.230223 | 25.387606 | 20.298035 | 21.979376 | 23.398493 | 21.14785 | 23.1577 | 19.912649 | 27.017929 | 22.913975 | 20.740683 | 22.961102 | 22.174267 | 21.698742 | 22.058704 | 22.272316 | 22.272924 | 21.890211 | 22.293858 | 20.950068 |
hep-th/0306207 | Paul H. Frampton | Paul H. Frampton and Thomas W. Kephart | Consistency Conditions for AdS/CFT Embeddings | 10 pages LaTeX | Int.J.Mod.Phys. A19 (2004) 593-598 | 10.1142/S0217751X04017902 | null | hep-th | null | The group embeddings used in orbifolding the AdS/CFT correspondence to arrive
at quiver gauge field theories are studied for both supersymmetric and
non-supersymmetric cases. For an orbifold $AdS_5 \times S^5/\Gamma$ the
conditions for embeddings of the finite group $\Gamma$ in the $SU(4) \sim O(6)$
isotropy of $S^5$... | [
{
"created": "Fri, 20 Jun 2003 19:58:30 GMT",
"version": "v1"
}
] | 2016-12-21 | [
[
"Frampton",
"Paul H.",
""
],
[
"Kephart",
"Thomas W.",
""
]
] | The group embeddings used in orbifolding the AdS/CFT correspondence to arrive at quiver gauge field theories are studied for both supersymmetric and non-supersymmetric cases. For an orbifold $AdS_5 \times S^5/\Gamma$ the conditions for embeddings of the finite group $\Gamma$ in the $SU(4) \sim O(6)$ isotropy of $S^5$ a... | 8.051947 | 7.152324 | 7.423009 | 6.739771 | 7.330126 | 7.274056 | 7.315204 | 7.004489 | 6.674556 | 8.317167 | 7.414824 | 7.383736 | 7.481437 | 7.104031 | 6.828272 | 7.128244 | 7.1566 | 7.300672 | 7.098575 | 7.677166 | 7.161747 |
2011.07062 | Nathan Benjamin | Nathan Benjamin, Christoph A. Keller, Hirosi Ooguri, Ida G. Zadeh | On Rational Points in CFT Moduli Spaces | 24 pages, 5 figures | null | 10.1007/JHEP04(2021)067 | CALT-TH 2020-050, IPMU20-0117 | hep-th | http://creativecommons.org/licenses/by/4.0/ | Motivated by the search for rational points in moduli spaces of
two-dimensional conformal field theories, we investigate how points with
enhanced symmetry algebras are distributed there. We first study the bosonic
sigma-model with $S^1$ target space in detail and uncover hitherto unknown
features. We find for instanc... | [
{
"created": "Fri, 13 Nov 2020 18:58:12 GMT",
"version": "v1"
}
] | 2021-04-28 | [
[
"Benjamin",
"Nathan",
""
],
[
"Keller",
"Christoph A.",
""
],
[
"Ooguri",
"Hirosi",
""
],
[
"Zadeh",
"Ida G.",
""
]
] | Motivated by the search for rational points in moduli spaces of two-dimensional conformal field theories, we investigate how points with enhanced symmetry algebras are distributed there. We first study the bosonic sigma-model with $S^1$ target space in detail and uncover hitherto unknown features. We find for instance ... | 10.109951 | 9.168083 | 10.603702 | 9.276316 | 9.897655 | 9.456646 | 9.563697 | 9.070015 | 8.722403 | 11.940035 | 8.574677 | 9.26902 | 9.592354 | 9.323312 | 9.158469 | 9.120425 | 9.114002 | 9.372757 | 9.608473 | 9.756988 | 9.074683 |
2008.00868 | O-Kab Kwon | Yoonbai Kim, O-Kab Kwon, D.D. Tolla | Super Yang-Mills Theories with Inhomogeneous Mass Deformations | 22 pages | null | 10.1007/JHEP12(2020)060 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the 4-dimensional ${\cal N}=\frac12$ and ${\cal N}=1$
inhomogeneously mass-deformed super Yang-Mills theories from the ${\cal N}
=1^*$ and ${\cal N} =2^*$ theories, respectively, and analyse their
supersymmetric vacua. The inhomogeneity is attributed to the dependence of
background fluxes in the type IIB... | [
{
"created": "Mon, 3 Aug 2020 13:37:06 GMT",
"version": "v1"
}
] | 2020-12-30 | [
[
"Kim",
"Yoonbai",
""
],
[
"Kwon",
"O-Kab",
""
],
[
"Tolla",
"D. D.",
""
]
] | We construct the 4-dimensional ${\cal N}=\frac12$ and ${\cal N}=1$ inhomogeneously mass-deformed super Yang-Mills theories from the ${\cal N} =1^*$ and ${\cal N} =2^*$ theories, respectively, and analyse their supersymmetric vacua. The inhomogeneity is attributed to the dependence of background fluxes in the type IIB s... | 6.622477 | 6.562614 | 7.553199 | 6.694129 | 6.37896 | 6.592221 | 6.545931 | 6.600687 | 6.439691 | 7.384403 | 6.376891 | 6.335595 | 6.713723 | 6.50737 | 6.397935 | 6.312048 | 6.379718 | 6.471715 | 6.391975 | 6.715204 | 6.276015 |
2003.04954 | Mario Martone | Philip Argyres and Mario Martone | Construction and classification of Coulomb branch geometries | 8 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a non-technical summary of the classification program, very dear to
the hearts of both authors, of four dimensional $\mathcal{N}=2$ superconformal
field theories (SCFTs) based on the study of their Coulomb branch geometries.
We outline the main ideas behind this program, review the most important
results thus... | [
{
"created": "Tue, 10 Mar 2020 20:15:31 GMT",
"version": "v1"
}
] | 2020-03-12 | [
[
"Argyres",
"Philip",
""
],
[
"Martone",
"Mario",
""
]
] | We give a non-technical summary of the classification program, very dear to the hearts of both authors, of four dimensional $\mathcal{N}=2$ superconformal field theories (SCFTs) based on the study of their Coulomb branch geometries. We outline the main ideas behind this program, review the most important results thus f... | 10.594153 | 10.041098 | 12.875451 | 9.900945 | 10.140477 | 10.634853 | 10.36689 | 10.336672 | 9.229538 | 13.485927 | 8.789525 | 9.71281 | 10.997803 | 10.019364 | 9.555305 | 9.578201 | 9.519299 | 9.624519 | 9.628448 | 10.625793 | 9.90064 |
hep-th/0006036 | Pietro Antonio Grassi | L.Baulieu (Paris U. IV-VII & Chicago U.), P.A.Grassi, D.Zwanziger (New
York U.) | Gauge and Topological Symmetries in the Bulk Quantization of Gauge
Theories | June 2000. 37pp. Improved discussion of the definition of observables
and derivation of the action | Nucl.Phys. B597 (2001) 583-614 | 10.1016/S0550-3213(00)00725-2 | LPTHE-00-20, NYU-TH-30-5-00 | hep-th hep-lat hep-ph | null | A gauge theory with 4 physical dimensions can be consistently expressed as a
renormalizable topological quantum field theory in 5 dimensions. We extend the
symmetries in the 5-dimensional framework to include not only a topological
BRST operator S that encodes the invisibility of the "bulk" (the fifth
dimension), but... | [
{
"created": "Mon, 5 Jun 2000 22:05:58 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Nov 2000 20:51:16 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Baulieu",
"L.",
"",
"Paris U. IV-VII & Chicago U."
],
[
"Grassi",
"P. A.",
"",
"New\n York U."
],
[
"Zwanziger",
"D.",
"",
"New\n York U."
]
] | A gauge theory with 4 physical dimensions can be consistently expressed as a renormalizable topological quantum field theory in 5 dimensions. We extend the symmetries in the 5-dimensional framework to include not only a topological BRST operator S that encodes the invisibility of the "bulk" (the fifth dimension), but a... | 11.589909 | 10.985424 | 11.743379 | 10.66213 | 11.793403 | 11.435061 | 11.806461 | 11.541718 | 11.601069 | 13.034516 | 10.517161 | 11.049058 | 11.251044 | 10.963861 | 10.841797 | 11.308232 | 10.823461 | 10.977411 | 11.13048 | 10.855103 | 10.867889 |
hep-th/0701151 | Bert Janssen | B. Janssen, Yolanda Lozano, Diego Rodriguez-Gomez | Adding magnetic flux to the baryon vertex | 6 pages, 2 figures. Contribution to the proceedings of the RTN
workshop in Napoli, Octobre 2006 | Fortsch.Phys.55:765-770,2007 | 10.1002/prop.200610352 | UG-FT-214/07, CAFPE-84/07, FFUOV-07/02 | hep-th | null | We generalise the baryon vertex configuration of AdS/CFT by adding magnetic
field on its worldvolume, dissolving D-string charge. A careful analysis of the
configuration shows that there is an upper bound on the number of dissolved
strings. We provide a microscopical description of this configuration in terms
of a di... | [
{
"created": "Tue, 16 Jan 2007 11:08:35 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Janssen",
"B.",
""
],
[
"Lozano",
"Yolanda",
""
],
[
"Rodriguez-Gomez",
"Diego",
""
]
] | We generalise the baryon vertex configuration of AdS/CFT by adding magnetic field on its worldvolume, dissolving D-string charge. A careful analysis of the configuration shows that there is an upper bound on the number of dissolved strings. We provide a microscopical description of this configuration in terms of a diel... | 15.755625 | 8.317623 | 20.733978 | 11.34732 | 12.569589 | 12.124727 | 11.958758 | 7.900394 | 10.908763 | 20.32629 | 10.620804 | 10.8608 | 18.607964 | 14.118379 | 13.689788 | 12.357514 | 13.299562 | 11.809565 | 14.314056 | 17.789068 | 12.049302 |
hep-th/0306222 | Cosmas Zachos | Cosmas Zachos | Membranes and Consistent Quantization of Nambu Dynamics | LaTeX2e, 8 pages, 1 figure. Invited talk at the 8th International
Wigner Symposium, 26-30 May 2003, New York, SPIRES Conf C03/05/26 | Phys.Lett.B570:82-88,2003 | 10.1016/j.physletb.2003.07.027 | ANL-HEP-PR-03-051 | hep-th | null | The dynamics of even topological open membranes relies on Nambu Brackets.
Consequently, such 2p-branes can be quantized through the consistent
quantization of the underlying Nambu dynamical structures. This is a summary
construction relying on the methods detailed in refs hep-th/0205063 and
hep-th/0212267.
| [
{
"created": "Mon, 23 Jun 2003 16:10:07 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Jul 2003 14:46:19 GMT",
"version": "v2"
},
{
"created": "Fri, 22 Aug 2003 15:42:38 GMT",
"version": "v3"
}
] | 2009-10-02 | [
[
"Zachos",
"Cosmas",
""
]
] | The dynamics of even topological open membranes relies on Nambu Brackets. Consequently, such 2p-branes can be quantized through the consistent quantization of the underlying Nambu dynamical structures. This is a summary construction relying on the methods detailed in refs hep-th/0205063 and hep-th/0212267. | 22.699806 | 19.757433 | 22.560154 | 19.443848 | 18.37661 | 19.63694 | 20.88888 | 17.584654 | 18.239889 | 23.261948 | 17.544188 | 21.509611 | 22.994953 | 20.244932 | 20.783381 | 20.405277 | 20.627525 | 20.638727 | 21.003942 | 21.956871 | 19.926962 |
1108.2567 | Eric Perlmutter | Per Kraus, Eric Perlmutter | Partition functions of higher spin black holes and their CFT duals | 28 pages; v2, added ref | JHEP 1111:061,2011 | 10.1007/JHEP11(2011)061 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find black hole solutions of D=3 higher-spin gravity in the hs[\lambda] +
hs[\lambda] Chern-Simons formulation. These solutions have a spin-3 chemical
potential, and carry nonzero values for an infinite number of charges of the
asymptotic W_{\infty}[\lambda] symmetry. Applying a previously developed set of
rules f... | [
{
"created": "Fri, 12 Aug 2011 05:46:09 GMT",
"version": "v1"
},
{
"created": "Fri, 16 Sep 2011 22:07:45 GMT",
"version": "v2"
}
] | 2015-05-30 | [
[
"Kraus",
"Per",
""
],
[
"Perlmutter",
"Eric",
""
]
] | We find black hole solutions of D=3 higher-spin gravity in the hs[\lambda] + hs[\lambda] Chern-Simons formulation. These solutions have a spin-3 chemical potential, and carry nonzero values for an infinite number of charges of the asymptotic W_{\infty}[\lambda] symmetry. Applying a previously developed set of rules for... | 9.56704 | 7.341979 | 12.823055 | 8.02377 | 7.795257 | 7.82768 | 8.225444 | 7.493512 | 7.486476 | 12.129775 | 7.330728 | 8.179794 | 9.909917 | 8.382121 | 8.533596 | 8.457597 | 8.346604 | 7.962501 | 8.258705 | 9.798074 | 8.049726 |
hep-th/9604198 | Michael Douglas | Michael R. Douglas | Gauge Fields and D-branes | harvmac, 9pp | J.Geom.Phys. 28 (1998) 255-262 | 10.1016/S0393-0440(97)00024-7 | RU-96-24 | hep-th | null | We prove that self-dual gauge fields in type I superstring theory are
equivalent to configurations of Dirichlet 5-branes, by showing that the
world-sheet theory of a Dirichlet 1-brane moving in a background of 5-branes
includes an ``ADHM sigma model.'' This provides an explicit construction of the
equivalent self-dua... | [
{
"created": "Tue, 30 Apr 1996 20:26:37 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Douglas",
"Michael R.",
""
]
] | We prove that self-dual gauge fields in type I superstring theory are equivalent to configurations of Dirichlet 5-branes, by showing that the world-sheet theory of a Dirichlet 1-brane moving in a background of 5-branes includes an ``ADHM sigma model.'' This provides an explicit construction of the equivalent self-dual ... | 10.152819 | 7.962255 | 12.384039 | 8.651847 | 7.71509 | 9.354177 | 8.706093 | 7.80046 | 8.14439 | 11.306603 | 8.543701 | 8.879751 | 10.19206 | 8.975135 | 8.859784 | 9.16402 | 9.117299 | 9.151565 | 8.987821 | 9.871975 | 8.985751 |
1707.04713 | Takafumi Suzuki | Shinichi Deguchi, Takafumi Suzuki | Twistor formulation of a massive particle with rigidity | 50 pages, Section 6 is revised, A reference added, minor corrections,
Published version | Nucl. Phys. B 932 (2018) 385 | 10.1016/j.nuclphysb.2018.05.016 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A massive rigid particle model in $(3+1)$ dimensions is reformulated in terms
of twistors. Beginning with a first-order Lagrangian, we establish a twistor
representation of the Lagrangian for a massive particle with rigidity. The
twistorial Lagrangian derived in this way remains invariant under a local $U(1)
\times U... | [
{
"created": "Sat, 15 Jul 2017 09:13:16 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jul 2017 09:53:19 GMT",
"version": "v2"
},
{
"created": "Fri, 1 Jun 2018 03:35:43 GMT",
"version": "v3"
}
] | 2018-06-04 | [
[
"Deguchi",
"Shinichi",
""
],
[
"Suzuki",
"Takafumi",
""
]
] | A massive rigid particle model in $(3+1)$ dimensions is reformulated in terms of twistors. Beginning with a first-order Lagrangian, we establish a twistor representation of the Lagrangian for a massive particle with rigidity. The twistorial Lagrangian derived in this way remains invariant under a local $U(1) \times U(1... | 8.61862 | 8.235455 | 8.040197 | 7.775668 | 8.195731 | 8.217257 | 8.339575 | 8.034372 | 7.710007 | 8.344648 | 8.103388 | 7.687497 | 7.631567 | 7.46695 | 7.70205 | 7.706398 | 7.791063 | 7.616107 | 7.872859 | 7.840741 | 7.438031 |
hep-th/9509115 | null | Karim Benakli | Perturbative Supersymmetry Breaking In Orbifolds With Wilson Line
Backgrounds | TEX 13 pages | Phys.Lett.B386:106-114,1996 | 10.1016/0370-2693(96)00902-1 | IC/95/306 | hep-th hep-ph | null | A way to break supersymmetry in perturbative superstring theory is the string
version of the Scherk-Schwarz mechanism. There, the fermions and bosons have
mass splitting due to different compactification boundary conditions. We
consider the implementation of this mechanism in abelian orbifold
compactifications with W... | [
{
"created": "Thu, 21 Sep 1995 15:59:38 GMT",
"version": "v1"
}
] | 2011-05-05 | [
[
"Benakli",
"Karim",
""
]
] | A way to break supersymmetry in perturbative superstring theory is the string version of the Scherk-Schwarz mechanism. There, the fermions and bosons have mass splitting due to different compactification boundary conditions. We consider the implementation of this mechanism in abelian orbifold compactifications with Wil... | 8.980549 | 8.960056 | 8.349587 | 8.144388 | 8.425755 | 8.580227 | 8.836518 | 8.319809 | 8.472502 | 9.73098 | 8.581133 | 8.381038 | 8.496756 | 8.31395 | 8.635335 | 8.398211 | 8.518324 | 8.491504 | 8.349194 | 8.64005 | 8.355365 |
hep-th/9903089 | Maria A. Lledo | R. D'Auria, S. Ferrara amd M. A. Lled\'o | On Central Charges and Hamiltonians for 0-brane dynamics | 23 pages, latex file | Phys.Rev.D60:084007,1999 | 10.1103/PhysRevD.60.084007 | CERN-TH/99-53 | hep-th | null | We consider general properties of central charges of zero branes and
associated duality invariants, in view of their double role, on the bulk and on
the world volume (quantum-mechanical) theory. A detailed study of the BPS
condition for the mass spectrum arising from toroidal compactifications is
given for 1/2, 1/4 a... | [
{
"created": "Wed, 10 Mar 1999 18:04:29 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"D'Auria",
"R.",
""
],
[
"Lledó",
"S. Ferrara amd M. A.",
""
]
] | We consider general properties of central charges of zero branes and associated duality invariants, in view of their double role, on the bulk and on the world volume (quantum-mechanical) theory. A detailed study of the BPS condition for the mass spectrum arising from toroidal compactifications is given for 1/2, 1/4 and... | 11.204517 | 11.636244 | 12.148619 | 10.050555 | 11.529032 | 11.368796 | 10.881426 | 9.983106 | 10.659081 | 12.538122 | 10.046818 | 10.724299 | 10.879455 | 10.457876 | 10.143765 | 10.663575 | 10.6821 | 10.600818 | 10.374688 | 11.161662 | 10.097634 |
1301.2500 | Miguel Paulos | Dhritiman Nandan, Miguel F. Paulos, Marcus Spradlin and Anastasia
Volovich | Star Integrals, Convolutions and Simplices | 23 pages | null | 10.1007/JHEP05(2013)105 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore single and multi-loop conformal integrals, such as the ones
appearing in dual conformal theories in flat space. Using Mellin amplitudes, a
large class of higher loop integrals can be written as simple
integro-differential operators on star integrals: one-loop $n$-gon integrals in
$n$ dimensions. These are ... | [
{
"created": "Fri, 11 Jan 2013 13:57:27 GMT",
"version": "v1"
}
] | 2015-06-12 | [
[
"Nandan",
"Dhritiman",
""
],
[
"Paulos",
"Miguel F.",
""
],
[
"Spradlin",
"Marcus",
""
],
[
"Volovich",
"Anastasia",
""
]
] | We explore single and multi-loop conformal integrals, such as the ones appearing in dual conformal theories in flat space. Using Mellin amplitudes, a large class of higher loop integrals can be written as simple integro-differential operators on star integrals: one-loop $n$-gon integrals in $n$ dimensions. These are kn... | 9.888477 | 10.120625 | 11.253016 | 9.574386 | 9.472183 | 10.449973 | 9.013602 | 9.564894 | 9.195592 | 11.036097 | 9.123825 | 9.665415 | 9.897166 | 9.43584 | 9.641648 | 9.776778 | 9.58108 | 9.303398 | 9.665195 | 10.049152 | 9.167944 |
1707.09175 | Stephen Stopyra | Arttu Rajantie and Stephen Stopyra | Standard Model vacuum decay in a de Sitter Background | 20 pages, 11 figures | Phys. Rev. D 97, 025012 (2018) | 10.1103/PhysRevD.97.025012 | IMPERIAL-TP-2017-AR-2 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a calculation of thick-wall Coleman-de-Luccia (CdL) bounces in the
Standard Model effective potential in a de Sitter background. The calculation
is performed including the effect of the bounce back-reaction on the metric,
which we compare with the case of a fixed de-Sitter background, and with
similar full... | [
{
"created": "Fri, 28 Jul 2017 10:17:46 GMT",
"version": "v1"
}
] | 2018-01-24 | [
[
"Rajantie",
"Arttu",
""
],
[
"Stopyra",
"Stephen",
""
]
] | We present a calculation of thick-wall Coleman-de-Luccia (CdL) bounces in the Standard Model effective potential in a de Sitter background. The calculation is performed including the effect of the bounce back-reaction on the metric, which we compare with the case of a fixed de-Sitter background, and with similar full-b... | 8.733583 | 8.896015 | 8.325317 | 7.682751 | 8.118956 | 8.146194 | 8.904815 | 8.55087 | 8.069087 | 9.202751 | 7.96864 | 8.195709 | 8.032557 | 8.067551 | 8.151175 | 8.373502 | 8.245014 | 8.19267 | 8.220281 | 8.464732 | 7.967519 |
0704.3570 | Matteo Beccaria | Matteo Beccaria | Anomalous dimensions at twist-3 in the sl(2) sector of N=4 SYM | 26 pages, JHEP style | JHEP 0706:044,2007 | 10.1088/1126-6708/2007/06/044 | null | hep-th | null | We consider twist-3 operators in the sl(2) sector of N=4 SYM built out of
three scalar fields with derivatives. We extract from the Bethe Ansatz
equations of this sector the exact lowest anomalous dimension gamma(s) of
scaling fields for several values of the operator spin s. We propose compact
closed expressions for... | [
{
"created": "Thu, 26 Apr 2007 15:46:25 GMT",
"version": "v1"
}
] | 2009-11-13 | [
[
"Beccaria",
"Matteo",
""
]
] | We consider twist-3 operators in the sl(2) sector of N=4 SYM built out of three scalar fields with derivatives. We extract from the Bethe Ansatz equations of this sector the exact lowest anomalous dimension gamma(s) of scaling fields for several values of the operator spin s. We propose compact closed expressions for t... | 11.862465 | 9.788433 | 12.742256 | 10.087881 | 9.905294 | 10.102503 | 11.171214 | 9.926752 | 9.500437 | 14.831153 | 9.987837 | 10.244209 | 11.768382 | 10.85812 | 10.401023 | 10.36741 | 10.969192 | 10.361533 | 10.727846 | 11.214416 | 10.197135 |
1208.3199 | Julian Sonner | Alexander Adam, Benedict Crampton, Julian Sonner and Benjamin Withers | Bosonic Fractionalisation Transitions | references added. minor changes. version published in JHEP | null | 10.1007/JHEP01(2013)127 | Imperial/TP/2012/JS/02 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | At finite density, charge in holographic systems can be sourced either by
explicit matter sources in the bulk or by bulk horizons. In this paper we find
bosonic solutions of both types, breaking a global U(1) symmetry in the former
case and leaving it unbroken in the latter. Using a minimal bottom-up model we
exhibit... | [
{
"created": "Wed, 15 Aug 2012 20:00:16 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Mar 2013 14:09:05 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Adam",
"Alexander",
""
],
[
"Crampton",
"Benedict",
""
],
[
"Sonner",
"Julian",
""
],
[
"Withers",
"Benjamin",
""
]
] | At finite density, charge in holographic systems can be sourced either by explicit matter sources in the bulk or by bulk horizons. In this paper we find bosonic solutions of both types, breaking a global U(1) symmetry in the former case and leaving it unbroken in the latter. Using a minimal bottom-up model we exhibit p... | 17.032648 | 15.564954 | 17.491699 | 14.978188 | 15.897019 | 14.842823 | 15.797869 | 15.091492 | 14.537962 | 20.60693 | 14.530235 | 14.612829 | 17.78616 | 15.32609 | 14.685062 | 14.631681 | 14.883579 | 14.735997 | 15.080048 | 16.630636 | 14.911379 |
2307.01973 | LiFang Li | Xiao-Xiong Zeng, Li-Fang Li, Peng Xu | Holographic Einstein rings of a black hole with a global monopole | revised version | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | The global monopole solutions which give rise to quite unusual physical
phenomena have captured considerable attention. In this paper, we study the
Einstein ring of the spherically symmetric AdS black hole solution with a
global monopole based on the AdS/CFT correspondence. With the help of the given
response functio... | [
{
"created": "Wed, 5 Jul 2023 01:05:26 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Aug 2023 05:18:49 GMT",
"version": "v2"
}
] | 2023-08-21 | [
[
"Zeng",
"Xiao-Xiong",
""
],
[
"Li",
"Li-Fang",
""
],
[
"Xu",
"Peng",
""
]
] | The global monopole solutions which give rise to quite unusual physical phenomena have captured considerable attention. In this paper, we study the Einstein ring of the spherically symmetric AdS black hole solution with a global monopole based on the AdS/CFT correspondence. With the help of the given response function ... | 11.934351 | 12.394651 | 9.275476 | 8.920058 | 11.159595 | 11.521295 | 12.702467 | 9.252152 | 11.643076 | 10.604135 | 11.679684 | 11.685706 | 11.300866 | 11.203286 | 11.827641 | 12.165717 | 12.169495 | 10.96596 | 11.639493 | 11.644379 | 12.120109 |
1002.2981 | Domenico Orlando | Amihay Hanany, Domenico Orlando, Susanne Reffert | Sublattice Counting and Orbifolds | 24 pages, 7 figures | JHEP 1006:051,2010 | 10.1007/JHEP06(2010)051 | Imperial/TP/10/AH/01, IPMU10-0025 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Abelian orbifolds of C^3 are known to be encoded by hexagonal brane tilings.
To date it is not known how to count all such orbifolds. We fill this gap by
employing number theoretic techniques from crystallography, and by making use
of Polya's Enumeration Theorem. The results turn out to be beautifully encoded
in term... | [
{
"created": "Tue, 16 Feb 2010 00:47:55 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Hanany",
"Amihay",
""
],
[
"Orlando",
"Domenico",
""
],
[
"Reffert",
"Susanne",
""
]
] | Abelian orbifolds of C^3 are known to be encoded by hexagonal brane tilings. To date it is not known how to count all such orbifolds. We fill this gap by employing number theoretic techniques from crystallography, and by making use of Polya's Enumeration Theorem. The results turn out to be beautifully encoded in terms ... | 8.871181 | 8.478348 | 9.696147 | 7.680758 | 7.653256 | 8.170978 | 8.418721 | 7.190307 | 8.041784 | 10.809588 | 7.217166 | 7.668961 | 8.83936 | 7.900087 | 7.589526 | 7.728115 | 7.745529 | 7.654655 | 7.885458 | 8.645504 | 7.892214 |
hep-th/9602162 | Ctirad Klimcik | C. Klimcik and P. Severa | Dressing Cosets | 11 pages, LaTeX | Phys.Lett. B381 (1996) 56-61 | 10.1016/0370-2693(96)00669-7 | CERN-TH/96-43 | hep-th | null | The account of the Poisson-Lie T-duality is presented for the case when the
action of the duality group on a target is not free. At the same time a
generalization of the picture is given when the duality group does not even act
on $\si$-model targets but only on their phase spaces. The outcome is a huge
class of dual... | [
{
"created": "Wed, 28 Feb 1996 16:05:14 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Klimcik",
"C.",
""
],
[
"Severa",
"P.",
""
]
] | The account of the Poisson-Lie T-duality is presented for the case when the action of the duality group on a target is not free. At the same time a generalization of the picture is given when the duality group does not even act on $\si$-model targets but only on their phase spaces. The outcome is a huge class of dualiz... | 11.112897 | 10.199905 | 12.120165 | 9.933418 | 10.491435 | 11.149199 | 10.272077 | 9.372724 | 10.054331 | 11.279302 | 9.550158 | 10.591402 | 10.998302 | 10.160553 | 9.867561 | 10.218385 | 10.29178 | 10.391671 | 10.324921 | 11.534948 | 9.731011 |
1104.5279 | Lasha Berezhiani | Lasha Berezhiani and Mehrdad Mirbabayi | Generalized Framework for Auxiliary Extra Dimensions | 12 pages | Phys.Lett.B701:654-659,2011 | 10.1016/j.physletb.2011.06.036 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The theory of gravity with an auxiliary extra dimension is known to give the
ghost-free cubic completion of the Fierz-Pauli mass term in the decoupling
limit. Our work generalizes the boundary condition in the auxiliary dimension
that avoids ghosts order-by-order, and to all orders, in the decoupling limit.
Furthermo... | [
{
"created": "Thu, 28 Apr 2011 02:37:20 GMT",
"version": "v1"
}
] | 2011-07-20 | [
[
"Berezhiani",
"Lasha",
""
],
[
"Mirbabayi",
"Mehrdad",
""
]
] | The theory of gravity with an auxiliary extra dimension is known to give the ghost-free cubic completion of the Fierz-Pauli mass term in the decoupling limit. Our work generalizes the boundary condition in the auxiliary dimension that avoids ghosts order-by-order, and to all orders, in the decoupling limit. Furthermore... | 11.645936 | 11.708843 | 11.644959 | 10.854831 | 11.425272 | 10.599355 | 11.583255 | 10.912806 | 10.776772 | 11.557442 | 11.083008 | 11.18924 | 11.573419 | 11.52478 | 11.201121 | 11.355842 | 11.20589 | 11.539446 | 11.540021 | 11.305058 | 10.639258 |
hep-th/0602209 | Dimitri Polyakov | Dimitri Polyakov | New Discrete States in Two-Dimensional Supergravity | 22 pages; typos corrected, 2 references added | Int.J.Mod.Phys.A22:1375-1394,2007 | 10.1142/S0217751X07035148 | null | hep-th gr-qc | null | Two-dimensional string theory is known to contain the set of discrete states
that are the SU(2) multiplets generated by the lowering operator of the SU(2)
current algebra.Their structure constants are defined by the area preserving
diffeomorphisms in two dimensions. We show that the interaction of $d=2$
superstrings ... | [
{
"created": "Tue, 21 Feb 2006 11:41:09 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Feb 2006 15:23:06 GMT",
"version": "v2"
},
{
"created": "Thu, 23 Feb 2006 15:05:56 GMT",
"version": "v3"
},
{
"created": "Mon, 27 Feb 2006 17:05:32 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Polyakov",
"Dimitri",
""
]
] | Two-dimensional string theory is known to contain the set of discrete states that are the SU(2) multiplets generated by the lowering operator of the SU(2) current algebra.Their structure constants are defined by the area preserving diffeomorphisms in two dimensions. We show that the interaction of $d=2$ superstrings wi... | 9.816583 | 9.674641 | 10.644876 | 9.381136 | 10.932386 | 10.100938 | 9.61752 | 9.773769 | 9.644889 | 10.011654 | 8.90256 | 9.59097 | 9.890984 | 9.358778 | 9.61537 | 9.842667 | 9.410798 | 9.589809 | 9.476681 | 10.047043 | 9.607776 |
hep-th/0208128 | B. Ram | B. Ram | On the quantum theory of pure gravitation | 9 pages | null | null | null | hep-th | null | A quantum theory of the region of pure gravitation was given earlier in two
papers [gr-qc/9908036 (Phys. Lett. A {\bf {265}}, 1 (2000)); gr-qc/0101056]. In
this paper I provide further insight into the physics of this region.
| [
{
"created": "Mon, 19 Aug 2002 05:47:30 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ram",
"B.",
""
]
] | A quantum theory of the region of pure gravitation was given earlier in two papers [gr-qc/9908036 (Phys. Lett. A {\bf {265}}, 1 (2000)); gr-qc/0101056]. In this paper I provide further insight into the physics of this region. | 12.650857 | 16.459194 | 10.19947 | 11.161606 | 11.083143 | 12.736845 | 13.232078 | 13.121112 | 11.70589 | 12.345827 | 13.818134 | 12.043262 | 11.298077 | 11.630689 | 11.677017 | 11.58816 | 12.135004 | 11.043328 | 11.420665 | 11.109951 | 11.718793 |
hep-th/9312035 | Harnad John | John Harnad and P. Winternitz | Classical and Quantum Integrable Systems in $\wt{\gr{gl}}(2)^{+*}$ and
Separation of Variables | 28 pages | Commun.Math.Phys. 172 (1995) 263-286 | 10.1007/BF02099428 | CRM--1921 (1993) | hep-th nlin.SI solv-int | null | Classical integrable Hamiltonian systems generated by elements of the Poisson
commuting ring of spectral invariants on rational coadjoint orbits of the loop
algebra $\wt{\gr{gl}}^{+*}(2,{\bf R})$ are integrated by separation of
variables in the Hamilton-Jacobi equation in hyperellipsoidal coordinates. The
canonically... | [
{
"created": "Fri, 3 Dec 1993 23:23:26 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Harnad",
"John",
""
],
[
"Winternitz",
"P.",
""
]
] | Classical integrable Hamiltonian systems generated by elements of the Poisson commuting ring of spectral invariants on rational coadjoint orbits of the loop algebra $\wt{\gr{gl}}^{+*}(2,{\bf R})$ are integrated by separation of variables in the Hamilton-Jacobi equation in hyperellipsoidal coordinates. The canonically q... | 11.141663 | 12.164407 | 13.238064 | 10.656731 | 11.33985 | 12.062924 | 11.675332 | 11.177118 | 10.737281 | 15.066362 | 10.415289 | 10.69132 | 10.587999 | 10.318048 | 10.772859 | 10.710189 | 10.709099 | 10.56403 | 10.063686 | 10.708157 | 10.111054 |
hep-th/9309089 | null | H. Arodz and A.L. Larsen | On dynamics of cylindrical and spherical relativistic domain walls of
finite thickness | 26 pages Latex + 4 figures (not included), Nordita 93/58 P | Phys.Rev. D49 (1994) 4154-4166 | 10.1103/PhysRevD.49.4154 | null | hep-th | null | Dynamics of cylindrical and spherical relativistic domain walls is
investigated with the help of a new method based on Taylor expansion of the
scalar field in a vicinity of the core of the wall. Internal oscillatory modes
for the domain walls are found. These modes are non-analytic in the "width" of
the domain wall. ... | [
{
"created": "Thu, 16 Sep 1993 09:47:12 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Arodz",
"H.",
""
],
[
"Larsen",
"A. L.",
""
]
] | Dynamics of cylindrical and spherical relativistic domain walls is investigated with the help of a new method based on Taylor expansion of the scalar field in a vicinity of the core of the wall. Internal oscillatory modes for the domain walls are found. These modes are non-analytic in the "width" of the domain wall. Ra... | 12.937186 | 11.511385 | 10.756336 | 9.862794 | 11.048427 | 11.329272 | 9.874747 | 10.220492 | 10.501528 | 10.275497 | 10.261764 | 10.222144 | 10.119957 | 9.819183 | 10.044579 | 10.176942 | 9.998814 | 10.117645 | 10.046047 | 9.778162 | 10.04783 |
hep-th/9304165 | Sun Chang Pu | Chang-Pu Sun | High-Order Adiabatic Approximation for Non-Hermitian Quantum System and
Complexization of Berry's Phase | ITP.SB-93-22,17 pages | null | 10.1088/0031-8949/48/4/002 | null | hep-th | null | In this paper the evolution of a quantum system drived by a non-Hermitian
Hamiltonian depending on slowly-changing parameters is studied by building an
universal high-order adiabatic approximation(HOAA) method with Berry's phase
,which is valid for either the Hermitian or the non-Hermitian cases. This
method can be r... | [
{
"created": "Sun, 2 May 1993 16:35:37 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Sun",
"Chang-Pu",
""
]
] | In this paper the evolution of a quantum system drived by a non-Hermitian Hamiltonian depending on slowly-changing parameters is studied by building an universal high-order adiabatic approximation(HOAA) method with Berry's phase ,which is valid for either the Hermitian or the non-Hermitian cases. This method can be reg... | 8.531704 | 9.714234 | 9.357627 | 9.177825 | 9.660378 | 9.719869 | 9.336356 | 8.811442 | 8.619382 | 9.767198 | 8.600851 | 8.636205 | 8.534686 | 8.836631 | 8.383228 | 9.079474 | 8.780271 | 8.557804 | 8.628716 | 8.52321 | 8.57694 |
hep-th/9803141 | Zurab Kakushadze | Zurab Kakushadze, Gary Shiu and S.-H. Henry Tye | Type IIB Orientifolds with NS-NS Antisymmetric Tensor Backgrounds | 13 pages, revtex, minor misprints corrected | Phys.Rev. D58 (1998) 086001 | 10.1103/PhysRevD.58.086001 | CLNS 98/1550, HUTP-97/A092, NUB 3173 | hep-th | null | We consider six dimensional N=1 space-time supersymmetric Type IIB
orientifolds with non-zero untwisted NS-NS sector B-field. The B-field is
quantized due to the requirement that the Type IIB spectrum be left-right
symmetric. The presence of the B-field results in rank reduction of both 99 and
55 open string sector g... | [
{
"created": "Tue, 17 Mar 1998 22:39:18 GMT",
"version": "v1"
},
{
"created": "Fri, 8 May 1998 06:52:08 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Nov 1998 08:32:06 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Kakushadze",
"Zurab",
""
],
[
"Shiu",
"Gary",
""
],
[
"Tye",
"S. -H. Henry",
""
]
] | We consider six dimensional N=1 space-time supersymmetric Type IIB orientifolds with non-zero untwisted NS-NS sector B-field. The B-field is quantized due to the requirement that the Type IIB spectrum be left-right symmetric. The presence of the B-field results in rank reduction of both 99 and 55 open string sector gau... | 7.976951 | 7.415341 | 9.802207 | 7.439291 | 8.130084 | 7.021262 | 7.410402 | 7.426382 | 7.594719 | 8.887062 | 6.575521 | 7.827319 | 7.990639 | 7.658126 | 7.783501 | 7.645414 | 7.51945 | 7.530687 | 7.619363 | 7.956128 | 7.599623 |
1304.0614 | Sergio Cecotti | Sergio Cecotti and Michele Del Zotto | The BPS spectrum of the 4d N=2 SCFT's H_1, H_2, D_4, E_6, E_7, E_8 | 14 pages | null | 10.1007/JHEP06(2013)075 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Extending results of arXiv:1112.3984, we show that all rank 1 N=2 SCFT's in
the sequence H_1, H_2, D_4 E_6, E_7, E_8 have canonical finite BPS chambers
containing precisely 2 h(F)=12(Delta-1) hypermultiplets. The BPS spectrum of
the canonical BPS chambers saturates the conformal central charge c, and
satisfies some i... | [
{
"created": "Tue, 2 Apr 2013 12:27:03 GMT",
"version": "v1"
}
] | 2015-06-15 | [
[
"Cecotti",
"Sergio",
""
],
[
"Del Zotto",
"Michele",
""
]
] | Extending results of arXiv:1112.3984, we show that all rank 1 N=2 SCFT's in the sequence H_1, H_2, D_4 E_6, E_7, E_8 have canonical finite BPS chambers containing precisely 2 h(F)=12(Delta-1) hypermultiplets. The BPS spectrum of the canonical BPS chambers saturates the conformal central charge c, and satisfies some int... | 15.428318 | 12.290619 | 17.049353 | 13.348407 | 12.657256 | 13.731338 | 13.80186 | 12.753186 | 11.421674 | 19.151939 | 12.748876 | 13.210255 | 16.301893 | 13.279196 | 13.65012 | 13.922989 | 13.411075 | 13.382213 | 12.735498 | 15.718119 | 12.131188 |
1507.01246 | Filip Blaschke | Filip Blaschke | Dynamical Realization of the Brane world Scenario Using Topological
Solitons | PhD. thesis, 146 pages, 10 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this thesis we discuss how the brane world scenario can be realized
dynamically within the field theoretical framework using topological solitons.
As a playground we consider a bosonic sector of a (4+1)-dimensional
supersymmetric gauge theory, which naturally supports soliton of co-dimension
one, a domain wall. We... | [
{
"created": "Sun, 5 Jul 2015 17:30:28 GMT",
"version": "v1"
}
] | 2015-07-07 | [
[
"Blaschke",
"Filip",
""
]
] | In this thesis we discuss how the brane world scenario can be realized dynamically within the field theoretical framework using topological solitons. As a playground we consider a bosonic sector of a (4+1)-dimensional supersymmetric gauge theory, which naturally supports soliton of co-dimension one, a domain wall. We f... | 8.708543 | 8.251527 | 9.061896 | 8.401162 | 8.541241 | 8.971845 | 8.78987 | 8.212152 | 8.161949 | 9.211567 | 8.249007 | 8.27389 | 8.300829 | 8.160565 | 8.18315 | 8.182568 | 8.160913 | 8.419708 | 8.216881 | 8.406464 | 7.957629 |
0811.2371 | Alain Ulacia Rey | A. Ulacia Rey | Contributions of Riemann invariants to the Entropy of Extremal Black
Holes | 16 pages, revised version, comments and references added, accepted
for publication in JHEP | JHEP 0908:107,2009 | 10.1088/1126-6708/2009/08/107 | ICIMAF 2008, -485 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the entropy function formalism introduced by A. Sen to obtain the
entropy of $AdS_{2}\times S^{d-2}$ extremal and static black holes in four and
five dimensions, with higher derivative terms of a general type. Starting from
a generalized Einstein--Maxwell action with nonzero cosmological constant, we
examine a... | [
{
"created": "Fri, 14 Nov 2008 16:18:10 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Aug 2009 00:55:31 GMT",
"version": "v2"
}
] | 2009-09-28 | [
[
"Rey",
"A. Ulacia",
""
]
] | We use the entropy function formalism introduced by A. Sen to obtain the entropy of $AdS_{2}\times S^{d-2}$ extremal and static black holes in four and five dimensions, with higher derivative terms of a general type. Starting from a generalized Einstein--Maxwell action with nonzero cosmological constant, we examine all... | 8.563295 | 7.344893 | 8.653163 | 7.175128 | 7.521557 | 7.37745 | 7.724948 | 7.095858 | 7.58839 | 9.730095 | 7.352824 | 7.146503 | 7.868325 | 7.4764 | 7.557068 | 7.604233 | 7.391666 | 7.401098 | 7.395366 | 7.814201 | 7.371182 |
1612.04334 | G\'abor S\'arosi | Vijay Balasubramanian, Ben Craps, Bart{\l}omiej Czech and G\'abor
S\'arosi | Echoes of chaos from string theory black holes | 26 pages, 9 figures, v3: discussion of dip time added | null | 10.1007/JHEP03(2017)154 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The strongly coupled D1-D5 conformal field theory is a microscopic model of
black holes which is expected to have chaotic dynamics. Here, we study the weak
coupling limit of the theory where it is integrable rather than chaotic. In
this limit, the operators creating microstates of the lowest mass black hole
are known... | [
{
"created": "Tue, 13 Dec 2016 20:00:43 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Dec 2016 21:24:56 GMT",
"version": "v2"
},
{
"created": "Mon, 3 Apr 2017 10:45:53 GMT",
"version": "v3"
}
] | 2017-04-04 | [
[
"Balasubramanian",
"Vijay",
""
],
[
"Craps",
"Ben",
""
],
[
"Czech",
"Bartłomiej",
""
],
[
"Sárosi",
"Gábor",
""
]
] | The strongly coupled D1-D5 conformal field theory is a microscopic model of black holes which is expected to have chaotic dynamics. Here, we study the weak coupling limit of the theory where it is integrable rather than chaotic. In this limit, the operators creating microstates of the lowest mass black hole are known e... | 9.222332 | 9.388737 | 10.317616 | 8.629104 | 9.537466 | 9.080995 | 9.483172 | 8.601042 | 8.788854 | 10.631586 | 8.647039 | 8.795501 | 9.297297 | 8.832758 | 9.210974 | 8.822455 | 8.872167 | 8.935205 | 8.943971 | 9.455101 | 8.841776 |
2405.19416 | Stefanos Robert Kousvos | Stefanos R. Kousvos, Alessandro Piazza and Alessandro Vichi | Exploring Replica-Potts CFTs in Two Dimensions | 47 pages, 19 figures | null | null | null | hep-th cond-mat.stat-mech cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate a numerical conformal bootstrap study of CFTs with $S_n \ltimes
(S_Q)^n$ global symmetry. These include CFTs that can be obtained as coupled
replicas of two-dimensional critical Potts models. Particular attention is paid
to the special case $S_3 \ltimes (S_3)^3$, which governs the critical behaviour
of th... | [
{
"created": "Wed, 29 May 2024 18:00:24 GMT",
"version": "v1"
}
] | 2024-05-31 | [
[
"Kousvos",
"Stefanos R.",
""
],
[
"Piazza",
"Alessandro",
""
],
[
"Vichi",
"Alessandro",
""
]
] | We initiate a numerical conformal bootstrap study of CFTs with $S_n \ltimes (S_Q)^n$ global symmetry. These include CFTs that can be obtained as coupled replicas of two-dimensional critical Potts models. Particular attention is paid to the special case $S_3 \ltimes (S_3)^3$, which governs the critical behaviour of thre... | 8.667029 | 9.291449 | 8.93082 | 8.721425 | 9.048199 | 8.617001 | 9.525506 | 9.07526 | 8.586494 | 10.099927 | 8.326851 | 8.562882 | 8.685428 | 8.308416 | 8.530798 | 8.30928 | 8.078321 | 8.214669 | 8.344372 | 8.920848 | 8.203926 |
0912.2954 | Jonathan Shock | Jonathan P. Shock, Javier Tarrio | A note on the velocity of holographic long-lived mesons | 4 pages, 2 figures | Phys.Lett.B688:244-247,2010 | 10.1016/j.physletb.2010.03.085 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study fluctuations of a U(1) gauge field on the worldvolume of Nf probe
D7-branes in the background of Nc black D3-branes with a finite baryon density.
The choice of mode corresponds to vector mesons in the dual gauge theory whose
mass and lifetime can be determined by a study of the quasinormal modes. The
speed o... | [
{
"created": "Tue, 15 Dec 2009 17:03:24 GMT",
"version": "v1"
}
] | 2010-05-07 | [
[
"Shock",
"Jonathan P.",
""
],
[
"Tarrio",
"Javier",
""
]
] | We study fluctuations of a U(1) gauge field on the worldvolume of Nf probe D7-branes in the background of Nc black D3-branes with a finite baryon density. The choice of mode corresponds to vector mesons in the dual gauge theory whose mass and lifetime can be determined by a study of the quasinormal modes. The speed of ... | 9.434462 | 7.943497 | 10.163327 | 8.107466 | 7.652549 | 7.590301 | 6.637627 | 6.77751 | 8.194001 | 10.434614 | 7.396872 | 7.876801 | 8.901138 | 8.162521 | 7.762047 | 7.868556 | 7.776523 | 8.162031 | 8.25958 | 9.4299 | 7.867155 |
1505.04837 | Hai Lin | Pablo Diaz, Hai Lin, Alvaro Veliz-Osorio | Graph duality as an instrument of Gauge-String correspondence | 34 pages. version published in journal | Journal of Mathematical Physics 57 (2016) 052302 | 10.1063/1.4949550 | null | hep-th gr-qc math-ph math.MP math.OA quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explore an identity between two branching graphs and propose a physical
meaning in the context of the gauge-gravity correspondence. From the
mathematical point of view, the identity equates probabilities associated with
$\mathbb{GT}$, the branching graph of the unitary groups, with probabilities
associated with $\... | [
{
"created": "Mon, 18 May 2015 23:00:10 GMT",
"version": "v1"
},
{
"created": "Sat, 21 May 2016 11:35:01 GMT",
"version": "v2"
}
] | 2023-02-16 | [
[
"Diaz",
"Pablo",
""
],
[
"Lin",
"Hai",
""
],
[
"Veliz-Osorio",
"Alvaro",
""
]
] | We explore an identity between two branching graphs and propose a physical meaning in the context of the gauge-gravity correspondence. From the mathematical point of view, the identity equates probabilities associated with $\mathbb{GT}$, the branching graph of the unitary groups, with probabilities associated with $\ma... | 13.073021 | 14.521893 | 15.29155 | 12.92197 | 13.404533 | 14.073201 | 13.879287 | 12.779371 | 13.51518 | 15.989616 | 12.432435 | 12.915834 | 14.703784 | 13.149854 | 12.959583 | 12.854106 | 12.793736 | 12.852046 | 13.536592 | 14.389492 | 12.642324 |
hep-th/9303108 | null | A. Fring, G. Mussardo and P. Simonetti | Form Factors of the Elementary Field in the Bullough-Dodd Model | 14 pages, LATEX file, ISAS/EP/92/208;USP-IFQSC/TH/92-51 | Phys.Lett. B307 (1993) 83-90 | 10.1016/0370-2693(93)90196-O | null | hep-th | null | We derive the recursive equations for the form factors of the local hermitian
operators in the Bullough-Dodd model. At the self-dual point of the theory, the
form factors of the fundamental field of the Bullough-Dodd model are equal to
those of the fundamental field of the Sinh-Gordon model at a specific value of
the... | [
{
"created": "Fri, 19 Mar 1993 08:55:44 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Fring",
"A.",
""
],
[
"Mussardo",
"G.",
""
],
[
"Simonetti",
"P.",
""
]
] | We derive the recursive equations for the form factors of the local hermitian operators in the Bullough-Dodd model. At the self-dual point of the theory, the form factors of the fundamental field of the Bullough-Dodd model are equal to those of the fundamental field of the Sinh-Gordon model at a specific value of the c... | 5.896762 | 5.334849 | 7.374656 | 5.073349 | 5.189117 | 4.880344 | 4.822003 | 4.852238 | 4.894819 | 7.358239 | 4.670488 | 5.171153 | 6.333863 | 5.099832 | 5.017598 | 5.134252 | 5.14108 | 4.958524 | 5.052745 | 6.37359 | 5.048877 |
1205.3791 | Andrzej G\"orlich | Jan Ambjorn, Jakub Gizbert-Studnicki, Andrzej G\"orlich, Jerzy
Jurkiewicz | The transfer matrix in four-dimensional CDT | 32 pages, 19 figures | JHEP 1209 (2012) 017 | 10.1007/JHEP09(2012)017 | null | hep-th gr-qc hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Causal Dynamical Triangulation model of quantum gravity (CDT) has a
transfer matrix, relating spatial geometries at adjacent (discrete lattice)
times. The transfer matrix uniquely determines the theory. We show that the
measurements of the scale factor of the (CDT) universe are well described by an
effective tran... | [
{
"created": "Wed, 16 May 2012 20:00:57 GMT",
"version": "v1"
}
] | 2016-02-10 | [
[
"Ambjorn",
"Jan",
""
],
[
"Gizbert-Studnicki",
"Jakub",
""
],
[
"Görlich",
"Andrzej",
""
],
[
"Jurkiewicz",
"Jerzy",
""
]
] | The Causal Dynamical Triangulation model of quantum gravity (CDT) has a transfer matrix, relating spatial geometries at adjacent (discrete lattice) times. The transfer matrix uniquely determines the theory. We show that the measurements of the scale factor of the (CDT) universe are well described by an effective transf... | 10.706573 | 7.39008 | 11.080948 | 8.456234 | 8.352308 | 7.92021 | 7.836907 | 8.343741 | 8.251629 | 12.425924 | 8.920838 | 9.290835 | 10.449819 | 9.647514 | 9.635553 | 9.768313 | 9.745093 | 9.810062 | 9.520101 | 10.168747 | 9.709404 |
hep-th/9411019 | Vipul Periwal | Vipul Periwal | Free energy decreases along Wilson renormalization group trajectories | 7 pages, TeX | Mod. Phys. Lett. A10 (1995) 1543 | 10.1142/S0217732395001666 | PUPT-1481 | hep-th | null | The free energy is shown to decrease along Wilson renormalization group
trajectories, in a dimension-independent fashion, for $d>2.$ The argument
assumes the monotonicity of the cutoff function, and positivity of a spectral
representation of the two point function. The argument is valid to all orders
in perturbation ... | [
{
"created": "Wed, 2 Nov 1994 23:06:20 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Periwal",
"Vipul",
""
]
] | The free energy is shown to decrease along Wilson renormalization group trajectories, in a dimension-independent fashion, for $d>2.$ The argument assumes the monotonicity of the cutoff function, and positivity of a spectral representation of the two point function. The argument is valid to all orders in perturbation th... | 15.012602 | 8.908021 | 12.788114 | 9.895578 | 9.546108 | 8.970034 | 9.430617 | 9.039528 | 9.700666 | 13.701519 | 9.697024 | 10.70405 | 11.902586 | 10.726685 | 10.665176 | 10.213735 | 10.334777 | 10.492514 | 10.815351 | 12.176949 | 10.150583 |
2009.07674 | Jean-Fran\c{c}ois Fortin | Jean-Fran\c{c}ois Fortin, Wen-Jie Ma, Witold Skiba | All Global One- and Two-Dimensional Higher-Point Conformal Blocks | 1+20 pages + appendixes, 10 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a full set of rules to directly express all $M$-point conformal
blocks in one- and two-dimensional conformal field theories, irrespective of
the topology. The $M$-point conformal blocks are power series expansion in some
carefully-chosen conformal cross-ratios. We then prove the rules for any
topology co... | [
{
"created": "Wed, 16 Sep 2020 13:33:57 GMT",
"version": "v1"
}
] | 2020-09-17 | [
[
"Fortin",
"Jean-François",
""
],
[
"Ma",
"Wen-Jie",
""
],
[
"Skiba",
"Witold",
""
]
] | We introduce a full set of rules to directly express all $M$-point conformal blocks in one- and two-dimensional conformal field theories, irrespective of the topology. The $M$-point conformal blocks are power series expansion in some carefully-chosen conformal cross-ratios. We then prove the rules for any topology cons... | 10.912436 | 10.034038 | 11.11353 | 9.705612 | 10.020246 | 10.027769 | 10.735614 | 10.028965 | 10.031425 | 11.755724 | 9.804851 | 10.564484 | 10.763142 | 10.280774 | 10.134254 | 10.104013 | 10.226068 | 10.604897 | 10.221776 | 10.659868 | 10.068265 |
hep-th/0111227 | Dimitri Polyakov | Dimitri Polyakov | BRST Properties of New Superstring States | 25 pages, harvmac.tex | Phys.Rev. D65 (2002) 084041 | 10.1103/PhysRevD.65.084041 | HIP-2001-61/TH | hep-th | null | Brane-like states are defined by physical vertex operators in NSR superstring
theory, existing at nonzero pictures only. These states exist both in open and
closed string theories, in the NS and NS-NS sectors respectively. In this paper
we present a detailed analysis of their BRST properties, giving a proof that
thes... | [
{
"created": "Mon, 26 Nov 2001 14:31:26 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Polyakov",
"Dimitri",
""
]
] | Brane-like states are defined by physical vertex operators in NSR superstring theory, existing at nonzero pictures only. These states exist both in open and closed string theories, in the NS and NS-NS sectors respectively. In this paper we present a detailed analysis of their BRST properties, giving a proof that these ... | 13.924695 | 11.858802 | 14.393242 | 11.716179 | 12.028943 | 11.864704 | 14.211843 | 11.490743 | 11.292863 | 15.109763 | 11.54647 | 11.676165 | 13.057481 | 12.285111 | 12.513959 | 11.640551 | 12.01487 | 11.796828 | 12.272725 | 12.787988 | 11.987424 |
hep-th/0305044 | Eric A. Nicholson | Eric Nicholson | Perturbative Wilsonian Formalism for Noncommutative Gauge Theories in
the Matrix Representation | PhD thesis, Latex, 84 pages, 13 figures | null | null | null | hep-th | null | We study the perturbative approach to the Wilsonian integration of
noncommutative gauge theories in the matrix representation. We begin by
motivating the study of noncommutative gauge theories and reviewing the matrix
formulation. We then systematically develop the perturbative treatment of UV
states and calculate bo... | [
{
"created": "Wed, 7 May 2003 03:05:32 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nicholson",
"Eric",
""
]
] | We study the perturbative approach to the Wilsonian integration of noncommutative gauge theories in the matrix representation. We begin by motivating the study of noncommutative gauge theories and reviewing the matrix formulation. We then systematically develop the perturbative treatment of UV states and calculate both... | 9.084717 | 9.055492 | 9.673342 | 8.895249 | 9.596478 | 8.765488 | 9.547264 | 9.283376 | 8.711805 | 9.877928 | 9.00007 | 9.033937 | 9.054775 | 8.944217 | 9.085841 | 9.141943 | 8.916944 | 8.842149 | 8.980221 | 9.224857 | 8.935284 |
hep-th/0304152 | S. Kalyana Rama | S. Kalyana Rama | Asymptotic Density of Open p-brane States with Zero-modes included | 9 pages, Latex. V 2: Results are for open p-branes only; Title
modified; a few references and an acknowledgement added | Phys.Lett. B566 (2003) 152-156 | 10.1016/S0370-2693(03)00799-8 | IMSc/2003/04/05 | hep-th gr-qc | null | We obtain the asymptotic density of open p-brane states with zero-modes
included. The resulting logarithmic correction to the p-brane entropy has a
coefficient - \frac{p + 2}{2 p}, and is independent of the dimension of the
embedding spacetime. Such logarithmic corrections to the entropy, with
precisely this coeffici... | [
{
"created": "Thu, 17 Apr 2003 10:46:30 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Apr 2003 11:38:18 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Rama",
"S. Kalyana",
""
]
] | We obtain the asymptotic density of open p-brane states with zero-modes included. The resulting logarithmic correction to the p-brane entropy has a coefficient - \frac{p + 2}{2 p}, and is independent of the dimension of the embedding spacetime. Such logarithmic corrections to the entropy, with precisely this coefficien... | 9.564774 | 7.820601 | 8.426163 | 7.487328 | 7.796247 | 8.184109 | 7.36666 | 7.11307 | 7.950494 | 9.217624 | 7.831892 | 7.960076 | 7.75214 | 8.065316 | 8.210804 | 7.899121 | 7.749829 | 7.90889 | 7.623993 | 8.382473 | 8.02493 |
0705.0143 | J. Antonio Garcia Zenteno | J. Antonio Garcia | DSR and Canonical Transformations: A Comment on a ``A Lagrangian for DSR
particle and the role of noncommutativity'' | 3 pages. Accepted in PRD. v2 Fixed typos, reference added, version
for PRD | Phys.Rev.D76:048501,2007 | 10.1103/PhysRevD.76.048501 | null | hep-th gr-qc math-ph math.MP | null | The aim of this comment is to call to the attention of DSR readers a basic
fact. The introduction of noncommutative structures in problems like the one
addressed in [1] is not necessary for the understanding of DSR physics. It can
be described just as the relativistic free particle problem in a different
parametrizat... | [
{
"created": "Tue, 1 May 2007 17:17:27 GMT",
"version": "v1"
},
{
"created": "Sat, 18 Aug 2007 02:26:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Garcia",
"J. Antonio",
""
]
] | The aim of this comment is to call to the attention of DSR readers a basic fact. The introduction of noncommutative structures in problems like the one addressed in [1] is not necessary for the understanding of DSR physics. It can be described just as the relativistic free particle problem in a different parametrizatio... | 18.292507 | 15.426126 | 17.16025 | 15.31447 | 14.732554 | 13.83823 | 15.069962 | 15.774639 | 15.673158 | 17.0576 | 15.540627 | 14.492382 | 15.707561 | 15.386169 | 14.892531 | 14.812799 | 14.692069 | 14.250914 | 15.731957 | 15.803389 | 15.355953 |
1711.02108 | Anton De La Fuente | Gabriel Cuomo, Anton de la Fuente, Alexander Monin, David
Pirtskhalava, and Riccardo Rattazzi | Rotating superfluids and spinning charged operators in conformal field
theory | 7 pages | Phys. Rev. D 97, 045012 (2018) | 10.1103/PhysRevD.97.045012 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the scaling dimensions of operators with large global charge and
spin in 2+1 dimensional conformal field theories. By the state-operator
correspondence, these operators correspond to superfluids with vortices and can
be systematically studied using effective field theory. As the spin increases
from zero ... | [
{
"created": "Mon, 6 Nov 2017 19:00:15 GMT",
"version": "v1"
}
] | 2018-02-19 | [
[
"Cuomo",
"Gabriel",
""
],
[
"de la Fuente",
"Anton",
""
],
[
"Monin",
"Alexander",
""
],
[
"Pirtskhalava",
"David",
""
],
[
"Rattazzi",
"Riccardo",
""
]
] | We calculate the scaling dimensions of operators with large global charge and spin in 2+1 dimensional conformal field theories. By the state-operator correspondence, these operators correspond to superfluids with vortices and can be systematically studied using effective field theory. As the spin increases from zero to... | 7.887056 | 7.023906 | 9.205195 | 6.960181 | 7.746536 | 7.203831 | 6.851621 | 6.737387 | 7.112485 | 8.920758 | 7.035455 | 7.38027 | 7.980958 | 7.460218 | 7.350671 | 7.51962 | 7.295739 | 7.546079 | 7.481432 | 8.035941 | 7.24463 |
hep-th/0003199 | Constantin Bizdadea | C. Bizdadea | Consistent interactions in the Hamiltonian BRST formalism | Latex 2.09, 13 pages, submitted to Phys. Lett. B | Acta Phys.Polon. B32 (2001) 2843-2862 | null | null | hep-th | null | A Hamiltonian BRST deformation procedure for obtaining consistent
interactions among fields with gauge freedom is proposed. The general theory is
exemplified on the three-dimensional Chern-Simons model.
| [
{
"created": "Wed, 22 Mar 2000 14:51:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bizdadea",
"C.",
""
]
] | A Hamiltonian BRST deformation procedure for obtaining consistent interactions among fields with gauge freedom is proposed. The general theory is exemplified on the three-dimensional Chern-Simons model. | 16.475878 | 11.408782 | 15.503466 | 10.897128 | 10.644006 | 10.748883 | 11.033148 | 10.985678 | 10.620241 | 15.815778 | 12.163939 | 12.170595 | 15.020113 | 11.919676 | 12.629169 | 12.341012 | 12.176347 | 12.300155 | 11.959574 | 14.547078 | 12.239714 |
2207.08835 | Amitabha Lahiri | Shantonu Mukherjee and Amitabha Lahiri | Spin-flux attachment by dimensional reduction of vortices | null | null | 10.1016/j.nuclphysb.2022.116050 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The description of a system of vortices in terms of dual fields provides a
window to new phases of the system. It was found recently that dualizing a
3+1-d boson-fermion system leads to a system of fermions and vortices
interacting via a 2-form field through a non-local term. Here we explore some
consequences of such... | [
{
"created": "Mon, 18 Jul 2022 18:00:03 GMT",
"version": "v1"
}
] | 2023-01-04 | [
[
"Mukherjee",
"Shantonu",
""
],
[
"Lahiri",
"Amitabha",
""
]
] | The description of a system of vortices in terms of dual fields provides a window to new phases of the system. It was found recently that dualizing a 3+1-d boson-fermion system leads to a system of fermions and vortices interacting via a 2-form field through a non-local term. Here we explore some consequences of such a... | 8.254154 | 7.666758 | 7.901378 | 7.118486 | 7.665212 | 7.403354 | 7.117255 | 7.018708 | 7.062311 | 8.504273 | 7.234442 | 7.122018 | 7.31931 | 7.020881 | 7.060784 | 6.950263 | 6.911817 | 7.127835 | 7.016466 | 7.513773 | 6.93654 |
2306.00941 | Shunyu Yao | Andreas Blommaert, Thomas G. Mertens, Shunyu Yao | Dynamical actions and q-representation theory for double-scaled SYK | 51 pages, v2: matches published version | JHEP02(2024)067 | 10.1007/JHEP02(2024)067 | null | hep-th math-ph math.MP math.QA math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that DSSYK amplitudes are reproduced by considering the quantum
mechanics of a constrained particle on the quantum group SU$_q(1,1)$. We
construct its left-and right-regular representations, and show that the
representation matrices reproduce two-sided wavefunctions and correlation
functions of DSSYK. We then... | [
{
"created": "Thu, 1 Jun 2023 17:41:54 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Feb 2024 00:36:09 GMT",
"version": "v2"
}
] | 2024-02-27 | [
[
"Blommaert",
"Andreas",
""
],
[
"Mertens",
"Thomas G.",
""
],
[
"Yao",
"Shunyu",
""
]
] | We show that DSSYK amplitudes are reproduced by considering the quantum mechanics of a constrained particle on the quantum group SU$_q(1,1)$. We construct its left-and right-regular representations, and show that the representation matrices reproduce two-sided wavefunctions and correlation functions of DSSYK. We then c... | 14.202435 | 13.414953 | 15.959079 | 13.54691 | 13.756188 | 13.870187 | 13.266241 | 14.214839 | 13.806604 | 16.945795 | 13.335845 | 13.896001 | 14.866116 | 14.017389 | 13.904655 | 14.208459 | 14.433228 | 13.880369 | 14.233471 | 14.524263 | 13.256926 |
1006.2623 | Dmitri Fursaev | Dmitri V. Fursaev | `Thermodynamics' of Minimal Surfaces and Entropic Origin of Gravity | 12 pages, 1 figure | Phys.Rev.D82:064013,2010 | 10.1103/PhysRevD.82.064013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Deformations of minimal surfaces lying in constant time slices in static
space-times are studied. An exact and universal formula for a change of the
area of a minimal surface under shifts of nearby point-like particles is found.
It allows one to introduce a local temperature on the surface and represent
variations of... | [
{
"created": "Mon, 14 Jun 2010 07:39:08 GMT",
"version": "v1"
}
] | 2014-11-21 | [
[
"Fursaev",
"Dmitri V.",
""
]
] | Deformations of minimal surfaces lying in constant time slices in static space-times are studied. An exact and universal formula for a change of the area of a minimal surface under shifts of nearby point-like particles is found. It allows one to introduce a local temperature on the surface and represent variations of i... | 13.812981 | 12.541794 | 14.744481 | 11.107306 | 12.662137 | 12.592514 | 12.661636 | 11.774501 | 12.074998 | 13.64035 | 12.524418 | 11.600649 | 11.862798 | 11.494552 | 11.471688 | 11.378942 | 11.885557 | 11.300033 | 11.714924 | 11.744241 | 12.289474 |
hep-th/0106218 | Tetsuyuki Muramatsu | Y. Kazama and T. Muramatsu | Fully Off-shell Effective Action and its Supersymmetry in Matrix Theory
II | 21 pages; v2: References and a footnote added | Class.Quant.Grav. 18 (2001) 5545-5560 | 10.1088/0264-9381/18/24/315 | UT-Komaba 01-02 | hep-th | null | In a previous work, we computed the fully off-shell effective action $\Gamma$
and the corresponding quantum-corrected supersymmetry (SUSY) transformation
operator $\delta_\epsilon$ for the so-called source-probe configuration in
Matrix theory at one loop at order 4 in the derivative expansion, and showed
that they sa... | [
{
"created": "Mon, 25 Jun 2001 07:17:47 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Oct 2001 13:22:03 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Kazama",
"Y.",
""
],
[
"Muramatsu",
"T.",
""
]
] | In a previous work, we computed the fully off-shell effective action $\Gamma$ and the corresponding quantum-corrected supersymmetry (SUSY) transformation operator $\delta_\epsilon$ for the so-called source-probe configuration in Matrix theory at one loop at order 4 in the derivative expansion, and showed that they sati... | 8.618604 | 7.41921 | 9.212742 | 7.37109 | 8.276784 | 7.687819 | 7.836661 | 7.871023 | 7.967597 | 8.885242 | 7.472324 | 7.904296 | 8.148339 | 7.712263 | 8.186365 | 7.532605 | 7.858524 | 7.833379 | 7.66568 | 8.473842 | 7.660994 |
1510.07077 | Yisong Yang Professor | Xiaosen Han and Yisong Yang | Magnetic Impurity Inspired Abelian Higgs Vortices | 19 pages | Journal of High Energy Physics 2 (2016) 046 | 10.1007/JHEP02(2016)046 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inspired by magnetic impurity considerations some broad classes of Abelian
Higgs and Chern--Simons--Higgs BPS vortex equations are derived and analyzed.
| [
{
"created": "Fri, 23 Oct 2015 22:15:43 GMT",
"version": "v1"
}
] | 2017-09-14 | [
[
"Han",
"Xiaosen",
""
],
[
"Yang",
"Yisong",
""
]
] | Inspired by magnetic impurity considerations some broad classes of Abelian Higgs and Chern--Simons--Higgs BPS vortex equations are derived and analyzed. | 39.133518 | 23.886082 | 39.629395 | 26.889038 | 27.093594 | 24.052036 | 23.86525 | 26.332336 | 29.233887 | 36.405621 | 23.425894 | 31.3332 | 36.661964 | 30.964756 | 29.983833 | 29.379486 | 29.880451 | 30.15266 | 30.87521 | 35.526386 | 29.538408 |
1208.5082 | Taeyoon Moon | Taeyoon Moon and Yun Soo Myung | Rank-3 finite temperature logarithmic conformal field theory | 19 pages, no figure | null | 10.1103/PhysRevD.86.084058 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a rank-3 finite temperature logarithmic conformal field theory
(LCFT) starting from a higher-derivative scalar field model in the BTZ black
hole background. Its zero temperature limit reduces to a rank-3 LCFT in the
AdS$_3$ background. For a tricritical generalized massive gravity, we read off
the log-sq... | [
{
"created": "Sat, 25 Aug 2012 00:17:21 GMT",
"version": "v1"
}
] | 2013-05-30 | [
[
"Moon",
"Taeyoon",
""
],
[
"Myung",
"Yun Soo",
""
]
] | We construct a rank-3 finite temperature logarithmic conformal field theory (LCFT) starting from a higher-derivative scalar field model in the BTZ black hole background. Its zero temperature limit reduces to a rank-3 LCFT in the AdS$_3$ background. For a tricritical generalized massive gravity, we read off the log-squa... | 12.389629 | 11.173699 | 13.8817 | 10.661399 | 11.66239 | 11.695177 | 10.631076 | 10.558915 | 9.886829 | 12.321053 | 10.682069 | 10.737434 | 11.354811 | 11.018508 | 11.256494 | 11.274433 | 11.203315 | 11.056041 | 10.860854 | 12.086018 | 11.268427 |
hep-th/0403215 | J. M. Speight | N.M. Romao and J.M. Speight | Slow Schroedinger dynamics of gauged vortices | 22 pages, 2 figures | Nonlinearity.17:1337-1355,2004 | 10.1088/0951-7715/17/4/010 | Max-Planck-Institut fuer Mathematik Preprint 2004 (02) | hep-th | null | Multivortex dynamics in Manton's Schroedinger--Chern--Simons variant of the
Landau-Ginzburg model of thin superconductors is studied within a moduli space
approximation. It is shown that the reduced flow on M_N, the N vortex moduli
space, is hamiltonian with respect to \omega_{L^2}, the L^2 Kaehler form on
\M_N. A pu... | [
{
"created": "Mon, 22 Mar 2004 13:55:21 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Romao",
"N. M.",
""
],
[
"Speight",
"J. M.",
""
]
] | Multivortex dynamics in Manton's Schroedinger--Chern--Simons variant of the Landau-Ginzburg model of thin superconductors is studied within a moduli space approximation. It is shown that the reduced flow on M_N, the N vortex moduli space, is hamiltonian with respect to \omega_{L^2}, the L^2 Kaehler form on \M_N. A pure... | 9.42712 | 9.500824 | 11.345891 | 9.185309 | 10.485504 | 9.853249 | 9.598317 | 9.559603 | 9.04136 | 11.396049 | 9.134122 | 9.095973 | 9.48867 | 9.257454 | 9.329218 | 8.964122 | 8.745606 | 9.252886 | 9.095251 | 9.081358 | 9.118675 |
1012.3958 | Om Prakash Singh Negi | O. P. S. Negi and H. Dehnen | Gauge Formulation for Two Potential Theory of Dyons | Key words- Dual electrodynamics, duality, gauge invariance, monopoles
and dyons; PACS No.- 14.80 Hv | null | 10.1007/s10773-011-0733-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dual electrodynamics and corresponding Maxwell's equations (in the presence
of monopole only) are revisited from the symmetry of duality and gauge
invariance. Accordingly, the manifestly covariant, dual symmetric and gauge
invariant two potential theory of generalized electromagnetic fields of dyons
has been develope... | [
{
"created": "Fri, 17 Dec 2010 18:42:24 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Negi",
"O. P. S.",
""
],
[
"Dehnen",
"H.",
""
]
] | Dual electrodynamics and corresponding Maxwell's equations (in the presence of monopole only) are revisited from the symmetry of duality and gauge invariance. Accordingly, the manifestly covariant, dual symmetric and gauge invariant two potential theory of generalized electromagnetic fields of dyons has been developed ... | 13.598207 | 12.300522 | 13.731754 | 12.769969 | 13.443048 | 12.998075 | 12.084977 | 12.582122 | 12.54636 | 13.935294 | 13.852377 | 13.463654 | 13.057188 | 12.834464 | 13.558298 | 13.264731 | 13.807521 | 13.143618 | 13.421128 | 13.493742 | 13.106308 |
hep-th/0404231 | Gaston Giribet | Gaston Giribet, Daniel Lopez-Fogliani | Remarks on free field realization of SL(2,R)/U(1) x U(1) WZNW model | 24 pages, no figures. v2 references added; accepted for publication
in JHEP | JHEP 0406:026,2004 | 10.1088/1126-6708/2004/06/026 | null | hep-th | null | Free field representations of vertex algebra in SL(2,R)/U(1) x U(1) WZNW
model are constructed by considering a twisted version of the
Bershadsky-Kutasov free field description of discrete states in the
two-dimensional black hole CFT. These correspond to conjugate representations
describing primary states in the mode... | [
{
"created": "Wed, 28 Apr 2004 21:27:21 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Jun 2004 17:29:16 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Giribet",
"Gaston",
""
],
[
"Lopez-Fogliani",
"Daniel",
""
]
] | Free field representations of vertex algebra in SL(2,R)/U(1) x U(1) WZNW model are constructed by considering a twisted version of the Bershadsky-Kutasov free field description of discrete states in the two-dimensional black hole CFT. These correspond to conjugate representations describing primary states in the model ... | 12.522996 | 12.09282 | 17.07757 | 12.185658 | 13.228957 | 11.585057 | 12.0622 | 11.730372 | 10.908731 | 14.808597 | 11.054426 | 11.305072 | 12.211638 | 11.054621 | 10.945349 | 11.532488 | 11.50733 | 11.240733 | 10.670983 | 12.508938 | 10.943248 |
1107.0643 | Roland Kirschner | D. Chicherin, S. Derkachov, D. Karakhanyan, R. Kirschner | Baxter operators for arbitrary spin II | 33 pages LaTex, version for publication | null | 10.1016/j.nuclphysb.2011.08.026 | null | hep-th math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper presents the second part of our study devoted to the construction
of Baxter operators for the homogeneous closed XXX spin chain with the quantum
space carrying infinite or finite-dimensional $s\ell_2$ representations. We
consider the Baxter operators used in \cite{BLZ,Shortcut}, formulate their
constructio... | [
{
"created": "Mon, 4 Jul 2011 14:46:28 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Sep 2011 09:33:56 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Chicherin",
"D.",
""
],
[
"Derkachov",
"S.",
""
],
[
"Karakhanyan",
"D.",
""
],
[
"Kirschner",
"R.",
""
]
] | This paper presents the second part of our study devoted to the construction of Baxter operators for the homogeneous closed XXX spin chain with the quantum space carrying infinite or finite-dimensional $s\ell_2$ representations. We consider the Baxter operators used in \cite{BLZ,Shortcut}, formulate their construction ... | 18.474094 | 17.888796 | 20.922705 | 18.09581 | 19.02317 | 19.757542 | 19.64558 | 17.821276 | 18.476839 | 22.0205 | 17.784637 | 18.378885 | 19.324188 | 18.058495 | 18.330408 | 17.957975 | 18.604492 | 18.345076 | 18.190393 | 19.459379 | 18.24098 |
1311.4363 | Hrvoje Nikolic | H. Nikolic | Suppressing Hawking radiation by quantum Zeno effect | 11 pages, revised, accepted for publication in Phys. Lett. B | Phys. Lett. B 733, 6 (2014) | 10.1016/j.physletb.2014.04.017 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present evidence that quantum Zeno effect, otherwise working only for
microscopic systems, may also work for large black holes (BH's). The
expectation that a BH geometry should behave classically at time intervals
larger than the Planck time t_Pl indicates that the quantum process of
measurement of classical degre... | [
{
"created": "Mon, 18 Nov 2013 13:11:18 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Apr 2014 09:49:43 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Nikolic",
"H.",
""
]
] | We present evidence that quantum Zeno effect, otherwise working only for microscopic systems, may also work for large black holes (BH's). The expectation that a BH geometry should behave classically at time intervals larger than the Planck time t_Pl indicates that the quantum process of measurement of classical degrees... | 12.016821 | 13.805482 | 11.730187 | 12.102453 | 12.085808 | 13.923813 | 12.795969 | 12.605987 | 11.405473 | 12.762904 | 11.39344 | 11.242944 | 11.334732 | 11.28094 | 11.71707 | 11.564763 | 11.604189 | 11.345508 | 11.461464 | 12.07182 | 10.917862 |
hep-th/9309093 | Dunbar | David C. Dunbar and Keith G. Joshi | Maverick Examples Of Coset Conformal Field Theories | 16pages , reportSWAT-93-07 | Mod.Phys.Lett. A8 (1993) 2803-2814 | 10.1142/S0217732393003196 | null | hep-th | null | We present coset conformal field theories whose spectrum is not determined by
the identification current method. In these ``maverick'' cosets there is a
larger symmetry identifying primary fields than under the identification
current. We find an A-D-E classification of these mavericks. }
| [
{
"created": "Fri, 17 Sep 1993 00:05:44 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Dunbar",
"David C.",
""
],
[
"Joshi",
"Keith G.",
""
]
] | We present coset conformal field theories whose spectrum is not determined by the identification current method. In these ``maverick'' cosets there is a larger symmetry identifying primary fields than under the identification current. We find an A-D-E classification of these mavericks. } | 27.23715 | 29.79146 | 26.951393 | 21.65234 | 23.673864 | 22.515436 | 27.113045 | 24.284311 | 19.708626 | 26.640497 | 22.602713 | 25.24535 | 26.389856 | 23.784031 | 25.054085 | 24.869743 | 24.528105 | 25.392616 | 25.003876 | 26.906155 | 24.294783 |
hep-th/0309196 | Armen Nersessian | Armen Nersessian and Armen Yeranyan | 3D Oscillator and Coulomb Systems reduced from Kahler spaces | To the memory of Professor Valery Ter-Antonyan, 11 pages | J.Phys.A37:2791-2802,2004 | 10.1088/0305-4470/37/7/020 | null | hep-th math-ph math.MP nlin.SI quant-ph | null | We define the oscillator and Coulomb systems on four-dimensional spaces with
U(2)-invariant Kahler metric and perform their Hamiltonian reduction to the
three-dimensional oscillator and Coulomb systems specified by the presence of
Dirac monopoles. We find the Kahler spaces with conic singularity, where the
oscillator... | [
{
"created": "Fri, 19 Sep 2003 10:16:47 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Nersessian",
"Armen",
""
],
[
"Yeranyan",
"Armen",
""
]
] | We define the oscillator and Coulomb systems on four-dimensional spaces with U(2)-invariant Kahler metric and perform their Hamiltonian reduction to the three-dimensional oscillator and Coulomb systems specified by the presence of Dirac monopoles. We find the Kahler spaces with conic singularity, where the oscillator a... | 8.453347 | 9.102695 | 9.397867 | 9.076518 | 8.099876 | 7.853485 | 9.045718 | 8.303782 | 9.040198 | 9.031531 | 8.536137 | 8.503677 | 9.025797 | 8.292519 | 8.616737 | 8.628708 | 8.469707 | 8.144565 | 8.40361 | 8.890868 | 8.593689 |
hep-th/0609087 | Dan Israel | Dan Israel and Eliezer Rabinovici | Rolling tachyon in anti-de Sitter space-time | JHEP style, 45 pages, one figure; v2: typos corrected, references
added, version to appear in JHEP | JHEP 0701:069,2007 | 10.1088/1126-6708/2007/01/069 | null | hep-th | null | We study the decay of the unstable D-particle in three-dimensional anti-de
Sitter space-time using worldsheet boundary conformal field theory methods. We
test the open string completeness conjecture in a background for which the
phase space available is only field-theoretic. This could present a serious
challenge to ... | [
{
"created": "Tue, 12 Sep 2006 22:05:37 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Jan 2007 13:17:14 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Israel",
"Dan",
""
],
[
"Rabinovici",
"Eliezer",
""
]
] | We study the decay of the unstable D-particle in three-dimensional anti-de Sitter space-time using worldsheet boundary conformal field theory methods. We test the open string completeness conjecture in a background for which the phase space available is only field-theoretic. This could present a serious challenge to th... | 12.133283 | 11.445186 | 12.641776 | 11.04973 | 11.773173 | 11.209484 | 11.333068 | 11.04183 | 10.86934 | 13.813651 | 10.935538 | 11.029145 | 12.356427 | 11.236896 | 11.123534 | 10.652697 | 11.22007 | 11.348875 | 11.294593 | 12.278511 | 11.106048 |
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