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values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1811.11577 | Hidenori Fukaya | Hidenori Fukaya | Why is quantum gravity so difficult (compared to QCD)? | 14 pages, misreading counting of degrees of freedom under the
vierbein postulate corrected | Soryushiron Kenkyu 25 (2016) 2 | null | OU-HET-990 | hep-th gr-qc hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gravity is difficult to quantize. This is a well-known fact but its reason is
given simply by non-renormalizability of the Newton constant and little is
discussed why among many quantum gauge theories, gravity is special. In this
essay we try to treat the gravity as one of many gauge theories, and discuss
how it is s... | [
{
"created": "Tue, 27 Nov 2018 06:20:54 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Dec 2018 03:19:42 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Mar 2020 02:48:01 GMT",
"version": "v3"
}
] | 2020-03-18 | [
[
"Fukaya",
"Hidenori",
""
]
] | Gravity is difficult to quantize. This is a well-known fact but its reason is given simply by non-renormalizability of the Newton constant and little is discussed why among many quantum gauge theories, gravity is special. In this essay we try to treat the gravity as one of many gauge theories, and discuss how it is spe... | 12.958165 | 11.704313 | 13.082831 | 10.675411 | 11.878636 | 11.823002 | 11.212745 | 11.163112 | 10.962029 | 11.971729 | 11.896935 | 11.801089 | 11.923105 | 11.416455 | 12.083797 | 12.223774 | 12.013128 | 11.803687 | 11.243279 | 12.11437 | 10.748915 |
1507.07556 | Angel M. Uranga | Renata Kallosh, Fernando Quevedo, Angel M. Uranga | String Theory Realizations of the Nilpotent Goldstino | 33 pages, 8 figures. v2: reference added, minor changes | null | 10.1007/JHEP12(2015)039 | DAMTP-2015-36, IFT-UAM/CSIC-15-079 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe in detail how the spectrum of a single anti-D3-brane in
four-dimensional orientifolded IIB string models reproduces precisely the field
content of a nilpotent chiral superfield with the only physical component
corresponding to the fermionic goldstino. In particular we explicitly consider
a single anti-D3-... | [
{
"created": "Mon, 27 Jul 2015 20:00:37 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Aug 2015 15:28:31 GMT",
"version": "v2"
}
] | 2016-01-27 | [
[
"Kallosh",
"Renata",
""
],
[
"Quevedo",
"Fernando",
""
],
[
"Uranga",
"Angel M.",
""
]
] | We describe in detail how the spectrum of a single anti-D3-brane in four-dimensional orientifolded IIB string models reproduces precisely the field content of a nilpotent chiral superfield with the only physical component corresponding to the fermionic goldstino. In particular we explicitly consider a single anti-D3-br... | 8.141173 | 7.568954 | 9.385757 | 7.676137 | 8.063648 | 8.097202 | 7.678171 | 7.795656 | 7.477361 | 9.90057 | 7.272041 | 7.288432 | 7.84123 | 7.783356 | 7.677331 | 7.794441 | 7.805047 | 7.708287 | 7.843427 | 7.773742 | 7.761329 |
1511.01406 | Luis Apolo | Luis Apolo | The covariant action of higher spin black holes in three dimensions | 20 pages; v2: clarified the origin of the boundary term at the
horizon, matches published version | JHEP05 (2016) 097 | 10.1007/JHEP05(2016)097 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a set of boundary terms for higher spin theories in AdS$_3$ that
lead to a well-defined variational principle compatible with Dirichlet boundary
conditions for the metric and higher spin fields. These boundary terms are
valid for higher spin theories in the Fefferman-Graham gauge and they allow us
to compu... | [
{
"created": "Wed, 4 Nov 2015 17:33:57 GMT",
"version": "v1"
},
{
"created": "Wed, 18 May 2016 13:07:36 GMT",
"version": "v2"
}
] | 2016-05-19 | [
[
"Apolo",
"Luis",
""
]
] | We propose a set of boundary terms for higher spin theories in AdS$_3$ that lead to a well-defined variational principle compatible with Dirichlet boundary conditions for the metric and higher spin fields. These boundary terms are valid for higher spin theories in the Fefferman-Graham gauge and they allow us to compute... | 6.637394 | 6.248378 | 8.72971 | 6.164244 | 7.141994 | 7.300343 | 7.087407 | 6.436769 | 6.473607 | 7.720593 | 6.402663 | 6.239607 | 6.833873 | 6.066347 | 6.409716 | 5.880379 | 5.978448 | 6.377771 | 5.992885 | 6.45409 | 6.176272 |
hep-th/9804099 | Renata Kallosh | Renata Kallosh and Antoine Van Proeyen | Conformal Symmetry of Supergravities in AdS spaces | 14 pages, Latex | Phys.Rev. D60 (1999) 026001 | 10.1103/PhysRevD.60.026001 | SU-ITP-98/23, KUL-TF-98/20 | hep-th | null | We show that the background field method applied to supergravity in adS
space-time provides the path integral for the theory in the bulk with conformal
symmetry associated with the isometry of the adS space. This in turn allows to
establish the rigid conformal invariance of the generating functional for the
supergrav... | [
{
"created": "Tue, 14 Apr 1998 23:32:04 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Kallosh",
"Renata",
""
],
[
"Van Proeyen",
"Antoine",
""
]
] | We show that the background field method applied to supergravity in adS space-time provides the path integral for the theory in the bulk with conformal symmetry associated with the isometry of the adS space. This in turn allows to establish the rigid conformal invariance of the generating functional for the supergravit... | 10.696177 | 12.038884 | 10.809122 | 10.255464 | 10.088093 | 12.01106 | 9.657714 | 11.039618 | 10.352592 | 10.808883 | 10.332199 | 9.926801 | 10.786872 | 9.739282 | 10.071312 | 10.026947 | 10.841304 | 10.46723 | 10.152175 | 10.456762 | 9.457905 |
0804.2110 | Yutaka Matsuo | Pei-Ming Ho, Ru-Chuen Hou and Yutaka Matsuo | Lie 3-Algebra and Multiple M2-branes | 28 pages | JHEP 0806:020,2008 | 10.1088/1126-6708/2008/06/020 | UT-08-08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the recent proposal of an N=8 supersymmetric action for multiple
M2-branes, we study the Lie 3-algebra in detail. In particular, we focus on the
fundamental identity and the relation with Nambu-Poisson bracket. Some new
algebras not known in the literature are found. Next we consider cubic matrix
represe... | [
{
"created": "Mon, 14 Apr 2008 18:17:17 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Apr 2008 11:54:36 GMT",
"version": "v2"
}
] | 2009-12-04 | [
[
"Ho",
"Pei-Ming",
""
],
[
"Hou",
"Ru-Chuen",
""
],
[
"Matsuo",
"Yutaka",
""
]
] | Motivated by the recent proposal of an N=8 supersymmetric action for multiple M2-branes, we study the Lie 3-algebra in detail. In particular, we focus on the fundamental identity and the relation with Nambu-Poisson bracket. Some new algebras not known in the literature are found. Next we consider cubic matrix represent... | 7.279272 | 6.236173 | 8.197984 | 6.455794 | 6.639365 | 6.938619 | 6.72441 | 6.736255 | 6.862859 | 8.468519 | 6.457818 | 6.760278 | 7.348686 | 6.990505 | 6.858924 | 6.927604 | 7.08793 | 7.035835 | 7.008454 | 7.529712 | 7.043158 |
1512.02532 | Marius de Leeuw | Isak Buhl-Mortensen, Marius de Leeuw, Charlotte Kristjansen and
Konstantin Zarembo | One-point Functions in AdS/dCFT from Matrix Product States | updated reference | null | 10.1007/JHEP02(2016)052 | NORDITA-2015-132, UUITP-26/15 | hep-th cond-mat.stat-mech nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One-point functions of certain non-protected scalar operators in the defect
CFT dual to the D3-D5 probe brane system with k units of world volume flux can
be expressed as overlaps between Bethe eigenstates of the Heisenberg spin chain
and a matrix product state. We present a closed expression of determinant form
for ... | [
{
"created": "Tue, 8 Dec 2015 16:42:34 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Dec 2015 19:11:53 GMT",
"version": "v2"
}
] | 2016-03-23 | [
[
"Buhl-Mortensen",
"Isak",
""
],
[
"de Leeuw",
"Marius",
""
],
[
"Kristjansen",
"Charlotte",
""
],
[
"Zarembo",
"Konstantin",
""
]
] | One-point functions of certain non-protected scalar operators in the defect CFT dual to the D3-D5 probe brane system with k units of world volume flux can be expressed as overlaps between Bethe eigenstates of the Heisenberg spin chain and a matrix product state. We present a closed expression of determinant form for th... | 6.684275 | 6.084748 | 8.761333 | 6.337131 | 6.402852 | 6.30471 | 6.403472 | 6.248587 | 6.486893 | 9.006082 | 6.014555 | 6.34477 | 7.525849 | 6.511182 | 6.772384 | 6.577849 | 6.398898 | 6.555027 | 6.627865 | 7.097223 | 6.531216 |
2209.12541 | Michel Rausch de Traubenberg | Florian Domingo, Michel Rausch de Traubenberg | Supergravity: Application in Particle Physics | Invited chapter for Handbook of Quantum Gravity (Eds. C. Bambi,
L.Modesto and I.L. Shapiro, Springer Singapore, expected in 2023) | null | null | null | hep-th hep-ph math-ph math.MP | http://creativecommons.org/licenses/by-nc-nd/4.0/ | We provide a pedagogical introduction to $N=1$ supergravity/supersymmetry in
relation to particle physics. The various steps in the construction of a
generic $N=1$ supergravity model are briefly described, and we focus on its low
energy supersymmetric limit. The conditions for supersymmetry and supergravity
breaking ... | [
{
"created": "Mon, 26 Sep 2022 09:51:16 GMT",
"version": "v1"
}
] | 2022-09-28 | [
[
"Domingo",
"Florian",
""
],
[
"de Traubenberg",
"Michel Rausch",
""
]
] | We provide a pedagogical introduction to $N=1$ supergravity/supersymmetry in relation to particle physics. The various steps in the construction of a generic $N=1$ supergravity model are briefly described, and we focus on its low energy supersymmetric limit. The conditions for supersymmetry and supergravity breaking ar... | 8.279838 | 7.859893 | 8.013833 | 7.696628 | 8.390594 | 8.450979 | 9.096837 | 8.774774 | 8.007471 | 7.454328 | 8.24048 | 7.779236 | 7.430841 | 7.788604 | 7.788585 | 7.940259 | 8.19578 | 8.036969 | 7.699694 | 7.627731 | 8.09827 |
hep-th/0109099 | David Wiltshire | Jorma Louko and David L. Wiltshire | Brane worlds with bolts | 18 pages, 1 eps figure, JHEP3 with epsfig; v2,v3 references added | JHEP 02 (2002) 007 | 10.1088/1126-6708/2002/02/007 | ADP-00-45/M93 | hep-th gr-qc hep-ph | null | We construct a family of (p+3)-dimensional brane worlds in which the brane
has one compact extra dimension, the bulk has two extra dimensions, and the
bulk closes regularly at codimension two submanifolds known as bolts. The
(p+1)-dimensional low energy spacetime M_{low} may be any Einstein space with
an arbitrary co... | [
{
"created": "Wed, 12 Sep 2001 21:32:32 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Sep 2001 03:06:09 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Feb 2002 23:18:58 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Louko",
"Jorma",
""
],
[
"Wiltshire",
"David L.",
""
]
] | We construct a family of (p+3)-dimensional brane worlds in which the brane has one compact extra dimension, the bulk has two extra dimensions, and the bulk closes regularly at codimension two submanifolds known as bolts. The (p+1)-dimensional low energy spacetime M_{low} may be any Einstein space with an arbitrary cosm... | 9.004615 | 8.639491 | 9.496313 | 8.506339 | 9.070885 | 9.477002 | 9.949277 | 9.401249 | 9.158277 | 10.424106 | 8.766744 | 8.52234 | 9.304009 | 9.135949 | 8.92072 | 8.729271 | 8.738864 | 8.73806 | 8.864595 | 9.199237 | 8.69188 |
1307.2774 | Olaf Hohm | Eric A. Bergshoeff, Sjoerd de Haan, Olaf Hohm, Wout Merbis, Paul K.
Townsend | Zwei-Dreibein Gravity | 5 pages, v2: refs. added, to appear in PRL, v3: addendum included to
correct statement about absence of Boulware-Deser ghosts, and to show how
this problem is solved by a restriction of parameters; main conclusion about
compatibility of bulk and boundary unitarity is unaffected | null | 10.1103/PhysRevLett.111.111102 | DAMTP-2013-34, LMU-ASC 47/13, RUG-2013-26 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a generally-covariant and parity-invariant "zwei-dreibein" action
for gravity in three space-time dimensions that propagates two massive spin-2
modes, unitarily, and we use Hamiltonian methods to confirm the absence of
unphysical degrees of freedom. We show how zwei-dreibein gravity unifies
previous "3D ma... | [
{
"created": "Wed, 10 Jul 2013 12:40:40 GMT",
"version": "v1"
},
{
"created": "Mon, 9 Sep 2013 09:41:15 GMT",
"version": "v2"
},
{
"created": "Tue, 17 Dec 2013 00:05:11 GMT",
"version": "v3"
}
] | 2013-12-18 | [
[
"Bergshoeff",
"Eric A.",
""
],
[
"de Haan",
"Sjoerd",
""
],
[
"Hohm",
"Olaf",
""
],
[
"Merbis",
"Wout",
""
],
[
"Townsend",
"Paul K.",
""
]
] | We present a generally-covariant and parity-invariant "zwei-dreibein" action for gravity in three space-time dimensions that propagates two massive spin-2 modes, unitarily, and we use Hamiltonian methods to confirm the absence of unphysical degrees of freedom. We show how zwei-dreibein gravity unifies previous "3D mass... | 9.981992 | 8.672824 | 9.774856 | 8.785971 | 9.013635 | 8.20645 | 8.920286 | 7.975062 | 7.903985 | 10.11317 | 8.551304 | 9.084804 | 9.927668 | 9.189985 | 8.945163 | 9.003922 | 9.280619 | 8.848766 | 9.306538 | 9.055678 | 9.207224 |
hep-th/9308093 | Jakub Rembielinski | J. Rembielinski | Quantum Braided Poincar\'E Group | LaTeX (A4), 11pp., KFT UL 7/93 | null | null | null | hep-th | null | A new deformation of the of the Poincar\'e group and of the Minkowski
space-time is given. From the mathematical point of view this deformation is
rather quantum-braided group. Global and local structure of this
quantum-braided Poincar\'e group is investigated. A kind of ``quantum metrics''
is introduced in the $q$-M... | [
{
"created": "Thu, 19 Aug 1993 09:25:42 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rembielinski",
"J.",
""
]
] | A new deformation of the of the Poincar\'e group and of the Minkowski space-time is given. From the mathematical point of view this deformation is rather quantum-braided group. Global and local structure of this quantum-braided Poincar\'e group is investigated. A kind of ``quantum metrics'' is introduced in the $q$-Min... | 11.754385 | 8.471425 | 10.322358 | 8.839438 | 9.386545 | 9.767878 | 9.712979 | 9.479212 | 9.198825 | 10.961613 | 8.856764 | 8.918774 | 9.300305 | 8.80519 | 8.641895 | 9.040858 | 8.845592 | 9.010549 | 8.835405 | 9.407963 | 8.942051 |
hep-th/0404183 | M. Movshev | M. Movshev, A. Schwarz | Algebraic structure of Yang-Mills theory | 68 pages, submitted to the next volume of I. M. Gelfand Seminar | null | null | null | hep-th math.QA | null | In the present paper we analyze algebraic structures arising in Yang-Mills
theory. The paper should be considered as a part of a project started with a
paper "On maximally supersymmetric Yang-Mills theories" devoted to maximally
supersymmetric Yang-Mills theories. In this paper we collected those of our
results which... | [
{
"created": "Fri, 23 Apr 2004 12:40:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Movshev",
"M.",
""
],
[
"Schwarz",
"A.",
""
]
] | In the present paper we analyze algebraic structures arising in Yang-Mills theory. The paper should be considered as a part of a project started with a paper "On maximally supersymmetric Yang-Mills theories" devoted to maximally supersymmetric Yang-Mills theories. In this paper we collected those of our results which a... | 6.634873 | 6.649328 | 6.887659 | 6.426736 | 6.789757 | 7.211219 | 6.862003 | 6.626215 | 6.389809 | 7.161608 | 6.449111 | 6.416885 | 6.590401 | 6.262987 | 6.382056 | 6.371896 | 6.541193 | 6.315671 | 6.399857 | 6.560468 | 6.646522 |
hep-th/0012013 | Ichiro Oda | Ichiro Oda | Localization of Bulk Fields on AdS_4 Brane in AdS_5 | 9 pages, LaTex 2e, minor corrections (to appear in Phys. Lett. B) | Phys.Lett. B508 (2001) 96-102 | 10.1016/S0370-2693(01)00376-8 | EDO-EP-35 | hep-th | null | We study the localization of various bulk fields on an $AdS_4$ brane in
$AdS_5$. In this case, for a small brane cosmological constant, all the bulk
fields ranging from scalar to graviton are naturally confined to the brane only
through the gravitational interaction. In particular, for the vector field we
can find an... | [
{
"created": "Sun, 3 Dec 2000 15:00:21 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Feb 2001 06:02:05 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Oda",
"Ichiro",
""
]
] | We study the localization of various bulk fields on an $AdS_4$ brane in $AdS_5$. In this case, for a small brane cosmological constant, all the bulk fields ranging from scalar to graviton are naturally confined to the brane only through the gravitational interaction. In particular, for the vector field we can find an i... | 9.440057 | 7.529877 | 8.536125 | 7.609429 | 8.008847 | 7.718179 | 7.892532 | 7.129924 | 7.654658 | 9.523793 | 8.049872 | 7.855737 | 8.506783 | 8.174855 | 8.124845 | 7.991532 | 8.010668 | 8.011983 | 7.954633 | 8.395442 | 7.935433 |
hep-th/9707119 | John Schwarz | John H. Schwarz | Remarks on the M5-Brane | 11 pages, latex, no figures; talk presented at Strings`97 | Nucl.Phys.Proc.Suppl. 68 (1998) 279-284 | 10.1016/S0920-5632(98)00161-3 | CALT-68-2126 | hep-th | null | The fivebrane of M theory -- the M5-brane -- is an especially interesting
object. It plays a central role in a geometric understanding of the
Seiberg-Witten solution of N=2 D=4 gauge theories as well as in certain new 6d
quantum theories. The low energy effective action is an interacting theory of a
(2,0) tensor mult... | [
{
"created": "Fri, 11 Jul 1997 18:11:12 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Schwarz",
"John H.",
""
]
] | The fivebrane of M theory -- the M5-brane -- is an especially interesting object. It plays a central role in a geometric understanding of the Seiberg-Witten solution of N=2 D=4 gauge theories as well as in certain new 6d quantum theories. The low energy effective action is an interacting theory of a (2,0) tensor multip... | 7.551855 | 6.187243 | 8.360139 | 6.590955 | 6.745861 | 6.71941 | 6.037111 | 6.933811 | 6.580219 | 8.880642 | 6.674807 | 6.687189 | 7.370269 | 6.679442 | 6.699931 | 6.730753 | 6.606354 | 6.765387 | 6.832318 | 7.506691 | 6.6683 |
hep-th/9804149 | Sandip Trivedi | Sumit R. Das and Sandip P. Trivedi | Three Brane Action and The Correspondence Between N=4 Yang Mills Theory
and Anti De Sitter Space | 12 pages, LaTex, no figures; error in the form of the final dimension
six operator corrected, some references and comments added, main conclusions
unchanged | Phys.Lett. B445 (1998) 142-149 | 10.1016/S0370-2693(98)01450-6 | TIFR-TH/98-10, fermilab-Pub-98/122-T | hep-th | null | Recently, a relation between N=4 Super Yang Mills in 3+1 dimensions and
supergravity in an $AdS_5$ background has been proposed. In this paper we
explore the idea that the correspondence between operators in the Yang Mills
theory and modes of the supergravity theory can be obtained by using the D3
brane action. Speci... | [
{
"created": "Wed, 22 Apr 1998 19:49:28 GMT",
"version": "v1"
},
{
"created": "Fri, 15 May 1998 19:15:59 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Das",
"Sumit R.",
""
],
[
"Trivedi",
"Sandip P.",
""
]
] | Recently, a relation between N=4 Super Yang Mills in 3+1 dimensions and supergravity in an $AdS_5$ background has been proposed. In this paper we explore the idea that the correspondence between operators in the Yang Mills theory and modes of the supergravity theory can be obtained by using the D3 brane action. Specifi... | 6.770799 | 6.900459 | 7.146484 | 6.246972 | 6.545671 | 6.513691 | 6.581737 | 6.569952 | 6.509102 | 7.137273 | 6.293806 | 6.266285 | 6.719457 | 6.427464 | 6.44205 | 6.335091 | 6.599456 | 6.318237 | 6.364091 | 6.837622 | 6.317894 |
hep-th/9710108 | Sergey Korenblit | A.N.Vall, S.E.Korenblit, V.M.Leviant, D.V.Naumov, A.V.Sinitskaya | Three-particle States in Nonrelativistic Four-fermion Model | 9 pages, LaTex, no figures | null | 10.1080/01422419808240883 | ISU-IAP-Th-97-02 | hep-th | null | On a nonrelativistic contact four-fermion model we have shown that the simple
Lambda-cut-off prescription together with definite fine-tuning of the Lambda
dependency of "bare"quantities lead to self-adjoint semi-bounded Hamiltonian in
one-, two- and three-particle sectors. The fixed self-adjoint extension and
exact s... | [
{
"created": "Tue, 14 Oct 1997 05:00:55 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Vall",
"A. N.",
""
],
[
"Korenblit",
"S. E.",
""
],
[
"Leviant",
"V. M.",
""
],
[
"Naumov",
"D. V.",
""
],
[
"Sinitskaya",
"A. V.",
""
]
] | On a nonrelativistic contact four-fermion model we have shown that the simple Lambda-cut-off prescription together with definite fine-tuning of the Lambda dependency of "bare"quantities lead to self-adjoint semi-bounded Hamiltonian in one-, two- and three-particle sectors. The fixed self-adjoint extension and exact sol... | 19.439569 | 20.341703 | 17.134729 | 18.082241 | 18.705845 | 16.811104 | 17.279432 | 18.897131 | 17.655874 | 20.852516 | 18.796976 | 17.702618 | 18.008423 | 17.479927 | 17.415138 | 17.280914 | 17.034405 | 17.409916 | 17.074286 | 18.896055 | 17.429996 |
1105.3796 | Raphael Bousso | Raphael Bousso and Leonard Susskind | The Multiverse Interpretation of Quantum Mechanics | 46 pages, 13 figures. v2, v3: references added | null | 10.1103/PhysRevD.85.045007 | null | hep-th astro-ph.CO gr-qc hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that the many-worlds of quantum mechanics and the many worlds of the
multiverse are the same thing, and that the multiverse is necessary to give
exact operational meaning to probabilistic predictions from quantum mechanics.
Decoherence - the modern version of wave-function collapse - is subjective in
that ... | [
{
"created": "Thu, 19 May 2011 06:16:28 GMT",
"version": "v1"
},
{
"created": "Sun, 19 Jun 2011 20:34:31 GMT",
"version": "v2"
},
{
"created": "Fri, 22 Jul 2011 20:11:15 GMT",
"version": "v3"
}
] | 2015-03-19 | [
[
"Bousso",
"Raphael",
""
],
[
"Susskind",
"Leonard",
""
]
] | We argue that the many-worlds of quantum mechanics and the many worlds of the multiverse are the same thing, and that the multiverse is necessary to give exact operational meaning to probabilistic predictions from quantum mechanics. Decoherence - the modern version of wave-function collapse - is subjective in that it d... | 8.251968 | 10.10222 | 9.235296 | 8.829136 | 10.539818 | 9.810196 | 9.996663 | 9.5587 | 9.053334 | 10.443031 | 8.574662 | 8.472175 | 8.919265 | 8.490875 | 8.807365 | 8.557178 | 8.634112 | 8.551316 | 8.462024 | 9.251839 | 8.463513 |
hep-th/9306018 | Philippe Di Francesco | P. Di Francesco, F. Lesage and J.-B. Zuber | Graph Rings and Integrable Perturbations of $N=2$ Superconformal
Theories | 44 pages, uuencoded, compressed tar file using harvmac and epsf, four
figures included, Saclay preprint SPhT 93/057 | Nucl.Phys. B408 (1993) 600-634 | 10.1016/0550-3213(93)90382-Y | null | hep-th | null | We show that the connection between certain integrable perturbations of $N=2$
superconformal theories and graphs found by Lerche and Warner extends to a
broader class. These perturbations are such that the generators of the
perturbed chiral ring may be diagonalized in an orthonormal basis. This allows
to define a dua... | [
{
"created": "Thu, 3 Jun 1993 14:14:33 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Di Francesco",
"P.",
""
],
[
"Lesage",
"F.",
""
],
[
"Zuber",
"J. -B.",
""
]
] | We show that the connection between certain integrable perturbations of $N=2$ superconformal theories and graphs found by Lerche and Warner extends to a broader class. These perturbations are such that the generators of the perturbed chiral ring may be diagonalized in an orthonormal basis. This allows to define a dual ... | 12.259629 | 11.267151 | 14.483083 | 11.29473 | 11.902756 | 11.975312 | 12.025415 | 12.076798 | 10.744723 | 15.661193 | 11.366262 | 11.550853 | 12.239045 | 11.192316 | 11.243625 | 11.597385 | 11.559817 | 11.078484 | 11.627971 | 12.218447 | 10.968564 |
hep-th/0610297 | Emilian Dudas | Emilian Dudas, Chloe Papineau and Stefan Pokorski | Moduli stabilization and uplifting with dynamically generated F-terms | 18 pages, no figures Comments and one reference added | JHEP 0702:028,2007 | 10.1088/1126-6708/2007/02/028 | CERN-PH-TH-2006-223 | hep-th | null | We use the F-term dynamical supersymmetry breaking models with metastable
vacua in order to uplift the vacuum energy in the KKLT moduli stabilization
scenario. The main advantage compared to earlier proposals is the manifest
supersymmetric treatment and the natural coexistence of a TeV gravitino mass
with a zero cosm... | [
{
"created": "Fri, 27 Oct 2006 17:01:02 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Nov 2006 11:44:58 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Dudas",
"Emilian",
""
],
[
"Papineau",
"Chloe",
""
],
[
"Pokorski",
"Stefan",
""
]
] | We use the F-term dynamical supersymmetry breaking models with metastable vacua in order to uplift the vacuum energy in the KKLT moduli stabilization scenario. The main advantage compared to earlier proposals is the manifest supersymmetric treatment and the natural coexistence of a TeV gravitino mass with a zero cosmol... | 9.215 | 9.523432 | 10.041323 | 8.983127 | 9.335214 | 9.285357 | 9.309547 | 8.807107 | 8.172195 | 9.202058 | 8.779696 | 8.65872 | 9.169179 | 8.664232 | 8.358986 | 8.896935 | 8.560457 | 8.412762 | 8.664273 | 9.04188 | 8.611403 |
1908.04394 | Peter Koroteev | Peter Koroteev | On Quiver W-algebras and Defects from Gauge Origami | 12 pages, 2 figures, typos corrected | Phys. Lett. B. Vol 800 10 January 2020 135101 | 10.1016/j.physletb.2019.135101 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note, using Nekrasov's gauge origami framework, we study two
different versions of the the BPS/CFT correspondence - first, the standard AGT
duality and, second, the quiver W algebra construction which has been developed
recently by Kimura and Pestun. The gauge origami enables us to work with both
dualities si... | [
{
"created": "Mon, 12 Aug 2019 21:05:38 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Oct 2019 22:20:36 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Nov 2019 21:05:12 GMT",
"version": "v3"
}
] | 2019-11-27 | [
[
"Koroteev",
"Peter",
""
]
] | In this note, using Nekrasov's gauge origami framework, we study two different versions of the the BPS/CFT correspondence - first, the standard AGT duality and, second, the quiver W algebra construction which has been developed recently by Kimura and Pestun. The gauge origami enables us to work with both dualities simu... | 12.770816 | 13.294452 | 15.421916 | 12.481546 | 12.12335 | 12.446071 | 12.279389 | 11.730081 | 12.116614 | 16.672947 | 12.684472 | 11.8434 | 12.773401 | 12.094968 | 11.648169 | 11.80414 | 11.911843 | 11.766778 | 12.021669 | 12.609867 | 12.025791 |
1210.6308 | Yosuke Imamura | Yosuke Imamura | Perturbative partition function for a squashed S^5 | 24 pages, 1 figure; v2: references added, errors corrected,
explanations added; v3: explanations improved, errors corrected, an overall
factor added to the final result | null | 10.1093/ptep/ptt044 | TIT/HEP-622 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the index of 6d N=(1,0) theories on S^5 x R containing vector and
hypermultiplets. We only consider the perturbative sector without instantons.
By compactifying R to S^1 with a twisted boundary condition and taking the
small radius limit, we derive the perturbative partition function on a squashed
S^5. The... | [
{
"created": "Tue, 23 Oct 2012 17:47:33 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Nov 2012 10:26:10 GMT",
"version": "v2"
},
{
"created": "Thu, 25 Apr 2013 06:58:08 GMT",
"version": "v3"
}
] | 2016-06-21 | [
[
"Imamura",
"Yosuke",
""
]
] | We compute the index of 6d N=(1,0) theories on S^5 x R containing vector and hypermultiplets. We only consider the perturbative sector without instantons. By compactifying R to S^1 with a twisted boundary condition and taking the small radius limit, we derive the perturbative partition function on a squashed S^5. The 1... | 9.861342 | 7.811561 | 10.376138 | 8.339927 | 8.253998 | 8.723012 | 8.480295 | 8.399338 | 8.418026 | 10.616009 | 8.210575 | 8.19773 | 8.438447 | 8.333385 | 8.510005 | 8.440736 | 8.147163 | 8.464433 | 8.250174 | 8.949143 | 8.222094 |
1010.1159 | Hagen Triendl | Hagen Triendl | Generalized Geometry and Partial Supersymmetry Breaking | 117 pages, Ph.D. thesis (Advisor: Jan Louis); v2: references added | Fortsch.Phys. 59 (2010) 76-164 | 10.1002/prop.201000090 | DESY-THESIS-2010-028 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This review article consists of two parts. In the first part we use the
formalism of (exceptional) generalized geometry to derive the scalar field
space of SU(2)xSU(2)-structure compactifications. We show that in contrast to
SU(3)xSU(3) structures, there is no dynamical SU(2)xSU(2) structure
interpolating between an ... | [
{
"created": "Wed, 6 Oct 2010 14:02:45 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Oct 2010 06:56:06 GMT",
"version": "v2"
}
] | 2011-01-05 | [
[
"Triendl",
"Hagen",
""
]
] | This review article consists of two parts. In the first part we use the formalism of (exceptional) generalized geometry to derive the scalar field space of SU(2)xSU(2)-structure compactifications. We show that in contrast to SU(3)xSU(3) structures, there is no dynamical SU(2)xSU(2) structure interpolating between an SU... | 5.434275 | 6.242021 | 6.84823 | 5.886896 | 6.180647 | 6.105666 | 6.034144 | 5.724638 | 5.963616 | 8.073952 | 6.087053 | 6.002638 | 6.033174 | 5.810868 | 5.907115 | 5.84487 | 5.986066 | 5.726563 | 5.711174 | 6.034962 | 5.83863 |
1507.02172 | Andrew Royston | Katrin Becker, Melanie Becker, Ilarion V. Melnikov, Daniel Robbins and
Andrew B. Royston | Some tree-level string amplitudes in the NSR formalism | 40+8 pages; v2: references added; v3: additional field theory checks
made; published version; v4: minor corrections; results unchanged | JHEP 12 (2015) 010 | 10.1007/JHEP12(2015)010 | MI-TH-1515 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate tree level scattering amplitudes for open strings using the NSR
formalism. We present a streamlined symmetry-based and pedagogical approach to
the computations, which we first develop by checking two-, three-, and
four-point functions involving bosons and fermions. We calculate the five-point
amplitude f... | [
{
"created": "Wed, 8 Jul 2015 14:30:11 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Aug 2015 18:03:32 GMT",
"version": "v2"
},
{
"created": "Fri, 8 Jan 2016 17:02:45 GMT",
"version": "v3"
},
{
"created": "Wed, 17 Aug 2016 16:57:39 GMT",
"version": "v4"
}
] | 2016-08-22 | [
[
"Becker",
"Katrin",
""
],
[
"Becker",
"Melanie",
""
],
[
"Melnikov",
"Ilarion V.",
""
],
[
"Robbins",
"Daniel",
""
],
[
"Royston",
"Andrew B.",
""
]
] | We calculate tree level scattering amplitudes for open strings using the NSR formalism. We present a streamlined symmetry-based and pedagogical approach to the computations, which we first develop by checking two-, three-, and four-point functions involving bosons and fermions. We calculate the five-point amplitude for... | 8.719559 | 9.428529 | 9.765351 | 8.639832 | 8.825761 | 9.095329 | 8.644954 | 9.403271 | 9.674397 | 10.454247 | 9.482396 | 8.88233 | 9.180766 | 8.806731 | 8.708059 | 8.878618 | 8.636732 | 8.621325 | 8.661273 | 9.263758 | 8.477387 |
1601.00921 | Andrew Strominger | Stephen W. Hawking, Malcolm J. Perry and Andrew Strominger | Soft Hair on Black Holes | 22 pages 2 figures | Phys. Rev. Lett. 116, 231301 (2016) | 10.1103/PhysRevLett.116.231301 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has recently been shown that BMS supertranslation symmetries imply an
infinite number of conservation laws for all gravitational theories in
asymptotically Minkowskian spacetimes. These laws require black holes to carry
a large amount of soft ($i.e.$ zero-energy) supertranslation hair. The presence
of a Maxwell fi... | [
{
"created": "Tue, 5 Jan 2016 17:48:33 GMT",
"version": "v1"
}
] | 2016-06-15 | [
[
"Hawking",
"Stephen W.",
""
],
[
"Perry",
"Malcolm J.",
""
],
[
"Strominger",
"Andrew",
""
]
] | It has recently been shown that BMS supertranslation symmetries imply an infinite number of conservation laws for all gravitational theories in asymptotically Minkowskian spacetimes. These laws require black holes to carry a large amount of soft ($i.e.$ zero-energy) supertranslation hair. The presence of a Maxwell fiel... | 6.828457 | 7.66216 | 8.662475 | 7.666265 | 8.089183 | 8.139366 | 8.603491 | 7.938005 | 7.693118 | 7.984006 | 7.746847 | 6.83156 | 7.210289 | 7.310595 | 7.147577 | 7.036706 | 7.008098 | 7.164267 | 6.898094 | 7.090927 | 6.967437 |
1803.03564 | Andr\'e Neveu | Andr\'e Neveu | A B\"acklund transformation for elliptic four-point conformal blocks | 9 pages, to be published in the Memorial Volume for Ludwig Faddeev | null | 10.1142/S0129055X18400123 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply an integral transformation to solutions of a partial differential
equation for five-point correlation functions in Liouville theory on a sphere
with one degenerate field $V_{-\frac{1}{2b}}$. By repeating this
transformation, we can reach a whole lattice of values for the conformal
dimensions of the four othe... | [
{
"created": "Fri, 9 Mar 2018 15:33:07 GMT",
"version": "v1"
}
] | 2018-08-15 | [
[
"Neveu",
"André",
""
]
] | We apply an integral transformation to solutions of a partial differential equation for five-point correlation functions in Liouville theory on a sphere with one degenerate field $V_{-\frac{1}{2b}}$. By repeating this transformation, we can reach a whole lattice of values for the conformal dimensions of the four other ... | 13.501974 | 10.651802 | 15.037993 | 10.478566 | 10.62324 | 10.247974 | 10.858478 | 10.450025 | 10.02043 | 16.062819 | 10.354638 | 10.234928 | 13.060131 | 9.932674 | 9.704468 | 9.882934 | 9.79283 | 10.733101 | 10.040638 | 12.672273 | 10.055052 |
hep-th/9603188 | null | Chan Hong-Mo, Jacqueline Faridani, Jakov Pfaudler, Tsou Sheung Tsun | Rudiments of Dual Feynman Rules for Yang-Mills Monopoles in Loop Space | 21 pages, LateX, no figures | Phys.Rev. D55 (1997) 5015-5026 | 10.1103/PhysRevD.55.5015 | RAL-TR-96-025 | hep-th | null | Dual Feynman rules for Dirac monopoles in Yang-Mills fields are obtained by
the Wu-Yang (1976) criterion in which dynamics result as a consequence of the
constraint defining the monopole as a topological obstruction in the field. The
usual path-integral approach is adopted, but using loop space variables of the
type ... | [
{
"created": "Thu, 28 Mar 1996 15:29:32 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Hong-Mo",
"Chan",
""
],
[
"Faridani",
"Jacqueline",
""
],
[
"Pfaudler",
"Jakov",
""
],
[
"Tsun",
"Tsou Sheung",
""
]
] | Dual Feynman rules for Dirac monopoles in Yang-Mills fields are obtained by the Wu-Yang (1976) criterion in which dynamics result as a consequence of the constraint defining the monopole as a topological obstruction in the field. The usual path-integral approach is adopted, but using loop space variables of the type in... | 11.100838 | 12.187744 | 11.536569 | 10.735857 | 11.352472 | 11.530003 | 11.011079 | 11.495039 | 10.910805 | 11.821774 | 10.727875 | 10.653972 | 10.859378 | 10.450817 | 10.960217 | 11.034723 | 11.114158 | 11.012886 | 10.732815 | 10.819936 | 10.583037 |
2101.06868 | Peter M. Lavrov | P.M. Lavrov | Covariant quantization of Yang-Mills theory in the first order formalism | 9 pages,v2: minor improvements of the text,v3:published version | Physics Letters B 816 (2021) 136182 | 10.1016/j.physletb.2021.136182 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper the Yang-Mills theory in the first order formalism is
studied. On classical level the first order formulation is equivalent to the
standard second order description of the Yang-Mills theory. It is proven that
both formulations remain equivalent on quantum level as well.
| [
{
"created": "Mon, 18 Jan 2021 04:12:42 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Jan 2021 06:43:05 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Mar 2021 01:28:51 GMT",
"version": "v3"
}
] | 2021-03-10 | [
[
"Lavrov",
"P. M.",
""
]
] | In the present paper the Yang-Mills theory in the first order formalism is studied. On classical level the first order formulation is equivalent to the standard second order description of the Yang-Mills theory. It is proven that both formulations remain equivalent on quantum level as well. | 6.493434 | 4.818657 | 5.671576 | 5.259451 | 5.001972 | 4.355576 | 4.920011 | 4.989594 | 5.417857 | 5.550154 | 4.92064 | 5.320583 | 5.875574 | 5.595737 | 5.156845 | 5.56141 | 5.309309 | 5.573336 | 5.62918 | 5.997589 | 5.276754 |
2210.09993 | Andrei Mironov | A. Mironov and A. Morozov | Spectral curves and $W$-representations of matrix models | 25 pages | J. High Energ. Phys. 2023 (2023) 116 | 10.1007/JHEP03(2023)116 | MIPT/TH-18/22; FIAN/TD-13/22; ITEP/TH-21/22; IITP/TH-20/22 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explain how the spectral curve can be extracted from the ${\cal
W}$-representation of a matrix model. It emerges from the part of the ${\cal
W}$-operator, which is linear in time-variables. A possibility of extracting
the spectral curve in this way is important because there are models where
matrix integrals are n... | [
{
"created": "Tue, 18 Oct 2022 16:57:03 GMT",
"version": "v1"
},
{
"created": "Sun, 23 Oct 2022 21:38:44 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Mar 2023 11:36:30 GMT",
"version": "v3"
}
] | 2023-03-21 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | We explain how the spectral curve can be extracted from the ${\cal W}$-representation of a matrix model. It emerges from the part of the ${\cal W}$-operator, which is linear in time-variables. A possibility of extracting the spectral curve in this way is important because there are models where matrix integrals are not... | 14.702027 | 12.513261 | 15.746626 | 12.916066 | 11.937385 | 12.87965 | 13.177032 | 11.877143 | 12.289058 | 15.876645 | 12.557787 | 13.693744 | 14.74367 | 13.950755 | 13.71594 | 14.014502 | 13.787674 | 13.693069 | 13.924354 | 14.44506 | 13.512044 |
hep-th/0301162 | Yang-Hui Evariste He | Yang-Hui He | Closed String Tachyons, Non-Supersymmetric Orbifolds and Generalised
McKay Correspondence | 21+1 pages, 4 figures, reference added and typos corrected | Adv.Theor.Math.Phys. 7 (2003) 121-144 | null | UPR-1027-T | hep-th | null | We study closed string tachyon condensation on general non-supersymmetric
orbifolds of C^2. Extending previous analyses on Abelian cases, we present the
classification of quotients by discrete finite subgroups of GL(2; C) as well as
the generalised Hirzebruch-Jung continued fractions associated with the
resolution da... | [
{
"created": "Wed, 22 Jan 2003 01:38:39 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2003 14:40:10 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Jan 2004 16:41:00 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"He",
"Yang-Hui",
""
]
] | We study closed string tachyon condensation on general non-supersymmetric orbifolds of C^2. Extending previous analyses on Abelian cases, we present the classification of quotients by discrete finite subgroups of GL(2; C) as well as the generalised Hirzebruch-Jung continued fractions associated with the resolution data... | 11.825377 | 12.922124 | 16.146341 | 11.731457 | 13.528564 | 13.557587 | 12.838936 | 11.4243 | 12.756678 | 17.31797 | 12.536296 | 11.859849 | 13.463304 | 11.634795 | 11.703012 | 12.230237 | 11.92392 | 11.341926 | 11.644517 | 13.053907 | 11.483389 |
hep-th/0305091 | Junji Suzuki | J. Suzuki (Shizuoka University) | The dilute A_L models and the integrable perturbations of unitary
minimal CFTs | 14 pages, 2 figures | J.Phys.A37:511-520,2004 | 10.1088/0305-4470/37/2/018 | null | hep-th | null | Recently, a set of thermodynamic Bethe ansatz equations is proposed by Dorey,
Pocklington and Tateo for unitary minimal models perturbed by \phi_{1,2} or
\phi_{2,1} operator. We examine their results in view of the lattice analogues,
dilute A_L models at regime 1 and 2. Taking M_{5,6}+\phi_{1,2} and
M_{3,4}+\phi_{2,1... | [
{
"created": "Mon, 12 May 2003 06:18:02 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Jun 2003 01:40:10 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Jul 2003 03:07:25 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Suzuki",
"J.",
"",
"Shizuoka University"
]
] | Recently, a set of thermodynamic Bethe ansatz equations is proposed by Dorey, Pocklington and Tateo for unitary minimal models perturbed by \phi_{1,2} or \phi_{2,1} operator. We examine their results in view of the lattice analogues, dilute A_L models at regime 1 and 2. Taking M_{5,6}+\phi_{1,2} and M_{3,4}+\phi_{2,1} ... | 7.60094 | 6.182723 | 9.88699 | 6.61523 | 6.730917 | 6.531207 | 6.77971 | 6.595524 | 6.419924 | 11.153197 | 6.46239 | 6.82902 | 8.373267 | 7.377503 | 7.017175 | 7.372062 | 7.070018 | 7.487514 | 7.085577 | 8.448916 | 7.050045 |
hep-th/0211238 | Itzhak Bars | Itzhak Bars | MSFT : Moyal Star Formulation of String Field Theory | 22 pages, LaTeX. v3 minor corrections | null | null | null | hep-th | null | The Moyal star formulation of string field theory is reviewed. The various
versions of the star product are compared and related to one another in a
regulated theory that resolves associativity anomalies. A summary of
computations and challenges is given.
| [
{
"created": "Mon, 25 Nov 2002 12:01:06 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Jan 2003 03:33:15 GMT",
"version": "v2"
},
{
"created": "Sat, 22 May 2004 18:45:14 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Bars",
"Itzhak",
""
]
] | The Moyal star formulation of string field theory is reviewed. The various versions of the star product are compared and related to one another in a regulated theory that resolves associativity anomalies. A summary of computations and challenges is given. | 26.228991 | 17.953142 | 24.096123 | 17.023594 | 17.535006 | 17.02553 | 17.257988 | 17.213144 | 17.287611 | 26.468075 | 16.977634 | 19.442509 | 23.370258 | 19.618351 | 19.314028 | 19.317934 | 19.588488 | 18.953836 | 19.736399 | 21.550743 | 19.112474 |
hep-th/0207284 | Juan Maldacena | Juan Maldacena and Liat Maoz | Strings on pp-waves and massive two dimensional field theories | harvmac, 26 pages, v2,3: references added, typos corrected | JHEP 0212 (2002) 046 | 10.1088/1126-6708/2002/12/046 | null | hep-th | null | We find a general class of pp-wave solutions of type IIB string theory such
that the light cone gauge worldsheet lagrangian is that of an interacting
massive field theory. When the light cone Lagrangian has (2,2) supersymmetry we
can find backgrounds that lead to arbitrary superpotentials on the worldsheet.
We consid... | [
{
"created": "Wed, 31 Jul 2002 16:03:35 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Aug 2002 17:13:00 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Nov 2002 19:22:28 GMT",
"version": "v3"
},
{
"created": "Fri, 28 Mar 2003 23:56:00 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Maldacena",
"Juan",
""
],
[
"Maoz",
"Liat",
""
]
] | We find a general class of pp-wave solutions of type IIB string theory such that the light cone gauge worldsheet lagrangian is that of an interacting massive field theory. When the light cone Lagrangian has (2,2) supersymmetry we can find backgrounds that lead to arbitrary superpotentials on the worldsheet. We consider... | 12.217273 | 11.05373 | 15.119738 | 10.495836 | 10.446176 | 12.183565 | 11.175788 | 11.479061 | 10.150829 | 14.15183 | 10.352332 | 10.945077 | 12.105677 | 10.930401 | 10.678684 | 11.022397 | 10.7513 | 11.201221 | 10.572865 | 11.903388 | 10.592973 |
1607.01139 | Shinji Hirano | Nana Cabo Bizet, Shinji Hirano | Revisiting constraints on uplifts to de Sitter vacua | 15 pages | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the issue of uplifting the potential to de Sitter (dS) vacua in
type IIB flux compactifications of Kachru, Kallosh, Linde and Trivedi (KKLT).
We shed light on some tension between two constraints on dS vacua in type IIB
string theory. One is the well-known and much-discussed constraint which leads
to the n... | [
{
"created": "Tue, 5 Jul 2016 07:51:52 GMT",
"version": "v1"
}
] | 2016-07-06 | [
[
"Bizet",
"Nana Cabo",
""
],
[
"Hirano",
"Shinji",
""
]
] | We revisit the issue of uplifting the potential to de Sitter (dS) vacua in type IIB flux compactifications of Kachru, Kallosh, Linde and Trivedi (KKLT). We shed light on some tension between two constraints on dS vacua in type IIB string theory. One is the well-known and much-discussed constraint which leads to the no-... | 9.444032 | 9.760191 | 10.297052 | 8.658468 | 9.0719 | 10.096823 | 9.638405 | 9.036488 | 9.034696 | 9.709719 | 9.193215 | 9.221402 | 9.17358 | 8.933248 | 8.9872 | 9.23283 | 8.902108 | 9.077584 | 8.965389 | 8.833076 | 9.027809 |
hep-th/0307222 | Hong Lu | J. Kerimo and H. Lu | New D=6, N=(1,1) Gauged Supergravity with Supersymmetric (Minkowski)_4 X
S^2 Vacuum | latex, 13 pages, typo corrected | Phys.Lett. B576 (2003) 219-226 | 10.1016/j.physletb.2003.09.076 | null | hep-th | null | We obtain a new gauged D=6, N=(1,1) pure supergravity by a generalised
consistent Kaluza-Klein reduction of M-theory on K3 \times R. The reduction
requires a conspiratory gauging of both the Cremmer-Julia type global (rigid)
symmetry and the homogeneous rescaling symmetry of the supergravity equations
of motion. The ... | [
{
"created": "Wed, 23 Jul 2003 18:38:47 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Aug 2003 19:18:50 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Kerimo",
"J.",
""
],
[
"Lu",
"H.",
""
]
] | We obtain a new gauged D=6, N=(1,1) pure supergravity by a generalised consistent Kaluza-Klein reduction of M-theory on K3 \times R. The reduction requires a conspiratory gauging of both the Cremmer-Julia type global (rigid) symmetry and the homogeneous rescaling symmetry of the supergravity equations of motion. The ga... | 7.913834 | 7.65081 | 9.156078 | 6.903548 | 7.334134 | 7.67151 | 7.712583 | 7.233913 | 7.330082 | 10.74512 | 6.827915 | 7.389607 | 8.287497 | 7.355418 | 7.583241 | 7.46711 | 7.240599 | 7.227365 | 7.345618 | 8.38076 | 7.317266 |
2010.03178 | Peter M. Lavrov | Peter M. Lavrov | Basic properties of an alternative flow equation in gravity theories | 13 pages, v2: published version | Eur. Phys. J. Plus (2021) 136:854 | 10.1140/epjp/s13360-021-01731-2 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Basic properties of alternative flow equation in Quantum Gravity are studied.
It is shown that the alternative flow equation for effective two-particle
irreducible effective action is gauge independent and does not depend on IR
parameter $k$ on shell.
| [
{
"created": "Wed, 7 Oct 2020 05:22:04 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Aug 2021 03:49:26 GMT",
"version": "v2"
}
] | 2021-08-23 | [
[
"Lavrov",
"Peter M.",
""
]
] | Basic properties of alternative flow equation in Quantum Gravity are studied. It is shown that the alternative flow equation for effective two-particle irreducible effective action is gauge independent and does not depend on IR parameter $k$ on shell. | 20.19758 | 14.508522 | 17.603182 | 14.352238 | 16.579594 | 15.052729 | 13.817298 | 15.025725 | 14.419349 | 14.294123 | 14.740513 | 15.273166 | 15.106856 | 15.333005 | 15.508538 | 15.477743 | 15.390473 | 15.579355 | 14.630555 | 16.652725 | 14.961359 |
hep-th/0108033 | null | S. Q. Wu and X. Cai | No New Quantum Thermal Effect of Dirac Particles in a Charged Vaidya -
de Sitter Black Hole | 12pt revtex, 10 pages, no figure, accepted for IL Nuovo Cimento B | Nuovo Cim.B116:907-914,2001 | null | null | hep-th | null | It is shown that Hawking radiation of Dirac particles does not exist for
$P_1, Q_2$ components but for $P_2, Q_1$ components in a charged Vaidya - de
Sitter black hole. Both the location and the temperature of the event horizon
change with time. The thermal radiation spectrum of Dirac particles is the same
as that of... | [
{
"created": "Tue, 7 Aug 2001 01:47:59 GMT",
"version": "v1"
}
] | 2010-11-11 | [
[
"Wu",
"S. Q.",
""
],
[
"Cai",
"X.",
""
]
] | It is shown that Hawking radiation of Dirac particles does not exist for $P_1, Q_2$ components but for $P_2, Q_1$ components in a charged Vaidya - de Sitter black hole. Both the location and the temperature of the event horizon change with time. The thermal radiation spectrum of Dirac particles is the same as that of K... | 7.498851 | 7.843477 | 6.102883 | 6.343098 | 7.171504 | 6.689678 | 7.258833 | 5.702611 | 6.713105 | 5.800257 | 7.062011 | 6.449107 | 6.203673 | 6.29886 | 6.763143 | 6.607188 | 6.631844 | 6.186958 | 6.53806 | 6.272724 | 6.788745 |
2101.04705 | Sergio H\"ortner | Hap\'e Fuhri Snethlage and Sergio H\"ortner | Manifest electric-magnetic duality in linearized conformal gravity | null | Phys. Rev. D 103, 105014 (2021) | 10.1103/PhysRevD.103.105014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a manifestly duality-symmetric formulation of the action principle
for conformal gravity linearized around Minkowski space-time. The analysis is
performed in the Hamiltonian formulation, the fourth-order character of the
equations of motion requiring the formal treatment of the three-dimensional
metric pert... | [
{
"created": "Tue, 12 Jan 2021 19:22:09 GMT",
"version": "v1"
}
] | 2021-05-26 | [
[
"Snethlage",
"Hapé Fuhri",
""
],
[
"Hörtner",
"Sergio",
""
]
] | We derive a manifestly duality-symmetric formulation of the action principle for conformal gravity linearized around Minkowski space-time. The analysis is performed in the Hamiltonian formulation, the fourth-order character of the equations of motion requiring the formal treatment of the three-dimensional metric pertur... | 8.300829 | 9.274515 | 9.708427 | 8.03209 | 8.515087 | 8.340403 | 10.046336 | 8.732228 | 8.414368 | 9.451479 | 8.263738 | 8.097376 | 8.171734 | 7.888034 | 8.236652 | 8.314054 | 8.100685 | 8.173365 | 8.130121 | 7.957412 | 8.089233 |
0904.0839 | Takayuki Hori | Takayuki Hori | Relativistic Particle in Complex Space Time | 15 pages | Prog.Theor.Phys.122:323-337,2009 | 10.1143/PTP.122.323 | TEP-09-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A modified version of the bilocal particle is presented in terms of complex
space time. Unusual constraint structure of the model is studied, and a new
concept of the physical equivalence is proposed in accordance with Dirac's
conjecture. It is found that in the quantum theory the physical state
conditions are compat... | [
{
"created": "Mon, 6 Apr 2009 04:13:55 GMT",
"version": "v1"
},
{
"created": "Wed, 27 May 2009 04:04:25 GMT",
"version": "v2"
}
] | 2009-11-19 | [
[
"Hori",
"Takayuki",
""
]
] | A modified version of the bilocal particle is presented in terms of complex space time. Unusual constraint structure of the model is studied, and a new concept of the physical equivalence is proposed in accordance with Dirac's conjecture. It is found that in the quantum theory the physical state conditions are compatib... | 18.764639 | 15.897304 | 17.481815 | 15.559377 | 17.883976 | 16.100597 | 15.653451 | 16.240297 | 15.799764 | 18.920137 | 16.416389 | 15.453702 | 16.019619 | 16.250185 | 16.081507 | 15.883306 | 15.617239 | 15.699434 | 16.213505 | 15.368418 | 14.967794 |
hep-th/0401022 | Gorbunov Ivan Vladislavovich | I.V. Gorbunov, S.L. Lyakhovich and A.A. Sharapov | Wick Quantization of Cotangent Bundles over Riemannian Manifolds | 18 pages, LaTex2e, replaced by journal version, misprints removed | J.Geom.Phys. 53 (2005) 98-121 | 10.1016/j.geomphys.2004.06.003 | null | hep-th math.QA math.SG | null | A simple geometric procedure is proposed for constructing Wick symbols on
cotangent bundles to Riemannian manifolds. The main ingredient of the
construction is a method of endowing the cotangent bundle with a formal
K\"ahler structure. The formality means that the metric is lifted from the
Riemannian manifold $Q$ to ... | [
{
"created": "Mon, 5 Jan 2004 19:53:48 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Jan 2004 14:54:45 GMT",
"version": "v2"
},
{
"created": "Sun, 11 Jul 2004 19:58:44 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Gorbunov",
"I. V.",
""
],
[
"Lyakhovich",
"S. L.",
""
],
[
"Sharapov",
"A. A.",
""
]
] | A simple geometric procedure is proposed for constructing Wick symbols on cotangent bundles to Riemannian manifolds. The main ingredient of the construction is a method of endowing the cotangent bundle with a formal K\"ahler structure. The formality means that the metric is lifted from the Riemannian manifold $Q$ to it... | 7.296044 | 7.211403 | 7.450126 | 6.476149 | 7.242859 | 7.458917 | 7.217024 | 7.499457 | 6.871188 | 7.937394 | 6.646873 | 6.724536 | 6.857801 | 6.674551 | 6.840369 | 6.883242 | 6.939035 | 6.758636 | 6.687175 | 6.977499 | 6.661316 |
hep-th/9506057 | Ramzi Khuri | M.J. Duff, Sergio Ferrara, Ramzi R. Khuri and Joachim Rahmfeld | Supersymmetry and Dual String Solitons | 13 pages, harvmac, (missing references added) | Phys.Lett.B356:479-486,1995 | 10.1016/0370-2693(95)00838-C | CTP-TAMU-50/94, CERN-TH/95-122, UCLA 95/TEP-15, McGill/95-23,
NI-94-035 | hep-th | null | We present new classes of string-like soliton solutions in ($N=1$; $D=10$),
($N=2$; $D=6$) and ($N=4$; $D=4$) heterotic string theory. Connections are made
between the solution-generating subgroup of the $T$-duality group of the
compactification and the number of spacetime supersymmetries broken. Analogous
solutions ... | [
{
"created": "Fri, 9 Jun 1995 00:36:15 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jun 1995 14:00:17 GMT",
"version": "v2"
}
] | 2009-07-09 | [
[
"Duff",
"M. J.",
""
],
[
"Ferrara",
"Sergio",
""
],
[
"Khuri",
"Ramzi R.",
""
],
[
"Rahmfeld",
"Joachim",
""
]
] | We present new classes of string-like soliton solutions in ($N=1$; $D=10$), ($N=2$; $D=6$) and ($N=4$; $D=4$) heterotic string theory. Connections are made between the solution-generating subgroup of the $T$-duality group of the compactification and the number of spacetime supersymmetries broken. Analogous solutions ar... | 6.179137 | 5.940465 | 6.456106 | 5.729488 | 6.180881 | 5.814516 | 6.607364 | 5.589311 | 6.224222 | 6.757399 | 6.053799 | 5.847946 | 6.340465 | 5.973778 | 5.792679 | 6.010637 | 5.774509 | 6.200222 | 5.864337 | 6.46611 | 5.764938 |
1510.01387 | Sebasti\'an Alberto Franchino Vi\~nas | Sebasti\'an A. Franchino-Vi\~nas | Worldline Formalism and Noncommutative Theories | Ph.D. thesis, in spanish, 166 pages, 8 figures. Advisor: P.A.G.
Pisani. Co-advisor: H.Falomir. En espa\~nol | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The objective of this Ph.D. thesis is the implementation of the Worldline
Formalism in the frame of Noncommutative Quantum Field Theories. The result is
a master formula for the 1-loop effective action that is applied to a number of
scalar models -- among them the Grosse-Wulkenhaar model. As a byproduct we find
an ex... | [
{
"created": "Mon, 5 Oct 2015 22:28:05 GMT",
"version": "v1"
}
] | 2015-10-07 | [
[
"Franchino-Viñas",
"Sebastián A.",
""
]
] | The objective of this Ph.D. thesis is the implementation of the Worldline Formalism in the frame of Noncommutative Quantum Field Theories. The result is a master formula for the 1-loop effective action that is applied to a number of scalar models -- among them the Grosse-Wulkenhaar model. As a byproduct we find an expr... | 10.415868 | 9.787959 | 12.529614 | 9.886422 | 9.969023 | 9.806759 | 9.54579 | 9.620377 | 9.702635 | 11.931685 | 10.074001 | 9.873188 | 10.373507 | 9.777701 | 9.501758 | 9.607057 | 9.857551 | 9.998677 | 9.8325 | 10.827724 | 10.465076 |
1607.06519 | Andrea Trivella | Andrea Trivella | Holographic Computations of the Quantum Information Metric | 21 pages, 5 figures | null | 10.1088/1361-6382/aa69a6 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we show how the Quantum Information Metric can be computed
holographically using a perturbative approach. In particular when the
deformation of the conformal field theory state is induced by a scalar operator
the corresponding bulk configuration reduces to a scalar field perturbatively
probing the unpert... | [
{
"created": "Thu, 21 Jul 2016 22:22:37 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Nov 2016 01:15:50 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Dec 2016 07:15:26 GMT",
"version": "v3"
},
{
"created": "Fri, 15 Sep 2017 19:16:16 GMT",
"version": "v4"
}
] | 2017-09-19 | [
[
"Trivella",
"Andrea",
""
]
] | In this note we show how the Quantum Information Metric can be computed holographically using a perturbative approach. In particular when the deformation of the conformal field theory state is induced by a scalar operator the corresponding bulk configuration reduces to a scalar field perturbatively probing the unpertur... | 8.012547 | 7.407404 | 8.85248 | 7.219813 | 7.264085 | 6.844859 | 7.300858 | 6.998564 | 7.308411 | 9.934892 | 7.009702 | 7.139469 | 7.719171 | 7.040064 | 7.076905 | 7.053815 | 7.29939 | 7.268415 | 7.229992 | 7.672878 | 7.30633 |
1609.01281 | Tom Rudelius | Jonathan J. Heckman, Patrick Jefferson, Tom Rudelius, Cumrun Vafa | Punctures for Theories of Class $\mathcal{S}_\Gamma$ | 39 pages | null | 10.1007/JHEP03(2017)171 | null | hep-th math.AC math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | With the aim of understanding compactifications of 6D superconformal field
theories to four dimensions, we study punctures for theories of class
$\mathcal{S}_{\Gamma}$. The class $\mathcal{S}_{\Gamma}$ theories arise from
M5-branes probing $\mathbb{C}^2 / \Gamma$, an ADE singularity. The resulting 4D
theories descend... | [
{
"created": "Mon, 5 Sep 2016 20:00:00 GMT",
"version": "v1"
}
] | 2017-04-26 | [
[
"Heckman",
"Jonathan J.",
""
],
[
"Jefferson",
"Patrick",
""
],
[
"Rudelius",
"Tom",
""
],
[
"Vafa",
"Cumrun",
""
]
] | With the aim of understanding compactifications of 6D superconformal field theories to four dimensions, we study punctures for theories of class $\mathcal{S}_{\Gamma}$. The class $\mathcal{S}_{\Gamma}$ theories arise from M5-branes probing $\mathbb{C}^2 / \Gamma$, an ADE singularity. The resulting 4D theories descend f... | 6.047699 | 6.001752 | 6.868223 | 5.618299 | 5.853955 | 5.913119 | 5.870501 | 5.606299 | 5.665863 | 7.979427 | 5.808272 | 5.710487 | 6.387629 | 5.606308 | 5.670062 | 5.694061 | 5.968328 | 5.761918 | 5.73199 | 6.278456 | 5.730552 |
1709.08189 | Ichiro Oda | Ichiro Oda | Gravitational Quantum Effects and Nonlocal Approach to the Cosmological
Constant Problem | 13 pages | null | null | DPUR/TH/57 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have recently presented a manifestly local and general coordinate
invariant formulation of a nonlocal approach to the cosmological constant
problem. In this article, we investigate quantum effects from both matter and
gravitational fields in this formulation. In particular, we pay our attention
to the gravitationa... | [
{
"created": "Sun, 24 Sep 2017 12:09:25 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Nov 2017 08:01:50 GMT",
"version": "v2"
}
] | 2017-11-28 | [
[
"Oda",
"Ichiro",
""
]
] | We have recently presented a manifestly local and general coordinate invariant formulation of a nonlocal approach to the cosmological constant problem. In this article, we investigate quantum effects from both matter and gravitational fields in this formulation. In particular, we pay our attention to the gravitational ... | 7.691378 | 6.498008 | 7.775207 | 6.792099 | 6.739782 | 6.521533 | 6.485364 | 7.048786 | 6.366249 | 7.683608 | 6.567628 | 6.816312 | 7.402055 | 7.017039 | 6.905029 | 6.868022 | 6.736414 | 6.876579 | 7.04187 | 7.375321 | 6.984356 |
1706.09652 | Rong-Xin Miao | Rong-Xin Miao and Chong-Sun Chu | Universality for Shape Dependence of Casimir Effects from Weyl Anomaly | 19 pages, 1 figure and 3 tables, references added, accepted for
publication in JHEP | null | 10.1007/JHEP03(2018)046 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We reveal elegant relations between the shape dependence of the Casimir
effects and Weyl anomaly in boundary conformal field theories (BCFT). We show
that for any BCFT which has a description in terms of an effective action, the
near boundary divergent behavior of the renormalized stress tensor is
completely determin... | [
{
"created": "Thu, 29 Jun 2017 09:42:10 GMT",
"version": "v1"
},
{
"created": "Fri, 7 Jul 2017 11:47:20 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Mar 2018 11:46:07 GMT",
"version": "v3"
}
] | 2018-04-04 | [
[
"Miao",
"Rong-Xin",
""
],
[
"Chu",
"Chong-Sun",
""
]
] | We reveal elegant relations between the shape dependence of the Casimir effects and Weyl anomaly in boundary conformal field theories (BCFT). We show that for any BCFT which has a description in terms of an effective action, the near boundary divergent behavior of the renormalized stress tensor is completely determined... | 8.076818 | 8.101442 | 8.991928 | 7.918788 | 8.797206 | 8.448671 | 8.813643 | 8.292251 | 7.911653 | 9.050358 | 8.200132 | 8.055624 | 8.434068 | 8.076524 | 8.041207 | 8.041006 | 8.00086 | 8.299596 | 8.065354 | 8.516748 | 7.964437 |
2011.07601 | Stefano Baiguera | Roberto Auzzi, Stefano Baiguera, G. Bruno De Luca, Andrea Legramandi,
Giuseppe Nardelli and Nicol\`o Zenoni | Geometry of quantum complexity | 41 pages, several figures; v2: journal version; v3: journal title | Phys. Rev. D 103, 106021 (2021) | 10.1103/PhysRevD.103.106021 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Computational complexity is a new quantum information concept that may play
an important role in holography and in understanding the physics of the black
hole interior. We consider quantum computational complexity for $n$ qubits
using Nielsen's geometrical approach. We investigate a choice of penalties
which, compare... | [
{
"created": "Sun, 15 Nov 2020 18:41:19 GMT",
"version": "v1"
},
{
"created": "Tue, 11 May 2021 07:54:55 GMT",
"version": "v2"
},
{
"created": "Wed, 19 May 2021 18:27:14 GMT",
"version": "v3"
}
] | 2021-05-21 | [
[
"Auzzi",
"Roberto",
""
],
[
"Baiguera",
"Stefano",
""
],
[
"De Luca",
"G. Bruno",
""
],
[
"Legramandi",
"Andrea",
""
],
[
"Nardelli",
"Giuseppe",
""
],
[
"Zenoni",
"Nicolò",
""
]
] | Computational complexity is a new quantum information concept that may play an important role in holography and in understanding the physics of the black hole interior. We consider quantum computational complexity for $n$ qubits using Nielsen's geometrical approach. We investigate a choice of penalties which, compared ... | 11.059216 | 9.721282 | 11.796876 | 10.055368 | 10.823729 | 9.963951 | 10.275344 | 10.039608 | 9.96084 | 11.726785 | 10.197039 | 9.85226 | 10.553648 | 9.488847 | 9.461848 | 9.802786 | 9.815989 | 9.82216 | 10.000668 | 10.725805 | 10.319959 |
1106.3029 | Philip Gibbs | Philip Gibbs | A Universe Programmed with Strings of Qubits | 9 pages, a fourth prize winner in the 2011 FQXi essay contest "Is
Reality Digital or Analog?" | null | null | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been suggested that reality works like a quantum computer, but such
claims are just words if they are not backed up by sound mathematics. In
pursuit of the fundamental equations I look to string theory where physicists
led by Mike Duff have noticed useful connections between the quantum gravity of
black holes ... | [
{
"created": "Sat, 11 Jun 2011 13:19:32 GMT",
"version": "v1"
}
] | 2011-06-16 | [
[
"Gibbs",
"Philip",
""
]
] | It has been suggested that reality works like a quantum computer, but such claims are just words if they are not backed up by sound mathematics. In pursuit of the fundamental equations I look to string theory where physicists led by Mike Duff have noticed useful connections between the quantum gravity of black holes an... | 16.094013 | 19.39781 | 19.582062 | 17.242287 | 19.710398 | 18.844114 | 17.658895 | 18.4939 | 17.56798 | 18.765125 | 16.302744 | 16.556229 | 17.043009 | 16.945637 | 16.985788 | 17.184744 | 16.605478 | 16.435932 | 16.987123 | 17.118473 | 16.291767 |
2001.10947 | Zahra Molaee | Ali Dokhani, Zahra Molaee, Ahmad Shirzad | Gauge generator for bi-gravity and multi-gravity models | 13 pages,published version in Nuclear Physics B | null | 10.1016/j.nuclphysb.2021.115360 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Following the Hamiltonian structure of bi-gravity and multi-gravity models in
the full phase space, we have constructed the generating functional of
diffeomorphism gauge symmetry. As is expected, this generator is constructed
from the first class constraints of the system. We show that this gauge
generator works well... | [
{
"created": "Wed, 29 Jan 2020 16:38:45 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Feb 2020 19:11:51 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Mar 2021 23:30:11 GMT",
"version": "v3"
}
] | 2021-04-07 | [
[
"Dokhani",
"Ali",
""
],
[
"Molaee",
"Zahra",
""
],
[
"Shirzad",
"Ahmad",
""
]
] | Following the Hamiltonian structure of bi-gravity and multi-gravity models in the full phase space, we have constructed the generating functional of diffeomorphism gauge symmetry. As is expected, this generator is constructed from the first class constraints of the system. We show that this gauge generator works well i... | 12.805876 | 9.886912 | 11.314283 | 10.527424 | 10.217259 | 10.454758 | 9.980317 | 10.045127 | 11.012975 | 12.354987 | 11.476809 | 10.990202 | 10.959635 | 10.700026 | 10.682183 | 11.04213 | 10.784537 | 11.758362 | 10.985675 | 10.864605 | 11.042233 |
hep-th/0106187 | Yaron Oz | Harald Ita and Yaron Oz | String Field Theory and the Fuzzy Sphere | 14 pages, Latex, typos corrected, ref. added | Phys.Lett.B519:129-136,2001 | 10.1016/S0370-2693(01)01109-1 | CERN-TH/2001-160 | hep-th | null | We use boundary string field theory to study open string tachyon condensation
on a three-sphere closed string background. We consider the closed string
background described by $SU(2)_k$ WZW model in the limit of large $k$. We
compute the exact tachyon potential and analyse the decay modes.
| [
{
"created": "Wed, 20 Jun 2001 15:13:48 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Jul 2001 18:34:10 GMT",
"version": "v2"
}
] | 2009-09-29 | [
[
"Ita",
"Harald",
""
],
[
"Oz",
"Yaron",
""
]
] | We use boundary string field theory to study open string tachyon condensation on a three-sphere closed string background. We consider the closed string background described by $SU(2)_k$ WZW model in the limit of large $k$. We compute the exact tachyon potential and analyse the decay modes. | 7.857703 | 5.837505 | 8.76516 | 5.857532 | 6.460773 | 5.838913 | 5.655219 | 5.995512 | 6.356686 | 8.738697 | 6.246212 | 6.440017 | 7.494648 | 6.315448 | 6.48085 | 6.331865 | 6.061061 | 6.41365 | 6.494887 | 7.008952 | 6.414807 |
0710.2598 | Skenderis Kostas | Joost Hoogeveen and Kostas Skenderis | BRST quantization of the pure spinor superstring | 31 pages | JHEP 0711:081,2007 | 10.1088/1126-6708/2007/11/081 | ITFA-2007-49 | hep-th | null | We present a derivation of the scattering amplitude prescription for the pure
spinor superstring from first principles, both in the minimal and non-minimal
formulations, and show that they are equivalent. This is achieved by first
coupling the worldsheet action to topological gravity and then proceeding to
BRST quant... | [
{
"created": "Mon, 15 Oct 2007 15:47:20 GMT",
"version": "v1"
}
] | 2009-05-20 | [
[
"Hoogeveen",
"Joost",
""
],
[
"Skenderis",
"Kostas",
""
]
] | We present a derivation of the scattering amplitude prescription for the pure spinor superstring from first principles, both in the minimal and non-minimal formulations, and show that they are equivalent. This is achieved by first coupling the worldsheet action to topological gravity and then proceeding to BRST quantiz... | 10.077996 | 9.46732 | 11.385694 | 9.19192 | 9.740738 | 9.158698 | 8.932279 | 9.288939 | 8.858141 | 11.694466 | 8.540507 | 9.36184 | 10.058594 | 9.30177 | 9.700216 | 9.329462 | 9.150051 | 9.410055 | 9.317038 | 10.524501 | 9.333441 |
hep-th/0601058 | Indrajit Mitra | Indrajit Mitra, Raghunath Ratabole and H. S. Sharatchandra | Instability in scalar channel of fermion-antifermion scattering
amplitude in massless QED_3 and anomalous dimensions of composite operators | 10 pages, uses axodraw.sty; minor additions, version to appear in
Mod. Phys. Lett. A | Mod.Phys.Lett.A22:297-306,2007 | 10.1142/S0217732307020981 | IMSc/2006/01/01 | hep-th cond-mat.supr-con hep-ph | null | Instability in the scalar channel of the fermion-antifermion scattering
amplitude in massless QED_3 for number of flavours less than the critical value
128/3\pi^2 is demonstrated. The anomalous dimensions of gauge-invariant
composite operators are determined to O(1/N). Exponentiation of the O(1/N)
infrared logarithm ... | [
{
"created": "Tue, 10 Jan 2006 14:46:02 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Mar 2006 14:35:57 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Jan 2007 14:06:41 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Mitra",
"Indrajit",
""
],
[
"Ratabole",
"Raghunath",
""
],
[
"Sharatchandra",
"H. S.",
""
]
] | Instability in the scalar channel of the fermion-antifermion scattering amplitude in massless QED_3 for number of flavours less than the critical value 128/3\pi^2 is demonstrated. The anomalous dimensions of gauge-invariant composite operators are determined to O(1/N). Exponentiation of the O(1/N) infrared logarithm is... | 10.830337 | 9.855248 | 9.022263 | 8.303762 | 9.296466 | 8.519386 | 9.535047 | 8.352555 | 9.316921 | 8.638009 | 9.145394 | 9.192388 | 9.0453 | 8.828419 | 8.636748 | 9.078632 | 8.729967 | 9.042856 | 8.9966 | 9.623143 | 8.709506 |
1808.01182 | Aalok Misra | Vikas Yadav and Aalok Misra | M-Theory Exotic Scalar Glueball Decays to Mesons at Finite Coupling | v3:49 pages, LaTeX, 2 Figures, accepted journal (JHEP) version | null | 10.1007/JHEP09(2018)133 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the pull-back of the perturbed type IIA metric corresponding to the
perturbation of arXiv:hep-th/1306.4339's M-theory uplift of
arXiv:hep-th/0902.1540's UV-complete top-down type IIB holographic dual of
large-$N$ thermal QCD, at finite coupling, we obtain the interaction Lagrangian
corresponding to exotic scala... | [
{
"created": "Thu, 2 Aug 2018 17:40:47 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Aug 2018 17:34:44 GMT",
"version": "v2"
},
{
"created": "Wed, 5 Sep 2018 06:23:53 GMT",
"version": "v3"
}
] | 2018-10-17 | [
[
"Yadav",
"Vikas",
""
],
[
"Misra",
"Aalok",
""
]
] | Using the pull-back of the perturbed type IIA metric corresponding to the perturbation of arXiv:hep-th/1306.4339's M-theory uplift of arXiv:hep-th/0902.1540's UV-complete top-down type IIB holographic dual of large-$N$ thermal QCD, at finite coupling, we obtain the interaction Lagrangian corresponding to exotic scalar ... | 10.284618 | 11.964481 | 10.732246 | 9.664969 | 10.770987 | 10.64677 | 10.533447 | 9.719453 | 9.494289 | 11.99807 | 10.4393 | 10.071871 | 10.161803 | 9.913097 | 10.093526 | 10.030964 | 10.336009 | 9.882708 | 10.349236 | 10.096334 | 9.942002 |
1204.2711 | In Yong Park | E. Hatefi, A. J. Nurmagambetov and I. Y. Park | $N^3$ entropy of M5 branes from dielectric effect | latex, 21 pages, missing figure added | Nucl. Phys. B866 (2013) 58-71 | 10.1016/j.nuclphysb.2012.08.014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We observe that the $N^3$ entropy behavior of near-extermal M5 branes can be
reproduced from SYM side with the role of Myers' terms. We start by
generalizing the Klebanov-Tseytlin (KT) supergravity solution that displays the
$N^3$ entropy behavior. The new feature of the general solution is visibility
of the "interna... | [
{
"created": "Thu, 12 Apr 2012 13:14:54 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Apr 2012 12:35:24 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Aug 2012 23:28:41 GMT",
"version": "v3"
},
{
"created": "Thu, 8 Nov 2012 13:22:20 GMT",
"version": "v4"
}
] | 2012-11-09 | [
[
"Hatefi",
"E.",
""
],
[
"Nurmagambetov",
"A. J.",
""
],
[
"Park",
"I. Y.",
""
]
] | We observe that the $N^3$ entropy behavior of near-extermal M5 branes can be reproduced from SYM side with the role of Myers' terms. We start by generalizing the Klebanov-Tseytlin (KT) supergravity solution that displays the $N^3$ entropy behavior. The new feature of the general solution is visibility of the "internal"... | 11.707715 | 10.844106 | 12.493634 | 10.853274 | 11.020211 | 11.56597 | 10.692556 | 10.948994 | 10.939045 | 14.462197 | 10.180604 | 10.693839 | 12.03458 | 10.831021 | 10.758235 | 10.920517 | 10.655419 | 10.99708 | 11.013268 | 12.071098 | 11.114174 |
hep-th/9509116 | D. V. Ahluwalia, Lanl | D.V.Ahluwalia (Los Alamos National Laboratory) | A New Type of Massive Spin-One Boson: and its Relation with Maxwell
Equations | Invited talk presented at "The Present Status of Quantum Theory of
Light: A Symposium to Honour Jean-Pierre Vigier,'' held at York University,
Toronto, August 27-30, 1995. 15 pages, latex (crckapb.sty needed) | The Present Status of the Quantum Theory of Light, S.Jeffers et
al. (eds.) pp. 443-457 (1997). | 10.1007/978-94-011-5682-0_42 | LA-UR-95-3306 | hep-th hep-ph | null | First, we show that in the $(1,0)\oplus(0,1)$ representation space there
exist not one but two theories for charged particles. In the Weinberg
construct, the boson and its antiboson carry {\it same} relative intrinsic
parity, whereas in our construct the relative intrinsic parities of the boson
and its antiboson are ... | [
{
"created": "Thu, 21 Sep 1995 19:25:53 GMT",
"version": "v1"
}
] | 2021-03-25 | [
[
"Ahluwalia",
"D. V.",
"",
"Los Alamos National Laboratory"
]
] | First, we show that in the $(1,0)\oplus(0,1)$ representation space there exist not one but two theories for charged particles. In the Weinberg construct, the boson and its antiboson carry {\it same} relative intrinsic parity, whereas in our construct the relative intrinsic parities of the boson and its antiboson are {\... | 11.395161 | 11.739045 | 11.200302 | 11.224797 | 11.509519 | 11.746949 | 11.363325 | 10.497055 | 10.3121 | 11.1279 | 11.016648 | 10.754859 | 10.640742 | 10.599119 | 11.232998 | 10.775582 | 10.965719 | 10.625164 | 10.970721 | 10.59188 | 10.668134 |
1906.08730 | Andre Lukas | Callum R. Brodie, Andrei Constantin, Rehan Deen, Andre Lukas | Machine Learning Line Bundle Cohomology | 24 pages, Latex, 19 figures | null | 10.1002/prop.201900087 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate different approaches to machine learning of line bundle
cohomology on complex surfaces as well as on Calabi-Yau three-folds. Standard
function learning based on simple fully connected networks with logistic
sigmoids is reviewed and its main features and shortcomings are discussed. It
has been observed ... | [
{
"created": "Thu, 20 Jun 2019 16:21:56 GMT",
"version": "v1"
}
] | 2020-02-19 | [
[
"Brodie",
"Callum R.",
""
],
[
"Constantin",
"Andrei",
""
],
[
"Deen",
"Rehan",
""
],
[
"Lukas",
"Andre",
""
]
] | We investigate different approaches to machine learning of line bundle cohomology on complex surfaces as well as on Calabi-Yau three-folds. Standard function learning based on simple fully connected networks with logistic sigmoids is reviewed and its main features and shortcomings are discussed. It has been observed re... | 13.253317 | 13.47156 | 16.012999 | 12.792422 | 13.122246 | 12.964924 | 15.160292 | 13.471622 | 12.624231 | 17.548969 | 11.996038 | 12.959516 | 14.116692 | 12.880022 | 13.205843 | 13.254994 | 13.147727 | 12.975577 | 12.892019 | 14.052193 | 12.445273 |
0903.3979 | Diego Chialva | Diego Chialva | String Mass Shifts | 38 pages plus references, typos corrected, notation and text improved | null | 10.1016/j.nuclphysb.2009.04.023 | NORDITA-2009-21 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study closed string one-loop amplitudes in string theory, in particular
the average mass shift for states at given mass and Neveu-Schwarz charges. Our
analysis is based only on well-defined string amplitudes and the exploitation
of symmetries and unitarity properties of the torus amplitudes. We obtain the
result D... | [
{
"created": "Tue, 24 Mar 2009 18:21:11 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Apr 2009 18:13:52 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"Chialva",
"Diego",
""
]
] | We study closed string one-loop amplitudes in string theory, in particular the average mass shift for states at given mass and Neveu-Schwarz charges. Our analysis is based only on well-defined string amplitudes and the exploitation of symmetries and unitarity properties of the torus amplitudes. We obtain the result Del... | 12.292011 | 13.656875 | 12.602831 | 11.546841 | 13.24698 | 13.334513 | 12.864622 | 12.770966 | 11.129314 | 13.964521 | 12.004087 | 12.178359 | 12.202846 | 11.519279 | 12.275613 | 12.274796 | 11.984783 | 11.833273 | 11.475304 | 11.397951 | 11.614887 |
hep-th/0605142 | Manfred Requardt | Manfred Requardt | Entanglement-Entropy for Groundstates, Low-lying and Highly Excited
Eigenstates of General (Lattice) Hamiltonians | 36 pages, no figures, Latex, addition of further references and
comments following the suggestions of referees, submitted to J.Phys.A | null | null | null | hep-th cond-mat.stat-mech gr-qc quant-ph | null | We investigate the behavior of entanglement-entropy on a broad scale, that
is, a large class of systems, Hamiltonians and states describing the
interaction of many degrees of freedom. It is one of our aims to show which
general characteristics are responsible for the different types of quantitative
behavior of entant... | [
{
"created": "Mon, 15 May 2006 11:40:43 GMT",
"version": "v1"
},
{
"created": "Tue, 16 May 2006 09:54:06 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Mar 2007 09:46:31 GMT",
"version": "v3"
},
{
"created": "Mon, 6 Aug 2007 11:41:48 GMT",
"version": "v4"
}
] | 2007-08-06 | [
[
"Requardt",
"Manfred",
""
]
] | We investigate the behavior of entanglement-entropy on a broad scale, that is, a large class of systems, Hamiltonians and states describing the interaction of many degrees of freedom. It is one of our aims to show which general characteristics are responsible for the different types of quantitative behavior of entantgl... | 11.001398 | 11.407091 | 11.716754 | 11.120621 | 11.911338 | 11.728979 | 11.675429 | 10.924674 | 11.266616 | 12.256699 | 11.324798 | 11.055269 | 10.941698 | 10.928829 | 10.997557 | 11.013484 | 10.936847 | 11.017881 | 10.814709 | 10.913997 | 10.736526 |
2308.00361 | Masataka Matsumoto | Shuta Ishigaki, Shunichiro Kinoshita, Masataka Matsumoto | Stark effect and dissociation of mesons in holographic conductor | 31 pages, 12 figures. v2: match published version | J. High Energ. Phys. 2023, 128 (2023) | 10.1007/JHEP11(2023)128 | null | hep-th cond-mat.str-el nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the meson spectrum of the ${\cal{N}}=4$ supersymmetric Yang-Mills
theory with ${\cal{N}}=2$ fundamental hypermultiplets for a finite electric
field by using the D3/D7 model. The spectrum for scalar and vector mesons is
computed by analyzing the (quasi-)normal modes for the fluctuations of the
D7-brane embedd... | [
{
"created": "Tue, 1 Aug 2023 08:07:58 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Nov 2023 12:59:29 GMT",
"version": "v2"
}
] | 2023-11-22 | [
[
"Ishigaki",
"Shuta",
""
],
[
"Kinoshita",
"Shunichiro",
""
],
[
"Matsumoto",
"Masataka",
""
]
] | We study the meson spectrum of the ${\cal{N}}=4$ supersymmetric Yang-Mills theory with ${\cal{N}}=2$ fundamental hypermultiplets for a finite electric field by using the D3/D7 model. The spectrum for scalar and vector mesons is computed by analyzing the (quasi-)normal modes for the fluctuations of the D7-brane embeddin... | 6.329351 | 5.49463 | 6.660004 | 5.903494 | 6.164479 | 5.745275 | 6.060212 | 5.557694 | 5.685497 | 6.52764 | 5.872207 | 5.796091 | 6.194921 | 5.949587 | 5.842461 | 6.096275 | 5.976591 | 5.756078 | 5.928773 | 6.240563 | 5.823373 |
hep-th/0607140 | Hrvoje Nikolic | H. Nikolic | Nonlocal black-hole thermodynamics and massive remnants | 7 pages, 1 figure included | null | null | null | hep-th astro-ph gr-qc | null | To alleviate the black-hole (BH) information problem, we study a
holographic-principle-inspired nonlocal model of Hawking radiation in which
radiated particles created at different times all have the same temperature
corresponding to the instantaneous BH mass. Consequently, the black hole loses
mass not only by conti... | [
{
"created": "Thu, 20 Jul 2006 09:53:27 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nikolic",
"H.",
""
]
] | To alleviate the black-hole (BH) information problem, we study a holographic-principle-inspired nonlocal model of Hawking radiation in which radiated particles created at different times all have the same temperature corresponding to the instantaneous BH mass. Consequently, the black hole loses mass not only by continu... | 12.505623 | 11.638472 | 10.561597 | 10.856679 | 12.833422 | 12.068632 | 12.677419 | 11.908291 | 11.268709 | 12.48629 | 11.671996 | 10.805188 | 11.309229 | 11.293939 | 11.188063 | 10.972525 | 11.642194 | 10.97686 | 11.411331 | 10.645805 | 11.286732 |
hep-th/0508232 | Nelia Mann | Nelia Mann and Joe Polchinski | Bethe Ansatz for a Quantum Supercoset Sigma Model | 30 pages, 1 figure, v2: references added | Phys.Rev.D72:086002,2005 | 10.1103/PhysRevD.72.086002 | null | hep-th | null | We study an integrable conformal OSp(2m + 2|2m) supercoset model as an analog
to the AdS_5 X S^5 superstring world-sheet theory. Using the known S-matrix for
this system, we obtain integral equations for states of large particle density
in an SU(2) sector, which are exact in the sigma model coupling constant. As a
ch... | [
{
"created": "Tue, 30 Aug 2005 19:10:58 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Sep 2005 00:10:20 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Mann",
"Nelia",
""
],
[
"Polchinski",
"Joe",
""
]
] | We study an integrable conformal OSp(2m + 2|2m) supercoset model as an analog to the AdS_5 X S^5 superstring world-sheet theory. Using the known S-matrix for this system, we obtain integral equations for states of large particle density in an SU(2) sector, which are exact in the sigma model coupling constant. As a chec... | 10.911622 | 11.571628 | 13.801099 | 9.451102 | 10.890559 | 10.690475 | 10.44386 | 10.061196 | 10.265945 | 13.915409 | 9.830388 | 9.664773 | 10.927868 | 9.743979 | 10.002068 | 10.127788 | 9.724868 | 9.671645 | 9.931087 | 11.442206 | 10.316918 |
2306.04589 | Rodrigo Ferreira Sobreiro | Rodrigo F. Sobreiro | Unifying fractons, gravitons and photons from a gauge theoretical
approach | 6 pages. No figures | null | null | null | hep-th cond-mat.str-el gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the first principles gauge theoretical construction of
relativistic gapless fracton theory recently developed by A. Blasi and N.
Maggiore. The difference is that, instead of considering a symmetric tensor
field, we consider a vector field with a gauge group index, (i.e.) the usual
Einstein-Cartan variable ... | [
{
"created": "Wed, 7 Jun 2023 16:40:13 GMT",
"version": "v1"
}
] | 2023-06-08 | [
[
"Sobreiro",
"Rodrigo F.",
""
]
] | We revisit the first principles gauge theoretical construction of relativistic gapless fracton theory recently developed by A. Blasi and N. Maggiore. The difference is that, instead of considering a symmetric tensor field, we consider a vector field with a gauge group index, (i.e.) the usual Einstein-Cartan variable us... | 16.944798 | 18.941233 | 19.450701 | 17.481623 | 18.882814 | 16.673441 | 16.897495 | 17.64999 | 17.107943 | 21.747583 | 17.438156 | 16.552874 | 16.446497 | 16.173576 | 16.888168 | 16.194771 | 15.956339 | 16.623363 | 16.616274 | 16.793789 | 15.9533 |
hep-th/9210058 | null | E. Ivanov, S. Krivonos and R.P. Malik | Boussinesq-type equations from nonlinear realizations of $W_3$ | 23 pages, LaTeX | Int. J. Mod. Phys. A8 (1993) 3199-3222 | 10.1142/S0217751X93001284 | null | hep-th | null | We construct new coset realizations of infinite-dimensional linear
$W_3^{\infty}$ symmetry associated with Zamolodchikov's $W_3$ algebra which are
different from the previously explored $sl_3$ Toda realization of
$W_3^{\infty}$. We deduce the Boussinesq and modified Boussinesq equations as
constraints on the geometry... | [
{
"created": "Sat, 10 Oct 1992 16:26:00 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ivanov",
"E.",
""
],
[
"Krivonos",
"S.",
""
],
[
"Malik",
"R. P.",
""
]
] | We construct new coset realizations of infinite-dimensional linear $W_3^{\infty}$ symmetry associated with Zamolodchikov's $W_3$ algebra which are different from the previously explored $sl_3$ Toda realization of $W_3^{\infty}$. We deduce the Boussinesq and modified Boussinesq equations as constraints on the geometry o... | 7.49002 | 7.748518 | 8.411875 | 7.301316 | 7.684832 | 7.237771 | 7.87412 | 7.450687 | 7.05037 | 8.534357 | 7.306141 | 7.261326 | 7.52968 | 7.27294 | 7.133778 | 7.264019 | 7.137015 | 7.150506 | 7.240131 | 7.574784 | 7.154271 |
hep-th/0205037 | Allan Joseph Medved | A.J.M. Medved (University of Alberta) | Big Bangs and Bounces on the Brane | 24 pages, Latex; references added and minor corrections | null | null | null | hep-th | null | In view of our accelerating universe, one of the outstanding theoretical
issues is the absence of a quantum-gravitational description of de Sitter
space. Although speculative, an intriguing circumvention may be found in the
realm of brane-world scenarios; where the physical universe can be interpreted
as a non-critic... | [
{
"created": "Mon, 6 May 2002 19:55:02 GMT",
"version": "v1"
},
{
"created": "Tue, 14 May 2002 13:08:41 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Medved",
"A. J. M.",
"",
"University of Alberta"
]
] | In view of our accelerating universe, one of the outstanding theoretical issues is the absence of a quantum-gravitational description of de Sitter space. Although speculative, an intriguing circumvention may be found in the realm of brane-world scenarios; where the physical universe can be interpreted as a non-critical... | 10.267184 | 9.087698 | 10.91131 | 8.920046 | 9.642303 | 10.234055 | 9.439443 | 9.449492 | 9.053144 | 10.417248 | 9.494079 | 9.819453 | 9.710019 | 9.292935 | 9.179908 | 9.441538 | 9.736603 | 9.349684 | 9.349485 | 9.699801 | 9.690156 |
2102.08982 | Masanori Hanada | Masanori Hanada | Bulk geometry in gauge/gravity duality and color degrees of freedom | 26 pages, 2 figures. V2: a version accepted for publication in Phys.
Rev. D. V3: Minor typos fixed, the published version | Phys. Rev. D 103, 106007 (2021) | 10.1103/PhysRevD.103.106007 | DMUS-MP-21/02 | hep-th | http://creativecommons.org/licenses/by/4.0/ | U($N$) supersymmetric Yang-Mills theory naturally appears as the low-energy
effective theory of a system of $N$ D-branes and open strings between them.
Transverse spatial directions emerge from scalar fields, which are $N\times N$
matrices with color indices; roughly speaking, the eigenvalues are the
locations of D-b... | [
{
"created": "Wed, 17 Feb 2021 19:16:56 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Apr 2021 02:07:26 GMT",
"version": "v2"
},
{
"created": "Thu, 6 May 2021 18:24:44 GMT",
"version": "v3"
}
] | 2021-05-12 | [
[
"Hanada",
"Masanori",
""
]
] | U($N$) supersymmetric Yang-Mills theory naturally appears as the low-energy effective theory of a system of $N$ D-branes and open strings between them. Transverse spatial directions emerge from scalar fields, which are $N\times N$ matrices with color indices; roughly speaking, the eigenvalues are the locations of D-bra... | 7.292225 | 7.196954 | 7.587652 | 6.804961 | 7.255981 | 6.960711 | 7.267166 | 6.968715 | 6.988505 | 7.855815 | 6.947395 | 6.688241 | 7.027481 | 6.823731 | 6.769543 | 6.622059 | 6.688128 | 6.622091 | 6.741283 | 7.18836 | 6.592909 |
1310.0253 | Jochen Zahn | Jochen Zahn | The excitation spectrum of rotating strings with masses at the ends | 13 pages, 1 figure, v2: Typos corrected, v3: final | JHEP 1312 (2013) 047 | 10.1007/JHEP12(2013)047 | UWThPh-2013-26 | hep-th hep-lat math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the spectrum of excitations of the rotating Nambu-Goto string with
masses at the ends. We find interesting quasi-massless modes in the limit of
slow rotation and comment on the nontrivial relation between world-sheet and
target space energy.
| [
{
"created": "Tue, 1 Oct 2013 11:41:35 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Oct 2013 14:24:30 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Dec 2013 09:50:50 GMT",
"version": "v3"
}
] | 2013-12-13 | [
[
"Zahn",
"Jochen",
""
]
] | We compute the spectrum of excitations of the rotating Nambu-Goto string with masses at the ends. We find interesting quasi-massless modes in the limit of slow rotation and comment on the nontrivial relation between world-sheet and target space energy. | 13.136873 | 9.747749 | 12.294291 | 9.430635 | 9.905549 | 10.511222 | 9.517535 | 12.075001 | 9.612258 | 11.862111 | 10.540067 | 12.386192 | 11.533917 | 11.506803 | 11.705445 | 11.707539 | 11.09903 | 11.721551 | 11.995667 | 11.173643 | 10.614874 |
1809.00026 | Diego Pontello | Ra\'ul E. Arias, Horacio Casini, Marina Huerta, Diego Pontello | Entropy and modular Hamiltonian for a free chiral scalar in two
intervals | null | Phys. Rev. D 98, 125008 (2018) | 10.1103/PhysRevD.98.125008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the analytic form of the vacuum modular Hamiltonian for a two
interval region and the algebra of a current $j(x)=\partial \phi(x)$
corresponding to a chiral free scalar $\phi$ in $d=2$. We also compute
explicitly the mutual information between the intervals. This model shows a
failure of Haag duality for... | [
{
"created": "Fri, 31 Aug 2018 19:12:40 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Oct 2018 14:56:41 GMT",
"version": "v2"
}
] | 2018-12-26 | [
[
"Arias",
"Raúl E.",
""
],
[
"Casini",
"Horacio",
""
],
[
"Huerta",
"Marina",
""
],
[
"Pontello",
"Diego",
""
]
] | We calculate the analytic form of the vacuum modular Hamiltonian for a two interval region and the algebra of a current $j(x)=\partial \phi(x)$ corresponding to a chiral free scalar $\phi$ in $d=2$. We also compute explicitly the mutual information between the intervals. This model shows a failure of Haag duality for t... | 10.675059 | 11.2139 | 13.089505 | 10.372307 | 11.122672 | 11.248113 | 10.926435 | 10.344724 | 10.589112 | 12.345288 | 10.338341 | 10.165406 | 11.201124 | 10.380313 | 10.477787 | 10.515326 | 10.738348 | 10.182564 | 10.283389 | 10.8421 | 10.448254 |
hep-th/9804161 | null | Masahiro Kubo, Ziro Maki, Mikio Nakahara (Kinki University), Takesi
Saito (Kwansei Gakuin University) | Grand Unification from Gauge Theory on $M_4 \times Z_N$ | 11 pages, 7 figures, style changed to revtex, added reference to
section 1, corrected typos | Prog.Theor.Phys. 100 (1998) 165-178 | 10.1143/PTP.100.165 | KUP-9801 | hep-th | null | The SU(5) grand unified theory (GUT) is derived from the geometrical point of
view of gauge theory on three-sheeted space-time, i.e., $M_4 \times Z_3$
manifold without recourse to noncommutative geometry. A derivation of SO(10)
GUT is also discussed in the same point of view.
| [
{
"created": "Fri, 24 Apr 1998 09:04:02 GMT",
"version": "v1"
},
{
"created": "Wed, 27 May 1998 09:14:37 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Kubo",
"Masahiro",
"",
"Kinki University"
],
[
"Maki",
"Ziro",
"",
"Kinki University"
],
[
"Nakahara",
"Mikio",
"",
"Kinki University"
],
[
"Saito",
"Takesi",
"",
"Kwansei Gakuin University"
]
] | The SU(5) grand unified theory (GUT) is derived from the geometrical point of view of gauge theory on three-sheeted space-time, i.e., $M_4 \times Z_3$ manifold without recourse to noncommutative geometry. A derivation of SO(10) GUT is also discussed in the same point of view. | 8.8819 | 7.333845 | 9.14025 | 8.405714 | 8.436604 | 7.588451 | 8.025312 | 8.316373 | 7.597564 | 9.108865 | 7.331226 | 7.912175 | 7.797099 | 7.734276 | 8.096701 | 8.355165 | 7.912439 | 8.001734 | 7.781931 | 7.910841 | 8.431165 |
hep-th/9408142 | null | A. Petermann, A. Zichichi | Explicit supertring vacua in a background of gravitational waves and
dilaton | 10 pages, latex, CERN-TH.7373/94 | Nuovo Cim.A108:97-104,1995 | 10.1007/BF02814860 | null | hep-th | null | We present an explicit solution of superstring effective equations,
represented by gravitational waves and dilaton backgrounds. Particular
solutions will be examined in a forthcoming note.
| [
{
"created": "Fri, 26 Aug 1994 08:40:32 GMT",
"version": "v1"
}
] | 2009-08-25 | [
[
"Petermann",
"A.",
""
],
[
"Zichichi",
"A.",
""
]
] | We present an explicit solution of superstring effective equations, represented by gravitational waves and dilaton backgrounds. Particular solutions will be examined in a forthcoming note. | 51.492836 | 47.059559 | 30.040249 | 37.726563 | 34.856579 | 41.059444 | 46.366356 | 42.778282 | 44.864475 | 41.368233 | 36.207302 | 45.540699 | 37.636318 | 38.416885 | 39.635433 | 40.523407 | 38.528084 | 44.196075 | 41.411949 | 41.145943 | 39.873611 |
hep-th/9502091 | Elena S. Suslova | A.Morozov | Matrix Models as Integrable Systems | 60 pages, LaTeX. Presented at Banff Conference, Banff, Canada, 15-23
August 1994. | null | null | ITEP-M2/95 | hep-th | null | The theory of matrix models is reviewed from the point of view of its
relation to integrable hierarchies. Determinantal formulas, relation to
conformal field models and the theory of Generalized Kontsevich model are
discussed in some detail. Attention is also paid to the group-theoretical
interpretation of $\tau$-fun... | [
{
"created": "Tue, 14 Feb 1995 23:13:47 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Morozov",
"A.",
""
]
] | The theory of matrix models is reviewed from the point of view of its relation to integrable hierarchies. Determinantal formulas, relation to conformal field models and the theory of Generalized Kontsevich model are discussed in some detail. Attention is also paid to the group-theoretical interpretation of $\tau$-funct... | 7.941905 | 7.488756 | 8.426221 | 6.750619 | 6.702764 | 6.958702 | 6.866774 | 7.435084 | 6.8659 | 8.540491 | 7.309499 | 7.075671 | 7.826575 | 7.164293 | 7.296367 | 7.163859 | 7.089095 | 7.32242 | 7.339847 | 7.792795 | 7.168154 |
1404.1607 | Charilaos Tsagkarakis Ph.D | F.K. Diakonos, G.C. Katsimiga, X.N. Maintas and C.E. Tsagkarakis | Symmetric solitonic excitations of the (1+1)-dimensional Abelian-Higgs
"classical vacuum" | 8 pages, 5 figures | Phys. Rev. E 91, 023202 (2015) | 10.1103/PhysRevE.91.023202 | null | hep-th cond-mat.supr-con nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the classical dynamics of the Abelian-Higgs model in (1+1)
space-time dimensions bf for the case of strongly broken gauge symmetry. In
this limit the wells of the potential are almost harmonic and sufficiently
deep, presenting a scenario far from the associated critical point. Using a
multiscale perturbation... | [
{
"created": "Sun, 6 Apr 2014 19:01:38 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Apr 2014 11:11:17 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Jun 2014 09:15:24 GMT",
"version": "v3"
},
{
"created": "Fri, 28 Nov 2014 19:58:53 GMT",
"version": "v4"
},
{
"cre... | 2015-03-05 | [
[
"Diakonos",
"F. K.",
""
],
[
"Katsimiga",
"G. C.",
""
],
[
"Maintas",
"X. N.",
""
],
[
"Tsagkarakis",
"C. E.",
""
]
] | We study the classical dynamics of the Abelian-Higgs model in (1+1) space-time dimensions bf for the case of strongly broken gauge symmetry. In this limit the wells of the potential are almost harmonic and sufficiently deep, presenting a scenario far from the associated critical point. Using a multiscale perturbation e... | 9.563152 | 10.68284 | 10.647925 | 9.549712 | 10.636157 | 10.27861 | 10.862036 | 10.325112 | 9.601595 | 11.083858 | 9.571475 | 9.774354 | 9.665071 | 9.568892 | 9.438758 | 9.622011 | 9.491565 | 9.766047 | 9.397299 | 9.795513 | 9.486524 |
1501.02499 | Edward Witten | Edward Witten | The Super Period Matrix With Ramond Punctures | 38 pp. plus appendices | null | 10.1016/j.geomphys.2015.02.017 | null | hep-th math-ph math.AG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the super period matrix of a super Riemann surface to the case
that Ramond punctures are present. For a super Riemann surface of genus g with
2r Ramond punctures, we define, modulo certain choices that generalize those in
the classical theory (and assuming a certain generic condition is satisfied), a
g|... | [
{
"created": "Sun, 11 Jan 2015 22:04:03 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Witten",
"Edward",
""
]
] | We generalize the super period matrix of a super Riemann surface to the case that Ramond punctures are present. For a super Riemann surface of genus g with 2r Ramond punctures, we define, modulo certain choices that generalize those in the classical theory (and assuming a certain generic condition is satisfied), a g|r ... | 10.018944 | 10.210699 | 12.185239 | 9.838289 | 9.669134 | 10.403573 | 9.56934 | 9.37938 | 9.852065 | 12.784019 | 9.767585 | 9.871017 | 10.458596 | 9.758229 | 9.759779 | 9.968811 | 9.666361 | 10.021641 | 9.595239 | 10.540627 | 9.712036 |
2301.01174 | Edouard Brezin | Edouard Brezin | Should we worry about renormalons in the epsilon-expansion? | null | null | null | null | hep-th cond-mat.stat-mech | http://creativecommons.org/publicdomain/zero/1.0/ | Turning the divergent epsilon-expansion into a numerically sensible
algorithm, relies on the knowledge of the behaviour of the large order
contributions. Two different pictures are known to compete there. The first one
was based on Lipatov's instantons, which is known to deal with the multiplicity
of Feynman diagrams... | [
{
"created": "Tue, 3 Jan 2023 16:04:04 GMT",
"version": "v1"
}
] | 2023-01-04 | [
[
"Brezin",
"Edouard",
""
]
] | Turning the divergent epsilon-expansion into a numerically sensible algorithm, relies on the knowledge of the behaviour of the large order contributions. Two different pictures are known to compete there. The first one was based on Lipatov's instantons, which is known to deal with the multiplicity of Feynman diagrams w... | 14.766902 | 16.081905 | 14.715219 | 13.580792 | 15.519304 | 15.312367 | 16.976196 | 16.383682 | 14.74163 | 15.249445 | 14.33986 | 14.050357 | 14.254876 | 13.872938 | 13.894434 | 14.556969 | 13.528732 | 13.514921 | 13.390604 | 14.232358 | 13.172078 |
hep-th/0701055 | Fiorenzo Bastianelli | Fiorenzo Bastianelli, Olindo Corradini, Emanuele Latini | Higher spin fields from a worldline perspective | 21 pages | JHEP 0702:072,2007 | 10.1088/1126-6708/2007/02/072 | null | hep-th | null | Higher spin fields in four dimensions, and more generally conformal fields in
arbitrary dimensions, can be described by spinning particle models with a
gauged SO(N) extended supergravity on the worldline. We consider here the
one-loop quantization of these models by studying the corresponding partition
function on th... | [
{
"created": "Mon, 8 Jan 2007 11:13:11 GMT",
"version": "v1"
}
] | 2010-10-27 | [
[
"Bastianelli",
"Fiorenzo",
""
],
[
"Corradini",
"Olindo",
""
],
[
"Latini",
"Emanuele",
""
]
] | Higher spin fields in four dimensions, and more generally conformal fields in arbitrary dimensions, can be described by spinning particle models with a gauged SO(N) extended supergravity on the worldline. We consider here the one-loop quantization of these models by studying the corresponding partition function on the ... | 7.923818 | 7.983469 | 9.093678 | 7.375888 | 7.685984 | 7.869241 | 8.056573 | 7.542073 | 7.20564 | 8.460983 | 7.471828 | 7.705571 | 7.618395 | 7.268938 | 7.718354 | 7.683218 | 7.728334 | 7.476657 | 7.499934 | 7.509514 | 7.544687 |
2401.16494 | Josh Cork | Josh Cork, Derek Harland | Finkelstein-Rubinstein constraints from ADHM data and rational maps | 1+11 pages, 1 figure. Matches journal version | Physics Letters B, Volume 850, 2024, 138542 | 10.1016/j.physletb.2024.138542 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We establish simple formulae for computing Finkelstein-Rubinstein signs for
Skyrme fields generated in two ways: from instanton ADHM data, and from
rational maps. This may be used to compute homotopy classes of general loops in
the configuration spaces of skyrmions, and as a result provide a useful tool
for a quantum... | [
{
"created": "Mon, 29 Jan 2024 19:08:53 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Mar 2024 18:12:01 GMT",
"version": "v2"
}
] | 2024-03-05 | [
[
"Cork",
"Josh",
""
],
[
"Harland",
"Derek",
""
]
] | We establish simple formulae for computing Finkelstein-Rubinstein signs for Skyrme fields generated in two ways: from instanton ADHM data, and from rational maps. This may be used to compute homotopy classes of general loops in the configuration spaces of skyrmions, and as a result provide a useful tool for a quantum t... | 20.091293 | 20.143438 | 20.499168 | 19.36677 | 19.666594 | 18.981514 | 19.363361 | 17.418627 | 17.430546 | 23.27154 | 17.940294 | 19.00786 | 21.979309 | 19.617674 | 19.651814 | 19.045935 | 18.768772 | 18.834053 | 19.095102 | 22.702024 | 19.408754 |
1808.00350 | J.-C. Wallet | Timoth\'e Poulain, Jean-Christophe Wallet | $\kappa$-Poincar\'e invariant orientable field theories at 1-loop | 18 pages. Misprints corrected, title shortened. Version to appear in
JHEP | JHEP 01 (2019) 064 | 10.1007/JHEP01(2019)064 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a family of $\kappa$-Poincar\'e invariant scalar field theories
on 4-d $\kappa$-Minkowski space with quartic orientable interaction, that is
for which $\phi$ and its conjugate $\phi^\dag$ alternate in the quartic
interaction, and whose kinetic operator is the square of a
$U_\kappa(iso(4))$-equivariant Dir... | [
{
"created": "Wed, 1 Aug 2018 15:00:41 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Jan 2019 14:23:55 GMT",
"version": "v2"
}
] | 2019-01-15 | [
[
"Poulain",
"Timothé",
""
],
[
"Wallet",
"Jean-Christophe",
""
]
] | We consider a family of $\kappa$-Poincar\'e invariant scalar field theories on 4-d $\kappa$-Minkowski space with quartic orientable interaction, that is for which $\phi$ and its conjugate $\phi^\dag$ alternate in the quartic interaction, and whose kinetic operator is the square of a $U_\kappa(iso(4))$-equivariant Dirac... | 11.625859 | 11.390771 | 11.891418 | 9.960059 | 10.881888 | 11.109999 | 11.410999 | 10.807911 | 10.807376 | 14.022985 | 10.690973 | 10.34067 | 11.278541 | 10.270988 | 10.825899 | 10.380073 | 10.413939 | 10.882879 | 10.468937 | 11.357919 | 10.300161 |
0912.2063 | Carlos Bonin | C. A. Bonin, R. Bufalo, B. M. Pimentel, G. E. R. Zambrano | Podolsky Electromagnetism at Finite Temperature: Implications on
Stefan-Boltzmann Law | 13 pages, submitted to Physical Review D | Phys.Rev.D81:025003,2010 | 10.1103/PhysRevD.81.025003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we study Podolsky electromagnetism in thermodynamic equilibrium.
We show that a Podolsky mass-dependent modification to the Stefan-Boltzmann law
is induced and we use experimental data to limit the possible values for this
free parameter.
| [
{
"created": "Thu, 10 Dec 2009 19:19:19 GMT",
"version": "v1"
}
] | 2011-05-20 | [
[
"Bonin",
"C. A.",
""
],
[
"Bufalo",
"R.",
""
],
[
"Pimentel",
"B. M.",
""
],
[
"Zambrano",
"G. E. R.",
""
]
] | In this work we study Podolsky electromagnetism in thermodynamic equilibrium. We show that a Podolsky mass-dependent modification to the Stefan-Boltzmann law is induced and we use experimental data to limit the possible values for this free parameter. | 15.437185 | 10.523399 | 12.870076 | 9.976717 | 11.854757 | 10.635384 | 10.07329 | 12.300545 | 10.655152 | 12.358814 | 11.499143 | 11.977546 | 11.944272 | 11.640251 | 12.30449 | 12.134974 | 11.61079 | 11.41988 | 10.804402 | 12.400847 | 12.747186 |
2002.07302 | Vitor Emanuel Rodino Lemes | A.R. de S\'a, M.A.L. Capri, V. E. R. Lemes | Covariant Mass and Geometrical setup in Euclidean gauge theories | 17 pages, no figures | Phys. Rev. D 101, 105003 (2020) | 10.1103/PhysRevD.101.105003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A nonlocal mass operator can be consistently set in local form through the
introduction of a set of additional fields with geometrical appropriated
properties. A local and polynomial gauge invariant action is thus identified.
Equations compatible with the study of renormalization, from the algebraic
point of view, ar... | [
{
"created": "Mon, 17 Feb 2020 23:37:47 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Apr 2020 17:54:15 GMT",
"version": "v2"
}
] | 2020-05-13 | [
[
"de Sá",
"A. R.",
""
],
[
"Capri",
"M. A. L.",
""
],
[
"Lemes",
"V. E. R.",
""
]
] | A nonlocal mass operator can be consistently set in local form through the introduction of a set of additional fields with geometrical appropriated properties. A local and polynomial gauge invariant action is thus identified. Equations compatible with the study of renormalization, from the algebraic point of view, are ... | 29.325817 | 22.664261 | 24.449663 | 21.598125 | 21.088684 | 21.34421 | 20.175594 | 21.714703 | 21.041775 | 24.66748 | 23.282967 | 22.200247 | 21.997904 | 21.981577 | 22.126459 | 22.433174 | 22.623014 | 22.92079 | 24.132626 | 23.16938 | 22.786858 |
0810.0703 | Ben Freivogel | Ben Freivogel | Anthropic Explanation of the Dark Matter Abundance | 10 pages; v3: published version, references added | JCAP 1003:022,2010 | 10.1088/1475-7516/2010/03/021 | null | hep-th astro-ph hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I use Bousso's causal diamond measure to make a statistical prediction for
the dark matter abundance, assuming an axion with a large decay constant f_a >>
10^{12} GeV. Using a crude approximation for observer formation, the prediction
agrees well with observation: 30% of observers form in regions with less dark
matte... | [
{
"created": "Fri, 3 Oct 2008 19:41:45 GMT",
"version": "v1"
},
{
"created": "Sun, 5 Oct 2008 20:44:33 GMT",
"version": "v2"
},
{
"created": "Wed, 10 Mar 2010 22:30:57 GMT",
"version": "v3"
}
] | 2015-05-13 | [
[
"Freivogel",
"Ben",
""
]
] | I use Bousso's causal diamond measure to make a statistical prediction for the dark matter abundance, assuming an axion with a large decay constant f_a >> 10^{12} GeV. Using a crude approximation for observer formation, the prediction agrees well with observation: 30% of observers form in regions with less dark matter ... | 9.553148 | 9.949189 | 8.917583 | 8.188941 | 9.427052 | 9.250837 | 9.101588 | 8.787023 | 7.926911 | 9.282516 | 8.924491 | 8.614838 | 9.02089 | 8.400762 | 8.607637 | 8.951402 | 8.567869 | 8.501223 | 8.307017 | 8.702307 | 8.306436 |
0912.1984 | Mahmood ul Hassan | Bushra Haider and M. Hassan | The U(N) chiral model and exact multi-solitons | null | J.Phys.A41:255202,2008 | 10.1088/1751-8113/41/25/255202 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use a binary Darboux transformation to obtain exact multisoliton solutions
of the principal chiral model and its noncommutative generalization. We also
show that the exact multisolitons of the noncommutative principal chiral model
in two dimensions and noncommutative (anti) self dual Yang Mills equations in
four d... | [
{
"created": "Thu, 10 Dec 2009 12:29:07 GMT",
"version": "v1"
}
] | 2010-03-16 | [
[
"Haider",
"Bushra",
""
],
[
"Hassan",
"M.",
""
]
] | We use a binary Darboux transformation to obtain exact multisoliton solutions of the principal chiral model and its noncommutative generalization. We also show that the exact multisolitons of the noncommutative principal chiral model in two dimensions and noncommutative (anti) self dual Yang Mills equations in four dim... | 5.967319 | 5.406307 | 6.735261 | 5.530723 | 5.506191 | 5.606834 | 5.613614 | 5.79012 | 5.195952 | 6.98929 | 5.608424 | 5.863318 | 6.217797 | 5.967844 | 5.912271 | 5.801669 | 5.678755 | 5.679666 | 5.715038 | 6.00906 | 5.801047 |
1704.05077 | Nima Lashkari | Nima Lashkari | Entanglement at a Scale and Renormalization Monotones | null | JHEP 1901(2019) 219 | 10.1007/JHEP01(2019)219 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the information content of the reduced density matrix of a region in
quantum field theory that cannot be recovered from its subregion density
matrices. We reconstruct the density matrix from its subregions using two
approaches: scaling maps and recovery maps. The vacuum of a scale-invariant
field theory is t... | [
{
"created": "Mon, 17 Apr 2017 18:07:08 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Oct 2017 04:14:40 GMT",
"version": "v2"
},
{
"created": "Wed, 23 Jan 2019 13:44:26 GMT",
"version": "v3"
}
] | 2019-01-30 | [
[
"Lashkari",
"Nima",
""
]
] | We study the information content of the reduced density matrix of a region in quantum field theory that cannot be recovered from its subregion density matrices. We reconstruct the density matrix from its subregions using two approaches: scaling maps and recovery maps. The vacuum of a scale-invariant field theory is the... | 10.395755 | 9.675323 | 10.152238 | 9.306084 | 11.002411 | 10.462484 | 10.042182 | 10.33289 | 9.874775 | 10.777172 | 10.263647 | 9.77041 | 10.574465 | 10.055254 | 9.838038 | 10.212578 | 10.575604 | 9.916058 | 10.112987 | 10.143811 | 10.010434 |
hep-th/0405244 | Ki-Myeong Lee | Ki-Myeong Lee | Chern-Simons Solitons, Chiral Model, and (affine) Toda Model on
Noncommutative Space | latex, JHEP style, 23 pages, no figure | JHEP 0408 (2004) 054 | 10.1088/1126-6708/2004/08/054 | KIAS-P04022, UTIG-05-04 | hep-th | null | We consider the Dunne-Jackiw-Pi-Trugenberger model of a U(N) Chern-Simons
gauge theory coupled to a nonrelativistic complex adjoint matter on
noncommutative space. Soliton configurations of this model are related the
solutions of the chiral model on noncommutative plane. A generalized
Uhlenbeck's uniton method for th... | [
{
"created": "Wed, 26 May 2004 18:33:34 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Lee",
"Ki-Myeong",
""
]
] | We consider the Dunne-Jackiw-Pi-Trugenberger model of a U(N) Chern-Simons gauge theory coupled to a nonrelativistic complex adjoint matter on noncommutative space. Soliton configurations of this model are related the solutions of the chiral model on noncommutative plane. A generalized Uhlenbeck's uniton method for the ... | 9.398513 | 8.959352 | 10.391282 | 9.010854 | 9.83886 | 8.268159 | 9.281798 | 8.992738 | 8.6606 | 12.45721 | 9.349149 | 8.945187 | 9.539324 | 9.038371 | 9.286043 | 8.842783 | 8.791505 | 9.055415 | 9.138965 | 9.672382 | 8.751252 |
hep-th/0406120 | Neil Barnaby | Neil Barnaby | Caustic Formation in Tachyon Effective Field Theories | 23 pages, 5 figures; accepted for publication in JHEP. Revised
derivation of eikonal equation for the DBI action. Added comments concerning
the relationship between p-adic string theory and tachyon matter. Added
second example of inhomogeneous evolution in p-adic string theory. Misleading
statements concerning ... | JHEP 0407:025,2004 | 10.1088/1126-6708/2004/07/025 | McGILL-14-04 | hep-th | null | Certain configurations of D-branes, for example wrong dimensional branes or
the brane-antibrane system, are unstable to decay. This instability is
described by the appearance of a tachyonic mode in the spectrum of open strings
ending on the brane(s). The decay of these unstable systems is described by the
rolling of ... | [
{
"created": "Mon, 14 Jun 2004 13:54:17 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jul 2004 13:29:01 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Barnaby",
"Neil",
""
]
] | Certain configurations of D-branes, for example wrong dimensional branes or the brane-antibrane system, are unstable to decay. This instability is described by the appearance of a tachyonic mode in the spectrum of open strings ending on the brane(s). The decay of these unstable systems is described by the rolling of th... | 6.192513 | 6.391583 | 6.689196 | 6.363883 | 6.307834 | 6.31762 | 6.451052 | 6.16414 | 6.169009 | 7.313465 | 6.04133 | 6.182479 | 6.076912 | 6.110957 | 5.985009 | 6.000266 | 6.006225 | 6.049351 | 6.130527 | 6.228142 | 6.109015 |
hep-th/0109050 | null | Justin Khoury, Burt A. Ovrut, Paul J. Steinhardt and Neil Turok | Density Perturbations in the Ekpyrotic Scenario | 36 pages, compressed and RevTex file, one postscript figure file.
Minor typographical and numerical errors corrected, discussion added. This
version to appear in Physical Review D | Phys.Rev.D66:046005,2002 | 10.1103/PhysRevD.66.046005 | null | hep-th astro-ph | null | We study the generation of density perturbations in the ekpyrotic scenario
for the early universe, including gravitational backreaction. We expose
interesting subtleties that apply to both inflationary and ekpyrotic models.
Our analysis includes a detailed proposal of how the perturbations generated in
a contracting ... | [
{
"created": "Thu, 6 Sep 2001 22:05:10 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Sep 2001 11:37:39 GMT",
"version": "v2"
},
{
"created": "Sun, 3 Mar 2002 10:28:26 GMT",
"version": "v3"
},
{
"created": "Wed, 6 Mar 2002 10:53:16 GMT",
"version": "v4"
}
] | 2009-09-15 | [
[
"Khoury",
"Justin",
""
],
[
"Ovrut",
"Burt A.",
""
],
[
"Steinhardt",
"Paul J.",
""
],
[
"Turok",
"Neil",
""
]
] | We study the generation of density perturbations in the ekpyrotic scenario for the early universe, including gravitational backreaction. We expose interesting subtleties that apply to both inflationary and ekpyrotic models. Our analysis includes a detailed proposal of how the perturbations generated in a contracting ph... | 8.443137 | 7.618659 | 8.320015 | 7.819175 | 7.69289 | 7.911798 | 7.139023 | 7.820363 | 7.691733 | 8.352924 | 7.517808 | 7.614883 | 8.24479 | 7.72668 | 7.998094 | 8.023968 | 7.982348 | 8.035378 | 7.873433 | 7.987797 | 7.983591 |
0704.2526 | Ralf Hofmann | Francesco Giacosa and Ralf Hofmann | Nonperturbative screening of the Landau pole | 11 pages, 3 figures | Phys.Rev.D77:065022,2008 | 10.1103/PhysRevD.77.065022 | KA-TP-09-2007 | hep-th | null | Based on the trace anomaly for the energy-momentum tensor, an effective
theory for the thermodynamics of the deconfining phase, and by assuming the
asymptotic behavior to be determined by one-loop perturbation theory we compute
the nonperturbative beta function for the fundamental coupling $g$ in SU(2) and
SU(3) Yang... | [
{
"created": "Thu, 19 Apr 2007 13:12:58 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Giacosa",
"Francesco",
""
],
[
"Hofmann",
"Ralf",
""
]
] | Based on the trace anomaly for the energy-momentum tensor, an effective theory for the thermodynamics of the deconfining phase, and by assuming the asymptotic behavior to be determined by one-loop perturbation theory we compute the nonperturbative beta function for the fundamental coupling $g$ in SU(2) and SU(3) Yang-M... | 7.772099 | 7.876709 | 7.433618 | 7.1952 | 7.548321 | 7.694056 | 8.078458 | 7.756453 | 6.945368 | 8.294999 | 7.089368 | 7.205593 | 6.78654 | 6.956412 | 7.210734 | 7.259851 | 6.991756 | 6.935732 | 7.030644 | 7.317476 | 7.259285 |
hep-th/0605229 | Claus Kiefer | Mariusz P. Dabrowski, Claus Kiefer, Barbara Sandhoefer | Quantum phantom cosmology | 21 pages, 6 figures | Phys.Rev. D74 (2006) 044022 | 10.1103/PhysRevD.74.044022 | null | hep-th astro-ph gr-qc | null | We apply the formalism of quantum cosmology to models containing a phantom
field. Three models are discussed explicitly: a toy model, a model with an
exponential phantom potential, and a model with phantom field accompanied by a
negative cosmological constant. In all these cases we calculate the classical
trajectorie... | [
{
"created": "Tue, 23 May 2006 12:59:09 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Dabrowski",
"Mariusz P.",
""
],
[
"Kiefer",
"Claus",
""
],
[
"Sandhoefer",
"Barbara",
""
]
] | We apply the formalism of quantum cosmology to models containing a phantom field. Three models are discussed explicitly: a toy model, a model with an exponential phantom potential, and a model with phantom field accompanied by a negative cosmological constant. In all these cases we calculate the classical trajectories ... | 6.213408 | 6.837587 | 6.356733 | 6.055161 | 6.550168 | 6.504957 | 6.503114 | 5.932676 | 6.479761 | 6.245907 | 6.523409 | 6.307494 | 6.368504 | 6.213797 | 6.227188 | 6.298648 | 6.212327 | 6.082795 | 6.203505 | 6.295456 | 6.375191 |
hep-th/0601142 | Dmitri Bykov | R.N.Baranov, D.V.Bykov, A.A.Slavnov | The condensate <tr(A_{\mu}^{2})> in commutative and noncommutative
theories | 7 pages, 1 figure | Theor.Math.Phys.148:1168-1173,2006; Teor.Mat.Fiz.148:350-356,2006 | 10.1007/s11232-006-0110-9 | null | hep-th | null | It is shown that gauge invariance of the operator \int dx
tr(A_{\mu}^{2}-\frac{2}{g \xi} x^{\nu} \theta_{\mu\nu} A^{\mu}) in
noncommutative gauge theory does not lead to gauge independence of its vacuum
condensate. Generalized Ward identities are obtained for Green's functions
involving operator \underset{\Omega \to ... | [
{
"created": "Thu, 19 Jan 2006 20:33:33 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jan 2006 22:21:58 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Baranov",
"R. N.",
""
],
[
"Bykov",
"D. V.",
""
],
[
"Slavnov",
"A. A.",
""
]
] | It is shown that gauge invariance of the operator \int dx tr(A_{\mu}^{2}-\frac{2}{g \xi} x^{\nu} \theta_{\mu\nu} A^{\mu}) in noncommutative gauge theory does not lead to gauge independence of its vacuum condensate. Generalized Ward identities are obtained for Green's functions involving operator \underset{\Omega \to \i... | 6.544866 | 7.171027 | 5.904655 | 6.208943 | 6.838852 | 6.72745 | 6.694454 | 6.732558 | 6.110958 | 6.893957 | 5.957716 | 5.994686 | 5.890355 | 5.911907 | 5.960603 | 6.105846 | 6.331526 | 6.20739 | 5.854944 | 5.886265 | 5.830886 |
hep-th/0207027 | Michael R. Douglas | David Berenstein and Michael R. Douglas | Seiberg Duality for Quiver Gauge Theories | 52 pages, 6 figures, Latex in JHEP format | null | null | RU-NHETC-2002-26 | hep-th | null | A popular way to study N=1 supersymmetric gauge theories is to realize them
geometrically in string theory, as suspended brane constructions, D-branes
wrapping cycles in Calabi-Yau manifolds, orbifolds, and otherwise. Among the
applications of this idea are simple derivations and generalizations of Seiberg
duality fo... | [
{
"created": "Tue, 2 Jul 2002 18:24:40 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Berenstein",
"David",
""
],
[
"Douglas",
"Michael R.",
""
]
] | A popular way to study N=1 supersymmetric gauge theories is to realize them geometrically in string theory, as suspended brane constructions, D-branes wrapping cycles in Calabi-Yau manifolds, orbifolds, and otherwise. Among the applications of this idea are simple derivations and generalizations of Seiberg duality for ... | 8.156258 | 8.453309 | 9.343502 | 8.148591 | 8.253524 | 8.622872 | 8.736387 | 8.832953 | 8.285883 | 9.810708 | 8.134214 | 8.28107 | 8.58144 | 8.330874 | 8.240315 | 8.383471 | 8.286183 | 8.249572 | 8.323311 | 8.733286 | 8.248101 |
hep-th/0409216 | Antonio Soares de Castro | Antonio S. de Castro, Marcelo Hott | Exact closed-form solutions of the Dirac equation with a scalar
exponential potential | 16 pages, 3 figures | Phys.Lett. A342 (2005) 53-59 | 10.1016/j.physleta.2005.05.039 | null | hep-th quant-ph | null | The problem of a fermion subject to a general scalar potential in a
two-dimensional world for nonzero eigenenergies is mapped into a
Sturm-Liouville problem for the upper component of the Dirac spinor. In the
specific circumstance of an exponential potential, we have an effective Morse
potential which reveals itself ... | [
{
"created": "Tue, 21 Sep 2004 20:13:25 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"de Castro",
"Antonio S.",
""
],
[
"Hott",
"Marcelo",
""
]
] | The problem of a fermion subject to a general scalar potential in a two-dimensional world for nonzero eigenenergies is mapped into a Sturm-Liouville problem for the upper component of the Dirac spinor. In the specific circumstance of an exponential potential, we have an effective Morse potential which reveals itself as... | 11.193027 | 10.211068 | 12.562188 | 9.945079 | 10.001827 | 9.300157 | 9.772699 | 10.063213 | 9.235217 | 13.56358 | 9.724649 | 10.164755 | 11.275069 | 10.844444 | 10.414721 | 9.998512 | 9.802999 | 10.457884 | 10.280017 | 11.377625 | 10.244813 |
1404.2493 | Dionisio Bazeia | D. Bazeia, L. Losano, M. A. Marques, R. Menezes | Compact Structures in Standard Field Theory | 6 pages, 11 figures; version published in EPL | EPL 107 (2014) 61001 | 10.1209/0295-5075/107/61001 | null | hep-th math-ph math.MP nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the presence of static solutions in models described by real
scalar field in two-dimensional spacetime. After taking advantage of a
procedure introduced sometime ago, we solve intricate nonlinear ordinary
differential equations and illustrate how to find compact structures in models
engendering standar... | [
{
"created": "Wed, 9 Apr 2014 14:00:38 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Apr 2014 20:12:10 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Sep 2014 11:39:04 GMT",
"version": "v3"
}
] | 2014-09-25 | [
[
"Bazeia",
"D.",
""
],
[
"Losano",
"L.",
""
],
[
"Marques",
"M. A.",
""
],
[
"Menezes",
"R.",
""
]
] | We investigate the presence of static solutions in models described by real scalar field in two-dimensional spacetime. After taking advantage of a procedure introduced sometime ago, we solve intricate nonlinear ordinary differential equations and illustrate how to find compact structures in models engendering standard ... | 20.992794 | 12.859961 | 18.927658 | 16.120152 | 14.567687 | 13.718822 | 11.671288 | 14.695482 | 14.782831 | 20.535641 | 15.536016 | 17.41934 | 19.989103 | 18.662577 | 18.139416 | 17.618559 | 18.539248 | 18.138487 | 18.079189 | 19.860098 | 18.132273 |
1202.5993 | Brett D. Altschul | Brett Altschul | Lorentz Violation and the Higgs Mechanism | 15 pages | Phys. Rev. D 86, 045008 (2012) | 10.1103/PhysRevD.86.045008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider scalar quantum electrodynamics in the Higgs phase and in the
presence of Lorentz violation. Spontaneous breaking of the gauge symmetry gives
rise to Lorentz-violating gauge field mass terms. These may cause the
longitudinal mode of the gauge field to propagate superluminally. The theory
may be quantized b... | [
{
"created": "Mon, 27 Feb 2012 16:38:57 GMT",
"version": "v1"
},
{
"created": "Mon, 20 May 2013 15:59:50 GMT",
"version": "v2"
}
] | 2013-05-21 | [
[
"Altschul",
"Brett",
""
]
] | We consider scalar quantum electrodynamics in the Higgs phase and in the presence of Lorentz violation. Spontaneous breaking of the gauge symmetry gives rise to Lorentz-violating gauge field mass terms. These may cause the longitudinal mode of the gauge field to propagate superluminally. The theory may be quantized by ... | 6.388137 | 5.481289 | 5.258324 | 5.393835 | 5.895488 | 6.099923 | 6.078454 | 5.937982 | 5.525878 | 6.546029 | 6.143891 | 6.270954 | 5.770194 | 5.674161 | 6.007479 | 5.650823 | 5.72502 | 6.115296 | 5.654578 | 6.076786 | 5.892799 |
hep-th/9804024 | Simon Dalley | S. Dalley | The Influence of Higher Fock States in Light-Cone Gauge Theories | 4 pages, REVTEX | Phys. Rev. D 58, 087705 (1998) | 10.1103/PhysRevD.58.087705 | CERN-TH/98-114 | hep-th hep-ph | null | In the light-cone Fock state expansion of gauge theories, the influence of
non-valence states may be significant in precision non-perturbative
calculations. In two-dimensional gauge theories, it is shown how these states
modify the behaviour of the light-cone wavefunction in significant ways
relative to endemic choic... | [
{
"created": "Thu, 2 Apr 1998 19:22:56 GMT",
"version": "v1"
}
] | 2016-08-25 | [
[
"Dalley",
"S.",
""
]
] | In the light-cone Fock state expansion of gauge theories, the influence of non-valence states may be significant in precision non-perturbative calculations. In two-dimensional gauge theories, it is shown how these states modify the behaviour of the light-cone wavefunction in significant ways relative to endemic choices... | 15.625665 | 16.903337 | 14.218537 | 12.879779 | 14.902991 | 15.342549 | 15.06587 | 14.768683 | 14.337473 | 13.314105 | 14.592566 | 14.386534 | 12.987721 | 12.993399 | 13.313903 | 14.803467 | 13.700154 | 14.712589 | 13.126247 | 13.817828 | 14.756867 |
hep-th/0404060 | Roland Kirschner | R. Kirschner | Parton interaction in super Yang Mills theory | 20 pages, 1 figure | JHEP 0407 (2004) 064 | 10.1088/1126-6708/2004/07/064 | LU-ITP 2004/12 | hep-th hep-ph | null | We apply the effective action scheme to the leading parton interactions in
${\cal N} = 1$ supersymmetric gauge theory. The effective interaction in the
Bjorken asymptotics at one loop is written in terms of parton superfield
vertices explicitely symmetric with respect to superconformal transformations.
| [
{
"created": "Wed, 7 Apr 2004 08:37:06 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Kirschner",
"R.",
""
]
] | We apply the effective action scheme to the leading parton interactions in ${\cal N} = 1$ supersymmetric gauge theory. The effective interaction in the Bjorken asymptotics at one loop is written in terms of parton superfield vertices explicitely symmetric with respect to superconformal transformations. | 15.761865 | 13.907894 | 12.689094 | 12.777398 | 14.639087 | 14.763177 | 15.162878 | 13.686272 | 12.200754 | 14.64998 | 13.381617 | 14.442174 | 13.786994 | 13.463602 | 12.935141 | 13.608949 | 12.970356 | 13.625937 | 12.9446 | 12.455179 | 13.257656 |
hep-th/0612197 | Pascal Vaudrevange | J.R. Bond, L. Kofman, S. Prokushkin, P.M. Vaudrevange | Roulette Inflation with K\"ahler Moduli and their Axions | Version submitted to Phys.Rev.D. 29 pages, 12 Figures, minor changes | Phys.Rev.D75:123511,2007 | 10.1103/PhysRevD.75.123511 | null | hep-th astro-ph gr-qc hep-ph | null | We study 2-field inflation models based on the ``large-volume'' flux
compactification of type IIB string theory. The role of the inflaton is played
by a K\"ahler modulus \tau corresponding to a 4-cycle volume and its axionic
partner \theta. The freedom associated with the choice of Calabi Yau manifold
and the non-per... | [
{
"created": "Tue, 19 Dec 2006 20:07:15 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Dec 2006 20:49:22 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Bond",
"J. R.",
""
],
[
"Kofman",
"L.",
""
],
[
"Prokushkin",
"S.",
""
],
[
"Vaudrevange",
"P. M.",
""
]
] | We study 2-field inflation models based on the ``large-volume'' flux compactification of type IIB string theory. The role of the inflaton is played by a K\"ahler modulus \tau corresponding to a 4-cycle volume and its axionic partner \theta. The freedom associated with the choice of Calabi Yau manifold and the non-pertu... | 16.585873 | 20.386171 | 18.736465 | 17.295111 | 17.792179 | 18.565451 | 18.409136 | 18.207382 | 17.753059 | 20.544691 | 16.582586 | 16.929348 | 16.586119 | 16.372679 | 16.92239 | 17.194994 | 17.189489 | 16.591837 | 16.014511 | 17.597441 | 16.358818 |
hep-th/0510106 | Yonezawa Nobuhiro | Nobuhiro Yonezawa and Izumi Tsutsui | Inequivalent Quantizations of the N = 3 Calogero model with Scale and
Mirror-S_3 Symmetry | 24 pages, LaTeX | J.Math.Phys. 47 (2006) 012104 | 10.1063/1.2162821 | null | hep-th | null | We study the inequivalent quantizations of the N = 3 Calogero model by
separation of variables, in which the model decomposes into the angular and the
radial parts. Our inequivalent quantizations respect the ` mirror-S_3\rq\
invariance (which realizes the symmetry under the cyclic permutations of the
particles) and t... | [
{
"created": "Thu, 13 Oct 2005 10:55:14 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Nov 2005 07:10:50 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Yonezawa",
"Nobuhiro",
""
],
[
"Tsutsui",
"Izumi",
""
]
] | We study the inequivalent quantizations of the N = 3 Calogero model by separation of variables, in which the model decomposes into the angular and the radial parts. Our inequivalent quantizations respect the ` mirror-S_3\rq\ invariance (which realizes the symmetry under the cyclic permutations of the particles) and the... | 10.822544 | 11.547939 | 11.713826 | 10.65137 | 11.492929 | 11.124744 | 12.072143 | 10.949271 | 10.581791 | 12.133263 | 10.552656 | 11.232328 | 10.859802 | 10.79895 | 10.796103 | 10.603591 | 10.710204 | 10.787119 | 10.623149 | 10.88968 | 10.486714 |
hep-th/0208085 | Arvind Rajaraman | Arvind Rajaraman | Comments on D-branes in flux backgrounds | 15 pages, latex | null | null | null | hep-th | null | We construct supergravity solutions for D-branes in nontrivial flux
backgrounds. We revisit the issue of charge quantization in this framework, and
show that in these backgrounds, charge need not be quantized. We also show in a
particular example that the semiclassical description of branes produces
integral charges.... | [
{
"created": "Mon, 12 Aug 2002 22:18:19 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rajaraman",
"Arvind",
""
]
] | We construct supergravity solutions for D-branes in nontrivial flux backgrounds. We revisit the issue of charge quantization in this framework, and show that in these backgrounds, charge need not be quantized. We also show in a particular example that the semiclassical description of branes produces integral charges. | 12.592788 | 10.057708 | 12.518322 | 11.163171 | 11.259809 | 11.238176 | 9.886157 | 10.474847 | 10.440109 | 14.043098 | 10.479641 | 10.283278 | 12.189577 | 11.098603 | 10.399061 | 10.922369 | 10.682122 | 10.898555 | 11.011082 | 11.85487 | 10.402298 |
1503.06770 | Hajime Otsuka | Hiroyuki Abe, Tatsuo Kobayashi, Hajime Otsuka and Yasufumi Takano | Realistic three-generation models from SO(32) heterotic string theory | 29 pages, Typos corrected, references added, and Sec. 3.3 is added | JHEP 1509 (2015) 056 | 10.1007/JHEP09(2015)056 | WUF-HEP-15-04, EPHOU-15-006 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We search for realistic supersymmetric standard-like models from SO(32)
heterotic string theory on factorizable tori with multiple magnetic fluxes.
Three chiral ganerations of quarks and leptons are derived from the adjoint and
vector representations of SO(12) gauge groups embedded in SO(32) adjoint
representation. M... | [
{
"created": "Mon, 23 Mar 2015 19:09:47 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Sep 2015 15:01:40 GMT",
"version": "v2"
}
] | 2015-09-30 | [
[
"Abe",
"Hiroyuki",
""
],
[
"Kobayashi",
"Tatsuo",
""
],
[
"Otsuka",
"Hajime",
""
],
[
"Takano",
"Yasufumi",
""
]
] | We search for realistic supersymmetric standard-like models from SO(32) heterotic string theory on factorizable tori with multiple magnetic fluxes. Three chiral ganerations of quarks and leptons are derived from the adjoint and vector representations of SO(12) gauge groups embedded in SO(32) adjoint representation. Mas... | 10.036456 | 8.787142 | 9.325725 | 8.612126 | 9.053329 | 8.88692 | 8.028694 | 9.145698 | 9.290288 | 11.038463 | 8.599018 | 8.811999 | 9.566901 | 9.065896 | 9.293432 | 8.638256 | 8.631929 | 9.159296 | 8.761988 | 9.89534 | 9.016201 |
hep-th/0111275 | Nikolaos Mavromatos | Nick E. Mavromatos (King's Coll. London) | String Cosmology | 64 pages latex, 11 eps figures, uses Springer-Verlag book style files | Lect.Notes Phys.592:392-457,2002 | null | KCL-PHYSICS-01; Proceedings of First Aegean Summer School on
Cosmology, Samos (Greece), September 2001 | hep-th gr-qc | null | `Old' String Theory is a theory of one-dimensional extended objects, whose
vibrations correspond to excitations of various target-space field modes
including gravity. In these lectures I will give an introduction to low-energy
Effective Target-Space Actions derived from conformal invariance conditions of
the underlyi... | [
{
"created": "Thu, 29 Nov 2001 16:39:56 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Mavromatos",
"Nick E.",
"",
"King's Coll. London"
]
] | `Old' String Theory is a theory of one-dimensional extended objects, whose vibrations correspond to excitations of various target-space field modes including gravity. In these lectures I will give an introduction to low-energy Effective Target-Space Actions derived from conformal invariance conditions of the underlying... | 14.347355 | 14.648421 | 15.03081 | 14.790689 | 14.570209 | 15.995515 | 15.384211 | 15.010777 | 14.034691 | 15.405569 | 13.987993 | 14.438077 | 14.296645 | 13.867879 | 14.282847 | 14.152609 | 13.544596 | 13.582644 | 14.171933 | 14.151085 | 14.312799 |
1304.7263 | Ira Z. Rothstein | Duff Neill (MIT) and Ira Z. Rothstein (CMU) | Classical Space-Times from the S Matrix | null | null | 10.1016/j.nuclphysb.2013.09.007 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that classical space-times can be derived directly from the S-matrix
for a theory of massive particles coupled to a massless spin two particle. As
an explicit example we derive the Schwarzchild space-time as a series in $G_N$.
At no point of the derivation is any use made of the Einstein-Hilbert action or
the... | [
{
"created": "Fri, 26 Apr 2013 19:42:59 GMT",
"version": "v1"
}
] | 2015-06-15 | [
[
"Neill",
"Duff",
"",
"MIT"
],
[
"Rothstein",
"Ira Z.",
"",
"CMU"
]
] | We show that classical space-times can be derived directly from the S-matrix for a theory of massive particles coupled to a massless spin two particle. As an explicit example we derive the Schwarzchild space-time as a series in $G_N$. At no point of the derivation is any use made of the Einstein-Hilbert action or the E... | 10.057131 | 10.81852 | 10.693926 | 10.403259 | 10.501621 | 10.914195 | 10.507075 | 10.625381 | 9.835144 | 11.534519 | 10.393571 | 10.017226 | 10.09503 | 9.816983 | 10.001653 | 9.745472 | 9.971911 | 9.881788 | 9.78911 | 9.893481 | 9.755619 |
0712.3324 | Raphael Bousso | Raphael Bousso, Ben Freivogel, and I-Sheng Yang | Boltzmann babies in the proper time measure | 15 pages, 2 figures, v3 PRD format minor editing addressing reviewers
comment | Phys.Rev.D77:103514,2008 | 10.1103/PhysRevD.77.103514 | null | hep-th astro-ph gr-qc | null | After commenting briefly on the role of the typicality assumption in science,
we advocate a phenomenological approach to the cosmological measure problem.
Like any other theory, a measure should be simple, general, well-defined, and
consistent with observation. This allows us to proceed by elimination. As an
example,... | [
{
"created": "Thu, 20 Dec 2007 19:52:48 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Jan 2008 00:45:19 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Apr 2008 18:33:54 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Bousso",
"Raphael",
""
],
[
"Freivogel",
"Ben",
""
],
[
"Yang",
"I-Sheng",
""
]
] | After commenting briefly on the role of the typicality assumption in science, we advocate a phenomenological approach to the cosmological measure problem. Like any other theory, a measure should be simple, general, well-defined, and consistent with observation. This allows us to proceed by elimination. As an example, w... | 11.187444 | 10.397482 | 11.274306 | 10.298192 | 10.54405 | 10.428115 | 11.296644 | 9.929562 | 10.788466 | 12.506189 | 10.46862 | 10.013469 | 10.627486 | 10.047489 | 9.987284 | 9.497763 | 9.958848 | 9.655409 | 9.952449 | 10.610279 | 9.501023 |
hep-th/0311103 | Karl Landsteiner | K. Landsteiner, C. I. Lazaroiu, R. Tatar | Puzzles for Matrix Models of Chiral Field Theories | Contribution to the proceedings of the 36th International Symposium
Ahrenshoop, Berlin, August 26-30, 2003; 6 Pages | Fortschr.Phys.52:590-595,2004 | 10.1002/prop.200310149 | IFT-UAM/CSIC-03-44, MAD-TH-03-3, LBNL-54038 | hep-th | null | We summarize the field-theory/matrix model correspondence for a chiral N=1
model with matter in the adjoint, antisymmetric and conjugate symmetric
representations as well as eight fundamentals to cancel the chiral anomaly. The
associated holomorphic matrix model is consistent only for two fundamental
fields, which re... | [
{
"created": "Wed, 12 Nov 2003 14:40:37 GMT",
"version": "v1"
},
{
"created": "Mon, 10 May 2004 14:05:49 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Landsteiner",
"K.",
""
],
[
"Lazaroiu",
"C. I.",
""
],
[
"Tatar",
"R.",
""
]
] | We summarize the field-theory/matrix model correspondence for a chiral N=1 model with matter in the adjoint, antisymmetric and conjugate symmetric representations as well as eight fundamentals to cancel the chiral anomaly. The associated holomorphic matrix model is consistent only for two fundamental fields, which requ... | 14.344998 | 13.577298 | 16.564434 | 12.451122 | 14.855083 | 13.389579 | 13.334367 | 12.180347 | 12.68466 | 17.271408 | 13.080848 | 13.120002 | 15.050257 | 13.148396 | 13.162431 | 13.975223 | 13.363223 | 13.15375 | 13.681657 | 14.489023 | 12.779883 |
hep-th/9211044 | hector DE Vega | D. Boyanovsky and H. J. de Vega | Quantum Rolling Down out of Equilibrium | 33 pages, Latex,LPTHE-PAR 92-33 PITT 92-06 | Phys.Rev. D47 (1993) 2343-2355 | 10.1103/PhysRevD.47.2343 | null | hep-th | null | In a scalar field theory, when the tree level potential admits broken
symmetry ground states, the quantum corrections to the static effective
potential are complex. (The imaginary part is a consequence of an instability
towards phase separation and the static effective potential is not a relevant
quantity for underst... | [
{
"created": "Tue, 10 Nov 1992 17:44:27 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Boyanovsky",
"D.",
""
],
[
"de Vega",
"H. J.",
""
]
] | In a scalar field theory, when the tree level potential admits broken symmetry ground states, the quantum corrections to the static effective potential are complex. (The imaginary part is a consequence of an instability towards phase separation and the static effective potential is not a relevant quantity for understan... | 12.602681 | 13.130032 | 12.148246 | 11.78492 | 13.195709 | 12.803059 | 13.062668 | 12.856282 | 11.79357 | 11.163198 | 12.517766 | 11.8207 | 12.085586 | 11.825294 | 11.711919 | 11.868617 | 11.935683 | 11.91726 | 11.334538 | 11.210746 | 12.329577 |
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