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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1309.1285 | Diederik Roest | Diederik Roest | Universality classes of inflation | 5 pages, 1 figure; v2: minor clarifications, refs added, JCAP version | JCAP 01 (2014) 007 | 10.1088/1475-7516/2014/01/007 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate all single-field, slow-roll inflationary models whose
slow-roll parameters scale as 1/N in the limit of a large number of e-folds N.
We proof that all such models belong to two universality classes, characterised
by a single parameter. One class contains small field models like hilltop
inflation, while... | [
{
"created": "Thu, 5 Sep 2013 09:07:38 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Dec 2013 15:52:46 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Roest",
"Diederik",
""
]
] | We investigate all single-field, slow-roll inflationary models whose slow-roll parameters scale as 1/N in the limit of a large number of e-folds N. We proof that all such models belong to two universality classes, characterised by a single parameter. One class contains small field models like hilltop inflation, while t... | 6.594547 | 6.191249 | 6.50154 | 5.979364 | 6.406497 | 6.079878 | 6.785987 | 5.81537 | 5.983528 | 6.525815 | 5.983646 | 6.378776 | 6.326006 | 6.277234 | 6.154729 | 6.164063 | 6.14102 | 6.288815 | 6.192978 | 6.265495 | 6.06211 |
0812.3551 | Paul Koerber | Claudio Caviezel, Paul Koerber, Simon Kors, Dieter Lust, Timm Wrase
and Marco Zagermann | On the Cosmology of Type IIA Compactifications on SU(3)-structure
Manifolds | LaTeX, 22 pages plus appendix; v2: references added, minor changes | JHEP 0904:010,2009 | 10.1088/1126-6708/2009/04/010 | MPP-2008-165, LMU-ASC 64/08, ESI-2105 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study cosmological properties of type IIA compactifications on
orientifolds of SU(3)-structure manifolds with non-vanishing geometric flux.
These compactifications give rise to effective 4D N=1 supergravity theories
that do not fall under some recently-proven no-go theorems against de Sitter
vacua and slow-roll in... | [
{
"created": "Thu, 18 Dec 2008 20:51:15 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Jan 2009 13:15:33 GMT",
"version": "v2"
}
] | 2009-04-17 | [
[
"Caviezel",
"Claudio",
""
],
[
"Koerber",
"Paul",
""
],
[
"Kors",
"Simon",
""
],
[
"Lust",
"Dieter",
""
],
[
"Wrase",
"Timm",
""
],
[
"Zagermann",
"Marco",
""
]
] | We study cosmological properties of type IIA compactifications on orientifolds of SU(3)-structure manifolds with non-vanishing geometric flux. These compactifications give rise to effective 4D N=1 supergravity theories that do not fall under some recently-proven no-go theorems against de Sitter vacua and slow-roll infl... | 9.057284 | 8.655512 | 9.904574 | 8.293412 | 8.358762 | 8.019365 | 8.524277 | 7.933161 | 7.858898 | 10.55985 | 7.895512 | 8.346897 | 8.900151 | 8.141517 | 8.115393 | 8.270482 | 8.230382 | 7.847246 | 8.129286 | 8.973488 | 8.047565 |
hep-th/9809155 | Manuel Calixto | V. Aldaya, M. Calixto and J.M. Cervero | Vacuum Radiation in Conformally Invariant Quantum Field Theory | Latex, 3 pages with no figures. Uses style file sprocl.sty.
Contribution to the 5th International Wigner Symposium, Viena (Austria)
August 1997. World Scientific, Singapore, Eds. P. Kasperkovitz and D. Grau
(1998) ISBN: 981-02-3464-3, pags. 201-203 | null | null | null | hep-th | null | Although the whole conformal group $SO(4,2)$ can be considered as a symmetry
in a classical massless field theory, the subgroup of special conformal
transformations (SCT), usually related to transitions to uniformly accelerated
frames, causes vacuum radiation in the corresponding quantum field theory, in
analogy to t... | [
{
"created": "Mon, 21 Sep 1998 16:08:05 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Aldaya",
"V.",
""
],
[
"Calixto",
"M.",
""
],
[
"Cervero",
"J. M.",
""
]
] | Although the whole conformal group $SO(4,2)$ can be considered as a symmetry in a classical massless field theory, the subgroup of special conformal transformations (SCT), usually related to transitions to uniformly accelerated frames, causes vacuum radiation in the corresponding quantum field theory, in analogy to the... | 12.982081 | 13.627274 | 12.42372 | 11.431735 | 13.69203 | 13.290744 | 12.302728 | 12.520097 | 12.391225 | 13.502725 | 13.182489 | 11.684636 | 12.041166 | 12.569489 | 12.09528 | 11.513501 | 11.602759 | 11.760672 | 11.974947 | 11.806411 | 13.065777 |
1407.7054 | Athanasios Chatzistavrakidis | Athanasios Chatzistavrakidis | Dynamical phase space from a SO(d,d) matrix model | 6 pages; clarifying changes and references added; published in the
Rapid Communications section of Phys. Rev. D | Phys. Rev. D 90, (2014) 121502(R) | 10.1103/PhysRevD.90.121502 | ITP-UH-11/14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that a matrix model with SO(d,d) global symmetry is derived from
a generalized Yang-Mills theory on the standard Courant algebroid. This model
keeps all the positive features of the well-studied type IIB matrix model, and
it has many additional welcome properties. We show that it does not only
capture the... | [
{
"created": "Fri, 25 Jul 2014 20:48:40 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Feb 2015 16:23:57 GMT",
"version": "v2"
}
] | 2015-02-03 | [
[
"Chatzistavrakidis",
"Athanasios",
""
]
] | It is shown that a matrix model with SO(d,d) global symmetry is derived from a generalized Yang-Mills theory on the standard Courant algebroid. This model keeps all the positive features of the well-studied type IIB matrix model, and it has many additional welcome properties. We show that it does not only capture the d... | 9.881042 | 9.275367 | 9.943725 | 9.030576 | 9.313131 | 9.642241 | 9.618039 | 9.233887 | 8.959176 | 10.165894 | 9.134638 | 9.073222 | 9.367466 | 9.08073 | 9.239025 | 9.146068 | 9.250844 | 9.318575 | 8.913857 | 9.029822 | 9.241528 |
1502.05138 | Junyu Liu | Junyu Liu, Yi Wang, Siyi Zhou | Inflation with Massive Vector Fields | 18 pages, 2 figures | JCAP 1508 (2015) 033 | 10.1088/1475-7516/2015/08/033 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the coupling between the inflaton and massive vector fields.
All renormalizable couplings with shift symmetry of the inflaton are
considered. The massive vector can be decomposed into a scalar mode and a
divergence-free vector mode. We show that the former naturally interacts with
the inflaton and the ... | [
{
"created": "Wed, 18 Feb 2015 07:04:24 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Feb 2015 09:26:49 GMT",
"version": "v2"
}
] | 2015-08-24 | [
[
"Liu",
"Junyu",
""
],
[
"Wang",
"Yi",
""
],
[
"Zhou",
"Siyi",
""
]
] | We investigate the coupling between the inflaton and massive vector fields. All renormalizable couplings with shift symmetry of the inflaton are considered. The massive vector can be decomposed into a scalar mode and a divergence-free vector mode. We show that the former naturally interacts with the inflaton and the la... | 7.290032 | 7.137948 | 6.669882 | 6.80956 | 7.542473 | 7.033363 | 6.614588 | 6.540158 | 7.096891 | 7.390506 | 6.645779 | 7.262536 | 6.966302 | 6.807756 | 6.844538 | 7.253948 | 6.781334 | 6.912106 | 7.022599 | 6.721925 | 6.750926 |
1910.04766 | Jaroslav Trnka | Karol Kampf, Jiri Novotny, Mikhail Shifman, Jaroslav Trnka | New Soft Theorems for Goldstone Boson Amplitudes | 5 pages, 2 figures | Phys. Rev. Lett. 124, 111601 (2020) | 10.1103/PhysRevLett.124.111601 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this letter we discuss new soft theorems for the Goldstone boson
amplitudes with non-vanishing soft limits. The standard argument is that the
non-linearly realized shift symmetry leads to the vanishing of scattering
amplitudes in the soft limit, known as the Alder zero. This statement involves
certain assumptions ... | [
{
"created": "Thu, 10 Oct 2019 18:00:01 GMT",
"version": "v1"
}
] | 2020-03-25 | [
[
"Kampf",
"Karol",
""
],
[
"Novotny",
"Jiri",
""
],
[
"Shifman",
"Mikhail",
""
],
[
"Trnka",
"Jaroslav",
""
]
] | In this letter we discuss new soft theorems for the Goldstone boson amplitudes with non-vanishing soft limits. The standard argument is that the non-linearly realized shift symmetry leads to the vanishing of scattering amplitudes in the soft limit, known as the Alder zero. This statement involves certain assumptions of... | 11.171116 | 12.186768 | 10.532573 | 10.832307 | 11.207451 | 10.978391 | 11.087382 | 10.917859 | 11.019593 | 11.045113 | 10.295725 | 10.12412 | 10.085637 | 10.042957 | 10.173635 | 9.951483 | 9.849209 | 10.137704 | 9.77163 | 10.021607 | 9.638398 |
0708.2471 | J. C. Wallet | Jean-Christophe Wallet | Noncommutative Induced Gauge Theories on Moyal Spaces | 24 pages, 6 figures. Talk given at the "International Conference on
Noncommutative Geometry and Physics", April 2007, Orsay (France). References
updated. To appear in J. Phys. Conf. Ser | J.Phys.Conf.Ser.103:012007,2008 | 10.1088/1742-6596/103/1/012007 | null | hep-th math-ph math.MP | null | Noncommutative field theories on Moyal spaces can be conveniently handled
within a framework of noncommutative geometry. Several renormalisable matter
field theories that are now identified are briefly reviewed. The construction
of renormalisable gauge theories on these noncommutative Moyal spaces, which
remains so f... | [
{
"created": "Sat, 18 Aug 2007 08:05:54 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Sep 2007 16:29:41 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Wallet",
"Jean-Christophe",
""
]
] | Noncommutative field theories on Moyal spaces can be conveniently handled within a framework of noncommutative geometry. Several renormalisable matter field theories that are now identified are briefly reviewed. The construction of renormalisable gauge theories on these noncommutative Moyal spaces, which remains so far... | 6.526678 | 7.510667 | 7.572662 | 7.079216 | 7.236506 | 7.303779 | 7.04683 | 7.136282 | 7.088413 | 8.851665 | 7.500077 | 6.908976 | 7.314013 | 7.072998 | 6.943968 | 6.837001 | 7.030771 | 7.054963 | 7.057282 | 7.284057 | 6.868407 |
1709.01954 | Nick R.D. Zhu | Jean-Emile Bourgine, Masayuki Fukuda, Yutaka Matsuo, Rui-Dong Zhu | Reflection states in Ding-Iohara-Miki algebra and brane-web for D-type
quiver | 27 pages, 11 figures. Details of translation in terms of IKV refined
topological vertex added in the second version | J. High Energ. Phys. (2017) 2017: 15 | 10.1007/JHEP12(2017)015 | KIAS-Q17026; UT-17-30 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Reflection states are introduced in the vertical and horizontal modules of
the Ding-Iohara-Miki (DIM) algebra (quantum toroidal $\mathfrak{gl}_1$). Webs
of DIM representations are in correspondence with $(p,q)$-web diagrams of type
IIB string theory, under the identification of the algebraic intertwiner of
Awata, Fei... | [
{
"created": "Wed, 6 Sep 2017 18:12:28 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Oct 2017 13:33:10 GMT",
"version": "v2"
}
] | 2017-12-08 | [
[
"Bourgine",
"Jean-Emile",
""
],
[
"Fukuda",
"Masayuki",
""
],
[
"Matsuo",
"Yutaka",
""
],
[
"Zhu",
"Rui-Dong",
""
]
] | Reflection states are introduced in the vertical and horizontal modules of the Ding-Iohara-Miki (DIM) algebra (quantum toroidal $\mathfrak{gl}_1$). Webs of DIM representations are in correspondence with $(p,q)$-web diagrams of type IIB string theory, under the identification of the algebraic intertwiner of Awata, Feigi... | 8.35663 | 7.885107 | 12.028424 | 7.644302 | 8.61539 | 7.616592 | 7.990226 | 7.578652 | 7.749414 | 13.786244 | 7.524125 | 7.588529 | 8.784806 | 7.665761 | 7.705073 | 7.697536 | 7.855987 | 7.359587 | 7.63807 | 8.224029 | 7.638697 |
2107.09077 | Mohammad Akhond | Mohammad Akhond, Federico Carta | Magnetic quivers from brane webs with O7$^+$-planes | 21 pages | JHEP10(2021)014 | 10.1007/JHEP10(2021)014 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We consider the Higgs branch of 5d fixed points engineered using brane webs
with an O7$^+$-plane. We use the brane construction to propose a set of rules
to extract the corresponding magnetic quivers. Such magnetic quivers are
generically framed non-simply-laced quivers containing unitary as well as
special unitary g... | [
{
"created": "Mon, 19 Jul 2021 18:00:04 GMT",
"version": "v1"
}
] | 2022-01-05 | [
[
"Akhond",
"Mohammad",
""
],
[
"Carta",
"Federico",
""
]
] | We consider the Higgs branch of 5d fixed points engineered using brane webs with an O7$^+$-plane. We use the brane construction to propose a set of rules to extract the corresponding magnetic quivers. Such magnetic quivers are generically framed non-simply-laced quivers containing unitary as well as special unitary gau... | 6.781299 | 5.764494 | 8.712042 | 5.947471 | 6.021242 | 5.89406 | 5.737551 | 5.610742 | 5.728512 | 9.091318 | 5.641253 | 6.217007 | 7.400647 | 6.464316 | 6.511249 | 6.112287 | 6.356464 | 6.362528 | 6.359953 | 6.948613 | 6.122 |
hep-th/0411032 | Ignatios Antoniadis | I. Antoniadis and S. Dimopoulos | Splitting Supersymmetry in String Theory | 27 pages, 3 figures | Nucl.Phys. B715 (2005) 120-140 | 10.1016/j.nuclphysb.2005.03.005 | CERN-PH-TH/2004-217 | hep-th hep-ph | null | We point out that type I string theory in the presence of internal magnetic
fields provides a concrete realization of split supersymmetry. To lowest order,
gauginos are massless while squarks and sleptons are superheavy. We build such
realistic U(3)xU(2)xU(1) models on stacks of magnetized D9-branes. Though not
unifi... | [
{
"created": "Tue, 2 Nov 2004 17:49:01 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Antoniadis",
"I.",
""
],
[
"Dimopoulos",
"S.",
""
]
] | We point out that type I string theory in the presence of internal magnetic fields provides a concrete realization of split supersymmetry. To lowest order, gauginos are massless while squarks and sleptons are superheavy. We build such realistic U(3)xU(2)xU(1) models on stacks of magnetized D9-branes. Though not unified... | 9.290467 | 9.942741 | 9.163575 | 8.820954 | 9.821738 | 9.982924 | 10.410976 | 9.195718 | 8.448272 | 9.539321 | 8.822893 | 9.261344 | 8.866283 | 8.688471 | 9.335445 | 9.335789 | 9.326881 | 9.197472 | 8.976644 | 8.995381 | 9.128179 |
0709.1932 | Andrei Micu | Sebastien Gurrieri, Andre Lukas, Andrei Micu | Heterotic String Compactifications on Half-flat Manifolds II | 31 pages | JHEP 0712:081,2007 | 10.1088/1126-6708/2007/12/081 | null | hep-th | null | In this paper, we continue the analysis of heterotic string compactifications
on half-flat mirror manifolds by including the 10-dimensional gauge fields. It
is argued, that the heterotic Bianchi identity is solved by a variant of the
standard embedding. Then, the resulting gauge group in four dimensions is still
E6 d... | [
{
"created": "Wed, 12 Sep 2007 17:08:03 GMT",
"version": "v1"
}
] | 2009-11-18 | [
[
"Gurrieri",
"Sebastien",
""
],
[
"Lukas",
"Andre",
""
],
[
"Micu",
"Andrei",
""
]
] | In this paper, we continue the analysis of heterotic string compactifications on half-flat mirror manifolds by including the 10-dimensional gauge fields. It is argued, that the heterotic Bianchi identity is solved by a variant of the standard embedding. Then, the resulting gauge group in four dimensions is still E6 des... | 9.896851 | 8.534185 | 11.802705 | 9.445759 | 9.422342 | 8.29286 | 9.32739 | 8.502069 | 9.003488 | 12.62618 | 9.09309 | 9.012388 | 9.396255 | 9.182549 | 9.198064 | 9.479971 | 8.898306 | 9.499119 | 9.291063 | 9.684843 | 8.904454 |
hep-th/0703289 | Anke Knauf | Rhiannon Gwyn, Anke Knauf | Conifolds and Geometric Transitions | 37 pages, v3: accepted for publication in Reviews of Modern Physics | Rev.Mod.Phys.8012:1419-1453,2008 | 10.1103/RevModPhys.80.1419 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Conifold geometries have recieved a lot of attention in string theory and
string-inspired cosmology recently, in particular the Klebanov-Strassler
background that is known as the "warped throat". It is our intention in this
article to give a pedagogical explanation for the singularity resolution in
this geometry and ... | [
{
"created": "Fri, 30 Mar 2007 17:10:53 GMT",
"version": "v1"
},
{
"created": "Wed, 9 May 2007 22:12:52 GMT",
"version": "v2"
},
{
"created": "Thu, 23 Oct 2008 19:54:55 GMT",
"version": "v3"
}
] | 2008-12-18 | [
[
"Gwyn",
"Rhiannon",
""
],
[
"Knauf",
"Anke",
""
]
] | Conifold geometries have recieved a lot of attention in string theory and string-inspired cosmology recently, in particular the Klebanov-Strassler background that is known as the "warped throat". It is our intention in this article to give a pedagogical explanation for the singularity resolution in this geometry and em... | 9.650953 | 9.847307 | 12.169219 | 9.620982 | 10.07678 | 9.760291 | 10.527557 | 9.341341 | 9.606697 | 12.610655 | 9.092673 | 9.143781 | 9.482325 | 9.054664 | 9.064206 | 9.257781 | 9.296957 | 9.132247 | 9.133299 | 9.613055 | 9.38755 |
1311.1257 | Ashoke Sen | Roji Pius, Arnab Rudra and Ashoke Sen | Mass Renormalization in String Theory: Special States | LaTeX file, 28 pages; v2: clarifications added; v3: minor changes | null | 10.1007/JHEP07(2014)058 | DAMTP-2013-62, HRI/ST/1306 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | String theory gives a well defined procedure for computing the S-matrix of
BPS or a class of massless states, but similar calculation for general massive
states is plagued with difficulties due to mass renormalization effect. In this
paper we describe a procedure for computing the renormalized masses and
S-matrix ele... | [
{
"created": "Wed, 6 Nov 2013 00:26:00 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Dec 2013 03:15:09 GMT",
"version": "v2"
},
{
"created": "Wed, 14 May 2014 21:18:00 GMT",
"version": "v3"
}
] | 2015-06-17 | [
[
"Pius",
"Roji",
""
],
[
"Rudra",
"Arnab",
""
],
[
"Sen",
"Ashoke",
""
]
] | String theory gives a well defined procedure for computing the S-matrix of BPS or a class of massless states, but similar calculation for general massive states is plagued with difficulties due to mass renormalization effect. In this paper we describe a procedure for computing the renormalized masses and S-matrix eleme... | 7.042817 | 6.672782 | 7.488697 | 6.586536 | 6.757153 | 6.745027 | 7.002318 | 6.889365 | 6.335656 | 7.477672 | 6.506948 | 6.694405 | 7.164932 | 6.926028 | 6.631017 | 6.817929 | 6.658862 | 6.701378 | 6.733812 | 7.239067 | 6.599171 |
1509.00953 | Takahiro Terada | Sergei V. Ketov and Takahiro Terada | Single-Superfield Helical-Phase Inflation | 11 pages, 3 figures (published version); more explanations and
references added, typos corrected, and figures improved | Phys. Lett. B 752, (2016), 108 | 10.1016/j.physletb.2015.11.039 | UT-15-33, DESY 15-163, IPMU 15-0143 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Large-field inflation in supergravity requires the approximate global
symmetry needed to protect flatness of the scalar potential. In helical-phase
inflation, the U(1) symmetry of the Kahler potential is assumed, the phase part
of the complex scalar of a chiral superfield plays the role of inflaton, and
the radial pa... | [
{
"created": "Thu, 3 Sep 2015 06:20:38 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Nov 2015 15:42:28 GMT",
"version": "v2"
}
] | 2015-11-24 | [
[
"Ketov",
"Sergei V.",
""
],
[
"Terada",
"Takahiro",
""
]
] | Large-field inflation in supergravity requires the approximate global symmetry needed to protect flatness of the scalar potential. In helical-phase inflation, the U(1) symmetry of the Kahler potential is assumed, the phase part of the complex scalar of a chiral superfield plays the role of inflaton, and the radial part... | 8.912598 | 9.035628 | 9.027224 | 8.33451 | 8.569356 | 8.52259 | 8.730692 | 8.282737 | 8.900213 | 9.537455 | 8.594825 | 8.382119 | 8.276832 | 7.924687 | 8.108655 | 8.183789 | 8.439414 | 8.231577 | 8.325928 | 7.887991 | 8.537886 |
1305.6048 | Melita Mnatsakanova | K.V. Antipin, M.N. Mnatsakanova and Yu.S. Vernov | Haag's Theorem in the Theories with Non-physical Particles | null | Int.J.Mod.Phys. A28 (2013) 1350076 | 10.1142/S0217751X13500760 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Haag's theorem is extended to the case of regular representations of the
canonical commutation relations in a non-degenerate indefinite inner product
space.
| [
{
"created": "Sun, 26 May 2013 18:42:19 GMT",
"version": "v1"
}
] | 2013-10-01 | [
[
"Antipin",
"K. V.",
""
],
[
"Mnatsakanova",
"M. N.",
""
],
[
"Vernov",
"Yu. S.",
""
]
] | Haag's theorem is extended to the case of regular representations of the canonical commutation relations in a non-degenerate indefinite inner product space. | 13.5033 | 7.877607 | 7.969166 | 6.812332 | 8.899163 | 8.257559 | 8.038447 | 8.554273 | 8.057303 | 6.251772 | 6.576705 | 7.184565 | 7.452279 | 7.983827 | 7.250093 | 7.028604 | 7.911729 | 7.970599 | 7.769781 | 7.830699 | 8.385495 |
1705.07769 | Azat Gainutdinov | Jonathan Bellet\^ete, Azat M. Gainutdinov, Jesper L. Jacobsen, Hubert
Saleur, Romain Vasseur | On the correspondence between boundary and bulk lattice models and
(logarithmic) conformal field theories | v2: 63 pp, few typos fixed, the final version in a special issue of J
Phys A | J. Phys A: Math. Theor. 50 (2017) 484002 | 10.1088/1751-8121/aa902b | LPTENS/17/11, ZMP-HH/17-16, Hamburger Beitrage zur Mathematik 659 | hep-th cond-mat.stat-mech math-ph math.MP math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The relationship between bulk and boundary properties is one of the founding
features of (Rational) Conformal Field Theory. Our goal in this paper is to
explore the possibility of having an equivalent relationship in the context of
lattice models. We focus on models based on the Temperley-Lieb algebra, and use
the co... | [
{
"created": "Mon, 22 May 2017 14:26:22 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Sep 2017 11:36:38 GMT",
"version": "v2"
}
] | 2022-11-29 | [
[
"Belletête",
"Jonathan",
""
],
[
"Gainutdinov",
"Azat M.",
""
],
[
"Jacobsen",
"Jesper L.",
""
],
[
"Saleur",
"Hubert",
""
],
[
"Vasseur",
"Romain",
""
]
] | The relationship between bulk and boundary properties is one of the founding features of (Rational) Conformal Field Theory. Our goal in this paper is to explore the possibility of having an equivalent relationship in the context of lattice models. We focus on models based on the Temperley-Lieb algebra, and use the conc... | 7.783974 | 9.541477 | 9.510408 | 8.089528 | 9.011082 | 8.673263 | 8.712294 | 8.27178 | 8.382201 | 10.157336 | 8.198846 | 7.935163 | 7.978588 | 7.722569 | 7.860141 | 7.772267 | 7.849987 | 7.805286 | 7.662243 | 7.815977 | 7.692227 |
hep-th/0311181 | Masaki Shigemori | Ken Intriligator, Per Kraus, Anton V. Ryzhov, Masaki Shigemori and
Cumrun Vafa | On Low Rank Classical Groups in String Theory, Gauge Theory and Matrix
Models | 41 pages, 1 table, harvmac. v2: minor corrections and references
added | Nucl.Phys.B682:45-82,2004 | 10.1016/j.nuclphysb.2003.12.030 | BRX TH-525, HUTP-03/A073, UCLA-03-TEP-29, UCSD-PTH-03-14 | hep-th | null | We consider N=1 supersymmetric U(N), SO(N), and Sp(N) gauge theories, with
two-index tensor matter and added tree-level superpotential, for general
breaking patterns of the gauge group. By considering the string theory
realization and geometric transitions, we clarify when glueball superfields
should be included and ... | [
{
"created": "Thu, 20 Nov 2003 17:52:59 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Dec 2003 03:03:43 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Intriligator",
"Ken",
""
],
[
"Kraus",
"Per",
""
],
[
"Ryzhov",
"Anton V.",
""
],
[
"Shigemori",
"Masaki",
""
],
[
"Vafa",
"Cumrun",
""
]
] | We consider N=1 supersymmetric U(N), SO(N), and Sp(N) gauge theories, with two-index tensor matter and added tree-level superpotential, for general breaking patterns of the gauge group. By considering the string theory realization and geometric transitions, we clarify when glueball superfields should be included and ex... | 11.172628 | 11.032714 | 12.198285 | 10.798484 | 10.45623 | 10.69871 | 11.008283 | 10.618942 | 10.396054 | 12.664136 | 10.371572 | 10.127325 | 11.719417 | 10.818925 | 10.287801 | 10.513871 | 10.40811 | 10.608901 | 10.69682 | 11.621593 | 10.660692 |
2104.03708 | Philip D. Mannheim | Philip D. Mannheim | Antilinear Symmetry and the Ghost Problem in Quantum Field Theory | 17 pages. To appear in the Proceedings of Virtual seminar series on
Pseudo-Hermitian Hamiltonians in Quantum Physics | null | null | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The recognition that the eigenvalues of a non-Hermitian Hamiltonian could all
be real if the Hamiltonian had an antilinear symmetry such as $PT$ stimulated
new insight into the underlying structure of quantum mechanics. Specifically,
it lead to the realization that Hilbert space could be richer than the
established D... | [
{
"created": "Thu, 8 Apr 2021 11:55:49 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Aug 2021 21:34:38 GMT",
"version": "v2"
}
] | 2021-08-13 | [
[
"Mannheim",
"Philip D.",
""
]
] | The recognition that the eigenvalues of a non-Hermitian Hamiltonian could all be real if the Hamiltonian had an antilinear symmetry such as $PT$ stimulated new insight into the underlying structure of quantum mechanics. Specifically, it lead to the realization that Hilbert space could be richer than the established Dir... | 7.985421 | 7.470739 | 9.286393 | 7.757729 | 8.372572 | 7.991835 | 8.176842 | 8.379786 | 8.200497 | 9.145272 | 8.202166 | 8.198072 | 8.081232 | 7.795627 | 7.827424 | 7.903329 | 8.073193 | 8.148008 | 8.050199 | 8.190767 | 7.895638 |
1711.09314 | James Edwards Dr | James P. Edwards and Olindo Corradini | Worldline colour fields and non-Abelian quantum field theory | 10 pages. To appear in Proceedings of the 6th International
Conference on New Frontiers in Physics (ICNFP 2017), published by European
Physical Journal Web of Conferences | null | 10.1051/epjconf/201818202038 | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the worldline approach to non-Abelian field theory the colour degrees of
freedom of the coupling to the gauge potential can be incorporated using
worldline "colour" fields. The colour fields generate Wilson loop interactions
whilst Chern-Simons terms project onto an irreducible representation of the
gauge group. W... | [
{
"created": "Sun, 26 Nov 2017 00:36:06 GMT",
"version": "v1"
}
] | 2018-08-29 | [
[
"Edwards",
"James P.",
""
],
[
"Corradini",
"Olindo",
""
]
] | In the worldline approach to non-Abelian field theory the colour degrees of freedom of the coupling to the gauge potential can be incorporated using worldline "colour" fields. The colour fields generate Wilson loop interactions whilst Chern-Simons terms project onto an irreducible representation of the gauge group. We ... | 16.708212 | 13.940873 | 15.717444 | 13.506913 | 13.769304 | 13.573346 | 14.641711 | 14.558711 | 13.855324 | 16.338316 | 14.746647 | 14.375786 | 13.870598 | 13.591556 | 13.961236 | 14.787649 | 14.421498 | 14.029363 | 13.894451 | 14.832144 | 14.716792 |
1702.06489 | Carlo Maccaferri | Pier Vittorio Larocca, Carlo Maccaferri | BCFT and OSFT moduli: an exact perturbative comparison | 26+5 pages, 10 figures V2: minor improvements, published version | Eur. Phys. J. C (2017) 77:806 | 10.1140/epjc/s10052-017-5379-3 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Starting from the pseudo-${\cal B}_0$ gauge solution for marginal
deformations in OSFT, we analytically compute the relation between the
perturbative deformation parameter $\tilde\lambda$ in the solution and the BCFT
marginal parameter $\lambda$, up to fifth order, by evaluating the Ellwood
invariants. We observe tha... | [
{
"created": "Tue, 21 Feb 2017 17:39:06 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Nov 2017 23:35:08 GMT",
"version": "v2"
}
] | 2017-11-30 | [
[
"Larocca",
"Pier Vittorio",
""
],
[
"Maccaferri",
"Carlo",
""
]
] | Starting from the pseudo-${\cal B}_0$ gauge solution for marginal deformations in OSFT, we analytically compute the relation between the perturbative deformation parameter $\tilde\lambda$ in the solution and the BCFT marginal parameter $\lambda$, up to fifth order, by evaluating the Ellwood invariants. We observe that ... | 13.385024 | 13.76436 | 14.627398 | 13.445253 | 13.06597 | 13.023197 | 12.372892 | 13.411122 | 14.906513 | 17.309706 | 11.800317 | 12.927434 | 14.086846 | 12.656234 | 12.872399 | 12.900592 | 12.910601 | 13.180136 | 13.277303 | 13.868299 | 12.921607 |
1706.02622 | Jesus Anero | Enrique Alvarez, Jesus Anero and Raquel Santos-Garcia | One-loop divergences in first order Einstein-Hilbert gravity | Some misprints have been correct | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One-loop counterterms are computed in the first order formalism for the
Einstein-Hilbert action with a minimally coupled scalar field using the
background field method and the heat kernel technique. The {\em off-shell}
divergent piece in the harmonic gauge is {\em exactly} the same as the one
first found by 't Hooft ... | [
{
"created": "Thu, 8 Jun 2017 14:53:08 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Jun 2017 14:23:12 GMT",
"version": "v2"
},
{
"created": "Thu, 22 Jun 2017 15:24:51 GMT",
"version": "v3"
},
{
"created": "Tue, 11 Jul 2017 12:36:03 GMT",
"version": "v4"
},
{
"cre... | 2021-09-14 | [
[
"Alvarez",
"Enrique",
""
],
[
"Anero",
"Jesus",
""
],
[
"Santos-Garcia",
"Raquel",
""
]
] | One-loop counterterms are computed in the first order formalism for the Einstein-Hilbert action with a minimally coupled scalar field using the background field method and the heat kernel technique. The {\em off-shell} divergent piece in the harmonic gauge is {\em exactly} the same as the one first found by 't Hooft an... | 7.137451 | 6.017115 | 6.270708 | 5.678043 | 6.554463 | 6.08755 | 5.878383 | 6.029521 | 6.150738 | 6.592693 | 6.051705 | 5.73833 | 5.869465 | 5.746935 | 5.743127 | 5.689438 | 5.551043 | 5.628293 | 5.796464 | 5.619559 | 5.940526 |
hep-th/9411226 | Denjoe O'Connor | M.A. van Eijck, Denjoe O'Connor and C.R. Stephens | Critical Temperature and Amplitude Ratios from a Finite-Temperature
Renormalization Group | 14 pages of LaTeX. Postscript figures available upon request form
denjoe@stp.dias.ie | Int.J.Mod.Phys. A10 (1995) 3343-3358 | 10.1142/S0217751X95001613 | DIAS-STP-94-33; ITFA-94-29; ICN-UNAM-94-07 | hep-th cond-mat | null | We study $\l\f^4$ theory using an environmentally friendly finite-temperature
renormalization group. We derive flow equations, using a fiducial temperature
as flow parameter, develop them perturbatively in an expansion free from
ultraviolet and infrared divergences, then integrate them numerically from zero
to temper... | [
{
"created": "Wed, 30 Nov 1994 03:05:32 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"van Eijck",
"M. A.",
""
],
[
"O'Connor",
"Denjoe",
""
],
[
"Stephens",
"C. R.",
""
]
] | We study $\l\f^4$ theory using an environmentally friendly finite-temperature renormalization group. We derive flow equations, using a fiducial temperature as flow parameter, develop them perturbatively in an expansion free from ultraviolet and infrared divergences, then integrate them numerically from zero to temperat... | 10.753839 | 9.635147 | 10.994355 | 8.914435 | 9.17919 | 9.930944 | 9.153481 | 9.742073 | 9.54217 | 11.55578 | 9.406671 | 9.859582 | 10.329578 | 9.400437 | 9.647433 | 9.587566 | 9.561003 | 9.457531 | 10.062803 | 10.6478 | 10.240239 |
hep-th/0701270 | Brett D. Altschul | Brett Altschul | Cerenkov Radiation in a Lorentz-Violating and Birefringent Vacuum | 17 pages, version to appear in Phys. Rev. D | Phys.Rev.D75:105003,2007 | 10.1103/PhysRevD.75.105003 | IUHET-505 | hep-th | null | We calculate the emission spectrum for vacuum Cerenkov radiation in
Lorentz-violating extensions of electrodynamics. We develop an approach that
works equally well if the presence or the absence of birefringence. In addition
to confirming earlier work, we present the first calculation relevant to
Cerenkov radiation i... | [
{
"created": "Tue, 30 Jan 2007 03:38:18 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Apr 2007 16:49:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Altschul",
"Brett",
""
]
] | We calculate the emission spectrum for vacuum Cerenkov radiation in Lorentz-violating extensions of electrodynamics. We develop an approach that works equally well if the presence or the absence of birefringence. In addition to confirming earlier work, we present the first calculation relevant to Cerenkov radiation in ... | 12.612132 | 11.404505 | 11.417489 | 11.158703 | 12.040081 | 11.212887 | 11.653166 | 11.259583 | 10.921302 | 12.323838 | 10.844382 | 11.584091 | 11.541529 | 11.187385 | 11.908825 | 11.625848 | 10.23565 | 11.432749 | 10.705112 | 11.099183 | 11.872109 |
hep-th/9504008 | Marco Aurelio do Rego Monteiro | M.R-Monteiro, I.Roditi, L.M.C.S.Rodrigues and S.Sciuto | The Role of the Central Element in the Quantum Algebra Underlying the
Twisted XXZ Chain | LaTeX file, 15 pages | Phys.Lett. B354 (1995) 389-395 | 10.1016/0370-2693(95)00684-D | DFTT 22/95 and CBPF-NF-17/95 | hep-th cond-mat | null | We study the relationship among the XXZ Heisenberg model and three models
obtained from it by various transformations. In particular, we emphasize the
role of a non trivial central element $t^Z$ in the underlying algebra and its
relationship with the twisted boundary conditions, $S^{\pm}_{N+1}=t^{\pm
N}S^{\pm}_1$.
| [
{
"created": "Tue, 4 Apr 1995 12:42:48 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"R-Monteiro",
"M.",
""
],
[
"Roditi",
"I.",
""
],
[
"Rodrigues",
"L. M. C. S.",
""
],
[
"Sciuto",
"S.",
""
]
] | We study the relationship among the XXZ Heisenberg model and three models obtained from it by various transformations. In particular, we emphasize the role of a non trivial central element $t^Z$ in the underlying algebra and its relationship with the twisted boundary conditions, $S^{\pm}_{N+1}=t^{\pm N}S^{\pm}_1$. | 11.167686 | 11.569577 | 12.496098 | 10.497194 | 10.989764 | 10.125587 | 11.89608 | 10.521912 | 11.053688 | 11.499827 | 10.106893 | 10.833412 | 11.781749 | 10.443231 | 10.450967 | 10.445977 | 10.414804 | 10.320043 | 10.646252 | 12.018035 | 10.064651 |
0903.1868 | Gerald V. Dunne | Gokce Basar, Gerald V. Dunne, Michael Thies | Inhomogeneous Condensates in the Thermodynamics of the Chiral NJL_2
model | 28 pages, 13 figures | Phys.Rev.D79:105012,2009 | 10.1103/PhysRevD.79.105012 | null | hep-th cond-mat.supr-con hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the thermodynamical properties, at finite density and nonzero
temperature, of the (1+1)-dimensional chiral Gross-Neveu model (the NJL_2
model), using the exact inhomogeneous (crystalline) condensate solutions to the
gap equation. The continuous chiral symmetry of the model plays a crucial role,
and the the... | [
{
"created": "Tue, 10 Mar 2009 22:24:49 GMT",
"version": "v1"
}
] | 2010-11-11 | [
[
"Basar",
"Gokce",
""
],
[
"Dunne",
"Gerald V.",
""
],
[
"Thies",
"Michael",
""
]
] | We analyze the thermodynamical properties, at finite density and nonzero temperature, of the (1+1)-dimensional chiral Gross-Neveu model (the NJL_2 model), using the exact inhomogeneous (crystalline) condensate solutions to the gap equation. The continuous chiral symmetry of the model plays a crucial role, and the therm... | 7.1994 | 6.822525 | 7.140434 | 6.628196 | 6.749458 | 7.161586 | 6.446375 | 6.750494 | 6.288316 | 7.453427 | 7.008328 | 6.901021 | 6.985001 | 6.936554 | 7.098835 | 6.91714 | 6.952927 | 6.926805 | 6.751704 | 7.039775 | 6.940864 |
1910.04795 | David Tennyson | Anthony Ashmore, Charles Strickland-Constable, David Tennyson, Daniel
Waldram | Generalising G$_\text{2}$ geometry: involutivity, moment maps and moduli | null | JHEP 01 (2021) 158 | 10.1007/JHEP01(2021)158 | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyse the geometry of generic Minkowski $\mathcal{N}=1$, $D=4$ flux
compactifications in string theory, the default backgrounds for string model
building. In M-theory they are the natural string theoretic extensions of
$\mathrm{G}_2$ holonomy manifolds. In type II theories, they extend the notion
of Calabi--Yau ... | [
{
"created": "Thu, 10 Oct 2019 18:20:06 GMT",
"version": "v1"
}
] | 2022-02-04 | [
[
"Ashmore",
"Anthony",
""
],
[
"Strickland-Constable",
"Charles",
""
],
[
"Tennyson",
"David",
""
],
[
"Waldram",
"Daniel",
""
]
] | We analyse the geometry of generic Minkowski $\mathcal{N}=1$, $D=4$ flux compactifications in string theory, the default backgrounds for string model building. In M-theory they are the natural string theoretic extensions of $\mathrm{G}_2$ holonomy manifolds. In type II theories, they extend the notion of Calabi--Yau ge... | 7.068172 | 7.751467 | 7.777602 | 6.89292 | 7.961129 | 7.758685 | 7.599409 | 7.186773 | 6.853702 | 9.309101 | 7.16542 | 6.889759 | 7.288589 | 6.96684 | 6.720939 | 6.975126 | 6.849193 | 6.737129 | 6.903519 | 7.28037 | 6.930584 |
hep-th/9310094 | Balakrishna Shankar | B. S. Balakrishna and K. T. Mahanthappa | Composite gauge field models with broken symmetries | 12 pages, COLO-HEP/325 | Phys.Rev.D49:2653-2657,1994 | 10.1103/PhysRevD.49.R2653 | null | hep-th hep-ph | null | We present a generalization of the non-Abelian version of the $CP^{N-1}$
models (also known as Grassmannian models) that involve composite gauge fields
to accommodate partial breaking of the non-Abelian gauge symmetry. For this to
be possible, in most cases, the constituent fields need to belong to an anomaly
free co... | [
{
"created": "Fri, 15 Oct 1993 14:07:47 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Oct 1993 21:44:39 GMT",
"version": "v2"
},
{
"created": "Mon, 18 Oct 1993 17:25:48 GMT",
"version": "v3"
}
] | 2010-01-06 | [
[
"Balakrishna",
"B. S.",
""
],
[
"Mahanthappa",
"K. T.",
""
]
] | We present a generalization of the non-Abelian version of the $CP^{N-1}$ models (also known as Grassmannian models) that involve composite gauge fields to accommodate partial breaking of the non-Abelian gauge symmetry. For this to be possible, in most cases, the constituent fields need to belong to an anomaly free comp... | 11.004371 | 11.431801 | 11.077815 | 10.378083 | 11.136045 | 11.788543 | 11.685035 | 10.543311 | 10.44513 | 11.886946 | 10.641537 | 10.494798 | 11.083349 | 10.588116 | 10.585061 | 10.226969 | 10.408718 | 10.754649 | 10.086177 | 10.506985 | 10.530128 |
0912.3051 | Filipe Moura | Filipe Moura | String-corrected dilatonic black holes in d dimensions | 9 pages. v2: extended discussion on thermodynamical properties;
reference added. Published version | Phys.Rev.D83:044002,2011 | 10.1103/PhysRevD.83.044002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We solve the dilaton field equation in the background of a spherically
symmetric black hole in bosonic or heterotic string theory with
curvature-squared corrections in arbitrary d spacetime dimensions. We then
apply this result to obtain a spherically symmetric black hole solution with
dilatonic charge and curvature-... | [
{
"created": "Wed, 16 Dec 2009 04:12:35 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Feb 2011 17:34:53 GMT",
"version": "v2"
}
] | 2011-02-15 | [
[
"Moura",
"Filipe",
""
]
] | We solve the dilaton field equation in the background of a spherically symmetric black hole in bosonic or heterotic string theory with curvature-squared corrections in arbitrary d spacetime dimensions. We then apply this result to obtain a spherically symmetric black hole solution with dilatonic charge and curvature-sq... | 6.488263 | 6.205863 | 6.306502 | 5.731812 | 5.757671 | 5.707494 | 5.950663 | 5.861514 | 5.593612 | 6.567102 | 5.947468 | 5.813398 | 6.202993 | 5.782793 | 5.671132 | 5.842248 | 5.712233 | 5.959973 | 5.870754 | 6.155767 | 5.881433 |
0908.1742 | Boris Pioline | Guillaume Bossard, Yann Michel, Boris Pioline | Extremal black holes, nilpotent orbits and the true fake superpotential | 47 pages + appendices, 7 figures; v2: minor corrections, to appear in
JHEP | JHEP 1001:038,2010 | 10.1007/JHEP01(2010)038 | AEI-2009-076 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dimensional reduction along time offers a powerful way to study stationary
solutions of 4D symmetric supergravity models via group-theoretical methods. We
apply this approach systematically to extremal, BPS and non-BPS, spherically
symmetric black holes, and obtain their "fake superpotential" W. The latter
provides f... | [
{
"created": "Wed, 12 Aug 2009 16:21:51 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jan 2010 14:12:51 GMT",
"version": "v2"
}
] | 2016-09-08 | [
[
"Bossard",
"Guillaume",
""
],
[
"Michel",
"Yann",
""
],
[
"Pioline",
"Boris",
""
]
] | Dimensional reduction along time offers a powerful way to study stationary solutions of 4D symmetric supergravity models via group-theoretical methods. We apply this approach systematically to extremal, BPS and non-BPS, spherically symmetric black holes, and obtain their "fake superpotential" W. The latter provides fir... | 10.325238 | 9.294449 | 11.796994 | 10.241204 | 9.692079 | 10.473074 | 10.169327 | 10.094526 | 9.566069 | 11.833854 | 9.335564 | 9.888734 | 10.459904 | 9.827407 | 9.980407 | 10.133736 | 9.737417 | 9.776526 | 9.834729 | 10.192476 | 9.780527 |
hep-th/0512192 | David Tong | David Tong | D-Branes in Field Theory | 23 Pages, 3 figures. v2: reference added | JHEP0602:030,2006 | 10.1088/1126-6708/2006/02/030 | null | hep-th | null | Certain gauge theories in four dimensions are known to admit semi-classical
D-brane solitons. These are domain walls on which vortex flux tubes may end.
The purpose of this paper is to develop an open-string description of these
D-branes. The dynamics of the domain walls is shown to be governed by a
Chern-Simons-Higg... | [
{
"created": "Thu, 15 Dec 2005 17:06:45 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Jan 2006 14:50:36 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Tong",
"David",
""
]
] | Certain gauge theories in four dimensions are known to admit semi-classical D-brane solitons. These are domain walls on which vortex flux tubes may end. The purpose of this paper is to develop an open-string description of these D-branes. The dynamics of the domain walls is shown to be governed by a Chern-Simons-Higgs ... | 9.567157 | 8.074532 | 9.338138 | 8.293207 | 8.33873 | 8.939168 | 8.335225 | 8.055414 | 8.167821 | 9.953224 | 8.390061 | 8.491135 | 9.174812 | 8.505667 | 8.757117 | 8.49787 | 8.441384 | 8.67161 | 8.3956 | 9.600977 | 8.646131 |
2111.03682 | Eric Lescano | Eric Lescano and Nahuel Mir\'on-Granese | Double Field Theory with matter and its cosmological application | V2: 28 pages. Discussions and references added | null | null | null | hep-th astro-ph.CO gr-qc | http://creativecommons.org/licenses/by/4.0/ | The phase space formulation of Double Field Theory (DFT) indicates that
statistical matter can be included in terms of (T-)duality multiplets. We
propose the inclusion of a perfect fluid in the geometry of DFT through a
generalized energy-momentum tensor written in terms of a DFT pressure, energy
density and velocity... | [
{
"created": "Fri, 5 Nov 2021 18:15:43 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jun 2022 11:51:15 GMT",
"version": "v2"
}
] | 2022-06-07 | [
[
"Lescano",
"Eric",
""
],
[
"Mirón-Granese",
"Nahuel",
""
]
] | The phase space formulation of Double Field Theory (DFT) indicates that statistical matter can be included in terms of (T-)duality multiplets. We propose the inclusion of a perfect fluid in the geometry of DFT through a generalized energy-momentum tensor written in terms of a DFT pressure, energy density and velocity. ... | 14.127736 | 13.605276 | 14.772 | 12.209944 | 13.90382 | 14.282087 | 12.971831 | 13.708552 | 13.396968 | 15.588982 | 13.455528 | 13.607362 | 13.388509 | 13.446363 | 13.734838 | 13.308076 | 13.355744 | 13.120741 | 13.01026 | 13.371225 | 13.454489 |
hep-th/9112001 | null | E. Raiten | Perturbations of a Stringy Black Hole | 15 p | Int.J.Mod.Phys. D1 (1993) 591-604 | 10.1142/S021827189200029X | null | hep-th | null | We extend the three dimensional stringy black hole of Horne and Horowitz to
four dimensions. After a brief discussion of the global properties of the
metric, we discuss the stability of the background with respect to small
perturbations, following the methods of Gilbert and of Chandrasekhar. The
potential for axial p... | [
{
"created": "Mon, 2 Dec 1991 22:38:05 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Dec 1991 01:09:45 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Raiten",
"E.",
""
]
] | We extend the three dimensional stringy black hole of Horne and Horowitz to four dimensions. After a brief discussion of the global properties of the metric, we discuss the stability of the background with respect to small perturbations, following the methods of Gilbert and of Chandrasekhar. The potential for axial per... | 7.947797 | 8.461655 | 7.702303 | 7.372206 | 7.320194 | 7.112625 | 8.919453 | 7.830156 | 7.986413 | 8.10778 | 7.231646 | 7.516282 | 7.795179 | 7.730909 | 8.188116 | 7.725276 | 7.719718 | 7.757324 | 8.208462 | 7.271029 | 7.472966 |
hep-th/0609063 | Hironobu Kihara | H. Itoyama, H. Kihara and R. Yoshioka | Partition Functions of Reduced Matrix Models with Classical Gauge Groups | 17 pages, 6 figures, typos corrected, more comments included, to
appear in Nuclear Physics B | Nucl.Phys.B762:285-300,2007 | 10.1016/j.nuclphysb.2006.11.001 | OCU-PHYS-253 | hep-th | null | We evaluate partition functions of matrix models which are given by
topologically twisted and dimensionally reduced actions of d=4 N=1 super
Yang-Mills theories with classical (semi-)simple gauge groups, SO(2N), SO(2N+1)
and USp(2N). The integrals reduce to those over the maximal tori by
semi-classical approximation ... | [
{
"created": "Sat, 9 Sep 2006 07:37:44 GMT",
"version": "v1"
},
{
"created": "Sat, 4 Nov 2006 10:30:58 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Itoyama",
"H.",
""
],
[
"Kihara",
"H.",
""
],
[
"Yoshioka",
"R.",
""
]
] | We evaluate partition functions of matrix models which are given by topologically twisted and dimensionally reduced actions of d=4 N=1 super Yang-Mills theories with classical (semi-)simple gauge groups, SO(2N), SO(2N+1) and USp(2N). The integrals reduce to those over the maximal tori by semi-classical approximation wh... | 12.578889 | 11.690187 | 13.285185 | 11.630919 | 12.044296 | 12.000419 | 12.551706 | 11.219541 | 10.853765 | 13.821401 | 12.042227 | 12.129439 | 12.360131 | 11.342422 | 11.689613 | 11.037436 | 11.589314 | 11.11265 | 11.872744 | 12.005283 | 11.253413 |
hep-th/0210098 | David Dudal | David Dudal and Henri Verschelde | The mass gap and vacuum energy of the Gross-Neveu model via the 2PPI
expansion | 14 pages,19 eps figures, revtex4 | Phys.Rev. D67 (2003) 025011 | 10.1103/PhysRevD.67.025011 | null | hep-th | null | We introduce the 2PPI (2-point-particle-irreducible) expansion, which sums
bubble graphs to all orders. We prove the renormalizibility of this summation.
We use it on the Gross-Neveu model to calculate the mass gap and vacuum energy.
After an optimization of the expansion, the final results are qualitatively
good.
| [
{
"created": "Thu, 10 Oct 2002 15:04:49 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Dudal",
"David",
""
],
[
"Verschelde",
"Henri",
""
]
] | We introduce the 2PPI (2-point-particle-irreducible) expansion, which sums bubble graphs to all orders. We prove the renormalizibility of this summation. We use it on the Gross-Neveu model to calculate the mass gap and vacuum energy. After an optimization of the expansion, the final results are qualitatively good. | 11.647566 | 9.4707 | 10.14298 | 9.479177 | 10.060893 | 9.701916 | 9.782843 | 8.779488 | 9.056075 | 11.355027 | 9.914929 | 9.835358 | 9.832786 | 9.781789 | 10.365941 | 10.203383 | 10.119054 | 10.246429 | 9.850595 | 9.519514 | 10.841254 |
1712.03235 | Marco Fazzi | Fabio Apruzzi, Marco Fazzi | AdS$_7$/CFT$_6$ with orientifolds | 91 pages, 6 figures, 4 tables, 4 appendices; v2: typos fixed, version
published in JHEP | null | 10.1007/JHEP01(2018)124 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | AdS$_7$ solutions of massive type IIA have been classified, and are dual to a
large class of six-dimensional $(1,0)$ SCFT's whose tensor branch deformations
are described by linear quivers of SU groups. Quivers and AdS vacua depend
solely on the group theory data of the NS5-D6-D8 brane configurations
engineering the ... | [
{
"created": "Fri, 8 Dec 2017 19:00:00 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Jan 2018 15:41:52 GMT",
"version": "v2"
}
] | 2018-03-14 | [
[
"Apruzzi",
"Fabio",
""
],
[
"Fazzi",
"Marco",
""
]
] | AdS$_7$ solutions of massive type IIA have been classified, and are dual to a large class of six-dimensional $(1,0)$ SCFT's whose tensor branch deformations are described by linear quivers of SU groups. Quivers and AdS vacua depend solely on the group theory data of the NS5-D6-D8 brane configurations engineering the fi... | 9.25897 | 7.836211 | 12.072163 | 8.230376 | 8.809808 | 8.434597 | 7.893037 | 7.968008 | 7.955289 | 11.256967 | 7.753271 | 7.910793 | 9.219136 | 8.123982 | 8.275403 | 7.894328 | 8.043924 | 7.744495 | 8.07572 | 8.811792 | 8.054807 |
1107.0758 | Steven Willison | Pablo Mora, Pablo Pais and Steven Willison | Gauged WZW models for space-time groups and gravitational actions | 26 pages, no figures | null | 10.1103/PhysRevD.84.044058 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate gauged Wess-Zumino-Witten models for space-time
groups as gravitational theories, following the trend of recent work by
Anabalon, Willison and Zanelli. We discuss the field equations in any dimension
and study in detail the simplest case of two space-time dimensions and gauge
group SO(2,1... | [
{
"created": "Mon, 4 Jul 2011 23:59:03 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Mora",
"Pablo",
""
],
[
"Pais",
"Pablo",
""
],
[
"Willison",
"Steven",
""
]
] | In this paper we investigate gauged Wess-Zumino-Witten models for space-time groups as gravitational theories, following the trend of recent work by Anabalon, Willison and Zanelli. We discuss the field equations in any dimension and study in detail the simplest case of two space-time dimensions and gauge group SO(2,1).... | 10.720081 | 12.741364 | 12.381961 | 9.530548 | 10.486934 | 10.963045 | 11.445979 | 10.727416 | 11.5411 | 10.757777 | 10.806969 | 10.079998 | 10.841269 | 9.703521 | 10.022661 | 10.227191 | 9.887242 | 9.934534 | 9.874865 | 10.776946 | 9.861764 |
1801.03658 | Yoji Koyama | Chong-Sun Chu, Yoji Koyama | Soft Hair of Dynamical Black Hole and Hawking Radiation | 26 pages. 2 figures. v2: References added | null | 10.1007/JHEP04(2018)056 | NCTS-TH/1801 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Soft hair of black hole has been proposed recently to play an important role
in the resolution of the black hole information paradox. Recent work has
emphasized that the soft modes cannot affect the black hole S-matrix due to
Weinberg soft theorems. However as soft hair is generated by supertranslation
of geometry wh... | [
{
"created": "Thu, 11 Jan 2018 08:10:00 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jan 2018 11:41:56 GMT",
"version": "v2"
}
] | 2018-05-09 | [
[
"Chu",
"Chong-Sun",
""
],
[
"Koyama",
"Yoji",
""
]
] | Soft hair of black hole has been proposed recently to play an important role in the resolution of the black hole information paradox. Recent work has emphasized that the soft modes cannot affect the black hole S-matrix due to Weinberg soft theorems. However as soft hair is generated by supertranslation of geometry whic... | 8.760352 | 7.852406 | 8.944807 | 7.434068 | 8.143425 | 8.370762 | 7.739104 | 7.834632 | 7.86795 | 8.722569 | 7.543399 | 7.674584 | 8.015924 | 7.843156 | 7.621153 | 7.344711 | 7.712739 | 7.37376 | 7.989867 | 7.94049 | 7.840722 |
1409.5421 | Yukihiro Fujimoto | Tomo-hiro Abe, Yukihiro Fujimoto, Tatsuo Kobayashi, Takashi Miura,
Kenji Nishiwaki, Makoto Sakamoto | Operator analysis of physical states on magnetized $T^{2}/Z_{N}$
orbifolds | 41 pages, 1 figure | null | 10.1016/j.nuclphysb.2014.11.022 | EHOU-14-003, HRI-P-14-02-001, KOBE-TH-14-02, KUNS-2485, OU-HET-827,
RECAPP-HRI-2014-004 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss an effective way for analyzing the system on the magnetized
twisted orbifolds in operator formalism, especially in the complicated cases
$T^{2}/Z_{3}$, $T^{2}/Z_{4}$ and $T^{2}/Z_{6}$. We can obtain the exact and
analytical results which can be applicable for any larger values of the
quantized magnetic flu... | [
{
"created": "Thu, 18 Sep 2014 19:43:19 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Dec 2014 22:15:04 GMT",
"version": "v2"
}
] | 2014-12-25 | [
[
"Abe",
"Tomo-hiro",
""
],
[
"Fujimoto",
"Yukihiro",
""
],
[
"Kobayashi",
"Tatsuo",
""
],
[
"Miura",
"Takashi",
""
],
[
"Nishiwaki",
"Kenji",
""
],
[
"Sakamoto",
"Makoto",
""
]
] | We discuss an effective way for analyzing the system on the magnetized twisted orbifolds in operator formalism, especially in the complicated cases $T^{2}/Z_{3}$, $T^{2}/Z_{4}$ and $T^{2}/Z_{6}$. We can obtain the exact and analytical results which can be applicable for any larger values of the quantized magnetic flux ... | 10.829411 | 12.431029 | 11.659063 | 10.967113 | 12.029336 | 11.217326 | 11.84091 | 11.278901 | 11.165849 | 11.746044 | 11.373332 | 11.073722 | 10.939064 | 10.854787 | 11.07458 | 11.110973 | 10.886997 | 10.713137 | 10.909908 | 11.216804 | 10.942656 |
hep-th/9601122 | Andjelka Andrasi | A. Andra\v{s}i, J.C. Taylor | Renormalization of Wilson Operators in Minkowski space | plain tex, 8 pages, 5 figures not included | Nucl.Phys. B516 (1998) 417-425 | 10.1016/S0550-3213(97)00769-4 | RBI-TH-01/96 | hep-th | null | We make some comments on the renormalization of Wilson operators (not just
vacuum -expectation values of Wilson operators), and the features which arise
in Minkowski space. If the Wilson loop contains a straight light-like segment,
charge renormalization does not work in a simple graph-by-graph way; but does
work whe... | [
{
"created": "Tue, 23 Jan 1996 10:48:55 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Andraši",
"A.",
""
],
[
"Taylor",
"J. C.",
""
]
] | We make some comments on the renormalization of Wilson operators (not just vacuum -expectation values of Wilson operators), and the features which arise in Minkowski space. If the Wilson loop contains a straight light-like segment, charge renormalization does not work in a simple graph-by-graph way; but does work when ... | 14.173906 | 13.660069 | 14.544636 | 13.077121 | 14.056465 | 14.457747 | 13.943635 | 13.616134 | 13.286552 | 14.626045 | 12.766069 | 12.665791 | 13.187808 | 12.684179 | 13.840783 | 13.437922 | 13.351511 | 14.025579 | 13.546879 | 13.297283 | 13.258598 |
hep-th/0509216 | David Tong | David Tong | TASI Lectures on Solitons | 139 (small) pages. Lots of figures. This is an extended write up of
lectures given at TASI, June 2005. v2-5: typos corrected, references added | null | null | null | hep-th | null | These lectures cover aspects of solitons with focus on applications to the
quantum dynamics of supersymmetric gauge theories and string theory. The
lectures consist of four sections, each dealing with a different soliton. We
start with instantons and work down in co-dimension to monopoles, vortices and,
eventually, d... | [
{
"created": "Wed, 28 Sep 2005 17:34:22 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Sep 2005 16:57:50 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Oct 2005 15:27:40 GMT",
"version": "v3"
},
{
"created": "Tue, 22 Nov 2005 12:51:03 GMT",
"version": "v4"
},
{
"cr... | 2007-05-23 | [
[
"Tong",
"David",
""
]
] | These lectures cover aspects of solitons with focus on applications to the quantum dynamics of supersymmetric gauge theories and string theory. The lectures consist of four sections, each dealing with a different soliton. We start with instantons and work down in co-dimension to monopoles, vortices and, eventually, dom... | 6.418219 | 6.069591 | 6.58074 | 5.990194 | 6.315773 | 6.058213 | 6.129915 | 6.258528 | 5.872868 | 7.255313 | 6.060966 | 5.945598 | 6.175798 | 5.833008 | 5.968435 | 6.110471 | 5.967993 | 6.042498 | 6.016784 | 6.037838 | 5.910755 |
1908.05281 | Indranil Halder | Indranil Halder | Global Symmetry and Maximal Chaos | 25 pages | null | null | null | hep-th cond-mat.quant-gas cond-mat.stat-mech cond-mat.str-el math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we study chaos in generic quantum systems with a global symmetry
generalizing seminal work [arXiv : 1503.01409] by Maldacena, Shenker and
Stanford. We conjecture a bound on instantaneous chaos exponent in a
thermodynamic ensemble at temperature $T$ and chemical potential $\mu$ for the
continuous global s... | [
{
"created": "Wed, 14 Aug 2019 18:00:05 GMT",
"version": "v1"
},
{
"created": "Sun, 18 Aug 2019 11:18:25 GMT",
"version": "v2"
},
{
"created": "Thu, 22 Aug 2019 07:27:36 GMT",
"version": "v3"
},
{
"created": "Wed, 25 Sep 2019 14:06:29 GMT",
"version": "v4"
},
{
"c... | 2019-10-23 | [
[
"Halder",
"Indranil",
""
]
] | In this note we study chaos in generic quantum systems with a global symmetry generalizing seminal work [arXiv : 1503.01409] by Maldacena, Shenker and Stanford. We conjecture a bound on instantaneous chaos exponent in a thermodynamic ensemble at temperature $T$ and chemical potential $\mu$ for the continuous global sym... | 8.326718 | 7.475727 | 8.963729 | 7.247794 | 7.320253 | 7.738368 | 7.807519 | 7.940439 | 7.082007 | 9.884892 | 7.79637 | 7.499593 | 8.586208 | 7.528601 | 7.526381 | 7.795641 | 7.515819 | 7.731819 | 7.525473 | 8.100023 | 7.7736 |
1508.00501 | Eliot Hijano | Eliot Hijano, Per Kraus, Eric Perlmutter, River Snively | Witten Diagrams Revisited: The AdS Geometry of Conformal Blocks | 54 pages + refs | null | 10.1007/JHEP01(2016)146 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a new method for decomposing Witten diagrams into conformal
blocks. The steps involved are elementary, requiring no explicit integration,
and operate directly in position space. Central to this construction is an
appealingly simple answer to the question: what object in AdS computes a
conformal block? The ... | [
{
"created": "Mon, 3 Aug 2015 17:36:45 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Sep 2015 03:25:44 GMT",
"version": "v2"
}
] | 2016-02-17 | [
[
"Hijano",
"Eliot",
""
],
[
"Kraus",
"Per",
""
],
[
"Perlmutter",
"Eric",
""
],
[
"Snively",
"River",
""
]
] | We develop a new method for decomposing Witten diagrams into conformal blocks. The steps involved are elementary, requiring no explicit integration, and operate directly in position space. Central to this construction is an appealingly simple answer to the question: what object in AdS computes a conformal block? The an... | 8.25587 | 7.831857 | 11.4568 | 7.878098 | 8.056607 | 9.131059 | 8.334204 | 8.390963 | 7.773933 | 10.100259 | 8.236644 | 8.029552 | 8.898445 | 8.182478 | 7.908998 | 8.310754 | 7.862705 | 8.120284 | 8.107539 | 9.059298 | 8.413871 |
hep-th/0311165 | Jose Alexandre Nogueira | J. A. Nogueira and D. Possa | Boundary Conditions as Mass Generation Mechanism for Complex Scalar
Fields | 8 pages | null | null | null | hep-th | null | We consider the effects of homogeneous Dirichlet's boundary conditions in the
scalar electrodynamics with self-interaction. We have found for a critical
scale of the compactification length that symmetry is restored and scalar field
develops mass and vector field does not.
| [
{
"created": "Tue, 18 Nov 2003 15:11:58 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nogueira",
"J. A.",
""
],
[
"Possa",
"D.",
""
]
] | We consider the effects of homogeneous Dirichlet's boundary conditions in the scalar electrodynamics with self-interaction. We have found for a critical scale of the compactification length that symmetry is restored and scalar field develops mass and vector field does not. | 23.552572 | 21.830633 | 21.60696 | 21.713232 | 20.334299 | 20.344948 | 20.067047 | 19.913794 | 20.600189 | 21.010054 | 18.823002 | 20.705133 | 22.127625 | 19.378675 | 19.474607 | 20.224613 | 18.982979 | 19.578602 | 20.204954 | 20.336308 | 19.435408 |
hep-th/0312216 | Keith R. Dienes | Keith R. Dienes, Michael Lennek | Adventures in Thermal Duality (I): Extracting Closed-Form Solutions for
Finite-Temperature Effective Potentials in String Theory | 25 pages, LaTeX, 3 figures | Phys.Rev. D70 (2004) 126005 | 10.1103/PhysRevD.70.126005 | null | hep-th cond-mat.stat-mech gr-qc hep-ph | null | Thermal duality, which relates the physics of closed strings at temperature T
to the physics at the inverse temperature 1/T, is one of the most intriguing
features of string thermodynamics. Unfortunately, the classical definitions of
thermodynamic quantities such as entropy and specific heat are not invariant
under t... | [
{
"created": "Thu, 18 Dec 2003 20:17:21 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Dienes",
"Keith R.",
""
],
[
"Lennek",
"Michael",
""
]
] | Thermal duality, which relates the physics of closed strings at temperature T to the physics at the inverse temperature 1/T, is one of the most intriguing features of string thermodynamics. Unfortunately, the classical definitions of thermodynamic quantities such as entropy and specific heat are not invariant under the... | 8.760277 | 8.215286 | 9.312199 | 8.333882 | 8.312086 | 8.418914 | 8.536243 | 8.375349 | 8.912828 | 9.763349 | 8.189793 | 8.121017 | 8.543546 | 8.227543 | 8.128533 | 8.13454 | 7.88586 | 8.17301 | 8.249505 | 8.765481 | 8.121594 |
2205.06208 | Mikhail Pavlov | Mikhail Pavlov | Example of the $4$-pt non-vacuum $\mathcal{W}_3$ classical block | V2: 18 pages, typos corrected, comments and references added | null | 10.1016/j.physletb.2023.137855 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this note, we study a special case of the $4$-pt non-vacuum classical
block associated with the $\mathcal{W}_3$ algebra. We formulate the monodromy
problem for the block and derive monodromy equations within the heavy-light
approximation. Fixing the remaining functional arbitrariness using parameters
of the $4$-pt... | [
{
"created": "Thu, 12 May 2022 16:45:48 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jul 2023 04:57:17 GMT",
"version": "v2"
}
] | 2023-07-25 | [
[
"Pavlov",
"Mikhail",
""
]
] | In this note, we study a special case of the $4$-pt non-vacuum classical block associated with the $\mathcal{W}_3$ algebra. We formulate the monodromy problem for the block and derive monodromy equations within the heavy-light approximation. Fixing the remaining functional arbitrariness using parameters of the $4$-pt v... | 8.640522 | 7.562662 | 9.909778 | 7.213607 | 7.258372 | 7.655629 | 7.660681 | 7.17314 | 7.654352 | 9.974545 | 7.182328 | 7.575923 | 8.609698 | 7.231075 | 7.356338 | 7.487792 | 7.306251 | 7.525085 | 7.284723 | 8.396715 | 7.568436 |
0908.2756 | Alexander Sevrin | Alexander Sevrin, Wieland Staessens, Alexander Wijns | An N=2 worldsheet approach to D-branes in bihermitian geometries: II.
The general case | LaTeX, JHEP3.cls, 57 pages | JHEP 0909:105,2009 | 10.1088/1126-6708/2009/09/105 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We complete the investigation of N=(2,2) supersymmetric nonlinear
sigma-models in the presence of a boundary. We study the full bihermitian
geometry parameterized by chiral, twisted chiral and semi-chiral superfields
and identify the D-brane configurations preserving an N=2 worldsheet
supersymmetry. Combining twisted... | [
{
"created": "Wed, 19 Aug 2009 14:47:02 GMT",
"version": "v1"
}
] | 2009-11-06 | [
[
"Sevrin",
"Alexander",
""
],
[
"Staessens",
"Wieland",
""
],
[
"Wijns",
"Alexander",
""
]
] | We complete the investigation of N=(2,2) supersymmetric nonlinear sigma-models in the presence of a boundary. We study the full bihermitian geometry parameterized by chiral, twisted chiral and semi-chiral superfields and identify the D-brane configurations preserving an N=2 worldsheet supersymmetry. Combining twisted w... | 7.801688 | 7.734972 | 8.861901 | 7.448794 | 7.895239 | 7.439207 | 7.777322 | 7.437816 | 7.308497 | 8.787431 | 7.26978 | 7.311208 | 8.36984 | 7.471871 | 7.356273 | 7.551923 | 7.568803 | 7.586614 | 7.476204 | 7.997571 | 7.340398 |
hep-th/9410174 | Valeri Dvoeglazov | Valeri V. Dvoeglazov (Zacatecas University, M\'exico) | Can the $2(2j+1)$ component Weinberg-Tucker-Hammer equations describe
the electromagnetic field? | LaTeX file. 7pp | Annales Fond.Broglie 23:116-120,1998 | null | EFUAZ FT-94-09-REV | hep-th | null | It is shown that the massless $j=1$ Weinberg-Tucker-Hammer equations reduce
to the Maxwell's equations for electromagnetic field under the definite choice
of field functions and initial and boundary conditions. Thus, the former appear
to be of use in a description of some physical processes for which that could
be ne... | [
{
"created": "Sun, 23 Oct 1994 19:22:44 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Dvoeglazov",
"Valeri V.",
"",
"Zacatecas University, México"
]
] | It is shown that the massless $j=1$ Weinberg-Tucker-Hammer equations reduce to the Maxwell's equations for electromagnetic field under the definite choice of field functions and initial and boundary conditions. Thus, the former appear to be of use in a description of some physical processes for which that could be nece... | 22.9785 | 21.693445 | 25.052891 | 21.476349 | 19.16925 | 19.311131 | 19.827988 | 20.758619 | 19.784628 | 25.400579 | 20.21435 | 20.012814 | 21.179316 | 21.036026 | 19.152971 | 20.573563 | 18.867037 | 21.22401 | 19.856543 | 21.769444 | 20.637827 |
hep-th/0212016 | Marco Krohn | Marco Krohn, Michael Flohr | Ghost Systems Revisited: Modified Virasoro Generators and Logarithmic
Conformal Field Theories | 24+1 pages LaTeX2e. Corrected an erroneous EU network number in the
acknowledgments to HPRN-CT-2002-00325 | JHEP 0301 (2003) 020 | 10.1088/1126-6708/2003/01/020 | ITP-UH-26/02 | hep-th | null | We study the possibility of extending ghost systems with higher spin to a
logarithmic conformal field theory. In particular we are interested in c=-26
which turns out to behave very differently to the already known c=-2 case. The
energy momentum tensor cannot be built anymore by a combination of derivatives
of genera... | [
{
"created": "Mon, 2 Dec 2002 16:06:09 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Nov 2003 11:17:43 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Krohn",
"Marco",
""
],
[
"Flohr",
"Michael",
""
]
] | We study the possibility of extending ghost systems with higher spin to a logarithmic conformal field theory. In particular we are interested in c=-26 which turns out to behave very differently to the already known c=-2 case. The energy momentum tensor cannot be built anymore by a combination of derivatives of generali... | 14.869558 | 13.952121 | 16.144533 | 14.25736 | 17.064037 | 16.636471 | 16.067755 | 13.775885 | 14.823517 | 20.559523 | 14.37744 | 14.313371 | 15.381259 | 13.893771 | 14.288358 | 13.963776 | 14.075993 | 14.104987 | 13.719276 | 15.458647 | 14.058362 |
hep-th/0210161 | Paul Fendley | Paul Fendley, Kareljan Schoutens and Jan de Boer | Lattice Models with N=2 Supersymmetry | 4 pages | Phys.Rev.Lett. 90 (2003) 120402 | 10.1103/PhysRevLett.90.120402 | null | hep-th cond-mat.stat-mech hep-lat | null | We introduce lattice models with explicit N=2 supersymmetry. In these
interacting models, the supersymmetry generators Q^+ and Q^- yield the
Hamiltonian H={Q^+,Q^-} on any graph. The degrees of freedom can be described
as either fermions with hard cores, or as quantum dimers. The Hamiltonian of
our simplest model con... | [
{
"created": "Thu, 17 Oct 2002 18:01:59 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Fendley",
"Paul",
""
],
[
"Schoutens",
"Kareljan",
""
],
[
"de Boer",
"Jan",
""
]
] | We introduce lattice models with explicit N=2 supersymmetry. In these interacting models, the supersymmetry generators Q^+ and Q^- yield the Hamiltonian H={Q^+,Q^-} on any graph. The degrees of freedom can be described as either fermions with hard cores, or as quantum dimers. The Hamiltonian of our simplest model conta... | 10.055861 | 11.154551 | 11.088033 | 10.045971 | 9.763603 | 10.46039 | 9.805928 | 10.910171 | 10.81733 | 12.582893 | 10.243179 | 9.870684 | 10.243338 | 9.576151 | 10.037596 | 9.828979 | 9.542454 | 9.67248 | 9.600513 | 10.610179 | 9.815478 |
1410.6316 | Andrei Barvinsky | A. O. Barvinsky | Holography beyond conformal invariance and AdS isometry? | 16 pages, LaTeX, prepared for a special issue of JETP dedicated to
the 60th birthday of Valery Rubakov | null | 10.1134/S1063776115030036 | CERN-PH-TH-2014-202 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We suggest that the principle of holographic duality can be extended beyond
conformal invariance and AdS isometry. Such an extension is based on a special
relation between functional determinants of the operators acting in the bulk
and on its boundary, provided that the boundary operator represents the inverse
propag... | [
{
"created": "Thu, 23 Oct 2014 10:39:58 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Barvinsky",
"A. O.",
""
]
] | We suggest that the principle of holographic duality can be extended beyond conformal invariance and AdS isometry. Such an extension is based on a special relation between functional determinants of the operators acting in the bulk and on its boundary, provided that the boundary operator represents the inverse propagat... | 9.395497 | 10.021828 | 11.638575 | 9.719717 | 10.313168 | 10.359439 | 9.920694 | 10.184916 | 9.446347 | 11.087318 | 9.263618 | 8.811313 | 9.604347 | 9.144745 | 9.117493 | 9.128734 | 9.339413 | 9.104273 | 9.401207 | 9.507044 | 8.932666 |
hep-th/0103108 | Danny Birmingham | Danny Birmingham and Soussan Mokhtari | The Cardy-Verlinde Formula and Taub-Bolt-AdS Spacetimes | 7 pages, Latex | Phys.Lett.B508:365-368,2001 | 10.1016/S0370-2693(01)00527-5 | null | hep-th | null | We consider the conformal field theory which is dual to the Taub-Bolt-AdS
spacetime. It is shown that the Cardy-Verlinde formula for the entropy of the
conformal field theory agrees precisely with the entropy of the Taub-Bolt-AdS
spacetime, at high temperatures. This result may be viewed as providing a
conformal fiel... | [
{
"created": "Wed, 14 Mar 2001 15:08:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Birmingham",
"Danny",
""
],
[
"Mokhtari",
"Soussan",
""
]
] | We consider the conformal field theory which is dual to the Taub-Bolt-AdS spacetime. It is shown that the Cardy-Verlinde formula for the entropy of the conformal field theory agrees precisely with the entropy of the Taub-Bolt-AdS spacetime, at high temperatures. This result may be viewed as providing a conformal field ... | 4.520372 | 3.793531 | 4.391378 | 3.855777 | 4.090379 | 3.66946 | 3.699067 | 3.747375 | 3.933778 | 4.291864 | 3.938892 | 3.880906 | 4.21017 | 3.844309 | 3.900124 | 3.854636 | 4.05432 | 3.977273 | 4.058972 | 4.025499 | 3.938172 |
hep-th/0302129 | Ignacio Navarro | Ignacio Navarro | Codimension Two Compactifications and the Cosmological Constant Problem | 4 pages, rextex 4 | JCAP 0309 (2003) 004 | 10.1088/1475-7516/2003/09/004 | null | hep-th gr-qc hep-ph | null | We consider solutions of six dimensional Einstein equations with two compact
dimensions. It is shown that one can introduce 3-branes in this background in
such a way that the effective four dimensional cosmological constant is
completely independent of the brane tensions. These tensions are completely
arbitrary, with... | [
{
"created": "Mon, 17 Feb 2003 17:54:39 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Navarro",
"Ignacio",
""
]
] | We consider solutions of six dimensional Einstein equations with two compact dimensions. It is shown that one can introduce 3-branes in this background in such a way that the effective four dimensional cosmological constant is completely independent of the brane tensions. These tensions are completely arbitrary, withou... | 11.776345 | 8.207217 | 10.435149 | 9.242129 | 8.662717 | 9.408126 | 9.139313 | 8.972273 | 8.668115 | 10.584242 | 8.938075 | 9.482787 | 10.413958 | 9.977274 | 9.879495 | 9.696873 | 9.497749 | 9.499556 | 9.721031 | 10.495356 | 9.817754 |
1609.06271 | Alexey Litvinov | Alexey Litvinov and Lev Spodyneiko | On W algebras commuting with a set of screenings | null | null | 10.1007/JHEP11(2016)138 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the problem of classification of all W algebras which commute
with a set of exponential screening operators. Assuming that the W algebra has
a nontrivial current of spin 3, we find equations satisfied by the screening
operators and classify their solutions.
| [
{
"created": "Tue, 20 Sep 2016 18:03:56 GMT",
"version": "v1"
}
] | 2016-12-21 | [
[
"Litvinov",
"Alexey",
""
],
[
"Spodyneiko",
"Lev",
""
]
] | We consider the problem of classification of all W algebras which commute with a set of exponential screening operators. Assuming that the W algebra has a nontrivial current of spin 3, we find equations satisfied by the screening operators and classify their solutions. | 11.656292 | 11.1234 | 14.73418 | 9.561684 | 11.569826 | 11.385802 | 11.830427 | 11.430673 | 9.788867 | 12.283591 | 10.697504 | 10.248685 | 11.928258 | 10.297618 | 10.736078 | 10.588433 | 10.695946 | 9.511041 | 10.290132 | 11.289935 | 11.289367 |
2207.06449 | Christopher Couzens Mr | Christopher Couzens and Koen Stemerdink | Universal spindles: D2's on $\Sigma$ and M5's on $\Sigma\times
\mathbb{H}^3$ | 31 pages, 3 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study the uplift of a 4d black hole in 4d Einstein--Maxwell supergravity
with a spindle horizon to massive type IIA and 11d supergravity on $S^4\times
\mathbb{H}^3$. The solutions exhibit features distinct to the uplift of the
same 4d solution to 11d supergravity on an $S^7$. In particular, whereas the
orbifold si... | [
{
"created": "Wed, 13 Jul 2022 18:02:51 GMT",
"version": "v1"
}
] | 2022-07-15 | [
[
"Couzens",
"Christopher",
""
],
[
"Stemerdink",
"Koen",
""
]
] | We study the uplift of a 4d black hole in 4d Einstein--Maxwell supergravity with a spindle horizon to massive type IIA and 11d supergravity on $S^4\times \mathbb{H}^3$. The solutions exhibit features distinct to the uplift of the same 4d solution to 11d supergravity on an $S^7$. In particular, whereas the orbifold sing... | 8.548816 | 6.764079 | 8.958882 | 7.019164 | 7.907099 | 7.324417 | 7.438101 | 7.106725 | 7.134504 | 9.425805 | 7.183635 | 7.557058 | 8.383766 | 7.687456 | 7.451467 | 7.914293 | 7.726318 | 7.594381 | 7.872106 | 8.12844 | 7.822101 |
hep-th/0004094 | Miguel Vazquez Mozo | A. Feinstein, K.E. Kunze and M.A. Vazquez-Mozo | Entropy generation and inflation in wave collision induced pre-big-bang
cosmology | 10 pages, latex. 1 postscript figure included. Bound on the incoming
focal lengths extended to strong-coupling terminated inflation. Section 3
expanded. Typos corrected and reference added. Final version to appear in
Phys. Lett. B | Phys.Lett. B491 (2000) 190-198 | 10.1016/S0370-2693(00)01021-2 | EHU-FT/0005, ITFA-2000-09, SPIN-2000/12 | hep-th astro-ph gr-qc | null | We study inflation and entropy generation in a recently proposed pre-big-bang
model universe produced in a collision of gravitational and dilaton waves. It
is shown that enough inflation occurs provided the incoming waves are
sufficiently weak. We also find that entropy in this model is dynamically
generated as the r... | [
{
"created": "Wed, 12 Apr 2000 19:48:36 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Sep 2000 10:08:01 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Feinstein",
"A.",
""
],
[
"Kunze",
"K. E.",
""
],
[
"Vazquez-Mozo",
"M. A.",
""
]
] | We study inflation and entropy generation in a recently proposed pre-big-bang model universe produced in a collision of gravitational and dilaton waves. It is shown that enough inflation occurs provided the incoming waves are sufficiently weak. We also find that entropy in this model is dynamically generated as the res... | 10.66554 | 11.055311 | 9.536829 | 9.983422 | 9.491899 | 10.555986 | 10.914132 | 9.766672 | 9.553201 | 11.121275 | 9.727889 | 10.203523 | 9.963306 | 9.685694 | 9.81126 | 10.232163 | 10.343495 | 9.730899 | 9.700356 | 10.032667 | 9.988133 |
1705.10323 | Sebastian Mizera | Sebastian Mizera, Guojun Zhang | A String Deformation of the Parke-Taylor Factor | 12+10 pages | Phys. Rev. D 96, 066016 (2017) | 10.1103/PhysRevD.96.066016 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Scattering amplitudes in a range of quantum field theories can be computed
using the Cachazo-He-Yuan (CHY) formalism. In theories with colour ordering,
the key ingredient is the so-called Parke-Taylor factor. In this note we give a
fully $\text{SL}(2,\mathbb{C})$-covariant definition and study the properties
of a new... | [
{
"created": "Mon, 29 May 2017 18:00:01 GMT",
"version": "v1"
}
] | 2017-09-20 | [
[
"Mizera",
"Sebastian",
""
],
[
"Zhang",
"Guojun",
""
]
] | Scattering amplitudes in a range of quantum field theories can be computed using the Cachazo-He-Yuan (CHY) formalism. In theories with colour ordering, the key ingredient is the so-called Parke-Taylor factor. In this note we give a fully $\text{SL}(2,\mathbb{C})$-covariant definition and study the properties of a new i... | 5.801922 | 5.864512 | 6.789976 | 5.543947 | 6.200623 | 5.489857 | 5.949968 | 5.441648 | 5.605983 | 6.633914 | 5.658577 | 5.337077 | 5.732951 | 5.433305 | 5.371336 | 5.368716 | 5.154653 | 5.335225 | 5.28621 | 5.789797 | 5.391277 |
0804.1876 | Koichi Murakami | Nobuyuki Ishibashi, Yutaka Baba, Koichi Murakami | D-branes and Closed String Field Theory | 8 pages, 2 figures, based on an invited talk presented at the
international workshop "Progress of String Theory and Quantum Field Theory"
(Osaka City University, December 7-10, 2007), to be published in the
proceedings | Int.J.Mod.Phys.A23:2220-2228,2008 | 10.1142/S0217751X0804086X | UTHEP-558, RIKEN-TH-127 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct solitonic states in the OSp invariant string field theory, which
are BRST invariant in the leading order of regularization parameter. One can
show that these solitonic states describe D-branes and ghost D-branes, by
calculating the scattering amplitudes.
| [
{
"created": "Fri, 11 Apr 2008 11:03:29 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Ishibashi",
"Nobuyuki",
""
],
[
"Baba",
"Yutaka",
""
],
[
"Murakami",
"Koichi",
""
]
] | We construct solitonic states in the OSp invariant string field theory, which are BRST invariant in the leading order of regularization parameter. One can show that these solitonic states describe D-branes and ghost D-branes, by calculating the scattering amplitudes. | 14.778633 | 7.190986 | 16.779137 | 7.674688 | 6.882796 | 7.166354 | 6.645256 | 7.758282 | 7.96993 | 14.013634 | 8.381643 | 10.062246 | 13.267076 | 10.512269 | 10.259191 | 9.914114 | 9.945741 | 10.814618 | 10.619623 | 13.516278 | 10.14127 |
hep-th/0006211 | Parthasarathi Majumdar | Saurya Das, Romesh K Kaul and Parthasarathi Majumdar | A new holographic entropy bound from quantum geometry | 4 pages revtex, no figures; some additions made in text, leading to
stronger results; minor changes in the list of references | Phys.Rev. D63 (2001) 044019 | 10.1103/PhysRevD.63.044019 | CGPG-00/6-5 | hep-th gr-qc | null | A new entropy bound, tighter than the standard holographic bound due to
Bekenstein, is derived for spacetimes with non-rotating isolated horizons, from
the quantum geometry approach in which the horizon is described by the boundary
degrees of freedom of a three dimensional Chern Simons theory.
| [
{
"created": "Tue, 27 Jun 2000 14:05:15 GMT",
"version": "v1"
},
{
"created": "Sat, 5 Aug 2000 09:58:49 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Das",
"Saurya",
""
],
[
"Kaul",
"Romesh K",
""
],
[
"Majumdar",
"Parthasarathi",
""
]
] | A new entropy bound, tighter than the standard holographic bound due to Bekenstein, is derived for spacetimes with non-rotating isolated horizons, from the quantum geometry approach in which the horizon is described by the boundary degrees of freedom of a three dimensional Chern Simons theory. | 9.519382 | 9.656749 | 8.576829 | 7.652557 | 9.515121 | 10.018251 | 11.040174 | 8.139585 | 8.878193 | 8.003543 | 9.130947 | 7.519911 | 7.78903 | 7.792596 | 8.031734 | 7.728911 | 7.860013 | 7.970383 | 7.89406 | 7.671929 | 7.709188 |
2107.01781 | Changhyun Ahn | Changhyun Ahn | Adding Complex Fermions to the Grassmannian-like Coset Model | 85 pages | null | 10.1140/epjc/s10052-021-09858-3 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In the ${\cal N}=2$ supersymmetric coset model, $\frac{SU(N+M)_k \times SO(2
N M)_1}{ SU(N)_{k+M} \times U(1)_{ N M (N+M)(k+N+M)}}$, we construct the
$SU(M)$ nonsinglet ${\cal N}=2$ multiplet of spins $(1, \frac{3}{2},
\frac{3}{2}, 2)$ in terms of coset fields. The next $SU(M)$ singlet and
nonsinglet ${\cal N}=2$ mul... | [
{
"created": "Mon, 5 Jul 2021 04:23:40 GMT",
"version": "v1"
}
] | 2022-01-05 | [
[
"Ahn",
"Changhyun",
""
]
] | In the ${\cal N}=2$ supersymmetric coset model, $\frac{SU(N+M)_k \times SO(2 N M)_1}{ SU(N)_{k+M} \times U(1)_{ N M (N+M)(k+N+M)}}$, we construct the $SU(M)$ nonsinglet ${\cal N}=2$ multiplet of spins $(1, \frac{3}{2}, \frac{3}{2}, 2)$ in terms of coset fields. The next $SU(M)$ singlet and nonsinglet ${\cal N}=2$ multi... | 3.804287 | 3.718086 | 4.292509 | 3.606256 | 3.886339 | 3.641039 | 3.68289 | 3.711467 | 3.731996 | 4.375186 | 3.619578 | 3.708763 | 3.932386 | 3.632586 | 3.693267 | 3.690045 | 3.698653 | 3.68679 | 3.70919 | 3.893188 | 3.700028 |
1411.2803 | Gianmassimo Tasinato | Gianmassimo Tasinato | A scenario for inflationary magnetogenesis without strong coupling
problem | 9 pages plus appendixes, no figures. Streamlined discussion,
reference to previous literature better acknowledged | null | 10.1088/1475-7516/2015/03/040 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Cosmological magnetic fields pervade the entire universe, from small to large
scales. Since they apparently extend into the intergalactic medium, it is
tantalizing to believe that they have a primordial origin, possibly being
produced during inflation. However, finding consistent scenarios for
inflationary magnetogen... | [
{
"created": "Tue, 11 Nov 2014 13:36:45 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Nov 2014 10:31:41 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Nov 2014 16:11:55 GMT",
"version": "v3"
},
{
"created": "Tue, 3 Mar 2015 18:54:09 GMT",
"version": "v4"
}
] | 2015-06-23 | [
[
"Tasinato",
"Gianmassimo",
""
]
] | Cosmological magnetic fields pervade the entire universe, from small to large scales. Since they apparently extend into the intergalactic medium, it is tantalizing to believe that they have a primordial origin, possibly being produced during inflation. However, finding consistent scenarios for inflationary magnetogenes... | 7.477279 | 8.596066 | 7.998766 | 7.907082 | 8.29086 | 8.763901 | 8.35595 | 8.727819 | 8.142757 | 7.95521 | 8.001875 | 7.614896 | 7.718197 | 7.614449 | 7.830104 | 7.493971 | 7.547738 | 7.532107 | 7.611278 | 7.406566 | 7.688944 |
1005.0049 | Andrei Mikhailov | Oscar A. Bedoya, L. Ibiapina Bevil\'aqua, Andrei Mikhailov, Victor O.
Rivelles | Notes on beta-deformations of the pure spinor superstring in AdS(5) x
S(5) | LaTeX, 74pp. | Nucl.Phys.B848:155-215,2011 | 10.1016/j.nuclphysb.2011.02.012 | IF-USP 1652, IPMU10-0070, ITEP-TH-20/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the properties of the vertex operator for the beta-deformation of
the superstring in AdS(5) x S(5) in the pure spinor formalism. We discuss the
action of supersymmetry on the infinitesimal beta-deformation, the application
of the homological perturbation theory, and the relation between the worldsheet
descri... | [
{
"created": "Sat, 1 May 2010 06:29:00 GMT",
"version": "v1"
}
] | 2015-03-17 | [
[
"Bedoya",
"Oscar A.",
""
],
[
"Beviláqua",
"L. Ibiapina",
""
],
[
"Mikhailov",
"Andrei",
""
],
[
"Rivelles",
"Victor O.",
""
]
] | We study the properties of the vertex operator for the beta-deformation of the superstring in AdS(5) x S(5) in the pure spinor formalism. We discuss the action of supersymmetry on the infinitesimal beta-deformation, the application of the homological perturbation theory, and the relation between the worldsheet descript... | 7.450087 | 5.753994 | 9.119217 | 5.782846 | 5.580932 | 6.787707 | 6.120561 | 5.844022 | 5.631922 | 11.654386 | 5.754611 | 5.866536 | 7.343772 | 6.211211 | 6.210818 | 6.162055 | 6.373413 | 6.191535 | 6.111714 | 7.62275 | 6.089648 |
0911.0148 | Hesam Soltanpanahi | Hesam Soltanpanahi | Near Horizon of 5D Rotating Black Holes from 2D Perspective | The last version to appear in the European Physical Journal C | Eur. Phys. J. C (2014) 74:2817 | 10.1140/epjc/s10052-014-2817-3 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the CFT dual to five dimensional extremal rotating black holes, by
investigating the two dimensional perspective of their near horizon geometry.
From two dimensional point of view, we show that both gauge fields, related to
the two rotations, appear in the same manner in the asymptotic symmetry and in
the as... | [
{
"created": "Sun, 1 Nov 2009 10:35:48 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Apr 2010 05:28:11 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Mar 2014 10:16:49 GMT",
"version": "v3"
}
] | 2014-04-01 | [
[
"Soltanpanahi",
"Hesam",
""
]
] | We study the CFT dual to five dimensional extremal rotating black holes, by investigating the two dimensional perspective of their near horizon geometry. From two dimensional point of view, we show that both gauge fields, related to the two rotations, appear in the same manner in the asymptotic symmetry and in the asso... | 9.629754 | 8.860057 | 10.105371 | 9.138938 | 9.162075 | 8.387204 | 9.12498 | 8.720778 | 9.053228 | 10.478771 | 9.347912 | 9.134368 | 9.667548 | 8.9873 | 9.246354 | 9.244919 | 9.078979 | 8.776939 | 9.2443 | 9.621702 | 8.76368 |
hep-th/0408245 | Sebastian Uhlmann | Sebastian Uhlmann (MIT) | A Note on kappa-Diagonal Surface States | 1+18 pages, 6 figures, LaTeX | JHEP 0411:003,2004 | 10.1088/1126-6708/2004/11/003 | null | hep-th | null | We classify all twist-even squeezed states in string field theory which are
diagonal in the kappa-basis and simultaneously surface states. For this
purpose, we derive a consistency condition for the maps defining kappa-diagonal
surface states. It restricts these maps to a two-parameter family of Jacobi
sine functions... | [
{
"created": "Tue, 31 Aug 2004 19:16:16 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Uhlmann",
"Sebastian",
"",
"MIT"
]
] | We classify all twist-even squeezed states in string field theory which are diagonal in the kappa-basis and simultaneously surface states. For this purpose, we derive a consistency condition for the maps defining kappa-diagonal surface states. It restricts these maps to a two-parameter family of Jacobi sine functions. ... | 26.609589 | 28.810001 | 28.225819 | 21.079113 | 23.793432 | 20.831238 | 27.095999 | 21.106909 | 25.048668 | 27.674242 | 21.459524 | 23.41888 | 24.773073 | 23.761383 | 24.119959 | 23.556559 | 24.048275 | 23.504374 | 23.777157 | 25.0084 | 24.139502 |
1110.4728 | Anastasia Doikou | Jean Avan, Anastasia Doikou | Liouville integrable defects: the non-linear Schrodinger paradigm | 22 pages, Latex. Minor misprints corrected | JHEP 01 (2012) 040 | 10.1007/JHEP01(2012)040 | null | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A systematic approach to Liouville integrable defects is proposed, based on
an underlying Poisson algebraic structure. The non-linear Schrodinger model in
the presence of a single particle-like defect is investigated through this
algebraic approach. Local integrals of motions are constructed as well as the
time compo... | [
{
"created": "Fri, 21 Oct 2011 08:13:34 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Oct 2011 13:24:20 GMT",
"version": "v2"
},
{
"created": "Tue, 10 Jan 2012 12:20:45 GMT",
"version": "v3"
},
{
"created": "Tue, 14 Feb 2012 16:17:56 GMT",
"version": "v4"
}
] | 2012-02-15 | [
[
"Avan",
"Jean",
""
],
[
"Doikou",
"Anastasia",
""
]
] | A systematic approach to Liouville integrable defects is proposed, based on an underlying Poisson algebraic structure. The non-linear Schrodinger model in the presence of a single particle-like defect is investigated through this algebraic approach. Local integrals of motions are constructed as well as the time compone... | 11.040293 | 10.900352 | 11.811183 | 10.200632 | 10.875461 | 10.903791 | 10.313298 | 10.407974 | 10.7224 | 12.714863 | 10.687098 | 10.55474 | 11.81725 | 10.864529 | 10.346524 | 10.191402 | 10.73704 | 10.80194 | 10.662741 | 11.699924 | 10.698605 |
1607.01178 | Rohit Mishra | Avirup Ghosh, Rohit Mishra | Generalized geodesic deviation equations and an entanglement first law
for rotating BTZ black holes | 25 pages, 4 figures, portion containing first law completely revised | Phys. Rev. D 94, 126005 (2016) | 10.1103/PhysRevD.94.126005 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The change in Holographic entanglement entropy (HEE) for small fluctuations
about pure AdS is given by a perturbative expansion of the area functional in
terms of the change in the bulk metric and the embedded extremal surface.
However it is known that change in the embedding appear at second order or
higher. In this... | [
{
"created": "Tue, 5 Jul 2016 10:21:05 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Dec 2016 12:38:24 GMT",
"version": "v2"
}
] | 2016-12-09 | [
[
"Ghosh",
"Avirup",
""
],
[
"Mishra",
"Rohit",
""
]
] | The change in Holographic entanglement entropy (HEE) for small fluctuations about pure AdS is given by a perturbative expansion of the area functional in terms of the change in the bulk metric and the embedded extremal surface. However it is known that change in the embedding appear at second order or higher. In this p... | 9.166154 | 8.886045 | 10.344736 | 9.055417 | 9.258372 | 9.32482 | 9.296906 | 8.981163 | 8.853251 | 10.877432 | 8.713999 | 9.12133 | 9.477852 | 9.175678 | 9.325428 | 9.428736 | 9.428635 | 8.924909 | 9.251054 | 9.422176 | 8.944956 |
0909.1389 | Raimar Wulkenhaar | Harald Grosse (Vienna) and Raimar Wulkenhaar (M\"unster) | Progress in solving a noncommutative quantum field theory in four
dimensions | 15 pages, LaTeX with xy-pic | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the noncommutative \phi^4_4-quantum field theory at the self-duality
point. This model is renormalisable to all orders as shown in earlier work of
us and does not have a Landau ghost problem. Using the Ward identity of
Disertori, Gurau, Magnen and Rivasseau, we obtain from the Schwinger-Dyson
equation a non-... | [
{
"created": "Tue, 8 Sep 2009 18:09:00 GMT",
"version": "v1"
}
] | 2009-09-09 | [
[
"Grosse",
"Harald",
"",
"Vienna"
],
[
"Wulkenhaar",
"Raimar",
"",
"Münster"
]
] | We study the noncommutative \phi^4_4-quantum field theory at the self-duality point. This model is renormalisable to all orders as shown in earlier work of us and does not have a Landau ghost problem. Using the Ward identity of Disertori, Gurau, Magnen and Rivasseau, we obtain from the Schwinger-Dyson equation a non-li... | 6.823926 | 7.213778 | 7.350349 | 6.58402 | 7.954629 | 7.711423 | 7.38469 | 7.235849 | 7.792572 | 8.45557 | 7.316513 | 6.730069 | 6.963881 | 6.691711 | 6.946863 | 6.887333 | 6.715788 | 6.922791 | 6.593723 | 7.119713 | 6.668679 |
2312.00876 | Bin Zhu | Tomasz R. Taylor, Bin Zhu | w(1+infinity) Algebra with a Cosmological Constant and the Celestial
Sphere | null | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that in the presence of a nonvanishing cosmological constant,
Strominger's infinite-dimensional $\mathrm{w_{1+\infty}}$ algebra of soft
graviton symmetries is modified in a simple way. The deformed algebra contains
a subalgebra generating $ SO(1,4)$ or $SO(2,3)$ symmetry groups of
$\text{dS}_4$ or $\text{... | [
{
"created": "Fri, 1 Dec 2023 19:04:03 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Dec 2023 20:13:04 GMT",
"version": "v2"
}
] | 2023-12-12 | [
[
"Taylor",
"Tomasz R.",
""
],
[
"Zhu",
"Bin",
""
]
] | It is shown that in the presence of a nonvanishing cosmological constant, Strominger's infinite-dimensional $\mathrm{w_{1+\infty}}$ algebra of soft graviton symmetries is modified in a simple way. The deformed algebra contains a subalgebra generating $ SO(1,4)$ or $SO(2,3)$ symmetry groups of $\text{dS}_4$ or $\text{Ad... | 5.427942 | 4.532089 | 5.620343 | 4.603429 | 4.879261 | 4.911224 | 4.691208 | 4.666178 | 4.679351 | 5.862791 | 4.625099 | 4.698331 | 5.006999 | 4.686296 | 4.6767 | 4.863432 | 4.895291 | 4.721662 | 4.85482 | 5.223998 | 4.728288 |
hep-th/0301233 | Yan-Gang Miao | Yan-Gang Miao and Nobuyoshi Ohta | Parent Actions, Dualities and New Weyl-invariant Actions of Bosonic
p-branes | 19 pages, 14 figures. The first section is modified slightly, and
references are added | JHEP 0304:010,2003 | 10.1088/1126-6708/2003/04/010 | OU-HET 429 | hep-th | null | By using the systematic approach of parent action method, we derive one
Weyl-noninvariant and two Weyl-invariant actions of bosonic $p$-branes ($p\geq
2$) starting from the Nambu-Goto action, and establish the duality symmetries
in this set of four actions. Moreover, we discover a new bosonic $p$-brane
action (includ... | [
{
"created": "Wed, 29 Jan 2003 08:47:53 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Mar 2003 06:45:19 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Miao",
"Yan-Gang",
""
],
[
"Ohta",
"Nobuyoshi",
""
]
] | By using the systematic approach of parent action method, we derive one Weyl-noninvariant and two Weyl-invariant actions of bosonic $p$-branes ($p\geq 2$) starting from the Nambu-Goto action, and establish the duality symmetries in this set of four actions. Moreover, we discover a new bosonic $p$-brane action (includin... | 10.421683 | 8.160251 | 9.686152 | 7.703008 | 8.307074 | 7.808022 | 7.894219 | 7.713332 | 7.587634 | 10.106714 | 7.660613 | 7.739277 | 8.877772 | 7.933959 | 7.961279 | 7.901526 | 8.024092 | 7.984973 | 7.921338 | 8.741845 | 7.820978 |
1301.0940 | Gaston Giribet | Juan Pablo Babaro, Gaston Giribet | On the description of surface operators in N=2* super Yang-Mills | 15 pages. v2 typo corrected, comments added. Invited article for MPLA | Mod. Phys. Lett. A28 (2013) 1330003 | 10.1142/S0217732313300036 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In Ref. [arXiv:1005.4469], Alday and Tachikawa observed that the Nekrasov
partition function of N=2 SU(2) superconformal gauge theories in the presence
of fundamental surface operators can be associated to conformal blocks of a 2D
CFT with affine sl(2) symmetry. This can be interpreted as the insertion of a
fundament... | [
{
"created": "Sat, 5 Jan 2013 20:40:19 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Feb 2013 21:31:12 GMT",
"version": "v2"
}
] | 2013-10-22 | [
[
"Babaro",
"Juan Pablo",
""
],
[
"Giribet",
"Gaston",
""
]
] | In Ref. [arXiv:1005.4469], Alday and Tachikawa observed that the Nekrasov partition function of N=2 SU(2) superconformal gauge theories in the presence of fundamental surface operators can be associated to conformal blocks of a 2D CFT with affine sl(2) symmetry. This can be interpreted as the insertion of a fundamental... | 5.834462 | 5.722579 | 6.897997 | 5.554152 | 5.852018 | 5.789237 | 5.561375 | 5.746977 | 5.345341 | 6.744359 | 5.200795 | 5.345452 | 5.788652 | 5.351473 | 5.395014 | 5.49427 | 5.479224 | 5.336745 | 5.410435 | 6.121592 | 5.313272 |
1010.2266 | Pavel Krtous | Valeri P. Frolov, Pavel Krtous | Charged particle in higher dimensional weakly charged rotating black
hole spacetime | 9 pages, no figures | Phys.Rev.D83:024016,2011 | 10.1103/PhysRevD.83.024016 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study charged particle motion in weakly charged higher dimensional black
holes. To describe the electromagnetic field we use a test field approximation
and use the higher dimensional Kerr-NUT-(A)dS metric as a background geometry.
It is shown that for a special configuration of the electromagnetic field the
equati... | [
{
"created": "Mon, 11 Oct 2010 23:44:01 GMT",
"version": "v1"
}
] | 2011-02-03 | [
[
"Frolov",
"Valeri P.",
""
],
[
"Krtous",
"Pavel",
""
]
] | We study charged particle motion in weakly charged higher dimensional black holes. To describe the electromagnetic field we use a test field approximation and use the higher dimensional Kerr-NUT-(A)dS metric as a background geometry. It is shown that for a special configuration of the electromagnetic field the equation... | 8.321808 | 9.574497 | 8.88297 | 8.742332 | 8.532841 | 9.642988 | 8.989398 | 8.219443 | 8.819384 | 9.652267 | 8.245435 | 8.428288 | 8.199736 | 7.977489 | 7.968442 | 7.93468 | 8.227101 | 7.725759 | 8.153145 | 8.169497 | 7.986481 |
hep-th/0604153 | Rubakov Valery | V.A. Rubakov | Phantom without UV pathology | 19 pages. Several misprints corrected, several points clarified,
several references added | Theor.Math.Phys.149:1651-1664,2006; Teor.Mat.Fiz.149:409-426,2006 | 10.1007/s11232-006-0149-7 | null | hep-th | null | We present a simple model in which the weak energy condition is violated for
spatially homogeneous, slowly evolving fields. The excitations about
Lorentz-violating background in Minkowski space do not contain ghosts, tachyons
or superluminal modes at spatial momenta ranging from some low scale epsilon to
the UV cutof... | [
{
"created": "Fri, 21 Apr 2006 18:24:13 GMT",
"version": "v1"
},
{
"created": "Wed, 17 May 2006 13:19:31 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Rubakov",
"V. A.",
""
]
] | We present a simple model in which the weak energy condition is violated for spatially homogeneous, slowly evolving fields. The excitations about Lorentz-violating background in Minkowski space do not contain ghosts, tachyons or superluminal modes at spatial momenta ranging from some low scale epsilon to the UV cutoff ... | 19.310427 | 18.21879 | 18.253725 | 17.036644 | 21.299631 | 19.063116 | 19.098663 | 17.694149 | 17.426245 | 20.344265 | 18.262644 | 18.298447 | 19.888641 | 18.485308 | 17.867947 | 17.682072 | 17.981964 | 18.138062 | 18.531912 | 19.921623 | 17.57868 |
0809.4512 | Itzhak Fouxon | Itzhak Fouxon and Yaron Oz | Conformal Field Theory as Microscopic Dynamics of Incompressible Euler
and Navier-Stokes Equations | 4 pages | Phys.Rev.Lett.101:261602,2008 | 10.1103/PhysRevLett.101.261602 | null | hep-th cond-mat.other nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the hydrodynamics of relativistic conformal field theories at
finite temperature. We show that the limit of slow motions of the ideal
hydrodynamics leads to the non-relativistic incompressible Euler equation. For
viscous hydrodynamics we show that the limit of slow motions leads to the
non-relativistic in... | [
{
"created": "Thu, 25 Sep 2008 23:33:29 GMT",
"version": "v1"
},
{
"created": "Sun, 28 Sep 2008 12:18:15 GMT",
"version": "v2"
}
] | 2009-01-14 | [
[
"Fouxon",
"Itzhak",
""
],
[
"Oz",
"Yaron",
""
]
] | We consider the hydrodynamics of relativistic conformal field theories at finite temperature. We show that the limit of slow motions of the ideal hydrodynamics leads to the non-relativistic incompressible Euler equation. For viscous hydrodynamics we show that the limit of slow motions leads to the non-relativistic inco... | 6.696614 | 6.466135 | 7.735785 | 6.342461 | 6.485469 | 6.654887 | 6.1001 | 6.365743 | 6.039209 | 7.40208 | 6.458433 | 6.608555 | 6.869012 | 6.584658 | 6.451722 | 6.653895 | 6.436734 | 6.529362 | 6.680005 | 6.617259 | 6.519351 |
1610.03733 | Robert Shrock | Robert Shrock | Study of the Six-Loop Beta Function of the $\lambda\phi^4_4$ Theory | 7 pages latex, 2 figures | Phys. Rev. D 94, 125026 (2016) | 10.1103/PhysRevD.94.125026 | YITP-SB-2016-41 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate whether the six-loop beta function of the $\lambda \phi^4_4$
theory exhibits evidence for an ultraviolet zero. As part of our analysis, we
calculate and analyze Pad\'e approximants to this beta function. Extending our
earlier results at the five-loop level, we find that in the range of $\lambda$
where ... | [
{
"created": "Wed, 12 Oct 2016 14:50:05 GMT",
"version": "v1"
}
] | 2017-01-04 | [
[
"Shrock",
"Robert",
""
]
] | We investigate whether the six-loop beta function of the $\lambda \phi^4_4$ theory exhibits evidence for an ultraviolet zero. As part of our analysis, we calculate and analyze Pad\'e approximants to this beta function. Extending our earlier results at the five-loop level, we find that in the range of $\lambda$ where th... | 6.856093 | 5.980541 | 7.092374 | 6.129668 | 5.96548 | 5.906778 | 5.771536 | 5.989896 | 5.66802 | 5.711941 | 5.792923 | 6.119973 | 6.311615 | 6.363422 | 6.148589 | 6.300716 | 6.331923 | 6.121544 | 6.281611 | 6.055715 | 6.192563 |
hep-th/0602027 | Angel Paredes | Roberto Casero, Carlos Nunez and Angel Paredes | Towards the String Dual of N=1 SQCD-like Theories | 70 pages, 5 figures; references added, minor changes | Phys.Rev.D73:086005,2006 | 10.1103/PhysRevD.73.086005 | CPHT-RR 010.0106, SWAT/06/454 | hep-th | null | We construct supergravity plus branes solutions, which we argue to be related
to 4d N=1 SQCD with a quartic superpotential. The geometries depend on the
ratio Nf/Nc which can be kept of order one, present a good singularity at the
origin and are weakly curved elsewhere. We support our field theory
interpretation by s... | [
{
"created": "Fri, 3 Feb 2006 17:54:10 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Mar 2006 10:11:22 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Casero",
"Roberto",
""
],
[
"Nunez",
"Carlos",
""
],
[
"Paredes",
"Angel",
""
]
] | We construct supergravity plus branes solutions, which we argue to be related to 4d N=1 SQCD with a quartic superpotential. The geometries depend on the ratio Nf/Nc which can be kept of order one, present a good singularity at the origin and are weakly curved elsewhere. We support our field theory interpretation by stu... | 13.628293 | 12.671293 | 15.20105 | 12.537395 | 13.242818 | 12.214746 | 12.591235 | 12.243392 | 12.514311 | 16.430393 | 12.251419 | 13.716025 | 14.860524 | 13.630289 | 12.954079 | 13.080389 | 12.700223 | 13.61196 | 13.212986 | 14.776967 | 13.158179 |
hep-th/9209054 | Sklyanin Evgueni | P. P. Kulish, E. K. Sklyanin | Algebraic Structures Related to Reflection Equations | 18 pages | J.Phys.A25:5963-5976,1992 | 10.1088/0305-4470/25/22/022 | YITP/-980 | hep-th math.QA nlin.SI solv-int | null | Quadratic algebras related to the reflection equations are introduced. They
are quantum group comodule algebras. The quantum group $F_q(GL(2))$ is taken as
the example. The properties of the algebras (center, representations,
realizations, real forms, fusion procedure etc) as well as the generalizations
are discussed... | [
{
"created": "Wed, 16 Sep 1992 03:34:32 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Kulish",
"P. P.",
""
],
[
"Sklyanin",
"E. K.",
""
]
] | Quadratic algebras related to the reflection equations are introduced. They are quantum group comodule algebras. The quantum group $F_q(GL(2))$ is taken as the example. The properties of the algebras (center, representations, realizations, real forms, fusion procedure etc) as well as the generalizations are discussed. | 13.191743 | 12.684376 | 14.996801 | 11.68326 | 11.385346 | 11.090751 | 10.710804 | 10.647288 | 10.778591 | 16.287651 | 11.542181 | 11.151783 | 13.24895 | 11.684282 | 11.498068 | 10.776424 | 10.859568 | 11.531218 | 11.805323 | 13.31694 | 10.572247 |
1406.5155 | Yu-tin Huang | Massimo Bianchi, Song He, Yu-tin Huang, Congkao Wen | More on Soft Theorems: Trees, Loops and Strings | 40 pages. V2, typos and references corrected | Phys. Rev. D 92, 065022 (2015) | 10.1103/PhysRevD.92.065022 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study soft theorems in a broader context, addressing their fate at loop
level and their universality in effective field theories and string theory. We
argue that for gauge theories in the planar limit, loop-level soft gluon
theorems can be made manifest already at the integrand level. In particular, we
show that t... | [
{
"created": "Thu, 19 Jun 2014 19:08:17 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Jun 2014 19:54:16 GMT",
"version": "v2"
}
] | 2015-09-30 | [
[
"Bianchi",
"Massimo",
""
],
[
"He",
"Song",
""
],
[
"Huang",
"Yu-tin",
""
],
[
"Wen",
"Congkao",
""
]
] | We study soft theorems in a broader context, addressing their fate at loop level and their universality in effective field theories and string theory. We argue that for gauge theories in the planar limit, loop-level soft gluon theorems can be made manifest already at the integrand level. In particular, we show that the... | 7.401711 | 7.928984 | 8.230404 | 7.364951 | 7.912663 | 7.835305 | 7.753375 | 7.207281 | 7.397092 | 8.687091 | 7.083066 | 7.56488 | 7.417407 | 7.226276 | 7.329302 | 7.413749 | 7.306441 | 7.286249 | 7.209786 | 7.469815 | 7.197434 |
1904.05580 | Timofey Snegirev | I. L. Buchbinder, M. V. Khabarov, T. V. Snegirev, Yu. M. Zinoviev | Lagrangian formulation for the infinite spin N=1 supermultiplets in d=4 | 1+12 pages, no figures | null | 10.1016/j.nuclphysb.2019.114717 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide an explicit Lagrangian construction for the massless infinite spin
N=1 supermultiplet in four dimensional Minkowski space. Such a supermultiplet
contains a pair of massless bosonic and a pair of massless fermionic infinite
spin fields with properly adjusted dimensionful parameters. We begin with the
gauge ... | [
{
"created": "Thu, 11 Apr 2019 08:50:11 GMT",
"version": "v1"
}
] | 2019-09-04 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Khabarov",
"M. V.",
""
],
[
"Snegirev",
"T. V.",
""
],
[
"Zinoviev",
"Yu. M.",
""
]
] | We provide an explicit Lagrangian construction for the massless infinite spin N=1 supermultiplet in four dimensional Minkowski space. Such a supermultiplet contains a pair of massless bosonic and a pair of massless fermionic infinite spin fields with properly adjusted dimensionful parameters. We begin with the gauge in... | 6.087445 | 4.752184 | 5.931902 | 5.312721 | 5.433222 | 5.128026 | 4.64466 | 4.94678 | 4.959749 | 6.545358 | 4.940891 | 5.385362 | 6.161112 | 5.476658 | 5.210342 | 5.290765 | 5.219026 | 5.378924 | 5.276757 | 5.95373 | 5.431011 |
1711.09839 | Kenta Suzuki | Sumit R. Das, Animik Ghosh, Antal Jevicki, Kenta Suzuki | Three Dimensional View of Arbitrary $q$ SYK models | 17 pages, 1 figure | null | 10.1007/JHEP02(2018)162 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In \url{arXiv:1704.07208} it was shown that the spectrum and bilocal
propagator of SYK model with four fermion interactions can be realized as a
three dimensional model in $AdS_2 \times S^1/Z_2$ with nontrivial boundary
conditions in the additional dimension. In this paper we show that a similar
picture holds for gen... | [
{
"created": "Mon, 27 Nov 2017 17:17:52 GMT",
"version": "v1"
}
] | 2018-04-04 | [
[
"Das",
"Sumit R.",
""
],
[
"Ghosh",
"Animik",
""
],
[
"Jevicki",
"Antal",
""
],
[
"Suzuki",
"Kenta",
""
]
] | In \url{arXiv:1704.07208} it was shown that the spectrum and bilocal propagator of SYK model with four fermion interactions can be realized as a three dimensional model in $AdS_2 \times S^1/Z_2$ with nontrivial boundary conditions in the additional dimension. In this paper we show that a similar picture holds for gener... | 7.053092 | 6.909958 | 7.514501 | 6.659669 | 7.086258 | 7.316075 | 7.195113 | 7.101659 | 6.509077 | 7.192081 | 6.755983 | 6.384843 | 6.86749 | 6.535454 | 6.583598 | 6.559418 | 6.520632 | 6.519063 | 6.515645 | 6.849787 | 6.442266 |
2211.09181 | Keshav Dasgupta | Suddhasattwa Brahma, Keshav Dasgupta, Mir-Mehedi Faruk, Bohdan
Kulinich, Viraj Meruliya, Brent Pym, Radu Tatar | Resurgence of a de Sitter Glauber-Sudarshan State: Nodal Diagrams and
Borel Resummation | 116 pages, 16 pdf figures, comments welcome; v2: Typos corrected,
references updated, final version appearing in Fortschritte der Physik | Fortsch. Phys, 2023, 2300136 | 10.1002/prop.202300136 | null | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We show that an explicit construction of a four-dimensional de Sitter space
may be performed using a diagrammatic approach via nodal diagrams emanating
from the path integral representation of the Glauber-Sudarshan state. Sum of
these diagrams typically leads to an asymptotic series of Gevrey kind which can
then be B... | [
{
"created": "Wed, 16 Nov 2022 20:04:51 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Oct 2023 12:52:26 GMT",
"version": "v2"
}
] | 2023-10-26 | [
[
"Brahma",
"Suddhasattwa",
""
],
[
"Dasgupta",
"Keshav",
""
],
[
"Faruk",
"Mir-Mehedi",
""
],
[
"Kulinich",
"Bohdan",
""
],
[
"Meruliya",
"Viraj",
""
],
[
"Pym",
"Brent",
""
],
[
"Tatar",
"Radu",
""
]
] | We show that an explicit construction of a four-dimensional de Sitter space may be performed using a diagrammatic approach via nodal diagrams emanating from the path integral representation of the Glauber-Sudarshan state. Sum of these diagrams typically leads to an asymptotic series of Gevrey kind which can then be Bor... | 12.343072 | 11.434736 | 12.442757 | 11.362017 | 11.255002 | 11.744537 | 11.554526 | 11.173399 | 11.733807 | 14.383911 | 11.198786 | 11.547802 | 11.949313 | 11.6565 | 11.291143 | 11.432681 | 11.371784 | 11.736288 | 11.552356 | 11.910471 | 11.232952 |
2309.06469 | Valentin Reys | Nikolay Bobev, Junho Hong, Valentin Reys | Holographic Thermal Observables and M2-branes | 22 pages; v2: additional comments included, accepted for publication
in JHEP | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use holography in conjunction with recent results from supersymmetric
localization to compute certain thermal observables for 3d $\mathcal{N}=2$
holographic SCFTs arising on the worldvolume of $N$ M2-branes. We obtain
results for the thermal free energy density on $S^1 \times \mathbb{R}^2$, the
Casimir energy on $... | [
{
"created": "Tue, 12 Sep 2023 18:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Nov 2023 09:46:14 GMT",
"version": "v2"
}
] | 2023-11-28 | [
[
"Bobev",
"Nikolay",
""
],
[
"Hong",
"Junho",
""
],
[
"Reys",
"Valentin",
""
]
] | We use holography in conjunction with recent results from supersymmetric localization to compute certain thermal observables for 3d $\mathcal{N}=2$ holographic SCFTs arising on the worldvolume of $N$ M2-branes. We obtain results for the thermal free energy density on $S^1 \times \mathbb{R}^2$, the Casimir energy on $T^... | 4.399663 | 3.930172 | 4.967881 | 3.993773 | 3.909851 | 3.808445 | 3.94148 | 4.035245 | 3.995221 | 4.64212 | 4.024565 | 4.000467 | 4.232997 | 4.093368 | 4.084079 | 4.096564 | 4.044705 | 4.073574 | 4.017078 | 4.329965 | 4.084168 |
2112.09049 | James Ingoldby | Joan Elias Miro, James Ingoldby | Hamiltonian Truncation with Larger Dimensions | 42 pages, 3 figures. To match published version | null | null | null | hep-th cond-mat.stat-mech hep-lat hep-ph | http://creativecommons.org/licenses/by/4.0/ | Hamiltonian Truncation (HT) is a numerical approach for calculating
observables in a Quantum Field Theory non-perturbatively. This approach can be
applied to theories constructed by deforming a conformal field theory with a
relevant operator of scaling dimension $\Delta$. UV divergences arise when
$\Delta$ is larger ... | [
{
"created": "Thu, 16 Dec 2021 17:39:26 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Apr 2022 12:40:33 GMT",
"version": "v2"
}
] | 2022-04-27 | [
[
"Miro",
"Joan Elias",
""
],
[
"Ingoldby",
"James",
""
]
] | Hamiltonian Truncation (HT) is a numerical approach for calculating observables in a Quantum Field Theory non-perturbatively. This approach can be applied to theories constructed by deforming a conformal field theory with a relevant operator of scaling dimension $\Delta$. UV divergences arise when $\Delta$ is larger th... | 6.871669 | 6.933012 | 7.807175 | 6.639081 | 6.951931 | 6.756691 | 6.4629 | 6.612576 | 6.618498 | 7.698112 | 6.58784 | 6.519811 | 6.851769 | 6.457178 | 6.473906 | 6.491028 | 6.379883 | 6.4609 | 6.361291 | 6.955277 | 6.421557 |
hep-th/0505130 | Alin Tirziu | I.Y. Park, A. Tirziu and A.A. Tseytlin | Semiclassical circular strings in AdS_5 and "long" gauge field strength
operators | 24 pages, 3 figures, v2: typos corrected; v3: misprint in eq.(2.15)
corrected | Phys.Rev.D71:126008,2005 | 10.1103/PhysRevD.71.126008 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider circular strings rotating with equal spins S_1=S_2=S in two
orthogonal planes in AdS_5 and suggest that they may be dual to "long" gauge
theory operators built out of self-dual components of gauge field strength. As
was found in hep-th/0404187, the one-loop anomalous dimensions of the such
gauge-theory op... | [
{
"created": "Mon, 16 May 2005 16:36:07 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Nov 2005 17:52:46 GMT",
"version": "v2"
},
{
"created": "Tue, 16 Feb 2010 16:14:26 GMT",
"version": "v3"
}
] | 2010-02-16 | [
[
"Park",
"I. Y.",
""
],
[
"Tirziu",
"A.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We consider circular strings rotating with equal spins S_1=S_2=S in two orthogonal planes in AdS_5 and suggest that they may be dual to "long" gauge theory operators built out of self-dual components of gauge field strength. As was found in hep-th/0404187, the one-loop anomalous dimensions of the such gauge-theory oper... | 8.213573 | 8.221931 | 9.225286 | 7.628939 | 8.529369 | 7.926281 | 8.034929 | 7.279923 | 7.469248 | 9.963551 | 7.619729 | 7.940535 | 8.276837 | 7.55764 | 8.001429 | 7.872887 | 8.109652 | 7.634249 | 7.594524 | 8.032162 | 7.674973 |
1611.03498 | Hardi Veerm\"ae | Martti Raidal, Hardi Veerm\"ae | On the Quantisation of Complex Higher Derivative Theories and Avoiding
the Ostrogradsky Ghost | 23 pages, extended discussion and updated references. Accepted for
publication in Nucl.Phys.B | null | 10.1016/j.nuclphysb.2017.01.024 | null | hep-th hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Generic higher derivative theories are believed to be fundamentally
unphysical because they contain Ostrogradsky ghosts. We show that within
complex classical mechanics it is possible to construct higher derivative
theories that circumvent the Ostrogradsky theorem and have a real energy
spectrum that is bounded from ... | [
{
"created": "Thu, 10 Nov 2016 21:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Jan 2017 18:20:03 GMT",
"version": "v2"
}
] | 2017-03-08 | [
[
"Raidal",
"Martti",
""
],
[
"Veermäe",
"Hardi",
""
]
] | Generic higher derivative theories are believed to be fundamentally unphysical because they contain Ostrogradsky ghosts. We show that within complex classical mechanics it is possible to construct higher derivative theories that circumvent the Ostrogradsky theorem and have a real energy spectrum that is bounded from be... | 12.802329 | 13.847748 | 12.796158 | 12.894783 | 14.683107 | 12.139628 | 13.370308 | 13.270388 | 12.409806 | 14.293642 | 13.101962 | 12.620328 | 11.751204 | 12.431767 | 12.414372 | 12.551986 | 12.210732 | 12.538268 | 12.515934 | 12.200402 | 12.8267 |
hep-th/0512341 | Andreas Gustavsson | Andreas Gustavsson | The non-Abelian tensor multiplet in loop space | 11 pages, v2: cleaner presentation, mistakes are corrected (and an
erroneous section was removed) | JHEP0601:165,2006 | 10.1088/1126-6708/2006/01/165 | null | hep-th | null | We introduce a non-Abelian tensor multiplet directly in the loop space
associated with flat six-dimensional Minkowski space-time, and derive the
supersymmetry variations for on-shell ${\cal{N}}=(2,0)$ supersymmetry.
| [
{
"created": "Fri, 30 Dec 2005 09:27:56 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Apr 2008 08:04:04 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Gustavsson",
"Andreas",
""
]
] | We introduce a non-Abelian tensor multiplet directly in the loop space associated with flat six-dimensional Minkowski space-time, and derive the supersymmetry variations for on-shell ${\cal{N}}=(2,0)$ supersymmetry. | 11.304205 | 9.115871 | 13.482889 | 8.767835 | 9.65431 | 8.853682 | 9.47098 | 9.047006 | 8.960491 | 13.768661 | 9.325462 | 9.386465 | 11.725023 | 9.154129 | 10.153543 | 9.821413 | 9.841844 | 9.605668 | 9.597945 | 12.599484 | 9.501035 |
hep-th/0605116 | Ant\^onio Scarpelli | C. R. Pontes, A. P. Baeta Scarpelli, Marcos Sampaio, M. C. Nemes | Implicit regularization beyond one loop order: scalar field theories | 14 pages, two columns, 3 figures | null | 10.1088/0954-3899/34/10/011 | null | hep-th | null | Implicit regularization (IR) has been shown as an useful momentum space tool
for perturbative calculations in dimension specific theories, such as chiral
gauge, topological and supersymmetric quantum field theoretical models at one
loop level. In this paper, we aim at generalizing systematically IR to be
applicable b... | [
{
"created": "Thu, 11 May 2006 16:26:44 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Apr 2007 09:20:07 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Pontes",
"C. R.",
""
],
[
"Scarpelli",
"A. P. Baeta",
""
],
[
"Sampaio",
"Marcos",
""
],
[
"Nemes",
"M. C.",
""
]
] | Implicit regularization (IR) has been shown as an useful momentum space tool for perturbative calculations in dimension specific theories, such as chiral gauge, topological and supersymmetric quantum field theoretical models at one loop level. In this paper, we aim at generalizing systematically IR to be applicable bey... | 14.924621 | 12.665014 | 13.133416 | 13.024703 | 13.257593 | 13.674479 | 13.800971 | 13.467169 | 12.526481 | 15.398302 | 13.146211 | 12.762856 | 13.852757 | 12.883901 | 13.374329 | 12.946974 | 13.020332 | 13.306232 | 12.586187 | 13.920619 | 14.033882 |
2304.14650 | Debabrata Ghorai | Debabrata Ghorai, Taewon Yuk, Sang-Jin Sin | Fermi arc in $p$-wave holographic superconductors | 21 pages, 14 figures, accepted version in JHEP | null | null | null | hep-th cond-mat.supr-con gr-qc | http://creativecommons.org/licenses/by/4.0/ | We have investigated the fermionic spectral function in $p$-wave holographic
superconductors. We show that the vector model with minimal coupling reveals a
$p$-wave spectral function with Fermi arc. This should be contrasted with the
previous investigation where $p$-wave arc was demonstrated in the presence of a
tens... | [
{
"created": "Fri, 28 Apr 2023 06:38:09 GMT",
"version": "v1"
},
{
"created": "Mon, 1 May 2023 09:00:44 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Sep 2023 14:16:44 GMT",
"version": "v3"
}
] | 2023-09-06 | [
[
"Ghorai",
"Debabrata",
""
],
[
"Yuk",
"Taewon",
""
],
[
"Sin",
"Sang-Jin",
""
]
] | We have investigated the fermionic spectral function in $p$-wave holographic superconductors. We show that the vector model with minimal coupling reveals a $p$-wave spectral function with Fermi arc. This should be contrasted with the previous investigation where $p$-wave arc was demonstrated in the presence of a tensor... | 11.661923 | 10.530389 | 11.444983 | 10.045722 | 10.639049 | 9.596698 | 10.136694 | 9.972816 | 10.165072 | 12.652155 | 9.914314 | 11.024055 | 11.265695 | 10.569267 | 10.659986 | 10.666303 | 10.252656 | 10.342326 | 10.598417 | 11.365758 | 10.535378 |
0712.2164 | George Siopsis | James Alsup and George Siopsis | Bjorken flow from an AdS Schwarzschild black hole | 5 pages in two-column RevTeX; sharpened discussion to appear in PRL | Phys.Rev.Lett.101:031602,2008 | 10.1103/PhysRevLett.101.031602 | UTHET-07-1101 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a large black hole in asymptotically AdS spacetime of arbitrary
dimension with a Minkowski boundary. By performing an appropriate slicing as we
approach the boundary, we obtain via holographic renormalization a gauge theory
fluid obeying Bjorken hydrodynamics in the limit of large longitudinal proper
time... | [
{
"created": "Thu, 13 Dec 2007 15:06:59 GMT",
"version": "v1"
},
{
"created": "Sat, 5 Jul 2008 05:48:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Alsup",
"James",
""
],
[
"Siopsis",
"George",
""
]
] | We consider a large black hole in asymptotically AdS spacetime of arbitrary dimension with a Minkowski boundary. By performing an appropriate slicing as we approach the boundary, we obtain via holographic renormalization a gauge theory fluid obeying Bjorken hydrodynamics in the limit of large longitudinal proper time. ... | 10.375163 | 10.583209 | 10.478631 | 9.916381 | 10.064456 | 10.810074 | 11.344322 | 10.272689 | 10.086222 | 11.844741 | 9.621443 | 10.036916 | 10.488232 | 9.882123 | 10.266386 | 9.503583 | 9.981121 | 9.731787 | 9.691138 | 10.510631 | 9.876428 |
hep-th/0105108 | Andreas Karch | Andreas Karch and Lisa Randall | Localized Gravity in String Theory | 4 pages, Revtex, a typo corrected and references added | Phys.Rev.Lett.87:061601,2001 | 10.1103/PhysRevLett.87.061601 | MIT-CTP-3147 | hep-th hep-ph | null | We propose a string realization of the AdS4 brane in AdS5 that is known to
localize gravity. Our theory is M D5 branes in the near horizon geometry of N
D3 branes, where M and N are appropriately tuned.
| [
{
"created": "Fri, 11 May 2001 18:23:53 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Jun 2001 21:58:17 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Karch",
"Andreas",
""
],
[
"Randall",
"Lisa",
""
]
] | We propose a string realization of the AdS4 brane in AdS5 that is known to localize gravity. Our theory is M D5 branes in the near horizon geometry of N D3 branes, where M and N are appropriately tuned. | 14.630168 | 10.510726 | 18.485432 | 10.6732 | 10.069283 | 10.720886 | 10.11308 | 11.245654 | 10.237397 | 14.639236 | 10.47033 | 11.141246 | 16.658285 | 10.906825 | 10.325908 | 10.526568 | 10.841123 | 11.208734 | 10.781639 | 14.995138 | 10.910579 |
2309.05268 | Augusto Sagnotti Prof. | J. Mourad (APC, U. Paris Cit\'e), A. Sagnotti (Scuola Normale
Superiore and INFN, Pisa) | Effective Orientifolds from Broken Supersymmetry | 23 pages, LaTeX. Comments added. Final version to appear in the
special issue of Journal of Physics A: Mathematical and Theoretical on
"Fields, Gravity, Strings and Beyond: In Memory of Stanley Deser'' | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We recently proposed a class of type IIB vacua that yield, at low energies,
four--dimensional Minkowski spaces with broken supersymmetry and a constant
string coupling. They are compactifications with an internal five-torus bearing
a five--form flux $\Phi$ and warp factors depending on a single coordinate. The
breaki... | [
{
"created": "Mon, 11 Sep 2023 06:56:35 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Dec 2023 21:28:15 GMT",
"version": "v2"
}
] | 2023-12-20 | [
[
"Mourad",
"J.",
"",
"APC, U. Paris Cité"
],
[
"Sagnotti",
"A.",
"",
"Scuola Normale\n Superiore and INFN, Pisa"
]
] | We recently proposed a class of type IIB vacua that yield, at low energies, four--dimensional Minkowski spaces with broken supersymmetry and a constant string coupling. They are compactifications with an internal five-torus bearing a five--form flux $\Phi$ and warp factors depending on a single coordinate. The breaking... | 14.352296 | 15.889031 | 15.892426 | 13.889046 | 16.528318 | 16.048891 | 15.777622 | 14.418308 | 14.420157 | 18.01935 | 14.11517 | 13.840687 | 14.643799 | 13.913018 | 13.719171 | 14.142666 | 14.464928 | 14.160584 | 13.958603 | 14.778358 | 14.062353 |
hep-th/9111020 | null | Michelle Bourdeau, Eli J. Mlawer, Harold Riggs, and Howard J.
Schnitzer | Topological Landau-Ginzburg Matter from Sp(N)_{K} Fusion Rings | 13 pages | Mod.Phys.Lett. A7 (1992) 689-700 | 10.1142/S0217732392000665 | null | hep-th | null | We find and analyze the Landau-Ginzburg potentials whose critical points
determine chiral rings which are exactly the fusion rings of Sp(N)_{K} WZW
models. The quasi-homogeneous part of the potential associated with Sp(N)_{K}
is the same as the quasi-homogeneous part of that associated with SU(N+1)_{K},
showing that ... | [
{
"created": "Fri, 8 Nov 1991 23:30:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Bourdeau",
"Michelle",
""
],
[
"Mlawer",
"Eli J.",
""
],
[
"Riggs",
"Harold",
""
],
[
"Schnitzer",
"Howard J.",
""
]
] | We find and analyze the Landau-Ginzburg potentials whose critical points determine chiral rings which are exactly the fusion rings of Sp(N)_{K} WZW models. The quasi-homogeneous part of the potential associated with Sp(N)_{K} is the same as the quasi-homogeneous part of that associated with SU(N+1)_{K}, showing that th... | 6.677617 | 6.70081 | 7.885531 | 6.433581 | 6.619127 | 6.533329 | 6.736029 | 6.889575 | 6.31277 | 7.684977 | 6.423746 | 6.438636 | 6.957992 | 6.522275 | 6.579059 | 6.391151 | 6.384725 | 6.469786 | 6.204596 | 6.71788 | 6.286895 |
hep-th/9301090 | Kanehisa Takasaki | Kanehisa Takasaki | Quasi-classical limit of BKP hierarchy and W-infinity symmeties | 12 pages, Kyoto University KUCP-0058/93 | Lett.Math.Phys. 28 (1993) 177-186 | 10.1007/BF00745149 | null | hep-th | null | Previous results on quasi-classical limit of the KP and Toda hierarchies are
now extended to the BKP hierarchy. Basic tools such as the Lax representation,
the Baker-Akhiezer function and the tau function are reformulated so as to fit
into the analysis of quasi-classical limit. Two subalgebras $\WB_{1+\infty}$
and $\... | [
{
"created": "Fri, 22 Jan 1993 05:43:42 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Jan 1993 03:56:09 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Apr 1993 01:50:19 GMT",
"version": "v3"
}
] | 2009-10-22 | [
[
"Takasaki",
"Kanehisa",
""
]
] | Previous results on quasi-classical limit of the KP and Toda hierarchies are now extended to the BKP hierarchy. Basic tools such as the Lax representation, the Baker-Akhiezer function and the tau function are reformulated so as to fit into the analysis of quasi-classical limit. Two subalgebras $\WB_{1+\infty}$ and $\wB... | 4.722004 | 4.39663 | 4.913379 | 4.347066 | 4.298471 | 4.729394 | 4.659006 | 4.621705 | 4.249964 | 4.944541 | 4.343598 | 4.255276 | 4.534965 | 4.249076 | 4.316941 | 4.383367 | 4.369211 | 4.398546 | 4.491595 | 4.750136 | 4.407887 |
hep-th/0412155 | James T. Liu | Benjamin A. Burrington, James T. Liu, W. A. Sabra | AdS_5 Black Holes with Fermionic Hair | 22 pages, Revtex 4, references added | Phys.Rev. D71 (2005) 105015 | 10.1103/PhysRevD.71.105015 | MCTP-04-70, CAMS/04-04 | hep-th | null | The study of new BPS objects in AdS_5 has led to a deeper understanding of
AdS/CFT. To help complete this picture, and to fully explore the consequences
of the supersymmetry algebra, it is also important to obtain new solutions with
bulk fermions turned on. In this paper we construct superpartners of the 1/2
BPS blac... | [
{
"created": "Wed, 15 Dec 2004 18:00:04 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Mar 2005 20:57:17 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Burrington",
"Benjamin A.",
""
],
[
"Liu",
"James T.",
""
],
[
"Sabra",
"W. A.",
""
]
] | The study of new BPS objects in AdS_5 has led to a deeper understanding of AdS/CFT. To help complete this picture, and to fully explore the consequences of the supersymmetry algebra, it is also important to obtain new solutions with bulk fermions turned on. In this paper we construct superpartners of the 1/2 BPS black ... | 8.041198 | 8.983907 | 8.908114 | 8.375402 | 8.839803 | 8.096756 | 9.21149 | 8.248838 | 8.514747 | 9.49189 | 8.229187 | 7.740519 | 8.07524 | 7.911642 | 8.068101 | 7.832642 | 8.105711 | 7.796428 | 8.106752 | 8.455331 | 7.731808 |
hep-th/0606193 | Gianluca Grignani | Davide Astolfi, Valentina Forini, Gianluca Grignani and Gordon W.
Semenoff | Finite size corrections and integrability of $\mathcal{N}=2$ SYM and
DLCQ strings on a pp-wave | 28 pages | JHEP0609:056,2006 | 10.1088/1126-6708/2006/09/056 | null | hep-th | null | We compute the planar finite size corrections to the spectrum of the
dilatation operator acting on two-impurity states of a certain limit of
conformal $\mathcal{N}=2$ quiver gauge field theory which is a $Z_M$-orbifold
of $\mathcal{N}=4$ supersymmetric Yang-Mills theory. We match the result to the
string dual, IIB su... | [
{
"created": "Tue, 20 Jun 2006 15:15:09 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Astolfi",
"Davide",
""
],
[
"Forini",
"Valentina",
""
],
[
"Grignani",
"Gianluca",
""
],
[
"Semenoff",
"Gordon W.",
""
]
] | We compute the planar finite size corrections to the spectrum of the dilatation operator acting on two-impurity states of a certain limit of conformal $\mathcal{N}=2$ quiver gauge field theory which is a $Z_M$-orbifold of $\mathcal{N}=4$ supersymmetric Yang-Mills theory. We match the result to the string dual, IIB supe... | 5.795717 | 5.977756 | 6.972467 | 5.951143 | 6.062954 | 6.122186 | 6.267839 | 5.871194 | 5.79146 | 6.9184 | 5.442401 | 5.697979 | 6.199856 | 5.742884 | 5.779317 | 5.772431 | 5.798172 | 5.686726 | 5.754672 | 5.983633 | 5.618342 |
2203.12625 | Pierre Heidmann | Ibrahima Bah, Pierre Heidmann and Peter Weck | Schwarzschild-like Topological Solitons | 38 pages + Appendix, 15 figures; v2: typos corrected | null | 10.1007/JHEP08(2022)269 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the first class of topological solitons in gravity that are
supported by internal electromagnetic flux with vanishing net charges. The
solutions are obtained in a six-dimensional Einstein-Maxwell theory with a
three-form flux, and admit an uplift to type IIB supergravity on T$^4$. They
are asymptotic to ... | [
{
"created": "Wed, 23 Mar 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Jun 2022 08:43:29 GMT",
"version": "v2"
}
] | 2022-09-14 | [
[
"Bah",
"Ibrahima",
""
],
[
"Heidmann",
"Pierre",
""
],
[
"Weck",
"Peter",
""
]
] | We construct the first class of topological solitons in gravity that are supported by internal electromagnetic flux with vanishing net charges. The solutions are obtained in a six-dimensional Einstein-Maxwell theory with a three-form flux, and admit an uplift to type IIB supergravity on T$^4$. They are asymptotic to a ... | 9.864212 | 9.544112 | 11.024093 | 9.014761 | 8.994095 | 9.916967 | 10.019126 | 9.495967 | 9.275767 | 11.517356 | 9.298354 | 9.713203 | 9.996425 | 9.436771 | 9.733441 | 9.668316 | 9.57676 | 9.895068 | 9.7804 | 9.913681 | 9.450974 |
1304.4138 | Alex Bernardini Dr. | Alex E. Bernardini and O. Bertolami | Equivalence between Born-Infeld tachyon and effective real scalar field
theories for brane structures in warped geometry | 15 pages, 3 figures | Phys. Lett. B 726 (2013) 512 | 10.1016/j.physletb.2013.08.064 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An equivalence between Born-Infeld and effective real scalar field theories
for brane structures is built in some specific warped space-time scenarios.
Once the equations of motion for tachyon fields related to the Born-Infeld
action are written as first-order equations, a simple analytical connection
with a particul... | [
{
"created": "Mon, 15 Apr 2013 15:46:59 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Jul 2013 11:10:54 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Aug 2013 16:38:19 GMT",
"version": "v3"
}
] | 2015-08-04 | [
[
"Bernardini",
"Alex E.",
""
],
[
"Bertolami",
"O.",
""
]
] | An equivalence between Born-Infeld and effective real scalar field theories for brane structures is built in some specific warped space-time scenarios. Once the equations of motion for tachyon fields related to the Born-Infeld action are written as first-order equations, a simple analytical connection with a particular... | 10.924049 | 10.962598 | 11.71209 | 11.194367 | 11.142778 | 11.506152 | 11.641061 | 11.371512 | 11.028674 | 12.199591 | 10.702302 | 10.758434 | 10.689992 | 10.777119 | 10.687265 | 10.787543 | 11.117812 | 10.934709 | 10.904525 | 10.894527 | 10.510646 |
0812.3488 | Catarina Bastos | C. Bastos, O. Bertolami, N. Dias and J. Prata | Noncommutative Quantum Cosmology | Proceedings of DICE2008, Castiglioncello, 22nd-26th September 2008,
Italy | J.Phys.Conf.Ser.174:012053,2009 | 10.1088/1742-6596/174/1/012053 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | One presents a phase-space noncommutative extension of Quantum Cosmology in
the context of a Kantowski-Sachs (KS) minisuperspace model. We obtain the
Wheeler-DeWitt (WDW) equation for the noncommutative system through the ADM
formalism and a suitable Seiberg-Witten map. The resulting WDW equation
explicitly depends o... | [
{
"created": "Thu, 18 Dec 2008 09:21:53 GMT",
"version": "v1"
}
] | 2009-07-24 | [
[
"Bastos",
"C.",
""
],
[
"Bertolami",
"O.",
""
],
[
"Dias",
"N.",
""
],
[
"Prata",
"J.",
""
]
] | One presents a phase-space noncommutative extension of Quantum Cosmology in the context of a Kantowski-Sachs (KS) minisuperspace model. We obtain the Wheeler-DeWitt (WDW) equation for the noncommutative system through the ADM formalism and a suitable Seiberg-Witten map. The resulting WDW equation explicitly depends on ... | 5.966401 | 4.825873 | 5.460336 | 4.866959 | 5.413078 | 5.676927 | 5.277034 | 4.80265 | 5.303976 | 5.944224 | 5.455927 | 5.413442 | 5.552969 | 5.378367 | 5.429699 | 5.496684 | 5.591589 | 5.410732 | 5.765485 | 5.632712 | 5.696831 |
2009.03785 | Ines Cavero-Pelaez | Ines Cavero-Pelaez, Jose M. Munoz-Castaneda and Cesar Romaniega | Casimir Energy for concentric $\delta$-$\delta'$ spheres | 9 pages, 8 figures We are submitting this manuscript for publication
in Physical Review D | Phys. Rev. D 103, 045005 (2021) | 10.1103/PhysRevD.103.045005 | null | hep-th cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the vacuum interaction of a scalar field and two concentric spheres
defined by a singular potential on their surfaces. The potential is a linear
combination of the Dirac-$\delta$ and its derivative. The presence of the delta
prime term in the potential causes that it behaves differently when it is seen
from ... | [
{
"created": "Tue, 8 Sep 2020 14:26:16 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jan 2021 07:24:41 GMT",
"version": "v2"
}
] | 2021-02-10 | [
[
"Cavero-Pelaez",
"Ines",
""
],
[
"Munoz-Castaneda",
"Jose M.",
""
],
[
"Romaniega",
"Cesar",
""
]
] | We study the vacuum interaction of a scalar field and two concentric spheres defined by a singular potential on their surfaces. The potential is a linear combination of the Dirac-$\delta$ and its derivative. The presence of the delta prime term in the potential causes that it behaves differently when it is seen from th... | 10.413479 | 11.833512 | 10.76818 | 9.920503 | 11.208953 | 11.794677 | 10.46025 | 10.371585 | 10.517189 | 11.088979 | 9.467525 | 10.157804 | 10.876141 | 10.145679 | 9.845108 | 9.932486 | 10.149155 | 9.833057 | 9.953199 | 10.277747 | 9.776552 |
1807.06940 | Takahiro Terada | Yohei Ema, Ryuichiro Kitano, Takahiro Terada | Unitarity constraint on the K\"ahler curvature | 20 pages, 2 figures; published version, minor changes, references
added | J. High Energ. Phys. (2018) 2018: 75 | 10.1007/JHEP09(2018)075 | KEK-TH-2065, KEK-Cosmo-226 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In supersymmetric theories, the signs of quartic terms in the K\"ahler
potential control the stability of non-supersymmetric field configurations. In
particular, in supersymmetric inflation models, the signs are important for the
stability of an inflationary trajectory as well as for the prediction of the
spectral in... | [
{
"created": "Wed, 18 Jul 2018 13:58:47 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Sep 2018 03:17:18 GMT",
"version": "v2"
}
] | 2018-09-20 | [
[
"Ema",
"Yohei",
""
],
[
"Kitano",
"Ryuichiro",
""
],
[
"Terada",
"Takahiro",
""
]
] | In supersymmetric theories, the signs of quartic terms in the K\"ahler potential control the stability of non-supersymmetric field configurations. In particular, in supersymmetric inflation models, the signs are important for the stability of an inflationary trajectory as well as for the prediction of the spectral inde... | 8.657354 | 9.016035 | 9.158434 | 8.154385 | 8.682098 | 8.560137 | 8.851415 | 8.040583 | 8.424994 | 9.291746 | 8.227983 | 7.917665 | 8.567365 | 7.998648 | 8.008078 | 8.011302 | 7.762926 | 7.740589 | 8.123825 | 8.517829 | 8.1938 |
hep-th/9706166 | Ramon Cova | R. J. Cova (Universidad del Zulia, University of Durham) and W. J.
Zakrzewski (University of Durham) | Soliton scattering in the O(3) model on a torus | 23 pages including 8 pages of figures, latex. To appear in
Nonlinearity | Nonlinearity10:1305-1317,1997 | 10.1088/0951-7715/10/5/015 | DTP 96-59 | hep-th | null | Using numerical simulations, the stability and scattering properties of the
O(3) model on a two-dimensional torus are studied. Its solitons are found to be
unstable but can be stabilized by the addition of a Skyrme term to the
Lagrangian. Scattering at right angles with respect to the initial direction of
motion is o... | [
{
"created": "Tue, 24 Jun 1997 10:03:22 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cova",
"R. J.",
"",
"Universidad del Zulia, University of Durham"
],
[
"Zakrzewski",
"W. J.",
"",
"University of Durham"
]
] | Using numerical simulations, the stability and scattering properties of the O(3) model on a two-dimensional torus are studied. Its solitons are found to be unstable but can be stabilized by the addition of a Skyrme term to the Lagrangian. Scattering at right angles with respect to the initial direction of motion is obs... | 9.736126 | 9.827849 | 9.836028 | 9.558069 | 9.706661 | 9.653403 | 9.421415 | 8.998424 | 8.802535 | 11.179768 | 8.816319 | 9.544048 | 9.465506 | 9.545521 | 9.192953 | 9.528209 | 9.61053 | 9.250127 | 9.435678 | 10.090828 | 9.083369 |
1909.03279 | Gordon Semenoff | Gianluca Grignani, Gordon W. Semenoff | Defect QED: Dielectric without a Dielectric, Monopole without a Monopole | 25 pages, 1 figure, clarified eq (8.8) | null | 10.1007/JHEP11(2019)114 | null | hep-th cond-mat.mes-hall cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a class of defect quantum field theories where the quantum field
theory in the 3+1-dimensional bulk is a free photon and charged matter and the
interactions of the photons with the charges occur entirely on a
2+1-dimensional defect. We observe that at the fully quantum level, the
effective action of such a t... | [
{
"created": "Sat, 7 Sep 2019 14:47:18 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Nov 2019 02:18:22 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Grignani",
"Gianluca",
""
],
[
"Semenoff",
"Gordon W.",
""
]
] | We study a class of defect quantum field theories where the quantum field theory in the 3+1-dimensional bulk is a free photon and charged matter and the interactions of the photons with the charges occur entirely on a 2+1-dimensional defect. We observe that at the fully quantum level, the effective action of such a the... | 12.490523 | 13.388343 | 13.167042 | 13.646313 | 13.804021 | 12.79126 | 13.965077 | 13.349951 | 12.777822 | 15.170312 | 12.385429 | 12.340676 | 12.672918 | 12.669837 | 12.858624 | 12.25882 | 12.741036 | 12.12151 | 12.185969 | 12.595349 | 12.22489 |
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