id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
2404.00698 | Hajime Otsuka | Hajime Otsuka and Ryo Yokokura | Stringy constraints on primordial electromagnetic fields in axion
inflation | 29 pages, v2: published version | null | 10.1007/JHEP07(2024)055 | KYUSHU-HET-287 | hep-th astro-ph.CO hep-ph | http://creativecommons.org/licenses/by/4.0/ | We study primordial electromagnetic fields in effective actions of string
theory. In contrast to a conventional scenario of producing primordial
electromagnetic fields induced by the axion inflation, we deal with the
Dirac-Born-Infeld action as a non-linear generation of Maxwell theory. It turns
out that the intensit... | [
{
"created": "Sun, 31 Mar 2024 14:30:52 GMT",
"version": "v1"
},
{
"created": "Sat, 20 Jul 2024 10:27:02 GMT",
"version": "v2"
}
] | 2024-07-23 | [
[
"Otsuka",
"Hajime",
""
],
[
"Yokokura",
"Ryo",
""
]
] | We study primordial electromagnetic fields in effective actions of string theory. In contrast to a conventional scenario of producing primordial electromagnetic fields induced by the axion inflation, we deal with the Dirac-Born-Infeld action as a non-linear generation of Maxwell theory. It turns out that the intensity ... | 10.653796 | 10.088078 | 10.743949 | 9.97711 | 10.24157 | 10.712566 | 9.703313 | 9.717005 | 9.693564 | 11.653441 | 10.483486 | 10.69933 | 10.61816 | 10.097263 | 10.173478 | 10.184537 | 10.54308 | 10.474402 | 10.560759 | 10.715203 | 10.189473 |
1902.02872 | Luis B Castro | Elvis J. Aquino Curi and Luis B. Castro and Antonio S. de Castro | Proper treatment of scalar and vector exponential potentials in the
Klein-Gordon equation: Scattering and bound states | 6 pages | Eur.Phys.J.Plus 134 (2019) no.6, 248 | 10.1140/epjp/i2019-12571-8 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We point out a misleading treatment in the literature regarding to
bound-state solutions for the $s$-wave Klein-Gordon equation with exponential
scalar and vector potentials. Following the appropriate procedure for an
arbitrary mixing of scalar and vector couplings, we generalize earlier works
and present the correct... | [
{
"created": "Thu, 7 Feb 2019 22:38:49 GMT",
"version": "v1"
}
] | 2019-07-25 | [
[
"Curi",
"Elvis J. Aquino",
""
],
[
"Castro",
"Luis B.",
""
],
[
"de Castro",
"Antonio S.",
""
]
] | We point out a misleading treatment in the literature regarding to bound-state solutions for the $s$-wave Klein-Gordon equation with exponential scalar and vector potentials. Following the appropriate procedure for an arbitrary mixing of scalar and vector couplings, we generalize earlier works and present the correct s... | 15.563971 | 16.304909 | 13.680668 | 13.786513 | 14.198772 | 12.95428 | 13.448841 | 13.687053 | 13.753801 | 14.76091 | 13.52493 | 14.973756 | 14.045051 | 13.820043 | 14.084368 | 13.978242 | 14.216222 | 14.766472 | 14.118617 | 13.776393 | 13.770131 |
hep-th/0407191 | Roberto Casadio | Roberto Casadio (University of Bologna), Cristiano Germani (DAMTP,
University of Cambridge) | Gravitational collapse and black hole evolution: do holographic black
holes eventually "anti-evaporate"? | 18 pages in RevTeX4 style, 11 eps figures included. Discussion on the
contribution of dissipation and clarifications added, version accepted for
publication in Prog. Theor. Phys. Vol. 114, No. 1 | Prog.Theor.Phys. 114 (2005) 23-56 | 10.1143/PTP.114.23 | DAMTP-2004-115 | hep-th astro-ph gr-qc hep-ph | null | We study the gravitational collapse of compact objects in the Brane-World. We
begin by arguing that the regularity of the five-dimensional geodesics does not
allow the energy-momentum tensor of matter on the brane to have (step-like)
discontinuities, which are instead admitted in the four-dimensional General
Relativi... | [
{
"created": "Wed, 21 Jul 2004 16:20:55 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Dec 2004 15:33:34 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Jan 2005 16:38:35 GMT",
"version": "v3"
},
{
"created": "Fri, 20 May 2005 03:11:16 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Casadio",
"Roberto",
"",
"University of Bologna"
],
[
"Germani",
"Cristiano",
"",
"DAMTP,\n University of Cambridge"
]
] | We study the gravitational collapse of compact objects in the Brane-World. We begin by arguing that the regularity of the five-dimensional geodesics does not allow the energy-momentum tensor of matter on the brane to have (step-like) discontinuities, which are instead admitted in the four-dimensional General Relativist... | 10.558422 | 9.608067 | 10.733715 | 9.434333 | 11.359238 | 11.274199 | 11.290401 | 9.706895 | 10.031368 | 11.414855 | 9.778457 | 10.107158 | 10.510115 | 10.106035 | 10.26494 | 10.352192 | 10.305055 | 9.888185 | 10.277308 | 10.63726 | 10.191726 |
1801.05027 | Tanmoy Paul | Tanmoy Paul and Soumitra SenGupta | Radion tunneling in modified theories of gravity | Title is slightly modified, boundary terms on the branes are added,
condition for negligible backreaction is added, some references are added.
The present article is recently accepted in Eur.Phys.J.C. arXiv admin note:
text overlap with arXiv:1701.01571 | null | 10.1140/epjc/s10052-018-5824-y | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a five dimensional warped spacetime where the bulk geometry is
governed by higher curvature $F(R)$ gravity. In this model, we determine the
modulus potential originating from the scalar degree of freedom of higher
curvature gravity. In the presence of this potential, we investigate the
possibility of modu... | [
{
"created": "Fri, 12 Jan 2018 05:25:27 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Apr 2018 04:14:23 GMT",
"version": "v2"
}
] | 2018-05-23 | [
[
"Paul",
"Tanmoy",
""
],
[
"SenGupta",
"Soumitra",
""
]
] | We consider a five dimensional warped spacetime where the bulk geometry is governed by higher curvature $F(R)$ gravity. In this model, we determine the modulus potential originating from the scalar degree of freedom of higher curvature gravity. In the presence of this potential, we investigate the possibility of modulu... | 9.88993 | 7.924129 | 8.466092 | 7.353822 | 8.174239 | 8.024919 | 7.790437 | 8.347723 | 7.348104 | 9.416723 | 8.702692 | 9.035088 | 8.582283 | 8.74325 | 8.442803 | 8.660752 | 8.653945 | 9.131251 | 8.501569 | 8.309464 | 9.065702 |
2110.13768 | Sunghyuk Park | Tobias Ekholm, Angus Gruen, Sergei Gukov, Piotr Kucharski, Sunghyuk
Park, Marko Sto\v{s}i\'c, Piotr Su{\l}kowski | Branches, quivers, and ideals for knot complements | 99 pages, 13 figures | J. Geom. Phys. 177 (2022), 104520 | 10.1016/j.geomphys.2022.104520 | null | hep-th math.GT math.QA math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the $F_K$ invariant, i.e. $\widehat{Z}$ for the complement of a
knot $K$ in the 3-sphere, the knots-quivers correspondence, and $A$-polynomials
of knots, and find several interconnections between them. We associate an $F_K$
invariant to any branch of the $A$-polynomial of $K$ and we work out explicit
ex... | [
{
"created": "Tue, 26 Oct 2021 15:21:02 GMT",
"version": "v1"
}
] | 2022-04-21 | [
[
"Ekholm",
"Tobias",
""
],
[
"Gruen",
"Angus",
""
],
[
"Gukov",
"Sergei",
""
],
[
"Kucharski",
"Piotr",
""
],
[
"Park",
"Sunghyuk",
""
],
[
"Stošić",
"Marko",
""
],
[
"Sułkowski",
"Piotr",
""
]
] | We generalize the $F_K$ invariant, i.e. $\widehat{Z}$ for the complement of a knot $K$ in the 3-sphere, the knots-quivers correspondence, and $A$-polynomials of knots, and find several interconnections between them. We associate an $F_K$ invariant to any branch of the $A$-polynomial of $K$ and we work out explicit expr... | 8.291549 | 8.674367 | 9.835538 | 8.586343 | 8.362325 | 8.861985 | 8.712377 | 8.502107 | 8.372406 | 10.763214 | 8.394086 | 8.387227 | 9.276916 | 8.384959 | 8.178748 | 8.367258 | 8.273533 | 8.362374 | 7.995525 | 8.992093 | 8.110771 |
1504.05946 | Jos\'e Manuel Izquierdo | J.J. Fernandez, J.M. Izquierdo and M.A. del Olmo | Contractions from $osp(1|32) \oplus osp(1|32)$ to the M-theory
superalgebra extended by additional fermionic generators | null | null | 10.1016/j.nuclphysb.2015.05.018 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study here the generalized Weimar-Woods contractions of the superalgebra
$osp(1|32) \oplus osp(1|32)$ in order to obtain a suitable algebra that could
describe the gauge group of $D=11$ supergravity. The contracted superalgebras
are assumed to be given in terms of fermionic extensions of the M-theory
superalgebra.... | [
{
"created": "Wed, 22 Apr 2015 10:26:20 GMT",
"version": "v1"
}
] | 2019-05-01 | [
[
"Fernandez",
"J. J.",
""
],
[
"Izquierdo",
"J. M.",
""
],
[
"del Olmo",
"M. A.",
""
]
] | We study here the generalized Weimar-Woods contractions of the superalgebra $osp(1|32) \oplus osp(1|32)$ in order to obtain a suitable algebra that could describe the gauge group of $D=11$ supergravity. The contracted superalgebras are assumed to be given in terms of fermionic extensions of the M-theory superalgebra. W... | 6.532515 | 6.202573 | 7.099001 | 5.604637 | 5.731737 | 6.075212 | 5.508437 | 5.724335 | 5.662145 | 7.559201 | 5.911183 | 6.177532 | 6.399083 | 5.86605 | 6.046424 | 6.016967 | 6.07721 | 5.901106 | 5.933872 | 6.040912 | 6.128115 |
hep-th/0203127 | A. Hatzinikitas | Ioannis Smyrnakis | Boundary States, Extended Symmetry Algebra and Module Structure for
certain Rational Torus Models | 12 pages | J.Math.Phys.43:6085-6095,2002 | 10.1063/1.1517168 | null | hep-th | null | The massless bosonic field compactified on the circle of rational $R^2$ is
reexamined in the presense of boundaries. A particular class of models
corresponding to $R^2=\frac{1}{2k}$ is distinguished by demanding the existence
of a consistent set of Newmann boundary states. The boundary states are
constructed explicit... | [
{
"created": "Thu, 14 Mar 2002 13:28:09 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Smyrnakis",
"Ioannis",
""
]
] | The massless bosonic field compactified on the circle of rational $R^2$ is reexamined in the presense of boundaries. A particular class of models corresponding to $R^2=\frac{1}{2k}$ is distinguished by demanding the existence of a consistent set of Newmann boundary states. The boundary states are constructed explicitly... | 9.577712 | 10.459001 | 9.68683 | 9.248345 | 10.719649 | 10.092831 | 10.29099 | 9.665693 | 9.47862 | 11.396915 | 9.889022 | 9.964653 | 9.908785 | 9.809649 | 9.607421 | 9.308455 | 9.607865 | 9.745198 | 9.954108 | 10.014302 | 9.554267 |
hep-th/0301093 | Rafael de Lima Rodrigues | R. de Lima Rodrigues and A. N. Vaidya | Dirac Oscillator via R-Deformed Heisenberg Algebra | Revtex, 5 pages. To appear into the Proceedings of the XXIII
Brazilian National Meeting on Particles and Fields (October/2002), site
www.sbf1.if.usp.br/eventos/enfpc/xxiii. Preprint CBPF-NF-030/02, site
www.cbpf.br | null | null | Preprint CBPF-NF-030/02 | hep-th | null | The complete energy spectrum for the Dirac oscillator via R-deformed
Heisenberg algebra is investigated.
| [
{
"created": "Tue, 14 Jan 2003 20:53:40 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Jan 2003 18:21:26 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Rodrigues",
"R. de Lima",
""
],
[
"Vaidya",
"A. N.",
""
]
] | The complete energy spectrum for the Dirac oscillator via R-deformed Heisenberg algebra is investigated. | 25.933626 | 13.379023 | 27.313507 | 24.747808 | 16.045498 | 13.605188 | 17.664707 | 16.794361 | 18.821573 | 32.767849 | 16.176445 | 20.179993 | 22.249987 | 19.993412 | 19.35272 | 18.275911 | 18.739328 | 18.159985 | 21.853807 | 25.351223 | 18.009256 |
1611.07557 | Carlos Tamarit | Alexis D. Plascencia and Carlos Tamarit | Gauge-independence of tunneling rates | 6 pages. Contribution to the Proceedings of the 38th International
Conference on High Energy Physics, ICHEP 2016, Chicago, IL, USA | PoS(ICHEP2016)345 | null | IPPP/16/118 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that tunneling rates can be defined in terms of a false-vacuum
effective action whose reality and convexity properties differ from those of
the corresponding groundstate functional. The tunneling rate is directly
related to the false-vacuum effective action evaluated at an extremal "quantum
bounce". The N... | [
{
"created": "Tue, 22 Nov 2016 22:24:43 GMT",
"version": "v1"
}
] | 2016-11-24 | [
[
"Plascencia",
"Alexis D.",
""
],
[
"Tamarit",
"Carlos",
""
]
] | It is shown that tunneling rates can be defined in terms of a false-vacuum effective action whose reality and convexity properties differ from those of the corresponding groundstate functional. The tunneling rate is directly related to the false-vacuum effective action evaluated at an extremal "quantum bounce". The Nie... | 13.006854 | 13.153735 | 11.600389 | 10.89857 | 12.054335 | 12.410625 | 10.858182 | 11.029413 | 11.296189 | 11.96861 | 11.203147 | 11.876322 | 11.588162 | 11.351736 | 11.431833 | 11.828881 | 11.841367 | 11.679244 | 11.626245 | 11.700132 | 11.53406 |
hep-th/9406090 | Jacques Distler | Jacques Distler and Shamit Kachru | Singlet Couplings and (0,2) Models | 22pp, harvmac+epsf, 2 figures included with uufiles, PUPT-1465 | Nucl.Phys.B430:13-30,1994 | 10.1016/0550-3213(94)90648-3 | null | hep-th | null | We use the quantum symmetries present in string compactification on
Landau-Ginzburg orbifolds to prove the existence of a large class of exactly
marginal (0,2) deformations of (2,2) superconformal theories. Analogous methods
apply to the more general (0,2) models introduced in \DK, lending further
credence to the fac... | [
{
"created": "Tue, 14 Jun 1994 18:17:44 GMT",
"version": "v1"
}
] | 2009-10-07 | [
[
"Distler",
"Jacques",
""
],
[
"Kachru",
"Shamit",
""
]
] | We use the quantum symmetries present in string compactification on Landau-Ginzburg orbifolds to prove the existence of a large class of exactly marginal (0,2) deformations of (2,2) superconformal theories. Analogous methods apply to the more general (0,2) models introduced in \DK, lending further credence to the fact ... | 11.092369 | 10.341604 | 12.257878 | 10.322255 | 10.865363 | 10.576931 | 10.667714 | 10.47366 | 9.825813 | 12.745286 | 10.115596 | 10.50932 | 11.032377 | 10.630182 | 10.358404 | 10.456991 | 10.774013 | 10.659596 | 10.521256 | 10.630166 | 10.450157 |
1412.8422 | Lilia Anguelova | Lilia Anguelova, Peter Suranyi, L.C. Rohana Wijewardhana | De Sitter Space in Gauge/Gravity Duality | 34 pages; minor clarifications and references added | Nucl. Phys. B899 (2015) 651 | 10.1016/j.nuclphysb.2015.08.020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate gauge/gravity duality for gauge theories in de Sitter space.
More precisely, we study a five-dimensional consistent truncation of type IIB
supergravity, which encompasses a wide variety of gravity duals of strongly
coupled gauge theories, including the Maldacena-Nunez solution and its walking
deformati... | [
{
"created": "Mon, 29 Dec 2014 18:45:30 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Feb 2015 21:05:17 GMT",
"version": "v2"
},
{
"created": "Thu, 3 Sep 2015 19:14:31 GMT",
"version": "v3"
}
] | 2015-12-09 | [
[
"Anguelova",
"Lilia",
""
],
[
"Suranyi",
"Peter",
""
],
[
"Wijewardhana",
"L. C. Rohana",
""
]
] | We investigate gauge/gravity duality for gauge theories in de Sitter space. More precisely, we study a five-dimensional consistent truncation of type IIB supergravity, which encompasses a wide variety of gravity duals of strongly coupled gauge theories, including the Maldacena-Nunez solution and its walking deformation... | 6.667574 | 6.805709 | 7.463459 | 6.862293 | 7.096352 | 7.040596 | 6.86542 | 6.473902 | 6.571754 | 7.80182 | 6.582701 | 6.503736 | 7.104924 | 6.433698 | 6.497973 | 6.541551 | 6.642499 | 6.566939 | 6.731053 | 7.187231 | 6.633821 |
1812.05406 | Tony Pinhero | Tony Pinhero | Natural $\alpha$-Attractors from ${\cal N}=1$ Supergravity via flat
K\"ahler Manifolds | 9 pages, 5 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present $\alpha$-attractor models for inflation based on ${\cal N}=1$
supergravity with flat K\"ahler manifolds. The function form of the associated
K\"ahler potential in these models are logarithmic square in nature and has a
visible shift symmetry in its composite canonical variables. The scalar
potential $V$ wi... | [
{
"created": "Thu, 13 Dec 2018 13:11:25 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Dec 2018 11:03:27 GMT",
"version": "v2"
}
] | 2018-12-19 | [
[
"Pinhero",
"Tony",
""
]
] | We present $\alpha$-attractor models for inflation based on ${\cal N}=1$ supergravity with flat K\"ahler manifolds. The function form of the associated K\"ahler potential in these models are logarithmic square in nature and has a visible shift symmetry in its composite canonical variables. The scalar potential $V$ with... | 13.059689 | 11.564444 | 13.608607 | 10.704428 | 12.724114 | 12.694559 | 12.94153 | 11.852925 | 10.681147 | 13.381887 | 11.10582 | 11.928762 | 12.345915 | 12.175749 | 12.17554 | 12.06744 | 12.41149 | 11.759816 | 11.707873 | 12.511011 | 12.279469 |
1003.2746 | Samir Mathur | Steven G. Avery, Borun D. Chowdhury, Samir D. Mathur | Excitations in the deformed D1D5 CFT | 26 pages, Latex, 4 figures | JHEP 1006:032,2010 | 10.1007/JHEP06(2010)032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform some simple computations for the first order deformation of the
D1D5 CFT off its orbifold point. It had been shown earlier that under this
deformation the vacuum state changes to a squeezed state (with the further
action of a supercharge). We now start with states containing one or two
initial quanta and w... | [
{
"created": "Sat, 13 Mar 2010 22:57:41 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Avery",
"Steven G.",
""
],
[
"Chowdhury",
"Borun D.",
""
],
[
"Mathur",
"Samir D.",
""
]
] | We perform some simple computations for the first order deformation of the D1D5 CFT off its orbifold point. It had been shown earlier that under this deformation the vacuum state changes to a squeezed state (with the further action of a supercharge). We now start with states containing one or two initial quanta and wri... | 13.338259 | 13.293799 | 15.330087 | 12.784629 | 13.076691 | 12.826536 | 14.081148 | 13.615433 | 12.510976 | 16.327942 | 12.847503 | 12.87639 | 14.046029 | 13.157885 | 13.320739 | 12.891542 | 12.519972 | 13.036727 | 12.830548 | 14.504604 | 12.73993 |
hep-th/0512206 | Martin Rocek | Martin Rocek, Cumrun Vafa, Stefan Vandoren | Hypermultiplets and Topological Strings | 21 pages, references added | JHEP0602:062,2006 | 10.1088/1126-6708/2006/02/062 | YITP-SB-05-39, HUTP-05/A055,ITP-UU-05/56,SPIN-05/36 | hep-th | null | The c-map relates classical hypermultiplet moduli spaces in compactifications
of type II strings on a Calabi-Yau threefold to vector multiplet moduli spaces
via a further compactification on a circle. We give an off-shell description of
the c-map in N=2 superspace. The superspace Lagrangian for the hypermultiplets
is... | [
{
"created": "Fri, 16 Dec 2005 14:00:02 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Dec 2005 01:41:06 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Rocek",
"Martin",
""
],
[
"Vafa",
"Cumrun",
""
],
[
"Vandoren",
"Stefan",
""
]
] | The c-map relates classical hypermultiplet moduli spaces in compactifications of type II strings on a Calabi-Yau threefold to vector multiplet moduli spaces via a further compactification on a circle. We give an off-shell description of the c-map in N=2 superspace. The superspace Lagrangian for the hypermultiplets is a... | 6.723397 | 5.95737 | 6.976581 | 5.73915 | 6.158455 | 5.972331 | 6.111007 | 5.899744 | 5.645127 | 7.355856 | 5.726407 | 6.000909 | 6.727481 | 6.164059 | 6.376066 | 5.908219 | 6.212847 | 6.420031 | 6.102829 | 6.865062 | 6.345426 |
0807.1046 | Jonas Schmidt | Wilfried Buchmuller, Jonas Schmidt | Higgs versus Matter in the Heterotic Landscape | 29 pages, 1 figure. Final version to appear in Nucl. Phys. B | Nucl.Phys.B807:265-289,2009 | 10.1016/j.nuclphysb.2008.09.011 | DESY 08-075 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In supersymmetric extensions of the standard model there is no basic
difference between Higgs and matter fields, which leads to the well known
problem of potentially large baryon and lepton number violating interactions.
Although these unwanted couplings can be forbidden by continuous or discrete
global symmetries, a... | [
{
"created": "Mon, 7 Jul 2008 15:37:57 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Sep 2008 09:51:46 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Buchmuller",
"Wilfried",
""
],
[
"Schmidt",
"Jonas",
""
]
] | In supersymmetric extensions of the standard model there is no basic difference between Higgs and matter fields, which leads to the well known problem of potentially large baryon and lepton number violating interactions. Although these unwanted couplings can be forbidden by continuous or discrete global symmetries, a t... | 7.735599 | 8.722882 | 7.864743 | 7.61021 | 7.744292 | 8.096475 | 7.796657 | 7.636641 | 7.421006 | 8.348948 | 7.804004 | 7.500587 | 7.722889 | 7.121744 | 7.480476 | 7.395073 | 7.364218 | 7.405035 | 7.402168 | 7.614462 | 7.338265 |
hep-th/0502028 | N. E. J. Bjerrum-Bohr | Steven J. Bidder, N. E. J. Bjerrum-Bohr, David C. Dunbar and Warren B.
Perkins | One-Loop Gluon Scattering Amplitudes in Theories with $N < 4$
Supersymmetries | 15 pages, minor typos corrected | Phys.Lett.B612:75-88,2005 | 10.1016/j.physletb.2005.02.045 | SWAT-05-425 | hep-th | null | Generalised unitarity techniques are used to calculate the coefficients of
box and triangle integral functions of one-loop gluon scattering amplitudes in
gauge theories with $N < 4$ supersymmetries. We show that the box coefficients
in N=1 and N=0 theories inherit the same coplanar and collinear constraints as
the co... | [
{
"created": "Wed, 2 Feb 2005 20:53:18 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Feb 2005 17:00:36 GMT",
"version": "v2"
},
{
"created": "Thu, 23 Mar 2006 12:13:23 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Bidder",
"Steven J.",
""
],
[
"Bjerrum-Bohr",
"N. E. J.",
""
],
[
"Dunbar",
"David C.",
""
],
[
"Perkins",
"Warren B.",
""
]
] | Generalised unitarity techniques are used to calculate the coefficients of box and triangle integral functions of one-loop gluon scattering amplitudes in gauge theories with $N < 4$ supersymmetries. We show that the box coefficients in N=1 and N=0 theories inherit the same coplanar and collinear constraints as the corr... | 7.114252 | 5.948925 | 6.968792 | 6.158542 | 6.628417 | 6.204315 | 6.45667 | 6.032126 | 6.127308 | 6.768649 | 6.254214 | 6.126145 | 6.773688 | 6.206358 | 6.188657 | 5.94904 | 5.998067 | 6.226617 | 5.943361 | 6.792064 | 6.431546 |
1302.5024 | Ehsan Hatefi | Ehsan Hatefi | Closed string Ramond-Ramond proposed higher derivative interactions on
fermionic amplitudes in IIB | 29 pages, figures are removed. Sections 3,4, and 5 are shortened. To
appear in NPB | Nucl.Phys. B880 (2014) 1-22 | 10.1016/j.nuclphysb.2014.01.001 | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complete form of the amplitude of one closed string Ramond-Ramond (RR),
two fermionic strings and one scalar field in IIB superstring theory has been
computed in detail. Deriving $<V_{C}V_{\bar\psi}V_{\psi} V_{\phi}>$ by using
suitable gauge fixing, we discover some new vertices and their higher
derivative correc... | [
{
"created": "Wed, 20 Feb 2013 16:34:36 GMT",
"version": "v1"
},
{
"created": "Sun, 9 Jun 2013 21:37:32 GMT",
"version": "v2"
},
{
"created": "Tue, 16 Jul 2013 12:29:27 GMT",
"version": "v3"
},
{
"created": "Fri, 3 Jan 2014 15:24:44 GMT",
"version": "v4"
}
] | 2014-01-23 | [
[
"Hatefi",
"Ehsan",
""
]
] | The complete form of the amplitude of one closed string Ramond-Ramond (RR), two fermionic strings and one scalar field in IIB superstring theory has been computed in detail. Deriving $<V_{C}V_{\bar\psi}V_{\psi} V_{\phi}>$ by using suitable gauge fixing, we discover some new vertices and their higher derivative correcti... | 14.275985 | 11.013382 | 15.007466 | 11.87478 | 11.036108 | 11.251988 | 10.838975 | 10.429719 | 11.507716 | 14.809945 | 10.872889 | 12.334138 | 13.796017 | 12.483795 | 11.928537 | 12.035662 | 12.234425 | 12.275818 | 12.429886 | 13.828035 | 12.374618 |
1707.01918 | Ulf Lindstr\"om | Chris Hull and Ulf Lindstr\"om | All $(4,0)$: Sigma Models with $(4,0)$ Off-Shell Supersymmetry | 13 pages | null | 10.1007/JHEP08(2017)129 | Imperial preprint: Imperial-TP-2017-CH-02, Uppsala preprint:
UUITP-20/17 | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Off-shell $(4,0)$ supermultiplets in 2-dimensions are formulated. These are
used to construct sigma models whose target spaces are vector bundles over
manifolds that are hyperk\"ahler with torsion. The off-shell supersymmetry
implies that the complex structures are simultaneously integrable and allows us
to write act... | [
{
"created": "Thu, 6 Jul 2017 18:06:33 GMT",
"version": "v1"
}
] | 2017-09-13 | [
[
"Hull",
"Chris",
""
],
[
"Lindström",
"Ulf",
""
]
] | Off-shell $(4,0)$ supermultiplets in 2-dimensions are formulated. These are used to construct sigma models whose target spaces are vector bundles over manifolds that are hyperk\"ahler with torsion. The off-shell supersymmetry implies that the complex structures are simultaneously integrable and allows us to write actio... | 11.959397 | 8.458661 | 12.446835 | 8.935641 | 10.126048 | 9.358272 | 10.062225 | 8.164888 | 8.44347 | 12.572035 | 8.871003 | 9.862199 | 11.221854 | 10.014492 | 9.737598 | 9.842172 | 9.955628 | 9.543314 | 9.978963 | 10.897281 | 9.905575 |
hep-th/9903064 | Jean-Pierre Derendinger | Jean-Pierre Derendinger | Temperature Instabilities in N=4 Strings | 7 pages, 32nd Int. Symposium Ahrenshoop, Buckow, Germany, Sept. 1-5,
1998 | Fortsch.Phys.48:77-82,2000 | 10.1002/(SICI)1521-3978(20001)48:1/3<77::AID-PROP77>3.0.CO;2-U | NEIP-99-003 | hep-th | null | An effective supergravity description of all instabilities of N_4=4
superstrings is derived. The construction is based on the N_4=4 BPS mass
formula at finite temperature and uses the properties of N_4=4 gauged
supergravity. It provides the boundaries of the various thermal phases in the
non-perturbative moduli space... | [
{
"created": "Mon, 8 Mar 1999 15:42:57 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Derendinger",
"Jean-Pierre",
""
]
] | An effective supergravity description of all instabilities of N_4=4 superstrings is derived. The construction is based on the N_4=4 BPS mass formula at finite temperature and uses the properties of N_4=4 gauged supergravity. It provides the boundaries of the various thermal phases in the non-perturbative moduli space. ... | 11.776196 | 9.439448 | 10.599145 | 9.143411 | 10.061126 | 9.706444 | 9.562737 | 9.073004 | 9.370556 | 10.662481 | 10.052598 | 9.690465 | 10.099198 | 9.520406 | 9.121876 | 9.168984 | 9.190091 | 9.29423 | 9.814093 | 10.483824 | 9.628579 |
hep-th/9908099 | Theodore A. Jacobson | Ted Jacobson and David Mattingly | Hawking radiation on a falling lattice | 11 pages, 7 figures, RevTex; paragraph added to introduction
discussing insensitivity to choice of lattice point worldlines, version
appearing in PRD | Phys.Rev.D61:024017,2000 | 10.1103/PhysRevD.61.024017 | NSF-ITP-99-097 | hep-th gr-qc hep-lat | null | Scalar field theory on a lattice falling freely into a 1+1 dimensional black
hole is studied using both WKB and numerical approaches. The outgoing modes are
shown to arise from incoming modes by a process analogous to a Bloch
oscillation, with an admixture of negative frequency modes corresponding to the
Hawking radi... | [
{
"created": "Fri, 13 Aug 1999 21:40:15 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Jan 2000 23:30:55 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Jacobson",
"Ted",
""
],
[
"Mattingly",
"David",
""
]
] | Scalar field theory on a lattice falling freely into a 1+1 dimensional black hole is studied using both WKB and numerical approaches. The outgoing modes are shown to arise from incoming modes by a process analogous to a Bloch oscillation, with an admixture of negative frequency modes corresponding to the Hawking radiat... | 12.06331 | 11.3172 | 11.223275 | 10.567415 | 10.98313 | 12.528201 | 12.157176 | 11.192667 | 11.660672 | 11.838669 | 11.467099 | 11.202653 | 11.141488 | 10.980236 | 10.953239 | 10.741923 | 11.235773 | 10.930838 | 11.491035 | 11.518534 | 11.402275 |
hep-th/0210191 | Nadir Belaloui | N. Belaloui and H. Bennacer | Poincare algebra and space-time critical dimensions for parabosonic
strings | Latex,16 pages; v2 : published version, with numbering of formulas
and conclusion corrected | Czech.J.Phys. 53 (2003) 769-783 | 10.1023/A:1025970432658 | null | hep-th | null | We construct the parabosonic string formalism based on the paraquantization
of both the center of mass variables and the excitation modes of the string. A
critical study of the different commutators of the Poincar\'{e} algebra based
on the redefinition of its generators and the direct treatment using trilinear
relati... | [
{
"created": "Sun, 20 Oct 2002 22:47:48 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Oct 2003 13:47:06 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Belaloui",
"N.",
""
],
[
"Bennacer",
"H.",
""
]
] | We construct the parabosonic string formalism based on the paraquantization of both the center of mass variables and the excitation modes of the string. A critical study of the different commutators of the Poincar\'{e} algebra based on the redefinition of its generators and the direct treatment using trilinear relation... | 14.187799 | 13.695145 | 15.487483 | 11.643101 | 15.217966 | 13.627225 | 13.876766 | 13.459587 | 12.897872 | 16.524891 | 13.242799 | 13.101075 | 13.857729 | 12.934109 | 13.567597 | 13.327343 | 13.579296 | 13.702284 | 12.725177 | 13.165402 | 12.894872 |
0810.1985 | Paul Chesler | Paul M. Chesler, Kristan Jensen, Andreas Karch, Laurence G. Yaffe | Light quark energy loss in strongly-coupled N = 4 supersymmetric
Yang-Mills plasma | 19 pages, 7 figures. Added discussion, published version | Phys.Rev.D79:125015,2009 | 10.1103/PhysRevD.79.125015 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the penetration depth of a light quark moving through a large
$N_c$, strongly coupled $\mathcal N = 4$ supersymmetric Yang-Mills plasma using
gauge/gravity duality and a combination of analytic and numerical techniques.
We find that the maximum distance a quark with energy $E$ can travel through a
plasma i... | [
{
"created": "Sat, 11 Oct 2008 00:14:55 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jul 2009 00:25:16 GMT",
"version": "v2"
}
] | 2009-08-03 | [
[
"Chesler",
"Paul M.",
""
],
[
"Jensen",
"Kristan",
""
],
[
"Karch",
"Andreas",
""
],
[
"Yaffe",
"Laurence G.",
""
]
] | We compute the penetration depth of a light quark moving through a large $N_c$, strongly coupled $\mathcal N = 4$ supersymmetric Yang-Mills plasma using gauge/gravity duality and a combination of analytic and numerical techniques. We find that the maximum distance a quark with energy $E$ can travel through a plasma is ... | 6.025944 | 5.333942 | 5.653115 | 5.097452 | 5.725884 | 5.203159 | 5.522132 | 5.288308 | 5.416734 | 6.706575 | 5.262498 | 5.231926 | 5.848358 | 5.390231 | 5.516585 | 5.498212 | 5.172776 | 5.325023 | 5.215589 | 5.820531 | 5.277016 |
2007.09494 | Diego Marqu\'es | Tomas Codina and Diego Marques | Generalized Dualities and Higher Derivatives | References added, published in JHEP | null | 10.1007/JHEP10(2020)002 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Generalized dualities had an intriguing incursion into Double Field Theory
(DFT) in terms of local $O(d,d)$ transformations. We review this idea and use
the higher derivative formulation of DFT to compute the first order corrections
to generalized dualities. Our main result is a unified expression that can be
easily ... | [
{
"created": "Sat, 18 Jul 2020 18:14:29 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jul 2020 02:19:47 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Oct 2020 11:38:36 GMT",
"version": "v3"
}
] | 2020-10-06 | [
[
"Codina",
"Tomas",
""
],
[
"Marques",
"Diego",
""
]
] | Generalized dualities had an intriguing incursion into Double Field Theory (DFT) in terms of local $O(d,d)$ transformations. We review this idea and use the higher derivative formulation of DFT to compute the first order corrections to generalized dualities. Our main result is a unified expression that can be easily sp... | 18.121534 | 16.440231 | 19.991571 | 17.205788 | 18.447695 | 18.456457 | 16.442862 | 19.086483 | 16.296047 | 19.47802 | 16.586134 | 16.838614 | 17.721823 | 16.855066 | 16.889074 | 17.662205 | 16.539808 | 17.067469 | 16.969673 | 18.451675 | 17.112452 |
1612.07565 | Tadashi Okazaki | Tadashi Okazaki, Douglas J. Smith | Mock Modular Index of M2-M5 Brane System | 47 pages, 8 figures; v2: references added | Phys. Rev. D 96, 026017 (2017) | 10.1103/PhysRevD.96.026017 | DCPT-16/63; NCTS-TH/1611 | hep-th math.AG math.NT math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present BPS indices of the supergroup WZW models that live on intersecting
M2-M5 brane systems. They can encode data of the stretched M2-branes between
M5-branes and count the BPS states. They are generally expressed in terms of
mock theta functions via the Kac-Wakimoto character formula of the affine Lie
superalg... | [
{
"created": "Thu, 22 Dec 2016 12:11:57 GMT",
"version": "v1"
},
{
"created": "Tue, 17 Jan 2017 01:01:51 GMT",
"version": "v2"
}
] | 2017-07-25 | [
[
"Okazaki",
"Tadashi",
""
],
[
"Smith",
"Douglas J.",
""
]
] | We present BPS indices of the supergroup WZW models that live on intersecting M2-M5 brane systems. They can encode data of the stretched M2-branes between M5-branes and count the BPS states. They are generally expressed in terms of mock theta functions via the Kac-Wakimoto character formula of the affine Lie superalgeb... | 8.46532 | 8.843589 | 11.327052 | 7.525085 | 7.664675 | 8.074469 | 8.552787 | 7.825 | 7.819312 | 11.083545 | 7.737595 | 7.832724 | 9.118956 | 7.866933 | 8.145266 | 7.828837 | 8.083356 | 7.696813 | 7.953952 | 8.853417 | 7.787848 |
2108.01539 | Xin Guo | Xin Guo and Kimball A. Milton and Gerard Kennedy and William P.
McNulty and Nima Pourtolami and Yang Li | The energetics of quantum vacuum friction: Field fluctuations | null | null | 10.1103/PhysRevD.104.116006 | null | hep-th physics.atom-ph quant-ph | http://creativecommons.org/licenses/by/4.0/ | Quantum fluctuations can induce a friction on a neutral but polarizable
particle and cause it to radiate energy even if the particle is moving in free
space filled with blackbody radiation, and is not in contact with or close to
any surface or other object. We explore the energetics of such a particle
moving uniforml... | [
{
"created": "Tue, 3 Aug 2021 14:44:50 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Aug 2021 07:39:42 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Aug 2021 15:26:34 GMT",
"version": "v3"
},
{
"created": "Sun, 17 Oct 2021 07:15:48 GMT",
"version": "v4"
}
] | 2021-12-22 | [
[
"Guo",
"Xin",
""
],
[
"Milton",
"Kimball A.",
""
],
[
"Kennedy",
"Gerard",
""
],
[
"McNulty",
"William P.",
""
],
[
"Pourtolami",
"Nima",
""
],
[
"Li",
"Yang",
""
]
] | Quantum fluctuations can induce a friction on a neutral but polarizable particle and cause it to radiate energy even if the particle is moving in free space filled with blackbody radiation, and is not in contact with or close to any surface or other object. We explore the energetics of such a particle moving uniformly ... | 9.228218 | 11.104809 | 10.151072 | 9.467196 | 10.242827 | 10.373311 | 9.847323 | 10.154535 | 9.27362 | 10.821056 | 9.989475 | 9.515924 | 9.387678 | 9.55592 | 9.757182 | 9.566028 | 9.872644 | 9.587132 | 9.539133 | 9.410821 | 9.352096 |
hep-th/9707085 | Harutada Sato | H-T. Sato | Note on thermodynamic fermion loop under constant magnetic field | 8 pages | J.Math.Phys. 39 (1998) 4540 | 10.1063/1.532524 | NBI-HE-97-30 | hep-th | null | The one-loop effective potential of a thermodynamic fermion loop under
constant magnetic field is studied. As expected, it can be interpreted
literally as a discretized sum of $(D-2)$-dimensional energy density above the
Dirac sea. Large/small mass expansions of the potential are also examined.
| [
{
"created": "Wed, 9 Jul 1997 12:59:58 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Sato",
"H-T.",
""
]
] | The one-loop effective potential of a thermodynamic fermion loop under constant magnetic field is studied. As expected, it can be interpreted literally as a discretized sum of $(D-2)$-dimensional energy density above the Dirac sea. Large/small mass expansions of the potential are also examined. | 25.25355 | 20.823139 | 21.268282 | 19.128784 | 19.592989 | 18.366398 | 20.685324 | 20.640257 | 20.360603 | 23.051506 | 19.812771 | 20.737661 | 20.78624 | 20.723679 | 20.448715 | 20.101572 | 20.03315 | 20.320904 | 20.118145 | 20.708851 | 19.57836 |
hep-th/9809015 | Klaus Behrndt | Klaus Behrndt | AdS gravity and field theories at fixpoints | 16 pages, 2 figure, LaTeX | null | null | null | hep-th | null | The renormalization group flow of the worldvolume theory depends very much
from the number of unbroken supersymmetries. In the dual $AdS$ picture we break
supersymmetry by adding different types of BPS black holes. We argue, that this
BPS black hole causes a non-trivial renormalization group flow in the
worldvolume f... | [
{
"created": "Wed, 2 Sep 1998 13:06:44 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Behrndt",
"Klaus",
""
]
] | The renormalization group flow of the worldvolume theory depends very much from the number of unbroken supersymmetries. In the dual $AdS$ picture we break supersymmetry by adding different types of BPS black holes. We argue, that this BPS black hole causes a non-trivial renormalization group flow in the worldvolume fie... | 10.399086 | 10.180368 | 11.023259 | 9.386083 | 10.531802 | 10.162627 | 10.942864 | 10.32084 | 10.440525 | 12.078183 | 9.506716 | 10.029546 | 10.522784 | 9.817904 | 9.812841 | 9.815697 | 9.68655 | 9.883855 | 9.721869 | 10.373702 | 9.614944 |
1806.01362 | Chandrima Paul | Chandrima Paul | Metallic and antiferromagnetic fixed points from gravity | 22 Pages, no figures | International Journal of Modern Physics A Vol. 33 (2018) 1850094 | 10.1142/S0217751X1850094X | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We consider SU(2)$\times$ U(1) gauge theory coupled to matter field in
adjoints and study RG group flow. We constructed Callan Symanzik equation and
subsequent $\beta$ functions and study the fixed points. We find there are two
fixed points, showing metallic and antiferromagnetic behaviour. We have shown
that metalli... | [
{
"created": "Mon, 4 Jun 2018 20:08:55 GMT",
"version": "v1"
}
] | 2018-06-06 | [
[
"Paul",
"Chandrima",
""
]
] | We consider SU(2)$\times$ U(1) gauge theory coupled to matter field in adjoints and study RG group flow. We constructed Callan Symanzik equation and subsequent $\beta$ functions and study the fixed points. We find there are two fixed points, showing metallic and antiferromagnetic behaviour. We have shown that metallic ... | 16.825335 | 13.070712 | 15.144152 | 13.828866 | 16.024122 | 14.977938 | 16.078508 | 15.43129 | 14.841354 | 15.810855 | 15.430216 | 15.124497 | 14.74317 | 14.489034 | 14.592614 | 15.513294 | 14.726606 | 14.412963 | 14.534573 | 14.853868 | 13.859239 |
hep-th/0702118 | Micha{\l} Spali\'nski | Michal Spalinski | On the Slow Roll Expansion for Brane Inflation | References added | JCAP 0704:018,2007 | 10.1088/1475-7516/2007/04/018 | null | hep-th | null | One possibility for identifying the inflaton in the framework of string
theory is that it is a $D$-brane modulus. This option involves a specific,
non-canonical form of the kinetic energy -- the Dirac-Born-Infeld action. This
note investigates the applicability of the slow roll approximation in
inflationary models of... | [
{
"created": "Thu, 15 Feb 2007 20:04:42 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Mar 2007 12:18:51 GMT",
"version": "v2"
},
{
"created": "Sun, 29 Apr 2007 15:02:21 GMT",
"version": "v3"
}
] | 2010-10-27 | [
[
"Spalinski",
"Michal",
""
]
] | One possibility for identifying the inflaton in the framework of string theory is that it is a $D$-brane modulus. This option involves a specific, non-canonical form of the kinetic energy -- the Dirac-Born-Infeld action. This note investigates the applicability of the slow roll approximation in inflationary models of t... | 8.716997 | 9.007606 | 8.389807 | 7.823722 | 8.705602 | 8.639864 | 9.462171 | 7.826118 | 8.354942 | 10.113302 | 8.200228 | 7.888586 | 7.773909 | 7.867517 | 7.702966 | 7.906207 | 8.103314 | 7.880874 | 8.069817 | 8.341679 | 8.32336 |
hep-th/9701042 | Argurio Riccardo | R. Argurio, F. Englert, L. Houart | Intersection Rules for p-Branes | 15 pages, LaTeX, no figures. One reference modified; to appear in
Phys. Lett. B | Phys.Lett.B398:61-68,1997 | 10.1016/S0370-2693(97)00205-0 | ULB-TH-97/01 | hep-th | null | We present a general rule determining how extremal branes can interesect in a
configuration with zero binding energy. The rule is derived in a model
independent way and in arbitrary spacetime dimensions $D$ by solving the
equations of motion of gravity coupled to a dilaton and several different
$n$-form field strengt... | [
{
"created": "Fri, 10 Jan 1997 15:36:30 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Feb 1997 10:33:24 GMT",
"version": "v2"
}
] | 2011-05-05 | [
[
"Argurio",
"R.",
""
],
[
"Englert",
"F.",
""
],
[
"Houart",
"L.",
""
]
] | We present a general rule determining how extremal branes can interesect in a configuration with zero binding energy. The rule is derived in a model independent way and in arbitrary spacetime dimensions $D$ by solving the equations of motion of gravity coupled to a dilaton and several different $n$-form field strengths... | 9.455597 | 9.041404 | 9.949659 | 8.485822 | 8.945314 | 8.76424 | 9.109936 | 9.007188 | 8.88653 | 10.551311 | 8.579719 | 8.673901 | 9.178238 | 8.733998 | 8.846507 | 8.588608 | 8.570938 | 8.60235 | 8.648013 | 9.303041 | 8.900758 |
hep-th/9909114 | Nuno Miguel Marques de Sousa | L. R. Huiszoon, A. N. Schellekens, N. Sousa | Klein Bottles and Simple Currents | 11 pages, LaTeX. References added, minor error corrected | Phys.Lett. B470 (1999) 95-102 | 10.1016/S0370-2693(99)01241-1 | NIKHEF 99-023 | hep-th | null | The standard Klein bottle coefficient in the construction of open descendants
is shown to equal the Frobenius-Schur indicator of a conformal field theory.
Other consistent Klein bottle projections are shown to correspond to simple
currents. These observations enable us to generalize the standard open string
construct... | [
{
"created": "Thu, 16 Sep 1999 09:13:45 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Sep 1999 15:21:09 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Huiszoon",
"L. R.",
""
],
[
"Schellekens",
"A. N.",
""
],
[
"Sousa",
"N.",
""
]
] | The standard Klein bottle coefficient in the construction of open descendants is shown to equal the Frobenius-Schur indicator of a conformal field theory. Other consistent Klein bottle projections are shown to correspond to simple currents. These observations enable us to generalize the standard open string constructio... | 16.718664 | 15.092244 | 15.4645 | 15.313214 | 14.568193 | 15.02521 | 13.646843 | 13.587454 | 13.956986 | 16.977184 | 14.272863 | 13.985522 | 17.480436 | 13.52205 | 14.444051 | 13.843601 | 14.734729 | 14.165252 | 13.725681 | 15.840499 | 13.65874 |
1806.10144 | G\'abor S\'arosi | Alexandre Belin, Aitor Lewkowycz, G\'abor S\'arosi | The boundary dual of the bulk symplectic form | 6 pages, 1 figure, v2: published version | null | 10.1016/j.physletb.2018.10.071 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the overlaps of wavefunctionals prepared by turning
on sources in the Euclidean path integral. For nearby states, these overlaps
give rise to a Kahler structure on the space of sources, which is naturally
induced by the Fubini-Study metric. The Kahler form obtained this way can also
be thought... | [
{
"created": "Tue, 26 Jun 2018 18:00:02 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Dec 2018 21:03:05 GMT",
"version": "v2"
}
] | 2018-12-12 | [
[
"Belin",
"Alexandre",
""
],
[
"Lewkowycz",
"Aitor",
""
],
[
"Sárosi",
"Gábor",
""
]
] | In this paper, we study the overlaps of wavefunctionals prepared by turning on sources in the Euclidean path integral. For nearby states, these overlaps give rise to a Kahler structure on the space of sources, which is naturally induced by the Fubini-Study metric. The Kahler form obtained this way can also be thought o... | 9.96652 | 8.417922 | 10.661178 | 8.483932 | 8.765383 | 9.033069 | 8.440759 | 8.48336 | 9.058536 | 10.870126 | 8.118551 | 8.439575 | 9.479294 | 8.583592 | 8.358105 | 9.17119 | 8.722192 | 8.337936 | 8.388124 | 9.380574 | 8.34996 |
hep-th/0003298 | J\"urgen Fuchs | J. Fuchs, C. Schweigert, J. Walcher | Projections in string theory and boundary states for Gepner models | 37 pages, LaTeX2e | Nucl.Phys. B588 (2000) 110-148 | 10.1016/S0550-3213(00)00487-9 | PAR-LPTHE 00-09, ETH-TH/00-2, CERN-TH/2000-0045 | hep-th | null | In string theory various projections have to be imposed to ensure
supersymmetry. We study the consequences of these projections in the presence
of world sheet boundaries. A-type boundary conditions come in several classes;
only boundary fields that do not change the class preserve supersymmetry. Our
analysis takes in... | [
{
"created": "Fri, 31 Mar 2000 20:05:49 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Fuchs",
"J.",
""
],
[
"Schweigert",
"C.",
""
],
[
"Walcher",
"J.",
""
]
] | In string theory various projections have to be imposed to ensure supersymmetry. We study the consequences of these projections in the presence of world sheet boundaries. A-type boundary conditions come in several classes; only boundary fields that do not change the class preserve supersymmetry. Our analysis takes in p... | 19.167887 | 19.899185 | 21.554941 | 15.958839 | 16.963634 | 19.137362 | 19.500948 | 18.462563 | 17.051561 | 22.878799 | 18.707693 | 16.665579 | 18.961218 | 16.98744 | 17.00701 | 16.719011 | 17.249689 | 17.478661 | 16.825468 | 18.943428 | 16.708662 |
hep-th/9601069 | null | V.A. Kazakov, M. Staudacher and T. Wynter | Exact Solution of Discrete Two-Dimensional R^2 Gravity | 27 pages, 6 ps figures, uses harvmac.tex and epsf, minor changes | Nucl.Phys. B471 (1996) 309-333 | 10.1016/0550-3213(96)00184-8 | LPTENS-95/56 and CERN-TH/95-352 | hep-th | null | We exactly solve a special matrix model of dually weighted planar graphs
describing pure two-dimensional quantum gravity with an R^2 interaction. It
permits us to study the intermediate regimes between the gravitating and flat
metric. Flat space is modeled by a regular square lattice, while localised
curvature is int... | [
{
"created": "Sun, 14 Jan 1996 17:39:39 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Jan 1996 22:04:17 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Feb 1996 14:17:10 GMT",
"version": "v3"
}
] | 2009-10-30 | [
[
"Kazakov",
"V. A.",
""
],
[
"Staudacher",
"M.",
""
],
[
"Wynter",
"T.",
""
]
] | We exactly solve a special matrix model of dually weighted planar graphs describing pure two-dimensional quantum gravity with an R^2 interaction. It permits us to study the intermediate regimes between the gravitating and flat metric. Flat space is modeled by a regular square lattice, while localised curvature is intro... | 17.385651 | 17.528675 | 18.350258 | 16.593103 | 16.474455 | 16.500269 | 16.204308 | 19.392622 | 16.563173 | 19.070648 | 16.317972 | 15.862226 | 16.677443 | 16.213743 | 15.963843 | 15.633303 | 16.278334 | 16.379786 | 15.931817 | 16.744478 | 15.780745 |
2211.09517 | George Robert Smith Mr. | George Robert Smith, Daniel Waldram | M-theory Moduli from Exceptional Complex Structures | 40 pages, 1 figure | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue the analysis of the geometry of generic Minkowski $\mathcal{N} =
1$, $D = 4$ flux compactifications in M-theory using exceptional generalised
geometry, including the calculation of the infinitesimal moduli spaces. The
backgrounds can be classified into two classes: type-0 and type-3. For type-0,
we review... | [
{
"created": "Thu, 17 Nov 2022 13:30:02 GMT",
"version": "v1"
}
] | 2022-11-18 | [
[
"Smith",
"George Robert",
""
],
[
"Waldram",
"Daniel",
""
]
] | We continue the analysis of the geometry of generic Minkowski $\mathcal{N} = 1$, $D = 4$ flux compactifications in M-theory using exceptional generalised geometry, including the calculation of the infinitesimal moduli spaces. The backgrounds can be classified into two classes: type-0 and type-3. For type-0, we review h... | 9.183177 | 8.666924 | 9.473751 | 8.920183 | 9.268242 | 9.800779 | 9.236384 | 9.239035 | 9.148223 | 10.526824 | 8.646751 | 8.700447 | 9.225361 | 8.827572 | 8.77067 | 8.624474 | 8.763377 | 8.801593 | 8.617118 | 9.203866 | 8.707262 |
1108.0473 | Noriaki Ikeda | Noriaki Ikeda and Kozo Koizumi | Current Algebras and QP Manifolds | 24 pages, typos correted | null | null | MISC-2011-14 | hep-th math-ph math.DG math.MP math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Generalized current algebras introduced by Alekseev and Strobl in two
dimensions are reconstructed by a graded manifold and a graded Poisson
brackets. We generalize their current algebras to higher dimensions. QP
manifolds provide the unified structures of current algebras in any dimension.
Current algebras give rise... | [
{
"created": "Tue, 2 Aug 2011 02:45:40 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Nov 2011 10:39:28 GMT",
"version": "v2"
},
{
"created": "Wed, 13 Feb 2013 12:27:01 GMT",
"version": "v3"
}
] | 2013-02-14 | [
[
"Ikeda",
"Noriaki",
""
],
[
"Koizumi",
"Kozo",
""
]
] | Generalized current algebras introduced by Alekseev and Strobl in two dimensions are reconstructed by a graded manifold and a graded Poisson brackets. We generalize their current algebras to higher dimensions. QP manifolds provide the unified structures of current algebras in any dimension. Current algebras give rise t... | 10.261099 | 10.356492 | 12.688014 | 9.700676 | 9.414447 | 10.500064 | 10.696042 | 10.318399 | 9.536929 | 13.119551 | 10.041768 | 9.622085 | 10.335052 | 9.768111 | 9.733833 | 9.795068 | 9.647694 | 9.962268 | 9.718464 | 11.011347 | 9.60544 |
2201.00105 | Benjamin C. Harms | Casey Cartwright, Benjamin Harms, Matthias Kaminski, Ronny Thomale | Topological confinement in Skyrme holography | 21 pages, 8 figures, new title, additional author | null | 10.1088/1361-6382/ac6c73 | null | hep-th cond-mat.str-el hep-ph nucl-th | http://creativecommons.org/licenses/by/4.0/ | We study phase transitions in five-dimensional Einstein Gravity with a
negative cosmological constant, coupled to a Skyrme matter field. These
transitions are topological generalizations of the Hawking-Page transition
between thermal Anti de Sitter (AdS) spacetime and an AdS black hole. Phases
are characterized by a ... | [
{
"created": "Sat, 1 Jan 2022 03:33:41 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Jan 2022 19:59:38 GMT",
"version": "v2"
}
] | 2022-06-08 | [
[
"Cartwright",
"Casey",
""
],
[
"Harms",
"Benjamin",
""
],
[
"Kaminski",
"Matthias",
""
],
[
"Thomale",
"Ronny",
""
]
] | We study phase transitions in five-dimensional Einstein Gravity with a negative cosmological constant, coupled to a Skyrme matter field. These transitions are topological generalizations of the Hawking-Page transition between thermal Anti de Sitter (AdS) spacetime and an AdS black hole. Phases are characterized by a to... | 6.816883 | 7.024435 | 7.550943 | 6.610623 | 7.398752 | 6.994382 | 7.047302 | 6.967366 | 7.286498 | 7.57818 | 6.896355 | 6.71001 | 6.964166 | 6.681537 | 6.74881 | 6.990844 | 6.974458 | 6.773695 | 6.990658 | 7.04212 | 6.888776 |
1606.03104 | Sebastian Garcia-Saenz | Angelo Esposito, Sebastian Garcia-Saenz, and Riccardo Penco | First Sound in Holographic Superfluids at Zero Temperature | 14 pages. Extended discussions in sections 3 and 4 | J. High Energ. Phys. (2016) 2016: 136 | 10.1007/JHEP12(2016)136 | null | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Within the context of AdS/CFT, the gravity dual of an s-wave superfluid is
given by scalar QED on an asymptotically AdS spacetime. While this conclusion
is vastly supported by numerical arguments, here we provide an analytical proof
that this is indeed the case. Working at zero temperature, we explicitly find
the qua... | [
{
"created": "Thu, 9 Jun 2016 20:05:33 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Aug 2016 14:27:39 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Dec 2016 15:13:20 GMT",
"version": "v3"
}
] | 2016-12-30 | [
[
"Esposito",
"Angelo",
""
],
[
"Garcia-Saenz",
"Sebastian",
""
],
[
"Penco",
"Riccardo",
""
]
] | Within the context of AdS/CFT, the gravity dual of an s-wave superfluid is given by scalar QED on an asymptotically AdS spacetime. While this conclusion is vastly supported by numerical arguments, here we provide an analytical proof that this is indeed the case. Working at zero temperature, we explicitly find the quadr... | 11.492359 | 11.290607 | 10.668794 | 10.241465 | 10.996938 | 11.384037 | 11.09796 | 10.09406 | 10.176921 | 12.065507 | 9.885462 | 10.775831 | 10.638536 | 10.332922 | 10.416139 | 10.441998 | 10.581998 | 10.359528 | 10.112656 | 10.114956 | 10.241233 |
hep-th/0005283 | Bin Chen | B. Chen, H. Itoyama, T. Matsuo and K. Murakami | Worldsheet and Spacetime Properties of p-p' System with B Field and
Noncommutative Geometry | 41 pages, 4 figures, Latex; revised version, typos corrected, comment
on spacetime picture and eq. (5.8) improved | Nucl.Phys. B593 (2001) 505-544 | 10.1016/S0550-3213(00)00615-5 | OU-HET 345 | hep-th | null | We study worldsheet and spacetime properties of the p-p' (p < p') open string
system with constant B_{ij} field viewed from the Dp' brane. The description of
this system in terms of the CFT with spin and twist fields leads us to consider
the renormal ordering procedure from the SL(2,R) invariant vacuum to the
oscilla... | [
{
"created": "Wed, 31 May 2000 11:51:30 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jun 2000 13:01:14 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Sep 2000 03:10:16 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Chen",
"B.",
""
],
[
"Itoyama",
"H.",
""
],
[
"Matsuo",
"T.",
""
],
[
"Murakami",
"K.",
""
]
] | We study worldsheet and spacetime properties of the p-p' (p < p') open string system with constant B_{ij} field viewed from the Dp' brane. The description of this system in terms of the CFT with spin and twist fields leads us to consider the renormal ordering procedure from the SL(2,R) invariant vacuum to the oscillato... | 15.171639 | 15.016347 | 17.993042 | 14.856775 | 15.937125 | 16.46834 | 14.879828 | 15.527044 | 15.097002 | 18.731998 | 15.028631 | 14.877601 | 16.881939 | 15.014908 | 14.693128 | 15.277896 | 15.198738 | 15.209743 | 15.182835 | 16.516197 | 15.085743 |
2204.09336 | Paul K. Townsend | Luca Mezincescu and Paul K. Townsend | On chiral bosons in 2D and 6D | 24 pages, minor corrections and further additional references in v3 | null | 10.1007/JHEP07(2022)142 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the Hamiltonian formulation of chiral 2k-form electrodynamics, the 2k-form
potential on the (4k+1)-space is defined up to the addition of either (i) a
closed $2k$-form or (ii) an exact 2k-form, depending on the choice of chirality
constraint. Case (i) is realized by the Floreanini-Jackiw 2D chiral boson (for
k=0) ... | [
{
"created": "Wed, 20 Apr 2022 09:12:39 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Apr 2022 20:49:46 GMT",
"version": "v2"
},
{
"created": "Thu, 30 Jun 2022 12:02:09 GMT",
"version": "v3"
}
] | 2022-08-10 | [
[
"Mezincescu",
"Luca",
""
],
[
"Townsend",
"Paul K.",
""
]
] | In the Hamiltonian formulation of chiral 2k-form electrodynamics, the 2k-form potential on the (4k+1)-space is defined up to the addition of either (i) a closed $2k$-form or (ii) an exact 2k-form, depending on the choice of chirality constraint. Case (i) is realized by the Floreanini-Jackiw 2D chiral boson (for k=0) an... | 7.716061 | 7.19995 | 7.865694 | 7.071959 | 8.239185 | 7.856392 | 7.584827 | 7.168058 | 7.191475 | 8.594792 | 6.915272 | 6.7901 | 7.176604 | 6.957422 | 7.203433 | 7.150485 | 7.056785 | 6.85988 | 7.254848 | 7.374339 | 7.117837 |
2207.03468 | Gerben Oling | Stefano Baiguera, Gerben Oling, Watse Sybesma, Benjamin T. S{\o}gaard | Conformal Carroll Scalars with Boosts | 29+6 pages, two figures; v2: minor changes, added references, v3:
expanded discussion of dimensional reduction, minor changes, one reference
added | SciPost Phys. 14, 086 (2023) | 10.21468/SciPostPhys.14.4.086 | NORDITA 2022-047 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct two distinct actions for scalar fields that are invariant under
local Carroll boosts and Weyl transformations. Conformal Carroll field theories
were recently argued to be related to the celestial holography description of
asymptotically flat spacetimes. However, only few explicit examples of such
theorie... | [
{
"created": "Thu, 7 Jul 2022 17:50:00 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Sep 2022 15:29:26 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Dec 2022 13:30:08 GMT",
"version": "v3"
}
] | 2023-04-26 | [
[
"Baiguera",
"Stefano",
""
],
[
"Oling",
"Gerben",
""
],
[
"Sybesma",
"Watse",
""
],
[
"Søgaard",
"Benjamin T.",
""
]
] | We construct two distinct actions for scalar fields that are invariant under local Carroll boosts and Weyl transformations. Conformal Carroll field theories were recently argued to be related to the celestial holography description of asymptotically flat spacetimes. However, only few explicit examples of such theories ... | 9.72096 | 8.691527 | 9.943541 | 8.596726 | 8.72648 | 8.652571 | 8.591037 | 9.043588 | 8.487654 | 11.140841 | 8.587054 | 8.669002 | 9.208106 | 8.770655 | 8.840719 | 8.861057 | 9.073439 | 8.716241 | 8.84446 | 9.418628 | 8.689449 |
hep-th/0701016 | Yifu Cai | Yi-fu Cai, Mingzhe Li, Jian-Xin Lu, Yun-Song Piao, Taotao Qiu, and
Xinmin Zhang | A String-Inspired Quintom Model Of Dark Energy | 6 pages, 4 figures, accepted by PLB | Phys.Lett.B651:1-7,2007 | 10.1016/j.physletb.2007.05.056 | null | hep-th astro-ph gr-qc hep-ph | null | We propose in this paper a quintom model of dark energy with a single scalar
field $\phi$ given by the lagrangian ${\cal
L}=-V(\phi)\sqrt{1-\alpha^\prime\nabla_{\mu}\phi\nabla^{\mu}\phi +\beta^\prime
\phi\Box\phi}$. In the limit of $\beta^\prime\to$0 our model reduces to the
effective low energy lagrangian of tachyon... | [
{
"created": "Tue, 2 Jan 2007 17:05:16 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Jan 2007 02:59:39 GMT",
"version": "v2"
},
{
"created": "Wed, 23 May 2007 11:52:23 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Cai",
"Yi-fu",
""
],
[
"Li",
"Mingzhe",
""
],
[
"Lu",
"Jian-Xin",
""
],
[
"Piao",
"Yun-Song",
""
],
[
"Qiu",
"Taotao",
""
],
[
"Zhang",
"Xinmin",
""
]
] | We propose in this paper a quintom model of dark energy with a single scalar field $\phi$ given by the lagrangian ${\cal L}=-V(\phi)\sqrt{1-\alpha^\prime\nabla_{\mu}\phi\nabla^{\mu}\phi +\beta^\prime \phi\Box\phi}$. In the limit of $\beta^\prime\to$0 our model reduces to the effective low energy lagrangian of tachyon c... | 5.225413 | 5.286356 | 4.785564 | 4.582131 | 5.015281 | 5.187225 | 5.466289 | 4.996239 | 4.98231 | 4.893081 | 4.778465 | 4.98234 | 5.106274 | 4.842593 | 5.073045 | 5.04749 | 5.172266 | 4.910225 | 5.081538 | 5.089034 | 5.239357 |
hep-th/9903111 | Henning Samtleben | K. Koepsell, H. Nicolai, H. Samtleben | On the Yangian Y(e_8) quantum symmetry of maximal supergravity in two
dimensions | 21 pages, LaTeX2e | JHEP 9904:023,1999 | 10.1088/1126-6708/1999/04/023 | AEI-103, LPTENS-99/08 | hep-th | null | We present the algebraic framework for the quantization of the classical
bosonic charge algebra of maximally extended (N=16) supergravity in two
dimensions, thereby taking the first steps towards an exact quantization of
this model. At the core of our construction is the Yangian algebra $Y(e_8)$
whose RTT presentatio... | [
{
"created": "Fri, 12 Mar 1999 08:01:05 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Koepsell",
"K.",
""
],
[
"Nicolai",
"H.",
""
],
[
"Samtleben",
"H.",
""
]
] | We present the algebraic framework for the quantization of the classical bosonic charge algebra of maximally extended (N=16) supergravity in two dimensions, thereby taking the first steps towards an exact quantization of this model. At the core of our construction is the Yangian algebra $Y(e_8)$ whose RTT presentation ... | 8.550183 | 7.466115 | 9.734249 | 7.679099 | 8.071952 | 8.439076 | 7.963818 | 7.872922 | 7.708789 | 10.035363 | 7.795112 | 7.907568 | 8.029184 | 7.723101 | 7.671617 | 7.710395 | 7.810307 | 7.682168 | 7.678583 | 8.596901 | 7.751862 |
1206.0468 | Matthew Dodelson | Matthew Dodelson | Transition Amplitudes in de Sitter Space | 15 pages, as published in JHEP, with clarifications and references
added | null | 10.1007/JHEP08(2012)011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Maldacena has shown that the wavefunction of the universe in de Sitter space
can be viewed as the partition function of a conformal field theory. In this
paper, we investigate this approach to the dS/CFT correspondence in further
detail. We emphasize that massive bulk fields are dual to two primary operators
on the b... | [
{
"created": "Sun, 3 Jun 2012 17:15:19 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Jun 2012 19:36:58 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Jul 2012 01:04:54 GMT",
"version": "v3"
},
{
"created": "Fri, 24 Aug 2012 21:02:54 GMT",
"version": "v4"
}
] | 2015-06-05 | [
[
"Dodelson",
"Matthew",
""
]
] | Maldacena has shown that the wavefunction of the universe in de Sitter space can be viewed as the partition function of a conformal field theory. In this paper, we investigate this approach to the dS/CFT correspondence in further detail. We emphasize that massive bulk fields are dual to two primary operators on the bou... | 7.425208 | 7.464113 | 7.297935 | 7.218859 | 7.332191 | 7.856379 | 7.528425 | 7.058149 | 7.492087 | 8.129898 | 7.397466 | 6.772642 | 7.150074 | 6.700216 | 6.781331 | 6.611529 | 6.772366 | 6.833001 | 6.624911 | 7.208127 | 6.845597 |
hep-th/9707050 | Pierre Mathieu | Pierre Mathieu and Gerard Watts | Probing integrable perturbations of conformal theories using singular
vectors II: N=1 superconformal theories | 30 pages, Latex2e (rotating.sty,amssymb.sty,a4wide.sty) | Nucl.Phys. B510 (1998) 577-607 | 10.1016/S0550-3213(97)00704-9 | LAVAL-PHY-97-23 and KCL-MTH-97-41 | hep-th | null | In this work we pursue the singular-vector analysis of the integrable
perturbations of conformal theories that was initiated in hep-th/9603088. Here
we consider the detailed study of the N=1 superconformal theory and show that
all integrable perturbations can be identified from a simple singular-vector
argument. We i... | [
{
"created": "Thu, 3 Jul 1997 21:17:30 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Mathieu",
"Pierre",
""
],
[
"Watts",
"Gerard",
""
]
] | In this work we pursue the singular-vector analysis of the integrable perturbations of conformal theories that was initiated in hep-th/9603088. Here we consider the detailed study of the N=1 superconformal theory and show that all integrable perturbations can be identified from a simple singular-vector argument. We ide... | 10.984557 | 9.705115 | 11.253263 | 9.163958 | 9.804942 | 10.450187 | 9.651011 | 9.70654 | 9.126532 | 11.253 | 9.418359 | 9.752397 | 9.76795 | 9.337273 | 9.74143 | 9.585082 | 9.716705 | 9.759186 | 9.322023 | 9.992973 | 9.619012 |
1710.10953 | Omer Gurdogan | James Drummond, Jack Foster, Omer Gurdogan | Cluster adjacency properties of scattering amplitudes | 6 pages, 3 figures. Symbols of integrals presented in four ancillary
files, as detailed in README.txt | Phys. Rev. Lett. 120, 161601 (2018) | 10.1103/PhysRevLett.120.161601 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We conjecture a new set of analytic relations for scattering amplitudes in
planar N=4 super Yang-Mills theory. They generalise the Steinmann relations and
are expressed in terms of the cluster algebras associated to Gr(4,n). In terms
of the symbol, they dictate which letters can appear consecutively. We study
heptago... | [
{
"created": "Mon, 30 Oct 2017 14:12:12 GMT",
"version": "v1"
}
] | 2018-04-25 | [
[
"Drummond",
"James",
""
],
[
"Foster",
"Jack",
""
],
[
"Gurdogan",
"Omer",
""
]
] | We conjecture a new set of analytic relations for scattering amplitudes in planar N=4 super Yang-Mills theory. They generalise the Steinmann relations and are expressed in terms of the cluster algebras associated to Gr(4,n). In terms of the symbol, they dictate which letters can appear consecutively. We study heptagon ... | 8.869817 | 7.1978 | 10.039097 | 7.803822 | 7.225143 | 8.059409 | 9.357975 | 7.458732 | 7.347 | 9.611752 | 8.4489 | 7.831659 | 9.292116 | 8.044141 | 8.253033 | 8.079429 | 8.222892 | 7.491199 | 7.88468 | 8.893787 | 7.67542 |
0807.1444 | Pang Yi | Yi Pang, Tower Wang | From N M2's to N D2's | 11 pages, 1 printable figure, close to the version published in
PhysRevD | Phys.Rev.D78:125007,2008 | 10.1103/PhysRevD.78.125007 | USTC-ICTS-08-12 | hep-th | http://creativecommons.org/licenses/by/3.0/ | In this short note, we reduce the N=6, U(N)xU(N) Chern-Simons gauge theories
to N=8, U(N) Yang-Mills gauge theories. This process corresponds to recovering
the world-volume theory of N D2-branes from that of N M2-branes in an
intermediate energy range. The supersymmetries are enhanced because in this
limit the branes... | [
{
"created": "Wed, 9 Jul 2008 13:18:08 GMT",
"version": "v1"
},
{
"created": "Wed, 30 Jul 2008 06:37:09 GMT",
"version": "v2"
},
{
"created": "Sun, 31 Aug 2008 07:28:39 GMT",
"version": "v3"
},
{
"created": "Wed, 6 May 2009 15:14:12 GMT",
"version": "v4"
}
] | 2009-05-06 | [
[
"Pang",
"Yi",
""
],
[
"Wang",
"Tower",
""
]
] | In this short note, we reduce the N=6, U(N)xU(N) Chern-Simons gauge theories to N=8, U(N) Yang-Mills gauge theories. This process corresponds to recovering the world-volume theory of N D2-branes from that of N M2-branes in an intermediate energy range. The supersymmetries are enhanced because in this limit the branes l... | 11.69126 | 10.092507 | 13.416998 | 9.54769 | 9.896846 | 10.064152 | 10.139299 | 9.855145 | 9.840823 | 12.275437 | 10.201639 | 10.173507 | 11.287621 | 9.972608 | 9.906709 | 9.678271 | 10.114252 | 10.295653 | 10.220514 | 11.188148 | 10.137767 |
0710.4249 | Alexander Burinskii | Alexander Burinskii | Complex Kerr Geometry, Twistors and the Dirac Electron | 12 pages, 3 figs. Talk at the conference QFEXT'07 | J.Phys.A41:164069,2008 | 10.1088/1751-8113/41/16/164069 | null | hep-th gr-qc quant-ph | null | The Kerr-Newman spinning particle displays some remarkable relations to the
Dirac electron and has a reach spinor structure which is based on a twistorial
description of the Kerr congruence determined by the Kerr theorem. We consider
the relation between this spinor-twistorial structure and spinors of the Dirac
equat... | [
{
"created": "Tue, 23 Oct 2007 14:16:30 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Mar 2008 15:09:42 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Burinskii",
"Alexander",
""
]
] | The Kerr-Newman spinning particle displays some remarkable relations to the Dirac electron and has a reach spinor structure which is based on a twistorial description of the Kerr congruence determined by the Kerr theorem. We consider the relation between this spinor-twistorial structure and spinors of the Dirac equatio... | 12.645258 | 11.028859 | 12.251261 | 11.264688 | 11.58825 | 11.274164 | 12.23403 | 10.943548 | 11.222097 | 12.460668 | 11.385644 | 11.639602 | 12.292536 | 11.953374 | 11.907785 | 11.627295 | 12.002633 | 11.790779 | 11.846473 | 12.815362 | 11.263117 |
0909.0087 | Pramod Shukla | Aalok Misra, Pramod Shukla | Soft SUSY Breaking Parameters and RG Running of Squark and Slepton
Masses in Large Volume Swiss Cheese Compactifications | v2:10 pages, LaTeX; change in title and new material added on
particle spectrum and FCNC constraints; to appear in PLB | Phys.Lett.B685:347-352,2010 | 10.1016/j.physletb.2010.02.011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider type IIB large volume compactifications involving orientifolds of
the Swiss-Cheese Calabi-Yau WCP^4[1; 1; 1; 6; 9] with a single mobile
space-time filling D3-brane and stacks of D7-branes wrapping the "big" divisor
(as opposed to the "small" divisor usually done in the literature thus far) as
well as supp... | [
{
"created": "Tue, 1 Sep 2009 04:46:34 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Feb 2010 05:44:40 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Misra",
"Aalok",
""
],
[
"Shukla",
"Pramod",
""
]
] | We consider type IIB large volume compactifications involving orientifolds of the Swiss-Cheese Calabi-Yau WCP^4[1; 1; 1; 6; 9] with a single mobile space-time filling D3-brane and stacks of D7-branes wrapping the "big" divisor (as opposed to the "small" divisor usually done in the literature thus far) as well as suppor... | 8.490255 | 7.963614 | 9.584835 | 8.424787 | 8.411158 | 8.544815 | 8.399662 | 8.380333 | 8.438567 | 10.725591 | 8.145363 | 8.782151 | 8.677089 | 8.491926 | 8.362082 | 8.685285 | 8.462351 | 8.628492 | 8.590022 | 8.96262 | 8.327847 |
1103.1381 | Pedro Pina Avelino | L. Sousa, P.P. Avelino | p-brane dynamics in (N+1)-dimensional FRW universes: a unified framework | 6 pages | Phys.Rev.D83:103507,2011 | 10.1103/PhysRevD.83.103507 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a velocity-dependent one-scale model describing p-brane dynamics
in flat homogeneous and isotropic backgrounds in a unified framework. We find
the corresponding scaling laws in frictionless and friction dominated regimes
considering both expanding and collapsing phases.
| [
{
"created": "Mon, 7 Mar 2011 21:00:02 GMT",
"version": "v1"
}
] | 2011-05-13 | [
[
"Sousa",
"L.",
""
],
[
"Avelino",
"P. P.",
""
]
] | We develop a velocity-dependent one-scale model describing p-brane dynamics in flat homogeneous and isotropic backgrounds in a unified framework. We find the corresponding scaling laws in frictionless and friction dominated regimes considering both expanding and collapsing phases. | 24.539927 | 15.059884 | 20.850447 | 16.405787 | 19.214527 | 19.85198 | 18.120216 | 16.867138 | 19.191397 | 20.859039 | 19.022871 | 21.061958 | 24.343178 | 20.802427 | 23.828804 | 20.764704 | 22.337864 | 21.839817 | 20.188148 | 21.162432 | 22.942347 |
1109.2278 | S. E. Korenblit | V.V. Semenov and S.E. Korenblit | Finite temperature Thirring model: from linearization through canonical
transformations to correct normal form of thermofield solution | 53 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that exact solvability of the finite temperature massless
Thirring model, as well as of its zero temperature case, in canonical
quantization scheme originates from the intrinsic hidden exact linearizability
of Heisenberg equations by means of dynamical mapping onto the Schr\"odinger
physical fields. The n... | [
{
"created": "Sun, 11 Sep 2011 04:26:52 GMT",
"version": "v1"
}
] | 2011-09-13 | [
[
"Semenov",
"V. V.",
""
],
[
"Korenblit",
"S. E.",
""
]
] | It is shown that exact solvability of the finite temperature massless Thirring model, as well as of its zero temperature case, in canonical quantization scheme originates from the intrinsic hidden exact linearizability of Heisenberg equations by means of dynamical mapping onto the Schr\"odinger physical fields. The nor... | 14.780931 | 14.03689 | 15.438481 | 13.877746 | 15.279086 | 14.310297 | 14.550292 | 13.487415 | 13.735545 | 16.718075 | 14.064279 | 14.150963 | 14.451329 | 14.288879 | 14.099252 | 14.333342 | 14.2716 | 13.995803 | 13.974607 | 14.736847 | 14.286713 |
hep-th/0405114 | Nelson R. F. Braga | Ricardo Amorim, Henrique Boschi-Filho and Nelson R. F. Braga | Remarks on gauge fixing and BRST quantization of noncommutative gauge
theories | 8 pages, no figures. In this revised version, we included the
explicit Seiberg Witten maps for antighost and auxiliary fields. We used this
expressions to show that it is not possible to relate the Lorentz gauge in
noncommutative and ordinary YM theories by the SW map, as claimed in the
previous version | Braz.J.Phys.35:645-651,2005 | 10.1590/S0103-97332005000400011 | null | hep-th | null | We consider the BRST gauge fixing procedure of the noncommutative Yang-Mills
theory and of the gauged U(N) Proca model. An extended Seiberg-Witten map
involving ghosts, antighosts and auxiliary fields for non Abelian gauge
theories is studied. We find that the extended map behaves differently for
these models. For th... | [
{
"created": "Wed, 12 May 2004 18:46:40 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Aug 2004 19:33:34 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Amorim",
"Ricardo",
""
],
[
"Boschi-Filho",
"Henrique",
""
],
[
"Braga",
"Nelson R. F.",
""
]
] | We consider the BRST gauge fixing procedure of the noncommutative Yang-Mills theory and of the gauged U(N) Proca model. An extended Seiberg-Witten map involving ghosts, antighosts and auxiliary fields for non Abelian gauge theories is studied. We find that the extended map behaves differently for these models. For the ... | 7.576773 | 7.099173 | 7.948663 | 7.126145 | 7.289527 | 6.95336 | 7.104965 | 6.595526 | 6.699206 | 8.773568 | 7.108582 | 7.382292 | 7.58157 | 7.195374 | 7.337813 | 7.050565 | 6.973963 | 7.368268 | 7.353484 | 7.309429 | 7.084766 |
1006.4369 | Jan Gutowski | J. Gutowski and G. Papadopoulos | Topology of supersymmetric N=1, D=4 supergravity horizons | 17 pages, latex. Alterations to introduction and section 3.3 | JHEP 1011:114,2010 | 10.1007/JHEP11(2010)114 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | All supersymmetric N=1, D=4 supergravity horizons have toroidal or spherical
topology, irrespective of whether the black hole preserves any supersymmetry.
| [
{
"created": "Tue, 22 Jun 2010 20:27:00 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Sep 2010 11:39:08 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Nov 2010 14:13:23 GMT",
"version": "v3"
}
] | 2010-11-30 | [
[
"Gutowski",
"J.",
""
],
[
"Papadopoulos",
"G.",
""
]
] | All supersymmetric N=1, D=4 supergravity horizons have toroidal or spherical topology, irrespective of whether the black hole preserves any supersymmetry. | 18.558928 | 15.136069 | 19.881752 | 13.827983 | 14.819026 | 14.243934 | 18.241842 | 14.818447 | 16.852776 | 23.663212 | 14.218937 | 11.712972 | 15.721319 | 13.370282 | 12.295174 | 13.178579 | 12.813004 | 13.137117 | 13.977225 | 16.567419 | 13.721216 |
hep-th/9804053 | Johanna Erdmenger | Johanna Erdmenger, Christian Rupp and Klaus Sibold | Conformal Transformation Properties of the Supercurrent in Four
Dimensional Supersymmetric Theories | 35 pages, AMS-LaTex, four ps figures. Two remarks added, misprints
corrected. To be published in Nuclear Physics B | Nucl.Phys. B530 (1998) 501-533 | 10.1016/S0550-3213(98)00476-3 | NTZ-7/98 | hep-th | null | We investigate the superconformal transformation properties of Green
functions with one or more insertions of the supercurrent in N=1 supersymmetric
quantum field theories. These Green functions are conveniently obtained by
coupling the supercurrent and its trace to a classical supergravity background.
We derive flat... | [
{
"created": "Tue, 7 Apr 1998 14:17:13 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Jul 1998 09:17:12 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Erdmenger",
"Johanna",
""
],
[
"Rupp",
"Christian",
""
],
[
"Sibold",
"Klaus",
""
]
] | We investigate the superconformal transformation properties of Green functions with one or more insertions of the supercurrent in N=1 supersymmetric quantum field theories. These Green functions are conveniently obtained by coupling the supercurrent and its trace to a classical supergravity background. We derive flat s... | 8.577669 | 8.806268 | 9.312615 | 8.000923 | 8.472466 | 8.822327 | 9.019866 | 8.362755 | 8.156839 | 10.184857 | 8.173869 | 8.504042 | 8.557895 | 8.423895 | 8.454516 | 8.207878 | 8.262321 | 8.270441 | 8.620439 | 8.546461 | 8.266776 |
hep-th/0510115 | Paul K. Townsend | Julian Sonner and Paul K. Townsend | Dilaton Domain Walls and Dynamical Systems | 30 pp, 11 figs, significant revision of original. Minor additional
corrections in version to appear in journal | Class.Quant.Grav.23:441-464,2006 | 10.1088/0264-9381/23/2/010 | DAMTP-2005-94 | hep-th | null | Domain wall solutions of $d$-dimensional gravity coupled to a dilaton field
$\sigma$ with an exponential potential $\Lambda e^{-\lambda\sigma}$ are shown
to be governed by an autonomous dynamical system, with a transcritical
bifurcation as a function of the parameter $\lambda$ when $\Lambda<0$. All
phase-plane trajec... | [
{
"created": "Fri, 14 Oct 2005 13:51:36 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Oct 2005 15:03:11 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Nov 2005 14:58:36 GMT",
"version": "v3"
},
{
"created": "Thu, 24 Nov 2005 15:37:32 GMT",
"version": "v4"
}
] | 2010-12-03 | [
[
"Sonner",
"Julian",
""
],
[
"Townsend",
"Paul K.",
""
]
] | Domain wall solutions of $d$-dimensional gravity coupled to a dilaton field $\sigma$ with an exponential potential $\Lambda e^{-\lambda\sigma}$ are shown to be governed by an autonomous dynamical system, with a transcritical bifurcation as a function of the parameter $\lambda$ when $\Lambda<0$. All phase-plane trajecto... | 9.702709 | 8.583725 | 9.367277 | 7.752262 | 8.281247 | 8.140969 | 8.694399 | 8.339153 | 8.342807 | 10.33103 | 7.696893 | 8.050997 | 8.563584 | 8.222045 | 8.326221 | 8.184768 | 8.104915 | 8.265272 | 8.19602 | 8.926637 | 8.199479 |
0908.1272 | Da-Wei Pang | Da-Wei Pang | R^2 Corrections to Asymptotically Lifshitz Spacetimes | 24 pages, Latex, typos fixed, accepted by JHEP | JHEP 0910:031,2009 | 10.1088/1126-6708/2009/10/031 | CQUeST-2009-0274 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $R^{2}$ corrections to five-dimensional asymptotically Lifshitz
spacetimes by adding Gauss-Bonnet terms in the effective action. For the
zero-temperature backgrounds we obtain exact solutions in both pure
Gauss-Bonnet gravity and Gauss-Bonnet gravity with non-trivial matter. The
dynamical exponent undergoes ... | [
{
"created": "Mon, 10 Aug 2009 06:16:28 GMT",
"version": "v1"
},
{
"created": "Sun, 11 Oct 2009 01:30:23 GMT",
"version": "v2"
}
] | 2009-10-29 | [
[
"Pang",
"Da-Wei",
""
]
] | We study $R^{2}$ corrections to five-dimensional asymptotically Lifshitz spacetimes by adding Gauss-Bonnet terms in the effective action. For the zero-temperature backgrounds we obtain exact solutions in both pure Gauss-Bonnet gravity and Gauss-Bonnet gravity with non-trivial matter. The dynamical exponent undergoes fi... | 9.046138 | 7.499831 | 9.313904 | 7.870847 | 6.940175 | 7.671456 | 7.866069 | 7.548855 | 7.530698 | 9.266515 | 7.282126 | 7.677557 | 8.693256 | 7.857021 | 7.743675 | 7.805487 | 7.664426 | 7.634591 | 7.631463 | 8.68054 | 7.637679 |
2203.14351 | V. Parameswaran Nair | V.P. Nair | Entanglement Entropy and Matter-Gravity Couplings for Fuzzy Geometry | 13 pages; Talk presented at eh workshop on "Quantum Geometry,Field
Theory and Gravity", Corfu Summer Institute 2021 | null | null | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this talk I discuss some features of the entanglement entropy for fuzzy
geometry, focusing on its dependence on the background fields and the spin
connection of the emergent continuous manifold in a large $N$ limit. Using the
Landau-Hall paradigm for fuzzy geometry, this is argued to be given by a
generalized Cher... | [
{
"created": "Sun, 27 Mar 2022 17:20:45 GMT",
"version": "v1"
}
] | 2022-03-29 | [
[
"Nair",
"V. P.",
""
]
] | In this talk I discuss some features of the entanglement entropy for fuzzy geometry, focusing on its dependence on the background fields and the spin connection of the emergent continuous manifold in a large $N$ limit. Using the Landau-Hall paradigm for fuzzy geometry, this is argued to be given by a generalized Chern-... | 16.287502 | 14.982937 | 16.660379 | 14.226561 | 16.36565 | 15.056416 | 15.879875 | 14.437123 | 14.559739 | 18.812138 | 14.609076 | 14.245699 | 15.108171 | 14.77261 | 15.023688 | 14.504172 | 14.915553 | 14.04268 | 14.679656 | 15.462049 | 14.723022 |
hep-th/9810110 | Kimyeong Lee | Kimyeong Lee | Sheets of BPS Monopoles and Instantons with Arbitrary Simple Gauge Group | LaTex file, 11 pages | Phys.Lett. B445 (1999) 387-393 | 10.1016/S0370-2693(98)01463-4 | SNUTP-98-113 | hep-th | null | We show that the BPS configurations of uniform field strength can be
interpreted as those for sheets of infinite number of BPS magnetic monopoles,
and found that the number of normalizable zero modes per each magnetic monopole
charge is four. We identify monopole sheets as the intersecting planes of D3
branes. Simila... | [
{
"created": "Thu, 15 Oct 1998 03:38:13 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Lee",
"Kimyeong",
""
]
] | We show that the BPS configurations of uniform field strength can be interpreted as those for sheets of infinite number of BPS magnetic monopoles, and found that the number of normalizable zero modes per each magnetic monopole charge is four. We identify monopole sheets as the intersecting planes of D3 branes. Similar ... | 15.363857 | 15.234092 | 16.272644 | 13.775546 | 14.951913 | 14.300672 | 14.417819 | 14.884782 | 14.679538 | 18.342009 | 13.51721 | 14.151283 | 15.399121 | 14.139772 | 14.099988 | 14.78072 | 14.194907 | 14.519911 | 14.658735 | 15.069076 | 13.78097 |
hep-th/9611059 | Arthur Lue | Arthur Lue (MIT) | Quantum effects on winding configurations in SU(2)-Higgs theory | 12 pages, 2 eps figures, RevTeX, psfig.sty included. Substantial
content changes. Analysis improved to include higher-loop effects | Phys.Rev.D55:6725-6729,1997 | 10.1103/PhysRevD.55.6725 | MIT-CTP-2585 | hep-th hep-ph | null | We examine the quantum corrections to the static energy for Higgs winding
configurations in order to ascertain whether such corrections may stabilize
solitons in the standard model. We evaluate the effective action for winding
configurations in Weinberg-Salam theory without U(1)-gauge fields or fermions.
For a config... | [
{
"created": "Fri, 8 Nov 1996 15:20:59 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Dec 1996 17:59:33 GMT",
"version": "v2"
}
] | 2009-12-30 | [
[
"Lue",
"Arthur",
"",
"MIT"
]
] | We examine the quantum corrections to the static energy for Higgs winding configurations in order to ascertain whether such corrections may stabilize solitons in the standard model. We evaluate the effective action for winding configurations in Weinberg-Salam theory without U(1)-gauge fields or fermions. For a configur... | 8.931467 | 10.082736 | 8.312682 | 8.426255 | 10.346828 | 10.186346 | 9.160985 | 9.806452 | 8.234353 | 10.536593 | 8.874494 | 8.784599 | 8.645541 | 8.39768 | 8.744088 | 8.794101 | 8.625583 | 8.84143 | 8.751052 | 8.832023 | 8.731745 |
1601.02836 | Sudarshan Ananth | Sudarshan Ananth, Lars Brink and Sucheta Majumdar | Exceptional versus superPoincar\'e algebra as the defining symmetry of
maximal supergravity | 22 pages | JHEP 1603 (2016) 051 | 10.1007/JHEP03(2016)051 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe how one may use either the superPoincar\'e algebra or the
exceptional algebra to construct maximal supergravity theories in the
light-cone formalism. The d=4 construction shows both symmetries albeit in a
non-linearly realized manner. In d=11, we find that we have to choose which of
these two symmetries t... | [
{
"created": "Tue, 12 Jan 2016 12:55:35 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Feb 2017 10:04:10 GMT",
"version": "v2"
}
] | 2020-02-25 | [
[
"Ananth",
"Sudarshan",
""
],
[
"Brink",
"Lars",
""
],
[
"Majumdar",
"Sucheta",
""
]
] | We describe how one may use either the superPoincar\'e algebra or the exceptional algebra to construct maximal supergravity theories in the light-cone formalism. The d=4 construction shows both symmetries albeit in a non-linearly realized manner. In d=11, we find that we have to choose which of these two symmetries to ... | 11.710373 | 11.805091 | 11.302918 | 11.303864 | 12.014627 | 10.680841 | 11.585717 | 11.862221 | 11.41061 | 12.218225 | 10.940688 | 10.59776 | 10.968593 | 10.756772 | 11.279254 | 10.45457 | 10.776733 | 10.620743 | 10.790432 | 11.571319 | 10.62968 |
0806.1218 | Juan Maldacena | Ofer Aharony, Oren Bergman, Daniel Louis Jafferis and Juan Maldacena | N=6 superconformal Chern-Simons-matter theories, M2-branes and their
gravity duals | 41 pages, 4 figures. v3: minor corrections, added references. v4:
added reference, minor changes, JHEP version | JHEP 0810:091,2008 | 10.1088/1126-6708/2008/10/091 | WIS/12/08-JUN-DPP | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct three dimensional Chern-Simons-matter theories with gauge groups
U(N)xU(N) and SU(N)xSU(N) which have explicit N=6 superconformal symmetry.
Using brane constructions we argue that the U(N)xU(N) theory at level k
describes the low energy limit of N M2-branes probing a C^4/Z_k singularity. At
large N the t... | [
{
"created": "Fri, 6 Jun 2008 19:43:48 GMT",
"version": "v1"
},
{
"created": "Sun, 8 Jun 2008 18:52:12 GMT",
"version": "v2"
},
{
"created": "Tue, 22 Jul 2008 12:11:00 GMT",
"version": "v3"
},
{
"created": "Thu, 23 Oct 2008 12:37:24 GMT",
"version": "v4"
}
] | 2009-07-09 | [
[
"Aharony",
"Ofer",
""
],
[
"Bergman",
"Oren",
""
],
[
"Jafferis",
"Daniel Louis",
""
],
[
"Maldacena",
"Juan",
""
]
] | We construct three dimensional Chern-Simons-matter theories with gauge groups U(N)xU(N) and SU(N)xSU(N) which have explicit N=6 superconformal symmetry. Using brane constructions we argue that the U(N)xU(N) theory at level k describes the low energy limit of N M2-branes probing a C^4/Z_k singularity. At large N the the... | 4.316737 | 4.196887 | 5.465845 | 4.101572 | 4.28941 | 4.391569 | 4.110095 | 4.100604 | 4.184317 | 5.56437 | 3.976801 | 3.920472 | 4.483 | 3.906112 | 4.07146 | 4.112485 | 4.002325 | 4.097075 | 3.980675 | 4.693027 | 4.01121 |
0810.5489 | Elcio Abdalla | Elcio Abdalla, Owen Pavel Fernandez Piedra, Jeferson de Oliveira and
C. Molina | Perturbations of Black p-Branes | 20 pages, major revisions | Phys.Rev.D81:064001,2010 | 10.1103/PhysRevD.81.064001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider black $p$-brane solutions of the low energy string action,
computing scalar perturbations. Using standard methods, we derive the wave
equations obeyed by the perturbations and treat them analytically and
numerically. We have found that tensorial perturbations obtained via a
gauge-invariant formalism leads... | [
{
"created": "Thu, 30 Oct 2008 13:48:06 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Jul 2009 23:16:02 GMT",
"version": "v2"
},
{
"created": "Fri, 5 Mar 2010 16:56:03 GMT",
"version": "v3"
}
] | 2010-04-06 | [
[
"Abdalla",
"Elcio",
""
],
[
"Piedra",
"Owen Pavel Fernandez",
""
],
[
"de Oliveira",
"Jeferson",
""
],
[
"Molina",
"C.",
""
]
] | We consider black $p$-brane solutions of the low energy string action, computing scalar perturbations. Using standard methods, we derive the wave equations obeyed by the perturbations and treat them analytically and numerically. We have found that tensorial perturbations obtained via a gauge-invariant formalism leads t... | 7.87087 | 7.607856 | 7.285599 | 7.050421 | 7.345303 | 7.106577 | 7.375724 | 6.962398 | 7.411317 | 7.60996 | 6.95223 | 7.358412 | 7.39885 | 7.009942 | 7.299861 | 7.210474 | 7.103513 | 6.963676 | 7.183127 | 7.286711 | 7.24308 |
hep-th/9906099 | Sanjay | Sanjay | On direct and crossed channel asymptotics of four-point functions in
AdS/CFT correspondence | Revised version, typos corrected, 9 pages, no figures | Mod.Phys.Lett.A14:1413-1420,1999 | 10.1142/S0217732399001516 | OUTP-99-28P | hep-th | null | We analyse the leading logarithmic singularities in direct and crossed
channel limit of the four-point functions in dilaton-axion sector of type IIB
supergravity on $AdS_{5}$ in AdS/CFT correspondence. Logarithms do not cancel
in the full correlator in both channels.
| [
{
"created": "Mon, 14 Jun 1999 16:19:17 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Jun 1999 13:55:12 GMT",
"version": "v2"
},
{
"created": "Thu, 16 Sep 1999 09:33:09 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Sanjay",
"",
""
]
] | We analyse the leading logarithmic singularities in direct and crossed channel limit of the four-point functions in dilaton-axion sector of type IIB supergravity on $AdS_{5}$ in AdS/CFT correspondence. Logarithms do not cancel in the full correlator in both channels. | 13.767006 | 11.944616 | 12.891607 | 10.326144 | 10.865037 | 9.858005 | 11.457771 | 10.372794 | 9.779275 | 12.707632 | 9.762975 | 10.445432 | 11.302704 | 10.088312 | 11.114558 | 10.254926 | 10.528134 | 10.019358 | 10.749496 | 11.057805 | 10.331209 |
hep-th/0304099 | Talalaev | D. Talalaev (ITEP, Moscow) | Riemann bilinear form and Poisson structure in Hitchin-type systems | 15 pages | null | null | ITEP-TH-22/03 | hep-th math.AG | null | In this paper we reinterpret the Poisson structure of the Hitchin-type system
in cohomological terms. The principal ingredient of a new interpretation in the
case of the Beauville system is the meromorphic cohomology of the spectral
curve, and the main result is the identification of the Riemann bilinear form
and the... | [
{
"created": "Thu, 10 Apr 2003 14:39:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Talalaev",
"D.",
"",
"ITEP, Moscow"
]
] | In this paper we reinterpret the Poisson structure of the Hitchin-type system in cohomological terms. The principal ingredient of a new interpretation in the case of the Beauville system is the meromorphic cohomology of the spectral curve, and the main result is the identification of the Riemann bilinear form and the s... | 16.257772 | 14.569934 | 18.033386 | 15.206185 | 15.920551 | 18.18125 | 16.095737 | 15.152699 | 14.047955 | 19.629066 | 15.258787 | 15.616354 | 17.33408 | 15.415427 | 14.777285 | 15.133081 | 16.078432 | 16.053875 | 15.534405 | 16.325109 | 14.537605 |
hep-th/9502136 | Nikolaos Batakis | Nikolaos A. Batakis | On the Classification of Spatially Homogeneous String Backgrounds | 12 pages, LaTeX, one Table included, no figures. | null | null | CERN--TH/95--41 | hep-th | null | A classification of all possible spatially homogeneous 4D string backgrounds
(HSBs) has been obtained by appropriate ramification of the existing nine
Bianchi types of homogeneous 3D spaces. A total of $24^2=576$ HSBs which have
been classified as distinct contains a subclass of 192 which includes all
possible FRW mo... | [
{
"created": "Thu, 23 Feb 1995 18:10:07 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Batakis",
"Nikolaos A.",
""
]
] | A classification of all possible spatially homogeneous 4D string backgrounds (HSBs) has been obtained by appropriate ramification of the existing nine Bianchi types of homogeneous 3D spaces. A total of $24^2=576$ HSBs which have been classified as distinct contains a subclass of 192 which includes all possible FRW mode... | 19.693754 | 21.907852 | 19.554247 | 17.652334 | 21.197224 | 19.545914 | 23.555721 | 19.035648 | 18.269163 | 21.093914 | 19.325487 | 18.491219 | 18.668127 | 17.835264 | 18.43342 | 18.211227 | 19.312546 | 19.05957 | 18.349375 | 18.658068 | 18.064709 |
hep-th/0304172 | Nobuyoshi Ohta | Nobuyoshi Ohta | A Study of Accelerating Cosmologies from Superstring/M theories | 20 pages, 17 figures, a typo corrected, to be published in Prog.
Theor. Phys | Prog.Theor.Phys.110:269-283,2003 | 10.1143/PTP.110.269 | OU-HET 438 | hep-th astro-ph gr-qc | null | We study aspects of the accelerating cosmologies obtained from the
compactification of vacuum solution and S2-branes of superstring/M theories.
Parameter dependence of the resulting expansion of our universe and internal
space is examined for all cases. We find that accelerating expansions are
obtained also from sphe... | [
{
"created": "Mon, 21 Apr 2003 06:37:08 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Apr 2003 01:41:57 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Jul 2003 02:43:36 GMT",
"version": "v3"
}
] | 2011-05-05 | [
[
"Ohta",
"Nobuyoshi",
""
]
] | We study aspects of the accelerating cosmologies obtained from the compactification of vacuum solution and S2-branes of superstring/M theories. Parameter dependence of the resulting expansion of our universe and internal space is examined for all cases. We find that accelerating expansions are obtained also from spheri... | 24.011726 | 22.680737 | 25.822702 | 22.835365 | 22.035246 | 22.95676 | 20.99098 | 22.042114 | 21.80308 | 25.744226 | 21.059311 | 22.681273 | 24.639803 | 23.218328 | 22.053841 | 23.418282 | 22.221476 | 23.813408 | 22.445318 | 23.08353 | 22.144144 |
0912.0789 | Mauricio Valenzuela | Mauricio Valenzuela | Higher-spin symmetries of the free Schrodinger equation | Accepted version in Advances in Mathematical Physics | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that the Schrodinger symmetry algebra of a free particle in d
spatial dimensions can be embedded into a representation of the higher-spin
algebra. The latter spans an infinite dimensional algebra of higher-order
symmetry generators of the free Schrodinger equation. An explicit
representation of the maxima... | [
{
"created": "Fri, 4 Dec 2009 07:58:45 GMT",
"version": "v1"
},
{
"created": "Sun, 6 Dec 2009 18:56:24 GMT",
"version": "v2"
},
{
"created": "Sat, 16 Apr 2011 21:31:29 GMT",
"version": "v3"
},
{
"created": "Thu, 23 Feb 2012 17:58:04 GMT",
"version": "v4"
},
{
"cre... | 2016-07-27 | [
[
"Valenzuela",
"Mauricio",
""
]
] | It is shown that the Schrodinger symmetry algebra of a free particle in d spatial dimensions can be embedded into a representation of the higher-spin algebra. The latter spans an infinite dimensional algebra of higher-order symmetry generators of the free Schrodinger equation. An explicit representation of the maximal ... | 9.500041 | 9.176387 | 10.448189 | 9.65475 | 8.885312 | 9.207564 | 8.945785 | 8.767805 | 9.132532 | 10.427337 | 9.009535 | 8.90813 | 9.616333 | 9.012568 | 8.822822 | 8.865119 | 8.918919 | 9.15912 | 8.999419 | 9.302919 | 8.635567 |
1810.11446 | Daniel Thompson | Saskia Demulder, Falk Hassler and Daniel C. Thompson | Doubled aspects of generalised dualities and integrable deformations | 55 pages | null | 10.1007/JHEP02(2019)189 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The worldsheet theories that describe Poisson-Lie T-dualisable
$\sigma$-models on group manifolds as well as integrable $\eta$, $\lambda$ and
$\beta$-deformations provide examples of ${\cal E}$-models. Here we show how
such ${\cal E}$-models can be given an elegant target space description within
Double Field Theory ... | [
{
"created": "Fri, 26 Oct 2018 17:52:17 GMT",
"version": "v1"
}
] | 2019-03-27 | [
[
"Demulder",
"Saskia",
""
],
[
"Hassler",
"Falk",
""
],
[
"Thompson",
"Daniel C.",
""
]
] | The worldsheet theories that describe Poisson-Lie T-dualisable $\sigma$-models on group manifolds as well as integrable $\eta$, $\lambda$ and $\beta$-deformations provide examples of ${\cal E}$-models. Here we show how such ${\cal E}$-models can be given an elegant target space description within Double Field Theory by... | 10.931787 | 9.771048 | 12.27195 | 9.734567 | 9.46706 | 9.349421 | 9.573408 | 8.905254 | 9.266908 | 12.256143 | 9.273983 | 10.14922 | 10.457729 | 9.861379 | 10.040315 | 9.807572 | 9.845282 | 10.071396 | 10.067153 | 10.676924 | 9.672385 |
1907.04836 | Sylvain Lacroix | Sylvain Lacroix | Constrained affine Gaudin models and diagonal Yang-Baxter deformations | 95 pages | J. Phys. A: Math. Theor. 53 (2020) 255203 | 10.1088/1751-8121/ab876e | ZMP-HH/19-12 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review and pursue further the study of constrained realisations of affine
Gaudin models, which form a large class of two-dimensional integrable field
theories with gauge symmetries. In particular, we develop a systematic gauging
procedure which allows to reformulate the non-constrained realisations of
affine Gaudi... | [
{
"created": "Wed, 10 Jul 2019 17:33:46 GMT",
"version": "v1"
}
] | 2020-06-08 | [
[
"Lacroix",
"Sylvain",
""
]
] | We review and pursue further the study of constrained realisations of affine Gaudin models, which form a large class of two-dimensional integrable field theories with gauge symmetries. In particular, we develop a systematic gauging procedure which allows to reformulate the non-constrained realisations of affine Gaudin ... | 7.272829 | 7.491406 | 7.44994 | 6.599918 | 7.365443 | 6.591679 | 6.92971 | 6.890285 | 6.780354 | 7.80113 | 6.585819 | 6.756211 | 7.061393 | 6.919238 | 6.921344 | 6.742099 | 6.703868 | 6.830701 | 6.670013 | 7.201149 | 6.855945 |
2312.12569 | Gleb Sumbatian | G. Sumbatian, E. Ievlev and A. Yung | Large-$N$ Solution and Effective Action of "Twisted-Mass'' Deformed
$\mathbb{CP}(N-1)$ Model | 21 pages, 3 figures | null | null | FTPI-MINN-23-25 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study effective dynamics of the non-supersymmetric two-dimensional
$\mathbb{CP}(N-1)$ model in the large $N$ limit. This model is deformed by a
mass term $m$ preserving $\mathbb{Z}_N$ symmetry of the Lagrangian. At small
$m$ the theory is strongly coupled and resembles the undeformed
$\mathbb{CP}(N-1)$ model, whil... | [
{
"created": "Tue, 19 Dec 2023 20:09:28 GMT",
"version": "v1"
}
] | 2023-12-21 | [
[
"Sumbatian",
"G.",
""
],
[
"Ievlev",
"E.",
""
],
[
"Yung",
"A.",
""
]
] | We study effective dynamics of the non-supersymmetric two-dimensional $\mathbb{CP}(N-1)$ model in the large $N$ limit. This model is deformed by a mass term $m$ preserving $\mathbb{Z}_N$ symmetry of the Lagrangian. At small $m$ the theory is strongly coupled and resembles the undeformed $\mathbb{CP}(N-1)$ model, while ... | 5.086063 | 4.76795 | 5.477444 | 4.79639 | 4.628511 | 4.512139 | 5.194769 | 4.667392 | 4.904677 | 6.474385 | 4.466452 | 4.926292 | 5.137752 | 4.921013 | 4.931194 | 4.875358 | 4.909917 | 4.799302 | 5.062603 | 5.189267 | 4.818281 |
hep-th/0104067 | Inyong Cho | Katherine Benson and Inyong Cho (Emory University) | A universe in a global monopole | 22 pages, 2 eps figures, revtex | Phys.Rev.D64:065026,2001 | 10.1103/PhysRevD.64.065026 | null | hep-th gr-qc hep-ph | null | We investigate brane physics in a universe with an extra dimensional global
monopole and negative bulk cosmological constant. The graviton zero mode is
naturally divergent; we thus invoke a physical cut-off to induce four
dimensional gravity on a brane at the monopole core. Independently, the massive
Kaluza-Klein mod... | [
{
"created": "Fri, 6 Apr 2001 23:10:59 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Benson",
"Katherine",
"",
"Emory University"
],
[
"Cho",
"Inyong",
"",
"Emory University"
]
] | We investigate brane physics in a universe with an extra dimensional global monopole and negative bulk cosmological constant. The graviton zero mode is naturally divergent; we thus invoke a physical cut-off to induce four dimensional gravity on a brane at the monopole core. Independently, the massive Kaluza-Klein modes... | 11.924109 | 11.679749 | 11.448709 | 10.771454 | 11.337298 | 11.179328 | 10.617409 | 10.823073 | 10.55726 | 11.694299 | 10.67968 | 11.059029 | 12.042973 | 10.823607 | 10.895347 | 10.947145 | 11.147521 | 11.331831 | 10.779683 | 11.655722 | 10.930945 |
hep-th/9504096 | Kaare Olaussen | Erling G. B. Hohler and K{\aa}re Olaussen | Using Conservation Laws to Solve Toda Field Theories | Latex, 24 pages | Int.J.Mod.Phys. A11 (1996) 1831-1854 | 10.1142/S0217751X96000961 | Theoretical Physics Seminar in Trondheim, No 7 1995 | hep-th | null | We investigate the question of how the knowledge of sufficiently many local
conservation laws for a model can be utilized to solve the model. We show that
for models where the conservation laws can be written in one-sided forms, like
$\barpartial Q_s = 0$, the problem can always be reduced to solving a closed
system ... | [
{
"created": "Tue, 18 Apr 1995 16:37:03 GMT",
"version": "v1"
}
] | 2016-08-15 | [
[
"Hohler",
"Erling G. B.",
""
],
[
"Olaussen",
"Kåre",
""
]
] | We investigate the question of how the knowledge of sufficiently many local conservation laws for a model can be utilized to solve the model. We show that for models where the conservation laws can be written in one-sided forms, like $\barpartial Q_s = 0$, the problem can always be reduced to solving a closed system of... | 10.582295 | 10.891099 | 10.624823 | 10.686916 | 10.804686 | 9.959098 | 11.46205 | 10.165702 | 10.867073 | 12.002472 | 10.520467 | 10.135821 | 10.348572 | 9.863518 | 10.286031 | 10.079154 | 9.567777 | 10.062603 | 10.024245 | 10.53014 | 9.674138 |
hep-th/9508114 | Forgacs Peter | Peter Forgacs and Jozsef Gyurusi (Research Ins. for Particle and Nucl.
Phys, Budapest) | Static spherically symmetric monopole solutions in the presence of a
dilaton field | 9 pages (incl. 14 figures in eps format) Latex. Figures are to be
decompressed from figs.uu included here as an uuencoded file. Cause of
resubmission:problem with the previously uuencoded file | Phys.Lett.B366:205-211,1996 | 10.1016/0370-2693(95)01321-0 | null | hep-th | null | A numerical study of static spherically symmetric monople solutions of a
spontaneously broken SU(2) gauge theory coupled to a dilaton field is
presented. Regular solutions seem to exist only up to a maximal value of the
dilaton coupling. In addition to the generalization of the 't Hooft-Polyakov
monopole a discrete f... | [
{
"created": "Wed, 23 Aug 1995 19:22:24 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Aug 1995 12:42:29 GMT",
"version": "v2"
}
] | 2010-11-19 | [
[
"Forgacs",
"Peter",
"",
"Research Ins. for Particle and Nucl.\n Phys, Budapest"
],
[
"Gyurusi",
"Jozsef",
"",
"Research Ins. for Particle and Nucl.\n Phys, Budapest"
]
] | A numerical study of static spherically symmetric monople solutions of a spontaneously broken SU(2) gauge theory coupled to a dilaton field is presented. Regular solutions seem to exist only up to a maximal value of the dilaton coupling. In addition to the generalization of the 't Hooft-Polyakov monopole a discrete fam... | 8.052831 | 5.895322 | 6.489263 | 5.7402 | 6.109728 | 5.724713 | 6.077907 | 5.571253 | 5.609597 | 6.589231 | 6.355692 | 6.264693 | 6.489977 | 6.317759 | 6.504125 | 6.141683 | 6.195756 | 6.327667 | 6.504308 | 6.454437 | 6.372256 |
hep-th/0202140 | Ishwaree Neupane | Y. M. Cho and Ishwaree P. Neupane | Anti-de Sitter Black Holes, Thermal Phase Transition and Holography in
Higher Curvature Gravity | 22 pages, Revtex 4, 12+1 figures, references added, section V
extended. To appear in PRD | Phys.Rev.D66:024044,2002 | 10.1103/PhysRevD.66.024044 | SNUTP-2002-04 | hep-th | null | We study anti-de Sitter black holes in the Einstein-Gauss-Bonnet and the
generic R^2 gravity theories, evaluate different thermodynamic quantities, and
also examine the possibilities of Hawking-Page type thermal phase transitions
in these theories. In the Einstein theory, with a possible cosmological term,
one observ... | [
{
"created": "Thu, 21 Feb 2002 07:23:21 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Apr 2002 20:22:47 GMT",
"version": "v2"
},
{
"created": "Mon, 17 Jun 2002 14:57:13 GMT",
"version": "v3"
}
] | 2011-05-05 | [
[
"Cho",
"Y. M.",
""
],
[
"Neupane",
"Ishwaree P.",
""
]
] | We study anti-de Sitter black holes in the Einstein-Gauss-Bonnet and the generic R^2 gravity theories, evaluate different thermodynamic quantities, and also examine the possibilities of Hawking-Page type thermal phase transitions in these theories. In the Einstein theory, with a possible cosmological term, one observes... | 8.673512 | 8.438123 | 8.854722 | 8.44147 | 8.553236 | 8.542618 | 8.997893 | 8.410748 | 8.162276 | 9.117182 | 8.363712 | 8.516132 | 8.522742 | 8.511817 | 8.706262 | 8.595911 | 8.792628 | 8.609634 | 8.489458 | 8.619468 | 8.703119 |
1910.00008 | Yusuke Kimura | Yusuke Kimura | $\frac{1}{2}$ Calabi-Yau 3-folds, Calabi-Yau 3-folds as double covers,
and F-theory with U(1)s | 22 pages. Some changes in section 4, section 5 expanded, and some
clarifications. References added | JHEP 02(2020)076 | 10.1007/JHEP02(2020)076 | KEK-TH-2158 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this study, we introduce a new class of rational elliptic 3-folds, which
we refer to as "1/2 Calabi-Yau 3-folds". We construct elliptically fibered
Calabi-Yau 3-folds by utilizing these rational elliptic 3-folds. The
construction yields a novel approach to build elliptically fibered Calabi-Yau
3-folds of various M... | [
{
"created": "Mon, 30 Sep 2019 08:53:38 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Oct 2019 16:21:37 GMT",
"version": "v2"
},
{
"created": "Mon, 28 Oct 2019 15:38:27 GMT",
"version": "v3"
},
{
"created": "Fri, 31 Jan 2020 10:45:59 GMT",
"version": "v4"
}
] | 2020-02-18 | [
[
"Kimura",
"Yusuke",
""
]
] | In this study, we introduce a new class of rational elliptic 3-folds, which we refer to as "1/2 Calabi-Yau 3-folds". We construct elliptically fibered Calabi-Yau 3-folds by utilizing these rational elliptic 3-folds. The construction yields a novel approach to build elliptically fibered Calabi-Yau 3-folds of various Mor... | 5.743388 | 5.30804 | 6.483778 | 5.287726 | 5.305377 | 5.139768 | 5.470467 | 5.172081 | 5.511822 | 7.160363 | 5.440244 | 5.545899 | 5.949338 | 5.580268 | 5.486583 | 5.583629 | 5.395113 | 5.454887 | 5.576715 | 5.75714 | 5.459025 |
0705.2534 | Ashok Das | Ashok Das and J. Frenkel | Thermal Operator and Dispersion Relation in QED at Finite Temperature
and Chemical Potential | 5 pages, revtex | Phys.Rev.D76:087701,2007 | 10.1103/PhysRevD.76.087701 | null | hep-th | null | Combining the thermal operator representation with the dispersion relation in
QED at finite temperature and chemical potential, we determine the complete
retarded photon self-energy only from its absorptive part at zero temperature.
As an application of this method, we show that, even for the case of a nonzero
chemic... | [
{
"created": "Thu, 17 May 2007 14:19:12 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Das",
"Ashok",
""
],
[
"Frenkel",
"J.",
""
]
] | Combining the thermal operator representation with the dispersion relation in QED at finite temperature and chemical potential, we determine the complete retarded photon self-energy only from its absorptive part at zero temperature. As an application of this method, we show that, even for the case of a nonzero chemical... | 10.486386 | 9.722355 | 8.883641 | 8.781341 | 9.664638 | 9.186961 | 10.129147 | 9.105175 | 9.157327 | 9.983562 | 8.638297 | 8.527096 | 9.265465 | 9.116876 | 8.756341 | 9.067599 | 8.971851 | 9.377634 | 9.181511 | 9.256671 | 9.502441 |
hep-th/9612211 | null | V. B. Kopeliovich, B. E. Stern (INR, Moscow, Russia) | SU(3)-skyrmions | 8 pages, 3 figures (available by request); extended talk at the
Conference Quarks-96, Yaroslavl', Russia, May 1996 | null | null | null | hep-th | null | The consideration of the bound skyrmions with large strangeness content is
continued. The connection between B=2 SO(3)-hedgehog and SU(2)-torus is
investigated and the quantization of the dipole- type configuration with large
strangeness content is described.
| [
{
"created": "Fri, 20 Dec 1996 12:01:24 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Kopeliovich",
"V. B.",
"",
"INR, Moscow, Russia"
],
[
"Stern",
"B. E.",
"",
"INR, Moscow, Russia"
]
] | The consideration of the bound skyrmions with large strangeness content is continued. The connection between B=2 SO(3)-hedgehog and SU(2)-torus is investigated and the quantization of the dipole- type configuration with large strangeness content is described. | 23.977501 | 18.370846 | 19.02182 | 16.12047 | 22.747509 | 19.133022 | 19.406382 | 19.233969 | 17.888096 | 19.070343 | 19.406206 | 19.844261 | 19.83427 | 18.69281 | 19.302908 | 20.787792 | 20.39024 | 19.591093 | 18.724064 | 19.618629 | 19.149439 |
hep-th/0501167 | Ali Imaanpur | Ali Imaanpur | Supersymmetric D3-branes in Five-Form Flux | 13 pages, latex file, minor changes, refs. added | JHEP 0503 (2005) 030 | 10.1088/1126-6708/2005/03/030 | IPM/P-2005/004 | hep-th | null | We consider multiple Euclidean D3-branes in a specific supergravity solution,
which consists of a self-dual 5-form RR field in a flat background. We propose
a deformation of ${\cal N}=4$ SYM action describing the dynamics of D3-branes
in this background. We look at the supersymmetries of ${\cal N}=4$ SYM theory
consi... | [
{
"created": "Thu, 20 Jan 2005 15:36:25 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Jan 2005 14:38:50 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Apr 2005 07:43:37 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Imaanpur",
"Ali",
""
]
] | We consider multiple Euclidean D3-branes in a specific supergravity solution, which consists of a self-dual 5-form RR field in a flat background. We propose a deformation of ${\cal N}=4$ SYM action describing the dynamics of D3-branes in this background. We look at the supersymmetries of ${\cal N}=4$ SYM theory consist... | 8.571333 | 7.805469 | 8.678992 | 7.582268 | 7.448854 | 7.504481 | 7.432257 | 7.594325 | 7.464957 | 9.291289 | 7.402872 | 7.551179 | 8.416027 | 7.706234 | 7.759366 | 7.781838 | 7.675839 | 7.651056 | 7.600525 | 8.24015 | 7.86034 |
1110.5905 | Gonzalo Torroba | Nathaniel Craig, Rouven Essig, Anson Hook, Gonzalo Torroba | Phases of N=1 supersymmetric chiral gauge theories | 35 pages, 5 figures | null | 10.1007/JHEP12(2011)074 | SLAC-PUB-14649; RUNHETC-2011-20; YITP-SB-11-35 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the phases of supersymmetric chiral gauge theories with an
antisymmetric tensor and (anti)fundamental flavors, in the presence of a
classically marginal superpotential deformation. Varying the number of flavors
that appear in the superpotential reveals rich infrared chiral dynamics and
novel dualities. The... | [
{
"created": "Wed, 26 Oct 2011 20:00:00 GMT",
"version": "v1"
}
] | 2015-05-30 | [
[
"Craig",
"Nathaniel",
""
],
[
"Essig",
"Rouven",
""
],
[
"Hook",
"Anson",
""
],
[
"Torroba",
"Gonzalo",
""
]
] | We analyze the phases of supersymmetric chiral gauge theories with an antisymmetric tensor and (anti)fundamental flavors, in the presence of a classically marginal superpotential deformation. Varying the number of flavors that appear in the superpotential reveals rich infrared chiral dynamics and novel dualities. The d... | 11.527328 | 13.173548 | 13.205311 | 10.229874 | 11.344998 | 11.56202 | 10.564012 | 10.71602 | 11.239272 | 12.355636 | 11.134098 | 11.221768 | 11.593307 | 10.789008 | 10.639605 | 11.337546 | 10.746605 | 11.148656 | 10.657871 | 11.509909 | 10.688512 |
hep-th/0107127 | Shibaji Roy | Indranil Mitra and Shibaji Roy | (NS5,D5,D3) bound state, OD3, OD5 limits and SL(2,Z) duality | 21 pages, Revtex, v3: minor corrections and physical meaning of the
parameters $l$ and $\tilde{l}$ is given, version to appear in PRD | Phys.Rev. D65 (2002) 106001 | 10.1103/PhysRevD.65.106001 | null | hep-th | null | We generalize the non-threshold bound state in type IIB supergravity of the
form (NS5, D5, D3) constructed by the present authors (in hep-th/0011236) to
non-zero asymptotic value of the axion $(\chi_0$). We identify the decoupling
limits corresponding to both the open D3-brane theory and open D5-brane theory
for this... | [
{
"created": "Sat, 14 Jul 2001 10:01:49 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Jul 2001 12:08:35 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Mar 2002 08:24:28 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Mitra",
"Indranil",
""
],
[
"Roy",
"Shibaji",
""
]
] | We generalize the non-threshold bound state in type IIB supergravity of the form (NS5, D5, D3) constructed by the present authors (in hep-th/0011236) to non-zero asymptotic value of the axion $(\chi_0$). We identify the decoupling limits corresponding to both the open D3-brane theory and open D5-brane theory for this s... | 5.867785 | 5.817385 | 6.629998 | 5.458956 | 5.671855 | 5.731243 | 5.780113 | 5.520513 | 5.688986 | 6.692029 | 5.677322 | 5.562547 | 6.223877 | 5.738146 | 5.760824 | 5.604702 | 5.746725 | 5.570191 | 5.660446 | 6.131659 | 5.501379 |
2311.04355 | Francisco Navarro-Lerida | Francisco Navarro-Lerida, Eugen Radu, D. H. Tchrakian | The effect of Skyrme--Chern-Simons dynamics on gauged Skyrmions in $2+1$
dimensions | 26 pages, 10 figures | null | null | DIAS-STP-23-25, IPARCOS-UCM-23-126 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the Skyrmion of the $SO(2)$ gauged $O(3)$ sigma model in $2+1$
dimensions in the presence of a Skyrme--Chern-Simons (SCS) term, and compare
its properties with the corresponding properties of the Skyrmion in the
presence of the usual Chern-Simons (CS) term. We find that these properties are
qualitatively lar... | [
{
"created": "Tue, 7 Nov 2023 21:30:23 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jan 2024 09:32:01 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Apr 2024 14:15:49 GMT",
"version": "v3"
},
{
"created": "Thu, 20 Jun 2024 18:58:15 GMT",
"version": "v4"
}
] | 2024-06-24 | [
[
"Navarro-Lerida",
"Francisco",
""
],
[
"Radu",
"Eugen",
""
],
[
"Tchrakian",
"D. H.",
""
]
] | We study the Skyrmion of the $SO(2)$ gauged $O(3)$ sigma model in $2+1$ dimensions in the presence of a Skyrme--Chern-Simons (SCS) term, and compare its properties with the corresponding properties of the Skyrmion in the presence of the usual Chern-Simons (CS) term. We find that these properties are qualitatively large... | 6.969285 | 7.726799 | 7.012238 | 6.640379 | 7.420111 | 6.70214 | 7.483669 | 7.004111 | 6.58644 | 7.66678 | 6.657773 | 6.635164 | 6.653544 | 6.643875 | 6.755066 | 6.704581 | 6.616894 | 6.447772 | 6.576 | 6.943314 | 6.634542 |
2006.06263 | R Loll | N. Klitgaard, R. Loll | How round is the quantum de Sitter universe? | 24 pages, 8 figures | null | 10.1140/epjc/s10052-020-08569-5 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the quantum Ricci curvature, which was introduced in earlier
work, in full, four-dimensional quantum gravity, formulated nonperturbatively
in terms of Causal Dynamical Triangulations (CDT). A key finding of the CDT
approach is the emergence of a universe of de Sitter-type, as evidenced by the
successfu... | [
{
"created": "Thu, 11 Jun 2020 09:11:31 GMT",
"version": "v1"
}
] | 2020-12-02 | [
[
"Klitgaard",
"N.",
""
],
[
"Loll",
"R.",
""
]
] | We investigate the quantum Ricci curvature, which was introduced in earlier work, in full, four-dimensional quantum gravity, formulated nonperturbatively in terms of Causal Dynamical Triangulations (CDT). A key finding of the CDT approach is the emergence of a universe of de Sitter-type, as evidenced by the successful ... | 8.463993 | 8.805224 | 9.086159 | 8.417988 | 8.724791 | 8.23537 | 9.368702 | 8.389507 | 8.362314 | 9.386035 | 8.093717 | 8.304422 | 8.683094 | 8.070456 | 8.225513 | 8.119333 | 8.187664 | 8.105819 | 8.2642 | 8.505127 | 8.152758 |
1203.1015 | Eva Silverstein | Joseph Polchinski and Eva Silverstein | Large-density field theory, viscosity, and "$2k_F$" singularities from
string duals | 28 pages. v2: added references | null | 10.1088/0264-9381/29/19/194008 | NSF-KITP-12-027; SLAC-PUB-14883; SU-ITP-12/08 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze systems where an effective large-N expansion arises naturally in
gauge theories without a large number of colors: a sufficiently large charge
density alone can produce a perturbative string ('tHooft) expansion. One
example is simply the well-known NS5/F1 system dual to $AdS_3\times T^4\times
S^3$, here vie... | [
{
"created": "Mon, 5 Mar 2012 19:26:51 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Mar 2012 19:15:43 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Polchinski",
"Joseph",
""
],
[
"Silverstein",
"Eva",
""
]
] | We analyze systems where an effective large-N expansion arises naturally in gauge theories without a large number of colors: a sufficiently large charge density alone can produce a perturbative string ('tHooft) expansion. One example is simply the well-known NS5/F1 system dual to $AdS_3\times T^4\times S^3$, here viewe... | 13.925134 | 14.02357 | 16.550657 | 13.729056 | 15.314971 | 14.766549 | 14.693439 | 14.600309 | 13.450233 | 17.537413 | 14.321986 | 13.684687 | 14.552104 | 13.635657 | 13.840284 | 13.925977 | 13.622141 | 13.8172 | 13.877024 | 14.968451 | 13.650546 |
2011.02002 | Romain Ruzziconi | Adrien Fiorucci, Romain Ruzziconi | Charge Algebra in Al(A)dS$_n$ Spacetimes | 48 pages, 1 figure, published version | null | 10.1007/JHEP05(2021)210 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The gravitational charge algebra of generic asymptotically locally (A)dS
spacetimes is derived in $n$ dimensions. The analysis is performed in the
Starobinsky/Fefferman-Graham gauge, without assuming any further boundary
condition than the minimal falloffs for conformal compactification. In
particular, the boundary s... | [
{
"created": "Tue, 3 Nov 2020 20:51:10 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jun 2021 14:52:35 GMT",
"version": "v2"
}
] | 2023-01-11 | [
[
"Fiorucci",
"Adrien",
""
],
[
"Ruzziconi",
"Romain",
""
]
] | The gravitational charge algebra of generic asymptotically locally (A)dS spacetimes is derived in $n$ dimensions. The analysis is performed in the Starobinsky/Fefferman-Graham gauge, without assuming any further boundary condition than the minimal falloffs for conformal compactification. In particular, the boundary str... | 7.886389 | 6.941461 | 8.326982 | 7.044219 | 7.049518 | 7.002773 | 7.019557 | 7.244359 | 7.170647 | 8.651886 | 6.951046 | 7.20909 | 7.706552 | 7.264677 | 7.308169 | 7.136693 | 7.539458 | 7.447254 | 7.287491 | 7.830362 | 7.352025 |
1612.06395 | Paul Romatschke | Masanori Hanada and Paul Romatschke | Lattice Simulations of 10d Yang-Mills toroidally compactified to 1d, 2d
and 4d | 30 pages, 13 figures; v2: minor changes; v3: minor changes | Phys. Rev. D 96, 094502 (2017) | 10.1103/PhysRevD.96.094502 | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Toroidally compactified Yang-Mills theory on the lattice is studied by using
the Hybrid Monte Carlo algorithm. When the compact dimensions are small, the
theory naturally reduces to Yang-Mills with scalars. We confirm previous
analytical and numerical results for pure gauge theory with scalars in (0+1)
dimensions and... | [
{
"created": "Mon, 19 Dec 2016 21:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Apr 2017 14:50:31 GMT",
"version": "v2"
},
{
"created": "Fri, 20 Oct 2017 16:12:21 GMT",
"version": "v3"
}
] | 2017-11-08 | [
[
"Hanada",
"Masanori",
""
],
[
"Romatschke",
"Paul",
""
]
] | Toroidally compactified Yang-Mills theory on the lattice is studied by using the Hybrid Monte Carlo algorithm. When the compact dimensions are small, the theory naturally reduces to Yang-Mills with scalars. We confirm previous analytical and numerical results for pure gauge theory with scalars in (0+1) dimensions and a... | 8.332445 | 8.164657 | 8.386579 | 7.79726 | 8.241852 | 8.689185 | 8.251838 | 7.828797 | 7.594334 | 8.512546 | 8.009891 | 7.84205 | 8.035142 | 7.684795 | 7.556503 | 7.991637 | 7.959437 | 7.657655 | 7.800011 | 7.947481 | 8.090384 |
1905.09290 | Paul Romatschke | Paul Romatschke | Analytic Transport from Weak to Strong Coupling in the O(N) model | 6 pages, 2 figures; v2: matches published version; v3: fixed typo in
Eq. (6) | Phys. Rev. D 100, 054029 (2019) | 10.1103/PhysRevD.100.054029 | null | hep-th cond-mat.str-el hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, a second-order transport coefficient (the curvature-matter
coupling $\kappa$) is calculated exactly for the 3+1d O(N) model at large N for
any coupling value. Since the theory is `trivial' in the sense of possessing a
Landau pole, the result for $\kappa$ only is free from cut-off artifacts much
below th... | [
{
"created": "Wed, 22 May 2019 18:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Sep 2019 15:36:35 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Nov 2019 16:29:06 GMT",
"version": "v3"
}
] | 2019-11-26 | [
[
"Romatschke",
"Paul",
""
]
] | In this work, a second-order transport coefficient (the curvature-matter coupling $\kappa$) is calculated exactly for the 3+1d O(N) model at large N for any coupling value. Since the theory is `trivial' in the sense of possessing a Landau pole, the result for $\kappa$ only is free from cut-off artifacts much below the ... | 14.193729 | 15.014771 | 15.950334 | 13.761838 | 13.315011 | 14.04267 | 14.66908 | 13.957249 | 13.780293 | 15.22851 | 13.236745 | 13.254957 | 13.790945 | 13.710791 | 13.119824 | 14.001081 | 13.365072 | 13.504397 | 13.22564 | 14.488197 | 13.460739 |
hep-th/0008109 | Ali Imaanpur | A. Imaanpur | On supermembrane actions on Calabi-Yau 3-folds | 6 pages, latex file | Phys.Lett. B492 (2000) 365-368 | 10.1016/S0370-2693(00)01097-2 | null | hep-th | null | In this note we examine the supermembrane action on Calabi-Yau 3-folds. We
write down the Dirac-Born-Infeld part of the action, and show that it is
invariant under the rigid spacetime supersymmetry.
| [
{
"created": "Sun, 13 Aug 2000 14:24:46 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Imaanpur",
"A.",
""
]
] | In this note we examine the supermembrane action on Calabi-Yau 3-folds. We write down the Dirac-Born-Infeld part of the action, and show that it is invariant under the rigid spacetime supersymmetry. | 6.220388 | 5.032308 | 6.539289 | 4.825669 | 4.962131 | 5.468195 | 4.957775 | 4.595462 | 4.93629 | 6.523865 | 4.830149 | 5.064079 | 5.901169 | 5.176917 | 4.982749 | 5.106164 | 5.06284 | 4.968832 | 5.016021 | 5.632341 | 4.68369 |
hep-th/9703134 | Ingo Gaida | Mirjam Cvetic and Ingo Gaida (University of Pennsylvania) | Duality Invariant Non-Extreme Black Holes in Toroidally Compactified
String Theory | Reference added, 20 pages, no figures | Nucl.Phys.B505:291-306,1997 | 10.1016/S0550-3213(97)00379-9 | UPR-734-T | hep-th | null | We present duality invariant structure of the thermodynamic quantities of
non-extreme black hole solutions of torodially compactified Type II (M-theory)
and heterotic string in five and four dimensions. These quantities are
parameterized by duality invariant combinations of charges and the
non-extremality parameter, ... | [
{
"created": "Wed, 19 Mar 1997 12:12:14 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Apr 1997 16:35:44 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Cvetic",
"Mirjam",
"",
"University of Pennsylvania"
],
[
"Gaida",
"Ingo",
"",
"University of Pennsylvania"
]
] | We present duality invariant structure of the thermodynamic quantities of non-extreme black hole solutions of torodially compactified Type II (M-theory) and heterotic string in five and four dimensions. These quantities are parameterized by duality invariant combinations of charges and the non-extremality parameter, wh... | 7.421578 | 7.574203 | 8.057236 | 6.395772 | 7.688972 | 7.227305 | 7.213665 | 7.159175 | 7.106841 | 9.234548 | 7.178491 | 7.072813 | 7.60292 | 7.027407 | 7.063989 | 7.150486 | 7.029736 | 6.944121 | 6.977665 | 7.542544 | 7.098405 |
hep-th/9811089 | Michele Maggiore | Michele Maggiore (INFN and Dept. of Phys., Pisa) and Antonio Riotto
(CERN) | D-branes and Cosmology | LaTeX file, 30 pages, 2 eps figures, 1 reference added | Nucl.Phys. B548 (1999) 427-445 | 10.1016/S0550-3213(99)00104-2 | CERN-TH/98-361 | hep-th astro-ph gr-qc hep-ph | null | D-branes, topological defects in string theory on which string endpoints can
live, may give new insight into the understanding of the cosmological evolution
of the Universe at early epochs. We analyze the dynamics of D-branes in curved
backgrounds and discuss the parameter space of M-theory as a function of the
coupl... | [
{
"created": "Tue, 10 Nov 1998 11:51:50 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Nov 1998 09:49:06 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Maggiore",
"Michele",
"",
"INFN and Dept. of Phys., Pisa"
],
[
"Riotto",
"Antonio",
"",
"CERN"
]
] | D-branes, topological defects in string theory on which string endpoints can live, may give new insight into the understanding of the cosmological evolution of the Universe at early epochs. We analyze the dynamics of D-branes in curved backgrounds and discuss the parameter space of M-theory as a function of the couplin... | 8.233315 | 8.616639 | 8.274166 | 7.954751 | 8.715421 | 8.823682 | 8.629038 | 8.763433 | 7.808307 | 8.935028 | 7.967382 | 8.040069 | 7.93545 | 7.841096 | 8.076931 | 7.929193 | 8.094697 | 7.789304 | 7.776262 | 8.107669 | 7.718006 |
1006.0145 | Timothy J. Hollowood | Timothy J. Hollowood and Graham M. Shore | The Effect of Gravitational Tidal Forces on Vacuum Polarization: How to
Undress a Photon | 13 pages, 1 figure, minor corrections | Phys.Lett.B691:279-284,2010 | 10.1016/j.physletb.2010.07.006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The effect of gravitational tidal forces on photon propagation in curved
spacetime is investigated. It is found that the imaginary part of the local
refractive index Im n(u;w) may be negative as well as positive, corresponding
to a local amplification as well as attenuation of the amplitude of the
renormalized photon... | [
{
"created": "Tue, 1 Jun 2010 14:51:03 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jun 2010 13:00:30 GMT",
"version": "v2"
}
] | 2014-11-21 | [
[
"Hollowood",
"Timothy J.",
""
],
[
"Shore",
"Graham M.",
""
]
] | The effect of gravitational tidal forces on photon propagation in curved spacetime is investigated. It is found that the imaginary part of the local refractive index Im n(u;w) may be negative as well as positive, corresponding to a local amplification as well as attenuation of the amplitude of the renormalized photon f... | 8.916496 | 8.253314 | 8.837956 | 8.661161 | 8.85336 | 8.278314 | 8.439263 | 8.88272 | 8.070328 | 9.73702 | 8.482758 | 8.327491 | 8.455434 | 8.4528 | 8.486395 | 8.406706 | 8.534311 | 8.583453 | 8.327719 | 8.638869 | 8.34553 |
hep-th/0511071 | Allen Stern | A. Pinzul and A. Stern | Noncommutative $AdS^3$ with Quantized Cosmological Constant | 16 pp | Class.Quant.Grav.23:1009,2006 | 10.1088/0264-9381/23/3/024 | null | hep-th gr-qc | null | We examine a recent deformation of three-dimensional anti-deSitter gravity
based on noncommutative Chern-Simons theory with gauge group $U(1,1)\times
U(1,1)$. In addition to a noncommutative analogue of 3D gravity, the theory
contains two addition gauge fields which decouple in the commutative limit. It
is well known... | [
{
"created": "Mon, 7 Nov 2005 01:32:25 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Pinzul",
"A.",
""
],
[
"Stern",
"A.",
""
]
] | We examine a recent deformation of three-dimensional anti-deSitter gravity based on noncommutative Chern-Simons theory with gauge group $U(1,1)\times U(1,1)$. In addition to a noncommutative analogue of 3D gravity, the theory contains two addition gauge fields which decouple in the commutative limit. It is well known t... | 7.463265 | 7.394019 | 8.047672 | 7.389822 | 7.15365 | 7.576282 | 7.361719 | 7.109201 | 7.351358 | 8.158809 | 7.123113 | 7.483659 | 7.561848 | 7.303939 | 7.349852 | 7.395559 | 7.401298 | 7.098368 | 7.215855 | 7.596876 | 6.941706 |
1606.00423 | Luc\'ia C\'ordova | Luc\'ia C\'ordova | Hexagon POPE: effective particles and tree level resummation | 29 pages, 8 figures | null | 10.1007/JHEP01(2017)051 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the resummation of the full Pentagon Operator Product Expansion
series of the hexagon Wilson loop in planar $\mathcal N=4$ SYM at tree level.
We do so by considering the one effective particle states formed by a
fundamental flux tube excitation and an arbitrary number of the so called
"small fermions" whic... | [
{
"created": "Wed, 1 Jun 2016 19:52:50 GMT",
"version": "v1"
}
] | 2017-02-01 | [
[
"Córdova",
"Lucía",
""
]
] | We present the resummation of the full Pentagon Operator Product Expansion series of the hexagon Wilson loop in planar $\mathcal N=4$ SYM at tree level. We do so by considering the one effective particle states formed by a fundamental flux tube excitation and an arbitrary number of the so called "small fermions" which ... | 13.15746 | 11.472504 | 15.234338 | 11.727497 | 11.828165 | 13.066122 | 12.979232 | 11.7776 | 12.623359 | 15.191032 | 11.090922 | 11.517962 | 13.352402 | 11.817772 | 11.955078 | 11.976809 | 12.254336 | 11.705867 | 12.174625 | 13.532252 | 11.498317 |
1608.07219 | Yusuke Kimura | Yusuke Kimura | Discrete Gauge Groups in F-theory Models on Genus-One Fibered Calabi-Yau
4-folds without Section | 29 pages. Some clarifications, updated acknowledgments, added
references | JHEP 04(2017)168 | 10.1007/JHEP04(2017)168 | YITP-16-98 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We determine the discrete gauge symmetries that arise in F-theory
compactifications on examples of genus-one fibered Calabi-Yau 4-folds without a
section. We construct genus-one fibered Calabi-Yau 4-folds using Fano
manifolds, cyclic 3-fold covers of Fano 4-folds, and Segre embeddings of
products of projective spaces... | [
{
"created": "Thu, 25 Aug 2016 16:54:53 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Sep 2016 19:24:13 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Sep 2016 16:55:42 GMT",
"version": "v3"
},
{
"created": "Mon, 28 Nov 2016 19:49:07 GMT",
"version": "v4"
},
{
"cre... | 2017-05-02 | [
[
"Kimura",
"Yusuke",
""
]
] | We determine the discrete gauge symmetries that arise in F-theory compactifications on examples of genus-one fibered Calabi-Yau 4-folds without a section. We construct genus-one fibered Calabi-Yau 4-folds using Fano manifolds, cyclic 3-fold covers of Fano 4-folds, and Segre embeddings of products of projective spaces. ... | 4.930036 | 4.850965 | 5.750465 | 4.906242 | 5.306063 | 5.135289 | 4.903982 | 4.937228 | 4.92003 | 6.101854 | 4.82076 | 4.851698 | 4.972036 | 4.882609 | 4.933657 | 4.77457 | 4.759438 | 4.804805 | 4.864907 | 4.847742 | 4.796383 |
0710.5557 | Marc de Montigny | M. Kobayashi, M. de Montigny, F.C. Khanna | CPT theorem in a (5+1) Galilean space-time | 11 pages, 0 figure | Phys.Lett.A372:3541-3547,2008 | 10.1016/j.physleta.2008.02.024 | null | hep-th | null | We extend the 5-dimensional Galilean space-time to a (5+1) Galilean
space-time in order to define a parity transformation in a covariant manner.
This allows us to discuss the discrete symmetries in the Galilean space-time,
which is embedded in the (5+1) Minkowski space-time. We discuss the Dirac-type
field, for which... | [
{
"created": "Tue, 30 Oct 2007 00:37:04 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kobayashi",
"M.",
""
],
[
"de Montigny",
"M.",
""
],
[
"Khanna",
"F. C.",
""
]
] | We extend the 5-dimensional Galilean space-time to a (5+1) Galilean space-time in order to define a parity transformation in a covariant manner. This allows us to discuss the discrete symmetries in the Galilean space-time, which is embedded in the (5+1) Minkowski space-time. We discuss the Dirac-type field, for which w... | 6.66493 | 5.587573 | 6.091866 | 5.457686 | 5.773559 | 5.942023 | 6.020835 | 5.465432 | 5.822372 | 6.212587 | 5.633121 | 5.886964 | 5.908229 | 5.82116 | 5.912713 | 5.873777 | 5.911918 | 5.934054 | 5.685138 | 6.121724 | 5.791615 |
hep-th/0107002 | Lubos Motl | Lubos Motl | Melvin Matrix Models | 9 pages, JHEP LaTeX | null | null | HEP-UK-0011 | hep-th | null | In this short note we construct the DLCQ description of the flux seven-branes
in type IIA string theory and discuss its basic properties. The matrix model
involves dipole fields. We explain the relation of this nonlocal matrix model
to various orbifolds. We also give a spacetime interpretation of the
Seiberg-Witten-l... | [
{
"created": "Sat, 30 Jun 2001 01:32:11 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Motl",
"Lubos",
""
]
] | In this short note we construct the DLCQ description of the flux seven-branes in type IIA string theory and discuss its basic properties. The matrix model involves dipole fields. We explain the relation of this nonlocal matrix model to various orbifolds. We also give a spacetime interpretation of the Seiberg-Witten-lik... | 16.429514 | 13.057852 | 17.831251 | 13.66521 | 12.538029 | 13.356729 | 13.007037 | 13.653013 | 12.247847 | 17.911175 | 14.003716 | 13.566786 | 15.244756 | 13.970216 | 13.447786 | 13.756747 | 13.539613 | 13.811389 | 13.907055 | 15.685337 | 13.79138 |
1304.5901 | Anastasia Doikou | Anastasia Doikou | Transmission matrices in gl(N) & U_q(gl(N)) quantum spin chains | 21 pages, Latex. Typos corrected | JHEP 08 (2013) 103 | 10.1007/JHEP08(2013)103 | null | hep-th cond-mat.stat-mech math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The gl(N) and U_q(gl(N)) quantum spin chains in the presence of integrable
spin impurities are considered. Within the Bethe ansatz formulation, we derive
the associated transmission amplitudes, and the corresponding transmission
matrices -representations of the underlying quadratic algebra- that physically
describe t... | [
{
"created": "Mon, 22 Apr 2013 10:03:23 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Aug 2013 16:44:34 GMT",
"version": "v2"
}
] | 2013-08-28 | [
[
"Doikou",
"Anastasia",
""
]
] | The gl(N) and U_q(gl(N)) quantum spin chains in the presence of integrable spin impurities are considered. Within the Bethe ansatz formulation, we derive the associated transmission amplitudes, and the corresponding transmission matrices -representations of the underlying quadratic algebra- that physically describe the... | 18.752821 | 12.750322 | 17.939493 | 14.13903 | 16.013056 | 15.040758 | 18.731239 | 14.664804 | 14.302011 | 16.944487 | 14.560235 | 13.74272 | 14.965794 | 13.022744 | 13.831286 | 14.124755 | 13.70199 | 13.91394 | 13.812884 | 15.952913 | 14.748352 |
1411.3148 | Elena-Mirela Babalic Dr | Elena Mirela Babalic, Calin Iuliu Lazaroiu | Foliated eight-manifolds for M-theory compactification | 63 pages, 2 figures | JHEP01(2015)140 | 10.1007/JHEP01(2015)140 | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We characterize compact eight-manifolds M which arise as internal spaces in
N=1 flux compactifications of M-theory down to AdS3 using the theory of
foliations, for the case when the internal part of the supersymmetry generator
is everywhere non-chiral. We prove that specifying such a supersymmetric
background is equi... | [
{
"created": "Wed, 12 Nov 2014 11:36:15 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Feb 2015 17:35:08 GMT",
"version": "v2"
}
] | 2015-02-11 | [
[
"Babalic",
"Elena Mirela",
""
],
[
"Lazaroiu",
"Calin Iuliu",
""
]
] | We characterize compact eight-manifolds M which arise as internal spaces in N=1 flux compactifications of M-theory down to AdS3 using the theory of foliations, for the case when the internal part of the supersymmetry generator is everywhere non-chiral. We prove that specifying such a supersymmetric background is equiva... | 9.790501 | 10.787186 | 13.292786 | 9.998808 | 11.385276 | 11.355812 | 10.465663 | 11.0532 | 9.76884 | 13.959685 | 10.374073 | 9.362804 | 10.406463 | 9.595782 | 9.440259 | 9.419225 | 9.358091 | 9.274795 | 9.666279 | 10.679655 | 9.478479 |
2011.04411 | T. Padmanabhan | T. Padmanabhan | A class of QFTs with higher derivative field equations leading to
standard dispersion relation for the particle excitations | null | Physics Letters B 811 (2020) 135912 | 10.1016/j.physletb.2020.135912 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given any (Feynman) propagator which is Lorentz and translation invariant, it
is possible to construct an action functional for a scalar field such that the
quantum field theory, obtained by path integral quantization, leads to this
propagator. In general, such a theory will involve derivatives of the field
higher th... | [
{
"created": "Mon, 9 Nov 2020 13:26:49 GMT",
"version": "v1"
}
] | 2020-11-10 | [
[
"Padmanabhan",
"T.",
""
]
] | Given any (Feynman) propagator which is Lorentz and translation invariant, it is possible to construct an action functional for a scalar field such that the quantum field theory, obtained by path integral quantization, leads to this propagator. In general, such a theory will involve derivatives of the field higher than... | 7.644047 | 8.420443 | 7.371656 | 7.546099 | 8.507869 | 7.701281 | 9.00398 | 7.334067 | 7.369735 | 7.51733 | 7.39696 | 7.414682 | 7.367832 | 7.279485 | 7.312473 | 7.203515 | 7.436423 | 7.174002 | 7.391974 | 7.50532 | 7.585299 |
hep-th/0410072 | Shankaranarayanan S. | S. Shankaranarayanan (ICTP, Trieste) and L. Sriramkumar (HRI,
Allahabad) | Planck scale effects and the suppression of power on the large scales in
the primordial spectrum | 5 Pages, 2 Figures; Talk presented at PASCOS-04; To be published in
proceedings (World Scientific, 2004) | null | 10.1142/9789812701756_0005 | null | hep-th astro-ph gr-qc | null | The enormous red-shifting of the modes during the inflationary epoch suggests
that physics at the very high energy scales may modify the primordial
perturbation spectrum. Therefore, the measurements of the anisotropies in the
Cosmic Microwave Background (CMB) could provide us with clues to understanding
physics beyon... | [
{
"created": "Thu, 7 Oct 2004 12:54:23 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Shankaranarayanan",
"S.",
"",
"ICTP, Trieste"
],
[
"Sriramkumar",
"L.",
"",
"HRI,\n Allahabad"
]
] | The enormous red-shifting of the modes during the inflationary epoch suggests that physics at the very high energy scales may modify the primordial perturbation spectrum. Therefore, the measurements of the anisotropies in the Cosmic Microwave Background (CMB) could provide us with clues to understanding physics beyond ... | 8.112319 | 7.653448 | 7.18939 | 7.032424 | 7.473896 | 7.871652 | 8.260018 | 7.103455 | 7.076386 | 7.978887 | 7.479207 | 7.356493 | 7.25485 | 7.289411 | 7.397559 | 7.454988 | 7.312945 | 7.267509 | 7.262554 | 7.439377 | 7.35324 |
hep-th/9311039 | Michael Martin Nieto | Michael Martin Nieto | Generalized Squeezed States from Generalized Coherent States | 12 pages, LA-UR-93-3731, to be published in the Proceedings of the
International Symposium on Coherent States: Past, Present, and Future, LaTex | null | null | null | hep-th | null | Both the coherent states and also the squeezed states of the harmonic
oscillator have long been understood from the three classical points of view:
the 1) displacement operator, 2) annihilation- (or ladder-) operator, and
minimum-uncertainty methods. For general systems, there is the same
understanding except for lad... | [
{
"created": "Sat, 6 Nov 1993 19:32:17 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Nieto",
"Michael Martin",
""
]
] | Both the coherent states and also the squeezed states of the harmonic oscillator have long been understood from the three classical points of view: the 1) displacement operator, 2) annihilation- (or ladder-) operator, and minimum-uncertainty methods. For general systems, there is the same understanding except for ladde... | 16.722321 | 16.693977 | 19.164255 | 17.190084 | 17.156023 | 17.110937 | 17.373213 | 16.932169 | 16.976448 | 19.480202 | 15.950504 | 16.179096 | 16.354935 | 15.843483 | 15.746044 | 16.367393 | 15.741228 | 15.432673 | 16.344521 | 16.071613 | 15.345271 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.