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 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0402033 | Charlotte Kristjansen | C. Kristjansen (NORDITA) | Three-spin Strings on AdS_5 x S^5 from N=4 SYM | 13 pages, v2: refs. added, minor textual changes, v3: more refs.
added | Phys.Lett. B586 (2004) 106-116 | 10.1016/j.physletb.2004.02.037 | NORDITA-2004-3 | hep-th | null | Using the integrable spin chain picture we study the one-loop anomalous
dimension of certain single trace scalar operators of N=4 SYM expected to
correspond to semi-classical string states on AdS_5 x S^5 with three large
angular momenta (J_1,J_2,J_3) on S^5. In particular, we investigate the
analyticity structure enc... | [
{
"created": "Wed, 4 Feb 2004 17:49:21 GMT",
"version": "v1"
},
{
"created": "Thu, 12 Feb 2004 11:20:53 GMT",
"version": "v2"
},
{
"created": "Wed, 18 Feb 2004 14:19:11 GMT",
"version": "v3"
}
] | 2016-09-06 | [
[
"Kristjansen",
"C.",
"",
"NORDITA"
]
] | Using the integrable spin chain picture we study the one-loop anomalous dimension of certain single trace scalar operators of N=4 SYM expected to correspond to semi-classical string states on AdS_5 x S^5 with three large angular momenta (J_1,J_2,J_3) on S^5. In particular, we investigate the analyticity structure encod... | 7.172508 | 6.816088 | 8.688054 | 6.386069 | 6.681708 | 6.414682 | 6.0516 | 6.553914 | 6.25367 | 9.02089 | 6.608196 | 6.56044 | 7.383636 | 6.56694 | 6.86602 | 6.48067 | 6.528228 | 6.711441 | 6.76125 | 7.616216 | 6.479452 |
hep-th/9910240 | Roy B. Tumlos | Jose A. Magpantay (National Institute of Physics, U.P. Diliman Q.C.,
Philippines) | The Parisi-Sourlas Mechanism in Yang-Mills Theory? | 13 pages, LATEX | Int.J.Mod.Phys. A15 (2000) 1613-1628 | 10.1142/S0217751X00000720 | null | hep-th | null | The Parisi-Sourlas mechanism is exhibited in pure Yang-Mills theory. Using
the new scalar degrees of freedom derived from the non-linear gauge condition,
we show that the non-perturbative sector of Yang-Mills theory is equivalent to
a 4D O(1,3) sigma model in a random field. We then show that the leading term
of this... | [
{
"created": "Fri, 29 Oct 1999 03:48:16 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Magpantay",
"Jose A.",
"",
"National Institute of Physics, U.P. Diliman Q.C.,\n Philippines"
]
] | The Parisi-Sourlas mechanism is exhibited in pure Yang-Mills theory. Using the new scalar degrees of freedom derived from the non-linear gauge condition, we show that the non-perturbative sector of Yang-Mills theory is equivalent to a 4D O(1,3) sigma model in a random field. We then show that the leading term of this e... | 8.110186 | 8.58276 | 8.328694 | 7.616448 | 8.195273 | 7.56212 | 7.912358 | 7.970926 | 7.208572 | 8.273989 | 7.643463 | 7.815901 | 7.691445 | 7.596147 | 7.45115 | 7.956853 | 7.642384 | 7.666654 | 7.415262 | 8.002634 | 7.591526 |
1402.1855 | Carlos A. S. Almeida | L. J. S. Sousa, C. A. S. Silva, D. M. Dantas, and C. A. S. Almeida | Vector and fermion fields on a bouncing brane with a decreasing warp
factor in a string-like defect | 15 pages, 5 figures. To appear in Physics Letters B. arXiv admin
note: text overlap with arXiv:1209.6016 | null | 10.1016/j.physletb.2014.02.010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a recent work, a model has been proposed where a brane is made of a scalar
field with bounce-type configurations and embedded in a bulk with a string-like
metric. This model produces an AdS scenario where the components of the energy
momentum tensor are finite and have its positivity ensured by a suitable choice
o... | [
{
"created": "Sat, 8 Feb 2014 14:34:06 GMT",
"version": "v1"
}
] | 2014-03-03 | [
[
"Sousa",
"L. J. S.",
""
],
[
"Silva",
"C. A. S.",
""
],
[
"Dantas",
"D. M.",
""
],
[
"Almeida",
"C. A. S.",
""
]
] | In a recent work, a model has been proposed where a brane is made of a scalar field with bounce-type configurations and embedded in a bulk with a string-like metric. This model produces an AdS scenario where the components of the energy momentum tensor are finite and have its positivity ensured by a suitable choice of ... | 10.98968 | 10.82329 | 10.626951 | 9.901002 | 10.167145 | 10.117189 | 10.621014 | 10.254663 | 10.028081 | 11.12746 | 10.200216 | 10.009794 | 10.778247 | 10.511252 | 10.012151 | 10.346776 | 9.912573 | 9.875811 | 10.376116 | 10.684234 | 10.234767 |
0810.0704 | Diego Bombardelli | Diego Bombardelli and Davide Fioravanti | Finite-Size Corrections of the $\mathbb{CP}^3$ Giant Magnons: the
L\"{u}scher terms | 20 pages, references added, improved and extended version | JHEP 0907:034,2009 | 10.1088/1126-6708/2009/07/034 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute classical and first quantum finite-size corrections to the
recently found giant magnon solutions in two different subspaces of
$\mathbb{CP}^3$. We use the L\"{u}scher approach on the recently proposed exact
S-matrix for $\mathcal{N}=6$ superconformal Chern-Simons theory. We compare our
results with the str... | [
{
"created": "Fri, 3 Oct 2008 19:47:01 GMT",
"version": "v1"
},
{
"created": "Fri, 30 Jan 2009 17:57:43 GMT",
"version": "v2"
}
] | 2009-07-22 | [
[
"Bombardelli",
"Diego",
""
],
[
"Fioravanti",
"Davide",
""
]
] | We compute classical and first quantum finite-size corrections to the recently found giant magnon solutions in two different subspaces of $\mathbb{CP}^3$. We use the L\"{u}scher approach on the recently proposed exact S-matrix for $\mathcal{N}=6$ superconformal Chern-Simons theory. We compare our results with the strin... | 7.135994 | 5.838906 | 9.083461 | 5.672456 | 6.078818 | 5.622856 | 6.096505 | 6.036888 | 5.985182 | 8.941163 | 5.673595 | 5.703111 | 7.153153 | 5.997402 | 6.064189 | 6.284801 | 6.36642 | 6.211709 | 6.49973 | 7.01529 | 6.288806 |
2207.06885 | Ilarion Melnikov | Peng Cheng, Ilarion V. Melnikov, and Ruben Minasian | Flat equivariant gerbes: holonomies and dualities | 65 pages, tikz figures; v2: typos corrected | null | 10.1007/JHEP04(2023)074 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We examine the role of global topological data associated to choices of
holonomy for flat gauge fields in string compactification. Our study begins
with perturbative string compactification on compact flat manifolds preserving
8 supercharges in 5 dimensions. By including non-trivial holonomy for Wilson
lines in the h... | [
{
"created": "Thu, 14 Jul 2022 13:04:38 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Mar 2023 09:54:14 GMT",
"version": "v2"
}
] | 2023-05-03 | [
[
"Cheng",
"Peng",
""
],
[
"Melnikov",
"Ilarion V.",
""
],
[
"Minasian",
"Ruben",
""
]
] | We examine the role of global topological data associated to choices of holonomy for flat gauge fields in string compactification. Our study begins with perturbative string compactification on compact flat manifolds preserving 8 supercharges in 5 dimensions. By including non-trivial holonomy for Wilson lines in the het... | 13.657545 | 13.418527 | 16.436516 | 12.760344 | 12.433793 | 11.679885 | 13.22799 | 12.695255 | 12.202901 | 16.978432 | 12.273229 | 12.346523 | 14.493383 | 12.659731 | 12.212893 | 12.603477 | 12.31522 | 12.803547 | 12.79967 | 13.961272 | 12.242057 |
hep-th/0303245 | Andreas Fring | Olalla A. Castro-Alvaredo and Andreas Fring | Breathers in the elliptic sine-Gordon model | 20 pages, Latex, one eps-figure | J.Phys.A36:10233-10249,2003 | 10.1088/0305-4470/36/40/008 | SFB288-preprint | hep-th math-ph math.MP | null | We provide new expressions for the scattering amplitudes in the
soliton-antisoliton sector of the elliptic sine-Gordon model in terms of cosets
of the affine Weyl group corresponding to infinite products of q-deformed gamma
functions. When relaxing the usual restriction on the coupling constants, the
model contains a... | [
{
"created": "Thu, 27 Mar 2003 16:25:54 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Castro-Alvaredo",
"Olalla A.",
""
],
[
"Fring",
"Andreas",
""
]
] | We provide new expressions for the scattering amplitudes in the soliton-antisoliton sector of the elliptic sine-Gordon model in terms of cosets of the affine Weyl group corresponding to infinite products of q-deformed gamma functions. When relaxing the usual restriction on the coupling constants, the model contains add... | 10.173525 | 9.980957 | 12.759665 | 9.790518 | 9.957547 | 10.706792 | 9.714188 | 10.687143 | 9.824809 | 12.698582 | 9.616235 | 10.00628 | 11.072948 | 10.716559 | 9.6595 | 10.593054 | 10.168803 | 10.208333 | 9.71183 | 10.425057 | 9.940279 |
hep-th/0512204 | Satoshi Nagaoka | Yoshihisa Kitazawa and Satoshi Nagaoka | Graviton Propagators on Fuzzy G/H | 22 pages, 1 figure. minor corrections | JHEP0602:001,2006 | 10.1088/1126-6708/2006/02/001 | KEK-TH-1060 | hep-th | null | We describe closed string modes by open Wilson lines in noncommutative (NC)
gauge theories on compact fuzzy G/H in IIB matrix model. In this construction
the world sheet cut-off is related to the spacetime cut-off since the string
bit of the symmetric traced Wilson line carries the minimum momentum on G/H. We
show th... | [
{
"created": "Fri, 16 Dec 2005 10:37:21 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Dec 2005 10:40:17 GMT",
"version": "v2"
},
{
"created": "Thu, 2 Feb 2006 00:47:58 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Kitazawa",
"Yoshihisa",
""
],
[
"Nagaoka",
"Satoshi",
""
]
] | We describe closed string modes by open Wilson lines in noncommutative (NC) gauge theories on compact fuzzy G/H in IIB matrix model. In this construction the world sheet cut-off is related to the spacetime cut-off since the string bit of the symmetric traced Wilson line carries the minimum momentum on G/H. We show that... | 17.302244 | 16.84503 | 16.921946 | 15.620796 | 16.371687 | 17.132616 | 15.563747 | 15.276988 | 16.505278 | 18.028687 | 16.098631 | 16.027592 | 16.383116 | 15.66876 | 15.978004 | 16.309357 | 15.719176 | 16.33094 | 15.877296 | 17.237219 | 15.552374 |
1209.4779 | Anja Marunovic | Anja Marunovic and Tomislav Prokopec | Antiscreening in perturbative quantum gravity and resolving the
Newtonian singularity | 17 pages, 7 figures; a discussion of the relation to the
Barvinsky-Vilkovisky formalism is included in v2; matches published version | Phys. Rev. D 87, 104027 (2013) | 10.1103/PhysRevD.87.104027 | null | hep-th astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the quantum corrections to the Newtonian potential induced by a
massless, nonminimally coupled scalar field on Minkowski background. We make
use of the graviton vacuum polarization calculated in our previous work and
solve the equation of motion nonperturbatively. When written as the
quantum-corrected ga... | [
{
"created": "Fri, 21 Sep 2012 10:43:49 GMT",
"version": "v1"
},
{
"created": "Fri, 30 Aug 2013 13:08:46 GMT",
"version": "v2"
}
] | 2013-09-02 | [
[
"Marunovic",
"Anja",
""
],
[
"Prokopec",
"Tomislav",
""
]
] | We calculate the quantum corrections to the Newtonian potential induced by a massless, nonminimally coupled scalar field on Minkowski background. We make use of the graviton vacuum polarization calculated in our previous work and solve the equation of motion nonperturbatively. When written as the quantum-corrected gaug... | 9.072121 | 9.677238 | 9.406616 | 8.538688 | 9.135651 | 9.300105 | 10.017614 | 8.977856 | 9.986256 | 9.221947 | 9.218136 | 9.191993 | 8.984179 | 8.963512 | 9.20891 | 9.266119 | 9.23572 | 9.009434 | 9.192955 | 9.094856 | 9.088378 |
2307.02038 | Mauricio Romo | Tsung-Ju Lee, Bong H. Lian and Mauricio Romo | Non-commutative resolutions as mirrors of singular Calabi--Yau varieties | 39 pages, LaTeX | null | null | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been conjectured that the hemisphere partition function
arXiv:1308.2217, arXiv:1308.2438 in a gauged linear sigma model (GLSM) computes
the central charge arXiv:math/0212237 of an object in the bounded derived
category of coherent sheaves for Calabi--Yau (CY) manifolds. There is also
evidence in arXiv:alg-geom... | [
{
"created": "Wed, 5 Jul 2023 05:43:35 GMT",
"version": "v1"
}
] | 2023-07-06 | [
[
"Lee",
"Tsung-Ju",
""
],
[
"Lian",
"Bong H.",
""
],
[
"Romo",
"Mauricio",
""
]
] | It has been conjectured that the hemisphere partition function arXiv:1308.2217, arXiv:1308.2438 in a gauged linear sigma model (GLSM) computes the central charge arXiv:math/0212237 of an object in the bounded derived category of coherent sheaves for Calabi--Yau (CY) manifolds. There is also evidence in arXiv:alg-geom/ ... | 7.537515 | 8.053857 | 8.930728 | 7.61627 | 8.634702 | 8.506684 | 8.138484 | 7.626353 | 7.623912 | 9.21234 | 7.720187 | 7.257174 | 7.50393 | 7.241036 | 7.26802 | 7.250028 | 7.22527 | 7.166625 | 7.204865 | 7.599346 | 7.143488 |
hep-th/0203234 | null | Everton M. C. Abreu, Alvaro de Souza Dutra and Clovis Wotzasek | New approaches in W-gravities | 28 pages, Latex | Phys.Rev. D66 (2002) 105008 | 10.1103/PhysRevD.66.105008 | null | hep-th | null | We have devoted an effort to study some nonlinear actions, characteristics of
the ${\cal W}$-theories, in the framework of the soldering formalism. We have
disclosed interesting new results concerning the embedding of the original
chiral ${\cal W}$-particles in different metrical spaces in the final soldered
action, ... | [
{
"created": "Tue, 26 Mar 2002 18:06:17 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Abreu",
"Everton M. C.",
""
],
[
"Dutra",
"Alvaro de Souza",
""
],
[
"Wotzasek",
"Clovis",
""
]
] | We have devoted an effort to study some nonlinear actions, characteristics of the ${\cal W}$-theories, in the framework of the soldering formalism. We have disclosed interesting new results concerning the embedding of the original chiral ${\cal W}$-particles in different metrical spaces in the final soldered action, i.... | 15.491539 | 14.963217 | 16.620705 | 15.169263 | 14.595159 | 15.759444 | 15.22169 | 14.727488 | 14.49537 | 16.748402 | 15.097642 | 14.807732 | 14.654496 | 14.876348 | 14.875631 | 14.717876 | 15.102672 | 14.653253 | 14.619958 | 14.173272 | 14.468277 |
2109.12122 | Javier Gomez Subils | Carlos Hoyos, Niko Jokela, Matti J\"arvinen, Javier G. Subils, Javier
Tarrio, Aleksi Vuorinen | Holographic approach to transport in dense QCD matter | 31 pages + appendices, 6 figures | null | 10.1103/PhysRevD.105.066014 | HIP-2021-23/TH, APCTP Pre2021-018, NORDITA 2021-077 | hep-th astro-ph.HE hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The transport properties of dense QCD matter play a crucial role in the
physics of neutron stars and their mergers, but are notoriously difficult to
study with traditional quantum field theory tools. Specializing to the case of
unpaired quark matter in beta equilibrium, we approach the problem through the
machinery o... | [
{
"created": "Fri, 24 Sep 2021 18:00:03 GMT",
"version": "v1"
}
] | 2022-04-06 | [
[
"Hoyos",
"Carlos",
""
],
[
"Jokela",
"Niko",
""
],
[
"Järvinen",
"Matti",
""
],
[
"Subils",
"Javier G.",
""
],
[
"Tarrio",
"Javier",
""
],
[
"Vuorinen",
"Aleksi",
""
]
] | The transport properties of dense QCD matter play a crucial role in the physics of neutron stars and their mergers, but are notoriously difficult to study with traditional quantum field theory tools. Specializing to the case of unpaired quark matter in beta equilibrium, we approach the problem through the machinery of ... | 7.455373 | 7.212774 | 7.287228 | 7.02125 | 7.186494 | 7.899437 | 7.591521 | 7.35581 | 6.808187 | 7.930709 | 6.98967 | 7.564526 | 6.945471 | 7.00334 | 7.408831 | 7.365294 | 7.314636 | 7.133675 | 7.040723 | 7.379062 | 7.36787 |
hep-th/9905166 | null | Toyohiro Tsurumaru, Izumi Tsutsui | On Topological Terms in the O(3) Nonlinear Sigma Model | 15 pages, 1 figure | Phys.Lett. B460 (1999) 94-102 | 10.1016/S0370-2693(99)00740-6 | KEK 99-19 | hep-th | null | Topological terms in the O(3) nonlinear sigma model in (1+1) and (2+1)
dimensions are re-examined based on the description of the SU(2)-valued field
$g$. We first show that the topological soliton term in (1+1) dimensions arises
from the unitary representations of the group characterizing the global
structure of the ... | [
{
"created": "Mon, 24 May 1999 05:53:57 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Tsurumaru",
"Toyohiro",
""
],
[
"Tsutsui",
"Izumi",
""
]
] | Topological terms in the O(3) nonlinear sigma model in (1+1) and (2+1) dimensions are re-examined based on the description of the SU(2)-valued field $g$. We first show that the topological soliton term in (1+1) dimensions arises from the unitary representations of the group characterizing the global structure of the sy... | 7.62507 | 7.762715 | 7.730227 | 7.210985 | 7.238589 | 7.896982 | 7.503131 | 7.076813 | 7.260612 | 8.344999 | 7.636145 | 7.18276 | 7.64743 | 7.297276 | 7.034679 | 7.317943 | 7.138055 | 7.011195 | 7.413514 | 7.542936 | 7.312516 |
1207.4073 | Mu-In Park | Mu-In Park | The Rotating Black Hole in Renormalizable Quantum Gravity: The
Three-Dimensional Ho\v{r}ava Gravity Case | Some more elaborate discussions on the thermodynamics issue, the
failure of the usual black hole thermodynamics, in the last paragraph of Sec.
IV, Typos Corrected, 11 pages, 3 figures, Accepted in PLB | null | 10.1016/j.physletb.2012.11.067 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently Ho\v{r}ava proposed a renormalizable quantum gravity, without the
ghost problem, by abandoning Einstein's equal-footing treatment of space and
time through the anisotropic scaling dimensions. Since then various interesting
aspects, including the exact black hole solutions have been studied but no
"rotating" ... | [
{
"created": "Tue, 17 Jul 2012 17:52:49 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jul 2012 07:57:57 GMT",
"version": "v2"
},
{
"created": "Tue, 27 Nov 2012 23:04:29 GMT",
"version": "v3"
}
] | 2015-06-05 | [
[
"Park",
"Mu-In",
""
]
] | Recently Ho\v{r}ava proposed a renormalizable quantum gravity, without the ghost problem, by abandoning Einstein's equal-footing treatment of space and time through the anisotropic scaling dimensions. Since then various interesting aspects, including the exact black hole solutions have been studied but no "rotating" bl... | 12.237613 | 10.480914 | 11.879511 | 10.820676 | 11.386333 | 11.009748 | 12.204626 | 11.408545 | 10.918198 | 13.495683 | 10.476892 | 11.139705 | 11.128551 | 10.814255 | 10.951091 | 10.841564 | 11.221734 | 10.469382 | 10.776009 | 10.964391 | 11.102116 |
1412.2806 | Philipp Kleinert | Ville Keranen, Philipp Kleinert | Non-equilibrium scalar two point functions in AdS/CFT | 41 pages, 13 figures; v2: added section 6.5 & references | JHEP 1504 (2015) 119 | 10.1007/JHEP04(2015)119 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the first part of the paper, we discuss different versions of the AdS/CFT
dictionary out of equilibrium. We show that the Skenderis - van Rees
prescription and the "extrapolate" dictionary are equivalent at the level of
"in-in" two point functions of free scalar fields in arbitrary asymptotically
AdS spacetimes. I... | [
{
"created": "Mon, 8 Dec 2014 22:46:54 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Feb 2015 19:36:51 GMT",
"version": "v2"
}
] | 2015-04-28 | [
[
"Keranen",
"Ville",
""
],
[
"Kleinert",
"Philipp",
""
]
] | In the first part of the paper, we discuss different versions of the AdS/CFT dictionary out of equilibrium. We show that the Skenderis - van Rees prescription and the "extrapolate" dictionary are equivalent at the level of "in-in" two point functions of free scalar fields in arbitrary asymptotically AdS spacetimes. In ... | 5.491017 | 5.159829 | 5.987143 | 5.038949 | 5.470988 | 5.329835 | 5.384994 | 4.901242 | 5.122288 | 5.839522 | 5.140015 | 5.100192 | 5.325057 | 5.179425 | 5.178378 | 5.229815 | 5.300022 | 5.234962 | 5.157243 | 5.308226 | 5.140934 |
hep-th/9710126 | null | M. Henningson | Global anomalies in M-theory | 14 pages, harvmac | Nucl.Phys. B515 (1998) 233-245 | 10.1016/S0550-3213(98)00003-0 | CERN-TH/97-277 | hep-th | null | We first consider M-theory formulated on an open eleven-dimensional
spin-manifold. There is then a potential anomaly under gauge transformations on
the E_8 bundle that is defined over the boundary and also under diffeomorphisms
of the boundary. We then consider M-theory configurations that include a
five-brane. In th... | [
{
"created": "Wed, 15 Oct 1997 19:31:43 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Henningson",
"M.",
""
]
] | We first consider M-theory formulated on an open eleven-dimensional spin-manifold. There is then a potential anomaly under gauge transformations on the E_8 bundle that is defined over the boundary and also under diffeomorphisms of the boundary. We then consider M-theory configurations that include a five-brane. In this... | 6.598722 | 6.733428 | 7.571893 | 6.228925 | 7.186333 | 6.495109 | 6.770723 | 6.390555 | 6.003148 | 8.135193 | 6.167673 | 6.199468 | 6.750558 | 6.181509 | 6.379862 | 6.285211 | 6.320384 | 6.278136 | 6.159875 | 6.435786 | 6.259318 |
1008.3801 | Ashoke Sen | Ipsita Mandal and Ashoke Sen | Black Hole Microstate Counting and its Macroscopic Counterpart | 38 pages, LaTeX, based on lectures at various schools; v2: updated
with recent results on sign of index, logarithmic corrections, localization
etc | Class.Quant.Grav.27:214003,2010 | 10.1088/0264-9381/27/21/214003 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We survey recent results on the exact dyon spectrum in a class of N=4
supersymmetric string theories, and discuss how the results can be understood
from the macroscopic viewpoint using AdS_2/CFT_1 correspondence. The comparison
between the microscopic and the macroscopic results includes power suppressed
corrections ... | [
{
"created": "Mon, 23 Aug 2010 11:56:53 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Apr 2012 06:47:50 GMT",
"version": "v2"
}
] | 2012-04-04 | [
[
"Mandal",
"Ipsita",
""
],
[
"Sen",
"Ashoke",
""
]
] | We survey recent results on the exact dyon spectrum in a class of N=4 supersymmetric string theories, and discuss how the results can be understood from the macroscopic viewpoint using AdS_2/CFT_1 correspondence. The comparison between the microscopic and the macroscopic results includes power suppressed corrections to... | 11.933014 | 11.18644 | 12.775255 | 10.318633 | 10.400978 | 10.152971 | 10.367783 | 9.134451 | 9.823977 | 12.058474 | 9.448316 | 9.783559 | 11.678646 | 10.049422 | 9.49172 | 10.054776 | 9.72574 | 10.026739 | 10.141273 | 11.111596 | 9.554947 |
hep-th/0605022 | Martin Rocek | Albert Ko and Martin Rocek | A Gravitational Effective Action on a Finite Triangulation as a Discrete
Model of Continuous Concepts | 7 pages, 1 figure; Presented at the 26th Winter School GEOMETRY AND
PHYSICS at Srni | null | null | YITP-SB-06-08, ITFA-2006-16 | hep-th | null | We recall how the Gauss-Bonnet theorem can be interpreted as a finite dimen-
sional index theorem. We describe the construction given in hep-th/0512293 of a
function that can be interpreted as a gravitational effective action on a
triangulation. The variation of this function under local rescalings of the
edge length... | [
{
"created": "Tue, 2 May 2006 13:09:45 GMT",
"version": "v1"
},
{
"created": "Thu, 4 May 2006 16:13:24 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Ko",
"Albert",
""
],
[
"Rocek",
"Martin",
""
]
] | We recall how the Gauss-Bonnet theorem can be interpreted as a finite dimen- sional index theorem. We describe the construction given in hep-th/0512293 of a function that can be interpreted as a gravitational effective action on a triangulation. The variation of this function under local rescalings of the edge lengths ... | 14.307536 | 14.177709 | 15.906346 | 12.337461 | 14.70601 | 14.346128 | 13.891741 | 14.135755 | 13.243153 | 16.08433 | 14.393214 | 13.422983 | 14.143353 | 13.694358 | 13.426917 | 12.762114 | 14.225389 | 13.341477 | 14.261227 | 13.905682 | 14.303779 |
1907.06193 | Lorenzo Bianchi | Lorenzo Bianchi | Marginal deformations and defect anomalies | 8 pages, v2: derivation on coupling independence for superconformal
surface defects added | Phys. Rev. D 100, 126018 (2019) | 10.1103/PhysRevD.100.126018 | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | We deform a defect conformal field theory by an exactly marginal bulk
operator and we consider the dependence on the marginal coupling of flat and
spherical defect expectation values. For even dimensional spherical defects we
find a logarithmic divergence which can be related to a $a$-type defect anomaly
coefficient.... | [
{
"created": "Sun, 14 Jul 2019 09:42:42 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Dec 2019 08:37:42 GMT",
"version": "v2"
}
] | 2019-12-25 | [
[
"Bianchi",
"Lorenzo",
""
]
] | We deform a defect conformal field theory by an exactly marginal bulk operator and we consider the dependence on the marginal coupling of flat and spherical defect expectation values. For even dimensional spherical defects we find a logarithmic divergence which can be related to a $a$-type defect anomaly coefficient. T... | 12.141931 | 11.204408 | 14.505517 | 11.356303 | 11.417046 | 11.929506 | 10.147882 | 10.918023 | 10.059915 | 14.952672 | 11.181716 | 10.846037 | 12.04301 | 10.965706 | 11.091949 | 10.573035 | 10.901016 | 10.8789 | 10.715571 | 11.688164 | 10.700883 |
hep-th/0312115 | Jacques Distler | Aaron Bergman, Jacques Distler and Uday Varadarajan | 1+1 Dimensional Critical String Theory and Holography | 9 pages, no figures. LaTeX2e (using utarticle.cls and utphys.bst) | null | null | UTTG-07-03 | hep-th | null | In hep-th/0310120, Goheer, Kleban and Susskind argued that the holographic
principle is inconsistent with the existence of stable, Lorentz invariant, 1+1
dimensional compactifications. We note some difficulties with their analysis
and present two novel backgrounds of string theory with 1+1 noncompact
dimensions that ... | [
{
"created": "Wed, 10 Dec 2003 22:13:53 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bergman",
"Aaron",
""
],
[
"Distler",
"Jacques",
""
],
[
"Varadarajan",
"Uday",
""
]
] | In hep-th/0310120, Goheer, Kleban and Susskind argued that the holographic principle is inconsistent with the existence of stable, Lorentz invariant, 1+1 dimensional compactifications. We note some difficulties with their analysis and present two novel backgrounds of string theory with 1+1 noncompact dimensions that sa... | 11.055367 | 10.547523 | 12.326206 | 10.10173 | 10.950911 | 10.314003 | 11.574492 | 11.660605 | 10.473975 | 13.247808 | 9.977702 | 9.073865 | 10.125781 | 9.49612 | 10.154071 | 10.396146 | 9.894807 | 9.310455 | 9.470788 | 10.057095 | 9.723567 |
1903.09503 | Nicolas Wink | Eduardo Grossi and Nicolas Wink | Resolving phase transitions with Discontinuous Galerkin methods | 19 pages, 9 figures; minor corrections | null | null | null | hep-th cond-mat.stat-mech hep-ph physics.comp-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate the applicability and advantages of Discontinuous Galerkin
(DG) schemes in the context of the Functional Renormalization Group (FRG). We
investigate the $O(N)$-model in the large $N$ limit. It is shown that the flow
equation for the effective potential can be cast into a conservative form. We
discuss r... | [
{
"created": "Fri, 22 Mar 2019 13:35:45 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Apr 2019 14:38:24 GMT",
"version": "v2"
},
{
"created": "Wed, 3 Jul 2019 14:11:00 GMT",
"version": "v3"
},
{
"created": "Tue, 15 Nov 2022 19:02:20 GMT",
"version": "v4"
}
] | 2022-11-17 | [
[
"Grossi",
"Eduardo",
""
],
[
"Wink",
"Nicolas",
""
]
] | We demonstrate the applicability and advantages of Discontinuous Galerkin (DG) schemes in the context of the Functional Renormalization Group (FRG). We investigate the $O(N)$-model in the large $N$ limit. It is shown that the flow equation for the effective potential can be cast into a conservative form. We discuss res... | 6.53165 | 6.292938 | 6.293562 | 5.924343 | 6.51014 | 6.548658 | 6.452028 | 6.054302 | 5.751594 | 7.074503 | 6.187334 | 6.001496 | 6.180872 | 5.938302 | 5.965623 | 5.939557 | 5.912321 | 5.928813 | 5.932752 | 6.270317 | 5.955687 |
hep-th/0010050 | Carlos A. S. Almeida | R. R. Landim, C. A. S. Almeida (Departamento de Fisica-UFC) | Topologically massive nonabelian BF models in arbitrary space-time
dimensions | 7 pages | Phys.Lett. B504 (2001) 147-151 | 10.1016/S0370-2693(01)00264-7 | null | hep-th | null | This work extends to the D-dimensional space-time the topological mass
generation mechanism of the nonabelian BF model in four dimensions. In order to
construct the gauge invariant nonabelian kinetic terms for a (D-2)-form B and a
1-form A, we introduce an auxiliary (D-3)-form V. Furthermore, we obtain a
complete set... | [
{
"created": "Sat, 7 Oct 2000 04:19:44 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Landim",
"R. R.",
"",
"Departamento de Fisica-UFC"
],
[
"Almeida",
"C. A. S.",
"",
"Departamento de Fisica-UFC"
]
] | This work extends to the D-dimensional space-time the topological mass generation mechanism of the nonabelian BF model in four dimensions. In order to construct the gauge invariant nonabelian kinetic terms for a (D-2)-form B and a 1-form A, we introduce an auxiliary (D-3)-form V. Furthermore, we obtain a complete set o... | 7.715005 | 6.488509 | 8.091702 | 6.059388 | 6.174108 | 5.963146 | 6.281094 | 5.586146 | 6.091591 | 8.249059 | 6.335035 | 6.783006 | 7.432323 | 6.532672 | 6.588247 | 6.478832 | 6.821867 | 6.598289 | 6.65246 | 7.305224 | 6.724136 |
hep-th/9111002 | null | H. Lu, C.N. Pope, X.J. Wang and K.W. Xu | Anomaly Freedom and Realisations for Super-$W_3$ Strings | 22 pages | Nucl.Phys.B379:24-46,1992 | 10.1016/0550-3213(92)90588-3 | null | hep-th | null | We construct new multi-field realisations of the $N=2$ super-$W_3$ algebra,
which are important for building super-$W_3$ string theories. We derive the
structure of the ghost vacuum for such theories, and use the result to
calculate the intercepts. These results determine the conditions for physical
states in the sup... | [
{
"created": "Fri, 1 Nov 1991 23:41:00 GMT",
"version": "v1"
}
] | 2009-10-07 | [
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Wang",
"X. J.",
""
],
[
"Xu",
"K. W.",
""
]
] | We construct new multi-field realisations of the $N=2$ super-$W_3$ algebra, which are important for building super-$W_3$ string theories. We derive the structure of the ghost vacuum for such theories, and use the result to calculate the intercepts. These results determine the conditions for physical states in the super... | 10.604248 | 8.197888 | 9.941294 | 9.206765 | 10.75582 | 8.830576 | 8.967999 | 8.900406 | 8.951474 | 10.512481 | 9.442413 | 9.466394 | 10.33522 | 9.507906 | 9.754647 | 9.685837 | 9.541055 | 9.275761 | 10.060831 | 10.124377 | 9.818895 |
1101.4783 | C. P. Martin Professsor | C.P.Martin | NC GUTs: A Status Report | 15 pages; 1 figure; talk given at the Workshop on Noncommutative
Field Theory and Gravity, Corfu, September 2010 | PoS CNCFG2010:026,2011 | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I review the main results that have been obtained so far on the construction
of noncommutative GUTs
| [
{
"created": "Tue, 25 Jan 2011 12:08:54 GMT",
"version": "v1"
}
] | 2011-05-18 | [
[
"Martin",
"C. P.",
""
]
] | I review the main results that have been obtained so far on the construction of noncommutative GUTs | 12.359165 | 7.477003 | 7.91008 | 7.999012 | 7.496495 | 6.54566 | 6.665115 | 7.226392 | 6.896914 | 7.396353 | 7.553915 | 7.046309 | 8.419234 | 7.474331 | 7.030811 | 6.725821 | 6.768462 | 7.512661 | 7.271304 | 8.002498 | 6.909655 |
1409.5984 | Thijs van den Broek | Wim Beenakker, Walter D. van Suijlekom, Thijs van den Broek | Supersymmetry and noncommutative geometry Part III: The noncommutative
supersymmetric Standard Model | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a previous paper we developed a formalism to construct (potentially)
supersymmetric theories in the context of noncommutative geometry. We apply
this formalism to explore the existence of a noncommutative version of the
minimal supersymmetric Standard Model (MSSM). We obtain the exact particle
content of the MSSM ... | [
{
"created": "Sun, 21 Sep 2014 13:59:33 GMT",
"version": "v1"
}
] | 2014-09-23 | [
[
"Beenakker",
"Wim",
""
],
[
"van Suijlekom",
"Walter D.",
""
],
[
"Broek",
"Thijs van den",
""
]
] | In a previous paper we developed a formalism to construct (potentially) supersymmetric theories in the context of noncommutative geometry. We apply this formalism to explore the existence of a noncommutative version of the minimal supersymmetric Standard Model (MSSM). We obtain the exact particle content of the MSSM an... | 9.920341 | 9.324133 | 9.86131 | 9.776713 | 10.248096 | 9.918414 | 9.447667 | 9.195827 | 9.526605 | 11.483882 | 8.669991 | 9.421842 | 9.902767 | 9.221281 | 9.295741 | 9.44874 | 8.858783 | 9.55277 | 9.584084 | 9.324973 | 9.105803 |
hep-th/0306023 | Nicolas Boulanger | Nicolas Boulanger, Sandrine Cnockaert and Marc Henneaux | A note on spin-s duality | Minor corrections, reference added | JHEP 0306 (2003) 060 | 10.1088/1126-6708/2003/06/060 | null | hep-th | null | Duality is investigated for higher spin ($s \geq 2$), free, massless, bosonic
gauge fields. We show how the dual formulations can be derived from a common
"parent", first-order action. This goes beyond most of the previous treatments
where higher-spin duality was investigated at the level of the equations of
motion o... | [
{
"created": "Tue, 3 Jun 2003 18:40:41 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jul 2003 19:13:16 GMT",
"version": "v2"
},
{
"created": "Sun, 7 Sep 2003 15:22:25 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Boulanger",
"Nicolas",
""
],
[
"Cnockaert",
"Sandrine",
""
],
[
"Henneaux",
"Marc",
""
]
] | Duality is investigated for higher spin ($s \geq 2$), free, massless, bosonic gauge fields. We show how the dual formulations can be derived from a common "parent", first-order action. This goes beyond most of the previous treatments where higher-spin duality was investigated at the level of the equations of motion onl... | 7.358603 | 6.876155 | 7.656142 | 6.858126 | 7.085817 | 7.42933 | 7.388761 | 6.991433 | 6.913025 | 7.828866 | 6.711427 | 6.696156 | 6.83275 | 6.70905 | 6.841166 | 6.748508 | 6.822539 | 6.737333 | 6.701944 | 6.699288 | 6.981866 |
1611.07981 | Marc Schneider | Stefan Hofmann and Marc Schneider | Non-Gaussian ground-state deformations near a black-hole singularity | 6 pages | Phys. Rev. D 95, 065033 (2017) | 10.1103/PhysRevD.95.065033 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The singularity theorem by Hawking and Penrose qualifies Schwarzschild
black-holes as geodesic incomplete space-times. Albeit this is a mathematically
rigorous statement, it requires an operational framework that allows to probe
the space-like singularity via a measurement process. Any such framework
necessarily has ... | [
{
"created": "Wed, 23 Nov 2016 21:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Apr 2017 07:21:51 GMT",
"version": "v2"
}
] | 2017-04-04 | [
[
"Hofmann",
"Stefan",
""
],
[
"Schneider",
"Marc",
""
]
] | The singularity theorem by Hawking and Penrose qualifies Schwarzschild black-holes as geodesic incomplete space-times. Albeit this is a mathematically rigorous statement, it requires an operational framework that allows to probe the space-like singularity via a measurement process. Any such framework necessarily has to... | 10.561768 | 11.137502 | 11.415078 | 10.660905 | 11.931975 | 11.364249 | 11.925036 | 11.073561 | 11.313816 | 11.405692 | 10.692274 | 10.418689 | 10.686585 | 10.480575 | 10.310656 | 10.586712 | 10.452756 | 10.603838 | 10.743565 | 10.415063 | 10.321076 |
1604.05003 | Subham Dutta Chowdhury | Subham Dutta Chowdhury, Justin R. David | Global gravitational anomalies and transport | 53 pages, Mathematica code for Wick contractions available on request | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the constraints imposed by global gravitational anomalies on
parity odd induced transport coefficients in even dimensions for theories with
chiral fermions, gravitinos and self dual tensors. The $\eta$-invariant for the
large diffeomorphism corresponding to the $T$ transformation on a torus
constraints... | [
{
"created": "Mon, 18 Apr 2016 06:03:05 GMT",
"version": "v1"
},
{
"created": "Mon, 23 May 2016 08:15:42 GMT",
"version": "v2"
}
] | 2016-05-24 | [
[
"Chowdhury",
"Subham Dutta",
""
],
[
"David",
"Justin R.",
""
]
] | We investigate the constraints imposed by global gravitational anomalies on parity odd induced transport coefficients in even dimensions for theories with chiral fermions, gravitinos and self dual tensors. The $\eta$-invariant for the large diffeomorphism corresponding to the $T$ transformation on a torus constraints t... | 8.991769 | 9.271704 | 10.22889 | 9.4065 | 9.282868 | 8.845022 | 8.424432 | 8.759876 | 9.005817 | 10.186191 | 8.7014 | 8.437811 | 9.049598 | 8.553771 | 8.266987 | 8.4924 | 8.408535 | 8.607402 | 8.600088 | 9.141046 | 8.278686 |
2103.14640 | Giorgos Anastasiou | Giorgos Anastasiou, Ignacio J. Araya, Robert B. Mann and Rodrigo Olea | Renormalized holographic entanglement entropy in Lovelock gravity | 38 pages,no figures, One reference added | null | 10.1007/JHEP06(2021)073 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the renormalization of Entanglement Entropy in holographic CFTs dual
to Lovelock gravity. It is known that the holographic EE in Lovelock gravity is
given by the Jacobson-Myers (JM) functional. As usual, due to the divergent
Weyl factor in the Fefferman-Graham expansion of the boundary metric for
Asymptotica... | [
{
"created": "Fri, 26 Mar 2021 17:55:23 GMT",
"version": "v1"
},
{
"created": "Sun, 13 Jun 2021 16:13:17 GMT",
"version": "v2"
},
{
"created": "Tue, 15 Jun 2021 22:48:12 GMT",
"version": "v3"
}
] | 2021-06-17 | [
[
"Anastasiou",
"Giorgos",
""
],
[
"Araya",
"Ignacio J.",
""
],
[
"Mann",
"Robert B.",
""
],
[
"Olea",
"Rodrigo",
""
]
] | We study the renormalization of Entanglement Entropy in holographic CFTs dual to Lovelock gravity. It is known that the holographic EE in Lovelock gravity is given by the Jacobson-Myers (JM) functional. As usual, due to the divergent Weyl factor in the Fefferman-Graham expansion of the boundary metric for Asymptoticall... | 6.751791 | 6.807885 | 8.268936 | 6.882514 | 7.638699 | 7.014493 | 6.97041 | 6.847635 | 6.642079 | 8.100402 | 6.625727 | 6.831464 | 6.854178 | 6.764564 | 6.600802 | 6.794524 | 6.878448 | 6.662759 | 6.812472 | 6.628557 | 6.779805 |
hep-th/0305027 | Marty Stock | R. Jackiw | Noncommuting fields and non-Abelian fluids | 16 pp., invited talk at "Renormalization Group and Anomalies in
Gravity and Cosmology", Ouro Preto, Brazil, March 2003. Minor typos corrected | null | 10.1016/S0920-5632(03)02400-9 | MIT-CTP-3369 | hep-th | null | The original ideas about noncommuting coordinates are recalled. The
connection between U(1) gauge fields defined on noncommuting coordinates and
fluid mechanics is explained. Non-Abelian fluid mechanics is described.
| [
{
"created": "Fri, 2 May 2003 17:20:21 GMT",
"version": "v1"
},
{
"created": "Fri, 2 May 2003 21:17:59 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Jackiw",
"R.",
""
]
] | The original ideas about noncommuting coordinates are recalled. The connection between U(1) gauge fields defined on noncommuting coordinates and fluid mechanics is explained. Non-Abelian fluid mechanics is described. | 17.507151 | 8.743142 | 14.464924 | 11.681066 | 10.765667 | 10.248636 | 10.385305 | 11.057757 | 10.149792 | 15.961503 | 11.28073 | 13.11831 | 15.152787 | 12.734248 | 13.540381 | 12.923985 | 12.676194 | 13.521828 | 13.275759 | 13.966516 | 13.533597 |
hep-th/9902169 | Shigeaki Yahikozawa | Masafumi Fukuma and Shigeaki Yahikozawa | Comments on D-Instantons in c<1 Strings | 12 pages with 1 figure, LaTex, Version to appear in PLB | Phys.Lett. B460 (1999) 71-78 | 10.1016/S0370-2693(99)00744-3 | YITP-99-9, RUP-99-2 | hep-th | null | We suggest that the boundary cosmological constant \zeta in c<1 unitary
string theory be regarded as the one-dimensional complex coordinate of the
target space on which the boundaries of world-sheets can live. From this
viewpoint we explicitly construct analogues of D-instantons which satisfy
Polchinski's ``combinato... | [
{
"created": "Tue, 23 Feb 1999 23:04:46 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Feb 1999 12:35:02 GMT",
"version": "v2"
},
{
"created": "Sat, 27 Feb 1999 11:33:06 GMT",
"version": "v3"
},
{
"created": "Fri, 18 Jun 1999 12:36:49 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Fukuma",
"Masafumi",
""
],
[
"Yahikozawa",
"Shigeaki",
""
]
] | We suggest that the boundary cosmological constant \zeta in c<1 unitary string theory be regarded as the one-dimensional complex coordinate of the target space on which the boundaries of world-sheets can live. From this viewpoint we explicitly construct analogues of D-instantons which satisfy Polchinski's ``combinatori... | 19.837978 | 15.880938 | 21.915636 | 17.162455 | 17.882036 | 18.978436 | 17.732132 | 18.623585 | 18.092768 | 24.45401 | 17.098906 | 18.506964 | 22.000853 | 18.428747 | 18.338305 | 18.891798 | 18.683876 | 19.126368 | 18.680126 | 21.167881 | 18.381269 |
hep-th/0008111 | Ken-iti Izawa | S. Hayakawa and K.-I. Izawa | Warped Compactification with an Abelian Gauge Theory | 6 pages, latex | Phys.Lett. B493 (2000) 380-382 | 10.1016/S0370-2693(00)01158-8 | UT-905 | hep-th | null | We investigate warped compactification with an abelian gauge theory in six
dimensions. The vanishing cosmological constant in four dimensions can
generically be realized with a regular metric even in a 3-brane background
without fine tuning of couplings.
| [
{
"created": "Mon, 14 Aug 2000 08:30:59 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Oct 2000 04:54:33 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Hayakawa",
"S.",
""
],
[
"Izawa",
"K. -I.",
""
]
] | We investigate warped compactification with an abelian gauge theory in six dimensions. The vanishing cosmological constant in four dimensions can generically be realized with a regular metric even in a 3-brane background without fine tuning of couplings. | 16.995167 | 14.228696 | 15.105953 | 13.385711 | 12.501893 | 14.118773 | 13.540811 | 14.271165 | 13.649506 | 15.912947 | 13.08133 | 14.609529 | 14.929019 | 13.953774 | 14.633723 | 13.335724 | 14.172487 | 13.199013 | 13.720888 | 15.068227 | 13.881378 |
1106.0295 | Gianluca Calcagni | Gianluca Calcagni | Discrete to continuum transition in multifractal spacetimes | 4 pages; v2: presentation clarified, typos corrected, results
unchanged; v3: matches the published version; v4: hyperlinks activated | Phys.Rev.D84:061501,2011 | 10.1103/PhysRevD.84.061501 | AEI-2011-030 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We outline a field theory on a multifractal spacetime. The measure in the
action is characterized by a varying Hausdorff dimension and logarithmic
oscillations governed by a fundamental physical length. A fine hierarchy of
length scales identifies different regimes, from a microscopic structure with
discrete symmetri... | [
{
"created": "Wed, 1 Jun 2011 19:59:52 GMT",
"version": "v1"
},
{
"created": "Sun, 5 Jun 2011 15:56:21 GMT",
"version": "v2"
},
{
"created": "Fri, 2 Sep 2011 09:47:48 GMT",
"version": "v3"
},
{
"created": "Mon, 5 Sep 2011 08:58:49 GMT",
"version": "v4"
}
] | 2011-09-29 | [
[
"Calcagni",
"Gianluca",
""
]
] | We outline a field theory on a multifractal spacetime. The measure in the action is characterized by a varying Hausdorff dimension and logarithmic oscillations governed by a fundamental physical length. A fine hierarchy of length scales identifies different regimes, from a microscopic structure with discrete symmetries... | 17.412395 | 16.796614 | 17.623423 | 16.25382 | 17.971382 | 16.965984 | 17.009293 | 15.724244 | 16.76078 | 18.184328 | 17.395725 | 17.039873 | 17.148752 | 16.495695 | 17.183033 | 16.723015 | 16.772818 | 16.705173 | 17.49968 | 16.520096 | 16.244959 |
2207.05101 | Dhruva K.S | Prabhav Jain, Sachin Jain, Bibhut Sahoo, Dhruva K.S, Aashna Zade | Mapping Large N Slightly Broken Higher Spin (SBHS) theory correlators to
Free theory correlators | 39 pages+28 pages appendices, Published version | J. High Energ. Phys. 2023, 173 (2023) | 10.1007/JHEP12(2023)173 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a systematic method to constrain any n-point correlation function
of spinning operators in Large N Slightly Broken Higher Spin (SBHS) theories.
As an illustration of the methodology, we work out the three point functions
which reproduce the previously known results. We then work out the four point
function... | [
{
"created": "Mon, 11 Jul 2022 18:00:05 GMT",
"version": "v1"
},
{
"created": "Wed, 31 Aug 2022 12:18:35 GMT",
"version": "v2"
},
{
"created": "Sat, 23 Mar 2024 08:10:57 GMT",
"version": "v3"
}
] | 2024-03-26 | [
[
"Jain",
"Prabhav",
""
],
[
"Jain",
"Sachin",
""
],
[
"Sahoo",
"Bibhut",
""
],
[
"S",
"Dhruva K.",
""
],
[
"Zade",
"Aashna",
""
]
] | We develop a systematic method to constrain any n-point correlation function of spinning operators in Large N Slightly Broken Higher Spin (SBHS) theories. As an illustration of the methodology, we work out the three point functions which reproduce the previously known results. We then work out the four point functions ... | 12.313711 | 11.543274 | 14.110864 | 11.022279 | 11.586652 | 11.098366 | 11.202236 | 11.457685 | 10.921926 | 13.865554 | 10.82772 | 11.091824 | 11.620225 | 11.524157 | 11.434786 | 11.552045 | 10.993171 | 10.976116 | 11.0617 | 11.847504 | 10.972045 |
1507.00818 | Arnab Kundu | Arnab Kundu | Effective Temperature in Steady-state Dynamics from Holography | 48 pages, 2 figures | null | null | null | hep-th cond-mat.stat-mech gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that, within the realm of gauge-gravity duality, for a large class
of systems in a steady-state there exists an effective thermodynamic
description. This description comes equipped with an effective temperature and
a free energy, but no well-defined notion of entropy. Such systems are
described by probe degr... | [
{
"created": "Fri, 3 Jul 2015 05:28:30 GMT",
"version": "v1"
}
] | 2015-07-06 | [
[
"Kundu",
"Arnab",
""
]
] | We argue that, within the realm of gauge-gravity duality, for a large class of systems in a steady-state there exists an effective thermodynamic description. This description comes equipped with an effective temperature and a free energy, but no well-defined notion of entropy. Such systems are described by probe degree... | 9.357618 | 9.163073 | 9.231557 | 8.655025 | 9.764401 | 9.06254 | 9.445128 | 8.941967 | 8.968846 | 10.544767 | 8.787756 | 9.002492 | 9.192581 | 8.641513 | 9.092732 | 8.865107 | 9.091575 | 8.617497 | 8.597348 | 9.29587 | 8.882701 |
1006.5145 | Tim Koslowski A | Tim A. Koslowski, Alessandro Sfondrini | Functional Renormalization of Noncommutative Scalar Field Theory | 38 pages, no figures, LaTeX | Int.J.Mod.Phys.A26:4009-4051,2011 | 10.1142/S0217751X11054048 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we apply the Functional Renormalization Group Equation (FRGE)
to the non-commutative scalar field theory proposed by Grosse and Wulkenhaar.
We derive the flow equation in the matrix representation and discuss the theory
space for the self-dual model. The features introduced by the external
dimensionful ... | [
{
"created": "Sat, 26 Jun 2010 14:34:55 GMT",
"version": "v1"
},
{
"created": "Sun, 3 Jul 2011 16:25:47 GMT",
"version": "v2"
}
] | 2011-09-19 | [
[
"Koslowski",
"Tim A.",
""
],
[
"Sfondrini",
"Alessandro",
""
]
] | In this paper we apply the Functional Renormalization Group Equation (FRGE) to the non-commutative scalar field theory proposed by Grosse and Wulkenhaar. We derive the flow equation in the matrix representation and discuss the theory space for the self-dual model. The features introduced by the external dimensionful sc... | 7.565872 | 7.739892 | 9.236171 | 6.765149 | 7.513343 | 7.129273 | 7.590572 | 7.464725 | 7.48736 | 8.18295 | 7.24514 | 7.044683 | 7.468328 | 6.953874 | 6.896282 | 7.120355 | 7.108132 | 7.027926 | 6.960991 | 7.243681 | 6.769734 |
1601.04658 | Marco Crisostomi | Marco Crisostomi, Matthew Hull, Kazuya Koyama and Gianmassimo Tasinato | Horndeski: beyond, or not beyond? | 19 pages, published version | JCAP03 (2016) 038 | 10.1088/1475-7516/2016/03/038 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Determining the most general, consistent scalar tensor theory of gravity is
important for building models of inflation and dark energy. In this work we
investigate the number of degrees of freedom present in the theory of beyond
Horndeski. We discuss how to construct the theory from the extrinsic curvature
of the con... | [
{
"created": "Mon, 18 Jan 2016 19:25:22 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Mar 2016 11:41:53 GMT",
"version": "v2"
}
] | 2016-03-23 | [
[
"Crisostomi",
"Marco",
""
],
[
"Hull",
"Matthew",
""
],
[
"Koyama",
"Kazuya",
""
],
[
"Tasinato",
"Gianmassimo",
""
]
] | Determining the most general, consistent scalar tensor theory of gravity is important for building models of inflation and dark energy. In this work we investigate the number of degrees of freedom present in the theory of beyond Horndeski. We discuss how to construct the theory from the extrinsic curvature of the const... | 8.746405 | 9.106649 | 9.361326 | 8.510442 | 8.623479 | 8.672847 | 8.891216 | 8.768882 | 8.586143 | 9.945299 | 8.919603 | 8.7409 | 8.617804 | 8.832056 | 8.443037 | 8.586867 | 8.543821 | 8.330588 | 8.551909 | 9.285691 | 8.672092 |
hep-th/0607072 | Gabriel Bengochea | Matias Aiello, Gabriel Bengochea and Rafael Ferraro | Anisotropic effects of background fields on Born-Infeld electromagnetic
waves | 4 pages, Revtex4, 1 figure, corrected typos, comments clarified,
version accepted for publication | Phys.Lett.A361:9-12,2007 | 10.1016/j.physleta.2006.09.027 | null | hep-th gr-qc physics.optics | null | We show exact solutions of Born-Infeld theory for electromagnetic plane waves
propagating in the presence of static background fields. The non-linear
character of Born-Infeld equations generates an interaction between background
and wave that changes the speed of propagation and adds a longitudinal
component to the w... | [
{
"created": "Tue, 11 Jul 2006 19:18:47 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Sep 2006 15:17:14 GMT",
"version": "v2"
}
] | 2011-07-19 | [
[
"Aiello",
"Matias",
""
],
[
"Bengochea",
"Gabriel",
""
],
[
"Ferraro",
"Rafael",
""
]
] | We show exact solutions of Born-Infeld theory for electromagnetic plane waves propagating in the presence of static background fields. The non-linear character of Born-Infeld equations generates an interaction between background and wave that changes the speed of propagation and adds a longitudinal component to the wav... | 9.55723 | 8.400528 | 8.899508 | 8.344199 | 8.833611 | 8.67699 | 9.558333 | 8.477256 | 8.746393 | 9.318819 | 8.622831 | 9.042745 | 9.161804 | 8.925017 | 9.036864 | 9.020281 | 9.176525 | 8.80734 | 8.594784 | 9.398067 | 8.791725 |
2405.17559 | Maria Knysh | Maria Knysh, Hong Liu, Natalia Pinzani-Fokeeva | New horizon symmetries, hydrodynamics, and quantum chaos | 36 pages+ appendices, 1 figure | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We generalize the formulation of horizon symmetries presented in previous
literature to include diffeomorphisms that can shift the location of the
horizon. In the context of the AdS/CFT duality, we show that horizon symmetries
can be interpreted on the boundary as emergent low-energy gauge symmetries. In
particular, ... | [
{
"created": "Mon, 27 May 2024 18:00:05 GMT",
"version": "v1"
}
] | 2024-05-29 | [
[
"Knysh",
"Maria",
""
],
[
"Liu",
"Hong",
""
],
[
"Pinzani-Fokeeva",
"Natalia",
""
]
] | We generalize the formulation of horizon symmetries presented in previous literature to include diffeomorphisms that can shift the location of the horizon. In the context of the AdS/CFT duality, we show that horizon symmetries can be interpreted on the boundary as emergent low-energy gauge symmetries. In particular, we... | 7.303627 | 7.029874 | 7.718069 | 7.485529 | 6.936343 | 6.641073 | 6.923548 | 6.33588 | 6.757953 | 7.526013 | 6.773624 | 6.944153 | 7.560749 | 6.930277 | 6.767955 | 6.918327 | 6.799345 | 6.896921 | 6.881775 | 7.399639 | 6.91151 |
hep-th/0011201 | Takayuki Matsuki | Takayuki Matsuki, Masashi Shiotani | Gauge Symmetry Breakdown due to Dyanamical versus Elementary Higgs | RevTeX, 10 pages, 5 figures | null | null | null | hep-th | null | We study in details on how gauge bosons can acquire mass when the chiral
symmetry dynamically breaks down for massless gauge theory without scalars.
Introducing dynamical scalar fields into the original gauge theory, we show
that when the chiral symmetry breaks down, the theory gives gauge boson masses
different from... | [
{
"created": "Wed, 22 Nov 2000 16:40:04 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Matsuki",
"Takayuki",
""
],
[
"Shiotani",
"Masashi",
""
]
] | We study in details on how gauge bosons can acquire mass when the chiral symmetry dynamically breaks down for massless gauge theory without scalars. Introducing dynamical scalar fields into the original gauge theory, we show that when the chiral symmetry breaks down, the theory gives gauge boson masses different from w... | 12.497534 | 11.745599 | 11.963021 | 11.483424 | 11.853977 | 12.309041 | 11.829769 | 11.314777 | 11.00827 | 12.480359 | 11.451163 | 11.279552 | 11.407936 | 11.225283 | 11.589358 | 11.484383 | 11.525704 | 11.156541 | 11.355414 | 11.738147 | 11.384485 |
hep-th/9705008 | Sergei Odintsov | A.A. Bytsenko, L.N. Granda and S.D. Odintsov | Exact Renormalization Group and Running Newtonian Coupling in Higher
Derivative Gravity | Latex file, 9 pages | JETP Lett.65:600-604,1997 | 10.1134/1.567411 | null | hep-th | null | We discuss exact renormalization group (RG) in $R^2$-gravity using effective
average action formalism. The truncated evolution equation for such a theory on
De Sitter background leads to the system of nonperturbative RG equations for
cosmological and gravitational coupling constants. Approximate solution of
these RG ... | [
{
"created": "Fri, 2 May 1997 09:27:23 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Bytsenko",
"A. A.",
""
],
[
"Granda",
"L. N.",
""
],
[
"Odintsov",
"S. D.",
""
]
] | We discuss exact renormalization group (RG) in $R^2$-gravity using effective average action formalism. The truncated evolution equation for such a theory on De Sitter background leads to the system of nonperturbative RG equations for cosmological and gravitational coupling constants. Approximate solution of these RG eq... | 14.117628 | 11.16011 | 9.142879 | 9.596094 | 11.012481 | 10.200146 | 9.954518 | 9.429138 | 10.555902 | 13.43968 | 11.010346 | 11.879107 | 11.859509 | 11.398269 | 11.819875 | 11.685094 | 11.35536 | 11.174611 | 12.134621 | 12.08707 | 11.405048 |
1807.04416 | Patrick Copinger | Patrick Copinger, Kenji Fukushima, Shi Pu | Axial Ward identity and the Schwinger mechanism -- Applications to the
real-time chiral magnetic effect and condensates | 5 pages, 2 figures | Phys. Rev. Lett. 121, 261602 (2018) | 10.1103/PhysRevLett.121.261602 | null | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We elucidate chirality production under parity breaking constant
electromagnetic fields, with which we clarify qualitative differences in and
out of equilibrium. For a strong magnetic field the pair production from the
Schwinger mechanism increments the chirality. The pair production rate is
exponentially suppressed ... | [
{
"created": "Thu, 12 Jul 2018 04:17:44 GMT",
"version": "v1"
}
] | 2019-01-02 | [
[
"Copinger",
"Patrick",
""
],
[
"Fukushima",
"Kenji",
""
],
[
"Pu",
"Shi",
""
]
] | We elucidate chirality production under parity breaking constant electromagnetic fields, with which we clarify qualitative differences in and out of equilibrium. For a strong magnetic field the pair production from the Schwinger mechanism increments the chirality. The pair production rate is exponentially suppressed wi... | 13.401358 | 14.798932 | 13.908603 | 12.862708 | 15.891374 | 14.413483 | 15.458566 | 14.45605 | 14.473577 | 15.19656 | 13.529697 | 13.939413 | 13.623671 | 13.608977 | 14.418455 | 14.239869 | 14.224762 | 13.935287 | 13.447408 | 13.666734 | 13.49215 |
hep-th/9405083 | Silvio Rabello | Silvio J. Rabello and Carlos Farina | On gauge invariance and the path integral | 4 pages, Latex, IF-UFRJ-94 | null | 10.1103/PhysRevA.51.2614 | null | hep-th cond-mat | null | Using a gauge covariant operator technique we deduce the path integral for a
charged particle in a stationary magnetic field, verifying the "midpoint rule"
for the discrete form of the interaction term with the vector potential.
| [
{
"created": "Thu, 12 May 1994 20:11:36 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Rabello",
"Silvio J.",
""
],
[
"Farina",
"Carlos",
""
]
] | Using a gauge covariant operator technique we deduce the path integral for a charged particle in a stationary magnetic field, verifying the "midpoint rule" for the discrete form of the interaction term with the vector potential. | 22.799673 | 20.769848 | 21.827751 | 16.220123 | 19.172829 | 19.191652 | 19.303946 | 19.235758 | 18.218012 | 18.77422 | 16.685644 | 18.110632 | 18.205151 | 16.301208 | 17.481777 | 17.174463 | 17.033077 | 17.124973 | 16.787897 | 18.420965 | 16.574955 |
hep-th/9612101 | Burkhard Kleihaus | Burkhard Kleihaus and Jutta Kunz (Universit\"at Oldenburg) | Static Axially Symmetric Solutions of Einstein-Yang-Mills-Dilaton Theory | 11 pages, including 2 postscript figures | Phys.Rev.Lett. 78 (1997) 2527-2530 | 10.1103/PhysRevLett.78.2527 | null | hep-th gr-qc | null | We construct static axially symmetric solutions of SU(2)
Einstein-Yang-Mills-dilaton theory. Like their spherically symmetric
counterparts, these solutions are nonsingular and asymptotically flat. The
solutions are characterized by the winding number n and the node number k of
the gauge field functions. For fixed n w... | [
{
"created": "Tue, 10 Dec 1996 13:10:24 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Kleihaus",
"Burkhard",
"",
"Universität Oldenburg"
],
[
"Kunz",
"Jutta",
"",
"Universität Oldenburg"
]
] | We construct static axially symmetric solutions of SU(2) Einstein-Yang-Mills-dilaton theory. Like their spherically symmetric counterparts, these solutions are nonsingular and asymptotically flat. The solutions are characterized by the winding number n and the node number k of the gauge field functions. For fixed n wit... | 5.51932 | 4.882398 | 4.441485 | 4.222691 | 4.334197 | 3.967701 | 4.498568 | 4.289639 | 4.735536 | 4.675021 | 4.830092 | 5.041768 | 5.165681 | 5.11293 | 4.886152 | 5.037794 | 5.155365 | 4.936729 | 5.271518 | 5.2609 | 5.08954 |
hep-th/0408237 | Hugo Reinhardt | H. Reinhardt and C. Feuchter | On the Yang-Mills wave functional in Coulomb gauge | 9 pages, no figures | Phys.Rev. D71 (2005) 105002 | 10.1103/PhysRevD.71.105002 | null | hep-th hep-ph | null | We investigate the dependence of the Yang-Mills wave functional in Coulomb
gauge on the Faddeev-Popov determinant. We use a Gaussian wave functional
multiplied by an arbitrary power of the Faddeev-Popov determinant. We show,
that within the resummation of one-loop diagrams the stationary vacuum energy
is independent ... | [
{
"created": "Tue, 31 Aug 2004 11:20:45 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Reinhardt",
"H.",
""
],
[
"Feuchter",
"C.",
""
]
] | We investigate the dependence of the Yang-Mills wave functional in Coulomb gauge on the Faddeev-Popov determinant. We use a Gaussian wave functional multiplied by an arbitrary power of the Faddeev-Popov determinant. We show, that within the resummation of one-loop diagrams the stationary vacuum energy is independent of... | 6.213799 | 6.416849 | 5.958634 | 5.781501 | 5.887477 | 6.43678 | 5.932989 | 6.031226 | 6.139894 | 6.234947 | 5.509587 | 5.967622 | 5.779183 | 5.580965 | 5.86389 | 6.056333 | 5.760252 | 5.912712 | 5.653345 | 5.699703 | 5.793481 |
1806.08367 | Eirik Eik Svanes | Anthony Ashmore and Xenia de la Ossa and Ruben Minasian and Charles
Strickland-Constable and Eirik Eik Svanes | Finite deformations from a heterotic superpotential: holomorphic
Chern--Simons and an $L_\infty$ algebra | 65 pages, including 5 appendices | JHEP 10 (2018) 179 | 10.1007/JHEP10(2018)179 | null | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider finite deformations of the Hull--Strominger system. Starting from
the heterotic superpotential, we identify complex coordinates on the off-shell
parameter space. Expanding the superpotential around a supersymmetric vacuum
leads to a third-order Maurer--Cartan equation that controls the moduli. The
resulti... | [
{
"created": "Thu, 21 Jun 2018 18:00:15 GMT",
"version": "v1"
}
] | 2022-02-04 | [
[
"Ashmore",
"Anthony",
""
],
[
"de la Ossa",
"Xenia",
""
],
[
"Minasian",
"Ruben",
""
],
[
"Strickland-Constable",
"Charles",
""
],
[
"Svanes",
"Eirik Eik",
""
]
] | We consider finite deformations of the Hull--Strominger system. Starting from the heterotic superpotential, we identify complex coordinates on the off-shell parameter space. Expanding the superpotential around a supersymmetric vacuum leads to a third-order Maurer--Cartan equation that controls the moduli. The resulting... | 11.08884 | 10.037498 | 14.671748 | 10.049417 | 10.770684 | 11.397141 | 10.836329 | 10.585139 | 11.081718 | 14.022413 | 11.167486 | 10.924423 | 11.651852 | 10.104703 | 10.681485 | 11.002658 | 11.257573 | 11.023156 | 10.283064 | 11.580954 | 10.382943 |
2212.14027 | Marco Fazzi | Marco Fazzi, Simone Giacomelli, Suvendu Giri | Hierarchies of RG flows in 6d $(1,0)$ massive E-strings | Part II of a series of papers; 37+11 pages; 13 figures | null | 10.1007/JHEP03(2023)089 | UUITP-60/22 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the analysis of arXiv:2208.11703 to the 6d $(1,0)$ SCFTs known as
massive E-string theories, which can be engineered in massive Type IIA with
$8-n_0<8$ D8-branes close to an O8$^-$ (or O8$^*$ if $n_0=8,9$). For each
choice of $n_0=1,\ldots,9$ the massive $E_{1+(8-n_0)}$-strings (including the
more exotic $\... | [
{
"created": "Wed, 28 Dec 2022 18:54:31 GMT",
"version": "v1"
}
] | 2023-03-16 | [
[
"Fazzi",
"Marco",
""
],
[
"Giacomelli",
"Simone",
""
],
[
"Giri",
"Suvendu",
""
]
] | We extend the analysis of arXiv:2208.11703 to the 6d $(1,0)$ SCFTs known as massive E-string theories, which can be engineered in massive Type IIA with $8-n_0<8$ D8-branes close to an O8$^-$ (or O8$^*$ if $n_0=8,9$). For each choice of $n_0=1,\ldots,9$ the massive $E_{1+(8-n_0)}$-strings (including the more exotic $\ti... | 8.281707 | 8.528136 | 9.378539 | 7.968524 | 8.859598 | 8.955344 | 8.662097 | 8.44752 | 8.044005 | 10.603492 | 7.880433 | 8.058069 | 8.597944 | 7.712033 | 8.011796 | 7.960482 | 7.955227 | 7.801057 | 7.8577 | 8.811222 | 7.697484 |
hep-th/9703060 | null | Itzhak Bars and Costas Kounnas | Theories with Two Times | Latex, 14 pages | Phys.Lett. B402 (1997) 25-32 | 10.1016/S0370-2693(97)00452-8 | CERN-TH/97-36, USC-97/HEP-B1, LPTENS-97/09 | hep-th | null | General considerations on the unification of A-type and B-type
supersymmetries in the context of interacting p-branes strongly suggest that
the signature of spacetime includes two timelike dimensions. This leads to the
puzzle of how ordinary physics with a single timelike dimension emerges. In
this letter we suggest ... | [
{
"created": "Fri, 7 Mar 1997 10:48:22 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Bars",
"Itzhak",
""
],
[
"Kounnas",
"Costas",
""
]
] | General considerations on the unification of A-type and B-type supersymmetries in the context of interacting p-branes strongly suggest that the signature of spacetime includes two timelike dimensions. This leads to the puzzle of how ordinary physics with a single timelike dimension emerges. In this letter we suggest th... | 12.390649 | 12.601957 | 12.89024 | 12.210537 | 12.926148 | 13.738175 | 12.827642 | 12.735484 | 12.052011 | 13.985892 | 11.951365 | 11.73033 | 11.887172 | 11.62796 | 11.821872 | 11.771563 | 11.807509 | 12.078393 | 11.804737 | 12.120727 | 11.403042 |
0808.2066 | Fernando Ruiz | S. Marculescu, F. Ruiz Ruiz | Seiberg--Witten maps for $\boldsymbol{SO(1,3)}$ gauge invariance and
deformations of gravity | 1 encapsulated figure | Phys.Rev.D79:025004,2009 | 10.1103/PhysRevD.79.025004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A family of diffeomorphism-invariant Seiberg--Witten deformations of gravity
is constructed. In a first step Seiberg--Witten maps for an SO(1,3) gauge
symmetry are obtained for constant deformation parameters. This includes maps
for the vierbein, the spin connection and the Einstein--Hilbert Lagrangian. In
a second s... | [
{
"created": "Thu, 14 Aug 2008 22:29:59 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Oct 2008 15:46:23 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Dec 2008 09:46:11 GMT",
"version": "v3"
}
] | 2010-05-28 | [
[
"Marculescu",
"S.",
""
],
[
"Ruiz",
"F. Ruiz",
""
]
] | A family of diffeomorphism-invariant Seiberg--Witten deformations of gravity is constructed. In a first step Seiberg--Witten maps for an SO(1,3) gauge symmetry are obtained for constant deformation parameters. This includes maps for the vierbein, the spin connection and the Einstein--Hilbert Lagrangian. In a second ste... | 7.087142 | 6.596641 | 6.844333 | 6.450096 | 6.717611 | 6.834533 | 6.64455 | 6.634605 | 6.674172 | 7.517077 | 6.688284 | 6.495719 | 6.900809 | 6.625783 | 6.647603 | 6.5304 | 6.357547 | 6.445963 | 6.627739 | 6.908134 | 6.467785 |
hep-th/9112069 | Michael Newman | David J. Gross and Michael J. Newman | Unitary And Hermitian Matrices In An External Field II: The Kontsevich
Model And Continuum Virasoro Constraints | 17 pages | Nucl.Phys. B380 (1992) 168-180 | 10.1016/0550-3213(92)90520-L | null | hep-th | null | We give a simple derivation of the Virasoro constraints in the Kontsevich
model, first derived by Witten. We generalize the method to a model of unitary
matrices, for which we find a new set of Virasoro constraints. Finally we
discuss the solution for symmetric matrices in an external field.
| [
{
"created": "Mon, 23 Dec 1991 19:02:37 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Gross",
"David J.",
""
],
[
"Newman",
"Michael J.",
""
]
] | We give a simple derivation of the Virasoro constraints in the Kontsevich model, first derived by Witten. We generalize the method to a model of unitary matrices, for which we find a new set of Virasoro constraints. Finally we discuss the solution for symmetric matrices in an external field. | 9.00796 | 7.750506 | 8.334198 | 7.185004 | 6.992275 | 7.695714 | 6.813485 | 7.794911 | 7.424576 | 9.292395 | 7.260952 | 7.23045 | 8.803066 | 7.694756 | 7.579 | 7.19776 | 7.427444 | 7.61665 | 7.803824 | 8.704037 | 7.627517 |
1306.6701 | Kenji Muneyuki | Kenji Muneyuki and Nobuyoshi Ohta | Renormalization of Higher Derivative Quantum Gravity Coupled to a Scalar
with Shift Symmetry | 11 pages. arXiv admin note: substantial text overlap with
arXiv:1201.2058. v2: minor corrections. v3: minor corrections to match the
published version | null | 10.1016/j.physletb.2013.07.054 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been suggested that higher-derivative gravity theories coupled to a
scalar field with shift symmetry may be an important candidate for a quantum
gravity. We show that this class of gravity theories are renormalizable in D =
3 and 4 dimensions.
| [
{
"created": "Fri, 28 Jun 2013 02:55:40 GMT",
"version": "v1"
},
{
"created": "Sat, 27 Jul 2013 00:36:34 GMT",
"version": "v2"
},
{
"created": "Wed, 7 Aug 2013 05:22:25 GMT",
"version": "v3"
}
] | 2015-06-16 | [
[
"Muneyuki",
"Kenji",
""
],
[
"Ohta",
"Nobuyoshi",
""
]
] | It has been suggested that higher-derivative gravity theories coupled to a scalar field with shift symmetry may be an important candidate for a quantum gravity. We show that this class of gravity theories are renormalizable in D = 3 and 4 dimensions. | 10.510084 | 7.964328 | 8.578122 | 7.417534 | 8.468069 | 8.208964 | 8.451589 | 7.691895 | 7.709783 | 9.368662 | 7.974024 | 8.04826 | 8.502129 | 7.741599 | 8.141641 | 8.251432 | 7.980928 | 7.876338 | 8.421803 | 8.239806 | 7.528267 |
0809.4728 | Hyun Seok Yang | Hyun Seok Yang | Emergent Spacetime and The Origin of Gravity | v3; 80 pages, Cosmetic revision for publication and references added,
to appear in JHEP | JHEP 0905:012,2009 | 10.1088/1126-6708/2009/05/012 | KIAS-P08059 | hep-th gr-qc hep-ph math.SG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an exposition on the geometrization of the electromagnetic force.
We show that, in noncommutative (NC) spacetime, there always exists a
coordinate transformation to locally eliminate the electromagnetic force, which
is precisely the Darboux theorem in symplectic geometry. As a consequence, the
electromagne... | [
{
"created": "Mon, 29 Sep 2008 19:56:00 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Jan 2009 11:14:10 GMT",
"version": "v2"
},
{
"created": "Thu, 30 Apr 2009 17:32:57 GMT",
"version": "v3"
}
] | 2009-06-30 | [
[
"Yang",
"Hyun Seok",
""
]
] | We present an exposition on the geometrization of the electromagnetic force. We show that, in noncommutative (NC) spacetime, there always exists a coordinate transformation to locally eliminate the electromagnetic force, which is precisely the Darboux theorem in symplectic geometry. As a consequence, the electromagneti... | 7.454621 | 6.907341 | 7.44558 | 7.12322 | 6.955502 | 6.936274 | 7.165709 | 6.910098 | 6.843336 | 8.159702 | 7.239265 | 7.164074 | 7.180762 | 7.180735 | 7.010716 | 7.076491 | 7.197216 | 7.090249 | 7.021338 | 7.188853 | 7.04184 |
2402.03446 | Michele Fossati | Michele Fossati, Filiberto Ares, Jerome Dubail, Pasquale Calabrese | Entanglement asymmetry in CFT and its relation to non-topological
defects | 37 pages, 7 figures | JHEP 2024, 59 (2024) | 10.1007/JHEP05(2024)059 | null | hep-th cond-mat.stat-mech quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The entanglement asymmetry is an information based observable that quantifies
the degree of symmetry breaking in a region of an extended quantum system. We
investigate this measure in the ground state of one dimensional critical
systems described by a CFT. Employing the correspondence between global
symmetries and de... | [
{
"created": "Mon, 5 Feb 2024 19:01:09 GMT",
"version": "v1"
}
] | 2024-05-14 | [
[
"Fossati",
"Michele",
""
],
[
"Ares",
"Filiberto",
""
],
[
"Dubail",
"Jerome",
""
],
[
"Calabrese",
"Pasquale",
""
]
] | The entanglement asymmetry is an information based observable that quantifies the degree of symmetry breaking in a region of an extended quantum system. We investigate this measure in the ground state of one dimensional critical systems described by a CFT. Employing the correspondence between global symmetries and defe... | 7.282531 | 7.986946 | 8.357422 | 7.8533 | 8.076631 | 8.453811 | 7.911459 | 7.823108 | 7.982 | 9.022237 | 7.646302 | 7.279743 | 7.894927 | 7.454376 | 7.263743 | 7.346542 | 7.359181 | 7.483438 | 7.440785 | 7.945522 | 7.250068 |
2108.00732 | Yunqin Zheng | Yasunori Lee, Yunqin Zheng | Comments on compatibility between Conformal symmetry and Continuous
higher-form symmetries | 14 pages, 5 tables | Phys. Rev. D 104, 085005 (2021) | 10.1103/PhysRevD.104.085005 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the compatibility between the conformal symmetry together with the
unitarity and the continuous higher-form symmetries. We show that the
d-dimensional unitary conformal field theories are not consistent with
continuous p-form symmetries for certain (d,p), assuming that the corresponding
conserved current is ... | [
{
"created": "Mon, 2 Aug 2021 09:00:18 GMT",
"version": "v1"
}
] | 2021-10-13 | [
[
"Lee",
"Yasunori",
""
],
[
"Zheng",
"Yunqin",
""
]
] | We study the compatibility between the conformal symmetry together with the unitarity and the continuous higher-form symmetries. We show that the d-dimensional unitary conformal field theories are not consistent with continuous p-form symmetries for certain (d,p), assuming that the corresponding conserved current is a ... | 10.092212 | 10.643554 | 12.466162 | 9.871797 | 11.05906 | 9.277957 | 9.167518 | 10.371122 | 9.395074 | 11.185603 | 9.682217 | 10.139877 | 9.99321 | 9.387723 | 9.60146 | 9.829012 | 9.615541 | 9.362989 | 9.502938 | 10.139367 | 9.563513 |
1904.11507 | Matthias Kaminski | Casey Cartwright and Matthias Kaminski | Correlations far from equilibrium in charged strongly coupled fluids
subjected to a strong magnetic field | v2: published version, minor changes, clarified relation to
anisotropies in heavy ion collisions, added references; v1: 25 figures, 14
tables, 57 pages, comments welcome | null | 10.1007/JHEP09(2019)072 | null | hep-th cond-mat.str-el hep-ph nucl-ex nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Within a holographic model, we calculate the time evolution of 2-point and
1-point correlation functions (of selected operators) within a charged strongly
coupled system of many particles. That system is thermalizing from an
anisotropic initial charged state far from equilibrium towards equilibrium
while subjected to... | [
{
"created": "Thu, 25 Apr 2019 18:00:02 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Sep 2019 17:11:08 GMT",
"version": "v2"
}
] | 2019-10-02 | [
[
"Cartwright",
"Casey",
""
],
[
"Kaminski",
"Matthias",
""
]
] | Within a holographic model, we calculate the time evolution of 2-point and 1-point correlation functions (of selected operators) within a charged strongly coupled system of many particles. That system is thermalizing from an anisotropic initial charged state far from equilibrium towards equilibrium while subjected to a... | 10.373148 | 10.750978 | 10.883541 | 10.167557 | 10.6996 | 10.819864 | 10.570875 | 10.887802 | 9.938507 | 11.387855 | 10.206897 | 9.884798 | 10.108018 | 10.077614 | 10.180724 | 10.301679 | 10.132294 | 10.05553 | 10.163994 | 10.154359 | 10.060627 |
1008.2156 | Paul S. Aspinwall | Paul S. Aspinwall, Ilarion V. Melnikov and M. Ronen Plesser | (0,2) Elephants | 51 pages, oversimplification in spectral sequence fixed | null | 10.1007/JHEP01(2012)060 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We enumerate massless E6 singlets for (0,2)-compactifications of the
heterotic string on a Calabi-Yau threefold with the "standard embedding" in
three distinct ways. In the large radius limit of the threefold, these singlets
count deformations of the Calabi-Yau together with its tangent bundle. In the
"small-radius" ... | [
{
"created": "Thu, 12 Aug 2010 16:04:43 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Dec 2010 16:31:32 GMT",
"version": "v2"
}
] | 2015-05-19 | [
[
"Aspinwall",
"Paul S.",
""
],
[
"Melnikov",
"Ilarion V.",
""
],
[
"Plesser",
"M. Ronen",
""
]
] | We enumerate massless E6 singlets for (0,2)-compactifications of the heterotic string on a Calabi-Yau threefold with the "standard embedding" in three distinct ways. In the large radius limit of the threefold, these singlets count deformations of the Calabi-Yau together with its tangent bundle. In the "small-radius" li... | 10.291649 | 9.422518 | 11.521976 | 10.02441 | 10.669429 | 10.841665 | 10.152535 | 9.773067 | 9.526282 | 12.510773 | 9.366609 | 9.901148 | 10.861706 | 9.91155 | 9.636333 | 9.84439 | 9.744085 | 10.051423 | 9.950148 | 10.507998 | 9.434205 |
hep-th/0412336 | Peter West | Peter West | Brane dynamics, central charges and E_{11} | 19 pages, plain tex | JHEP0503:077,2005 | 10.1088/1126-6708/2005/03/077 | KCL-MTH-04-18 | hep-th | null | We consider a theory in which supersymmetry is partially spontaneously broken
and show that the dynamical fields in the same supersymmetric multiplet as the
Goldstino are Goldstone bosons whose corresponding generators are central
charges in the underlying supersymmetry algebra. We illustrate how this works
for four ... | [
{
"created": "Fri, 31 Dec 2004 18:53:49 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"West",
"Peter",
""
]
] | We consider a theory in which supersymmetry is partially spontaneously broken and show that the dynamical fields in the same supersymmetric multiplet as the Goldstino are Goldstone bosons whose corresponding generators are central charges in the underlying supersymmetry algebra. We illustrate how this works for four di... | 12.118917 | 9.415531 | 12.084574 | 9.685793 | 10.214935 | 10.190467 | 10.18571 | 9.694195 | 9.571786 | 12.247012 | 9.669975 | 10.75964 | 11.49245 | 10.478938 | 10.617277 | 10.641973 | 10.911906 | 10.662031 | 10.868185 | 11.858112 | 10.279194 |
hep-th/0307168 | Shahn Majid | G.A. Goldin and S. Majid | On the Fock space for nonrelativistic anyon fields and braided tensor
products | Added some references, more explicit formulae for the discrete case
and remark on partition function. 25 pages latex, no figures | J.Math.Phys.45:3770-3787,2004 | 10.1063/1.1787620 | null | hep-th math.QA | null | We realize the physical N-anyon Hilbert spaces, introduced previously via
unitary representations of the group of diffeomorphisms of the plane, as N-fold
braided-symmetric tensor products of the 1-particle Hilbert space. This
perspective provides a convenient Fock space construction for nonrelativistic
anyon quantum ... | [
{
"created": "Thu, 17 Jul 2003 22:58:45 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Oct 2003 19:20:48 GMT",
"version": "v2"
}
] | 2011-08-17 | [
[
"Goldin",
"G. A.",
""
],
[
"Majid",
"S.",
""
]
] | We realize the physical N-anyon Hilbert spaces, introduced previously via unitary representations of the group of diffeomorphisms of the plane, as N-fold braided-symmetric tensor products of the 1-particle Hilbert space. This perspective provides a convenient Fock space construction for nonrelativistic anyon quantum fi... | 15.187433 | 18.423605 | 17.485121 | 16.24831 | 17.51054 | 18.69146 | 19.091341 | 16.613621 | 16.204695 | 19.074455 | 15.031828 | 16.107914 | 15.592759 | 15.680521 | 15.565061 | 15.931167 | 15.611567 | 15.156791 | 15.669788 | 16.3885 | 15.409603 |
hep-th/0305233 | Wang-Chang Su | Wang-Chang Su | Class of Exact Solutions of the SU(3) Skyrme Model | 15 pages, no figure | Phys.Lett. B568 (2003) 167-175 | 10.1016/j.physletb.2003.06.024 | null | hep-th | null | Recently, Hirayama and Yamashita have presented an ansatz that allows us to
construct a class of solutions for the SU(2) Skyrme model. Though these
solutions are not solitonic, they provide us with an example on how the plane
wave solutions arise in nonlinear field theories. In this paper, we investigate
the applicab... | [
{
"created": "Tue, 27 May 2003 06:15:40 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Su",
"Wang-Chang",
""
]
] | Recently, Hirayama and Yamashita have presented an ansatz that allows us to construct a class of solutions for the SU(2) Skyrme model. Though these solutions are not solitonic, they provide us with an example on how the plane wave solutions arise in nonlinear field theories. In this paper, we investigate the applicabil... | 7.705817 | 7.56151 | 7.948519 | 6.918046 | 7.952053 | 7.608122 | 7.576694 | 7.195696 | 7.251573 | 7.70432 | 7.309681 | 7.649597 | 7.567553 | 7.37164 | 7.770229 | 7.883281 | 7.3666 | 7.665313 | 7.391673 | 7.714468 | 7.440411 |
2403.13232 | Jarah Evslin | Jarah Evslin and Kehinde Ogundipe | Perturbative Approach to Time-Dependent Quantum Solitons | 30 pages, no figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently we have introduced a lightweight, perturbative approach to quantum
solitons. Thus far, our approach has been largely limited to configurations
consisting of a single soliton plus a finite number of mesons, whose classical
limit is an isolated stationary or rigidly moving soliton. In this paper, with
an eye t... | [
{
"created": "Wed, 20 Mar 2024 01:43:40 GMT",
"version": "v1"
}
] | 2024-03-21 | [
[
"Evslin",
"Jarah",
""
],
[
"Ogundipe",
"Kehinde",
""
]
] | Recently we have introduced a lightweight, perturbative approach to quantum solitons. Thus far, our approach has been largely limited to configurations consisting of a single soliton plus a finite number of mesons, whose classical limit is an isolated stationary or rigidly moving soliton. In this paper, with an eye to ... | 11.217224 | 11.123264 | 11.507275 | 10.751644 | 10.737033 | 10.645351 | 10.508098 | 10.711369 | 10.949517 | 12.245769 | 10.117255 | 10.989022 | 11.224273 | 10.58528 | 10.632831 | 10.846997 | 10.697493 | 10.642843 | 10.897757 | 11.470394 | 10.638769 |
hep-th/9701180 | Manuel Calixto Molina | M. Calixto, V. Aldaya and M. Navarro | Quantum Field Theory in a Symmetric Curved Space from a Second
Quantization on a Group | 31 pages, LaTeX, no figures; substantial improvement, new material
added; to appear in Int. J. Mod. Phys. A | Int.J.Mod.Phys.A15:4011-4044,2000 | 10.1142/S0217751X00001233 | SWAT/247 | hep-th | null | In this article we propose a `second quantization' scheme especially suitable
to deal with non-trivial, highly symmetric phase spaces, implemented within a
more general Group Approach to Quantization, which recovers the standard
Quantum Field Theory (QFT) for ordinary relativistic linear fields. We
emphasize, among i... | [
{
"created": "Thu, 30 Jan 1997 11:27:45 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Mar 2000 11:52:42 GMT",
"version": "v2"
}
] | 2016-12-28 | [
[
"Calixto",
"M.",
""
],
[
"Aldaya",
"V.",
""
],
[
"Navarro",
"M.",
""
]
] | In this article we propose a `second quantization' scheme especially suitable to deal with non-trivial, highly symmetric phase spaces, implemented within a more general Group Approach to Quantization, which recovers the standard Quantum Field Theory (QFT) for ordinary relativistic linear fields. We emphasize, among its... | 18.164148 | 18.366541 | 17.139025 | 16.730789 | 15.75893 | 17.746056 | 17.939125 | 17.050634 | 16.713228 | 17.420126 | 16.72121 | 16.059809 | 16.087328 | 15.776577 | 15.994699 | 16.1437 | 16.08737 | 16.233023 | 16.443054 | 15.279546 | 16.027857 |
2211.17253 | Alejandro Vilar Lopez | Ben Craps, Marine De Clerck, Alejandro Vilar L\'opez | Definitions of entwinement | 30 pages + 1 appendix, 1 figure | null | 10.1007/JHEP03(2023)079 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Entwinement was first introduced as the CFT dual to extremal, non-minimal
geodesics of quotiented AdS$_3$ spaces. It was heuristically meant to capture
the entanglement of internal, gauged degrees of freedom, for instance in the
symmetric product orbifold CFT of the D1/D5 brane system. The literature now
contains dif... | [
{
"created": "Wed, 30 Nov 2022 18:51:25 GMT",
"version": "v1"
}
] | 2023-03-29 | [
[
"Craps",
"Ben",
""
],
[
"De Clerck",
"Marine",
""
],
[
"López",
"Alejandro Vilar",
""
]
] | Entwinement was first introduced as the CFT dual to extremal, non-minimal geodesics of quotiented AdS$_3$ spaces. It was heuristically meant to capture the entanglement of internal, gauged degrees of freedom, for instance in the symmetric product orbifold CFT of the D1/D5 brane system. The literature now contains diffe... | 10.359052 | 10.211411 | 11.058512 | 9.021796 | 10.223458 | 9.90566 | 9.124695 | 9.522045 | 9.526823 | 11.462393 | 9.079096 | 9.482349 | 9.60519 | 9.212523 | 9.265187 | 9.216269 | 9.335267 | 9.497908 | 9.232235 | 9.652704 | 9.032983 |
hep-th/0402086 | Sami Mohammad | M. Sami, V. Sahni | Quintessential Inflation on the Brane and the Relic Gravity Wave
Background | 9 pages, 5 eps figures. Discussion and one eps figure summarizing the
GB correction to steep brane world inflation added, typos corrected and
references added; final version to appear in PRD | Phys.Rev. D70 (2004) 083513 | 10.1103/PhysRevD.70.083513 | null | hep-th astro-ph gr-qc hep-ph | null | Quintessential inflation describes a scenario in which both inflation and
dark energy (quintessence) are described by the same scalar field. In
conventional braneworld models of quintessential inflation gravitational
particle production is used to reheat the universe. This reheating mechanism is
very inefficient and ... | [
{
"created": "Wed, 11 Feb 2004 07:59:02 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Feb 2004 06:35:20 GMT",
"version": "v2"
},
{
"created": "Sat, 11 Sep 2004 04:50:37 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Sami",
"M.",
""
],
[
"Sahni",
"V.",
""
]
] | Quintessential inflation describes a scenario in which both inflation and dark energy (quintessence) are described by the same scalar field. In conventional braneworld models of quintessential inflation gravitational particle production is used to reheat the universe. This reheating mechanism is very inefficient and re... | 7.213616 | 6.33871 | 6.291152 | 5.863877 | 6.319655 | 6.498905 | 6.8698 | 5.819373 | 5.900358 | 6.215587 | 6.217732 | 6.294285 | 6.099121 | 5.982843 | 6.158257 | 6.174982 | 6.110568 | 5.99556 | 5.984246 | 6.229653 | 6.341235 |
1405.3157 | Gabor Takacs | M. Lencses and G. Takacs | Excited state TBA and renormalized TCSA in the scaling Potts model | 39 pages, 5 eps figures. v2: reference added. v3: several misprints
corrected, and an important step in the derivation of counter terms (in
section 3.4.1) is explained in more detail | JHEP 09 (2014) 052 | 10.1007/JHEP09(2014)052 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the field theory describing the scaling limit of the Potts
quantum spin chain using a combination of two approaches. The first is the
renormalized truncated conformal space approach (TCSA), while the second one is
a new thermodynamic Bethe Ansatz (TBA) system for the excited state spectrum in
finite volum... | [
{
"created": "Tue, 13 May 2014 14:07:11 GMT",
"version": "v1"
},
{
"created": "Wed, 21 May 2014 11:35:38 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Jul 2014 12:41:38 GMT",
"version": "v3"
}
] | 2014-09-11 | [
[
"Lencses",
"M.",
""
],
[
"Takacs",
"G.",
""
]
] | We consider the field theory describing the scaling limit of the Potts quantum spin chain using a combination of two approaches. The first is the renormalized truncated conformal space approach (TCSA), while the second one is a new thermodynamic Bethe Ansatz (TBA) system for the excited state spectrum in finite volume.... | 6.964999 | 7.651129 | 8.16805 | 7.072809 | 7.487999 | 7.45248 | 7.481099 | 7.021069 | 6.808852 | 8.515884 | 6.976253 | 6.954954 | 7.175212 | 6.868768 | 6.972408 | 7.101879 | 7.14837 | 7.009854 | 6.867768 | 7.244418 | 6.866794 |
1311.1853 | Tuna Yildirim Ph.D. | Tuna Yildirim | Topologically Massive Yang-Mills Theory and Link Invariants | 18 pages, 1 figure, Final version accepted for publication in IJMPA | Int.J.Mod.Phys.A, 30,1550034 (2015) | 10.1142/S0217751X15500347 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Topologically massive Yang-Mills theory is studied in the framework of
geometric quantization. Since this theory has a mass gap proportional to the
topological mass m, Yang-Mills contribution decays exponentially at very large
distances compared to 1/m, leaving a pure Chern-Simons theory with level number
k. In this ... | [
{
"created": "Fri, 8 Nov 2013 00:17:20 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Nov 2013 10:30:41 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Jun 2014 07:50:35 GMT",
"version": "v3"
},
{
"created": "Sun, 15 Feb 2015 02:56:33 GMT",
"version": "v4"
}
] | 2015-02-17 | [
[
"Yildirim",
"Tuna",
""
]
] | Topologically massive Yang-Mills theory is studied in the framework of geometric quantization. Since this theory has a mass gap proportional to the topological mass m, Yang-Mills contribution decays exponentially at very large distances compared to 1/m, leaving a pure Chern-Simons theory with level number k. In this pa... | 6.744802 | 5.288141 | 6.933549 | 5.76928 | 5.04043 | 4.967695 | 4.839108 | 5.344575 | 5.434105 | 7.363852 | 5.873565 | 6.147337 | 6.404823 | 6.220552 | 5.814344 | 5.926417 | 5.926626 | 5.983752 | 6.377035 | 6.454572 | 6.04636 |
2212.14062 | Matthieu Vilatte | Nehal Mittal, P. Marios Petropoulos, David Rivera-Betancour and
Matthieu Vilatte | Ehlers, Carroll, Charges and Dual Charges | V1: Latex 1+46 pages, V2: JHEP version, ammended by a footnote (nb
44) in Appendix B | JHEP07 (2023) 065 | 10.1007/JHEP07(2023)065 | CPHT-RR047.072022 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We unravel the boundary manifestation of Ehlers' hidden M\"obius symmetry
present in four-dimensional Ricci-flat spacetimes that enjoy a time-like
isometry and are Petrov-algebraic. This is achieved in a designated gauge,
shaped in the spirit of flat holography, where the Carrollian three-dimensional
nature of the nu... | [
{
"created": "Wed, 28 Dec 2022 19:01:33 GMT",
"version": "v1"
},
{
"created": "Sun, 9 Jul 2023 20:38:42 GMT",
"version": "v2"
}
] | 2023-07-11 | [
[
"Mittal",
"Nehal",
""
],
[
"Petropoulos",
"P. Marios",
""
],
[
"Rivera-Betancour",
"David",
""
],
[
"Vilatte",
"Matthieu",
""
]
] | We unravel the boundary manifestation of Ehlers' hidden M\"obius symmetry present in four-dimensional Ricci-flat spacetimes that enjoy a time-like isometry and are Petrov-algebraic. This is achieved in a designated gauge, shaped in the spirit of flat holography, where the Carrollian three-dimensional nature of the null... | 19.214663 | 17.159861 | 19.152109 | 16.806486 | 19.684931 | 17.337111 | 18.329773 | 17.301186 | 16.555405 | 20.967262 | 16.710356 | 16.89922 | 18.377851 | 16.645191 | 16.564047 | 17.052719 | 16.83692 | 16.917067 | 17.134941 | 18.930717 | 16.355434 |
hep-th/0309263 | Dipankar Chakrabarti | Dipankar Chakrabarti, A. Harindranath, Lubomir Martinovic and J. P.
Vary | Kinks in Discrete Light Cone Quantization | 10 pages, 3 figures | Phys.Lett. B582 (2004) 196-202 | 10.1016/j.physletb.2003.12.049 | null | hep-th | null | We investigate non-trivial topological structures in Discrete Light Cone
Quantization (DLCQ) through the example of the broken symmetry phase of the two
dimensional $\phi^4$ theory using anti periodic boundary condition (APBC). We
present evidence for degenerate ground states which is both a signature of
spontaneous ... | [
{
"created": "Tue, 30 Sep 2003 05:45:02 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Chakrabarti",
"Dipankar",
""
],
[
"Harindranath",
"A.",
""
],
[
"Martinovic",
"Lubomir",
""
],
[
"Vary",
"J. P.",
""
]
] | We investigate non-trivial topological structures in Discrete Light Cone Quantization (DLCQ) through the example of the broken symmetry phase of the two dimensional $\phi^4$ theory using anti periodic boundary condition (APBC). We present evidence for degenerate ground states which is both a signature of spontaneous sy... | 11.528573 | 10.469653 | 11.294466 | 10.287654 | 11.280392 | 10.780537 | 11.259968 | 10.604865 | 10.234365 | 11.908404 | 10.73605 | 11.086553 | 10.768899 | 10.962434 | 11.125622 | 11.0043 | 10.866488 | 11.394597 | 10.774405 | 10.885957 | 11.017316 |
hep-th/0505226 | Jorge Russo | J. Lopez Carballo and J.G. Russo | New Bubble Decays In Kaluza-Klein Theories | 15 pages | JHEP 0508 (2005) 053 | 10.1088/1126-6708/2005/08/053 | UB-ECM-PF-05/13 | hep-th | null | We describe new bubble decays in pure D+1 dimensional Einstein theory with
two compact directions. The instanton solution is constructed by analytic
continuation of the Kaluza-Klein electrically charged black hole solution. We
show that the instanton describes the decay of a Kaluza-Klein vacuum M^{D-1} x
T^2 with a n... | [
{
"created": "Wed, 25 May 2005 11:02:11 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Carballo",
"J. Lopez",
""
],
[
"Russo",
"J. G.",
""
]
] | We describe new bubble decays in pure D+1 dimensional Einstein theory with two compact directions. The instanton solution is constructed by analytic continuation of the Kaluza-Klein electrically charged black hole solution. We show that the instanton describes the decay of a Kaluza-Klein vacuum M^{D-1} x T^2 with a non... | 9.335782 | 8.485472 | 9.733648 | 8.369827 | 8.231416 | 9.06036 | 8.575692 | 8.243076 | 8.432294 | 11.166586 | 8.260721 | 8.850026 | 9.299416 | 8.524364 | 9.077472 | 8.403703 | 8.881737 | 8.53575 | 8.329456 | 9.458945 | 8.602404 |
2106.02642 | Matti Jarvinen | Romuald A. Janik, Matti Jarvinen, Jacob Sonnenschein | A simple description of holographic domain walls in confining theories
-- extended hydrodynamics | 51 pages, 11 figures. v2: references updated | null | 10.1007/JHEP09(2021)129 | APCTP Pre2021 - 011 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the context of theories with a first order phase transition, we propose a
general covariant description of coexisting phases separated by domain walls
using an additional order parameter-like degree of freedom. In the case of a
holographic Witten model with a confining and deconfined phase, the resulting
model ext... | [
{
"created": "Fri, 4 Jun 2021 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Jun 2021 12:42:15 GMT",
"version": "v2"
}
] | 2021-10-04 | [
[
"Janik",
"Romuald A.",
""
],
[
"Jarvinen",
"Matti",
""
],
[
"Sonnenschein",
"Jacob",
""
]
] | In the context of theories with a first order phase transition, we propose a general covariant description of coexisting phases separated by domain walls using an additional order parameter-like degree of freedom. In the case of a holographic Witten model with a confining and deconfined phase, the resulting model exten... | 16.294559 | 16.725849 | 15.685714 | 14.367911 | 15.695789 | 15.910078 | 16.215221 | 15.616986 | 14.787604 | 15.619146 | 14.619906 | 14.805451 | 15.133728 | 14.563335 | 14.810329 | 14.654846 | 14.470113 | 14.805695 | 14.927032 | 15.31446 | 14.055647 |
hep-th/9404018 | null | C. Duval, Z. Horv\'ath, P.A. Horv\'athy | The Nappi-Witten example and gravitational waves | null | null | null | null | hep-th | null | The vanishing of the anomaly in the recent example of Nappi and Witten,
constructed from the Wess-Zumino-Witten model based on a certain non-semisimple
group, follows from a more general result valid for gravitational waves. The
construction of the metric is explained.}
| [
{
"created": "Tue, 5 Apr 1994 08:52:59 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Duval",
"C.",
""
],
[
"Horváth",
"Z.",
""
],
[
"Horváthy",
"P. A.",
""
]
] | The vanishing of the anomaly in the recent example of Nappi and Witten, constructed from the Wess-Zumino-Witten model based on a certain non-semisimple group, follows from a more general result valid for gravitational waves. The construction of the metric is explained.} | 17.569454 | 13.1519 | 15.592696 | 13.512733 | 13.948174 | 14.52851 | 15.05279 | 13.327117 | 13.063561 | 16.004793 | 13.752201 | 13.489873 | 14.940314 | 14.044415 | 13.177631 | 13.505229 | 13.89512 | 13.436139 | 14.382564 | 15.462856 | 13.783178 |
0710.1680 | Motomu Tsuda | K. Shima, M. Tsuda and W. Lang | On vacuum structures of N = 2 LSUSY QED equivalent to N = 2 NLSUSY model | 10 pages, correct form of the potential given as a footnote | Phys.Lett.B659:741-745,2008; Erratum-ibid.Phys.Lett.B672:413,2009 | 10.1016/j.physletb.2007.11.036 10.1016/j.physletb.2007.12.043 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The vacuum structure of N = 2 linear supersymmetry (LSUSY) invariant QED,
which is equivalent to N = 2 nonlinear supersymmetry (NLSUSY) model, is studied
explicitly in two dimensional space-time (d = 2). Two different isometries
SO(1,3) and SO(3,1) appear for the vacuum field configuration corresponding to
the variou... | [
{
"created": "Tue, 9 Oct 2007 03:49:11 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Oct 2007 05:14:20 GMT",
"version": "v2"
},
{
"created": "Mon, 3 Dec 2007 03:39:42 GMT",
"version": "v3"
},
{
"created": "Sun, 30 Dec 2007 08:46:51 GMT",
"version": "v4"
},
{
"cre... | 2009-06-19 | [
[
"Shima",
"K.",
""
],
[
"Tsuda",
"M.",
""
],
[
"Lang",
"W.",
""
]
] | The vacuum structure of N = 2 linear supersymmetry (LSUSY) invariant QED, which is equivalent to N = 2 nonlinear supersymmetry (NLSUSY) model, is studied explicitly in two dimensional space-time (d = 2). Two different isometries SO(1,3) and SO(3,1) appear for the vacuum field configuration corresponding to the various ... | 8.547319 | 6.91775 | 8.135934 | 7.35509 | 7.695594 | 7.192166 | 7.366987 | 7.756971 | 7.360978 | 9.316525 | 7.268317 | 7.75978 | 8.282195 | 7.523428 | 7.813939 | 7.825302 | 7.318355 | 7.511758 | 7.5065 | 8.360362 | 7.52142 |
hep-th/0405037 | Satoshi Yamada | Shozo Uehara and Satoshi Yamada | From supermembrane to super Yang-Mills theory | 18 pages, typos corrected, to appear in Nucl. Phys. B | Nucl.Phys. B696 (2004) 36-54 | 10.1016/j.nuclphysb.2004.07.005 | DPNU-04-10 | hep-th | null | We derive p+1-dimensional (p=1,2) maximally supersymmetric U(N) Yang-Mills
theory from the wrapped supermembrane on $R^{11-p}\times T^{p}$ in the
light-cone gauge by using the matrix regularization. The elements of the
matrices in the super Yang-Mills theory are given by the Fourier coefficients
in the supermembrane ... | [
{
"created": "Wed, 5 May 2004 13:09:18 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Jul 2004 11:52:40 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Uehara",
"Shozo",
""
],
[
"Yamada",
"Satoshi",
""
]
] | We derive p+1-dimensional (p=1,2) maximally supersymmetric U(N) Yang-Mills theory from the wrapped supermembrane on $R^{11-p}\times T^{p}$ in the light-cone gauge by using the matrix regularization. The elements of the matrices in the super Yang-Mills theory are given by the Fourier coefficients in the supermembrane th... | 11.067052 | 9.395307 | 12.988927 | 9.047095 | 9.243855 | 8.962978 | 9.382504 | 9.13148 | 8.841022 | 13.702169 | 9.331592 | 9.24809 | 10.777416 | 9.61167 | 9.300061 | 9.442145 | 9.620101 | 8.964148 | 9.849958 | 10.597571 | 9.09073 |
0704.3667 | Martin B. Halpern | M.B.Halpern | The Orbifolds of Permutation-Type as Physical String Systems at
Multiples of c=26 IV. Orientation Orbifolds Include Orientifolds | 22 pages, typos corrected | Phys.Rev.D76:026004,2007 | 10.1103/PhysRevD.76.026004 | null | hep-th math-ph math.MP | null | In this fourth paper of the series, I clarify the somewhat mysterious
relation between the large class of {\it orientation orbifolds} (with twisted
open-string CFT's at $\hat c=52$) and {\it orientifolds} (with untwisted open
strings at $c=26$), both of which have been associated to division by
world-sheet orientatio... | [
{
"created": "Fri, 27 Apr 2007 06:44:54 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Jul 2007 05:55:15 GMT",
"version": "v2"
},
{
"created": "Mon, 31 Dec 2007 08:50:55 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Halpern",
"M. B.",
""
]
] | In this fourth paper of the series, I clarify the somewhat mysterious relation between the large class of {\it orientation orbifolds} (with twisted open-string CFT's at $\hat c=52$) and {\it orientifolds} (with untwisted open strings at $c=26$), both of which have been associated to division by world-sheet orientation-... | 16.426754 | 14.358491 | 16.621326 | 15.236409 | 15.287165 | 14.923454 | 16.502306 | 15.086924 | 14.664444 | 20.035553 | 15.514026 | 14.954841 | 15.585336 | 14.905283 | 15.564389 | 15.303104 | 14.627577 | 15.231477 | 15.550535 | 16.164398 | 14.821174 |
hep-th/0311176 | Manuel Asorey | M. Asorey | Vacuum energy and $\theta$--vacuum | 8 pages, 1 figure. Invited talk at "Renormalization Group and
Anomalies in Gravity and Cosmology", Ouro Preto,Brazil, March 17-23, 2003.v2:
Added references | null | 10.1016/S0920-5632(03)02395-8 | null | hep-th | null | The highly non-trivial structure of the $\theta$--vacuum encodes many of the
fundamental properties of gauge theories. In particular, the response of the
vacuum to the $\theta$--term perturbation is sensitive to the existence of
confinement, chiral symmetry breaking, etc. We analyze the dependence of the
vacuum energ... | [
{
"created": "Wed, 19 Nov 2003 20:32:14 GMT",
"version": "v1"
},
{
"created": "Thu, 18 Dec 2003 15:26:26 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Asorey",
"M.",
""
]
] | The highly non-trivial structure of the $\theta$--vacuum encodes many of the fundamental properties of gauge theories. In particular, the response of the vacuum to the $\theta$--term perturbation is sensitive to the existence of confinement, chiral symmetry breaking, etc. We analyze the dependence of the vacuum energy ... | 8.324315 | 8.203335 | 7.8461 | 7.74197 | 8.217815 | 8.5662 | 8.438663 | 7.925765 | 7.687064 | 9.305826 | 8.253479 | 7.998505 | 7.904051 | 7.750251 | 7.686848 | 7.711415 | 7.993655 | 7.880996 | 7.715036 | 7.876274 | 7.924753 |
hep-th/0603167 | David Dudal | M.A.L. Capri, D. Dudal, J.A. Gracey, V.E.R. Lemes, R.F. Sobreiro, S.P.
Sorella, R. Thibes, H. Verschelde | The infrared behavior of the gluon and ghost propagators in SU(2)
Yang-Mills theory in the maximal Abelian gauge | 6 pages. Talk given by S.P. Sorella at the "I Latin American Workshop
on High Energy Phenomenology (I LAWHEP)", December 1-3 2005, Instituto de
Fisica, UFRGS, Porto Alegre, Rio Grande Do Sul, Brasil | Braz.J.Phys.37:591-596,2007 | 10.1590/S0103-97332007000400019 | LTH-695 | hep-th | null | We report on some recent analytical results on the behaviour of the gluon and
ghost propagators in Euclidean SU(2) Yang-Mills theory quantized in the maximal
Abelian gauge (MAG). This gauge is of particular interest for the dual
superconductivity picture to explain color confinement. Two kinds of effects
are taken in... | [
{
"created": "Tue, 21 Mar 2006 13:48:01 GMT",
"version": "v1"
}
] | 2011-08-04 | [
[
"Capri",
"M. A. L.",
""
],
[
"Dudal",
"D.",
""
],
[
"Gracey",
"J. A.",
""
],
[
"Lemes",
"V. E. R.",
""
],
[
"Sobreiro",
"R. F.",
""
],
[
"Sorella",
"S. P.",
""
],
[
"Thibes",
"R.",
""
],
[
"Verschel... | We report on some recent analytical results on the behaviour of the gluon and ghost propagators in Euclidean SU(2) Yang-Mills theory quantized in the maximal Abelian gauge (MAG). This gauge is of particular interest for the dual superconductivity picture to explain color confinement. Two kinds of effects are taken into... | 5.88107 | 5.171124 | 6.174319 | 5.371342 | 5.489217 | 5.62909 | 5.273425 | 5.085348 | 5.147467 | 5.920774 | 5.118417 | 5.192414 | 5.694182 | 5.471828 | 5.556613 | 5.250521 | 5.397964 | 5.56315 | 5.453773 | 5.867378 | 5.350855 |
hep-th/0112254 | Vitor Cardoso | Vitor Cardoso, Jose' P. S. Lemos | Black hole collision with a scalar particle in three dimensional anti-de
Sitter spacetime | 5 pages, 3 figures;minor improvements; references added | Phys.Rev. D65 (2002) 104032 | 10.1103/PhysRevD.65.104032 | null | hep-th gr-qc | null | We study the collision between a BTZ black hole and a test particle coupled
to a scalar field. We compute the power spectrum, the energy radiated and the
plunging waveforms for this process. We show that for late times the signal is
dominated by the quasinormal ringing. In terms of the AdS/CFT correspondence
the bulk... | [
{
"created": "Sat, 29 Dec 2001 17:59:39 GMT",
"version": "v1"
},
{
"created": "Wed, 15 May 2002 13:12:10 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Cardoso",
"Vitor",
""
],
[
"Lemos",
"Jose' P. S.",
""
]
] | We study the collision between a BTZ black hole and a test particle coupled to a scalar field. We compute the power spectrum, the energy radiated and the plunging waveforms for this process. We show that for late times the signal is dominated by the quasinormal ringing. In terms of the AdS/CFT correspondence the bulk g... | 13.777308 | 13.966736 | 14.45543 | 12.717783 | 14.425851 | 13.715254 | 15.522232 | 12.839805 | 13.233308 | 13.981669 | 13.379217 | 12.955487 | 13.453209 | 13.20127 | 13.187641 | 13.100981 | 13.139094 | 12.891115 | 13.735238 | 13.563483 | 12.910078 |
2402.08176 | Muxin Han | Muxin Han | Representations of a quantum-deformed Lorentz algebra, Clebsch-Gordan
map, and Fenchel-Nielsen representation of quantum complex flat connections
at level-$k$ | 28 pages, 4 figures | null | null | null | hep-th gr-qc math-ph math.GT math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A family of infinite-dimensional irreducible $\star$-representations on
$\mathcal{H}\simeq L^2(\mathbb{R})\otimes\mathbb{C}^k$ is defined for a
quantum-deformed Lorentz algebra $U_\mathbf{q}(sl_2)\otimes
U_{\tilde{\mathbf{q}}}(sl_2)$, where $\mathbf{q}=\exp[\frac{2\pi i}{k}(1+b^2)]$
and $\tilde{\mathbf{q}}=\exp[\frac... | [
{
"created": "Tue, 13 Feb 2024 02:26:49 GMT",
"version": "v1"
}
] | 2024-02-15 | [
[
"Han",
"Muxin",
""
]
] | A family of infinite-dimensional irreducible $\star$-representations on $\mathcal{H}\simeq L^2(\mathbb{R})\otimes\mathbb{C}^k$ is defined for a quantum-deformed Lorentz algebra $U_\mathbf{q}(sl_2)\otimes U_{\tilde{\mathbf{q}}}(sl_2)$, where $\mathbf{q}=\exp[\frac{2\pi i}{k}(1+b^2)]$ and $\tilde{\mathbf{q}}=\exp[\frac{2... | 4.397627 | 5.176527 | 4.587462 | 4.614066 | 5.19509 | 5.27096 | 5.198983 | 4.90853 | 4.471842 | 4.73725 | 4.61174 | 4.632141 | 4.623964 | 4.413628 | 4.565556 | 4.603209 | 4.46027 | 4.51199 | 4.549231 | 4.677826 | 4.429895 |
1111.6660 | Lubomir Martinovic | Lubomir Martinovic | Exactly solvable models and spontaneous symmetry breaking | 6 pages, the author's contribution at LIGHTCONE 2011 conference,
Dallas, Texas, May 23-27, 2011 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a few two-dimensional models with massive and massless fermions in
the hamiltonian framework and in both conventional and light-front forms of
field theory. The new ingredient is a modification of the canonical procedure
by taking into account solutions of the operator field equations. After
summarizing the ... | [
{
"created": "Tue, 29 Nov 2011 01:26:52 GMT",
"version": "v1"
}
] | 2011-11-30 | [
[
"Martinovic",
"Lubomir",
""
]
] | We study a few two-dimensional models with massive and massless fermions in the hamiltonian framework and in both conventional and light-front forms of field theory. The new ingredient is a modification of the canonical procedure by taking into account solutions of the operator field equations. After summarizing the ma... | 11.313096 | 11.949652 | 11.874935 | 10.830993 | 10.770607 | 11.101462 | 11.315899 | 10.679945 | 10.391212 | 13.148423 | 10.131289 | 10.795102 | 11.489102 | 10.779832 | 11.058797 | 10.820271 | 10.555282 | 10.966311 | 10.887276 | 11.289542 | 10.664119 |
1605.08052 | Washington Taylor | Samuel B. Johnson and Washington Taylor | Enhanced gauge symmetry in 6D F-theory models and tuned elliptic
Calabi-Yau threefolds | 101 pages, 3 figures, 25 tables; v2: references added, some technical
corrections, minor typos corrected | null | 10.1002/prop.201600074 | MIT-CTP-4645 | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We systematically analyze the local combinations of gauge groups and matter
that can arise in 6D F-theory models over a fixed base. We compare the
low-energy constraints of anomaly cancellation to explicit F-theory
constructions using Weierstrass and Tate forms, and identify some new local
structures in the "swamplan... | [
{
"created": "Wed, 25 May 2016 20:00:05 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Jun 2016 00:13:14 GMT",
"version": "v2"
}
] | 2016-11-03 | [
[
"Johnson",
"Samuel B.",
""
],
[
"Taylor",
"Washington",
""
]
] | We systematically analyze the local combinations of gauge groups and matter that can arise in 6D F-theory models over a fixed base. We compare the low-energy constraints of anomaly cancellation to explicit F-theory constructions using Weierstrass and Tate forms, and identify some new local structures in the "swampland'... | 10.609346 | 11.899731 | 12.941289 | 10.960857 | 12.277606 | 12.086782 | 11.954722 | 11.476725 | 11.020124 | 15.214847 | 11.077918 | 10.949665 | 11.083231 | 10.737949 | 10.963047 | 10.672486 | 10.731013 | 10.641585 | 10.73845 | 11.536885 | 10.667976 |
hep-th/9311038 | Massimo Porrati | S. Ferrara, A. Masiero, M. Porrati and R. Stora | Bardeen-Anomaly and Wess-Zumino Term in the Supersymmetric Standard
Model | 21 pages, (plain TeX), CERN.TH-6845/93, DFPD 93/TH/32,
UCLA/93/TEP/13, NYU-TH-93/10/01, ENSLAPP-A442/93 | Nucl.Phys. B417 (1994) 238-256 | 10.1016/0550-3213(94)90545-2 | null | hep-th hep-ph | null | We construct the Bardeen anomaly and its related Wess-Zumino term in the
supersymmetric standard model. In particular we show that it can be written in
terms of a composite linear superfield related to supersymmetrized Chern-Simons
forms, in very much the same way as the Green-Schwarz term in four-dimensional
string ... | [
{
"created": "Fri, 5 Nov 1993 21:29:57 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ferrara",
"S.",
""
],
[
"Masiero",
"A.",
""
],
[
"Porrati",
"M.",
""
],
[
"Stora",
"R.",
""
]
] | We construct the Bardeen anomaly and its related Wess-Zumino term in the supersymmetric standard model. In particular we show that it can be written in terms of a composite linear superfield related to supersymmetrized Chern-Simons forms, in very much the same way as the Green-Schwarz term in four-dimensional string th... | 9.130943 | 8.891178 | 9.266791 | 8.630657 | 8.582156 | 8.820803 | 8.594515 | 8.836275 | 8.442686 | 10.555515 | 8.85575 | 8.757051 | 8.616358 | 8.691534 | 9.33734 | 8.880553 | 8.799841 | 9.005358 | 8.328233 | 9.33817 | 8.657144 |
0806.3255 | Matthias Blau | Matthias Blau, Martin O'Loughlin | DLCQ and Plane Wave Matrix Big Bang Models | 29 pages, v2: reference added + minor cosmetic corrections | JHEP 0809:097,2008 | 10.1088/1126-6708/2008/09/097 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the generalisations of the Craps-Sethi-Verlinde matrix big bang
model to curved, in particular plane wave, space-times, beginning with a
careful discussion of the DLCQ procedure. Singular homogeneous plane waves are
ideal toy-models of realistic space-time singularities since they have been
shown to arise un... | [
{
"created": "Thu, 19 Jun 2008 18:04:04 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Aug 2008 12:45:48 GMT",
"version": "v2"
}
] | 2011-06-02 | [
[
"Blau",
"Matthias",
""
],
[
"O'Loughlin",
"Martin",
""
]
] | We study the generalisations of the Craps-Sethi-Verlinde matrix big bang model to curved, in particular plane wave, space-times, beginning with a careful discussion of the DLCQ procedure. Singular homogeneous plane waves are ideal toy-models of realistic space-time singularities since they have been shown to arise univ... | 16.018307 | 14.95858 | 15.722655 | 14.881223 | 15.6551 | 14.992861 | 15.093489 | 15.867498 | 14.349313 | 16.759274 | 17.465319 | 14.103407 | 14.450402 | 13.33307 | 13.800054 | 14.038674 | 14.187596 | 13.893894 | 13.719243 | 14.054605 | 13.869037 |
hep-th/0508089 | Herman Verlinde | Herman Verlinde and Martijn Wijnholt | Building the Standard Model on a D3-brane | 37 pages, 9 figures | JHEP 0701:106,2007 | 10.1088/1126-6708/2007/01/106 | PUPT-2165 | hep-th | null | We motivate and apply a bottom-up approach to string phenomenology, which
aims to construct the Standard Model as a decoupled world-volume theory on a
D3-brane. As a concrete proposal for such a construction, we consider a single
probe D3-brane on a partial resolution of a del Pezzo 8 singularity. The
resulting world... | [
{
"created": "Fri, 12 Aug 2005 19:27:47 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Aug 2005 23:45:34 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Verlinde",
"Herman",
""
],
[
"Wijnholt",
"Martijn",
""
]
] | We motivate and apply a bottom-up approach to string phenomenology, which aims to construct the Standard Model as a decoupled world-volume theory on a D3-brane. As a concrete proposal for such a construction, we consider a single probe D3-brane on a partial resolution of a del Pezzo 8 singularity. The resulting world-v... | 7.586394 | 7.37563 | 7.712906 | 6.769842 | 7.233783 | 7.222142 | 7.110429 | 7.181808 | 6.678227 | 8.329003 | 6.940428 | 6.771092 | 7.283059 | 6.91243 | 6.799067 | 6.948807 | 6.888319 | 6.608489 | 6.819311 | 7.02786 | 6.9363 |
1803.05452 | Henrik Johansson | Thales Azevedo, Marco Chiodaroli, Henrik Johansson and Oliver
Schlotterer | Heterotic and bosonic string amplitudes via field theory | 38+5 pages | null | 10.1007/JHEP10(2018)012 | UUITP-07/18, NORDITA-2018-020 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Previous work has shown that massless tree amplitudes of the type I and IIA/B
superstrings can be dramatically simplified by expressing them as double copies
between field-theory amplitudes and scalar disk/sphere integrals, the latter
containing all the $\alpha'$-corrections. In this work, we pinpoint similar
double-... | [
{
"created": "Wed, 14 Mar 2018 18:02:05 GMT",
"version": "v1"
}
] | 2018-11-14 | [
[
"Azevedo",
"Thales",
""
],
[
"Chiodaroli",
"Marco",
""
],
[
"Johansson",
"Henrik",
""
],
[
"Schlotterer",
"Oliver",
""
]
] | Previous work has shown that massless tree amplitudes of the type I and IIA/B superstrings can be dramatically simplified by expressing them as double copies between field-theory amplitudes and scalar disk/sphere integrals, the latter containing all the $\alpha'$-corrections. In this work, we pinpoint similar double-co... | 8.4306 | 9.204779 | 10.734475 | 8.737216 | 8.671889 | 8.464519 | 8.148265 | 8.196285 | 8.591499 | 11.318106 | 8.193355 | 7.990925 | 9.023966 | 8.024896 | 7.735174 | 7.632782 | 8.045375 | 7.817514 | 8.105885 | 9.360936 | 8.219658 |
0802.2956 | Christopher Herzog | Christopher P. Herzog, Stefan A. Stricker, Aleksi Vuorinen | Remarks on Heavy-Light Mesons from AdS/CFT | 29 pages, 9 figures; v2 section 5 rewritten to include discussion of
long strings, other minor improvements, ref added | JHEP 0805:070,2008 | 10.1088/1126-6708/2008/05/070 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the AdS/CFT correspondence to compute the energy spectrum of
heavy-light mesons in a N=2 SU(N) super Yang-Mills theory with two massive
hypermultiplets. In the heavy quark limit, similar to QCD, we find that the
excitation energies are independent of the heavy quark mass. We also make some
remarks about relate... | [
{
"created": "Wed, 20 Feb 2008 22:36:46 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Mar 2008 21:21:42 GMT",
"version": "v2"
}
] | 2009-01-06 | [
[
"Herzog",
"Christopher P.",
""
],
[
"Stricker",
"Stefan A.",
""
],
[
"Vuorinen",
"Aleksi",
""
]
] | We use the AdS/CFT correspondence to compute the energy spectrum of heavy-light mesons in a N=2 SU(N) super Yang-Mills theory with two massive hypermultiplets. In the heavy quark limit, similar to QCD, we find that the excitation energies are independent of the heavy quark mass. We also make some remarks about related ... | 6.269819 | 5.644007 | 6.429886 | 5.322608 | 5.750004 | 5.573571 | 5.311732 | 5.945775 | 5.365263 | 6.56092 | 5.357042 | 5.448781 | 5.889128 | 5.528864 | 5.5879 | 5.665394 | 5.477916 | 5.54208 | 5.466273 | 6.160962 | 5.702216 |
2201.12232 | Sergey Derkachov | S. Derkachov, A.P. Isaev, L. Shumilov | Conformal Triangles and Zig-Zag Diagrams | null | null | 10.1016/j.physletb.2022.137150 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | A convenient integral representation for zig-zag four-point and two-point
planar Feynman diagrams relevant to the bi-scalar D-dimensional fishnet field
theory is obtained. This representation gives a possibility to evaluate exactly
diagrams of the zig-zag series in special cases. In particular, we give a
fairly simpl... | [
{
"created": "Fri, 28 Jan 2022 16:39:12 GMT",
"version": "v1"
},
{
"created": "Sat, 26 Mar 2022 19:23:01 GMT",
"version": "v2"
}
] | 2022-05-11 | [
[
"Derkachov",
"S.",
""
],
[
"Isaev",
"A. P.",
""
],
[
"Shumilov",
"L.",
""
]
] | A convenient integral representation for zig-zag four-point and two-point planar Feynman diagrams relevant to the bi-scalar D-dimensional fishnet field theory is obtained. This representation gives a possibility to evaluate exactly diagrams of the zig-zag series in special cases. In particular, we give a fairly simple ... | 13.894299 | 12.606554 | 15.381687 | 12.394422 | 12.634032 | 12.105077 | 11.133357 | 12.790777 | 12.020024 | 14.212253 | 11.484213 | 11.656725 | 12.485186 | 11.920514 | 12.280663 | 12.306509 | 12.058758 | 12.343361 | 11.978311 | 12.587753 | 12.786128 |
2202.05781 | Nicol\'as Grandi | Jos\'e D. Edelstein, Nicol\'as Grandi, Alberto Rivadulla S\'anchez | Holographic superconductivity in Einsteinian Cubic Gravity | 19 pages, 8 figures, replaced by revised version with minor
correeections | J. High Energ. Phys. 2022, 188 (2022) | 10.1007/JHEP05(2022)188 | null | hep-th cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the condensation of a charged scalar field in a $(3+1)$-dimensional
asymptotically AdS background in the context of Einsteinian cubic gravity,
featuring a holographic superconductor with higher curvature corrections
corresponding to a CFT with a non-vanishing value of the stress tensor
three-point function $... | [
{
"created": "Fri, 11 Feb 2022 17:24:33 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Feb 2022 16:10:32 GMT",
"version": "v2"
}
] | 2022-06-14 | [
[
"Edelstein",
"José D.",
""
],
[
"Grandi",
"Nicolás",
""
],
[
"Sánchez",
"Alberto Rivadulla",
""
]
] | We study the condensation of a charged scalar field in a $(3+1)$-dimensional asymptotically AdS background in the context of Einsteinian cubic gravity, featuring a holographic superconductor with higher curvature corrections corresponding to a CFT with a non-vanishing value of the stress tensor three-point function $t_... | 7.413842 | 6.715197 | 7.598095 | 6.836847 | 6.544626 | 6.856593 | 7.149124 | 6.332791 | 6.71808 | 7.716144 | 6.138647 | 6.919932 | 7.098726 | 6.833951 | 6.829768 | 6.895931 | 6.732244 | 6.858964 | 6.924393 | 7.44683 | 6.69481 |
hep-th/9206038 | null | Gerald Dunne and Nuria Rius | A Comment on the Relationship Between Differential and Dimensional
Renormalization | null | Phys.Lett. B293 (1992) 367-374 | 10.1016/0370-2693(92)90897-D | null | hep-th | null | We show that there is a very simple relationship between differential and
dimensional renormalization of low-order Feynman graphs in renormalizable
massless quantum field theories. The beauty of the differential approach is
that it achieves the same finite results as dimensional renormalization without
the need to mo... | [
{
"created": "Tue, 9 Jun 1992 17:32:05 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dunne",
"Gerald",
""
],
[
"Rius",
"Nuria",
""
]
] | We show that there is a very simple relationship between differential and dimensional renormalization of low-order Feynman graphs in renormalizable massless quantum field theories. The beauty of the differential approach is that it achieves the same finite results as dimensional renormalization without the need to modi... | 11.275682 | 9.619685 | 10.106806 | 9.215954 | 9.631367 | 9.41069 | 9.481584 | 8.780443 | 9.570269 | 11.662173 | 9.208379 | 10.128422 | 10.213313 | 9.383433 | 9.973078 | 10.24199 | 9.689502 | 10.619025 | 9.930347 | 10.102623 | 9.300215 |
2203.05491 | Debarshi Basu | Debarshi Basu | Balanced Partial Entanglement in Flat Holography | 25 pages, 3 figures; v2: minor modifications, typos corrected,
references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We advance a construction for the balanced partial entanglement entropy (BPE)
for bipartite mixed states in a class of $(1+1)$-dimensional Galilean conformal
field theories dual to Einstein gravity and topologically massive gravity in
asymptotically flat spacetimes. We compare our results with the entanglement
wedge ... | [
{
"created": "Thu, 10 Mar 2022 17:21:15 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Mar 2022 18:26:27 GMT",
"version": "v2"
}
] | 2022-03-22 | [
[
"Basu",
"Debarshi",
""
]
] | We advance a construction for the balanced partial entanglement entropy (BPE) for bipartite mixed states in a class of $(1+1)$-dimensional Galilean conformal field theories dual to Einstein gravity and topologically massive gravity in asymptotically flat spacetimes. We compare our results with the entanglement wedge cr... | 7.395099 | 4.753788 | 8.721086 | 5.553698 | 5.207141 | 4.91888 | 5.048866 | 5.065518 | 5.368436 | 9.345627 | 5.439134 | 6.077004 | 7.725134 | 6.614578 | 6.447503 | 6.375756 | 6.065563 | 6.683503 | 6.413462 | 7.88464 | 6.20855 |
hep-th/0202179 | null | J.G. Russo and A.A. Tseytlin | On solvable models of type IIB superstring in NS-NS and R-R plane wave
backgrounds | 36 pages, harvmac. v2: discussion of equivalence of the supergravity
parts of the spectra of the NS-NS and R-R models added in sect.5.3; v3: added
remark on periodicity of the NS-NS spectrum; v4: minor correction in sect.6.2 | JHEP 0204:021,2002 | 10.1088/1126-6708/2002/04/021 | null | hep-th | null | We consider type IIB string in the two plane-wave backgrounds which may be
interpreted as special limits of the AdS_3 x S^3 metric supported by either the
NS-NS or R-R 3-form field. The NS-NS plane-wave string model is equivalent to a
direct generalization of the Nappi-Witten model, with its spectrum being
similar to... | [
{
"created": "Tue, 26 Feb 2002 20:59:00 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Feb 2002 20:53:54 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Mar 2002 19:51:29 GMT",
"version": "v3"
},
{
"created": "Sun, 24 Mar 2002 16:24:15 GMT",
"version": "v4"
}
] | 2009-11-07 | [
[
"Russo",
"J. G.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We consider type IIB string in the two plane-wave backgrounds which may be interpreted as special limits of the AdS_3 x S^3 metric supported by either the NS-NS or R-R 3-form field. The NS-NS plane-wave string model is equivalent to a direct generalization of the Nappi-Witten model, with its spectrum being similar to t... | 8.512349 | 7.574462 | 9.685885 | 7.786042 | 7.83565 | 8.006526 | 7.909588 | 8.068631 | 7.902987 | 10.176064 | 7.858072 | 7.950471 | 8.738922 | 7.974309 | 8.194265 | 8.096482 | 8.085954 | 8.094026 | 8.190277 | 8.7587 | 8.095949 |
hep-th/9502138 | Paul Montague | P.S. Montague | Third and Higher Order NFPA Twisted Constructions of Conformal Field
Theories from Lattices | LaTeX 46 pages | Nucl.Phys.B441:337-382,1995 | 10.1016/0550-3213(95)00115-9 | null | hep-th | null | We investigate orbifold constructions of conformal field theories from
lattices by no-fixed-point automorphisms (NFPA's) $Z_p$ for $p$ prime, $p>2$,
concentrating on the case $p=3$. Explicit expressions are given for most of the
relevant vertex operators, and we consider the locality relations necessary for
these to ... | [
{
"created": "Fri, 24 Feb 1995 05:11:15 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Montague",
"P. S.",
""
]
] | We investigate orbifold constructions of conformal field theories from lattices by no-fixed-point automorphisms (NFPA's) $Z_p$ for $p$ prime, $p>2$, concentrating on the case $p=3$. Explicit expressions are given for most of the relevant vertex operators, and we consider the locality relations necessary for these to de... | 11.281854 | 10.323613 | 13.588658 | 10.731033 | 10.311686 | 10.75582 | 12.339267 | 10.585755 | 10.356263 | 13.822079 | 10.627421 | 10.858785 | 12.208139 | 10.947418 | 10.509518 | 10.522458 | 11.307967 | 10.933737 | 10.762387 | 12.169993 | 10.769446 |
0911.3380 | Xingang Chen | Xingang Chen, Yi Wang | Quasi-Single Field Inflation and Non-Gaussianities | 56 pages, v4, minor revision with added comments, JCAP version | JCAP 1004:027,2010 | 10.1088/1475-7516/2010/04/027 | null | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In quasi-single field inflation models, massive isocurvature modes, that are
coupled to the inflaton and have mass of order the Hubble parameter, can have
nontrivial impacts on density perturbations, especially non-Gaussianities. We
study a simple example of quasi-single field inflation in terms of turning
inflaton t... | [
{
"created": "Tue, 17 Nov 2009 19:20:45 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Nov 2009 00:56:43 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Feb 2010 16:18:33 GMT",
"version": "v3"
},
{
"created": "Sat, 24 Apr 2010 15:03:29 GMT",
"version": "v4"
}
] | 2010-05-07 | [
[
"Chen",
"Xingang",
""
],
[
"Wang",
"Yi",
""
]
] | In quasi-single field inflation models, massive isocurvature modes, that are coupled to the inflaton and have mass of order the Hubble parameter, can have nontrivial impacts on density perturbations, especially non-Gaussianities. We study a simple example of quasi-single field inflation in terms of turning inflaton tra... | 12.405052 | 12.686272 | 12.505219 | 11.536307 | 11.548842 | 12.156066 | 12.431089 | 12.213766 | 11.728954 | 13.965851 | 12.140011 | 11.577602 | 11.340935 | 11.039865 | 11.523805 | 12.1644 | 11.54025 | 11.292532 | 11.283216 | 12.654432 | 11.33041 |
hep-th/0406209 | Theodora Ioannidou Dr | Yves Brihaye and Theodora Ioannidou | SU(5) Gravitating Monopoles | 12 pages, 3 Figures | Class.Quant.Grav.22:1077-1086,2005 | 10.1088/0264-9381/22/6/010 | null | hep-th | null | Spherically symmetric solutions of the SU(5) Einstein-Yang-Mills-Higgs system
are constructed using the harmonic map ansatz \cite{IS}. This way the problem
reduces to solving a set of ordinary differential equations for the appropriate
profile functions.
| [
{
"created": "Wed, 23 Jun 2004 13:36:08 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Brihaye",
"Yves",
""
],
[
"Ioannidou",
"Theodora",
""
]
] | Spherically symmetric solutions of the SU(5) Einstein-Yang-Mills-Higgs system are constructed using the harmonic map ansatz \cite{IS}. This way the problem reduces to solving a set of ordinary differential equations for the appropriate profile functions. | 8.902272 | 6.205128 | 7.060796 | 6.399415 | 6.34347 | 6.764752 | 5.924405 | 5.985569 | 6.121287 | 7.221533 | 6.897272 | 6.128815 | 6.901539 | 6.433619 | 6.328523 | 6.501235 | 6.45571 | 6.313114 | 6.297638 | 6.659503 | 6.526619 |
hep-th/9602075 | Ahmed Hindawi | Ahmed Hindawi, Burt A. Ovrut, Daniel Waldram | Soft Supersymmetry Breaking Induced by Higher-Derivative
Supergravitation in the Electroweak Standard Model | LaTeX2e with AMS-LaTeX 1.2, 13 pages | Phys.Lett. B381 (1996) 154-162 | 10.1016/0370-2693(96)00549-7 | UPR-691T | hep-th hep-ph | null | We show how spontaneous supersymmetry breaking in the vacuum state of
higher-derivative supergravity is transmitted, as explicit soft
supersymmetry-breaking terms, to the effective Lagrangian of the standard
electroweak model. The general structure of the soft supersymmetry breaking
terms is presented and a new scena... | [
{
"created": "Thu, 15 Feb 1996 00:51:59 GMT",
"version": "v1"
},
{
"created": "Sun, 29 Dec 1996 00:23:16 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Hindawi",
"Ahmed",
""
],
[
"Ovrut",
"Burt A.",
""
],
[
"Waldram",
"Daniel",
""
]
] | We show how spontaneous supersymmetry breaking in the vacuum state of higher-derivative supergravity is transmitted, as explicit soft supersymmetry-breaking terms, to the effective Lagrangian of the standard electroweak model. The general structure of the soft supersymmetry breaking terms is presented and a new scenari... | 8.803081 | 8.323403 | 7.497329 | 8.146766 | 7.581166 | 7.576083 | 7.695411 | 8.492519 | 7.466441 | 8.102482 | 7.96905 | 8.397195 | 7.714893 | 8.122355 | 8.026537 | 8.217903 | 8.045733 | 8.30411 | 7.98985 | 7.53314 | 7.822118 |
2312.13267 | Ricardo Monteiro | George Doran, Ricardo Monteiro, Sam Wikeley | On the anomaly interpretation of amplitudes in self-dual Yang-Mills and
gravity | 41 pages, 2 figures. v2: published version with substantial
improvements, including new section 4 | null | null | QMUL-PH-23-26, UUITP--38/23 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We investigate the integrability anomalies arising in the self-dual sectors
of gravity and Yang-Mills theory, focusing on their connection to both the
chiral anomaly and the trace anomaly. The anomalies in the self-dual sectors
generate the one-loop all-plus amplitudes of gravitons and gluons, and have
recently been ... | [
{
"created": "Wed, 20 Dec 2023 18:47:55 GMT",
"version": "v1"
},
{
"created": "Thu, 13 Jun 2024 14:03:16 GMT",
"version": "v2"
}
] | 2024-06-14 | [
[
"Doran",
"George",
""
],
[
"Monteiro",
"Ricardo",
""
],
[
"Wikeley",
"Sam",
""
]
] | We investigate the integrability anomalies arising in the self-dual sectors of gravity and Yang-Mills theory, focusing on their connection to both the chiral anomaly and the trace anomaly. The anomalies in the self-dual sectors generate the one-loop all-plus amplitudes of gravitons and gluons, and have recently been st... | 7.79732 | 7.806508 | 8.408657 | 7.771385 | 7.92302 | 8.057825 | 7.574264 | 7.579348 | 7.570606 | 8.795693 | 7.864246 | 7.77727 | 7.984078 | 7.791732 | 7.840178 | 7.76801 | 7.850932 | 7.821814 | 7.907599 | 7.955659 | 7.680106 |
hep-th/0311268 | Alexandre C. Tort | A A Bytsenko, V S Mendes and A C Tort | Thermodynamics of Abelian Gauge Fields in Real Hyperbolic Spaces | Six pages, Revtex4 style, no figures; small typo corrected | Int.J.Mod.Phys. A20 (2005) 2847-2857 | 10.1142/S0217751X05020823 | null | hep-th | null | We work with $N-$dimensional compact real hyperbolic space $X_{\Gamma}$ with
universal covering $M$ and fundamental group $\Gamma$. Therefore, $M$ is the
symmetric space $G/K$, where $G=SO_1(N,1)$ and $K=SO(N)$ is a maximal compact
subgroup of $G$. We regard $\Gamma$ as a discrete subgroup of $G$ acting
isometrically... | [
{
"created": "Thu, 27 Nov 2003 16:48:53 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Dec 2003 14:30:28 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Bytsenko",
"A A",
""
],
[
"Mendes",
"V S",
""
],
[
"Tort",
"A C",
""
]
] | We work with $N-$dimensional compact real hyperbolic space $X_{\Gamma}$ with universal covering $M$ and fundamental group $\Gamma$. Therefore, $M$ is the symmetric space $G/K$, where $G=SO_1(N,1)$ and $K=SO(N)$ is a maximal compact subgroup of $G$. We regard $\Gamma$ as a discrete subgroup of $G$ acting isometrically o... | 7.765741 | 8.588063 | 8.382024 | 7.621193 | 8.340547 | 8.449688 | 8.419461 | 8.259312 | 7.727931 | 8.928889 | 7.781321 | 7.545996 | 7.734068 | 7.632179 | 7.51316 | 7.527102 | 7.773008 | 7.672242 | 7.601208 | 7.918834 | 7.42483 |
1111.1828 | Neil Copland | Neil B. Copland | A Double Sigma Model for Double Field Theory | 26 pages, v1: 37 pages, v2: references added, v3: updated to match
published version - background and detail of calculations substantially
condensed, motivation expanded, refs added, results unchanged | Journal of High Energy Physics, 2012, Volume 2012, Number 4, 44 | 10.1007/JHEP04(2012)044 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We define a sigma model with doubled target space and calculate its
background field equations. These coincide with generalised metric equation of
motion of double field theory, thus the double field theory is the effective
field theory for the sigma model.
| [
{
"created": "Tue, 8 Nov 2011 08:42:58 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Nov 2011 06:37:44 GMT",
"version": "v2"
},
{
"created": "Thu, 26 Apr 2012 01:14:11 GMT",
"version": "v3"
}
] | 2012-04-27 | [
[
"Copland",
"Neil B.",
""
]
] | We define a sigma model with doubled target space and calculate its background field equations. These coincide with generalised metric equation of motion of double field theory, thus the double field theory is the effective field theory for the sigma model. | 12.540723 | 10.65088 | 14.22748 | 9.722754 | 10.365975 | 9.740378 | 11.572392 | 9.616883 | 9.1803 | 14.476361 | 10.700042 | 10.023374 | 12.894353 | 9.96594 | 9.88868 | 9.65846 | 10.32997 | 9.995293 | 10.396488 | 13.652031 | 9.464375 |
hep-th/0202072 | Oleg Lunin | Oleg Lunin, Samir D. Mathur | Statistical interpretation of Bekenstein entropy for systems with a
stretched horizon | 4 pages, 3 figures, Revtex; comment added in the discussion | Phys.Rev.Lett. 88 (2002) 211303 | 10.1103/PhysRevLett.88.211303 | OHSTPY-HEP-T-02-002 | hep-th gr-qc | null | For the 2-charge extremal holes in string theory we show that the Bekenstein
entropy obtained from the area of the stretched horizon has a statistical
interpretation as a `coarse graining entropy': different microstates give
geometries that differ near r=0 and the stretched horizon cuts off the metric
at r=b where th... | [
{
"created": "Mon, 11 Feb 2002 19:59:12 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Feb 2002 19:04:48 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Lunin",
"Oleg",
""
],
[
"Mathur",
"Samir D.",
""
]
] | For the 2-charge extremal holes in string theory we show that the Bekenstein entropy obtained from the area of the stretched horizon has a statistical interpretation as a `coarse graining entropy': different microstates give geometries that differ near r=0 and the stretched horizon cuts off the metric at r=b where thes... | 20.797478 | 16.7341 | 19.427361 | 14.150511 | 17.274065 | 16.330013 | 13.856697 | 16.71332 | 15.254024 | 22.614164 | 15.92682 | 14.467456 | 15.646993 | 14.690878 | 13.786892 | 14.305975 | 14.819895 | 14.293895 | 14.784748 | 14.754616 | 15.795238 |
0706.2294 | Niko Jokela | Kari Enqvist, Niko Jokela, Esko Keski-Vakkuri, Lotta Mether | On the origin of thermal string gas | 16 pages, 4 figures, v2: references added | JCAP 0710:001,2007 | 10.1088/1475-7516/2007/10/001 | HIP-2007-34/TH | hep-th astro-ph gr-qc | null | We investigate decaying D-branes as the origin of the thermal string gas of
string gas cosmology. We consider initial configurations of low-dimensional
branes and argue that they can time evolve to thermal string gas. We find that
there is a range in the weak string coupling and fast brane decay time regimes,
where t... | [
{
"created": "Fri, 15 Jun 2007 13:42:27 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Sep 2007 09:05:38 GMT",
"version": "v2"
}
] | 2009-11-18 | [
[
"Enqvist",
"Kari",
""
],
[
"Jokela",
"Niko",
""
],
[
"Keski-Vakkuri",
"Esko",
""
],
[
"Mether",
"Lotta",
""
]
] | We investigate decaying D-branes as the origin of the thermal string gas of string gas cosmology. We consider initial configurations of low-dimensional branes and argue that they can time evolve to thermal string gas. We find that there is a range in the weak string coupling and fast brane decay time regimes, where the... | 23.36783 | 20.475336 | 25.001223 | 20.272333 | 21.245325 | 20.123859 | 19.671156 | 22.015753 | 19.539211 | 27.24897 | 17.969616 | 22.097425 | 20.588572 | 19.312895 | 20.470612 | 20.442329 | 20.488489 | 21.458481 | 20.423403 | 21.568451 | 19.843102 |
0708.2950 | Anirban Basu | Anirban Basu | The D^4 R^4 term in type IIB string theory on T^2 and U-duality | 25 pages, LaTeX | Phys.Rev.D77:106003,2008 | 10.1103/PhysRevD.77.106003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a manifestly U-duality invariant modular form for the D^4 R^4
interaction in type IIB string theory compactified on T^2. It receives
perturbative contributions upto two loops, and non-perturbative contributions
from D-instantons and (p,q) string instantons wrapping T^2. We provide evidence
for this modular... | [
{
"created": "Wed, 22 Aug 2007 02:56:52 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Aug 2008 14:27:43 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Basu",
"Anirban",
""
]
] | We propose a manifestly U-duality invariant modular form for the D^4 R^4 interaction in type IIB string theory compactified on T^2. It receives perturbative contributions upto two loops, and non-perturbative contributions from D-instantons and (p,q) string instantons wrapping T^2. We provide evidence for this modular f... | 6.304487 | 4.548616 | 7.710699 | 5.010685 | 4.834199 | 4.791211 | 4.642253 | 5.11601 | 4.891806 | 7.424612 | 5.11666 | 5.488478 | 6.470464 | 5.583714 | 5.504314 | 5.694347 | 5.677474 | 5.679217 | 5.607791 | 6.487874 | 5.7669 |
1305.6737 | Jan Rosseel | Roel Andringa, Eric A. Bergshoeff, Jan Rosseel and Ergin Sezgin | Newton-Cartan Supergravity | 24 pages, v2 : references added | null | 10.1088/0264-9381/30/20/205005 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a supersymmetric extension of three-dimensional Newton-Cartan
gravity by gauging a super-Bargmann algebra. In order to obtain a non-trivial
supersymmetric extension of the Bargmann algebra one needs at least two
supersymmetries leading to a N=2 super-Bargmann algebra. Due to the fact that
there is a univ... | [
{
"created": "Wed, 29 May 2013 09:23:39 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Jun 2013 16:39:49 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Andringa",
"Roel",
""
],
[
"Bergshoeff",
"Eric A.",
""
],
[
"Rosseel",
"Jan",
""
],
[
"Sezgin",
"Ergin",
""
]
] | We construct a supersymmetric extension of three-dimensional Newton-Cartan gravity by gauging a super-Bargmann algebra. In order to obtain a non-trivial supersymmetric extension of the Bargmann algebra one needs at least two supersymmetries leading to a N=2 super-Bargmann algebra. Due to the fact that there is a univer... | 7.554088 | 7.591964 | 7.486607 | 7.101192 | 7.589597 | 7.661708 | 7.474176 | 7.037104 | 6.955513 | 7.343609 | 6.724543 | 7.275758 | 7.388405 | 7.054837 | 7.557669 | 7.279782 | 7.090815 | 6.897978 | 7.312357 | 7.693949 | 7.247813 |
2109.03826 | Sandipan Kundu | Sandipan Kundu | Subleading Bounds on Chaos | 35 pages, 5 figures; In v2 it has been clarified that the MSS bound
and its generalizations can be derived from a weaker factorization assumption | null | 10.1007/JHEP04(2022)010 | null | hep-th cond-mat.stat-mech gr-qc nlin.CD quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Chaos, in quantum systems, can be diagnosed by certain out-of-time-order
correlators (OTOCs) that obey the chaos bound of Maldacena, Shenker, and
Stanford (MSS). We begin by deriving a dispersion relation for this class of
OTOCs, implying that they must satisfy many more constraints beyond the MSS
bound. Motivated by... | [
{
"created": "Wed, 8 Sep 2021 18:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Dec 2021 22:06:19 GMT",
"version": "v2"
}
] | 2022-04-20 | [
[
"Kundu",
"Sandipan",
""
]
] | Chaos, in quantum systems, can be diagnosed by certain out-of-time-order correlators (OTOCs) that obey the chaos bound of Maldacena, Shenker, and Stanford (MSS). We begin by deriving a dispersion relation for this class of OTOCs, implying that they must satisfy many more constraints beyond the MSS bound. Motivated by t... | 7.439673 | 7.694369 | 7.775676 | 6.961689 | 7.368526 | 7.463837 | 7.691313 | 7.365138 | 7.484422 | 7.999929 | 6.92315 | 6.954855 | 7.149615 | 7.028723 | 7.063701 | 7.152266 | 7.030247 | 6.906779 | 6.901746 | 7.149109 | 6.941379 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.