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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1306.2962 | Song He | Freddy Cachazo, Song He, Ellis Ye Yuan | Scattering in Three Dimensions from Rational Maps | 21 pages | null | 10.1007/JHEP10(2013)141 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complete tree-level S-matrix of four dimensional ${\cal N}=4$ super
Yang-Mills and ${\cal N} = 8$ supergravity has compact forms as integrals over
the moduli space of certain rational maps. In this note we derive formulas for
amplitudes in three dimensions by using the fact that when amplitudes are
dressed with p... | [
{
"created": "Wed, 12 Jun 2013 20:05:27 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Cachazo",
"Freddy",
""
],
[
"He",
"Song",
""
],
[
"Yuan",
"Ellis Ye",
""
]
] | The complete tree-level S-matrix of four dimensional ${\cal N}=4$ super Yang-Mills and ${\cal N} = 8$ supergravity has compact forms as integrals over the moduli space of certain rational maps. In this note we derive formulas for amplitudes in three dimensions by using the fact that when amplitudes are dressed with pro... | 10.606729 | 9.882185 | 11.656797 | 9.867048 | 10.641106 | 10.199983 | 11.110937 | 10.202174 | 10.235824 | 12.582277 | 9.593744 | 9.885719 | 10.783326 | 10.016912 | 10.274136 | 10.126013 | 10.144918 | 9.89652 | 10.111209 | 10.739593 | 9.991252 |
hep-th/0005057 | Martin Porrmann | Martin Porrmann | The Concept of Particle Weights in Local Quantum Field Theory | PhD thesis, 124 pages, amslatex, mathptm | null | null | null | hep-th math-ph math.MP | null | The concept of particle weights has been introduced by Buchholz and the
author in order to obtain a unified treatment of particles as well as (charged)
infraparticles which do not permit a definition of mass and spin according to
Wigner's theory. Particle weights arise as temporal limits of physical states
in the vac... | [
{
"created": "Sat, 6 May 2000 13:30:57 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Porrmann",
"Martin",
""
]
] | The concept of particle weights has been introduced by Buchholz and the author in order to obtain a unified treatment of particles as well as (charged) infraparticles which do not permit a definition of mass and spin according to Wigner's theory. Particle weights arise as temporal limits of physical states in the vacuu... | 13.810332 | 14.945244 | 15.744847 | 14.378798 | 14.805642 | 15.227783 | 15.47707 | 14.546207 | 15.698376 | 16.212395 | 14.752312 | 13.880925 | 14.119863 | 13.694452 | 13.667021 | 13.656438 | 13.559176 | 13.711654 | 13.834046 | 14.035806 | 14.159036 |
1603.01105 | Luis E. Oxman | L. E. Oxman, D. Vercauteren | Exploring center vortices in SU(2) and SU(3) relativistic
Yang-Mills-Higgs models | 25 pages, 5 figures | null | 10.1103/PhysRevD.95.025001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop numerical tools and apply them to solve the relativistic
Yang--Mills--Higgs equations in a model where the SU(N) symmetry is
spontaneously broken to its center. In SU(2) and SU(3), we obtain the different
field profiles for infinite and finite center vortices, with endpoints at
external monopole sources. E... | [
{
"created": "Thu, 3 Mar 2016 14:05:58 GMT",
"version": "v1"
}
] | 2017-02-01 | [
[
"Oxman",
"L. E.",
""
],
[
"Vercauteren",
"D.",
""
]
] | We develop numerical tools and apply them to solve the relativistic Yang--Mills--Higgs equations in a model where the SU(N) symmetry is spontaneously broken to its center. In SU(2) and SU(3), we obtain the different field profiles for infinite and finite center vortices, with endpoints at external monopole sources. Exp... | 18.274752 | 16.840246 | 17.693676 | 14.921888 | 16.328114 | 17.305248 | 17.288406 | 16.731262 | 15.002913 | 16.73069 | 15.896831 | 16.391926 | 16.76782 | 16.605692 | 15.951101 | 15.634242 | 15.617776 | 15.896117 | 16.33283 | 15.889195 | 16.49634 |
1201.5118 | Vitor Cardoso | Vitor Cardoso, Leonardo Gualtieri, Carlos Herdeiro, Ulrich Sperhake,
Paul M. Chesler, Luis Lehner, Seong Chan Park, Harvey S. Reall, Carlos F.
Sopuerta, Daniela Alic, Oscar J. C. Dias, Roberto Emparan, Valeria Ferrari,
Steven B. Giddings, Mahdi Godazgar, Ruth Gregory, Veronika E. Hubeny, Akihiro
Ishibashi, Greg... | NR/HEP: roadmap for the future | 68 pages, 4 Figures | null | 10.1088/0264-9381/29/24/244001 | null | hep-th astro-ph.HE gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Physics in curved spacetime describes a multitude of phenomena, ranging from
astrophysics to high energy physics. The last few years have witnessed further
progress on several fronts, including the accurate numerical evolution of the
gravitational field equations, which now allows highly nonlinear phenomena to
be tam... | [
{
"created": "Tue, 24 Jan 2012 21:00:04 GMT",
"version": "v1"
}
] | 2015-06-03 | [
[
"Cardoso",
"Vitor",
""
],
[
"Gualtieri",
"Leonardo",
""
],
[
"Herdeiro",
"Carlos",
""
],
[
"Sperhake",
"Ulrich",
""
],
[
"Chesler",
"Paul M.",
""
],
[
"Lehner",
"Luis",
""
],
[
"Park",
"Seong Chan",
""
],... | Physics in curved spacetime describes a multitude of phenomena, ranging from astrophysics to high energy physics. The last few years have witnessed further progress on several fronts, including the accurate numerical evolution of the gravitational field equations, which now allows highly nonlinear phenomena to be tamed... | 11.386111 | 10.464034 | 10.909679 | 10.2879 | 10.940107 | 11.194272 | 10.901291 | 10.313898 | 11.321328 | 11.136896 | 10.395343 | 10.706988 | 10.008544 | 10.008499 | 10.285231 | 10.402 | 10.689692 | 9.969351 | 10.330465 | 10.202566 | 10.211018 |
hep-th/9608167 | Shahin Sheikh Jabbari | H. Arfaei and M.M. Sheikh Jabbari | Different D-brane Interactions | Tex, 12 pages. Typographical errors are corrected, minor changes
done, acknowledgements added | Phys.Lett.B394:288-296,1997 | 10.1016/S0370-2693(97)00022-1 | IPM-96-163 | hep-th | null | We use rotation of one D-brane with respect to the other to reveal the hidden
structure of D-branes in type-II theories. This is done by calculation of the
interaction amplitude for two different parallel and angled branes. The
analysis of strings with different boundary conditions at the ends is also
given. The stab... | [
{
"created": "Sun, 25 Aug 1996 20:48:47 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Sep 1996 14:31:41 GMT",
"version": "v2"
}
] | 2009-10-07 | [
[
"Arfaei",
"H.",
""
],
[
"Jabbari",
"M. M. Sheikh",
""
]
] | We use rotation of one D-brane with respect to the other to reveal the hidden structure of D-branes in type-II theories. This is done by calculation of the interaction amplitude for two different parallel and angled branes. The analysis of strings with different boundary conditions at the ends is also given. The stable... | 14.236732 | 15.537394 | 15.310626 | 13.578486 | 13.384719 | 14.625628 | 13.802047 | 14.030161 | 13.571383 | 16.961281 | 13.555197 | 14.1229 | 13.743535 | 13.634404 | 13.936346 | 14.008613 | 13.805088 | 14.337453 | 14.302492 | 14.772092 | 13.622106 |
hep-th/9801167 | Andrei G. Pronko | A.G. Izergin, A.G. Pronko, N.I. Abarenkova | Temperature correlators in the one-dimensional Hubbard model in the
strong coupling limit | 14 pages, LaTeX; some comments are added, a few misprints are
corrected | Phys.Lett. A245 (1998) 537-547 | 10.1016/S0375-9601(98)00442-3 | PDMI PREPRINT - 5/1998 | hep-th | null | We consider the one-dimensional Hubbard model with the infinitely strong
repulsion. The two-point dynamical temperature correlation functions are
calculated. They are represented as Fredholm determinants of linear integrable
integral operators.
| [
{
"created": "Mon, 26 Jan 1998 10:01:39 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Jan 1998 02:11:25 GMT",
"version": "v2"
},
{
"created": "Tue, 19 May 1998 18:55:03 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Izergin",
"A. G.",
""
],
[
"Pronko",
"A. G.",
""
],
[
"Abarenkova",
"N. I.",
""
]
] | We consider the one-dimensional Hubbard model with the infinitely strong repulsion. The two-point dynamical temperature correlation functions are calculated. They are represented as Fredholm determinants of linear integrable integral operators. | 14.29 | 16.617456 | 18.146938 | 13.041081 | 13.802123 | 13.827906 | 15.998342 | 15.856332 | 13.435713 | 21.045624 | 13.047102 | 13.924562 | 18.846613 | 15.088334 | 15.568746 | 13.882593 | 15.333282 | 15.205341 | 16.121582 | 16.723206 | 13.68177 |
2106.08753 | Nick Evans | Jesus Cruz Rojas, Nick Evans, Jack Mitchell | Domain Wall Fermions on the Brane | 15 pages, 12 figures | Phys. Rev. D 104, 054029 (2021) | 10.1103/PhysRevD.104.054029 | null | hep-th hep-lat hep-ph | http://creativecommons.org/licenses/by/4.0/ | We study domain wall fermions and their condensation in the D3/probe D7
system. A spatially dependent mass term for the N=2 hypermultiplet can be
arranged to isolate distinct two component fermions on two 2+1 dimensional
domain walls. We argue that the system shows condensation/mass generation
analogous to the D3/pro... | [
{
"created": "Wed, 16 Jun 2021 13:01:20 GMT",
"version": "v1"
}
] | 2021-09-29 | [
[
"Rojas",
"Jesus Cruz",
""
],
[
"Evans",
"Nick",
""
],
[
"Mitchell",
"Jack",
""
]
] | We study domain wall fermions and their condensation in the D3/probe D7 system. A spatially dependent mass term for the N=2 hypermultiplet can be arranged to isolate distinct two component fermions on two 2+1 dimensional domain walls. We argue that the system shows condensation/mass generation analogous to the D3/probe... | 13.585464 | 13.988955 | 15.094991 | 13.953236 | 14.437037 | 14.519421 | 13.324934 | 13.165698 | 13.720222 | 16.661375 | 12.942513 | 13.245284 | 14.069736 | 13.609289 | 13.91834 | 13.107277 | 13.529355 | 13.532372 | 13.708868 | 13.957711 | 13.109481 |
hep-th/9912204 | null | Ralph Blumenhagen, Lars Goerlich and Boris Kors | Supersymmetric 4D Orientifolds of Type IIA with D6-branes at Angles | 28 pages, LaTeX, 6 figures; v2: slight modification of closed string
spectra | JHEP 0001 (2000) 040 | 10.1088/1126-6708/2000/01/040 | HUB-EP-99/63 | hep-th | null | We study a certain class of four-dimensional N=1 supersymmetric orientifolds
for which the world-sheet parity transformation is combined with a complex
conjugation in the compact directions. We investigate in detail the
orientifolds of the Z_3, Z_4, Z_6 and Z_6' toroidal orbifolds finding solutions
to the tadpole can... | [
{
"created": "Tue, 21 Dec 1999 16:02:53 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jan 2000 14:07:01 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Blumenhagen",
"Ralph",
""
],
[
"Goerlich",
"Lars",
""
],
[
"Kors",
"Boris",
""
]
] | We study a certain class of four-dimensional N=1 supersymmetric orientifolds for which the world-sheet parity transformation is combined with a complex conjugation in the compact directions. We investigate in detail the orientifolds of the Z_3, Z_4, Z_6 and Z_6' toroidal orbifolds finding solutions to the tadpole cance... | 6.488851 | 4.933259 | 6.925212 | 5.021225 | 4.86656 | 4.969307 | 4.968942 | 4.710254 | 5.12198 | 6.095539 | 4.967585 | 5.194489 | 6.108586 | 5.301476 | 5.310573 | 5.451137 | 5.45776 | 5.31945 | 5.257346 | 6.310401 | 5.476071 |
1510.00709 | Benson Way | Benjamin E. Niehoff, Jorge E. Santos, and Benson Way | Towards a violation of cosmic censorship | 21 pages, 1 figure | null | 10.1088/0264-9381/33/18/185012 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Numerical evidence suggests that the superradiant instability of Kerr-AdS
black holes and "black resonators" evolves to smaller and smaller scales
towards a "limiting" black resonator. Using $AdS_4$ supergravity, we argue that
this putative endpoint to the superradiant instability does not exist.
| [
{
"created": "Fri, 2 Oct 2015 20:04:14 GMT",
"version": "v1"
}
] | 2016-09-21 | [
[
"Niehoff",
"Benjamin E.",
""
],
[
"Santos",
"Jorge E.",
""
],
[
"Way",
"Benson",
""
]
] | Numerical evidence suggests that the superradiant instability of Kerr-AdS black holes and "black resonators" evolves to smaller and smaller scales towards a "limiting" black resonator. Using $AdS_4$ supergravity, we argue that this putative endpoint to the superradiant instability does not exist. | 12.020362 | 10.664429 | 10.722939 | 10.348283 | 11.866456 | 11.227015 | 10.453157 | 9.420941 | 11.468603 | 13.892742 | 11.285715 | 12.283509 | 11.817437 | 11.347496 | 12.067725 | 12.03842 | 11.791244 | 11.639593 | 11.651098 | 12.050575 | 11.433082 |
hep-th/9903120 | Yuji Sugawara | Yuji Sugawara (Univ. of Tokyo) | N=(0,4) Quiver $SCFT_2$ and Supergravity on $AdS_3 \times S^2$ | 31 pages, section 3 and 4 are improved, some errata are corrected,
the final version to be published in JHEP | JHEP 9906:035,1999 | 10.1088/1126-6708/1999/06/035 | UT-835 | hep-th | null | We study the proposed duality between the 5-dimensional
supergravity/superstring on $AdS_3\times S^2$ and the 2-dimensional N=(0,4)
SCFT defined on the boundary of AdS-space. We construct explicitly the N=(0,4)
SCFT by imposing the `quiver projection' developed by Douglas-Moore on the
N=(4,4) SCFT of symmetric orbifo... | [
{
"created": "Mon, 15 Mar 1999 05:41:03 GMT",
"version": "v1"
},
{
"created": "Wed, 5 May 1999 05:39:39 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Jul 1999 02:10:00 GMT",
"version": "v3"
}
] | 2010-02-03 | [
[
"Sugawara",
"Yuji",
"",
"Univ. of Tokyo"
]
] | We study the proposed duality between the 5-dimensional supergravity/superstring on $AdS_3\times S^2$ and the 2-dimensional N=(0,4) SCFT defined on the boundary of AdS-space. We construct explicitly the N=(0,4) SCFT by imposing the `quiver projection' developed by Douglas-Moore on the N=(4,4) SCFT of symmetric orbifold... | 6.59445 | 6.510599 | 6.912053 | 6.308852 | 6.695407 | 6.127049 | 6.950228 | 6.249634 | 6.571143 | 7.223658 | 6.471751 | 6.378862 | 6.402804 | 6.486338 | 6.381155 | 6.226193 | 6.281826 | 6.143694 | 6.377082 | 6.608503 | 6.462186 |
2401.14449 | Ben Heidenreich | Ben Heidenreich and Matteo Lotito | Proving the Weak Gravity Conjecture in Perturbative String Theory, Part
I: The Bosonic String | 33 pages plus appendices, 6 figures | null | null | ACF-T24-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a complete proof of the Weak Gravity Conjecture in any
perturbative bosonic string theory in spacetime dimension $D\ge6$. Our proof
works by relating the black hole extremality bound to long range forces, which
are more easily calculated on the worldsheet, closing the gaps in partial
arguments in the exist... | [
{
"created": "Thu, 25 Jan 2024 19:00:00 GMT",
"version": "v1"
}
] | 2024-01-29 | [
[
"Heidenreich",
"Ben",
""
],
[
"Lotito",
"Matteo",
""
]
] | We present a complete proof of the Weak Gravity Conjecture in any perturbative bosonic string theory in spacetime dimension $D\ge6$. Our proof works by relating the black hole extremality bound to long range forces, which are more easily calculated on the worldsheet, closing the gaps in partial arguments in the existin... | 12.551208 | 11.581141 | 13.154613 | 11.200008 | 12.383018 | 12.833512 | 12.628551 | 11.119867 | 11.169086 | 15.725477 | 11.250497 | 11.406708 | 12.099917 | 11.996199 | 12.189012 | 11.797473 | 11.551913 | 11.475466 | 12.098802 | 12.237782 | 11.717763 |
1508.04139 | Evgeny Skvortsov D | Nicolas Boulanger, Pan Kessel, E.D. Skvortsov, Massimo Taronna | Higher Spin Interactions in Four Dimensions: Vasiliev vs. Fronsdal | 56 pages=40+Appendices; 1 figure; typos fixed, one ref added | null | 10.1088/1751-8113/49/9/095402 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider four-dimensional Higher-Spin Theory at the first nontrivial order
corresponding to the cubic action. All Higher-Spin interaction vertices are
explicitly obtained from Vasiliev's equations. In particular, we obtain the
vertices that are not determined solely by the Higher-Spin algebra structure
constants. ... | [
{
"created": "Mon, 17 Aug 2015 20:04:41 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Dec 2015 13:35:52 GMT",
"version": "v2"
}
] | 2016-02-17 | [
[
"Boulanger",
"Nicolas",
""
],
[
"Kessel",
"Pan",
""
],
[
"Skvortsov",
"E. D.",
""
],
[
"Taronna",
"Massimo",
""
]
] | We consider four-dimensional Higher-Spin Theory at the first nontrivial order corresponding to the cubic action. All Higher-Spin interaction vertices are explicitly obtained from Vasiliev's equations. In particular, we obtain the vertices that are not determined solely by the Higher-Spin algebra structure constants. Th... | 13.002268 | 12.708399 | 14.250394 | 11.621267 | 12.613268 | 13.307013 | 11.574558 | 12.128453 | 12.458202 | 14.53615 | 12.166971 | 12.007808 | 12.1085 | 12.362654 | 12.269223 | 12.139089 | 12.389369 | 11.962329 | 12.278505 | 12.815406 | 11.992756 |
1910.02604 | Ulf Leonhardt | Ulf Leonhardt | Comment on Self-Stress on a Dielectric Ball and Casimir-Polder Forces | null | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In our paper [Ann. Phys. (NY) 395, 326 (2018)] we calculate the Casimir
stress on a sphere immersed in a homogeneous background, assuming
dispersionless dielectrics. Our results appear to challenge the conventional
picture of Casimir forces. The paper [arXiv:1909.05721] criticises our approach
without offering an alt... | [
{
"created": "Mon, 7 Oct 2019 04:29:18 GMT",
"version": "v1"
}
] | 2019-10-08 | [
[
"Leonhardt",
"Ulf",
""
]
] | In our paper [Ann. Phys. (NY) 395, 326 (2018)] we calculate the Casimir stress on a sphere immersed in a homogeneous background, assuming dispersionless dielectrics. Our results appear to challenge the conventional picture of Casimir forces. The paper [arXiv:1909.05721] criticises our approach without offering an alter... | 9.110196 | 9.643427 | 9.140764 | 8.930154 | 8.938684 | 9.210163 | 10.191302 | 8.410571 | 9.588273 | 9.926269 | 8.587124 | 8.65351 | 8.627523 | 8.314998 | 8.459713 | 8.586949 | 8.620154 | 8.326258 | 8.563296 | 8.583969 | 8.534119 |
hep-th/0403147 | Jianxin Lu | J. X. Lu and S. Roy | Supergravity approach to tachyon condensation on the brane-antibrane
system | 9 pages | Phys.Lett. B599 (2004) 313-318 | 10.1016/j.physletb.2004.08.047 | USTC-ICTS-04-07, MCTP-04-17 | hep-th | null | We study the tachyon condensation on the D-brane--antiD-brane system from the
supergravity point of view. The non-supersymmetric supergravity solutions with
symmetry ISO($p,1$) $\times$ SO($9-p$) are known to be characterized by three
parameters. By interpreting this solution as coincident $N$ D$p$-branes and
${\bar ... | [
{
"created": "Sun, 14 Mar 2004 03:35:40 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Lu",
"J. X.",
""
],
[
"Roy",
"S.",
""
]
] | We study the tachyon condensation on the D-brane--antiD-brane system from the supergravity point of view. The non-supersymmetric supergravity solutions with symmetry ISO($p,1$) $\times$ SO($9-p$) are known to be characterized by three parameters. By interpreting this solution as coincident $N$ D$p$-branes and ${\bar N}... | 6.041543 | 5.633795 | 6.823329 | 5.700966 | 5.850051 | 5.729629 | 5.519967 | 5.75989 | 5.721038 | 7.526645 | 5.539546 | 5.508913 | 6.338635 | 5.66577 | 5.628757 | 5.699607 | 5.627927 | 5.701437 | 5.860326 | 6.386047 | 5.658577 |
hep-th/0609161 | Oscar A. Bedoya | Oscar A. Bedoya, Osvaldo Chandia | One-loop Conformal Invariance of the Type II Pure Spinor Superstring in
a Curved Background | 24 pages, harvmac tex, references added to section 1 | JHEP 0701:042,2007 | 10.1088/1126-6708/2007/01/042 | IFT-P 033/2006 | hep-th | null | We compute the one-loop beta function for the Type II superstring using the
pure spinor formalism in a generic supergravity background. It is known that
the classical pure spinor BRST symmetry puts the background fields on-shell. In
this paper we show that the one-loop beta functions vanish as a consequence of
the cl... | [
{
"created": "Fri, 22 Sep 2006 20:47:43 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Oct 2006 21:49:33 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Bedoya",
"Oscar A.",
""
],
[
"Chandia",
"Osvaldo",
""
]
] | We compute the one-loop beta function for the Type II superstring using the pure spinor formalism in a generic supergravity background. It is known that the classical pure spinor BRST symmetry puts the background fields on-shell. In this paper we show that the one-loop beta functions vanish as a consequence of the clas... | 7.249703 | 6.201548 | 7.514355 | 5.80918 | 5.69663 | 5.746272 | 5.704001 | 5.390823 | 5.350171 | 8.129583 | 5.744537 | 6.119774 | 7.649216 | 6.628701 | 6.311592 | 6.472253 | 6.213382 | 6.474662 | 6.392497 | 7.624266 | 6.110862 |
hep-th/0203227 | Aref'eva Irina | I.Ya.Aref'eva, A.A.Giryavets and A.S.Koshelev | NS Ghost Slivers | 27 pages, LATEX | Phys.Lett. B536 (2002) 138-146 | 10.1016/S0370-2693(02)01759-8 | null | hep-th | null | Neveu-Schwarz ghost slivers in pictures zero and minus one are constructed.
In particular, using algebraic methods $\beta$, $\gamma$ ghost sliver in the -1
picture is obtained. The algebraic method consists in solving a projector
equation in an algebra, where the multiplication is defined by a pure 3-string
vertex wi... | [
{
"created": "Sun, 24 Mar 2002 18:07:48 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Aref'eva",
"I. Ya.",
""
],
[
"Giryavets",
"A. A.",
""
],
[
"Koshelev",
"A. S.",
""
]
] | Neveu-Schwarz ghost slivers in pictures zero and minus one are constructed. In particular, using algebraic methods $\beta$, $\gamma$ ghost sliver in the -1 picture is obtained. The algebraic method consists in solving a projector equation in an algebra, where the multiplication is defined by a pure 3-string vertex with... | 17.222086 | 15.76858 | 19.56716 | 14.823539 | 16.900343 | 17.257183 | 16.309164 | 15.810525 | 15.466045 | 21.07667 | 15.696568 | 14.606583 | 16.042433 | 15.123607 | 14.813328 | 14.330502 | 14.598088 | 14.531621 | 14.646278 | 15.888941 | 15.818896 |
1602.04926 | Ahmed Farag Ali | Amani Ashour, Mir Faizal, Ahmed Farag Ali, Fay\c{c}al Hammad | Branes in Gravity's Rainbow | 12 pages, REVTeX 4, 5 figures. Accepted for Publication in The
European Physical Journal C | Eur.Phys.J. C76 (2016) no.5, 264 | 10.1140/epjc/s10052-016-4124-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we investigate the thermodynamics of black $p$-branes (BB) in
the context of Gravity's Rainbow. We investigate this using rainbow functions
that have been motivated from loop quantum gravity and $\kappa$-Minkowski
noncommutative spacetime. Then for the sake of comparison, we examine a couple
of other ra... | [
{
"created": "Tue, 16 Feb 2016 07:22:19 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Apr 2016 14:12:40 GMT",
"version": "v2"
}
] | 2016-05-17 | [
[
"Ashour",
"Amani",
""
],
[
"Faizal",
"Mir",
""
],
[
"Ali",
"Ahmed Farag",
""
],
[
"Hammad",
"Fayçal",
""
]
] | In this work, we investigate the thermodynamics of black $p$-branes (BB) in the context of Gravity's Rainbow. We investigate this using rainbow functions that have been motivated from loop quantum gravity and $\kappa$-Minkowski noncommutative spacetime. Then for the sake of comparison, we examine a couple of other rain... | 7.531868 | 7.347425 | 7.257846 | 7.273237 | 7.359746 | 7.510665 | 8.14221 | 7.14952 | 7.481777 | 7.757298 | 7.627347 | 7.11217 | 7.30121 | 7.293984 | 7.045793 | 7.107994 | 7.379572 | 7.166852 | 7.160828 | 7.156056 | 7.069575 |
hep-th/9411191 | York Xylander | C. Wieczerkowski, Y. Xylander | Improved actions, the perfect action, and scaling by perturbation theory
in Wilsons renormalization group: the two dimensional $O(N)$-invariant non
linear $\sigma$-model in the hierarchical approximation | 13 pages in LaTeX, 5 uuencoded PS figures included with epsfig.sty
(including of ps-files fixed) | Nucl.Phys. B440 (1995) 393-404 | 10.1016/0550-3213(95)00066-2 | MS-TPI-94-14,DESY-94-223 | hep-th hep-lat | null | We propose a method using perturbation theory in the running coupling
constant and the idea of scaling to determine improved actions for lattice
field theories combining Wilson's renormalization group with Symanzik's
improvement program . The method is based on the analysis of a single
renormalization group transform... | [
{
"created": "Fri, 25 Nov 1994 15:46:36 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Nov 1994 09:25:42 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Wieczerkowski",
"C.",
""
],
[
"Xylander",
"Y.",
""
]
] | We propose a method using perturbation theory in the running coupling constant and the idea of scaling to determine improved actions for lattice field theories combining Wilson's renormalization group with Symanzik's improvement program . The method is based on the analysis of a single renormalization group transformat... | 12.76002 | 10.762501 | 14.608213 | 11.531857 | 11.656606 | 13.079125 | 12.148422 | 11.652412 | 11.925477 | 13.761628 | 12.606811 | 11.759051 | 12.808228 | 11.737419 | 11.669333 | 11.631637 | 11.705585 | 11.388829 | 11.901445 | 12.864554 | 11.928384 |
2008.00179 | Takahisa Igata | Takahisa Igata, Shinya Tomizawa | Stable circular orbits in higher-dimensional multi-black hole spacetimes | 22 pages, 4 figures; v2: minor revisions, add references; v3:
published version | Phys. Rev. D 102, 084003 (2020) | 10.1103/PhysRevD.102.084003 | KEK-TH-2248, KEK-Cosmo-262, TTI-MATHPHYS-1 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the dynamics of particles, particularly focusing on circular
orbits in the higher-dimensional Majumdar-Papapetrou (MP) spacetimes with two
equal mass black holes. It is widely known that in the 5D
Schwarzschild-Tangherlini and Myers-Perry backgrounds, there are no stable
circular orbits. In contrast, we s... | [
{
"created": "Sat, 1 Aug 2020 05:55:16 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Sep 2020 07:48:26 GMT",
"version": "v2"
},
{
"created": "Thu, 1 Oct 2020 15:27:13 GMT",
"version": "v3"
}
] | 2020-10-07 | [
[
"Igata",
"Takahisa",
""
],
[
"Tomizawa",
"Shinya",
""
]
] | We consider the dynamics of particles, particularly focusing on circular orbits in the higher-dimensional Majumdar-Papapetrou (MP) spacetimes with two equal mass black holes. It is widely known that in the 5D Schwarzschild-Tangherlini and Myers-Perry backgrounds, there are no stable circular orbits. In contrast, we sho... | 5.081931 | 5.388922 | 4.751173 | 4.687815 | 5.207994 | 4.814131 | 5.416501 | 4.618797 | 5.104594 | 4.879835 | 4.988303 | 4.935288 | 4.845065 | 4.845163 | 4.917055 | 4.830049 | 5.03894 | 4.826079 | 5.072521 | 4.912132 | 4.881036 |
1401.0740 | Anton Kapustin | Anton Kapustin, Nathan Seiberg | Coupling a QFT to a TQFT and Duality | 53 pages, harvmac. v2: references added | null | 10.1007/JHEP04(2014)001 | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider coupling an ordinary quantum field theory with an infinite number
of degrees of freedom to a topological field theory. On R^d the new theory
differs from the original one by the spectrum of operators. Sometimes the local
operators are the same but there are different line operators, surface
operators, etc... | [
{
"created": "Fri, 3 Jan 2014 22:05:38 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Jan 2014 02:43:06 GMT",
"version": "v2"
}
] | 2015-06-18 | [
[
"Kapustin",
"Anton",
""
],
[
"Seiberg",
"Nathan",
""
]
] | We consider coupling an ordinary quantum field theory with an infinite number of degrees of freedom to a topological field theory. On R^d the new theory differs from the original one by the spectrum of operators. Sometimes the local operators are the same but there are different line operators, surface operators, etc. ... | 8.71226 | 8.643312 | 9.650695 | 9.053671 | 8.713326 | 8.484703 | 9.33413 | 8.43808 | 8.554445 | 10.865843 | 8.633707 | 8.356016 | 8.733459 | 8.306214 | 8.501333 | 8.663627 | 8.506366 | 8.509508 | 8.371165 | 8.71797 | 7.92132 |
hep-th/0408105 | Friedel Epple | Friedel Epple | Induced Gravity on Intersecting Branes | references added, minor changes to discussion of path integral
normalization on page 5 | JHEP0409:021,2004 | 10.1088/1126-6708/2004/09/021 | DAMTP-2004-82 | hep-th | null | We establish Einstein-Hilbert gravity couplings in the effective action for
Intersecting Brane Worlds. The four-dimensional induced Planck mass is
determined by calculating graviton scattering amplitudes at one-loop in the
string perturbation expansion. We derive a general formula linking the induced
Planck mass for ... | [
{
"created": "Thu, 12 Aug 2004 19:09:21 GMT",
"version": "v1"
},
{
"created": "Fri, 13 Aug 2004 15:52:19 GMT",
"version": "v2"
},
{
"created": "Sat, 16 Oct 2004 20:02:46 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Epple",
"Friedel",
""
]
] | We establish Einstein-Hilbert gravity couplings in the effective action for Intersecting Brane Worlds. The four-dimensional induced Planck mass is determined by calculating graviton scattering amplitudes at one-loop in the string perturbation expansion. We derive a general formula linking the induced Planck mass for N=... | 12.221332 | 11.256252 | 13.282511 | 11.495261 | 11.059062 | 10.769015 | 10.593751 | 11.445909 | 11.641816 | 14.633663 | 11.244335 | 10.898841 | 12.665651 | 11.173745 | 11.749702 | 11.425787 | 11.798922 | 11.781394 | 11.316344 | 12.799149 | 11.106937 |
2102.04480 | Yixuan Li | Yixuan Li | Black Holes and the Swampland: the Deep Throat revelations | 29 pages, 2 figures. V2: reference added. V3: revised version
accepted for publication in JHEP. V4: Added funding information | null | 10.1007/JHEP06(2021)065 | JHEP06(2021)065 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Multi-centered bubbling solutions are black hole microstate geometries that
arise as smooth solutions of 5-dimensional $\mathcal{N}=2$ Supergravity. When
these solutions reach the scaling limit, their resulting geometries develop an
infinitely deep throat and look arbitrarily close to a black hole geometry. We
depict... | [
{
"created": "Mon, 8 Feb 2021 19:00:07 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Mar 2021 15:42:51 GMT",
"version": "v2"
},
{
"created": "Thu, 27 May 2021 08:59:30 GMT",
"version": "v3"
},
{
"created": "Mon, 19 Jul 2021 16:27:28 GMT",
"version": "v4"
}
] | 2021-07-20 | [
[
"Li",
"Yixuan",
""
]
] | Multi-centered bubbling solutions are black hole microstate geometries that arise as smooth solutions of 5-dimensional $\mathcal{N}=2$ Supergravity. When these solutions reach the scaling limit, their resulting geometries develop an infinitely deep throat and look arbitrarily close to a black hole geometry. We depict a... | 9.048572 | 8.031116 | 10.11925 | 8.213635 | 8.530107 | 8.171461 | 8.591563 | 8.01862 | 8.084548 | 9.838772 | 8.308723 | 8.257094 | 8.583515 | 8.19063 | 8.28453 | 8.043254 | 7.974349 | 8.409867 | 8.039704 | 8.499339 | 8.384583 |
1906.02234 | Marjorie Schillo | Adam Bzowski and Marjorie Schillo | Dimensional regularization for holographic RG flows | 30 pages + references | null | 10.1007/JHEP10(2019)025 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we present a holographic renormalization scheme for
asymptotically anti-de Sitter spacetimes in which the dual renormalization
scheme of the boundary field theory is dimensional regularization. This
constitutes a new level of precision in the holographic dictionary and paves
the way for the exact matchi... | [
{
"created": "Wed, 5 Jun 2019 18:18:31 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Sep 2019 14:23:57 GMT",
"version": "v2"
}
] | 2019-10-23 | [
[
"Bzowski",
"Adam",
""
],
[
"Schillo",
"Marjorie",
""
]
] | In this work, we present a holographic renormalization scheme for asymptotically anti-de Sitter spacetimes in which the dual renormalization scheme of the boundary field theory is dimensional regularization. This constitutes a new level of precision in the holographic dictionary and paves the way for the exact matching... | 9.320419 | 9.622009 | 9.563464 | 9.451967 | 10.037034 | 9.898554 | 9.821455 | 9.622303 | 9.386561 | 10.465433 | 9.305666 | 9.224238 | 9.122032 | 9.096106 | 9.144418 | 8.990896 | 9.344923 | 9.065395 | 9.110458 | 9.370173 | 8.836909 |
2305.00267 | Ming Zhang | Ting-Feng Gong, Jie Jiang, Ming Zhang | Holographic thermodynamics of rotating black holes | 21 pages, 5 captioned figures, published version | null | 10.1007/JHEP06(2023)105 | null | hep-th gr-qc | http://creativecommons.org/licenses/by-nc-nd/4.0/ | We provide mass/energy formulas for the extended thermodynamics, mixed
thermodynamics, and holographic conformal field theory (CFT) thermodynamics for
the charged and rotating Kerr-Newman Anti-de Sitter black holes. Then for the
CFT thermal states dual to the black hole, we find the first-order phase
transitions and ... | [
{
"created": "Sat, 29 Apr 2023 14:34:37 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Jun 2023 07:34:44 GMT",
"version": "v2"
},
{
"created": "Sat, 24 Jun 2023 09:04:39 GMT",
"version": "v3"
}
] | 2023-06-27 | [
[
"Gong",
"Ting-Feng",
""
],
[
"Jiang",
"Jie",
""
],
[
"Zhang",
"Ming",
""
]
] | We provide mass/energy formulas for the extended thermodynamics, mixed thermodynamics, and holographic conformal field theory (CFT) thermodynamics for the charged and rotating Kerr-Newman Anti-de Sitter black holes. Then for the CFT thermal states dual to the black hole, we find the first-order phase transitions and cr... | 9.792817 | 8.00938 | 9.374537 | 8.091303 | 8.147122 | 8.728538 | 8.390771 | 8.010079 | 8.184665 | 9.759448 | 8.092462 | 8.51875 | 9.13236 | 8.70593 | 8.457244 | 8.908009 | 8.999148 | 8.619201 | 8.641646 | 9.210078 | 8.710229 |
2310.12042 | Sebastian Grieninger | Sebastian Grieninger, Dmitri E. Kharzeev, Ismail Zahed | Entanglement entropy in a time-dependent holographic Schwinger pair
creation | 9 pages, 6 figures; | Phys. Rev. D 108, 126014 (2023) | 10.1103/PhysRevD.108.126014 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the entanglement of a Schwinger pair created by a time-dependent
pulse. In the semi-classical approximation, the pair creation by a pulse of
external electric field is captured by a periodic worldline instanton. At
strong gauge coupling, the gauge-gravity dual worldsheet instanton exhibits a
falling wormho... | [
{
"created": "Wed, 18 Oct 2023 15:26:59 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Dec 2023 19:45:07 GMT",
"version": "v2"
}
] | 2023-12-20 | [
[
"Grieninger",
"Sebastian",
""
],
[
"Kharzeev",
"Dmitri E.",
""
],
[
"Zahed",
"Ismail",
""
]
] | We analyze the entanglement of a Schwinger pair created by a time-dependent pulse. In the semi-classical approximation, the pair creation by a pulse of external electric field is captured by a periodic worldline instanton. At strong gauge coupling, the gauge-gravity dual worldsheet instanton exhibits a falling wormhole... | 14.58086 | 15.016256 | 15.245897 | 14.202399 | 13.712559 | 14.858912 | 17.22839 | 14.388746 | 14.570024 | 15.596458 | 13.844925 | 14.245529 | 13.392685 | 14.228048 | 14.096291 | 14.017446 | 14.152251 | 14.260943 | 14.374072 | 13.160642 | 13.427516 |
1701.09035 | Muge Boz | M. K. G\"um\"u\c{s} and M. Boz | Gauge fixing problem and the constrained quantization | 15 pages. Two references are added and few typos are corrected in the
second version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, the quantization of the Yang-Mills theory is worked out by
means of Dirac's canonical quantization method, using the generalized Coulomb
gauge fixing conditions. Following the construction of the matrix composed of
all the second class constraints of the theory, its convenience within the
framework of t... | [
{
"created": "Tue, 31 Jan 2017 13:47:01 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Feb 2017 11:36:56 GMT",
"version": "v2"
}
] | 2017-02-03 | [
[
"Gümüş",
"M. K.",
""
],
[
"Boz",
"M.",
""
]
] | In this work, the quantization of the Yang-Mills theory is worked out by means of Dirac's canonical quantization method, using the generalized Coulomb gauge fixing conditions. Following the construction of the matrix composed of all the second class constraints of the theory, its convenience within the framework of the... | 9.701044 | 8.852594 | 8.722998 | 8.454016 | 9.253282 | 9.627283 | 9.234797 | 8.478117 | 8.875027 | 9.39336 | 8.583983 | 8.345846 | 8.491861 | 8.454082 | 8.761535 | 8.708395 | 8.556346 | 8.732128 | 8.617474 | 8.874534 | 8.727817 |
hep-th/0305148 | Emil J. Martinec | Emil J. Martinec | The Annular Report on Non-Critical String Theory | 29 pages (latex), 4 (.eps) figures. v2: minor changes, references
added | null | null | EFI-03-22 | hep-th gr-qc | null | Recent results on the annulus partition function in Liouville field theory
are applied to non-critical string theory, both below and above the critical
dimension. Liouville gravity coupled to $c\le 1$ matter has a dual formulation
as a matrix model. Two well-known matrix model results are reproduced precisely
using t... | [
{
"created": "Sun, 18 May 2003 14:51:33 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Jun 2003 17:13:08 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Martinec",
"Emil J.",
""
]
] | Recent results on the annulus partition function in Liouville field theory are applied to non-critical string theory, both below and above the critical dimension. Liouville gravity coupled to $c\le 1$ matter has a dual formulation as a matrix model. Two well-known matrix model results are reproduced precisely using the... | 7.638923 | 7.254129 | 8.676271 | 7.146417 | 7.745383 | 7.288033 | 7.736154 | 7.374323 | 7.525347 | 9.675732 | 7.26749 | 7.338654 | 8.043257 | 7.738205 | 7.681055 | 7.535057 | 7.61965 | 7.331405 | 7.877964 | 8.16085 | 7.28987 |
hep-th/9304164 | Carlo RovellI | Carlo Rovelli | The basis of the Ponzano-Regge-Turaev-Viro-Ooguri model is the loop
representation basis | 16 pages | Phys.Rev. D48 (1993) 2702-2707 | 10.1103/PhysRevD.48.2702 | pitt-gr-4-93 | hep-th math.QA | null | We show that the Hilbert space basis that defines the Ponzano-Regge-
Turaev-Viro-Ooguri combinatorial definition of 3-d Quantum Gravity is the same
as the one that defines the Loop Representation. We show how to compute lengths
in Witten's 3-d gravity and how to reconstruct the 2-d geometry from a state of
Witten's t... | [
{
"created": "Sat, 1 May 1993 03:11:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Rovelli",
"Carlo",
""
]
] | We show that the Hilbert space basis that defines the Ponzano-Regge- Turaev-Viro-Ooguri combinatorial definition of 3-d Quantum Gravity is the same as the one that defines the Loop Representation. We show how to compute lengths in Witten's 3-d gravity and how to reconstruct the 2-d geometry from a state of Witten's the... | 8.607457 | 9.043855 | 8.350163 | 8.245957 | 8.632545 | 8.932644 | 9.211565 | 8.635153 | 8.471049 | 8.49966 | 8.185504 | 8.071033 | 8.286014 | 8.22115 | 8.120296 | 8.219677 | 8.141676 | 7.908811 | 8.457746 | 8.367434 | 7.910349 |
hep-th/0510260 | Natalia Kiriushcheva | N. Kiriushcheva and S.V. Kuzmin | On Hamiltonian formulation of the Einstein-Hilbert action in two
dimensions | 9 pages | Mod.Phys.Lett.A21:899-906,2006 | 10.1142/S0217732306020202 | null | hep-th | null | It is shown that the well-known triviality of the Einstein field equations in
two dimensions is not a sufficient condition for the Einstein-Hilbert action to
be a total divergence, if the general covariance is to be preserved, that is, a
coordinate system is not fixed. Consequently, a Hamiltonian formulation is
possi... | [
{
"created": "Sun, 30 Oct 2005 18:54:25 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Kiriushcheva",
"N.",
""
],
[
"Kuzmin",
"S. V.",
""
]
] | It is shown that the well-known triviality of the Einstein field equations in two dimensions is not a sufficient condition for the Einstein-Hilbert action to be a total divergence, if the general covariance is to be preserved, that is, a coordinate system is not fixed. Consequently, a Hamiltonian formulation is possibl... | 10.696703 | 10.071285 | 10.362146 | 9.122251 | 11.549982 | 10.482467 | 10.927347 | 9.670026 | 9.511059 | 10.784827 | 9.816941 | 9.531389 | 9.957027 | 9.763312 | 9.228115 | 9.473392 | 9.906995 | 9.197956 | 9.789775 | 10.093169 | 9.530978 |
hep-th/9901075 | P. M. Sutcliffe | Michael Singer and Paul Sutcliffe | Symmetric Instantons and Skyrme Fields | 22 pages plus 1 figure in GIF format | Nonlinearity 12 (1999) 987-1003 | 10.1088/0951-7715/12/4/315 | null | hep-th | null | By explicit construction of the ADHM data, we prove the existence of a charge
seven instanton with icosahedral symmetry. By computing the holonomy of this
instanton we obtain a Skyrme field which approximates the minimal energy charge
seven Skyrmion. We also present a one parameter family of tetrahedrally
symmetric i... | [
{
"created": "Mon, 18 Jan 1999 19:03:25 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Singer",
"Michael",
""
],
[
"Sutcliffe",
"Paul",
""
]
] | By explicit construction of the ADHM data, we prove the existence of a charge seven instanton with icosahedral symmetry. By computing the holonomy of this instanton we obtain a Skyrme field which approximates the minimal energy charge seven Skyrmion. We also present a one parameter family of tetrahedrally symmetric ins... | 7.841739 | 6.581942 | 8.118694 | 7.233239 | 7.148803 | 6.879581 | 6.985015 | 6.367836 | 6.904699 | 8.41818 | 7.342456 | 7.146626 | 7.73682 | 7.048634 | 7.025285 | 7.056338 | 7.120129 | 7.014512 | 6.976111 | 7.624991 | 7.419268 |
2210.07025 | Rijun Huang | Rijun Huang, Qingjun Jin, Yi Li | Wilson Lines and Boundary Operators of BCFW Shifts | 28 pages, 5 figures, improve the writing and correct some typos | null | 10.1007/JHEP12(2022)023 | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Boundary operators are gauge invariant operators whose form factors
correspond to boundary contributions of BCFW shifts. In gauge theory, the
boundary operators contain infinite series, which are constrained by gauge
symmetry. We compute the boundary operators of all possible BCFW shifts in
Yang-Mills theory and QCD,... | [
{
"created": "Thu, 13 Oct 2022 13:36:25 GMT",
"version": "v1"
},
{
"created": "Sun, 6 Nov 2022 13:58:57 GMT",
"version": "v2"
}
] | 2022-12-12 | [
[
"Huang",
"Rijun",
""
],
[
"Jin",
"Qingjun",
""
],
[
"Li",
"Yi",
""
]
] | Boundary operators are gauge invariant operators whose form factors correspond to boundary contributions of BCFW shifts. In gauge theory, the boundary operators contain infinite series, which are constrained by gauge symmetry. We compute the boundary operators of all possible BCFW shifts in Yang-Mills theory and QCD, a... | 10.443479 | 8.990826 | 10.381917 | 9.323915 | 9.046132 | 9.178265 | 9.910109 | 9.178611 | 8.634462 | 9.724733 | 9.354975 | 9.664769 | 8.987489 | 9.30181 | 9.636497 | 9.289149 | 9.493911 | 9.561723 | 9.268441 | 9.674094 | 9.166985 |
2303.16305 | Gregory Korchemsky | M. Beccaria, G.P. Korchemsky, A.A. Tseytlin | Non-planar corrections in orbifold/orientifold $\mathcal N=2$
superconformal theories from localization | 54 pages. v2: minor clarifications | null | 10.1007/JHEP05(2023)165 | IPhT-T23/015, Imperial-TP-AT-2023-01 | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study non-planar corrections in two special $\mathcal N=2$ superconformal
$SU(N)$ gauge theories that are planar-equivalent to $\mathcal N=4$ SYM theory:
two-nodes quiver model with equal couplings and $\mathcal N=2$ vector multiplet
coupled to two hypermultiplets in rank-2 symmetric and antisymmetric
representati... | [
{
"created": "Tue, 28 Mar 2023 20:57:06 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Apr 2023 08:06:23 GMT",
"version": "v2"
}
] | 2023-06-07 | [
[
"Beccaria",
"M.",
""
],
[
"Korchemsky",
"G. P.",
""
],
[
"Tseytlin",
"A. A.",
""
]
] | We study non-planar corrections in two special $\mathcal N=2$ superconformal $SU(N)$ gauge theories that are planar-equivalent to $\mathcal N=4$ SYM theory: two-nodes quiver model with equal couplings and $\mathcal N=2$ vector multiplet coupled to two hypermultiplets in rank-2 symmetric and antisymmetric representation... | 5.671881 | 5.232849 | 6.374467 | 5.536543 | 5.747279 | 5.546353 | 5.531703 | 5.13345 | 5.381497 | 7.07302 | 5.475605 | 5.579289 | 5.837957 | 5.520988 | 5.678431 | 5.680972 | 5.585683 | 5.625599 | 5.598144 | 5.795089 | 5.524535 |
hep-th/9908141 | Hajime Aoki | H. Aoki, N. Ishibashi, S. Iso, H. Kawai, Y. Kitazawa and T. Tada | Noncommutative Yang-Mills in IIB Matrix Model | 21pages, LaTeX, no figures, typos corrected | Nucl.Phys. B565 (2000) 176-192 | 10.1016/S0550-3213(99)00633-1 | KEK-TH-637, KUNS-1595 | hep-th | null | We show that twisted reduced models can be interpreted as noncommutative
Yang-Mills theory. Based upon this correspondence, we obtain noncommutative
Yang-Mills theory with D-brane backgrounds in IIB matrix model. We propose that
IIB matrix model with D-brane backgrounds serve as a concrete definition of
noncommutativ... | [
{
"created": "Fri, 20 Aug 1999 17:21:27 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Aug 1999 09:17:27 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Aoki",
"H.",
""
],
[
"Ishibashi",
"N.",
""
],
[
"Iso",
"S.",
""
],
[
"Kawai",
"H.",
""
],
[
"Kitazawa",
"Y.",
""
],
[
"Tada",
"T.",
""
]
] | We show that twisted reduced models can be interpreted as noncommutative Yang-Mills theory. Based upon this correspondence, we obtain noncommutative Yang-Mills theory with D-brane backgrounds in IIB matrix model. We propose that IIB matrix model with D-brane backgrounds serve as a concrete definition of noncommutative ... | 10.013399 | 8.287978 | 9.782494 | 8.490116 | 9.059711 | 7.747786 | 8.087862 | 8.318343 | 8.52522 | 10.358028 | 8.509107 | 8.883978 | 9.617105 | 9.177484 | 9.319275 | 9.080816 | 8.777196 | 9.025115 | 9.087213 | 9.543839 | 9.062839 |
2105.02129 | Herman Verlinde | Herman Verlinde | Wormholes in Quantum Mechanics | 15 pages plus Appendix, 10 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a geometric path integral definition of wormhole partition
functions in a general class of 1D quantum systems obtained by quantizing a
phase space. We compute the wormhole partition function in a semi-classical
limit and in some simple examples. The partition function of the n-fold
wormhole is found to b... | [
{
"created": "Wed, 5 May 2021 15:35:12 GMT",
"version": "v1"
}
] | 2021-05-06 | [
[
"Verlinde",
"Herman",
""
]
] | We introduce a geometric path integral definition of wormhole partition functions in a general class of 1D quantum systems obtained by quantizing a phase space. We compute the wormhole partition function in a semi-classical limit and in some simple examples. The partition function of the n-fold wormhole is found to be ... | 9.90421 | 10.562398 | 11.708873 | 9.666227 | 10.01577 | 10.560622 | 9.975851 | 9.489003 | 9.553535 | 11.394593 | 9.585749 | 10.01399 | 10.38765 | 9.934216 | 9.973083 | 9.92663 | 9.417278 | 9.960463 | 9.808254 | 10.333591 | 9.823876 |
hep-th/0404059 | Yuichi Hoshino | Yuichi Hoshino | Mass singularity and confining property in $QED_3$ | 22pages,4figures,revtex4,Notational sloppiness are crrected.Submitted
to JHEP | JHEP0409:048,2004 | 10.1088/1126-6708/2004/09/048 | null | hep-th | null | We discuss the properties of the position space fermion propagator in three
dimensional QED which has been found previouly based on Ward-Takahashi-identity
for soft-photon emission vertex and spectral representation.There is a new type
of mass singularity which governs the long distance behaviour.It leads the
propaga... | [
{
"created": "Wed, 7 Apr 2004 07:51:56 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Jul 2004 01:07:15 GMT",
"version": "v10"
},
{
"created": "Mon, 20 Sep 2004 11:32:38 GMT",
"version": "v11"
},
{
"created": "Thu, 8 Apr 2004 01:26:09 GMT",
"version": "v2"
},
{
"c... | 2008-11-26 | [
[
"Hoshino",
"Yuichi",
""
]
] | We discuss the properties of the position space fermion propagator in three dimensional QED which has been found previouly based on Ward-Takahashi-identity for soft-photon emission vertex and spectral representation.There is a new type of mass singularity which governs the long distance behaviour.It leads the propagato... | 23.083244 | 20.029415 | 23.850864 | 20.456858 | 23.642921 | 20.706408 | 21.723164 | 21.532833 | 22.13109 | 26.890404 | 21.791861 | 22.283873 | 22.702221 | 22.125372 | 22.782492 | 22.872025 | 22.46179 | 23.164558 | 21.498163 | 22.647511 | 22.719965 |
1707.07390 | Gabriele Tartaglino-Mazzucchelli | Sergei M. Kuzenko and Gabriele Tartaglino-Mazzucchelli | New nilpotent ${\cal N}= 2$ superfields | 20 pages; V3: typos corrected | Phys. Rev. D 97, 026003 (2018) | 10.1103/PhysRevD.97.026003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose new off-shell models for spontaneously broken local ${\cal N}=2$
supersymmetry, in which the supergravity multiplet couples to nilpotent
Goldstino superfields that contain either a gauge one-form or a gauge two-form
in addition to spin-1/2 Goldstone fermions and auxiliary fields. In the case of
${\cal N}=2... | [
{
"created": "Mon, 24 Jul 2017 03:37:58 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Aug 2017 10:20:52 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Jan 2018 10:49:34 GMT",
"version": "v3"
}
] | 2018-01-17 | [
[
"Kuzenko",
"Sergei M.",
""
],
[
"Tartaglino-Mazzucchelli",
"Gabriele",
""
]
] | We propose new off-shell models for spontaneously broken local ${\cal N}=2$ supersymmetry, in which the supergravity multiplet couples to nilpotent Goldstino superfields that contain either a gauge one-form or a gauge two-form in addition to spin-1/2 Goldstone fermions and auxiliary fields. In the case of ${\cal N}=2$ ... | 5.932461 | 5.741444 | 6.805595 | 5.610254 | 5.628197 | 5.217035 | 5.935657 | 5.493486 | 5.453454 | 7.651518 | 5.695651 | 5.211409 | 5.888909 | 5.379564 | 5.570176 | 5.57325 | 5.43943 | 5.57615 | 5.393656 | 6.266828 | 5.340901 |
0911.0364 | Brandon Carter | Brandon Carter | Fields In Nonaffine Bundles II. Gauge coupled generalization of harmonic
mappings and their Bunting identities | 12 page Latex file with some minor misprint corrections and added
color for article originally published in black and white | Phys.Rev.D33:991-996,1986 | 10.1103/PhysRevD.33.991 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The general purpose bitensorially gauge-covariant differentiation procedure
set up in the preceding article is specialised to the particular case of
bundles with nonlinear fibres that are endowed with a torsion free Riemannian
or pseudo-Riemannian structure. This formalism is used to generalize the class
of harmonic ... | [
{
"created": "Mon, 2 Nov 2009 17:55:10 GMT",
"version": "v1"
}
] | 2009-11-05 | [
[
"Carter",
"Brandon",
""
]
] | The general purpose bitensorially gauge-covariant differentiation procedure set up in the preceding article is specialised to the particular case of bundles with nonlinear fibres that are endowed with a torsion free Riemannian or pseudo-Riemannian structure. This formalism is used to generalize the class of harmonic ma... | 18.925613 | 21.517237 | 22.166243 | 17.56798 | 21.290422 | 22.289818 | 21.950666 | 19.68445 | 18.976055 | 24.928841 | 19.256691 | 19.515148 | 19.530605 | 18.44503 | 19.464302 | 19.813433 | 19.351616 | 19.160522 | 19.197853 | 19.57205 | 18.624334 |
0712.3699 | Klaus Bering | Igor A. Batalin and Klaus Bering | Odd Scalar Curvature in Anti-Poisson Geometry | 9 pages, LaTeX. v2: Minor changes. v3: Published version | Phys.Lett.B663:132-135,2008 | 10.1016/j.physletb.2008.03.066 | null | hep-th math-ph math.MP math.SG | null | Recent works have revealed that the recipe for field-antifield quantization
of Lagrangian gauge theories can be considerably relaxed when it comes to
choosing a path integral measure \rho if a zero-order term \nu_{\rho} is added
to the \Delta operator. The effects of this odd scalar term \nu_{\rho} become
relevant at... | [
{
"created": "Fri, 21 Dec 2007 13:57:01 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Jan 2008 11:20:30 GMT",
"version": "v2"
},
{
"created": "Fri, 11 Apr 2008 12:28:02 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Batalin",
"Igor A.",
""
],
[
"Bering",
"Klaus",
""
]
] | Recent works have revealed that the recipe for field-antifield quantization of Lagrangian gauge theories can be considerably relaxed when it comes to choosing a path integral measure \rho if a zero-order term \nu_{\rho} is added to the \Delta operator. The effects of this odd scalar term \nu_{\rho} become relevant at t... | 14.076593 | 12.588174 | 13.771577 | 12.350248 | 12.568144 | 12.065142 | 13.29564 | 12.014918 | 12.189097 | 15.644411 | 12.360065 | 11.605864 | 12.973817 | 11.636386 | 12.074698 | 11.678558 | 11.409778 | 11.959373 | 11.932809 | 13.159522 | 12.174936 |
2212.04783 | Nathan Moynihan | Mariana Carrillo Gonz\'alez, William T. Emond, Nathan Moynihan,
Justinas Rumbutis and Chris D. White | Mini-twistors and the Cotton Double Copy | null | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | The double copy relates quantities in gauge, gravity and related theories. A
well-known procedure for relating exact classical solutions is the Weyl double
copy in four spacetime dimensions, and a three-dimensional analogue of this --
the Cotton double copy -- has recently been found for topologically massive
gauge t... | [
{
"created": "Fri, 9 Dec 2022 11:24:20 GMT",
"version": "v1"
}
] | 2022-12-12 | [
[
"González",
"Mariana Carrillo",
""
],
[
"Emond",
"William T.",
""
],
[
"Moynihan",
"Nathan",
""
],
[
"Rumbutis",
"Justinas",
""
],
[
"White",
"Chris D.",
""
]
] | The double copy relates quantities in gauge, gravity and related theories. A well-known procedure for relating exact classical solutions is the Weyl double copy in four spacetime dimensions, and a three-dimensional analogue of this -- the Cotton double copy -- has recently been found for topologically massive gauge the... | 11.362039 | 10.008864 | 11.493581 | 9.922121 | 10.270487 | 9.930121 | 9.962778 | 9.920063 | 9.248695 | 13.103394 | 9.628068 | 9.935997 | 10.732795 | 10.15247 | 9.924756 | 10.210964 | 10.199636 | 10.095951 | 10.297401 | 10.89214 | 10.064612 |
hep-th/9707042 | Ashoke Sen | Ashoke Sen | Dynamics of Multiple Kaluza-Klein Monopoles in M- and String Theory | LaTeX file, 12 pages | Adv.Theor.Math.Phys.1:115-126,1998 | null | MRI-PHY/P970716 | hep-th | null | We analyse the world-volume theory of multiple Kaluza-Klein monopoles in
string and M-theory by identifying the appropriate zero modes of various
fields. The results are consistent with supersymmetry, and all conjectured
duality symmetries. In particular for M-theory and type IIA string theory, the
low energy dynamic... | [
{
"created": "Thu, 3 Jul 1997 16:39:22 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Sen",
"Ashoke",
""
]
] | We analyse the world-volume theory of multiple Kaluza-Klein monopoles in string and M-theory by identifying the appropriate zero modes of various fields. The results are consistent with supersymmetry, and all conjectured duality symmetries. In particular for M-theory and type IIA string theory, the low energy dynamics ... | 5.702866 | 5.113878 | 6.643868 | 5.319549 | 5.542844 | 5.399451 | 4.969908 | 5.333272 | 5.315794 | 6.786769 | 5.066057 | 5.079548 | 5.608331 | 5.085991 | 5.260302 | 5.07105 | 5.135619 | 5.125154 | 5.121872 | 5.498177 | 5.012053 |
0903.3365 | In\^es Aniceto | Michael C. Abbott, In\^es Aniceto and Olof Ohlsson Sax | Dyonic Giant Magnons in CP^3: Strings and Curves at Finite J | 22 pages, 3 figures, 2 tables. v2 adds note on breather solution, and
minor clarifications | Phys.Rev.D80:026005,2009 | 10.1103/PhysRevD.80.026005 | BROWN-HET 1580, UUITP-11/09 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper studies giant magnons in AdS_4 x CP^3 using both the string
sigma-model and the algebraic curve. We complete the dictionary of solutions by
finding the dyonic generalisation of the CP^1 string solution, which matches
the `small' giant magnon in the algebraic curve, and by pointing out that the
solution rec... | [
{
"created": "Thu, 19 Mar 2009 16:50:02 GMT",
"version": "v1"
},
{
"created": "Thu, 21 May 2009 01:10:59 GMT",
"version": "v2"
}
] | 2010-12-16 | [
[
"Abbott",
"Michael C.",
""
],
[
"Aniceto",
"Inês",
""
],
[
"Sax",
"Olof Ohlsson",
""
]
] | This paper studies giant magnons in AdS_4 x CP^3 using both the string sigma-model and the algebraic curve. We complete the dictionary of solutions by finding the dyonic generalisation of the CP^1 string solution, which matches the `small' giant magnon in the algebraic curve, and by pointing out that the solution recen... | 11.074551 | 9.499223 | 13.155355 | 9.47874 | 9.639812 | 9.743625 | 9.543848 | 9.005858 | 9.198656 | 14.098972 | 9.324888 | 9.453145 | 11.192494 | 9.711358 | 9.522408 | 9.625717 | 9.575876 | 9.662306 | 9.397344 | 10.748271 | 9.6945 |
1203.0582 | Julio Oliva | Alex Giacomini, Gaston Giribet, Mauricio Leston, Julio Oliva, Sourya
Ray | Scalar field perturbations in asymptotically Lifshitz black holes | 13 pages, no figures. v2: 14 pages, references added. To appear on
PRD | Phys. Rev. D 85, 124001 (2012) | 10.1103/PhysRevD.85.124001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider scalar field perturbations about asymptotically Lifshitz black
holes with dynamical exponent z in D dimensions. We show that, for suitable
boundary conditions, these Lifshitz black holes are stable under scalar field
perturbations. For z=2, we explicitly compute the quasinormal mode frecuencies,
which res... | [
{
"created": "Fri, 2 Mar 2012 22:34:09 GMT",
"version": "v1"
},
{
"created": "Thu, 3 May 2012 20:24:31 GMT",
"version": "v2"
}
] | 2012-06-05 | [
[
"Giacomini",
"Alex",
""
],
[
"Giribet",
"Gaston",
""
],
[
"Leston",
"Mauricio",
""
],
[
"Oliva",
"Julio",
""
],
[
"Ray",
"Sourya",
""
]
] | We consider scalar field perturbations about asymptotically Lifshitz black holes with dynamical exponent z in D dimensions. We show that, for suitable boundary conditions, these Lifshitz black holes are stable under scalar field perturbations. For z=2, we explicitly compute the quasinormal mode frecuencies, which resul... | 7.727639 | 7.31349 | 6.895553 | 6.531088 | 6.553382 | 6.782338 | 7.096949 | 6.291907 | 6.814581 | 7.814498 | 6.443209 | 6.694325 | 7.511414 | 6.840518 | 6.949953 | 6.793022 | 6.968656 | 6.587015 | 6.851944 | 7.067123 | 6.838309 |
1012.3192 | Jeff Greensite | R. Alkofer, D. Diakonov, J. Pawlowski, H. Reinhardt, V. Zakharov, D.
Zwanziger, and J. Greensite | Panel discussion: What {\it don't} we know about confinement? | 8 pages. Roundtable discussion at the Quark Confinement and Hadron
Spectrum 9 conference (Madrid, Aug. 29 - Sep. 3, 2010). To appear in the
conference proceedings, published by the AIP. v2: References added. v3:
Reference corrected | null | 10.1063/1.3574936 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The participants in this discussion session of the QCHS 9 meeting were each
asked the following question: "What would be the most useful piece of
information that you could obtain, by whatever means, that would advance your
own program, and/or our general understanding of confinement?" This proceedings
contains a bri... | [
{
"created": "Tue, 14 Dec 2010 22:52:08 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Dec 2010 22:51:38 GMT",
"version": "v2"
},
{
"created": "Tue, 4 Jan 2011 19:29:21 GMT",
"version": "v3"
}
] | 2016-02-18 | [
[
"Alkofer",
"R.",
""
],
[
"Diakonov",
"D.",
""
],
[
"Pawlowski",
"J.",
""
],
[
"Reinhardt",
"H.",
""
],
[
"Zakharov",
"V.",
""
],
[
"Zwanziger",
"D.",
""
],
[
"Greensite",
"J.",
""
]
] | The participants in this discussion session of the QCHS 9 meeting were each asked the following question: "What would be the most useful piece of information that you could obtain, by whatever means, that would advance your own program, and/or our general understanding of confinement?" This proceedings contains a brief... | 14.554665 | 15.561205 | 13.028123 | 10.670556 | 14.903222 | 12.363589 | 14.010941 | 14.978845 | 10.756834 | 11.938293 | 12.931734 | 13.276306 | 11.624618 | 11.557875 | 13.207027 | 12.143542 | 12.064245 | 12.478339 | 11.323709 | 11.068857 | 12.293032 |
1603.07691 | M. Abdul Wasay | Muhammad Abdul Wasay | Supersymmetric quantum mechanics and topology | 26 pages | Adv.High Energy Phys. 2016 (2016) 3906746 | 10.1155/2016/3906746 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Supersymmetric quantum mechanical models are computed by the Path integral
approach. In the $\beta\rightarrow0$ limit, the integrals localize to the zero
modes. This allows us to perform the index computations exactly because of
supersymmetric localization, and we will show how the geometry of target space
enters the... | [
{
"created": "Sun, 13 Mar 2016 08:30:28 GMT",
"version": "v1"
}
] | 2016-03-31 | [
[
"Wasay",
"Muhammad Abdul",
""
]
] | Supersymmetric quantum mechanical models are computed by the Path integral approach. In the $\beta\rightarrow0$ limit, the integrals localize to the zero modes. This allows us to perform the index computations exactly because of supersymmetric localization, and we will show how the geometry of target space enters the p... | 11.664231 | 12.592652 | 14.025723 | 11.680503 | 12.028742 | 11.521399 | 12.635364 | 12.065734 | 11.351467 | 15.548396 | 11.922482 | 11.288327 | 13.358384 | 11.94892 | 11.488962 | 11.606724 | 11.848252 | 11.287789 | 11.93854 | 13.439363 | 11.506725 |
hep-th/0606034 | Eric R. Sharpe | S. Hellerman, A. Henriques, T. Pantev, E. Sharpe, M. Ando | Cluster decomposition, T-duality, and gerby CFT's | 61 pages, LaTeX; v2,3: typos fixed; v4: writing improved in several
sections; v5: typos fixed | Adv.Theor.Math.Phys.11:751-818,2007 | 10.4310/ATMP.2007.v11.n5.a2 | null | hep-th | null | In this paper we study CFT's associated to gerbes. These theories suffer from
a lack of cluster decomposition, but this problem can be resolved: the CFT's
are the same as CFT's for disconnected targets. Such theories also lack cluster
decomposition, but in that form, the lack is manifestly not very problematic.
In pa... | [
{
"created": "Mon, 5 Jun 2006 15:16:18 GMT",
"version": "v1"
},
{
"created": "Tue, 6 Jun 2006 12:02:52 GMT",
"version": "v2"
},
{
"created": "Fri, 16 Jun 2006 18:24:46 GMT",
"version": "v3"
},
{
"created": "Fri, 18 Aug 2006 13:04:01 GMT",
"version": "v4"
},
{
"cre... | 2016-10-04 | [
[
"Hellerman",
"S.",
""
],
[
"Henriques",
"A.",
""
],
[
"Pantev",
"T.",
""
],
[
"Sharpe",
"E.",
""
],
[
"Ando",
"M.",
""
]
] | In this paper we study CFT's associated to gerbes. These theories suffer from a lack of cluster decomposition, but this problem can be resolved: the CFT's are the same as CFT's for disconnected targets. Such theories also lack cluster decomposition, but in that form, the lack is manifestly not very problematic. In part... | 13.685184 | 14.750575 | 16.88809 | 12.986208 | 14.319265 | 14.279007 | 12.74779 | 12.937205 | 12.426434 | 16.038767 | 13.32239 | 12.891878 | 14.473228 | 12.546866 | 13.140431 | 13.379274 | 13.379291 | 13.118185 | 13.057201 | 14.074963 | 12.782757 |
hep-th/0512114 | Alessandra Agostini | Alessandra Agostini | kappa-Minkowski representations on Hilbert spaces | 23 pag. Latex, correction of a couple of typos, reference added,
title slightly changed | J.Math.Phys.48:052305,2007 | 10.1063/1.2738360 | null | hep-th | null | The algebra of functions on kappa-Minkowski noncommutative spacetime is
studied as algebra of operators on Hilbert spaces. The representations of this
algebra are constructed and classified. This new approach leads to a natural
construction of integration in kappa-Minkowski spacetime in terms of the usual
trace of op... | [
{
"created": "Fri, 9 Dec 2005 21:29:56 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Jun 2007 20:35:01 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Jun 2007 10:08:12 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Agostini",
"Alessandra",
""
]
] | The algebra of functions on kappa-Minkowski noncommutative spacetime is studied as algebra of operators on Hilbert spaces. The representations of this algebra are constructed and classified. This new approach leads to a natural construction of integration in kappa-Minkowski spacetime in terms of the usual trace of oper... | 8.912827 | 6.744218 | 7.767936 | 6.693603 | 6.669958 | 7.127496 | 6.211232 | 6.763529 | 6.120096 | 9.529553 | 6.864504 | 6.941978 | 7.799843 | 6.936325 | 7.093175 | 7.027816 | 7.187483 | 7.013845 | 7.218294 | 7.785672 | 6.91288 |
hep-th/0110066 | Rey Soojong | Y. Kiem, S.-S. Kim, S.-J. Rey, H.-T. Sato | Anatomy of Two-Loop Effective Action in Noncommutative Field Theories | 27 pages, Latex, 6 figures using pictex, v2. typos corrected | Nucl.Phys. B641 (2002) 256-284 | 10.1016/S0550-3213(02)00589-8 | SNUST 01-0901, PUPT 2009 | hep-th | null | We compute, at two-loop order, one-particle-irreducible Green functions and
effective action in noncommutative $\lambda[\Phi^3]_\star$-theory for both
planar (g=0, h=3) and nonplanar (g=1, h=1) contributions. We adopt worldline
formulation of the Feynman diagrammatics so that relation to string theory
diagrammatics i... | [
{
"created": "Mon, 8 Oct 2001 10:44:54 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Oct 2001 06:54:57 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Kiem",
"Y.",
""
],
[
"Kim",
"S. -S.",
""
],
[
"Rey",
"S. -J.",
""
],
[
"Sato",
"H. -T.",
""
]
] | We compute, at two-loop order, one-particle-irreducible Green functions and effective action in noncommutative $\lambda[\Phi^3]_\star$-theory for both planar (g=0, h=3) and nonplanar (g=1, h=1) contributions. We adopt worldline formulation of the Feynman diagrammatics so that relation to string theory diagrammatics is ... | 9.249572 | 9.173096 | 9.756915 | 8.462646 | 8.956961 | 9.152571 | 9.498254 | 8.533683 | 8.31004 | 9.666769 | 8.360981 | 9.114813 | 9.09325 | 8.348326 | 8.578628 | 8.870953 | 8.415903 | 8.702408 | 8.760117 | 8.885955 | 8.594784 |
1302.2050 | Fabio Zwirner | Fabio Zwirner | Quantum corrections to broken N=8 supergravity | 6 pages: contribution to the proceedings of ICHEP2012, The 36th
International Conference on High Energy Physics, 4-11 July 2012, Melbourne,
Australia | null | null | DFPD-2013-TH-02 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The discovery of the Higgs boson and the non-discovery (so far) of additional
particles at the TeV scale underline our poor understanding of the hierarchy
problems in the physics of the fundamental interactions. Loosely motivated by
this consideration, I review some recent results on the classical and quantum
stabili... | [
{
"created": "Fri, 8 Feb 2013 14:39:31 GMT",
"version": "v1"
}
] | 2013-02-11 | [
[
"Zwirner",
"Fabio",
""
]
] | The discovery of the Higgs boson and the non-discovery (so far) of additional particles at the TeV scale underline our poor understanding of the hierarchy problems in the physics of the fundamental interactions. Loosely motivated by this consideration, I review some recent results on the classical and quantum stability... | 9.677359 | 8.641615 | 9.668797 | 8.047063 | 10.429791 | 10.110303 | 10.11266 | 9.191532 | 9.599211 | 9.58485 | 8.955242 | 9.058831 | 9.698116 | 9.122581 | 9.262223 | 9.30976 | 9.473042 | 9.264835 | 8.968349 | 9.699363 | 9.201766 |
1108.2909 | Alexander Zhidenko | R. A. Konoplya and A. Zhidenko | Superradiance and instability of the charged Myers-Perry black holes in
the G\"{o}del Universe | 7 pages, 9 figures | Phys. Rev. D 84, 104022 (2011) | 10.1103/PhysRevD.84.104022 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider scalar field perturbations of the asymptotically G\"odel
5-dimensional charged rotating black holes with two equal angular momenta. It
is shown that the spectrum of proper oscillations of the perturbation includes
superradiant unstable modes. The reason for the instability is the confining
Dirichlet bound... | [
{
"created": "Sun, 14 Aug 2011 22:50:47 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Sep 2011 20:14:31 GMT",
"version": "v2"
}
] | 2011-11-09 | [
[
"Konoplya",
"R. A.",
""
],
[
"Zhidenko",
"A.",
""
]
] | We consider scalar field perturbations of the asymptotically G\"odel 5-dimensional charged rotating black holes with two equal angular momenta. It is shown that the spectrum of proper oscillations of the perturbation includes superradiant unstable modes. The reason for the instability is the confining Dirichlet boundar... | 7.652417 | 7.27963 | 7.511446 | 7.20718 | 7.81195 | 7.099561 | 6.921204 | 6.794082 | 6.820596 | 7.64124 | 7.340233 | 7.112243 | 7.132989 | 6.923471 | 6.886251 | 7.101381 | 7.031468 | 7.26289 | 6.888611 | 7.317503 | 6.827573 |
1410.4815 | Daniel Litim | Kevin Falls, Daniel F. Litim, Konstantinos Nikolakopoulos, Christoph
Rahmede | Further evidence for asymptotic safety of quantum gravity | 44 pages, 17 figures, explanations and Sec VII D added; to appear
(PRD) | Phys. Rev. D 93, 104022 (2016) | 10.1103/PhysRevD.93.104022 | DO-TH 14/26, KA-TP-2014-30 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The asymptotic safety conjecture is examined for quantum gravity in four
dimensions. Using the renormalisation group, we find evidence for an
interacting UV fixed point for polynomial actions up to the 34th power in the
Ricci scalar. The extrapolation to infinite polynomial order is given, and the
self-consistency of... | [
{
"created": "Fri, 17 Oct 2014 18:23:56 GMT",
"version": "v1"
},
{
"created": "Mon, 25 Apr 2016 17:36:28 GMT",
"version": "v2"
}
] | 2016-05-18 | [
[
"Falls",
"Kevin",
""
],
[
"Litim",
"Daniel F.",
""
],
[
"Nikolakopoulos",
"Konstantinos",
""
],
[
"Rahmede",
"Christoph",
""
]
] | The asymptotic safety conjecture is examined for quantum gravity in four dimensions. Using the renormalisation group, we find evidence for an interacting UV fixed point for polynomial actions up to the 34th power in the Ricci scalar. The extrapolation to infinite polynomial order is given, and the self-consistency of t... | 10.812537 | 11.063385 | 10.462742 | 10.113252 | 10.708642 | 10.41592 | 10.395645 | 10.845603 | 10.134892 | 11.182851 | 10.564725 | 10.728345 | 11.054871 | 10.376699 | 10.652801 | 10.56204 | 10.805868 | 10.192966 | 10.918658 | 11.059667 | 10.562234 |
hep-th/9412161 | null | D.V. Fursaev | Temperature and Entropy of a Quantum Black Hole and Conformal Anomaly | 10 pages, Latex file | Phys.Rev.D51:5352-5355,1995 | 10.1103/PhysRevD.51.5352 | JINR E2-94-484 | hep-th | null | Attention is paid to the fact that temperature of a classical black hole can
be derived from the extremality condition of its free energy with respect to
variation of the mass of a hole. For a quantum Schwarzschild black hole
evaporating massless particles the same condition is shown to result in the
following one-lo... | [
{
"created": "Mon, 19 Dec 1994 08:54:32 GMT",
"version": "v1"
}
] | 2009-12-30 | [
[
"Fursaev",
"D. V.",
""
]
] | Attention is paid to the fact that temperature of a classical black hole can be derived from the extremality condition of its free energy with respect to variation of the mass of a hole. For a quantum Schwarzschild black hole evaporating massless particles the same condition is shown to result in the following one-loop... | 7.70921 | 8.067708 | 7.526659 | 7.250923 | 8.560188 | 8.304216 | 8.595313 | 7.730475 | 7.456827 | 7.563361 | 7.895673 | 7.37385 | 7.40199 | 7.157447 | 7.664423 | 7.27954 | 7.456868 | 7.338532 | 7.379839 | 7.289039 | 7.380376 |
hep-th/0312035 | Juan L. Manes | Juan L. Manes | String Form Factors | 18 pages, 3 figures. Typos corrected, 1 footnote (in Section 4) and 1
reference added | JHEP 0401 (2004) 033 | 10.1088/1126-6708/2004/01/033 | EHU-FT/03-05 | hep-th | null | We compute the cross section for scattering of light string probes by
randomly excited closed strings. For high energy probes, the cross section
factorizes and can be used to define effective form factors for the excited
targets. These form factors are well defined without the need for infinite
subtractions and conta... | [
{
"created": "Wed, 3 Dec 2003 14:20:11 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Dec 2003 15:15:44 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Manes",
"Juan L.",
""
]
] | We compute the cross section for scattering of light string probes by randomly excited closed strings. For high energy probes, the cross section factorizes and can be used to define effective form factors for the excited targets. These form factors are well defined without the need for infinite subtractions and contain... | 13.796546 | 13.981495 | 13.474441 | 12.827477 | 14.279698 | 13.685447 | 14.116702 | 14.465621 | 13.691149 | 15.21089 | 13.065759 | 12.551276 | 12.893912 | 13.425518 | 13.115242 | 12.915995 | 13.111772 | 12.725535 | 13.161725 | 13.416709 | 12.903062 |
hep-th/0307212 | Christian Brouder | Christian Brouder | Quantum field theory of degenerate systems | 4 pages, no figure | null | null | null | hep-th | null | To set up a self-consistent quantum field theory of degenerate systems, the
unperturbed state should be described by a density matrix instead of a pure
state. This increases the combinatorial complexity of the many-body equations.
Hopf algebraic techniques are used to deal with this complexity and show that
the Schwi... | [
{
"created": "Tue, 22 Jul 2003 12:49:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Brouder",
"Christian",
""
]
] | To set up a self-consistent quantum field theory of degenerate systems, the unperturbed state should be described by a density matrix instead of a pure state. This increases the combinatorial complexity of the many-body equations. Hopf algebraic techniques are used to deal with this complexity and show that the Schwing... | 9.54059 | 8.827558 | 8.902017 | 8.462868 | 8.755339 | 9.327425 | 8.949179 | 8.698323 | 8.469123 | 10.518602 | 8.46988 | 8.346707 | 8.365086 | 8.272286 | 8.160708 | 8.25675 | 8.50395 | 8.254213 | 8.190502 | 8.486411 | 8.597356 |
hep-th/0306250 | de Mello Koch | Paul L. H. Cook, Robert de Mello Koch and Jeff Murugan | Non-Abelian BIonic Brane Intersections | 17 pages uses harvmac; v2: small typos corrected, refs added | Phys.Rev.D68:126007,2003 | 10.1103/PhysRevD.68.126007 | null | hep-th | null | We study "fuzzy funnel" solutions to the non-Abelian equations of motion of
the D-string. Our funnel describes n^6/360 coincident D-strings ending on n^3/6
D7-branes, in terms of a fuzzy six-sphere which expands along the string. We
also provide a dual description of this configuration in terms of the world
volume th... | [
{
"created": "Wed, 25 Jun 2003 16:42:45 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Jul 2003 13:01:12 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Cook",
"Paul L. H.",
""
],
[
"Koch",
"Robert de Mello",
""
],
[
"Murugan",
"Jeff",
""
]
] | We study "fuzzy funnel" solutions to the non-Abelian equations of motion of the D-string. Our funnel describes n^6/360 coincident D-strings ending on n^3/6 D7-branes, in terms of a fuzzy six-sphere which expands along the string. We also provide a dual description of this configuration in terms of the world volume theo... | 12.660679 | 12.00069 | 15.232246 | 10.839685 | 10.411493 | 9.807702 | 10.301922 | 11.448744 | 9.824616 | 14.71953 | 10.935499 | 10.554364 | 11.719604 | 10.873119 | 10.593991 | 10.739378 | 10.082699 | 10.497898 | 10.380053 | 12.472723 | 10.92344 |
hep-th/0309238 | Lubos Motl | Robbert Dijkgraaf, Lubos Motl | Matrix string theory, contact terms, and superstring field theory | 26 pages, 3 EPS figures, JHEP3 LaTeX; references added | null | null | HUTP-03/A063, ITFA-2003-45, HEP-UK-0019 | hep-th | null | In this note, we first explain the equivalence between the interaction
Hamiltonian of Green-Schwarz light-cone gauge superstring field theory and the
twist field formalism known from matrix string theory. We analyze the role of
the large N limit in matrix string theory, in particular in relation with
conformal pertur... | [
{
"created": "Thu, 25 Sep 2003 20:06:12 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Oct 2003 20:05:21 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Dijkgraaf",
"Robbert",
""
],
[
"Motl",
"Lubos",
""
]
] | In this note, we first explain the equivalence between the interaction Hamiltonian of Green-Schwarz light-cone gauge superstring field theory and the twist field formalism known from matrix string theory. We analyze the role of the large N limit in matrix string theory, in particular in relation with conformal perturba... | 11.643942 | 12.340995 | 12.613951 | 11.321374 | 11.455073 | 11.660811 | 11.860977 | 10.981064 | 10.811251 | 12.080276 | 11.05934 | 11.047276 | 11.078161 | 10.726619 | 11.153871 | 11.205807 | 11.213449 | 11.09316 | 11.089569 | 11.052986 | 10.685436 |
2009.14368 | Ryo Yokokura | Yoshimasa Hidaka, Muneto Nitta, Ryo Yokokura | Global 3-group symmetry and 't Hooft anomalies in axion electrodynamics | 30 + 39 pages, 46 figures; v2: references and discussions added,
published version | JHEP 01 (2021) 173 | 10.1007/JHEP01(2021)173 | KEK-TH-2254, J-PARC-TH-0225, RIKEN-iTHEMS-Report-20 | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate a higher-group structure of massless axion electrodynamics in
$(3+1)$ dimensions. By using the background gauging method, we show that the
higher-form symmetries necessarily have a global semistrict 3-group (2-crossed
module) structure, and exhibit 't Hooft anomalies of the 3-group. In
particular, we f... | [
{
"created": "Wed, 30 Sep 2020 01:11:03 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Feb 2021 14:28:47 GMT",
"version": "v2"
}
] | 2021-02-10 | [
[
"Hidaka",
"Yoshimasa",
""
],
[
"Nitta",
"Muneto",
""
],
[
"Yokokura",
"Ryo",
""
]
] | We investigate a higher-group structure of massless axion electrodynamics in $(3+1)$ dimensions. By using the background gauging method, we show that the higher-form symmetries necessarily have a global semistrict 3-group (2-crossed module) structure, and exhibit 't Hooft anomalies of the 3-group. In particular, we fin... | 7.995769 | 6.150742 | 8.317943 | 6.452179 | 7.233712 | 6.878613 | 7.009042 | 6.15543 | 6.214189 | 8.899296 | 6.058619 | 6.772672 | 7.973722 | 6.866214 | 6.754658 | 6.86311 | 6.993516 | 7.080648 | 6.991912 | 7.817955 | 6.733932 |
1409.3874 | Benson Way | Harvey S. Reall, Norihiro Tanahashi, and Benson Way | Shock Formation in Lovelock Theories | 43 pages, 5 figures | Phys. Rev. D 91, 044013 (2015) | 10.1103/PhysRevD.91.044013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that Lovelock theories of gravity suffer from shock formation,
unlike General Relativity. We consider the propagation of (i) a discontinuity
in curvature, and (ii) weak, high frequency, gravitational waves. Such
disturbances propagate along characteristic hypersurfaces of a "background"
spacetime and their a... | [
{
"created": "Fri, 12 Sep 2014 21:47:47 GMT",
"version": "v1"
}
] | 2015-03-05 | [
[
"Reall",
"Harvey S.",
""
],
[
"Tanahashi",
"Norihiro",
""
],
[
"Way",
"Benson",
""
]
] | We argue that Lovelock theories of gravity suffer from shock formation, unlike General Relativity. We consider the propagation of (i) a discontinuity in curvature, and (ii) weak, high frequency, gravitational waves. Such disturbances propagate along characteristic hypersurfaces of a "background" spacetime and their amp... | 8.455575 | 8.582676 | 8.226584 | 7.969196 | 8.68766 | 8.274042 | 8.985192 | 8.106905 | 8.196192 | 8.871363 | 7.710711 | 8.200171 | 8.224566 | 7.961811 | 8.331155 | 7.904602 | 8.311254 | 8.041838 | 8.129741 | 8.367496 | 7.787022 |
1209.5357 | Jeffrey Pennington | Jeffrey Pennington | The six-point remainder function to all loop orders in the multi-Regge
limit | 25 pages, 1 figure | null | 10.1007/JHEP01(2013)059 | SLAC-PUB-15251 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an all-orders formula for the six-point amplitude of planar
maximally supersymmetric N=4 Yang-Mills theory in the leading-logarithmic
approximation of multi-Regge kinematics. In the MHV helicity configuration, our
results agree with an integral formula of Lipatov and Prygarin through at least
14 loops. A d... | [
{
"created": "Mon, 24 Sep 2012 18:28:57 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Pennington",
"Jeffrey",
""
]
] | We present an all-orders formula for the six-point amplitude of planar maximally supersymmetric N=4 Yang-Mills theory in the leading-logarithmic approximation of multi-Regge kinematics. In the MHV helicity configuration, our results agree with an integral formula of Lipatov and Prygarin through at least 14 loops. A dif... | 7.593578 | 7.653096 | 9.287363 | 7.609946 | 8.12795 | 7.921443 | 7.991506 | 7.385604 | 7.049469 | 9.663831 | 7.399923 | 7.64742 | 7.863845 | 7.460629 | 7.667881 | 7.519485 | 7.523842 | 7.440712 | 7.489649 | 7.891845 | 7.299952 |
1003.0684 | Juan Manuel Romero | Juan M. Romero, R. Bernal-Jaquez, O. Gonzalez-Gaxiola | Is it possible to relate MOND with Horava Gravity? | 9 pages,no figures. Minor changes. References added | Mod. Phys. Lett. A25:2501-2506,2010 | 10.1142/S0217732310033396 | null | hep-th | http://creativecommons.org/licenses/by/3.0/ | In this work we present a scalar field theory invariant under space-time
anisotropic transformations with a dynamic exponet $z$. It is shown that this
theory possess symmetries similar to Horava gravity and that in the limit $z=0$
the equations of motion of the non-relativistic MOND theory are obtained. This
result a... | [
{
"created": "Tue, 2 Mar 2010 21:14:20 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Apr 2010 16:17:19 GMT",
"version": "v2"
},
{
"created": "Fri, 15 Oct 2010 16:36:44 GMT",
"version": "v3"
}
] | 2010-10-18 | [
[
"Romero",
"Juan M.",
""
],
[
"Bernal-Jaquez",
"R.",
""
],
[
"Gonzalez-Gaxiola",
"O.",
""
]
] | In this work we present a scalar field theory invariant under space-time anisotropic transformations with a dynamic exponet $z$. It is shown that this theory possess symmetries similar to Horava gravity and that in the limit $z=0$ the equations of motion of the non-relativistic MOND theory are obtained. This result all... | 8.966509 | 8.699354 | 7.97225 | 7.844314 | 8.012977 | 7.793774 | 8.060442 | 7.731327 | 7.177378 | 8.515197 | 7.604424 | 7.817988 | 8.046157 | 7.829348 | 7.675971 | 7.750699 | 7.583416 | 7.590297 | 7.728929 | 7.957583 | 7.786173 |
1506.01368 | Marco Scalisi | Marco Scalisi | Cosmological $\alpha$-Attractors and de Sitter Landscape | 14 pages, 3 figures. v3: minor clarifications and refs added. JHEP
version | JHEP12(2015)134 | 10.1007/JHEP12(2015)134 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a unified description of cosmological $\alpha$-attractors and
late-time acceleration, in excellent agreement with the latest Planck data. Our
construction involves two superfields playing distinctive roles: one is the
dynamical field and its evolution determines inflation and dark energy, the
other is nilp... | [
{
"created": "Wed, 3 Jun 2015 19:56:03 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Jul 2015 19:14:52 GMT",
"version": "v2"
},
{
"created": "Sat, 26 Dec 2015 19:48:05 GMT",
"version": "v3"
}
] | 2015-12-29 | [
[
"Scalisi",
"Marco",
""
]
] | We provide a unified description of cosmological $\alpha$-attractors and late-time acceleration, in excellent agreement with the latest Planck data. Our construction involves two superfields playing distinctive roles: one is the dynamical field and its evolution determines inflation and dark energy, the other is nilpot... | 12.630894 | 12.960408 | 12.965585 | 11.559139 | 13.029265 | 13.249866 | 13.361035 | 12.552359 | 11.83962 | 12.907526 | 12.534143 | 11.947891 | 12.216202 | 11.759346 | 12.368344 | 12.09832 | 12.116415 | 12.308278 | 11.943002 | 12.536529 | 11.864565 |
1509.07431 | Parinya Karndumri | Parinya Karndumri | Non-semisimple gauging of a magical N=4 supergravity in three dimensions | 22 pages, no figure, typos and operator dimension corrected | JHEP12(2015)153 | 10.1007/JHEP12(2015)153 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a new $N=4$ non-semisimple gauged supergravity in three
dimensions with $E_{6(2)}/SU(6)\times SU(2)$ scalar manifold and $SO(4)\ltimes
\mathbf{T}^6$ gauge group. Depending on the values of the gauge coupling
constants, the theory admits both the maximally supersymmetric $AdS_3$ vacuum
preserving $SO(4)$ ... | [
{
"created": "Thu, 24 Sep 2015 16:48:21 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Oct 2015 14:30:38 GMT",
"version": "v2"
},
{
"created": "Wed, 23 Dec 2015 11:12:28 GMT",
"version": "v3"
}
] | 2015-12-24 | [
[
"Karndumri",
"Parinya",
""
]
] | We construct a new $N=4$ non-semisimple gauged supergravity in three dimensions with $E_{6(2)}/SU(6)\times SU(2)$ scalar manifold and $SO(4)\ltimes \mathbf{T}^6$ gauge group. Depending on the values of the gauge coupling constants, the theory admits both the maximally supersymmetric $AdS_3$ vacuum preserving $SO(4)$ ga... | 4.608828 | 3.837194 | 5.513266 | 3.929203 | 4.061846 | 3.897797 | 3.795013 | 3.832319 | 3.708039 | 5.11831 | 3.979679 | 4.273351 | 4.800071 | 4.223535 | 4.216184 | 4.312761 | 4.097481 | 4.276186 | 4.315619 | 4.750514 | 4.205906 |
hep-th/0511237 | Atsushi Higuchi | Atsushi Higuchi | Possible Constraints on String Theory in Closed Space with Symmetries | 8 pages, presented at NATO Advanced Research Workshop on
Noncommutative Structures in Mathematics and Physics, Kiev, Ukraine, 24-27
Sep 2000 | Noncommutative structures in mathematics and physics (Kluwer,
2001), pp. 465-473 | null | null | hep-th astro-ph gr-qc | null | It is well known that certain quadratic constraints have to be imposed on
linearized gravity in closed space with symmetries. We review this phenomenon
and discuss one of the constraints which arise in linearized gravity on static
flat torus in detail. Then we point out that the mode with negative kinetic
energy, whi... | [
{
"created": "Wed, 23 Nov 2005 21:55:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Higuchi",
"Atsushi",
""
]
] | It is well known that certain quadratic constraints have to be imposed on linearized gravity in closed space with symmetries. We review this phenomenon and discuss one of the constraints which arise in linearized gravity on static flat torus in detail. Then we point out that the mode with negative kinetic energy, which... | 18.782713 | 15.165802 | 15.37863 | 14.41517 | 15.655635 | 16.204865 | 16.699404 | 14.49836 | 14.767777 | 16.329739 | 15.897534 | 14.321498 | 14.697058 | 14.447533 | 15.08543 | 14.748415 | 14.809525 | 14.284199 | 15.919792 | 14.956059 | 15.228234 |
1801.01172 | Masafumi Shimojo | Masafumi Shimojo, Satoshi Ishihara, Hironobu Kataoka, Atsuko Matsukawa
and Hikaru Sato | The superspace representation of Super Yang-Mills theory on NCG | arXiv admin note: text overlap with arXiv:1311.4671 | Prog Theor Exp Phys (2018) | 10.1093/ptep/pty046 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A few years ago, we found the supersymmetric(SUSY) counterpart of the
spectral triple which specified noncommutative geometry(NCG). Based on "the
triple", we considered the SUSY version of the spectral action principle and
had derived the action of super Yang--Mills theory, minimal supersymmetric
standard model, and ... | [
{
"created": "Mon, 25 Dec 2017 08:01:55 GMT",
"version": "v1"
}
] | 2019-12-06 | [
[
"Shimojo",
"Masafumi",
""
],
[
"Ishihara",
"Satoshi",
""
],
[
"Kataoka",
"Hironobu",
""
],
[
"Matsukawa",
"Atsuko",
""
],
[
"Sato",
"Hikaru",
""
]
] | A few years ago, we found the supersymmetric(SUSY) counterpart of the spectral triple which specified noncommutative geometry(NCG). Based on "the triple", we considered the SUSY version of the spectral action principle and had derived the action of super Yang--Mills theory, minimal supersymmetric standard model, and su... | 11.162835 | 10.734425 | 12.268656 | 10.149184 | 10.734703 | 10.68268 | 10.447362 | 10.461816 | 10.150058 | 12.198108 | 10.171902 | 10.276031 | 10.621133 | 10.285369 | 10.463001 | 10.616909 | 10.27516 | 10.522681 | 10.401196 | 10.834823 | 10.469974 |
hep-th/0602083 | Sean Nowling | Shinsuke Kawai, Esko Keski-Vakkuri, Robert G. Leigh, Sean Nowling | Fractional S-branes on a Spacetime Orbifold | 22 pages, 6 eps figures | Phys.Rev.D73:106004,2006 | 10.1103/PhysRevD.73.106004 | null | hep-th | null | Unstable D-branes are central objects in string theory, and exist also in
time-dependent backgrounds. In this paper we take first steps to studying brane
decay in spacetime orbifolds. As a concrete model we focus on the R^{1,d}/Z_2
orbifold. We point out that on a spacetime orbifold there exist two kinds of
S-branes,... | [
{
"created": "Wed, 8 Feb 2006 16:55:13 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kawai",
"Shinsuke",
""
],
[
"Keski-Vakkuri",
"Esko",
""
],
[
"Leigh",
"Robert G.",
""
],
[
"Nowling",
"Sean",
""
]
] | Unstable D-branes are central objects in string theory, and exist also in time-dependent backgrounds. In this paper we take first steps to studying brane decay in spacetime orbifolds. As a concrete model we focus on the R^{1,d}/Z_2 orbifold. We point out that on a spacetime orbifold there exist two kinds of S-branes, f... | 11.986465 | 11.778586 | 12.982183 | 10.458896 | 11.13132 | 10.319725 | 11.699715 | 10.215978 | 10.566689 | 14.331862 | 10.66464 | 10.925132 | 11.140816 | 10.867998 | 10.671983 | 10.386375 | 10.787492 | 10.77148 | 10.934406 | 11.186017 | 10.754836 |
hep-th/9802074 | Misha Stephanov | Horatiu Nastase, Misha Stephanov, Peter van Nieuwenhuizen and Anton
Rebhan | Topological boundary conditions, the BPS bound, and elimination of
ambiguities in the quantum mass of solitons | 38 pages | Nucl.Phys. B542 (1999) 471-514 | 10.1016/S0550-3213(98)00773-1 | ITP-SB 98-9, TUW 98-01 | hep-th | null | We fix the long-standing ambiguity in the 1-loop contribution to the mass of
a 1+1-dimensional supersymmetric soliton by adopting a set of boundary
conditions which follow from the symmetries of the action and which depend only
on the topology of the sector considered, and by invoking a physical principle
that ought ... | [
{
"created": "Wed, 11 Feb 1998 19:55:05 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Nastase",
"Horatiu",
""
],
[
"Stephanov",
"Misha",
""
],
[
"van Nieuwenhuizen",
"Peter",
""
],
[
"Rebhan",
"Anton",
""
]
] | We fix the long-standing ambiguity in the 1-loop contribution to the mass of a 1+1-dimensional supersymmetric soliton by adopting a set of boundary conditions which follow from the symmetries of the action and which depend only on the topology of the sector considered, and by invoking a physical principle that ought to... | 8.831233 | 8.771014 | 9.482801 | 8.482095 | 9.00626 | 9.027109 | 9.167255 | 8.760573 | 8.211607 | 10.398884 | 8.340331 | 8.574558 | 8.75605 | 8.315483 | 8.754631 | 8.485128 | 8.402609 | 8.500588 | 8.661281 | 8.626554 | 8.460689 |
hep-th/9110054 | Konstadinos Sfetsos | I. Bars and K. Sfetsos | Generalized Duality and Singular Strings in Higher Dimensions | 17 pages | Mod.Phys.Lett. A7 (1992) 1091-1104 | 10.1142/S0217732392000963 | null | hep-th | null | Deformations of gauged WZW actions are constructed for any pair $(G,H)$ by
taking different embeddings of the gauge group $H\subset G$ as it acts on the
left and right of the group element $g$. This leads to models that are dual to
each other, generalizing the axial/vector duality of the two dimensional black
hole ma... | [
{
"created": "Fri, 18 Oct 1991 20:36:24 GMT",
"version": "v1"
},
{
"created": "Thu, 24 Oct 1991 03:57:58 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Bars",
"I.",
""
],
[
"Sfetsos",
"K.",
""
]
] | Deformations of gauged WZW actions are constructed for any pair $(G,H)$ by taking different embeddings of the gauge group $H\subset G$ as it acts on the left and right of the group element $g$. This leads to models that are dual to each other, generalizing the axial/vector duality of the two dimensional black hole mani... | 9.108686 | 9.081653 | 10.018626 | 8.723495 | 8.524329 | 8.833259 | 8.82837 | 8.329768 | 8.859429 | 10.375243 | 8.0127 | 8.539883 | 9.087976 | 8.757063 | 8.430029 | 8.633314 | 8.447835 | 8.658105 | 8.693039 | 9.011946 | 8.616491 |
1807.07474 | Matteo Baggioli | Lasma Alberte, Matteo Baggioli, Victor Cancer Castillo, Oriol Pujolas | Elasticity bounds from Effective Field Theory | v3: erratum added to the original paper published in PRD | Phys. Rev. D 100, 065015 (2019) | 10.1103/PhysRevD.100.065015 | CCTP-2018-3, ITCP-IPP 2017/22 | hep-th cond-mat.soft cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Phonons in solid materials can be understood as the Goldstone bosons of the
spontaneously broken spacetime symmetries. As such their low energy dynamics
are greatly constrained and can be captured by standard effective field theory
(EFT) methods. In particular, knowledge of the nonlinear stress-strain curves
complete... | [
{
"created": "Thu, 19 Jul 2018 14:56:19 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Sep 2019 09:06:49 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Jun 2020 14:18:21 GMT",
"version": "v3"
}
] | 2020-06-11 | [
[
"Alberte",
"Lasma",
""
],
[
"Baggioli",
"Matteo",
""
],
[
"Castillo",
"Victor Cancer",
""
],
[
"Pujolas",
"Oriol",
""
]
] | Phonons in solid materials can be understood as the Goldstone bosons of the spontaneously broken spacetime symmetries. As such their low energy dynamics are greatly constrained and can be captured by standard effective field theory (EFT) methods. In particular, knowledge of the nonlinear stress-strain curves completely... | 9.413779 | 9.395202 | 8.971869 | 9.209414 | 9.654613 | 9.216259 | 9.338847 | 9.166574 | 8.772872 | 9.395927 | 8.974813 | 8.783244 | 8.753813 | 8.672049 | 8.500041 | 8.547853 | 8.422226 | 8.270326 | 8.615187 | 8.910011 | 8.641234 |
hep-th/0410009 | J. Mourad | J. Mourad | Continuous spin and tensionless strings | 13 pages; v2 added references; v3 discussion added | null | null | null | hep-th | null | A classical action is proposed which upon quantisation yields massless
particles belonging to the continuous spin representation of the Poincar\'e
group. The string generalisation of the action is identical to the tensionless
extrinsic curvature action proposed by Savvidy. We show that the BRST
quantisation of the st... | [
{
"created": "Fri, 1 Oct 2004 13:08:13 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Oct 2004 13:08:01 GMT",
"version": "v2"
},
{
"created": "Thu, 14 Apr 2005 14:38:02 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Mourad",
"J.",
""
]
] | A classical action is proposed which upon quantisation yields massless particles belonging to the continuous spin representation of the Poincar\'e group. The string generalisation of the action is identical to the tensionless extrinsic curvature action proposed by Savvidy. We show that the BRST quantisation of the stri... | 9.843884 | 8.811255 | 10.950388 | 8.23719 | 9.86167 | 8.66758 | 8.506378 | 8.471971 | 8.622552 | 10.551057 | 8.335865 | 8.212989 | 9.411727 | 8.587953 | 8.381128 | 8.21909 | 8.522818 | 8.423121 | 8.515071 | 9.335764 | 8.182275 |
1008.2506 | Yu-Chieh Chung | Yu-Chieh Chung | On Global Flipped SU(5) GUTs in F-theory | 45 pages, 12 tables, 1 figure; typos corrected, footnotes added, and
a reference added | JHEP 1103:126,2011 | 10.1007/JHEP03(2011)126 | MIFPA-10-38 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct an SU(4) spectral divisor and its factorization of types (3,1)
and (2,2) based on the construction proposed in [1]. We calculate the chiral
spectra of flipped SU(5) GUTs by using the spectral divisor construction. The
results agree with those from the analysis of semi-local spectral covers. Our
computati... | [
{
"created": "Sun, 15 Aug 2010 09:12:09 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Mar 2011 01:57:35 GMT",
"version": "v2"
}
] | 2011-03-31 | [
[
"Chung",
"Yu-Chieh",
""
]
] | We construct an SU(4) spectral divisor and its factorization of types (3,1) and (2,2) based on the construction proposed in [1]. We calculate the chiral spectra of flipped SU(5) GUTs by using the spectral divisor construction. The results agree with those from the analysis of semi-local spectral covers. Our computation... | 10.99629 | 10.453289 | 11.61977 | 10.067331 | 10.532581 | 10.715275 | 10.611168 | 9.455445 | 10.316016 | 12.017356 | 9.630386 | 10.38002 | 10.334301 | 10.13112 | 10.084162 | 10.230171 | 9.980683 | 10.137329 | 10.17195 | 10.563004 | 10.095735 |
hep-th/0312234 | Hiroaki Kanno | Tohru Eguchi and Hiroaki Kanno | Geometric transitions, Chern-Simons gauge theory and Veneziano type
amplitudes | 16 pages, 2 figures, (v2,3) minor changes, to appear in Phys. Lett. B | Phys.Lett. B585 (2004) 163-172 | 10.1016/j.physletb.2004.01.085 | null | hep-th | null | We consider the geometric transition and compute the all-genus topological
string amplitudes expressed in terms of Hopf link invariants and topological
vertices of Chern-Simons gauge theory. We introduce an operator technique of
2-dimensional CFT which greatly simplifies the computations. We in particular
show that i... | [
{
"created": "Fri, 19 Dec 2003 03:37:09 GMT",
"version": "v1"
},
{
"created": "Sat, 27 Dec 2003 05:47:54 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Feb 2004 05:04:57 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Eguchi",
"Tohru",
""
],
[
"Kanno",
"Hiroaki",
""
]
] | We consider the geometric transition and compute the all-genus topological string amplitudes expressed in terms of Hopf link invariants and topological vertices of Chern-Simons gauge theory. We introduce an operator technique of 2-dimensional CFT which greatly simplifies the computations. We in particular show that in ... | 10.655821 | 10.262359 | 12.928975 | 10.05197 | 11.201028 | 10.80777 | 11.593593 | 10.197702 | 10.346401 | 11.833959 | 9.796642 | 10.468021 | 11.154485 | 10.257625 | 10.847635 | 10.342085 | 10.911273 | 10.129432 | 10.248281 | 10.849625 | 10.207451 |
1811.09641 | Sa\v{s}o Grozdanov | Sa\v{s}o Grozdanov | On the connection between hydrodynamics and quantum chaos in holographic
theories with stringy corrections | V2: 20 pages, 1 figure. References added. Version to appear in JHEP | JHEP 1901 (2019) 048 | 10.1007/JHEP01(2019)048 | MIT-CTP/5085 | hep-th cond-mat.str-el gr-qc nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Pole-skipping is a recently discovered signature of many-body quantum chaos
in collective energy dynamics. It establishes a precise connection between
resummed, all-order hydrodynamics and the underlying microscopic chaos. In this
paper, we demonstrate the existence of pole-skipping in holographic conformal
field the... | [
{
"created": "Fri, 23 Nov 2018 19:00:28 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Jan 2019 14:25:57 GMT",
"version": "v2"
}
] | 2019-01-07 | [
[
"Grozdanov",
"Sašo",
""
]
] | Pole-skipping is a recently discovered signature of many-body quantum chaos in collective energy dynamics. It establishes a precise connection between resummed, all-order hydrodynamics and the underlying microscopic chaos. In this paper, we demonstrate the existence of pole-skipping in holographic conformal field theor... | 6.323231 | 5.744534 | 6.604939 | 5.757385 | 6.078165 | 6.242899 | 5.99476 | 5.871396 | 5.582611 | 6.790399 | 5.80934 | 5.876417 | 6.014463 | 5.930158 | 5.86867 | 5.984066 | 5.934333 | 6.090687 | 5.835735 | 6.011747 | 5.964316 |
hep-th/9401040 | M. B. Paranjape | T. Gisiger and M. B. Paranjape | Low Energy Skyrmion-Skyrmion Scattering | 18 pages, UdeM-LPN-TH-94-187, plain tex | Phys.Rev. D50 (1994) 1010-1015 | 10.1103/PhysRevD.50.1010 | null | hep-th | null | We study the scattering of two Skyrmions at low energy and large separation.
We use the method proposed by Manton for truncating the degrees of freedom of
the system from infinite to a manageable finite number. This corresponds to
identifying the manifold consisting of the union of the low energy critical
points of t... | [
{
"created": "Tue, 11 Jan 1994 03:55:05 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jan 1994 16:58:59 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Gisiger",
"T.",
""
],
[
"Paranjape",
"M. B.",
""
]
] | We study the scattering of two Skyrmions at low energy and large separation. We use the method proposed by Manton for truncating the degrees of freedom of the system from infinite to a manageable finite number. This corresponds to identifying the manifold consisting of the union of the low energy critical points of the... | 11.054908 | 13.076816 | 11.508374 | 11.263159 | 11.565535 | 12.18397 | 11.998172 | 11.814893 | 11.567484 | 12.262629 | 11.175695 | 11.16257 | 11.840631 | 11.140658 | 11.379533 | 10.78369 | 11.158979 | 10.777178 | 10.934258 | 11.291181 | 10.847582 |
hep-th/9310039 | null | R. Fiore, D. Galeazzi, L. Masperi and A. Megevand | Strings And Non-Topological Solitons | 12 pages. 5 figures | Mod.Phys.Lett. A9 (1994) 557-568 | 10.1142/S0217732394003798 | CNEA-CAB IT3079/DFUC | hep-th | null | We have numerically calculated topological andnon-topological solitons in two
spatial dimensions with Chern-Simons term. Their quantum stability, as well as
that of the Maxwell vortex, is analyzed by means of bounce instantons which
involve three-dimensional strings and non-topological solitons.
| [
{
"created": "Thu, 7 Oct 1993 11:59:20 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Fiore",
"R.",
""
],
[
"Galeazzi",
"D.",
""
],
[
"Masperi",
"L.",
""
],
[
"Megevand",
"A.",
""
]
] | We have numerically calculated topological andnon-topological solitons in two spatial dimensions with Chern-Simons term. Their quantum stability, as well as that of the Maxwell vortex, is analyzed by means of bounce instantons which involve three-dimensional strings and non-topological solitons. | 23.872545 | 20.839832 | 23.001028 | 20.756086 | 22.073563 | 23.443745 | 19.660812 | 20.019131 | 20.739614 | 24.056568 | 21.877876 | 20.747236 | 20.660843 | 20.011435 | 18.809807 | 20.120272 | 19.08337 | 19.798826 | 20.403687 | 20.978508 | 21.2355 |
1603.02768 | Igor Samsonov | I.L. Buchbinder, E.A. Ivanov, I.B. Samsonov | The low-energy N=4 SYM effective action in diverse harmonic superspaces | 102 pages, v2: references added | null | 10.1134/S1063779617030042 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review various superspace approaches to the description of the low-energy
effective action in N=4 super Yang-Mills (SYM) theory. We consider the
four-derivative part of the low-energy effective action in the Coulomb branch.
The typical components of this effective action are the gauge field F^4/X^4 and
the scalar ... | [
{
"created": "Wed, 9 Mar 2016 02:46:56 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Mar 2016 05:49:49 GMT",
"version": "v2"
},
{
"created": "Fri, 1 Apr 2016 06:29:27 GMT",
"version": "v3"
}
] | 2017-08-23 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Ivanov",
"E. A.",
""
],
[
"Samsonov",
"I. B.",
""
]
] | We review various superspace approaches to the description of the low-energy effective action in N=4 super Yang-Mills (SYM) theory. We consider the four-derivative part of the low-energy effective action in the Coulomb branch. The typical components of this effective action are the gauge field F^4/X^4 and the scalar fi... | 7.609569 | 6.765752 | 8.082531 | 6.806202 | 6.828207 | 6.9417 | 6.921355 | 6.540388 | 6.939953 | 9.089994 | 6.937529 | 7.177414 | 7.578386 | 6.984153 | 7.043129 | 6.887116 | 6.926663 | 6.900434 | 6.989192 | 7.651197 | 6.824272 |
hep-th/9902204 | David Fairlie | D.B. Fairlie (University of Durham) | Dirac-Born -Infeld Equations | 9 pages, LaTeX | Phys.Lett. B456 (1999) 141-146 | 10.1016/S0370-2693(99)00495-5 | DTP/99/11 | hep-th gr-qc | null | Properties of the Dirac-Born-Infeld Lagrangian analogous to those of the
Nambu-Goto String are analysed. In particular the Lagrangian is shown to be
constant or zero on the space of solutions of the equations of motion if the
Lagrangian is taken to any power other than 1/2.
| [
{
"created": "Fri, 26 Feb 1999 12:43:51 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Fairlie",
"D. B.",
"",
"University of Durham"
]
] | Properties of the Dirac-Born-Infeld Lagrangian analogous to those of the Nambu-Goto String are analysed. In particular the Lagrangian is shown to be constant or zero on the space of solutions of the equations of motion if the Lagrangian is taken to any power other than 1/2. | 7.776628 | 6.777112 | 6.625946 | 6.742505 | 6.880947 | 6.968156 | 6.035505 | 6.051405 | 7.149459 | 7.771521 | 6.335959 | 6.667619 | 6.914747 | 6.807247 | 6.665009 | 6.671881 | 6.398427 | 6.695517 | 6.688367 | 6.889364 | 6.575887 |
hep-th/0205227 | Danielsson | Ulf H. Danielsson | Inflation, holography, and the choice of vacuum in de Sitter space | 16 pages. v2: references added and improved discussion about
consistency of vacua | JHEP 0207 (2002) 040 | 10.1088/1126-6708/2002/07/040 | null | hep-th | null | A family of de Sitter vacua introduced in hep-th/0203198 as plausible initial
conditions for inflation, are discussed from the point of view of de Sitter
holography. The vacua are argued to be physically acceptable and the
inflationary picture provides a physical interpretation of a subfamily of de
Sitter invariant v... | [
{
"created": "Wed, 22 May 2002 18:14:54 GMT",
"version": "v1"
},
{
"created": "Wed, 29 May 2002 09:46:04 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Danielsson",
"Ulf H.",
""
]
] | A family of de Sitter vacua introduced in hep-th/0203198 as plausible initial conditions for inflation, are discussed from the point of view of de Sitter holography. The vacua are argued to be physically acceptable and the inflationary picture provides a physical interpretation of a subfamily of de Sitter invariant vac... | 12.42666 | 10.533191 | 11.768208 | 10.914645 | 10.680846 | 11.465853 | 10.496984 | 9.944624 | 10.163439 | 12.239436 | 10.222305 | 10.343822 | 11.481646 | 10.845103 | 10.873254 | 11.016271 | 10.890718 | 10.480148 | 10.69475 | 11.602157 | 10.579372 |
hep-th/9310140 | Fis. Teorica. Valladolid. | A. Ballesteros, F.J. Herranz, M.A. del Olmo and M. Santander | 4D Quantum Affine Algebras and Space--Time q-Symmetries | 13 pages, AMS-TEX file | J.Math.Phys. 35 (1994) 4928-4940 | 10.1063/1.530823 | UVA/93-101 | hep-th math.QA | null | A global model of $q$-deformation for the quasi--orthogonal Lie algebras
generating the groups of motions of the four--dimensional affine Cayley--Klein
geometries is obtained starting from the three dimensional deformations. It is
shown how the main algebraic classical properties of the CK systems can be
implemented ... | [
{
"created": "Thu, 21 Oct 1993 13:45:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ballesteros",
"A.",
""
],
[
"Herranz",
"F. J.",
""
],
[
"del Olmo",
"M. A.",
""
],
[
"Santander",
"M.",
""
]
] | A global model of $q$-deformation for the quasi--orthogonal Lie algebras generating the groups of motions of the four--dimensional affine Cayley--Klein geometries is obtained starting from the three dimensional deformations. It is shown how the main algebraic classical properties of the CK systems can be implemented in... | 12.650251 | 11.021114 | 12.016938 | 10.65002 | 10.871437 | 11.983561 | 11.686573 | 11.117731 | 11.087961 | 13.781095 | 11.852883 | 11.033042 | 11.164901 | 10.92555 | 10.889305 | 10.873213 | 10.809512 | 10.788291 | 11.158774 | 11.372538 | 10.750178 |
hep-th/0205184 | Andreas Brandhuber | Per Berglund, Andreas Brandhuber | Matter From G(2) Manifolds | 29 pages; v2: typos, references | Nucl.Phys. B641 (2002) 351-375 | 10.1016/S0550-3213(02)00612-0 | CITUSC/02-016, CALT-68-2385 | hep-th | null | We describe how chiral matter charged under SU(N) and SO(2N) gauge groups
arises from codimension seven singularities in compactifications of M-theory on
manifolds with G(2) holonomy. The geometry of these spaces is that of a cone
over a six-dimensional Einstein space which can be constructed by (multiple)
unfolding ... | [
{
"created": "Sat, 18 May 2002 01:48:13 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Jun 2002 09:57:56 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Berglund",
"Per",
""
],
[
"Brandhuber",
"Andreas",
""
]
] | We describe how chiral matter charged under SU(N) and SO(2N) gauge groups arises from codimension seven singularities in compactifications of M-theory on manifolds with G(2) holonomy. The geometry of these spaces is that of a cone over a six-dimensional Einstein space which can be constructed by (multiple) unfolding of... | 9.659551 | 8.53091 | 9.90254 | 8.676781 | 8.823394 | 9.291921 | 8.948271 | 8.630126 | 8.492199 | 10.655541 | 8.32435 | 8.928971 | 8.933603 | 8.700773 | 8.930859 | 8.663888 | 8.795492 | 8.670877 | 8.608563 | 9.014109 | 8.696644 |
hep-th/0501126 | Jorge Conde | Jorge Conde | Propagators from characteristic surfaces | 5 pages. To appear in the proceedings of 27th Spanish Relativity
Meeting: Beyond General Relativity (ERES 2004), Madrid, Spain, 23-25 Sep 2004 | null | null | IFT-UAM-CSIC 05-03 | hep-th | null | We study the Goursat or characteristic problem, i.e. a hyperbolic equation
with given data on a surface (the half of the standard Cauchy problem), with
some kind of dimensional regularization procedure to deal with the divergences
that appear. We will also comment some possible relation with a holographic
setup.
| [
{
"created": "Mon, 17 Jan 2005 11:42:50 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Conde",
"Jorge",
""
]
] | We study the Goursat or characteristic problem, i.e. a hyperbolic equation with given data on a surface (the half of the standard Cauchy problem), with some kind of dimensional regularization procedure to deal with the divergences that appear. We will also comment some possible relation with a holographic setup. | 18.85391 | 18.386192 | 18.504255 | 19.022705 | 17.365679 | 20.799932 | 20.098959 | 17.023727 | 17.988842 | 21.015944 | 18.237341 | 16.06011 | 19.027874 | 16.73875 | 17.051573 | 17.322908 | 16.920038 | 16.276197 | 17.183498 | 17.881683 | 16.536959 |
hep-th/9604006 | Alexey A. Deriglazov | A.A. Deriglazov and A.V. Galajinsky | The Green--Schwarz Superstring in Extended Configuration Space and
Infinitely Reducible First Class Constraints Problem | 14 pages, LaTeX | Phys.Rev. D54 (1996) 5195-5202 | 10.1103/PhysRevD.54.5195 | null | hep-th | null | The Green--Schwarz superstring action is modified to include some set of
additional (on-shell trivial) variables. A complete constraints system of the
theory turns out to be reducible both in the original and in additional
variable sectors. The initial $8s$ first class constraints and $8c$ second
class ones are shown... | [
{
"created": "Tue, 2 Apr 1996 08:57:48 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Deriglazov",
"A. A.",
""
],
[
"Galajinsky",
"A. V.",
""
]
] | The Green--Schwarz superstring action is modified to include some set of additional (on-shell trivial) variables. A complete constraints system of the theory turns out to be reducible both in the original and in additional variable sectors. The initial $8s$ first class constraints and $8c$ second class ones are shown t... | 14.736113 | 12.952337 | 17.504629 | 13.482963 | 14.476479 | 15.418349 | 14.960046 | 13.878678 | 13.301 | 17.334005 | 12.729361 | 14.617721 | 13.223941 | 13.406487 | 14.195828 | 14.012744 | 13.753818 | 14.127954 | 14.386192 | 13.946721 | 13.214293 |
1908.05962 | Mahdi Godazgar | Hadi Godazgar, Mahdi Godazgar, C.N. Pope | Taub-NUT from the Dirac monopole | 16 pages; few typos corrected | Phys.Lett.B 798 (2019) | 10.1016/j.physletb.2019.134938 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Writing the metric of an asymptotically flat spacetime in Bondi coordinates
provides an elegant way of formulating the Einstein equation as a
characteristic value problem. In this setting, we find that a specific class of
asymptotically flat spacetimes, including stationary solutions, contains a
Maxwell gauge field a... | [
{
"created": "Fri, 16 Aug 2019 13:11:12 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Feb 2021 20:37:39 GMT",
"version": "v2"
}
] | 2021-02-24 | [
[
"Godazgar",
"Hadi",
""
],
[
"Godazgar",
"Mahdi",
""
],
[
"Pope",
"C. N.",
""
]
] | Writing the metric of an asymptotically flat spacetime in Bondi coordinates provides an elegant way of formulating the Einstein equation as a characteristic value problem. In this setting, we find that a specific class of asymptotically flat spacetimes, including stationary solutions, contains a Maxwell gauge field as ... | 10.4247 | 9.141651 | 8.454559 | 7.580615 | 9.10555 | 8.46082 | 8.366552 | 8.066314 | 8.71417 | 8.95075 | 8.187192 | 8.277582 | 8.074384 | 8.231794 | 8.500142 | 8.515808 | 8.311048 | 8.479843 | 8.450342 | 8.083797 | 8.442568 |
1304.6016 | Helv\'ecio Geovani Fargnoli Filho | L. C. T. Brito, H. G. Fargnoli, A. P. Ba\^eta Scarpelli | Aspects of Quantum Corrections in a Lorentz-violating Extension of the
Abelian Higgs Model | Subtle changes to match the published version. Some references added | Phys. Rev. D 87, 125023 (2013) | 10.1103/PhysRevD.87.125023 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate new aspects related to the abelian gauge-Higgs model with the
addition of the Carroll-Field-Jackiw term. We focus on one-loop quantum
corrections to the photon and Higgs sectors due to spontaneous breaking of
gauge symmetry and show that new finite and definite Lorentz-breaking terms are
induced. Speci... | [
{
"created": "Mon, 22 Apr 2013 16:57:53 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jul 2013 18:52:51 GMT",
"version": "v2"
}
] | 2013-07-11 | [
[
"Brito",
"L. C. T.",
""
],
[
"Fargnoli",
"H. G.",
""
],
[
"Scarpelli",
"A. P. Baêta",
""
]
] | We investigate new aspects related to the abelian gauge-Higgs model with the addition of the Carroll-Field-Jackiw term. We focus on one-loop quantum corrections to the photon and Higgs sectors due to spontaneous breaking of gauge symmetry and show that new finite and definite Lorentz-breaking terms are induced. Specifi... | 12.827823 | 10.843592 | 14.044452 | 11.396238 | 11.353157 | 11.049237 | 10.8694 | 11.095459 | 10.943879 | 13.959572 | 10.578002 | 12.111189 | 12.53626 | 11.83487 | 12.363712 | 11.61666 | 11.830963 | 12.034098 | 11.793867 | 13.199753 | 11.619721 |
hep-th/9409120 | null | T. A. Osborn and F. H. Molzahn | Moyal Quantum Mechanics: The Semiclassical Heisenberg Dynamics | 50, MANIT-94-01 | Annals Phys. 241 (1995) 79-127 | 10.1006/aphy.1995.1057 | null | hep-th | null | The Moyal--Weyl description of quantum mechanics provides a comprehensive
phase space representation of dynamics. The Weyl symbol image of the Heisenberg
picture evolution operator is regular in $\hbar$. Its semiclassical expansion
`coefficients,' acting on symbols that represent observables, are simple,
globally def... | [
{
"created": "Wed, 21 Sep 1994 03:08:31 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Osborn",
"T. A.",
""
],
[
"Molzahn",
"F. H.",
""
]
] | The Moyal--Weyl description of quantum mechanics provides a comprehensive phase space representation of dynamics. The Weyl symbol image of the Heisenberg picture evolution operator is regular in $\hbar$. Its semiclassical expansion `coefficients,' acting on symbols that represent observables, are simple, globally defin... | 13.20069 | 15.640812 | 15.136838 | 13.702193 | 14.398634 | 14.781326 | 14.102873 | 15.210853 | 14.168308 | 14.98512 | 14.068095 | 12.493856 | 13.555233 | 12.802567 | 13.255651 | 12.647715 | 12.684524 | 12.917892 | 12.924882 | 13.620488 | 12.71787 |
2305.09451 | Roland Bittleston | Roland Bittleston, Simon Heuveline and David Skinner | The Celestial Chiral Algebra of Self-Dual Gravity on Eguchi-Hanson Space | 33 pages + 12 page appendix, 3 figures; v2: published in JHEP | JHEP 09 (2023) 008 | 10.1007/JHEP09(2023)008 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the twistor description of classical self-dual Einstein gravity
in the presence of a defect operator wrapping a certain $\mathbb{CP}^1$. The
backreaction of this defect deforms the flat twistor space to that of
Eguchi-Hanson space. We show that the celestial chiral algebra of self-dual
gravity on the Eguc... | [
{
"created": "Tue, 16 May 2023 14:13:46 GMT",
"version": "v1"
},
{
"created": "Sat, 2 Sep 2023 13:12:51 GMT",
"version": "v2"
}
] | 2023-09-06 | [
[
"Bittleston",
"Roland",
""
],
[
"Heuveline",
"Simon",
""
],
[
"Skinner",
"David",
""
]
] | We consider the twistor description of classical self-dual Einstein gravity in the presence of a defect operator wrapping a certain $\mathbb{CP}^1$. The backreaction of this defect deforms the flat twistor space to that of Eguchi-Hanson space. We show that the celestial chiral algebra of self-dual gravity on the Eguchi... | 7.772061 | 7.518778 | 8.206385 | 6.872962 | 7.813103 | 7.191358 | 7.359842 | 7.189196 | 7.038614 | 9.001803 | 6.816364 | 7.361382 | 7.427977 | 7.077456 | 7.450433 | 7.410684 | 7.318279 | 7.178545 | 7.251747 | 7.699138 | 7.112085 |
2408.06791 | Pawel Caputa | Pawel Caputa, Souradeep Purkayastha, Abhigyan Saha, Piotr Su{\l}kowski | Musings on SVD and pseudo entanglement entropies | 52 pages, 20 figures | null | null | CALT-2024-029, YITP-24-97 | hep-th math-ph math.MP math.QA quant-ph | http://creativecommons.org/licenses/by/4.0/ | Pseudo-entropy and SVD entropy are generalizations of the entanglement
entropy that involve post-selection. In this work we analyze their properties
as measures on the spaces of quantum states and argue that their excess
provides useful characterization of a difference between two (i.e. pre-selected
and post-selected... | [
{
"created": "Tue, 13 Aug 2024 10:23:52 GMT",
"version": "v1"
}
] | 2024-08-14 | [
[
"Caputa",
"Pawel",
""
],
[
"Purkayastha",
"Souradeep",
""
],
[
"Saha",
"Abhigyan",
""
],
[
"Sułkowski",
"Piotr",
""
]
] | Pseudo-entropy and SVD entropy are generalizations of the entanglement entropy that involve post-selection. In this work we analyze their properties as measures on the spaces of quantum states and argue that their excess provides useful characterization of a difference between two (i.e. pre-selected and post-selected) ... | 12.731131 | 11.87586 | 13.615114 | 11.573482 | 12.121845 | 12.223356 | 12.197159 | 11.054718 | 10.292991 | 14.627549 | 11.947837 | 11.440379 | 12.468804 | 11.728806 | 11.657248 | 11.561672 | 11.663817 | 11.61053 | 11.579893 | 12.180287 | 12.180144 |
hep-th/0607007 | Tom Banks | T. Banks | II_{\infty} Factors and M-theory in Asymptotically Flat Space-Time | JHEP LaTex, 20 pages | null | null | RU-06-08, SCIPP-06-07 | hep-th | null | I discuss a formulation of M-theory at null infinity, which is based on
general principles of holographic space-time, and is manifestly covariant. The
construction utilizes a certain Type II Von Neumann algebra, which provides a
kinematic framework, alternative to Fock Space, for describing the scattering
states of e... | [
{
"created": "Mon, 3 Jul 2006 19:18:45 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Banks",
"T.",
""
]
] | I discuss a formulation of M-theory at null infinity, which is based on general principles of holographic space-time, and is manifestly covariant. The construction utilizes a certain Type II Von Neumann algebra, which provides a kinematic framework, alternative to Fock Space, for describing the scattering states of ele... | 18.325613 | 16.302986 | 18.759642 | 17.015892 | 17.457947 | 15.83835 | 17.591988 | 18.353287 | 16.228062 | 20.884424 | 15.859685 | 15.89821 | 17.354818 | 16.25182 | 15.851021 | 15.545316 | 15.408908 | 16.404219 | 16.539412 | 17.085062 | 15.891627 |
hep-th/9802157 | Matteo Buzzacchi | She-Sheng Xue | Whether composite fermion states with ``wrong'' chiralities dissolve
into cuts | 24 pages, LaTex and 6 Feynman diagrams are not included | null | null | null | hep-th hep-lat hep-ph | null | In the possible scaling region for lattice chiral fermions advocated in
hep-lat/9609037, no hard spontaneous symmetry breaking occurs and doublers are
gauge-invariantly decoupled via mixing with composite three-fermion-states.
However the strong coupling expansion breaks down due to no ``static limit''
for the low-en... | [
{
"created": "Mon, 23 Feb 1998 08:56:52 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Xue",
"She-Sheng",
""
]
] | In the possible scaling region for lattice chiral fermions advocated in hep-lat/9609037, no hard spontaneous symmetry breaking occurs and doublers are gauge-invariantly decoupled via mixing with composite three-fermion-states. However the strong coupling expansion breaks down due to no ``static limit'' for the low-ener... | 14.553076 | 14.63798 | 14.476734 | 13.304576 | 17.356871 | 14.704444 | 15.096504 | 14.245709 | 13.327314 | 14.801036 | 13.545454 | 13.633851 | 13.16932 | 13.407011 | 13.522676 | 13.618855 | 13.214495 | 13.569096 | 13.210841 | 13.707976 | 13.576402 |
1603.09183 | Roldao da Rocha | R. J. Bueno Rogerio, J. M. Hoff da Silva, S. H. Pereira, Roldao da
Rocha | A framework to a mass dimension one fermionic sigma model | 6 pages, to appear in EPL | Europhysics Letters 113 (2016) 60001 | 10.1209/0295-5075/113/60001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper a mass dimension one fermionic sigma model, realized by the
eigenspinors of the charge conjugation operator with dual helicity (Elko
spinors), is developed. Such spinors are chosen as a specific realization of
mass dimension one spinors, wherein the non-commutative fermionic feature is
ruled by torsion.... | [
{
"created": "Wed, 30 Mar 2016 13:32:11 GMT",
"version": "v1"
}
] | 2016-04-06 | [
[
"Rogerio",
"R. J. Bueno",
""
],
[
"da Silva",
"J. M. Hoff",
""
],
[
"Pereira",
"S. H.",
""
],
[
"da Rocha",
"Roldao",
""
]
] | In this paper a mass dimension one fermionic sigma model, realized by the eigenspinors of the charge conjugation operator with dual helicity (Elko spinors), is developed. Such spinors are chosen as a specific realization of mass dimension one spinors, wherein the non-commutative fermionic feature is ruled by torsion. M... | 11.660211 | 11.269265 | 11.059532 | 10.733311 | 10.828883 | 10.631875 | 11.088067 | 10.261867 | 10.626918 | 11.579491 | 10.955755 | 11.749198 | 11.811409 | 11.110875 | 10.693464 | 11.25279 | 11.027068 | 10.873599 | 11.240855 | 11.283877 | 11.52122 |
hep-th/9608020 | Kazuo Gouroku | Kazuo Ghoroku | String loop correction and the condensation of tachyon in 2d gravity | 13 pages, latex | null | null | FIT-HE-96-81 | hep-th | null | Quantum theory of 2d gravity is examined by including a special quantum
correction, which corresponds to the open string loop corrections and provides
a new conformal anomaly for the corresponding $\sigma$ model. This anomaly
leads to the condensation of the tachyon, and the resultant effective theory
implies a possi... | [
{
"created": "Mon, 5 Aug 1996 03:03:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ghoroku",
"Kazuo",
""
]
] | Quantum theory of 2d gravity is examined by including a special quantum correction, which corresponds to the open string loop corrections and provides a new conformal anomaly for the corresponding $\sigma$ model. This anomaly leads to the condensation of the tachyon, and the resultant effective theory implies a possibi... | 15.286749 | 13.786596 | 14.643387 | 12.809254 | 12.154938 | 12.683193 | 12.701835 | 12.369075 | 13.064116 | 13.799483 | 12.755455 | 13.471915 | 13.774505 | 12.851605 | 13.272346 | 12.938031 | 13.407001 | 13.343325 | 13.175734 | 14.023787 | 13.073062 |
hep-th/9710121 | Shahin S. Jabbari | M.M. Sheikh-Jabbari | Classification of Different Branes at Angles | Tex, 11 page, no figures | Phys.Lett.B420:279-284,1998 | 10.1016/S0370-2693(97)01550-5 | IPM-97-247 | hep-th | null | In this paper, we consider two D-branes rotated with respect to each other,
and argue that in this way one can find brane configurations preserving ${1 \f
16}$ of SUSY. Also we classify different brane configurations preserving ${1 \f
2}$, ${1 \f 4}$, ${3 \f 16}$,${1 \f 8}$, ${1 \f 16}$ of SUSY.
| [
{
"created": "Wed, 15 Oct 1997 13:31:29 GMT",
"version": "v1"
}
] | 2009-10-07 | [
[
"Sheikh-Jabbari",
"M. M.",
""
]
] | In this paper, we consider two D-branes rotated with respect to each other, and argue that in this way one can find brane configurations preserving ${1 \f 16}$ of SUSY. Also we classify different brane configurations preserving ${1 \f 2}$, ${1 \f 4}$, ${3 \f 16}$,${1 \f 8}$, ${1 \f 16}$ of SUSY. | 6.594149 | 5.821845 | 6.487501 | 5.413968 | 5.419781 | 5.391132 | 5.8303 | 6.163966 | 5.432716 | 7.334363 | 5.218465 | 5.521993 | 5.941828 | 5.593618 | 5.630194 | 5.613656 | 5.463368 | 5.813092 | 5.208012 | 5.806189 | 5.369478 |
1405.4266 | Ilarion Melnikov | Marco Bertolini, Ilarion V. Melnikov, and M. Ronen Plesser | Accidents in (0,2) Landau-Ginzburg theories | 37 pages; expanded conformal perturbation theory discussion in v2;
fixed an accident in section 3.5 in v3 | null | 10.1007/JHEP12(2014)157 | MIFPA-14-17, NSF-KITP-14-043 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the role of accidental symmetries in two-dimensional (0,2)
superconformal field theories obtained by RG flow from (0,2) Landau-Ginzburg
theories. These accidental symmetries are ubiquitous, and, unlike in the case
of (2,2) theories, their identification is key to correctly identifying the IR
fixed point and ... | [
{
"created": "Fri, 16 May 2014 18:42:58 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Oct 2014 15:47:54 GMT",
"version": "v2"
},
{
"created": "Thu, 23 Oct 2014 14:54:07 GMT",
"version": "v3"
}
] | 2015-06-19 | [
[
"Bertolini",
"Marco",
""
],
[
"Melnikov",
"Ilarion V.",
""
],
[
"Plesser",
"M. Ronen",
""
]
] | We study the role of accidental symmetries in two-dimensional (0,2) superconformal field theories obtained by RG flow from (0,2) Landau-Ginzburg theories. These accidental symmetries are ubiquitous, and, unlike in the case of (2,2) theories, their identification is key to correctly identifying the IR fixed point and it... | 5.81266 | 5.38175 | 6.660847 | 5.404954 | 5.52604 | 5.614427 | 5.135389 | 5.21157 | 5.25373 | 6.731456 | 5.30465 | 5.215349 | 5.799037 | 5.376859 | 5.215555 | 5.153489 | 5.160813 | 5.094828 | 5.220509 | 5.858788 | 5.287015 |
hep-th/0208071 | Kiwoon Choi | Kiwoon Choi and Ian-Woo Kim | One loop gauge couplings in AdS5 | RevTeX, 22 pages, 2 figures, some typos corrected and notations
changed | Phys.Rev. D67 (2003) 045005 | 10.1103/PhysRevD.67.045005 | KAIST-TH 02/18 | hep-th hep-ph | null | We calculate the full 1-loop corrections to the low energy coupling of bulk
gauge boson in a slice of AdS5 which are induced by generic 5-dimensional
scalar, Dirac fermion, and vector fields with arbitrary Z_2 times Z_2' orbifold
boundary conditions. In supersymmetric limit, our results correctly reproduce
the result... | [
{
"created": "Fri, 9 Aug 2002 13:26:24 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Sep 2002 15:06:18 GMT",
"version": "v2"
},
{
"created": "Sat, 10 Jan 2004 03:49:24 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Choi",
"Kiwoon",
""
],
[
"Kim",
"Ian-Woo",
""
]
] | We calculate the full 1-loop corrections to the low energy coupling of bulk gauge boson in a slice of AdS5 which are induced by generic 5-dimensional scalar, Dirac fermion, and vector fields with arbitrary Z_2 times Z_2' orbifold boundary conditions. In supersymmetric limit, our results correctly reproduce the results ... | 9.813295 | 9.46535 | 8.417025 | 7.926211 | 9.519759 | 9.943215 | 9.210284 | 9.008883 | 8.698427 | 8.454083 | 8.700062 | 8.876202 | 9.046199 | 8.115643 | 8.949455 | 9.267738 | 8.774315 | 8.933543 | 8.159542 | 8.762894 | 8.696497 |
hep-th/0307286 | Bindu Anubha Bambah | B. Bambah (1), C. Mukku (2) ((1) University of Hyderabad, Hyderabad,
India, (2) Panjab University, Chandigarh, India) | Charged vs. Neutral particle creation in expanding Universes: A Quantum
Field Theoretic Treatment | Presented by B. Bambah at the International Congress of Mathematical
Physics, 2003 held in Lisbon, Portugal, July 2003 | null | null | null | hep-th gr-qc | null | A complete quantum field theoretic study of charged and neutral particle
creation in a rapidly/adiabatically expanding Friedman-Robertson-Walker metric
for an O(4) scalar field theory with quartic interactions (admitting a phase
transition) is given. Quantization is carried out by inclusion of quantum
fluctuations. W... | [
{
"created": "Wed, 30 Jul 2003 04:40:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bambah",
"B.",
""
],
[
"Mukku",
"C.",
""
]
] | A complete quantum field theoretic study of charged and neutral particle creation in a rapidly/adiabatically expanding Friedman-Robertson-Walker metric for an O(4) scalar field theory with quartic interactions (admitting a phase transition) is given. Quantization is carried out by inclusion of quantum fluctuations. We ... | 11.582359 | 11.452703 | 10.091896 | 9.948119 | 10.493809 | 11.11349 | 11.410102 | 10.452325 | 10.879521 | 10.837179 | 10.686188 | 10.638627 | 10.093535 | 10.128079 | 10.595563 | 10.840004 | 10.63345 | 10.712738 | 10.465132 | 10.571233 | 10.465665 |
1108.3771 | Papantonopoulos Eleftherios | Bertha Cuadros-Melgar, Eleftherios Papantonopoulos, Minas Tsoukalas
and Vassilios Zamarias | Massive Gravity with Anisotropic Scaling | 16 pages, 4 figures, change of title, discussion on the effect of
Lorentz violating mass terms is added. To appear in PRD. arXiv admin note:
text overlap with arXiv:0911.1299 | Phys. Rev. D85, 124035 (2012) | 10.1103/PhysRevD.85.124035 | null | hep-th gr-qc | http://creativecommons.org/licenses/by-nc-sa/3.0/ | We study a massive gravity theory which is Lorentz violating all the way from
ultraviolet to infrared energy scales. At short distances the theory breaks
diffeomorphism invariance and time and space scale differently. Dynamical
metric fields are introduced which upon linearization over a Minkowski
background correspo... | [
{
"created": "Thu, 18 Aug 2011 14:52:32 GMT",
"version": "v1"
},
{
"created": "Fri, 18 May 2012 12:02:32 GMT",
"version": "v2"
}
] | 2012-07-13 | [
[
"Cuadros-Melgar",
"Bertha",
""
],
[
"Papantonopoulos",
"Eleftherios",
""
],
[
"Tsoukalas",
"Minas",
""
],
[
"Zamarias",
"Vassilios",
""
]
] | We study a massive gravity theory which is Lorentz violating all the way from ultraviolet to infrared energy scales. At short distances the theory breaks diffeomorphism invariance and time and space scale differently. Dynamical metric fields are introduced which upon linearization over a Minkowski background correspond... | 10.268394 | 9.75012 | 8.804609 | 9.416431 | 10.074597 | 10.299572 | 10.216794 | 9.362748 | 9.434504 | 9.812914 | 9.336082 | 10.135038 | 9.358751 | 9.536513 | 9.450427 | 9.746415 | 9.66971 | 9.566808 | 9.470057 | 9.801195 | 9.540795 |
hep-th/0405018 | Charles B. Thorn | Charles B. Thorn | Renormalization of Quantum Fields on the Lightcone Worldsheet I: Scalar
Fields | 18 pages, 3 figures | Nucl.Phys. B699 (2004) 427-452 | 10.1016/j.nuclphysb.2004.08.028 | null | hep-th | null | We show that the lightcone worldsheet formalism, constructed to represent the
sum of the bare planar diagrams of scalar \phi^3 field theory, survives the
renormalization procedure in space-time dimensions D not greater than 6.
Specifically this means that all the counter-terms, necessary to produce a
successful renor... | [
{
"created": "Mon, 3 May 2004 19:07:18 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Thorn",
"Charles B.",
""
]
] | We show that the lightcone worldsheet formalism, constructed to represent the sum of the bare planar diagrams of scalar \phi^3 field theory, survives the renormalization procedure in space-time dimensions D not greater than 6. Specifically this means that all the counter-terms, necessary to produce a successful renorma... | 8.668943 | 8.429306 | 9.867319 | 8.088407 | 8.571173 | 8.088418 | 8.405644 | 7.991775 | 8.179029 | 9.595537 | 7.934245 | 8.574399 | 8.751015 | 8.452089 | 8.451321 | 8.302279 | 8.367976 | 8.571707 | 8.696755 | 8.951524 | 8.32999 |
hep-th/0512037 | Mahdi Torabian | M. Ali-Akbari, M. M. Sheikh-Jabbari, M. Torabian | Extensions of AdS_5 x S^5 and the Plane-wave Superalgebras and Their
Realization in the Tiny Graviton Matrix Theory | 27 pages, LaTeX | JHEP 0603:065,2006 | 10.1088/1126-6708/2006/03/065 | IPM/P-2005/080 | hep-th | null | In this paper we consider all consistent extensions of the AdS_5 x S^5
superalgebra, psu(2,2|4), to incorporate brane charges by introducing both
bosonic and fermionic (non)central extensions. We study the Inonu-Wigner
contraction of the extended psu(2,2|4) under the Penrose limit to obtain the
most general consisten... | [
{
"created": "Sun, 4 Dec 2005 16:32:02 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Dec 2005 15:22:55 GMT",
"version": "v2"
},
{
"created": "Sat, 24 Dec 2005 11:30:05 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Ali-Akbari",
"M.",
""
],
[
"Sheikh-Jabbari",
"M. M.",
""
],
[
"Torabian",
"M.",
""
]
] | In this paper we consider all consistent extensions of the AdS_5 x S^5 superalgebra, psu(2,2|4), to incorporate brane charges by introducing both bosonic and fermionic (non)central extensions. We study the Inonu-Wigner contraction of the extended psu(2,2|4) under the Penrose limit to obtain the most general consistent ... | 7.599581 | 6.681377 | 9.41074 | 6.527012 | 7.43479 | 6.84439 | 6.876698 | 6.633163 | 6.135808 | 9.389688 | 6.469432 | 6.944211 | 7.620777 | 6.793029 | 6.911248 | 7.061771 | 6.867427 | 6.804729 | 7.059381 | 7.334775 | 6.838296 |
hep-th/0608199 | Saharian | E.R. Bezerra de Mello, A.A. Saharian | Vacuum polarization by a composite topological defect | 11 pages, 2 figures | Phys.Lett.B642:129-136,2006 | 10.1016/j.physletb.2006.09.014 | null | hep-th gr-qc quant-ph | null | In this paper we analyze one-loop quantum effects of a scalar field induced
by a composite topological defect consisting a cosmic string on a p-dimensional
brane and a (m+1)-dimensional global monopole in the transverse extra
dimensions. The corresponding Green function is presented as a sum of two
terms. The first o... | [
{
"created": "Mon, 28 Aug 2006 12:30:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Saharian",
"A. A.",
""
]
] | In this paper we analyze one-loop quantum effects of a scalar field induced by a composite topological defect consisting a cosmic string on a p-dimensional brane and a (m+1)-dimensional global monopole in the transverse extra dimensions. The corresponding Green function is presented as a sum of two terms. The first one... | 8.043823 | 4.856333 | 8.065298 | 6.467927 | 5.979892 | 5.595441 | 5.694668 | 6.170407 | 6.142868 | 9.144361 | 6.010631 | 6.164742 | 7.62809 | 6.812711 | 6.889689 | 6.41358 | 6.530711 | 6.971577 | 6.847705 | 8.30988 | 6.960555 |
1512.01226 | Anirbit | Anirbit Mukherjee | Renyi entropy of the critical O(N) model | 20 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we explore a certain definition of "alternate quantization"
for the critical O(N) model. We elaborate on a prescription to evaluate the
Renyi entropy of alternately quantized critical O(N) model. We show that there
exists new saddles of the q-Renyi free energy functional corresponding to
putting certa... | [
{
"created": "Thu, 3 Dec 2015 20:56:16 GMT",
"version": "v1"
}
] | 2015-12-04 | [
[
"Mukherjee",
"Anirbit",
""
]
] | In this article we explore a certain definition of "alternate quantization" for the critical O(N) model. We elaborate on a prescription to evaluate the Renyi entropy of alternately quantized critical O(N) model. We show that there exists new saddles of the q-Renyi free energy functional corresponding to putting certain... | 18.806282 | 17.243126 | 17.755369 | 14.965173 | 15.634638 | 15.385204 | 16.686394 | 16.616718 | 17.033146 | 17.598763 | 15.68408 | 15.593442 | 17.260878 | 15.999036 | 15.372496 | 15.738256 | 15.972451 | 16.030069 | 15.805249 | 17.335358 | 16.547132 |
1803.08985 | P Klimas | L.A. Ferreira, P. Klimas, A. Wereszczynski and W.J. Zakrzewski | Some Comments on BPS systems | 27 pages, 17 figures | null | 10.1088/1751-8121/ab2ae6 | null | hep-th nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We look at simple BPS systems involving more than one field. We discuss the
conditions that have to be imposed on various terms in Lagrangians involving
many fields to produce BPS systems and then look in more detail at the simplest
of such cases. We analyse in detail BPS systems involving 2 interacting
Sine-Gordon l... | [
{
"created": "Fri, 23 Mar 2018 21:29:19 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Jan 2019 14:07:30 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"Ferreira",
"L. A.",
""
],
[
"Klimas",
"P.",
""
],
[
"Wereszczynski",
"A.",
""
],
[
"Zakrzewski",
"W. J.",
""
]
] | We look at simple BPS systems involving more than one field. We discuss the conditions that have to be imposed on various terms in Lagrangians involving many fields to produce BPS systems and then look in more detail at the simplest of such cases. We analyse in detail BPS systems involving 2 interacting Sine-Gordon lik... | 10.512268 | 9.392998 | 11.067654 | 9.876859 | 9.334684 | 9.456115 | 9.941213 | 9.780706 | 9.094213 | 11.578656 | 9.479872 | 9.590106 | 10.276316 | 9.939734 | 9.811623 | 9.720508 | 9.806316 | 9.762726 | 10.220548 | 10.140824 | 9.603523 |
2302.08569 | Giovanni Amelino-Camelia | Giovanni Amelino-Camelia, Giuseppe Fabiano, Domenico Frattulillo | Total momentum and other Noether charges for particles interacting in a
quantum spacetime | 9 pages, Latex | null | null | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There has been strong interest in the fate of relativistic symmetries in some
quantum spacetimes, also because of its possible relevance for high-precision
experimental tests of relativistic properties. However, the main technical
results obtained so far concern the description of suitably deformed
relativistic-symme... | [
{
"created": "Thu, 16 Feb 2023 20:30:48 GMT",
"version": "v1"
}
] | 2023-02-20 | [
[
"Amelino-Camelia",
"Giovanni",
""
],
[
"Fabiano",
"Giuseppe",
""
],
[
"Frattulillo",
"Domenico",
""
]
] | There has been strong interest in the fate of relativistic symmetries in some quantum spacetimes, also because of its possible relevance for high-precision experimental tests of relativistic properties. However, the main technical results obtained so far concern the description of suitably deformed relativistic-symmetr... | 13.66134 | 13.831905 | 14.341905 | 12.837166 | 14.100301 | 13.383109 | 14.006673 | 12.507182 | 12.772697 | 14.678596 | 12.691602 | 13.075917 | 12.736845 | 12.656797 | 12.622296 | 12.870343 | 12.845821 | 12.549041 | 12.525832 | 12.940022 | 13.105306 |
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