id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1802.10263 | Grigory Tarnopolsky | Igor R. Klebanov, Alexey Milekhin, Fedor Popov, Grigory Tarnopolsky | Spectra of Eigenstates in Fermionic Tensor Quantum Mechanics | 42 pages, 1 figure. v2: minor improvements, references added. v3:
minor corrections. v4: minor improvements | Phys. Rev. D 97, 106023 (2018) | 10.1103/PhysRevD.97.106023 | PUPT-2552 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the $O(N_1)\times O(N_2)\times O(N_3)$ symmetric quantum mechanics
of 3-index Majorana fermions. When the ranks $N_i$ are all equal, this model
has a large $N$ limit which is dominated by the melonic Feynman diagrams. We
derive an integral formula which computes the number of $SO(N_1)\times
SO(N_2)\times SO(... | [
{
"created": "Wed, 28 Feb 2018 05:06:35 GMT",
"version": "v1"
},
{
"created": "Sun, 25 Mar 2018 22:19:21 GMT",
"version": "v2"
},
{
"created": "Thu, 5 Jul 2018 06:55:04 GMT",
"version": "v3"
},
{
"created": "Tue, 31 Jul 2018 03:03:52 GMT",
"version": "v4"
}
] | 2018-08-01 | [
[
"Klebanov",
"Igor R.",
""
],
[
"Milekhin",
"Alexey",
""
],
[
"Popov",
"Fedor",
""
],
[
"Tarnopolsky",
"Grigory",
""
]
] | We study the $O(N_1)\times O(N_2)\times O(N_3)$ symmetric quantum mechanics of 3-index Majorana fermions. When the ranks $N_i$ are all equal, this model has a large $N$ limit which is dominated by the melonic Feynman diagrams. We derive an integral formula which computes the number of $SO(N_1)\times SO(N_2)\times SO(N_... | 5.419546 | 5.493606 | 5.862377 | 5.146841 | 5.216193 | 5.307472 | 4.971683 | 5.285882 | 5.15624 | 5.947873 | 5.011661 | 5.325127 | 5.525027 | 5.203315 | 5.14915 | 5.373657 | 5.282782 | 5.274541 | 5.273926 | 5.631748 | 5.228801 |
0705.3532 | Hiroaki Nakajima | Katsushi Ito, Hiroaki Nakajima, Shin Sasaki | Deformation of Super Yang-Mills Theories in R-R 3-form Background | v2: reference added, v3: published version in JHEP | JHEP 0707:068,2007 | 10.1088/1126-6708/2007/07/068 | TIT/HEP-572, HIP-2007-29/TH | hep-th | null | We study deformation of N=2 and N=4 super Yang-Mills theories, which are
obtained as the low-energy effective theories on the (fractional) D3-branes in
the presence of constant Ramond-Ramond 3-form background. We calculate the
Lagrangian at the second order in the deformation parameter from open string
disk amplitude... | [
{
"created": "Thu, 24 May 2007 09:10:24 GMT",
"version": "v1"
},
{
"created": "Thu, 31 May 2007 05:33:49 GMT",
"version": "v2"
},
{
"created": "Sat, 28 Jul 2007 12:44:21 GMT",
"version": "v3"
}
] | 2009-04-17 | [
[
"Ito",
"Katsushi",
""
],
[
"Nakajima",
"Hiroaki",
""
],
[
"Sasaki",
"Shin",
""
]
] | We study deformation of N=2 and N=4 super Yang-Mills theories, which are obtained as the low-energy effective theories on the (fractional) D3-branes in the presence of constant Ramond-Ramond 3-form background. We calculate the Lagrangian at the second order in the deformation parameter from open string disk amplitudes.... | 6.405816 | 5.307986 | 6.626828 | 5.556066 | 5.2554 | 5.515464 | 5.341231 | 5.391045 | 5.633172 | 6.96233 | 5.442156 | 6.007934 | 6.519401 | 5.918594 | 5.720448 | 5.674235 | 5.730266 | 5.813176 | 5.896821 | 6.373611 | 5.860932 |
hep-th/0401191 | Giovanni Felder | Giovanni Felder and Roman Riser (ETH Zurich) | Holomorphic matrix integrals | 9 pages, 1 figure, reference added | Nucl.Phys. B691 (2004) 251-258 | 10.1016/j.nuclphysb.2004.05.010 | null | hep-th | null | We study a class of holomorphic matrix models. The integrals are taken over
middle dimensional cycles in the space of complex square matrices. As the size
of the matrices tends to infinity, the distribution of eigenvalues is given by
a measure with support on a collection of arcs in the complex planes. We show
that t... | [
{
"created": "Mon, 26 Jan 2004 07:02:23 GMT",
"version": "v1"
},
{
"created": "Fri, 6 Feb 2004 15:35:57 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Felder",
"Giovanni",
"",
"ETH Zurich"
],
[
"Riser",
"Roman",
"",
"ETH Zurich"
]
] | We study a class of holomorphic matrix models. The integrals are taken over middle dimensional cycles in the space of complex square matrices. As the size of the matrices tends to infinity, the distribution of eigenvalues is given by a measure with support on a collection of arcs in the complex planes. We show that the... | 9.169962 | 9.100631 | 9.675649 | 8.390651 | 9.377381 | 9.257697 | 8.096177 | 7.928234 | 8.703091 | 10.288461 | 8.003375 | 8.128619 | 8.641857 | 8.20905 | 8.191593 | 8.136947 | 8.214361 | 8.160715 | 7.886891 | 8.386965 | 7.929101 |
0808.1357 | Carlo Angelantonj | C. Angelantonj, C. Kounnas, H. Partouche and N. Toumbas | Resolution of Hagedorn singularity in superstrings with gravito-magnetic
fluxes | LaTeX, 1+23 pages. v2 Section 2.1 expanded. Misprints corrected. To
appear in Nuclear Physics B | Nucl.Phys.B809:291-307,2009 | 10.1016/j.nuclphysb.2008.10.010 | LPTENS 08/43, CPHT-RR055.0708, DFTT 24/2008 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider closed type II and orientifold backgrounds where supersymmetry is
spontaneously broken by asymmetric geometrical fluxes. We show that these can
be used to describe thermal ensembles with chemical potentials associated to
"gravito-magnetic" fluxes. The thermal free energy is computed at the one-loop
string... | [
{
"created": "Sat, 9 Aug 2008 14:16:31 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Nov 2008 14:22:14 GMT",
"version": "v2"
}
] | 2008-12-18 | [
[
"Angelantonj",
"C.",
""
],
[
"Kounnas",
"C.",
""
],
[
"Partouche",
"H.",
""
],
[
"Toumbas",
"N.",
""
]
] | We consider closed type II and orientifold backgrounds where supersymmetry is spontaneously broken by asymmetric geometrical fluxes. We show that these can be used to describe thermal ensembles with chemical potentials associated to "gravito-magnetic" fluxes. The thermal free energy is computed at the one-loop string l... | 7.78426 | 8.115989 | 8.645891 | 8.36987 | 8.298246 | 8.349116 | 8.346766 | 8.264194 | 7.777624 | 9.65169 | 7.747066 | 7.726941 | 7.880942 | 7.6623 | 7.584913 | 7.73649 | 7.681053 | 7.741584 | 7.613527 | 7.771722 | 7.618423 |
2407.04789 | Bin Zhu | Romain Ruzziconi, Stephan Stieberger, Tomasz R. Taylor, Bin Zhu | Differential Equations for Carrollian Amplitudes | 29 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Differential equations are powerful tools in the study of correlation
functions in conformal field theories (CFTs). Carrollian amplitudes behave as
correlation functions of Carrollian CFT that holographically describes
asymptotically flat spacetime. We derive linear differential equations
satisfied by Carrollian MHV ... | [
{
"created": "Fri, 5 Jul 2024 18:04:05 GMT",
"version": "v1"
}
] | 2024-07-09 | [
[
"Ruzziconi",
"Romain",
""
],
[
"Stieberger",
"Stephan",
""
],
[
"Taylor",
"Tomasz R.",
""
],
[
"Zhu",
"Bin",
""
]
] | Differential equations are powerful tools in the study of correlation functions in conformal field theories (CFTs). Carrollian amplitudes behave as correlation functions of Carrollian CFT that holographically describes asymptotically flat spacetime. We derive linear differential equations satisfied by Carrollian MHV gl... | 9.580638 | 8.065254 | 9.908145 | 7.614059 | 8.278719 | 7.659368 | 7.381755 | 7.953249 | 7.393111 | 10.80855 | 8.742861 | 8.306577 | 9.002625 | 8.398468 | 7.972615 | 8.534959 | 8.18769 | 8.693153 | 8.512136 | 9.247749 | 8.363951 |
0901.1182 | Christoffer Petersson | Gabriele Ferretti, Christoffer Petersson | Non-Perturbative Effects on a Fractional D3-Brane | 18 pages, v3: refs added | null | 10.1088/1126-6708/2009/03/040 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we study the N=1 abelian gauge theory on the world volume of a
single fractional D3-brane. In the limit where gravitational interactions are
not completely decoupled we find that a superpotential and a fermionic bilinear
condensate are generated by a D-brane instanton effect. A related situation
arises f... | [
{
"created": "Fri, 9 Jan 2009 16:51:41 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jan 2009 16:22:08 GMT",
"version": "v2"
},
{
"created": "Mon, 2 Mar 2009 16:04:56 GMT",
"version": "v3"
}
] | 2009-11-13 | [
[
"Ferretti",
"Gabriele",
""
],
[
"Petersson",
"Christoffer",
""
]
] | In this note we study the N=1 abelian gauge theory on the world volume of a single fractional D3-brane. In the limit where gravitational interactions are not completely decoupled we find that a superpotential and a fermionic bilinear condensate are generated by a D-brane instanton effect. A related situation arises for... | 9.334411 | 8.501603 | 10.123169 | 9.221549 | 9.064076 | 8.696976 | 9.057142 | 8.545243 | 9.06602 | 11.157722 | 8.572665 | 8.825292 | 9.469781 | 8.748163 | 8.66232 | 9.05489 | 9.161313 | 8.88842 | 8.992978 | 9.381774 | 8.90827 |
1405.5215 | Christoph Adam | C. Adam, T. Romanczukiewicz, J. Sanchez-Guillen, A. Wereszczynski | Magnetothermodynamics of BPS baby skyrmions | Latex, 39 pages, 14 figures. v2: New results and references added,
physical interpretation partly changed | null | 10.1007/JHEP11(2014)095 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The magnetothermodynamics of skyrmion type matter described by the gauged BPS
baby Skyrme model at zero temperature is investigated. We prove that the BPS
property of the model is preserved also for boundary conditions corresponding
to an asymptotically constant magnetic field. The BPS bound and the
corresponding BPS... | [
{
"created": "Tue, 20 May 2014 20:00:07 GMT",
"version": "v1"
},
{
"created": "Sat, 7 Jun 2014 18:02:14 GMT",
"version": "v2"
}
] | 2015-06-19 | [
[
"Adam",
"C.",
""
],
[
"Romanczukiewicz",
"T.",
""
],
[
"Sanchez-Guillen",
"J.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | The magnetothermodynamics of skyrmion type matter described by the gauged BPS baby Skyrme model at zero temperature is investigated. We prove that the BPS property of the model is preserved also for boundary conditions corresponding to an asymptotically constant magnetic field. The BPS bound and the corresponding BPS e... | 8.596288 | 8.751224 | 8.785037 | 8.783587 | 8.594536 | 8.789781 | 8.404451 | 8.120044 | 7.74343 | 9.94535 | 8.308975 | 8.230743 | 8.75731 | 8.520883 | 8.46135 | 8.24142 | 8.172124 | 8.272642 | 8.36142 | 8.898162 | 8.382515 |
hep-th/9311021 | Henry Tye | S.-H.H. Tye | Status of Fractional Superstrings | 15 pages | null | null | null | hep-th | null | A brief review of the motivation and the present status of Fractional
Superstring is presented. Talk at ``Strings 93'', Berkeley, May 1993.
| [
{
"created": "Wed, 3 Nov 1993 16:01:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Tye",
"S. -H. H.",
""
]
] | A brief review of the motivation and the present status of Fractional Superstring is presented. Talk at ``Strings 93'', Berkeley, May 1993. | 21.845951 | 7.454038 | 14.038841 | 7.641068 | 8.276642 | 7.965851 | 7.177238 | 7.304807 | 7.456034 | 21.696585 | 7.688527 | 10.386481 | 13.785676 | 10.34409 | 10.713243 | 11.8511 | 10.338131 | 11.477501 | 10.305039 | 13.8499 | 11.653005 |
2010.06106 | Masashi Zenkai | Tadakatsu Sakai and Masashi Zenkai | Comments on contact terms and conformal manifolds in the AdS/CFT
correspondence | 16 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the contact terms that appear in the correlation functions of
exactly marginal operators using the AdS/CFT correspondence. It is known that
CFT with an exactly marginal deformation requires the existence of the contact
terms with their coefficients having a geometrical interpretation in the
context of confor... | [
{
"created": "Tue, 13 Oct 2020 01:22:45 GMT",
"version": "v1"
}
] | 2020-10-14 | [
[
"Sakai",
"Tadakatsu",
""
],
[
"Zenkai",
"Masashi",
""
]
] | We study the contact terms that appear in the correlation functions of exactly marginal operators using the AdS/CFT correspondence. It is known that CFT with an exactly marginal deformation requires the existence of the contact terms with their coefficients having a geometrical interpretation in the context of conforma... | 8.104222 | 8.277493 | 8.896893 | 7.817276 | 8.367168 | 8.200672 | 7.98447 | 8.072628 | 7.921417 | 9.590207 | 7.937049 | 7.846909 | 8.215414 | 7.927699 | 7.935655 | 7.983488 | 7.835497 | 7.945556 | 7.756664 | 8.209766 | 7.900826 |
1402.2557 | Fabio Riccioni | Eric A. Bergshoeff, Fabio Riccioni and Luca Romano | Towards a classification of branes in theories with eight supercharges | 47 pages, 8 figures | null | 10.1007/JHEP05(2014)070 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a classification of half-supersymmetric branes in quarter-maximal
supergravity theories with scalars parametrising coset manifolds. Guided by the
results previously obtained for the half-maximal theories, we are able to show
that half-supersymmetric branes correspond to the real longest weights of the
repr... | [
{
"created": "Tue, 11 Feb 2014 16:44:25 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Bergshoeff",
"Eric A.",
""
],
[
"Riccioni",
"Fabio",
""
],
[
"Romano",
"Luca",
""
]
] | We provide a classification of half-supersymmetric branes in quarter-maximal supergravity theories with scalars parametrising coset manifolds. Guided by the results previously obtained for the half-maximal theories, we are able to show that half-supersymmetric branes correspond to the real longest weights of the repres... | 8.737079 | 8.676257 | 10.504973 | 8.223023 | 9.195277 | 8.302135 | 9.050775 | 8.017919 | 8.68185 | 10.909216 | 8.317028 | 8.350257 | 9.105312 | 8.269795 | 8.266486 | 8.277321 | 8.250353 | 8.289026 | 8.241669 | 8.622161 | 8.07741 |
2201.08762 | Leonid Bork Dr | L.V. Bork, N.B. Muzhichkov, E.S. Sozinov | Infrared properties of five-point massive amplitudes in N=4 SYM on the
Coulomb branch | 29 pages, 7 figures v3: minor changes, typos corrected | null | 10.1007/JHEP08(2022)173 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the structure of the five-point W boson scattering amplitude
in N=4 SYM on the Coulomb branch in a small mass limit. We show that up to two
loops the IR divergences exponentiate and are controlled by the $\Gamma_{oct}$
anomalous dimension similar to the four-point amplitude case considered
recently in ... | [
{
"created": "Fri, 21 Jan 2022 16:21:22 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Jan 2022 19:42:12 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Apr 2022 15:33:33 GMT",
"version": "v3"
}
] | 2022-09-07 | [
[
"Bork",
"L. V.",
""
],
[
"Muzhichkov",
"N. B.",
""
],
[
"Sozinov",
"E. S.",
""
]
] | We investigate the structure of the five-point W boson scattering amplitude in N=4 SYM on the Coulomb branch in a small mass limit. We show that up to two loops the IR divergences exponentiate and are controlled by the $\Gamma_{oct}$ anomalous dimension similar to the four-point amplitude case considered recently in th... | 9.425331 | 6.580545 | 8.627872 | 7.69776 | 8.285517 | 7.36322 | 7.903652 | 7.113449 | 7.515713 | 8.894738 | 7.550636 | 7.900172 | 8.567583 | 8.087984 | 8.119488 | 8.256097 | 8.007801 | 7.999529 | 8.348998 | 8.25424 | 8.032071 |
0709.3069 | Srikumar Sen Gupta | Srikumar Sen Gupta | Brane Solutions in Time Dependent Backgrounds in D = 11 Supergravity and
in Type II String Theories | 20 pages | Int.J.Mod.Phys.A23:2525-2540,2008 | 10.1142/S0217751X08039797 | null | hep-th | null | We obtain explicit time dependent brane solutions in M-theory as well as in
string theory by solving the reduced equations of motion (which follow from
11-d supergravity) for a class of brane solutions in curved backgrounds. The
behaviour of our solutions in both asymptotic and near-horizon limits are
studied. It is ... | [
{
"created": "Wed, 19 Sep 2007 16:55:15 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gupta",
"Srikumar Sen",
""
]
] | We obtain explicit time dependent brane solutions in M-theory as well as in string theory by solving the reduced equations of motion (which follow from 11-d supergravity) for a class of brane solutions in curved backgrounds. The behaviour of our solutions in both asymptotic and near-horizon limits are studied. It is sh... | 13.894872 | 11.622445 | 13.92417 | 11.815738 | 11.287364 | 12.226788 | 11.617386 | 12.335746 | 11.649521 | 15.393934 | 11.798541 | 12.81569 | 13.583898 | 12.681005 | 12.509291 | 12.533478 | 12.626765 | 12.81118 | 12.792711 | 14.163891 | 12.859685 |
1004.0554 | Alejandra Castro | Alejandra Castro, Cynthia Keeler and Finn Larsen | Three Dimensional Origin of AdS_2 Quantum Gravity | 28 pages | JHEP 1007:033,2010 | 10.1007/JHEP07(2010)033 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study AdS_2 quantum gravity with emphasis on consistency with results from
AdS_3. We lift AdS_2 black holes to three dimensions and map fluctuations
around the solutions. Comparison with near extremal BTZ are discussed, with due
emphasis on global aspects. The results confirm that parameters like central
charges a... | [
{
"created": "Mon, 5 Apr 2010 02:16:33 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Castro",
"Alejandra",
""
],
[
"Keeler",
"Cynthia",
""
],
[
"Larsen",
"Finn",
""
]
] | We study AdS_2 quantum gravity with emphasis on consistency with results from AdS_3. We lift AdS_2 black holes to three dimensions and map fluctuations around the solutions. Comparison with near extremal BTZ are discussed, with due emphasis on global aspects. The results confirm that parameters like central charges and... | 12.272564 | 12.322863 | 13.552726 | 11.957433 | 13.726471 | 12.995794 | 12.644374 | 11.789065 | 12.319304 | 15.119168 | 10.907885 | 12.245818 | 12.028611 | 11.931933 | 12.129194 | 12.057174 | 12.640787 | 11.999844 | 11.877364 | 12.852962 | 11.612676 |
hep-th/9805148 | Mkrtchyan Ruben | R. Manvelyan, A. Melikyan and R. Mkrtchyan | Representations and BPS states of 10+2 superalgebra | Minor changes.Accepted for publication in Mod.Phys.Lett.A.Latex file | Mod.Phys.Lett. A13 (1998) 2147-2152 | 10.1142/S0217732398002278 | null | hep-th | null | The 12d supersymmetry algebra is considered, and classification of BPS states
for some canonical form of second-rank central charge is given. It is shown,
that possible fractions of survived supersymmetry can be 1/16, 1/8, 3/16, 1/4,
5/16 and 1/2, the values 3/8, 7/16 cannot be achieved in this way. The
consideration... | [
{
"created": "Fri, 22 May 1998 10:53:09 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Aug 1998 12:19:36 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Manvelyan",
"R.",
""
],
[
"Melikyan",
"A.",
""
],
[
"Mkrtchyan",
"R.",
""
]
] | The 12d supersymmetry algebra is considered, and classification of BPS states for some canonical form of second-rank central charge is given. It is shown, that possible fractions of survived supersymmetry can be 1/16, 1/8, 3/16, 1/4, 5/16 and 1/2, the values 3/8, 7/16 cannot be achieved in this way. The consideration o... | 10.165915 | 8.241722 | 10.088314 | 8.50938 | 9.526171 | 8.191887 | 8.646358 | 7.727538 | 8.771688 | 9.635923 | 8.464476 | 8.382685 | 9.225345 | 8.663543 | 8.589052 | 8.91556 | 8.404873 | 8.47651 | 8.292525 | 9.342838 | 8.550756 |
hep-th/9703093 | Homayoun Hamidian | H. Hamidian (Stockholm University) | Quantum Critical Behavior in Gauged Yukawa Matrix Field Theories with
Quenched Disorder | 8 pages, LaTeX, 1 eps figure | Phys.Lett. B403 (1997) 108-113 | 10.1016/S0370-2693(97)00469-3 | null | hep-th cond-mat | null | We use the Wilson-Fisher $\epsilon$ expansion to study quantum critical
behavior in gauged Yukawa matrix field theories with weak quenched disorder. We
find that the resulting quantum critical behavior is in the universality class
of the pure system. As in the pure system, the phase transition is typically
first orde... | [
{
"created": "Wed, 12 Mar 1997 13:30:33 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Hamidian",
"H.",
"",
"Stockholm University"
]
] | We use the Wilson-Fisher $\epsilon$ expansion to study quantum critical behavior in gauged Yukawa matrix field theories with weak quenched disorder. We find that the resulting quantum critical behavior is in the universality class of the pure system. As in the pure system, the phase transition is typically first order,... | 8.922622 | 8.864827 | 7.838889 | 8.340841 | 9.077589 | 9.605328 | 9.393398 | 9.089253 | 8.598865 | 9.751513 | 8.257473 | 8.698786 | 8.725575 | 8.400347 | 8.650261 | 8.82312 | 8.609251 | 8.602414 | 8.18983 | 8.501122 | 8.680079 |
hep-th/0401189 | Mauricio Cataldo MC | M. Cataldo, J. Crisostomo, S. del Campo and P. Salgado | On Magnetic solution to 2+1 Einstein--Maxwell gravity | 3 pages, accepted for publication | Phys. Lett. B 584 (2004) 123-126 | 10.1016/j.physletb.2004.01.062 | null | hep-th | null | The three--dimensional magnetic solution to the Einstein--Maxwell field
equations have been considered by some authors. Several interpretations have
been formulated for this magnetic spacetime. Up to now this solution has been
considered as a two--parameter self--consistent field. We point out that the
parameter rela... | [
{
"created": "Sun, 25 Jan 2004 15:33:07 GMT",
"version": "v1"
}
] | 2014-10-15 | [
[
"Cataldo",
"M.",
""
],
[
"Crisostomo",
"J.",
""
],
[
"del Campo",
"S.",
""
],
[
"Salgado",
"P.",
""
]
] | The three--dimensional magnetic solution to the Einstein--Maxwell field equations have been considered by some authors. Several interpretations have been formulated for this magnetic spacetime. Up to now this solution has been considered as a two--parameter self--consistent field. We point out that the parameter relate... | 14.071842 | 14.465273 | 12.702003 | 12.660686 | 14.069389 | 13.751762 | 13.788075 | 12.542249 | 12.845868 | 12.392766 | 14.406538 | 13.198389 | 12.704636 | 12.31345 | 12.425255 | 12.970291 | 13.107205 | 12.926885 | 13.1237 | 13.211197 | 13.040774 |
1905.01444 | Gregory Korchemsky | G. P. Korchemsky | Energy correlations in the end-point region | 31 pages, 1 figure | null | 10.1007/JHEP01(2020)008 | IPhT-T19/041 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The energy-energy correlation (EEC) measures the angular distribution of the
energy that flows through two calorimeters separated by some relative angle in
the final state created by a source. We study this observable in the limit of
small and large angles when it describes the correlation between particles
belonging... | [
{
"created": "Sat, 4 May 2019 06:49:00 GMT",
"version": "v1"
}
] | 2020-01-29 | [
[
"Korchemsky",
"G. P.",
""
]
] | The energy-energy correlation (EEC) measures the angular distribution of the energy that flows through two calorimeters separated by some relative angle in the final state created by a source. We study this observable in the limit of small and large angles when it describes the correlation between particles belonging, ... | 8.574423 | 9.329245 | 9.095033 | 8.065044 | 8.518946 | 8.805713 | 8.505959 | 8.030683 | 8.403608 | 9.595661 | 8.180885 | 7.978111 | 8.255919 | 8.264052 | 8.030028 | 8.16804 | 8.657615 | 8.216448 | 8.225094 | 8.613935 | 8.160926 |
0812.2992 | Lorenz von Smekal | Lorenz von Smekal, Alexander Jorkowski, Dhagash Mehta and Andre
Sternbeck | Lattice Landau gauge via Stereographic Projection | 5 pages, talk presented at the 8th Conference Quark Confinement and
the Hadron Spectrum, September 1-6, 2008, Mainz, Germany | PoS Confinement8:048,2008 | null | ADP-08-15/T675 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complete cancellation of Gribov copies and the Neuberger 0/0 problem of
lattice BRST can be avoided in modified lattice Landau gauge. In compact U(1),
where the problem is a lattice artifact, there remain to be Gribov copies but
their number is exponentially reduced. Moreover, there is no cancellation of
copies t... | [
{
"created": "Tue, 16 Dec 2008 07:52:28 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"von Smekal",
"Lorenz",
""
],
[
"Jorkowski",
"Alexander",
""
],
[
"Mehta",
"Dhagash",
""
],
[
"Sternbeck",
"Andre",
""
]
] | The complete cancellation of Gribov copies and the Neuberger 0/0 problem of lattice BRST can be avoided in modified lattice Landau gauge. In compact U(1), where the problem is a lattice artifact, there remain to be Gribov copies but their number is exponentially reduced. Moreover, there is no cancellation of copies the... | 15.952859 | 19.012678 | 16.586035 | 16.430075 | 16.374756 | 18.563498 | 18.387274 | 15.874163 | 15.937675 | 18.74612 | 16.926603 | 15.740271 | 15.351434 | 15.199224 | 15.393464 | 16.115883 | 15.667266 | 15.144028 | 14.96025 | 15.472964 | 15.277932 |
hep-th/9110025 | Nigel J. Burroughs | Nigel J. Burroughs | Coadjoint Orbits of the Generalised Sl(2) Sl(3) Kdv Hierarchies | 37 pages | Nucl.Phys. B379 (1992) 340-376 | 10.1016/0550-3213(92)90600-G | null | hep-th math.QA | null | In this paper we develop two coadjoint orbit constructions for the phase
spaces of the generalised $Sl(2)$ and $Sl(3)$ KdV hierachies. This involves the
construction of two group actions in terms of Yang Baxter operators, and an
Hamiltonian reduction of the coadjoint orbits. The Poisson brackets are
reproduced by the... | [
{
"created": "Wed, 9 Oct 1991 22:27:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Burroughs",
"Nigel J.",
""
]
] | In this paper we develop two coadjoint orbit constructions for the phase spaces of the generalised $Sl(2)$ and $Sl(3)$ KdV hierachies. This involves the construction of two group actions in terms of Yang Baxter operators, and an Hamiltonian reduction of the coadjoint orbits. The Poisson brackets are reproduced by the K... | 11.533015 | 10.392093 | 11.625643 | 10.431586 | 11.221961 | 10.860575 | 10.696904 | 10.894262 | 10.116206 | 14.112328 | 10.667633 | 10.027626 | 11.308814 | 9.871564 | 10.260066 | 10.392989 | 10.52071 | 10.271485 | 10.109409 | 10.997295 | 10.22877 |
hep-th/0108169 | Alexander Sevrin | Paul Koerber and Alexander Sevrin | The non-abelian open superstring effective action through order
$\alpha'{}^3$ | LaTeX, 29 pages; references added, typos corrected, following
suggestions of referee: title, introduction and conclusions altered | JHEP 0110:003,2001 | 10.1088/1126-6708/2001/10/003 | null | hep-th | null | Using the method developed in {\tt hep-th/0103015}, we determine the
non-abelian Born-Infeld action through ${\cal O}(\alpha'{}^3)$. We start from
solutions to a Yang-Mills theory which define a stable holomorphic vector
bundle. Subsequently we investigate its deformation away from this limit.
Through $ {\cal O}(\alp... | [
{
"created": "Wed, 22 Aug 2001 19:09:12 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Sep 2001 16:24:19 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Koerber",
"Paul",
""
],
[
"Sevrin",
"Alexander",
""
]
] | Using the method developed in {\tt hep-th/0103015}, we determine the non-abelian Born-Infeld action through ${\cal O}(\alpha'{}^3)$. We start from solutions to a Yang-Mills theory which define a stable holomorphic vector bundle. Subsequently we investigate its deformation away from this limit. Through $ {\cal O}(\alpha... | 9.14763 | 7.946265 | 9.296752 | 7.931669 | 8.149384 | 7.8365 | 8.150997 | 7.693176 | 7.969196 | 8.690368 | 8.028139 | 8.573963 | 8.709858 | 8.367715 | 8.441797 | 8.409956 | 8.364861 | 8.638602 | 8.288978 | 8.697142 | 8.514927 |
hep-th/0603104 | Daniel Robbins | Emil J. Martinec, Daniel Robbins and Savdeep Sethi | Toward the End of Time | 31 pages, reference added | JHEP0608:025,2006 | 10.1088/1126-6708/2006/08/025 | EFI-06-03 | hep-th | null | The null-brane space-time provides a simple model of a big crunch/big bang
singularity. A non-perturbative definition of M-theory on this space-time was
recently provided using matrix theory. We derive the fermion couplings for this
matrix model and study the leading quantum effects. These effects include
particle pr... | [
{
"created": "Tue, 14 Mar 2006 00:54:59 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Apr 2006 20:42:14 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Martinec",
"Emil J.",
""
],
[
"Robbins",
"Daniel",
""
],
[
"Sethi",
"Savdeep",
""
]
] | The null-brane space-time provides a simple model of a big crunch/big bang singularity. A non-perturbative definition of M-theory on this space-time was recently provided using matrix theory. We derive the fermion couplings for this matrix model and study the leading quantum effects. These effects include particle prod... | 10.75372 | 9.983524 | 12.873971 | 9.92964 | 10.031775 | 10.10273 | 10.691417 | 10.121646 | 10.052609 | 11.962111 | 9.500783 | 9.924461 | 10.885845 | 10.187751 | 9.823648 | 10.143153 | 9.859401 | 10.228305 | 9.824258 | 10.89838 | 9.977034 |
1612.01692 | Emanuel Malek | Emanuel Malek | 7-dimensional ${\cal N}=2$ Consistent Truncations using $\mathrm{SL}(5)$
Exceptional Field Theory | 46 pages; v2: minor changes, published version | JHEP 1706 (2017) 026 | 10.1007/JHEP06(2017)026 | LMU-ASC 61/16 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how to construct seven-dimensional half-maximally supersymmetric
consistent truncations of 11-/10-dimensional SUGRA using $\mathrm{SL}(5)$
exceptional field theory. Such truncations are defined on generalised
$\mathrm{SU}(2)$-structure manifolds and give rise to seven-dimensional
half-maximal gauged supergrav... | [
{
"created": "Tue, 6 Dec 2016 07:58:34 GMT",
"version": "v1"
},
{
"created": "Mon, 19 Jun 2017 12:50:08 GMT",
"version": "v2"
}
] | 2017-06-28 | [
[
"Malek",
"Emanuel",
""
]
] | We show how to construct seven-dimensional half-maximally supersymmetric consistent truncations of 11-/10-dimensional SUGRA using $\mathrm{SL}(5)$ exceptional field theory. Such truncations are defined on generalised $\mathrm{SU}(2)$-structure manifolds and give rise to seven-dimensional half-maximal gauged supergravit... | 5.019981 | 5.38874 | 5.611897 | 4.81941 | 5.220619 | 5.502918 | 5.106941 | 5.347785 | 5.234342 | 6.660593 | 4.941504 | 4.847861 | 5.056959 | 4.650127 | 4.778759 | 4.795146 | 4.758674 | 4.652094 | 4.751062 | 5.039248 | 4.758703 |
0901.2641 | Francisco Diego Mazzitelli | Ezequiel Alvarez and Francisco D. Mazzitelli | Long range Casimir force induced by transverse electromagnetic modes | 9 pages, 5 figures. A statement about the boundary conditions for the
Hertz potentials has been corrected. Some typos have been fixed. Results
remain unchanged | Phys.Rev.D79:045019,2009 | 10.1103/PhysRevD.79.045019 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the interaction of two perfectly conducting plates of arbitrary
shape that are inside a non-simply connected cylinder with transverse section
of the same shape. We show that the existence of transverse electromagnetic
(TEM) modes produces a Casimir force that decays only as $1/a^2$, where $a$ is
the dista... | [
{
"created": "Sat, 17 Jan 2009 14:48:50 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Mar 2009 13:35:08 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Apr 2009 19:01:13 GMT",
"version": "v3"
}
] | 2010-04-21 | [
[
"Alvarez",
"Ezequiel",
""
],
[
"Mazzitelli",
"Francisco D.",
""
]
] | We consider the interaction of two perfectly conducting plates of arbitrary shape that are inside a non-simply connected cylinder with transverse section of the same shape. We show that the existence of transverse electromagnetic (TEM) modes produces a Casimir force that decays only as $1/a^2$, where $a$ is the distanc... | 6.480449 | 7.594652 | 6.966334 | 6.518548 | 6.737009 | 7.114267 | 6.628634 | 6.884037 | 6.8839 | 8.388409 | 6.499249 | 6.741644 | 6.700385 | 6.603587 | 6.674796 | 6.599397 | 6.522467 | 6.508935 | 6.621438 | 6.943963 | 6.479089 |
2312.07452 | Carlo Heissenberg | Alessandro Georgoudis, Carlo Heissenberg, Rodolfo Russo | An eikonal-inspired approach to the gravitational scattering waveform | 40 pages, v2: presentation improved | null | null | QMUL-PH-23-34 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the amplitude-based derivation of gravitational waveform for the
scattering of two scalar black holes at subleading post-Minkowskian (PM) order.
We take an eikonal-inspired approach to the two-massive-particle cut needed in
the KMOC framework, as highlighted in arXiv:2308.02125, and show that its
effect is... | [
{
"created": "Tue, 12 Dec 2023 17:25:10 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Jan 2024 14:45:42 GMT",
"version": "v2"
}
] | 2024-01-22 | [
[
"Georgoudis",
"Alessandro",
""
],
[
"Heissenberg",
"Carlo",
""
],
[
"Russo",
"Rodolfo",
""
]
] | We revisit the amplitude-based derivation of gravitational waveform for the scattering of two scalar black holes at subleading post-Minkowskian (PM) order. We take an eikonal-inspired approach to the two-massive-particle cut needed in the KMOC framework, as highlighted in arXiv:2308.02125, and show that its effect is t... | 9.776922 | 8.938736 | 9.627383 | 8.522023 | 8.965122 | 9.53191 | 9.263864 | 8.377338 | 9.433426 | 9.856242 | 8.915011 | 8.943568 | 9.132926 | 8.868648 | 8.8005 | 9.021972 | 8.792593 | 8.740378 | 8.91763 | 9.53004 | 8.988943 |
hep-th/0609079 | Spyros Avramis | Spyros D. Avramis, Konstadinos Sfetsos and Dimitrios Zoakos | On the velocity and chemical-potential dependence of the heavy-quark
interaction in N=4 SYM plasmas | 24 pages, 10 figures; v2: energy regularization discussed in detail,
references added, version to appear in Phys. Rev. D | Phys.Rev.D75:025009,2007 | 10.1103/PhysRevD.75.025009 | null | hep-th | null | We consider the interaction of a heavy quark-antiquark pair moving in N=4 SYM
plasma in the presence of non-vanishing chemical potentials. Of particular
importance is the maximal length beyond which the interaction is practically
turned off. We propose a simple phenomenological law that takes into account
the velocit... | [
{
"created": "Tue, 12 Sep 2006 14:46:22 GMT",
"version": "v1"
},
{
"created": "Sun, 10 Dec 2006 21:14:17 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Avramis",
"Spyros D.",
""
],
[
"Sfetsos",
"Konstadinos",
""
],
[
"Zoakos",
"Dimitrios",
""
]
] | We consider the interaction of a heavy quark-antiquark pair moving in N=4 SYM plasma in the presence of non-vanishing chemical potentials. Of particular importance is the maximal length beyond which the interaction is practically turned off. We propose a simple phenomenological law that takes into account the velocity ... | 13.086783 | 10.805327 | 12.065107 | 10.011959 | 11.18227 | 11.996439 | 11.785142 | 9.509885 | 10.487466 | 12.54168 | 10.719099 | 10.952106 | 12.799677 | 11.42412 | 11.47325 | 11.446122 | 11.174861 | 11.526438 | 11.285479 | 12.75294 | 10.779997 |
1309.2281 | Jean-Luc Lehners | Lorenzo Battarra and Jean-Luc Lehners | On the Quantum-To-Classical Transition for Ekpyrotic Perturbations | 32 pages, 4 figures | Phys. Rev. D 89, 063516 (2014) | 10.1103/PhysRevD.89.063516 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the processes of quantum squeezing and decoherence of density
perturbations produced during a slowly contracting ekpyrotic phase in which
entropic perturbations are converted to curvature perturbations before the
bounce to an expanding phase. During the generation phase, the entropic
fluctuations evolve in... | [
{
"created": "Mon, 9 Sep 2013 20:00:00 GMT",
"version": "v1"
}
] | 2014-03-26 | [
[
"Battarra",
"Lorenzo",
""
],
[
"Lehners",
"Jean-Luc",
""
]
] | We examine the processes of quantum squeezing and decoherence of density perturbations produced during a slowly contracting ekpyrotic phase in which entropic perturbations are converted to curvature perturbations before the bounce to an expanding phase. During the generation phase, the entropic fluctuations evolve into... | 7.683975 | 7.499196 | 7.164948 | 6.685367 | 7.339425 | 7.651908 | 7.533177 | 6.836201 | 7.109688 | 7.297273 | 7.110901 | 7.38151 | 7.569155 | 7.381626 | 7.218414 | 7.129208 | 7.146707 | 7.34542 | 7.26369 | 7.618944 | 6.867982 |
1306.6730 | Balachandran Sathiapalan | B. Sathiapalan | Loop Variables and Gauge Invariant Exact Renormalization Group Equations
for Closed String Theory | 44 pages Latex. Some minor modifications | null | 10.1142/S0217751X13501169 | IMSC/2013/05/04 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formulate the Exact Renormalization Group on the string world sheet for
closed string backgrounds. The same techniques that were used for open strings
is used here. There are some subtleties. One is that holomorphic factorization
of the closed string vertex operators does not hold in the presence of a cutoff
on th... | [
{
"created": "Fri, 28 Jun 2013 06:50:08 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Aug 2013 04:35:15 GMT",
"version": "v2"
}
] | 2015-06-16 | [
[
"Sathiapalan",
"B.",
""
]
] | We formulate the Exact Renormalization Group on the string world sheet for closed string backgrounds. The same techniques that were used for open strings is used here. There are some subtleties. One is that holomorphic factorization of the closed string vertex operators does not hold in the presence of a cutoff on the ... | 13.268151 | 13.804284 | 14.307778 | 12.520306 | 13.338526 | 14.060909 | 13.529613 | 13.904045 | 13.772853 | 15.029537 | 13.077545 | 12.530238 | 12.622609 | 12.411851 | 12.799142 | 13.130585 | 12.658249 | 12.654912 | 12.79531 | 13.261248 | 12.605188 |
hep-th/0605286 | Daniel Are\'an | Daniel Arean | Killing spinors of some supergravity solutions | M.Sc. Thesis, 72 pages, LaTeX | null | null | null | hep-th | null | We compute explicitly the Killing spinors of some ten dimensional
supergravity solutions. We begin with a 10d metric of the form
$\RR^{1,3}\times{\cal Y}_6$, where ${\cal Y}_6$ is either the singular conifold
or any of its resolutions. Then, we move on to the Klebanov-Witten and
Klebanov-Tseytlin backgrounds, both co... | [
{
"created": "Tue, 30 May 2006 10:32:26 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Arean",
"Daniel",
""
]
] | We compute explicitly the Killing spinors of some ten dimensional supergravity solutions. We begin with a 10d metric of the form $\RR^{1,3}\times{\cal Y}_6$, where ${\cal Y}_6$ is either the singular conifold or any of its resolutions. Then, we move on to the Klebanov-Witten and Klebanov-Tseytlin backgrounds, both cons... | 5.251246 | 5.352191 | 5.824589 | 5.132091 | 5.205334 | 5.196244 | 5.237424 | 5.163778 | 5.226339 | 6.412531 | 5.23594 | 5.16868 | 5.319646 | 5.193935 | 5.06512 | 5.166829 | 5.235218 | 4.995344 | 5.1537 | 5.311451 | 5.095875 |
hep-th/0403036 | Jerzy Szwed | Jerzy Szwed | The "square root" of the Dirac equation and solutions on superspace | 9 pages | Acta Phys.Polon. B37 (2006) 455-462 | null | CPT-2004/P.008 | hep-th hep-ph | null | The "square root" of the Dirac operator derived on the superspace is used to
construct supersymmetric field equations. In addition to the recently found
solution - a vector supermultiplet I demonstrate how a chiral supermultiplet
follows as the solution. Both vector and chiral supermultiplets are shown to
obey approp... | [
{
"created": "Tue, 2 Mar 2004 13:55:48 GMT",
"version": "v1"
},
{
"created": "Wed, 26 May 2004 14:14:20 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Jun 2004 10:50:01 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Szwed",
"Jerzy",
""
]
] | The "square root" of the Dirac operator derived on the superspace is used to construct supersymmetric field equations. In addition to the recently found solution - a vector supermultiplet I demonstrate how a chiral supermultiplet follows as the solution. Both vector and chiral supermultiplets are shown to obey appropri... | 13.963077 | 12.136601 | 12.946437 | 11.78154 | 13.229911 | 13.124688 | 11.990088 | 11.310974 | 12.221273 | 13.421361 | 11.72847 | 12.662653 | 12.714113 | 11.85773 | 11.968976 | 12.328828 | 12.449808 | 13.314109 | 12.468257 | 13.469802 | 12.808954 |
hep-th/9302076 | Shahn Majid | Shahn Majid | Free Braided Differential Calculus, Braided Binomial Theorem and the
Braided Exponential Map | 19 pages | J.Math.Phys. 34 (1993) 4843-4856 | 10.1063/1.530326 | DAMTP/93-3 | hep-th math.QA | null | Braided differential operators $\del^i$ are obtained by differentiating the
addition law on the braided covector spaces introduced previously (such as the
braided addition law on the quantum plane). These are affiliated to a
Yang-Baxter matrix $R$. The quantum eigenfunctions $\exp_R(\vecx|\vecv)$ of the
$\del^i$ (bra... | [
{
"created": "Wed, 17 Feb 1993 11:52:34 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Majid",
"Shahn",
""
]
] | Braided differential operators $\del^i$ are obtained by differentiating the addition law on the braided covector spaces introduced previously (such as the braided addition law on the quantum plane). These are affiliated to a Yang-Baxter matrix $R$. The quantum eigenfunctions $\exp_R(\vecx|\vecv)$ of the $\del^i$ (braid... | 11.684279 | 13.159955 | 14.100106 | 11.951066 | 12.767245 | 13.773845 | 12.719123 | 12.548961 | 11.622846 | 14.506029 | 12.006845 | 11.291956 | 11.080282 | 11.241317 | 11.143094 | 11.389899 | 11.397143 | 11.081515 | 11.378793 | 11.274836 | 10.963515 |
1410.4669 | Dimitrios Tsimpis | Jean-Marc Richard, Robin Terrisse and Dimitrios Tsimpis | On the spin-2 Kaluza-Klein spectrum of AdS4 x S2(B4) | 13 pages, 9 figures | null | 10.1007/JHEP12(2014)144 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We perform a numerical study of the four-dimensional spin-2 Kaluza-Klein
spectrum of supersymmetric AdS$_4\times S^2(\mathcal{B}_4)$ vacua and show that
they do not exhibit scale separation. Our methods are generally applicable to
similar problems where the compactification geometry is not known analytically,
hence a... | [
{
"created": "Fri, 17 Oct 2014 09:11:21 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Richard",
"Jean-Marc",
""
],
[
"Terrisse",
"Robin",
""
],
[
"Tsimpis",
"Dimitrios",
""
]
] | We perform a numerical study of the four-dimensional spin-2 Kaluza-Klein spectrum of supersymmetric AdS$_4\times S^2(\mathcal{B}_4)$ vacua and show that they do not exhibit scale separation. Our methods are generally applicable to similar problems where the compactification geometry is not known analytically, hence an ... | 10.175761 | 9.529136 | 10.381356 | 9.060402 | 9.346318 | 9.902148 | 9.213862 | 8.765888 | 9.31983 | 11.810639 | 8.738345 | 8.756845 | 10.431407 | 9.017564 | 9.298421 | 9.17271 | 9.273366 | 8.971864 | 9.500326 | 9.922845 | 8.840966 |
1410.3288 | James Edwards Mr | James P. Edwards and Paul Mansfield | Delta-function Interactions for the Bosonic and Spinning Strings and the
Generation of Abelian Gauge Theory | 68 pages, 9 figures Minor corrections to Appendix C | null | 10.1007/JHEP01(2015)127 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct contact interactions for bosonic and spinning strings. In the
tensionless limit of the spinning string this reproduces the super-Wilson loop
that couples spinor matter to Abelian gauge theory. Adding boundary terms that
quantise the motion of charges results in a string model equivalent to spinor
QED. Th... | [
{
"created": "Mon, 13 Oct 2014 12:55:06 GMT",
"version": "v1"
},
{
"created": "Fri, 17 Oct 2014 15:46:48 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Nov 2014 10:09:26 GMT",
"version": "v3"
}
] | 2015-06-23 | [
[
"Edwards",
"James P.",
""
],
[
"Mansfield",
"Paul",
""
]
] | We construct contact interactions for bosonic and spinning strings. In the tensionless limit of the spinning string this reproduces the super-Wilson loop that couples spinor matter to Abelian gauge theory. Adding boundary terms that quantise the motion of charges results in a string model equivalent to spinor QED. The ... | 19.146727 | 18.954226 | 20.455893 | 17.821518 | 18.080465 | 18.012314 | 17.942543 | 16.833845 | 18.452133 | 20.192904 | 17.321253 | 18.541798 | 19.180578 | 18.150396 | 18.958466 | 18.06361 | 18.133678 | 18.649199 | 18.295469 | 19.406168 | 17.644796 |
1802.06720 | Oleg Novikov | Alexander A. Andrianov, Chen Lan, Oleg O. Novikov, Yi-Fan Wang | Integrable Minisuperspace Models with Liouville Field: Energy Density
Self-Adjointness and Semiclassical Wave Packets | Main points emphasized, less important material shortened; 24 pages,
13 figures | Eur. Phys. J. C (2018) 78: 786 | 10.1140/epjc/s10052-018-6255-5 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The homogeneous cosmological models with a Liouville scalar field are
investigated in classical and quantum context of Wheeler-DeWitt
geometrodynamics. In the quantum case of quintessence field with potential
unbounded from below and phantom field, the energy density operators are not
essentially self-adjoint and sel... | [
{
"created": "Mon, 19 Feb 2018 17:32:28 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Mar 2018 12:45:11 GMT",
"version": "v2"
},
{
"created": "Fri, 25 May 2018 07:36:56 GMT",
"version": "v3"
}
] | 2018-10-16 | [
[
"Andrianov",
"Alexander A.",
""
],
[
"Lan",
"Chen",
""
],
[
"Novikov",
"Oleg O.",
""
],
[
"Wang",
"Yi-Fan",
""
]
] | The homogeneous cosmological models with a Liouville scalar field are investigated in classical and quantum context of Wheeler-DeWitt geometrodynamics. In the quantum case of quintessence field with potential unbounded from below and phantom field, the energy density operators are not essentially self-adjoint and self-... | 18.592028 | 22.252829 | 17.878069 | 17.316149 | 19.521254 | 17.010952 | 20.32588 | 17.896482 | 18.753229 | 19.837723 | 19.576567 | 18.818235 | 18.026148 | 17.953417 | 17.6798 | 17.62628 | 18.570206 | 17.34844 | 19.219547 | 17.969313 | 18.299482 |
2406.07334 | Akash Jain | Akash Jain | Fractonic solids | 5 pages + bibliography and supplementary material; a supplementary
mathematica notebook is included containing the details of dispersion
relations | null | null | null | hep-th cond-mat.stat-mech cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Fractons are exotic quasiparticles whose mobility in space is restricted by
symmetries. In potential real-world realisations, fractons are likely lodged to
a physical material rather than absolute space. Motivated by this, we propose
and explore a new symmetry principle that restricts the motion of fractons
relative ... | [
{
"created": "Tue, 11 Jun 2024 15:02:51 GMT",
"version": "v1"
}
] | 2024-06-12 | [
[
"Jain",
"Akash",
""
]
] | Fractons are exotic quasiparticles whose mobility in space is restricted by symmetries. In potential real-world realisations, fractons are likely lodged to a physical material rather than absolute space. Motivated by this, we propose and explore a new symmetry principle that restricts the motion of fractons relative to... | 11.917681 | 12.981246 | 13.499193 | 11.68791 | 13.126328 | 12.732318 | 13.318143 | 11.227859 | 11.994778 | 14.0057 | 11.900205 | 11.196381 | 11.185088 | 10.828886 | 11.105719 | 11.483232 | 11.332287 | 11.253424 | 11.285554 | 11.560437 | 11.022644 |
0906.4160 | Gyula Fodor | Gyula Fodor, P\'eter Forg\'acs, Zal\'an Horv\'ath, M\'ark Mezei | Oscillons in dilaton-scalar theories | extended discussion on stability, to appear in JHEP, 29 pages, 7
figures | JHEP 0908:106,2009 | 10.1088/1126-6708/2009/08/106 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown by both analytical methods and numerical simulations that
extremely long living spherically symmetric oscillons appear in virtually any
real scalar field theory coupled to a massless dilaton (DS theories). In fact
such "dilatonic" oscillons are already present in the simplest non-trivial DS
theory -- a fr... | [
{
"created": "Tue, 23 Jun 2009 12:57:30 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Aug 2009 13:53:56 GMT",
"version": "v2"
}
] | 2009-09-28 | [
[
"Fodor",
"Gyula",
""
],
[
"Forgács",
"Péter",
""
],
[
"Horváth",
"Zalán",
""
],
[
"Mezei",
"Márk",
""
]
] | It is shown by both analytical methods and numerical simulations that extremely long living spherically symmetric oscillons appear in virtually any real scalar field theory coupled to a massless dilaton (DS theories). In fact such "dilatonic" oscillons are already present in the simplest non-trivial DS theory -- a free... | 12.676276 | 11.698189 | 11.28168 | 10.52091 | 11.206087 | 10.797093 | 11.404837 | 11.254725 | 11.085565 | 13.645288 | 11.260171 | 11.376945 | 11.97208 | 11.609276 | 11.244469 | 11.604813 | 10.938151 | 11.381965 | 11.390624 | 11.842795 | 11.450268 |
hep-th/9703009 | Jnanadeva Maharana | Jnanadeva Maharana | S-duality and Compactification of type IIB Superstring Action | 14 pages, latex, no figures, references added, typos corrected and
two equations added | Phys.Lett. B402 (1997) 64-70 | 10.1016/S0370-2693(97)00444-9 | FERMILAB-PUB-97/046-T | hep-th | null | The SL(2,R) invaraint ten dimensional type IIB superstring effective action
is compactified on a torus to D spacetime dimensions. The transformation
properties of scalar, vector and tensor fields, appearing after the dimensional
reduction, are obtained in order to maintain the SL(2,R)} invariance of the
reduced effec... | [
{
"created": "Fri, 28 Feb 1997 20:09:54 GMT",
"version": "v1"
},
{
"created": "Wed, 19 Mar 1997 17:24:48 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Maharana",
"Jnanadeva",
""
]
] | The SL(2,R) invaraint ten dimensional type IIB superstring effective action is compactified on a torus to D spacetime dimensions. The transformation properties of scalar, vector and tensor fields, appearing after the dimensional reduction, are obtained in order to maintain the SL(2,R)} invariance of the reduced effecti... | 9.981968 | 7.751431 | 9.93799 | 7.700001 | 8.424604 | 7.846151 | 8.240001 | 8.03479 | 7.875485 | 11.008252 | 8.222307 | 8.648844 | 9.192977 | 8.52407 | 8.647387 | 8.692604 | 8.380884 | 8.818559 | 8.834687 | 9.512278 | 8.826509 |
1012.2883 | P.A.G. Pisani | S.A. Franchino Vi\~nas and P.A.G. Pisani | Semi-transparent Boundary Conditions in the Worldline Formalism | 12 pages | J.Phys.A44:295401,2011 | 10.1088/1751-8113/44/29/295401 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The interaction of a quantum field with a background containing a Dirac delta
function with support on a surface of codimension 1 represents a particular
kind of matching conditions on that surface for the field. In this article we
show that the worldline formalism can be applied to this model. We obtain the
asymptot... | [
{
"created": "Mon, 13 Dec 2010 21:20:52 GMT",
"version": "v1"
}
] | 2011-06-21 | [
[
"Viñas",
"S. A. Franchino",
""
],
[
"Pisani",
"P. A. G.",
""
]
] | The interaction of a quantum field with a background containing a Dirac delta function with support on a surface of codimension 1 represents a particular kind of matching conditions on that surface for the field. In this article we show that the worldline formalism can be applied to this model. We obtain the asymptotic... | 8.307708 | 8.019056 | 9.522445 | 7.416693 | 7.860433 | 7.670249 | 7.694218 | 7.309806 | 7.696189 | 9.184401 | 7.12534 | 7.375308 | 7.992483 | 7.905214 | 7.86201 | 7.89327 | 7.375138 | 7.741971 | 7.80211 | 8.027161 | 7.732433 |
hep-th/0408005 | Giovanni Arcioni | Giovanni Arcioni | On 't Hooft's S-matrix Ansatz for quantum black holes | 22 Pages. Latex File | JHEP0410:032,2004 | 10.1088/1126-6708/2004/10/032 | null | hep-th | null | The S-matrix Ansatz has been proposed by 't Hooft to overcome difficulties
and apparent contradictions of standard quantum field theory close to the black
hole horizon. In this paper we revisit and explore some of its aspects. We
start by computing gravitational backreaction effects on the properties of the
Hawking r... | [
{
"created": "Sun, 1 Aug 2004 08:08:28 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Arcioni",
"Giovanni",
""
]
] | The S-matrix Ansatz has been proposed by 't Hooft to overcome difficulties and apparent contradictions of standard quantum field theory close to the black hole horizon. In this paper we revisit and explore some of its aspects. We start by computing gravitational backreaction effects on the properties of the Hawking rad... | 15.100677 | 15.348447 | 16.059881 | 14.777486 | 16.028067 | 15.751867 | 15.250059 | 15.748418 | 13.954623 | 15.821679 | 15.007495 | 14.640601 | 15.022945 | 14.604852 | 15.06553 | 14.654559 | 14.722278 | 14.622329 | 14.415497 | 14.482471 | 14.651458 |
1403.7185 | Martin Wolf | Branislav Jurco, Christian Saemann and Martin Wolf | Semistrict Higher Gauge Theory | v4: 76 pages, minor errors fixed, published version | JHEP 04 (2015) 087 | 10.1007/JHEP04(2015)087 | EMPG-14-06, DMUS-MP-14/02 | hep-th math-ph math.CT math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop semistrict higher gauge theory from first principles. In
particular, we describe the differential Deligne cohomology underlying
semistrict principal 2-bundles with connective structures. Principal 2-bundles
are obtained in terms of weak 2-functors from the Cech groupoid to weak Lie
2-groups. As is demonstr... | [
{
"created": "Thu, 27 Mar 2014 19:40:05 GMT",
"version": "v1"
},
{
"created": "Tue, 6 May 2014 08:20:24 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Jan 2015 13:00:09 GMT",
"version": "v3"
},
{
"created": "Wed, 29 Apr 2015 14:04:13 GMT",
"version": "v4"
}
] | 2015-04-30 | [
[
"Jurco",
"Branislav",
""
],
[
"Saemann",
"Christian",
""
],
[
"Wolf",
"Martin",
""
]
] | We develop semistrict higher gauge theory from first principles. In particular, we describe the differential Deligne cohomology underlying semistrict principal 2-bundles with connective structures. Principal 2-bundles are obtained in terms of weak 2-functors from the Cech groupoid to weak Lie 2-groups. As is demonstrat... | 7.115135 | 8.364424 | 8.943178 | 6.912644 | 8.162428 | 8.056684 | 7.778143 | 7.460532 | 7.719429 | 8.975138 | 7.453946 | 7.388659 | 7.243207 | 6.844737 | 7.163913 | 6.987953 | 7.124689 | 6.903973 | 6.998137 | 7.643448 | 6.940315 |
2012.15521 | Arsenii Pikalov | A. Pikalov | Holographic model of exciton condensation in double monolayer Dirac
semimetal | 1 figure | null | 10.1134/S0021364021040020 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | In this paper we consider holographic model of exciton condensation in double
monolayer Dirac semimetal. Excitons is a bound states of an electron and a
hole. Being Bose particles, excitons can form a Bose-Einstein condensate. We
study formation of two types of condensates. In first case both the electron
and the hol... | [
{
"created": "Thu, 31 Dec 2020 09:50:02 GMT",
"version": "v1"
}
] | 2021-03-17 | [
[
"Pikalov",
"A.",
""
]
] | In this paper we consider holographic model of exciton condensation in double monolayer Dirac semimetal. Excitons is a bound states of an electron and a hole. Being Bose particles, excitons can form a Bose-Einstein condensate. We study formation of two types of condensates. In first case both the electron and the hole ... | 4.875558 | 4.687789 | 5.100819 | 4.598556 | 4.941178 | 4.820607 | 4.889534 | 4.366388 | 4.511823 | 5.190413 | 4.583892 | 4.518335 | 4.66381 | 4.615635 | 4.660624 | 4.728882 | 4.684775 | 4.601823 | 4.555631 | 4.641055 | 4.480818 |
0910.2560 | Miloslav Znojil | Miloslav Znojil | Fundamental length in quantum theories with PT-symmetric Hamiltonians
II: The case of quantum graphs | 33 pp., 6 figures | Phys.Rev.D80:105004,2009 | 10.1103/PhysRevD.80.105004 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Manifestly non-Hermitian quantum graphs with real spectra are introduced and
shown tractable as a new class of phenomenological models with several
appealing descriptive properties. For illustrative purposes, just equilateral
star-graphs are considered here in detail, with non-Hermiticities introduced by
interactions... | [
{
"created": "Wed, 14 Oct 2009 09:08:50 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Znojil",
"Miloslav",
""
]
] | Manifestly non-Hermitian quantum graphs with real spectra are introduced and shown tractable as a new class of phenomenological models with several appealing descriptive properties. For illustrative purposes, just equilateral star-graphs are considered here in detail, with non-Hermiticities introduced by interactions a... | 17.676731 | 20.4007 | 20.418039 | 18.722921 | 23.927708 | 20.768635 | 22.090199 | 19.297808 | 18.708923 | 20.400711 | 18.015585 | 18.23056 | 18.722248 | 18.3909 | 18.333736 | 18.324902 | 18.345854 | 18.423748 | 18.826176 | 18.643877 | 17.947317 |
0806.4900 | James Bedford | James Bedford and David Berman | A note on Quantum Aspects of Multiple Membranes | 12 pages, 2 figures. Uses axodraw. v3: Reference corrected, footnotes
modified | Phys.Lett.B668:67-71,2008 | 10.1016/j.physletb.2008.08.021 | Imperial-TP-08-JB-01; QMUL-PH-08-14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we investigate quantum aspects of the newly proposed theory of
multiple membranes put forward by Bagger and Lambert. In particular we analyse
the possibility of a finite renormalisation of the coupling at one loop.
| [
{
"created": "Mon, 30 Jun 2008 18:58:34 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Jul 2008 09:48:27 GMT",
"version": "v2"
},
{
"created": "Mon, 4 Aug 2008 10:17:31 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Bedford",
"James",
""
],
[
"Berman",
"David",
""
]
] | In this note we investigate quantum aspects of the newly proposed theory of multiple membranes put forward by Bagger and Lambert. In particular we analyse the possibility of a finite renormalisation of the coupling at one loop. | 14.980855 | 8.240608 | 13.114682 | 9.11149 | 8.417749 | 9.201556 | 8.561894 | 8.365003 | 9.638662 | 12.391 | 9.57595 | 9.178848 | 11.823323 | 10.192955 | 9.682703 | 9.68895 | 9.949424 | 9.665056 | 9.769492 | 11.842124 | 9.190623 |
1801.09337 | Peter Lowdon | Peter Lowdon | Dyson-Schwinger equation constraints on the gluon propagator in BRST
quantised QCD | 8 pages; v2: matches published version | Phys. Lett. B 786, 399 (2018) | 10.1016/j.physletb.2018.10.023 | SLAC-PUB-17219 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The gluon propagator plays a central role in determining the dynamics of QCD.
In this work we demonstrate for BRST quantised QCD that the Dyson-Schwinger
equation imposes significant analytic constraints on the structure of this
propagator. In particular, we find that these constraints control the
appearance of massl... | [
{
"created": "Mon, 29 Jan 2018 01:30:28 GMT",
"version": "v1"
},
{
"created": "Tue, 30 Oct 2018 15:57:49 GMT",
"version": "v2"
}
] | 2018-10-31 | [
[
"Lowdon",
"Peter",
""
]
] | The gluon propagator plays a central role in determining the dynamics of QCD. In this work we demonstrate for BRST quantised QCD that the Dyson-Schwinger equation imposes significant analytic constraints on the structure of this propagator. In particular, we find that these constraints control the appearance of massles... | 10.304866 | 9.84965 | 8.845588 | 8.851575 | 9.026417 | 8.510881 | 8.750641 | 8.384206 | 8.082273 | 9.051011 | 8.862131 | 9.297162 | 9.081611 | 8.852995 | 9.181688 | 9.37722 | 8.930552 | 8.755969 | 8.818332 | 9.350466 | 8.675144 |
hep-th/9310164 | Dr John W. Barrett | John W. Barrett and Bruce W. Westbury | Spherical Categories | 16 pages. Minor corrections | Adv.Math.143:357-375,1999 | 10.1006/aima.1998.1800 | null | hep-th math.QA | null | This paper is a study of monoidal categories with duals where the tensor
product need not be commutative. The motivating examples are categories of
representations of Hopf algebras and the motivating application is the
definition of 6j-symbols as used in topological field theories.
We introduce the new notion of a ... | [
{
"created": "Mon, 25 Oct 1993 15:45:14 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Jul 1998 00:24:24 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Barrett",
"John W.",
""
],
[
"Westbury",
"Bruce W.",
""
]
] | This paper is a study of monoidal categories with duals where the tensor product need not be commutative. The motivating examples are categories of representations of Hopf algebras and the motivating application is the definition of 6j-symbols as used in topological field theories. We introduce the new notion of a sphe... | 5.461334 | 6.188329 | 6.230689 | 5.623902 | 6.209777 | 6.659171 | 6.362764 | 5.652082 | 5.877104 | 6.147739 | 5.701531 | 5.600991 | 5.725172 | 5.559507 | 5.617645 | 5.531845 | 5.633927 | 5.518966 | 5.379493 | 5.494851 | 5.519853 |
hep-th/0507046 | Pavel Yu. Moshin | D.M. Gitman, P.Yu.Moshin, A.A. Reshetnyak | An Embedding of the BV Quantization into an N=1 Local Superfield
Formalism | 12 pages, LaTex, corrected typos, extended Introduction | Phys.Lett. B621 (2005) 295-308 | 10.1016/j.physletb.2005.06.071 | null | hep-th | null | We propose an N=1 superfield formulation of Lagrangian quantization in
general hypergauges by extending a reducible gauge theory to a superfield model
with a local dependence on a Grassmann parameter $\theta$. By means of
$\theta$-local functions of the quantum and gauge-fixing actions in terms of
Darboux coordinates... | [
{
"created": "Wed, 6 Jul 2005 01:48:53 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Aug 2005 18:12:39 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Gitman",
"D. M.",
""
],
[
"Moshin",
"P. Yu.",
""
],
[
"Reshetnyak",
"A. A.",
""
]
] | We propose an N=1 superfield formulation of Lagrangian quantization in general hypergauges by extending a reducible gauge theory to a superfield model with a local dependence on a Grassmann parameter $\theta$. By means of $\theta$-local functions of the quantum and gauge-fixing actions in terms of Darboux coordinates o... | 11.577081 | 8.490774 | 13.696072 | 9.55582 | 10.930529 | 8.533783 | 8.853888 | 8.565331 | 9.328824 | 13.985473 | 9.443765 | 10.753667 | 11.744053 | 11.020897 | 11.354811 | 11.16116 | 10.64049 | 10.700138 | 10.874178 | 11.810916 | 10.51457 |
1804.03279 | Kei-Ichi Kondo | Kei-Ichi Kondo | Gauge-independent Brout-Englert-Higgs mechanism and Yang-Mills theory
with a gauge-invariant gluon mass term | 21 pages, no figures; version published | Eur. Phys. J. C 78 (2018) 577 | 10.1140/epjc/s10052-018-6051-2 | CHIBA-EP-230 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For the Yang-Mills theory coupled to a single scalar field in the fundamental
representation of the gauge group, we present a gauge-independent description
of the Brout-Englert-Higgs mechanism by which massless gauge bosons acquire
their mass. The new description should be compared with the conventional
gauge-depende... | [
{
"created": "Tue, 10 Apr 2018 00:03:33 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Apr 2018 16:55:41 GMT",
"version": "v2"
},
{
"created": "Sun, 1 Jul 2018 15:50:58 GMT",
"version": "v3"
},
{
"created": "Wed, 18 Jul 2018 15:08:56 GMT",
"version": "v4"
}
] | 2018-08-15 | [
[
"Kondo",
"Kei-Ichi",
""
]
] | For the Yang-Mills theory coupled to a single scalar field in the fundamental representation of the gauge group, we present a gauge-independent description of the Brout-Englert-Higgs mechanism by which massless gauge bosons acquire their mass. The new description should be compared with the conventional gauge-dependent... | 7.446219 | 7.485816 | 8.502049 | 7.5076 | 7.641837 | 7.340502 | 7.781462 | 7.08698 | 7.125948 | 8.682196 | 7.187173 | 6.999133 | 7.353054 | 7.030814 | 6.994273 | 7.334355 | 7.122853 | 7.205553 | 7.228761 | 7.480409 | 7.023558 |
hep-th/0307084 | Senarath P. de Alwis | S.P. de Alwis | On Potentials from Fluxes | 24 pages, changes in concluding section, added references | Phys.Rev. D68 (2003) 126001 | 10.1103/PhysRevD.68.126001 | COLO-HEP 490 | hep-th | null | We discuss the compactification of type IIB supergravity with fluxes to
generate a potential for the moduli. In particular we resolve an apparent
conflict with the no-go theorem for de Sitter space. It is shown that a
positive potential for certain moduli is possible in situations where the
volume modulus has no crit... | [
{
"created": "Tue, 8 Jul 2003 19:00:07 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Jul 2003 22:48:32 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"de Alwis",
"S. P.",
""
]
] | We discuss the compactification of type IIB supergravity with fluxes to generate a potential for the moduli. In particular we resolve an apparent conflict with the no-go theorem for de Sitter space. It is shown that a positive potential for certain moduli is possible in situations where the volume modulus has no critic... | 8.475847 | 7.307631 | 8.323199 | 7.461705 | 8.002728 | 7.685178 | 7.529789 | 8.083568 | 7.688458 | 8.770791 | 7.066813 | 7.452622 | 7.901762 | 7.617363 | 7.453358 | 7.527343 | 7.644995 | 7.589021 | 7.743814 | 7.75144 | 7.519362 |
hep-th/9905015 | Timothy J. Hollowood | N. Michael Davies, Timothy J. Hollowood, Valentin V. Khoze and Michael
P. Mattis | Gluino Condensate and Magnetic Monopoles in Supersymmetric Gluodynamics | 23 pages, amstex, minor corrections | Nucl.Phys.B559:123-142,1999 | 10.1016/S0550-3213(99)00434-4 | null | hep-th hep-ph | null | We examine supersymmetric SU(N) gauge theories on R^3*S^1 with a circle of
circumference beta. These theories interpolate between four-dimensional N=1
pure gauge theory for beta=infinity and three-dimensional N=2 gauge theory for
beta=0. The dominant field configurations of the R^3*S^1 SU(N) theories in the
semi-clas... | [
{
"created": "Mon, 3 May 1999 18:56:23 GMT",
"version": "v1"
},
{
"created": "Tue, 11 May 1999 14:01:29 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Nov 1999 19:18:38 GMT",
"version": "v3"
}
] | 2009-07-09 | [
[
"Davies",
"N. Michael",
""
],
[
"Hollowood",
"Timothy J.",
""
],
[
"Khoze",
"Valentin V.",
""
],
[
"Mattis",
"Michael P.",
""
]
] | We examine supersymmetric SU(N) gauge theories on R^3*S^1 with a circle of circumference beta. These theories interpolate between four-dimensional N=1 pure gauge theory for beta=infinity and three-dimensional N=2 gauge theory for beta=0. The dominant field configurations of the R^3*S^1 SU(N) theories in the semi-classi... | 7.719134 | 7.776084 | 7.997717 | 7.303564 | 7.445825 | 7.533738 | 7.616317 | 7.611233 | 7.425036 | 8.576155 | 7.143731 | 7.525073 | 7.71269 | 7.310397 | 7.418362 | 7.440072 | 7.58504 | 7.478252 | 7.408286 | 7.802319 | 7.278883 |
1805.01919 | Skenderis Kostas | Michela Petrini, Henning Samtleben, Stanislav Schmidt and Kostas
Skenderis | The 10d Uplift of the GPPZ Solution | 45 pages, v3: JHEP version, Mathematica file with the IIB solution
and the verification of Einstein equations attached, corrected some typos,
v4: Note Added, typos corrected | J. High Energ. Phys. (2018) 2018: 26 | 10.1007/JHEP07(2018)026 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the uplift of the GPPZ solution of the five-dimensional maximal
supergravity to ten dimensions. The five dimensional solution involves two real
scalar fields, with one of them encoding holographically the (norm of the
complex) supersymmetric ${\mathcal N}=1$ mass deformation and the other the
real part of ... | [
{
"created": "Fri, 4 May 2018 19:33:48 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Jun 2018 10:41:58 GMT",
"version": "v2"
},
{
"created": "Fri, 6 Jul 2018 11:46:47 GMT",
"version": "v3"
},
{
"created": "Thu, 7 Feb 2019 13:44:18 GMT",
"version": "v4"
}
] | 2019-02-08 | [
[
"Petrini",
"Michela",
""
],
[
"Samtleben",
"Henning",
""
],
[
"Schmidt",
"Stanislav",
""
],
[
"Skenderis",
"Kostas",
""
]
] | We present the uplift of the GPPZ solution of the five-dimensional maximal supergravity to ten dimensions. The five dimensional solution involves two real scalar fields, with one of them encoding holographically the (norm of the complex) supersymmetric ${\mathcal N}=1$ mass deformation and the other the real part of th... | 6.079596 | 6.016973 | 6.287958 | 5.647926 | 5.930421 | 6.155458 | 5.960908 | 5.778075 | 5.900729 | 6.83221 | 5.667592 | 5.592 | 5.983286 | 5.596614 | 5.674074 | 5.797657 | 5.684356 | 5.710965 | 5.739088 | 5.86469 | 5.652238 |
1107.2357 | Cesar Fosco | C. Ccapa Ttira, C. D. Fosco, F. D. Mazzitelli | Lifshitz formula for the Casimir force and the Gelfand-Yaglom theorem | 13 pages, 1 figure | null | 10.1088/1751-8113/44/46/465403 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a Quantum Field Theory derivation of Lifshitz formula for the
Casimir force due to a fluctuating real scalar field in $d+1$ dimensions. The
field is coupled to two imperfect, thick, plane mirrors, which are modeled by
background potentials localized on their positions. The derivation proceeds
from the calc... | [
{
"created": "Tue, 12 Jul 2011 17:43:39 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Ttira",
"C. Ccapa",
""
],
[
"Fosco",
"C. D.",
""
],
[
"Mazzitelli",
"F. D.",
""
]
] | We provide a Quantum Field Theory derivation of Lifshitz formula for the Casimir force due to a fluctuating real scalar field in $d+1$ dimensions. The field is coupled to two imperfect, thick, plane mirrors, which are modeled by background potentials localized on their positions. The derivation proceeds from the calcul... | 11.160577 | 9.902076 | 11.09046 | 9.606582 | 9.570629 | 8.912534 | 10.249617 | 9.575819 | 9.819759 | 12.836086 | 9.732585 | 10.638211 | 10.486501 | 10.157727 | 10.382357 | 10.557679 | 10.871466 | 10.805593 | 10.227683 | 10.908846 | 10.198996 |
hep-th/9409019 | null | John Hiller, Steve Pinsky, and Brett van de Sande | Spontaneous symmetry breaking of (1+1)-dimensional $\bf \phi^4$ theory
in light-front field theory (III) | 21 pages; OHSTPY-HEP-TH-94-014 and DOE/ER/01545-63 | Phys.Rev. D51 (1995) 726-733 | 10.1103/PhysRevD.51.726 | null | hep-th | null | We investigate (1+1)-dimensional $\phi^4$ field theory in the symmetric and
broken phases using discrete light-front quantization. We calculate the
perturbative solution of the zero-mode constraint equation for both the
symmetric and broken phases and show that standard renormalization of the
theory yields finite res... | [
{
"created": "Sat, 3 Sep 1994 16:38:55 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Hiller",
"John",
""
],
[
"Pinsky",
"Steve",
""
],
[
"van de Sande",
"Brett",
""
]
] | We investigate (1+1)-dimensional $\phi^4$ field theory in the symmetric and broken phases using discrete light-front quantization. We calculate the perturbative solution of the zero-mode constraint equation for both the symmetric and broken phases and show that standard renormalization of the theory yields finite resul... | 8.146073 | 7.272797 | 7.812443 | 7.527704 | 7.829027 | 7.795225 | 7.77185 | 7.390317 | 7.395528 | 8.049107 | 7.48082 | 7.46547 | 7.996696 | 7.556263 | 7.6121 | 7.843652 | 7.589072 | 7.528563 | 7.607674 | 8.019131 | 7.544361 |
hep-th/0212149 | Andre van Tonder | Andre van Tonder (Brown University) | Cohomology and Decomposition of Tensor Product Representations of
SL(2,R) | 22 pages, no figures, Latex2e Added section on product of finite and
continuous series | Nucl.Phys. B677 (2004) 614-632 | 10.1016/j.nuclphysb.2003.10.029 | BROWN-HET-1338 | hep-th math.RT | null | We analyze the decomposition of tensor products between infinite dimensional
(unitary) and finite-dimensional (non-unitary) representations of SL(2,R).
Using classical results on indefinite inner product spaces, we derive explicit
decomposition formulae, true modulo a natural cohomological reduction, for the
tensor p... | [
{
"created": "Thu, 12 Dec 2002 22:08:58 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Nov 2003 21:10:29 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"van Tonder",
"Andre",
"",
"Brown University"
]
] | We analyze the decomposition of tensor products between infinite dimensional (unitary) and finite-dimensional (non-unitary) representations of SL(2,R). Using classical results on indefinite inner product spaces, we derive explicit decomposition formulae, true modulo a natural cohomological reduction, for the tensor pro... | 17.44459 | 18.819653 | 15.110776 | 13.670003 | 15.742449 | 15.951027 | 14.931561 | 17.592554 | 14.77231 | 16.236021 | 14.216401 | 14.573788 | 16.363535 | 15.991446 | 15.412277 | 15.148998 | 15.172355 | 15.431725 | 14.943819 | 15.877596 | 14.956105 |
2204.07590 | Suzanne Bintanja | Luis Apolo, Alexandre Belin, Suzanne Bintanja, Alejandra Castro,
Christoph A. Keller | Deforming Symmetric Product Orbifolds: A tale of moduli and higher spin
currents | 47 pages, v2: minor changes, v3: version as published in JHEP | JHEP 8, 159 (2022) | 10.1007/JHEP08(2022)159 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze how deforming symmetric product orbifolds of two-dimensional
$\mathcal{N}=2$ conformal field theories by an exactly marginal operator lifts
higher spin currents present at the orbifold point. We find on the one hand
that these currents are universally lifted regardless of the underlying CFT. On
the other h... | [
{
"created": "Fri, 15 Apr 2022 18:00:04 GMT",
"version": "v1"
},
{
"created": "Wed, 11 May 2022 09:20:38 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Aug 2022 12:19:56 GMT",
"version": "v3"
}
] | 2022-08-25 | [
[
"Apolo",
"Luis",
""
],
[
"Belin",
"Alexandre",
""
],
[
"Bintanja",
"Suzanne",
""
],
[
"Castro",
"Alejandra",
""
],
[
"Keller",
"Christoph A.",
""
]
] | We analyze how deforming symmetric product orbifolds of two-dimensional $\mathcal{N}=2$ conformal field theories by an exactly marginal operator lifts higher spin currents present at the orbifold point. We find on the one hand that these currents are universally lifted regardless of the underlying CFT. On the other han... | 6.931323 | 6.538797 | 8.480137 | 6.720985 | 6.49392 | 6.554155 | 6.29439 | 6.439599 | 6.424947 | 7.908835 | 6.253588 | 6.730677 | 7.258704 | 6.668059 | 6.70525 | 6.663574 | 6.47875 | 6.623616 | 6.585277 | 7.236847 | 6.560414 |
2407.16538 | Jose Antonio Oller | J. A. Oller and Marcela Pel\'aez | Unitarization of the one-loop graviton-graviton scattering amplitudes
and study of the graviball | 12 pages, 3 figures | null | null | null | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | From the graviton-graviton scattering amplitudes calculated perturbatively in
quantum gravity to the one-loop order, we develop further a formalism that
allows one to calculate infrared-finite partial-wave amplitudes fulfilling
perturbative unitarity. As a result of this process a parameter dubbed $\ln a$
emerges tha... | [
{
"created": "Tue, 23 Jul 2024 14:47:49 GMT",
"version": "v1"
}
] | 2024-07-24 | [
[
"Oller",
"J. A.",
""
],
[
"Peláez",
"Marcela",
""
]
] | From the graviton-graviton scattering amplitudes calculated perturbatively in quantum gravity to the one-loop order, we develop further a formalism that allows one to calculate infrared-finite partial-wave amplitudes fulfilling perturbative unitarity. As a result of this process a parameter dubbed $\ln a$ emerges that ... | 12.182068 | 13.578442 | 11.864353 | 11.587726 | 12.740289 | 12.632568 | 12.420585 | 12.489678 | 11.490197 | 13.062151 | 12.51077 | 11.809973 | 11.150745 | 11.049983 | 11.427193 | 11.810826 | 11.841689 | 11.774635 | 10.933635 | 11.077085 | 11.928892 |
1204.0126 | Daniel Kabat | Daniel Kabat, Gilad Lifschytz, Shubho Roy, Debajyoti Sarkar | Holographic representation of bulk fields with spin in AdS/CFT | 45 pages, LaTeX, 1 figure. v2: corrected typo in equation (75) | null | 10.1103/PhysRevD.86.026004 | NSF-KITP-12-045 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop the representation of bulk fields with spin one and spin two in
anti-de Sitter space, as non-local observables in the dual CFT. Working in
holographic gauge in the bulk, at leading order in 1/N bulk gauge fields are
obtained by smearing boundary currents over a sphere on the complexified
boundary, while li... | [
{
"created": "Sat, 31 Mar 2012 19:45:02 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Jul 2012 17:30:50 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Kabat",
"Daniel",
""
],
[
"Lifschytz",
"Gilad",
""
],
[
"Roy",
"Shubho",
""
],
[
"Sarkar",
"Debajyoti",
""
]
] | We develop the representation of bulk fields with spin one and spin two in anti-de Sitter space, as non-local observables in the dual CFT. Working in holographic gauge in the bulk, at leading order in 1/N bulk gauge fields are obtained by smearing boundary currents over a sphere on the complexified boundary, while line... | 9.511865 | 8.642889 | 10.449836 | 8.853103 | 9.180617 | 9.057125 | 7.907819 | 8.728301 | 8.717265 | 11.045473 | 8.417167 | 9.087429 | 9.885881 | 9.037048 | 9.280107 | 9.121469 | 8.88864 | 9.03021 | 8.747566 | 10.354194 | 8.970278 |
1610.04163 | Kallosh Renata | Sergio Ferrara and Renata Kallosh | Seven-Disk Manifold, alpha-attractors and B-modes | 11 p, 1 figure | Phys. Rev. D 94, 126015 (2016) | 10.1103/PhysRevD.94.126015 | CERN-TH-2016-214 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Cosmological alpha-attractor models in \cN=1 supergravity are based on
hyperbolic geometry of a Poincar\'e disk with the radius square {\cal
R}^2=3\alpha. The predictions for the B-modes, r\approx 3\alpha {4\over N^2},
depend on moduli space geometry and are robust for a rather general class of
potentials. Here we no... | [
{
"created": "Thu, 13 Oct 2016 16:35:47 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Oct 2016 20:11:06 GMT",
"version": "v2"
}
] | 2017-01-04 | [
[
"Ferrara",
"Sergio",
""
],
[
"Kallosh",
"Renata",
""
]
] | Cosmological alpha-attractor models in \cN=1 supergravity are based on hyperbolic geometry of a Poincar\'e disk with the radius square {\cal R}^2=3\alpha. The predictions for the B-modes, r\approx 3\alpha {4\over N^2}, depend on moduli space geometry and are robust for a rather general class of potentials. Here we noti... | 10.359295 | 10.994797 | 12.185797 | 10.489907 | 11.117264 | 12.886961 | 12.357285 | 10.236492 | 10.810264 | 12.485953 | 10.384271 | 10.247566 | 10.806329 | 10.154424 | 10.589951 | 10.760725 | 10.612573 | 10.060728 | 10.05394 | 10.949947 | 10.313741 |
hep-th/9511058 | Rolf Schimmrigk | Monika Lynker and Rolf Schimmrigk | Conifold Transitions and Mirror Symmetries | 23 pages | Nucl.Phys. B484 (1997) 562-582 | 10.1016/S0550-3213(96)00557-3 | NSF-ITP-95-141, BONN-TH-95-20 | hep-th | null | Recent work initiated by Strominger has lead to a consistent physical
interpretation of certain types of transitions between different string vacua.
These transitions, discovered several years ago, involve singular conifold
configurations which connect distinct Calabi-Yau manifolds. In this paper we
discuss a number ... | [
{
"created": "Thu, 9 Nov 1995 07:42:45 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Lynker",
"Monika",
""
],
[
"Schimmrigk",
"Rolf",
""
]
] | Recent work initiated by Strominger has lead to a consistent physical interpretation of certain types of transitions between different string vacua. These transitions, discovered several years ago, involve singular conifold configurations which connect distinct Calabi-Yau manifolds. In this paper we discuss a number of... | 10.760255 | 11.213993 | 12.035506 | 10.84021 | 11.491983 | 11.420115 | 11.065845 | 10.800413 | 10.744579 | 12.315018 | 10.530025 | 10.770969 | 11.026145 | 10.76411 | 10.916397 | 11.001666 | 10.858811 | 10.829084 | 10.615085 | 10.986794 | 10.594373 |
1412.4499 | Diego Rubiera-Garcia | Francisco S. N. Lobo, Gonzalo J. Olmo, and D. Rubiera-Garcia | Crystal clear lessons on the microstructure of space-time and modified
gravity | 7 pages; some minor corrections added | Phys. Rev. D 91, 124001 (2015) | 10.1103/PhysRevD.91.124001 | IFIC/14-82 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that a microscopic structure for space-time such as that expected in
a quantum foam scenario, in which microscopic wormholes and other topological
structures should play a relevant role, might lead to an effective
metric-affine geometry at larger scales. This idea is supported by the role
that microscopic de... | [
{
"created": "Mon, 15 Dec 2014 08:52:06 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Jun 2015 05:36:59 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"Lobo",
"Francisco S. N.",
""
],
[
"Olmo",
"Gonzalo J.",
""
],
[
"Rubiera-Garcia",
"D.",
""
]
] | We argue that a microscopic structure for space-time such as that expected in a quantum foam scenario, in which microscopic wormholes and other topological structures should play a relevant role, might lead to an effective metric-affine geometry at larger scales. This idea is supported by the role that microscopic defe... | 12.439172 | 13.342094 | 10.809674 | 10.802661 | 12.158718 | 12.150558 | 13.476381 | 11.208 | 12.458302 | 12.061182 | 12.500022 | 11.512044 | 11.446293 | 11.436634 | 11.583494 | 11.639677 | 12.027411 | 11.630564 | 11.869675 | 11.824835 | 11.66753 |
hep-th/0206001 | Hyun Seok Yang | Bum-Hoon Lee and Hyun Seok Yang | Propagators in Noncommutative Instantons | 28 pages, Latex, v2: A few typos corrected | Phys.Rev. D66 (2002) 045027 | 10.1103/PhysRevD.66.045027 | SOGANG-HEP 298/02 | hep-th hep-ph | null | We explicitly construct Green functions for a field in an arbitrary
representation of gauge group propagating in noncommutative instanton
backgrounds based on the ADHM construction. The propagators for spinor and
vector fields can be constructed in terms of those for the scalar field in
noncommutative instanton backg... | [
{
"created": "Mon, 3 Jun 2002 05:50:40 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jun 2002 09:50:40 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Lee",
"Bum-Hoon",
""
],
[
"Yang",
"Hyun Seok",
""
]
] | We explicitly construct Green functions for a field in an arbitrary representation of gauge group propagating in noncommutative instanton backgrounds based on the ADHM construction. The propagators for spinor and vector fields can be constructed in terms of those for the scalar field in noncommutative instanton backgro... | 6.326136 | 5.613842 | 6.46788 | 5.701041 | 5.287784 | 5.698781 | 5.503719 | 5.4265 | 5.370869 | 7.052738 | 5.524225 | 5.677609 | 6.346845 | 5.793872 | 5.561834 | 5.598846 | 5.626035 | 5.744774 | 5.917403 | 6.346336 | 5.733216 |
2302.04827 | Gustavo Brito | Gustavo P. de Brito, Philipe De Fabritiis, Antonio D. Pereira | Refined Gribov-Zwanziger theory coupled to scalar fields in the Landau
gauge | 18 pages + refs.; 6 figures; Matches the journal version | null | 10.1103/PhysRevD.107.114006 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Refined Gribov-Zwanziger (RGZ) action in the Landau gauge accounts for
the existence of infinitesimal Gribov copies as well as the dynamical formation
of condensates in the infrared of Euclidean Yang-Mills theories. We couple
scalar fields to the RGZ action and compute the one-loop scalar propagator in
the adjoin... | [
{
"created": "Thu, 9 Feb 2023 18:31:55 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Sep 2023 16:59:04 GMT",
"version": "v2"
}
] | 2023-09-11 | [
[
"de Brito",
"Gustavo P.",
""
],
[
"De Fabritiis",
"Philipe",
""
],
[
"Pereira",
"Antonio D.",
""
]
] | The Refined Gribov-Zwanziger (RGZ) action in the Landau gauge accounts for the existence of infinitesimal Gribov copies as well as the dynamical formation of condensates in the infrared of Euclidean Yang-Mills theories. We couple scalar fields to the RGZ action and compute the one-loop scalar propagator in the adjoint ... | 6.854884 | 5.95442 | 6.376325 | 5.691506 | 5.879004 | 5.828968 | 6.265109 | 5.76789 | 5.730329 | 6.443921 | 5.706187 | 6.042635 | 6.482946 | 5.962708 | 6.011082 | 6.108139 | 6.057845 | 5.952624 | 6.189843 | 6.343111 | 6.181142 |
1710.09994 | Yasuyuki Hatsuda | Dongmin Gang, Yasuyuki Hatsuda | S-duality resurgence in SL(2) Chern-Simons theory | 23 pages | null | 10.1007/JHEP07(2018)053 | RUP-17-22 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find that an S-duality in SL(2) Chern-Simons theory for hyperbolic
3-manifolds emerges by the Borel resummation of a semiclassical expansion
around a particular flat connection associated to the hyperbolic structure. We
demonstrate it numerically with two representative examples of hyperbolic
3-manifolds.
| [
{
"created": "Fri, 27 Oct 2017 05:50:45 GMT",
"version": "v1"
}
] | 2018-08-01 | [
[
"Gang",
"Dongmin",
""
],
[
"Hatsuda",
"Yasuyuki",
""
]
] | We find that an S-duality in SL(2) Chern-Simons theory for hyperbolic 3-manifolds emerges by the Borel resummation of a semiclassical expansion around a particular flat connection associated to the hyperbolic structure. We demonstrate it numerically with two representative examples of hyperbolic 3-manifolds. | 9.87696 | 7.828605 | 10.647938 | 7.931408 | 7.709108 | 8.169864 | 7.690116 | 7.900442 | 8.353112 | 10.28158 | 7.661574 | 8.228185 | 8.639238 | 8.556962 | 8.0172 | 8.209606 | 8.085483 | 8.349172 | 8.845644 | 8.057187 | 8.456732 |
hep-th/9507139 | Moretti Walter | Valter Moretti, Luciano Vanzo (Dept. Phys. Univ. Trento Italy) | Thermal Wightman Functions and Renormalized Stress Tensors in the
Rindler Wedge | More comments and formulas added in the case of spin 1, a few signs
changed in some formulas, it will appear on Phys. Lett | Phys.Lett. B375 (1996) 54-59 | 10.1016/0370-2693(96)00223-7 | UTF 352 | hep-th gr-qc | null | The Wightman functions in the Rindler portion of Minkowski space-time are
presented for any value of the temperature and for massless spin fields up to
s=1 and the renormalized stress tensor relative to Minkowski vacuum is
discussed. A gauge ambiguity in the vector case is pointed out.
| [
{
"created": "Wed, 26 Jul 1995 10:11:02 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Feb 1996 09:55:09 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Moretti",
"Valter",
"",
"Dept. Phys. Univ. Trento Italy"
],
[
"Vanzo",
"Luciano",
"",
"Dept. Phys. Univ. Trento Italy"
]
] | The Wightman functions in the Rindler portion of Minkowski space-time are presented for any value of the temperature and for massless spin fields up to s=1 and the renormalized stress tensor relative to Minkowski vacuum is discussed. A gauge ambiguity in the vector case is pointed out. | 17.98992 | 13.540059 | 13.919737 | 12.580667 | 12.804783 | 14.374908 | 14.444385 | 14.542109 | 12.461155 | 17.470417 | 12.379324 | 13.457001 | 13.885437 | 12.699297 | 14.125863 | 15.901181 | 14.372752 | 13.117484 | 12.611828 | 13.726416 | 13.607366 |
2009.11305 | Ronak M Soni | Adam Levine, Arvin Shahbazi-Moghaddam, Ronak M Soni | Seeing the Entanglement Wedge | 53 pages, 7 figures; version accepted for publication | JHEP06(2021)134 | 10.1007/JHEP06(2021)134 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the problem of revealing the entanglement wedge using simple
operations. We ask what operation a semiclassical observer can do to bring the
entanglement wedge into causal contact with the boundary, via backreaction.
In a generic perturbative class of states, we propose a unitary operation in
the causal wed... | [
{
"created": "Wed, 23 Sep 2020 18:00:04 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Oct 2020 01:23:20 GMT",
"version": "v2"
},
{
"created": "Fri, 11 Jun 2021 21:51:22 GMT",
"version": "v3"
}
] | 2021-06-24 | [
[
"Levine",
"Adam",
""
],
[
"Shahbazi-Moghaddam",
"Arvin",
""
],
[
"Soni",
"Ronak M",
""
]
] | We study the problem of revealing the entanglement wedge using simple operations. We ask what operation a semiclassical observer can do to bring the entanglement wedge into causal contact with the boundary, via backreaction. In a generic perturbative class of states, we propose a unitary operation in the causal wedge w... | 11.785682 | 12.89862 | 13.803663 | 12.313409 | 13.347255 | 12.735988 | 14.246437 | 12.724409 | 12.661633 | 15.177927 | 12.334602 | 11.874748 | 12.233873 | 11.570607 | 11.411491 | 11.778808 | 12.177589 | 11.827223 | 11.960047 | 13.153324 | 11.342037 |
1102.0739 | Gerry McKeon | D.G.C. McKeon | The Renormalization Group and the Effective Action | null | null | 10.1139/P11-021 | null | hep-th | http://creativecommons.org/licenses/by/3.0/ | The renormalization group is used to sum the leading-log (LL) contributions
to the effective action for a large constant external gauge field in terms of
the one-loop renormalization group (RG) function beta, the next-to-leading-log
(NLL) contributions in terms of the two-loop RG function etc. The log
independent pie... | [
{
"created": "Thu, 3 Feb 2011 17:31:31 GMT",
"version": "v1"
}
] | 2015-05-27 | [
[
"McKeon",
"D. G. C.",
""
]
] | The renormalization group is used to sum the leading-log (LL) contributions to the effective action for a large constant external gauge field in terms of the one-loop renormalization group (RG) function beta, the next-to-leading-log (NLL) contributions in terms of the two-loop RG function etc. The log independent piece... | 8.034149 | 6.91458 | 7.843657 | 6.766915 | 7.008883 | 6.915791 | 7.273717 | 6.765936 | 6.951297 | 8.311347 | 6.710999 | 7.151541 | 7.165874 | 6.824505 | 7.233502 | 7.045459 | 7.148375 | 6.845933 | 7.04074 | 7.176861 | 7.014687 |
1704.05855 | Harold Erbin | Corinne de Lacroix and Harold Erbin and Eirik E. Svanes | Minisuperspace computation of the Mabuchi spectrum | 23 pages; v2: minor improvements, match published version | null | 10.1088/1361-6382/aad7f3 | LPTENS/17/08 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was shown recently that, beside the traditional Liouville action, other
functionals appear in the gravitational action of two-dimensional quantum
gravity in the conformal gauge, the most important one being the Mabuchi
functional. In a letter we proposed a minisuperspace action for this theory and
used it to perfo... | [
{
"created": "Wed, 19 Apr 2017 18:00:07 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Aug 2018 13:22:31 GMT",
"version": "v2"
}
] | 2018-08-07 | [
[
"de Lacroix",
"Corinne",
""
],
[
"Erbin",
"Harold",
""
],
[
"Svanes",
"Eirik E.",
""
]
] | It was shown recently that, beside the traditional Liouville action, other functionals appear in the gravitational action of two-dimensional quantum gravity in the conformal gauge, the most important one being the Mabuchi functional. In a letter we proposed a minisuperspace action for this theory and used it to perform... | 9.988958 | 8.720465 | 9.586521 | 8.962365 | 8.844872 | 9.015141 | 8.677904 | 8.776742 | 8.843415 | 9.689548 | 8.967629 | 8.960291 | 9.180744 | 9.172931 | 9.133009 | 8.941197 | 9.134706 | 9.006163 | 9.326274 | 9.580519 | 9.277291 |
1103.4759 | Roldao da Rocha | Roldao da Rocha, Alex E. Bernardini, J. M. Hoff da Silva | Exotic Dark Spinor Fields | 24 pages. Part of Section 2 was sent to Appendix. References updated | JHEP 1104:110,2011 | 10.1007/JHEP04(2011)110 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Exotic dark spinor fields are introduced and investigated in the context of
inequivalent spin structures on arbitrary curved spacetimes, which induces an
additional term on the associated Dirac operator, related to a Cech cohomology
class. For the most kinds of spinor fields, any exotic term in the Dirac
operator can... | [
{
"created": "Thu, 24 Mar 2011 13:19:35 GMT",
"version": "v1"
},
{
"created": "Thu, 12 May 2011 09:40:35 GMT",
"version": "v2"
}
] | 2011-05-13 | [
[
"da Rocha",
"Roldao",
""
],
[
"Bernardini",
"Alex E.",
""
],
[
"da Silva",
"J. M. Hoff",
""
]
] | Exotic dark spinor fields are introduced and investigated in the context of inequivalent spin structures on arbitrary curved spacetimes, which induces an additional term on the associated Dirac operator, related to a Cech cohomology class. For the most kinds of spinor fields, any exotic term in the Dirac operator can b... | 12.443582 | 13.235372 | 13.80574 | 12.68973 | 12.460228 | 13.871424 | 13.712746 | 12.403573 | 12.443286 | 13.414173 | 12.631466 | 11.900187 | 12.777391 | 12.311357 | 12.277999 | 12.621862 | 12.279835 | 12.199135 | 12.569852 | 12.528234 | 12.060546 |
0905.2856 | Pavel Yu. Moshin | A.V. Timoshkin | Specially Coupled Dark Energy in the Oscillating FRW Cosmology | 4 pages | Open Astron.J.2:39-42,2009 | 10.2174/1874381100902010039 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a four-dimensional flat-space Friedman universe, which is filled
with two interacting ideal fluids (the coupling of dark energy with dark matter
of special form). The gravitational equations of motion are solved. It is shown
that in some cases there appears a periodic universe with finite-time
cosmologica... | [
{
"created": "Mon, 18 May 2009 11:00:23 GMT",
"version": "v1"
}
] | 2009-09-07 | [
[
"Timoshkin",
"A. V.",
""
]
] | We consider a four-dimensional flat-space Friedman universe, which is filled with two interacting ideal fluids (the coupling of dark energy with dark matter of special form). The gravitational equations of motion are solved. It is shown that in some cases there appears a periodic universe with finite-time cosmological ... | 17.427637 | 16.486553 | 15.433638 | 15.531272 | 14.973228 | 15.340782 | 15.398037 | 14.961758 | 15.537735 | 16.358604 | 14.923396 | 15.249289 | 15.781671 | 15.899218 | 15.85034 | 16.366049 | 16.145502 | 15.752316 | 17.011499 | 15.798973 | 15.862952 |
2012.11693 | Joe Davighi | Joe Davighi, Nakarin Lohitsiri | Omega vs. pi, and 6d anomaly cancellation | 36 pages, 6 figures. Footnotes added to clarify notation for
eta-invariant. Matches version accepted for publication | null | 10.1007/JHEP05(2021)267 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we review the role of homotopy groups in determining
non-perturbative (henceforth `global') gauge anomalies, in light of recent
progress understanding global anomalies using bordism. We explain why
non-vanishing of $\pi_d(G)$ is neither a necessary nor a sufficient condition
for there being a possible gl... | [
{
"created": "Mon, 21 Dec 2020 21:40:27 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Nov 2021 16:40:17 GMT",
"version": "v2"
}
] | 2021-11-12 | [
[
"Davighi",
"Joe",
""
],
[
"Lohitsiri",
"Nakarin",
""
]
] | In this note we review the role of homotopy groups in determining non-perturbative (henceforth `global') gauge anomalies, in light of recent progress understanding global anomalies using bordism. We explain why non-vanishing of $\pi_d(G)$ is neither a necessary nor a sufficient condition for there being a possible glob... | 6.430677 | 6.929078 | 6.541613 | 6.046662 | 6.827001 | 6.927278 | 6.86482 | 6.426245 | 6.263206 | 7.522056 | 6.248602 | 6.022964 | 6.240172 | 6.011712 | 6.123201 | 6.017423 | 5.979239 | 6.15847 | 6.018907 | 6.172468 | 5.864271 |
2003.07381 | Vladimir Rosenhaus | Vladimir Rosenhaus | Chaos in the Quantum Field Theory $S$-matrix | v2 - minor changes, 5 pages | Phys. Rev. Lett. 127, 021601 (2021) | 10.1103/PhysRevLett.127.021601 | null | hep-th cond-mat.str-el nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A number of studies have shown that chaos occurs in scattering: the outgoing
deflection angle is seen to be an erratic function of the impact parameter. We
propose to extend this to quantum field theory, and to use erratic behavior of
the many-particle $S$-matrix as a probe of chaos.
| [
{
"created": "Mon, 16 Mar 2020 18:01:11 GMT",
"version": "v1"
},
{
"created": "Fri, 28 May 2021 00:36:28 GMT",
"version": "v2"
}
] | 2021-07-14 | [
[
"Rosenhaus",
"Vladimir",
""
]
] | A number of studies have shown that chaos occurs in scattering: the outgoing deflection angle is seen to be an erratic function of the impact parameter. We propose to extend this to quantum field theory, and to use erratic behavior of the many-particle $S$-matrix as a probe of chaos. | 16.068893 | 14.194844 | 14.218429 | 13.380175 | 14.241729 | 11.894676 | 13.256992 | 13.087757 | 12.211792 | 14.406964 | 13.582955 | 12.174556 | 12.764508 | 12.095894 | 12.837503 | 12.622763 | 11.881695 | 12.269129 | 12.187195 | 13.579257 | 13.259445 |
hep-th/9209037 | null | E. Bergshoeff, A. Sevrin and X. Shen | A Derivation of the BRST Operator for Non-Critical W-Strings | TEX file, pp14, UG-8/92, CERN-TH.6647/92,LBL-32806 | Phys.Lett. B296 (1992) 95-103 | 10.1016/0370-2693(92)90808-H | null | hep-th | null | We derive the recently proposed BRST charge for non-critical W strings from a
Lagragian approach. The basic observation is that, despite appearances, the
combination of two classical ``matter'' and ``Toda'' w_3 systems leads to a
closed modified gauge algebra, which is of the so-called soft type. Based on
these obser... | [
{
"created": "Fri, 11 Sep 1992 16:34:20 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Bergshoeff",
"E.",
""
],
[
"Sevrin",
"A.",
""
],
[
"Shen",
"X.",
""
]
] | We derive the recently proposed BRST charge for non-critical W strings from a Lagragian approach. The basic observation is that, despite appearances, the combination of two classical ``matter'' and ``Toda'' w_3 systems leads to a closed modified gauge algebra, which is of the so-called soft type. Based on these observa... | 25.962009 | 20.214388 | 28.337 | 20.152248 | 22.580471 | 23.354908 | 21.54501 | 21.529655 | 21.211702 | 31.296535 | 22.114361 | 21.437944 | 27.379406 | 21.685129 | 22.1546 | 22.226244 | 21.571016 | 22.960827 | 22.3722 | 26.691137 | 21.315279 |
hep-th/0104072 | Karim Ait Moussa | Karim Ait Moussa | On the (im)possibility of a supersymmetric extension of NGT | 17 pages, Latex,two references added, minor changes for clarity, v3:
E-mail changed, v4 : Ref(9) corrected | Class.Quant.Grav.20:193-204,2003 | 10.1088/0264-9381/20/1/314 | null | hep-th | null | We investigate the possibility of constructing a locally supersymmetric
extension of NGT (Nonsymmetric Gravitation Theory), based on the graded
extension of the Poincare group. In the framework of the simple model that we
propose, we end up with a no-go result, namely the impossibility of cancelling
some linear contr... | [
{
"created": "Mon, 9 Apr 2001 01:57:54 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Oct 2002 17:12:15 GMT",
"version": "v2"
},
{
"created": "Thu, 24 Oct 2002 13:42:47 GMT",
"version": "v3"
},
{
"created": "Mon, 28 Oct 2002 10:34:34 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Moussa",
"Karim Ait",
""
]
] | We investigate the possibility of constructing a locally supersymmetric extension of NGT (Nonsymmetric Gravitation Theory), based on the graded extension of the Poincare group. In the framework of the simple model that we propose, we end up with a no-go result, namely the impossibility of cancelling some linear contrib... | 10.059819 | 10.773665 | 10.296382 | 8.660217 | 9.590788 | 9.208976 | 9.828848 | 8.987585 | 9.336283 | 9.503577 | 9.138549 | 8.754652 | 8.95414 | 8.858969 | 8.912627 | 9.315285 | 9.077229 | 8.907418 | 9.315642 | 8.980134 | 9.055438 |
2105.10526 | Jakob Salzer | Kevin Nguyen and Jakob Salzer | Celestial IR divergences and the effective action of supertranslation
modes | 24 pages, one figure | JHEP 09 (2021) 144 | 10.1007/JHEP09(2021)144 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Infrared divergences in perturbative gravitational scattering amplitudes have
been recently argued to be governed by the two-point function of the
supertranslation Goldstone mode on the celestial sphere. We show that the form
of this celestial two-point function simply derives from an effective action
that also contr... | [
{
"created": "Fri, 21 May 2021 18:29:29 GMT",
"version": "v1"
}
] | 2021-11-30 | [
[
"Nguyen",
"Kevin",
""
],
[
"Salzer",
"Jakob",
""
]
] | Infrared divergences in perturbative gravitational scattering amplitudes have been recently argued to be governed by the two-point function of the supertranslation Goldstone mode on the celestial sphere. We show that the form of this celestial two-point function simply derives from an effective action that also control... | 10.197848 | 7.68413 | 8.742746 | 7.811709 | 8.115948 | 7.593359 | 7.864602 | 8.080411 | 7.688508 | 9.442411 | 8.221635 | 8.160669 | 8.01881 | 7.908947 | 7.920144 | 8.211895 | 8.197171 | 8.162826 | 8.42325 | 8.272549 | 8.13614 |
hep-th/9711050 | Bodo Geyer | B. Geyer (Leipzig University) and D. M"ulsch (Wissenschaftszentrum
e.V.) | Symmetry properties of massive gauge theories in nonlinear background
gauges: Background dependence of Green functions | 10 pages, LATEX | null | null | NTZ-29/97 | hep-th | null | Nonabelian gauge theories with a generic background field A_mu in nonlinear
gauges due to Delbourgo and Jarvis are investigated. The A_mu-dependence is
completely determined by the help of a linear differential equation which
obtaines from the Kluberg-Stern-Zuber and the Lee identity. Its integration
leads to a relat... | [
{
"created": "Fri, 7 Nov 1997 16:17:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Geyer",
"B.",
"",
"Leipzig University"
],
[
"M\"ulsch",
"D.",
"",
"Wissenschaftszentrum\n e.V."
]
] | Nonabelian gauge theories with a generic background field A_mu in nonlinear gauges due to Delbourgo and Jarvis are investigated. The A_mu-dependence is completely determined by the help of a linear differential equation which obtaines from the Kluberg-Stern-Zuber and the Lee identity. Its integration leads to a relatio... | 14.114811 | 15.199516 | 14.996625 | 13.617685 | 14.303494 | 16.164791 | 15.11493 | 14.732084 | 13.845585 | 19.192549 | 13.629678 | 13.058446 | 13.566685 | 12.747186 | 13.145897 | 13.086312 | 12.971819 | 13.485577 | 12.627506 | 14.295991 | 12.639699 |
0712.3529 | Vladimir Nesterenko | V.V. Nesterenko | Surface modes and photonic modes in Casimir calculations for a compact
cylinder | 8 pages, no tables and figures, RevTex4 | J.Phys.A41:164005,2008 | 10.1088/1751-8113/41/16/164005 | null | hep-th | null | A rigorous formulation of the problem of calculating the electromagnetic
vacuum energy of an infinite dielectric cylinder is discussed. It is shown that
the physically relevant spectrum of electromagnetic excitations includes the
surface modes and photonic modes. The mathematical procedure of summing over
this spectr... | [
{
"created": "Thu, 20 Dec 2007 19:00:21 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Nesterenko",
"V. V.",
""
]
] | A rigorous formulation of the problem of calculating the electromagnetic vacuum energy of an infinite dielectric cylinder is discussed. It is shown that the physically relevant spectrum of electromagnetic excitations includes the surface modes and photonic modes. The mathematical procedure of summing over this spectrum... | 14.900937 | 14.473403 | 14.286614 | 13.135464 | 15.426581 | 14.16518 | 14.153773 | 13.428985 | 12.604424 | 14.833229 | 14.172029 | 13.620907 | 13.843559 | 13.579604 | 13.556571 | 13.843222 | 13.401805 | 13.213168 | 13.353315 | 13.617881 | 13.832364 |
2301.10668 | Dmitri Sorokin | Igor A. Bandos and Dmitri P. Sorokin | Superembedding approach to superstrings and super-p-branes | 61 page; v2: typos corrected, references added. Chapter for the
Section "String Theories" (Eds. C. Angelantonj and I. Antoniadis) of the
"Handbook of Quantum Gravity" (Eds. C. Bambi, L. Modesto and I.L. Shapiro,
Springer Singapore, expected in 2023) | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review a geometrical, so called superembedding, approach to the
description of the dynamics of point-like and extended supersymmetric objects
(superbranes) in String Theory. The approach is based on a supersymmetric
extension of the classical surface theory to the description of superbrane
dynamics by means of emb... | [
{
"created": "Wed, 25 Jan 2023 16:16:05 GMT",
"version": "v1"
},
{
"created": "Sun, 10 Mar 2024 17:39:33 GMT",
"version": "v2"
}
] | 2024-03-12 | [
[
"Bandos",
"Igor A.",
""
],
[
"Sorokin",
"Dmitri P.",
""
]
] | We review a geometrical, so called superembedding, approach to the description of the dynamics of point-like and extended supersymmetric objects (superbranes) in String Theory. The approach is based on a supersymmetric extension of the classical surface theory to the description of superbrane dynamics by means of embed... | 8.098463 | 7.910487 | 8.737573 | 7.402863 | 7.725958 | 8.055985 | 7.952764 | 7.552613 | 7.499528 | 9.361106 | 7.529926 | 7.561439 | 8.195631 | 7.708588 | 7.7638 | 7.609749 | 7.856776 | 7.692838 | 7.64038 | 8.019242 | 7.618524 |
hep-th/9501141 | Rupak Chatterjee | Rupak Chatterjee | Dynamical Symmetries and Nambu Mechanics | 9 pages, Latex, Section four on the SO(4)-Kepler problem has been
expanded | Lett. Math. Phys. 36 (1996) 117 | 10.1007/BF00714375 | hep-th/9501141 | hep-th | null | It is shown that several Hamiltonian systems possessing dynamical or hidden
symmetries can be realized within the framework of Nambu's generalized
mechanics. Among such systems are the SU(n)-isotropic harmonic oscillator and
the SO(4)-Kepler problem. As required by the formulation of Nambu dynamics, the
integrals of ... | [
{
"created": "Tue, 31 Jan 1995 19:16:40 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Feb 1995 16:49:46 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Chatterjee",
"Rupak",
""
]
] | It is shown that several Hamiltonian systems possessing dynamical or hidden symmetries can be realized within the framework of Nambu's generalized mechanics. Among such systems are the SU(n)-isotropic harmonic oscillator and the SO(4)-Kepler problem. As required by the formulation of Nambu dynamics, the integrals of mo... | 10.402027 | 10.1652 | 10.271574 | 9.001434 | 10.43039 | 9.695247 | 9.781133 | 9.73927 | 9.823558 | 11.113933 | 9.582948 | 9.072707 | 9.671502 | 9.187651 | 9.119112 | 9.080358 | 8.957785 | 9.253784 | 9.189688 | 9.677206 | 9.197432 |
hep-th/9509031 | Leonardo Castellani | Leonardo Castellani and Alberto Perotto | Free Differential Algebras: Their Use in Field Theory and Dual
Formulation | 10 pages, latex, no figures. Talk presented at the 4-th Colloquium on
"Quantum Groups and Integrable Sysytems", Prague, June 1995 | Lett.Math.Phys.38:321-330,1996 | 10.1007/BF00398356 | DFTT-52/95 | hep-th | null | The gauging of free differential algebras (FDA's) produces gauge field
theories containing antisymmetric tensors. The FDA's extend the Cartan-Maurer
equations of ordinary Lie algebras by incorporating p-form potentials ($p >
1$). We study here the algebra of FDA transformations. To every p-form in the
FDA we associat... | [
{
"created": "Thu, 7 Sep 1995 10:45:19 GMT",
"version": "v1"
}
] | 2011-04-15 | [
[
"Castellani",
"Leonardo",
""
],
[
"Perotto",
"Alberto",
""
]
] | The gauging of free differential algebras (FDA's) produces gauge field theories containing antisymmetric tensors. The FDA's extend the Cartan-Maurer equations of ordinary Lie algebras by incorporating p-form potentials ($p > 1$). We study here the algebra of FDA transformations. To every p-form in the FDA we associate ... | 11.924494 | 10.513803 | 12.562489 | 9.808372 | 11.073722 | 11.143711 | 9.813812 | 9.959436 | 9.452671 | 12.541103 | 9.740988 | 10.66815 | 11.050423 | 10.151984 | 10.95459 | 10.090929 | 10.68198 | 10.858011 | 10.175265 | 11.608194 | 10.192291 |
1201.2314 | Renato Nobili | Renato Nobili | The Conformal Universe I: Physical and Mathematical Basis of Conformal
General Relativity | 44, 2 figs | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is the first of three papers on Conformal General Relativity (CGR),
which differs from Einstein's General Relativity (GR) in that it requires
action--integral invariance under local scale transformations in addition to
general coordinate transformations. The theory is here introduced in the
semiclassical approxi... | [
{
"created": "Wed, 11 Jan 2012 14:47:36 GMT",
"version": "v1"
},
{
"created": "Sat, 7 Dec 2013 19:32:51 GMT",
"version": "v2"
},
{
"created": "Mon, 22 Dec 2014 09:52:54 GMT",
"version": "v3"
},
{
"created": "Thu, 24 Mar 2016 01:45:32 GMT",
"version": "v4"
},
{
"cr... | 2016-08-16 | [
[
"Nobili",
"Renato",
""
]
] | This is the first of three papers on Conformal General Relativity (CGR), which differs from Einstein's General Relativity (GR) in that it requires action--integral invariance under local scale transformations in addition to general coordinate transformations. The theory is here introduced in the semiclassical approxima... | 8.463566 | 9.265285 | 8.735826 | 8.602535 | 9.143591 | 9.218549 | 9.369814 | 8.660742 | 8.387747 | 9.332484 | 8.376597 | 8.359352 | 8.245356 | 8.269603 | 8.279516 | 8.320902 | 8.348254 | 8.301914 | 8.397634 | 8.447853 | 8.274817 |
2001.11745 | Clay James Grewcoe | Clay James Grewcoe, Larisa Jonke | Courant sigma model and $L_\infty$-algebras | 34 pages. v2: typos corrected, published version | Fortsch.Phys. 68 (2020) 6, 2000021 | 10.1002/prop.202000021 | RBI-ThPhys-2020-04 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Courant sigma model is a 3-dimensional topological sigma model of AKSZ
type which has been used for the systematic description of closed strings in
non-geometric flux backgrounds. In particular, the expression for the fluxes
and their Bianchi identities coincide with the local form of the axioms of a
Courant alge... | [
{
"created": "Fri, 31 Jan 2020 10:14:01 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Apr 2020 16:12:05 GMT",
"version": "v2"
}
] | 2020-08-28 | [
[
"Grewcoe",
"Clay James",
""
],
[
"Jonke",
"Larisa",
""
]
] | The Courant sigma model is a 3-dimensional topological sigma model of AKSZ type which has been used for the systematic description of closed strings in non-geometric flux backgrounds. In particular, the expression for the fluxes and their Bianchi identities coincide with the local form of the axioms of a Courant algebr... | 5.074041 | 4.446262 | 5.68766 | 4.562857 | 4.910557 | 5.135875 | 4.57857 | 4.598125 | 4.697762 | 6.171383 | 4.539159 | 4.405318 | 5.130466 | 4.640606 | 4.440504 | 4.544253 | 4.505379 | 4.604993 | 4.512301 | 5.237631 | 4.504019 |
1512.04071 | Roberto Casadio | R. Casadio, A. Giugno and O. Micu | Horizon Quantum Mechanics: a hitchhiker's guide to quantum black holes | 45 pages, 26 figures. Review paper to appear in IJMPD | null | 10.1142/S0218271816300068 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is congruous with the quantum nature of the world to view the space-time
geometry as an emergent structure that shows classical features only at some
observational level. One can thus conceive the space-time manifold as a purely
theoretical arena, where quantum states are defined, with the additional
freedom of ch... | [
{
"created": "Sun, 13 Dec 2015 15:57:09 GMT",
"version": "v1"
}
] | 2016-03-16 | [
[
"Casadio",
"R.",
""
],
[
"Giugno",
"A.",
""
],
[
"Micu",
"O.",
""
]
] | It is congruous with the quantum nature of the world to view the space-time geometry as an emergent structure that shows classical features only at some observational level. One can thus conceive the space-time manifold as a purely theoretical arena, where quantum states are defined, with the additional freedom of chan... | 15.028743 | 17.398935 | 15.217698 | 15.16043 | 15.443885 | 16.944902 | 16.610754 | 14.995313 | 15.071296 | 16.023016 | 15.195778 | 14.668783 | 14.778433 | 14.600601 | 14.967881 | 15.063105 | 15.03037 | 14.603296 | 14.83238 | 15.061693 | 14.36561 |
1501.05562 | Carlos Mafra | Carlos R. Mafra, Oliver Schlotterer | A solution to the non-linear equations of D=10 super Yang-Mills theory | 6 pages, v2: published version | Phys. Rev. D 92, 066001 (2015) | 10.1103/PhysRevD.92.066001 | AEI-2015-005, DAMTP-2015-5 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this letter, we present a formal solution to the non-linear field
equations of ten-dimensional super Yang--Mills theory. It is assembled from
products of linearized superfields which have been introduced as multiparticle
superfields in the context of superstring perturbation theory. Their explicit
form follows rec... | [
{
"created": "Thu, 22 Jan 2015 16:31:52 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Sep 2015 20:15:32 GMT",
"version": "v2"
}
] | 2015-09-22 | [
[
"Mafra",
"Carlos R.",
""
],
[
"Schlotterer",
"Oliver",
""
]
] | In this letter, we present a formal solution to the non-linear field equations of ten-dimensional super Yang--Mills theory. It is assembled from products of linearized superfields which have been introduced as multiparticle superfields in the context of superstring perturbation theory. Their explicit form follows recur... | 12.184588 | 10.807058 | 13.989572 | 10.350864 | 9.83634 | 10.622313 | 10.790293 | 10.68829 | 10.739135 | 15.066821 | 10.938951 | 10.495431 | 11.129994 | 10.408743 | 10.394315 | 10.551044 | 10.366025 | 10.117699 | 10.622348 | 11.713265 | 10.779346 |
hep-th/9912223 | Israel Klich | Israel Klich and August Romeo | Regularized Casimir energy for an infinite dielectric cylinder subject
to light-velocity conservation | null | Phys.Lett. B476 (2000) 369-378 | 10.1016/S0370-2693(00)00118-0 | null | hep-th cond-mat.stat-mech quant-ph | null | The Casimir energy of a dilute dielectric cylinder, with the same
light-velocity as in its surrounding medium, is evaluated exactly to first
order in $\xi^2$ and numerically to higher orders in $\xi^2$. The first part is
carried out using addition formulas for Bessel functions, and no Debye
expansions are required.
| [
{
"created": "Wed, 22 Dec 1999 14:58:40 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Klich",
"Israel",
""
],
[
"Romeo",
"August",
""
]
] | The Casimir energy of a dilute dielectric cylinder, with the same light-velocity as in its surrounding medium, is evaluated exactly to first order in $\xi^2$ and numerically to higher orders in $\xi^2$. The first part is carried out using addition formulas for Bessel functions, and no Debye expansions are required. | 12.648767 | 12.166503 | 15.133298 | 10.921484 | 10.389166 | 12.142878 | 12.05501 | 10.425374 | 9.836351 | 15.498055 | 11.266141 | 10.951558 | 12.607388 | 11.163208 | 10.320092 | 10.778174 | 10.556441 | 10.279402 | 10.635911 | 12.182547 | 10.473204 |
1309.4925 | Takashi Miura | Tomo-hiro Abe, Yukihiro Fujimoto, Tatsuo Kobayashi, Takashi Miura,
Kenji Nishiwaki, Makoto Sakamoto | $Z_N$ twisted orbifold models with magnetic flux | 34 pages, 4 figures | JHEP01(2014)065 | 10.1007/JHEP01(2014)065 | KOBE-TH-13-07, KUNS-2463, HRI-P-13-09-001, RECAPP-HRI-2013-019 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose new backgrounds of extra dimensions to lead to four-dimensional
chiral models with three generations of matter fermions, that is $T^2/Z_N$
twisted orbifolds with magnetic fluxes. We consider gauge theory on
six-dimensional space-time, which contains the $T^2/Z_N$ orbifold with magnetic
flux, Scherk-Schwarz... | [
{
"created": "Thu, 19 Sep 2013 10:49:54 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Jan 2014 06:19:16 GMT",
"version": "v2"
}
] | 2014-01-27 | [
[
"Abe",
"Tomo-hiro",
""
],
[
"Fujimoto",
"Yukihiro",
""
],
[
"Kobayashi",
"Tatsuo",
""
],
[
"Miura",
"Takashi",
""
],
[
"Nishiwaki",
"Kenji",
""
],
[
"Sakamoto",
"Makoto",
""
]
] | We propose new backgrounds of extra dimensions to lead to four-dimensional chiral models with three generations of matter fermions, that is $T^2/Z_N$ twisted orbifolds with magnetic fluxes. We consider gauge theory on six-dimensional space-time, which contains the $T^2/Z_N$ orbifold with magnetic flux, Scherk-Schwarz p... | 7.90721 | 7.412704 | 7.669051 | 7.23397 | 7.406341 | 7.4855 | 7.031208 | 7.084411 | 7.123936 | 7.983856 | 7.510003 | 7.417976 | 7.884697 | 7.209123 | 7.250566 | 7.129665 | 7.245365 | 7.405227 | 7.324851 | 7.650584 | 7.278214 |
hep-th/9904141 | Jens Schnittger | J. Rasmussen, J. Schnittger | Negative Screenings in Conformal Field Theory and 2D Gravity: The
Braiding Matrix | 31 pages, LaTeX, 1 figure | Nucl.Phys. B574 (2000) 525-550 | 10.1016/S0550-3213(99)00799-3 | TIFR/TH/99-18 | hep-th | null | We consider an extension of the Coulomb gas picture which is motivated by
Liouville theory and contains negative powers of screening operators on the
same footing as positive ones. The braiding problem for chiral vertex operators
in this extended framework is analyzed. We propose explicit expressions for the
R-matrix... | [
{
"created": "Tue, 20 Apr 1999 20:56:26 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Rasmussen",
"J.",
""
],
[
"Schnittger",
"J.",
""
]
] | We consider an extension of the Coulomb gas picture which is motivated by Liouville theory and contains negative powers of screening operators on the same footing as positive ones. The braiding problem for chiral vertex operators in this extended framework is analyzed. We propose explicit expressions for the R-matrix w... | 12.343016 | 13.617575 | 15.586027 | 12.112207 | 13.035729 | 13.358215 | 13.102313 | 12.976941 | 12.450258 | 14.929791 | 11.580404 | 11.875736 | 13.413949 | 11.73365 | 11.786528 | 11.995257 | 12.341002 | 12.001964 | 11.903454 | 12.982491 | 11.908893 |
2201.03404 | Stuart Dowker | J.S.Dowker | Renyi entropy for monodromy defects of higher derivative free fields on
even-dimensional spheres | 12 pages. 1 fig. Minor errors corrected. Comparison section rewritten
and extended. Acknowledgement and reference added | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Explicit polynomial forms for R\'enyi and entanglement entropies are given on
even --dimensional spheres which possess a codimension--2 U(1) monodromy
defect. Free scalar and Dirac fields are treated and higher-derivative
propagation operators employed. The central charge, $C_T$, is also calculated.
Comparison with e... | [
{
"created": "Mon, 10 Jan 2022 15:36:51 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Jan 2022 15:49:27 GMT",
"version": "v2"
}
] | 2022-01-21 | [
[
"Dowker",
"J. S.",
""
]
] | Explicit polynomial forms for R\'enyi and entanglement entropies are given on even --dimensional spheres which possess a codimension--2 U(1) monodromy defect. Free scalar and Dirac fields are treated and higher-derivative propagation operators employed. The central charge, $C_T$, is also calculated. Comparison with exi... | 21.812336 | 15.276604 | 21.161787 | 14.815327 | 16.323603 | 15.613025 | 15.493578 | 13.534807 | 14.212484 | 23.566957 | 14.444023 | 16.531775 | 18.558928 | 16.623253 | 18.095671 | 16.900162 | 16.528105 | 17.220919 | 17.541372 | 17.969532 | 16.530556 |
1908.10470 | Mary K. Gaillard | Mary K. Gaillard and Jacob Leedom | Anomaly cancellation in effective supergravity from the heterotic string
with an anomalous U(1) | 37 pages. arXiv admin note: text overlap with arXiv:1711.01023 | null | 10.1016/j.nuclphysb.2019.114785 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that a choice of Pauli-Villars regulators allows the cancellation of
all conformal and chiral anomalies in an effective field theory from Z_3
compactification of the heterotic string with two Wilson lines and an anomalous
U(1).
| [
{
"created": "Tue, 27 Aug 2019 21:22:06 GMT",
"version": "v1"
}
] | 2019-10-09 | [
[
"Gaillard",
"Mary K.",
""
],
[
"Leedom",
"Jacob",
""
]
] | We show that a choice of Pauli-Villars regulators allows the cancellation of all conformal and chiral anomalies in an effective field theory from Z_3 compactification of the heterotic string with two Wilson lines and an anomalous U(1). | 11.376709 | 8.702269 | 8.782926 | 7.431612 | 7.462029 | 8.096313 | 8.775061 | 8.036997 | 7.641471 | 9.331556 | 8.343807 | 8.599779 | 8.374798 | 8.779633 | 8.578739 | 8.730456 | 8.506218 | 9.09736 | 8.744941 | 8.949534 | 8.832827 |
2302.06603 | Jordan Cotler | Jordan Cotler, Kristan Jensen | Isometric evolution in de Sitter quantum gravity | 12+8 pages, 4 figures; v2: typos fixed | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study time evolution in two simple models of de Sitter quantum gravity,
Jackiw-Teitelboim gravity and a minisuperspace approximation to Einstein
gravity with a positive cosmological constant. In the former we find that time
evolution is isometric rather than unitary, and find suggestions that this is
true in Einst... | [
{
"created": "Mon, 13 Feb 2023 18:59:01 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Feb 2023 22:36:43 GMT",
"version": "v2"
}
] | 2023-02-20 | [
[
"Cotler",
"Jordan",
""
],
[
"Jensen",
"Kristan",
""
]
] | We study time evolution in two simple models of de Sitter quantum gravity, Jackiw-Teitelboim gravity and a minisuperspace approximation to Einstein gravity with a positive cosmological constant. In the former we find that time evolution is isometric rather than unitary, and find suggestions that this is true in Einstei... | 10.129591 | 8.821012 | 10.322486 | 8.859249 | 9.609373 | 8.732518 | 8.899521 | 9.106445 | 8.540755 | 10.693867 | 8.874825 | 9.282253 | 9.543587 | 9.396879 | 9.394258 | 9.218096 | 9.136136 | 9.356014 | 9.122428 | 9.968427 | 9.259875 |
2405.00776 | Alessandro Tomasiello | Alessandro Tomasiello | Higher spins and Finsler geometry | 36 pages | null | null | null | hep-th gr-qc math-ph math.DG math.MP | http://creativecommons.org/licenses/by/4.0/ | Finsler geometry is a natural generalization of (pseudo-)Riemannian geometry,
where the line element is not the square root of a quadratic form but a more
general homogeneous function. Parameterizing this in terms of symmetric tensors
suggests a possible interpretation in terms of higher-spin fields. We will see
here... | [
{
"created": "Wed, 1 May 2024 18:00:04 GMT",
"version": "v1"
}
] | 2024-05-03 | [
[
"Tomasiello",
"Alessandro",
""
]
] | Finsler geometry is a natural generalization of (pseudo-)Riemannian geometry, where the line element is not the square root of a quadratic form but a more general homogeneous function. Parameterizing this in terms of symmetric tensors suggests a possible interpretation in terms of higher-spin fields. We will see here t... | 11.880211 | 11.800434 | 12.828547 | 10.890398 | 12.652251 | 12.192745 | 11.254988 | 11.846496 | 11.225301 | 13.412273 | 11.192576 | 11.002624 | 10.095595 | 10.368341 | 10.759848 | 10.865467 | 11.177019 | 10.695813 | 10.500423 | 10.627031 | 10.90426 |
hep-th/9808023 | Peter Bantay | Peter Bantay | Orbifoldization, covering surfaces and uniformization theory | 6 pages | Lett.Math.Phys. 57 (2001) 1-5 | null | ITP Budapest 542 | hep-th | null | The connection between the theory of permutation orbifolds, covering surfaces
and uniformization is investigated, and the higher genus partition functions of
an arbitrary permutation orbifold are expressed in terms of those of the
original theory.
| [
{
"created": "Wed, 5 Aug 1998 14:12:08 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bantay",
"Peter",
""
]
] | The connection between the theory of permutation orbifolds, covering surfaces and uniformization is investigated, and the higher genus partition functions of an arbitrary permutation orbifold are expressed in terms of those of the original theory. | 15.31159 | 11.321345 | 15.413074 | 10.209823 | 11.313776 | 10.822598 | 10.404565 | 10.428774 | 10.851761 | 17.672537 | 12.608566 | 11.02374 | 14.964384 | 12.005342 | 11.987636 | 12.046617 | 11.145956 | 11.786207 | 12.458033 | 13.318703 | 11.756598 |
hep-th/0512243 | Jan Pieter van der Schaar | Brian Greene, Maulik Parikh and Jan Pieter van der Schaar | Universal Correction to the Inflationary Vacuum | 23 pages, 3 eps figures, uses JHEP.cls, small corrections and added
references | JHEP0604:057,2006 | 10.1088/1126-6708/2006/04/057 | CU-TP-1136 | hep-th | null | The Bunch-Davies state appears precisely thermal to a free-falling observer
in de Sitter space. However, precise thermality is unphysical because it
violates energy conservation. Instead, the true spectrum must take a certain
different form, with the Boltzmann factor $\exp(-\beta \omega_k)$ replaced by
$\exp(\Delta S... | [
{
"created": "Tue, 20 Dec 2005 20:05:19 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Feb 2006 16:37:37 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Greene",
"Brian",
""
],
[
"Parikh",
"Maulik",
""
],
[
"van der Schaar",
"Jan Pieter",
""
]
] | The Bunch-Davies state appears precisely thermal to a free-falling observer in de Sitter space. However, precise thermality is unphysical because it violates energy conservation. Instead, the true spectrum must take a certain different form, with the Boltzmann factor $\exp(-\beta \omega_k)$ replaced by $\exp(\Delta S)$... | 7.573473 | 7.091179 | 8.606222 | 6.781219 | 7.415161 | 7.379712 | 7.584579 | 7.041675 | 8.079186 | 8.027986 | 7.668542 | 6.828811 | 7.049112 | 6.957914 | 7.022326 | 7.333951 | 7.204225 | 7.044833 | 7.113122 | 7.114439 | 7.062866 |
hep-th/9811156 | Joseph A. Minahan | Joseph A. Minahan (Caltech) | Glueball Mass Spectra and Other Issues for Supergravity Duals of QCD
Models | 19 pages, harvmac(b); v2: minor corrections, reference added | JHEP 9901:020,1999 | 10.1088/1126-6708/1999/01/020 | CALT-68-2203 | hep-th | null | We derive WKB expressions for glueball masses of various finite temperature
supergravity models. The results are very close to recent numerical
computations. We argue that the spectra has some universality that depends only
on the dimension of the AdS space and the singularity structure of the horizon.
This explains ... | [
{
"created": "Mon, 16 Nov 1998 23:43:44 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Dec 1998 19:47:34 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Minahan",
"Joseph A.",
"",
"Caltech"
]
] | We derive WKB expressions for glueball masses of various finite temperature supergravity models. The results are very close to recent numerical computations. We argue that the spectra has some universality that depends only on the dimension of the AdS space and the singularity structure of the horizon. This explains th... | 10.743298 | 11.609423 | 10.864285 | 10.163458 | 11.424095 | 11.043206 | 11.557268 | 11.160635 | 10.590939 | 11.583975 | 10.21523 | 10.493156 | 10.205563 | 10.201099 | 10.38581 | 10.527673 | 10.728724 | 10.553366 | 10.429306 | 10.448869 | 10.266864 |
1304.7978 | Rafael I. Nepomechie | Rafael I. Nepomechie and Chunguang Wang | Algebraic Bethe ansatz for singular solutions | 10 pages; v2: refs added; v3: new section on general singular
solutions, and more references | null | null | UMTG-275 | hep-th math-ph math.MP nlin.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Bethe equations for the isotropic periodic spin-1/2 Heisenberg chain with
N sites have solutions containing i/2, -i/2 that are singular: both the
corresponding energy and the algebraic Bethe ansatz vector are divergent. Such
solutions must be carefully regularized. We consider a regularization involving
a paramet... | [
{
"created": "Tue, 30 Apr 2013 12:52:49 GMT",
"version": "v1"
},
{
"created": "Thu, 2 May 2013 19:57:42 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Jul 2013 13:48:25 GMT",
"version": "v3"
}
] | 2013-07-10 | [
[
"Nepomechie",
"Rafael I.",
""
],
[
"Wang",
"Chunguang",
""
]
] | The Bethe equations for the isotropic periodic spin-1/2 Heisenberg chain with N sites have solutions containing i/2, -i/2 that are singular: both the corresponding energy and the algebraic Bethe ansatz vector are divergent. Such solutions must be carefully regularized. We consider a regularization involving a parameter... | 9.951125 | 11.024831 | 13.582932 | 9.904264 | 10.464034 | 11.362501 | 9.849331 | 9.337127 | 10.247026 | 12.39717 | 9.586499 | 9.434765 | 11.105389 | 9.493604 | 10.030204 | 9.13159 | 9.872263 | 9.702117 | 9.312105 | 11.02396 | 8.931766 |
hep-th/9701119 | Jens Hoppe | J. Froehlich, J. Hoppe (ETH Zuerich) | On Zero-Mass Ground States in Super-Membrane Matrix Models | 16 pp., LaTex | null | 10.1007/s002200050280 | ETH-TH/96-53 | hep-th | null | We recall a formulation of super-membrane theory in terms of certain matrix
models. These models are known to have a mass spectrum given by the positive
half-axis. We show that, for the simplest such matrix model, a normalizable
zero-mass ground state does not exist.
| [
{
"created": "Thu, 23 Jan 1997 16:15:03 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Froehlich",
"J.",
"",
"ETH Zuerich"
],
[
"Hoppe",
"J.",
"",
"ETH Zuerich"
]
] | We recall a formulation of super-membrane theory in terms of certain matrix models. These models are known to have a mass spectrum given by the positive half-axis. We show that, for the simplest such matrix model, a normalizable zero-mass ground state does not exist. | 14.456526 | 11.836041 | 14.260193 | 11.180551 | 11.010076 | 12.248019 | 11.183758 | 9.687158 | 10.725261 | 15.441294 | 11.253116 | 12.249578 | 13.157367 | 12.067233 | 12.163685 | 12.394655 | 12.623425 | 12.170931 | 12.598928 | 14.18698 | 11.647758 |
2206.10547 | Leonardo Pipolo De Gioia | Leonardo Pipolo de Gioia, Ana-Maria Raclariu | Eikonal Approximation in Celestial CFT | 39 pages, 3 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We identify an eikonal regime in celestial CFT$_2$ in which massless 2-2
scattering is dominated by t-channel exchange. We derive a formula for the
celestial amplitude that resums exchanges of arbitrary integer spin to all
orders in the coupling. The resulting eikonal phase takes the same form as in
flat space with t... | [
{
"created": "Tue, 21 Jun 2022 17:26:14 GMT",
"version": "v1"
}
] | 2022-06-22 | [
[
"de Gioia",
"Leonardo Pipolo",
""
],
[
"Raclariu",
"Ana-Maria",
""
]
] | We identify an eikonal regime in celestial CFT$_2$ in which massless 2-2 scattering is dominated by t-channel exchange. We derive a formula for the celestial amplitude that resums exchanges of arbitrary integer spin to all orders in the coupling. The resulting eikonal phase takes the same form as in flat space with the... | 7.896649 | 7.235169 | 8.355841 | 6.842918 | 7.441074 | 6.992251 | 7.376757 | 7.041481 | 6.784989 | 8.482285 | 6.853123 | 7.022418 | 7.287706 | 7.164944 | 7.108729 | 6.896 | 7.318136 | 7.162075 | 7.244856 | 7.449832 | 7.008245 |
hep-th/0403288 | Keshav Dasgupta | Melanie Becker, Keshav Dasgupta, Anke Knauf, Radu Tatar | Geometric Transitions, Flops and Non-Kahler Manifolds: I | Harvmac, 79 pages, 1 .eps figure; v4: Text further expanded with
additional results, typos corrected and references added | Nucl.Phys. B702 (2004) 207-268 | 10.1016/j.nuclphysb.2004.09.020 | SU-ITP-04/10, UCB-PTH-04/09, LBNL-54768, UMD-PP-04/035 | hep-th | null | We construct a duality cycle which provides a complete supergravity
description of geometric transitions in type II theories via a flop in
M-theory. This cycle connects the different supergravity descriptions before
and after the geometric transitions. Our construction reproduces many of the
known phenomena studied e... | [
{
"created": "Tue, 30 Mar 2004 21:20:45 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Apr 2004 05:22:33 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Sep 2004 19:23:04 GMT",
"version": "v3"
},
{
"created": "Fri, 2 Dec 2005 23:29:14 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Becker",
"Melanie",
""
],
[
"Dasgupta",
"Keshav",
""
],
[
"Knauf",
"Anke",
""
],
[
"Tatar",
"Radu",
""
]
] | We construct a duality cycle which provides a complete supergravity description of geometric transitions in type II theories via a flop in M-theory. This cycle connects the different supergravity descriptions before and after the geometric transitions. Our construction reproduces many of the known phenomena studied ear... | 10.229617 | 9.674172 | 12.410359 | 9.494425 | 10.434967 | 9.933798 | 10.282699 | 10.223292 | 9.923192 | 12.95815 | 9.222484 | 9.790456 | 10.465386 | 9.836978 | 9.816405 | 10.294493 | 9.756285 | 9.972329 | 9.882509 | 10.579515 | 9.800863 |
1510.04324 | Arkady Vainshtein | Jin Chen, Xiaoyi Cui, Mikhail Shifman, and Arkady Vainshtein | On Isometry Anomalies in Minimal N=(0,1) and N=(0,2) Sigma Models | 28 pages, 2 figures | null | 10.1142/S0217751X16501475 | FTPI-MINN-14/35, UMN-TH-3406/14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The two-dimensional minimal supersymmetric sigma models with homogeneous
target spaces $G/H$ and chiral fermions of the same chirality are revisited. We
demonstrate that the Moore-Nelson consistency condition revealing a global
anomaly in CP(N-1) (with N>2 and ${\mathcal N}=(0,2)$ supersymmetry) due to a
nontrivial f... | [
{
"created": "Wed, 14 Oct 2015 21:29:11 GMT",
"version": "v1"
}
] | 2016-10-12 | [
[
"Chen",
"Jin",
""
],
[
"Cui",
"Xiaoyi",
""
],
[
"Shifman",
"Mikhail",
""
],
[
"Vainshtein",
"Arkady",
""
]
] | The two-dimensional minimal supersymmetric sigma models with homogeneous target spaces $G/H$ and chiral fermions of the same chirality are revisited. We demonstrate that the Moore-Nelson consistency condition revealing a global anomaly in CP(N-1) (with N>2 and ${\mathcal N}=(0,2)$ supersymmetry) due to a nontrivial fir... | 7.039516 | 7.346126 | 7.522558 | 6.957278 | 7.145822 | 7.496595 | 6.952318 | 7.236108 | 6.963058 | 7.964283 | 6.798328 | 6.693949 | 7.327355 | 6.816455 | 7.0398 | 7.003712 | 6.978997 | 6.658465 | 7.078757 | 6.894055 | 6.767491 |
1205.5679 | Harmen J. Warringa | Harmen J. Warringa | Dynamics of the Chiral Magnetic Effect in a weak magnetic field | 13 pages, 7 figures, revtex | null | 10.1103/PhysRevD.86.085029 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the real-time dynamics of the chiral magnetic effect in
quantum electrodynamics (QED) and quantum chromodynamics (QCD). We consider a
field configuration of parallel (chromo)electric and (chromo)magnetic fields
with a weak perpendicular electromagnetic magnetic field. The chiral magnetic
effect induces... | [
{
"created": "Fri, 25 May 2012 12:36:22 GMT",
"version": "v1"
}
] | 2015-03-20 | [
[
"Warringa",
"Harmen J.",
""
]
] | We investigate the real-time dynamics of the chiral magnetic effect in quantum electrodynamics (QED) and quantum chromodynamics (QCD). We consider a field configuration of parallel (chromo)electric and (chromo)magnetic fields with a weak perpendicular electromagnetic magnetic field. The chiral magnetic effect induces a... | 7.371739 | 7.511495 | 6.451261 | 6.855589 | 7.406344 | 7.542278 | 8.093383 | 7.456471 | 6.731692 | 7.141613 | 7.074144 | 7.272222 | 7.022026 | 7.141615 | 7.236637 | 7.261992 | 7.167199 | 7.429187 | 7.060953 | 7.013391 | 7.191994 |
1706.06104 | Kazuya Yonekura | Hiroyuki Shimizu and Kazuya Yonekura | Anomaly constraints on deconfinement and chiral phase transition | 6 pages, references added; v3:references added and minor change | Phys. Rev. D 97, 105011 (2018) | 10.1103/PhysRevD.97.105011 | IPMU 17-0082 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study constraints on thermal phase transitions of ${\rm SU}(N_c)$ gauge
theories by using the 't Hooft anomaly involving the center symmetry and chiral
symmetry. We consider two cases of massless fermions: (i) adjoint fermions, and
(ii) $N_f$ flavors of fundamental fermions with a nontrivial greatest common
diviso... | [
{
"created": "Mon, 19 Jun 2017 18:00:03 GMT",
"version": "v1"
},
{
"created": "Thu, 6 Jul 2017 11:38:01 GMT",
"version": "v2"
},
{
"created": "Thu, 24 May 2018 04:04:57 GMT",
"version": "v3"
}
] | 2018-05-25 | [
[
"Shimizu",
"Hiroyuki",
""
],
[
"Yonekura",
"Kazuya",
""
]
] | We study constraints on thermal phase transitions of ${\rm SU}(N_c)$ gauge theories by using the 't Hooft anomaly involving the center symmetry and chiral symmetry. We consider two cases of massless fermions: (i) adjoint fermions, and (ii) $N_f$ flavors of fundamental fermions with a nontrivial greatest common divisor ... | 5.496012 | 5.376914 | 6.233398 | 5.566802 | 5.525843 | 5.52063 | 5.493694 | 5.389454 | 5.875033 | 6.553513 | 5.549438 | 5.314683 | 5.697129 | 5.444469 | 5.435096 | 5.526886 | 5.542791 | 5.387497 | 5.513211 | 5.645439 | 5.391346 |
1701.00764 | Amir-Kian Kashani-Poor | Jie Gu, Min-xin Huang, Amir-Kian Kashani-Poor, Albrecht Klemm | Refined BPS invariants of 6d SCFTs from anomalies and modularity | 64 pages; v2: typos corrected | null | 10.1007/JHEP05(2017)130 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | F-theory compactifications on appropriate local elliptic Calabi-Yau manifolds
engineer six dimensional superconformal field theories and their mass
deformations. The partition function $Z_{top}$ of the refined topological
string on these geometries captures the particle BPS spectrum of this class of
theories compacti... | [
{
"created": "Tue, 3 Jan 2017 18:10:42 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Feb 2018 13:19:05 GMT",
"version": "v2"
}
] | 2018-02-14 | [
[
"Gu",
"Jie",
""
],
[
"Huang",
"Min-xin",
""
],
[
"Kashani-Poor",
"Amir-Kian",
""
],
[
"Klemm",
"Albrecht",
""
]
] | F-theory compactifications on appropriate local elliptic Calabi-Yau manifolds engineer six dimensional superconformal field theories and their mass deformations. The partition function $Z_{top}$ of the refined topological string on these geometries captures the particle BPS spectrum of this class of theories compactifi... | 8.650197 | 8.810711 | 10.18778 | 8.519361 | 9.113863 | 8.971252 | 9.143986 | 8.763488 | 8.846587 | 12.400162 | 8.596842 | 8.489699 | 8.884721 | 8.268042 | 8.496067 | 8.626618 | 8.43755 | 8.399822 | 8.440618 | 9.060143 | 8.376569 |
2211.11198 | Michael P. Kinach | Michael P. Kinach, Matthew W. Choptuik | Dynamical evolution of $U(1)$ gauged Q-balls in axisymmetry | 16 pages, 14 figures; v2: updated to reflect minor changes in
published version | Phys. Rev. D 107, 035022 (2023) | 10.1103/PhysRevD.107.035022 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the dynamics of $U(1)$ gauged Q-balls using fully non-linear
numerical evolutions in axisymmetry. Focusing on two models with logarithmic
and polynomial scalar field potentials, we numerically evolve perturbed gauged
Q-ball configurations in order to assess their stability and determine the fate
of unstable ... | [
{
"created": "Mon, 21 Nov 2022 06:14:42 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Mar 2023 21:43:45 GMT",
"version": "v2"
}
] | 2023-04-04 | [
[
"Kinach",
"Michael P.",
""
],
[
"Choptuik",
"Matthew W.",
""
]
] | We study the dynamics of $U(1)$ gauged Q-balls using fully non-linear numerical evolutions in axisymmetry. Focusing on two models with logarithmic and polynomial scalar field potentials, we numerically evolve perturbed gauged Q-ball configurations in order to assess their stability and determine the fate of unstable co... | 5.756191 | 5.372792 | 5.618547 | 4.981833 | 5.468404 | 5.064724 | 5.565047 | 5.138626 | 5.305423 | 5.94065 | 5.326644 | 5.702613 | 5.923563 | 5.600734 | 5.510549 | 5.434689 | 5.562418 | 5.40483 | 5.685859 | 5.849357 | 5.629613 |
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