id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1006.4132 | Stanislaw D. Glazek | Stanislaw D. Glazek | Non-local structure of renormalized Hamiltonian densities on the
light-front hyperplane in space-time | latex, 41 pages, 5 figures | Acta Phys.Polon.B41:1937-1976,2010 | null | IFT/10/05 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | When canonical Hamiltonians of local quantum field theories are transformed
using a renormalization group procedure for effective particles, the resulting
interaction terms are non-local. The range of their non-locality depends on the
arbitrary parameter of scale, which characterizes the size of effective
particles i... | [
{
"created": "Mon, 21 Jun 2010 18:05:16 GMT",
"version": "v1"
}
] | 2014-11-21 | [
[
"Glazek",
"Stanislaw D.",
""
]
] | When canonical Hamiltonians of local quantum field theories are transformed using a renormalization group procedure for effective particles, the resulting interaction terms are non-local. The range of their non-locality depends on the arbitrary parameter of scale, which characterizes the size of effective particles in ... | 16.491144 | 13.358572 | 17.403147 | 14.250813 | 16.345661 | 14.356549 | 14.832575 | 14.2844 | 13.86285 | 15.379542 | 14.385832 | 14.422983 | 15.206212 | 14.190414 | 14.717402 | 14.662951 | 14.967039 | 14.617094 | 14.308386 | 15.604872 | 14.798699 |
1710.05125 | Hirohumi Sawayanagi | Hirohumi Sawayanagi | Condensate $\langle A_{\mu}^+A_{\mu}^-\rangle$ and massive magnetic
potential in Euclidean gauge theories | To appear in Progress of Theoretical and Experimental Physics | Prog Theor Exp Phys (2017) | 10.1093/ptep/ptx149 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Euclidean $SU(2)$ gauge theory is studied in a nonlinear gauge. In this
theory, ghost condensation happens and gauge fields acquire tachyonic masses.
It is shown that these tachyonic masses are removed by a gauge field condensate
$\langle A_{\mu}^+A_{\mu}^-\rangle$. Because of the ghost condensation,
monopole solutio... | [
{
"created": "Sat, 14 Oct 2017 02:31:19 GMT",
"version": "v1"
}
] | 2019-12-06 | [
[
"Sawayanagi",
"Hirohumi",
""
]
] | Euclidean $SU(2)$ gauge theory is studied in a nonlinear gauge. In this theory, ghost condensation happens and gauge fields acquire tachyonic masses. It is shown that these tachyonic masses are removed by a gauge field condensate $\langle A_{\mu}^+A_{\mu}^-\rangle$. Because of the ghost condensation, monopole solutions... | 6.658909 | 6.145182 | 6.089973 | 5.822692 | 6.895504 | 6.128248 | 5.863379 | 6.360765 | 5.748124 | 7.452065 | 6.137943 | 5.900735 | 6.218429 | 6.117041 | 6.150298 | 6.052043 | 6.100437 | 6.147779 | 6.22737 | 6.168954 | 6.136783 |
1705.06482 | Gao-Liang Zhou | Gao-Liang Zhou, Zheng-Xin Yan and Xin Zhang | Equivalence Between the Gauge $n\cdot\partial n\cdot A=0$ and the Axial
Gauge | 5pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Discontinuity of gauge theory in the gauge condition $n\cdot\partial n\cdot
A=0$, which emerges at $n\cdot k=0$, is studied here. Such discontinuity is
different from that one confronts in axial gauge and can not be regularized by
conventional analytical continuation method. The Faddeev-Popov determinate of
the gauge... | [
{
"created": "Thu, 18 May 2017 09:05:28 GMT",
"version": "v1"
}
] | 2017-05-19 | [
[
"Zhou",
"Gao-Liang",
""
],
[
"Yan",
"Zheng-Xin",
""
],
[
"Zhang",
"Xin",
""
]
] | Discontinuity of gauge theory in the gauge condition $n\cdot\partial n\cdot A=0$, which emerges at $n\cdot k=0$, is studied here. Such discontinuity is different from that one confronts in axial gauge and can not be regularized by conventional analytical continuation method. The Faddeev-Popov determinate of the gauge $... | 9.60201 | 10.327523 | 9.903889 | 9.039021 | 9.946371 | 10.330224 | 10.76171 | 10.060551 | 9.565154 | 10.359834 | 9.836753 | 9.347167 | 9.379369 | 9.409438 | 9.647205 | 9.206548 | 9.290999 | 9.315145 | 9.36228 | 9.450361 | 9.210502 |
1506.02450 | Asuka Ito | Asuka Ito, Jiro Soda | Designing Anisotropic Inflation with Form Fields | 27 pages, 8 figures | Phys. Rev. D 92, 123533 (2015) | 10.1103/PhysRevD.92.123533 | KOBE-TH-15-05 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study inflation with anisotropic hair induced by form fields. In four
dimensions, the relevant form fields are gauge (one-form) fields and two-form
fields. Assuming the exponential form of potential and gauge kinetic functions,
we find new exact power-law solutions endowed with anisotropic hair. We also
explore th... | [
{
"created": "Mon, 8 Jun 2015 11:43:33 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Jan 2016 05:58:13 GMT",
"version": "v2"
}
] | 2016-01-11 | [
[
"Ito",
"Asuka",
""
],
[
"Soda",
"Jiro",
""
]
] | We study inflation with anisotropic hair induced by form fields. In four dimensions, the relevant form fields are gauge (one-form) fields and two-form fields. Assuming the exponential form of potential and gauge kinetic functions, we find new exact power-law solutions endowed with anisotropic hair. We also explore the ... | 7.918046 | 8.053865 | 8.053013 | 7.698294 | 7.87721 | 8.281555 | 8.098879 | 7.613219 | 7.778463 | 8.321253 | 7.344442 | 7.795013 | 7.589126 | 7.618254 | 7.631914 | 7.752386 | 7.72955 | 7.796043 | 7.541984 | 7.687945 | 7.736438 |
1210.0966 | Miao Rongxin | Miao Li and Rong-Xin Miao | A New Model of Holographic Dark Energy with Action Principle | 11 pages, no figures, typo corrected, English improved | null | null | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new model of holographic dark energy with an action. It is the
first time that one can derive a HDE model from the action principle. The
puzzles of causality and circular logic about HDE have been completely solved
in this model. The evolution of the universe only depends on the present state
of the univ... | [
{
"created": "Wed, 3 Oct 2012 02:52:58 GMT",
"version": "v1"
},
{
"created": "Sun, 7 Oct 2012 01:15:37 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Nov 2012 14:48:07 GMT",
"version": "v3"
}
] | 2012-11-26 | [
[
"Li",
"Miao",
""
],
[
"Miao",
"Rong-Xin",
""
]
] | We propose a new model of holographic dark energy with an action. It is the first time that one can derive a HDE model from the action principle. The puzzles of causality and circular logic about HDE have been completely solved in this model. The evolution of the universe only depends on the present state of the univer... | 13.636997 | 14.015577 | 13.50855 | 12.114232 | 12.142938 | 13.071905 | 12.787478 | 11.154886 | 12.794017 | 13.662656 | 11.977185 | 12.91097 | 12.968516 | 12.735909 | 13.10962 | 13.025669 | 12.766027 | 12.514814 | 13.104652 | 12.831472 | 13.057195 |
1902.11286 | Marcus Spradlin | John Golden, Andrew J. McLeod, Marcus Spradlin, Anastasia Volovich | The Sklyanin Bracket and Cluster Adjacency at All Multiplicity | 25 pages; v2: added reference | null | 10.1007/JHEP03(2019)195 | LCTP-19-03 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that the Sklyanin Poisson bracket on Gr(4,n) can be used to
efficiently test whether an amplitude in planar ${\cal{N}}=4$ supersymmetric
Yang-Mills theory satisfies cluster adjacency. We use this test to show that
cluster adjacency is satisfied by all one- and two-loop MHV amplitudes in this
theory, once sui... | [
{
"created": "Thu, 28 Feb 2019 18:43:21 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Mar 2019 17:24:11 GMT",
"version": "v2"
}
] | 2019-05-01 | [
[
"Golden",
"John",
""
],
[
"McLeod",
"Andrew J.",
""
],
[
"Spradlin",
"Marcus",
""
],
[
"Volovich",
"Anastasia",
""
]
] | We argue that the Sklyanin Poisson bracket on Gr(4,n) can be used to efficiently test whether an amplitude in planar ${\cal{N}}=4$ supersymmetric Yang-Mills theory satisfies cluster adjacency. We use this test to show that cluster adjacency is satisfied by all one- and two-loop MHV amplitudes in this theory, once suita... | 9.569105 | 9.684319 | 12.836717 | 8.722868 | 9.702309 | 9.302571 | 9.53536 | 9.054584 | 7.928852 | 12.860629 | 8.118472 | 9.404677 | 10.416834 | 9.112617 | 9.680124 | 9.511088 | 9.035893 | 9.314084 | 9.16128 | 10.173544 | 9.170261 |
1203.2182 | Piotr Sulkowski | Hiroyuki Fuji, Sergei Gukov, Piotr Su{\l}kowski | Volume Conjecture: Refined and Categorified | with an appendix by Hidetoshi Awata; 92 pages, 24 figures | Adv. Theor. Math. Phys. 16, 6 (2012) 1669-1777 | 10.4310/ATMP.2012.v16.n6.a3 | CALT-68-2866 | hep-th math.AG math.GT math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The generalized volume conjecture relates asymptotic behavior of the colored
Jones polynomials to objects naturally defined on an algebraic curve, the zero
locus of the A-polynomial $A(x,y)$. Another "family version" of the volume
conjecture depends on a quantization parameter, usually denoted $q$ or $\hbar$;
this qu... | [
{
"created": "Fri, 9 Mar 2012 21:00:05 GMT",
"version": "v1"
}
] | 2017-05-23 | [
[
"Fuji",
"Hiroyuki",
""
],
[
"Gukov",
"Sergei",
""
],
[
"Sułkowski",
"Piotr",
""
]
] | The generalized volume conjecture relates asymptotic behavior of the colored Jones polynomials to objects naturally defined on an algebraic curve, the zero locus of the A-polynomial $A(x,y)$. Another "family version" of the volume conjecture depends on a quantization parameter, usually denoted $q$ or $\hbar$; this quan... | 7.532026 | 9.024909 | 9.548245 | 8.226439 | 8.498861 | 8.72675 | 9.717058 | 8.574963 | 8.062813 | 9.874043 | 8.323686 | 7.694222 | 7.860844 | 7.846463 | 7.573865 | 7.758751 | 7.653604 | 7.468287 | 7.892651 | 8.274559 | 7.530159 |
1502.08044 | Yanyan Bu | Yanyan Bu and Michael Lublinsky | Linearly resummed hydrodynamics in a weakly curved spacetime | 24 pages + appendices, 1 table, 6 muti-figures | null | 10.1007/JHEP04(2015)136 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend our study of all-order linearly resummed hydrodynamics in a flat
space~\cite{1406.7222,1409.3095} to fluids in weakly curved spaces. The
underlying microscopic theory is a finite temperature $\mathcal{N}=4$
super-Yang-Mills theory at strong coupling. The AdS/CFT correspondence relates
black brane solutions ... | [
{
"created": "Fri, 27 Feb 2015 20:24:01 GMT",
"version": "v1"
}
] | 2015-05-20 | [
[
"Bu",
"Yanyan",
""
],
[
"Lublinsky",
"Michael",
""
]
] | We extend our study of all-order linearly resummed hydrodynamics in a flat space~\cite{1406.7222,1409.3095} to fluids in weakly curved spaces. The underlying microscopic theory is a finite temperature $\mathcal{N}=4$ super-Yang-Mills theory at strong coupling. The AdS/CFT correspondence relates black brane solutions of... | 7.31896 | 7.69566 | 8.398036 | 7.45684 | 7.942876 | 8.040195 | 7.487017 | 7.475081 | 7.4306 | 8.645449 | 7.546739 | 7.164409 | 7.522872 | 7.195788 | 7.165236 | 7.50198 | 7.112279 | 7.291231 | 7.207641 | 7.478754 | 7.118805 |
2203.12636 | Matteo Morittu | Gianguido Dall'Agata, Maxim Emelin, Fotis Farakos, Matteo Morittu | Anti-brane uplift instability from goldstino condensation | 40 pages, 6 plots. v2: references added and minor clarifications | null | 10.1007/JHEP08(2022)005 | null | hep-th cond-mat.stat-mech hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the possible appearance of composite states of the goldstino
in models with four-dimensional non-linear supersymmetry and we provide a
description of their dynamics in terms of a K\"ahler potential and a
superpotential. Our analysis shows that the critical point corresponding to the
Volkov-Akulov model... | [
{
"created": "Wed, 23 Mar 2022 18:00:08 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Apr 2022 09:20:08 GMT",
"version": "v2"
}
] | 2022-08-24 | [
[
"Dall'Agata",
"Gianguido",
""
],
[
"Emelin",
"Maxim",
""
],
[
"Farakos",
"Fotis",
""
],
[
"Morittu",
"Matteo",
""
]
] | We investigate the possible appearance of composite states of the goldstino in models with four-dimensional non-linear supersymmetry and we provide a description of their dynamics in terms of a K\"ahler potential and a superpotential. Our analysis shows that the critical point corresponding to the Volkov-Akulov model i... | 11.183755 | 10.175285 | 11.205639 | 9.522302 | 10.161273 | 10.710624 | 9.794671 | 10.081483 | 9.451213 | 10.515069 | 10.172023 | 10.414773 | 10.78501 | 10.455415 | 9.884548 | 10.473768 | 10.094728 | 10.137433 | 10.607803 | 10.951435 | 10.371202 |
1712.09955 | Jia-Hui Huang | Jia-Hui Huang | Group constraint relations for five-point amplitudes in gauge theories
with SO(N) and Sp(2N) groups | 20 pages, reference added, typo corrected | null | 10.1016/j.nuclphysb.2021.115370 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper,linear constraint relations among loop-order five-point
color-ordered amplitudes in $SO(N)$ and $Sp(2N)$ gauge theories are derived
with the group-theoretic method. These constrains are derived up to four-loop
order. It is found that in both theories, there are $n=6,22,34,44,50$ linear
constraint relati... | [
{
"created": "Thu, 28 Dec 2017 18:00:58 GMT",
"version": "v1"
},
{
"created": "Sun, 31 Dec 2017 14:57:15 GMT",
"version": "v2"
}
] | 2021-03-15 | [
[
"Huang",
"Jia-Hui",
""
]
] | In this paper,linear constraint relations among loop-order five-point color-ordered amplitudes in $SO(N)$ and $Sp(2N)$ gauge theories are derived with the group-theoretic method. These constrains are derived up to four-loop order. It is found that in both theories, there are $n=6,22,34,44,50$ linear constraint relation... | 7.310919 | 6.927806 | 6.2309 | 6.71293 | 7.930523 | 6.772083 | 6.025398 | 6.268908 | 6.361466 | 7.145803 | 7.332929 | 6.165264 | 6.347407 | 6.371987 | 6.295741 | 6.347637 | 6.269537 | 6.241597 | 6.044298 | 6.325574 | 6.432052 |
2012.12343 | Ishmael Takyi | I. Takyi, B. Barnes, J. Ackora-Prah | Vacuum Polarization Energy of the Kinks in the Sinh-Deformed Models | 12 pages, 8 figures, 4 tables | Turk J Phys, 45, (2021), 194-206 | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the one-loop quantum corrections to the kink energies of the
sinh-deformed $\phi^{4}$ and $\varphi^{6}$ models in one space and one time
dimensions. These models are constructed from the well-known polynomial
$\phi^{4}$ and $\varphi^{6}$ models by a deformation procedure. We also compute
the vacuum polariz... | [
{
"created": "Tue, 22 Dec 2020 20:33:12 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Sep 2021 14:35:01 GMT",
"version": "v2"
}
] | 2021-09-08 | [
[
"Takyi",
"I.",
""
],
[
"Barnes",
"B.",
""
],
[
"Ackora-Prah",
"J.",
""
]
] | We compute the one-loop quantum corrections to the kink energies of the sinh-deformed $\phi^{4}$ and $\varphi^{6}$ models in one space and one time dimensions. These models are constructed from the well-known polynomial $\phi^{4}$ and $\varphi^{6}$ models by a deformation procedure. We also compute the vacuum polarizat... | 5.308273 | 5.19102 | 6.777555 | 5.437292 | 6.263592 | 5.495028 | 5.376503 | 5.857393 | 5.521657 | 6.271172 | 5.400069 | 5.370422 | 6.011584 | 5.304938 | 5.713735 | 5.40503 | 5.341711 | 5.591727 | 5.328297 | 5.595669 | 5.330171 |
1906.08252 | Valentina Giangreco M. Puletti | J. Angel-Ramelli, V. Giangreco M. Puletti, L. Thorlacius | Entanglement Entropy in Generalised Quantum Lifshitz Models | 60 pages (including appendices), 5 figures; v2: references added,
presentation improved, conclusions unchanged, v3: matching published version | null | 10.1007/JHEP08(2019)072 | null | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute universal finite corrections to entanglement entropy for
generalised quantum Lifshitz models in arbitrary odd spacetime dimensions.
These are generalised free field theories with Lifshitz scaling symmetry, where
the dynamical critical exponent $z$ equals the number of spatial dimensions
$d$, and which gene... | [
{
"created": "Wed, 19 Jun 2019 17:51:53 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Jun 2019 17:51:52 GMT",
"version": "v2"
},
{
"created": "Tue, 13 Aug 2019 16:31:59 GMT",
"version": "v3"
}
] | 2019-09-04 | [
[
"Angel-Ramelli",
"J.",
""
],
[
"Puletti",
"V. Giangreco M.",
""
],
[
"Thorlacius",
"L.",
""
]
] | We compute universal finite corrections to entanglement entropy for generalised quantum Lifshitz models in arbitrary odd spacetime dimensions. These are generalised free field theories with Lifshitz scaling symmetry, where the dynamical critical exponent $z$ equals the number of spatial dimensions $d$, and which genera... | 5.60976 | 5.938643 | 5.599249 | 5.682466 | 5.510217 | 5.742349 | 5.795322 | 5.950761 | 5.582374 | 5.991327 | 5.844346 | 5.417907 | 5.765113 | 5.456928 | 5.706544 | 5.535757 | 5.710106 | 5.527874 | 5.458613 | 5.490574 | 5.498918 |
2106.12780 | Omer Faruk Dayi | \"O.F.Dayi and E. Kilin\c{c}arslan | Quantum Kinetic Equation for Fluids of Spin-1/2 Fermions | Comments and refs added. Published version | JHEP11(2021)086 | 10.1007/JHEP11(2021)086 | null | hep-th hep-ph math.AP | http://creativecommons.org/licenses/by/4.0/ | Fluid of spin-1/2 fermions is represented by a complex scalar field and a
four-vector field coupled both to the scalar and the Dirac fields. We present
the underlying action and show that the resulting equations of motion are
identical to the (hydrodynamic) Euler equations in the presence of Coriolis
force. As a cons... | [
{
"created": "Thu, 24 Jun 2021 06:11:29 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Sep 2021 11:24:43 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Nov 2021 13:39:33 GMT",
"version": "v3"
}
] | 2021-11-16 | [
[
"Dayi",
"Ö. F.",
""
],
[
"Kilinçarslan",
"E.",
""
]
] | Fluid of spin-1/2 fermions is represented by a complex scalar field and a four-vector field coupled both to the scalar and the Dirac fields. We present the underlying action and show that the resulting equations of motion are identical to the (hydrodynamic) Euler equations in the presence of Coriolis force. As a conseq... | 11.751433 | 11.681929 | 11.502478 | 11.099239 | 12.150679 | 12.201737 | 12.203137 | 11.109008 | 11.537122 | 12.399866 | 11.138638 | 11.197725 | 11.005442 | 11.000772 | 11.10398 | 11.186227 | 11.523731 | 11.107347 | 10.675337 | 11.668176 | 11.279743 |
2010.08498 | Hasmik Poghosyan Mrs | Hasmik Poghosyan | Recursion relation for instanton counting for $SU(2)$ ${\cal N}=2$ SYM
in NS limit of $\Omega$ background | 28 pages, 6 figures, some clarifications and citations added,
published version | null | 10.1007/JHEP05(2021)088 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate different ways of deriving the A-cycle period as
a series in instanton counting parameter $q$ for ${\cal N}=2$ SYM with up to
four antifundamental hypermultiplets in NS limit of $\Omega$ background. We
propose a new method for calculating the period and demonstrate its efficiency
by expli... | [
{
"created": "Fri, 16 Oct 2020 16:55:21 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Oct 2020 09:11:06 GMT",
"version": "v2"
},
{
"created": "Wed, 19 May 2021 05:29:54 GMT",
"version": "v3"
}
] | 2021-06-02 | [
[
"Poghosyan",
"Hasmik",
""
]
] | In this paper we investigate different ways of deriving the A-cycle period as a series in instanton counting parameter $q$ for ${\cal N}=2$ SYM with up to four antifundamental hypermultiplets in NS limit of $\Omega$ background. We propose a new method for calculating the period and demonstrate its efficiency by explici... | 12.093901 | 11.904155 | 12.326882 | 11.3361 | 11.682182 | 11.907712 | 11.971598 | 11.322593 | 11.020532 | 13.19027 | 10.986306 | 10.585288 | 11.036994 | 10.267061 | 10.723279 | 10.52147 | 10.588047 | 10.620335 | 10.486429 | 10.882059 | 10.236514 |
hep-th/0008169 | I. L. Buchbinder | I.L. Buchbinder | Low-Energy Effective Action in N=4 Super Yang-Mills Theories | 9 pages, LaTeX, Talk given at the Conference "Quantization, Gauge
Theory, and Strings" dedicated to the memory of Professor Efim Fradkin, June
5-10, 2000, Moscow, to be published in the Proceedings | null | null | null | hep-th | null | We review a recent progress in constructing low-energy effective action in
N=4 super Yang-Mills theories. Using harmonic superspace approach we consider
N=4 SYM in terms of unconstrained N=2 superfield and apply N=2 background field
method to finding effective action for N=4 SU(n) SYM broken down to
U(n)$^{n-1}$. Gen... | [
{
"created": "Tue, 22 Aug 2000 11:06:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Buchbinder",
"I. L.",
""
]
] | We review a recent progress in constructing low-energy effective action in N=4 super Yang-Mills theories. Using harmonic superspace approach we consider N=4 SYM in terms of unconstrained N=2 superfield and apply N=2 background field method to finding effective action for N=4 SU(n) SYM broken down to U(n)$^{n-1}$. Gener... | 9.912622 | 5.818182 | 9.298061 | 6.678957 | 7.80377 | 7.818458 | 7.945285 | 6.462173 | 6.798323 | 10.810104 | 6.826264 | 8.072131 | 8.723349 | 8.017037 | 8.737246 | 8.649388 | 8.336765 | 7.842027 | 8.069466 | 9.00895 | 7.918171 |
hep-th/9901021 | Edward Witten | C. Robin Graham and Edward Witten | Conformal Anomaly Of Submanifold Observables In AdS/CFT Correspondence | 11 pp | Nucl.Phys.B546:52-64,1999 | 10.1016/S0550-3213(99)00055-3 | null | hep-th | null | We analyze the conformal invariance of submanifold observables associated
with $k$-branes in the AdS/CFT correspondence. For odd $k$, the resulting
observables are conformally invariant, and for even $k$, they transform with a
conformal anomaly that is given by a local expression which we analyze in
detail for $k=2$
| [
{
"created": "Wed, 6 Jan 1999 13:12:40 GMT",
"version": "v1"
}
] | 2010-04-07 | [
[
"Graham",
"C. Robin",
""
],
[
"Witten",
"Edward",
""
]
] | We analyze the conformal invariance of submanifold observables associated with $k$-branes in the AdS/CFT correspondence. For odd $k$, the resulting observables are conformally invariant, and for even $k$, they transform with a conformal anomaly that is given by a local expression which we analyze in detail for $k=2$ | 6.083036 | 5.566742 | 6.513128 | 6.060339 | 5.323158 | 5.298091 | 5.529905 | 5.529855 | 5.517145 | 6.659738 | 5.392045 | 5.798735 | 6.404627 | 5.785528 | 5.290045 | 5.678901 | 5.584888 | 5.811069 | 5.75933 | 6.604225 | 5.531951 |
hep-th/0312309 | Axel Krause | Axel Krause (Maryland U.) | On the Bekenstein-Hawking Entropy, Non-Commutative Branes and
Logarithmic Corrections | 17 pages, 2 figures; refs. added | Int.J.Mod.Phys.A21:4449-4461,2006 | 10.1142/S0217751X06033878 | UMD-PP-04-014 | hep-th | null | We extend earlier work on the origin of the Bekenstein-Hawking entropy to
higher-dimensional spacetimes. The mechanism of counting states is shown to
work for all spacetimes associated with a Euclidean doublet
$(E_1,M_1)+(E_2,M_2)$ of electric-magnetic dual brane pairs of type II
string-theory or M-theory wrapping th... | [
{
"created": "Tue, 30 Dec 2003 17:05:35 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 2004 22:47:28 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Jun 2006 22:01:51 GMT",
"version": "v3"
}
] | 2011-07-19 | [
[
"Krause",
"Axel",
"",
"Maryland U."
]
] | We extend earlier work on the origin of the Bekenstein-Hawking entropy to higher-dimensional spacetimes. The mechanism of counting states is shown to work for all spacetimes associated with a Euclidean doublet $(E_1,M_1)+(E_2,M_2)$ of electric-magnetic dual brane pairs of type II string-theory or M-theory wrapping the ... | 12.266746 | 12.454415 | 12.399402 | 10.97832 | 10.941434 | 12.023765 | 12.237902 | 10.562117 | 11.510982 | 12.187 | 10.379134 | 11.078248 | 11.409778 | 10.711287 | 10.392479 | 11.291275 | 11.173212 | 11.024554 | 11.252666 | 11.527536 | 11.103246 |
hep-th/0107104 | Amitabha Lahiri | Amitabha Lahiri (Bose Ctr., Kolkata) | Gauge transformations of the non-Abelian two-form | ReVTeX3.1, 4 pages | Mod.Phys.Lett. A17 (2002) 1643-1650 | 10.1142/S0217732302007752 | null | hep-th | null | A novel inhomogeneous gauge transformation law is proposed for a non-Abelian
adjoint two-form in four dimensions. Rules for constructing actions invariant
under this are given. The auxiliary vector field which appears in some of these
models transforms like a second connection in the theory. Another local
symmetry le... | [
{
"created": "Thu, 12 Jul 2001 13:52:42 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Lahiri",
"Amitabha",
"",
"Bose Ctr., Kolkata"
]
] | A novel inhomogeneous gauge transformation law is proposed for a non-Abelian adjoint two-form in four dimensions. Rules for constructing actions invariant under this are given. The auxiliary vector field which appears in some of these models transforms like a second connection in the theory. Another local symmetry leav... | 18.830475 | 16.073563 | 20.858955 | 18.224327 | 19.716373 | 14.970212 | 18.696224 | 19.316063 | 16.323175 | 25.157421 | 17.425983 | 16.814859 | 19.454582 | 17.78948 | 17.889414 | 16.711475 | 16.604338 | 17.114254 | 17.049337 | 19.369484 | 16.70063 |
hep-th/0103174 | Masato Arai | Masato Arai and Nobuchika Okada | Potential analysis of N=2 SUSY gauge theory with the Fayet-Iliopoulos
term | 8 pages, Latex. Contribution to the proceedings of the D.V.Volkov's
memorial conference ``Supersymmetry and Quantum Field Theory'', Kharkov, July
25-29,2000, to be published in Nuclear Physics B Conference Supplements | Nucl.Phys.Proc.Suppl.102:219-226,2001 | 10.1016/S0920-5632(01)01559-6 | KEK-TH-751 | hep-th | null | We analyze the vacuum structure of spontaneously broken N=2 supersymmetric
gauge theory with the Fayet-Iliopoulos term. Our theory is based on the gauge
group SU(2) \times U(1) with N_f=2 massless quark hypermultiplets having the
same U(1) charges. In the classical potential, there are degenerate vacua even
in the ab... | [
{
"created": "Wed, 21 Mar 2001 05:11:37 GMT",
"version": "v1"
}
] | 2011-08-11 | [
[
"Arai",
"Masato",
""
],
[
"Okada",
"Nobuchika",
""
]
] | We analyze the vacuum structure of spontaneously broken N=2 supersymmetric gauge theory with the Fayet-Iliopoulos term. Our theory is based on the gauge group SU(2) \times U(1) with N_f=2 massless quark hypermultiplets having the same U(1) charges. In the classical potential, there are degenerate vacua even in the abse... | 6.935524 | 4.827644 | 6.687212 | 5.654476 | 5.055717 | 4.888954 | 4.865129 | 5.003255 | 5.467045 | 7.087266 | 5.336021 | 6.35025 | 6.712325 | 6.123917 | 6.169437 | 6.047313 | 6.117652 | 6.212437 | 6.233984 | 6.783553 | 6.205702 |
1004.0098 | Sujay Ashok | Sujay K. Ashok and Nemani V. Suryanarayana | Supersymmetric Electromagnetic Waves on Giants and Dual-Giants | 18 pages | null | 10.1007/JHEP05(2012)074 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We set up the BPS equations for a D3-brane moving in AdS_5 \times S^5 which
preserves two supercharges and with all bosonic fields turned on in the
world-volume theory. By solving these, we find generalizations of Mikhailov
giants and wobbling dual-giants that include electromagnetic waves propagating
on their world-... | [
{
"created": "Thu, 1 Apr 2010 10:10:54 GMT",
"version": "v1"
}
] | 2015-05-18 | [
[
"Ashok",
"Sujay K.",
""
],
[
"Suryanarayana",
"Nemani V.",
""
]
] | We set up the BPS equations for a D3-brane moving in AdS_5 \times S^5 which preserves two supercharges and with all bosonic fields turned on in the world-volume theory. By solving these, we find generalizations of Mikhailov giants and wobbling dual-giants that include electromagnetic waves propagating on their world-vo... | 11.551629 | 9.934832 | 12.597775 | 9.231748 | 9.787785 | 8.409148 | 9.038799 | 9.718003 | 9.366319 | 12.166926 | 8.88047 | 9.701583 | 10.653584 | 9.45055 | 9.678701 | 9.721981 | 9.44177 | 9.573226 | 9.464287 | 10.87913 | 9.841151 |
1603.02956 | Guillermo Ballesteros | Guillermo Ballesteros, Denis Comelli, Luigi Pilo | Massive and modified gravity as self-gravitating media | 41 pages, new section, to appear in Phys. Rev. D | Phys. Rev. D 94, 124023 (2016) | 10.1103/PhysRevD.94.124023 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the effective field theory that describes the low-energy physics of
self-gravitating media. The field content consists of four derivatively coupled
scalar fields that can be identified with the internal comoving coordinates of
the medium. Imposing SO(3) internal spatial invariance, the theory describes
super... | [
{
"created": "Wed, 9 Mar 2016 16:43:39 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Nov 2016 11:14:01 GMT",
"version": "v2"
}
] | 2016-12-28 | [
[
"Ballesteros",
"Guillermo",
""
],
[
"Comelli",
"Denis",
""
],
[
"Pilo",
"Luigi",
""
]
] | We study the effective field theory that describes the low-energy physics of self-gravitating media. The field content consists of four derivatively coupled scalar fields that can be identified with the internal comoving coordinates of the medium. Imposing SO(3) internal spatial invariance, the theory describes superso... | 12.044411 | 13.739511 | 12.505184 | 11.617156 | 13.003 | 12.774117 | 12.608491 | 11.144745 | 12.780777 | 12.538278 | 11.99403 | 12.466739 | 12.021332 | 11.958245 | 12.14517 | 12.021403 | 11.691921 | 11.78333 | 11.983558 | 12.368371 | 12.038123 |
hep-th/0103060 | M. D. Maia | M. D. Maia & E. M. Monte | Geometric Stability of Brane-worlds | 8 pages revtex, twocolumn, no figures | null | null | null | hep-th gr-qc | null | The stability conditions for coordinate gauge independent perturbations of
brane-worlds are analyzed. It is shown that, these conditions lead to the
Einstein-Hilbert dynamics and to a confined gauge potential, independently of
models and metric ansatzes. The size of the extra dimensions are estimated
without assuming... | [
{
"created": "Fri, 9 Mar 2001 12:41:15 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Maia",
"M. D.",
""
],
[
"Monte",
"E. M.",
""
]
] | The stability conditions for coordinate gauge independent perturbations of brane-worlds are analyzed. It is shown that, these conditions lead to the Einstein-Hilbert dynamics and to a confined gauge potential, independently of models and metric ansatzes. The size of the extra dimensions are estimated without assuming a... | 26.994587 | 28.353937 | 24.234396 | 23.658146 | 25.706968 | 25.054956 | 27.063902 | 24.802883 | 24.405821 | 25.434042 | 23.74996 | 26.225237 | 25.09239 | 24.532543 | 25.315742 | 25.397823 | 26.197721 | 24.31838 | 25.880159 | 25.587297 | 23.865925 |
2111.12765 | Enrico Maria Malatesta | Ludovico T. Giorgini, Ulrich D. Jentschura, Enrico M. Malatesta,
Giorgio Parisi, Tommaso Rizzo, Jean Zinn-Justin | Correlation Functions of the Anharmonic Oscillator: Numerical
Verification of Two-Loop Corrections to the Large-Order Behavior | 18 pages, 4 figures | null | 10.1103/PhysRevD.105.105012 | null | hep-th cond-mat.dis-nn cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, the large-order behavior of correlation functions of the
$O(N)$-anharmonic oscillator has been analyzed by us in [L. T. Giorgini et el.,
Phys. Rev. D 101, 125001 (2020)]. Two-loop corrections about the instanton
configurations were obtained for the partition function, and the two-point and
four-point functi... | [
{
"created": "Wed, 24 Nov 2021 19:54:21 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Dec 2021 15:26:52 GMT",
"version": "v2"
}
] | 2022-06-01 | [
[
"Giorgini",
"Ludovico T.",
""
],
[
"Jentschura",
"Ulrich D.",
""
],
[
"Malatesta",
"Enrico M.",
""
],
[
"Parisi",
"Giorgio",
""
],
[
"Rizzo",
"Tommaso",
""
],
[
"Zinn-Justin",
"Jean",
""
]
] | Recently, the large-order behavior of correlation functions of the $O(N)$-anharmonic oscillator has been analyzed by us in [L. T. Giorgini et el., Phys. Rev. D 101, 125001 (2020)]. Two-loop corrections about the instanton configurations were obtained for the partition function, and the two-point and four-point function... | 8.136031 | 8.363698 | 8.46924 | 8.048072 | 9.163104 | 8.595827 | 8.956493 | 8.567679 | 7.925269 | 10.56954 | 7.958885 | 7.986228 | 8.199561 | 7.623565 | 7.722372 | 7.861138 | 8.262327 | 7.554583 | 7.680963 | 8.074032 | 8.044072 |
2205.06869 | Azadeh Mohammadi | Jo\~ao G. F. Campos and Azadeh Mohammadi | Kink-antikink collision in the supersymmetric $\phi^4$ model | null | null | 10.1007/JHEP08(2022)180 | null | hep-th nlin.PS | http://creativecommons.org/licenses/by/4.0/ | This paper investigates a model containing $\phi^4$ kinks interacting with
fermions. The fermion back-reaction is included in the equations of motion,
which affects the kink-antikink collisions. We show that the fermion field
generates a force that can be either attractive or repulsive. Moreover, we
investigate three... | [
{
"created": "Fri, 13 May 2022 19:57:11 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Dec 2022 18:48:11 GMT",
"version": "v2"
}
] | 2022-12-09 | [
[
"Campos",
"João G. F.",
""
],
[
"Mohammadi",
"Azadeh",
""
]
] | This paper investigates a model containing $\phi^4$ kinks interacting with fermions. The fermion back-reaction is included in the equations of motion, which affects the kink-antikink collisions. We show that the fermion field generates a force that can be either attractive or repulsive. Moreover, we investigate three d... | 10.021017 | 7.313881 | 9.254395 | 7.992485 | 7.712109 | 7.882086 | 8.448565 | 7.673764 | 7.984965 | 10.836538 | 7.93574 | 8.392624 | 9.393963 | 8.667238 | 8.361945 | 8.315003 | 8.631797 | 8.37129 | 8.954507 | 9.225189 | 8.615887 |
hep-th/0105114 | Dumitru Baleanu | Dumitru Baleanu, Yurdahan Guler | Multi Hamilton-Jacobi quantization of O(3) nonlinear sigma model | 10 pages, LaTeX, to be published in Mod. Phys. Lett. A | Mod.Phys.Lett. A16 (2001) 873-880 | 10.1142/S0217732301004157 | CU-MBB-10/2001 | hep-th | null | The O(3) non-linear sigma model is investigated using multi Hamilton-Jacobi
formalism. The integrability conditions are investigated and the results are in
agreement with those obtained by Dirac's method. By choosing an adequate
extension of phase space we describe the transformed system by a set of three
Hamilton-Ja... | [
{
"created": "Sat, 12 May 2001 17:51:10 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Baleanu",
"Dumitru",
""
],
[
"Guler",
"Yurdahan",
""
]
] | The O(3) non-linear sigma model is investigated using multi Hamilton-Jacobi formalism. The integrability conditions are investigated and the results are in agreement with those obtained by Dirac's method. By choosing an adequate extension of phase space we describe the transformed system by a set of three Hamilton-Jaco... | 23.084009 | 12.708647 | 12.689978 | 10.908592 | 12.829159 | 10.921038 | 12.148292 | 11.473598 | 12.470633 | 13.817799 | 10.946173 | 10.976083 | 12.136738 | 11.416935 | 11.293736 | 10.680648 | 10.609081 | 10.845189 | 11.511215 | 12.019555 | 10.509317 |
0911.4274 | Olaf Hohm | Daniel Grumiller, Olaf Hohm | AdS_3/LCFT_2 - Correlators in New Massive Gravity | 10 pages, v2: incorrect statement in conclusions deleted, reference
added, v3: version to appear in Phys. Lett. B | Phys.Lett.B686:264-267,2010 | 10.1016/j.physletb.2010.02.065 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate 2-point correlators for New Massive Gravity at the chiral point
and find that they behave precisely as those of a logarithmic conformal field
theory, which is characterized in addition to the central charges c_L = c_R = 0
by `new anomalies' b_L = b_R = -\sigma\frac{12\ell}{G_N}, where \sigma is the
sign ... | [
{
"created": "Mon, 23 Nov 2009 19:17:47 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Dec 2009 18:18:05 GMT",
"version": "v2"
},
{
"created": "Mon, 1 Mar 2010 14:49:51 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Grumiller",
"Daniel",
""
],
[
"Hohm",
"Olaf",
""
]
] | We calculate 2-point correlators for New Massive Gravity at the chiral point and find that they behave precisely as those of a logarithmic conformal field theory, which is characterized in addition to the central charges c_L = c_R = 0 by `new anomalies' b_L = b_R = -\sigma\frac{12\ell}{G_N}, where \sigma is the sign of... | 8.068502 | 6.919931 | 9.228895 | 6.405047 | 7.28282 | 7.166014 | 7.121676 | 6.811829 | 6.889296 | 9.185697 | 6.793616 | 7.080544 | 7.841853 | 6.869596 | 7.188899 | 7.204985 | 7.185033 | 6.981083 | 7.076661 | 7.994543 | 7.039733 |
hep-th/9201054 | null | Michael B. Green | Temperature Dependence of String Theory in the Presence of World-Sheet
Boundaries | 13 pages | Phys.Lett.B282:380-386,1992 | 10.1016/0370-2693(92)90656-O | null | hep-th | null | The effect of world-sheet boundaries on the temperature-dependence of bosonic
string theory is studied to first order in string perturbation theory. The
high- temperature behaviour of a theory with Dirichlet boundary conditions has
features suggestive of the high-temperature limit of the confining phase of
large-$n$ ... | [
{
"created": "Mon, 27 Jan 1992 09:24:07 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jan 1992 12:43:49 GMT",
"version": "v2"
}
] | 2010-11-01 | [
[
"Green",
"Michael B.",
""
]
] | The effect of world-sheet boundaries on the temperature-dependence of bosonic string theory is studied to first order in string perturbation theory. The high- temperature behaviour of a theory with Dirichlet boundary conditions has features suggestive of the high-temperature limit of the confining phase of large-$n$ $S... | 9.987587 | 7.909663 | 9.511191 | 7.46181 | 7.772964 | 7.685821 | 8.276104 | 8.037458 | 7.364608 | 8.685283 | 7.740194 | 8.34513 | 8.917377 | 8.457264 | 8.143777 | 7.872454 | 8.17689 | 8.381092 | 8.424171 | 8.774809 | 8.158303 |
hep-th/9911192 | Gesualdo Delfino | G. Delfino | Correlators in integrable quantum field theory. The scaling RSOS models | 22 pages, latex | Nucl.Phys. B583 (2000) 597-613 | 10.1016/S0550-3213(00)00324-2 | null | hep-th cond-mat | null | The study of the scaling limit of two-dimensional models of statistical
mechanics within the framework of integrable field theory is illustrated
through the example of the RSOS models. Starting from the exact description of
regime III in terms of colliding particles, we compute the correlation
functions of the therma... | [
{
"created": "Wed, 24 Nov 1999 15:13:44 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Delfino",
"G.",
""
]
] | The study of the scaling limit of two-dimensional models of statistical mechanics within the framework of integrable field theory is illustrated through the example of the RSOS models. Starting from the exact description of regime III in terms of colliding particles, we compute the correlation functions of the thermal,... | 9.980048 | 9.95453 | 13.142259 | 9.568071 | 9.878787 | 10.157855 | 10.433447 | 10.013514 | 9.983669 | 13.346574 | 9.319747 | 9.520041 | 10.02667 | 9.353995 | 9.571745 | 9.662617 | 9.730346 | 9.396826 | 9.524829 | 10.181039 | 9.35862 |
hep-th/0304211 | Troost Jan | Jan Troost and Asato Tsuchiya | Three-dimensional black hole entropy | 20 pages, 2 figures; v2: error corrected, conclusions changed | JHEP 0306 (2003) 029 | 10.1088/1126-6708/2003/06/029 | null | hep-th | null | We discuss in detail the properties of gravity with a negative cosmological
constant as viewed in Cherns-Simons theory on a line times a disc. We reanalyze
the problem of computing the BTZ entropy, and show how the demand of unitarity
and modular invariance of the boundary conformal field theory severely
constrain pr... | [
{
"created": "Thu, 24 Apr 2003 21:59:21 GMT",
"version": "v1"
},
{
"created": "Sat, 3 May 2003 17:24:53 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Troost",
"Jan",
""
],
[
"Tsuchiya",
"Asato",
""
]
] | We discuss in detail the properties of gravity with a negative cosmological constant as viewed in Cherns-Simons theory on a line times a disc. We reanalyze the problem of computing the BTZ entropy, and show how the demand of unitarity and modular invariance of the boundary conformal field theory severely constrain prop... | 15.684555 | 16.540909 | 16.11347 | 15.301794 | 15.854395 | 17.765743 | 16.560856 | 15.141747 | 15.284932 | 17.099237 | 15.893395 | 16.001057 | 16.366583 | 15.564382 | 14.783508 | 15.277844 | 15.31489 | 15.174819 | 15.763604 | 15.923137 | 15.08374 |
1105.6300 | Xiang-Song Chen | Xiang-Song Chen, Ben-Chao Zhu, Niall \'O Murchadha | Spin and orbital angular momentum of the tensor gauge field | 10 pages, no figure | null | null | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Following the recent studies of the trickiness in spin and orbital angular
momentum of the vector gauge fields, we perform here a parallel analysis for
the tensor gauge field, which has certain relation to gravitation. Similarly to
the vector case, we find a nice feature that after removing all gauge degrees
of freed... | [
{
"created": "Tue, 31 May 2011 14:30:22 GMT",
"version": "v1"
}
] | 2011-06-01 | [
[
"Chen",
"Xiang-Song",
""
],
[
"Zhu",
"Ben-Chao",
""
],
[
"Murchadha",
"Niall Ó",
""
]
] | Following the recent studies of the trickiness in spin and orbital angular momentum of the vector gauge fields, we perform here a parallel analysis for the tensor gauge field, which has certain relation to gravitation. Similarly to the vector case, we find a nice feature that after removing all gauge degrees of freedom... | 19.082661 | 18.826063 | 16.365974 | 17.342922 | 17.820944 | 17.14753 | 18.73012 | 17.673794 | 17.976568 | 18.811686 | 16.937208 | 16.704874 | 17.524937 | 17.463785 | 16.684284 | 17.143646 | 17.148817 | 16.519041 | 17.148993 | 16.772003 | 17.007387 |
hep-th/9210128 | Michel Talon | J. Avan and M. Talon | Classical R-matrix structure for the Calogero model | Latex file 9 pages | Phys.Lett. B303 (1993) 33-37 | 10.1016/0370-2693(93)90039-K | null | hep-th | null | A classical R-matrix structure is described for the Lax representation of the
integrable n-particle chains of Calogero-Olshanetski-Perelo\-mov. This R-matrix
is dynamical, non antisymmetric and non-invertible. It immediately triggers the
integrability of the Type I, II and III potentials, and the algebraic
structures... | [
{
"created": "Fri, 23 Oct 1992 15:50:01 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Avan",
"J.",
""
],
[
"Talon",
"M.",
""
]
] | A classical R-matrix structure is described for the Lax representation of the integrable n-particle chains of Calogero-Olshanetski-Perelo\-mov. This R-matrix is dynamical, non antisymmetric and non-invertible. It immediately triggers the integrability of the Type I, II and III potentials, and the algebraic structures a... | 18.631464 | 21.504442 | 24.050982 | 16.055153 | 19.477016 | 20.551161 | 18.248955 | 20.105412 | 20.229933 | 28.699594 | 18.076542 | 16.734663 | 20.093349 | 16.972672 | 17.172209 | 17.605682 | 16.571136 | 16.328791 | 16.341709 | 19.170763 | 16.018536 |
hep-th/0104188 | Bodo Geyer | Bodo Geyer and Dietmar M\"ulsch | Algebraic renormalization of twisted N=2 supersymmetry with Z=2 central
extension | 37 pages, AMSTEX | Nucl.Phys. B616 (2001) 437-475 | 10.1016/S0550-3213(01)00466-7 | U Leipzig, NTZ 04/2001 | hep-th | null | We study the renormalizability of (massive) topological QCD based on the
algebraic BRST technique by adopting a non-covariant Landau type gauge and
making use of the full topological superalgebra. The most general local counter
terms are determined and it is shown that in the presence of central charges
the BRST coho... | [
{
"created": "Mon, 23 Apr 2001 13:10:41 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Geyer",
"Bodo",
""
],
[
"Mülsch",
"Dietmar",
""
]
] | We study the renormalizability of (massive) topological QCD based on the algebraic BRST technique by adopting a non-covariant Landau type gauge and making use of the full topological superalgebra. The most general local counter terms are determined and it is shown that in the presence of central charges the BRST cohomo... | 12.892993 | 12.304036 | 12.746769 | 10.589135 | 11.822447 | 13.253655 | 11.624385 | 12.788811 | 11.436416 | 13.573032 | 11.246059 | 11.738944 | 11.822411 | 11.203638 | 11.305082 | 11.747495 | 11.763112 | 11.655781 | 11.113564 | 11.494568 | 11.020289 |
hep-th/9807189 | Delius | Gustav W. Delius | Restricting affine Toda theory to the half-line | 39 pages, 4 ps figures | JHEP 9809:016,1998 | 10.1088/1126-6708/1998/09/016 | null | hep-th math-ph math.MP nlin.SI solv-int | null | We restrict affine Toda field theory to the half-line by imposing certain
boundary conditions at $x=0$. The resulting theory possesses the same spectrum
of solitons and breathers as affine Toda theory on the whole line. The
classical solutions describing the reflection of these particles off the
boundary are obtained... | [
{
"created": "Mon, 27 Jul 1998 06:58:14 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Delius",
"Gustav W.",
""
]
] | We restrict affine Toda field theory to the half-line by imposing certain boundary conditions at $x=0$. The resulting theory possesses the same spectrum of solitons and breathers as affine Toda theory on the whole line. The classical solutions describing the reflection of these particles off the boundary are obtained f... | 8.558772 | 9.100057 | 10.395665 | 8.10793 | 9.222919 | 8.657771 | 9.467772 | 8.301423 | 8.337901 | 11.435383 | 8.360833 | 8.282337 | 8.788217 | 8.097789 | 8.140984 | 8.157496 | 8.442996 | 7.840016 | 7.932821 | 8.825007 | 7.825225 |
1708.08654 | Mohammad Hassan Vahidinia | S.M. Noorbakhsh and M.H. Vahidinia | Extremal Vanishing Horizon Kerr-AdS Black Holes at Ultraspinning Limit | 29 pages, 3 figures, references added, typos corrected, revised
version to match published version | JHEP 1801 (2018) 042 | 10.1007/JHEP01(2018)042 | IPM/P-2017/093 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | By utilizing the ultraspinning limit we generate a new class of extremal
vanishing horizon (EVH) black holes in odd dimensions ($d\geq5$). Starting from
the general multi-spinning Kerr-AdS metrics, we show the EVH limit commutes
with the ultraspinning limit, in which the resulting solutions possess a
non-compact but ... | [
{
"created": "Tue, 29 Aug 2017 09:23:07 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Apr 2019 12:37:17 GMT",
"version": "v2"
}
] | 2019-04-09 | [
[
"Noorbakhsh",
"S. M.",
""
],
[
"Vahidinia",
"M. H.",
""
]
] | By utilizing the ultraspinning limit we generate a new class of extremal vanishing horizon (EVH) black holes in odd dimensions ($d\geq5$). Starting from the general multi-spinning Kerr-AdS metrics, we show the EVH limit commutes with the ultraspinning limit, in which the resulting solutions possess a non-compact but fi... | 10.502567 | 9.002007 | 9.922514 | 8.962842 | 10.536624 | 9.554625 | 10.071722 | 9.365278 | 9.335564 | 11.948194 | 9.557775 | 9.794283 | 10.021139 | 9.815116 | 10.150053 | 10.1718 | 9.923604 | 9.646746 | 9.798769 | 10.420351 | 9.591286 |
0901.0577 | Ali Chamseddine | Ali H. Chamseddine | Noncommutative Geometry as the Key to Unlock the Secrets of Space-Time | Contribution to a special volume in honor of Alain Connes in occasion
of his 60th birthday. To be published in the Proceedings series of the Clay
Mathematics Institute. Editors E. Blanchard et al | null | null | Clay Math.Proc. 11 (2010) 127-148 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I give a summary of the progress made on using the elegant construction of
Alain Connes noncommutaive geometry to explore the nature of space-time at very
high energies. In particular I show that by making very few natural and weak
assumptions about the structure of the noncommutative space, one can deduce the
struct... | [
{
"created": "Tue, 6 Jan 2009 11:14:21 GMT",
"version": "v1"
}
] | 2019-08-20 | [
[
"Chamseddine",
"Ali H.",
""
]
] | I give a summary of the progress made on using the elegant construction of Alain Connes noncommutaive geometry to explore the nature of space-time at very high energies. In particular I show that by making very few natural and weak assumptions about the structure of the noncommutative space, one can deduce the structur... | 12.958468 | 10.853241 | 10.13302 | 9.751101 | 11.469851 | 10.663733 | 10.115768 | 9.924716 | 9.747222 | 12.343069 | 9.921784 | 10.136191 | 11.463937 | 10.151919 | 10.648504 | 10.236317 | 10.569904 | 10.217361 | 9.939923 | 10.887325 | 10.595772 |
hep-th/9906223 | Itzhak Bars | I. Bars, C. Deliduman, D. Minic | Strings, Branes and Two-Time Physics | Latex, 12 pages | Phys.Lett. B466 (1999) 135-143 | 10.1016/S0370-2693(99)01127-2 | USC-99/HEP-B2 | hep-th | null | We generalize the ideas and formalism of Two-Time Physics from particle
dynamics to some specific examples of string and p-brane (p >= 1) dynamics. The
two-time string or p-brane action can be gauge fixed to produce various
one-time string or p-brane actions that are dual to each other under gauge
transformations. We... | [
{
"created": "Mon, 28 Jun 1999 23:59:00 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Bars",
"I.",
""
],
[
"Deliduman",
"C.",
""
],
[
"Minic",
"D.",
""
]
] | We generalize the ideas and formalism of Two-Time Physics from particle dynamics to some specific examples of string and p-brane (p >= 1) dynamics. The two-time string or p-brane action can be gauge fixed to produce various one-time string or p-brane actions that are dual to each other under gauge transformations. We d... | 8.424558 | 6.759053 | 8.034291 | 6.839839 | 6.738537 | 6.589705 | 6.732734 | 6.924565 | 6.950001 | 7.512746 | 6.594996 | 7.212998 | 8.255356 | 7.287611 | 7.383365 | 7.530226 | 7.51411 | 7.299119 | 7.384273 | 8.187009 | 7.304421 |
hep-th/9905059 | Yosuke Imamura | Yosuke Imamura | String junctions on backgrounds with a positively charged orientifold
plane | 16 pages + 3 eps figures, LaTeX, a reference added | JHEP 9907 (1999) 024 | 10.1088/1126-6708/1999/07/024 | YITP-99-24 | hep-th | null | By means of the heterotic/type IIB duality, we study properties of junctions
on backgrounds with a positively charged orientifold seven-plane and D-branes,
which are expected to give seven dimensional Sp(r) gauge theories. We give a
modified BPS condition for the junctions and show that it reproduces the
adjoint repr... | [
{
"created": "Sun, 9 May 1999 14:13:31 GMT",
"version": "v1"
},
{
"created": "Fri, 27 Aug 1999 16:06:58 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Imamura",
"Yosuke",
""
]
] | By means of the heterotic/type IIB duality, we study properties of junctions on backgrounds with a positively charged orientifold seven-plane and D-branes, which are expected to give seven dimensional Sp(r) gauge theories. We give a modified BPS condition for the junctions and show that it reproduces the adjoint repres... | 14.054996 | 13.327839 | 16.302406 | 13.135235 | 14.112856 | 13.670087 | 13.396757 | 12.523743 | 13.025277 | 18.811546 | 12.139806 | 12.967688 | 14.42079 | 12.864128 | 13.163125 | 12.590469 | 13.199466 | 12.761341 | 12.954283 | 14.148533 | 12.361272 |
hep-th/9706097 | Juan Maldacena | Sergio Ferrara and Juan M. Maldacena | Branes, central charges and U-duality invariant BPS conditions | 15 pages, no figures, typos corrected | Class.Quant.Grav. 15 (1998) 749-758 | 10.1088/0264-9381/15/4/004 | null | hep-th | null | In extended supergravity theories there are $p$-brane solutions preserving
different numbers of supersymmetries, depending on the charges, the spacetime
dimension and the number of original supersymmetries (8, 16 or 32). We find
U-duality invariant conditions on the quantized charges which specify the
number of super... | [
{
"created": "Thu, 12 Jun 1997 20:42:25 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Aug 1997 14:24:32 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Ferrara",
"Sergio",
""
],
[
"Maldacena",
"Juan M.",
""
]
] | In extended supergravity theories there are $p$-brane solutions preserving different numbers of supersymmetries, depending on the charges, the spacetime dimension and the number of original supersymmetries (8, 16 or 32). We find U-duality invariant conditions on the quantized charges which specify the number of supersy... | 6.126482 | 6.186746 | 6.070229 | 5.929775 | 5.775106 | 6.324708 | 6.414253 | 6.128323 | 5.898131 | 7.374898 | 5.669397 | 6.119878 | 6.221191 | 5.658217 | 5.837071 | 5.755247 | 5.652239 | 5.795846 | 5.746612 | 6.452177 | 5.791623 |
2108.11742 | Saeedeh Sadeghian | Hovhannes Demirchian and Saeedeh Sadeghian | Separability of Klein-Gordon Equation on Near Horizon Extremal
Myers-Perry Black Hole | 7 pages, references added, minor typos fixed | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We investigate the separability of Klein-Gordon equation on near horizon of
d-dimensional rotating Myers-Perry black hole in two limits : 1) generic
extremal case and 2) extremal vanishing horizon case. In the first case , there
is a relation between the mass and rotation parameters so that black hole
temperature van... | [
{
"created": "Thu, 26 Aug 2021 12:39:18 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Sep 2021 09:10:40 GMT",
"version": "v2"
}
] | 2021-09-07 | [
[
"Demirchian",
"Hovhannes",
""
],
[
"Sadeghian",
"Saeedeh",
""
]
] | We investigate the separability of Klein-Gordon equation on near horizon of d-dimensional rotating Myers-Perry black hole in two limits : 1) generic extremal case and 2) extremal vanishing horizon case. In the first case , there is a relation between the mass and rotation parameters so that black hole temperature vanis... | 8.334816 | 7.440956 | 7.237691 | 7.348395 | 7.836975 | 7.979966 | 8.338816 | 7.518903 | 6.820911 | 8.517727 | 7.322251 | 7.65601 | 7.326485 | 7.238664 | 7.322268 | 7.437431 | 7.467297 | 7.440079 | 7.15566 | 7.442371 | 7.297956 |
2110.04303 | Cameron V. Cogburn | Cameron V. Cogburn | CFT$_2$ in the Bulk | 35 pages, 2 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We study non-Gaussian bulk 2d CFTs in AdS$_2$ using boundary CFT techniques
and recent results in JT/Schwarzian gravity. We highlight the constraints on
the operator content of a theory imposed by the boundary conditions by
examining the relation between correlator coefficients and OPE coefficients in
the presence of... | [
{
"created": "Fri, 8 Oct 2021 18:00:00 GMT",
"version": "v1"
}
] | 2021-10-12 | [
[
"Cogburn",
"Cameron V.",
""
]
] | We study non-Gaussian bulk 2d CFTs in AdS$_2$ using boundary CFT techniques and recent results in JT/Schwarzian gravity. We highlight the constraints on the operator content of a theory imposed by the boundary conditions by examining the relation between correlator coefficients and OPE coefficients in the presence of a... | 13.025266 | 11.119997 | 12.123922 | 11.342481 | 12.252032 | 11.39174 | 12.160576 | 11.590406 | 10.769744 | 13.106708 | 11.480677 | 11.778025 | 13.053254 | 12.172013 | 12.368852 | 12.47717 | 11.74035 | 12.12246 | 12.097024 | 13.082616 | 11.678655 |
hep-th/0410144 | Gary McCartor | G. McCartor | Induced Operators in QCD | 8 pages. Talk presented at Light-Cone 2004 at the VU Amsterdam | Few Body Syst.36:181-188,2005 | 10.1007/s00601-004-0098-3 | SMUHEP/03/1 | hep-th | null | Light-cone quantization always involves the solution of differential
constraint equations. The solutions to these equations include integration
constants (fields independent of $x_-$). These fields are unphysical but when
they are consistently removed from the dynamics, additional operators (induced
operators), which... | [
{
"created": "Tue, 12 Oct 2004 21:44:25 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"McCartor",
"G.",
""
]
] | Light-cone quantization always involves the solution of differential constraint equations. The solutions to these equations include integration constants (fields independent of $x_-$). These fields are unphysical but when they are consistently removed from the dynamics, additional operators (induced operators), which w... | 14.590058 | 15.776497 | 14.064 | 14.009885 | 14.639159 | 15.30312 | 14.419105 | 13.95661 | 13.745842 | 14.873735 | 14.171548 | 14.462628 | 13.842536 | 13.922359 | 14.03281 | 14.269682 | 14.05174 | 14.074596 | 13.608286 | 14.239754 | 13.793688 |
hep-th/0106162 | Hong Lu | M. Cvetic, G.W. Gibbons, James T. Liu, H. Lu and C.N. Pope | A New Fractional D2-brane, G_2 Holonomy and T-duality | Latex, 13 pages | Class.Quant.Grav.19:5163-5172,2002 | 10.1088/0264-9381/19/20/310 | null | hep-th | null | Recently, a new example of a complete non-compact Ricci-flat metric of G_2
holonomy was constructed, which has an asymptotically locally conical structure
at infinity with a circular direction whose radius stabilises. In this paper we
find a regular harmonic 3-form in this metric, which we then use in order to
obtain... | [
{
"created": "Tue, 19 Jun 2001 22:16:56 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Cvetic",
"M.",
""
],
[
"Gibbons",
"G. W.",
""
],
[
"Liu",
"James T.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
]
] | Recently, a new example of a complete non-compact Ricci-flat metric of G_2 holonomy was constructed, which has an asymptotically locally conical structure at infinity with a circular direction whose radius stabilises. In this paper we find a regular harmonic 3-form in this metric, which we then use in order to obtain a... | 8.590234 | 7.141147 | 9.057926 | 7.437619 | 7.419088 | 7.635876 | 7.560112 | 8.00851 | 7.240421 | 10.44041 | 6.982566 | 7.052668 | 8.323735 | 7.289487 | 7.351504 | 7.384515 | 7.371037 | 7.134262 | 7.4694 | 8.393936 | 7.286474 |
1106.3307 | Daniel Robbins | Katrin Becker, Guangyu Guo and Daniel Robbins | Disc amplitudes, picture changing and space-time actions | 55 pages, 1 figure | null | 10.1007/JHEP01(2012)127 | MIFPA-11-18 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study in detail the procedure for obtaining couplings of D-branes to
closed string fields by evaluating string theory disc amplitudes. We perform a
careful construction of the relevant vertex operators and discuss the effects
of inserting the boundary state which encodes the presence of the D-brane. We
confront th... | [
{
"created": "Thu, 16 Jun 2011 18:54:38 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Becker",
"Katrin",
""
],
[
"Guo",
"Guangyu",
""
],
[
"Robbins",
"Daniel",
""
]
] | We study in detail the procedure for obtaining couplings of D-branes to closed string fields by evaluating string theory disc amplitudes. We perform a careful construction of the relevant vertex operators and discuss the effects of inserting the boundary state which encodes the presence of the D-brane. We confront the ... | 10.725537 | 9.690814 | 12.62143 | 10.303649 | 10.030101 | 11.031528 | 10.642174 | 9.899245 | 9.816228 | 12.184258 | 10.289258 | 10.471182 | 11.010489 | 10.444978 | 10.256835 | 10.378982 | 10.269111 | 10.346137 | 10.250338 | 10.979349 | 9.953301 |
1705.07943 | Ning Bao | Ning Bao and Hirosi Ooguri | On Distinguishability of Black Hole Microstates | 12 pages, 3 figures, Correction added to section 3 and references
added | Phys. Rev. D 96, 066017 (2017) | 10.1103/PhysRevD.96.066017 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the Holevo information to estimate distinguishability of microstates
of a black hole in anti-de Sitter space by measurements one can perform on a
subregion of a Cauchy surface of the dual conformal field theory. We find that
microstates are not distinguishable at all until the subregion reaches a
certain size ... | [
{
"created": "Mon, 22 May 2017 18:44:30 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Sep 2017 21:16:21 GMT",
"version": "v2"
}
] | 2017-09-27 | [
[
"Bao",
"Ning",
""
],
[
"Ooguri",
"Hirosi",
""
]
] | We use the Holevo information to estimate distinguishability of microstates of a black hole in anti-de Sitter space by measurements one can perform on a subregion of a Cauchy surface of the dual conformal field theory. We find that microstates are not distinguishable at all until the subregion reaches a certain size an... | 6.44676 | 6.375086 | 7.899384 | 6.424654 | 6.57738 | 6.585526 | 6.417558 | 6.335836 | 6.556009 | 7.418003 | 6.407462 | 6.276637 | 6.644799 | 6.238174 | 6.267665 | 6.415776 | 6.333818 | 6.508098 | 6.157879 | 6.542676 | 6.433215 |
1806.10877 | Georgi Dvali | Gia Dvali and Cesar Gomez | On Exclusion of Positive Cosmological Constant | 2 pages | null | 10.1002/prop.201800092 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Some time ago we have suggested that positive vacuum energy exhibits a finite
quantum break time, which can be a signal that a positive cosmological constant
is inconsistent. From the requirement that Universe never undergoes through
quantum breaking, we have derived an absolute lower bound on the speed of
variation ... | [
{
"created": "Thu, 28 Jun 2018 11:02:12 GMT",
"version": "v1"
}
] | 2021-07-28 | [
[
"Dvali",
"Gia",
""
],
[
"Gomez",
"Cesar",
""
]
] | Some time ago we have suggested that positive vacuum energy exhibits a finite quantum break time, which can be a signal that a positive cosmological constant is inconsistent. From the requirement that Universe never undergoes through quantum breaking, we have derived an absolute lower bound on the speed of variation of... | 19.8549 | 20.455322 | 19.039284 | 17.264528 | 19.233133 | 19.69445 | 19.450674 | 17.816233 | 19.164116 | 19.355358 | 18.117622 | 19.446028 | 18.843664 | 18.565256 | 18.472002 | 18.988636 | 17.943211 | 18.712818 | 18.047575 | 18.889896 | 18.284733 |
1908.02416 | John F. Donoghue | John F. Donoghue and Gabriel Menezes | Unitarity, stability and loops of unstable ghosts | 24 pages, 12 figures, some typos corrected and a discussion of
related work improved | Phys. Rev. D 100, 105006 (2019) | 10.1103/PhysRevD.100.105006 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a new understanding of the unstable ghost-like resonance which
appears in theories such as quadratic gravity and Lee-Wick type theories.
Quantum corrections make this resonance unstable, such that it does not appear
in the asymptotic spectrum. We prove that these theories are unitary to all
orders. Unitari... | [
{
"created": "Wed, 7 Aug 2019 01:54:19 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Aug 2019 18:54:37 GMT",
"version": "v2"
}
] | 2019-11-20 | [
[
"Donoghue",
"John F.",
""
],
[
"Menezes",
"Gabriel",
""
]
] | We present a new understanding of the unstable ghost-like resonance which appears in theories such as quadratic gravity and Lee-Wick type theories. Quantum corrections make this resonance unstable, such that it does not appear in the asymptotic spectrum. We prove that these theories are unitary to all orders. Unitarity... | 13.801475 | 15.641126 | 15.293884 | 13.915851 | 14.839887 | 14.166852 | 15.580191 | 14.416513 | 14.55506 | 15.694677 | 14.046521 | 13.922362 | 14.139335 | 13.975264 | 14.131782 | 14.248923 | 13.593215 | 13.865082 | 13.873108 | 14.139732 | 14.520431 |
0911.4518 | Per Kraus | Eric D'Hoker and Per Kraus | Charged Magnetic Brane Solutions in AdS_5 and the fate of the third law
of thermodynamics | 45 pages v2: added note about subsequent results found in
arXiv:1003.1302 | JHEP 1003:095,2010 | 10.1007/JHEP03(2010)095 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct asymptotically AdS_5 solutions to 5-dimensional Einstein-Maxwell
theory with Chern-Simons term which are dual to 4-dimensional gauge theories,
including N=4 SYM theory, in the presence of a constant background magnetic
field B and a uniform electric charge density \rho. For the solutions
corresponding to... | [
{
"created": "Mon, 23 Nov 2009 23:30:08 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 2010 16:16:23 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"D'Hoker",
"Eric",
""
],
[
"Kraus",
"Per",
""
]
] | We construct asymptotically AdS_5 solutions to 5-dimensional Einstein-Maxwell theory with Chern-Simons term which are dual to 4-dimensional gauge theories, including N=4 SYM theory, in the presence of a constant background magnetic field B and a uniform electric charge density \rho. For the solutions corresponding to s... | 6.881596 | 6.455451 | 6.881404 | 6.562384 | 6.963433 | 6.589954 | 6.700658 | 6.714275 | 6.708186 | 7.809223 | 6.332416 | 6.464963 | 6.788186 | 6.546813 | 6.453298 | 6.589555 | 6.633241 | 6.566648 | 6.500225 | 6.896994 | 6.522925 |
1512.01576 | Miguel Riquelme | Alfredo Perez, Miguel Riquelme, David Tempo, Ricardo Troncoso | Asymptotic structure of the Einstein-Maxwell theory on AdS$_{3}$ | 18 pages, no figures | null | 10.1007/JHEP02(2016)015 | CECS-PHY-15/08 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The asymptotic structure of AdS spacetimes in the context of General
Relativity coupled to the Maxwell field in three spacetime dimensions is
analyzed. Although the fall-off of the fields is relaxed with respect to that
of Brown and Henneaux, the variation of the canonical generators associated to
the asymptotic Kill... | [
{
"created": "Fri, 4 Dec 2015 22:01:51 GMT",
"version": "v1"
}
] | 2016-03-23 | [
[
"Perez",
"Alfredo",
""
],
[
"Riquelme",
"Miguel",
""
],
[
"Tempo",
"David",
""
],
[
"Troncoso",
"Ricardo",
""
]
] | The asymptotic structure of AdS spacetimes in the context of General Relativity coupled to the Maxwell field in three spacetime dimensions is analyzed. Although the fall-off of the fields is relaxed with respect to that of Brown and Henneaux, the variation of the canonical generators associated to the asymptotic Killin... | 6.758472 | 7.551869 | 7.43694 | 6.591025 | 7.03741 | 7.026272 | 6.847075 | 7.043905 | 6.567256 | 7.96642 | 6.534992 | 6.455151 | 6.806104 | 6.614185 | 6.540546 | 6.537365 | 6.47643 | 6.470245 | 6.57443 | 6.616908 | 6.601261 |
hep-th/9409057 | Shahn Majid | Shahn Majid | Duality Principle and Braided Geometry | 24 pages | null | 10.1007/3-540-59163-X_265 | DAMTP/94-69 | hep-th math.QA | null | We give an overview of a new kind symmetry in physics which exists between
observables and states and which is made possible by the language of Hopf
algebras and quantum geometry. It has been proposed by the author as a feature
of Planck scale physics. More recent work includes corresponding results at the
semiclassi... | [
{
"created": "Sat, 10 Sep 1994 23:14:55 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Majid",
"Shahn",
""
]
] | We give an overview of a new kind symmetry in physics which exists between observables and states and which is made possible by the language of Hopf algebras and quantum geometry. It has been proposed by the author as a feature of Planck scale physics. More recent work includes corresponding results at the semiclassica... | 15.022476 | 15.462414 | 15.758307 | 15.174063 | 16.579206 | 16.608286 | 15.775099 | 15.214814 | 14.909505 | 18.583483 | 15.586685 | 15.079882 | 15.23423 | 14.996046 | 14.818358 | 14.945006 | 15.310656 | 14.842947 | 15.189794 | 15.104007 | 14.952732 |
hep-th/9902110 | Nikita Nekrassov | Nikita Nekrasov and Samson L. Shatashvili | On Non-Supersymmetric CFT in Four Dimensions | harvmac, 4 pp; v2. Z_4 field content corrected, references reworked | Phys.Rept. 320 (1999) 127-129 | 10.1016/S0370-1573(99)00059-9 | ITEP-TH-06/99, HUTP-99/A007 | hep-th | null | We show that the $\mathcal{N}=0$ theories on the self-dual D3-branes of Type
0 string theory are in the class of the previously considered tadpole-free
orbifolds of $\mathcal{N} = 4$ theory (although they have SO(6) global
symmetry) and hence have vanishing beta function in the planar limit to all
orders in 't Hooft ... | [
{
"created": "Mon, 15 Feb 1999 23:16:32 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Apr 1999 23:37:21 GMT",
"version": "v2"
}
] | 2017-09-07 | [
[
"Nekrasov",
"Nikita",
""
],
[
"Shatashvili",
"Samson L.",
""
]
] | We show that the $\mathcal{N}=0$ theories on the self-dual D3-branes of Type 0 string theory are in the class of the previously considered tadpole-free orbifolds of $\mathcal{N} = 4$ theory (although they have SO(6) global symmetry) and hence have vanishing beta function in the planar limit to all orders in 't Hooft co... | 5.733773 | 5.506205 | 5.975396 | 5.634049 | 5.876718 | 5.794623 | 5.951143 | 5.368345 | 5.568841 | 6.854618 | 5.41907 | 5.710752 | 5.956595 | 5.609434 | 5.696988 | 5.670628 | 5.794095 | 5.814577 | 5.64879 | 5.860562 | 5.612832 |
hep-th/0611161 | Antonio Soares de Castro | Luis B. Castro and Antonio S. de Castro | Confinement of spin-0 and spin-1/2 particles in a mixed vector-scalar
coupling with unequal shapes for the potentials | 9 pages, 3 figures | Phys.Scripta75:170-173,2007 | 10.1088/0031-8949/75/2/009 | null | hep-th quant-ph | null | The Klein-Gordon and the Dirac equations with vector and scalar potentials
are investigated under a more general condition, $V_{v}=V_{s} +
\mathrm{const.}$ These isospectral problems are solved in a case of squared
trigonometric potential functions and bound states for either particles or
antiparticles are found. The... | [
{
"created": "Tue, 14 Nov 2006 23:04:56 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Castro",
"Luis B.",
""
],
[
"de Castro",
"Antonio S.",
""
]
] | The Klein-Gordon and the Dirac equations with vector and scalar potentials are investigated under a more general condition, $V_{v}=V_{s} + \mathrm{const.}$ These isospectral problems are solved in a case of squared trigonometric potential functions and bound states for either particles or antiparticles are found. The e... | 9.534611 | 6.640446 | 9.236406 | 7.476438 | 8.576308 | 9.119621 | 9.016736 | 7.832952 | 7.741673 | 9.75364 | 7.803521 | 8.086056 | 8.468846 | 7.889134 | 8.223256 | 8.376643 | 8.415548 | 8.401669 | 8.007969 | 8.625278 | 8.187079 |
0909.3714 | Michael Thies | Christian Boehmer, Michael Thies | Large N solution of generalized Gross-Neveu model with two coupling
constants | 16 pages, 13 figures; v2: small corrections, improved readability;
v3: typos in references corrected | Phys.Rev.D80:125038,2009 | 10.1103/PhysRevD.80.125038 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Gross-Neveu model in 1+1 dimensions is generalized to the case of
different scalar and pseudoscalar coupling constants. This enables us to
interpolate smoothly between the standard massless Gross-Neveu models with
either discrete or continuous chiral symmetry. We present the solution of the
generalized model in t... | [
{
"created": "Mon, 21 Sep 2009 08:59:25 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Dec 2009 08:42:17 GMT",
"version": "v2"
},
{
"created": "Thu, 7 Jan 2010 09:10:03 GMT",
"version": "v3"
}
] | 2010-01-08 | [
[
"Boehmer",
"Christian",
""
],
[
"Thies",
"Michael",
""
]
] | The Gross-Neveu model in 1+1 dimensions is generalized to the case of different scalar and pseudoscalar coupling constants. This enables us to interpolate smoothly between the standard massless Gross-Neveu models with either discrete or continuous chiral symmetry. We present the solution of the generalized model in the... | 6.417992 | 5.577328 | 5.758683 | 5.378312 | 6.431595 | 6.02557 | 5.84913 | 5.69113 | 5.29894 | 6.276867 | 5.765614 | 5.733535 | 6.06119 | 5.700556 | 5.867957 | 6.140333 | 6.008093 | 5.895912 | 5.871541 | 6.139405 | 5.827136 |
1309.5042 | Nele Callebaut | Nele Callebaut, David Dudal | A magnetic instability of the non-Abelian Sakai-Sugimoto model | 42 pages, v2: version accepted for publication in JHEP | null | 10.1007/JHEP01(2014)055 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this follow-up paper of 1105.2217 we further discuss the occurrence of a
magnetically induced tachyonic instability of the rho meson in the two-flavour
Sakai-Sugimoto model, uplifting two remaining approximations in the previous
paper. That is, firstly, the magnetically induced splitting of the branes is
now taken... | [
{
"created": "Thu, 19 Sep 2013 16:33:36 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Dec 2013 18:21:34 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Callebaut",
"Nele",
""
],
[
"Dudal",
"David",
""
]
] | In this follow-up paper of 1105.2217 we further discuss the occurrence of a magnetically induced tachyonic instability of the rho meson in the two-flavour Sakai-Sugimoto model, uplifting two remaining approximations in the previous paper. That is, firstly, the magnetically induced splitting of the branes is now taken i... | 11.035861 | 11.030591 | 10.451161 | 9.69453 | 10.625939 | 10.768507 | 10.328815 | 10.067235 | 9.946099 | 11.936514 | 10.205997 | 10.097083 | 10.144423 | 9.927374 | 10.066942 | 10.234779 | 10.041066 | 9.97261 | 10.231254 | 10.161837 | 9.894685 |
1910.05131 | Jerzy Lukierski | Richard Kerner and Jerzy Lukierski | Towards a $Z_3$-graded approach to quarks' symmetries | 20 pages, 1 figure; submitted to Proceedings of ISOS26 Conference
held in Prague, Czech Republik (08-012.07.2019); to appear in Journal of
Physics (Conference Series). arXiv admin note: text overlap with
arXiv:1801.01403; v2 corrected formula (31), version to appear in Journal of
Physics, Conference Series | null | 10.1088/1742-6596/1416/1/012016 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Colour $SU(3)$ group is an exact symmetry of Quantum Chromodynamics, which
describes strong interactions between quarks and gluons. Supplemented by two
internal symmetries, $SU(2)$ and $U(1)$, it serves as the internal symmetry of
the Standard Model, describing as well the electroweak interactions of quarks
and lepto... | [
{
"created": "Thu, 10 Oct 2019 17:40:27 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Nov 2019 14:41:36 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Kerner",
"Richard",
""
],
[
"Lukierski",
"Jerzy",
""
]
] | Colour $SU(3)$ group is an exact symmetry of Quantum Chromodynamics, which describes strong interactions between quarks and gluons. Supplemented by two internal symmetries, $SU(2)$ and $U(1)$, it serves as the internal symmetry of the Standard Model, describing as well the electroweak interactions of quarks and leptons... | 7.730186 | 7.447132 | 7.637185 | 7.328451 | 7.43796 | 7.50379 | 7.6506 | 7.191669 | 7.479308 | 7.572361 | 7.216311 | 7.364491 | 7.256481 | 7.205512 | 7.194969 | 7.37352 | 7.456776 | 7.10844 | 7.20018 | 7.452144 | 7.017345 |
0902.1770 | Sho Yaida | Sho Yaida | Landscape versus Swampland for Higher Derivative Gravity | 2 pages, prepared for the Proceedings of the Cargese Summer School
2008 | Nucl.Phys.Proc.Suppl.192-193:201-202,2009 | 10.1016/j.nuclphysbps.2009.07.081 | SU-ITP-09/07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We survey recent studies of Gauss-Bonnet gravity and its dual conformal field
theories, including their relation to the violation of the Kovtun-Starinets-Son
viscosity bound. Via holography, we can also study properties such as
microcausality and unitarity of boundary field theory duals. Such studies in
turn supply c... | [
{
"created": "Tue, 10 Feb 2009 22:57:03 GMT",
"version": "v1"
}
] | 2009-10-06 | [
[
"Yaida",
"Sho",
""
]
] | We survey recent studies of Gauss-Bonnet gravity and its dual conformal field theories, including their relation to the violation of the Kovtun-Starinets-Son viscosity bound. Via holography, we can also study properties such as microcausality and unitarity of boundary field theory duals. Such studies in turn supply con... | 12.524651 | 11.495434 | 14.695884 | 10.480388 | 12.208429 | 11.402231 | 10.93394 | 10.908049 | 10.21896 | 14.220099 | 10.494428 | 10.568277 | 11.975256 | 10.733846 | 11.267852 | 10.685349 | 10.611529 | 10.7544 | 10.867545 | 12.674784 | 10.918128 |
hep-th/0204078 | Takehiro Azuma | Takehiro Azuma, Hikaru Kawai | Matrix model with manifest general coordinate invariance | 15 pages, 2 figures (V5) some explanation added. (V6) some typos
corrected. To appear in Phys. Lett. B | Phys.Lett. B538 (2002) 393-405 | 10.1016/S0370-2693(02)02021-X | KUNS-1776 | hep-th | null | We present a formulation of a matrix model which manifestly possesses the
general coordinate invariance when we identify the large $N$ matrices with
differential operators. In order to build a matrix model which has the local
Lorentz invariance, we investigate how the $so(9,1)$ Lorentz symmetry and the
$u(N)$ gauge s... | [
{
"created": "Tue, 9 Apr 2002 10:31:31 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Apr 2002 14:06:40 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Apr 2002 14:01:05 GMT",
"version": "v3"
},
{
"created": "Thu, 2 May 2002 15:03:36 GMT",
"version": "v4"
},
{
"cre... | 2015-06-26 | [
[
"Azuma",
"Takehiro",
""
],
[
"Kawai",
"Hikaru",
""
]
] | We present a formulation of a matrix model which manifestly possesses the general coordinate invariance when we identify the large $N$ matrices with differential operators. In order to build a matrix model which has the local Lorentz invariance, we investigate how the $so(9,1)$ Lorentz symmetry and the $u(N)$ gauge sym... | 7.449724 | 7.5074 | 8.244637 | 7.028772 | 7.199768 | 6.907123 | 6.729455 | 7.389176 | 6.857483 | 8.081359 | 7.258768 | 7.467173 | 7.655003 | 7.429276 | 7.327911 | 7.245546 | 7.389914 | 7.502943 | 7.345129 | 7.444205 | 7.200789 |
1012.5681 | Mihailo \v{C}ubrovi\'c | Mihailo \v{C}ubrovi\'c, Jan Zaanen, Koenraad Schalm | Constructing the AdS dual of a Fermi liquid: AdS Black holes with Dirac
hair | 26 pages, 6 figures; sections 2-3 substantially revised for improved
clarity | null | 10.1007/JHEP10(2011)017 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide new evidence that the holographic dual to a strongly coupled
charged Fermi Liquid has a non-zero fermion density in the bulk. We show that
the pole-strength of the stable quasiparticle characterizing the Fermi surface
is encoded in the spatially averaged AdS probability density of a single
normalizable fer... | [
{
"created": "Tue, 28 Dec 2010 00:34:37 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Jan 2011 21:08:54 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Jul 2011 16:36:11 GMT",
"version": "v3"
}
] | 2015-05-20 | [
[
"Čubrović",
"Mihailo",
""
],
[
"Zaanen",
"Jan",
""
],
[
"Schalm",
"Koenraad",
""
]
] | We provide new evidence that the holographic dual to a strongly coupled charged Fermi Liquid has a non-zero fermion density in the bulk. We show that the pole-strength of the stable quasiparticle characterizing the Fermi surface is encoded in the spatially averaged AdS probability density of a single normalizable fermi... | 12.135402 | 12.702549 | 12.09521 | 10.42411 | 11.93174 | 12.100353 | 11.767117 | 10.940354 | 10.264991 | 13.626059 | 11.217291 | 10.982297 | 11.349408 | 10.951428 | 10.985756 | 10.999028 | 11.007918 | 10.789837 | 11.213387 | 11.581724 | 10.897871 |
1612.03631 | Georgios Pastras | Georgios Pastras | Static Elliptic Minimal Surfaces in AdS(4) | 47 pages, 15 figures | Eur. Phys. J. C (2017) 77: 797 | 10.1140/epjc/s10052-017-5292-9 | null | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Ryu-Takayanagi conjecture connects the entanglement entropy in the
boundary CFT to the area of open co-dimension two minimal surfaces in the bulk.
Especially in AdS(4), the latter are two-dimensional surfaces, and, thus,
solutions of a Euclidean non-linear sigma model on a symmetric target space
that can be reduc... | [
{
"created": "Mon, 12 Dec 2016 11:54:48 GMT",
"version": "v1"
}
] | 2017-12-12 | [
[
"Pastras",
"Georgios",
""
]
] | The Ryu-Takayanagi conjecture connects the entanglement entropy in the boundary CFT to the area of open co-dimension two minimal surfaces in the bulk. Especially in AdS(4), the latter are two-dimensional surfaces, and, thus, solutions of a Euclidean non-linear sigma model on a symmetric target space that can be reduced... | 7.637253 | 7.751715 | 9.241083 | 8.091683 | 8.251738 | 8.974591 | 8.730285 | 8.575538 | 8.005436 | 10.851395 | 8.02072 | 7.797108 | 8.184792 | 7.723084 | 7.854701 | 7.645928 | 7.781579 | 7.990781 | 7.87157 | 8.124862 | 7.663092 |
hep-th/0312281 | Ruben Mkrtchyan | H. Mkrtchyan and R. Mkrtchyan | 10d N=1 Massless BPS supermultiplets | LaTeX, 15 pages, 2 references added, comment to eq.(21) changed, text
improved | Mod.Phys.Lett. A19 (2004) 931-944 | 10.1142/S0217732304013817 | null | hep-th | null | We consider d=10 N=1 supersymmetry algebra with maximal number of tensor
charges Z and introduce a class of orbits of Z, invariant w.r.t. the $T_8$
subgroup of massless particles' little group $T_8\ltimes SO(8)$. For that class
of orbits we classify all possible orbits and little groups, which appear to be
semidirect... | [
{
"created": "Tue, 23 Dec 2003 22:10:02 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Jan 2004 19:36:42 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Mkrtchyan",
"H.",
""
],
[
"Mkrtchyan",
"R.",
""
]
] | We consider d=10 N=1 supersymmetry algebra with maximal number of tensor charges Z and introduce a class of orbits of Z, invariant w.r.t. the $T_8$ subgroup of massless particles' little group $T_8\ltimes SO(8)$. For that class of orbits we classify all possible orbits and little groups, which appear to be semidirect p... | 10.888207 | 10.695283 | 11.402479 | 10.379291 | 11.159424 | 11.21671 | 10.571596 | 10.823365 | 11.009087 | 12.300973 | 10.519161 | 10.54663 | 10.629652 | 10.342464 | 10.661898 | 10.416967 | 10.687456 | 10.446209 | 10.588012 | 10.825114 | 10.465916 |
hep-th/0604058 | Steven Gubser | A. Dymarsky, S. Gubser, Z. Guralnik, and J. Maldacena | Calibrated Surfaces and Supersymmetric Wilson Loops | 28 pages, 2 figures | JHEP0609:057,2006 | 10.1088/1126-6708/2006/09/057 | PUPT-2194, Brown HET-1467, ITEP-TH-12-06 | hep-th | null | We study the dual gravity description of supersymmetric Wilson loops whose
expectation value is unity. They are described by calibrated surfaces that end
on the boundary of anti de-Sitter space and are pseudo-holomorphic with respect
to an almost complex structure on an eight-dimensional slice of AdS_5 x S^5.
The reg... | [
{
"created": "Fri, 7 Apr 2006 22:17:04 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Dymarsky",
"A.",
""
],
[
"Gubser",
"S.",
""
],
[
"Guralnik",
"Z.",
""
],
[
"Maldacena",
"J.",
""
]
] | We study the dual gravity description of supersymmetric Wilson loops whose expectation value is unity. They are described by calibrated surfaces that end on the boundary of anti de-Sitter space and are pseudo-holomorphic with respect to an almost complex structure on an eight-dimensional slice of AdS_5 x S^5. The regul... | 9.647422 | 7.380255 | 9.962346 | 7.060376 | 7.352343 | 7.900472 | 7.300705 | 7.587062 | 7.714939 | 11.452481 | 7.595154 | 8.148546 | 9.376736 | 8.219458 | 8.364751 | 8.341764 | 8.573372 | 8.422136 | 8.317911 | 9.408751 | 7.674714 |
2105.08220 | Giulia Aleixo | Giulia Aleixo, Herondy Mota | Thermal Casimir effect for the scalar field in flat spacetime under a
helix boundary condition | 16 pages, new discussions and appendix added, to be published in PRD | Phys. Rev. D 104, 045012 (2021) | 10.1103/PhysRevD.104.045012 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we consider the generalized zeta function method to obtain
temperature corrections to the vacuum (Casimir) energy density, at zero
temperature, associated with quantum vacuum fluctuations of a scalar field
subjected to a helix boundary condition and whose modes propagate in
(3+1)-dimensional Euclidean sp... | [
{
"created": "Tue, 18 May 2021 01:23:28 GMT",
"version": "v1"
},
{
"created": "Thu, 20 May 2021 23:16:24 GMT",
"version": "v2"
},
{
"created": "Thu, 29 Jul 2021 15:28:01 GMT",
"version": "v3"
}
] | 2021-08-25 | [
[
"Aleixo",
"Giulia",
""
],
[
"Mota",
"Herondy",
""
]
] | In this work we consider the generalized zeta function method to obtain temperature corrections to the vacuum (Casimir) energy density, at zero temperature, associated with quantum vacuum fluctuations of a scalar field subjected to a helix boundary condition and whose modes propagate in (3+1)-dimensional Euclidean spac... | 7.407129 | 6.671955 | 7.229194 | 6.418353 | 6.859972 | 6.477876 | 6.953049 | 6.569739 | 6.636588 | 7.71082 | 6.800001 | 6.855732 | 7.0204 | 6.752492 | 6.953702 | 7.040553 | 6.700275 | 6.816683 | 6.909124 | 7.026414 | 6.910826 |
0805.4328 | Mu-In Park | Mu-in Park | Constraint Dynamics and Gravitons in Three Dimensions | Published version in JHEP | JHEP 0809:084,2008 | 10.1088/1126-6708/2008/09/084 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The complete non-linear three-dimensional Einstein gravity with gravitational
Chern-Simons term and cosmological constant are studied in dreibein
formulation. The constraints and their algebras are computed in an explicit
form. From counting the number of first and second class constraints, the
number of dynamical de... | [
{
"created": "Wed, 28 May 2008 13:40:49 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Jun 2008 06:49:11 GMT",
"version": "v2"
},
{
"created": "Tue, 5 Aug 2008 12:35:08 GMT",
"version": "v3"
},
{
"created": "Tue, 23 Sep 2008 01:51:08 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Park",
"Mu-in",
""
]
] | The complete non-linear three-dimensional Einstein gravity with gravitational Chern-Simons term and cosmological constant are studied in dreibein formulation. The constraints and their algebras are computed in an explicit form. From counting the number of first and second class constraints, the number of dynamical degr... | 10.446991 | 9.335407 | 11.606024 | 9.79809 | 10.612531 | 9.248907 | 8.578744 | 8.738122 | 9.00579 | 11.248073 | 9.098641 | 9.476613 | 9.297668 | 9.030061 | 9.574354 | 9.400176 | 9.500559 | 9.241036 | 9.392892 | 9.801036 | 9.287214 |
1404.7154 | Jan Manschot | Jan Manschot, Boris Pioline and Ashoke Sen | The Coulomb Branch Formula for Quiver Moduli Spaces | 24 pages. v2: final version; minor changes, including a new diagram | Confluentes Mathematici 9 (2017) 2, 49-69 | 10.5802/cml.41 | CERN-PH-TH-2014-074 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In recent series of works, by translating properties of multi-centered
supersymmetric black holes into the language of quiver representations, we
proposed a formula that expresses the Hodge numbers of the moduli space of
semi-stable representations of quivers with generic superpotential in terms of
a set of invariant... | [
{
"created": "Mon, 28 Apr 2014 20:03:34 GMT",
"version": "v1"
},
{
"created": "Fri, 8 Dec 2017 11:21:42 GMT",
"version": "v2"
}
] | 2018-01-22 | [
[
"Manschot",
"Jan",
""
],
[
"Pioline",
"Boris",
""
],
[
"Sen",
"Ashoke",
""
]
] | In recent series of works, by translating properties of multi-centered supersymmetric black holes into the language of quiver representations, we proposed a formula that expresses the Hodge numbers of the moduli space of semi-stable representations of quivers with generic superpotential in terms of a set of invariants ... | 8.670349 | 7.042138 | 9.937496 | 7.171639 | 8.313566 | 7.709884 | 7.590806 | 7.370451 | 7.513352 | 10.870492 | 8.050908 | 7.668606 | 8.161957 | 7.880489 | 7.67006 | 7.95524 | 7.928716 | 7.457975 | 7.684282 | 8.28356 | 7.910716 |
1109.2331 | Michael Mattes Dr. | M.Mattes and M.Sorg | Quadrupole Approximation for Para-Positronium in Relativistic
Schr\"odinger Theory | 153 pages, 9 figures and 6 tables | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The non-relativistic energy levels of para-positronium are calculated in the
quadrupole approximation of the interaction potential. This approximation
technique takes into account the anisotropy of the electrostatic
electron-positron interaction in the lowest order. The states due to different
values of the quantum n... | [
{
"created": "Sun, 11 Sep 2011 17:15:30 GMT",
"version": "v1"
}
] | 2011-09-13 | [
[
"Mattes",
"M.",
""
],
[
"Sorg",
"M.",
""
]
] | The non-relativistic energy levels of para-positronium are calculated in the quadrupole approximation of the interaction potential. This approximation technique takes into account the anisotropy of the electrostatic electron-positron interaction in the lowest order. The states due to different values of the quantum num... | 9.951834 | 10.112634 | 10.995578 | 10.136819 | 11.093191 | 11.407757 | 10.878016 | 10.446308 | 9.880439 | 10.327379 | 10.409361 | 10.373606 | 10.083647 | 10.05909 | 10.084224 | 10.277138 | 10.076826 | 10.279073 | 10.083817 | 10.105341 | 9.932828 |
1407.0801 | Hiroshi Kunitomo | Hiroshi Kunitomo | First-Order Equations of Motion for Heterotic String Field Theory | 24 pages, uses PTPTeX.cls, v2:typos | null | 10.1093/ptep/ptu125 | YITP-14-52 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the equations of motion of the full heterotic string field theory
including both the Neveu-Schwarz and the Ramond sectors. It is shown that they
can be formulated in the form of an infinite number of first-order equations
for an infinite number of independent string fields. We prove that the
conventional ... | [
{
"created": "Thu, 3 Jul 2014 07:37:18 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Aug 2014 02:07:20 GMT",
"version": "v2"
}
] | 2014-09-24 | [
[
"Kunitomo",
"Hiroshi",
""
]
] | We consider the equations of motion of the full heterotic string field theory including both the Neveu-Schwarz and the Ramond sectors. It is shown that they can be formulated in the form of an infinite number of first-order equations for an infinite number of independent string fields. We prove that the conventional eq... | 11.884091 | 10.738202 | 12.501929 | 10.418572 | 10.659103 | 11.310265 | 10.398613 | 10.256527 | 10.643171 | 13.304811 | 10.499222 | 9.962064 | 10.639383 | 9.926356 | 10.206602 | 10.47762 | 10.318274 | 10.404145 | 10.083043 | 10.721067 | 10.174888 |
2312.12512 | Jaydeep Kumar Basak | Jaydeep Kumar Basak, Debarshi Basu, Vinay Malvimat, Himanshu Parihar
and Gautam Sengupta | Holographic Reflected Entropy and Islands in Interface CFTs | 68 pages, 28 figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the reflected entropy for various mixed state configurations
in the two dimensional holographic conformal field theories sharing a common
interface (ICFTs). In the AdS$_3$/ICFT$_2$ framework, we compute the
holographic reflected entropy for the required configurations in the vacuum
state of the ICFT$_{... | [
{
"created": "Tue, 19 Dec 2023 19:00:03 GMT",
"version": "v1"
}
] | 2023-12-21 | [
[
"Basak",
"Jaydeep Kumar",
""
],
[
"Basu",
"Debarshi",
""
],
[
"Malvimat",
"Vinay",
""
],
[
"Parihar",
"Himanshu",
""
],
[
"Sengupta",
"Gautam",
""
]
] | We investigate the reflected entropy for various mixed state configurations in the two dimensional holographic conformal field theories sharing a common interface (ICFTs). In the AdS$_3$/ICFT$_2$ framework, we compute the holographic reflected entropy for the required configurations in the vacuum state of the ICFT$_{\t... | 8.261456 | 6.759748 | 9.622103 | 6.860104 | 7.025411 | 7.056241 | 7.128464 | 6.742234 | 6.687561 | 10.314083 | 7.224847 | 7.306489 | 8.858035 | 7.69591 | 7.348737 | 7.281619 | 7.310592 | 7.514669 | 7.733472 | 8.882438 | 7.547549 |
hep-th/9308003 | Martin Land | M. C. Land, N. Shnerb, and L. P. Horwitz | On Feynman's Approach to the Foundations of Gauge Theory | This is a complete re-write of our paper, using new techniques, with
a new section on non-Abelian gauge fields. (36 pages, latex, no figures) | null | null | TAUP-2076-93 | hep-th | null | In 1948, Feynman showed Dyson how the Lorentz force and Maxwell equations
could be derived from commutation relations coordinates and velocities. Several
authors noted that the derived equations are not Lorentz covariant and so are
not the standard Maxwell theory. In particular, Hojman and Shepley proved that
the exi... | [
{
"created": "Mon, 2 Aug 1993 11:40:22 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Jan 1995 07:00:19 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Land",
"M. C.",
""
],
[
"Shnerb",
"N.",
""
],
[
"Horwitz",
"L. P.",
""
]
] | In 1948, Feynman showed Dyson how the Lorentz force and Maxwell equations could be derived from commutation relations coordinates and velocities. Several authors noted that the derived equations are not Lorentz covariant and so are not the standard Maxwell theory. In particular, Hojman and Shepley proved that the exist... | 10.078784 | 11.150818 | 11.362396 | 10.480742 | 11.043302 | 10.399408 | 11.264022 | 10.906428 | 10.212008 | 11.789819 | 9.971329 | 9.807956 | 10.095889 | 9.909555 | 9.774131 | 9.652281 | 10.191648 | 10.087217 | 9.901082 | 10.057756 | 9.901108 |
hep-th/9812042 | A. Sagnotti | Fabio Riccioni, Augusto Sagnotti | Self-dual Tensors in Six-Dimensional Supergravity | 14 pages, LATEX. LATEX error corrected | null | null | null | hep-th | null | We review some properties of the field equations of six-dimensional (1,0)
supergravity coupled to tensor and vector multiplets, and in particular their
relation to covariant and consistent anomalies and a peculiar Noether identity
for the energy-momentum tensor. We also describe a lagrangian formulation for
this syst... | [
{
"created": "Fri, 4 Dec 1998 16:52:04 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Jan 1999 12:07:13 GMT",
"version": "v2"
},
{
"created": "Fri, 22 Jan 1999 12:04:56 GMT",
"version": "v3"
},
{
"created": "Mon, 25 Jan 1999 17:52:42 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Riccioni",
"Fabio",
""
],
[
"Sagnotti",
"Augusto",
""
]
] | We review some properties of the field equations of six-dimensional (1,0) supergravity coupled to tensor and vector multiplets, and in particular their relation to covariant and consistent anomalies and a peculiar Noether identity for the energy-momentum tensor. We also describe a lagrangian formulation for this system... | 11.620148 | 7.974056 | 13.93127 | 8.004679 | 8.788602 | 8.4905 | 8.337304 | 8.062817 | 7.656036 | 13.342024 | 8.795482 | 8.938804 | 10.814995 | 9.904869 | 9.25534 | 9.381095 | 8.887507 | 9.803923 | 9.186724 | 10.519084 | 9.473679 |
hep-th/0501091 | Lee Smolin | Lee Smolin | Falsifiable predictions from semiclassical quantum gravity | 9 pages | Nucl.Phys. B742 (2006) 142-157 | 10.1016/j.nuclphysb.2006.02.017 | null | hep-th astro-ph gr-qc hep-ph | null | Quantum gravity is studied in a semiclassical approximation and it is found
that to first order in the Planck length the effect of quantum gravity is to
make the low energy effective spacetime metric energy dependent. The
diffeomorphism invariance of the semiclassical theory forbids the appearance of
a preferred fram... | [
{
"created": "Wed, 12 Jan 2005 21:01:07 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Apr 2005 09:38:27 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Smolin",
"Lee",
""
]
] | Quantum gravity is studied in a semiclassical approximation and it is found that to first order in the Planck length the effect of quantum gravity is to make the low energy effective spacetime metric energy dependent. The diffeomorphism invariance of the semiclassical theory forbids the appearance of a preferred frame ... | 10.046423 | 11.446482 | 11.031573 | 10.361753 | 10.844605 | 10.701218 | 11.600715 | 10.760589 | 10.419258 | 11.753177 | 9.965427 | 10.447232 | 10.523275 | 10.315833 | 10.547415 | 10.440801 | 10.316109 | 10.256938 | 10.390232 | 10.280849 | 10.257792 |
hep-th/9608179 | Dmitri Gitman | D.M. Gitman and S.I. Zlatev | Spin Factor in Path Integral Representation for Dirac Propagator in
External Fields | 34 pages, LaTeX | Phys.Rev.D55:7701-7714,1997 | 10.1103/PhysRevD.55.7701 | IFUSP/P-1236, August/1996 | hep-th | null | We study the spin factor problem both in $3+1$ and $2+1$ dimensions which are
essentially different for spin factor construction. Doing all Grassmann
integrations in the corresponding path integral representations for Dirac
propagator we get representations with spin factor in arbitrary external field.
Thus, the prop... | [
{
"created": "Tue, 27 Aug 1996 19:19:33 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Gitman",
"D. M.",
""
],
[
"Zlatev",
"S. I.",
""
]
] | We study the spin factor problem both in $3+1$ and $2+1$ dimensions which are essentially different for spin factor construction. Doing all Grassmann integrations in the corresponding path integral representations for Dirac propagator we get representations with spin factor in arbitrary external field. Thus, the propag... | 11.740752 | 11.750231 | 12.354378 | 10.807105 | 12.349939 | 12.220576 | 11.698961 | 11.586342 | 11.231016 | 13.186337 | 11.262117 | 11.344974 | 11.757298 | 11.396632 | 11.256019 | 11.661226 | 11.762349 | 11.696283 | 11.610787 | 11.529749 | 11.198158 |
0808.2781 | Balasubramanian Ananthanarayan | B. Ananthanarayan | A note on the heat kernel coefficients for nonminimal operators | 9 pages, plain latex, accepted for publication by Journal of Physics
A | J.Phys.A41:415402,2008 | 10.1088/1751-8113/41/41/415402 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider certain results for the heat kernel of nonminimal operators. The
general expressions provided by Gusynin and Kornyak resulting from symbolic
computation programmes for n dimensions are evaluated for 4 dimensions which
are checked against results given by Barvinsky and Vilkovisky. We also check
that the re... | [
{
"created": "Wed, 20 Aug 2008 16:47:26 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Ananthanarayan",
"B.",
""
]
] | We consider certain results for the heat kernel of nonminimal operators. The general expressions provided by Gusynin and Kornyak resulting from symbolic computation programmes for n dimensions are evaluated for 4 dimensions which are checked against results given by Barvinsky and Vilkovisky. We also check that the resu... | 24.613956 | 24.39579 | 24.462887 | 20.002008 | 23.920248 | 23.883976 | 23.9335 | 22.131174 | 22.976646 | 27.397957 | 22.116041 | 21.998335 | 23.432066 | 21.552557 | 21.994184 | 22.621447 | 23.065224 | 21.213326 | 22.419544 | 24.801767 | 22.681517 |
0706.3473 | Eugene Loginov | E.K. Loginov | On a class of gauge theories | 18 pages, LaTeX, no figures | J.Math.Phys.48:073522,2007 | 10.1063/1.2749173 | null | hep-th | null | We give a framework to describe gauge theory in which a nonassociative
Moufang loop takes the place of the structure group. The structure of such
gauge theory has many formal similarities with that of Yang-Mills theory. We
extend the gauge invariance to this theory and construct an on-shell version of
N=1 supersymmet... | [
{
"created": "Sat, 23 Jun 2007 19:36:24 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Loginov",
"E. K.",
""
]
] | We give a framework to describe gauge theory in which a nonassociative Moufang loop takes the place of the structure group. The structure of such gauge theory has many formal similarities with that of Yang-Mills theory. We extend the gauge invariance to this theory and construct an on-shell version of N=1 supersymmetri... | 12.99177 | 10.120025 | 12.993415 | 10.780365 | 10.611854 | 10.851976 | 10.875852 | 10.472258 | 9.989043 | 13.212517 | 10.882017 | 10.840022 | 12.215055 | 10.95124 | 10.9391 | 11.138093 | 10.799027 | 11.246932 | 10.806212 | 12.34038 | 11.090034 |
1702.03694 | Pan Kessel | Pan Kessel | The Very Basics of Higher-Spin Theory | Contribution to the proceedings of the XII Modave Summer School in
Mathematical Physics | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | These notes are based on two lectures given at the Twelfth Modave Summer
School in Mathematical Physics 2016. The Fronsdal equation and action for both
Minkowski and (A)dS backgrounds are discussed in detail.
| [
{
"created": "Mon, 13 Feb 2017 10:04:13 GMT",
"version": "v1"
}
] | 2017-02-14 | [
[
"Kessel",
"Pan",
""
]
] | These notes are based on two lectures given at the Twelfth Modave Summer School in Mathematical Physics 2016. The Fronsdal equation and action for both Minkowski and (A)dS backgrounds are discussed in detail. | 12.225309 | 7.297487 | 9.566176 | 7.845977 | 7.633306 | 7.142117 | 8.081423 | 7.620541 | 6.98007 | 8.650525 | 7.844232 | 8.472429 | 8.191861 | 7.689384 | 7.709796 | 8.143395 | 8.052913 | 7.831079 | 8.078148 | 8.202768 | 7.43954 |
hep-th/9705066 | Igor V. Volovich | I.V.Volovich | On the Second Quantization of M(atrix) Theory | 3 pages, Latex, an explicit expression for the interaction
Hamiltonian in the Boltzmannian Fock space is given | null | null | SMI-14-97/5 | hep-th | null | The second quantization of M(atrix) theory in the free (Boltzmannian) Fock
space is considered. It provides a possible framework to the recent Susskind
proposal that U(N) supersymmetic Yang-Mills theories for all N might be
embedded in a single dynamical system. The second quantization of M(atrix)
theory can also be ... | [
{
"created": "Sun, 11 May 1997 14:46:29 GMT",
"version": "v1"
},
{
"created": "Thu, 15 May 1997 16:36:22 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Volovich",
"I. V.",
""
]
] | The second quantization of M(atrix) theory in the free (Boltzmannian) Fock space is considered. It provides a possible framework to the recent Susskind proposal that U(N) supersymmetic Yang-Mills theories for all N might be embedded in a single dynamical system. The second quantization of M(atrix) theory can also be us... | 10.882075 | 9.574988 | 11.409719 | 9.181368 | 8.957619 | 9.008319 | 9.557333 | 9.336937 | 8.823436 | 12.545238 | 9.193887 | 9.263365 | 10.467193 | 10.106256 | 9.644085 | 9.521255 | 9.371496 | 9.515786 | 9.841937 | 10.083032 | 9.826696 |
hep-th/9608079 | null | Hirosi Ooguri and Cumrun Vafa | Summing up D-Instantons | 8 pages, harvmac; a reference added, typoes corrected | Phys.Rev.Lett.77:3296-3298,1996 | 10.1103/PhysRevLett.77.3296 | HUTP-96/A036, UCB-PTH-96/36, LBNL-39220 | hep-th | null | We investigate quantum corrections to the moduli space for hypermultiplets
for type IIA near a conifold singularity. We find a unique quantum deformation
based on symmetry arguments which is consistent with a recent conjecture. The
correction can be interpreted as an infinite sum coming from multiple wrappings
of the... | [
{
"created": "Mon, 12 Aug 1996 22:17:24 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Aug 1996 23:16:28 GMT",
"version": "v2"
}
] | 2009-09-17 | [
[
"Ooguri",
"Hirosi",
""
],
[
"Vafa",
"Cumrun",
""
]
] | We investigate quantum corrections to the moduli space for hypermultiplets for type IIA near a conifold singularity. We find a unique quantum deformation based on symmetry arguments which is consistent with a recent conjecture. The correction can be interpreted as an infinite sum coming from multiple wrappings of the E... | 13.185372 | 11.39426 | 12.466364 | 10.503837 | 11.090548 | 10.083101 | 11.424497 | 9.84691 | 11.035721 | 14.10496 | 10.964129 | 11.493962 | 12.567598 | 11.034035 | 11.45919 | 11.372435 | 11.179391 | 11.257755 | 10.913277 | 12.272019 | 10.68226 |
hep-th/0703192 | Jos\'e M. Figueroa-O'Farrill | Jos\'e Figueroa-O'Farrill, Emily Hackett-Jones and George Moutsopoulos | The Killing superalgebra of ten-dimensional supergravity backgrounds | 21 pages; V2: 3 references added; V3: 1 reference added and two
imprecisions corrected; V4: small changes due to error in a separate paper | Class.Quant.Grav.24:3291-3308,2007 | 10.1088/0264-9381/24/13/010 | EMPG-07-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the Killing superalgebra of supersymmetric backgrounds of
ten-dimensional heterotic and type II supergravities and prove that it is a Lie
superalgebra. We also show that if the fraction of supersymmetry preserved by
the background is greater than 1/2, in the heterotic case, or greater than 3/4
in the typ... | [
{
"created": "Wed, 21 Mar 2007 23:12:09 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Mar 2007 17:54:15 GMT",
"version": "v2"
},
{
"created": "Wed, 9 May 2007 17:57:44 GMT",
"version": "v3"
},
{
"created": "Thu, 2 Aug 2012 12:38:26 GMT",
"version": "v4"
}
] | 2012-08-03 | [
[
"Figueroa-O'Farrill",
"José",
""
],
[
"Hackett-Jones",
"Emily",
""
],
[
"Moutsopoulos",
"George",
""
]
] | We construct the Killing superalgebra of supersymmetric backgrounds of ten-dimensional heterotic and type II supergravities and prove that it is a Lie superalgebra. We also show that if the fraction of supersymmetry preserved by the background is greater than 1/2, in the heterotic case, or greater than 3/4 in the type ... | 4.529161 | 4.224335 | 4.969487 | 4.065211 | 3.705756 | 3.860339 | 4.076438 | 3.955228 | 3.80873 | 5.071569 | 3.981674 | 4.185822 | 4.683383 | 4.151129 | 4.347457 | 4.255054 | 4.137938 | 4.107125 | 4.23695 | 4.697949 | 4.143167 |
hep-th/9309130 | Uwe Ritschel | Uwe Ritschel | Autonomous Renormalization of Phi^4 in Finite Geometry | 8 pages, Latex | Phys.Lett. B318 (1993) 617-622 | 10.1016/0370-2693(93)90463-R | null | hep-th hep-ph | null | The autonomous renormalization of the O(N)-symmetric scalar theory is based
on an infinite re-scaling of constant fields, whereas finite-momentum modes
remain finite. The natural framework for a detailed analysis of this method is
a system of finite size, where all non-constant modes can be integrated out
perturbativ... | [
{
"created": "Fri, 24 Sep 1993 13:24:06 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Ritschel",
"Uwe",
""
]
] | The autonomous renormalization of the O(N)-symmetric scalar theory is based on an infinite re-scaling of constant fields, whereas finite-momentum modes remain finite. The natural framework for a detailed analysis of this method is a system of finite size, where all non-constant modes can be integrated out perturbativel... | 16.559885 | 15.252754 | 16.871538 | 15.135921 | 16.271976 | 16.77141 | 15.212398 | 16.181658 | 15.503222 | 18.234381 | 16.957035 | 16.792645 | 15.431971 | 15.565253 | 16.502426 | 16.93265 | 16.083303 | 15.747249 | 15.718977 | 15.721703 | 15.727768 |
1611.05821 | Raphael Bousso | Raphael Bousso | Universal Limit on Communication | 4 pages, 2 figures; v2: minor changes | Phys. Rev. Lett. 119, 140501 (2017) | 10.1103/PhysRevLett.119.140501 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I derive a universal upper bound on the capacity of any communication channel
between two distant systems. The Holevo quantity, and hence the mutual
information, is at most of order $E \Delta t / \hbar$, where $E$ is the average
energy of the signal, and $\Delta t$ is the amount of time for which detectors
operate. T... | [
{
"created": "Thu, 17 Nov 2016 19:10:27 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Dec 2016 23:01:06 GMT",
"version": "v2"
}
] | 2017-10-11 | [
[
"Bousso",
"Raphael",
""
]
] | I derive a universal upper bound on the capacity of any communication channel between two distant systems. The Holevo quantity, and hence the mutual information, is at most of order $E \Delta t / \hbar$, where $E$ is the average energy of the signal, and $\Delta t$ is the amount of time for which detectors operate. The... | 9.179407 | 10.711591 | 9.896926 | 8.673254 | 10.170918 | 10.655282 | 9.504689 | 9.394391 | 9.518525 | 10.011506 | 8.863744 | 8.963793 | 8.868478 | 8.725363 | 8.623678 | 8.463201 | 8.88769 | 8.570527 | 8.578134 | 8.553858 | 8.534499 |
hep-th/0603146 | Tatsumi Aoyama | T. Aoyama, H. Kawai | Higher Order Terms of Improved Mean Field Approximation for IIB Matrix
Model and Emergence of Four-dimensional Space-time | 13 pages | Prog.Theor.Phys.116:405-415,2006 | 10.1143/PTP.116.405 | RIKEN-TH-67 | hep-th | null | The spontaneous breakdown of SO(10) symmetry of the IIB matrix model has been
studied by using the improved mean field approximation (IMFA). In this report,
the eighth-order contribution to the improved perturbative series is obtained,
which involves evaluation of 20410 planar two-particle irreducible vacuum
diagrams... | [
{
"created": "Sun, 19 Mar 2006 08:15:29 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Aoyama",
"T.",
""
],
[
"Kawai",
"H.",
""
]
] | The spontaneous breakdown of SO(10) symmetry of the IIB matrix model has been studied by using the improved mean field approximation (IMFA). In this report, the eighth-order contribution to the improved perturbative series is obtained, which involves evaluation of 20410 planar two-particle irreducible vacuum diagrams. ... | 14.855186 | 12.934297 | 15.555608 | 13.61728 | 14.151081 | 13.12876 | 13.340692 | 14.071627 | 12.947017 | 17.164562 | 13.304323 | 13.489177 | 15.335615 | 13.697003 | 13.430019 | 13.299556 | 13.065627 | 14.253407 | 13.330273 | 14.775037 | 13.719221 |
2212.00195 | Daniel S. Freed | Daniel S. Freed | Introduction to topological symmetry in QFT | 14 pages, 7 figures. v2 fixed title in announcement. v3 has redrawn
figures for publication | null | null | null | hep-th math-ph math.AT math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This brief note publicizes the quantum framework for symmetry that is
developed in our joint paper arXiv:2209.07471 with Greg Moore and Constantin
Teleman. We include additional motivation and an application to a selection
rule for line defects in 4-dimensional gauge theories.
| [
{
"created": "Thu, 1 Dec 2022 00:41:46 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Dec 2022 17:07:48 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Jul 2023 11:23:03 GMT",
"version": "v3"
}
] | 2023-07-07 | [
[
"Freed",
"Daniel S.",
""
]
] | This brief note publicizes the quantum framework for symmetry that is developed in our joint paper arXiv:2209.07471 with Greg Moore and Constantin Teleman. We include additional motivation and an application to a selection rule for line defects in 4-dimensional gauge theories. | 22.352003 | 20.157007 | 23.333698 | 20.113049 | 19.631491 | 20.73904 | 19.559431 | 20.450335 | 20.939667 | 27.488028 | 19.061689 | 20.025486 | 20.619286 | 19.578585 | 19.196701 | 20.056442 | 19.798954 | 19.83963 | 20.69335 | 21.876673 | 20.404217 |
hep-th/9506095 | null | A. Bassetto, L. Griguolo and G. Nardelli | Yang-Mills theories on the space-time $S_1 \times R$ cylinder:
equal-time quantization in light-cone gauge and Wilson loops | 21 pages, revtex, one figure included | null | null | null | hep-th | null | Pure Yang-Mills theories on the $S_1\times R$ cylinder are quantized in
light-cone gauge $A_-=0$ by means of ${\bf equal-time}$ commutation relations.
Positive and negative frequency components are excluded from the ``physical"
Hilbert space by imposing Gauss' law in a weak sense. Zero modes, related to
the winding o... | [
{
"created": "Wed, 14 Jun 1995 08:03:46 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bassetto",
"A.",
""
],
[
"Griguolo",
"L.",
""
],
[
"Nardelli",
"G.",
""
]
] | Pure Yang-Mills theories on the $S_1\times R$ cylinder are quantized in light-cone gauge $A_-=0$ by means of ${\bf equal-time}$ commutation relations. Positive and negative frequency components are excluded from the ``physical" Hilbert space by imposing Gauss' law in a weak sense. Zero modes, related to the winding on ... | 17.14394 | 14.343743 | 16.100298 | 12.706286 | 15.065863 | 14.464562 | 15.363637 | 13.424603 | 14.083032 | 16.076353 | 12.470597 | 13.15667 | 13.350023 | 13.011144 | 13.513229 | 13.659428 | 12.85113 | 13.113794 | 13.291397 | 13.729367 | 13.107021 |
1305.3919 | Csaba Csaki | B. Bellazzini, C. Csaki, J. Hubisz, J. Serra and J. Terning | A Naturally Light Dilaton and a Small Cosmological Constant | 30 pages, 3 figures | null | 10.1140/epjc/s10052-014-2790-x | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a non-supersymmetric theory with a naturally light dilaton. It is
based on a 5D holographic description of a conformal theory perturbed by a
close-to-marginal operator of dimension 4-epsilon, which develops a condensate.
As long as the dimension of the perturbing operator remains very close to
marginal (ev... | [
{
"created": "Thu, 16 May 2013 20:00:05 GMT",
"version": "v1"
}
] | 2015-06-16 | [
[
"Bellazzini",
"B.",
""
],
[
"Csaki",
"C.",
""
],
[
"Hubisz",
"J.",
""
],
[
"Serra",
"J.",
""
],
[
"Terning",
"J.",
""
]
] | We present a non-supersymmetric theory with a naturally light dilaton. It is based on a 5D holographic description of a conformal theory perturbed by a close-to-marginal operator of dimension 4-epsilon, which develops a condensate. As long as the dimension of the perturbing operator remains very close to marginal (even... | 9.2928 | 9.470799 | 9.881708 | 8.778967 | 9.711379 | 9.510622 | 9.246636 | 8.90314 | 9.400708 | 10.949091 | 9.391164 | 9.136951 | 9.386586 | 9.13648 | 9.192899 | 9.327828 | 9.341408 | 9.448509 | 9.124501 | 9.370328 | 9.257738 |
hep-th/9510238 | Valeri Dvoeglazov | Valeri V. Dvoeglazov (Zacatecas U., M\'exico) | Fermion-Fermion and Boson-Boson Amplitudes: Surprising Similarities | LaTeX file (sprocl.sty), 4pp. Presented at the IV Wigner Symp | Hadronic J.Suppl.10:359,1995 | null | EFUAZ FT-95-18 | hep-th | null | Amplitudes for boson-boson and fermion-boson interactions are calculated in
the second order of perturbation theory in the Lobachevsky space. An essential
ingredient of the used model is the Weinberg's $2(2j+1)$ component formalism
for describing a particle of spin $j$, recently developed substantially. The
boson-bos... | [
{
"created": "Tue, 31 Oct 1995 17:59:15 GMT",
"version": "v1"
}
] | 2011-04-15 | [
[
"Dvoeglazov",
"Valeri V.",
"",
"Zacatecas U., México"
]
] | Amplitudes for boson-boson and fermion-boson interactions are calculated in the second order of perturbation theory in the Lobachevsky space. An essential ingredient of the used model is the Weinberg's $2(2j+1)$ component formalism for describing a particle of spin $j$, recently developed substantially. The boson-boson... | 9.059643 | 5.995998 | 9.062078 | 7.535197 | 7.284647 | 6.354299 | 6.645806 | 7.014423 | 7.194047 | 10.575461 | 7.895173 | 8.077264 | 8.778741 | 8.099701 | 7.993383 | 7.992965 | 8.242105 | 7.999241 | 8.048709 | 8.492672 | 8.326366 |
hep-th/9304013 | Noureddine Mohammedi | Noureddine Mohammedi | Naked Singularities in Four-Dimensional String Backgrounds | 15 pages, Latex file, BONN-HE-93-11 | Phys.Rev. D48 (1993) 3784-3792 | 10.1103/PhysRevD.48.3784 | null | hep-th gr-qc | null | It is shown that gauged nonlinear sigma models can be always deformed by
terms proportional to the field strength of the gauge fields (nonminimal
gauging). These deformations can be interpreted as perturbations, by marginal
operators, of conformal coset models. When applied to the
SL(2,R)*SU(2)/[U(1)*U(1)] WZWN model... | [
{
"created": "Mon, 5 Apr 1993 10:14:14 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Mohammedi",
"Noureddine",
""
]
] | It is shown that gauged nonlinear sigma models can be always deformed by terms proportional to the field strength of the gauge fields (nonminimal gauging). These deformations can be interpreted as perturbations, by marginal operators, of conformal coset models. When applied to the SL(2,R)*SU(2)/[U(1)*U(1)] WZWN model, ... | 9.028888 | 9.376196 | 8.767738 | 7.652045 | 8.189386 | 8.281202 | 8.285204 | 7.824567 | 7.960818 | 10.85885 | 7.603452 | 8.219211 | 8.965379 | 8.026468 | 8.170286 | 8.185787 | 7.972287 | 8.034037 | 8.246482 | 9.082512 | 8.211221 |
1106.2266 | Sean Downes | Sean Downes, Bhaskar Dutta, Kuver Sinha | Catastrophic Inflation | 20 pages, 6 figures; v2: general discussion reworked for clarity,
minor terminology changes throughout. accepted to PRD | Phys.Rev.D84:063524,2011 | 10.1103/PhysRevD.84.063524 | MIFPA-11-21 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study inflection point inflation using Singularity Theory, which relates
degenerate critical points of functions to their local behavior. This approach
illuminates universal features of small-field models and gives analytic control
over parametrized families of scalar potentials near inflationary solutions.
The be... | [
{
"created": "Sat, 11 Jun 2011 22:47:40 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Sep 2011 20:34:22 GMT",
"version": "v2"
}
] | 2011-09-28 | [
[
"Downes",
"Sean",
""
],
[
"Dutta",
"Bhaskar",
""
],
[
"Sinha",
"Kuver",
""
]
] | We study inflection point inflation using Singularity Theory, which relates degenerate critical points of functions to their local behavior. This approach illuminates universal features of small-field models and gives analytic control over parametrized families of scalar potentials near inflationary solutions. The beha... | 11.32355 | 11.435648 | 11.661735 | 10.897187 | 11.125224 | 11.226882 | 11.095416 | 10.668147 | 10.987639 | 12.888101 | 10.831576 | 11.015037 | 10.875382 | 11.000977 | 10.719593 | 11.124012 | 11.127441 | 11.164433 | 10.827183 | 11.324965 | 10.666222 |
hep-th/0511270 | Anastasios Psinas | Anastasios Psinas | Quantum Cosmology Aspects Of D3 Branes and Tachyon Dynamics | 29 pages, 3 figures, REVTeX 4; v2 clarifications, comments and
references added; v3 more typos corrected, additional comments on the
minisuperspace description of unstable universes, version published in JHEP | JHEP0604:042,2006 | 10.1088/1126-6708/2006/04/042 | null | hep-th | null | We investigate aspects of quantum cosmology in relation to string cosmology
systems that are described in terms of the Dirac-Born-Infeld action. Using the
Silverstein-Tong model, we analyze the Wheeler-DeWitt equation for the rolling
scalar and gravity as well for $R\times{S^3}$ universe, by obtaining the wave
functi... | [
{
"created": "Sun, 27 Nov 2005 02:16:19 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Dec 2005 05:58:40 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Sep 2006 00:52:15 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Psinas",
"Anastasios",
""
]
] | We investigate aspects of quantum cosmology in relation to string cosmology systems that are described in terms of the Dirac-Born-Infeld action. Using the Silverstein-Tong model, we analyze the Wheeler-DeWitt equation for the rolling scalar and gravity as well for $R\times{S^3}$ universe, by obtaining the wave function... | 10.581074 | 11.00127 | 10.646609 | 10.441132 | 10.047491 | 10.824041 | 10.823432 | 10.375931 | 10.147637 | 11.205209 | 10.290068 | 9.959888 | 9.740408 | 9.742092 | 10.266403 | 10.155128 | 10.069382 | 9.866004 | 9.702128 | 9.893248 | 9.365854 |
1907.13064 | Floyd Williams | Floyd L.Williams | Exploring a cold plasma-2d black hole connection | The paper consists of 15 pages,with no figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using a resonance nonlinear Schrodinger equation as a bridge,we explore a
direct connection of cold plasma physics to two-dimensional black
holes.Namely,we compute and diagonalize a metric attached to the propagation of
magneto-acoustic waves in a cold plasma subject to a transverse magnetic
field,and we construct an... | [
{
"created": "Mon, 29 Jul 2019 17:11:42 GMT",
"version": "v1"
}
] | 2019-07-31 | [
[
"Williams",
"Floyd L.",
""
]
] | Using a resonance nonlinear Schrodinger equation as a bridge,we explore a direct connection of cold plasma physics to two-dimensional black holes.Namely,we compute and diagonalize a metric attached to the propagation of magneto-acoustic waves in a cold plasma subject to a transverse magnetic field,and we construct an e... | 17.123714 | 16.949839 | 15.28188 | 16.364086 | 18.392233 | 16.672201 | 16.856199 | 14.534618 | 16.594809 | 22.532116 | 14.922728 | 16.41836 | 17.403114 | 16.46542 | 15.830147 | 16.691357 | 16.274006 | 15.997712 | 16.332405 | 17.011816 | 15.454863 |
1705.00752 | Pietro Antonio Grassi | P. Fr\'e and P. A. Grassi | The Integral Form of D=3 Chern-Simons Theories Probing ${\mathbb
C}^n/\Gamma$ Singularities | 41 pp, no figures | null | 10.1002/prop.201700040 | ARC-17-01, YITP-17-48 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider D=3 supersymmetric Chern-Simons gauge theories both from the
point of view of their formal structure and of their applications to the
$\mathrm{AdS_4/CFT_3}$ correspondence. From the structural view-point, we use
the new formalism of integral forms in superspace that utilizes the rheonomic
Lagrangians and ... | [
{
"created": "Tue, 2 May 2017 01:08:46 GMT",
"version": "v1"
}
] | 2017-11-22 | [
[
"Fré",
"P.",
""
],
[
"Grassi",
"P. A.",
""
]
] | We consider D=3 supersymmetric Chern-Simons gauge theories both from the point of view of their formal structure and of their applications to the $\mathrm{AdS_4/CFT_3}$ correspondence. From the structural view-point, we use the new formalism of integral forms in superspace that utilizes the rheonomic Lagrangians and th... | 8.679753 | 9.287786 | 10.35413 | 9.196533 | 8.897463 | 8.783749 | 8.887232 | 8.498659 | 8.86323 | 9.986774 | 8.668582 | 8.551596 | 8.959716 | 8.637088 | 8.604116 | 8.511322 | 8.489889 | 8.475286 | 8.51228 | 8.931884 | 8.56861 |
2006.00967 | Konstantinos Pallikaris | Jos\'e Pablo Figueroa and Konstantinos Pallikaris | Quartic Horndeski, planar black holes, holographic aspects and universal
bounds | LaTeX, 35 pages, 3 figures, as published in J. High Energ. Phys.
2020, 90 (2020) | J. High Energ. Phys. 2020, 90 (2020) | 10.1007/JHEP09(2020)090 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we consider a specific shift-invariant quartic Horndeski model,
deriving new planar black hole solutions with axionic hair. We explore these
solutions in terms of their horizon structure and their thermodynamic
properties. We use the gauge/gravity dictionary to derive the DC transport
coefficients of th... | [
{
"created": "Mon, 1 Jun 2020 14:24:59 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Jun 2020 05:59:15 GMT",
"version": "v2"
},
{
"created": "Sat, 12 Sep 2020 10:52:55 GMT",
"version": "v3"
}
] | 2020-09-15 | [
[
"Figueroa",
"José Pablo",
""
],
[
"Pallikaris",
"Konstantinos",
""
]
] | In this work, we consider a specific shift-invariant quartic Horndeski model, deriving new planar black hole solutions with axionic hair. We explore these solutions in terms of their horizon structure and their thermodynamic properties. We use the gauge/gravity dictionary to derive the DC transport coefficients of the ... | 17.180168 | 15.593302 | 16.893833 | 15.402557 | 15.571784 | 15.176552 | 16.11775 | 14.567565 | 14.873344 | 15.947342 | 16.255827 | 15.24353 | 15.858263 | 14.918209 | 14.931611 | 15.013773 | 15.286488 | 15.13148 | 15.238473 | 15.569844 | 15.507462 |
hep-th/9407006 | R. Mohayaee | R. Mohayaee | Path-integral quantization of $W_\infty$ gravity | 9 pages, Imperial/TP/93-94/43, Plain TeX | Phys.Lett. B335 (1994) 388-394 | 10.1016/0370-2693(94)90369-7 | null | hep-th | null | We consider the anomalies of $W_\infty$ gravity in the context of
path-integralquantization. We derive the ghost-loop anomalies to all orders in
$\hbar$ directly from the path-integral measure by the Fujikawa method. We also
show that in the matter sector the higher-loop anomalies can be obtained by
implementation of... | [
{
"created": "Fri, 1 Jul 1994 18:39:55 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Mohayaee",
"R.",
""
]
] | We consider the anomalies of $W_\infty$ gravity in the context of path-integralquantization. We derive the ghost-loop anomalies to all orders in $\hbar$ directly from the path-integral measure by the Fujikawa method. We also show that in the matter sector the higher-loop anomalies can be obtained by implementation of t... | 9.893651 | 8.819817 | 11.341004 | 8.987305 | 9.773668 | 9.423575 | 8.775207 | 9.118899 | 8.994931 | 10.476357 | 8.765258 | 9.086653 | 10.837711 | 9.437842 | 9.568393 | 9.156434 | 8.805141 | 9.095143 | 9.748365 | 10.790259 | 9.760789 |
1712.07637 | Anxo Biasi | Anxo Biasi, Pablo Carracedo, Javier Mas, Daniele Musso and Alexandre
Serantes | Floquet Scalar Dynamics in Global AdS | 58 pages, 43 figs, several improvements, final version to appear in
JHEP | null | 10.1007/JHEP04(2018)137 | null | hep-th cond-mat.other nlin.PS quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study periodically driven scalar fields and the resulting geometries with
global AdS asymptotics. These solutions describe the strongly coupled dynamics
of dual finite-size quantum systems under a periodic driving which we interpret
as Floquet condensates. They span a continuous two-parameter space that extends
th... | [
{
"created": "Wed, 20 Dec 2017 18:47:45 GMT",
"version": "v1"
},
{
"created": "Wed, 2 May 2018 10:44:02 GMT",
"version": "v2"
}
] | 2018-05-23 | [
[
"Biasi",
"Anxo",
""
],
[
"Carracedo",
"Pablo",
""
],
[
"Mas",
"Javier",
""
],
[
"Musso",
"Daniele",
""
],
[
"Serantes",
"Alexandre",
""
]
] | We study periodically driven scalar fields and the resulting geometries with global AdS asymptotics. These solutions describe the strongly coupled dynamics of dual finite-size quantum systems under a periodic driving which we interpret as Floquet condensates. They span a continuous two-parameter space that extends the ... | 15.776851 | 18.214642 | 18.291927 | 16.08128 | 18.208992 | 19.947308 | 17.029919 | 18.05961 | 16.266224 | 17.792997 | 15.933488 | 16.042078 | 15.382553 | 15.267434 | 15.95882 | 16.093042 | 15.737469 | 15.553579 | 15.255364 | 15.617136 | 15.10847 |
hep-th/9910164 | Lubos Motl | Tom Banks, Lubos Motl | A nonsupersymmetric matrix orbifold | JHEP LaTeX, 22 pages | JHEP 0003 (2000) 027 | 10.1088/1126-6708/2000/03/027 | RU-99-24 | hep-th | null | We construct the matrix description for a twisted version of the IIA string
theory on S^1 with fermions antiperiodic around a spatial circle. The result is
a 2+1-dimensional U(N) x U(N) nonsupersymmetric Yang-Mills theory with
fermionic matter transforming in the (N,Nbar). The two U(N)'s are exchanged if
one goes aro... | [
{
"created": "Wed, 20 Oct 1999 22:46:38 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Banks",
"Tom",
""
],
[
"Motl",
"Lubos",
""
]
] | We construct the matrix description for a twisted version of the IIA string theory on S^1 with fermions antiperiodic around a spatial circle. The result is a 2+1-dimensional U(N) x U(N) nonsupersymmetric Yang-Mills theory with fermionic matter transforming in the (N,Nbar). The two U(N)'s are exchanged if one goes aroun... | 12.080234 | 11.232746 | 12.873817 | 10.718469 | 11.149215 | 10.862061 | 11.919016 | 10.479036 | 10.955637 | 15.406414 | 10.323997 | 11.308668 | 12.264251 | 10.789914 | 11.420141 | 11.033574 | 10.841394 | 10.725895 | 10.506113 | 11.993456 | 11.027575 |
0802.0710 | Michael Pawellek | Michael Pawellek | Quantum mass correction for the twisted kink | 18 pages, 2 figures;v2:references and discussion added, typos
corrected | J. Phys. A 42 045404,2009 | 10.1088/1751-8113/42/4/045404 | FAU-TP3-08/1 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an analytic result for the 1-loop quantum mass correction in
semiclassical quantization for the twisted \phi^4 kink on S^1 without explicit
knowledge of the fluctuation spectrum. For this purpose we use the contour
integral representation of the spectral zeta function. By solving the Bethe
ansatz equations... | [
{
"created": "Wed, 6 Feb 2008 09:57:02 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 2008 13:03:10 GMT",
"version": "v2"
}
] | 2012-10-02 | [
[
"Pawellek",
"Michael",
""
]
] | We present an analytic result for the 1-loop quantum mass correction in semiclassical quantization for the twisted \phi^4 kink on S^1 without explicit knowledge of the fluctuation spectrum. For this purpose we use the contour integral representation of the spectral zeta function. By solving the Bethe ansatz equations f... | 15.096613 | 11.911638 | 15.339136 | 12.674901 | 13.246614 | 13.568665 | 13.509109 | 12.63324 | 12.069317 | 14.532442 | 12.31482 | 13.105948 | 14.248536 | 12.9683 | 13.140719 | 12.527207 | 12.433786 | 12.923276 | 12.687965 | 14.580818 | 12.731626 |
hep-th/0611014 | Rafael Hernandez | Cesar Gomez, Rafael Hernandez | Integrability and non-perturbative effects in the AdS/CFT correspondence | 8 pages. Latex | Phys.Lett.B644:375-378,2007 | 10.1016/j.physletb.2006.12.007 | null | hep-th | null | We present a non-perturbative resummation of the asymptotic strong-coupling
expansion for the dressing phase factor of the AdS_5xS^5 string S-matrix. The
non-perturbative resummation provides a general form for the coefficients in
the weak-coupling expansion, in agreement with crossing symmetry and
transcendentality.... | [
{
"created": "Wed, 1 Nov 2006 15:18:48 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gomez",
"Cesar",
""
],
[
"Hernandez",
"Rafael",
""
]
] | We present a non-perturbative resummation of the asymptotic strong-coupling expansion for the dressing phase factor of the AdS_5xS^5 string S-matrix. The non-perturbative resummation provides a general form for the coefficients in the weak-coupling expansion, in agreement with crossing symmetry and transcendentality. T... | 7.165013 | 6.12369 | 7.398801 | 5.841043 | 6.37697 | 6.14023 | 6.109497 | 5.838493 | 5.70804 | 8.107882 | 6.066108 | 6.424981 | 7.463097 | 6.573721 | 6.586325 | 6.192092 | 6.242918 | 6.348562 | 6.232518 | 7.07483 | 6.112432 |
0812.0773 | S. Prem Kumar | Adi Armoni, S. Prem Kumar and Jefferson M. Ridgway | Z(N) Domain walls in hot N=4 SYM at weak and strong coupling | 29 pages, 2 figures; v2: normalization of strong-coupling tension
formula corrected, equations 5.14, 5.16 and 5.17 clarified; v3:
regularisation of eq.(3.31) corrected. Conclusions unchanged | JHEP 0901:076,2009 | 10.1088/1126-6708/2009/01/076 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the tensions of domain walls in the deconfined phase of N=4 SUSY
Yang-Mills theory on R^3 x S^1, at weak and strong coupling. We calculate the
k-wall tension at one-loop order and find that it is proportional to k(N-k)
(Casimir scaling). The two-loops analysis suggests that Casimir scaling
persists to this o... | [
{
"created": "Wed, 3 Dec 2008 19:49:49 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Dec 2008 11:24:33 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Feb 2009 10:12:01 GMT",
"version": "v3"
}
] | 2009-02-12 | [
[
"Armoni",
"Adi",
""
],
[
"Kumar",
"S. Prem",
""
],
[
"Ridgway",
"Jefferson M.",
""
]
] | We study the tensions of domain walls in the deconfined phase of N=4 SUSY Yang-Mills theory on R^3 x S^1, at weak and strong coupling. We calculate the k-wall tension at one-loop order and find that it is proportional to k(N-k) (Casimir scaling). The two-loops analysis suggests that Casimir scaling persists to this ord... | 5.463805 | 4.966142 | 6.666088 | 5.265434 | 5.391155 | 5.617269 | 5.63709 | 5.059949 | 5.206926 | 6.304662 | 5.001264 | 5.044032 | 6.079957 | 5.415954 | 5.27638 | 4.875416 | 5.150007 | 5.060252 | 5.417943 | 6.133782 | 5.062143 |
1111.5190 | Takeshi Morita | Gautam Mandal and Takeshi Morita | What is the gravity dual of the confinement/deconfinement transition in
holographic QCD? | 6 pages, 1 figure, based on the proceedings of the Seventh
International Conference `Quantum Theory and Symmetries', held in Prague 2011
and XVII European Workshop on String Theory 2011, held in Padua; v2: minor
corrections | null | 10.1088/1742-6596/343/1/012079 | TIFR/TH/11-49, CCTP-2011-39 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the gravity dual of four dimensional pure Yang-Mills theory through
D4 branes, as proposed by Witten (holographic QCD). In this holographic QCD, it
has been widely believed that the confinement phase in the pure Yang-Mills
theory corresponds to the AdS D4 soliton in gravity and the deconfinement phase
corres... | [
{
"created": "Tue, 22 Nov 2011 13:19:21 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Mar 2012 14:00:30 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Mandal",
"Gautam",
""
],
[
"Morita",
"Takeshi",
""
]
] | We study the gravity dual of four dimensional pure Yang-Mills theory through D4 branes, as proposed by Witten (holographic QCD). In this holographic QCD, it has been widely believed that the confinement phase in the pure Yang-Mills theory corresponds to the AdS D4 soliton in gravity and the deconfinement phase correspo... | 6.445996 | 6.460113 | 6.664279 | 6.268869 | 6.1481 | 5.937874 | 5.979082 | 6.118451 | 5.784853 | 6.826247 | 5.859597 | 5.971839 | 6.433164 | 6.180755 | 6.313424 | 6.172081 | 6.173999 | 6.211893 | 6.155838 | 6.353321 | 5.98179 |
hep-th/0108024 | Yu-Wen Lee | Yeong-Chuan Kao and Yu-Wen Lee | Schwinger model on a half-line | 4 pages, no figure. Final version to be published on Phys. Rev. D | Phys.Rev. D65 (2002) 067701 | 10.1103/PhysRevD.65.067701 | null | hep-th | null | We study the Schwinger model on a half-line in this paper. In particular, we
investigate the behavior of the chiral condensate near the edge of the line.
The effect of the chosen boundary condition is emphasized. The extension to the
finite temperature case is straightforward in our approach.
| [
{
"created": "Mon, 6 Aug 2001 08:30:30 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Jan 2002 07:37:24 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Kao",
"Yeong-Chuan",
""
],
[
"Lee",
"Yu-Wen",
""
]
] | We study the Schwinger model on a half-line in this paper. In particular, we investigate the behavior of the chiral condensate near the edge of the line. The effect of the chosen boundary condition is emphasized. The extension to the finite temperature case is straightforward in our approach. | 8.861971 | 7.17696 | 7.886016 | 6.835069 | 7.257715 | 6.955599 | 7.143886 | 7.114965 | 7.266734 | 8.009449 | 7.3663 | 7.202019 | 8.240006 | 7.360708 | 7.437786 | 7.872617 | 7.667895 | 7.499465 | 7.504644 | 7.764996 | 7.387209 |
hep-th/0407201 | Stepanyantz Konstantin | K.V.Stepanyantz | Investigation of the anomaly puzzle in N=1 supersymmetric
electrodynamics | LaTeX, 22 pages, 1 eps figure | Theor.Math.Phys. 142 (2005) 29-47; Teor.Mat.Fiz. 142 (2005) 37-57 | 10.1007/s11232-005-0053-6 | null | hep-th | null | Using Schwinger-Dyson equations and Ward identities in N=1 supersymmetric
electrodynamics, regularized by higher derivatives, we find, that it is
possible to calculate some contributions to the two-point Green function of the
gauge field and to the beta-function exactly to all orders of the perturbation
theory. The r... | [
{
"created": "Thu, 22 Jul 2004 18:59:25 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Stepanyantz",
"K. V.",
""
]
] | Using Schwinger-Dyson equations and Ward identities in N=1 supersymmetric electrodynamics, regularized by higher derivatives, we find, that it is possible to calculate some contributions to the two-point Green function of the gauge field and to the beta-function exactly to all orders of the perturbation theory. The res... | 8.150087 | 6.01162 | 8.110022 | 6.797515 | 6.260509 | 6.427634 | 5.890831 | 6.023296 | 6.408857 | 8.780696 | 6.72217 | 7.524676 | 8.585132 | 7.204034 | 7.346017 | 7.174146 | 7.451343 | 7.299586 | 7.295349 | 7.905195 | 7.111003 |
1309.5093 | Daniele Musso | Andrea Amoretti, Alessandro Braggio, Nicola Maggiore, Nicodemo
Magnoli, Daniele Musso | Coexistence of two vector order parameters: a holographic model for
ferromagnetic superconductivity | 45 pages, 19 figures | JHEP 1401 (2014) 054 | 10.1007/JHEP01(2014)054 | null | hep-th cond-mat.str-el cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a generalization of the standard holographic p-wave superconductor
featuring two interacting vector order parameters. Basing our argument on the
symmetry and linear response properties of the model, we propose it as a
holographic effective theory describing a strongly coupled ferromagnetic
superconductor. We... | [
{
"created": "Thu, 19 Sep 2013 20:03:28 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Oct 2013 14:20:38 GMT",
"version": "v2"
},
{
"created": "Sun, 26 Jan 2014 09:26:13 GMT",
"version": "v3"
}
] | 2014-03-12 | [
[
"Amoretti",
"Andrea",
""
],
[
"Braggio",
"Alessandro",
""
],
[
"Maggiore",
"Nicola",
""
],
[
"Magnoli",
"Nicodemo",
""
],
[
"Musso",
"Daniele",
""
]
] | We study a generalization of the standard holographic p-wave superconductor featuring two interacting vector order parameters. Basing our argument on the symmetry and linear response properties of the model, we propose it as a holographic effective theory describing a strongly coupled ferromagnetic superconductor. We s... | 13.889237 | 13.562277 | 14.323817 | 12.013255 | 13.793626 | 13.879684 | 14.026108 | 13.206612 | 13.809983 | 14.474395 | 11.826509 | 12.713947 | 13.530973 | 12.480034 | 12.762893 | 12.699899 | 12.908803 | 13.295139 | 12.631162 | 13.446173 | 12.481966 |
1011.3533 | Christoph Uhlemann | Thorsten Ohl and Christoph F. Uhlemann | The Boundary Multiplet of N=4 SU(2)xU(1) Gauged Supergravity on
Asymptotically-AdS_5 | 23 pages; to appear in JHEP | JHEP 1106:086,2011 | 10.1007/JHEP06(2011)086 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider N=4 SU(2)xU(1) gauged supergravity on asymptotically-AdS_5
backgrounds. By a near-boundary analysis we determine the boundary-dominant
components of the bulk fields from their partially gauge-fixed field equations.
Subdominant components are projected out in the boundary limit and we find a
reduced set of... | [
{
"created": "Mon, 15 Nov 2010 21:53:42 GMT",
"version": "v1"
},
{
"created": "Mon, 6 Jun 2011 20:25:48 GMT",
"version": "v2"
}
] | 2011-06-24 | [
[
"Ohl",
"Thorsten",
""
],
[
"Uhlemann",
"Christoph F.",
""
]
] | We consider N=4 SU(2)xU(1) gauged supergravity on asymptotically-AdS_5 backgrounds. By a near-boundary analysis we determine the boundary-dominant components of the bulk fields from their partially gauge-fixed field equations. Subdominant components are projected out in the boundary limit and we find a reduced set of b... | 6.473196 | 6.297112 | 7.037222 | 6.242899 | 6.907864 | 6.463828 | 6.061219 | 6.29778 | 6.320462 | 7.810452 | 6.445203 | 6.522291 | 6.390521 | 6.263713 | 6.528523 | 6.281642 | 6.320564 | 6.448795 | 6.227447 | 6.416539 | 6.181567 |
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