id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9610076 | Joseph A. Minahan | Joseph A. Minahan and Dennis Nemeschansky | Superconformal Fixed Points with E_n Global Symmetry | 23 pages, harvmac (b), Mathematica file available at
http://physics.usc.edu/~minahan/Math/e8.ma | Nucl.Phys. B489 (1997) 24-46 | 10.1016/S0550-3213(97)00039-4 | USC-96/23 | hep-th | null | We obtain the elliptic curve and the Seiberg-Witten differential for an $N=2$
superconformal field theory which has an $E_8$ global symmetry at the strong
coupling point $\tau=e^{\pi i/3}$. The differential has 120 poles corresponding
to half the charged states in the fundamental representation of $E_8$, with the
oth... | [
{
"created": "Thu, 10 Oct 1996 20:47:54 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Minahan",
"Joseph A.",
""
],
[
"Nemeschansky",
"Dennis",
""
]
] | We obtain the elliptic curve and the Seiberg-Witten differential for an $N=2$ superconformal field theory which has an $E_8$ global symmetry at the strong coupling point $\tau=e^{\pi i/3}$. The differential has 120 poles corresponding to half the charged states in the fundamental representation of $E_8$, with the other... | 8.268167 | 7.279954 | 8.964299 | 7.706451 | 8.972247 | 6.971159 | 7.842453 | 7.414679 | 7.199699 | 9.376898 | 7.638866 | 7.619598 | 8.27332 | 7.715945 | 7.848476 | 7.777519 | 8.051957 | 7.811074 | 7.841481 | 8.037295 | 7.526601 |
1504.00206 | Samuel Abreu | Samuel Abreu, Ruth Britto, Hanna Gr\"onqvist | Cuts and coproducts of massive triangle diagrams | 60 pages | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Relations between multiple unitarity cuts and coproducts of Feynman integrals
are extended to allow for internal masses. These masses introduce new branch
cuts, whose discontinuities can be derived by placing single propagators on
shell and identified as particular entries of the coproduct. First entries of
the copro... | [
{
"created": "Wed, 1 Apr 2015 12:50:28 GMT",
"version": "v1"
}
] | 2015-04-02 | [
[
"Abreu",
"Samuel",
""
],
[
"Britto",
"Ruth",
""
],
[
"Grönqvist",
"Hanna",
""
]
] | Relations between multiple unitarity cuts and coproducts of Feynman integrals are extended to allow for internal masses. These masses introduce new branch cuts, whose discontinuities can be derived by placing single propagators on shell and identified as particular entries of the coproduct. First entries of the coprodu... | 16.010963 | 15.122409 | 15.859893 | 14.84746 | 16.275066 | 14.867505 | 15.788184 | 14.880633 | 15.076298 | 18.438461 | 15.288251 | 15.555089 | 15.342178 | 14.998825 | 15.192669 | 14.932216 | 14.854906 | 14.756635 | 14.838428 | 15.527454 | 14.822984 |
2308.08199 | Lance Dixon | Lance J. Dixon and Yu-Ting Liu | An Eight Loop Amplitude via Antipodal Duality | 50 pages, 3 figures, 6 tables, 8 loops | null | null | SLAC-PUB-17693 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the six-particle maximally-helicity-violating (MHV) amplitude in
planar ${\cal N}=4$ super-Yang-Mills theory at eight loops, using antipodal
duality and the recently computed eight-loop three-point form factor for the
chiral stress energy tensor multiplet. Antipodal duality maps the form factor
symbol to t... | [
{
"created": "Wed, 16 Aug 2023 07:58:24 GMT",
"version": "v1"
}
] | 2023-08-17 | [
[
"Dixon",
"Lance J.",
""
],
[
"Liu",
"Yu-Ting",
""
]
] | We compute the six-particle maximally-helicity-violating (MHV) amplitude in planar ${\cal N}=4$ super-Yang-Mills theory at eight loops, using antipodal duality and the recently computed eight-loop three-point form factor for the chiral stress energy tensor multiplet. Antipodal duality maps the form factor symbol to the... | 8.643946 | 7.520315 | 9.766406 | 7.859738 | 7.447501 | 7.878252 | 8.282278 | 7.187491 | 7.827569 | 11.469902 | 7.631539 | 7.97269 | 8.529831 | 8.050076 | 8.346666 | 8.126539 | 8.37972 | 8.254707 | 7.642336 | 8.555203 | 7.991102 |
1703.08186 | Christoph Uhlemann | Eric D'Hoker, Michael Gutperle, Christoph F. Uhlemann | Warped $AdS_6\times S^2$ in Type IIB supergravity II: Global solutions
and five-brane webs | 58 pages, 9 figures; v2: minor corrections; v3: integration constant
c_6 fixed | null | 10.1007/JHEP05(2017)131 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the construction of holographic duals to five-dimensional
superconformal quantum field theories, we obtain global solutions to Type IIB
supergravity invariant under the superalgebra $F(4)$ on a space-time of the
form $AdS_6 \times S^2$ warped over a two-dimensional Riemann surface $\Sigma$.
In earlier wo... | [
{
"created": "Thu, 23 Mar 2017 18:00:10 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Apr 2017 16:44:59 GMT",
"version": "v2"
},
{
"created": "Mon, 12 Feb 2018 17:39:49 GMT",
"version": "v3"
}
] | 2018-02-13 | [
[
"D'Hoker",
"Eric",
""
],
[
"Gutperle",
"Michael",
""
],
[
"Uhlemann",
"Christoph F.",
""
]
] | Motivated by the construction of holographic duals to five-dimensional superconformal quantum field theories, we obtain global solutions to Type IIB supergravity invariant under the superalgebra $F(4)$ on a space-time of the form $AdS_6 \times S^2$ warped over a two-dimensional Riemann surface $\Sigma$. In earlier work... | 5.872914 | 5.253062 | 6.475163 | 5.255138 | 5.73243 | 5.929187 | 5.633525 | 5.511832 | 5.207993 | 6.510838 | 5.572482 | 5.664567 | 6.014654 | 5.574769 | 5.906208 | 5.809133 | 5.696252 | 5.583955 | 5.708549 | 6.069183 | 5.639496 |
hep-th/0604200 | Fabricio Augusto Barone Rangel | R.M. Cavalcanti, C. Farina, F.A. Barone | Radiative Corrections to Casimir Effect in the $\lambda\phi^{4}$ Model | 24 latex pages | null | null | null | hep-th | null | We calculate radiative corrections to the Casimir effect for the massive
complex scalar field with the $\lambda\phi^{4}$ self-interaction in $d+1$
dimensions. We consider the field submitted to four types of boundary
conditions on two parallel planes, namely: (i) quasi-periodic boundary
conditions, which interpolates... | [
{
"created": "Thu, 27 Apr 2006 04:37:17 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Cavalcanti",
"R. M.",
""
],
[
"Farina",
"C.",
""
],
[
"Barone",
"F. A.",
""
]
] | We calculate radiative corrections to the Casimir effect for the massive complex scalar field with the $\lambda\phi^{4}$ self-interaction in $d+1$ dimensions. We consider the field submitted to four types of boundary conditions on two parallel planes, namely: (i) quasi-periodic boundary conditions, which interpolates c... | 4.860985 | 3.995237 | 4.984692 | 4.112294 | 4.081766 | 4.167326 | 4.211424 | 4.281567 | 4.064593 | 5.344988 | 4.056956 | 4.357377 | 4.63547 | 4.477047 | 4.457204 | 4.532069 | 4.510271 | 4.402569 | 4.451294 | 4.806309 | 4.36914 |
1711.09913 | Yuya Kusuki | Yuya Kusuki, Tadashi Takayanagi | Renyi Entropy for Local Quenches in 2D CFTs from Numerical Conformal
Blocks | 24 pages, 8 figures | null | 10.1007/JHEP01(2018)115 | YITP-17-126, IPMU17-0163 | hep-th cond-mat.stat-mech cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the time evolution of Renyi entanglement entropy for locally excited
states in two dimensional large central charge CFTs. It generically shows a
logarithmical growth and we compute the coefficient of $\log t$ term. Our
analysis covers the entire parameter regions with respect to the replica number
$n$ and th... | [
{
"created": "Mon, 27 Nov 2017 19:00:04 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Dec 2017 12:22:21 GMT",
"version": "v2"
},
{
"created": "Mon, 15 Jan 2018 04:29:46 GMT",
"version": "v3"
}
] | 2018-03-14 | [
[
"Kusuki",
"Yuya",
""
],
[
"Takayanagi",
"Tadashi",
""
]
] | We study the time evolution of Renyi entanglement entropy for locally excited states in two dimensional large central charge CFTs. It generically shows a logarithmical growth and we compute the coefficient of $\log t$ term. Our analysis covers the entire parameter regions with respect to the replica number $n$ and the ... | 7.651137 | 7.332397 | 8.383796 | 6.970672 | 7.784748 | 7.82222 | 7.573278 | 7.317955 | 7.611623 | 8.74339 | 7.360428 | 7.357103 | 7.464139 | 7.234399 | 7.485955 | 7.4461 | 7.518231 | 7.390215 | 7.722606 | 7.666615 | 7.225854 |
2007.09224 | Giorgio Torrieri | Giorgio Torrieri | Fluctuating Relativistic hydrodynamics from Crooks theorem | Small typos fixed in accordance to proofs | null | 10.1007/JHEP02(2021)175 | null | hep-th hep-lat hep-ph nucl-th physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the Crooks fluctuation theorem together with Zubarev hydrodynamics to
develop a bottom-up theory of hydrodynamic fluctuations. We also use
thermodynamic uncertainity relations to estimate bottom-up limits to
dissipative transport coefficients.
| [
{
"created": "Fri, 17 Jul 2020 20:56:44 GMT",
"version": "v1"
},
{
"created": "Sat, 16 Jan 2021 01:38:06 GMT",
"version": "v2"
},
{
"created": "Sat, 20 Feb 2021 01:40:18 GMT",
"version": "v3"
}
] | 2021-03-17 | [
[
"Torrieri",
"Giorgio",
""
]
] | We use the Crooks fluctuation theorem together with Zubarev hydrodynamics to develop a bottom-up theory of hydrodynamic fluctuations. We also use thermodynamic uncertainity relations to estimate bottom-up limits to dissipative transport coefficients. | 20.329054 | 24.128874 | 20.781414 | 17.935183 | 19.356594 | 20.585489 | 20.974718 | 18.975042 | 19.39184 | 22.478785 | 18.168104 | 17.954033 | 19.642784 | 18.725096 | 19.084238 | 17.506132 | 16.603207 | 20.170122 | 17.556231 | 18.230999 | 18.342957 |
hep-th/0405239 | John F. Donoghue | Barry R. Holstein and John F. Donoghue | Classical Physics and Quantum Loops | 15 pages, 3 figures | Phys.Rev.Lett. 93 (2004) 201602 | 10.1103/PhysRevLett.93.201602 | null | hep-th hep-ph nucl-th | null | The standard picture of the loop expansion associates a factor of h-bar with
each loop, suggesting that the tree diagrams are to be associated with
classical physics, while loop effects are quantum mechanical in nature. We
discuss examples wherein classical effects arise from loop contributions and
display the relati... | [
{
"created": "Wed, 26 May 2004 15:26:41 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Holstein",
"Barry R.",
""
],
[
"Donoghue",
"John F.",
""
]
] | The standard picture of the loop expansion associates a factor of h-bar with each loop, suggesting that the tree diagrams are to be associated with classical physics, while loop effects are quantum mechanical in nature. We discuss examples wherein classical effects arise from loop contributions and display the relation... | 20.68379 | 17.150984 | 15.392143 | 15.055116 | 14.991537 | 13.287275 | 14.456792 | 17.122873 | 15.512409 | 15.66849 | 16.608025 | 16.250456 | 15.157242 | 15.312675 | 15.218366 | 15.922418 | 15.250703 | 15.587446 | 15.579073 | 15.947181 | 16.188873 |
hep-th/9501113 | null | I. Bandos, P. Pasti, D. Sorokin, M. Tonin and D. Volkov | SUPERSTRINGS AND SUPERMEMBRANES IN THE DOUBLY SUPERSYMMETRIC GEOMETRICAL
APPROACH | 45 pages, LaTeX, 3 appendicies | Nucl.Phys.B446:79-118,1995 | 10.1016/0550-3213(95)00267-V | DFPD 95/TH/02 | hep-th | null | We perform a generalization of the geometrical approach to describing
extended objects for studying the doubly supersymmetric twistor--like
formulation of super--p--branes. Some basic features of embedding world
supersurface into target superspace specified by a geometrodynamical condition
are considered. It is shown... | [
{
"created": "Tue, 24 Jan 1995 15:36:39 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Bandos",
"I.",
""
],
[
"Pasti",
"P.",
""
],
[
"Sorokin",
"D.",
""
],
[
"Tonin",
"M.",
""
],
[
"Volkov",
"D.",
""
]
] | We perform a generalization of the geometrical approach to describing extended objects for studying the doubly supersymmetric twistor--like formulation of super--p--branes. Some basic features of embedding world supersurface into target superspace specified by a geometrodynamical condition are considered. It is shown t... | 10.519731 | 10.449175 | 12.473321 | 9.598645 | 10.130147 | 10.045034 | 11.187007 | 9.607202 | 9.582066 | 13.483104 | 10.094929 | 9.892431 | 10.989268 | 10.133784 | 9.964967 | 9.857422 | 9.815961 | 10.171322 | 9.931622 | 10.486574 | 10.158983 |
hep-th/9712186 | Volker Schomerus | A. Recknagel and V. Schomerus | D-branes in Gepner models | 40 pages, some corrections, references added | Nucl.Phys. B531 (1998) 185-225 | 10.1016/S0550-3213(98)00468-4 | IHES/P/97/91, DESY 97-253 | hep-th | null | We discuss D-branes from a conformal field theory point of view. In this
approach, branes are described by boundary states providing sources for closed
string modes, independently of classical notions. The boundary states must
satisfy constraints which fall into two classes: The first consists of gluing
conditions be... | [
{
"created": "Thu, 18 Dec 1997 16:59:58 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Feb 1998 20:23:32 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Recknagel",
"A.",
""
],
[
"Schomerus",
"V.",
""
]
] | We discuss D-branes from a conformal field theory point of view. In this approach, branes are described by boundary states providing sources for closed string modes, independently of classical notions. The boundary states must satisfy constraints which fall into two classes: The first consists of gluing conditions betw... | 12.472708 | 11.671322 | 14.664933 | 11.856297 | 12.42684 | 11.756612 | 12.604692 | 11.968813 | 11.836388 | 15.654847 | 11.452998 | 11.545899 | 12.406285 | 11.643076 | 11.848357 | 11.385017 | 11.475652 | 11.600693 | 11.495231 | 12.390079 | 11.523072 |
2208.14032 | So Matsuura | So Matsuura and Kazutoshi Ohta | Graph Zeta Functions and Wilson Loops in Kazakov-Migdal Model | 32 pages, 3 figures, typos corrected | null | null | null | hep-th hep-lat math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | In this paper, we consider an extended Kazakov-Migdal model defined on an
arbitrary graph. The partition function of the model, which is expressed as the
summation of all Wilson loops on the graph, turns out to be represented by the
Bartholdi zeta function weighted by unitary matrices on the edges of the graph.
The p... | [
{
"created": "Tue, 30 Aug 2022 07:27:15 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Sep 2022 07:05:26 GMT",
"version": "v2"
},
{
"created": "Tue, 1 Nov 2022 01:05:47 GMT",
"version": "v3"
}
] | 2022-11-02 | [
[
"Matsuura",
"So",
""
],
[
"Ohta",
"Kazutoshi",
""
]
] | In this paper, we consider an extended Kazakov-Migdal model defined on an arbitrary graph. The partition function of the model, which is expressed as the summation of all Wilson loops on the graph, turns out to be represented by the Bartholdi zeta function weighted by unitary matrices on the edges of the graph. The par... | 7.961257 | 7.673857 | 8.870475 | 7.751505 | 7.748385 | 7.943188 | 7.624984 | 7.546016 | 7.623361 | 9.533012 | 7.663856 | 7.459534 | 7.990671 | 7.349174 | 7.418537 | 7.566155 | 7.479153 | 7.454586 | 7.358677 | 8.002927 | 7.469457 |
2209.10454 | Venkatesa Chandrasekaran | Venkatesa Chandrasekaran, Geoff Penington, Edward Witten | Large N algebras and generalized entropy | 57 pages + appendices | null | 10.1007/JHEP04(2023)009 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a Type II$_\infty$ von Neumann algebra that describes the large
$N$ physics of single-trace operators in AdS/CFT in the microcanonical
ensemble, where there is no need to include perturbative $1/N$ corrections.
Using only the extrapolate dictionary, we show that the entropy of
semiclassical states on thi... | [
{
"created": "Wed, 21 Sep 2022 15:58:21 GMT",
"version": "v1"
}
] | 2023-04-19 | [
[
"Chandrasekaran",
"Venkatesa",
""
],
[
"Penington",
"Geoff",
""
],
[
"Witten",
"Edward",
""
]
] | We construct a Type II$_\infty$ von Neumann algebra that describes the large $N$ physics of single-trace operators in AdS/CFT in the microcanonical ensemble, where there is no need to include perturbative $1/N$ corrections. Using only the extrapolate dictionary, we show that the entropy of semiclassical states on this ... | 9.238843 | 9.560656 | 10.83128 | 8.888592 | 9.437262 | 9.01238 | 9.151297 | 9.624771 | 8.828795 | 12.005815 | 8.610963 | 8.973448 | 9.956497 | 9.035555 | 9.02506 | 9.02339 | 9.026482 | 9.392861 | 9.150982 | 9.978936 | 9.253555 |
hep-th/9604156 | null | Gilad Lifschytz (Brandeis University) | Comparing D-branes to Black-branes | 14 pages, Latex, final version to appear in Phys. Lett. B | Phys.Lett. B388 (1996) 720-726 | 10.1016/S0370-2693(96)01218-X | BRX-TH-394 | hep-th | null | We calculate the potential between two different stationary D-branes and the
velocity dependent potential between two different moving D-branes. We identify
configurations with some unbroken supersymmetry, using a zero force condition.
The potentials are compared with an eleven dimensional calculation of the
scatteri... | [
{
"created": "Wed, 24 Apr 1996 17:15:54 GMT",
"version": "v1"
},
{
"created": "Tue, 7 May 1996 16:18:06 GMT",
"version": "v2"
},
{
"created": "Fri, 11 Oct 1996 18:10:43 GMT",
"version": "v3"
}
] | 2016-09-06 | [
[
"Lifschytz",
"Gilad",
"",
"Brandeis University"
]
] | We calculate the potential between two different stationary D-branes and the velocity dependent potential between two different moving D-branes. We identify configurations with some unbroken supersymmetry, using a zero force condition. The potentials are compared with an eleven dimensional calculation of the scattering... | 11.979156 | 10.087182 | 12.69739 | 10.899364 | 11.484432 | 10.105838 | 11.011995 | 10.618851 | 10.568146 | 14.344626 | 10.735568 | 11.296734 | 11.828675 | 11.452708 | 12.192144 | 11.049514 | 11.167175 | 11.204372 | 11.75682 | 11.743698 | 11.268784 |
1003.0795 | Takahisa Igata | Takahisa Igata and Hideki Ishihara | Toroidal Spiral Strings in Higher-dimensional Spacetime | 4 pages, 2 figures. Proceedings of 19th Workshop in General
Relativity and Gravitation in Japan (JGRG19) | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report on our progress in research of separability of the Nambu-Goto
equation for test strings with a symmetric configuration in a shape of toroidal
spiral in a five-dimensional Kerr-AdS black hole. In particular, for a Hopf
loop string which is a special class of the toroidal spirals, we show the
complete separat... | [
{
"created": "Wed, 3 Mar 2010 13:19:29 GMT",
"version": "v1"
}
] | 2010-03-04 | [
[
"Igata",
"Takahisa",
""
],
[
"Ishihara",
"Hideki",
""
]
] | We report on our progress in research of separability of the Nambu-Goto equation for test strings with a symmetric configuration in a shape of toroidal spiral in a five-dimensional Kerr-AdS black hole. In particular, for a Hopf loop string which is a special class of the toroidal spirals, we show the complete separatio... | 13.006858 | 10.468768 | 11.876142 | 10.130673 | 10.425155 | 10.347452 | 10.721809 | 10.484021 | 10.989703 | 13.463226 | 9.864573 | 10.793131 | 11.674405 | 10.749012 | 10.555847 | 10.888607 | 10.338491 | 10.845843 | 10.609599 | 11.570091 | 11.032485 |
0902.1552 | Carlos Mafra | Carlos R. Mafra | Superstring Scattering Amplitudes with the Pure Spinor Formalism | Ph.D Thesis from Sept. 2008, 108 pages, v2,v3: added references | null | null | IFT-T.007/08 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This thesis discusses how the pure spinor formalism can be used to
efficiently compute superstring scattering amplitudes. We emphasize the pure
spinor superspace form of the kinematic factors, where the simplifying features
of this language have allowed an explicit relation among the massless
four-point amplitudes at... | [
{
"created": "Tue, 10 Feb 2009 19:18:24 GMT",
"version": "v1"
},
{
"created": "Sun, 15 Feb 2009 19:22:08 GMT",
"version": "v2"
},
{
"created": "Thu, 26 Mar 2009 16:16:13 GMT",
"version": "v3"
}
] | 2009-03-26 | [
[
"Mafra",
"Carlos R.",
""
]
] | This thesis discusses how the pure spinor formalism can be used to efficiently compute superstring scattering amplitudes. We emphasize the pure spinor superspace form of the kinematic factors, where the simplifying features of this language have allowed an explicit relation among the massless four-point amplitudes at t... | 9.070177 | 8.529589 | 9.200944 | 8.647209 | 9.286092 | 9.509801 | 8.942528 | 8.759508 | 8.523515 | 9.57458 | 8.244579 | 8.732786 | 8.900558 | 8.72364 | 8.793671 | 8.816192 | 8.736326 | 8.806887 | 8.817419 | 8.966003 | 8.759414 |
hep-th/0603232 | Olaf Lechtenfeld | Olaf Lechtenfeld, Alexander D. Popov, Richard J. Szabo | Rank Two Quiver Gauge Theory, Graded Connections and Noncommutative
Vortices | 1+39 pages | JHEP 0609:054,2006 | 10.1088/1126-6708/2006/09/054 | null | hep-th | null | We consider equivariant dimensional reduction of Yang-Mills theory on K"ahler
manifolds of the form M times CP^1 times CP^1. This induces a rank two quiver
gauge theory on M which can be formulated as a Yang-Mills theory of graded
connections on M. The reduction of the Yang-Mills equations on M times CP^1
times CP^1 ... | [
{
"created": "Wed, 29 Mar 2006 19:26:00 GMT",
"version": "v1"
}
] | 2010-02-03 | [
[
"Lechtenfeld",
"Olaf",
""
],
[
"Popov",
"Alexander D.",
""
],
[
"Szabo",
"Richard J.",
""
]
] | We consider equivariant dimensional reduction of Yang-Mills theory on K"ahler manifolds of the form M times CP^1 times CP^1. This induces a rank two quiver gauge theory on M which can be formulated as a Yang-Mills theory of graded connections on M. The reduction of the Yang-Mills equations on M times CP^1 times CP^1 in... | 8.55125 | 8.146995 | 9.532078 | 7.681249 | 7.404383 | 7.553639 | 8.116521 | 7.254202 | 7.848693 | 11.082873 | 7.545937 | 7.954127 | 8.624145 | 8.118192 | 8.529386 | 8.34798 | 8.41862 | 8.340508 | 8.146536 | 9.023527 | 8.226106 |
hep-th/9209031 | null | J.E.Nelson and T.Regge | Invariants of 2+1 Quantum Gravity | 10 pages, plain TEX, no figures, DFTT 46/92 | Commun.Math.Phys. 155 (1993) 561-568 | 10.1007/BF02096728 | null | hep-th gr-qc | null | In [1,2] we established and discussed the algebra of observables for 2+1
gravity at both the classical and quantum level. Here our treatment broadens
and extends previous results to any genus $g$ with a systematic discussion of
the centre of the algebra. The reduction of the number of independent
observables to $6g-6... | [
{
"created": "Thu, 10 Sep 1992 18:42:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Nelson",
"J. E.",
""
],
[
"Regge",
"T.",
""
]
] | In [1,2] we established and discussed the algebra of observables for 2+1 gravity at both the classical and quantum level. Here our treatment broadens and extends previous results to any genus $g$ with a systematic discussion of the centre of the algebra. The reduction of the number of independent observables to $6g-6 (... | 11.904146 | 10.778124 | 9.53863 | 10.098195 | 10.160459 | 10.957638 | 10.174237 | 9.012076 | 10.167686 | 11.287806 | 10.397534 | 10.277655 | 9.884698 | 9.558645 | 10.020334 | 9.57621 | 9.882215 | 9.702346 | 9.79599 | 10.168393 | 9.837672 |
0906.3898 | V. Didenko | V.E. Didenko and M.A. Vasiliev | Static BPS black hole in 4d higher-spin gauge theory | 16 pages, no figures, A section with the analysis of global
symmetries is added. It is shown that the obtained solution is static and
supersymmetric. The title is changed correspondingly. Clarifications and
references added. Typos related to reality conditions fixed | Phys.Lett.B682:305-315,2009 | 10.1016/j.physletb.2009.11.023 | FIAN/TD/10-09 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find exact spherically symmetric solution of 4d nonlinear bosonic
higher-spin gauge theory, that preserves a quarter of supersymmetries of N=2
supersymmetric 4d higher-spin gauge theory. In the weak field regime it
describes $AdS_4$ Schwarzschild black hole in the spin two sector along with
non-zero massless field... | [
{
"created": "Sun, 21 Jun 2009 21:05:13 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Sep 2009 11:44:43 GMT",
"version": "v2"
},
{
"created": "Fri, 13 Dec 2013 21:57:17 GMT",
"version": "v3"
}
] | 2013-12-17 | [
[
"Didenko",
"V. E.",
""
],
[
"Vasiliev",
"M. A.",
""
]
] | We find exact spherically symmetric solution of 4d nonlinear bosonic higher-spin gauge theory, that preserves a quarter of supersymmetries of N=2 supersymmetric 4d higher-spin gauge theory. In the weak field regime it describes $AdS_4$ Schwarzschild black hole in the spin two sector along with non-zero massless fields ... | 12.621995 | 10.340404 | 12.587955 | 9.879136 | 10.638144 | 10.650073 | 9.863708 | 10.14832 | 8.801734 | 14.64049 | 8.853519 | 9.82337 | 11.092105 | 9.63083 | 9.514731 | 9.444751 | 9.275647 | 9.714831 | 9.565656 | 10.832767 | 8.920222 |
hep-th/9610055 | Manfred Requardt | Manfred Requardt | Emergence of Space-Time on the Planck Scale described as an Unfolding
Phase Transition within the Scheme of Dynamical Cellular Networks and Random
Graphs | 36 pages, Latex | null | null | Re-96-03 | hep-th gr-qc | null | As in an earlier paper we start from the hypothesis that physics on the
Planck scale should be described by means of concepts taken from ``discrete
mathematics''. This goal is realized by developing a scheme being based on the
dynamical evolution of a particular class of ``cellular networks'' being
capable of perform... | [
{
"created": "Wed, 9 Oct 1996 09:22:15 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Requardt",
"Manfred",
""
]
] | As in an earlier paper we start from the hypothesis that physics on the Planck scale should be described by means of concepts taken from ``discrete mathematics''. This goal is realized by developing a scheme being based on the dynamical evolution of a particular class of ``cellular networks'' being capable of performin... | 16.724636 | 20.154936 | 17.114172 | 16.830132 | 18.443485 | 18.500391 | 19.706661 | 17.363716 | 16.701839 | 18.854675 | 17.717499 | 16.692242 | 16.642668 | 16.36231 | 16.64356 | 16.853397 | 16.781662 | 16.227903 | 16.292707 | 16.580887 | 16.564327 |
hep-th/9605227 | Jan Ambjorn | J. Ambjorn, A. Sedrakyan | The measure in three dimensional Nambu-Goto string theory | 8 pages, Latex | Phys.Lett. B386 (1996) 99-105 | 10.1016/0370-2693(96)00904-5 | NBI-HE-96-21 | hep-th | null | We show that the measure of the three dimensional Nambu-Goto string theory
has a simple decomposition as a measure on two parameter group of induced
area-preserving transformations of the immersed surface and a trivial measure
for the area of the surface.
| [
{
"created": "Fri, 31 May 1996 14:02:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ambjorn",
"J.",
""
],
[
"Sedrakyan",
"A.",
""
]
] | We show that the measure of the three dimensional Nambu-Goto string theory has a simple decomposition as a measure on two parameter group of induced area-preserving transformations of the immersed surface and a trivial measure for the area of the surface. | 22.018326 | 15.485161 | 19.838272 | 14.737009 | 17.615196 | 19.298317 | 14.803873 | 18.593649 | 13.999958 | 21.221479 | 14.995371 | 16.499018 | 18.509977 | 16.395296 | 16.096571 | 17.03826 | 16.635445 | 16.850525 | 15.788486 | 15.879548 | 16.476105 |
2112.11614 | Edward Witten | Edward Witten | Why Does Quantum Field Theory In Curved Spacetime Make Sense? And What
Happens To The Algebra of Observables In The Thermodynamic Limit? | 43 pp, minor corrections in v. 5 | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article aims to explain some of the basic facts about the questions
raised in the title, without the technical details that are available in the
literature. We provide a gentle introduction to some rather classical results
about quantum field theory in curved spacetime and about the thermodynamic
limit of quantu... | [
{
"created": "Wed, 22 Dec 2021 01:39:20 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Jan 2022 23:24:44 GMT",
"version": "v2"
},
{
"created": "Wed, 2 Feb 2022 17:11:17 GMT",
"version": "v3"
},
{
"created": "Mon, 11 Jul 2022 19:35:07 GMT",
"version": "v4"
},
{
"cre... | 2022-07-26 | [
[
"Witten",
"Edward",
""
]
] | This article aims to explain some of the basic facts about the questions raised in the title, without the technical details that are available in the literature. We provide a gentle introduction to some rather classical results about quantum field theory in curved spacetime and about the thermodynamic limit of quantum ... | 11.054213 | 9.247007 | 9.751472 | 9.049113 | 8.987346 | 9.345645 | 9.331089 | 8.640031 | 9.420604 | 9.942728 | 9.598989 | 9.23804 | 10.240203 | 9.832252 | 9.523957 | 9.283032 | 9.359614 | 9.355838 | 9.57416 | 10.366416 | 9.445662 |
hep-th/9611029 | George Papadopoulos | G. Papadopoulos | The Universality of M-branes | Many changes have been made in the text and some references have been
added. 8 pages, Latex, Talk at the Imperial College Workshop 5-10 July | null | 10.1142/9781848160927_0025 | DAMTP-R/52 | hep-th | null | We review the evidence for the various dualities amongst the five D=10
superstring theories and for the existence of M-theory using the associated
effective supergravity theories. We also summarise the combinatorial technics
developed for constructing BPS solutions in D=11 supergravity theory and
conjecture that all ... | [
{
"created": "Tue, 5 Nov 1996 20:02:20 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Jan 1997 18:53:12 GMT",
"version": "v2"
}
] | 2016-12-21 | [
[
"Papadopoulos",
"G.",
""
]
] | We review the evidence for the various dualities amongst the five D=10 superstring theories and for the existence of M-theory using the associated effective supergravity theories. We also summarise the combinatorial technics developed for constructing BPS solutions in D=11 supergravity theory and conjecture that all th... | 8.858734 | 8.547655 | 8.830623 | 8.006856 | 8.234557 | 7.724817 | 8.096596 | 8.209543 | 8.489741 | 9.462309 | 7.945291 | 8.459124 | 9.121349 | 8.475845 | 8.606125 | 8.144382 | 8.663623 | 8.461003 | 8.351247 | 8.701375 | 7.82386 |
hep-th/0108185 | Stefan Groot Nibbelink | S. Groot Nibbelink | Dimensional regularization of a compact dimension | 12 pages, LaTeX, 1 figure, some minor changes and references added | Nucl.Phys.B619:373-384,2001 | 10.1016/S0550-3213(01)00539-9 | null | hep-th hep-ph | null | An extension of dimensional regularization to the case of compact dimensions
is presented. The procedure preserves the Kaluza-Klein tower structure, but has
a regulator specific to the compact dimension. Possible 5 and 4 dimensional
divergent as well as manifest finite contributions of (one-loop) Feynman graphs
can e... | [
{
"created": "Fri, 24 Aug 2001 12:52:42 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Nov 2001 18:02:56 GMT",
"version": "v2"
}
] | 2011-10-11 | [
[
"Nibbelink",
"S. Groot",
""
]
] | An extension of dimensional regularization to the case of compact dimensions is presented. The procedure preserves the Kaluza-Klein tower structure, but has a regulator specific to the compact dimension. Possible 5 and 4 dimensional divergent as well as manifest finite contributions of (one-loop) Feynman graphs can eas... | 17.95978 | 16.314421 | 16.256912 | 14.387403 | 17.197355 | 14.59442 | 16.126293 | 15.814918 | 15.374197 | 18.553406 | 15.386111 | 14.798608 | 16.294989 | 15.220658 | 16.310154 | 15.710697 | 15.185639 | 15.019125 | 15.431769 | 16.084543 | 15.079037 |
2308.15824 | Steffen Pottel | Steffen Pottel and Klaus Sibold | On the Perturbative Quantization of Einstein-Hilbert Gravity Embedded in
a Higher Derivative Model II | 21 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a previous paper we presented the renormalization of Einstein-Hilbert
gravity under inclusion of higher derivative terms and proposed a projection
down to the physical state space of Einstein-Hilbert. In the present paper we
describe this procedure in more detail via decomposing the original double-pole
field $h^{... | [
{
"created": "Wed, 30 Aug 2023 07:54:42 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Apr 2024 18:47:25 GMT",
"version": "v2"
}
] | 2024-04-19 | [
[
"Pottel",
"Steffen",
""
],
[
"Sibold",
"Klaus",
""
]
] | In a previous paper we presented the renormalization of Einstein-Hilbert gravity under inclusion of higher derivative terms and proposed a projection down to the physical state space of Einstein-Hilbert. In the present paper we describe this procedure in more detail via decomposing the original double-pole field $h^{\m... | 13.039282 | 14.271443 | 14.183777 | 13.185759 | 14.141937 | 13.247223 | 13.680322 | 12.852979 | 12.517689 | 15.141188 | 13.453568 | 12.955873 | 12.78718 | 12.592745 | 12.725522 | 13.051483 | 12.324519 | 12.908502 | 12.287786 | 13.182028 | 12.55578 |
1001.4532 | Jeong-Hyuck Park | Kanghoon Lee and Jeong-Hyuck Park | Partonic description of a supersymmetric p-brane | 1+16 pages, no figure; References added and Concluding section
expanded. Final version to appear in JHEP | JHEP 1004:043,2010 | 10.1007/JHEP04(2010)043 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider supersymmetric extensions of a recently proposed partonic
description of a bosonic p-brane which reformulates the Nambu-Goto action as an
interacting multi-particle action with Filippov-Lie algebra gauge symmetry. We
construct a worldline supersymmetric action by postulating, among others, a
p-form fermio... | [
{
"created": "Tue, 26 Jan 2010 07:52:18 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Feb 2010 03:20:47 GMT",
"version": "v2"
},
{
"created": "Tue, 30 Mar 2010 08:01:00 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Lee",
"Kanghoon",
""
],
[
"Park",
"Jeong-Hyuck",
""
]
] | We consider supersymmetric extensions of a recently proposed partonic description of a bosonic p-brane which reformulates the Nambu-Goto action as an interacting multi-particle action with Filippov-Lie algebra gauge symmetry. We construct a worldline supersymmetric action by postulating, among others, a p-form fermion.... | 10.564156 | 10.468693 | 12.098983 | 10.100695 | 9.763312 | 9.944586 | 9.976988 | 9.995523 | 9.580384 | 12.649137 | 9.208385 | 9.830409 | 11.502622 | 9.976149 | 9.883525 | 9.830271 | 10.097718 | 10.090597 | 10.296026 | 11.039089 | 9.773974 |
1012.3473 | Willem Westra | Jurjen F. Koksma and W. Westra | A Causal Alternative to Feynman's Propagator | 31 pages, 3 figures | null | null | ITP-UU-10/43, SPIN-10/36 | hep-th gr-qc hep-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Feynman propagator used in the conventional in-out formalism in quantum
field theory is not a causal propagator as wave packets are propagated
virtually instantaneously outside the causal region of the initial state. We
formulate a causal in-out formalism in quantum field theory by making use of
the Wheeler propa... | [
{
"created": "Wed, 15 Dec 2010 21:17:44 GMT",
"version": "v1"
}
] | 2010-12-17 | [
[
"Koksma",
"Jurjen F.",
""
],
[
"Westra",
"W.",
""
]
] | The Feynman propagator used in the conventional in-out formalism in quantum field theory is not a causal propagator as wave packets are propagated virtually instantaneously outside the causal region of the initial state. We formulate a causal in-out formalism in quantum field theory by making use of the Wheeler propaga... | 11.025062 | 10.318636 | 11.405712 | 10.855296 | 11.123545 | 11.283425 | 11.899413 | 10.314383 | 11.05475 | 12.758691 | 10.369147 | 11.17268 | 10.529871 | 10.531484 | 10.522017 | 10.696236 | 10.563207 | 10.993586 | 10.528217 | 10.984892 | 10.571155 |
0812.5042 | Pulak Ranjan Giri | Pulak Ranjan Giri, T. Shreecharan | Observations on spacetime symmetry and non-commutativity | 3 pages, no figure, revtex | null | null | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider both the co-ordinates and momenta to be non-commutative and
define a non-commutative version of Lorentz symmetry which has a smooth limit
to the standard Lorentz symmetry. The Poincar\acute{e} algebra in this
spacetime has also been discussed.
| [
{
"created": "Tue, 30 Dec 2008 09:47:58 GMT",
"version": "v1"
}
] | 2008-12-31 | [
[
"Giri",
"Pulak Ranjan",
""
],
[
"Shreecharan",
"T.",
""
]
] | We consider both the co-ordinates and momenta to be non-commutative and define a non-commutative version of Lorentz symmetry which has a smooth limit to the standard Lorentz symmetry. The Poincar\acute{e} algebra in this spacetime has also been discussed. | 10.258939 | 8.629622 | 8.737391 | 8.184551 | 8.460933 | 8.603467 | 8.007264 | 7.982796 | 7.684397 | 10.041744 | 8.796671 | 8.422842 | 8.936715 | 8.011395 | 8.21017 | 8.84066 | 7.883428 | 8.409758 | 8.118956 | 8.727893 | 8.443159 |
1409.7175 | Rabin Banerjee | Rabin Banerjee, Subir Ghosh, Arpan Krishna Mitra | Hamiltonian analysis of interacting fluids | 19 pages, no figures, expanded version,new references, published in
EPJC (2015) 75:207 | null | 10.1140/epjc/s10052-015-3412-y | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Ideal fluid dynamics is studied as a relativistic field theory with
particular importance on its hamiltonian structure. The Schwinger condition,
whose integrated version yields the stress tensor conservation, is explicitly
verified both in equal-time and light-cone coordinate systems. We also consider
the hamiltonian... | [
{
"created": "Thu, 25 Sep 2014 08:07:58 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Jan 2015 07:01:43 GMT",
"version": "v2"
},
{
"created": "Tue, 19 May 2015 12:21:31 GMT",
"version": "v3"
}
] | 2015-06-11 | [
[
"Banerjee",
"Rabin",
""
],
[
"Ghosh",
"Subir",
""
],
[
"Mitra",
"Arpan Krishna",
""
]
] | Ideal fluid dynamics is studied as a relativistic field theory with particular importance on its hamiltonian structure. The Schwinger condition, whose integrated version yields the stress tensor conservation, is explicitly verified both in equal-time and light-cone coordinate systems. We also consider the hamiltonian f... | 13.477952 | 13.289651 | 14.656928 | 13.158844 | 13.156853 | 11.721149 | 11.402243 | 12.427927 | 13.205687 | 16.466436 | 12.237846 | 11.963136 | 13.037476 | 12.305637 | 12.458425 | 11.981178 | 12.366574 | 12.291556 | 12.513379 | 12.758542 | 12.110905 |
hep-th/0606163 | Masanori Hanada | Masanori Hanada | Regularization of the Covariant Derivative on Curved Space by Finite
Matrices | 21pages, no figure, to appear in Prog. Theor. Phys | Prog.Theor.Phys.115:1189-1209,2006 | 10.1143/PTP.115.1189 | null | hep-th | null | In a previous paper [M.~Hanada, H.~Kawai and Y.~Kimura, Prog. Theor. Phys.
114 (2005), 1295] it is shown that a covariant derivative on any n-dimensional
Riemannian manifold can be expressed in terms of a set of n matrices, and a new
interpretation of IIB matrix model, in which the diffeomorphism, the local
Lorentz s... | [
{
"created": "Sat, 17 Jun 2006 09:09:38 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Hanada",
"Masanori",
""
]
] | In a previous paper [M.~Hanada, H.~Kawai and Y.~Kimura, Prog. Theor. Phys. 114 (2005), 1295] it is shown that a covariant derivative on any n-dimensional Riemannian manifold can be expressed in terms of a set of n matrices, and a new interpretation of IIB matrix model, in which the diffeomorphism, the local Lorentz sym... | 7.960186 | 7.741481 | 7.837513 | 7.632565 | 7.45516 | 7.508928 | 8.285667 | 7.698747 | 7.95941 | 8.493621 | 7.818976 | 7.280994 | 7.484547 | 7.11579 | 7.395895 | 7.519346 | 7.311494 | 7.433454 | 7.171298 | 7.609819 | 7.538436 |
hep-th/9311148 | null | J. Ellis, N. Mavromatos, and D. Nanopoulos | A Liouville String Approach to Microscopic Time and Cosmology | Latex 23 pages, no figures, CERN-TH.7000/93, CTP-TAMU-66/93 | null | null | null | hep-th astro-ph gr-qc hep-ph | null | In the non-critical string framework that we have proposed recently, the time
$t$ is identified with a dynamical local renormalization group scale, the
Liouville mode, and behaves as a statistical evolution parameter, flowing
irreversibly from an infrared fixed point - which we conjecture to be a
topological string p... | [
{
"created": "Thu, 25 Nov 1993 02:00:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ellis",
"J.",
""
],
[
"Mavromatos",
"N.",
""
],
[
"Nanopoulos",
"D.",
""
]
] | In the non-critical string framework that we have proposed recently, the time $t$ is identified with a dynamical local renormalization group scale, the Liouville mode, and behaves as a statistical evolution parameter, flowing irreversibly from an infrared fixed point - which we conjecture to be a topological string pha... | 13.654149 | 12.455515 | 13.261782 | 12.13885 | 11.605066 | 12.752834 | 11.902171 | 12.359035 | 12.041809 | 13.999691 | 12.435761 | 12.12021 | 12.351971 | 11.844084 | 11.827888 | 11.445909 | 11.711947 | 12.072776 | 11.669636 | 12.212823 | 11.855775 |
hep-th/9412212 | Tsuguo Mogami | T. Mogami | Temporal-gauge String Field with Open Strings | 8 pages, LaTeX | Phys.Lett. B351 (1995) 439-444 | 10.1016/0370-2693(95)00423-I | KEK-TH-426 | hep-th | null | A string field theory including open string fields is constructed in the
temporal gauge. It consists of string interaction vertices similar to the
light-cone gauge string field theory. A slight modification of the definition
of the time coordinate is needed because of the existence of the open string
end points.
| [
{
"created": "Sat, 24 Dec 1994 03:20:54 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Mogami",
"T.",
""
]
] | A string field theory including open string fields is constructed in the temporal gauge. It consists of string interaction vertices similar to the light-cone gauge string field theory. A slight modification of the definition of the time coordinate is needed because of the existence of the open string end points. | 11.547402 | 10.336059 | 12.631053 | 9.701504 | 9.61614 | 9.390244 | 9.829577 | 10.366045 | 10.367385 | 14.10822 | 10.090941 | 9.783788 | 12.03631 | 10.029964 | 9.67739 | 9.604295 | 9.962605 | 10.132173 | 10.220012 | 11.152211 | 10.568934 |
hep-th/0607216 | Christoph Adam | C. Adam, J. Sanchez-Guillen, A. Wereszczynski | Soliton stability in some knot soliton models | 27 pages, LaTex file | J.Math.Phys.48:022305,2007 | 10.1063/1.2435986 | null | hep-th | null | We study the issue of stability of static soliton-like solutions in some
non-linear field theories which allow for knotted field configurations.
Concretely, we investigate the AFZ model, based on a Lagrangian quartic in
first derivatives with infinitely many conserved currents, for which infinitely
many soliton solut... | [
{
"created": "Wed, 26 Jul 2006 17:48:06 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Adam",
"C.",
""
],
[
"Sanchez-Guillen",
"J.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | We study the issue of stability of static soliton-like solutions in some non-linear field theories which allow for knotted field configurations. Concretely, we investigate the AFZ model, based on a Lagrangian quartic in first derivatives with infinitely many conserved currents, for which infinitely many soliton solutio... | 8.330297 | 7.627842 | 8.561096 | 7.518273 | 8.251016 | 8.417426 | 7.885846 | 8.099162 | 7.755572 | 8.759059 | 7.640341 | 7.80454 | 7.963829 | 7.852064 | 7.894367 | 7.848825 | 7.639658 | 7.811473 | 7.608099 | 7.914408 | 7.636044 |
1101.4745 | Stefano Bellucci | Stefano Bellucci, Vinod Chandra, Bhupendra Nath Tiwari | Strong Interactions, (De)coherence and Quarkonia | 8 pages, Keywords: CPT symmetry, decoherence, Lorentz symmetry
breaking; PACS: 02.40.-k; 14.40.Pq; 12.40.Nn; 14.70.Dj; conference proceeding
of Discrete 2010, 6-11 December 2010, Roma (Italy); the Symposium proceedings
will be published online in a special volume of Journal of Physics:
Conference Series | J. Phys.: Conf. Ser. 335 (2011) 012062 | 10.1088/1742-6596/335/1/012062 | null | hep-th hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quarkonia are the central objects to explore the non-perturbative nature of
non-abelian gauge theories. We describe the confinement-deconfinement phases
for heavy quarkonia in a hot QCD medium and thereby the statistical nature of
the inter-quark forces. In the sense of one-loop quantum effects, we propose
that the "... | [
{
"created": "Tue, 25 Jan 2011 08:14:41 GMT",
"version": "v1"
}
] | 2012-03-22 | [
[
"Bellucci",
"Stefano",
""
],
[
"Chandra",
"Vinod",
""
],
[
"Tiwari",
"Bhupendra Nath",
""
]
] | Quarkonia are the central objects to explore the non-perturbative nature of non-abelian gauge theories. We describe the confinement-deconfinement phases for heavy quarkonia in a hot QCD medium and thereby the statistical nature of the inter-quark forces. In the sense of one-loop quantum effects, we propose that the "qu... | 13.130733 | 13.395473 | 13.414589 | 13.067287 | 13.693241 | 13.615225 | 14.102513 | 13.587531 | 13.081203 | 14.181621 | 12.539121 | 12.860727 | 12.795679 | 12.536968 | 12.55543 | 13.064468 | 12.873652 | 12.735679 | 12.343825 | 12.812916 | 12.694205 |
hep-th/0404186 | Jacques L. Rubin | Jacques L. Rubin, Thierry Grandou | Spacetime deployments parametrized by gravitational and electromagnetic
fields | 26 pages, LaTeX2e, file macro "suppl.sty", correction in the
definition of germs and local rings | null | null | INLN 2004/01 | hep-th gr-qc | null | On the basis of a "Punctual" Equivalence Principle of the general relativity
context, we consider spacetimes with measurements of conformally invariant
physical properties. Then, applying the Pfaff theory for PDE to a particular
conformally equivariant system of differential equations, we make explicit the
dependence... | [
{
"created": "Fri, 23 Apr 2004 16:36:00 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Apr 2004 13:58:53 GMT",
"version": "v2"
},
{
"created": "Tue, 4 May 2004 06:05:57 GMT",
"version": "v3"
},
{
"created": "Wed, 6 Oct 2004 13:18:35 GMT",
"version": "v4"
},
{
"cre... | 2007-05-23 | [
[
"Rubin",
"Jacques L.",
""
],
[
"Grandou",
"Thierry",
""
]
] | On the basis of a "Punctual" Equivalence Principle of the general relativity context, we consider spacetimes with measurements of conformally invariant physical properties. Then, applying the Pfaff theory for PDE to a particular conformally equivariant system of differential equations, we make explicit the dependence o... | 24.24832 | 27.347301 | 26.229033 | 24.207043 | 26.528667 | 28.015068 | 27.59119 | 22.499611 | 25.309334 | 23.054749 | 25.902073 | 22.482897 | 22.506672 | 22.704884 | 22.556953 | 22.665125 | 22.394745 | 22.471685 | 22.639585 | 22.195969 | 23.483463 |
1307.0266 | Dong-han Yeom | Jakob Hansen, Bum-Hoon Lee, Chanyong Park, Dong-han Yeom | Inside and outside stories of black-branes in anti de Sitter space | 27 pages, 12 figures | Class.Quant.Grav.30:235022,2013 | 10.1088/0264-9381/30/23/235022 | YITP-13-59 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we investigate the dynamics inside and outside of black-branes
in anti de Sitter space by numerical simulations using double-null formalism.
We prepare a charged planar matter shell which, due to a negative cosmological
constant, collapses and dynamically forms a black-brane with an apparent
horizon, a... | [
{
"created": "Mon, 1 Jul 2013 03:20:21 GMT",
"version": "v1"
},
{
"created": "Sat, 2 Nov 2013 07:20:29 GMT",
"version": "v2"
}
] | 2013-11-05 | [
[
"Hansen",
"Jakob",
""
],
[
"Lee",
"Bum-Hoon",
""
],
[
"Park",
"Chanyong",
""
],
[
"Yeom",
"Dong-han",
""
]
] | In this paper, we investigate the dynamics inside and outside of black-branes in anti de Sitter space by numerical simulations using double-null formalism. We prepare a charged planar matter shell which, due to a negative cosmological constant, collapses and dynamically forms a black-brane with an apparent horizon, a s... | 13.14521 | 15.342707 | 13.53361 | 13.029937 | 13.363385 | 14.679776 | 15.716624 | 12.743408 | 13.496647 | 13.193484 | 12.718534 | 13.580322 | 13.117675 | 12.602042 | 13.233819 | 13.508852 | 13.098761 | 12.716773 | 13.446529 | 13.189796 | 13.160914 |
1803.05173 | Alexander Reshetnyak | Alexander A. Reshetnyak | Constrained BRST-BFV and BRST-BV Lagrangians for half-integer HS fields
on $R^{1,d-1}$ | 11 pages, extended contribution to the Proceedings of the
International Workshop "Supersymmetry and Quantum Symmetries" (SQS'2017,
31.07.2017 - 5.08.2017, Dubna, Russia); 3 references, acknowledgements added,
final version, typos corrected | Physics of Particles and Nuclei 49(5) (2018) 952-957 | 10.1134/S1063779618050349 | null | hep-th math-ph math.DS math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Gauge invariant Lagrangian descriptions of irreducible and reducible
half-integer higher-spin mixed-symmetric massless and massive representations
of the Poincare group with off-shell algebraic constraints are constructed
within a metric-like formulation in a $d$-dimensional flat space-time on the
basis of a suggeste... | [
{
"created": "Wed, 14 Mar 2018 09:26:17 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Mar 2018 12:56:43 GMT",
"version": "v2"
},
{
"created": "Tue, 10 Jul 2018 00:55:07 GMT",
"version": "v3"
},
{
"created": "Tue, 21 Aug 2018 14:05:25 GMT",
"version": "v4"
},
{
"c... | 2018-10-25 | [
[
"Reshetnyak",
"Alexander A.",
""
]
] | Gauge invariant Lagrangian descriptions of irreducible and reducible half-integer higher-spin mixed-symmetric massless and massive representations of the Poincare group with off-shell algebraic constraints are constructed within a metric-like formulation in a $d$-dimensional flat space-time on the basis of a suggested ... | 17.617268 | 15.203899 | 21.904547 | 15.588202 | 15.462909 | 14.348703 | 14.832747 | 14.669768 | 15.772876 | 22.833439 | 16.101444 | 17.549894 | 18.106457 | 16.84762 | 16.230019 | 17.499147 | 17.689445 | 17.709986 | 17.256704 | 19.12154 | 16.990862 |
1307.6850 | Julian Sonner | Julian Sonner | Holographic Schwinger Effect and the Geometry of Entanglement | 4 pages, 2 figures; version as published in journal; title change to
conform with APS conventions; clarifications added, references updated | Phys. Rev. Lett. 111, 211603 (2013) | 10.1103/PhysRevLett.111.211603 | MIT-CTP 4483 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this note we point out that the recently proposed bulk dual of an
entangled pair of a quark and an anti-quark corresponds to the Lorentzian
continuation of the tunneling instanton describing Schwinger pair creation in
the dual field theory. This observation supports and further explains the claim
by Jensen & Karch... | [
{
"created": "Thu, 25 Jul 2013 19:44:11 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Aug 2013 14:02:52 GMT",
"version": "v2"
},
{
"created": "Mon, 23 Dec 2013 20:06:48 GMT",
"version": "v3"
}
] | 2013-12-24 | [
[
"Sonner",
"Julian",
""
]
] | In this note we point out that the recently proposed bulk dual of an entangled pair of a quark and an anti-quark corresponds to the Lorentzian continuation of the tunneling instanton describing Schwinger pair creation in the dual field theory. This observation supports and further explains the claim by Jensen & Karch t... | 10.133265 | 8.714315 | 10.318448 | 8.47528 | 8.836395 | 9.245036 | 8.426667 | 8.341319 | 9.088787 | 11.556348 | 8.886005 | 8.490452 | 9.505866 | 9.06945 | 8.555595 | 8.560774 | 8.339355 | 8.59487 | 8.902819 | 9.442438 | 8.652342 |
hep-th/9510055 | Rolf Schimmrigk | Ralph Blumenhagen, Rolf Schimmrigk and Andreas Wisskirchen | The (0,2) Exactly Solvable Structure of Chiral Rings, Landau-Ginzburg
Theories and Calabi-Yau Manifolds | 34 pages, minor changes | Nucl.Phys. B461 (1996) 460-492 | 10.1016/0550-3213(96)00011-9 | BONN-TH-95-17, IFP-601-UNC, NSF-ITP-95-120 | hep-th | null | We identify the exactly solvable theory of the conformal fixed point of (0,2)
Calabi-Yau sigma-models and their Landau-Ginzburg phases. To this end we
consider a number of (0,2) models constructed from a particular (2,2) exactly
solvable theory via the method of simple currents. In order to establish the
relation bet... | [
{
"created": "Tue, 10 Oct 1995 06:56:33 GMT",
"version": "v1"
},
{
"created": "Wed, 27 Mar 1996 12:49:03 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Blumenhagen",
"Ralph",
""
],
[
"Schimmrigk",
"Rolf",
""
],
[
"Wisskirchen",
"Andreas",
""
]
] | We identify the exactly solvable theory of the conformal fixed point of (0,2) Calabi-Yau sigma-models and their Landau-Ginzburg phases. To this end we consider a number of (0,2) models constructed from a particular (2,2) exactly solvable theory via the method of simple currents. In order to establish the relation betwe... | 6.39843 | 6.119418 | 6.931828 | 5.934024 | 6.15942 | 5.813515 | 5.99525 | 6.482132 | 5.885993 | 7.354909 | 5.816988 | 6.066569 | 6.610409 | 5.999772 | 6.094868 | 6.120606 | 6.103805 | 5.958912 | 6.035678 | 6.602491 | 5.86782 |
1901.01762 | Matej Pavsic | Matej Pav\v{s}i\v{c} | A Novel View on Successive Quantizations, Leading to Increasingly More
"Miraculous" States | 16 pages; A reference is added, and some typos are corrected | null | 10.1142/S0217732319501861 | null | hep-th quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A series of successive quantizations is considered, starting with the
quantization of a non relativistic or relativistic point particle: 1)
quantization of a particle's position, 2) quantization of wave function, 3)
quantization of wave functional. The latter step implies that the wave packet
profiles forming the sta... | [
{
"created": "Mon, 7 Jan 2019 12:00:35 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Apr 2019 11:02:30 GMT",
"version": "v2"
}
] | 2019-09-04 | [
[
"Pavšič",
"Matej",
""
]
] | A series of successive quantizations is considered, starting with the quantization of a non relativistic or relativistic point particle: 1) quantization of a particle's position, 2) quantization of wave function, 3) quantization of wave functional. The latter step implies that the wave packet profiles forming the state... | 12.537133 | 12.190765 | 11.423986 | 11.293184 | 12.937809 | 12.942172 | 12.358867 | 12.135705 | 11.774501 | 12.984466 | 11.325392 | 11.168005 | 10.847457 | 11.071594 | 11.137517 | 11.501766 | 11.039858 | 11.064665 | 11.028501 | 11.482196 | 11.052467 |
hep-th/9711031 | Marco Serone | Marco Serone | A comment on the $R^4$-coupling in (M)atrix Theory | LaTex file, 12 pages, no figures; references and some comments added | Phys.Lett. B422 (1998) 88-92 | 10.1016/S0370-2693(98)00011-2 | UvA-WINS-Wisk. 97-13 | hep-th | null | By scaling arguments we show that the presence of a $R^4$-term in the eleven
dimensional supergravity effective lagrangian, if it is visible in (M)atrix
theory, should produce a correction to the five-loops effective lagrangian of
two moving D0-branes.
| [
{
"created": "Wed, 5 Nov 1997 18:03:03 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Dec 1997 11:18:12 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Serone",
"Marco",
""
]
] | By scaling arguments we show that the presence of a $R^4$-term in the eleven dimensional supergravity effective lagrangian, if it is visible in (M)atrix theory, should produce a correction to the five-loops effective lagrangian of two moving D0-branes. | 15.696286 | 12.37975 | 15.291083 | 12.452675 | 12.913628 | 13.34946 | 12.320577 | 11.949207 | 12.472598 | 15.630288 | 12.733993 | 12.307105 | 13.34108 | 13.096103 | 12.383484 | 11.916442 | 11.878934 | 12.408342 | 12.399674 | 13.42979 | 12.902991 |
hep-th/0106078 | In Yong Park | I.Y. Park | Strong Coupling Limit of Open String: Born-Infeld Analysis | 15 pages, 2 figures, minor typos corrected, to appear in Phys. Rev. D | Phys.Rev.D64:081901,2001 | 10.1103/PhysRevD.64.081901 | null | hep-th | null | We consider a large coupling limit of a Born-Infeld action in a curved
background of an arbitrary metric and a constant two form field. Following
hep-th/0009061, we go to the Hamiltonian description. The Hamiltonian can be
dualized and the dual action admits a string-like configuration as its
solution. We interpret i... | [
{
"created": "Mon, 11 Jun 2001 16:39:06 GMT",
"version": "v1"
},
{
"created": "Sat, 16 Jun 2001 15:42:08 GMT",
"version": "v2"
},
{
"created": "Tue, 14 Aug 2001 20:55:08 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Park",
"I. Y.",
""
]
] | We consider a large coupling limit of a Born-Infeld action in a curved background of an arbitrary metric and a constant two form field. Following hep-th/0009061, we go to the Hamiltonian description. The Hamiltonian can be dualized and the dual action admits a string-like configuration as its solution. We interpret it ... | 15.291101 | 13.215523 | 15.45022 | 12.705142 | 13.6337 | 14.071513 | 14.473998 | 14.051386 | 13.533833 | 16.43009 | 13.461355 | 13.479976 | 15.458554 | 13.861883 | 13.935197 | 13.526971 | 13.738486 | 13.715982 | 13.970737 | 14.69833 | 13.587016 |
2208.01426 | Tadashi Okazaki | Yasuyuki Hatsuda, Tadashi Okazaki | $\mathcal{N}=2^{*}$ Schur indices | 61 pages | JHEP01(2023)029 | 10.1007/JHEP01(2023)029 | RUP-22-17, KIAS-P22059 | hep-th math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find closed-form expressions for the Schur indices of 4d
$\mathcal{N}=2^{*}$ super Yang-Mills theory with unitary gauge groups for
arbitrary ranks via the Fermi-gas formulation. They can be written as a sum
over the Young diagrams associated with spectral zeta functions of an ideal
Fermi-gas system. These function... | [
{
"created": "Tue, 2 Aug 2022 13:02:04 GMT",
"version": "v1"
}
] | 2023-01-12 | [
[
"Hatsuda",
"Yasuyuki",
""
],
[
"Okazaki",
"Tadashi",
""
]
] | We find closed-form expressions for the Schur indices of 4d $\mathcal{N}=2^{*}$ super Yang-Mills theory with unitary gauge groups for arbitrary ranks via the Fermi-gas formulation. They can be written as a sum over the Young diagrams associated with spectral zeta functions of an ideal Fermi-gas system. These functions ... | 10.793823 | 9.196077 | 11.218871 | 9.347345 | 10.623356 | 9.142584 | 9.434472 | 9.529118 | 9.169024 | 13.40936 | 9.279052 | 9.694189 | 10.490632 | 9.507251 | 9.960847 | 10.194776 | 9.817899 | 9.755391 | 10.06814 | 10.715944 | 9.537352 |
hep-th/9810002 | Christofer Cronstrom | Christofer Cronstrom | The Generalisation of the Coulomb Gauge to Yang-Mills Theory | 8 pages | null | null | HIP-1998-61/TH | hep-th | null | I consider the problem of generalising the Abelian Coulomb gauge condition to
the non-Abelian Yang-Mills theory, with an arbitrary compact and semi-simple
gauge group. It is shown that a straightforward generalisation exists, which
reduces the Gauss law into a form involving the gauge potentials only, but not
their t... | [
{
"created": "Thu, 1 Oct 1998 10:52:49 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Cronstrom",
"Christofer",
""
]
] | I consider the problem of generalising the Abelian Coulomb gauge condition to the non-Abelian Yang-Mills theory, with an arbitrary compact and semi-simple gauge group. It is shown that a straightforward generalisation exists, which reduces the Gauss law into a form involving the gauge potentials only, but not their tim... | 8.24273 | 8.201415 | 8.206323 | 7.505571 | 8.014773 | 8.688363 | 8.360472 | 7.549813 | 7.989414 | 9.115056 | 7.619705 | 7.317268 | 7.364056 | 7.396872 | 7.317103 | 7.332603 | 7.486166 | 7.548024 | 7.253188 | 7.488767 | 7.273353 |
hep-th/0609220 | Natalia Kiriushcheva | R. N. Ghalati, N. Kiriushcheva, S. V. Kuzmin and D. G. C. McKeon | Canonical Analysis of the First Order Form of Topologically Massive
Electrodynamics | 8 pages | null | null | null | hep-th | null | The first order form of a three dimensional U(1) gauge theory in which a
gauge invariant mass term appears is analyzed using the Dirac procedure. The
form of the gauge transformation which leaves the action invariant is derived
from the constraints present.
| [
{
"created": "Fri, 29 Sep 2006 14:57:02 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ghalati",
"R. N.",
""
],
[
"Kiriushcheva",
"N.",
""
],
[
"Kuzmin",
"S. V.",
""
],
[
"McKeon",
"D. G. C.",
""
]
] | The first order form of a three dimensional U(1) gauge theory in which a gauge invariant mass term appears is analyzed using the Dirac procedure. The form of the gauge transformation which leaves the action invariant is derived from the constraints present. | 14.87942 | 7.333158 | 10.316835 | 8.492519 | 9.813213 | 9.673031 | 9.901212 | 7.923475 | 8.512763 | 11.780477 | 9.017413 | 10.270293 | 11.857033 | 10.504255 | 10.925873 | 10.411913 | 10.878296 | 10.258222 | 11.104372 | 11.752526 | 10.521587 |
hep-th/0003233 | Marek Olechowski | Krzysztof A. Meissner and Marek Olechowski | Anomaly cancellation in M-theory on orbifolds | latex, 14 pages | Nucl.Phys. B590 (2000) 161-172 | 10.1016/S0550-3213(00)00456-9 | IFT-7/2000 | hep-th | null | We present calculation of the anomaly cancellation in M-theory on orbifolds
$S^1/Z_2$ and $T^5/Z_2$ in the upstairs approach. The main requirement that
allows one to uniquely define solutions to the modified Bianchi identities in
this case is that the field strength $G$ be globally defined on $S^1$ or $T^5$
and prope... | [
{
"created": "Mon, 27 Mar 2000 14:51:28 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Meissner",
"Krzysztof A.",
""
],
[
"Olechowski",
"Marek",
""
]
] | We present calculation of the anomaly cancellation in M-theory on orbifolds $S^1/Z_2$ and $T^5/Z_2$ in the upstairs approach. The main requirement that allows one to uniquely define solutions to the modified Bianchi identities in this case is that the field strength $G$ be globally defined on $S^1$ or $T^5$ and properl... | 9.101117 | 9.386806 | 10.057158 | 8.674989 | 9.036742 | 8.818102 | 9.404477 | 8.927367 | 8.914074 | 10.308169 | 8.712126 | 9.058389 | 8.978267 | 8.754768 | 8.648155 | 8.826068 | 8.8334 | 8.765024 | 8.768562 | 9.193733 | 8.632255 |
hep-th/9210061 | Ergin Sezgin | R. Percacci and E. Sezgin | Symmetries of P-Branes | 15 pages, CTP-TAMU-32/92, SISSA 182/92/EP | Int. J. Mod. Phys. A8 (1993) 5367-5382 | 10.1142/S0217751X93002137 | null | hep-th | null | Using canonical methods, we study the invariance properties of a bosonic
$p$--brane propagating in a curved background locally diffeomorphic to $M\times
G$, where $M$ is spacetime and $G$ a group manifold. The action is that of a
gauged sigma model in $p+1$ dimensions coupled to a Yang--Mills field and a
$(p+1)$--for... | [
{
"created": "Sun, 11 Oct 1992 18:39:47 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Percacci",
"R.",
""
],
[
"Sezgin",
"E.",
""
]
] | Using canonical methods, we study the invariance properties of a bosonic $p$--brane propagating in a curved background locally diffeomorphic to $M\times G$, where $M$ is spacetime and $G$ a group manifold. The action is that of a gauged sigma model in $p+1$ dimensions coupled to a Yang--Mills field and a $(p+1)$--form ... | 6.259332 | 5.855235 | 6.604848 | 5.855873 | 6.085088 | 5.445723 | 5.859561 | 5.62288 | 5.784746 | 6.756058 | 5.623289 | 5.666355 | 5.933064 | 5.618227 | 5.795879 | 5.768121 | 5.863601 | 5.762473 | 5.79569 | 5.978558 | 5.762042 |
hep-th/9806185 | Alexander Vilenkin | Alexander Vilenkin (Tufts University) | Unambiguous probabilities in an eternally inflating universe | 7 pages, Final version (minor changes), to appear in Phys. Rev. Lett | Phys.Rev.Lett. 81 (1998) 5501-5504 | 10.1103/PhysRevLett.81.5501 | null | hep-th astro-ph gr-qc | null | ``Constants of Nature'' and cosmological parameters may in fact be variables
related to some slowly-varying fields. In models of eternal inflation, such
fields will take different values in different parts of the universe. Here I
show how one can assign probabilities to values of the ``constants'' measured
by a typic... | [
{
"created": "Mon, 22 Jun 1998 14:54:42 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Nov 1998 18:00:17 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Vilenkin",
"Alexander",
"",
"Tufts University"
]
] | ``Constants of Nature'' and cosmological parameters may in fact be variables related to some slowly-varying fields. In models of eternal inflation, such fields will take different values in different parts of the universe. Here I show how one can assign probabilities to values of the ``constants'' measured by a typical... | 13.220788 | 10.840772 | 10.053748 | 9.785574 | 10.739882 | 10.026524 | 9.43373 | 10.040111 | 9.657104 | 10.746616 | 10.555661 | 10.560966 | 11.358832 | 10.494285 | 10.487017 | 10.52511 | 10.535665 | 10.246941 | 9.902281 | 10.49022 | 11.082894 |
1804.01737 | Toshihiro Ota | Tetsuya Akutagawa, Koji Hashimoto, Takeshi Miyazaki, Toshihiro Ota | Phase diagram of QCD chaos in linear sigma models and holography | 25 pages, 7 figures | PTEP 2018 (2018) no.6, 063B01 | 10.1093/ptep/pty055 | OU-HET-966 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Measuring chaos of QCD-like theories is a challenge for formulating a novel
characterization of quantum gauge theories. We define a chaos phase diagram of
QCD allowing us to locate chaos in the parameter space of energy of homogeneous
meson condensates and the QCD parameters such as pion/quark mass. We draw the
chaos... | [
{
"created": "Thu, 5 Apr 2018 08:50:41 GMT",
"version": "v1"
}
] | 2019-04-17 | [
[
"Akutagawa",
"Tetsuya",
""
],
[
"Hashimoto",
"Koji",
""
],
[
"Miyazaki",
"Takeshi",
""
],
[
"Ota",
"Toshihiro",
""
]
] | Measuring chaos of QCD-like theories is a challenge for formulating a novel characterization of quantum gauge theories. We define a chaos phase diagram of QCD allowing us to locate chaos in the parameter space of energy of homogeneous meson condensates and the QCD parameters such as pion/quark mass. We draw the chaos p... | 13.086862 | 13.387361 | 12.548215 | 12.227079 | 13.429472 | 13.905288 | 14.346072 | 13.170824 | 12.542424 | 13.625753 | 12.608073 | 12.180888 | 12.048941 | 12.050857 | 11.965734 | 12.495879 | 12.160692 | 12.183275 | 12.021256 | 12.213787 | 12.427925 |
hep-th/9912279 | Edward Witten | Gregory Moore and Edward Witten | Self-Duality, Ramond-Ramond Fields, and K-Theory | 35 pp | JHEP 0005:032,2000 | 10.1088/1126-6708/2000/05/032 | null | hep-th | null | Just as D-brane charge of Type IIA and Type IIB superstrings is classified,
respectively, by K^1(X) and K(X), Ramond-Ramond fields in these theories are
classified, respectively, by K(X) and K^1(X). By analyzing a recent proposal
for how to interpret quantum self-duality of RR fields, we show that the Dirac
quantizat... | [
{
"created": "Thu, 30 Dec 1999 20:57:16 GMT",
"version": "v1"
}
] | 2010-04-07 | [
[
"Moore",
"Gregory",
""
],
[
"Witten",
"Edward",
""
]
] | Just as D-brane charge of Type IIA and Type IIB superstrings is classified, respectively, by K^1(X) and K(X), Ramond-Ramond fields in these theories are classified, respectively, by K(X) and K^1(X). By analyzing a recent proposal for how to interpret quantum self-duality of RR fields, we show that the Dirac quantizatio... | 10.479291 | 11.264728 | 11.866693 | 10.279178 | 11.493146 | 11.382005 | 10.225864 | 10.26055 | 9.746322 | 13.167091 | 10.364284 | 10.408483 | 10.393182 | 9.578315 | 9.920467 | 10.190255 | 9.603131 | 9.563599 | 9.745915 | 10.604271 | 9.449424 |
0806.2667 | Erik Plauschinn | Ralph Blumenhagen, Sebastian Moster, Erik Plauschinn | String GUT Scenarios with Stabilised Moduli | 22 pages, 13 figures; v2: refs. and explanation added | Phys.Rev.D78:066008,2008 | 10.1103/PhysRevD.78.066008 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Taking into account the recently proposed poly-instanton corrections to the
superpotential and combining the race-track with a KKLT respectively LARGE
Volume Scenario in an intricate manner, we show that we gain exponential
control over the parameters in an effective superpotential. This allows us to
dynamically stab... | [
{
"created": "Tue, 17 Jun 2008 13:19:59 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Jul 2008 18:44:55 GMT",
"version": "v2"
}
] | 2009-02-23 | [
[
"Blumenhagen",
"Ralph",
""
],
[
"Moster",
"Sebastian",
""
],
[
"Plauschinn",
"Erik",
""
]
] | Taking into account the recently proposed poly-instanton corrections to the superpotential and combining the race-track with a KKLT respectively LARGE Volume Scenario in an intricate manner, we show that we gain exponential control over the parameters in an effective superpotential. This allows us to dynamically stabil... | 14.251307 | 15.647003 | 13.997314 | 13.156084 | 14.136715 | 15.178582 | 15.052866 | 13.792576 | 12.714244 | 12.858645 | 14.513439 | 13.911306 | 13.406068 | 13.063178 | 13.270245 | 13.454524 | 13.427586 | 13.448818 | 13.173178 | 13.433177 | 13.174456 |
hep-th/0011144 | Haewon Lee | Haewon Lee, W. S. l'Yi | Domain walls, stabilities, and the mass hierarchy of the Randall-Sundrum
Model | 15 pages, 4 figures | null | null | null | hep-th | null | Randall-Sundrum model, which has a scalar field, is used to investigate the
domain structure of the extra dimension and to obtain a possible solution of
the mass hierarchy problem. It is found that when the domain wall size is
comparable to that of domains, domains become unstable. To construct a reliable
theory, a r... | [
{
"created": "Thu, 16 Nov 2000 04:32:26 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Lee",
"Haewon",
""
],
[
"l'Yi",
"W. S.",
""
]
] | Randall-Sundrum model, which has a scalar field, is used to investigate the domain structure of the extra dimension and to obtain a possible solution of the mass hierarchy problem. It is found that when the domain wall size is comparable to that of domains, domains become unstable. To construct a reliable theory, a reg... | 10.940892 | 10.206238 | 10.365377 | 10.493664 | 11.214504 | 11.588378 | 10.260099 | 10.115424 | 10.241863 | 11.369586 | 9.955245 | 10.460295 | 10.393782 | 9.993731 | 10.34719 | 9.924439 | 10.044035 | 10.173102 | 10.013674 | 10.2797 | 9.808832 |
0906.5501 | Jonas Schmidt | Jonas Schmidt | Local Grand Unification in the Heterotic Landscape | 141 pages, 6 figures, Ph.D. thesis | Fortsch.Phys.58:3-111,2010 | 10.1002/prop.200900079 | DESY-THESIS-2009-020 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the possibility that the unification of the electroweak
interactions and the strong force arises from string theory, at energies
significantly lower than the string scale. As a tool, an effective grand
unified field theory in six dimensions is derived from an anisotropic orbifold
compactification of the h... | [
{
"created": "Tue, 30 Jun 2009 12:58:33 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Sep 2009 08:39:22 GMT",
"version": "v2"
}
] | 2010-02-04 | [
[
"Schmidt",
"Jonas",
""
]
] | We consider the possibility that the unification of the electroweak interactions and the strong force arises from string theory, at energies significantly lower than the string scale. As a tool, an effective grand unified field theory in six dimensions is derived from an anisotropic orbifold compactification of the het... | 10.009283 | 10.321795 | 10.115438 | 9.508227 | 10.663495 | 9.888279 | 9.975292 | 10.130803 | 9.696636 | 10.739892 | 9.602507 | 9.908116 | 9.869 | 9.770272 | 9.886438 | 9.917014 | 9.809392 | 9.723363 | 9.974077 | 9.771167 | 9.758697 |
1106.3845 | Mans Henningson | Mans Henningson | Boundary conditions for GL-twisted N=4 SYM | 14 pages, 1 figure, minor changes | null | 10.1103/PhysRevD.86.085003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider topologically twisted N=4 supersymmetric Yang-Mills theory on a
four-manifold of the form V = W \times R_+ or V = W \times I, where W is a
Riemannian three-manifold. Different kinds of boundary conditions apply at
infinity or at finite distance. We verify that each of these conditions defines
a `middle-di... | [
{
"created": "Mon, 20 Jun 2011 09:30:10 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Jul 2011 13:02:59 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Henningson",
"Mans",
""
]
] | We consider topologically twisted N=4 supersymmetric Yang-Mills theory on a four-manifold of the form V = W \times R_+ or V = W \times I, where W is a Riemannian three-manifold. Different kinds of boundary conditions apply at infinity or at finite distance. We verify that each of these conditions defines a `middle-dime... | 9.578011 | 9.120913 | 10.627201 | 8.572248 | 9.287744 | 8.777368 | 9.033306 | 9.325122 | 9.216987 | 11.181377 | 8.448322 | 9.099438 | 9.407951 | 8.566089 | 9.31485 | 8.839206 | 9.065259 | 8.78017 | 9.060088 | 9.415446 | 9.128289 |
1412.3253 | Victor S. Fadin | V.S. Fadin | Discontinuities of multi-Regge amplitudes | 4 pages, Invited talk presented by V.S. Fadin at "DIFFRACTION 2014",
May 10 - 15, 2014, Primosten (Croatia) (to be published in the AIP Conference
Proceedings | null | 10.1063/1.4915996 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the BFKL approach, discontinuities of multiple production amplitudes in
invariant masses of produced particles are discussed. It turns out that they
are in evident contradiction with the BDS ansatz for $n$-gluon amplitudes in
the planar $N$=4 SYM at $n\ge 6$. An explicit expression for the NLO
discontinuity of the... | [
{
"created": "Wed, 10 Dec 2014 10:51:58 GMT",
"version": "v1"
}
] | 2015-06-23 | [
[
"Fadin",
"V. S.",
""
]
] | In the BFKL approach, discontinuities of multiple production amplitudes in invariant masses of produced particles are discussed. It turns out that they are in evident contradiction with the BDS ansatz for $n$-gluon amplitudes in the planar $N$=4 SYM at $n\ge 6$. An explicit expression for the NLO discontinuity of the t... | 8.605941 | 8.669386 | 8.652466 | 7.76125 | 8.288781 | 9.348199 | 7.948347 | 8.21733 | 7.792629 | 9.342208 | 7.285562 | 7.919546 | 8.274153 | 7.884043 | 7.910078 | 7.693366 | 7.680696 | 8.090286 | 7.650797 | 7.697146 | 7.779525 |
hep-th/0311230 | Cristiano Germani | Cristiano Germani | Astrophysical and Cosmological Consequences of the Dynamical
Localization of Gravity | PhD thesis, ICG University of Portsmouth (UK); 106+14 pages, 5
figures; v2 reference added | null | null | null | hep-th astro-ph gr-qc | null | In this thesis I review cosmological and astrophysical exact models for
Randall-Sundrum-type braneworlds and their physical implications. I present new
insights and show their analogies with quantum theories via the holographic
idea. In astrophysics I study the two fundamental models of a spherically
symmetric static... | [
{
"created": "Mon, 24 Nov 2003 17:56:16 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Dec 2003 11:47:38 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Germani",
"Cristiano",
""
]
] | In this thesis I review cosmological and astrophysical exact models for Randall-Sundrum-type braneworlds and their physical implications. I present new insights and show their analogies with quantum theories via the holographic idea. In astrophysics I study the two fundamental models of a spherically symmetric static s... | 11.960316 | 12.401332 | 12.018475 | 11.780993 | 12.967146 | 12.955435 | 13.713116 | 12.219278 | 12.490701 | 12.939219 | 11.917811 | 11.71574 | 11.618965 | 11.698736 | 12.019032 | 11.911087 | 11.759169 | 11.78238 | 12.096786 | 11.926393 | 11.795469 |
2206.05781 | Georgios Pastras | Dimitrios Katsinis and Georgios Pastras | Entanglement in harmonic systems at coherent states | 30 pages | null | null | null | hep-th quant-ph | http://creativecommons.org/licenses/by/4.0/ | It is well-known that entanglement entropy in field theory at its ground
state is dominated by an area law term, presenting a similarity to the entropy
of black holes. It is interesting to investigate whether this similarity can be
extended by showing that gravitational dynamics emerges from the first law of
entangle... | [
{
"created": "Sun, 12 Jun 2022 16:25:27 GMT",
"version": "v1"
}
] | 2022-06-14 | [
[
"Katsinis",
"Dimitrios",
""
],
[
"Pastras",
"Georgios",
""
]
] | It is well-known that entanglement entropy in field theory at its ground state is dominated by an area law term, presenting a similarity to the entropy of black holes. It is interesting to investigate whether this similarity can be extended by showing that gravitational dynamics emerges from the first law of entangleme... | 12.238464 | 12.762792 | 12.818682 | 11.648835 | 12.589311 | 12.268468 | 12.181022 | 11.929649 | 11.815994 | 13.057823 | 11.916095 | 11.745049 | 12.092494 | 12.252967 | 11.806954 | 11.692336 | 11.938387 | 11.664576 | 12.294981 | 12.610198 | 11.992644 |
2307.00832 | Aritra Ghosh | Aritra Ghosh | Statistical ensembles and logarithmic corrections to black hole entropy | null | Class. Quant. Grav. 40, 155013 (2023) | 10.1088/1361-6382/acdbfe | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we consider general statistical ensembles and compute
logarithmic corrections to the microcanonical entropy resulting due to
thermodynamic fluctuations which are controlled by the boundary conditions,
i.e. due to choice of ensemble. The framework is applied to the case of
non-extremal black holes to gi... | [
{
"created": "Mon, 3 Jul 2023 08:17:50 GMT",
"version": "v1"
}
] | 2023-07-17 | [
[
"Ghosh",
"Aritra",
""
]
] | In this paper, we consider general statistical ensembles and compute logarithmic corrections to the microcanonical entropy resulting due to thermodynamic fluctuations which are controlled by the boundary conditions, i.e. due to choice of ensemble. The framework is applied to the case of non-extremal black holes to give... | 7.615272 | 7.870892 | 7.345176 | 7.253472 | 7.831999 | 7.717805 | 8.222603 | 7.289917 | 7.696721 | 8.035301 | 7.616354 | 7.290597 | 7.246829 | 7.143648 | 7.15936 | 7.397113 | 7.329539 | 7.355156 | 7.23146 | 7.425358 | 7.4432 |
1105.3998 | Per Kraus | Eric D'Hoker and Per Kraus | Charged Magnetic Brane Correlators and Twisted Virasoro Algebras | 67 pages | null | 10.1103/PhysRevD.84.065010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Prior work using gauge/gravity duality has established the existence of a
quantum critical point in the phase diagram of 3+1-dimensional gauge theories
at finite charge density and background magnetic field. The critical theory,
obtained by tuning the dimensionless charge density to magnetic field ratio,
exhibits non... | [
{
"created": "Thu, 19 May 2011 23:10:07 GMT",
"version": "v1"
}
] | 2013-05-29 | [
[
"D'Hoker",
"Eric",
""
],
[
"Kraus",
"Per",
""
]
] | Prior work using gauge/gravity duality has established the existence of a quantum critical point in the phase diagram of 3+1-dimensional gauge theories at finite charge density and background magnetic field. The critical theory, obtained by tuning the dimensionless charge density to magnetic field ratio, exhibits nontr... | 7.454092 | 7.168081 | 8.083985 | 7.35422 | 7.509953 | 6.816285 | 7.674232 | 7.711706 | 7.561668 | 8.971375 | 7.287147 | 6.964618 | 7.465795 | 7.053975 | 6.999035 | 7.014894 | 7.116572 | 7.126726 | 7.050762 | 7.063972 | 7.037704 |
0809.2684 | C. P. Martin | C.P. Martin and C. Tamarit (Universidad Complutense de Madrid) | The Seiberg-Witten map and supersymmetry | 28 pages. No figures | JHEP0811:087,2008 | 10.1088/1126-6708/2008/11/087 | FTI/UCM 133-2008 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The lack of any local solution to the first-order-in-h omegamn Seiberg-Witten
(SW) map equations for U(1) vector superfields compels us to obtain the most
general solution to those equations that is a quadratic polynomial in the
ordinary vector superfield, v, its chiral and antichiral projections and the
susy covaria... | [
{
"created": "Tue, 16 Sep 2008 16:28:24 GMT",
"version": "v1"
}
] | 2008-12-18 | [
[
"Martin",
"C. P.",
"",
"Universidad Complutense de Madrid"
],
[
"Tamarit",
"C.",
"",
"Universidad Complutense de Madrid"
]
] | The lack of any local solution to the first-order-in-h omegamn Seiberg-Witten (SW) map equations for U(1) vector superfields compels us to obtain the most general solution to those equations that is a quadratic polynomial in the ordinary vector superfield, v, its chiral and antichiral projections and the susy covariant... | 10.482314 | 11.400783 | 11.203531 | 10.530055 | 10.622791 | 10.668303 | 10.49802 | 10.838267 | 11.069564 | 12.234164 | 10.413556 | 9.626194 | 10.68983 | 10.118705 | 10.541207 | 10.538863 | 10.197143 | 10.55388 | 10.120649 | 11.02456 | 10.160652 |
1106.4353 | Bin Wang | Yunqi Liu, Qiyuan Pan, Bin Wang | Holographic superconductor developed in BTZ black hole background with
backreactions | accepted for publication in Phys.Lett.B | null | 10.1016/j.physletb.2011.06.062 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a holographic superconductor in BTZ black hole background with
backreactions. We investigate the influence of the backreaction on the
condensation of the scalar hair and the dynamics of perturbation in the
background spacetime. When the Breitenlohner-Freedman bound is approached, we
argue that only one of ... | [
{
"created": "Wed, 22 Jun 2011 00:31:45 GMT",
"version": "v1"
}
] | 2015-05-28 | [
[
"Liu",
"Yunqi",
""
],
[
"Pan",
"Qiyuan",
""
],
[
"Wang",
"Bin",
""
]
] | We develop a holographic superconductor in BTZ black hole background with backreactions. We investigate the influence of the backreaction on the condensation of the scalar hair and the dynamics of perturbation in the background spacetime. When the Breitenlohner-Freedman bound is approached, we argue that only one of tw... | 8.598729 | 7.411739 | 8.061971 | 7.827465 | 8.096778 | 7.786049 | 7.624857 | 7.114307 | 7.828781 | 7.902518 | 7.380253 | 8.177715 | 8.560637 | 8.250203 | 8.210205 | 8.463844 | 8.347229 | 8.531602 | 8.282916 | 8.555766 | 8.327434 |
hep-th/9811032 | Helia Hollmann | I. Gaida, H. R. Hollmann, J. M. Stewart (Cambridge U., DAMTP) | Classical and Quantum Analysis of Repulsive Singularities in Four
Dimensional Extended Supergravity | 20 pages, 14 figures | Class.Quant.Grav. 16 (1999) 2231-2246 | 10.1088/0264-9381/16/7/306 | DAMTP-R-98-29 | hep-th gr-qc | null | Non--minimal repulsive singularities (``repulsons'') in extended supergravity
theories are investigated. The short distance antigravity properties of the
repulsons are tested at the classical and the quantum level by a scalar
test--particle. Using a partial wave expansion it is shown that the particle
gets totally re... | [
{
"created": "Tue, 3 Nov 1998 09:25:29 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Gaida",
"I.",
"",
"Cambridge U., DAMTP"
],
[
"Hollmann",
"H. R.",
"",
"Cambridge U., DAMTP"
],
[
"Stewart",
"J. M.",
"",
"Cambridge U., DAMTP"
]
] | Non--minimal repulsive singularities (``repulsons'') in extended supergravity theories are investigated. The short distance antigravity properties of the repulsons are tested at the classical and the quantum level by a scalar test--particle. Using a partial wave expansion it is shown that the particle gets totally refl... | 12.686223 | 11.902997 | 12.49013 | 11.005668 | 11.026067 | 13.030191 | 12.999145 | 12.410771 | 11.475135 | 13.092241 | 11.382719 | 11.42065 | 11.775646 | 11.305377 | 11.814819 | 11.786072 | 11.662986 | 11.679111 | 11.628631 | 11.786148 | 11.141312 |
hep-th/9707006 | null | Alexander A.Vlasov | Classical Electrodynamics: Problems of Radiation Reaction | 18 pages, LATEX | enlarged version of talk given at XX International Workshop on the
Fundamental Problems of High Energy Physics and Field Theory, 24-26 June
1997, Protvino, Russia | null | null | hep-th | null | There are known problems of Lorentz-Dirac equation for moving with
acceleration charged particle in classical electrodynamics. The model of
extended in one dimension particle is proposed and shown that electromagnetic
self-interaction can lead (with appropriate choice of retarded and advanced
interactions) to zero ch... | [
{
"created": "Tue, 1 Jul 1997 09:26:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Vlasov",
"Alexander A.",
""
]
] | There are known problems of Lorentz-Dirac equation for moving with acceleration charged particle in classical electrodynamics. The model of extended in one dimension particle is proposed and shown that electromagnetic self-interaction can lead (with appropriate choice of retarded and advanced interactions) to zero chan... | 20.525255 | 25.904322 | 19.955679 | 18.884794 | 20.25695 | 22.484955 | 22.047274 | 20.385687 | 21.643602 | 19.504597 | 20.088535 | 21.367918 | 19.246748 | 19.540148 | 21.018179 | 20.631765 | 20.87923 | 19.720644 | 20.393108 | 18.86647 | 20.028193 |
hep-th/9308090 | null | \Mary K. Gaillard and Vidyut Jain | Supergravity Coupled to Chiral Matter at One Loop | 33 pages, LBL-34457, UCB-PTH-93-22 | Phys.Rev. D49 (1994) 1951-1965 | 10.1103/PhysRevD.49.1951 | null | hep-th hep-ph | null | We extend earlier calculations of the one-loop contributions to the effective
bose Lagrangian in supergravity coupled to chiral matter. We evaluate all
logarithmically divergent contributions for arbitrary background scalar fields
and space-time metric. We show that, with a judicious choice of gauge fixing
and of the... | [
{
"created": "Wed, 18 Aug 1993 21:50:39 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Gaillard",
"\\Mary K.",
""
],
[
"Jain",
"Vidyut",
""
]
] | We extend earlier calculations of the one-loop contributions to the effective bose Lagrangian in supergravity coupled to chiral matter. We evaluate all logarithmically divergent contributions for arbitrary background scalar fields and space-time metric. We show that, with a judicious choice of gauge fixing and of the d... | 7.620884 | 7.780282 | 7.913562 | 7.328635 | 8.079202 | 7.513943 | 7.598271 | 7.498165 | 7.34567 | 8.175585 | 7.331697 | 7.195624 | 7.576173 | 7.12547 | 7.135058 | 7.238153 | 7.061464 | 7.389109 | 7.136796 | 7.833185 | 7.213266 |
hep-th/9311168 | Christoph Schweigert | Christoph Schweigert | Poincare Polynomials and Level Rank Dualities in the $N=2$ Coset
Construction | 14 pages in LaTeX, HD-THEP-93-43 | Theor.Math.Phys. 98 (1994) 326-334; Teor.Mat.Fiz. 98 (1994)
467-478 | 10.1007/BF01102209 | null | hep-th | null | We review the coset construction of conformal field theories; the emphasis is
on the construction of the Hilbert spaces for these models, especially if fixed
points occur. This is applied to the $N=2$ superconformal cosets constructed by
Kazama and Suzuki. To calculate heterotic string spectra we reformulate the
Gepn... | [
{
"created": "Mon, 29 Nov 1993 14:12:31 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Schweigert",
"Christoph",
""
]
] | We review the coset construction of conformal field theories; the emphasis is on the construction of the Hilbert spaces for these models, especially if fixed points occur. This is applied to the $N=2$ superconformal cosets constructed by Kazama and Suzuki. To calculate heterotic string spectra we reformulate the Gepner... | 9.867105 | 7.738917 | 11.39898 | 8.133923 | 7.764624 | 7.577533 | 7.444664 | 7.674853 | 7.824082 | 12.397741 | 8.094795 | 8.607327 | 10.066414 | 8.501848 | 8.822476 | 8.477555 | 8.699846 | 8.415859 | 8.813764 | 9.913606 | 8.578355 |
hep-th/0512139 | Forough Nasseri | Forough Nasseri | Time variation of the gravitational coupling constant in decrumpling
cosmology | 11 pages | null | null | null | hep-th | null | Within the framework of a model universe with time variable space dimension
(TVSD) model, known as decrumpling or TVSD model, we study the time variation
of the gravitational coupling constant. Using observational bounds on the
present time variation of the gravitational Newton's constant in
three-dimensional space w... | [
{
"created": "Tue, 13 Dec 2005 11:04:33 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Apr 2006 16:12:15 GMT",
"version": "v2"
},
{
"created": "Thu, 18 Oct 2007 15:33:03 GMT",
"version": "v3"
}
] | 2007-10-18 | [
[
"Nasseri",
"Forough",
""
]
] | Within the framework of a model universe with time variable space dimension (TVSD) model, known as decrumpling or TVSD model, we study the time variation of the gravitational coupling constant. Using observational bounds on the present time variation of the gravitational Newton's constant in three-dimensional space we ... | 8.102397 | 5.078004 | 6.716227 | 5.569993 | 5.332122 | 5.244657 | 5.057997 | 4.980711 | 5.289766 | 7.892942 | 5.834372 | 6.897774 | 7.419671 | 6.967271 | 7.089635 | 6.869818 | 6.777055 | 6.58433 | 7.003976 | 7.092812 | 6.641777 |
1203.6281 | Gang Chen | Gang Chen | Ward Identity implied recursion relations in Yang-Mills theory | 10 pages, 3 figures | null | 10.1103/PhysRevD.86.027701 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Ward identity in gauge theory constrains the behavior of the amplitudes.
We discuss the Ward identity for amplitudes with a pair of shifted lines with
complex momenta. This will induce a recursion relation identical to BCFW
recursion relations at the finite poles of the complexified amplitudes.
Furthermore, accor... | [
{
"created": "Wed, 28 Mar 2012 14:36:33 GMT",
"version": "v1"
},
{
"created": "Thu, 5 Apr 2012 11:31:59 GMT",
"version": "v2"
}
] | 2013-05-30 | [
[
"Chen",
"Gang",
""
]
] | The Ward identity in gauge theory constrains the behavior of the amplitudes. We discuss the Ward identity for amplitudes with a pair of shifted lines with complex momenta. This will induce a recursion relation identical to BCFW recursion relations at the finite poles of the complexified amplitudes. Furthermore, accordi... | 12.894899 | 12.349771 | 12.00425 | 11.221118 | 11.203668 | 12.230613 | 10.214957 | 11.591691 | 11.680639 | 12.840986 | 11.510817 | 11.358561 | 11.848639 | 11.800187 | 11.79421 | 11.414376 | 11.651127 | 11.303665 | 11.707053 | 11.504715 | 11.628014 |
0708.3933 | Gregory Korchemsky | B. Basso, G. P. Korchemsky, J. Kotanski | Cusp anomalous dimension in maximally supersymmetric Yang-Mills theory
at strong coupling | 5 pages. v3: minor corrections, references and important note added | Phys.Rev.Lett.100:091601, 2008 | 10.1103/PhysRevLett.100.091601 | LPT-Orsay-07-74 | hep-th hep-ph | null | We construct an exact analytical solution to the integral equation which is
believed to describe logarithmic growth of the anomalous dimensions of high
spin operators in planar N=4 super Yang-Mills theory and use it to determine
the strong coupling expansion of the cusp anomalous dimension.
| [
{
"created": "Wed, 29 Aug 2007 10:58:08 GMT",
"version": "v1"
},
{
"created": "Sun, 2 Sep 2007 06:30:06 GMT",
"version": "v2"
},
{
"created": "Thu, 24 Jan 2008 08:10:57 GMT",
"version": "v3"
}
] | 2011-01-28 | [
[
"Basso",
"B.",
""
],
[
"Korchemsky",
"G. P.",
""
],
[
"Kotanski",
"J.",
""
]
] | We construct an exact analytical solution to the integral equation which is believed to describe logarithmic growth of the anomalous dimensions of high spin operators in planar N=4 super Yang-Mills theory and use it to determine the strong coupling expansion of the cusp anomalous dimension. | 7.103901 | 5.749059 | 6.831248 | 5.228742 | 5.470266 | 5.785821 | 5.543973 | 5.767746 | 5.70022 | 5.306513 | 5.242527 | 5.507928 | 6.396369 | 5.509034 | 5.861762 | 5.58476 | 5.598293 | 5.751482 | 5.408793 | 6.363191 | 5.65625 |
2312.17126 | Zheyan Wan | Zheyan Wan, Juven Wang, Shing-Tung Yau, Yi-Zhuang You | C-R-T Fractionalization, Fermions, and Mod 8 Periodicity | 39 pages, 5 figures, 17 tables, see C-P-T fractionalization in
arXiv:2109.15320, and an application of domain wall dimensional reduction in
arXiv:2312.14928 | null | null | null | hep-th cond-mat.str-el hep-ph | http://creativecommons.org/licenses/by/4.0/ | Charge conjugation (C), mirror reflection (R), time reversal (T), and fermion
parity $(-1)^{\rm F}$ are basic discrete spacetime and internal symmetries of
the Dirac fermions. In this article, we determine the group, called the C-R-T
fractionalization, which is a group extension of $\mathbb{Z}_2^{\rm
C}\times\mathbb{... | [
{
"created": "Thu, 28 Dec 2023 17:04:36 GMT",
"version": "v1"
}
] | 2024-01-19 | [
[
"Wan",
"Zheyan",
""
],
[
"Wang",
"Juven",
""
],
[
"Yau",
"Shing-Tung",
""
],
[
"You",
"Yi-Zhuang",
""
]
] | Charge conjugation (C), mirror reflection (R), time reversal (T), and fermion parity $(-1)^{\rm F}$ are basic discrete spacetime and internal symmetries of the Dirac fermions. In this article, we determine the group, called the C-R-T fractionalization, which is a group extension of $\mathbb{Z}_2^{\rm C}\times\mathbb{Z}... | 4.463328 | 4.404744 | 4.637433 | 4.47236 | 4.52779 | 4.684536 | 4.602247 | 4.50258 | 4.35472 | 5.056184 | 4.482791 | 4.321926 | 4.459164 | 4.272992 | 4.330196 | 4.271563 | 4.337599 | 4.336481 | 4.293643 | 4.510507 | 4.348484 |
hep-th/0004081 | Christian Hilmoine | Christian Hilmoine, Rune Niclasen | The Microscopic Spectral Density of the Dirac Operator derived from
Gaussian Orthogonal and Symplectic Ensembles | 35 pages, 8 figures, Some equations simplified | Phys.Rev. D62 (2000) 096013 | 10.1103/PhysRevD.62.096013 | null | hep-th | null | The microscopic spectral correlations of the Dirac operator in Yang-Mills
theories coupled to fermions in (2+1) dimensions can be related to three
universality classes of Random Matrix Theory. In the microscopic limit the
Orthogonal Ensemble (OE) corresponds to a theory with 2 colors and fermions in
the fundamental r... | [
{
"created": "Tue, 11 Apr 2000 19:45:19 GMT",
"version": "v1"
},
{
"created": "Fri, 12 May 2000 11:09:48 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Hilmoine",
"Christian",
""
],
[
"Niclasen",
"Rune",
""
]
] | The microscopic spectral correlations of the Dirac operator in Yang-Mills theories coupled to fermions in (2+1) dimensions can be related to three universality classes of Random Matrix Theory. In the microscopic limit the Orthogonal Ensemble (OE) corresponds to a theory with 2 colors and fermions in the fundamental rep... | 6.716854 | 6.13443 | 7.271957 | 6.20036 | 6.15789 | 6.308689 | 6.24838 | 6.258484 | 6.231 | 6.942627 | 5.963346 | 6.242369 | 6.49447 | 6.081031 | 6.113515 | 6.250956 | 6.082644 | 6.171546 | 6.017528 | 6.387759 | 6.024915 |
1109.5121 | Jean-Francois Dufaux | Jean-Francois Dufaux | Constraints on Cosmic Super-Strings from Kaluza-Klein Emission | v3: misprints corrected and refs. added, to appear in PRL | Phys. Rev. Lett. 109, 011601 (2012) | 10.1103/PhysRevLett.109.011601 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Cosmic super-strings interact generically with a tower of light and/or
strongly coupled Kaluza-Klein (KK) modes associated with the geometry of the
internal space. We study the production of KK particles by cosmic super-string
loops, and show that it is constrained by Big Bang Nucleosynthesis. We study
the resulting ... | [
{
"created": "Fri, 23 Sep 2011 16:13:22 GMT",
"version": "v1"
},
{
"created": "Fri, 20 Jan 2012 18:50:29 GMT",
"version": "v2"
},
{
"created": "Fri, 29 Jun 2012 15:39:16 GMT",
"version": "v3"
}
] | 2012-07-20 | [
[
"Dufaux",
"Jean-Francois",
""
]
] | Cosmic super-strings interact generically with a tower of light and/or strongly coupled Kaluza-Klein (KK) modes associated with the geometry of the internal space. We study the production of KK particles by cosmic super-string loops, and show that it is constrained by Big Bang Nucleosynthesis. We study the resulting co... | 9.286269 | 7.102218 | 7.650615 | 7.235282 | 8.929447 | 8.089066 | 9.182302 | 7.729312 | 7.467979 | 9.233044 | 7.574175 | 8.035837 | 8.471395 | 7.685121 | 8.233177 | 8.273808 | 8.546382 | 8.216971 | 7.904683 | 8.301599 | 7.958014 |
1911.10171 | Alexandre Streicher | Alexandre Streicher | SYK Correlators for All Energies | null | null | 10.1007/JHEP02(2020)048 | null | hep-th cond-mat.stat-mech cond-mat.str-el quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Sachdev-Ye-Kitaev (SYK) model, a theory of N Majorana fermions with
q-body interactions, becomes in the large q limit a conformally-broken
Liouville field theory. Taking this limit preserves many interesting properties
of the model, yet makes the theory as a whole much more tractable. Accordingly,
we produce nove... | [
{
"created": "Fri, 22 Nov 2019 18:11:46 GMT",
"version": "v1"
}
] | 2020-03-18 | [
[
"Streicher",
"Alexandre",
""
]
] | The Sachdev-Ye-Kitaev (SYK) model, a theory of N Majorana fermions with q-body interactions, becomes in the large q limit a conformally-broken Liouville field theory. Taking this limit preserves many interesting properties of the model, yet makes the theory as a whole much more tractable. Accordingly, we produce novel ... | 13.69078 | 14.785062 | 14.819799 | 13.534603 | 14.652732 | 14.15189 | 13.966323 | 14.072886 | 13.90208 | 16.128828 | 13.672936 | 13.410508 | 13.694629 | 13.297984 | 13.621244 | 13.608877 | 13.682471 | 13.484034 | 13.235833 | 13.771274 | 13.188833 |
hep-th/9804163 | Nobuyuki Ishibashi | Nobuyuki Ishibashi (KEK) | p-branes from (p-2)-branes in the Bosonic String Theory | 16 pages, latex. The treatment of boundary interactions is corrected | Nucl.Phys. B539 (1999) 107-120 | 10.1016/S0550-3213(98)00718-4 | KEK-TH-570 | hep-th | null | We show that Dirichlet p-brane can be expressed as a configuration of
infinitely many Dirichlet (p-2)-branes in the bosonic string theory. Using this
fact, we interpret the massless fields on the p-brane worldvolume as
deformations of the configuration of the (p-2)-branes. Especially we find that
the worldvolume gaug... | [
{
"created": "Sat, 25 Apr 1998 03:06:00 GMT",
"version": "v1"
},
{
"created": "Fri, 15 May 1998 05:29:02 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Ishibashi",
"Nobuyuki",
"",
"KEK"
]
] | We show that Dirichlet p-brane can be expressed as a configuration of infinitely many Dirichlet (p-2)-branes in the bosonic string theory. Using this fact, we interpret the massless fields on the p-brane worldvolume as deformations of the configuration of the (p-2)-branes. Especially we find that the worldvolume gauge ... | 6.414384 | 4.852944 | 6.166427 | 5.253133 | 5.472672 | 5.241102 | 5.005368 | 5.094011 | 4.870245 | 6.836553 | 4.927062 | 5.171485 | 5.918046 | 5.232748 | 5.366755 | 5.335574 | 5.26232 | 5.399317 | 5.268452 | 6.386059 | 5.173151 |
1207.4753 | Ulf Lindstr\"om | Malin G\"oteman, Ulf Lindstr\"om and Martin Rocek | Semichiral Sigma Models with 4D Hyperkaehler Geometry | 19 pages | null | 10.1007/JHEP01(2013)073 | UUITP-14/12 Uppsala; YITP-SB-12-23 Stony Brook | hep-th math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Semichiral sigma models with a four-dimensional target space do not support
extended N=(4,4) supersymmetries off-shell arXiv:0903.2376, arXiv:0912.4724. We
contribute towards the understanding of the non-manifest on-shell
transformations in (2,2) superspace by analyzing the extended on-shell
supersymmetry of such mod... | [
{
"created": "Thu, 19 Jul 2012 18:33:06 GMT",
"version": "v1"
}
] | 2015-06-05 | [
[
"Göteman",
"Malin",
""
],
[
"Lindström",
"Ulf",
""
],
[
"Rocek",
"Martin",
""
]
] | Semichiral sigma models with a four-dimensional target space do not support extended N=(4,4) supersymmetries off-shell arXiv:0903.2376, arXiv:0912.4724. We contribute towards the understanding of the non-manifest on-shell transformations in (2,2) superspace by analyzing the extended on-shell supersymmetry of such model... | 14.73004 | 12.001635 | 15.815694 | 11.050998 | 12.412049 | 11.348561 | 11.570472 | 12.066287 | 10.888073 | 16.510481 | 12.026898 | 10.915166 | 13.201392 | 12.260582 | 11.90667 | 11.985198 | 11.681486 | 11.976004 | 12.297035 | 13.977946 | 12.461095 |
hep-th/0401108 | Stephen G. Naculich | S. G. Naculich, H. J. Schnitzer, N. Wyllard | Matrix models and N=2 gauge theory | 6 pages, AMSLaTeX (ws-procs9x6.cls included). Presented at QTS3
(Cincinnati, Ohio, Sept. 10-14, 2003) | null | 10.1142/9789812702340_0043 | BRX-TH-530, BOW-PH-130, CERN-PH-TH/2004-005 | hep-th | null | We describe how the ingredients and results of the Seiberg-Witten solution to
N=2 supersymmetric U(N) gauge theory may be obtained from a matrix model.
| [
{
"created": "Thu, 15 Jan 2004 17:51:18 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Naculich",
"S. G.",
""
],
[
"Schnitzer",
"H. J.",
""
],
[
"Wyllard",
"N.",
""
]
] | We describe how the ingredients and results of the Seiberg-Witten solution to N=2 supersymmetric U(N) gauge theory may be obtained from a matrix model. | 10.421498 | 5.536869 | 9.308773 | 6.194093 | 6.194977 | 5.879485 | 5.767665 | 5.81743 | 6.215551 | 9.790874 | 6.122756 | 6.626751 | 8.850121 | 6.742363 | 6.23684 | 6.287122 | 6.576044 | 6.436377 | 6.452227 | 7.837169 | 6.561944 |
hep-th/0510120 | Stephen Adler | Stephen L. Adler | Structure of Fluctuation Terms in the Trace Dynamics Ward Identity | TeX; 14 pages. Dedicated to Rafael Sorkin on the occasion of his 60th
birthday | J.Phys. A39 (2006) 1397-1404 | 10.1088/0305-4470/39/6/013 | null | hep-th hep-ph math-ph math.MP quant-ph | null | We give a detailed analysis of the anti-self-adjoint operator contribution to
the fluctuation terms in the trace dynamics Ward identity. This clarifies the
origin of the apparent inconsistency between two forms of this identity
discussed in Chapter 6 of our recent book on emergent quantum theory.
| [
{
"created": "Fri, 14 Oct 2005 19:00:23 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Adler",
"Stephen L.",
""
]
] | We give a detailed analysis of the anti-self-adjoint operator contribution to the fluctuation terms in the trace dynamics Ward identity. This clarifies the origin of the apparent inconsistency between two forms of this identity discussed in Chapter 6 of our recent book on emergent quantum theory. | 20.169405 | 23.233343 | 22.598734 | 20.07188 | 20.862049 | 21.184473 | 22.627319 | 18.612673 | 20.057222 | 26.887327 | 20.19405 | 20.61434 | 20.485041 | 19.720543 | 20.396168 | 20.698664 | 20.600332 | 19.505629 | 19.467918 | 21.275955 | 20.211699 |
hep-th/0211187 | Tsuda | K. Shima, M. Tsuda and M. Sawaguchi | On linearization of superon-graviton model(SGM) | 10 pages, Latex, some more discussions added | EconfC0306234:586-592,2003 | null | SIT-LP-02/11 | hep-th | null | Referring to the supermultiplet of N=1 supergravity (SUGRA) the linearization
of N=1 SGM action describing the nonlinear supersymmetric (NL SUSY)
gravitational interaction of superon (Nambu-Goldstone fermion) is attempted.
The field contents of on-shell SUGRA supermultiplet are realized as the
composites, though they... | [
{
"created": "Wed, 20 Nov 2002 08:29:48 GMT",
"version": "v1"
},
{
"created": "Tue, 3 Jun 2003 08:36:13 GMT",
"version": "v2"
},
{
"created": "Fri, 20 Jun 2003 07:13:26 GMT",
"version": "v3"
},
{
"created": "Tue, 12 Aug 2003 02:36:00 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Shima",
"K.",
""
],
[
"Tsuda",
"M.",
""
],
[
"Sawaguchi",
"M.",
""
]
] | Referring to the supermultiplet of N=1 supergravity (SUGRA) the linearization of N=1 SGM action describing the nonlinear supersymmetric (NL SUSY) gravitational interaction of superon (Nambu-Goldstone fermion) is attempted. The field contents of on-shell SUGRA supermultiplet are realized as the composites, though they h... | 15.351286 | 10.431773 | 16.042816 | 11.695395 | 10.205976 | 11.355778 | 10.074203 | 10.525544 | 10.698549 | 16.854889 | 11.770583 | 12.128633 | 14.020116 | 12.370744 | 12.409833 | 12.550513 | 11.83379 | 12.406469 | 13.203837 | 13.863329 | 12.522961 |
hep-th/0105139 | Mohammad Garousi | Mohammad R. Garousi | Dirac-Born-Infeld action, Seiberg-Witten map, and Wilson Lines | 24 pages, Latex, revised some parts in such a way that not to be
concluded that the proposed non-commutative action is identical to the DBI
action in the SW limit, references added | Nucl.Phys. B611 (2001) 467-487 | 10.1016/S0550-3213(01)00355-8 | IPM/P-2001/009 | hep-th | null | We write the recently conjectured action for transformation of the ordinary
Born-Infeld action under the Seiberg-Witten map with one open Wilson contour in
a manifestly non-commutative gauge invariant form. This action contains the
non-constant closed string fields, higher order derivatives of the
non-commutative gau... | [
{
"created": "Tue, 15 May 2001 04:53:43 GMT",
"version": "v1"
},
{
"created": "Mon, 28 May 2001 12:31:32 GMT",
"version": "v2"
},
{
"created": "Sat, 7 Jul 2001 09:13:37 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Garousi",
"Mohammad R.",
""
]
] | We write the recently conjectured action for transformation of the ordinary Born-Infeld action under the Seiberg-Witten map with one open Wilson contour in a manifestly non-commutative gauge invariant form. This action contains the non-constant closed string fields, higher order derivatives of the non-commutative gauge... | 8.516157 | 7.667559 | 9.399833 | 7.670815 | 8.240551 | 8.059203 | 7.615983 | 8.071095 | 7.918022 | 8.799068 | 7.607151 | 7.865114 | 8.353991 | 7.782748 | 7.956782 | 7.737814 | 7.860012 | 7.672165 | 7.649584 | 8.290084 | 7.793036 |
1407.1820 | Philip D. Mannheim | Philip D. Mannheim | $PT$ Symmetry, Conformal Symmetry, and the Metrication of
Electromagnetism | 15 pages, revtex4. Version expanded to include explanatory
introduction | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present some interesting connections between $PT$ symmetry and conformal
symmetry. We use them to develop a metricated theory of electromagnetism in
which the electromagnetic field is present in the geometric connection.
However, unlike Weyl who first advanced this possibility, we do not take the
connection to be ... | [
{
"created": "Mon, 7 Jul 2014 19:43:21 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Jul 2014 16:51:39 GMT",
"version": "v2"
},
{
"created": "Wed, 28 Jan 2015 17:19:36 GMT",
"version": "v3"
}
] | 2015-01-29 | [
[
"Mannheim",
"Philip D.",
""
]
] | We present some interesting connections between $PT$ symmetry and conformal symmetry. We use them to develop a metricated theory of electromagnetism in which the electromagnetic field is present in the geometric connection. However, unlike Weyl who first advanced this possibility, we do not take the connection to be re... | 9.733756 | 10.556995 | 9.588252 | 9.30724 | 9.978866 | 10.990804 | 10.486226 | 10.591377 | 9.943649 | 10.112892 | 9.412173 | 9.768421 | 9.434542 | 9.405964 | 9.533619 | 9.515452 | 9.571756 | 9.176287 | 9.714839 | 9.470971 | 9.338758 |
hep-th/9412027 | Senarath P. de Alwis | S. P. de Alwis and N. Ohta | On the Entropy of Quantum Fields in Black Hole Backgrounds | 10 pages, phyzzx (added references) | null | null | COLO-HEP-347, OU-HET 207 | hep-th gr-qc | null | We show that the partition function for a scalar field in a static spacetime
background can be expressed as a functional integral in the corresponding
optical space, and point out that the difference between this and the
functional integral in the original metric is a Liouville type action. A
general formula for the ... | [
{
"created": "Sat, 3 Dec 1994 07:02:09 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Dec 1994 21:57:53 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"de Alwis",
"S. P.",
""
],
[
"Ohta",
"N.",
""
]
] | We show that the partition function for a scalar field in a static spacetime background can be expressed as a functional integral in the corresponding optical space, and point out that the difference between this and the functional integral in the original metric is a Liouville type action. A general formula for the fr... | 9.282858 | 8.618268 | 8.434597 | 7.837416 | 9.044232 | 8.75342 | 8.024738 | 8.472879 | 8.363997 | 8.745647 | 8.566599 | 8.165167 | 8.491659 | 8.546712 | 8.568376 | 8.395648 | 8.370091 | 8.32954 | 8.405363 | 8.226119 | 8.405938 |
hep-th/9703226 | Roman Jackiw | R. Jackiw and S-Y. Pi | Seeking an Even-Parity Mass Term for 3-D Gauge Theory | 11 pages, revtex | Phys.Lett.B403:297-303,1997 | 10.1016/S0370-2693(97)00520-0 | MIT-CTP-2615 | hep-th hep-ph | null | Mass-gap calculations in three-dimensional gauge theories are discussed. Also
we present a Chern--Simons-like mass-generating mechanism which preserves
parity and is realized non-perturbatively.
| [
{
"created": "Mon, 31 Mar 1997 19:06:17 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Jackiw",
"R.",
""
],
[
"Pi",
"S-Y.",
""
]
] | Mass-gap calculations in three-dimensional gauge theories are discussed. Also we present a Chern--Simons-like mass-generating mechanism which preserves parity and is realized non-perturbatively. | 25.999075 | 20.888981 | 22.220531 | 16.696728 | 19.432503 | 18.980631 | 19.412231 | 19.007599 | 17.955235 | 19.672474 | 20.990551 | 20.363583 | 20.894867 | 19.6157 | 20.010756 | 21.893801 | 21.271563 | 20.489201 | 19.564665 | 20.121317 | 19.839771 |
1905.04339 | Luca Ciambelli | Luca Ciambelli and Robert G. Leigh | Weyl Connections and their Role in Holography | v5; 27 pages, minor typos corrected | Phys. Rev. D 101, 086020 (2020) | 10.1103/PhysRevD.101.086020 | CPHT-RR020.052019 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is a well-known property of holographic theories that diffeomorphism
invariance in the bulk space-time implies Weyl invariance of the dual
holographic field theory in the sense that the field theory couples to a
conformal class of background metrics. The usual Fefferman-Graham formalism,
which provides us with a h... | [
{
"created": "Fri, 10 May 2019 18:41:59 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Jun 2019 22:28:59 GMT",
"version": "v2"
},
{
"created": "Fri, 1 Nov 2019 14:09:38 GMT",
"version": "v3"
},
{
"created": "Wed, 22 Apr 2020 14:44:26 GMT",
"version": "v4"
},
{
"cre... | 2022-01-31 | [
[
"Ciambelli",
"Luca",
""
],
[
"Leigh",
"Robert G.",
""
]
] | It is a well-known property of holographic theories that diffeomorphism invariance in the bulk space-time implies Weyl invariance of the dual holographic field theory in the sense that the field theory couples to a conformal class of background metrics. The usual Fefferman-Graham formalism, which provides us with a hol... | 8.262439 | 8.43788 | 8.949512 | 8.07866 | 8.594966 | 8.435099 | 8.595386 | 8.2486 | 8.443066 | 8.743524 | 7.911482 | 8.118789 | 8.185689 | 8.194744 | 8.19486 | 8.193712 | 8.177651 | 8.210297 | 8.03364 | 8.140519 | 8.086837 |
hep-th/0406084 | John M. Cornwall | John M. Cornwall | A three-dimensional scalar field theory model of center vortices and its
relation to k-string tensions | 21 pages; RevTeX4; 4 .eps figures | Phys.Rev. D70 (2004) 065005 | 10.1103/PhysRevD.70.065005 | UCLA/04/TEP/5 | hep-th | null | In d=3 SU(N) gauge theory, we study a scalar field theory model of center
vortices that furnishes an approach to the determination of so-called k-string
tensions. This model is constructed from string-like quantum solitons
introduced previously, and exploits the well-known relation between string
partition functions ... | [
{
"created": "Wed, 9 Jun 2004 21:23:01 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Cornwall",
"John M.",
""
]
] | In d=3 SU(N) gauge theory, we study a scalar field theory model of center vortices that furnishes an approach to the determination of so-called k-string tensions. This model is constructed from string-like quantum solitons introduced previously, and exploits the well-known relation between string partition functions an... | 12.459818 | 12.607228 | 12.377247 | 12.181544 | 13.034336 | 12.472672 | 12.369226 | 12.993688 | 11.772906 | 13.700191 | 11.949789 | 11.736963 | 11.964653 | 11.641194 | 11.806313 | 11.990849 | 11.831629 | 11.52103 | 11.5488 | 12.007997 | 12.037326 |
1507.05771 | Rohit Kumar | R. Kumar and Amitabha Lahiri | Dimensional reduction of four-dimensional topologically massive gauge
theory | LaTex File: 10 pages, no figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study topologically massive (B \wedge F) Abelian and non-Abelian gauge
theories in four dimensions, and reduce them to three dimensions by assuming
that the fields do not propagate in one of the spatial directions. For certain
gauge choices the reduced theories are the Jackiw-Pi models of massive gauge
fields.
| [
{
"created": "Tue, 21 Jul 2015 10:05:48 GMT",
"version": "v1"
}
] | 2015-07-22 | [
[
"Kumar",
"R.",
""
],
[
"Lahiri",
"Amitabha",
""
]
] | We study topologically massive (B \wedge F) Abelian and non-Abelian gauge theories in four dimensions, and reduce them to three dimensions by assuming that the fields do not propagate in one of the spatial directions. For certain gauge choices the reduced theories are the Jackiw-Pi models of massive gauge fields. | 10.759976 | 8.307458 | 10.330569 | 8.418745 | 9.711073 | 8.786448 | 8.666383 | 8.611611 | 8.079946 | 12.325224 | 7.715195 | 8.970654 | 10.760987 | 8.550678 | 8.650081 | 9.204002 | 8.604223 | 9.356936 | 8.67472 | 9.644722 | 8.196526 |
hep-th/0112006 | Katrin Wendland | Katrin Wendland | Orbifold Constructions of K3: A Link between Conformal Field Theory and
Geometry | 26 pages; references and clarifying remarks added, minor typos
corrected; final version to be published (Proc. of the Workshop on
"Mathematical Aspects of Orbifold String Theory", Madison, Wisconsin, May
4-8, 2001) | in: Orbifolds in mathematics and physics (Madison, WI, 2001),
333-358, Contemp. Math., 310, Amer. Math. Soc., Providence, RI, 2002 | null | null | hep-th math-ph math.MP | null | We discuss geometric aspects of orbifold conformal field theories in the
moduli space of N=(4,4) superconformal field theories with central charge c=6.
Part of this note consists of a summary of our earlier results on the location
of these theories within the moduli space [NW01,Wen] and the action of a
specific versi... | [
{
"created": "Sat, 1 Dec 2001 18:32:06 GMT",
"version": "v1"
},
{
"created": "Wed, 8 May 2002 05:37:23 GMT",
"version": "v2"
}
] | 2020-04-28 | [
[
"Wendland",
"Katrin",
""
]
] | We discuss geometric aspects of orbifold conformal field theories in the moduli space of N=(4,4) superconformal field theories with central charge c=6. Part of this note consists of a summary of our earlier results on the location of these theories within the moduli space [NW01,Wen] and the action of a specific version... | 10.436189 | 10.066752 | 12.561954 | 10.213861 | 10.054157 | 10.195247 | 10.691483 | 10.024595 | 10.014074 | 12.796949 | 9.587584 | 9.592827 | 10.560117 | 9.575922 | 9.805708 | 9.733108 | 10.006058 | 9.667844 | 9.774023 | 10.101885 | 9.652165 |
2205.00154 | Yutaka Hosotani | Yutaka Hosotani | Universality in Anomaly Flow | 25 pages, 13 figures. Comments and references are added | Prog Theor Exp Phys (2022) | 10.1093/ptep/ptac084 | OU-HET-1144 | hep-th hep-ph | http://creativecommons.org/licenses/by/4.0/ | Universality in anomaly flow by an Aharonov-Bohm (AB) phase $\theta_H$ is
shown in the flat $M^4 \times (S^1/Z_2)$ spacetime and in the Randall-Sundrum
(RS) warped space. We analyze $SU(2)$ gauge theory with doublet fermions. With
orbifold boundary conditions the $U(1)$ part of gauge symmetry remains unbroken
at $\th... | [
{
"created": "Sat, 30 Apr 2022 04:03:03 GMT",
"version": "v1"
},
{
"created": "Tue, 31 May 2022 05:36:46 GMT",
"version": "v2"
}
] | 2022-07-06 | [
[
"Hosotani",
"Yutaka",
""
]
] | Universality in anomaly flow by an Aharonov-Bohm (AB) phase $\theta_H$ is shown in the flat $M^4 \times (S^1/Z_2)$ spacetime and in the Randall-Sundrum (RS) warped space. We analyze $SU(2)$ gauge theory with doublet fermions. With orbifold boundary conditions the $U(1)$ part of gauge symmetry remains unbroken at $\thet... | 6.799668 | 6.914274 | 5.934011 | 6.180856 | 6.859053 | 7.138124 | 6.563226 | 6.685161 | 5.950662 | 6.563654 | 6.68924 | 6.265222 | 5.959176 | 5.973392 | 6.32422 | 6.279202 | 6.367604 | 6.246476 | 6.059503 | 6.264292 | 6.464458 |
hep-th/0004200 | Marty Stock | Frieder Lenz, John W. Negele, Lochlainn O'Raifeartaigh, Michael Thies | Phases and Residual Gauge Symmetries of Higgs Models | 30 pages, LaTeX with amsmath macros; updated to include minor
corrections in proof; email correspondence to J.W. Negele,
negele@mitlns.mit.edu | Annals Phys. 285 (2000) 25-60 | 10.1006/aphy.2000.6072 | FAU-TP3-00/4, DIAS-STP-00-08, MIT-CTP-2974 | hep-th hep-ph | null | After elimination of the redundant variables, gauge theories may still
exhibit symmetries associated with the gauge fields. The role of these residual
gauge symmetries is discussed within the Abelian Higgs model and the
Georgi-Glashow model. In the different phases of these models, these symmetries
are realized diffe... | [
{
"created": "Thu, 27 Apr 2000 21:16:33 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Jul 2000 17:12:49 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Lenz",
"Frieder",
""
],
[
"Negele",
"John W.",
""
],
[
"O'Raifeartaigh",
"Lochlainn",
""
],
[
"Thies",
"Michael",
""
]
] | After elimination of the redundant variables, gauge theories may still exhibit symmetries associated with the gauge fields. The role of these residual gauge symmetries is discussed within the Abelian Higgs model and the Georgi-Glashow model. In the different phases of these models, these symmetries are realized differe... | 8.463181 | 7.664644 | 7.633306 | 7.227934 | 8.107176 | 7.576314 | 7.487331 | 7.071775 | 7.208399 | 7.446313 | 7.214636 | 7.439513 | 7.250825 | 7.2489 | 7.706159 | 7.328223 | 7.488354 | 7.359969 | 7.300459 | 7.452135 | 7.292274 |
2310.15236 | Alexander Zhiboedov | Matthew Dodelson, Cristoforo Iossa, Robin Karlsson, Alexandru
Lupsasca, and Alexander Zhiboedov | Black hole bulk-cone singularities | 63 pages, 17 figures | null | null | CERN-TH-2023-192 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Lorentzian correlators of local operators exhibit surprising singularities in
theories with gravity duals. These are associated with null geodesics in an
emergent bulk geometry. We analyze singularities of the thermal response
function dual to propagation of waves on the AdS Schwarzschild black hole
background. We de... | [
{
"created": "Mon, 23 Oct 2023 18:00:08 GMT",
"version": "v1"
}
] | 2023-10-25 | [
[
"Dodelson",
"Matthew",
""
],
[
"Iossa",
"Cristoforo",
""
],
[
"Karlsson",
"Robin",
""
],
[
"Lupsasca",
"Alexandru",
""
],
[
"Zhiboedov",
"Alexander",
""
]
] | Lorentzian correlators of local operators exhibit surprising singularities in theories with gravity duals. These are associated with null geodesics in an emergent bulk geometry. We analyze singularities of the thermal response function dual to propagation of waves on the AdS Schwarzschild black hole background. We deri... | 11.292856 | 11.75298 | 12.219936 | 10.699021 | 12.03511 | 11.232302 | 12.466045 | 10.964802 | 11.044147 | 12.386738 | 11.36054 | 11.336306 | 10.80401 | 10.820906 | 11.205375 | 11.188257 | 10.943075 | 10.710213 | 10.717393 | 10.90777 | 11.043843 |
1506.05016 | Edi Halyo | Edi Halyo | Extremal Black Hole Entropy from Horizon Conformal Field Theories | 15 pages | null | null | SU-ITP-15/09 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the entropy of extremal $D=4$ Reissner--Nordstrom black holes
can be computed from horizon CFTs with central charges and conformal weights
fixed by the dimensionless Rindler energy. This is possible in the simultaneous
extremal and near horizon limit of the black hole which takes the geometry to
an $AdS_... | [
{
"created": "Tue, 16 Jun 2015 16:12:18 GMT",
"version": "v1"
}
] | 2015-06-17 | [
[
"Halyo",
"Edi",
""
]
] | We show that the entropy of extremal $D=4$ Reissner--Nordstrom black holes can be computed from horizon CFTs with central charges and conformal weights fixed by the dimensionless Rindler energy. This is possible in the simultaneous extremal and near horizon limit of the black hole which takes the geometry to an $AdS_2$... | 10.207736 | 8.43595 | 9.341763 | 8.399834 | 9.288372 | 8.660643 | 8.278029 | 8.706892 | 8.771527 | 10.14362 | 8.35202 | 8.805197 | 8.907571 | 8.294513 | 8.707131 | 8.871331 | 8.539451 | 8.423459 | 8.671075 | 8.68268 | 8.475255 |
2102.04424 | Paolo Valtancoli | P. Valtancoli | On the area of the sphere in a Snyder geometry | 7 pages, no figures | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We compute the area of a generic d-sphere in a Snyder geometry.
| [
{
"created": "Mon, 8 Feb 2021 18:36:02 GMT",
"version": "v1"
}
] | 2021-02-09 | [
[
"Valtancoli",
"P.",
""
]
] | We compute the area of a generic d-sphere in a Snyder geometry. | 67.733116 | 31.738977 | 50.732796 | 33.509251 | 35.223484 | 33.888462 | 44.871986 | 36.36285 | 32.246975 | 56.651752 | 33.62624 | 45.409866 | 55.799919 | 45.632732 | 43.309822 | 43.107498 | 43.630787 | 44.443798 | 48.069565 | 49.449272 | 40.456276 |
1610.08968 | Chris Akers | Chris Akers, Jason Koeller, Stefan Leichenauer, Adam Levine | Geometric Constraints from Subregion Duality Beyond the Classical Regime | 27 Pages, 5 Figures, V2: Added citations, fixed typos, V3: Clarified
many issues, replaced a figure, fixed typos | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Subregion duality in AdS/CFT implies certain constraints on the geometry:
entanglement wedges must contain causal wedges, and nested boundary regions
must have nested entanglement wedges. We elucidate the logical connections
between these statements and the Quantum Focussing Conjecture, Quantum Null
Energy Condition,... | [
{
"created": "Thu, 27 Oct 2016 19:56:07 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Oct 2016 19:57:50 GMT",
"version": "v2"
},
{
"created": "Thu, 17 Nov 2016 20:42:43 GMT",
"version": "v3"
}
] | 2016-11-18 | [
[
"Akers",
"Chris",
""
],
[
"Koeller",
"Jason",
""
],
[
"Leichenauer",
"Stefan",
""
],
[
"Levine",
"Adam",
""
]
] | Subregion duality in AdS/CFT implies certain constraints on the geometry: entanglement wedges must contain causal wedges, and nested boundary regions must have nested entanglement wedges. We elucidate the logical connections between these statements and the Quantum Focussing Conjecture, Quantum Null Energy Condition, B... | 8.630546 | 7.137146 | 8.790587 | 7.070457 | 7.586782 | 6.507977 | 6.846264 | 7.549016 | 6.720489 | 10.951576 | 6.551942 | 6.703239 | 7.796741 | 7.224535 | 7.003731 | 7.073959 | 6.682003 | 7.073649 | 7.027075 | 7.528771 | 7.107284 |
hep-th/0312071 | Sungho Hong | Sungho Hong (U. Pennsylvania), Sukjin Yoon, Matthew J. Strassler (U.
Washington) | Quarkonium from the Fifth Dimension | 57 pages, LaTeX, 5 figures | JHEP0404:046,2004 | 10.1088/1126-6708/2004/04/046 | UW/PT 03-31, UPR-1057-T | hep-th | null | Adding fundamental matter of mass m_Q to N=4 Yang Mills theory, we study
quarkonium, and "generalized quarkonium" containing light adjoint particles. At
large 't Hooft coupling the states of spin<=1 are anomalously light (Kruczenski
et al., hep-th/0304032). We examine their form factors, and show these hadrons
are un... | [
{
"created": "Fri, 5 Dec 2003 21:22:33 GMT",
"version": "v1"
},
{
"created": "Mon, 8 Dec 2003 23:20:34 GMT",
"version": "v2"
},
{
"created": "Sat, 20 Mar 2004 00:49:58 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Hong",
"Sungho",
"",
"U. Pennsylvania"
],
[
"Yoon",
"Sukjin",
"",
"U.\n Washington"
],
[
"Strassler",
"Matthew J.",
"",
"U.\n Washington"
]
] | Adding fundamental matter of mass m_Q to N=4 Yang Mills theory, we study quarkonium, and "generalized quarkonium" containing light adjoint particles. At large 't Hooft coupling the states of spin<=1 are anomalously light (Kruczenski et al., hep-th/0304032). We examine their form factors, and show these hadrons are unli... | 15.040378 | 13.736744 | 15.802604 | 13.330838 | 14.474822 | 13.73363 | 13.570399 | 14.779222 | 13.362198 | 16.431513 | 13.168994 | 13.437502 | 14.417059 | 13.576095 | 13.92513 | 13.458368 | 13.755716 | 13.007934 | 13.815772 | 14.169788 | 14.219112 |
hep-th/0203267 | Michael Haack | Sergei Gukov and Michael Haack | IIA String Theory on Calabi-Yau Fourfolds with Background Fluxes | 39 pages, no figures, references added | Nucl.Phys. B639 (2002) 95-128 | 10.1016/S0550-3213(02)00442-X | ROM2F/2002/07, ITEP-TH-07/02, HUTP-01/A074 | hep-th | null | Looking for string vacua with fixed moduli, we study compactifications of
type IIA string theory on Calabi-Yau fourfolds in the presence of generic
Ramond-Ramond fields. We explicitly derive the (super)potential induced by
Ramond-Ramond fluxes performing a Kaluza-Klein reduction of the ten-dimensional
effective actio... | [
{
"created": "Thu, 28 Mar 2002 09:00:02 GMT",
"version": "v1"
},
{
"created": "Tue, 9 Apr 2002 08:57:21 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Gukov",
"Sergei",
""
],
[
"Haack",
"Michael",
""
]
] | Looking for string vacua with fixed moduli, we study compactifications of type IIA string theory on Calabi-Yau fourfolds in the presence of generic Ramond-Ramond fields. We explicitly derive the (super)potential induced by Ramond-Ramond fluxes performing a Kaluza-Klein reduction of the ten-dimensional effective action.... | 6.702888 | 5.857594 | 7.327041 | 6.052011 | 6.512019 | 6.432407 | 6.265884 | 6.329738 | 6.372543 | 7.430622 | 6.296627 | 6.0371 | 6.321249 | 6.067783 | 6.228271 | 6.107457 | 6.000853 | 6.169733 | 6.122237 | 6.331928 | 6.031868 |
1207.5388 | Ram Brustein | Ram Brustein, A. J. M. Medved | Universal stress-tensor correlation functions of strongly coupled
conformal fluids | v2: 23 pages, 1 figure, substantial additions, clarifications and
explanations. In particular about the relationship to experiment. Figure
includes more panels, added references. Version replaced to match published
version | null | 10.1016/j.physletb.2013.06.002 | null | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have shown in two accompanying papers that, for Einstein gravity, the
graviton multi-point functions are universal in a particular kinematic region
and depend only on the (generalized) Mandelstam variable s. The effects of the
leading corrections to Einstein gravity were shown to be similarly universal,
inducing a... | [
{
"created": "Mon, 23 Jul 2012 13:32:15 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Jun 2013 13:14:16 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Brustein",
"Ram",
""
],
[
"Medved",
"A. J. M.",
""
]
] | We have shown in two accompanying papers that, for Einstein gravity, the graviton multi-point functions are universal in a particular kinematic region and depend only on the (generalized) Mandelstam variable s. The effects of the leading corrections to Einstein gravity were shown to be similarly universal, inducing a s... | 9.578274 | 9.45423 | 9.39762 | 9.152279 | 9.982373 | 9.74178 | 10.28985 | 9.506841 | 9.074767 | 10.040501 | 9.583359 | 9.278488 | 9.244547 | 9.079868 | 9.209301 | 9.098379 | 9.200235 | 9.021096 | 9.01723 | 9.112694 | 9.321988 |
1910.14612 | Junjie Rao | Junjie Rao | All-loop Mondrian Reduction of 4-particle Amplituhedron at Positive
Infinity | 19 pages, 14 figures | Nucl. Phys. B 957C (2020) 115086 | 10.1016/j.nuclphysb.2020.115086 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article introduces a systematic framework to understand (not to derive
yet) the all-loop 4-particle amplituhedron in planar N=4 SYM, utilizing both
positivity and the Mondrian diagrammatics. Its key idea is the simplest one so
far: we can decouple one or more sets of loop variables (x,y,z,w) from the rest
by jus... | [
{
"created": "Thu, 31 Oct 2019 17:00:22 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Jun 2020 16:40:54 GMT",
"version": "v2"
}
] | 2020-06-23 | [
[
"Rao",
"Junjie",
""
]
] | This article introduces a systematic framework to understand (not to derive yet) the all-loop 4-particle amplituhedron in planar N=4 SYM, utilizing both positivity and the Mondrian diagrammatics. Its key idea is the simplest one so far: we can decouple one or more sets of loop variables (x,y,z,w) from the rest by just ... | 16.803503 | 16.893845 | 18.729242 | 16.629118 | 18.53767 | 19.031918 | 18.057991 | 17.457533 | 17.323624 | 21.999781 | 16.198811 | 16.062952 | 16.592087 | 16.801382 | 15.691056 | 16.397621 | 16.132982 | 15.933591 | 16.382866 | 16.753651 | 15.749077 |
hep-th/9805206 | David R. Morrison | Paul S. Aspinwall and David R. Morrison | Non-Simply-Connected Gauge Groups and Rational Points on Elliptic Curves | 15 pages, 2 embedded figures, some spurious U(1)'s removed | JHEP 9807 (1998) 012 | 10.1088/1126-6708/1998/07/012 | DUKE-CGTP-98-02, NSF-ITP-98-027 | hep-th | null | We consider the F-theory description of non-simply-connected gauge groups
appearing in the E8 x E8 heterotic string. The analysis is closely tied to the
arithmetic of torsion points on an elliptic curve. The general form of the
corresponding elliptic fibration is given for all finite subgroups of E8 which
are applica... | [
{
"created": "Thu, 28 May 1998 21:45:49 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Dec 1998 15:29:28 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Aspinwall",
"Paul S.",
""
],
[
"Morrison",
"David R.",
""
]
] | We consider the F-theory description of non-simply-connected gauge groups appearing in the E8 x E8 heterotic string. The analysis is closely tied to the arithmetic of torsion points on an elliptic curve. The general form of the corresponding elliptic fibration is given for all finite subgroups of E8 which are applicabl... | 6.913118 | 6.835183 | 7.615631 | 6.547951 | 6.524787 | 6.473776 | 6.991479 | 5.971571 | 6.534251 | 7.238034 | 6.782563 | 6.797136 | 7.2928 | 6.534463 | 6.540467 | 6.851696 | 6.622346 | 6.404057 | 6.596058 | 7.193808 | 6.460906 |
hep-th/0307262 | Mikhail Ivanov | M. G. Ivanov | The models of delocalized membranes | 5 pages, LaTeX | Grav.Cosmol. 9 (2003) 45-49 | null | null | hep-th | null | The generally adopted approach in theory of relativistic strings and
membranes, is similar to use of Lagrange coordinates in continious media
mechanics. One can use an alternative approach, which is similar to use of
Euler coordinates. Under such approach the consideration of thick (delocalized)
membranes is natural.... | [
{
"created": "Sun, 27 Jul 2003 10:23:39 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ivanov",
"M. G.",
""
]
] | The generally adopted approach in theory of relativistic strings and membranes, is similar to use of Lagrange coordinates in continious media mechanics. One can use an alternative approach, which is similar to use of Euler coordinates. Under such approach the consideration of thick (delocalized) membranes is natural. M... | 17.925705 | 18.923958 | 17.951191 | 16.796181 | 19.212286 | 17.289265 | 18.610359 | 16.54031 | 18.465586 | 18.696861 | 16.309824 | 17.722103 | 16.879831 | 17.131485 | 17.017998 | 17.613531 | 17.119808 | 17.364359 | 17.254107 | 17.232143 | 16.703978 |
hep-th/9311145 | Jacek Rozynek | Kostas Vlachos and Anna Okopinska | Optimized Perturbation Methods for the Free Energy of the Anharmonic
Oscillator | 8 pages, preprint | Phys.Lett. A186 (1994) 375-381 | 10.1016/0375-9601(94)90697-1 | null | hep-th | null | Two possibile applications of the optimized expansion for the free energy of
the quantum-mechanical anharmonic oscillator are discussed. The first method is
for the finite temperature effective potential; the second one, for the
classical effective potential. The results of both methods show a quick
convergence and a... | [
{
"created": "Wed, 24 Nov 1993 10:33:20 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Vlachos",
"Kostas",
""
],
[
"Okopinska",
"Anna",
""
]
] | Two possibile applications of the optimized expansion for the free energy of the quantum-mechanical anharmonic oscillator are discussed. The first method is for the finite temperature effective potential; the second one, for the classical effective potential. The results of both methods show a quick convergence and agr... | 19.567921 | 17.459743 | 19.28595 | 18.131643 | 22.025145 | 24.370573 | 23.590933 | 21.559963 | 18.804247 | 17.914324 | 17.254541 | 18.950195 | 17.355221 | 17.678919 | 17.670748 | 18.420528 | 17.614782 | 17.74682 | 17.151201 | 18.397034 | 18.118656 |
1712.09937 | Henriette Elvang | Henriette Elvang, Callum R. T. Jones, Marios Hadjiantonis, and Shruti
Paranjape | On the Supersymmetrization of Galileon Theories in Four Dimensions | 8 pages, no figures | null | 10.1016/j.physletb.2018.04.032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use on-shell amplitude techniques to study the possible $\mathcal{N}=1$
supersymmetrizations of Galileon theories in 3+1 dimensions, both in the limit
of decoupling from DBI and without. Our results are that (1) the quartic
Galileon has a supersymmetrization compatible with Galileon shift symmetry
($\phi \to \phi ... | [
{
"created": "Thu, 28 Dec 2017 17:14:46 GMT",
"version": "v1"
}
] | 2018-05-02 | [
[
"Elvang",
"Henriette",
""
],
[
"Jones",
"Callum R. T.",
""
],
[
"Hadjiantonis",
"Marios",
""
],
[
"Paranjape",
"Shruti",
""
]
] | We use on-shell amplitude techniques to study the possible $\mathcal{N}=1$ supersymmetrizations of Galileon theories in 3+1 dimensions, both in the limit of decoupling from DBI and without. Our results are that (1) the quartic Galileon has a supersymmetrization compatible with Galileon shift symmetry ($\phi \to \phi +c... | 5.453156 | 6.146262 | 5.596045 | 5.456935 | 5.782347 | 5.792629 | 5.733794 | 5.744349 | 5.797743 | 6.15893 | 5.480558 | 5.658437 | 5.532793 | 5.531496 | 5.444296 | 5.450868 | 5.515585 | 5.480389 | 5.36305 | 5.50268 | 5.342295 |
hep-th/9206079 | Nemanja M. Kaloper | Nemanja Kaloper | Stringy Cosmic Strings and Axion Cohomology | 22 pages (plain TeX), UMN-TH-1024/92 | Phys.Rev. D47 (1993) 2403-2410 | 10.1103/PhysRevD.47.2403 | null | hep-th | null | The static stationary axially symmetric background ("infinite cosmic string")
of the $D=4$ string theory provided with an axion charge is studied in the
effective theory approach. The most general exact solution is constructed. It
is found that the Kalb-Ramond axion charge, present in the string topology
$R^{3} \time... | [
{
"created": "Fri, 19 Jun 1992 19:00:15 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Kaloper",
"Nemanja",
""
]
] | The static stationary axially symmetric background ("infinite cosmic string") of the $D=4$ string theory provided with an axion charge is studied in the effective theory approach. The most general exact solution is constructed. It is found that the Kalb-Ramond axion charge, present in the string topology $R^{3} \times ... | 17.376074 | 17.493681 | 17.943159 | 14.613139 | 17.101255 | 16.221958 | 17.233862 | 15.835765 | 17.077578 | 17.797001 | 16.054123 | 15.90778 | 16.224751 | 15.518506 | 15.772367 | 16.067142 | 15.965458 | 16.238806 | 15.643371 | 16.0187 | 15.724908 |
hep-th/9912042 | K. A. Saraikin | Kirill Saraikin | Conformal Blocks and Correlators in WZNW Model. I. Genus Zero | LaTeX, 25pp | null | null | ITEP-TH-52/99 | hep-th | null | We consider the free field approach or bosonization technique for the
Wess-Zumino-Novikov-Witten model with arbitrary Kac-Moody algebra on Riemann
surface of genus zero. This subject was much studied previously, and the paper
can be partially taken as a brief survey. The way to obtain well-known
Schechtman-Varchenko ... | [
{
"created": "Mon, 6 Dec 1999 15:01:12 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Saraikin",
"Kirill",
""
]
] | We consider the free field approach or bosonization technique for the Wess-Zumino-Novikov-Witten model with arbitrary Kac-Moody algebra on Riemann surface of genus zero. This subject was much studied previously, and the paper can be partially taken as a brief survey. The way to obtain well-known Schechtman-Varchenko so... | 10.689562 | 11.398187 | 13.767962 | 11.62117 | 12.282045 | 12.356719 | 11.283573 | 11.64741 | 10.935205 | 13.208617 | 11.179511 | 11.059991 | 11.808066 | 10.946283 | 11.151767 | 11.514416 | 11.269669 | 11.33273 | 10.712176 | 11.506021 | 10.767015 |
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