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/0312209 | C. Hofman | Bartomeu Fiol, Christiaan Hofman and Ernesto Lozano-Tellechea | Causal Structure of d=5 Vacua and Axisymmetric Spacetimes | LaTeX, 36 pages, 3 figures; v2: added reference | JHEP 0402 (2004) 034 | 10.1088/1126-6708/2004/02/034 | WIS/35/03-DEC-DPP | hep-th | null | We study the structure of closed timelike curves (CTCs) for the near horizon
limit of the five dimensional BMPV black hole, in its overrotating regime. We
argue that Bousso's holographic screens are inside the chronologically safe
region, extending a similar observation of Boyda et al. hep-th/0212087 for
Goedel type ... | [
{
"created": "Wed, 17 Dec 2003 20:48:33 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Jan 2004 13:12:44 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Fiol",
"Bartomeu",
""
],
[
"Hofman",
"Christiaan",
""
],
[
"Lozano-Tellechea",
"Ernesto",
""
]
] | We study the structure of closed timelike curves (CTCs) for the near horizon limit of the five dimensional BMPV black hole, in its overrotating regime. We argue that Bousso's holographic screens are inside the chronologically safe region, extending a similar observation of Boyda et al. hep-th/0212087 for Goedel type so... | 10.926289 | 12.56215 | 12.164548 | 10.682448 | 10.878454 | 11.347112 | 11.783161 | 11.249012 | 11.032919 | 13.022592 | 11.803361 | 10.451991 | 11.425156 | 10.489974 | 10.355967 | 10.397592 | 10.597829 | 10.452963 | 10.257074 | 10.384479 | 10.046977 |
hep-th/9801159 | Nick Evans | Nick Evans (Boston University) | Quark Condensates in Non-Supersymmetric MQCD | 16 pages, 1 ps figure, corrected some typos, updated references | Nucl.Phys. B532 (1998) 124-136 | 10.1016/S0550-3213(98)00455-6 | BUHEP-98-03 | hep-th | null | A set of non-supersymmetric minimal area embeddings of an M-theory 5-brane
are considered. The field theories on the surface of the 5-brane have the field
content of N=2 SQCD with fundamental representation matter fields. By suitable
choice of curve parameters the N=2 and N=1 superpartners may be decoupled
leaving a ... | [
{
"created": "Fri, 23 Jan 1998 18:33:10 GMT",
"version": "v1"
},
{
"created": "Sun, 14 Jun 1998 16:05:24 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Evans",
"Nick",
"",
"Boston University"
]
] | A set of non-supersymmetric minimal area embeddings of an M-theory 5-brane are considered. The field theories on the surface of the 5-brane have the field content of N=2 SQCD with fundamental representation matter fields. By suitable choice of curve parameters the N=2 and N=1 superpartners may be decoupled leaving a se... | 14.274741 | 13.59549 | 13.994508 | 13.286511 | 12.985713 | 13.92367 | 13.163849 | 14.418087 | 13.479555 | 14.905948 | 12.492147 | 12.894552 | 12.746071 | 12.93306 | 13.721952 | 13.362796 | 13.382915 | 12.939203 | 13.449695 | 12.565259 | 12.501098 |
0705.3440 | Klaus Bering | K. Bering | Semidensities, Second-Class Constraints and Conversion in Anti-Poisson
Geometry | 32 pages, LaTeX. v2: Minor changes. v3: Published version | J.Math.Phys.49:043516,2008 | 10.1063/1.2890672 | null | hep-th math-ph math.MP math.SG | null | We consider Khudaverdian's geometric version of a Batalin-Vilkovisky (BV)
operator \Delta_E in the case of a degenerate anti-Poisson manifold. The
characteristic feature of such an operator (aside from being a Grassmann-odd,
nilpotent, second-order differential operator) is that it sends semidensities
to semidensitie... | [
{
"created": "Wed, 23 May 2007 18:09:57 GMT",
"version": "v1"
},
{
"created": "Sun, 30 Sep 2007 09:48:48 GMT",
"version": "v2"
},
{
"created": "Fri, 25 Apr 2008 19:12:48 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Bering",
"K.",
""
]
] | We consider Khudaverdian's geometric version of a Batalin-Vilkovisky (BV) operator \Delta_E in the case of a degenerate anti-Poisson manifold. The characteristic feature of such an operator (aside from being a Grassmann-odd, nilpotent, second-order differential operator) is that it sends semidensities to semidensities.... | 8.722985 | 8.039279 | 10.464565 | 7.68287 | 8.444016 | 8.140632 | 8.158395 | 8.413925 | 7.64778 | 10.798891 | 8.058334 | 8.353833 | 8.611905 | 7.943402 | 8.182667 | 7.782438 | 8.175492 | 7.90573 | 7.947393 | 8.962605 | 7.885684 |
1109.3552 | Derek Harland | Derek Harland and Christoph N\"olle | Instantons and Killing spinors | 40 pages, 2 figures v2: author email addresses and affiliations added | JHEP03(2012)082 | 10.1007/JHEP03(2012)082 | ITP-UH-08/11; DCPT-11/47 | hep-th math-ph math.DG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate instantons on manifolds with Killing spinors and their cones.
Examples of manifolds with Killing spinors include nearly Kaehler 6-manifolds,
nearly parallel G_2-manifolds in dimension 7, Sasaki-Einstein manifolds, and
3-Sasakian manifolds. We construct a connection on the tangent bundle over
these mani... | [
{
"created": "Fri, 16 Sep 2011 08:57:56 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Sep 2011 15:21:48 GMT",
"version": "v2"
}
] | 2015-03-19 | [
[
"Harland",
"Derek",
""
],
[
"Nölle",
"Christoph",
""
]
] | We investigate instantons on manifolds with Killing spinors and their cones. Examples of manifolds with Killing spinors include nearly Kaehler 6-manifolds, nearly parallel G_2-manifolds in dimension 7, Sasaki-Einstein manifolds, and 3-Sasakian manifolds. We construct a connection on the tangent bundle over these manifo... | 5.055245 | 5.664999 | 6.0272 | 5.024531 | 5.480489 | 5.780964 | 5.369212 | 5.051914 | 5.057318 | 6.318558 | 5.147735 | 5.055247 | 5.281332 | 5.146271 | 5.073053 | 5.095501 | 4.968633 | 4.951858 | 5.074766 | 5.57244 | 4.977327 |
2107.09674 | James Bonifacio | James Bonifacio | Bootstrap Bounds on Closed Hyperbolic Manifolds | 32 pages, 10 figures | null | 10.1007/JHEP02(2022)025 | null | hep-th math.DG math.SP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The eigenvalues of the Laplace-Beltrami operator and the integrals of
products of eigenfunctions must satisfy certain consistency conditions on
compact Riemannian manifolds. These consistency conditions are derived by using
spectral decompositions to write quadruple overlap integrals in terms of
products of triple ov... | [
{
"created": "Tue, 20 Jul 2021 18:00:00 GMT",
"version": "v1"
}
] | 2022-02-23 | [
[
"Bonifacio",
"James",
""
]
] | The eigenvalues of the Laplace-Beltrami operator and the integrals of products of eigenfunctions must satisfy certain consistency conditions on compact Riemannian manifolds. These consistency conditions are derived by using spectral decompositions to write quadruple overlap integrals in terms of products of triple over... | 5.384152 | 5.336504 | 6.235285 | 5.382851 | 5.636123 | 5.478837 | 5.710154 | 5.508921 | 5.331875 | 6.224277 | 5.20168 | 5.275715 | 5.37328 | 5.169001 | 5.208891 | 5.11586 | 5.237033 | 5.167273 | 5.198418 | 5.349922 | 5.178908 |
hep-th/9508118 | Waichi Ogura | Yukinori Yasui (Osaka City U.) and Waichi Ogura (Osaka U.) | Vortex Filament in Three-manifold and the Duistermaat-Heckman Formula | Revised to include Figure2 (a PostScript file). 15 pages, LaTex2e, 2
figures | null | 10.1016/0375-9601(95)00906-X | OU-HET 219 | hep-th | null | Symplectic geometry of the vortex filament in a curved three-manifold is
investigated. There appears an infinite sequence of constants of motion in
involution in the case of constant curvature. The Duistermaat-Heckman formula
is examined perturbatively for the classical partition function in our model
and verified up... | [
{
"created": "Thu, 24 Aug 1995 08:22:35 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Sep 1995 06:57:39 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Sep 1995 12:31:35 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"Yasui",
"Yukinori",
"",
"Osaka City U."
],
[
"Ogura",
"Waichi",
"",
"Osaka U."
]
] | Symplectic geometry of the vortex filament in a curved three-manifold is investigated. There appears an infinite sequence of constants of motion in involution in the case of constant curvature. The Duistermaat-Heckman formula is examined perturbatively for the classical partition function in our model and verified up t... | 12.199884 | 11.234383 | 13.352933 | 10.746345 | 10.429035 | 12.108004 | 10.925877 | 10.708409 | 11.494261 | 16.40799 | 10.589721 | 11.024271 | 12.031116 | 11.181602 | 11.642352 | 11.285023 | 11.773959 | 11.341237 | 11.617629 | 12.345482 | 11.116654 |
hep-th/9704006 | Hossein Sarmadi | E. Gava, K.S. Narain and M.H. Sarmadi | On the Bound States of p- and (p+2)-Branes | 34 pages, Latex | Nucl.Phys. B504 (1997) 214-238 | 10.1016/S0550-3213(97)00508-7 | IC/97/24 | hep-th | null | We study bound states of D-p-branes and D-(p+2)-branes. By switching on a
large magnetic field F on the (p+2) brane, the problem is shown to admit a
perturbative analysis in an expansion in inverse powers of F. It is found that,
to the leading order in 1/F, the quartic potential of the tachyonic state from
the open s... | [
{
"created": "Tue, 1 Apr 1997 18:59:17 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Gava",
"E.",
""
],
[
"Narain",
"K. S.",
""
],
[
"Sarmadi",
"M. H.",
""
]
] | We study bound states of D-p-branes and D-(p+2)-branes. By switching on a large magnetic field F on the (p+2) brane, the problem is shown to admit a perturbative analysis in an expansion in inverse powers of F. It is found that, to the leading order in 1/F, the quartic potential of the tachyonic state from the open str... | 7.657797 | 8.148599 | 9.011853 | 7.755022 | 8.188819 | 8.071067 | 8.208324 | 7.854598 | 7.693118 | 10.02982 | 7.753755 | 7.541801 | 8.284646 | 7.723134 | 7.60574 | 7.578943 | 7.702662 | 7.676771 | 7.551635 | 8.166298 | 7.424824 |
2112.01196 | Ian Jack | I. Jack and D.R.T. Jones | Scaling dimensions at large charge for cubic $\phi^3$ theory in six
dimensions | 14 pages, 2 figures, reference added, typos corrected | null | 10.1103/PhysRevD.105.045021 | LTH1284 | hep-th | http://creativecommons.org/licenses/by/4.0/ | The $O(N)$ model with scalar quartic interactions at its ultraviolet fixed
point, and the $O(N)$ model with scalar cubic interactions at its infra-red
fixed point are conjectured to be equivalent. This has been checked by
comparing various features of the two models at their respective fixed points.
Recently, the sca... | [
{
"created": "Thu, 2 Dec 2021 13:08:22 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Dec 2021 09:22:15 GMT",
"version": "v2"
},
{
"created": "Sun, 6 Feb 2022 11:24:14 GMT",
"version": "v3"
},
{
"created": "Tue, 28 Jun 2022 16:22:39 GMT",
"version": "v4"
}
] | 2022-06-29 | [
[
"Jack",
"I.",
""
],
[
"Jones",
"D. R. T.",
""
]
] | The $O(N)$ model with scalar quartic interactions at its ultraviolet fixed point, and the $O(N)$ model with scalar cubic interactions at its infra-red fixed point are conjectured to be equivalent. This has been checked by comparing various features of the two models at their respective fixed points. Recently, the scali... | 7.038767 | 6.54936 | 7.496783 | 6.513779 | 6.877381 | 6.882556 | 6.704854 | 6.684648 | 6.891057 | 7.241679 | 6.638271 | 6.583612 | 7.062672 | 6.87314 | 6.787032 | 6.630344 | 6.79111 | 6.784137 | 6.752426 | 6.858915 | 6.853003 |
2110.01956 | Matheus Ara\'ujo Marques | D. Bazeia, M.A. Liao and M.A. Marques | Impurity-like solutions in vortex systems coupled to a neutral field | 6 pages, 5 figures | Phys. Lett. B 825 (2022) 136862 | 10.1016/j.physletb.2021.136862 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, a Maxwell-Higgs system is coupled to a neutral scalar field
that engenders $Z_2$ symmetry. At critical coupling, the resulting field
equations may be identified with those of a Maxwell-Higgs model doped with an
impurity whose form changes according to properties of the neutral scalar
field, such as the ... | [
{
"created": "Tue, 5 Oct 2021 11:36:39 GMT",
"version": "v1"
}
] | 2022-01-06 | [
[
"Bazeia",
"D.",
""
],
[
"Liao",
"M. A.",
""
],
[
"Marques",
"M. A.",
""
]
] | In this work, a Maxwell-Higgs system is coupled to a neutral scalar field that engenders $Z_2$ symmetry. At critical coupling, the resulting field equations may be identified with those of a Maxwell-Higgs model doped with an impurity whose form changes according to properties of the neutral scalar field, such as the to... | 14.067961 | 10.864613 | 13.32535 | 11.805798 | 11.7472 | 11.060713 | 11.606635 | 11.125044 | 11.258985 | 14.159197 | 11.530607 | 11.634624 | 13.566992 | 12.341547 | 12.008447 | 12.323501 | 11.915658 | 12.249698 | 12.4045 | 12.671898 | 12.629298 |
1309.1476 | Alexandros Kehagias | Fotis Farakos, Sergio Ferrara, Alex Kehagias, Massimo Porrati | Supersymmetry Breaking by Higher Dimension Operators | 28 pages | null | 10.1016/j.nuclphysb.2013.12.016 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss a supersymmetry breaking mechanism for N = 1 theories triggered by
higher dimensional op- erators. We consider such operators for real linear and
chiral spinor superfields that break superymmetry and reduce to the
Volkov-Akulov action. We also consider supersymmetry breaking induced by a
higher dimensional... | [
{
"created": "Thu, 5 Sep 2013 20:03:46 GMT",
"version": "v1"
}
] | 2015-06-17 | [
[
"Farakos",
"Fotis",
""
],
[
"Ferrara",
"Sergio",
""
],
[
"Kehagias",
"Alex",
""
],
[
"Porrati",
"Massimo",
""
]
] | We discuss a supersymmetry breaking mechanism for N = 1 theories triggered by higher dimensional op- erators. We consider such operators for real linear and chiral spinor superfields that break superymmetry and reduce to the Volkov-Akulov action. We also consider supersymmetry breaking induced by a higher dimensional o... | 7.58871 | 8.619627 | 8.337986 | 7.67021 | 7.530704 | 7.806948 | 7.962383 | 8.030501 | 7.839569 | 8.916072 | 7.47067 | 7.656483 | 7.491997 | 7.499784 | 7.592985 | 7.71768 | 7.680049 | 7.612512 | 7.684869 | 7.91913 | 7.498384 |
hep-th/9306155 | Vadim Kuznetsov | J. C. Eilbeck, V. Z. Enol'skii, Vadim B. Kuznetsov and A. V. Tsiganov | Linear $r$-matrix algebra for classical separable systems | 15 pages | J.Phys. A27 (1994) 567-578 | 10.1088/0305-4470/27/2/038 | University of Amsterdam Math 93-11 | hep-th nlin.SI solv-int | null | We consider a hierarchy of the natural type Hamiltonian systems of $n$
degrees of freedom with polynomial potentials separable in general ellipsoidal
and general paraboloidal coordinates. We give a Lax representation in terms of
$2\times 2$ matrices for the whole hierarchy and construct the associated
linear $r$-matr... | [
{
"created": "Tue, 29 Jun 1993 09:05:56 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Eilbeck",
"J. C.",
""
],
[
"Enol'skii",
"V. Z.",
""
],
[
"Kuznetsov",
"Vadim B.",
""
],
[
"Tsiganov",
"A. V.",
""
]
] | We consider a hierarchy of the natural type Hamiltonian systems of $n$ degrees of freedom with polynomial potentials separable in general ellipsoidal and general paraboloidal coordinates. We give a Lax representation in terms of $2\times 2$ matrices for the whole hierarchy and construct the associated linear $r$-matrix... | 12.082624 | 11.889502 | 14.130765 | 11.124943 | 11.74048 | 11.10373 | 11.283133 | 10.914005 | 12.539252 | 14.462266 | 11.785926 | 11.046398 | 12.587381 | 11.335193 | 11.423962 | 11.118639 | 12.073519 | 11.340342 | 11.856439 | 11.866147 | 11.241863 |
1509.09056 | Pietro Antonio Grassi | P. Fr\'e, P.A. Grassi, and A.S. Sorin | Hyperinstantons, the Beltrami Equation, and Triholomorphic Maps | 45 pages, Latex2e, 4 figures | null | 10.1002/prop.201500061 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the Beltrami equation for hydrodynamics and we show that its
solutions can be viewed as instanton solutions of a more general system of
equations. The latter are the equations of motion for an ${\cal N}=2$ sigma
model on 4-dimensional worldvolume (which is taken locally HyperK\"ahler) with
a 4-dimensional... | [
{
"created": "Wed, 30 Sep 2015 08:12:38 GMT",
"version": "v1"
}
] | 2016-12-21 | [
[
"Fré",
"P.",
""
],
[
"Grassi",
"P. A.",
""
],
[
"Sorin",
"A. S.",
""
]
] | We consider the Beltrami equation for hydrodynamics and we show that its solutions can be viewed as instanton solutions of a more general system of equations. The latter are the equations of motion for an ${\cal N}=2$ sigma model on 4-dimensional worldvolume (which is taken locally HyperK\"ahler) with a 4-dimensional H... | 8.590343 | 9.208212 | 9.216768 | 8.919669 | 8.82803 | 8.641354 | 9.321494 | 8.695807 | 8.587875 | 9.559878 | 8.621861 | 8.359061 | 8.710001 | 8.289876 | 8.214173 | 8.63444 | 8.377069 | 8.349747 | 8.316758 | 8.358628 | 8.086143 |
1002.3159 | Kristan Jensen | Kristan Jensen, Andreas Karch, Dam T. Son, and Ethan G. Thompson | Holographic Berezinskii-Kosterlitz-Thouless Transitions | 4 pages, 1 figure | Phys.Rev.Lett.105:041601,2010 | 10.1103/PhysRevLett.105.041601 | INT-PUB-10-011 | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find the first example of a quantum Berenzinskii-Kosterlitz-Thouless (BKT)
phase transition in two spatial dimensions via holography. This transition
occurs in the D3/D5 system at nonzero density and magnetic field. At any
nonzero temperature, the BKT scaling is destroyed and the transition becomes
second order wi... | [
{
"created": "Wed, 17 Feb 2010 19:02:58 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Jensen",
"Kristan",
""
],
[
"Karch",
"Andreas",
""
],
[
"Son",
"Dam T.",
""
],
[
"Thompson",
"Ethan G.",
""
]
] | We find the first example of a quantum Berenzinskii-Kosterlitz-Thouless (BKT) phase transition in two spatial dimensions via holography. This transition occurs in the D3/D5 system at nonzero density and magnetic field. At any nonzero temperature, the BKT scaling is destroyed and the transition becomes second order with... | 8.321596 | 5.676414 | 9.144106 | 7.043653 | 7.090935 | 6.330199 | 6.796415 | 6.204198 | 6.448309 | 8.016965 | 6.338679 | 7.065461 | 8.391633 | 7.213803 | 7.300641 | 7.117218 | 7.119067 | 6.68933 | 7.141286 | 8.259018 | 7.148665 |
1511.03008 | Jian-Pin Wu | Xiao-Mei Kuang and Jian-Pin Wu | Transport coefficients from hyperscaling violating black brane: shear
viscosity and conductivity | 16 pages, 4 figures, references added | Phys.Lett. B773 (2017) 422-427 | 10.1016/j.physletb.2017.08.060 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate two transport coefficients, shear viscosity and conductivity,
in a non-relativistic boundary filed theory without hyperscaling symmetry,
which is dual to a bulk charged hyperscaling violating black brane. Employing
matching method, we obtain that the ratio of shear viscosity and the entropy
density is ... | [
{
"created": "Tue, 10 Nov 2015 07:50:39 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Nov 2015 16:40:46 GMT",
"version": "v2"
}
] | 2017-09-13 | [
[
"Kuang",
"Xiao-Mei",
""
],
[
"Wu",
"Jian-Pin",
""
]
] | We investigate two transport coefficients, shear viscosity and conductivity, in a non-relativistic boundary filed theory without hyperscaling symmetry, which is dual to a bulk charged hyperscaling violating black brane. Employing matching method, we obtain that the ratio of shear viscosity and the entropy density is al... | 9.396743 | 8.524295 | 11.184947 | 8.477715 | 8.640398 | 8.65299 | 8.973062 | 8.814916 | 8.723561 | 11.165295 | 8.537525 | 8.94456 | 9.558994 | 8.883351 | 8.814369 | 8.868038 | 9.116921 | 9.021916 | 8.893538 | 9.692658 | 8.747868 |
1407.1256 | Seiya Nishiyama | Seiya Nishiyama and Joao da Providencia | SO(2N)/U(N) Riccati-Hartree-Bogoliubov Equation Based on the SO(2N) Lie
Algebra of the Fermion Operators | Published version, 19 pages. arXiv admin note: text overlap with
arXiv:0712.4208 | International Journal of Geometric Methods in Modern Physics
Vol.12 (2015) 1550035 (26 pages) | 10.1142/S0219887815500358 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we present the induced representation of SO(2N) canonical
transformation group and introduce SO(2N)/U(N) coset variables. We give a
derivation of the time dependent Hartree-Bogoliubov (TDHB) equation on the
Kaehler coset space G/H=SO(2N)/U(N) from the Euler-Lagrange equation of motion
for the coset vari... | [
{
"created": "Fri, 4 Jul 2014 14:58:35 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Jul 2014 09:33:29 GMT",
"version": "v2"
},
{
"created": "Mon, 9 Feb 2015 05:15:42 GMT",
"version": "v3"
}
] | 2015-02-10 | [
[
"Nishiyama",
"Seiya",
""
],
[
"da Providencia",
"Joao",
""
]
] | In this paper we present the induced representation of SO(2N) canonical transformation group and introduce SO(2N)/U(N) coset variables. We give a derivation of the time dependent Hartree-Bogoliubov (TDHB) equation on the Kaehler coset space G/H=SO(2N)/U(N) from the Euler-Lagrange equation of motion for the coset variab... | 10.54579 | 11.891824 | 11.985975 | 11.32337 | 11.412623 | 10.910797 | 11.715796 | 11.409617 | 10.617264 | 13.762589 | 11.09613 | 10.501806 | 11.076178 | 10.59144 | 10.08326 | 10.530107 | 10.217749 | 10.51686 | 10.347891 | 11.736282 | 10.680113 |
hep-th/9509026 | Leon Takhtajan | Leon A. Takhtajan | Equivalence of Geometric h<1/2 and Standard c>25 Approaches to
Two-Dimensional Quantum Gravity | 10 pages, latex | Mod.Phys.Lett. A11 (1996) 93-101 | 10.1142/S0217732396000126 | null | hep-th | null | We show equivalence between the standard weak coupling regime c>25 of the
two-dimensional quantum gravity and regime h<1/2 of the original geometric
approach of Polyakov [1,2], developed in [3,4,5].
| [
{
"created": "Wed, 6 Sep 1995 22:35:49 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Takhtajan",
"Leon A.",
""
]
] | We show equivalence between the standard weak coupling regime c>25 of the two-dimensional quantum gravity and regime h<1/2 of the original geometric approach of Polyakov [1,2], developed in [3,4,5]. | 22.081259 | 17.095055 | 25.426342 | 17.223244 | 16.199436 | 17.618687 | 19.501896 | 20.763186 | 19.151224 | 22.528242 | 16.279541 | 17.078531 | 20.343231 | 17.871058 | 17.177958 | 17.150858 | 18.062965 | 18.211189 | 16.986261 | 21.240772 | 16.222042 |
hep-th/0311057 | M. A. Gonzalez Leon | A. Alonso Izquierdo, M.A. Gonzalez Leon, W. Garcia Fuertes, M. de la
Torre Mayado and J. Mateos Guilarte | Degenerate BPS Domain Walls: Classical and Quantum Dynamics | 12 pages, 7 figures. To be published in the Proceedings of:
Symmetries And Gravity In Field Theory, Workshop in honour of Prof. J. A. de
Azcarraga. June 9-11, 2003. Salamanca (Spain). References added and minor
corrections | null | null | null | hep-th | null | We discuss classical and quantum aspects of the dynamics of a family of
domain walls arising in a generalized Wess-Zumino model. These domain walls can
be embedded in ${\cal N}=1$ supergravity as exact solutions and are composed of
two basic lumps.
| [
{
"created": "Fri, 7 Nov 2003 11:58:09 GMT",
"version": "v1"
},
{
"created": "Wed, 17 Dec 2003 10:43:41 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Izquierdo",
"A. Alonso",
""
],
[
"Leon",
"M. A. Gonzalez",
""
],
[
"Fuertes",
"W. Garcia",
""
],
[
"Mayado",
"M. de la Torre",
""
],
[
"Guilarte",
"J. Mateos",
""
]
] | We discuss classical and quantum aspects of the dynamics of a family of domain walls arising in a generalized Wess-Zumino model. These domain walls can be embedded in ${\cal N}=1$ supergravity as exact solutions and are composed of two basic lumps. | 10.619411 | 7.00022 | 8.454206 | 7.665762 | 7.976631 | 8.458799 | 7.28631 | 7.144609 | 6.913627 | 8.738843 | 7.305244 | 8.114732 | 9.201012 | 8.212132 | 8.200438 | 8.091552 | 8.092489 | 8.2923 | 8.29905 | 8.812848 | 7.944777 |
1003.2840 | Joohan Lee | Joohan Lee, Tae Hoon Lee, and Phillial Oh | Coupling of Brans-Dicke scalar field with Horava-Lifshitz gravity | 7pages, LATEX | null | 10.1016/j.physletb.2011.06.022 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We look for a Brans-Dicke type of generalization of the Horava-Lifshitz
gravity. It is shown that such a generalization is possible within the detailed
balance condition. Classically, the resulting theory reduces in the IR limit to
the usual Brans-Dicke theory with a negative cosmological constant for certain
values ... | [
{
"created": "Mon, 15 Mar 2010 02:37:26 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Dec 2010 16:19:02 GMT",
"version": "v2"
}
] | 2015-05-18 | [
[
"Lee",
"Joohan",
""
],
[
"Lee",
"Tae Hoon",
""
],
[
"Oh",
"Phillial",
""
]
] | We look for a Brans-Dicke type of generalization of the Horava-Lifshitz gravity. It is shown that such a generalization is possible within the detailed balance condition. Classically, the resulting theory reduces in the IR limit to the usual Brans-Dicke theory with a negative cosmological constant for certain values of... | 7.176768 | 5.848279 | 5.791042 | 5.544276 | 5.727079 | 6.18189 | 5.795437 | 5.675329 | 5.592834 | 5.964868 | 6.194827 | 5.75822 | 6.148396 | 5.832691 | 5.927587 | 5.946945 | 6.114329 | 5.862048 | 5.885385 | 5.947074 | 5.881014 |
0912.4326 | M. P. Garcia del Moral | M.P. Garcia del Moral and A. Restuccia | Non-abelian D=11 Supermembrane | Contribution to the Proceedings of the Dubna International SQS'09
Workshop ("Supersymmetries and Quantum Symmetries-2009", July 29 - August 3,
2009. 12pg, Latex | Phys.Part.Nucl.Lett.8:202-208,2011 | 10.1134/S1547477111030071 | FFUOV-09/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We obtain a U(M) action for supermembranes with central charges in the Light
Cone Gauge (LCG). The theory realizes all of the symmetries and constraints of
the supermembrane together with the invariance under a U(M) gauge group with M
arbitrary. The worldvolume action has (LCG) N=8 supersymmetry and it
corresponds to... | [
{
"created": "Tue, 22 Dec 2009 06:14:59 GMT",
"version": "v1"
}
] | 2011-08-17 | [
[
"del Moral",
"M. P. Garcia",
""
],
[
"Restuccia",
"A.",
""
]
] | We obtain a U(M) action for supermembranes with central charges in the Light Cone Gauge (LCG). The theory realizes all of the symmetries and constraints of the supermembrane together with the invariance under a U(M) gauge group with M arbitrary. The worldvolume action has (LCG) N=8 supersymmetry and it corresponds to M... | 12.96141 | 8.132791 | 15.587525 | 10.832526 | 13.878751 | 7.888573 | 8.528411 | 9.536654 | 10.2269 | 18.03401 | 11.228676 | 11.81373 | 13.953496 | 12.389573 | 12.803892 | 12.118637 | 11.953239 | 11.81549 | 12.429003 | 14.51244 | 11.99118 |
0902.1365 | Carl Bender | Carl M. Bender and Philip D. Mannheim | PT symmetry and necessary and sufficient conditions for the reality of
energy eigenvalues | 11 pages, no figures | Phys.Lett.A374:1616-1620,2010 | 10.1016/j.physleta.2010.02.032 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Despite its common use in quantum theory, the mathematical requirement of
Dirac Hermiticity of a Hamiltonian is sufficient to guarantee the reality of
energy eigenvalues but not necessary. By establishing three theorems, this
paper gives physical conditions that are both necessary and sufficient. First,
it is shown t... | [
{
"created": "Mon, 9 Feb 2009 05:01:18 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Bender",
"Carl M.",
""
],
[
"Mannheim",
"Philip D.",
""
]
] | Despite its common use in quantum theory, the mathematical requirement of Dirac Hermiticity of a Hamiltonian is sufficient to guarantee the reality of energy eigenvalues but not necessary. By establishing three theorems, this paper gives physical conditions that are both necessary and sufficient. First, it is shown tha... | 7.276575 | 7.128055 | 8.302527 | 6.820251 | 7.444153 | 7.761755 | 7.826148 | 7.019768 | 6.653165 | 7.814576 | 7.133237 | 6.93497 | 7.306881 | 6.931996 | 7.094813 | 6.963982 | 6.817564 | 6.968565 | 7.101498 | 7.389492 | 7.359305 |
hep-th/0310223 | Raphael Bousso | Raphael Bousso | Harmonic resolution as a holographic quantum number | 19 pages | JHEP 0403 (2004) 054 | 10.1088/1126-6708/2004/03/054 | null | hep-th | null | The Bekenstein bound takes the holographic principle into the realm of flat
space, promising new insights on the relation of non-gravitational physics to
quantum gravity. This makes it important to obtain a precise formulation of the
bound. Conventionally, one specifies two macroscopic quantities, mass and
spatial wi... | [
{
"created": "Thu, 23 Oct 2003 19:48:38 GMT",
"version": "v1"
},
{
"created": "Sat, 31 Jan 2004 00:01:31 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Bousso",
"Raphael",
""
]
] | The Bekenstein bound takes the holographic principle into the realm of flat space, promising new insights on the relation of non-gravitational physics to quantum gravity. This makes it important to obtain a precise formulation of the bound. Conventionally, one specifies two macroscopic quantities, mass and spatial widt... | 13.453437 | 12.815021 | 14.524087 | 12.811438 | 14.184366 | 14.402283 | 14.155313 | 13.658366 | 13.247675 | 15.376887 | 13.293447 | 13.206955 | 13.571266 | 13.495412 | 13.314686 | 13.314567 | 12.881828 | 12.527063 | 12.840528 | 13.716993 | 13.16095 |
hep-th/0103260 | Bonneau Guy | G. Bonneau and P.Y. Casteill | Dualised sigma-models at the two-loop order | 11 pages, latex file,some references added | Nucl.Phys. B607 (2001) 293-304 | 10.1016/S0550-3213(01)00216-4 | PAR/LPTHE/01-14 | hep-th | null | We adress ourselves the question of the quantum equivalence of non abelian
dualised $\si$-models on the simple example of the T-dualised $SU(2)
\si$-model. This theory is classically canonically equivalent to the standard
chiral $SU(2) \si$-model. It is known that the equivalence also holds at the
first order in pert... | [
{
"created": "Fri, 30 Mar 2001 10:19:24 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Apr 2001 14:32:14 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Bonneau",
"G.",
""
],
[
"Casteill",
"P. Y.",
""
]
] | We adress ourselves the question of the quantum equivalence of non abelian dualised $\si$-models on the simple example of the T-dualised $SU(2) \si$-model. This theory is classically canonically equivalent to the standard chiral $SU(2) \si$-model. It is known that the equivalence also holds at the first order in pertur... | 12.925516 | 10.938475 | 13.510137 | 12.103308 | 11.470101 | 11.50799 | 10.472392 | 11.795683 | 11.180237 | 14.361982 | 10.916623 | 11.119726 | 12.59905 | 12.264815 | 11.670595 | 11.857183 | 12.03406 | 12.032414 | 12.422672 | 12.934864 | 11.78235 |
hep-th/0010103 | C. Hofman | Christiaan Hofman and Jae-Suk Park | Cohomological Yang-Mills Theories on Kahler 3-Folds | 32 pages, LaTeX | Nucl.Phys.B600:133-162,2001 | 10.1016/S0550-3213(01)00024-4 | SPIN-1999/26, ITFA-99-30, RUNHETC-2000-37, CU-TP-957 | hep-th | null | We study topological gauge theories with N=(2,0) supersymmetry based on
stable bundles on general Kahler 3-folds. In order to have a theory that is
well defined and well behaved, we consider a model based on an extension of the
usual holomorphic bundle by including a holomorphic 3-form. The correlation
functions of t... | [
{
"created": "Thu, 12 Oct 2000 18:23:58 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Hofman",
"Christiaan",
""
],
[
"Park",
"Jae-Suk",
""
]
] | We study topological gauge theories with N=(2,0) supersymmetry based on stable bundles on general Kahler 3-folds. In order to have a theory that is well defined and well behaved, we consider a model based on an extension of the usual holomorphic bundle by including a holomorphic 3-form. The correlation functions of the... | 7.929878 | 9.032945 | 8.964381 | 7.864015 | 8.19963 | 8.833443 | 8.622588 | 8.448105 | 7.637482 | 9.452006 | 8.51393 | 7.994256 | 8.584007 | 7.843824 | 7.775942 | 8.127318 | 7.830227 | 7.976831 | 7.801063 | 7.954925 | 7.812634 |
2212.00468 | Michael Ponds | Sergei M. Kuzenko, James La Fontaine and Michael Ponds | Induced action for superconformal higher-spin multiplets using SCFT
techniques | 12 pages; V2: Comments and Appendix A added; V3: Published Version | null | 10.1016/j.physletb.2023.137818 | null | hep-th | http://creativecommons.org/licenses/by-nc-sa/4.0/ | Recently, the interacting $\mathcal{N}=1$ superconformal higher-spin theory
in four dimensions has been proposed within the induced action approach. In
this paper we initiate a program of computing perturbative corrections to the
corresponding action and explicitly evaluate all quadratic terms. This is
achieved by em... | [
{
"created": "Thu, 1 Dec 2022 12:46:47 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Dec 2022 09:36:55 GMT",
"version": "v2"
},
{
"created": "Tue, 14 Mar 2023 01:34:44 GMT",
"version": "v3"
}
] | 2023-04-05 | [
[
"Kuzenko",
"Sergei M.",
""
],
[
"La Fontaine",
"James",
""
],
[
"Ponds",
"Michael",
""
]
] | Recently, the interacting $\mathcal{N}=1$ superconformal higher-spin theory in four dimensions has been proposed within the induced action approach. In this paper we initiate a program of computing perturbative corrections to the corresponding action and explicitly evaluate all quadratic terms. This is achieved by empl... | 10.101521 | 7.571395 | 10.749242 | 8.065099 | 8.904941 | 8.090386 | 8.329711 | 7.926262 | 8.066935 | 11.796127 | 8.574423 | 8.422865 | 9.557638 | 8.540921 | 8.477066 | 8.224628 | 8.333163 | 8.44381 | 8.757904 | 9.221092 | 8.513948 |
0706.0355 | Douglas Lundholm | Volker Bach, Jens Hoppe, Douglas Lundholm | Dynamical Symmetries in Supersymmetric Matrix Models | null | Doc. Math. 13 (2008), 103-116 | null | null | hep-th | null | We reveal a dynamical SU(2) symmetry in the asymptotic description of
supersymmetric matrix models. We also consider a recursive approach for
determining the ground state, and point out some additional properties of the
model(s).
| [
{
"created": "Sun, 3 Jun 2007 22:35:53 GMT",
"version": "v1"
}
] | 2008-11-12 | [
[
"Bach",
"Volker",
""
],
[
"Hoppe",
"Jens",
""
],
[
"Lundholm",
"Douglas",
""
]
] | We reveal a dynamical SU(2) symmetry in the asymptotic description of supersymmetric matrix models. We also consider a recursive approach for determining the ground state, and point out some additional properties of the model(s). | 21.972139 | 17.152996 | 19.004408 | 17.587185 | 18.979326 | 18.619673 | 19.945305 | 18.219654 | 17.262993 | 20.105871 | 18.364683 | 19.530828 | 22.065039 | 19.276659 | 19.386496 | 19.145849 | 19.147635 | 19.203045 | 19.222984 | 21.5348 | 19.552013 |
hep-th/9511168 | Trugenberger Carlo | M. C. Diamantini, P. Sodano, C. A. Trugenberger | Gauge Theories of Josephson Junction Arrays | 39 pages, harvmac, two figures available on request | Nucl.Phys. B474 (1996) 641-677 | 10.1016/0550-3213(96)00309-4 | CERN-TH/95-294 | hep-th cond-mat | null | We show that the zero-temperature physics of planar Josephson junction arrays
in the self-dual approximation is governed by an Abelian gauge theory with
periodic mixed Chern-Simons term describing the charge-vortex coupling. The
periodicity requires the existence of (Euclidean) topological excitations which
determine... | [
{
"created": "Thu, 23 Nov 1995 14:15:18 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Diamantini",
"M. C.",
""
],
[
"Sodano",
"P.",
""
],
[
"Trugenberger",
"C. A.",
""
]
] | We show that the zero-temperature physics of planar Josephson junction arrays in the self-dual approximation is governed by an Abelian gauge theory with periodic mixed Chern-Simons term describing the charge-vortex coupling. The periodicity requires the existence of (Euclidean) topological excitations which determine t... | 9.721444 | 9.883688 | 11.173857 | 9.414155 | 9.996423 | 9.431818 | 9.597102 | 9.315032 | 9.542718 | 10.452118 | 8.998834 | 9.804314 | 10.206768 | 9.821909 | 9.80381 | 9.745101 | 9.909536 | 9.794724 | 9.94806 | 10.485842 | 9.569954 |
1511.03102 | Yu-Xiao Liu | Yun-Zhi Du, Li Zhao, Xiang-Nan Zhou, Yi Zhong, and Yu-Xiao Liu | Localization of Gravitino Field on Thin Branes | v2: 18 pages, 14 figures | Annals Phys. 388 (2018) 69-88 | 10.1016/j.aop.2017.10.021 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we investigate the localization of a bulk gravitino field on
the scalar-tensor branes and compare the result with that in the
Randall-Sundrum-1 (RS1) model. The coupled chiral equations for the
Kaluza-Klein (KK) modes of the gravitino field are obtained by fixing the gauge
$\Psi_5=0$ and using the chir... | [
{
"created": "Tue, 10 Nov 2015 13:30:08 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Apr 2017 10:29:00 GMT",
"version": "v2"
},
{
"created": "Tue, 21 Nov 2017 11:29:02 GMT",
"version": "v3"
}
] | 2017-11-22 | [
[
"Du",
"Yun-Zhi",
""
],
[
"Zhao",
"Li",
""
],
[
"Zhou",
"Xiang-Nan",
""
],
[
"Zhong",
"Yi",
""
],
[
"Liu",
"Yu-Xiao",
""
]
] | In this paper, we investigate the localization of a bulk gravitino field on the scalar-tensor branes and compare the result with that in the Randall-Sundrum-1 (RS1) model. The coupled chiral equations for the Kaluza-Klein (KK) modes of the gravitino field are obtained by fixing the gauge $\Psi_5=0$ and using the chiral... | 6.58886 | 5.988308 | 6.516529 | 5.90204 | 5.706816 | 6.203514 | 6.144939 | 5.936383 | 5.782094 | 6.884955 | 6.059404 | 6.103955 | 6.113498 | 5.955123 | 6.095566 | 5.937232 | 6.069499 | 5.889801 | 5.895181 | 6.2809 | 5.939032 |
hep-th/0404249 | Keiichi Shigechi | Keiichi Shigechi, Miki Wadati and Ning Wang | WDVV equation and Triple-product Relation | Latex,11 pages,no figures | Nucl.Phys. B706 (2005) 518-530 | 10.1016/j.nuclphysb.2004.11.060 | null | hep-th | null | We study the relation between the WDVV equations and the $\tau$-function of
the noncommutative KP (NCKP) hierarchy. WDVV-like equations (Hirota
triple-product relation) in the noncommutative context appear as a consequence
of the non-trivial equation for $\tau$-function of the NC KP hierarchy, while
the prepotential ... | [
{
"created": "Fri, 30 Apr 2004 09:44:47 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Shigechi",
"Keiichi",
""
],
[
"Wadati",
"Miki",
""
],
[
"Wang",
"Ning",
""
]
] | We study the relation between the WDVV equations and the $\tau$-function of the noncommutative KP (NCKP) hierarchy. WDVV-like equations (Hirota triple-product relation) in the noncommutative context appear as a consequence of the non-trivial equation for $\tau$-function of the NC KP hierarchy, while the prepotential in... | 7.377757 | 7.283628 | 8.22115 | 7.398981 | 7.662383 | 7.563545 | 8.634077 | 7.808741 | 7.26615 | 8.912025 | 7.053144 | 7.256237 | 7.524169 | 7.049078 | 7.27202 | 7.403082 | 7.247879 | 7.114456 | 6.980971 | 7.560024 | 7.015258 |
hep-th/9905131 | Askold Duviryak | A. Duviryak (Inst. for Cond. Matt. Phys.) | Classical mechanics of relativistic particle with colour | 8 pages, presented at 3rd Int. Conf. "Symmetry in Nonlin. Math.
Phys." (12-18 July 1999, Kyiv) | Proc. of Inst. of Math. of NAS of Ukraine, Vol. 30, pp. 473-480
(2000) | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Classical description of relativistic pointlike particle with intrinsic
degrees of freedom such as isospin or colour is proposed. It is based on the
Lagrangian of general form defined on the tangent bundle over a principal fibre
bundle. It is shown that the dynamics splits into the external dynamics which
describes t... | [
{
"created": "Tue, 18 May 1999 16:21:14 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Oct 2019 16:24:41 GMT",
"version": "v2"
}
] | 2019-10-24 | [
[
"Duviryak",
"A.",
"",
"Inst. for Cond. Matt. Phys."
]
] | Classical description of relativistic pointlike particle with intrinsic degrees of freedom such as isospin or colour is proposed. It is based on the Lagrangian of general form defined on the tangent bundle over a principal fibre bundle. It is shown that the dynamics splits into the external dynamics which describes the... | 13.551304 | 12.274853 | 12.49925 | 11.712995 | 13.258102 | 13.320214 | 12.469774 | 12.493163 | 11.120798 | 13.391976 | 11.313514 | 11.891084 | 12.06268 | 12.045135 | 12.06522 | 11.971033 | 11.851665 | 11.579844 | 11.798662 | 12.138616 | 11.67681 |
2310.19050 | Federica Muscolino | Alexander Kamenshchik and Federica Muscolino | Looking for Carroll particles in two time spacetime | 11 pages, 1 figure | null | null | null | hep-th gr-qc quant-ph | http://creativecommons.org/licenses/by/4.0/ | We make an attempt to describe Carroll particles with a non-vanishing value
of energy (i.e. the Carroll particles which always stay in rest) in the
framework of two time physics, developed in the series of papers by I. Bars and
his co-authors. In the spacetime with one additional time dimension and one
additional spa... | [
{
"created": "Sun, 29 Oct 2023 15:51:41 GMT",
"version": "v1"
}
] | 2023-10-31 | [
[
"Kamenshchik",
"Alexander",
""
],
[
"Muscolino",
"Federica",
""
]
] | We make an attempt to describe Carroll particles with a non-vanishing value of energy (i.e. the Carroll particles which always stay in rest) in the framework of two time physics, developed in the series of papers by I. Bars and his co-authors. In the spacetime with one additional time dimension and one additional space... | 12.578217 | 12.927588 | 13.083408 | 12.022317 | 11.928796 | 12.479136 | 13.03553 | 12.162811 | 11.997189 | 13.461503 | 12.131844 | 11.310383 | 12.177703 | 11.720216 | 11.681467 | 11.705898 | 11.707305 | 11.356795 | 11.812287 | 12.400635 | 11.502814 |
2109.13781 | Sebastian Dumitru | Sebastian Dumitru and Burt A. Ovrut | Heterotic $M$-Theory Hidden Sectors with an Anomalous $U(1)$ Gauge
Symmetry | 47 pages, extended the analysis to include the five-brane brane
contribution | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The hidden sector of heterotic $M$-theory vacua whose gauge bundle contains
an anomalous $U(1)$ factor is discussed in detail. The mathematical formalism
for computing the inhomogeneous transformation of the dilaton and K\"ahler
moduli axions under an anomalous $U(1)$ transformation is presented. Along with
matter mu... | [
{
"created": "Tue, 28 Sep 2021 15:00:06 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Oct 2021 22:17:07 GMT",
"version": "v2"
}
] | 2021-10-15 | [
[
"Dumitru",
"Sebastian",
""
],
[
"Ovrut",
"Burt A.",
""
]
] | The hidden sector of heterotic $M$-theory vacua whose gauge bundle contains an anomalous $U(1)$ factor is discussed in detail. The mathematical formalism for computing the inhomogeneous transformation of the dilaton and K\"ahler moduli axions under an anomalous $U(1)$ transformation is presented. Along with matter mult... | 8.194133 | 8.972368 | 8.305705 | 8.511342 | 8.831871 | 9.058652 | 8.252217 | 8.020475 | 8.343063 | 8.915874 | 7.9079 | 7.990106 | 7.884487 | 8.113188 | 8.066331 | 7.977854 | 7.741298 | 7.899455 | 7.766226 | 8.136084 | 7.81059 |
2008.10574 | Christoph Nega | Kilian B\"onisch, Fabian Fischbach, Albrecht Klemm, Christoph Nega and
Reza Safari | Analytic Structure of all Loop Banana Amplitudes | 40 pages, 1 figure, new appendix concerning a pari program to compute
equal mass amplitude, minor corrections the paper is now also published in
JHEP but under the name "Analytic structure of all loop banana integrals",
some changes are done in the published version | Journal of High Energy Physics 2021 | 10.1007/JHEP05(2021)066 | BONN-TH-2020-06 | hep-th hep-ph math.AG math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the Gelfand-Kapranov-Zelevinsk\u{\i} system for the primitive
cohomology of an infinite series of complete intersection Calabi-Yau manifolds,
whose dimension is the loop order minus one, we completely clarify the analytic
structure of all banana amplitudes with arbitrary masses. In particular, we
find that the ... | [
{
"created": "Mon, 24 Aug 2020 17:25:17 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Oct 2020 10:09:26 GMT",
"version": "v2"
},
{
"created": "Fri, 14 May 2021 13:56:14 GMT",
"version": "v3"
}
] | 2021-05-17 | [
[
"Bönisch",
"Kilian",
""
],
[
"Fischbach",
"Fabian",
""
],
[
"Klemm",
"Albrecht",
""
],
[
"Nega",
"Christoph",
""
],
[
"Safari",
"Reza",
""
]
] | Using the Gelfand-Kapranov-Zelevinsk\u{\i} system for the primitive cohomology of an infinite series of complete intersection Calabi-Yau manifolds, whose dimension is the loop order minus one, we completely clarify the analytic structure of all banana amplitudes with arbitrary masses. In particular, we find that the le... | 10.859122 | 12.628898 | 12.359179 | 10.486406 | 11.301827 | 12.019883 | 11.575912 | 11.251951 | 10.811332 | 13.576632 | 11.124718 | 10.461686 | 10.731679 | 10.422292 | 10.572156 | 10.657475 | 10.293881 | 10.232348 | 10.610201 | 10.93334 | 10.472115 |
hep-th/9811126 | Klemm Dietmar | Dietmar Klemm (University of Trento, Italy) | Rotating Black Branes wrapped on Einstein Spaces | 11 pages, RevTeX, no figures, thermodynamical discussion and 2
references added | JHEP 9811:019,1998 | 10.1088/1126-6708/1998/11/019 | UTF 426 | hep-th gr-qc | null | We present new rotating black brane solutions which solve Einstein's
equations with cosmological constant $\Lambda$ in arbitrary dimension $d$. For
negative $\Lambda$, the branes naturally appear in AdS supergravity
compactifications, and should therefore play some role in the AdS/CFT
correspondence. The spacetimes a... | [
{
"created": "Fri, 13 Nov 1998 15:09:25 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Nov 1998 16:05:47 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Klemm",
"Dietmar",
"",
"University of Trento, Italy"
]
] | We present new rotating black brane solutions which solve Einstein's equations with cosmological constant $\Lambda$ in arbitrary dimension $d$. For negative $\Lambda$, the branes naturally appear in AdS supergravity compactifications, and should therefore play some role in the AdS/CFT correspondence. The spacetimes are... | 7.334923 | 6.604047 | 6.745759 | 6.490613 | 6.874659 | 6.594119 | 7.429878 | 6.418183 | 6.59773 | 7.169478 | 6.297943 | 6.630201 | 6.580459 | 6.548342 | 6.552041 | 6.29952 | 6.364 | 6.122669 | 6.452707 | 6.943864 | 6.355306 |
0707.2859 | Hendrik De Bie | Hendrik De Bie, Frank Sommen | A Clifford analysis approach to superspace | 15 pages, accepted for publication in Annals of Physics | null | 10.1016/j.aop.2007.04.012 | null | hep-th math-ph math.MP | null | A new framework for studying superspace is given, based on methods from
Clifford analysis. This leads to the introduction of both orthogonal and
symplectic Clifford algebra generators, allowing for an easy and canonical
introduction of a super-Dirac operator, a super-Laplace operator and the like.
This framework is t... | [
{
"created": "Thu, 19 Jul 2007 09:29:39 GMT",
"version": "v1"
}
] | 2007-07-20 | [
[
"De Bie",
"Hendrik",
""
],
[
"Sommen",
"Frank",
""
]
] | A new framework for studying superspace is given, based on methods from Clifford analysis. This leads to the introduction of both orthogonal and symplectic Clifford algebra generators, allowing for an easy and canonical introduction of a super-Dirac operator, a super-Laplace operator and the like. This framework is the... | 10.538773 | 11.238406 | 11.052301 | 9.451456 | 10.683832 | 11.245595 | 11.452179 | 10.95165 | 10.255277 | 11.862987 | 10.04209 | 10.352254 | 10.894556 | 10.04876 | 9.89768 | 10.553364 | 10.346766 | 10.134057 | 10.058111 | 10.243279 | 9.938643 |
hep-th/0605172 | Andrew Cohen | Andrew G. Cohen and Daniel Z. Freedman | Sim(2) and SUSY | 10 pages, revtex4. Note added and sign corrected | JHEP 0707:039,2007 | 10.1088/1126-6708/2007/07/039 | MIT_CTP 3744 | hep-th | null | The proposal of hep-ph/0601236, that the laws of physics in flat spacetime
need be invariant only under a SIM(2) subgroup of the Lorentz group, is
extended to include supersymmetry. $\mathcal{N}=1$ SUSY gauge theories which
include SIM(2) couplings for the fermions in chiral multiplets are formulated.
These theories ... | [
{
"created": "Wed, 17 May 2006 18:29:09 GMT",
"version": "v1"
},
{
"created": "Sun, 8 Apr 2007 13:52:46 GMT",
"version": "v2"
}
] | 2009-10-08 | [
[
"Cohen",
"Andrew G.",
""
],
[
"Freedman",
"Daniel Z.",
""
]
] | The proposal of hep-ph/0601236, that the laws of physics in flat spacetime need be invariant only under a SIM(2) subgroup of the Lorentz group, is extended to include supersymmetry. $\mathcal{N}=1$ SUSY gauge theories which include SIM(2) couplings for the fermions in chiral multiplets are formulated. These theories co... | 10.175409 | 9.252674 | 8.627068 | 8.595392 | 9.19456 | 9.237543 | 9.634915 | 9.652764 | 8.344231 | 8.763968 | 9.48403 | 9.053831 | 9.212738 | 9.078041 | 9.430721 | 9.71422 | 9.16827 | 9.42137 | 9.152658 | 8.877029 | 9.257304 |
2308.07695 | Hiren Kakkad | Hiren Kakkad | Scattering Amplitudes in the Yang-Mills sector of Quantum Chromodynamics | Thesis, 236 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a new Minkowski space action for the pure gluonic sector of QCD
that implements new interaction vertices local in the light-cone time with at
least four legs and fixed helicities - the lowest vertex is the four-point MHV
(Maximally Helicity Violating), higher point vertices include $\mathrm{N}^k
\mathrm{MHV... | [
{
"created": "Tue, 15 Aug 2023 10:52:07 GMT",
"version": "v1"
}
] | 2023-08-16 | [
[
"Kakkad",
"Hiren",
""
]
] | We derive a new Minkowski space action for the pure gluonic sector of QCD that implements new interaction vertices local in the light-cone time with at least four legs and fixed helicities - the lowest vertex is the four-point MHV (Maximally Helicity Violating), higher point vertices include $\mathrm{N}^k \mathrm{MHV}$... | 10.916771 | 10.744984 | 10.989845 | 10.407857 | 10.262972 | 10.294259 | 10.909189 | 10.716086 | 10.060749 | 11.67487 | 10.10477 | 10.545697 | 10.409974 | 10.039281 | 9.922232 | 10.256471 | 10.208138 | 10.392719 | 10.041715 | 10.148514 | 10.150462 |
1801.06858 | Ferenc Niedermayer | Ferenc Niedermayer and Peter Weisz | Casimir squared correction to the standard rotator Hamiltonian for the
O($n$) sigma-model in the delta-regime | 25 pages, 1 figure | null | 10.1007/JHEP05(2018)070 | MPP-2017-214 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a previous paper we found that the isospin susceptibility of the O($n$)
sigma-model calculated in the standard rotator approximation differs from the
next-to-next to leading order chiral perturbation theory result in terms
vanishing like $1/\ell\,,$ for $\ell=L_t/L\to\infty$ and further showed that
this deviation ... | [
{
"created": "Sun, 21 Jan 2018 17:28:33 GMT",
"version": "v1"
}
] | 2018-06-13 | [
[
"Niedermayer",
"Ferenc",
""
],
[
"Weisz",
"Peter",
""
]
] | In a previous paper we found that the isospin susceptibility of the O($n$) sigma-model calculated in the standard rotator approximation differs from the next-to-next to leading order chiral perturbation theory result in terms vanishing like $1/\ell\,,$ for $\ell=L_t/L\to\infty$ and further showed that this deviation co... | 11.157929 | 10.35911 | 12.478535 | 10.430619 | 10.392625 | 10.174717 | 11.268368 | 11.768576 | 9.900751 | 12.744064 | 9.684331 | 10.69128 | 10.79677 | 10.220736 | 10.160507 | 10.587399 | 10.738523 | 10.099466 | 10.479928 | 10.11201 | 10.227154 |
hep-th/0207108 | Soo-Jong Rey | Soo-Jong Rey | Exact Answers to Approximate Questions: Noncommutative Dipoles, Open
Wilson Lines, and UV-IR Duality | short lecture at 2001 Les Houches summer school | null | null | SNUST 02-0701 | hep-th | null | In this lecture, I put forward conjectures asserting that, in all
noncommutative field theories, (1) open Wilson lines and their descendants
constitute a complete set of interpolating operators of `noncommutative
dipoles', obeying dipole relation, (2) infrared dynamics of the noncommutative
dipoles is dual to ultravi... | [
{
"created": "Thu, 11 Jul 2002 14:56:04 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rey",
"Soo-Jong",
""
]
] | In this lecture, I put forward conjectures asserting that, in all noncommutative field theories, (1) open Wilson lines and their descendants constitute a complete set of interpolating operators of `noncommutative dipoles', obeying dipole relation, (2) infrared dynamics of the noncommutative dipoles is dual to ultraviol... | 8.488839 | 8.76078 | 8.171465 | 8.004209 | 7.988688 | 8.311625 | 8.148662 | 7.655638 | 7.995492 | 8.422584 | 7.949133 | 7.845604 | 7.905227 | 7.694848 | 7.760069 | 8.153946 | 7.501794 | 7.860778 | 7.598222 | 7.804137 | 7.704205 |
hep-th/0207234 | Kokorelis | Christos Kokorelis | Exact Standard model Structures from Intersecting D5-Branes | 71 pages, 8 figures, LaTex, 45 tables, RR tadpoles unchanged, Brane
recombination guarantees gauge breaking `homology flow' transitions between
six, five and four stack D5 SM quivers | Nucl.Phys.B677:115-163,2004 | 10.1016/j.nuclphysb.2003.11.007 | FTUAM-02-20, IFT-UAM/CSIC-02-17 | hep-th hep-ph | null | We discuss the appearance of non-supersymmetric compactifications with
exactly the Standard Model (SM) at low energies, in the context of IIB
orientifold constructions with
D5 branes intersecting at angles on the $T^4$ tori, of the orientifold of
$T^4 \times (\C /Z_N)$.
We discuss constructions where the Standard... | [
{
"created": "Thu, 25 Jul 2002 17:53:43 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Aug 2002 20:43:25 GMT",
"version": "v2"
},
{
"created": "Fri, 21 Mar 2003 16:07:22 GMT",
"version": "v3"
},
{
"created": "Sun, 23 Mar 2003 10:55:16 GMT",
"version": "v4"
}
] | 2014-11-18 | [
[
"Kokorelis",
"Christos",
""
]
] | We discuss the appearance of non-supersymmetric compactifications with exactly the Standard Model (SM) at low energies, in the context of IIB orientifold constructions with D5 branes intersecting at angles on the $T^4$ tori, of the orientifold of $T^4 \times (\C /Z_N)$. We discuss constructions where the Standard Model... | 13.298443 | 12.630334 | 13.856804 | 12.813787 | 12.544082 | 12.964572 | 13.028731 | 13.02028 | 13.240137 | 16.052404 | 13.265677 | 12.981596 | 13.152644 | 13.442766 | 13.221879 | 13.546229 | 13.529816 | 12.794407 | 13.1967 | 13.59692 | 12.769698 |
hep-th/9801202 | Ergin Sezgin | C.S. Chu, P.S. Howe and E. Sezgin | Strings and D-Branes with Boundaries | 12 pages, Latex | Phys.Lett. B428 (1998) 59-67 | 10.1016/S0370-2693(98)00376-1 | null | hep-th | null | The covariant field equations of ten-dimensional super D-branes are obtained
by considering fundamental strings whose ends lie in the superworldsurface of
the D-brane. By considering in a similar fashion Dp-branes ending on
D(p+2)-branes we derive equations describing D-branes with dual potentials, as
well as the vec... | [
{
"created": "Fri, 30 Jan 1998 00:29:18 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Chu",
"C. S.",
""
],
[
"Howe",
"P. S.",
""
],
[
"Sezgin",
"E.",
""
]
] | The covariant field equations of ten-dimensional super D-branes are obtained by considering fundamental strings whose ends lie in the superworldsurface of the D-brane. By considering in a similar fashion Dp-branes ending on D(p+2)-branes we derive equations describing D-branes with dual potentials, as well as the vecto... | 15.791777 | 15.702557 | 18.577822 | 13.785209 | 16.913561 | 16.576456 | 14.278741 | 13.826486 | 15.337308 | 20.397873 | 13.629617 | 13.124006 | 17.01461 | 14.322304 | 13.755345 | 14.044516 | 13.58008 | 14.236234 | 13.719162 | 16.789581 | 13.041744 |
hep-th/9510203 | null | M. P. Fry | QED in strong, finite-flux magnetic fields | 10 pages, postscript (in uuencoded compressed tar file) | Phys.Rev. D53 (1996) 980-983 | 10.1103/PhysRevD.53.980 | null | hep-th | null | Lower bounds are placed on the fermionic determinants of Euclidean quantum
electrodynamics in two and four dimensions in the presence of a smooth,
finite-flux, static, unidirectional magnetic field $B(r) =(0,0,B(r))$, where
$B(r) \geq 0$ or $B(r) \leq 0$, and $r$ is a point in the xy-plane.
| [
{
"created": "Tue, 24 Oct 1995 11:27:32 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Fry",
"M. P.",
""
]
] | Lower bounds are placed on the fermionic determinants of Euclidean quantum electrodynamics in two and four dimensions in the presence of a smooth, finite-flux, static, unidirectional magnetic field $B(r) =(0,0,B(r))$, where $B(r) \geq 0$ or $B(r) \leq 0$, and $r$ is a point in the xy-plane. | 6.996129 | 5.571118 | 7.787471 | 6.286469 | 7.499849 | 7.155386 | 6.844548 | 6.455293 | 6.081114 | 8.329036 | 6.220077 | 6.22937 | 7.26216 | 6.759822 | 6.611303 | 6.551316 | 6.393481 | 6.70796 | 7.093049 | 7.365081 | 6.445953 |
hep-th/0211216 | Albrecht Klemm | Albrecht Klemm, Marcos Marino and Stefan Theisen | Gravitational corrections in supersymmetric gauge theory and matrix
models | 27 pages, one eps figure | JHEP 0303:051,2003 | 10.1088/1126-6708/2003/03/051 | AEI-2002-090, HU-EP-02/48, HUTP-02/A060 | hep-th | null | Gravitational corrections in N=1 and N=2 supersymmetric gauge theories are
obtained from topological string amplitudes. We show how they are recovered in
matrix model computations. This provides a test of the proposal by Dijkgraaf
and Vafa beyond the planar limit. Both, matrix model and topological string
theory, are... | [
{
"created": "Fri, 22 Nov 2002 14:10:39 GMT",
"version": "v1"
}
] | 2010-04-06 | [
[
"Klemm",
"Albrecht",
""
],
[
"Marino",
"Marcos",
""
],
[
"Theisen",
"Stefan",
""
]
] | Gravitational corrections in N=1 and N=2 supersymmetric gauge theories are obtained from topological string amplitudes. We show how they are recovered in matrix model computations. This provides a test of the proposal by Dijkgraaf and Vafa beyond the planar limit. Both, matrix model and topological string theory, are u... | 6.682108 | 6.22697 | 8.067554 | 5.801612 | 6.557184 | 6.61073 | 6.046416 | 6.141982 | 5.980575 | 8.505638 | 5.957938 | 5.931765 | 6.763546 | 6.104445 | 6.096248 | 6.031083 | 6.139576 | 6.133331 | 5.939002 | 6.870917 | 5.980071 |
1407.0305 | Marcin Pi\k{a}tek dr. | Marcin Piatek, Artur R. Pietrykowski | Classical irregular block, N=2 pure gauge theory and Mathieu equation | 47 pages, 3 figures | null | 10.1007/JHEP12(2014)032 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Combining the semiclassical/Nekrasov-Shatashvili limit of the AGT conjecture
and the Bethe/gauge correspondence results in a triple correspondence which
identifies classical conformal blocks with twisted superpotentials and then
with Yang-Yang functions. In this paper the triple correspondence is studied in
the simpl... | [
{
"created": "Tue, 1 Jul 2014 16:21:43 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Piatek",
"Marcin",
""
],
[
"Pietrykowski",
"Artur R.",
""
]
] | Combining the semiclassical/Nekrasov-Shatashvili limit of the AGT conjecture and the Bethe/gauge correspondence results in a triple correspondence which identifies classical conformal blocks with twisted superpotentials and then with Yang-Yang functions. In this paper the triple correspondence is studied in the simples... | 10.427432 | 10.54617 | 12.581792 | 10.225859 | 11.660742 | 10.658766 | 10.529253 | 10.056392 | 10.1732 | 12.593841 | 10.230574 | 9.856903 | 10.523687 | 10.202372 | 10.438299 | 10.638216 | 10.23527 | 10.036923 | 10.08064 | 10.512974 | 10.085787 |
hep-th/0307245 | Eric R. Sharpe | E. Sharpe | Lectures on D-branes and Sheaves | 87 pages, LaTeX, 1 figure; v2: material on Freed-Witten added | null | null | ILL-(TH)-03-6 | hep-th | null | These notes are a writeup of lectures given at the twelfth Oporto meeting on
``Geometry, Topology, and Physics,'' and at the Adelaide workshop ``Strings and
Mathematics 2003,'' primarily geared towards a physics audience. We review
current work relating boundary states in the open string B model on Calabi-Yau
manifol... | [
{
"created": "Thu, 24 Jul 2003 16:11:58 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Aug 2003 16:18:54 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Sharpe",
"E.",
""
]
] | These notes are a writeup of lectures given at the twelfth Oporto meeting on ``Geometry, Topology, and Physics,'' and at the Adelaide workshop ``Strings and Mathematics 2003,'' primarily geared towards a physics audience. We review current work relating boundary states in the open string B model on Calabi-Yau manifolds... | 13.793434 | 13.933081 | 15.045592 | 12.492567 | 14.922866 | 14.177425 | 15.044606 | 13.847308 | 13.054925 | 16.640944 | 14.561371 | 12.651627 | 12.945178 | 12.610619 | 12.533964 | 12.57254 | 12.809669 | 12.221282 | 12.469943 | 13.177581 | 12.579225 |
2009.14667 | F. David Wandler | Erich Poppitz and F. David Wandler | Topological terms and anomaly matching in effective field theories on
$\mathbb{R}^3\times S^1$: I. Abelian symmetries and intermediate scales | 70 pages, 9 figures. Version to appear in JHEP. Typos fixed,
references added | null | 10.1007/JHEP01(2021)091 | null | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly calculate the topological terms that arise in IR effective
field theories for $SU(N)$ gauge theories on $\mathbb{R}^3 \times S^1$ by
integrating out all but the lightest modes. We then show how these terms match
all global-symmetry 't Hooft anomalies of the UV description. We limit our
discussion to the... | [
{
"created": "Wed, 30 Sep 2020 13:41:55 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Dec 2020 20:18:20 GMT",
"version": "v2"
}
] | 2021-02-03 | [
[
"Poppitz",
"Erich",
""
],
[
"Wandler",
"F. David",
""
]
] | We explicitly calculate the topological terms that arise in IR effective field theories for $SU(N)$ gauge theories on $\mathbb{R}^3 \times S^1$ by integrating out all but the lightest modes. We then show how these terms match all global-symmetry 't Hooft anomalies of the UV description. We limit our discussion to theor... | 9.40274 | 9.668005 | 10.662848 | 8.462545 | 9.670734 | 9.62324 | 9.623826 | 9.386286 | 9.090107 | 10.671199 | 9.148153 | 9.068713 | 9.609826 | 9.116138 | 8.913987 | 8.965054 | 8.875186 | 9.488028 | 9.166619 | 9.567223 | 8.792803 |
1010.4418 | Pulak Ranjan Giri | Debabrata Sinha, Pulak Ranjan Giri | A Family of Non-commutative geometries | 5 pages, revtex | Mod. Phys. Lett. A26:2213-2221,2011 | 10.1142/S0217732311036619 | null | hep-th cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is shown that the non-commutativity in quantum Hall system may get
modified. The self-adjoint extension of the corresponding Hamiltonian leads to
a family of non-commutative geometries labeled by the self-adjoint extension
parameters. We explicitly perform an exact calculation using a singular
interaction and show... | [
{
"created": "Thu, 21 Oct 2010 10:45:52 GMT",
"version": "v1"
}
] | 2011-09-28 | [
[
"Sinha",
"Debabrata",
""
],
[
"Giri",
"Pulak Ranjan",
""
]
] | It is shown that the non-commutativity in quantum Hall system may get modified. The self-adjoint extension of the corresponding Hamiltonian leads to a family of non-commutative geometries labeled by the self-adjoint extension parameters. We explicitly perform an exact calculation using a singular interaction and show t... | 10.033459 | 8.805218 | 10.167334 | 8.362041 | 9.296863 | 9.143618 | 9.394758 | 8.634103 | 8.264579 | 10.031899 | 8.227153 | 8.659009 | 9.364079 | 9.093862 | 8.775718 | 8.690845 | 8.755331 | 8.990065 | 8.714039 | 9.433629 | 8.821812 |
1712.08016 | Andrei Mironov | H. Awata, H. Kanno, A. Mironov, A. Morozov, K. Suetake, Y. Zenkevich | $(q,t)$-KZ equations for quantum toroidal algebra and Nekrasov partition
functions on ALE spaces | 56 pages | J. High Energ. Phys. 2018 (2018) 192 | 10.1007/JHEP03(2018)192 | FIAN/TD-30/17; IITP/TH-24/17; ITEP/TH-41/17 | hep-th math-ph math.MP math.QA math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe the general strategy for lifting the Wess-Zumino-Witten model
from the level of one-loop Kac-Moody $U_q(\widehat{\mathfrak{g}})_k$ to generic
quantum toroidal algebras. A nearly exhaustive presentation is given for the
two series $U_{q,t}(\widehat{\widehat{\mathfrak{gl}}}_1)$ and
$U_{q,t}(\widehat{\wideha... | [
{
"created": "Thu, 21 Dec 2017 15:30:49 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Mar 2018 08:15:29 GMT",
"version": "v2"
}
] | 2018-04-10 | [
[
"Awata",
"H.",
""
],
[
"Kanno",
"H.",
""
],
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
],
[
"Suetake",
"K.",
""
],
[
"Zenkevich",
"Y.",
""
]
] | We describe the general strategy for lifting the Wess-Zumino-Witten model from the level of one-loop Kac-Moody $U_q(\widehat{\mathfrak{g}})_k$ to generic quantum toroidal algebras. A nearly exhaustive presentation is given for the two series $U_{q,t}(\widehat{\widehat{\mathfrak{gl}}}_1)$ and $U_{q,t}(\widehat{\widehat{... | 7.006281 | 7.039437 | 9.122437 | 7.13377 | 7.391616 | 7.541509 | 7.622536 | 6.881129 | 7.108596 | 10.044862 | 6.93755 | 7.141423 | 7.637243 | 6.989827 | 6.99453 | 6.983902 | 7.184361 | 6.920329 | 7.004884 | 7.396692 | 7.015471 |
0709.3791 | Hiroyuki Abe | Hiroyuki Abe, Yutaka Sakamura | Moduli stabilization in 5D gauged supergravity with universal
hypermultiplet and boundary superpotentials | 25 pages, 2 figures | Nucl.Phys.B796:224-245,2008 | 10.1016/j.nuclphysb.2007.12.009 | YITP-07-57, OU-HET 586/2007 | hep-th hep-ph | null | We study a four-dimensional effective theory of the five-dimensional (5D)
gauged supergravity with a universal hypermultiplet and perturbative
superpotential terms at the orbifold fixed points. Among eight independent
isometries of the scalar manifold, we focus on three directions for gauging by
the graviphoton. The ... | [
{
"created": "Mon, 24 Sep 2007 15:20:12 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Abe",
"Hiroyuki",
""
],
[
"Sakamura",
"Yutaka",
""
]
] | We study a four-dimensional effective theory of the five-dimensional (5D) gauged supergravity with a universal hypermultiplet and perturbative superpotential terms at the orbifold fixed points. Among eight independent isometries of the scalar manifold, we focus on three directions for gauging by the graviphoton. The cl... | 6.98795 | 5.921066 | 7.660915 | 5.708596 | 5.442864 | 5.864564 | 5.215109 | 5.808382 | 5.772446 | 8.196892 | 6.052743 | 6.542427 | 7.058152 | 6.801419 | 6.510917 | 6.420545 | 6.612861 | 6.595068 | 6.646534 | 7.272687 | 6.798861 |
hep-th/0701241 | Kazuya Koyama | Kazuya Koyama, Andrew Mennim, V.A. Rubakov, David Wands and Takashi
Hiramatsu | Primordial perturbations from slow-roll inflation on a brane | 23 pages, 10 figures | JCAP 0704:001,2007 | 10.1088/1475-7516/2007/04/001 | null | hep-th astro-ph gr-qc hep-ph | null | In this paper we quantise scalar perturbations in a Randall-Sundrum-type
model of inflation where the inflaton field is confined to a single brane
embedded in five-dimensional anti-de Sitter space-time. In the high energy
regime, small-scale inflaton fluctuations are strongly coupled to metric
perturbations in the bu... | [
{
"created": "Fri, 26 Jan 2007 14:23:26 GMT",
"version": "v1"
}
] | 2010-10-27 | [
[
"Koyama",
"Kazuya",
""
],
[
"Mennim",
"Andrew",
""
],
[
"Rubakov",
"V. A.",
""
],
[
"Wands",
"David",
""
],
[
"Hiramatsu",
"Takashi",
""
]
] | In this paper we quantise scalar perturbations in a Randall-Sundrum-type model of inflation where the inflaton field is confined to a single brane embedded in five-dimensional anti-de Sitter space-time. In the high energy regime, small-scale inflaton fluctuations are strongly coupled to metric perturbations in the bulk... | 5.64387 | 5.394833 | 5.251948 | 5.02666 | 5.281019 | 5.627165 | 5.311885 | 5.044785 | 5.148913 | 5.162093 | 5.299428 | 5.249786 | 5.026879 | 5.192937 | 5.214926 | 5.16937 | 5.110047 | 5.14035 | 5.1464 | 5.132506 | 5.236598 |
0801.3851 | Zhong Chao Wu | Zhong Chao Wu | Commutativity of Substitution and Variation in Actions of Quantum Field
Theory | 11 pages | Phys.Rev.D80:105001,2009 | 10.1103/PhysRevD.80.105001 | ZJUT-08-01 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There exists a paradox in quantum field theory: substituting a field
configuration which solves a subset of the field equations into the action and
varying it is not necessarily equivalent to substituting that configuration
into the remaining field equations. We take the $S^4$ and Freund-Rubin-like
instantons as two ... | [
{
"created": "Fri, 25 Jan 2008 20:09:17 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Jan 2008 19:24:40 GMT",
"version": "v2"
},
{
"created": "Wed, 11 Nov 2009 21:56:40 GMT",
"version": "v3"
}
] | 2009-11-11 | [
[
"Wu",
"Zhong Chao",
""
]
] | There exists a paradox in quantum field theory: substituting a field configuration which solves a subset of the field equations into the action and varying it is not necessarily equivalent to substituting that configuration into the remaining field equations. We take the $S^4$ and Freund-Rubin-like instantons as two ex... | 19.482832 | 18.882355 | 18.655958 | 18.225784 | 19.153534 | 19.203329 | 19.535975 | 18.4589 | 16.871525 | 19.149849 | 15.981384 | 16.614496 | 17.75843 | 16.434429 | 16.807373 | 16.923044 | 17.763517 | 17.281105 | 16.437292 | 18.072325 | 16.825848 |
hep-th/9512213 | Nobuyuki Sakai | Nobuyuki Sakai, Yoonbai Kim and Kei-ichi Maeda | Bubbles with an O(3) Symmetric Scalar Field in Curved Spacetime | 3 pages, latex, uuencoded postscript figures; talk given at 7th
Marcel Grossmann Meeting on General Relativity, Stanford University, July
24-29, 1994 | null | null | WU-AP/41/95 | hep-th astro-ph gr-qc | null | We study the first-order phase transition in a model of scalar field with
$O(3)$ symmetry coupled to gravity, and, in high temperature limit, discuss the
existence of new bubble solution with a global monopole at the center of the
bubble.
| [
{
"created": "Thu, 28 Dec 1995 19:46:36 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Sakai",
"Nobuyuki",
""
],
[
"Kim",
"Yoonbai",
""
],
[
"Maeda",
"Kei-ichi",
""
]
] | We study the first-order phase transition in a model of scalar field with $O(3)$ symmetry coupled to gravity, and, in high temperature limit, discuss the existence of new bubble solution with a global monopole at the center of the bubble. | 12.058812 | 9.193723 | 8.312263 | 7.675429 | 8.583689 | 7.687355 | 8.642726 | 7.842941 | 9.097685 | 8.328502 | 8.989137 | 9.585082 | 9.74278 | 9.420422 | 9.730757 | 9.608786 | 9.677627 | 9.198248 | 9.889462 | 9.424493 | 9.169881 |
hep-th/0604108 | Michael McGuigan | Michael McGuigan | Cosmological Constant Seesaw in String/M-Theory | 25 pages, 0 figures | null | null | null | hep-th | null | In this paper we extend the Cosmological Constant Seesaw treatment of
hep-th/0602112 to String/M-Theory where the cosmological constant is finite. We
discuss how transitions between different $\lambda$, one of Planckian vacuum
energy, can give rise to a large $M_{Pl}^4$ denominator in the Cosmological
Constant Seesaw... | [
{
"created": "Fri, 14 Apr 2006 22:44:12 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"McGuigan",
"Michael",
""
]
] | In this paper we extend the Cosmological Constant Seesaw treatment of hep-th/0602112 to String/M-Theory where the cosmological constant is finite. We discuss how transitions between different $\lambda$, one of Planckian vacuum energy, can give rise to a large $M_{Pl}^4$ denominator in the Cosmological Constant Seesaw r... | 11.153634 | 11.913774 | 11.740713 | 11.25479 | 11.999803 | 11.803485 | 11.354151 | 11.032682 | 11.111183 | 12.711774 | 10.634208 | 11.132048 | 11.117264 | 10.62854 | 10.895267 | 10.858335 | 10.99896 | 10.745821 | 10.993829 | 11.143905 | 10.821154 |
0710.0388 | Alessandro Fabbri | R. Balbinot, A. Fabbri, S. Farese, R. Parentani | Hawking radiation from extremal and non-extremal black holes | 18 pages, latex | Phys.Rev.D76:124010,2007 | 10.1103/PhysRevD.76.124010 | null | hep-th gr-qc | null | The relationship between Hawking radiation emitted by non extremal and
extremal Reissner Nordstrom black holes is critically analyzed. A careful study
of a series of regular collapsing geometries reveals that the stress energy
tensor stays regular in the extremal limit and is smoothly connected to that of
non extrema... | [
{
"created": "Mon, 1 Oct 2007 21:27:23 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Balbinot",
"R.",
""
],
[
"Fabbri",
"A.",
""
],
[
"Farese",
"S.",
""
],
[
"Parentani",
"R.",
""
]
] | The relationship between Hawking radiation emitted by non extremal and extremal Reissner Nordstrom black holes is critically analyzed. A careful study of a series of regular collapsing geometries reveals that the stress energy tensor stays regular in the extremal limit and is smoothly connected to that of non extremal ... | 11.904834 | 11.132954 | 11.598193 | 11.255302 | 12.40672 | 11.475253 | 12.899001 | 11.225897 | 11.169332 | 11.463153 | 11.682503 | 11.483564 | 11.475293 | 11.409139 | 11.525766 | 11.953155 | 11.685433 | 11.47317 | 11.287275 | 11.110513 | 11.442261 |
1306.2512 | Alessandro Sfondrini | Riccardo Borsato, Olof Ohlsson Sax, Alessandro Sfondrini, Bogdan
Stefanski, Alessandro Torrielli | Dressing phases of AdS3/CFT2 | 29 pages, 4 figures; v2: note added, minor changes | null | 10.1103/PhysRevD.88.066004 | DMUS-MP-13/14; ITP-UU-13/14; SPIN-13/10 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We determine the all-loop dressing phases of the AdS3/CFT2 integrable system
related to type IIB string theory on AdS3 x S3 x T4 by solving the recently
found crossing relations and studying their singularity structure. The two
resulting phases present a novel structure with respect to the ones appearing
in AdS5/CFT4... | [
{
"created": "Tue, 11 Jun 2013 13:01:32 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Jun 2013 12:06:50 GMT",
"version": "v2"
}
] | 2013-09-18 | [
[
"Borsato",
"Riccardo",
""
],
[
"Sax",
"Olof Ohlsson",
""
],
[
"Sfondrini",
"Alessandro",
""
],
[
"Stefanski",
"Bogdan",
""
],
[
"Torrielli",
"Alessandro",
""
]
] | We determine the all-loop dressing phases of the AdS3/CFT2 integrable system related to type IIB string theory on AdS3 x S3 x T4 by solving the recently found crossing relations and studying their singularity structure. The two resulting phases present a novel structure with respect to the ones appearing in AdS5/CFT4 a... | 6.749335 | 5.975277 | 8.306699 | 6.080443 | 5.98649 | 6.063922 | 6.268939 | 5.747489 | 5.968965 | 10.757801 | 6.379811 | 5.853548 | 7.421642 | 6.117994 | 6.072161 | 5.936224 | 6.087931 | 6.035512 | 6.101721 | 7.115991 | 6.011006 |
2012.02355 | Nava Gaddam | Nava Gaddam and Nico Groenenboom | Soft graviton exchange and the information paradox | 54 pages + Appendices; v3: typos corrected, references added; v4:
corrected eqns 4.81 and 4.83 v5: Published version | Phys. Rev. D 109, 026007 (2024) | 10.1103/PhysRevD.109.026007 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We show that there is a remarkable phase in quantum gravity where
gravitational scattering amplitudes mediated by virtual gravitons can be
calculated explicitly in effective field theory, when the impact parameter $b$
satisfies $L_{Pl}\ll b \lesssim R_S$, with $R_S$ being the Schwarzschild
radius. This phase captures... | [
{
"created": "Fri, 4 Dec 2020 01:17:45 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Apr 2021 21:18:52 GMT",
"version": "v2"
},
{
"created": "Thu, 21 Jul 2022 10:24:01 GMT",
"version": "v3"
},
{
"created": "Fri, 22 Jul 2022 10:27:13 GMT",
"version": "v4"
},
{
"cr... | 2024-01-18 | [
[
"Gaddam",
"Nava",
""
],
[
"Groenenboom",
"Nico",
""
]
] | We show that there is a remarkable phase in quantum gravity where gravitational scattering amplitudes mediated by virtual gravitons can be calculated explicitly in effective field theory, when the impact parameter $b$ satisfies $L_{Pl}\ll b \lesssim R_S$, with $R_S$ being the Schwarzschild radius. This phase captures c... | 7.270247 | 7.477151 | 7.890766 | 7.493956 | 6.957698 | 7.380099 | 7.716536 | 7.192657 | 7.17962 | 8.267923 | 7.542088 | 7.096027 | 7.359767 | 7.190424 | 7.030117 | 7.306748 | 7.265619 | 7.251374 | 7.260841 | 7.416934 | 7.277839 |
1512.09106 | Jay Armas | Jay Armas, Niels A. Obers and Marco Sanchioni | Gravitational Tension, Spacetime Pressure and Black Hole Volume | v3: 42pp, improved discussion in section 6, to be published in JHEP | JHEP 1609 (2016) 124 | 10.1007/JHEP09(2016)124 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the first law of black hole thermodynamics in the presence of
surrounding gravitational fields and argue that variations of these fields are
naturally incorporated in the first law by defining gravitational tension or
gravitational binding energy. We demonstrate that this notion can also be
applied in Anti-d... | [
{
"created": "Wed, 30 Dec 2015 20:35:13 GMT",
"version": "v1"
},
{
"created": "Fri, 18 Mar 2016 22:17:11 GMT",
"version": "v2"
},
{
"created": "Thu, 1 Sep 2016 19:36:58 GMT",
"version": "v3"
}
] | 2016-10-03 | [
[
"Armas",
"Jay",
""
],
[
"Obers",
"Niels A.",
""
],
[
"Sanchioni",
"Marco",
""
]
] | We study the first law of black hole thermodynamics in the presence of surrounding gravitational fields and argue that variations of these fields are naturally incorporated in the first law by defining gravitational tension or gravitational binding energy. We demonstrate that this notion can also be applied in Anti-de ... | 11.650301 | 12.232371 | 12.441926 | 11.130909 | 11.604405 | 12.030523 | 11.575962 | 11.029739 | 11.640359 | 12.488952 | 11.053432 | 11.337265 | 11.152881 | 11.177153 | 11.690224 | 11.16377 | 11.566839 | 11.25552 | 10.786643 | 11.440158 | 11.212758 |
hep-th/9811230 | Nikita Nekrasov | S.Gubser, N. Nekrasov, S. L. Shatashvili | Generalized Conifolds and 4d N=1 SCFT | harvmac 27pp; v2. refs added, typos corrected, abstract renormalized,
v3. more of that sort, version to appear in JHEP | JHEP 9905:003,1999 | 10.1088/1126-6708/1999/05/003 | HUTP-98/A051, ITEP-TH-64/98, YCTP-P29/98 | hep-th | null | This paper lays groundwork for the detailed study of the non-trivial
renormalization group flow connecting supersymmetric fixed points in four
dimensions using string theory on AdS spaces. Specifically, we consider
D3-branes placed at singularities of Calabi-Yau threefolds which generalize the
conifold singularity an... | [
{
"created": "Fri, 27 Nov 1998 22:10:19 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Feb 1999 23:19:41 GMT",
"version": "v2"
},
{
"created": "Sun, 9 May 1999 16:38:51 GMT",
"version": "v3"
}
] | 2017-09-07 | [
[
"Gubser",
"S.",
""
],
[
"Nekrasov",
"N.",
""
],
[
"Shatashvili",
"S. L.",
""
]
] | This paper lays groundwork for the detailed study of the non-trivial renormalization group flow connecting supersymmetric fixed points in four dimensions using string theory on AdS spaces. Specifically, we consider D3-branes placed at singularities of Calabi-Yau threefolds which generalize the conifold singularity and ... | 6.175877 | 5.903443 | 7.161481 | 5.926555 | 6.291405 | 5.732978 | 5.819073 | 5.972571 | 5.856729 | 7.550638 | 5.826824 | 5.922941 | 6.729893 | 5.966796 | 6.162436 | 5.910929 | 5.82353 | 6.120194 | 5.949518 | 6.769507 | 6.097575 |
1201.2448 | Makoto Sakamoto | Makoto Sakamoto | Hidden quantum-mechanical supersymmetry in extra dimensions | This review was given at 13th Regional Conference on Mathematical
Physics, Antalya, Turkey, October 27-31, 2010 | null | null | KOBE-TH-12-02 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study higher dimensional field theories with extra dimensions from a 4d
spectrum point of view. It is shown that 4d mass spectra of spinor, gauge and
gravity field theories are governed by quantum-mechanical supersymmetry. The 4d
massless modes turn out to correspond to zero energy vacuum states of the
supersymmet... | [
{
"created": "Thu, 12 Jan 2012 00:20:19 GMT",
"version": "v1"
}
] | 2012-01-13 | [
[
"Sakamoto",
"Makoto",
""
]
] | We study higher dimensional field theories with extra dimensions from a 4d spectrum point of view. It is shown that 4d mass spectra of spinor, gauge and gravity field theories are governed by quantum-mechanical supersymmetry. The 4d massless modes turn out to correspond to zero energy vacuum states of the supersymmetry... | 11.927135 | 10.12999 | 10.581347 | 9.411119 | 10.886395 | 10.177617 | 10.084015 | 9.693868 | 9.893019 | 11.194044 | 9.65044 | 10.422587 | 10.582298 | 10.187013 | 9.829427 | 10.629499 | 9.660151 | 9.89998 | 9.704718 | 10.76985 | 10.26366 |
hep-th/0310212 | Wung-Hong Huang | Wung-Hong Huang | Thermal Instability of Giant Graviton in Matrix Model on PP-wave
Background | Latex, 8 pages, typos corrected, mention the elliptic deformation of
giant graviton | Phys.Rev. D69 (2004) 067701 | 10.1103/PhysRevD.69.067701 | null | hep-th | null | The thermal instability of the giant graviton is investigated within the BMN
matrix model. We calculate the one-loop thermal correction of the quantum
fluctuation around the trivial vacuum and giant graviton respectively. From the
exact formula of the free energy we see that at low temperature the giant
graviton is u... | [
{
"created": "Thu, 23 Oct 2003 07:48:27 GMT",
"version": "v1"
},
{
"created": "Tue, 2 Dec 2003 13:07:06 GMT",
"version": "v2"
},
{
"created": "Tue, 23 Dec 2003 10:25:32 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Huang",
"Wung-Hong",
""
]
] | The thermal instability of the giant graviton is investigated within the BMN matrix model. We calculate the one-loop thermal correction of the quantum fluctuation around the trivial vacuum and giant graviton respectively. From the exact formula of the free energy we see that at low temperature the giant graviton is uns... | 8.812171 | 7.454524 | 8.754798 | 7.504224 | 7.641349 | 7.881205 | 7.207306 | 7.395667 | 7.571075 | 9.430662 | 7.431937 | 7.915934 | 8.392019 | 7.989806 | 8.250304 | 7.760441 | 7.926215 | 8.516947 | 7.902685 | 8.896648 | 7.784719 |
hep-th/9910216 | Peter Mayr | P. Mayr | Non-perturbative N=1 strings from geometric singularities | LaTex, 11 pp | Class.Quant.Grav.17:1205-1214,2000 | 10.1088/0264-9381/17/5/329 | CERN-TH/99-327 | hep-th | null | The study of curved D-brane geometries in type II strings implies a general
relation between local singularities $\cx W$ of Calabi-Yau manifolds and
gravity free supersymmetric QFT's. The minimal supersymmetric case is described
by F-theory compactifications on $\cx W$ and can be used as a starting point to
define mi... | [
{
"created": "Wed, 27 Oct 1999 09:48:52 GMT",
"version": "v1"
}
] | 2011-04-15 | [
[
"Mayr",
"P.",
""
]
] | The study of curved D-brane geometries in type II strings implies a general relation between local singularities $\cx W$ of Calabi-Yau manifolds and gravity free supersymmetric QFT's. The minimal supersymmetric case is described by F-theory compactifications on $\cx W$ and can be used as a starting point to define mini... | 13.391862 | 11.678 | 15.564049 | 11.368349 | 11.489469 | 11.865335 | 11.062897 | 12.435953 | 10.491768 | 15.64656 | 11.941175 | 12.246821 | 14.095037 | 12.571399 | 11.723603 | 11.938457 | 11.948975 | 12.232866 | 13.021486 | 13.575715 | 12.311818 |
hep-th/0309057 | Emilian Dudas | E. Dudas, J. Mourad and C. Timirgaziu | On cosmologically induced hierarchies in string theory | 12 pages, LaTeX, interpretation of the solution clarified, typos
corrected, references added | JCAP 0403 (2004) 005 | 10.1088/1475-7516/2004/03/005 | CPHT RR 042.0703, LPT-ORSAY 03-57 | hep-th | null | We propose, within a perturbative string theory example, a cosmological way
to generate a large hierarchy between the observed Planck mass and the
fundamental string scale. Time evolution results in three large space
dimensions, one additional dimension transverse to our world and five small
internal dimensions with ... | [
{
"created": "Thu, 4 Sep 2003 16:52:37 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Sep 2003 16:12:46 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Dudas",
"E.",
""
],
[
"Mourad",
"J.",
""
],
[
"Timirgaziu",
"C.",
""
]
] | We propose, within a perturbative string theory example, a cosmological way to generate a large hierarchy between the observed Planck mass and the fundamental string scale. Time evolution results in three large space dimensions, one additional dimension transverse to our world and five small internal dimensions with a ... | 13.082996 | 12.571186 | 12.590014 | 12.129613 | 14.610146 | 13.208539 | 13.719018 | 13.171877 | 12.312466 | 12.827918 | 12.80634 | 12.646361 | 12.396035 | 12.043817 | 12.401312 | 12.890617 | 11.932436 | 11.95574 | 11.923521 | 12.448209 | 12.419432 |
0812.4607 | Orfeu Bertolami | Orfeu Bertolami and Carlos A. D. Zarro | Stability Conditions For a Noncommutative Scalar Field Coupled to
Gravity | 12 pages. Version to match the one to appear in Physics Letters B | Phys.Lett.B673:83-89,2009 | 10.1016/j.physletb.2009.02.001 | DF/IST-8.2008 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a noncommutative scalar field with a covariantly constant
noncommutative parameter in a curved space-time background. For a potential as
a noncommutative polynomial it is shown that the stability conditions are
unaffected by the noncommutativity, a result that is valid irrespective whether
space-time has ... | [
{
"created": "Thu, 25 Dec 2008 13:24:12 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Feb 2009 13:59:06 GMT",
"version": "v2"
}
] | 2011-08-02 | [
[
"Bertolami",
"Orfeu",
""
],
[
"Zarro",
"Carlos A. D.",
""
]
] | We consider a noncommutative scalar field with a covariantly constant noncommutative parameter in a curved space-time background. For a potential as a noncommutative polynomial it is shown that the stability conditions are unaffected by the noncommutativity, a result that is valid irrespective whether space-time has ho... | 10.138468 | 7.811916 | 8.685709 | 8.124296 | 7.966706 | 8.171132 | 8.155342 | 7.580213 | 8.447634 | 8.887069 | 7.765864 | 7.928892 | 8.694399 | 8.299113 | 8.3315 | 8.37483 | 8.319354 | 8.439052 | 8.233014 | 8.47156 | 8.115767 |
hep-th/9510109 | Jorge Russo | A. Fabbri and J.G. Russo | Soluble models in 2d dilaton gravity | 15 pages, harvmac, 3 figures | Phys.Rev.D53:6995-7002,1996 | 10.1103/PhysRevD.53.6995 | CERN-TH/95-267, SISSA-ISAS/118/95/EP | hep-th | null | A one-parameter class of simple models of two-dimensional dilaton gravity,
which can be exactly solved including back-reaction effects, is investigated at
both classical and quantum levels. This family contains the RST model as a
special case, and it continuously interpolates between models having a flat
(Rindler) ge... | [
{
"created": "Mon, 16 Oct 1995 17:11:48 GMT",
"version": "v1"
}
] | 2011-09-09 | [
[
"Fabbri",
"A.",
""
],
[
"Russo",
"J. G.",
""
]
] | A one-parameter class of simple models of two-dimensional dilaton gravity, which can be exactly solved including back-reaction effects, is investigated at both classical and quantum levels. This family contains the RST model as a special case, and it continuously interpolates between models having a flat (Rindler) geom... | 9.093574 | 7.045518 | 8.682772 | 7.922469 | 8.207341 | 8.437768 | 7.730025 | 8.057793 | 7.517296 | 9.516162 | 7.948605 | 8.021157 | 8.507287 | 8.158964 | 8.151531 | 7.717643 | 7.996839 | 7.946958 | 8.204285 | 8.451323 | 8.140867 |
hep-th/9401003 | null | G. Bonneau, G. Valent | Local heterotic geometry in holomorphic coordinates | 27 pages, latex file, report number PAR/LPTHE/93-56 | Class.Quant.Grav.11:1133-1154,1994 | 10.1088/0264-9381/11/5/004 | null | hep-th | null | In the same spirit as done for N=2 and N=4 supersymmetric non-linear $\si$
models in 2 space-time dimensions by Zumino and Alvarez- Gaum\'e and Freedman,
we analyse the (2,0) and (4,0) heterotic geometry in holomorphic coordinates.
We study the properties of the torsion tensor and give the conditions under
which (2,0... | [
{
"created": "Mon, 3 Jan 1994 16:07:57 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jan 1994 16:59:39 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Bonneau",
"G.",
""
],
[
"Valent",
"G.",
""
]
] | In the same spirit as done for N=2 and N=4 supersymmetric non-linear $\si$ models in 2 space-time dimensions by Zumino and Alvarez- Gaum\'e and Freedman, we analyse the (2,0) and (4,0) heterotic geometry in holomorphic coordinates. We study the properties of the torsion tensor and give the conditions under which (2,0) ... | 9.662787 | 8.60189 | 10.192527 | 8.519782 | 9.480629 | 8.667192 | 9.206434 | 9.324551 | 8.985849 | 10.825181 | 8.816391 | 8.847802 | 9.17277 | 8.679789 | 8.354082 | 8.93402 | 8.890103 | 8.830966 | 8.52181 | 9.391195 | 8.582385 |
0812.1549 | Matteo Cardella Dr. | Matteo Cardella | A novel method for computing torus amplitudes for $\mathbb{Z}_{N}$
orbifolds without the unfolding technique | 15 pages, 2 figures,V2: style improved, typos corrected, references
added | JHEP 0905:010,2009 | 10.1088/1126-6708/2009/05/010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A novel method for computing torus amplitudes in orbifold compactifications
is suggested. It applies universally for every Abelian $\mathbb{Z}_{N}$
orbifold without requiring the unfolding technique. This method follows from
the possibility of obtaining integrals over fundamental domains of every Hecke
congruence sub... | [
{
"created": "Mon, 8 Dec 2008 20:19:20 GMT",
"version": "v1"
},
{
"created": "Sun, 8 Mar 2009 15:25:34 GMT",
"version": "v2"
}
] | 2010-01-15 | [
[
"Cardella",
"Matteo",
""
]
] | A novel method for computing torus amplitudes in orbifold compactifications is suggested. It applies universally for every Abelian $\mathbb{Z}_{N}$ orbifold without requiring the unfolding technique. This method follows from the possibility of obtaining integrals over fundamental domains of every Hecke congruence subgr... | 17.701385 | 14.296506 | 18.727806 | 15.226183 | 14.74515 | 13.723735 | 13.923821 | 14.685405 | 15.153512 | 22.433441 | 14.756948 | 15.078857 | 15.736951 | 15.02218 | 14.957339 | 14.951568 | 15.117208 | 14.825503 | 14.461562 | 16.745619 | 15.102974 |
2003.11034 | Koen Stemerdink | Chris Hull, Eric Marcus, Koen Stemerdink, Stefan Vandoren | Black holes in string theory with duality twists | Main text 48 pages. v2: minor revisions | null | 10.1007/JHEP07(2020)086 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider 5D supersymmetric black holes in string theory compactifications
that partially break supersymmetry. We compactify type IIB on $T^4$ and then
further compactify on a circle with a duality twist to give Minkowski vacua
preserving partial supersymmetry ($\mathcal{N}=6,4,2,0$) in five dimensions.
The effecti... | [
{
"created": "Tue, 24 Mar 2020 18:00:03 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jun 2020 12:46:50 GMT",
"version": "v2"
}
] | 2020-08-26 | [
[
"Hull",
"Chris",
""
],
[
"Marcus",
"Eric",
""
],
[
"Stemerdink",
"Koen",
""
],
[
"Vandoren",
"Stefan",
""
]
] | We consider 5D supersymmetric black holes in string theory compactifications that partially break supersymmetry. We compactify type IIB on $T^4$ and then further compactify on a circle with a duality twist to give Minkowski vacua preserving partial supersymmetry ($\mathcal{N}=6,4,2,0$) in five dimensions. The effective... | 7.720936 | 7.292815 | 8.719547 | 7.46807 | 7.648751 | 7.340704 | 7.620557 | 7.485391 | 7.144263 | 8.901928 | 7.366643 | 7.43358 | 8.293872 | 7.268558 | 7.440494 | 7.463654 | 7.215866 | 7.252241 | 7.485431 | 7.888805 | 7.27817 |
hep-th/0203154 | Oleg Ruchayskiy | Alexey Boyarsky, Jeffrey A. Harvey, Oleg Ruchayskiy | A Toy Model of the M5-brane: Anomalies of Monopole Strings in Five
Dimensions | 32 pages, LaTeX | Annals Phys. 301 (2002) 1-21 | 10.1006/aphy.2002.6294 | null | hep-th | null | We study a five-dimensional field theory which contains a monopole (string)
solution with chiral fermion zero modes. This monostring solution is a close
analog of the fivebrane solution of M-theory. The cancellation of normal bundle
anomalies parallels that for the M-theory fivebrane, in particular, the
presence of a... | [
{
"created": "Sun, 17 Mar 2002 22:35:08 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Boyarsky",
"Alexey",
""
],
[
"Harvey",
"Jeffrey A.",
""
],
[
"Ruchayskiy",
"Oleg",
""
]
] | We study a five-dimensional field theory which contains a monopole (string) solution with chiral fermion zero modes. This monostring solution is a close analog of the fivebrane solution of M-theory. The cancellation of normal bundle anomalies parallels that for the M-theory fivebrane, in particular, the presence of a C... | 10.84535 | 9.064496 | 10.237022 | 8.554869 | 9.509982 | 9.66593 | 9.445003 | 9.149756 | 9.424299 | 12.488467 | 9.885073 | 9.696056 | 10.664839 | 9.661253 | 9.914456 | 9.890548 | 9.704046 | 9.921629 | 9.255225 | 10.81503 | 9.776897 |
hep-th/0411084 | Eugen Radu | Eugen Radu and D. H. Tchrakian | New axially symmetric Yang-Mills-Higgs solutions with negative
cosmological constant | 18 pages, 7 figures; v2: typos corrected | Phys.Rev. D71 (2005) 064002 | 10.1103/PhysRevD.71.064002 | null | hep-th gr-qc | null | We construct numerically new axially symmetric solutions of SU(2)
Yang-Mills-Higgs theory in $(3+1)$ anti-de Sitter spacetime. Two types of
finite energy, regular configurations are considered: multimonopole solutions
with magnetic charge $n>1$ and monopole-antimonopole pairs with zero net
magnetic charge. A somewhat... | [
{
"created": "Mon, 8 Nov 2004 12:43:22 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Mar 2005 17:54:45 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Radu",
"Eugen",
""
],
[
"Tchrakian",
"D. H.",
""
]
] | We construct numerically new axially symmetric solutions of SU(2) Yang-Mills-Higgs theory in $(3+1)$ anti-de Sitter spacetime. Two types of finite energy, regular configurations are considered: multimonopole solutions with magnetic charge $n>1$ and monopole-antimonopole pairs with zero net magnetic charge. A somewhat d... | 7.142947 | 5.829369 | 6.603572 | 6.212812 | 6.143085 | 5.912948 | 6.090142 | 6.267356 | 6.192751 | 7.222851 | 5.836309 | 6.589937 | 6.857831 | 6.433837 | 6.651557 | 6.502132 | 6.464829 | 6.553996 | 6.465646 | 6.964066 | 6.52564 |
1505.02645 | A. Bashir | M. Jamil Aslam, A. Bashir, L.X. Gutierrez-Guerrero | Local Gauge Transformation for the Quark Propagator in an SU(N) Gauge
Theory | 8 pages, no figures | Phys. Rev. D 93, 076001 (2016) | 10.1103/PhysRevD.93.076001 | null | hep-th hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In an SU(N) gauge field theory, the n-point Green functions, namely,
propagators and vertices, transform under the simultaneous local gauge
variations of the gluon vector potential and the quark matter field in such a
manner that the physical observables remain invariant. In this article, we
derive this intrinsically... | [
{
"created": "Mon, 11 May 2015 14:46:51 GMT",
"version": "v1"
}
] | 2016-04-06 | [
[
"Aslam",
"M. Jamil",
""
],
[
"Bashir",
"A.",
""
],
[
"Gutierrez-Guerrero",
"L. X.",
""
]
] | In an SU(N) gauge field theory, the n-point Green functions, namely, propagators and vertices, transform under the simultaneous local gauge variations of the gluon vector potential and the quark matter field in such a manner that the physical observables remain invariant. In this article, we derive this intrinsically n... | 8.228029 | 9.755559 | 8.585625 | 8.331359 | 8.978473 | 8.924383 | 8.663088 | 8.82676 | 7.905267 | 8.283773 | 8.398941 | 7.97766 | 8.042567 | 7.910123 | 8.536754 | 8.024286 | 7.877524 | 8.091943 | 7.704669 | 7.82093 | 8.236245 |
1912.06929 | Amlan Chakraborty | Taushif Ahmed, Pulak Banerjee, Amlan Chakraborty, Prasanna K. Dhani,
V. Ravindran, Satyajit Seth | Infrared structure of $\mathcal{N}$ = 4 SYM and leading
transcendentality principle in gauge theory | 10 pages, Contribution to the 14th International Symposium on
Radiative Corrections (RADCOR2019), 9-13 September 2019, Palais des Papes,
Avignon, France | PoS(RADCOR2019)059 | null | MPP-2019-247 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a detailed study on the infrared structure of $\mathcal{N}=4$ SYM
and its connection to QCD. Calculation of collinear splitting functions helps
to understand the structure and thus one can get infrared safe cross sections.
We also demonstrate the factorization property that soft plus virtual part of
the cr... | [
{
"created": "Sat, 14 Dec 2019 21:14:22 GMT",
"version": "v1"
}
] | 2019-12-30 | [
[
"Ahmed",
"Taushif",
""
],
[
"Banerjee",
"Pulak",
""
],
[
"Chakraborty",
"Amlan",
""
],
[
"Dhani",
"Prasanna K.",
""
],
[
"Ravindran",
"V.",
""
],
[
"Seth",
"Satyajit",
""
]
] | We present a detailed study on the infrared structure of $\mathcal{N}=4$ SYM and its connection to QCD. Calculation of collinear splitting functions helps to understand the structure and thus one can get infrared safe cross sections. We also demonstrate the factorization property that soft plus virtual part of the cros... | 14.601913 | 13.691569 | 13.912906 | 12.342395 | 13.753274 | 15.196795 | 13.441035 | 13.65651 | 12.345638 | 15.309115 | 14.369768 | 13.666561 | 14.545361 | 13.327473 | 13.465021 | 13.948311 | 14.083226 | 14.054374 | 13.42346 | 14.228876 | 13.815596 |
hep-th/0202191 | Seungjoon Hyun | Seungjoon Hyun and Hyeonjoon Shin | Dynamical Aspects on Duality between SYM and NCOS from D2-F1 Bound State | 16 pages, latex2e, 2 figures; v2 : Improved version with corrections
in eq. (33) and other minor corrections. One reference added | JHEP 0204 (2002) 044 | 10.1088/1126-6708/2002/04/044 | KIAS-P01031 | hep-th | null | It has been shown that (2+1)-dimensional N=8 super Yang-Mills (SYM) theory
with electric flux is related to (2+1)- dimensional noncommutative open string
(NCOS) theory by `2-11' flip. This implies that the instanton process in SYM
theory, which corresponds to D0-brane exchange (M-momentum transfer) between
D2-branes,... | [
{
"created": "Wed, 27 Feb 2002 13:51:07 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Apr 2002 09:56:26 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Hyun",
"Seungjoon",
""
],
[
"Shin",
"Hyeonjoon",
""
]
] | It has been shown that (2+1)-dimensional N=8 super Yang-Mills (SYM) theory with electric flux is related to (2+1)- dimensional noncommutative open string (NCOS) theory by `2-11' flip. This implies that the instanton process in SYM theory, which corresponds to D0-brane exchange (M-momentum transfer) between D2-branes, i... | 9.805297 | 9.312573 | 10.377477 | 8.956777 | 9.473274 | 9.450553 | 9.37018 | 9.085481 | 9.288036 | 11.527815 | 9.028105 | 9.103992 | 9.749525 | 9.185609 | 9.400035 | 9.22263 | 9.257319 | 9.453163 | 9.389301 | 10.11711 | 9.236561 |
1907.12110 | Lin Chen | Bin Chen, Lin Chen and Cheng-Yong Zhang | Surface/State correspondence and $T\overline{T}$ deformation | 7 pages, 4 figures | Phys. Rev. D 101, 106011 (2020) | 10.1103/PhysRevD.101.106011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The surface/state correspondence suggests that the bulk co-dimensional two
surface could be dual to the quantum state in the holographic conformal field
theory(CFT). Inspired by the cutoff-AdS/$T\overline{T}$-deformed-CFT
correspondence, we propose that the quantum states of two-dimensional
$T\overline{T}$-deformed h... | [
{
"created": "Sun, 28 Jul 2019 17:10:18 GMT",
"version": "v1"
}
] | 2020-05-20 | [
[
"Chen",
"Bin",
""
],
[
"Chen",
"Lin",
""
],
[
"Zhang",
"Cheng-Yong",
""
]
] | The surface/state correspondence suggests that the bulk co-dimensional two surface could be dual to the quantum state in the holographic conformal field theory(CFT). Inspired by the cutoff-AdS/$T\overline{T}$-deformed-CFT correspondence, we propose that the quantum states of two-dimensional $T\overline{T}$-deformed hol... | 8.386635 | 6.651754 | 9.596116 | 6.958625 | 7.503078 | 6.476634 | 7.225363 | 6.486412 | 6.614799 | 10.533321 | 7.099825 | 7.324827 | 8.256679 | 7.465787 | 7.532113 | 7.47714 | 7.465104 | 7.539121 | 7.154698 | 8.326295 | 7.534737 |
hep-th/0608105 | Kazuo Ghoroku | Iver Brevik and Kazuo Ghoroku | Shear Viscosity of Yang-Mills Theory in the Confinement Phase | 11 pages latex, 2 figures; minor changes in the discussion, reference
added. To appear in Int. J. Mod. Phys. D | Int.J.Mod.Phys.D16:1249-1260,2007 | 10.1142/S0218271807010766 | FIT HE-06-02 | hep-th gr-qc | null | In terms of a simple holographic model, we study the absorption cross section
and the shear viscosity of a pure Yang-Mills field at low temperature where the
system is in the confinement phase. Then we expect that the glueball states are
the dominant modes in this phase. In our holographic model an infrared cutoff
r_... | [
{
"created": "Wed, 16 Aug 2006 08:37:51 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Mar 2007 09:03:22 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Brevik",
"Iver",
""
],
[
"Ghoroku",
"Kazuo",
""
]
] | In terms of a simple holographic model, we study the absorption cross section and the shear viscosity of a pure Yang-Mills field at low temperature where the system is in the confinement phase. Then we expect that the glueball states are the dominant modes in this phase. In our holographic model an infrared cutoff r_m ... | 8.257518 | 8.935798 | 7.687925 | 8.100327 | 8.037704 | 8.533783 | 8.621466 | 8.693818 | 7.897897 | 8.582807 | 7.972963 | 7.769763 | 7.848334 | 7.715883 | 8.112031 | 8.104282 | 7.979325 | 8.135191 | 7.611872 | 7.728085 | 7.85152 |
hep-th/0401072 | Richard Szabo | Giovanni Landi, Fedele Lizzi and Richard J. Szabo | Matrix Quantum Mechanics and Soliton Regularization of Noncommutative
Field Theory | 70 pages, 4 figures; v2: References added and updated | Adv.Theor.Math.Phys.8:1-82,2004 | null | DSF-36-03, HWM-03-30, EMPG-03-22 | hep-th math-ph math.MP | null | We construct an approximation to field theories on the noncommutative torus
based on soliton projections and partial isometries which together form a
matrix algebra of functions on the sum of two circles. The matrix quantum
mechanics is applied to the perturbative dynamics of scalar field theory, to
tachyon dynamics ... | [
{
"created": "Mon, 12 Jan 2004 13:20:40 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Jan 2004 12:28:20 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Landi",
"Giovanni",
""
],
[
"Lizzi",
"Fedele",
""
],
[
"Szabo",
"Richard J.",
""
]
] | We construct an approximation to field theories on the noncommutative torus based on soliton projections and partial isometries which together form a matrix algebra of functions on the sum of two circles. The matrix quantum mechanics is applied to the perturbative dynamics of scalar field theory, to tachyon dynamics in... | 9.06288 | 8.042873 | 9.046932 | 7.93537 | 7.986679 | 8.056719 | 8.373902 | 8.609499 | 8.179363 | 8.52019 | 7.822608 | 8.023671 | 8.835793 | 8.157661 | 8.271476 | 8.032623 | 8.0416 | 8.132583 | 8.259572 | 8.590277 | 8.024666 |
1206.2015 | Bin Chen | Bin Chen, Shen-xiu Liu and Jia-ju Zhang | Thermodynamics of Black Hole Horizons and Kerr/CFT Correspondence | 29 pages; match published version | null | 10.1007/JHEP11(2012)017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate the thermodynamics of the inner horizon and its
implication on the holographic description of the black hole. We focus on the
black holes with two physical horizons. Under reasonable assumption, we prove
that the first law of thermodynamics of the outer horizon always indicates that
of th... | [
{
"created": "Sun, 10 Jun 2012 10:25:26 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Nov 2012 00:33:25 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Chen",
"Bin",
""
],
[
"Liu",
"Shen-xiu",
""
],
[
"Zhang",
"Jia-ju",
""
]
] | In this paper we investigate the thermodynamics of the inner horizon and its implication on the holographic description of the black hole. We focus on the black holes with two physical horizons. Under reasonable assumption, we prove that the first law of thermodynamics of the outer horizon always indicates that of the ... | 6.878576 | 6.822785 | 7.086992 | 6.722255 | 6.87897 | 6.346959 | 6.635852 | 6.700313 | 6.543664 | 7.342752 | 6.632074 | 6.703135 | 6.900363 | 6.699538 | 6.680871 | 6.827899 | 6.720345 | 6.67279 | 6.789573 | 7.136137 | 6.697146 |
hep-th/0510040 | Miguel Vazquez-Mozo | Luis Alvarez-Gaume, Miguel A. Vazquez-Mozo | Introductory Lectures on Quantum Field Theory | 112 pages, 18 figures, LaTeX, cernrep style, feynmf. v4 typos
corrected and references added. v3 includes a new section on Feynman diagrams
and an expanded discussion on RG fixed points | CERN Yellow Report CERN-2010-001, pp. 1-96 | null | CERN-PH-TH-2009-257 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In these lectures we present a few topics in Quantum Field Theory in detail.
Some of them are conceptual and some more practical. They have been selected
because they appear frequently in current applications to Particle Physics and
String Theory.
| [
{
"created": "Wed, 5 Oct 2005 14:25:14 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Jun 2006 11:48:39 GMT",
"version": "v2"
},
{
"created": "Fri, 12 Feb 2010 15:00:49 GMT",
"version": "v3"
},
{
"created": "Wed, 20 Feb 2013 13:51:25 GMT",
"version": "v4"
}
] | 2013-02-21 | [
[
"Alvarez-Gaume",
"Luis",
""
],
[
"Vazquez-Mozo",
"Miguel A.",
""
]
] | In these lectures we present a few topics in Quantum Field Theory in detail. Some of them are conceptual and some more practical. They have been selected because they appear frequently in current applications to Particle Physics and String Theory. | 13.145238 | 10.239724 | 11.065028 | 10.429381 | 10.118008 | 10.962673 | 9.461453 | 11.30346 | 10.354905 | 12.394064 | 9.934972 | 10.103002 | 10.239939 | 10.140298 | 9.853197 | 9.758718 | 10.022731 | 10.171999 | 9.981799 | 10.609695 | 10.211214 |
hep-th/9201033 | Yuri Makeenko | L. Chekhov and Yu. Makeenko | The Multicritical Kontsevich-Penner Model | 13 pages | Mod.Phys.Lett. A7 (1992) 1223-1236 | 10.1142/S0217732392003700 | null | hep-th | null | We consider the hermitian matrix model with an external field entering the
quadratic term $\tr(\Lambda X\Lambda X)$ and Penner--like interaction term
$\alpha N(\log(1+X)-X)$. An explicit solution in the leading order in $N$ is
presented. The critical behaviour is given by the second derivative of the free
energy in $... | [
{
"created": "Thu, 16 Jan 1992 21:28:00 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Chekhov",
"L.",
""
],
[
"Makeenko",
"Yu.",
""
]
] | We consider the hermitian matrix model with an external field entering the quadratic term $\tr(\Lambda X\Lambda X)$ and Penner--like interaction term $\alpha N(\log(1+X)-X)$. An explicit solution in the leading order in $N$ is presented. The critical behaviour is given by the second derivative of the free energy in $\a... | 13.640112 | 13.624583 | 15.028914 | 13.311982 | 14.159062 | 14.41454 | 14.073235 | 13.77249 | 13.384551 | 16.414703 | 13.077348 | 13.629872 | 13.540423 | 12.814581 | 13.462745 | 13.082042 | 13.303174 | 12.719875 | 12.830671 | 13.730618 | 12.985133 |
0808.0696 | Michael Pawellek | Michael Pawellek | Quantization of Sine-Gordon solitons on the circle: semiclassical vs.
exact results | 20 pages, 5 figures | Nucl.Phys.B810:527-541,2009 | 10.1016/j.nuclphysb.2008.10.001 | FAU-TP3-08-06 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the semiclassical quantization of sine-Gordon solitons on the
circle with periodic and anti-periodic boundary conditions. The 1-loop quantum
corrections to the mass of the solitons are determined using zeta function
regularization in the integral representation. We compare the semiclassical
results with e... | [
{
"created": "Tue, 5 Aug 2008 17:42:56 GMT",
"version": "v1"
}
] | 2009-02-02 | [
[
"Pawellek",
"Michael",
""
]
] | We consider the semiclassical quantization of sine-Gordon solitons on the circle with periodic and anti-periodic boundary conditions. The 1-loop quantum corrections to the mass of the solitons are determined using zeta function regularization in the integral representation. We compare the semiclassical results with exa... | 8.961182 | 7.335356 | 9.11647 | 7.665175 | 7.495111 | 7.472183 | 7.146147 | 7.037372 | 7.678909 | 8.90962 | 7.606756 | 7.567696 | 8.508465 | 7.953897 | 7.836097 | 7.998166 | 7.849779 | 7.786123 | 7.903122 | 8.396453 | 8.024584 |
hep-th/0204014 | Chengbo Guan | Z. Chang, C. B. Guan | Dynamics of Massive Scalar Fields in dS Space and the dS/CFT
Correspondence | latex, 14 pages and 3 figures | Int.J.Mod.Phys. A17 (2002) 4591-4600 | 10.1142/S0217751X02012302 | null | hep-th | null | Global geometric properties of dS space are presented explicitly in various
coordinates. A Robertson-Walker like metric is deduced, which is convenient to
be used in study of dynamics in dS space. Singularities of wavefunctions of
massive scalar fields at boundary are demonstrated. A bulk-boundary propagator
is const... | [
{
"created": "Tue, 2 Apr 2002 06:16:54 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Chang",
"Z.",
""
],
[
"Guan",
"C. B.",
""
]
] | Global geometric properties of dS space are presented explicitly in various coordinates. A Robertson-Walker like metric is deduced, which is convenient to be used in study of dynamics in dS space. Singularities of wavefunctions of massive scalar fields at boundary are demonstrated. A bulk-boundary propagator is constru... | 16.954027 | 17.293692 | 16.965607 | 14.412733 | 16.701851 | 15.939074 | 15.206041 | 16.046787 | 15.033606 | 14.894334 | 14.852736 | 13.748552 | 14.901342 | 13.844127 | 14.208723 | 13.572268 | 13.592365 | 13.144029 | 13.405905 | 14.64837 | 13.055703 |
hep-th/0412207 | Sebastian Franco | Sebastian Franco, Yang-Hui He, Christopher Herzog and Johannes Walcher | Chaotic Cascades for D-branes on Singularities | 6 pages, 1 figure. Based on the presentation of S. F. at Cargese
Summer School 2004. To appear in the proceedings. V.2.: references added | null | null | null | hep-th | null | We briefly review our work on the cascading renormalization group flows for
gauge theories on D-branes probing Calabi-Yau singularities. Such RG flows are
sometimes chaotic and exhibit duality walls. We construct supergravity
solutions dual to logarithmic flows for these theories. We make new
observations about a sur... | [
{
"created": "Fri, 17 Dec 2004 23:05:25 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Feb 2005 20:56:43 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Franco",
"Sebastian",
""
],
[
"He",
"Yang-Hui",
""
],
[
"Herzog",
"Christopher",
""
],
[
"Walcher",
"Johannes",
""
]
] | We briefly review our work on the cascading renormalization group flows for gauge theories on D-branes probing Calabi-Yau singularities. Such RG flows are sometimes chaotic and exhibit duality walls. We construct supergravity solutions dual to logarithmic flows for these theories. We make new observations about a surfa... | 19.535532 | 16.862799 | 23.032164 | 15.346891 | 16.480583 | 17.336271 | 15.761312 | 15.304447 | 14.71151 | 23.260799 | 16.084904 | 17.296974 | 17.821688 | 15.878958 | 17.249996 | 16.681429 | 16.845091 | 15.886501 | 16.888273 | 17.690702 | 15.948756 |
2203.09709 | Tatsuya Ogawa | Yota Endo, Hideki Ishihara, and Tatsuya Ogawa | Relativistic Nontopological Soliton Stars in a U(1) Gauge Higgs Model | 22 pages, 32 figures, final version accepted in PRD | null | 10.1103/PhysRevD.105.104041 | OCU-PHYS 558, AP-GR 179, NITEP 132 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study spherically symmetric nontopological soliton stars (NTS stars)
numerically in the coupled system of a complex scalar field, a U(1) gauge
field, a complex Higgs scalar field, and Einstein gravity, where the symmetry
is broken spontaneously. The gravitational mass of NTS stars is limited by a
maximum mass for ... | [
{
"created": "Fri, 18 Mar 2022 03:01:36 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Mar 2022 05:50:12 GMT",
"version": "v2"
},
{
"created": "Thu, 14 Apr 2022 06:03:24 GMT",
"version": "v3"
}
] | 2022-06-01 | [
[
"Endo",
"Yota",
""
],
[
"Ishihara",
"Hideki",
""
],
[
"Ogawa",
"Tatsuya",
""
]
] | We study spherically symmetric nontopological soliton stars (NTS stars) numerically in the coupled system of a complex scalar field, a U(1) gauge field, a complex Higgs scalar field, and Einstein gravity, where the symmetry is broken spontaneously. The gravitational mass of NTS stars is limited by a maximum mass for a ... | 8.491861 | 9.742312 | 9.182018 | 8.28484 | 8.392732 | 8.287821 | 9.667656 | 8.145868 | 8.661031 | 9.528097 | 8.539807 | 8.776847 | 8.17942 | 8.251689 | 8.514211 | 8.594163 | 8.726724 | 8.334926 | 8.659117 | 8.089579 | 8.816413 |
hep-th/9812146 | Jacques Bros | Jacques Bros, Daniel Iagolnitzer | Universality of low-energy scattering in three-dimensional field theory | 4 pages, 2 figures, LaTex | Phys.Rev.D59:081701,1999 | 10.1103/PhysRevD.59.081701 | SPhT t98/026 | hep-th | null | Universal low-energy behaviour ${2 m c}\over{\ln |s-4m^2|}$ of the scattering
function of particles of positive mass m near the threshold $s=4m^2$, and
${\pi} \over {\ln |s-4m^2|}$ for the corresponding S-wave phase-shift, is
established for weakly coupled field theory models with a positive mass m in
space-time dime... | [
{
"created": "Thu, 17 Dec 1998 15:32:58 GMT",
"version": "v1"
}
] | 2009-12-30 | [
[
"Bros",
"Jacques",
""
],
[
"Iagolnitzer",
"Daniel",
""
]
] | Universal low-energy behaviour ${2 m c}\over{\ln |s-4m^2|}$ of the scattering function of particles of positive mass m near the threshold $s=4m^2$, and ${\pi} \over {\ln |s-4m^2|}$ for the corresponding S-wave phase-shift, is established for weakly coupled field theory models with a positive mass m in space-time dimens... | 11.044447 | 11.5102 | 12.233868 | 10.81388 | 12.334311 | 12.336279 | 11.512546 | 11.932869 | 10.877432 | 12.159891 | 11.437818 | 10.357646 | 10.202312 | 9.661694 | 10.019547 | 10.016405 | 10.047692 | 10.07561 | 9.801394 | 9.961648 | 9.750304 |
hep-th/0312044 | Mikhail Ivanov | M. G. Ivanov | String fluids and membrane media | 6 pages, LaTeX, The paper is based upon talk at SQS'03 (Dubna);
Discussion of different string fluid models and some references are added | null | null | null | hep-th | null | String (membrane) theory could be considered as degenerate case of
relativistic continuous media theory. The paper presents models of media, which
are continuous distributions of interacting membranes, strings or particles.
| [
{
"created": "Thu, 4 Dec 2003 13:47:12 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Jan 2004 15:29:41 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Ivanov",
"M. G.",
""
]
] | String (membrane) theory could be considered as degenerate case of relativistic continuous media theory. The paper presents models of media, which are continuous distributions of interacting membranes, strings or particles. | 26.186308 | 23.092884 | 24.45941 | 21.473644 | 21.398369 | 22.466156 | 24.661129 | 20.335924 | 20.074869 | 25.338539 | 23.149668 | 21.225706 | 22.037605 | 22.602518 | 22.144382 | 22.652176 | 21.708061 | 20.994234 | 22.926615 | 23.685139 | 20.905298 |
0802.0660 | Niclas Wyllard | Mans Henningson, Niclas Wyllard | Zero-energy states of N = 4 SYM on T^3: S-duality and the mapping class
group | 17 pages | JHEP 0804:066,2008 | 10.1088/1126-6708/2008/04/066 | null | hep-th | null | We continue our studies of the low-energy spectrum of N=4 super-Yang-Mills
theory on a spatial three-torus. In two previous papers, we computed the
spectrum of normalizable zero-energy states for all choices of gauge group and
all values of the electric and magnetic 't Hooft fluxes, and checked its
invariance under t... | [
{
"created": "Tue, 5 Feb 2008 16:32:03 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Henningson",
"Mans",
""
],
[
"Wyllard",
"Niclas",
""
]
] | We continue our studies of the low-energy spectrum of N=4 super-Yang-Mills theory on a spatial three-torus. In two previous papers, we computed the spectrum of normalizable zero-energy states for all choices of gauge group and all values of the electric and magnetic 't Hooft fluxes, and checked its invariance under the... | 6.639759 | 5.943407 | 7.209251 | 5.904036 | 6.452744 | 6.383667 | 5.999357 | 6.330802 | 6.329225 | 7.446573 | 5.83533 | 6.08238 | 6.282897 | 6.277908 | 5.990123 | 6.053269 | 6.212839 | 6.223349 | 5.916359 | 6.568254 | 6.143247 |
hep-th/0610192 | Nelson Pinto-Neto | Emanuel J. C. Pinho and Nelson Pinto-Neto | Scalar and Vector Perturbations in Quantum Cosmological Backgrounds | 19 pages, no figure | Phys.Rev.D76:023506,2007 | 10.1103/PhysRevD.76.023506 | null | hep-th | null | Generalizing a previous work concerning cosmological linear tensor
perturbations, we show that the lagrangians and hamiltonians of cosmological
linear scalar and vector perturbations can be put in simple form through the
implementation of canonical transformations and redefinitions of the lapse
function, without ever... | [
{
"created": "Tue, 17 Oct 2006 11:45:08 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Pinho",
"Emanuel J. C.",
""
],
[
"Pinto-Neto",
"Nelson",
""
]
] | Generalizing a previous work concerning cosmological linear tensor perturbations, we show that the lagrangians and hamiltonians of cosmological linear scalar and vector perturbations can be put in simple form through the implementation of canonical transformations and redefinitions of the lapse function, without ever u... | 9.64391 | 8.485892 | 8.567365 | 8.899396 | 8.86155 | 8.444587 | 8.571237 | 8.084203 | 8.238358 | 10.038721 | 8.765026 | 9.101934 | 8.5971 | 8.571829 | 8.682873 | 8.618734 | 8.772479 | 8.454225 | 8.69135 | 9.175326 | 8.754091 |
hep-th/9312170 | Shahn Majid | Shahn Majid and Ulrich Meyer | Braided Matrix Structure of $q$-Minkowski Space and $q$-Poincare Group | 12 pages | Z.Phys. C63 (1994) 357-362 | 10.1007/BF01411029 | DAMTP/93-68 | hep-th math.QA | null | We clarify the relation between the approach to $q$-Minkowski space of
Carow-Watamura et al. with an approach based on the idea of $2\times 2$ braided
Hermitean matrices. The latter are objects like super-matrices but with
Bose-Fermi statistics replaced by braid statistics. We also obtain new R-matrix
formulae for th... | [
{
"created": "Tue, 21 Dec 1993 17:26:11 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Majid",
"Shahn",
""
],
[
"Meyer",
"Ulrich",
""
]
] | We clarify the relation between the approach to $q$-Minkowski space of Carow-Watamura et al. with an approach based on the idea of $2\times 2$ braided Hermitean matrices. The latter are objects like super-matrices but with Bose-Fermi statistics replaced by braid statistics. We also obtain new R-matrix formulae for the ... | 10.683571 | 10.907838 | 13.096422 | 10.723072 | 10.655679 | 11.663241 | 11.200446 | 9.455112 | 11.572141 | 14.518212 | 10.163044 | 9.199971 | 9.648388 | 9.711913 | 9.687999 | 9.085136 | 9.662315 | 9.152845 | 9.59272 | 11.019906 | 9.138487 |
1410.4715 | Daniele Marmiroli | Daniele Marmiroli | Phase structure of $\mathcal{N}=2^*$ SYM on ellipsoids | 41 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyse the phase structure of an $\mathcal{N}=2$ massive deformation of
$\mathcal{N}=4$ SYM theory on an four-dimensional ellipsoid using recent
results on supersymmetric localisation. Besides the 't~Hooft coupling
$\lambda$, the relevant parameters appearing in the theory and discriminating
between the different... | [
{
"created": "Fri, 17 Oct 2014 13:15:10 GMT",
"version": "v1"
}
] | 2014-10-20 | [
[
"Marmiroli",
"Daniele",
""
]
] | We analyse the phase structure of an $\mathcal{N}=2$ massive deformation of $\mathcal{N}=4$ SYM theory on an four-dimensional ellipsoid using recent results on supersymmetric localisation. Besides the 't~Hooft coupling $\lambda$, the relevant parameters appearing in the theory and discriminating between the different p... | 6.983371 | 7.049118 | 8.073525 | 6.832956 | 7.538599 | 7.485074 | 7.336441 | 7.537594 | 7.149731 | 8.291827 | 7.182191 | 6.75644 | 7.278923 | 6.917416 | 6.995083 | 7.037895 | 6.88778 | 7.026738 | 6.995554 | 7.207201 | 6.867418 |
2303.10710 | Claudio Coriano | Claudio Corian\`o, Stefano Lionetti, Matteo Maria Maglio | Parity-Odd 3-Point Functions from CFT in Momentum Space and the Chiral
Anomaly | 32 pages, 2 figures, revised version with typo corrections | null | 10.1140/epjc/s10052-023-11661-1 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We illustrate how the Conformal Ward Identities (CWI) in momentum space for
parity-odd correlators determine the structure of a chiral anomaly interaction,
taking the example of the VVA (vector/vector/axial-vector) and AAA correlators
in momentum space. Only the conservation and the anomalous WIs, together with
the B... | [
{
"created": "Sun, 19 Mar 2023 16:41:16 GMT",
"version": "v1"
},
{
"created": "Wed, 22 Mar 2023 15:40:13 GMT",
"version": "v2"
},
{
"created": "Fri, 7 Jul 2023 11:45:06 GMT",
"version": "v3"
},
{
"created": "Mon, 9 Oct 2023 12:12:52 GMT",
"version": "v4"
}
] | 2023-10-10 | [
[
"Corianò",
"Claudio",
""
],
[
"Lionetti",
"Stefano",
""
],
[
"Maglio",
"Matteo Maria",
""
]
] | We illustrate how the Conformal Ward Identities (CWI) in momentum space for parity-odd correlators determine the structure of a chiral anomaly interaction, taking the example of the VVA (vector/vector/axial-vector) and AAA correlators in momentum space. Only the conservation and the anomalous WIs, together with the Bos... | 13.287962 | 14.705771 | 13.116753 | 12.861255 | 13.646837 | 14.056247 | 13.563787 | 14.120294 | 13.137604 | 14.329122 | 13.373165 | 13.300958 | 12.852976 | 12.558951 | 12.794239 | 13.019891 | 12.586664 | 12.849412 | 12.711141 | 13.142123 | 12.577065 |
hep-th/0304241 | Esko Keski-Vakkuri | Rahul Biswas, Esko Keski-Vakkuri, Robert G. Leigh, Sean Nowling and
Eric Sharpe | The Taming of Closed Time-like Curves | 37 pages, LaTeX2e, uses amssymb, amsmath and epsf macros, 8 eps and 3
ps figures; (v2): Two additional comments + one reference added; (v3):
corrections in discussion of CTCs + some clarifications | JHEP 0401:064,2004 | 10.1088/1126-6708/2004/01/064 | HIP-2003-28/TH, CERN-TH/2003-097 | hep-th gr-qc | null | We consider a $R^{1,d}/Z_2$ orbifold, where $Z_2$ acts by time and space
reversal, also known as the embedding space of the elliptic de Sitter space.
The background has two potentially dangerous problems: time-nonorientability
and the existence of closed time-like curves. We first show that closed causal
curves disap... | [
{
"created": "Mon, 28 Apr 2003 15:09:40 GMT",
"version": "v1"
},
{
"created": "Thu, 29 May 2003 11:08:31 GMT",
"version": "v2"
},
{
"created": "Wed, 26 Nov 2003 09:20:50 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Biswas",
"Rahul",
""
],
[
"Keski-Vakkuri",
"Esko",
""
],
[
"Leigh",
"Robert G.",
""
],
[
"Nowling",
"Sean",
""
],
[
"Sharpe",
"Eric",
""
]
] | We consider a $R^{1,d}/Z_2$ orbifold, where $Z_2$ acts by time and space reversal, also known as the embedding space of the elliptic de Sitter space. The background has two potentially dangerous problems: time-nonorientability and the existence of closed time-like curves. We first show that closed causal curves disappe... | 9.172398 | 9.337614 | 10.081051 | 9.247088 | 8.914164 | 9.183897 | 9.751615 | 9.280828 | 9.229098 | 10.335594 | 9.214486 | 8.83075 | 9.245777 | 8.989042 | 8.693076 | 8.87391 | 8.997814 | 8.830511 | 9.101332 | 9.129393 | 8.857119 |
2301.13702 | Carlo Angelantonj | Carlo Angelantonj, Ioannis Florakis and Giorgio Leone | Tachyons and Misaligned Supersymmetry in Closed String Vacua | 32 pages. Improvement based on an exact Rademacher expansion of the
Fourier coefficients of characters. Appendix A added. Refs added | null | 10.1007/JHEP06(2023)174 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a remarkable paper, Dienes discovered that the absence of physical
tachyons in closed string theory is intimately related to oscillations in the
net number of bosonic minus fermionic degrees of freedom, a pattern predicted
by an underlying misaligned supersymmetry. The average of these oscillations
was linked to a... | [
{
"created": "Tue, 31 Jan 2023 15:22:00 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Mar 2023 23:18:35 GMT",
"version": "v2"
}
] | 2023-07-26 | [
[
"Angelantonj",
"Carlo",
""
],
[
"Florakis",
"Ioannis",
""
],
[
"Leone",
"Giorgio",
""
]
] | In a remarkable paper, Dienes discovered that the absence of physical tachyons in closed string theory is intimately related to oscillations in the net number of bosonic minus fermionic degrees of freedom, a pattern predicted by an underlying misaligned supersymmetry. The average of these oscillations was linked to an ... | 8.476364 | 8.606987 | 8.329981 | 7.887726 | 8.407084 | 8.458182 | 8.651302 | 8.358101 | 7.991755 | 8.715241 | 7.827633 | 7.731806 | 7.946636 | 7.614111 | 7.514787 | 7.770935 | 7.819817 | 7.604368 | 7.718085 | 8.059893 | 7.62531 |
2404.18994 | Pierre Heidmann | Rapha\"el Dulac and Pierre Heidmann | Building the Blocks of Schwarzschild | v2: published version; 36 pages + Appendix, 19 figures | null | 10.1007/JHEP07(2024)234 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate that the Schwarzschild black hole can be ``resolved'' into
bound states of Reissner-Nordstr\"om black holes in four dimensions. These
bound states closely resemble the Schwarzschild geometry from the asymptotic
region up to an infinitesimal distance away from the Schwarzschild horizon.
Below this scale... | [
{
"created": "Mon, 29 Apr 2024 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 31 Jul 2024 10:39:43 GMT",
"version": "v2"
}
] | 2024-08-01 | [
[
"Dulac",
"Raphaël",
""
],
[
"Heidmann",
"Pierre",
""
]
] | We demonstrate that the Schwarzschild black hole can be ``resolved'' into bound states of Reissner-Nordstr\"om black holes in four dimensions. These bound states closely resemble the Schwarzschild geometry from the asymptotic region up to an infinitesimal distance away from the Schwarzschild horizon. Below this scale, ... | 11.873072 | 12.028645 | 11.644528 | 11.227921 | 12.088237 | 11.16007 | 11.429514 | 10.770448 | 11.641094 | 11.451242 | 11.095146 | 11.089596 | 11.703221 | 11.026582 | 11.162988 | 10.92425 | 11.136252 | 11.047733 | 11.3576 | 11.716628 | 11.059139 |
2110.15112 | Nafiz Ishtiaque | Nafiz Ishtiaque, Seyed Faroogh Moosavian, Surya Raghavendran and Junya
Yagi | Superspin chains from superstring theory | 49+14 pages. v2: corrected typos in section 3.4.2 | SciPost Phys. 13 (2022) 083 | 10.21468/SciPostPhys.13.4.083 | null | hep-th math-ph math.MP nlin.SI | http://creativecommons.org/licenses/by/4.0/ | We present a correspondence between two-dimensional $\mathcal{N} = (2,2)$
supersymmetric gauge theories and rational integrable $\mathfrak{gl}(m|n)$ spin
chains with spin variables taking values in Verma modules. To explain this
correspondence, we realize the gauge theories as configurations of branes in
string theor... | [
{
"created": "Thu, 28 Oct 2021 13:53:11 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Dec 2022 03:16:04 GMT",
"version": "v2"
}
] | 2022-12-13 | [
[
"Ishtiaque",
"Nafiz",
""
],
[
"Moosavian",
"Seyed Faroogh",
""
],
[
"Raghavendran",
"Surya",
""
],
[
"Yagi",
"Junya",
""
]
] | We present a correspondence between two-dimensional $\mathcal{N} = (2,2)$ supersymmetric gauge theories and rational integrable $\mathfrak{gl}(m|n)$ spin chains with spin variables taking values in Verma modules. To explain this correspondence, we realize the gauge theories as configurations of branes in string theory ... | 6.020139 | 5.75493 | 7.499604 | 5.452393 | 5.762028 | 5.701634 | 5.996308 | 5.755049 | 5.336245 | 8.866931 | 5.701012 | 6.077824 | 6.376163 | 5.679901 | 5.786518 | 5.820907 | 5.966428 | 5.608379 | 5.613934 | 6.079863 | 5.667299 |
hep-th/9406084 | Rim Chai Ho | K. H. Cho and S. U. Park | Deformed Algebras from Inverse Schwinger Method | 14 pages, Jeonju University Report, Latex | J.Phys. A28 (1995) 1005-1016 | 10.1088/0305-4470/28/4/023 | null | hep-th | null | We consider a problem which may be viewed as an inverse one to the Schwinger
realization of Lie algebra, and suggest a procedure of deforming the
so-obtained algebra. We illustrate the method through a few simple examples
extending Schwinger's $su(1,1)$ construction. As results, various q-deformed
algebras are (re-)p... | [
{
"created": "Tue, 14 Jun 1994 12:24:56 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Cho",
"K. H.",
""
],
[
"Park",
"S. U.",
""
]
] | We consider a problem which may be viewed as an inverse one to the Schwinger realization of Lie algebra, and suggest a procedure of deforming the so-obtained algebra. We illustrate the method through a few simple examples extending Schwinger's $su(1,1)$ construction. As results, various q-deformed algebras are (re-)pro... | 14.238698 | 13.225804 | 13.748975 | 12.176192 | 13.291552 | 14.133783 | 13.468292 | 12.319311 | 12.168757 | 15.416246 | 13.504056 | 12.321766 | 13.626019 | 12.743557 | 12.795066 | 12.805204 | 12.472756 | 12.418206 | 12.66438 | 13.342361 | 13.188944 |
hep-th/0406054 | Artemio Gonzalez-Lopez | A. Enciso, F. Finkel, A. Gonzalez-Lopez, M.A. Rodriguez | Haldane-Shastry spin chains of BC_N type | LaTeX, 26 pages, 3 figures, to appear in Nucl. Phys. B | Nucl.Phys. B707 (2005) 553-576 | 10.1016/j.nuclphysb.2004.10.064 | null | hep-th cond-mat.str-el nlin.SI | null | We introduce four types of SU(2M+1) spin chains which can be regarded as the
BC_N versions of the celebrated Haldane-Shastry chain. These chains depend on
two free parameters and, unlike the original Haldane-Shastry chain, their sites
need not be equally spaced. We prove that all four chains are solvable by
deriving ... | [
{
"created": "Sat, 5 Jun 2004 11:49:45 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Dec 2004 14:29:47 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Enciso",
"A.",
""
],
[
"Finkel",
"F.",
""
],
[
"Gonzalez-Lopez",
"A.",
""
],
[
"Rodriguez",
"M. A.",
""
]
] | We introduce four types of SU(2M+1) spin chains which can be regarded as the BC_N versions of the celebrated Haldane-Shastry chain. These chains depend on two free parameters and, unlike the original Haldane-Shastry chain, their sites need not be equally spaced. We prove that all four chains are solvable by deriving an... | 7.568414 | 7.324795 | 8.965757 | 7.68436 | 8.017705 | 8.08012 | 7.938289 | 7.52301 | 7.566777 | 9.174101 | 7.516577 | 7.71032 | 8.239567 | 7.636826 | 7.66841 | 7.55879 | 7.580562 | 7.491012 | 7.545199 | 8.133363 | 7.650023 |
1607.01315 | Nikolaos Mavromatos | Nick E. Mavromatos and Sarben Sarkar | Magnetic Monopoles from Global Monopoles in the presence of Kalb-Ramond
Torsion | 27 pages revtex, no figures, expanded version, updated references,
updated discussion (within string theory) with details, justifying the
induction of a magnetic-monopole type field by the Kalb-Ramond axion field,
no effect on conclusions | Phys. Rev. D 95, 104025 (2017) | 10.1103/PhysRevD.95.104025 | KCL-PH-TH-2016-40 | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Possible classical solutions for electromagnetic monopoles induced by
gravitational (global) monopoles in the presence of torsion are found. Such
solutions rely on a non-zero (Kalb-Ramond) torsion strength, which may
characterise low energy theories inspired from string models. Bounds from the
current run of the LHC ... | [
{
"created": "Tue, 5 Jul 2016 16:24:00 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Nov 2016 17:31:10 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Feb 2017 11:18:14 GMT",
"version": "v3"
}
] | 2017-05-24 | [
[
"Mavromatos",
"Nick E.",
""
],
[
"Sarkar",
"Sarben",
""
]
] | Possible classical solutions for electromagnetic monopoles induced by gravitational (global) monopoles in the presence of torsion are found. Such solutions rely on a non-zero (Kalb-Ramond) torsion strength, which may characterise low energy theories inspired from string models. Bounds from the current run of the LHC ex... | 16.282518 | 15.272764 | 13.831905 | 14.356071 | 14.287554 | 14.471503 | 14.779081 | 14.99896 | 13.360687 | 14.334073 | 15.043036 | 14.576515 | 14.85253 | 14.845318 | 14.870628 | 14.737188 | 14.3314 | 13.921343 | 13.953033 | 14.32866 | 14.113334 |
1507.05420 | Timothy J. Hollowood | Calan Appadu and Timothy J. Hollowood | Beta Function of k Deformed AdS_5 x S^5 String Theory | 26 pages, some typos corrected | null | 10.1007/JHEP11(2015)095 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculate the one loop beta function for the would-be marginal coupling on
the world sheet of the k deformed sigma models associated to a quantum group
with q=exp(i pi/k). This includes the bosonic principal chiral models and
symmetric space sigma models but also the k deformed semi-symmetric space sigma
model des... | [
{
"created": "Mon, 20 Jul 2015 09:06:20 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Sep 2015 15:50:42 GMT",
"version": "v2"
}
] | 2016-01-20 | [
[
"Appadu",
"Calan",
""
],
[
"Hollowood",
"Timothy J.",
""
]
] | We calculate the one loop beta function for the would-be marginal coupling on the world sheet of the k deformed sigma models associated to a quantum group with q=exp(i pi/k). This includes the bosonic principal chiral models and symmetric space sigma models but also the k deformed semi-symmetric space sigma model descr... | 7.740445 | 7.10056 | 9.819194 | 7.228809 | 7.947019 | 7.879302 | 8.076133 | 7.196796 | 7.442721 | 10.031122 | 7.238761 | 7.667532 | 8.106892 | 7.419054 | 7.544818 | 7.467999 | 7.647576 | 7.540133 | 7.686442 | 7.889428 | 7.144275 |
2203.00021 | Nicola Pedron | Michele Cicoli, Francisco G. Pedro, Nicola Pedron | Secondary GWs and PBHs in string inflation: formation and detectability | 16 pages, 5 figures | null | 10.1088/1475-7516/2022/08/030 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive the spectrum and analyse the detectability prospects of secondary
gravity waves (GWs) associated to primordial black hole (PBH) production in a
class of string inflationary models called Fibre Inflation. The inflationary
potential features a near inflection point that induces a period of ultra
slow-roll res... | [
{
"created": "Mon, 28 Feb 2022 19:00:04 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Jul 2022 15:16:30 GMT",
"version": "v2"
}
] | 2022-08-24 | [
[
"Cicoli",
"Michele",
""
],
[
"Pedro",
"Francisco G.",
""
],
[
"Pedron",
"Nicola",
""
]
] | We derive the spectrum and analyse the detectability prospects of secondary gravity waves (GWs) associated to primordial black hole (PBH) production in a class of string inflationary models called Fibre Inflation. The inflationary potential features a near inflection point that induces a period of ultra slow-roll respo... | 8.130152 | 8.665118 | 7.749364 | 7.304529 | 7.829247 | 8.175358 | 7.999218 | 8.048491 | 7.596731 | 8.466516 | 8.320375 | 7.847932 | 7.414251 | 7.493794 | 7.836646 | 7.773057 | 7.706058 | 7.760184 | 7.629045 | 7.76277 | 7.702477 |
0711.2173 | Ludwik Turko | Ludwik Turko | Statistical ensemble equivalence problem | 5 pages, Talk given at the conference ''New Trends in High Energy
Physics'', Crimea 2007, Yalta, 15-22 September 2007 | null | null | null | hep-th cond-mat.stat-mech | null | A problem of the equivalence of statistical ensembles is critically analyzed.
It is shown, that although different probability distributions of statistical
physics have the same behavior in the thermodynamic limit, there are physical
observables -- semi-intensive variables -- which keep memory of the underlying
ensem... | [
{
"created": "Wed, 14 Nov 2007 11:55:27 GMT",
"version": "v1"
}
] | 2007-11-17 | [
[
"Turko",
"Ludwik",
""
]
] | A problem of the equivalence of statistical ensembles is critically analyzed. It is shown, that although different probability distributions of statistical physics have the same behavior in the thermodynamic limit, there are physical observables -- semi-intensive variables -- which keep memory of the underlying ensembl... | 12.684898 | 14.255301 | 11.40249 | 10.996872 | 11.226596 | 12.873462 | 13.516184 | 11.453143 | 11.677042 | 11.735276 | 10.36058 | 11.504622 | 10.894863 | 11.42451 | 11.324706 | 11.739534 | 11.394041 | 11.386386 | 11.273965 | 11.228044 | 10.738046 |
1104.3135 | Tristan Hubsch | Tristan Hubsch | Weaving Worldsheet Supermultiplets from the Worldlines Within | Extended version, with added discussion of complex and quaternionic
tensor products demonstrating that certain quotient supermultiplets do not
factorize over any ground field | Adv. in Th. Math. Phys. 17 (2013)1-72 | 10.4310/ATMP.2013.v17.n5.a2 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the fact that every worldsheet is ruled by two (light-cone) copies of
worldlines, the recent classification of off-shell supermultiplets of
N-extended worldline supersymmetry is extended to construct standard off-shell
and also unidextrous (on the half-shell) supermultiplets of worldsheet
(p,q)-supersymmetry wi... | [
{
"created": "Fri, 15 Apr 2011 19:27:55 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Jan 2014 03:23:19 GMT",
"version": "v2"
}
] | 2016-03-08 | [
[
"Hubsch",
"Tristan",
""
]
] | Using the fact that every worldsheet is ruled by two (light-cone) copies of worldlines, the recent classification of off-shell supermultiplets of N-extended worldline supersymmetry is extended to construct standard off-shell and also unidextrous (on the half-shell) supermultiplets of worldsheet (p,q)-supersymmetry with... | 19.626213 | 21.798813 | 23.3585 | 18.615782 | 19.793941 | 23.68749 | 20.319618 | 19.986635 | 18.738207 | 24.34795 | 19.423134 | 17.921995 | 20.636728 | 18.171803 | 18.257759 | 18.360044 | 18.688248 | 18.004108 | 19.061066 | 20.853119 | 18.448223 |
hep-th/0105248 | Gaston Giribet | Gaston Giribet | Prelogarithmic operators and Jordan blocks in SL(2)_k affine algebra | 16 pages. Corrected some typos, references and comments added | Mod.Phys.Lett. A16 (2001) 821-834 | 10.1142/S0217732301004029 | null | hep-th | null | The free field description of logarithmic and prelogarithmic operators in non
compact Wess-Zumino-Witten model is analysed. We study the structure of the
Jordan blocks of the SL(2)_k affine algebra and the role of the puncture
operator in the theory in relation with the unitarity bound.
| [
{
"created": "Thu, 24 May 2001 13:46:02 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Jun 2001 17:01:19 GMT",
"version": "v2"
},
{
"created": "Sun, 31 Mar 2002 20:34:03 GMT",
"version": "v3"
}
] | 2009-11-07 | [
[
"Giribet",
"Gaston",
""
]
] | The free field description of logarithmic and prelogarithmic operators in non compact Wess-Zumino-Witten model is analysed. We study the structure of the Jordan blocks of the SL(2)_k affine algebra and the role of the puncture operator in the theory in relation with the unitarity bound. | 14.862122 | 12.929068 | 15.980412 | 11.427801 | 12.749493 | 14.00576 | 13.049617 | 13.812203 | 12.613605 | 20.491512 | 12.350251 | 13.768733 | 16.061975 | 13.339613 | 13.18265 | 13.252009 | 13.323879 | 13.121463 | 13.463573 | 15.952574 | 13.327689 |
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