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|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/0008084 | Mariano Cadoni | Mariano Cadoni and Marco Cavaglia' | Open strings, 2D gravity and AdS/CFT correspondence | 22 pages, Typeset using REVTEX | Phys.Rev. D63 (2001) 084024 | 10.1103/PhysRevD.63.084024 | INFNCA-TH0013 | hep-th | null | We present a detailed discussion of the duality between dilaton gravity on
AdS_2 and open strings. The correspondence between the two theories is
established using their symmetries and field theoretical, thermodynamic, and
statistical arguments. We use the dual conformal field theory to describe
two-dimensional black... | [
{
"created": "Thu, 10 Aug 2000 11:22:24 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Cadoni",
"Mariano",
""
],
[
"Cavaglia'",
"Marco",
""
]
] | We present a detailed discussion of the duality between dilaton gravity on AdS_2 and open strings. The correspondence between the two theories is established using their symmetries and field theoretical, thermodynamic, and statistical arguments. We use the dual conformal field theory to describe two-dimensional black h... | 8.989013 | 8.368069 | 8.807265 | 7.933672 | 8.256502 | 7.776329 | 7.723776 | 8.35816 | 7.940367 | 8.590944 | 8.68314 | 8.479884 | 8.438302 | 8.342787 | 8.2091 | 8.225007 | 8.237675 | 8.236159 | 8.080951 | 8.298872 | 8.184265 |
1905.03795 | Takahiro Uetoko | Takahiro Nishinaka and Takahiro Uetoko | Argyres-Douglas theories and Liouville Irregular States | 37 pages, no figures, v2: minor changes | null | 10.1007/JHEP09(2019)104 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study irregular states of rank-two and three in Liouville theory, based on
an ansatz proposed by D. Gaiotto and J. Teschner. Using these irregular states,
we evaluate asymptotic expansions of irregular conformal blocks corresponding
to the partition functions of $(A_1,A_3)$ and $(A_1,D_4)$ Argyres-Douglas
theories... | [
{
"created": "Thu, 9 May 2019 18:00:10 GMT",
"version": "v1"
},
{
"created": "Thu, 23 May 2019 04:52:10 GMT",
"version": "v2"
}
] | 2019-10-02 | [
[
"Nishinaka",
"Takahiro",
""
],
[
"Uetoko",
"Takahiro",
""
]
] | We study irregular states of rank-two and three in Liouville theory, based on an ansatz proposed by D. Gaiotto and J. Teschner. Using these irregular states, we evaluate asymptotic expansions of irregular conformal blocks corresponding to the partition functions of $(A_1,A_3)$ and $(A_1,D_4)$ Argyres-Douglas theories f... | 9.525111 | 8.750597 | 10.328321 | 9.10604 | 8.427413 | 9.05906 | 8.686152 | 7.978075 | 8.049954 | 12.435708 | 8.510208 | 8.567395 | 9.216832 | 8.527886 | 9.048638 | 8.675756 | 8.831576 | 8.411482 | 8.523311 | 9.378539 | 8.632818 |
2404.08346 | Reinoud Slagter | Reinoud Jan Slagter | New instanton on a warped Kerr spacetime | 6 pages. 11 figures. Submitted to journal-- review V5: remark added
below Eq.4 | null | null | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We find an exact time-dependent instanton solution on a vacuum Kerr-like
warped spacetime in conformal dilaton gravity. Remarkably, the metric solution
results from a first-order PDE, allowing the connection with self-duality. The
antipodal boundary condition on the hypersurface of a Klein bottle $\sim
\mathbb{C}^1\t... | [
{
"created": "Fri, 12 Apr 2024 09:21:52 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Apr 2024 08:36:27 GMT",
"version": "v2"
},
{
"created": "Thu, 25 Jul 2024 17:56:29 GMT",
"version": "v3"
},
{
"created": "Sat, 27 Jul 2024 19:47:18 GMT",
"version": "v4"
},
{
"c... | 2024-08-13 | [
[
"Slagter",
"Reinoud Jan",
""
]
] | We find an exact time-dependent instanton solution on a vacuum Kerr-like warped spacetime in conformal dilaton gravity. Remarkably, the metric solution results from a first-order PDE, allowing the connection with self-duality. The antipodal boundary condition on the hypersurface of a Klein bottle $\sim \mathbb{C}^1\tim... | 14.470772 | 15.917006 | 14.128093 | 14.510693 | 15.429896 | 14.985203 | 15.268384 | 14.02984 | 15.315105 | 15.914255 | 14.436359 | 14.333307 | 13.938891 | 14.09824 | 14.383547 | 14.512263 | 14.207235 | 13.802501 | 14.363593 | 14.405405 | 14.181982 |
hep-th/9802040 | Nami Fux Svaiter | F. S. Nogueira (Ecole Polytechnique), M. B. Silva Neto and N. F.
Svaiter (C.B.P.F.) | Non trivial critical exponents for finite temperature chiral transitions
at fixed total fermion number | 14 pages Latex, no figures, final version to be published in Phys.
Lett. B | Phys.Lett. B441 (1998) 339 | 10.1016/S0370-2693(98)01189-7 | CBPF-NF-006/98 | hep-th cond-mat.stat-mech hep-ph | null | We analyze the finite temperature chiral restoration transition of the
$(D=d+1)$-dimensional Gross-Neveu model for the case of a large number of
flavors and fixed total fermion number. This leads to the study of the model
with a nonzero imaginary chemical potential. In this formulation of the theory,
we have obtained... | [
{
"created": "Fri, 6 Feb 1998 20:21:59 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Feb 1998 22:48:10 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Jun 1998 20:22:06 GMT",
"version": "v3"
},
{
"created": "Tue, 15 Sep 1998 16:24:47 GMT",
"version": "v4"
}
] | 2009-10-31 | [
[
"Nogueira",
"F. S.",
"",
"Ecole Polytechnique"
],
[
"Neto",
"M. B. Silva",
"",
"C.B.P.F."
],
[
"Svaiter",
"N. F.",
"",
"C.B.P.F."
]
] | We analyze the finite temperature chiral restoration transition of the $(D=d+1)$-dimensional Gross-Neveu model for the case of a large number of flavors and fixed total fermion number. This leads to the study of the model with a nonzero imaginary chemical potential. In this formulation of the theory, we have obtained t... | 11.018301 | 11.161481 | 10.65279 | 10.015605 | 11.415304 | 10.872659 | 11.039228 | 11.089638 | 10.212099 | 11.456512 | 10.496902 | 10.581074 | 10.594011 | 10.208786 | 10.292034 | 10.385006 | 10.218263 | 10.280326 | 10.095776 | 10.786478 | 10.185482 |
2305.01283 | Jiaqi Chen | Jiaqi Chen, Bo Feng, Li Lin Yang | Intersection theory rules symbology | 12 pages, 1 figure, recieved version | Sci. China-Phys. Mech. Astron. 67, 221011 (2024) | 10.1007/s11433-023-2239-8 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a novel method to determine the structure of symbols for any
family of polylogarithmic Feynman integrals. Using the d log-bases and simple
formulas for the leading order and next-to-leading contributions to the
intersection numbers, we give a streamlined procedure to compute the entries in
the coefficient ... | [
{
"created": "Tue, 2 May 2023 09:35:57 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Jul 2023 07:29:48 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Sep 2023 11:05:12 GMT",
"version": "v3"
}
] | 2024-01-12 | [
[
"Chen",
"Jiaqi",
""
],
[
"Feng",
"Bo",
""
],
[
"Yang",
"Li Lin",
""
]
] | We propose a novel method to determine the structure of symbols for any family of polylogarithmic Feynman integrals. Using the d log-bases and simple formulas for the leading order and next-to-leading contributions to the intersection numbers, we give a streamlined procedure to compute the entries in the coefficient ma... | 13.690179 | 13.409467 | 13.841895 | 12.433961 | 13.018923 | 14.408105 | 13.997605 | 13.773191 | 11.876871 | 14.957294 | 12.448725 | 13.283477 | 12.943743 | 12.642945 | 13.513381 | 13.589003 | 13.440212 | 13.297035 | 12.923874 | 13.389751 | 12.599589 |
hep-th/9210017 | Young Park | Youngchul Park and Andrew Strominger | Supersymmetry and Positive Energy in Classical and Quantum
Two-Dimensional Dilaton Gravity | 21 pages | Phys.Rev.D47:1569-1575,1993 | 10.1103/PhysRevD.47.1569 | UCSBTH-92-39 | hep-th | null | An $N = 1$ supersymmetric version of two dimensional dilaton gravity coupled
to matter is considered. It is shown that the linear dilaton vacuum
spontaneously breaks half the supersymmetries, leaving broken a linear
combination of left and right supersymmetries which squares to time
translations. Supersymmetry sugges... | [
{
"created": "Fri, 2 Oct 1992 23:14:33 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Park",
"Youngchul",
""
],
[
"Strominger",
"Andrew",
""
]
] | An $N = 1$ supersymmetric version of two dimensional dilaton gravity coupled to matter is considered. It is shown that the linear dilaton vacuum spontaneously breaks half the supersymmetries, leaving broken a linear combination of left and right supersymmetries which squares to time translations. Supersymmetry suggests... | 7.540942 | 7.703145 | 7.71876 | 6.937096 | 7.614269 | 7.301025 | 7.483933 | 7.058378 | 7.495939 | 8.116846 | 7.307045 | 7.053808 | 7.293034 | 7.126102 | 7.253807 | 7.272125 | 7.133707 | 7.069865 | 7.109633 | 7.385409 | 7.254045 |
hep-th/0007165 | Jamila Douari | J.Douari and Y.Hassouni | Fractional Supersymmetry through Generalized Anyonic algebra | 8 pages | Acta Phys.Slov.51:175-182,2001 | null | null | hep-th | null | The construction of anyonic operators and algebra is generalized by using
quons operators. Therefore, the particular versionof fractional supersymmetry
is constructed on the two-dimensional lattice by associating two generalized
anyons of different kinds. The fractional supersymmetry Hamiltonian operator is
obtained ... | [
{
"created": "Thu, 20 Jul 2000 16:46:29 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Aug 2000 13:05:59 GMT",
"version": "v2"
}
] | 2011-07-19 | [
[
"Douari",
"J.",
""
],
[
"Hassouni",
"Y.",
""
]
] | The construction of anyonic operators and algebra is generalized by using quons operators. Therefore, the particular versionof fractional supersymmetry is constructed on the two-dimensional lattice by associating two generalized anyons of different kinds. The fractional supersymmetry Hamiltonian operator is obtained on... | 18.663681 | 14.720498 | 18.791632 | 14.887703 | 14.670375 | 14.727933 | 14.349409 | 15.935771 | 14.556945 | 19.909401 | 14.578403 | 15.334554 | 17.547693 | 15.719641 | 14.748569 | 14.710461 | 15.125611 | 14.617887 | 15.52761 | 16.287193 | 15.604857 |
hep-th/9605171 | Jorge Gamboa | J. Gamboa, V. O. Rivelles and J. Zanelli | Global Anomalies and Anyons in 1+1 Dimensions | Changed title. To be published in Physics Letters B | Phys.Lett. B395 (1997) 264-268 | 10.1016/S0370-2693(97)00042-7 | null | hep-th cond-mat | null | We consider the analog in one spatial dimension of the Bose-Fermi
transmutation for planar systems. A quantum mechanical system of a spin 1/2
particle coupled to an abelian gauge field, which is classically invariant
under gauge transformations and charge conjugation is studied. It is found that
unless the flux enclo... | [
{
"created": "Wed, 22 May 1996 22:18:46 GMT",
"version": "v1"
},
{
"created": "Tue, 10 Dec 1996 20:46:33 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Gamboa",
"J.",
""
],
[
"Rivelles",
"V. O.",
""
],
[
"Zanelli",
"J.",
""
]
] | We consider the analog in one spatial dimension of the Bose-Fermi transmutation for planar systems. A quantum mechanical system of a spin 1/2 particle coupled to an abelian gauge field, which is classically invariant under gauge transformations and charge conjugation is studied. It is found that unless the flux enclose... | 9.93607 | 10.146798 | 10.061414 | 9.261278 | 8.561647 | 9.893502 | 10.868309 | 9.262628 | 9.423459 | 12.032905 | 8.929423 | 9.446516 | 9.815207 | 9.550697 | 8.992929 | 9.517968 | 9.458455 | 9.779638 | 9.259476 | 10.932407 | 8.945532 |
1912.10991 | Andrew Turner | Nikhil Raghuram, Washington Taylor, and Andrew P. Turner | General F-theory models with tuned $(\operatorname{SU}(3) \times
\operatorname{SU}(2) \times \operatorname{U}(1)) / \mathbb{Z}_6$ symmetry | 36 pages, LaTeX | null | 10.1007/JHEP04(2020)008 | MIT-CTP-5169 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct a general form for an F-theory Weierstrass model over a general
base giving a 6D or 4D supergravity theory with gauge group
$(\operatorname{SU}(3) \times \operatorname{SU}(2) \times \operatorname{U}(1))
/ \mathbb{Z}_6$ and generic associated matter, which includes the matter
content of the standard model... | [
{
"created": "Mon, 23 Dec 2019 17:37:38 GMT",
"version": "v1"
},
{
"created": "Fri, 15 May 2020 20:55:15 GMT",
"version": "v2"
}
] | 2021-01-06 | [
[
"Raghuram",
"Nikhil",
""
],
[
"Taylor",
"Washington",
""
],
[
"Turner",
"Andrew P.",
""
]
] | We construct a general form for an F-theory Weierstrass model over a general base giving a 6D or 4D supergravity theory with gauge group $(\operatorname{SU}(3) \times \operatorname{SU}(2) \times \operatorname{U}(1)) / \mathbb{Z}_6$ and generic associated matter, which includes the matter content of the standard model. ... | 7.677003 | 7.412415 | 8.92895 | 7.12493 | 7.757226 | 7.788656 | 7.674018 | 6.915276 | 7.789692 | 8.953538 | 7.160511 | 7.29631 | 7.477129 | 7.404722 | 7.28897 | 7.55955 | 7.356782 | 7.165887 | 7.419281 | 7.723317 | 7.216938 |
1408.2796 | Alberto Molgado | Jasel Berra-Montiel, Alberto Molgado, C\'esar D. Palacios-Garc\'ia | Causal Poisson bracket via deformation quantization | 25 pages, no figures, published version | IJGMMP 13 (2016) 1650104 | 10.1142/S0219887816501048 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Starting with the well-defined product of quantum fields at two spacetime
points, we explore an associated Poisson structure for classical field theories
within the deformation quantization formalism. We realize that the induced
star-product is naturally related to the standard Moyal product through an
appropriate ca... | [
{
"created": "Tue, 12 Aug 2014 18:40:33 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Aug 2014 14:56:42 GMT",
"version": "v2"
},
{
"created": "Tue, 12 Jul 2016 18:33:01 GMT",
"version": "v3"
}
] | 2016-07-13 | [
[
"Berra-Montiel",
"Jasel",
""
],
[
"Molgado",
"Alberto",
""
],
[
"Palacios-García",
"César D.",
""
]
] | Starting with the well-defined product of quantum fields at two spacetime points, we explore an associated Poisson structure for classical field theories within the deformation quantization formalism. We realize that the induced star-product is naturally related to the standard Moyal product through an appropriate caus... | 12.677863 | 13.07136 | 12.88804 | 12.175531 | 12.441229 | 11.937803 | 12.559257 | 12.250673 | 12.248717 | 13.050559 | 12.368129 | 11.996596 | 12.366406 | 11.92645 | 12.327687 | 11.878404 | 12.015466 | 11.950128 | 12.111722 | 12.48863 | 12.15472 |
0804.2907 | Davide Gaiotto | Davide Gaiotto and Edward Witten | Janus Configurations, Chern-Simons Couplings, And The Theta-Angle in N=4
Super Yang-Mills Theory | 66 pp | JHEP 1006:097,2010 | 10.1007/JHEP06(2010)097 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize the half-BPS Janus configuration of four-dimensional N=4 super
Yang-Mills theory to allow the theta-angle, as well as the gauge coupling, to
vary with position. We show that the existence of this generalization is
closely related to the existence of novel three-dimensional Chern-Simons
theories with N=4... | [
{
"created": "Thu, 17 Apr 2008 21:21:53 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Gaiotto",
"Davide",
""
],
[
"Witten",
"Edward",
""
]
] | We generalize the half-BPS Janus configuration of four-dimensional N=4 super Yang-Mills theory to allow the theta-angle, as well as the gauge coupling, to vary with position. We show that the existence of this generalization is closely related to the existence of novel three-dimensional Chern-Simons theories with N=4 s... | 6.91285 | 6.403469 | 7.631532 | 6.156423 | 5.831779 | 6.47227 | 6.662459 | 6.60802 | 6.530789 | 8.189371 | 6.256047 | 6.444805 | 6.683983 | 6.654703 | 6.356216 | 6.737046 | 6.619524 | 6.570877 | 6.562667 | 6.649082 | 6.475445 |
0911.1814 | Keisuke Izumi | Keisuke Izumi and Shinji Mukohyama | Stellar center is dynamical in Horava-Lifshitz gravity | 9 pages; minor corrections, order of sections changed, reference
added (v2) | Phys.Rev.D81:044008,2010 | 10.1103/PhysRevD.81.044008 | IPMU09-0136 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In Horava-Lifshitz gravity, regularity of a solution requires smoothness of
not only the spacetime geometry but also the foliation. As a result, the
regularity condition at the center of a star is more restrictive than in
general relativity. Assuming that the energy density is a piecewise-continuous,
non-negative fun... | [
{
"created": "Tue, 10 Nov 2009 01:35:58 GMT",
"version": "v1"
},
{
"created": "Wed, 20 Jan 2010 07:41:03 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Izumi",
"Keisuke",
""
],
[
"Mukohyama",
"Shinji",
""
]
] | In Horava-Lifshitz gravity, regularity of a solution requires smoothness of not only the spacetime geometry but also the foliation. As a result, the regularity condition at the center of a star is more restrictive than in general relativity. Assuming that the energy density is a piecewise-continuous, non-negative funct... | 8.055501 | 7.276133 | 7.634514 | 7.334481 | 7.667625 | 7.701681 | 7.508777 | 7.579203 | 7.33411 | 8.118241 | 7.317027 | 7.374805 | 7.257824 | 7.112867 | 7.209343 | 7.120576 | 7.075731 | 7.204865 | 7.139453 | 6.965461 | 7.165406 |
2305.01647 | Marcia Tenser | Luigi Castiglioni, Silvia Penati, Marcia Tenser, Diego Trancanelli | Wilson loops and defect RG flows in ABJM | 40 pages, 17 figures; minor changes and references added | JHEP 2306 (2023) 157 | 10.1007/JHEP06(2023)157 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We continue our study of renormalization group (RG) flows on Wilson loop
defects in ABJM theory, which we have initiated in arXiv:2211.16501. We
generalize that analysis by including non-supersymmetric fixed points and RG
trajectories. To this end, we first determine the ``ordinary",
non-supersymmetric Wilson loops, ... | [
{
"created": "Tue, 2 May 2023 17:59:08 GMT",
"version": "v1"
},
{
"created": "Fri, 5 May 2023 11:55:01 GMT",
"version": "v2"
}
] | 2023-06-28 | [
[
"Castiglioni",
"Luigi",
""
],
[
"Penati",
"Silvia",
""
],
[
"Tenser",
"Marcia",
""
],
[
"Trancanelli",
"Diego",
""
]
] | We continue our study of renormalization group (RG) flows on Wilson loop defects in ABJM theory, which we have initiated in arXiv:2211.16501. We generalize that analysis by including non-supersymmetric fixed points and RG trajectories. To this end, we first determine the ``ordinary", non-supersymmetric Wilson loops, wh... | 10.497146 | 9.881042 | 11.14526 | 9.705912 | 10.234748 | 9.693151 | 9.753361 | 9.750769 | 9.338143 | 12.372845 | 9.578826 | 9.755921 | 9.935955 | 9.666299 | 9.89242 | 9.622719 | 9.773513 | 9.707888 | 9.933231 | 10.212081 | 9.462197 |
2001.00934 | Dine Ousmane Samary | Vincent Lahoche and Dine Ousmane Samary | Pedagogical comments about nonperturbative Ward-constrained melonic
renormalization group flow | 16 pages, 9 figures. arXiv admin note: substantial text overlap with
arXiv:1904.05655 | Physical Review D 101, 024001 (2020) | 10.1103/PhysRevD.101.024001 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper, in addition to our recent works, intends to explore the behavior
of the Wetterich flow equations in the portion of the theory space spanned by
non-branching melons constrained with Ward-identities. We focus on a rank-5
just-renormalizable tensorial group field theory and consider a non-trivial
extension o... | [
{
"created": "Thu, 2 Jan 2020 20:08:10 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jul 2021 19:22:29 GMT",
"version": "v2"
},
{
"created": "Fri, 11 Feb 2022 12:27:18 GMT",
"version": "v3"
}
] | 2022-02-14 | [
[
"Lahoche",
"Vincent",
""
],
[
"Samary",
"Dine Ousmane",
""
]
] | This paper, in addition to our recent works, intends to explore the behavior of the Wetterich flow equations in the portion of the theory space spanned by non-branching melons constrained with Ward-identities. We focus on a rank-5 just-renormalizable tensorial group field theory and consider a non-trivial extension of ... | 21.153078 | 21.761108 | 21.254068 | 19.579639 | 20.346739 | 21.841692 | 21.414164 | 20.64418 | 19.396395 | 22.557146 | 20.045023 | 21.931622 | 22.260662 | 21.111799 | 21.766052 | 21.764938 | 21.902401 | 21.231709 | 21.186562 | 21.669558 | 20.408251 |
0912.0055 | Pei-Ming Ho | Pei-Ming Ho | Nambu Bracket for M Theory | 13 pages, prepared for The Fourth International Symposium on
Symmetries in Subatomic Physics (SSP 2009), minor modification, references
added | Nucl.Phys.A844:95c-108c,2010 | 10.1016/j.nuclphysa.2010.05.020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we give a concise review of recent progress in our
understanding of the Lie 3-algebra and their application to the
Bagger-Lambert-Gustavsson model describing multiple M2-branes in M theory.
| [
{
"created": "Tue, 1 Dec 2009 02:15:08 GMT",
"version": "v1"
},
{
"created": "Tue, 19 Jan 2010 07:50:24 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Ho",
"Pei-Ming",
""
]
] | In this article we give a concise review of recent progress in our understanding of the Lie 3-algebra and their application to the Bagger-Lambert-Gustavsson model describing multiple M2-branes in M theory. | 6.946715 | 4.296529 | 8.405552 | 4.810915 | 4.749381 | 4.77879 | 4.52782 | 4.665008 | 4.660527 | 6.644197 | 4.708818 | 4.748672 | 5.77598 | 4.888789 | 4.591837 | 4.713063 | 4.652246 | 5.157158 | 4.731882 | 5.623978 | 4.962893 |
0806.3057 | Oleg Evnin | Oleg Evnin and Timothy Nguyen | On discrete features of the wave equation in singular pp-wave
backgrounds | 10 pages; v2: references and clarifications added, minor typos
corrected | JHEP 0809:105,2008 | 10.1088/1126-6708/2008/09/105 | null | hep-th gr-qc | http://creativecommons.org/licenses/by-nc-sa/3.0/ | We analyze the wave equation in families of pp-wave geometries developing
strong localized scale-invariant singularities in certain limits. For both
cases of well-localized pp-waves and the so-called null-cosmologies, we observe
an intriguing discrete dependence of the existence of a singular limit on the
normalizati... | [
{
"created": "Wed, 18 Jun 2008 17:56:44 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Jul 2008 19:36:21 GMT",
"version": "v2"
}
] | 2011-06-02 | [
[
"Evnin",
"Oleg",
""
],
[
"Nguyen",
"Timothy",
""
]
] | We analyze the wave equation in families of pp-wave geometries developing strong localized scale-invariant singularities in certain limits. For both cases of well-localized pp-waves and the so-called null-cosmologies, we observe an intriguing discrete dependence of the existence of a singular limit on the normalization... | 20.853624 | 19.684381 | 18.121265 | 17.33873 | 18.609051 | 17.360861 | 21.218191 | 16.744373 | 17.746572 | 21.385307 | 19.935141 | 18.216608 | 19.189919 | 18.780134 | 17.591837 | 18.404709 | 19.031292 | 18.17618 | 18.997437 | 19.063511 | 17.820065 |
1805.10743 | Kohta Hatakeyama | Kohta Hatakeyama, Asato Tsuchiya | Equivalence of large-$N$ gauge theories on a group manifold and its
coset space | 11 pages, 4 figures, published version | Phys. Lett. B 782 (2018) 503 | 10.1016/j.physletb.2018.05.065 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It was shown in arXiv:0912.1456 that the large-$N$ reduction holds on group
manifolds in the sense that a large-$N$ gauge theory on a group manifold is
realized by a matrix model which is obtained by dimensionally reducing the
original theory to zero dimension. In this note, generalizing the above
statement, we show ... | [
{
"created": "Mon, 28 May 2018 02:42:19 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Jul 2018 02:13:48 GMT",
"version": "v2"
}
] | 2018-07-03 | [
[
"Hatakeyama",
"Kohta",
""
],
[
"Tsuchiya",
"Asato",
""
]
] | It was shown in arXiv:0912.1456 that the large-$N$ reduction holds on group manifolds in the sense that a large-$N$ gauge theory on a group manifold is realized by a matrix model which is obtained by dimensionally reducing the original theory to zero dimension. In this note, generalizing the above statement, we show th... | 6.079514 | 5.316112 | 5.979066 | 5.174174 | 5.650452 | 5.549243 | 5.366167 | 5.06111 | 5.23033 | 6.359818 | 5.398691 | 5.45562 | 5.922935 | 5.652017 | 5.662005 | 5.490705 | 5.524943 | 5.489703 | 5.601568 | 5.862706 | 5.63051 |
hep-th/9311073 | null | D.C.Cabra and C.M.Na\'on | 2D Ising Model with a Defect Line | 8 pages, report La Plata 93-08 | Mod. Phys. Lett. A9 (1994) 2107-2112 | 10.1142/S0217732394001969 | null | hep-th | null | We study the two-dimensional Ising model with a defect line and evaluate
multipoint energy correlation functions using non-perturbative
field-theoretical methods. We also discuss the evaluation of the two spin
correlator on the defect line.
| [
{
"created": "Thu, 11 Nov 1993 19:08:33 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Cabra",
"D. C.",
""
],
[
"Naón",
"C. M.",
""
]
] | We study the two-dimensional Ising model with a defect line and evaluate multipoint energy correlation functions using non-perturbative field-theoretical methods. We also discuss the evaluation of the two spin correlator on the defect line. | 10.988422 | 11.493518 | 9.826156 | 10.27415 | 9.847171 | 10.903461 | 11.623975 | 10.711004 | 10.368946 | 11.410293 | 9.939528 | 10.444393 | 10.393395 | 10.236636 | 10.142969 | 10.050064 | 10.255578 | 10.661592 | 10.819641 | 10.461891 | 9.595229 |
2005.05273 | Dominik Miketa | Antoine Bourget, Amihay Hanany, Dominik Miketa | Quiver origami: discrete gauging and folding | 63 pages, 23 figures | Journal of High Energy Physics 2021 | 10.1007/JHEP01(2021)086 | 86 (2021) | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study two types of discrete operations on Coulomb branches of $3d$
$\mathcal{N}=4$ quiver gauge theories using both abelianisation and the
monopole formula. We generalise previous work on discrete quotients of Coulomb
branches and introduce novel wreathed quiver theories. We further study quiver
folding which prod... | [
{
"created": "Mon, 11 May 2020 17:17:53 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Aug 2020 12:26:11 GMT",
"version": "v2"
}
] | 2021-01-19 | [
[
"Bourget",
"Antoine",
""
],
[
"Hanany",
"Amihay",
""
],
[
"Miketa",
"Dominik",
""
]
] | We study two types of discrete operations on Coulomb branches of $3d$ $\mathcal{N}=4$ quiver gauge theories using both abelianisation and the monopole formula. We generalise previous work on discrete quotients of Coulomb branches and introduce novel wreathed quiver theories. We further study quiver folding which produc... | 10.361293 | 8.051022 | 11.023827 | 7.897965 | 8.218007 | 8.768146 | 8.955187 | 7.943449 | 7.917535 | 13.1981 | 7.797772 | 8.387545 | 10.370613 | 8.481095 | 8.345405 | 8.619217 | 8.381799 | 8.464228 | 8.490967 | 10.333137 | 8.584894 |
2110.01115 | Yi-Zhuang You | Jonathan Lam, Yi-Zhuang You | Machine Learning Statistical Gravity from Multi-Region Entanglement
Entropy | 10 pages, 10 figures | Phys. Rev. Research 3, 043199 (2021) | 10.1103/PhysRevResearch.3.043199 | null | hep-th cond-mat.dis-nn cond-mat.stat-mech quant-ph | http://creativecommons.org/licenses/by/4.0/ | The Ryu-Takayanagi formula directly connects quantum entanglement and
geometry. Yet the assumption of static geometry lead to an exponentially small
mutual information between far-separated disjoint regions, which does not hold
in many systems such as free fermion conformal field theories. In this work, we
proposed a... | [
{
"created": "Sun, 3 Oct 2021 22:46:41 GMT",
"version": "v1"
}
] | 2023-05-17 | [
[
"Lam",
"Jonathan",
""
],
[
"You",
"Yi-Zhuang",
""
]
] | The Ryu-Takayanagi formula directly connects quantum entanglement and geometry. Yet the assumption of static geometry lead to an exponentially small mutual information between far-separated disjoint regions, which does not hold in many systems such as free fermion conformal field theories. In this work, we proposed a m... | 11.993277 | 12.756045 | 13.435752 | 12.871632 | 13.798434 | 13.417266 | 13.150728 | 13.489107 | 12.089669 | 14.303744 | 12.731853 | 12.066094 | 12.153915 | 11.862602 | 12.055173 | 11.158248 | 11.975592 | 11.701891 | 11.670321 | 12.012066 | 11.922279 |
hep-th/9411106 | Chakrabarti Amitabha | B. Abdesselam, D. Arnaudon, A. Chakrabarti | Representations of $SO(5)_{q}$ and Non-Minimal $q$-Deformation | 11 pages, Tex.file | J.Phys. A28 (1995) 3701-3708 | 10.1088/0305-4470/28/13/014 | Ecole polytechnique preprint A337.1194 | hep-th math.QA q-alg | null | Representations of $SO(5)_{q}$ can be constructed on bases such that either
the Chevalley triplet $(e_{1},\;f_{1},\;h_{1})$ or $(e_{2},\;f_{2},\;h_{2})$
has the standard $SU(2)_{q}$ matrix elements. The other triplet in each cases
has a more complicated action. The $q$-deformation of such representations
present stri... | [
{
"created": "Tue, 15 Nov 1994 17:08:38 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Abdesselam",
"B.",
""
],
[
"Arnaudon",
"D.",
""
],
[
"Chakrabarti",
"A.",
""
]
] | Representations of $SO(5)_{q}$ can be constructed on bases such that either the Chevalley triplet $(e_{1},\;f_{1},\;h_{1})$ or $(e_{2},\;f_{2},\;h_{2})$ has the standard $SU(2)_{q}$ matrix elements. The other triplet in each cases has a more complicated action. The $q$-deformation of such representations present striki... | 11.277939 | 11.198425 | 12.569525 | 10.936401 | 11.453902 | 11.009394 | 10.361793 | 10.332687 | 10.162179 | 12.542685 | 10.582114 | 10.70903 | 11.297318 | 10.734859 | 10.604349 | 10.405248 | 10.457951 | 10.482347 | 10.439805 | 11.307045 | 10.599865 |
hep-th/9408128 | Alex Kovner | A. Kovner and B. Rosenstein | Fermionic Operators from Bosonic Fields in 3+1 Dimensions | 8 pages, two figures available on request, LA-UR-94-2863 | Phys.Lett. B342 (1995) 381-386 | 10.1016/0370-2693(94)01362-G | null | hep-th | null | We present a construction of fermionic operators in 3+1 dimensions in terms
of bosonic fields in the framework of $QED_4$. The basic bosonic variables are
the electric fields $E_i$ and their conjugate momenta $A_i$. Our construction
generalizes the analogous constuction of fermionic operators in 2+1 dimensions.
Loose... | [
{
"created": "Tue, 23 Aug 1994 21:13:15 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Kovner",
"A.",
""
],
[
"Rosenstein",
"B.",
""
]
] | We present a construction of fermionic operators in 3+1 dimensions in terms of bosonic fields in the framework of $QED_4$. The basic bosonic variables are the electric fields $E_i$ and their conjugate momenta $A_i$. Our construction generalizes the analogous constuction of fermionic operators in 2+1 dimensions. Loosely... | 7.685235 | 7.11691 | 7.757748 | 7.486104 | 7.176527 | 7.304729 | 7.456189 | 7.444159 | 7.210254 | 7.993539 | 7.134059 | 7.062348 | 7.530824 | 7.390184 | 7.724319 | 7.53782 | 7.445717 | 7.349463 | 7.395937 | 7.279938 | 7.197628 |
2202.04702 | Adrien Fiorucci | Laura Donnay, Adrien Fiorucci, Yannick Herfray, Romain Ruzziconi | Carrollian Perspective on Celestial Holography | 9 pages, 1 figure, published version (PRL) | null | 10.1103/PhysRevLett.129.071602 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We show that a $3d$ sourced conformal Carrollian field theory has the right
kinematic properties to holographically describe gravity in $4d$ asymptotically
flat spacetime. The external sources encode the leaks of gravitational
radiation at null infinity. The Ward identities of this theory are shown to
reproduce those... | [
{
"created": "Wed, 9 Feb 2022 19:52:15 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Aug 2022 08:35:08 GMT",
"version": "v2"
}
] | 2022-08-31 | [
[
"Donnay",
"Laura",
""
],
[
"Fiorucci",
"Adrien",
""
],
[
"Herfray",
"Yannick",
""
],
[
"Ruzziconi",
"Romain",
""
]
] | We show that a $3d$ sourced conformal Carrollian field theory has the right kinematic properties to holographically describe gravity in $4d$ asymptotically flat spacetime. The external sources encode the leaks of gravitational radiation at null infinity. The Ward identities of this theory are shown to reproduce those o... | 9.429388 | 7.659636 | 10.20594 | 8.107742 | 8.60584 | 7.267756 | 8.409679 | 7.823781 | 7.681306 | 11.614059 | 7.9218 | 8.269571 | 9.674329 | 8.603182 | 8.308137 | 8.099172 | 8.18302 | 8.301534 | 8.122754 | 9.631314 | 8.105598 |
hep-th/9805128 | Marcony Silva Cunha | H.R. Christiansen, M.S. Cunha, J.A. Helayel-Neto, L.R.U. Manssur,
A.L.M.A. Nogueira | Self-dual vortices in a Maxwell-Chern-Simons model with non-minimal
coupling | 12 pages, 9 figures, 2 tables; some typos corrected, one reference
updated. To be published in the Int. J. Mod. Phys. A (1999) | Int.J.Mod.Phys. A14 (1999) 1721-1736 | 10.1142/S0217751X99000877 | CBPF-NF-034/98 | hep-th | null | We find self-dual vortex solutions in a Maxwell-Chern-Simons model with
anomalous magnetic moment. From a recently developed N=2-supersymmetric
extension, we obtain the proper Bogomol'nyi equations together with a Higgs
potential allowing both topological and non-topological phases in the theory.
| [
{
"created": "Wed, 20 May 1998 18:18:04 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Feb 1999 21:34:35 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Christiansen",
"H. R.",
""
],
[
"Cunha",
"M. S.",
""
],
[
"Helayel-Neto",
"J. A.",
""
],
[
"Manssur",
"L. R. U.",
""
],
[
"Nogueira",
"A. L. M. A.",
""
]
] | We find self-dual vortex solutions in a Maxwell-Chern-Simons model with anomalous magnetic moment. From a recently developed N=2-supersymmetric extension, we obtain the proper Bogomol'nyi equations together with a Higgs potential allowing both topological and non-topological phases in the theory. | 13.190305 | 10.26528 | 13.119774 | 9.808065 | 9.946339 | 9.584659 | 8.470059 | 9.00197 | 9.8867 | 13.257328 | 9.874426 | 10.185688 | 12.14241 | 11.48985 | 10.566425 | 10.791885 | 10.138238 | 10.701442 | 10.892806 | 12.612453 | 10.666303 |
1310.4886 | Matthew Headrick | Cesar A. Agon, Matthew Headrick, Daniel L. Jafferis, and Skyler Kasko | Disk entanglement entropy for a Maxwell field | 34 pages | Phys. Rev. D 89, 025018 (2014) | 10.1103/PhysRevD.89.025018 | BRX-TH-672 | hep-th cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In three dimensions, the pure Maxwell theory with compact U(1) gauge group is
dual to a free compact scalar, and flows from the Maxwell theory with
non-compact gauge group in the ultraviolet to a non-compact free massless
scalar theory in the infrared. We compute the vacuum disk entanglement entropy
all along this fl... | [
{
"created": "Fri, 18 Oct 2013 02:18:38 GMT",
"version": "v1"
}
] | 2014-02-05 | [
[
"Agon",
"Cesar A.",
""
],
[
"Headrick",
"Matthew",
""
],
[
"Jafferis",
"Daniel L.",
""
],
[
"Kasko",
"Skyler",
""
]
] | In three dimensions, the pure Maxwell theory with compact U(1) gauge group is dual to a free compact scalar, and flows from the Maxwell theory with non-compact gauge group in the ultraviolet to a non-compact free massless scalar theory in the infrared. We compute the vacuum disk entanglement entropy all along this flow... | 7.28886 | 6.758217 | 8.221296 | 6.727561 | 7.3128 | 7.018029 | 6.577827 | 6.911146 | 6.485172 | 8.857941 | 6.758231 | 6.663346 | 7.186736 | 6.835713 | 6.718622 | 6.823966 | 6.684516 | 6.911973 | 6.859258 | 7.060277 | 6.752742 |
1112.1054 | Gregory Giecold | Gregory Giecold | Remark on the Baryonic Branch of the Warped Deformed Conifold | 11 pages. v2: references added, updated comment on arXiv:1111.6567 | JHEP(06)(2012)035 | 10.1007/JHEP06(2012)035 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has recently been suggested that a superpotential for the baryonic branch
of the Klebanov-Strassler field theory (KS) should exist for a sector of the
dual supergravity fields. In this note we would like to argue that if extended
to cover the whole set of supergravity fields a would-be superpotential does
not have... | [
{
"created": "Mon, 5 Dec 2011 20:42:34 GMT",
"version": "v1"
},
{
"created": "Sun, 10 Jun 2012 00:35:38 GMT",
"version": "v2"
}
] | 2015-06-03 | [
[
"Giecold",
"Gregory",
""
]
] | It has recently been suggested that a superpotential for the baryonic branch of the Klebanov-Strassler field theory (KS) should exist for a sector of the dual supergravity fields. In this note we would like to argue that if extended to cover the whole set of supergravity fields a would-be superpotential does not have a... | 10.145036 | 10.380498 | 12.060075 | 9.889474 | 9.905174 | 9.907649 | 10.422272 | 10.353789 | 10.091379 | 11.969463 | 10.164636 | 9.334168 | 10.03901 | 9.599607 | 9.557697 | 9.498793 | 9.544319 | 9.288492 | 9.678182 | 10.188707 | 9.667317 |
hep-th/9205101 | Ohta | Nobuyoshi Ohta and Hisao Suzuki | Interactions of Discrete States with Nonzero Ghost Number \\ in $c=1$
$2D$ Gravity | 10 pages, OS-GE 25-92 | Mod.Phys.Lett. A7 (1992) 2723-2730 | 10.1142/S0217732392002184 | null | hep-th | null | We study the interactions of the discrete states with nonzero ghost number in
$c=1$ two-dimensional ($2D$) quantum gravity. By using the vertex operator
representations, it is shown that their interactions are given by the structure
constants of the group of the area preserving diffeomorphism similar to those
of vani... | [
{
"created": "Thu, 28 May 1992 01:01:52 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ohta",
"Nobuyoshi",
""
],
[
"Suzuki",
"Hisao",
""
]
] | We study the interactions of the discrete states with nonzero ghost number in $c=1$ two-dimensional ($2D$) quantum gravity. By using the vertex operator representations, it is shown that their interactions are given by the structure constants of the group of the area preserving diffeomorphism similar to those of vanish... | 13.364094 | 9.316478 | 11.823115 | 10.097985 | 10.238396 | 9.564848 | 9.209038 | 9.656199 | 9.873294 | 12.205447 | 9.68816 | 10.275738 | 12.206847 | 11.193418 | 10.463483 | 10.457231 | 10.1709 | 10.57239 | 11.011706 | 12.056237 | 10.325371 |
0704.0955 | Matthias Wapler | Nemani V. Suryanarayana and Matthias C. Wapler | Charges from Attractors | 25 pages; references and comments added, typos fixed, minor changes
to notation, minor clarifications in the discussions; final version published
in CQG | Class.Quant.Grav.24:5047-5072,2007 | 10.1088/0264-9381/24/20/009 | null | hep-th gr-qc | null | We describe how to recover the quantum numbers of extremal black holes from
their near horizon geometries. This is achieved by constructing the
gravitational Noether-Wald charges which can be used for non-extremal black
holes as well. These charges are shown to be equivalent to the U(1) charges of
appropriately dimen... | [
{
"created": "Sat, 7 Apr 2007 20:03:07 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Oct 2007 07:15:00 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Suryanarayana",
"Nemani V.",
""
],
[
"Wapler",
"Matthias C.",
""
]
] | We describe how to recover the quantum numbers of extremal black holes from their near horizon geometries. This is achieved by constructing the gravitational Noether-Wald charges which can be used for non-extremal black holes as well. These charges are shown to be equivalent to the U(1) charges of appropriately dimensi... | 7.397182 | 7.264653 | 7.567739 | 7.057746 | 7.116961 | 6.840566 | 6.836775 | 6.730071 | 6.751154 | 8.021825 | 6.697928 | 7.160453 | 7.424539 | 7.149003 | 6.903354 | 7.096941 | 6.766596 | 6.998477 | 7.107989 | 7.236265 | 6.885305 |
1909.00434 | Erik Jonathan Lindgren | Jonathan Lindgren | Black hole formation, holographic thermalization and the AdS/CFT
correspondence | 195 pages; PhD Thesis, Vrije Universiteit Brussel/Universit\'e Libre
de Bruxelles, 2017 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The AdS/CFT correspondence is one of the most important discoveries in
theoretical physics in recent years. It states that certain quantum mechanical
theories can actually be described by classical gravity in one higher
dimension, in a spacetime called anti-de Sitter (AdS) space. What makes this
duality so useful is ... | [
{
"created": "Sun, 1 Sep 2019 17:27:57 GMT",
"version": "v1"
}
] | 2019-09-04 | [
[
"Lindgren",
"Jonathan",
""
]
] | The AdS/CFT correspondence is one of the most important discoveries in theoretical physics in recent years. It states that certain quantum mechanical theories can actually be described by classical gravity in one higher dimension, in a spacetime called anti-de Sitter (AdS) space. What makes this duality so useful is th... | 6.094584 | 6.538968 | 6.483581 | 6.270788 | 6.28584 | 6.530659 | 6.152989 | 6.162142 | 6.396319 | 6.598421 | 6.369774 | 6.181474 | 6.271224 | 6.180079 | 6.175841 | 6.231738 | 6.126482 | 6.122341 | 6.104017 | 6.236511 | 6.165685 |
1005.5029 | Anatoly Kotikov Vassilievich | A. V. Kotikov | The property of maximal transcendentality in the N=4 Supersymmetric
Yang-Mills | 21 pages; to be published in "Subtleties in Quantum Field Theories
(Lev Lipatov Festschrift)", D. Diakonov, ed., Gatchina, 2010 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present results for the universal anomalous dimension \gamma_{uni}(j) of
Wilson twist-2 operators in the N=4 Supersymmetric Yang-Mills theory in the
first four orders of perturbation theory.
| [
{
"created": "Thu, 27 May 2010 11:08:46 GMT",
"version": "v1"
}
] | 2010-05-28 | [
[
"Kotikov",
"A. V.",
""
]
] | We present results for the universal anomalous dimension \gamma_{uni}(j) of Wilson twist-2 operators in the N=4 Supersymmetric Yang-Mills theory in the first four orders of perturbation theory. | 10.056318 | 7.304801 | 8.048872 | 6.418725 | 8.560514 | 8.586555 | 9.789641 | 7.429585 | 6.619061 | 7.755179 | 7.9357 | 7.772262 | 7.835559 | 7.894173 | 7.742526 | 8.969926 | 8.528281 | 8.82612 | 7.740942 | 8.186913 | 8.085522 |
hep-th/0110142 | Marika Taylor-Robinson | Marika Taylor-Robinson | Higher dimensional formulation of counterterms | 28 pages, LaTeX | null | null | null | hep-th | null | It is by now well established that divergences of the on-shell action for
asymptotically AdS solutions can be cancelled by adding covariant local
boundary counterterms to the action. Here we show that although one can still
renormalise the action for asymptotically $AdS_p \times S^q$ solutions using
local boundary co... | [
{
"created": "Tue, 16 Oct 2001 15:11:23 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Taylor-Robinson",
"Marika",
""
]
] | It is by now well established that divergences of the on-shell action for asymptotically AdS solutions can be cancelled by adding covariant local boundary counterterms to the action. Here we show that although one can still renormalise the action for asymptotically $AdS_p \times S^q$ solutions using local boundary coun... | 8.960763 | 6.927519 | 9.324493 | 7.484342 | 7.735278 | 7.718878 | 7.713484 | 6.843595 | 8.107833 | 9.044592 | 7.559718 | 7.989113 | 8.309567 | 8.140622 | 8.039442 | 7.846596 | 7.807706 | 7.933381 | 8.232022 | 8.581377 | 7.665133 |
hep-th/0011289 | Kraniotis | D. Bailin, G. V. Kraniotis, A. Love | Supersymmetric Standard Models on D-Branes | 10 pages, LaTeX file, version to appear in Phys.Lett.B | Phys.Lett. B502 (2001) 209-215 | 10.1016/S0370-2693(01)00150-2 | SUSX-TH-00-017, RHCPP 00-03T | hep-th hep-ph | null | Type IIB superstring models with the standard model gauge group on D3-branes
and with massless matter associated with open strings joining D3-branes to
D3-branes or D3-branes to ${\rm D}7_3$-branes are studied. Models with gauge
coupling constant unification at an intermediate scale between about $10^{10}$
and $10^{1... | [
{
"created": "Thu, 30 Nov 2000 17:02:29 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Dec 2000 08:45:40 GMT",
"version": "v2"
},
{
"created": "Sun, 28 Jan 2001 18:39:45 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Bailin",
"D.",
""
],
[
"Kraniotis",
"G. V.",
""
],
[
"Love",
"A.",
""
]
] | Type IIB superstring models with the standard model gauge group on D3-branes and with massless matter associated with open strings joining D3-branes to D3-branes or D3-branes to ${\rm D}7_3$-branes are studied. Models with gauge coupling constant unification at an intermediate scale between about $10^{10}$ and $10^{12}... | 7.286105 | 5.875336 | 5.915648 | 5.80771 | 6.236558 | 6.25549 | 5.855808 | 5.977142 | 5.559288 | 7.147689 | 5.725057 | 5.918256 | 5.725431 | 5.704148 | 6.103346 | 6.004611 | 6.048238 | 5.651184 | 5.758976 | 5.765469 | 6.111887 |
2110.07623 | Cassiano Daniel | Karim Benakli, Nathan Berkovits, Cassiano A. Daniel and Matheus Lize | Higher-Spin States of the Superstring in an Electromagnetic Background | 36 pages + appendix, corrected statement in the introduction | null | 10.1007/JHEP12(2021)112 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Constructing a consistent four-dimensional Lagrangian for charged massive
higher-spin fields propagating in an electromagnetic background is an open
problem. In 1989, Argyres and Nappi used bosonic open string field theory to
construct a Lagrangian for charged massive spin-2 fields in a constant
electromagnetic backg... | [
{
"created": "Thu, 14 Oct 2021 18:00:05 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Oct 2021 17:45:54 GMT",
"version": "v2"
}
] | 2022-01-05 | [
[
"Benakli",
"Karim",
""
],
[
"Berkovits",
"Nathan",
""
],
[
"Daniel",
"Cassiano A.",
""
],
[
"Lize",
"Matheus",
""
]
] | Constructing a consistent four-dimensional Lagrangian for charged massive higher-spin fields propagating in an electromagnetic background is an open problem. In 1989, Argyres and Nappi used bosonic open string field theory to construct a Lagrangian for charged massive spin-2 fields in a constant electromagnetic backgro... | 4.802879 | 4.381003 | 4.953405 | 4.16608 | 4.534061 | 4.557663 | 4.968825 | 4.292077 | 4.224557 | 4.965228 | 4.49357 | 4.348182 | 4.617448 | 4.45221 | 4.352921 | 4.268102 | 4.323337 | 4.428888 | 4.42415 | 4.643761 | 4.366402 |
1708.08066 | Shin Sasaki | Shin Sasaki, Masaya Yata | Gauge Five-brane Solutions of Co-dimension Two in Heterotic Supergravity | 24 pages, 4 figures, typos corrected, version published in JHEP | JHEP 10 (2017) 214 | 10.1007/JHEP10(2017)214 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue to study the BPS gauge five-brane solutions of codimension two in
ten-dimensional heterotic supergravity. The geometry including the dilaton and
the NS-NS $B$-field are sourced from the monopole chain in $\mathbb{R}^2 \times
S^1$. We find that the geometry is asymptotically Ricci flat and the dilaton is
n... | [
{
"created": "Sun, 27 Aug 2017 08:42:20 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Nov 2017 03:45:51 GMT",
"version": "v2"
}
] | 2018-01-17 | [
[
"Sasaki",
"Shin",
""
],
[
"Yata",
"Masaya",
""
]
] | We continue to study the BPS gauge five-brane solutions of codimension two in ten-dimensional heterotic supergravity. The geometry including the dilaton and the NS-NS $B$-field are sourced from the monopole chain in $\mathbb{R}^2 \times S^1$. We find that the geometry is asymptotically Ricci flat and the dilaton is no ... | 10.771275 | 9.75553 | 10.702695 | 8.962703 | 9.328934 | 10.195709 | 10.079669 | 9.86036 | 9.595634 | 11.860787 | 9.387548 | 9.788552 | 10.267204 | 9.82961 | 9.601998 | 9.552513 | 9.582504 | 9.51794 | 9.962486 | 10.34758 | 9.512837 |
1001.0912 | Brandon Carter | Brandon Carter | Fields in nonaffine bundles. IV. Harmonious non-Abelian currents in
string defects | 22 pages Latex | Phys.Rev.D82:103531,2010 | 10.1103/PhysRevD.82.103531 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article continues the study of the category of harmonious field models
that was recently introduced as a kinetically non-linear generalisation of the
well known harmonic category of multiscalar fields over a supporting brane
wordsheet in a target space with a curved Riemannian metric. Like the perfectly
harmonio... | [
{
"created": "Wed, 6 Jan 2010 15:04:45 GMT",
"version": "v1"
}
] | 2010-12-23 | [
[
"Carter",
"Brandon",
""
]
] | This article continues the study of the category of harmonious field models that was recently introduced as a kinetically non-linear generalisation of the well known harmonic category of multiscalar fields over a supporting brane wordsheet in a target space with a curved Riemannian metric. Like the perfectly harmonious... | 21.502016 | 25.872528 | 22.68507 | 22.598074 | 23.328802 | 25.021658 | 24.860357 | 23.802334 | 23.412481 | 26.493361 | 21.276781 | 23.363897 | 21.775097 | 21.151402 | 21.395298 | 22.073374 | 22.210262 | 22.29878 | 22.171148 | 21.790243 | 21.165443 |
1905.08807 | Steven B. Giddings | Steven B. Giddings | Black holes in the quantum universe | 11 pages + refs | null | 10.1098/rsta.2019.0029 | CERN-TH-2019-077 | hep-th astro-ph.HE gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A succinct summary is given of the problem of reconciling observation of
black hole-like objects with quantum mechanics. If quantum black holes behave
like subsystems, and also decay, their information must be transferred to their
environments. Interactions that accomplish this with `minimal' departure from a
standar... | [
{
"created": "Tue, 21 May 2019 18:00:01 GMT",
"version": "v1"
}
] | 2020-07-01 | [
[
"Giddings",
"Steven B.",
""
]
] | A succinct summary is given of the problem of reconciling observation of black hole-like objects with quantum mechanics. If quantum black holes behave like subsystems, and also decay, their information must be transferred to their environments. Interactions that accomplish this with `minimal' departure from a standard ... | 23.554684 | 21.086601 | 21.260986 | 19.06086 | 18.90811 | 21.240953 | 22.665947 | 17.804884 | 20.882397 | 19.312986 | 21.8741 | 21.181118 | 18.418865 | 18.841578 | 19.539459 | 19.973082 | 19.965622 | 19.094719 | 19.612923 | 18.403528 | 21.404741 |
1202.1514 | Kazuya Yonekura | Kazuya Yonekura | On the Trace Anomaly and the Anomaly Puzzle in N=1 Pure Yang-Mills | 25 pages, 1 figure; v2:slight correction in sec.5, minor addition in
appendix | null | 10.1007/JHEP03(2012)029 | UT-12-01, IPMU-12-0014 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The trace anomaly of the energy-momentum tensor is usually quoted in the form
which is proportional to the beta function of the theory. However, there are in
general many definitions of gauge couplings depending on renormalization
schemes, and hence many beta functions. In particular, N=1 supersymmetric pure
Yang-Mil... | [
{
"created": "Tue, 7 Feb 2012 20:18:40 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Feb 2012 12:59:41 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Yonekura",
"Kazuya",
""
]
] | The trace anomaly of the energy-momentum tensor is usually quoted in the form which is proportional to the beta function of the theory. However, there are in general many definitions of gauge couplings depending on renormalization schemes, and hence many beta functions. In particular, N=1 supersymmetric pure Yang-Mills... | 5.800502 | 6.269223 | 6.115237 | 5.9616 | 6.273082 | 6.290995 | 6.047997 | 6.066763 | 5.853967 | 7.132146 | 6.064916 | 6.061853 | 6.079827 | 5.828877 | 6.066191 | 5.988675 | 6.195724 | 5.998201 | 5.983973 | 6.124004 | 5.870424 |
1808.04981 | Deepali Mishra | Deepali Mishra, Yogesh K. Srivastava, Amitabh Virmani | A Generalised Garfinkle-Vachaspati Transform | 40 pages, no figures | null | 10.1007/s10714-018-2477-y | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Garfinkle-Vachaspati transform is a deformation of a metric in terms of a
null, hypersurface orthogonal, Killing vector $k^\mu$. We explore a
generalisation of this deformation in type IIB supergravity taking motivation
from certain studies of the D1-D5 system. We consider solutions of minimal
six-dimensional sup... | [
{
"created": "Wed, 15 Aug 2018 06:37:36 GMT",
"version": "v1"
}
] | 2018-11-28 | [
[
"Mishra",
"Deepali",
""
],
[
"Srivastava",
"Yogesh K.",
""
],
[
"Virmani",
"Amitabh",
""
]
] | The Garfinkle-Vachaspati transform is a deformation of a metric in terms of a null, hypersurface orthogonal, Killing vector $k^\mu$. We explore a generalisation of this deformation in type IIB supergravity taking motivation from certain studies of the D1-D5 system. We consider solutions of minimal six-dimensional super... | 6.245938 | 6.262221 | 6.699538 | 6.140719 | 6.899187 | 6.44675 | 6.725742 | 6.365794 | 6.080353 | 7.106616 | 5.948709 | 6.043021 | 6.181685 | 5.958379 | 6.060528 | 6.063435 | 5.984746 | 6.034802 | 6.001177 | 6.343516 | 5.955675 |
1401.0888 | Francesco Nitti | Elias Kiritsis, Wenliang Li and Francesco Nitti | Holographic RG flow and the Quantum Effective Action | 85 pages, 6 figures. v2: three subsections and one appendix added
with a more detailed discussion of local RG transformations, RG invariance of
the renormalized action, trace identities and scheme dependence; discussion
added about the distinction between RG-invariant and RG scale-dependent
operators; details a... | Fortschr. Phys. 62, No. 5-6, 389-454 (2014) | 10.1002/prop.201400007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The calculation of the full (renormalized) holographic action is undertaken
in general Einstein-scalar theories. The appropriate formalism is developed and
the renormalized effective action is calculated up to two derivatives in the
metric and scalar operators. The holographic RG equations involve Ricci flow
for the ... | [
{
"created": "Sun, 5 Jan 2014 12:37:32 GMT",
"version": "v1"
},
{
"created": "Fri, 31 Jan 2014 16:01:53 GMT",
"version": "v2"
}
] | 2014-06-26 | [
[
"Kiritsis",
"Elias",
""
],
[
"Li",
"Wenliang",
""
],
[
"Nitti",
"Francesco",
""
]
] | The calculation of the full (renormalized) holographic action is undertaken in general Einstein-scalar theories. The appropriate formalism is developed and the renormalized effective action is calculated up to two derivatives in the metric and scalar operators. The holographic RG equations involve Ricci flow for the sp... | 11.038753 | 10.899836 | 11.014329 | 9.647743 | 11.2216 | 10.132849 | 9.553262 | 10.357848 | 10.713951 | 11.589351 | 10.307206 | 10.367624 | 10.828085 | 10.695621 | 10.583842 | 10.658875 | 10.589474 | 10.520722 | 10.299174 | 11.098742 | 10.02296 |
hep-th/9607173 | Marcelo Ubriaco | Marcelo R. Ubriaco | High and low temperature behavior of a quantum group fermion gas | LaTeX file, 14 pages, 2 figures, uses psfig.sty | Mod.Phys.Lett. A11 (1996) 2325-2334 | 10.1142/S0217732396002319 | null | hep-th | null | We consider the simplest $SU_{q}(2)$ invariant fermionic hamiltonian and
calculate the low and high temperature behavior for the two distinct cases
$q>1$ and $q<1$. For low temperatures we find that entropy values for the Fermi
case are an upper bound for those corresponding to $q\neq 1$. At high
temperatures we find... | [
{
"created": "Mon, 22 Jul 1996 16:59:00 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Ubriaco",
"Marcelo R.",
""
]
] | We consider the simplest $SU_{q}(2)$ invariant fermionic hamiltonian and calculate the low and high temperature behavior for the two distinct cases $q>1$ and $q<1$. For low temperatures we find that entropy values for the Fermi case are an upper bound for those corresponding to $q\neq 1$. At high temperatures we find t... | 9.132096 | 9.172675 | 10.024099 | 9.088077 | 9.331841 | 8.914267 | 9.189315 | 8.777131 | 8.48263 | 10.368873 | 8.740712 | 8.637079 | 9.714685 | 8.688342 | 8.78235 | 8.902974 | 8.443784 | 8.805068 | 9.115843 | 9.265033 | 8.65098 |
1206.2383 | Pablo G. Camara | Mikel Berasaluce-Gonzalez, Pablo G. Camara, Fernando Marchesano, Diego
Regalado and Angel M. Uranga | Non-Abelian discrete gauge symmetries in 4d string models | 58 pages; minor typos corrected and references added | null | 10.1007/JHEP09(2012)059 | IFT-UAM/CSIC-12-53 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the realization of non-Abelian discrete gauge symmetries in 4d field
theory and string theory compactifications. The underlying structure
generalizes the Abelian case, and follows from the interplay between gaugings
of non-Abelian isometries of the scalar manifold and field identifications
making axion-like ... | [
{
"created": "Mon, 11 Jun 2012 21:33:16 GMT",
"version": "v1"
},
{
"created": "Thu, 30 Aug 2012 16:45:02 GMT",
"version": "v2"
}
] | 2015-06-05 | [
[
"Berasaluce-Gonzalez",
"Mikel",
""
],
[
"Camara",
"Pablo G.",
""
],
[
"Marchesano",
"Fernando",
""
],
[
"Regalado",
"Diego",
""
],
[
"Uranga",
"Angel M.",
""
]
] | We study the realization of non-Abelian discrete gauge symmetries in 4d field theory and string theory compactifications. The underlying structure generalizes the Abelian case, and follows from the interplay between gaugings of non-Abelian isometries of the scalar manifold and field identifications making axion-like fi... | 7.748787 | 7.840426 | 8.728771 | 7.609116 | 8.704081 | 9.0268 | 8.236779 | 7.431353 | 7.832367 | 9.051597 | 7.561921 | 7.774537 | 7.735158 | 7.490515 | 7.898409 | 7.623137 | 7.821866 | 7.474317 | 7.389655 | 7.912405 | 7.383582 |
0805.1685 | Giuseppe De Risi | G. De Risi | Non-singular Brane cosmology with a Kalb-Ramond field | Talk given at the "43rd Rencontres de Moriond", La Thuile (Val
d'Aosta, Italy), March 15 - 22, 2008 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a model in which a 3-brane is embedded in a warped 5-dimensional
background with a dilaton and a Kalb-Ramond 2-form. We show that it is possible
to find static solutions of the form of charged dS/AdS-like black hole which
could have a negative mass parameter. The motion of the 3-brane in this bulk
generate... | [
{
"created": "Mon, 12 May 2008 16:56:12 GMT",
"version": "v1"
}
] | 2008-05-13 | [
[
"De Risi",
"G.",
""
]
] | We present a model in which a 3-brane is embedded in a warped 5-dimensional background with a dilaton and a Kalb-Ramond 2-form. We show that it is possible to find static solutions of the form of charged dS/AdS-like black hole which could have a negative mass parameter. The motion of the 3-brane in this bulk generates ... | 9.828557 | 7.496537 | 10.077208 | 8.36974 | 7.538501 | 7.753041 | 7.482515 | 7.84346 | 8.707273 | 10.476251 | 7.881881 | 8.77707 | 9.270256 | 8.756308 | 8.527032 | 8.566764 | 8.44788 | 8.489667 | 8.603612 | 9.537248 | 8.828865 |
1308.1163 | Shoichi Ichinose | Shoichi Ichinose | New Approach to Cosmological Fluctuation using the Background Field
Method and CMB Power Spectrum | 6 pages, 5 figures, Presentation at
APPC12(Makuhari,Chiba,Japan,2013.7.14-19), JPS Conference Proceedings (in
press) | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new field theory formulation is presented for the analysis of the CMB power
spectrum distribution in the cosmology. The background-field formalism is fully
used. Stimulated by the recent idea of the {\it emergent} gravity, the
gravitational (metric) field $g_\mn$ is not taken as the quantum-field, but as
the backgr... | [
{
"created": "Tue, 6 Aug 2013 03:00:46 GMT",
"version": "v1"
},
{
"created": "Wed, 9 Oct 2013 06:09:53 GMT",
"version": "v2"
},
{
"created": "Mon, 21 Oct 2013 03:16:49 GMT",
"version": "v3"
}
] | 2013-10-22 | [
[
"Ichinose",
"Shoichi",
""
]
] | A new field theory formulation is presented for the analysis of the CMB power spectrum distribution in the cosmology. The background-field formalism is fully used. Stimulated by the recent idea of the {\it emergent} gravity, the gravitational (metric) field $g_\mn$ is not taken as the quantum-field, but as the backgrou... | 17.019442 | 17.9545 | 16.974646 | 15.77933 | 17.471979 | 17.790565 | 17.856934 | 17.00186 | 16.020128 | 18.970814 | 16.525007 | 16.373634 | 16.687256 | 16.79751 | 16.461891 | 16.530802 | 16.799694 | 16.816839 | 16.604088 | 16.805553 | 16.637701 |
hep-th/0301228 | Sohrab Rahvar | R. Mansouri, M. Borhani, S. Khakshournia | Spherically Symmetric Thick Branes in Vacuum | 8 pages | Int.J.Mod.Phys.A19:4687-4694,2004 | 10.1142/S0217751X04019652 | null | hep-th | null | We consider a spherical thick 3-brane immersed in a five-dimensional bulk
spacetime. We demonstrate how the thick brane equation of motion expanded in
powers of the thickness of the brane can be obtained from the expected junction
conditions on the boundaries of thick brane with the two embedding spacetimes.
It is sh... | [
{
"created": "Tue, 28 Jan 2003 12:15:05 GMT",
"version": "v1"
}
] | 2010-11-19 | [
[
"Mansouri",
"R.",
""
],
[
"Borhani",
"M.",
""
],
[
"Khakshournia",
"S.",
""
]
] | We consider a spherical thick 3-brane immersed in a five-dimensional bulk spacetime. We demonstrate how the thick brane equation of motion expanded in powers of the thickness of the brane can be obtained from the expected junction conditions on the boundaries of thick brane with the two embedding spacetimes. It is show... | 12.770298 | 11.480679 | 11.652232 | 10.749437 | 11.525567 | 11.661735 | 12.487502 | 11.745772 | 13.5282 | 12.275104 | 13.263375 | 12.228406 | 11.830088 | 12.281869 | 11.521539 | 11.860307 | 12.004424 | 11.554353 | 12.228814 | 11.484366 | 11.875278 |
1412.0936 | Driba Tolla Dr. | Loriano Bonora and Driba D.Tolla | Comments on lump solutions in SFT | 30 pages, no figures | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze a recently proposed scheme to construct analytic lump solutions in
open SFT. We argue that in order for the scheme to be operative and guarantee
background independence it must be implemented in the same 2D conformal field
theory in which SFT is formulated. We outline and discuss two different
possible app... | [
{
"created": "Tue, 2 Dec 2014 14:47:55 GMT",
"version": "v1"
}
] | 2014-12-03 | [
[
"Bonora",
"Loriano",
""
],
[
"Tolla",
"Driba D.",
""
]
] | We analyze a recently proposed scheme to construct analytic lump solutions in open SFT. We argue that in order for the scheme to be operative and guarantee background independence it must be implemented in the same 2D conformal field theory in which SFT is formulated. We outline and discuss two different possible appro... | 16.244219 | 14.900096 | 15.966528 | 14.969144 | 14.140704 | 14.237214 | 14.505908 | 13.408651 | 15.466341 | 16.718147 | 14.857431 | 15.277612 | 15.692503 | 14.981802 | 15.106742 | 14.943181 | 15.037144 | 15.168814 | 15.084038 | 14.686119 | 14.783341 |
1904.01876 | Peng-Xiang Hao | Bin Chen, Peng-Xiang Hao, Wei Song | R\'enyi Mutual Information in Holographic Warped CFTs | 41 pages; minor revision, note added | null | 10.1007/JHEP10(2019)037 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The study of R\'enyi mutual information (RMI) sheds light on the AdS/CFT
correspondence beyond classical order. In this article, we study the R\'enyi
mutual information between two intervals at large distance in two-dimensional
holographic warped conformal field theory, which is conjectured to be dual to
the gravity ... | [
{
"created": "Wed, 3 Apr 2019 09:32:47 GMT",
"version": "v1"
},
{
"created": "Fri, 24 May 2019 10:28:23 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Chen",
"Bin",
""
],
[
"Hao",
"Peng-Xiang",
""
],
[
"Song",
"Wei",
""
]
] | The study of R\'enyi mutual information (RMI) sheds light on the AdS/CFT correspondence beyond classical order. In this article, we study the R\'enyi mutual information between two intervals at large distance in two-dimensional holographic warped conformal field theory, which is conjectured to be dual to the gravity on... | 9.784051 | 7.865765 | 10.45578 | 8.008832 | 8.269944 | 8.366286 | 8.75701 | 7.88763 | 8.181737 | 10.663753 | 7.869449 | 8.578473 | 9.342285 | 8.66333 | 8.649349 | 8.34866 | 8.675806 | 8.597228 | 8.668974 | 9.333514 | 8.736408 |
hep-th/9205036 | Kareljan Schoutens | Alfred S. Goldhaber | Solitons with integer fermion number | 12 pages | null | null | ITP-SB-92-08 | hep-th | null | Necessary and sufficient conditions are found for any object in $3+1$
dimensions to have integer rather than fractional fermion number. Nontrivial
examples include the Jackiw-Rebbi monopole and the already well studied
Su-Schrieffer-Heeger soliton, both displaying integer multiples of elementary
charges in combinatio... | [
{
"created": "Wed, 13 May 1992 20:27:18 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Goldhaber",
"Alfred S.",
""
]
] | Necessary and sufficient conditions are found for any object in $3+1$ dimensions to have integer rather than fractional fermion number. Nontrivial examples include the Jackiw-Rebbi monopole and the already well studied Su-Schrieffer-Heeger soliton, both displaying integer multiples of elementary charges in combinations... | 16.615107 | 14.596529 | 15.758554 | 14.798221 | 16.691769 | 17.361031 | 17.163513 | 14.444695 | 14.356317 | 19.192581 | 14.598433 | 14.837307 | 14.909769 | 14.47485 | 14.598352 | 13.490329 | 14.685017 | 13.793583 | 14.157523 | 14.346196 | 13.562549 |
2107.06069 | Istvan Nandori | I. G. Marian, U. D. Jentschura, N. Defenu, A. Trombettoni, I. Nandori | Vacuum Energy and Renormalization of the Field-Independent Term | 19 pages, 4 figures, final version published in JCAP | JCAP 03 (2022) 062 | 10.1088/1475-7516/2022/03/062 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Due to its construction, the nonperturbative renormalization group (RG)
evolution of the constant, field-independent term (which is constant with
respect to field variations but depends on the RG scale $k$) requires special
care within the Functional Renormalization Group (FRG) approach. In several
instances, the con... | [
{
"created": "Thu, 24 Jun 2021 11:34:09 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Mar 2022 08:51:05 GMT",
"version": "v2"
}
] | 2022-04-01 | [
[
"Marian",
"I. G.",
""
],
[
"Jentschura",
"U. D.",
""
],
[
"Defenu",
"N.",
""
],
[
"Trombettoni",
"A.",
""
],
[
"Nandori",
"I.",
""
]
] | Due to its construction, the nonperturbative renormalization group (RG) evolution of the constant, field-independent term (which is constant with respect to field variations but depends on the RG scale $k$) requires special care within the Functional Renormalization Group (FRG) approach. In several instances, the const... | 7.742557 | 7.946695 | 7.901504 | 7.531601 | 8.267911 | 7.998822 | 8.054852 | 7.550738 | 7.695851 | 8.302108 | 7.744569 | 7.524149 | 7.286414 | 7.47535 | 7.527134 | 7.468825 | 7.634554 | 7.381383 | 7.669334 | 7.469103 | 7.446667 |
hep-th/9505158 | Hector DE Vega | H.J. de Vega | STRINGS IN COSMOLOGICAL SPACETIMES AND THEIR BACK-REACTION | Lecture delivered at STRINGS '95, Future Perspectives in String
Theory, USC, Los Angeles, march 13 - 18, 1995, 12 pages, LaTex | null | null | null | hep-th | null | This is a short review on strings in curved spacetimes. We start by recalling
the classical and quantum string behaviour in singular plane waves backgrounds.
We then report on the string behaviour in cosmological spacetimes (FRW, de
Sitter, power inflation) which is by now largerly understood. Recent progress
on self... | [
{
"created": "Thu, 25 May 1995 12:55:02 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"de Vega",
"H. J.",
""
]
] | This is a short review on strings in curved spacetimes. We start by recalling the classical and quantum string behaviour in singular plane waves backgrounds. We then report on the string behaviour in cosmological spacetimes (FRW, de Sitter, power inflation) which is by now largerly understood. Recent progress on self-c... | 9.528938 | 8.970571 | 9.654992 | 8.636812 | 9.317417 | 9.463019 | 9.81268 | 9.067829 | 9.206779 | 9.902913 | 8.481207 | 9.089971 | 8.476577 | 8.547549 | 8.721677 | 9.260207 | 8.977894 | 8.88005 | 8.729651 | 8.73157 | 8.729254 |
1309.4318 | Aliaksei Halavanau | A. Halavanau and Yakov Shnir | Isorotating Baby Skyrmions | 12pages, 6 figures | Phys. Rev. D 88, 085028 (2013) | 10.1103/PhysRevD.88.085028 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss how internal rotation with fixed angular frequency can affect the
solitons in the baby Skyrme model in which the global O(3) symmetry is broken
to the SO(2). Two particular choices of the potential term are considered, the
"old" potential and the "new" double vacuum potential, We do not impose any
assumpti... | [
{
"created": "Tue, 17 Sep 2013 14:15:48 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Oct 2013 16:54:25 GMT",
"version": "v2"
}
] | 2013-10-30 | [
[
"Halavanau",
"A.",
""
],
[
"Shnir",
"Yakov",
""
]
] | We discuss how internal rotation with fixed angular frequency can affect the solitons in the baby Skyrme model in which the global O(3) symmetry is broken to the SO(2). Two particular choices of the potential term are considered, the "old" potential and the "new" double vacuum potential, We do not impose any assumption... | 14.834629 | 10.253908 | 13.640265 | 11.598492 | 11.241131 | 10.710743 | 12.054682 | 11.567645 | 11.219154 | 13.433783 | 12.168571 | 11.5972 | 12.420889 | 11.810136 | 11.986581 | 11.621865 | 12.360111 | 11.861949 | 11.951681 | 13.351682 | 11.435053 |
0802.3578 | Jonas Bj\"ornsson | Jonas Bjornsson, Stephen Hwang | On the unitarity of gauged non-compact world-sheet supersymmetric WZNW
models | 19 pages, 1 table v3: One reference added, typo's corrected, to
appear in Nucl. Phys. B | Nucl.Phys.B812:525-539,2009 | 10.1016/j.nuclphysb.2008.12.011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we generalize our investigation of the unitarity of non-compact
WZNW models connected to Hermitian symmetric spaces to the N=1 world-sheet
supersymmetric extension of these models. We will prove that these models have
a unitary spectrum in a BRST approach for antidominant highest weight
representations ... | [
{
"created": "Mon, 25 Feb 2008 09:48:50 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Nov 2008 14:39:05 GMT",
"version": "v2"
},
{
"created": "Wed, 21 Jan 2009 15:04:00 GMT",
"version": "v3"
}
] | 2009-02-16 | [
[
"Bjornsson",
"Jonas",
""
],
[
"Hwang",
"Stephen",
""
]
] | In this paper we generalize our investigation of the unitarity of non-compact WZNW models connected to Hermitian symmetric spaces to the N=1 world-sheet supersymmetric extension of these models. We will prove that these models have a unitary spectrum in a BRST approach for antidominant highest weight representations if... | 11.068492 | 10.64912 | 13.236334 | 9.829546 | 10.423208 | 9.940474 | 10.003015 | 9.701614 | 9.717165 | 12.961451 | 9.907625 | 10.117997 | 11.453479 | 9.700533 | 9.79252 | 10.178266 | 9.724735 | 10.054942 | 9.602479 | 11.220347 | 9.687728 |
0903.5345 | Veselin Filev | Veselin G. Filev, Clifford V. Johnson, Jonathan P. Shock | Universal Holographic Chiral Dynamics in an External Magnetic Field | 41 pages, 11 figures, references added | JHEP 0908:013,2009 | 10.1088/1126-6708/2009/08/013 | DIAS-STP-09-07 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we further extend the investigation of holographic gauge
theories in external magnetic fields, continuing earlier work. We study the
phenomenon of magnetic catalysis of mass generation in 1+3 and 1+2 dimensions,
using D3/D7- and D3/D5-brane systems, respectively. We obtain the low energy
effective action... | [
{
"created": "Mon, 30 Mar 2009 23:54:24 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Apr 2009 19:19:40 GMT",
"version": "v2"
}
] | 2009-11-16 | [
[
"Filev",
"Veselin G.",
""
],
[
"Johnson",
"Clifford V.",
""
],
[
"Shock",
"Jonathan P.",
""
]
] | In this work we further extend the investigation of holographic gauge theories in external magnetic fields, continuing earlier work. We study the phenomenon of magnetic catalysis of mass generation in 1+3 and 1+2 dimensions, using D3/D7- and D3/D5-brane systems, respectively. We obtain the low energy effective actions ... | 5.392751 | 5.166254 | 5.723895 | 5.078638 | 5.377244 | 5.204275 | 4.95732 | 4.917605 | 5.149911 | 5.761316 | 5.071603 | 5.143612 | 5.423093 | 5.162198 | 5.149262 | 5.081121 | 5.201909 | 5.110144 | 5.243577 | 5.374903 | 5.148655 |
1402.6805 | Yi-Jian Du | Yi-Jian Du, Bo Feng, Chih-Hao Fu | Dual-color decompositions at one-loop level in Yang-Mills theory | 26 pages,5 figures | null | 10.1007/JHEP06(2014)157 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we extend the construction of dual color decomposition in
Yang-Mills theory to one-loop level, i.e., we show how to write one-loop
integrands in Yang-Mills theory to the dual DDM-form and the dual trace-form.
In dual forms, integrands are decomposed in terms of color-ordered one-loop
integrands for colo... | [
{
"created": "Thu, 27 Feb 2014 06:58:11 GMT",
"version": "v1"
}
] | 2015-06-18 | [
[
"Du",
"Yi-Jian",
""
],
[
"Feng",
"Bo",
""
],
[
"Fu",
"Chih-Hao",
""
]
] | In this work, we extend the construction of dual color decomposition in Yang-Mills theory to one-loop level, i.e., we show how to write one-loop integrands in Yang-Mills theory to the dual DDM-form and the dual trace-form. In dual forms, integrands are decomposed in terms of color-ordered one-loop integrands for color ... | 13.967109 | 12.044212 | 14.514765 | 11.90806 | 13.187173 | 12.737771 | 13.094214 | 12.343884 | 11.069387 | 14.92282 | 12.284792 | 11.741737 | 12.533465 | 11.887611 | 12.715585 | 12.683976 | 12.205407 | 12.155785 | 11.511778 | 13.320754 | 12.458302 |
hep-th/0510151 | Takahashi Hidenori | T. Fujita, M. Hiramoto, T. Homma, M. Matsumoto, H. Takahashi | Re-Interpretation of Spontaneous Symmetry Breaking in Quantum Field
Theory and Goldstone Theorem | 10pages, 2 figures | null | null | null | hep-th hep-ph | null | We present a new picture of global symmetry breaking in quantum field theory
and propose a novel realization of symmetry breaking phenomena in terms of the
conserved charge associated with its symmetry. In particular, the fermion
condensate of the vacuum state is examined when the spontaneous chiral symmetry
breaking... | [
{
"created": "Tue, 18 Oct 2005 07:38:54 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Fujita",
"T.",
""
],
[
"Hiramoto",
"M.",
""
],
[
"Homma",
"T.",
""
],
[
"Matsumoto",
"M.",
""
],
[
"Takahashi",
"H.",
""
]
] | We present a new picture of global symmetry breaking in quantum field theory and propose a novel realization of symmetry breaking phenomena in terms of the conserved charge associated with its symmetry. In particular, the fermion condensate of the vacuum state is examined when the spontaneous chiral symmetry breaking t... | 8.325878 | 8.229738 | 8.509136 | 8.36968 | 8.37473 | 7.956306 | 8.316774 | 8.100375 | 8.283886 | 8.986915 | 8.388394 | 7.841226 | 8.273725 | 7.914212 | 8.007003 | 7.998324 | 7.934268 | 7.917639 | 8.033548 | 8.093655 | 7.89682 |
hep-th/9807208 | O. Loughlin Martin | M.J. O'Loughlin, S. Randjbar-Daemi | AdS(3) x R as a target space for the (2,1) string theory | 14 pages, latex | Nucl.Phys. B543 (1999) 170-182 | 10.1016/S0550-3213(98)00872-4 | null | hep-th | null | We study a target space geometry of the form $AdS_3 \times {\bf R}$ for the
$(2,1)$ heterotic string. This target space arises as the near horizon limit of
a solitonic configuration in 2+2 dimensions. We investigate the null isometries
of this space and discuss the reduction to 1+1 dimensions of the target space
geom... | [
{
"created": "Tue, 28 Jul 1998 16:41:14 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"O'Loughlin",
"M. J.",
""
],
[
"Randjbar-Daemi",
"S.",
""
]
] | We study a target space geometry of the form $AdS_3 \times {\bf R}$ for the $(2,1)$ heterotic string. This target space arises as the near horizon limit of a solitonic configuration in 2+2 dimensions. We investigate the null isometries of this space and discuss the reduction to 1+1 dimensions of the target space geomet... | 8.290606 | 6.971623 | 8.363274 | 7.400651 | 7.148541 | 7.88208 | 7.254485 | 7.330789 | 7.078256 | 9.763138 | 7.09876 | 7.313993 | 8.071995 | 7.25658 | 7.512096 | 7.308514 | 7.400054 | 7.35227 | 7.351988 | 7.62813 | 7.205655 |
1504.01370 | Yanyan Bu | Yanyan Bu, Michael Lublinsky and Amir Sharon | Hydrodynamics dual to Einstein-Gauss-Bonnet gravity: all-order gradient
resummation | v1: 23 pages, 8 multi-figures, one appendix; v2: title changed, we
improved numerical calculations and found the Gauss-Bonnet corrected memory
functions still have no support at negative times, and we removed wrong
statement about causality violation in previous version; v3: minor revision,
to appear in JHEP | null | null | null | hep-th gr-qc hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Relativistic hydrodynamics dual to Einstein-Gauss-Bonnet gravity in
asymptotic $\textrm{AdS}_5$ space is under study. To linear order in the
amplitude of the fluid velocity and temperature, we derive the fluid's
stress-energy tensor via an all-order resummation of the derivative terms. Each
order is accompanied by ne... | [
{
"created": "Mon, 6 Apr 2015 19:50:31 GMT",
"version": "v1"
},
{
"created": "Mon, 13 Apr 2015 19:44:11 GMT",
"version": "v2"
},
{
"created": "Sun, 14 Jun 2015 13:57:18 GMT",
"version": "v3"
}
] | 2015-06-16 | [
[
"Bu",
"Yanyan",
""
],
[
"Lublinsky",
"Michael",
""
],
[
"Sharon",
"Amir",
""
]
] | Relativistic hydrodynamics dual to Einstein-Gauss-Bonnet gravity in asymptotic $\textrm{AdS}_5$ space is under study. To linear order in the amplitude of the fluid velocity and temperature, we derive the fluid's stress-energy tensor via an all-order resummation of the derivative terms. Each order is accompanied by new ... | 11.237112 | 10.696078 | 13.476551 | 9.810919 | 10.250648 | 10.468683 | 9.712083 | 10.387877 | 10.356747 | 11.829724 | 9.922767 | 9.348866 | 11.312031 | 10.285545 | 9.704574 | 9.472928 | 9.731709 | 10.2498 | 9.677958 | 11.251154 | 9.733437 |
0902.0290 | Chethan Krishnan | Chethan Krishnan, Carlo Maccaferri, Harvendra Singh | M2-brane Flows and the Chern-Simons Level | v4: figure with typo replaced, clarifications added. 35 pp | JHEP 0905:114,2009 | 10.1088/1126-6708/2009/05/114 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Chern-Simons level k of ABJM gauge theory captures the orbifolding in the
dual geometry. This suggests that if we move the membranes away from the tip of
the orbifold to a smooth point, it should trigger an RG flow that changes the
level to k=1 in the IR. We construct an explicit supergravity solution that is
dua... | [
{
"created": "Mon, 2 Feb 2009 14:32:10 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Feb 2009 18:12:37 GMT",
"version": "v2"
},
{
"created": "Thu, 28 May 2009 00:00:43 GMT",
"version": "v3"
},
{
"created": "Fri, 6 Nov 2009 11:10:50 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Krishnan",
"Chethan",
""
],
[
"Maccaferri",
"Carlo",
""
],
[
"Singh",
"Harvendra",
""
]
] | The Chern-Simons level k of ABJM gauge theory captures the orbifolding in the dual geometry. This suggests that if we move the membranes away from the tip of the orbifold to a smooth point, it should trigger an RG flow that changes the level to k=1 in the IR. We construct an explicit supergravity solution that is dual ... | 10.022869 | 9.386674 | 12.772177 | 10.03688 | 10.424381 | 10.195852 | 9.991935 | 9.204487 | 9.885099 | 14.343395 | 9.734819 | 9.480706 | 10.512676 | 9.574422 | 9.765752 | 9.494771 | 9.409023 | 9.430887 | 9.836814 | 10.921219 | 9.42416 |
1009.1695 | Reiji Yoshioka | Reiji Yoshioka | Effects of Matrix Orientifolding to Two-Loop Effective Action of Bosonic
IIB Matrix Model | 16 pages, 3 figures | null | null | OCU-PHYS 337 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the spacetime structures which are described by the IIB matrix model
with orientifolding. Matrix orientifolding that preserves supersymmetries
yields the mirror image point with respect to a four-dimensional plane for each
spacetime point that corresponds to the eigenvalue of the bosonic matrix. In
order to ... | [
{
"created": "Thu, 9 Sep 2010 07:14:21 GMT",
"version": "v1"
}
] | 2010-09-10 | [
[
"Yoshioka",
"Reiji",
""
]
] | We study the spacetime structures which are described by the IIB matrix model with orientifolding. Matrix orientifolding that preserves supersymmetries yields the mirror image point with respect to a four-dimensional plane for each spacetime point that corresponds to the eigenvalue of the bosonic matrix. In order to co... | 11.90382 | 10.823365 | 11.733438 | 10.587259 | 10.854012 | 11.560172 | 11.444206 | 10.669661 | 11.168902 | 14.788155 | 10.262881 | 10.74903 | 12.179642 | 10.22654 | 10.638612 | 10.675187 | 10.359905 | 10.634367 | 10.398683 | 11.72939 | 9.963403 |
0706.4475 | Liu Zhao | Liu Zhao | Black chain of pearls in 5D de Sitter spacetime | 4 pages, 3 figures. Wrong statements on stability based on error
incaculations corrected. New references added | null | null | null | hep-th | null | We analyze some exact chain-shaped black hole solutions in 5-dimensional
spacetime. Unlike usual black string and black ring solutions, the topology of
the horizons of the new solutions are neither $\mathbb{R}\times R^{2}$ nor
$S^1\times S^2$ but rather like several topological spheres concatenating each
other at sin... | [
{
"created": "Fri, 29 Jun 2007 19:22:52 GMT",
"version": "v1"
},
{
"created": "Sun, 1 Jul 2007 18:07:43 GMT",
"version": "v2"
}
] | 2007-07-02 | [
[
"Zhao",
"Liu",
""
]
] | We analyze some exact chain-shaped black hole solutions in 5-dimensional spacetime. Unlike usual black string and black ring solutions, the topology of the horizons of the new solutions are neither $\mathbb{R}\times R^{2}$ nor $S^1\times S^2$ but rather like several topological spheres concatenating each other at singl... | 8.810141 | 9.121084 | 8.442954 | 7.957348 | 8.994282 | 8.158811 | 9.454592 | 8.340997 | 8.385679 | 8.260486 | 7.726834 | 8.470171 | 8.299814 | 7.970664 | 8.260595 | 8.254008 | 8.345898 | 7.774631 | 8.751176 | 8.388631 | 8.235752 |
hep-th/9912260 | C. T. Chan | Chuan-Tsung Chan (National Taiwan University) | Exact Scattering States of Dirac-Born-Infeld Equation with Constant
Background Fields | 18 pages, latex, no figures | Phys.Rev. D62 (2000) 026002 | 10.1103/PhysRevD.62.026002 | null | hep-th | null | Exact solutions to the Dirac-Born-Infeld equation, which describes
scatterings of localized wave packets in the presence of constant background
fields, are derived in this paper.
| [
{
"created": "Mon, 27 Dec 1999 22:47:58 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Chan",
"Chuan-Tsung",
"",
"National Taiwan University"
]
] | Exact solutions to the Dirac-Born-Infeld equation, which describes scatterings of localized wave packets in the presence of constant background fields, are derived in this paper. | 11.689053 | 7.864306 | 8.397646 | 8.819074 | 10.001941 | 8.572185 | 8.337318 | 8.211413 | 8.053852 | 12.477652 | 8.645434 | 11.313061 | 10.236887 | 10.165441 | 10.075653 | 11.011979 | 10.905939 | 10.791636 | 10.247732 | 11.058794 | 10.167265 |
hep-th/9301013 | Michael Fry | M. P. Fry | Fermionic Determinant of the Massive Schwinger Model | null | Phys.Rev. D47 (1993) 2629-2632 | 10.1103/PhysRevD.47.2629 | null | hep-th | null | A representation for the fermionic determinant of the massive Schwinger
model, or $QED_2$, is obtained that makes a clean separation between the
Schwinger model and its massive counterpart. From this it is shown that the
index theorem for $QED_2$ follows from gauge invariance, that the Schwinger
model's contribution ... | [
{
"created": "Tue, 5 Jan 1993 16:11:22 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Fry",
"M. P.",
""
]
] | A representation for the fermionic determinant of the massive Schwinger model, or $QED_2$, is obtained that makes a clean separation between the Schwinger model and its massive counterpart. From this it is shown that the index theorem for $QED_2$ follows from gauge invariance, that the Schwinger model's contribution to... | 9.894526 | 8.79661 | 8.354036 | 7.919736 | 8.456927 | 8.582128 | 8.507015 | 8.361963 | 7.484138 | 10.183318 | 8.156672 | 8.127814 | 8.441618 | 8.161648 | 8.425667 | 8.489526 | 8.154196 | 8.498829 | 7.874038 | 8.410096 | 8.091459 |
0807.5010 | Mitsuhiro Kato | Masako Asano and Mitsuhiro Kato | General Linear Gauges and Amplitudes in Open String Field Theory | 32 pages | Nucl.Phys.B807:348-372,2009 | 10.1016/j.nuclphysb.2008.09.004 | UT-Komaba/08-12 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A general class of gauges for open string field theory, for which the gauge
fixing condition is given by linear equations with respect to string field, is
investigated in detail. This class of gauges includes almost all known ones
like Siegel gauge and its various extensions such as a-gauges proposed by the
present a... | [
{
"created": "Thu, 31 Jul 2008 08:23:45 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Asano",
"Masako",
""
],
[
"Kato",
"Mitsuhiro",
""
]
] | A general class of gauges for open string field theory, for which the gauge fixing condition is given by linear equations with respect to string field, is investigated in detail. This class of gauges includes almost all known ones like Siegel gauge and its various extensions such as a-gauges proposed by the present aut... | 10.765544 | 10.539042 | 11.952909 | 9.379704 | 10.220645 | 9.825984 | 9.840858 | 9.623341 | 9.247539 | 11.857733 | 9.063105 | 9.656772 | 10.519347 | 9.613555 | 9.712877 | 9.592765 | 9.565244 | 10.099009 | 9.587559 | 10.806265 | 9.248468 |
hep-th/9411236 | Parthasarathi Mitra | P. Mitra | Exclusion statistics and many-particle states | 6 pages, revtex | null | null | SISSA-191/94/EP | hep-th cond-mat | null | The thermodynamic distribution function for exclusion statistics is derived.
Creation and annihilation operators for particles obeying such statistics are
discussed. A connection with anyons is pointed out.
| [
{
"created": "Wed, 30 Nov 1994 17:37:23 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Mitra",
"P.",
""
]
] | The thermodynamic distribution function for exclusion statistics is derived. Creation and annihilation operators for particles obeying such statistics are discussed. A connection with anyons is pointed out. | 12.693735 | 9.898535 | 10.467719 | 9.72325 | 9.704321 | 9.614591 | 9.585484 | 10.280997 | 9.75023 | 10.907388 | 11.061228 | 10.990629 | 11.25178 | 10.315883 | 10.657642 | 11.011289 | 10.52358 | 10.792016 | 10.837755 | 11.166938 | 11.501038 |
hep-th/0103164 | Harold Steinacker | H. Grosse, J. Madore, H. Steinacker | Field Theory on the q-deformed Fuzzy Sphere II: Quantization | LaTex file, 44 pages | J.Geom.Phys. 43 (2002) 205-240 | 10.1016/S0393-0440(02)00023-2 | LMU-TPW 1-01, LPT-ORSAY 01-22, UWThPh-2001-10 | hep-th math.QA | null | We study the second quantization of field theory on the q-deformed fuzzy
sphere for real q. This is performed using a path-integral over the modes,
which generate a quasiassociative algebra. The resulting models have a manifest
U_q(su(2)) symmetry with a smooth limit q -> 1, and satisfy positivity and
twisted bosonic... | [
{
"created": "Tue, 20 Mar 2001 23:04:20 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Grosse",
"H.",
""
],
[
"Madore",
"J.",
""
],
[
"Steinacker",
"H.",
""
]
] | We study the second quantization of field theory on the q-deformed fuzzy sphere for real q. This is performed using a path-integral over the modes, which generate a quasiassociative algebra. The resulting models have a manifest U_q(su(2)) symmetry with a smooth limit q -> 1, and satisfy positivity and twisted bosonic s... | 13.363873 | 11.866133 | 14.156844 | 11.504923 | 12.103132 | 12.491197 | 12.004024 | 12.624704 | 11.834669 | 14.156764 | 11.304682 | 12.041354 | 13.559649 | 12.32842 | 12.035728 | 12.096806 | 12.237771 | 12.381214 | 12.330395 | 13.328159 | 12.240581 |
hep-th/0006055 | Srinath Cheluvaraja | S.Cheluvaraja (Louisiana State University) | Z(2) vortex solution in a field theory | 14 pages latex | null | null | LSUHE 344-2000 | hep-th | null | We present a finite energy topological Z(2) vortex solution in a 2+1
dimensional SO(3) gauge field theory minimally coupled to a matrix valued Higgs
field. The vortex carries a Z(2) magnetic charge and obeys a modulo two
addition property. The core of this vortex has a structure similar to that of
the Abrikosov vorte... | [
{
"created": "Wed, 7 Jun 2000 22:46:31 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Cheluvaraja",
"S.",
"",
"Louisiana State University"
]
] | We present a finite energy topological Z(2) vortex solution in a 2+1 dimensional SO(3) gauge field theory minimally coupled to a matrix valued Higgs field. The vortex carries a Z(2) magnetic charge and obeys a modulo two addition property. The core of this vortex has a structure similar to that of the Abrikosov vortex ... | 10.483386 | 11.571526 | 10.376282 | 10.323756 | 11.930041 | 11.121366 | 11.920477 | 11.346583 | 10.709867 | 10.712773 | 10.465935 | 10.881948 | 10.333879 | 10.253184 | 10.768847 | 10.20807 | 10.460153 | 10.68973 | 10.328557 | 10.400959 | 10.335629 |
2312.00120 | Tom Rudelius | Tom Rudelius | Persistence of the Pattern in the Interior of 5d Moduli Spaces | 5 pages | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Castellano, Ruiz, and Valenzuela recently observed a remarkable "pattern" in
infinite-distance limits of moduli spaces in quantum gravity, which relates the
field space variation of the mass of the lightest tower of particles to the
field space variation of the species scale. In this work, we show how a version
of th... | [
{
"created": "Thu, 30 Nov 2023 19:00:00 GMT",
"version": "v1"
}
] | 2023-12-04 | [
[
"Rudelius",
"Tom",
""
]
] | Castellano, Ruiz, and Valenzuela recently observed a remarkable "pattern" in infinite-distance limits of moduli spaces in quantum gravity, which relates the field space variation of the mass of the lightest tower of particles to the field space variation of the species scale. In this work, we show how a version of this... | 10.827309 | 8.895012 | 10.799149 | 8.813682 | 9.62117 | 8.764932 | 8.536713 | 8.198365 | 9.047057 | 11.788627 | 9.162317 | 9.276729 | 9.546324 | 9.102667 | 9.02861 | 9.496148 | 8.821949 | 9.349831 | 8.765109 | 9.651273 | 9.469704 |
hep-th/9110034 | David Kutasov | M. Bershadsky and D. Kutasov | Open String Theory in 1+1 Dimensions | 10 pages | Phys.Lett.B274:331-337,1992 | 10.1016/0370-2693(92)91993-J | null | hep-th | null | We show that tree level open two dimensional string theory is exactly
solvable; the solution exhibits some unusual features, and is qualitatively
different from the closed case. The open string ``tachyon'' S -- matrix
describes free fermions, which can be interpreted as the quarks at the ends of
the string. These ``q... | [
{
"created": "Mon, 14 Oct 1991 14:19:40 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Bershadsky",
"M.",
""
],
[
"Kutasov",
"D.",
""
]
] | We show that tree level open two dimensional string theory is exactly solvable; the solution exhibits some unusual features, and is qualitatively different from the closed case. The open string ``tachyon'' S -- matrix describes free fermions, which can be interpreted as the quarks at the ends of the string. These ``qua... | 13.70811 | 12.390084 | 15.51726 | 11.618349 | 12.477083 | 12.248022 | 12.018821 | 13.337098 | 12.048059 | 15.487509 | 11.268706 | 12.152701 | 14.194464 | 12.544195 | 12.694366 | 12.108133 | 12.175906 | 12.215703 | 12.022683 | 13.531852 | 11.973111 |
hep-th/0403190 | Marcus Spradlin | Radu Roiban, Marcus Spradlin, Anastasia Volovich | On the Tree-Level S-Matrix of Yang-Mills Theory | 20 pages, 2 figures, harvmac. v2: proof of parity symmetry added | Phys.Rev.D70:026009,2004 | 10.1103/PhysRevD.70.026009 | null | hep-th hep-ph | null | In this note we further investigate the procedure for computing tree-level
amplitudes in Yang-Mills theory from connected instantons in the B-model on
P^{3|4}, emphasizing that the problem of calculating Feynman diagrams is recast
into the problem of finding solutions to a certain set of algebraic equations.
We show ... | [
{
"created": "Fri, 19 Mar 2004 01:39:02 GMT",
"version": "v1"
},
{
"created": "Sun, 21 Mar 2004 19:39:12 GMT",
"version": "v2"
}
] | 2011-05-05 | [
[
"Roiban",
"Radu",
""
],
[
"Spradlin",
"Marcus",
""
],
[
"Volovich",
"Anastasia",
""
]
] | In this note we further investigate the procedure for computing tree-level amplitudes in Yang-Mills theory from connected instantons in the B-model on P^{3|4}, emphasizing that the problem of calculating Feynman diagrams is recast into the problem of finding solutions to a certain set of algebraic equations. We show th... | 9.489216 | 8.822532 | 9.232193 | 8.47438 | 8.574441 | 9.178096 | 9.136003 | 8.730905 | 7.964298 | 10.67733 | 8.508883 | 8.345703 | 9.306578 | 8.60218 | 8.547151 | 8.571405 | 8.630579 | 8.621419 | 8.265788 | 9.115491 | 8.292938 |
1507.02660 | Niall Macpherson | Yolanda Lozano, Niall T. Macpherson, Jes\'us Montero | A $\mathcal{N}=2$ Supersymmetric $AdS_4$ Solution in M-theory with
Purely Magnetic Flux | 19 pages plus appendices. v2 metadata amended, reference added | null | 10.1007/JHEP10(2015)004 | FPAUO-15/06 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find a new $\mathcal{N}=2$ $AdS_4$ solution in M-theory supported by
purely magnetic flux via a sequence of abelian and non-abelian T-dualities.
This provides the second known example in this class besides the uplift of the
Pernici and Sezgin solution to 7d gauged supergravity constructed in the
eighties. We compu... | [
{
"created": "Thu, 9 Jul 2015 19:10:36 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Jul 2015 12:47:39 GMT",
"version": "v2"
}
] | 2018-10-26 | [
[
"Lozano",
"Yolanda",
""
],
[
"Macpherson",
"Niall T.",
""
],
[
"Montero",
"Jesús",
""
]
] | We find a new $\mathcal{N}=2$ $AdS_4$ solution in M-theory supported by purely magnetic flux via a sequence of abelian and non-abelian T-dualities. This provides the second known example in this class besides the uplift of the Pernici and Sezgin solution to 7d gauged supergravity constructed in the eighties. We compute... | 6.583475 | 6.117406 | 8.175442 | 5.902038 | 6.215207 | 6.190593 | 6.101233 | 6.098715 | 6.028261 | 8.861903 | 6.167467 | 6.184886 | 6.997634 | 6.304035 | 6.543395 | 6.20086 | 6.387342 | 6.038599 | 6.232433 | 6.987901 | 6.319267 |
0802.3391 | Cumrun Vafa | Chris Beasley, Jonathan J. Heckman, Cumrun Vafa | GUTs and Exceptional Branes in F-theory - I | v2: 121 pages, 5 figures, reference and clarification added | JHEP 0901:058,2009 | 10.1088/1126-6708/2009/01/058 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by potential phenomenological applications, we develop the
necessary tools for building GUT models in F-theory. This approach is quite
flexible because the local geometrical properties of singularities in F-theory
compactifications encode the physical content of the theory. In particular, we
show how geomet... | [
{
"created": "Mon, 25 Feb 2008 16:59:39 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Nov 2008 01:22:07 GMT",
"version": "v2"
}
] | 2010-04-06 | [
[
"Beasley",
"Chris",
""
],
[
"Heckman",
"Jonathan J.",
""
],
[
"Vafa",
"Cumrun",
""
]
] | Motivated by potential phenomenological applications, we develop the necessary tools for building GUT models in F-theory. This approach is quite flexible because the local geometrical properties of singularities in F-theory compactifications encode the physical content of the theory. In particular, we show how geometry... | 10.379637 | 10.387373 | 11.338452 | 10.423895 | 10.228626 | 10.492802 | 10.745302 | 10.101571 | 9.679001 | 12.117537 | 9.75201 | 9.894719 | 10.527956 | 10.051556 | 9.916606 | 10.046576 | 10.179971 | 10.230361 | 9.765456 | 10.424468 | 10.377121 |
hep-th/0506090 | S. Stieberger | D. Lust, S. Reffert, W. Schulgin, S. Stieberger | Moduli Stabilization in Type IIB Orientifolds (I) | 97 pages + 2 figs, harvmac | Nucl.Phys.B766:68-149,2007 | 10.1016/j.nuclphysb.2006.12.018 | LMU-ASC 45/05, MPP-2005-59 | hep-th | null | We discuss flux quantization and moduli stabilization in toroidal type IIB
Z_N - or Z_N x Z_M -orientifolds, focusing mainly on their orbifold limits.
After presenting a detailed discussion of their moduli spaces and effective
actions, we study the supersymmetric vacuum structure of these models and
derive criteria f... | [
{
"created": "Mon, 13 Jun 2005 19:43:31 GMT",
"version": "v1"
},
{
"created": "Thu, 16 Nov 2006 17:04:48 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Lust",
"D.",
""
],
[
"Reffert",
"S.",
""
],
[
"Schulgin",
"W.",
""
],
[
"Stieberger",
"S.",
""
]
] | We discuss flux quantization and moduli stabilization in toroidal type IIB Z_N - or Z_N x Z_M -orientifolds, focusing mainly on their orbifold limits. After presenting a detailed discussion of their moduli spaces and effective actions, we study the supersymmetric vacuum structure of these models and derive criteria for... | 8.150134 | 8.227431 | 11.08878 | 7.450604 | 7.01949 | 7.923304 | 7.631876 | 7.618973 | 7.777741 | 9.767163 | 7.61684 | 7.606589 | 9.004948 | 8.058747 | 7.443926 | 7.713578 | 7.52046 | 7.742922 | 7.632745 | 8.385659 | 7.769223 |
2301.02587 | Roberto Emparan | Roberto Emparan, Raimon Luna, Ryotaku Suzuki, Marija Toma\v{s}evi\'c,
Benson Way | Holographic duals of evaporating black holes | 27 pages, 13 figures. v2: 31 pages, 16 figures. Improved discussions,
refs added. v3: matches published version | JHEP05(2023)182 | 10.1007/JHEP05(2023)182 | CPHT-RR057.112022, TTI-MATHPHYS-18 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe the dynamical evaporation of a black hole as the classical
evolution in time of a black hole in an Anti-de Sitter braneworld. A bulk black
hole whose horizon intersects the brane yields the classical bulk dual of a
black hole coupled to quantum conformal fields. The evaporation of this black
hole happens ... | [
{
"created": "Fri, 6 Jan 2023 16:34:28 GMT",
"version": "v1"
},
{
"created": "Tue, 14 Feb 2023 23:13:53 GMT",
"version": "v2"
},
{
"created": "Sun, 28 May 2023 12:34:23 GMT",
"version": "v3"
}
] | 2023-05-30 | [
[
"Emparan",
"Roberto",
""
],
[
"Luna",
"Raimon",
""
],
[
"Suzuki",
"Ryotaku",
""
],
[
"Tomašević",
"Marija",
""
],
[
"Way",
"Benson",
""
]
] | We describe the dynamical evaporation of a black hole as the classical evolution in time of a black hole in an Anti-de Sitter braneworld. A bulk black hole whose horizon intersects the brane yields the classical bulk dual of a black hole coupled to quantum conformal fields. The evaporation of this black hole happens wh... | 12.586061 | 11.195003 | 13.968917 | 11.975901 | 12.317522 | 11.297455 | 11.5761 | 11.371096 | 11.344114 | 14.467408 | 11.328097 | 11.232736 | 12.701838 | 11.69043 | 12.062134 | 11.332717 | 11.907379 | 11.624414 | 11.640742 | 11.756273 | 11.67523 |
2007.00623 | Ricardo Monteiro | Joseph A. Farrow, Yvonne Geyer, Arthur E. Lipstein, Ricardo Monteiro,
Ricardo Stark-Much\~ao | Propagators, BCFW Recursion and New Scattering Equations at One Loop | 62 pages + appendices, 12 figures. v2: minor changes, published
version | null | 10.1007/JHEP10(2020)074 | QMUL-PH-20-15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate how loop-level propagators arise from tree level via a
forward-limit procedure in two modern approaches to scattering amplitudes,
namely the BCFW recursion relations and the scattering equations formalism. In
the first part of the paper, we revisit the BCFW construction of one-loop
integrands in moment... | [
{
"created": "Wed, 1 Jul 2020 17:13:28 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Sep 2020 21:24:14 GMT",
"version": "v2"
}
] | 2020-10-28 | [
[
"Farrow",
"Joseph A.",
""
],
[
"Geyer",
"Yvonne",
""
],
[
"Lipstein",
"Arthur E.",
""
],
[
"Monteiro",
"Ricardo",
""
],
[
"Stark-Muchão",
"Ricardo",
""
]
] | We investigate how loop-level propagators arise from tree level via a forward-limit procedure in two modern approaches to scattering amplitudes, namely the BCFW recursion relations and the scattering equations formalism. In the first part of the paper, we revisit the BCFW construction of one-loop integrands in momentum... | 9.183785 | 9.214375 | 9.987191 | 8.419367 | 8.884726 | 8.785407 | 8.476684 | 8.517187 | 8.748213 | 10.446336 | 8.254337 | 8.68963 | 8.824736 | 8.50964 | 8.469376 | 8.547862 | 8.520286 | 8.870293 | 8.677128 | 9.126557 | 8.720365 |
1002.1391 | Aram Saharian | S. Bellucci, A. A. Saharian, V. M. Bardeghyan | Induced fermionic current in toroidally compactified spacetimes with
applications to cylindrical and toroidal nanotubes | 18 pages, 5 figures, explicit regularization procedure added | Phys.Rev.D82:065011,2010 | 10.1103/PhysRevD.82.065011 | null | hep-th cond-mat.mes-hall gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The vacuum expectation value of the fermionic current is evaluated for a
massive spinor field in spacetimes with an arbitrary number of toroidally
compactified spatial dimensions in presence of a constant gauge field. By using
the Abel-Plana type summation formula and the zeta function technique we
present the fermio... | [
{
"created": "Mon, 8 Feb 2010 11:51:58 GMT",
"version": "v1"
},
{
"created": "Sun, 22 Aug 2010 20:21:43 GMT",
"version": "v2"
}
] | 2010-11-12 | [
[
"Bellucci",
"S.",
""
],
[
"Saharian",
"A. A.",
""
],
[
"Bardeghyan",
"V. M.",
""
]
] | The vacuum expectation value of the fermionic current is evaluated for a massive spinor field in spacetimes with an arbitrary number of toroidally compactified spatial dimensions in presence of a constant gauge field. By using the Abel-Plana type summation formula and the zeta function technique we present the fermioni... | 6.389177 | 3.783011 | 6.614231 | 4.33094 | 4.727991 | 4.398821 | 4.079487 | 3.977218 | 4.213421 | 7.28095 | 4.453712 | 5.23277 | 6.087367 | 5.499311 | 5.381157 | 5.183643 | 5.279705 | 5.454842 | 5.523607 | 6.133394 | 5.593025 |
2309.14438 | Napat Poovuttikul | Arpit Das, Adrien Florio, Nabil Iqbal, Napat Poovuttikul | Higher-form symmetry and chiral transport in real-time lattice $U(1)$
gauge theory | 24 pages + appendix, 9 figures. Clarifications added. Comments are
welcomed | null | null | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study classical lattice simulations of theories of electrodynamics coupled
to charged matter at finite temperature, interpreting them using the
higher-form symmetry formulation of magnetohydrodynamics (MHD). We compute
transport coefficients using classical Kubo formulas on the lattice and show
that the properties... | [
{
"created": "Mon, 25 Sep 2023 18:00:54 GMT",
"version": "v1"
},
{
"created": "Thu, 28 Mar 2024 15:16:25 GMT",
"version": "v2"
}
] | 2024-03-29 | [
[
"Das",
"Arpit",
""
],
[
"Florio",
"Adrien",
""
],
[
"Iqbal",
"Nabil",
""
],
[
"Poovuttikul",
"Napat",
""
]
] | We study classical lattice simulations of theories of electrodynamics coupled to charged matter at finite temperature, interpreting them using the higher-form symmetry formulation of magnetohydrodynamics (MHD). We compute transport coefficients using classical Kubo formulas on the lattice and show that the properties o... | 12.400008 | 12.467812 | 12.891531 | 12.198834 | 13.07628 | 13.149147 | 12.915462 | 12.697653 | 12.751177 | 13.927225 | 12.433114 | 12.489346 | 12.890999 | 12.197046 | 12.328087 | 12.003511 | 12.91078 | 11.853135 | 12.027604 | 12.044086 | 11.883227 |
2311.17322 | Atakan Hilmi F{\i}rat | Theodore Erler and Atakan Hilmi F{\i}rat | Wilsonian effective potentials and closed string field theory | 36 pages, 14 figures, 3 tables | JHEP02(2024)018 | 10.1007/JHEP02(2024)018 | MIT-CTP/5648 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate Wilsonian effective field theory as a model for the
construction of the tachyon potential and nonperturbative vacua in closed
string field theory. In a number of cases we are able to find the effective
potential exactly, and observe what appear to be universal features. We find
that the effective field... | [
{
"created": "Wed, 29 Nov 2023 02:34:51 GMT",
"version": "v1"
}
] | 2024-02-06 | [
[
"Erler",
"Theodore",
""
],
[
"Fırat",
"Atakan Hilmi",
""
]
] | We investigate Wilsonian effective field theory as a model for the construction of the tachyon potential and nonperturbative vacua in closed string field theory. In a number of cases we are able to find the effective potential exactly, and observe what appear to be universal features. We find that the effective field t... | 10.268457 | 11.070197 | 10.685722 | 10.101393 | 10.926768 | 10.88686 | 11.170773 | 10.341396 | 9.94428 | 10.849438 | 9.718814 | 9.633748 | 9.939797 | 9.737166 | 9.956923 | 9.565866 | 9.405807 | 9.984113 | 9.802399 | 10.098504 | 9.925646 |
hep-th/0507129 | Juraj Bohacik | Juraj Bohacik and Peter Presnajder | Nonperturbative approach to(Wiener) functional integral with $\phi^4$
interaction | Presented at "Path integrals. From quantum information to cosmology",
8th International conference, Prague, June 6--10, 2005 | null | null | null | hep-th | null | We propose the another, in principe nonperturbative, method of the evaluation
of the Wiener functional integral for $\phi^4$ term in the action. All infinite
summations in the results are proven to be convergent. We finf the
"generalized" Gelfand -- Yaglom differential equation implying the functional
integral in the... | [
{
"created": "Thu, 14 Jul 2005 09:10:07 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Bohacik",
"Juraj",
""
],
[
"Presnajder",
"Peter",
""
]
] | We propose the another, in principe nonperturbative, method of the evaluation of the Wiener functional integral for $\phi^4$ term in the action. All infinite summations in the results are proven to be convergent. We finf the "generalized" Gelfand -- Yaglom differential equation implying the functional integral in the c... | 21.087645 | 25.521574 | 21.332663 | 19.595097 | 18.626936 | 20.24935 | 22.433805 | 20.364695 | 19.574528 | 20.525143 | 19.998877 | 18.91287 | 20.207294 | 18.81605 | 19.114492 | 18.964748 | 19.166639 | 19.960905 | 18.921576 | 20.114445 | 18.882778 |
1704.02530 | Konstantin Stepanyantz | I.L.Buchbinder, E.A.Ivanov, B.S.Merzlikin, K.V.Stepanyantz | Supergraph analysis of the one-loop divergences in $6D$, ${\cal N} =
(1,0)$ and ${\cal N} = (1,1)$ gauge theories | 32 pages, 5 figures | null | 10.1016/j.nuclphysb.2017.05.010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the one-loop effective action for $6D,$ ${\cal N}=(1,0)$
supersymmetric Yang--Mills (SYM) theory with hypermultiplets and $6D,$ ${\cal
N}=(1,1)$ SYM theory as a subclass of the former, using the off-shell
formulation of these theories in $6D,$ ${\cal N}=(1,0)$ harmonic superspace. We
develop the correspondin... | [
{
"created": "Sat, 8 Apr 2017 19:47:22 GMT",
"version": "v1"
}
] | 2017-06-28 | [
[
"Buchbinder",
"I. L.",
""
],
[
"Ivanov",
"E. A.",
""
],
[
"Merzlikin",
"B. S.",
""
],
[
"Stepanyantz",
"K. V.",
""
]
] | We study the one-loop effective action for $6D,$ ${\cal N}=(1,0)$ supersymmetric Yang--Mills (SYM) theory with hypermultiplets and $6D,$ ${\cal N}=(1,1)$ SYM theory as a subclass of the former, using the off-shell formulation of these theories in $6D,$ ${\cal N}=(1,0)$ harmonic superspace. We develop the corresponding ... | 5.460592 | 4.701447 | 6.016347 | 4.92018 | 5.022876 | 4.876336 | 4.790871 | 4.603655 | 4.818767 | 6.433393 | 4.995303 | 4.899575 | 5.544078 | 5.162504 | 5.077432 | 4.980611 | 5.005896 | 5.028954 | 5.008372 | 5.504282 | 5.147305 |
0811.3866 | Jarah Evslin | Jarah Evslin and Ruben Minasian | Topology Change from (Heterotic) Narain T-Duality | 31 pages, 1 figure (xymatrix), typo fixed, ref added | Nucl.Phys.B820:213-236,2009 | 10.1016/j.nuclphysb.2009.05.021 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Narain T-duality on a nontrivially fibered n-torus bundle in the
presence of a topologically nontrivial NS H flux. The action of the duality
group on the topology and H flux of the corresponding type II and heterotic
string backgrounds is determined. The topology change is specialized to the
case of super... | [
{
"created": "Mon, 24 Nov 2008 13:21:36 GMT",
"version": "v1"
},
{
"created": "Sat, 13 Dec 2008 16:47:41 GMT",
"version": "v2"
}
] | 2009-07-22 | [
[
"Evslin",
"Jarah",
""
],
[
"Minasian",
"Ruben",
""
]
] | We consider Narain T-duality on a nontrivially fibered n-torus bundle in the presence of a topologically nontrivial NS H flux. The action of the duality group on the topology and H flux of the corresponding type II and heterotic string backgrounds is determined. The topology change is specialized to the case of supersy... | 9.396788 | 9.344741 | 11.730632 | 9.461359 | 8.763432 | 8.768892 | 8.907225 | 9.197399 | 8.73757 | 11.252126 | 9.081694 | 8.884476 | 9.860892 | 8.927224 | 8.885505 | 8.898756 | 8.854864 | 9.265235 | 9.006502 | 9.695797 | 9.30011 |
hep-th/0406170 | Peng Wang | Peng Wang, Xin-He Meng (Nankai U.) | Codimension Two Branes in Einstein-Gauss-Bonnet Gravity | 16 pages, no figures. v2: References added; v3: Reference added,
Sec.4 and 5 combined into one; v4: References added, minor corrections, to
appear in Physical Review D | Phys.Rev. D71 (2005) 024023 | 10.1103/PhysRevD.71.024023 | null | hep-th | null | Codimension two branes play an interesting role in attacking the cosmological
constant problem. Recently, in order to handle some problems in codimension two
branes in Einstein gravity, Bostock {\it et al.} have proposed using
six-dimensional Einstein-Gauss-Bonnet (EGB) gravity instead of six-dimensional
Einstein gra... | [
{
"created": "Mon, 21 Jun 2004 08:15:01 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Jun 2004 05:30:10 GMT",
"version": "v2"
},
{
"created": "Fri, 30 Jul 2004 07:39:29 GMT",
"version": "v3"
},
{
"created": "Fri, 14 Jan 2005 07:41:45 GMT",
"version": "v4"
}
] | 2009-11-10 | [
[
"Wang",
"Peng",
"",
"Nankai U."
],
[
"Meng",
"Xin-He",
"",
"Nankai U."
]
] | Codimension two branes play an interesting role in attacking the cosmological constant problem. Recently, in order to handle some problems in codimension two branes in Einstein gravity, Bostock {\it et al.} have proposed using six-dimensional Einstein-Gauss-Bonnet (EGB) gravity instead of six-dimensional Einstein gravi... | 6.782314 | 6.133048 | 6.300932 | 6.066193 | 6.696619 | 6.354975 | 6.193853 | 6.41228 | 6.488588 | 6.962863 | 6.098781 | 6.180395 | 6.07246 | 6.129007 | 6.273937 | 6.286283 | 6.226093 | 6.115283 | 5.80085 | 6.20555 | 6.270858 |
hep-th/9703187 | Roger Sollie | I. Brevik, R. Sollie | On the Casimir energy for a 2N-piece relativistic string | 22 pages, LaTeX. To appear in J. Math. Physics, June 1997 | J.Math.Phys.38:2774-2785,1997 | 10.1063/1.532018 | null | hep-th | null | The Casimir energy for the transverse oscillations of a piecewise uniform
closed string is calculated. The string consists of 2N pieces of equal length,
of alternating type I and type II material, and is taken to be relativistic in
the sense that the velocity of sound always equals the velocity of light. By
means of ... | [
{
"created": "Wed, 26 Mar 1997 13:36:36 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Brevik",
"I.",
""
],
[
"Sollie",
"R.",
""
]
] | The Casimir energy for the transverse oscillations of a piecewise uniform closed string is calculated. The string consists of 2N pieces of equal length, of alternating type I and type II material, and is taken to be relativistic in the sense that the velocity of sound always equals the velocity of light. By means of a ... | 10.026108 | 8.715208 | 9.977177 | 8.504091 | 10.238626 | 9.037056 | 9.478036 | 8.546776 | 8.673343 | 11.164281 | 9.007477 | 8.957281 | 9.65965 | 9.198128 | 9.349811 | 9.329885 | 9.331949 | 9.187033 | 9.386944 | 9.597563 | 9.384377 |
hep-th/0509205 | Makoto Sakaguchi | Holger B. Nielsen and Masao Ninomiya | Unification of Cosmology and Second Law of Thermodynamics: Solving
Cosmological Constant Problem, and Inflation | 12 pages, revtex4 | Prog.Theor.Phys.116:851-871,2007 | 10.1143/PTP.116.851 | null | hep-th gr-qc | null | We seek here to unify the second law of thermodynamics with the other laws,
or at least to put up a law behind the second law of thermodynamics. Assuming
no fine tuning, concretely by a random Hamiltonian, we argue just from
equations of motion -- but {\em without} second law -- that entropy cannot go
first up and th... | [
{
"created": "Wed, 28 Sep 2005 02:19:51 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Nielsen",
"Holger B.",
""
],
[
"Ninomiya",
"Masao",
""
]
] | We seek here to unify the second law of thermodynamics with the other laws, or at least to put up a law behind the second law of thermodynamics. Assuming no fine tuning, concretely by a random Hamiltonian, we argue just from equations of motion -- but {\em without} second law -- that entropy cannot go first up and then... | 18.293228 | 20.906229 | 20.371746 | 18.661798 | 20.246023 | 21.562229 | 20.868338 | 20.232403 | 18.978096 | 19.904869 | 18.553751 | 18.318592 | 18.351492 | 18.029556 | 18.245844 | 18.066181 | 18.6637 | 18.321655 | 17.956472 | 18.259586 | 17.974634 |
2107.04881 | Khai Ming Wong | Dan Zhu, Khai-Ming Wong and Guo-Quan Wong | Oscillating monopole-antimonopole pair in the Weinberg-Salam model | A corrected, rewritten and up-to-date version is separately submitted
to arXiv:2207.06768 | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate further the properties of axially symmetrical
monopole-antimonopole pair in the standard Weinberg-Salam theory. These
numerical solutions behave quite differently from their counterparts in the
SU(2) Yang-Mills-Higgs theory as the poles are now bounded by a flux string.
Our results confirm that the ene... | [
{
"created": "Sat, 10 Jul 2021 17:56:52 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Jul 2022 08:37:12 GMT",
"version": "v2"
}
] | 2022-07-18 | [
[
"Zhu",
"Dan",
""
],
[
"Wong",
"Khai-Ming",
""
],
[
"Wong",
"Guo-Quan",
""
]
] | We investigate further the properties of axially symmetrical monopole-antimonopole pair in the standard Weinberg-Salam theory. These numerical solutions behave quite differently from their counterparts in the SU(2) Yang-Mills-Higgs theory as the poles are now bounded by a flux string. Our results confirm that the energ... | 9.480926 | 9.46642 | 10.187384 | 8.888976 | 9.87867 | 9.035852 | 9.460882 | 9.153363 | 8.802774 | 10.563664 | 8.687664 | 9.155437 | 9.348609 | 9.106098 | 9.006889 | 8.733763 | 8.822058 | 9.22202 | 8.928595 | 9.105593 | 8.994775 |
hep-th/0401139 | Kentaro Hori | Kentaro Hori | Boundary RG Flows of N=2 Minimal Models | 29 pages | null | null | null | hep-th | null | We study boundary renormalization group flows of N=2 minimal models using
Landau-Ginzburg description of B-type. A simple algebraic relation of matrices
is relevant. We determine the pattern of the flows and identify the operators
that generate them. As an application, we show that the charge lattice of
B-branes in t... | [
{
"created": "Wed, 21 Jan 2004 18:35:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Hori",
"Kentaro",
""
]
] | We study boundary renormalization group flows of N=2 minimal models using Landau-Ginzburg description of B-type. A simple algebraic relation of matrices is relevant. We determine the pattern of the flows and identify the operators that generate them. As an application, we show that the charge lattice of B-branes in the... | 12.50166 | 12.230169 | 15.227776 | 13.186264 | 12.632345 | 12.704942 | 14.048969 | 11.741905 | 10.991667 | 15.405925 | 12.054816 | 12.540899 | 14.256484 | 11.915365 | 12.067219 | 12.49254 | 12.431199 | 12.642906 | 12.04324 | 14.089403 | 12.261339 |
1710.01046 | Ugo Bruzzo | Ugo Bruzzo and Anna Fino and Pietro Fr\'e | The K\"ahler Quotient Resolution of $\mathbb{C}^3/\Gamma$ singularities,
the McKay correspondence and D=3 $\mathcal{N}=2$ Chern-Simons gauge theories | 120 pages, 7 figures. v2: 121 pages, a few minor changes. v3:
references added. v4: 122 pages, 9 figures, minor changes in the
presentation. Final version to be published in Commun. Math. Phys | Commun. Math. Phys. 365 (2019) 93-214 | 10.1007/s00220-018-3203-z | ARC-17-6 | hep-th math-ph math.AG math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We advocate that a generalized Kronheimer construction of the K\"ahler
quotient crepant resolution $\mathcal{M}_\zeta \longrightarrow
\mathbb{C}^3/\Gamma$ of an orbifold singularity where $\Gamma\subset
\mathrm{SU(3)}$ is a finite subgroup naturally defines the field content and
interaction structure of a superconfor... | [
{
"created": "Tue, 3 Oct 2017 09:24:33 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Nov 2017 13:31:43 GMT",
"version": "v2"
},
{
"created": "Mon, 27 Nov 2017 17:24:26 GMT",
"version": "v3"
},
{
"created": "Sun, 20 May 2018 08:43:40 GMT",
"version": "v4"
}
] | 2019-01-23 | [
[
"Bruzzo",
"Ugo",
""
],
[
"Fino",
"Anna",
""
],
[
"Fré",
"Pietro",
""
]
] | We advocate that a generalized Kronheimer construction of the K\"ahler quotient crepant resolution $\mathcal{M}_\zeta \longrightarrow \mathbb{C}^3/\Gamma$ of an orbifold singularity where $\Gamma\subset \mathrm{SU(3)}$ is a finite subgroup naturally defines the field content and interaction structure of a superconforma... | 7.864732 | 8.558135 | 8.926251 | 7.811774 | 8.111196 | 8.163841 | 7.937918 | 7.837457 | 7.819073 | 9.285011 | 7.762328 | 7.609609 | 7.78547 | 7.59276 | 7.664079 | 7.603499 | 7.748533 | 7.646767 | 7.553327 | 7.720325 | 7.5407 |
hep-th/0409019 | Jianxin Lu | J. X. Lu and S. Roy | Delocalized, non-SUSY $p$-branes, tachyon condensation and tachyon
matter | 15 pages, typos corrected | JHEP0411:008,2004 | 10.1088/1126-6708/2004/11/008 | USTC-ICTS-04-20, MCTP-04-52 | hep-th | null | We construct non-supersymmetric $p$-brane solutions of type II supergravities
in arbitrary dimensions ($d$) delocalized in one of the spatial transverse
directions. By a Wick rotation we convert these solutions into Euclidean
$p$-branes delocalized in the transverse time-like direction. The former
solutions in $d=10$... | [
{
"created": "Thu, 2 Sep 2004 02:00:57 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Sep 2004 16:29:12 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Lu",
"J. X.",
""
],
[
"Roy",
"S.",
""
]
] | We construct non-supersymmetric $p$-brane solutions of type II supergravities in arbitrary dimensions ($d$) delocalized in one of the spatial transverse directions. By a Wick rotation we convert these solutions into Euclidean $p$-branes delocalized in the transverse time-like direction. The former solutions in $d=10$ n... | 4.674407 | 4.401704 | 5.183776 | 4.226858 | 4.671072 | 4.127892 | 4.294085 | 4.225257 | 4.240759 | 5.223306 | 4.223819 | 4.525348 | 4.883704 | 4.473847 | 4.458947 | 4.463571 | 4.500899 | 4.504346 | 4.514709 | 4.884456 | 4.365397 |
hep-th/9310110 | null | H.M. Babujian and R. Flume | Off-Shell Bethe Ansatz Equation for Gaudin Magnets and Solutions of
Knizhnik-Zamolodchikov Equations | 10 pages (LaTeX), BONN-HE-93-30, YPI 1407 (18)-93 | Mod.Phys.Lett. A9 (1994) 2029-2040 | 10.1142/S0217732394001891 | null | hep-th | null | We generalize the previously established connection between the off-shell
Bethe ansatz equation for inhomogeneous SU(2) lattice vertex models in the
quasiclassical limit and the solutions of the SU(2) Knizhnik-Zamolodchikov
equations to the case of arbitrary simple Lie algebras.
| [
{
"created": "Mon, 18 Oct 1993 15:33:12 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Babujian",
"H. M.",
""
],
[
"Flume",
"R.",
""
]
] | We generalize the previously established connection between the off-shell Bethe ansatz equation for inhomogeneous SU(2) lattice vertex models in the quasiclassical limit and the solutions of the SU(2) Knizhnik-Zamolodchikov equations to the case of arbitrary simple Lie algebras. | 5.807708 | 4.848228 | 7.267979 | 5.162221 | 4.720422 | 5.224609 | 4.446487 | 4.757288 | 4.717208 | 6.942471 | 5.007683 | 5.17561 | 6.441549 | 5.269564 | 5.181058 | 5.313191 | 5.353855 | 5.132357 | 5.416692 | 6.119002 | 5.279413 |
hep-th/0702215 | Andjelo Samsarov | Sasa Kresic-Juric, Stjepan Meljanac, Marko Stojic | Covariant realizations of kappa-deformed space | 31 pages, no figures, LaTeX | Eur.Phys.J.C51:229-240,2007 | 10.1140/epjc/s10052-007-0285-8 | null | hep-th | null | We study a Lie algebra type $\kappa$-deformed space with undeformed rotation
algebra and commutative vector-like Dirac derivatives in a covariant way. Space
deformation depends on an arbitrary vector. Infinitely many covariant
realizations in terms of commuting coordinates of undeformed space and their
derivatives ar... | [
{
"created": "Tue, 27 Feb 2007 19:12:57 GMT",
"version": "v1"
},
{
"created": "Thu, 29 May 2008 15:44:43 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Kresic-Juric",
"Sasa",
""
],
[
"Meljanac",
"Stjepan",
""
],
[
"Stojic",
"Marko",
""
]
] | We study a Lie algebra type $\kappa$-deformed space with undeformed rotation algebra and commutative vector-like Dirac derivatives in a covariant way. Space deformation depends on an arbitrary vector. Infinitely many covariant realizations in terms of commuting coordinates of undeformed space and their derivatives are ... | 17.87365 | 15.037349 | 17.722528 | 14.943402 | 15.983918 | 16.762161 | 17.588791 | 14.838563 | 14.211403 | 18.368608 | 15.054861 | 15.047902 | 17.211554 | 15.497653 | 15.642912 | 16.259548 | 16.471462 | 16.091764 | 15.963368 | 16.766661 | 15.148146 |
2312.05298 | Adrien Florio | Adrien Florio | Two-fermion negativity and confinement in the Schwinger model | 6 pages 6 figures | null | null | null | hep-th cond-mat.str-el hep-lat hep-ph quant-ph | http://creativecommons.org/licenses/by/4.0/ | We consider the fermionic (logarithmic) negativity between two fermionic
modes in the Schwinger model. Recent results pointed out that fermionic systems
can exhibit stronger entanglement than bosonic systems, exhibiting a negativity
that decays only algebraically. The Schwinger model is described by fermionic
excitat... | [
{
"created": "Fri, 8 Dec 2023 19:00:00 GMT",
"version": "v1"
}
] | 2023-12-12 | [
[
"Florio",
"Adrien",
""
]
] | We consider the fermionic (logarithmic) negativity between two fermionic modes in the Schwinger model. Recent results pointed out that fermionic systems can exhibit stronger entanglement than bosonic systems, exhibiting a negativity that decays only algebraically. The Schwinger model is described by fermionic excitatio... | 8.051423 | 8.587087 | 8.876021 | 8.56874 | 9.173967 | 9.943151 | 9.592779 | 9.163013 | 8.953062 | 9.485974 | 8.416848 | 7.879435 | 7.859616 | 7.883204 | 7.995759 | 7.726786 | 8.131869 | 8.37055 | 7.922664 | 7.7032 | 7.772897 |
1111.0872 | Mariano Chernicoff | Mariano Chernicoff, J. Antonio Garcia, Alberto Guijosa and Juan F.
Pedraza | Holographic Lessons for Quark Dynamics | Invited review for a Journal of Physics G topical volume on
gauge/gravity duality applications to QCD matter and ultrarelativistic
heavy-ion collisions. v2: Reference added | J.Phys.G G39, 054002 (2012) | 10.1088/0954-3899/39/5/054002 | UTTG-22-11; TCC-024-11 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give a brief overview of recent results obtained through the gauge/gravity
correspondence, concerning the propagation of a heavy quark in strongly-coupled
conformal field theories (such as N=4 super-Yang-Mills), both at zero and
finite temperature. In the vacuum, we discuss energy loss, radiation damping,
signal p... | [
{
"created": "Thu, 3 Nov 2011 15:14:00 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Nov 2011 10:36:16 GMT",
"version": "v2"
}
] | 2012-09-24 | [
[
"Chernicoff",
"Mariano",
""
],
[
"Garcia",
"J. Antonio",
""
],
[
"Guijosa",
"Alberto",
""
],
[
"Pedraza",
"Juan F.",
""
]
] | We give a brief overview of recent results obtained through the gauge/gravity correspondence, concerning the propagation of a heavy quark in strongly-coupled conformal field theories (such as N=4 super-Yang-Mills), both at zero and finite temperature. In the vacuum, we discuss energy loss, radiation damping, signal pro... | 8.947625 | 8.57921 | 10.606948 | 8.180966 | 8.021484 | 8.203918 | 7.752285 | 7.419492 | 8.773765 | 10.11079 | 7.997811 | 8.525927 | 9.570339 | 8.747303 | 8.891237 | 8.732142 | 9.079464 | 8.529328 | 8.918285 | 9.687457 | 8.426448 |
hep-th/0411147 | Xavier Calmet | Xavier Calmet | Space-Time Symmetries of Noncommutative Spaces | 7 pages, v2: typos corrected, to appear in Phys. Rev. D | Phys.Rev. D71 (2005) 085012 | 10.1103/PhysRevD.71.085012 | null | hep-th hep-ph math-ph math.MP | null | We define a noncommutative Lorentz symmetry for canonical noncommutative
spaces. The noncommutative vector fields and the derivatives transform under a
deformed Lorentz transformation. We show that the star product is invariant
under noncommutative Lorentz transformations. We then apply our idea to the
case of action... | [
{
"created": "Mon, 15 Nov 2004 19:56:56 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Apr 2005 20:52:37 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Calmet",
"Xavier",
""
]
] | We define a noncommutative Lorentz symmetry for canonical noncommutative spaces. The noncommutative vector fields and the derivatives transform under a deformed Lorentz transformation. We show that the star product is invariant under noncommutative Lorentz transformations. We then apply our idea to the case of actions ... | 8.08259 | 7.489854 | 8.081684 | 6.883462 | 7.772289 | 7.178467 | 6.963562 | 6.969946 | 7.459132 | 8.549873 | 6.867002 | 7.2408 | 7.843862 | 7.357692 | 7.429376 | 7.297348 | 7.45163 | 7.324318 | 7.596564 | 7.817375 | 7.06453 |
hep-th/0411058 | Philippe Brax | Ph. Brax, N. Chatillon and D. A. Steer | Effective actions of a Gauss-Bonnet brane world with brane curvature
terms | 14 pages | Phys.Lett. B608 (2005) 130-141 | 10.1016/j.physletb.2004.12.034 | null | hep-th | null | We consider a warped brane world scenario with two branes, Gauss-Bonnet
gravity in the bulk, and brane localised curvature terms. When matter is
present on both branes, we investigate the linear equations of motion and
distinguish three regimes. At very high energy and for an observer on the
positive tension brane, g... | [
{
"created": "Thu, 4 Nov 2004 17:29:45 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Brax",
"Ph.",
""
],
[
"Chatillon",
"N.",
""
],
[
"Steer",
"D. A.",
""
]
] | We consider a warped brane world scenario with two branes, Gauss-Bonnet gravity in the bulk, and brane localised curvature terms. When matter is present on both branes, we investigate the linear equations of motion and distinguish three regimes. At very high energy and for an observer on the positive tension brane, gra... | 7.704933 | 8.088779 | 8.537218 | 7.421767 | 7.870721 | 8.172674 | 7.603169 | 7.852309 | 7.010026 | 8.319057 | 7.540373 | 7.649294 | 7.923665 | 7.599119 | 7.456729 | 7.702296 | 7.45162 | 7.336049 | 7.270177 | 7.706242 | 7.602196 |
hep-th/9703142 | Boris Rusakov | B.Rusakov (Oxford University) | Exactly Soluble QCD and Confinement of Quarks | 12 pages, LaTeX (substantial revision and reorganization of the text;
the emphasis redirected to the physics of the approach; no change in the
resulting model and conclusion) | Nucl.Phys. B507 (1997) 691-706 | 10.1016/S0550-3213(97)00604-4 | OUTP-97-13P | hep-th hep-lat hep-ph | null | An exactly soluble non-perturbative model of the pure gauge QCD is derived as
a weak coupling limit of the lattice theory in plaquette formulation. The model
represents QCD as a theory of the weakly interacting field strength fluxes. The
area law behavior of the Wilson loop average is a direct result of this
represen... | [
{
"created": "Thu, 20 Mar 1997 15:45:29 GMT",
"version": "v1"
},
{
"created": "Mon, 24 Mar 1997 14:36:08 GMT",
"version": "v2"
},
{
"created": "Sun, 13 Apr 1997 20:39:22 GMT",
"version": "v3"
},
{
"created": "Fri, 18 Jul 1997 12:37:59 GMT",
"version": "v4"
}
] | 2009-10-30 | [
[
"Rusakov",
"B.",
"",
"Oxford University"
]
] | An exactly soluble non-perturbative model of the pure gauge QCD is derived as a weak coupling limit of the lattice theory in plaquette formulation. The model represents QCD as a theory of the weakly interacting field strength fluxes. The area law behavior of the Wilson loop average is a direct result of this representa... | 9.382694 | 9.466081 | 9.766041 | 8.30019 | 9.612519 | 8.44191 | 10.053278 | 9.820485 | 9.397827 | 10.083591 | 9.1717 | 8.77688 | 9.308282 | 9.056905 | 8.805001 | 8.919707 | 9.161067 | 8.460812 | 8.781635 | 9.600179 | 8.938254 |
hep-th/0312186 | Claudio Dappiaggi | Giovanni Arcioni, Claudio Dappiaggi | Holography in asymptotically flat space-times and the BMS group | 31 pages, several changes in section 3 and 7 and references updated | Class.Quant.Grav.21:5655,2004 | 10.1088/0264-9381/21/23/022 | RI-12-03, FNT/T 2003/15 | hep-th gr-qc math-ph math.MP | null | In a previous paper (hep-th/0306142) we have started to explore the
holographic principle in the case of asymptotically flat space-times and
analyzed in particular different aspects of the Bondi-Metzner-Sachs (BMS)
group, namely the asymptotic symmetry group of any asymptotically flat
space-time. We continue this inv... | [
{
"created": "Tue, 16 Dec 2003 15:04:04 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Nov 2004 15:27:01 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Arcioni",
"Giovanni",
""
],
[
"Dappiaggi",
"Claudio",
""
]
] | In a previous paper (hep-th/0306142) we have started to explore the holographic principle in the case of asymptotically flat space-times and analyzed in particular different aspects of the Bondi-Metzner-Sachs (BMS) group, namely the asymptotic symmetry group of any asymptotically flat space-time. We continue this inves... | 9.618769 | 9.422314 | 10.154119 | 9.040135 | 9.339164 | 9.095388 | 10.625601 | 9.374945 | 9.555956 | 10.836176 | 9.119056 | 9.2792 | 9.422441 | 9.086536 | 9.301733 | 9.065488 | 9.384525 | 8.977404 | 9.23201 | 9.307625 | 9.164972 |
hep-th/9910153 | Christian Rupp | Christian Rupp | Conformal Transformation Properties of the B-type Supercurrent | 37 pages, AMSLaTeX, needs font rsfs and style mathrsfs | null | null | NTZ 23/1999 | hep-th | null | We investigate the superconformal transformation properties of the
supercurrent as well as of the superconformal anomalies themselves in d=4, N=1
supersymmetric quantum field theory. Matter supercurrent and anomalies are
coupled to a classical background of minimal supergravity fields. On flat
superspace, there exist... | [
{
"created": "Tue, 19 Oct 1999 13:18:20 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rupp",
"Christian",
""
]
] | We investigate the superconformal transformation properties of the supercurrent as well as of the superconformal anomalies themselves in d=4, N=1 supersymmetric quantum field theory. Matter supercurrent and anomalies are coupled to a classical background of minimal supergravity fields. On flat superspace, there exist t... | 11.037281 | 11.358659 | 12.604999 | 10.696394 | 12.470954 | 12.10908 | 10.571026 | 11.052829 | 10.289946 | 14.21376 | 10.439847 | 10.592562 | 10.511836 | 10.594667 | 11.049541 | 10.625894 | 10.532247 | 10.70402 | 10.474162 | 10.643834 | 10.359161 |
1809.08228 | Daniel Schubring | Daniel Schubring and Mikhail Shifman | Interpolating Between $CP(N-1)$ and $S^{2N-1}$ Target Spaces | 35 pages, 1 figure | Phys. Rev. D 101, 045003 (2020) | 10.1103/PhysRevD.101.045003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Some magnetic phenomena in correlated electron systems were recently shown to
be described in the continuum limit by a class of sigma models which present a
U(1) Hopf fibration over CP(1). In this paper we study a generalization of such
models with a target space given by a U(1) fibration over Grassmannian
manifolds,... | [
{
"created": "Fri, 21 Sep 2018 17:52:19 GMT",
"version": "v1"
},
{
"created": "Thu, 31 Jan 2019 19:37:22 GMT",
"version": "v2"
}
] | 2020-02-12 | [
[
"Schubring",
"Daniel",
""
],
[
"Shifman",
"Mikhail",
""
]
] | Some magnetic phenomena in correlated electron systems were recently shown to be described in the continuum limit by a class of sigma models which present a U(1) Hopf fibration over CP(1). In this paper we study a generalization of such models with a target space given by a U(1) fibration over Grassmannian manifolds, o... | 8.691843 | 8.384266 | 9.533746 | 8.404664 | 8.706676 | 9.242183 | 8.979074 | 8.563687 | 8.394919 | 9.276384 | 8.126999 | 8.546914 | 8.928238 | 8.507384 | 8.383372 | 8.386682 | 8.183705 | 8.360371 | 8.321892 | 9.044267 | 8.143932 |
hep-th/0303098 | Tekin Dereli | A.H.Bilge (Istanbul Tech U), T.Dereli (Koc U), S.Kocak (Anadolu U) | Seiberg-Witten type monopole equations on 8-manifolds with Spin(7)
holonomy as minimizers of a quadratic action | 18 pages, LATEX file, no figures | JHEP 0304 (2003) 003 | 10.1088/1126-6708/2003/04/003 | null | hep-th | null | We obtain an elliptic system of monopole equations on 8-manifolds with
Spin(7) holonomy by minimizing an action involving negative spinors coupled to
an Abelian gauge fields.
| [
{
"created": "Tue, 11 Mar 2003 16:04:17 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Bilge",
"A. H.",
"",
"Istanbul Tech U"
],
[
"Dereli",
"T.",
"",
"Koc U"
],
[
"Kocak",
"S.",
"",
"Anadolu U"
]
] | We obtain an elliptic system of monopole equations on 8-manifolds with Spin(7) holonomy by minimizing an action involving negative spinors coupled to an Abelian gauge fields. | 15.149175 | 11.972837 | 19.337702 | 13.987534 | 12.981642 | 14.203734 | 13.857316 | 13.384944 | 10.988241 | 21.421936 | 11.484307 | 11.885957 | 13.562338 | 14.242908 | 12.914726 | 13.192905 | 12.642228 | 13.22568 | 14.188777 | 12.721709 | 12.029769 |
1205.2953 | Rafael Sorkin | Rafael D. Sorkin | Expressing entropy globally in terms of (4D) field-correlations | plainTeX, 14 pages, 2 figures. To appear in proceedings of ICGC2011,
held Goa, Journal of Physics Conference Series. Most current version is
available at http://www.perimeterinstitute.ca/personal/rsorkin/some.papers/
(or wherever my home-page may be, such as
http://www.physics.syr.edu/~sorkin/some.papers/) | null | null | null | hep-th gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We express the entropy of a scalar field phi directly in terms of its
spacetime correlation function W(x,y) = <phi(x) phi(y)>, assuming that the
higher correlators are of "Gaussian" form. The resulting formula associates an
entropy S(R) to any spacetime region R; and when R is globally hyperbolic with
Cauchy surface ... | [
{
"created": "Mon, 14 May 2012 07:40:07 GMT",
"version": "v1"
}
] | 2012-05-15 | [
[
"Sorkin",
"Rafael D.",
""
]
] | We express the entropy of a scalar field phi directly in terms of its spacetime correlation function W(x,y) = <phi(x) phi(y)>, assuming that the higher correlators are of "Gaussian" form. The resulting formula associates an entropy S(R) to any spacetime region R; and when R is globally hyperbolic with Cauchy surface Si... | 8.533559 | 8.821949 | 8.462589 | 8.362647 | 8.581433 | 8.738895 | 8.381953 | 9.22839 | 8.535472 | 8.438486 | 8.939358 | 8.492568 | 8.069347 | 8.377997 | 8.256181 | 8.009218 | 8.389825 | 8.135047 | 7.973362 | 8.613588 | 8.372173 |
hep-th/0605196 | Steven B. Giddings | Steven B. Giddings | Black hole information, unitarity, and nonlocality | 34 pages, 4 figures. Major revision of hep-th/0604047. v2: minor
corrections and added reference | Phys.Rev.D74:106005,2006 | 10.1103/PhysRevD.74.106005 | null | hep-th gr-qc | null | The black hole information paradox apparently indicates the need for a
fundamentally new ingredient in physics. The leading contender is nonlocality.
Possible mechanisms for the nonlocality needed to restore unitarity to black
hole evolution are investigated. Suggestions that such dynamics arises from
ultra-planckian... | [
{
"created": "Fri, 19 May 2006 19:12:21 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Jun 2006 04:25:14 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Giddings",
"Steven B.",
""
]
] | The black hole information paradox apparently indicates the need for a fundamentally new ingredient in physics. The leading contender is nonlocality. Possible mechanisms for the nonlocality needed to restore unitarity to black hole evolution are investigated. Suggestions that such dynamics arises from ultra-planckian m... | 18.334948 | 19.233234 | 19.424101 | 18.32996 | 19.547678 | 20.272465 | 18.799728 | 17.774967 | 18.198267 | 21.032862 | 18.164103 | 17.398003 | 18.774643 | 17.288212 | 17.897038 | 17.48242 | 17.875601 | 18.070339 | 17.679926 | 18.554728 | 17.568632 |
0903.0281 | Daniele Bettinelli | Daniele Bettinelli, Ruggero Ferrari, Andrea Quadri | One-loop Self-energies in the Electroweak Model with Nonlinearly
Realized Gauge Group | 29 pages, final version published by Phys. Rev. D, some typos
corrected in eqs.(5), (18) and (19). The errors have a pure editing origin.
Therefore they do not affect the content of the paper | Phys.Rev.D79:125028,2009 | 10.1103/PhysRevD.79.125028 | MIT-CTP-4015, IFUM-937-FT | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We evaluate at one loop the self-energies in generic D dimensions for the W,Z
mesons in the Electroweak model where the gauge group is nonlinearly realized.
In this model the Higgs boson parameters are absent, while a second mass
parameter appears together with a scale for the radiative corrections. We
estimate these... | [
{
"created": "Mon, 2 Mar 2009 12:43:37 GMT",
"version": "v1"
},
{
"created": "Fri, 19 Nov 2010 14:00:39 GMT",
"version": "v2"
}
] | 2010-11-22 | [
[
"Bettinelli",
"Daniele",
""
],
[
"Ferrari",
"Ruggero",
""
],
[
"Quadri",
"Andrea",
""
]
] | We evaluate at one loop the self-energies in generic D dimensions for the W,Z mesons in the Electroweak model where the gauge group is nonlinearly realized. In this model the Higgs boson parameters are absent, while a second mass parameter appears together with a scale for the radiative corrections. We estimate these p... | 17.493111 | 15.515306 | 15.151211 | 15.030062 | 16.250937 | 16.700083 | 15.494124 | 15.601286 | 16.042458 | 16.389942 | 15.026464 | 16.215979 | 14.756396 | 14.463818 | 15.065055 | 16.477692 | 14.953474 | 15.420253 | 14.960061 | 15.379851 | 15.330618 |
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