id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9510217 | Giuseppe Bimonte | A.P. Balachandran, G. Bimonte, E. Ercolessi, G. Landi, F. Lizzi, G.
Sparano and P. Teotonio-Sobrinho | Noncommutative Lattices as Finite Approximations and Their
Noncommutative Geometries | 37 pages, 12 eps figures, uses psbox.tex To appear in J. Geom. and
Physics, a problem due to the mailer hopefully solved | J.Geom.Phys. 18 (1996) 163-194 | 10.1016/0393-0440(95)00006-2 | IC/94/80 | hep-th | null | Lattice discretizations of continuous manifolds are common tools used in a
variety of physical contexts. Conventional discrete approximations, however,
cannot capture all aspects of the original manifold, notably its topology. In
this paper we discuss an approximation scheme due to Sorkin which correctly
reproduces i... | [
{
"created": "Mon, 30 Oct 1995 12:30:09 GMT",
"version": "v1"
},
{
"created": "Tue, 31 Oct 1995 18:41:52 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Balachandran",
"A. P.",
""
],
[
"Bimonte",
"G.",
""
],
[
"Ercolessi",
"E.",
""
],
[
"Landi",
"G.",
""
],
[
"Lizzi",
"F.",
""
],
[
"Sparano",
"G.",
""
],
[
"Teotonio-Sobrinho",
"P.",
""
]
] | Lattice discretizations of continuous manifolds are common tools used in a variety of physical contexts. Conventional discrete approximations, however, cannot capture all aspects of the original manifold, notably its topology. In this paper we discuss an approximation scheme due to Sorkin which correctly reproduces imp... | 9.302471 | 8.60059 | 9.267586 | 8.301312 | 9.971012 | 9.863335 | 9.443838 | 8.465909 | 8.293758 | 10.465294 | 8.979598 | 8.478303 | 8.78037 | 8.664371 | 8.527055 | 8.605469 | 8.798152 | 8.515924 | 8.672132 | 9.235341 | 8.911097 |
1202.1290 | Alessio Marrani | Sergio Ferrara, Renata Kallosh, Alessio Marrani | Degeneration of Groups of Type E7 and Minimal Coupling in Supergravity | 1+40 pages, 5 Tables; v2 : 1+41 pages, Sec. 3 extended, Sec. 3.1
replaced, Sec. 4.3 removed, one Ref. added, other minor changes | null | 10.1007/JHEP06(2012)074 | CERN-PH-TH/2012-026; SU-ITP-2012-06 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study properties of D = 4, N >1 extended supergravities (and related
compactifications of superstring theory) and their consistent truncation to the
phenomenologically interesting models of N = 1 supergravity. This involves a
detailed classification of the "degenerations" of the duality groups of type
E7, when the... | [
{
"created": "Mon, 6 Feb 2012 21:06:24 GMT",
"version": "v1"
},
{
"created": "Tue, 5 Jun 2012 18:34:07 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Ferrara",
"Sergio",
""
],
[
"Kallosh",
"Renata",
""
],
[
"Marrani",
"Alessio",
""
]
] | We study properties of D = 4, N >1 extended supergravities (and related compactifications of superstring theory) and their consistent truncation to the phenomenologically interesting models of N = 1 supergravity. This involves a detailed classification of the "degenerations" of the duality groups of type E7, when the c... | 15.142118 | 14.189457 | 15.62416 | 14.843354 | 13.961812 | 14.703938 | 14.272833 | 13.740118 | 13.946677 | 16.434494 | 13.774764 | 14.013056 | 14.792153 | 13.91822 | 14.206833 | 14.344982 | 14.021107 | 14.319341 | 13.83275 | 14.285106 | 14.01225 |
hep-th/0002070 | Miguel Vazquez Mozo | A. Feinstein, K.E. Kunze and M.A. Vazquez-Mozo | Initial Conditions and the Structure of the Singularity in Pre-Big-Bang
Cosmology | 18 pages, LaTeX, epsfig. 3 figures included. Minor changes; paragraph
added in the introduction, references added and typos corrected. Final
version published in Classical and Quantum Gravity | Class.Quant.Grav.17:3599-3616,2000 | 10.1088/0264-9381/17/18/301 | EHU-FT/0001, ITFA-00-03, SPIN-2000/02 | hep-th astro-ph gr-qc | null | We propose a picture, within the pre-big-bang approach, in which the universe
emerges from a bath of plane gravitational and dilatonic waves. The waves
interact gravitationally breaking the exact plane symmetry and lead generically
to gravitational collapse resulting in a singularity with the Kasner-like
structure. T... | [
{
"created": "Wed, 9 Feb 2000 18:16:49 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Sep 2000 10:07:07 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Feinstein",
"A.",
""
],
[
"Kunze",
"K. E.",
""
],
[
"Vazquez-Mozo",
"M. A.",
""
]
] | We propose a picture, within the pre-big-bang approach, in which the universe emerges from a bath of plane gravitational and dilatonic waves. The waves interact gravitationally breaking the exact plane symmetry and lead generically to gravitational collapse resulting in a singularity with the Kasner-like structure. The... | 11.7262 | 13.055099 | 11.569526 | 11.171198 | 12.558242 | 12.532948 | 13.041436 | 11.21417 | 11.861327 | 12.871039 | 11.539411 | 10.74783 | 10.546615 | 10.617876 | 10.449265 | 10.485984 | 10.936487 | 10.510227 | 11.126693 | 10.820541 | 10.855249 |
2301.08261 | Cesar D\'iaz | Daniel \'Avila, C\'esar D\'iaz, Leonardo Pati\~no | Complexity of Magnetization and Magnetic Simplification | 17 pages, 15 figures. Published version, updated figures 4,6,12 and
some extra comments about these were added | Avila, D., D\'iaz, C., & Pati\~no, L. (2023). Complexity of
magnetization and magnetic simplification. Phys. Rev. D, 107, 106003 | 10.1103/PhysRevD.107.106003 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the complexity=volume (CV) prescription to study the effect of a
magnetic field on the computational complexity for states in the gauge theories
dual to two different gravitational models. In one of these theories the
complexity increases with the intensity of the magnetic field, while in the
other a more inte... | [
{
"created": "Thu, 19 Jan 2023 19:00:03 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Jul 2023 17:05:18 GMT",
"version": "v2"
}
] | 2023-07-27 | [
[
"Ávila",
"Daniel",
""
],
[
"Díaz",
"César",
""
],
[
"Patiño",
"Leonardo",
""
]
] | We use the complexity=volume (CV) prescription to study the effect of a magnetic field on the computational complexity for states in the gauge theories dual to two different gravitational models. In one of these theories the complexity increases with the intensity of the magnetic field, while in the other a more intere... | 13.471131 | 12.198578 | 13.331735 | 11.251781 | 11.211349 | 11.868046 | 11.40433 | 10.894083 | 10.932215 | 13.936805 | 10.859417 | 10.878093 | 12.055305 | 10.617152 | 10.732991 | 10.764935 | 10.777574 | 10.61893 | 10.972806 | 12.036901 | 10.773714 |
1103.5745 | Kurt Hinterbichler | Garrett Goon, Kurt Hinterbichler, Mark Trodden | Symmetries for Galileons and DBI scalars on curved space | 52 pages, 3 figures | JCAP 07 (2011) 017 | 10.1088/1475-7516/2011/07/017 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a general class of four-dimensional effective field theories
which include curved space Galileons and DBI theories possessing nonlinear
shift-like symmetries. These effective theories arise from purely gravitational
actions for 3-branes probing higher dimensional spaces. In the simplest case of
a Minkows... | [
{
"created": "Tue, 29 Mar 2011 20:00:00 GMT",
"version": "v1"
}
] | 2011-07-20 | [
[
"Goon",
"Garrett",
""
],
[
"Hinterbichler",
"Kurt",
""
],
[
"Trodden",
"Mark",
""
]
] | We introduce a general class of four-dimensional effective field theories which include curved space Galileons and DBI theories possessing nonlinear shift-like symmetries. These effective theories arise from purely gravitational actions for 3-branes probing higher dimensional spaces. In the simplest case of a Minkowski... | 8.162595 | 7.00953 | 8.471284 | 7.353709 | 8.053823 | 8.001822 | 7.559958 | 7.90745 | 7.501452 | 8.895905 | 7.222024 | 7.497033 | 8.041059 | 7.573871 | 7.868678 | 7.692676 | 7.629405 | 7.751602 | 7.592011 | 7.97787 | 7.523815 |
1910.14224 | Jacob Bourjaily | Jacob L. Bourjaily, Andrew J. McLeod, Cristian Vergu, Matthias Volk,
Matt von Hippel, Matthias Wilhelm | Rooting Out Letters: Octagonal Symbol Alphabets and Algebraic Number
Theory | 25 pages, 4 figures; detailed results available as ancillary files | JHEP 02 (2020) 025 | 10.1007/JHEP02(2020)025 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is widely expected that NMHV amplitudes in planar, maximally
supersymmetric Yang-Mills theory require symbol letters that are not rationally
expressible in terms of momentum-twistor (or cluster) variables starting at two
loops for eight particles. Recent advances in loop integration technology have
made this an `e... | [
{
"created": "Thu, 31 Oct 2019 02:40:06 GMT",
"version": "v1"
}
] | 2022-08-24 | [
[
"Bourjaily",
"Jacob L.",
""
],
[
"McLeod",
"Andrew J.",
""
],
[
"Vergu",
"Cristian",
""
],
[
"Volk",
"Matthias",
""
],
[
"von Hippel",
"Matt",
""
],
[
"Wilhelm",
"Matthias",
""
]
] | It is widely expected that NMHV amplitudes in planar, maximally supersymmetric Yang-Mills theory require symbol letters that are not rationally expressible in terms of momentum-twistor (or cluster) variables starting at two loops for eight particles. Recent advances in loop integration technology have made this an `exp... | 17.455923 | 19.278551 | 19.116425 | 16.529982 | 18.869362 | 18.877625 | 17.998047 | 16.974934 | 17.145489 | 19.440441 | 15.63459 | 15.754234 | 17.155081 | 16.573994 | 16.965176 | 16.50889 | 16.649572 | 16.831007 | 16.180595 | 17.12007 | 16.959003 |
0911.0266 | Hideki Ishihara | Takahisa Igata and Hideki Ishihara | Toroidal Spiral Nambu-Goto Strings around Higher-Dimensional Black Holes | 9 pages, 5 figures | Phys.Rev.D82:044014,2010 | 10.1103/PhysRevD.82.044014 | OCU-PHYS 321, AP-GR 72 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present solutions of the Nambu-Goto equation for test strings in a shape
of toroidal spiral in five-dimensional spacetimes. In particular, we show that
stationary toroidal spirals exist around the five-dimensional Myers-Perry black
holes. We also show the existence of innermost stationary toroidal spirals
around t... | [
{
"created": "Mon, 2 Nov 2009 09:32:29 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Igata",
"Takahisa",
""
],
[
"Ishihara",
"Hideki",
""
]
] | We present solutions of the Nambu-Goto equation for test strings in a shape of toroidal spiral in five-dimensional spacetimes. In particular, we show that stationary toroidal spirals exist around the five-dimensional Myers-Perry black holes. We also show the existence of innermost stationary toroidal spirals around the... | 9.28429 | 7.910469 | 9.160899 | 7.527004 | 8.517396 | 7.903133 | 8.095166 | 8.061354 | 8.902288 | 9.892774 | 7.781541 | 8.967767 | 9.05228 | 8.420028 | 8.426313 | 8.799993 | 8.817835 | 8.361623 | 9.018301 | 8.582344 | 8.393746 |
hep-th/0009125 | Henrique Boschi-Filho | P. F. Borges, H. Boschi-Filho and C. Farina | The effect of a topological gauge field on Bose-Einstein condensation | 12 Latex pages, revises and extends work in hep-th/9812045 | Phys.Lett. B460 (1999) 376-382 | 10.1016/S0370-2693(99)00739-X | null | hep-th cond-mat | null | We show that Bose-Einstein condensation of charged scalar fields interacting
with a topological gauge field at finite temperature is inhibited except for
special values of the topological field. We also show that fermions interacting
with this topological gauge field can condense for some values of the gauge
field.
| [
{
"created": "Fri, 15 Sep 2000 14:40:29 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Borges",
"P. F.",
""
],
[
"Boschi-Filho",
"H.",
""
],
[
"Farina",
"C.",
""
]
] | We show that Bose-Einstein condensation of charged scalar fields interacting with a topological gauge field at finite temperature is inhibited except for special values of the topological field. We also show that fermions interacting with this topological gauge field can condense for some values of the gauge field. | 8.362215 | 7.259124 | 8.141249 | 6.69733 | 7.663218 | 7.166582 | 7.866511 | 7.472275 | 7.192854 | 7.75065 | 7.281901 | 7.931686 | 8.514908 | 7.674803 | 7.718856 | 7.753648 | 7.945978 | 7.636927 | 8.460739 | 8.588403 | 7.561057 |
1709.02290 | Andrei Mironov | A. Mironov, A. Morozov and A. Sleptsov | On $6j$-symbols for symmetric representations of $U_q(\mathfrak{su}_N)$ | 9 pages | Pis'ma v ZhETF, 106 (2017) 607 | 10.1134/S0021364017220040 | FIAN/TD-18/17; IITP/TH-14/17; ITEP/TH-23/17 | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Explicit expressions are found for the $6j$ symbols in symmetric
representations of quantum $\mathfrak{su}_N$ through appropriate hypergeometric
Askey-Wilson (q-Racah) polynomials. This generalizes the well-known classical
formulas for $U_q(\mathfrak{su}_2)$ and provides a link to conformal theories
and matrix models... | [
{
"created": "Thu, 7 Sep 2017 14:51:07 GMT",
"version": "v1"
},
{
"created": "Wed, 18 Oct 2017 08:48:54 GMT",
"version": "v2"
}
] | 2017-12-06 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
],
[
"Sleptsov",
"A.",
""
]
] | Explicit expressions are found for the $6j$ symbols in symmetric representations of quantum $\mathfrak{su}_N$ through appropriate hypergeometric Askey-Wilson (q-Racah) polynomials. This generalizes the well-known classical formulas for $U_q(\mathfrak{su}_2)$ and provides a link to conformal theories and matrix models. | 10.315716 | 9.932907 | 11.535913 | 9.144044 | 9.108564 | 9.063627 | 9.128824 | 10.721288 | 8.758823 | 10.96029 | 9.354778 | 9.342497 | 9.30542 | 9.801378 | 9.284788 | 9.515945 | 9.200435 | 10.20357 | 9.336955 | 9.942728 | 9.369398 |
hep-th/0207066 | Frank Ferrari | Frank Ferrari (University of Neuchatel and Ecole Normale Superieure) | Spectral asymmetry and supersymmetry | 9 pages; v2: typos corrected | Phys.Lett. B548 (2002) 68-72 | 10.1016/S0370-2693(02)02820-4 | NEIP-02-005, LPTENS-02/38 | hep-th cond-mat math-ph math.MP | null | Fractional charges, and in particular the spectral asymmetry eta of certain
Dirac operators, can appear in the central charge of supersymmetric field
theories. This yields unexpected analyticity constraints on eta from which
classic results can be recovered in an elegant way. The method could also be
applied in the c... | [
{
"created": "Mon, 8 Jul 2002 13:35:56 GMT",
"version": "v1"
},
{
"created": "Thu, 17 Oct 2002 10:37:29 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Ferrari",
"Frank",
"",
"University of Neuchatel and Ecole Normale Superieure"
]
] | Fractional charges, and in particular the spectral asymmetry eta of certain Dirac operators, can appear in the central charge of supersymmetric field theories. This yields unexpected analyticity constraints on eta from which classic results can be recovered in an elegant way. The method could also be applied in the con... | 19.290981 | 19.370583 | 19.062284 | 17.468937 | 19.016804 | 19.850271 | 21.402945 | 21.672043 | 18.071489 | 22.18862 | 17.868135 | 18.314829 | 21.077478 | 17.420799 | 17.797724 | 19.217165 | 18.762928 | 17.851044 | 17.18449 | 19.581165 | 18.136358 |
hep-th/0606209 | Alessio Marrani | Stefano Bellucci, Sergio Ferrara, Murat Gunaydin, Alessio Marrani | Charge Orbits of Symmetric Special Geometries and Attractors | 63 pages, 9 Tables. v2: typos fixed, Refs. added, accepted for
publication in IJMPA | Int.J.Mod.Phys.A21:5043-5098,2006 | 10.1142/S0217751X06034355 | CERN-PH-TH/2006-108, LNF-06-16-P, UCLA/06/TEP/18 | hep-th | null | We study the critical points of the black hole scalar potential $V_{BH}$ in
N=2, d=4 supergravity coupled to $n_{V}$ vector multiplets, in an
asymptotically flat extremal black hole background described by a
2(n_{V}+1)-dimensional dyonic charge vector and (complex) scalar fields which
are coordinates of a special K\"... | [
{
"created": "Wed, 21 Jun 2006 15:32:53 GMT",
"version": "v1"
},
{
"created": "Tue, 26 Sep 2006 08:58:53 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Bellucci",
"Stefano",
""
],
[
"Ferrara",
"Sergio",
""
],
[
"Gunaydin",
"Murat",
""
],
[
"Marrani",
"Alessio",
""
]
] | We study the critical points of the black hole scalar potential $V_{BH}$ in N=2, d=4 supergravity coupled to $n_{V}$ vector multiplets, in an asymptotically flat extremal black hole background described by a 2(n_{V}+1)-dimensional dyonic charge vector and (complex) scalar fields which are coordinates of a special K\"{a... | 7.346928 | 6.728043 | 8.318349 | 6.860946 | 7.154473 | 6.557081 | 6.730707 | 6.931658 | 6.768155 | 8.779963 | 6.806639 | 7.185931 | 7.747894 | 7.297365 | 7.130058 | 7.226885 | 7.151614 | 7.129427 | 7.319909 | 7.919919 | 7.049367 |
1809.03611 | Edwin Ireson | Edwin Ireson | Worldsheets in Holography: Computing Corrections to the Veneziano
Amplitude | 24 pages, 7 figures, in preparation for submission to MPLA | null | 10.1142/S0217732319300027 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a brief summary of a method to calculate improvements to the
Veneziano Amplitude, creating sub-leading non-linearities in the Regge
trajectory of states. We formulate it as an extension of a computation by
Makeenko and Olesen. We begin in a confining gauge theory coupled to matter,
rewriting the meson scat... | [
{
"created": "Mon, 10 Sep 2018 21:52:11 GMT",
"version": "v1"
}
] | 2019-05-22 | [
[
"Ireson",
"Edwin",
""
]
] | We provide a brief summary of a method to calculate improvements to the Veneziano Amplitude, creating sub-leading non-linearities in the Regge trajectory of states. We formulate it as an extension of a computation by Makeenko and Olesen. We begin in a confining gauge theory coupled to matter, rewriting the meson scatte... | 17.791006 | 18.095968 | 18.924067 | 17.2337 | 17.798677 | 17.923235 | 17.680014 | 17.519184 | 16.890554 | 20.94499 | 17.392128 | 18.74217 | 18.103436 | 17.785261 | 18.210978 | 18.485386 | 18.156666 | 18.270813 | 17.494637 | 18.551937 | 17.772675 |
hep-th/9502072 | null | A. Ceresole, R. D'Auria, S. Ferrara and A. Van Proeyen | Duality Transformations in Supersymmetric Yang-Mills Theories coupled to
Supergravity, | 41 pages, harvmac, no figures. References added, and minor printing
error corrected. | Nucl.Phys. B444 (1995) 92-124 | 10.1016/0550-3213(95)00175-R | CERN-TH 7547/94, POLFIS-TH. 01/95, UCLA 94/TEP/45, KUL-TF-95/4 | hep-th | null | We consider duality transformations in N=2, d=4 Yang--Mills theory coupled to
N=2 supergravity. A symplectic and coordinate covariant framework is
established, which allows one to discuss stringy `classical and quantum duality
symmetries' (monodromies), incorporating T and S dualities. In particular, we
shall be able... | [
{
"created": "Mon, 13 Feb 1995 17:38:56 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Mar 1995 17:59:09 GMT",
"version": "v2"
}
] | 2016-09-06 | [
[
"Ceresole",
"A.",
""
],
[
"D'Auria",
"R.",
""
],
[
"Ferrara",
"S.",
""
],
[
"Van Proeyen",
"A.",
""
]
] | We consider duality transformations in N=2, d=4 Yang--Mills theory coupled to N=2 supergravity. A symplectic and coordinate covariant framework is established, which allows one to discuss stringy `classical and quantum duality symmetries' (monodromies), incorporating T and S dualities. In particular, we shall be able t... | 9.761495 | 10.258958 | 11.592083 | 10.309632 | 10.734808 | 10.656529 | 9.789437 | 10.170841 | 10.000486 | 12.915902 | 10.157896 | 9.866256 | 10.878129 | 10.097058 | 10.122401 | 9.865011 | 10.203509 | 9.75102 | 9.844056 | 10.582924 | 9.870425 |
hep-th/9504138 | null | S. Krivonos, A. Sorin and F. Toppan | On the Super-NLS Equation and its Relation with N=2 Super-KdV within
Coset Approach | 10 pages, LaTex | Phys.Lett. A206 (1995) 146-152 | 10.1016/0375-9601(95)00651-I | JINR E2-95-185; DFPD 95-TH-24 | hep-th | null | A manifestly $N=2$ supersymmetric coset formalism is introduced to describe
integrable hierarchies. It is applied to analyze the super-NLS equation. It
possesses an $N=2$ symmetry since it can be obtained from a manifest $N=2$
coset algebra construction. A remarkable result is here discussed: the
existence of a B\"{a... | [
{
"created": "Wed, 26 Apr 1995 12:12:39 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Krivonos",
"S.",
""
],
[
"Sorin",
"A.",
""
],
[
"Toppan",
"F.",
""
]
] | A manifestly $N=2$ supersymmetric coset formalism is introduced to describe integrable hierarchies. It is applied to analyze the super-NLS equation. It possesses an $N=2$ symmetry since it can be obtained from a manifest $N=2$ coset algebra construction. A remarkable result is here discussed: the existence of a B\"{a}c... | 9.450058 | 9.151781 | 10.286491 | 8.258489 | 8.823605 | 8.786378 | 9.017634 | 8.517073 | 8.100306 | 10.631294 | 8.665633 | 8.134066 | 8.784601 | 8.328069 | 8.628304 | 8.416475 | 8.330541 | 8.337712 | 8.180804 | 8.661442 | 8.260345 |
2303.14200 | Adam Tropper | Adam Tropper and Tianli Wang | Lorentz Symmetry and IR Structure of The BFSS Matrix Model | 25 + 7 pages | null | 10.1007/JHEP07(2023)150 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The BFSS matrix model relates flat space M-theory to a large N limit of
matrix quantum mechanics describing N D0-branes. M-theory, being a theory of
gravity in flat space, has a rich infrared structure that includes various soft
theorems and an infinite set of conserved charges associated to asymptotic
symmetries. In... | [
{
"created": "Fri, 24 Mar 2023 18:00:00 GMT",
"version": "v1"
}
] | 2023-08-09 | [
[
"Tropper",
"Adam",
""
],
[
"Wang",
"Tianli",
""
]
] | The BFSS matrix model relates flat space M-theory to a large N limit of matrix quantum mechanics describing N D0-branes. M-theory, being a theory of gravity in flat space, has a rich infrared structure that includes various soft theorems and an infinite set of conserved charges associated to asymptotic symmetries. In t... | 8.270488 | 8.129727 | 8.399049 | 7.706765 | 8.145561 | 8.216264 | 7.678429 | 7.658261 | 7.669166 | 8.918727 | 7.376366 | 7.896212 | 7.790025 | 7.674531 | 7.784009 | 7.797413 | 7.683211 | 7.691322 | 7.6858 | 7.818199 | 7.553349 |
1907.12292 | A. Emir Gumrukcuoglu | A. Emir Gumrukcuoglu, Ryo Namba | Role of matter in gravitation: going beyond the Einstein-Maxwell theory | 5 pages; v2 update to match the published version | Phys. Rev. D 100, 124064 (2019) | 10.1103/PhysRevD.100.124064 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For field theories in curved spacetime, defining how matter gravitates is
part of the theory building process. In this letter, we adopt Bekenstein's
multiple geometries approach to allow part of the matter sector to follow the
geodesics on a general pseudo-Riemannian geometry, constructed from a tensor
and a $U(1)$ g... | [
{
"created": "Mon, 29 Jul 2019 09:25:16 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Jan 2020 07:08:18 GMT",
"version": "v2"
}
] | 2020-01-03 | [
[
"Gumrukcuoglu",
"A. Emir",
""
],
[
"Namba",
"Ryo",
""
]
] | For field theories in curved spacetime, defining how matter gravitates is part of the theory building process. In this letter, we adopt Bekenstein's multiple geometries approach to allow part of the matter sector to follow the geodesics on a general pseudo-Riemannian geometry, constructed from a tensor and a $U(1)$ gau... | 14.812802 | 14.973495 | 13.630084 | 13.130638 | 14.410646 | 15.446986 | 14.905177 | 13.619789 | 13.526607 | 13.914315 | 13.105024 | 13.14988 | 13.030226 | 12.971334 | 13.275869 | 12.988815 | 13.297023 | 13.164546 | 13.795359 | 13.452929 | 13.099785 |
hep-th/0510101 | Archil Kobakhidze | Laura Mersini-Houghton | Do We Have Evidence for New Physics in the Sky? | Invited Review to appear in MPLA. Based on work done with Steen
Hannestad | Mod.Phys.Lett. A21 (2006) 1-22 | 10.1142/S0217732306019268 | pp 1-21 | hep-th astro-ph hep-ph | null | Predicting signatures of string theory on cosmological observables is not
sufficient. Often the observable effects string theory may impact upon the
cosmological arena may equally be predicted by features of inflationary
physics. The question: what observable signatures are unique to new physics, is
thus of crucial i... | [
{
"created": "Wed, 12 Oct 2005 16:38:10 GMT",
"version": "v1"
}
] | 2009-11-11 | [
[
"Mersini-Houghton",
"Laura",
""
]
] | Predicting signatures of string theory on cosmological observables is not sufficient. Often the observable effects string theory may impact upon the cosmological arena may equally be predicted by features of inflationary physics. The question: what observable signatures are unique to new physics, is thus of crucial imp... | 21.022438 | 25.8221 | 21.163275 | 20.504307 | 25.841345 | 23.266596 | 22.374508 | 24.02692 | 21.080576 | 23.303465 | 22.669649 | 19.311579 | 19.524971 | 19.606916 | 19.783533 | 19.022045 | 20.219261 | 18.942028 | 20.077366 | 19.943708 | 21.186922 |
1104.1349 | Neven Bilic | Neven Bilic | Vacuum fluctuations in a supersymmetric model in FRW spacetime | 19 pages, accepted for publication in Phys. Rev. D | Phys.Rev.D83:105003,2011 | 10.1103/PhysRevD.83.105003 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a noninteracting supersymmetric model in an expanding FRW spacetime.
A soft supersymmetry breaking induces a nonzero contribution to the vacuum
energy density. A short distance cutoff of the order of Planck length provides
a scale for the vacuum energy density comparable with the observed cosmological
consta... | [
{
"created": "Thu, 7 Apr 2011 14:58:55 GMT",
"version": "v1"
}
] | 2011-05-13 | [
[
"Bilic",
"Neven",
""
]
] | We study a noninteracting supersymmetric model in an expanding FRW spacetime. A soft supersymmetry breaking induces a nonzero contribution to the vacuum energy density. A short distance cutoff of the order of Planck length provides a scale for the vacuum energy density comparable with the observed cosmological constant... | 10.831995 | 10.339545 | 10.139923 | 9.261678 | 10.554335 | 10.808033 | 10.819842 | 9.831397 | 9.733221 | 9.689209 | 10.290382 | 10.104927 | 9.668777 | 9.661136 | 10.221255 | 9.978178 | 10.141335 | 10.053002 | 10.050448 | 9.907042 | 9.895791 |
0911.2546 | Gabriele Tartaglino-Mazzucchelli | Gabriele Tartaglino-Mazzucchelli | 2D N=(4,4) superspace supergravity and bi-projective superfields | 50+1 pages, LaTeX; V2: 52 pages, typos corrected, comments added,
version published in JHEP | JHEP 1004:034,2010 | 10.1007/JHEP04(2010)034 | UMD-PP-09-046 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a new superspace formulation for N=(4,4) conformal supergravity in
two dimensions. This is based on a geometry where the structure group of the
curved superspace is chosen to be SO(1,1) x SU(2)_L x SU(2)_R. The off-shell
supergravity multiplet possesses super-Weyl transformations generated by an
unconstrai... | [
{
"created": "Fri, 13 Nov 2009 19:16:05 GMT",
"version": "v1"
},
{
"created": "Thu, 8 Apr 2010 11:52:10 GMT",
"version": "v2"
}
] | 2010-04-23 | [
[
"Tartaglino-Mazzucchelli",
"Gabriele",
""
]
] | We propose a new superspace formulation for N=(4,4) conformal supergravity in two dimensions. This is based on a geometry where the structure group of the curved superspace is chosen to be SO(1,1) x SU(2)_L x SU(2)_R. The off-shell supergravity multiplet possesses super-Weyl transformations generated by an unconstraine... | 6.80799 | 6.684886 | 8.381462 | 6.555604 | 6.888361 | 7.042115 | 6.856792 | 6.685137 | 6.841536 | 8.758162 | 7.078783 | 6.725758 | 7.25502 | 6.939486 | 6.982247 | 6.881248 | 7.018266 | 6.926619 | 6.707549 | 7.208645 | 6.719511 |
1312.6196 | Benjamin Horowitz | Benjamin Horowitz | Group Theoretical Approach to the Construction of Conformal Field
Theories | 7 pages, 3 figures | null | null | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A conformal field theory (CFT) is a quantum field theory which is invariant
under conformal transformations; a group action that preserve angles but not
necessarily lengths. There are two traditional approaches to the construction
of CFTs: analyzing a statistical system near a critical point as a euclidean
field theo... | [
{
"created": "Sat, 21 Dec 2013 03:17:32 GMT",
"version": "v1"
}
] | 2013-12-24 | [
[
"Horowitz",
"Benjamin",
""
]
] | A conformal field theory (CFT) is a quantum field theory which is invariant under conformal transformations; a group action that preserve angles but not necessarily lengths. There are two traditional approaches to the construction of CFTs: analyzing a statistical system near a critical point as a euclidean field theory... | 9.175641 | 7.959695 | 9.102169 | 8.37347 | 8.623147 | 8.167049 | 8.857176 | 8.859628 | 8.214009 | 9.96673 | 7.981158 | 8.297556 | 8.411486 | 8.11674 | 8.204267 | 7.84195 | 8.066737 | 8.122044 | 8.116575 | 8.601926 | 8.16865 |
2111.12075 | Josef Kluson | J. Kluson | New Non-Relativistic String in AdS(5)xS(5) | 17 pages | null | null | null | hep-th | http://creativecommons.org/publicdomain/zero/1.0/ | We study non-relativistic limit of AdS(5)xS(5) background and determine
corresponding Newton-Cartan fields. We also find canonical form of the new
non-relativistic string in this background and discuss its formulation in the
uniform light-cone gauge.
| [
{
"created": "Tue, 23 Nov 2021 18:47:50 GMT",
"version": "v1"
}
] | 2021-11-24 | [
[
"Kluson",
"J.",
""
]
] | We study non-relativistic limit of AdS(5)xS(5) background and determine corresponding Newton-Cartan fields. We also find canonical form of the new non-relativistic string in this background and discuss its formulation in the uniform light-cone gauge. | 11.575976 | 6.815564 | 12.624569 | 7.861421 | 7.376069 | 7.366239 | 7.546865 | 7.135448 | 8.13314 | 11.386046 | 7.799337 | 8.308413 | 12.273904 | 8.717681 | 8.42621 | 7.718762 | 8.18525 | 8.071346 | 8.464504 | 11.461597 | 8.326834 |
1904.13394 | Congkao Wen | Michael B. Green, Congkao Wen | Modular Forms and $SL(2, {\mathbb Z})$-covariance of type IIB
superstring theory | 58 pages, 4 figures. v2: typos corrected, JHEP version | null | 10.1007/JHEP06(2019)087 | QMUL-PH-19-07, DAMTP-2019-15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The local higher-derivative interactions that enter into the low-energy
expansion of the effective action of type IIB superstring theory with constant
complex modulus generally violate the $U(1)$ R-symmetry of IIB supergravity by
$q_U$ units. These interactions have coefficients that transform as
non-holomorphic modu... | [
{
"created": "Tue, 30 Apr 2019 17:57:48 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Jun 2019 10:16:22 GMT",
"version": "v2"
}
] | 2019-07-24 | [
[
"Green",
"Michael B.",
""
],
[
"Wen",
"Congkao",
""
]
] | The local higher-derivative interactions that enter into the low-energy expansion of the effective action of type IIB superstring theory with constant complex modulus generally violate the $U(1)$ R-symmetry of IIB supergravity by $q_U$ units. These interactions have coefficients that transform as non-holomorphic modula... | 6.540978 | 6.91609 | 7.261083 | 6.626986 | 7.438632 | 6.929548 | 6.931025 | 6.789346 | 6.543951 | 7.940566 | 6.3731 | 6.533388 | 6.63209 | 6.474109 | 6.591502 | 6.55254 | 6.651433 | 6.521891 | 6.447119 | 6.716188 | 6.495942 |
1804.08566 | Alesandro Santos A. F. Santos | A. F. Santos and Faqir C. Khanna | Lorentz violation, M\"oller scattering and finite temperature | 12 pages, 1 figure, accepted for publication in Adv. High Energy Phys | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Lorentz and CPT symmetries may be violated in new physics that emerges at
very high energy scale, i.e., at the Planck scale. The differential cross
section of the M\"oller scattering, due to Lorentz violation at finite
temperature is calculated. Lorentz-violating effects emerge from an interaction
vertex due to a CPT... | [
{
"created": "Mon, 23 Apr 2018 17:03:01 GMT",
"version": "v1"
}
] | 2018-04-24 | [
[
"Santos",
"A. F.",
""
],
[
"Khanna",
"Faqir C.",
""
]
] | Lorentz and CPT symmetries may be violated in new physics that emerges at very high energy scale, i.e., at the Planck scale. The differential cross section of the M\"oller scattering, due to Lorentz violation at finite temperature is calculated. Lorentz-violating effects emerge from an interaction vertex due to a CPT-o... | 7.180053 | 6.177881 | 6.318573 | 6.118464 | 6.469944 | 7.582164 | 6.422986 | 6.169124 | 5.826241 | 6.812389 | 6.462885 | 6.523998 | 6.381225 | 6.414099 | 6.530191 | 6.126647 | 6.36336 | 6.393979 | 6.11095 | 6.271192 | 6.378742 |
hep-th/9211007 | Samir Mathur | Brian R. Greene, Samir D. Mathur and Christopher M. O'Neill | Eluding the no-hair conjecture: Black holes in spontaneously broken
gauge theories | 35 pages, phyzzx, (CLNS-92/1162, CTP-2160) | Phys.Rev. D47 (1993) 2242-2259 | 10.1103/PhysRevD.47.2242 | null | hep-th | null | We study regular and black hole solutions to the coupled classical
Einstein--Yang-Mills--Higgs system. It has long been thought that black hole
solutions in the spontaneously broken phase of such a theory could have no
nontrivial field structure outside of the horizon. We first show that the
standard black hole no-ha... | [
{
"created": "Mon, 2 Nov 1992 16:01:19 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Nov 1992 01:45:35 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Greene",
"Brian R.",
""
],
[
"Mathur",
"Samir D.",
""
],
[
"O'Neill",
"Christopher M.",
""
]
] | We study regular and black hole solutions to the coupled classical Einstein--Yang-Mills--Higgs system. It has long been thought that black hole solutions in the spontaneously broken phase of such a theory could have no nontrivial field structure outside of the horizon. We first show that the standard black hole no-hair... | 8.405126 | 8.783357 | 7.795039 | 7.934209 | 8.213968 | 8.45318 | 9.142857 | 8.195422 | 8.33598 | 9.21572 | 8.925873 | 8.626859 | 8.137684 | 8.085487 | 8.220159 | 8.368641 | 8.30218 | 8.241633 | 8.101785 | 8.237287 | 8.086858 |
hep-th/0511238 | Artyom Yurov | A.V. Yurov, V.A. Yurov | One more observational consequence of many-worlds quantum theory | 4 pages, RevTeX, 1 table | null | null | null | hep-th | null | Using new cosmological doomsday argument Page predicts that the maximal
lifetime of de Sitter universe should be $t_{max}=10^{60}$ yr which is way too
small in comparison with strings predictions ($t_f>$googleplex). However, since
this prediction is dependant on the total number of human observations, we show
that Pa... | [
{
"created": "Wed, 23 Nov 2005 22:32:21 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Yurov",
"A. V.",
""
],
[
"Yurov",
"V. A.",
""
]
] | Using new cosmological doomsday argument Page predicts that the maximal lifetime of de Sitter universe should be $t_{max}=10^{60}$ yr which is way too small in comparison with strings predictions ($t_f>$googleplex). However, since this prediction is dependant on the total number of human observations, we show that Page... | 19.046053 | 20.776539 | 17.364971 | 17.95085 | 19.619719 | 20.129738 | 20.749975 | 20.506355 | 18.417465 | 20.055731 | 19.178268 | 18.153538 | 17.57933 | 17.854259 | 19.041735 | 19.045938 | 18.563091 | 17.717342 | 17.460049 | 17.76469 | 16.999434 |
1502.03108 | Blagoje Oblak | Blagoje Oblak | Characters of the BMS Group in Three Dimensions | 22 pages. v2: Updated references [5], [7] and [45]. Published in
Communications in Mathematical Physics. The final publication is available at
Springer via http://dx.doi.org/10.1007/s00220-015-2408-7 | Communications in Mathematical Physics (2015), pages 1-20 | 10.1007/s00220-015-2408-7 | null | hep-th math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the Frobenius formula, we evaluate characters associated with certain
induced representations of the centrally extended BMS$_3$ group. This
computation involves a functional integral over a coadjoint orbit of the
Virasoro group; a delta function localizes the integral to a single point,
allowing us to obtain an... | [
{
"created": "Tue, 10 Feb 2015 21:00:21 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jun 2015 08:39:57 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Oblak",
"Blagoje",
""
]
] | Using the Frobenius formula, we evaluate characters associated with certain induced representations of the centrally extended BMS$_3$ group. This computation involves a functional integral over a coadjoint orbit of the Virasoro group; a delta function localizes the integral to a single point, allowing us to obtain an e... | 9.926688 | 8.750976 | 10.070692 | 8.342946 | 8.637219 | 8.551617 | 8.634488 | 8.280354 | 8.6287 | 11.292503 | 8.483644 | 8.620878 | 9.662149 | 8.788939 | 8.300584 | 8.925697 | 8.530422 | 8.429114 | 8.59119 | 9.230608 | 8.583721 |
hep-th/9406156 | Andrei Johansen | Andrei Johansen | Realization of $W_{1+\infty}$ and Virasoro Algebras in Supersymmetric
Theories on Four Manifolds | Latex, 13 pages, NBI-HE-94-35. Minor stylistic changes | Mod.Phys.Lett. A9 (1994) 2611-2622 | 10.1142/S0217732394002458 | null | hep-th | null | We demonstrate that a supersymmetric theory twisted on a K\"ahler four
manifold $M=\Sigma_1 \times \Sigma_2 ,$ where $\Sigma_{1,2}$ are 2D Riemann
surfaces, possesses a "left-moving" conformal stress tensor on $\Sigma_1$
($\Sigma_2$) in the BRST cohomology. The central charge of the Virasoro algebra
has a purely geom... | [
{
"created": "Thu, 23 Jun 1994 14:35:05 GMT",
"version": "v1"
},
{
"created": "Mon, 18 Jul 1994 17:40:25 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Johansen",
"Andrei",
""
]
] | We demonstrate that a supersymmetric theory twisted on a K\"ahler four manifold $M=\Sigma_1 \times \Sigma_2 ,$ where $\Sigma_{1,2}$ are 2D Riemann surfaces, possesses a "left-moving" conformal stress tensor on $\Sigma_1$ ($\Sigma_2$) in the BRST cohomology. The central charge of the Virasoro algebra has a purely geomet... | 5.990902 | 5.750526 | 6.646858 | 5.38516 | 5.548526 | 5.76828 | 5.94911 | 5.662242 | 5.611036 | 6.816662 | 5.425602 | 5.563307 | 6.085629 | 5.644711 | 5.630139 | 5.54959 | 5.445304 | 5.534747 | 5.526898 | 5.953623 | 5.564051 |
hep-th/0607107 | Jose Francisco Gomes | J.F. Gomes, L.H. Ymai and A.H. Zimerman | Soliton Solutions for the Super mKdV and sinh-Gordon Hierarchy | To appear in Phys. Lett. A | Phys.Lett.A359:630-637,2006 | 10.1016/j.physleta.2006.07.018 | null | hep-th | null | The dressing and vertex operator formalism is emploied to study the soliton
solutions of the N=1 super mKdV and sinh-Gordon models. Explicit two and four
vertex solutions are constructed. The relation between the soliton solutions of
both models is verified.
| [
{
"created": "Mon, 17 Jul 2006 13:33:49 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Gomes",
"J. F.",
""
],
[
"Ymai",
"L. H.",
""
],
[
"Zimerman",
"A. H.",
""
]
] | The dressing and vertex operator formalism is emploied to study the soliton solutions of the N=1 super mKdV and sinh-Gordon models. Explicit two and four vertex solutions are constructed. The relation between the soliton solutions of both models is verified. | 15.34579 | 11.268792 | 15.342699 | 11.443074 | 12.27902 | 11.810655 | 10.649037 | 11.906902 | 10.747097 | 17.903208 | 12.309199 | 13.193484 | 15.147745 | 12.822395 | 12.967362 | 12.785326 | 12.692576 | 12.728585 | 11.95869 | 14.210779 | 13.073136 |
2306.07327 | Flavio Tonioni | Gary Shiu, Flavio Tonioni, Hung V. Tran | Late-time attractors and cosmic acceleration | 26 pages (13 figures) + appendices; v2: minor improvements | null | null | null | hep-th astro-ph.CO gr-qc math.DS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove the conditions under which scaling cosmologies are inevitable
late-time attractors of multi-field multi-exponential potentials, independently
of initial conditions. The advantage of such scaling cosmologies is that the
time dependence of the fields and of the scale factor is known analytically,
thus allowing... | [
{
"created": "Mon, 12 Jun 2023 18:00:02 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Sep 2023 15:50:02 GMT",
"version": "v2"
}
] | 2023-09-25 | [
[
"Shiu",
"Gary",
""
],
[
"Tonioni",
"Flavio",
""
],
[
"Tran",
"Hung V.",
""
]
] | We prove the conditions under which scaling cosmologies are inevitable late-time attractors of multi-field multi-exponential potentials, independently of initial conditions. The advantage of such scaling cosmologies is that the time dependence of the fields and of the scale factor is known analytically, thus allowing l... | 11.180484 | 11.388574 | 10.607174 | 9.595602 | 11.238325 | 11.053224 | 11.572343 | 10.346173 | 10.056325 | 11.135791 | 10.349046 | 10.495128 | 10.731333 | 10.262635 | 10.508303 | 10.468209 | 10.344928 | 10.345076 | 10.424526 | 10.519829 | 10.447571 |
0904.4112 | Jianxin Lu | J. X. Lu and Shan-Shan Xu | The open string pair-production rate enhancement by a magnetic flux | 33 pages, no figures, a few points refined to the published version
JHEP09(2009)093 | JHEP 0909:093,2009 | 10.1088/1126-6708/2009/09/093 | USTC-ICTS-09-05 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the amplitude calculations of \cite{Lu:2009yx} to exhaust the
remaining cases for which one set of D$_p$ branes carrying a flux (electric or
magnetic) is placed parallel at separation to the other set carrying also a
flux but with the two fluxes sharing at most one common field-strength index.
We then find ... | [
{
"created": "Mon, 27 Apr 2009 08:36:33 GMT",
"version": "v1"
},
{
"created": "Wed, 3 Jun 2009 07:34:52 GMT",
"version": "v2"
},
{
"created": "Mon, 24 Aug 2009 22:15:47 GMT",
"version": "v3"
},
{
"created": "Mon, 28 Sep 2009 15:24:38 GMT",
"version": "v4"
}
] | 2009-10-02 | [
[
"Lu",
"J. X.",
""
],
[
"Xu",
"Shan-Shan",
""
]
] | We extend the amplitude calculations of \cite{Lu:2009yx} to exhaust the remaining cases for which one set of D$_p$ branes carrying a flux (electric or magnetic) is placed parallel at separation to the other set carrying also a flux but with the two fluxes sharing at most one common field-strength index. We then find th... | 9.944469 | 8.323565 | 11.302663 | 9.05784 | 9.156222 | 9.249794 | 8.64585 | 8.985571 | 9.173143 | 12.468061 | 8.654727 | 9.581067 | 10.249819 | 9.635784 | 9.476046 | 9.426864 | 9.608662 | 9.472168 | 9.587742 | 10.188844 | 9.669316 |
hep-th/0210101 | Hang Bae Kim | Chanju Kim (Ewha W.U.), Hang Bae Kim (Lausanne U.), Yoonbai Kim
(Sungkyunkwan U.) | Rolling Tachyons in String Cosmology | More references added. A version to be published in Phys.Lett.B | Phys.Lett. B552 (2003) 111-118 | 10.1016/S0370-2693(02)03126-X | null | hep-th astro-ph hep-ph | null | We study the role of rolling tachyons in the cosmological model with
dilatonic gravity. In the string frame, flat space solutions of both
initial-stage and late-time are obtained in closed form. In the Einstein frame,
we show that every expanding solution is decelerating.
| [
{
"created": "Thu, 10 Oct 2002 16:54:22 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Oct 2002 08:12:20 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Nov 2002 13:28:37 GMT",
"version": "v3"
}
] | 2010-04-05 | [
[
"Kim",
"Chanju",
"",
"Ewha W.U."
],
[
"Kim",
"Hang Bae",
"",
"Lausanne U."
],
[
"Kim",
"Yoonbai",
"",
"Sungkyunkwan U."
]
] | We study the role of rolling tachyons in the cosmological model with dilatonic gravity. In the string frame, flat space solutions of both initial-stage and late-time are obtained in closed form. In the Einstein frame, we show that every expanding solution is decelerating. | 18.777617 | 11.359877 | 13.184391 | 12.584984 | 13.738778 | 13.648724 | 13.686272 | 13.055625 | 12.684421 | 13.681432 | 12.056355 | 14.67013 | 13.565065 | 13.718966 | 14.477839 | 14.697755 | 15.105917 | 13.686709 | 13.928235 | 14.677082 | 14.320717 |
1001.5324 | Wu JianPin | Yi Ling and Jian-Pin Wu | A note on entropic force and brane cosmology | 5 pages, no figures;references added | JCAP 1008:017,2010 | 10.1088/1475-7516/2010/08/017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently Verlinde proposed that gravity is an entropic force caused by
information changes when a material body moves away from the holographic
screen. In this note we apply this argument to brane cosmology, and show that
the cosmological equation can be derived from this holographic scenario.
| [
{
"created": "Fri, 29 Jan 2010 05:05:42 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Feb 2010 07:04:40 GMT",
"version": "v2"
}
] | 2010-09-15 | [
[
"Ling",
"Yi",
""
],
[
"Wu",
"Jian-Pin",
""
]
] | Recently Verlinde proposed that gravity is an entropic force caused by information changes when a material body moves away from the holographic screen. In this note we apply this argument to brane cosmology, and show that the cosmological equation can be derived from this holographic scenario. | 7.132555 | 6.336857 | 6.833858 | 5.53296 | 6.654403 | 6.407762 | 6.589985 | 6.246883 | 5.860063 | 7.555389 | 5.279815 | 5.93362 | 6.369802 | 5.825993 | 6.063436 | 6.136827 | 5.810424 | 5.955046 | 6.214532 | 6.01659 | 6.062576 |
hep-th/9610159 | Massimo Porrati | A. Giveon, M. Porrati | Aspects of Dualities | Contribution to the proceedings of ICHEP '96, Warsaw, July 25-31,
1996; presented by A. Giveon | null | null | RI-8-96, NYU-TH-96/10/01 | hep-th | null | In this talk, some aspects of duality symmetries are presented.
| [
{
"created": "Mon, 21 Oct 1996 18:30:14 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Giveon",
"A.",
""
],
[
"Porrati",
"M.",
""
]
] | In this talk, some aspects of duality symmetries are presented. | 18.427214 | 5.870165 | 7.376078 | 6.681394 | 6.499371 | 6.536494 | 6.26255 | 6.029712 | 6.636905 | 7.284974 | 6.487107 | 7.022811 | 8.340469 | 6.97362 | 7.203664 | 7.30401 | 7.191913 | 7.199959 | 7.295143 | 8.4334 | 7.301199 |
2106.01791 | Kirill Bazarov | E. T. Akhmedov, K. V. Bazarov, D. V. Diakonov | Quantum fields in the future Rindler wedge | 18 pages, 2 figures. Language is improved, more arguments are given
and clarified, substantial changes | Phys. Rev. D 104, 085008 (2021) | 10.1103/PhysRevD.104.085008 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider interacting massive scalar quantum field theory in the future
Rindler wedge. This is a model example of quantum field theory in curved
space--time. On this simple example we show how dynamics of correlation
functions depends on the choice of initial Cauchy surface, basis of modes and
on the choice of init... | [
{
"created": "Thu, 3 Jun 2021 12:24:06 GMT",
"version": "v1"
},
{
"created": "Fri, 10 Sep 2021 09:41:20 GMT",
"version": "v2"
}
] | 2021-10-13 | [
[
"Akhmedov",
"E. T.",
""
],
[
"Bazarov",
"K. V.",
""
],
[
"Diakonov",
"D. V.",
""
]
] | We consider interacting massive scalar quantum field theory in the future Rindler wedge. This is a model example of quantum field theory in curved space--time. On this simple example we show how dynamics of correlation functions depends on the choice of initial Cauchy surface, basis of modes and on the choice of initia... | 12.271868 | 11.468202 | 11.838979 | 10.963024 | 11.068393 | 11.092893 | 11.023659 | 10.451968 | 10.21325 | 12.131562 | 11.061585 | 11.145807 | 11.29317 | 11.288479 | 11.0407 | 11.350018 | 11.51181 | 10.850123 | 10.897416 | 11.390876 | 10.974573 |
hep-th/9209096 | null | M. Nolasco, C.Reina | Topological Observables in Semiclassical Field Theories | 11 pages | Phys.Lett.B297:82-88,1992 | 10.1016/0370-2693(92)91073-I | null | hep-th | null | We give a geometrical set up for the semiclassical approximation to euclidean
field theories having families of minima (instantons) parametrized by suitable
moduli spaces ${\cal M}$. The standard examples are of course Yang-Mills theory
and non-linear $\sigma$-models. The relevant space here is a family of measure
sp... | [
{
"created": "Thu, 24 Sep 1992 14:33:08 GMT",
"version": "v1"
}
] | 2010-11-01 | [
[
"Nolasco",
"M.",
""
],
[
"Reina",
"C.",
""
]
] | We give a geometrical set up for the semiclassical approximation to euclidean field theories having families of minima (instantons) parametrized by suitable moduli spaces ${\cal M}$. The standard examples are of course Yang-Mills theory and non-linear $\sigma$-models. The relevant space here is a family of measure spac... | 6.665587 | 7.205472 | 7.015517 | 6.590811 | 6.795198 | 7.057496 | 7.263794 | 7.09219 | 6.804143 | 7.19608 | 6.638 | 6.501803 | 6.660471 | 6.532377 | 6.305393 | 6.269927 | 6.555759 | 6.560817 | 6.619842 | 6.621569 | 6.767437 |
hep-th/0701145 | Changhyun Ahn | Changhyun Ahn | Meta-Stable Brane Configuration with Orientifold 6 Plane | 21 pp, 3 colored figures; stability arguments added in page 11 and
12, a typo in figure 3 corrected, and to appear in JHEP | JHEP 0705:053,2007 | 10.1088/1126-6708/2007/05/053 | null | hep-th | null | We present the intersecting brane configuration of type IIA string theory
corresponding to the meta-stable nonsupersymmetric vacua in four dimensional
N=1 supersymmetric SU(N_c) gauge theory with a symmetric flavor, a conjugate
symmetric flavor and fundamental flavors. By studying the previously known
supersymmetric ... | [
{
"created": "Tue, 16 Jan 2007 07:11:30 GMT",
"version": "v1"
},
{
"created": "Mon, 14 May 2007 04:48:25 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Ahn",
"Changhyun",
""
]
] | We present the intersecting brane configuration of type IIA string theory corresponding to the meta-stable nonsupersymmetric vacua in four dimensional N=1 supersymmetric SU(N_c) gauge theory with a symmetric flavor, a conjugate symmetric flavor and fundamental flavors. By studying the previously known supersymmetric M5... | 7.019738 | 4.452072 | 7.473109 | 4.870704 | 5.134336 | 5.019743 | 4.787019 | 4.72965 | 4.884362 | 8.129018 | 5.008512 | 5.875726 | 6.978805 | 6.1488 | 6.273439 | 5.987451 | 6.142293 | 6.057574 | 5.904567 | 6.95822 | 6.179522 |
hep-th/0207242 | Sedra | A. Boulahoual and M.B. Sedra | The Moyal Momentum Algebra | 6 pages, Latex file | Afr. J. Math. Phys. V2, N1 (2005)111-113 | null | null | hep-th | null | We introduce in this short note some aspects of the Moyal momentum algebra
that we call the Das-Popowicz Mm algebra. Our interest on this algebra is
motivated by the central role that it can play in the formulation of integrable
models and in higher conformal spin theories.
| [
{
"created": "Fri, 26 Jul 2002 19:16:52 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Aug 2002 15:46:15 GMT",
"version": "v2"
},
{
"created": "Mon, 13 Mar 2006 00:34:10 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Boulahoual",
"A.",
""
],
[
"Sedra",
"M. B.",
""
]
] | We introduce in this short note some aspects of the Moyal momentum algebra that we call the Das-Popowicz Mm algebra. Our interest on this algebra is motivated by the central role that it can play in the formulation of integrable models and in higher conformal spin theories. | 18.652111 | 18.717209 | 22.541737 | 18.857094 | 17.13817 | 17.844141 | 18.907316 | 18.913187 | 17.479923 | 27.319317 | 17.30867 | 17.792381 | 21.893848 | 18.150452 | 18.257532 | 18.148197 | 18.717167 | 17.267168 | 18.73773 | 20.184322 | 17.635065 |
hep-th/9608023 | Peter Hodges | P.J. Hodges and Noureddine Mohammedi | Anti-field Formalism and Non-Abelian Duality | 13 pages, LaTeX2e | Phys.Lett. B388 (1996) 761-768 | 10.1016/S0370-2693(96)01210-5 | SHEP 96/18 | hep-th | null | The act of implementing non-Abelian duality in two dimensional sigma models
results unavoidably in an additional reducible symmetry. The Batalin-Vilkovisky
formalism is employed to handle this new symmetry. Valuable lessons are learnt
here with respect to non-Abelian duality. We emphasise, in particular, the
effects ... | [
{
"created": "Mon, 5 Aug 1996 15:02:13 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Hodges",
"P. J.",
""
],
[
"Mohammedi",
"Noureddine",
""
]
] | The act of implementing non-Abelian duality in two dimensional sigma models results unavoidably in an additional reducible symmetry. The Batalin-Vilkovisky formalism is employed to handle this new symmetry. Valuable lessons are learnt here with respect to non-Abelian duality. We emphasise, in particular, the effects of... | 12.431045 | 10.257104 | 12.392658 | 10.045827 | 10.571331 | 11.309834 | 10.240373 | 11.383888 | 9.986576 | 13.099601 | 11.42053 | 11.309013 | 11.484709 | 11.053061 | 11.28172 | 11.290206 | 11.03875 | 11.1648 | 11.120132 | 11.658731 | 12.056306 |
2001.11784 | Eugeny Babichev | Eugeny Babichev | Emergence of ghosts in Horndeski theory | 14 pages, 4 figures; v2: clarifications added, matches published
version | JHEP07(2020)038 | 10.1007/JHEP07(2020)038 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that starting from initial conditions with stable perturbations,
evolution of a galileon scalar field results in the appearance of a ghost later
on. To demonstrate this, we consider a theory with k-essence and cubic galileon
Lagrangians on a fixed Minkowski background. Explicit analytical solutions of
simple ... | [
{
"created": "Fri, 31 Jan 2020 12:04:10 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Jul 2020 19:25:52 GMT",
"version": "v2"
}
] | 2020-08-26 | [
[
"Babichev",
"Eugeny",
""
]
] | We show that starting from initial conditions with stable perturbations, evolution of a galileon scalar field results in the appearance of a ghost later on. To demonstrate this, we consider a theory with k-essence and cubic galileon Lagrangians on a fixed Minkowski background. Explicit analytical solutions of simple wa... | 14.170926 | 14.730153 | 13.637977 | 13.18926 | 13.655481 | 13.66433 | 13.858118 | 13.372827 | 12.736317 | 15.181383 | 12.990989 | 12.440662 | 13.915019 | 13.066686 | 13.067179 | 13.798586 | 12.936749 | 13.11855 | 13.305979 | 13.821051 | 12.92576 |
hep-th/0607022 | Steven Gubser | Joshua J. Friess, Steven S. Gubser, Georgios Michalogiorgakis, and
Silviu S. Pufu | The stress tensor of a quark moving through N=4 thermal plasma | 33 pages, 5 figures. v2: improved low K discussion; other minor
improvements | Phys.Rev.D75:106003,2007 | 10.1103/PhysRevD.75.106003 | PUPT-2201 | hep-th hep-ph | null | We develop the linear equations that describe graviton perturbations of
AdS_5-Schwarzschild generated by a string trailing behind an external quark
moving with constant velocity. Solving these equations allows us to evaluate
the stress tensor in the boundary gauge theory. Components of the stress tensor
exhibit direc... | [
{
"created": "Tue, 4 Jul 2006 19:54:25 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Jul 2006 19:25:14 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Friess",
"Joshua J.",
""
],
[
"Gubser",
"Steven S.",
""
],
[
"Michalogiorgakis",
"Georgios",
""
],
[
"Pufu",
"Silviu S.",
""
]
] | We develop the linear equations that describe graviton perturbations of AdS_5-Schwarzschild generated by a string trailing behind an external quark moving with constant velocity. Solving these equations allows us to evaluate the stress tensor in the boundary gauge theory. Components of the stress tensor exhibit directi... | 12.362459 | 9.920896 | 11.937886 | 10.713514 | 10.569588 | 8.990355 | 10.292445 | 8.770362 | 10.348701 | 14.213964 | 10.121829 | 11.230079 | 11.605532 | 10.948034 | 11.293555 | 10.852662 | 11.473728 | 11.148641 | 11.177001 | 11.830339 | 11.175791 |
hep-th/0103223 | John McGreevy | Shamit Kachru and John McGreevy | M-theory on Manifolds of G_2 Holonomy and Type IIA Orientifolds | 14 pages, minor correction and references added | JHEP 0106:027,2001 | 10.1088/1126-6708/2001/06/027 | SU-ITP-01/14, SLAC-PUB-8799 | hep-th | null | We demonstrate that M-theory compactifications on 7-manifolds of G_2
holonomy, which yield 4d N=1 supersymmetric systems, often admit at special
loci in their moduli space a description as type IIA orientifolds. In this way,
we are able to find new dualities of special IIA orientifolds, including
dualities which rela... | [
{
"created": "Mon, 26 Mar 2001 23:52:59 GMT",
"version": "v1"
},
{
"created": "Wed, 28 Mar 2001 17:53:49 GMT",
"version": "v2"
}
] | 2010-05-28 | [
[
"Kachru",
"Shamit",
""
],
[
"McGreevy",
"John",
""
]
] | We demonstrate that M-theory compactifications on 7-manifolds of G_2 holonomy, which yield 4d N=1 supersymmetric systems, often admit at special loci in their moduli space a description as type IIA orientifolds. In this way, we are able to find new dualities of special IIA orientifolds, including dualities which relate... | 8.045817 | 7.445618 | 8.535869 | 7.144969 | 7.452277 | 8.223799 | 7.620786 | 7.450562 | 7.582144 | 9.961506 | 7.127041 | 7.254573 | 7.897302 | 7.238921 | 7.344853 | 7.487108 | 7.26693 | 7.307917 | 7.459285 | 8.336748 | 7.103294 |
1206.6758 | Gurdeep Sehmbi | Gurdeep S. Sehmbi | Branes and Geometry in String and M-Theory | PhD Thesis, 143 pages | null | null | DCPT-12/27 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This thesis is based on two papers by the author and consists of two parts.
We review the recent developments in the theory of multiple M2-branes and
3-algebras leading to multiple D2-brane theories. The inclusion of flux terms
for the supersymmetric BLG and ABJM theories of closed M2-branes is discussed
and then gen... | [
{
"created": "Thu, 28 Jun 2012 16:40:17 GMT",
"version": "v1"
}
] | 2012-06-29 | [
[
"Sehmbi",
"Gurdeep S.",
""
]
] | This thesis is based on two papers by the author and consists of two parts. We review the recent developments in the theory of multiple M2-branes and 3-algebras leading to multiple D2-brane theories. The inclusion of flux terms for the supersymmetric BLG and ABJM theories of closed M2-branes is discussed and then gener... | 10.898874 | 11.087951 | 11.840097 | 10.529562 | 12.030113 | 11.576443 | 11.115714 | 11.192708 | 10.67689 | 13.145966 | 11.059477 | 10.973843 | 11.22039 | 10.718694 | 11.06497 | 11.133502 | 10.901666 | 10.872443 | 10.982771 | 11.227774 | 11.017045 |
hep-th/0011145 | Kai Chen | Kai Chen, Bo-yu Hou and Wen-Li Yang | The Lax pairs for elliptic C_n and BC_n Ruijsenaars-Schneider models and
their spectral curves | LaTeX2e, 25 pages, 1 table, some references added and rearranged
together with misprints corrected | J. Math. Phys. 42, 4894-4914 (2001) | 10.1063/1.1389091 | null | hep-th | null | We study the elliptic C_n and BC_n Ruijsenaars-Schneider models which is
elliptic generalization of system given in hep-th/0006004. The Lax pairs for
these models are constructed by Hamiltonian reduction technology. We show that
the spectral curves can be parameterized by the involutive integrals of motion
for these ... | [
{
"created": "Thu, 16 Nov 2000 11:27:46 GMT",
"version": "v1"
},
{
"created": "Thu, 23 Nov 2000 04:01:46 GMT",
"version": "v2"
},
{
"created": "Sun, 21 Jan 2001 04:07:21 GMT",
"version": "v3"
}
] | 2012-10-30 | [
[
"Chen",
"Kai",
""
],
[
"Hou",
"Bo-yu",
""
],
[
"Yang",
"Wen-Li",
""
]
] | We study the elliptic C_n and BC_n Ruijsenaars-Schneider models which is elliptic generalization of system given in hep-th/0006004. The Lax pairs for these models are constructed by Hamiltonian reduction technology. We show that the spectral curves can be parameterized by the involutive integrals of motion for these mo... | 11.052197 | 9.669216 | 13.400942 | 9.894304 | 10.902526 | 9.792158 | 10.404895 | 10.226806 | 9.525462 | 12.430659 | 10.131893 | 10.036078 | 12.294315 | 10.556733 | 9.867191 | 10.073794 | 10.166228 | 10.154666 | 10.405783 | 11.947881 | 10.276095 |
hep-th/9511055 | null | V. G. Ksenzov | On the Calculation of the Vacuum Energy Density in Sigma Models | 9 pages, latex | Phys.Lett. B367 (1996) 237-241 | 10.1016/0370-2693(95)01420-9 | EV 95-01 | hep-th hep-ph | null | The vacuum energy density is calculated for the $O(N)$ nonlinear sigma models
in two dimensions. To obtain $\varepsilon_{vac}$ we assume that each point of
the space in which non-perturbative f\/ields are determined can be replaced by
a sphere $S^2$ having a small radius $r$ which approaches zero at the very end
of t... | [
{
"created": "Wed, 8 Nov 1995 13:38:57 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Ksenzov",
"V. G.",
""
]
] | The vacuum energy density is calculated for the $O(N)$ nonlinear sigma models in two dimensions. To obtain $\varepsilon_{vac}$ we assume that each point of the space in which non-perturbative f\/ields are determined can be replaced by a sphere $S^2$ having a small radius $r$ which approaches zero at the very end of the... | 10.465955 | 10.273114 | 9.842816 | 9.521341 | 11.361691 | 11.072571 | 10.504458 | 9.9581 | 9.47538 | 10.368714 | 8.850881 | 9.177173 | 9.776482 | 9.236805 | 9.477614 | 10.031995 | 9.535401 | 9.692688 | 9.133216 | 9.339767 | 9.985168 |
hep-th/9807022 | Adi Armoni | A. Armoni, Y. Frishman and J. Sonnenschein | Screening in Supersymmetric Gauge Theories in Two Dimensions | 8 pages, Latex. Minor changes. Accepted to Phys.Lett.B | Phys.Lett. B449 (1999) 76-80 | 10.1016/S0370-2693(99)00018-0 | TAUP-2509-98, WIS-98/19/July-DPP | hep-th | null | We show that the string tension in N=1 two-dimensional super Yang-Mills
theory vanishes independently of the representation of the quark anti-quark
external source. We argue that this result persists in SQCD_2 and in
two-dimensional gauge theories with extended supersymmetry or in chiral
invariant models with at leas... | [
{
"created": "Thu, 2 Jul 1998 17:31:46 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jan 1999 14:55:16 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Armoni",
"A.",
""
],
[
"Frishman",
"Y.",
""
],
[
"Sonnenschein",
"J.",
""
]
] | We show that the string tension in N=1 two-dimensional super Yang-Mills theory vanishes independently of the representation of the quark anti-quark external source. We argue that this result persists in SQCD_2 and in two-dimensional gauge theories with extended supersymmetry or in chiral invariant models with at least ... | 9.981906 | 9.348005 | 10.667025 | 9.659397 | 9.374247 | 10.534247 | 9.075004 | 9.457096 | 10.245365 | 10.879975 | 9.652813 | 9.36066 | 10.406008 | 9.979288 | 9.824719 | 9.78618 | 9.785731 | 9.500776 | 10.124248 | 10.833294 | 9.176803 |
1309.7273 | Adriano Contillo | Adriano Contillo, Stefan Rechenberger, Frank Saueressig | Renormalization group flow of Ho\v{r}ava-Lifshitz gravity at low
energies | 32 pages, 6 figures | null | 10.1007/JHEP12(2013)017 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The functional renormalization group equation for projectable
Ho\v{r}ava-Lifshitz gravity is used to derive the non-perturbative beta
functions for the Newton's constant, cosmological constant and anisotropy
parameter. The resulting coupled differential equations are studied in detail
and exemplary RG trajectories ar... | [
{
"created": "Fri, 27 Sep 2013 15:24:20 GMT",
"version": "v1"
}
] | 2015-06-17 | [
[
"Contillo",
"Adriano",
""
],
[
"Rechenberger",
"Stefan",
""
],
[
"Saueressig",
"Frank",
""
]
] | The functional renormalization group equation for projectable Ho\v{r}ava-Lifshitz gravity is used to derive the non-perturbative beta functions for the Newton's constant, cosmological constant and anisotropy parameter. The resulting coupled differential equations are studied in detail and exemplary RG trajectories are ... | 5.746613 | 5.643148 | 5.839108 | 5.236338 | 5.607419 | 5.462384 | 5.622298 | 5.616461 | 5.630216 | 6.234427 | 5.448833 | 5.732443 | 5.550781 | 5.41221 | 5.563531 | 5.486822 | 5.544189 | 5.425632 | 5.475121 | 5.766413 | 5.294753 |
hep-th/0507271 | Shahn Majid | Shahn Majid | Noncommutative Model with Spontaneous Time Generation and Planckian
bound | Some corrections to quantum polar coordinates formulae in sec 6. 19
pages ams-latex and 2 .eps figures | J.Math.Phys. 46 (2005) 103520 | 10.1063/1.2084748 | null | hep-th gr-qc math.QA | null | We illustrate the thesis that if time did not exist, we would have to create
it if space is noncommutative, and extend functions by something like
Schroedinger's equation. We propose that the phenomenon is a somewhat general
mechanism within noncommutative geometry for `spontaneous time generation'. We
show in detail... | [
{
"created": "Wed, 27 Jul 2005 18:39:18 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Aug 2005 19:51:09 GMT",
"version": "v2"
},
{
"created": "Wed, 31 Aug 2005 14:30:28 GMT",
"version": "v3"
},
{
"created": "Thu, 20 Oct 2005 19:09:32 GMT",
"version": "v4"
}
] | 2009-11-11 | [
[
"Majid",
"Shahn",
""
]
] | We illustrate the thesis that if time did not exist, we would have to create it if space is noncommutative, and extend functions by something like Schroedinger's equation. We propose that the phenomenon is a somewhat general mechanism within noncommutative geometry for `spontaneous time generation'. We show in detail h... | 13.803686 | 15.669851 | 15.177141 | 13.756553 | 14.794216 | 15.193901 | 16.386131 | 14.976341 | 14.002492 | 15.437448 | 14.355598 | 14.35885 | 14.148868 | 13.868895 | 13.74555 | 14.429254 | 13.873898 | 13.471251 | 13.580944 | 15.024701 | 14.144129 |
2012.13308 | Yangrui Hu | Aleksander J. Cianciara, S. James Gates Jr, Yangrui Hu, and Renee Kirk | The 300 "Correlators" Suggests 4D, $\cal N$ = 1 SUSY Is a Solution to a
Set of Sudoku Puzzles | LaTeX twice, 39 pages, 14 figures, 28 tables (v2 added one table and
associated content, v3 note added in proof comment) | null | 10.1007/JHEP05(2021)077 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A conjecture is made that the weight space for 4D, $\cal N$-extended
supersymmetrical representations is embedded within the permutahedra associated
with permutation groups ${\mathbb{S}}{}_{d}$. Adinkras and Coxeter Groups
associated with minimal representations of 4D, $\cal N$ = 1 supersymmetry
provide evidence supp... | [
{
"created": "Thu, 24 Dec 2020 16:11:33 GMT",
"version": "v1"
},
{
"created": "Fri, 25 Dec 2020 23:33:59 GMT",
"version": "v2"
},
{
"created": "Tue, 29 Dec 2020 14:43:42 GMT",
"version": "v3"
},
{
"created": "Sat, 16 Jan 2021 02:54:24 GMT",
"version": "v4"
},
{
"c... | 2021-05-21 | [
[
"Cianciara",
"Aleksander J.",
""
],
[
"Gates",
"S. James",
"Jr"
],
[
"Hu",
"Yangrui",
""
],
[
"Kirk",
"Renee",
""
]
] | A conjecture is made that the weight space for 4D, $\cal N$-extended supersymmetrical representations is embedded within the permutahedra associated with permutation groups ${\mathbb{S}}{}_{d}$. Adinkras and Coxeter Groups associated with minimal representations of 4D, $\cal N$ = 1 supersymmetry provide evidence suppor... | 12.600623 | 13.023552 | 14.739911 | 11.815327 | 12.921527 | 12.600335 | 12.828462 | 13.113295 | 12.183978 | 15.743582 | 11.773415 | 11.639101 | 12.384349 | 11.739946 | 12.048645 | 11.780845 | 11.485338 | 11.77232 | 11.686269 | 12.291727 | 11.728727 |
0710.5866 | Andrzej Wereszczynski | C. Adam, J. Sanchez-Guillen and A. Wereszczynski | A first integration of some knot soliton models | null | Phys.Lett.B659:761-767,2008 | 10.1016/j.physletb.2007.11.089 | null | hep-th | null | Recently it has been shown that there exists a sector within the
Faddeev-Niemi model for which the equations of motion may be reduced to first
order equations. However, no solutions to that sector have been given. It is
not even known whether this sector contains topologically nontrivial solutions,
at all.
Here, we... | [
{
"created": "Wed, 31 Oct 2007 13:59:19 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Adam",
"C.",
""
],
[
"Sanchez-Guillen",
"J.",
""
],
[
"Wereszczynski",
"A.",
""
]
] | Recently it has been shown that there exists a sector within the Faddeev-Niemi model for which the equations of motion may be reduced to first order equations. However, no solutions to that sector have been given. It is not even known whether this sector contains topologically nontrivial solutions, at all. Here, we sho... | 8.380277 | 7.431849 | 9.674198 | 7.648569 | 7.798415 | 8.051222 | 7.575767 | 7.157663 | 7.437641 | 9.825574 | 7.690173 | 7.68983 | 8.258721 | 7.813134 | 7.824785 | 7.651531 | 7.937723 | 7.729515 | 7.963649 | 8.774158 | 7.830726 |
1003.0991 | Kumar S. Gupta | Kumar S. Gupta, E. Harikumar, Siddhartha Sen and M. Sivakumar | The Central Charge of the Warped AdS^3 Black Hole | 6 pages, Latex file | Mod.Phys.Lett.A25:2065-2070,2010 | 10.1142/S0217732310033438 | SINP/TNP/2010/02 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The AdS/CFT conjecture offers the possibility of a quantum description for a
black hole in terms of a CFT. This has led to the study of general AdS^3 type
black holes with a view to constructing an explicit toy quantum black hole
model. Such a CFT description would be characterized by its central charge and
the dimen... | [
{
"created": "Thu, 4 Mar 2010 09:00:30 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 2010 05:29:13 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Gupta",
"Kumar S.",
""
],
[
"Harikumar",
"E.",
""
],
[
"Sen",
"Siddhartha",
""
],
[
"Sivakumar",
"M.",
""
]
] | The AdS/CFT conjecture offers the possibility of a quantum description for a black hole in terms of a CFT. This has led to the study of general AdS^3 type black holes with a view to constructing an explicit toy quantum black hole model. Such a CFT description would be characterized by its central charge and the dimensi... | 9.791157 | 9.648137 | 10.964404 | 9.148323 | 9.737707 | 9.897152 | 9.723424 | 9.456539 | 9.55 | 10.880376 | 9.810497 | 9.451375 | 9.431993 | 9.800176 | 9.844997 | 9.815258 | 10.102648 | 9.818229 | 9.653484 | 9.885851 | 9.404663 |
1811.11619 | Abhiram Kidambi | Andreas Banlaki, Abhishek Chowdhury, Abhiram Kidambi, Maria Schimpf | On Mathieu moonshine and Gromov-Witten invariants | 28 pages, 2 tables, appendices taken from arXiv:1711.09698. V2:
Corrected typos, added references | null | 10.1007/JHEP02(2020)082 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that a large number of $CY_3$ manifolds are involved in an intricate
way in Mathieu moonshine viz. their Gromov--Witten invariants are related to
the expansion coefficients of the twined/ twisted--twined elliptic genera of
$K3$. We use the string duality between CHL orbifolds of heterotic string
theory on $K3... | [
{
"created": "Wed, 28 Nov 2018 15:19:40 GMT",
"version": "v1"
},
{
"created": "Wed, 8 May 2019 19:03:01 GMT",
"version": "v2"
},
{
"created": "Mon, 6 Jan 2020 04:24:47 GMT",
"version": "v3"
}
] | 2021-06-21 | [
[
"Banlaki",
"Andreas",
""
],
[
"Chowdhury",
"Abhishek",
""
],
[
"Kidambi",
"Abhiram",
""
],
[
"Schimpf",
"Maria",
""
]
] | We show that a large number of $CY_3$ manifolds are involved in an intricate way in Mathieu moonshine viz. their Gromov--Witten invariants are related to the expansion coefficients of the twined/ twisted--twined elliptic genera of $K3$. We use the string duality between CHL orbifolds of heterotic string theory on $K3 \... | 7.354923 | 7.167199 | 9.301857 | 6.852233 | 8.117185 | 7.353905 | 6.696245 | 7.059413 | 6.655879 | 9.676442 | 7.186158 | 6.856578 | 8.161728 | 6.845175 | 7.14194 | 7.014025 | 6.750717 | 7.030326 | 6.944174 | 7.731802 | 6.834645 |
2007.15650 | Junjie Rao | Ryota Kojima, Junjie Rao | Triangulation-free Trivialization of 2-loop MHV Amplituhedron | 10 pages | JHEP 2010 (2020) 140 | 10.1007/JHEP10(2020)140 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article introduces a new approach to implement positivity for the 2-loop
n-particle MHV amplituhedron, circumventing the conventional triangulation with
respect to positive variables of each cell carved out by the sign flips. This
approach is universal for all linear positive conditions and hence free of
case-by... | [
{
"created": "Thu, 30 Jul 2020 17:59:53 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Nov 2020 19:33:46 GMT",
"version": "v2"
}
] | 2020-11-06 | [
[
"Kojima",
"Ryota",
""
],
[
"Rao",
"Junjie",
""
]
] | This article introduces a new approach to implement positivity for the 2-loop n-particle MHV amplituhedron, circumventing the conventional triangulation with respect to positive variables of each cell carved out by the sign flips. This approach is universal for all linear positive conditions and hence free of case-by-c... | 20.371595 | 20.688486 | 23.915653 | 19.723269 | 20.813053 | 21.273497 | 21.998522 | 20.551044 | 20.198149 | 26.027193 | 20.234274 | 21.383806 | 21.449514 | 19.997374 | 20.469242 | 19.855371 | 20.638851 | 20.695517 | 19.770514 | 21.815123 | 19.941298 |
hep-th/9905226 | Gianguido Dall'Agata | Anna Ceresole, Gianguido Dall'Agata, Riccardo D'Auria and Sergio
Ferrara | Spectrum of Type IIB Supergravity on AdS_5 x T^{11}: Predictions on N =
1 SCFT's | 39+1 pages, LaTeX2e, uses package LaTeXsym. Misprints and minor
polishing | Phys.Rev.D61:066001,2000 | 10.1103/PhysRevD.61.066001 | CERN-TH/99-156; DFTT 99/29; LPTENS 99/19 | hep-th | null | We derive the full Kaluza-Klein spectrum of type IIB supergravity
compactified on AdS_5 x T^{11} with T^{11} = (SU(2) x SU(2))/U(1). From the
knowledge of the spectrum and general multiplet shortening conditions, we make
a refined test of the AdS/CFT correspondence, by comparison between various
shortenings of SU(2,2... | [
{
"created": "Mon, 31 May 1999 15:45:07 GMT",
"version": "v1"
},
{
"created": "Mon, 14 Jun 1999 14:38:37 GMT",
"version": "v2"
},
{
"created": "Tue, 27 Jul 1999 16:21:49 GMT",
"version": "v3"
}
] | 2010-04-06 | [
[
"Ceresole",
"Anna",
""
],
[
"Dall'Agata",
"Gianguido",
""
],
[
"D'Auria",
"Riccardo",
""
],
[
"Ferrara",
"Sergio",
""
]
] | We derive the full Kaluza-Klein spectrum of type IIB supergravity compactified on AdS_5 x T^{11} with T^{11} = (SU(2) x SU(2))/U(1). From the knowledge of the spectrum and general multiplet shortening conditions, we make a refined test of the AdS/CFT correspondence, by comparison between various shortenings of SU(2,2|1... | 7.963923 | 6.113677 | 9.202587 | 7.036278 | 7.001148 | 7.186981 | 7.102554 | 7.130975 | 6.777276 | 11.074967 | 7.091433 | 7.382801 | 8.449587 | 7.154639 | 6.98572 | 7.749414 | 6.819134 | 7.516009 | 7.172234 | 8.233043 | 7.263457 |
1112.0260 | Junya Yagi | Junya Yagi | On the six-dimensional origin of the AGT correspondence | References added. 14 pages | JHEP 02 (2012) 020 | 10.1007/JHEP02(2012)020 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We argue that the six-dimensional (2,0) superconformal theory defined on M
\times C, with M being a four-manifold and C a Riemann surface, can be twisted
in a way that makes it topological on M and holomorphic on C. Assuming the
existence of such a twisted theory, we show that its chiral algebra contains a
W-algebra ... | [
{
"created": "Thu, 1 Dec 2011 18:20:34 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Dec 2011 20:40:32 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Feb 2012 14:11:45 GMT",
"version": "v3"
},
{
"created": "Fri, 2 Mar 2012 23:28:14 GMT",
"version": "v4"
}
] | 2012-03-06 | [
[
"Yagi",
"Junya",
""
]
] | We argue that the six-dimensional (2,0) superconformal theory defined on M \times C, with M being a four-manifold and C a Riemann surface, can be twisted in a way that makes it topological on M and holomorphic on C. Assuming the existence of such a twisted theory, we show that its chiral algebra contains a W-algebra wh... | 6.300026 | 6.266806 | 7.872649 | 5.85976 | 5.885062 | 5.657902 | 6.304532 | 5.904684 | 5.673359 | 9.084613 | 6.187057 | 6.017174 | 7.04537 | 5.949137 | 5.86766 | 6.059228 | 5.78914 | 5.865801 | 5.888601 | 6.604094 | 5.679517 |
hep-th/9210075 | Alexandre T. Filippov | A.T. Filippov, A.P. Isaev and A.B. Kurdikov | On Paragrassmann Differential Calculus | 19pp | Theor.Math.Phys. 94 (1993) 150-165; Teor.Mat.Fiz. 94N2 (1993)
213-231 | 10.1007/BF01019327 | null | hep-th | null | Explicit general constructions of paragrassmann calculus with one and many
variables are given. Relations of the paragrassmann calculus to quantum groups
are outlined and possible physics applications are briefly discussed. This
paper is the same as the original 9210075 except added Appendix and minor
changes in Ackn... | [
{
"created": "Wed, 14 Oct 1992 07:11:42 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Nov 1992 09:49:25 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"Filippov",
"A. T.",
""
],
[
"Isaev",
"A. P.",
""
],
[
"Kurdikov",
"A. B.",
""
]
] | Explicit general constructions of paragrassmann calculus with one and many variables are given. Relations of the paragrassmann calculus to quantum groups are outlined and possible physics applications are briefly discussed. This paper is the same as the original 9210075 except added Appendix and minor changes in Acknow... | 18.813723 | 16.771128 | 20.324741 | 14.751362 | 17.032066 | 16.584652 | 16.874987 | 16.718288 | 14.912819 | 19.138538 | 15.747568 | 15.942054 | 18.241047 | 16.683464 | 16.218817 | 15.772715 | 16.4398 | 16.300159 | 16.90073 | 18.919542 | 16.702501 |
2203.15562 | Rajeev Singh | Arpan Das, Wojciech Florkowski, Avdhesh Kumar, Radoslaw Ryblewski,
Rajeev Singh | Semi-classical kinetic theory for massive spin-half fermions with
leading-order spin effects | Revised version | Acta Physica Polonica B vol. 54, article 8-A4 (2023) | 10.5506/APhysPolB.54.8-A4 | INT-PUB-23-032 | hep-th hep-ph nucl-th | http://creativecommons.org/licenses/by/4.0/ | We consider the quantum kinetic-theory description for interacting massive
spin-half fermions using the Wigner function formalism. We derive a general
kinetic theory description assuming that the spin effects appear at the
classical and quantum level. To track the effect of such different
contributions we use the sem... | [
{
"created": "Mon, 28 Mar 2022 09:46:58 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Aug 2023 16:23:56 GMT",
"version": "v2"
}
] | 2023-09-11 | [
[
"Das",
"Arpan",
""
],
[
"Florkowski",
"Wojciech",
""
],
[
"Kumar",
"Avdhesh",
""
],
[
"Ryblewski",
"Radoslaw",
""
],
[
"Singh",
"Rajeev",
""
]
] | We consider the quantum kinetic-theory description for interacting massive spin-half fermions using the Wigner function formalism. We derive a general kinetic theory description assuming that the spin effects appear at the classical and quantum level. To track the effect of such different contributions we use the semi-... | 15.729562 | 15.640715 | 16.776974 | 15.08123 | 16.18844 | 16.529106 | 16.510221 | 15.193285 | 15.053465 | 16.850426 | 15.65372 | 15.863353 | 15.806323 | 15.634664 | 14.682604 | 15.789917 | 15.520945 | 14.644773 | 15.906718 | 16.276606 | 15.432527 |
1512.00249 | Kazuma Shimizu | Tomoki Nosaka, Kazuma Shimizu, Seiji Terashima | Large N behavior of mass deformed ABJM theory | 25 pages,3 figures; v2: typos corrected, a comment on solution II
added, footnotes added, references added | null | 10.1007/JHEP03(2016)063 | YITP-15-106 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, using the localization technique we analyze the large N limit
of the mass deformed Aharony-Bergman-Jafferis-Maldacena (ABJM) theory on the
three sphere with a finite mass parameter and finite Chern-Simons levels. We
find two different solutions of the saddle point equations in the large N
limit. With t... | [
{
"created": "Tue, 1 Dec 2015 13:21:29 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Aug 2016 03:45:49 GMT",
"version": "v2"
}
] | 2016-08-26 | [
[
"Nosaka",
"Tomoki",
""
],
[
"Shimizu",
"Kazuma",
""
],
[
"Terashima",
"Seiji",
""
]
] | In this paper, using the localization technique we analyze the large N limit of the mass deformed Aharony-Bergman-Jafferis-Maldacena (ABJM) theory on the three sphere with a finite mass parameter and finite Chern-Simons levels. We find two different solutions of the saddle point equations in the large N limit. With the... | 5.947845 | 5.071877 | 7.444419 | 5.24383 | 5.329012 | 5.036818 | 4.997544 | 5.175897 | 5.022521 | 6.760713 | 5.382911 | 5.08864 | 5.932207 | 5.35011 | 5.27498 | 5.02812 | 4.9791 | 5.180502 | 5.158171 | 5.793168 | 5.093493 |
hep-th/9311036 | Martin Schlichenmaier | Martin Schlichenmaier | Differential Operator Algebras on compact Riemann Surfaces | 11 pages, AmsTeX 2.1 and psbox macros | null | null | Mannheimer Manuskripte 164 | hep-th alg-geom math.QA | null | Invited talk at the International Symposium on Generalized Symmetries in
Physics at the Arnold-Sommerfeld-Institute, Clausthal, Germany, July 26 -- July
29, 1993. This talk reviews results on the structure of algebras consisting of
meromorphic differential operators which are holomorphic outside a finite set
of point... | [
{
"created": "Fri, 5 Nov 1993 11:08:01 GMT",
"version": "v1"
}
] | 2009-09-25 | [
[
"Schlichenmaier",
"Martin",
""
]
] | Invited talk at the International Symposium on Generalized Symmetries in Physics at the Arnold-Sommerfeld-Institute, Clausthal, Germany, July 26 -- July 29, 1993. This talk reviews results on the structure of algebras consisting of meromorphic differential operators which are holomorphic outside a finite set of points ... | 7.986258 | 9.966765 | 9.09387 | 8.056166 | 8.425024 | 9.516691 | 9.785796 | 8.555742 | 8.982705 | 10.065279 | 8.896585 | 7.628436 | 7.901613 | 7.381824 | 7.825743 | 7.549183 | 7.832108 | 7.345049 | 7.679945 | 7.785685 | 7.809043 |
hep-th/9508085 | Michael Dine | Michael Dine | Coming to Terms with Strongly Coupled Strings | 5 pages compressed postscript | null | null | SCIPP 95/25 | hep-th | null | The holomorphy of the superpotential along with symmetries gives very strong
constraints on any stringy non-perturbative effects. This observation suggests
an approach to string phenomenology. (Presented at ``Strings 95'', March 1995.
| [
{
"created": "Thu, 17 Aug 1995 21:59:08 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Dine",
"Michael",
""
]
] | The holomorphy of the superpotential along with symmetries gives very strong constraints on any stringy non-perturbative effects. This observation suggests an approach to string phenomenology. (Presented at ``Strings 95'', March 1995. | 15.434248 | 12.283621 | 16.931684 | 11.364046 | 12.193845 | 11.020084 | 11.686489 | 10.942475 | 11.215266 | 14.721087 | 10.220342 | 12.017706 | 14.961527 | 12.663713 | 12.971266 | 13.003035 | 12.11323 | 13.518286 | 12.190443 | 14.970922 | 12.038176 |
1904.06154 | Lorenzo Luis Salcedo | C. Garcia-Recio and L. L. Salcedo | Renormalization of vector fields with mass-like coupling in curved
spacetime | 14 pages, no figures | null | 10.1140/epjc/s10052-019-6930-1 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the method of covariant symbols we compute the divergent part of the
effective action of the Proca field with non-minimal mass term. Specifically a
quantum Abelian vector field with a non-derivative coupling to an external
tensor field in curved spacetime in four dimensions is considered. Relatively
explicit ex... | [
{
"created": "Fri, 12 Apr 2019 10:48:57 GMT",
"version": "v1"
}
] | 2019-06-26 | [
[
"Garcia-Recio",
"C.",
""
],
[
"Salcedo",
"L. L.",
""
]
] | Using the method of covariant symbols we compute the divergent part of the effective action of the Proca field with non-minimal mass term. Specifically a quantum Abelian vector field with a non-derivative coupling to an external tensor field in curved spacetime in four dimensions is considered. Relatively explicit expr... | 12.732535 | 11.417185 | 12.427746 | 11.559743 | 12.542194 | 11.206876 | 11.277629 | 11.0701 | 11.407414 | 13.156365 | 11.41344 | 10.982726 | 11.667669 | 11.159627 | 11.283756 | 11.021514 | 11.360868 | 11.355809 | 11.180202 | 11.747355 | 11.06305 |
hep-th/0505193 | Shinji Tsujikawa | Gianluca Calcagni, Shinji Tsujikawa, M Sami | Dark energy and cosmological solutions in second-order string gravity | 35 pages, 7 figures | Class.Quant.Grav.22:3977-4006,2005 | 10.1088/0264-9381/22/19/011 | null | hep-th astro-ph gr-qc hep-ph | null | We study the cosmological evolution based upon a $D$-dimensional action in
low-energy effective string theory in the presence of second-order curvature
corrections and a modulus scalar field (dilaton or compactification modulus). A
barotropic perfect fluid coupled to the scalar field is also allowed. Phase
space anal... | [
{
"created": "Mon, 23 May 2005 02:53:44 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Sep 2005 09:46:09 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Calcagni",
"Gianluca",
""
],
[
"Tsujikawa",
"Shinji",
""
],
[
"Sami",
"M",
""
]
] | We study the cosmological evolution based upon a $D$-dimensional action in low-energy effective string theory in the presence of second-order curvature corrections and a modulus scalar field (dilaton or compactification modulus). A barotropic perfect fluid coupled to the scalar field is also allowed. Phase space analys... | 9.571619 | 9.119905 | 8.819149 | 8.75813 | 8.930241 | 9.145423 | 9.529047 | 8.938725 | 8.924796 | 9.551472 | 8.805153 | 9.242768 | 9.317124 | 9.28159 | 9.163138 | 9.335702 | 9.180035 | 9.282995 | 9.404493 | 9.49574 | 9.279966 |
1901.05869 | Arnau Koemans Collado | Arnau Koemans Collado and Steven Thomas | Eikonal Scattering in Kaluza-Klein Gravity | 27 pages, 4 figures | null | 10.1007/JHEP04(2019)171 | QMUL-PH-19-01 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study eikonal scattering in the context of Kaluza-Klein theory by
considering a massless scalar field coupled to Einstein's gravity in 5D
compactified to 4D on a manifold $M_4\times S^1 $. We also examine various
different kinematic limits of the resulting eikonal. In the ultra-relativistic
scattering case we find... | [
{
"created": "Thu, 17 Jan 2019 16:21:12 GMT",
"version": "v1"
},
{
"created": "Wed, 1 May 2019 10:43:00 GMT",
"version": "v2"
}
] | 2019-05-02 | [
[
"Collado",
"Arnau Koemans",
""
],
[
"Thomas",
"Steven",
""
]
] | We study eikonal scattering in the context of Kaluza-Klein theory by considering a massless scalar field coupled to Einstein's gravity in 5D compactified to 4D on a manifold $M_4\times S^1 $. We also examine various different kinematic limits of the resulting eikonal. In the ultra-relativistic scattering case we find c... | 7.516527 | 7.670457 | 7.449113 | 7.017125 | 6.924528 | 6.908832 | 6.993946 | 6.731749 | 7.318847 | 8.149879 | 6.912772 | 6.860594 | 7.2049 | 7.001255 | 7.102587 | 7.031108 | 7.113862 | 7.159969 | 6.908093 | 7.144023 | 6.938489 |
2106.04568 | Hong-Jian He | Yan-Feng Hang, Hong-Jian He | Structure of Kaluza-Klein Graviton Scattering Amplitudes from
Gravitational Equivalence Theorem and Double-Copy | 90 pages. Final version inclulding the exact KK double-copy of NLO
amplitudes. Conclusions unchanged, typos corrected and references added. Its
companion Letter paper appeared in arXiv:2207.11214 | Phys. Rev. D105 (2022) 084005, no.8 | 10.1103/PhysRevD.105.084005 | null | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We study the structure of scattering amplitudes of the Kaluza-Klein (KK)
gravitons and of the gravitational KK Goldstone bosons in the compactified 5d
General Relativity (GR). We analyze the geometric "Higgs" mechanism for
mass-generation of KK gravitons under compactification with a general $R_\xi$
gauge-fixing, whi... | [
{
"created": "Tue, 8 Jun 2021 17:54:37 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Jun 2021 17:39:40 GMT",
"version": "v2"
},
{
"created": "Fri, 23 Jul 2021 17:36:54 GMT",
"version": "v3"
},
{
"created": "Thu, 28 Jul 2022 17:47:49 GMT",
"version": "v4"
}
] | 2022-07-29 | [
[
"Hang",
"Yan-Feng",
""
],
[
"He",
"Hong-Jian",
""
]
] | We study the structure of scattering amplitudes of the Kaluza-Klein (KK) gravitons and of the gravitational KK Goldstone bosons in the compactified 5d General Relativity (GR). We analyze the geometric "Higgs" mechanism for mass-generation of KK gravitons under compactification with a general $R_\xi$ gauge-fixing, which... | 5.832963 | 5.752357 | 6.522886 | 5.457342 | 6.337972 | 5.604077 | 5.403315 | 5.586372 | 5.563789 | 6.30823 | 5.57832 | 5.707084 | 5.944866 | 5.747489 | 5.843867 | 5.72759 | 5.641542 | 5.713949 | 5.738075 | 5.83105 | 5.704413 |
1210.1856 | Paulina Suchanek | Volker Schomerus and Paulina Suchanek | Liouville's Imaginary Shadow | 31 pages | JHEP12(2012)020 | 10.1007/JHEP12(2012)020 | DESY 12-165 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | N=1 super Liouville field theory is one of the simplest non-rational
conformal field theories. It possesses various important extensions and
interesting applications, e.g. to the AGT relation with 4D gauge theory or the
construction of the OSP(1|2) WZW model. In both setups, the N=1 Liouville field
is accompanied by ... | [
{
"created": "Fri, 5 Oct 2012 20:03:37 GMT",
"version": "v1"
}
] | 2013-05-31 | [
[
"Schomerus",
"Volker",
""
],
[
"Suchanek",
"Paulina",
""
]
] | N=1 super Liouville field theory is one of the simplest non-rational conformal field theories. It possesses various important extensions and interesting applications, e.g. to the AGT relation with 4D gauge theory or the construction of the OSP(1|2) WZW model. In both setups, the N=1 Liouville field is accompanied by an... | 9.1517 | 8.860341 | 10.776743 | 8.722417 | 8.893207 | 9.211745 | 9.012887 | 8.888673 | 8.801133 | 11.659936 | 9.13884 | 8.767954 | 9.509959 | 9.099513 | 8.763402 | 8.38679 | 8.63932 | 8.750799 | 8.563409 | 9.70345 | 8.842058 |
hep-th/0001154 | Christian Jaekel | Christian Jaekel | The Reeh-Schlieder property for ground states | plain tex, 11 pages, An unnecessary strong assumption has been
replaced by a more adequate one in Definition 2.1 | Annalen Phys. 12 (2003) 289-299 | 10.1002/andp.200310012 | null | hep-th | null | Recently it has been shown that the Reeh-Schlieder property w.r.t. thermal
equilibrium states is a direct consequence of locality, additivity and the
relativistic KMS condition. Here we extend this result to ground states.
| [
{
"created": "Mon, 24 Jan 2000 15:37:13 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Jan 2000 13:40:54 GMT",
"version": "v2"
},
{
"created": "Thu, 10 Feb 2000 14:28:49 GMT",
"version": "v3"
}
] | 2009-10-31 | [
[
"Jaekel",
"Christian",
""
]
] | Recently it has been shown that the Reeh-Schlieder property w.r.t. thermal equilibrium states is a direct consequence of locality, additivity and the relativistic KMS condition. Here we extend this result to ground states. | 10.104277 | 6.04309 | 8.007893 | 6.836469 | 8.711544 | 7.10641 | 6.391115 | 6.654337 | 7.556926 | 9.306239 | 7.179073 | 8.690125 | 8.698761 | 7.843483 | 8.88629 | 8.262731 | 8.564017 | 7.773426 | 8.567242 | 9.516233 | 8.137189 |
1308.6425 | Hiroshi Kawabe | Hiroshi Kawabe | Causal dynamical triangulation for non-critical open-closed string field
theory | 15pages, 22figures, typos corrected | Phys.Lett.B729(2014)91-98 | 10.1016/j.physletb.2013.12.046 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extend the 2 dimensional Causal Dynamical Triangulation (CDT) model from
the usual model of closed string to the one of open-closed string. The
matrix-vector model describing the loop gas model is modified so as to possess
the nature of the CDT, i.e. the time foliation structure. Stochastic
quantization method pro... | [
{
"created": "Thu, 29 Aug 2013 10:39:06 GMT",
"version": "v1"
},
{
"created": "Wed, 4 Sep 2013 11:12:56 GMT",
"version": "v2"
}
] | 2014-01-16 | [
[
"Kawabe",
"Hiroshi",
""
]
] | We extend the 2 dimensional Causal Dynamical Triangulation (CDT) model from the usual model of closed string to the one of open-closed string. The matrix-vector model describing the loop gas model is modified so as to possess the nature of the CDT, i.e. the time foliation structure. Stochastic quantization method produ... | 14.475834 | 13.314458 | 14.670644 | 12.311683 | 13.635345 | 13.724697 | 13.064609 | 11.88344 | 13.204915 | 17.807001 | 13.465401 | 12.772086 | 14.111705 | 12.934319 | 13.410489 | 13.62844 | 12.77595 | 13.459597 | 12.807971 | 13.493482 | 12.639661 |
hep-th/9212058 | null | A. Toon | Particle Content in Topological Field Theories | 9p, OUTP-92-30P | Mod.Phys.Lett. A9 (1994) 29-40 | 10.1142/S0217732394000058 | null | hep-th | null | By demanding that the path integral measure of topological field theories be
metric independent, we can derive powerful constraints on the particle content
of a topological field theory as well as on the dimensionality of space-time.
| [
{
"created": "Wed, 9 Dec 1992 18:45:42 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Toon",
"A.",
""
]
] | By demanding that the path integral measure of topological field theories be metric independent, we can derive powerful constraints on the particle content of a topological field theory as well as on the dimensionality of space-time. | 12.843063 | 8.770688 | 8.938256 | 8.841318 | 8.270606 | 7.688607 | 8.923917 | 8.60113 | 8.023599 | 9.624634 | 8.973325 | 9.224614 | 8.783008 | 8.745719 | 8.983738 | 9.110415 | 8.881721 | 9.042108 | 8.857538 | 9.235658 | 8.938968 |
1403.7407 | Elcio Abdalla | Kai Lin and Elcio Abdalla | Holographic Superconductors in a Rotating Spacetime | 9 pages, 5 figures, paper completely rewritten and improved. Version
to appear in EPJC | null | 10.1140/epjc/s10052-014-3144-4 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider holographic superconductors in a rotating black string spacetime.
In view of the mandatory introduction of the $A_\varphi$ component of the
vector potential we are left with three equations to be solved. Their solutions
show that the effect of the rotating parameter $a$ influences the critical
temperature... | [
{
"created": "Fri, 28 Mar 2014 15:05:10 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Jun 2014 19:36:48 GMT",
"version": "v2"
},
{
"created": "Fri, 17 Oct 2014 13:29:42 GMT",
"version": "v3"
}
] | 2015-06-19 | [
[
"Lin",
"Kai",
""
],
[
"Abdalla",
"Elcio",
""
]
] | We consider holographic superconductors in a rotating black string spacetime. In view of the mandatory introduction of the $A_\varphi$ component of the vector potential we are left with three equations to be solved. Their solutions show that the effect of the rotating parameter $a$ influences the critical temperature $... | 10.821809 | 9.2494 | 9.389518 | 8.919654 | 9.231944 | 9.808732 | 9.52027 | 9.726874 | 9.088846 | 9.864198 | 8.737684 | 10.006332 | 8.990052 | 9.230625 | 9.243145 | 9.044927 | 9.28839 | 9.094692 | 9.726544 | 9.032765 | 9.642461 |
hep-th/9806149 | Dongsu Bak | Dongsu Bak, Joohan Lee, and Hyunsoo Min | Dynamics of BPS States in the Dirac-Born-Infeld Theory | 19 pages, 4 figures References added, Typographical errors are
corrected | Phys. Rev. D 59, 045011 (1999) | 10.1103/PhysRevD.59.045011 | UOSTP-98-102, SNUTP-98-059 | hep-th | null | The Dirac-Born-Infeld action with transverse scalar fields is considered to
study the dynamics of various BPS states. We first describe the characteristic
properties of the so-called 1/2 and 1/4 BPS states on the D3 brane, which can
be interpreted as F/D-strings ending on a D3-brane in Type IIB string theory
picture.... | [
{
"created": "Thu, 18 Jun 1998 11:30:05 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Jul 1998 05:20:04 GMT",
"version": "v2"
}
] | 2016-08-25 | [
[
"Bak",
"Dongsu",
""
],
[
"Lee",
"Joohan",
""
],
[
"Min",
"Hyunsoo",
""
]
] | The Dirac-Born-Infeld action with transverse scalar fields is considered to study the dynamics of various BPS states. We first describe the characteristic properties of the so-called 1/2 and 1/4 BPS states on the D3 brane, which can be interpreted as F/D-strings ending on a D3-brane in Type IIB string theory picture. W... | 8.247559 | 7.538021 | 8.423431 | 7.575807 | 7.397147 | 7.319979 | 7.265805 | 7.953173 | 7.378521 | 9.302317 | 7.486475 | 7.663162 | 8.285791 | 7.680641 | 7.72507 | 7.520827 | 7.658639 | 7.651753 | 7.697148 | 8.344943 | 7.553374 |
hep-th/9712081 | Jose Carlos Brunelli | J. C. Brunelli and Ashok Das | A Lax Representation for the Born-Infeld Equation | Latex, 14 pages, Note and references added, incorporating connection
with hyperbolic Monge-Amp\`ere equations | Phys.Lett. B426 (1998) 57-63 | 10.1016/S0370-2693(98)00265-2 | null | hep-th nlin.SI solv-int | null | We study the Born-Infeld equation from a Lagrangian point of view emphasizing
the duality symmetry present in such systems. We obtain the Hamiltonian
formulation directly from the Lagrangian. We also show that this system admits
a dispersionless nonstandard Lax representation which directly leads to all the
conserved... | [
{
"created": "Mon, 8 Dec 1997 16:47:45 GMT",
"version": "v1"
},
{
"created": "Thu, 22 Jan 1998 11:16:52 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Brunelli",
"J. C.",
""
],
[
"Das",
"Ashok",
""
]
] | We study the Born-Infeld equation from a Lagrangian point of view emphasizing the duality symmetry present in such systems. We obtain the Hamiltonian formulation directly from the Lagrangian. We also show that this system admits a dispersionless nonstandard Lax representation which directly leads to all the conserved c... | 10.544477 | 9.952975 | 10.215827 | 9.443022 | 9.446052 | 11.019472 | 9.740413 | 9.853491 | 9.907172 | 9.93839 | 9.410687 | 9.833995 | 10.664459 | 9.964107 | 10.166502 | 9.675642 | 9.642219 | 9.601967 | 9.71666 | 10.41379 | 9.636535 |
2204.12239 | Zi-Qing Xiao | Zi-Qing Xiao, Run-Qiu Yang | On Penrose inequality in holography | 15 pages, 3 figures | null | 10.1103/PhysRevD.107.026013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The recent holographic deduction of Penrose inequality only assumes null
energy condition while the weak or dominant energy condition is required in
usual geometric proof. This paper makes a step toward filling up gap between
these two approaches. For planar/spherically symmetrically asymptotically
Schwarzschild anti... | [
{
"created": "Tue, 26 Apr 2022 11:43:47 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Aug 2022 07:50:42 GMT",
"version": "v2"
}
] | 2023-02-01 | [
[
"Xiao",
"Zi-Qing",
""
],
[
"Yang",
"Run-Qiu",
""
]
] | The recent holographic deduction of Penrose inequality only assumes null energy condition while the weak or dominant energy condition is required in usual geometric proof. This paper makes a step toward filling up gap between these two approaches. For planar/spherically symmetrically asymptotically Schwarzschild anti-d... | 10.915286 | 11.586381 | 10.636248 | 9.987424 | 11.119896 | 11.023758 | 11.237935 | 10.276564 | 10.566488 | 11.163719 | 10.474762 | 10.439176 | 10.740287 | 10.283865 | 10.982224 | 10.513174 | 10.497192 | 10.756731 | 10.635359 | 10.627759 | 10.934815 |
1403.4805 | Ralph Blumenhagen | Ralph Blumenhagen | A Course on Noncommutative Geometry in String Theory | 18 pages, contribution to the proceedings of the Workshop on
Noncommutative Field Theory and Gravity, September 8 - 15, 2013, Corfu,
Greece, v2: refs. added | null | 10.1002/prop.201400014 | MPP-2014-54 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this pedagogical mini course the basics of the derivation of the
noncommutative structures appearing in string theory are reviewed. First we
discuss the well established appearance of the noncommutative Moyal-Weyl
star-product in the correlation functions of open string vertex operators on a
magnetized D-brane. Se... | [
{
"created": "Wed, 19 Mar 2014 14:11:24 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Apr 2014 08:17:26 GMT",
"version": "v2"
}
] | 2016-01-20 | [
[
"Blumenhagen",
"Ralph",
""
]
] | In this pedagogical mini course the basics of the derivation of the noncommutative structures appearing in string theory are reviewed. First we discuss the well established appearance of the noncommutative Moyal-Weyl star-product in the correlation functions of open string vertex operators on a magnetized D-brane. Seco... | 9.766974 | 9.0138 | 9.970582 | 8.664086 | 8.590744 | 8.561888 | 9.116297 | 7.976688 | 7.992323 | 9.948921 | 8.449764 | 8.649988 | 9.189441 | 8.787516 | 8.496892 | 8.757571 | 8.529569 | 8.631392 | 8.585265 | 9.335237 | 8.490582 |
1108.5131 | Chong-Sun Chu | Chong-Sun Chu | A Theory of Non-Abelian Tensor Gauge Field with Non-Abelian Gauge
Symmetry G x G | 18 pages. LaTeX. V2: references and a comment added v3: published
version | null | null | DCPT-11/43 | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Chern-Simon action of the ABJM theory is not gauge invariant in the
presence of a boundary. In the paper arXiv:0909.2333, this was shown to imply
the existence of a Kac-Moody symmetry on the theory of multiple self-dual
strings. In this paper we conjecture that the Kac-Moody symmetry induces a
U(N)x U(N) gauge sy... | [
{
"created": "Thu, 25 Aug 2011 16:48:03 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Sep 2011 14:55:31 GMT",
"version": "v2"
},
{
"created": "Wed, 26 Sep 2012 14:48:00 GMT",
"version": "v3"
}
] | 2012-09-27 | [
[
"Chu",
"Chong-Sun",
""
]
] | The Chern-Simon action of the ABJM theory is not gauge invariant in the presence of a boundary. In the paper arXiv:0909.2333, this was shown to imply the existence of a Kac-Moody symmetry on the theory of multiple self-dual strings. In this paper we conjecture that the Kac-Moody symmetry induces a U(N)x U(N) gauge symm... | 7.928542 | 8.18276 | 9.283133 | 7.337193 | 8.028855 | 7.506502 | 7.625813 | 7.795221 | 7.765188 | 9.540217 | 7.236301 | 7.585463 | 8.222002 | 7.377864 | 7.60788 | 7.766532 | 7.735424 | 7.608684 | 7.526334 | 7.912057 | 7.568276 |
hep-th/0404218 | Lepe Samuel | Norman Cruz and Samuel Lepe | On the thermal description of the BTZ black holes | 7 pages. Accepted by Phys. Lett. B | Phys.Lett. B593 (2004) 235-241 | 10.1016/j.physletb.2004.04.072 | GACG-04/08 | hep-th | null | We investigate the limitations on the thermal description of three
dimensional BTZ black holes. We derive on physical grounds three basic mass
scales that are relevant to characterize these limitations. The Planck mass in
2+1 dimensions indicate the limits where the black hole can emit Hawking's
radiation. We show th... | [
{
"created": "Tue, 27 Apr 2004 21:49:16 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Cruz",
"Norman",
""
],
[
"Lepe",
"Samuel",
""
]
] | We investigate the limitations on the thermal description of three dimensional BTZ black holes. We derive on physical grounds three basic mass scales that are relevant to characterize these limitations. The Planck mass in 2+1 dimensions indicate the limits where the black hole can emit Hawking's radiation. We show that... | 20.704014 | 20.869223 | 18.806301 | 18.091833 | 21.350508 | 20.521717 | 19.617357 | 19.37742 | 19.2428 | 19.560125 | 19.345652 | 20.371464 | 19.846338 | 19.207554 | 18.81871 | 19.233065 | 19.357796 | 20.007378 | 19.957811 | 19.868505 | 19.028242 |
hep-th/0309215 | Plamen Bozhilov | P. Bozhilov | M2-brane Solutions in AdS_7xS^4 | LaTeX, 18 pages, no figures; V2: cosmetic changes to match the
version published in JHEP | JHEP 0310 (2003) 032 | 10.1088/1126-6708/2003/10/032 | null | hep-th | null | We consider different M2-brane configurations in the M-theory AdS_7xS^4
background, with field theory dual A_{N-1}(2,0) SCFT. New membrane solutions
are found and compared with the recently obtained ones.
| [
{
"created": "Tue, 23 Sep 2003 09:22:24 GMT",
"version": "v1"
},
{
"created": "Wed, 5 Nov 2003 09:30:32 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Bozhilov",
"P.",
""
]
] | We consider different M2-brane configurations in the M-theory AdS_7xS^4 background, with field theory dual A_{N-1}(2,0) SCFT. New membrane solutions are found and compared with the recently obtained ones. | 12.905227 | 9.894874 | 14.653016 | 10.831339 | 9.84701 | 8.001247 | 9.371223 | 8.63012 | 10.090809 | 16.998129 | 9.974272 | 9.762647 | 12.285765 | 9.710557 | 10.260433 | 9.787427 | 10.237987 | 10.117146 | 10.411922 | 12.083194 | 10.071809 |
1903.06757 | Jean-Luc Lehners | Alice Di Tucci and Jean-Luc Lehners | The No-Boundary Proposal as a Path Integral with Robin Boundary
Conditions | 5 pages, 3 figures, v2: replaced with published version | Phys. Rev. Lett. 122, 201302 (2019) | 10.1103/PhysRevLett.122.201302 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Realising the no-boundary proposal of Hartle and Hawking as a consistent
gravitational path integral has been a long-standing puzzle. In particular, it
was demonstrated by Feldbrugge et al. that the sum over all universes starting
from zero size results in an unstable saddle point geometry. Here we show that
in the c... | [
{
"created": "Fri, 15 Mar 2019 19:00:38 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Jun 2019 08:46:47 GMT",
"version": "v2"
}
] | 2019-06-04 | [
[
"Di Tucci",
"Alice",
""
],
[
"Lehners",
"Jean-Luc",
""
]
] | Realising the no-boundary proposal of Hartle and Hawking as a consistent gravitational path integral has been a long-standing puzzle. In particular, it was demonstrated by Feldbrugge et al. that the sum over all universes starting from zero size results in an unstable saddle point geometry. Here we show that in the con... | 9.469459 | 9.395376 | 9.254706 | 8.885716 | 9.82252 | 10.084309 | 9.658607 | 8.674166 | 9.626975 | 10.037265 | 9.97231 | 8.518247 | 8.62585 | 8.491995 | 8.656759 | 8.643459 | 8.698846 | 8.387421 | 8.771585 | 9.16271 | 8.678473 |
1110.0488 | Federico Galli | V. Balasubramanian, A. Bernamonti, N. Copland, B. Craps and F. Galli | Thermalization of mutual and tripartite information in strongly coupled
two dimensional conformal field theories | 12 pages, 8 figures, v2: cosmetic changes to match the published
version | PhysRevD.84.105017,2011 | 10.1103/PhysRevD.84.105017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The mutual and tripartite information between pairs and triples of disjoint
regions in a quantum field theory are sensitive probes of the spread of
correlations in an equilibrating system. We compute these quantities in
strongly coupled two-dimensional conformal field theories with a gravity dual
following the homoge... | [
{
"created": "Mon, 3 Oct 2011 20:27:53 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Dec 2011 18:24:52 GMT",
"version": "v2"
}
] | 2011-12-05 | [
[
"Balasubramanian",
"V.",
""
],
[
"Bernamonti",
"A.",
""
],
[
"Copland",
"N.",
""
],
[
"Craps",
"B.",
""
],
[
"Galli",
"F.",
""
]
] | The mutual and tripartite information between pairs and triples of disjoint regions in a quantum field theory are sensitive probes of the spread of correlations in an equilibrating system. We compute these quantities in strongly coupled two-dimensional conformal field theories with a gravity dual following the homogeno... | 11.191794 | 10.477982 | 11.282385 | 9.631062 | 10.450933 | 10.225038 | 10.510929 | 9.436962 | 9.291287 | 12.643934 | 9.758357 | 10.458509 | 10.684481 | 10.140221 | 10.101173 | 10.174492 | 10.126505 | 10.431813 | 9.927443 | 10.296778 | 10.305214 |
hep-th/9810125 | Robert Marnelius | Robert Marnelius, Niclas Sandstrom | Basics of BRST quantization on inner product spaces | 32 pages,Latexfile,improved presentation and several new remarks | Int.J.Mod.Phys. A15 (2000) 833-868 | 10.1142/S0217751X00000409 | ITP-Goteborg 98-16 | hep-th | null | There is an elaborated abstract form of BRST quantization on inner product
spaces within the operator formalism which leads to BRST invariant states of
the form |ph>=e^{[Q,\psi]} |\phi> where \psi is a gauge fixing fermion, and
where |\phi> is a BRST invariant state determined by simple hermitian
conditions. These st... | [
{
"created": "Fri, 16 Oct 1998 10:27:22 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Aug 1999 09:05:07 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Marnelius",
"Robert",
""
],
[
"Sandstrom",
"Niclas",
""
]
] | There is an elaborated abstract form of BRST quantization on inner product spaces within the operator formalism which leads to BRST invariant states of the form |ph>=e^{[Q,\psi]} |\phi> where \psi is a gauge fixing fermion, and where |\phi> is a BRST invariant state determined by simple hermitian conditions. These stat... | 13.203026 | 11.110937 | 14.393455 | 11.759231 | 12.713292 | 12.085761 | 12.058415 | 11.167275 | 12.070122 | 15.335524 | 11.619189 | 11.627767 | 12.825138 | 11.760183 | 12.579018 | 11.951658 | 11.632477 | 11.695341 | 11.79936 | 13.146025 | 11.874224 |
hep-th/9710179 | Dr R. Szabo | L. Cooper, I.I. Kogan and R.J. Szabo | Mirror Maps in Chern-Simons Gauge Theory | 40 pages LaTeX, 4 postscript files, uses psfig.sty; minor textual
changes, typos corrected, references added | Annals Phys. 268 (1998) 61-104 | 10.1006/aphy.1998.5832 | OUTP-97-57P | hep-th cond-mat | null | We describe mirror symmetry in N=2 superconformal field theories in terms of
a dynamical topology changing process of the principal fiber bundle associated
with a topological membrane. We show that the topological symmetries of
Calabi-Yau sigma-models can be obtained from discrete geometric transformations
of compact... | [
{
"created": "Thu, 23 Oct 1997 19:17:25 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Mar 1998 18:00:59 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Cooper",
"L.",
""
],
[
"Kogan",
"I. I.",
""
],
[
"Szabo",
"R. J.",
""
]
] | We describe mirror symmetry in N=2 superconformal field theories in terms of a dynamical topology changing process of the principal fiber bundle associated with a topological membrane. We show that the topological symmetries of Calabi-Yau sigma-models can be obtained from discrete geometric transformations of compact C... | 10.577745 | 11.002855 | 11.515119 | 9.733312 | 10.397696 | 9.782089 | 9.967138 | 9.519835 | 9.710034 | 11.182065 | 9.628543 | 9.588247 | 10.58459 | 9.821035 | 9.643772 | 9.681406 | 9.976346 | 9.169727 | 9.606825 | 10.125564 | 9.373797 |
hep-th/0406172 | Peng Wang | Peng Wang, Xin-He Meng (Nankai U.) | Note on the Radion Effective Potential in the Presence of Branes | 6 pages, no figures. Some discussion clarified, conclusion unchanged.
To appear in Phys. Rev. D | Phys.Rev. D70 (2004) 087901 | 10.1103/PhysRevD.70.087901 | null | hep-th gr-qc hep-ph | null | In String Theory compactification, branes are often invoked to get the
desired form of the radion effective potential. Current popular way of doing
this assumes that the introduction of branes will not modify the background
geometry in an important way. In this paper, we show by an explicit example
that at least in t... | [
{
"created": "Mon, 21 Jun 2004 08:56:22 GMT",
"version": "v1"
},
{
"created": "Sun, 12 Sep 2004 10:25:15 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Wang",
"Peng",
"",
"Nankai U."
],
[
"Meng",
"Xin-He",
"",
"Nankai U."
]
] | In String Theory compactification, branes are often invoked to get the desired form of the radion effective potential. Current popular way of doing this assumes that the introduction of branes will not modify the background geometry in an important way. In this paper, we show by an explicit example that at least in the... | 10.098083 | 8.35974 | 8.80848 | 8.129324 | 8.317103 | 8.53125 | 8.930087 | 9.131439 | 8.971556 | 8.905106 | 9.061922 | 8.941716 | 8.896452 | 8.596494 | 8.791218 | 8.670577 | 8.903997 | 8.753923 | 8.491851 | 8.599323 | 9.008051 |
2103.08596 | Michael Knyazev | M. A. Knyazev | Kink-like solution for the Lorentz0violating \phi^4 theory equation of
motion with dissipation | 7 pages | null | null | null | hep-th nlin.PS nlin.SI | http://creativecommons.org/licenses/by/4.0/ | A (1+1)-dimension equation of motion for \phi^4 theory is considered for the
case of simultaneou taking into account the processes of dissipation and
violation the Lorentz-invariance. A topological non-trivial solution of
one-kink type for this equation is constructed in an analytical form. The
modofied Hirota method... | [
{
"created": "Mon, 15 Mar 2021 12:54:27 GMT",
"version": "v1"
}
] | 2021-03-17 | [
[
"Knyazev",
"M. A.",
""
]
] | A (1+1)-dimension equation of motion for \phi^4 theory is considered for the case of simultaneou taking into account the processes of dissipation and violation the Lorentz-invariance. A topological non-trivial solution of one-kink type for this equation is constructed in an analytical form. The modofied Hirota method f... | 16.427479 | 15.242851 | 16.241159 | 14.836167 | 15.837565 | 14.575051 | 15.469081 | 15.870428 | 13.123243 | 16.595263 | 13.718933 | 14.402902 | 14.734196 | 14.369053 | 14.304749 | 14.592852 | 13.723323 | 14.262478 | 13.617923 | 14.066186 | 14.129366 |
1002.1831 | Victor Mikhaylov | Victor Mikhaylov | On the Fermionic Frequencies of Circular Strings | 13 pages, 1 figure | J.Phys.A43:335401,2010 | 10.1088/1751-8113/43/33/335401 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the semiclassical computation of the fluctuation spectrum around
different circular string solutions in AdS_5xS^5 and AdS_4xCP^3, starting from
the Green-Schwarz action. It has been known that the results for these
frequencies obtained from the algebraic curve and from the worldsheet
computations sometimes... | [
{
"created": "Tue, 9 Feb 2010 11:59:32 GMT",
"version": "v1"
}
] | 2014-11-20 | [
[
"Mikhaylov",
"Victor",
""
]
] | We revisit the semiclassical computation of the fluctuation spectrum around different circular string solutions in AdS_5xS^5 and AdS_4xCP^3, starting from the Green-Schwarz action. It has been known that the results for these frequencies obtained from the algebraic curve and from the worldsheet computations sometimes d... | 9.884552 | 8.024911 | 10.72635 | 9.116345 | 8.890852 | 9.246001 | 8.297436 | 8.192271 | 7.734684 | 11.088467 | 8.515916 | 8.578237 | 9.991323 | 8.682455 | 8.793855 | 8.805525 | 8.615797 | 9.020421 | 8.858086 | 10.912169 | 8.707241 |
hep-th/0208043 | Omer Faruk Dayi | O.F. Dayi and B. Yapiskan | Hamiltonian formulation of Noncommutative D3--Brane | 15 pages, no figures | JHEP 0210 (2002) 022 | 10.1088/1126-6708/2002/10/022 | null | hep-th | null | Lagrangians of the Abelian Gauge Theory and its dual are related in terms of
a shifted action. We show that in d=4 constrained Hamiltonian formulation of
the shifted action yields Hamiltonian description of the dual theory, without
referring to its Lagrangian. We apply this method, at the first order in the
noncommut... | [
{
"created": "Tue, 6 Aug 2002 10:27:54 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Dayi",
"O. F.",
""
],
[
"Yapiskan",
"B.",
""
]
] | Lagrangians of the Abelian Gauge Theory and its dual are related in terms of a shifted action. We show that in d=4 constrained Hamiltonian formulation of the shifted action yields Hamiltonian description of the dual theory, without referring to its Lagrangian. We apply this method, at the first order in the noncommutat... | 9.046583 | 9.213199 | 9.222955 | 8.495584 | 8.993199 | 8.503013 | 9.404125 | 9.016203 | 8.426326 | 10.432873 | 8.659813 | 8.465723 | 8.811829 | 8.405737 | 8.595099 | 8.682885 | 8.663898 | 8.633862 | 8.641681 | 8.857494 | 8.337571 |
2008.03376 | Francisco Fern\'andez Dr. | Francisco M. Fern\'andez | Comment on: "Relativistic quantum dynamics of a charged particle in
cosmic string spacetime in the presence of magnetic field and scalar
potential''. Eur. Phys. J. C (2012) 72:2051 | null | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the results of a paper on ``Relativistic quantum dynamics of a
charged particle in cosmic string spacetime in the presence of magnetic field
and scalar potential''. We show that the authors did not obtain the spectrum of
the eigenvalue equation but only one eigenvalue for a specific relationship
between mo... | [
{
"created": "Wed, 15 Jul 2020 19:00:27 GMT",
"version": "v1"
}
] | 2020-08-11 | [
[
"Fernández",
"Francisco M.",
""
]
] | We analyze the results of a paper on ``Relativistic quantum dynamics of a charged particle in cosmic string spacetime in the presence of magnetic field and scalar potential''. We show that the authors did not obtain the spectrum of the eigenvalue equation but only one eigenvalue for a specific relationship between mode... | 11.392683 | 11.718458 | 11.656936 | 10.94558 | 11.356181 | 11.461105 | 13.079228 | 10.897261 | 10.139312 | 10.040056 | 10.863381 | 10.49993 | 11.357001 | 10.436883 | 10.438921 | 10.794731 | 10.543955 | 10.163596 | 10.658563 | 10.656387 | 10.646409 |
1009.2947 | Yuko Urakawa | Yuko Urakawa and Takahiro Tanaka | Natural selection of inflationary vacuum required by infra-red
regularity and gauge-invariance | 12 pages; v3: several descriptions are added; v4: accepted version in
PTP | Prog.Theor.Phys.125:1067-1089,2011 | 10.1143/PTP.125.1067 | YITP-10-81 | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has been an issue of debate whether the inflationary infrared(IR)
divergences are physical or not. Our claim is that, at least, in single-field
models, the answer is "No," and that the spurious IR divergence is originating
from the careless treatment of the gauge modes. In our previous work we have
explicitly show... | [
{
"created": "Wed, 15 Sep 2010 15:00:23 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Oct 2010 15:14:47 GMT",
"version": "v2"
},
{
"created": "Thu, 10 Feb 2011 23:11:36 GMT",
"version": "v3"
},
{
"created": "Sat, 21 May 2011 15:32:53 GMT",
"version": "v4"
}
] | 2011-08-19 | [
[
"Urakawa",
"Yuko",
""
],
[
"Tanaka",
"Takahiro",
""
]
] | It has been an issue of debate whether the inflationary infrared(IR) divergences are physical or not. Our claim is that, at least, in single-field models, the answer is "No," and that the spurious IR divergence is originating from the careless treatment of the gauge modes. In our previous work we have explicitly shown ... | 9.65846 | 7.632482 | 9.300791 | 8.206362 | 8.303258 | 7.818162 | 8.447781 | 7.843469 | 7.845077 | 9.30311 | 9.038712 | 8.378715 | 8.627602 | 8.437218 | 8.578007 | 8.49468 | 8.405159 | 8.257984 | 8.250853 | 8.497605 | 8.332416 |
1605.06725 | John Klauder | John R. Klauder | Mixed Models: Combining Incompatible Scalar Models in Any Spacetime
Dimension | 14 pages | null | 10.1142/S0217751X17500014 | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Traditionally, covariant scalar field theory models are either super
renormalizable, strictly renormalizable, or nonrenormalizable. The goal of
`Mixed Models' is to make sense of sums of these distinct examples, e.g.,
$g\varphi^4_3+g'\varphi^6_3+g''\varphi^8_3$, which includes an example of each
kind for spacetime di... | [
{
"created": "Sun, 22 May 2016 01:46:42 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Jan 2017 22:54:10 GMT",
"version": "v2"
}
] | 2017-02-01 | [
[
"Klauder",
"John R.",
""
]
] | Traditionally, covariant scalar field theory models are either super renormalizable, strictly renormalizable, or nonrenormalizable. The goal of `Mixed Models' is to make sense of sums of these distinct examples, e.g., $g\varphi^4_3+g'\varphi^6_3+g''\varphi^8_3$, which includes an example of each kind for spacetime dime... | 10.795995 | 11.497341 | 11.113042 | 11.236678 | 11.600399 | 11.413138 | 11.823637 | 11.14379 | 11.309736 | 12.440052 | 10.491427 | 10.817984 | 10.731092 | 10.411424 | 10.495749 | 10.422928 | 10.373128 | 10.419394 | 10.407902 | 10.945743 | 10.07055 |
1511.08187 | Philipp Kleinert | Ville Keranen, Philipp Kleinert | Thermalization of Wightman functions in AdS/CFT and quasinormal modes | 15 pages, 12 figures; v2: typos corrected, conclusions clarified; v3:
modified section IV, added Appendices A-D, as published in PRD | Phys. Rev. D 94, 026010 (2016) | 10.1103/PhysRevD.94.026010 | OUTP-15-29P | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the time evolution of Wightman two-point functions of scalar fields
in AdS$_3$-Vaidya, a spacetime undergoing gravitational collapse. In the
boundary field theory, the collapse corresponds to a quench process where the
dual 1+1 dimensional CFT is taken out of equilibrium and subsequently
thermalizes. From th... | [
{
"created": "Wed, 25 Nov 2015 20:19:06 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Dec 2015 15:57:43 GMT",
"version": "v2"
},
{
"created": "Wed, 10 Aug 2016 16:22:57 GMT",
"version": "v3"
}
] | 2016-08-11 | [
[
"Keranen",
"Ville",
""
],
[
"Kleinert",
"Philipp",
""
]
] | We study the time evolution of Wightman two-point functions of scalar fields in AdS$_3$-Vaidya, a spacetime undergoing gravitational collapse. In the boundary field theory, the collapse corresponds to a quench process where the dual 1+1 dimensional CFT is taken out of equilibrium and subsequently thermalizes. From the ... | 6.197873 | 5.916273 | 6.242495 | 5.605246 | 5.644129 | 5.547598 | 5.653175 | 5.625815 | 5.72157 | 6.596683 | 5.807947 | 5.851806 | 5.96144 | 5.732986 | 5.855063 | 5.653128 | 5.707099 | 5.693655 | 5.794016 | 5.871878 | 5.836652 |
1401.1197 | Luis Apolo | Luis Apolo and Massimo Porrati | Free boundary conditions and the AdS$_3$/CFT$_2$ correspondence | 27 pages; v2: corrected sign of Kac-Moody level, added comments on
unitarity of the dual theory, added references, published version | JHEP 03 (2014) 116 | 10.1007/JHEP03(2014)116 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the recently proposed free boundary conditions for AdS$_3$ are
dual to two-dimensional quantum gravity in certain fixed gauges. In particular,
we note that an appropriate identification of the generator of Virasoro
transformations leads to a vanishing total central charge in agreement with the
theory at ... | [
{
"created": "Mon, 6 Jan 2014 20:53:33 GMT",
"version": "v1"
},
{
"created": "Tue, 1 Apr 2014 00:05:34 GMT",
"version": "v2"
}
] | 2014-04-02 | [
[
"Apolo",
"Luis",
""
],
[
"Porrati",
"Massimo",
""
]
] | We show that the recently proposed free boundary conditions for AdS$_3$ are dual to two-dimensional quantum gravity in certain fixed gauges. In particular, we note that an appropriate identification of the generator of Virasoro transformations leads to a vanishing total central charge in agreement with the theory at th... | 11.236391 | 10.896512 | 11.362312 | 10.136189 | 10.413906 | 10.329473 | 10.688037 | 10.694387 | 10.210168 | 13.444189 | 9.245717 | 9.364637 | 9.912422 | 9.278669 | 9.208919 | 9.842742 | 9.902401 | 9.582607 | 9.567978 | 10.16138 | 9.227094 |
hep-th/9308121 | Christof Schmidhuber | Christof Schmidhuber, Caltech Ph.D. thesis | Extending the Theory of Random Surfaces | 75 pages, Tex | null | null | null | hep-th | null | The theory of embedded random surfaces, equivalent to two--dimensional
quantum gravity coupled to matter, is reviewed, further developed and partly
generalized to four dimensions. It is shown that the action of the Liouville
field theory that describes random surfaces contains terms that have not been
noticed previou... | [
{
"created": "Thu, 26 Aug 1993 15:04:13 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Schmidhuber",
"Christof",
""
],
[
"thesis",
"Caltech Ph. D.",
""
]
] | The theory of embedded random surfaces, equivalent to two--dimensional quantum gravity coupled to matter, is reviewed, further developed and partly generalized to four dimensions. It is shown that the action of the Liouville field theory that describes random surfaces contains terms that have not been noticed previousl... | 7.680332 | 7.131768 | 7.887912 | 6.978093 | 7.750098 | 7.20976 | 7.213747 | 6.777203 | 7.081196 | 8.031503 | 7.270396 | 6.727325 | 7.329411 | 6.941081 | 6.979215 | 6.840101 | 6.758049 | 6.834274 | 6.889087 | 7.210708 | 6.859454 |
2209.00008 | Petr Kravchuk | Simon Caron-Huot, Murat Kologlu, Petr Kravchuk, David Meltzer, David
Simmons-Duffin | Detectors in weakly-coupled field theories | 58 pages + appendices, 21 figure | null | 10.1007/JHEP04(2023)014 | CALT-TH 2022-31 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate a study of asymptotic detector operators in weakly-coupled field
theories. These operators describe measurements that can be performed at future
null infinity in a collider experiment. In a conformal theory they can be
identified with light-ray operators, and thus have a direct relation to the
spectrum of... | [
{
"created": "Wed, 31 Aug 2022 18:00:00 GMT",
"version": "v1"
}
] | 2023-04-26 | [
[
"Caron-Huot",
"Simon",
""
],
[
"Kologlu",
"Murat",
""
],
[
"Kravchuk",
"Petr",
""
],
[
"Meltzer",
"David",
""
],
[
"Simmons-Duffin",
"David",
""
]
] | We initiate a study of asymptotic detector operators in weakly-coupled field theories. These operators describe measurements that can be performed at future null infinity in a collider experiment. In a conformal theory they can be identified with light-ray operators, and thus have a direct relation to the spectrum of t... | 8.594404 | 8.028673 | 9.232452 | 8.131777 | 8.613453 | 8.558151 | 8.33785 | 8.444132 | 8.496645 | 8.873766 | 8.009558 | 8.363843 | 8.162243 | 8.246785 | 8.501972 | 8.579059 | 8.487326 | 8.559342 | 8.278644 | 8.54878 | 8.237775 |
hep-th/0404173 | Andrei Mikhailov | Andrei Mikhailov | Supersymmetric null-surfaces | v4: added a reference to the earlier work; corrected the formula for
the stabilizer of the BMN vacuum; added the discussion of the complex
structure of the odd coordinates in Section 3.2 | JHEP0409:068,2004 | 10.1088/1126-6708/2004/09/068 | CALT-68-2494 | hep-th | null | Single trace operators with the large R-charge in supersymmetric Yang-Mills
theory correspond to the null-surfaces in $AdS_5\times S^5$. We argue that the
moduli space of the null-surfaces is the space of contours in the
super-Grassmanian parametrizing the complex $(2|2)$-dimensional subspaces of
the complex $(4|4)$-... | [
{
"created": "Thu, 22 Apr 2004 18:17:50 GMT",
"version": "v1"
},
{
"created": "Fri, 14 May 2004 21:34:20 GMT",
"version": "v2"
},
{
"created": "Mon, 20 Sep 2004 23:58:00 GMT",
"version": "v3"
},
{
"created": "Sat, 16 Apr 2005 01:08:33 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Mikhailov",
"Andrei",
""
]
] | Single trace operators with the large R-charge in supersymmetric Yang-Mills theory correspond to the null-surfaces in $AdS_5\times S^5$. We argue that the moduli space of the null-surfaces is the space of contours in the super-Grassmanian parametrizing the complex $(2|2)$-dimensional subspaces of the complex $(4|4)$-di... | 7.064222 | 6.985558 | 7.74134 | 6.600515 | 6.927669 | 7.102547 | 6.345049 | 6.145371 | 6.216593 | 7.707109 | 6.434375 | 6.105466 | 6.654707 | 6.251832 | 6.333647 | 6.286781 | 6.650658 | 6.215245 | 6.329749 | 6.659029 | 6.107366 |
2201.10503 | Soumitra SenGupta | Arko Bhaumik and Soumitra SenGupta | Moduli stabilization with bulk scalar in nested doubly warped braneworld
model | 19 Pages, 1 Figure | null | 10.1140/epjc/s10052-022-10973-y | null | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | We examine the modulus stabilization mechanism of a warped geometry model
with nested warping. Such a model with multiple moduli is known to offer a
possible resolution of the fermion mass hierarchy problem in the standard
model. A six dimensional doubly warped braneworld model under consideration
admits two distinct... | [
{
"created": "Tue, 25 Jan 2022 17:53:16 GMT",
"version": "v1"
}
] | 2022-12-14 | [
[
"Bhaumik",
"Arko",
""
],
[
"SenGupta",
"Soumitra",
""
]
] | We examine the modulus stabilization mechanism of a warped geometry model with nested warping. Such a model with multiple moduli is known to offer a possible resolution of the fermion mass hierarchy problem in the standard model. A six dimensional doubly warped braneworld model under consideration admits two distinct m... | 12.146439 | 11.960942 | 12.013017 | 11.78904 | 12.589872 | 12.501904 | 12.191708 | 11.828038 | 11.243694 | 12.462064 | 11.975898 | 11.896094 | 12.202766 | 11.445549 | 11.791636 | 11.535996 | 11.732839 | 11.491723 | 11.637499 | 11.741192 | 11.588231 |
hep-th/0310065 | Dzo Mikulovic | Dzo Mikulovic | Seiberg-Witten Map for Superfields on Canonically Deformed N=1, d=4
Superspace | 24 pages, LaTeX; typos corrected, two comments added | JHEP 0401 (2004) 063 | 10.1088/1126-6708/2004/01/063 | LMU-TPW 2003-10 | hep-th | null | In this paper we construct Seiberg-Witten maps for superfields on canonically
deformed N=1, d=4 Minkowski and Euclidean superspace. On Minkowski superspace
we show that the Seiberg-Witten map is not compatible with locality,
(anti)chirality and supersymmetry at the same time. On Euclidean superspace we
show that ther... | [
{
"created": "Tue, 7 Oct 2003 15:07:03 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Oct 2003 10:00:16 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Feb 2004 11:07:13 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Mikulovic",
"Dzo",
""
]
] | In this paper we construct Seiberg-Witten maps for superfields on canonically deformed N=1, d=4 Minkowski and Euclidean superspace. On Minkowski superspace we show that the Seiberg-Witten map is not compatible with locality, (anti)chirality and supersymmetry at the same time. On Euclidean superspace we show that there ... | 3.416033 | 3.35987 | 3.679043 | 3.124318 | 3.153056 | 3.332039 | 3.280512 | 3.081578 | 3.198814 | 3.588023 | 3.208888 | 3.220744 | 3.350865 | 3.213844 | 3.192849 | 3.290508 | 3.292032 | 3.136897 | 3.332131 | 3.39373 | 3.179269 |
hep-th/9807008 | Bjoern Andreas | B. Andreas, G. Curio and D. Lust | The Neveu-Schwarz Five-Brane and its Dual Geometries | 18pp, added references | JHEP 9810:022,1998 | 10.1088/1126-6708/1998/10/022 | null | hep-th | null | In this paper we discuss two aspects of duality transformations on the
Neveu-Schwarz (NS) 5-brane solutions in type II and heterotic string theories.
First we demonstrate that the non-extremal NS 5-brane background is U-dual to
its CGHS limit, a two-dimensional black hole times $S^3\times T^5$; an
intermediate step i... | [
{
"created": "Wed, 1 Jul 1998 16:33:38 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Jul 1998 14:42:15 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Andreas",
"B.",
""
],
[
"Curio",
"G.",
""
],
[
"Lust",
"D.",
""
]
] | In this paper we discuss two aspects of duality transformations on the Neveu-Schwarz (NS) 5-brane solutions in type II and heterotic string theories. First we demonstrate that the non-extremal NS 5-brane background is U-dual to its CGHS limit, a two-dimensional black hole times $S^3\times T^5$; an intermediate step is ... | 6.717959 | 6.862704 | 7.442599 | 6.389789 | 6.836637 | 6.842036 | 6.67788 | 6.384655 | 6.525695 | 7.313898 | 6.515084 | 6.530347 | 6.767923 | 6.569476 | 6.549053 | 6.461143 | 6.552161 | 6.542524 | 6.556401 | 6.651904 | 6.471245 |
1707.06351 | Ken-Ji Hamada | Ken-ji Hamada | BRST Conformal Symmetry as A Background-Free Nature of Quantum Gravity | 44 pages, 2 figures, sentences about our inflation model added,
ref.46 is corrected | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum gravity that describes the world beyond the Planck scale should be
formulated in a background-metric independent manner. Such a background-free
nature can be represented as a gauge equivalency under conformal
transformations, called the BRST conformal symmetry. In this review, we present
quantum field theorie... | [
{
"created": "Thu, 20 Jul 2017 02:49:06 GMT",
"version": "v1"
},
{
"created": "Fri, 28 Jul 2017 01:55:51 GMT",
"version": "v2"
}
] | 2017-08-01 | [
[
"Hamada",
"Ken-ji",
""
]
] | Quantum gravity that describes the world beyond the Planck scale should be formulated in a background-metric independent manner. Such a background-free nature can be represented as a gauge equivalency under conformal transformations, called the BRST conformal symmetry. In this review, we present quantum field theories ... | 11.429024 | 11.959959 | 12.980397 | 11.283167 | 11.907851 | 11.601707 | 11.784693 | 11.819189 | 11.333544 | 12.858296 | 11.438284 | 11.433796 | 11.046901 | 11.129766 | 11.514654 | 11.059607 | 11.368203 | 11.189938 | 11.015254 | 11.058016 | 10.969403 |
hep-th/0611073 | Davi Rodrigues | Davi C. Rodrigues | Electromagnetic Dualities on Noncommutative Space-Time and Symplectic
Formalisms | 162 pages, 7 figures, Ph.D. thesis (Portuguese) | null | null | null | hep-th | null | In this thesis we analyze extensions of classical electromagnetic dualities
to the noncommutative (NC) 3D and 4D space-times. It is known that the
noncomutativity parameter theta becomes its Hodge dual *theta through the NC 4D
electromagnetic duality [under the Slowly Varying Fields (SVF) limit], this is
a nontrivial... | [
{
"created": "Tue, 7 Nov 2006 04:52:48 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Rodrigues",
"Davi C.",
""
]
] | In this thesis we analyze extensions of classical electromagnetic dualities to the noncommutative (NC) 3D and 4D space-times. It is known that the noncomutativity parameter theta becomes its Hodge dual *theta through the NC 4D electromagnetic duality [under the Slowly Varying Fields (SVF) limit], this is a nontrivial t... | 10.915887 | 9.470901 | 10.662349 | 9.475047 | 10.197593 | 9.542096 | 10.559965 | 9.591302 | 9.694156 | 11.107056 | 9.395842 | 10.069645 | 10.327579 | 9.865018 | 9.80483 | 9.87239 | 10.156008 | 9.909052 | 10.0606 | 10.598728 | 10.126312 |
hep-th/9609055 | Thomas Heinzl | T. Heinzl (University of Regensburg) | Hamiltonian Approach to the Gribov Problem | 4 pages, 2 PICTEX figures, uses espcrc2.sty, talk presented at QCD
96, July 4-12, Montpellier, France | Nucl.Phys.Proc.Suppl. 54A (1997) 194-197 | 10.1016/S0920-5632(97)00039-X | TPR-96-18 | hep-th hep-ph | null | We study the Gribov problem within a Hamiltonian formulation of pure
Yang-Mills theory. For a particular gauge fixing, a finite volume modification
of the axial gauge, we find an exact characterization of the space of
gauge-inequivalent gauge configurations.
| [
{
"created": "Fri, 6 Sep 1996 11:18:31 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Heinzl",
"T.",
"",
"University of Regensburg"
]
] | We study the Gribov problem within a Hamiltonian formulation of pure Yang-Mills theory. For a particular gauge fixing, a finite volume modification of the axial gauge, we find an exact characterization of the space of gauge-inequivalent gauge configurations. | 9.978829 | 8.268493 | 9.815102 | 8.84976 | 7.890154 | 8.681862 | 8.566384 | 8.079989 | 8.843121 | 10.476667 | 8.384607 | 8.776472 | 9.863544 | 9.231813 | 8.909187 | 8.663896 | 8.719358 | 8.408619 | 9.052607 | 9.686536 | 9.14673 |
1406.1161 | Howard Schnitzer | Howard J. Schnitzer | Mutual R\'enyi information for two disjoint compound systems | 10 pages, typos corrected | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The leading term for the mutual R\'enyi information is studied for two widely
separated identical compound systems for free scalar fields in $(d+1)$
Euclidean space. The compound system consists of two identical spheres in
contact, with a result consistent with a universal form for the leading term
for the mutual R\'... | [
{
"created": "Wed, 4 Jun 2014 19:37:59 GMT",
"version": "v1"
},
{
"created": "Mon, 20 Oct 2014 19:11:15 GMT",
"version": "v2"
},
{
"created": "Mon, 3 Nov 2014 19:39:16 GMT",
"version": "v3"
}
] | 2014-11-04 | [
[
"Schnitzer",
"Howard J.",
""
]
] | The leading term for the mutual R\'enyi information is studied for two widely separated identical compound systems for free scalar fields in $(d+1)$ Euclidean space. The compound system consists of two identical spheres in contact, with a result consistent with a universal form for the leading term for the mutual R\'en... | 16.549469 | 11.887121 | 12.992175 | 12.171586 | 11.759713 | 15.050985 | 14.224738 | 13.064699 | 12.798205 | 15.554823 | 13.637008 | 14.22286 | 13.845857 | 13.978439 | 14.642214 | 13.733175 | 14.973328 | 14.15912 | 14.548045 | 14.693747 | 14.502972 |
hep-th/0409064 | Xiaojun Wang | Xiao-Jun Wang | D3-branes in conifold and D5-brane wrapping on a supersymmetric 2-cycle | The paper has been withdraw by author | null | null | null | hep-th | null | The paper has been withdraw by author due to a crucial error in equation 10.
| [
{
"created": "Mon, 6 Sep 2004 14:59:47 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Sep 2004 04:32:18 GMT",
"version": "v2"
},
{
"created": "Thu, 23 Sep 2004 08:47:23 GMT",
"version": "v3"
},
{
"created": "Sun, 10 Oct 2004 08:19:22 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Wang",
"Xiao-Jun",
""
]
] | The paper has been withdraw by author due to a crucial error in equation 10. | 34.630348 | 20.170511 | 21.306255 | 16.886408 | 28.017073 | 16.040178 | 17.530113 | 19.115974 | 17.046894 | 21.283983 | 18.854797 | 26.720158 | 23.188042 | 24.654541 | 24.206123 | 27.769655 | 25.313047 | 22.319382 | 25.938271 | 23.814833 | 22.775877 |
hep-th/0108031 | Tim Morris | Michael D. Turner | The derivative expansion of the exact renormalization group | Thesis, August 1996. LaTeX, 125 pages,28 figs | null | null | null | hep-th | null | We formulate a method of performing non-perturbative calculations in quantum
field theory, based upon a derivative expansion of the exact renormalization
group. We then proceed to apply this method to the calculation of critical
exponents for three dimensional O(N) symmetric theory. Finally we discuss how
the approxi... | [
{
"created": "Mon, 6 Aug 2001 21:01:41 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Turner",
"Michael D.",
""
]
] | We formulate a method of performing non-perturbative calculations in quantum field theory, based upon a derivative expansion of the exact renormalization group. We then proceed to apply this method to the calculation of critical exponents for three dimensional O(N) symmetric theory. Finally we discuss how the approxima... | 10.571969 | 8.75288 | 9.689382 | 9.092968 | 9.229484 | 9.388519 | 8.689438 | 8.978362 | 8.143974 | 10.645211 | 8.653119 | 9.220004 | 9.900967 | 9.801106 | 9.733717 | 9.38769 | 9.436414 | 9.356569 | 9.798448 | 9.81065 | 9.557791 |
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