id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1503.01024 | Mark Trodden | Mark Trodden | Constructing Galileons | 15 pages, To appear in the proceedings of the DISCRETE 2014
conference, King's College London, December 2014 | null | 10.1088/1742-6596/631/1/012013 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this plenary talk delivered at the DISCRETE 2014 conference in London, I
briefly summarize the ideas behind and attractive properties of the Galileon
field theories, and describe a broad class of scalar field theories that share
these properties. After describing how Galileons arise, and commenting on their
fascin... | [
{
"created": "Tue, 3 Mar 2015 17:39:36 GMT",
"version": "v1"
}
] | 2015-09-02 | [
[
"Trodden",
"Mark",
""
]
] | In this plenary talk delivered at the DISCRETE 2014 conference in London, I briefly summarize the ideas behind and attractive properties of the Galileon field theories, and describe a broad class of scalar field theories that share these properties. After describing how Galileons arise, and commenting on their fascinat... | 11.990808 | 11.741598 | 12.266938 | 11.695846 | 10.39231 | 11.284079 | 9.813001 | 10.956056 | 10.801268 | 11.166382 | 10.438187 | 10.614425 | 12.033648 | 11.385444 | 11.215487 | 10.779976 | 11.193973 | 10.962828 | 10.934991 | 12.112372 | 10.7217 |
2210.14923 | Ying-Hsuan Lin | Jan Albert, Justin Kaidi, Ying-Hsuan Lin | Topological modularity of Supermoonshine | 28 pages + appendices; v2: publication version | null | 10.1093/ptep/ptad034 | null | hep-th math-ph math.AT math.MP math.NT math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The theory of topological modular forms (TMF) predicts that elliptic genera
of physical theories satisfy a certain divisibility property, determined by the
theory's gravitational anomaly. In this note we verify this prediction in
Duncan's Supermoonshine module, as well as in tensor products and orbifolds
thereof. Alo... | [
{
"created": "Wed, 26 Oct 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Mar 2023 16:33:23 GMT",
"version": "v2"
}
] | 2023-03-28 | [
[
"Albert",
"Jan",
""
],
[
"Kaidi",
"Justin",
""
],
[
"Lin",
"Ying-Hsuan",
""
]
] | The theory of topological modular forms (TMF) predicts that elliptic genera of physical theories satisfy a certain divisibility property, determined by the theory's gravitational anomaly. In this note we verify this prediction in Duncan's Supermoonshine module, as well as in tensor products and orbifolds thereof. Along... | 14.221831 | 13.402638 | 17.12904 | 12.477228 | 13.960441 | 12.723408 | 12.136772 | 10.999902 | 12.120896 | 18.307577 | 11.641589 | 12.064713 | 14.493875 | 13.30679 | 13.695168 | 13.479163 | 12.885277 | 12.841425 | 12.461574 | 16.46447 | 12.593319 |
2202.02946 | Yuan Zhong | Jun Feng and Yuan Zhong | Scalar perturbation of gravitating double-kink solutions | 6 pages, 4 figures, final version published by EPL | EPL 137 (2022) 49001 | 10.1209/0295-5075/ac56ae | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | In this letter, a two-dimensional (2D) gravity-scalar model is studied. This
model supports interesting double-kink solutions, and the corresponding metric
solutions can be derived analytically. Depending on a tunable parameter $c$,
the metric can be symmetric or asymmetric. The Schr\"odinger-like equation for
normal... | [
{
"created": "Mon, 7 Feb 2022 05:10:28 GMT",
"version": "v1"
},
{
"created": "Fri, 29 Apr 2022 14:32:12 GMT",
"version": "v2"
}
] | 2022-05-02 | [
[
"Feng",
"Jun",
""
],
[
"Zhong",
"Yuan",
""
]
] | In this letter, a two-dimensional (2D) gravity-scalar model is studied. This model supports interesting double-kink solutions, and the corresponding metric solutions can be derived analytically. Depending on a tunable parameter $c$, the metric can be symmetric or asymmetric. The Schr\"odinger-like equation for normal m... | 9.594213 | 8.736679 | 8.519981 | 8.054211 | 8.618948 | 8.451278 | 8.36567 | 8.681672 | 8.156691 | 9.546142 | 8.47397 | 8.706471 | 8.620022 | 8.533805 | 8.668156 | 8.532413 | 8.585907 | 8.279741 | 8.592774 | 8.319681 | 8.396943 |
hep-th/9805122 | null | Laurent Baulieu and Eliezer Rabinovici | Self-Duality and New TQFTs for Forms | teX-file | JHEP 9806:006,1998 | 10.1088/1126-6708/1998/06/006 | CERN-TH: 98-96,RI: 98-10,LPTHE: 98-17 | hep-th | null | We discuss theories containing higher-order forms in various dimensions. We
explain how Chern--Simons-type theories of forms can be defined from TQFTs in
one less dimension. We also exhibit new TQFTs with interacting Yang--Mills
fields and higher--order forms. They are obtained by the dimensional reduction
of TQFTs w... | [
{
"created": "Tue, 19 May 1998 17:44:07 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Baulieu",
"Laurent",
""
],
[
"Rabinovici",
"Eliezer",
""
]
] | We discuss theories containing higher-order forms in various dimensions. We explain how Chern--Simons-type theories of forms can be defined from TQFTs in one less dimension. We also exhibit new TQFTs with interacting Yang--Mills fields and higher--order forms. They are obtained by the dimensional reduction of TQFTs who... | 13.912968 | 12.752897 | 15.273441 | 12.548072 | 12.510767 | 14.133763 | 13.107521 | 13.661932 | 12.730951 | 16.112747 | 12.540486 | 12.770742 | 14.055855 | 12.584738 | 12.04152 | 12.513031 | 12.820498 | 12.713665 | 12.666851 | 13.389605 | 12.349532 |
hep-th/0501069 | D. Toublan | D. Toublan | A large Nc perspective on the QCD phase diagram | 5 pages | Phys.Lett. B621 (2005) 145-150 | 10.1016/j.physletb.2005.06.064 | null | hep-th hep-lat hep-ph nucl-th | null | The transition between the hadronic phase and the quark gluon plasma phase at
nonzero temperature and quark chemical potentials is studied within the
large-Nc expansion of QCD.
| [
{
"created": "Mon, 10 Jan 2005 19:48:32 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Jul 2005 19:19:34 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Toublan",
"D.",
""
]
] | The transition between the hadronic phase and the quark gluon plasma phase at nonzero temperature and quark chemical potentials is studied within the large-Nc expansion of QCD. | 6.704191 | 6.427314 | 4.585093 | 4.835036 | 5.463572 | 5.713658 | 5.79705 | 6.467222 | 4.922566 | 4.694075 | 6.177718 | 5.9952 | 5.229291 | 5.161093 | 5.639332 | 6.128902 | 5.567397 | 5.857481 | 5.160834 | 5.317755 | 5.659421 |
0812.1944 | Jiajun Xu | S.-H. Henry Tye, Jiajun Xu and Yang Zhang | Multi-field Inflation with a Random Potential | More clarifications and references added | JCAP 0904:018,2009 | 10.1088/1475-7516/2009/04/018 | null | hep-th astro-ph hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the possibility of inflation in the cosmic landscape, which may
be approximated by a complicated potential, we study the density perturbations
in multi-field inflation with a random potential. The random potential causes
the inflaton to undergo a Brownian motion with a drift in the D-dimensional
field sp... | [
{
"created": "Wed, 10 Dec 2008 16:07:14 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Jan 2009 21:12:55 GMT",
"version": "v2"
},
{
"created": "Thu, 12 Mar 2009 13:50:17 GMT",
"version": "v3"
}
] | 2009-04-24 | [
[
"Tye",
"S. -H. Henry",
""
],
[
"Xu",
"Jiajun",
""
],
[
"Zhang",
"Yang",
""
]
] | Motivated by the possibility of inflation in the cosmic landscape, which may be approximated by a complicated potential, we study the density perturbations in multi-field inflation with a random potential. The random potential causes the inflaton to undergo a Brownian motion with a drift in the D-dimensional field spac... | 8.942364 | 9.787408 | 9.350616 | 8.73647 | 9.31588 | 10.175014 | 9.82341 | 9.207108 | 8.695074 | 9.836804 | 9.284228 | 8.99223 | 8.901256 | 8.673736 | 8.990667 | 8.919375 | 8.825569 | 8.928579 | 8.896371 | 9.129201 | 8.862331 |
2006.00764 | Michael Maziashvili | Michael Maziashvili | Mean lifetime of a false vacuum in terms of the Krylov-Fock non-escape
probability | 14 pages | Phys. Rev. D 102, 076006 (2020) | 10.1103/PhysRevD.102.076006 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Krylov-Fock expression of non-decay (or survival) probability, which
allows to evaluate the deviations from the exponential decay law (nowadays well
established experimentally), is more informative as it readily provides the
distribution function for the lifetime as a random quantity. Guided by the well
establish... | [
{
"created": "Mon, 1 Jun 2020 07:33:55 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Oct 2020 07:02:43 GMT",
"version": "v2"
}
] | 2020-10-14 | [
[
"Maziashvili",
"Michael",
""
]
] | The Krylov-Fock expression of non-decay (or survival) probability, which allows to evaluate the deviations from the exponential decay law (nowadays well established experimentally), is more informative as it readily provides the distribution function for the lifetime as a random quantity. Guided by the well established... | 13.514595 | 13.583402 | 13.550393 | 13.108109 | 13.625474 | 13.803012 | 14.484838 | 13.924643 | 12.812159 | 14.121978 | 12.712486 | 12.671883 | 13.11648 | 12.722674 | 12.92912 | 12.654966 | 12.926041 | 12.999492 | 12.789016 | 12.852696 | 13.226296 |
1311.2945 | Jaewon Song | Prarit Agarwal and Jaewon Song | New N=1 Dualities from M5-branes and Outer-automorphism Twists | 56 pages, 29 colored figures; v2: minor corrections, references added | null | 10.1007/JHEP03(2014)133 | UCSD-PTH-13-13 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We generalize recent construction of four-dimensional $\mathcal{N}=1$ SCFT
from wrapping six-dimensional $\mathcal{N}=(2,0)$ theory on a Riemann surface
to the case of $D$-type with outer-automorphism twists. This construction
allows us to build various dual theories for a class of $\mathcal{N}=1$ quiver
theories of ... | [
{
"created": "Tue, 12 Nov 2013 21:00:22 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Feb 2014 00:17:17 GMT",
"version": "v2"
}
] | 2015-06-17 | [
[
"Agarwal",
"Prarit",
""
],
[
"Song",
"Jaewon",
""
]
] | We generalize recent construction of four-dimensional $\mathcal{N}=1$ SCFT from wrapping six-dimensional $\mathcal{N}=(2,0)$ theory on a Riemann surface to the case of $D$-type with outer-automorphism twists. This construction allows us to build various dual theories for a class of $\mathcal{N}=1$ quiver theories of $S... | 6.174671 | 6.300959 | 7.486546 | 6.040133 | 6.340685 | 6.522888 | 6.091617 | 5.813803 | 6.09563 | 7.844529 | 5.973489 | 5.811527 | 6.405838 | 5.886777 | 6.08938 | 6.002448 | 5.847712 | 5.793267 | 5.89737 | 5.998865 | 5.599469 |
1909.06995 | Minxin Huang | Min-xin Huang | Note on S-channel factorization in multitrace
Berenstein-Maldacena-Nastase correlators | 22 pages, 9 figures. v2: major revisions in section 3. v3: minor
clarifications, journal version. v4: a further correction about parameter
counting in section 3 | Phys. Rev. D 101, 026013 (2020) | 10.1103/PhysRevD.101.026013 | USTC-ICTS-19-24 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a previous paper we proposed a factorization principle for the correlation
functions of Berenstein-Maldacena-Nastase (BMN) operators in free
$\mathcal{N}=4$ super-Yang-Mills theory. These correlators are conjectured to
described physical string amplitudes in an infinitely curved Ramond-Ramond
pp-wave background. T... | [
{
"created": "Mon, 16 Sep 2019 05:35:47 GMT",
"version": "v1"
},
{
"created": "Mon, 4 Nov 2019 07:51:12 GMT",
"version": "v2"
},
{
"created": "Sun, 12 Jan 2020 03:16:33 GMT",
"version": "v3"
},
{
"created": "Mon, 13 Apr 2020 01:23:22 GMT",
"version": "v4"
}
] | 2020-04-14 | [
[
"Huang",
"Min-xin",
""
]
] | In a previous paper we proposed a factorization principle for the correlation functions of Berenstein-Maldacena-Nastase (BMN) operators in free $\mathcal{N}=4$ super-Yang-Mills theory. These correlators are conjectured to described physical string amplitudes in an infinitely curved Ramond-Ramond pp-wave background. The... | 8.516689 | 8.09582 | 9.657074 | 7.124886 | 7.460405 | 7.343032 | 6.954275 | 7.330031 | 6.808721 | 10.045903 | 7.184813 | 7.244256 | 7.914743 | 7.200881 | 7.196836 | 7.337153 | 7.53621 | 7.369026 | 7.249324 | 7.829091 | 7.218692 |
0908.0434 | Alexander Schenkel | Alexander Schenkel | Symmetry Reduction and Exact Solutions in Twisted Noncommutative Gravity | LaTeX 11 pages, appolb.cls style. Seminar talk at the 49. Cracow
School of Theoretical Physics "Non-perturbative Gravity and Quantum
Chromodynamics". To appear in Acta Physica Polonica B | Acta Physica Polonica B Proc. Suppl. 2: 657-667, 2009 | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the noncommutative gravity of Wess et al. and discuss its physical
applications. We define noncommutative symmetry reduction and construct
deformed symmetric solutions of the noncommutative Einstein equations. We apply
our framework to find explicit deformed cosmological and black hole solutions
and discuss... | [
{
"created": "Tue, 4 Aug 2009 12:45:21 GMT",
"version": "v1"
}
] | 2010-01-05 | [
[
"Schenkel",
"Alexander",
""
]
] | We review the noncommutative gravity of Wess et al. and discuss its physical applications. We define noncommutative symmetry reduction and construct deformed symmetric solutions of the noncommutative Einstein equations. We apply our framework to find explicit deformed cosmological and black hole solutions and discuss t... | 9.66453 | 10.058195 | 9.264939 | 8.448806 | 9.732141 | 9.910937 | 10.195825 | 9.364619 | 10.411922 | 9.45975 | 8.679601 | 8.859525 | 9.710038 | 8.676764 | 9.056352 | 9.351931 | 8.763584 | 8.512258 | 9.265719 | 9.442069 | 8.796444 |
1602.04761 | Shankhadeep Chakrabortty | Shankhadeep Chakrabortty, Tanay K. Dey | Back reaction effects on the dynamics of heavy probes in heavy quark
cloud | 29 pages, 21 figures | null | null | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We holographically study the effect of back reaction on the hydrodynamical
properties of $\mathcal{N} = 4$ strongly coupled super Yang-Mills (SYM) thermal
plasma. The back reaction we consider arises from the presence of static heavy
quarks uniformly distributed over $\mathcal{N} = 4$ SYM plasma. In order to
study th... | [
{
"created": "Mon, 15 Feb 2016 18:47:23 GMT",
"version": "v1"
}
] | 2016-02-16 | [
[
"Chakrabortty",
"Shankhadeep",
""
],
[
"Dey",
"Tanay K.",
""
]
] | We holographically study the effect of back reaction on the hydrodynamical properties of $\mathcal{N} = 4$ strongly coupled super Yang-Mills (SYM) thermal plasma. The back reaction we consider arises from the presence of static heavy quarks uniformly distributed over $\mathcal{N} = 4$ SYM plasma. In order to study the ... | 6.629535 | 6.159645 | 6.879978 | 6.215922 | 6.464217 | 6.075331 | 6.041644 | 6.077419 | 5.920398 | 6.829158 | 5.831639 | 6.209134 | 6.345572 | 6.279578 | 6.396633 | 6.373743 | 6.478532 | 6.11627 | 6.297911 | 6.671176 | 6.189898 |
hep-th/0603250 | Julio Cesar Mejia-Ambriz | Tzihue Cisneros-Perez, Alfredo Herrera-Aguilar, Julio Cesar
Mejia-Ambriz and Violeta Rojas-Macias | Gowdy Cosmological Models from Stringy Black Holes | 7 pages in latex, no figures, Talk presented at the V Mexican
Workshop on Gravitation and Mathematical Physics, Morelia, Michoacan, Mexico,
November 24-28, 2003 | null | null | null | hep-th | null | In the framework of 4D Einstein-Maxwell Dilaton-Axion theory we show how to
obtain a family of both unpolarized and polarized S^1XS^2 Gowdy cosmological
models endowed with nontrivial axion, dilaton and electromagnetic fields from a
solitonic rotating black hole-type solution by interchanging the r and t
coordinates ... | [
{
"created": "Fri, 31 Mar 2006 03:35:43 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Sep 2006 18:56:35 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Cisneros-Perez",
"Tzihue",
""
],
[
"Herrera-Aguilar",
"Alfredo",
""
],
[
"Mejia-Ambriz",
"Julio Cesar",
""
],
[
"Rojas-Macias",
"Violeta",
""
]
] | In the framework of 4D Einstein-Maxwell Dilaton-Axion theory we show how to obtain a family of both unpolarized and polarized S^1XS^2 Gowdy cosmological models endowed with nontrivial axion, dilaton and electromagnetic fields from a solitonic rotating black hole-type solution by interchanging the r and t coordinates in... | 9.635726 | 9.683551 | 9.632026 | 8.868368 | 8.756383 | 8.766666 | 8.793305 | 8.517992 | 8.756113 | 8.944696 | 8.973175 | 8.670289 | 8.819468 | 8.609544 | 8.333389 | 8.559247 | 8.727736 | 8.564806 | 8.363064 | 8.758558 | 8.312346 |
hep-th/9912010 | Masafumi Fukuma | Masafumi Fukuma, Takeshi Oota, Hirokazu Tanaka | Weyl Groups in AdS(3)/CFT(2) | 20 pages, 3 figues | Prog.Theor.Phys.103:447-462,2000 | 10.1143/PTP.103.447 | YITP-99-70 | hep-th | null | The system of D1 and D5 branes with a Kaluza-Klein momentum is
re-investigated using the five-dimensional U-duality group E_{6(+6)}(Z). We
show that the residual U-duality symmetry that keeps this D1-D5-KK system
intact is generically given by a lift of the Weyl group of F_{4(+4)}, embedded
as a finite subgroup in E_... | [
{
"created": "Wed, 1 Dec 1999 22:22:35 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Fukuma",
"Masafumi",
""
],
[
"Oota",
"Takeshi",
""
],
[
"Tanaka",
"Hirokazu",
""
]
] | The system of D1 and D5 branes with a Kaluza-Klein momentum is re-investigated using the five-dimensional U-duality group E_{6(+6)}(Z). We show that the residual U-duality symmetry that keeps this D1-D5-KK system intact is generically given by a lift of the Weyl group of F_{4(+4)}, embedded as a finite subgroup in E_{6... | 7.292504 | 7.27858 | 8.719508 | 7.023705 | 7.95477 | 7.65758 | 6.994492 | 7.282315 | 7.171676 | 8.430559 | 7.141566 | 6.811839 | 7.301202 | 6.789679 | 7.198138 | 6.930078 | 6.935302 | 6.937468 | 6.927742 | 6.98013 | 6.672098 |
1206.0664 | Loriano Bonora | Loriano Bonora, Andrey Bytsenko and Emilio Elizalde | String Partition Functions, Hilbert Schemes, and Affine Lie Algebra
Representations on Homology Groups | 56 pages, review paper, in honour of J.S.Dowker. arXiv admin note:
text overlap with arXiv:0905.1285, arXiv:math/0006201, arXiv:math/0412089,
arXiv:math/0403547 by other authors | null | 10.1088/1751-8113/45/37/374002 | SISSA/12/2012/EP | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This review paper contains a concise introduction to highest weight
representations of infinite dimensional Lie algebras, vertex operator algebras
and Hilbert schemes of points, together with their physical applications to
elliptic genera of superconformal quantum mechanics and superstring models. The
common link of ... | [
{
"created": "Mon, 4 Jun 2012 16:23:25 GMT",
"version": "v1"
}
] | 2015-06-05 | [
[
"Bonora",
"Loriano",
""
],
[
"Bytsenko",
"Andrey",
""
],
[
"Elizalde",
"Emilio",
""
]
] | This review paper contains a concise introduction to highest weight representations of infinite dimensional Lie algebras, vertex operator algebras and Hilbert schemes of points, together with their physical applications to elliptic genera of superconformal quantum mechanics and superstring models. The common link of al... | 6.924205 | 10.549937 | 11.59479 | 9.831984 | 11.548022 | 10.944354 | 10.973934 | 11.1176 | 10.955896 | 12.306068 | 10.115945 | 9.121171 | 9.478965 | 8.867988 | 9.598574 | 9.331356 | 9.233386 | 8.791409 | 9.130251 | 9.862295 | 8.678802 |
1511.00682 | Chris Halcrow | C. J. Halcrow | Vibrational quantisation of the B=7 Skyrmion | 24 pages, 6 figures | Nucl. Phys. B 904, 106-123, 2016 | 10.1016/j.nuclphysb.2016.01.011 | DAMTP-2015-67 | hep-th nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the inclusion of the most important vibrational modes in the
quantisation of the dodecahedral $B=7$ Skyrmion. In contrast to a rigid body
quantisation, this formalism allows a spin $\frac{3}{2}$ state to lie below the
spin $\frac{7}{2}$ state, in agreement with experimental data. There is also a
low lying... | [
{
"created": "Mon, 2 Nov 2015 21:00:00 GMT",
"version": "v1"
}
] | 2016-02-03 | [
[
"Halcrow",
"C. J.",
""
]
] | We consider the inclusion of the most important vibrational modes in the quantisation of the dodecahedral $B=7$ Skyrmion. In contrast to a rigid body quantisation, this formalism allows a spin $\frac{3}{2}$ state to lie below the spin $\frac{7}{2}$ state, in agreement with experimental data. There is also a low lying s... | 6.486612 | 6.458732 | 6.915391 | 6.271984 | 6.663256 | 6.506599 | 6.71377 | 6.593687 | 6.156014 | 6.673451 | 6.270104 | 6.505103 | 7.068089 | 6.402234 | 6.394942 | 6.473281 | 6.359566 | 6.508872 | 6.31112 | 6.653801 | 6.374756 |
hep-th/0207283 | Panagiota Kanti | P. Kanti (CERN), I. Olasagasti and K. Tamvakis (Univ. of Ioannina) | Schwarzschild Black Branes and Strings in higher-dimensional Brane
Worlds | 22 pages, Latex file | Phys.Rev. D66 (2002) 104026 | 10.1103/PhysRevD.66.104026 | CERN-TH/2002-162 | hep-th gr-qc hep-ph | null | We consider branes embedded in spacetimes of codimension one and two, with a
warped metric tensor for the subspace parallel to the brane. We study a variety
of brane-world solutions arising by introducing a Schwarzschild-like black hole
metric on the brane and we investigate the properties of the corresponding
higher... | [
{
"created": "Wed, 31 Jul 2002 16:00:35 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Kanti",
"P.",
"",
"CERN"
],
[
"Olasagasti",
"I.",
"",
"Univ. of Ioannina"
],
[
"Tamvakis",
"K.",
"",
"Univ. of Ioannina"
]
] | We consider branes embedded in spacetimes of codimension one and two, with a warped metric tensor for the subspace parallel to the brane. We study a variety of brane-world solutions arising by introducing a Schwarzschild-like black hole metric on the brane and we investigate the properties of the corresponding higher-d... | 11.196609 | 12.09903 | 10.362823 | 10.783968 | 10.726145 | 10.918903 | 10.66447 | 10.828107 | 10.398328 | 11.073215 | 9.669476 | 10.833596 | 10.31652 | 10.137876 | 10.409203 | 10.558339 | 10.18893 | 10.467824 | 10.106378 | 10.714035 | 10.193181 |
hep-th/0106080 | Mahmut Hortacsu | M. Hortacsu | Explicit Examples on Conformal Invariance | 9 Pages, Tex | Int.J.Theor.Phys. 42 (2003) 49 | null | null | hep-th | null | We study examples where conformal invariance implies rational critical
indices, triviality of the underlying quantum field theory and emergence of
hypergeometric functions as solutions of the field equations.
| [
{
"created": "Mon, 11 Jun 2001 11:21:13 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Hortacsu",
"M.",
""
]
] | We study examples where conformal invariance implies rational critical indices, triviality of the underlying quantum field theory and emergence of hypergeometric functions as solutions of the field equations. | 23.949854 | 23.526693 | 23.924561 | 19.576595 | 23.714182 | 30.840036 | 26.39024 | 22.853079 | 21.750828 | 22.810467 | 22.902655 | 20.765333 | 21.773149 | 20.393105 | 19.724323 | 22.086992 | 21.361927 | 21.557949 | 21.009817 | 20.492855 | 21.429813 |
hep-th/9708058 | null | Dieter Mayer, Alexander Ushveridze | Bethe Ansatz in Quantum Mechanics. 1. The Inverse Method of Separation
of Variables | 17 pages, LaTeX | null | null | null | hep-th | null | In this paper we formulate a general method for building completely
integrable quantum systems. The method is based on the use of the so-called
multi-parameter spectral equations, i.e. equations with several spectral
parameters. We show that any such equation, after eliminating some spectral
parameters by means of th... | [
{
"created": "Mon, 11 Aug 1997 18:46:43 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Mayer",
"Dieter",
""
],
[
"Ushveridze",
"Alexander",
""
]
] | In this paper we formulate a general method for building completely integrable quantum systems. The method is based on the use of the so-called multi-parameter spectral equations, i.e. equations with several spectral parameters. We show that any such equation, after eliminating some spectral parameters by means of the ... | 7.388848 | 7.611708 | 7.629632 | 7.425617 | 6.878436 | 8.448469 | 7.30679 | 7.184134 | 7.51039 | 8.485448 | 7.175022 | 7.2239 | 7.093402 | 7.275251 | 6.998585 | 7.127995 | 7.269116 | 7.087296 | 6.932383 | 7.388215 | 7.164384 |
0809.2912 | Leopoldo A. Pando Zayas | Ibrahima Bah, Leopoldo A. Pando Zayas and Cesar A. Terrero-Escalante | Holographic Geometric Entropy at Finite Temperature from Black Holes in
Global Anti de Sitter Spaces | v2: 33 pages, 9 figures. Added an appendix. Other minor modifications
to clarify the contents | null | 10.1142/S0217751X12500480 | MCTP-08-57 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using a holographic proposal for the geometric entropy we study its behavior
in the geometry of Schwarzschild black holes in global $AdS_p$ for $p=3,4,5$.
Holographically, the entropy is determined by a minimal surface. On the gravity
side, due to the presence of a horizon on the background, generically there are
two... | [
{
"created": "Wed, 17 Sep 2008 11:44:51 GMT",
"version": "v1"
},
{
"created": "Tue, 13 Jan 2009 21:22:51 GMT",
"version": "v2"
}
] | 2015-05-13 | [
[
"Bah",
"Ibrahima",
""
],
[
"Zayas",
"Leopoldo A. Pando",
""
],
[
"Terrero-Escalante",
"Cesar A.",
""
]
] | Using a holographic proposal for the geometric entropy we study its behavior in the geometry of Schwarzschild black holes in global $AdS_p$ for $p=3,4,5$. Holographically, the entropy is determined by a minimal surface. On the gravity side, due to the presence of a horizon on the background, generically there are two s... | 9.174773 | 8.625364 | 9.69525 | 8.401052 | 9.022056 | 8.816459 | 8.954024 | 7.932666 | 8.846359 | 9.431454 | 8.363654 | 8.43187 | 9.080276 | 8.563401 | 8.310715 | 8.630937 | 8.57629 | 8.52564 | 8.396925 | 9.100019 | 8.512106 |
1704.03214 | Davoud Kamani | Elham Maghsoodi and Davoud Kamani | Interaction of the branes in the Presence of the Background Fields: the
Dynamical Non-intersecting Perpendicular Wrapped-Fractional Configuration | 13 pages, Latex2e, no figure. Minor corrections to Eqs. (3.3) and
(3.5) | Int. J. Mod. Phys. A 32, 1750063 (2017) | 10.1142/S0217751X17500634 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We shall obtain the interaction of the D$p_1$- and D$p_2$-branes in the
toroidal-orbifold spacetime $\mathit{T}^{n}\times\mathbb{R}^{1, d-n-5}
\times\mathbb{C}^{2}/\mathbb{Z}_{2}$. The configuration of the branes is:
non-intersecting, perpendicular, moving-rotating, wrapped-fractional with
background fields. For this... | [
{
"created": "Tue, 11 Apr 2017 09:36:58 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jul 2017 10:43:07 GMT",
"version": "v2"
}
] | 2017-07-25 | [
[
"Maghsoodi",
"Elham",
""
],
[
"Kamani",
"Davoud",
""
]
] | We shall obtain the interaction of the D$p_1$- and D$p_2$-branes in the toroidal-orbifold spacetime $\mathit{T}^{n}\times\mathbb{R}^{1, d-n-5} \times\mathbb{C}^{2}/\mathbb{Z}_{2}$. The configuration of the branes is: non-intersecting, perpendicular, moving-rotating, wrapped-fractional with background fields. For this, ... | 9.213485 | 7.143348 | 10.209253 | 7.87809 | 8.311055 | 7.347395 | 7.41251 | 7.161611 | 7.609565 | 10.418786 | 7.314259 | 8.013105 | 9.365428 | 8.395453 | 8.150167 | 8.329719 | 8.222768 | 8.339915 | 8.602749 | 9.286336 | 8.565492 |
1203.0015 | Thomas Hartman | Matthias R. Gaberdiel, Thomas Hartman, and Kewang Jin | Higher Spin Black Holes from CFT | 24 pages; v2 reference added | JHEP 1204 (2012) 103 | 10.1007/JHEP04(2012)103 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Higher spin gravity in three dimensions has explicit black holes solutions,
carrying higher spin charge. We compute the free energy of a charged black hole
from the holographic dual, a 2d CFT with extended conformal symmetry, and find
exact agreement with the bulk thermodynamics. In the CFT, higher spin
corrections t... | [
{
"created": "Wed, 29 Feb 2012 21:04:07 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Jun 2012 10:10:02 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Gaberdiel",
"Matthias R.",
""
],
[
"Hartman",
"Thomas",
""
],
[
"Jin",
"Kewang",
""
]
] | Higher spin gravity in three dimensions has explicit black holes solutions, carrying higher spin charge. We compute the free energy of a charged black hole from the holographic dual, a 2d CFT with extended conformal symmetry, and find exact agreement with the bulk thermodynamics. In the CFT, higher spin corrections to ... | 8.29847 | 8.064594 | 10.545338 | 7.903759 | 7.428604 | 8.561739 | 8.150078 | 8.085707 | 7.248208 | 8.558376 | 7.936005 | 8.231237 | 8.669972 | 8.169546 | 7.971992 | 8.000769 | 8.233947 | 8.023818 | 8.077305 | 8.814476 | 7.908521 |
2104.08221 | Olaf Baake | Olaf Baake, Christos Charmousis, Mokhtar Hassaine, Miguel San Juan | Regular black holes and gravitational particle-like solutions in generic
DHOST theories | 20 pages, 5 figures (added new references) | null | 10.1088/1475-7516/2021/06/021 | null | hep-th gr-qc | http://creativecommons.org/licenses/by/4.0/ | We construct regular, asymptotically flat black holes of higher order scalar
tensor (DHOST) theories, which are obtained by making use of a generalized
Kerr-Schild solution generating method. The solutions depend on a mass
integration constant, admit a smooth core of chosen regularity, and generically
have an inner a... | [
{
"created": "Fri, 16 Apr 2021 16:56:39 GMT",
"version": "v1"
},
{
"created": "Sat, 24 Jul 2021 18:59:58 GMT",
"version": "v2"
}
] | 2021-07-27 | [
[
"Baake",
"Olaf",
""
],
[
"Charmousis",
"Christos",
""
],
[
"Hassaine",
"Mokhtar",
""
],
[
"Juan",
"Miguel San",
""
]
] | We construct regular, asymptotically flat black holes of higher order scalar tensor (DHOST) theories, which are obtained by making use of a generalized Kerr-Schild solution generating method. The solutions depend on a mass integration constant, admit a smooth core of chosen regularity, and generically have an inner and... | 16.923674 | 17.13796 | 14.843358 | 15.306801 | 15.567072 | 15.492777 | 17.856764 | 13.355283 | 14.868204 | 15.459358 | 16.350315 | 16.019337 | 15.200777 | 15.272167 | 15.679146 | 15.229392 | 17.068623 | 15.772698 | 16.36208 | 15.574854 | 15.858396 |
2112.00766 | Clifford V. Johnson | Clifford V. Johnson | Consistency Conditions for Non-Perturbative Completions of JT Gravity | 19 pages, 13 figures, 1 trumpet v2: Clarifying remarks made about a
class of solutions | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This is a careful examination of the key components of a large $N$ random
matrix model method for going beyond ordinary JT gravity's topological
expansion to define non-perturbative physics. It is offered as a simple and
(hopefully) clear framework within which any proposed non-perturbative
definition should fit, and... | [
{
"created": "Wed, 1 Dec 2021 19:00:06 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Jun 2022 04:08:55 GMT",
"version": "v2"
}
] | 2022-06-03 | [
[
"Johnson",
"Clifford V.",
""
]
] | This is a careful examination of the key components of a large $N$ random matrix model method for going beyond ordinary JT gravity's topological expansion to define non-perturbative physics. It is offered as a simple and (hopefully) clear framework within which any proposed non-perturbative definition should fit, and h... | 17.894634 | 17.764965 | 19.622515 | 16.602695 | 17.972719 | 17.000389 | 16.524536 | 16.419209 | 16.222185 | 20.388296 | 15.98622 | 17.481998 | 17.376661 | 16.564873 | 17.006369 | 16.958195 | 17.227194 | 17.15037 | 16.547882 | 17.80759 | 16.410223 |
hep-th/0609211 | Daniel Krefl | Michael Haack, Daniel Krefl, Dieter Lust, Antoine Van Proeyen and
Marco Zagermann | Gaugino Condensates and D-terms from D7-branes | 34 pages, 1 figure, LaTeX2e; References added, open issue concerning
higher derivative corrections clarified, other minor changes | JHEP 0701:078,2007 | 10.1088/1126-6708/2007/01/078 | LMU-ASC 64/06, MPP-2006-123, KUL-TF-06/24 | hep-th | null | We investigate, at the microscopic level, the compatibility between D-term
potentials from world-volume fluxes on D7-branes and non-perturbative
superpotentials arising from gaugino condensation on a different stack of
D7-branes. This is motivated by attempts to construct metastable de Sitter
vacua in type IIB string... | [
{
"created": "Thu, 28 Sep 2006 18:11:50 GMT",
"version": "v1"
},
{
"created": "Tue, 21 Nov 2006 16:06:26 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Haack",
"Michael",
""
],
[
"Krefl",
"Daniel",
""
],
[
"Lust",
"Dieter",
""
],
[
"Van Proeyen",
"Antoine",
""
],
[
"Zagermann",
"Marco",
""
]
] | We investigate, at the microscopic level, the compatibility between D-term potentials from world-volume fluxes on D7-branes and non-perturbative superpotentials arising from gaugino condensation on a different stack of D7-branes. This is motivated by attempts to construct metastable de Sitter vacua in type IIB string t... | 6.217729 | 6.627014 | 7.081823 | 6.199652 | 6.145839 | 6.465221 | 6.654478 | 6.324979 | 6.42592 | 7.210182 | 6.21313 | 6.518905 | 6.42382 | 6.281045 | 6.348831 | 6.408036 | 6.211773 | 6.224997 | 6.456172 | 6.545027 | 6.266544 |
2006.13964 | Jean-Fran\c{c}ois Fortin | Jean-Fran\c{c}ois Fortin, Wen-Jie Ma, Witold Skiba | Seven-Point Conformal Blocks in the Extended Snowflake Channel and
Beyond | 1+24 pages (+36 pages of appendixes), 8 figures | null | 10.1103/PhysRevD.102.125007 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Seven-point functions have two inequivalent topologies or channels. The comb
channel has been computed previously and here we compute scalar conformal
blocks in the extended snowflake channel in $d$ dimensions. Our computation
relies on the known action of the differential operator that sets up the
operator product e... | [
{
"created": "Wed, 24 Jun 2020 18:04:24 GMT",
"version": "v1"
}
] | 2020-12-30 | [
[
"Fortin",
"Jean-François",
""
],
[
"Ma",
"Wen-Jie",
""
],
[
"Skiba",
"Witold",
""
]
] | Seven-point functions have two inequivalent topologies or channels. The comb channel has been computed previously and here we compute scalar conformal blocks in the extended snowflake channel in $d$ dimensions. Our computation relies on the known action of the differential operator that sets up the operator product exp... | 8.361525 | 7.22787 | 8.877469 | 7.414459 | 8.023993 | 7.709421 | 7.617326 | 7.373046 | 7.568085 | 9.631556 | 7.596237 | 7.736115 | 7.66545 | 7.672899 | 7.925146 | 7.677408 | 7.642628 | 7.629592 | 7.644076 | 8.188262 | 7.849494 |
hep-th/9707063 | null | Friedemann Brandt, Joaquim Gomis, Joan Simon | The rigid symmetries of bosonic D-strings | 7 pages, revtex, no figures | Phys.Lett.B419:148-156,1998 | 10.1016/S0370-2693(97)01443-3 | UB-ECM-PF-97/12 | hep-th | null | We analyse the classical symmetries of bosonic D-string actions and
generalizations thereof. Among others, we show that the simplest actions of
this type have infinitely many nontrivial rigid symmetries which act
nontrivially and nonlinearly both on the target space coordinates and on the
U(1) gauge field, and form a... | [
{
"created": "Mon, 7 Jul 1997 04:16:37 GMT",
"version": "v1"
}
] | 2011-07-19 | [
[
"Brandt",
"Friedemann",
""
],
[
"Gomis",
"Joaquim",
""
],
[
"Simon",
"Joan",
""
]
] | We analyse the classical symmetries of bosonic D-string actions and generalizations thereof. Among others, we show that the simplest actions of this type have infinitely many nontrivial rigid symmetries which act nontrivially and nonlinearly both on the target space coordinates and on the U(1) gauge field, and form a K... | 10.18296 | 8.07446 | 9.781798 | 8.179136 | 8.482224 | 8.61537 | 9.006618 | 7.866766 | 7.843243 | 10.454393 | 8.177497 | 8.631521 | 9.368029 | 8.596622 | 8.809331 | 8.863809 | 8.612532 | 8.396877 | 8.818833 | 9.063098 | 8.809792 |
hep-th/9909195 | Jan Ambjorn | J. Ambjorn, B. Durhuus, T. Jonsson | Branched Polymers Re-Revisited | 5 pages | null | null | NBI-HE-99-36 | hep-th hep-lat | null | We point out some misconceptions in a recent paper by H. Aoki et al.
[hep-th/9909060]. In particular, the claim that the two-point function of
branched polymers behaves as 1/p^4 instead of 1/p^2 for large p is mistaken and
in no way a precondition for the Hausdorff dimension of branched polymers
having the well known... | [
{
"created": "Tue, 28 Sep 1999 09:21:55 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ambjorn",
"J.",
""
],
[
"Durhuus",
"B.",
""
],
[
"Jonsson",
"T.",
""
]
] | We point out some misconceptions in a recent paper by H. Aoki et al. [hep-th/9909060]. In particular, the claim that the two-point function of branched polymers behaves as 1/p^4 instead of 1/p^2 for large p is mistaken and in no way a precondition for the Hausdorff dimension of branched polymers having the well known v... | 9.786356 | 8.687768 | 8.603751 | 8.157514 | 8.846089 | 8.29899 | 8.136043 | 8.115199 | 7.836482 | 9.98746 | 8.426188 | 8.167452 | 8.707567 | 7.97301 | 7.988126 | 7.785836 | 8.022395 | 8.008952 | 8.108614 | 8.694846 | 8.021899 |
hep-th/0606009 | Riuji Mochizuki | Riuji Mochizuki | Eternally accelerating spacelike braneworld cosmologies | 8 pages, Mod. Phys. Lett. A Vol.21, No.40(2006) 2989-2996 | Mod.Phys.Lett.A21:2989-2996,2006 | 10.1142/S0217732306022456 | null | hep-th | null | We construct an eternally inflating spacelike brane world model. If the space
dimension of the brane is three (SM2) or six (SM5) for M theory or four (SD3)
for superstring theory, a time-dependent $n$-form field would supply a constant
energy density and cause exponentially expansion of the spacelike brane. In
these ... | [
{
"created": "Thu, 1 Jun 2006 08:10:15 GMT",
"version": "v1"
},
{
"created": "Fri, 2 Jun 2006 12:04:55 GMT",
"version": "v2"
},
{
"created": "Mon, 5 Jun 2006 10:47:19 GMT",
"version": "v3"
},
{
"created": "Fri, 9 Jun 2006 10:52:10 GMT",
"version": "v4"
},
{
"creat... | 2008-11-26 | [
[
"Mochizuki",
"Riuji",
""
]
] | We construct an eternally inflating spacelike brane world model. If the space dimension of the brane is three (SM2) or six (SM5) for M theory or four (SD3) for superstring theory, a time-dependent $n$-form field would supply a constant energy density and cause exponentially expansion of the spacelike brane. In these ca... | 11.936266 | 12.687763 | 12.049202 | 11.054584 | 11.507702 | 11.632261 | 11.408853 | 11.092884 | 11.407018 | 11.648768 | 10.456028 | 11.744666 | 11.871886 | 11.385324 | 11.414991 | 11.313201 | 11.76093 | 11.047854 | 11.438171 | 11.511643 | 10.908922 |
1712.09364 | Jay Armas | Jay Armas, Troels Harmark, Niels A. Obers | Extremal Black Hole Horizons | v2: 30pp, 12 figures; comments and reference added; comparison
between approximate and analytic black ring and Myers-Perry solutions added;
to be published in JHEP | JHEP 1803 (2018) 099 | 10.1007/JHEP03(2018)099 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the blackfold effective theory applied to extremal Kerr branes we
provide evidence for the existence of new stationary extremal black hole
solutions in asymptotically flat spacetime with both single and multiple
disconnected horizons. These include extremal doubly-spinning black rings,
black saturns, di-rings a... | [
{
"created": "Tue, 26 Dec 2017 19:00:06 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Mar 2018 11:35:31 GMT",
"version": "v2"
}
] | 2018-04-10 | [
[
"Armas",
"Jay",
""
],
[
"Harmark",
"Troels",
""
],
[
"Obers",
"Niels A.",
""
]
] | Using the blackfold effective theory applied to extremal Kerr branes we provide evidence for the existence of new stationary extremal black hole solutions in asymptotically flat spacetime with both single and multiple disconnected horizons. These include extremal doubly-spinning black rings, black saturns, di-rings and... | 8.001131 | 6.530374 | 7.653932 | 6.288457 | 7.262203 | 7.247169 | 6.755896 | 6.769503 | 6.2807 | 7.984099 | 6.230331 | 7.24066 | 7.432553 | 6.875727 | 7.187723 | 7.203183 | 7.114369 | 6.927882 | 6.924718 | 7.557615 | 7.001285 |
hep-th/9602066 | Walter Troost | Frederik Denef, Joris Raeymaekers, Urban M. Studer, Walter Troost | Classical Tunneling from the Lorentz-Dirac Equation | 9 pages, REVTEX, one eps-figure | null | null | KUL-TF-94/21 | hep-th astro-ph hep-ph | null | The classical equation of motion of a charged point particle, including its
radiation reaction, is described by the Lorentz-Dirac equation. We found a new
class of solutions that describe tunneling (in a completely classical
context!). For nonrelativistic electrons and a square barrier, the solution is
elementary and... | [
{
"created": "Tue, 13 Feb 1996 11:19:23 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Denef",
"Frederik",
""
],
[
"Raeymaekers",
"Joris",
""
],
[
"Studer",
"Urban M.",
""
],
[
"Troost",
"Walter",
""
]
] | The classical equation of motion of a charged point particle, including its radiation reaction, is described by the Lorentz-Dirac equation. We found a new class of solutions that describe tunneling (in a completely classical context!). For nonrelativistic electrons and a square barrier, the solution is elementary and e... | 17.115959 | 19.72563 | 16.892225 | 17.586712 | 16.187016 | 16.977812 | 17.650112 | 16.797342 | 17.391062 | 17.08288 | 16.773415 | 16.634842 | 16.333086 | 15.822978 | 16.784456 | 16.215689 | 16.324421 | 15.95933 | 16.630739 | 15.743712 | 16.472919 |
2003.05563 | Taro Tani | Naoto Kan, Shun'ya Mizoguchi, Taro Tani | Half-hypermultiplets and incomplete/complete resolutions in F-theory | 50 pages, 16 figures, v2: minor corrections | null | 10.1007/JHEP08(2020)063 | KEK-TH-2196 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider resolutions of codimension-two enhanced singularities from
$SO(12)$ to $E_7$ and from $E_7$ to $E_8$ in six-dimensional F-theory, where a
half-hypermultiplet arises for generic complex structures achieving them. The
exceptional fibers at the enhanced point exhibit different structures depending
on how the... | [
{
"created": "Thu, 12 Mar 2020 01:13:32 GMT",
"version": "v1"
},
{
"created": "Wed, 12 Aug 2020 07:53:19 GMT",
"version": "v2"
}
] | 2020-12-02 | [
[
"Kan",
"Naoto",
""
],
[
"Mizoguchi",
"Shun'ya",
""
],
[
"Tani",
"Taro",
""
]
] | We consider resolutions of codimension-two enhanced singularities from $SO(12)$ to $E_7$ and from $E_7$ to $E_8$ in six-dimensional F-theory, where a half-hypermultiplet arises for generic complex structures achieving them. The exceptional fibers at the enhanced point exhibit different structures depending on how the c... | 9.623517 | 11.38559 | 11.241163 | 9.748023 | 10.927985 | 11.234772 | 11.095739 | 10.245268 | 9.820424 | 12.327049 | 9.975692 | 9.499384 | 9.727968 | 9.325244 | 9.722668 | 9.867286 | 9.450459 | 9.483717 | 9.454308 | 9.898983 | 9.28907 |
hep-th/9802018 | George Leontaris | E.G. Floratos, G.K. Leontaris | A Note on the Supersymmetries of the Self-Dual Supermembrane | Latex file, 12pages, no figures | Phys.Lett. B428 (1998) 75-81 | 10.1016/S0370-2693(98)00398-0 | null | hep-th | null | In this letter we discuss the supersymmetry issue of the self dual
supermembranes in (8+1) and (4+1)-dimensions. We find that all genuine
solutions of the (8+1)-dimensional supermembrane, based on the exceptional
group G_2, preserve one of the sixteen supersymmetries while all solutions in
(4+1)-dimensions preserve e... | [
{
"created": "Wed, 4 Feb 1998 08:28:44 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Floratos",
"E. G.",
""
],
[
"Leontaris",
"G. K.",
""
]
] | In this letter we discuss the supersymmetry issue of the self dual supermembranes in (8+1) and (4+1)-dimensions. We find that all genuine solutions of the (8+1)-dimensional supermembrane, based on the exceptional group G_2, preserve one of the sixteen supersymmetries while all solutions in (4+1)-dimensions preserve eig... | 6.942922 | 6.599661 | 7.390566 | 6.067656 | 5.776297 | 5.818212 | 6.265237 | 6.100655 | 6.161385 | 6.819075 | 6.072929 | 6.072525 | 6.694603 | 5.903552 | 5.958383 | 6.039955 | 5.906586 | 6.123681 | 5.931293 | 6.441804 | 5.937891 |
hep-th/9910073 | Libin Fu | Yishi Duan, Libin Fu | The General Decomposition Theory of SU(2) Gauge Potential, Topological
Structure and Bifurcation of SU(2) Chern Density | revtex, 21pages, no figure | J.Math.Phys. 39 (1998) 4343-4355 | 10.1063/1.532515 | null | hep-th | null | By means of the geometric algebra the general decomposition of SU(2) gauge
potential on the sphere bundle of a compact and oriented 4-dimensional manifold
is given. Using this decomposition theory the SU(2) Chern density has been
studied in detail. It shows that the SU(2) Chern density can be expressed in
terms of th... | [
{
"created": "Fri, 8 Oct 1999 07:39:52 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Duan",
"Yishi",
""
],
[
"Fu",
"Libin",
""
]
] | By means of the geometric algebra the general decomposition of SU(2) gauge potential on the sphere bundle of a compact and oriented 4-dimensional manifold is given. Using this decomposition theory the SU(2) Chern density has been studied in detail. It shows that the SU(2) Chern density can be expressed in terms of the ... | 12.353979 | 11.198684 | 13.462465 | 11.551963 | 11.862153 | 11.88508 | 11.481207 | 11.844674 | 12.292172 | 13.016683 | 11.598445 | 11.864936 | 11.724039 | 11.542437 | 11.728923 | 11.761925 | 12.151226 | 11.556546 | 11.745587 | 11.592274 | 11.766233 |
1402.0828 | Tom Banks | T. Banks | Supersymmetry Breaking and the Cosmological Constant | 50 pages LaTeX2e, to be published in Int. J. Mod. Phys. A. The
section on Supersymmetric Large Extra Dimensions is derived from C. Burgess'
marvelous Les Houches lectures on this topic, arXiv:1309.4133 . This version
corrects many typos and missing references from the previous one. Third
version has corrections... | null | 10.1142/S0217751X14300105 | RUNHETC-2014-05 SCIPP 14/04 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | I review three attempts to explain the small value of the cosmological
constant, and their connection to SUSY breaking. They are The String Landscape,
Supersymmetric Large Extra Dimensions (SLED), and the Holographic Space-time
Formalism invented by Fischler and myself.
| [
{
"created": "Tue, 4 Feb 2014 18:49:04 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Apr 2014 19:22:30 GMT",
"version": "v2"
},
{
"created": "Thu, 22 May 2014 15:57:48 GMT",
"version": "v3"
}
] | 2015-06-18 | [
[
"Banks",
"T.",
""
]
] | I review three attempts to explain the small value of the cosmological constant, and their connection to SUSY breaking. They are The String Landscape, Supersymmetric Large Extra Dimensions (SLED), and the Holographic Space-time Formalism invented by Fischler and myself. | 12.660247 | 9.750031 | 10.949112 | 9.035981 | 8.313103 | 8.446592 | 9.384502 | 7.679742 | 7.598878 | 11.598132 | 8.84621 | 9.97967 | 10.749135 | 9.911122 | 9.681487 | 10.092168 | 9.709659 | 9.510599 | 9.244589 | 9.9252 | 9.90326 |
0811.4465 | Brett McInnes | Brett McInnes | Horizon Complementarity and Casimir Violations of the Null Energy
Condition | 30 pages including 7 figures | null | null | null | hep-th astro-ph gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The principle of horizon complementarity is an attempt to extend ideas about
black hole complementarity to all horizons, including cosmological ones. The
idea is that the degrees of freedom necessary to describe the interior of the
cosmic horizon of one observer in a given universe are in fact sufficient to
account f... | [
{
"created": "Thu, 27 Nov 2008 04:23:31 GMT",
"version": "v1"
},
{
"created": "Sat, 23 May 2009 08:36:49 GMT",
"version": "v2"
}
] | 2009-05-23 | [
[
"McInnes",
"Brett",
""
]
] | The principle of horizon complementarity is an attempt to extend ideas about black hole complementarity to all horizons, including cosmological ones. The idea is that the degrees of freedom necessary to describe the interior of the cosmic horizon of one observer in a given universe are in fact sufficient to account for... | 12.088971 | 11.884035 | 12.38447 | 11.447713 | 13.263761 | 12.736413 | 12.556364 | 11.638534 | 11.479702 | 12.119061 | 11.618126 | 12.038796 | 11.597302 | 11.395981 | 11.856483 | 11.525934 | 11.606325 | 11.732011 | 11.793954 | 11.880568 | 11.096615 |
hep-th/9904206 | Per Osland | Odd Magne Ogreid and Per Osland (Bergen) | More Series related to the Euler Series | 17 pages, LaTeX, uses elsart.cls | J.Comput.Appl.Math. 136 (2001) 389-403 | null | Bergen 1999-04 | hep-th hep-ph math-ph math.MP | null | We present results for infinite series appearing in Feynman diagram
calculations, many of which are similar to the Euler series. These include both
one-, two- and three-dimensional series. All these series can be expressed in
terms of zeta(2) and zeta(3).
| [
{
"created": "Thu, 29 Apr 1999 13:01:16 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ogreid",
"Odd Magne",
"",
"Bergen"
],
[
"Osland",
"Per",
"",
"Bergen"
]
] | We present results for infinite series appearing in Feynman diagram calculations, many of which are similar to the Euler series. These include both one-, two- and three-dimensional series. All these series can be expressed in terms of zeta(2) and zeta(3). | 9.500921 | 8.275855 | 8.493386 | 8.616604 | 8.356215 | 7.711669 | 9.856218 | 8.480628 | 8.043262 | 9.199949 | 8.68428 | 9.266205 | 8.948977 | 8.331265 | 9.549882 | 8.946511 | 9.364459 | 9.184137 | 8.91306 | 9.145876 | 9.323652 |
1603.06168 | Alexander Torres Gomez Dr. | Elizabeth Gasparim, Bruno Suzuki, Alexander Torres-Gomez and Carlos A.
B. Varea | Topological String Partition Function on Generalised Conifolds | v2 has small corrections, has improved exposition. Revised version to
appear in: "Journal of Mathematical Physics" | Journal of Mathematical Physics 58, 042303 (2017) | 10.1063/1.4980013 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the partition function on a generalised conifold $C_{m,n}$ with
${m+n \choose m}$ crepant resolutions can be equivalently computed on the
compound du Val singularity $A_{m+n-1}\times \mathbb C$ with a unique crepant
resolution.
| [
{
"created": "Sun, 20 Mar 2016 00:27:43 GMT",
"version": "v1"
},
{
"created": "Wed, 26 Apr 2017 12:58:28 GMT",
"version": "v2"
}
] | 2017-04-27 | [
[
"Gasparim",
"Elizabeth",
""
],
[
"Suzuki",
"Bruno",
""
],
[
"Torres-Gomez",
"Alexander",
""
],
[
"Varea",
"Carlos A. B.",
""
]
] | We show that the partition function on a generalised conifold $C_{m,n}$ with ${m+n \choose m}$ crepant resolutions can be equivalently computed on the compound du Val singularity $A_{m+n-1}\times \mathbb C$ with a unique crepant resolution. | 10.093925 | 9.495699 | 15.159943 | 9.569109 | 9.014305 | 11.518407 | 8.826141 | 10.006061 | 9.948273 | 17.479557 | 10.940928 | 9.275787 | 12.426366 | 9.357772 | 10.140235 | 9.659176 | 8.972324 | 9.573139 | 9.46665 | 10.743537 | 8.99878 |
1508.01608 | Justin David R | Subham Dutta Chowdhury, Justin R. David | Anomalous transport at weak coupling | 70 pages, 13 figures, typos corrected, added clarifications and a
reference | null | null | null | hep-th cond-mat.quant-gas | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We evaluate the contribution of chiral fermions in $d=2, 4, 6$, chiral
bosons, a chiral gravitino like theory in $d=2$ and chiral gravitinos in $d=6$
to all the leading parity odd transport coefficients at one loop. This is done
by using finite temperature field theory to evaluate the relevant Kubo
formulae. For chir... | [
{
"created": "Fri, 7 Aug 2015 05:18:11 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Sep 2015 00:54:46 GMT",
"version": "v2"
}
] | 2015-09-03 | [
[
"Chowdhury",
"Subham Dutta",
""
],
[
"David",
"Justin R.",
""
]
] | We evaluate the contribution of chiral fermions in $d=2, 4, 6$, chiral bosons, a chiral gravitino like theory in $d=2$ and chiral gravitinos in $d=6$ to all the leading parity odd transport coefficients at one loop. This is done by using finite temperature field theory to evaluate the relevant Kubo formulae. For chiral... | 7.866811 | 8.162424 | 8.48687 | 7.941346 | 8.45521 | 8.463678 | 8.390503 | 8.036731 | 7.749019 | 8.775345 | 7.619996 | 7.644058 | 7.913981 | 7.698079 | 7.575003 | 7.506618 | 7.448183 | 7.589803 | 7.768671 | 8.163421 | 7.435344 |
hep-th/9501053 | Banks Tomas | T. Banks, M.Berkooz, P.J. Steinhardt | The Cosmological Moduli Problem, Supersymmetry Breaking and Stability in
Postinflationary Cosmology | harvmac | Phys.Rev.D52:705-716,1995 | 10.1103/PhysRevD.52.705 | RU-94-92 | hep-th astro-ph hep-ph | null | A survey of solutions to the cosmological moduli problem in string theory.
The only extant proposal which may work is Intermediate Scale Inflation as
proposed by Randall and Thomas. Supersymmetry preserving dynamics which could
give large masses to the moduli is strongly constrained by cosmology and
requires the exis... | [
{
"created": "Fri, 13 Jan 1995 17:54:52 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Banks",
"T.",
""
],
[
"Berkooz",
"M.",
""
],
[
"Steinhardt",
"P. J.",
""
]
] | A survey of solutions to the cosmological moduli problem in string theory. The only extant proposal which may work is Intermediate Scale Inflation as proposed by Randall and Thomas. Supersymmetry preserving dynamics which could give large masses to the moduli is strongly constrained by cosmology and requires the existe... | 13.63163 | 15.504228 | 14.333383 | 13.79053 | 14.211884 | 15.688704 | 15.175275 | 13.163199 | 13.177418 | 14.229779 | 12.991318 | 14.033122 | 13.506665 | 13.422408 | 13.343364 | 13.973461 | 13.906909 | 13.93543 | 12.760798 | 12.728597 | 13.289664 |
1009.5690 | Ufuk Aydemir | Ufuk Aydemir, Luca Grisa, and Lorenzo Sorbo | Dynamical Four-Form Fields | 5 pages | Phys.Rev.D83:063516,2011 | 10.1103/PhysRevD.83.063516 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an example of a gauge-invariant Lagrangian that contains four
derivatives and describes one massive, non-ghostlike, degree of freedom.
| [
{
"created": "Tue, 28 Sep 2010 20:39:37 GMT",
"version": "v1"
}
] | 2011-03-22 | [
[
"Aydemir",
"Ufuk",
""
],
[
"Grisa",
"Luca",
""
],
[
"Sorbo",
"Lorenzo",
""
]
] | We present an example of a gauge-invariant Lagrangian that contains four derivatives and describes one massive, non-ghostlike, degree of freedom. | 14.0176 | 9.494796 | 10.211446 | 9.174812 | 11.157053 | 10.042527 | 11.487508 | 11.291768 | 10.492721 | 11.561557 | 9.708131 | 11.616679 | 11.539424 | 10.9812 | 11.559381 | 10.315085 | 11.109212 | 11.005602 | 11.647782 | 12.231867 | 10.851891 |
hep-th/0311216 | Ioannis Giannakis | Ioannis Giannakis, James T. Liu and Hai-cang Ren | The Radion in the Karch-Randall Braneworld | 19 pages, Plain Tex | Nucl.Phys. B681 (2004) 120-136 | 10.1016/j.nuclphysb.2004.01.004 | RU03-05B, MCTP-03-47 | hep-th gr-qc | null | In a braneworld context, the radion is a massless mode coupling to the trace
of the matter stress tensor. Since the radion also governs the separation
between branes, it is expected to decouple from the physical spectrum in single
brane scenarios, such as the one-brane Randall-Sundrum model. However, contrary
to expe... | [
{
"created": "Mon, 24 Nov 2003 17:11:48 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Giannakis",
"Ioannis",
""
],
[
"Liu",
"James T.",
""
],
[
"Ren",
"Hai-cang",
""
]
] | In a braneworld context, the radion is a massless mode coupling to the trace of the matter stress tensor. Since the radion also governs the separation between branes, it is expected to decouple from the physical spectrum in single brane scenarios, such as the one-brane Randall-Sundrum model. However, contrary to expect... | 6.502032 | 6.039173 | 6.300083 | 5.824739 | 6.113183 | 5.938044 | 5.905503 | 6.08744 | 5.724295 | 6.823351 | 6.214715 | 5.78832 | 6.006759 | 5.965231 | 5.774496 | 5.682324 | 5.836936 | 5.859874 | 6.073774 | 6.395051 | 5.775432 |
hep-th/9904080 | Mark D. Roberts | Mark D. Roberts | A Generalized Higgs Model | Discussion of the principles involved added, 6 pages | null | null | null | hep-th gr-qc | null | The Higgs model is generalized so that in addition to the radial Higgs field
there are fields which correspond to the themasy and entropy. The model is
further generalized to include state and sign parameters. A reduction to the
standard Higgs model is given and how to break symmetry using a non-zero VEV
(vacuum expe... | [
{
"created": "Sun, 11 Apr 1999 12:30:14 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Dec 2000 19:29:40 GMT",
"version": "v2"
},
{
"created": "Thu, 30 May 2002 19:07:01 GMT",
"version": "v3"
},
{
"created": "Sun, 14 Dec 2003 16:53:17 GMT",
"version": "v4"
}
] | 2007-05-23 | [
[
"Roberts",
"Mark D.",
""
]
] | The Higgs model is generalized so that in addition to the radial Higgs field there are fields which correspond to the themasy and entropy. The model is further generalized to include state and sign parameters. A reduction to the standard Higgs model is given and how to break symmetry using a non-zero VEV (vacuum expect... | 20.290884 | 22.306763 | 20.504892 | 18.515257 | 19.904356 | 19.630451 | 21.101841 | 20.893961 | 18.762339 | 20.063135 | 19.771957 | 19.031975 | 19.165319 | 19.204937 | 18.607157 | 19.139004 | 18.377254 | 18.613005 | 19.37122 | 18.889622 | 18.23402 |
1909.05489 | Hiroshi Suzuki | Masahiro Ashie, Okuto Morikawa, Hiroshi Suzuki, Hiromasa Takaura and
Kengo Takeuchi | Infrared renormalon in $SU(N)$ QCD(adj.) on $\mathbb{R}^3\times S^1$ | 24 pages, 1 figure, the final version to appear in PTEP | Prog Theor Exp Phys (2020) | 10.1093/ptep/ptz157 | KYUSHU-HET-198 | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the infrared renormalon in the gluon condensate in the $SU(N)$ gauge
theory with $n_W$-flavor adjoint Weyl fermions (QCD(adj.))
on~$\mathbb{R}^3\times S^1$ with the $\mathbb{Z}_N$ twisted boundary
conditions. We rely on the so-called large-$\beta_0$ approximation as a
conventional tool to analyze the renorma... | [
{
"created": "Thu, 12 Sep 2019 07:23:51 GMT",
"version": "v1"
},
{
"created": "Sat, 12 Oct 2019 12:09:46 GMT",
"version": "v2"
},
{
"created": "Fri, 17 Jan 2020 14:30:57 GMT",
"version": "v3"
}
] | 2020-02-12 | [
[
"Ashie",
"Masahiro",
""
],
[
"Morikawa",
"Okuto",
""
],
[
"Suzuki",
"Hiroshi",
""
],
[
"Takaura",
"Hiromasa",
""
],
[
"Takeuchi",
"Kengo",
""
]
] | We study the infrared renormalon in the gluon condensate in the $SU(N)$ gauge theory with $n_W$-flavor adjoint Weyl fermions (QCD(adj.)) on~$\mathbb{R}^3\times S^1$ with the $\mathbb{Z}_N$ twisted boundary conditions. We rely on the so-called large-$\beta_0$ approximation as a conventional tool to analyze the renormalo... | 5.639997 | 5.747125 | 5.910968 | 5.550065 | 5.882184 | 5.865649 | 6.072291 | 5.643788 | 5.461469 | 6.82542 | 5.836478 | 5.666591 | 5.705913 | 5.652161 | 5.792033 | 5.64328 | 5.761909 | 5.650456 | 5.470823 | 5.570755 | 5.540547 |
1705.02578 | Sergey Pavluchenko A. | Sergey A. Pavluchenko | Cosmological dynamics of spatially flat Einstein-Gauss-Bonnet models in
various dimensions: High-dimensional $\Lambda$-term case | 31 pages, 6 figures, 4 tables | Eur. Phys. J. C 77, 503 (2017) | 10.1140/epjc/s10052-017-5056-6 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we perform a systematic study of spatially flat
$[(3+D)+1]$-dimensional Einstein-Gauss-Bonnet cosmological models with
$\Lambda$-term. We consider models that topologically are the product of two
flat isotropic subspaces with different scale factors. One of these subspaces
is three-dimensional and repre... | [
{
"created": "Sun, 7 May 2017 08:16:12 GMT",
"version": "v1"
}
] | 2017-08-21 | [
[
"Pavluchenko",
"Sergey A.",
""
]
] | In this paper we perform a systematic study of spatially flat $[(3+D)+1]$-dimensional Einstein-Gauss-Bonnet cosmological models with $\Lambda$-term. We consider models that topologically are the product of two flat isotropic subspaces with different scale factors. One of these subspaces is three-dimensional and represe... | 5.778662 | 5.169742 | 5.937478 | 5.443081 | 5.361188 | 5.334156 | 5.450409 | 5.297105 | 5.334795 | 6.567723 | 5.411523 | 5.73823 | 5.77824 | 5.631167 | 5.704267 | 5.67235 | 5.7054 | 5.571454 | 5.72208 | 5.782019 | 5.696483 |
hep-th/0105283 | Yuji Satoh | Kazuo Hosomichi and Yuji Satoh | Operator product expansion in SL(2) conformal field theory | 10 pages, latex, discussion on primaries added, shortened version to
appear in MPL A | Mod.Phys.Lett.A17:683-693,2002 | 10.1142/S021773230200703X | YITP-01-47, UTHEP-442 | hep-th | null | In the conformal field theories having affine SL(2) symmetry, we study the
operator product expansion (OPE) involving primary fields in highest weight
representations. For this purpose, we analyze properties of primary fields with
definite SL(2) weights, and calculate their two- and three-point functions.
Using these... | [
{
"created": "Tue, 29 May 2001 07:41:40 GMT",
"version": "v1"
},
{
"created": "Wed, 25 Jul 2001 10:13:27 GMT",
"version": "v2"
},
{
"created": "Wed, 27 Mar 2002 11:38:47 GMT",
"version": "v3"
},
{
"created": "Thu, 28 Mar 2002 11:05:47 GMT",
"version": "v4"
},
{
"c... | 2014-11-18 | [
[
"Hosomichi",
"Kazuo",
""
],
[
"Satoh",
"Yuji",
""
]
] | In the conformal field theories having affine SL(2) symmetry, we study the operator product expansion (OPE) involving primary fields in highest weight representations. For this purpose, we analyze properties of primary fields with definite SL(2) weights, and calculate their two- and three-point functions. Using these c... | 6.915656 | 6.204281 | 7.221326 | 6.452198 | 6.790592 | 6.309741 | 6.136465 | 6.484449 | 6.02992 | 7.183492 | 6.225657 | 6.544753 | 7.068335 | 6.547421 | 6.65359 | 6.376113 | 6.273785 | 6.609484 | 6.469441 | 6.972379 | 6.507841 |
hep-th/0306251 | Hiroshi Umetsu | Machiko Hatsuda, Satoshi Iso and Hiroshi Umetsu | Noncommutative Superspace, Supermatrix and Lowest Landau Level | 29 pages, Latex. A subsection is added to explain the Seiberg's
noncommutative superspace as a constrained system | Nucl.Phys. B671 (2003) 217-242 | 10.1016/j.nuclphysb.2003.08.013 | KEK-TH-896 | hep-th | null | By using graded (super) Lie algebras, we can construct noncommutative
superspace on curved homogeneous manifolds. In this paper, we take a flat limit
to obtain flat noncommutative superspace. We particularly consider $d=2$ and
$d=4$ superspaces based on the graded Lie algebras $osp(1|2)$, $su(2|1)$ and
$psu(2|2)$. Ja... | [
{
"created": "Wed, 25 Jun 2003 18:43:48 GMT",
"version": "v1"
},
{
"created": "Thu, 3 Jul 2003 14:10:25 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Hatsuda",
"Machiko",
""
],
[
"Iso",
"Satoshi",
""
],
[
"Umetsu",
"Hiroshi",
""
]
] | By using graded (super) Lie algebras, we can construct noncommutative superspace on curved homogeneous manifolds. In this paper, we take a flat limit to obtain flat noncommutative superspace. We particularly consider $d=2$ and $d=4$ superspaces based on the graded Lie algebras $osp(1|2)$, $su(2|1)$ and $psu(2|2)$. Jaco... | 6.934051 | 6.216798 | 6.519154 | 6.083258 | 5.623906 | 6.142718 | 5.986821 | 6.271266 | 5.833466 | 7.067203 | 5.925294 | 6.077274 | 6.268279 | 6.029897 | 6.012053 | 5.921535 | 6.168256 | 5.822274 | 6.030343 | 6.39974 | 5.916823 |
1107.3232 | Igor Bandos A. | Igor A. Bandos and Carlos Meliveo | Three form potential in (special) minimal supergravity superspace and
supermembrane supercurrent | 18 pages, no figures. V2: Important references added. The abstract
and presentation have been changed to reflect the overloop with that.
Submitted to the QTS7 Proceedings. J. Phys. style used | null | 10.1088/1742-6596/343/1/012012 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This contribution begins the study of the complete superfield Lagrangian
description of the interacting system of D=4 N=1 supergravity (SUGRA) and
supermembrane. Firstly, we review a 'three form supergravity' by Ovrut and
Waldram, which we prefer to call 'special minimal supergravity'. This off-shell
formulation of s... | [
{
"created": "Sat, 16 Jul 2011 13:00:50 GMT",
"version": "v1"
},
{
"created": "Wed, 2 Nov 2011 15:23:01 GMT",
"version": "v2"
}
] | 2015-05-28 | [
[
"Bandos",
"Igor A.",
""
],
[
"Meliveo",
"Carlos",
""
]
] | This contribution begins the study of the complete superfield Lagrangian description of the interacting system of D=4 N=1 supergravity (SUGRA) and supermembrane. Firstly, we review a 'three form supergravity' by Ovrut and Waldram, which we prefer to call 'special minimal supergravity'. This off-shell formulation of sim... | 9.487537 | 9.294724 | 10.861609 | 9.052919 | 9.352421 | 8.657889 | 9.437475 | 8.59867 | 8.588033 | 10.987256 | 8.322681 | 9.091904 | 9.625327 | 9.218848 | 9.026849 | 9.05431 | 9.114006 | 9.047777 | 9.070726 | 9.53519 | 8.739216 |
1904.11728 | Takao Suyama | Takao Suyama | Linear Chern-Simons-matter Theories in the Planar Limit | 24 pages, 3 figures | null | 10.1007/JHEP08(2019)083 | KEK-TH-2126 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study ${\cal N}=3$ linear Chern-Simons-matter theories in the planar
limit. The matter content of the theory is depicted by a linear-shape diagram
with $n$ nodes and $n-1$ links for any $n$. The free energy and the vevs of BPS
Wilson loops are given in terms of a single 1-form on $\mathbb{CP}^1$ which can
be deter... | [
{
"created": "Fri, 26 Apr 2019 09:13:06 GMT",
"version": "v1"
}
] | 2019-09-04 | [
[
"Suyama",
"Takao",
""
]
] | We study ${\cal N}=3$ linear Chern-Simons-matter theories in the planar limit. The matter content of the theory is depicted by a linear-shape diagram with $n$ nodes and $n-1$ links for any $n$. The free energy and the vevs of BPS Wilson loops are given in terms of a single 1-form on $\mathbb{CP}^1$ which can be determi... | 8.072418 | 6.708032 | 8.053741 | 6.556448 | 6.691071 | 7.050494 | 7.252397 | 6.590102 | 6.678545 | 8.657585 | 6.75356 | 7.046871 | 7.110965 | 6.804883 | 6.917606 | 6.685731 | 6.833869 | 6.830956 | 6.852922 | 7.213354 | 7.041457 |
hep-th/0209123 | Petko Al. Nikolov | Petko A. Nikolov, Gergana R. Ruseva | Dimensional Reduction of Dirac Operator | 11 pages, LATEX, | J.Math.Phys. 47 (2006) 073503 | 10.1063/1.2217811 | null | hep-th | null | We construct an explicit example of dimensional reduction of the free
massless Dirac operator with an internal SU(3) symmetry, defined on a
twelve-dimensional manifold that is the total space of a principal SU(3)-bundle
over a four-dimensional (nonflat) pseudo-Riemannian manifold. Upon dimensional
reduction the free ... | [
{
"created": "Sat, 14 Sep 2002 15:21:34 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Feb 2008 10:40:41 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Nikolov",
"Petko A.",
""
],
[
"Ruseva",
"Gergana R.",
""
]
] | We construct an explicit example of dimensional reduction of the free massless Dirac operator with an internal SU(3) symmetry, defined on a twelve-dimensional manifold that is the total space of a principal SU(3)-bundle over a four-dimensional (nonflat) pseudo-Riemannian manifold. Upon dimensional reduction the free tw... | 9.055367 | 9.85164 | 9.112001 | 8.717066 | 9.535383 | 10.259158 | 9.678357 | 9.289402 | 9.063893 | 9.703984 | 9.17036 | 9.505203 | 8.994055 | 8.844213 | 9.200863 | 8.885874 | 8.929469 | 9.216018 | 8.746858 | 9.10954 | 9.163914 |
hep-th/9902073 | Daniel Kabat | Daniel Kabat (IAS), Gilad Lifschytz (Princeton University) | Gauge theory origins of supergravity causal structure | 20 pages, LaTeX. v2: added references, expanded discussion of
Gaussian approximation, added comments on M(atrix) causality | JHEP 9905:005,1999 | 10.1088/1126-6708/1999/05/005 | IASSNS-HEP-99/18, PUPT-1817 | hep-th | null | We discuss the gauge theory mechanisms which are responsible for the causal
structure of the dual supergravity. For D-brane probes we show that the light
cone structure and Killing horizons of supergravity emerge dynamically. They
are associated with the appearance of new light degrees of freedom in the gauge
theory,... | [
{
"created": "Wed, 10 Feb 1999 18:27:32 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 1999 03:07:56 GMT",
"version": "v2"
}
] | 2010-02-03 | [
[
"Kabat",
"Daniel",
"",
"IAS"
],
[
"Lifschytz",
"Gilad",
"",
"Princeton University"
]
] | We discuss the gauge theory mechanisms which are responsible for the causal structure of the dual supergravity. For D-brane probes we show that the light cone structure and Killing horizons of supergravity emerge dynamically. They are associated with the appearance of new light degrees of freedom in the gauge theory, w... | 10.108851 | 9.86036 | 10.279152 | 9.202712 | 9.737545 | 9.159696 | 9.463568 | 9.804575 | 8.833333 | 10.864415 | 9.598956 | 8.994865 | 9.583708 | 8.683191 | 9.238045 | 9.410692 | 9.125744 | 9.381116 | 9.247999 | 9.434414 | 8.924998 |
1904.00060 | Andrei Parnachev | Robin Karlsson, Manuela Kulaxizi, Andrei Parnachev and Petar Tadi\'c | Black Holes and Conformal Regge Bootstrap | 39 pages, harvmac; v2: minor corrections, a reference added. v3:
discussion of the flat space limit added, typos fixed | JHEP10(2019)046 | 10.1007/JHEP10(2019)046 | TCDMATH 19-02 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Highly energetic particles traveling in the background of an asymptotically
AdS black hole experience a Shapiro time delay and an angle deflection. These
quantities are related to the Regge limit of a heavy-heavy-light-light
four-point function of scalar operators in the dual CFT. The Schwarzschild
radius of the blac... | [
{
"created": "Fri, 29 Mar 2019 19:22:27 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Jun 2019 15:07:45 GMT",
"version": "v2"
},
{
"created": "Thu, 15 Aug 2019 20:20:04 GMT",
"version": "v3"
}
] | 2019-10-28 | [
[
"Karlsson",
"Robin",
""
],
[
"Kulaxizi",
"Manuela",
""
],
[
"Parnachev",
"Andrei",
""
],
[
"Tadić",
"Petar",
""
]
] | Highly energetic particles traveling in the background of an asymptotically AdS black hole experience a Shapiro time delay and an angle deflection. These quantities are related to the Regge limit of a heavy-heavy-light-light four-point function of scalar operators in the dual CFT. The Schwarzschild radius of the black ... | 7.665761 | 7.28614 | 9.072446 | 6.677877 | 6.791503 | 7.069262 | 6.47508 | 6.870965 | 7.159543 | 10.437742 | 6.741739 | 6.838666 | 7.613832 | 7.128296 | 7.344066 | 7.206409 | 7.236257 | 7.236984 | 7.274416 | 7.7128 | 7.155558 |
2111.11958 | Giovani Peruzzo | David Dudal, Duifje Maria van Egmond, Igor Figueiredo Justo, Giovani
Peruzzo, Silvio Paolo Sorella | Gauge Invariant Description of the $SU(2)$ Higgs model: Ward identities
and Renormalization | null | null | 10.1103/PhysRevD.105.065018 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The renormalization properties of two local gauge invariant composite
operators $(O,R^a_{\mu})$ corresponding, respectively, to the gauge invariant
description of the Higgs particle and of the massive gauge vector boson, are
analyzed to all orders in perturbation theory by means of the algebraic
renormalization in th... | [
{
"created": "Tue, 23 Nov 2021 15:52:57 GMT",
"version": "v1"
}
] | 2022-04-13 | [
[
"Dudal",
"David",
""
],
[
"van Egmond",
"Duifje Maria",
""
],
[
"Justo",
"Igor Figueiredo",
""
],
[
"Peruzzo",
"Giovani",
""
],
[
"Sorella",
"Silvio Paolo",
""
]
] | The renormalization properties of two local gauge invariant composite operators $(O,R^a_{\mu})$ corresponding, respectively, to the gauge invariant description of the Higgs particle and of the massive gauge vector boson, are analyzed to all orders in perturbation theory by means of the algebraic renormalization in the ... | 6.339915 | 5.978163 | 6.625738 | 6.434904 | 6.525432 | 6.206616 | 6.520822 | 6.19729 | 6.212474 | 7.448016 | 6.211602 | 6.042895 | 6.510038 | 6.270092 | 6.381122 | 6.121456 | 6.168157 | 6.074579 | 6.264257 | 6.483686 | 6.229998 |
2212.02316 | Anna Pachol | Jerzy Lukierski, Stjepan Meljanac, Salvatore Mignemi, Anna Pacho{\l} | Quantum perturbative solutions of extended Snyder and Yang models with
spontaneous symmetry breaking | 11 pages; published version | null | 10.1016/j.physletb.2023.138261 | null | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose $\hbar$-expansions as perturbative solutions of quantum extended
Snyder and Yang models, with $\hbar$-independent classical zero-th order terms
responsible for the spontaneous breaking of $D=4$ and $D=5$ de Sitter
symmetries. In such models, with algebraic basis spanned by $\hat o(D,1)$ Lie
algebra generat... | [
{
"created": "Mon, 5 Dec 2022 14:42:11 GMT",
"version": "v1"
},
{
"created": "Wed, 13 Sep 2023 16:15:48 GMT",
"version": "v2"
},
{
"created": "Wed, 25 Oct 2023 09:11:10 GMT",
"version": "v3"
}
] | 2023-10-26 | [
[
"Lukierski",
"Jerzy",
""
],
[
"Meljanac",
"Stjepan",
""
],
[
"Mignemi",
"Salvatore",
""
],
[
"Pachoł",
"Anna",
""
]
] | We propose $\hbar$-expansions as perturbative solutions of quantum extended Snyder and Yang models, with $\hbar$-independent classical zero-th order terms responsible for the spontaneous breaking of $D=4$ and $D=5$ de Sitter symmetries. In such models, with algebraic basis spanned by $\hat o(D,1)$ Lie algebra generator... | 12.040989 | 12.109057 | 12.696773 | 11.531013 | 12.861485 | 11.942267 | 12.081118 | 11.645089 | 11.861743 | 13.363978 | 11.663311 | 11.806406 | 12.475632 | 11.587289 | 12.097763 | 11.753479 | 12.44825 | 11.617914 | 11.931745 | 12.179982 | 11.40367 |
hep-th/0311157 | Peter Horvathy | P. A. Horvathy and P. C. Stichel | Moving vortices in noncommutative gauge theory | Latex, 6 pages, no figures. A result similar to ours was obtained,
independently, by Hadasz et al. in the revised version of their paper | Phys.Lett. B583 (2004) 353-356 | 10.1016/j.physletb.2003.12.063 | null | hep-th | null | Exact time-dependent solutions of nonrelativistic noncommutative Chern -
Simons gauge theory are presented in closed analytic form. They are different
from (indeed orthogonal to) those discussed recently by Hadasz, Lindstrom,
Rocek and von Unge. Unlike theirs, our solutions can move with an arbitrary
constant velocit... | [
{
"created": "Tue, 18 Nov 2003 07:46:29 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Nov 2003 07:05:25 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Horvathy",
"P. A.",
""
],
[
"Stichel",
"P. C.",
""
]
] | Exact time-dependent solutions of nonrelativistic noncommutative Chern - Simons gauge theory are presented in closed analytic form. They are different from (indeed orthogonal to) those discussed recently by Hadasz, Lindstrom, Rocek and von Unge. Unlike theirs, our solutions can move with an arbitrary constant velocity,... | 11.730503 | 12.295731 | 13.469237 | 10.740235 | 11.271358 | 9.947248 | 10.445239 | 10.070875 | 10.313556 | 15.346946 | 11.115878 | 10.035657 | 12.685703 | 10.117634 | 10.017172 | 10.685762 | 10.567418 | 10.283618 | 10.39806 | 10.613298 | 9.660297 |
hep-th/9407138 | null | Martin Markl and Steve Shnider | Drinfel'd algebra deformations, homotopy comodules and the associahedra | 44 pages | null | null | null | hep-th math.QA | null | The aim of this work is to construct a cohomology theory controlling the
deformations of a general Drinfel'd algebra. The task is accomplished in three
steps. The first step is the construction of a modified cobar complex adapted
to a non-coassociative comultiplication. The following two steps each involve a
new, hig... | [
{
"created": "Thu, 21 Jul 1994 14:36:42 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Markl",
"Martin",
""
],
[
"Shnider",
"Steve",
""
]
] | The aim of this work is to construct a cohomology theory controlling the deformations of a general Drinfel'd algebra. The task is accomplished in three steps. The first step is the construction of a modified cobar complex adapted to a non-coassociative comultiplication. The following two steps each involve a new, highl... | 6.479063 | 7.360957 | 7.764175 | 6.962812 | 8.045477 | 7.708013 | 7.767923 | 7.259453 | 7.412006 | 7.91614 | 7.030535 | 6.587623 | 6.671277 | 6.628683 | 6.815938 | 6.662055 | 6.728867 | 6.774755 | 6.684601 | 6.777162 | 6.586783 |
hep-th/0601026 | Hiroshi Suzuki | Masashi Hayakawa and Hiroshi Suzuki | Gauge Anomaly associated with the Majorana Fermion in $8k+1$ dimensions | 10 pages, uses PTPTeX.cls, the final version to appear in Prog.
Theor. Phys | Prog.Theor.Phys. 115 (2006) 1129-1136 | 10.1143/PTP.115.1129 | RIKEN-TH-62 | hep-th hep-lat | null | Using an elementary method, we show that an odd number of Majorana fermions
in $8k+1$ dimensions suffer from a gauge anomaly that is analogous to the
Witten global gauge anomaly. This anomaly cannot be removed without sacrificing
the perturbative gauge invariance. Our construction of higher-dimensional
examples ($k g... | [
{
"created": "Thu, 5 Jan 2006 07:17:19 GMT",
"version": "v1"
},
{
"created": "Fri, 26 May 2006 08:31:58 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Hayakawa",
"Masashi",
""
],
[
"Suzuki",
"Hiroshi",
""
]
] | Using an elementary method, we show that an odd number of Majorana fermions in $8k+1$ dimensions suffer from a gauge anomaly that is analogous to the Witten global gauge anomaly. This anomaly cannot be removed without sacrificing the perturbative gauge invariance. Our construction of higher-dimensional examples ($k geq... | 14.041716 | 12.624578 | 12.346828 | 11.241796 | 13.224861 | 12.795826 | 12.147215 | 12.008037 | 12.284216 | 12.744843 | 12.147574 | 12.088134 | 11.883964 | 11.752319 | 11.693725 | 12.38173 | 12.246758 | 11.850948 | 11.446219 | 12.421491 | 11.704486 |
1004.3500 | Anastasios Taliotis | Anastasios Taliotis | Heavy Ion Collisions with Transverse Dynamics from Evolving AdS
Geometries | 60 pages, 7 figures | JHEP 1009:102,2010 | 10.1007/JHEP09(2010)102 | null | hep-th gr-qc hep-ph nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Currently there exists no known way to construct the Stress-Energy Tensor
$(T_{\mu \nu})$ of the produced medium in heavy ion collisions at strong
coupling from purely theoretical grounds. In this paper, some steps are taken
in that direction. In particular, the evolution of $T_{\mu \nu}$ at strong
coupling and at hi... | [
{
"created": "Tue, 20 Apr 2010 16:45:41 GMT",
"version": "v1"
},
{
"created": "Sun, 11 Jul 2010 19:28:11 GMT",
"version": "v2"
},
{
"created": "Wed, 1 Dec 2010 00:29:33 GMT",
"version": "v3"
}
] | 2010-12-02 | [
[
"Taliotis",
"Anastasios",
""
]
] | Currently there exists no known way to construct the Stress-Energy Tensor $(T_{\mu \nu})$ of the produced medium in heavy ion collisions at strong coupling from purely theoretical grounds. In this paper, some steps are taken in that direction. In particular, the evolution of $T_{\mu \nu}$ at strong coupling and at high... | 8.129539 | 8.474821 | 8.44911 | 7.730927 | 7.990932 | 7.917112 | 8.44727 | 8.374185 | 7.931183 | 8.467423 | 7.879162 | 7.883462 | 7.878086 | 7.765394 | 7.761027 | 7.866423 | 7.720796 | 7.7454 | 7.72934 | 8.096073 | 7.847666 |
1207.7130 | Everton Murilo Carvalho Abreu | Everton M. C. Abreu and N\'elio Sasaki | Noncommutative wormholes and the energy conditions | 7 pages. Preprint format | null | null | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is a very well known fact that the energy conditions concerning Lorentzian
wormhole (WH) solutions of Einstein equations are violated. Consequently,
attempts to avoid the violation of the energy conditions constitutes one of the
main areas of research in WH physics. On the other hand, the current literature
show u... | [
{
"created": "Mon, 30 Jul 2012 23:12:53 GMT",
"version": "v1"
}
] | 2012-08-01 | [
[
"Abreu",
"Everton M. C.",
""
],
[
"Sasaki",
"Nélio",
""
]
] | It is a very well known fact that the energy conditions concerning Lorentzian wormhole (WH) solutions of Einstein equations are violated. Consequently, attempts to avoid the violation of the energy conditions constitutes one of the main areas of research in WH physics. On the other hand, the current literature show us ... | 8.497595 | 9.126512 | 7.685082 | 7.751888 | 8.466817 | 8.293464 | 9.164707 | 6.823796 | 8.577071 | 6.727342 | 8.500663 | 8.093758 | 7.804335 | 7.842029 | 7.969891 | 7.776807 | 8.197198 | 7.571392 | 8.196385 | 7.704733 | 8.185698 |
hep-th/9508158 | Lev F. M. | Felix M. Lev | The Problem of Constructing the Current Operators in Quantum Field
Theory | 7 pages, LaTeX | null | null | null | hep-th | null | Lorentz invariance of the current operators implies that they satisfy the
well-known commutation relations with the representation operators of the
Lorentz group. It is shown that if the standard construction of the current
operators in quantum field theory is used then the commutation relations are
broken by the Sch... | [
{
"created": "Tue, 29 Aug 1995 09:17:44 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Lev",
"Felix M.",
""
]
] | Lorentz invariance of the current operators implies that they satisfy the well-known commutation relations with the representation operators of the Lorentz group. It is shown that if the standard construction of the current operators in quantum field theory is used then the commutation relations are broken by the Schwi... | 8.350012 | 6.721331 | 7.129959 | 6.607615 | 7.069163 | 6.964509 | 7.34301 | 7.519918 | 6.373426 | 7.261611 | 6.796695 | 6.749447 | 6.884079 | 6.490254 | 6.625181 | 6.550773 | 6.552098 | 6.881335 | 6.35434 | 6.515699 | 6.698802 |
1208.4036 | Xi Yin | Simone Giombi, Xi Yin | The Higher Spin/Vector Model Duality | 55 pages, 1 figure. Contribution to J. Phys. A special volume on
"Higher Spin Theories and AdS/CFT" edited by M. R. Gaberdiel and M. Vasiliev.
v2: references added | null | 10.1088/1751-8113/46/21/214003 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper is mainly a review of the dualities between Vasiliev's higher spin
gauge theories in AdS4 and three dimensional large N vector models, with focus
on the holographic calculation of correlation functions of higher spin
currents. We also present some new results in the computation of parity odd
structures in ... | [
{
"created": "Mon, 20 Aug 2012 15:12:26 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Aug 2012 15:43:09 GMT",
"version": "v2"
}
] | 2015-06-11 | [
[
"Giombi",
"Simone",
""
],
[
"Yin",
"Xi",
""
]
] | This paper is mainly a review of the dualities between Vasiliev's higher spin gauge theories in AdS4 and three dimensional large N vector models, with focus on the holographic calculation of correlation functions of higher spin currents. We also present some new results in the computation of parity odd structures in th... | 10.699512 | 7.36257 | 10.709418 | 7.535369 | 7.445232 | 7.30208 | 7.610518 | 7.784719 | 7.788515 | 11.702826 | 8.227192 | 8.066378 | 9.270318 | 8.216479 | 8.540976 | 7.690622 | 8.607141 | 8.074876 | 8.057564 | 9.539774 | 8.13925 |
hep-th/0009230 | Stefan Schraml | John Madore, Stefan Schraml, Peter Schupp, Julius Wess | External Fields as Intrinsic Geometry | 19 pages, Latex | Eur.Phys.J.C18:785-794,2001 | 10.1007/s100520100566 | null | hep-th | null | There is an interesting dichotomy between a space-time metric considered as
external field in a flat background and the same considered as an intrinsic
part of the geometry of space-time. We shall describe and compare two other
external fields which can be absorbed into an appropriate redefinition of the
geometry, th... | [
{
"created": "Thu, 28 Sep 2000 12:42:19 GMT",
"version": "v1"
}
] | 2009-01-07 | [
[
"Madore",
"John",
""
],
[
"Schraml",
"Stefan",
""
],
[
"Schupp",
"Peter",
""
],
[
"Wess",
"Julius",
""
]
] | There is an interesting dichotomy between a space-time metric considered as external field in a flat background and the same considered as an intrinsic part of the geometry of space-time. We shall describe and compare two other external fields which can be absorbed into an appropriate redefinition of the geometry, this... | 15.298843 | 16.679127 | 14.738018 | 14.770556 | 16.466629 | 16.161116 | 16.458704 | 16.149668 | 15.904556 | 15.390073 | 15.801057 | 15.15976 | 14.996046 | 14.590454 | 14.874479 | 15.466023 | 15.538613 | 14.995557 | 14.94202 | 15.516198 | 15.172641 |
1003.1668 | Leonard Fister | Leonard Fister, Reinhard Alkofer, Kai Schwenzer | On the Infrared Behavior of Landau Gauge Yang-Mills Theory with a
Fundamentally Charged Scalar Field | 8 pages, PDFLaTex | Phys. Lett. B688:237-243, 2010 | 10.1016/j.physletb.2010.04.001 | null | hep-th hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently it has been shown that infrared singularities of Landau gauge QCD
can confine static quarks via a linearly rising potential. We show that the
same mechanism can also provide a confining interaction between charged scalar
fields in the fundamental representation. This confirms that within this
scenario static... | [
{
"created": "Mon, 8 Mar 2010 16:42:55 GMT",
"version": "v1"
}
] | 2010-05-07 | [
[
"Fister",
"Leonard",
""
],
[
"Alkofer",
"Reinhard",
""
],
[
"Schwenzer",
"Kai",
""
]
] | Recently it has been shown that infrared singularities of Landau gauge QCD can confine static quarks via a linearly rising potential. We show that the same mechanism can also provide a confining interaction between charged scalar fields in the fundamental representation. This confirms that within this scenario static c... | 12.444691 | 12.581533 | 10.286553 | 10.221627 | 10.799244 | 12.675321 | 11.751938 | 10.671563 | 10.922379 | 10.806215 | 11.135876 | 11.63796 | 10.500113 | 10.806739 | 10.852434 | 11.332152 | 10.944622 | 10.80441 | 10.861372 | 10.823502 | 10.80457 |
hep-th/9903077 | Carmelo Perez Martin | C.P. Martin and D. Sanchez-Ruiz (Departamento de Fisica Teorica I,
Universidad Complutense de Madrid, Spain) | The One-loop UV Divergent Structure of U(1) Yang-Mills Theory on
Noncommutative R^4 | 8 pages. A missing complex "i" is included in the field strength and
the divergent contributions corrected accordingly. As a result the model
turns out to be asymptotically free | Phys.Rev.Lett. 83 (1999) 476-479 | 10.1103/PhysRevLett.83.476 | FT/UCM-15-99 | hep-th | null | We show that U(1) Yang-Mills theory on noncommutative R^4 can be renormalized
at the one-loop level by multiplicative dimensional renormalization of the
coupling constant and fields of the theory. We compute the beta function of the
theory and conclude that the theory is asymptotically free. We also show that
the Wey... | [
{
"created": "Tue, 9 Mar 1999 17:57:02 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Mar 1999 16:11:17 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Martin",
"C. P.",
"",
"Departamento de Fisica Teorica I,\n Universidad Complutense de Madrid, Spain"
],
[
"Sanchez-Ruiz",
"D.",
"",
"Departamento de Fisica Teorica I,\n Universidad Complutense de Madrid, Spain"
]
] | We show that U(1) Yang-Mills theory on noncommutative R^4 can be renormalized at the one-loop level by multiplicative dimensional renormalization of the coupling constant and fields of the theory. We compute the beta function of the theory and conclude that the theory is asymptotically free. We also show that the Weyl-... | 5.463883 | 5.176861 | 5.48983 | 4.525991 | 5.082734 | 4.590356 | 4.519702 | 4.784405 | 4.505502 | 5.585355 | 4.545334 | 4.762784 | 5.509389 | 5.087471 | 4.925771 | 5.031029 | 4.936913 | 4.740542 | 5.140994 | 5.62864 | 5.12149 |
hep-th/9204003 | Srinandan Dasmahapatra | Srinandan Dasmahapatra, Rinat Kedem and Barry McCoy | Physics beyond quasi-particles: Spectrum and completeness of the 3 state
superintegrable chiral Potts model | (39 pages) | Nucl.Phys. B396 (1993) 506-540 | 10.1016/0550-3213(93)90662-9 | null | hep-th | null | We find the rules which count the energy levels of the 3 state
superintegrable chiral Potts model and demonstrate that these rules are
complete. We then derive the complete spectrum of excitations in the
thermodynamic limit in the massive phase and demonstrate the existence of
excitations which do not have a quasi-pa... | [
{
"created": "Thu, 2 Apr 1992 19:33:45 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Dasmahapatra",
"Srinandan",
""
],
[
"Kedem",
"Rinat",
""
],
[
"McCoy",
"Barry",
""
]
] | We find the rules which count the energy levels of the 3 state superintegrable chiral Potts model and demonstrate that these rules are complete. We then derive the complete spectrum of excitations in the thermodynamic limit in the massive phase and demonstrate the existence of excitations which do not have a quasi-part... | 12.689157 | 10.278618 | 13.690718 | 10.617972 | 10.816567 | 11.009682 | 11.66444 | 11.293858 | 10.135566 | 13.73926 | 9.562325 | 10.311872 | 12.526218 | 11.378055 | 10.996406 | 10.348959 | 10.629473 | 10.784763 | 11.03475 | 12.932792 | 10.356771 |
hep-th/0207241 | Zarembo | A.A. Tseytlin, K. Zarembo | Wilson loops in N=4 SYM theory: rotation in S5 | 22 pages, 2 figures | Phys.Rev.D66:125010,2002 | 10.1103/PhysRevD.66.125010 | ITEP-TH-34/02 | hep-th | null | We study Wilson loops in N=4 SYM theory which are non-constant in the scalar
(S5) directions and open string solutions associated with them in the context
of AdS/CFT correspondence. An interplay between Minkowskian and Euclidean
pictures turns out to be non-trivial for time-dependent Wilson loops. We find
that in the... | [
{
"created": "Fri, 26 Jul 2002 14:34:21 GMT",
"version": "v1"
}
] | 2009-09-17 | [
[
"Tseytlin",
"A. A.",
""
],
[
"Zarembo",
"K.",
""
]
] | We study Wilson loops in N=4 SYM theory which are non-constant in the scalar (S5) directions and open string solutions associated with them in the context of AdS/CFT correspondence. An interplay between Minkowskian and Euclidean pictures turns out to be non-trivial for time-dependent Wilson loops. We find that in the S... | 6.530917 | 6.873706 | 7.450284 | 6.378644 | 7.053483 | 6.281473 | 6.642521 | 6.515435 | 6.629325 | 7.734368 | 6.695386 | 6.227407 | 6.953619 | 6.503564 | 6.560008 | 6.389574 | 6.378997 | 6.345006 | 6.443624 | 6.977419 | 6.345132 |
2403.03285 | Konstantinos Rigatos | Konstantinos C. Rigatos, Shaodong Zhou | Bootstrapping AdS$_2 \times$ S$^2$ hypermultiplets: hidden
four-dimensional conformal symmetry | v1: 23+3 pages, 1 brane scan, 3 Witten diagrams, v2: added ref and
comments | null | 10.1007/JHEP04(2024)128 | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We bootstrap the $4$-point amplitude of $\mathcal{N}=2$ hypermultiplets in
$\text{AdS}_2 \times \text{S}^2$ at tree-level and for arbitrary external
weights. We hereby explicitly demonstrate the existence of a hidden
four-dimensional conformal symmetry that was used as an assumption in previous
studies to derive this... | [
{
"created": "Tue, 5 Mar 2024 19:36:24 GMT",
"version": "v1"
},
{
"created": "Mon, 11 Mar 2024 03:16:21 GMT",
"version": "v2"
},
{
"created": "Thu, 25 Apr 2024 03:15:17 GMT",
"version": "v3"
}
] | 2024-04-26 | [
[
"Rigatos",
"Konstantinos C.",
""
],
[
"Zhou",
"Shaodong",
""
]
] | We bootstrap the $4$-point amplitude of $\mathcal{N}=2$ hypermultiplets in $\text{AdS}_2 \times \text{S}^2$ at tree-level and for arbitrary external weights. We hereby explicitly demonstrate the existence of a hidden four-dimensional conformal symmetry that was used as an assumption in previous studies to derive this r... | 11.063053 | 7.93565 | 9.093027 | 7.796632 | 7.501582 | 7.537097 | 7.288169 | 7.460359 | 8.2024 | 10.743616 | 8.029012 | 8.004662 | 9.327403 | 7.947973 | 8.153817 | 7.994086 | 8.141274 | 8.321073 | 7.822696 | 8.657932 | 8.296073 |
1009.4639 | Eugenio Megias | K. Veschgini, E. Megias, H.J. Pirner | Trouble Finding the Optimal AdS/QCD | 4 pages, 3 figures | Phys.Lett.B696:495-498,2011 | 10.1016/j.physletb.2011.01.011 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the bottom-up approach to AdS/QCD based on a five-dimensional gravity
dilaton action the exponential of the dilaton field is usually identified as
the strong or 't Hooft coupling. There is currently no model known which fits
the measurements of the running coupling and lattice results for pressure at
the same time... | [
{
"created": "Thu, 23 Sep 2010 15:34:23 GMT",
"version": "v1"
},
{
"created": "Tue, 11 Jan 2011 10:55:15 GMT",
"version": "v2"
}
] | 2011-03-07 | [
[
"Veschgini",
"K.",
""
],
[
"Megias",
"E.",
""
],
[
"Pirner",
"H. J.",
""
]
] | In the bottom-up approach to AdS/QCD based on a five-dimensional gravity dilaton action the exponential of the dilaton field is usually identified as the strong or 't Hooft coupling. There is currently no model known which fits the measurements of the running coupling and lattice results for pressure at the same time. ... | 17.252962 | 12.954817 | 12.854042 | 13.607293 | 14.933273 | 14.551066 | 14.010943 | 14.178713 | 12.713744 | 15.364659 | 15.366352 | 13.591737 | 12.532755 | 12.703094 | 13.033982 | 13.232437 | 12.762464 | 13.230645 | 13.085642 | 12.851266 | 14.607192 |
hep-th/9406037 | Noriyuki Humita | Noriyuki Fumita | Quantum Vacuum and Anomalies | 12 pages, 2 figures included in a uuencoded file, phyzzx, OU-HEP-193 | Int.J.Mod.Phys. A10 (1995) 2579-2588 | 10.1142/S0217751X95001224 | null | hep-th | null | Chiral, conformal and ghost number anomalies are discussed from the viewpoint
of the quantum vacuum in Hamiltonian formalism. After introducing the energy
cut-off, we derive known anomalies in a new way. We show that the physical
origin of the anomalies is the zero point fluctuation of bosonic or fermionic
field. We ... | [
{
"created": "Wed, 8 Jun 1994 05:40:22 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Fumita",
"Noriyuki",
""
]
] | Chiral, conformal and ghost number anomalies are discussed from the viewpoint of the quantum vacuum in Hamiltonian formalism. After introducing the energy cut-off, we derive known anomalies in a new way. We show that the physical origin of the anomalies is the zero point fluctuation of bosonic or fermionic field. We fi... | 11.852306 | 10.831883 | 11.610756 | 10.835024 | 11.173519 | 12.022407 | 11.250387 | 11.271302 | 10.747623 | 11.648596 | 10.795701 | 10.578916 | 10.994139 | 10.65356 | 10.9354 | 10.714792 | 10.526222 | 10.726542 | 10.702238 | 10.992872 | 10.297345 |
hep-th/0208162 | Joanna Gonera | Katarzyna Bolonek, Piotr Kosinski | On uncertainty relations in noncommutative quantum mechanics | 8 pages, revised version, few references added | Phys.Lett. B547 (2002) 51-54 | 10.1016/S0370-2693(02)02731-4 | null | hep-th | null | We discuss the uncertainty relations in quantum mechanics on noncommutative
plane. In particular, we show that, for a given state at most one out of three
basic nontrivial uncertainty relations can be saturated. We consider also in
some detail the case of angular momentum eigenstates.
| [
{
"created": "Thu, 22 Aug 2002 13:31:53 GMT",
"version": "v1"
},
{
"created": "Thu, 29 Aug 2002 13:26:25 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Bolonek",
"Katarzyna",
""
],
[
"Kosinski",
"Piotr",
""
]
] | We discuss the uncertainty relations in quantum mechanics on noncommutative plane. In particular, we show that, for a given state at most one out of three basic nontrivial uncertainty relations can be saturated. We consider also in some detail the case of angular momentum eigenstates. | 9.874396 | 9.680397 | 11.631894 | 9.502471 | 8.641602 | 8.980258 | 10.23495 | 8.670432 | 9.858853 | 12.136961 | 9.041575 | 9.633192 | 10.368072 | 9.607485 | 8.719143 | 8.869431 | 9.333149 | 9.072178 | 9.719611 | 10.148703 | 8.961063 |
hep-th/9508141 | Jonathan Evans | Jonathan M. Evans and Timothy J. Hollowood | Exact Results for Integrable Asymptotically-free Field Theories | 16 pages, latex, no figures | Nucl.Phys.Proc.Suppl. 45A (1996) 130-139 | null | CERN-TH/95-230, SWAT/94-95/63 | hep-th | null | An account is given of a technique for testing the equivalence between an
exact factorizable S-matrix and an asymptotically-free Lagrangian field theory
in two space-time dimensions. The method provides a way of resolving CDD
ambiguities in the S-matrix and it also allows for an exact determination of
the physical ma... | [
{
"created": "Fri, 25 Aug 1995 17:01:29 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Evans",
"Jonathan M.",
""
],
[
"Hollowood",
"Timothy J.",
""
]
] | An account is given of a technique for testing the equivalence between an exact factorizable S-matrix and an asymptotically-free Lagrangian field theory in two space-time dimensions. The method provides a way of resolving CDD ambiguities in the S-matrix and it also allows for an exact determination of the physical mass... | 9.311296 | 8.171101 | 9.49781 | 7.369219 | 8.094566 | 7.894749 | 7.634063 | 7.097979 | 7.403384 | 9.646661 | 7.834477 | 7.277199 | 8.098297 | 7.364752 | 7.485316 | 7.695769 | 7.485027 | 7.638296 | 7.197574 | 8.38373 | 7.479904 |
hep-th/0201238 | Ralf Lehnert | Ralf Lehnert | Some Considerations Regarding Lorentz-Violating Theories | 10 pages, presented at the Second Meeting on CPT and Lorentz
Symmetry, Bloomington, Indiana, August 2001 | null | 10.1142/9789812778123_0021 | null | hep-th | null | We investigate the compatibility of Lorentz-violating quantum field theories
with the requirements of causality and stability. A general renormalizable
model for free massive fermions indicates that these requirements are satisfied
at low energies provided the couplings controlling the breaking are small.
However, fo... | [
{
"created": "Tue, 29 Jan 2002 17:40:03 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Lehnert",
"Ralf",
""
]
] | We investigate the compatibility of Lorentz-violating quantum field theories with the requirements of causality and stability. A general renormalizable model for free massive fermions indicates that these requirements are satisfied at low energies provided the couplings controlling the breaking are small. However, for ... | 10.813489 | 11.415536 | 11.844092 | 10.795248 | 11.021021 | 11.037292 | 11.596716 | 10.869454 | 11.132704 | 12.686036 | 10.496187 | 10.669409 | 11.012274 | 10.970154 | 11.035166 | 11.28688 | 10.96602 | 10.674961 | 10.796584 | 11.373576 | 10.662927 |
1703.07993 | Enrique Alvarez | Enrique Alvarez, Jesus Anero and Sergio Gonzalez-Martin | Quadratic gravity in first order formalism | 50 pages, additions and new section. Version to be published in JCAP;
Spotted errata corrected | null | 10.1088/1475-7516/2017/10/008 | FTUAM-17-3; IFT-UAM/CSIC-17-015 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the most general action for gravity which is quadratic in
curvature. In this case first order and second order formalisms are not
equivalent. This framework is a good candidate for a unitary and renormalizable
theory of the gravitational field; in particular, there are no propagators
falling down faster t... | [
{
"created": "Thu, 23 Mar 2017 10:41:02 GMT",
"version": "v1"
},
{
"created": "Mon, 22 May 2017 08:14:09 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Jul 2017 15:06:45 GMT",
"version": "v3"
},
{
"created": "Thu, 14 Sep 2017 09:01:35 GMT",
"version": "v4"
},
{
"c... | 2017-12-22 | [
[
"Alvarez",
"Enrique",
""
],
[
"Anero",
"Jesus",
""
],
[
"Gonzalez-Martin",
"Sergio",
""
]
] | We consider the most general action for gravity which is quadratic in curvature. In this case first order and second order formalisms are not equivalent. This framework is a good candidate for a unitary and renormalizable theory of the gravitational field; in particular, there are no propagators falling down faster tha... | 12.386239 | 9.357004 | 12.88415 | 11.330953 | 12.238444 | 10.060366 | 10.412076 | 10.225866 | 11.312435 | 13.311157 | 11.46089 | 11.633087 | 12.604025 | 11.99122 | 12.545544 | 12.065749 | 11.763328 | 11.822078 | 12.099624 | 12.770493 | 12.07509 |
hep-th/9611094 | Arvind Rajaraman | Renata Kallosh, Arvind Rajaraman and Wing Kai Wong | Supersymmetric Rotating Black Holes and Attractors | 7 pages,latex | Phys.Rev.D55:3246-3249,1997 | 10.1103/PhysRevD.55.3246 | SU-ITP-96-49 | hep-th | null | Five-dimensional stringy rotating black holes are embedded into N=2
supergravity interacting with one vector multiplet. The existence of an
unbroken supersymmetry of the rotating solution is proved directly by solving
the Killing spinor equations. The asymptotic enhancement of supersymmetry near
the horizon in the pr... | [
{
"created": "Wed, 13 Nov 1996 22:31:34 GMT",
"version": "v1"
}
] | 2009-12-30 | [
[
"Kallosh",
"Renata",
""
],
[
"Rajaraman",
"Arvind",
""
],
[
"Wong",
"Wing Kai",
""
]
] | Five-dimensional stringy rotating black holes are embedded into N=2 supergravity interacting with one vector multiplet. The existence of an unbroken supersymmetry of the rotating solution is proved directly by solving the Killing spinor equations. The asymptotic enhancement of supersymmetry near the horizon in the pres... | 9.868957 | 8.643686 | 10.504308 | 8.788232 | 9.182498 | 9.295614 | 8.752067 | 9.033946 | 8.820393 | 10.122942 | 8.487898 | 8.437706 | 9.146074 | 9.012054 | 8.631731 | 8.9958 | 8.735014 | 8.387375 | 8.754283 | 9.479377 | 8.683527 |
hep-th/0301076 | O.-Kab Kwon | Chanju Kim, Hang Bae Kim, Yoonbai Kim, O-Kab Kwon | Electromagnetic String Fluid in Rolling Tachyon | LaTeX, 18 pages, 1 figure, minor corrections | JHEP 0303 (2003) 008 | 10.1088/1126-6708/2003/03/008 | null | hep-th | null | We study Born-Infeld type effective action for unstable D3-brane system
including a tachyon and an Abelian gauge field, and find the rolling tachyon
with constant electric and magnetic fields as the most general homogeneous
solution. Tachyonic vacua are characterized by magnitudes of the electric and
magnetic fields ... | [
{
"created": "Mon, 13 Jan 2003 14:55:16 GMT",
"version": "v1"
},
{
"created": "Thu, 20 Feb 2003 12:04:42 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Mar 2003 04:03:36 GMT",
"version": "v3"
}
] | 2009-11-10 | [
[
"Kim",
"Chanju",
""
],
[
"Kim",
"Hang Bae",
""
],
[
"Kim",
"Yoonbai",
""
],
[
"Kwon",
"O-Kab",
""
]
] | We study Born-Infeld type effective action for unstable D3-brane system including a tachyon and an Abelian gauge field, and find the rolling tachyon with constant electric and magnetic fields as the most general homogeneous solution. Tachyonic vacua are characterized by magnitudes of the electric and magnetic fields an... | 11.728867 | 11.206841 | 12.608699 | 10.66498 | 11.018963 | 11.404882 | 10.275427 | 10.516331 | 10.423636 | 12.433413 | 11.302924 | 11.140441 | 12.47788 | 11.183377 | 11.278845 | 10.872829 | 11.154817 | 11.068378 | 11.244839 | 12.421964 | 11.347744 |
2104.14194 | Andrew McLeod | John Golden and Andrew J. McLeod | The Two-Loop Remainder Function for Eight and Nine Particles | 36 pages, 3 figures, 2 tables | null | 10.1007/JHEP06(2021)142 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Two-loop MHV amplitudes in planar ${\cal N} = 4$ supersymmetric Yang Mills
theory are known to exhibit many intriguing forms of cluster-algebraic
structure. We leverage this structure to upgrade the symbols of the eight- and
nine-particle amplitudes to complete analytic functions. This is done by
systematically proje... | [
{
"created": "Thu, 29 Apr 2021 08:29:43 GMT",
"version": "v1"
}
] | 2021-07-14 | [
[
"Golden",
"John",
""
],
[
"McLeod",
"Andrew J.",
""
]
] | Two-loop MHV amplitudes in planar ${\cal N} = 4$ supersymmetric Yang Mills theory are known to exhibit many intriguing forms of cluster-algebraic structure. We leverage this structure to upgrade the symbols of the eight- and nine-particle amplitudes to complete analytic functions. This is done by systematically project... | 12.648939 | 11.72497 | 12.730815 | 11.051569 | 11.698348 | 10.911107 | 12.035992 | 11.503671 | 11.115438 | 14.676844 | 11.798671 | 11.100142 | 11.987604 | 11.123622 | 11.879601 | 11.362929 | 11.344254 | 11.392958 | 11.02868 | 11.978893 | 11.112365 |
hep-th/0209202 | Kokorelis | Christos Kokorelis | Deformed Intersecting D6-Brane GUTS I | 45 pages, 1 figure, LaTex, The discussion on the hidden orthogonal
U(1) D6-branes extended | JHEP 0211 (2002) 027 | 10.1088/1126-6708/2002/11/027 | FTUAM-02/23, IFT-UAM/CSIC-02-39 | hep-th hep-ph | null | By employing D6-branes intersecting at angles in $D = 4$ type IIA strings, we
construct {\em four stack string GUT models} (PS-I class), that contain at low
energy {\em exactly the three generation Standard model} with no extra matter
and/or extra gauge group factors. These classes of models are based on the
Pati-Sal... | [
{
"created": "Tue, 24 Sep 2002 12:44:25 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Sep 2002 12:56:49 GMT",
"version": "v2"
},
{
"created": "Mon, 16 Dec 2002 18:00:02 GMT",
"version": "v3"
}
] | 2016-09-06 | [
[
"Kokorelis",
"Christos",
""
]
] | By employing D6-branes intersecting at angles in $D = 4$ type IIA strings, we construct {\em four stack string GUT models} (PS-I class), that contain at low energy {\em exactly the three generation Standard model} with no extra matter and/or extra gauge group factors. These classes of models are based on the Pati-Salam... | 12.320704 | 8.376444 | 12.902828 | 10.099266 | 9.116071 | 8.567803 | 9.130818 | 8.942516 | 9.735337 | 13.43678 | 10.123745 | 11.497254 | 11.889915 | 11.301606 | 11.248448 | 10.994469 | 10.95279 | 10.913799 | 11.033106 | 12.208168 | 11.270418 |
1101.2174 | Mairi Sakellariadou | Mairi Sakellariadou | Cosmology within Noncommutative Spectral Geometry | 14 pages. Invited talk in the Corfu Summer Institute on Elementary
Particles and Physics - Workshop on Non Commutative Field Theory and Gravity,
September 8-12, 2010 Corfu Greece | PoS CNCFG2010:028,2010 | null | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Close to the Planck energy scale, the quantum nature of space-time reveals
itself and all forces, including gravity, should be unified so that all
interactions correspond to just one underlying symmetry. In the absence of a
full quantum gravity theory, one may follow an effective approach and consider
space-time as t... | [
{
"created": "Tue, 11 Jan 2011 18:16:07 GMT",
"version": "v1"
}
] | 2015-03-17 | [
[
"Sakellariadou",
"Mairi",
""
]
] | Close to the Planck energy scale, the quantum nature of space-time reveals itself and all forces, including gravity, should be unified so that all interactions correspond to just one underlying symmetry. In the absence of a full quantum gravity theory, one may follow an effective approach and consider space-time as the... | 10.945578 | 11.231083 | 11.585657 | 10.748801 | 11.290613 | 10.474191 | 10.557163 | 10.041653 | 11.019499 | 11.667486 | 11.03669 | 10.920869 | 10.753998 | 10.716268 | 10.99194 | 10.699557 | 10.637103 | 10.615897 | 10.773578 | 10.867692 | 10.576799 |
hep-th/0503089 | Peng Zhang | Bin Chen, Ya-Li He, Peng Zhang and Xing-Chang Song | Flat Currents of the Green-Schwarz Superstrings in AdS_5 x S^1 and AdS_3
x S^3 backgrounds | 18 pages, LaTeX file. References added and typos corrected | Phys.Rev. D71 (2005) 086007 | 10.1103/PhysRevD.71.086007 | null | hep-th | null | We construct a one-parameter family of flat currents in AdS_5 x S^1 and AdS_3
x S^3 Green-Schwarz superstrings, which would naturally lead to a hierarchy of
classical conserved nonlocal charges. In the former case we rewrite the AdS_5 x
S^1 string using a new Z_4-graded base of the superalgebra su(2,2|2). In both
cas... | [
{
"created": "Thu, 10 Mar 2005 14:23:17 GMT",
"version": "v1"
},
{
"created": "Fri, 11 Mar 2005 02:25:13 GMT",
"version": "v2"
},
{
"created": "Mon, 14 Mar 2005 04:42:08 GMT",
"version": "v3"
},
{
"created": "Sun, 20 Mar 2005 06:30:44 GMT",
"version": "v4"
}
] | 2009-11-11 | [
[
"Chen",
"Bin",
""
],
[
"He",
"Ya-Li",
""
],
[
"Zhang",
"Peng",
""
],
[
"Song",
"Xing-Chang",
""
]
] | We construct a one-parameter family of flat currents in AdS_5 x S^1 and AdS_3 x S^3 Green-Schwarz superstrings, which would naturally lead to a hierarchy of classical conserved nonlocal charges. In the former case we rewrite the AdS_5 x S^1 string using a new Z_4-graded base of the superalgebra su(2,2|2). In both cases... | 8.405033 | 7.802138 | 9.954101 | 8.044785 | 8.535727 | 8.485632 | 8.504813 | 7.613235 | 7.883274 | 11.694238 | 7.250968 | 7.77514 | 8.53351 | 7.818225 | 7.97012 | 7.7618 | 7.746488 | 7.512655 | 8.172041 | 8.869286 | 7.74345 |
hep-th/0506185 | Manvelyan Ruben | Ruben Manvelyan and Werner Ruehl | The quantum one loop trace anomaly of the higher spin conformal
conserved currents in the bulk of $AdS_{4}$ | 23 pages, Latex, misprints corrected, v.3 two sections added, v.4
published version in Nucl. Phys. B | Nucl.Phys. B733 (2006) 104-122 | 10.1016/j.nuclphysb.2005.10.034 | null | hep-th | null | An analysis of the structure and singularities of the one loop two point
function of the higher spin traceless and conserved currents constructed from
the single scalar field in $AdS$ space is presented. The detailed
renormalization procedure is constructed and the quantum violation of the
traceless Ward identity is ... | [
{
"created": "Wed, 22 Jun 2005 07:56:38 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Jul 2005 11:36:11 GMT",
"version": "v2"
},
{
"created": "Mon, 17 Oct 2005 10:35:31 GMT",
"version": "v3"
},
{
"created": "Tue, 7 Feb 2006 10:09:37 GMT",
"version": "v4"
}
] | 2010-04-05 | [
[
"Manvelyan",
"Ruben",
""
],
[
"Ruehl",
"Werner",
""
]
] | An analysis of the structure and singularities of the one loop two point function of the higher spin traceless and conserved currents constructed from the single scalar field in $AdS$ space is presented. The detailed renormalization procedure is constructed and the quantum violation of the traceless Ward identity is in... | 11.868676 | 9.809623 | 10.969424 | 8.972569 | 9.778226 | 9.223509 | 9.176829 | 9.530958 | 9.100164 | 13.156921 | 9.326636 | 8.97884 | 10.43548 | 9.701744 | 9.62993 | 9.635404 | 9.572913 | 9.806791 | 9.513692 | 10.236238 | 9.38986 |
1702.03934 | Ashoke Sen | Ashoke Sen | Soft Theorems in Superstring Theory | LaTex file, 21 pages; v2: references updated, other minor changes;
v3: minor clarifications added | JHEP 1706 (2017) 113 | 10.1007/JHEP06(2017)113 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use insights from superstring field theory to prove the subleading soft
graviton theorem for tree amplitudes of (compactified) heterotic and type II
string theories for arbitrary number of finite energy NS (NSNS) sector external
states but only one soft graviton. We also prove the leading soft graviton
theorem in ... | [
{
"created": "Mon, 13 Feb 2017 19:00:03 GMT",
"version": "v1"
},
{
"created": "Sat, 15 Apr 2017 07:53:46 GMT",
"version": "v2"
},
{
"created": "Sat, 22 Jul 2017 16:38:03 GMT",
"version": "v3"
}
] | 2017-07-25 | [
[
"Sen",
"Ashoke",
""
]
] | We use insights from superstring field theory to prove the subleading soft graviton theorem for tree amplitudes of (compactified) heterotic and type II string theories for arbitrary number of finite energy NS (NSNS) sector external states but only one soft graviton. We also prove the leading soft graviton theorem in th... | 8.01128 | 6.548394 | 8.142695 | 6.656725 | 7.098199 | 7.037648 | 7.1663 | 6.340158 | 6.822792 | 10.139297 | 6.654835 | 6.902867 | 7.676474 | 7.384878 | 7.083214 | 7.012206 | 6.906631 | 6.971041 | 6.913444 | 7.577477 | 7.034911 |
hep-th/9602118 | Paul Aspinwall | Paul S. Aspinwall and Mark Gross | Heterotic-Heterotic String Duality and Multiple K3 Fibrations | 13 pages, LaTeX | Phys.Lett. B382 (1996) 81-88 | 10.1016/0370-2693(96)00551-5 | CLNS-96/1402 | hep-th | null | A type IIA string compactified on a Calabi-Yau manifold which admits a K3
fibration is believed to be equivalent to a heterotic string in four
dimensions. We study cases where a Calabi-Yau manifold can have more than one
such fibration leading to equivalences between perturbatively inequivalent
heterotic strings. Thi... | [
{
"created": "Wed, 21 Feb 1996 19:12:26 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Aspinwall",
"Paul S.",
""
],
[
"Gross",
"Mark",
""
]
] | A type IIA string compactified on a Calabi-Yau manifold which admits a K3 fibration is believed to be equivalent to a heterotic string in four dimensions. We study cases where a Calabi-Yau manifold can have more than one such fibration leading to equivalences between perturbatively inequivalent heterotic strings. This ... | 6.535834 | 5.869352 | 7.495342 | 6.286456 | 7.044583 | 6.197107 | 6.253622 | 5.908101 | 6.069659 | 7.69891 | 6.127848 | 6.288201 | 6.881199 | 6.116293 | 6.169748 | 6.281937 | 6.312813 | 6.226367 | 6.313509 | 6.543903 | 6.285317 |
1209.5817 | O-Kab Kwon | Yoonbai Kim, O-Kab Kwon, D. D. Tolla | Partially Supersymmetric ABJM Theory with Flux | 22 pages, 1 figure | null | 10.1007/JHEP11(2012)169 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Starting with generic Wess-Zumino type coupling to constant four-form and the
dual seven-form field strengths in the ABJM theory, we obtain mass-deformed
theories with ${\cal N}=2,4$ supersymmetries. These theories contain massless
scalar fields and allow the implementation of the Mukhi-Papageorgakis Higgsing
procedu... | [
{
"created": "Wed, 26 Sep 2012 02:22:26 GMT",
"version": "v1"
}
] | 2015-06-11 | [
[
"Kim",
"Yoonbai",
""
],
[
"Kwon",
"O-Kab",
""
],
[
"Tolla",
"D. D.",
""
]
] | Starting with generic Wess-Zumino type coupling to constant four-form and the dual seven-form field strengths in the ABJM theory, we obtain mass-deformed theories with ${\cal N}=2,4$ supersymmetries. These theories contain massless scalar fields and allow the implementation of the Mukhi-Papageorgakis Higgsing procedure... | 8.633775 | 8.197844 | 9.242467 | 8.062201 | 8.579774 | 8.650497 | 8.827088 | 8.477808 | 8.264957 | 10.462994 | 7.626044 | 8.032822 | 8.240431 | 7.791457 | 7.986245 | 8.258328 | 8.068563 | 8.116918 | 7.973528 | 8.382353 | 7.966664 |
1402.1934 | Seyed Morteza Hosseini | Farid Charmchi, Siamak S. Gousheh and Seyed Morteza Hosseini | One-loop quantum correction to the mass of the supersymmetric Kink in (1
+ 1) dimensions using the exact spectra and the phase shifts | 15 pages, 3 figures, V2: Paper revised, references added, published
version | J. Phys. A: Math. Theor. 47 (2014) 335401 | 10.1088/1751-8113/47/33/335401 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute the quantum correction to the mass of the kink at the one-loop
level in (1+1) dimensions with minimal supersymmetry. In this paper we discuss
this issue from the Casimir energy perspective using phase shifts along with
the mode number cut-off regularization method. Exact solutions and in
particular an exac... | [
{
"created": "Sun, 9 Feb 2014 11:19:46 GMT",
"version": "v1"
},
{
"created": "Thu, 7 Aug 2014 12:36:31 GMT",
"version": "v2"
}
] | 2014-08-08 | [
[
"Charmchi",
"Farid",
""
],
[
"Gousheh",
"Siamak S.",
""
],
[
"Hosseini",
"Seyed Morteza",
""
]
] | We compute the quantum correction to the mass of the kink at the one-loop level in (1+1) dimensions with minimal supersymmetry. In this paper we discuss this issue from the Casimir energy perspective using phase shifts along with the mode number cut-off regularization method. Exact solutions and in particular an exact ... | 8.722885 | 8.164647 | 8.797263 | 8.021862 | 8.221839 | 8.669828 | 8.417904 | 8.287821 | 8.246258 | 8.872938 | 8.109011 | 8.281267 | 8.592423 | 8.248075 | 8.232256 | 8.313993 | 8.45696 | 8.350173 | 8.481065 | 8.534763 | 8.41626 |
2302.00684 | Carlos Heredia Pimienta | Carlos Heredia and Josep Llosa | Infinite Derivatives vs Integral Operators. The Moeller-Zwiebach Puzzle | 19 pages, 3 figures | 2024 J. Phys. A: Math. Theor. 57 235202 | 10.1088/1751-8121/ad4aa5 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the relationship between integral and infinite-derivative operators.
In particular, we examine the operator $p^{\frac12\,\partial_t^2}\,$ that
appears in the theory of $p$-adic string fields, as well as the Moyal product
that arises in non-commutative theories. We also attempt to clarify the
apparent paradox... | [
{
"created": "Wed, 1 Feb 2023 19:00:01 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Feb 2023 16:14:25 GMT",
"version": "v2"
},
{
"created": "Fri, 24 May 2024 10:22:59 GMT",
"version": "v3"
}
] | 2024-05-27 | [
[
"Heredia",
"Carlos",
""
],
[
"Llosa",
"Josep",
""
]
] | We study the relationship between integral and infinite-derivative operators. In particular, we examine the operator $p^{\frac12\,\partial_t^2}\,$ that appears in the theory of $p$-adic string fields, as well as the Moyal product that arises in non-commutative theories. We also attempt to clarify the apparent paradox p... | 13.118348 | 14.405075 | 16.029852 | 12.758649 | 16.118664 | 12.589249 | 13.391934 | 13.030318 | 12.242258 | 15.325179 | 12.962648 | 12.002353 | 13.625997 | 12.287879 | 12.313735 | 12.1952 | 12.207222 | 12.388879 | 13.128135 | 13.228696 | 12.566808 |
0907.1824 | Nadareishvili Teimuraz Pavel | T. Nadareishvili, A. Khelashvili | Generalization of Hypervirial and Feynman-Hellmann Theorems for Singular
Potentials | 14 pages | null | null | null | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using well-known methods we generalize (hyper)virial theorems to case of
singular potential. Discussion is performed for most general second order
differential equation, which involves all physically interesting cases, as
Schrodinger and Klein-Gordon equations with singular potentials. Some physical
consequences are ... | [
{
"created": "Fri, 10 Jul 2009 16:43:32 GMT",
"version": "v1"
},
{
"created": "Thu, 19 Nov 2009 21:09:32 GMT",
"version": "v2"
}
] | 2009-11-19 | [
[
"Nadareishvili",
"T.",
""
],
[
"Khelashvili",
"A.",
""
]
] | Using well-known methods we generalize (hyper)virial theorems to case of singular potential. Discussion is performed for most general second order differential equation, which involves all physically interesting cases, as Schrodinger and Klein-Gordon equations with singular potentials. Some physical consequences are di... | 16.855042 | 16.871759 | 15.141491 | 15.562533 | 17.065739 | 14.578159 | 18.714544 | 15.038345 | 15.161022 | 18.30094 | 16.265848 | 15.49179 | 15.796811 | 15.099208 | 15.198086 | 15.062967 | 14.981209 | 14.549363 | 14.712684 | 15.097487 | 14.988339 |
2003.08405 | Edward Hardy | Joan Elias Miro, Edward Hardy | Exploring Hamiltonian Truncation in $\bf{d=2+1}$ | 51 pages, 14 figures | Phys. Rev. D 102, 065001 (2020) | 10.1103/PhysRevD.102.065001 | null | hep-th cond-mat.stat-mech cond-mat.str-el hep-lat hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We initiate the application of Hamiltonian Truncation methods to solve
strongly coupled QFTs in $d=2+1$. By analysing perturbation theory with a
Hamiltonian Truncation regulator, we pinpoint the challenges of such an
approach and propose a way that these can be addressed. This enables us to
formulate Hamiltonian Trun... | [
{
"created": "Wed, 18 Mar 2020 18:00:13 GMT",
"version": "v1"
}
] | 2020-09-09 | [
[
"Miro",
"Joan Elias",
""
],
[
"Hardy",
"Edward",
""
]
] | We initiate the application of Hamiltonian Truncation methods to solve strongly coupled QFTs in $d=2+1$. By analysing perturbation theory with a Hamiltonian Truncation regulator, we pinpoint the challenges of such an approach and propose a way that these can be addressed. This enables us to formulate Hamiltonian Trunca... | 9.022472 | 8.442992 | 9.214761 | 8.159505 | 8.756226 | 8.190207 | 8.344845 | 8.184889 | 8.203603 | 9.777011 | 8.008362 | 8.363782 | 8.876758 | 8.914172 | 8.510959 | 8.846254 | 8.601419 | 8.511182 | 8.695649 | 9.532896 | 8.650407 |
0905.4123 | Yoshiharu Kawamura | Yoshiharu Kawamura, Takashi Miura | Equivalence Classes of Boundary Conditions in SU(N) Gauge Theory on
2-dimensional Orbifolds | 18 pages, 4 figures, revised version for publication in PTP | Prog.Theor.Phys.122:847-864,2010 | 10.1143/PTP.122.847 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study equivalence classes of boundary conditions in an SU(N) gauge theory
on six-dimensional space-time including two-dimensional orbifold. For five
kinds of two-dimensional orbifolds $S^1/Z_2 \times S^1/Z_2$ and $T^2/Z_m$
$(m=2,3,4,6)$, orbifold conditions and those gauge transformation properties
are given and t... | [
{
"created": "Tue, 26 May 2009 06:21:07 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Aug 2009 10:16:01 GMT",
"version": "v2"
}
] | 2010-01-15 | [
[
"Kawamura",
"Yoshiharu",
""
],
[
"Miura",
"Takashi",
""
]
] | We study equivalence classes of boundary conditions in an SU(N) gauge theory on six-dimensional space-time including two-dimensional orbifold. For five kinds of two-dimensional orbifolds $S^1/Z_2 \times S^1/Z_2$ and $T^2/Z_m$ $(m=2,3,4,6)$, orbifold conditions and those gauge transformation properties are given and the... | 8.770679 | 7.960378 | 8.419303 | 7.586055 | 8.126828 | 8.504533 | 10.164607 | 8.318355 | 7.821771 | 7.508266 | 7.764003 | 8.716894 | 8.597513 | 8.217881 | 8.204347 | 8.115296 | 8.71393 | 8.523492 | 8.217751 | 8.391313 | 8.123852 |
hep-th/9411223 | Franco Ferrari | Franco Ferrari | Gauge Field Theories on Riemann Surfaces | 22 pages, Plain TeX, to appear in Helv. Phys. Acta | Helv.Phys.Acta 67:702-722,1994 | null | UTF 321-94 | hep-th | null | In this paper the free gauge field theories on a Riemann surface of any genus
are quantized in the covariant gauge. The propagators of the gauge fields are
explicitly derived and their properties are analysed in details. As an
application, the correlation functions of a Yang-Mills field theory with gauge
group $SU(N)... | [
{
"created": "Tue, 29 Nov 1994 18:16:18 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Ferrari",
"Franco",
""
]
] | In this paper the free gauge field theories on a Riemann surface of any genus are quantized in the covariant gauge. The propagators of the gauge fields are explicitly derived and their properties are analysed in details. As an application, the correlation functions of a Yang-Mills field theory with gauge group $SU(N)$ ... | 8.238538 | 5.366257 | 7.400282 | 6.316183 | 5.851079 | 5.905034 | 5.941382 | 5.932915 | 6.239159 | 6.901329 | 6.198658 | 6.483523 | 6.928762 | 6.36524 | 6.537884 | 6.614384 | 6.382569 | 6.580363 | 6.450545 | 6.886888 | 6.480251 |
1208.4577 | BingKan Xue | BingKan Xue | The four fixed points of scale invariant single field cosmological
models | 24 pages, 6 figures | JCAP 1210 (2012) 054 | 10.1088/1475-7516/2012/10/054 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a new set of flow parameters to describe the time dependence of
the equation of state and the speed of sound in single field cosmological
models. A scale invariant power spectrum is produced if these flow parameters
satisfy specific dynamical equations. We analyze the flow of these parameters
and find fo... | [
{
"created": "Wed, 22 Aug 2012 19:05:13 GMT",
"version": "v1"
}
] | 2015-04-14 | [
[
"Xue",
"BingKan",
""
]
] | We introduce a new set of flow parameters to describe the time dependence of the equation of state and the speed of sound in single field cosmological models. A scale invariant power spectrum is produced if these flow parameters satisfy specific dynamical equations. We analyze the flow of these parameters and find four... | 11.402504 | 10.668033 | 11.682024 | 9.958817 | 9.889729 | 9.851455 | 11.006787 | 10.158828 | 10.944727 | 12.147663 | 10.137625 | 11.152211 | 12.730042 | 10.876171 | 10.851042 | 10.499215 | 10.603523 | 10.516674 | 10.791036 | 11.791734 | 10.294927 |
2211.13261 | Christian Saemann | Leron Borsten, Branislav Jurco, Hyungrok Kim, Tommaso Macrelli,
Christian Saemann, Martin Wolf | Kinematic Lie Algebras From Twistor Spaces | v2: presentation improved, typos fixed, published version | Phys. Rev. Lett. 131, 041603 (2023) | 10.1103/PhysRevLett.131.041603 | DMUS--MP--22/23, EMPG--22--22 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze theories with color-kinematics duality from an algebraic
perspective and find that any such theory has an underlying BV${}^{\color{gray}
\blacksquare}$-algebra structure, extending the ideas of arXiv:1912.03110.
Conversely, we show that any theory with a BV${}^{\color{gray}
\blacksquare}$-algebra features ... | [
{
"created": "Wed, 23 Nov 2022 19:17:54 GMT",
"version": "v1"
},
{
"created": "Thu, 21 Sep 2023 14:04:15 GMT",
"version": "v2"
}
] | 2023-09-22 | [
[
"Borsten",
"Leron",
""
],
[
"Jurco",
"Branislav",
""
],
[
"Kim",
"Hyungrok",
""
],
[
"Macrelli",
"Tommaso",
""
],
[
"Saemann",
"Christian",
""
],
[
"Wolf",
"Martin",
""
]
] | We analyze theories with color-kinematics duality from an algebraic perspective and find that any such theory has an underlying BV${}^{\color{gray} \blacksquare}$-algebra structure, extending the ideas of arXiv:1912.03110. Conversely, we show that any theory with a BV${}^{\color{gray} \blacksquare}$-algebra features a ... | 5.729711 | 5.417571 | 6.106368 | 5.457924 | 5.660261 | 5.040548 | 5.443895 | 5.118816 | 5.327551 | 6.876863 | 5.351702 | 5.428937 | 5.958379 | 5.476685 | 5.496231 | 5.428793 | 5.40947 | 5.53909 | 5.408318 | 5.989436 | 5.362669 |
hep-th/0212101 | Zurab Kakushadze | Olindo Corradini, Alberto Iglesias and Zurab Kakushadze | Toward Solving the Cosmological Constant Problem? | 45 pages, revtex, 8 eps figures | Int.J.Mod.Phys. A18 (2003) 3221 | 10.1142/S0217751X0301509X | YITP-SB-02-25 | hep-th | null | We discuss the cosmological constant problem in the context of higher
codimension brane world scenarios with infinite-volume extra dimensions. In
particular, by adding higher curvature terms in the bulk action we are able to
find smooth solutions with the property that the 4-dimensional part of the
brane world-volume... | [
{
"created": "Tue, 10 Dec 2002 01:09:25 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Corradini",
"Olindo",
""
],
[
"Iglesias",
"Alberto",
""
],
[
"Kakushadze",
"Zurab",
""
]
] | We discuss the cosmological constant problem in the context of higher codimension brane world scenarios with infinite-volume extra dimensions. In particular, by adding higher curvature terms in the bulk action we are able to find smooth solutions with the property that the 4-dimensional part of the brane world-volume i... | 7.776195 | 5.818348 | 7.728609 | 6.224514 | 6.3862 | 5.759589 | 5.870167 | 5.910447 | 5.902865 | 7.396722 | 5.846383 | 6.537949 | 7.174595 | 6.604207 | 6.839311 | 6.461834 | 6.503712 | 6.568706 | 6.78704 | 6.878039 | 6.521537 |
1903.08664 | Francesco Sgarlata | Brando Bellazzini, Francesco Riva, Javi Serra and Francesco Sgarlata | Massive Higher Spins: Effective Theory and Consistency | 22 pages, 2 figures and 2 appendices; v2 improved discussion, extra
appendix and references added | null | 10.1007/JHEP10(2019)189 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We construct the effective field theory for a single massive higher-spin
particle in flat spacetime. Positivity bounds of the S-matrix force the cutoff
of the theory to be well below the naive strong-coupling scale, forbid any
potential and make therefore higher-derivative operators important even at low
energy. As i... | [
{
"created": "Wed, 20 Mar 2019 18:00:05 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Jun 2019 18:00:00 GMT",
"version": "v2"
}
] | 2020-01-08 | [
[
"Bellazzini",
"Brando",
""
],
[
"Riva",
"Francesco",
""
],
[
"Serra",
"Javi",
""
],
[
"Sgarlata",
"Francesco",
""
]
] | We construct the effective field theory for a single massive higher-spin particle in flat spacetime. Positivity bounds of the S-matrix force the cutoff of the theory to be well below the naive strong-coupling scale, forbid any potential and make therefore higher-derivative operators important even at low energy. As int... | 13.36792 | 14.461094 | 14.974409 | 12.64729 | 13.887516 | 12.734889 | 11.533913 | 12.935715 | 13.073393 | 16.740562 | 13.54526 | 12.566706 | 13.744334 | 13.397226 | 12.984852 | 13.4615 | 13.62395 | 12.857557 | 13.13274 | 13.40183 | 13.079821 |
hep-th/9503090 | null | R.P. Manvelyan, D.H. Tchrakian | A HIERARCHY OF GAUGED GRASSMANIAN MODELS IN $4p$ DIMENSIONS WITH
SELF-DUAL INSTANTONS | latex file, 13 pages | Phys.Lett. B352 (1995) 321-326 | 10.1016/0370-2693(95)00487-6 | YERPHI-1436(6)-95 | hep-th | null | We present a hierarchy of gauged Grassmanian models in $4p$ dimensions, where
the gauge field takes its values in the $2^{2p- 1}\times 2^{2p-1}$ chiral
representation of SO(4p). The actions of all these models are absolutely
minimised by a hierarchy of self-duality equations, all of which reduce to a
single pair of c... | [
{
"created": "Tue, 14 Mar 1995 09:18:37 GMT",
"version": "v1"
}
] | 2019-08-17 | [
[
"Manvelyan",
"R. P.",
""
],
[
"Tchrakian",
"D. H.",
""
]
] | We present a hierarchy of gauged Grassmanian models in $4p$ dimensions, where the gauge field takes its values in the $2^{2p- 1}\times 2^{2p-1}$ chiral representation of SO(4p). The actions of all these models are absolutely minimised by a hierarchy of self-duality equations, all of which reduce to a single pair of cou... | 10.157728 | 10.278533 | 9.738608 | 9.445108 | 9.861413 | 10.335073 | 11.527105 | 10.887034 | 10.473603 | 11.526987 | 9.953467 | 9.655959 | 9.609778 | 9.436967 | 9.504089 | 9.577848 | 9.418147 | 9.67161 | 9.701828 | 9.999631 | 9.714028 |
hep-th/0512344 | George Savvidy K | G.Savvidy and T.Tsukioka | Gauge invariant Lagrangian for non-Abelian tensor gauge fields of fourth
rank | 27 pages, LaTex file | Prog.Theor.Phys.117:729-743,2007 | 10.1143/PTP.117.729 | NRCPS-HE-05-63 | hep-th | null | Using generalized field strength tensors for non-Abelian tensor gauge fields
one can explicitly construct all possible Lorentz invariant quadratic forms for
rank-4 non-Abelian tensor gauge fields and demonstrate that there exist only
two linear combinations of them which form a gauge invariant Lagrangian.
Together wi... | [
{
"created": "Thu, 29 Dec 2005 22:23:11 GMT",
"version": "v1"
},
{
"created": "Sat, 31 Dec 2005 10:43:23 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Savvidy",
"G.",
""
],
[
"Tsukioka",
"T.",
""
]
] | Using generalized field strength tensors for non-Abelian tensor gauge fields one can explicitly construct all possible Lorentz invariant quadratic forms for rank-4 non-Abelian tensor gauge fields and demonstrate that there exist only two linear combinations of them which form a gauge invariant Lagrangian. Together with... | 10.737007 | 8.988419 | 9.545243 | 8.697527 | 9.079159 | 8.810417 | 9.455031 | 9.251933 | 7.90591 | 10.218985 | 8.525565 | 9.160897 | 9.24394 | 9.278112 | 9.468358 | 8.982911 | 9.319267 | 9.113455 | 9.259359 | 9.569657 | 9.611075 |
2111.10987 | Mohammad R. Garousi | Mohammad R. Garousi | Higher-derivative field redefinitions in the presence of boundary | 27 pages, no figure, Latex file;v2:extend the cosmological reduction
to the general one-dimensional reduction which includes timelike or spacelike
boundary; v3:it appears in EPJC | null | 10.1140/epjc/s10052-022-10611-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently it has been proposed that the consistency with T-duality requires
the effective action of string theory at order $\alpha'^n$ satisfies the least
action principle provided that the values of the massless fields and their
derivatives up to order $n$ are known on the boundary. In this paper we
speculate that th... | [
{
"created": "Mon, 22 Nov 2021 05:05:34 GMT",
"version": "v1"
},
{
"created": "Wed, 15 Dec 2021 09:45:27 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Jul 2022 05:51:12 GMT",
"version": "v3"
}
] | 2022-08-10 | [
[
"Garousi",
"Mohammad R.",
""
]
] | Recently it has been proposed that the consistency with T-duality requires the effective action of string theory at order $\alpha'^n$ satisfies the least action principle provided that the values of the massless fields and their derivatives up to order $n$ are known on the boundary. In this paper we speculate that this... | 8.41216 | 8.73877 | 9.602513 | 8.26454 | 9.325018 | 8.530936 | 8.504947 | 8.474586 | 8.295622 | 11.316652 | 8.359605 | 8.496906 | 8.751831 | 8.215557 | 8.239743 | 8.351077 | 8.231619 | 8.366832 | 8.122412 | 8.561839 | 8.135281 |
hep-th/0703098 | Sergey Solodukhin N. | G. W. Gibbons and S. N. Solodukhin | The Geometry of Small Causal Diamonds | 17 pages, no figures; Misprints in eqs.(62), (65), (66) and (81)
corrected; a new note on page 13 (with 2 new equations) added | Phys.Lett.B649:317-324,2007 | 10.1016/j.physletb.2007.03.068 | DAMTP-2007-22 | hep-th gr-qc math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The geometry of causal diamonds or Alexandrov open sets whose initial and
final events $p$ and $q$ respectively have a proper-time separation $\tau$
small compared with the curvature scale is a universal. The corrections from
flat space are given as a power series in $\tau$ whose coefficients involve the
curvature at... | [
{
"created": "Fri, 9 Mar 2007 18:51:24 GMT",
"version": "v1"
},
{
"created": "Sun, 11 Mar 2007 22:44:01 GMT",
"version": "v2"
},
{
"created": "Wed, 12 Aug 2015 15:41:06 GMT",
"version": "v3"
}
] | 2015-08-13 | [
[
"Gibbons",
"G. W.",
""
],
[
"Solodukhin",
"S. N.",
""
]
] | The geometry of causal diamonds or Alexandrov open sets whose initial and final events $p$ and $q$ respectively have a proper-time separation $\tau$ small compared with the curvature scale is a universal. The corrections from flat space are given as a power series in $\tau$ whose coefficients involve the curvature at t... | 8.22121 | 9.090006 | 8.903498 | 8.343785 | 8.768478 | 8.341818 | 8.62912 | 8.565545 | 8.15278 | 8.921194 | 8.39395 | 7.882177 | 8.036765 | 8.011379 | 8.234882 | 8.379618 | 8.232471 | 8.129815 | 7.881643 | 8.041819 | 8.076944 |
0901.4773 | Leonardo Pati\~no | Leonardo Patino, G. Toledo Sanchez | Hadron production in electron-positron annihilation computed from the
gauge gravity correspondence | 7 pages, 1 figure. Extended version with minor changes in emphasis
and references added | Phys.Rev.D80:126019,2009 | 10.1103/PhysRevD.80.126019 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide a non-perturbative expression for the hadron production in
electron-positron annihilation at zero temperature in a strongly coupled,
large-Nc SU(Nc) field theory with Nf << Nc quark flavors. The resulting
expressions are valid to leading order in the electromagnetic coupling constant
but non-perturbatively... | [
{
"created": "Fri, 30 Jan 2009 20:50:18 GMT",
"version": "v1"
},
{
"created": "Wed, 6 Jan 2010 07:16:25 GMT",
"version": "v2"
}
] | 2010-04-21 | [
[
"Patino",
"Leonardo",
""
],
[
"Sanchez",
"G. Toledo",
""
]
] | We provide a non-perturbative expression for the hadron production in electron-positron annihilation at zero temperature in a strongly coupled, large-Nc SU(Nc) field theory with Nf << Nc quark flavors. The resulting expressions are valid to leading order in the electromagnetic coupling constant but non-perturbatively i... | 10.680408 | 11.375978 | 11.733549 | 10.463395 | 11.520553 | 11.922427 | 10.254652 | 11.507743 | 10.372653 | 13.141579 | 10.374939 | 10.342127 | 10.436226 | 10.164176 | 10.215177 | 10.452557 | 10.351593 | 10.57416 | 10.427488 | 10.889373 | 10.506832 |
1306.4914 | Amjad Ashoorioon | Amjad Ashoorioon, Konstantinos Dimopoulos, M. M. Sheikh-Jabbari and
Gary Shiu | Reconciliation of High Energy Scale Models of Inflation with Planck | v1: 5 pages, 1 figure; v2: added references; v3: matched the
published version | JCAP02(2014)025 | 10.1088/1475-7516/2014/02/025 | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The inflationary cosmology paradigm is very successful in explaining the CMB
anisotropy to the percent level. Besides the dependence on the inflationary
model, the power spectra, spectral tilt and non-Gaussianity of the CMB
temperature fluctuations also depend on the initial state of inflation. Here,
we examine to wh... | [
{
"created": "Thu, 20 Jun 2013 15:37:04 GMT",
"version": "v1"
},
{
"created": "Mon, 1 Jul 2013 16:27:12 GMT",
"version": "v2"
},
{
"created": "Thu, 6 Feb 2014 13:26:42 GMT",
"version": "v3"
}
] | 2014-02-18 | [
[
"Ashoorioon",
"Amjad",
""
],
[
"Dimopoulos",
"Konstantinos",
""
],
[
"Sheikh-Jabbari",
"M. M.",
""
],
[
"Shiu",
"Gary",
""
]
] | The inflationary cosmology paradigm is very successful in explaining the CMB anisotropy to the percent level. Besides the dependence on the inflationary model, the power spectra, spectral tilt and non-Gaussianity of the CMB temperature fluctuations also depend on the initial state of inflation. Here, we examine to what... | 8.580808 | 8.814672 | 8.758867 | 8.087107 | 8.568964 | 9.130348 | 9.036272 | 8.780167 | 8.387632 | 8.979866 | 8.722353 | 8.596188 | 8.346767 | 8.123657 | 8.589509 | 8.317324 | 8.291618 | 8.235543 | 8.180855 | 8.491084 | 8.320699 |
1407.0306 | Andrea Amoretti | Andrea Amoretti, Alessandro Braggio, Nicola Maggiore, Nicodemo Magnoli
and Daniele Musso | Analytic DC thermo-electric conductivities in holography with massive
gravitons | 9 pages, no figures, minor comments added, version to appear on PRD | Phys. Rev. D 91 (2015), 025002 | 10.1103/PhysRevD.91.025002 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We provide an analytical derivation of the thermo-electric transport
coefficients of the simplest momentum-dissipating model in gauge/gravity where
the lack of momentum conservation is realized by means of explicit graviton
mass in the bulk. We rely on the procedure recently described by Donos and
Gauntlett in the co... | [
{
"created": "Tue, 1 Jul 2014 16:24:12 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Dec 2014 10:16:33 GMT",
"version": "v2"
}
] | 2015-01-09 | [
[
"Amoretti",
"Andrea",
""
],
[
"Braggio",
"Alessandro",
""
],
[
"Maggiore",
"Nicola",
""
],
[
"Magnoli",
"Nicodemo",
""
],
[
"Musso",
"Daniele",
""
]
] | We provide an analytical derivation of the thermo-electric transport coefficients of the simplest momentum-dissipating model in gauge/gravity where the lack of momentum conservation is realized by means of explicit graviton mass in the bulk. We rely on the procedure recently described by Donos and Gauntlett in the cont... | 11.814532 | 9.937485 | 16.011562 | 9.982913 | 10.225175 | 10.060299 | 10.537501 | 10.522019 | 10.911002 | 16.84483 | 9.481053 | 11.138435 | 11.3946 | 11.020965 | 11.434434 | 10.636134 | 10.454987 | 10.428658 | 11.028622 | 11.17868 | 10.456984 |
hep-th/9301078 | null | Alain Dasnieres de Veigy and Stephane Ouvry | Topological 2-Dimensional Quantum Mechanics | 18 pages, Orsay Report IPNO/TH 92-101 | Phys.Lett. B307 (1993) 91-99 | 10.1016/0370-2693(93)90197-P | null | hep-th | null | We define a Chern- Simons Lagrangian for a system of planar particles
topologically interacting at a distance. The anyon model appears as a
particular case where all the particles are identical. We propose exact N-body
eigenstates, set up a perturbative algorithm, discuss the case where some
particles are fixed on a ... | [
{
"created": "Tue, 19 Jan 1993 10:45:13 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Jan 1993 11:54:47 GMT",
"version": "v2"
}
] | 2009-10-22 | [
[
"de Veigy",
"Alain Dasnieres",
""
],
[
"Ouvry",
"Stephane",
""
]
] | We define a Chern- Simons Lagrangian for a system of planar particles topologically interacting at a distance. The anyon model appears as a particular case where all the particles are identical. We propose exact N-body eigenstates, set up a perturbative algorithm, discuss the case where some particles are fixed on a la... | 12.517934 | 13.427202 | 13.242963 | 11.857196 | 12.684191 | 12.773008 | 12.363707 | 11.540682 | 11.884754 | 14.264151 | 11.330975 | 12.254091 | 13.00451 | 11.867624 | 12.64786 | 12.357665 | 12.463728 | 12.275064 | 12.227542 | 13.170897 | 12.672176 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.